diff --git a/.decent_ci-Linux.yaml b/.decent_ci-Linux.yaml
index 486eea2d906..8c96ba199af 100644
--- a/.decent_ci-Linux.yaml
+++ b/.decent_ci-Linux.yaml
@@ -3,9 +3,8 @@ compilers:
     version: "4.8"
     build_package_generator: "STGZ"
     release_build_enable_pgo: true
-    release_build_training_cmake_extra_flags: -DPROFILE_GENERATE:BOOL=ON -DPROFILE_USE:BOOL=OFF -DENABLE_REGRESSION_TESTING:BOOL=OFF
     release_build_training_ctest_filter:  -R  "integration.(RefBldg.*|.*Slab|.*[^g]Basement|.*5Zone.*|Rad|Pip|.*Network.*|Window|CentralChillerHeaterSystem_Cooling_Heating|CmplxGlz_.*|ConvectionAdaptiveSmallOffice|DElight.*|DaylightingDevice.*|DisplacementVent_Nat_AirflowNetwork_AdaptiveComfort|DOADualDuctSchool|EMS.*|Flr_Rf_8Sides|FluidCooler|GSHP.*|GeneratorswithPV|HeatPumpWaterToAir.*|HospitalBaselineReheatReportEMS|HospitalLowEnergy|MicroCogeneration|PlantApplicationsGuide.*|PlateHeatExchanger|PurchAirWithDaylighting|RefrigeratedWarehouse|SolarCollectorFlatPlateWater|SurfaceTest|ThermalChimneyTest|UserDefinedRoomAirPatterns|VSHeatPumpWaterToAirEquationFit|WaterHeater.*|_CTFTestsPart2|_HybridVentilationControlGlobalAN|CentralChillerHeaterSystem)"
-    release_build_cmake_extra_flags: -DPROFILE_GENERATE:BOOL=OFF -DPROFILE_USE:BOOL=ON -DENABLE_REGRESSION_TESTING:BOOL=ON -DBUILD_DOCS:BOOL=OFF
+    release_build_cmake_extra_flags: -DPROFILE_GENERATE:BOOL=OFF -DPROFILE_USE:BOOL=ON -DENABLE_REGRESSION_TESTING:BOOL=ON -DBUILD_DOCS:BOOL=ON
     cmake_extra_flags: -DBUILD_FORTRAN=ON -DBUILD_PACKAGE:BOOL=ON -DBUILD_TESTING:BOOL=ON -DENABLE_REGRESSION_TESTING:BOOL=ON -DREGRESSION_BASELINE_PATH:PATH=$REGRESSION_BASELINE -DREGRESSION_SCRIPT_PATH:PATH=$REGRESSION_DIR -DREGRESSION_BASELINE_SHA:STRING=$REGRESSION_BASELINE_SHA -DCOMMIT_SHA=$COMMIT_SHA -DENABLE_GTEST_DEBUG_MODE:BOOL=OFF -DBUILD_PERFORMANCE_TESTS:BOOL=ON -DVALGRIND_ANALYZE_PERFORMANCE_TESTS:BOOL=ON
     collect_performance_results: true
 
diff --git a/.decent_ci-MacOS.yaml b/.decent_ci-MacOS.yaml
index 3ed019232ad..2f65fcc8970 100644
--- a/.decent_ci-MacOS.yaml
+++ b/.decent_ci-MacOS.yaml
@@ -1,5 +1,5 @@
 compilers:
   - name: clang
-    release_build_cmake_extra_flags: -DENABLE_LTO:BOOL=ON -DBUILD_DOCS:BOOL=OFF
+    release_build_cmake_extra_flags: -DENABLE_LTO:BOOL=ON -DBUILD_DOCS:BOOL=ON
     cmake_extra_flags: -DBUILD_FORTRAN=ON -DBUILD_PACKAGE:BOOL=ON -DBUILD_TESTING:BOOL=ON -DENABLE_REGRESSION_TESTING:BOOL=ON -DREGRESSION_BASELINE_PATH:PATH=$REGRESSION_BASELINE -DREGRESSION_SCRIPT_PATH:PATH=$REGRESSION_DIR -DREGRESSION_BASELINE_SHA:STRING=$REGRESSION_BASELINE_SHA -DCOMMIT_SHA=$COMMIT_SHA -DENABLE_GTEST_DEBUG_MODE:BOOL=OFF -DBUILD_PYTHON_TESTS:BOOL=ON
 
diff --git a/.decent_ci-Windows.yaml b/.decent_ci-Windows.yaml
index f3a0c23ed15..a53d917a6a2 100644
--- a/.decent_ci-Windows.yaml
+++ b/.decent_ci-Windows.yaml
@@ -1,14 +1,12 @@
 compilers:
   - name: Visual Studio
     version: 12
-    release_build_enable_pgo: false
-    release_build_cmake_extra_flags: -DENABLE_LTO:BOOL=ON -DBUILD_DOCS:BOOL=OFF
+    release_build_cmake_extra_flags: -DBUILD_DOCS:BOOL=ON
     cmake_extra_flags: -DBUILD_FORTRAN:BOOL=ON -DBUILD_PACKAGE:BOOL=ON -DBUILD_TESTING:BOOL=ON -DENABLE_REGRESSION_TESTING:BOOL=ON -DREGRESSION_BASELINE_PATH:PATH=%REGRESSION_BASELINE% -DREGRESSION_SCRIPT_PATH:PATH=%REGRESSION_DIR% -DREGRESSION_BASELINE_SHA:STRING=%REGRESSION_BASELINE_SHA% -DCOMMIT_SHA=%COMMIT_SHA% -DENABLE_GTEST_DEBUG_MODE:BOOL=OFF -DBUILD_PYTHON_TESTS:BOOL=ON
   - name: Visual Studio
     version: 12
     architecture: Win64
-    release_build_enable_pgo: false
-    release_build_cmake_extra_flags: -DENABLE_LTO:BOOL=ON -DBUILD_DOCS:BOOL=OFF
+    release_build_cmake_extra_flags: -DBUILD_DOCS:BOOL=ON
     cmake_extra_flags: -DBUILD_FORTRAN:BOOL=ON -DBUILD_PACKAGE:BOOL=ON -DBUILD_TESTING:BOOL=ON -DENABLE_REGRESSION_TESTING:BOOL=ON -DREGRESSION_BASELINE_PATH:PATH=%REGRESSION_BASELINE% -DREGRESSION_SCRIPT_PATH:PATH=%REGRESSION_DIR% -DREGRESSION_BASELINE_SHA:STRING=%REGRESSION_BASELINE_SHA% -DCOMMIT_SHA=%COMMIT_SHA% -DENABLE_GTEST_DEBUG_MODE:BOOL=OFF -DBUILD_PYTHON_TESTS:BOOL=ON
 
 
diff --git a/.gitignore b/.gitignore
index cde64fca609..30695ce6e31 100644
--- a/.gitignore
+++ b/.gitignore
@@ -23,14 +23,6 @@
 # now that we have python, ignore some things
 *.pyc
 
-# ignore the site build folder for mkdocs
-doc/src/site*
-# and also ignore the concatenated markdown docs that are temporarily created for the pdf target
-doc/src/docs/EngineeringReference/EngRef.md
-doc/src/docs/InputOutputReference/IORef.md
-# and oddly enough we want to ignore the mkdocs yml file that is created conditionally depending on html vs pdf target
-doc/src/mkdocs.yml
-
 # build folder, if the dev chooses to put it there
 #  could also do a wildcard for build-* if we suggest that naming approach
 #  which could be useful for: build-eclipse, build-vs2013, build, etc.
@@ -45,3 +37,6 @@ Builds
 .cproject
 .idea
 .se
+
+# vim temp file:
+*.swp
diff --git a/CMakeLists.txt b/CMakeLists.txt
index 0c3bbd6f260..f9eb628f61b 100644
--- a/CMakeLists.txt
+++ b/CMakeLists.txt
@@ -58,15 +58,7 @@ option( BUILD_PACKAGE "Build package" OFF )
 option( BUILD_TESTING "Build testing targets" OFF )
 option( BUILD_FORTRAN "Build Fortran stuff" OFF )
 option( BUILD_VALIDATION_REPORTS "Build validation reports" OFF )
-option( BUILD_DOCS "Build markdown based documentation" OFF )
-
-if (BUILD_DOCS)
-  option( BUILD_MONOLITHIC_ENGINEERINGREFERENCE  "Build all-in-one EngineeringReference (has caveats)" ON )
-
-  if (BUILD_PACKAGE)
-    option( PACKAGE_BUILT_DOCS "Add built docs to package" OFF )
-  endif()
-endif()
+option( BUILD_DOCS "Build LaTeX-pdf documentation" OFF )
 
 # Turning ENABLE_GTEST_DEBUG_MODE ON will cause assertions and exceptions to halt the test case and unwind.
 # Turn this option OFF for automated testing.
@@ -130,18 +122,6 @@ set( CMAKE_LIBRARY_OUTPUT_DIRECTORY "${CMAKE_BINARY_DIR}/Products" )
 set( CMAKE_ARCHIVE_OUTPUT_DIRECTORY "${CMAKE_BINARY_DIR}/Products" )
 set( CMAKE_RUNTIME_OUTPUT_DIRECTORY "${CMAKE_BINARY_DIR}/Products" )
 
-# Advanced, time consuming compiler optimization options
-
-option(ENABLE_LTO "Enable link-time-optimization" FALSE)
-option(PROFILE_GENERATE "Generate profile data" FALSE)
-option(PROFILE_USE "Use profile data" FALSE)
-
-
-if (PROFILE_USE AND PROFILE_GENERATE)
-  message(SEND_ERROR "Cannot enable PROFILE_USE and PROFILE_GENERATE simultaneously")
-endif()
-
-
 include(cmake/ProjectMacros.cmake)
 include(cmake/CompilerFlags.cmake)
 
@@ -241,132 +221,6 @@ if( BUILD_PACKAGE )
   include(cmake/Install.cmake)
 endif()
 
-
-set(OPTIMIZABLE_TARGETS
-  sqlite objexx bcvtb epexpat epfmiimport miniziplib DElight energyplus energyplusapi energypluslib
-    )
-if(NOT APPLE AND NOT MSVC)
-  list(APPEND OPTIMIZABLE_TARGETS parser)
-endif()
-
-if(NOT MSVC)
-  list(APPEND OPTIMIZABLE_TARGETS objexx_tests energyplus_tests)
-endif()
-
-if(MSVC AND (PROFILE_GENERATE OR PROFILE_USE OR ENABLE_LTO) )
-  get_filename_component(LINKER_DIR "${CMAKE_LINKER}" PATH)
-  get_filename_component(LINKER_DIR_NAME "${LINKER_DIR}" NAME)
-
-  if (MSVC12)
-    set(PGORTVER "120")
-  elseif(MSVC14)
-    set(PGORTVER "140")
-  endif()
-
-  message("Examining ${LINKER_DIR_NAME} for PGO RT DLL")
-
-  if ("${LINKER_DIR_NAME}" MATCHES ".*amd64.*")
-    get_filename_component(LINKER_PARENT_DIR "${LINKER_DIR}" PATH)
-    set(PGORTDIR "${LINKER_PARENT_DIR}/amd64")
-    message("Retrieving amd64 PGO dll from: ${PGORTDIR}")
-  else()
-    set(PGORTDIR "${LINKER_DIR}")
-  endif()
-
-  file(COPY "${PGORTDIR}/pgort${PGORTVER}.dll" DESTINATION "${CMAKE_BINARY_DIR}/Products/Release" )
-
-  foreach(target ${OPTIMIZABLE_TARGETS})
-    get_target_property(targ_link_flags ${target} LINK_FLAGS)
-    get_target_property(targ_static_link_flags ${target} STATIC_LIBRARY_FLAGS)
-    get_target_property(targ_compile_flags ${target} COMPILE_FLAGS)
-
-    # message("${target}: ${targ_link_flags}; ${targ_static_link_flags}; ${targ_compile_flags}")
-    if(targ_link_flags STREQUAL "targ_link_flags-NOTFOUND")
-      set(targ_link_flags "")
-    endif()
-
-    if(targ_static_link_flags STREQUAL "targ_static_link_flags-NOTFOUND")
-      set(targ_static_link_flags "")
-    endif()
-
-    if(targ_compile_flags STREQUAL "targ_compile_flags-NOTFOUND")
-      set(targ_compile_flags "")
-    endif()
-
-    if (ENABLE_LTO OR PROFILE_GENERATE OR PROFILE_USE)
-      set(targ_compile_flags "${targ_compile_flags} /GL")
-    endif()
-
-    if(ENABLE_LTO AND NOT PROFILE_GENERATE AND NOT PROFILE_USE)
-      set(targ_link_flags "${targ_link_flags} /LTCG")
-      set(targ_static_link_flags "${targ_static_link_flags} /LTCG")
-    endif()
-
-    if (PROFILE_GENERATE)
-      set(targ_link_flags "${targ_link_flags} /LTCG:PGI")
-      set(targ_static_link_flags "${targ_static_link_flags} /LTCG")
-    endif()
-
-    if (PROFILE_USE)
-      set(targ_link_flags "${targ_link_flags} /LTCG:PGO")
-      set(targ_static_link_flags "${targ_static_link_flags} /LTCG")
-    endif()
-
-    set_target_properties(${target} PROPERTIES LINK_FLAGS "${targ_link_flags}" STATIC_LIBRARY_FLAGS "${targ_static_link_flags}"
-       COMPILE_FLAGS "${targ_compile_flags}")
-
-  endforeach()
-
-elseif (CMAKE_COMPILER_IS_GNUCXX)
-  if(ENABLE_LTO)
-    set_target_properties(${OPTIMIZABLE_TARGETS}
-      PROPERTIES LINK_FLAGS "-flto=7 -fno-use-linker-plugin" COMPILE_FLAGS "-flto=7 -fno-use-linker-plugin")
-    set_target_properties(energyplus
-      PROPERTIES LINK_FLAGS "-flto=7 -fuse-linker-plugin -fwhole-program" COMPILE_FLAGS "-flto=7 -fuse-linker-plugin -fwhole-program")
-  endif()
-
-  if (PROFILE_GENERATE)
-    set_target_properties(${OPTIMIZABLE_TARGETS} energyplus_tests TestEnergyPlusCallbacks
-      PROPERTIES LINK_FLAGS "-fprofile-generate"  COMPILE_FLAGS "-fprofile-generate")
-  endif()
-
-  if (PROFILE_USE)
-    set_target_properties(${OPTIMIZABLE_TARGETS}
-      PROPERTIES LINK_FLAGS "-fprofile-use"  COMPILE_FLAGS "-fprofile-use")
-  endif()
-
-  if (PROFILE_USE AND ENABLE_LTO)
-    set_target_properties(${OPTIMIZABLE_TARGETS}
-      PROPERTIES LINK_FLAGS "-flto=7 -fno-use-linker-plugin -fprofile-use" COMPILE_FLAGS "-flto=7 -fno-use-linker-plugin -fprofile-use")
-    set_target_properties(energyplus
-      PROPERTIES LINK_FLAGS "-flto=7 -fuse-linker-plugin -fwhole-program -fprofile-use" COMPILE_FLAGS "-flto=7 -fuse-linker-plugin -fwhole-program -fprofile-use")
-  endif()
-elseif ("${CMAKE_CXX_COMPILER_ID}" STREQUAL "Clang" ) # Clang
-  if(ENABLE_LTO)
-    set_target_properties(energyplus
-      PROPERTIES LINK_FLAGS "-flto" COMPILE_FLAGS "-flto")
-  endif()
-
-  if (PROFILE_GENERATE)
-    set_target_properties(${OPTIMIZABLE_TARGETS}
-      PROPERTIES LINK_FLAGS "-fprofile-instr-generate" COMPILE_FLAGS "-fprofile-instr-generate")
-  endif()
-
-  if (PROFILE_USE)
-    set_target_properties(${OPTIMIZABLE_TARGETS}
-      PROPERTIES LINK_FLAGS "-fprofile-instr-use=${CMAKE_BINARY_DIR}/profdata" COMPILE_FLAGS "-fprofile-instr-use=${CMAKE_BINARY_DIR}/profdata")
-  endif()
-
-  if (PROFILE_USE AND ENABLE_LTO)
-    set_target_properties(${OPTIMIZABLE_TARGETS}
-      PROPERTIES LINK_FLAGS "-flto -fprofile-instr-use=${CMAKE_BINARY_DIR}/profdata" COMPILE_FLAGS "-flto -fprofile-instr-use=${CMAKE_BINARY_DIR}/profdata")
-  endif()
-
-
-endif()
-
-
-
 if (BUILD_VALIDATION_REPORTS)
   include(ExternalProject)
   ExternalProject_Add(ValidationReports
@@ -380,7 +234,19 @@ if (BUILD_VALIDATION_REPORTS)
     )
 endif()
 
-
 if (BUILD_DOCS)
-  add_subdirectory(doc/src)
+  # this _should_ find the xelatex compiler, but for some reason it isn't populating for me
+  find_package(LATEX)
+  # so we'll create a cache variable which will be available to the add_subdirectory call below
+  set(XELATEX "XeLaTeX Compiler" CACHE INTERNAL "")
+  # and we'll simply take the found pdflatex compiler path and replace pdflatex with xelatex
+  string(REPLACE pdflatex xelatex XELATEX ${PDFLATEX_COMPILER})
+  # and then verify it actually exists at that location...which it should pretty much every time...
+  if( EXISTS ${XELATEX} )
+    # and if it does, just add the doc/CMakeLists commands
+    add_subdirectory(doc)
+  else()
+    # and if it doesn't, clearly state why it fails
+    message( FATAL_ERROR "Expected to find xelatex at: ${XELATEX} ; check your LaTeX installation")
+  endif()
 endif()
diff --git a/cmake/BuildDocumentation.cmake b/cmake/BuildDocumentation.cmake
new file mode 100644
index 00000000000..7799f8714ba
--- /dev/null
+++ b/cmake/BuildDocumentation.cmake
@@ -0,0 +1,12 @@
+# Caller needs to set:
+  # XELATEX, the path to the xelatex compiler
+  # INNAME, the name of the input tex file
+  # OUTNAME, the pretty output name for the pdf
+  # ORIGINAL_CMAKE_SOURCE_DIR, the root of the source repo
+  # ORIGINAL_CMAKE_BINARY_DIR, the root fo the build tree
+# this will get more complicated as we add things like bibtex and makeindex, for now just copy the files into the build tree, execute xelatex twice and rename the output
+#message("Hoping to copy from ${ORIGINAL_CMAKE_SOURCE_DIR}/doc/${INNAME} to ${ORIGINAL_CMAKE_BINARY_DIR}/doc-build/${INNAME}")
+execute_process( COMMAND cmake -E copy_directory ${ORIGINAL_CMAKE_SOURCE_DIR}/doc/${INNAME} ${ORIGINAL_CMAKE_BINARY_DIR}/doc-build/${INNAME})
+execute_process( COMMAND ${XELATEX} -interaction=nonstopmode ${INNAME}.tex )
+execute_process( COMMAND ${XELATEX} -interaction=nonstopmode ${INNAME}.tex )
+file( RENAME "${INNAME}.pdf" "../${OUTNAME}.pdf" )
diff --git a/cmake/CMakeCPackOptions.cmake.in b/cmake/CMakeCPackOptions.cmake.in
index 197b7cd2d95..9340582e463 100644
--- a/cmake/CMakeCPackOptions.cmake.in
+++ b/cmake/CMakeCPackOptions.cmake.in
@@ -213,6 +213,6 @@ if("${CPACK_GENERATOR}" STREQUAL "PackageMaker")
   set(CPACK_PACKAGE_RELOCATABLE false)
   set( CPACK_PACKAGE_VENDOR "usdoe" )
   configure_file(@CMAKE_SOURCE_DIR@/cmake/CPack.Info.plist.in.in "@CMAKE_BINARY_DIR@/Modules/CPack.Info.plist.in")
-  set(CPACK_RESOURCE_FILE_README "@CMAKE_BINARY_DIR@/install_temp/readme.html")
+  set(CPACK_RESOURCE_FILE_README "@CMAKE_SOURCE_DIR@/release/readme.html")
 endif()
 
diff --git a/cmake/Install.cmake b/cmake/Install.cmake
index d6c08a33108..df993b81ee1 100644
--- a/cmake/Install.cmake
+++ b/cmake/Install.cmake
@@ -56,14 +56,13 @@ install(FILES "${DOCS_OUT}/ExampleFiles-ObjectsLink.html" DESTINATION "./Example
 # Watch out! GITHUB_TOKEN could go out of scope by the time install target is run.
 # Better to move this condition into the install CODE.
 if(NOT "$ENV{GITHUB_TOKEN}" STREQUAL "")
-  install(CODE "execute_process(COMMAND \"${PYTHON_EXECUTABLE}\" \"${CMAKE_SOURCE_DIR}/doc/tools/create_changelog.py\" \"${CMAKE_SOURCE_DIR}\" \"${DOCS_OUT}/changelog.md\" \"${DOCS_OUT}/changelog.html\" \"${GIT_EXECUTABLE}\" \"$ENV{GITHUB_TOKEN}\" \"${PREV_RELEASE_SHA}\")")
+	install(CODE "execute_process(COMMAND \"${PYTHON_EXECUTABLE}\" \"${CMAKE_SOURCE_DIR}/doc/tools/create_changelog.py\" \"${CMAKE_SOURCE_DIR}\" \"${DOCS_OUT}/changelog.md\" \"${DOCS_OUT}/changelog.html\" \"${GIT_EXECUTABLE}\" \"$ENV{GITHUB_TOKEN}\" \"${PREV_RELEASE_SHA}\" \"${CPACK_PACKAGE_VERSION}\")")
   install(FILES "${DOCS_OUT}/changelog.html" DESTINATION "./" OPTIONAL)
 else()
   message(WARNING "No GITHUB_TOKEN found in environment; package won't be complete")
 endif()
 
 # Install files that are in the current repo
-INSTALL(FILES "${CMAKE_SOURCE_DIR}/doc/index.html" DESTINATION "./Documentation")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/AirCooledChiller.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/ASHRAE_2005_HOF_Materials.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/Boilers.idf" DESTINATION "./DataSets")
@@ -79,11 +78,11 @@ INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/FluidPropertiesRefData.idf" DESTINAT
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/FossilFuelEnvironmentalImpactFactors.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/GLHERefData.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/GlycolPropertiesRefData.idf" DESTINATION "./DataSets")
-INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/LCCusePriceEscalationDataSet2010.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/LCCusePriceEscalationDataSet2011.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/LCCusePriceEscalationDataSet2012.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/LCCusePriceEscalationDataSet2013.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/LCCusePriceEscalationDataSet2014.idf" DESTINATION "./DataSets")
+INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/LCCusePriceEscalationDataSet2015.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/MoistureMaterials.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/PerfCurves.idf" DESTINATION "./DataSets")
 INSTALL(FILES "${CMAKE_SOURCE_DIR}/datasets/PrecipitationSchedulesUSA.idf" DESTINATION "./DataSets")
@@ -392,30 +391,21 @@ configure_file("${CMAKE_SOURCE_DIR}/cmake/CMakeCPackOptions.cmake.in"
   "${CMAKE_BINARY_DIR}/CMakeCPackOptions.cmake" @ONLY)
 set(CPACK_PROJECT_CONFIG_FILE "${CMAKE_BINARY_DIR}/CMakeCPackOptions.cmake")
 
-
-
-
-if (NOT PACKAGE_BUILT_DOCS)
-  # remote files.  All of these should eventually be generated from content in the EnergyPlusTeam project.
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/Acknowledgements.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/AuxiliaryPrograms.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/EMS_Application_Guide.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/EngineeringReference.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/ExternalInterfaces_Application_Guide.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/GettingStarted.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/InputOutputReference.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/InterfaceDeveloper.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/ModuleDeveloper.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/OutputDetailsAndExamples.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/PlantApplicationGuide.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/Tips_and_Tricks_Using_EnergyPlus.pdf" "./Documentation")
-  install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/Using_EnergyPlus_for_Compliance.pdf" "./Documentation")
-
-  # Should this be included or no? There is no .md source for generating
-  #install_remote(FILES "https://raw.github.com/NREL/EnergyPlusBuildSupport/${BUILDSUPPORTREF}/docs/pdf/ProgrammingStandard.pdf" "./Documentation")
-endif()
-
-
+if ( BUILD_DOCS )
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/Acknowledgements.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/AuxiliaryPrograms.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/EMSApplicationGuide.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/EngineeringReference.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/ExternalInterfacesApplicationGuide.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/GettingStarted.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/InputOutputReference.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/InterfaceDeveloper.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/ModuleDeveloper.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/OutputDetailsAndExamples.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/PlantApplicationGuide.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/TipsAndTricksUsingEnergyPlus.pdf" DESTINATION "./Documentation")
+	install(FILES "${CMAKE_BINARY_DIR}/doc-build/UsingEnergyPlusForCompliance.pdf" DESTINATION "./Documentation")
+endif ()
 
 INCLUDE(CPack)
 
diff --git a/datasets/LCCusePriceEscalationDataSet2010.idf b/datasets/LCCusePriceEscalationDataSet2010.idf
deleted file mode 100644
index 3f0622ac1a7..00000000000
--- a/datasets/LCCusePriceEscalationDataSet2010.idf
+++ /dev/null
@@ -1,2547 +0,0 @@
-! The source of the values for the following objects is:
-!
-!    NISTIR 85-3273-25
-!
-!    ENERGY PRICE INDICES AND DISCOUNT FACTORS
-!    FOR LIFE-CYCLE COST ANALYSIS
-!
-!    Annual Supplement to NIST Handbook 135 and NBS Special Publication 709
-!
-!    April 1, 2010 to March 31, 2011
-!
-!    Data for the Federal Methodology for Life-Cycle Cost Analysis, Title 10, CFR, Part 436, Subpart A;
-!    and for the Energy Conservation Mandatory Performance Standards for New Federal Residential Buildings,
-!    Title 10, CFR, Part 435
-!
-!    Amy S. Rushing
-!    Joshua D. Kneifel
-!    Barbara C. Lippiatt
-!
-! These are factors for the United States and regions of the United States.
-!
-! The factors are from a file available upon request from NIST called ENCOSTxx.TXT and are
-! converted into EnergyPlus objects using a spreadsheet called ConvertENCOSTtoEnergyPlusLifeCycleCost.xls
-! which is available upon request.
-
-! The objects and syntax in this dataset comply with EnergyPlus, Version 8.4.0 and above, unless otherwise noted.
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Residential-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9374,                  !- Year 1 Escalation
-    0.9790,                  !- Year 2 Escalation
-    1.0138,                  !- Year 3 Escalation
-    1.0127,                  !- Year 4 Escalation
-    1.0096,                  !- Year 5 Escalation
-    1.0177,                  !- Year 6 Escalation
-    1.0279,                  !- Year 7 Escalation
-    1.0334,                  !- Year 8 Escalation
-    1.0327,                  !- Year 9 Escalation
-    1.0382,                  !- Year 10 Escalation
-    1.0454,                  !- Year 11 Escalation
-    1.0494,                  !- Year 12 Escalation
-    1.0564,                  !- Year 13 Escalation
-    1.0587,                  !- Year 14 Escalation
-    1.0549,                  !- Year 15 Escalation
-    1.0566,                  !- Year 16 Escalation
-    1.0630,                  !- Year 17 Escalation
-    1.0707,                  !- Year 18 Escalation
-    1.0857,                  !- Year 19 Escalation
-    1.0953,                  !- Year 20 Escalation
-    1.1063,                  !- Year 21 Escalation
-    1.1165,                  !- Year 22 Escalation
-    1.1227,                  !- Year 23 Escalation
-    1.1292,                  !- Year 24 Escalation
-    1.1349,                  !- Year 25 Escalation
-    1.1414,                  !- Year 26 Escalation
-    1.1480,                  !- Year 27 Escalation
-    1.1550,                  !- Year 28 Escalation
-    1.1617,                  !- Year 29 Escalation
-    1.1686;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Residential-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0022,                  !- Year 1 Escalation
-    1.0503,                  !- Year 2 Escalation
-    1.1083,                  !- Year 3 Escalation
-    1.1530,                  !- Year 4 Escalation
-    1.1843,                  !- Year 5 Escalation
-    1.2312,                  !- Year 6 Escalation
-    1.2714,                  !- Year 7 Escalation
-    1.3076,                  !- Year 8 Escalation
-    1.3350,                  !- Year 9 Escalation
-    1.3562,                  !- Year 10 Escalation
-    1.3668,                  !- Year 11 Escalation
-    1.3774,                  !- Year 12 Escalation
-    1.3936,                  !- Year 13 Escalation
-    1.4054,                  !- Year 14 Escalation
-    1.4204,                  !- Year 15 Escalation
-    1.4355,                  !- Year 16 Escalation
-    1.4484,                  !- Year 17 Escalation
-    1.4645,                  !- Year 18 Escalation
-    1.4858,                  !- Year 19 Escalation
-    1.4980,                  !- Year 20 Escalation
-    1.5187,                  !- Year 21 Escalation
-    1.5410,                  !- Year 22 Escalation
-    1.5623,                  !- Year 23 Escalation
-    1.5851,                  !- Year 24 Escalation
-    1.6086,                  !- Year 25 Escalation
-    1.6276,                  !- Year 26 Escalation
-    1.6460,                  !- Year 27 Escalation
-    1.6639,                  !- Year 28 Escalation
-    1.6823,                  !- Year 29 Escalation
-    1.7013;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Residential-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0451,                  !- Year 1 Escalation
-    1.0736,                  !- Year 2 Escalation
-    1.0562,                  !- Year 3 Escalation
-    1.0396,                  !- Year 4 Escalation
-    1.0419,                  !- Year 5 Escalation
-    1.0459,                  !- Year 6 Escalation
-    1.0475,                  !- Year 7 Escalation
-    1.0498,                  !- Year 8 Escalation
-    1.0538,                  !- Year 9 Escalation
-    1.0601,                  !- Year 10 Escalation
-    1.0696,                  !- Year 11 Escalation
-    1.0839,                  !- Year 12 Escalation
-    1.0934,                  !- Year 13 Escalation
-    1.0949,                  !- Year 14 Escalation
-    1.1005,                  !- Year 15 Escalation
-    1.1108,                  !- Year 16 Escalation
-    1.1242,                  !- Year 17 Escalation
-    1.1416,                  !- Year 18 Escalation
-    1.1630,                  !- Year 19 Escalation
-    1.1851,                  !- Year 20 Escalation
-    1.2104,                  !- Year 21 Escalation
-    1.2271,                  !- Year 22 Escalation
-    1.2358,                  !- Year 23 Escalation
-    1.2508,                  !- Year 24 Escalation
-    1.2627,                  !- Year 25 Escalation
-    1.2737,                  !- Year 26 Escalation
-    1.2856,                  !- Year 27 Escalation
-    1.2983,                  !- Year 28 Escalation
-    1.3109,                  !- Year 29 Escalation
-    1.3244;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Residential-LPG,  !- Name
-    PropaneGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9884,                  !- Year 1 Escalation
-    1.0207,                  !- Year 2 Escalation
-    1.0640,                  !- Year 3 Escalation
-    1.1015,                  !- Year 4 Escalation
-    1.1262,                  !- Year 5 Escalation
-    1.1491,                  !- Year 6 Escalation
-    1.1695,                  !- Year 7 Escalation
-    1.1898,                  !- Year 8 Escalation
-    1.2022,                  !- Year 9 Escalation
-    1.2109,                  !- Year 10 Escalation
-    1.2193,                  !- Year 11 Escalation
-    1.2269,                  !- Year 12 Escalation
-    1.2364,                  !- Year 13 Escalation
-    1.2462,                  !- Year 14 Escalation
-    1.2556,                  !- Year 15 Escalation
-    1.2618,                  !- Year 16 Escalation
-    1.2709,                  !- Year 17 Escalation
-    1.2800,                  !- Year 18 Escalation
-    1.2920,                  !- Year 19 Escalation
-    1.3011,                  !- Year 20 Escalation
-    1.3127,                  !- Year 21 Escalation
-    1.3251,                  !- Year 22 Escalation
-    1.3385,                  !- Year 23 Escalation
-    1.3520,                  !- Year 24 Escalation
-    1.3658,                  !- Year 25 Escalation
-    1.3782,                  !- Year 26 Escalation
-    1.3898,                  !- Year 27 Escalation
-    1.4018,                  !- Year 28 Escalation
-    1.4138,                  !- Year 29 Escalation
-    1.4258;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Commercial-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.8973,                  !- Year 1 Escalation
-    0.9195,                  !- Year 2 Escalation
-    0.9398,                  !- Year 3 Escalation
-    0.9253,                  !- Year 4 Escalation
-    0.9212,                  !- Year 5 Escalation
-    0.9317,                  !- Year 6 Escalation
-    0.9450,                  !- Year 7 Escalation
-    0.9545,                  !- Year 8 Escalation
-    0.9578,                  !- Year 9 Escalation
-    0.9670,                  !- Year 10 Escalation
-    0.9792,                  !- Year 11 Escalation
-    0.9881,                  !- Year 12 Escalation
-    1.0014,                  !- Year 13 Escalation
-    1.0094,                  !- Year 14 Escalation
-    1.0061,                  !- Year 15 Escalation
-    1.0094,                  !- Year 16 Escalation
-    1.0175,                  !- Year 17 Escalation
-    1.0280,                  !- Year 18 Escalation
-    1.0491,                  !- Year 19 Escalation
-    1.0647,                  !- Year 20 Escalation
-    1.0841,                  !- Year 21 Escalation
-    1.1030,                  !- Year 22 Escalation
-    1.1157,                  !- Year 23 Escalation
-    1.1279,                  !- Year 24 Escalation
-    1.1391,                  !- Year 25 Escalation
-    1.1465,                  !- Year 26 Escalation
-    1.1535,                  !- Year 27 Escalation
-    1.1601,                  !- Year 28 Escalation
-    1.1671,                  !- Year 29 Escalation
-    1.1740;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Commercial-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0110,                  !- Year 1 Escalation
-    1.0699,                  !- Year 2 Escalation
-    1.1372,                  !- Year 3 Escalation
-    1.1890,                  !- Year 4 Escalation
-    1.2317,                  !- Year 5 Escalation
-    1.2854,                  !- Year 6 Escalation
-    1.3301,                  !- Year 7 Escalation
-    1.3722,                  !- Year 8 Escalation
-    1.4039,                  !- Year 9 Escalation
-    1.4291,                  !- Year 10 Escalation
-    1.4434,                  !- Year 11 Escalation
-    1.4595,                  !- Year 12 Escalation
-    1.4764,                  !- Year 13 Escalation
-    1.4867,                  !- Year 14 Escalation
-    1.5036,                  !- Year 15 Escalation
-    1.5204,                  !- Year 16 Escalation
-    1.5359,                  !- Year 17 Escalation
-    1.5553,                  !- Year 18 Escalation
-    1.5806,                  !- Year 19 Escalation
-    1.5942,                  !- Year 20 Escalation
-    1.6175,                  !- Year 21 Escalation
-    1.6440,                  !- Year 22 Escalation
-    1.6686,                  !- Year 23 Escalation
-    1.6945,                  !- Year 24 Escalation
-    1.7210,                  !- Year 25 Escalation
-    1.7437,                  !- Year 26 Escalation
-    1.7644,                  !- Year 27 Escalation
-    1.7858,                  !- Year 28 Escalation
-    1.8071,                  !- Year 29 Escalation
-    1.8291;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Commercial-Residual Oil,  !- Name
-    FuelOil#2,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0022,                  !- Year 1 Escalation
-    1.1020,                  !- Year 2 Escalation
-    1.2278,                  !- Year 3 Escalation
-    1.3243,                  !- Year 4 Escalation
-    1.3742,                  !- Year 5 Escalation
-    1.4306,                  !- Year 6 Escalation
-    1.4859,                  !- Year 7 Escalation
-    1.5412,                  !- Year 8 Escalation
-    1.6030,                  !- Year 9 Escalation
-    1.6367,                  !- Year 10 Escalation
-    1.6605,                  !- Year 11 Escalation
-    1.6833,                  !- Year 12 Escalation
-    1.7072,                  !- Year 13 Escalation
-    1.7310,                  !- Year 14 Escalation
-    1.7538,                  !- Year 15 Escalation
-    1.7657,                  !- Year 16 Escalation
-    1.7842,                  !- Year 17 Escalation
-    1.8080,                  !- Year 18 Escalation
-    1.8319,                  !- Year 19 Escalation
-    1.8579,                  !- Year 20 Escalation
-    1.8937,                  !- Year 21 Escalation
-    1.9208,                  !- Year 22 Escalation
-    1.9360,                  !- Year 23 Escalation
-    1.9761,                  !- Year 24 Escalation
-    1.9989,                  !- Year 25 Escalation
-    2.0293,                  !- Year 26 Escalation
-    2.0640,                  !- Year 27 Escalation
-    2.0998,                  !- Year 28 Escalation
-    2.1356,                  !- Year 29 Escalation
-    2.1725;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Commercial-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0703,                  !- Year 1 Escalation
-    1.1280,                  !- Year 2 Escalation
-    1.1301,                  !- Year 3 Escalation
-    1.1123,                  !- Year 4 Escalation
-    1.1133,                  !- Year 5 Escalation
-    1.1186,                  !- Year 6 Escalation
-    1.1175,                  !- Year 7 Escalation
-    1.1196,                  !- Year 8 Escalation
-    1.1238,                  !- Year 9 Escalation
-    1.1312,                  !- Year 10 Escalation
-    1.1406,                  !- Year 11 Escalation
-    1.1584,                  !- Year 12 Escalation
-    1.1700,                  !- Year 13 Escalation
-    1.1721,                  !- Year 14 Escalation
-    1.1763,                  !- Year 15 Escalation
-    1.1889,                  !- Year 16 Escalation
-    1.2036,                  !- Year 17 Escalation
-    1.2246,                  !- Year 18 Escalation
-    1.2497,                  !- Year 19 Escalation
-    1.2760,                  !- Year 20 Escalation
-    1.3075,                  !- Year 21 Escalation
-    1.3263,                  !- Year 22 Escalation
-    1.3347,                  !- Year 23 Escalation
-    1.3515,                  !- Year 24 Escalation
-    1.3641,                  !- Year 25 Escalation
-    1.3778,                  !- Year 26 Escalation
-    1.3945,                  !- Year 27 Escalation
-    1.4113,                  !- Year 28 Escalation
-    1.4281,                  !- Year 29 Escalation
-    1.4449;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Commercial-Coal,  !- Name
-    Coal,                    !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9807,                  !- Year 1 Escalation
-    0.9807,                  !- Year 2 Escalation
-    0.9768,                  !- Year 3 Escalation
-    0.9807,                  !- Year 4 Escalation
-    0.9768,                  !- Year 5 Escalation
-    0.9691,                  !- Year 6 Escalation
-    0.9653,                  !- Year 7 Escalation
-    0.9614,                  !- Year 8 Escalation
-    0.9537,                  !- Year 9 Escalation
-    0.9498,                  !- Year 10 Escalation
-    0.9421,                  !- Year 11 Escalation
-    0.9459,                  !- Year 12 Escalation
-    0.9498,                  !- Year 13 Escalation
-    0.9537,                  !- Year 14 Escalation
-    0.9498,                  !- Year 15 Escalation
-    0.9537,                  !- Year 16 Escalation
-    0.9498,                  !- Year 17 Escalation
-    0.9537,                  !- Year 18 Escalation
-    0.9575,                  !- Year 19 Escalation
-    0.9653,                  !- Year 20 Escalation
-    0.9653,                  !- Year 21 Escalation
-    0.9653,                  !- Year 22 Escalation
-    0.9691,                  !- Year 23 Escalation
-    0.9730,                  !- Year 24 Escalation
-    0.9768,                  !- Year 25 Escalation
-    0.9807,                  !- Year 26 Escalation
-    0.9846,                  !- Year 27 Escalation
-    0.9846,                  !- Year 28 Escalation
-    0.9884,                  !- Year 29 Escalation
-    0.9923;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Industrial-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.8501,                  !- Year 1 Escalation
-    0.8774,                  !- Year 2 Escalation
-    0.9010,                  !- Year 3 Escalation
-    0.8745,                  !- Year 4 Escalation
-    0.8660,                  !- Year 5 Escalation
-    0.8811,                  !- Year 6 Escalation
-    0.8957,                  !- Year 7 Escalation
-    0.9055,                  !- Year 8 Escalation
-    0.9071,                  !- Year 9 Escalation
-    0.9169,                  !- Year 10 Escalation
-    0.9308,                  !- Year 11 Escalation
-    0.9413,                  !- Year 12 Escalation
-    0.9576,                  !- Year 13 Escalation
-    0.9690,                  !- Year 14 Escalation
-    0.9658,                  !- Year 15 Escalation
-    0.9695,                  !- Year 16 Escalation
-    0.9813,                  !- Year 17 Escalation
-    0.9959,                  !- Year 18 Escalation
-    1.0220,                  !- Year 19 Escalation
-    1.0420,                  !- Year 20 Escalation
-    1.0644,                  !- Year 21 Escalation
-    1.0859,                  !- Year 22 Escalation
-    1.0998,                  !- Year 23 Escalation
-    1.1136,                  !- Year 24 Escalation
-    1.1259,                  !- Year 25 Escalation
-    1.1336,                  !- Year 26 Escalation
-    1.1401,                  !- Year 27 Escalation
-    1.1466,                  !- Year 28 Escalation
-    1.1536,                  !- Year 29 Escalation
-    1.1601;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Industrial-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0268,                  !- Year 1 Escalation
-    1.0955,                  !- Year 2 Escalation
-    1.1642,                  !- Year 3 Escalation
-    1.2165,                  !- Year 4 Escalation
-    1.2642,                  !- Year 5 Escalation
-    1.3198,                  !- Year 6 Escalation
-    1.3643,                  !- Year 7 Escalation
-    1.4061,                  !- Year 8 Escalation
-    1.4395,                  !- Year 9 Escalation
-    1.4650,                  !- Year 10 Escalation
-    1.4820,                  !- Year 11 Escalation
-    1.5016,                  !- Year 12 Escalation
-    1.5173,                  !- Year 13 Escalation
-    1.5258,                  !- Year 14 Escalation
-    1.5422,                  !- Year 15 Escalation
-    1.5598,                  !- Year 16 Escalation
-    1.5755,                  !- Year 17 Escalation
-    1.5958,                  !- Year 18 Escalation
-    1.6213,                  !- Year 19 Escalation
-    1.6364,                  !- Year 20 Escalation
-    1.6599,                  !- Year 21 Escalation
-    1.6867,                  !- Year 22 Escalation
-    1.7116,                  !- Year 23 Escalation
-    1.7377,                  !- Year 24 Escalation
-    1.7652,                  !- Year 25 Escalation
-    1.7881,                  !- Year 26 Escalation
-    1.8090,                  !- Year 27 Escalation
-    1.8306,                  !- Year 28 Escalation
-    1.8522,                  !- Year 29 Escalation
-    1.8744;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Industrial-Residual Oil,  !- Name
-    FuelOil#2,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0120,                  !- Year 1 Escalation
-    1.1034,                  !- Year 2 Escalation
-    1.2199,                  !- Year 3 Escalation
-    1.3092,                  !- Year 4 Escalation
-    1.3554,                  !- Year 5 Escalation
-    1.4076,                  !- Year 6 Escalation
-    1.4588,                  !- Year 7 Escalation
-    1.5100,                  !- Year 8 Escalation
-    1.5673,                  !- Year 9 Escalation
-    1.5984,                  !- Year 10 Escalation
-    1.6205,                  !- Year 11 Escalation
-    1.6416,                  !- Year 12 Escalation
-    1.6647,                  !- Year 13 Escalation
-    1.6867,                  !- Year 14 Escalation
-    1.7078,                  !- Year 15 Escalation
-    1.7189,                  !- Year 16 Escalation
-    1.7349,                  !- Year 17 Escalation
-    1.7580,                  !- Year 18 Escalation
-    1.7801,                  !- Year 19 Escalation
-    1.8042,                  !- Year 20 Escalation
-    1.8373,                  !- Year 21 Escalation
-    1.8624,                  !- Year 22 Escalation
-    1.8765,                  !- Year 23 Escalation
-    1.9137,                  !- Year 24 Escalation
-    1.9347,                  !- Year 25 Escalation
-    1.9629,                  !- Year 26 Escalation
-    1.9950,                  !- Year 27 Escalation
-    2.0281,                  !- Year 28 Escalation
-    2.0612,                  !- Year 29 Escalation
-    2.0954;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Industrial-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.1582,                  !- Year 1 Escalation
-    1.2677,                  !- Year 2 Escalation
-    1.2845,                  !- Year 3 Escalation
-    1.2576,                  !- Year 4 Escalation
-    1.2576,                  !- Year 5 Escalation
-    1.2626,                  !- Year 6 Escalation
-    1.2593,                  !- Year 7 Escalation
-    1.2593,                  !- Year 8 Escalation
-    1.2643,                  !- Year 9 Escalation
-    1.2727,                  !- Year 10 Escalation
-    1.2862,                  !- Year 11 Escalation
-    1.3114,                  !- Year 12 Escalation
-    1.3283,                  !- Year 13 Escalation
-    1.3316,                  !- Year 14 Escalation
-    1.3384,                  !- Year 15 Escalation
-    1.3552,                  !- Year 16 Escalation
-    1.3771,                  !- Year 17 Escalation
-    1.4091,                  !- Year 18 Escalation
-    1.4461,                  !- Year 19 Escalation
-    1.4848,                  !- Year 20 Escalation
-    1.5337,                  !- Year 21 Escalation
-    1.5640,                  !- Year 22 Escalation
-    1.5758,                  !- Year 23 Escalation
-    1.5993,                  !- Year 24 Escalation
-    1.6162,                  !- Year 25 Escalation
-    1.6380,                  !- Year 26 Escalation
-    1.6650,                  !- Year 27 Escalation
-    1.6919,                  !- Year 28 Escalation
-    1.7189,                  !- Year 29 Escalation
-    1.7458;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    NorthEast  Industrial-Coal,  !- Name
-    Coal,                    !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9862,                  !- Year 1 Escalation
-    0.9862,                  !- Year 2 Escalation
-    0.9758,                  !- Year 3 Escalation
-    0.9758,                  !- Year 4 Escalation
-    0.9723,                  !- Year 5 Escalation
-    0.9654,                  !- Year 6 Escalation
-    0.9654,                  !- Year 7 Escalation
-    0.9585,                  !- Year 8 Escalation
-    0.9550,                  !- Year 9 Escalation
-    0.9516,                  !- Year 10 Escalation
-    0.9481,                  !- Year 11 Escalation
-    0.9516,                  !- Year 12 Escalation
-    0.9516,                  !- Year 13 Escalation
-    0.9516,                  !- Year 14 Escalation
-    0.9481,                  !- Year 15 Escalation
-    0.9516,                  !- Year 16 Escalation
-    0.9481,                  !- Year 17 Escalation
-    0.9516,                  !- Year 18 Escalation
-    0.9585,                  !- Year 19 Escalation
-    0.9585,                  !- Year 20 Escalation
-    0.9619,                  !- Year 21 Escalation
-    0.9619,                  !- Year 22 Escalation
-    0.9654,                  !- Year 23 Escalation
-    0.9689,                  !- Year 24 Escalation
-    0.9723,                  !- Year 25 Escalation
-    0.9758,                  !- Year 26 Escalation
-    0.9758,                  !- Year 27 Escalation
-    0.9792,                  !- Year 28 Escalation
-    0.9827,                  !- Year 29 Escalation
-    0.9827;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Residential-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9579,                  !- Year 1 Escalation
-    0.9684,                  !- Year 2 Escalation
-    0.9831,                  !- Year 3 Escalation
-    0.9917,                  !- Year 4 Escalation
-    0.9950,                  !- Year 5 Escalation
-    1.0022,                  !- Year 6 Escalation
-    1.0047,                  !- Year 7 Escalation
-    1.0036,                  !- Year 8 Escalation
-    1.0025,                  !- Year 9 Escalation
-    1.0054,                  !- Year 10 Escalation
-    1.0104,                  !- Year 11 Escalation
-    1.0140,                  !- Year 12 Escalation
-    1.0176,                  !- Year 13 Escalation
-    1.0223,                  !- Year 14 Escalation
-    1.0201,                  !- Year 15 Escalation
-    1.0173,                  !- Year 16 Escalation
-    1.0176,                  !- Year 17 Escalation
-    1.0194,                  !- Year 18 Escalation
-    1.0245,                  !- Year 19 Escalation
-    1.0320,                  !- Year 20 Escalation
-    1.0374,                  !- Year 21 Escalation
-    1.0435,                  !- Year 22 Escalation
-    1.0460,                  !- Year 23 Escalation
-    1.0525,                  !- Year 24 Escalation
-    1.0601,                  !- Year 25 Escalation
-    1.0644,                  !- Year 26 Escalation
-    1.0683,                  !- Year 27 Escalation
-    1.0723,                  !- Year 28 Escalation
-    1.0759,                  !- Year 29 Escalation
-    1.0798;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Residential-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9810,                  !- Year 1 Escalation
-    1.0324,                  !- Year 2 Escalation
-    1.0985,                  !- Year 3 Escalation
-    1.1450,                  !- Year 4 Escalation
-    1.1786,                  !- Year 5 Escalation
-    1.2294,                  !- Year 6 Escalation
-    1.2734,                  !- Year 7 Escalation
-    1.3125,                  !- Year 8 Escalation
-    1.3413,                  !- Year 9 Escalation
-    1.3639,                  !- Year 10 Escalation
-    1.3755,                  !- Year 11 Escalation
-    1.3872,                  !- Year 12 Escalation
-    1.4037,                  !- Year 13 Escalation
-    1.4171,                  !- Year 14 Escalation
-    1.4330,                  !- Year 15 Escalation
-    1.4495,                  !- Year 16 Escalation
-    1.4630,                  !- Year 17 Escalation
-    1.4801,                  !- Year 18 Escalation
-    1.5034,                  !- Year 19 Escalation
-    1.5162,                  !- Year 20 Escalation
-    1.5382,                  !- Year 21 Escalation
-    1.5627,                  !- Year 22 Escalation
-    1.5847,                  !- Year 23 Escalation
-    1.6092,                  !- Year 24 Escalation
-    1.6349,                  !- Year 25 Escalation
-    1.6557,                  !- Year 26 Escalation
-    1.6752,                  !- Year 27 Escalation
-    1.6954,                  !- Year 28 Escalation
-    1.7156,                  !- Year 29 Escalation
-    1.7358;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Residential-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0494,                  !- Year 1 Escalation
-    1.0766,                  !- Year 2 Escalation
-    1.0524,                  !- Year 3 Escalation
-    1.0393,                  !- Year 4 Escalation
-    1.0484,                  !- Year 5 Escalation
-    1.0585,                  !- Year 6 Escalation
-    1.0625,                  !- Year 7 Escalation
-    1.0675,                  !- Year 8 Escalation
-    1.0746,                  !- Year 9 Escalation
-    1.0847,                  !- Year 10 Escalation
-    1.0968,                  !- Year 11 Escalation
-    1.1159,                  !- Year 12 Escalation
-    1.1240,                  !- Year 13 Escalation
-    1.1200,                  !- Year 14 Escalation
-    1.1230,                  !- Year 15 Escalation
-    1.1371,                  !- Year 16 Escalation
-    1.1563,                  !- Year 17 Escalation
-    1.1804,                  !- Year 18 Escalation
-    1.2056,                  !- Year 19 Escalation
-    1.2339,                  !- Year 20 Escalation
-    1.2661,                  !- Year 21 Escalation
-    1.2853,                  !- Year 22 Escalation
-    1.2954,                  !- Year 23 Escalation
-    1.3135,                  !- Year 24 Escalation
-    1.3317,                  !- Year 25 Escalation
-    1.3478,                  !- Year 26 Escalation
-    1.3639,                  !- Year 27 Escalation
-    1.3800,                  !- Year 28 Escalation
-    1.3962,                  !- Year 29 Escalation
-    1.4133;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Residential-LPG,!- Name
-    PropaneGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9981,                  !- Year 1 Escalation
-    1.0410,                  !- Year 2 Escalation
-    1.0987,                  !- Year 3 Escalation
-    1.1478,                  !- Year 4 Escalation
-    1.1806,                  !- Year 5 Escalation
-    1.2112,                  !- Year 6 Escalation
-    1.2383,                  !- Year 7 Escalation
-    1.2660,                  !- Year 8 Escalation
-    1.2822,                  !- Year 9 Escalation
-    1.2941,                  !- Year 10 Escalation
-    1.3055,                  !- Year 11 Escalation
-    1.3160,                  !- Year 12 Escalation
-    1.3284,                  !- Year 13 Escalation
-    1.3413,                  !- Year 14 Escalation
-    1.3541,                  !- Year 15 Escalation
-    1.3632,                  !- Year 16 Escalation
-    1.3751,                  !- Year 17 Escalation
-    1.3875,                  !- Year 18 Escalation
-    1.4032,                  !- Year 19 Escalation
-    1.4156,                  !- Year 20 Escalation
-    1.4314,                  !- Year 21 Escalation
-    1.4476,                  !- Year 22 Escalation
-    1.4657,                  !- Year 23 Escalation
-    1.4838,                  !- Year 24 Escalation
-    1.5019,                  !- Year 25 Escalation
-    1.5181,                  !- Year 26 Escalation
-    1.5334,                  !- Year 27 Escalation
-    1.5491,                  !- Year 28 Escalation
-    1.5648,                  !- Year 29 Escalation
-    1.5810;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Commercial-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9341,                  !- Year 1 Escalation
-    0.9321,                  !- Year 2 Escalation
-    0.9369,                  !- Year 3 Escalation
-    0.9369,                  !- Year 4 Escalation
-    0.9422,                  !- Year 5 Escalation
-    0.9538,                  !- Year 6 Escalation
-    0.9590,                  !- Year 7 Escalation
-    0.9598,                  !- Year 8 Escalation
-    0.9618,                  !- Year 9 Escalation
-    0.9683,                  !- Year 10 Escalation
-    0.9775,                  !- Year 11 Escalation
-    0.9851,                  !- Year 12 Escalation
-    0.9944,                  !- Year 13 Escalation
-    1.0068,                  !- Year 14 Escalation
-    1.0076,                  !- Year 15 Escalation
-    1.0084,                  !- Year 16 Escalation
-    1.0120,                  !- Year 17 Escalation
-    1.0165,                  !- Year 18 Escalation
-    1.0253,                  !- Year 19 Escalation
-    1.0369,                  !- Year 20 Escalation
-    1.0458,                  !- Year 21 Escalation
-    1.0562,                  !- Year 22 Escalation
-    1.0627,                  !- Year 23 Escalation
-    1.0735,                  !- Year 24 Escalation
-    1.0835,                  !- Year 25 Escalation
-    1.0920,                  !- Year 26 Escalation
-    1.1004,                  !- Year 27 Escalation
-    1.1088,                  !- Year 28 Escalation
-    1.1169,                  !- Year 29 Escalation
-    1.1253;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Commercial-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9946,                  !- Year 1 Escalation
-    1.0566,                  !- Year 2 Escalation
-    1.1295,                  !- Year 3 Escalation
-    1.1827,                  !- Year 4 Escalation
-    1.2266,                  !- Year 5 Escalation
-    1.2825,                  !- Year 6 Escalation
-    1.3291,                  !- Year 7 Escalation
-    1.3722,                  !- Year 8 Escalation
-    1.4039,                  !- Year 9 Escalation
-    1.4289,                  !- Year 10 Escalation
-    1.4437,                  !- Year 11 Escalation
-    1.4599,                  !- Year 12 Escalation
-    1.4774,                  !- Year 13 Escalation
-    1.4882,                  !- Year 14 Escalation
-    1.5051,                  !- Year 15 Escalation
-    1.5233,                  !- Year 16 Escalation
-    1.5381,                  !- Year 17 Escalation
-    1.5583,                  !- Year 18 Escalation
-    1.5846,                  !- Year 19 Escalation
-    1.5988,                  !- Year 20 Escalation
-    1.6231,                  !- Year 21 Escalation
-    1.6500,                  !- Year 22 Escalation
-    1.6757,                  !- Year 23 Escalation
-    1.7026,                  !- Year 24 Escalation
-    1.7316,                  !- Year 25 Escalation
-    1.7552,                  !- Year 26 Escalation
-    1.7768,                  !- Year 27 Escalation
-    1.7991,                  !- Year 28 Escalation
-    1.8213,                  !- Year 29 Escalation
-    1.8442;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Commercial-Residual Oil,  !- Name
-    FuelOil#2,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0955,                  !- Year 1 Escalation
-    1.1499,                  !- Year 2 Escalation
-    1.2192,                  !- Year 3 Escalation
-    1.2782,                  !- Year 4 Escalation
-    1.3132,                  !- Year 5 Escalation
-    1.3460,                  !- Year 6 Escalation
-    1.3758,                  !- Year 7 Escalation
-    1.4072,                  !- Year 8 Escalation
-    1.4228,                  !- Year 9 Escalation
-    1.4295,                  !- Year 10 Escalation
-    1.4437,                  !- Year 11 Escalation
-    1.4579,                  !- Year 12 Escalation
-    1.4720,                  !- Year 13 Escalation
-    1.4870,                  !- Year 14 Escalation
-    1.5019,                  !- Year 15 Escalation
-    1.5093,                  !- Year 16 Escalation
-    1.5213,                  !- Year 17 Escalation
-    1.5377,                  !- Year 18 Escalation
-    1.5570,                  !- Year 19 Escalation
-    1.5794,                  !- Year 20 Escalation
-    1.6033,                  !- Year 21 Escalation
-    1.6249,                  !- Year 22 Escalation
-    1.6473,                  !- Year 23 Escalation
-    1.6696,                  !- Year 24 Escalation
-    1.6928,                  !- Year 25 Escalation
-    1.7166,                  !- Year 26 Escalation
-    1.7405,                  !- Year 27 Escalation
-    1.7651,                  !- Year 28 Escalation
-    1.7897,                  !- Year 29 Escalation
-    1.8151;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Commercial-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0788,                  !- Year 1 Escalation
-    1.1404,                  !- Year 2 Escalation
-    1.1404,                  !- Year 3 Escalation
-    1.1318,                  !- Year 4 Escalation
-    1.1429,                  !- Year 5 Escalation
-    1.1539,                  !- Year 6 Escalation
-    1.1576,                  !- Year 7 Escalation
-    1.1626,                  !- Year 8 Escalation
-    1.1700,                  !- Year 9 Escalation
-    1.1823,                  !- Year 10 Escalation
-    1.1958,                  !- Year 11 Escalation
-    1.2167,                  !- Year 12 Escalation
-    1.2266,                  !- Year 13 Escalation
-    1.2217,                  !- Year 14 Escalation
-    1.2241,                  !- Year 15 Escalation
-    1.2401,                  !- Year 16 Escalation
-    1.2623,                  !- Year 17 Escalation
-    1.2919,                  !- Year 18 Escalation
-    1.3202,                  !- Year 19 Escalation
-    1.3522,                  !- Year 20 Escalation
-    1.3916,                  !- Year 21 Escalation
-    1.4138,                  !- Year 22 Escalation
-    1.4249,                  !- Year 23 Escalation
-    1.4458,                  !- Year 24 Escalation
-    1.4680,                  !- Year 25 Escalation
-    1.4865,                  !- Year 26 Escalation
-    1.5062,                  !- Year 27 Escalation
-    1.5259,                  !- Year 28 Escalation
-    1.5456,                  !- Year 29 Escalation
-    1.5665;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Commercial-Coal,!- Name
-    Coal,                    !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0067,                  !- Year 1 Escalation
-    1.0201,                  !- Year 2 Escalation
-    1.0134,                  !- Year 3 Escalation
-    1.0234,                  !- Year 4 Escalation
-    1.0301,                  !- Year 5 Escalation
-    1.0234,                  !- Year 6 Escalation
-    1.0268,                  !- Year 7 Escalation
-    1.0234,                  !- Year 8 Escalation
-    1.0134,                  !- Year 9 Escalation
-    1.0067,                  !- Year 10 Escalation
-    1.0000,                  !- Year 11 Escalation
-    1.0000,                  !- Year 12 Escalation
-    0.9967,                  !- Year 13 Escalation
-    0.9967,                  !- Year 14 Escalation
-    0.9900,                  !- Year 15 Escalation
-    0.9967,                  !- Year 16 Escalation
-    0.9933,                  !- Year 17 Escalation
-    0.9967,                  !- Year 18 Escalation
-    0.9967,                  !- Year 19 Escalation
-    1.0000,                  !- Year 20 Escalation
-    1.0033,                  !- Year 21 Escalation
-    1.0067,                  !- Year 22 Escalation
-    1.0100,                  !- Year 23 Escalation
-    1.0134,                  !- Year 24 Escalation
-    1.0201,                  !- Year 25 Escalation
-    1.0234,                  !- Year 26 Escalation
-    1.0268,                  !- Year 27 Escalation
-    1.0268,                  !- Year 28 Escalation
-    1.0301,                  !- Year 29 Escalation
-    1.0334;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Industrial-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.8930,                  !- Year 1 Escalation
-    0.8843,                  !- Year 2 Escalation
-    0.8849,                  !- Year 3 Escalation
-    0.8751,                  !- Year 4 Escalation
-    0.8768,                  !- Year 5 Escalation
-    0.8913,                  !- Year 6 Escalation
-    0.8982,                  !- Year 7 Escalation
-    0.8994,                  !- Year 8 Escalation
-    0.9011,                  !- Year 9 Escalation
-    0.9075,                  !- Year 10 Escalation
-    0.9173,                  !- Year 11 Escalation
-    0.9260,                  !- Year 12 Escalation
-    0.9370,                  !- Year 13 Escalation
-    0.9497,                  !- Year 14 Escalation
-    0.9503,                  !- Year 15 Escalation
-    0.9503,                  !- Year 16 Escalation
-    0.9555,                  !- Year 17 Escalation
-    0.9636,                  !- Year 18 Escalation
-    0.9757,                  !- Year 19 Escalation
-    0.9890,                  !- Year 20 Escalation
-    1.0006,                  !- Year 21 Escalation
-    1.0133,                  !- Year 22 Escalation
-    1.0208,                  !- Year 23 Escalation
-    1.0335,                  !- Year 24 Escalation
-    1.0463,                  !- Year 25 Escalation
-    1.0567,                  !- Year 26 Escalation
-    1.0665,                  !- Year 27 Escalation
-    1.0769,                  !- Year 28 Escalation
-    1.0868,                  !- Year 29 Escalation
-    1.0972;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Industrial-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0106,                  !- Year 1 Escalation
-    1.0809,                  !- Year 2 Escalation
-    1.1532,                  !- Year 3 Escalation
-    1.2069,                  !- Year 4 Escalation
-    1.2546,                  !- Year 5 Escalation
-    1.3110,                  !- Year 6 Escalation
-    1.3554,                  !- Year 7 Escalation
-    1.3979,                  !- Year 8 Escalation
-    1.4290,                  !- Year 9 Escalation
-    1.4542,                  !- Year 10 Escalation
-    1.4695,                  !- Year 11 Escalation
-    1.4894,                  !- Year 12 Escalation
-    1.5046,                  !- Year 13 Escalation
-    1.5133,                  !- Year 14 Escalation
-    1.5298,                  !- Year 15 Escalation
-    1.5477,                  !- Year 16 Escalation
-    1.5630,                  !- Year 17 Escalation
-    1.5836,                  !- Year 18 Escalation
-    1.6094,                  !- Year 19 Escalation
-    1.6240,                  !- Year 20 Escalation
-    1.6472,                  !- Year 21 Escalation
-    1.6744,                  !- Year 22 Escalation
-    1.7003,                  !- Year 23 Escalation
-    1.7275,                  !- Year 24 Escalation
-    1.7573,                  !- Year 25 Escalation
-    1.7805,                  !- Year 26 Escalation
-    1.8017,                  !- Year 27 Escalation
-    1.8236,                  !- Year 28 Escalation
-    1.8455,                  !- Year 29 Escalation
-    1.8674;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Industrial-Residual Oil,  !- Name
-    FuelOil#2,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.1075,                  !- Year 1 Escalation
-    1.1646,                  !- Year 2 Escalation
-    1.2363,                  !- Year 3 Escalation
-    1.2957,                  !- Year 4 Escalation
-    1.3316,                  !- Year 5 Escalation
-    1.3651,                  !- Year 6 Escalation
-    1.3956,                  !- Year 7 Escalation
-    1.4276,                  !- Year 8 Escalation
-    1.4436,                  !- Year 9 Escalation
-    1.4505,                  !- Year 10 Escalation
-    1.4657,                  !- Year 11 Escalation
-    1.4794,                  !- Year 12 Escalation
-    1.4939,                  !- Year 13 Escalation
-    1.5099,                  !- Year 14 Escalation
-    1.5252,                  !- Year 15 Escalation
-    1.5328,                  !- Year 16 Escalation
-    1.5450,                  !- Year 17 Escalation
-    1.5617,                  !- Year 18 Escalation
-    1.5816,                  !- Year 19 Escalation
-    1.6044,                  !- Year 20 Escalation
-    1.6296,                  !- Year 21 Escalation
-    1.6509,                  !- Year 22 Escalation
-    1.6738,                  !- Year 23 Escalation
-    1.6966,                  !- Year 24 Escalation
-    1.7203,                  !- Year 25 Escalation
-    1.7447,                  !- Year 26 Escalation
-    1.7698,                  !- Year 27 Escalation
-    1.7950,                  !- Year 28 Escalation
-    1.8201,                  !- Year 29 Escalation
-    1.8453;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Industrial-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.2028,                  !- Year 1 Escalation
-    1.3248,                  !- Year 2 Escalation
-    1.3465,                  !- Year 3 Escalation
-    1.3366,                  !- Year 4 Escalation
-    1.3524,                  !- Year 5 Escalation
-    1.3661,                  !- Year 6 Escalation
-    1.3701,                  !- Year 7 Escalation
-    1.3760,                  !- Year 8 Escalation
-    1.3858,                  !- Year 9 Escalation
-    1.3996,                  !- Year 10 Escalation
-    1.4154,                  !- Year 11 Escalation
-    1.4449,                  !- Year 12 Escalation
-    1.4567,                  !- Year 13 Escalation
-    1.4429,                  !- Year 14 Escalation
-    1.4449,                  !- Year 15 Escalation
-    1.4705,                  !- Year 16 Escalation
-    1.5039,                  !- Year 17 Escalation
-    1.5453,                  !- Year 18 Escalation
-    1.5866,                  !- Year 19 Escalation
-    1.6339,                  !- Year 20 Escalation
-    1.6890,                  !- Year 21 Escalation
-    1.7244,                  !- Year 22 Escalation
-    1.7382,                  !- Year 23 Escalation
-    1.7697,                  !- Year 24 Escalation
-    1.7992,                  !- Year 25 Escalation
-    1.8307,                  !- Year 26 Escalation
-    1.8602,                  !- Year 27 Escalation
-    1.8917,                  !- Year 28 Escalation
-    1.9232,                  !- Year 29 Escalation
-    1.9567;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    MidWest  Industrial-Coal,!- Name
-    Coal,                    !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9913,                  !- Year 1 Escalation
-    0.9957,                  !- Year 2 Escalation
-    0.9913,                  !- Year 3 Escalation
-    1.0043,                  !- Year 4 Escalation
-    1.0173,                  !- Year 5 Escalation
-    1.0260,                  !- Year 6 Escalation
-    1.0303,                  !- Year 7 Escalation
-    1.0346,                  !- Year 8 Escalation
-    1.0303,                  !- Year 9 Escalation
-    1.0260,                  !- Year 10 Escalation
-    1.0173,                  !- Year 11 Escalation
-    1.0173,                  !- Year 12 Escalation
-    1.0087,                  !- Year 13 Escalation
-    1.0043,                  !- Year 14 Escalation
-    1.0043,                  !- Year 15 Escalation
-    1.0087,                  !- Year 16 Escalation
-    1.0043,                  !- Year 17 Escalation
-    1.0087,                  !- Year 18 Escalation
-    1.0130,                  !- Year 19 Escalation
-    1.0173,                  !- Year 20 Escalation
-    1.0216,                  !- Year 21 Escalation
-    1.0216,                  !- Year 22 Escalation
-    1.0260,                  !- Year 23 Escalation
-    1.0303,                  !- Year 24 Escalation
-    1.0346,                  !- Year 25 Escalation
-    1.0433,                  !- Year 26 Escalation
-    1.0476,                  !- Year 27 Escalation
-    1.0476,                  !- Year 28 Escalation
-    1.0519,                  !- Year 29 Escalation
-    1.0563;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Residential-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9602,                  !- Year 1 Escalation
-    0.9784,                  !- Year 2 Escalation
-    0.9960,                  !- Year 3 Escalation
-    0.9983,                  !- Year 4 Escalation
-    0.9970,                  !- Year 5 Escalation
-    1.0030,                  !- Year 6 Escalation
-    1.0109,                  !- Year 7 Escalation
-    1.0123,                  !- Year 8 Escalation
-    1.0083,                  !- Year 9 Escalation
-    1.0106,                  !- Year 10 Escalation
-    1.0146,                  !- Year 11 Escalation
-    1.0163,                  !- Year 12 Escalation
-    1.0186,                  !- Year 13 Escalation
-    1.0232,                  !- Year 14 Escalation
-    1.0259,                  !- Year 15 Escalation
-    1.0295,                  !- Year 16 Escalation
-    1.0348,                  !- Year 17 Escalation
-    1.0398,                  !- Year 18 Escalation
-    1.0524,                  !- Year 19 Escalation
-    1.0657,                  !- Year 20 Escalation
-    1.0790,                  !- Year 21 Escalation
-    1.0906,                  !- Year 22 Escalation
-    1.0975,                  !- Year 23 Escalation
-    1.1042,                  !- Year 24 Escalation
-    1.1115,                  !- Year 25 Escalation
-    1.1188,                  !- Year 26 Escalation
-    1.1257,                  !- Year 27 Escalation
-    1.1330,                  !- Year 28 Escalation
-    1.1403,                  !- Year 29 Escalation
-    1.1476;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Residential-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9964,                  !- Year 1 Escalation
-    1.0456,                  !- Year 2 Escalation
-    1.1067,                  !- Year 3 Escalation
-    1.1529,                  !- Year 4 Escalation
-    1.1849,                  !- Year 5 Escalation
-    1.2336,                  !- Year 6 Escalation
-    1.2750,                  !- Year 7 Escalation
-    1.3136,                  !- Year 8 Escalation
-    1.3420,                  !- Year 9 Escalation
-    1.3640,                  !- Year 10 Escalation
-    1.3752,                  !- Year 11 Escalation
-    1.3865,                  !- Year 12 Escalation
-    1.4037,                  !- Year 13 Escalation
-    1.4161,                  !- Year 14 Escalation
-    1.4321,                  !- Year 15 Escalation
-    1.4481,                  !- Year 16 Escalation
-    1.4618,                  !- Year 17 Escalation
-    1.4784,                  !- Year 18 Escalation
-    1.5015,                  !- Year 19 Escalation
-    1.5139,                  !- Year 20 Escalation
-    1.5359,                  !- Year 21 Escalation
-    1.5596,                  !- Year 22 Escalation
-    1.5827,                  !- Year 23 Escalation
-    1.6070,                  !- Year 24 Escalation
-    1.6307,                  !- Year 25 Escalation
-    1.6509,                  !- Year 26 Escalation
-    1.6704,                  !- Year 27 Escalation
-    1.6900,                  !- Year 28 Escalation
-    1.7095,                  !- Year 29 Escalation
-    1.7291;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Residential-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0451,                  !- Year 1 Escalation
-    1.0731,                  !- Year 2 Escalation
-    1.0519,                  !- Year 3 Escalation
-    1.0451,                  !- Year 4 Escalation
-    1.0578,                  !- Year 5 Escalation
-    1.0680,                  !- Year 6 Escalation
-    1.0714,                  !- Year 7 Escalation
-    1.0748,                  !- Year 8 Escalation
-    1.0799,                  !- Year 9 Escalation
-    1.0893,                  !- Year 10 Escalation
-    1.1020,                  !- Year 11 Escalation
-    1.1190,                  !- Year 12 Escalation
-    1.1327,                  !- Year 13 Escalation
-    1.1395,                  !- Year 14 Escalation
-    1.1463,                  !- Year 15 Escalation
-    1.1565,                  !- Year 16 Escalation
-    1.1675,                  !- Year 17 Escalation
-    1.1871,                  !- Year 18 Escalation
-    1.2117,                  !- Year 19 Escalation
-    1.2381,                  !- Year 20 Escalation
-    1.2687,                  !- Year 21 Escalation
-    1.2849,                  !- Year 22 Escalation
-    1.2908,                  !- Year 23 Escalation
-    1.3044,                  !- Year 24 Escalation
-    1.3172,                  !- Year 25 Escalation
-    1.3299,                  !- Year 26 Escalation
-    1.3427,                  !- Year 27 Escalation
-    1.3563,                  !- Year 28 Escalation
-    1.3699,                  !- Year 29 Escalation
-    1.3844;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Residential-LPG,  !- Name
-    PropaneGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9947,                  !- Year 1 Escalation
-    1.0282,                  !- Year 2 Escalation
-    1.0738,                  !- Year 3 Escalation
-    1.1130,                  !- Year 4 Escalation
-    1.1385,                  !- Year 5 Escalation
-    1.1625,                  !- Year 6 Escalation
-    1.1838,                  !- Year 7 Escalation
-    1.2055,                  !- Year 8 Escalation
-    1.2184,                  !- Year 9 Escalation
-    1.2272,                  !- Year 10 Escalation
-    1.2359,                  !- Year 11 Escalation
-    1.2443,                  !- Year 12 Escalation
-    1.2538,                  !- Year 13 Escalation
-    1.2641,                  !- Year 14 Escalation
-    1.2740,                  !- Year 15 Escalation
-    1.2808,                  !- Year 16 Escalation
-    1.2900,                  !- Year 17 Escalation
-    1.2998,                  !- Year 18 Escalation
-    1.3120,                  !- Year 19 Escalation
-    1.3215,                  !- Year 20 Escalation
-    1.3341,                  !- Year 21 Escalation
-    1.3470,                  !- Year 22 Escalation
-    1.3607,                  !- Year 23 Escalation
-    1.3748,                  !- Year 24 Escalation
-    1.3893,                  !- Year 25 Escalation
-    1.4022,                  !- Year 26 Escalation
-    1.4144,                  !- Year 27 Escalation
-    1.4269,                  !- Year 28 Escalation
-    1.4395,                  !- Year 29 Escalation
-    1.4521;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Commercial-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9393,                  !- Year 1 Escalation
-    0.9518,                  !- Year 2 Escalation
-    0.9638,                  !- Year 3 Escalation
-    0.9572,                  !- Year 4 Escalation
-    0.9549,                  !- Year 5 Escalation
-    0.9646,                  !- Year 6 Escalation
-    0.9751,                  !- Year 7 Escalation
-    0.9782,                  !- Year 8 Escalation
-    0.9755,                  !- Year 9 Escalation
-    0.9802,                  !- Year 10 Escalation
-    0.9864,                  !- Year 11 Escalation
-    0.9895,                  !- Year 12 Escalation
-    0.9942,                  !- Year 13 Escalation
-    1.0023,                  !- Year 14 Escalation
-    1.0062,                  !- Year 15 Escalation
-    1.0109,                  !- Year 16 Escalation
-    1.0183,                  !- Year 17 Escalation
-    1.0264,                  !- Year 18 Escalation
-    1.0424,                  !- Year 19 Escalation
-    1.0579,                  !- Year 20 Escalation
-    1.0735,                  !- Year 21 Escalation
-    1.0886,                  !- Year 22 Escalation
-    1.0976,                  !- Year 23 Escalation
-    1.1065,                  !- Year 24 Escalation
-    1.1151,                  !- Year 25 Escalation
-    1.1248,                  !- Year 26 Escalation
-    1.1345,                  !- Year 27 Escalation
-    1.1442,                  !- Year 28 Escalation
-    1.1544,                  !- Year 29 Escalation
-    1.1641;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Commercial-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0007,                  !- Year 1 Escalation
-    1.0634,                  !- Year 2 Escalation
-    1.1352,                  !- Year 3 Escalation
-    1.1895,                  !- Year 4 Escalation
-    1.2348,                  !- Year 5 Escalation
-    1.2927,                  !- Year 6 Escalation
-    1.3401,                  !- Year 7 Escalation
-    1.3847,                  !- Year 8 Escalation
-    1.4174,                  !- Year 9 Escalation
-    1.4439,                  !- Year 10 Escalation
-    1.4592,                  !- Year 11 Escalation
-    1.4760,                  !- Year 12 Escalation
-    1.4941,                  !- Year 13 Escalation
-    1.5052,                  !- Year 14 Escalation
-    1.5233,                  !- Year 15 Escalation
-    1.5415,                  !- Year 16 Escalation
-    1.5575,                  !- Year 17 Escalation
-    1.5784,                  !- Year 18 Escalation
-    1.6056,                  !- Year 19 Escalation
-    1.6209,                  !- Year 20 Escalation
-    1.6453,                  !- Year 21 Escalation
-    1.6739,                  !- Year 22 Escalation
-    1.7010,                  !- Year 23 Escalation
-    1.7296,                  !- Year 24 Escalation
-    1.7589,                  !- Year 25 Escalation
-    1.7833,                  !- Year 26 Escalation
-    1.8056,                  !- Year 27 Escalation
-    1.8286,                  !- Year 28 Escalation
-    1.8516,                  !- Year 29 Escalation
-    1.8746;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Commercial-Residual Oil,  !- Name
-    FuelOil#2,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.1442,                  !- Year 1 Escalation
-    1.1992,                  !- Year 2 Escalation
-    1.2679,                  !- Year 3 Escalation
-    1.3260,                  !- Year 4 Escalation
-    1.3623,                  !- Year 5 Escalation
-    1.3955,                  !- Year 6 Escalation
-    1.4257,                  !- Year 7 Escalation
-    1.4574,                  !- Year 8 Escalation
-    1.4732,                  !- Year 9 Escalation
-    1.4800,                  !- Year 10 Escalation
-    1.4951,                  !- Year 11 Escalation
-    1.5094,                  !- Year 12 Escalation
-    1.5230,                  !- Year 13 Escalation
-    1.5389,                  !- Year 14 Escalation
-    1.5540,                  !- Year 15 Escalation
-    1.5615,                  !- Year 16 Escalation
-    1.5736,                  !- Year 17 Escalation
-    1.5902,                  !- Year 18 Escalation
-    1.6098,                  !- Year 19 Escalation
-    1.6325,                  !- Year 20 Escalation
-    1.6574,                  !- Year 21 Escalation
-    1.6785,                  !- Year 22 Escalation
-    1.7011,                  !- Year 23 Escalation
-    1.7238,                  !- Year 24 Escalation
-    1.7472,                  !- Year 25 Escalation
-    1.7713,                  !- Year 26 Escalation
-    1.7962,                  !- Year 27 Escalation
-    1.8211,                  !- Year 28 Escalation
-    1.8460,                  !- Year 29 Escalation
-    1.8709;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Commercial-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0795,                  !- Year 1 Escalation
-    1.1433,                  !- Year 2 Escalation
-    1.1422,                  !- Year 3 Escalation
-    1.1389,                  !- Year 4 Escalation
-    1.1568,                  !- Year 5 Escalation
-    1.1702,                  !- Year 6 Escalation
-    1.1736,                  !- Year 7 Escalation
-    1.1769,                  !- Year 8 Escalation
-    1.1837,                  !- Year 9 Escalation
-    1.1971,                  !- Year 10 Escalation
-    1.2116,                  !- Year 11 Escalation
-    1.2340,                  !- Year 12 Escalation
-    1.2520,                  !- Year 13 Escalation
-    1.2609,                  !- Year 14 Escalation
-    1.2676,                  !- Year 15 Escalation
-    1.2811,                  !- Year 16 Escalation
-    1.2945,                  !- Year 17 Escalation
-    1.3191,                  !- Year 18 Escalation
-    1.3483,                  !- Year 19 Escalation
-    1.3796,                  !- Year 20 Escalation
-    1.4166,                  !- Year 21 Escalation
-    1.4367,                  !- Year 22 Escalation
-    1.4412,                  !- Year 23 Escalation
-    1.4569,                  !- Year 24 Escalation
-    1.4726,                  !- Year 25 Escalation
-    1.4882,                  !- Year 26 Escalation
-    1.5062,                  !- Year 27 Escalation
-    1.5241,                  !- Year 28 Escalation
-    1.5420,                  !- Year 29 Escalation
-    1.5610;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Commercial-Coal,  !- Name
-    Coal,                    !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9606,                  !- Year 1 Escalation
-    0.9333,                  !- Year 2 Escalation
-    0.9152,                  !- Year 3 Escalation
-    0.9061,                  !- Year 4 Escalation
-    0.8848,                  !- Year 5 Escalation
-    0.8697,                  !- Year 6 Escalation
-    0.8636,                  !- Year 7 Escalation
-    0.8576,                  !- Year 8 Escalation
-    0.8515,                  !- Year 9 Escalation
-    0.8485,                  !- Year 10 Escalation
-    0.8424,                  !- Year 11 Escalation
-    0.8424,                  !- Year 12 Escalation
-    0.8364,                  !- Year 13 Escalation
-    0.8333,                  !- Year 14 Escalation
-    0.8303,                  !- Year 15 Escalation
-    0.8333,                  !- Year 16 Escalation
-    0.8273,                  !- Year 17 Escalation
-    0.8303,                  !- Year 18 Escalation
-    0.8333,                  !- Year 19 Escalation
-    0.8364,                  !- Year 20 Escalation
-    0.8394,                  !- Year 21 Escalation
-    0.8394,                  !- Year 22 Escalation
-    0.8424,                  !- Year 23 Escalation
-    0.8485,                  !- Year 24 Escalation
-    0.8455,                  !- Year 25 Escalation
-    0.8485,                  !- Year 26 Escalation
-    0.8485,                  !- Year 27 Escalation
-    0.8515,                  !- Year 28 Escalation
-    0.8545,                  !- Year 29 Escalation
-    0.8545;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Industrial-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9061,                  !- Year 1 Escalation
-    0.8993,                  !- Year 2 Escalation
-    0.9004,                  !- Year 3 Escalation
-    0.8895,                  !- Year 4 Escalation
-    0.8869,                  !- Year 5 Escalation
-    0.8983,                  !- Year 6 Escalation
-    0.9102,                  !- Year 7 Escalation
-    0.9133,                  !- Year 8 Escalation
-    0.9113,                  !- Year 9 Escalation
-    0.9170,                  !- Year 10 Escalation
-    0.9232,                  !- Year 11 Escalation
-    0.9284,                  !- Year 12 Escalation
-    0.9351,                  !- Year 13 Escalation
-    0.9445,                  !- Year 14 Escalation
-    0.9486,                  !- Year 15 Escalation
-    0.9538,                  !- Year 16 Escalation
-    0.9621,                  !- Year 17 Escalation
-    0.9720,                  !- Year 18 Escalation
-    0.9896,                  !- Year 19 Escalation
-    1.0078,                  !- Year 20 Escalation
-    1.0254,                  !- Year 21 Escalation
-    1.0415,                  !- Year 22 Escalation
-    1.0519,                  !- Year 23 Escalation
-    1.0623,                  !- Year 24 Escalation
-    1.0716,                  !- Year 25 Escalation
-    1.0825,                  !- Year 26 Escalation
-    1.0939,                  !- Year 27 Escalation
-    1.1053,                  !- Year 28 Escalation
-    1.1168,                  !- Year 29 Escalation
-    1.1287;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Industrial-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0227,                  !- Year 1 Escalation
-    1.0949,                  !- Year 2 Escalation
-    1.1671,                  !- Year 3 Escalation
-    1.2221,                  !- Year 4 Escalation
-    1.2717,                  !- Year 5 Escalation
-    1.3294,                  !- Year 6 Escalation
-    1.3755,                  !- Year 7 Escalation
-    1.4195,                  !- Year 8 Escalation
-    1.4519,                  !- Year 9 Escalation
-    1.4787,                  !- Year 10 Escalation
-    1.4938,                  !- Year 11 Escalation
-    1.5144,                  !- Year 12 Escalation
-    1.5309,                  !- Year 13 Escalation
-    1.5399,                  !- Year 14 Escalation
-    1.5571,                  !- Year 15 Escalation
-    1.5757,                  !- Year 16 Escalation
-    1.5922,                  !- Year 17 Escalation
-    1.6135,                  !- Year 18 Escalation
-    1.6403,                  !- Year 19 Escalation
-    1.6554,                  !- Year 20 Escalation
-    1.6802,                  !- Year 21 Escalation
-    1.7077,                  !- Year 22 Escalation
-    1.7352,                  !- Year 23 Escalation
-    1.7641,                  !- Year 24 Escalation
-    1.7944,                  !- Year 25 Escalation
-    1.8184,                  !- Year 26 Escalation
-    1.8404,                  !- Year 27 Escalation
-    1.8631,                  !- Year 28 Escalation
-    1.8858,                  !- Year 29 Escalation
-    1.9092;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Industrial-Residual Oil,  !- Name
-    FuelOil#2,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.1042,                  !- Year 1 Escalation
-    1.1612,                  !- Year 2 Escalation
-    1.2312,                  !- Year 3 Escalation
-    1.2905,                  !- Year 4 Escalation
-    1.3262,                  !- Year 5 Escalation
-    1.3589,                  !- Year 6 Escalation
-    1.3894,                  !- Year 7 Escalation
-    1.4213,                  !- Year 8 Escalation
-    1.4373,                  !- Year 9 Escalation
-    1.4441,                  !- Year 10 Escalation
-    1.4593,                  !- Year 11 Escalation
-    1.4730,                  !- Year 12 Escalation
-    1.4875,                  !- Year 13 Escalation
-    1.5034,                  !- Year 14 Escalation
-    1.5186,                  !- Year 15 Escalation
-    1.5255,                  !- Year 16 Escalation
-    1.5384,                  !- Year 17 Escalation
-    1.5551,                  !- Year 18 Escalation
-    1.5749,                  !- Year 19 Escalation
-    1.5970,                  !- Year 20 Escalation
-    1.6221,                  !- Year 21 Escalation
-    1.6441,                  !- Year 22 Escalation
-    1.6662,                  !- Year 23 Escalation
-    1.6890,                  !- Year 24 Escalation
-    1.7125,                  !- Year 25 Escalation
-    1.7369,                  !- Year 26 Escalation
-    1.7620,                  !- Year 27 Escalation
-    1.7871,                  !- Year 28 Escalation
-    1.8122,                  !- Year 29 Escalation
-    1.8373;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Industrial-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.2372,                  !- Year 1 Escalation
-    1.3888,                  !- Year 2 Escalation
-    1.4083,                  !- Year 3 Escalation
-    1.4034,                  !- Year 4 Escalation
-    1.4377,                  !- Year 5 Escalation
-    1.4621,                  !- Year 6 Escalation
-    1.4621,                  !- Year 7 Escalation
-    1.4645,                  !- Year 8 Escalation
-    1.4743,                  !- Year 9 Escalation
-    1.4963,                  !- Year 10 Escalation
-    1.5208,                  !- Year 11 Escalation
-    1.5648,                  !- Year 12 Escalation
-    1.5990,                  !- Year 13 Escalation
-    1.6161,                  !- Year 14 Escalation
-    1.6235,                  !- Year 15 Escalation
-    1.6430,                  !- Year 16 Escalation
-    1.6675,                  !- Year 17 Escalation
-    1.7139,                  !- Year 18 Escalation
-    1.7702,                  !- Year 19 Escalation
-    1.8337,                  !- Year 20 Escalation
-    1.9095,                  !- Year 21 Escalation
-    1.9438,                  !- Year 22 Escalation
-    1.9438,                  !- Year 23 Escalation
-    1.9731,                  !- Year 24 Escalation
-    2.0073,                  !- Year 25 Escalation
-    2.0416,                  !- Year 26 Escalation
-    2.0807,                  !- Year 27 Escalation
-    2.1198,                  !- Year 28 Escalation
-    2.1589,                  !- Year 29 Escalation
-    2.1980;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    South  Industrial-Coal,  !- Name
-    Coal,                    !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9905,                  !- Year 1 Escalation
-    0.9810,                  !- Year 2 Escalation
-    0.9652,                  !- Year 3 Escalation
-    0.9620,                  !- Year 4 Escalation
-    0.9620,                  !- Year 5 Escalation
-    0.9557,                  !- Year 6 Escalation
-    0.9557,                  !- Year 7 Escalation
-    0.9494,                  !- Year 8 Escalation
-    0.9462,                  !- Year 9 Escalation
-    0.9430,                  !- Year 10 Escalation
-    0.9399,                  !- Year 11 Escalation
-    0.9399,                  !- Year 12 Escalation
-    0.9335,                  !- Year 13 Escalation
-    0.9335,                  !- Year 14 Escalation
-    0.9304,                  !- Year 15 Escalation
-    0.9335,                  !- Year 16 Escalation
-    0.9304,                  !- Year 17 Escalation
-    0.9335,                  !- Year 18 Escalation
-    0.9367,                  !- Year 19 Escalation
-    0.9399,                  !- Year 20 Escalation
-    0.9430,                  !- Year 21 Escalation
-    0.9430,                  !- Year 22 Escalation
-    0.9462,                  !- Year 23 Escalation
-    0.9525,                  !- Year 24 Escalation
-    0.9494,                  !- Year 25 Escalation
-    0.9525,                  !- Year 26 Escalation
-    0.9557,                  !- Year 27 Escalation
-    0.9589,                  !- Year 28 Escalation
-    0.9589,                  !- Year 29 Escalation
-    0.9620;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Residential-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0042,                  !- Year 1 Escalation
-    1.0172,                  !- Year 2 Escalation
-    1.0299,                  !- Year 3 Escalation
-    1.0371,                  !- Year 4 Escalation
-    1.0342,                  !- Year 5 Escalation
-    1.0303,                  !- Year 6 Escalation
-    1.0280,                  !- Year 7 Escalation
-    1.0241,                  !- Year 8 Escalation
-    1.0215,                  !- Year 9 Escalation
-    1.0254,                  !- Year 10 Escalation
-    1.0316,                  !- Year 11 Escalation
-    1.0364,                  !- Year 12 Escalation
-    1.0397,                  !- Year 13 Escalation
-    1.0358,                  !- Year 14 Escalation
-    1.0358,                  !- Year 15 Escalation
-    1.0442,                  !- Year 16 Escalation
-    1.0540,                  !- Year 17 Escalation
-    1.0608,                  !- Year 18 Escalation
-    1.0696,                  !- Year 19 Escalation
-    1.0804,                  !- Year 20 Escalation
-    1.0917,                  !- Year 21 Escalation
-    1.1015,                  !- Year 22 Escalation
-    1.1083,                  !- Year 23 Escalation
-    1.1161,                  !- Year 24 Escalation
-    1.1233,                  !- Year 25 Escalation
-    1.1304,                  !- Year 26 Escalation
-    1.1373,                  !- Year 27 Escalation
-    1.1441,                  !- Year 28 Escalation
-    1.1513,                  !- Year 29 Escalation
-    1.1581;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Residential-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9923,                  !- Year 1 Escalation
-    1.0816,                  !- Year 2 Escalation
-    1.1548,                  !- Year 3 Escalation
-    1.2021,                  !- Year 4 Escalation
-    1.2193,                  !- Year 5 Escalation
-    1.2305,                  !- Year 6 Escalation
-    1.2790,                  !- Year 7 Escalation
-    1.3180,                  !- Year 8 Escalation
-    1.3392,                  !- Year 9 Escalation
-    1.3481,                  !- Year 10 Escalation
-    1.3617,                  !- Year 11 Escalation
-    1.3676,                  !- Year 12 Escalation
-    1.3830,                  !- Year 13 Escalation
-    1.3972,                  !- Year 14 Escalation
-    1.4090,                  !- Year 15 Escalation
-    1.4184,                  !- Year 16 Escalation
-    1.4415,                  !- Year 17 Escalation
-    1.4616,                  !- Year 18 Escalation
-    1.4823,                  !- Year 19 Escalation
-    1.5047,                  !- Year 20 Escalation
-    1.5319,                  !- Year 21 Escalation
-    1.5591,                  !- Year 22 Escalation
-    1.5644,                  !- Year 23 Escalation
-    1.5816,                  !- Year 24 Escalation
-    1.6164,                  !- Year 25 Escalation
-    1.6407,                  !- Year 26 Escalation
-    1.6596,                  !- Year 27 Escalation
-    1.6791,                  !- Year 28 Escalation
-    1.6986,                  !- Year 29 Escalation
-    1.7181;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Residential-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0521,                  !- Year 1 Escalation
-    1.0758,                  !- Year 2 Escalation
-    1.0370,                  !- Year 3 Escalation
-    1.0209,                  !- Year 4 Escalation
-    1.0313,                  !- Year 5 Escalation
-    1.0455,                  !- Year 6 Escalation
-    1.0559,                  !- Year 7 Escalation
-    1.0664,                  !- Year 8 Escalation
-    1.0758,                  !- Year 9 Escalation
-    1.0891,                  !- Year 10 Escalation
-    1.0967,                  !- Year 11 Escalation
-    1.1071,                  !- Year 12 Escalation
-    1.0976,                  !- Year 13 Escalation
-    1.0701,                  !- Year 14 Escalation
-    1.0730,                  !- Year 15 Escalation
-    1.0929,                  !- Year 16 Escalation
-    1.1166,                  !- Year 17 Escalation
-    1.1384,                  !- Year 18 Escalation
-    1.1611,                  !- Year 19 Escalation
-    1.1820,                  !- Year 20 Escalation
-    1.2085,                  !- Year 21 Escalation
-    1.2284,                  !- Year 22 Escalation
-    1.2427,                  !- Year 23 Escalation
-    1.2626,                  !- Year 24 Escalation
-    1.2796,                  !- Year 25 Escalation
-    1.2948,                  !- Year 26 Escalation
-    1.3090,                  !- Year 27 Escalation
-    1.3242,                  !- Year 28 Escalation
-    1.3393,                  !- Year 29 Escalation
-    1.3555;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Residential-LPG,   !- Name
-    PropaneGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9861,                  !- Year 1 Escalation
-    1.0210,                  !- Year 2 Escalation
-    1.0682,                  !- Year 3 Escalation
-    1.1086,                  !- Year 4 Escalation
-    1.1352,                  !- Year 5 Escalation
-    1.1597,                  !- Year 6 Escalation
-    1.1819,                  !- Year 7 Escalation
-    1.2041,                  !- Year 8 Escalation
-    1.2172,                  !- Year 9 Escalation
-    1.2259,                  !- Year 10 Escalation
-    1.2346,                  !- Year 11 Escalation
-    1.2430,                  !- Year 12 Escalation
-    1.2529,                  !- Year 13 Escalation
-    1.2632,                  !- Year 14 Escalation
-    1.2735,                  !- Year 15 Escalation
-    1.2798,                  !- Year 16 Escalation
-    1.2889,                  !- Year 17 Escalation
-    1.2989,                  !- Year 18 Escalation
-    1.3115,                  !- Year 19 Escalation
-    1.3214,                  !- Year 20 Escalation
-    1.3337,                  !- Year 21 Escalation
-    1.3468,                  !- Year 22 Escalation
-    1.3611,                  !- Year 23 Escalation
-    1.3757,                  !- Year 24 Escalation
-    1.3904,                  !- Year 25 Escalation
-    1.4035,                  !- Year 26 Escalation
-    1.4166,                  !- Year 27 Escalation
-    1.4296,                  !- Year 28 Escalation
-    1.4427,                  !- Year 29 Escalation
-    1.4558;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Commercial-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9933,                  !- Year 1 Escalation
-    1.0067,                  !- Year 2 Escalation
-    1.0158,                  !- Year 3 Escalation
-    1.0140,                  !- Year 4 Escalation
-    1.0067,                  !- Year 5 Escalation
-    1.0007,                  !- Year 6 Escalation
-    0.9958,                  !- Year 7 Escalation
-    0.9888,                  !- Year 8 Escalation
-    0.9831,                  !- Year 9 Escalation
-    0.9842,                  !- Year 10 Escalation
-    0.9870,                  !- Year 11 Escalation
-    0.9888,                  !- Year 12 Escalation
-    0.9909,                  !- Year 13 Escalation
-    0.9856,                  !- Year 14 Escalation
-    0.9821,                  !- Year 15 Escalation
-    0.9870,                  !- Year 16 Escalation
-    0.9944,                  !- Year 17 Escalation
-    0.9996,                  !- Year 18 Escalation
-    1.0063,                  !- Year 19 Escalation
-    1.0137,                  !- Year 20 Escalation
-    1.0225,                  !- Year 21 Escalation
-    1.0313,                  !- Year 22 Escalation
-    1.0358,                  !- Year 23 Escalation
-    1.0407,                  !- Year 24 Escalation
-    1.0460,                  !- Year 25 Escalation
-    1.0506,                  !- Year 26 Escalation
-    1.0551,                  !- Year 27 Escalation
-    1.0593,                  !- Year 28 Escalation
-    1.0636,                  !- Year 29 Escalation
-    1.0681;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Commercial-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9967,                  !- Year 1 Escalation
-    1.0892,                  !- Year 2 Escalation
-    1.1684,                  !- Year 3 Escalation
-    1.2210,                  !- Year 4 Escalation
-    1.2510,                  !- Year 5 Escalation
-    1.2750,                  !- Year 6 Escalation
-    1.3256,                  !- Year 7 Escalation
-    1.3695,                  !- Year 8 Escalation
-    1.3948,                  !- Year 9 Escalation
-    1.4081,                  !- Year 10 Escalation
-    1.4234,                  !- Year 11 Escalation
-    1.4387,                  !- Year 12 Escalation
-    1.4547,                  !- Year 13 Escalation
-    1.4674,                  !- Year 14 Escalation
-    1.4827,                  !- Year 15 Escalation
-    1.4960,                  !- Year 16 Escalation
-    1.5200,                  !- Year 17 Escalation
-    1.5433,                  !- Year 18 Escalation
-    1.5679,                  !- Year 19 Escalation
-    1.5912,                  !- Year 20 Escalation
-    1.6212,                  !- Year 21 Escalation
-    1.6518,                  !- Year 22 Escalation
-    1.6631,                  !- Year 23 Escalation
-    1.6844,                  !- Year 24 Escalation
-    1.7210,                  !- Year 25 Escalation
-    1.7470,                  !- Year 26 Escalation
-    1.7690,                  !- Year 27 Escalation
-    1.7909,                  !- Year 28 Escalation
-    1.8129,                  !- Year 29 Escalation
-    1.8349;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Commercial-Residual Oil,  !- Name
-    FuelOil#2,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.3506,                  !- Year 1 Escalation
-    1.4485,                  !- Year 2 Escalation
-    1.5372,                  !- Year 3 Escalation
-    1.6042,                  !- Year 4 Escalation
-    1.6456,                  !- Year 5 Escalation
-    1.6584,                  !- Year 6 Escalation
-    1.7035,                  !- Year 7 Escalation
-    1.7359,                  !- Year 8 Escalation
-    1.7540,                  !- Year 9 Escalation
-    1.7547,                  !- Year 10 Escalation
-    1.7660,                  !- Year 11 Escalation
-    1.7720,                  !- Year 12 Escalation
-    1.7840,                  !- Year 13 Escalation
-    1.7991,                  !- Year 14 Escalation
-    1.8126,                  !- Year 15 Escalation
-    1.8179,                  !- Year 16 Escalation
-    1.8442,                  !- Year 17 Escalation
-    1.8698,                  !- Year 18 Escalation
-    1.8909,                  !- Year 19 Escalation
-    1.9127,                  !- Year 20 Escalation
-    1.9368,                  !- Year 21 Escalation
-    1.9571,                  !- Year 22 Escalation
-    1.9661,                  !- Year 23 Escalation
-    1.9842,                  !- Year 24 Escalation
-    2.0090,                  !- Year 25 Escalation
-    2.0339,                  !- Year 26 Escalation
-    2.0579,                  !- Year 27 Escalation
-    2.0828,                  !- Year 28 Escalation
-    2.1076,                  !- Year 29 Escalation
-    2.1332;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Commercial-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0826,                  !- Year 1 Escalation
-    1.1365,                  !- Year 2 Escalation
-    1.1204,                  !- Year 3 Escalation
-    1.1089,                  !- Year 4 Escalation
-    1.1227,                  !- Year 5 Escalation
-    1.1422,                  !- Year 6 Escalation
-    1.1548,                  !- Year 7 Escalation
-    1.1674,                  !- Year 8 Escalation
-    1.1800,                  !- Year 9 Escalation
-    1.1984,                  !- Year 10 Escalation
-    1.2087,                  !- Year 11 Escalation
-    1.2225,                  !- Year 12 Escalation
-    1.2110,                  !- Year 13 Escalation
-    1.1800,                  !- Year 14 Escalation
-    1.1869,                  !- Year 15 Escalation
-    1.2110,                  !- Year 16 Escalation
-    1.2397,                  !- Year 17 Escalation
-    1.2683,                  !- Year 18 Escalation
-    1.2936,                  !- Year 19 Escalation
-    1.3188,                  !- Year 20 Escalation
-    1.3509,                  !- Year 21 Escalation
-    1.3750,                  !- Year 22 Escalation
-    1.3911,                  !- Year 23 Escalation
-    1.4151,                  !- Year 24 Escalation
-    1.4358,                  !- Year 25 Escalation
-    1.4541,                  !- Year 26 Escalation
-    1.4713,                  !- Year 27 Escalation
-    1.4897,                  !- Year 28 Escalation
-    1.5080,                  !- Year 29 Escalation
-    1.5275;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Commercial-Coal,   !- Name
-    Coal,                    !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9828,                  !- Year 1 Escalation
-    0.9914,                  !- Year 2 Escalation
-    0.9971,                  !- Year 3 Escalation
-    1.0000,                  !- Year 4 Escalation
-    1.0172,                  !- Year 5 Escalation
-    1.0344,                  !- Year 6 Escalation
-    1.0458,                  !- Year 7 Escalation
-    1.0544,                  !- Year 8 Escalation
-    1.0630,                  !- Year 9 Escalation
-    1.0745,                  !- Year 10 Escalation
-    1.0860,                  !- Year 11 Escalation
-    1.1032,                  !- Year 12 Escalation
-    1.1089,                  !- Year 13 Escalation
-    1.1175,                  !- Year 14 Escalation
-    1.1232,                  !- Year 15 Escalation
-    1.1375,                  !- Year 16 Escalation
-    1.1490,                  !- Year 17 Escalation
-    1.1633,                  !- Year 18 Escalation
-    1.1777,                  !- Year 19 Escalation
-    1.1948,                  !- Year 20 Escalation
-    1.2092,                  !- Year 21 Escalation
-    1.2235,                  !- Year 22 Escalation
-    1.2350,                  !- Year 23 Escalation
-    1.2493,                  !- Year 24 Escalation
-    1.2693,                  !- Year 25 Escalation
-    1.2779,                  !- Year 26 Escalation
-    1.2779,                  !- Year 27 Escalation
-    1.2808,                  !- Year 28 Escalation
-    1.2837,                  !- Year 29 Escalation
-    1.2837;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Industrial-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9822,                  !- Year 1 Escalation
-    0.9857,                  !- Year 2 Escalation
-    0.9881,                  !- Year 3 Escalation
-    0.9837,                  !- Year 4 Escalation
-    0.9778,                  !- Year 5 Escalation
-    0.9753,                  !- Year 6 Escalation
-    0.9738,                  !- Year 7 Escalation
-    0.9699,                  !- Year 8 Escalation
-    0.9674,                  !- Year 9 Escalation
-    0.9718,                  !- Year 10 Escalation
-    0.9778,                  !- Year 11 Escalation
-    0.9827,                  !- Year 12 Escalation
-    0.9886,                  !- Year 13 Escalation
-    0.9842,                  !- Year 14 Escalation
-    0.9812,                  !- Year 15 Escalation
-    0.9896,                  !- Year 16 Escalation
-    0.9990,                  !- Year 17 Escalation
-    1.0064,                  !- Year 18 Escalation
-    1.0148,                  !- Year 19 Escalation
-    1.0242,                  !- Year 20 Escalation
-    1.0356,                  !- Year 21 Escalation
-    1.0459,                  !- Year 22 Escalation
-    1.0519,                  !- Year 23 Escalation
-    1.0568,                  !- Year 24 Escalation
-    1.0627,                  !- Year 25 Escalation
-    1.0692,                  !- Year 26 Escalation
-    1.0756,                  !- Year 27 Escalation
-    1.0820,                  !- Year 28 Escalation
-    1.0884,                  !- Year 29 Escalation
-    1.0949;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Industrial-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0133,                  !- Year 1 Escalation
-    1.1045,                  !- Year 2 Escalation
-    1.1803,                  !- Year 3 Escalation
-    1.2335,                  !- Year 4 Escalation
-    1.2728,                  !- Year 5 Escalation
-    1.3081,                  !- Year 6 Escalation
-    1.3560,                  !- Year 7 Escalation
-    1.3999,                  !- Year 8 Escalation
-    1.4278,                  !- Year 9 Escalation
-    1.4444,                  !- Year 10 Escalation
-    1.4611,                  !- Year 11 Escalation
-    1.4817,                  !- Year 12 Escalation
-    1.4963,                  !- Year 13 Escalation
-    1.5063,                  !- Year 14 Escalation
-    1.5230,                  !- Year 15 Escalation
-    1.5389,                  !- Year 16 Escalation
-    1.5595,                  !- Year 17 Escalation
-    1.5835,                  !- Year 18 Escalation
-    1.6094,                  !- Year 19 Escalation
-    1.6287,                  !- Year 20 Escalation
-    1.6574,                  !- Year 21 Escalation
-    1.6880,                  !- Year 22 Escalation
-    1.7046,                  !- Year 23 Escalation
-    1.7285,                  !- Year 24 Escalation
-    1.7625,                  !- Year 25 Escalation
-    1.7878,                  !- Year 26 Escalation
-    1.8090,                  !- Year 27 Escalation
-    1.8310,                  !- Year 28 Escalation
-    1.8530,                  !- Year 29 Escalation
-    1.8749;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Industrial-Residual Oil,  !- Name
-    FuelOil#2,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0793,                  !- Year 1 Escalation
-    1.1466,                  !- Year 2 Escalation
-    1.2390,                  !- Year 3 Escalation
-    1.3193,                  !- Year 4 Escalation
-    1.3735,                  !- Year 5 Escalation
-    1.4167,                  !- Year 6 Escalation
-    1.4558,                  !- Year 7 Escalation
-    1.4980,                  !- Year 8 Escalation
-    1.5291,                  !- Year 9 Escalation
-    1.5412,                  !- Year 10 Escalation
-    1.5602,                  !- Year 11 Escalation
-    1.5793,                  !- Year 12 Escalation
-    1.5934,                  !- Year 13 Escalation
-    1.6165,                  !- Year 14 Escalation
-    1.6386,                  !- Year 15 Escalation
-    1.6486,                  !- Year 16 Escalation
-    1.6546,                  !- Year 17 Escalation
-    1.6727,                  !- Year 18 Escalation
-    1.6998,                  !- Year 19 Escalation
-    1.7279,                  !- Year 20 Escalation
-    1.7580,                  !- Year 21 Escalation
-    1.7871,                  !- Year 22 Escalation
-    1.8163,                  !- Year 23 Escalation
-    1.8464,                  !- Year 24 Escalation
-    1.8775,                  !- Year 25 Escalation
-    1.9096,                  !- Year 26 Escalation
-    1.9428,                  !- Year 27 Escalation
-    1.9749,                  !- Year 28 Escalation
-    2.0080,                  !- Year 29 Escalation
-    2.0422;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Industrial-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.1779,                  !- Year 1 Escalation
-    1.2759,                  !- Year 2 Escalation
-    1.2613,                  !- Year 3 Escalation
-    1.2414,                  !- Year 4 Escalation
-    1.2613,                  !- Year 5 Escalation
-    1.2868,                  !- Year 6 Escalation
-    1.3049,                  !- Year 7 Escalation
-    1.3212,                  !- Year 8 Escalation
-    1.3358,                  !- Year 9 Escalation
-    1.3593,                  !- Year 10 Escalation
-    1.3702,                  !- Year 11 Escalation
-    1.3848,                  !- Year 12 Escalation
-    1.3630,                  !- Year 13 Escalation
-    1.3067,                  !- Year 14 Escalation
-    1.3122,                  !- Year 15 Escalation
-    1.3485,                  !- Year 16 Escalation
-    1.3902,                  !- Year 17 Escalation
-    1.4301,                  !- Year 18 Escalation
-    1.4646,                  !- Year 19 Escalation
-    1.5009,                  !- Year 20 Escalation
-    1.5499,                  !- Year 21 Escalation
-    1.5844,                  !- Year 22 Escalation
-    1.6044,                  !- Year 23 Escalation
-    1.6407,                  !- Year 24 Escalation
-    1.6697,                  !- Year 25 Escalation
-    1.6969,                  !- Year 26 Escalation
-    1.7241,                  !- Year 27 Escalation
-    1.7532,                  !- Year 28 Escalation
-    1.7840,                  !- Year 29 Escalation
-    1.8131;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    West  Industrial-Coal,   !- Name
-    Coal,                    !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0040,                  !- Year 1 Escalation
-    1.0160,                  !- Year 2 Escalation
-    1.0160,                  !- Year 3 Escalation
-    1.0160,                  !- Year 4 Escalation
-    1.0200,                  !- Year 5 Escalation
-    1.0160,                  !- Year 6 Escalation
-    1.0200,                  !- Year 7 Escalation
-    1.0200,                  !- Year 8 Escalation
-    1.0200,                  !- Year 9 Escalation
-    1.0200,                  !- Year 10 Escalation
-    1.0200,                  !- Year 11 Escalation
-    1.0240,                  !- Year 12 Escalation
-    1.0240,                  !- Year 13 Escalation
-    1.0240,                  !- Year 14 Escalation
-    1.0200,                  !- Year 15 Escalation
-    1.0240,                  !- Year 16 Escalation
-    1.0240,                  !- Year 17 Escalation
-    1.0280,                  !- Year 18 Escalation
-    1.0320,                  !- Year 19 Escalation
-    1.0360,                  !- Year 20 Escalation
-    1.0480,                  !- Year 21 Escalation
-    1.0560,                  !- Year 22 Escalation
-    1.0640,                  !- Year 23 Escalation
-    1.0760,                  !- Year 24 Escalation
-    1.0840,                  !- Year 25 Escalation
-    1.0920,                  !- Year 26 Escalation
-    1.0920,                  !- Year 27 Escalation
-    1.0960,                  !- Year 28 Escalation
-    1.1000,                  !- Year 29 Escalation
-    1.1000;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Residential-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9642,                  !- Year 1 Escalation
-    0.9840,                  !- Year 2 Escalation
-    1.0029,                  !- Year 3 Escalation
-    1.0064,                  !- Year 4 Escalation
-    1.0051,                  !- Year 5 Escalation
-    1.0099,                  !- Year 6 Escalation
-    1.0153,                  !- Year 7 Escalation
-    1.0160,                  !- Year 8 Escalation
-    1.0134,                  !- Year 9 Escalation
-    1.0166,                  !- Year 10 Escalation
-    1.0221,                  !- Year 11 Escalation
-    1.0249,                  !- Year 12 Escalation
-    1.0285,                  !- Year 13 Escalation
-    1.0313,                  !- Year 14 Escalation
-    1.0313,                  !- Year 15 Escalation
-    1.0345,                  !- Year 16 Escalation
-    1.0400,                  !- Year 17 Escalation
-    1.0451,                  !- Year 18 Escalation
-    1.0559,                  !- Year 19 Escalation
-    1.0671,                  !- Year 20 Escalation
-    1.0780,                  !- Year 21 Escalation
-    1.0879,                  !- Year 22 Escalation
-    1.0940,                  !- Year 23 Escalation
-    1.1007,                  !- Year 24 Escalation
-    1.1077,                  !- Year 25 Escalation
-    1.1145,                  !- Year 26 Escalation
-    1.1208,                  !- Year 27 Escalation
-    1.1272,                  !- Year 28 Escalation
-    1.1340,                  !- Year 29 Escalation
-    1.1403;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Residential-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0006,                  !- Year 1 Escalation
-    1.0498,                  !- Year 2 Escalation
-    1.1092,                  !- Year 3 Escalation
-    1.1545,                  !- Year 4 Escalation
-    1.1856,                  !- Year 5 Escalation
-    1.2320,                  !- Year 6 Escalation
-    1.2728,                  !- Year 7 Escalation
-    1.3101,                  !- Year 8 Escalation
-    1.3373,                  !- Year 9 Escalation
-    1.3588,                  !- Year 10 Escalation
-    1.3696,                  !- Year 11 Escalation
-    1.3803,                  !- Year 12 Escalation
-    1.3967,                  !- Year 13 Escalation
-    1.4086,                  !- Year 14 Escalation
-    1.4239,                  !- Year 15 Escalation
-    1.4392,                  !- Year 16 Escalation
-    1.4522,                  !- Year 17 Escalation
-    1.4692,                  !- Year 18 Escalation
-    1.4907,                  !- Year 19 Escalation
-    1.5037,                  !- Year 20 Escalation
-    1.5246,                  !- Year 21 Escalation
-    1.5478,                  !- Year 22 Escalation
-    1.5693,                  !- Year 23 Escalation
-    1.5920,                  !- Year 24 Escalation
-    1.6157,                  !- Year 25 Escalation
-    1.6338,                  !- Year 26 Escalation
-    1.6520,                  !- Year 27 Escalation
-    1.6701,                  !- Year 28 Escalation
-    1.6887,                  !- Year 29 Escalation
-    1.7080;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Residential-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0490,                  !- Year 1 Escalation
-    1.0763,                  !- Year 2 Escalation
-    1.0518,                  !- Year 3 Escalation
-    1.0381,                  !- Year 4 Escalation
-    1.0463,                  !- Year 5 Escalation
-    1.0563,                  !- Year 6 Escalation
-    1.0609,                  !- Year 7 Escalation
-    1.0663,                  !- Year 8 Escalation
-    1.0727,                  !- Year 9 Escalation
-    1.0827,                  !- Year 10 Escalation
-    1.0936,                  !- Year 11 Escalation
-    1.1090,                  !- Year 12 Escalation
-    1.1153,                  !- Year 13 Escalation
-    1.1099,                  !- Year 14 Escalation
-    1.1144,                  !- Year 15 Escalation
-    1.1281,                  !- Year 16 Escalation
-    1.1453,                  !- Year 17 Escalation
-    1.1662,                  !- Year 18 Escalation
-    1.1889,                  !- Year 19 Escalation
-    1.2144,                  !- Year 20 Escalation
-    1.2434,                  !- Year 21 Escalation
-    1.2616,                  !- Year 22 Escalation
-    1.2716,                  !- Year 23 Escalation
-    1.2888,                  !- Year 24 Escalation
-    1.3043,                  !- Year 25 Escalation
-    1.3170,                  !- Year 26 Escalation
-    1.3306,                  !- Year 27 Escalation
-    1.3451,                  !- Year 28 Escalation
-    1.3597,                  !- Year 29 Escalation
-    1.3751;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Residential-LPG,  !- Name
-    PropaneGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9934,                  !- Year 1 Escalation
-    1.0297,                  !- Year 2 Escalation
-    1.0797,                  !- Year 3 Escalation
-    1.1222,                  !- Year 4 Escalation
-    1.1506,                  !- Year 5 Escalation
-    1.1766,                  !- Year 6 Escalation
-    1.1998,                  !- Year 7 Escalation
-    1.2237,                  !- Year 8 Escalation
-    1.2377,                  !- Year 9 Escalation
-    1.2476,                  !- Year 10 Escalation
-    1.2575,                  !- Year 11 Escalation
-    1.2662,                  !- Year 12 Escalation
-    1.2769,                  !- Year 13 Escalation
-    1.2881,                  !- Year 14 Escalation
-    1.2992,                  !- Year 15 Escalation
-    1.3066,                  !- Year 16 Escalation
-    1.3170,                  !- Year 17 Escalation
-    1.3277,                  !- Year 18 Escalation
-    1.3413,                  !- Year 19 Escalation
-    1.3516,                  !- Year 20 Escalation
-    1.3652,                  !- Year 21 Escalation
-    1.3793,                  !- Year 22 Escalation
-    1.3950,                  !- Year 23 Escalation
-    1.4102,                  !- Year 24 Escalation
-    1.4259,                  !- Year 25 Escalation
-    1.4387,                  !- Year 26 Escalation
-    1.4515,                  !- Year 27 Escalation
-    1.4651,                  !- Year 28 Escalation
-    1.4787,                  !- Year 29 Escalation
-    1.4928;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Commercial-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9413,                  !- Year 1 Escalation
-    0.9539,                  !- Year 2 Escalation
-    0.9654,                  !- Year 3 Escalation
-    0.9589,                  !- Year 4 Escalation
-    0.9568,                  !- Year 5 Escalation
-    0.9636,                  !- Year 6 Escalation
-    0.9705,                  !- Year 7 Escalation
-    0.9723,                  !- Year 8 Escalation
-    0.9708,                  !- Year 9 Escalation
-    0.9755,                  !- Year 10 Escalation
-    0.9823,                  !- Year 11 Escalation
-    0.9870,                  !- Year 12 Escalation
-    0.9935,                  !- Year 13 Escalation
-    0.9993,                  !- Year 14 Escalation
-    0.9993,                  !- Year 15 Escalation
-    1.0029,                  !- Year 16 Escalation
-    1.0090,                  !- Year 17 Escalation
-    1.0162,                  !- Year 18 Escalation
-    1.0292,                  !- Year 19 Escalation
-    1.0418,                  !- Year 20 Escalation
-    1.0548,                  !- Year 21 Escalation
-    1.0681,                  !- Year 22 Escalation
-    1.0760,                  !- Year 23 Escalation
-    1.0843,                  !- Year 24 Escalation
-    1.0923,                  !- Year 25 Escalation
-    1.1052,                  !- Year 26 Escalation
-    1.1146,                  !- Year 27 Escalation
-    1.1222,                  !- Year 28 Escalation
-    1.1301,                  !- Year 29 Escalation
-    1.1377;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Commercial-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0046,                  !- Year 1 Escalation
-    1.0684,                  !- Year 2 Escalation
-    1.1381,                  !- Year 3 Escalation
-    1.1906,                  !- Year 4 Escalation
-    1.2331,                  !- Year 5 Escalation
-    1.2849,                  !- Year 6 Escalation
-    1.3307,                  !- Year 7 Escalation
-    1.3732,                  !- Year 8 Escalation
-    1.4044,                  !- Year 9 Escalation
-    1.4283,                  !- Year 10 Escalation
-    1.4429,                  !- Year 11 Escalation
-    1.4588,                  !- Year 12 Escalation
-    1.4761,                  !- Year 13 Escalation
-    1.4867,                  !- Year 14 Escalation
-    1.5040,                  !- Year 15 Escalation
-    1.5212,                  !- Year 16 Escalation
-    1.5372,                  !- Year 17 Escalation
-    1.5571,                  !- Year 18 Escalation
-    1.5823,                  !- Year 19 Escalation
-    1.5976,                  !- Year 20 Escalation
-    1.6222,                  !- Year 21 Escalation
-    1.6494,                  !- Year 22 Escalation
-    1.6726,                  !- Year 23 Escalation
-    1.6992,                  !- Year 24 Escalation
-    1.7278,                  !- Year 25 Escalation
-    1.7523,                  !- Year 26 Escalation
-    1.7742,                  !- Year 27 Escalation
-    1.7961,                  !- Year 28 Escalation
-    1.8181,                  !- Year 29 Escalation
-    1.8400;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Commercial-Residual Oil,  !- Name
-    FuelOil#2,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0191,                  !- Year 1 Escalation
-    1.1202,                  !- Year 2 Escalation
-    1.2436,                  !- Year 3 Escalation
-    1.3362,                  !- Year 4 Escalation
-    1.3872,                  !- Year 5 Escalation
-    1.4404,                  !- Year 6 Escalation
-    1.4947,                  !- Year 7 Escalation
-    1.5489,                  !- Year 8 Escalation
-    1.6085,                  !- Year 9 Escalation
-    1.6394,                  !- Year 10 Escalation
-    1.6617,                  !- Year 11 Escalation
-    1.6851,                  !- Year 12 Escalation
-    1.7085,                  !- Year 13 Escalation
-    1.7319,                  !- Year 14 Escalation
-    1.7543,                  !- Year 15 Escalation
-    1.7670,                  !- Year 16 Escalation
-    1.7840,                  !- Year 17 Escalation
-    1.8085,                  !- Year 18 Escalation
-    1.8319,                  !- Year 19 Escalation
-    1.8585,                  !- Year 20 Escalation
-    1.8936,                  !- Year 21 Escalation
-    1.9213,                  !- Year 22 Escalation
-    1.9383,                  !- Year 23 Escalation
-    1.9755,                  !- Year 24 Escalation
-    2.0000,                  !- Year 25 Escalation
-    2.0277,                  !- Year 26 Escalation
-    2.0606,                  !- Year 27 Escalation
-    2.0957,                  !- Year 28 Escalation
-    2.1309,                  !- Year 29 Escalation
-    2.1660;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Commercial-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0788,                  !- Year 1 Escalation
-    1.1393,                  !- Year 2 Escalation
-    1.1370,                  !- Year 3 Escalation
-    1.1267,                  !- Year 4 Escalation
-    1.1358,                  !- Year 5 Escalation
-    1.1484,                  !- Year 6 Escalation
-    1.1530,                  !- Year 7 Escalation
-    1.1587,                  !- Year 8 Escalation
-    1.1655,                  !- Year 9 Escalation
-    1.1781,                  !- Year 10 Escalation
-    1.1906,                  !- Year 11 Escalation
-    1.2100,                  !- Year 12 Escalation
-    1.2192,                  !- Year 13 Escalation
-    1.2146,                  !- Year 14 Escalation
-    1.2192,                  !- Year 15 Escalation
-    1.2352,                  !- Year 16 Escalation
-    1.2546,                  !- Year 17 Escalation
-    1.2808,                  !- Year 18 Escalation
-    1.3082,                  !- Year 19 Escalation
-    1.3368,                  !- Year 20 Escalation
-    1.3733,                  !- Year 21 Escalation
-    1.3950,                  !- Year 22 Escalation
-    1.4041,                  !- Year 23 Escalation
-    1.4235,                  !- Year 24 Escalation
-    1.4406,                  !- Year 25 Escalation
-    1.4566,                  !- Year 26 Escalation
-    1.4737,                  !- Year 27 Escalation
-    1.4920,                  !- Year 28 Escalation
-    1.5103,                  !- Year 29 Escalation
-    1.5297;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Commercial-Coal,  !- Name
-    Coal,                    !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9900,                  !- Year 1 Escalation
-    0.9933,                  !- Year 2 Escalation
-    0.9866,                  !- Year 3 Escalation
-    0.9900,                  !- Year 4 Escalation
-    0.9900,                  !- Year 5 Escalation
-    0.9866,                  !- Year 6 Escalation
-    0.9900,                  !- Year 7 Escalation
-    0.9866,                  !- Year 8 Escalation
-    0.9799,                  !- Year 9 Escalation
-    0.9766,                  !- Year 10 Escalation
-    0.9732,                  !- Year 11 Escalation
-    0.9766,                  !- Year 12 Escalation
-    0.9766,                  !- Year 13 Escalation
-    0.9799,                  !- Year 14 Escalation
-    0.9766,                  !- Year 15 Escalation
-    0.9799,                  !- Year 16 Escalation
-    0.9799,                  !- Year 17 Escalation
-    0.9833,                  !- Year 18 Escalation
-    0.9900,                  !- Year 19 Escalation
-    0.9967,                  !- Year 20 Escalation
-    1.0000,                  !- Year 21 Escalation
-    1.0033,                  !- Year 22 Escalation
-    1.0067,                  !- Year 23 Escalation
-    1.0134,                  !- Year 24 Escalation
-    1.0201,                  !- Year 25 Escalation
-    1.0268,                  !- Year 26 Escalation
-    1.0268,                  !- Year 27 Escalation
-    1.0301,                  !- Year 28 Escalation
-    1.0334,                  !- Year 29 Escalation
-    1.0334;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Industrial-Electricity,  !- Name
-    Electricity,             !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9086,                  !- Year 1 Escalation
-    0.9071,                  !- Year 2 Escalation
-    0.9112,                  !- Year 3 Escalation
-    0.8993,                  !- Year 4 Escalation
-    0.8962,                  !- Year 5 Escalation
-    0.9066,                  !- Year 6 Escalation
-    0.9148,                  !- Year 7 Escalation
-    0.9169,                  !- Year 8 Escalation
-    0.9164,                  !- Year 9 Escalation
-    0.9231,                  !- Year 10 Escalation
-    0.9308,                  !- Year 11 Escalation
-    0.9375,                  !- Year 12 Escalation
-    0.9463,                  !- Year 13 Escalation
-    0.9546,                  !- Year 14 Escalation
-    0.9556,                  !- Year 15 Escalation
-    0.9592,                  !- Year 16 Escalation
-    0.9675,                  !- Year 17 Escalation
-    0.9768,                  !- Year 18 Escalation
-    0.9923,                  !- Year 19 Escalation
-    1.0072,                  !- Year 20 Escalation
-    1.0222,                  !- Year 21 Escalation
-    1.0372,                  !- Year 22 Escalation
-    1.0459,                  !- Year 23 Escalation
-    1.0563,                  !- Year 24 Escalation
-    1.0666,                  !- Year 25 Escalation
-    1.0774,                  !- Year 26 Escalation
-    1.0878,                  !- Year 27 Escalation
-    1.0971,                  !- Year 28 Escalation
-    1.1069,                  !- Year 29 Escalation
-    1.1167;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Industrial-Distillate Oil,  !- Name
-    FuelOil#1,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0175,                  !- Year 1 Escalation
-    1.0935,                  !- Year 2 Escalation
-    1.1655,                  !- Year 3 Escalation
-    1.2201,                  !- Year 4 Escalation
-    1.2672,                  !- Year 5 Escalation
-    1.3190,                  !- Year 6 Escalation
-    1.3647,                  !- Year 7 Escalation
-    1.4078,                  !- Year 8 Escalation
-    1.4394,                  !- Year 9 Escalation
-    1.4630,                  !- Year 10 Escalation
-    1.4791,                  !- Year 11 Escalation
-    1.4993,                  !- Year 12 Escalation
-    1.5148,                  !- Year 13 Escalation
-    1.5236,                  !- Year 14 Escalation
-    1.5404,                  !- Year 15 Escalation
-    1.5585,                  !- Year 16 Escalation
-    1.5754,                  !- Year 17 Escalation
-    1.5969,                  !- Year 18 Escalation
-    1.6231,                  !- Year 19 Escalation
-    1.6386,                  !- Year 20 Escalation
-    1.6642,                  !- Year 21 Escalation
-    1.6925,                  !- Year 22 Escalation
-    1.7167,                  !- Year 23 Escalation
-    1.7436,                  !- Year 24 Escalation
-    1.7739,                  !- Year 25 Escalation
-    1.7988,                  !- Year 26 Escalation
-    1.8203,                  !- Year 27 Escalation
-    1.8425,                  !- Year 28 Escalation
-    1.8647,                  !- Year 29 Escalation
-    1.8869;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Industrial-Residual Oil,  !- Name
-    FuelOil#2,               !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.0846,                  !- Year 1 Escalation
-    1.1527,                  !- Year 2 Escalation
-    1.2365,                  !- Year 3 Escalation
-    1.3038,                  !- Year 4 Escalation
-    1.3440,                  !- Year 5 Escalation
-    1.3826,                  !- Year 6 Escalation
-    1.4179,                  !- Year 7 Escalation
-    1.4540,                  !- Year 8 Escalation
-    1.4795,                  !- Year 9 Escalation
-    1.4918,                  !- Year 10 Escalation
-    1.5082,                  !- Year 11 Escalation
-    1.5238,                  !- Year 12 Escalation
-    1.5411,                  !- Year 13 Escalation
-    1.5583,                  !- Year 14 Escalation
-    1.5747,                  !- Year 15 Escalation
-    1.5829,                  !- Year 16 Escalation
-    1.5961,                  !- Year 17 Escalation
-    1.6149,                  !- Year 18 Escalation
-    1.6355,                  !- Year 19 Escalation
-    1.6585,                  !- Year 20 Escalation
-    1.6847,                  !- Year 21 Escalation
-    1.7077,                  !- Year 22 Escalation
-    1.7291,                  !- Year 23 Escalation
-    1.7537,                  !- Year 24 Escalation
-    1.7775,                  !- Year 25 Escalation
-    1.8030,                  !- Year 26 Escalation
-    1.8300,                  !- Year 27 Escalation
-    1.8571,                  !- Year 28 Escalation
-    1.8842,                  !- Year 29 Escalation
-    1.9113;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Industrial-Natural gas,  !- Name
-    NaturalGas,              !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    1.2090,                  !- Year 1 Escalation
-    1.3390,                  !- Year 2 Escalation
-    1.3518,                  !- Year 3 Escalation
-    1.3412,                  !- Year 4 Escalation
-    1.3667,                  !- Year 5 Escalation
-    1.3859,                  !- Year 6 Escalation
-    1.3881,                  !- Year 7 Escalation
-    1.3945,                  !- Year 8 Escalation
-    1.4051,                  !- Year 9 Escalation
-    1.4222,                  !- Year 10 Escalation
-    1.4414,                  !- Year 11 Escalation
-    1.4733,                  !- Year 12 Escalation
-    1.4925,                  !- Year 13 Escalation
-    1.4861,                  !- Year 14 Escalation
-    1.4925,                  !- Year 15 Escalation
-    1.5181,                  !- Year 16 Escalation
-    1.5458,                  !- Year 17 Escalation
-    1.5885,                  !- Year 18 Escalation
-    1.6354,                  !- Year 19 Escalation
-    1.6887,                  !- Year 20 Escalation
-    1.7505,                  !- Year 21 Escalation
-    1.7846,                  !- Year 22 Escalation
-    1.7932,                  !- Year 23 Escalation
-    1.8252,                  !- Year 24 Escalation
-    1.8550,                  !- Year 25 Escalation
-    1.8849,                  !- Year 26 Escalation
-    1.9168,                  !- Year 27 Escalation
-    1.9510,                  !- Year 28 Escalation
-    1.9851,                  !- Year 29 Escalation
-    2.0213;                  !- Year 30 Escalation
-
-  LifeCycleCost:UsePriceEscalation,
-    U.S. Avg  Industrial-Coal,  !- Name
-    Coal,                    !- Resource
-    2010,                    !- Escalation Start Year
-    January,                 !- Escalation Start Month
-    0.9926,                  !- Year 1 Escalation
-    0.9926,                  !- Year 2 Escalation
-    0.9852,                  !- Year 3 Escalation
-    0.9852,                  !- Year 4 Escalation
-    0.9926,                  !- Year 5 Escalation
-    0.9889,                  !- Year 6 Escalation
-    0.9926,                  !- Year 7 Escalation
-    0.9889,                  !- Year 8 Escalation
-    0.9852,                  !- Year 9 Escalation
-    0.9815,                  !- Year 10 Escalation
-    0.9779,                  !- Year 11 Escalation
-    0.9779,                  !- Year 12 Escalation
-    0.9705,                  !- Year 13 Escalation
-    0.9705,                  !- Year 14 Escalation
-    0.9705,                  !- Year 15 Escalation
-    0.9742,                  !- Year 16 Escalation
-    0.9705,                  !- Year 17 Escalation
-    0.9742,                  !- Year 18 Escalation
-    0.9779,                  !- Year 19 Escalation
-    0.9815,                  !- Year 20 Escalation
-    0.9852,                  !- Year 21 Escalation
-    0.9852,                  !- Year 22 Escalation
-    0.9889,                  !- Year 23 Escalation
-    0.9963,                  !- Year 24 Escalation
-    1.0000,                  !- Year 25 Escalation
-    1.0037,                  !- Year 26 Escalation
-    1.0037,                  !- Year 27 Escalation
-    1.0074,                  !- Year 28 Escalation
-    1.0111,                  !- Year 29 Escalation
-    1.0111;                  !- Year 30 Escalation
-
diff --git a/datasets/LCCusePriceEscalationDataSet2015.idf b/datasets/LCCusePriceEscalationDataSet2015.idf
new file mode 100644
index 00000000000..eb2550a1a53
--- /dev/null
+++ b/datasets/LCCusePriceEscalationDataSet2015.idf
@@ -0,0 +1,2607 @@
+! The source of the values for the following objects is:
+!
+!    NISTIR 85-3273-30
+! 
+!    ENERGY PRICE INDICES AND DISCOUNT FACTORS
+!    FOR LIFE-CYCLE COST ANALYSIS - 2015
+!
+!    Annual Supplement to NIST Handbook 135
+!
+!    Priya Lavappa
+!    Joshua D. Kneifel
+!
+! These are factors for the United States and regions of the United States. 
+!
+! The factors are from a file available upon request from NIST called ENCOSTxx.TXT and are 
+! converted into EnergyPlus objects using a spreadsheet called ConvertENCOSTtoEnergyPlusLifeCycleCost.xls
+! which is available upon request.
+ 
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Residential-Electricity,  !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9934,                              !- Year 1 Escalation
+    0.9945,                              !- Year 2 Escalation
+    1.0108,                              !- Year 3 Escalation
+    1.0454,                              !- Year 4 Escalation
+    1.0869,                              !- Year 5 Escalation
+    1.1299,                              !- Year 6 Escalation
+    1.1572,                              !- Year 7 Escalation
+    1.1779,                              !- Year 8 Escalation
+    1.1914,                              !- Year 9 Escalation
+    1.2110,                              !- Year 10 Escalation
+    1.2232,                              !- Year 11 Escalation
+    1.2287,                              !- Year 12 Escalation
+    1.2379,                              !- Year 13 Escalation
+    1.2388,                              !- Year 14 Escalation
+    1.2412,                              !- Year 15 Escalation
+    1.2404,                              !- Year 16 Escalation
+    1.2456,                              !- Year 17 Escalation
+    1.2525,                              !- Year 18 Escalation
+    1.2598,                              !- Year 19 Escalation
+    1.2655,                              !- Year 20 Escalation
+    1.2697,                              !- Year 21 Escalation
+    1.2759,                              !- Year 22 Escalation
+    1.2913,                              !- Year 23 Escalation
+    1.3116,                              !- Year 24 Escalation
+    1.3264,                              !- Year 25 Escalation
+    1.3354,                              !- Year 26 Escalation
+    1.3431,                              !- Year 27 Escalation
+    1.3510,                              !- Year 28 Escalation
+    1.3588,                              !- Year 29 Escalation
+    1.3667;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Residential-Distillate Oil,  !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9839,                              !- Year 1 Escalation
+    1.0264,                              !- Year 2 Escalation
+    1.0338,                              !- Year 3 Escalation
+    1.0435,                              !- Year 4 Escalation
+    1.0563,                              !- Year 5 Escalation
+    1.0734,                              !- Year 6 Escalation
+    1.0934,                              !- Year 7 Escalation
+    1.1145,                              !- Year 8 Escalation
+    1.1360,                              !- Year 9 Escalation
+    1.1580,                              !- Year 10 Escalation
+    1.1820,                              !- Year 11 Escalation
+    1.2055,                              !- Year 12 Escalation
+    1.2324,                              !- Year 13 Escalation
+    1.2593,                              !- Year 14 Escalation
+    1.2872,                              !- Year 15 Escalation
+    1.3156,                              !- Year 16 Escalation
+    1.3434,                              !- Year 17 Escalation
+    1.3733,                              !- Year 18 Escalation
+    1.4036,                              !- Year 19 Escalation
+    1.4354,                              !- Year 20 Escalation
+    1.4672,                              !- Year 21 Escalation
+    1.5000,                              !- Year 22 Escalation
+    1.5362,                              !- Year 23 Escalation
+    1.5719,                              !- Year 24 Escalation
+    1.6062,                              !- Year 25 Escalation
+    1.6399,                              !- Year 26 Escalation
+    1.6742,                              !- Year 27 Escalation
+    1.7099,                              !- Year 28 Escalation
+    1.7466,                              !- Year 29 Escalation
+    1.7842;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Residential-Natural gas,  !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0021,                              !- Year 1 Escalation
+    1.0589,                              !- Year 2 Escalation
+    1.1147,                              !- Year 3 Escalation
+    1.1874,                              !- Year 4 Escalation
+    1.2516,                              !- Year 5 Escalation
+    1.3063,                              !- Year 6 Escalation
+    1.3453,                              !- Year 7 Escalation
+    1.3779,                              !- Year 8 Escalation
+    1.4063,                              !- Year 9 Escalation
+    1.4305,                              !- Year 10 Escalation
+    1.4411,                              !- Year 11 Escalation
+    1.4295,                              !- Year 12 Escalation
+    1.4105,                              !- Year 13 Escalation
+    1.3968,                              !- Year 14 Escalation
+    1.3863,                              !- Year 15 Escalation
+    1.3884,                              !- Year 16 Escalation
+    1.4011,                              !- Year 17 Escalation
+    1.4179,                              !- Year 18 Escalation
+    1.4337,                              !- Year 19 Escalation
+    1.4579,                              !- Year 20 Escalation
+    1.4779,                              !- Year 21 Escalation
+    1.5126,                              !- Year 22 Escalation
+    1.5579,                              !- Year 23 Escalation
+    1.6116,                              !- Year 24 Escalation
+    1.6600,                              !- Year 25 Escalation
+    1.6832,                              !- Year 26 Escalation
+    1.6989,                              !- Year 27 Escalation
+    1.7158,                              !- Year 28 Escalation
+    1.7326,                              !- Year 29 Escalation
+    1.7495;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Residential-LPG,          !- Name
+    PropaneGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0075,                              !- Year 1 Escalation
+    1.0344,                              !- Year 2 Escalation
+    1.0443,                              !- Year 3 Escalation
+    1.0518,                              !- Year 4 Escalation
+    1.0566,                              !- Year 5 Escalation
+    1.0605,                              !- Year 6 Escalation
+    1.0649,                              !- Year 7 Escalation
+    1.0712,                              !- Year 8 Escalation
+    1.0772,                              !- Year 9 Escalation
+    1.0831,                              !- Year 10 Escalation
+    1.0906,                              !- Year 11 Escalation
+    1.0970,                              !- Year 12 Escalation
+    1.1025,                              !- Year 13 Escalation
+    1.1088,                              !- Year 14 Escalation
+    1.1156,                              !- Year 15 Escalation
+    1.1235,                              !- Year 16 Escalation
+    1.1338,                              !- Year 17 Escalation
+    1.1429,                              !- Year 18 Escalation
+    1.1512,                              !- Year 19 Escalation
+    1.1603,                              !- Year 20 Escalation
+    1.1690,                              !- Year 21 Escalation
+    1.1773,                              !- Year 22 Escalation
+    1.1856,                              !- Year 23 Escalation
+    1.1963,                              !- Year 24 Escalation
+    1.2085,                              !- Year 25 Escalation
+    1.2176,                              !- Year 26 Escalation
+    1.2260,                              !- Year 27 Escalation
+    1.2343,                              !- Year 28 Escalation
+    1.2426,                              !- Year 29 Escalation
+    1.2509;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Commercial-Electricity,   !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9852,                              !- Year 1 Escalation
+    0.9832,                              !- Year 2 Escalation
+    0.9946,                              !- Year 3 Escalation
+    1.0316,                              !- Year 4 Escalation
+    1.0718,                              !- Year 5 Escalation
+    1.1160,                              !- Year 6 Escalation
+    1.1437,                              !- Year 7 Escalation
+    1.1648,                              !- Year 8 Escalation
+    1.1767,                              !- Year 9 Escalation
+    1.1953,                              !- Year 10 Escalation
+    1.2044,                              !- Year 11 Escalation
+    1.2092,                              !- Year 12 Escalation
+    1.2221,                              !- Year 13 Escalation
+    1.2215,                              !- Year 14 Escalation
+    1.2212,                              !- Year 15 Escalation
+    1.2149,                              !- Year 16 Escalation
+    1.2184,                              !- Year 17 Escalation
+    1.2249,                              !- Year 18 Escalation
+    1.2315,                              !- Year 19 Escalation
+    1.2369,                              !- Year 20 Escalation
+    1.2406,                              !- Year 21 Escalation
+    1.2469,                              !- Year 22 Escalation
+    1.2662,                              !- Year 23 Escalation
+    1.2908,                              !- Year 24 Escalation
+    1.3084,                              !- Year 25 Escalation
+    1.3181,                              !- Year 26 Escalation
+    1.3255,                              !- Year 27 Escalation
+    1.3330,                              !- Year 28 Escalation
+    1.3406,                              !- Year 29 Escalation
+    1.3483;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Commercial-Distillate Oil,  !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9834,                              !- Year 1 Escalation
+    1.0065,                              !- Year 2 Escalation
+    1.0091,                              !- Year 3 Escalation
+    1.0202,                              !- Year 4 Escalation
+    1.0348,                              !- Year 5 Escalation
+    1.0529,                              !- Year 6 Escalation
+    1.0766,                              !- Year 7 Escalation
+    1.0992,                              !- Year 8 Escalation
+    1.1219,                              !- Year 9 Escalation
+    1.1451,                              !- Year 10 Escalation
+    1.1698,                              !- Year 11 Escalation
+    1.1945,                              !- Year 12 Escalation
+    1.2212,                              !- Year 13 Escalation
+    1.2479,                              !- Year 14 Escalation
+    1.2751,                              !- Year 15 Escalation
+    1.3033,                              !- Year 16 Escalation
+    1.3320,                              !- Year 17 Escalation
+    1.3632,                              !- Year 18 Escalation
+    1.3950,                              !- Year 19 Escalation
+    1.4277,                              !- Year 20 Escalation
+    1.4605,                              !- Year 21 Escalation
+    1.4947,                              !- Year 22 Escalation
+    1.5320,                              !- Year 23 Escalation
+    1.5688,                              !- Year 24 Escalation
+    1.6040,                              !- Year 25 Escalation
+    1.6393,                              !- Year 26 Escalation
+    1.6746,                              !- Year 27 Escalation
+    1.7113,                              !- Year 28 Escalation
+    1.7491,                              !- Year 29 Escalation
+    1.7879;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Commercial-Residual Oil,  !- Name
+    FuelOil#2,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0084,                              !- Year 1 Escalation
+    1.0565,                              !- Year 2 Escalation
+    1.0588,                              !- Year 3 Escalation
+    1.0740,                              !- Year 4 Escalation
+    1.0939,                              !- Year 5 Escalation
+    1.1183,                              !- Year 6 Escalation
+    1.1443,                              !- Year 7 Escalation
+    1.1718,                              !- Year 8 Escalation
+    1.2000,                              !- Year 9 Escalation
+    1.2282,                              !- Year 10 Escalation
+    1.2588,                              !- Year 11 Escalation
+    1.2901,                              !- Year 12 Escalation
+    1.3214,                              !- Year 13 Escalation
+    1.3534,                              !- Year 14 Escalation
+    1.3878,                              !- Year 15 Escalation
+    1.4244,                              !- Year 16 Escalation
+    1.4611,                              !- Year 17 Escalation
+    1.4962,                              !- Year 18 Escalation
+    1.5351,                              !- Year 19 Escalation
+    1.5748,                              !- Year 20 Escalation
+    1.6153,                              !- Year 21 Escalation
+    1.6557,                              !- Year 22 Escalation
+    1.6985,                              !- Year 23 Escalation
+    1.7641,                              !- Year 24 Escalation
+    1.8481,                              !- Year 25 Escalation
+    1.9107,                              !- Year 26 Escalation
+    1.9641,                              !- Year 27 Escalation
+    2.0198,                              !- Year 28 Escalation
+    2.0763,                              !- Year 29 Escalation
+    2.1351;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Commercial-Natural gas,   !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0190,                              !- Year 1 Escalation
+    1.0819,                              !- Year 2 Escalation
+    1.1301,                              !- Year 3 Escalation
+    1.2149,                              !- Year 4 Escalation
+    1.2953,                              !- Year 5 Escalation
+    1.3611,                              !- Year 6 Escalation
+    1.4094,                              !- Year 7 Escalation
+    1.4474,                              !- Year 8 Escalation
+    1.4795,                              !- Year 9 Escalation
+    1.5088,                              !- Year 10 Escalation
+    1.5161,                              !- Year 11 Escalation
+    1.4942,                              !- Year 12 Escalation
+    1.4605,                              !- Year 13 Escalation
+    1.4342,                              !- Year 14 Escalation
+    1.4123,                              !- Year 15 Escalation
+    1.4079,                              !- Year 16 Escalation
+    1.4167,                              !- Year 17 Escalation
+    1.4298,                              !- Year 18 Escalation
+    1.4430,                              !- Year 19 Escalation
+    1.4649,                              !- Year 20 Escalation
+    1.4854,                              !- Year 21 Escalation
+    1.5219,                              !- Year 22 Escalation
+    1.5746,                              !- Year 23 Escalation
+    1.6374,                              !- Year 24 Escalation
+    1.6930,                              !- Year 25 Escalation
+    1.7222,                              !- Year 26 Escalation
+    1.7442,                              !- Year 27 Escalation
+    1.7675,                              !- Year 28 Escalation
+    1.7909,                              !- Year 29 Escalation
+    1.8143;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Commercial-Coal,          !- Name
+    Coal,                                !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0065,                              !- Year 1 Escalation
+    1.0211,                              !- Year 2 Escalation
+    1.0276,                              !- Year 3 Escalation
+    1.0324,                              !- Year 4 Escalation
+    1.0454,                              !- Year 5 Escalation
+    1.0567,                              !- Year 6 Escalation
+    1.0600,                              !- Year 7 Escalation
+    1.0632,                              !- Year 8 Escalation
+    1.0632,                              !- Year 9 Escalation
+    1.0648,                              !- Year 10 Escalation
+    1.0681,                              !- Year 11 Escalation
+    1.0697,                              !- Year 12 Escalation
+    1.0729,                              !- Year 13 Escalation
+    1.0762,                              !- Year 14 Escalation
+    1.0810,                              !- Year 15 Escalation
+    1.0859,                              !- Year 16 Escalation
+    1.0924,                              !- Year 17 Escalation
+    1.0972,                              !- Year 18 Escalation
+    1.1005,                              !- Year 19 Escalation
+    1.1037,                              !- Year 20 Escalation
+    1.1070,                              !- Year 21 Escalation
+    1.1135,                              !- Year 22 Escalation
+    1.1199,                              !- Year 23 Escalation
+    1.1248,                              !- Year 24 Escalation
+    1.1313,                              !- Year 25 Escalation
+    1.1361,                              !- Year 26 Escalation
+    1.1410,                              !- Year 27 Escalation
+    1.1475,                              !- Year 28 Escalation
+    1.1524,                              !- Year 29 Escalation
+    1.1588;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Industrial-Electricity,   !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9575,                              !- Year 1 Escalation
+    0.9444,                              !- Year 2 Escalation
+    0.9530,                              !- Year 3 Escalation
+    0.9817,                              !- Year 4 Escalation
+    1.0193,                              !- Year 5 Escalation
+    1.0642,                              !- Year 6 Escalation
+    1.0922,                              !- Year 7 Escalation
+    1.1130,                              !- Year 8 Escalation
+    1.1247,                              !- Year 9 Escalation
+    1.1406,                              !- Year 10 Escalation
+    1.1503,                              !- Year 11 Escalation
+    1.1534,                              !- Year 12 Escalation
+    1.1592,                              !- Year 13 Escalation
+    1.1558,                              !- Year 14 Escalation
+    1.1537,                              !- Year 15 Escalation
+    1.1506,                              !- Year 16 Escalation
+    1.1561,                              !- Year 17 Escalation
+    1.1637,                              !- Year 18 Escalation
+    1.1703,                              !- Year 19 Escalation
+    1.1765,                              !- Year 20 Escalation
+    1.1817,                              !- Year 21 Escalation
+    1.1903,                              !- Year 22 Escalation
+    1.2100,                              !- Year 23 Escalation
+    1.2366,                              !- Year 24 Escalation
+    1.2573,                              !- Year 25 Escalation
+    1.2687,                              !- Year 26 Escalation
+    1.2777,                              !- Year 27 Escalation
+    1.2867,                              !- Year 28 Escalation
+    1.2957,                              !- Year 29 Escalation
+    1.3047;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Industrial-Distillate Oil,  !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9843,                              !- Year 1 Escalation
+    1.0314,                              !- Year 2 Escalation
+    1.0422,                              !- Year 3 Escalation
+    1.0540,                              !- Year 4 Escalation
+    1.0693,                              !- Year 5 Escalation
+    1.0879,                              !- Year 6 Escalation
+    1.1135,                              !- Year 7 Escalation
+    1.1361,                              !- Year 8 Escalation
+    1.1582,                              !- Year 9 Escalation
+    1.1807,                              !- Year 10 Escalation
+    1.2048,                              !- Year 11 Escalation
+    1.2299,                              !- Year 12 Escalation
+    1.2549,                              !- Year 13 Escalation
+    1.2800,                              !- Year 14 Escalation
+    1.3060,                              !- Year 15 Escalation
+    1.3330,                              !- Year 16 Escalation
+    1.3605,                              !- Year 17 Escalation
+    1.3915,                              !- Year 18 Escalation
+    1.4229,                              !- Year 19 Escalation
+    1.4548,                              !- Year 20 Escalation
+    1.4872,                              !- Year 21 Escalation
+    1.5201,                              !- Year 22 Escalation
+    1.5570,                              !- Year 23 Escalation
+    1.5933,                              !- Year 24 Escalation
+    1.6277,                              !- Year 25 Escalation
+    1.6621,                              !- Year 26 Escalation
+    1.6970,                              !- Year 27 Escalation
+    1.7328,                              !- Year 28 Escalation
+    1.7692,                              !- Year 29 Escalation
+    1.8070;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Industrial-Residual Oil,  !- Name
+    FuelOil#2,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0093,                              !- Year 1 Escalation
+    1.0738,                              !- Year 2 Escalation
+    1.0815,                              !- Year 3 Escalation
+    1.0970,                              !- Year 4 Escalation
+    1.1172,                              !- Year 5 Escalation
+    1.1413,                              !- Year 6 Escalation
+    1.1685,                              !- Year 7 Escalation
+    1.1964,                              !- Year 8 Escalation
+    1.2252,                              !- Year 9 Escalation
+    1.2539,                              !- Year 10 Escalation
+    1.2849,                              !- Year 11 Escalation
+    1.3168,                              !- Year 12 Escalation
+    1.3486,                              !- Year 13 Escalation
+    1.3812,                              !- Year 14 Escalation
+    1.4161,                              !- Year 15 Escalation
+    1.4534,                              !- Year 16 Escalation
+    1.4907,                              !- Year 17 Escalation
+    1.5264,                              !- Year 18 Escalation
+    1.5660,                              !- Year 19 Escalation
+    1.6064,                              !- Year 20 Escalation
+    1.6475,                              !- Year 21 Escalation
+    1.6887,                              !- Year 22 Escalation
+    1.7321,                              !- Year 23 Escalation
+    1.7989,                              !- Year 24 Escalation
+    1.8843,                              !- Year 25 Escalation
+    1.9480,                              !- Year 26 Escalation
+    2.0023,                              !- Year 27 Escalation
+    2.0590,                              !- Year 28 Escalation
+    2.1165,                              !- Year 29 Escalation
+    2.1762;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Industrial-Natural gas,   !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0194,                              !- Year 1 Escalation
+    1.2050,                              !- Year 2 Escalation
+    1.3934,                              !- Year 3 Escalation
+    1.5706,                              !- Year 4 Escalation
+    1.7091,                              !- Year 5 Escalation
+    1.8227,                              !- Year 6 Escalation
+    1.9058,                              !- Year 7 Escalation
+    1.9751,                              !- Year 8 Escalation
+    2.0360,                              !- Year 9 Escalation
+    2.0942,                              !- Year 10 Escalation
+    2.1025,                              !- Year 11 Escalation
+    2.0609,                              !- Year 12 Escalation
+    2.0028,                              !- Year 13 Escalation
+    1.9501,                              !- Year 14 Escalation
+    1.9086,                              !- Year 15 Escalation
+    1.9003,                              !- Year 16 Escalation
+    1.9141,                              !- Year 17 Escalation
+    1.9391,                              !- Year 18 Escalation
+    1.9640,                              !- Year 19 Escalation
+    2.0055,                              !- Year 20 Escalation
+    2.0388,                              !- Year 21 Escalation
+    2.1080,                              !- Year 22 Escalation
+    2.2022,                              !- Year 23 Escalation
+    2.3158,                              !- Year 24 Escalation
+    2.4183,                              !- Year 25 Escalation
+    2.4737,                              !- Year 26 Escalation
+    2.5152,                              !- Year 27 Escalation
+    2.5596,                              !- Year 28 Escalation
+    2.6039,                              !- Year 29 Escalation
+    2.6482;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    NorthEast  Industrial-Coal,          !- Name
+    Coal,                                !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0000,                              !- Year 1 Escalation
+    1.0030,                              !- Year 2 Escalation
+    1.0030,                              !- Year 3 Escalation
+    1.0090,                              !- Year 4 Escalation
+    1.0241,                              !- Year 5 Escalation
+    1.0422,                              !- Year 6 Escalation
+    1.0572,                              !- Year 7 Escalation
+    1.0633,                              !- Year 8 Escalation
+    1.0663,                              !- Year 9 Escalation
+    1.0723,                              !- Year 10 Escalation
+    1.0783,                              !- Year 11 Escalation
+    1.0843,                              !- Year 12 Escalation
+    1.0934,                              !- Year 13 Escalation
+    1.1054,                              !- Year 14 Escalation
+    1.1114,                              !- Year 15 Escalation
+    1.1235,                              !- Year 16 Escalation
+    1.1295,                              !- Year 17 Escalation
+    1.1386,                              !- Year 18 Escalation
+    1.1446,                              !- Year 19 Escalation
+    1.1506,                              !- Year 20 Escalation
+    1.1566,                              !- Year 21 Escalation
+    1.1687,                              !- Year 22 Escalation
+    1.1807,                              !- Year 23 Escalation
+    1.1928,                              !- Year 24 Escalation
+    1.2048,                              !- Year 25 Escalation
+    1.2139,                              !- Year 26 Escalation
+    1.2229,                              !- Year 27 Escalation
+    1.2349,                              !- Year 28 Escalation
+    1.2440,                              !- Year 29 Escalation
+    1.2530;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Residential-Electricity,    !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0337,                              !- Year 1 Escalation
+    1.0617,                              !- Year 2 Escalation
+    1.0651,                              !- Year 3 Escalation
+    1.0680,                              !- Year 4 Escalation
+    1.0862,                              !- Year 5 Escalation
+    1.1029,                              !- Year 6 Escalation
+    1.1135,                              !- Year 7 Escalation
+    1.1222,                              !- Year 8 Escalation
+    1.1254,                              !- Year 9 Escalation
+    1.1357,                              !- Year 10 Escalation
+    1.1429,                              !- Year 11 Escalation
+    1.1487,                              !- Year 12 Escalation
+    1.1542,                              !- Year 13 Escalation
+    1.1550,                              !- Year 14 Escalation
+    1.1559,                              !- Year 15 Escalation
+    1.1588,                              !- Year 16 Escalation
+    1.1634,                              !- Year 17 Escalation
+    1.1692,                              !- Year 18 Escalation
+    1.1746,                              !- Year 19 Escalation
+    1.1790,                              !- Year 20 Escalation
+    1.1810,                              !- Year 21 Escalation
+    1.1841,                              !- Year 22 Escalation
+    1.1914,                              !- Year 23 Escalation
+    1.2009,                              !- Year 24 Escalation
+    1.2115,                              !- Year 25 Escalation
+    1.2179,                              !- Year 26 Escalation
+    1.2228,                              !- Year 27 Escalation
+    1.2280,                              !- Year 28 Escalation
+    1.2329,                              !- Year 29 Escalation
+    1.2380;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Residential-Distillate Oil, !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9833,                              !- Year 1 Escalation
+    0.9985,                              !- Year 2 Escalation
+    0.9970,                              !- Year 3 Escalation
+    1.0086,                              !- Year 4 Escalation
+    1.0218,                              !- Year 5 Escalation
+    1.0400,                              !- Year 6 Escalation
+    1.0607,                              !- Year 7 Escalation
+    1.0824,                              !- Year 8 Escalation
+    1.1047,                              !- Year 9 Escalation
+    1.1280,                              !- Year 10 Escalation
+    1.1528,                              !- Year 11 Escalation
+    1.1796,                              !- Year 12 Escalation
+    1.2069,                              !- Year 13 Escalation
+    1.2352,                              !- Year 14 Escalation
+    1.2640,                              !- Year 15 Escalation
+    1.2944,                              !- Year 16 Escalation
+    1.3237,                              !- Year 17 Escalation
+    1.3551,                              !- Year 18 Escalation
+    1.3869,                              !- Year 19 Escalation
+    1.4193,                              !- Year 20 Escalation
+    1.4522,                              !- Year 21 Escalation
+    1.4866,                              !- Year 22 Escalation
+    1.5240,                              !- Year 23 Escalation
+    1.5599,                              !- Year 24 Escalation
+    1.5959,                              !- Year 25 Escalation
+    1.6313,                              !- Year 26 Escalation
+    1.6667,                              !- Year 27 Escalation
+    1.7036,                              !- Year 28 Escalation
+    1.7410,                              !- Year 29 Escalation
+    1.7800;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Residential-Natural gas,    !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9845,                              !- Year 1 Escalation
+    0.9835,                              !- Year 2 Escalation
+    0.9897,                              !- Year 3 Escalation
+    1.0227,                              !- Year 4 Escalation
+    1.0702,                              !- Year 5 Escalation
+    1.1054,                              !- Year 6 Escalation
+    1.1240,                              !- Year 7 Escalation
+    1.1384,                              !- Year 8 Escalation
+    1.1488,                              !- Year 9 Escalation
+    1.1622,                              !- Year 10 Escalation
+    1.1829,                              !- Year 11 Escalation
+    1.1901,                              !- Year 12 Escalation
+    1.1839,                              !- Year 13 Escalation
+    1.1818,                              !- Year 14 Escalation
+    1.1860,                              !- Year 15 Escalation
+    1.2014,                              !- Year 16 Escalation
+    1.2231,                              !- Year 17 Escalation
+    1.2428,                              !- Year 18 Escalation
+    1.2624,                              !- Year 19 Escalation
+    1.2820,                              !- Year 20 Escalation
+    1.3006,                              !- Year 21 Escalation
+    1.3140,                              !- Year 22 Escalation
+    1.3357,                              !- Year 23 Escalation
+    1.3771,                              !- Year 24 Escalation
+    1.4215,                              !- Year 25 Escalation
+    1.4432,                              !- Year 26 Escalation
+    1.4597,                              !- Year 27 Escalation
+    1.4752,                              !- Year 28 Escalation
+    1.4917,                              !- Year 29 Escalation
+    1.5093;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Residential-LPG,            !- Name
+    PropaneGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0069,                              !- Year 1 Escalation
+    1.0337,                              !- Year 2 Escalation
+    1.0433,                              !- Year 3 Escalation
+    1.0507,                              !- Year 4 Escalation
+    1.0556,                              !- Year 5 Escalation
+    1.0598,                              !- Year 6 Escalation
+    1.0641,                              !- Year 7 Escalation
+    1.0705,                              !- Year 8 Escalation
+    1.0764,                              !- Year 9 Escalation
+    1.0817,                              !- Year 10 Escalation
+    1.0892,                              !- Year 11 Escalation
+    1.0956,                              !- Year 12 Escalation
+    1.1010,                              !- Year 13 Escalation
+    1.1079,                              !- Year 14 Escalation
+    1.1143,                              !- Year 15 Escalation
+    1.1223,                              !- Year 16 Escalation
+    1.1325,                              !- Year 17 Escalation
+    1.1416,                              !- Year 18 Escalation
+    1.1501,                              !- Year 19 Escalation
+    1.1587,                              !- Year 20 Escalation
+    1.1677,                              !- Year 21 Escalation
+    1.1752,                              !- Year 22 Escalation
+    1.1838,                              !- Year 23 Escalation
+    1.1944,                              !- Year 24 Escalation
+    1.2062,                              !- Year 25 Escalation
+    1.2153,                              !- Year 26 Escalation
+    1.2238,                              !- Year 27 Escalation
+    1.2318,                              !- Year 28 Escalation
+    1.2399,                              !- Year 29 Escalation
+    1.2484;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Commercial-Electricity,     !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0213,                              !- Year 1 Escalation
+    1.0429,                              !- Year 2 Escalation
+    1.0425,                              !- Year 3 Escalation
+    1.0432,                              !- Year 4 Escalation
+    1.0583,                              !- Year 5 Escalation
+    1.0711,                              !- Year 6 Escalation
+    1.0788,                              !- Year 7 Escalation
+    1.0850,                              !- Year 8 Escalation
+    1.0850,                              !- Year 9 Escalation
+    1.0945,                              !- Year 10 Escalation
+    1.0993,                              !- Year 11 Escalation
+    1.1033,                              !- Year 12 Escalation
+    1.1103,                              !- Year 13 Escalation
+    1.1103,                              !- Year 14 Escalation
+    1.1096,                              !- Year 15 Escalation
+    1.1114,                              !- Year 16 Escalation
+    1.1154,                              !- Year 17 Escalation
+    1.1213,                              !- Year 18 Escalation
+    1.1268,                              !- Year 19 Escalation
+    1.1308,                              !- Year 20 Escalation
+    1.1323,                              !- Year 21 Escalation
+    1.1374,                              !- Year 22 Escalation
+    1.1458,                              !- Year 23 Escalation
+    1.1557,                              !- Year 24 Escalation
+    1.1671,                              !- Year 25 Escalation
+    1.1737,                              !- Year 26 Escalation
+    1.1788,                              !- Year 27 Escalation
+    1.1840,                              !- Year 28 Escalation
+    1.1887,                              !- Year 29 Escalation
+    1.1938;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Commercial-Distillate Oil,  !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9835,                              !- Year 1 Escalation
+    1.0165,                              !- Year 2 Escalation
+    1.0225,                              !- Year 3 Escalation
+    1.0339,                              !- Year 4 Escalation
+    1.0484,                              !- Year 5 Escalation
+    1.0669,                              !- Year 6 Escalation
+    1.0903,                              !- Year 7 Escalation
+    1.1133,                              !- Year 8 Escalation
+    1.1352,                              !- Year 9 Escalation
+    1.1582,                              !- Year 10 Escalation
+    1.1826,                              !- Year 11 Escalation
+    1.2091,                              !- Year 12 Escalation
+    1.2350,                              !- Year 13 Escalation
+    1.2615,                              !- Year 14 Escalation
+    1.2884,                              !- Year 15 Escalation
+    1.3169,                              !- Year 16 Escalation
+    1.3458,                              !- Year 17 Escalation
+    1.3772,                              !- Year 18 Escalation
+    1.4087,                              !- Year 19 Escalation
+    1.4411,                              !- Year 20 Escalation
+    1.4736,                              !- Year 21 Escalation
+    1.5075,                              !- Year 22 Escalation
+    1.5444,                              !- Year 23 Escalation
+    1.5808,                              !- Year 24 Escalation
+    1.6163,                              !- Year 25 Escalation
+    1.6512,                              !- Year 26 Escalation
+    1.6861,                              !- Year 27 Escalation
+    1.7226,                              !- Year 28 Escalation
+    1.7600,                              !- Year 29 Escalation
+    1.7984;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Commercial-Residual Oil,    !- Name
+    FuelOil#2,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0077,                              !- Year 1 Escalation
+    1.0720,                              !- Year 2 Escalation
+    1.0807,                              !- Year 3 Escalation
+    1.1009,                              !- Year 4 Escalation
+    1.1258,                              !- Year 5 Escalation
+    1.1556,                              !- Year 6 Escalation
+    1.1883,                              !- Year 7 Escalation
+    1.2229,                              !- Year 8 Escalation
+    1.2584,                              !- Year 9 Escalation
+    1.2949,                              !- Year 10 Escalation
+    1.3333,                              !- Year 11 Escalation
+    1.3727,                              !- Year 12 Escalation
+    1.4121,                              !- Year 13 Escalation
+    1.4534,                              !- Year 14 Escalation
+    1.4966,                              !- Year 15 Escalation
+    1.5418,                              !- Year 16 Escalation
+    1.5879,                              !- Year 17 Escalation
+    1.6321,                              !- Year 18 Escalation
+    1.6820,                              !- Year 19 Escalation
+    1.7320,                              !- Year 20 Escalation
+    1.7829,                              !- Year 21 Escalation
+    1.8329,                              !- Year 22 Escalation
+    1.8866,                              !- Year 23 Escalation
+    1.9702,                              !- Year 24 Escalation
+    2.0759,                              !- Year 25 Escalation
+    2.1547,                              !- Year 26 Escalation
+    2.2219,                              !- Year 27 Escalation
+    2.2920,                              !- Year 28 Escalation
+    2.3641,                              !- Year 29 Escalation
+    2.4380;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Commercial-Natural gas,     !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0000,                              !- Year 1 Escalation
+    0.9894,                              !- Year 2 Escalation
+    0.9800,                              !- Year 3 Escalation
+    1.0106,                              !- Year 4 Escalation
+    1.0613,                              !- Year 5 Escalation
+    1.0967,                              !- Year 6 Escalation
+    1.1167,                              !- Year 7 Escalation
+    1.1309,                              !- Year 8 Escalation
+    1.1403,                              !- Year 9 Escalation
+    1.1533,                              !- Year 10 Escalation
+    1.1733,                              !- Year 11 Escalation
+    1.1781,                              !- Year 12 Escalation
+    1.1686,                              !- Year 13 Escalation
+    1.1639,                              !- Year 14 Escalation
+    1.1651,                              !- Year 15 Escalation
+    1.1804,                              !- Year 16 Escalation
+    1.2005,                              !- Year 17 Escalation
+    1.2205,                              !- Year 18 Escalation
+    1.2394,                              !- Year 19 Escalation
+    1.2583,                              !- Year 20 Escalation
+    1.2759,                              !- Year 21 Escalation
+    1.2889,                              !- Year 22 Escalation
+    1.3101,                              !- Year 23 Escalation
+    1.3526,                              !- Year 24 Escalation
+    1.3986,                              !- Year 25 Escalation
+    1.4233,                              !- Year 26 Escalation
+    1.4410,                              !- Year 27 Escalation
+    1.4599,                              !- Year 28 Escalation
+    1.4788,                              !- Year 29 Escalation
+    1.4976;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Commercial-Coal,            !- Name
+    Coal,                                !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0062,                              !- Year 1 Escalation
+    1.0280,                              !- Year 2 Escalation
+    1.0342,                              !- Year 3 Escalation
+    1.0404,                              !- Year 4 Escalation
+    1.0559,                              !- Year 5 Escalation
+    1.0652,                              !- Year 6 Escalation
+    1.0714,                              !- Year 7 Escalation
+    1.0776,                              !- Year 8 Escalation
+    1.0807,                              !- Year 9 Escalation
+    1.0870,                              !- Year 10 Escalation
+    1.0932,                              !- Year 11 Escalation
+    1.0994,                              !- Year 12 Escalation
+    1.1056,                              !- Year 13 Escalation
+    1.1118,                              !- Year 14 Escalation
+    1.1180,                              !- Year 15 Escalation
+    1.1242,                              !- Year 16 Escalation
+    1.1304,                              !- Year 17 Escalation
+    1.1366,                              !- Year 18 Escalation
+    1.1429,                              !- Year 19 Escalation
+    1.1522,                              !- Year 20 Escalation
+    1.1584,                              !- Year 21 Escalation
+    1.1677,                              !- Year 22 Escalation
+    1.1770,                              !- Year 23 Escalation
+    1.1894,                              !- Year 24 Escalation
+    1.1988,                              !- Year 25 Escalation
+    1.2081,                              !- Year 26 Escalation
+    1.2205,                              !- Year 27 Escalation
+    1.2298,                              !- Year 28 Escalation
+    1.2391,                              !- Year 29 Escalation
+    1.2516;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Industrial-Electricity,     !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0086,                              !- Year 1 Escalation
+    1.0206,                              !- Year 2 Escalation
+    1.0153,                              !- Year 3 Escalation
+    1.0177,                              !- Year 4 Escalation
+    1.0355,                              !- Year 5 Escalation
+    1.0513,                              !- Year 6 Escalation
+    1.0619,                              !- Year 7 Escalation
+    1.0715,                              !- Year 8 Escalation
+    1.0743,                              !- Year 9 Escalation
+    1.0863,                              !- Year 10 Escalation
+    1.0950,                              !- Year 11 Escalation
+    1.1017,                              !- Year 12 Escalation
+    1.1079,                              !- Year 13 Escalation
+    1.1079,                              !- Year 14 Escalation
+    1.1079,                              !- Year 15 Escalation
+    1.1098,                              !- Year 16 Escalation
+    1.1156,                              !- Year 17 Escalation
+    1.1237,                              !- Year 18 Escalation
+    1.1309,                              !- Year 19 Escalation
+    1.1376,                              !- Year 20 Escalation
+    1.1420,                              !- Year 21 Escalation
+    1.1501,                              !- Year 22 Escalation
+    1.1626,                              !- Year 23 Escalation
+    1.1775,                              !- Year 24 Escalation
+    1.1933,                              !- Year 25 Escalation
+    1.2029,                              !- Year 26 Escalation
+    1.2106,                              !- Year 27 Escalation
+    1.2182,                              !- Year 28 Escalation
+    1.2259,                              !- Year 29 Escalation
+    1.2341;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Industrial-Distillate Oil,  !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9837,                              !- Year 1 Escalation
+    1.0000,                              !- Year 2 Escalation
+    1.0005,                              !- Year 3 Escalation
+    1.0120,                              !- Year 4 Escalation
+    1.0274,                              !- Year 5 Escalation
+    1.0456,                              !- Year 6 Escalation
+    1.0705,                              !- Year 7 Escalation
+    1.0926,                              !- Year 8 Escalation
+    1.1142,                              !- Year 9 Escalation
+    1.1368,                              !- Year 10 Escalation
+    1.1603,                              !- Year 11 Escalation
+    1.1852,                              !- Year 12 Escalation
+    1.2092,                              !- Year 13 Escalation
+    1.2337,                              !- Year 14 Escalation
+    1.2591,                              !- Year 15 Escalation
+    1.2860,                              !- Year 16 Escalation
+    1.3129,                              !- Year 17 Escalation
+    1.3431,                              !- Year 18 Escalation
+    1.3738,                              !- Year 19 Escalation
+    1.4050,                              !- Year 20 Escalation
+    1.4367,                              !- Year 21 Escalation
+    1.4688,                              !- Year 22 Escalation
+    1.5048,                              !- Year 23 Escalation
+    1.5403,                              !- Year 24 Escalation
+    1.5739,                              !- Year 25 Escalation
+    1.6075,                              !- Year 26 Escalation
+    1.6416,                              !- Year 27 Escalation
+    1.6766,                              !- Year 28 Escalation
+    1.7121,                              !- Year 29 Escalation
+    1.7490;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Industrial-Residual Oil,    !- Name
+    FuelOil#2,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0080,                              !- Year 1 Escalation
+    1.0966,                              !- Year 2 Escalation
+    1.1125,                              !- Year 3 Escalation
+    1.1325,                              !- Year 4 Escalation
+    1.1584,                              !- Year 5 Escalation
+    1.1892,                              !- Year 6 Escalation
+    1.2241,                              !- Year 7 Escalation
+    1.2600,                              !- Year 8 Escalation
+    1.2968,                              !- Year 9 Escalation
+    1.3337,                              !- Year 10 Escalation
+    1.3735,                              !- Year 11 Escalation
+    1.4143,                              !- Year 12 Escalation
+    1.4552,                              !- Year 13 Escalation
+    1.4970,                              !- Year 14 Escalation
+    1.5418,                              !- Year 15 Escalation
+    1.5896,                              !- Year 16 Escalation
+    1.6375,                              !- Year 17 Escalation
+    1.6833,                              !- Year 18 Escalation
+    1.7341,                              !- Year 19 Escalation
+    1.7859,                              !- Year 20 Escalation
+    1.8386,                              !- Year 21 Escalation
+    1.8904,                              !- Year 22 Escalation
+    1.9462,                              !- Year 23 Escalation
+    2.0329,                              !- Year 24 Escalation
+    2.1424,                              !- Year 25 Escalation
+    2.2231,                              !- Year 26 Escalation
+    2.2938,                              !- Year 27 Escalation
+    2.3665,                              !- Year 28 Escalation
+    2.4402,                              !- Year 29 Escalation
+    2.5169;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Industrial-Natural gas,     !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9797,                              !- Year 1 Escalation
+    1.0111,                              !- Year 2 Escalation
+    1.0628,                              !- Year 3 Escalation
+    1.1238,                              !- Year 4 Escalation
+    1.1959,                              !- Year 5 Escalation
+    1.2477,                              !- Year 6 Escalation
+    1.2736,                              !- Year 7 Escalation
+    1.2939,                              !- Year 8 Escalation
+    1.3068,                              !- Year 9 Escalation
+    1.3216,                              !- Year 10 Escalation
+    1.3512,                              !- Year 11 Escalation
+    1.3549,                              !- Year 12 Escalation
+    1.3383,                              !- Year 13 Escalation
+    1.3290,                              !- Year 14 Escalation
+    1.3290,                              !- Year 15 Escalation
+    1.3475,                              !- Year 16 Escalation
+    1.3789,                              !- Year 17 Escalation
+    1.4048,                              !- Year 18 Escalation
+    1.4307,                              !- Year 19 Escalation
+    1.4584,                              !- Year 20 Escalation
+    1.4843,                              !- Year 21 Escalation
+    1.5009,                              !- Year 22 Escalation
+    1.5305,                              !- Year 23 Escalation
+    1.5933,                              !- Year 24 Escalation
+    1.6599,                              !- Year 25 Escalation
+    1.6969,                              !- Year 26 Escalation
+    1.7264,                              !- Year 27 Escalation
+    1.7560,                              !- Year 28 Escalation
+    1.7856,                              !- Year 29 Escalation
+    1.8152;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    MidWest  Industrial-Coal,            !- Name
+    Coal,                                !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0234,                              !- Year 1 Escalation
+    1.0469,                              !- Year 2 Escalation
+    1.0547,                              !- Year 3 Escalation
+    1.0664,                              !- Year 4 Escalation
+    1.0859,                              !- Year 5 Escalation
+    1.1016,                              !- Year 6 Escalation
+    1.1172,                              !- Year 7 Escalation
+    1.1289,                              !- Year 8 Escalation
+    1.1367,                              !- Year 9 Escalation
+    1.1445,                              !- Year 10 Escalation
+    1.1523,                              !- Year 11 Escalation
+    1.1641,                              !- Year 12 Escalation
+    1.1719,                              !- Year 13 Escalation
+    1.1836,                              !- Year 14 Escalation
+    1.1914,                              !- Year 15 Escalation
+    1.1992,                              !- Year 16 Escalation
+    1.2070,                              !- Year 17 Escalation
+    1.2188,                              !- Year 18 Escalation
+    1.2266,                              !- Year 19 Escalation
+    1.2344,                              !- Year 20 Escalation
+    1.2422,                              !- Year 21 Escalation
+    1.2500,                              !- Year 22 Escalation
+    1.2578,                              !- Year 23 Escalation
+    1.2695,                              !- Year 24 Escalation
+    1.2813,                              !- Year 25 Escalation
+    1.2930,                              !- Year 26 Escalation
+    1.3047,                              !- Year 27 Escalation
+    1.3203,                              !- Year 28 Escalation
+    1.3320,                              !- Year 29 Escalation
+    1.3438;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Residential-Electricity,      !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0284,                              !- Year 1 Escalation
+    1.0395,                              !- Year 2 Escalation
+    1.0347,                              !- Year 3 Escalation
+    1.0365,                              !- Year 4 Escalation
+    1.0534,                              !- Year 5 Escalation
+    1.0718,                              !- Year 6 Escalation
+    1.0815,                              !- Year 7 Escalation
+    1.0911,                              !- Year 8 Escalation
+    1.0947,                              !- Year 9 Escalation
+    1.1029,                              !- Year 10 Escalation
+    1.1092,                              !- Year 11 Escalation
+    1.1153,                              !- Year 12 Escalation
+    1.1174,                              !- Year 13 Escalation
+    1.1156,                              !- Year 14 Escalation
+    1.1156,                              !- Year 15 Escalation
+    1.1189,                              !- Year 16 Escalation
+    1.1255,                              !- Year 17 Escalation
+    1.1331,                              !- Year 18 Escalation
+    1.1394,                              !- Year 19 Escalation
+    1.1457,                              !- Year 20 Escalation
+    1.1506,                              !- Year 21 Escalation
+    1.1569,                              !- Year 22 Escalation
+    1.1678,                              !- Year 23 Escalation
+    1.1804,                              !- Year 24 Escalation
+    1.1973,                              !- Year 25 Escalation
+    1.2073,                              !- Year 26 Escalation
+    1.2145,                              !- Year 27 Escalation
+    1.2221,                              !- Year 28 Escalation
+    1.2293,                              !- Year 29 Escalation
+    1.2369;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Residential-Distillate Oil,   !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9836,                              !- Year 1 Escalation
+    1.0149,                              !- Year 2 Escalation
+    1.0183,                              !- Year 3 Escalation
+    1.0278,                              !- Year 4 Escalation
+    1.0406,                              !- Year 5 Escalation
+    1.0585,                              !- Year 6 Escalation
+    1.0783,                              !- Year 7 Escalation
+    1.0996,                              !- Year 8 Escalation
+    1.1214,                              !- Year 9 Escalation
+    1.1437,                              !- Year 10 Escalation
+    1.1680,                              !- Year 11 Escalation
+    1.1923,                              !- Year 12 Escalation
+    1.2190,                              !- Year 13 Escalation
+    1.2463,                              !- Year 14 Escalation
+    1.2745,                              !- Year 15 Escalation
+    1.3033,                              !- Year 16 Escalation
+    1.3315,                              !- Year 17 Escalation
+    1.3617,                              !- Year 18 Escalation
+    1.3930,                              !- Year 19 Escalation
+    1.4247,                              !- Year 20 Escalation
+    1.4569,                              !- Year 21 Escalation
+    1.4906,                              !- Year 22 Escalation
+    1.5268,                              !- Year 23 Escalation
+    1.5629,                              !- Year 24 Escalation
+    1.5976,                              !- Year 25 Escalation
+    1.6323,                              !- Year 26 Escalation
+    1.6670,                              !- Year 27 Escalation
+    1.7032,                              !- Year 28 Escalation
+    1.7398,                              !- Year 29 Escalation
+    1.7780;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Residential-Natural gas,      !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9870,                              !- Year 1 Escalation
+    0.9724,                              !- Year 2 Escalation
+    0.9757,                              !- Year 3 Escalation
+    1.0097,                              !- Year 4 Escalation
+    1.0575,                              !- Year 5 Escalation
+    1.0908,                              !- Year 6 Escalation
+    1.1062,                              !- Year 7 Escalation
+    1.1224,                              !- Year 8 Escalation
+    1.1402,                              !- Year 9 Escalation
+    1.1556,                              !- Year 10 Escalation
+    1.1734,                              !- Year 11 Escalation
+    1.1815,                              !- Year 12 Escalation
+    1.1840,                              !- Year 13 Escalation
+    1.1888,                              !- Year 14 Escalation
+    1.1840,                              !- Year 15 Escalation
+    1.2018,                              !- Year 16 Escalation
+    1.2196,                              !- Year 17 Escalation
+    1.2407,                              !- Year 18 Escalation
+    1.2585,                              !- Year 19 Escalation
+    1.2731,                              !- Year 20 Escalation
+    1.2982,                              !- Year 21 Escalation
+    1.3314,                              !- Year 22 Escalation
+    1.3655,                              !- Year 23 Escalation
+    1.4019,                              !- Year 24 Escalation
+    1.4522,                              !- Year 25 Escalation
+    1.4757,                              !- Year 26 Escalation
+    1.4887,                              !- Year 27 Escalation
+    1.5008,                              !- Year 28 Escalation
+    1.5138,                              !- Year 29 Escalation
+    1.5276;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Residential-LPG,              !- Name
+    PropaneGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0090,                              !- Year 1 Escalation
+    1.0363,                              !- Year 2 Escalation
+    1.0465,                              !- Year 3 Escalation
+    1.0546,                              !- Year 4 Escalation
+    1.0593,                              !- Year 5 Escalation
+    1.0640,                              !- Year 6 Escalation
+    1.0687,                              !- Year 7 Escalation
+    1.0755,                              !- Year 8 Escalation
+    1.0815,                              !- Year 9 Escalation
+    1.0879,                              !- Year 10 Escalation
+    1.0956,                              !- Year 11 Escalation
+    1.1020,                              !- Year 12 Escalation
+    1.1079,                              !- Year 13 Escalation
+    1.1152,                              !- Year 14 Escalation
+    1.1220,                              !- Year 15 Escalation
+    1.1305,                              !- Year 16 Escalation
+    1.1412,                              !- Year 17 Escalation
+    1.1506,                              !- Year 18 Escalation
+    1.1596,                              !- Year 19 Escalation
+    1.1689,                              !- Year 20 Escalation
+    1.1779,                              !- Year 21 Escalation
+    1.1864,                              !- Year 22 Escalation
+    1.1954,                              !- Year 23 Escalation
+    1.2069,                              !- Year 24 Escalation
+    1.2193,                              !- Year 25 Escalation
+    1.2291,                              !- Year 26 Escalation
+    1.2376,                              !- Year 27 Escalation
+    1.2462,                              !- Year 28 Escalation
+    1.2551,                              !- Year 29 Escalation
+    1.2637;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Commercial-Electricity,       !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0138,                              !- Year 1 Escalation
+    1.0184,                              !- Year 2 Escalation
+    1.0106,                              !- Year 3 Escalation
+    1.0117,                              !- Year 4 Escalation
+    1.0265,                              !- Year 5 Escalation
+    1.0445,                              !- Year 6 Escalation
+    1.0537,                              !- Year 7 Escalation
+    1.0636,                              !- Year 8 Escalation
+    1.0657,                              !- Year 9 Escalation
+    1.0734,                              !- Year 10 Escalation
+    1.0784,                              !- Year 11 Escalation
+    1.0837,                              !- Year 12 Escalation
+    1.0862,                              !- Year 13 Escalation
+    1.0833,                              !- Year 14 Escalation
+    1.0816,                              !- Year 15 Escalation
+    1.0837,                              !- Year 16 Escalation
+    1.0890,                              !- Year 17 Escalation
+    1.0964,                              !- Year 18 Escalation
+    1.1024,                              !- Year 19 Escalation
+    1.1084,                              !- Year 20 Escalation
+    1.1137,                              !- Year 21 Escalation
+    1.1204,                              !- Year 22 Escalation
+    1.1317,                              !- Year 23 Escalation
+    1.1458,                              !- Year 24 Escalation
+    1.1635,                              !- Year 25 Escalation
+    1.1737,                              !- Year 26 Escalation
+    1.1808,                              !- Year 27 Escalation
+    1.1879,                              !- Year 28 Escalation
+    1.1953,                              !- Year 29 Escalation
+    1.2023;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Commercial-Distillate Oil,    !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9839,                              !- Year 1 Escalation
+    1.0181,                              !- Year 2 Escalation
+    1.0236,                              !- Year 3 Escalation
+    1.0351,                              !- Year 4 Escalation
+    1.0497,                              !- Year 5 Escalation
+    1.0682,                              !- Year 6 Escalation
+    1.0918,                              !- Year 7 Escalation
+    1.1144,                              !- Year 8 Escalation
+    1.1370,                              !- Year 9 Escalation
+    1.1601,                              !- Year 10 Escalation
+    1.1846,                              !- Year 11 Escalation
+    1.2097,                              !- Year 12 Escalation
+    1.2363,                              !- Year 13 Escalation
+    1.2629,                              !- Year 14 Escalation
+    1.2900,                              !- Year 15 Escalation
+    1.3186,                              !- Year 16 Escalation
+    1.3477,                              !- Year 17 Escalation
+    1.3793,                              !- Year 18 Escalation
+    1.4109,                              !- Year 19 Escalation
+    1.4431,                              !- Year 20 Escalation
+    1.4757,                              !- Year 21 Escalation
+    1.5103,                              !- Year 22 Escalation
+    1.5474,                              !- Year 23 Escalation
+    1.5840,                              !- Year 24 Escalation
+    1.6192,                              !- Year 25 Escalation
+    1.6543,                              !- Year 26 Escalation
+    1.6899,                              !- Year 27 Escalation
+    1.7265,                              !- Year 28 Escalation
+    1.7637,                              !- Year 29 Escalation
+    1.8023;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Commercial-Residual Oil,      !- Name
+    FuelOil#2,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0077,                              !- Year 1 Escalation
+    1.0692,                              !- Year 2 Escalation
+    1.0752,                              !- Year 3 Escalation
+    1.0932,                              !- Year 4 Escalation
+    1.1154,                              !- Year 5 Escalation
+    1.1419,                              !- Year 6 Escalation
+    1.1709,                              !- Year 7 Escalation
+    1.2017,                              !- Year 8 Escalation
+    1.2333,                              !- Year 9 Escalation
+    1.2658,                              !- Year 10 Escalation
+    1.3000,                              !- Year 11 Escalation
+    1.3342,                              !- Year 12 Escalation
+    1.3692,                              !- Year 13 Escalation
+    1.4060,                              !- Year 14 Escalation
+    1.4444,                              !- Year 15 Escalation
+    1.4855,                              !- Year 16 Escalation
+    1.5265,                              !- Year 17 Escalation
+    1.5658,                              !- Year 18 Escalation
+    1.6094,                              !- Year 19 Escalation
+    1.6538,                              !- Year 20 Escalation
+    1.6991,                              !- Year 21 Escalation
+    1.7436,                              !- Year 22 Escalation
+    1.7915,                              !- Year 23 Escalation
+    1.8658,                              !- Year 24 Escalation
+    1.9598,                              !- Year 25 Escalation
+    2.0299,                              !- Year 26 Escalation
+    2.0897,                              !- Year 27 Escalation
+    2.1521,                              !- Year 28 Escalation
+    2.2154,                              !- Year 29 Escalation
+    2.2812;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Commercial-Natural gas,       !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9821,                              !- Year 1 Escalation
+    0.9493,                              !- Year 2 Escalation
+    0.9363,                              !- Year 3 Escalation
+    0.9692,                              !- Year 4 Escalation
+    1.0209,                              !- Year 5 Escalation
+    1.0567,                              !- Year 6 Escalation
+    1.0726,                              !- Year 7 Escalation
+    1.0905,                              !- Year 8 Escalation
+    1.1085,                              !- Year 9 Escalation
+    1.1234,                              !- Year 10 Escalation
+    1.1403,                              !- Year 11 Escalation
+    1.1453,                              !- Year 12 Escalation
+    1.1423,                              !- Year 13 Escalation
+    1.1423,                              !- Year 14 Escalation
+    1.1313,                              !- Year 15 Escalation
+    1.1483,                              !- Year 16 Escalation
+    1.1652,                              !- Year 17 Escalation
+    1.1841,                              !- Year 18 Escalation
+    1.2000,                              !- Year 19 Escalation
+    1.2109,                              !- Year 20 Escalation
+    1.2348,                              !- Year 21 Escalation
+    1.2667,                              !- Year 22 Escalation
+    1.2975,                              !- Year 23 Escalation
+    1.3323,                              !- Year 24 Escalation
+    1.3871,                              !- Year 25 Escalation
+    1.4139,                              !- Year 26 Escalation
+    1.4289,                              !- Year 27 Escalation
+    1.4448,                              !- Year 28 Escalation
+    1.4607,                              !- Year 29 Escalation
+    1.4776;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Commercial-Coal,              !- Name
+    Coal,                                !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0065,                              !- Year 1 Escalation
+    1.0174,                              !- Year 2 Escalation
+    1.0174,                              !- Year 3 Escalation
+    1.0261,                              !- Year 4 Escalation
+    1.0392,                              !- Year 5 Escalation
+    1.0545,                              !- Year 6 Escalation
+    1.0654,                              !- Year 7 Escalation
+    1.0697,                              !- Year 8 Escalation
+    1.0719,                              !- Year 9 Escalation
+    1.0763,                              !- Year 10 Escalation
+    1.0806,                              !- Year 11 Escalation
+    1.0850,                              !- Year 12 Escalation
+    1.0915,                              !- Year 13 Escalation
+    1.1002,                              !- Year 14 Escalation
+    1.1068,                              !- Year 15 Escalation
+    1.1155,                              !- Year 16 Escalation
+    1.1198,                              !- Year 17 Escalation
+    1.1285,                              !- Year 18 Escalation
+    1.1329,                              !- Year 19 Escalation
+    1.1373,                              !- Year 20 Escalation
+    1.1438,                              !- Year 21 Escalation
+    1.1547,                              !- Year 22 Escalation
+    1.1656,                              !- Year 23 Escalation
+    1.1765,                              !- Year 24 Escalation
+    1.1852,                              !- Year 25 Escalation
+    1.1939,                              !- Year 26 Escalation
+    1.2004,                              !- Year 27 Escalation
+    1.2070,                              !- Year 28 Escalation
+    1.2157,                              !- Year 29 Escalation
+    1.2222;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Industrial-Electricity,       !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0031,                              !- Year 1 Escalation
+    1.0016,                              !- Year 2 Escalation
+    0.9901,                              !- Year 3 Escalation
+    0.9912,                              !- Year 4 Escalation
+    1.0067,                              !- Year 5 Escalation
+    1.0223,                              !- Year 6 Escalation
+    1.0301,                              !- Year 7 Escalation
+    1.0389,                              !- Year 8 Escalation
+    1.0441,                              !- Year 9 Escalation
+    1.0545,                              !- Year 10 Escalation
+    1.0628,                              !- Year 11 Escalation
+    1.0706,                              !- Year 12 Escalation
+    1.0727,                              !- Year 13 Escalation
+    1.0717,                              !- Year 14 Escalation
+    1.0717,                              !- Year 15 Escalation
+    1.0768,                              !- Year 16 Escalation
+    1.0857,                              !- Year 17 Escalation
+    1.0955,                              !- Year 18 Escalation
+    1.1038,                              !- Year 19 Escalation
+    1.1127,                              !- Year 20 Escalation
+    1.1210,                              !- Year 21 Escalation
+    1.1314,                              !- Year 22 Escalation
+    1.1454,                              !- Year 23 Escalation
+    1.1636,                              !- Year 24 Escalation
+    1.1848,                              !- Year 25 Escalation
+    1.1983,                              !- Year 26 Escalation
+    1.2092,                              !- Year 27 Escalation
+    1.2196,                              !- Year 28 Escalation
+    1.2305,                              !- Year 29 Escalation
+    1.2409;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Industrial-Distillate Oil,    !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9832,                              !- Year 1 Escalation
+    1.0054,                              !- Year 2 Escalation
+    1.0074,                              !- Year 3 Escalation
+    1.0197,                              !- Year 4 Escalation
+    1.0350,                              !- Year 5 Escalation
+    1.0542,                              !- Year 6 Escalation
+    1.0798,                              !- Year 7 Escalation
+    1.1025,                              !- Year 8 Escalation
+    1.1242,                              !- Year 9 Escalation
+    1.1479,                              !- Year 10 Escalation
+    1.1720,                              !- Year 11 Escalation
+    1.1966,                              !- Year 12 Escalation
+    1.2213,                              !- Year 13 Escalation
+    1.2469,                              !- Year 14 Escalation
+    1.2725,                              !- Year 15 Escalation
+    1.3006,                              !- Year 16 Escalation
+    1.3292,                              !- Year 17 Escalation
+    1.3608,                              !- Year 18 Escalation
+    1.3918,                              !- Year 19 Escalation
+    1.4239,                              !- Year 20 Escalation
+    1.4564,                              !- Year 21 Escalation
+    1.4899,                              !- Year 22 Escalation
+    1.5269,                              !- Year 23 Escalation
+    1.5633,                              !- Year 24 Escalation
+    1.5978,                              !- Year 25 Escalation
+    1.6323,                              !- Year 26 Escalation
+    1.6673,                              !- Year 27 Escalation
+    1.7033,                              !- Year 28 Escalation
+    1.7398,                              !- Year 29 Escalation
+    1.7777;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Industrial-Residual Oil,      !- Name
+    FuelOil#2,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0093,                              !- Year 1 Escalation
+    1.0729,                              !- Year 2 Escalation
+    1.0805,                              !- Year 3 Escalation
+    1.0975,                              !- Year 4 Escalation
+    1.1195,                              !- Year 5 Escalation
+    1.1466,                              !- Year 6 Escalation
+    1.1754,                              !- Year 7 Escalation
+    1.2059,                              !- Year 8 Escalation
+    1.2373,                              !- Year 9 Escalation
+    1.2686,                              !- Year 10 Escalation
+    1.3025,                              !- Year 11 Escalation
+    1.3373,                              !- Year 12 Escalation
+    1.3720,                              !- Year 13 Escalation
+    1.4076,                              !- Year 14 Escalation
+    1.4458,                              !- Year 15 Escalation
+    1.4864,                              !- Year 16 Escalation
+    1.5271,                              !- Year 17 Escalation
+    1.5661,                              !- Year 18 Escalation
+    1.6093,                              !- Year 19 Escalation
+    1.6542,                              !- Year 20 Escalation
+    1.6983,                              !- Year 21 Escalation
+    1.7432,                              !- Year 22 Escalation
+    1.7907,                              !- Year 23 Escalation
+    1.8636,                              !- Year 24 Escalation
+    1.9568,                              !- Year 25 Escalation
+    2.0263,                              !- Year 26 Escalation
+    2.0856,                              !- Year 27 Escalation
+    2.1475,                              !- Year 28 Escalation
+    2.2102,                              !- Year 29 Escalation
+    2.2754;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Industrial-Natural gas,       !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9577,                              !- Year 1 Escalation
+    1.0045,                              !- Year 2 Escalation
+    1.0802,                              !- Year 3 Escalation
+    1.1648,                              !- Year 4 Escalation
+    1.2673,                              !- Year 5 Escalation
+    1.3274,                              !- Year 6 Escalation
+    1.3497,                              !- Year 7 Escalation
+    1.3764,                              !- Year 8 Escalation
+    1.4009,                              !- Year 9 Escalation
+    1.4298,                              !- Year 10 Escalation
+    1.4655,                              !- Year 11 Escalation
+    1.4722,                              !- Year 12 Escalation
+    1.4566,                              !- Year 13 Escalation
+    1.4499,                              !- Year 14 Escalation
+    1.4432,                              !- Year 15 Escalation
+    1.4788,                              !- Year 16 Escalation
+    1.5167,                              !- Year 17 Escalation
+    1.5546,                              !- Year 18 Escalation
+    1.5924,                              !- Year 19 Escalation
+    1.6192,                              !- Year 20 Escalation
+    1.6548,                              !- Year 21 Escalation
+    1.6927,                              !- Year 22 Escalation
+    1.7305,                              !- Year 23 Escalation
+    1.7951,                              !- Year 24 Escalation
+    1.8998,                              !- Year 25 Escalation
+    1.9532,                              !- Year 26 Escalation
+    1.9866,                              !- Year 27 Escalation
+    2.0223,                              !- Year 28 Escalation
+    2.0579,                              !- Year 29 Escalation
+    2.0935;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    South  Industrial-Coal,              !- Name
+    Coal,                                !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0103,                              !- Year 1 Escalation
+    1.0256,                              !- Year 2 Escalation
+    1.0282,                              !- Year 3 Escalation
+    1.0333,                              !- Year 4 Escalation
+    1.0462,                              !- Year 5 Escalation
+    1.0615,                              !- Year 6 Escalation
+    1.0744,                              !- Year 7 Escalation
+    1.0795,                              !- Year 8 Escalation
+    1.0821,                              !- Year 9 Escalation
+    1.0872,                              !- Year 10 Escalation
+    1.0923,                              !- Year 11 Escalation
+    1.0974,                              !- Year 12 Escalation
+    1.1051,                              !- Year 13 Escalation
+    1.1128,                              !- Year 14 Escalation
+    1.1205,                              !- Year 15 Escalation
+    1.1308,                              !- Year 16 Escalation
+    1.1385,                              !- Year 17 Escalation
+    1.1462,                              !- Year 18 Escalation
+    1.1513,                              !- Year 19 Escalation
+    1.1564,                              !- Year 20 Escalation
+    1.1641,                              !- Year 21 Escalation
+    1.1744,                              !- Year 22 Escalation
+    1.1846,                              !- Year 23 Escalation
+    1.1949,                              !- Year 24 Escalation
+    1.2051,                              !- Year 25 Escalation
+    1.2128,                              !- Year 26 Escalation
+    1.2231,                              !- Year 27 Escalation
+    1.2308,                              !- Year 28 Escalation
+    1.2385,                              !- Year 29 Escalation
+    1.2487;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Residential-Electricity,       !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0335,                              !- Year 1 Escalation
+    1.0516,                              !- Year 2 Escalation
+    1.0443,                              !- Year 3 Escalation
+    1.0397,                              !- Year 4 Escalation
+    1.0457,                              !- Year 5 Escalation
+    1.0539,                              !- Year 6 Escalation
+    1.0596,                              !- Year 7 Escalation
+    1.0610,                              !- Year 8 Escalation
+    1.0624,                              !- Year 9 Escalation
+    1.0687,                              !- Year 10 Escalation
+    1.0743,                              !- Year 11 Escalation
+    1.0772,                              !- Year 12 Escalation
+    1.0755,                              !- Year 13 Escalation
+    1.0718,                              !- Year 14 Escalation
+    1.0721,                              !- Year 15 Escalation
+    1.0740,                              !- Year 16 Escalation
+    1.0772,                              !- Year 17 Escalation
+    1.0817,                              !- Year 18 Escalation
+    1.0851,                              !- Year 19 Escalation
+    1.0891,                              !- Year 20 Escalation
+    1.0939,                              !- Year 21 Escalation
+    1.1004,                              !- Year 22 Escalation
+    1.1075,                              !- Year 23 Escalation
+    1.1140,                              !- Year 24 Escalation
+    1.1191,                              !- Year 25 Escalation
+    1.1234,                              !- Year 26 Escalation
+    1.1274,                              !- Year 27 Escalation
+    1.1313,                              !- Year 28 Escalation
+    1.1353,                              !- Year 29 Escalation
+    1.1393;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Residential-Distillate Oil,    !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9841,                              !- Year 1 Escalation
+    1.0039,                              !- Year 2 Escalation
+    1.0043,                              !- Year 3 Escalation
+    1.0159,                              !- Year 4 Escalation
+    1.0304,                              !- Year 5 Escalation
+    1.0478,                              !- Year 6 Escalation
+    1.0675,                              !- Year 7 Escalation
+    1.0883,                              !- Year 8 Escalation
+    1.1095,                              !- Year 9 Escalation
+    1.1317,                              !- Year 10 Escalation
+    1.1558,                              !- Year 11 Escalation
+    1.1814,                              !- Year 12 Escalation
+    1.2074,                              !- Year 13 Escalation
+    1.2344,                              !- Year 14 Escalation
+    1.2619,                              !- Year 15 Escalation
+    1.2904,                              !- Year 16 Escalation
+    1.3189,                              !- Year 17 Escalation
+    1.3483,                              !- Year 18 Escalation
+    1.3792,                              !- Year 19 Escalation
+    1.4096,                              !- Year 20 Escalation
+    1.4409,                              !- Year 21 Escalation
+    1.4742,                              !- Year 22 Escalation
+    1.5094,                              !- Year 23 Escalation
+    1.5441,                              !- Year 24 Escalation
+    1.5784,                              !- Year 25 Escalation
+    1.6122,                              !- Year 26 Escalation
+    1.6459,                              !- Year 27 Escalation
+    1.6811,                              !- Year 28 Escalation
+    1.7168,                              !- Year 29 Escalation
+    1.7540;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Residential-Natural gas,       !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9709,                              !- Year 1 Escalation
+    0.9700,                              !- Year 2 Escalation
+    0.9822,                              !- Year 3 Escalation
+    1.0178,                              !- Year 4 Escalation
+    1.0619,                              !- Year 5 Escalation
+    1.0965,                              !- Year 6 Escalation
+    1.1172,                              !- Year 7 Escalation
+    1.1340,                              !- Year 8 Escalation
+    1.1453,                              !- Year 9 Escalation
+    1.1649,                              !- Year 10 Escalation
+    1.1874,                              !- Year 11 Escalation
+    1.1949,                              !- Year 12 Escalation
+    1.1893,                              !- Year 13 Escalation
+    1.1874,                              !- Year 14 Escalation
+    1.1912,                              !- Year 15 Escalation
+    1.2024,                              !- Year 16 Escalation
+    1.2202,                              !- Year 17 Escalation
+    1.2381,                              !- Year 18 Escalation
+    1.2540,                              !- Year 19 Escalation
+    1.2737,                              !- Year 20 Escalation
+    1.2952,                              !- Year 21 Escalation
+    1.3102,                              !- Year 22 Escalation
+    1.3327,                              !- Year 23 Escalation
+    1.3646,                              !- Year 24 Escalation
+    1.3955,                              !- Year 25 Escalation
+    1.4133,                              !- Year 26 Escalation
+    1.4283,                              !- Year 27 Escalation
+    1.4424,                              !- Year 28 Escalation
+    1.4583,                              !- Year 29 Escalation
+    1.4733;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Residential-LPG,               !- Name
+    PropaneGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0103,                              !- Year 1 Escalation
+    1.0384,                              !- Year 2 Escalation
+    1.0487,                              !- Year 3 Escalation
+    1.0568,                              !- Year 4 Escalation
+    1.0617,                              !- Year 5 Escalation
+    1.0662,                              !- Year 6 Escalation
+    1.0711,                              !- Year 7 Escalation
+    1.0778,                              !- Year 8 Escalation
+    1.0840,                              !- Year 9 Escalation
+    1.0899,                              !- Year 10 Escalation
+    1.0975,                              !- Year 11 Escalation
+    1.1042,                              !- Year 12 Escalation
+    1.1104,                              !- Year 13 Escalation
+    1.1167,                              !- Year 14 Escalation
+    1.1238,                              !- Year 15 Escalation
+    1.1323,                              !- Year 16 Escalation
+    1.1426,                              !- Year 17 Escalation
+    1.1515,                              !- Year 18 Escalation
+    1.1605,                              !- Year 19 Escalation
+    1.1694,                              !- Year 20 Escalation
+    1.1788,                              !- Year 21 Escalation
+    1.1869,                              !- Year 22 Escalation
+    1.1954,                              !- Year 23 Escalation
+    1.2061,                              !- Year 24 Escalation
+    1.2186,                              !- Year 25 Escalation
+    1.2280,                              !- Year 26 Escalation
+    1.2365,                              !- Year 27 Escalation
+    1.2450,                              !- Year 28 Escalation
+    1.2535,                              !- Year 29 Escalation
+    1.2620;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Commercial-Electricity,        !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0278,                              !- Year 1 Escalation
+    1.0420,                              !- Year 2 Escalation
+    1.0309,                              !- Year 3 Escalation
+    1.0227,                              !- Year 4 Escalation
+    1.0234,                              !- Year 5 Escalation
+    1.0272,                              !- Year 6 Escalation
+    1.0290,                              !- Year 7 Escalation
+    1.0268,                              !- Year 8 Escalation
+    1.0243,                              !- Year 9 Escalation
+    1.0265,                              !- Year 10 Escalation
+    1.0306,                              !- Year 11 Escalation
+    1.0322,                              !- Year 12 Escalation
+    1.0278,                              !- Year 13 Escalation
+    1.0205,                              !- Year 14 Escalation
+    1.0177,                              !- Year 15 Escalation
+    1.0164,                              !- Year 16 Escalation
+    1.0164,                              !- Year 17 Escalation
+    1.0186,                              !- Year 18 Escalation
+    1.0199,                              !- Year 19 Escalation
+    1.0221,                              !- Year 20 Escalation
+    1.0249,                              !- Year 21 Escalation
+    1.0297,                              !- Year 22 Escalation
+    1.0347,                              !- Year 23 Escalation
+    1.0398,                              !- Year 24 Escalation
+    1.0452,                              !- Year 25 Escalation
+    1.0477,                              !- Year 26 Escalation
+    1.0493,                              !- Year 27 Escalation
+    1.0508,                              !- Year 28 Escalation
+    1.0527,                              !- Year 29 Escalation
+    1.0543;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Commercial-Distillate Oil,     !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9832,                              !- Year 1 Escalation
+    1.0251,                              !- Year 2 Escalation
+    1.0340,                              !- Year 3 Escalation
+    1.0468,                              !- Year 4 Escalation
+    1.0621,                              !- Year 5 Escalation
+    1.0809,                              !- Year 6 Escalation
+    1.1040,                              !- Year 7 Escalation
+    1.1262,                              !- Year 8 Escalation
+    1.1484,                              !- Year 9 Escalation
+    1.1716,                              !- Year 10 Escalation
+    1.1958,                              !- Year 11 Escalation
+    1.2214,                              !- Year 12 Escalation
+    1.2475,                              !- Year 13 Escalation
+    1.2742,                              !- Year 14 Escalation
+    1.3008,                              !- Year 15 Escalation
+    1.3284,                              !- Year 16 Escalation
+    1.3575,                              !- Year 17 Escalation
+    1.3881,                              !- Year 18 Escalation
+    1.4196,                              !- Year 19 Escalation
+    1.4507,                              !- Year 20 Escalation
+    1.4827,                              !- Year 21 Escalation
+    1.5163,                              !- Year 22 Escalation
+    1.5528,                              !- Year 23 Escalation
+    1.5883,                              !- Year 24 Escalation
+    1.6233,                              !- Year 25 Escalation
+    1.6578,                              !- Year 26 Escalation
+    1.6923,                              !- Year 27 Escalation
+    1.7283,                              !- Year 28 Escalation
+    1.7653,                              !- Year 29 Escalation
+    1.8033;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Commercial-Residual Oil,       !- Name
+    FuelOil#2,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0082,                              !- Year 1 Escalation
+    1.1052,                              !- Year 2 Escalation
+    1.1256,                              !- Year 3 Escalation
+    1.1461,                              !- Year 4 Escalation
+    1.1726,                              !- Year 5 Escalation
+    1.2053,                              !- Year 6 Escalation
+    1.2400,                              !- Year 7 Escalation
+    1.2768,                              !- Year 8 Escalation
+    1.3146,                              !- Year 9 Escalation
+    1.3524,                              !- Year 10 Escalation
+    1.3943,                              !- Year 11 Escalation
+    1.4351,                              !- Year 12 Escalation
+    1.4770,                              !- Year 13 Escalation
+    1.5209,                              !- Year 14 Escalation
+    1.5669,                              !- Year 15 Escalation
+    1.6159,                              !- Year 16 Escalation
+    1.6650,                              !- Year 17 Escalation
+    1.7120,                              !- Year 18 Escalation
+    1.7640,                              !- Year 19 Escalation
+    1.8182,                              !- Year 20 Escalation
+    1.8713,                              !- Year 21 Escalation
+    1.9254,                              !- Year 22 Escalation
+    1.9826,                              !- Year 23 Escalation
+    2.0705,                              !- Year 24 Escalation
+    2.1839,                              !- Year 25 Escalation
+    2.2666,                              !- Year 26 Escalation
+    2.3381,                              !- Year 27 Escalation
+    2.4127,                              !- Year 28 Escalation
+    2.4893,                              !- Year 29 Escalation
+    2.5679;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Commercial-Natural gas,        !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0124,                              !- Year 1 Escalation
+    1.0135,                              !- Year 2 Escalation
+    1.0124,                              !- Year 3 Escalation
+    1.0495,                              !- Year 4 Escalation
+    1.0991,                              !- Year 5 Escalation
+    1.1385,                              !- Year 6 Escalation
+    1.1622,                              !- Year 7 Escalation
+    1.1824,                              !- Year 8 Escalation
+    1.1948,                              !- Year 9 Escalation
+    1.2151,                              !- Year 10 Escalation
+    1.2410,                              !- Year 11 Escalation
+    1.2477,                              !- Year 12 Escalation
+    1.2387,                              !- Year 13 Escalation
+    1.2331,                              !- Year 14 Escalation
+    1.2365,                              !- Year 15 Escalation
+    1.2466,                              !- Year 16 Escalation
+    1.2669,                              !- Year 17 Escalation
+    1.2838,                              !- Year 18 Escalation
+    1.2995,                              !- Year 19 Escalation
+    1.3221,                              !- Year 20 Escalation
+    1.3446,                              !- Year 21 Escalation
+    1.3581,                              !- Year 22 Escalation
+    1.3829,                              !- Year 23 Escalation
+    1.4189,                              !- Year 24 Escalation
+    1.4538,                              !- Year 25 Escalation
+    1.4741,                              !- Year 26 Escalation
+    1.4921,                              !- Year 27 Escalation
+    1.5101,                              !- Year 28 Escalation
+    1.5282,                              !- Year 29 Escalation
+    1.5462;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Commercial-Coal,               !- Name
+    Coal,                                !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0224,                              !- Year 1 Escalation
+    1.0399,                              !- Year 2 Escalation
+    1.0474,                              !- Year 3 Escalation
+    1.0549,                              !- Year 4 Escalation
+    1.0623,                              !- Year 5 Escalation
+    1.0723,                              !- Year 6 Escalation
+    1.0823,                              !- Year 7 Escalation
+    1.0923,                              !- Year 8 Escalation
+    1.1072,                              !- Year 9 Escalation
+    1.1147,                              !- Year 10 Escalation
+    1.1197,                              !- Year 11 Escalation
+    1.1347,                              !- Year 12 Escalation
+    1.1421,                              !- Year 13 Escalation
+    1.1571,                              !- Year 14 Escalation
+    1.1671,                              !- Year 15 Escalation
+    1.1721,                              !- Year 16 Escalation
+    1.1870,                              !- Year 17 Escalation
+    1.1970,                              !- Year 18 Escalation
+    1.2120,                              !- Year 19 Escalation
+    1.2244,                              !- Year 20 Escalation
+    1.2319,                              !- Year 21 Escalation
+    1.2494,                              !- Year 22 Escalation
+    1.2618,                              !- Year 23 Escalation
+    1.2818,                              !- Year 24 Escalation
+    1.2943,                              !- Year 25 Escalation
+    1.3017,                              !- Year 26 Escalation
+    1.3092,                              !- Year 27 Escalation
+    1.3192,                              !- Year 28 Escalation
+    1.3267,                              !- Year 29 Escalation
+    1.3367;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Industrial-Electricity,        !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0197,                              !- Year 1 Escalation
+    1.0231,                              !- Year 2 Escalation
+    1.0103,                              !- Year 3 Escalation
+    1.0069,                              !- Year 4 Escalation
+    1.0108,                              !- Year 5 Escalation
+    1.0182,                              !- Year 6 Escalation
+    1.0226,                              !- Year 7 Escalation
+    1.0256,                              !- Year 8 Escalation
+    1.0265,                              !- Year 9 Escalation
+    1.0344,                              !- Year 10 Escalation
+    1.0413,                              !- Year 11 Escalation
+    1.0447,                              !- Year 12 Escalation
+    1.0413,                              !- Year 13 Escalation
+    1.0369,                              !- Year 14 Escalation
+    1.0374,                              !- Year 15 Escalation
+    1.0393,                              !- Year 16 Escalation
+    1.0428,                              !- Year 17 Escalation
+    1.0487,                              !- Year 18 Escalation
+    1.0536,                              !- Year 19 Escalation
+    1.0590,                              !- Year 20 Escalation
+    1.0649,                              !- Year 21 Escalation
+    1.0737,                              !- Year 22 Escalation
+    1.0841,                              !- Year 23 Escalation
+    1.0929,                              !- Year 24 Escalation
+    1.1008,                              !- Year 25 Escalation
+    1.1067,                              !- Year 26 Escalation
+    1.1121,                              !- Year 27 Escalation
+    1.1175,                              !- Year 28 Escalation
+    1.1229,                              !- Year 29 Escalation
+    1.1288;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Industrial-Distillate Oil,     !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9838,                              !- Year 1 Escalation
+    0.9951,                              !- Year 2 Escalation
+    0.9951,                              !- Year 3 Escalation
+    1.0074,                              !- Year 4 Escalation
+    1.0236,                              !- Year 5 Escalation
+    1.0423,                              !- Year 6 Escalation
+    1.0678,                              !- Year 7 Escalation
+    1.0909,                              !- Year 8 Escalation
+    1.1130,                              !- Year 9 Escalation
+    1.1371,                              !- Year 10 Escalation
+    1.1612,                              !- Year 11 Escalation
+    1.1853,                              !- Year 12 Escalation
+    1.2118,                              !- Year 13 Escalation
+    1.2373,                              !- Year 14 Escalation
+    1.2619,                              !- Year 15 Escalation
+    1.2894,                              !- Year 16 Escalation
+    1.3184,                              !- Year 17 Escalation
+    1.3484,                              !- Year 18 Escalation
+    1.3803,                              !- Year 19 Escalation
+    1.4108,                              !- Year 20 Escalation
+    1.4428,                              !- Year 21 Escalation
+    1.4767,                              !- Year 22 Escalation
+    1.5130,                              !- Year 23 Escalation
+    1.5479,                              !- Year 24 Escalation
+    1.5833,                              !- Year 25 Escalation
+    1.6177,                              !- Year 26 Escalation
+    1.6521,                              !- Year 27 Escalation
+    1.6880,                              !- Year 28 Escalation
+    1.7248,                              !- Year 29 Escalation
+    1.7627;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Industrial-Residual Oil,       !- Name
+    FuelOil#2,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0093,                              !- Year 1 Escalation
+    1.1070,                              !- Year 2 Escalation
+    1.1276,                              !- Year 3 Escalation
+    1.1481,                              !- Year 4 Escalation
+    1.1749,                              !- Year 5 Escalation
+    1.2078,                              !- Year 6 Escalation
+    1.2428,                              !- Year 7 Escalation
+    1.2798,                              !- Year 8 Escalation
+    1.3179,                              !- Year 9 Escalation
+    1.3560,                              !- Year 10 Escalation
+    1.3971,                              !- Year 11 Escalation
+    1.4393,                              !- Year 12 Escalation
+    1.4815,                              !- Year 13 Escalation
+    1.5257,                              !- Year 14 Escalation
+    1.5720,                              !- Year 15 Escalation
+    1.6204,                              !- Year 16 Escalation
+    1.6698,                              !- Year 17 Escalation
+    1.7171,                              !- Year 18 Escalation
+    1.7706,                              !- Year 19 Escalation
+    1.8241,                              !- Year 20 Escalation
+    1.8776,                              !- Year 21 Escalation
+    1.9321,                              !- Year 22 Escalation
+    1.9897,                              !- Year 23 Escalation
+    2.0782,                              !- Year 24 Escalation
+    2.1914,                              !- Year 25 Escalation
+    2.2757,                              !- Year 26 Escalation
+    2.3477,                              !- Year 27 Escalation
+    2.4228,                              !- Year 28 Escalation
+    2.4990,                              !- Year 29 Escalation
+    2.5782;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Industrial-Natural gas,        !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9884,                              !- Year 1 Escalation
+    1.0406,                              !- Year 2 Escalation
+    1.1025,                              !- Year 3 Escalation
+    1.1721,                              !- Year 4 Escalation
+    1.2418,                              !- Year 5 Escalation
+    1.2959,                              !- Year 6 Escalation
+    1.3288,                              !- Year 7 Escalation
+    1.3540,                              !- Year 8 Escalation
+    1.3714,                              !- Year 9 Escalation
+    1.4043,                              !- Year 10 Escalation
+    1.4410,                              !- Year 11 Escalation
+    1.4391,                              !- Year 12 Escalation
+    1.4081,                              !- Year 13 Escalation
+    1.3849,                              !- Year 14 Escalation
+    1.3733,                              !- Year 15 Escalation
+    1.3830,                              !- Year 16 Escalation
+    1.4120,                              !- Year 17 Escalation
+    1.4333,                              !- Year 18 Escalation
+    1.4545,                              !- Year 19 Escalation
+    1.4855,                              !- Year 20 Escalation
+    1.5164,                              !- Year 21 Escalation
+    1.5338,                              !- Year 22 Escalation
+    1.5687,                              !- Year 23 Escalation
+    1.6209,                              !- Year 24 Escalation
+    1.6712,                              !- Year 25 Escalation
+    1.7060,                              !- Year 26 Escalation
+    1.7350,                              !- Year 27 Escalation
+    1.7660,                              !- Year 28 Escalation
+    1.7969,                              !- Year 29 Escalation
+    1.8279;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    West  Industrial-Coal,               !- Name
+    Coal,                                !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0279,                              !- Year 1 Escalation
+    1.0348,                              !- Year 2 Escalation
+    1.0314,                              !- Year 3 Escalation
+    1.0348,                              !- Year 4 Escalation
+    1.0453,                              !- Year 5 Escalation
+    1.0592,                              !- Year 6 Escalation
+    1.0697,                              !- Year 7 Escalation
+    1.0836,                              !- Year 8 Escalation
+    1.0976,                              !- Year 9 Escalation
+    1.1010,                              !- Year 10 Escalation
+    1.1045,                              !- Year 11 Escalation
+    1.1115,                              !- Year 12 Escalation
+    1.1220,                              !- Year 13 Escalation
+    1.1289,                              !- Year 14 Escalation
+    1.1394,                              !- Year 15 Escalation
+    1.1463,                              !- Year 16 Escalation
+    1.1533,                              !- Year 17 Escalation
+    1.1638,                              !- Year 18 Escalation
+    1.1707,                              !- Year 19 Escalation
+    1.1777,                              !- Year 20 Escalation
+    1.1847,                              !- Year 21 Escalation
+    1.1951,                              !- Year 22 Escalation
+    1.2021,                              !- Year 23 Escalation
+    1.2125,                              !- Year 24 Escalation
+    1.2195,                              !- Year 25 Escalation
+    1.2300,                              !- Year 26 Escalation
+    1.2439,                              !- Year 27 Escalation
+    1.2544,                              !- Year 28 Escalation
+    1.2683,                              !- Year 29 Escalation
+    1.2787;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Residential-Electricity,   !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0246,                              !- Year 1 Escalation
+    1.0387,                              !- Year 2 Escalation
+    1.0381,                              !- Year 3 Escalation
+    1.0441,                              !- Year 4 Escalation
+    1.0627,                              !- Year 5 Escalation
+    1.0819,                              !- Year 6 Escalation
+    1.0932,                              !- Year 7 Escalation
+    1.1025,                              !- Year 8 Escalation
+    1.1068,                              !- Year 9 Escalation
+    1.1161,                              !- Year 10 Escalation
+    1.1229,                              !- Year 11 Escalation
+    1.1274,                              !- Year 12 Escalation
+    1.1302,                              !- Year 13 Escalation
+    1.1285,                              !- Year 14 Escalation
+    1.1285,                              !- Year 15 Escalation
+    1.1305,                              !- Year 16 Escalation
+    1.1356,                              !- Year 17 Escalation
+    1.1415,                              !- Year 18 Escalation
+    1.1472,                              !- Year 19 Escalation
+    1.1523,                              !- Year 20 Escalation
+    1.1559,                              !- Year 21 Escalation
+    1.1613,                              !- Year 22 Escalation
+    1.1709,                              !- Year 23 Escalation
+    1.1825,                              !- Year 24 Escalation
+    1.1955,                              !- Year 25 Escalation
+    1.2034,                              !- Year 26 Escalation
+    1.2099,                              !- Year 27 Escalation
+    1.2161,                              !- Year 28 Escalation
+    1.2226,                              !- Year 29 Escalation
+    1.2291;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Residential-Distillate Oil,  !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9843,                              !- Year 1 Escalation
+    1.0240,                              !- Year 2 Escalation
+    1.0304,                              !- Year 3 Escalation
+    1.0402,                              !- Year 4 Escalation
+    1.0530,                              !- Year 5 Escalation
+    1.0706,                              !- Year 6 Escalation
+    1.0902,                              !- Year 7 Escalation
+    1.1118,                              !- Year 8 Escalation
+    1.1334,                              !- Year 9 Escalation
+    1.1555,                              !- Year 10 Escalation
+    1.1790,                              !- Year 11 Escalation
+    1.2035,                              !- Year 12 Escalation
+    1.2300,                              !- Year 13 Escalation
+    1.2570,                              !- Year 14 Escalation
+    1.2849,                              !- Year 15 Escalation
+    1.3134,                              !- Year 16 Escalation
+    1.3413,                              !- Year 17 Escalation
+    1.3713,                              !- Year 18 Escalation
+    1.4022,                              !- Year 19 Escalation
+    1.4335,                              !- Year 20 Escalation
+    1.4654,                              !- Year 21 Escalation
+    1.4988,                              !- Year 22 Escalation
+    1.5351,                              !- Year 23 Escalation
+    1.5709,                              !- Year 24 Escalation
+    1.6052,                              !- Year 25 Escalation
+    1.6390,                              !- Year 26 Escalation
+    1.6734,                              !- Year 27 Escalation
+    1.7092,                              !- Year 28 Escalation
+    1.7460,                              !- Year 29 Escalation
+    1.7837;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Residential-Natural gas,   !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9855,                              !- Year 1 Escalation
+    0.9952,                              !- Year 2 Escalation
+    1.0125,                              !- Year 3 Escalation
+    1.0550,                              !- Year 4 Escalation
+    1.1061,                              !- Year 5 Escalation
+    1.1437,                              !- Year 6 Escalation
+    1.1678,                              !- Year 7 Escalation
+    1.1871,                              !- Year 8 Escalation
+    1.2035,                              !- Year 9 Escalation
+    1.2208,                              !- Year 10 Escalation
+    1.2392,                              !- Year 11 Escalation
+    1.2430,                              !- Year 12 Escalation
+    1.2372,                              !- Year 13 Escalation
+    1.2343,                              !- Year 14 Escalation
+    1.2334,                              !- Year 15 Escalation
+    1.2459,                              !- Year 16 Escalation
+    1.2642,                              !- Year 17 Escalation
+    1.2835,                              !- Year 18 Escalation
+    1.3009,                              !- Year 19 Escalation
+    1.3211,                              !- Year 20 Escalation
+    1.3423,                              !- Year 21 Escalation
+    1.3655,                              !- Year 22 Escalation
+    1.3954,                              !- Year 23 Escalation
+    1.4368,                              !- Year 24 Escalation
+    1.4802,                              !- Year 25 Escalation
+    1.5024,                              !- Year 26 Escalation
+    1.5169,                              !- Year 27 Escalation
+    1.5323,                              !- Year 28 Escalation
+    1.5477,                              !- Year 29 Escalation
+    1.5632;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Residential-LPG,           !- Name
+    PropaneGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0097,                              !- Year 1 Escalation
+    1.0369,                              !- Year 2 Escalation
+    1.0475,                              !- Year 3 Escalation
+    1.0554,                              !- Year 4 Escalation
+    1.0609,                              !- Year 5 Escalation
+    1.0655,                              !- Year 6 Escalation
+    1.0701,                              !- Year 7 Escalation
+    1.0775,                              !- Year 8 Escalation
+    1.0840,                              !- Year 9 Escalation
+    1.0900,                              !- Year 10 Escalation
+    1.0983,                              !- Year 11 Escalation
+    1.1052,                              !- Year 12 Escalation
+    1.1117,                              !- Year 13 Escalation
+    1.1186,                              !- Year 14 Escalation
+    1.1255,                              !- Year 15 Escalation
+    1.1347,                              !- Year 16 Escalation
+    1.1449,                              !- Year 17 Escalation
+    1.1546,                              !- Year 18 Escalation
+    1.1643,                              !- Year 19 Escalation
+    1.1735,                              !- Year 20 Escalation
+    1.1832,                              !- Year 21 Escalation
+    1.1915,                              !- Year 22 Escalation
+    1.2007,                              !- Year 23 Escalation
+    1.2118,                              !- Year 24 Escalation
+    1.2252,                              !- Year 25 Escalation
+    1.2344,                              !- Year 26 Escalation
+    1.2427,                              !- Year 27 Escalation
+    1.2510,                              !- Year 28 Escalation
+    1.2598,                              !- Year 29 Escalation
+    1.2686;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Commercial-Electricity,    !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0131,                              !- Year 1 Escalation
+    1.0218,                              !- Year 2 Escalation
+    1.0184,                              !- Year 3 Escalation
+    1.0235,                              !- Year 4 Escalation
+    1.0396,                              !- Year 5 Escalation
+    1.0580,                              !- Year 6 Escalation
+    1.0681,                              !- Year 7 Escalation
+    1.0761,                              !- Year 8 Escalation
+    1.0785,                              !- Year 9 Escalation
+    1.0869,                              !- Year 10 Escalation
+    1.0915,                              !- Year 11 Escalation
+    1.0956,                              !- Year 12 Escalation
+    1.0986,                              !- Year 13 Escalation
+    1.0952,                              !- Year 14 Escalation
+    1.0932,                              !- Year 15 Escalation
+    1.0926,                              !- Year 16 Escalation
+    1.0959,                              !- Year 17 Escalation
+    1.1013,                              !- Year 18 Escalation
+    1.1056,                              !- Year 19 Escalation
+    1.1100,                              !- Year 20 Escalation
+    1.1133,                              !- Year 21 Escalation
+    1.1187,                              !- Year 22 Escalation
+    1.1288,                              !- Year 23 Escalation
+    1.1412,                              !- Year 24 Escalation
+    1.1543,                              !- Year 25 Escalation
+    1.1616,                              !- Year 26 Escalation
+    1.1673,                              !- Year 27 Escalation
+    1.1727,                              !- Year 28 Escalation
+    1.1784,                              !- Year 29 Escalation
+    1.1838;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Commercial-Distillate Oil, !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9840,                              !- Year 1 Escalation
+    1.0150,                              !- Year 2 Escalation
+    1.0200,                              !- Year 3 Escalation
+    1.0315,                              !- Year 4 Escalation
+    1.0461,                              !- Year 5 Escalation
+    1.0646,                              !- Year 6 Escalation
+    1.0881,                              !- Year 7 Escalation
+    1.1112,                              !- Year 8 Escalation
+    1.1337,                              !- Year 9 Escalation
+    1.1567,                              !- Year 10 Escalation
+    1.1813,                              !- Year 11 Escalation
+    1.2068,                              !- Year 12 Escalation
+    1.2334,                              !- Year 13 Escalation
+    1.2599,                              !- Year 14 Escalation
+    1.2869,                              !- Year 15 Escalation
+    1.3155,                              !- Year 16 Escalation
+    1.3445,                              !- Year 17 Escalation
+    1.3761,                              !- Year 18 Escalation
+    1.4076,                              !- Year 19 Escalation
+    1.4397,                              !- Year 20 Escalation
+    1.4727,                              !- Year 21 Escalation
+    1.5068,                              !- Year 22 Escalation
+    1.5438,                              !- Year 23 Escalation
+    1.5809,                              !- Year 24 Escalation
+    1.6159,                              !- Year 25 Escalation
+    1.6510,                              !- Year 26 Escalation
+    1.6860,                              !- Year 27 Escalation
+    1.7226,                              !- Year 28 Escalation
+    1.7601,                              !- Year 29 Escalation
+    1.7987;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Commercial-Residual Oil,   !- Name
+    FuelOil#2,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0078,                              !- Year 1 Escalation
+    1.0582,                              !- Year 2 Escalation
+    1.0606,                              !- Year 3 Escalation
+    1.0761,                              !- Year 4 Escalation
+    1.0963,                              !- Year 5 Escalation
+    1.1211,                              !- Year 6 Escalation
+    1.1475,                              !- Year 7 Escalation
+    1.1755,                              !- Year 8 Escalation
+    1.2042,                              !- Year 9 Escalation
+    1.2337,                              !- Year 10 Escalation
+    1.2648,                              !- Year 11 Escalation
+    1.2966,                              !- Year 12 Escalation
+    1.3284,                              !- Year 13 Escalation
+    1.3618,                              !- Year 14 Escalation
+    1.3967,                              !- Year 15 Escalation
+    1.4340,                              !- Year 16 Escalation
+    1.4713,                              !- Year 17 Escalation
+    1.5070,                              !- Year 18 Escalation
+    1.5474,                              !- Year 19 Escalation
+    1.5877,                              !- Year 20 Escalation
+    1.6289,                              !- Year 21 Escalation
+    1.6700,                              !- Year 22 Escalation
+    1.7135,                              !- Year 23 Escalation
+    1.7803,                              !- Year 24 Escalation
+    1.8665,                              !- Year 25 Escalation
+    1.9293,                              !- Year 26 Escalation
+    1.9845,                              !- Year 27 Escalation
+    2.0411,                              !- Year 28 Escalation
+    2.0986,                              !- Year 29 Escalation
+    2.1584;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Commercial-Natural gas,    !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0000,                              !- Year 1 Escalation
+    1.0024,                              !- Year 2 Escalation
+    1.0059,                              !- Year 3 Escalation
+    1.0494,                              !- Year 4 Escalation
+    1.1081,                              !- Year 5 Escalation
+    1.1516,                              !- Year 6 Escalation
+    1.1763,                              !- Year 7 Escalation
+    1.1974,                              !- Year 8 Escalation
+    1.2150,                              !- Year 9 Escalation
+    1.2338,                              !- Year 10 Escalation
+    1.2515,                              !- Year 11 Escalation
+    1.2503,                              !- Year 12 Escalation
+    1.2385,                              !- Year 13 Escalation
+    1.2303,                              !- Year 14 Escalation
+    1.2233,                              !- Year 15 Escalation
+    1.2338,                              !- Year 16 Escalation
+    1.2503,                              !- Year 17 Escalation
+    1.2679,                              !- Year 18 Escalation
+    1.2844,                              !- Year 19 Escalation
+    1.3020,                              !- Year 20 Escalation
+    1.3231,                              !- Year 21 Escalation
+    1.3478,                              !- Year 22 Escalation
+    1.3784,                              !- Year 23 Escalation
+    1.4230,                              !- Year 24 Escalation
+    1.4712,                              !- Year 25 Escalation
+    1.4959,                              !- Year 26 Escalation
+    1.5147,                              !- Year 27 Escalation
+    1.5323,                              !- Year 28 Escalation
+    1.5511,                              !- Year 29 Escalation
+    1.5711;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Commercial-Coal,           !- Name
+    Coal,                                !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0129,                              !- Year 1 Escalation
+    1.0284,                              !- Year 2 Escalation
+    1.0361,                              !- Year 3 Escalation
+    1.0412,                              !- Year 4 Escalation
+    1.0541,                              !- Year 5 Escalation
+    1.0644,                              !- Year 6 Escalation
+    1.0722,                              !- Year 7 Escalation
+    1.0773,                              !- Year 8 Escalation
+    1.0851,                              !- Year 9 Escalation
+    1.0902,                              !- Year 10 Escalation
+    1.0954,                              !- Year 11 Escalation
+    1.1031,                              !- Year 12 Escalation
+    1.1082,                              !- Year 13 Escalation
+    1.1186,                              !- Year 14 Escalation
+    1.1237,                              !- Year 15 Escalation
+    1.1289,                              !- Year 16 Escalation
+    1.1392,                              !- Year 17 Escalation
+    1.1443,                              !- Year 18 Escalation
+    1.1546,                              !- Year 19 Escalation
+    1.1598,                              !- Year 20 Escalation
+    1.1675,                              !- Year 21 Escalation
+    1.1804,                              !- Year 22 Escalation
+    1.1881,                              !- Year 23 Escalation
+    1.2010,                              !- Year 24 Escalation
+    1.2113,                              !- Year 25 Escalation
+    1.2191,                              !- Year 26 Escalation
+    1.2294,                              !- Year 27 Escalation
+    1.2371,                              !- Year 28 Escalation
+    1.2448,                              !- Year 29 Escalation
+    1.2552;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Industrial-Electricity,    !- Name
+    Electricity,                         !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0014,                              !- Year 1 Escalation
+    1.0029,                              !- Year 2 Escalation
+    0.9952,                              !- Year 3 Escalation
+    0.9990,                              !- Year 4 Escalation
+    1.0158,                              !- Year 5 Escalation
+    1.0336,                              !- Year 6 Escalation
+    1.0441,                              !- Year 7 Escalation
+    1.0532,                              !- Year 8 Escalation
+    1.0575,                              !- Year 9 Escalation
+    1.0686,                              !- Year 10 Escalation
+    1.0767,                              !- Year 11 Escalation
+    1.0825,                              !- Year 12 Escalation
+    1.0849,                              !- Year 13 Escalation
+    1.0829,                              !- Year 14 Escalation
+    1.0829,                              !- Year 15 Escalation
+    1.0858,                              !- Year 16 Escalation
+    1.0925,                              !- Year 17 Escalation
+    1.1007,                              !- Year 18 Escalation
+    1.1074,                              !- Year 19 Escalation
+    1.1146,                              !- Year 20 Escalation
+    1.1213,                              !- Year 21 Escalation
+    1.1304,                              !- Year 22 Escalation
+    1.1438,                              !- Year 23 Escalation
+    1.1601,                              !- Year 24 Escalation
+    1.1779,                              !- Year 25 Escalation
+    1.1884,                              !- Year 26 Escalation
+    1.1970,                              !- Year 27 Escalation
+    1.2057,                              !- Year 28 Escalation
+    1.2143,                              !- Year 29 Escalation
+    1.2229;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Industrial-Distillate Oil, !- Name
+    FuelOil#1,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9839,                              !- Year 1 Escalation
+    1.0034,                              !- Year 2 Escalation
+    1.0054,                              !- Year 3 Escalation
+    1.0171,                              !- Year 4 Escalation
+    1.0327,                              !- Year 5 Escalation
+    1.0513,                              !- Year 6 Escalation
+    1.0767,                              !- Year 7 Escalation
+    1.0997,                              !- Year 8 Escalation
+    1.1217,                              !- Year 9 Escalation
+    1.1447,                              !- Year 10 Escalation
+    1.1686,                              !- Year 11 Escalation
+    1.1935,                              !- Year 12 Escalation
+    1.2185,                              !- Year 13 Escalation
+    1.2434,                              !- Year 14 Escalation
+    1.2688,                              !- Year 15 Escalation
+    1.2962,                              !- Year 16 Escalation
+    1.3245,                              !- Year 17 Escalation
+    1.3558,                              !- Year 18 Escalation
+    1.3866,                              !- Year 19 Escalation
+    1.4179,                              !- Year 20 Escalation
+    1.4501,                              !- Year 21 Escalation
+    1.4834,                              !- Year 22 Escalation
+    1.5200,                              !- Year 23 Escalation
+    1.5557,                              !- Year 24 Escalation
+    1.5904,                              !- Year 25 Escalation
+    1.6246,                              !- Year 26 Escalation
+    1.6588,                              !- Year 27 Escalation
+    1.6945,                              !- Year 28 Escalation
+    1.7312,                              !- Year 29 Escalation
+    1.7688;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Industrial-Residual Oil,   !- Name
+    FuelOil#2,                           !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0086,                              !- Year 1 Escalation
+    1.0866,                              !- Year 2 Escalation
+    1.0986,                              !- Year 3 Escalation
+    1.1158,                              !- Year 4 Escalation
+    1.1381,                              !- Year 5 Escalation
+    1.1647,                              !- Year 6 Escalation
+    1.1947,                              !- Year 7 Escalation
+    1.2256,                              !- Year 8 Escalation
+    1.2573,                              !- Year 9 Escalation
+    1.2890,                              !- Year 10 Escalation
+    1.3242,                              !- Year 11 Escalation
+    1.3585,                              !- Year 12 Escalation
+    1.3937,                              !- Year 13 Escalation
+    1.4305,                              !- Year 14 Escalation
+    1.4691,                              !- Year 15 Escalation
+    1.5094,                              !- Year 16 Escalation
+    1.5506,                              !- Year 17 Escalation
+    1.5901,                              !- Year 18 Escalation
+    1.6346,                              !- Year 19 Escalation
+    1.6792,                              !- Year 20 Escalation
+    1.7238,                              !- Year 21 Escalation
+    1.7693,                              !- Year 22 Escalation
+    1.8173,                              !- Year 23 Escalation
+    1.8919,                              !- Year 24 Escalation
+    1.9863,                              !- Year 25 Escalation
+    2.0557,                              !- Year 26 Escalation
+    2.1166,                              !- Year 27 Escalation
+    2.1792,                              !- Year 28 Escalation
+    2.2427,                              !- Year 29 Escalation
+    2.3087;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Industrial-Natural gas,    !- Name
+    NaturalGas,                          !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    0.9706,                              !- Year 1 Escalation
+    1.0273,                              !- Year 2 Escalation
+    1.1027,                              !- Year 3 Escalation
+    1.1824,                              !- Year 4 Escalation
+    1.2725,                              !- Year 5 Escalation
+    1.3312,                              !- Year 6 Escalation
+    1.3606,                              !- Year 7 Escalation
+    1.3878,                              !- Year 8 Escalation
+    1.4088,                              !- Year 9 Escalation
+    1.4340,                              !- Year 10 Escalation
+    1.4696,                              !- Year 11 Escalation
+    1.4696,                              !- Year 12 Escalation
+    1.4486,                              !- Year 13 Escalation
+    1.4361,                              !- Year 14 Escalation
+    1.4277,                              !- Year 15 Escalation
+    1.4507,                              !- Year 16 Escalation
+    1.4822,                              !- Year 17 Escalation
+    1.5136,                              !- Year 18 Escalation
+    1.5430,                              !- Year 19 Escalation
+    1.5723,                              !- Year 20 Escalation
+    1.6059,                              !- Year 21 Escalation
+    1.6352,                              !- Year 22 Escalation
+    1.6730,                              !- Year 23 Escalation
+    1.7358,                              !- Year 24 Escalation
+    1.8197,                              !- Year 25 Escalation
+    1.8637,                              !- Year 26 Escalation
+    1.8973,                              !- Year 27 Escalation
+    1.9287,                              !- Year 28 Escalation
+    1.9623,                              !- Year 29 Escalation
+    1.9979;                              !- Year 30 Escalation
+
+
+LifeCycleCost:UsePriceEscalation,
+    U.S. Avg  Industrial-Coal,           !- Name
+    Coal,                                !- Resource
+    2016,                                !- Escalation Start Year
+    January,                             !- Escalation Start Month
+    1.0160,                              !- Year 1 Escalation
+    1.0353,                              !- Year 2 Escalation
+    1.0385,                              !- Year 3 Escalation
+    1.0449,                              !- Year 4 Escalation
+    1.0609,                              !- Year 5 Escalation
+    1.0769,                              !- Year 6 Escalation
+    1.0897,                              !- Year 7 Escalation
+    1.0994,                              !- Year 8 Escalation
+    1.1058,                              !- Year 9 Escalation
+    1.1122,                              !- Year 10 Escalation
+    1.1186,                              !- Year 11 Escalation
+    1.1282,                              !- Year 12 Escalation
+    1.1346,                              !- Year 13 Escalation
+    1.1442,                              !- Year 14 Escalation
+    1.1538,                              !- Year 15 Escalation
+    1.1635,                              !- Year 16 Escalation
+    1.1699,                              !- Year 17 Escalation
+    1.1795,                              !- Year 18 Escalation
+    1.1859,                              !- Year 19 Escalation
+    1.1923,                              !- Year 20 Escalation
+    1.2019,                              !- Year 21 Escalation
+    1.2115,                              !- Year 22 Escalation
+    1.2212,                              !- Year 23 Escalation
+    1.2340,                              !- Year 24 Escalation
+    1.2436,                              !- Year 25 Escalation
+    1.2885,                              !- Year 26 Escalation
+    1.3141,                              !- Year 27 Escalation
+    1.3237,                              !- Year 28 Escalation
+    1.3333,                              !- Year 29 Escalation
+    1.3462;                              !- Year 30 Escalation
+
diff --git a/doc/.gitignore b/doc/.gitignore
new file mode 100644
index 00000000000..2f3591a1c23
--- /dev/null
+++ b/doc/.gitignore
@@ -0,0 +1,55 @@
+## Core latex/pdflatex auxiliary files:
+*.aux
+*.lof
+*.log
+*.lot
+*.fls
+*.out
+*.toc
+*.fmt
+
+## Intermediate documents:
+*.dvi
+*-converted-to.*
+# these rules might exclude image files for figures etc.
+# *.ps
+# *.eps
+*.pdf
+
+## Bibliography auxiliary files (bibtex/biblatex/biber):
+*.bbl
+*.bcf
+*.blg
+*-blx.aux
+*-blx.bib
+*.brf
+*.run.xml
+
+## Build tool auxiliary files:
+*.fdb_latexmk
+*.synctex
+*.synctex.gz
+*.synctex.gz(busy)
+*.pdfsync
+
+## Auxiliary and intermediate files from other packages:
+# algorithms
+*.alg
+*.loa
+
+# hyperref
+*.brf
+
+# listings
+*.lol
+
+# makeidx
+*.idx
+*.ilg
+*.ind
+*.ist
+
+# nomencl
+*.nlo
+
+# Texpad
diff --git a/doc/CMakeLists.txt b/doc/CMakeLists.txt
new file mode 100644
index 00000000000..d5b3c766912
--- /dev/null
+++ b/doc/CMakeLists.txt
@@ -0,0 +1,59 @@
+# the only thing that really needs to be set outside of here is the XELATEX variable, the path to the xelatex compiler
+
+# the root doc build directory will be created at configure time, but lets not copy anything over until build time.
+file(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build)
+
+# add a configure rule to the header file though
+configure_file(${CMAKE_SOURCE_DIR}/doc/header.tex ${CMAKE_BINARY_DIR}/doc-build/header.tex COPYONLY)
+configure_file(${CMAKE_SOURCE_DIR}/doc/title.tex ${CMAKE_BINARY_DIR}/doc-build/title.tex COPYONLY)
+
+# add each of the documents, they have their own CMakeLists.txt files
+add_subdirectory(acknowledgements)
+add_subdirectory(auxiliary-programs)
+add_subdirectory(ems-application-guide)
+add_subdirectory(engineering-reference)
+add_subdirectory(external-interfaces-application-guide)
+add_subdirectory(getting-started)
+add_subdirectory(input-output-reference)
+add_subdirectory(interface-developer)
+add_subdirectory(module-developer)
+add_subdirectory(output-details-and-examples)
+add_subdirectory(plant-application-guide)
+add_subdirectory(tips-and-tricks-using-energyplus)
+add_subdirectory(using-energyplus-for-compliance)
+
+# we still need to find wkhtmltopdf and pandoc for building validation reports
+if (BUILD_VALIDATION_REPORTS)
+
+  # wkhtmltopdf
+  if(MSVC)
+    find_program(WKHTMLTOPDF_EXECUTABLE 
+      wkhtmltopdf
+      PATHS "C:/Program Files/wkhtmltopdf/bin" "C:/Program Files (x86)/wkhtmltopdf/bin")
+  else()
+    find_program(WKHTMLTOPDF_EXECUTABLE 
+      wkhtmltopdf
+      )
+  endif()
+  execute_process(COMMAND ${WKHTMLTOPDF_EXECUTABLE} -V 
+    OUTPUT_VARIABLE wkhtmltopdfversionout)
+  string(REGEX MATCH "([0-9]+\\.?)+" WKHTMLTOPDF_VER "${wkhtmltopdfversionout}")
+  string(FIND "${wkhtmltopdfversionout}" "with patched qt" WKHTMLTOPDF_PATCHEDQT )
+  if (WKHTMLTOPDF_VER VERSION_LESS "0.12.2.1")
+    message(FATAL_ERROR "wkhtmltopdf version 0.12.2.1 or greater required")
+  endif()
+  if (WKHTMLTOPDF_PATCHEDQT LESS "0")
+    message(FATAL_ERROR "wkhtmltopdf with special patchedqt build required")
+  endif()
+  
+  # pandoc
+  find_program(PANDOC_EXECUTABLE pandoc)
+  file(MAKE_DIRECTORY ${CMAKE_CURRENT_BINARY_DIR}/Products)
+  execute_process(COMMAND ${PANDOC_EXECUTABLE} -v 
+    OUTPUT_VARIABLE pandocversionout)
+  string(REGEX MATCH "([0-9]+\\.?)+" PANDOC_VER "${pandocversionout}")
+  if (PANDOC_VER VERSION_LESS "1.13.2")
+    message(FATAL_ERROR "pandoc version 1.13.2 or greater required")
+  endif()
+
+endif()
diff --git a/doc/acknowledgements/CMakeLists.txt b/doc/acknowledgements/CMakeLists.txt
new file mode 100644
index 00000000000..ede2f16aac5
--- /dev/null
+++ b/doc/acknowledgements/CMakeLists.txt
@@ -0,0 +1,31 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/acknowledgements.tex
+  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/src/notices-and-acknowledgments.tex
+  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/src/notices-and-acknowledgments/copyright-notice.tex
+  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/src/notices-and-acknowledgments/other-software-included-or-referenced.tex
+  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/src/notices-and-acknowledgments/other-acknowledgments.tex
+  ${CMAKE_SOURCE_DIR}/doc/title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+) 
+
+SET( SOURCE_FILENAME "acknowledgements" )
+SET( OUTPUT_FILENAME "Acknowledgements" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/acknowledgements/acknowledgements.tex b/doc/acknowledgements/acknowledgements.tex
new file mode 100644
index 00000000000..2d009020cce
--- /dev/null
+++ b/doc/acknowledgements/acknowledgements.tex
@@ -0,0 +1,26 @@
+\input{../header}
+
+\title{Acknowledgements and Copyright Notices}
+
+\hypersetup{unicode=true,
+            pdftitle={Acknowledgements and Copyright Notices},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/notices-and-acknowledgments}
+
+\input{src/notices-and-acknowledgments/copyright-notice}
+
+\input{src/notices-and-acknowledgments/other-software-included-or-referenced}
+
+\input{src/notices-and-acknowledgments/other-acknowledgments}
+
+\end{document}
diff --git a/doc/acknowledgements/media/ep.png b/doc/acknowledgements/media/ep.png
new file mode 100644
index 00000000000..a808760c870
Binary files /dev/null and b/doc/acknowledgements/media/ep.png differ
diff --git a/doc/acknowledgements/src/notices-and-acknowledgments.tex b/doc/acknowledgements/src/notices-and-acknowledgments.tex
new file mode 100644
index 00000000000..c07b8e39578
--- /dev/null
+++ b/doc/acknowledgements/src/notices-and-acknowledgments.tex
@@ -0,0 +1,3 @@
+\input{../title}
+
+\chapter{Notices and Acknowledgments}\label{notices-and-acknowledgments}
diff --git a/doc/acknowledgements/src/notices-and-acknowledgments/copyright-notice.tex b/doc/acknowledgements/src/notices-and-acknowledgments/copyright-notice.tex
new file mode 100644
index 00000000000..92110142fe7
--- /dev/null
+++ b/doc/acknowledgements/src/notices-and-acknowledgments/copyright-notice.tex
@@ -0,0 +1,85 @@
+\section{Copyright Notice}\label{copyright-notice}
+
+Copyright (c) 1996-2015 The Board of Trustees of the University of Illinois and The Regents of the University of California through Ernest Orlando Lawrence Berkeley National Laboratory. All rights reserved.
+
+Portions of the EnergyPlusâ„¢ software package have been developed and copyrighted by other individuals, companies and institutions. These portions have been incorporated into the EnergyPlus software package under license.
+
+\textbf{In addition to the primary authorship of the LBNL Simulation Research Group (}\href{http://simulationresearch.lbl.gov/}{\textbf{http://simulationresearch.lbl.gov/}}\textbf{) and the UIUC Building Systems Laboratory, the following have contributed to EnergyPlus Versions (includes all minor revisions):}
+
+Portions of the EnergyPlus weather processor were developed by US Department of Energy, Office of Building Technologies.
+
+Portions of the input processing, output processing, weather processor, BLAST Translator were developed by US Army Corps of Engineers, Construction Engineering Research Laboratories, 2902 Newmark Drive, Champaign IL~ 61821. \url{http://www.erdc.usace.army.mil/Locations/ConstructionEngineeringResearchLaboratory.aspx}
+
+Portions of this software package were developed for Ernest Orlando Lawrence Berkeley National Laboratory and Florida Solar Energy Center by Linda Lawrie of DHL Consulting.
+
+Portions of this software package were developed for Ernest Orlando Lawrence Berkeley National Laboratory and Florida Solar Energy Center by C.O. Pedersen Associates.
+
+Portions of the EnergyPlus utility software (EP-Launch, IDFEditor, DOE2Translator, HVAC-Diagram, ExpandObjects, CSVProc, ParametricPreprocessor, AppGPostProcess, EP-Compare, and convertESOMTR) were developed by GARD Analytics, Inc. 115 S. Wilke Road, Suite 105, Arlington Heights, IL, USA, \textless{}info@gard.com\textgreater{}, \href{http://www.gard.com/}{www.gard.com}. GARD Analytics performed independent verification and validation testing of the software after developing the testing strategy and plan. GARD Analytics was also responsible for gas absorption chiller, desiccant dehumidifier, ice storage (simple), table reports, economics and life cycle costing.
+
+Portions of flow resolver, chiller models (absorption, electric, const cop, engine-driven, gas-turbine), generator models (diesel electric, gas turbine), furnace models, heat recovery loop, plant loop, plant condenser loop, air-change dependent inside film coefficients were developed by Oklahoma State University, 110 Engineering North, Stillwater, OK 74078.
+
+Portions of EnergyPlus related to the models for EMPD moisture calculations, DX coils, furnace/unitary systems, air-to-air heat pumps, changeover-bypass VAV systems, packaged terminal heat pumps, cooling towers, AirflowNetwork, refrigerated cases, reformulated and electric EIR chillers, desuperheater air and water heating coils, heat pump water heaters, desiccant and generic air-to-air heat exchangers, window screens, and thermal comfort controls were developed by University of Central Florida, Florida Solar Energy Center (FSEC), 1679 Clearlake Road, Cocoa, FL~ 32922, \href{http://www.fsec.ucf.edu/}{www.fsec.ucf.edu/}.
+
+Portions of the refrigeration model and the exhaust-fired absorption chiller model were developed by Oak Ridge National Laboratory, Bethel Valley Road, Oak Ridge, Tennessee 37831.
+
+Portions of EnergyPlus were developed by the National Renewable Energy Laboratory (NREL), 1617 Cole Blvd, Golden, CO 80401.
+
+Portions of EnergyPlus related to transformer losses model, autosizing calculations, life cycle costing and chemical battery storage model were developed by Pacific Northwest National Laboratory (PNNL), P.O. Box 999, Richland, WA 99352.
+
+EnergyPlus v1.0.1, v1.0.2, v1.0.3, v1.1, v1.1.1 (Wintel platform) included a link to TRNSYS (The Transient Energy System Simulation Tool) for photovoltaic calculations developed by Thermal Energy System Specialists, 2916 Marketplace Drive, Suite 104, Madison, WI 53719; Tel: (608) 274-2577. EnergyPlus v1.2 and later includes Photovoltaic calculations implemented in EnergyPlus by Thermal Energy System Specialists. This model was originally developed by Oystein Ulleberg, Institute for Energy Technology, Norway -- based on the Duffie and Beckman equivalent one-diode model.
+
+Portions of this software package that convert certain stand-alone heat transfer models for slab-on-grade and basement foundations were developed by William Bahnfleth, Cynthia Cogil, and Edward Clements, Department of Architectural Engineering, Pennsylvania State University, 224 Engineering Unit A, University Park, Pennsylvania 16802-1416, (814) 863-2076.
+
+The concept and initial implementation for the EnergyPlus COM/DLL version (Wintel platform) was made possible through cooperation with DesignBuilder Software, Ltd, Andy Tindale -- an EnergyPlus collaborative developer.
+
+The thickness, conductivity, density and specific heat values of the material layers for the constructions in the Composite Wall Construction reference data set have been taken from the ASHRAE report ``Modeling Two- and Three-Dimensional Heat Transfer through Composite Wall and Roof Assemblies in Hourly Energy Simulation Programs (1145-TRP),'' by Enermodal Engineering Limited, Oak Ridge National Laboratory, and the Polish Academy of Sciences, January 2001.
+
+EnergyPlus v1.2 and later versions contains DELight2, a simulation engine for daylighting and electric lighting system analysis developed at Ernest Orlando Lawrence Berkeley National Laboratory.
+
+EnergyPlus v1.2.2 through v3.1 contained links to SPARK, a simulation engine for detailed system modeling developed at Ernest Orlando Lawrence Berkeley National Laboratory in conjunction with Ayres Sowell Associates, Inc.
+
+The airflow calculation portion of the EnergyPlus AirflowNetwork model was based on AIRNET written by George Walton of the National Institute for Standards and Technology (NIST), 100 Bureau Drive, Gaithersburg, MD 20899. The EnergyPlus AirflowNetwork model also includes portions of stack effect and detailed large opening from an early version of COMIS (Conjunction Of Multizone Infiltration Specialists) developed by a multinational, multi-institutional effort under the auspices of the International Energy Agency's Buildings and Community Systems Agreement working group focusing on multizone air flow modeling (Annex 23) and now administered by the Swiss Federal Laboratories for Materials Testing and Research (EMPA), Division 175, Überlandstrasse 129, CH-8600 Dübendorf, Switzerland.
+
+The EnergyPlus model for displacement ventilation and cross-ventilation (version v1.2 and later) was developed by Guilherme Carrilho da Graça (Department of Mechanical and Aerospace Engineering, University of California, San Diego and NaturalWorks) and Paul Linden (Department of Mechanical and Aerospace Engineering, University of California, San Diego).
+
+The EnergyPlus models for UFAD served zones were developed by Anna Liu and Paul Linden at the Department of Mechanical and Aerospace Engineering, University of California, San Diego.
+
+ASHRAE research project 1254-RP supported the development of the following features first added in EnergyPlus v1.2.2: 
+\begin{itemize}
+  \item DXSystem:AirLoop enhancements (valid as OA system equipment, new humidity control options)
+  \item New set point managers: SET POINT MANAGER:SINGLE ZONE HEATING, SET POINT MANAGER:SINGLE ZONE COOLING, and SET POINT MANAGER:OUTSIDE AIR PRETREAT
+  \item New 2-stage DX coil with enhanced dehumidification option:
+  \begin{itemize}
+    \item COIL:DX:MultiMode:CoolingEmpirical
+  \end{itemize}
+  \item Additional DESICCANT DEHUMIDIFIER:SOLID setpoint control option
+\end{itemize}
+
+American Society of Heating Refrigerating and Air-Conditioning Engineers, Inc., 1791 Tullie Circle, N.E., Atlanta, GA 30329\footnote{\url{http://www.ashrae.org/}}. Work performed by GARD Analytics, Inc., 115 S. Wilke Road, Suite 105, Arlington Heights, IL, USA\footnote{url{info@gard.com}; \url{http://www.gard.com/}}, November 2004. These items were renamed in V3.0 to:
+\begin{itemize}
+  \item SetpointManager:SingleZone:Heating
+  \item SetpointManager:SingleZone:Cooling
+  \item SetpointManager:OutdoorAirPretreat
+  \item Coil:Cooling:DX:TwoStageWithHumidityControlMode
+  \item Dehumidifier:Desiccant:NoFans
+\end{itemize}
+
+The Ecoroof (Green Roof) model, first introduced in EnergyPlus v2.0, was developed at Portland State University, by David Sailor and his students. It is based on the FASST vegetation models developed by Frankenstein and Koenig for the US Army Corps of Engineers.
+
+The HAMT (Heat And Moisture Transfer) model, first introduced in EnergyPlus v3.0.0 was developed by Phillip Biddulph, Complex Built Environment Systems, The Bartlett School of Graduate Studies, University College London, Gower Street, London WC1E 6BT, United Kingdom. \url{http://www.cbes.ucl.ac.uk/}.
+
+The SQLite output module, first introduced in EnergyPlus v3.0.0, was developed by Gregory B. Stark, P.E., Building Synergies, LLC, 1860 Washington Street, Suite 208, Denver, Colorado 80203, United States.
+
+Refrigeration compressor performance data and refrigeration practices were provided by CDH Energy, Cazenovia, NY 12035.
+
+The external interface was developed by Michael Wetter and Philip Haves (Lawrence Berkeley National Laboratory) and by Rui Zhang (Carnegie Mellon University). An earlier upgrade to a development version of EnergyPlus 3.0 was implemented by Charles Corbin, Anthony Florita, Gregor Henze and Peter May-Ostendorp (University of Colorado at Boulder).
+
+Various suggestions for time reduction, improved documentation and other items have been incorporated from Autodesk, Inc., Bentley Systems, and others.
+
+Particular recognition goes to Noel Keen (LBNL Computational Research Division) and Geof Sawaya (Oak Ridge National Laboratory fellow) who have done extensive profiling and creation of time reduction features that have gone into the code.
+
+Second Law modified the WaterToAirHeatPump:EquationFit module to include the variable ``WaterCyclingMode''. This variable determines whether the heat pump water flow is constant, whether it cycles with the compressor, or whether it is constant when the heat pump is active. WaterFlowMode is set by the HVAC wrapper object; either ZoneHVAC:WaterToAirHeatPump or AirLoopHVAC:UnitaryHeatPump:WaterToAir. Second Law, Burlington, VT, Karen Walkerman.
+
+\textbf{NOTICE:} The U.S. Government is granted for itself and others acting on its behalf a paid-up, nonexclusive, irrevocable, worldwide license in this data to reproduce, prepare derivative works, and perform publicly and display publicly. Beginning five (5) years after permission to assert copyright is granted, subject to two possible five year renewals, the U.S. Government is granted for itself and others acting on its behalf a paid-up, non-exclusive, irrevocable worldwide license in this data to reproduce, prepare derivative works, distribute copies to the public, perform publicly and display publicly, and to permit others to do so.
+
+\textbf{TRADEMARKS:} EnergyPlus is a trademark of the US Department of Energy.
diff --git a/doc/acknowledgements/src/notices-and-acknowledgments/other-acknowledgments.tex b/doc/acknowledgements/src/notices-and-acknowledgments/other-acknowledgments.tex
new file mode 100644
index 00000000000..a7bacb8ae78
--- /dev/null
+++ b/doc/acknowledgements/src/notices-and-acknowledgments/other-acknowledgments.tex
@@ -0,0 +1,13 @@
+\section{Other Acknowledgments}\label{other-acknowledgments}
+
+This work was supported by the Assistant Secretary for Energy Efficiency and Renewable Energy, Office of Building Technologies of the US Department of Energy -- under the guidance of Dru Crawley from inception through March 2010.
+
+Additional support was provided by the Gas Technology Institute and the California Energy Commission.
+
+The ice thermal storage module development was supported by the U.S. Department of Energy Office of Electricity Delivery and Energy Reliability.
+
+The HAMT (Heat And Moisture Transfer) model was supported by the Engineering and Physical Sciences Research Council (EPSRC), the UK government agency for funding research and training in engineering and the physical sciences.
+
+The SQLite output module was funded by Building Synergies, LLC and was made possible by inclusion of software code from the SQLite project (\textless{}http://www.sqlite.org/\textgreater{}).
+
+~
diff --git a/doc/acknowledgements/src/notices-and-acknowledgments/other-software-included-or-referenced.tex b/doc/acknowledgements/src/notices-and-acknowledgments/other-software-included-or-referenced.tex
new file mode 100644
index 00000000000..cb488dfac1f
--- /dev/null
+++ b/doc/acknowledgements/src/notices-and-acknowledgments/other-software-included-or-referenced.tex
@@ -0,0 +1,223 @@
+\section{Other Software included or referenced directly}\label{other-software-included-or-referenced-directly}
+
+The following notices apply to those EnergyPlus distributions which include the interface to BCVTB or Functional Mock-up Units.
+
+\subsection{ZLIB DATA COMPRESSION LIBRARY}\label{zlib-data-compression-library}
+
+zlib 1.2.5 is a general purpose data compression library.~ All the code is thread safe.~ The data format used by the zlib library is described by RFCs (Request for Comments) 1950 to 1952 in the files http://www.ietf.org/rfc/rfc1950.txt (zlib format), rfc1951.txt (deflate format) and rfc1952.txt (gzip format).
+
+All functions of the compression library are documented in the file zlib.h (volunteer to write man pages welcome, contact zlib@gzip.org).~ A usage example of the library is given in the file example.c which also tests that the library is working correctly. ~Another example is given in the file minigzip.c.~ The compression library itself is composed of all source files except example.c and minigzip.c.
+
+To compile all files and run the test program, follow the instructions given at the top of Makefile.in.~ In short ``./configure; make test'', and if that goes well, ``make install'' should work for most flavors of Unix.~ For Windows, use one of the special makefiles in win32/ or contrib/vstudio/ .~ For VMS, use make\_vms.com.~ Questions about zlib should be sent to \textless{}zlib@gzip.org\textgreater{}, or to Gilles Vollant \textless{}info@winimage.com\textgreater{} for the Windows DLL version.~ The zlib home page is http://zlib.net/ .~ Before reporting a problem, please check this site to verify that you have the latest version of zlib; otherwise get the latest version and check whether the problem still exists or not.
+
+PLEASE read the zlib FAQ \textgreater{}http://zlib.net/zlib\_faq.html\textless{} before asking for help.
+
+Mark Nelson \textless{}markn@ieee.org\textgreater{} wrote an article about zlib for the Jan.~ 1997 issue of Dr.~ Dobb's Journal; a copy of the article is available online\footnote{\url{http://marknelson.us/1997/01/01/zlib-engine/}}.
+
+The changes made in version 1.2.5 are documented in the file ChangeLog.
+
+Unsupported third party contributions are provided in directory contrib/ .
+
+zlib is available in Java using the java.util.zip package, documented online\footnote{\url{http://java.sun.com/developer/technicalArticles/Programming/compression/}}.
+
+A Perl interface to zlib written by Paul Marquess \textless{}pmqs@cpan.org\textgreater{} is available at CPAN (Comprehensive Perl Archive Network) sites, including \textless{}http://search.cpan.org/\textasciitilde{}pmqs/IO-Compress-Zlib/\textgreater{} .
+
+A Python interface to zlib written by A.M. Kuchling \textless{}amk@amk.ca\textgreater{} is available in Python 1.5 and later versions, see \textless{}http://www.python.org/doc/lib/module-zlib.html\textgreater{}.
+
+zlib is built into tcl: \textless{}http://wiki.tcl.tk/4610\textgreater{} .
+
+An experimental package to read and write files in .zip format, written on top of zlib by Gilles Vollant \textless{}info@winimage.com\textgreater{}, is available in the contrib/minizip directory of zlib.
+
+Notes for some targets:
+
+\begin{itemize}
+\item
+  For Windows DLL versions, please see win32/DLL\_FAQ.txt
+\item
+  For 64-bit Irix, deflate.c must be compiled without any optimization. With -O, one libpng test fails. The test works in 32 bit mode (with the -n32~~ compiler flag). The compiler bug has been reported to SGI.
+\item
+  zlib doesn't work with gcc 2.6.3 on a DEC 3000/300LX under OSF/1 2.1 it works when compiled with cc.
+\item
+  On Digital Unix 4.0D (formely OSF/1) on AlphaServer, the cc option -std1 is necessary to get gzprintf working correctly. This is done by configure.
+\item
+  zlib doesn't work on HP-UX 9.05 with some versions of /bin/cc. It works with other compilers. Use ``make test'' to check your compiler.
+\item
+  gzdopen is not supported on RISCOS or BEOS.
+\item
+  For PalmOs, see \textless{}http://palmzlib.sourceforge.net/\textgreater{}
+\end{itemize}
+
+Acknowledgments:
+
+~ The deflate format used by zlib was defined by Phil Katz.~ The deflate and zlib specifications were written by L.~ Peter Deutsch.~ Thanks to all the people who reported problems and suggested various improvements in zlib; they are too numerous to cite here.
+
+Copyright notice:
+
+~(C) 1995-2010 Jean-loup Gailly and Mark Adler
+
+This software is provided `as-is', without any express or implied warranty.~ In no event will the authors be held liable for any damages arising from the use of this software.
+
+Permission is granted to anyone to use this software for any purpose, including commercial applications, and to alter it and redistribute it freely, subject to the following restrictions:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  The origin of this software must not be misrepresented; you must not claim that you wrote the original software. If you use this software in a product, an acknowledgment in the product documentation would be appreciated but is not required.
+\item
+  Altered source versions must be plainly marked as such, and must not be misrepresented as being the original software.
+\item
+  This notice may not be removed or altered from any source distribution.
+\end{enumerate}
+
+~ Jean-loup Gailly~~~~~~~ Mark Adler
+
+~ jloup@gzip.org~~~~~~~~~ madler@alumni.caltech.edu
+
+~
+
+If you use the zlib library in a product, we would appreciate *not* receiving lengthy legal documents to sign.~ The sources are provided for free but without warranty of any kind.~ The library has been entirely written by Jean-loup Gailly and Mark Adler; it does not include third-party code.
+
+If you redistribute modified sources, we would appreciate that you include in the file ChangeLog history information documenting your changes.~ Please read the FAQ for more information on the distribution of modified source versions.
+
+\subsection{ExPat Copying Notice}\label{expat-copying-notice}
+
+Copyright (c) 1998, 1999, 2000 Thai Open Source Software Center Ltd
+
+Permission is hereby granted, free of charge, to any person obtaining a copy of this software and associated documentation files (the ``Software''), to deal in the Software without restriction, including without limitation the rights to use, copy, modify, merge, publish, distribute, sublicense, and/or sell copies of the Software, and to permit persons to whom the Software is furnished to do so, subject to the following conditions:
+
+The above copyright notice and this permission notice shall be included in all copies or substantial portions of the Software.
+
+THE SOFTWARE IS PROVIDED ``AS IS'', WITHOUT WARRANTY OF ANY KIND, EXPRESS OR IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY, FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT. IN NO EVENT SHALL THE AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING FROM, OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER DEALINGS IN THE SOFTWARE.
+
+\subsection{FMU SDK license}\label{fmu-sdk-license}
+
+Copyright (c) 2008-2011, QTronic GmbH. All rights reserved.
+
+The FmuSdk is licensed by the copyright holder under the BSD License\footnote{\url{http://www.opensource.org/licenses/bsd-license.html}}: Redistribution and use in source and binary forms, with or without modification, are permitted provided that the following conditions are met:
+
+\begin{itemize}
+\item
+  Redistributions of source code must retain the above copyright notice, this list of conditions and the following disclaimer.
+\item
+  Redistributions in binary form must reproduce the above copyright notice, this list of conditions and the following disclaimer in the documentation and/or other materials provided with the distribution.
+\end{itemize}
+
+THIS SOFTWARE IS PROVIDED BY QTRONIC GMBH ``AS IS'' AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL QTRONIC GMBH BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
+
+\subsection{Minizip Notice}\label{minizip-notice}
+
+Condition of use and distribution are the same than zlib :
+
+This software is provided `as-is', without any express or implied warranty.~ In no event will the authors be held liable for any damages arising from the use of this software.
+
+Permission is granted to anyone to use this software for any purpose, including commercial applications, and to alter it and redistribute it freely, subject to the following restrictions:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  The origin of this software must not be misrepresented; you must not claim that you wrote the original software. If you use this software in a product, an acknowledgment in the product documentation would be appreciated but is not required.
+\item
+  Altered source versions must be plainly marked as such, and must not be misrepresented as being the original software.
+\item
+  This notice may not be removed or altered from any source distribution.
+\end{enumerate}
+
+\subsection{MODELISAR Notice}\label{modelisar-notice}
+
+Copyright (c) 2008-2010, MODELISAR consortium. All rights reserved.
+
+This file is licensed by the copyright holders under the BSD License\footnote{\url{http://www.opensource.org/licenses/bsd-license.html\textgreater}}:
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+Redistribution and use in source and binary forms, with or withoutmodification, are permitted provided that the following conditions are met:
+
+\begin{itemize}
+\item
+  Redistributions of source code must retain the above copyright notice, this list of conditions and the following disclaimer.
+\item
+  Redistributions in binary form must reproduce the above copyright notice, this list of conditions and the following disclaimer in the documentation and/or other materials provided with the distribution.
+\item
+  Neither the name of the copyright holders nor the names of its contributors may be used to endorse or promote products derived from this software without specific prior written permission.
+\end{itemize}
+
+THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS ``AS IS'' AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
+
+\subsection{Functional Mock-up Unit for Co-Simulation Import Notice}\label{functional-mock-up-unit-for-co-simulation-import-notice}
+
+Functional Mock-up Unit for Co-Simulation Import in EnergyPlus Copyright (c) 2012, The Regents of the University of California, through Lawrence Berkeley National Laboratory (subject to receipt of any required approvals from the U.S. Dept. of Energy). All rights reserved.
+
+If you have questions about your rights to use or distribute this software, please contact Berkeley Lab's Technology Transfer Department at \textless{}TTD@lbl.gov\textgreater{}.
+
+NOTICE.~ This software was developed under partial funding from the U.S. Department of Energy.~ As such, the U.S. Government has been granted for itself and others acting on its behalf a paid-up, nonexclusive, irrevocable, worldwide license in the Software to reproduce, prepare derivative works, and perform publicly and display publicly.~ Beginning five (5) years after the date permission to assert copyright is obtained from the U.S. Department of Energy, and subject to any subsequent five (5) year renewals, the U.S. Government is granted for itself and others acting on its behalf a paid-up, nonexclusive, irrevocable, worldwide license in the Software to reproduce, prepare derivative works, distribute copies to the public, perform publicly and display publicly, and to permit others to do so.
+
+Modified BSD License agreement
+
+Functional Mock-up Unit for Co-Simulation Import in EnergyPlus Copyright (c) 2012, The Regents of the University of California, through Lawrence Berkeley National Laboratory (subject to receipt of any required approvals from the U.S. Dept. of Energy).~ All rights reserved.
+
+Redistribution and use in source and binary forms, with or without modification, are permitted provided that the following conditions are met:
+
+Redistributions of source code must retain the above copyright notice, this list of conditions and the following disclaimer.
+
+Redistributions in binary form must reproduce the above copyright notice, this list of conditions and the following disclaimer in the documentation and/or other materials provided with the distribution.
+
+Neither the name of the University of California, Lawrence Berkeley National Laboratory, U.S. Dept. of Energy nor the names of its contributors may be used to endorse or promote products derived from this software without specific prior written permission.
+
+THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS ``AS IS'' AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT OWNER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
+
+You are under no obligation whatsoever to provide any bug fixes, patches, or upgrades to the features, functionality or performance of the source code (``Enhancements'') to anyone; however, if you choose to make your Enhancements available either publicly, or directly to Lawrence Berkeley National Laboratory, without imposing a separate written license agreement for such Enhancements, then you hereby grant the following license: a non-exclusive, royalty-free perpetual license to install, use, modify, prepare derivative works, incorporate into other computer software, distribute, and sublicense such enhancements or derivative works thereof, in binary and source code form.
+
+\subsection{Functional Mock-up Unit Export of EnergyPlus Notice}\label{functional-mock-up-unit-export-of-energyplus-notice}
+
+Functional Mock-up Unit Export of EnergyPlus (c)2013, The Regents of the University of California, through Lawrence Berkeley National Laboratory (subject to receipt of any required approvals from the U.S. Department of Energy). All rights reserved.
+
+If you have questions about your rights to use or distribute this software, please contact Berkeley Lab's Technology Transfer Department at \textless{}TTD@lbl.gov\textgreater{}.referring to ``Functional Mock-up Unit Export of EnergyPlus (LBNL Ref 2013-088)''.
+
+NOTICE: This software was produced by The Regents of the University of California under Contract No. DE-AC02-05CH11231 with the Department of Energy.
+
+For 5 years from November 1, 2012, the Government is granted for itself and others acting on its behalf a nonexclusive, paid-up, irrevocable worldwide license in this data to reproduce, prepare derivative works, and perform publicly and display publicly, by or on behalf of the Government. There is provision for the possible extension of the term of this license.
+
+Subsequent to that period or any extension granted, the Government is granted for itself and others acting on its behalf a nonexclusive, paid-up, irrevocable worldwide license in this data to reproduce, prepare derivative works, distribute copies to the public, perform publicly and display publicly, and to permit others to do so. The specific term of the license can be identified by inquiry made to Lawrence Berkeley National Laboratory or DOE. Neither the United States nor the United States Department of Energy, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any data, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights.
+
+Copyright (c) 2013, The Regents of the University of California, Department of Energy contract-operators of the Lawrence Berkeley National Laboratory.
+
+All rights reserved.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\tightlist
+\item
+  Redistribution and use in source and binary forms, with or without modification, are permitted provided that the following conditions are met: 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\item
+  Redistributions of source code must retain the copyright notice, this list of conditions and the following disclaimer.
+\item
+  Redistributions in binary form must reproduce the copyright notice, this list of conditions and the following disclaimer in the documentation and/or other materials provided with the distribution.
+\item
+  Neither the name of the University of California, Lawrence Berkeley National Laboratory, U.S. Dept. of Energy nor the names of its contributors may be used to endorse or promote products derived from this software without specific prior written permission. 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS ``AS IS''
+\end{enumerate}
+
+AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT OWNER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  You are under no obligation whatsoever to provide any bug fixes, patches, or upgrades to the features, functionality or performance of the source code (``Enhancements'') to anyone; however, if you choose to make your Enhancements available either publicly, or directly to Lawrence Berkeley National Laboratory, without imposing a separate written license agreement for such Enhancements, then you hereby grant the following license: a non-exclusive, royalty-free perpetual license to install, use, modify, prepare derivative works, incorporate into other computer software, distribute, and sublicense such enhancements or derivative works thereof, in binary and source code form.
+\end{enumerate}
+
+NOTE: This license corresponds to the ``revised BSD'' or ``3-clause BSD''
+
+License and includes the following modification: Paragraph 3. has been added.
diff --git a/doc/auxiliary-programs/CMakeLists.txt b/doc/auxiliary-programs/CMakeLists.txt
new file mode 100644
index 00000000000..936499cd943
--- /dev/null
+++ b/doc/auxiliary-programs/CMakeLists.txt
@@ -0,0 +1,207 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/../header.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/auxiliary-programs.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/auxiliary-energyplus-programs.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/background.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/weather-format-for-simulation-programs.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/weather-data-availability.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/using-the-weather-converter.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/definitions-file-custom-file-processing.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/reports-files-produced-by-the-weather.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/k-ppen-climate-classification.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/ashrae-climate-classification.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/energyplus-weather-file-epw-data-dictionary.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/epw-csv-format-in-out.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/missing-weather-file-data.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/source-weather-data-formats.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/data-sources-uncertainty.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/advanced-use-accessing-weather-conversion.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/references.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/weather-converter-program/web-resources.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/use-of-the-ground-temperatures-with-slabs.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/slab-configuration-drawing.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/running-the-slab-program.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/technical-details-on-files-for-ground-heat.tex
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+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/references-001.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/view-factor-calculation-program.tex
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+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/view-factor-calculation-program/additional-information.tex
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+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/using-older-version-input-files-transition/converting-imf-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/epdrawgui.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/epdrawgui/main-tab.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/epdrawgui/option-tab.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/input-macros.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/input-macros/introduction-001.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/input-macros/running-the-ep-macro-program.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/input-macros/incorporating-external-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/input-macros/selectively-accepting-or-skipping-lines-of.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/input-macros/defining-blocks-of-input.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/input-macros/macro-debugging-and-listing-control.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/input-macros/listing-format.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-diagram.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-diagram/introduction-002.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/coeffconv-coeffcheck.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/coeffconv-coeffcheck/coeffconv.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/coeffconv-coeffcheck/coeffcheck.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/coeffconv-coeffcheck/running-the-coeffconv-or-coeffcheck-programs.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/expandobjects.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/expandobjects/introduction-003.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/expandobjects/hvac-template-objects-processed.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/expandobjects/ground-heat-transfer-objects-processed.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/expandobjects/building-surface-objects-processed.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/csvproc.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/convertesomtr.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/calcsoilsurftemp-program.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/calcsoilsurftemp-program/running-the-program.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/calcsoilsurftemp-program/program-inputs.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/calcsoilsurftemp-program/program-outputs.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/introduction-004.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/inputs.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/rated-data.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/performance-data.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/outputs.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/error-message.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/notes.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/references-002.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/parametric-spreadsheets.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-water-heat-pump-parameter.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-air-heat-pump-parameter-coefficient.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-air-heat-pump-parameter-coefficient-001.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/parametric-spreadsheets/g-function-spreadsheet.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/parametricpreprocessor.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/appgpostprocess-appendix-g-postprocessing.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/blasttranslator.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/doe2translator.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/running-console-applications.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/running-console-applications/modifying-the-batch-file.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/technical-details-of-running-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/technical-details-of-running-energyplus/ep-launch-program.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/technical-details-of-running-energyplus/ep-launch-lite.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/technical-details-of-running-energyplus/energyplus-file-extensions.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/technical-details-of-running-energyplus/runeplus-batch-file.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/technical-details-of-running-energyplus/running-energyplus-by-hand.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/technical-details-of-running-energyplus/runeplus-details.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/technical-details-of-running-energyplus/rundirmulti-batch-file.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/technical-details-of-running-energyplus/energyplus-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/creating-input-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/creating-input-files/idd-conventions.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/creating-input-files/idfeditor.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/manipulating-output-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/src/manipulating-output-files/ep-compare.tex
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/../title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image001.jpg
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image002.jpg
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image003.jpg
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image006.jpg
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image007.jpg
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+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image107.png
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image108.png
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image109.png
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+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image118.png
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image119.png
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image120.png
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image121.png
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image122.png
+  ${CMAKE_SOURCE_DIR}/doc/auxiliary-programs/media/image123.png
+) 
+
+SET( SOURCE_FILENAME "auxiliary-programs" )
+SET( OUTPUT_FILENAME "AuxiliaryPrograms" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/auxiliary-programs/auxiliary-programs.tex b/doc/auxiliary-programs/auxiliary-programs.tex
new file mode 100644
index 00000000000..a6b58550cfc
--- /dev/null
+++ b/doc/auxiliary-programs/auxiliary-programs.tex
@@ -0,0 +1,224 @@
+\input{../header}
+
+\title{Auxiliary Programs}
+
+\hypersetup{unicode=true,
+            pdftitle={Auxiliary Programs},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/auxiliary-energyplus-programs}
+
+\input{src/weather-converter-program}
+
+\input{src/weather-converter-program/background}
+
+\input{src/weather-converter-program/weather-format-for-simulation-programs}
+
+\input{src/weather-converter-program/weather-data-availability}
+
+\input{src/weather-converter-program/using-the-weather-converter}
+
+\input{src/weather-converter-program/definitions-file-custom-file-processing}
+
+\input{src/weather-converter-program/reports-files-produced-by-the-weather}
+
+\input{src/weather-converter-program/k-ppen-climate-classification}
+
+\input{src/weather-converter-program/ashrae-climate-classification}
+
+\input{src/weather-converter-program/energyplus-weather-file-epw-data-dictionary}
+
+\input{src/weather-converter-program/epw-csv-format-in-out}
+
+\input{src/weather-converter-program/missing-weather-file-data}
+
+\input{src/weather-converter-program/source-weather-data-formats}
+
+\input{src/weather-converter-program/data-sources-uncertainty}
+
+\input{src/weather-converter-program/advanced-use-accessing-weather-conversion}
+
+\input{src/weather-converter-program/references}
+
+\input{src/weather-converter-program/web-resources}
+
+\input{src/ground-heat-transfer-in-energyplus}
+
+\input{src/ground-heat-transfer-in-energyplus/use-of-the-ground-temperatures-with-slabs}
+
+\input{src/ground-heat-transfer-in-energyplus/slab-configuration-drawing}
+
+\input{src/ground-heat-transfer-in-energyplus/running-the-slab-program}
+
+\input{src/ground-heat-transfer-in-energyplus/technical-details-on-files-for-ground-heat}
+
+\input{src/ground-heat-transfer-in-energyplus/slab-program-output-files}
+
+\input{src/ground-heat-transfer-in-energyplus/description-of-the-objects-in-the-e-slabght}
+
+\input{src/ground-heat-transfer-in-energyplus/using-ground-temperatures-with-basements}
+
+\input{src/ground-heat-transfer-in-energyplus/running-the-basement-program}
+
+\input{src/ground-heat-transfer-in-energyplus/technical-details-on-files-for-ground-heat-001}
+
+\input{src/ground-heat-transfer-in-energyplus/basement-program-output-files}
+
+\input{src/ground-heat-transfer-in-energyplus/the-basement-idd}
+
+\input{src/ground-heat-transfer-in-energyplus/description-of-the-objects-in-the-basementght}
+
+\input{src/ground-heat-transfer-in-energyplus/using-the-interface-surface-temperature}
+
+\input{src/ground-heat-transfer-in-energyplus/references-001}
+
+\input{src/view-factor-calculation-program}
+
+\input{src/view-factor-calculation-program/using-the-view-factor-interface-program}
+
+\input{src/view-factor-calculation-program/additional-information}
+
+\input{src/using-older-version-input-files-transition}
+
+\input{src/using-older-version-input-files-transition/idf-version-updater}
+
+\input{src/using-older-version-input-files-transition/transition-console-program-details}
+
+\input{src/using-older-version-input-files-transition/idf-version-converter-transition-file-lists}
+
+\input{src/using-older-version-input-files-transition/converting-imf-files}
+
+\input{src/epdrawgui}
+
+\input{src/epdrawgui/main-tab}
+
+\input{src/epdrawgui/option-tab}
+
+\input{src/input-macros}
+
+\input{src/input-macros/introduction-001}
+
+\input{src/input-macros/running-the-ep-macro-program}
+
+\input{src/input-macros/incorporating-external-files}
+
+\input{src/input-macros/selectively-accepting-or-skipping-lines-of}
+
+\input{src/input-macros/defining-blocks-of-input}
+
+\input{src/input-macros/macro-debugging-and-listing-control}
+
+\input{src/input-macros/listing-format}
+
+%\input{src/hvac-diagram}
+
+\input{src/hvac-diagram/introduction-002}
+
+\input{src/coeffconv-coeffcheck}
+
+\input{src/coeffconv-coeffcheck/coeffconv}
+
+\input{src/coeffconv-coeffcheck/coeffcheck}
+
+\input{src/coeffconv-coeffcheck/running-the-coeffconv-or-coeffcheck-programs}
+
+\input{src/expandobjects}
+
+\input{src/expandobjects/introduction-003}
+
+\input{src/expandobjects/hvac-template-objects-processed}
+
+\input{src/expandobjects/ground-heat-transfer-objects-processed}
+
+\input{src/expandobjects/building-surface-objects-processed}
+
+\input{src/csvproc}
+
+\input{src/convertesomtr}
+
+\input{src/calcsoilsurftemp-program}
+
+\input{src/calcsoilsurftemp-program/running-the-program}
+
+\input{src/calcsoilsurftemp-program/program-inputs}
+
+\input{src/calcsoilsurftemp-program/program-outputs}
+
+\input{src/hvac-performance-curve-fit-tool}
+
+\input{src/hvac-performance-curve-fit-tool/introduction-004}
+
+\input{src/hvac-performance-curve-fit-tool/inputs}
+
+\input{src/hvac-performance-curve-fit-tool/rated-data}
+
+\input{src/hvac-performance-curve-fit-tool/performance-data}
+
+\input{src/hvac-performance-curve-fit-tool/outputs}
+
+\input{src/hvac-performance-curve-fit-tool/error-message}
+
+\input{src/hvac-performance-curve-fit-tool/notes}
+
+\input{src/hvac-performance-curve-fit-tool/references-002}
+
+\input{src/parametric-spreadsheets}
+
+\input{src/parametric-spreadsheets/water-to-water-heat-pump-parameter}
+
+\input{src/parametric-spreadsheets/water-to-air-heat-pump-parameter-coefficient}
+
+\input{src/parametric-spreadsheets/water-to-air-heat-pump-parameter-coefficient-001}
+
+\input{src/parametric-spreadsheets/g-function-spreadsheet}
+
+\input{src/parametricpreprocessor}
+
+\input{src/appgpostprocess-appendix-g-postprocessing}
+
+\input{src/blasttranslator}
+
+\input{src/doe2translator}
+
+\input{src/running-console-applications}
+
+\input{src/running-console-applications/modifying-the-batch-file}
+
+\input{src/technical-details-of-running-energyplus}
+
+\input{src/technical-details-of-running-energyplus/ep-launch-program}
+
+\input{src/technical-details-of-running-energyplus/ep-launch-lite}
+
+\input{src/technical-details-of-running-energyplus/energyplus-file-extensions}
+
+\input{src/technical-details-of-running-energyplus/runeplus-batch-file}
+
+\input{src/technical-details-of-running-energyplus/running-energyplus-by-hand}
+
+\input{src/technical-details-of-running-energyplus/runeplus-details}
+
+\input{src/technical-details-of-running-energyplus/rundirmulti-batch-file}
+
+\input{src/technical-details-of-running-energyplus/energyplus-files}
+
+\input{src/creating-input-files}
+
+\input{src/creating-input-files/idd-conventions}
+
+\input{src/creating-input-files/idfeditor}
+
+\input{src/manipulating-output-files}
+
+\input{src/manipulating-output-files/ep-compare}
+
+\end{document}
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diff --git a/doc/auxiliary-programs/src/appgpostprocess-appendix-g-postprocessing.tex b/doc/auxiliary-programs/src/appgpostprocess-appendix-g-postprocessing.tex
new file mode 100644
index 00000000000..f8d91fe3c99
--- /dev/null
+++ b/doc/auxiliary-programs/src/appgpostprocess-appendix-g-postprocessing.tex
@@ -0,0 +1,43 @@
+\chapter{AppGPostProcess - Appendix G PostProcessing program}\label{appgpostprocess---appendix-g-postprocessing-program}
+
+The baseline for Standard 90.1 Appendix G requires simulating the baseline building in four cardinal directions and comparing the average of those simulation results with the proposed building simulation results. The AppGPostProcess utility helps perform the averaging needed. The utility takes the four HTML files generated by EnergyPlus and creates an average HTML file. In addition, the AppGPostProcess utility takes the four CSV files (based on ESO files) and creates an average CSV file as well as averaging the meter CSV files (based on the MTR files). The source files must have specific names for this utility to work:
+
+fileNameRoot-G000.csv
+
+fileNameRoot-G090.csv
+
+fileNameRoot-G180.csv
+
+fileNameRoot-G270.csv
+
+fileNameRoot-G000Meter.csv
+
+fileNameRoot-G090Meter.csv
+
+fileNameRoot-G180Meter.csv
+
+fileNameRoot-G270Meter.csv
+
+fileNameRoot-G000Table.html
+
+fileNameRoot-G090Table.html
+
+fileNameRoot-G180Table.html
+
+fileNameRoot-G270Table.html
+
+Where ``fileNameRoot'' can be the characters typically used to name files without extension. A single command line argument is passed to the AppGPostProcess utility which is the name of one of the HTML files. The remaining file names will be used based on any of the HTML files selected.
+
+The utility creates the files
+
+fileNameRoot-GAVG.csv
+
+fileNameRoot-GAVGMeter.csv
+
+fileNameRoot-GAVGTable.html
+
+The numeric values in the output files are the average results from the four corresponding source files. In the HTML file, if not all the four files contain a numeric value, then the four values are displayed instead. The source files must have identical structure for AppGPostProcess to work. For CSV files, the same number of rows and the same number of columns are needed each file. This means that monthly or hourly values should be included in the CSV file, and not TimeStep values. For HTML files, the same reports should be included in each and the IDF files should be identical.
+
+The intention is that the four baseline IDF files would be identical except for the use of the Compliance:Building object and only the value of the field ``Building Rotation for Appendix G'' would change.
+
+EP-Launch can be used to run both the AppGPostProcess program by using the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch.
diff --git a/doc/auxiliary-programs/src/auxiliary-energyplus-programs.tex b/doc/auxiliary-programs/src/auxiliary-energyplus-programs.tex
new file mode 100644
index 00000000000..9f2709448b7
--- /dev/null
+++ b/doc/auxiliary-programs/src/auxiliary-energyplus-programs.tex
@@ -0,0 +1,47 @@
+\input{../title}
+
+\chapter{Auxiliary Programs Introduction}\label{auxiliary-programs-introduction}
+
+This document will describe several of the ``auxiliary programs'' of the EnergyPlus system in more detail. Some of these programs are only available or only distributed for certain platforms. Typically, the programs are available on the Windows platform. Within the descriptions, other platforms will be noted as applicable. These programs include:
+
+\textbf{Weather Converter Program} (aka ``Weather'')
+
+\textbf{Ground Heat Transfer in EnergyPlus} - Procedure for Ground Temperature creation
+
+\textbf{View Factor Calculation Program} - Auxiliary program used to calculate View Factors which can be used with EnergyPlus
+
+\textbf{Using Older Version Input Files - Transition} - to convert input files from one version to another upon release of a new version
+
+\textbf{EPDraw} - Create DXF files from your input files
+
+\textbf{Input Macros} - Use a macro language to increase efficiency in creating EnergyPlus input files. Unfortunately, IDF files containing macros cannot be read in the IDF Editor.
+
+\textbf{HVAC Diagram} - Use a post processing program to diagram your HVAC inputs.
+
+\textbf{CoeffConv/CoeffCheck} - Convert DOE-2 temperature dependent curves (Fahrenheit) to EnergyPlus temperature curves (Centigrade/Celsius)
+
+\textbf{ExpandObjects} - Some technical details of the Expand Objects program which preprocessed HVACTemplate:* and GroundHeatTransfer:* objects for use inside EnergyPlus.
+
+\textbf{CSVproc} - Get simple statistics from CSV output files.
+
+\textbf{convertESOMTR} - convert your outputs to Inch-Pound (default) or other custom unit conversions.
+
+\textbf{CalcSoilSurfTemp Program} - calculate soil surface parameters used in the Earth Tube simulation
+
+\textbf{HVAC Performance Curve Fit Tool}- generates HVAC performance curves in EnergyPlus IDF format
+
+\textbf{Parametric Spreadsheets} - Parametric spreadsheets are available to help illustrate or calculate some parameters/coefficients.
+
+\textbf{ParametricPreprocessor} \textbf{-} Special objects can be inserted in IDF files and generate a series of IDF files from a single source IDF file that contains parametric objects and expressions. Unlike using the macro language, these input files are capable of being read in the IDF Editor.
+
+\textbf{AppGPostProcess - Appendix G PostProcessing program} - The ASHRAE 90.1 Appendix G postprocessing program takes simulation outputs and processes them to help meet Appendix G requirements..
+
+\textbf{BLASTTranslator} - The BLAST translator can take BLAST (Building Loads Analysis and System Thermodynamics) input files and make them ready for running in EnergyPlus.
+
+\textbf{DOE2Translator} - The DOE-2 translator can take DOE-2 program input files and make them ready for running in EnergyPlus.
+
+\textbf{Running Console Applications} - this section describes how to run console applications that are part of EnergyPlus and how you might modify these to your specific needs. Instructions for running individual programs are included in their descriptions.
+
+\textbf{Technical Details of Running EnergyPlus} - this section gives full instructions on both EP-Launch and the IDF-Editor as well as some more details on running EnergyPlus manually.
+
+\textbf{EP-Compare} - A utility to graphically compare tabular results from multiple simulation files.
diff --git a/doc/auxiliary-programs/src/blasttranslator.tex b/doc/auxiliary-programs/src/blasttranslator.tex
new file mode 100644
index 00000000000..5676e678148
--- /dev/null
+++ b/doc/auxiliary-programs/src/blasttranslator.tex
@@ -0,0 +1,25 @@
+\chapter{BLASTTranslator}\label{blasttranslator}
+
+The BLAST Translator will produce an IDF file from an existing BLAST Input File (usually called \textless{}something\textgreater{}.bin. For anyone that is unfamiliar, BLAST stands for the Building Loads Analysis and Systems Thermodynamics computer program. Documentation is included here though the BLAST Translator is no longer included with the EnergyPlus Installation - it is available as a special download for those who need it.
+
+A special batch file (\textbf{RunXLate.bat}) can be used to run the translation program. Similar to running EnergyPlus (see above), you run this batch file:
+
+RunXLate \textless{}blastinputfile\textgreater{}
+
+Where \textless{}blastinputfile\textgreater{} is the part of the file name without extension. The program produces a .idf file of the same name.
+
+The BLASTTranslator uses an ``Energy+.ini'' file for some parameters. For example:
+
+\begin{lstlisting}
+[program]
+dir =
+ver =
+surf = group
+\end{lstlisting}
+
+\begin{lstlisting}
+[weather]
+dir =
+\end{lstlisting}
+
+The above BLASTTranslator ini file sets the ``version'' of EnergyPlus to the current version and has the ``surf'' parameter set to ``group''. This BLASTTranslator run will produce an EnergyPlus input file for the current release version format and will name surfaces by Zone and Class (e.g.~ZN001:Wall001). The alternative ``Consecutive'' will number surfaces in sequence.
diff --git a/doc/auxiliary-programs/src/calcsoilsurftemp-program.tex b/doc/auxiliary-programs/src/calcsoilsurftemp-program.tex
new file mode 100644
index 00000000000..50c882afe1e
--- /dev/null
+++ b/doc/auxiliary-programs/src/calcsoilsurftemp-program.tex
@@ -0,0 +1,16 @@
+\chapter{CalcSoilSurfTemp Program}\label{calcsoilsurftemp-program}
+
+The CalcSoilSurfTemp program calculates three important parameters for the simulation of the earth tube:
+
+\begin{itemize}
+\item
+  the annual average soil surface temperature
+\item
+  the amplitude of soil surface temperature
+\item
+  the phase constant of soil surface temperature
+\end{itemize}
+
+Since soil temperature is one of the most significant factors affecting the overall performance of earth tube system, soil temperature around the earth tube should be accurately predicted.
+
+Before the soil temperature around earth tube can be calculated during the running period of earth tube model in EnergyPlus, the ground surface temperature straight above earth tube should be predicted. Using CalcSoilSurfTemp program, these parameters are predicted by considering the convective heat transfer between the air and ground, solar radiation absorption by the ground, long-wave radiation emitted from the soil, and latent heat loss due to the moisture evaporation at the ground surface.
diff --git a/doc/auxiliary-programs/src/calcsoilsurftemp-program/program-inputs.tex b/doc/auxiliary-programs/src/calcsoilsurftemp-program/program-inputs.tex
new file mode 100644
index 00000000000..57f3d0cfd71
--- /dev/null
+++ b/doc/auxiliary-programs/src/calcsoilsurftemp-program/program-inputs.tex
@@ -0,0 +1,47 @@
+\section{Program Inputs}\label{program-inputs}
+
+In order to use the CalcSoilSurfTemp program, a weather data file is used. The entire year of weather data is used to calculate parameters of the soil surface temperature.
+
+The CalcSoilSurfTemp program is simple and requires only two input fields: soil condition and soil surface condition. First, the user will see the four following options in the screen for the selection of the soil condition:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  HEAVY AND SATURATED
+\item
+  HEAVY AND DAMP
+\item
+  HEAVY AND DRY
+\item
+  LIGHT AND DRY
+\end{enumerate}
+
+Among them, the user should select the number corresponding to the particular soil condition. This determines the thermal diffusivity and thermal conductivity of the surrounding soil.
+
+After the selection of soil condition, the user should also select the number corresponding to the condition of the ground surface above the earth tube from the eight following options:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  BARE AND WET
+\item
+  BARE AND MOIST
+\item
+  BARE AND ARID
+\item
+  BARE AND DRY
+\item
+  COVERED AND WET
+\item
+  COVERED AND MOIST
+\item
+  COVERED AND ARID
+\item
+  COVERED AND DRY
+\end{enumerate}
+
+This determines the absorption coefficient and the fraction of evaporation rate of the ground surface.
+
+Note that both soil condition and soil surface condition are the average of the year - not a particular time period within the year.
+
+From this information and an analysis of the weather data, the CalcSoilSurfTemp program calculates the annual average soil surface temperature, the amplitude of soil surface temperature, and the phase constant of soil surface temperature. The user must then add these parameters as input parameter into earth tube model in EnergyPlus.
diff --git a/doc/auxiliary-programs/src/calcsoilsurftemp-program/program-outputs.tex b/doc/auxiliary-programs/src/calcsoilsurftemp-program/program-outputs.tex
new file mode 100644
index 00000000000..06662acb5f9
--- /dev/null
+++ b/doc/auxiliary-programs/src/calcsoilsurftemp-program/program-outputs.tex
@@ -0,0 +1,153 @@
+\section{Program Outputs}\label{program-outputs}
+
+As noted earlier, there are three output parameters and they are automatically saved in the CalcSoilSurfTemp.out file. The basic concept and description of three output parameters are as follows.
+
+\textbf{Annual Average Soil Surface Temperature}
+
+This is the annual average value of soil surface temperature.
+
+\textbf{Amplitude of Soil Surface Temperature}
+
+This is the difference between the maximum and minimum soil surface temperature of the whole year divided by two.
+
+\textbf{Phase Constant of Soil Surface Temperature}
+
+This is the time elapsed from the beginning of the year at which the soil surface temperature reaches the minimum value in the year.
+
+These values are placed in the ZoneEarthTube object numeric fields (12, 13, 14) of similar names. The ZoneEarthTube IDD definition with these fields highlighted is included:
+
+\begin{lstlisting}
+
+ZoneEarthtube,
+  \min-fields 22
+  \memo  Earth Tube is specified as a design level which is modified by a Schedule fraction, temperature difference and wind speed:
+  \memo  Earthtube = Edesign * Fschedule * (A + B*|(Tzone-Todb)| + C*WindSpd + D * WindSpd**2)
+  A1, \field Zone Name
+  \required-field
+  \type object-list
+  \object-list ZoneNames
+  A2, \field Schedule Name
+  \required-field
+  \type object-list
+  \object-list ScheduleNames
+  N1, \field Design Flow Rate
+  \required-field
+  \units m3/s
+  \note  "Edesign" in Equation
+  \type real
+  \minimum 0
+  N2, \field Minimum Zone Temperature when Cooling
+  \required-field
+  \note this is the indoor temperature below which the earth tube is shut off
+  \units C
+  \type real
+  \minimum -100
+  \maximum 100
+  N3, \field Maximum Zone Temperature when Heating
+  \required-field
+  \note this is the indoor temperature above which the earth tube is shut off
+  \units C
+  \type real
+  \minimum -100
+  \maximum 100
+  N4, \field Delta Temperature
+  \required-field
+  \note This is the temperature difference between indoor and outdoor below which the earth tube is shut off
+  \units deltaC
+  \type real
+  \minimum 0
+  A3, \field Earthtube Type
+  \required-field
+  \type choice
+  \key Natural
+  \key Intake
+  \key Exhaust
+  \default Natural
+  N5, \field Fan Pressure Rise
+  \required-field
+  \note pressure rise across the fan
+  \type real
+  \units Pa
+  \minimum 0
+  \default 0
+  N6, \field Fan Total Efficiency
+  \required-field
+  \type real
+  \minimum> 0
+  \default 1
+  N7, \field Pipe Radius
+  \required-field
+  \units m
+  \type real
+  \minimum> 0
+  \default 1
+  N8, \field Pipe Thickness
+  \required-field
+  \units m
+  \type real
+  \minimum> 0
+  \default 0.2
+  N9, \field Pipe Length
+  \required-field
+  \units m
+  \type real
+  \minimum> 0
+  \default 15
+  N10, \field Pipe Thermal Conductivity
+  \required-field
+  \units W/m-K
+  \type real
+  \minimum> 0
+  \default 200
+  N11, \field Pipe Depth Under Ground Surface
+  \required-field
+  \units m
+  \type real
+  \minimum> 0
+  \default 3
+  A4, \field Soil Condition
+  \required-field
+  \type choice
+  \key HeavyAndSaturated
+  \key HeavyAndDamp
+  \key HeavyAndDry
+  \key LightAndDry
+  \default HeavyAndDamp
+  N12, \field Average Soil Surface Temperature
+  \required-field
+  \units C
+  \type real
+  \default 0
+  N13, \field Amplitude of Soil Surface Temperature
+  \required-field
+  \units C
+  \type real
+  \minimum 0
+  \default 0
+  N14, \field Phase Constant of Soil Surface Temperature
+  \required-field
+  \units days
+  \type real
+  \minimum 0
+  \default 0
+  N15, \field Constant Term Flow Coefficient
+  \required-field
+  \note  "A" in Equation
+  \type real
+  \default 1
+  N16, \field Temperature Term Flow Coefficient
+  \required-field
+  \note  "B" in Equation
+  \type real
+  \default 0
+  N17, \field Velocity Term Flow Coefficient
+  \required-field
+  \note  "C" in Equation
+  \type real
+  \default 0
+  N18; \field Velocity Squared Term Flow Coefficient
+  \required-field
+  \note  "D" in Equation
+  \type real
+  \default 0
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/calcsoilsurftemp-program/running-the-program.tex b/doc/auxiliary-programs/src/calcsoilsurftemp-program/running-the-program.tex
new file mode 100644
index 00000000000..8b73df20851
--- /dev/null
+++ b/doc/auxiliary-programs/src/calcsoilsurftemp-program/running-the-program.tex
@@ -0,0 +1,41 @@
+\section{Running the Program}\label{running-the-program}
+
+EP-Launch can be used to run the CalcSoilSurfTemp program. CalcSoilSurfTemp is one of the options on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the CalcSoilSurfTemp program.
+
+You can also run the CalcSoilSurfTemp program as a console application with a batch file RunCalcSoilSurfTemp. The argument to the batch file is the name of the weather file to be used. Steps to running this program follow:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Open a DOS command prompt window (Start à Programs à Accessories à Command Prompt)
+\item
+  Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
+\end{enumerate}
+
+C:
+
+CD \textbackslash{}\textless{}root folder\textgreater{}\textless{}/span\textgreater{}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Change to the calculate surface soil temperature folder:
+\end{enumerate}
+
+CD PreProcess\textbackslash{}CalcSoilSurfTemp
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Run the program:
+\end{enumerate}
+
+runcalcsoilsurftemp USA\_IL\_Chicago-OHare\_TMY2
+
+When installed, the batch file automatically points the path for weather data to the installed weather data path. If you save your weather files in a different location, you will need to modify the batch file or create your own with your own folder paths.
+
+Note that the program is interactive (expects user responses) from the command line. These inputs are described in the following section.
diff --git a/doc/auxiliary-programs/src/coeffconv-coeffcheck.tex b/doc/auxiliary-programs/src/coeffconv-coeffcheck.tex
new file mode 100644
index 00000000000..b5643fd816e
--- /dev/null
+++ b/doc/auxiliary-programs/src/coeffconv-coeffcheck.tex
@@ -0,0 +1,3 @@
+\chapter{CoeffConv/CoeffCheck}\label{coeffconvcoeffcheck}
+
+These two programs are stored in the PreProcess folder of your EnergyPlus installation under a folder CoeffConv.
diff --git a/doc/auxiliary-programs/src/coeffconv-coeffcheck/coeffcheck.tex b/doc/auxiliary-programs/src/coeffconv-coeffcheck/coeffcheck.tex
new file mode 100644
index 00000000000..5c42323419f
--- /dev/null
+++ b/doc/auxiliary-programs/src/coeffconv-coeffcheck/coeffcheck.tex
@@ -0,0 +1,38 @@
+\section{CoeffCheck}\label{coeffcheck}
+
+CoeffCheck is a program to print out a performance map given a bi-quadratic performance curve.
+
+EP-Launch can be used to run the CoeffCheck program. CoeffCheck is one of the options on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the CoeffCheck program. When using EP-Launch to run CoeffCheck the input file must have the file extension .cci and will create an output file with the file extension .cco.
+
+You can also run the CoeffCheck program as a console application. The input file then must be from file CoeffCheckInput.txt (status = OLD). There are 6 lines of ascii input.
+
+For example:
+
+\begin{lstlisting}
+VarSpeedCoolCapFt
+0.476428E+00,0.401147E-01,0.226411E-03,-0.827136E-03,-0.732240E-05,-0.446278E-03
+12.777778,23.888889
+23.888889,46.111111
+19.444444,35.0
+2.777778
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  The 1st line is the user selected name of the curve.
+\item
+  The 2nd line contains the 6 biquadratic curve coefficients, comma separated.
+\item
+  The 3rd line contains the min and max values of the 1st independent variable, comma separated
+\item
+  The 4th line contains the min and max values of the 2nd independent variable, comma separated
+\item
+  The 5th line contains the rated values of the 1st \& 2nd independent variables, comma separated
+\item
+  The 6th line contains the delta T for the output performance map
+\end{itemize}
+
+The output file is CoeffCheckOutput.txt (status = NEW).
+
+There is an example input file and an example output file installed with the program.
diff --git a/doc/auxiliary-programs/src/coeffconv-coeffcheck/coeffconv.tex b/doc/auxiliary-programs/src/coeffconv-coeffcheck/coeffconv.tex
new file mode 100644
index 00000000000..0c401b87db6
--- /dev/null
+++ b/doc/auxiliary-programs/src/coeffconv-coeffcheck/coeffconv.tex
@@ -0,0 +1,46 @@
+\section{CoeffConv}\label{coeffconv}
+
+CoeffConv is a program to convert DOE-2 temperature dependent curves in Fahrenheit to EnergyPlus curves in Centigrade. The program converts the DOE-2 coefficients of a biquadratic curve to the equivalent EnergyPlus biquadratic curve coefficients.
+
+EP-Launch can be used to run the CoeffConv program. CoeffConv is one of the options on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the CoeffConv program. When using EP-Launch to run CoeffConv the input file must have the file extension .coi and will create an output file with the file extension .coo.
+
+You can also run the CoeffConv program as a console application. The input file then must be from file CoeffConvInput.txt (status = OLD). There are 6 lines of ascii input.
+
+For example:
+
+\begin{lstlisting}
+VarSpeedCoolCapFt
+-0.29382,0.0222213,0.00006988,0.0040928,-0.00000226,-0.00013774
+55.,75.
+75.,115.
+67.0,95.0
+5.0
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  The 1st line is the user selected name of the curve.
+\item
+  The 2nd line contains the 6 biquadratic curve coefficients, comma separated. These are the Doe-2 coefficients.
+\item
+  The 3rd line contains the min and max values of the 1st independent variable, comma separated, deg F.
+\item
+  The 4th line contains the min and max values of the 2nd independent variable, comma separated, deg F.
+\item
+  The 5th line contains the rated values of the 1st \& 2nd independent variables, comma separated, deg F.
+\item
+  The 6th line contains the delta T for the output performance maps.
+\end{itemize}
+
+All the input lines should start in column 1.
+
+The above sequence can be repeated up to 100 times.
+
+The output file is CoeffConvOutput.txt (status = NEW) (that means you need to delete any existing CoeffConvOutput.txt).
+
+The output file will contain the EnergyPlus idf input for the curve, as well as any error messages;
+
+Also, the DOE-2 and EnergyPlus curve values at the rating point (where the value should be 1.0) and performance maps for the curves - both DOE-2 and EnergyPlus.
+
+There is an example input file and an example output file installed with the program.
diff --git a/doc/auxiliary-programs/src/coeffconv-coeffcheck/running-the-coeffconv-or-coeffcheck-programs.tex b/doc/auxiliary-programs/src/coeffconv-coeffcheck/running-the-coeffconv-or-coeffcheck-programs.tex
new file mode 100644
index 00000000000..64ff91b571f
--- /dev/null
+++ b/doc/auxiliary-programs/src/coeffconv-coeffcheck/running-the-coeffconv-or-coeffcheck-programs.tex
@@ -0,0 +1,37 @@
+\section{Running the CoeffConv or CoeffCheck programs}\label{running-the-coeffconv-or-coeffcheck-programs}
+
+EP-Launch can be used to run both the CoeffConv and CoeffCheck programs. CoeffConv and CoeffCheck are two of the options on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the CoeffConv and CoeffCheck programs.
+
+You can also run both programs as console applications and, because they are small, they are automatically installed with EnergyPlus. You will need to open a command window using the following steps:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Open a DOS command prompt window (Start -\textgreater{} Programs -\textgreater{} Accessories -\textgreater{} Command Prompt)
+\item
+  Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
+\end{enumerate}
+
+C:
+
+CD \textbackslash{}\textless{}rootfolder\textgreater{}\textless{}/span\textgreater{}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Change to the specific folder for the coefficient conversion applications:
+\end{enumerate}
+
+CD PreProcess\textbackslash{}CoeffConv
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Run the program:
+\end{enumerate}
+
+After creating your files as shown above, enter either CoeffConv or CoeffCheck as desired. The folder also contains a ``readme.txt'' file which you can peruse.
diff --git a/doc/auxiliary-programs/src/convertesomtr.tex b/doc/auxiliary-programs/src/convertesomtr.tex
new file mode 100644
index 00000000000..3a9d49ddef2
--- /dev/null
+++ b/doc/auxiliary-programs/src/convertesomtr.tex
@@ -0,0 +1,26 @@
+\chapter{convertESOMTR}\label{convertesomtr}
+
+This simple post processing utility will convert the raw data ``ESO'' and ``MTR'' files to IP (Inch-Pound) units before later processing into CSV files. EP-Launch has an option to automatically convert to IP units that invokes convertESOMTR, see VIEW - Options - Miscellaneous dialog box. The ReadVarsESO program will take these converted files and make them into normal CSV files but will have IP units. The RunEPlus batch file does not include this option but could be edited to perform the same functions if desired.
+
+Technically speaking, the convertESOMTR program uses the ``convert.txt'' file which contains the conversion factors. It creates files ``ip.eso'' and ``ip.mtr'' as appropriate. The batch examples then renames the old eplusout.eso to eplusout.esoold, old eplusout.mtr to eplusout.mtrold and the ip files to the default eplusout.eso, eplusout.mtr.
+
+The convert.txt file contains the conversion factors using three different commands.
+
+conv,\textless{}si-unit\textgreater{},\textless{}ip-unit\textgreater{},\textless{}multiplier\textgreater{},\textless{}offset\textgreater{}
+
+wild,\textless{}match-string\textgreater{},\textless{}si-unit\textgreater{},\textless{}ip-unit\textgreater{}
+
+vari,\textless{}variable-name-no-units\textgreater{},\textless{}si-unit\textgreater{},\textless{}ip-unit\textgreater{}
+
+If a specific variable needs to be converted, the `vari' line may be used to convert the units on that specific variable only. To convert a class of variables that contains a specific string of characters in the names of the variables, the `wild' line may be used. The `conv' lines are the lines that actually create the conversion factors. If no `vari' or `wild' match a variable, then it is converted used the first `conv' line that matches. The default convert.txt file contains some conversions for Inch-Pound units but any set of units may be used by editing the convert.txt file. Note that the convert.txt file uses the standard EnergyPlus comment character (!).
+
+A snippet of the convert.txt file:
+
+\begin{lstlisting}
+! Power
+!------------------------------
+!    (1 kW / 1000 W)
+conv,W,kW,0.001,0
+!    (1 Btuh/ 0.2928751 W) * (1 kBtuh/1000 Btuh)
+conv,W,kBtuh,3.41442E-03,0
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/creating-input-files.tex b/doc/auxiliary-programs/src/creating-input-files.tex
new file mode 100644
index 00000000000..74e592aad83
--- /dev/null
+++ b/doc/auxiliary-programs/src/creating-input-files.tex
@@ -0,0 +1,17 @@
+\chapter{Creating Input Files}\label{creating-input-files}
+
+EnergyPlus has several options for the user to create input files. One of the goals of EnergyPlus was to make a simple, readable input file for the program. More of this background and explanation is contained in the Interface Developer's Guide. Understanding the Input Data Dictionary (IDD) is the key to reading the input file. We have set some conventions for commenting the IDD so that the units, minimum, maximum, and other information. This changes some of the information that is shown in the Interface Developer's guide. The Energy+.idd (delivered with the install program) contains the most current information. In addition to the four methods for creating inputs described below, several other items are described that may assist you in getting the results you want from EnergyPlus in a timely manner.
+
+Four methods (with the installed program) are available to create input files:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  IDFEditor - this is a very simple, ``intelligent'' editor that reads the IDD and IDFs and allows creation/revision of IDF files. It can be run from a shortcut in the main EnergyPlus directory (created as part of the install) or directly from EP-Launch.
+\item
+  BLAST Translator - if you already have BLAST and/or BLAST input files, this program will produce the bulk of a translation to EnergyPlus for you. It generates a complete IDF file but does not include specifics for Systems or Plants. (It does include the System and Plant schedules that were in the BLAST deck). Many of the sample files included with the install started out as BLAST input files.
+\item
+  DOE-2 Translator - if you already have DOE-2.1e input files, this program will produce the bulk of a translation to EnergyPlus for you. It generates a IMF (input macro file) that must be run through the EnergyPlus Macro (EPMacro) program before it can be used by EnergyPlus.
+\item
+  Hand editing - for simple changes to an existing file (such as one of the sample files), you can hand edit a file using your knowledge of the IDD, comments in the IDF file, and a text editor such as NOTEPADâ„¢ (Wordpadâ„¢ for large files). For creating HVAC simulations - the HVACtemplate objects provide a quick way to start at HVAC simulation.
+\end{enumerate}
diff --git a/doc/auxiliary-programs/src/creating-input-files/idd-conventions.tex b/doc/auxiliary-programs/src/creating-input-files/idd-conventions.tex
new file mode 100644
index 00000000000..66dd64cebbb
--- /dev/null
+++ b/doc/auxiliary-programs/src/creating-input-files/idd-conventions.tex
@@ -0,0 +1,332 @@
+\section{IDD Conventions}\label{idd-conventions}
+
+The following is a basic description of the structure of the IDD (it's actually taken directly from the IDD file). As noted within, ! signifies a comment character as does the \textbackslash{}. \textbackslash{} has also been adopted as a convention for including more specific comments about each field in an object. These have been used with success in the IDFEditor and it is hoped the flexibility will provide other interface developers with useful information.
+
+\begin{lstlisting}
+! Object Description
+! ------------------
+! To define an object (a record with data), develop a key word that is unique
+! Each data item to the object can be A (Alphanumeric string) or N (numeric)
+! Number each A and N.  This will show how the data items will be put into the
+! arrays that are passed to the Input Processor "Get" (GetObjectItem) routines.
+! All alpha fields are limited to 100 characters.  Numeric fields should be
+! valid numerics (can include such as 1.0E+05) and are placed into double
+! precision variables.
+!
+! NOTE: Even though a field may be optional, a comma representing that field
+!   must be included (unless it is the last field in the object).  Since the
+!   entire input is "field-oriented" and not "keyword-oriented", the EnergyPlus
+!   Input Processor must have some representation (even if blank) for each
+!   field.
+!
+! Object Documentation
+! --------------------
+! In addition, the following special comments appear one per line and
+! most are followed by a value.  Comments may apply to a field or the object
+! or a group of objects.
+!
+! Field-level comments:
+!
+!  \field           Name of field
+!                     (should be succinct and readable, blanks are encouraged)
+!
+!  \note            Note describing the field and its valid values
+!
+!  \required-field  To flag fields which may not be left blank
+!                     (this comment has no "value")
+!
+!  \begin-extensible  Marks the first field at which the object accepts an extensible
+!                   field set.  A fixed number of fields from this marker define the
+!                   extensible field set, see the object code \extensible for
+!                   more information.
+!
+!  \units           Units (must be from EnergyPlus standard units list)
+!                   EnergyPlus units are standard SI units
+!
+!  \ip-units        IP-Units (for use by input processors with IP units)
+!                   This is only used if the default conversion is not
+!                   appropriate.
+!
+!  \unitsBasedOnField  For fields that may have multiple possible units, indicates
+!                   the field in the object that can be used to determine
+!                   the units. The field reference is in the A2 form.
+!
+!  \minimum         Minimum that includes the following value
+!
+!  \minimum>        Minimum that must be > than the following value
+!
+!  \maximum         Maximum that includes the following value
+!
+!  \maximum<        Maximum that must be < than the following value
+!
+!  \default         Default for the field (if N/A then omit entire line)
+!
+!  \deprecated      This field is not really used and will be deleted from the object.
+!                   The information is gotten internally within the program.
+!
+!  \autosizable     Flag to indicate that this field can be used with the Auto
+!                   Sizing routines to produce calculated results for the
+!                   field.  If a value follows this, then that will be used
+!                   when the "Autosize" feature is flagged.  To trigger
+!                   autosizing for a field, enter Autosize as the field's
+!                   value.  Only applicable to numeric fields.
+!
+! \autocalculatable Flag to indicate that this field can be automatically
+!                   calculated. To trigger auto calculation for a field, enter
+!                   Autocalculate as the field's value.  Only applicable to
+!                   numeric fields.
+!
+!  \type            Type of data for the field -
+!                     integer
+!                     real
+!                     alpha       (arbitrary string),
+!                     choice      (alpha with specific list of choices, see
+!                                 \key)
+!                     object-list (link to a list of objects defined elsewhere,
+!                                  see \object-list and \reference)
+!                     node        (name used in connecting HVAC components)
+!
+!  \retaincase      Retains the alphabetic case for alpha type fields
+!
+!  \key             Possible value for "\type choice" (blanks are significant)
+!                     use multiple \key lines to indicate all valid choices
+!
+!  \object-list     Name of a list of user-provided object names that are valid
+!                     entries for this field (used with "\reference")
+!                     see Zone and BuildingSurface:Detailed objects below for
+!                     examples.
+!                  ** Note that a field may have multiple \object-list commands.
+!
+!  \reference       Name of a list of names to which this object belongs
+!                     used with "\type object-list" and with "\object-list"
+!                     see Zone and BuildingSurface:Detailed objects below for
+!                     examples:
+!
+!                        Zone,
+!                          A1 , \field Name
+!                               \type alpha
+!                               \reference ZoneNames
+!
+!                        BuildingSurface:Detailed,
+!                          A4 , \field Zone Name
+!                               \note Zone the surface is a part of
+!                               \type object-list
+!                               \object-list ZoneNames
+!
+!             For each zone, the field "Name" may be referenced
+!             by other objects, such as BuildingSurface:Detailed, so it is
+!             commented with "\reference ZoneNames"
+!             Fields that reference a zone name, such as BuildingSurface:Detailed's
+!             "Zone Name", are commented as
+!             "\type object-list" and "\object-list ZoneNames"
+!             ** Note that a field may have multiple \reference commands.
+!             ** This is useful if the object belongs to a small specific
+!             object-list as well as a larger more general object-list.
+!
+! Object-level comments:
+!
+!  \memo            Memo describing the object
+!
+!  \unique-object   To flag objects which should appear only once in an idf
+!                     (this comment has no "value")
+!
+!  \required-object To flag objects which are required in every idf
+!                     (this comment has no "value")
+!
+!  \min-fields      Minimum number of fields that should be included in the
+!                   object.  If appropriate, the Input Processor will fill
+!                   any missing fields with defaults (for numeric fields).
+!                   It will also supply that number of fields to the "get"
+!                   routines using blanks for alpha fields (note -- blanks
+!                   may not be allowable for some alpha fields).
+!
+!  \obsolete        This object has been replaced though is kept (and is read)
+!                   in the current version.  Please refer to documentation as
+!                   to the dispersal of the object.  If this object is
+!                   encountered in an IDF, the InputProcessor will post an
+!                   appropriate message to the error file.
+!                   usage:  \obsolete New = >[New object name]
+!
+!  \extensible:<#>  This object is dynamically extensible -- meaning, if you
+!           change the IDD appropriately (if the object has a simple list
+!           structure -- just add items to the list arguments (i.e. BRANCH
+!           LIST). These will be automatically redimensioned and used during
+!           the simulation. <#> should be entered by the developer to signify
+!           how many of the last fields are needed to be extended (and EnergyPlus
+!           will attempt to auto-extend the object).  The first field of the first
+!           instance of the extensible field set is marked with \begin-extensible.
+!
+!  \begin-extensible See previous item, marks beginning of extensible fields in
+!                   an object.
+!
+!  \format          The object should have a special format when saved in
+!                   the IDF Editor with the special format option enabled.
+!                   The options include SingleLine, Vertices, CompactSchedule,
+!                   FluidProperties, ViewFactors, and Spectral.
+!                   The SingleLine option puts all the fields for the object
+!                   on a single line. The Vertices option is used in objects
+!                   that use X, Y and Z fields to format those three fields
+!                   on a single line.
+!                   The CompactSchedule formats that specific object.
+!                   The FluidProperty option formats long lists of fluid
+!                   properties to ten values per line.
+!                   The ViewFactor option formats three fields related to
+!                   view factors per line.
+!                   The Spectral option formats the four fields related to
+!                   window glass spectral data per line.
+!
+!   \reference-class-name Adds the name of the class to the reference list
+!                   similar to \reference.
+!
+! Group-level comments:
+!
+!  \group          Name for a group of related objects
+!
+!
+! Notes on comments
+! -----------------
+!
+! 1.  If a particular comment is not applicable (such as units, or default)
+! then simply omit the comment rather than indicating N/A.
+!
+! 2.  Memos and notes should be brief (recommend 5 lines or less per block).
+! More extensive explanations are expected to be in the user documentation
+!
+! Default IP conversions (no \ip-units necessary)
+!     m                      = >   ft                  3.281
+!     W                      = >   Btu/h               3.412
+!     m3/s                   = >   ft3/min             2118.6438
+!     C                      = >   F                   1.8 (plus 32)
+!     kg/J                   = >   lb/Btu              2325.83774250441
+!     Pa                     = >   psi                 0.0001450377
+!     W/m-K                  = >   Btu-in/h-ft2-F      6.93481276005548
+!     W/K                    = >   Btu/h-F             1.8987
+!     deltaC                 = >   deltaF              1.8
+!     m2                     = >   ft2                 10.764961
+!     K                      = >   R                   1.8
+!     1/K                    = >   1/R                 0.555555556
+!     (kg/s)/W               = >   (lbm/sec)/(Btu/hr)  0.646078115385742
+!     J/kg                   = >   Btu/lb              0.00042986 (plus 7.686)
+!     kg-H2O/kg-air          = >   lb-H2O/lb-air       1
+!     kJ/kg                  = >   Btu/lb              0.429925
+!     lux                    = >   foot-candles        0.092902267
+!     kg/m3                  = >   lb/ft3              0.062428
+!     kg/s                   = >   lb/s                2.2046
+!     kg/s-m                 = >   lb/s-ft             0.67194
+!     m3                     = >   ft3                 35.319837041
+!     m3                     = >   gal                 264.172
+!     W/m2-K                 = >   Btu/h-ft2-F         0.176110194261872
+!     1/m                    = >   1/ft                0.304785126485827
+!     J/kg-K                 = >   Btu/lb-F            0.000239005736137667
+!     J/m3-K                 = >   Btu/ft3-F           1.49237004739337E-05
+!     m/s                    = >   ft/min              196.86
+!     m/s                    = >   miles/hr            2.2369
+!     m2-K/W                 = >   ft2-F-hr/Btu        5.678263
+!     W/m2                   = >   Btu/h-ft2           0.316957210776545
+!     A/K                    = >   A/F                 0.555555555555556
+!     g/kg                   = >   grains/lb           7.00000
+!     g/m-s                  = >   lb/ft-s             0.000671968949659
+!     g/m-s-K                = >   lb/ft-s-F           0.000373574867724868
+!     J/K                    = >   Btu/F               0.000526917584820558
+!     J/kg-K2                = >   Btu/lb-F2           0.000132889924714692
+!     J/m3                   = >   Btu/ft3             2.68096514745308E-05
+!     kg/kg-K                = >   lb/lb-F             0.555555555555556
+!     kPa                    = >   psi                 0.145038
+!     kPa                    = >   inHg                0.29523
+!     m2/s                   = >   ft2/s               10.764961
+!     m3/kg                  = >   ft3/lb              16.018
+!     m3/m3                  = >   ft3/ft3             1
+!     N-s/m2                 = >   lbf-s/ft2           0.0208857913669065
+!     V/K                    = >   V/F                 0.555555555555556
+!     W/m-K2                 = >   Btu/h-F2-ft         0.321418310071648
+!     m3/s-m                 = >   ft3/min-ft          645.89
+!     J/m2-K                 = >   Btu/ft2-F           4.89224766847393E-05
+!     cycles/hr              = >   cycles/hr           1
+!     kg/kg                  = >   lb/lb               1
+!     J/J                    = >   Btu/Btu             1
+!     g/GJ                   = >   lb/MWh              0.00793664091373665
+!     L/GJ                   = >   gal/kWh             0.000951022349025202
+!     m3/GJ                  = >   ft3/MWh             127.13292
+!     m3/s-m2                = >   ft3/min-ft2         196.85
+!     m3/s-person            = >   ft3/min-person      2118.6438
+!     W/m2-K2                = >   Btu/h-ft2-F2        0.097826
+!     g/MJ                   = >   lb/MWh              7.93664091373665
+!     L/MJ                   = >   gal/kWh             0.951022349025202
+!     m3/MJ                  = >   ft3/kWh             127.13292
+!     W/W                    = >   Btuh/Btuh           1
+!     $/m2                   = >   $/ft2               0.0928939733269818
+!     $                      = >   $                   1
+!     $/kW                   = >   $/(kBtuh/h)         0.293083235638921
+!     $/m3                   = >   $/ft3               0.0283127014102352
+!     years                  = >   years               1
+!     $/(W/K)                = >   $/(Btu/h-F)         0.52667614683731
+!     $/(m3/s)               = >   $/(ft3/min)         0.000472000059660808
+!     W/m                    = >   Btu/h-ft            1.04072
+!     K/m                    = >   F/ft                0.54861322767449
+!     W/s                    = >   W/s                 1
+!     kmol                   = >   kmol                1
+!     J                      = >   Wh                  0.000277777777777778
+!     GJ                     = >   ton-hrs             78.9889415481832
+!     kg/m2                  = >   lb/ft2              0.204794053596664
+!     kg                     = >   lb                  2.2046
+!     percent/K              = >   percent/F           0.555555555555556
+!     kg/s2                  = >   lb/s2               2.2046
+!     g/mol                  = >   lb/mol              0.0022046
+!     deltaJ/kg              = >   deltaBtu/lb         0.0004299
+!     person/m2              = >   person/ft2          0.0928939733269818
+!     m2/person              = >   ft2/person          10.764961
+!     W/person               = >   Btu/h-person        3.412
+!     m3/person              = >   ft3/person          35.319837041
+!     m3/hr-person           = >   ft3/hr-person       35.319837041
+!     m3/m2                  = >   ft3/ft2             3.281
+!     m3/hr-m2               = >   ft3/hr-ft2          3.281
+!     m3/hr                  = >   ft3/hr              35.319837041
+!     s/m                    = >   s/ft                0.304785126485827
+!     m2/m                   = >   ft2/ft              3.281
+!     L/day                  = >   pint/day            2.11337629827348
+!     L/kWh                  = >   pint/kWh            2.11337629827348
+!     kg/Pa-s-m2             = >   lb/psi-s-ft2        1412.00523459398
+!     m/hr                   = >   ft/hr               3.281
+!     Mode                   = >   Mode                1
+!     Control                = >   Control             1
+!     Availability           = >   Availability        1
+!     rev/min                = >   rev/min             1
+!     W/(m3/s)               = >   W/(ft3/min)         0.0004719475
+!     VA                     = >   VA                  1
+!     N-m                    = >   lbf-in              8.85074900525547
+!     m3/s-W                 = >   ft3-h/min-Btu       621.099127332943
+!     cm2                    = >   inch2               0.15500031000062
+!     kg/m                   = >   lb/ft               0.67196893069637
+!     m/yr                   = >   inch/yr             39.37
+!
+! Other conversions supported (needs the \ip-units code)
+!
+!     m                      = >   in                  39.37
+!     W                      = >   W                   1
+!     m3/s                   = >   gal/min             15852
+!     m3/s                   = >   lbH2O/hr            7936289.998
+!     Pa                     = >   inHg                0.00029613
+!     Pa                     = >   inH2O               0.00401463
+!     Pa                     = >   ftH2O               0.00033455
+!     W/person               = >   W/person            1
+!     W/m2                   = >   W/m2                1
+!     W/m2                   = >   W/ft2               0.0928939733269818
+!     W/m-K                  = >   Btu/h-ft-F          0.577796066000163
+!
+! Units fields that are not translated
+!     deg
+!     hr
+!     A
+!     dimensionless
+!     V
+!     ohms
+!     A/V
+!     eV
+!     percent
+!     s
+!     W/m2 or deg C
+!     W/m2, W or deg C
+!     minutes
+!     1/hr
+! **************************************************************************
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/creating-input-files/idfeditor.tex b/doc/auxiliary-programs/src/creating-input-files/idfeditor.tex
new file mode 100644
index 00000000000..463d594b0b8
--- /dev/null
+++ b/doc/auxiliary-programs/src/creating-input-files/idfeditor.tex
@@ -0,0 +1,190 @@
+\section{IDFEditor}\label{idfeditor}
+
+IDF Editor is an optional component of the EnergyPlus installation. For users who want a simple way of creating or editing EnergyPlus input data files (IDF), IDF Editor provides this service. The IDF Editor does not check inputs for validity, although some numeric fields are highlighted if out of range and some text fields are highlighted if they contain an invalid reference. For instructions and rules that must be followed when creating an IDF file the user should refer to the \href{../../EnergyPlusFromStarTeam/EnergyPlusFromStarTeam/Documentation/sources/InputOutputReference.pdf}{\emph{Input/Output Reference}} document.
+
+\begin{figure}[hbtp] % fig 49
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image115.png}
+\caption{IDF Editor Screen. \protect \label{fig:idf-editor-screen.}}
+\end{figure}
+
+\subsection{Start IDF Editor}\label{start-idf-editor}
+
+IDF Editor should be located in the EnergyPlus\textbackslash{}PreProcessor\textbackslash{}IDFEditor directory where you installed EnergyPlus. By double clicking on the IDF Editor icon you will get a screen similar to the one shown above. IDF Editor works in conjunction with the current EnergyPlus Input Data Directory (IDD) file that resides in the directory where EnergyPlus is installed. Another way to start the IDF Editor is from EP-Launch. Multiple IDF files can be opened at once.
+
+\subsection{Creating or Selecting an Input Data File}\label{creating-or-selecting-an-input-data-file}
+
+Creating a new input data file or selecting an existing input data file can be accomplished either through use of the File menu on the menu bar at the top of the screen or through use of the New File icon button or Open File icon button on the tool bar.
+
+\subsection{Class List and Objects}\label{class-list-and-objects}
+
+The classes that can be used to make up an IDF file have been organized into groups as shown in the `Class List' portion of the screen. A class is made up of a group of objects. Select a class from the list by clicking on and highlighting the class. The field to the left of the selected class in the `Class List' will either contain {[}------{]} to indicate that this class has no objects in the IDF file or it will contain a number like {[}0003{]} to indicate the number of times the object currently appears in the IDF file. For example, for the BuildingSurface:Detailed class selected in the screen above under the Thermal Zone Description/Geometry group, there are 40 objects in the IDF file. The details for these 40 objects or any new object that is defined are displayed in columns within the grid. Each object is made up of fields and can be used to further define the object. Any units attached to each field are shown in the second column. You may need to scroll down the `field' list or maximize the application to see all of the fields. Likewise, you may need to scroll to the right of the main grid to see other objects.
+
+Options under the view menu can change how you use the Class List. To display only classes that contain objects select the ``show classes with objects only'' option on the ``View'' menu. You can also toggle this feature on and off with CTRL+L. If the file is empty and has no objects, this toggle does not impact the display.
+
+The ``Show Quick Select Dropdowns'' view menu option adds two new input fields to the main screen. The input fields can be used to go quickly to different classes in the main list of classes. By typing in the top input field, the group that starts with those letters are displayed. After selecting one and pressing the tab button, classes in that group are shown and by typing the first few letters, you can easily select a specific class. Pressing tab again displays that class and it objects. This method allows for quick selection of classes if you remember the group name and class name.
+
+\subsection{Changing Values}\label{changing-values}
+
+By clicking and highlighting a value within an object, several things happen:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Any user comments from the IDF file will be displayed in the `Comments from IDF' portion of the screen
+\item
+  Any notes contained in the IDD for this input field will be displayed in the `Explanation of Keyword' portion of the screen
+\item
+  The value can be edited. Depending on the field, a drop down list may display the default value, maximum and minimum, or other keywords that can be used with the field.
+\item
+  Numeric fields that can be autosized will include ``autosize'' as a selection in the drop down list.
+\item
+  Some numeric fields have a maximum and/or minimum value specified in the IDD. If the value entered is outside this range, the cell will be highlighted in pale orange.
+\item
+  For values that are names of nodes, a new dialog box titled ``Edit or Select Node Name'' can be shown when the small button is pressed that is on the right side in each node name cell as described in the next section.
+\end{enumerate}
+
+\subsection{Edit or Select Node Names Dialog}\label{edit-or-select-node-names-dialog}
+
+The following dialog box is displayed when the small button is pressed that is on the right side of cells used for node names. Double clicking on cells containing node names can also make the dialog box appear.
+
+\begin{figure}[hbtp] % fig 50
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image116.png}
+\caption{Edit or Select Node Name Dialog Box \protect \label{fig:edit-or-select-node-name-dialog-box}}
+\end{figure}
+
+To enter a new node name, type it in the ``Node Name'' field near the top of the dialog. To select a name of a node that is already being used in the file, choose a node name from the list shown on the left of the dialog box and labeled ``Other Node Names.'' When a node name is selected from the list on the left side of the dialog box, the box near the bottom left shown as ``Where Selected Other Node Name Appears in File'' will display the name of the class, name of the object and name of the field for each other location in the file that node name is currently be used.
+
+The Other Node Names list on the left side of the dialog box may contain a very long list of node names depending on the complexity of the HVAC system. To help with this, four options are available just above the list titled All, Recent, Containing, and Class or Field. The All option shows all node names used in the file while the other options are used to narrow the list down to only certain node names. The Recent option shows only node names that have recently been edited. The Containing option shows a list on the right side of the dialog box called ``Filter by Contents'' which shows all of the various words used as part of node names. These words can be selected and the Other Node Names list will only show node names that contain those words. By selecting words from this list, the list of Other Node Names can be shortened very quickly. The last option, Class or Field, shows a hierarchical list on the right side titled Filter by Object or Field containing the list of classes and fields that can have node names. By selecting an object or a field, the Other Node Names list on the right shows only node names that are present in the selected object or field. This is another way of quickly shortening the list of Other Node Names so that the appropriate node name can be selected.
+
+Finally, the Containing Text field just above the OK button can be typed in. Whatever you type limits the Other Node Names list to just those characters. The more typed, the shorter the list becomes. This is another method of quickly finding the node name used in other parts of the file. The Containing Text field is usually used with the All option but can be used with the other display options as well.
+
+\subsection{Working with Objects}\label{working-with-objects}
+
+To delete an object, first click on any value for the object and then click on the ``Del Obj'' button. To add a new object, click on the ``New Obj'' button and a new object column with fields set to blanks, zeros, or default values will be added to the far right of the grid. The ``Dup Obj'' button is similar to ``New Obj'', but copies the values of the fields of the currently selected object. Copying and pasting an object or groups of objects is also possible using the ``Copy Obj'' and ``Paste Obj'' buttons. These allow objects to be copied between files are also good for copying from files in the DataSets subdirectory. (Also see the Edit menu to perform these functions.)
+
+\subsection{File Menu}\label{file-menu-000}
+
+The File menu can be used for creating or selecting input files just like the buttons on the IDF Editor screen (see the \emph{Creating or Selecting an Input File} section above). In addition, the File menu is used to save a file or exit the IDF Editor. More than one file can be opened at a time.
+
+The ``File'', ``Save Options'' screen is shown below.
+
+\begin{figure}[hbtp] % fig 51
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image117.png}
+\caption{IDF Editor Save Options Screen. \protect \label{fig:idf-editor-save-options-screen.}}
+\end{figure}
+
+The save options allow the order of the objects in the file to be sorted by type of object or to keep the original order of the objects (for an existing file). The placement of new objects when the original order is specified can be either at the top or bottom of the file.
+
+In addition, the Save Options also allow certain objects to be written to the file using a specific format that some users prefer.
+
+The settings for the save options are kept for each file saved from the IDF Editor.
+
+The ``Set as Default'' option allows you to keep the save options intact for files that have not been saved yet with a version of IDF Editor that has this capability.
+
+The Help that is available from the Save Options screen is reproduced below:
+
+\begin{itemize}
+\item
+  The save options are related to the layout of the IDF file after it is saved. These options are not important if you never edit the IDF file with a text editor.
+\item
+  The sorted order of saving objects is the traditional way the IDF Editor sorts objects within files. Each type of object is presented in groups in the order they appear in the Energy+.IDD. The other options preserve the original order of the objects from the file but each object will be still be reformatted. By preserving the order, the objects are not rearranged so you can group them using a text editor and they will stay in that order. New objects are placed either near the top of the file or near the bottom of the file so that they can be easily found when using a text editor.
+\item
+  You can also choose to specially format some objects. This affects how individual fields in objects are arranged when saved. Selecting this option will format the following objects on a single line: Report, Report Meter, Report Variable, Version, Timestep in Hour, Inside Convection Algorithm, Outside Convection Algorithm, Solution Algorithm, Shadowing Calculations, Ground Reflectances, and GroundTemperatures:Deep. In addition, Schedule:Compact objects will be formatted to have two field for some lines. With this option, objects with geometric vertices are formatted to have the X, Y, and Z values on the same line. Those objects include: Surface:HeatTransfer, Surface:HeatTransfer:Sub, Surface:Shading:Detached:Fixed, Surface:Shading:Detached:Building and Surface:Shading:Attached.
+\item
+  These options are saved for each file. If a file has not been saved with IDF Editor yet, the default is used but if a file does not specify the default values for these can also be set by using the set as default option. The saved file keeps these options by using the !-option line with SortedOrder, OriginalOrderTop, OriginalOrderBottom, and UseSpecialFormat."
+\item
+  Full line comments which begin with ``!'' are preserved by IDF Editor and become associated with the object immediately followin the comment line(s).
+\item
+  Endline comments which begin with ``!'' are preserved by IDF Editor and are placed immediately before the object they are found in.
+\item
+  Endline comment which being with ``!-'' are automatic comments which IDF Editor will overwrite with the field name and units. User-provided text which follows ``!-'' will be lost. User comments should be added above the pertinent object using ``!'' to begin the line.
+\end{itemize}
+
+Also on the File menu is the Open DataSet menu and submenu. This allows you to open any input file that appears in the DataSet subdirectory and copy objects from them into another file. This is required because EnergyPlus does not read the DataSet files, it is up to you to include objects from them.
+
+\subsection{Edit Menu}\label{edit-menu-000}
+
+The Edit Menu offers options to create a new object, duplicate an object, and delete an object as well as finding and searching. The object options are the same operations as can be accomplished by using the `New Obj', `Dup Obj' and `Del Obj' buttons (see the \emph{Working with Objects} section above). In addition, the ``Next Row after Enter'' option can be toggled. When this option is on, the selection moves down one row after pressing Enter. The copy and paste object commands allow a single object to be copied within a file or between files. The pasted object appears as the last object in the class. This capability makes it easier to utilize the data in the DataSets directory.
+
+The Find Class menu item brings up the following dialog box used to search through the Class List:
+
+\begin{figure}[hbtp] % fig 52
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image118.png}
+\caption{Find Class Dialog Box \protect \label{fig:find-class-dialog-box}}
+\end{figure}
+
+The Find Class dialog can be used to find class names quickly and can be activated by the CTRL-F keyboard combination. The Find Previous Class (CTRL-T) and Find Next Class (CTRL-G) can continue the searching process for the next and previous times that the searched text is found in the Class List. If you find this option useful you may also want to try the Show Quick Select Dropdowns option under the View menu which also speeds up searching through the Class List.
+
+The Search and Replace menu item or CTRL-H activates the following dialog box:
+
+\begin{figure}[hbtp] % fig 53
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image119.png}
+\caption{Search and Replace Diaglog Box \protect \label{fig:search-and-replace-diaglog-box}}
+\end{figure}
+
+The Search and Replace dialog box can be used to find and change each instance of text being searched with some replacement text. The Search and Replace dialog is used to search and replace values of fields rather than classes like the Find Class dialog. To use the Search and Replace dialog, enter the text being searched in the Find What field and press the Find button. After the Find button is pressed, the list shows the places in the file that the text appears. For each time the text is found, the entire field value is shown followed by the class name, name of the object, and the name of the field in parentheses. Each item in the list can be selected using the check box to the left. The All and None buttons will select all or none of the items found. After the locations are selected that need to be replaced, you should enter the text in the Replace With field. When the Replace Selected button is pressed the value in each of locations that were checked will be replaced with the Replace with text.
+
+The dialog will usually open with the Find What field filled with the value of the currently selected cell. If the current cell has just been changed, the Find What and the Replace With fields will contain the before and after values of the change in the current cell. This makes it easy to change other instances in the file to be consistent with the changes just made. If renaming objects, the recommended approach is to rename the object and select the cell again and open the Search and Replace dialog. This will show other places in the file that use that object name that also may need to be changed.
+
+\subsection{View Menu}\label{view-menu-000}
+
+The View menu offers options for units and column widths. The Narrow/Medium/Wide Column options set the standard column width for items in the object grid. Individual columns can also be resized by dragging the column separator. The displayed value is rounded and/or expressed in scientific notation to fit within the column width.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  EnergyPlus input files are always in SI units. However, selecting ``Inch-Pound'' (IP) units in the View menu displays and edits values in IP units in the IDF editor. The IP unit will be displayed in the units column of the object grid. Some SI units convert to multiple IP units. For example, W becomes Btu/hr for heating and cooling capacity but remains as W for lighting and electrical equipment.
+\item
+  All conversion factors used in the IDF editor are documented in a block of comments near the top of the Energy+.IDD file.
+\item
+  Schedules, fluid properties and curves now support IP unit conversions. For curves, the minimum and maximum values are converted but the coefficients are not.
+\end{enumerate}
+
+To display only classes that contain objects select the ``show classes with objects only'' option on the ``View'' menu. You can also toggle this feature on and off with CTRL+L. If the file is empty and has no objects, this toggle does not impact the display.
+
+The ``Show Quick Select Dropdowns'' option, which can also be turned on and off with CTRL-Q, displays two dropdown lists above the class list that can be quickly used to select classes. The first list displays the possible groups. Once those are selected, the second list contains only the classes within that group. This option may be used to quickly access classes while avoiding scrolling through the long class list. In addition these pull down menus may be used with the keyboard to select groups and class names based on the first few letters of the names.
+
+The figure below shows the ``Layout Options'' also accessible under the View menu.
+
+\begin{figure}[hbtp] % fig 54
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image120.png}
+\caption{IDF Editor Layout Options Screen. \protect \label{fig:idf-editor-layout-options-screen.}}
+\end{figure}
+
+This option allows for different arrangements of the layout for the main screen of the IDF Editor. Select one of the four layouts available.
+
+The ``Show Quick Select Dropdowns'' view menu option adds two new input fields to the main screen. The input fields can be used to go quickly to different classes in the main list of classes.
+
+The ``Validity Check'' function has replaced and expanded upon the old ``Check Out-of-Range'' function. It can also be started by using CTRL-R. The ``Validity Check'' function performs three kinds of validity checks and displays the results as shown in the dialog box below:
+
+\begin{figure}[hbtp] % fig 55
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image121.png}
+\caption{Validity Check Dialog Box \protect \label{fig:validity-check-dialog-box}}
+\end{figure}
+
+The list displays the values and locations for objects with values that are either above the maximum or below the minimum values. This allows you to check your input for out-of-range values prior to running EnergyPlus. It also displays fields that contain invalid references. An invalid reference is when a name is used that should be the name of object but no object exists that uses that name. For example, if a Construction object references a layer named IN20 but no Material (or Material:NoMass, etc.) object is named IN20. When viewing the class that contains invalid references, those references are shown with a different background color similar to numbers that are out of range. The ``Validity Check'' dialog also shows when an entry for a field is not one of the possible lists of choices. The Goto button allows you to jump directly to the selected identified problems. The Perform Validity Check When Saving File can be turned on and off and automatically performs the check whenever the file is saved.
+
+\subsection{Help Menu}\label{help-menu-000}
+
+The Help menu offers options to open the EnergyPlus documentation files.
+
+\subsection{Caveats}\label{caveats-000}
+
+Remember to save any changes made before you create or edit another input file.
+
+No ``Run EnergyPlus'' button is available. Save your IDF file and use EP-Launch to execute an EnergyPlus run.
+
+You cannot edit comments in the `Comments from IDF' section of the screen.
+
+The use of point ``.'' or comma ``,'' as the decimal symbol is controlled by the windows system settings. This setting is found in the Control Panel, Regional Options, Number tab, Decimal Symbol field. IDF Editor will use the current decimal symbol to signify the start of the fractional portion of the number and will ignore other symbols. The idf file is always written using point ``.'' as the decimal symbol.
+
+\subsection{Bugs}\label{bugs-000}
+
+Please report any bugs to the helpdesk (email to energyplus-support@gard.com) so that we can fix them prior to the next release.
diff --git a/doc/auxiliary-programs/src/csvproc.tex b/doc/auxiliary-programs/src/csvproc.tex
new file mode 100644
index 00000000000..b277061050a
--- /dev/null
+++ b/doc/auxiliary-programs/src/csvproc.tex
@@ -0,0 +1,104 @@
+\chapter{CSVproc}\label{csvproc}
+
+This simple post processing utility may be useful when doing parametric analyses. It takes a CSV (comma separated values file) and performs some simple statistics. It is a very small application with no interface. It is typically executed from the command line.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Open a DOS command prompt window (Start à Programs à Accessories à Command Prompt)
+\item
+  Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
+\end{enumerate}
+
+C:
+
+CD \textbackslash{}\textless{}root folder\textgreater{}\textless{}/span\textgreater{}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Change to the specific folder for the coefficient conversion applications:
+\end{enumerate}
+
+CD PostProcess
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Run the program:
+\end{enumerate}
+
+CSVproc \textless{}filename\textgreater{}
+
+Where \textless{}filename\textgreater{} is the name of a CSV file, including extension. There is a simple readme.txt file in the folder. The program performs some simple statistics on each column and creates a new file with the same name without extension and -PROC.CSV added to the name.
+
+The statistics performed on each column are:
+
+\begin{itemize}
+\item
+  SUM
+\item
+  MAX
+\item
+  MIN
+\item
+  AVERAGE
+\item
+  COUNT
+\item
+  COUNTIF \textgreater{} 0
+\item
+  COUNTIF \textgreater{} 5
+\item
+  COUNTIF \textgreater{} 10
+\item
+  COUNTIF \textgreater{} 15
+\item
+  COUNTIF \textgreater{} 20
+\item
+  COUNTIF \textgreater{} 25
+\item
+  COUNTIF \textgreater{} 30
+\item
+  COUNTIF \textgreater{} 35
+\item
+  COUNTIF \textgreater{} 40
+\item
+  COUNTIF \textgreater{} 45
+\item
+  COUNTIF \textgreater{} 50
+\item
+  COUNTIF \textgreater{} 55
+\item
+  COUNTIF \textgreater{} 60
+\item
+  COUNTIF \textgreater{} 65
+\item
+  COUNTIF \textgreater{} 70
+\item
+  COUNTIF \textgreater{} 75
+\item
+  COUNTIF \textgreater{} 80
+\item
+  COUNTIF \textgreater{} 85
+\item
+  COUNTIF \textgreater{} 90
+\item
+  COUNTIF \textgreater{} 95
+\item
+  COUNTIF \textgreater{} 100
+\item
+  COUNTIF = 1
+\item
+  COUNTIF \textless{} 19.9
+\item
+  COUNTIF \textgreater{} 24.0
+\end{itemize}
+
+Obviously, not all statistics are relevant for every output report variable. The average is based on the sum divided by the number of non-blank rows. The average is not based on the length of time for that timestep. Due to this, CSVproc is best suited for an hourly output file.
+
+Source code is available upon request from jglazer@gard.com.
diff --git a/doc/auxiliary-programs/src/doe2translator.tex b/doc/auxiliary-programs/src/doe2translator.tex
new file mode 100644
index 00000000000..7de9d6f5422
--- /dev/null
+++ b/doc/auxiliary-programs/src/doe2translator.tex
@@ -0,0 +1,61 @@
+\chapter{DOE2Translator}\label{doe2translator}
+
+The DOE2Translator program creates an EnergyPlus input file from a DOE-2.1E input file. The translation is not intended to be complete but simply an aid to help you move your library of DOE-2.1E input files into EnergyPlus. You should look over the resulting EnergyPlus input file, review the documentation of EnergyPlus, and make any necessary edits to the translated file. Documentation is included here though the BLAST Translator is no longer included with the EnergyPlus Installation - it is available as a special download for those who need it.
+
+To use the DOE2Translator program, at the DOS prompt (or the command prompt for Windows NT/2000 systems), go to the directory that the DOE2Translator is located. That directory is likely to be:
+
+c:\textbackslash{}EnergyPlus\textbackslash{}PreProcess\textbackslash{}DOE2Translator
+
+In this directory there should be several files:
+
+DOE2Translator.exe - the program
+
+D2E\_macr.txt - a support file that contains the header of the translated file
+
+D2comkey.dat - a support file that contains a list of DOE-2 keywords
+
+Samp4n.inp - sample DOE-2.1E input file
+
+Samp4n.imf - the EnergyPlus macro input file resulting from the sample
+
+To use the DOE2Translator simply type
+
+DOE2Translator \textless{}file\textgreater{}
+
+Where you substitute the file you want to translate for \textless{}file\textgreater{} without a file extension. The ``.inp'' file extension is assumed. For example, if you want to translate one of the sample DOE-2.1E input files you would type:
+
+DOE2Translator samp1b
+
+The \textless{}file\textgreater{} can also have a full path, but it should not have an extension. If you have spaces in your path name, enclose the whole thing in ``.
+
+Several files get created when you run the DOE2Translator program. In the same directory as the DOE-2.1E input file, a new file with the same name and the file extension of ``.imf'' contains the EnergyPlus translation.
+
+This is an EnergyPlus macro file and the macro processor EPMacro needs to be used. The DOE2Tranlator uses many macros so using EPMacro is essensial. EP-Launch automatically runs EP-Macro when an ``.imf'' file is selected. In the translated file, comments shown with a tilde ``\textasciitilde{}'' are messages from the DOE2Translator program that may be helpful in understanding the limits of the translation.
+
+The D2EP.log file contains a detailed log of the translation process. The D2E\_TEMP.txt file contains an intermediate version of the log file. Both of these files are created in the same directory as the DOE2Translator program and can usually be deleted.
+
+Since DOE-2.1e and EnergyPlus share a common macro language, many macro features are passed to the EnergyPlus file unchanged, including \#\#set1, \#\#if, \#\#def and other macro commands. References to macro variables (i.e., ``var{[}{]}'') and expressions (i.e., " \#{[}x{[}{]} + 1{]}``) are usually passed through to the resulting EneryPlus IMF unless the DOE2Translator needs to understand that field during the translation process. The DOE2Translator does not evaluate macro expressions and if it needs to understand a field value and a macro is present instead will use a default value for the field instead. Most fields do not need to be understood by the translator and are directly passed through to the IMF file unchanged.
+
+Files that are included with the \#\#include are not translated automatically and would each need to be run through the DOE2Translator. If the included file does not have the INP extension it would need to be changed prior to the translation. In addition, the user would need to edit the \#\#include commands to use the IMF extension instead of the INP extension.
+
+In this version of the DOE2Translator program, translation is limited to the following DOE-2 commands, which represent the majority of the building envelope and internal gains:
+
+\begin{lstlisting}
+    SPACE (except SHAPE = BOX)
+    SPACE-CONDITIONS
+    DAY-SCHEDULE (except use of HOURS and VALUES keywords)
+    WEEK-SCHEDULE (except use of DAYS and DAY-SCHEDULE keywords)
+    SCHEDULE (except use of WEEK-SCHEDULE keyword)
+    MATERIAL
+    LAYERS
+    CONSTRUCTION
+    EXTERIOR-WALL, ROOF (except polygon)
+    INTERIOR-WALL
+    FIXED-SHADE
+    WINDOW
+    DOOR
+    RUN-PERIOD
+    DESIGN-DAY
+    LIKE
+    SET-DEFAULT
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/epdrawgui.tex b/doc/auxiliary-programs/src/epdrawgui.tex
new file mode 100644
index 00000000000..3a81f4d6a4a
--- /dev/null
+++ b/doc/auxiliary-programs/src/epdrawgui.tex
@@ -0,0 +1,11 @@
+\chapter{EPDrawGUI}\label{epdrawgui}
+
+The EPDrawGUI program is a simple utility that can be used to generate a dxf file from an input file without running EnergyPlus. It is a simple cross platform application is stored in the Preprocess subfolder of the EnergyPlus folder upon installation. A companion DLL (EPlusDrw.dll) is also needed in the same folder. And its library folders are required in a subfolder (EPDrawGUI Libs).
+
+\begin{figure}[hbtp] % fig 30
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image028.png}
+\caption{EPDrawGUI Main Screen \protect \label{fig:epdrawgui-main-screen}}
+\end{figure}
+
+Help is offered on the Main Tab and on the Options Tab when you place the mouse, without clicking, over the buttons, check boxes, and option boxes. In addition, the program copyright information is displayed when the mouse is over the Version number text in the lower left corner.
diff --git a/doc/auxiliary-programs/src/epdrawgui/main-tab.tex b/doc/auxiliary-programs/src/epdrawgui/main-tab.tex
new file mode 100644
index 00000000000..9f65938398e
--- /dev/null
+++ b/doc/auxiliary-programs/src/epdrawgui/main-tab.tex
@@ -0,0 +1,9 @@
+\section{Main Tab}\label{main-tab}
+
+The Main Tab, shown in Figure~\ref{fig:epdrawgui-main-screen}, contains the ``Create DXF from IDF'' button which is the button to use to create a DXF file from an IDF file, the main function of the EPDrawGUI program. This is the primary button that you will need to use. When pressed, you select an IDF file that you want to use as the basis for a drawing. If the ``Show DXF File After Created'' check box is check, when the ``Create DXF from IDF'' button is pressed, the drawing will be viewed immediately after the DXF file is created. Normally, the viewer for DXF files is automatically found but if the program cannot find a drawing viewer program, you can select one manually on the Options Tab.
+
+\begin{figure}[hbtp] % fig 31
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image029.png}
+\caption{EPDrawGUI Options Tab \protect \label{fig:epdrawgui-options-tab}}
+\end{figure}
diff --git a/doc/auxiliary-programs/src/epdrawgui/option-tab.tex b/doc/auxiliary-programs/src/epdrawgui/option-tab.tex
new file mode 100644
index 00000000000..03e79eeebef
--- /dev/null
+++ b/doc/auxiliary-programs/src/epdrawgui/option-tab.tex
@@ -0,0 +1,45 @@
+\section{Option Tab}\label{option-tab}
+
+The Option Tab, shown in Figure~\ref{fig:epdrawgui-options-tab}, contains an additional option to control some complex drawings as well as ways to select the DXF file viewer and view DXF files.
+
+The ``View DXF File'' button is used to select a previously created DXF file and view it with the DXF file viewer. The DXF viewer is usually found automatically but if this function does not work, you may want to select the DXF file viewer manually using the Select DXF Viewer button.
+
+The ``Select DXF Viewer'' button allows you to manually select the program used to display DXF files. Normally, it is not necessary to use this function since the DXF file viewer program is automatically detected but if the wrong file viewer is automatically detected or no file viewer is detected, this button can be used to select the viewer program.
+
+For IDF files that contain surfaces with more than four sides, the options under ``Polygons with 5+ Sides'' can affect the way the drawing is shown. Polygons with \textgreater{}4 sides do not display with the DXF 3DFACE command used for surfaces of 3 and 4 sides which subsequently will display very nicely as a ``solid'' in many DXF viewers.
+
+Thus there are four options which the user may choose to display \textgreater{}4 sided polygons.
+
+\begin{itemize}
+\tightlist
+\item
+  Attempt Triangulation
+\end{itemize}
+
+This option attempts simple triangulation for the polygon (\textgreater{}4 sides) surfaces. This triangulation will show in the wireframe views but will appear as a solid face in 3D views. This triangulation is only for drawing purposes and does not affect the simulations in any way. The triangle algorithm is not perfect and warnings do result when the software cannot triangulate a surface. If unable to triangulate simply, a warning error is generated to the .EPDerr file.
+
+\begin{itemize}
+\tightlist
+\item
+  Thick Polyline
+\end{itemize}
+
+With this option, the \textgreater{}4 sided polygon appears as a thicker line in all views of the building model. This option creates a `thick' line at the border of the polygon (\textgreater{}4 sides) surfaces. It will look like a hole in the drawing with a thicker edge. This thick border shows in wireframe as well as 3D views and can be confusing, due to overlap with other surfaces.
+
+\begin{itemize}
+\tightlist
+\item
+  Regular Polyline
+\end{itemize}
+
+With this option, the \textgreater{}4 sided polygon appears as a wire frame line in all views of the building model. This option creates a `regular' polyline for all polygon (\textgreater{}4 sides) surfaces. It will look like a hole in the drawing. Also, it will look the same in both wireframe and 3D views.
+
+\begin{itemize}
+\tightlist
+\item
+  Wireframe
+\end{itemize}
+
+This option creates a wireframe drawing (all lines) for all surfaces. All surfaces will appear as lines in both wireframe and 3D views.
+
+Note that the EPDrawGUI program only processes building and shading surfaces. It does not process daylighting reference points though the similar option in the EnergyPlus program (Report, Surfaces, DXF;) does show the daylighting reference points (but not illuminance map points) in the DXF view.
diff --git a/doc/auxiliary-programs/src/expandobjects.tex b/doc/auxiliary-programs/src/expandobjects.tex
new file mode 100644
index 00000000000..c737c90ebad
--- /dev/null
+++ b/doc/auxiliary-programs/src/expandobjects.tex
@@ -0,0 +1 @@
+\chapter{ExpandObjects}\label{expandobjects}
diff --git a/doc/auxiliary-programs/src/expandobjects/building-surface-objects-processed.tex b/doc/auxiliary-programs/src/expandobjects/building-surface-objects-processed.tex
new file mode 100644
index 00000000000..4eb16a2afce
--- /dev/null
+++ b/doc/auxiliary-programs/src/expandobjects/building-surface-objects-processed.tex
@@ -0,0 +1,16 @@
+\section{Building Surface Objects Processed}\label{building-surface-objects-processed}
+
+The building surface objects that are currently modified by the ExpandObjects preprocessor are:
+
+\begin{itemize}
+\item
+  BuildingSurface:Detailed
+\item
+  Wall:Detailed
+\item
+  RoofCeiling:Detailed
+\item
+  Floor:Detailed
+\item
+  Site:GroundTemperature:BuildingSurface
+\end{itemize}
diff --git a/doc/auxiliary-programs/src/expandobjects/ground-heat-transfer-objects-processed.tex b/doc/auxiliary-programs/src/expandobjects/ground-heat-transfer-objects-processed.tex
new file mode 100644
index 00000000000..602a6d480e3
--- /dev/null
+++ b/doc/auxiliary-programs/src/expandobjects/ground-heat-transfer-objects-processed.tex
@@ -0,0 +1,58 @@
+\section{Ground Heat Transfer Objects Processed}\label{ground-heat-transfer-objects-processed}
+
+The GroundHeatTransfer objects that are currently read by the ExpandObjects preprocessor are:
+
+\begin{itemize}
+\item
+  GroundHeatTransfer:Control
+\item
+  GroundHeatTransfer:Slab:Materials
+\item
+  GroundHeatTransfer:Slab:MatlProps
+\item
+  GroundHeatTransfer:Slab:BoundConds
+\item
+  GroundHeatTransfer:Slab:BldgProps
+\item
+  GroundHeatTransfer:Slab:Insulation
+\item
+  GroundHeatTransfer:Slab:EquivalentSlab
+\item
+  GroundHeatTransfer:Slab:AutoGrid
+\item
+  GroundHeatTransfer:Slab:ManualGrid
+\item
+  GroundHeatTransfer:Slab:XFACE
+\item
+  GroundHeatTransfer:Slab:YFACE
+\item
+  GroundHeatTransfer:Slab:ZFACE
+\item
+  GroundHeatTransfer:Basement:SimParameters
+\item
+  GroundHeatTransfer:Basement:MatlProps
+\item
+  GroundHeatTransfer:Basement:Insulation
+\item
+  GroundHeatTransfer:Basement:SurfaceProps
+\item
+  GroundHeatTransfer:Basement:BldgData
+\item
+  GroundHeatTransfer:Basement:Interior
+\item
+  GroundHeatTransfer:Basement:ComBldg
+\item
+  GroundHeatTransfer:Basement:EquivSlab
+\item
+  GroundHeatTransfer:Basement:EquivAutoGrid
+\item
+  GroundHeatTransfer:Basement:AutoGrid
+\item
+  GroundHeatTransfer:Basement:ManualGrid
+\item
+  GroundHeatTransfer:Basement:XFACE
+\item
+  GroundHeatTransfer:Basement:YFACE
+\item
+  GroundHeatTransfer:Basement:ZFACEHVACTemplate:Thermostat
+\end{itemize}
diff --git a/doc/auxiliary-programs/src/expandobjects/hvac-template-objects-processed.tex b/doc/auxiliary-programs/src/expandobjects/hvac-template-objects-processed.tex
new file mode 100644
index 00000000000..d7c90a0f0a0
--- /dev/null
+++ b/doc/auxiliary-programs/src/expandobjects/hvac-template-objects-processed.tex
@@ -0,0 +1,50 @@
+\section{HVAC Template Objects Processed}\label{hvac-template-objects-processed}
+
+The HVACTemplate objects that are currently read by the ExpandObjects preprocessor are:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:IdealLoadsAirSystem
+\item
+  HVACTemplate:Zone:FanCoil
+\item
+  HVACTemplate:Zone:PTAC
+\item
+  HVACTemplate:Zone:PTHP
+\item
+  HVACTemplate:Zone:Unitary
+\item
+  HVACTemplate:Zone:VAV
+\item
+  HVACTemplate:Zone:VAV:FanPowered
+\item
+  HVACTemplate:Zone:WatertoAirHeatPump
+\item
+  HVACTemplate:System:Unitary
+\item
+  HVACTemplate:System:UnitaryHeatPump:AirToAir
+\item
+  HVACTemplate:System:VAV
+\item
+  HVACTemplate:System:PackagedVAV
+\item
+  HVACTemplate:System:DedicatedOutdoorAir
+\item
+  HVACTemplate:Plant:ChilledWaterLoop
+\item
+  HVACTemplate:Plant:Chiller
+\item
+  HVACTemplate:Plant:Chiller:ObjectReference
+\item
+  HVACTemplate:Plant:Tower
+\item
+  HVACTemplate:Plant:Tower:ObjectReference
+\item
+  HVACTemplate:Plant:HotWaterLoop
+\item
+  HVACTemplate:Plant:Boiler
+\item
+  HVACTemplate:Plant:Boiler:ObjectReference
+\end{itemize}
diff --git a/doc/auxiliary-programs/src/expandobjects/introduction-003.tex b/doc/auxiliary-programs/src/expandobjects/introduction-003.tex
new file mode 100644
index 00000000000..dc6a95c32b7
--- /dev/null
+++ b/doc/auxiliary-programs/src/expandobjects/introduction-003.tex
@@ -0,0 +1,7 @@
+\section{Introduction}\label{introduction-001}
+
+The ExpandObjects program uses HVACTemplate objects in the IDF file to ``expand'' them into full fledged objects for EnergyPlus. Read more details of the systems and the individual fields in the HVACTemplate objects in the Input Output Reference document.
+
+ExpandObjects also processes GroundHeatTransfer objects, sends an input file to the Slab and Basement preprocessors, and replaces ground heat transfer boundary condition fields in building surface objects. Read more details of the ground heat transfer processing in the Input Output Reference.
+
+Technically speaking, the ExpandObjects program is a preprocessor that is currently used with the HVACTemplate objects. The preprocessor reads an \textbf{idf} file and generates an expanded.idf file (usually with the extension .\textbf{expidf}). The original idf file contains objects that will be read by the preprocessor and those that are ignored by the preprocessor. The objects read can be either commented out or left as is. The objects created by the preprocessor in the expanded.idf file should require no further preprocessing. The preprocessor does not read the EnergyPlus Data Dictionary file (Energy+.IDD) and does limited validation. Most of the object values that are created are ``passed'' through from input objects. This allows EnergyPlus to provide most of the validation. If errors are found, error messages are passed to the EnergyPlus program using the Output:Preprocessor object. These errors will be shown in the usual EnergyPlus error file. When used with EP-Launch, the expanded.idf file is renamed to the original file name with the extension \textbf{expidf}.
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus.tex
new file mode 100644
index 00000000000..e99dfbe365a
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus.tex
@@ -0,0 +1 @@
+\chapter{Ground Heat Transfer in EnergyPlus}\label{ground-heat-transfer-in-energyplus}
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/basement-program-output-files.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/basement-program-output-files.tex
new file mode 100644
index 00000000000..3d707a9fe13
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/basement-program-output-files.tex
@@ -0,0 +1,11 @@
+\section{Basement Program Output Files}\label{basement-program-output-files}
+
+The following output files are created by the Basement program and saved in the output file path specified in the RunBasement.bat file:
+
+*.audit - Audit file. Input errors are reported here as well as other information about the progress of the program..
+
+*.out - Summary of inputs, location data, and grid coordinates
+
+*.csv - Monthly temperatures and fluxes for each surface.
+
+*.idf - the EPObjects.txt file - ready to be included in an EnergyPlus input file (idf)
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/description-of-the-objects-in-the-basementght.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/description-of-the-objects-in-the-basementght.tex
new file mode 100644
index 00000000000..5208aed24bd
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/description-of-the-objects-in-the-basementght.tex
@@ -0,0 +1,418 @@
+\section{Description of the Objects in the BasementGHT.idd}\label{description-of-the-objects-in-the-basementght.idd}
+
+These objects also appear in the main Energy+.IDD file with the prefix ``GroundHeatTransfer:Basement:''
+
+\subsection{SimParameters or GroundHeatTransfer:Basement:SimParameters Object}\label{simparameters-or-groundheattransferbasementsimparameters-object}
+
+\subsubsection{Field: F: Multiplier for the ADI solution:}\label{field-f-multiplier-for-the-adi-solution}
+
+This field specifies an alternating direction iteration scheme multiplier. It should normally be set to 0.1. It can be increased if the soil conductivity is high.
+
+\subsubsection{Field: IYRS: Maximum number of yearly iterations:}\label{field-iyrs-maximum-number-of-yearly-iterations}
+
+This specifies the maximum number of years the simulation will be allowed to run. If convergence is reached, the simulation will not run this long. It can be used to stop simulation before quasi steady convergence state is reached.
+
+\subsection{MatlProps or GroundHeatTransfer:Basement:MatlProps Object}\label{matlprops-or-groundheattransferbasementmatlprops-object}
+
+\subsubsection{Field: NMAT: Number of materials in this domain}\label{field-nmat-number-of-materials-in-this-domain}
+
+This field specifies the number of materials whose properties are going to be specified. The order of the materials is not adjustable so six materials need to be specified. For the EnergyPlus basement application, only the foundation wall, floor slab, soil, and gravel are used.
+
+\subsubsection{Field: Density for Foundation Wall}\label{field-density-for-foundation-wall}
+
+This field is the density (kg/m3) of the foundation wall. Typical value is 2243.
+
+\subsubsection{Field: Density for Floor Slab}\label{field-density-for-floor-slab}
+
+This field is the density (kg/m3) of the floor slab. Typical value is 2243.
+
+\subsubsection{Field: Density for Ceiling}\label{field-density-for-ceiling}
+
+This field is the density (kg/m3) of the ceiling. Typical value is 311.
+
+\subsubsection{Field: Density for Soil}\label{field-density-for-soil}
+
+This field is the density (kg/m3) of soil. Typical value is 1500.
+
+\subsubsection{Field: Density for Gravel}\label{field-density-for-gravel}
+
+This field is the density (kg/m3) of gravel. Typical value is 2000.
+
+\subsubsection{Field: Density for Wood}\label{field-density-for-wood}
+
+This field is the density (kg/m3) of wood. Typical value is 449.
+
+\subsubsection{Field: Specific Heat for Foundation Wall}\label{field-specific-heat-for-foundation-wall}
+
+This field is the specific heat (J/kg-K) of the foundation wall. Typical value is 880.
+
+\subsubsection{Field: Specific Heat for Floor Slab}\label{field-specific-heat-for-floor-slab}
+
+This field is the specific heat (J/kg-K) of the floor slab. Typical value is 880.
+
+\subsubsection{Field: Specific Heat for Ceiling}\label{field-specific-heat-for-ceiling}
+
+This field is the specific heat (J/kg-K) of the ceiling. Typical value is 1530.
+
+\subsubsection{Field: Specific Heat for Soil}\label{field-specific-heat-for-soil}
+
+This field is the specific heat (J/kg-K) of soil. Typical value is 840.
+
+\subsubsection{Field: Specific Heat for Gravel}\label{field-specific-heat-for-gravel}
+
+This field is the specific heat (J/kg-K) of gravel. Typical value is 720.
+
+\subsubsection{Field: Specific Heat for Wood}\label{field-specific-heat-for-wood}
+
+This field is the specific heat (J/kg-K) of wood. Typical value is 1530.
+
+\subsubsection{Field: Thermal Conductivity for Foundation Wall}\label{field-thermal-conductivity-for-foundation-wall}
+
+This field is the thermal conductivity (W/m-K) of the foundation wall. Typical value is 1.4.
+
+\subsubsection{Field: Thermal Conductivity for Floor Slab}\label{field-thermal-conductivity-for-floor-slab}
+
+This field is the thermal conductivity (W/m-K) of the floor slab. Typical value is 1.4.
+
+\subsubsection{Field: Thermal Conductivity for Ceiling}\label{field-thermal-conductivity-for-ceiling}
+
+This field is the thermal conductivity (W/m-K) of the ceiling. Typical value is 0.09.
+
+\subsubsection{Field: Thermal Conductivity for Soil}\label{field-thermal-conductivity-for-soil}
+
+This field is the thermal conductivity (W/m-K) of soil. Typical value is 1.1.
+
+\subsubsection{Field: Thermal Conductivity for Gravel}\label{field-thermal-conductivity-for-gravel}
+
+This field is the thermal conductivity (W/m-K) of gravel. Typical value is 1.9.
+
+\subsubsection{Field: Thermal Conductivity for Wood}\label{field-thermal-conductivity-for-wood}
+
+This field is the thermal conductivity (W/m-K) of wood. Typical value is 0.12.
+
+\subsection{Insulation or GroundHeatTransfer:Basement:Insulation Object}\label{insulation-or-groundheattransferbasementinsulation-object}
+
+This object describes the insulation.
+
+\subsubsection{Field: REXT: R Value of any exterior insulation}\label{field-rext-r-value-of-any-exterior-insulation}
+
+This field is the R value (m2-K/W) of any exterior insulation.
+
+\subsubsection{Field: INSFULL: Flag: Is the wall fully insulated?}\label{field-insfull-flag-is-the-wall-fully-insulated}
+
+This field uses ``true'' for fully insulated walls and ``false'' for insulation half way down the side wall from the grade line.
+
+\subsection{SurfaceProps or GroundHeatTransfer:Basement:SurfaceProps Object}\label{surfaceprops-or-groundheattransferbasementsurfaceprops-object}
+
+The first six fields in this object specify the parameters used in the surface heat transfer boundary condition determination. They are specified for no snow and snow covered conditions.
+
+\subsubsection{Field: ALBEDO: Surface albedo for No snow conditions}\label{field-albedo-surface-albedo-for-no-snow-conditions}
+
+This field specifies the surface solar albedo for no snow conditions. Solar albedo is more commonly available than the solar absorptivity. The total solar energy absorbed by a horizontal surface is (1-albedo)*(Total solar). Typical value for this field is 0.16.
+
+\subsubsection{Field: ALBEDO: Surface albedo for snow conditions}\label{field-albedo-surface-albedo-for-snow-conditions}
+
+This field specifies the surface solar albedo for snow covered conditions. Solar albedo is more commonly available than the solar absorptivity. The total solar energy absorbed by a horizontal surface is (1-albedo)*(Total solar). Typical value for this field is 0.40.
+
+\subsubsection{Field: EPSLN: Surface emissivity No Snow}\label{field-epsln-surface-emissivity-no-snow}
+
+This field specifies the long wavelength or thermal radiation emissivity for the ground surface under no snow conditions. Typical value is 0.94.
+
+\subsubsection{Field: EPSLN: Surface emissivity with Snow}\label{field-epsln-surface-emissivity-with-snow}
+
+This field specifies the long wavelength or thermal radiation emissivity for the ground surface under snow covered conditions. Typical value is 0.86.
+
+\subsubsection{Field: VEGHT: Surface roughness No snow conditions}\label{field-veght-surface-roughness-no-snow-conditions}
+
+This field specifies the surface roughness or vegetation height (cm) that is used in determining the convective heat transfer coefficient on the surface under no snow conditions. Typical value is 6.0.
+
+\subsubsection{Field: VEGHT: Surface roughness snow conditions}\label{field-veght-surface-roughness-snow-conditions}
+
+This field specifies the surface roughness or vegetation height (cm) that is used in determining the convective heat transfer coefficient on the surface under snow covered conditions. Typical value is 0.25.
+
+\subsubsection{Field: PET: Flag, Potential evapotranspiration on?}\label{field-pet-flag-potential-evapotranspiration-on}
+
+This field is a flag that invokes the evapotranspiration calculation at the surface. This covers all forms of latent heat transfer from the surface. It normally should be included. The user enters ``true'' for ``yes'' and ``false'' for no.
+
+\subsection{BldgData or GroundHeatTransfer:Basement:BldgData Object}\label{bldgdata-or-groundheattransferbasementbldgdata-object}
+
+This object specifies the major configuration parameters for the basement. The 3-D grid used in the simulation has the capability of including a gravel ``fill'' around the basement. Thus several dimensions must be specified. All units are in meters.
+
+\subsubsection{Field: DWALL: Wall thickness}\label{field-dwall-wall-thickness}
+
+This field specifies the basement wall thickness (m). Typical value is 0.2.
+
+\subsubsection{Field: DSLAB: Floor Slab thickness}\label{field-dslab-floor-slab-thickness}
+
+This field specifies the thickness of the floor slab (m). Typical value is 0.25.
+
+\subsubsection{Field: DGRAVXY: Width of gravel pit beside basement wall}\label{field-dgravxy-width-of-gravel-pit-beside-basement-wall}
+
+This field specifies the width of the gravel ``fill'' bed beside the basement wall (m).
+
+\subsubsection{Field: DGRAVZN: Gravel depth extending above the floor slab}\label{field-dgravzn-gravel-depth-extending-above-the-floor-slab}
+
+This field specifies the depth of the gravel fill above the floor slab (m).
+
+\subsubsection{Field: DGRAVZP: Gravel depth below the floor slab}\label{field-dgravzp-gravel-depth-below-the-floor-slab}
+
+This field specifies the depth of the gravel fill below the floor slab (m).
+
+\subsection{Interior or GroundHeatTransfer:Basement:Interior Object}\label{interior-or-groundheattransferbasementinterior-object}
+
+This object provides the information needed to simulate the boundary conditions inside the basement.
+
+\subsubsection{Field: COND: Flag: Is the basement conditioned?}\label{field-cond-flag-is-the-basement-conditioned}
+
+This flag indicates that the basement temperature is controlled. For EnergyPlus runs, this should be TRUE.
+
+\subsubsection{Field: HIN: Downward convection only heat transfer coefficient}\label{field-hin-downward-convection-only-heat-transfer-coefficient}
+
+This field specifies the convection only heat transfer coefficient for floors (downward heat flux - W/m2-K).
+
+\subsubsection{Field: HIN: Upward convection only heat transfer coefficient}\label{field-hin-upward-convection-only-heat-transfer-coefficient}
+
+This field specifies the convection only heat transfer coefficient for floors (upward heat flux - W/m2-K).
+
+\subsubsection{Field: HIN: Horizontal convection only heat transfer coefficient}\label{field-hin-horizontal-convection-only-heat-transfer-coefficient}
+
+This field specifies the convection only heat transfer coefficient for walls (horizontal heat flux - W/m2-K).
+
+\subsubsection{Field: HIN: Downward combined (convection and radiation) heat transfer coefficient}\label{field-hin-downward-combined-convection-and-radiation-heat-transfer-coefficient}
+
+This field specifies the combined thermal radiation and convection heat transfer coefficient for floors (downward heat flux - W/m2-K).
+
+\subsubsection{Field: HIN: Upward combined (convection and radiation) heat transfer coefficient}\label{field-hin-upward-combined-convection-and-radiation-heat-transfer-coefficient}
+
+This field specifies the combined thermal radiation and convection heat transfer coefficient for floors (upward heat flux - W/m2-K).
+
+\subsubsection{Field: HIN: Horizontal combined (convection and radiation) heat transfer coefficient}\label{field-hin-horizontal-combined-convection-and-radiation-heat-transfer-coefficient}
+
+This field specifies the combined thermal radiation and convection heat transfer coefficient for walls (horizontal heat flux - W/m2-K).
+
+\subsection{ComBldg or GroundHeatTransfer:Basement:ComBldg Object}\label{combldg-or-groundheattransferbasementcombldg-object}
+
+This object specifies the 12 monthly average basement temperatures (air temperature). The last field allows a daily sine wave variation to be placed on the inside temperature. During testing, it was found that entering values for the daily sine wave amplitude had very little effect on the results.
+
+\subsubsection{Field: January average temperature}\label{field-january-average-temperature}
+
+This field is the average air temperature (C) for the basement for January.
+
+\subsubsection{Field: February average temperature}\label{field-february-average-temperature}
+
+This field is the average air temperature (C) for the basement for February.
+
+\subsubsection{Field: March average temperature}\label{field-march-average-temperature}
+
+This field is the average air temperature (C) for the basement for March.
+
+\subsubsection{Field: April average temperature}\label{field-april-average-temperature}
+
+This field is the average air temperature (C) for the basement for April.
+
+\subsubsection{Field: May average temperature}\label{field-may-average-temperature}
+
+This field is the average air temperature (C) for the basement for May.
+
+\subsubsection{Field: June average temperature}\label{field-june-average-temperature}
+
+This field is the average air temperature (C) for the basement for June.
+
+\subsubsection{Field: July average temperature}\label{field-july-average-temperature}
+
+This field is the average air temperature (C) for the basement for July.
+
+\subsubsection{Field: August average temperature}\label{field-august-average-temperature}
+
+This field is the average air temperature (C) for the basement for August.
+
+\subsubsection{Field: September average temperature}\label{field-september-average-temperature}
+
+This field is the average air temperature (C) for the basement for September.
+
+\subsubsection{Field: October average temperature}\label{field-october-average-temperature}
+
+This field is the average air temperature (C) for the basement for October.
+
+\subsubsection{Field: November average temperature}\label{field-november-average-temperature}
+
+This field is the average air temperature (C) for the basement for November.
+
+\subsubsection{Field: December average temperature}\label{field-december-average-temperature}
+
+This field is the average air temperature (C) for the basement for December.
+
+\subsubsection{Field: Daily variation sine wave amplitude}\label{field-daily-variation-sine-wave-amplitude}
+
+This field is the amplitude (variation) for a daily sine wave variation to be placed on the inside temperature. This has been shown to have little effect on results so zero can be used safely.
+
+\subsection{EquivSlab or GroundHeatTransfer:Basement:EquivSlab Object}\label{equivslab-or-groundheattransferbasementequivslab-object}
+
+This object provides the information needed to do the simulation as an equivalent square geometry by utilizing the area to perimeter ratio. This procedure was shown to be accurate by Cogil (1998).
+
+\subsubsection{Field: APRatio: The area to perimeter ratio for this slab}\label{field-apratio-the-area-to-perimeter-ratio-for-this-slab}
+
+This field specifies the Area to Perimeter (A/P) ratio for the slab.
+
+\subsubsection{Field: EquivSizing: Flag}\label{field-equivsizing-flag}
+
+This field should always be TRUE unless the user wants to specifically look at the differences between the long wall and the short wall on a rectangular configuration.
+
+\subsection{EquivAutoGrid or GroundHeatTransfer:Basement:EquivAutoGrid Object}\label{equivautogrid-or-groundheattransferbasementequivautogrid-object}
+
+This is a necessary object when the EquivSizing Flag in the EquivSlab object is TRUE. This object provides the information needed to set up the three dimensional conduction grid surrounding the basement.
+
+\subsubsection{Field: CLEARANCE: Distance from outside of wall to edge of 3-D ground domain}\label{field-clearance-distance-from-outside-of-wall-to-edge-of-3-d-ground-domain}
+
+This field specifies the distance to the outside of the field from the basement wall. It has been determined that 15 meters is quite satisfactory.
+
+\subsubsection{Field: SlabDepth: Thickness of the floor slab}\label{field-slabdepth-thickness-of-the-floor-slab}
+
+This field specifies the thickness of the slab in meters. Note that the slab top surface is level with the ground surface, so this is the depth into the ground. The slab depth has a significant effect on the temperature calculation, and it is also important for the auto-grid process. The finite difference grids are set in such a way that they use the slab thickness to determine the vertical grid spacing. Because of this, autogridding will fail if the slab thickness is specified larger than 0.25 meters. The program also is set up so that the slab is a single finite difference cell in the vertical direction. Thus, if the slab thickness is set too large, the accuracy of the calculation may be suspect. Typical value is 0.1.
+
+\subsubsection{Field: BaseDepth: Depth of the basement wall below grade}\label{field-basedepth-depth-of-the-basement-wall-below-grade}
+
+This field specifies the depth of the basement wall below grade level (m). This is the height of the wall above the footing.
+
+Field N2 specifies the height of the basement wall above the grade level. This should be zero for EnergyPlus runs since if an above grade segment is to be simulated, it should be done with EnergyPlus not with the basement program.
+
+Field N3 specifies the floor slab thickness.
+
+Field N4 specifies the depth of the basement wall below grade level. This is the height of the wall above the footing.
+
+\subsection{Sample idf File - Basement}\label{sample-idf-file---basement}
+
+\begin{lstlisting}
+
+! Minneapolis Test Cases
+  SimParameters,
+  0.1,     ! [F: Multiplier for the ADI solution: 0<F<1.0,
+  !         typically 0.1 (0.5 for high k
+  1;       ! [IYRS: Maximum number of iterations: typically 25-30
+
+  MatlProps,
+  6, ! [NMAT: Number of materials in this domain, UP TO 6]
+  2242.6, 2242.6, 311.66, 1500.0, 2000.0, 448.5,! [RHO(1-6): Matl density
+  !(Fndn wall, Floor Slab, Ceiling,Soil, Gravel, Wood), kg/m3, ]
+  880.0, 880.0, 1513.0, 840.0, 720.0, 1630.0,!       [CP(1-6): Specific Heat: J/kg-K,
+  1.402, 1.402, 0.093, 0.5, 1.9, 0.119;  !       [TCON(1-6): Conductivity: W/m-K
+
+  Insulation,
+  5.0, ! [REXT: R Value of any exterior insulation, K/(W/m2)]
+  TRUE; ! [INSFULL: Flag: Is the wall fully insulated? TRUE/FALSE]
+
+  SurfaceProps,
+  .16, .40, ! [ALBEDO: Surface albedo array, .16 .40]
+  .94, .86, ! [EPSLN: Surface emissivity No Snow/ Snow .94 .86]
+  6.0, 0.25, ! [VEGHT: Surface roughness NS/S, cm, 6.0, 0.25]
+  TRUE;! [PET: Flag, Potential evapotranspiration on? T/F]
+  !                Typically, PET is True
+
+  BldgData,
+  .2, ! [DWALL: Wall thickness, m, .2]
+  .1, ! [DSLAB: Floor slab thickness, m, 0.1]
+  .3, ! [DGRAVXY: Width of gravel pit beside footing, m, 0.3]
+  .2, ! [DGRAVZN: Gravel depth above the floor slab, m, 0.2]
+  .1;! [DGRAVZP: Gravel depth below the floor slab, m, 0.1]
+
+  Interior,
+  TRUE, ! [COND: Flag: Is the basement conditioned? TRUE/FALSE]
+  ! [HIN: Indoor convective heat transfer coefficients, W/m2-K
+  !       Convection Only: 1)Q Downward 2)Q Upward 3)Q Horizontal
+  !       Conv and Radiation: 4)Q Downward 5)Q Upward 6)Q Horizontal]
+  0.92, !Q Downward Convection Only
+  4.04,!Q Upward Convection Only
+  3.08,!Q HorizontalConvection Only
+  6.13, !Q Downward Conv and Radiation
+  9.26, !Q Upward Conv and Radiation
+  8.29;!Q Horizontal Conv and Radiation
+
+  EquivSlab,
+  15.0, ! [APRatio: The area to perimeter ratio for this slab: m]
+  TRUE;! [EquivSizing: Flag: Will the dimensions of an equivalent
+  !             slab be calculated (TRUE) or will the dimensions be
+  !              input directly? (FALSE)]
+  !             Only advanced special simulations should use FALSE.
+
+  EquivAutoGrid,   ! NOTE: EquivAutoGrid necessary when EquivSizing = TRUE
+  !                This is the normal case.
+  ! If the modelled building is not a rectangle or square, Equivalent
+  ! sizing MUST be used to get accurate results
+  15, ! [CLEARANCE: Distance from outside of wall to edge, 15m]
+  .1,  ! [SlabDepth: Thickness of the floor slab, m, 0.1]
+  2.4; ! [BaseDepth: Depth of the basement wall below grade, m]
+
+  ComBldg, !  Commercial building
+  20.,  !  Jan Ave basement temp
+  20.,  !  Feb Ave basement temp
+  20.,  !  Mar Ave basement temp
+  20.,  !  Apr Ave basement temp
+  20.,  !  May Ave basement temp
+  20.,  !  Jun Ave basement temp
+  20.,  !  Jul Ave basement temp
+  20.,  !  Aug Ave basement temp
+  20.,  !  Sep Ave basement temp
+  20.,  !  Oct Ave basement temp
+  20.,  !  Nov Ave basement temp
+  20.,  !  Dec Ave basement temp
+  0.0;  !  Daily variation Sine Wave amplitude
+\end{lstlisting}
+
+\subsection{Additional Objects}\label{additional-objects}
+
+There are five additional objects in the IDD that can be used under very special situations by researchers who want to generate special calculation grids. They are normally not useful to EnergyPlus users. They will be shown as IDD sections only. They do not need to be in the IDF.
+
+\begin{lstlisting}
+AutoGrid,
+\memo AutoGrid only necessary when EquivSizing is false
+\memo If the modelled building is not a rectangle or square, Equivalent
+\memo sizing MUST be used to get accurate results
+       N1, \field CLEARANCE: Distance from outside of wall to edge, 15m]
+       N2, \field SLABX: X dimension of the building slab, 0-60.0 m]
+       N3, \field SLABY: Y dimension of the building slab, 0-60.0 m]
+       N4, \field ConcAGHeight: Height of the fndn wall above grade, m]
+       N5, \field SlabDepth: Thickness of the floor slab, m, 0.1]
+       N6; \field BaseDepth: Depth of the basement wall below grade, m]
+\end{lstlisting}
+
+\begin{lstlisting}
+ManualGrid,
+\memo Manual Grid only necessary using manual gridding (not recommended)
+       N1, \field NX: Number of cells in the X direction: 20]
+       N2, \field NY: Number of cells in the Y direction: 20]
+       N3, \field NZAG: Number of cells in the Z direction. above grade: 4 Always]
+       N4, \field NZBG: Number of cells in Z direction. below grade: 10-35]
+       N5, \field IBASE: X direction cell indicator of slab edge: 5-20]
+       N6, \field JBASE: Y direction cell indicator of slab edge: 5-20]
+       N7; \field KBASE: Z direction cell indicator of the top of the floor slab: 5-20]
+\end{lstlisting}
+
+\begin{lstlisting}
+XFACE,
+\memo This is only needed when using manual gridding (not recommended)
+\memo XFACE: X Direction cell face coordinates: m
+       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
+       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
+       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
+       N39, N40, N41, N42, N43, N44;
+\end{lstlisting}
+
+\begin{lstlisting}
+YFACE,
+\memo This is only needed when using manual gridding (not recommended)
+\memo YFACE: Y Direction cell face coordinates: m
+       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
+       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
+       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
+       N39, N40, N41, N42, N43, N44;
+\end{lstlisting}
+
+\begin{lstlisting}
+ZFACE,
+\memo This is only needed when using manual gridding (not recommended)
+\memo ZFACE: Z Direction cell face coordinates: m
+       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
+       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
+       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
+       N39, N40;
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/description-of-the-objects-in-the-e-slabght.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/description-of-the-objects-in-the-e-slabght.tex
new file mode 100644
index 00000000000..7d943c9a433
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/description-of-the-objects-in-the-e-slabght.tex
@@ -0,0 +1,524 @@
+\section{Description of the Objects in the E+SlabGHT.IDD}\label{description-of-the-objects-in-the-eslabght.idd}
+
+These objects also appear in the main Energy+.IDD file with the prefix ``GroundHeatTransfer:Slab:''
+
+\subsection{Materials or GroundHeatTransfer:Slab:Materials Object}\label{materials-or-groundheattransferslabmaterials-object}
+
+The materials object gives an overall description of the ground heat transfer model.
+
+\subsubsection{Field: NMAT: Number of Materials}\label{field-nmat-number-of-materials}
+
+This field specifies the number of different materials that will be used in the model. Typically only a ground material and a slab material are used.
+
+\subsubsection{Field: Albedo: Surface Albedo: NoSnow}\label{field-albedo-surface-albedo-nosnow}
+
+\subsubsection{Field: Albedo: Surface Albedo: Snow}\label{field-albedo-surface-albedo-snow}
+
+Two fields specify the albedo value of the surface: first for no snow coverage days; second for days with snow coverage. The albedo is the solar reflectivity of the surface, and can vary from 0.05 for blacktop to 0.95 for fresh snow. Typical values for North America reported by Bahnfleth range from 0.16 to 0.4.
+
+\subsubsection{Field EPSLW: Surface Emissivity: NoSnow}\label{field-epslw-surface-emissivity-nosnow}
+
+\subsubsection{Field EPSLW: Surface Emissivity: Snow}\label{field-epslw-surface-emissivity-snow}
+
+This field specifies the long wavelength (thermal) emissivity of the ground surface. It is primarily important for nighttime radiation to the sky, and a value of 0.95 for both snow and no snow is reasonable.
+
+\subsubsection{Field: Z0 Surface Roughness: NoSnow}\label{field-z0-surface-roughness-nosnow}
+
+\subsubsection{Field: Z0 Surface Roughness: Snow}\label{field-z0-surface-roughness-snow}
+
+These two fields specify a surface roughness that is used in the determination of the convection heat transfer coefficient between the ground surface and the air. This roughness is based on boundary layer considerations, and specifies the height at which an experimentally measured velocity profile goes to zero. The units are centimeters, not meters. Typical values are 0.75 cm for no snow, and 0.05 cm for snow.
+
+\subsubsection{Field: HIN: Indoor Hconv: Downward Flow}\label{field-hin-indoor-hconv-downward-flow}
+
+\subsubsection{Field: HIN: Indoor Hconv: Upward Flow}\label{field-hin-indoor-hconv-upward-flow}
+
+These fields specify the combined convective and radiative heat transfer coefficient between the slab top inside surface and the room air for the cases where heat is flowing downward, and upward. The program toggles between the two if the direction of the heat flux changes. Typical values can be found in the ASHRAE Handbook of Fundamentals, but should be about 6 W/(m\(^{2}\)-K) for downward heat flow and 9 W/(m\(^{2}\)-K) for upward heat flow.
+
+The Materials object in the IDD is shown below.
+
+\begin{lstlisting}
+
+Materials,
+  N1, \field NMAT: Number of materials
+  \note typical 2
+  N2, \field ALBEDO: Surface Albedo: No Snow
+  \note typical value = 0-1
+  N3, \field ALBEDO: Surface Albedo: Snow
+  \note typical value = 0-1
+  N4, \field EPSLW: Surface Emissivity: No Snow
+  \note typical value = 0.9
+  N5, \field EPSLW: Surface Emissivity: Snow
+  \note typical value = 0.9
+  N6, \field Z0: Surface Roughness: No Snow
+  \note typical value = 0-10 cm
+  N7, \field Z0: Surface Roughness: Snow
+  \note typical value = 0-10
+  N8, \field HIN: Indoor HConv: Downward Flow
+  \note typical value = 4-10
+  \units W/m2-K
+  N9; \field HIN: Indoor HConv: Upward
+  \note typical value = 4-10
+  \units W/m2-K
+\end{lstlisting}
+
+\subsection{MatlProps or GroundHeatTransfer:Slab:MatlProps Object}\label{matlprops-or-groundheattransferslabmatlprops-object}
+
+This object contains the material properties that describe the materials used in the model. The fields are quite self explanatory and consist of the following:
+
+\subsubsection{Field: RHO: Slab Material Density}\label{field-rho-slab-material-density}
+
+\subsubsection{Field: RHO: Soil Density}\label{field-rho-soil-density}
+
+These two fields specify the density of the slab material and the soil in SI units of kg/m\(^{3}\)
+
+\subsubsection{Field: CP: Slab CP}\label{field-cp-slab-cp}
+
+\subsubsection{Field: CP: Soil CP}\label{field-cp-soil-cp}
+
+These two fields specify the specific heat of the slab and soil in SI units of J/(kg-K).
+
+\subsubsection{Field: TCON: Slab K}\label{field-tcon-slab-k}
+
+\subsubsection{Field: TCON: Soil K}\label{field-tcon-soil-k}
+
+These two fields specify the thermal conductivity of the slab and soil in W/(m\(^{2}\)-K)
+
+The IDD object is shown below:
+
+\begin{lstlisting}
+MatlProps,
+        N1, \field RHO: Slab Material density
+            \note typical value = 2300.0
+            \units kg/m3
+        N2, \field RHO: Soil Density
+            \note typical value = 1200.0
+            \units kg/m3
+        N3, \field CP: Slab CP
+            \note typical value = 650.0
+            \units J/kg-K
+        N4, \field CP: Soil CP
+            \note typical value = 1200.0
+            \units J/kg-K
+        N5, \field TCON: Slab k
+            \note typical value = .9
+            \units W/m2-K
+        N6; \field TCON: Soil k
+            \note typical value = 1.0
+            \units W/m2-K
+\end{lstlisting}
+
+\subsection{BoundConds or GroundHeatTransfer:Slab:BoundConds Object}\label{boundconds-or-groundheattransferslabboundconds-object}
+
+This object supplies some of the boundary conditions used in the simulation.
+
+\subsubsection{Field: EVTR: Is surface evapotranspiration modeled}\label{field-evtr-is-surface-evapotranspiration-modeled}
+
+This field specifies whether or not to use the evapotransporation model. Evapotransportation comprises all of the processes at the ground surface the involve exchanges of latent heat. The inclusion of evapotransporation in the calculation has the greatest effect in warm dry climates, primarily on the ground surface temperature. This field can be used to turn the evapotransporation off and on to check sensitivity to it.
+
+\subsubsection{Field: FIXBC: is the lower boundary at a fixed temperature}\label{field-fixbc-is-the-lower-boundary-at-a-fixed-temperature}
+
+This field permits using a fixed temperature at the lower surface of the model instead of a zero heat flux condition. This change normally has a very small effect on the results. If the flag is set to use a specified temperature, the program calculates an undisturbed temperature profile and used the value at the model depth. The model depth is set by the program using the domain size from the EquivAutoGrid object below.
+
+\subsubsection{Field: TDEEPin}\label{field-tdeepin}
+
+The fixed lower level temperature as described in the FIXBC field.
+
+\subsubsection{Field: USPHflag: Is the ground surface h specified by the user?}\label{field-usphflag-is-the-ground-surface-h-specified-by-the-user}
+
+This field flags the use of a user specified heat transfer coefficient on the ground surface. This condition is used primarily for testing. For normal runs (USPHflag is FALSE), the program calculates the heat transfer coefficient using the weather conditions.
+
+\subsubsection{Field: USERH: User specified ground surface heat transfer coeff}\label{field-userh-user-specified-ground-surface-heat-transfer-coeff}
+
+This field supplies the value of the heat transfer coefficient if USPHflag is TRUE. W/(m\(^{2}\)-K)
+
+The BoundConds object is shown below:
+
+\begin{lstlisting}
+BoundConds,
+        A1, \field EVTR: Is surface evapotranspiration modeled
+            \type choice
+            \key TRUE
+            \key FALSE
+        A2, \field FIXBC: is the lower boundary at a fixed temperature
+            \type choice
+            \key TRUE
+            \key FALSE
+            \note FALSE selects the zero flux lower boundary condition
+        N1, \field TDEEPin,
+            \note User input lower boundary temperature if FIXBC is TRUE
+            \units C
+            \note Blank for FIXBC FALSE or
+            \note to use the calculated 1-D deep ground temperature.
+        A3, \field USRHflag: Is the ground surface h specified by the user?
+            \type choice
+            \key TRUE
+            \key FALSE
+        N2; \field USERH: User specified ground surface heat transfer coeff
+            \units W/(m2-K)
+            \note Used only if USRHflag is TRUE
+\end{lstlisting}
+
+\subsection{BldgProps or GroundHeatTransfer:Slab:BldgProps Object}\label{bldgprops-or-groundheattransferslabbldgprops-object}
+
+This object provides information about the building and its operating conditions.
+
+\subsubsection{Field: IYRS Number of years to iterate}\label{field-iyrs-number-of-years-to-iterate}
+
+This field specifies the number of years to iterate. This means that the simulation comes to an either an annual steady periodic condition by converging to a tolerance (see ConvTol field) or it runs for this number of years. A ten year maximum is usually sufficient. It is important to note that the ground heat transfer behavior will change during the first several years of operating a ground contact structure. It takes several years to change from the undisturbed profile to the disturbed profile under a building.
+
+\subsubsection{Field: Shape Slab shape}\label{field-shape-slab-shape}
+
+Use only the value 0 here. Only a rectangular shape is implemented.
+
+\subsubsection{Field: HBLDG: Building Height}\label{field-hbldg-building-height}
+
+This field supplies the building height. This is used to calculate the building shadowing on the ground. Height is in meters.
+
+\subsubsection{Field: TIN1 - TIN12 \textless{}month\textgreater{} Indoor Average temperature set point}\label{field-tin1---tin12-month-indoor-average-temperature-set-point}
+
+The next twelve fields specify the average indoor building set point temperatures for each month of the year. These fields are useful for simulating a building that is not temperature controlled for some of the year. In such a case, the average indoor set point temperatures can be obtained by first running the model in EnergyPlus with an insulated floor boundary condition, and then using the resulting monthly average zone temperatures in these fields.
+
+\subsubsection{Field: TINAmp: Daily Indoor sine wave variation amplitude}\label{field-tinamp-daily-indoor-sine-wave-variation-amplitude}
+
+This field permits imposing a daily sinusoidal variation in the indoor setpoint temperature to simulate the effect of a setback profile. The value specified will be the amplitude of the sine wave.
+
+\subsubsection{Field: ConvTol: Convergence Tolerance}\label{field-convtol-convergence-tolerance}
+
+This final field specifies the convergence tolerance used to control the iteration. When the temperature change of all nodes is less than the convergence value, iteration ceases.
+
+The entire BldgProps Object is shown below.
+
+\begin{lstlisting}
+BldgProps,
+      N1, \field IYRS: Number of years to iterate
+          \note typical value = 10
+      N2, \field Shape: Slab shape
+          \note only value = 0
+      N3, \field HBLDG: Building height
+          \note typical value = 0-20
+          \units m
+      N4, \field TIN1: January Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N5, \field TIN2: February Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N6, \field TIN3: March Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N7, \field TIN4: April Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N8, \field TIN5: May Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N9, \field TIN6: June Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N10, \field TIN7: July Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N11, \field TIN8: August Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N12, \field TIN9: September Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N13, \field TIN10: October Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N14, \field TIN11: NovemberIndoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N15, \field TIN12: December Indoor Average temperature set point
+          \note typical value = 22
+          \units C
+      N16, \field TINAmp: Daily Indoor sine wave variation amplitude
+           \note typical value: 0
+           \units C
+      N17; \field ConvTol: Convergence Tolerance
+           \note typical value = 0.1
+\end{lstlisting}
+
+\subsection{Insulation or GroundHeatTransfer:Slab:Insulation Object}\label{insulation-or-groundheattransferslabinsulation-object}
+
+This object supplies the information about insulation used around the slab. There are two possible configurations: under the slab or vertical insulation around the slab.
+
+\subsubsection{Field RINS: R value of under slab insulation}\label{field-rins-r-value-of-under-slab-insulation}
+
+This field provides the thermal resistance value of the under slab insulation. It should be zero if the vertical insulation configuration is selected. Units are m\(^{2}\) K/W.
+
+\subsubsection{Field DINS: Width of strip of under slab insulation}\label{field-dins-width-of-strip-of-under-slab-insulation}
+
+This specifies the width of the perimeter strip of insulation under the slab in meters. Again a zero value should be used for the vertical insulation configuration. Units are m.
+
+\subsubsection{Field RVINS: R value of vertical insulation}\label{field-rvins-r-value-of-vertical-insulation}
+
+This field specifies the thermal resistance of the vertical insulation. It should be zero if the under slab insulation configuration is in effect. Units are m\(^{2}\) K/W.
+
+\subsubsection{Field ZVINS: Depth of vertical insulation}\label{field-zvins-depth-of-vertical-insulation}
+
+This field specifies the depth of the vertical insulation into the ground in meters. Note that it starts at the slab upper surface and extends into the ground. Only .2 .4 .6 .8 1.0 1.5 2.0 2.5 or 3.0 m should be used. Units are m.
+
+\subsubsection{Field IVINS: Flag: Is there vertical insulation?}\label{field-ivins-flag-is-there-vertical-insulation}
+
+This final field specifies that vertical the vertical insulation configuration is being used. The value of 1 specifies yes and 0 specifies no.
+
+The Insulation object is shown below.
+
+\begin{lstlisting}
+Insulation,
+        N1, \field RINS: R value of under slab insulation
+            \note typical value = 0-2.0
+            \units m2-K/W
+        N2, \field DINS: Width of strip of under slab insulation
+            \note typical value = 0-2.0
+            \units m
+        N3, \field RVINS: R value of vertical insulation
+            \note typical value = 0-3.0
+            \units m2-K/W
+        N4, \field ZVINS: Depth of vertical insulation
+            \note only use values = .2 .4 .6 .8 1.0 1.5 2.0 2.5 3.0
+            \units m
+        N5; \field IVINS: Flag: Is there vertical insulation
+            \note values: 1 = yes 0 = no
+\end{lstlisting}
+
+\subsection{EquivalentSlab or GroundHeatTransfer:Slab:EquivalentSlab Object}\label{equivalentslab-or-groundheattransferslabequivalentslab-object}
+
+This object provides the basic information for running a model that uses the area over perimeter ratio of the slab to determine the size of an equivalent rectangular slab.
+
+\subsubsection{Field APRatio: The area to perimeter ratio for this slab}\label{field-apratio-the-area-to-perimeter-ratio-for-this-slab-000}
+
+This field specifies the area over perimeter ratio of the slab in meters.
+
+\subsubsection{Field SLABDEPTH: Thickness of slab on grade}\label{field-slabdepth-thickness-of-slab-on-grade}
+
+This field specifies the thickness of the slab in meters. Note that the slab top surface is level with the ground surface, so this is the depth into the ground. The slab depth has a significant effect on the temperature calculation, and it is also important for the auto-grid process. The finite difference grids are set in such a way that they use the slab thickness to determine the vertical grid spacing. Because of this, autogridding will fail if the slab thickness is specified larger than 0.25 meters. The program also is set up so that the slab is a single finite difference cell in the vertical direction. Thus, if the slab thickness is set too large, the accuracy of the calculation may be suspect. The results with three different slab thicknesses are shown below.
+
+All other inputs for the runs were the same. It is clear that the slab thickness has a significant effect because of the horizontal component of conduction in both directions in the slab.
+
+\subsubsection{Field CLEARANCE: Distance from edge of slab to domain edge}\label{field-clearance-distance-from-edge-of-slab-to-domain-edge}
+
+This field specifies the distance from the slab to the edge of the area that will be modeled with the grid system. It is the basic size dimension that is used to set the horizontal extent of the domain. The units are meters, and 15 meters is a reasonable value.
+
+\subsubsection{Field ZCLEARANCE: Distance from bottom of slab to domain bottom}\label{field-zclearance-distance-from-bottom-of-slab-to-domain-bottom}
+
+This field specifies the vertical distance from the slab to the bottom edge of the area that will be modeled with the grid system. It is the basic size dimension that is used to set vertical extent of the domain. The units are meters, and 15 meters is a reasonable value.
+
+The object is shown below.
+
+\begin{lstlisting}
+EquivalentSlab,
+\memo Using an equivalent slab allows non-rectangular shapes to be modeled accurately
+        N1, \field APRatio: The area to perimeter ratio for this slab
+            \units m
+        N2, \field SLABDEPTH: Thickness of slab on grade
+            \note typical value = 0.1
+            \units m
+        N3, \field CLEARANCE: Distance from edge of slab to domain edge
+            \note typical value = 15.0
+            \units m
+        N4; \field ZCLEARANCE: Distance from bottom of slab to domain bottom
+            \note typical value = 15.0
+            \units m
+\end{lstlisting}
+
+\begin{figure}[hbtp] % fig 21
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image019.jpg}
+\caption{Graph of Slab Outside Temperature vs Slab Thickness \protect \label{fig:graph-of-slab-outside-temperature-vs-slab}}
+\end{figure}
+
+\textbf{The EquivSlab object and the EquivAutoGrid Objects that follow have been replaced by the EquivalentSlab object above. They are included in the idd so that old idf files can still be read.}
+
+\subsection{EquivSlab Object - Obsolete}\label{equivslab-object---obsolete}
+
+This object provides the basic information for running a model that uses the area over perimeter ratio of the slab to determine the size of an equivalent rectangular slab.
+
+\subsubsection{Field APRatio: The area to perimeter ratio for this slab}\label{field-apratio-the-area-to-perimeter-ratio-for-this-slab-1}
+
+This field specifies the area over perimeter ratio of the slab in meters.
+
+\subsubsection{Field: EquivSizing}\label{field-equivsizing}
+
+This field value should be TRUE. This means that the program will determine the dimensions of the equivalent slab that satisfactorily models the A/P ratio.
+
+The object is shown below.
+
+\begin{lstlisting}
+EquivSlab,
+\memo Using an equivalent slab allows non-rectangular shapes to be modeled accurately
+\memo The simulation default should be EquivSizing = True
+        N1, \field APRatio: The area to perimeter ratio for this slab
+            \units m
+        A1; \field EquivSizing:
+            \note Flag: Will the dimensions of an equivalent slab
+            \note be calculated (TRUE) or will the dimensions be input directly? (FALSE)
+            \note It is recommended that EnergyPlus users use TRUE.
+\end{lstlisting}
+
+\subsection{EquivAutoGrid Object - Obsolete}\label{equivautogrid-object---obsolete}
+
+This object provides the information needed by the program to automatically generate the calculation grid when the slab is described as an equivalent slab. It is necessary for EnergyPlus users because equivalent slab is the appropriate option.
+
+\subsubsection{Field SLABDEPTH: Thickness of slab on grade}\label{field-slabdepth-thickness-of-slab-on-grade-1}
+
+This field specifies the thickness of the slab in meters. Note that the slab top surface is level with the ground surface, so this is the depth into the ground. The slab depth has a significant effect on the temperature calculation, and it is also important for the auto-grid process. The finite difference grids are set in such a way that they use the slab thickness to determine the vertical grid spacing. Because of this, autogridding will fail if the slab thickness is specified larger than 0.25 meters. The program also is set up so that the slab is a single finite difference cell in the vertical direction. Thus, if the slab thickness is set too large, the accuracy of the calculation may be suspect. The results with three different slab thicknesses are shown below.
+
+All other inputs for the runs were the same. It is clear that the slab thickness has a significant effect because of the horizontal component of conduction in both directions in the slab.
+
+\subsubsection{Field CLEARANCE: Distance from edge of slab to domain edge}\label{field-clearance-distance-from-edge-of-slab-to-domain-edge-1}
+
+This field specifies the distance from the slab to the edge of the area that will be modeled with the grid system. It is the basic size dimension that is used to set both the horizontal and vertical extent of the domain. The units are meters, and 15 meters is a reasonable value.
+
+The EquivAutoGrid object is shown below.
+
+\begin{lstlisting}
+EquivAutoGrid, \memo  EquivAutoGrid only necessary when EquivSizing is true
+               \memo  EnergyPlus users normally use this option.
+        N1, \field SLABDEPTH: Thickness of slab on grade
+            \note typical value = 0.1
+            \units m
+        N2; \field CLEARANCE: Distance from edge of slab to domain edge
+            \note typical value = 15.0
+            \units m
+\end{lstlisting}
+
+\subsection{Additional Objects}\label{additional-objects-000}
+
+There are five additional objects in the IDD that can be used under very special situations by researchers who want to generate special calculation grids. They are normally not useful to EnergyPlus users. They will be shown as IDD sections only. They do not need to be in the IDF.
+
+\begin{lstlisting}
+AutoGrid,   \memo AutoGrid only necessary when EquivSizing is false
+            \memo  Not normally needed by EnergyPlus users.
+        N1, \field SLABX: X dimension of the building slab
+            \note typical values = 0-60.0
+            \units m
+        N2, \field SLABY: Y dimension of the building slab
+            \note typical values = 0-60.0
+            \units m
+        N3, \field SLABDEPTH: Thickness of slab on grade
+            \note typical value = .1
+            \units m
+        N4; \field CLEARANCE: Distance from edge of slab to domain edge
+            \note typical value = 15.0
+            \units m
+\end{lstlisting}
+
+\begin{lstlisting}
+ManualGrid, \memo Manual Grid only necessary using manual gridding (not recommended)
+            \memo   Used only in special cases.
+        N1, \field NX: Number of cells in the X direction
+            \note typical values = 15
+        N2, \field NY: Number of cells in the Y direction
+            \note typical values = 15
+        N3, \field NZ: Number of cells in the Z direction
+            \note typical values = 15
+        N4, \field IBOX: X direction cell indicator of slab edge
+            \note typical values = 1-10
+        N5; \field JBOX: Y direction cell indicator of slab edge
+            \note typical values = 1-10
+\end{lstlisting}
+
+\begin{lstlisting}
+XFACE,  \memo This is only needed when using manual gridding (not recommended)
+        \memo XFACE: X Direction cell face coordinates: m
+  N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
+  N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26, N27, N28, N29,
+  N30, N31, N32, N33, N34, N35, N36, N37, N38, N39, N40;
+\end{lstlisting}
+
+\begin{lstlisting}
+YFACE,  \memo This is only needed when using manual gridding (not recommended)
+        \memo YFACE: Y Direction cell face coordinates: m,
+  N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
+  N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26, N27, N28, N29,
+  N30, N31, N32, N33, N34, N35, N36, N37, N38, N39, N40;
+\end{lstlisting}
+
+\begin{lstlisting}
+ZFACE,  \memo This is only needed when usuing manual gridding (not recommended)
+        \memo ZFACE: Z Direction cell face coordinates: m
+        N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
+        N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25;
+\end{lstlisting}
+
+\subsection{Sample IDF File - Slab Program}\label{sample-idf-file---slab-program}
+
+A sample IDF file is shown below.
+
+\begin{lstlisting}
+
+!-Generator IDFEditor 1.12
+  !-NOTE: All comments with '!-' are ignored by the IDFEditor and are generated automatically.
+  !-      Use '!' comments if they need to be retained when using the IDFEditor.
+
+  !-   = = = = = = = = = = =  ALL OBJECTS IN CLASS: MATERIALS = = = = = = = = = = =
+
+  Materials,
+  2,           !- NMAT: Number of materials
+  0.158,       !- ALBEDO: Surface Albedo: No Snow
+  0.379,       !- ALBEDO: Surface Albedo: Snow
+  0.9,         !- EPSLW: Surface Emissivity: No Snow
+  0.9,         !- EPSLW: Surface Emissivity: Snow
+  0.75,        !- Z0: Surface Roughness: No Snow
+  0.03,        !- Z0: Surface Roughness: Snow
+  6.13,        !- HIN: Indoor HConv: Downward Flow {W/m2-K}
+  9.26;        !- HIN: Indoor HConv: Upward {W/m2-K}
+
+  !-   = = = = = = = = = = =  ALL OBJECTS IN CLASS: MATLPROPS = = = = = = = = = = =
+
+  MatlProps,
+  2300,        !- RHO: Slab Material density {kg/m3}
+  1200,        !- RHO: Soil Density {kg/m3}
+  653,         !- CP: Slab CP {J/kg-K}
+  1200,        !- CP: Soil CP {J/kg-K}
+  0.93,        !- TCON: Slab k {W/m-K}
+  1;           !- TCON: Soil k {W/m-K}
+
+  !-   = = = = = = = = = = =  ALL OBJECTS IN CLASS: BOUNDCONDS = = = = = = = = = = =
+
+  BoundConds,
+  TRUE,        !- EVTR: Is surface evapotranspiration modeled
+  TRUE,        !- FIXBC: is the lower boundary at a fixed temperature
+  FALSE;       !- OLDTG: is there an old ground temperature file
+
+  !-   = = = = = = = = = = =  ALL OBJECTS IN CLASS: BLDGPROPS = = = = = = = = = = =
+
+  BldgProps,
+  10,          !- IYRS: Number of years to iterate
+  0,           !- Shape: Slab shape
+  4,           !- HBLDG: Building height {m}
+  18,          !- TIN1: January Indoor Average temperature set point {C}
+  18,          !- TIN2: February Indoor Average temperature set point {C}
+  18,          !- TIN3: March Indoor Average temperature set point {C}
+  20,          !- TIN4: April Indoor Average temperature set point {C}
+  20,          !- TIN5: May Indoor Average temperature set point {C}
+  20,          !- TIN6: June Indoor Average temperature set point {C}
+  22,          !- TIN7: July Indoor Average temperature set point {C}
+  22,          !- TIN8: August Indoor Average temperature set point {C}
+  22,          !- TIN9: September Indoor Average temperature set point {C}
+  22,          !- TIN10: October Indoor Average temperature set point {C}
+  20,          !- TIN11: NovemberIndoor Average temperature set point {C}
+  20,          !- TIN12: December Indoor Average temperature set point {C}
+  0,           !- TINAmp: Daily sine wave variation amplitude {C}
+  0.10;        !- ConvTol: Convergence Tolerance
+
+  !-   = = = = = = = = = = =  ALL OBJECTS IN CLASS: INSULATION = = = = = = = = = = =
+
+  Insulation,
+  0.,          !- RINS: R value of under slab insulation {m2-K/W}
+  0.,          !- DINS: Width of strip of under slab insulation {m}
+  2.0,         !- RVINS: R value of vertical insulation {m2-K/W}
+  2.0,         !- ZVINS: Depth of vertical insulation {m}
+  1;           !- IVINS: Flag: Is there vertical insulation
+
+  !-   = = = = = = = = = = =  ALL OBJECTS IN CLASS: EQUIVSLAB = = = = = = = = = = =
+
+  EquivalentSlab,
+  10,          !- APRatio: The area to perimeter ratio for this slab {m}
+  0.1,         !- SLABDEPTH: Thickness of slab on grade {m}
+  15,          !- CLEARANCE: Distance from edge of slab to domain edge {m}
+  10;          !-ZCLEARANCE: Distance from bottom of slab to domain bottom
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/references-001.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/references-001.tex
new file mode 100644
index 00000000000..151c88e4e9d
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/references-001.tex
@@ -0,0 +1,9 @@
+\section{References}\label{references-000}
+
+Bahnfleth, W.P. 1989. \emph{Three Dimensional Modeling of Heat Transfer from Slab Floors}, Ph.D.~dissertation, also published as USACERL TM E-89/11, University of Illinois.
+
+Bahnfleth, W.P. and C.O. Pedersen. 1990. A Three Dimensional Numerical Study of Slab-on-Grade Heat Transfer. \emph{ASHRAE Transactions} Pt. 2, 96:61-72.
+
+Clements, Edward. 2004. \emph{Three Dimensional Foundation Heat Transfer Modules for Whole-Building Energy Analysis}, MS Thesis, Pennsylvania State University.
+
+Cogil, Cynthia A. 1998. Modeling of Basement Heat Transfer and Parametric Study of Basement Insulation for Low Energy Housing. MS Thesis of Architectural Engineering, Pennsylvania State University.
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/running-the-basement-program.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/running-the-basement-program.tex
new file mode 100644
index 00000000000..3466a1b6887
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/running-the-basement-program.tex
@@ -0,0 +1,47 @@
+\section{Running the Basement Program}\label{running-the-basement-program}
+
+EP-Launch can be used to run the Basement program.
+
+If the Basement Objects (see The Basement idd below) are located in the standard EnergyPlus IDF input file than the Single Input File and Group of Input File tabs of EP-Launch can be used and the Basement preprocessor will be called automatically during the simulation process. In this case the Basement objects should all appear with the object name starting with ``\textbf{GroundHeatTransfer:Basement:}'' This option also requires a \textbf{GroundHeatTransfer:Control} object in the EnergyPlus idf file (see Input Output Reference).
+
+If the Basement objects are located in a separate file, they should be run using the Basement option on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the Basement program.
+
+You can also run the Basement program as a console application. To execute it, we have provided the batch file:
+
+RunBasement
+
+Steps for running the program
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Open a DOS command prompt window (Start -\textgreater{} Programs -\textgreater{} Accessories -\textgreater{} Command Prompt)
+\item
+  Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
+\end{enumerate}
+
+C:
+
+CD \textbackslash{}\textless{}rootfolder\textgreater{}\textless{}/span\textgreater{}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Change to the specific folder for the console application:
+\end{enumerate}
+
+CD PreProcess\textbackslash{}GrndTempCalc
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Run the program (for example use the example included with the install):
+\end{enumerate}
+
+RunBasement BasementExample USA\_IL\_Chicago-OHare\_TMY2
+
+In the following section, some description of modifying the batch file and details on files that the basement program uses are given.
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/running-the-slab-program.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/running-the-slab-program.tex
new file mode 100644
index 00000000000..881c7562ebc
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/running-the-slab-program.tex
@@ -0,0 +1,47 @@
+\section{Running the Slab Program}\label{running-the-slab-program}
+
+EP-Launch can be used to run the Slab program using two different methods.
+
+If the Slab objects (see Description of the Objects in the E+SlabGHT.IDD) are located in the standard EnergyPlus IDF input file than the Single Input File and Group of Input File tabs of EP-Launch can be used and the Slab preprocessor will be called automatically during the simulation process. In this case the Slab objects should all appear with the object name starting with ``\textbf{GroundHeatTransfer:Slab:}'' This option also requires a \textbf{GroundHeatTransfer:Control} object in the EnergyPlus idf file (see Input Output Reference).
+
+If the Slab objects are located in a separate file, they should be run using the Slab option on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the Slab program.
+
+You can also run the slab program as a console application. To execute it, we have provided the batch file:
+
+RunSlab
+
+Steps for running the program
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Open a DOS command prompt window (Start à Programs à Accessories à Command Prompt)
+\item
+  Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
+\end{enumerate}
+
+C:
+
+CD \textbackslash{}\textless{}rootfolder\textgreater{}\textless{}/span\textgreater{}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Change to the specific folder for the console application:
+\end{enumerate}
+
+CD PreProcess\textbackslash{}GrndTempCalc
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Run the program (for example use the example included with the install):
+\end{enumerate}
+
+RunSlab SlabExample USA\_IL\_Chicago-OHare\_TMY2
+
+In the following section, some description of modifying the batch file and details on files that the slab program uses are given.
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/slab-configuration-drawing.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/slab-configuration-drawing.tex
new file mode 100644
index 00000000000..dc6ad5e39a8
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/slab-configuration-drawing.tex
@@ -0,0 +1,9 @@
+\section{Slab configuration Drawing}\label{slab-configuration-drawing}
+
+The slab configuration used in the slab model is a ``slab in grade'' model. That is, the slab top surface is assumed level with the outside earth surface. If a ``slab on grade'' configuration, having the bottom surface of the slab level with the outside earth surface is desired, the best approximation is to use the horizontal insulation configuration. The edge of the slab will have a small thermal resistance due to the two dimensional path through the earth, but the effect is small. In any case, uninsulated slab edges are certainly not recommended in cold climates.
+
+\begin{figure}[hbtp] % fig 20
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image018.jpg}
+\caption{Slab-in-grade illustration \protect \label{fig:slab-in-grade-illustration}}
+\end{figure}
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/slab-program-output-files.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/slab-program-output-files.tex
new file mode 100644
index 00000000000..3e0d9610511
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/slab-program-output-files.tex
@@ -0,0 +1,138 @@
+\section{Slab Program Output Files}\label{slab-program-output-files}
+
+The following output files are created by the Slab program and saved in the output file path specified in the RunSlab.bat file:
+
+*\_slab.ger - Error file. Input errors are reported here.
+
+*\_slab.out - Summary of inputs, location data, and grid coordinates
+
+*\_slab.gtp - Monthly ground temperatures and EnergyPlus idf objects
+
+\subsection{EnergyPlus idf Objects from Slab Program}\label{energyplus-idf-objects-from-slab-program}
+
+If the objects are placed in the normal EnergyPlus input IDF file using the ``GroundHeatTransfer:Slab:'' prefix, then the values resulting from the Slab preprocessor will be automatically included in the simulation at run time. The surfaces can reference these values using Outside Boundary Conditions of:
+
+\begin{itemize}
+\item
+  GroundSlabPreprocessorAverage
+\item
+  GroundSlabPreprocessorCore
+\item
+  GroundSlabPreprocessorPerimeter
+\end{itemize}
+
+The objects that support this include:
+
+\begin{itemize}
+\item
+  BuildingSurface:Detailed
+\item
+  Wall:Detailed
+\item
+  RoofCeiling:Detailed
+\item
+  Floor:Detailed
+\end{itemize}
+
+The slab program is capable of supplying the EnergyPlus idf objects needed to use the slab program outputs directly by copying the objects into the EnergyPlus idf file. The file containing these objects has the extension gtp, and an example is shown below. It contains the output temperatures and heat fluxes, and in addition it contains an OtherSideCoefficient object example as mentioned above, and three compact schedule objects that can be used to describe the average, core and perimeter temperatures directly in EnergyPlus. The Name in the compact schedule corresponds to the GroundTemperatureScheduleName in the OtherSideCoefficient object.
+
+= = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+
+CHECK CONVERGENCE MESSAGE AT END OF THIS FILE!
+
+= = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+
+\begin{lstlisting}
+   Monthly Slab Outside Face Temperatures, C and Heat Fluxes(loss), W/(m^2)
+ Perimeter Area: 304.00  Core Area: 1296.00
+       Month   TAverage   TPerimeter    TCore      TInside AverageFlux PerimeterFlux CoreFlux
+          1      17.74     16.41        18.05       18.00       0.88        5.39       -0.17
+          2      17.49     16.15        17.81       18.00       1.73        6.29        0.66
+          3      17.45     16.23        17.74       18.00       1.86        6.02        0.88
+          4      18.96     17.86        19.22       20.00       3.51        7.24        2.64
+          5      19.22     18.22        19.45       20.00       2.66        6.04        1.86
+          6      19.28     18.38        19.49       20.00       2.44        5.48        1.73
+          7      20.83     19.98        21.03       22.00       3.96        6.87        3.28
+          8      21.12     20.39        21.29       22.00       2.98        5.47        2.40
+          9      21.18     20.46        21.35       22.00       2.76        5.22        2.19
+         10      21.17     20.23        21.39       22.00       2.82        6.02        2.08
+         11      19.64     18.63        19.88       20.00       1.22        4.63        0.42
+         12      19.36     18.14        19.65       20.00       2.16        6.30        1.19
+\end{lstlisting}
+
+\begin{lstlisting}
+! OTHER SIDE COEFFICIENT OBJECT EXAMPLE FOR IDF FILE
+ SurfaceProperty:OtherSideCoefficients,
+ ExampleOSC,                !- OtherSideCoeff Name \*\*\*CHANGE THIS!\*\*\*
+ 0,                         !- Combined convective/radiative film coefficient
+ 1,                         !- N2,User selected Constant Temperature {C}
+ 1,                         !- Coefficient modifying the user selected constant temperature
+ 0,                         !- Coefficient modifying the external dry bulb temperature
+ 0,                         !- Coefficient modifying the ground temperature
+ 0,                         !- Coefficient modifying the wind speed term (s/m)
+ 0,                         !- Coefficient modifying the zone air temperature
+                            !  part of the equation
+ GroundTempCompactSchedName; !- Name of Schedule for values of const
+                            ! temperature. Schedule values replace N2.
+                            !  \*\*\*REPLACE WITH CORRECT NAME\*\*\*
+\end{lstlisting}
+
+\begin{lstlisting}
+Schedule:Compact,
+MonthlyAveSurfaceTemp, !Name
+Temperature ,            !- ScheduleType
+Through:   1/31,
+For:AllDays,
+Until:24:00,
+ 17.74    ,
+Through:   2/28,
+For:AllDays,
+Until:24:00,
+ 17.49    ,
+Through:   3/31,
+For:AllDays,
+Until:24:00,
+ 17.45    ,
+Through:   4/30,
+For:AllDays,
+Until:24:00,
+ 18.96    ,
+Through:   5/31,
+For:AllDays,
+Until:24:00,
+ 19.22    ,
+Through:   6/30,
+For:AllDays,
+Until:24:00,
+ 19.28    ,
+Through:   7/31,
+For:AllDays,
+Until:24:00,
+ 20.83    ,
+Through:   8/31,
+For:AllDays,
+Until:24:00,
+ 21.12    ,
+Through:   9/30,
+For:AllDays,
+Until:24:00,
+ 21.18    ,
+Through:  10/31,
+For:AllDays,
+Until:24:00,
+ 21.17    ,
+Through:  11/30,
+For:AllDays,
+Until:24:00,
+ 19.64    ,
+Through:  12/31,
+For:AllDays,
+Until:24:00,
+ 19.36    ;
+\end{lstlisting}
+
+ - compact schedules for MonthlyPerimeterTemp and MonthlyCoreTemp are included.
+
+\begin{lstlisting}
+  Convergence has been gained.
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/technical-details-on-files-for-ground-heat-001.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/technical-details-on-files-for-ground-heat-001.tex
new file mode 100644
index 00000000000..7b201932057
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/technical-details-on-files-for-ground-heat-001.tex
@@ -0,0 +1,24 @@
+\section{Technical Details on Files for Ground Heat Transfer with Basements}\label{technical-details-on-files-for-ground-heat-transfer-with-basements}
+
+The basement program used to calculate the results is included with the EnergyPlus distribution. It requires an input file named BasementGHTin.idf in input data file format. The needed corresponding idd file is BasementGHT.idd. An EnergyPlus weather file for the location is also needed. A batch file, RunBasement, is placed in the same folder with the program and sample files. To use it (Command mode or DOS mode), one may modify several important lines:
+
+\begin{lstlisting}
+:Instructions:
+:  Complete the following path and program names.
+:  path names must have a following \\ or errors will happen
+ set program\_path =
+ set program\_name = Basement.exe
+ set input\_path =
+ set output\_path =
+ set weather\_path = C:\\EnergyPlus\\WeatherData\\
+\end{lstlisting}
+
+and then in command mode issue the run command:
+
+\begin{lstlisting}
+RunBasement myinput Chicago
+\end{lstlisting}
+
+Where you would have myinput.idf in ``input\_path'' and Chicago would be the name of the .epw file in the ``weather\_path''.
+
+You should set up the command mode so that it does not automatically close the window at the end of program termination if you want to see the commands as they run and know for sure that no errors occurred.
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/technical-details-on-files-for-ground-heat.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/technical-details-on-files-for-ground-heat.tex
new file mode 100644
index 00000000000..53c998ccee7
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/technical-details-on-files-for-ground-heat.tex
@@ -0,0 +1,24 @@
+\section{Technical Details on Files for Ground Heat Transfer with Slabs}\label{technical-details-on-files-for-ground-heat-transfer-with-slabs}
+
+The slab program used to calculate the results is included with the EnergyPlus distribution. It requires an input file named GHTin.idf in input data file format. The needed corresponding idd file is SlabGHT.idd. An EnergyPlus weather file for the location is also needed. A batch file, RunSlab, is placed in the same folder with the program and sample files. To use it (Command mode or DOS mode), one may modify several important lines:
+
+\begin{lstlisting}
+:Instructions:
+:  Complete the following path and program names.
+:  path names must have a following \\ or errors will happen
+ set program\_path =
+ set program\_name = Slab.exe
+ set input\_path =
+ set output\_path =
+ set weather\_path = C:\\EnergyPlus\\WeatherData\\
+\end{lstlisting}
+
+and then in command mode issue the run command:
+
+\begin{lstlisting}
+RunSlab myinput Chicago
+\end{lstlisting}
+
+Where you would have myinput.idf in ``input\_path'' and Chicago would be the name of the .epw file in the ``weather\_path''.
+
+You should set up the command mode so that it does not automatically close the window at the end of program termination if you want to see the commands as they run and know for sure that no errors occurred.
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/the-basement-idd.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/the-basement-idd.tex
new file mode 100644
index 00000000000..796570f7d42
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/the-basement-idd.tex
@@ -0,0 +1,265 @@
+\section{The Basement idd}\label{the-basement-idd}
+
+The basement idd objects and fields are shown below. These objects also appear in the main Energy+.IDD file with the prefix ``GroundHeatTransfer:Basement:''
+
+\begin{lstlisting}
+! Basement foundation heat transfer module Input Data Dictionary file
+! Created:    August 18, 2000
+! Written by: Edward Clements
+! Modified for EnergyPlus Auxiliary Application by C. O. Pedersen 10/04
+! Description format: FORTRAN var.: description, units, typ. values
+\end{lstlisting}
+
+\begin{lstlisting}
+SimParameters,
+      N1,\field F: Multiplier for the ADI solution:
+         \note 0<F<1.0,
+         \note typically 0.1 (0.5 for high k soil]
+      N2; \field IYRS: Maximum number of yearly iterations:
+         \note typically 15-30]
+\end{lstlisting}
+
+\begin{lstlisting}
+MatlProps,
+     N1, \field NMAT: Number of materials in this domain
+         \maximum 6
+     N2, \field Density for Foundation Wall
+         \note typical value 2243
+         \units kg/m3
+     N3, \field density for Floor Slab
+         \note typical value 2243
+         \units kg/m3
+     N4, \field density for Ceiling
+         \note typical value 311
+         \units kg/m3
+     N5, \field density for Soil
+         \note typical value 1500
+         \units kg/m3
+     N6, \field density for Gravel
+         \note typical value 2000
+         \units kg/m3
+     N7, \field density for Wood
+         \note typical value 449
+         \units kg/m3
+     N8,  \field Specific heat for foundation wall
+          \note typical value 880
+          \units J/kg-K
+     N9,  \field Specific heat for floor slab
+          \note typical value 880
+          \units J/kg-K
+     N10, \field Specific heat for ceiling
+          \note typical value 1530
+          \units J/kg-K
+     N11, \field Specific heat for soil
+          \note typical value 840
+          \units J/kg-K
+     N12, \field Specific heat for gravel
+          \note typical value 720
+          \units J/kg-K
+     N13, \field Specific heat for wood
+          \note typical value 1530
+          \units J/kg-K
+     N14, \field Thermal conductivity for foundation wall
+          \note typical value 1.4
+          \units W/m-K
+     N15, \field Thermal conductivity for floor slab
+          \note typical value 1.4
+          \units W/m-K
+     N16, \field Thermal conductivity for ceiling
+          \note typical value 0.09
+          \units W/m-K
+     N17,  \field thermal conductivity for soil
+          \note typical value 1.1
+          \units W/m-K
+     N18, \field thermal conductivity for gravel
+          \note typical value 1.9
+          \units W/m-K
+     N19; \field thermal conductivity for wood
+          \note typical value 0.12
+          \units W/m-K
+\end{lstlisting}
+
+\begin{lstlisting}
+Insulation,
+     N1, \field REXT: R Value of any exterior insulation, K/(W/m2)]
+         \units m2-K/W
+     A1; \field INSFULL: Flag: Is the wall fully insulated?
+         \note  True for full insulation
+         \note  False for insulation half way down side wall from grade line
+\end{lstlisting}
+
+\begin{lstlisting}
+SurfaceProps,
+     N1, \field ALBEDO: Surface albedo for No snow conditions
+         \note typical value 0.16
+     N2, \field ALBEDO: Surface albedo for snow conditions
+         \note typical value 0.40
+     N3, \field EPSLN: Surface emissivity No Snow
+         \note typical value 0.94
+     N4, \field EPSLN: Surface emissivity  with Snow
+         \note typical value 0.86
+     N5, \field VEGHT: Surface roughness No snow conditions,cm
+         \note typical value 6.0
+         \units cm
+     N6, \field VEGHT: Surface roughness Snow conditions, cm, ]
+         \note typical value 0.25
+         \units cm
+     A1; \field PET: Flag, Potential evapotranspiration on? T/F]
+         \note  Typically, PET is True
+\end{lstlisting}
+
+\begin{lstlisting}
+BldgData,
+     N1, \field DWALL: Wall thickness,
+         \note typical value .2]
+         \units m
+     N2, \field DSLAB: Floor slab thickness,
+         \units m
+         \maximum 0.25
+     N3, \field DGRAVXY: Width of gravel pit beside basement wall
+         \units  m
+     N4, \field DGRAVZN: Gravel depth extending above the floor slab
+         \units m
+     N5; \field DGRAVZP: Gravel depth below the floor slab,
+         \units m
+         \note typical value 0.1
+\end{lstlisting}
+
+\begin{lstlisting}
+Interior,
+   A1, \field COND: Flag: Is the basement conditioned?
+       \note TRUE or FALSE
+       \note for EnergyPlus this should be TRUE
+   N1, \field HIN: Downward convection only heat transfer coefficient
+       \units W/m2-K
+   N2, \field HIN: Upward convection only heat transfer coefficient
+       \units W/m2-K
+   N3, \field HIN: Horizontal convection only heat transfer coefficient
+       \units W/m2-K
+   N4, \field HIN: Downward combined (convection and radiation) heat transfer coefficient
+       \units W/m2-K
+   N5, \field HIN: Upward combined (convection and radiation) heat transfer coefficient
+       \units W/m2-K
+   N6; \field HIN: Horizontal combined (convection and radiation) heat transfer coefficient
+       \units W/m2-K
+\end{lstlisting}
+
+\begin{lstlisting}
+ComBldg,
+\memo ComBldg contains the monthly average temperatures (C) and possibility of daily variation amplitude
+   N1,  \field January average temperature
+        \units C
+   N2,  \field February average temperature
+        \units C
+   N3,  \field March average temperature
+        \units C
+   N4,  \field April average temperature
+        \units C
+   N5,  \field May average temperature
+        \units C
+   N6,  \field June average temperature
+        \units C
+   N7,  \field July average temperature
+        \units C
+   N8,  \field August average temperature
+        \units C
+   N9,  \field September average temperature
+        \units C
+   N10, \field October average temperature
+        \units C
+   N11, \field November average temperature
+        \units C
+   N12, \field December average temperature
+        \units C
+   N13; \field Daily variation sine wave amplitude
+        \units C
+        \note (Normally zero, just for checking)
+\end{lstlisting}
+
+\begin{lstlisting}
+EquivSlab,  !  Supplies the EquivSizing Flag
+    ! Using an equivalent slab allows non-rectangular shapes to be
+    !    modeled accurately.
+    ! The simulation default should be EquivSizing = True
+   N1, \field APRatio: The area to perimeter ratio for this slab
+       \ units m
+   A1; \field EquivSizing: Flag
+         \note Will the dimensions of an equivalent slab be calculated (TRUE)
+         \note or will the dimensions be input directly? (FALSE)]
+         \note Only advanced special simulations should use FALSE.
+\end{lstlisting}
+
+\begin{lstlisting}
+EquivAutoGrid,
+     \memo EquivAutoGrid necessary when EquivSizing = TRUE, TRUE is is the normal case.
+       N1, \field CLEARANCE: Distance from outside of wall to edge of 3-D ground domain
+         \units m
+         \note typical value 15m
+       N2, \field SlabDepth: Thickness of the floor slab
+         \units m
+         \note typical value 0.1m
+       N3; \field BaseDepth: Depth of the basement wall below grade
+         \units m
+\end{lstlisting}
+
+\begin{lstlisting}
+!
+! ******** The following input objects are required only for special cases.
+!
+\end{lstlisting}
+
+\begin{lstlisting}
+AutoGrid,   ! NOTE: AutoGrid only necessary when EquivSizing is false
+! If the modelled building is not a rectangle or square, Equivalent
+! sizing MUST be used to get accurate results
+       N1, \field CLEARANCE: Distance from outside of wall to edge, 15m]
+       N2, \field SLABX: X dimension of the building slab, 0-60.0 m]
+       N3, \field SLABY: Y dimension of the building slab, 0-60.0 m]
+       N4, \field ConcAGHeight: Height of the fndn wall above grade, m]
+       N5, \field SlabDepth: Thickness of the floor slab, m, 0.1]
+       N6; \field BaseDepth: Depth of the basement wall below grade, m]
+\end{lstlisting}
+
+\begin{lstlisting}
+ManualGrid, ! NOTE: Manual Grid only necessary using manual gridding
+!  (not recommended)
+       N1, \field NX: Number of cells in the X direction: 20]
+       N2, \field NY: Number of cells in the Y direction: 20]
+       N3, \field NZAG: Number of cells in the Z direction
+!              above grade: 4 Always]
+       N4, \field NZBG: Number of cells in Z dir. below grade: 10-35]
+       N5, \field IBASE: X direction cell indicator of slab edge: 5-20]
+       N6, \field JBASE: Y direction cell indicator of slab edge: 5-20]
+       N7; \field KBASE: Z direction cell indicator
+!              of the top of the floor slab: 5-20]
+\end{lstlisting}
+
+\begin{lstlisting}
+XFACE,       ! NOTE: This is only needed when using manual gridding
+!  (not recommended)
+!       [XFACE: X Direction cell face coordinates: m]
+       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
+       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
+       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
+       N39, N40, N41, N42, N43, N44;
+\end{lstlisting}
+
+\begin{lstlisting}
+YFACE,  !NOTE: This is only needed when using manual gridding
+!  (not recommended)
+!       [YFACE: Y Direction cell face coordinates: m],
+       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
+       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
+       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
+       N39, N40, N41, N42, N43, N44;
+\end{lstlisting}
+
+\begin{lstlisting}
+ZFACE,  !NOTE: This is only needed when using manual gridding
+!  (not recommended)
+!       [ZFACE: Z Direction cell face coordinates: m]
+       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
+       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
+       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
+      N39, N40;
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/use-of-the-ground-temperatures-with-slabs.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/use-of-the-ground-temperatures-with-slabs.tex
new file mode 100644
index 00000000000..f81c21bbe0d
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/use-of-the-ground-temperatures-with-slabs.tex
@@ -0,0 +1,163 @@
+\section{Caution}\label{caution}
+
+For ground-contact surfaces in EnergyPlus, it is important to specify appropriate ground temperatures. Do not use the ``undisturbed'' ground temperatures from the weather data. These values are too extreme for the soil under a conditioned building. For best results, use the Slab or Basement program described in this section to calculate custom monthly average ground temperatures. This is especially important for residential applications and very small buildings. If one of these ground temperature preprocessors is not used, for typical commercial buildings in the USA, a reasonable default value is 2C less than the average indoor space temperature.
+
+\section{Introduction}\label{introduction-003}
+
+There are two difficulties behind linking ground heat transfer calculations to EnergyPlus. One is the fact that the conduction calculations in EnergyPlus (and in DOE-2 and BLAST previously) are one-dimensional and the ground heat transfer calculations are two or three-dimensional. This causes severe modeling problems irrespective of the methods being used for the ground heat transfer calculation. The other difficulty is the markedly different time scales involved in the processes. Basically, the zone model is on an hour scale and the ground heat transfer is on a monthly time scale. The basic heat balance based zone model of EnergyPlus has to be considered as the foundation for building energy simulation at the present time and for some time in the future. Thus, it is necessary to be able to relate ground heat transfer calculations to that model.
+
+The heat balance zone model considers a single room or thermal zone in a building and performs a heat balance on it. A fundamental modeling assumption is that the faces of the enclosure are isothermal planes. A ground heat transfer calculation usually considers an entire building and the earth that surrounds it, resulting in non-isothermal face planes where there is ground contact. While it is not impossible to imagine multi-zone, whole building models that include the surrounding earth and non-isothermal building surfaces, such models will not be practical for some time in the future, and their usefulness even then is not clear.
+
+The EnergyPlus development team addressed the problem and decided that the most reasonable first step would be to partially decouple the ground heat transfer calculation from the thermal zone calculation. The most important parameter for the zone calculation is the outside face temperature of the building surface that is in contact with the ground. Thus this becomes a reasonable ``separation plane'' for the two calculations. It was further decided that the current usage of monthly average ground temperature was reasonable for this separation plane temperature as well, since the time scales of the building heat transfer processes are so much shorter than those of the ground heat transfer processes.
+
+Using the separation plane premise, the 3D ground heat transfer programs for slabs developed by Bahnfleth (1989, 1990) were modified by Clements (2004) to produce outside face temperatures. EnergyPlus permits separate monthly average inside temperatures as input. The program produces outside face temperatures for the core area and the perimeter area of the slab. It is described in the section ``Use of the Ground Temperatures with Slabs'' below.
+
+A 3D basement program also is included with EnergyPlus. This is described below in Using Ground Temperatures with Basements. It uses the same principle as the slab procedure; it determines the outside face (surface) temperature of the walls and floor of a basement in contact with the ground.
+
+It should be noted that either for slabs or basements the ground heat transfer is usually small unless the building is very small or has some special characteristics.
+
+Multiple Ground Temperatures shows how the OtherSideCoefficients object of EnergyPlus can be used to supply multiple ground temperatures.
+
+\section{Use of the Ground Temperatures with Slabs}\label{use-of-the-ground-temperatures-with-slabs}
+
+The Slab program produces temperature profiles for the outside surface at the core and at the perimeter of the slab. It also produces the average based on the perimeter and core areas used in the calculation. This allows the user to apply the Slab temperatures one of two ways in EnergyPlus:
+
+\emph{Option 1 - Core and Perimeter Temperatures}: The EnergyPlus OtherSideCoefficients object can be used to provide two sets of twelve monthly average ground temperature values. In this way, both the perimeter and the core values from the Slab program can be used in the succeeding EnergyPlus run. This method assumes that the floor slab will be described using at least two different heat transfer surfaces. The use of OtherSideCoefficients to provide additional ground contact surfaces is described in detail in the ``Multiple Ground Temperatures'' section below.
+
+\emph{Option 2 - Average Temperatures:} Use the monthly average temperatures produced by the Slab program in the EnergyPlus GroundTemperatures object. This will provide an average ground temperature at the outside face of any heat transfer surface whose OutsideFaceEnvironment field is set to ``ground''.
+
+EnergyPlus accepts twelve separate monthly average inside temperatures. In addition, it is possible to add an hourly sinusoidal variation of the inside temperature with a 24 hour period sine function. This was included to show the effect of something such as night setback on the face temperature. Generally, the effect is quite small.
+
+First the results for a monthly specified constant average inside temperature. The location is Minneapolis, and the slab is insulated.
+
+\begin{lstlisting}
+Monthly Slab Outside Face Temperatures, C
+Perimeter Area: 304.00  Core Area: 1296.00
+Month   Average   Perimeter    Core      Inside
+1      17.67     16.11      18.03       18.0
+2      17.45     15.92      17.81       18.0
+3      17.43     16.07      17.74       18.0
+4      19.00     17.82      19.27       20.0
+5      19.24     18.23      19.48       20.0
+6      19.31     18.42      19.52       20.0
+7      20.92     20.14      21.11       22.0
+8      21.17     20.44      21.35       22.0
+9      21.22     20.45      21.40       22.0
+10      21.21     20.26      21.44       22.0
+11      19.62     18.54      19.88       20.0
+12      19.35     17.99      19.67       20.0
+\end{lstlisting}
+
+The resulting heat flux is shown below. The inside heat transfer coefficient and slab thermal properties are specified in the input file. For this example the total thermal resistance from the inside air to the slab bottom surface was 0.27 (m\(^{2}\) C)/W. This value is controlled by the user with the inside heat transfer coefficient and slab thermal properties values in the slab program input file.
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+Month & Average & Perimeter & Core & Inside & Perimeter Heat Flux W/m & Average Heat Flux W/m \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Month & Average & Perimeter & Core & Inside & Perimeter Heat Flux W/m & Average Heat Flux W/m \tabularnewline
+\midrule
+\endhead
+
+1 & 17.51 & 16.03 & 17.86 & 18 & 7.30 & 1.81 \tabularnewline
+2 & 17.29 & 15.85 & 17.63 & 18 & 7.96 & 2.63 \tabularnewline
+3 & 17.27 & 16 & 17.57 & 18 & 7.41 & 2.70 \tabularnewline
+4 & 18.87 & 17.77 & 19.13 & 20 & 8.26 & 4.19 \tabularnewline
+5 & 19.11 & 18.16 & 19.34 & 20 & 6.81 & 3.30 \tabularnewline
+6 & 19.17 & 18.34 & 19.37 & 20 & 6.15 & 3.07 \tabularnewline
+7 & 20.81 & 20.07 & 20.98 & 22 & 7.15 & 4.41 \tabularnewline
+8 & 21.05 & 20.36 & 21.21 & 22 & 6.07 & 3.52 \tabularnewline
+9 & 21.09 & 20.38 & 21.26 & 22 & 6.00 & 3.37 \tabularnewline
+10 & 21.08 & 20.19 & 21.29 & 22 & 6.70 & 3.41 \tabularnewline
+11 & 19.47 & 18.45 & 19.71 & 20 & 5.74 & 1.96 \tabularnewline
+12 & 19.2 & 17.92 & 19.51 & 20 & 7.70 & 2.96 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Then for the same conditions, the results with a 2 degree C amplitude 24-hour sine wave variation. Notice that the inside temperatures are the same since they are monthly averages and the daily variation oscillates about the mean. The core and perimeter slab temperatures are affected slightly.
+
+\begin{lstlisting}
+Monthly Slab Outside Face Temperatures, C
+Perimeter Area: 304.00  Core Area: 1296.00
+Month   Average   Perimeter    Core      Inside
+1      17.51     16.03      17.86       18.0
+2      17.29     15.85      17.63       18.0
+3      17.27     16.00      17.57       18.0
+4      18.87     17.77      19.13       20.0
+5      19.11     18.16      19.34       20.0
+6      19.17     18.34      19.37       20.0
+7      20.81     20.07      20.98       22.0
+8      21.05     20.36      21.21       22.0
+9      21.09     20.38      21.26       22.0
+10      21.08     20.19      21.29       22.0
+11      19.47     18.45      19.71       20.0
+12      19.20     17.92      19.51       20.0
+\end{lstlisting}
+
+An example of a 24-hour inside temperature profile for this case is shown below. The sine wave amplitude was 2 C.
+
+\begin{lstlisting}
+Day       Hour   Perim Out Ts    Core Out Ts    Inside Temp
+1           1   17.30827       19.15832       18.51749
+1           2   17.29503       19.15274       18.99974
+1           3   17.30236       19.16732       19.41389
+1           4   17.32258       19.19376       19.73175
+1           5   17.34834       19.22526       19.93166
+1           6   17.37288       19.25529       20.00000
+1           7   17.39023       19.27798       19.93212
+1           8   17.39544       19.28838       19.73265
+1           9   17.38485       19.28117       19.41517
+1          10   17.35602       19.24733       19.00130
+1          11   17.30590       19.18686       18.51924
+1          12   17.23507       19.10210       18.00180
+1          13   17.14650       18.99703       17.48425
+1          14   17.04291       18.87713       17.00183
+1          15   16.92873       18.74895       16.58738
+1          16   16.81076       18.61963       16.26915
+1          17   16.69609       18.49656       16.06881
+1          18   16.59243       18.38671       16.00000
+1          19   16.50669       18.29626       16.06741
+1          20   16.44276       18.23010       16.26645
+1          21   16.40369       18.19161       16.58356
+1          22   16.38873       18.18218       16.99714
+1          23   16.39435       18.19834       17.47902
+1          24   16.41942       18.23298       17.99639
+\end{lstlisting}
+
+A plot of the daily profiles is shown below. Note that the inside temperature change of 4 C produces only a small change in the slab lower face temperature.
+
+\begin{figure}[hbtp] % fig 19
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image017.jpg}
+\caption{Daily Temperature Profiles (Slab) \protect \label{fig:daily-temperature-profiles-slab}}
+\end{figure}
+
+The resulting heat fluxes are shown below. They can be compared with the fluxes shown above for the constant inside temperature run. The changes resulting from a fairly large 4 C daily temperature variation are probably not significant.
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+Month & Average & Perimeter & Core & Inside & Perimeter Heat Flux W/m & Average Heat Flux W/m \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Month & Average & Perimeter & Core & Inside & Perimeter Heat Flux W/m & Average Heat Flux W/m \tabularnewline
+\midrule
+\endhead
+
+1 & 17.51 & 16.03 & 17.86 & 18 & 7.30 & 1.81 \tabularnewline
+2 & 17.29 & 15.85 & 17.63 & 18 & 7.96 & 2.63 \tabularnewline
+3 & 17.27 & 16 & 17.57 & 18 & 7.41 & 2.70 \tabularnewline
+4 & 18.87 & 17.77 & 19.13 & 20 & 8.26 & 4.19 \tabularnewline
+5 & 19.11 & 18.16 & 19.34 & 20 & 6.81 & 3.30 \tabularnewline
+6 & 19.17 & 18.34 & 19.37 & 20 & 6.15 & 3.07 \tabularnewline
+7 & 20.81 & 20.07 & 20.98 & 22 & 7.15 & 4.41 \tabularnewline
+8 & 21.05 & 20.36 & 21.21 & 22 & 6.07 & 3.52 \tabularnewline
+9 & 21.09 & 20.38 & 21.26 & 22 & 6.00 & 3.37 \tabularnewline
+10 & 21.08 & 20.19 & 21.29 & 22 & 6.70 & 3.41 \tabularnewline
+11 & 19.47 & 18.45 & 19.71 & 20 & 5.74 & 1.96 \tabularnewline
+12 & 19.2 & 17.92 & 19.51 & 20 & 7.70 & 2.96 \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/using-ground-temperatures-with-basements.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/using-ground-temperatures-with-basements.tex
new file mode 100644
index 00000000000..0aab88d7800
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/using-ground-temperatures-with-basements.tex
@@ -0,0 +1,23 @@
+\section{Using Ground Temperatures with Basements}\label{using-ground-temperatures-with-basements}
+
+The basement routine is used to calculate the face (surface) temperatures on the outside of the basement wall or the floor slab. This is the plane between the outside insulation and the basement wall. The insulation thermal resistance can range from zero (no insulation) to any reasonable value. The units are K/(W/m\(^{2}\)). The program will simulate two conditions: full insulation from grade to the footing or half insulation that extends halfway down from grade to footing. The temperature on this plane is used with the OtherSideCoefficients object in EnergyPlus to supply the outside face temperature of the walls or slab.
+
+\begin{figure}[hbtp] % fig 22
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image020.jpg}
+\caption{Basement Configuration \protect \label{fig:basement-configuration}}
+\end{figure}
+
+The output from the program is a csv file, named MonthlyResults.csv, as shown below.
+
+\begin{figure}[hbtp] % fig 23
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image021.jpg}
+\caption{Output from Basement program \protect \label{fig:output-from-basement-program}}
+\end{figure}
+
+Column B gives the basement zone temperature. This can vary month by month as will be explained later. Column C is the monthly average wall outside face temperature, as shown in the diagram above. Column D is the corresponding average monthly average inside wall face temperature. Columns E and F contain the same information for the basement floor slab. Columns G-J contain the same information for the upper half and the lower half of the basement walls.
+
+Columns K through N contain the monthly average heat flux for the floor, the walls, the upper half of the walls and the lower half of the walls. The flux is reported in units of W/m\(^{2}\).
+
+The program also produces an output file named EPObjects.TXT. This file contains the necessary idf objects to make it easy to include the wall outside surface temperatures in an EnergyPlus input file. Idf objects for all of the temperatures in the output file shown above are included. These objects are explained in detail in the section Using the Interface Surface Temperature Results in EnergyPlus.
diff --git a/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/using-the-interface-surface-temperature.tex b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/using-the-interface-surface-temperature.tex
new file mode 100644
index 00000000000..32beea95d69
--- /dev/null
+++ b/doc/auxiliary-programs/src/ground-heat-transfer-in-energyplus/using-the-interface-surface-temperature.tex
@@ -0,0 +1,190 @@
+\section{Using the Interface Surface Temperature Results in EnergyPlus}\label{using-the-interface-surface-temperature-results-in-energyplus}
+
+If the objects are placed in the normal EnergyPlus input IDF file using the ``GroundHeatTransfer:Basement:'' prefix, then the values resulting from the Basement preprocessor will be automatically included in the simulation at run time. The surfaces can reference these values using Outside Boundary Conditions of:
+
+\begin{itemize}
+\item
+  GroundBasementPreprocessorAverageWall
+\item
+  GroundBasementPreprocessorAverageFloor
+\item
+  GroundBasementPreprocessorUpperWall
+\item
+  GroundBasementPreprocessorLowerWall
+\end{itemize}
+
+The objects that support this include:
+
+\begin{itemize}
+\item
+  BuildingSurface:Detailed
+\item
+  Wall:Detailed
+\item
+  RoofCeiling:Detailed
+\item
+  Floor:Detailed
+\end{itemize}
+
+The monthly results from the basement program are used with the SurfaceProperty:OtherSideCoefficients object in EnergyPlus. The idd corresponding to that object is shown below. The two applicable fields are N2 and A2. N2 should have the value 1.0. It will be modified by a schedule that is named in A2, and that temperature will be used on the outside of the surface specified as having the OtherSideCoeffcients named in A1.
+
+\begin{lstlisting}
+
+SurfaceProperty:OtherSideCoefficients,
+  \memo This object sets the other side conditions for a surface in a variety of ways.
+  \min-fields 8
+  A1, \field Name
+  \required-field
+  \reference OSCNames
+  \reference OutFaceEnvNames
+  N1, \field Combined Convective/Radiative Film Coefficient
+  \required-field
+  \type real
+  \note if>0, this field becomes the exterior convective/radiative film coefficient
+  \note and the other fields are used to calculate the outdoor air temperature
+  \note then exterior surface temperature based on outdoor air and specified coefficient
+  \note if< = 0, then remaining fields calculate the outside surface temperature
+  \note following fields are used in the equation:
+  \note SurfTemp = N7*TempZone + N4*OutdoorDry-bulb + N2*N3 + GroundTemp*N5 + WindSpeed*N6*OutdoorDry-bulb
+  N2, \field Constant Temperature
+  \units C
+  \type real
+  \default 0
+  \note This parameter will be overwritten by the values from the Constant Temperature Schedule Name (below) if one is present
+  N3, \field Constant Temperature Coefficient
+  \note This coefficient is used even with a Schedule.  It should normally be 1.0 in that case
+  \default 1
+  N4, \field External Dry-Bulb Temperature Coefficient
+  \type real
+  \default 0
+  N5, \field Ground Temperature Coefficient
+  \type real
+  \default 0
+  N6, \field Wind Speed Coefficient
+  \type real
+  \default 0
+  N7, \field Zone Air Temperature Coefficient
+  \type real
+  \default 0
+  A2; \field Constant Temperature Schedule Name
+  \note Name of schedule for values of constant temperature.
+  \note Schedule values replace any value specified in the field Constant Temperature.
+  \type object-list
+  \object-list ScheduleNames
+\end{lstlisting}
+
+A sample idf for this object is shown below.
+
+\begin{lstlisting}
+
+SurfaceProperty:OtherSideCoefficients, OSCCoef:Zn005:Wall003, !- OSC Name
+  !  Example input for second ground temperature
+  0.0000000E+00,    !- OSC SurfFilmCoef
+  0.000000    ,    !- OSC Temp
+  1.000000    ,    !- OSC Temp Coef
+  0.000000    ,    !- OSC dry-bulb
+  0.000000    ,    !- OSC GrndTemp
+  0.000000    ,    !- OSC WindSpdCoeff
+  0.000000    ,    !- OSC ZoneAirTemp
+  GroundTempSched;  !  Name of schedule defining additional ground temperature.
+\end{lstlisting}
+
+The OSC object can be repeated for as many outside temperatures as needed. A more detailed explanation of how to use this object is contained in the next section, and an example object is output by the program in the file EPObjects.txt.
+
+\subsection{Multiple Ground Temperatures}\label{multiple-ground-temperatures}
+
+These three objects show how the OtherSideCoefficients object can be used to provide extra ground temperatures for surfaces exposed to different ground temperatures.
+
+Here is the surface description. Note that the OutsideFaceEnvironment is specified as OtherSideCoeff.
+
+\begin{lstlisting}
+
+BuildingSurface:Detailed,
+  OSCTest:South Wall,      !- User Supplied Surface Name
+  Wall,                    !- Surface Type
+  Exterior,                !- Construction Name of the Surface
+  OSCTest,                 !- Zone
+  OtherSideCoefficients,   !- Outside Boundary Condition
+  ExampleOSC,              !- Outside Boundary Condition Object
+  NoSun  ,                 !- Sun Exposure
+  NoWind  ,                !- Wind Exposure
+  0.5,                     !- View Factor to Ground
+  4,                       !- Number of Vertices
+  0,0,0,                   !- Vertex 1 X,Y,Z-coordinates {m}
+  6.096,0,0,               !- Vertex 2 X,Y,Z-coordinates {m}
+  6.096,0,4.572,           !- Vertex 3 X,Y,Z-coordinates {m}
+  0,0,4.572;               !- Vertex 4 X,Y,Z-coordinates {m}
+\end{lstlisting}
+
+The OtherSideCoefficients object has to supply the basic form of the environment. Note that the name corresponds to thee name in the Surface object. This object also supplies the name of a schedule that will provide the monthly ground temperature values.
+
+\begin{lstlisting}
+
+SurfaceProperty:OtherSideCoefficients,
+  ExampleOSC,              !- OtherSideCoeff Name
+  0,                       !- Combined convective/radiative film coefficient
+  1,                       !- User selected Constant Temperature {C}
+  1,                       !- Coefficient modifying the user selected constant temperature
+  0,                       !- Coefficient modifying the external dry bulb temperature
+  0,                       !- Coefficient modifying the ground temperature
+  0,                       !- Coefficient modifying the wind speed term (s/m)
+  0,                       !- Coefficient modifying the zone air temperature part of the equation
+  GroundTempCompactSched;  !- Schedule Name for values of "const" temperature. Schedule values replace N2.
+\end{lstlisting}
+
+The schedule named in the last field of the OtherSideCoefficients object must be supplied. In compact schedule format it would appear as shown below. Again, objects for each of the surface temperatures are produced by the program and output in the file EPObjects.txt.
+
+\begin{lstlisting}
+
+Schedule:Compact,
+  GroundTempCompactSched,  !- Name
+  Temperature ,            !- ScheduleType
+  Through: 1/31,           !- Complex Field \#1
+  For:AllDays,             !- Complex Field \#2
+  Until: 24:00,            !- Complex Field \#3
+  16,                      !- Complex Field \#4
+  Through: 2/28,           !- Complex Field \#5
+  For:AllDays,             !- Complex Field \#6
+  Until: 24:00,            !- Complex Field \#7
+  17,                      !- Complex Field \#8
+  Through: 3/31,           !- Complex Field \#9
+  For:AllDays,             !- Complex Field \#10
+  Until: 24:00,            !- Complex Field \#11
+  18,                      !- Complex Field \#12
+  Through: 4/30,           !- Complex Field \#13
+  For:AllDays,             !- Complex Field \#14
+  Until: 24:00,            !- Complex Field \#15
+  19,                      !- Complex Field \#16
+  Through: 5/31,           !- Complex Field \#17
+  For:AllDays,             !- Complex Field \#18
+  Until: 24:00,            !- Complex Field \#19
+  20,                      !- Complex Field \#20
+  Through: 6/30,           !- Complex Field \#21
+  For:AllDays,             !- Complex Field \#22
+  Until: 24:00,            !- Complex Field \#23
+  20,                      !- Complex Field \#24
+  Through: 7/31,           !- Complex Field \#25
+  For:AllDays,             !- Complex Field \#26
+  Until: 24:00,            !- Complex Field \#27
+  20,                      !- Complex Field \#28
+  Through: 8/31,           !- Complex Field \#29
+  For:AllDays,             !- Complex Field \#30
+  Until: 24:00,            !- Complex Field \#31
+  19,                      !- Complex Field \#32
+  Through: 9/30,           !- Complex Field \#33
+  For:AllDays,             !- Complex Field \#34
+  Until: 24:00,            !- Complex Field \#35
+  18,                      !- Complex Field \#36
+  Through: 10/31,          !- Complex Field \#37
+  For:AllDays,             !- Complex Field \#38
+  Until: 24:00,            !- Complex Field \#39
+  17,                      !- Complex Field \#40
+  Through: 11/30,          !- Complex Field \#41
+  For:AllDays,             !- Complex Field \#42
+  Until: 24:00,            !- Complex Field \#43
+  16,                      !- Complex Field \#44
+  Through: 12/31,          !- Complex Field \#45
+  For:AllDays,             !- Complex Field \#46
+  Until: 24:00,            !- Complex Field \#47
+  16;                      !- Complex Field \#48
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/hvac-diagram.tex b/doc/auxiliary-programs/src/hvac-diagram.tex
new file mode 100644
index 00000000000..3917d60c259
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-diagram.tex
@@ -0,0 +1 @@
+\chapter{HVAC Diagram}\label{hvac-diagram}
diff --git a/doc/auxiliary-programs/src/hvac-diagram/introduction-002.tex b/doc/auxiliary-programs/src/hvac-diagram/introduction-002.tex
new file mode 100644
index 00000000000..19ca26b8b98
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-diagram/introduction-002.tex
@@ -0,0 +1,197 @@
+\section{Introduction}\label{introduction-000}
+
+The HVAC-Diagram program is a simple utility that can be used to generate a svg file based on the bnd file generated by EnergyPlus. It is a stored in the primary EnergyPlus\textbackslash{}PostProcessor folder upon installation.
+
+It creates a series of diagrams for the layout of the HVAC system components. The SVG file can be viewed with a number of internet browser plug-ins such as produced by Adobe that can be downloaded at \href{http://www.adobe.com/svg}{www.adobe.com/svg}. To get help within the Adobe viewer, right click anywhere on the drawing.
+
+Each diagram should be read from left to right, which is the direction of the flow of the fluid through the components.
+
+The HVAC-Diagram program is automatically called when using EP-Launch but can also be included in other batch files. To view the drawing in EP-Launch, click on the drawing button. You can zoom in on this drawing and with the ``copy'' command, paste a zoomed in portion as a bitmap in your document.
+
+\begin{figure}[hbtp] % fig 32
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image030.jpg}
+\caption{HVAC Diagram -- SVG Drawing \protect \label{fig:hvac-diagram-svg-drawing}}
+\end{figure}
+
+Objects that are recognized by the HVAC diagram are shown in Table~\ref{table:hvac-diagram-object-names-primary-sort-colors} (sorted by Object Name) and Table~\ref{table:hvac-diagram-object-names-and-color-primary} (sorted by color).
+
+% table 30
+\begin{longtable}[c]{@{}ll@{}}
+\caption{HVAC Diagram Object Names (primary sort) Colors \label{table:hvac-diagram-object-names-primary-sort-colors}} \tabularnewline
+\toprule 
+Object Name & Color \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{HVAC Diagram Object Names (primary sort) Colors} \tabularnewline
+\toprule 
+Object Name & Color \tabularnewline
+\midrule
+\endhead
+
+AirLoopHVAC:ReturnPlenum & lightgreen \tabularnewline
+AirLoopHVAC:SupplyPlenum & lightgreen \tabularnewline
+AirLoopHVAC:ZoneMixer & wheat \tabularnewline
+AirLoopHVAC:ZoneSplitter & wheat \tabularnewline
+AirTerminal:DualDuct:ConstantVolume & wheat \tabularnewline
+AirTerminal:DualDuct:VAV & wheat \tabularnewline
+AirTerminal:SingleDuct:Uncontrolled & none \tabularnewline
+AirTerminal:SingleDuct:VAV:NoReheat & wheat \tabularnewline
+AirTerminal:SingleDuct:VAV:Reheat & wheat \tabularnewline
+Boiler:HotWater & indianred \tabularnewline
+Chiller:Absorption & powderblue \tabularnewline
+Chiller:CombustionTurbine & powderblue \tabularnewline
+Chiller:ConstantCOP & powderblue \tabularnewline
+Chiller:Electric & powderblue \tabularnewline
+Chiller:EngineDriven & powderblue \tabularnewline
+ChillerHeater:Absorption:DirectFired & powderblue \tabularnewline
+Coil:Cooling:DX:MultiSpeed & skyblue \tabularnewline
+Coil:Cooling:DX:SingleSpeed & skyblue \tabularnewline
+Coil:Cooling:Water & skyblue \tabularnewline
+Coil:Cooling:Water:DetailedGeometry & skyblue \tabularnewline
+Coil:Cooling:WaterToAirHeatPump:EquationFit & skyblue \tabularnewline
+Coil:Cooling:WaterToAirHeatPump:ParameterEstimation & skyblue \tabularnewline
+Coil:Heating:DX:SingleSpeed & skyblue \tabularnewline
+Coil:Heating:Electric & salmon \tabularnewline
+Coil:Heating:Gas & salmon \tabularnewline
+Coil:Heating:Water & salmon \tabularnewline
+Coil:Heating:WaterToAirHeatPump:EquationFit & salmon \tabularnewline
+Coil:Heating:WaterToAirHeatPump:ParameterEstimation & salmon \tabularnewline
+Connector:Mixer & lightgreen \tabularnewline
+Connector:Splitter & wheat \tabularnewline
+Controller:OutdoorAir & none \tabularnewline
+Controller:WaterCoil & none \tabularnewline
+CoolingTower:SingleSpeed & pink \tabularnewline
+Dehumidifier:Desiccant:NoFans & tan \tabularnewline
+DistrictCooling & none \tabularnewline
+DistrictHeating & none \tabularnewline
+EvaporativeCooler:Direct:CelDekPad & aliceblue \tabularnewline
+EvaporativeCooler:Indirect:CelDekPad & aliceblue \tabularnewline
+EvaporativeCooler:Indirect:ResearchSpecial & aliceblue \tabularnewline
+Fan:ConstantVolume & silver \tabularnewline
+Fan:OnOff & silver \tabularnewline
+Fan:VariableVolume & silver \tabularnewline
+Fan:ZoneExhaust & silver \tabularnewline
+Generator:CombustionTurbine & orange \tabularnewline
+Generator:InternalCombustionEngine & orange \tabularnewline
+GroundHeatExchanger:Pond & paleturquoise \tabularnewline
+GroundHeatExchanger:Surface & paleturquoise \tabularnewline
+GroundHeatExchanger:Vertical & paleturquoise \tabularnewline
+HeatExchanger:AirToAir:FlatPlate & paleturquoise \tabularnewline
+HeatExchanger:AirToAir:SensibleAndLatent & paleturquoise \tabularnewline
+HeatExchanger:Hydronic & paleturquoise \tabularnewline
+HeatPump:WaterToWater:EquationFit:Cooling & lightslategray \tabularnewline
+HeatPump:WaterToWater:EquationFit:Heating & lightslategray \tabularnewline
+HeatPump:WaterToWater:ParameterEstimation:Cooling & lightslategray \tabularnewline
+HeatPump:WaterToWater:ParameterEstimation:Heating & lightslategray \tabularnewline
+Humidifier:Steam:Electric & lavender \tabularnewline
+LoadProfile:Plant & none \tabularnewline
+OutdoorAir:Mixer & lawngreen \tabularnewline
+OutdoorAir:NodeList & none \tabularnewline
+Pipe:Adiabatic & wheat \tabularnewline
+PlantLoopConnection & wheat \tabularnewline
+Pump:ConstantSpeed & springgreen \tabularnewline
+Pump:VariableSpeed & springgreen \tabularnewline
+SolarCollector:FlatPlate:Water & yellow \tabularnewline
+WaterHeater:Mixed & orange \tabularnewline
+WaterHeater:Stratified & orange \tabularnewline
+ZoneHVAC:Baseboard:Convective:Water & salmon \tabularnewline
+ZoneHVAC:EnergyRecoveryVentilator:Controller & none \tabularnewline
+ZoneHVAC:EquipmentConnections & chartreuse \tabularnewline
+ZoneHVAC:IdealLoadsAirSystem & none \tabularnewline
+ZoneHVAC:LowTemperatureRadiant:ConstantFlow & orangered \tabularnewline
+ZoneHVAC:LowTemperatureRadiant:VariableFlow & orangered \tabularnewline
+ZoneHVAC:UnitVentilator & sandybrown \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 31
+\begin{longtable}[c]{@{}ll@{}}
+\caption{HVAC Diagram Object Names and Color (primary sort) \label{table:hvac-diagram-object-names-and-color-primary}} \tabularnewline
+\toprule 
+Object Name & Color \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{HVAC Diagram Object Names and Color (primary sort)} \tabularnewline
+\toprule 
+Object Name & Color \tabularnewline
+\midrule
+\endhead
+
+EvaporativeCooler:Direct:CelDekPad & aliceblue \tabularnewline
+EvaporativeCooler:Indirect:CelDekPad & aliceblue \tabularnewline
+EvaporativeCooler:Indirect:ResearchSpecial & aliceblue \tabularnewline
+ZoneHVAC:EquipmentConnections & chartreuse \tabularnewline
+Boiler:HotWater & indianred \tabularnewline
+Humidifier:Steam:Electric & lavender \tabularnewline
+OutdoorAir:Mixer & lawngreen \tabularnewline
+AirLoopHVAC:ReturnPlenum & lightgreen \tabularnewline
+AirLoopHVAC:SupplyPlenum & lightgreen \tabularnewline
+Connector:Mixer & lightgreen \tabularnewline
+HeatPump:WaterToWater:EquationFit:Cooling & lightslategray \tabularnewline
+HeatPump:WaterToWater:EquationFit:Heating & lightslategray \tabularnewline
+HeatPump:WaterToWater:ParameterEstimation:Cooling & lightslategray \tabularnewline
+HeatPump:WaterToWater:ParameterEstimation:Heating & lightslategray \tabularnewline
+AirTerminal:SingleDuct:Uncontrolled & none \tabularnewline
+Controller:OutdoorAir & none \tabularnewline
+Controller:WaterCoil & none \tabularnewline
+DistrictCooling & none \tabularnewline
+DistrictHeating & none \tabularnewline
+LoadProfile:Plant & none \tabularnewline
+OutdoorAir:NodeList & none \tabularnewline
+ZoneHVAC:EnergyRecoveryVentilator:Controller & none \tabularnewline
+ZoneHVAC:IdealLoadsAirSystem & none \tabularnewline
+Generator:CombustionTurbine & orange \tabularnewline
+Generator:InternalCombustionEngine & orange \tabularnewline
+WaterHeater:Mixed & orange \tabularnewline
+WaterHeater:Stratified & orange \tabularnewline
+ZoneHVAC:LowTemperatureRadiant:ConstantFlow & orangered \tabularnewline
+ZoneHVAC:LowTemperatureRadiant:VariableFlow & orangered \tabularnewline
+GroundHeatExchanger:Pond & paleturquoise \tabularnewline
+GroundHeatExchanger:Surface & paleturquoise \tabularnewline
+GroundHeatExchanger:Vertical & paleturquoise \tabularnewline
+HeatExchanger:AirToAir:FlatPlate & paleturquoise \tabularnewline
+HeatExchanger:AirToAir:SensibleAndLatent & paleturquoise \tabularnewline
+HeatExchanger:Hydronic & paleturquoise \tabularnewline
+CoolingTower:SingleSpeed & pink \tabularnewline
+Chiller:Absorption & powderblue \tabularnewline
+Chiller:CombustionTurbine & powderblue \tabularnewline
+Chiller:ConstantCOP & powderblue \tabularnewline
+Chiller:Electric & powderblue \tabularnewline
+Chiller:EngineDriven & powderblue \tabularnewline
+ChillerHeater:Absorption:DirectFired & powderblue \tabularnewline
+Coil:Heating:Electric & salmon \tabularnewline
+Coil:Heating:Gas & salmon \tabularnewline
+Coil:Heating:Water & salmon \tabularnewline
+Coil:Heating:WaterToAirHeatPump:EquationFit & salmon \tabularnewline
+Coil:Heating:WaterToAirHeatPump:ParameterEstimation & salmon \tabularnewline
+ZoneHVAC:Baseboard:Convective:Water & salmon \tabularnewline
+ZoneHVAC:UnitVentilator & sandybrown \tabularnewline
+Fan:ConstantVolume & silver \tabularnewline
+Fan:OnOff & silver \tabularnewline
+Fan:VariableVolume & silver \tabularnewline
+Fan:ZoneExhaust & silver \tabularnewline
+Coil:Cooling:DX:MultiSpeed & skyblue \tabularnewline
+Coil:Cooling:DX:SingleSpeed & skyblue \tabularnewline
+Coil:Cooling:Water & skyblue \tabularnewline
+Coil:Cooling:Water:DetailedGeometry & skyblue \tabularnewline
+Coil:Cooling:WaterToAirHeatPump:EquationFit & skyblue \tabularnewline
+Coil:Cooling:WaterToAirHeatPump:ParameterEstimation & skyblue \tabularnewline
+Coil:Heating:DX:SingleSpeed & skyblue \tabularnewline
+Pump:ConstantSpeed & springgreen \tabularnewline
+Pump:VariableSpeed & springgreen \tabularnewline
+Dehumidifier:Desiccant:NoFans & tan \tabularnewline
+AirLoopHVAC:ZoneMixer & wheat \tabularnewline
+AirLoopHVAC:ZoneSplitter & wheat \tabularnewline
+AirTerminal:DualDuct:ConstantVolume & wheat \tabularnewline
+AirTerminal:DualDuct:VAV & wheat \tabularnewline
+AirTerminal:SingleDuct:VAV:NoReheat & wheat \tabularnewline
+AirTerminal:SingleDuct:VAV:Reheat & wheat \tabularnewline
+Connector:Splitter & wheat \tabularnewline
+Pipe:Adiabatic & wheat \tabularnewline
+PlantLoopConnection & wheat \tabularnewline
+SolarCollector:FlatPlate:Water & yellow \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool.tex b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool.tex
new file mode 100644
index 00000000000..0a60835d9a9
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool.tex
@@ -0,0 +1 @@
+\chapter{HVAC Performance Curve Fit Tool}\label{hvac-performance-curve-fit-tool}
diff --git a/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/error-message.tex b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/error-message.tex
new file mode 100644
index 00000000000..9b9ad73b4dc
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/error-message.tex
@@ -0,0 +1,3 @@
+\section{Error Message}\label{error-message}
+
+Reports progress of the curve object generation calculation starting from reading input data to error massage output file ``errorCurveObjects.txt''. This error message file provides information whether the tool run successfully or not. Also points to the step where problem occurred.
diff --git a/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/inputs.tex b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/inputs.tex
new file mode 100644
index 00000000000..85893ae0066
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/inputs.tex
@@ -0,0 +1,31 @@
+\section{Inputs}\label{inputs}
+
+First step in curve generation is to select appropriate parameters from the dropdown menu. These inputs define the DX Coil Type, Curve Type, Independent Variable and the Units type. The choices available for each input parameters are described in the following table. Once these input parameters are selected the tool read in the values and automatically populates labels for each of the independent and dependent variables. The labels guide users to enter the data for each variable in the corresponding worksheet input range. Two sets of input data are required for curve generation: Rated, and Performance Data.
+
+\begin{longtable}{p{2in}|p{4in}}
+
+\toprule
+Input Parameter & Input Description \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule
+Input Parameter & Input Description \tabularnewline
+\midrule
+\endhead 
+DX Coil Type & \emph{Cooling}: Applicable for DX cooling coil single speed; 
+               \emph{Heating}: Applicable for DX heating coil single speed; 
+               \emph{Other}: Applicable for any equipment that use the three curve types
+\tabularnewline
+Independent Variables & Temperature and Flow 
+\tabularnewline
+Curve Types & \emph{Biquadratic}: Capacity and EIR as a function of temperature;
+              \emph{Cubic}: Capacity and EIR as a function of flow fraction or temperature;
+              \emph{Quadratic}: Capacity and EIR as a function of flow fraction
+\tabularnewline
+Units & \emph{IP}: Temperature in °F, Capacity in kBtu/h, Power in kW, and Flow in CFM;
+        \emph{SI}: Temperature in °C, Capacity in kW, Power in kW, and Flow in m/s 
+\tabularnewline
+Curve Object Name & This input is optional. This string is appended to the default curve object name, or if left blank the default curve object name will be displayed. A curve object is named is created by concatenation as follows: (User-specified curve object name) + ``DXCoilType'' + one of: [``CAPFTEMP'', ``CAPFFF'', ``EIRFTEMP'', ``EIRFFF'']\tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/introduction-004.tex b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/introduction-004.tex
new file mode 100644
index 00000000000..1837dd4a4e0
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/introduction-004.tex
@@ -0,0 +1,19 @@
+\section{Introduction}\label{introduction-002}
+
+This auxiliary tool generates HVAC performance curves in EnergyPlus curve object format. For each set of performance data entered, Capacity and EIR performance curves are generated, and these curves are generated either as a function of temperature(s) or flow fraction. The Capacity and EIR of Cooling DX Coils as a function of temperatures require only Biquadratic curve whereas Capacity and EIR of Heating DX Coils may use Biquadratic, Cubic and Quadratic curves. The selection of either of these curves is dependent on availability of performance data. The Capacity and EIR as a function of flow fraction allows either Cubic or Quadratic curve type. The curve types allowed are:
+
+Biquadratic: \(\text{CurveValue} = a_0 + a_1 X + a_2 X^2 + a_3 Y + a_4 Y^2 + a_5 XY\)
+
+Cubic: \(\text{CurveValue} = a_0 + a_1 X + a_2 X^2 + a_3 X^3\)
+
+Quadratic: \(\text{CurveValue} = a_0 + a_1 X + a_2 X^2\)
+
+These performance curves as a function of temperatures are generated for a given set of input data at a given speed. The curves as a function of flow fraction are generated at the rated temperature conditions. The rated test condition is the AHRI standard test condition (AHRI 2003;2007; 2008). The AHRI standard test condition may vary by the equipment type. For multiple speeds or multiple stage DX Coils, different curve sets can be generated by entering a different set of data for each speed or stage at a time. The tool automatically populates the labels for each data inputs variable when users select the Coil Type, Independent Variables, Curve Type, and Units. The curve fit tool interface in Figure~\ref{fig:main-menu-screen-of-the-weather-converter} shows labels selected to generate capacity and EIR biquadratic curves as function of temperatures for DX cooling coil.
+
+\begin{figure}[hbtp] % fig 33
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image034.jpg}
+\caption{Curve Fit Tool Input Interface \protect \label{fig:curve-fit-tool-input-interface}}
+\end{figure}
+
+The tool can be used for Coil:Cooing:DX:SingleSpeed, Coil:Heating:DX:SingleSpeed, Coil:Cooing:DX:TwoSpeed (high and low speed) , CoilPerformance:DX:Cooling (each stage), and any HVAC equipment that use Biquadratic, Cubic or Quadratic curves. To add this flexibility generic input data labels can be populated by selecting ``Other'' for DX Coil Type input field, located in Cell B3 in Figure~\ref{fig:curve-fit-tool-input-interface}.
diff --git a/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/notes.tex b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/notes.tex
new file mode 100644
index 00000000000..756591f3fe0
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/notes.tex
@@ -0,0 +1,3 @@
+\section{Notes}\label{notes}
+
+This tool has been tested on Ubuntu 11 using Libre Office and MS Office Macintosh 2011 machines. But the button for running the macro may not be imported properly on Ubuntu hence users may have to run the tool manually by selecting ``\textbf{ManageCurveFit}'' and ``\textbf{SaveCurveObjToTextFile}'' subroutine from the macro list.
diff --git a/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/outputs.tex b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/outputs.tex
new file mode 100644
index 00000000000..818c453f200
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/outputs.tex
@@ -0,0 +1,52 @@
+\section{Outputs}\label{outputs}
+
+The generated curves are post-processed to make sure that the curve value is 1.0 at the rated condition. The post processing is applied only if the curve value at the rated condition deviates by a value less than or equal to 0.025 and the performance data set contains the rated data set as one the data points. The coefficients of these curves are displayed on the ``OUTPUT'' tab as shown in Figure~\ref{fig:delta-db-trigger-selection}.
+
+\begin{figure}[hbtp] % fig 34
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image036.jpg}
+\caption{Curve Fit Tool Output Interface \protect \label{fig:curve-fit-tool-output-interface}}
+\end{figure}
+
+Besides the curve coefficients, the goodness of curve fit indicator statistical parameters \emph{R\(^{2}\)} is also reported. The \emph{R\(^{2}\)} is the ratio of the sum of the squared deviations of the curve fit values from the mean to the sum of the squared deviations of the original data from the mean. R squared values closer to 1.0 are good. The tool has an option to save the curve objects to an output file by running another macro (SaveCurveObjToTextFile). The option output files and the directory path are specified in the OUPUT tab in cells C2 and C3, respectively, as shown in Figure~\ref{fig:curve-fit-tool-output-interface}. If the output file name and path are left blank, then default names, ``EplusCurveObjects.IDF'' and the local directory where the tool is located are used. The local directory where the tool is located must not have write restriction.
+
+Sample EnergyPlus curve objects output file generated using this auxiliary tool.
+
+\begin{lstlisting}
+
+Curve:Biquadratic,
+  HeatPumpCoolingCAPFTemp,      !- Name
+  1.4248528695,                !- Coefficient1 Constant
+  -0.0554469607,                !- Coefficient2 x
+  0.0027506982,                !- Coefficient3 x**2
+  -0.0017453896,                !- Coefficient4 y
+  -0.0000081,                   !- Coefficient5 y**2
+  -0.0004638975,                !- Coefficient6 x*y
+  13.8888888889,                !- Minimum Value of x
+  22.2222222222,                !- Maximum Value of x
+  29.4444444444,                !- Minimum Value of y
+  46.1111111111,                !- Maximum Value of y
+  0.7875,                       !- Minimum Curve Output
+  1.1725,                       !- Maximum Curve Output
+  Temperature,                  !- Input Unit Type for X
+  Temperature,                  !- Input Unit Type for Y
+  Dimensionless;                !- Output Unit Type
+
+  Curve:Biquadratic,
+  HeatPump1CoolingEIRFTemp,     !- Name
+  0.1566419771,                 !- Coefficient1 Constant
+  0.0522807347,                 !- Coefficient2 x
+  -0.0017986792,                !- Coefficient3 x**2
+  0.009523995,                  !- Coefficient4 y
+  0.0002405903,                 !- Coefficient5 y**2
+  -0.0001781171,                !- Coefficient6 x*y
+  13.8888888889,                !- Minimum Value of x
+  22.2222222222,                !- Maximum Value of x
+  29.4444444444,                !- Minimum Value of y
+  46.1111111111,                !- Maximum Value of y
+  0.8216,                       !- Minimum Curve Output
+  1.3703,                       !- Maximum Curve Output
+  Temperature,                  !- Input Unit Type for X
+  Temperature,                  !- Input Unit Type for Y
+  Dimensionless;                !- Output Unit Type
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/performance-data.tex b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/performance-data.tex
new file mode 100644
index 00000000000..b7adbaef61c
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/performance-data.tex
@@ -0,0 +1,5 @@
+\section{Performance Data}\label{performance-data}
+
+The performance data set entered depends on the type of independent variables selected. To generate performance curves (e.g.~DX Coils) as a function of temperatures require the capacity and power data at various combinations of indoor and outdoor coil entering air temperatures at a rated supply air flow rate. And performance curves (e.g.~DX Coil) as function of flow fraction require capacity and power data at various supply air flow rates and rated indoor and outdoor coil entering air (or water) temperatures. The performance data set may include the rated data as one of the data points. The performance data set is entered starting from row 15 and down for each of the variables as shown in Figure~\ref{fig:curve-fit-tool-input-interface}.
+
+The total cooling and heating capacities must be the gross values, i.e., not corrected for the supply fan heating effect. Also the input power has to exclude the supply air fan power, but includes other miscellaneous power inputs (e.g.~control panel power). If manufacturers provide the total power, then the supply fan power must be deducted from the former. If the capacity and power data are normalized values, then enter 1.0 for rated gross capacity and power in the \textbf{\emph{Rated Data}} input Cells range (B11:E11 in the INPUT tab). Two samples of performance and rated data set are included in the ``\textbf{INSTRUCTION}'' tab.
diff --git a/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/rated-data.tex b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/rated-data.tex
new file mode 100644
index 00000000000..acc4bd14eea
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/rated-data.tex
@@ -0,0 +1,3 @@
+\section{Rated Data}\label{rated-data}
+
+The rated data is used to normalize the performance data set. The rated test conditions depend on the equipment type. For DX cooling coil the rated test temperatures are 67°F (19.4°C) indoor coil entering wet bulb, 80°F (26.7°C) indoor coil entering dry bulb and 95°F (35.0°C) outdoor coil entering dry bulb air temperatures per ANSI/AHRI Std. 210/240 (AHRI 2008). If the rated test temperatures are different from the values populated by the tool, then the user may enter the applicable values manually. The rated data can be one of the performance data points depending on the speed or stage. The rated data set is entered in the Cells range ``B11:E11'' of the INPUT tab as shown in Figure~\ref{fig:main-menu-screen-of-the-weather-converter}.
diff --git a/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/references-002.tex b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/references-002.tex
new file mode 100644
index 00000000000..8498450f999
--- /dev/null
+++ b/doc/auxiliary-programs/src/hvac-performance-curve-fit-tool/references-002.tex
@@ -0,0 +1,7 @@
+\section{References}\label{references-001}
+
+AHRI 2008. ANSI/AHRI Standard 210/240: 2008 Standard for Performance Rating of Unitary Air-Conditioning \& Air-Source Heat Pump Equipment. Arlington, VA: Air-Conditioning, Heating, and Refrigeration Institute.
+
+AHRI 2007. ANSI/AHRI Standard 340/360: 2007 Standard for Performance Rating of Commercial and Industrial Unitary Air-Conditioning and Heat Pump Equipment. Arlington, VA: Air-Conditioning, Heating, and Refrigeration Institute.
+
+AHRI 2003. ANSI/AHRI Standard 550/590: 2003 Standard for Performance Rating Of Water -Chilling Packages Using The Vapor Compression Cycle. Arlington, VA: Air-Conditioning, Heating, and Refrigeration Institute.
diff --git a/doc/auxiliary-programs/src/input-macros.tex b/doc/auxiliary-programs/src/input-macros.tex
new file mode 100644
index 00000000000..575d9d6e4a8
--- /dev/null
+++ b/doc/auxiliary-programs/src/input-macros.tex
@@ -0,0 +1 @@
+\chapter{Input Macros}\label{input-macros}
diff --git a/doc/auxiliary-programs/src/input-macros/defining-blocks-of-input.tex b/doc/auxiliary-programs/src/input-macros/defining-blocks-of-input.tex
new file mode 100644
index 00000000000..fd51c8c4c7d
--- /dev/null
+++ b/doc/auxiliary-programs/src/input-macros/defining-blocks-of-input.tex
@@ -0,0 +1,227 @@
+\section{Defining Blocks of Input}\label{defining-blocks-of-input}
+
+The \textbf{\#\#def} command allows a block of input text to be defined and given a name. The block of text can then be inserted anywhere in the EnergyPlus input stream by simply referencing the name of the block. (This process is called macro expansion.) The block can have parameters (also called arguments) that can be given different values each time the block is referenced.
+
+The syntax of the \textbf{\#\#def} command is as follows:
+
+\begin{lstlisting}
+        unique name
+           |         zero or more arguments   macro text
+           |            |                     |
+           |            |                     |
+    ##def  macro-name [ arg1 arg2,arg3 ...]   text line 1
+  |_     |           | |    |_   |   _|     |
+    |    |           | |      |  |  |       |
+    |    |           | |      |  |  |       
+zero    one       zero_|     space(s)       one
+or      or        or         or comma       or
+more    more      more                      more
+spaces  spaces    spaces                    spaces
+\end{lstlisting}
+
+Example: Define a schedule macro with name ``All\_Const'':
+
+\begin{lstlisting}
+**##def** All_Const[x]
+**       ** Fraction, WeekON, 1,1, 12,31;
+    WEEKSCHEDULE, WeekON,
+        DayON,DayON,DayON,
+        DayON,DayON,DayON,
+        DayON,DayON,DayON,
+        DayON,DayON,DayON;
+    DAYSCHEDULE, DayON, Fraction,
+        x,x,x,x,x,x,x,x,x,x,x,x,
+        x,x,x,x,x,x,x,x,x,x,x,x ;
+**##enddef**
+\end{lstlisting}
+
+Then, in the EnergyPlus input stream (file in.imf), when we write :
+
+\begin{lstlisting}
+
+SCHEDULE, Constant At 0.8, All_Const[0.8]
+\end{lstlisting}
+
+the result (file out.idf) is equivalent to:
+
+\begin{lstlisting}
+SCHEDULE, Constant At 0.8,
+        Fraction, WeekON, 1,1, 12,31;
+    WEEKSCHEDULE, WeekON,
+        DayON,DayON,DayON,
+        DayON,DayON,DayON,
+        DayON,DayON,DayON,
+        DayON,DayON,DayON;
+    DAYSCHEDULE, DayON, Fraction,
+        0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,
+        0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8 ;
+\end{lstlisting}
+
+Macro definitions may have one or more arguments; the maximum number of arguments is 32. When a macro with arguments is referenced, its arguments must be given values. When a macro has no arguments, the brackets are still required both for macro definition and reference.
+
+Caution: Square brackets {[} {]} have been used in some versions of EnergyPlus inputs as comment/units fields. These will be expanded if left in the IDF and sent to EPMacro.
+
+Macro names must be unique (except see \textbf{\#\#set1} below); i.e., when a macro name is defined it cannot be defined again. Macro names are limited to 40 characters.
+
+To summarize, commands you use to define macros are the following:
+
+\textbf{\#\#def} macro-name {[}\textbf{arg1},..,\textbf{arg\emph{n}} {]} macro-text
+
+Defines a macro with the name macro-name and arguments ``arg1'' through ``arg\emph{n}''. ``Macro-text'' is one or more lines of text. If there are no arguments, the syntax is \textbf{\#\#def} macro-name macro-text.
+
+\textbf{\#\#enddef}
+
+Indicates the end of the macro definition initiated by \textbf{\#\#def.}
+
+\textbf{\#\#def1} macro-name {[}\textbf{arg1},..,\textbf{arg\emph{n}} {]} macro-text
+
+This is the same as \textbf{\#\#def} but there is only one line of text so that the terminating command \textbf{\#\#enddef} is not required.
+
+\textbf{\#\#set1} macro-name macro-text
+
+Like \textbf{\#\#def1} but has no arguments and macro-text is evaluated before storing. ``Macro-text is evaluated'' means that if macro-text contains other macros, these macros will be expanded, and the expanded text becomes the macro-text defined by \textbf{\#\#set1}.
+
+Example:
+
+\begin{lstlisting}
+                **\#\#def1**   xx  123
+                **\#\#set1**   yy  xx[]
+\end{lstlisting}
+
+is equivalent to: \textbf{\#\#set1} yy 123
+
+\textbf{\#\#set1} can also be used to redefine macro-name.
+
+\textbf{\#\#set1} x 0 . . .
+
+\textbf{\#\#set1} x \textbf{\#eval}{[} x{[}{]}+1 {]}
+
+(see Arithmetic Operations for description of the \textbf{\#eval} macro.)
+
+\subsection{Arithmetic Operations}\label{arithmetic-operations}
+
+The built-in macro called \textbf{\#eval{[} {]}} can be used to perform arithmetic, literal, and logical operations. It can be abbreviated to \textbf{\# {[} {]}.}
+
+\#eval{[} X OP Y {]} or \#{[} X OP Y {]}
+
+gives the result X OP Y. The allowed values for X, OP, and Y, and the corresponding result, are shown in the following table.
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\toprule 
+X* & OP ** & Y & Result \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+X* & OP ** & Y & Result \tabularnewline
+\midrule
+\endhead
+
+number & + (plus) & number & number \tabularnewline
+number & - (minus) & number & number \tabularnewline
+number & * (times) & number & number \tabularnewline
+number & / (divided by) & number & number \tabularnewline
+number & min & number & number \tabularnewline
+number & max & number & number \tabularnewline
+number & mod & number & number \tabularnewline
+number & ** (power) & number & number \tabularnewline
+SIN & OF & number (degrees) & number \tabularnewline
+COS & OF & number (degrees) & number \tabularnewline
+TAN & OF & number (degrees) & number \tabularnewline
+SQRT & OF & number & number \tabularnewline
+ABS & OF & number & number \tabularnewline
+ASIN & OF & number & number (degrees) \tabularnewline
+ACOS & OF & number & number (degrees) \tabularnewline
+ATAN & OF & number & number \tabularnewline
+INT & OF & number & number \tabularnewline
+LOG10 & OF & number & number \tabularnewline
+LOG & OF & number & number \tabularnewline
+literal1 & // (concatenate) & literal2 & literal "literal1literal2" \tabularnewline
+literal1 & /// (concatenate) & literal2 & literal "literal1 literal2" \tabularnewline
+literal & EQS (=) & literal & logical (true or false) case sensitive \tabularnewline
+literal & NES (\(\neq\)) & literal & logical (true or false) case sensitive \tabularnewline
+literal & EQSU (=) & literal & logical (true or false) not case sensitive \tabularnewline
+literal & NESU (\(\neq\)) & literal & logical (true or false) not case sensitive \tabularnewline
+logical & AND & logical & logical (true or false) \tabularnewline
+logical & OR & logical & logical (true or false) \tabularnewline
+ & NOT & logical & logical (true or false) \tabularnewline
+number & EQ (=) & number & logical (true or false) \tabularnewline
+number & NE (\(\neq\)) & number & logical (true or false) \tabularnewline
+number & GT (>) & number & logical (true or false) \tabularnewline
+number & GE (\(\geq\)) & number & logical (true or false) \tabularnewline
+number & LT (<) & number & logical (true or false) \tabularnewline
+number & LE (\(\leq\)) & number & logical (true or false) \tabularnewline
+* Upper or lower case is allowed for SIN, COS, etc. \tabularnewline
+** Upper or lower case is allowed for OF, EQS, etc. \tabularnewline
+\bottomrule
+\end{longtable}
+
+Example
+
+\textbf{\#eval{[}** 1 + 2 **{]}} when expanded becomes 3.
+
+\textbf{\#eval{[}** 1 +}\#eval\textbf{{[}2 * 3{]} **{]}} when expanded becomes 7.
+
+Example
+
+\textbf{\#\#set1} city{[}{]} Washington
+
+DesignDay, \#{[} city{[} {]} /// SUMMER {]}, ! Design Day Name
+
+gives
+
+\begin{lstlisting}
+ DesignDay, "Washington SUMMER", ! Design Day Name
+\end{lstlisting}
+
+The following example illustrates the use of \textbf{\#eval} inside \textbf{\#if} commands:
+
+\textbf{\#\#if} \textbf{\#{[}** city{[} {]} EQS Chicago **{]}}
+
+\textbf{\#\#if} \textbf{\#{[}\#{[}** city{[} {]} EQS Chicago {]} and}\#{[}** occup{[} {]} NES low **{]}** **{]}**
+
+Notes:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\tightlist
+\item
+  For logical values:
+\end{enumerate}
+
+False = 0 or BLANK,
+
+True = any other character
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  A literal must be enclosed inside a pair of double quotes if it contains BLANKs or reserved characters like {[} {]} ( ) ,
+\end{enumerate}
+
+E.g., ``abc *def''
+
+Otherwise, the quotes around the literals are optional.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Literal concatenation operators // and /// produce quoted literals.
+\end{enumerate}
+
+E.g., \# {[} large /// office {]} gives ``large office''
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{3}
+\item
+  Literals are case sensitive. For example, ``Chicago'', ``CHICAGO'' and ``chicago'' are distinct.
+\item
+  EQS and NES are case sensitive string comparisons. EQSU and NESU are case insensitive string comparisons.
+\item
+  Literals are limited to 40 characters.
+\end{enumerate}
diff --git a/doc/auxiliary-programs/src/input-macros/incorporating-external-files.tex b/doc/auxiliary-programs/src/input-macros/incorporating-external-files.tex
new file mode 100644
index 00000000000..1a243132038
--- /dev/null
+++ b/doc/auxiliary-programs/src/input-macros/incorporating-external-files.tex
@@ -0,0 +1,143 @@
+\section{Incorporating External Files}\label{incorporating-external-files}
+
+\textbf{\#\#include} \{includefilename\}
+
+This command puts all of the lines in an external file into the EnergyPlus input stream starting right after the command line. The name of the file that is included is the concatenation of \{prefixpathname\}, entered using \textbf{\#\#fileprefix} , and \{includefilename\}. The lines in the external file will be listed in the resultant IDF file. When all the lines in the external file have been read in, input reverts back to the original input file at the line following the \textbf{\#\#include} command.
+
+\textbf{\#\#fileprefix} \{prefixpathname\}
+
+specifies a pathname that will be prefixed to the filename given in an \textbf{\#\#include} command. The \textbf{\#\#fileprefix} command allows commonly-used include files to be kept in a directory other than the directory in which the current input file resides.
+
+Example: on a PC, the combination
+
+\textbf{\#\#fileprefix} C:\textbackslash{}EnergyPlus\textbackslash{}Library
+
+\textbf{\#\#include} SCHEDULES.IDF
+
+will include into the EnergyPlus input stream the file whose full name is
+
+C:\textbackslash{}EnergyPlus\textbackslash{}Library\textbackslash{}SCHEDULES.IDF
+
+\textbf{\#\#includesilent} \{includefilename\}
+
+This command is identical to \textbf{\#\#include}, except that the lines in the included file will not be listed in the EP-MACRO echo.
+
+\textbf{\#\#nosilent}
+
+Overrides the listing suppression of \textbf{\#\#includesilent}. Used for debugging purposes only. After \textbf{\#\#nosilent} , all following \textbf{\#\#includesilent} commands are treated as \textbf{\#\#include} commands.
+
+Example: Assume the following files contain the indicated lines:
+
+\begin{longtable}[c]{@{}lll@{}}
+\toprule 
+Main input file: & First external file: & Second external file: \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Main input file: & First external file: & Second external file: \tabularnewline
+\midrule
+\endhead
+
+input1.inp & file2.inp & file3.inp \tabularnewline
+line 1a & line 2a & line 3a \tabularnewline
+\#\#include file2.inp & line 2b & line 3b \tabularnewline
+line 1b & \#\#include file3.inp & line 3c \tabularnewline
+line 1c & line 2c & line 3d \tabularnewline
+\bottomrule
+\end{longtable}
+
+The end result of processing \textbf{\#\#include} input1.inp will be:
+
+\begin{lstlisting}
+line 1a     (from input1.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 2a     (from file2.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 2b    (from file2.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 2c     (from file2.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 1b    (from input1.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 1c     (from input1.inp)
+\end{lstlisting}
+
+External files can also contain \textbf{\#\#include} commands, as shown in the following example:
+
+\begin{longtable}[c]{@{}lll@{}}
+\toprule 
+Main input file: & First external file: & Second external file: \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Main input file: & First external file: & Second external file: \tabularnewline
+\midrule
+\endhead
+
+input1.inp & file2.inp & file3.inp \tabularnewline
+line 1a & line 2a & line 3a \tabularnewline
+\#\#include file2.inp & line 2b & line 3b \tabularnewline
+line 1b & \#\#include file3.inp & line 3c \tabularnewline
+line 1c & line 2c & line 3d \tabularnewline
+\bottomrule
+\end{longtable}
+
+The end result of processing \textbf{\#\#include} input1.tmp will be:
+
+\begin{lstlisting}
+line 1a     (from input1.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 2a     (from file2.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 2b    (from file2.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 3a     (from file3.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 3b    (from file3.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 3c     (from file3.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 3d    (from file3.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 2c     (from file2.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 1b    (from input1.inp)
+\end{lstlisting}
+
+\begin{lstlisting}
+line 1c     (from input1.inp)
+\end{lstlisting}
+
+Note: Up to nine \textbf{\#\#include} commands can be nested. However, there should be no recursion. This is an example of a recursion:
+
+file1.inp contains \textbf{\#\#include} file2.inp
+
+file2.inp contains \textbf{\#\#include} file1.inp
diff --git a/doc/auxiliary-programs/src/input-macros/introduction-001.tex b/doc/auxiliary-programs/src/input-macros/introduction-001.tex
new file mode 100644
index 00000000000..3a8b458a3ed
--- /dev/null
+++ b/doc/auxiliary-programs/src/input-macros/introduction-001.tex
@@ -0,0 +1,18 @@
+\section{Introduction}\label{introduction}
+
+The Input Macros feature increases the flexibility of the EnergyPlus input files. This feature is intended for advanced users who are already familiar with EnergyPlus IDF files and need to prepare input manually. The basic capabilities are:
+
+\begin{itemize}
+\item
+  Incorporating external files containing pieces of IDF into the main EnergyPlus input stream.
+\item
+  Selectively accepting or skipping portions of the input.
+\item
+  Defining a block of input with parameters and later referencing this block.
+\item
+  Performing arithmetic and logical operations on the input.
+\item
+  Input macro debugging and listing control.
+\end{itemize}
+
+These capabilities are invoked in the EP-MACRO program by using macro commands. Macro commands are preceded by \#\# to distinguish them from regular EnergyPlus input commands. After execution by the EP-MACRO processor, macro commands produce regular lines of EnergyPlus input that are shown in the resultant IDF file (\textbf{out.idf}) and, subsequently, in the EnergyPlus echo print (\textbf{audit.out}). Following are descriptions of the macro commands associated with the above capabilities. A detailed example of input macros is given at the end of this section; you should review it before reading the macro command descriptions.
diff --git a/doc/auxiliary-programs/src/input-macros/listing-format.tex b/doc/auxiliary-programs/src/input-macros/listing-format.tex
new file mode 100644
index 00000000000..a0cd6439a99
--- /dev/null
+++ b/doc/auxiliary-programs/src/input-macros/listing-format.tex
@@ -0,0 +1,23 @@
+\section{Listing Format}\label{listing-format}
+
+The format of listing from EP-MACRO gives information about the status of the input macros, as shown in the following:
+
+\begin{lstlisting}
+ 1. 1.1  * 123 * ...... EnergyPlus input line
+ -  - -  ------- ----------------------------------
+ |  | |     |     echo of EnergyPlus input line
+ |  | |     |
+ |  | |    line number ( if the current line is being skipped
+ |  | |                  by " ##if... " etc, this is indicated
+ |  | |                  by printing "- 123 -" instead of
+ |  | |                  "* 123 *" in the line number field;
+ |  | |                  if the current line is part of a
+ |  | |                  macro command, it is indicated by
+ |  | |                  printing "# 123 #" )
+ |  | |
+ |  | macro expansion nesting level
+ |  |
+ |"##if" nesting level
+ |
+ "##include" nesting level
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/input-macros/macro-debugging-and-listing-control.tex b/doc/auxiliary-programs/src/input-macros/macro-debugging-and-listing-control.tex
new file mode 100644
index 00000000000..7e9a8886de0
--- /dev/null
+++ b/doc/auxiliary-programs/src/input-macros/macro-debugging-and-listing-control.tex
@@ -0,0 +1,147 @@
+\section{Macro Debugging and Listing Control}\label{macro-debugging-and-listing-control}
+
+\textbf{\#\#list}
+
+Turn on listing; echo of input lines on the OUTPUT file is enabled. This is the default condition.
+
+\textbf{\#\#nolist}
+
+Turn off listing; echo of input lines on the output file is disabled.
+
+\textbf{\#\#show}
+
+Start printing expanded line on output file. After this command, if a macro expansion was done, the expanded line is printed on the output file. In this way you can see the end result of macro expansions, which is the input as seen by the EnergyPlus Input processor.
+
+\textbf{\#\#noshow}
+
+Stop printing expanded line on output file. This is the default condition.
+
+\textbf{\#\#showdetail}
+
+Start printing each macro expansion. After this command, every time a macro expansion is done the result of the expansion is printed. This can produce lots of output.
+
+\textbf{\#\#noshowdetail}
+
+Stop printing each macro expansion. This is the default condition.
+
+\#\#expandcomment
+
+Comment fields may contain macro expansion directions. Following this command, the macros will be expanded in comments.
+
+For example, you might have:
+
+\#\#set1 Location = ``Colorado Springs, CO''
+
+! Simulation run for Location{[}{]}
+
+If \#\#expandcomment preceded the set1 command, then the output would look like:
+
+! Simulation run for Colorado Springs, CO
+
+\#\#noexpandcomment
+
+This does not expand macros in comment fields. This is the default condition.
+
+\textbf{\#\#traceback}
+
+Give full traceback when printing an error message. After this command, if there is a EP-MACRO error, a full traceback of the macro expansions in progress is printed. This is the default condition.
+
+\textbf{\#\#notraceback}
+
+Don't give full traceback when printing an error message.
+
+\textbf{\#\#write}
+
+Start writing expanded text into file 22. This is similar to \textbf{\#\#show} except that the expanded lines are written into file 22. Therefore, file 22 will contain only the text that will be seen by the EnergyPlus processor. This file is used only for debugging purposes. It allows you to see what the macro-processed input file looks like.
+
+\textbf{\#\#nowrite}
+
+Stop writing expanded text into file 22. This is the default condition.
+
+\textbf{\#\#symboltable}
+
+Prints table of current macro names. All of the macro names that are defined will be printed.
+
+\textbf{\#\#clear}
+
+Clear all macro definitions. All the macro names defined up to this point will be deleted.
+
+\textbf{\#\#reserve} TEXT \emph{k} NAMES \emph{l} STACK \emph{m}
+
+Allocates memory.
+
+Reserves \emph{k} words of space in AA array for macro definition storage.
+
+Reserves \emph{l} positions in macro definition names table.
+
+Reserves \emph{m} words of stack space.
+
+If used, the \textbf{\#\#reserve} command must precede all other macro commands in the EP-MACRO input. This command should be used only if one or more of the following error messages is received:
+
+``Need more memory for storing macro definitions''
+
+Use ``\textbf{\#\#reserve} TEXT nnnnnn'' command to get more memory. Current value of \emph{nnnnnn} is: \_ \_ \_
+
+``Macro table capacity exceeded''
+
+Use ``\textbf{\#\#reserve} NAMES nnnnnn'' command to get more memory. Current value of \emph{nnnnnn} is: \_ \_ \_
+
+``Macro stack overflow''
+
+Use ``\textbf{\#\#reserve} STACK nnnnnn'' command to get more memory. Current value of \emph{nnnnnn} is: \_ \_ \_
+
+\textbf{\#\#! \textless{}comment\textgreater{}}
+
+Allows you to enter comment lines inside a macro. \textbf{\textless{}comment\textgreater{}} is printed in the EP-MACRO echo but is not acted on by the macro processor.
+
+\emph{Example:}
+
+This example shows the use of the \textbf{\#\#set}, \textbf{\#\#include}, \textbf{\#\#eval} and \textbf{\#\#if} commands. Let an external file called cities.idf contain the following text:
+
+** \#\#if \#**{[} city{[} {]} \textbf{EQS} CHICAGO {]}
+
+Location,Chicago IL, !- Location Name
+
+41.880, !- Latitude
+
+-87.63, !- Longitude
+
+-6.0, !- Time Zone
+
+2.; !- Elevation \{m\}
+
+\textbf{\#\#elseif \#}{[} city{[} {]} \textbf{EQS} WASHINGTON {]}
+
+Location,Washington DC, !- Location Name
+
+38.9, !- Latitude
+
+-77.0, !- Longitude
+
+-5.0, !- Time Zone
+
+15.; !- Elevation \{m\}
+
+\textbf{\#\#else}
+
+** ** ERROR --- City Undefined
+
+\textbf{\#\#endif}
+
+Then the EnergyPlus input
+
+\textbf{\#\#set1} city{[} {]} CHICAGO
+
+\textbf{\#\#include} cities.idf
+
+will be converted, after macro processing, to:
+
+Location,Chicago IL, !- Location Name
+
+41.880, !- Latitude
+
+-87.63, !- Longitude
+
+-6.0, !- Time Zone
+
+2.; !- Elevation \{m\}
diff --git a/doc/auxiliary-programs/src/input-macros/running-the-ep-macro-program.tex b/doc/auxiliary-programs/src/input-macros/running-the-ep-macro-program.tex
new file mode 100644
index 00000000000..ca3f7a57e84
--- /dev/null
+++ b/doc/auxiliary-programs/src/input-macros/running-the-ep-macro-program.tex
@@ -0,0 +1,25 @@
+\section{Running the EP-Macro program}\label{running-the-ep-macro-program}
+
+The EP-Macro program is run automatically from the batch files (RunEPlus or EPL-Run from EP-Launch). Skip this small section if you are using either the RunEPlus batch file or EP-Launch. If you wish to run it by hand, it is found in the main folder of the EnergyPlus install (bin folder in the Linux install). Note that in EP-Launch and other script files for use with EP-Macro the convention is to name the file \textless{}filename\textgreater{}.imf (input macro file). If you name it \textless{}filename\textgreater{}.idf (input data file), the scripts will most likely think it is a ``normal'' EnergyPlus input file and ignore using EP-Macro on it - giving you a less than desireable result.
+
+% table 29
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Files used in EP-Macro program \label{table:files-used-in-ep-macro-program}} \tabularnewline
+\toprule 
+File Name & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Files used in EP-Macro program} \tabularnewline
+\toprule 
+File Name & Description \tabularnewline
+\midrule
+\endhead
+
+in.imf & Input file containing the macro commands \tabularnewline
+audit.out & audit of the EPMacro run \tabularnewline
+out.idf & Output file that can be run with EnergyPlus \tabularnewline
+\bottomrule
+\end{longtable}
+
+The EP-Macro program is a Console Application, so to run by hand you would need to open a command prompt in the Main EnergyPlus install folder. Then, you would need to copy your input file containing the macro commands from its folder to this folder with the name ``in.imf''. The installed name of the EP-Macro program is ``epmacro.exe''. After execution, you can save the out.idf in an appropriate folder or rename it to in.idf in order to execute EnergyPlus. You can view the audit.out file for any errors that might have occurred during EP-Macro processing.
diff --git a/doc/auxiliary-programs/src/input-macros/selectively-accepting-or-skipping-lines-of.tex b/doc/auxiliary-programs/src/input-macros/selectively-accepting-or-skipping-lines-of.tex
new file mode 100644
index 00000000000..bb40930d64d
--- /dev/null
+++ b/doc/auxiliary-programs/src/input-macros/selectively-accepting-or-skipping-lines-of.tex
@@ -0,0 +1,99 @@
+\section{Selectively Accepting or Skipping Lines of Input}\label{selectively-accepting-or-skipping-lines-of-input}
+
+The \textbf{\#\#if} series of commands is used to selectively accept or skip lines of input according to the following sequence:
+
+```idf \textbf{\#\#if} \{condition1\} line1a line1b \ldots{}
+
+\textbf{\#\#elseif} \{condition2\} line2a line2b \ldots{}
+
+\textbf{\#\#elseif} \{condition3\textbf{\}} line3a line3b \ldots{}
+
+\textbf{\#\#else} line N a line N b \ldots{}
+
+\textbf{\#\#endif}
+
+Then the lines that will be included into the EnergyPlus input stream are:
+
+\begin{lstlisting}
+
+If {condition 1} is TRUE,
+  line1a
+  line1b
+  ...
+
+  otherwise
+
+  If {condition 2} is TRUE,
+  line2a
+  line2b
+  ...
+
+  otherwise
+
+  If {condition 3} is TRUE,
+  line3a
+  line3b
+  ...
+
+  otherwise
+
+  If {condition 1}, {condition 2}, {condition 3} are all FALSE.
+  line N a
+  line N b
+  ...
+\end{lstlisting}
+
+There are six different \textbf{\#\#if\ldots{}} commands:
+
+Command
+
+Result
+
+\textbf{\#\#ifdef}
+
+\begin{description}
+\item[\{macro name\}]
+if macro name defined, include following lines
+\end{description}
+
+\textbf{\#\#ifndef}
+
+\begin{description}
+\item[\{macro name\}]
+if macro name NOT defined, include following lines
+\end{description}
+
+\textbf{\#\#if}
+
+\begin{description}
+\item[\{condition\}]
+if condition is TRUE, include following lines
+\end{description}
+
+\textbf{\#\#elseif}
+
+\begin{description}
+\item[\{condition\}]
+if condition is TRUE, and previous conditions are FALSE, include
+\end{description}
+
+following lines
+
+\begin{description}
+\item[\textbf{\#\#else}]
+if all previous conditions are FALSE, include following lines
+\item[\textbf{\#\#endif}]
+indicates the end of the if block
+\end{description}
+
+Notes:
+
+\{macro name\} is explained in section \emph{Defining Blocks of Input}, below.
+
+\{condition\} is 0 or BLANK meaning FALSE, and any other character meaning TRUE.
+
+\textbf{\#\#ifdef} and \textbf{\#\#ifndef} do not have corresponding \textbf{\#\#elseif} commands, but they do have
+
+\begin{lstlisting}
+   corresponding  **\#\#else**  and  **\#\#endif**  commands.
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/manipulating-output-files.tex b/doc/auxiliary-programs/src/manipulating-output-files.tex
new file mode 100644
index 00000000000..0f1778cf8d2
--- /dev/null
+++ b/doc/auxiliary-programs/src/manipulating-output-files.tex
@@ -0,0 +1 @@
+\chapter{Manipulating Output Files}\label{manipulating-output-files}
diff --git a/doc/auxiliary-programs/src/manipulating-output-files/ep-compare.tex b/doc/auxiliary-programs/src/manipulating-output-files/ep-compare.tex
new file mode 100644
index 00000000000..2403e672a56
--- /dev/null
+++ b/doc/auxiliary-programs/src/manipulating-output-files/ep-compare.tex
@@ -0,0 +1,25 @@
+\section{EP-Compare}\label{ep-compare}
+
+The EP-Compare program is intended to be used to compare the tabular results of several simulations including the ABUPS summary report. To generate tabular reports in EnergyPlus use the Output:Table:SummaryReports object and make sure the OutputControl:Table:Style includes HTML output. EP-Compare displays bar graphs and monthly line graphs for most of the tabular reports. It can be used in Windows, Linux and Macintosh systems. The main screen is shown below:
+
+\begin{figure}[hbtp] % fig 56
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image122.png}
+\caption{EP-Compare Main Screen \protect \label{fig:ep-compare-main-screen}}
+\end{figure}
+
+The main screen shows both the graph being displayed at the bottom and allows the user to select a graph from a list at the top. The list of graphs is based on each table name and subtable name and then has a list of graphs supported including stacked bars, simple bar, 100\% stacked bars, side-by-side bars, and monthly line graphs. The program window can be resized.
+
+The first time the program is started no graphs are shown because no files have been selected. To select files use the ``Manage Files'' button. This brings up the Manage Files dialog box shown below:
+
+\begin{figure}[hbtp] % fig 57
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image123.png}
+\caption{EP-Compare Dialog box \protect \label{fig:ep-compare-dialog-box}}
+\end{figure}
+
+This dialog lets you add and remove files from the list of files. The files selected should be HTML or HTM files that are produced by EnergyPlus when using the Output:Table:SummaryReports object with OutputControl:Table:Style set to produce HTML files. It is best to compare files that have similar reports otherwise missing values will be shown as zeros.The dialog also provides a button to add entire directories of files but that adding too many files makes the graphs difficult to understand. To change the order that files appear in the graph, the files can be dragged up and down the list of files in the Manage Files dialog. The dialog box window can be resized to view longer files names if necessary.
+
+When EP-Compare is started again, the files last selected are shown in the graph if they are still available.
+
+The Copy button allows the current graph (as it is sized in the window) to be copied to another application such as Microsoft Word or PowerPoint. To paste a copied image to those programs use the Paste Special option and select one of the bitmap formats.
diff --git a/doc/auxiliary-programs/src/parametric-spreadsheets.tex b/doc/auxiliary-programs/src/parametric-spreadsheets.tex
new file mode 100644
index 00000000000..3b2ed1b7e02
--- /dev/null
+++ b/doc/auxiliary-programs/src/parametric-spreadsheets.tex
@@ -0,0 +1,3 @@
+\chapter{Parametric Spreadsheets}\label{parametric-spreadsheets}
+
+Several spreadsheet applications are included in the Preprocess\textbackslash{}ParametricSpreadsheets folder. These include spreadsheets (Excelâ„¢) for the Water Source heat pumps and Water to Air heat pumps.
diff --git a/doc/auxiliary-programs/src/parametric-spreadsheets/g-function-spreadsheet.tex b/doc/auxiliary-programs/src/parametric-spreadsheets/g-function-spreadsheet.tex
new file mode 100644
index 00000000000..3257cde4c25
--- /dev/null
+++ b/doc/auxiliary-programs/src/parametric-spreadsheets/g-function-spreadsheet.tex
@@ -0,0 +1,20 @@
+\section{G-Function Spreadsheet}\label{g-function-spreadsheet}
+
+The spreadsheet (g-function\_library.xls) has comparison plots for different configurations/grouts for the Ground Heat Exchanger:Vertical. A user can see how the boreholes interact with each other in different configurations. It has the actual screen shot (GLHEPro) showing the conditions/inputs used to obtain the data. GLHEPro is not included with EnergyPlus and it or something similar should be used to generate similar values. Some of the values used in getting g-functions are not used in the EnergyPlus Ground loop model, but the spreadsheet screen shot gives an idea of what the inputs were in obtaining the g-functions.
+
+The reference data set GLHERefData.idf contains sets of parameters for the Ground Heat Exchangers:
+
+``This file contains sample input for the ground loop heat exchanger model. The response of the borehole/ground is found from the `G-function' that is defined in the input as series of `n' pairs of values (LNTTSn, GNFCn). It is important to note that the G-functions have to be calculated for specific GHE configurations and borehole resitance, length and borehole/ length ratio. That is, the parameters for the units vary with each design. The data in this file are intended as examples/samples and may not represent actual designs.
+
+The sample data has been calculated for a number of configurations:
+
+\begin{itemize}
+\item
+  1 x 2 boreholes
+\item
+  4 x 4 boreholes
+\item
+  8 x 8 boreholes
+\end{itemize}
+
+Data is given for both `standard' grout (k = 0.744 W/m.K) and `thermally enhanced' grout (k = 1.471 W/m.K). The flow rate per borehole is .1514 kg/s. The pipe given is 0.75in. Dia. SDR11 HDPE. The fluid is water. The borehole/length ratio is 0.06 (76.2m/4.572m {[}300ft/15ft{]})
diff --git a/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-air-heat-pump-parameter-coefficient-001.tex b/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-air-heat-pump-parameter-coefficient-001.tex
new file mode 100644
index 00000000000..d3ddd8158fc
--- /dev/null
+++ b/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-air-heat-pump-parameter-coefficient-001.tex
@@ -0,0 +1,205 @@
+\section{Water-to-Air Heat Pump Parameter / Coefficient Generator (Heating Mode)}\label{water-to-air-heat-pump-parameter-coefficient-generator-heating-mode}
+
+This document gives brief instructions on generating the parameters/ coefficients for the water-to-air heat pump models in heating mode. The Excelâ„¢ spreadsheets (WaterAir\_PE\_Heating.xls) are used. The spreadsheet generates:
+
+\begin{itemize}
+\item
+  parameters for the parameter estimation based model.
+\item
+  coefficients for the curve-fit model.
+\end{itemize}
+
+The following theses have detailed information about the curve-fit model and parameter estimation based model:
+
+Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at \href{http://www.hvac.okstate.edu}{www.hvac.okstate.edu})
+
+Shenoy,Arun. 2004. Simulation, Modeling and Analysis of Water to Air Heat Pump. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at \href{http://www.hvac.okstate.edu}{www.hvac.okstate.edu})
+
+Tang,C.C. 2004. Modeling Packaged Heat Pumps in a Quasi-Steady State Energy Simulation Program. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at \href{http://www.hvac.okstate.edu}{www.hvac.okstate.edu})
+
+\subsection{Step 1: Catalog Data Input}\label{step-1-catalog-data-input}
+
+Data points are obtained from the heat pump manufacturer data. Minimum data points for the parameter estimation based model are 32 data points according to Jin (2002). The curve-fit model performance is not affected by the number of data points and a minimum of 5 data points is required since the governing equations require 5 coefficients. The data points must have varying inlet conditions (e.g.~air flow rates, inlet water temperatures, and etc.) that covers the entire range of the heat pump operating conditions. Correction tables provided by the manufacturer should be used to extend the catalog data range in order to have a good set of parameters/coefficients.
+
+\begin{itemize}
+\item
+  Using the heat pump performance data, enter the values to Table~\ref{table:comparison-of-ee-with-esp-rdoe-2blast-weather} in worksheet ``CATALOG DATA''. The values can be in SI or IP units.
+\item
+  Click on Button 1 based on the units used.
+\end{itemize}
+
+For IP units:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image054.png}
+\caption{}
+\end{figure}
+
+For SI units:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image055.png}
+\caption{}
+\end{figure}
+
+\begin{itemize}
+\item
+  The program will convert the values to the desired units and display them on Table~\ref{table:input-file-extensions-with-implied-data-types} in worksheet ``INPUT'' which will be used by the parameter/coefficient generator program.
+\item
+  The button shown below is used for clearing Table~\ref{table:comparison-of-ee-with-esp-rdoe-2blast-weather} (worksheet ``CATALOG DATA'') and Table~\ref{table:input-file-extensions-with-implied-data-types} (worksheet ``INPUT''). It is advisable to clear the tables before generating parameters/coefficients for a new heat pump model.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image056.png}
+\caption{}
+\end{figure}
+
+After Table~\ref{table:input-file-extensions-with-implied-data-types} is created, the parameters/coefficients are then calculated as follows:
+
+\begin{itemize}
+\item
+  Worksheet ``ParamEstimator'' is used for generating the parameters for the parameter estimation based model using Nelder Mead Simplex. Refer to the steps in the Parameter Estimation Procedure.
+\item
+  Worksheet ``CoeffCalculator'' is used for calculate the coefficients for the curve-fit model using the generalized least square method. Refer to the steps in the Curve Fit Model procedure.
+\end{itemize}
+
+\subsection{Parameter Estimation Procedure}\label{parameter-estimation-procedure}
+
+\subsubsection{Step 2a: Generating First Set of Parameters (PE-Based Model)}\label{step-2a-generating-first-set-of-parameters-pe-based-model}
+
+\begin{itemize}
+\item
+  Using Table~\ref{table:input-file-extensions-with-implied-data-types}, the program can generate parameters. The user must fill all the cells colored light blue in worksheet ``ParamEstimator''.
+\item
+  \textbf{Accuracy:} Start with a low accuracy for faster convergence, recommended value of 0.001.
+\item
+  \textbf{Compressor Type:} User is allowed to select from 3 types of compressors: scroll, rotary or reciprocating. Contact the manufacturer to make sure that the compressor selected is correct. Wrong type of compressor selected would lead to the program crashing or inaccurate parameters.
+\item
+  \textbf{Refrigerant:} Contact the manufacturer on the refrigerant used to generate the catalog data and select from the list of refrigerants. Usually the refrigerant used is R22. .
+\item
+  \textbf{Source Side Fluid:} Select the type of fluid used for the source side. 0: Water, 1: Antifreeze Mixture. Note that the number of parameters will change depending on the type of fluid. Antifreeze mixture requires one additional parameter.
+\item
+  \textbf{Which Initial Guess?:} The user may choose a set of initial guesses(1-5) that will be used by the optimization routine in generating the parameters. Start with 1, which is the set of initial guesses 1 at column B.
+\item
+  \textbf{Initial Guess:} Initial guess for all the parameters. For Initial Guess 1, enter a value of 1 for all the parameters except for the loss factor (less than 1.0). The loss factor should be less than 1.0 because the efficiency of the compressor should be less than 100\%. Adjust the values in Initial Guess 1 if the program happens to crash and try again.
+\item
+  Now click on Button 2 shown below to generate the parameters.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image057.png}
+\caption{}
+\end{figure}
+
+It will take some time to generate the parameters depending on the number of data points. The parameters generated will be displayed at Parameters 1.
+
+\begin{itemize}
+\item
+  Look at the error analysis of Error 1, which gives the user a summary of the errors for Heating Capacity, Heating Absorption and Power. An average error of 5-8\% is achievable for all the values.
+\item
+  The errors for all the individual catalog data points are displayed in worksheet ``RESULT''.
+\end{itemize}
+
+\subsubsection{Step 2b: Improving the Set of Parameters (PE-Based Model)}\label{step-2b-improving-the-set-of-parameters-pe-based-model}
+
+\begin{itemize}
+\item
+  After the initial set of parameters has been generated, the user can increase the accuracy of the parameters by using parameters generated as the initial guess for the second simulation and increasing the accuracy of the program.
+\item
+  Copy and Paste Parameters 1 to Initial Guess 2.
+\item
+  Change the initial guess indicator \textbf{(Which Initial Guess?)} from 1 to 2.
+\item
+  Increase the accuracy by twice. For example, set accuracy to 0.000001.
+\item
+  Now click on Button 2 shown below to generate the second set of parameters.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image041.png}
+\caption{}
+\end{figure}
+
+The simulation time would most likely be less but it depends on the accuracy value as well. And the parameters generated will be displayed at Parameter 2.
+
+\begin{itemize}
+\item
+  Compare Error 2 to Error 1, the error values should be less, which means that the parameters are getting better and more accurate.
+\item
+  Repeat the steps in 2a and 2b until a desired set of error values is achieved or the errors stop decreasing
+\end{itemize}
+
+\subsubsection{Step 3: Generating EnergyPlus Input Parameters}\label{step-3-generating-energyplus-input-parameters}
+
+\begin{itemize}
+\tightlist
+\item
+  Click on the Button 3 shown below to convert and arrange the parameters generated to fit EnergyPlus Input File (IDF), which will be listed from cell B46:B54.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image058.png}
+\caption{}
+\end{figure}
+
+\begin{itemize}
+\tightlist
+\item
+  The button shown below in worksheet ``ParamEstimator'' is used for clearing Initial Guess (2-5), Parameters(1-5), Error(1-5), EnergyPlus Input parameters and Result(1-5) in worksheet ``RESULT''.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image059.png}
+\caption{}
+\end{figure}
+
+\subsection{End Parameter Estimation Procedure}\label{end-parameter-estimation-procedure}
+
+\subsection{Curve Fit Model Procedure}\label{curve-fit-model-procedure}
+
+\subsubsection{Step 2: Generating the coefficients (Curve-Fit Model)}\label{step-2-generating-the-coefficients-curve-fit-model}
+
+\begin{itemize}
+\item
+  Using Table~\ref{table:input-file-extensions-with-implied-data-types}, the program can generate the coefficients. The user must fill all the cells colored light blue in Worksheet ``CoeffCalculator''.
+\item
+  \textbf{RatedAirVolFlowRate:} Rated volumetric air flow rate (m\(^{3}\)/s) which corresponds to the highest heating capacity listed in the catalog data.
+\item
+  \textbf{RatedWaterVolFlowRate:} Rated volumetric water flow rate (m\(^{3}\)/s) which corresponds to the highest heating capacity listed in the catalog data.
+\item
+  \textbf{RatedTotalCap:} Rated heating capacity (W) which is the highest heating capacity listed in the catalog data.
+\item
+  \textbf{RatedPower:} Rated power consumption (W) which corresponds to the highest heating capacity listed in the catalog data.
+\item
+  Now click on Button 2 shown below to calculate the coefficients.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image060.png}
+\caption{}
+\end{figure}
+
+\begin{itemize}
+\item
+  The coefficients for the corresponding curves are listed at cell B12:C16. Error analysis of model are listed at cell B19:B27.
+\item
+  The errors for all the individual catalog data points are displayed in worksheet ``RESULT''.
+\item
+  The button shown below in worksheet ``CoeffCalculator'' is used for clearing the coefficients, the error analysis and the outputs in worksheet ``RESULT''.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image059.png}
+\caption{}
+\end{figure}
+
+\subsection{End Curve Fit Model Procedure}\label{end-curve-fit-model-procedure}
diff --git a/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-air-heat-pump-parameter-coefficient.tex b/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-air-heat-pump-parameter-coefficient.tex
new file mode 100644
index 00000000000..46ee1d6e010
--- /dev/null
+++ b/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-air-heat-pump-parameter-coefficient.tex
@@ -0,0 +1,205 @@
+\section{Water-to-Air Heat Pump Parameter / Coefficient Generator (Cooling)}\label{water-to-air-heat-pump-parameter-coefficient-generator-cooling}
+
+This document gives brief instructions on generating the parameters or coefficients for the water-to-air heat pump models in cooling mode. The Excelâ„¢ spreadsheets (WaterAir\_PE\_Cooling.xls) are used. The spreadsheet generates:
+
+\begin{itemize}
+\item
+  parameters for the parameter estimation based model.
+\item
+  coefficients for the curve-fit model.
+\end{itemize}
+
+The following theses have detailed information about the curve-fit model and parameter estimation based model:
+
+Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at \href{http://www.hvac.okstate.edu}{www.hvac.okstate.edu})
+
+Shenoy,Arun. 2004. Simulation, Modeling and Analysis of Water to Air Heat Pump. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at \href{http://www.hvac.okstate.edu}{www.hvac.okstate.edu})
+
+Tang,C.C. 2004. Modeling Packaged Heat Pumps in a Quasi-Steady State Energy Simulation Program. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at \href{http://www.hvac.okstate.edu}{www.hvac.okstate.edu})
+
+\subsection{Step 1: Catalog Data Input}\label{step-1-catalog-data-input-000}
+
+Data points are obtained from the heat pump manufacturer data. Minimum data points for the parameter estimation based model are 32 data points according to Jin (2002). The curve-fit model performance is not affected by the number of data points and a minimum of 6 data points is required since the sensible cooling capacity requires 6 coefficients. The data points must have varying inlet conditions (e.g.~air flow rates, inlet water temperatures, and etc.) that covers the entire range of the heat pump operating conditions. Correction tables provided by the manufacturer should be used to extend the catalog data range in order to have a good set of parameters/coefficients.
+
+\begin{itemize}
+\item
+  Using the heat pump performance data, enter the values to Table~\ref{table:comparison-of-ee-with-esp-rdoe-2blast-weather} in worksheet ``CATALOG DATA''. The values can be in SI or IP units.
+\item
+  Click on Button 1 based on the units used.
+\end{itemize}
+
+For IP units:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image046.png}
+\caption{}
+\end{figure}
+
+For SI units:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image047.png}
+\caption{}
+\end{figure}
+
+\begin{itemize}
+\item
+  The program will convert the values to the desired units and display them on Table~\ref{table:input-file-extensions-with-implied-data-types} in worksheet ``INPUT''. Then the program will discard bad catalog points by calculating the relative humidity of the exiting air at the load side (relative humidity should be less or equal to 1). Table~\ref{table:lst-file-structure} in worksheet ``INPUT'' shows the input catalog data that will be used by the parameter/coefficient generator program.
+\item
+  The button shown below is used clearing Table~\ref{table:comparison-of-ee-with-esp-rdoe-2blast-weather} (worksheet ``CATALOG DATA''), Table~\ref{table:input-file-extensions-with-implied-data-types}, and Table~\ref{table:lst-file-structure} (worksheet ``INPUT''). It is advisable to clear the tables before generating parameters/coefficients for a new heat pump model.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image048.png}
+\caption{}
+\end{figure}
+
+After Table~\ref{table:lst-file-structure} is created, the parameters/coefficients are then calculated as follows:
+
+\begin{itemize}
+\item
+  Worksheet ``ParamEstimator'' is used for generating the parameters for the parameter estimation based model using Nelder Mead Simplex. Refer to the steps in the Parameter Estimation Procedure.
+\item
+  Worksheet ``CoeffCalculator'' is used for calculate the coefficients for the curve-fit model using the generalized least square method. Refer to the steps in the Curve Fit Model procedure.
+\end{itemize}
+
+\subsection{Parameter Estimation Procedure}\label{parameter-estimation-procedure-000}
+
+\subsubsection{Step 2a: Generating First Set of Parameters (PE-Based Model)}\label{step-2a-generating-first-set-of-parameters-pe-based-model-000}
+
+\begin{itemize}
+\item
+  Using contents of Table~\ref{table:lst-file-structure}, the program can generate parameters. The user must fill all the cells colored light blue in worksheet ``ParamEstimator''.
+\item
+  \textbf{Accuracy:} Start with a low accuracy for faster convergence, recommended value of 0.001.
+\item
+  \textbf{Compressor Type:} User is allowed to select from 3 types of compressors: scroll, rotary or reciprocating. Contact the manufacturer to make sure that the compressor selected is correct. Wrong type of compressor selected would lead to the program crashing or inaccurate parameters.
+\item
+  \textbf{Refrigerant:} Contact the manufacturer on the refrigerant used to generate the catalog data and select from the list of refrigerants. Usually the refrigerant used is R22. .
+\item
+  \textbf{Which Initial Guess?:} The user may choose a set of initial guesses(1-5) that will be used by the optimization routine in generating the parameters. Start with 1, which is the set of initial guesses 1 at column B.
+\item
+  \textbf{Initial Guess:} Initial guess for all the parameters. For Initial Guess 1, enter a value of 1 for all the parameters except for the loss factor (less than 1.0). The loss factor should be less than 1.0 because the efficiency of the compressor should be less than 100\%. Adjust the values in Initial Guess 1 if the program happens to crash and try again.
+\item
+  Now click on Button 2 shown below to generate the parameters.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image049.png}
+\caption{}
+\end{figure}
+
+It will take some time to generate the parameters depending on the number of data points. The parameters generated will be displayed at Parameters 1.
+
+\begin{itemize}
+\item
+  Look at the error analysis of Error 1, which gives the user a summary of the errors for Qtotal, Qsensible, Qsource and Power. An average error of 5-8\% is achievable for all the values.
+\item
+  The errors for all the individual catalog data points are displayed in worksheet ``RESULT''.
+\end{itemize}
+
+\subsubsection{Step 2b: Improving the Set of Parameters (PE-Based Model)}\label{step-2b-improving-the-set-of-parameters-pe-based-model-000}
+
+\begin{itemize}
+\item
+  After the initial set of parameters has been generated, the user can increase the accuracy of the parameters by using parameters generated as the initial guess for the second simulation and increasing the accuracy of the program.
+\item
+  Copy and Paste Parameters 1 to Initial Guess 2.
+\item
+  Change the initial guess indicator \textbf{(Which Initial Guess?)} from 1 to 2.
+\item
+  Increase the accuracy by twice. For example, set accuracy to 0.000001.
+\item
+  Now click on Button 2 shown below to generate the second set of parameters.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image041.png}
+\caption{}
+\end{figure}
+
+The simulation time would most likely be less but it depends on the accuracy value as well. The parameters generated will be displayed at Parameter 2.
+
+\begin{itemize}
+\item
+  Compare Error 2 to Error 1, the error values should be less which means that the parameters are getting better and more accurate.
+\item
+  Repeat the steps in 2a and 2b until a desired set of error values is achieved or the errors stop decreasing
+\end{itemize}
+
+\subsubsection{Step 3: Generating EnergyPlus Input Parameters}\label{step-3-generating-energyplus-input-parameters-000}
+
+\begin{itemize}
+\tightlist
+\item
+  Click on the Button 3 shown below to convert and arrange the parameters generated to fit EnergyPlus Input File (IDF), which will be listed from cell B52:B61.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image050.png}
+\caption{}
+\end{figure}
+
+\begin{itemize}
+\tightlist
+\item
+  The button shown below in worksheet ``ParamEstimator'' is used for clearing Initial Guess (2-5), Parameters(1-5), Error(1-5), EnergyPlus Input parameters and Result(1-5) in worksheet ``RESULT''.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image051.png}
+\caption{}
+\end{figure}
+
+\subsection{End Parameter Estimation Procedure}\label{end-parameter-estimation-procedure-000}
+
+\subsection{Curve Fit Model Procedure}\label{curve-fit-model-procedure-000}
+
+\subsubsection{Step 2: Generating the coefficients (Curve-Fit Model)}\label{step-2-generating-the-coefficients-curve-fit-model-000}
+
+\begin{itemize}
+\item
+  Using the contents of Table~\ref{table:lst-file-structure}, the program can generate the coefficients. The user must fill all the cells colored light blue in worksheet ``CoeffCalculator''.
+\item
+  \textbf{RatedAirVolFlowRate:} Rated volumetric air flow rate (m\(^{3}\)/s) which corresponds to the highest total cooling capacity listed in the catalog data.
+\item
+  \textbf{RatedWaterVolFlowRate:} Rated volumetric water flow rate (m\(^{3}\)/s) which corresponds to the highest total cooling capacity listed in the catalog data.
+\item
+  \textbf{RatedTotalCap:} Rated total cooling capacity (W) which is the highest total cooling capacity listed in the catalog data.
+\item
+  \textbf{RatedSensCap:} Rated sensible cooling capacity (W) which corresponds to the highest total cooling capacity listed in the catalog data.
+\item
+  \textbf{RatedPower:} Rated power consumption (W) which corresponds to the highest total cooling capacity listed in the catalog data.
+\item
+  Now click on Button 2 shown below to calculate the coefficients.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image052.png}
+\caption{}
+\end{figure}
+
+\begin{itemize}
+\item
+  The coefficients for the corresponding curves are listed at cell B12:D17. Error analysis of model are listed at cell B19:B30.
+\item
+  The errors for all the individual catalog data points are displayed in worksheet ``RESULT''.
+\item
+  The button shown below in worksheet ``CoeffCalculator'' is used for clearing the coefficients, the error analysis and the outputs in worksheet ``RESULT''.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image053.png}
+\caption{}
+\end{figure}
+
+\subsection{End Curve Fit Model Procedure}\label{end-curve-fit-model-procedure-000}
diff --git a/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-water-heat-pump-parameter.tex b/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-water-heat-pump-parameter.tex
new file mode 100644
index 00000000000..6300cd07e40
--- /dev/null
+++ b/doc/auxiliary-programs/src/parametric-spreadsheets/water-to-water-heat-pump-parameter.tex
@@ -0,0 +1,203 @@
+\section{Water-to-Water Heat Pump Parameter / Coefficient Generator (Cooling and Heating Mode)}\label{water-to-water-heat-pump-parameter-coefficient-generator-cooling-and-heating-mode}
+
+This document gives brief instructions on generating the parameters/ coefficients for the water-to-water heat pump models in cooling and heating mode. The Excelâ„¢ spreadsheets (WaterWater\_PE\_Cooling.xls and WaterWater\_PE\_Heating.xls) are used. Since the spreadsheet functions are very similar for both cooling and heating modes, only one instruction document is supplied. The spreadsheet generates:
+
+\begin{itemize}
+\item
+  parameters for the parameter estimation based model.
+\item
+  coefficients for the curve-fit model.
+\end{itemize}
+
+The following theses have detailed information about the curve-fit model and parameter estimation based model:
+
+Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at \href{http://www.hvac.okstate.edu}{www.hvac.okstate.edu})
+
+Shenoy,Arun. 2004. Simulation, Modeling and Analysis of Water to Air Heat Pump. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at \href{http://www.hvac.okstate.edu}{www.hvac.okstate.edu})
+
+Tang,C.C. 2004. Modeling Packaged Heat Pumps in a Quasi-Steady State Energy Simulation Program. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at \href{http://www.hvac.okstate.edu}{www.hvac.okstate.edu})
+
+\subsection{Step 1: Catalog Data Input}\label{step-1-catalog-data-input-001}
+
+Data points are obtained from the heat pump manufacturer data. Minimum data points for the parameter estimation based model are 32 data points according to Jin (2002). The curve-fit model performance is not affected by the number of data points and a minimum of 5 data points is required since the governing equations require 6 coefficients. The data points must have varying inlet conditions (e.g.~water flow rates, inlet water temperatures, etc.) that covers the entire range of the heat pump operating conditions. Correction tables provided by the manufacturer should be used to extend the catalog data range in order to have a good set of parameters/coefficients.
+
+\begin{itemize}
+\item
+  Using the heat pump performance data, enter the values to Table~\ref{table:comparison-of-ee-with-esp-rdoe-2blast-weather} in worksheet ``CATALOG DATA''. The values can be in SI or IP units.
+\item
+  Click on Button 1 based on the units used.
+\end{itemize}
+
+For IP units:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image037.png}
+\caption{}
+\end{figure}
+
+For SI units:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image038.png}
+\caption{}
+\end{figure}
+
+\begin{itemize}
+\item
+  The program will convert the values to the desired units and display them on Table~\ref{table:input-file-extensions-with-implied-data-types} in worksheet ``INPUT''.
+\item
+  The button shown below is used clearing Table~\ref{table:comparison-of-ee-with-esp-rdoe-2blast-weather} (worksheet ``CATALOG DATA''), and Table~\ref{table:input-file-extensions-with-implied-data-types} (worksheet ``INPUT''). It is advisable to clear the tables before generating parameters/coefficients for a new heat pump model.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image039.png}
+\caption{}
+\end{figure}
+
+After Table~\ref{table:input-file-extensions-with-implied-data-types} is created, the parameters/coefficients are then calculated as follows:
+
+\begin{itemize}
+\item
+  Worksheet ``ParamEstimator'' is used for generating the parameters for the parameter estimation based model using Nelder Mead Simplex. Refer to the steps in the Parameter Estimation Procedure.
+\item
+  Worksheet ``CoeffCalculator'' is used for calculate the coefficients for the curve-fit model using the generalized least square method. Refer to the steps in the Curve Fit Model procedure.
+\end{itemize}
+
+\subsection{Parameter Estimation Procedure}\label{parameter-estimation-procedure-001}
+
+\subsubsection{Step 2a: Generating First Set of Parameters (PE-Based Model)}\label{step-2a-generating-first-set-of-parameters-pe-based-model-001}
+
+\begin{itemize}
+\item
+  Using Table~\ref{table:input-file-extensions-with-implied-data-types}, the program can generate parameters. The user must fill all the cells colored light blue in worksheet ``ParamEstimator''.
+\item
+  \textbf{Accuracy:} Start with a low accuracy for faster convergence, recommended value of 0.001.
+\item
+  \textbf{Compressor Type:} Only reciprocating compressor is currently available in EnergyPlus. One might be able to generate parameters for heat pump model with different compressor types but this might result in unrealistic parameters.
+\item
+  \textbf{Refrigerant:} Contact the manufacturer on the refrigerant used to generate the catalog data and select from the list of refrigerants. Usually the refrigerant used is R22. .
+\item
+  \textbf{Which Initial Guess?:} The user may choose a set of initial guesses(1-5) that will be used by the optimization routine in generating the parameters. Start with 1, which is the set of initial guess 1 at column B.
+\item
+  \textbf{Initial Guess:} Initial guess for all the parameters. For Initial Guess 1, enter a value of 1 for all the parameters except for the loss factor (less than 1.0). The loss factor should be less than 1.0 because the efficiency of the compressor should be less than 100\%. Adjust the values in Initial Guess 1 if the program happens to crash and try again.
+\item
+  Now click on Button 2 shown below to generate the parameters.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image040.png}
+\caption{}
+\end{figure}
+
+It will take some time to generate the parameters depending on the number of data points. The parameters generated will be displayed at Parameters 1.
+
+\begin{itemize}
+\item
+  Look at the error analysis of Error 1 which gives the user a summary of the errors for Qload, Qsource and Power. An average error of 5-8\% is achievable for all the values.
+\item
+  The errors for all the individual catalog data points are displayed in worksheet ``RESULT''.
+\end{itemize}
+
+\subsubsection{Step 2b: Improving the Set of Parameters (PE-Based Model)}\label{step-2b-improving-the-set-of-parameters-pe-based-model-001}
+
+\begin{itemize}
+\item
+  After the initial set of parameters has been generated, the user can increase the accuracy of the parameters by using parameters generated as the initial guess for the second simulation and increasing the accuracy of the program.
+\item
+  Copy and Paste Parameters 1 to Initial Guess 2.
+\item
+  Change the initial guess indicator (\textbf{Which Initial Guess?:)} from 1 to 2.
+\item
+  Increase the accuracy by twice. For example, set accuracy to 0.000001.
+\item
+  Now click on Button 2 shown below to generate the second set of parameters.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image041.png}
+\caption{}
+\end{figure}
+
+The simulation time would most likely be less but it depends on the accuracy value as well. And the parameters generated will be displayed at Parameter 2.
+
+\begin{itemize}
+\item
+  Compare Error 2 to Error 1, the error values should be less which means that the parameters are getting better and more accurate.
+\item
+  Repeat the steps in 2a and 2b until a desired set of error values is achieved or the errors stop decreasing
+\end{itemize}
+
+\subsubsection{Step 3: Generating EnergyPlus Input Parameters}\label{step-3-generating-energyplus-input-parameters-001}
+
+\begin{itemize}
+\tightlist
+\item
+  Click on the Button 3 shown below to convert and arrange the parameters generated to fit EnergyPlus Input File (IDF) which will be listed from cell B52:B59 for cooling mode and B46:B54 for heating mode.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image042.png}
+\caption{}
+\end{figure}
+
+\begin{itemize}
+\tightlist
+\item
+  The button shown below in worksheet ``ParamEstimator'' is used for clearing Initial Guess (2-5), Parameters(1-5), Error(1-5), EnergyPlus Input parameters and Result(1-5) in worksheet ``RESULT''.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image043.png}
+\caption{}
+\end{figure}
+
+\subsection{End Parameter Estimation Procedure}\label{end-parameter-estimation-procedure-001}
+
+\subsection{Curve Fit Model Procedure}\label{curve-fit-model-procedure-001}
+
+\subsubsection{Step 2: Generating the coefficients (Curve-Fit Model)}\label{step-2-generating-the-coefficients-curve-fit-model-001}
+
+\begin{itemize}
+\item
+  Using Table~\ref{table:input-file-extensions-with-implied-data-types}, the program is ready to generate the coefficients. User is required to fill all the cells colored light blue in worksheet ``CoeffCalculator''.
+\item
+  \textbf{RatedLoadVolFlowRate:} Rated load side volumetric flow rate (m\(^{3}\)/s) which corresponds to the highest load side heat transfer rate listed in the catalog data.
+\item
+  \textbf{RatedSourceVolFlowRate:} Rated source side volumetric flow rate (m\(^{3}\)/s) which corresponds to the highest load side heat transfer rate listed in the catalog data.
+\item
+  \textbf{RatedQload:} Rated load side heat transfer rate (W) which is the highest load side heat transfer rate listed in the catalog data.
+\item
+  \textbf{RatedPower:} Rated power consumption (W) which corresponds to the highest load side heat transfer rate listed in the catalog data.
+\item
+  Now click on Button 2 shown below to calculate the coefficients.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image044.png}
+\caption{}
+\end{figure}
+
+\begin{itemize}
+\item
+  The coefficients for the corresponding curves are listed at cell B12:C16. Error analysis of model is listed at cell B19:B27.
+\item
+  The errors for all the individual catalog data points are displayed in worksheet ``RESULT''.
+\item
+  The button shown below in worksheet ``CoeffCalculator'' is used for clearing the coefficients, the error analysis and the outputs in worksheet ``RESULT''.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image045.png}
+\caption{}
+\end{figure}
+
+\subsection{End Curve Fit Model Procedure}\label{end-curve-fit-model-procedure-001}
diff --git a/doc/auxiliary-programs/src/parametricpreprocessor.tex b/doc/auxiliary-programs/src/parametricpreprocessor.tex
new file mode 100644
index 00000000000..ab80991cc1a
--- /dev/null
+++ b/doc/auxiliary-programs/src/parametricpreprocessor.tex
@@ -0,0 +1,27 @@
+\chapter{ParametricPreprocessor}\label{parametricpreprocessor}
+
+The parametric preprocessor used to create a series of resulting IDF files from a single source IDF file that contains parametric objects and expressions. The parametric objects in EnergyPlus are interpreted by the ParametricPreprocessor and are:
+
+\begin{itemize}
+\tightlist
+\item
+  Parametric:SetValueForRun
+\item
+  Parametric:Logic
+\item
+  Parametric:RunControl
+\item
+  Parametric:FileNameSuffix
+\end{itemize}
+
+The ParametricPreprocessor reads the source IDF file and removes the Parametric objects shown above, processes these objects and any embedded expressions and produces a series of resulting IDF files, one for each ``run'' described by the objects.
+
+An intermediate file called parametric.int is used that contains references to all embedded expressions that will need to be substituted into the file.
+
+An error file called parametric.err is also produced to help debug problems with the objects.
+
+The Parametric objects are described in detail in the InputOutputReference document.
+
+ParametricPreprocessor can be called at the command line with the name of the source file as the only argument.
+
+The ParametricPreprocessor is used in the batch files that come with EnergyPlus and is used by EP-Launch automatically.
diff --git a/doc/auxiliary-programs/src/running-console-applications.tex b/doc/auxiliary-programs/src/running-console-applications.tex
new file mode 100644
index 00000000000..c090f40feda
--- /dev/null
+++ b/doc/auxiliary-programs/src/running-console-applications.tex
@@ -0,0 +1,39 @@
+\chapter{Running Console Applications}\label{running-console-applications}
+
+Several of the auxiliary programs included with EnergyPlus are Console Applications. This designation means that they are executed from the ``command window'' (Windows OS) or terminal window (Linux OS). We will include generic instructions for the Windows OS use of these applications in this section. Each program will also include specifics for the Windows OS in the individual program documentation.
+
+As installed, the batch files that accompany console applications will be set so that file extensions are not included for input parameters, paths to installed data (such as weather data) will be set automatically, and these paths can be modified by the user as desired. (Instructions included a bit later in this section).
+
+Generally, the steps for executing a console application is:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Open a DOS command prompt window (Start à Programs à Accessories à Command Prompt)
+\item
+  Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
+\end{enumerate}
+
+C:
+
+CD \textbackslash{}\textless{}root folder\textgreater{}\textless{}/span\textgreater{}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Change to the specific folder for the console application:
+\end{enumerate}
+
+CD \textless{}folder\textgreater{}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Run the program:
+\end{enumerate}
+
+\textless{}batchfile\textgreater{} \textless{}input parameters\textgreater{}
diff --git a/doc/auxiliary-programs/src/running-console-applications/modifying-the-batch-file.tex b/doc/auxiliary-programs/src/running-console-applications/modifying-the-batch-file.tex
new file mode 100644
index 00000000000..c61edbc242b
--- /dev/null
+++ b/doc/auxiliary-programs/src/running-console-applications/modifying-the-batch-file.tex
@@ -0,0 +1,48 @@
+\section{Modifying the batch file}\label{modifying-the-batch-file}
+
+Generally, the batch files set several environment variables that govern the execution of the specific program.
+
+% table 32
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Environment Variables used in Batch Files \label{table:environment-variables-used-in-batch-files}} \tabularnewline
+\toprule 
+Environment Variable Name & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Environment Variables used in Batch Files} \tabularnewline
+\toprule 
+Environment Variable Name & Description \tabularnewline
+\midrule
+\endhead
+
+Program Path & Specific or relative program path \tabularnewline
+Program Name & Name of program \tabularnewline
+Input\_Path & Input Path Specification \tabularnewline
+Output\_Path & Output Path Specification \tabularnewline
+Weather\_Path & Weather Data Path Specification \tabularnewline
+\bottomrule
+\end{longtable}
+
+Or, as seen in the batch file text:
+
+\begin{lstlisting}
+:Instructions:
+:  Complete the following path and program names.
+:  path names must have a following \ or errors will happen
+ set program_path =
+ set program_name = <specific program name will be here>
+ set input_path =
+ set output_path =
+ set weather_path = ..\..\WeatherData\
+\end{lstlisting}
+
+As the instructions in the batch file show, the path character must terminate the path specification or errors can occur. The ``weather\_path'' specification shows an example of using a ``relative'' path specification. Depending on the program, this specification, of course, might change.
+
+\begin{lstlisting}
+set weather_path = ..\..\WeatherData\
+\end{lstlisting}
+
+What the specification says is that above (..) and above again (..) and then ``WeatherData'' is where the weather data files are located. This kind of relative path would be true for most ``Preprocess'' programs in the installed folders. The following illustrates the folder tree: (this is usually EnergyPlusV) Preprocess Specific Program Folders WeatherData
+
+Thus, the user can simply put the name of the weather data file onto the batch file run and it will look for that file in the installed WeatherData folder.
diff --git a/doc/auxiliary-programs/src/technical-details-of-running-energyplus.tex b/doc/auxiliary-programs/src/technical-details-of-running-energyplus.tex
new file mode 100644
index 00000000000..33c81ff4a0e
--- /dev/null
+++ b/doc/auxiliary-programs/src/technical-details-of-running-energyplus.tex
@@ -0,0 +1,3 @@
+\chapter{Technical Details of Running EnergyPlus}\label{technical-details-of-running-energyplus}
+
+This section will contain the details of running EnergyPlus - more (and some duplicated) information on EP-Launch (basic discussion included in the Getting Started manual) and ``by hand'' - describing the batch files that are included with the install. The first parts of this section deal with using EnergyPlus on a Wintel/Windows OS system. Though similar commands can be used on other OS - such as Linux, they will not be exactly the same commands (usually).
diff --git a/doc/auxiliary-programs/src/technical-details-of-running-energyplus/energyplus-file-extensions.tex b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/energyplus-file-extensions.tex
new file mode 100644
index 00000000000..7e945f7547a
--- /dev/null
+++ b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/energyplus-file-extensions.tex
@@ -0,0 +1,135 @@
+\section{EnergyPlus File Extensions}\label{energyplus-file-extensions}
+
+This section will present a list (perhaps not complete) of EnergyPlus file extensions and what they mean. This will help you after the EP-Launch program finishes.
+
+\subsection{Input Files}\label{input-files}
+
+The following files are input to the EnergyPlus program.
+
+\subsubsection{IDD}\label{idd}
+
+The \emph{input data dictionary} (IDD) is an ascii (text) file containing a list of all possible EnergyPlus objects and a specification of the data each object requires. This file is analogous to the DOE-2 keyword file. The \emph{Guide for Interface Developers} contains a full description of the input data dictionary.
+
+\subsubsection{idf}\label{idf}
+
+The \emph{input data file} (IDF) is an ascii file containing the data describing the building and HVAC system to be simulated. Many example files are installed as part of the EnergyPlus installation. Additionally, a spreadsheet file ``ExampleFiles.xls'' contains columnar descriptions of each file's features.
+
+\subsubsection{imf}\label{imf}
+
+The \emph{input macro file} (IMF) is an ascii file containing the data describing the building and HVAC system to be simulated and will have some contents of ``macro'' commands. The Auxiliary programs document describes use of the macro commands and the program that processes them - EP-Macro. Many example files are installed as part of the EnergyPlus installation.
+
+\subsubsection{ini}\label{ini}
+
+This is the EnergyPlus initialization file. It is an optional ascii input file that allows the user to specify the path for the directory containing Energy+.idd. This file, using the actual directories of the install, will be created during the install. Unless you change where the EnergyPlus.exe file resides, you will not need to change this file.
+
+\subsubsection{epw}\label{epw}
+
+The \emph{EnergyPlus weather} file is an ascii file containing the hourly or sub-hourly weather data needed by the simulation program. The data format is described in detail in the Auxiliary Programs Document. It is also described succinctly in the Input Output Reference document.
+
+\subsection{Output Files}\label{output-files}
+
+More information (and more up-to-date) about output files is shown in the \href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details and Examples} Document.
+
+\subsubsection{err}\label{err}
+
+A text file containing the error messages issued by EnergyPlus. \textbf{This is the first output that should be examined after a simulation.}Error messages may be issued by EnergyPlus during its input phase or during the simulation. There are three levels of error severity: \emph{fatal}, \emph{severe}, and \emph{warning} as well as simple \emph{``message''} lines. A fatal error causes the program to terminate immediately. The following table illustrates the necessary actions.
+
+% table 33
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Error Message Levels - Required Actions \label{table:error-message-levels-required-actions}} \tabularnewline
+\toprule 
+Error Level & Action \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Error Message Levels - Required Actions} \tabularnewline
+\toprule 
+Error Level & Action \tabularnewline
+\midrule
+\endhead
+
+Information & Informative, usually a follow-on to one of the others. No action required. \tabularnewline
+Warning & Take note. Fix as applicable. \tabularnewline
+Severe & Should Fix \tabularnewline
+Fatal & Program will abort \tabularnewline
+\bottomrule
+\end{longtable}
+
+An example of an error message due to an input syntax error is:
+
+\begin{lstlisting}
+** Severe  ** Did not find " DessignDay" in list of Objects
+   **  Fatal  ** Errors occurred on processing IDF file -
+       probable incorrect IDD file. View "audit.out" for details.
+   ************* EnergyPlus Terminated--Error(s) Detected.
+\end{lstlisting}
+
+\subsubsection{audit}\label{audit}
+
+This is an text file which echoes the IDD and IDF files, flagging syntax errors in either file. Note that both \emph{err} and \emph{audit} will show most of the error messages caused by input syntax errors; however only \emph{err} will show errors issued during the actual simulation. The \emph{audit} can be used when you need to see the context of the error message to fully ascertain the cause. The \emph{audit} file also contains potentially extra information that may be useful from the input scan.
+
+\subsubsection{eso}\label{eso}
+
+The \emph{EnergyPlus Standard Output} (ESO) is a text file containing the time varying simulation output. The format of the file is discussed in the \emph{Guide for Interface Developers} and the \emph{InputOutputReference}. The contents of the file are controlled by \emph{Output:Variable} commands in the IDF file. Although the ESO is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
+
+\subsubsection{mtr}\label{mtr}
+
+The \emph{EnergyPlus Meter Output} (MTR) is a text file containing the time varying simulation output. The format of the file is similar to the ESO file. As described in the Getting Started document, meters are a powerful reporting tool in EnergyPlus. Values are grouped onto logical meters and can be viewed the same way that the ESO variables are used. The contents of the file are controlled by \emph{Output:Meter} commands in the IDF file. Although the MTR is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
+
+\subsubsection{mtd}\label{mtd}
+
+This file contains all the details (i.e., which report variables are on a meter and, conversely, what meters contain) about meters.
+
+\subsubsection{eio}\label{eio}
+
+The \emph{EnergyPlus Invariant Output} (EIO) is a text file containing output that does not vary with time. For instance, location information (latitude, longitude, time zone, altitude) appears on this file.
+
+\subsubsection{rdd}\label{rdd}
+
+\subsubsection{mdd}\label{mdd}
+
+The \emph{Report (variable) Data Dictionary} (RDD) is a text file listing those variables available for reporting (on the ESO) for this particular simulation. Which variables are available for output depends on the actual simulation problem described in the IDF. The \emph{Report (meter) Data Dictionary} (MDD) is a text file listing those variables available for reporting (on the MTR) for this particular simulation. Which meters are available for output depends on the actual simulation problem described in the IDF. A simulation with no chiller would not permit the output of any chiller report variables. The user may need to examine the RDD or MDD to find out which report variables are available in a particular simulation. The RDD and MDD are written only if the following is included in the IDF file.
+
+\begin{lstlisting}
+Output:VariableDictionary, Regular;
+\end{lstlisting}
+
+A variant produces the same files in a IDF ``ready'' format.
+
+\begin{lstlisting}
+Output:VariableDictionary, IDF;
+\end{lstlisting}
+
+\subsubsection{dbg}\label{dbg}
+
+This is a text file containing \emph{debug} output for use by EnergyPlus developers. Generally developers will add debug print statements wherever in the code that that they wish. There is a ``standard'' debug output that prints out conditions at all the HVAC nodes. This output is triggered by placing
+
+\begin{lstlisting}
+Output:DebuggingData,1;
+\end{lstlisting}
+
+in the IDF file. If Output:DebuggingData, 0 is entered, you will get an empty eplusout.dbg file.
+
+\subsubsection{dxf}\label{dxf}
+
+This is a file in AutoCad DXF format showing all the surfaces defined in the IDF file. It provides a means of viewing the building geometry. The DXF file from EnergyPlus highlights different building elements (shading, walls, subsurfaces) in differing colors. A number of programs can read and display DXF files. Output of this file is triggered by
+
+\begin{lstlisting}
+Output:Reports, Surfaces, DXF;
+\end{lstlisting}
+
+in the IDF.
+
+\subsubsection{sln}\label{sln}
+
+A text file containing the coordinates of the vertices of the surfaces in the IDF.
+
+Output of this file is triggered by
+
+Output:Reports, Surfaces, Lines;
+
+in the IDF.
+
+\subsection{Postprocessing Program/Files}\label{postprocessing-programfiles}
+
+A postprocessing program \emph{ReadVarsESO.exe} is available that will read an ESO or MTR file and produce a file that can be read by Excelâ„¢. It can use an input file or not. In batch mode it is run by the little batch file \emph{RunReadESO.bat}: Further information on this program is provided in the \href{file:///E:/Docs4PDFs/InputOutputReference.pdf}{Input Output Reference} under a section heading called ``Using ReadVarsESO''.
diff --git a/doc/auxiliary-programs/src/technical-details-of-running-energyplus/energyplus-files.tex b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/energyplus-files.tex
new file mode 100644
index 00000000000..c9738962ba3
--- /dev/null
+++ b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/energyplus-files.tex
@@ -0,0 +1,143 @@
+\section{EnergyPlus Files}\label{energyplus-files}
+
+\subsection{Input Files}\label{input-files-000}
+
+The following files are input to the EnergyPlus program.
+
+\subsubsection{Energy+.idd}\label{energy.idd}
+
+The \emph{input data dictionary} (IDD) is an ascii (text) file containing a list of all possible EnergyPlus objects and a specification of the data each object requires. This file is analogous to the DOE-2 keyword file. The \emph{Guide for Interface Developers} contains a full description of the input data dictionary.
+
+\subsubsection{in.idf}\label{in.idf}
+
+The \emph{input data file} (IDF) is an ascii file containing the data describing the building and HVAC system to be simulated. The \emph{Guide for Interface Developers} shows examples of IDF input. Many example files are installed as part of the EnergyPlus installation.
+
+\subsubsection{in.imf}\label{in.imf}
+
+The \emph{input macro file} (IMF) is an ascii file that is formatted for the EP-Macro program. Output from the EP-Macro program will be the standard in.idf format. IMF files are not directly read by EnergyPlus.
+
+\subsubsection{Energy+.ini}\label{energy.ini}
+
+This is the EnergyPlus initialization file. It is an optional ascii input file that allows the user to specify the path for the directory containing Energy+.idd. This file, using the actual directories of the install, will be created during the install. An example is:
+
+\begin{lstlisting}
+[program]
+dir = C:\EnergyPlus
+\end{lstlisting}
+
+\begin{lstlisting}
+[weather]
+dir =
+\end{lstlisting}
+
+\begin{lstlisting}
+[BasementGHT]
+dir = PreProcess\GrndTempCalc
+\end{lstlisting}
+
+\begin{lstlisting}
+[SlabGHT]
+dir = PreProcess\GrndTempCalc
+\end{lstlisting}
+
+Under {[}program{]}, dir should indicate the folder where EnergyPlus is installed (e.g.~C:\textbackslash{}Program Files\textbackslash{}EnergyPlusV2-0-0 or C:\textbackslash{}EnergyPlusV2-0-0). This is automatically generated during the install and may be the ``shortened form'' of these folder names. The ``weather'' portion of the initialization file is unused for normal EnergyPlus. {[}BasementGHT{]} and {[}SlabGHT{]} are used by the EP-Launch program when the Utilities tab is used to execute the Basement and Slab programs, respectively.
+
+\subsubsection{in.epw}\label{in.epw}
+
+The \emph{EnergyPlus weather} file is an ascii file containing the hourly or sub-hourly weather data needed by the simulation program. The data format is described in this document in the section: EnergyPlus Weather File (EPW) Data Dictionary.
+
+\subsection{Output Files}\label{output-files-000}
+
+More information (and more up-to-date) about output files is shown in the \href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details and Examples} Document.
+
+\subsubsection{eplusout.err}\label{eplusout.err}
+
+A text file containing the error messages issued by EnergyPlus. This is the first output that should be examined after a simulation. Error messages are issued by EnergyPlus during its input phase or during the simulation. There are three levels of error severity: \emph{fatal}, \emph{severe}, and \emph{warning} as well as simple \emph{``message''} lines. A fatal error causes the program to terminate immediately. The following table illustrates the necessary actions.
+
+% table 34
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Error Message Levels - Required Actions \label{table:error-message-levels-required-actions-001}} \tabularnewline
+\toprule 
+Error Level & Action \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Error Message Levels - Required Actions} \tabularnewline
+\toprule 
+Error Level & Action \tabularnewline
+\midrule
+\endhead
+
+"Information" & Informative, usually a follow-on to one of the others. No action required. \tabularnewline
+Warning & Take note. Fix as applicable. \tabularnewline
+Severe & Should Fix \tabularnewline
+Fatal & Program will abort \tabularnewline
+\bottomrule
+\end{longtable}
+
+An example of an error message due to an input syntax error is:
+
+\begin{lstlisting}
+** Severe  ** Did not find " DessignDay" in list of Objects
+   **  Fatal  ** Errors occurred on processing IDF file -
+       probable incorrect IDD file. View "audit.out" for details.
+   ************* EnergyPlus Terminated--Error(s) Detected.
+\end{lstlisting}
+
+\subsubsection{eplusout.audit}\label{eplusout.audit}
+
+This is an text file which echoes the IDD and IDF files, flagging syntax errors in either file. Note that both \emph{eplusout.err} and \emph{eplusout.audit} will show the error messages caused by input syntax errors; however only \emph{eplusout.err} will show errors issued during the actual simulation. \emph{eplusout.audit} can be used when you need to see the context of the error message to fully ascertain the cause.
+
+\subsubsection{eplusout.eso}\label{eplusout.eso}
+
+The \emph{EnergyPlus Standard Output} (ESO) is a text file containing the time varying simulation output. The format of the file is discussed in the \emph{Guide for Interface Developers} and the \emph{InputOutputReference}. The contents of the file are controlled by \emph{Report Variable} commands in the IDF file. Although the ESO is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
+
+\subsubsection{eplusout.mtr}\label{eplusout.mtr}
+
+The \emph{EnergyPlus Meter Output} (MTR) is a text file containing the time varying simulation output. The format of the file is similar to the ESO file. Meters are a powerful reporting tool in EnergyPlus. Values are grouped onto logical meters and can be viewed the same way that the ESO variables are used. The contents of the file are controlled by \emph{Report Meter} commands in the IDF file. Although the MTR is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
+
+\subsubsection{eplusout.eio}\label{eplusout.eio}
+
+The \emph{EnergyPlus Invariant Output} (EIO) is a text file containing output that does not vary with time. For instance, location information (latitude, longitude, time zone, altitude) appears on this file.
+
+\subsubsection{eplusout.rdd}\label{eplusout.rdd}
+
+The \emph{Report (variable) Data Dictionary} (RDD) is a text file listing those variables available for reporting (on the ESO or MTR) for this particular simulation. Which variables are available for output on the ESO or MTR depends on the actual simulation problem described in the IDF. A simulation with no chiller would not permit the output of any chiller report variables. The user may need to examine the RDD to find out which report variables are available in a particular simulation. The RDD is written only if
+
+\begin{lstlisting}
+Output:VariableDictionary, <either Regular or IDF>;
+\end{lstlisting}
+
+appears in the input (IDF) file.
+
+\subsubsection{eplusout.dbg}\label{eplusout.dbg}
+
+This is a text file containing \emph{debug} output for use by EnergyPlus developers. Generally developers will add debug print statements wherever in the code that that they wish. There is a ``standard'' debug output that prints out conditions at all the HVAC nodes. This output is triggered by placing
+
+DEBUG OUTPUT,1;
+
+in the IDF file. If DEBUG OUTPUT, 0 is entered, you will get an empty eplusout.dbg file.
+
+\subsubsection{eplusout.dxf}\label{eplusout.dxf}
+
+This is a file in AutoCad DXF format showing all the surfaces defined in the IDF file. It provides a means of viewing the building geometry. The DXF file from EnergyPlus highlights different building elements (shading, walls, subsurfaces) in differing colors. A number of programs can read and display DXF files. One that works well is Volo View Express, available free from the Autodesk web site. Output of this file is triggered by
+
+Report, Surfaces, DXF;
+
+in the IDF.
+
+\subsubsection{eplusout.sln}\label{eplusout.sln}
+
+A text file containing the coordinates of the vertices of the surfaces in the IDF.
+
+Output of this file is triggered by
+
+Report, Surfaces, Lines;
+
+in the IDF.
+
+\subsection{Postprocessing Program/Files}\label{postprocessing-programfiles-000}
+
+A postprocessing program \emph{ReadVarsESO.exe} is available that will read an ESO or MTR file and produce a file that can be read by Excelâ„¢. It can use an input file or not. In batch mode it is run by the little batch file \emph{RunReadESO.bat}: Further information on this program is provided in the \href{file:///E:/Docs4PDFs/InputOutputReference.pdf}{Input Output Reference} as well as the \href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details and Examples} documents.
+
+You can also used the CSVProc and convertESOMTR described earlier in this document as part of your post processing strategy.
diff --git a/doc/auxiliary-programs/src/technical-details-of-running-energyplus/ep-launch-lite.tex b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/ep-launch-lite.tex
new file mode 100644
index 00000000000..6333436b079
--- /dev/null
+++ b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/ep-launch-lite.tex
@@ -0,0 +1,3 @@
+\section{EP-Launch Lite}\label{ep-launch-lite}
+
+EP-Launch Lite is a small application included with the EnergyPlus Macintosh installation. It is a small GUI application that provides a simple way to run EnergyPlus models. Its purpose is similar to EP-Launch but it is a much simpler application with fewer features.
diff --git a/doc/auxiliary-programs/src/technical-details-of-running-energyplus/ep-launch-program.tex b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/ep-launch-program.tex
new file mode 100644
index 00000000000..759b0353b8c
--- /dev/null
+++ b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/ep-launch-program.tex
@@ -0,0 +1,393 @@
+\section{EP-Launch Program}\label{ep-launch-program}
+
+EP-Launch is an optional component of the EnergyPlus Windows installation (it is not available for Linux and Mac platforms). For users that want a simple way of selecting files and running EnergyPlus, EP-Launch provides this and more. In addition, EP-Launch can help open a text editor for the input and output files, open a spreadsheet for the postprocessor results files, a web browser for the tabular results file, and start up a viewer for the selected drawing file.
+
+\begin{figure}[hbtp] % fig 35
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image101.png}
+\caption{EP-Launch Screen \protect \label{fig:ep-launch-screen}}
+\end{figure}
+
+\subsection{Start EP-Launch}\label{start-ep-launch}
+
+EP-Launch is located in the main directory/folder for EnergyPlus. In addition, it is available on the shortcut menu for EnergyPlus. By double clicking on the EP-Launch icon you get the screen shown above (Figure~\ref{fig:ep-launch-screen}) for running a single input file. The EP-Launch program simply starts other programs and allows you to avoid having to use the DOS command line prompt to run EnergyPlus. More help is provided for the program under the ``Help'' menu.
+
+\subsection{Selecting Input and Weather Files}\label{selecting-input-and-weather-files}
+
+The input file and weather files can be selected on the Single Input File tab from the two pull down lists which show recently used files or you can press the ``Browse\ldots{}'' buttons to locate an input or weather file that you have created yourself. If this is your first time using EP-Launch, the pull down lists will show some files from the ExampleFiles subdirectory. These are not the only examples, use browse to open other example files from the ExampleFiles subdirectory or other EnergyPlus input files.
+
+\subsection{Running a Single Input File}\label{running-a-single-input-file}
+
+On the Single Input File tab, after you select the weather and input files simply push the ``Simulate\ldots{}'' button to start the EnergyPlus building energy simulation engine. At this point a black DOS window should pop up on your screen and show the progress of your simulation. The simulation is complete when the black DOS box closes. The EnergyPlus program black DOS window will show scrolling text as the simulation procedure progresses. If you would like to see these messages more slowly you have two options:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Press the ``Control-S'' key combination to try to stop the progress and any key to continue.
+\item
+  Under the ``View'' menu on the EP-Launch program, select ``Options'' then ``Command Window'' then check ``Pause During Simulation'' and this will pause the process immediately after EnergyPlus executes. To continue after the pause, press any key.
+\end{enumerate}
+
+If the file contains Parametric objects, the single input file may cause multiple simulations to be performed. If multiple simulations are performed, the output files will be listed on the History tab and will be named with either the file suffixes defined in the input file or with a serial number.
+
+Multiple single input file and group simulations can be started at the same time. On a computer with multiple-processors or multiple-cores, this will enable the simulations to complete more quickly than starting one after another.
+
+\subsection{Looking at the Results}\label{looking-at-the-results}
+
+After you have run a simulation and the black DOS window closes, EnergyPlus has completed, and a status message is displayed (see figure below):
+
+\begin{figure}[hbtp] % fig 36
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image102.png}
+\caption{EP-Launch Finish Status. \protect \label{fig:ep-launch-finish-status.}}
+\end{figure}
+
+This status gives you a quick overview of whether there were warning (\textbf{should look at}), severe (\textbf{should probably fix}) or fatal (\textbf{must fix}) errors in the run as well as the time it took for the simulation to complete. After pressing ``OK'' from this box, selecting ``ERR/EIO/BND Output Files Only'' from the ``View'' menu will display the ERR, EIO, and BND files - useful when errors may have occurred. Alternatively, pressing the F2 function key will display the same three files.
+
+Another way to open files easily is by using the View Results buttons as shown in 29. Two different panels of buttons can be used under View Results, one shown by using the ``All'' tab on the left edge and by using the ``Sets'' tab on the left edge. The ``All'' tab shows all the various files by file extension that can be viewed individually. Files available for view based on the current input file name, are ``enabled'' (extension names clearly readable).
+
+\begin{figure}[hbtp] % fig 37
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image103.png}
+\caption{EP-Launch with the Sets tab of View Results \protect \label{fig:ep-launch-with-the-sets-tab-of-view-results}}
+\end{figure}
+
+The figure above shows the same main screen of EP-Launch but with the ``Sets'' tab selected on the left edge of the View Results section. The buttons on this tab can open many files at the same time and are a shortcut to opening the files that may be commonly used. The Text Output Files, Drawing Files, and Spreadsheets buttons cause several different results files to open at once based on the currently selected Input File. The HTML file opens just the tabular results file if that file was produced (see \emph{OutputControl:Table:Style}). The buttons labeled as Set 1 to Set 8 allow you to select which sets of files you want to open. Press the ``Define'' button in order to define the files to view.
+
+\begin{figure}[hbtp] % fig 38
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image104.png}
+\caption{Define Files to View \protect \label{fig:define-files-to-view}}
+\end{figure}
+
+When the ``Define'' button is pressed on the Sets tab of the View Results section of the main screen, the dialog box in the figure above is shown. This allows the files extensions to be selected that would be opened for each of the Set 1 to Set 8 buttons. One or many files can be selected for each of the Set buttons. This allows you to define exactly which files you want opened.
+
+The content of each file extension is listed below. The contents (along with examples) are discussed in the \href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details} document.
+
+By pressing the ``Text Output Files'' button, a text editor will open each of the text output files. Up to 29 files will open, if they exist. Selecting ``Single File'' from the `View' menu displays a menu of all available output files from which any file can be opened individually. Each file may also be opened with an associated function key. The output files and function key shortcuts are listed below:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Variable - tabulated results in comma, tab or space delimited format (generated by the ReadVarsESO postprocessor) (F4)
+\item
+  ESO - raw report variable output (F5),
+\item
+  RDD - list of output variables available from the run (F6).
+\item
+  MDD - list of output meters available from the run (Shift-Ctrl-F3)
+\item
+  EIO - additional EnergyPlus results (F7),
+\item
+  ERR - list of errors and warnings (F8),
+\item
+  BND - HVAC system node and component connection details (F9),
+\item
+  MTR - raw report meter output (F11),
+\item
+  MTD - list of meter component variables (F12)
+\item
+  METER File - tabulated meter report in comma, tab or space delimited format (generated by the ReadVarsESO postprocessor) (Ctrl-F4)
+\item
+  ZSZ - zone sizing details in comma, tab or space delimited format (Ctrl+F5)
+\item
+  SSZ - system sizing details in comma, tab or space delimited format (Ctrl+F6)
+\item
+  AUDIT - input file echo with input processor errors and warnings (Ctrl+F8)
+\item
+  SLN - output from ``report, surfaces, lines'' (Ctrl+F9)
+\item
+  DBG - output from the debug command (Ctrl+F11)
+\item
+  SHD - output related to shading (Ctrl+F12)
+\item
+  SVG - HVAC Diagram (Shift+ F4)
+\item
+  EPMIDF - clean idf file after EP-Macro processing (Shift+F5)
+\item
+  EPMDET - EP-Macro detailed output with errors and warnings (Shift+F6)
+\item
+  MAP - daylighting illuminance map (Shift+F7)
+\item
+  TABLE - tabulated report of bin and monthly data in comma, tab or space delimited or HTML format (Shift+F8)
+\item
+  VMRL - drawing file in VRML (Virtual Reality Markup Language) format (Shift F+F11)
+\item
+  DXF - drawing file in AutoCAD DXF format (Shift+F12)
+\item
+  Delight IN - DElight input generated from EnergyPlus processed input (Shift+Ctrl+F4)
+\item
+  Delight OUT - Detailed DElight output (Shift+Ctrl+F5)
+\item
+  Delight ELDMP - DElight reference point illuminance per time step (Shift+Ctrl+F6)
+\item
+  Delight DFDMP - DElight warning and error messages (Shift+Ctrl+F7)
+\item
+  EXPIDF - Expanded IDF when using HVACTemplate objects (Shift+Ctrl+F8)
+\item
+  Group Error - combined error files for a group run. (Shift+Ctrl+F9)
+\item
+  VCpErr - Transition program error file (Shift+Ctrl+F11)
+\item
+  Screen (Shift+Ctrl+f12)
+\item
+  Proc CSV - Simple statistiscs generated from CSVProc (also see Create Statistics File option under View-Options).
+\item
+  EDD - Energy Management System details.
+\end{enumerate}
+
+Clicking on the ``Drawing File'' button will open the generated DXF file if an appropriate viewer has been configured (see \emph{Selecting Viewers and Editors} below). The DXF file is a CAD format that displays the physical shape of the building being modeled in three dimensions. The ``Drawing File'' button also opens the HVAC diagram generated with the HVAC-Diagram utility (see Auxiliary Programs).
+
+Clicking on the ``Spreadsheets'' buttons will open any generated CSV files if an appropriate viewer has been configured (see \emph{Selecting Viewers and Editors} below).
+
+\subsection{Viewing the Drawing File without Running a Simulation}\label{viewing-the-drawing-file-without-running-a-simulation}
+
+The ``Drawing'' button (or the View menu Drawing File option) will automatically run EPDrawGUI if the DXF file does not exist or it is older than the input file. This allows the building geometry to be viewed without running a full simulation. For more information about EPDrawGUI, see the EPDrawGUI section in this document.
+
+\subsection{Editing the Input Files}\label{editing-the-input-files}
+
+The input file, called IDF file that is selected from the top pull-down list, can be edited by pressing one of two buttons in the ``Input File'' area. The ``Edit - Text Editor'' button will start a text editor and the ``Edit - IDF Editor'' will start the separate program called the IDF Editor. Remember to save any changes you make in either editor before returning to EP-Launch to run the simulations again.
+
+\subsection{File Menu}\label{file-menu}
+
+The File menu can be used for selecting input and weather files just like the ``Browse\ldots{}'' buttons (see the \emph{Selecting Input and Weather Files} section above)
+
+If you are upgrading from the previous version of EnergyPlus you can use the ``File'', ``Transition'' menu option to upgrade your EnergyPlus input files (IDF and IMF) to the most recent version (see the section Using Older Version Input Files - Transition for more information about the Transition program). This EP-Launch option only works for upgrading input files one version.
+
+\subsection{Edit Menu}\label{edit-menu}
+
+No cutting or pasting is used in this program so the edit menu shows options that duplicate the functions of the ``Edit - Text Editor'' and ``Edit - IDF Editor'' buttons. In addition, the weather file and the postprocessor command file (rvi) may be opened in the text editor.
+
+\subsection{View Menu}\label{view-menu}
+
+The View menu (see Figure~\ref{fig:ep-launch-view-menu}) duplicates the options in the ``View Results'' area of the main screen (see the \emph{Looking at the Results} section above) and allows opening of selected output files. You can also open the folders that contain the active input and weather files. Opening a single file is under a submenu and is very similar to the Quick Open Panel for Single Simulation described above. Selecting ``HTML File'' from the ``View'' menu will open any user created files saved in the format: \textless{}filename\textgreater{}table.html (see \emph{OutputControl:Table:Style}).
+
+\begin{figure}[hbtp] % fig 39
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image105.png}
+\caption{EP-Launch View Menu \protect \label{fig:ep-launch-view-menu}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 40
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image106.png}
+\caption{EP-Launch Options Screen. \protect \label{fig:ep-launch-options-screen.}}
+\end{figure}
+
+The ``View'' menu also accesses the ``Options'' menu item shown in Figure~\ref{fig:ep-launch-options-screen.} that is used to control many of the optional features of EP-Launch. These optional features are described below:
+
+\subsubsection{Command Window Options}\label{command-window-options}
+
+\textbf{Pause During Simulation (Unless Minimized)} - Stops the progress of the EnergyPlus run at different points. This does not stop the simulation itself but pauses before or after important events as files are copied or utility programs are run. It is usually used only for diagnosing problems with the EPL-RUN batch file. The feature is also described in the \emph{Running a Single Input File} section above.
+
+\textbf{Minimize Single Simulation Command Window} - For a single input file, minimizes the Command Window that EP-Launch uses to run EnergyPlus. The command window will appear only in the Windows taskbar and the command window will not be visible. You can restore the command window be clicking on the taskbar item labeled ``EnergyPlus Process''. This option should be used with caution since you will not see any indication of the simulation being complete other than the ``EnergyPlus Process'' taskbar item will disappear.
+
+\textbf{Minimum Group Simulation Command Window} - For a group of input files, minimizes the Command Window that EP-Launch uses to run EnergyPlus. This is a good option when working on something else on your computer at the same time as the group of simulations is running since the command window normally becomes the front window each time a new simulation starts. This option prevents the command window coming to the front for each simulation. The command window will appear only in the Windows taskbar and the command window will not be visible. You can restore the command window be clicking on the taskbar item labeled ``EnergyPlus Process''. This option should be used with caution since you will not see any indication of the simulation being complete other than the ``EnergyPlus Process'' taskbar item will not be present.
+
+\textbf{Number of Simultaneous Processes} - Select the maximum number of simulations that should be able to be run at the same time. For a computer with multiple processors or multiple cores, this will allow better utilization of the computers power. The value selected should correspond to the number of processors/cores but higher or lower number can be used as well.
+
+\textbf{Disable Multi-Threading} - Check this box if you wish to disable the built in multi-threading capabilities of EnergyPlus. Portions of EnergyPlus have been programmed to use more than one processor, or CPU core, at the same time during a single simulation. This multithreading may not be desirable when running more than one simulation at a time on the same computer (because it can actually run more slowly). When this check box is checked multi-threading is turned off. The check box sets the \textbf{EP\_OMP\_NUM\_THREADS} environmental variable to 1. The multi-threading capability of EnergyPlus can also be controlled using the \textbf{ProgramControl} object field called Number of Threads Allowed. That field takes precedence over the setting of the checkbox. Also note that when multiple simulations are started from EP-Launch, this automatically disables multithreading by setting the EP\_OMP\_NUM\_THREADS environmental variable to 1 whether this box is checked or not. The ProgramControl object is described in the Input Output Reference document.
+
+\subsubsection{Interface Options}\label{interface-options}
+
+\textbf{Extra Wide Window} - Select this option to make the main EP-Launch window wider. This is useful when files are used with very long file path names.
+
+\textbf{Alternative layout} - Changes the layout of the EP-Launch window to an alternative arrangement of buttons.
+
+\subsubsection{Miscellaneous Options}\label{miscellaneous-options}
+
+\textbf{Tab Delimited Open with Spreadsheet} - Selecting ``Single File'' and then ``Main Results File'' from the ``View'' menu or pressing the F4 function key will open TAB files with the default spreadsheet application rather than the text editor. Comma-separated variable (CSV) is the default setting for viewing tabulated results set in the RVI file. If the user changes the setting for viewing tabulated results to TAB or TXT format, selecting ``Single File'' and then ``Main Results File'' from the ``View'' menu or pressing the F4 function key will open the files in the default text editor. TAB files, when selected, will also be opened by the text editor when the ``Text Output Files'' button is pressed after a successful run.
+
+\textbf{Allow More Than 250 Columns} - Tabulated data that exceeds 250 columns, the MS Excel maximum, will be truncated to that limit unless ``Allow \textgreater{}250 Columns'' is selected. Excel versions prior to 2007 were limited to 255 columns in a sheet; later versions allow unlimited number of columns. This limitation may not be true for other spreadsheet programs.
+
+\textbf{Check VERSION Prior to Simulation} - Automatically check the VERSION object in the selected EnergyPlus input file prior to simulation and if it is an older version than the current version will run the Transition program to update the file.
+
+\textbf{Convert ESO/MTR to IP Units} - Runs the convertESOMTR utility program (see AuxiliaryPrograms documentation for more information). This utility will convert the ESO and MTR files into Inch-Pound units. The CSV file created from these files will also be in Inch-Pound units.
+
+\textbf{Create Statistics File} - Runs the CSVProc utility program (see the AuxiliaryPrograms documentation for more information) and creates the -Proc.csv file. This file contains some simple statistics on each variable in the normal CSV file.
+
+\textbf{Create Batch File to Run EnergyPlus} - Traditionally EP-Launch has created a batch file in order to execute EnergyPlus with the various options chosen. This can cause problems with some operating systems, such as Windows Vista, when set to a higher security setting. This option can be unchecked and a batch file is not created when running EnergyPlus instead parameters are passed to an existing batch file.
+
+\textbf{Run ParametricPreprocessor} - When this option is checked, if Parametric objects are present in the file, the ParametricPreprocessor will be run prior to the first simulation and if multiple simulations are needed they will all be executed. See the Auxiliary Programs documentation for details.
+
+\textbf{Check for Updates to EnergyPlus} - When this option is checked, EP-Launch will check every seven days if an update to EnergyPlus or any of the files distributed with EnergyPlus are available to download. If they are available a message will be shown upon start up. You can also manually check by going to HELP .. CHECK FOR UPDATES.
+
+\subsubsection{Text Editor Options}\label{text-editor-options}
+
+EP-Launch will start a text editor when editing a IDF file or when viewing many of the results files. The text editor that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the text editor of your choice. The Auto Find button will automatically find the program that is associated with the TXT file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a text editor is available immediately. The most common text editor is NOTEPAD.EXE and is built into Windows but many other text editors are also available.
+
+\subsubsection{Drawing Viewer Options}\label{drawing-viewer-options}
+
+The default drawing viewer is the application associated with DXF files. This can be changed to your favorite drawing program by using the Select button then locating the executable file for your favorite drawing software capable of reading a DXF file. The Auto Find button will automatically find the program that is associated with the DXF file extension and use that program. A variety of programs (free of charge) can render DXF files for viewing. The \href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details} document lists some of these programs as well as displaying what a DXF rendered file looks like on the screen.
+
+\subsubsection{VRML Viewer Options}\label{vrml-viewer-options}
+
+EP-Launch will start a VRML Viewer when a building drawing is created using the Report, Surfaces, VRML option in your IDF file. The VRML Viewer that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the VRML Viewer of your choice. The Auto Find button will automatically find the program that is associated with the WRL file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a VRML Viewer is available immediately. Many other VRML Viewers are available.
+
+\subsubsection{Spreadsheet Options}\label{spreadsheet-options}
+
+EP-Launch will start a spreadsheet program when viewing many of the results files. The spreadsheet that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the spreadsheet program of your choice. The Auto Find button will automatically find the program that is associated with the CSV file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a spreadsheet program is available immediately.
+
+\subsubsection{Diagramming Options}\label{diagramming-options}
+
+EP-Launch will start a diagramming program to view SVG files from HVAC Diagram. The diagramming program that will be used is shown but can be changed by either pressing the Select button, the Auto Find button, the Use Firefox button or the Use Opera button. The Select button allows you to find the diagramming program of your choice but make sure it is capable of opening SVG files. The Auto Find button will automatically find the program that is associated with the SVG file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a spreadsheet program is available immediately. Since both Firefox and Opera web browsers can view SVG files, those buttons will select those respective browsers if available.
+
+\subsubsection{HTML Browser Options}\label{html-browser-options}
+
+EP-Launch will start a HTML browser program when viewing the tabular results file when HTML is chosen in OutputControl:Table:Style. The HTML browser that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the HTML browser of your choice. The Auto Find button will automatically find the program that is associated with the HTML file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a HTML browser is available immediately.
+
+\subsubsection{ESO Viewer Options}\label{eso-viewer-options}
+
+By default, ESO files are opened with a text editor. ESO files are the raw output file containing results from EnergyPlus for Report Variable objects. They are often processed into CSV files to make it easier to view them. At least one utility program has been developed to view ESO files directly (see the EnergyPlus.gov web site under ``Interfaces \& Other Tools'', ``Third-party EnergyPlus Tools). The Auto Find and Select buttons work the same way as other viewer selectors. If no special ESO viewer is selected the box will be shown as empty. It can also be emptied by using the Clear button.
+
+\subsubsection{PDF Viewer Options}\label{pdf-viewer-options}
+
+EP-Launch will start a PDF viewer program when opening the EnergyPlus documentation under the Help menu. The PDF Viewer that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the PDF Viewer of your choice. The Auto Find button will automatically find the program that is associated with the PDF file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a PDF Viewer is available immediately.
+
+\subsubsection{File Association Options}\label{file-association-options}
+
+When installing EnergyPlus, you are given an option if you want IDF, IMF, and EPG files associated with EP-Launch. This allows double clicking on files with those extensions and having EP-Launch start automatically with those files. If during the install that option is not selected or if you have changed the program that opens IDF, IMF and EPG files and want to change it back to EP-Launch, the button for this option will do that.
+
+\subsubsection{Reset Options}\label{reset-options}
+
+Two reset options are available here.
+
+The \textbf{Auto Find All File Viewers} button will autofind all the file viewers in one step. This is equivalent to pressing the Auto Find button for each viewer program.
+
+The \textbf{Reset All Options and Exit} button will clear all options and restore the default values used when first invoking EP-Launch for the first time. This also clears the list of recently used IDF and weather files. This option will exit EP-Launch and you will have to start EP-Launch again.
+
+\subsection{Help Menu}\label{help-menu}
+
+The Help menu can be used to open the EnergyPlus documentation files and the EP-Launch help file. In addition, you can check for updates to the EnergyPlus program and other files in the EnergyPlus distribution.
+
+\subsection{Recently Used Files}\label{recently-used-files}
+
+The recently used input, weather and group file pull down lists can hold a maximum of twenty items. These lists, like the viewers selected, are saved between times you use the EP-Launch program.
+
+\subsection{Running Groups of Input Files}\label{running-groups-of-input-files}
+
+If you are running EnergyPlus on one file or even just a few different files, the easiest way to do this is on the Single Simulation tab. If you are performing an analysis of a building which requires running EnergyPlus for a larger number of times, you may want to consider the Group of Input Files tab, shown below. You may also want to set the Number of Simultaneous Processes option under View Options Command Window so that the simulations are completed as fast as your computer will allow.
+
+\begin{figure}[hbtp] % fig 41
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image107.png}
+\caption{EP-Launch Group of Input Files Tab. \protect \label{fig:ep-launch-group-of-input-files-tab.}}
+\end{figure}
+
+This tab lets you manage EPG, EnergyPlus Group files which contain a list of simulations that need to be performed. The EPG file is simply a text file that contains on each line the input file and weather file names to be used for a simulation along with how the output files should be named and a counter.
+
+You do not need to manually create EPG files, instead press the New Group button on the Group of Input Files Tab and a step-by-step ``wizard'' will help to create a new EPG, EnergyPlus Group file. The first step of the wizard is to selected the EnergyPlus input files that should be simulated as part of the group:
+
+\begin{figure}[hbtp] % fig 42
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image108.png}
+\caption{EP-Launch Step 1 of New Group Wizard. \protect \label{fig:ep-launch-step-1-of-new-group-wizard.}}
+\end{figure}
+
+Use the boxes next to each file to select the files to be simulated. The path to files shown may be changed using the ``path'' button. Once the files in a certain directory are selected the ``next'' button should be pressed. If additional files are desired in different directories, you will get a chance to add them to the EnergyPlus group file in a later step.
+
+Select one or several weather files using the second step of the wizard, shown below:
+
+\begin{figure}[hbtp] % fig 43
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image109.png}
+\caption{EP-Launch Step 2 of New Group Wizard. \protect \label{fig:ep-launch-step-2-of-new-group-wizard.}}
+\end{figure}
+
+The next step is to review the simulations selected. Each combination of weather file and input file is initially shown. Each simulation is displayed as a single row. You may select a row and delete the simulation at this point. In addition, if additional simulations are desired, the ``Add more simulations button'' brings you back to the first step of the wizard to add more file.
+
+\begin{figure}[hbtp] % fig 44
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image110.png}
+\caption{EP-Launch Step 3 of New Group Wizard. \protect \label{fig:ep-launch-step-3-of-new-group-wizard.}}
+\end{figure}
+
+The next step of the wizard allows you to decide exactly where you want the output files located and what they should be named. For most people just trying to group their simulations and wanting the output files in the same directory as the input files, just select ``Original Input File Locations''.
+
+\begin{figure}[hbtp] % fig 45
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image111.png}
+\caption{EP-Launch Step 4 of New Group Wizard. \protect \label{fig:ep-launch-step-4-of-new-group-wizard.}}
+\end{figure}
+
+More advanced users may choose to define their locations for the output files using symbols that define the name of the directory and file name using:
+
+\%I = input file name
+
+\%G = group file name
+
+\%W = weather file name
+
+\%N = repeat number for IMF files
+
+\%J = input file path
+
+\%H = group file path
+
+\%X = weather file path
+
+Each of these symbols may be used in the location field and substitutions will be made for each when defining the output file location.
+
+For macro files (they have an extension IMF instead of IDF) used in a parametric analysis, the macro file may be run repeatedly up to 999 times. Each time they are simulated a new COUNTER.INC file is created which sets a macro parameter. The COUNTER.INC file should be included using the \#\#include statement in the macro file.
+
+Finally, you can save the EPG, EnergyPlus Group, file wherever you would like.
+
+To run the simulations press the ``Simulate Group'' button on the Group of Input Files tab. To prevent a specific simulation from being performed, edit the file and use a comment character (an exclamation point) to comment out the line.
+
+When the group of input file simulations is running, the title bar of EP-Launch will show the progress.
+
+\subsection{History of Simulations Performed}\label{history-of-simulations-performed}
+
+The History tab allows you to see what files were associated with a particular simulation that was performed. The list shows the date and time of the simulation along with the input and weather file names.
+
+\begin{figure}[hbtp] % fig 46
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image112.png}
+\caption{EP-Launch History Tab. \protect \label{fig:ep-launch-history-tab.}}
+\end{figure}
+
+You can expand the level of detail by clicking on the plus signs or double clicking on the entry. The detail shown includes the names of all the input and output files associated with that simulation along with the message summary of the warnings and errors generated. It is possible that a file may be shown that no longer exists.
+
+The View Files button will display the selected file using a spreadsheet, text editor, DXF file viewer, SVG file viewer, or HTML web browser. When groups of simulations are performed using the Group of Input File tab and User Defined Locations are used for the output files, the history view is the only way to access those files using EP-Launch.
+
+The history tab displays the HISTORY.CSV file that is located in the same directory as EP-Launch. If EP-Launch seems to be starting slowly, it is possible that the history file has grown very large. It may be deleted or renamed and a new history file will be automatically created during the next simulation. The HISTORY.CSV file may also be opened in a spreadsheet program.
+
+\subsection{Utilities Tab}\label{utilities-tab}
+
+The utilities tab shown in the following figure allows several utility programs that come with EnergyPlus to be used directly. More information on each utility is also available in the AuxiliaryPrograms documentation.
+
+\begin{figure}[hbtp] % fig 47
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image113.png}
+\caption{EP-Launch Utilities Tab. \protect \label{fig:ep-launch-utilities-tab.}}
+\end{figure}
+
+For each utility, input files can be selected by using the Browse Button. The input file can be opened using a text editor and, for certain utilities, the IDF Editor. If a weather file is needed for a utility it can also be selected. For other utilities, no weather file is needed and that portion of the screen is not shown. The appropriate output files can be opened by the ``Open'' button near the bottom of the screen. To run the utility, use the ``Run'' button in the lower left corner of the screen above the ``Exit'' button.
+
+In addition, for each utility, a brief description of the function of the utility is shown in the about box but much more information is available in the AuxiliaryPrograms documentation.
+
+\subsection{Caveats}\label{caveats}
+
+Remember to save changes made in the editor before you run another simulation.
+
+The simulation cannot write new results to open files which are locked by another application.
+
+You will need to close the spreadsheet program that views the resulting CSV files prior to another simulation and you may need to close the text editor windows also (depending on your editor).
+
+The EPL-RUN.BAT batch file is used to run EnergyPlus from the EP-Launch program. It can be edited with care if other postprocessors or preprocessors are to be used.
+
+\subsection{When things go wrong}\label{when-things-go-wrong}
+
+Though EnergyPlus has had several releases (including beta releases prior to initial release), there still may be problems when input files meet with EnergyPlus. If you are using EP-Launch when this happens, you will see a window appear as in the figure below (Figure~\ref{fig:energyplus-crash-within-ep-launch.}). Follow the instructions listed on the screen.
+
+\begin{figure}[hbtp] % fig 48
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image114.png}
+\caption{EnergyPlus crash within EP-Launch. \protect \label{fig:energyplus-crash-within-ep-launch.}}
+\end{figure}
+
+\subsection{Bugs}\label{bugs}
+
+The EP-Launch program has been through several ``releases'' but there is still a chance you will find bugs. Please report them to the energyplus-support@gard.com address so that we can fix them prior to the release.
+
+If the pull-down lists ever are shown as blank the ``reset'' button may be used. This unlabeled button is very small in the lower left-hand corner of the main screen. It removes the items shown in the recently used file list and causes the program to forget the selected viewers and text editors; and exits the program. When you start EP-Launch again, you will need to make these selections (viewers and text editors) again.
diff --git a/doc/auxiliary-programs/src/technical-details-of-running-energyplus/rundirmulti-batch-file.tex b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/rundirmulti-batch-file.tex
new file mode 100644
index 00000000000..5e1d0701972
--- /dev/null
+++ b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/rundirmulti-batch-file.tex
@@ -0,0 +1,9 @@
+\section{RunDirMulti Batch File}\label{rundirmulti-batch-file}
+
+The RunDirMulti.bat batch file runs all the IDF files in the directory that it is located in. The batch file is used to run EnergyPlus simulations using the RunEPlus.bat for all the files in the current directory across multiple separate processor cores. It has two parameters, the weather file name to use for simulations and the number of processors.
+
+RunDirMulti \textless{}weather file\textgreater{} (opt) \textless{}number processor cores\textgreater{} (opt)
+
+The RunDirMulti batch file loops through the files located in the current directory and puts RunEPlus calls to each file into as many temporary batch files as processor cores and then starts each of the batch files. No load balancing between the cores is achieved using this method. The RunDirMulti.bat file should be located in a directory that contains the IDF files. Editing of the file may be necessary to match the directory that EnergyPlus is installed in.
+
+Since the batch file starts up other batch files in different CMD windows, the only way to know that the simulations are all complete is when all of the other CMD windows are closed. Those windows are named ``Batch Simulation\textless{}n\textgreater{}'' where n is 1 to the number of processor cores you selected to use.
diff --git a/doc/auxiliary-programs/src/technical-details-of-running-energyplus/runeplus-batch-file.tex b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/runeplus-batch-file.tex
new file mode 100644
index 00000000000..1db51398787
--- /dev/null
+++ b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/runeplus-batch-file.tex
@@ -0,0 +1,9 @@
+\section{RunEPlus batch file}\label{runeplus-batch-file}
+
+It is simple to run EnergyPlus: open a DOS or CMD box in the EnergyPlus directory and use the RunEPlus.bat procedure file. The procedure file takes two arguments - the input file name (containing the building description) and the weather file name:
+
+RunEPlus \textless{}input\_file\_name\textgreater{} \textless{}weather\_file\_name\textgreater{}
+
+Though it's possible to supply arguments to the batch file with embedded blanks, it's better practice not to. More extensive information about the intricacies of EnergyPlus execution is given in the next parts of this section.
+
+As installed, the RunEPlus is ready to run the sample files that are included. If you wish to create and run other files, you may wish to modify the batch file to your own preferences. See ``RunEPlus details'' later in this document for parts of the batch file that you will need to modify.
diff --git a/doc/auxiliary-programs/src/technical-details-of-running-energyplus/runeplus-details.tex b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/runeplus-details.tex
new file mode 100644
index 00000000000..79159cfeee9
--- /dev/null
+++ b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/runeplus-details.tex
@@ -0,0 +1,60 @@
+\section{RunEPlus details}\label{runeplus-details}
+
+A procedure (batch) file is the normal way to run a console application. The \emph{installed} procedure file \textbf{RunEPlus.bat} can be used to execute EnergyPlus and deal with all the file handling and postprocessing. It can accommodate running the EPMacro program if you name your files appropriately. And it can use ExpandObjects to expand the special ``HVACTemplate'' objects into ``normal'' IDF objects.
+
+The ``set'' statements near the beginning of the procedure file can be customized for each local system. Thus ``program\_path'' should be set to the directory path where the program executable resides on your local computer, ``program\_name'' should be set to the name of the EnergyPlus executable file, ``input\_path'' should be set to the directory path containing the input (IDF) file, and so forth. Each of the path environment variables must have ``\textbackslash{}'' as the final character or things won't run correctly. As mentioned before, the batch file is executed by typing:
+
+RunEPlus \textless{}input\_filename\textgreater{} \textless{}weather\_filename\textgreater{}
+
+where \textless{}input\_filename\textgreater{} is the name of the IDF file, without the file extension, and \textless{}weather\_filename\textgreater{} is the name of the weather file, without the file extension.The \textless{}input\_filename\textgreater{} can also be a complete path to the file (without extension) and it will work.
+
+In addition, RunEPlus can be called from a different directory and the temporary files will be created in the directory it is called from. This enables multiple RunEPlus.bat to be used with multiple processors or a multiple-core processor without the temporary files of one set of simulations interfering with another. Each call to RunEPlus.bat should be from different directories.
+
+Instructions appear at the top of the batch file:
+
+\begin{lstlisting}
+:Instructions:
+:  Complete the following path and program names.
+:  path names must have a following \ or errors will happen
+:  does not have the capability to run input macro files (yet)
+:   %program_path% contains the path to the executable as well as IDD and is
+:                  the root directory
+:   %program_name% contains the name of the executable (normally EnergyPlus.exe)
+:   %input_path%   contains the path to the input file (passed in as first argument)
+:   %output_path%  contains the path where the result files should be stored
+:   %post_proc%    contains the path to the post processing program (ReadVarsESO)
+:   %weather_path% contains the path to the weather files (used with optional argument 2)
+:   %pausing%      contains Y if pause should occur between major portions of
+:                  batch file (mostly commented out)
+:   %maxcol%       contains "250" if limited to 250 columns otherwise contains
+:                  "nolimit" if unlimited (used when calling readVarsESO)
+\end{lstlisting}
+
+\begin{lstlisting}
+ echo = = = = = %0 (Run EnergyPlus) %1 %2 = = = = = Start = = = = =
+ set program_path =
+ set program_name = EnergyPlus.exe
+ set input_path = ExampleFiles\
+ set output_path = Test\
+ set post_proc = PostProcess\
+ set weather_path = WeatherData\
+ set pausing = N
+ set maxcol = 250
+\end{lstlisting}
+
+\begin{lstlisting}
+:  This batch file will perform the following steps:
+:
+:   1. Clean up directory by deleting old working files from prior run
+:   2. Clean up target directory
+:   3. Copy %1.idf (input) into In.idf
+:   4. Copy %2 (weather) into In.epw
+:   5. Execute EnergyPlus
+:   6. If available Copy %1.rvi (post processor commands) into Eplusout.inp
+:   7. Execute ReadVarsESO.exe (the Post Processing Program)
+:   8. If available Copy %1.mvi (post processor commands) into test.mvi
+:       or create appropriate input to get meter output from eplusout.mtr
+:   9. Execute ReadVarsESO.exe (the Post Processing Program) for meter output
+:  10. Copy Eplusout.* to %1.*
+:  11. Clean up working directory.
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/technical-details-of-running-energyplus/running-energyplus-by-hand.tex b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/running-energyplus-by-hand.tex
new file mode 100644
index 00000000000..a64d8251ec8
--- /dev/null
+++ b/doc/auxiliary-programs/src/technical-details-of-running-energyplus/running-energyplus-by-hand.tex
@@ -0,0 +1,42 @@
+\section{Running EnergyPlus by Hand}\label{running-energyplus-by-hand}
+
+EnergyPlus runs as a console application with optional command line arguments. The arguments may be listed by typing \lstinline!energyplus --help! (on any operating system) and \lstinline!man energyplus! (on Unix-based operating systems, Mac OS X and Linux). For more information about the command line interface, see https://github.com/NREL/EnergyPlus/blob/develop/doc/running-energyplus-from-command-line.md. The remainder of this section describes running EnergyPlus in legacy mode (i.e.~no command-line arguments) on Windows OS.
+
+To run the program bring up the command prompt and ``cd'' to the directory containing the executable. Assume that the executable is called \emph{EnergyPlus.exe}. In the same directory EnergyPlus expects \emph{in.idf}, the input data file; \emph{Energy+.idd}, the data dictionary file; \emph{in.epw}, the weather file (needed only if there is a RunPeriod in the input); and optionally \emph{Energy+.ini}, the initialization file. Typing ``EnergyPlus'' (and hitting the \emph{Enter} key) will execute the program. EnergyPlus will write messages to the command window as it runs. A simulation with two design days and one run period looks like:
+
+\begin{lstlisting}
+ EnergyPlus Starting
+ EnergyPlus, Version 1.3
+ Warming up
+ Initializing Response Factors
+ Calculating CTFs for "EXTWALL80", Construction \#1
+ Calculating CTFs for "PARTITION06", Construction \#2
+ Calculating CTFs for "FLOOR SLAB 8 IN", Construction \#3
+ Calculating CTFs for "ROOF34", Construction \#4
+ Initializing Window Optical Properties
+ Initializing Solar Calculations
+ Initializing HVAC
+ Warming up
+ Warming up
+ Warming up
+ Performing Zone Sizing Simulation
+ Warming up
+ Warming up
+ Warming up
+ Performing Zone Sizing Simulation
+ Initializing New Environment Parameters
+ Warming up {1}
+ Warming up {2}
+ Warming up {3}
+ Warming up {4}
+ Starting Simulation at 01/14 for CHICAGO IL UNITED STATES TMY2 94846 WMO# = 725340
+ Initializing New Environment Parameters
+ Warming up {1}
+ Warming up {2}
+ Warming up {3}
+ Warming up {4}
+ Starting Simulation at 07/07 for CHICAGO IL UNITED STATES TMY2 94846 WMO# = 725340
+ EnergyPlus Run Time = 00hr 00min  7.31sec
+\end{lstlisting}
+
+When execution is finished, \emph{eplusout.err} and \emph{eplusout.audit} will always appear. If the program terminated with an input error, these may be the only output files. If the program runs normally, \emph{eplusout.eio} will appear. Depending on what was requested in the input, the other output files described above will also be written.
diff --git a/doc/auxiliary-programs/src/using-older-version-input-files-transition.tex b/doc/auxiliary-programs/src/using-older-version-input-files-transition.tex
new file mode 100644
index 00000000000..b2ae565bf3a
--- /dev/null
+++ b/doc/auxiliary-programs/src/using-older-version-input-files-transition.tex
@@ -0,0 +1,3 @@
+\chapter{Using Older Version Input Files - Transition}\label{using-older-version-input-files---transition}
+
+The transition program(s) are console programs that assist users in converting input files from prior release versions to the current (or interim). Sometimes many changes are made to the input file syntax; sometimes very few but the Transition program(s) can do the fastest job of making the conversions. An ObjectStatus spreadsheet is also included for those who want the details of each object's change.
diff --git a/doc/auxiliary-programs/src/using-older-version-input-files-transition/converting-imf-files.tex b/doc/auxiliary-programs/src/using-older-version-input-files-transition/converting-imf-files.tex
new file mode 100644
index 00000000000..428b7d5d29d
--- /dev/null
+++ b/doc/auxiliary-programs/src/using-older-version-input-files-transition/converting-imf-files.tex
@@ -0,0 +1,38 @@
+\section{Converting imf files}\label{converting-imf-files}
+
+The transition/conversion programs can ``automatically'' transition imf (ep-macro) files. One note of caution: if your macro file contains \#if statements in the form:
+
+\begin{lstlisting}
+
+PEOPLE,
+  ZONE ONE,                !- Zone Name
+  **\#\#if \#[DoSizing[] EQSU Y]**
+  \#[FAREA[] / OCCDENPEAK[]],        !- Number of People
+  **\#\#else**
+  \#[FAREA[] / OCCDENAVG[]],         !- Number of People
+  **\#\#endif   **
+  OCCSCHED[],       !- Number of People SCHEDULE Name (real--fraction)
+  0.5000000,        !- Fraction Radiant
+  Activity Sch;     !- Activity level SCHEDULE Name (units W/person, real)
+\end{lstlisting}
+
+They should look like this:
+
+\begin{lstlisting}
+
+**\#\#if \#[DoSizing[] EQSU Y]**
+  PEOPLE,
+  ZONE ONE,                !- Zone Name
+  \#[FAREA[] / OCCDENPEAK[]],       !- Number of People
+  OCCSCHED[],       !-   Number of People SCHEDULE Name (real--fraction)
+  0.5000000,        !- Fraction Radiant
+  Activity Sch;     !- Activity level SCHEDULE Name (units W/person, real)
+  **\#\#else**
+  PEOPLE,
+  ZONE ONE,                !- Zone Name
+  \#[FAREA[] / OCCDENAVG[]],        !- Number of People
+  OCCSCHED[],       !- Number of People SCHEDULE Name (real--fraction)
+  0.5000000,        !- Fraction Radiant
+  Activity Sch;     !- Activity level SCHEDULE Name (units W/person, real)
+  **\#\#endif   **
+\end{lstlisting}
diff --git a/doc/auxiliary-programs/src/using-older-version-input-files-transition/idf-version-converter-transition-file-lists.tex b/doc/auxiliary-programs/src/using-older-version-input-files-transition/idf-version-converter-transition-file-lists.tex
new file mode 100644
index 00000000000..709737aaa71
--- /dev/null
+++ b/doc/auxiliary-programs/src/using-older-version-input-files-transition/idf-version-converter-transition-file-lists.tex
@@ -0,0 +1,19 @@
+\section{IDF Version Converter / Transition File Lists}\label{idf-version-converter-transition-file-lists}
+
+Both the console program and the IDF-Version Updater (see) can use a text file of file names to perform the transitions. The file is a very simple list of file names:
+
+\begin{lstlisting}
+FileName1
+FileName2
+\end{lstlisting}
+
+But you must include the path name in the file if it is not in the same folder as the transition set of programs:
+
+\begin{lstlisting}
+C:\Myfiles\abc.idf
+C:\My Working Files\abcdef.idf
+D:\OtherFiles\xxxxxyyyyy.idf
+Etc
+\end{lstlisting}
+
+Note that the files need not be in the same folder. And, if you use the IDF Version Updater app, they need not all be the same version! If you use the straight batch files form the CMD line, all files in this list must be the same starting version and you will need to select that version when you run the batch file. List files have the implicit transition options seen in the following section.
diff --git a/doc/auxiliary-programs/src/using-older-version-input-files-transition/idf-version-updater.tex b/doc/auxiliary-programs/src/using-older-version-input-files-transition/idf-version-updater.tex
new file mode 100644
index 00000000000..35f8d6e893b
--- /dev/null
+++ b/doc/auxiliary-programs/src/using-older-version-input-files-transition/idf-version-updater.tex
@@ -0,0 +1,35 @@
+\section{IDF Version Updater}\label{idf-version-updater}
+
+The transition programs have been written as console applications similar to EnergyPlus. However, that may not be the easiest for users who want to transition several versions or several files at one time. Thus the IDF Version Updater GUI application was created.
+
+The IDF Version Updater lives in the folder with the multiple transition programs -- see Figure~\ref{fig:transition-gui-screen}. Note that this application is also available from the EP-Launch Utilities tab (utility: IDFVersionUpdater). If you need to convert files from older than V6.0, the transition program set will need to be downloaded before use. Once ``IDF Version Updater'' is selected from the Utilities pulldown list, click on the ``Run IDF Version Updater'' box and the single window shown below appears:
+
+\begin{figure}[hbtp] % fig 29
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image027.jpg}
+\caption{Transition GUI screen \protect \label{fig:transition-gui-screen}}
+\end{figure}
+
+Using the program is quite simple. As the window indicates, you press ``Choose File to Update'' to select a file or list of files (see IDF Version Converter / Transition File Lists) to convert. If doing multiple transitions using a transition file list you also press the ``Choose File to Update, a browse window will appear at the bottom of which is a pulldown list for the''Files of Type``. Select the''Text File With List of EnergyPlus Files (*.lst)" (see the section IDF Version Converter / Transition File Lists for format of this .lst file) option. Once a file is found, its version is checked and appears as the ``Current Version''. By default, the latest ``New Version'' will be selected by the program - you can override this by choosing a different file version as the end version. The ``Update File'' button will then be able to be selected and the conversion will be done. The audit from the multiple transitions will be able to be viewed once the process is complete. If you are doing multiple transitions (e.g., from V2.2 to V6), you can select the check box ``Create Intermediate Files'' and after each transition, a file for the resultant version will be created and labeled \textless{}filename\textgreater{})\_Vx.idf (where x is an abbreviated version number).
+
+The converted file becomes the new \textless{}file\textgreater{}.idf and the original file is saved in the original folder as \textless{}file\textgreater{}\_original.idf. To delete the original file instead of saving it, check the ``Delete Original Files'' checkbox.
+
+% table 27
+\begin{longtable}[c]{p{2.5in}p{3.5in}}
+\caption{IDF Version Updater Output Files and Descriptions. \label{table:idf-version-updater-output-files}} \tabularnewline
+\toprule 
+Transition Output File Name & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{IDF Version Updater Output Files and Descriptions.} \tabularnewline
+\toprule 
+Transition Output File Name & Description \tabularnewline
+\midrule
+\endhead
+
+< filename > \_Transition.audit & This is the contents of what you would see on the screen if you sat and watched the transition process during a console run. If you convert multiple versions, all the messages are shown in this file. \tabularnewline
+< filename > .idf & Converted results to the latest version or version selected. \tabularnewline
+< filename > \_Vxxx.idf & If you don't select "create intermediate versions", this will only be the original version. Otherwise will have each version. \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/auxiliary-programs/src/using-older-version-input-files-transition/transition-console-program-details.tex b/doc/auxiliary-programs/src/using-older-version-input-files-transition/transition-console-program-details.tex
new file mode 100644
index 00000000000..8fcc87c7c5e
--- /dev/null
+++ b/doc/auxiliary-programs/src/using-older-version-input-files-transition/transition-console-program-details.tex
@@ -0,0 +1,32 @@
+\section{Transition Console Program Details}\label{transition-console-program-details}
+
+For those who are interested, this is the detailed description of the Transition console applications including the current one. There are methods to use the program set from the command line; those details are not included in this document but available from EnergyPlus Support group.
+
+TransitionVA-B-C-to-VD-E-F.exe is the transition program that converts files from version ``A-B-C'' to ``D-E-F'', and is distributed in the ``D-E-F'' installer package. It uses several important files that are included in the ``EnergyPlus'' installation folder, in the PreProcess/IDFVersionUpdator subdirectory.
+
+% table 28
+\begin{longtable}[c]{p{2.14in}p{3.85in}}
+\caption{Transition files for current release \label{table:transition-files-for-current-release}} \tabularnewline
+\toprule 
+File Name & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Transition files for current release} \tabularnewline
+\toprule 
+File Name & Description \tabularnewline
+\midrule
+\endhead
+
+TransitionVA-B-C-to-VD-E-F.exe & The executable program \tabularnewline
+VA-B-C-Energy+.idd & Base, starting, version Energy+.idd file \tabularnewline
+VD-E-F-Energy+.idd & Target, new idd file; Identical to Energy+.idd when distributed \tabularnewline
+Report Variables A-B-C to D-E-F.csv & Report variable name changes \tabularnewline
+\bottomrule
+\end{longtable}
+
+Another file ``RulesA-B-C-to-D-E-F.xls'' is not used directly by the program but contains the ``rules'' for translating objects from version A-B-C release to the D-E-F release. The ObjectStatus file can also be viewed - it will show if deleted objects are automatically transitioned to the new input file versions.
+
+There are several methods to executing the transition program - these methods give you the most flexibility in changing files from one version to the next. The easiest transition is through the EP-Launch program which can detect if the input file about to be run is of the same version as the IDD or not and suggest transitioning. You can also manually transition from the file menu in EP-Launch. (To have this feature, you must also have the files from the preceding table in the same folder as EP-Launch - which is usually the folder that also has the EnergyPlus.exe program).
+
+There are two command line methods to execute the transition version (from the Command Prompt). One is to simply use the file name you want transitioned (including .rvi or .mvi file names) or you can use a file name with a .lst extension and simply enter file names to be done in a text file. When you execute the transition program in this fashion, you will get the ``typical'' program defaults of a ``full'' transition, field names will be shown at each field with units, and any blank fields will be left blank rather than filled in with the current defaults.
diff --git a/doc/auxiliary-programs/src/view-factor-calculation-program.tex b/doc/auxiliary-programs/src/view-factor-calculation-program.tex
new file mode 100644
index 00000000000..746ece4c4ca
--- /dev/null
+++ b/doc/auxiliary-programs/src/view-factor-calculation-program.tex
@@ -0,0 +1,3 @@
+\chapter{View Factor Calculation Program}\label{view-factor-calculation-program}
+
+EnergyPlus has the capability of accepting user defined view factors for special research situations. This option is not recommended for general use because the normal approximate view factor determination within EnergyPlus accounts for such practical things as thermal mass (furniture), and realistic exchange limits. However, when a user desires to supply view factors, this auxiliary program can be used to calculate them for a variety of configurations. The program is named View3D, and was developed at NIST (1). This document will describe how to use the program.
diff --git a/doc/auxiliary-programs/src/view-factor-calculation-program/additional-information.tex b/doc/auxiliary-programs/src/view-factor-calculation-program/additional-information.tex
new file mode 100644
index 00000000000..a8285b55b3c
--- /dev/null
+++ b/doc/auxiliary-programs/src/view-factor-calculation-program/additional-information.tex
@@ -0,0 +1,5 @@
+\section{Additional Information}\label{additional-information}
+
+The interface and this document do not describe all of the features of the View3D program. Additional information can be found in the NIST document View3D32.pdf that accompanies the distribution. For example, if an obstruction wall is desired, it can be placed using the interface, but then the ``C'' at the left end of the row describing that surface in the input file should be changed to ``O''. The program can then be rerun with the new input file. If View3D.exe is double clicked, it will ask for the names of the input file and the output file.
+
+An additional point should be emphasized. The program will not calculate view factors for walls containing windows. That is all surfaces must be convex. Therefore, a wall containing a subsurface must be described as four sections surrounding the subsurface. They can be combined using the ``comb'' column as described in the View3D document. However, this in not necessary if the user is willing to work with a few additional surfaces.
diff --git a/doc/auxiliary-programs/src/view-factor-calculation-program/using-the-view-factor-interface-program.tex b/doc/auxiliary-programs/src/view-factor-calculation-program/using-the-view-factor-interface-program.tex
new file mode 100644
index 00000000000..ac40bb4fd3a
--- /dev/null
+++ b/doc/auxiliary-programs/src/view-factor-calculation-program/using-the-view-factor-interface-program.tex
@@ -0,0 +1,177 @@
+\section{Associated Files}\label{associated-files}
+
+Three files come with the auxiliary view factor package. They are:
+
+\begin{itemize}
+\item
+  View3D.exe
+\item
+  ViewFactorInterface.xls
+\item
+  View3D32.doc
+\end{itemize}
+
+The first is the executable program that calculates the view factors. The second is an excel interface that will set up the input files and execute View3D.exe. The third file is the documentation file from NIST that contains some explanation of the program.
+
+\section{Using the View Factor Interface program}\label{using-the-view-factor-interface-program}
+
+The interface program has two main sheets. One, named ZoneSheet, uses surface areas, tilts and facing directions to develop the input for View3D. The other one, named VerticesZoneSheet, uses the surface vertices to develop the input for View3D. The sheets are shown in Figure~\ref{fig:view-factor-interface-zonesheet} and Figure~\ref{fig:view-factor-interface-verticeszonesheet}.
+
+\begin{figure}[hbtp] % fig 24
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image022.png}
+\caption{View Factor Interface ZoneSheet \protect \label{fig:view-factor-interface-zonesheet}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 25
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image023.png}
+\caption{View Factor Interface VerticesZoneSheet \protect \label{fig:view-factor-interface-verticeszonesheet}}
+\end{figure}
+
+Either sheet can be used to generate an input file for the View3D program. An example of that file is shown below.
+
+\begin{lstlisting}
+T Test case from Excel interface
+C encl =  1  list =  2  eps =  0.0001  maxu =  8  maxo =  8  mino =  0  emit =  0
+F  3
+V  1  50  0  0
+V  2  0  0  0
+V  3  0  0  8
+V  4  50  0  8
+S  1  1  2  3  4   0  0   .999  SouthWall
+! = = = = = = = = = = = = = = = = = = = = = = = = =
+V  5  50  60  0
+V  6  50.00025  0  0
+V  7  50.00026  0  8
+V  8  50.00001  60  8
+S  2  5  6  7  8   0  0   .999  EastWall
+! = = = = = = = = = = = = = = = = = = = = = = = = =
+V  9  0  60  0
+V  10  50  60.00014  0
+V  11  50  60.00015  8
+V  12  0  60.00001  8
+S  3  9  10  11  12   0  0   .999  NorthWall
+! = = = = = = = = = = = = = = = = = = = = = = = = =
+V  13  0  0  0
+V  14  0  60  0
+V  15  0  60  8
+V  16  0  0  8
+S  4  13  14  15  16   0  0   .999  WestWall
+! = = = = = = = = = = = = = = = = = = = = = = = = =
+V  17  0  0  0
+V  18  50  1.377901E-04  0
+V  19  49.99984  60.00014  0
+V  20 -1.653482E-04  60  0
+S  5  17  18  19  20   0  0   .999  Floor
+! = = = = = = = = = = = = = = = = = = = = = = = = =
+V  21  0  60  8
+V  22  50  60.00014  8
+V  23  50.00016  1.373291E-04  8.000166
+V  24  1.653482E-04  0  8.000166
+S  6  21  22  23  24   0  0   .999  Roof
+! = = = = = = = = = = = = = = = = = = = = = = = = =
+End Of Data
+\end{lstlisting}
+
+Notice the title from row 6 on the interface appears at the top of the input file, and the control line information in rows 7 and 8 appear below the title line in a line with the character C at the left end. The explanation of the control parameters from the program document states:
+
+(C c) The control line includes the following parameters (in order): name = value
+
+eps = 1.0e-4
+
+integration convergence criterion for both adaptive integration and view obstruction. This is not an exact measure of the accuracy of the computed view factors, but smaller values will usually lead to more precise values. The convergence criteria should not be less than about 1.0e-6 because many of the intermediate calculations are accurate only to single (32-bit) precision.
+
+maxU = 8
+
+maximum recursions used in computing the unobstructed view factors.
+
+maxO = 8
+
+maximum recursions used in computing the obstructed view factors. Limiting the maximum number of recursions limits the total execution time of the program but may prevent reaching the specified convergence.
+
+minO = 0
+
+minimum recursions: used in computing the obstructed view factors. This can help in cases where an obstruction occurs very near the view between the edges of two surfaces. The normal adaptive integration may miss the obstruction. Increasing this value from its normal value of 0 to 1 or 2 may catch the obstruction. This is probably not necessary except when very accurate view factors are desired. It can add considerably to execution time.
+
+row = 0
+
+selected row for computing view factors (0 = all rows)
+
+col = 0
+
+selected column for computing view factors (0 = all columns)
+
+encl = 0
+
+1 indicates that the surfaces form an enclosure; 0 indicates that they do not. This data is used to adjust the view factors of an enclosure to guarantee conservation of energy.
+
+emit = 0
+
+1 indicates that diffuse reflectance effects will be included in the computed view factors; 0 indicates they will not, i.e., surfaces will be considered `black'.
+
+out = 0
+
+view factor output file format - 1 = \ldots{}gence criterion for the numerical integration used to compute view factors between surfaces that have view obstructing surfaces between them.
+
+list = 0
+
+computational summary written to the VIEW3D.LOG file; 0 gives minimal information; 1 gives slightly more; 2 prints all the view factors; 3 causes dumping of some intermediate values.
+
+The values of the parameters shown on the interface sheets are reasonable defaults, and they should need to be adjusted only rarely.
+
+In the upper right corner of either sheet is a button that causes two files to be generated and View3D to be executed. The two files generated are the input file that uses the name from cell D13 with the extension vs3, and a file with the same name and an extension dxf. VoloView can be used with this file to generate a wire frame drawing of the zone being analyzed.
+
+Two paths are needed for executing the program. The directory path where the vs3 and dxf files will be placed is specified in cell D11. This directory can be selected using the Browse button in cell B11. The path to the View3D.exe program is specified by cell D15. This directory can be selected with the Browse button in cell B15.
+
+If you are using the ZoneSheet, the zone surfaces are described in the region from row 17 to row 27. Each column supplies the details for one surface. Additional surface columns can be added by copying and pasting a desired starting column to the right of column H. If either the surface height or base surface length is zero, the gross area cell will be zero and column is ignored. The facing direction of the surface is the direction an inward normal to the surface would point. So, the south wall of a zone faces north or 0 degrees. Note that this is different from EnergyPlus where the facing direction of a surface is based on the outward normal. The facing direction becomes just slightly more difficult with horizontal surfaces like floors and ceilings. The key to determining their facing direction is to visualize them being rotated slightly into the zone around their base surface axis. In the example, both ceiling and floor are chosen to face south. The tilt of a surface is relative to a horizontal upward facing (in the conventional sense) surface such as a floor. A ceiling or flat roof it tilted 180 degrees. Vertical surfaces have a tilt of 90 degrees.
+
+The remaining information needed to describe the surfaces is the coordinates of the lower left hand corner of the surface when viewed from inside the zone. This is where the visualization of a slight rotation of the floor and roof becomes helpful. Consider the roof surface on the sheet. Its base side lies along the east west axis since it faces south. With a slight inward rotation, it is clear that the lower left hand corner is the northwest corner of the roof. This corner has coordinates of 0, 60, and 8.
+
+If the VerticesZoneSheet is being used, the description of the surfaces consists only of the vertices. For this program, the vertices are specified in a counter clockwise rotation order if looking at the surface from the inside, and in a clockwise rotation order if looking from the outside.
+
+The vs3 file produced is shown previously and the dxf file generates the wire frame drawing shown in Figure~\ref{fig:dxf-format-of-example-zone}.
+
+\begin{figure}[hbtp] % fig 26
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image024.png}
+\caption{DXF Format of Example Zone \protect \label{fig:dxf-format-of-example-zone}}
+\end{figure}
+
+The input file and the output files produced by View3D are read into the interface spreadsheet, and appear on new worksheets.
+
+Figure~\ref{fig:files-brought-into-the-interface-workbook} shows the lower corner of the interface sheet with the additional sheet tabs.
+
+\begin{figure}[hbtp] % fig 27
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image025.png}
+\caption{Files brought into the Interface Workbook \protect \label{fig:files-brought-into-the-interface-workbook}}
+\end{figure}
+
+The results file is named with the name in cell D13 with an extension of out. This file is shown below.
+
+\begin{lstlisting}
+View3D 3.2 0 1 0 6
+400 480 400 480 3000 3000
+0.000000 0.078244 0.029324 0.078217 0.407109 0.407106
+0.065204 0.000000 0.065204 0.044282 0.412652 0.412659
+0.029324 0.078245 0.000000 0.078217 0.407110 0.407105
+0.065181 0.044282 0.065181 0.000000 0.412679 0.412677
+0.054281 0.066024 0.054281 0.066029 0.000000 0.759385
+0.054281 0.066025 0.054281 0.066028 0.759385 0.000000
+0.999 0.999 0.999 0.999 0.999 0.999
+\end{lstlisting}
+
+Excel macro capabilities are used by the interface to convert the text to columns and add the surface names and other headings. The modified results are placed on the Results worksheet as shown in Figure~\ref{fig:view-factors-with-surface-names-inserted}.
+
+\begin{figure}[hbtp] % fig 28
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image026.png}
+\caption{View Factors with Surface Names Inserted \protect \label{fig:view-factors-with-surface-names-inserted}}
+\end{figure}
+
+The results file information is used to generate a UserViewFactor object for EnergyPlus. This object is located in the first column of a new worksheet named UserVFObject. This column can simply be copied and inserted into the EnergyPlus idf file.
+
+If the results sheet does not appear, or the program terminates, the sheet named View3Dlog or the output file by the same name should be consulted. It contains a complete history of the execution. Any problem with the input file or the calculations should show up there.
+
+The extra sheets generated by the VBA macros will be deleted if the program is called with the run button while they are present. The user will be queried to make sure the sheets should be deleted. During the succeeding run, new sheets will be created.
diff --git a/doc/auxiliary-programs/src/weather-converter-program.tex b/doc/auxiliary-programs/src/weather-converter-program.tex
new file mode 100644
index 00000000000..81d6a25e576
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program.tex
@@ -0,0 +1,7 @@
+\chapter{Weather Converter Program}\label{weather-converter-program}
+
+The Weather Converter program is stored in the EnergyPlus folder area under ``PreProcess'' and subsequently in the ``WeatherConverter'' folder.
+
+To perform annual/run period simulations in EnergyPlus, one needs weather data. Most weather data is still issued in an hour by hour (hourly) format though as you will see, EnergyPlus and its weather converter can accept data that has a finer resolution on the data (such as every 10 or 15 minutes).
+
+The special weather format (EPW) used in EnergyPlus is a simple, ascii format as is common in the rest of the inputs for EnergyPlus.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/advanced-use-accessing-weather-conversion.tex b/doc/auxiliary-programs/src/weather-converter-program/advanced-use-accessing-weather-conversion.tex
new file mode 100644
index 00000000000..acfda722e5e
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/advanced-use-accessing-weather-conversion.tex
@@ -0,0 +1,236 @@
+\section{Advanced use - accessing weather conversion capabilities}\label{advanced-use---accessing-weather-conversion-capabilities}
+
+\subsection{Interface to the EPlusWth.dll}\label{interface-to-the-epluswth.dll}
+
+To provide information for outside developers/interfaces that might want to use the basic weather processing utility from within their interface, the EPlusWth.dll was developed. It is actually used by the weather converter utility. In addition to the basic interface calls, six important files are also used by this library. These are placed in the WeatherConverter folder during install of EnergyPlus.
+
+\subsection{Files used by EPlusWth.dll}\label{files-used-by-epluswth.dll}
+
+Each of the files is in a general comma-delimited format. Thus, they can be easily viewed by importing into a spreadsheet program such as Excelâ„¢. The files are used to support information lacking in the source data files and/or supply additional information used during the conversion process. In each case (with one exception), there will be a single or set of ``header'' records describing each column of the file and then the data values of the file will follow on subsequent records. Each of the files is described briefly in the next few sections.
+
+\subsubsection{Abbreviations.csv}\label{abbreviations.csv}
+
+This file does not have a header record, but it consists of 3 columns. It is used for data files that might have 2-character abbreviations for US States or Canadian provinces and provides a translation to the full name and 3-character country code. Likewise, it can use the full name of these items to obtain the 2-character abbreviation or 3-character country code.
+
+\subsubsection{WBANLocations.csv}\label{wbanlocations.csv}
+
+In many older data sets, the station identifier for the weather data uses the WBAN (Weather Bureau Army-Navy) designation system. This has largely been superseded by the WMO (World Meteorological Organization) designation for station collection site identifiers. This file provides a translation between the two identifier systems. In addition, this file contains latitude, longitude, time zone and elevation information for the sites.
+
+\subsubsection{Cal Climate Zone Lat Long data.csv}\label{cal-climate-zone-lat-long-data.csv}
+
+Note that this file has spaces in the name. The California c limate zone data source files do not have standard station identifiers. Rather they use a climate zone designator from 1-16. This file is used to obtain the latitude, longitude, time zone and elevation data for these climate zones. The WYEC2 ``File Source Code'' (field 2, column 6 of each data record) is used to determine that the file is a California compliance type file.
+
+\subsubsection{ASHRAE\_2009\_Yearly\_DesignConditions.csv}\label{ashraeux5f2009ux5fyearlyux5fdesignconditions.csv}
+
+The three files for design conditions have roughly the same format. These are the values from the ASHRAE Handbook of Fundamentals, 2009, Chapter 14, Appendix. The WMO station identifier is used to determine the design condition values that apply to a source data file and, thus, are included in the DESIGN CONDITION header record on the EPW file produced as part of the conversion. This information is also included in the statistical report file (STAT) produced from the weather converter utility. In addition, these are used to supply the information for the design day object (DDY) file creation.
+
+\subsection{Public calls to EPlusWth.dll}\label{public-calls-to-epluswth.dll}
+
+Several points of the library are made available for use with external programs. In each case the parameters passed will be described along with the Visual Basicâ„¢ (VB6) code that is used to declare them as well as Fortran 90 style ``Interface'' statements to the same calls. The library is placed in the same folder with the weather converter utility - you may need to copy it to your program's folder if you choose to add external calls from your program to it.
+
+\subsubsection{SetupPWInternalDataPath}\label{setuppwinternaldatapath}
+
+This call designates the ``path'' to the files listed above. This is the location where the ProcessWeather call will expect to find the files. Having this incorrectly specified is not fatal, but will probably cause confusion.
+
+VB declaration statement:
+
+Private Declare Sub SetupPWInternalDataPath Lib ``EPlusWth'' (ByVal strPath As String, ByVal InPathLen As Long)
+
+And a call from a VB program:
+
+\begin{lstlisting}
+Call SetupPWInternalDataPath(AppPath, Len(AppPath))
+\end{lstlisting}
+
+Likewise for Fortran 90/95:
+
+\begin{lstlisting}[language=Fortran]
+  INTERFACE
+    SUBROUTINE SetupPWInternalDataPath (Path)
+    CHARACTER(len = \*), INTENT(IN) :: Path    ! Path where data files reside
+    END SUBROUTINE
+  END INTERFACE
+\end{lstlisting}
+
+And then calling it from Fortran:
+
+\begin{lstlisting}[language=Fortran]
+Character(len = 255) DataPath
+CALL SetupPWInternalDataPath(trim(DataPath))
+\end{lstlisting}
+
+\subsubsection{SetFixOutOfRangeData}\label{setfixoutofrangedata}
+
+As shown earlier (file menu option in the weather converter utility), there is an option to ``fix'' out of range data or not. By default, this is turned off (does not fix data). Again a character convention (``yes'' for fixing; ``no'' for not fixing) is used. Case of the actual string is ignored.
+
+VB Declaration statement:
+
+Private Declare Sub SetFixOutOfRangeData Lib ``EPlusWth'' (ByVal strValue As String, ByVal strValueLen As Long)
+
+And calling it from VB:
+
+\begin{lstlisting}
+    Global FixOutOfRangeData As String
+    FixOutOfRangeData = "Yes"
+    Call SetFixOutOfRangeData(FixOutOfRangeData, Len(FixOutOfRangeData))
+\end{lstlisting}
+
+For Fortran 90/95:
+
+\begin{lstlisting}[language=Fortran]
+  INTERFACE
+    SUBROUTINE SetFixOutOfRangeData (YesNo)
+    CHARACTER(len = \*),INTENT(IN) :: YesNo    ! 'yes' to set fixing option;
+                                            ! 'no' to not
+    END SUBROUTINE
+  END INTERFACE
+\end{lstlisting}
+
+And then calling it:
+
+\begin{lstlisting}[language=Fortran]
+CALL SetFixOutOfRangeData('no')
+\end{lstlisting}
+
+\subsubsection{SetDefaultChgLimit}\label{setdefaultchglimit}
+
+This call sets the value for the DB trigger shown earlier. Both values passed in are strings and are specific to the dialog shown earlier:
+
+% table 24
+\begin{longtable}[c]{p{1.0in}p{2.0in}p{1.2in}p{1.8in}}
+\caption{Trigger Limit Call Values \label{table:trigger-limit-call-values}} \tabularnewline
+\toprule 
+Trigger Limit & Result & Ignore Calc Trigger & Result \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Trigger Limit Call Values} \tabularnewline
+\toprule 
+Trigger Limit & Result & Ignore Calc Trigger & Result \tabularnewline
+\midrule
+\endhead
+
+0 & use only calculated trigger & 0 & Uses Calculated Trigger \tabularnewline
+1 & use 5°C & 1 & Ignores calculated trigger \tabularnewline
+2 & use 10°C &  &  \tabularnewline
+3 & use 15°C &  &  \tabularnewline
+\bottomrule
+\end{longtable}
+
+You can also choose to ignore the calculated trigger entirely. If you do not ``ignore'' the calculated trigger, then the trigger is the minimum of the calculated and your trigger limit selection.
+
+VB Declaration Statement:
+
+\begin{lstlisting}
+Private Declare Sub SetDefaultChgLimit Lib "EPlusWth" (ByVal strValue As String, ByVal strValueLen As Long, ByVal strValue As String, ByVal strValueLen As Long)
+\end{lstlisting}
+
+And a call from VB:
+
+\begin{lstlisting}
+    Call SetDefaultChgLimit(TriggerLimit, Len(TriggerLimit), IgnoreCalcTrigger, Len(IgnoreCalcTrigger))
+\end{lstlisting}
+
+\subsubsection{ProcessWeather}\label{processweather}
+
+The ``meat'' of the processing is done by this routine. It gets passed the input file name (source data), the input file type, output file name, and output file type. As an output it can provide a notice that the processing was successful or not.
+
+VB Declaration Statement:
+
+\begin{lstlisting}
+Private Declare Sub ProcessWeather Lib "EPlusWth" (ByVal strInType As String, ByVal InTypeLen As Long, ByVal strOutType As String, ByVal OutTypeLen As Long, ByVal strInFileName As String, ByVal InFileNameLen As Long, ByVal strOutFileName As String, ByVal OutFileNameLen As Long, ErrorFlag As Boolean, Optional ByVal strOutFileURL As String, Optional ByVal OutFileURLlen As Long)
+\end{lstlisting}
+
+Calling it from VB:
+
+\begin{lstlisting}
+Call ProcessWeather(InputFileDataType, Len(InputFileDataType),
+      OutputFileDataType, Len(OutputFileDataType),
+      InputFileName, Len(InputFileName),
+      OutputFileName, Len(OutputFileName),
+      ErrorFlag)
+\end{lstlisting}
+
+Valid values for the Input File Data Type are shown in the following table:
+
+% table 25
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Valid Input File Types for ``ProcessWeather'' call \label{table:valid-input-file-types-for-processweather}} \tabularnewline
+\toprule 
+Input File Type & Source Data file Format Type \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Valid Input File Types for ``ProcessWeather'' call} \tabularnewline
+\toprule 
+Input File Type & Source Data file Format Type \tabularnewline
+\midrule
+\endhead
+
+TMY2 or TM2 & TMY2 data file \tabularnewline
+IWEC or IWC & IWEC data file \tabularnewline
+SAMSON or DAT & SAMSON data file \tabularnewline
+WYEC2 or WY2 & WYEC2 data file \tabularnewline
+FMT or TXT & DOE-2 Formatted data file \tabularnewline
+CLM or ESP-r & ESP-r formatted data file \tabularnewline
+BLAST or ASC & BLAST ASCII formatted data file \tabularnewline
+EPW & EnergyPlus EPW file \tabularnewline
+CSV & EnergyPlus CSV file \tabularnewline
+TMY & TMY data files \tabularnewline
+WEA & Eco-Tect WEA files \tabularnewline
+SWERA or SWE & SWERA data files \tabularnewline
+< any > & Custom - must have "def" file \tabularnewline
+\bottomrule
+\end{longtable}
+
+Valid values for the Output File Type(s) are shown in the following table:
+
+% table 26
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Valid Output File Types for the ``ProcessWeather'' call \label{table:valid-output-file-types-for}} \tabularnewline
+\toprule 
+Output File Type & File(s) produced \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Valid Output File Types for the ``ProcessWeather'' call} \tabularnewline
+\toprule 
+Output File Type & File(s) produced \tabularnewline
+\midrule
+\endhead
+
+EPW & EPW and RPT files \tabularnewline
+CSV & CSV and RPT files \tabularnewline
+BOTH & EPW, CSV and RPT files \tabularnewline
+RPT & RPT file \tabularnewline
+\bottomrule
+\end{longtable}
+
+For Input and Output file names, the complete paths should be included.
+
+ErrorFlag will be returned as ``true'' if an error occurs during processing or ``false'' if the process is successful.
+
+Fortran 90/95 Declaration:
+
+\begin{lstlisting}[language=Fortran]
+INTERFACE
+  SUBROUTINE ProcessWeather(InType,OutType,InFileName,OutFileName,ErrFlag)
+    CHARACTER(len = \*), INTENT(IN) :: InType       ! InputFile Type
+    CHARACTER(len = \*), INTENT(IN) :: OutType      ! OutputFile Type
+    CHARACTER(len = \*), INTENT(IN) :: InFileName   ! InputFile Name (Full path)
+    CHARACTER(len = \*), INTENT(IN) :: OutFileName  ! OutputFileName (Full path)
+    LOGICAL(Byte2), INTENT(OUT)  :: ErrFlag      ! If errors are found,
+                                                 ! set to true and put
+                                                 ! description put in file.
+  END SUBROUTINE
+END INTERFACE
+\end{lstlisting}
+
+And calling it from Fortran:
+
+\begin{lstlisting}[language=Fortran]
+call processweather(trim(intype),trim(outtype),    &
+                    trim(infilename),trim(outfilename),errflag)
+\end{lstlisting}
+
+Note that the file where error messages will be placed is the RPT file. If the value of the output file path is incorrect, you may need to search for this file by using the RPT extension.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/ashrae-climate-classification.tex b/doc/auxiliary-programs/src/weather-converter-program/ashrae-climate-classification.tex
new file mode 100644
index 00000000000..30ac1589389
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/ashrae-climate-classification.tex
@@ -0,0 +1,3 @@
+\section{ASHRAE Climate Classification}\label{ashrae-climate-classification}
+
+For the ASHRAE 90.1 and 90.2 standards (2004), a climate zone classification scheme was introduced, similar to the Köppen classification. The methodology is described in two ASHRAE Transactions papers - Briggs - 2002.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/background.tex b/doc/auxiliary-programs/src/weather-converter-program/background.tex
new file mode 100644
index 00000000000..ab1f9ba357f
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/background.tex
@@ -0,0 +1,15 @@
+\section{Background}\label{background}
+
+All building simulation programs employ some means of representing local climatic conditions relative to the building models. For example, Radiance (Ward 1996) needs a description of sky conditions and illuminance values to calculate solar distribution through a window and within a space. Three of the widely used energy simulation programs in the UK and US, ESP-r (ESRU 1999), BLAST (UI 1998), and DOE-2 (Winkelmann et al. 1993) also use weather conditions to simulate the response of a building. But even after 30 years of significant development advances in simulation capabilities, these programs use the same climate representations as in the past-a simple set of hourly temperature, humidity, wind speed and direction, and atmospheric pressure and solar radiation or cloud cover data. These data are often `typical' data derived from hourly observations at a specific location by the national weather service or meteorological office. Examples of these typical data include TMY2 (NREL 1995) and WYEC2 (ASHRAE 1997) in the United States and Canada and TRY (CEC 1985) in Europe. The TMY2 and WYEC2 typical weather years contain more solar radiation and illumination data than older formats such as TMY (NCDC 1983), WYEC (ASHRAE 1985), and TRY (NCDC 1981) in the U.S. Crawley (1998) demonstrated that the methods used to select data for the US TMY2 and European TRY data sets better fits the long-term climate patterns.
+
+Radiation and illumination data are becoming increasingly necessary in simulation programs. Anyone who has ever attempted to measure daylight factors will be familiar with the fluctuations in lighting levels under partly cloudy conditions. The expansion and contraction of lightweight building components also shares sensitivity to rapid fluctuations in solar radiation. Single-sided ventilation is dependant on wind pressure fluctuations and pedestrians in many cities are acquainted with the disarming tendency of the wind to guest and change direction. It is increasingly the case that design questions touch on such issues.
+
+In a research context, the advent of tools such as LabVIEW (National Instruments Corporation 1999) have made it possible for increasing numbers of researchers to acquire and process test-cell data. The increasing use of building energy management systems (BEMS) has also provided high frequency information from which simulation could be used as a predictive tool for future control strategies. Other issues of control, particularly of advanced daylighting control require sub-hourly illumination data to ensure that possible control regimes are tested under realistic conditions. Janak (1997) observed that the differences between 5 minute and hourly illumination data could result in prediction variations approaching 40\%.
+
+Thus far, projects that mix empirical and simulation-based work have had to store and access such data via temporal database facilities (ESRU 1999). As the number of high quality datasets increases so does the need to encapsulate such information in a form that can be broadly distributed. The simulation community must also consider the uncertainty in high frequency performance predictions that are based on boundary conditions that have been sampled at one or two magnitudes less temporal resolution.
+
+The simulation community must also consider practitioner demands and issues of quality assurance. Someone who is not a native of Copenhagen may not know that there are three or four recognizable patterns of winter weather that should be included in detailed assessments. A data set that lacks documentation or is dependent on separately held lists of assumptions can be effectively useless.
+
+In the absence of data within the weather data format, the simulation programs must calculate these data often with older calculation methods. As the simulation programs have become more capable, data at hourly resolution is no longer enough-interpolating between hourly observations does not accurately represent weather conditions that change much more frequently such as illumination.
+
+We have developed a generalized weather data format for use by energy simulation programs has been developed and adopted by both ESP-r (in the UK) and EnergyPlus (in the US). Anticipating the need for data at time steps less than one hour, the format includes a minute field to facilitate the use of sub hourly data. The data include basic location identifiers such as location name, data source, latitude, longitude, time zone, elevation, peak design conditions, holidays, daylight saving period, typical and extreme periods, ground temperatures, period(s) covered by the data and space for descriptive comments. The time step data include dry bulb and dew point temperature, relative humidity, station pressure, solar radiation (global, extraterrestrial, horizontal infrared, direct, and diffuse), illuminance, wind direction and speed, sky cover, and current weather.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/data-sources-uncertainty.tex b/doc/auxiliary-programs/src/weather-converter-program/data-sources-uncertainty.tex
new file mode 100644
index 00000000000..70d5e452744
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/data-sources-uncertainty.tex
@@ -0,0 +1,168 @@
+\section{Data Sources/Uncertainty}\label{data-sourcesuncertainty}
+
+More recent weather data source files have introduced the concept of data sources and uncertainty flags for many of the fields. The EnergyPlus weather format faithfully reproduces these fields as appropriate for the input source data types. By and large, most of the data sources and uncertainties have used the TMY2 established fields and values (See following table). As noted earlier, to enhance readability and reduce obfuscation, the EnergyPlus format for the data source and uncertainty flags collates them into one large field. Each data element still has its data source and uncertainty: it is positionally embodied depending on its place in the EPW data record.
+
+% table 19
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Key to Data Source and Uncertainty Flags \label{table:key-to-data-source-and-uncertainty-flags}} \tabularnewline
+\toprule 
+Data Flag & Flag Values \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Key to Data Source and Uncertainty Flags} \tabularnewline
+\toprule 
+Data Flag & Flag Values \tabularnewline
+\midrule
+\endhead
+
+Dry Bulb Temperature Data Source & A-F \tabularnewline
+Dry Bulb Temperature Data Uncertainty & 0-9 \tabularnewline
+Dew Point Temperature Data Source & A-F \tabularnewline
+Dew Point Temperature Data Uncertainty & 0-9 \tabularnewline
+Relative Humidity Data Source & A-F \tabularnewline
+Relative Humidity Data Uncertainty & 0-9 \tabularnewline
+Atmospheric Station Pressure Data Source & A-F \tabularnewline
+Atmospheric Station Pressure Data Uncertainty & 0-9 \tabularnewline
+Horizontal Infrared Radiation Data Source & A-H, ? \tabularnewline
+Horizontal Infrared Radiation Data Uncertainty & 0-9 \tabularnewline
+Global Horizontal Radiation Data Source & A-H, ? \tabularnewline
+Global Horizontal Radiation Data Uncertainty & 0-9 \tabularnewline
+Direct Normal Radiation Data Source & A-H, ? \tabularnewline
+Direct Normal Radiation Data Uncertainty & 0-9 \tabularnewline
+Diffuse Horizontal Radiation Data Source & A-H, ? \tabularnewline
+Diffuse Horizontal Radiation Data Uncertainty & 0-9 \tabularnewline
+Global Horizontal Illuminance Data Source & I, ? \tabularnewline
+Global Horizontal Illuminance Data Uncertainty & 0-9 \tabularnewline
+Direct Normal Illuminance Data Source & I, ? \tabularnewline
+Direct Normal Illuminance Data Uncertainty & 0-9 \tabularnewline
+Diffuse Horizontal Illuminance Data Source & I, ? \tabularnewline
+Diffuse Horizontal Illuminance Data Uncertainty & 0-9 \tabularnewline
+Zenith Luminance Data Source & I, ? \tabularnewline
+Zenith Luminance Data Uncertainty & 0-9 \tabularnewline
+Wind Direction Data Source & A-F \tabularnewline
+Wind Direction Data Uncertainty & 0-9 \tabularnewline
+Wind Speed Data Source & A-F \tabularnewline
+Wind Speed Data Uncertainty & 0-9 \tabularnewline
+Total Sky Cover Data Source & A-F \tabularnewline
+Total Sky Cover Data Uncertainty & 0-9 \tabularnewline
+Opaque Sky Cover Data Source & A-F \tabularnewline
+Opaque Sky Cover Data Uncertainty & 0-9 \tabularnewline
+Visibility Data Source & A-F, ? \tabularnewline
+Visibility Data Uncertainty & 0-9 \tabularnewline
+Ceiling Height Data Source & A-F, ? \tabularnewline
+Ceiling Height Data Uncertainty & 0-9 \tabularnewline
+Precipitable Water Data Source & A-F \tabularnewline
+Precipitable Water Data Uncertainty & 0-9 \tabularnewline
+Broadband Aerosol Optical Depth Data Source & A-F \tabularnewline
+Broadband Aerosol Optical Depth Data Uncertainty & 0-9 \tabularnewline
+Snow Depth Data Source & A-F, ? \tabularnewline
+Snow Cover Data Uncertainty & 0-9 \tabularnewline
+Days Since Last Snowfall Data Source & A-F, ? \tabularnewline
+Days Since Last Snowfall Data Uncertainty & 0-9 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The definition of the solar radiation source flags and solar radiation uncertainty flags are shown in the following two tables:
+
+% table 20
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Solar Radiation and Illuminance Data Source Flag Codes \label{table:solar-radiation-and-illuminance-data-source}} \tabularnewline
+\toprule 
+Flag Code & Definition \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Solar Radiation and Illuminance Data Source Flag Codes} \tabularnewline
+\toprule 
+Flag Code & Definition \tabularnewline
+\midrule
+\endhead
+
+A & Post-1976 measured solar radiation data as received from NCDC or other sources \tabularnewline
+B & Same as "A" except the global horizontal data underwent a calibration correction \tabularnewline
+C & Pre-1976 measured global horizontal data (direct and diffuse were not measured before 1976), adjusted from solar to local time, usually with a calibration correction \tabularnewline
+D & Data derived from the other two elements of solar radiation using the relationship, global = diffuse + direct ´ cosine (zenith) \tabularnewline
+E & Modeled solar radiation data using inputs of observed sky cover (cloud amount) and aerosol optical depths derived from direct normal data collected at the same location \tabularnewline
+F & Modeled solar radiation data using interpolated sky cover and aerosol optical depths derived from direct normal data collected at the same location \tabularnewline
+G & Modeled solar radiation data using observed sky cover and aerosol optical depths estimated from geographical relationships \tabularnewline
+H & Modeled solar radiation data using interpolated sky cover and estimated aerosol optical depths \tabularnewline
+I & Modeled illuminance or luminance data derived from measured or modeled solar radiation data \tabularnewline
+? & Source does not fit any of the above categories. Used for nighttime values and missing data \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 21
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Solar Radiation and Illuminance Data Uncertainty Flag Codes \label{table:solar-radiation-and-illuminance-data}} \tabularnewline
+\toprule 
+Flag & Uncertainty Range (\%) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Solar Radiation and Illuminance Data Uncertainty Flag Codes} \tabularnewline
+\toprule 
+Flag & Uncertainty Range (\%) \tabularnewline
+\midrule
+\endhead
+
+1 & Not used \tabularnewline
+2 & 2 - 4 \tabularnewline
+3 & 4 - 6 \tabularnewline
+4 & 6 - 9 \tabularnewline
+5 & 9 - 13 \tabularnewline
+6 & 13 - 18 \tabularnewline
+7 & 18 - 25 \tabularnewline
+8 & 25 - 35 \tabularnewline
+9 & 35 - 50 \tabularnewline
+0 & Not applicable \tabularnewline
+\bottomrule
+\end{longtable}
+
+Finally, the Meteorological data source and uncertainty flag/codes are shown in the following two tables:
+
+% table 22
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Meteorological Data Source Flag Codes \label{table:meteorological-data-source-flag-codes}} \tabularnewline
+\toprule 
+Flag & Definition \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Meteorological Data Source Flag Codes} \tabularnewline
+\toprule 
+Flag & Definition \tabularnewline
+\midrule
+\endhead
+
+A & Data as received from NCDC, converted to SI units \tabularnewline
+B & Linearly interpolated \tabularnewline
+C & Non-linearly interpolated to fill data gaps from 6 to 47 hours in length \tabularnewline
+D & Not used \tabularnewline
+E & Modeled or estimated, except: precipitable water, calculated from radiosonde data; dew point temperature calculated from dry bulb temperature and relative humidity; and relative humidity calculated from dry bulb temperature and dew point temperature \tabularnewline
+F & Precipitable water, calculated from surface vapor pressure; aerosol optical depth, estimated from geographic correlation \tabularnewline
+? & Source does not fit any of the above. Used mostly for missing data \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 23
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Meteorological Uncertainty Flag Codes \label{table:meteorological-uncertainty-flag-codes}} \tabularnewline
+\toprule 
+Flag & Definition \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Meteorological Uncertainty Flag Codes} \tabularnewline
+\toprule 
+Flag & Definition \tabularnewline
+\midrule
+\endhead
+
+1- 6 & Not used \tabularnewline
+7 & Uncertainty consistent with NWS practices and the instrument or observation used to obtain the data \tabularnewline
+8 & Greater uncertainty than 7 because values were interpolated or estimated \tabularnewline
+9 & Greater uncertainty than 8 or unknown. \tabularnewline
+0 & Not definable. \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/auxiliary-programs/src/weather-converter-program/definitions-file-custom-file-processing.tex b/doc/auxiliary-programs/src/weather-converter-program/definitions-file-custom-file-processing.tex
new file mode 100644
index 00000000000..6cab527042a
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/definitions-file-custom-file-processing.tex
@@ -0,0 +1,778 @@
+\section{Definitions File \& Custom File Processing}\label{definitions-file-custom-file-processing}
+
+\subsection{\texorpdfstring{Description of ``Def'' input file}{Description of Def input file}}\label{description-of-def-input-file}
+
+Some of the data formats have inherent omissions (e.g.~TMY does not have location data, BLAST ASCII does not have elevations). In order to overcome this limitation and to provide further flexibility, a definitions file (extension must be .def) is implemented. By naming this with the same ``file name'' as your input file (in the same folder), the weather converter will read the format and use that data, as appropriate, in the file conversions. The .def file uses Fortran ``Namelist'' input fields as shown in the example below. For flexibility, you can also define a ``presets.def'' file (such as when you have a list of files to process and the format or some portion is all the same between the group of files. The two def files (one named the same as the file name for the raw data and one named presets.def) will both be processed. Conflicts between the two will be shown in the .audit file. The set of namelist groups is:
+
+\begin{itemize}
+\item
+  \&location - Location data
+\item
+  \&miscdata - Comments to be applied to ``COMMENT2'' in the EPW file and ``Source Data''
+\item
+  \&wthdata - weather data specifications including file type, custom formats
+\item
+  \&datacontrol - user specified control over ``missing'' data (Custom format only)
+\end{itemize}
+
+\textbf{Note that the ``Def'' formats are entirely different from the usual IDF formats of EnergyPlus. No commas separate fields. No semicolon terminates the entry.}
+
+\begin{lstlisting}
+&location
+City = 'Hong Kong'
+StateProv = ' '
+Country = 'CHN'
+InLat = 22.75
+InLong = 115
+InTime = 8
+InElev = 0
+InWMO = 450040
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&miscdata
+Comments1 = 'This file was given to us by....'
+SourceData = 'Original xyz data'
+/
+\end{lstlisting}
+
+The ``slash'' (/) character terminating each block is very important - omissions results in incorrect reading of data.
+
+Definitions File Details are shown in the following table. You may leave out a field if you wish - the program will use whatever default is applicable (or usable) from the data format. All data formats accept this additional file. Only Custom format currently uses the \&datacontrol element. And only Custom format input type uses the Data Elements, Format and Conversion factors from the \&wthdata element.
+
+Note that strings in the ``def'' should be enclosed in single quotes if there is more than one word in the string - if only one word, quotes do not need to be used.
+
+% table 4
+\begin{longtable}[c]{p{2.12in}p{1.5in}p{2.37in}}
+\caption{Definitions File \&location description \label{table:definitions-file-location-description}} \tabularnewline
+\toprule 
+\& location Field Description & Field Name & Type \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Definitions File \&location description} \tabularnewline
+\toprule 
+\& location Field Description & Field Name & Type \tabularnewline
+\midrule
+\endhead
+
+Name of City & City & String \tabularnewline
+State or Province & StateProv & String \tabularnewline
+Country Code & Country & String (3 characters) \tabularnewline
+Latitude (N+/S-) & InLat & Numeric \tabularnewline
+Longitude (W-/E+) & InLong & Numeric \tabularnewline
+Time Zone (GMT +/-) & InTime & Numeric \tabularnewline
+Elevation (meters) & InElev & Numeric \tabularnewline
+WMO \# & InWMO & Numeric or String (6 characters) \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Expected Formats for \&location}\label{expected-formats-for-location}
+
+\subsubsection{Fields: City, StateProv, Country}\label{fields-city-stateprov-country}
+
+These fields are string variables. If Country is \emph{not} included, an attempt to use the State/Prov entry may be used to determine country. Otherwise, these fields are not validated and are used to create part of the ``location'' header record in the EPW file. City can be up to 30 characters in length; StateProv up to 15 characters; Country up to 10 characters (standard 3 character abbreviation preferred).
+
+\subsubsection{Fields: InLat, InLong}\label{fields-inlat-inlong}
+
+These fields are decimal equivalent for Latitude and Longitude. The convention is North Latitude is positive; South is negative. Likewise, East Longitude is positive; West Longitude is negative. That is, if your latitude is N 30° 15' (North 30 degrees, 15 minutes) then your input is +30.25.
+
+\subsubsection{Field: InTime}\label{field-intime}
+
+This field is the decimal equivalent for the Time Zone value. The convention is GMT +/-. That is, if your time zone is ``behind'' GMT time by 6 hours, your input would be -6.
+
+\subsubsection{Field: InElev}\label{field-inelev}
+
+This field is the location elevation in meters. Range can be from -300 to 6096. (These are the values from EnergyPlus - there is no validation of these in the weather converter.)
+
+\subsubsection{Field: InWMO}\label{field-inwmo}
+
+This field is the WMO (World Meterological Organization) number for the location. Though not validated per se, if found in the ``design conditions'' auxiliary files, the Design Day information can be generated.
+
+% table 5
+\begin{longtable}[c]{@{}lll@{}}
+\caption{Definitions File - \&miscdata description \label{table:definitions-file-miscdata-description}} \tabularnewline
+\toprule 
+\& mischata Field Description & Field Name & Type \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Definitions File - \&miscdata description} \tabularnewline
+\toprule 
+\& mischata Field Description & Field Name & Type \tabularnewline
+\midrule
+\endhead
+
+String for Comments 1 header & Comments1 & String \tabularnewline
+String for Comments 2 header & Comments2 & String \tabularnewline
+String for Source Data in Location header & SourceData & String \tabularnewline
+URL for output & OutputURL & String \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Expected Formats for \&miscdata}\label{expected-formats-for-miscdata}
+
+\subsubsection{Fields: Comments1, Comments2}\label{fields-comments1-comments2}
+
+These are strings. After concatenation, they become part of the comment header lines in the EPW headers. Up to 150 characters each is allowed.
+
+\subsubsection{Field: SourceData}\label{field-sourcedata}
+
+This string is applied to the ``Source Data'' field in the Location Header. Up to 60 characters is allowed.
+
+\subsubsection{Field: OutputURL}\label{field-outputurl}
+
+When a list of files is being processed, one of the outputs that results from the processing is a KML (Keyhole Markup Language) file that can be used with Google Earth to pinpoint the locations of the weather site. This field can be used to set this URL for later output. The list file format also includes a URL as its third (optional) parameter. If included, this input would overwrite other URL designations.
+
+% table 6
+\begin{longtable}[c]{p{2.71in}p{1.5in}p{1.79in}}
+\caption{Definitions file - \&wthdata description \label{table:definitions-file-wthdata-description}} \tabularnewline
+\toprule 
+\& wthdata Field Description & Field Name & Type \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Definitions file - \&wthdata description} \tabularnewline
+\toprule 
+\& wthdata Field Description & Field Name & Type \tabularnewline
+\midrule
+\endhead
+
+Input File Type & InputFileType & String \tabularnewline
+Number of records per hour & NumInHour & Integer \tabularnewline
+Data Element Names & DataElements & Strings \tabularnewline
+Data Units & DataUnits & Strings \tabularnewline
+Multiplicative Conversion Factors for Data & DataConversionFactors & Numeric \tabularnewline
+Special Missing Values & DataMissingValues & Numeric \tabularnewline
+Format for input & InFormat & Format String or "delimited" \tabularnewline
+Delimiter Character & DelimiterChar &  \tabularnewline
+Decimal Delimiter Character & DecimalSymbolChar & String \tabularnewline
+Date Separator & DateSeparator & String (single character) \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Expected Formats for \&wthdata}\label{expected-formats-for-wthdata}
+
+\subsubsection{Field: InputFileType}\label{field-inputfiletype}
+
+You can always use this field and def file to ``override'' the default input format type that depends on the extension of your file (see Table~\ref{table:input-file-extensions-with-implied-data-types}. Input File Extensions with implied Data types). A complete set of valid values for Input File types is shown in the following table. Data Files are described more fully in the section Source Weather Data Formats that occurs later in this document.
+
+% table 7
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Input File Type Values \label{table:input-file-type-values}} \tabularnewline
+\toprule 
+Value & File Type Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Input File Type Values} \tabularnewline
+\toprule 
+Value & File Type Description \tabularnewline
+\midrule
+\endhead
+
+Tmy or ,tm2 & TMY2 Data File \tabularnewline
+Iwec or iwc & IWEC Data File \tabularnewline
+Samson or dat & SAMSON Data File \tabularnewline
+wyec2 or wy2 & WYEC2 Data File \tabularnewline
+Fmt or txt & DOE-2 FMT File \tabularnewline
+Clm or esp-r & ESP-r Formatted (CLM) data file \tabularnewline
+Blast or asc & BLAST ASCII Data File \tabularnewline
+Tmy & TMY Data File \tabularnewline
+Epw & EPW Data File \tabularnewline
+Csv & EPW - CSV Data File \tabularnewline
+Wea & Ecotect wea Data File \tabularnewline
+Swera or swe & SWERA Data File \tabularnewline
+Custom or User & Custom Data File \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Field: NumInHour}\label{field-numinhour}
+
+This field can be used to specify multi-interval (per hour) files. Without this field, the only formats that can have multiple intervals per hour are the EPW and CSV file formats - using the header record DataPeriods value for that field.
+
+\subsubsection{\texorpdfstring{Fields below only used in ``Custom'' format processing}{Fields below only used in Custom format processing}}\label{fields-below-only-used-in-custom-format-processing}
+
+\subsubsection{Field: DataElements}\label{field-dataelements}
+
+For custom files, you will need to indicate which data elements are in which positions of the raw data file. The fields must come from a standardized list of names see following tables that include internal names (short and long - as shown in Table 8) as well as the EnergyPlus CSV format names (short and long - shown in Table~\ref{table:names-from-the-energyplus-csv-files}) plus some further elements that can be specified when the standard data elements are not part of the raw data (as shown in Table~\ref{table:auxiliary-data-for-custom-files}). ``Ignore'' is used to skip a raw data field that is not applicable to the weather converter formats. Note that variables listed in the following table (in italics) are allowed for flexibility - i.e.~wetbulb temperature can be used to determine relative humidity and/or dewpoint temperature. The following three tables illustrate the names for data elements.
+
+\begin{longtable}[c]{p{1.5in}p{2.5in}p{1.0in}p{1.0in}}
+
+\caption{Internal Data Element Names (directly applicable to EPW) \label{table:internal-data-element-names-directly}} \tabularnewline
+\toprule 
+Short Name & Long Name & Default EPW Units & Used by EnergyPlus \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Internal Data Element Names (directly applicable to EPW)} \tabularnewline
+\toprule
+Short Name & Long Name & Default EPW Units & Used by EnergyPlus \tabularnewline
+\midrule
+\endhead
+
+year & Year & - & n \tabularnewline
+month & Month & - & y \tabularnewline
+day & Day & - & y \tabularnewline
+hour & hour & - & y \tabularnewline
+minute & minute & - & n \tabularnewline
+datasource & datasource & - & n \tabularnewline
+drybulb & dry\_bulb\_temperature & C & y \tabularnewline
+dewpoint & dew\_point\_temperature & C & y \tabularnewline
+relhum & relative\_humidity & \% & y \tabularnewline
+atmos\_pressure & atmospheric\_pressure & Pa & y \tabularnewline
+exthorrad & extraterrestrial\_horizontal\_radiation & Wh/m2 & n \tabularnewline
+extdirrad & extraterrestrial\_direct\_normal\_radiation & Wh/m2 & n \tabularnewline
+horirsky & horizontal\_infrared\_radiation\_intensity\_from\_sky & Wh/m2 & y \tabularnewline
+glohorrad & global\_horizontal\_radiation & Wh/m2 & n \tabularnewline
+dirnorrad & direct\_normal\_radiation & Wh/m2 & y \tabularnewline
+difhorrad & diffuse\_horizontal\_radiation & Wh/m2 & y \tabularnewline
+glohorillum & global\_horizontal\_illuminance & lux & n \tabularnewline
+dirnorillum & direct\_normal\_illuminance & lux & n \tabularnewline
+difhorillum & diffuse\_horizontal\_illuminance & lux & n \tabularnewline
+zenlum & zenith\_luminance & lux & n \tabularnewline
+winddir & wind\_direction & degrees & y \tabularnewline
+windspd & wind\_speed & m/2 & y \tabularnewline
+totskycvr & total\_sky\_cover & tenths & n \tabularnewline
+opaqskycvr & opaque\_sky\_cover & tenths & n \tabularnewline
+visibility & visibility & km & n \tabularnewline
+ceiling\_hgt & ceiling\_height & m & n \tabularnewline
+presweathobs & present\_weather\_observation & - & y \tabularnewline
+presweathcodes & present\_weather\_codes & - & y \tabularnewline
+precip\_wtr & precipitable\_water & mm & n \tabularnewline
+aerosol\_opt\_depth & aerosol\_optical\_depth & thousandths & N \tabularnewline
+snowdepth & snow\_depth & cm & Y \tabularnewline
+days\_last\_snow & days\_since\_last\_snow & - & N \tabularnewline
+Albedo & albedo & - & N \tabularnewline
+liq\_precip\_depth & liquid\_precip\_depth & mm & Y \tabularnewline
+liq\_precip\_rate & liquid\_precip\_rate & Hour & N \tabularnewline
+\bottomrule
+\end{longtable}
+
+The following table illustrates that the EnergyPlus CSV header names can be used for data elements in DEF files, if desired.
+
+% table 9
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Names from the EnergyPlus CSV files \label{table:names-from-the-energyplus-csv-files}} \tabularnewline
+\toprule 
+Short Name & Long Name & Default EPW Units & Used by EnergyPlus \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Names from the EnergyPlus CSV files} \tabularnewline
+\toprule 
+Short Name & Long Name & Default EPW Units & Used by EnergyPlus \tabularnewline
+\midrule
+\endhead
+
+Date & Date (used to derive Month/Day) & - & N \tabularnewline
+hh:mm & HH:MM (used to derive hour/minute) & - & N \tabularnewline
+datasource & datasource & - & N \tabularnewline
+Drybulb & dry bulb temperature & C & Y \tabularnewline
+dewpoint & dew point temperature & C & Y \tabularnewline
+Relhum & relative humidity & \% & Y \tabularnewline
+atmos pressure & atmospheric pressure & Pa & Y \tabularnewline
+exthorzrad & extraterrestrial horizontal radiation & Wh/m2 & N \tabularnewline
+extdirrad & extraterrestrial direct normal radiation & Wh/m2 & N \tabularnewline
+horzirsky & horizontal infrared radiation intensity from sky & Wh/m2 & Y \tabularnewline
+glohorzrad & global horizontal radiation & Wh/m2 & N \tabularnewline
+dirnorzrad & direct normal radiation & Wh/m2 & Y \tabularnewline
+difhorzrad & diffuse horizontal radiation & Wh/m2 & Y \tabularnewline
+glohorzillum & global horizontal illuminance & lux & N \tabularnewline
+dirnorzillum & direct normal illuminance & lux & N \tabularnewline
+difhorzillum & diffuse horizontal illuminance & lux & N \tabularnewline
+Zenlum & zenith luminance & lux & N \tabularnewline
+winddir & wind direction & degrees & Y \tabularnewline
+windspd & wind speed & m/2 & Y \tabularnewline
+totskycvr & total sky cover & tenths & N \tabularnewline
+opaqskycvr & opaque sky cover & tenths & N \tabularnewline
+visibility & visibility & km & N \tabularnewline
+ceiling hgt & ceiling height & m & N \tabularnewline
+presweathobs & present weather observation & - & Y \tabularnewline
+presweathcodes & present weather codes & - & Y \tabularnewline
+precip wtr & precipitable water & mm & N \tabularnewline
+aerosol opt depth & aerosol optical depth & thousandths & N \tabularnewline
+snowdepth & snow depth & cm & Y \tabularnewline
+days last snow & days since last snow & - & N \tabularnewline
+Albedo & albedo & - & N \tabularnewline
+rain & liquid precipitation depth & mm & Y \tabularnewline
+rain quantity & liquid precipitation rate & Hour & N \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Custom Files - Auxiliary Data}\label{custom-files---auxiliary-data}
+
+Often raw data files will not have the preceding elements but similar elements that can be used to derive the values used in the EPW files and in EnergyPlus. (For example, dew point temperature and relative humidity are needed and can be derived from dry builb temperature and a humidity indicating element such as wet bulb temperature or humidity ratio). The following table contains the data element names that can be used in the Weather Converter program to derive other data which will then be placed into the EPW data fields.
+
+% table 10
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Auxiliary Data for Custom Files \label{table:auxiliary-data-for-custom-files}} \tabularnewline
+\toprule 
+Short Name & Long Name & Units & Useh by EnergyPlus \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Auxiliary Data for Custom Files} \tabularnewline
+\toprule 
+Short Name & Long Name & Units & Useh by EnergyPlus \tabularnewline
+\midrule
+\endhead
+
+wetbulb & wet\_bulb\_temperature & C & N \tabularnewline
+humratio & humidity\_ratio & g/kg & N \tabularnewline
+dirhorrad & direct\_horizontal\_radiation & Wh/m2 & N \tabularnewline
+interval & Interval & unit & N \tabularnewline
+hour\_yr & hour\_of\_year & hour & N \tabularnewline
+time & Time & hh:mm & N \tabularnewline
+hh:mm & HH:MM & hh:mm & N \tabularnewline
+Date & Date & mm/dd/yyyy & N \tabularnewline
+\bottomrule
+\end{longtable}
+
+Explanation of these data elements follows:
+
+\subsubsection{Wetbulb (Wet Bulb Temperature)}\label{wetbulb-wet-bulb-temperature}
+
+If you have the wet bulb temperature, this data element can be used to derive the dew point temperature and relative humidity.
+
+\subsubsection{HumRatio (Humidity Ratio)}\label{humratio-humidity-ratio}
+
+If you have the humidity ratio, this data element can be used to derive the dew point temperature and relative humidity.
+
+\subsubsection{Dirhorrad (Direct Horizontal Radiation)}\label{dirhorrad-direct-horizontal-radiation}
+
+If you have direct horizontal radiation (and at least one other solar element from global horizontal radiation or diffuse horizontal radaition), this data element will be used to derive the direct normal radiation.
+
+\subsubsection{Interval}\label{interval}
+
+If your ``number of records per hour'' is \textgreater{}1, then you can designate each interval of that hour with this field.
+
+\subsubsection{Hour\_Of\_Year}\label{hourux5fofux5fyear}
+
+If you wish, you can just put in the hour of the year for each record. Note that if no date element is entered, then the default is that the data is in hour of the year (including possible number of records per hour).
+
+\subsubsection{Time (or HH:MM)}\label{time-or-hhmm}
+
+Time can be entered (rather than hour) and the units must be hh:mm; this is then decoded on each record to the appropriate hour.
+
+\subsubsection{Date}\label{date}
+
+Dates can be entered as month, day, and year. The units field must be entered and should designate the format for the date decoding. Date separator characters for this field are entered in the DateSeparator item. Default date separator is ``/'' and that is what is used in the table that shows the allowable units:
+
+% table 11
+\begin{longtable}[c]{@{}lll@{}}
+\caption{Allowable hate formats for Custom Data entries. \label{table:allowable-hate-formats-for-custom-data}} \tabularnewline
+\toprule 
+Units Format & Interpretation & Example \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Allowable hate formats for Custom Data entries.} \tabularnewline
+\toprule 
+Units Format & Interpretation & Example \tabularnewline
+\midrule
+\endhead
+
+mm/dd/yyyy mm/dd/yy m/d/y & Month, day, year & 12/13/2009 \tabularnewline
+yyyy/mm/dd yy/mm/dd y/m/d & Year, month, day & 2009/12/13 \tabularnewline
+dd/mm/yyyy dd/mm/yy d/m/y & Day, month, year & 13/12/2009 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Field: DataUnits}\label{field-dataunits}
+
+There should be as many DataUnits entries as DataElement entries. These are not generally used but may be used in the future for automatic conversions. The exception to this is ``temperature'' fields. Use ``f'' for Fahrenheit, ``k'' for Kelvin temperatures. Note that the DataConversionFactor for this field will be applied prior to conversion. (Many formats use integer numbers to represent values that are in tenths, for example.)
+
+\subsubsection{Field: DataConversionFactors}\label{field-dataconversionfactors}
+
+There should be as many DataConversionFactors entries as DataElement entries. These factors are multiplicative factors (i.e.~the input value is multiplied by this factor) and can be used to process input data into the values used in the EPW weather files.
+
+\subsubsection{Field: DataMissingValues}\label{field-datamissingvalues}
+
+There should be as many entries (though some can be blank) as DataElement entries. The values entered will override the default ``missing'' values (from the EPW data dictionary) and, whereas the defaults may be interpreted as a \textgreater{} = missing value (i.e. \textgreater{} = 999), these values will be exact (i.e. = -999.)
+
+\subsubsection{Field: InFormat}\label{field-informat}
+
+The value in this field should be ``delimited'' if you are using a free format data file or specify a ``Fortran style'' format statement.
+
+\subsubsection{Field: DelimiterChar}\label{field-delimiterchar}
+
+If you use a ``delimited'' format file, you need to specify a delimiter character. Only a single character may be specified.
+
+\subsubsection{Field: DecimalSymbolChar}\label{field-decimalsymbolchar}
+
+A single character can be used to specify the decimal ``point'' character. Default is the US Standard ``.''. With use of DelimiterChar and this field, one can essentially use the fields to specify European Standard Excel export formats.
+
+\subsubsection{Field: DateSeparator}\label{field-dateseparator}
+
+If you are entering the aforementiond ``date'' Data Element and your date separator is a character other than slash (``/''), then you need to enter a single character so the program can interpret your date entries.
+
+% table 12
+\begin{longtable}[c]{p{1.81in}p{1.65in}p{2.52in}}
+\caption{Definitions file - \&datacontrol description \label{table:definitions-file-datacontrol-description}} \tabularnewline
+\toprule 
+\& datacontrol Field Description & Field Name & Type \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Definitions file - \&datacontrol description} \tabularnewline
+\toprule 
+\& datacontrol Field Description & Field Name & Type \tabularnewline
+\midrule
+\endhead
+
+Records to Skip & NumRecordsToSkip & Integer \tabularnewline
+Records to Read & MaxNumRecordsToRead & Integer \tabularnewline
+Missing Data Action & MissingDataAction &  \tabularnewline
+Missing Wind Direction Action & MissingWindDirAction &  \tabularnewline
+Missing Wind Direction Value & MissingWindDirValue & Real \tabularnewline
+Missing Opaque Sky Cover Action & MissingOpaqueSkyCoverAction &  \tabularnewline
+Missing Opaque Sky Cover Value & MissingOpaqueSkyCoverValue & Real (Value 0.0 to 10.0) - tenths of sky cover \tabularnewline
+Maximum Wind Speed & MaxWindSpeed & Real \tabularnewline
+Maximum Direct Solar & MaxDirectSolar & Real \tabularnewline
+Maximum Diffuse Solar & MaxDiffuseSolar & Real \tabularnewline
+Maximum Illuminance Value & MaxIlluminanceValue & Real \tabularnewline
+Generate Solar Radiation Warnings & GenerateSolarRadiationWarnings &  \tabularnewline
+Generate Illuminance Warnings & GenerateIlluminanceWarnings &  \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Expected Formats for \&datacontrol}\label{expected-formats-for-datacontrol}
+
+Most of the items in this element are particularly applicable to custom format input files. Currently, they are only used in custom files, but may be more generally applicable in future releases.
+
+\subsubsection{Field: NumRecordsToSkip}\label{field-numrecordstoskip}
+
+This is an integer number of records to skip during processing. You might use this if your input file has some information at the top of the file.
+
+\subsubsection{Field: MaxNumRecordsToRead}\label{field-maxnumrecordstoread}
+
+This is an integer number of records to read (typically 8760 for a full year). You might use this if your input file has some information after the data records.
+
+\subsubsection{Fields: MissingDataAction, MissingWindDirAction, MissingOpaqueSkyCoverAction}\label{fields-missingdataaction-missingwinddiraction-missingopaqueskycoveraction}
+
+These fields tell the converter program what to do with ``missing'' data. Missing data can be found in two forms: totally not included in the DataElements or a missing value (as defined in the EPW format). Valid values for these fields are:
+
+\begin{itemize}
+\item
+  DEFAULT - use the default processing that the weather converter already uses - starts off with a specific value and updates if data is found.
+\item
+  CONSTANT - use a constant value to replace all missing data
+\item
+  RANDOM - use a random number to generate the missing data
+\end{itemize}
+
+An additional value for MissingOpaqueSkyCoverAction is:
+
+\begin{itemize}
+\tightlist
+\item
+  TOTALSKY - use the value for Total Sky Cover
+\end{itemize}
+
+\subsubsection{Fields: MissingWindDirValue, MissingOpaqueSkyCoverValue}\label{fields-missingwinddirvalue-missingopaqueskycovervalue}
+
+The values specified in this field are used with the action fields previously mentioned.
+
+\subsubsection{Field: MaxWindSpeed}\label{field-maxwindspeed}
+
+The default maximum wind speed (40m/s) may not be enough for some locations - this allows the override capability.
+
+\subsubsection{Field: MaxDirectSolar, MaxDiffuseSolar, MaxIlluminanceValue}\label{field-maxdirectsolar-maxdiffusesolar-maxilluminancevalue}
+
+Default maximum solar values may not be enough for some locations - this allows the override capability.
+
+\subsubsection{Field: GenerateSolarRadiationWarnings, GenerateIlluminanceWarnings}\label{field-generatesolarradiationwarnings-generateilluminancewarnings}
+
+If you don't want to see extra warnings when input values are greater than max values (default or as specified in previous fields), use NO as the keyword. Use YES to make sure you see the warnings. Default is YES.
+
+\subsection{Def File Examples}\label{def-file-examples}
+
+In the following examples, every attempt has been made to make sure that these work with the Weather Converter program. However, we cannot foresee all possible combinations. \textbf{Caveat emptor - user beware.}
+
+Here's an example where the delimiter between fields is a semi-colon (;) and the decimal symbol character is a comma (,) - typical of some non-USA regional settings:
+
+\begin{lstlisting}
+&location
+City = <cityname>
+StateProv = <state/province>
+Country = <country>
+InWMO = <wmo>
+InLat = <latitude>
+InLong = <longitude>
+InElev = <elevation>
+InTime = <timezone>
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&wthdata
+NumInHour = 1
+InputFileType = 'CUSTOM'
+InFormat = 'DELIMITED'
+DataElements = Date,HH:MM,Datasource,Dry Bulb Temperature,Dew Point Temperature,Relative Humidity,Atmospheric Pressure,Extraterrestrial Horizontal Radiation,Extraterrestrial Direct Normal Radiation,Horizontal Infrared Radiation Intensity from Sky,Global Horizontal Radiation,Direct Normal Radiation,Diffuse Horizontal Radiation,Global Horizontal Illuminance,Direct Normal Illuminance,Diffuse Horizontal Illuminance,Zenith Luminance,Wind Direction,Wind Speed,Total Sky Cover,Opaque Sky Cover,Visibility,Ceiling Height,Present Weather Observation,Present Weather Codes,Precipitable Water,Aerosol Optical Depth,Snow Depth,Days Since Last Snow,Albedo,Liquid Precipitation Depth,Liquid Precipitation Quantity
+DataUnits = 'mm.dd.yyyy','hh:mm','x','x','x','x','C','C','%','Pa','Wh/m2','Wh/m2','Wh/m2','Wh/m2','Wh/m2','Wh/m2','lux','lux','lux','Cd/m2','deg','m/s','tenths','tenths','km','m','x','x','mm','{.001}','cm','x','{.01}','mm','hr'
+DataConversionFactors = 1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1
+DelimiterChar = ';'
+DateSeparator = '.'
+DecimalSymbolChar = ','
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&datacontrol
+NumRecordsToSkip = 19
+MaxNumRecordsToRead = 8784
+MissingWindDirAction = RANDOM
+/
+\end{lstlisting}
+
+Figure 4. DEF file for with non-standard field delimiter and decimal symbol
+
+Here's an example of a file used to ``enhance'' a DOE-2 FMT file:
+
+\begin{lstlisting}
+&location
+City = 'Kelburn'
+StateProv = 'Wellington'
+Country = 'NZL'
+InWMO = 934360
+InLat = -42.3333
+InLong = 174.8
+InElev = 8
+InTime = 1
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&wthdata
+NumInHour = 1
+InputFileType = 'FMT'
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&miscdata
+Comments1 = 'Standard Data Files for Computer Thermal Simulation of Solar Low Energy Non-residential Buildings; ven der Werff, Amor, and Donn 1990'
+Comments2 = 'Full Actual year of dataSource data is TRY format converted to DOE-2 format;'
+/
+\end{lstlisting}
+
+Figure 5. DEF file for DOE-2 FMT file
+
+Here's an example of a fixed format used for custom file processing. Note that random sky cover is used, to facilitate calculating Horizontal IR from Sky that is used in EnergyPlus. Also, random wind direction is used because the data set does not contain wind direction.
+
+\begin{lstlisting}
+&location
+City = 'Torino-Caselle'
+StateProv = ' '
+Country = 'ITA'
+InWMO = 160590
+InLat = 45.18333
+InLong = 7.65
+InElev = 282
+InTime = 1
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&wthdata
+NumInHour = 1
+InputFileType = 'CUSTOM'
+InFormat = '(I2, I2, I2, F7.2, F7.2, F5.1, F5.1, F5.1)'
+DataElements = Month,Day,Hour,DirNorRad,DifHorRad,DryBulb,Wind\_Speed,Relative\_Humidity
+DataUnits = ,,,'kJ/M2','kJ/M2','C','m/s','%'
+DataConversionFactors = 1,1,1,.2777778,.2777778,1,1,1
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&miscdata
+Comments1 = 'Italian Climate Data Set Gianni de Giorgio'
+Comments2 = 'Period of record 1951-1970'
+SourceData = 'IGDG Data Set'
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&datacontrol
+MissingOpaqueSkyCoverAction = RANDOM
+MissingWindDirAction = RANDOM
+/
+\end{lstlisting}
+
+Figure 6. DEF file for formatted custom file.
+
+An example of a free format custom file. Here, there were several lines of text after the numeric data at the end of the file - thus we used the number of records to read parameter rather than hand editing each input file.
+
+\begin{lstlisting}
+&location
+City = 'Beijing'
+StateProv = 'Beijing'
+Country = 'CHN'
+InWMO = '545110'
+InLat = 39.92
+InLong = 116.27
+InElev = 55
+InTime = 8
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&miscdata
+Comments1 = 'China Data Set - Zhang/Huang'
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&wthdata
+NumInHour = 1
+InputFileType = 'CUSTOM'
+InFormat = 'DELIMITED'
+DataElements = Ignore,Year,Month,Day,Hour,Ignore,DryBulb,DewPoint,Ignore,Relative\_Humidity,Ignore,DirNorRad,DifHorRad,WindDir,Wind\_Speed,OpaqSkyCvr,Atmos\_Pressure
+DataUnits = x,x,x,x,x,x,'k','k',x,'%',x,'wh/m2','wh/m2','deg','m/s',x,'Pa'
+DataConversionFactors = 1,1,1,1,1,1,.1,.1,1,1,1,1,1,1,.1,.1,10
+DelimiterChar = ' '
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&datacontrol
+NumRecordsToSkip = 0
+MaxNumRecordsToRead = 8760
+/
+\end{lstlisting}
+
+Figure 7. DEF File for delimited custom file.
+
+Suppose you have a file that is ``almost'' TMY2 format. You can easily specify a Def file to treat it as a custom file rather than a TMY2 file (which, by standards, will have the data filled).
+
+\begin{lstlisting}
+&location
+City = <cityname>
+StateProv = <state/province>
+Country = <country>
+InWMO = <wmo>
+InLat = <latitude>
+InLong = <longitude>
+InElev = <elevation>
+InTime = <timezone>
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&wthdata
+NumInHour = 1
+InputFileType = 'CUSTOM'
+InFormat = '(1X,I2,I2,I2,I2,I4,I4,I4,A2,I4,A2,I4,A2,I4,A2,I4,A2,I4,A2,I4,A2,I2,A2,I2,A2,I4,A2,I4,A2,I3,A2,I4,A2,I3,A2,I3,A2,I4,A2,I5,A2,I1,A9,I3,A2,I3,A2,I3,A2,I2,A2)'
+DataElements = ignore,year,month,day,hour,ExtHorzRad,ExtDirNormRad,GloHorzRad,ignore,DirNormRad,ignore,DifHorzRad,ignore,GloHorzIllum,ignore,DirNormIllum,ignore,DifHorzIllum,ignore,ZenithLum,ignore,ignore,ignore,ignore,ignore,DryBulb,ignore,DewPoint,ignore,RelHumid,ignore,Pressure,ignore,WindDir,ignore,WindSpd,ignore,Visibility,ignore,CeilHgt,ignore,ObsIndicator,WeatherCodes,PrecWtr,ignore,AerOptDepth,ignore,SnowDepth,ignore,DaysSnow,ignore
+DataUnits = 'x','x','x','x','x','x','Wh/m2','Wh/m2','Wh/m2','x','Wh/m2','x','Wh/m2','x','lux','x','lux','x','lux','x','Cd/m2','x','x','x','x','x','C','x','C','x','%','x','x','x','deg','x','m/s','x','x','x','x','x','x','x','x','x','x','x','x','x','x','x'
+DataConversionFactors = 1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,0.1,1,0.1,1,1,1,100,1,1,1,0.1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&miscdata
+Comments1 = 'Custom DEF format for TMY2 formatted files.'
+SourceData = 'TMY2'
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&datacontrol
+NumRecordsToSkip = 1
+MaxNumRecordsToRead = 8784
+MissingWindDirAction = RANDOM
+MissingDataAction = DEFAULT
+MissingOpaqueSkyCoverAction = RANDOM
+/
+\end{lstlisting}
+
+Figure 8. DEF File for almost TMY2 files.
+
+Finally, an example of using an EPW file as a custom file with a DEF format. Note that the specially formatted CSV files from EnergyPlus can be automatically read in and this format is provided as an extra bonus.
+
+\begin{lstlisting}
+&location
+City = <cityname>
+StateProv = <state/province>
+Country = <country>
+InWMO = <wmo>
+InLat = <latitude>
+InLong = <longitude>
+InElev = <elevation>
+InTime = <timezone>
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&wthdata
+NumInHour = 1
+InputFileType = 'CUSTOM'
+InFormat = 'DELIMITED'
+DataElements = year,month,day,hour,minute,datasource,Dry\_Bulb\_Temperature,Dew\_Point\_Temperature,Relative\_Humidity,Atmospheric\_Pressure,Extraterrestrial\_Horizontal\_Radiation,Extraterrestrial\_Direct\_Normal\_Radiation,Horizontal\_Infrared\_Radiation\_Intensity\_from\_Sky,Global\_Horizontal\_Radiation,Direct\_Normal\_Radiation,Diffuse\_Horizontal\_Radiation,Global\_Horizontal\_Illuminance,Direct\_Normal\_Illuminance,Diffuse\_Horizontal\_Illuminance,Zenith\_Luminance,Wind\_Direction,Wind\_Speed,Total\_Sky\_Cover,Opaque\_Sky\_Cover,Visibility,Ceiling\_Height,Present\_Weather\_Observation,Present\_Weather\_Codes,Precipitable\_Water,Aerosol\_Optical\_Depth,Snow\_Depth,Days\_Since\_Last\_Snow,Albedo,Liquid\_Precipitation\_Depth,Liquid\_Precipitation\_Quantity
+DataUnits = 'x','x','x','x','x','x','C','C','%','Pa','Wh/m2','Wh/m2','Wh/m2','Wh/m2','Wh/m2','Wh/m2','lux','lux','lux','Cd/m2','deg','m/s','tenths','tenths','km','m','x','x','mm','{.001}','cm','x','{.01}','mm','hr'
+DataConversionFactors = 1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1
+DelimiterChar = ','
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&miscdata
+Comments1 = 'Standard EPW Custom def format for reading EPW files in EnergyPlus Weather Converter'
+SourceData = 'EPW'
+/
+\end{lstlisting}
+
+\begin{lstlisting}
+&datacontrol
+NumRecordsToSkip = 8
+MaxNumRecordsToRead = 8784
+MissingWindDirAction = RANDOM
+/
+\end{lstlisting}
+
+Figure 9. DEF File for EPW files.
+
+\subsection{Custom File Processing}\label{custom-file-processing}
+
+In ``normal'' file processing, conversion from the input data elements to the EPW data elements is automatic. In ``custom'' file processing, there is limited flexibility in this regard. For example, the user may use ``wet bulb'' temperature in their inputs - this will allow the weather converter to calculate appropriate values for dew point temperature (if it is missing) and/or relative humidity. Again, limited calculations/derivations are done - should one input wet bulb temperature along with dew point temperature and relative humidity. Likewise, if only values for global horizontal radiation and diffuse horizontal radiation are given, the program will calculate a value for direct normal radiation using commonly recognized relationships between these values.
+
+\subsection{Custom File Processing - Solar Radiation Value Calculation}\label{custom-file-processing---solar-radiation-value-calculation}
+
+EnergyPlus only uses the solar radiation data for Direct Normal and Diffuse Horizontal radation in its calculations. But many data sources have only Global Horizontal (sometimes called Total) or none of the solar radiation elements.
+
+With any two of the solar components, it is reasonable to use the simple relationship of Global, Diffuse and Direct, such as:
+
+\begin{equation}
+Global_{horizontalradiation} = Direct_{horizontalradiation}+Diffuse_{horizontalradiation}
+\end{equation}
+
+Using known solar position (calculated internally by the Weather converter from latitude, longitude, date and hour), one has:
+
+\begin{equation}
+Direct_{normalradiation} = \frac{Direct_{horizontalradiation}}{\sin(Solar_{height}}
+\end{equation}
+
+Thus, having two of the solar radiation components makes it relatively simple to derive the third.
+
+However, many data sources may not have any solar radiation components. A study was undertaken to find an appropriate solar model to fill in missing solar data for weather files. The goal was to determine one or more possible solar models to use in the weather conversion/creation process. One model seemed better overall with the usual given data from the sources than others. The model, termed Zhang-Huang, has been used in a variety of locations and data creations, including the upcoming IWEC2 data. The model uses a simplistic approach of recent drybulb temperatures, sky cover, global solar constant and solar position. This model is only used when all solar values are missing from the incoming data. When global radiation is available, then a different model (Perez split) is used to split the global into direct normal and diffuse horizontal values.
+
+Results, of course, can vary depending on locations.
+
+For example, in Brisbane AUS, comparing the solar creation with the original IWEC data looks very good:
+
+\begin{figure}[hbtp] % fig 10
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image006.jpg}
+\caption{Solar radiation comparison - IWEC vs Weather Solar Model (Brisbane AUS) \protect \label{fig:solar-radiation-comparison-iwec-vs-weather}}
+\end{figure}
+
+Of course, there are other locations that don't compare quite as well:
+
+\begin{figure}[hbtp] % fig 11
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image007.jpg}
+\caption{Comparison of IWEC vs Weather program Solar Model (Singapore) \protect \label{fig:comparison-of-iwec-vs-weather-program-solar}}
+\end{figure}
diff --git a/doc/auxiliary-programs/src/weather-converter-program/energyplus-weather-file-epw-data-dictionary.tex b/doc/auxiliary-programs/src/weather-converter-program/energyplus-weather-file-epw-data-dictionary.tex
new file mode 100644
index 00000000000..8dfad5a81a3
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/energyplus-weather-file-epw-data-dictionary.tex
@@ -0,0 +1,681 @@
+\section{EnergyPlus Weather File (EPW) Data Dictionary}\label{energyplus-weather-file-epw-data-dictionary}
+
+The ``data dictionary'' for EnergyPlus Weather Data is shown below. Note that semi-colons do NOT terminate lines in the EnergyPlus Weather Data. It helps if you have familiarity with the IDD conventions please view them in the Input Output Reference document. Briefly, we have similar ``\textbackslash{}'' conventions that are important for reading the following tables:
+
+\textbackslash{}minimum, \textbackslash{}minimum\textgreater{} - values for this field must be either \textgreater{} = or \textgreater{} than the following number
+
+\textbackslash{}maximum, \textbackslash{}maximum\textless{} - values for this field must be either \textless{} = or \textless{} than the following number
+
+\textbackslash{}missing - if values in this field are \textgreater{} = the following number, it is considered ``missing'' and missing data rules will apply
+
+\textbackslash{}default - blank fields will receive the following as ``default'' values
+
+\textbackslash{}units - expected units for the field. Standard EnergyPlus units are shown in the Input Output Reference Document.
+
+Note that in the header records where ``date'' is used, the interpretation is shown in the following table.
+
+% table 14
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Weather File Date Field Interpretation \label{table:weather-file-date-field-interpretation}} \tabularnewline
+\toprule 
+Field Contents & Interpretation & Header Applicability \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Weather File Date Field Interpretation} \tabularnewline
+\toprule 
+Field Contents & Interpretation & Header Applicability \tabularnewline
+\midrule
+\endhead
+
+< number > & Julian Day of Year & All date fields \tabularnewline
+< number >  /  < number > & Month / Day & All date fields \tabularnewline
+< number >  /  < number >  /  < number > & Month / Day / Year & DataPeriod only - special multiple year file - ref: RunPeriod:CustomRange object in IDF / Input Output Reference document \tabularnewline
+< number >  Month & Day and Month & All date fields \tabularnewline
+Month  < number > & Day and Month & All date fields \tabularnewline
+< number >  Weekday in Month & Numbered weekday of month & Holiday, DaylightSavingPeriod \tabularnewline
+Last Weekday In Month & Last weekday of month & Holiday, DaylightSavingPeriod \tabularnewline
+\bottomrule
+\end{longtable}
+
+In the table, Month can be one of (January, February, March, April, May, June, July, August, September, October, November, December). Abbreviations of the first three characters are also valid.
+
+In the table, Weekday can be one of (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday). Abbreviations of the first three characters are also valid.
+
+\begin{lstlisting}
+!ESP(r)/EnergyPlus Weather Format
+!April 2002
+\memo Dates in the EPW file can be several formats:
+\memo <number>/<number>  (month/day)
+\memo <number> Month
+\memo Month <number>
+\memo <number> (taken to be Julian day of year)
+\memo Months are January, February, March, April, May,
+\memo            June, July, August, September, October, November, December
+\memo Months can be the first 3 letters of the month
+\end{lstlisting}
+
+\begin{lstlisting}
+LOCATION,
+   A1, \field city
+   \type alpha
+   A2, \field State Province Region
+   \type alpha
+   A3, \field Country
+   \type alpha
+   A4, \field Source
+   \type alpha
+   N1, \field WMO
+    \note usually a 6 digit field. Used as alpha in EnergyPlus
+    \type alpha
+   N2 , \field Latitude
+       \units deg
+       \minimum -90.0
+       \maximum +90.0
+       \default 0.0
+       \note + is North, - is South, degree minutes represented in decimal (i.e. 30 minutes is .5)
+       \type real
+   N3 , \field Longitude
+       \units deg
+       \minimum -180.0
+       \maximum +180.0
+       \default 0.0
+       \note - is West, + is East, degree minutes represented in decimal (i.e. 30 minutes is .5)
+       \type real
+   N4 , \field TimeZone
+       \units hr - not on standard units list???
+       \minimum -12.0
+       \maximum +12.0
+       \default 0.0
+       \note  Time relative to GMT.
+       \type real
+   N5 ; \field Elevation
+       \units m
+       \minimum -1000.0
+       \maximum< +9999.9
+       \default 0.0
+       \type real
+\end{lstlisting}
+
+The Location header record duplicates the information required for the Location Object. When only a Run Period object is used (i.e.~a weather file), then the Location Object Is not needed. When a Run Period and Design Day objects are entered, then the Location on the weather file (as described previously) is used and overrides any Location Object entry.
+
+\begin{lstlisting}
+DESIGN CONDITIONS,
+     N1, \field Number of Design Conditions
+     A1, \field Design Condition Source
+         \note current sources are ASHRAE HOF 2009 US Design Conditions, Canadian Design Conditions
+         \note and World Design Conditions
+     A2, \field Design Condition Type (HEATING)
+       \note fields here will be dependent on the source, they are shown in a header/data format 
+       \note in both the .rpt and .csv files that are produced by the WeatherConverter program
+     ...
+     An, \field Design Condition Type (COOLING)
+       \note same as note on Heating Design Conditions
+\end{lstlisting}
+
+The Design Conditions header record encapsulates matching (using WMO\# -- World Meteorological Organization Station Number) design conditions for a weather file location. Currently only those design conditions contained in the ASHRAE Handbook of Fundamentals 2009 are contained in the weather files. These conditions can be used as desired. In addition, Design Day definition files have been created of all World, Canada, and United States Design Conditions. These files are available in the DataSet folder of the EnergyPlus installation.
+
+\begin{lstlisting}
+TYPICAL/EXTREME PERIODS,
+     N1, \field Number of Typical/Extreme Periods
+     A1, \field Typical/Extreme Period 1 Name
+     A2, \field Typical/Extreme Period 1 Type
+     A3, \field Period 1 Start Day
+     A4, \field Period 1 End Day
+     \note repeat (A1-A3) until number of typical periods
+ -- etc to # of periods entered
+\end{lstlisting}
+
+Using a heuristic method, the weather converter can determine typical and extreme weather periods for full year weather files. These will then be shown on the Typical/Extreme Periods header record. These are also reported in the statistical report output from the Weather Converter.
+
+\begin{lstlisting}
+GROUND TEMPERATURES,
+       N1, Number of Ground Temperature Depths
+       N2, \field Ground Temperature Depth 1
+         \units m
+       N3, \field Depth 1 Soil Conductivity
+         \units W/m-K,
+       N4, \field Depth 1 Soil Density
+         \units kg/m3
+       N5, \field Depth 1 Soil Specific Heat
+         \units J/kg-K,
+       N6, \field Depth 1 January Average Ground Temperature
+        \units C
+       N7, \field Depth 1 February Average Ground Temperature
+        \units C
+       N8, \field Depth 1 March Average Ground Temperature
+        \units C
+       N9, \field Depth 1 April Average Ground Temperature
+        \units C
+       N10, \field Depth 1 May Average Ground Temperature
+        \units C
+       N11, \field Depth 1 June Average Ground Temperature
+        \units C
+       N12, \field Depth 1 July Average Ground Temperature
+        \units C
+       N13, \field Depth 1 August Average Ground Temperature
+        \units C
+       N14, \field Depth 1 September Average Ground Temperature
+        \units C
+       N15, \field Depth 1 October Average Ground Temperature
+        \units C
+       N16, \field Depth 1 November Average Ground Temperature
+        \units C
+       N17, \field Depth 1 December Average Ground Temperature
+        \units C
+      \note repeat above (N2-N17) to number of ground temp depths indicated
+-- etc to # of depths entered
+\end{lstlisting}
+
+The weather converter program can use a full year weather data file to calculate ``undisturbed'' ground temperatures based on temperatures. Since an important part of soil heat transfer includes soil properties such as conductivity, density and specific heat AND these cannot be calculated from simple weather observations, this header record is provided primarilyfor user information. However, with the FC construction option, these are automatically selected (.5 depth) for use if the user does not include values in the Site:GroundTemperature:FcfactorMethod object.
+
+As noted in the statistics report, the ``undisturbed'' ground temperatures calculated by the weather converter should not be used in building losses but are appropriate to be used in the GroundTemperatures:Surface and GroundTemperatures:Deep objects. The reasoning (for building losses) is that these values are too extreme for the soil under a conditioned building. For best results, use the Slab or Basement program described in this document to calculate custom monthly average ground temperatures (see the Ground Heat Transfer section). This is especially important for residential applications and very small buildings. If one of these ground temperature preprocessors is not used, for typical commercial buildings in the USA, a reasonable default value is 2C less than the average indoor space temperature.
+
+\begin{lstlisting}
+HOLIDAYS/DAYLIGHT SAVING,
+     A1, \field LeapYear Observed
+      \type choice
+      \key Yes
+      \key No
+      \note Yes if Leap Year will be observed for this file
+      \note No if Leap Year days (29 Feb) should be ignored in this file
+     A2, \field Daylight Saving Start Day
+     A3, \field Daylight Saving End Day
+     N1, \field Number of Holidays (essentially unlimited)
+     A4, \field Holiday 1 Name
+     A5, \field Holiday 1 Day
+     \note repeat above two fields until Number of Holidays is reached
+-- etc to # of Holidays entered
+\end{lstlisting}
+
+The Holidays / Daylight Saving header record details the start and end dates of Daylight Saving Time and other special days such as might be recorded for the weather file. These can be used by keying ``Yes'' for appropriate fields in the Run Period Object.
+
+Note: EnergyPlus processed weather files available on the EnergyPlus web site: have neither special days specified nor daylight saving period.
+
+For example, using a RunPeriod:
+
+\begin{lstlisting}
+
+RunPeriod,
+  1,                       !- Begin Month
+  1,                       !- Begin Day Of Month
+  12,                      !- End Month
+  31,                      !- End Day Of Month
+  Wednesday,               !- Day Of Week For Start Day
+  Yes,                     !- Use WeatherFile Holidays/Special Days
+  No,                      !- Use WeatherFile DaylightSavingPeriod
+  Yes,                     !- Apply Weekend Holiday Rule
+  Yes,                     !- Use WeatherFile Rain Indicators
+  Yes;                     !- Use WeatherFile Snow Indicators
+\end{lstlisting}
+
+Will use any holidays specified in the Holidays / Daylight Saving header record of the weather file but will not use the Daylight Saving Period that is specified there (if any). In addition, the user can specify Special Day Periods via the Special Day Period object and/or Daylight Saving Period via the Daylight Saving Period object to additionally specify these items.
+
+\begin{lstlisting}
+COMMENTS 1, A1 \field Comments_1
+COMMENTS 2, A1 \field Comments_2
+\end{lstlisting}
+
+The Comment header records may provide additional information about the weather data source or other information which may not fit in other header record formats.
+
+\begin{lstlisting}
+DATA PERIODS,
+     N1, \field Number of Data Periods
+     N2, \field Number of Records per hour
+     A1, \field Data Period 1 Name/Description
+     A2, \field Data Period 1 Start Day of Week
+       \type choice
+       \key  Sunday
+       \key  Monday
+       \key  Tuesday
+       \key  Wednesday
+       \key  Thursday
+       \key  Friday
+       \key  Saturday
+     A3, \field Data Period 1 Start Day
+     A4, \field Data Period 1 End Day
+     \note repeat above to number of data periods
+-- etc to # of periods entered
+\end{lstlisting}
+
+A weather file may contain several ``data periods'' though this is not required (and, in fact, may be detrimental). In addition, a weather file may contain multiple records per hour BUT these must match the Number of Time Steps In Hour for the simulation. Multiple interval data files can be valued when you want to be sure of the weather values for each time step (rather than relying on ``interpolated'' weather data). A weather file may also contain several consecutive years of weather data. EnergyPlus will automatically process the extra years when the Number of Years field is used in the RunPeriod object. Sorry - there is no way to jump into a year in the middle of the EPW file.
+
+Note that a Run Period object may not cross Data Period boundary lines.
+
+For those interested in creating their own weather data in the CSV or EPW formats or reading the .csv and .epw files that are produced by the Weather Converter program, the fields are shown in the following ``IDD'' description. Items shown in bold are used directly in the EnergyPlus program.
+
+\begin{lstlisting}
+! Actual data does not have a descriptor
+     N1, \field Year
+     N2, \field Month
+     N3, \field Day
+     N4, \field Hour
+     N5, \field Minute
+     A1, \field Data Source and Uncertainty Flags
+     \note Initial day of weather file is checked by EnergyPlus for validity (as shown below)
+     \note Each field is checked for "missing" as shown below. Reasonable values, calculated
+     \note values or the last "good" value is substituted.
+     N6, \field Dry Bulb Temperature
+        \units C
+        \minimum> -70
+        \maximum< 70
+        \missing 99.9
+     N7, \field Dew Point Temperature
+        \units C
+        \minimum> -70
+        \maximum< 70
+        \missing 99.9
+     N8, \field Relative Humidity
+         \missing 999.
+         \minimum 0
+         \maximum 110
+     N9, \field Atmospheric Station Pressure
+        \units Pa
+        \missing 999999.
+        \minimum> 31000
+        \maximum< 120000
+     N10, \field Extraterrestrial Horizontal Radiation
+        \units Wh/m2
+        \missing 9999.
+        \minimum 0
+     N11, \field Extraterrestrial Direct Normal Radiation
+        \units Wh/m2
+        \missing 9999.
+        \minimum 0
+     N12, \field Horizontal Infrared Radiation Intensity
+        \units Wh/m2
+        \missing 9999.
+        \minimum 0
+     N13, \field Global Horizontal Radiation
+        \units Wh/m2
+        \missing 9999.
+        \minimum 0
+     N14, \field Direct Normal Radiation
+        \units Wh/m2
+        \missing 9999.
+        \minimum 0
+     N15, \field Diffuse Horizontal Radiation
+        \units Wh/m2
+        \missing 9999.
+        \minimum 0
+     N16, \field Global Horizontal Illuminance
+        \units lux
+        \missing 999999.
+        \note will be missing if > = 999900
+        \minimum 0
+     N17, \field Direct Normal Illuminance
+        \units lux
+        \missing 999999.
+        \note will be missing if > = 999900
+        \minimum 0
+     N18, \field Diffuse Horizontal Illuminance
+        \units lux
+        \missing 999999.
+        \note will be missing if > = 999900
+        \minimum 0
+     N19, \field Zenith Luminance
+        \units Cd/m2
+        \missing 9999.
+        \note will be missing if > = 9999
+        \minimum 0
+     N20, \field Wind Direction
+        \units degrees
+        \missing 999.
+        \minimum 0
+        \maximum 360
+     N21, \field Wind Speed
+        \units m/s
+        \missing 999.
+        \minimum 0
+        \maximum 40
+     N22, \field Total Sky Cover
+        \missing 99
+        \minimum 0
+        \maximum 10
+     N23, \field Opaque Sky Cover (used if Horizontal IR Intensity missing)
+        \missing 99
+        \minimum 0
+        \maximum 10
+     N24, \field Visibility
+        \units km
+        \missing 9999
+     N25, \field Ceiling Height
+        \units m
+        \missing 99999
+     N26, \field Present Weather Observation
+     N27, \field Present Weather Codes
+     N28, \field Precipitable Water
+        \units mm
+        \missing 999
+     N29, \field Aerosol Optical Depth
+        \units thousandths
+        \missing .999
+     N30, \field Snow Depth
+        \units cm
+        \missing 999
+     N31, \field Days Since Last Snowfall
+        \missing 99
+     N32, \field Albedo
+        \missing 999
+     N33, \field Liquid Precipitation Depth
+          \units mm
+        \missing 999
+     N34; \field Liquid Precipitation Quantity
+          \units hr
+        \missing 99
+\end{lstlisting}
+
+\subsection{Data Field Descriptions}\label{data-field-descriptions}
+
+Descriptions of the fields are taken from the IWEC manual - as descriptive of what should be contained in the data fields.
+
+\subsubsection{Field: Year}\label{field-year}
+
+This is the Year of the data. Not really used in EnergyPlus. Used in the Weather Converter program for display in audit file.
+
+\subsubsection{Field: Month}\label{field-month}
+
+This is the month (1-12) for the data. Cannot be missing.
+
+\subsubsection{Field: Day}\label{field-day}
+
+This is the day (dependent on month) for the data. Cannot be missing.
+
+\subsubsection{Field: Hour}\label{field-hour}
+
+This is the hour of the data. (1 - 24). Hour 1 is 00:01 to 01:00. Cannot be missing.
+
+\subsubsection{Field: Minute}\label{field-minute}
+
+This is the minute field. (1..60)
+
+\subsubsection{Field: Data Source and Uncertainty Flags}\label{field-data-source-and-uncertainty-flags}
+
+The data source and uncertainty flags from various formats (usually shown with each field) are consolidated in the E/E+ EPW format. More is shown about Data Source and Uncertainty in Data Sources/Uncertainty section later in this document.
+
+\subsubsection{Field: Dry Bulb Temperature}\label{field-dry-bulb-temperature}
+
+This is the dry bulb temperature in C at the time indicated. Note that this is a full numeric field (i.e.~23.6) and not an integer representation with tenths. Valid values range from -70°C to 70°C. Missing value for this field is 99.9.
+
+\subsubsection{Field: Dew Point Temperature}\label{field-dew-point-temperature}
+
+This is the dew point temperature in C at the time indicated. Note that this is a full numeric field (i.e.~23.6) and not an integer representation with tenths. Valid values range from -70°C to 70°C. Missing value for this field is 99.9.
+
+\subsubsection{Field: Relative Humidity}\label{field-relative-humidity}
+
+This is the Relative Humidity in percent at the time indicated. Valid values range from 0\% to 110\%. Missing value for this field is 999.
+
+\subsubsection{Field: Atmospheric Station Pressure}\label{field-atmospheric-station-pressure}
+
+This is the station pressure in Pa at the time indicated. Valid values range from 31,000 to 120,000. (These values were chosen from the standard barometric pressure for all elevations of the World). Missing value for this field is 999999.
+
+\subsubsection{Field: Extraterrestrial Horizontal Radiation}\label{field-extraterrestrial-horizontal-radiation}
+
+This is the Extraterrestrial Horizontal Radiation in Wh/m2. It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 9999.
+
+\subsubsection{Field: Extraterrestrial Direct Normal Radiation}\label{field-extraterrestrial-direct-normal-radiation}
+
+This is the Extraterrestrial Direct Normal Radiation in Wh/m2. (Amount of solar radiation in Wh/m2 received on a surface normal to the rays of the sun at the top of the atmosphere during the number of minutes preceding the time indicated). It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 9999.
+
+\subsubsection{Field: Horizontal Infrared Radiation Intensity}\label{field-horizontal-infrared-radiation-intensity}
+
+This is the Horizontal Infrared Radiation Intensity in Wh/m2. If it is missing, it is calculated from the Opaque Sky Cover field as shown in the following explanation. It should have a minimum value of 0; missing value for this field is 9999.
+
+\begin{equation}
+Horizontal_{IR} = \epsilon\sigma T^4_{drybulb}
+\end{equation}
+
+where
+
+\begin{itemize}
+\tightlist
+\item
+  \(Horizontal_{IR}\) is the horizontal IR intensity \{W/m\(^{2}\)\}
+\item
+  \(\epsilon\) is the sky emissivity
+\item
+  \(\sigma\) is the Stefan-Boltzmann constant = 5.6697e-8 W/m\(^{2}\)-K\(^{4}\)
+\item
+  \(T_{drybulb}\) is the drybulb temperature \{K\}
+\end{itemize}
+
+The sky emissivity is given by
+
+\begin{equation}
+\epsilon = \left( 0.787 +0.764 \ln\left(\frac{T_{dewpoint}}{273}\right)\right)\left( 1 + 0.0224N + 0.0035N^2 + 0.00028N^3 \right)
+\end{equation}
+
+where
+
+\begin{itemize}
+\tightlist
+\item
+  \(T_{dewpoint}\) is the dewpoint temperature \{K\}
+\item
+  \(N\) is the opaque sky cover \{tenths\}
+\end{itemize}
+
+Example: Clear sky (\(N = 0\) ), \(T_{drybulb} = 273+20 = 293 K\) , \(T_{dewpoint} = 273+10 = 283 K\) :
+
+\(\epsilon = 0.787 + 0.764*0.036 = 0.815\)
+
+\(Horizontal_{IR} = 0.815*5.6697e-8*(293^4) = 340.6 W/m^2\)
+
+References (Walton, 1983) (Clark, Allen, 1978) for these calculations are contained in the references section at the end of this list of fields.
+
+\subsubsection{Field: Global Horizontal Radiation}\label{field-global-horizontal-radiation}
+
+This is the Global Horizontal Radiation in Wh/m2. (Total amount of direct and diffuse solar radiation in Wh/m2 received on a horizontal surface during the number of minutes preceding the time indicated.) It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 9999.
+
+\subsubsection{Field: Direct Normal Radiation}\label{field-direct-normal-radiation}
+
+This is the Direct Normal Radiation in Wh/m2. (Amount of solar radiation in Wh/m2 received directly from the solar disk on a surface perpendicular to the sun's rays, during the number of minutes preceding the time indicated.) If the field is missing (\(\ge 9999\) ) or invalid (\(<0\) ), it is set to 0. Counts of such missing values are totaled and presented at the end of the runperiod.
+
+\subsubsection{Field: Diffuse Horizontal Radiation}\label{field-diffuse-horizontal-radiation}
+
+This is the Diffuse Horizontal Radiation in Wh/m2. (Amount of solar radiation in Wh/m2 received from the sky (excluding the solar disk) on a horizontal surface during the number of minutes preceding the time indicated.) If the field is missing (\(\ge 9999\) ) or invalid (\(<0\) ), it is set to 0. Counts of such missing values are totaled and presented at the end of the runperiod.
+
+\subsubsection{Field: Global Horizontal Illuminance}\label{field-global-horizontal-illuminance}
+
+This is the Global Horizontal Illuminance in lux. (Average total amount of direct and diffuse illuminance in hundreds of lux received on a horizontal surface during the number of minutes preceding the time indicated.) It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 999999 and will be considered missing if greater than or equal to 999900.
+
+\subsubsection{Field: Direct Normal Illuminance}\label{field-direct-normal-illuminance}
+
+This is the Direct Normal Illuminance in lux. (Average amount of illuminance in hundreds of lux received directly from the solar disk on a surface perpendicular to the sun's rays, during the number of minutes preceding the time indicated.) It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 999999 and will be considered missing if greater than or equal to 999900.
+
+\subsubsection{Field: Diffuse Horizontal Illuminance}\label{field-diffuse-horizontal-illuminance}
+
+This is the Diffuse Horizontal Illuminance in lux. (Average amount of illuminance in hundreds of lux received from the sky (excluding the solar disk) on a horizontal surface during the number of minutes preceding the time indicated.) It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 999999 and will be considered missing if greater than or equal to 999900.
+
+\subsubsection{Field: Zenith Luminance}\label{field-zenith-luminance}
+
+This is the Zenith Illuminance in Cd/m2. (Average amount of luminance at the sky's zenith in tens of Cd/m2 during the number of minutes preceding the time indicated.) It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 9999.
+
+\subsubsection{Field: Wind Direction}\label{field-wind-direction}
+
+This is the Wind Direction in degrees where the convention is that North = 0.0, East = 90.0, South = 180.0, West = 270.0. (Wind direction in degrees at the time indicated. If calm, direction equals zero.) Values can range from 0 to 360. Missing value is 999.
+
+\subsubsection{Field: Wind Speed}\label{field-wind-speed}
+
+This is the wind speed in m/sec. (Wind speed at time indicated.) Values can range from 0 to 40. Missing value is 999.
+
+\subsubsection{Field: Total Sky Cover}\label{field-total-sky-cover}
+
+This is the value for total sky cover (tenths of coverage). (i.e.~1 is 1/10 covered. 10 is total coverage). (Amount of sky dome in tenths covered by clouds or obscuring phenomena at the hour indicated at the time indicated.) Minimum value is 0; maximum value is 10; missing value is 99.
+
+\subsubsection{Field: Opaque Sky Cover}\label{field-opaque-sky-cover}
+
+This is the value for opaque sky cover (tenths of coverage). (i.e.~1 is 1/10 covered. 10 is total coverage). (Amount of sky dome in tenths covered by clouds or obscuring phenomena that prevent observing the sky or higher cloud layers at the time indicated.) This is not used unless the field for Horizontal Infrared Radiation Intensity is missing and then it is used to calculate Horizontal Infrared Radiation Intensity. Minimum value is 0; maximum value is 10; missing value is 99.
+
+\subsubsection{Field: Visibility}\label{field-visibility}
+
+This is the value for visibility in km. (Horizontal visibility at the time indicated.) It is not currently used in EnergyPlus calculations. Missing value is 9999.
+
+\subsubsection{Field: Ceiling Height}\label{field-ceiling-height}
+
+This is the value for ceiling height in m. (77777 is unlimited ceiling height. 88888 is cirroform ceiling.) It is not currently used in EnergyPlus calculations. Missing value is 99999.
+
+\subsubsection{Field: Present Weather Observation}\label{field-present-weather-observation}
+
+If the value of the field is 0, then the observed weather codes are taken from the following field. If the value of the field is 9, then ``missing'' weather is assumed. Since the primary use of these fields (Present Weather Observation and Present Weather Codes) is for rain/wet surfaces, a missing observation field or a missing weather code implies no rain.
+
+% table 15
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{3.0in}}
+\caption{Present Weather Observation Values \label{table:present-weather-observation-values}} \tabularnewline
+\toprule 
+Element & Values & Definition \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Present Weather Observation Values} \tabularnewline
+\toprule 
+Element & Values & Definition \tabularnewline
+\midrule
+\endhead
+
+Observation Indicator & 0 or 9 & 0 = Weather observation made; 9 = Weather observation not made, or missing \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Field: Present Weather Codes}\label{field-present-weather-codes}
+
+The present weather codes field is assumed to follow the TMY2 conventions for this field. Note that though this field may be represented as numeric (e.g.~in the CSV format), it is really a text field of 9 single digits. This convention along with values for each ``column'' (left to right) is presented in Table~\ref{table:weather-codes-field-interpretation}. Note that some formats (e.g.~TMY) does not follow this convention - as much as possible, the present weather codes are converted to this convention during WeatherConverter processing. Also note that the most important fields are those representing liquid precipitation - where the surfaces of the building would be wet. EnergyPlus uses ``Snow Depth'' to determine if snow is on the ground.
+
+% table 16
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Weather Codes Field Interpretation \label{table:weather-codes-field-interpretation}} \tabularnewline
+\toprule 
+Column - Poisition in Field & Element Description & Possible Values & Definition \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Weather Codes Field Interpretation} \tabularnewline
+\toprule 
+Column - Poisition in Field & Element Description & Possible Values & Definition \tabularnewline
+\midrule
+\endhead
+
+1 & Occurrence ofThunderstorm,Tornado, orSquall & 0 - 2, 4, 6- 9 & 0 = Thunderstorm-lightning and thunder. Wind gusts less than 25.7 m/s, and hail, if any, less than 1.9 cm diameter   
+    1 = Heavy or severe thunderstorm-frequent intense lightning and thunder. Wind gusts greater than 25.7 m/s and hail, if any, 1.9 cm or greater diameter   
+    2 = Report of tornado or waterspout   
+    4 = Moderate squall-sudden increase of windspeed by at least 8.2 m/s, reaching 11.3 m/s or more and lasting for at least 1 minute   
+    6 = Water spout (beginning January 1984)   
+    7 = Funnel cloud (beginning January 1984)   
+    8 = Tornado (beginning January 1984)   
+    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9 \tabularnewline
+2 & Occurrence ofRain, RainShowers, orFreezing Rain & 0 - 9 & 0 = Light rain   
+    1 = Moderate rain   
+    2 = Heavy rain   
+    3 = Light rain showers   
+    4 = Moderate rain showers   
+    5 = Heavy rain showers   
+    6 = Light freezing rain   
+    7 = Moderate freezing rain   
+    8 = Heavy freezing rain   
+    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9    
+    Notes:   
+    Light = up to 0.25 cm per hour    
+    Moderate = 0.28to 0.76 cm per hour    
+    Heavy = greater than 0.76cm per hour \tabularnewline
+3 & Occurrence ofRain Squalls,Drizzle, orFreezing Drizzle & 0, 1, 3-9 & 0 = Light rain squalls   
+    1 = Moderate rain squalls   
+    3 = Light drizzle   
+    4 = Moderate drizzle   
+    5 = Heavy drizzle   
+    6 = Light freezing drizzle   
+    7 = Moderate freezing drizzle   
+    8 = Heavy freezing drizzle   
+    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9   
+    Notes: When drizzle or freezing drizzle occurswith other weather phenomena: Light = up to0.025 cm per hour Moderate = 0.025 to 0.051cm per hour Heavy = greater than 0.051 cmper hour When drizzle or freezing drizzle occurs alone:    
+    Light = visibility 1 km or greater    
+    Moderate = visibility between 0.5 and 1 km    
+    Heavy = visibility 0.5 km or less \tabularnewline
+4 & Occurrence ofSnow, SnowPellets, or IceCrystals & 0 - 9 & 0 = Light snow   
+    1 = Moderate snow   
+    2 = Heavy snow   
+    3 = Light snow pellets   
+    4 = Moderate snow pellets   
+    5 = Heavy snow pellets   
+    6 = Light ice crystals   
+    7 = Moderate ice crystals   
+    8 = Heavy ice crystals   
+    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9    
+    Notes:Beginning in April 1963, any occurrence of icecrystals is recorded as a 7. \tabularnewline
+5 & Occurrence ofSnow Showers,Snow Squalls, orSnow Grains & 0 - 7, 9 & 0 = Light snow   
+    1 = Moderate snow showers   
+    2 = Heavy snow showers   
+    3 = Light snow squall   
+    4 = Moderate snow squall   
+    5 = Heavy snow squall   
+    6 = Light snow grains   
+    7 = Moderate snow grains   
+    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9 \tabularnewline
+6 & Occurrence ofSleet, SleetShowers, or Hail & 0 - 2, 4, 9 & 0 = Light ice pellet showers   
+    1 = Moderate ice pellet showers   
+    2 = Heavy ice pellet showers   
+    4 = Hail   
+    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9   
+    Notes: Prior to April 1970, ice pellets werecoded as sleet. Beginning in April 1970, sleetand small hail were redefined as ice pellets andare coded as 0, 1, or 2. \tabularnewline
+7 & Occurrence ofFog, BlowingDust, or Blowing Sand & 0 - 9 & 0 = Fog   
+    1 = Ice fog   
+    2 = Ground fog   
+    3 = Blowing dust   
+    4 = Blowing sand   
+    5 = Heavy fog   
+    6 = Glaze (beginning 1984)   
+    7 = Heavy ice fog (beginning 1984)   
+    8 = Heavy ground fog (beginning 1984)   
+    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9   
+    Notes:These values recorded only when visibility isless than 11 km. \tabularnewline
+8 & Occurrence ofSmoke, Haze,Smoke andHaze, BlowingSnow, BlowingSpray, or Dust & 0 - 7, 9 & 0 = Smoke   
+    1 = Haze   
+    2 = Smoke and haze   
+    3 = Dust   
+    4 = Blowing snow   
+    5 = Blowing spray   
+    6 = Dust storm (beginning 1984)   
+    7 = Volcanic ash   
+    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9   
+    Notes: These values recorded only when visibility is less than 11 km. \tabularnewline
+9 & Occurrence ofIce Pellets & 0 - 2, 9 & 0 = Light ice pellets   
+    1 = Moderate ice pellets   
+    2 = Heavy ice pellets   
+    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9 \tabularnewline
+\bottomrule
+\end{longtable}
+
+For example, a Present Weather Observation (previous field) of 0 and a Present Weather Codes field of 929999999 notes that there is heavy rain for this data period (usually hourly but depends on the number of intervals per hour field in the ``Data Periods'' record).
+
+\subsubsection{Field: Precipitable Water}\label{field-precipitable-water}
+
+This is the value for Precipitable Water in mm. (This is not rain - rain is inferred from the PresWeathObs field but a better result is from the Liquid Precipitation Depth field)). It is not currently used in EnergyPlus calculations (primarily due to the unreliability of the reporting of this value). Missing value is 999.
+
+\subsubsection{Field: Aerosol Optical Depth}\label{field-aerosol-optical-depth}
+
+This is the value for Aerosol Optical Depth in thousandths. It is not currently used in EnergyPlus calculations. Missing value is .999.
+
+\subsubsection{Field: Snow Depth}\label{field-snow-depth}
+
+This is the value for Snow Depth in cm. This field is used to tell when snow is on the ground and, thus, the ground reflectance may change. Missing value is 999.
+
+\subsubsection{Field: Days Since Last Snowfall}\label{field-days-since-last-snowfall}
+
+This is the value for Days Since Last Snowfall. It is not currently used in EnergyPlus calculations. Missing value is 99.
+
+\subsubsection{Field: Albedo}\label{field-albedo}
+
+The ratio (unitless) of reflected solar irradiance to global horizontal irradiance. It is not currently used in EnergyPlus.
+
+\subsubsection{Field: Liquid Precipitation Depth}\label{field-liquid-precipitation-depth}
+
+The amount of liquid precipitation (mm) observed at the indicated time for the period indicated in the liquid precipitation quantity field. If this value is not missing, then it is used and overrides the ``precipitation'' flag as rainfall. Conversely, if the precipitation flag shows rain and this field is missing or zero, it is set to 1.5 (mm).
+
+\subsubsection{Field: Liquid Precipitation Quantity}\label{field-liquid-precipitation-quantity}
+
+The period of accumulation (hr) for the liquid precipitation depth field. It is not currently used in EnergyPlus.
+
+\subsection{References}\label{references}
+
+Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards, p.~21.
+
+Clark, G. and C. Allen, ``The Estimation of Atmospheric Radiation for Clear and Cloudy Skies,'' Proceedings 2nd National Passive Solar Conference (AS/ISES), 1978, pp.~675-678.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/epw-csv-format-in-out.tex b/doc/auxiliary-programs/src/weather-converter-program/epw-csv-format-in-out.tex
new file mode 100644
index 00000000000..83a2026bfbb
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/epw-csv-format-in-out.tex
@@ -0,0 +1,109 @@
+\section{EPW CSV Format (In/Out)}\label{epw-csv-format-inout}
+
+EPW CSV Format to the Weather Converter is a special CSV format which echoes the format of the EPW file. For the ``header'' records in the CSV file, they are basically the same as the header records for the EPW file (see above). However, in the CSV file, each header is shown and then the data. Partial year files will not have all of these headers ``filled'' in. Also see Figure~\ref{fig:energyplus-epw-csv-file-spreadsheet-view}. EnergyPlus EPW CSV file (spreadsheet view) and Figure~\ref{fig:energyplus-epw-csv-data-records-spreadsheet}. EnergyPlus EPW CSV Data Records (spreadsheet view) for snapshot pictures of the EnergyPlus EPW CSV file as shown in a spreadsheet.
+
+\subsection{Location Header/Data (CSV)}\label{location-headerdata-csv}
+
+Location Title,Latitude \{N+/S-\},Longitude \{E+/W-\},TimeZone \{+/- GMT\},Elevation \{m\}
+
+LOCATION\_SYDNEY\_\_AUS\_IWEC Data\_947670,-33.95,151.18,10.0,3.0
+
+LOCATION + the city, state/province, country and WMO fields from the EPW file are concatenated to form the ``Location Title''. The latitude, longitude, time zone and elevation fields are numeric.
+
+\subsection{Design Conditions Header/Data (CSV)}\label{design-conditions-headerdata-csv}
+
+If there are design conditions, then the format is as follows:
+
+Number of Design Conditions,Title of Design Condition,Design Stat,HDB 99.6\%,HDB 99\%,X WS 1\%,X WS 2.5\%,X WS 5\%,CM WS .4\%,CM MDB .4\%,CM WS 1\%,CM MDB 1\%,MWS 99.6\%,PWD 99.6\%,MWS .4\%,PWD .4\%,X MnDB Max,X MnDB Min,X StdDB Max,X StdDB Min,Design Stat,CDB .4\%,C MWB .4\%,CDB 1\%,C MWB 1\%,CDB 2\%,C MWB 2\%,E WB .4\%,E MDB .4\%,E WB 1\%,E MDB 1\%,E WB 2\%,E MDB 2\%,DP .4\%,HR .4\%,MDB .4\%,DP 1\%,HR 1\%,MDB 1\%,DP 2\%,HR 2\%,MDB 2\%,DB Range
+
+,,Units,\{°C\},\{°C\},\{m/s\},\{m/s\},\{m/s\},\{m/s\},\{°C\},\{m/s\},\{°C\},\{m/s\},\{Degree\},\{m/s\},\{Degree\},\{°C\},\{°C\},\{°C\},\{°C\},Units,\{°C\},\{°C\},\{°C\},\{°C\},\{°C\},\{°C\},\{°C\},\{°C\},\{°C\},\{°C\},\{°C\},\{°C\},\{°C\},\{g/kg\},\{°C\},\{°C\},\{g/kg\},\{°C\},\{°C\},\{g/kg\},\{°C\},\{°C\}
+
+1,World Climate Design Data 2001 ASHRAE Handbook,HEATING,5.8,6.8,11.3,9.9,8.8,11.1,14.2,9.1,13.4,1.1,320,5.3,300,39.3,3.1,2.9,1.9,COOLING,32.2,20,29.5,19.7,27.9,20.1,23,28,22.3,26.2,21.7,25.3,21.7,16.4,24.8,21.1,15.8,24.3,20.6,15.3,23.9,6.7
+
+However, if there are no design conditions, then the format looks like:
+
+Number of Design Conditions,Title of Design Condition,
+
+0
+
+Theoretically, there can be more than one design condition included.
+
+\subsection{Typical/Extreme Periods Header/Data (CSV)}\label{typicalextreme-periods-headerdata-csv}
+
+The results from the typical / extreme period heuristic calculation are shown.
+
+Number of Typical/Extreme Periods,Period Name,Period Type,Period Start Day,Period End Day,\textless{}repeat to \# periods\textgreater{}
+
+6,Summer - Week Nearest Max Temperature For Period,Extreme,1/ 4,1/10,Summer - Week Nearest Average Temperature For Period,Typical,11/29,12/ 5,Winter - Week Nearest Min Temperature For Period,Extreme,7/ 3,7/ 9,Winter - Week Nearest Average Temperature For Period,Typical,6/ 5,6/11,Autumn - Week Nearest Average Temperature For Period,Typical,3/22,3/28,Spring - Week Nearest Average Temperature For Period,Typical,8/ 1,8/ 7
+
+\subsection{Ground Temperatures Header/Data (CSV)}\label{ground-temperatures-headerdata-csv}
+
+The results from the ground temperature heuristic calculation are shown, typically for 3 depths. Users may also fill in the blank fields (soil conductivity, soil density, soil specific heat) with known values and/or perform their own calculations and depths and supply those. These should be considered ``undisturbed'' ground temperatures - temperatures of soil that have not been disturbed by construction. They are not considered appropriate for calculations of building losses.
+
+The program uses a heuristic, time lagged calculation based on dry bulb temperature and location. References on the topic are found in Kusuda (see references).
+
+Number of Ground Temperature Depths,Ground Temperature Depth \{m\},Soil Conductivity \{W/m-K\},Soil Density \{kg/m3\},Soil Specific Heat \{J/kg-K\},Jan \{C\},Feb\{C\},Mar \{C\},Apr \{C\},May \{C\},Jun \{C\},Jul \{C\},Aug \{C\},Sep \{C\},Oct \{C\},Nov \{C\},Dec \{C\},\textless{}repeat to Number of temperature depths\textgreater{}
+
+3,.5,,,,20.69,22.30,22.69,22.26,19.95,17.43,15.09,13.43,12.99,13.86,15.84,18.29,2,,,,19.18,20.71,21.41,21.40,20.16,18.43,16.58,15.03,14.25,14.45,15.59,17.28,4,,,,18.18,19.38,20.10,20.30,19.82,18.80,17.56,16.35,15.56,15.39,15.89,16.89
+
+\subsection{Holiday/Daylight Saving Header/Data (CSV)}\label{holidaydaylight-saving-headerdata-csv}
+
+If these data are entered, the weather converter will process them. Default weather processing contains no holidays or daylight saving period. Of course, these can also be specified in your input data file for EnergyPlus and do not need to be embedded in the weather file.
+
+Leap Year Observed?,Daylight Saving Start Date,Daylight Saving End Date,Number of Holidays,Holiday Name,Holiday Date,\textless{}repeat for \# Holidays\textgreater{}
+
+No,0,0,0
+
+\subsection{Comment 1 Header/Data (CSV)}\label{comment-1-headerdata-csv}
+
+Some original data files fill the comment 1 header and some do not. Typically, it will display at least a ``station'' number and potentially more information.
+
+Comment Line \#1
+
+``IWEC- WMO\#947670 - South-west Pacific -- Original Source Data (c) 2001 American Society of Heating, Refrigerating and Air-Conditioning Engineers (ASHRAE), Inc., Atlanta, GA, USA. www.ashrae.org All rights reserved as noted in the License Agreement and Additional Conditions. DISCLAIMER OF WARRANTIES: The data is provided `as is' without warranty of any kind, either expressed or implied. The entire risk as to the quality and performance of the data is with you. In no event will ASHRAE or its contractors be liable to you for any damages, including without limitation any lost profits, lost savings, or other incidental or consequential damages arising out of the use or inability to use this data.''
+
+\subsection{Comment 2 Header/Data (CSV)}\label{comment-2-headerdata-csv}
+
+Comment Line \#2
+
+-- Ground temps produced with a standard soil diffusivity of 2.3225760E-03 \{m**2/day\}
+
+\subsection{Data Period Header/Data (CSV)}\label{data-period-headerdata-csv}
+
+Number of Data Periods {[}DP{]},Number of Intervals per Hour,DP Name/Description,DP Start Day of Week,DP Start Day, DP End Day,\textless{}repeat to \# Data Periods\textgreater{}
+
+1,1,Data,Sunday, 1/ 1,12/31
+
+\subsection{Data Records (CSV)}\label{data-records-csv}
+
+The field ``names'' for each item are shown. First, the ``short'' names:
+
+Date,HH:MM,Datasource,DryBulb \{C\},DewPoint \{C\},RelHum \{\%\},Atmos Pressure \{Pa\},ExtHorzRad \{Wh/m2\},ExtDirRad \{Wh/m2\},HorzIRSky \{Wh/m2\},GloHorzRad \{Wh/m2\},DirNormRad \{Wh/m2\},DifHorzRad \{Wh/m2\},GloHorzIllum \{lux\},DirNormIllum \{lux\},DifHorzIllum \{lux\},ZenLum \{Cd/m2\},WindDir \{deg\},WindSpd \{m/s\},TotSkyCvr \{.1\},OpaqSkyCvr \{.1\},Visibility \{km\},Ceiling Hgt \{m\},PresWeathObs,PresWeathCodes,Precip Wtr \{mm\},Aerosol Opt Depth \{.001\},SnowDepth \{cm\},Days Last Snow,Albedo \{.01\},Rain \{mm\},Rain Quantity \{hr\}
+
+Then, the longer names:
+
+Date,HH:MM,Datasource,Dry Bulb Temperature \{C\},Dew Point Temperature \{C\},Relative Humidity \{\%\},Atmospheric Pressure \{Pa\},Extraterrestrial Horizontal Radiation \{Wh/m2\},Extraterrestrial Direct Normal Radiation \{Wh/m2\},Horizontal Infrared Radiation Intensity from Sky \{Wh/m2\},Global Horizontal Radiation \{Wh/m2\},Direct Normal Radiation \{Wh/m2\},Diffuse Horizontal Radiation \{Wh/m2\},Global Horizontal Illuminance \{lux\},Direct Normal Illuminance \{lux\},Diffuse Horizontal Illuminance \{lux\},Zenith Luminance \{Cd/m2\},Wind Direction \{deg\},Wind Speed \{m/s\},Total Sky Cover \{.1\},Opaque Sky Cover \{.1\},Visibility \{km\},Ceiling Height \{m\},Present Weather Observation,Present Weather Codes,Precipitable Water \{mm\},Aerosol Optical Depth \{.001\},Snow Depth \{cm\},Days Since Last Snow,Albedo \{.01\},Liquid Precipitation Depth \{mm\},Liquid Precipitation Quantity \{hr\}
+
+As noted previously, these headers and data are in the identical order to the items in the EPW records. Then the data is shown:
+
+1983/1/1,01:00,C9C9C9C9*0?9?9?9?9?9?9?9*0C8C8C8C8*0*0E8*0*0,26.2,19.2,65,101100,0,1415,412,0,0,0,0,0,0,0,180,6.5,9,7,23.3,77777,9,'999999999,0,0.2300,0,88
+
+The Date and Time fields need a bit of description. The Date field (e.g.~1983/1/1) uses your standard system date for formatting. In the EPW file, these are three separate fields (year, month, and day in this example). The time field combines the hours and minutes into one field (hh:mm). This makes it easier for graphing with spreadsheet programs but a bit harder if you use the CSV format as input.
+
+Each data item field obeys the same ``missing'' and other content rules as shown above in the EnergyPlus Weather File (EPW) Data Dictionary.
+
+\begin{figure}[hbtp] % fig 17
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image015.png}
+\caption{EnergyPlus EPW CSV file (spreadsheet view) \protect \label{fig:energyplus-epw-csv-file-spreadsheet-view}}
+\end{figure}
+
+The figure above shows how the EnergyPlus EPW CSV file (initial header records) looks when opened in a spreadsheet. Each header record is shown in bold with data following the headers..
+
+\begin{figure}[hbtp] % fig 18
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image016.png}
+\caption{EnergyPlus EPW CSV Data Records (spreadsheet view) \protect \label{fig:energyplus-epw-csv-data-records-spreadsheet}}
+\end{figure}
+
+The above figure shows how the data periods header record and the individual data records look when opened in a spread sheet. Again, the headers are shown in bold. Note that there are two header records for the data records - one with short names - one with longer more descriptive names.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/k-ppen-climate-classification.tex b/doc/auxiliary-programs/src/weather-converter-program/k-ppen-climate-classification.tex
new file mode 100644
index 00000000000..5275895de66
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/k-ppen-climate-classification.tex
@@ -0,0 +1,84 @@
+\section{Köppen Climate Classification}\label{kuxf6ppen-climate-classification}
+
+Various attempts have been made to classify the climates of the earth into climatic regions. One notable, yet ancient and misguided example is that of Aristotle's Temperate, Torrid, and Frigid Zones. However, the 20th century classification developed by German climatologist and amateur botanist Wladimir Köppen (1846-1940) continues to be the authoritative map of the world climates in use today.
+
+Introduced in 1928 as a wall map co-authored with student Rudolph Geiger, the Köppen system of classification (map) was updated and modified by Köppen until his death. Since that time, it has been modified by several geographers.
+
+The modified Köppen Climate Classification System is the most widely used system for classifying the world's climates. Its categories are based on the annual and monthly averages of temperature and precipitation. The Köppen system recognizes six major climatic types; each type is designated by a capital letter.
+
+In addition to the major climate types, each category is further sub-divided into sub-categories based on temperature and precipitation. There are only 24 sub-categories possible - making the general schemes quite easy to comprehend.
+
+For example, the U.S. states located along the Gulf of Mexico are designated as ``Cfa.'' The ``C'' represents the ``mild mid-latitude'' category, the second letter ``f'' stands for the German word \emph{feucht} or ``moist,'' and the third letter ``a'' indicates that the average temperature of the warmest month is above 22°C. Thus, ``Cfa'' gives us a good indication of the climate of this region, a mild mid-latitude climate with no dry season and a hot summer.
+
+The Köppen classification code (and some statistics) was adapted (with permission of Peter Schild) from the COMIS weather program code.
+
+% table 13
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Köppen Climate Classification -- Major Groups \label{table:kppen-climate-classification-major-groups}} \tabularnewline
+\toprule 
+Köppen Climate Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Köppen Climate Classification -- Major Groups} \tabularnewline
+\toprule 
+Köppen Climate Type & Description \tabularnewline
+\midrule
+\endhead
+
+A & Tropical Moist Climates: all months have average temperatures above 18 degrees Celsius \tabularnewline
+B & Dry Climates: with deficient precipitation during most of the year \tabularnewline
+C & Moist Mid-latitude Climates with Mild Winters \tabularnewline
+D & Moist Mid-Latitude Climates with Cold Winters \tabularnewline
+E & Polar Climates: with extremely cold winters and summers \tabularnewline
+H & Highland areas: Due to mountainous areas, this classification can encompass any of the previous five. \tabularnewline
+\bottomrule
+\end{longtable}
+
+More details on each of the major categories and sub-categories follow:
+
+\subsection{Tropical Moist Climates (A)}\label{tropical-moist-climates-a}
+
+Tropical moist climates extend northward and southward from the equator to about 15 to 25 degrees of latitude. In these climates all months have average temperatures greater than 18 degrees Celsius. Annual precipitation is greater than 1500 mm. Three minor Köppen climate types exist in the A group and their designation is based on seasonal distribution of rainfall. \textbf{Af} or tropical wet is a tropical the climate where precipitation occurs all year long. Monthly temperature variations in this climate are less than 3 degrees Celsius. Because of intense surface heating and high humidity cumulus and cumulonimbus clouds form early in the afternoons almost every day. Daily highs are about 32 degrees Celsius while night time temperatures average 22 degrees Celsius. \textbf{Am} is a tropical monsoon climate. Annual rainfall is equal to or greater than \textbf{Af}, but falls in the 7 to 9 hottest months. During the dry season very little rainfall occurs. The tropical wet and dry or savanna (\textbf{Aw}) has an extended dry season during winter. Precipitation during the wet season is usually less than 1000 millimeters and only during the summer season.
+
+\subsection{Dry Climates (B)}\label{dry-climates-b}
+
+The most obvious climatic feature of these climates is potential evaporation and transpiration exceeds precipitation. These climates extend from 20 - 35 degrees North and South of the equator and in large continental regions of the mid-latitudes often surrounded by mountains. Minor types of this climate include: \textbf{Bw} - dry arid (desert) is a true desert climate. It covers 12 \% of the earth's land surface and is dominated by xerophytic vegetation. \textbf{Bs} - dry semiarid (steppe) is a grassland climate that covers 14\% of the earth's land surface. It receives more precipitation than the \textbf{Bw} either from the inter-tropical convergence zone or from mid-latitude cyclones.
+
+\subsection{Moist Subtropical Mid-Latitude Climates (C)}\label{moist-subtropical-mid-latitude-climates-c}
+
+This climate generally has warm and humid summers with mild winters. Its extent is from 30 to 50 degrees of latitude mainly on the eastern and western borders of most continents. During the winter the main weather feature is the mid-latitude cyclone. Convective thunderstorms dominate summer months. Three minor types exist: \textbf{Cfa} - humid subtropical; \textbf{Cs} - mediterranean; and \textbf{Cfb} - marine. The humid subtropical climate (\textbf{Cfa}) has hot muggy summers and mainly thunderstorms. Winters are mild and precipitation during this season comes from mid-latitude cyclones. A good example of a \textbf{Cfa} climate is the southeastern USA. \textbf{Cfb}, marine, climates are found on the western coasts of continents. They have a humid climate with short dry summer. Heavy precipitation occurs during the mild winters because of continuous presence of mid-latitude cyclones. Mediterranean climates (\textbf{Cs}) receive rain primarily during winter season from the mid-latitude cyclone. Extreme summer aridity is caused by the sinking air of the subtropical highs and may exist for up to 5 months. Locations in North America are from Portland, Oregon to all of California.
+
+\subsection{Moist Continental Mid-latitude Climates (D)}\label{moist-continental-mid-latitude-climates-d}
+
+Moist continental mid-latitude climates have warm to cool summers and cold winters. The location of these climates is pole ward of the C climates. The warmest month is greater than 10º C, while the coldest month is less than -30º C. Winters are severe with snowstorms, strong winds, bitter cold from Continental Polar or Arctic air masses. Like the C climates there are three minor types: \textbf{Dw} - dry winters; \textbf{Ds} - dry summers; and \textbf{Df} - wet all seasons.
+
+\subsection{Polar Climates (E)}\label{polar-climates-e}
+
+Polar climates have year-round cold temperatures with warmest month less than 10º C. Polar climates are found on the northern coastal areas of North America and Europe, Asia and on the landmasses of Greenland and Antarctica. Two minor climate types exist. \textbf{ET} or polar tundra is a climate where the soil is permanently frozen to depths of hundreds of meters, a condition known as permafrost. Vegetation is dominated by mosses, lichens, dwarf trees and scattered woody shrubs. \textbf{EF} or polar ice caps has a surface that is permanently covered with snow and ice.
+
+\subsection{Highlands Areas (H)}\label{highlands-areas-h}
+
+Highland areas can encompass any of the previously mentioned major categories -- the determining factor is one of altitude (temperature decreases roughly 2º C for every increase of 305 m). This is a complex climate zone. Highland regions roughly correspond to the major categories change in temperature with latitude - with one important exception. Seasons only exist in highlands if they also exist in the nearby lowland regions. For example, although \textbf{A} climates have cooler temperatures at higher elevations, the seasonal changes of \textbf{C}, \textbf{D} and \textbf{E} climates are not present.
+
+The following shows an overview of the world and its Köppen classifications.
+
+\begin{figure}[hbtp] % fig 14
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image010.jpg}
+\caption{World viewed as Köppen Climate Zones \protect \label{fig:world-viewed-as-kppen-climate-zones}}
+\end{figure}
+
+And a more basic view with monthly dry bulb temperature and dew point temperatures for these zones (Northern Hemisphere).
+
+\begin{figure}[hbtp] % fig 15
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image011.png}
+\caption{Monthly Dry Bulb Temperatures in Köppen Climates (Northern Hemisphere) \protect \label{fig:monthly-dry-bulb-temperatures-in-kppen}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 16
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image012.png}
+\caption{Monthly Dew Point in Köppen Climates (Northern Hemisphere) \protect \label{fig:monthly-dew-point-in-kppen-climates-northern}}
+\end{figure}
diff --git a/doc/auxiliary-programs/src/weather-converter-program/missing-weather-file-data.tex b/doc/auxiliary-programs/src/weather-converter-program/missing-weather-file-data.tex
new file mode 100644
index 00000000000..161fe1e83dd
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/missing-weather-file-data.tex
@@ -0,0 +1,38 @@
+\section{Missing Weather File Data}\label{missing-weather-file-data}
+
+The following data contains ``missing'' descriptors; a new concept not introduced previously in our IDD conventions. In this case, it will be processed as though those values are ``missing'' in the weather conversions. This may not always be desirable though the weather processor will fill in ``missing'' value with something ``appropriate''. Eventually, these missing values will be available through the weather processor. Until then, the following are used for initial missing conditions. When a valid value is encountered from weather data, however, it will become the new ``missing'' replacement value:
+
+% table 17
+\begin{longtable}[c]{p{1.83in}p{2.67in}p{1.5in}}
+\caption{Missing weather replacement values \label{table:missing-weather-replacement-values}} \tabularnewline
+\toprule 
+Data item & Supplied Value & Units \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Missing weather replacement values} \tabularnewline
+\toprule 
+Data item & Supplied Value & Units \tabularnewline
+\midrule
+\endhead
+
+Dry Bulb Temperature & 6 & C \tabularnewline
+Dew Point Temperature & 3 & C \tabularnewline
+Relative Humidity & 50 & \% \tabularnewline
+Atmospheric Pressure & Standard** Barometric Pressure (altitude based) & Pa \tabularnewline
+Wind Speed & 2.5 & m/s \tabularnewline
+Wind Direction & 180 & Deg \tabularnewline
+Total Sky Cover & 5 & (tenths) \tabularnewline
+Opaque Sky Cover & 5 & (tenths) \tabularnewline
+Visibility & 777.7 & Km \tabularnewline
+Ceiling Height & 77777 & m \tabularnewline
+Precipitable Water & 0 & Mm \tabularnewline
+Aerosol Optical Depth & 0 & Broadband turbidity \tabularnewline
+Snow Depth & 0 & Cm \tabularnewline
+Days Since Last Snow & 88 & Days \tabularnewline
+Radiation Values (Direct/Diffuse) & 0.0 & Wh/m2 \tabularnewline
+Illuminance Values & 0.0 & lux (or CD/m2) \tabularnewline
+\bottomrule
+\end{longtable}
+
+**Standard Barometric pressure based on location elevation is taken from ASHRAE 2001 Handbook of Fundamentals, pages 6.1 \& 6.2.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/references.tex b/doc/auxiliary-programs/src/weather-converter-program/references.tex
new file mode 100644
index 00000000000..81a6b38f461
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/references.tex
@@ -0,0 +1,73 @@
+\section{References}\label{references-002}
+
+ASHRAE. 1985. \emph{Weather Year for Energy Calculations}. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 1997. \emph{WYEC2 Weather Year for Energy Calculations 2, Toolkit and Data}, Atlanta: ASHRAE.
+
+ASHRAE. 2001. \emph{International Weather for Energy Calculations (IWEC Weather Files) Users Manual and CD-ROM}, Atlanta: ASHRAE
+
+ASHRAE. 2004. \emph{ANSI/ASHRAE Standard 90.2-2004}, ``Energy-Efficient Design of Low-Rise Residential Buildings,'' September 2004. Atlanta: American Society of Heating, Refrigerating, and Air-conditioning Engineers.
+
+ASHRAE. 2004. \emph{ANSI/ASHRAE/IESNA Standard 90.1-2004}, ``Energy-Efficient Design of Buildings Except Low-Rise Residential,'' September 2004. Atlanta: American Society of Heating, Refrigerating, and Air-conditioning Engineers.
+
+ASHRAE, 2009. Handbook of Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-conditioning Engineers.
+
+Briggs, Robert S., Robert G. Lucas, and Z. Todd Taylor. 2002. ``Climate Classification for Building Energy Codes and Standards: Part 1 - Development Process'' in \emph{ASHRAE Transactions 2002}, 109, Pt 1. Atlanta: ASHRAE.
+
+Briggs, Robert S., Robert G. Lucas, and Z. Todd Taylor. 2002. ``Climate Classification for Building Energy Codes and Standards: Part 2 - Zone Definitions, Maps and Comparisons'' in \emph{ASHRAE Transactions}, 109, Pt 1. Atlanta: ASHRAE.
+
+Buhl, W.F. 1998. DOE-2 Weather Processor, DOE2.1E Documentation Update, Berkeley: Lawrence Berkeley National Laboratory.
+
+COMIS Weather Program, http://www.byggforsk.no/hybvent/COMISweather.htm
+
+China Meteorological Bureau, Climate Information Center, Climate Data Office and Tsinghua University, Department of Building Science and Technology. 2005. China Standard Weather Data for Analyzing Building Thermal Conditions, April 2005. Beijing: China Building Industry Publishing House, ISBN 7-112-07273-3 (13228). http://www.china-building.com.cn.
+
+Commission of the European Community. 1985. \emph{Test Reference Years,} Weather data sets for computer simulations of solar energy systems and energy consumption in buildings, CEC, DG XII. Brussels, Belgium: Commission of the European Community.
+
+Crawley, Drury B., Linda K. Lawrie, Curtis O. Pedersen, Richard J. Liesen, Daniel E. Fisher, Richard K. Strand, Russell D. Taylor, Frederick C. Winkelmann, W.F. Buhl, A. Ender Erdem, and Y. Joe Huang. 1999. ``EnergyPlus, A New-Generation Building Energy Simulation Program,'' in \emph{Proceedings of Building Simulation '99}, Kyoto, Japan. IBPSA.
+
+Crawley, Drury B. 1998. ``Which Weather Data Should You Use for Energy Simulations of Commercial Buildings?,'' \emph{ASHRAE Transactions}, pp.~498-515, Vol. 104, Pt. 2. Atlanta: ASHRAE. http://energyplus.gov/pdfs/bibliography/whichweatherdatashouldyouuseforenergysimulations.pdf
+
+Crawley, Drury B., Jon Hand, and Linda K. Lawrie, 1999. ``Improving the Weather Information Available to Simulation Programs'', in \emph{Proceedings of Building Simulation '99}, Kyoto, Japan. September 1999. IBPSA.
+
+Energy Simulation Research Unit. 1999. http://www.strath.ac.uk/Departments/ESRU
+
+Janak, M. 1997. ``Coupling Building Energy and Lighting Simulation,'' in \emph{Proceedings of Building Simulation 97}, September 1997, Volume II pp 313-319, Prague, Czech Republic, IBPSA.
+
+Köppen, W. 1931. Grundriss der Klimakunde. Berlin: Walter de Gruyter \& Co.
+
+Kusuda, T., ``Earth Temperatures Beneath Five Different Surfaces'', Institute for Applied Technology, NBS Report 10-373, 1971, NBS, Washington DC 20234.
+
+Kusuda, T., Least Squares Technique for the Analysis of Periodic Temperature of the Earth's Surface Region, NBS Journal of Research, Vol. 71C, Jan-Mar. 1967, pp 43-50.
+
+National Instruments Corporation. 1999. \emph{LabVIEW User Manual}. Austin, Texas: National Instruments Corporation.
+
+McDonald, Iain, and Paul Strachan. 1998. ``Practical Application of Uncertainty Analysis'' in \emph{Proceedings of EPIC 98: Second International Conference on Energy Performance and Indoor Climate in Buildings}, Lyon, France, 19-21 November 1998.
+
+National Climatic Data Center (NCDC). 1976. \emph{Test Reference Year (TRY)}, Tape Reference Manual, TD-9706, September 1976. Asheville, North Carolina: National Climatic Data Center, U.S. Department of Commerce.
+
+NCDC. 1981. \emph{Typical Meteorological Year User's Manual, TD-9734, Hourly Solar Radiation -- Surface Meteorological Observations}, May 1981. Asheville, North Carolina: National Climatic Data Center, U.S. Department of Commerce.
+
+NCDC. 1981. \emph{Meteorological Observations}, May 1981. Asheville, North Carolina: National Climatic Data Center, U.S. Department of Commerce.
+
+NCDC. 1993. \emph{Solar and Meteorological Surface Observation Network, 1961-1990, Version 1.0}, September 1993. Asheville, North Carolina: National Climatic Data Center, U.S. Department of Commerce.
+
+National Renewable Energy Laboratory (NREL). 1995. \emph{User's Manual for TMY2s (Typical Meteorological Years)}, NREL/SP-463-7668, and \emph{TMY2s, Typical Meteorological Years Derived from the 1961-1990 National Solar Radiation Data Base}, June 1995, CD-ROM. Golden, Colorado: National Renewable Energy Laboratory.
+
+http://rredc.nrel.gov/solar/pubs/tmy2/
+
+Numerical Logics. 1999. Canadian Weather for Energy Calculations, Users Manual and CD-ROM. Downsview, Ontario: Environment Canada.
+
+Oliver, John E. 1991. ``The History, Status and Future of Climatic Classification,'' in Physical Geography 1991, Vol 12, No. 3, pp.~231-251.
+
+Perez R, Ineichen P, Maxwell E, Seals R and Zelenka. A 1992. Dynamic Global-to-Direct Irradiance Conversion Models. \emph{ASHRAE Transactions-Research Series},354-369.
+
+Perez R, Ineichen P, Seals R, Michalsky J and Stewart R. 1990. Modeling daylight.availability and irradiance components from direct and global irradiance. \emph{Solar.Energy}44, 271-289.
+
+University of Illinois. 1998. \emph{BLAST User's Guide.} Building Systems Laboratory, University of Illinois. Urbana, Illinois: University of Illinois, Department of Industrial and Mechanical Engineering.
+
+Ward. G. 1996. \emph{Radiance.} Berkeley: Lawrence Berkeley National Laboratory.
+
+Winkelmann, F.C., W.F. Buhl, B. Birdsall, A. E. Erdem, and K. Ellington. 1994. \emph{DOE-2.1E Supplement}, DE-940-11218. Lawrence Berkeley Laboratory, Berkeley, California. Springfield, Virginia: NTIS.
+
+Zhang, Q. Y., Y. J. Huang. 2002. ``Development of Typical Year Weather Files for Chinese Locations'', in ASHRAE Transactions, Volume 108, Part 2.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/reports-files-produced-by-the-weather.tex b/doc/auxiliary-programs/src/weather-converter-program/reports-files-produced-by-the-weather.tex
new file mode 100644
index 00000000000..4315fbc9608
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/reports-files-produced-by-the-weather.tex
@@ -0,0 +1,783 @@
+\section{Reports/Files Produced by the Weather Converter}\label{reportsfiles-produced-by-the-weather-converter}
+
+Minimally, two outputs are produced for every weather converter run: an audit / log file and a statistical report file. The audit / log file shows details of the processing (including any errors) as well as the statistical report. The statistical report produced from the weather conversion process is a short, but complete, picture of the weather data on the file. A single file (.stat extension) is produced of the ``statistics'' about the data file. A feature of the weather converter is to look in several design condition files for possible design conditions for the location from the stored design condition files (source: ASHRAE Handbook of Fundamentals, 2001). If found (WMO (World Meteorological Organization) id is used for matching), these will be shown in the report as well as included in the output data files (EPW and CSV, as applicable). In addition, the Köppen classification scheme is used to characterize the climate based on the data file's contents. Other statistics are given as well to help you visualize the data.
+
+In the ``reporting'' section of the file, each line contains ``tab-delimited'' elements. This will allow you to easily place the data into a spreadsheet program for further refinement but the tabs are not as intrusive for ``normal viewing'' as commas.
+
+\subsection{Audit / Log File}\label{audit-log-file}
+
+As an example, the initial portion of an audit file is shown (illustrating the error reporting):
+
+\begin{lstlisting}
+ -Input File Type = WY2, with FileName = D:\DevTests\Release\WeatherData\04772.wy2
+ -Out of Range Data items will NOT be corrected.
+ Warning ** Dew Point =   5.00&deg;C > Dry Bulb =   4.90&deg;C on date = 5/ 1 at hour = 4
+ Warning ** Dew Point =   4.80&deg;C > Dry Bulb =   4.40&deg;C on date = 5/ 1 at hour = 5
+ Warning ** Dew Point =   4.70&deg;C > Dry Bulb =   3.80&deg;C on date = 5/ 1 at hour = 6
+ Warning ** Suspected missing data line after processing          365  days
+  Month =           0  Day =           0  Hour =           0
+  Processing continues but may be in error
+ Warning ** Suspected Blank line after processing          365  days
+ ** Remaining records, if any, will be ignored
+ Warning ** Missing Data Found on Source Weather Data File
+ ** Missing (and corrected) Aerosol Optical Depth, Number of items = 8760
+ Warning ** Out of Range Data Found on Weather Data File
+ ** Out of Range Dew Point Temperatures > Dry Bulb Temperatures, Number of items =    3
+\end{lstlisting}
+
+\begin{lstlisting}
+ - Start Date/End Date for Weather Source
+ Start Date = Jan  1; End Date = Dec 31
+\end{lstlisting}
+
+\begin{lstlisting}
+ - Actual Data Years for Monthly Data**
+             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+              1966  1980  1964  1964  1968  1970  1977  1981  1979  1969  1974  1960
+ - ** Not all weather data sources represent contiguous years.
+ - ** Monthly data values may come from different years.
+\end{lstlisting}
+
+\begin{lstlisting}
+ - Data Sources should be checked for relevancy to these statistics.
+\end{lstlisting}
+
+\begin{lstlisting}
+ Average Delta DB Change =  0.76&deg;C ; Std Dev =  0.73&deg;C
+ Average Delta DP Change =  0.62&deg;C ; Std Dev =  0.69&deg;C
+ Average Delta Relative Humidity Change =  3.50% ; Std Dev =  3.63%
+ Average Delta Wind Speed Change =  0.93m/s ; Std Dev =  0.88m/s
+ Hourly Dry Bulb temperature change trigger = minimum of  11.07&deg;C  and  10.&deg;C
+     11.07&deg;C = calculated trigger based on mean change in dry-bulb temperature and standard deviation shown above
+     10.&deg;C = trigger set by user
+\end{lstlisting}
+
+\begin{lstlisting}
+ -Output File Type = epw, with FileName = D:\DevTests\Release\WeatherData\Out\CAN\_Ottawa-International\_Airport\_CWEC.epw
+ -Output File Type = csv, with FileName = D:\DevTests\Release\WeatherData\Out\CAN\_Ottawa-International\_Airport\_CWEC.csv
+\end{lstlisting}
+
+\subsection{Statistical Report File}\label{statistical-report-file}
+
+As will be seen in comparison with a ``statistical'' report shown following, the audit file may contain some details about the data that the statistical report does not (such as the data years for the weather data). Some basic statistics are shown first:
+
+\begin{lstlisting}
+Statistics for USA_CA_San.Francisco.Intl.AP.724940_TMY3
+ Location -- San Francisco Intl Ap CA USA
+      {N 37&deg; 37'} {W 122&deg; 24'} {GMT -8.0 Hours}
+ Elevation --     2m above sea level
+ Standard Pressure at Elevation -- 101301Pa
+ Data Source -- TMY3
+\end{lstlisting}
+
+\begin{lstlisting}
+ WMO Station 724940
+\end{lstlisting}
+
+\begin{lstlisting}
+- Displaying Design Conditions from "Climate Design Data 2009 ASHRAE Handbook"
+ - ASHRAE design conditions are carefully generated from a period of record
+ - (typically 30 years) to be representative of that location and to be suitable
+ - for use in heating/cooling load calculations.
+\end{lstlisting}
+
+\begin{lstlisting}
+      Design Stat   ColdestMonth  DB996  DB990  DP996  HR_DP996      DB_DP996      DP990  HR_DP990       DB_DP990      WS004c DB_WS004c     WS010c DB_WS010c     WS_DB996      WD_DB996
+      Units  {}     {&deg;C}   {&deg;C}   {&deg;C}   {}     {&deg;C}   {&deg;C}   {}     {&deg;C}   {m/s}  {&deg;C}   {m/s}  {&deg;C}       {m/s}  {deg}
+      Heating       1      3.8    4.9    -3.7   2.8    10.7   -1.2   3.4    11.2   12.9   12.1   11.6       12.2   2.2    150
+\end{lstlisting}
+
+\begin{lstlisting}
+      Design Stat   HottestMonth  DBR    DB004  WB_DB004      DB010  WB_DB010      DB020  WB_DB020       WB004  DB_WB004      WB010  DB_WB010      WB020  DB_WB020      WS_DB004      WD_DB004      DP004       HR_DP004      DB_DP004      DP010  HR_DP010      DB_DP010      DP020  HR_DP020      DB_DP020       EN004  DB_EN004      EN010  DB_EN010      EN020  DB_EN020      \#Hrs_8-4_&_DB-12.8/20.6
+      Units  {}     {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}       {&deg;C}   {m/s}  {deg}  {&deg;C}   {}     {&deg;C}   {&deg;C}   {}     {&deg;C}   {&deg;C}   {}     {&deg;C}   {kJ/kg}       {&deg;C}   {kJ/kg}       {&deg;C}   {kJ/kg}       {&deg;C}   {}
+      Cooling       8      8.5    28.3   17.2   25.7   16.7   23.6   16.2   18.6   25.7   17.8   23.9   17       22.4   5.9    310    16.1   11.5   19.9   15.3   10.9   19.2   14.7   10.4   18.7   52.4   25.8       49.8   23.8   47.6   22.4   2038
+\end{lstlisting}
+
+\begin{lstlisting}
+      Design Stat   WS010  WS025  WS050  WBmax  DBmin_mean    DBmax_mean    DBmin_stddev  DBmax_stddev       DBmin05years  DBmax05years  DBmin10years  DBmax10years  DBmin20years  DBmax20years  DBmin50years       DBmax50years
+      Units  {m/s}  {m/s}  {m/s}  {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}       {&deg;C}   {&deg;C}   {&deg;C}
+      Extremes      12.8   11.5   10.6   22.3   1.8    34.6   1.5    2.3    0.8    36.2   -0.1   37.5   -0.9    38.8   -1.9   40.5
+\end{lstlisting}
+
+\begin{lstlisting}
+ - Displaying Monthly Design Conditions "Climate Design Data 2009 ASHRAE Handbook"
+ - Monthly Optical Sky Depth Beam (taub) and Diffuse (taud)
+                                 Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct       Nov    Dec
+                   taub (beam)   0.316  0.326  0.334  0.362  0.368  0.353  0.371  0.365  0.352  0.335       0.320  0.318
+                taud (diffuse)   2.608  2.528  2.525  2.345  2.360  2.496  2.395  2.435  2.518  2.545       2.611  2.538
+\end{lstlisting}
+
+\begin{lstlisting}
+                          taub   = Clear Sky Optical Depth for Beam Irradiance
+                          taud   = Clear Sky Optical Depth for Diffuse Irradiance
+\end{lstlisting}
+
+\begin{lstlisting}
+ - Monthly Solar Irradiance Wh/m$^{2}$ (noon on 21st of month)
+                     ib (beam)    879   910   933   918   912   923   903   904   901   887   866     846
+                  id (diffuse)     79    93   100   124   123   108   118   112    99    90    78       80
+\end{lstlisting}
+
+\begin{lstlisting}
+                            ib   = Clear Sky Noon Beam Normal Irradiance on 21st Day
+                            id   = Clear Sky Noon Diffuse Horizontal Irradiance on 21st Day
+\end{lstlisting}
+
+\begin{lstlisting}
+ - Monthly Drybulb and Mean Coincident Wetbulb Temperatures&deg;C
+                                 Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct       Nov    Dec
+                  Drybulb 0.4%   17.8  21.1  23.3  26.9  28.3  31.5  29.4  29.2  31.1  29.5  22.7   17.5
+        Coincident Wetbulb 0.4%   12.1  13.9  14.4  16.2  17.3  17.7  18.4  18.2  18.0  16.5  14.0   12.9
+                  Drybulb 2.0%   15.8  17.9  19.8  22.5  23.7  25.6  25.3  25.0  27.1  25.5  20.0   16.2
+        Coincident Wetbulb 2.0%   12.1  12.7  13.4  14.4  15.8  16.7  17.3  17.5  17.1  15.6  13.5   13.0
+                  Drybulb 5.0%   14.6  16.2  17.6  19.5  21.1  22.3  22.7  22.9  23.9  22.6  18.2   15.2
+        Coincident Wetbulb 5.0%   11.8  12.6  13.0  13.6  15.1  15.8  16.5  16.8  16.6  15.2  13.4   12.5
+                  Drybulb 10.%   13.5  15.0  16.2  17.5  19.1  20.6  21.2  21.5  21.8  20.5  16.8   14.2
+        Coincident Wetbulb 10.%   11.2  12.1  12.5  12.9  14.1  15.1  15.9  16.2  16.1  14.9  13.3   11.7
+\end{lstlisting}
+
+\begin{lstlisting}
+                  Drybulb 0.4%   = 0.4% Monthly Design Drybulb Temperature
+        Coincident Wetbulb 0.4%   = 0.4% Monthly Mean Coincident Wetbulb Temperature
+                  Drybulb 2.0%   = 2.0% Monthly Design Drybulb Temperature
+        Coincident Wetbulb 2.0%   = 2.0% Monthly Mean Coincident Wetbulb Temperature
+                  Drybulb 5.0%   = 5.0% Monthly Design Drybulb Temperature
+        Coincident Wetbulb 5.0%   = 5.0% Monthly Mean Coincident Wetbulb Temperature
+                  Drybulb 10.%   = 10.% Monthly Design Drybulb Temperature
+        Coincident Wetbulb 10.%   = 10.% Monthly Mean Coincident Wetbulb Temperature
+\end{lstlisting}
+
+Or, if the weather converter must calculate the design stats:
+
+\begin{lstlisting}
+-EnergyPlus Weather Converter V7.1.0.010
+ Statistics for FaroCST
+ Location -- Faro - PRT 
+      {N 37&deg;  2'} {E   7&deg; 55'} {GMT +0.0 Hours}
+ Elevation --   100m above sea level
+ Standard Pressure at Elevation -- 100129Pa
+ Data Source -- Custom-085790
+\end{lstlisting}
+
+\begin{lstlisting}
+ WMO Station 085790
+\end{lstlisting}
+
+\begin{lstlisting}
+ - Displaying Design Conditions calculated from this weather file.
+ -  The following design temperature statistics are calculated based on THIS weather file ONLY
+ -  and may not be representative of a long-term  period of record normally used for
+ -  design temperatures. Also, note that dew point temperatures are listed where
+ -  wet-bulb temperatures are normally presented.
+\end{lstlisting}
+
+\begin{lstlisting}
+       Design Stat   Coldest Month HDB 99.6%     HDB 99%
+         Units         {}          {C}         {C} 
+        Heating     3      5.6   6.0
+\end{lstlisting}
+
+\begin{lstlisting}
+       Design Stat   Hottest Month CDB .4%       CDB 1% CDB 2% CDP .4%       CDP 1% CDP 2%
+         Units         {}         {C}          {C}   {C}   {C}          {C}   {C}
+        Cooling     8     33.3  32.5  31.8  22.6  22.0  21.7
+\end{lstlisting}
+
+\begin{lstlisting}
+       Design Stat   Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+         Units     {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}
+       Max WS  0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0
+\end{lstlisting}
+
+\begin{lstlisting}
+ - Heating/Cooling Degree Days/Hours calculated from this weather file are later in this report.
+\end{lstlisting}
+
+These are followed by groupings of Monthly temperature data.
+
+\begin{lstlisting}
+
+- Monthly Statistics for Dry Bulb temperatures&deg;C
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  Maximum       16.7  22.2  23.9  28.3  29.4  32.8  26.7  29.4  30.0  26.7  20.6  16.1 
+  Day:Hour     19:13  14:13  12:15  2:15  1:12  30:14  12:13  2:13  15:14  20:14  1:14  1:15 
+
+  Minimum        2.2   5.0   4.4   8.3   8.9   9.4  11.1  11.1  11.1   7.8   3.3   2.8 
+  Day:Hour     24:06  26:07  23:05  19:05  4:02  22:03  1:04  28:05  7:02  31:05  30:05  26:05 
+
+  Daily Avg     9.6   11.3  12.7  13.7  15.0  15.3  15.9  16.6  16.7  15.1  12.8  10.7  
+
+  - Maximum Dry Bulb temperature of  32.8&deg;C on Jun 30
+  - Minimum Dry Bulb temperature of   2.2&deg;C on Jan 24
+
+  - Monthly Statistics for Extreme Dry Bulb temperatures&deg;C
+  \#Days      Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  Max > = 32                                         1                                        
+  Max < =  0                                                                                  
+  Min < =  0                                                                                  
+  Min < = -18                                                                                  
+
+  - Monthly Statistics for Dew Point temperatures&deg;C
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  Maximum      13.3  12.2  13.9  15.0  16.7  16.1  14.0  16.7  16.7  14.4  14.4  13.9  
+  Day:Hour     17:12  21:04  29:15  2:14  14:09  5:12  8:14  3:10  23:12  6:14  11:12  7:03 
+
+  Minimum      -1.1  0.6   -1.1  -0.6  0.0   5.0   6.1   4.4   7.8   -1.7  -3.3  -5.6  
+  Day:Hour     24:05  24:07  12:15  12:13  2:17  18:17  2:13  30:12  15:17  16:21  21:21  19:12 
+
+  Daily Avg     6.4   6.6   8.1   8.2   9.4   10.0  10.7  11.5  12.5  9.4   8.3   6.1   
+
+  - Maximum Dew Point temperature of  16.7&deg;C on May 14
+  - Minimum Dew Point temperature of  -5.6&deg;C on Dec 19
+  For the dry bulb and dew point temperatures, an average hourly report, by month, is also given:
+  - Average Hourly Statistics for Dry Bulb temperatures&deg;C
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  0:01- 1:00    8.9   9.9  10.6  11.6  12.3  12.1  13.4  14.0  14.4  13.3  11.6   9.7 
+  1:01- 2:00    8.7   9.5  10.3  11.4  12.1  12.0  13.2  13.7  14.3  12.7  11.2   9.4 
+  2:01- 3:00    8.3   9.0  10.1  11.3  12.0  11.7  13.1  13.5  14.1  12.4  11.0   9.2 
+  3:01- 4:00    7.8   8.6  10.0  11.2  12.0  11.6  12.9  13.4  14.0  12.4  11.1   8.9 
+  4:01- 5:00    7.9   8.5   9.7  11.0  11.8  11.5  13.4  13.3  13.8  12.0  10.6   8.7 
+  5:01- 6:00    7.8   8.4   9.6  11.3  12.4  12.3  13.8  13.5  13.9  12.2  10.8   8.5 
+  6:01- 7:00    7.9   8.3   9.8  12.2  14.0  14.1  14.3  14.9  14.6  12.5  10.9   8.5 
+  7:01- 8:00    7.9   9.2  11.5  13.1  15.5  15.7  15.4  16.3  16.1  14.3  11.5   8.9 
+  8:01- 9:00    8.8  10.1  12.6  14.1  16.6  16.6  16.5  17.5  17.4  15.3  12.6   9.9 
+  9:01-10:00    9.5  11.0  13.7  15.0  17.7  17.7  17.5  18.4  18.5  16.1  13.2  10.9 
+  10:01-11:00   10.1  12.1  14.5  16.2  18.8  19.1  18.4  19.6  19.6  17.2  13.8  11.5 
+  11:01-12:00   10.6  13.2  15.6  16.8  19.3  19.9  19.3  20.6  20.5  18.0  14.3  11.9 
+  12:01-13:00   11.4  14.2  16.4  17.1  19.2  20.6  20.2  21.3  21.3  18.9  14.9  12.5 
+  13:01-14:00   11.5  14.5  16.9  17.0  19.0  20.5  19.8  21.5  21.4  19.2  15.4  12.9 
+  14:01-15:00   11.9  14.8  16.8  17.0  18.4  19.7  19.4  21.1  21.0  19.1  15.7  13.0 
+  15:01-16:00   11.6  15.1  16.0  16.7  17.6  18.8  19.0  20.1  19.9  18.2  15.4  13.0 
+  16:01-17:00   11.0  14.1  15.1  15.8  16.7  17.6  18.0  18.8  18.8  17.0  14.3  12.4 
+  17:01-18:00   10.6  13.1  13.8  14.4  15.7  16.6  16.9  17.4  17.0  15.8  13.7  12.0 
+  18:01-19:00   10.3  12.2  12.7  13.3  14.4  15.3  15.8  16.1  15.9  15.3  13.4  11.5 
+  19:01-20:00   10.0  11.8  12.3  12.9  13.4  13.8  15.3  15.4  15.6  14.9  13.0  11.1 
+  20:01-21:00    9.7  11.4  11.7  12.6  13.2  13.3  14.8  15.0  15.1  14.5  12.6  10.6 
+  21:01-22:00    9.6  11.0  11.6  12.3  13.0  12.9  14.2  14.7  14.8  14.2  12.1  10.4 
+  22:01-23:00    9.5  10.6  11.3  12.0  12.7  12.5  14.0  14.3  14.6  13.8  12.1  10.3 
+  23:01-24:00    9.2  10.3  11.1  11.8  12.4  12.5  13.7  14.3  14.5  13.5  11.7  10.0 
+  Max Hour      15    16    14    13    12    13    13    14    14    14    15    15  
+  Min Hour       6     7     6     5     5     5     4     5     5     5     5     6  
+
+  - Average Hourly Statistics for Dew Point temperatures&deg;C
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  0:01- 1:00    6.7   6.6   8.0   8.1   9.5   9.7   9.9  11.4  12.3   9.7   8.0   5.7 
+  1:01- 2:00    6.6   6.1   7.7   8.1   9.4   9.6  10.1  11.2  12.3   9.3   8.0   5.8 
+  2:01- 3:00    6.3   5.9   7.4   8.2   9.3   9.4  10.0  11.2  12.2   9.1   7.6   5.9 
+  3:01- 4:00    5.9   5.9   7.7   8.0   9.3   9.5   9.7  11.0  12.1   8.9   8.0   5.8 
+  4:01- 5:00    5.9   5.6   7.6   8.0   9.2   9.4   9.9  11.0  12.1   9.1   7.6   5.5 
+  5:01- 6:00    5.9   5.5   7.5   8.1   9.4   9.8  10.1  11.1  12.1   9.1   7.8   5.7 
+  6:01- 7:00    6.0   5.7   7.6   8.5   9.7  10.3  10.2  11.6  12.4   9.5   7.8   5.8 
+  7:01- 8:00    5.9   6.1   8.4   8.8   9.7  10.6  10.8  11.8  12.7  10.4   7.9   6.1 
+  8:01- 9:00    6.1   6.8   8.8   9.0  10.0  10.8  11.0  12.1  12.9  10.4   8.2   6.3 
+  9:01-10:00    6.1   7.3   8.8   8.9   9.7  10.9  11.0  12.4  13.2  10.4   8.1   6.3 
+  10:01-11:00    6.4   7.1   8.5   8.7   9.8  10.8  11.4  12.0  13.4   9.9   8.3   6.2 
+  11:01-12:00    6.3   6.8   8.3   8.6   9.5  10.6  11.5  11.8  13.3   9.7   8.1   6.2 
+  12:01-13:00    6.2   6.9   8.3   8.5   9.4  10.5  11.5  11.6  12.8   9.2   8.3   6.5 
+  13:01-14:00    6.3   6.8   8.0   8.7   9.2  10.2  11.6  11.5  12.6   9.3   8.4   6.6 
+  14:01-15:00    6.4   7.1   8.4   8.1   9.2  10.1  11.5  11.4  12.4   8.8   8.7   6.4 
+  15:01-16:00    6.6   7.6   8.0   7.7   9.0   9.9  11.4  11.2  12.4   8.9   8.6   6.3 
+  16:01-17:00    6.6   7.1   7.9   7.8   9.0   9.7  11.2  11.4  12.3   9.0   9.3   6.7 
+  17:01-18:00    6.6   6.8   7.9   7.8   9.1   9.6  11.0  11.4  12.3   8.9   9.4   6.7 
+  18:01-19:00    6.5   6.7   7.9   7.9   9.4   9.6  10.6  11.4  12.3   9.0   9.1   6.7 
+  19:01-20:00    6.5   6.5   7.9   8.0   9.3   9.6  10.7  11.5  12.4   9.2   8.9   6.3 
+  20:01-21:00    6.6   6.6   8.2   7.7   9.5   9.6  10.6  11.5  12.4   9.3   8.5   6.2 
+  21:01-22:00    6.8   6.8   8.0   8.1   9.5   9.7  10.2  11.4  12.5   9.5   8.6   6.0 
+  22:01-23:00    6.7   6.6   8.3   8.0   9.7   9.7  10.4  11.5  12.4   9.6   8.4   6.1 
+  23:01-24:00    6.6   6.5   8.4   8.1   9.6   9.6  10.3  10.7  12.4   9.4   8.5   5.9 
+  Max Hour      22    16     9     9     9    10    14    10    11     9    18    19  
+  Min Hour       6     6     3    16    16     5     4    24     4    15     3     5  
+
+
+  Humidity/precipitation: Relative Humidity (both monthly and average hourly by month)
+  - Monthly Statistics for Relative Humidity %
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+  Maximum        100    96    96   100   100    96    93    96   100    96    96   100
+  Day:Hour     7:05  6:04  20:22  9:03  25:02  5:01  18:04  7:02  4:07  7:07  11:07  7:05
+
+
+  Minimum         23    30    22    24    25    30    25    36    19    20    32    25
+  Day:Hour    17:15  14:13  4:16  5:10  9:12  17:10  2:13  14:13  28:15  30:13  20:15  24:15
+
+
+  Daily Avg       77    75    70    72    73    73    71    74    72    73    74    79
+
+
+  - Average Hourly Relative Humidity %
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+  0:01- 1:00     83    81    77    81    85    84    83    86    84    81    81    84
+  1:01- 2:00     84    82    75    80    87    84    83    86    85    82    81    85
+  2:01- 3:00     86    83    76    83    88    85    83    87    85    82    82    86
+  3:01- 4:00     87    84    78    82    87    85    83    87    85    83    83    85
+  4:01- 5:00     88    84    79    83    88    83    81    88    85    83    83    86
+  5:01- 6:00     89    84    80    83    88    81    80    88    85    83    83    86
+  6:01- 7:00     89    84    80    79    81    80    78    84    82    83    83    86
+  7:01- 8:00     88    82    75    73    74    75    73    77    78    78    79    86
+  8:01- 9:00     83    81    70    70    68    69    68    71    71    74    74    82
+  9:01-10:00     77    79    68    65    64    64    62    67    65    70    70    79
+  10:01-11:00     74    74    65    62    59    62    59    60    59    65    66    76
+  11:01-12:00     69    69    59    60    55    60    56    57    54    60    63    73
+  12:01-13:00     65    63    58    59    53    58    53    55    52    55    59    71
+  13:01-14:00     62    63    58    60    54    59    55    55    54    56    61    68
+  14:01-15:00     61    63    58    60    56    60    56    57    56    58    62    67
+  15:01-16:00     61    62    59    62    59    60    58    61    58    59    64    69
+  16:01-17:00     66    65    62    63    62    65    62    63    63    64    67    74
+  17:01-18:00     71    68    67    66    67    69    67    69    67    69    70    76
+  18:01-19:00     74    71    71    69    73    74    72    75    73    73    73    76
+  19:01-20:00     77    73    72    73    79    76    75    79    76    75    74    77
+  20:01-21:00     78    74    74    75    81    78    77    82    78    77    76    78
+  21:01-22:00     79    76    76    76    83    80    80    83    79    78    77    79
+  22:01-23:00     79    78    76    78    84    81    81    84    81    79    78    82
+  23:01-24:00     82    79    76    79    84    83    82    84    82    80    80    82
+  Max Hour       7     7     7     5     5     4     1     6     5     5     7     7
+  Min Hour      15    16    15    13    13    13    13    13    13    13    13    15
+
+
+  - Monthly Indicators for Precipitation/Moisture (kPa)
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+  0.8   1.1   0.9   1.0   1.1   1.2   1.3   1.3   1.3   1.2   1.1   0.9
+
+
+  Wind and Wind Chill/Heat Index
+  - Monthly Statistics for Wind Chill/Heat Index temperatures&deg;C **
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+  Minimum WC      -1    -1    -6    -1    -2     4                         9     0    -8
+  Day:Hour     19:09  2:10  16:06  15:04  5:24  1:23                     27:04  27:04  28:04
+
+
+  Average WC       6     7     4     5     5     6                         9     7     4
+  Avg Del WC       1     2     5     3     4     4                         0     2     3
+  \# Hours WC    293   166   258   159    56    10                         3    86   358
+
+
+  Maximum HI                                             27    28                    
+  Day:Hour                                            2:10  15:11                    
+
+
+  Average HI                                             27    28                    
+  Avg Del HI                                              0     0                    
+  \# Hours HI                                             1     1                    
+
+
+  - **WindChill/HeatIndex Temps -- statistics...only those different from Air Temps
+
+
+
+
+  - Monthly Wind Direction % {N = 0 or 360,E = 90,S = 180,W = 270}
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+  North           20    11     6     5     4     3     7     6     9     8    16    27
+  NorthEast       10    10     6     3     3     2     3     3     5     6     6    13
+  East             8     8     6     3     2     1     1     3     3     5     9     8
+  SouthEast       13     7     6     2     1     0     0     0     1     6    17    17
+  South           18    10     9     5     3     1     0     1     5    14    14    12
+  SouthWest        7     6    19     8     5     2     1     6     7     8    11     4
+  West             9    14    31    35    32    59    21    32    22    16    10     5
+  NorthWest       15    35    18    39    50    33    66    50    49    36    17    15
+
+
+  - Monthly Statistics for Wind Speed m/s
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+  Maximum       11.8  14.9  17.0  12.9  15.9  11.8  12.4  13.4  14.9  10.8   8.8  13.4
+  Day:Hour    29:12  10:22  2:15  9:16  10:17  10:16  4:16  29:14  11:15  22:19  3:10  27:13
+
+
+  Minimum        0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0
+  Day:Hour     1:04  1:10  4:04  4:19  8:05  17:07  1:07  1:07  1:07  3:04  2:01  2:03
+
+
+  Daily Avg      2.5   3.5   5.1   4.8   6.5   5.6   5.7   5.5   4.8   3.9   2.7   3.6
+
+
+  - Maximum Wind Speed of  17.0 m/s on Mar  2
+  - Minimum Wind Speed of   0.0 m/s on Jan  1
+
+
+  Rain/Albedo:
+  - Monthly Statistics for Liquid Precipitation mm
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+  Total        47    0     3     24    22    0     0     0     2     14    21    72  
+
+
+  - Monthly Statistics for Albedo
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+  Average      0.160  0.000  0.130  0.130  0.130  0.140  0.000  0.000  0.180  0.180  0.160  0.210
+
+
+
+
+  Solar Radiation
+  - Monthly Statistics for Solar Radiation  (Direct Normal, Diffuse, Global Horizontal) Wh/m$^{2}$
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  Direct Avg   2537  3829  4485  5123  5691  6743  6867  6329  6017  4178  3080  3314  
+
+  Direct Max   5405  7987  8803  8786  10462  10595  10692  10218  8485  7348  6194  6730  
+  Day        27    18    20    18    23     2    25     3    10     3     2    25  
+
+  Diffuse Avg   1127  1300  1763  2344  2335  2247  2148  1998  1643  1610  1252  912   
+
+  Global Avg   2136  3160  4402  5672  6419  7148  7129  6401  5460  3761  2530  2127  
+  - Maximum Direct Normal Solar of 10692 Wh/m$^{2}$ on Jul 25
+
+  - Average Hourly Statistics for Direct Normal Solar Radiation Wh/m$^{2}$
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  0:01- 1:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  1:01- 2:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  2:01- 3:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  3:01- 4:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  4:01- 5:00      0     0     0     0     0     1     0     0     0     0     0     0 
+  5:01- 6:00      0     0     0    25    47    87    51    22     1     0     0     0 
+  6:01- 7:00      0     2    38   194   201   283   200   162    85    64     0     0 
+  7:01- 8:00     50    98   210   340   345   413   310   304   239   279   168    63 
+  8:01- 9:00    220   246   309   407   439   509   444   466   365   383   297   266 
+  9:01-10:00    277   338   424   470   526   575   525   554   523   399   372   375 
+  10:01-11:00    288   449   477   456   561   599   617   594   653   438   428   413 
+  11:01-12:00    303   467   531   546   576   641   657   643   744   445   426   473 
+  12:01-13:00    342   498   537   504   572   653   705   666   732   533   360   455 
+  13:01-14:00    398   494   535   536   579   687   732   675   730   537   414   461 
+  14:01-15:00    326   487   481   494   553   659   712   678   688   478   314   403 
+  15:01-16:00    295   413   433   403   499   570   660   621   593   393   229   306 
+  16:01-17:00     37   273   348   363   395   499   584   488   447   186    73   101 
+  17:01-18:00      2    65   153   285   286   368   432   352   208    44     0     0 
+  18:01-19:00      0     0     8   100   107   186   222   103     9     0     0     0 
+  19:01-20:00      0     0     0     0     2    13    14     2     0     0     0     0 
+  20:01-21:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  21:01-22:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  22:01-23:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  23:01-24:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  Max Hour*     14    13    13    12    14    14    14    15    12    14    11*   12  
+  Min Hour       1     1     1     1     1     1     1     1     1     1     1     1  
+
+  - Average Hourly Statistics for Diffuse Horizontal Solar Radiation Wh/m$^{2}$
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  0:01- 1:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  1:01- 2:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  2:01- 3:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  3:01- 4:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  4:01- 5:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  5:01- 6:00      0     0     0     1    26    35    24    12     0     0     0     0 
+  6:01- 7:00      0     1    14    45    81    79    73    56    36     5     0     0 
+  7:01- 8:00      2    28    70   107   135   129   140   112    98    61    28    11 
+  8:01- 9:00     51    82   124   155   190   177   182   159   146   118    84    57 
+  9:01-10:00    105   123   169   225   215   192   199   196   181   155   127   100 
+  10:01-11:00    146   164   203   268   255   235   224   219   192   208   167   131 
+  11:01-12:00    174   187   227   267   260   232   242   225   189   226   192   141 
+  12:01-13:00    176   173   224   281   249   242   211   231   190   225   205   153 
+  13:01-14:00    170   178   227   258   244   221   205   207   178   191   178   134 
+  14:01-15:00    148   154   194   226   211   201   192   184   156   184   147    98 
+  15:01-16:00    122   118   159   216   188   190   167   154   134   144   114    67 
+  16:01-17:00     34    71   100   162   149   148   137   128    95    91    10    20 
+  17:01-18:00      0    24    49   126    93   109    96    81    46     3     0     0 
+  18:01-19:00      0     0     2     9    39    54    47    31     3     0     0     0 
+  19:01-20:00      0     0     0     0     0     5     9     1     0     0     0     0 
+  20:01-21:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  21:01-22:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  22:01-23:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  23:01-24:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  Max Hour*     13    12    14    13    12    13    12    13    11*   12    13    13  
+  Min Hour       1     1     1     1     1     1     1     1     1     1     1     1  
+
+  - Average Hourly Statistics for Global Horizontal Solar Radiation Wh/m$^{2}$
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  0:01- 1:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  1:01- 2:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  2:01- 3:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  3:01- 4:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  4:01- 5:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  5:01- 6:00      0     0     0     2    31    45    29    14     0     0     0     0 
+  6:01- 7:00      0     1    17    83   136   165   127    91    47     8     0     0 
+  7:01- 8:00      3    39   119   237   295   330   282   234   175   122    47    15 
+  8:01- 9:00     92   150   254   383   469   511   462   429   330   269   164   108 
+  9:01-10:00    197   268   414   558   625   650   607   600   520   368   277   222 
+  10:01-11:00    272   409   532   641   749   773   769   717   684   486   382   306 
+  11:01-12:00    326   473   626   746   800   845   863   805   790   531   425   367 
+  12:01-13:00    353   490   638   726   787   872   886   840   786   589   401   373 
+  13:01-14:00    365   476   619   708   763   855   879   797   735   528   381   336 
+  14:01-15:00    280   409   505   595   656   751   786   716   613   433   269   239 
+  15:01-16:00    206   281   381   463   523   594   634   560   445   292   170   135 
+  16:01-17:00     40   135   221   321   349   421   456   366   252   131    15    27 
+  17:01-18:00      0    30    73   196   184   244   254   187    80     4     0     0 
+  18:01-19:00      0     0     2    14    53    87    86    44     3     0     0     0 
+  19:01-20:00      0     0     0     0     0     5    11     1     0     0     0     0 
+  20:01-21:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  21:01-22:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  22:01-23:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  23:01-24:00      0     0     0     0     0     0     0     0     0     0     0     0 
+  Max Hour      14    13    13    12    12    13    13    13    12    13    12    13  
+  Min Hour       1     1     1     1     1     1     1     1     1     1     1     1  
+
+  - Average Hourly Statistics for Total Sky Cover %
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  0:01- 1:00     59    43    54    47    43    28    37    41    42    31    49    42 
+  1:01- 2:00     60    46    60    53    41    26    41    40    51    33    45    40 
+  2:01- 3:00     62    52    59    48    43    27    45    41    55    30    46    43 
+  3:01- 4:00     60    55    61    52    42    31    50    38    59    30    46    44 
+  4:01- 5:00     63    57    65    56    50    40    52    45    65    33    49    43 
+  5:01- 6:00     62    61    60    53    54    37    55    52    64    39    54    38 
+  6:01- 7:00     60    63    59    59    55    36    58    54    63    41    55    38 
+  7:01- 8:00     61    67    63    51    51    34    52    54    62    42    52    43 
+  8:01- 9:00     65    68    64    48    48    32    45    42    59    44    49    50 
+  9:01-10:00     64    71    59    43    46    29    38    38    43    40    44    50 
+  10:01-11:00     63    66    54    42    45    30    32    35    33    37    46    52 
+  11:01-12:00     58    64    55    42    48    26    26    33    25    36    42    49 
+  12:01-13:00     52    59    53    43    46    27    19    30    25    35    39    50 
+  13:01-14:00     50    61    55    40    46    24    18    27    22    34    41    48 
+  14:01-15:00     49    62    62    39    44    24    17    27    20    31    43    44 
+  15:01-16:00     47    64    59    41    47    25    16    26    20    32    46    43 
+  16:01-17:00     47    62    56    43    48    27    19    31    21    27    46    44 
+  17:01-18:00     49    61    57    40    45    27    24    33    22    29    46    45 
+  18:01-19:00     47    59    51    40    43    29    27    36    18    26    46    42 
+  19:01-20:00     51    54    45    39    42    31    28    37    18    25    47    41 
+  20:01-21:00     53    49    47    41    39    30    27    38    19    27    44    42 
+  21:01-22:00     54    44    45    43    39    26    29    40    27    26    46    45 
+  22:01-23:00     58    43    46    40    38    30    32    38    32    27    44    44 
+  23:01-24:00     55    41    50    40    38    26    36    41    39    26    46    49 
+  Max Hour       9    10     5     7     7     5     7     7     5     9     7    11  
+  Min Hour      16    24    22    15    23    14    16    16    19    20    13     6  
+
+  - Average Hourly Statistics for Opaque Sky Cover %
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
+  0:01- 1:00     57    36    41    41    38    28    36    35    38    26    44    36 
+  1:01- 2:00     57    38    44    45    34    26    40    36    46    30    43    35 
+  2:01- 3:00     58    39    43    43    37    27    44    36    51    27    43    37 
+  3:01- 4:00     57    41    49    50    39    31    48    34    57    28    45    37 
+  4:01- 5:00     60    43    45    54    45    39    50    36    62    30    47    35 
+  5:01- 6:00     60    46    46    52    45    36    54    41    57    37    51    33 
+  6:01- 7:00     58    48    49    58    48    35    56    45    52    39    52    32 
+  7:01- 8:00     59    49    46    50    44    31    50    46    52    40    49    38 
+  8:01- 9:00     62    51    50    46    40    29    43    36    47    43    48    43 
+  9:01-10:00     61    53    43    41    37    26    37    32    34    38    43    44 
+  10:01-11:00     59    50    41    40    35    27    30    31    25    36    45    44 
+  11:01-12:00     55    46    35    40    35    22    25    26    16    34    38    41 
+  12:01-13:00     49    42    33    40    33    21    18    23    15    30    37    43 
+  13:01-14:00     46    41    34    38    34    18    15    20    13    30    36    40 
+  14:01-15:00     45    40    37    37    32    20    15    18    13    27    40    42 
+  15:01-16:00     44    39    37    39    33    22    13    19    14    29    42    39 
+  16:01-17:00     41    40    36    41    36    24    16    24    16    25    44    39 
+  17:01-18:00     46    39    38    38    34    24    21    22    16    27    42    40 
+  18:01-19:00     44    40    30    38    36    24    25    26    14    24    42    36 
+  19:01-20:00     45    37    27    36    36    27    26    29    14    23    42    36 
+  20:01-21:00     49    35    31    37    35    27    25    33    16    25    39    35 
+  21:01-22:00     49    32    32    40    35    25    27    36    22    23    41    38 
+  22:01-23:00     53    33    31    38    33    30    31    35    26    24    41    39 
+  23:01-24:00     52    33    35    38    31    26    35    36    33    23    43    43 
+  Max Hour       9    10     9     7     7     5     7     8     5     9     7    10  
+  Min Hour      17    22    20    20    24    14    16    15    14    20    14     7
+\end{lstlisting}
+
+The program calculated ``undisturbed'' ground temperatures:
+
+\begin{lstlisting}
+
+- Monthly Calculated "undisturbed" Ground Temperatures**&deg;C
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+  0.5 m       9.8   9.5  10.1  11.5  13.4  15.1  16.3  16.7  16.0  14.6  12.8  11.0
+  2.0 m      11.0  10.4  10.6  11.4  12.6  14.0  15.1  15.7  15.6  14.8  13.5  12.1
+  4.0 m      12.0  11.4  11.3  11.6  12.4  13.3  14.2  14.8  14.9  14.5  13.8  12.8
+
+
+  - **These ground temperatures should NOT BE USED in the GroundTemperatures object to compute building floor losses.
+  -   The temperatures for 0.5 m depth can be used for GroundTemperatures:Surface.
+  -   The temperatures for 4.0 m depth can be used for GroundTemperatures:Deep.
+  -   Calculations use a standard soil diffusivity of 2.3225760E-03 {m**2/day}
+  As noted in the above statistics calculation, the "undisturbed" ground temperatures calculated by the weather converter should not be used in building losses but are appropriate to be used in the GroundTemperatures:Surface and GroundTemperatures:Deep objects. The reasoning (for building losses) is that these values are too extreme for the soil under a conditioned building. For best results, use the Slab or Basement program described in this document to calculate custom monthly average ground temperatures (see the Ground Heat Transfer section). This is especially important for residential applications and very small buildings. If one of these ground temperature preprocessors is not used, for typical commercial buildings in the USA, a reasonable default value is 2C less than the average indoor space temperature.
+  Heating/cooling degree days from the weather file are shown.  Long term heating/cooling degree days are shown earlier if available from ASHRAE HOF for the location/WMO.
+  - Monthly Heating/Cooling Degree Days/Hours
+  Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
+  HDD 10C         52     3     7     1     0     0     0     0     0     0     1    36
+  HDD 18C        290   188   223   173   130   100    73    59    54    92   169   273
+
+
+  CDD 10C         10    39    32    68   118   142   188   189   200   157    72    10
+  CDD 18C          0     0     0     0     0     3    14     0    14     1     0     0
+
+
+  CDH 20C          0     9     0    45    93   136   330   223   410   129     0     0
+  CDH 23C          0     0     0     5    13    41   167    50   169    13     0     0
+  CDH 27C          0     0     0     0     0     0    61     5    59     0     0     0
+
+
+  - 1227 annual cooling degree-days (10&deg;C baseline)
+  -  100 annual heating degree-days (10&deg;C baseline)
+
+
+  -   32 annual cooling degree-days (18&deg;C baseline)
+  - 1825 annual heating degree-days (18&deg;C baseline)
+  In the preceding display for degree-days, users more familiar with degree days to a Fahrenheit temperature base, may wish to multiply the degree day or degree hour values by 9/5.
+  And then the K&ouml;ppen, ASHRAE and typical/extreme period calculations:
+  - Climate type "Cfb" (K&ouml;ppen classification)**
+  - Marine west coastal (warm summer, mild winter, rain all year, lat. 35-60&deg;N)
+  * - **Note that the K&ouml;ppen classification shown here is derived algorithmically from the source weather data.*
+  * -   It may not be indicative of the long term climate for this location.*
+
+
+  - Climate type "3C" (ASHRAE Standards 90.1-2004 and 90.2-2004 Climate Zone)**
+  - Warm - Marine, Probable K&ouml;ppen classification = Cs, Dry Summer Subtropical (Mediterranean)
+  * - **Note that the ASHRAE classification shown here is derived algorithmically from the source weather data.*
+  * -   It may not be indicative of the long term climate for this location.*
+
+
+  - Typical/Extreme Period Determination
+
+
+  - Summer is Jul:Sep
+  Extreme Summer Week (nearest maximum temperature for summer)
+  Extreme Hot Week Period selected: Sep 23:Sep 29, Maximum Temp =  35.10&deg;C, Deviation = |16.393|&deg;C
+  Typical Summer Week (nearest average temperature for summer)
+  Typical Week Period selected: Aug 19:Aug 25, Average Temp =  16.27&deg;C, Deviation = | 0.032|&deg;C
+
+
+  - Winter is Jan:Mar
+  Extreme Winter Week (nearest minimum temperature for winter)
+  Extreme Cold Week Period selected: Jan 22:Jan 28, Minimum Temp =  -0.40&deg;C, Deviation = | 8.532|&deg;C
+  Typical Winter Week (nearest average temperature for winter)
+  Typical Week Period selected: Mar  5:Mar 11, Average Temp =  10.19&deg;C, Deviation = | 0.417|&deg;C
+
+
+  - Autumn is Oct:Dec
+  Typical Autumn Week (nearest average temperature for autumn)
+  Typical Week Period selected: Nov 12:Nov 18, Average Temp =  12.19&deg;C, Deviation = | 0.990|&deg;C
+
+
+  - Spring is Apr:Jun
+  Typical Spring Week (nearest average temperature for spring)
+  Typical Week Period selected: May 13:May 19, Average Temp =  13.59&deg;C, Deviation = | 0.018|&deg;C
+\end{lstlisting}
+
+As this data is all tab-delimited, putting in a spreadsheet and displaying is not difficult:
+
+\begin{figure}[hbtp] % fig 12
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image008.jpg}
+\caption{Monthly Dry Bulb Data in SpreadSheet (for graphing) \protect \label{fig:monthly-dry-bulb-data-in-spreadsheet-for}}
+\end{figure}
+
+And these can be easily used to produce graphs:
+
+\begin{figure}[hbtp] % fig 13
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image009.png}
+\caption{Graph of Spreadsheet Data \protect \label{fig:graph-of-spreadsheet-data}}
+\end{figure}
+
+\subsection{Design Day Calculations Output}\label{design-day-calculations-output}
+
+Using the WMO field (or determining it from the WBAN field), the Weather Converter performs table look up in the Design Condition files to see if there are recorded design conditions for the subject location. If this location is found, then design day objects are produced on the resultant design day object (ddy extension) file - ready for inclusion into an EnergyPlus input data file. If no design conditions are located, then the design day object file will still include a location object for inclusion with EnergyPlus. However, statistics using the weather file are displayed to the statistics file - these ``can'' be used to create your own design day definitions but you should read the warning that is issued and take care if your weather file is only a ``single instance'' weather data representation.
+
+The location objects as well as the design condition objects are constrained by the data source. Some data sources do not have elevation information - thus, a location object from such a source will have an elevation of 0.0. Likewise, the time zone of some locations may not be available from the source data nor other data resources that the weather converter uses. A time zone will be estimated from the standard meridian of the location (determined by the longitude) but it may not be accurate. A user needs to be aware of these limitations when taking the design day files from the weather converter.
+
+Note that you can always include a ``def'' file with this data to assure accuracy regardless of input format limitations.
+
+An excerpt of a design day output is shown in the following (actual design day objects have been deleted for brevity). Note that with the 2009 ASHRAE HOF climate conditions, a possible DaylightSavingPeriod object may be included.
+
+\begin{lstlisting}
+
+! The following Location and Design Day data are produced as possible from the indicated data source.
+  ! Wind Speeds follow the indicated design conditions rather than traditional values (6.7 m/s heating, 3.35 m/s cooling)
+  ! No special attempts at re-creating or determining missing data parts (e.g. Wind speed or direction)
+  ! are done.  Therefore, you should look at the data and fill in any incorrect values as you desire.
+
+
+  Site:Location,
+  Chicago Ohare Intl Ap_IL_USA Design_Conditions,     !- Location Name
+  41.98,     !- Latitude {N+ S-}
+  -87.92,     !- Longitude {W- E+}
+  -6.00,     !- Time Zone Relative to GMT {GMT+/-}
+  201.00;     !- Elevation {m}
+
+
+  !  WMO = 725300 Time Zone = NAC: (GMT-06:00) Central Time (US & Canada)
+  !  Data Source = ASHRAE 2009 Annual Design Conditions
+  RunPeriodControl:DaylightSavingTime,
+  2nd Sunday in March,    !- StartDate
+  2nd Sunday in November;    !- EndDate
+
+
+  ! Using Design Conditions from "Climate Design Data 2009 ASHRAE Handbook"
+  ! Chicago Ohare Intl Ap_IL_USA Extreme Annual Wind Speeds, 1% = 11.1m/s, 2.5% = 9.4m/s, 5% = 8.6m/s
+  ! Chicago Ohare Intl Ap_IL_USA Extreme Annual Temperatures, Max Drybulb = -23.7&deg;C Min Drybulb = 35.9&deg;C
+
+
+  ! Chicago Ohare Intl Ap_IL_USA Annual Heating Design Conditions Wind Speed = 4.9m/s Wind Dir = 270
+  ! Chicago Ohare Intl Ap Annual Cooling Design Conditions Wind Speed = 5.2m/s Wind Dir = 230
+
+  ! Coldest Month = January
+  ! Chicago Ohare Intl Ap IL USA Annual Heating 99.6%, MaxDB = -20&deg;C
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Heating 99%, MaxDB = -16.6&deg;C
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (DB = >MWB) 1%, MaxDB = 31.6&deg;C MWB = 23&deg;C
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Humidification 99.6% Design Conditions DP = >MCDB, DP = -25.7&deg;C
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Humidification 99% Design Conditions DP = >MCDB, DP = -22.1&deg;C
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Heating Wind 99.6% Design Conditions WS = >MCDB, WS = 12.4m/s
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Heating Wind 99% Design Conditions WS = >MCDB, WS = 11.4m/s
+
+
+
+
+  ! Hottest Month = July
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (DB = >MWB) .4%, MaxDB = 33.3&deg;C MWB = 23.7&deg;C
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Heating Design Conditions Wind Speed = 4.9m/s Wind Dir = 270
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (DB = >MWB) 2%, MaxDB = 30.1&deg;C MWB = 22.1&deg;C
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (WB = >MDB) .4%, MDB = 31.2&deg;C WB = 25.5&deg;C
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (WB = >MDB) 1%, MDB = 29.6&deg;C WB = 24.5&deg;C
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (WB = >MDB) 2%, MDB = 28.1&deg;C WB = 23.5&deg;C
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (DP = >MDB) .4%, MDB = 28.9&deg;C DP = 23.8&deg;C HR = 0.0192
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (DP = >MDB) 1%, MDB = 27.7&deg;C DP = 22.9&deg;C HR = 0.0180
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (DP = >MDB) 2%, MDB = 26.5&deg;C DP = 21.9&deg;C HR = 0.0170
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (Enthalpy = >MDB) .4%, MDB = 31.4&deg;C Enthalpy = 79.2kJ/kg
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (Enthalpy = >MDB) 1%, MDB = 29.6&deg;C Enthalpy = 75.1kJ/kg
+
+
+  ! Chicago Ohare Intl Ap IL USA Annual Cooling (Enthalpy = >MDB) 2%, MDB = 28.2&deg;C Enthalpy = 70.9kJ/kg
+\end{lstlisting}
+
+Design day ``definitions'' originate in the ASHRAE Handbook of Fundamentals. Prior to 1997, these conditions were described for winter and summer (heating and cooling). They were based on seasonal percentages.
+
+EnergyPlus uses the design day object values and creates an entire day of weather data - this is described more fully in the Input Output Reference under the \textbf{DesignDay} object. The weather converter program assigns ``SummerDesignDay'' and ``WinterDesignDay'' day types by default - these day types influence ``scheduling'' of various elements. How to use these effectively is described during the \textbf{DesignDay} and \textbf{Schedule} objects discussions in the Input Output Reference.
+
+Beginning in 1997, and continuing (the latest version was published in 2009), the design condition data is based on annual percentages. In addition, only locations with long-term hourly observations data (on which to form the basis) are included.
+
+\subsubsection{{[}From ASHRAE Handbook of Fundamentals, 2009{]}:}\label{from-ashrae-handbook-of-fundamentals-2009}
+
+Design data based on dry-bulb temperature represent peak occurrences of the sensible component of ambient outdoor conditions. Design values based on wet-bulb temperature are related to the enthalpy of the outdoor air. Conditions based on dew point relate to the peaks of the humidity ratio. The designer, engineer, or other user must decide which set(s) of conditions and probability of occurrence apply to the design situation under consideration.
+
+The 99.6\% and 99\% Heating conditions are often used in the sizing of heating equipment.
+
+The 0.4, 1.0, and 2.0\% dry-bulb temperatures and mean coincident wet-bulb temperatures (i.e., DB = \textgreater{}MWB) often represent conditions on hot, mostly sunny days. These are often used in sizing cooling equipment such as chillers or air-conditioning units.
+
+Design conditions based on wet-bulb temperatures (i.e., WB = \textgreater{}MDB) represent extremes of the total sensible plus latent heat of outdoor air. This information is useful for cooling towers, evaporative coolers, and fresh air ventilation system design.
+
+Design conditions based on dew-point temperatures (i.e., DP = \textgreater{}MDB) are directly related to extremes of humidity ratio, which represent peak moisture loads from the weather. Extreme dew-point conditions may occur on days with moderate dry-bulb temperatures, resulting in high relative humidity. These values are especially useful for humidity control applications, such as desiccant cooling and dehumidification, cooling-based dehumidification, and fresh-air ventilation systems. The values are also used as a check point when analyzing the behavior of cooling systems at part-load conditions, particularly when such systems are used for humidity control as a secondary function. Humidity ratio values are calculated from the corresponding dew-point temperature and the standard pressure at the location's elevation.
+
+The enthalpy design conditions (i.e.~Enthalpy = \textgreater{} MDB) gives the annual enthalpy for the cooling season; this is used for calculating cooling loads caused by infiltration and/or ventilation into buildings. Enthalpy represents the total heat content of air (the sum of its sensible and latent energies). Cooling loads can be easily calculated knowing the conditions of both the outdoor ambient and the building's interior air.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/source-weather-data-formats.tex b/doc/auxiliary-programs/src/weather-converter-program/source-weather-data-formats.tex
new file mode 100644
index 00000000000..2a01731c393
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/source-weather-data-formats.tex
@@ -0,0 +1,201 @@
+\section{Source Weather Data Formats}\label{source-weather-data-formats}
+
+Source weather data for building energy simulation programs can be broken into two major classes: \emph{historical data} and \emph{typical weather years}. Historical data is just ``real'' data: usually measured (but sometimes modeled) data from a particular location for a given period of record. Typical years are ersatz years assembled to match the long term data from a particular location using a particular statistical measure. Typical data may also be ``real'' data but may not be a contiguous year - the data may be comprised of months from multiple years.
+
+The primary source for historical weather data is the U.S. National Climatic Data Center (NCDC) in Asheville, NC: http://www.ncdc.noaa.gov/. NCDC can provide hourly historical data for thousands of locations around the world. This data may not always be complete; data items or periods of record may be missing.
+
+\subsection{Data Set vs.~Data Format}\label{data-set-vs.data-format}
+
+In this document as well in many others, you will read about a certain ``data set'' and you will also read about data in a ``certain'' format - e.g., the TMY2 data set and the TMY2 data format. Simply stated, a data set refers to a set of data files developed around a set of procedures for selection and usually with a specific purpose for use. A data format is merely the identification of data elements in a data file. In the TMY2 example, the TMY2 data set was developed as described below and the format of the data is usually called a TMY2 format.
+
+Any data \emph{could} be put into a TMY2 format, but it wouldn't necessarily be selected using the same procedures as the TMY2 data set.
+
+\subsection{SAMSON Data Set/Format}\label{samson-data-setformat}
+
+A highly reliable source of historical data for U.S. locations is the Solar and Meteorological Surface Observational Network (SAMSON) data set assembled by the National Renewable Energy Laboratory (NREL) in Golden, CO: http://www.nrel.gov/. The SAMSON data set contains a 30 year (1961 to 1990) period of record for 239 locations and are available from the NCDC.
+
+SAMSON also describes a file format. Though no data from the SAMSON data set are available for download in EPW format, the weather conversion utility can read and process this file format.
+
+\subsection{TMY2 Data Set/Format}\label{tmy2-data-setformat}
+
+The TMY2 are data sets of hourly values of solar radiation and meteorological elements for a 1-year period. Their intended use is for computer simulations of solar energy conversion systems and building systems to facilitate performance comparisons of different system types, configurations, and locations in the United States and its territories. Because they represent typical rather than extreme conditions, they are not suited for designing systems to meet the worst-case conditions occurring at a location. The data are available from the National Renewable Energy Laboratory for download or on CD.
+
+TMY3 files have somewhat replaced TMY2 files but all TMY2 files are available for download from the website.
+
+\subsection{Solar and Wind Energy Resource Assessment (SWERA) Format}\label{solar-and-wind-energy-resource-assessment-swera-format}
+
+The Solar and Wind Energy Resource Assessment (SWERA) project, funded by the United Nations Environment Program, is developing high quality information on solar and wind energy resources in 14 developing countries. Currently typical year hourly data are available for 156 locations in Belize, Brazil, China, Cuba, El Salvador, Ethiopia, Ghana, Guatemala, Honduras, Kenya, Maldives, Nicaragua, and Sri Lanka. The data are available from the SWERA project web site. http://swera.unep.net/;
+
+The SWERA format is very similar to the TMY2 format except: WMO stations are used (6 character) in the header and 4 digit years have been adopted in the data lines.
+
+\subsection{WYEC2 Data Set/Format}\label{wyec2-data-setformat}
+
+Culminating in the early 1980s, ASHRAE published their ``Weather Year for Energy Calculations'' (WYEC) hourly weather files for 51 US and Canadian locations. These files were intended to support the then growing interest in computer simulation of energy use in buildings. In the late 1980s, a major revision was initiated - this included the addition of 26 Typical Meteorological Year (TMY) hourly weather files to the original WYEC data set and a number of improvements.
+
+The work of revising and improving the WYEC data base was performed by at the National Renewable Energy Laboratory (NREL) as part of the Solar Radiation Resource Assessment Program (SRRAP), during the period 1989 through 1993. Richard Perez, at the State University of New York at Albany -- Atmospheric Sciences Research Center provided a substantial contribution to this work. The resulting set of 77 revised and corrected hourly weather files are referred to as WYEC Version 2 or ``WYEC2'' data set.
+
+The WYEC2 format is used as the format for several other data sets. The WYEC2 data set, however, was not made available for download though, of course, those files can be read if desired with the EnergyPlus Weather Converter utility.
+
+\subsection{Canadian Weather for Energy Calculations (CWEC)}\label{canadian-weather-for-energy-calculations-cwec}
+
+Produced by Numerical Logics in collaboration with Environment Canada and the National Research Council of Canada, the CWEC were derived using a methodology similar to the TMY2 and TMY. CWEC hourly files represent weather conditions that result in approximately average heating and cooling loads in buildings. The National Energy Code of Canada requires the use of a CWEC file representative of a location when the performance path and customized design calculations are chosen as the means of building energy consumption compliance. The CWEC follow the ASHRAE WYEC2 format and were derived from the Canadian Energy and Engineering Data Sets (CWEEDS) of hourly weather information for Canada from the 1953-1995 period of record.
+
+The 80 CWEC files contain hourly weather observations representing an artificial one-year period specifically designed for building energy calculations. All 80 locations in the CWEC data set are available for download in EnergyPlus weather format.
+
+\subsection{International Weather for Energy Calculations (IWEC)}\label{international-weather-for-energy-calculations-iwec}
+
+The IWEC are the result of ASHRAE Research Project 1015 conducted by Numerical Logics and Bodycote Materials Testing Canada for ASHRAE Technical Committee 4.2 Weather Information. The IWEC data files are `typical' weather files suitable for use with building energy simulation programs for 227 locations outside the USA and Canada.
+
+The files are derived from up to 18 years of DATSAV3 hourly weather data originally archived at the U S National Climatic Data Center. The weather data is supplemented by solar radiation estimated on an hourly basis from earth-sun geometry and hourly weather elements, particularly cloud amount information. The IWEC CD-ROM is available from ASHRAE.
+
+The Department of Energy has licensed the IWEC data from ASHRAE. Our license with ASHRAE allows us to: ``Distribute versions of the individual IWEC files in converted format suitable for EnergyPlus (EPW). Make the EnergyPlus versions of the IWEC files available to users at no cost via this EnergyPlus web site.'' All 227 locations in the IWEC data set are available for download in EnergyPlus weather format.
+
+The IWEC source data is © 2001 American Society of Heating, Refrigerating and Air-Conditioning Engineers (ASHRAE), Inc., Atlanta, GA, USA. http://www.ashrae.org/ All rights reserved as noted in the License Agreement and Additional Conditions.
+
+IWEC also describes a data format, very similar to the TMY2 data format.
+
+\subsection{Typical Meteorological Year (TMY)}\label{typical-meteorological-year-tmy}
+
+Data for 230 locations in the USA plus four locations in Cuba, Marshall Islands, Palau, and Puerto Rico, derived from a 1948-1980 period of record. Many of the locations in the TMY data set were subsequently updated by the TMY2.
+
+Similar to the TMY2, the TMY are data sets of hourly values of solar radiation and meteorological elements for a 1-year period. Their intended use is for computer simulations of solar energy conversion systems and building systems to facilitate performance comparisons of different system types, configurations, and locations in the United States and its territories. Because they represent typical rather than extreme conditions, they are not suited for designing systems to meet the worst-case conditions occurring at a location. The data are available for purchase from the National Climatic Data Center.
+
+All TMY locations are available for download in EnergyPlus weather format.
+
+TMY also describes a data format.
+
+\subsection{California Climate Zones 2 (CTZ2)}\label{california-climate-zones-2-ctz2}
+
+Updated weather data for 16 California climate zones for use to demonstrate compliance with Title 24 with approved building energy simulation programs. All 16 CTZ2 weather files are available for download in EnergyPlus weather format. The original source data is available from the California Energy Commission. These source data files are described using the WYEC2 format.
+
+\subsection{Solar and Wind Energy Resource Assessment (SWERA)}\label{solar-and-wind-energy-resource-assessment-swera}
+
+The Solar and Wind Energy Resource Assessment (SWERA) project, funded by the United Nations Environment Program, is developing high quality information on solar and wind energy resources in 13 developing countries. Currently typical year hourly data are available for 48 locations in Belize, Cuba, El Salvador, Guatemala, Honduras, Maldives, Nicaragua, and Sri Lanka. The data are available from the SWERA project web site. SWERA plans to release new data for Brazil, Ethiopia, Ghana, Kenya, and Nepal over the coming few months. These source data files are described using the SWERA format.
+
+\subsection{Spanish Weather for Energy Calculations (SWEC)}\label{spanish-weather-for-energy-calculations-swec}
+
+Originally developed for use with Calener, a new program for building energy labelling in Spain, these weather files cover all 52 Spanish provincial capitals. Calener was developed by the Grupo de Termotecnia of the Escuela Superior de Ingeneiros in Seville for the Spanish Government. The weather files were synthetically generated using Climed (Portuguese software developed by Ricardo Aguiar) from mean monthly data coming from the Spanish Meteorological National Institute. These weather files were converted from the DOE-2 binary to EnergyPlus format and include constant wind speeds of 6.7 m/s.
+
+For more information on these weather files, contact: Profesor Luis Pérez-Lombard (\href{file:///E:/Docs4PDFs/lpl@tmt.us.es}{lpl@tmt.us.es}) Escuela Superior de Ingenieros
+
+\subsection{\texorpdfstring{Italian Climatic data collection ``Gianni De Giorgio'' (IGDG)}{Italian Climatic data collection Gianni De Giorgio (IGDG)}}\label{italian-climatic-data-collection-gianni-de-giorgio-igdg}
+
+Developed for use in simulating renewable energy technologies, this set of 66 weather files is based on a 1951-1970 period of record. The data were created by Professor Livio Mazzarella, Politecnico di Milano, and is named in honor of Gianni de Giorgio.
+
+\subsection{Chinese Typical Year Weather (CTYW)}\label{chinese-typical-year-weather-ctyw}
+
+Developed for use in simulating building heating and air conditioning loads and energy use, and for calculating renewable energy utilization, this set of 57 weather files is based on a 1982-1997 period of record with data obtained from the U. S. National Climatic Data Center. The data were created by Prof.~ZHANG Qingyuan of Tsukuba University Japan, in collaboration with Joe Huang of Lawrence Berkeley National Laboratory. The original typical year weather files are contained in: Zhang Qingyuan and Joe Huang. 2004. Chinese Typical Year Weather Data for Architectural Use (in Chinese). ISBN 7-111-14810-X. Beijing: China Machine Press. Available from: China Machine Press; No. 22 Baiwanzhuang Dajie; Beijing, CHINA 100037.
+
+The CTYW files are no longer available for download from the web site.
+
+\subsection{INETI Synthetic data for Portugal}\label{ineti-synthetic-data-for-portugal}
+
+Two weather files for Portugal developed by Ricardo Aguiar of Instituto Nacional de Engenharia, Tecnologia e Inovação (INETI). Synthetic data set based on spatially interpolation of public climatic data published by Instituto de Meteorologia 1951-80 combined with INETI owned data and other freely available data sources. INETI has granted DOE permission to distribute versions of the individual INETI files in converted format suitable for EnergyPlus (EPW) and make those files available to users at no cost via this EnergyPlus web site.
+
+The INETI synthetic data are © 2005 Instituto Nacional de Engenharia, Tecnologia e Inovação, Lisboa, Portugal. http://www.ineti.pt
+
+\subsection{ISHRAE India Weather Data Files (ISHRAE)}\label{ishrae-india-weather-data-files-ishrae}
+
+Developed for use in simulating building heating and air conditioning loads and energy use, and for calculating renewable energy utilization, this set of 58 weather files was developed by the Indian Society of Heating, Refrigerating, and Air-Conditioning Engineers (ISHRAE). The source data are Copyright 2005 ISHRAE. ISHRAE has made these data available to DOE under license for use at no cost to the EnergyPlus user community.
+
+\subsection{City University of Hong Kong (CUHK) Data Set}\label{city-university-of-hong-kong-cuhk-data-set}
+
+CityUHK-45007 -- WMO\#450070 Typical year file Hong Kong originally in IWEC format spreadsheet jointly developed by Dr TT Chow and ALS Chan of the City University of Hong Kong supported by a CERG grant from the Research Grants Council of the Hong Kong Special Administrative Region of China. Solar radiation measured from observatory station at 22.32N 114.17'E 65m above mean sea level.
+
+\subsection{Chinese Standard Weather Data (CSWD)}\label{chinese-standard-weather-data-cswd}
+
+Developed for use in simulating building heating and air conditioning loads and energy use, and for calculating renewable energy utilization, this set of 270 typical hourly data weather files. These data were developed by Dr.~Jiang Yi, Department of Building Science and Technology at Tsinghua University and China Meteorological Bureau. The source data include annual design data, typical year data, and extreme years for maximum enthalpy, and maximum and minimum temperature and solar radiation.
+
+China Meteorological Bureau, Climate Information Center, Climate Data Office and Tsinghua University, Department of Building Science and Technology. 2005. China Standard Weather Data for Analyzing Building Thermal Conditions, April 2005. Beijing: China Building Industry Publishing House, ISBN 7-112-07273-3 (13228). http://www.china-building.com.cn.
+
+\subsection{Kuwait Weather Data from Kuwait Institute for Scientific Research (KISR)}\label{kuwait-weather-data-from-kuwait-institute-for-scientific-research-kisr}
+
+Two weather files for Kuwait based on measured meteorological data for Kuwait International Airport and KISR's coastal weather station. Provided by KISR in spreadsheet format.
+
+\subsection{Egyptian Weather for Energy Calculations (EWEC)}\label{egyptian-weather-for-energy-calculations-ewec}
+
+Developed for standards development and energy simulation by Joe Huang from data provided by National Climatic Data Center for periods of record from 12 to 21 years, all ending in 2003. Joe Huang and Associates, Moraga, California, USA.
+
+\subsection{Israel weather data (MSI)}\label{israel-weather-data-msi}
+
+Weather data for Israel locations developed by Faculty of Civil and Environmental Engineering, Technion - Israel Institute of Technology, Haifa, Israel, from data provided by the Israel Meteorological Service.
+
+\subsection{Representative Meteorological Year (RMY) Australia Climatic Data}\label{representative-meteorological-year-rmy-australia-climatic-data}
+
+RMY Australia Representative Meteorological Year Climate Files Developed for the Australia Greenhouse Office for use in complying with Building Code of Australia. These data are licensed through ACADS BSG Ltd for use by EnergyPlus users. For use in any other formats, users must contact ACADS BSG Ltd for licensing information.
+
+The RMY data are © 2006 Commonwealth of Australia, Department of the Environment and Water Resources, Australia Greenhouse Office, Canberra, ACT, Australia. \href{https://web.archive.org/web/20070608213812/http://www.greenhouse.gov.au/buildings/code.html}{www.greenhouse.gov.au/buildings/code.html} (URL has since been removed, so replaced with a link on The Internet Archive from 2007.) All intellectual property rights reserved.
+
+\subsection{Iranian Typical Meteorological Year (ITMY)}\label{iranian-typical-meteorological-year-itmy}
+
+Typical year weather files have been created for Tehran from weather data for 1992 through 2003 published by the Islamic Republic of Iran Meteorological Organization (IRIMO) for Tehran Mehrabad. Developed for standards development and energy simulation by Joe Huang, White Box Technologies.
+
+\subsection{New Zealand National Institute of Water \& Atmospheric Research Ltd (NIWA)}\label{new-zealand-national-institute-of-water-atmospheric-research-ltd-niwa}
+
+The New Zealand Energy Efficiency and Conservation Authority (EECA) has developed a Home Energy Rating Scheme (HERS) for New Zealand households based on software simulation of energy loss and demand. The software requires hourly data to represent the different climates zones around New Zealand, especially for larger population centres. These climate data consist of hourly records for an artificial year created from twelve representative months.
+
+Liley, J Ben, Hisako Shiona, James Sturman, David S Wratt. 2007. Typical Meteorological Years for the New Zealand Home Energy Rating Scheme. Prepared for the Energy Efficiency and Conservation Authority. NIWA Client Report: LAU2007- 02-JBL. NIWA, Omakau, New Zealand.
+
+\subsection{Chartered Institution of Building Services Engineers (CIBSE)}\label{chartered-institution-of-building-services-engineers-cibse}
+
+The CIBSE, in association with the (UK) Met Office has produced `Test Reference Years' and `Design Summer Years' for 14 UK locations for use with building energy simulation software. The data sets are available in various formats, including EnergyPlus/ESP-r. These data are NOT available on the EnergyPlus web site. For further details, see:
+
+\href{file:///E:/Docs4PDFs/www.cibse.org/index.cfm\%3fgo\%20=\%20publications.view\&PubID\%20=\%20332\&S1\%20=\%20y\&L1\%20=\%200\&L2\%20=\%200}{www.cibse.org/index.cfm?go = publications.view\&PubID = 332\&S1 = y\&L1 = 0\&L2 = 0}
+
+\subsection{Meteonorm Data}\label{meteonorm-data}
+
+Meteonorm software can be used when there is no measured data near the location for the simulation. Meteonorm extrapolates hourly data from statistical data for a location. Where statistical data aren't available, Meteonorm interpolates from other nearby sites. Generally a statistical approach is a last resort -- weather files generated from statistics will not demonstrate the normal hour-to-hour and day-to-day variability seen in measured data. Meteonorm version 6 will directly write EPW files.
+
+\subsection{Other Formats}\label{other-formats}
+
+The data sets and formats described above are some of the newest formats available for use with building simulation programs. Source data comes in various formats. Typically the files are ASCII, but the data items, units, item location, and record length vary from format to format. NCDC can provide historical data in a variety of formats: TD-3280, TD-3510, TD-9950 (DATSAV2), TD-9956 (DATSAV3) and TD-1440 (CD144). The EnergyPlus weather processor cannot process any of the types directly.
+
+% table 18
+{\scriptsize
+\begin{longtable}[c]{p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}}
+\caption{Summary of Downloadable Weather Data by Type \label{table:summary-of-downloadable-weather-data-by-type}} \tabularnewline
+\toprule 
+Source & \multicolumn{8}{l}{WMO Region} &  \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Summary of Downloadable Weather Data by Type} \tabularnewline
+\toprule 
+Source & \multicolumn{8}{l}{WMO Region} &  \tabularnewline
+\midrule
+\endhead
+
+ & \multicolumn{3}{l}{North and Central America} &  &  &  &  &  &  \tabularnewline
+ & USA & Canada & Central America & Africa & Asia & South America & Southwest Pacific & Europe & Total \tabularnewline
+ETMY &  &  &  & 11 &  &  &  &  & 11 \tabularnewline
+IGDG &  &  &  &  &  &  &  & 66 & 66 \tabularnewline
+IMGW &  &  &  &  &  &  &  & 61 & 61 \tabularnewline
+INETI &  &  &  &  &  &  &  & 2 & 2 \tabularnewline
+ISHRAE &  &  &  &  & 58 &  &  &  & 58 \tabularnewline
+ITMY &  &  &  &  & 1 &  &  &  & 1 \tabularnewline
+IWEC &  &  & 5 & 12 & 49 & 19 & 20 & 122 & 227 \tabularnewline
+KISR &  &  &  &  & 2 &  &  &  & 2 \tabularnewline
+Los Alamos TMY2 & 1 &  &  &  &  &  &  &  & 1 \tabularnewline
+MSI &  &  &  &  &  &  &  & 4 & 4 \tabularnewline
+NIWA &  &  &  &  &  &  & 16 &  & 16 \tabularnewline
+RMY &  &  &  &  &  &  & 80 &  & 80 \tabularnewline
+SWEC &  &  &  & 2 &  &  &  & 50 & 52 \tabularnewline
+SWERA &  &  & 37 & 33 & 66 & 20 &  &  & 156 \tabularnewline
+TMY & 229 &  & 1 &  &  &  & 4 &  & 234 \tabularnewline
+TMY2 & 235 &  & 1 &  &  &  & 1 &  & 237 \tabularnewline
+TMY3 & 1011 &  & 7 &  &  &  & 2 &  & 1020 \tabularnewline
+Totals & 1476 & 0 & 51 & 58 & 176 & 39 & 123 & 305 &  \tabularnewline
+\bottomrule
+\end{longtable}}
+
+One other format worth mentioning is TRY. TRY is ``test reference year'' data that did not include solar radiation data. ``Test Reference Year'' is a term that usually denotes selection of a specific year of ``real'' data based on some statistical procedure. The original TRY data (TD-9706) was based on an ASHRAE procedure to select the data from a ``period of record''. ``The principle of the selection is to eliminate years in the period of record containing months with extremely high or low mean temperatures until only one year remains.'' The weather conversion utility cannot process data in ``TRY'' format. However, many organizations develop data for reference year data (e.g.~European TRY, Moisture Reference Data).
+
+\subsection{Custom Format}\label{custom-format}
+
+Using a ``definitions'' file (see Description of ``Def'' input file), the weather converter can process a wide range of data formats. In the table above, both the GDG and CTYW weather data was processed by a custom format approach.
+
+\subsection{Solar Data}\label{solar-data}
+
+Source weather data files may or may not contain solar data. All of the files that can be processed by the EnergyPlus Weather conversion utility contain solar data. The weather processor will transfer this data to the EPW weather file and the EnergyPlus simulation program will use it.
+
+Historical weather data files in CD144 format do not contain solar data nor is such data generally available for a specific location and time period. In this case, ersatz solar data must be generated from cloud cover and other data using sky models and regression formulas. Currently, neither the Weather Conversion utility nor the EnergyPlus program synthesizes this data. However, the weather conversion utility can use any two of the commonly recorded data (i.e.~two of Global Horizontal Radiation, Horizontal Diffuse Radiation and Direct Normal (or Direct Horizontal) Radiation to calculate the EnergyPlus primary solar data of Direct Normal and Horizontal Diffuse Radiation values).
diff --git a/doc/auxiliary-programs/src/weather-converter-program/using-the-weather-converter.tex b/doc/auxiliary-programs/src/weather-converter-program/using-the-weather-converter.tex
new file mode 100644
index 00000000000..550379a7129
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/using-the-weather-converter.tex
@@ -0,0 +1,194 @@
+\section{Using the Weather Converter}\label{using-the-weather-converter}
+
+We developed a utility for the E/E format to read standard weather service file types such as SAMSON and newer `typical year' weather files such as TMY2, WYEC2, and IWEC. The utility also reads ESP-r (CLM format), DOE-2 (fmt format), BLAST (Ascii format) files and other files.
+
+The utility translates and extends typical weather data into the E/E format. The processor makes the calculations necessary for supplying data (when data is missing) and calculates the Horizontal Infrared Radiation Intensity values-not typically currently an observed value reported by the meteorological offices through the world. The utility also prepares an statistical summary of the weather data set as part of the processing. An additional ``output format'' from the utility is a comma-delimited file that can easily be imported into a spreadsheet program such as Excelâ„¢ for further user perusal, charting and/or editing.
+
+The utility consists of two parts: a user interface that executes on standard Wintel systems and a DLL that does the work of the processing. The DLL interface is described in a later section for those developers who might wish to access it directly.
+
+The user front end is a simple to use program with standard graphical user interface menus. It is executed from the Start Menu programs using the specific folder where the EnergyPlus program was installed. (e.g., Start Menu -\textgreater{} EnergyPlus \textless{}version\textgreater{} -\textgreater{} WeatherConverter). For convenience, it automatically opens with the ``convert'' option.
+
+EP-Launch can also be used to run the weather utility program. Weather is one of the options on the Utilities tab in EP-Launch. See the section on EP-Launch in this document for more information on how to use EP-Launch with the weather utility program.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image001.jpg}
+\caption{Main menu screen of the Weather Converter Utility \protect \label{fig:main-menu-screen-of-the-weather-converter}}
+\end{figure}
+
+\subsection{File Menu}\label{file-menu-001}
+
+The file menu has four options:
+
+\subsubsection{Fix Out of Range Data}\label{fix-out-of-range-data}
+
+This is a toggle option that once selected is saved in the registry with other options (for example, screen size) for the program. As shown in the IDD type description of the Weather Data, there are minimum and maximum values for several of the fields. The weather converter program can ignore these (and just report them) or it can try to fix them with appropriate values. If the option is ``checked'', then the processor will try to fix the data; if it is blank, the processor will not fix the data though it will report any out of range data that it finds.
+
+\subsubsection{Select Delta DB Trigger}\label{select-delta-db-trigger}
+
+Depending on the quality control and accuracy of the weather data collection, time period (usually hour to hour) changes in some data values may make the data suspect for that time period. This selection brings up the screen shown below and will allow the user some control over the actual value reporting. Note that this data is not ``fixed'', merely reported by the program in the audit output file.
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image002.jpg}
+\caption{Delta DB Trigger Selection \protect \label{fig:delta-db-trigger-selection}}
+\end{figure}
+
+Though only one ``trigger'' value is selected from this screen, consecutive values of dry-bulb temperature, dew-point temperature and wind speed are reported using appropriate calculated values. Both dew-point and wind speed use a calculated value based on mean of their values over the entire data period and standard deviation from that mean, heuristically derived.
+
+An excerpt from the audit file is illustrative:
+
+Average Delta DB Change = 0.78°C ; Std Dev = 0.83°C
+
+Average Delta DP Change = 0.68°C ; Std Dev = 0.78°C
+
+Average Delta Relative Humidity Change = 4.02\% ; Std Dev = 4.22\%
+
+Average Delta Wind Speed Change = 0.91m/s ; Std Dev = 0.88m/s
+
+Hourly Dry Bulb temperature change trigger = minimum of 12.13°C and 10.°C
+
+\begin{lstlisting}
+ 12.13°C = calculated trigger based on mean change in dry-bulb temperature and standard deviation shown above
+\end{lstlisting}
+
+\begin{lstlisting}
+ 10.°C = trigger set by user
+\end{lstlisting}
+
+Here the calculated DB trigger would be 12.13°C, but the user chosen trigger is 10°C. Changes \textgreater{} = 10°C will be reported.
+
+\begin{itemize}
+\item
+  Delta DB/DP Range Triggered for Apr 30
+\item
+  Change in DB = 11.60°C, Hour = 14
+\end{itemize}
+
+Such detail allows the user to hand edit the incoming data, if desired.
+
+\subsubsection{Delete File}\label{delete-file}
+
+You may use this menu option to browse your computer and delete files.
+
+\subsubsection{Input Folder = \textgreater{} Output Folder}\label{input-folder-output-folder}
+
+Choosing this option (a check will show and will carry over from one use to the next) sets the output folder for saving files to be the same as the input folder where the original files are located.
+
+\subsubsection{Exit}\label{exit}
+
+This choice exits the program.
+
+\subsection{Converting Data}\label{converting-data}
+
+This screen is automatically shown when you start the program - it will allow you to select raw data for processing, change the default type (based on file extension), select the kind of conversion you want, select where and what name to store for the processed data, and process the data. An ``almost'' completed screen shows:
+
+\begin{figure}[hbtp] % fig 3
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image003.jpg}
+\caption{Convert Data Screen selections \protect \label{fig:convert-data-screen-selections}}
+\end{figure}
+
+The screen is navigated by choosing the following buttons on the left portion of the screen. Interpretation from the program is shown in the status boxes on the right portion of the screen.
+
+\subsubsection{Select File to Convert}\label{select-file-to-convert}
+
+Selecting this command button brings up a common dialog interface that allows you to select a file for conversion from a specific set of default file extensions. These are shown in the following table. Note that you can (mostly) override the default file extension by the use of a simple DEF file and change the input file type.
+
+% table 2
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Input File Extensions with implied Data types \label{table:input-file-extensions-with-implied-data-types}} \tabularnewline
+\toprule 
+File Extension & Implicit Data File Type \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Input File Extensions with implied Data types} \tabularnewline
+\toprule 
+File Extension & Implicit Data File Type \tabularnewline
+\midrule
+\endhead
+
+LST & Processing List of Files \tabularnewline
+< any >  or CST & Custom - must have "def" file as specified below \tabularnewline
+EPW & EnergyPlus E/E \tabularnewline
+CSV & Comma Delimited File (EPW Format) Note: special EnergyPlus CSV format. For other CSV files use the DEF file and describe the format. \tabularnewline
+TM2 & TMY2 \tabularnewline
+TMY & TMY \tabularnewline
+IWC & IWEC \tabularnewline
+WY2 & WYEC2 \tabularnewline
+DAT & SAMSON \tabularnewline
+FMT & DOE-2 Formatted File \tabularnewline
+CLM & ESP-r Climate Formatted File \tabularnewline
+ASC & BLAST ASCII \tabularnewline
+SWE & SWERA \tabularnewline
+WEA & Ecotect WEA file \tabularnewline
+\bottomrule
+\end{longtable}
+
+Of course, the ``all files'' (*.*) may be used as well. If the file selected is not one of the above types, you will be cautioned to use the ``override default type'' button to select the correct type before proceeding. Most of the data file types are described in other publications and won't be described in detail here.
+
+Note on the input CSV format: It is the EPW CSV format. The CSV format must mirror the output CSV format very closely. The processor expects a Location header record and the headers for the data fields as a minimum (as well as the data that supports those header fields). If you have a differently formatted file, possible comma delimited, investigate the ``custom'' format option.
+
+The LST data type allows you to specify a list of files to be ``batch processed''. The format of this file is very simple (however, the default extensions from the preceding table \textbf{must} be used \textbf{or} you must include a ``def'' file - see below for details).
+
+Each line of the LST file can have a columnar structure as shown in the following table or can have the input file separated from the output file with a TAB character.
+
+% table 3
+\begin{longtable}[c]{p{1.52in}p{4.47in}}
+\caption{LST File Structure \label{table:lst-file-structure}} \tabularnewline
+\toprule 
+Columns & Contents \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{LST File Structure} \tabularnewline
+\toprule 
+Columns & Contents \tabularnewline
+\midrule
+\endhead
+
+1-45 & Name of Input File to be Processed \tabularnewline
+46-105 (or follow the first name with a \{TAB\}) & Output File with: EPW - same as output type "EPW" CSV - same as output type "CSV" Both - same as output type "both" Rpt - same as output type "rpt" \tabularnewline
+106-end (or follow the second name with a \{TAB\}) & URL for KML output \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Definitions File}\label{definitions-file}
+
+An auxiliary file, the Definitions File (extension .def) can be used to specify additional or replacement characteristics for the incoming data. This file is fully described in the section ``Definitions File \& Custom File Processing'' later in this document.
+
+\subsubsection{Override Default Type}\label{override-default-type}
+
+This button is used as described above to select the correct data type for a file that might have one of the standard ``default'' extensions but may, in fact, be a data file of an entirely different type. For example, the BLAST ASCII files as they exist on the BLAST CD have extensions of .dat - our default type for the SAMSON data. You must select the proper data type for your data or the processor probably won't work anywhere near what you expect.
+
+\subsubsection{Select Output Format}\label{select-output-format}
+
+You may select from four options of output format:
+
+\begin{itemize}
+\item
+  EPW Format -- both an epw file and a statistical report file are produced
+\item
+  CSV Format - both a csv file and a statistical report file are produced
+\item
+  Both EPW and CSV - epw, csv, and statistical report files are produced
+\item
+  Rpt only - only a statistical report file is produced (output extension is ``stat'')
+\end{itemize}
+
+Note that the CSV file is very similar to the EPW format file but is ready to be imported into a spreadsheet program such as Excelâ„¢ and has some additional ``header'' records in front of each EPW style header record
+
+\subsubsection{Save File As\ldots{}}\label{save-file-as}
+
+This button allows you to select the location to save your file set from the output format selection. The utility automatically places a ``data type'' extension on the file name to show its original data file type.
+
+Note on Save As\ldots{} Since you select the ``save as'' file name from a dialog, the processor DOES NOT warn you of overwriting previous files of the same name. In addition, if you have previously saved several types (e.g.~EPW and CSV) but this time only save the RPT - it DOES NOT create new of the others nor does it delete the previous ones.
+
+\subsubsection{Convert File}\label{convert-file}
+
+Pressing this button causes the processing of the data to proceed. If you choose a ``.lst'' input format, you will see messages as each once is completed and/or has errors. If you choose a single data file, you will see a similar message box once the processing is done (or has terminated due to errors).
+
+\subsection{Help}\label{help}
+
+No online help is available. This brings up an ``about'' box for the program.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/weather-data-availability.tex b/doc/auxiliary-programs/src/weather-converter-program/weather-data-availability.tex
new file mode 100644
index 00000000000..16bb1a961f3
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/weather-data-availability.tex
@@ -0,0 +1,65 @@
+\section{Weather Data Availability}\label{weather-data-availability}
+
+Typically, acquisition of weather data has been a user's burden. Though this will remain the case in many instances for EnergyPlus users, the EnergyPlus team has been successful in making a wealth of US, Canadian and International data available to our users. To summarize, the weather data for 2092 locations is available at the EnergyPlus web site: \href{http://www.energyplus.gov}{www.energyplus.gov}
+
+The details are shown in Table~\ref{table:summary-of-downloadable-weather-data-by-type}. Summary of Downloadable Weather Data by Type. This data has been selected with the energy simulation user in mind. All the data (as well as the statistical reports - described later in this document) are downloadable for individual locations.
+
+% table 1
+\begin{longtable}[c]{>{\raggedright}p{3in}llll}
+
+\caption{Comparison of E/E with ESP-r/DOE-2/BLAST Weather Data Formats \label{table:comparison-of-ee-with-esp-rdoe-2blast-weather}} \tabularnewline
+\toprule 
+Data Element & DOE-2 & BLAST & ESP-r & E/E \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Comparison of E/E with ESP-r/DOE-2/BLAST Weather Data Formats} \tabularnewline
+\toprule 
+Data Element & DOE-2 & BLAST & ESP-r & E/E \tabularnewline
+\midrule
+\endhead
+
+Location (name, latitude, longitude, elevation, time zone) & X & X & X & X \tabularnewline
+Data source &  &  &  & X \tabularnewline
+Commentary &  &  & X & X \tabularnewline
+Design conditions &  &  &  & X \tabularnewline
+Typical/extreme periods &  &  & X & X \tabularnewline
+Data periods &  &  &  & X \tabularnewline
+Holiday/Daylight Saving &  & X &  & X \tabularnewline
+Solar Angles/Equation of Time Hours &  & X &  &  \tabularnewline
+Degree Days &  & X &  & X \tabularnewline
+Year & X & X & X & X \tabularnewline
+Month & X & X & X & X \tabularnewline
+Day & X & X & X & X \tabularnewline
+Hour & X & X & X & X \tabularnewline
+Minute &  &  &  & X \tabularnewline
+Data source and uncertainty flags &  &  &  & X \tabularnewline
+Dry bulb temperature & X & X & X & X \tabularnewline
+Wet bulb temperature & X & X &  &  \tabularnewline
+Dew point temperature & X &  &  & X \tabularnewline
+Atmospheric station pressure & X & X &  & X \tabularnewline
+Humidity ratio & X & X &  &  \tabularnewline
+Relative humidity &  &  & X & X \tabularnewline
+Enthalpy & X &  &  &  \tabularnewline
+Density & X &  &  &  \tabularnewline
+Wind Speed & X & X & X & X \tabularnewline
+Wind Direction & X & X & X & X \tabularnewline
+Infrared Sky Temperature &  & X &  & X \tabularnewline
+Solar Radiation (global, normal, diffuse) & X & X & X & X \tabularnewline
+Illuminance (global, normal, diffuse) &  &  &  & X \tabularnewline
+Sky cover (cloud amount) & X &  &  & X \tabularnewline
+Opaque sky cover &  &  &  & X \tabularnewline
+Visibility &  &  &  & X \tabularnewline
+Ceiling height &  &  &  & X \tabularnewline
+Clearness (monthly) & X &  &  &  \tabularnewline
+"Undisturbed" Ground temperatures (monthly) & X &  &  & X \tabularnewline
+Present weather observation and codes (rain, snow) &  & X &  & X \tabularnewline
+Precipitable water &  &  &  & X \tabularnewline
+Aerosol optical depth &  &  &  & X \tabularnewline
+Snow depth &  &  &  & X \tabularnewline
+Days since last snowfall &  &  &  & X \tabularnewline
+Albedo &  &  &  & X \tabularnewline
+Liquid Precipitation Depth &  &  &  & X \tabularnewline
+Liquid Precipitation Quantity &  &  &  & X \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/auxiliary-programs/src/weather-converter-program/weather-format-for-simulation-programs.tex b/doc/auxiliary-programs/src/weather-converter-program/weather-format-for-simulation-programs.tex
new file mode 100644
index 00000000000..e8b6bab6624
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/weather-format-for-simulation-programs.tex
@@ -0,0 +1,17 @@
+\section{Weather Format for Simulation Programs}\label{weather-format-for-simulation-programs}
+
+For these reasons, we developed a generalized weather data format for use with two major simulation programs-ESP-r and EnergyPlus (Crawley et al. 1999). All the data are in SI units. The format is simple, text-based with comma-separated data. It is based on the data available within the TMY2 weather format but has been rearranged to facilitate visual inspection of the data. The TMY2 data are a strict, position-specific format-filling missing data with nines and zero values with zeroes. The new weather data format contains commas to facilitate data reading and analysis with spreadsheet programs. By eliminating redundant `fill' values, the size of each file is only slightly larger than the original TMY2 format. Details about the TMY2 format can be found in the TMY2 User's manual (see references at the end of this section).
+
+The traditional distribution of data source and uncertainty flags within the raw data fields carries with it not only the need for many field separators, it obfuscates the relationships between non-numerical data. In a set of minute data, which could easily require hundreds of thousands of records, the space penalty is considerable. In the E/E file format, all data source and uncertainty fields have been clumped together as a single field immediately following the day and time stamp. For applications where uncertainty is not an issue such data can be easily ignored. When it is important, a single text field is conceptually and computationally easy to parse.
+
+Another difference between the EnergyPlus/ESP-r (E/E) format and TMY2 is the addition of two new data fields-minute and infrared sky. The minute field facilitates use of data observed at intervals of less than one hour such as measured data from a research study of energy efficiency for a particular building. This will allow easier and more accurate calibration of a simulation model to measured data than possible in the past. The infrared sky field allows the programs to calculate the effective sky temperature for re-radiation during nighttime.
+
+The last difference is that a full year of data (such as 8760 hours) is not required-subsets of years are acceptable. Which periods are covered by the data is described in the files. Periods of typical weather patterns based on analysis of the data are also included within the format. A side-by-side comparison of data included in the E/E weather format with data previously used by ESP-r, DOE-2, and BLAST is shown in Table~\ref{table:comparison-of-ee-with-esp-rdoe-2blast-weather}. A deficiency noted within ESP-r for example is the lack of correcting air volumes for elevation change-many of the users of ESP-r are in relatively low elevations. For DOE-2 and BLAST, neither program used illumination data in daylighting calculations or infrared sky temperatures-it was always recalculated at time of use.
+
+By including the uncertainty and data source information found in TMY2, users now can evaluate the potential impact of weather variability on the performance of the building.
+
+McDonald and Strachan (1998) are introducing uncertainty analysis into ESP-r.
+
+We use the EnergyPlus data dictionary format to describe the E/E weather data set. (See the end of this document). Each line in the format is preceded by a keyword such as LOCATION, DESIGN CONDITIONS, followed by a list of variables beginning either with A or N and a number. A stands for alphanumeric; N for numeric. The number following A/N is the sequence of that number in the keyword list. Commas separate data. (Refer to the IDD Conventions document in ``\href{InputOutputReference.pdf}{Input Output Reference}'' for further explanation of the format). The header information consists of eight lines (keywords): LOCATION, DESIGN CONDITIONS, TYPICAL/EXTREME PERIODS, GROUND TEMPERATURES, HOLIDAYS/DAYLIGHT SAVINGS, COMMENTS 1, COMMENTS 2, and DATA PERIODS. This is followed by the time step data.
+
+The first eight lines or header within each E/E weather file define basic location information such as longitude, latitude, time zone, elevation, annual design conditions, monthly average ground temperatures, typical and extreme periods, holidays/daylight saving periods, and data periods included. There is also space for users to document any special features or information about the file such as sources of data.
diff --git a/doc/auxiliary-programs/src/weather-converter-program/web-resources.tex b/doc/auxiliary-programs/src/weather-converter-program/web-resources.tex
new file mode 100644
index 00000000000..ea24abd3241
--- /dev/null
+++ b/doc/auxiliary-programs/src/weather-converter-program/web-resources.tex
@@ -0,0 +1,19 @@
+\section{Web Resources}\label{web-resources}
+
+Building Energy Tools Directory, a directory of information on 340+ energy tools from around the world.
+
+http://www.energytoolsdirectory.gov/
+
+Energy Systems Research Unit, University of Strathclyde, authors of ESP-r, up-to-date information on ESP-r and other energy systems research and software development.
+
+http://www.strath.ac.uk/Departments/ESRU
+
+EnergyPlus, up-to-date information on the current status of EnergyPlus and working with the team, and documentation such as input data structure, output data structure, and licensing opportunities. Additional weather files may be posted here as well.
+
+http://www.energyplus.gov
+
+Description of the SWERA project. http://swera.unep.net/swera/
+
+Weather Analytics (\href{http://www.wxaglobal.com}{www.wxaglobal.com}) - Site specific weather files in EnergyPlus format based on the latest 30 years of hourly data are now available from the private sector company Weather Analytics for any official weather station or over 600,000 35-km grid tiles across the globe. These files are built by integrating hourly weather station observations and the new NOAA reanalysis data sets. Both Typical Meteorological Year (TMY) files and individual, Actual Meteorological Year (AMY) files are available as well as files constructed from the previous 12 months.
+
+Meteonorm (\href{http://www.meteonorm.com}{www.meteonorm.com}) - Files for specific locations can be purchased in EnergyPlus format from Meteonorm company. Meteonorm extrapolates hourly data from statistical data for a location. Where statistical data aren't available, Meteonorm interpolates from other nearby sites. Generally a statistical approach is a last resort--weather files generated from statistics will not demonstrate the normal hour-to-hour and day-to-day variability seen in measured data.
diff --git a/doc/ems-application-guide/CMakeLists.txt b/doc/ems-application-guide/CMakeLists.txt
new file mode 100644
index 00000000000..e75d9c28fe8
--- /dev/null
+++ b/doc/ems-application-guide/CMakeLists.txt
@@ -0,0 +1,97 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/ems-application-guide.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/application-guide-for-ems.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/application-guide-for-ems/background.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/application-guide-for-ems/organization.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/energyplus-runtime-language.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/energyplus-runtime-language/statement-keywords.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/energyplus-runtime-language/variables.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/energyplus-runtime-language/expressions.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/energyplus-runtime-language/built-in-functions.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/internal-variables.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/internal-variables/zone-geometry.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/internal-variables/internal-gains.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/internal-variables/hvac-systems.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/internal-variables/on-site-electricity-production.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/internal-variables/sizing.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-sensors.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-sensors/variable-types.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-sensors/schedules.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-actuators.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-actuators/hvac-systems-001.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-actuators/thermal-envelope.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-actuators/air-movement.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-actuators/internal-gains-and-exterior-lights.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-actuators/on-site-electricity-production-001.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-actuators/refrigeration.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-actuators/general.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-actuators/sizing-001.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/begin-new-environment.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/after-new-environment-warmup-is-complete.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/begin-timestep-before-predictor.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/after-predictor-before-hvac-managers.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/after-predictor-after-hvac-managers.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/inside-hvac-system-iteration-loop.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/end-of-zone-timestep-before-reporting.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/end-of-zone-timestep-after-reporting.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/end-of-system-timestep-before-hvac-reporting.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/end-of-system-timestep-after-hvac-reporting.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/end-of-zone-sizing.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/end-of-system-sizing.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/after-component-model-input-has-been-read-in.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-calling-points/user-defined-component-model.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/user-defined-component-models.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/user-defined-component-models/common-characteristics.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/user-defined-component-models/zone-forced-air-unit.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/user-defined-component-models/air-terminal-unit.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/user-defined-component-models/air-coil.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/user-defined-component-models/plant-component.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-1-whole-building-average-zone-air.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-2-traditional-setpoint.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-3-hygro-thermal-window-opening.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-4-halt-program-based-on-constraint.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-5-computed-schedule.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-6-window-shade-control.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-7-constant-volume-purchased-air.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-8-system-sizing-with-discrete-package.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-9-demand-management.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-10-plant-loop-override-control.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-11-performance-curve-result-override.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-12-variable-refrigerant-flow-system.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/ems-examples/example-13-surface-construction-actuator-for.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/debugging-ems-programs.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/debugging-ems-programs/err-file.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/debugging-ems-programs/edd-file.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/debugging-ems-programs/line-trace.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/src/debugging-ems-programs/debugging-strategies.tex
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/../title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/media/image003.jpg
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/media/image004.jpg
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/media/image005.jpg
+  ${CMAKE_SOURCE_DIR}/doc/ems-application-guide/media/image011.jpg
+) 
+
+SET( SOURCE_FILENAME "ems-application-guide" )
+SET( OUTPUT_FILENAME "EMSApplicationGuide" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/ems-application-guide/ems-application-guide.tex b/doc/ems-application-guide/ems-application-guide.tex
new file mode 100644
index 00000000000..5aae1575a47
--- /dev/null
+++ b/doc/ems-application-guide/ems-application-guide.tex
@@ -0,0 +1,150 @@
+\input{../header}
+
+\title{Application Guide for EMS}
+
+\hypersetup{unicode=true,
+            pdftitle={Application Guide for EMS},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/application-guide-for-ems}
+
+\input{src/application-guide-for-ems/background}
+
+\input{src/application-guide-for-ems/organization}
+
+\input{src/energyplus-runtime-language}
+
+\input{src/energyplus-runtime-language/statement-keywords}
+
+\input{src/energyplus-runtime-language/variables}
+
+\input{src/energyplus-runtime-language/expressions}
+
+\input{src/energyplus-runtime-language/built-in-functions}
+
+\input{src/internal-variables}
+
+\input{src/internal-variables/zone-geometry}
+
+\input{src/internal-variables/internal-gains}
+
+\input{src/internal-variables/hvac-systems}
+
+\input{src/internal-variables/on-site-electricity-production}
+
+\input{src/internal-variables/sizing}
+
+\input{src/ems-sensors}
+
+\input{src/ems-sensors/variable-types}
+
+\input{src/ems-sensors/schedules}
+
+\input{src/ems-actuators}
+
+\input{src/ems-actuators/hvac-systems-001}
+
+\input{src/ems-actuators/thermal-envelope}
+
+\input{src/ems-actuators/air-movement}
+
+\input{src/ems-actuators/internal-gains-and-exterior-lights}
+
+\input{src/ems-actuators/on-site-electricity-production-001}
+
+\input{src/ems-actuators/refrigeration}
+
+\input{src/ems-actuators/general}
+
+\input{src/ems-actuators/sizing-001}
+
+\input{src/ems-calling-points}
+
+\input{src/ems-calling-points/begin-new-environment}
+
+\input{src/ems-calling-points/after-new-environment-warmup-is-complete}
+
+\input{src/ems-calling-points/begin-timestep-before-predictor}
+
+\input{src/ems-calling-points/after-predictor-before-hvac-managers}
+
+\input{src/ems-calling-points/after-predictor-after-hvac-managers}
+
+\input{src/ems-calling-points/inside-hvac-system-iteration-loop}
+
+\input{src/ems-calling-points/end-of-zone-timestep-before-reporting}
+
+\input{src/ems-calling-points/end-of-zone-timestep-after-reporting}
+
+\input{src/ems-calling-points/end-of-system-timestep-before-hvac-reporting}
+
+\input{src/ems-calling-points/end-of-system-timestep-after-hvac-reporting}
+
+\input{src/ems-calling-points/end-of-zone-sizing}
+
+\input{src/ems-calling-points/end-of-system-sizing}
+
+\input{src/ems-calling-points/after-component-model-input-has-been-read-in}
+
+\input{src/ems-calling-points/user-defined-component-model}
+
+\input{src/user-defined-component-models}
+
+\input{src/user-defined-component-models/common-characteristics}
+
+\input{src/user-defined-component-models/zone-forced-air-unit}
+
+\input{src/user-defined-component-models/air-terminal-unit}
+
+\input{src/user-defined-component-models/air-coil}
+
+\input{src/user-defined-component-models/plant-component}
+
+\input{src/ems-examples}
+
+\input{src/ems-examples/example-1-whole-building-average-zone-air}
+
+\input{src/ems-examples/example-2-traditional-setpoint}
+
+\input{src/ems-examples/example-3-hygro-thermal-window-opening}
+
+\input{src/ems-examples/example-4-halt-program-based-on-constraint}
+
+\input{src/ems-examples/example-5-computed-schedule}
+
+\input{src/ems-examples/example-6-window-shade-control}
+
+\input{src/ems-examples/example-7-constant-volume-purchased-air}
+
+\input{src/ems-examples/example-8-system-sizing-with-discrete-package}
+
+\input{src/ems-examples/example-9-demand-management}
+
+\input{src/ems-examples/example-10-plant-loop-override-control}
+
+\input{src/ems-examples/example-11-performance-curve-result-override}
+
+\input{src/ems-examples/example-12-variable-refrigerant-flow-system}
+
+\input{src/ems-examples/example-13-surface-construction-actuator-for}
+
+\input{src/debugging-ems-programs}
+
+\input{src/debugging-ems-programs/err-file}
+
+\input{src/debugging-ems-programs/edd-file}
+
+\input{src/debugging-ems-programs/line-trace}
+
+\input{src/debugging-ems-programs/debugging-strategies}
+
+\end{document}
diff --git a/doc/src/docs/EMS_Application_Guide/media/ep.gif b/doc/ems-application-guide/media/ep.gif
similarity index 100%
rename from doc/src/docs/EMS_Application_Guide/media/ep.gif
rename to doc/ems-application-guide/media/ep.gif
diff --git a/doc/ems-application-guide/media/ep.png b/doc/ems-application-guide/media/ep.png
new file mode 100644
index 00000000000..a808760c870
Binary files /dev/null and b/doc/ems-application-guide/media/ep.png differ
diff --git a/doc/src/docs/EMS_Application_Guide/media/image003.jpg b/doc/ems-application-guide/media/image003.jpg
similarity index 100%
rename from doc/src/docs/EMS_Application_Guide/media/image003.jpg
rename to doc/ems-application-guide/media/image003.jpg
diff --git a/doc/src/docs/EMS_Application_Guide/media/image004.jpg b/doc/ems-application-guide/media/image004.jpg
similarity index 100%
rename from doc/src/docs/EMS_Application_Guide/media/image004.jpg
rename to doc/ems-application-guide/media/image004.jpg
diff --git a/doc/src/docs/EMS_Application_Guide/media/image005.jpg b/doc/ems-application-guide/media/image005.jpg
similarity index 100%
rename from doc/src/docs/EMS_Application_Guide/media/image005.jpg
rename to doc/ems-application-guide/media/image005.jpg
diff --git a/doc/src/docs/EMS_Application_Guide/media/image011.jpg b/doc/ems-application-guide/media/image011.jpg
similarity index 100%
rename from doc/src/docs/EMS_Application_Guide/media/image011.jpg
rename to doc/ems-application-guide/media/image011.jpg
diff --git a/doc/ems-application-guide/src/application-guide-for-ems.tex b/doc/ems-application-guide/src/application-guide-for-ems.tex
new file mode 100644
index 00000000000..878fe2f5e09
--- /dev/null
+++ b/doc/ems-application-guide/src/application-guide-for-ems.tex
@@ -0,0 +1,7 @@
+\input{../title}
+
+\chapter{Introduction}\label{introduction}
+
+This document provides an in-depth look at the Energy Management System (EMS) feature in EnergyPlus and provides a way to develop custom control and modeling routines for EnergyPlus models. EMS is an advanced feature of EnergyPlus and is not for beginners. You will need to write your own custom computer programs and have a thorough understanding of how you want your models to behave. If you are intimidated by the idea of writing computer programs to adjust the fine details of how an EnergyPlus model runs, be aware that EMS is not for all (or even most) users. However, if you relish the idea of being able to write small computer programs that override some annoying behavior, you may find that writing Erl programs can solve many problems faced by energy modelers. EMS is a complicated feature~ and this application guide augments the Input/Output Reference by providing an overall discussion of how to use EMS.
+
+EMS provides high-level, supervisory control to override selected aspects of EnergyPlus modeling. A small programming language called EnergyPlus Runtime Language (Erl) is used to describe the control algorithms. EnergyPlus interprets and executes your Erl program as the model is being run. This guide serves as a programming manual for Erl and attempts to show you how to customize your EnergyPlus simulations.
diff --git a/doc/ems-application-guide/src/application-guide-for-ems/background.tex b/doc/ems-application-guide/src/application-guide-for-ems/background.tex
new file mode 100644
index 00000000000..f5de3cfea1f
--- /dev/null
+++ b/doc/ems-application-guide/src/application-guide-for-ems/background.tex
@@ -0,0 +1,3 @@
+\section{Background}\label{background}
+
+We used the operations manual for a common commercial brand of EMS to guide the initial formulation of Erl. The circa 2000 EMS language from a major manufacturer is a good example because it uses a full-featured EMS language and does not rely on a graphical user interface.
diff --git a/doc/ems-application-guide/src/application-guide-for-ems/organization.tex b/doc/ems-application-guide/src/application-guide-for-ems/organization.tex
new file mode 100644
index 00000000000..5e340ecb37b
--- /dev/null
+++ b/doc/ems-application-guide/src/application-guide-for-ems/organization.tex
@@ -0,0 +1,3 @@
+\section{Organization}\label{organization}
+
+We first describe Erl, then discuss its rules and features, including syntax for writing statements, variables, expressions, and built-in functions. We then discuss sensors, actuators, and calling points for the EMS. Then we describe a set of examples applications for EMS. The last section provides information about debugging Erl programs.
diff --git a/doc/ems-application-guide/src/debugging-ems-programs.tex b/doc/ems-application-guide/src/debugging-ems-programs.tex
new file mode 100644
index 00000000000..36eb7287030
--- /dev/null
+++ b/doc/ems-application-guide/src/debugging-ems-programs.tex
@@ -0,0 +1,3 @@
+\chapter{Debugging EMS Programs}\label{debugging-ems-programs}
+
+This section discusses approaches to debugging Erl programs. As you develop your own programs, you will need to identify and correct coding problems. The task of debugging an Erl program is challenging. Compared to most programming, with integrated development environments and sophisticated debugging interfaces, the Erl programmer has only rudimentary tools available for debugging. If you have some type of developer license and EnergyPlus source code, you could debug Erl programs inside a full-featured debugging environment (such as IVF integrated into VS9). But this is only for extremely advanced users and developers implementing EMS related code inside EnergyPlus. Most users' EMS should have little need to deal with compilers and development environments, because enough information is produced by EnergyPlus when it runs their Erl programs. This section examines output related to EMS in an effort to help you debug your Erl programs.
diff --git a/doc/ems-application-guide/src/debugging-ems-programs/debugging-strategies.tex b/doc/ems-application-guide/src/debugging-ems-programs/debugging-strategies.tex
new file mode 100644
index 00000000000..07946db9d0e
--- /dev/null
+++ b/doc/ems-application-guide/src/debugging-ems-programs/debugging-strategies.tex
@@ -0,0 +1,28 @@
+\section{Debugging Strategies}\label{debugging-strategies}
+
+This section attempts to provide some debugging tips.
+
+There is no debugging environment, so the main way to obtain information is to use verbose mode and trace each line.
+
+Say, for example, we are trying to debug the following line:
+
+\begin{lstlisting}
+ ELSEIF (Hour > = 5) && (Hour < 19)  && (DayOfWeek > = 2) && (DayOfWeek < = 6) ,
+\end{lstlisting}
+
+The line trace, shown next, shows only the result of the logical condition, i.e., 0.0 (highlighted) if overall it is false or 1.0 if overall it is true.
+
+\begin{lstlisting}
+MYCOMPUTEDHEATINGSETPOINTPROG,Line 10,ELSEIF (HOUR > = 5) && (HOUR < 19)  && (DAYOFWEEK > = 2) && (DAYOFWEEK < = 6),0.0, Occurrence info = CHICAGO IL USA TMY2-94846 WMO\# = 725300, 09/23 10:20 - 10:30
+\end{lstlisting}
+
+To debug what is going on with the individual terms in the logical expression, we can add some otherwise useless statements so line traces contain an echo of the current values of the HOUR and DAYOFWEEK built-in variables. So if we add the following lines before the start of the IF block,
+
+\begin{lstlisting}
+    Set locHour = Hour, ! echo out for debug
+    Set locDay = DayOfWeek, ! echo out for debug
+\end{lstlisting}
+
+We will see the values that Hour and DayOfWeek contain in the debug output. The local variables Erl variables locHour and locDay do not need to be used for anything, but by adding these Erl statements we can glean debugging insights.
+
+The line of Erl code is switched to all uppercase on input, so the line trace differs from the input file in that all characters are capitalized. If the input file was developed using a CamelCase convention, it may be much more difficult to read in the line trace output. Thus, the underscore character ``\_'' may be a more useful convention for inputting Erl code because it will be more readable in the debugging traces.
diff --git a/doc/ems-application-guide/src/debugging-ems-programs/edd-file.tex b/doc/ems-application-guide/src/debugging-ems-programs/edd-file.tex
new file mode 100644
index 00000000000..6b087e446e8
--- /dev/null
+++ b/doc/ems-application-guide/src/debugging-ems-programs/edd-file.tex
@@ -0,0 +1,5 @@
+\section{EDD File}\label{edd-file}
+
+If the Erl programs are processed and start running, the EDD becomes a primary source of information for debugging. The EDD file is the output file associated only with the EMS. When a line of Erl code is executed, and full trace is selected, the program will output records that are useful for debugging.
+
+It is very important to be careful with the EDD file. There are options to control how verbose the EDD file becomes with modes such as only the errors or a full trace. The full trace option should be used with care because a full line-by-line trace of EMS program execution for an annual run can easily create an enormous file that is too large for most computer systems.
diff --git a/doc/ems-application-guide/src/debugging-ems-programs/err-file.tex b/doc/ems-application-guide/src/debugging-ems-programs/err-file.tex
new file mode 100644
index 00000000000..46a651ee9d1
--- /dev/null
+++ b/doc/ems-application-guide/src/debugging-ems-programs/err-file.tex
@@ -0,0 +1,5 @@
+\section{ERR File}\label{err-file}
+
+A key output file to review is the ERR file (eplusout.err), the one with the ``.err'' file extension. This is the common error file for all of EnergyPlus, and many EMS-related errors will appear there. The file might contain critical problems that arose while the Erl programs were being read in and processed. Although the EDD file will likely be the focus of most debugging, remember the ERR file. Also, sometimes no EDD file is produced from a run. This occurs when problems are captured early during input processing and the program fatals out before an Erl program is run. Depending on the run manager you use to execute EnergyPlus, the EDD file may be from a previous run, so check the file creation times for ERR and EDD.
+
+An especially important error revealed in the ERR file is truncation from too long input. Each program line in Erl is limited to 100 characters. (It becomes useful to keep variable names shorter in Erl because the line length limit can be onerous.)~ If there are more than 100 characters, the program truncates the line to the first 100. This will often throw a severe error that halts because the truncated line is not a valid statement. But an unlucky truncation may form a viable line of code and the program will run. Truncation of any Erl program line is surely a bad thing, so it is important to check the ERR file.
diff --git a/doc/ems-application-guide/src/debugging-ems-programs/line-trace.tex b/doc/ems-application-guide/src/debugging-ems-programs/line-trace.tex
new file mode 100644
index 00000000000..afeb8a47d1b
--- /dev/null
+++ b/doc/ems-application-guide/src/debugging-ems-programs/line-trace.tex
@@ -0,0 +1,25 @@
+\section{Line Trace}\label{line-trace}
+
+You can use the EDD file to examine the execution of every line of code. If you request a verbose level of debugging output in the Output:EnergyManagementSystem input object, the EDD file will contain a series of text records that trace the execution of each line of Erl code. Traces contain the name of the program, the program line number, the text of the line, the result returned by executing the line (if any), and a timestamp that indicates when it was executed during the environment period. Note that the EDD file is only produced if you have EMS/Erl programs in your input file.
+
+An example of a single trace follows. This is one record, or single line of text from one of the traces in an EDD file.
+
+\begin{lstlisting}
+VAV1MIXEDAIRMANAGERS,Line 1,SET VAV_1_COOLC_SETPOINT = SEASONAL_RESET_SAT_SCHED - ( T_VAV1FANOUT - T_VAV1FANIN),13.0000000000000, During Warmup, Occurrence info = CHICAGO IL USA TMY2-94846 WMO\# = 725300, 01/01 18:30 - 18:45
+\end{lstlisting}
+
+Each block of text is separated by comma, so the trace information could be read into a spreadsheet and formatted to columns using comma separation.
+
+``VAV1MIXEDAIRMANAGERS'' is the name of a user-defined Erl Program.
+
+``Line 1'' indicates that this trace is from the first line of the Erl program called VAV1MIXEDAIRMANAGERS.
+
+The next block of text, ``SET VAV\_1\_COOLC\_SETPOINT = SEASONAL\_RESET\_SAT\_SCHED - ( T\_VAV1FANOUT - T\_VAV1FANIN)'' is the Erl program statement contained at Line 1 in the Erl program called VAV1MIXEDAIRMANAGERS.
+
+The value ``13.0000000000000'' is the result of this particular SET statement. The value of 13.0 has been assigned to the variable called VAV\_1\_COOLC\_SETPOINT.
+
+The next block of text ``During Warmup'' indicates that the line was executed while the simulation was in a warm up phase. (Warmup happens during the beginning of each environment period to precondition the model's transients with the conditions of the first day.)
+
+The next block of text ``Occurrence info = CHICAGO IL USA TMY2-94846 WMO\# = 725300'' indicates the environment period being simulated. This is a weather-file-based RunPeriod for Chicago using TMY2 data source associated with weather station number 725300.
+
+The last block of text ``01/01 18:30 - 18:45'' is the date and time of day for the simulation timestep when the Erl program line was executed.
diff --git a/doc/ems-application-guide/src/ems-actuators.tex b/doc/ems-application-guide/src/ems-actuators.tex
new file mode 100644
index 00000000000..771755030b6
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-actuators.tex
@@ -0,0 +1,9 @@
+\chapter{EMS Actuators}\label{ems-actuators}
+
+This section provides details about EMS actuators, the conduits by which Erl programs control EnergyPlus simulations. They \emph{actuate} selected features inside EnergyPlus. Rather than add a new set of controls and component models that have EMS awareness, they generally override established features.
+
+Internal to EnergyPlus are two separate lists of actuators:~ those that are available for use, and those that are being used in the EMS. While implementing the EMS, developers have added code to control points to make them available for use in EMS. The actuators available in a given model depend on the non-EMS-related content of the input file. Similar to how EnergyPlus reports the available output variables to the RDD file, a list of available actuators is written to the EDD file (depending on the settings in Output:EnergyManagementSystem). Note that the EDD file is ONLY produced if you have set up EMS / Erl programs. To use an actuator in EMS, you need to enter an EnergyManagementSystem:Actuator input object. The EDD file contains information needed for this input object; however, it is not available until after the output has been generated from a previous run. If you do not see a particular actuator in the EDD output file, it is not available in EMS for that particular model. There is no way to create a new actuator (except by modifying EnergyPlus source code); you can only customize the behavior of current actuators. If you need an actuator that you suspect could be provided by the program but is not available, you can use the regular system(s) for user support to request it be added to the program. New actuators are added to the program from time to time so the availability of actuators will grow with each new release.
+
+Actuators override things inside EnergyPlus whenever the actuator's Erl variable is set to a value other than ``Null.''~ Null is a special built-in variable used to deactivate an actuator. Once an actuator starts overriding, it will continue to do so until the actuator's Erl variable is set to Null. You should set the actuators to Null whenever you want the EMS to revert to normal operation.
+
+The rest of this section provides details about specific actuators.
diff --git a/doc/ems-application-guide/src/ems-actuators/air-movement.tex b/doc/ems-application-guide/src/ems-actuators/air-movement.tex
new file mode 100644
index 00000000000..4df3ce88ba3
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-actuators/air-movement.tex
@@ -0,0 +1,23 @@
+\section{Air Movement}\label{air-movement}
+
+\subsection{Zone Infiltration}\label{zone-infiltration}
+
+An actuator called ``Zone Infiltration'' is available with a control type called ``Air Exchange Flow Rate'' (m\(^{3}\)/s). This provides override control over the zone-by-zone infiltration rate. The unique identifier is the name of the ZoneInfiltration object.
+
+\subsection{Zone Ventilation}\label{zone-ventilation}
+
+An actuator called ``Zone Ventilation'' is available with a control type called ``Air Exchange Flow Rate'' (m\(^{3}\)/s). This provides override control over the zone-by-zone ventilation rate. This simple ventilation model is provided by the input object ZoneVentilation. The unique identifier is the name of the ZoneVentilation object.
+
+\subsection{Zone Mixing}\label{zone-mixing}
+
+An actuator called ``ZoneMixing'' is available with a control type called ``Air Exchange Flow Rate'' (m\(^{3}\)/s). This provides override control over the zone-to-zone mixing rate. This simple air movement model is provided by the input object ZoneMixing. The unique identifier is the name of the ZoneMixing object.
+
+\subsection{Zone Cross Mixing}\label{zone-cross-mixing}
+
+An actuator called ``ZoneCrossMixing'' is available with a control type called ``Air Exchange Flow Rate'' (m\(^{3}\)/s). This provides override control over the interzonal mixing rate. This is the simple air movement model provided by the input object ZoneCrossMixing. The unique identifier is the name of the ZoneCrossMixing object.
+
+\subsection{Airflow Network Openings}\label{airflow-network-openings}
+
+An actuator called ``AirFlow Network Window/Door Opening'' is available with a control type called ``Venting Opening Factor.''~ It is available in models that have operable openings in the Airflow Network model and that are entered by using either AirflowNetwork:MultiZone:Component:DetailedOpening or AirflowNetwork:MultiZone:Component:SimpleOpening input objects. This control allows you to use EMS to vary the size of the opening during the airflow model calculations, such as for natural and hybrid ventilation.
+
+The unique identifier is the name of the window or door, not the name of the associated airflow network input objects. The actuator control involves setting the value of the opening factor between 0.0 and 1.0.
diff --git a/doc/ems-application-guide/src/ems-actuators/general.tex b/doc/ems-application-guide/src/ems-actuators/general.tex
new file mode 100644
index 00000000000..10b1b3cab55
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-actuators/general.tex
@@ -0,0 +1,17 @@
+\section{General}\label{general}
+
+\subsection{Schedules}\label{schedules}
+
+A series of actuators is available for overriding schedule values. The following actuators are available with the control type called ``Schedule Value'':~ Schedule:Year, Schedule:Compact, Schedule:File, and Schedule:Constant. The units are not known by the schedule and are determined by the model that references the schedule. The unique identifier is the name of schedule.
+
+If you try to use a particular schedule as input to calculations that modify that schedule, you will be in a circular situation with unexpected results. The modified schedule will lose the original information (unless the actuator is set to Null) and the modifications will be reapplied on top of previous modifications. When this situation arises, use a copy of the original schedule as input to the Erl program so you have the original schedule values.
+
+\subsection{Curves}\label{curves}
+
+An advanced actuator called ``Curve'' with a control type called ``Curve Result'' is available whenever any generic curve objects are used. This allows you to override the results generated by these curves. The units are not known by the actuator and depend on how the curve is being used by the component model that calls it.
+
+This actuator must be used with caution. The EMS does not necessarily have access to the independent variables used by the models when the curves are evaluated during normal evaluation, so in most situations you will probably need to examine EnergyPlus source code to use this actuator correctly.
+
+\subsection{Weather Data}\label{weather-data}
+
+A series of actuators are available for overriding the values of weather data that are normally derived from the .epw weather file.~ These provide the ability to alter weather data and were originally requested for use with ExternalInterface for using measured data.~ The following can be overridden: outdoor drybulb, outdoor dewpoint, outdoor relative humidity, diffuse solar, direct solar, wind speed, and wind direction.
diff --git a/doc/ems-application-guide/src/ems-actuators/hvac-systems-001.tex b/doc/ems-application-guide/src/ems-actuators/hvac-systems-001.tex
new file mode 100644
index 00000000000..655c42ba8ee
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-actuators/hvac-systems-001.tex
@@ -0,0 +1,149 @@
+\section{HVAC Systems}\label{hvac-systems}
+
+\subsection{System Node Setpoints}\label{system-node-setpoints}
+
+A series of actuators is available for all the setpoints that can be placed on system nodes. System nodes are used to define air and plant loops, and a natural application of EMS is to control the setpoints at these nodes. The node actuators are all called ``System Node Setpoint.''~ There are nine control types:
+
+\begin{itemize}
+\item
+  Temperature Setpoint, (°C)
+\item
+  Temperature Minimum Setpoint (°C)
+\item
+  Temperature Maximum Setpoint (°C)
+\item
+  Humidity Ratio Setpoint (kgWater/kgDryAir)
+\item
+  Humidity Ratio Minimum Setpoint (kgWater/kgDryAir)
+\item
+  Humidity Ratio Maximum Setpoint (kgWater/kgDryAir)
+\item
+  Mass Flow Rate Setpoint (kg/s)
+\item
+  Mass Flow Rate Minimum Setpoint (kg/s)
+\item
+  Mass Flow Rate Maximum Setpoint (units kg/s)
+\end{itemize}
+
+Using these actuators is natural with an EMS. Typically, the controller would place the setpoint on the outlet node. Then the component's low-level controller should operate to meet the leaving setpoint. Setting the setpoints on nodes should be a common application for the EMS.
+
+Although all nine possible setpoints are available as EMS actuators, it does not follow that EnergyPlus can use all of them. Most components can use only one or two setpoints. If a component cannot control to meet the setpoints on a node, the actuator will do nothing.
+
+\subsection{Zone HVAC Control}\label{zone-hvac-control}
+
+Several actuators relate to HVAC zone controls for temperature, humidity, and comfort.
+
+\begin{itemize}
+\item
+  Two actuators called ``Zone Temperature Control'' are available with the control types of ``Heating Setpoint'' and ``Cooling Setpoint.''~ These enable you to directly override the zone-by-zone heating and cooling setpoints. The units are in degrees Celsius. The unique identifier is the zone name.
+\item
+  Two actuators called ``Zone Humidity Control'' are available with the control types ``Relative Humidity Humidifying Setpoint'' and ``Relative Humidity Dehumidifying Setpoint.'' ~These enable you to directly override the zone-by-zone humidity control setpoints. The units are in percent relative humidity. The unique identifier is the zone name.
+\item
+  Two actuators called ``Zone Comfort Control'' are available with the control types ``Heating Setpoint'' and ``Cooling Setpoint.''~ These enable you to directly override the zone-by-zone comfort control setpoints. The units are predicted mean vote (PMV). The unique identifier is the zone name.
+\end{itemize}
+
+\subsection{Plant Supervisory Control}\label{plant-supervisory-control}
+
+Several levels of actuators are available for on/off supervisory control of Plant systems.
+
+\begin{itemize}
+\item
+  Each plant (and condenser) loop has an actuator called ``Plant Loop Overall'' available with the control type ``On/Off Supervisory.''~ Setting the value of this actuator to 1.0 directs the overall plant to loop to run normally based on other controls. Setting the value of this actuator to 0.0 directs the overall plant loop to shut down regardless of what other controls indicate.
+\item
+  Each plant (and condenser) loop has actuators called ``Supply Side Half Loop'' and ``Demand Side Half Loop'' that are available with the control type ``On/Off Supervisory.''~ Setting the value of this actuator to 1.0 directs the plant's loop side to run normally based on other controls. Setting the value of this actuator to 0.0 directs the plant's loop side to shut down regardless of what other controls indicate.
+\item
+  Each plant (and condenser) loop has a series of actuators called ``Supply Side Branch'' and ``Demand Side Branch'' that are available with the control type ``On/Off Supervisory.''~ These are available for each individual branch in a loop. Setting the value of this actuator to 1.0 directs the plant's branch to run normally based on other controls. Setting the value of this actuator to 0.0 directs the plant's branch to shut down regardless of what other controls indicate.
+\item
+  Each plant (and condenser) loop has a series of actuators called ``Plant Component *'' that are available with the control type ``On/Off Supervisory.''~ These are available for each individual component on a loop. Setting the value of this actuator to 1.0 directs the component to run normally based on other controls. Setting the value of this actuator to 0.0 directs the component to shut down regardless of what other controls indicate.
+\end{itemize}
+
+\subsection{Outdoor Air System Node Conditions}\label{outdoor-air-system-node-conditions}
+
+Actuators called ``Outdoor Air System Node'' are available with control types called ``Drybulb Temperature'' and ``Wetbulb Temperature.''~ The units are degrees Celsius. These actuators are available for all system nodes that are listed in either an OutdoorAir:Node or OutdoorAir:NodeList input object. You should probably set both the drybulb and wetbulb temperatures to ensure a full description of the moist air conditions.
+
+The air system and many component models require you to specify a node as an outdoor air node to obtain values for the outdoor conditions. For example, outdoor air nodes are used at the inlet to an outdoor air mixer or at the inlet of the heat rejection side of a component model. Typically this is the weather data value for outdoor conditions. But local variations in microclimate may shift the local outdoor air temperature to differ slightly from the weather data. (Currently the only local variation model for this effect in EnergyPlus varies the outdoor air conditions as a function of height.)~ If you want to experiment with other models for local variations in outdoor air conditions, this EMS actuator allows you to override the outdoor temperature at a particular system node with any model that can be implemented in an Erl program. For example (although better models for the changes in conditions may need be developed), this actuator could be used to examine the energy impacts of warmer outdoor air temperatures experienced by a rooftop packaged HVAC system sitting on a black roof or the cooler conditions experienced by a unit that is located on the shaded side of a building.~ Another example is to make use of a separate model, outside of EnergyPlus, for some unique type of component (such as a labyrinth or earth-tube) that preconditions outdoor air; the results of that model could be fed into the air system model in EnergyPlus using these actuators.
+
+\subsection{AirLoopHVAC Availability Status}\label{airloophvac-availability-status}
+
+This actuator is available in all models with central, or primary, air systems that are entered with the object ``AirLoopHVAC.''~ Various availability managers use the air loop's availability status to override control of the central air system fan. The fan may be scheduled to be unavailable during certain times to shut down the system when it is not needed. However, there may be times when the air system should be started to protect from freezing, for example. This actuator can force an air system to start up or shut down.
+
+The control is actuated by setting values for the availability status. The settings are numeric, but represent discrete states the status can take. The following settings are valid:
+
+\begin{itemize}
+\item
+  0.0 ( = NoAction). This tells the air system to do whatever it would usually do without any special override status.
+\item
+  1.0 ( = ForceOff). This overrides the air system to shut down when it would normally want to run.
+\item
+  2.0 ( = CycleOn). This overrides the air system to start up when it would normally be off.
+\item
+  3.0 ( = CycleOnZoneFansOnly). This overrides only the zone fans (not the central fans) if they would normally be off.
+\end{itemize}
+
+\subsection{Ideal Loads Air System}\label{ideal-loads-air-system}
+
+An actuator called ``Ideal Loads Air System'' is available with control types called ``Air Mass Flow Rate'' (supply air), ``Outdoor Air Mass Flow Rate,'' ``Air Temperature,'' and ``Air Humidity Ratio.'' ~These are available in models that use the ideal loads air system, formerly known as purchased air. The units are kg/s for mass flow rate, C for temperature and kgWater/kgDryAir for humidity ratio. The unique identifier is the user-defined name of the ZoneHVAC:IdealLoadsAirSystem input object.
+
+For Air Temperature and Air Humidity Ratio, the overrides are absolute. They are applied after all other limits have been checked. For mass flow rate, the overrides are not absolute, in that the model has additional internal controls that may not always be overridden. The internal controls will still apply the capacity and flow rate limits if defined in the input object. The EMS override affects the flow rate only if the air system is on. If the air system is ``off,'' the mass flow is zero regardless of the actuator setting. The internal model controls will turn off the air system if the zone is in the dead band or if it is scheduled ``off'' by availability managers. This behavior allows you to use the internal controls to determine when the air should cycle on, as for a constant volume system that cycles to achieve control. If both the Air Mass Flow Rate and Outdoor Air Mass Flow Rate are overridden, the Outdoor Air Mass Flow Rate will not be allowed to be greater than the override value for Air Mass Flow Rate.
+
+\subsection{Fan}\label{fan}
+
+Actuators called ``Fan'' are available with the control types ``Fan Air Mass Flow Rate,'' ``Fan Pressure Rise,'' and ``Fan Total Efficiency.''~ These provide direct control over the fan operation in an air system. The EMS program can override the flow rate by using kg/s. It can override the total pressure rise at the fan by using Pascals. And it can override the fan efficiency on a scale from 0.0 to 1.0. The unique identifier is the name of the fan in the Fan input objects.
+
+An actuator is also available for overriding the autosize value for the fan's design air flow rate.~ This actuator is called ``Fan'' and the control type is ``'Fan Autosized Air Flow Rate'' with units in m\(^{3}\)/s. It is only useful from the calling point named AfterComponentInputReadIn.
+
+\subsection{DX Cooling Coils}\label{dx-cooling-coils}
+
+Actuators are available for overriding the autosize values related to the size of single speed DX coils.~ Actuators called ``Coil:Cooling:DX:SingleSpeed'' are available with control types ``Autosized Rated Air Flow Rate'' (in m3/s), ``Autosized Rated Sensible Heat Ratio'' (in W/W), and ``Autosized Rated Total Cooling Capacity'' (in W).~ These are only useful from the calling point named AfterComponentInputReadIn.
+
+\subsection{Unitary Equipment}\label{unitary-equipment}
+
+Actuators called ``Unitary HVAC'' are available with the control types ``Sensible Load Request'' and ``Moisture Load Request.''~ These control the operation of unitary equipment. Normally these systems operate to meet zone loads, but these actuators allow you to override the controls of unitary systems. The units are in Watts. The unique identifier is the name of the unitary equipment in the input objects.
+
+Actuators are available for overriding the autosize values related to supply air flow rates some unitary HVAC equipment.~ These actuators allow selectively altering the outcome of sizing routines and are used from the calling point named AfterComponentInputReadIn.~ The units are m\(^{3}\)/s.
+
+\begin{itemize}
+\item
+  An actuator called ``AirLoopHVAC:Unitary:Furnace:HeatOnly'' is available with control type ``Autosized Supply Air Flow Rate.''
+\item
+  An actuator called ``AirLoopHVAC:UnitaryHeatOnly'' is available with control type ``Autosized Supply Air Flow Rate.''
+\item
+  Actuators called ``AirLoopHVAC:Unitary:Furnace:HeatCool'' and ``AirLoopHVAC:UnitaryHeatCool''are available with control types ``Autosized Supply Air Flow Rate,''~ ``Autosized Supply Air Flow Rate During Cooling Operation,'' ``Autosized Supply Air Flow Rate During Heating Operation,'' and ``Autosized Supply Air Flow Rate During No Heating or Cooling Operation.''
+\item
+  An actuator called ``AirLoopHVAC:UnitaryHeatPump:AirToAir'' is available with control type ``Autosized Supply Air Flow Rate.''
+\item
+  An actuator called ``AirLoopHVAC:UnitaryHeatPump:WaterToAir'' is available with control type ``Autosized Supply Air Flow Rate.''
+\end{itemize}
+
+\subsection{AirTerminal:SingleDuct:Uncontrolled}\label{airterminalsingleductuncontrolled}
+
+An actuator called ``AirTerminal:SingleDuct:Uncontrolled'' is available with a control type called ``Mass Flow Rate.''~ This actuator is available in models that use the direct air terminal. The units are kg/s. This actuator is used to control the flow rate. Normally, the flow rate of direct air terminals is fixed by the input or sizing results, but this actuator provides a way to override the flow with Erl programs.
+
+\subsection{Outdoor Air Controller}\label{outdoor-air-controller}
+
+An actuator called ``Outdoor Air Controller'' is available with the control type called ``Air Mass Flow Rate.'' ~This provides override control over the rate of outdoor air. The units are kg/s. The unique identifier is the name of the Controller:OutdoorAir input object.
+
+\subsection{Plant Load Profile}\label{plant-load-profile}
+
+Actuators called ``Plant Load Profile'' are available with the control types called ``Mass Flow Rate'' (in kg/s) and ``Power'' (in W). The unique identifier is the name of the LoadProfile:Plant input object. These actuators provide override control over the loads placed on a plant system by a plant load profile.
+
+\subsection{Pump}\label{pump}
+
+An actuator called ``Pump'' is available with the control type ``Pump Mass Flow Rate'' (in kg/s). This allows you to override the flow rate produced by a pump. The unique identifier is the name of Pump Input object.
+
+\subsection{Window Air Conditioner}\label{window-air-conditioner}
+
+An actuator called ``Window Air Conditioner'' is available with a control type called ``Part Load Ratio.''~ This is nondimensional and takes numbers between 0.0 and 1.0. The unique identifier is the name of the ZoneHVAC:WindowAirConditioner input object.
+
+\subsection{Low Temperature Radiant Hydronic}\label{low-temperature-radiant-hydronic}
+
+Actuators called ``Hydronic Low Temp Radiant'' and ``Constant Flow Low Temp Radiant'' are available with the control type ``Water Mass Flow Rate'' (in kg/s). This allows you to override the flow of water through hydronic radiant systems. The unique identifier is the name of either the ZoneHVAC:LowTemperatureRadiant:VariableFlow or ZoneHVAC:LowTemperature\\
+Radiant:ConstantFlow input objects.
+
+\subsection{Variable Refrigerant Flow Heat Pump Air Conditioner}\label{variable-refrigerant-flow-heat-pump-air-conditioner}
+
+An actuator called ``Variable Refrigerant Flow Heat Pump'' is available with a control type called ``Operating Mode.''~ This is nondimensional and takes numbers between 0.0 and 2.0 where 0.0 means the system is off, 1.0 means the system is in cooling mode, and 2.0 means the system is in heating mode. The unique identifier is the name of the AirConditioner:VariableRefrigerantFlow input object.
+
+\subsection{Variable Refrigerant Flow Terminal Unit}\label{variable-refrigerant-flow-terminal-unit}
+
+An actuator called ``Variable Refrigerant Flow Terminal Unit'' is available with a control type called ``Part Load Ratio.''~ This is nondimensional and takes numbers between 0.0 and 1.0. The unique identifier is the name of the ZoneHVAC:TerminalUnit:VariableRefrigerantFlow input object. This control over rides the part-load ratio of the terminal unit and can be applied only when the cooling or heating minimum and maximum outdoor temperature limits of the condenser (i.e., the AirConditioner:VariableRefrigerantFlow object) are not exceeded.
diff --git a/doc/ems-application-guide/src/ems-actuators/internal-gains-and-exterior-lights.tex b/doc/ems-application-guide/src/ems-actuators/internal-gains-and-exterior-lights.tex
new file mode 100644
index 00000000000..1de92fc3e35
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-actuators/internal-gains-and-exterior-lights.tex
@@ -0,0 +1,39 @@
+\section{Internal Gains and Exterior Lights}\label{internal-gains-and-exterior-lights}
+
+\subsection{People}\label{people}
+
+An actuator called ``People'' is available with a control type called ``Number of People.''~ This allows you to dictate the number of people in a zone. The units are persons. The unique identifier is the name of the people input object. Because you cannot really control people, this is an example the EMS in EnergyPlus departing from the real world of building EMS.
+
+\subsection{Lights}\label{lights}
+
+An actuator called ``Lights'' is available with a control type called ``Electric Power Level'' (in W)~ This allows you to set the lighting power associated with each Lights input object. The unique identifier is the name of the Lights input object.
+
+\subsection{Electric Equipment}\label{electric-equipment}
+
+An actuator called ``ElectricEquipment'' is available with a control type called ``Electric Power Level'' (in W). This allows you to set the power associated with each ElectricEquipment input object. The unique identifier is the name of the ElectricEquipment input object.
+
+\subsection{Gas Equipment}\label{gas-equipment}
+
+An actuator called ``GasEquipment'' is available with a control type called ``Gas Power Level'' (in W). This allows you to set the power associated with each GasEquipment input object.~ The unique identifier is the name of the GasEquipment input object.
+
+\subsection{Hot Water Equipment}\label{hot-water-equipment}
+
+An actuator called ``HotWaterEquipment'' is available with a control type called ``District Heating Power Level'' (in W). This allows you to set the power associated with each HotWaterEquipment input object. The unique identifier is the name of the HotWaterEquipment input object.
+
+\subsection{Steam Equipment}\label{steam-equipment}
+
+An actuator called ``SteamEquipment'' is available with a control type called ``District Heating Power Level'' (in W). This allows you to set the power associated with each SteamEquipment input object. The unique identifier is the name of the SteamEquipment input object.
+
+\subsection{Other Equipment}\label{other-equipment}
+
+An actuator called ``OtherEquipment'' is available with a control type called ``Power Level'' (in W). This allows you to set the power associated with each OtherEquipment input object. The unique identifier is the name of the OtherEquipment input object.
+
+Other equipment offers a way to adjust the zone air energy balance without consuming any energy resources.
+
+\subsection{Baseboard}\label{baseboard}
+
+An actuator called ``ZoneBaseboard:OutdoorTemperatureControlled'' is available with a control type called ``Power Level'' (in W). The unique identifier is the name of the ZoneBaseboard:OutdoorTemperatureControlled input object.
+
+\subsection{Exterior Lights}\label{exterior-lights}
+
+An actuator called ``ExteriorLights'' is available with a control type called ``Electric Power'' (in W). The unique identifier is the name of the Exterior:Lights input object.
diff --git a/doc/ems-application-guide/src/ems-actuators/on-site-electricity-production-001.tex b/doc/ems-application-guide/src/ems-actuators/on-site-electricity-production-001.tex
new file mode 100644
index 00000000000..ff469a073d3
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-actuators/on-site-electricity-production-001.tex
@@ -0,0 +1,13 @@
+\section{On-Site Electricity Production}\label{on-site-electricity-production}
+
+\subsection{Generator Dispatch}\label{generator-dispatch}
+
+An actuator called ``On-Site Generator Control'' is available with a control type called ``Requested Power.'' This actuator is available in models that have on-site electrical generators. The units are Watts. This control allows you to use the EMS to override how requests for power generation are dispatched.
+
+The unique identifier is the name of each generator. The Erl programs should set the actuator value with Watts. Depending on the type and limitations of the generator being modeled, the power production may not exactly meet what is requested.
+
+\subsection{Electrical Storage}\label{electrical-storage}
+
+Actuators called ``Electrical Storage'' are available with control types called ``Power Draw Rate'' and ``Power Charge Rate'' (in W). These are available in models that have ElectricLoadCenter:Storage:Simple input objects. These controls allow you to use the EMS to override the rate of charging or drawing from storage.
+
+The unique identifiers are the names of the storage objects. For a given timestep, the electrical storage device can only charge or draw. If the EMS tries to override charge and draw during the same timestep, the program will find the larger of the two and apply the difference in that direction.
diff --git a/doc/ems-application-guide/src/ems-actuators/refrigeration.tex b/doc/ems-application-guide/src/ems-actuators/refrigeration.tex
new file mode 100644
index 00000000000..7aa7a879f97
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-actuators/refrigeration.tex
@@ -0,0 +1,5 @@
+\section{Refrigeration}\label{refrigeration}
+
+\subsection{Condenser Operation}\label{condenser-operation}
+
+An actuator called ``Refrigeration:System'' is available with a control type called ``Minimum Condensing Temperature.''~ This actuator is available in models that use the Refrigeration:System object.~ This actuator allows the user to override the usually constant value that is input into the field called Minimum Condensing Temperature in the Refrigeration:System object.~ This allows operating the condenser using custom control algorithms.
diff --git a/doc/ems-application-guide/src/ems-actuators/sizing-001.tex b/doc/ems-application-guide/src/ems-actuators/sizing-001.tex
new file mode 100644
index 00000000000..f5735069a44
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-actuators/sizing-001.tex
@@ -0,0 +1,41 @@
+\section{Sizing}\label{sizing}
+
+\subsection{Sizing:Zone}\label{sizingzone}
+
+A series of actuators called ``Sizing:Zone'' is available. These offer a way to override the results of zone sizing calculations. The unique identifier for each is the name of the Zone Input object. The following control types are available:
+
+\begin{itemize}
+\item
+  Zone Design Heating Air Mass Flow Rate (kg/s)
+\item
+  Zone Design Cooling Air Mass Flow Rate (kg/s)
+\item
+  Zone Design Heating Load (W)
+\item
+  Zone Design Cooling Load (W)
+\item
+  Zone Design Heating Vol Flow (m\(^{3}\)/s)
+\item
+  Zone Design Cooling Vol Flow (m\(^{3}\)/s)
+\end{itemize}
+
+\subsection{System Sizing}\label{system-sizing}
+
+A series of actuators called ``Sizing:System'' is available. These offer a way to override the results of air system sizing calculations. The unique identifier is the name of the AirLoopHVAC input object. The following control types are available:
+
+\begin{itemize}
+\item
+  Main Supply Volume Flow Rate (m\(^{3}\)/s)
+\item
+  Main Supply Coincident Peak Cooling Mass Flow Rate (kg/s)
+\item
+  Main Supply Coincident Peak Heating Mass Flow Rate (kg/s)
+\item
+  Main Supply Noncoincident Peak Cooling Mass Flow Rate (kg/s)
+\item
+  Main Supply Noncoincident Peak Heating Mass Flow Rate (kg/s)
+\item
+  Main Heating Volume Flow Rate (m\(^{3}\)/s)
+\item
+  Main Cooling Volume Flow Rate (m\(^{3}\)/s)
+\end{itemize}
diff --git a/doc/ems-application-guide/src/ems-actuators/thermal-envelope.tex b/doc/ems-application-guide/src/ems-actuators/thermal-envelope.tex
new file mode 100644
index 00000000000..53707ec01a9
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-actuators/thermal-envelope.tex
@@ -0,0 +1,67 @@
+\section{Thermal Envelope}\label{thermal-envelope}
+
+\subsection{Window Shading Control}\label{window-shading-control}
+
+This actuator is available in models that also have the WindowProperty:ShadingControl input objects. The user-defined name for the WindowProperty:ShadingControl is not used to identify unique window shading controls; rather, the window name is used to identify the actuator. This is because there could be multiple windows, all with shades, each of which is governed by a single WindowProperty:ShadingControl input object. The EMS actuator can override the control actions for each window separately.
+
+The control is actuated by setting values for the control status. The settings are numeric but represent discrete states the control can take. The appropriate values depend on the type and position of the shading device. There are three basic types of shading devices:~ switchable glazings, shades, and blinds. (Shades are described with WindowMaterial:Shade input objects. Blinds are described with WindowMaterial:Blind input objects.)~ Shades and blinds can be situated in the exterior, between the glass, or in the interior.
+
+The following settings are valid and must be used:
+
+\begin{itemize}
+\item
+  --1.0: ~~~ No shading device.
+\item
+  0.0: ~~~~~ Shading device is off (applies to shades and blinds).
+\item
+  1.0: ~~~~~ Interior shade is on.
+\item
+  2.0:~~~~~~ Glazing is switched to a darker state (switchable glazings only).
+\item
+  3.0: ~~~~~ Exterior shade is on.
+\item
+  6.0: ~~~~~ Interior blind is on.
+\item
+  7.0: ~~~~~ Exterior blind is on.
+\item
+  8.0: ~~~~~ Between-glass shade is on.
+\item
+  9.0: ~~~~~ Between-glass blind is on.
+\end{itemize}
+
+\subsection{Slat Angle}\label{slat-angle}
+
+If the shading device is a blind, there is also a control type called ``Slat Angle.''~ This angle control is a continuous numeric value from 0.0 to 180.0. The angle is defined as between the glazing system's outward normal and the slat's outward normal (see the diagram in the input output reference under WindowMaterial:Blind).
+
+\subsection{Surface Convection Heat Transfer Coefficient}\label{surface-convection-heat-transfer-coefficient}
+
+Two actuators called ``Surface'' are available with the control types of ``Interior Surface Convection Heat Transfer Coefficient'' and ``Exterior Surface Convection Heat Transfer Coefficient.''~ These provide direct control over the convection coefficient. The units are W/m\(^{2}\)-K. The unique identifier is the surface name.
+
+This actuator controls the heat transfer modeling. Changes in air distribution systems can affect the interior surface convection coefficients. A sheltered exterior surface may have a lower surface heat transfer coefficient. This actuator provides a method of applying new models for convection coefficients.
+
+\subsection{Material Surface Properties}\label{material-surface-properties}
+
+Three actuators are available for controlling the surface properties material related to absorptance. Those material layers used in a Construction object that lie at the outside and the inside of the assembly determine the surface properties of a heat transfer surface.~ Actuators called ``Material'' are available with the control types ``Surface Property Solar Absorptance,'' ``Surface Property Thermal Absorptance,'' and ``Surface Property Visible Absorptance.''~ These are dimensionless parameters between 0.0 and 1.0.~ These actuators are useful for modeling switchable coatings such as thermochromic paints.
+
+\subsection{Surface Construction State}\label{surface-construction-state}
+
+An actuator is available for controlling the construction assigned to a surface that can be useful for modeling dynamic technologies for thermal envelopes.~ These actuators are called ``Surface'' and have a control type ``Construction State.''~ This actuator is used in conjunction with the input object called EnergyManagementSystem:ConstructionIndexVariable.~ Each Construction object defined in an input file has an index that points to where the data for that construction are stored in the program's internal data structures.~ The EnergyManagementSystem:ConstructionIndexVariable input object is used to create and fill a global Erl variable with the value that points to the specific construction named in the object. The Erl variable is what you assign to the construction state actuator's variable to override the construction assigned to a particular surface.~ When the actuator is set to Null, the surface reverts to the Construction originally referenced by the surface in the input file.
+
+Using the surface construction state actuator brings with it a high degree of risk when it comes to modeling thermal heat capacity and transient heat transfer in opaque surfaces.~ If this actuator is used inappropriately, for example to assign different constructions, to a single surface, that have radically different heat storage capacities, then the heat transfer modeling results may not be physically accurate.~ When a construction state is overridden using this actuator, the thermal history data that evolved while using the previous construction are reused for the new construction. When this actuator is used, the program attempts to detect if incompatible constructions are being assigned. In some cases it issues a warning and allows the assignments to proceed, in others it warns and doesn't allow the assignment to proceed.~ If the original construction assigned to a surface has internal source/sink (defined using Construction:InternalSource) then any assignments to the surface must also be internal source constructions.~ If using the heat transfer algorithm called ConductionFiniteDifference, then the constructions must have the same number of finite difference nodes or the assignment is not allowed.~ The construction state actuator cannot be used in conjunction with the heat transfer algorithms called ConductionFiniteDifferenceSimplified or CombinedHeatAndMoistureFiniteElement.
+
+\subsection{Surface Boundary Conditions}\label{surface-boundary-conditions}
+
+Four actuators, called ``Other Side Boundary Conditions,'' are available for controlling the convection and radiation boundary conditions for surfaces that use ``OtherSideConditionsModel.''~ Each instance of a SurfaceProperty:OtherSideConditionsModel object will make available these actuators with the following four control types:
+
+\begin{itemize}
+\item
+  ``Convection Bulk Air Temperature.''~ This is the temperature of the ambient air exposed to the surface, in degrees C.~ This is the temperature used for surface convection heat transfer boundary conditions on the outdoor, outside-face, other side of the surface.
+\item
+  ``Convection Heat Transfer Coefficient.''~ This is the heat transfer coefficient, in W/(m-K) used for surface convection boundary conditions on the outdoor, outside-face, or other side of the surface.
+\item
+  ``Radiation Effective Temperature.''~ This is the effective temperature of the environment surrounding the surface, in degrees C.~ This is the temperature used for surface thermal radiation heat transfer boundary conditions on the outdoor, outside-face, other side of the surface.
+\item
+  ``Radiation Linear Heat Transfer Coefficient.''~ This is the linearized heat transfer coefficient, in W/(m-K), used for surface thermal radiation boundary conditions on the outdoor, outside-face, or other side of the surface.
+\end{itemize}
+
+When using these actuators, values should be set for all four types.~ This boundary condition has no solar, only convection and radiation.
diff --git a/doc/ems-application-guide/src/ems-calling-points.tex b/doc/ems-application-guide/src/ems-calling-points.tex
new file mode 100644
index 00000000000..69552f5b282
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points.tex
@@ -0,0 +1,31 @@
+\chapter{EMS Calling Points}\label{ems-calling-points}
+
+This section provides an overview of EnergyPlus's program flow and describes the various places where you can use the EMS to initiate calls for custom controlling. The input object EnergyManagementSystem:ProgramCallingManager requires the user describe the timing for when the Erl programs are run. These \emph{EMS Calling Points} correspond to places inside the EnergyPlus program where and when the EMS can be called to do something. The EMS offers a wide range of calling points. This section attempts to explain what you need to know about the EnergyPlus program flow so you can better understand which calling point to use for a particular application. Because the EMS needs to interact with the rest of the EnergyPlus computer program, you need a fairly high level of understanding of the inner workings of EnergyPlus. Finding the right point to insert your Erl override is a challenge. This is a complicated computer program. Using an interpreted language to override its calculations is no simple thing and should not be taken lightly.
+
+The best calling point will depend on the type of actuator being controlled and the intent of the override activity. Unfortunately, there is no easy way to explain the inner workings of a model as large as EnergyPlus, so this section includes only a brief overview. We attempt to provide useful recommendations for the types of control that are best suited for particular calling points. But for the full details you will need to refer to the EnergyPlus source code, which you can obtain with a developer license.
+
+This section starts with a series of three figures and then discusses them and the 14 calling points. Figure~\ref{fig:overall-program-flow-and-ems-calling-points} shows the overall flow of an EnergyPlus model with some EMS calling points. Figure~\ref{fig:timestep-sequence-with-ems-calling-points} shows the sequence for a single timestep with the remaining EMS calling points. Figure~\ref{fig:system-timestep-sequence-with-ems-calling} is similar but shows the calling points for shortened system timesteps. These diagram the flow of procedures during a run from top to bottom.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image003.jpg}
+\caption{Overall Program Flow and EMS Calling Points \protect \label{fig:overall-program-flow-and-ems-calling-points}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image004.jpg}
+\caption{Timestep Sequence with EMS Calling Points \protect \label{fig:timestep-sequence-with-ems-calling-points}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 3
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image005.jpg}
+\caption{System Timestep Sequence with EMS Calling Points \protect \label{fig:system-timestep-sequence-with-ems-calling}}
+\end{figure}
+
+When EnergyPlus runs a model, it first does various sizing and setup activities and then models the environment periods you ask for; e.g., design days and run periods. The built-in variable called CurrentEnvironment indentifies which of these is being simulated and any given time. Figure~\ref{fig:overall-program-flow-and-ems-calling-points} diagrams the overall program flow starting at the top and listing certain key steps in outline form. EnergyPlus models contain a lot of input, and the internal processes to acquire and process that input take some time to complete. Before the model starts doing final calculations, it may have to do various sizing calculations and automatically design the size of components. It will also go through special setup periods that model a truncated set of timesteps for each environment period. In the diagram, this initial phase is not finished until just before the design periods begin. Two EMS calling points that occur only once in a given run, EndOfZoneSizing and EndOfSystemSizing, can be triggered during this initial setup phase. During the phase called ``Setup Simulation,'' the various timestep-based calling points diagrammed in Figure~\ref{fig:timestep-sequence-with-ems-calling-points} will also be called.
+
+Another thing that happens during the setup phase described above is that individual HVAC component models access their input data and do various setup calculations in preparation for the rest of the simulation.~~ An EMS calling point (added for Version 7) called ``AfterComponentInputReadIn'' is available for selected HVAC components that allows triggering Erl programs at a point just after the component's input data have been read in but before the component's sizing routines have executed.~ This calling point is intended to be used with various actuators that are setup to override the autosize values that result from sizing.
+
+To model environment periods, EnergyPlus runs through a serious of timesteps. Figure~\ref{fig:timestep-sequence-with-ems-calling-points} diagrams the program flow for a single timestep where the timestep for the system modeling is equal to that for the zone load modeling. The \emph{system} timestep can be shorter than the \emph{zone} timestep. The usual process of modeling a timestep is to first calculate the zone loads during the ``Predictor,'' then model the response of the HVAC systems, and then calculate the resulting zone conditions during the ``Corrector.''~ Within the HVAC system modeling, some system iterations are used to iteratively solve a system of systems. Figure~\ref{fig:system-timestep-sequence-with-ems-calling} is a slightly modified version Figure~\ref{fig:timestep-sequence-with-ems-calling-points} that diagrams the situation when the timestep of the system calculations has been reduced to half the length of the zone timestep.
diff --git a/doc/ems-application-guide/src/ems-calling-points/after-component-model-input-has-been-read-in.tex b/doc/ems-application-guide/src/ems-calling-points/after-component-model-input-has-been-read-in.tex
new file mode 100644
index 00000000000..f9ff255a61f
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/after-component-model-input-has-been-read-in.tex
@@ -0,0 +1,3 @@
+\section{After Component Model Input has Been Read In}\label{after-component-model-input-has-been-read-in}
+
+The calling point called ``AfterComponentInputReadIn'' is used to alter the results of individual autosize fields.~ It executes whenever one of the selected components has finished reading in its input data.~ Those, and only those, component models that have some type of actuator with an ``Autosized'' control type will also have this calling point.~ This same calling point identifier is used for different HVAC components so programs executed from this point will be repeated.~ Currently this calling point exists in three different places:~ (1) after DX coil input, (2) after fan input, and (3) after unitary system input.
diff --git a/doc/ems-application-guide/src/ems-calling-points/after-new-environment-warmup-is-complete.tex b/doc/ems-application-guide/src/ems-calling-points/after-new-environment-warmup-is-complete.tex
new file mode 100644
index 00000000000..ffd40058433
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/after-new-environment-warmup-is-complete.tex
@@ -0,0 +1,3 @@
+\section{After New Environment Warmup Is Complete}\label{after-new-environment-warmup-is-complete}
+
+The calling point referred to with the keyword ``AfterNewEnvironmentWarmUpIsComplete'' occurs once near at the beginning of each environment period but after any warmup days are complete. This is similar to the previous calling point. Warmup days are used to condition the transient aspects of the model before proceeding with the first day. This will not be useful for control actions, but would be useful for reinitializing Erl programs with fresh values after the warmup days have finished running and the model is about to start the final timestep calculations for a particular environment period.
diff --git a/doc/ems-application-guide/src/ems-calling-points/after-predictor-after-hvac-managers.tex b/doc/ems-application-guide/src/ems-calling-points/after-predictor-after-hvac-managers.tex
new file mode 100644
index 00000000000..2c9ffe91c95
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/after-predictor-after-hvac-managers.tex
@@ -0,0 +1,3 @@
+\section{After Predictor After HVAC Managers}\label{after-predictor-after-hvac-managers}
+
+The calling point called ``AfterPredictorAfterHVACManagers'' occurs after the predictor and after the traditional HVAC managers have been called. It occurs at each timestep after the predictor executes and after the SetpointManager and AvailabilityManager models are called. It is useful for a variety of control actions. However, if there are conflicts, SetpointManager or AvailabilityManager actions may be overwritten by EMS control actions.
diff --git a/doc/ems-application-guide/src/ems-calling-points/after-predictor-before-hvac-managers.tex b/doc/ems-application-guide/src/ems-calling-points/after-predictor-before-hvac-managers.tex
new file mode 100644
index 00000000000..e9e447c07cd
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/after-predictor-before-hvac-managers.tex
@@ -0,0 +1,3 @@
+\section{After Predictor Before HVAC Managers}\label{after-predictor-before-hvac-managers}
+
+The calling point called ``AfterPredictorBeforeHVACManagers'' occurs after predictor and before the traditional HVAC managers are called. It occurs at each timestep just after the predictor executes but before SetpointManager and AvailabilityManager models are called. It is useful for a variety of control actions. However, if there are conflicts, the EMS control actions could be overwritten by other SetpointManager or AvailabilityManager actions.
diff --git a/doc/ems-application-guide/src/ems-calling-points/begin-new-environment.tex b/doc/ems-application-guide/src/ems-calling-points/begin-new-environment.tex
new file mode 100644
index 00000000000..4207522b2a0
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/begin-new-environment.tex
@@ -0,0 +1,3 @@
+\section{Begin New Environment}\label{begin-new-environment}
+
+The calling point referred to with the keyword ``BeginNewEnvironment'' occurs once near the beginning of each environment period. Environment periods include sizing periods, design days, and run periods. This calling point will not be useful for control actions, but is useful for initializing variables and calculations that do not need to be repeated during each timestep. Once a value is set, Erl variables remember the value during the course of a simulation. Considerable repetition can be avoided by designing Erl programs to use this calling point for initializations and calculations that are needed only once. It is not called during individual timesteps.
diff --git a/doc/ems-application-guide/src/ems-calling-points/begin-timestep-before-predictor.tex b/doc/ems-application-guide/src/ems-calling-points/begin-timestep-before-predictor.tex
new file mode 100644
index 00000000000..84592ebbaa1
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/begin-timestep-before-predictor.tex
@@ -0,0 +1,3 @@
+\section{Begin Timestep Before Predictor}\label{begin-timestep-before-predictor}
+
+The calling point called ``BeginTimestepBeforePredictor'' occurs near the beginning of each timestep but before the predictor executes. ``Predictor'' refers to the step in EnergyPlus modeling when the zone loads are calculated. This calling point is useful for controlling components that affect the thermal loads the HVAC systems will then attempt to meet. Programs called from this point might actuate the building envelope or internal gains based on current weather or on the results from the previous timestep. Demand management routines might use this calling point to reduce lighting or process loads, change thermostat settings, operate window shades, etc.
diff --git a/doc/ems-application-guide/src/ems-calling-points/end-of-system-sizing.tex b/doc/ems-application-guide/src/ems-calling-points/end-of-system-sizing.tex
new file mode 100644
index 00000000000..e096dce63fb
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/end-of-system-sizing.tex
@@ -0,0 +1,3 @@
+\section{End of System Sizing}\label{end-of-system-sizing}
+
+The calling point called ``EndOfSystemSizing'' is used to alter the results of air system sizing calculations. It executes only once per simulation and is not useful for control applications.
diff --git a/doc/ems-application-guide/src/ems-calling-points/end-of-system-timestep-after-hvac-reporting.tex b/doc/ems-application-guide/src/ems-calling-points/end-of-system-timestep-after-hvac-reporting.tex
new file mode 100644
index 00000000000..01b02f530d6
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/end-of-system-timestep-after-hvac-reporting.tex
@@ -0,0 +1,3 @@
+\section{End of System Timestep After HVAC Reporting}\label{end-of-system-timestep-after-hvac-reporting}
+
+The calling point called ``EndOfSystemTimestepAfterHVACReporting'' occurs at the end of a system timestep after output variable reporting is finalized.
diff --git a/doc/ems-application-guide/src/ems-calling-points/end-of-system-timestep-before-hvac-reporting.tex b/doc/ems-application-guide/src/ems-calling-points/end-of-system-timestep-before-hvac-reporting.tex
new file mode 100644
index 00000000000..ec3df540824
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/end-of-system-timestep-before-hvac-reporting.tex
@@ -0,0 +1,3 @@
+\section{End of System Timestep Before HVAC Reporting}\label{end-of-system-timestep-before-hvac-reporting}
+
+The calling point called ``EndOfSystemTimestepBeforeHVACReporting'' occurs near the end of a system timestep but before output variable reporting is finalized. It is useful for custom output variables that use the SystemTimestep reporting frequency.
diff --git a/doc/ems-application-guide/src/ems-calling-points/end-of-zone-sizing.tex b/doc/ems-application-guide/src/ems-calling-points/end-of-zone-sizing.tex
new file mode 100644
index 00000000000..3f241fa3151
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/end-of-zone-sizing.tex
@@ -0,0 +1,3 @@
+\section{End of Zone Sizing}\label{end-of-zone-sizing}
+
+The calling point called ``EndOfZoneSizing'' is used to alter the results of zone sizing calculations. It executes only once per simulation during the early stages and only if the model includes zone sizing calculations. It is not useful for control applications.
diff --git a/doc/ems-application-guide/src/ems-calling-points/end-of-zone-timestep-after-reporting.tex b/doc/ems-application-guide/src/ems-calling-points/end-of-zone-timestep-after-reporting.tex
new file mode 100644
index 00000000000..e68092a7ce5
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/end-of-zone-timestep-after-reporting.tex
@@ -0,0 +1,3 @@
+\section{End of Zone Timestep After Reporting}\label{end-of-zone-timestep-after-reporting}
+
+The calling point called ``EndOfZoneTimestepAfterZoneReporting'' occurs at the end of a zone timestep after output variable reporting is finalized. It is useful for preparing calculations that will go into effect the next timestep. Its capabilities are similar to BeginTimestepBeforePredictor, except that input data for current time, date, and weather data align with different timesteps.
diff --git a/doc/ems-application-guide/src/ems-calling-points/end-of-zone-timestep-before-reporting.tex b/doc/ems-application-guide/src/ems-calling-points/end-of-zone-timestep-before-reporting.tex
new file mode 100644
index 00000000000..62353f4e6c3
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/end-of-zone-timestep-before-reporting.tex
@@ -0,0 +1,3 @@
+\section{End of Zone Timestep Before Reporting}\label{end-of-zone-timestep-before-reporting}
+
+The calling point called ``EndOfZoneTimestepBeforeZoneReporting'' occurs near the end of a zone timestep but before output variable reporting is finalized. It is useful for custom output variables that use the ZoneTimestep reporting frequency.
diff --git a/doc/ems-application-guide/src/ems-calling-points/inside-hvac-system-iteration-loop.tex b/doc/ems-application-guide/src/ems-calling-points/inside-hvac-system-iteration-loop.tex
new file mode 100644
index 00000000000..0b4c70b6dd6
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/inside-hvac-system-iteration-loop.tex
@@ -0,0 +1,3 @@
+\section{Inside HVAC System Iteration Loop}\label{inside-hvac-system-iteration-loop}
+
+The calling point called ``InsideHVACSystemIterationLoop'' occurs before HVAC systems are modeled. Within a timestep, EnergyPlus loops over the HVAC model to solve a system of systems. It recurs after each HVAC system iteration within each timestep and can be used for a variety of control actions that affect system operation. Being within the iteration loop can increase the accuracy of control modeling when the inputs to the controls are also changing interactively. The disadvantage is extra computational expense.
diff --git a/doc/ems-application-guide/src/ems-calling-points/user-defined-component-model.tex b/doc/ems-application-guide/src/ems-calling-points/user-defined-component-model.tex
new file mode 100644
index 00000000000..f98467038d8
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-calling-points/user-defined-component-model.tex
@@ -0,0 +1,3 @@
+\section{User Defined Component Model}\label{user-defined-component-model}
+
+The calling point called ``UserDefinedComponentModel'' is used with Erl programs that are associated with user defined component models.~ This calling point is executed whenever a user-defined component model is called to simulate.~ The user defined component models track which program calling managers are associated with the specific component and only those calling managers are executed when this calling point is triggered. This calling point is only used with calling managers referenced by the following input objects: PlantComponent:UserDefined, Coil:UserDefined, ZoneHVAC:ForcedAir:UserDefined, or AirTerminal:SingleDuct:UserDefined.
diff --git a/doc/ems-application-guide/src/ems-examples.tex b/doc/ems-application-guide/src/ems-examples.tex
new file mode 100644
index 00000000000..0691fdd0346
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples.tex
@@ -0,0 +1,5 @@
+\chapter{EMS Examples}\label{ems-examples}
+
+This section provides examples that demonstrate how to use the EMS. Each example provides a problem statement, discusses how to approach a solution using EMS, and provides example EMS input objects. For each example a complete input data file is provided with the EnergyPlus release (you can find this in the ExampleFiles\textbackslash{} directory).
+
+A range of example applications is presented here. Each is presented in isolation for simplicity, but a much more comprehensive approach to EMS programs is also possible.
diff --git a/doc/ems-application-guide/src/ems-examples/example-1-whole-building-average-zone-air.tex b/doc/ems-application-guide/src/ems-examples/example-1-whole-building-average-zone-air.tex
new file mode 100644
index 00000000000..34d937c72b9
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-1-whole-building-average-zone-air.tex
@@ -0,0 +1,134 @@
+\section{Example 1. Whole-Building Average Zone Air Temperature}\label{example-1.-whole-building-average-zone-air-temperature}
+
+\subsection{Problem Statement}\label{problem-statement}
+
+Although EnergyPlus can report an enormous number of output variables, you may want a custom report variable such as one for the average temperature in the building. Only zone-by-zone indoor air temperatures are available. Because it is nearly always important to check that models are properly controlling zone air conditions, you may need to examine air temperature results from your models. Compared to scanning across the many zones in a large building, you could save time when checking a model if you have a single value for a whole-building average temperature. Of course, you could calculate such a value after a run by postprocessing, but redoing this for every run is cumbersome and time consuming. Therefore, it would be more convenient to automatically calculate such a value inside the program and output it in the usual manner. For example, if we take the Small Office Reference Building (RefBldgSmallOfficeNew2004\_Chicago.idf), is there a way to create a custom report variable that provides a weighted average for the indoor temperature of all the occupied zones in a model?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion}
+
+This is a fairly simple example in that the EMS controls nothing. There are no actuators.
+
+The example file has six zones, but one is an attic that we do not care about. Therefore, the main inputs, or EMS sensors, will be the zone air temperatures for the five occupied zones. We will use EnergyManagementSystem:Sensor objects to obtain the values for the air temperatures by mapping to the output variable called ``Zone Mean Air Temperature.''
+
+A model for average temperature can be constructed by using the zone air volumes as weights so larger zones have more influence than smaller zones on the resulting average. The model equation we will implement in EMS for our new report variable is
+
+\begin{equation}
+T_{average} = \frac{\sum\left(T_{zone}\text{Vol}_{zone}\right)}{\sum\left(\text{Vol}_{zone}\right)}
+\end{equation}
+
+The example file specifies the zone volume in its zone objects so we have the data needed for the weighting factors from elsewhere in the IDF. However, a study could vary the geometry such that the volumes differ from one simulation to another. Zone Air Volume is available as internal data, so we will use EnergyManagementSystem:InternalVariable input objects to assign these weighting factors into global Erl variables. If we did not know beforehand that Zone Air Volume was an available internal variable, we would have had to prerun the model with some EMS-related objects and the appropriate level of reporting selected in an Output:EnergyManagementSystem object, and then studied the EDD output file. Note that the EDD file is only produced if you have EMS/Erl programs in your input file.
+
+The custom output variable will be defined by using an EnergyManagementSystem:OutputVariable input object. This requires the Erl variable to be global, so we need to declare a variable. Let's call it AverageBuildingTemp, to be global using an EnergyManagementSystem:GlobalVariable object so we have a way to connect the result calculated in the Erl program to the custom output.
+
+There are two main considerations when selecting an EMS calling point:
+
+\begin{itemize}
+\item
+  The call should be toward the end of the zone timestep so the zone air temperature calculations are finalized.
+\item
+  The call should be before reporting updates so our new value is available before the reporting is finalized.
+\end{itemize}
+
+We therefore choose the EMS calling point with the key of ``EndOfZoneTimestepBeforeReporting.''
+
+\subsection{EMS Input Objects}\label{ems-input-objects}
+
+A set of input objects to solve this problem appears below and is included in the example file called ``EMSCustomOutputVariable.idf.''
+
+\begin{lstlisting}
+
+EnergyManagementSystem:Sensor,
+     T1, !Name
+     Perimeter_ZN_1 ,! Output:Variable or Output:Meter Index Key Name
+     Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
+
+
+   EnergyManagementSystem:Sensor,
+     T2, !Name
+     Perimeter_ZN_2 , ! Output:Variable or Output:Meter Index Key Name
+     Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
+
+
+   EnergyManagementSystem:Sensor,
+     T3, !Name
+     Perimeter_ZN_3 , ! Output:Variable or Output:Meter Index Key Name
+     Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
+
+
+   EnergyManagementSystem:Sensor,
+     T4, !Name
+     Perimeter_ZN_4, ! Output:Variable or Output:Meter Index Key Name
+     Zone Mean Air Temperature ;! Output:Variable or Output:Meter Name
+
+
+   EnergyManagementSystem:Sensor,
+     T5, !Name
+     Core_ZN , ! Output:Variable or Output:Meter Index Key Name
+     Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
+
+
+   EnergyManagementSystem:ProgramCallingManager,
+     Average Building Temperature , ! Name
+     EndOfZoneTimestepBeforeZoneReporting , ! EnergyPlus Model Calling Point
+     AverageZoneTemps ; ! Program Name 1
+
+
+   EnergyManagementSystem:GlobalVariable,
+     AverageBuildingTemp;
+
+
+   EnergyManagementSystem:OutputVariable,
+     Weighted Average Building Zone Air Temperature [C], ! Name
+     AverageBuildingTemp, ! EMS Variable Name
+     Averaged, ! Type of Data in Variable
+     ZoneTimeStep ; ! Update Frequency
+
+
+   EnergyManagementSystem:InternalVariable,
+     Zn1vol,
+     Perimeter_ZN_1,
+     Zone Air Volume;
+
+
+   EnergyManagementSystem:InternalVariable,
+     Zn2vol,
+     Perimeter_ZN_2,
+     Zone Air Volume;
+
+
+   EnergyManagementSystem:InternalVariable,
+     Zn3vol,
+     Perimeter_ZN_3,
+     Zone Air Volume;
+
+
+   EnergyManagementSystem:InternalVariable,
+     Zn4vol,
+     Perimeter_ZN_4,
+     Zone Air Volume;
+
+
+   EnergyManagementSystem:InternalVariable,
+     Zn5vol,
+     Core_ZN ,
+     Zone Air Volume;
+
+
+   EnergyManagementSystem:Program,
+     AverageZoneTemps , ! Name
+     SET SumNumerator = T1*Zn1vol + T2*Zn2vol + T3*Zn3vol + T4*Zn4vol + T5*Zn5vol,
+     SET SumDenominator = Zn1vol + Zn2vol + Zn3vol + Zn4vol + Zn5vol,
+     SET AverageBuildingTemp = SumNumerator / SumDenominator;
+
+
+   Output:EnergyManagementSystem,
+     Verbose,
+     Verbose,
+     Verbose;
+
+
+   Output:Variable,
+     *,                       !- Key Value
+     Weighted Average Building Zone Air Temperature,  !- Variable Name
+     timestep;                  !- Reporting Frequency
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-10-plant-loop-override-control.tex b/doc/ems-application-guide/src/ems-examples/example-10-plant-loop-override-control.tex
new file mode 100644
index 00000000000..353aaed1e58
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-10-plant-loop-override-control.tex
@@ -0,0 +1,87 @@
+\section{Example 10. Plant Loop Override Control}\label{example-10.-plant-loop-override-control}
+
+\subsection{Problem Statement}\label{problem-statement-000}
+
+A common occurrence in EnergyPlus central plant simulations is for a component to be designed well, but during the course of an annual simulation, it is operated outside of its allowable region.~ This is due to the governing control strategies (operating schemes).~ These operation schemes may not have the intelligence to say, turn off a cooling tower when the outdoor temperature is too low.
+
+Within the EnergyPlus example files, the cooling tower offers warnings stating that the tower temperature is going below a low temperature limit.~ We should ask, can we use a simple EMS addition to an input file to override the loop and turn off the cooling tower to avoid these situations and therefore the warnings?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-000}
+
+For this example, we will start with the example file that is packaged with EnergyPlus called EcoRoofOrlando.idf.~ This is one example of an input file where a cooling tower throws warnings due to operating at too low of a temperature.~ Although the input file has many aspects related to zone and HVAC, we will only be interested in the loop containing the tower, which is a \emph{CondenserLoop} named \emph{Chiller Plant Condenser Loop.} The loop has a minimum loop temperature of 5 degrees Celsius, as specified by the \emph{CondenserLoop} object.
+
+In order to avoid these warnings and properly shut off the tower, EMS will be used to check the outdoor temperature and shut down the whole loop.~ Special care must be taken when manipulating plant and condenser loops with EMS.~ The most robust way found is to both disable the loop equipment and also override (turn off) the loop.~ Skipping either of these can cause mismatches where either components are still expecting flow but the pump is not running, or the pump is trying to force flow through components which are disabled.~ Either of these cases can cause unstable conditions and possibly fatal flow errors.
+
+The outdoor air temperature must be checked in order to determine what the EMS needs to do at a particular point in the simulation.~ This is handled by use of an EMS sensor monitoring the Outdoor Dry Bulb standard E+ output variable.
+
+To manage the loop and pump, actuators are employed on both.~ The pump actuator is a mass flow rate override.~ This can be used to set the flow to zero, effectively shutting off the pump.~ The loop actuator is an on/off supervisory control, which allows you to ``shut the entire loop down.''~ This actuator will not actually shut the loop down, it effectively empties the equipment availability list, so that there is no equipment available to reject/absorb load on the supply side.~ If you use this actuator alone to ``shut down the loop,'' you may find that the pump is still flowing fluid around the loop, but the equipment will not be running.
+
+The EMS calling point chosen is ``\emph{InsideHVACSystemIterationLoop,}'' so that the operation will be updated every time the plant loops are simulated.
+
+The Erl program is quite simple for this case.~ If the outdoor dry bulb temperature goes below a certain value, the loop and pump actuators are set to zero.~ If the outdoor temperature is equal to or above this value, the actuators are set to \emph{Null}, relinquishing control back to the regular operation schemes.~ In modifying this specific input file it was found that the outdoor dry bulb temperature which removed these warnings was six degrees Celsius.~ We also create a custom output variable called ``EMS Condenser Flow Override On'' to easily record when the overrides have occurred.
+
+\subsection{EMS Input Objects}\label{ems-input-objects-000}
+
+The main input objects that implement this example of plant loop control are listed below and are included in the example file called ``EMSPlantLoopOverrideControl.idf.''~ The addition of the EMS objects properly shuts down the loop as the outdoor temperature go below the transition value, and the simulation error file shows no warnings for the tower outlet temperature.
+
+\begin{lstlisting}
+
+  EnergyManagementSystem:Sensor,
+      OutdoorTemp,         !- Name
+      Environment,         !- Output:Variable Index Key Name
+      Site Outdoor Air Drybulb Temperature;    !- Output:Variable Name
+
+
+    EnergyManagementSystem:Actuator,
+      Actuator_Loop,       !- Name
+      Chiller Plant Condenser Loop, !- Actuated Component Unique Name
+      Plant Loop Overall,  !- Actuated Component Type
+      On/Off Supervisory;  !- Actuated Component Control Type
+
+
+    EnergyManagementSystem:Actuator,
+      PumpFlowOverride,    !- Name
+      Chiller Plant Cnd Circ Pump,  !- Actuated Component Unique Name
+      Pump,                !- Actuated Component Type
+      Pump Mass Flow Rate; !- Actuated Component Control Type
+
+
+    EnergyManagementSystem:GlobalVariable,
+      PumpFlowOverrideReport;
+
+
+    EnergyManagementSystem:OutputVariable,
+      EMS Condenser Flow Override On [On/Off], !- Name
+      PumpFlowOverrideReport,    !- EMS Variable Name
+      Averaged,            !- Type of Data in Variable
+      SystemTimeStep;      !- Update Frequency
+
+
+
+
+
+
+    EnergyManagementSystem:ProgramCallingManager,
+      Condenser OnOff Management,
+      InsideHVACSystemIterationLoop,
+      TowerControl;
+
+
+    EnergyManagementSystem:Program,
+      TowerControl,
+      IF (OutdoorTemp < 6.0),
+        SET Actuator_Loop = 0.0,
+        SET PumpFlowOverride = 0.0,
+        SET PumpFlowOverrideReport = 1.0,
+      ELSE,
+        SET Actuator_Loop = Null,
+        SET PumpFlowOverride = Null,
+        SET PumpFlowOverrideReport = 0.0,
+      ENDIF;
+
+
+    Output:Variable,
+      *,
+      EMS Condenser Flow Override On,
+      Hourly;
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-11-performance-curve-result-override.tex b/doc/ems-application-guide/src/ems-examples/example-11-performance-curve-result-override.tex
new file mode 100644
index 00000000000..4d986d9c2d7
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-11-performance-curve-result-override.tex
@@ -0,0 +1,182 @@
+\section{Example 11. Performance Curve Result Override}\label{example-11.-performance-curve-result-override}
+
+\subsection{Problem Statement}\label{problem-statement-001}
+
+The output of EnergyPlus performance curves (or tables) can be modified as necessary to simulate hardware or controls that cannot be accurately realized using a single performance curve. This example describes a method for modifying the capacity of a DX cooling coil via the DX coil objects Total Cooling Capacity Function of Temperature performance curve object.
+
+A particular manufacturer controls the DX cooling coil such that the capacity of the coil changes at 31°C outdoor air dry-bulb temperature. The following EMS program logic will calculate alternate inputs for cooling coil capacity and over-write the existing performance curve results.
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-001}
+
+For this example, we will start with the equation for cooling capacity of the DX coil object (ref. Coil:Cooling:DX:SingleSpeed). From the engineering reference, the equation used to calculate the cooling capacity is:
+
+\begin{equation}
+\text{TotCapTempModFac} = a + b \left( T_{wb,i} \right) + c \left( T_{wb,i} \right) + d \left( T_{c,i} \right) + e \left( T_{c,i} \right) + f \left( T_{wb,i} \right)\left( T_{c,i} \right)
+\end{equation}
+
+The first term (Twb,i) refers to the cooling coil inlet air wet-bulb temperature and the second (Tc,i) refers to the outdoor condenser inlet air dry-bulb temperature. Using the EMS, a new total capacity as a function of temperature value will be calculated and used during the simulation. The Energyplus input objects for the cooling coil capacity curve, the associated outdoor air mixer object, and the original cooling capacity performance curve are shown here.
+
+\begin{lstlisting}
+
+  Coil:Cooling:DX:SingleSpeed,
+      Zone1PTHPDXCoolCoil,     !- Name
+      CoolingCoilAvailSched,   !- Availability Schedule Name
+      8750.0,                  !- Rated Total Cooling Capacity {W}
+      0.75,                    !- Rated Sensible Heat Ratio
+      3.0,                     !- Rated COP
+      0.5,                     !- Rated Air Flow Rate {m3/s}
+      ,          !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
+      Zone1PTHPFanOutletNode,  !- Air Inlet Node Name
+      Zone1PTHPDXCoolCoilOutletNode,  !- Air Outlet Node Name
+      HPACCoolCapFT,    !- Total Cooling Capacity f(Temperature) Curve Name
+      HPACCoolCapFFF,   !- Total Cooling Capacity f(Flow Fraction) Curve Name
+      HPACEIRFT,        !- Energy Input Ratio f(Temperature) Curve Name
+      HPACEIRFFF,       !- Energy Input Ratio f(Flow Fraction) Curve Name
+      HPACPLFFPLR;      !- Part Load Fraction Correlation Curve Name
+
+
+    OutdoorAir:Mixer,
+      Zone1PTHPOAMixer,        !- Name
+      Zone1PTHPOAMixerOutletNode,  !- Mixed Air Node Name
+      Zone1PTHPOAInNode,       !- Outdoor Air Stream Node Name
+      Zone1PTHPExhNode,        !- Relief Air Stream Node Name
+      Zone1PTHPAirInletNode;   !- Return Air Stream Node Name
+
+
+    Curve:Biquadratic,
+      HPACCoolCapFT,           !- Name
+      0.942587793,             !- Coefficient1 Constant
+      0.009543347,             !- Coefficient2 x
+      0.000683770,             !- Coefficient3 x**2
+      -0.011042676,            !- Coefficient4 y
+      0.000005249,             !- Coefficient5 y**2
+      -0.000009720,            !- Coefficient6 x*y
+\end{lstlisting}
+
+Note that the Total Cooling Capacity Function of Temperature Curve Name is HPACCoolCapFT and the inlet air node for this cooling coil is Zone1PTHPFanOutletNode. From the mixer object, the outdoor air node name is Zone1PTHPOAInNode. The existing cooling capacity performance curve name is HPACCoolCapFT. These node or object names will be used in the EMS program to point to the node or object as required.
+
+\subsection{EMS Input Objects}\label{ems-input-objects-001}
+
+The main input objects that implement this example for over-riding a performance curve result are listed below. Note that the node wet-bulb temperature at the inlet node of the cooling coil is calculated both using the node wet-bulb temperature and the psychrometric function to calculate a wet-bulb temperature from dry-bulb temperature and humidity ratio. The node wet-bulb temperature EMS sensor is left in this example for the sole purpose of showing how to access this node variable in a direct and indirect manner.
+
+Referring to the cooling capacity equation above, a new equation must be developed to represent this same performance aspect of the cooling coil. Since, in this example, the cooling capacity changes at 31°C, one of the coefficients is modified and used in the IF block to modify the cooling capacity above and below this outdoor air temperature limit. Note also that the coefficients used in the EMS program are all positive values and the negative sign is accounted for the CurveInput equation. Also, the value of C2 was changed to a negative value to represent the change in performance at 31°C. To calculate the new performance curve results, EMS sensors are placed at the cooling coil air inlet node to capture air dry-bulb temperature and humidity ratio, and at the outdoor air mixer outdoor air node inlet to capture outdoor air dry-bulb temperature and pressure. The curve input equation is identical to the equation shown above except that 1) the equation coefficients are all positive and any negative coefficients are accounted for in the equation itself, and 2) alternate coefficients (actually only C2a in this example) are used for the second equation. The results of this example show a marked difference in the cooling capacity above 31°C.
+
+\begin{lstlisting}
+
+  EnergyManagementSystem:ProgramCallingManager,
+      EMSBasedCurveManager,  !- Name
+      AfterPredictorBeforeHVACManagers,  !- EnergyPlus Model Calling Point
+      CurveOverwriteMGR;     !- Program Name 1
+
+
+    EnergyManagementSystem:Program,
+      CurveOverwriteMGR,
+      SET TTmp = CoilInletDBT,
+      SET WTmp = CoilInletW,
+      SET PTmp = Pressure,
+      SET MyWB = @TwbFnTdbWPb TTmp WTmp PTmp,
+      SET IVOne = CoilInletWBT,
+      SET IVOne = MyWB,
+      SET IVTwo = OAT,
+      SET IVThree = IVOne*IVTwo,
+      SET C1 = 0.942567793,
+      SET C2 = 0.009543347,
+      SET C2a = 0.009543347, !-  -0.009543347
+      SET C3 = 0.00068377,
+      SET C4 = 0.011042676, !-  -0.011042676
+      SET C5 = 0.000005249,
+      SET C6 = 0.000009720, !-  -0.000009720
+      IF OAT < 31.0,
+        SET CurveInput = C1 + (C2*IVOne) + (C3*IVOne*IVone) - (C4*IVTwo) + (C5*IVTwo*IVTwo) - (C6*IVThree),
+      ELSE,
+        SET CurveInput = C1 - (C2a*IVOne) + (C3*IVOne*IVone) - (C4*IVTwo) + (C5*IVTwo*IVTwo) - (C6*IVThree),
+      ENDIF,
+      SET CurveOverwrite = CurveInput;
+
+
+
+
+    EnergyManagementSystem:Actuator,
+      CurveOverwrite,    !- Name
+      HPACCOOLCAPFT,     !- Actuated Component Unique Name
+      Curve,             !- Actuated Component Type
+      Curve Result;      !- Actuated Component Control Type
+
+
+    EnergyManagementSystem:Sensor,
+      ActualCurve,           !- Name
+      HPACCOOLCAPFT,     !- Output:Variable or Output:Meter Index Key Name
+      Performance Curve Output Value;  !- Output:Variable or Output:Meter Name
+
+
+    EnergyManagementSystem:Sensor,
+      CoilInletWBT,          !- Name
+      Zone1PTHPFanOutletNode, !- Output:Variable or Output:Meter Index Key Name
+      System Node Wetbulb Temperature; !- Output:Variable or Output:Meter Name
+
+
+    EnergyManagementSystem:Sensor,
+      Pressure,          !- Name
+      Zone1PTHPOAInNode,     !- Output:Variable or Output:Meter Index Key Name
+      System Node Pressure ;  !- Output:Variable or Output:Meter Name
+
+
+    EnergyManagementSystem:Sensor,
+      CoilInletDBT,          !- Name
+      Zone1PTHPFanOutletNode, !- Output:Variable or Output:Meter Index Key Name
+      System Node Temperature;  !- Output:Variable or Output:Meter Name
+
+
+    EnergyManagementSystem:Sensor,
+      CoilInletW,          !- Name
+      Zone1PTHPFanOutletNode, !- Output:Variable or Output:Meter Index Key Name
+      System Node Humidity Ratio;  !- Output:Variable or Output:Meter Name
+
+
+    EnergyManagementSystem:Sensor,
+      OAT,          !- Name
+      Zone1PTHPOAInNode,     !- Output:Variable or Output:Meter Index Key Name
+      System Node Temperature;  !- Output:Variable or Output:Meter Name
+
+
+    EnergyManagementSystem:OutputVariable,
+      ERLCurveValue, ! Name
+      ActualCurve,   ! EMS Variable Name
+      Averaged,      ! Type of Data in Variable
+      ZoneTimeStep ; ! Update Frequency
+
+
+    EnergyManagementSystem:OutputVariable,
+      NewCurveValue, ! Name
+      CurveInput,    ! EMS Variable Name
+      Averaged,      ! Type of Data in Variable
+      ZoneTimeStep ; ! Update Frequency
+
+
+    Output:EnergyManagementSystem,
+      Verbose,       !- Actuator Availability Dictionary Reporting
+      Verbose,       !- Internal Variable Availability Dictionary Reporting
+      Verbose;       !- EMS Runtime Language Debug Output Level
+
+
+    Output:Variable,
+      *,
+      ERLCurveValue,
+      Hourly;
+
+
+   Output:Variable, HPACCOOLCAPFT,
+       Performance Curve Output Value,Hourly;
+   Output:Variable, HPACCOOLCAPFT,
+       Performance Curve Input Variable 1 Value,Hourly;
+   Output:Variable, HPACCOOLCAPFT,
+       Performance Curve Input Variable 2 Value,Hourly;
+   Output:Variable, Zone1PTHPFanOutletNode,
+       System Node Wetbulb Temperature, Hourly;
+\end{lstlisting}
+
+\begin{figure}[hbtp] % fig 4
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image011.jpg}
+\caption{Results of Performance Curve Override \protect \label{fig:results-of-performance-curve-override}}
+\end{figure}
diff --git a/doc/ems-application-guide/src/ems-examples/example-12-variable-refrigerant-flow-system.tex b/doc/ems-application-guide/src/ems-examples/example-12-variable-refrigerant-flow-system.tex
new file mode 100644
index 00000000000..66dc8d16f08
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-12-variable-refrigerant-flow-system.tex
@@ -0,0 +1,81 @@
+\section{Example 12. Variable Refrigerant Flow System Override}\label{example-12.-variable-refrigerant-flow-system-override}
+
+\subsection{Problem Statement}\label{problem-statement-002}
+
+The variable refrigerant flow heat pump air conditioner has several available thermostat control options. These operation control schemes may not provide the type of control desired. How can we use a simple EMS addition to an input file that can override the specified thermostat control logic and set an alternate mode of operation?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-002}
+
+Depending on the type of thermostat control logic, the EnergyPlus program will review the loads in each zone, the number of zones in cooling or heating, the deviation from set point temperature, etc. to determine the mode of operation for the heat pump condenser. Alternate control logic may be developed to more accurately reflect the operation of a specific manufacturers product, or investigate other control techniques. This control logic may be added to an input file and used as the operating control logic of the heat pump.
+
+This simple example shows how to use EMS actuators to SET the operating mode and cause a specific terminal unit to operate at a specified part-load ratio (PLR). When setting the terminal unit PLR, the terminal unit will turn on only if the condenser is allowed to operate according to the minimum and maximum outdoor temperature limits.
+
+\subsection{EMS Input Objects}\label{ems-input-objects-002}
+
+The main input objects that implement this example are the variable refrigerant flow actuators that control the VRF system and specific terminal unit. Note that the terminal unit PLR can be controlled without controlling the mode of the VRF condenser, however, the specific terminal unit will operate in whatever mode the existing operation control scheme chooses. This example program simply ``sets'' the operating mode and PLR, other more complex control algorithms can be developed by the user as needed.
+
+\begin{lstlisting}
+
+  Output:EnergyManagementSystem,
+      Verbose,                 !- Actuator Availability Dictionary Reporting
+      Verbose,                 !- Internal Variable Availability Dictionary Reporting
+      Verbose;                 !- EMS Runtime Language Debug Output Level
+
+
+    EnergyManagementSystem:ProgramCallingManager,
+      VRF OnOff Management,     !- Name
+      InsideHVACSystemIterationLoop,  !- EnergyPlus Model Calling Point
+      VRFControl;               !- Program Name 1
+
+
+    EnergyManagementSystem:Program,
+      VRFControl,               !- Name
+      SET VRF_Actuator_OnOff = VRF_Status_Heating, !- Program Line 2
+      SET VRF_TerminalUnit1_PLR = 0.5;
+
+
+    EnergyManagementSystem:Actuator,
+      VRF_Actuator_OnOff,       !- Name
+      VRF Heat Pump,            !- Actuated Component Unique Name
+      Variable Refrigerant Flow Heat Pump,      !- Actuated Component Type
+      Operating Mode;           !- Actuated Component Control Type
+
+
+    EnergyManagementSystem:Actuator,
+      VRF_TerminalUnit1_PLR,    !- Name
+      TU1,                      !- Actuated Component Unique Name
+      Variable Refrigerant Flow Terminal Unit,  !- Actuated Component Type
+      Part Load Ratio;          !- Actuated Component Control Type
+
+
+    EnergyManagementSystem:OutputVariable,
+      Erl VRF Control Status,   !- Name
+      VRF_Actuator_OnOff,       !- EMS Variable Name
+      Averaged,                 !- Type of Data in Variable
+      SystemTimeStep;           !- Update Frequency
+
+
+    Output:Variable,*,Erl VRF Control Status, detailed;
+    Output:Variable,*,VRF Heat Pump Operating Mode, detailed;
+    Output:Variable,*,Cooling Coil Runtime Fraction, detailed;
+    Output:Variable,*,Heating Coil Runtime Fraction, detailed;
+
+
+    EnergyManagementSystem:ProgramCallingManager,
+      Init VRF Control Mode Constants,  !- Name
+      BeginNewEnvironment,           !- EnergyPlus Model Calling Point
+      InitializeVRFControlModes;     !- Program Name 1
+
+
+    EnergyManagementSystem:Program,
+      InitializeVRFControlModes,     !- Name
+      Set VRF_Status_Off = 0.0,      !- Program Line 1
+      Set VRF_Status_Cooling = 1.0,  !- Program Line 2
+      Set VRF_Status_Heating = 2.0;  !- Program Line 3
+
+
+    EnergyManagementSystem:GlobalVariable,
+      VRF_Status_Off,                !- Erl Variable 1 Name
+      VRF_Status_Cooling,            !- Erl Variable 2 Name
+      VRF_Status_Heating;            !- Erl Variable 3 Name
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-13-surface-construction-actuator-for.tex b/doc/ems-application-guide/src/ems-examples/example-13-surface-construction-actuator-for.tex
new file mode 100644
index 00000000000..d2a7f228ca0
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-13-surface-construction-actuator-for.tex
@@ -0,0 +1,141 @@
+\section{Example 13. Surface Construction Actuator for Thermochromic Window}\label{example-13.-surface-construction-actuator-for-thermochromic-window}
+
+\subsection{Problem Statement}\label{problem-statement-003}
+
+There are a variety of novel new technologies for dynamic thermal envelopes that are the subject of research and development. Can we use EMS to investigate dynamic envelope technologies?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-003}
+
+As an example, we will show how to use the EMS to replicate a thermochromic window.~ EnergyPlus already has a dedicated model for thermochromic windows (see the input object WindowMaterial:GlazingGroup:Thermochromic) that is demonstrated in the example file called ThermochromicWindow.idf.~ For this EMS example we will start with that file, remove the WindowMaterial:GlazingGroup:Thermochromic and emulate the thermochromic window using the EMS actuator called ``Surface'' with the control type ``Construction State.''
+
+The first step is to create the individual Construction objects that will represent the individual states.~ The original thermochromic example file already includes a series of WindowMaterial:Glazing input objects that correspond to the properties of the thermochromic glazing at different temperatures.~ These glazing layers are then used in a series of Construction objects that represent the entire glazing system description at each temperature ``state.''~ Separate EnergyManagementSystem:ConstructionIndexVariable objects are then added for each Construction to setup Erl variables that point to each construction.
+
+The control algorithm is very simple.~ The temperature of the glazing is used in a long IF-ELSEIF-ELSE-ENDIF block to select the appropriate construction to assign the surface.~ In this case the native thermochromic model has an important advantage in that the dedicated model can access the temperature of the middle pane in a triple glazed window whereas the EMS model can only access the temperature of the outside pane or the inside pane.~ Here we use the temperature of the outside face of the surface because it is closer to the temperature of the middle pane (which can be much higher when in direct sun).
+
+\subsection{EMS Input Objects}\label{ems-input-objects-003}
+
+The main input objects that implement this example of EMS-based thermochromic glazing system are listed below.~ The surface called ``Perimeter\_ZN\_1\_wall\_south\_Window\_1'' is the one being actuated by EMS and we can observe the outcomes of the override by reporting the output variable called Surface Construction Index.~ See the example file called EMSThermochromicWindow.idf.
+
+\begin{lstlisting}
+
+  Construction,
+      TCwindow_25,                !- Name
+      Clear3PPG,               !- Outside Layer
+      AIR 3MM,                 !- Layer 2
+      WO18RT25,              !- Layer 3
+      AIR 8MM,                 !- Layer 4
+      SB60Clear3PPG;           !- Layer 5
+
+
+    EnergyManagementSystem:ConstructionIndexVariable,
+      TCwindow_25,
+      TCwindow_25;
+
+
+    Construction,
+      TCwindow_27,                !- Name
+      Clear3PPG,               !- Outside Layer
+      AIR 3MM,                 !- Layer 2
+      WO18RT27,              !- Layer 3
+      AIR 8MM,                 !- Layer 4
+      SB60Clear3PPG;           !- Layer 5
+
+
+    EnergyManagementSystem:ConstructionIndexVariable,
+      TCwindow_27,
+      TCwindow_27;
+  <<SNIPPED states between 27C and 80C>>
+
+
+    Construction,
+      TCwindow_80,                !- Name
+      Clear3PPG,               !- Outside Layer
+      AIR 3MM,                 !- Layer 2
+      WO18RT80,              !- Layer 3
+      AIR 8MM,                 !- Layer 4
+      SB60Clear3PPG;           !- Layer 5
+
+
+    EnergyManagementSystem:ConstructionIndexVariable,
+      TCwindow_80,
+      TCwindow_80;
+
+
+    Construction,
+      TCwindow_85,                !- Name
+      Clear3PPG,               !- Outside Layer
+      AIR 3MM,                 !- Layer 2
+      WO18RT85,              !- Layer 3
+      AIR 8MM,                 !- Layer 4
+      SB60Clear3PPG;           !- Layer 5
+
+
+    EnergyManagementSystem:ConstructionIndexVariable,
+      TCwindow_85,
+      TCwindow_85;
+
+
+    EnergyManagementSystem:Sensor,
+      Win1_Tout,
+      Perimeter_ZN_1_wall_south_Window_1,
+      Surface Outside Face Temperature;
+
+
+    EnergyManagementSystem:Actuator,
+      Win1_Construct,
+      Perimeter_ZN_1_wall_south_Window_1,
+      Surface,
+      Construction State;
+
+
+    EnergyManagementSystem:ProgramCallingManager,
+      My thermochromic window emulator,
+      BeginTimestepBeforePredictor,
+      ZN_1_wall_south_Window_1_Control;
+
+
+    EnergyManagementSystem:Program,
+      ZN_1_wall_south_Window_1_Control,
+      IF Win1_Tout < = 26.0 ,
+        Set Win1_Construct = TCwindow_25,
+      ELSEIF Win1_Tout < = 28.0 ,
+        SEt Win1_Construct = TCwindow_27,
+      ELSEIF Win1_Tout < = 30.0 ,
+        SET Win1_Construct = TCwindow_29,
+      ELSEIF Win1_Tout < = 32.0 ,
+        SET Win1_Construct = TCwindow_31,
+      ELSEIF Win1_Tout < = 34.0 ,
+        SET Win1_Construct = TCwindow_33,
+      ELSEIF Win1_Tout < = 36.0 ,
+        SET Win1_Construct = TCwindow_35,
+      ELSEIF Win1_Tout < = 38.0 ,
+        SET Win1_Construct = TCwindow_37,
+      ELSEIF Win1_Tout < = 40.0 ,
+        SET Win1_Construct = TCwindow_39,
+      ELSEIF Win1_Tout < = 42.0 ,
+        SET Win1_Construct = TCwindow_41,
+      ELSEIF Win1_Tout < = 44.0 ,
+        SET Win1_Construct = TCwindow_43,
+      ELSEIF Win1_Tout < = 47.5 ,
+        SET Win1_Construct = TCwindow_45,
+      ELSEIF Win1_Tout < = 52.5 ,
+        SET Win1_Construct = TCwindow_50,
+      ELSEIF Win1_Tout < = 57.5 ,
+        SET Win1_Construct = TCwindow_55,
+      ELSEIF Win1_Tout < = 62.5 ,
+        SET Win1_Construct = TCwindow_60,
+      ELSEIF Win1_Tout < = 67.5 ,
+        SET Win1_Construct = TCwindow_65,
+      ELSEIF Win1_Tout < = 72.5 ,
+        SET Win1_Construct = TCwindow_70,
+      ELSEIF Win1_Tout < = 77.5 ,
+        SET Win1_Construct = TCwindow_75,
+      ELSEIF Win1_Tout < = 82.5 ,
+        SET Win1_Construct = TCwindow_80,
+      ELSE ,
+        SET Win1_Construct = TCwindow_85,
+      ENDIF;
+
+
+  Output:Variable, Perimeter_ZN_1_wall_south_Window_1, Surface Construction Index, timestep;
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-2-traditional-setpoint.tex b/doc/ems-application-guide/src/ems-examples/example-2-traditional-setpoint.tex
new file mode 100644
index 00000000000..585d20613fe
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-2-traditional-setpoint.tex
@@ -0,0 +1,182 @@
+\section{Example 2. Traditional Setpoint and Availability Managers}\label{example-2.-traditional-setpoint-and-availability-managers}
+
+\subsection{Problem Statement}\label{problem-statement-004}
+
+The traditional way of modeling supervisory control of HVAC systems in EnergyPlus is to use SetpointManagers and AvailabilityManagers. To gain experience with EMS, we should ask, Is there a way to take a model such as the Large Office Reference Building (RefBldgLargeOfficeNew2004\_Chicago.idf) and replicate the traditional HVAC managers by using only the EMS?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-004}
+
+A review of the example file shows that three types of traditional HVAC managers are being used:~ scheduled setpoints, mixed air setpoints, and night cycle availability. We will discuss these separately.
+
+The input object SetpointManager:Scheduled functions by placing a setpoint value on a specified node based on the value in a schedule. Therefore, our EMS program will do the same. First we will need to access the schedule. In this example, a schedule called Seasonal-Reset-Supply-Air-Temp-Sch contains the temperature values desired for the air system's supply deck. We use an EnergyManagementSystem:Sensor object based on the output variable called ``Schedule Value'' to fill schedule values into an Erl variable called Seasonal\_Reset\_SAT\_Sched. Once we have the sensor and actuator setup, putting the setpoint on the node involves a single line of Erl code, ``SET VAV\_1\_SAT\_setpoint = Seasonal\_Reset\_SAT\_Sched.''
+
+The input object SetpointManager:Mixed air functions by placing a setpoint value on a specified node based on the value of the setpoint at another node and the temperature rise across the fan. The temperature rise is found by taking the temperature at the fan outlet node and subtracting the temperature at the fan inlet node. The EMS needs two additional sensors to obtain these temperatures, which are set up by using a pair EnergyManagementSystem:Sensor objects. The example file has three mixed air setpoint managers that place setpoints on the outlet of the outdoor air mixer, the outlet of the cooling coil, and the outlet of the heating coil. Therefore, we need three actuators to place setpoints at these three nodes, which are set up using three EnergyManagementSystem:Actuator objects. Each mixed air setpoint calculation is a simple single-line of program code such as ``SET VAV\_1\_CoolC\_Setpoint = Seasonal\_Reset\_SAT\_Sched - (T\_VAV1FanOut - T\_VAV1FanIn).''
+
+The input object AvailabilityManager:NightCycle functions by monitoring zone temperature and starting up the air system (if needed) to keep the building within the thermostat range. The sensors here are the zone air temperatures, which are set up by using EnergyManagementSystem:Sensor objects in the same way as for Example 1. We will need one zone temperature sensor for each zone that is served by the air system so we can emulate the ``CycleOnAny'' model being used. The other sensors we need are the desired zone temperatures used by the thermostat. We access these temperatures directly from the schedules (HTGSETP\_SCH and CLGSETP\_SCH in the example) by using EnergyManagementSystem:Sensor objects. To control the air system's operation status, we use an EnergyManagementSystem:Actuator object that is assigned to an ``AirLoopHVAC'' component type using the control variable called ``Availability Status.''~ EnergyPlus recognizes four availability states that control the behavior of the air system. Inside EnergyPlus these are integers, but EMS has only real-valued variables, so we will use the following whole numbers:
+
+\begin{itemize}
+\item
+  NoAction = 0.0
+\item
+  ForceOff = 1.0
+\item
+  CycleOn = 2.0
+\item
+  CycleOnZoneFansOnly = 3.0.
+\end{itemize}
+
+The traditional AvailabilityManager:NightCycle object operates by turning on the system for a prescribed amount of time (1800 seconds in the example file), and then turning it off for the same amount of time. You should be able to model this starting and stopping in EMS by using Trend variables to record the history of the actions. However, this cycling is not necessarily how real buildings are operated, and for this example we do not try to precisely emulate the traditional EnergyPlus night cycle manager. Rather, we use a simpler temperature-based control to start and stop the air system for the night cycle. The algorithm first assumes an offset tolerance of 0.83°C and calculates limits for when heating should turn on and off and when cooling should turn on and off. It then finds the maximum and minimum zone temperatures for all the zones attached to the air system. These use the @Max and @Min built-in functions, which take on two operators at a time. Then a series of logic statements is used to compare temperatures and decide what the availability status of the air system should be.
+
+\subsection{EMS Input Objects}\label{ems-input-objects-004}
+
+EMS examples are provided for the three types of traditional HVAC managers. The full set to run with no traditional managers is provided in the example file ``EMSReplaceTraditionalManagers\_LargeOffice.idf.''
+
+Example input objects that replicate a scheduled setpoint manager using EMS follow.
+
+\begin{lstlisting}
+
+EnergyManagementSystem:Sensor,
+     Seasonal_Reset_SAT_Sched, !Name
+     Seasonal-Reset-Supply-Air-Temp-Sch , ! Output:Variable Index Key Name
+     Schedule Value;   ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Actuator,
+     VAV_1_SAT_setpoint,                ! Name
+     VAV_1 Supply Equipment Outlet Node,      ! Component Name
+     System Node Setpoint,              ! Component Type
+     Temperature Setpoint;              ! Control Variable
+
+
+  EnergyManagementSystem:Program,
+     VAV_1_SchedSetpoint , ! Name
+     SET VAV_1_SAT_setpoint = Seasonal_Reset_SAT_Sched;
+
+
+  Example input objects that replicate a mixed air setpoint manager using EMS follow.
+  EnergyManagementSystem:Sensor,
+     T_VAV1FanIn, !Name
+     VAV_1_HeatC-VAV_1_FanNode , ! Output:Variable Key Name
+     System Node Temperature; ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Sensor,
+     T_VAV1FanOut, !Name
+     VAV_1 Supply Equipment Outlet Node, ! Output:Variable Index Key Name
+     System Node Temperature ; ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Actuator,
+     VAV_1_CoolC_Setpoint,            ! Name
+     VAV_1_CoolC-VAV_1_HeatCNode ,    ! Component Name
+     System Node Setpoint,            ! Component Type
+     Temperature Setpoint;            ! Control Variable
+
+
+  EnergyManagementSystem:Actuator,
+     VAV_1_HeatC_Setpoint,                            ! Name
+     VAV_1_HeatC-VAV_1_FanNode ,                  ! Component Name
+     System Node Setpoint,                          ! Component Type
+     Temperature Setpoint;            ! Control Variable
+
+
+  EnergyManagementSystem:Actuator,
+     VAV_1_OA_Setpoint,                            ! Name
+     VAV_1_OA-VAV_1_CoolCNode ,                  ! Component Name
+     System Node Setpoint,                          ! Component Type
+     Temperature Setpoint;            ! Control Variable
+
+
+
+
+  EnergyManagementSystem:Program,
+     VAV1MixedAirManagers , ! Name
+     SET VAV_1_CoolC_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV1FanOut - T_VAV1FanIn),
+     SET VAV_1_HeatC_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV1FanOut - T_VAV1FanIn),
+     SET VAV_1_OA_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV1FanOut - T_VAV1FanIn);
+
+
+  Example input objects for a night cycle availability manager follow.
+  EnergyManagementSystem:Actuator,
+    VAV_1_NightCycleStatus,   ! Name
+    VAV_1,                    ! Component Name
+    AirLoopHVAC,              ! Component Type
+    Availability Status;      ! Control Variable
+
+
+
+
+  EnergyManagementSystem:Sensor,
+    heating_setpoint,                  ! Name
+    HTGSETP_SCH ,         ! Output:Variable or Output:Meter Index Key Name
+    Schedule Value ; ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Sensor,
+    cooling_setpoint,                  ! Name
+    CLGSETP_SCH ,         ! Output:Variable or Output:Meter Index Key Name
+    Schedule Value ; ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Sensor,
+    TzoneVAV1_1,                  ! Name
+    Core_bottom ,         ! Output:Variable or Output:Meter Index Key Name
+    Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Sensor,
+    TzoneVAV1_2,                  ! Name
+    Perimeter_bot_ZN_3 ,         ! Output:Variable Key Name
+    Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Sensor,
+    TzoneVAV1_3,                  ! Name
+    Perimeter_bot_ZN_2 ,         ! Output:Variable Key Name
+    Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Sensor,
+    TzoneVAV1_4,                  ! Name
+    Perimeter_bot_ZN_1 ,         ! Output:Variable Key Name
+    Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Sensor,
+    TzoneVAV1_5,                  ! Name
+    Perimeter_bot_ZN_4 ,         ! Output:Variable Key Name
+    Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Program,
+     VAV_1_NightCycleMGR , ! Name
+     SET Toffset = 0.8333  ,  ! 1.5F
+     SET NoAction = 0.0 ,
+     SET ForceOff = 1.0 ,
+     SET CycleOn = 2.0 ,
+     SET CycleOnZoneFansOnly = 3.0 ,
+     SET VAV1_heating_TurnOn  = heating_setpoint - Toffset ,
+     SET VAV1_heating_TurnOff = heating_setpoint + Toffset ,
+     SET VAV1_cooling_TurnOn  = cooling_setpoint + Toffset ,
+     SET VAV1_cooling_TurnOff = cooling_setpoint - Toffset ,
+     ! find max and min for "cycleOnAny" operation
+     SET Tmin = @MIN TzoneVAV1_1 TzoneVAV1_2  ,
+     SET Tmin = @MIN Tmin        TzoneVAV1_3  ,
+     SET Tmin = @MIN Tmin        TzoneVAV1_4  ,
+     SET Tmin = @MIN Tmin        TzoneVAV1_5  ,
+     SET Tmax = @MAX TzoneVAV1_1 TzoneVAV1_2  ,
+     SET Tmax = @MAX Tmax        TzoneVAV1_3  ,
+     SET Tmax = @MAX Tmax        TzoneVAV1_4  ,
+     SET Tmax = @MAX Tmax        TzoneVAV1_5  ,
+     IF Tmin < VAV1_heating_TurnOn ,
+       SET VAV_1_NightCycleStatus = CycleOn,
+       RETURN,  ! need to exit early or cooling check could also trigger
+     ELSEIF Tmin > VAV1_heating_TurnOff,
+       SET VAV_1_NightCycleStatus = NoAction,
+     ENDIF,
+     IF Tmax > VAV1_cooling_TurnOn,
+       SET VAV_1_NightCycleStatus = CycleOn,
+     ELSEIF Tmax < VAV1_cooling_TurnOff,
+       SET VAV_1_NightCycleStatus = NoAction   ,
+     ENDIF;
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-3-hygro-thermal-window-opening.tex b/doc/ems-application-guide/src/ems-examples/example-3-hygro-thermal-window-opening.tex
new file mode 100644
index 00000000000..a17482ad96d
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-3-hygro-thermal-window-opening.tex
@@ -0,0 +1,91 @@
+\section{Example 3. Hygro-thermal Window Opening Control for Airflow Network}\label{example-3.-hygro-thermal-window-opening-control-for-airflow-network}
+
+\subsection{Problem Statement}\label{problem-statement-005}
+
+A user of EnergyPlus version 3.1 posted the following question on the Yahoo! list (circa spring 2009):
+
+I am currently trying to model a simple ventilation system based on an
+
+exhaust fan and outdoor air variable aperture paths that open according to
+
+the indoor relative humidity.
+
+As I didn't find any object to directly do this, I am trying to use an
+
+AirflowNetwork: MultiZone: Component: DetailedOpening object and its
+
+AirflowNetwork: multizone: Surface object to model the variable aperture. But
+
+the Ventilation Control Mode of the surface object can only be done via
+
+Temperature or Enthalpy controls (or other not interesting for my purpose),
+
+and not via humidity.
+
+So my questions are:
+
+1- is it possible to make the surface object variable according to the
+
+relative humidity? (maybe adapting the program?)
+
+2- or is there an other way to make it?
+
+Because the traditional EnergyPlus controls for window openings do not support humidity-based controls (or did not as of Version 3.1), the correct response to Question \#1 was ``No.''~ But with the EMS, we can now answer Question \#2 as ``Yes.''~ How can we take the example file called HybridVentilationControl.idf and implement humidity-based control for a detailed opening in the airflow network model?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-005}
+
+The main EMS sensor will be the zone air humidity, so we use an EnergyManagementSystem:Sensor object that maps to the output variable called System Node Relative Humidity for the zone's air node. This zone has the detailed opening.
+
+The EMS will actuate the opening in an airflow network that is defined by the input object AirflowNetwork:MultiZone:Component:DetailedOpening. The program will setup the actuator for this internally, but we need to use an EnergyManagementSystem:Actuator object to declare that we want to use the actuator and provide the variable name we want for the Erl programs.
+
+Because we do not know the exactly what the user had in mind, for this example we assume that the desired behavior for the opening area is that the opening should vary linearly with room air relative humidity. When the humidity increases, we want the opening to be larger. When the humidity decreases, we want the opening to be smaller. For relative humidity below 25\% we close the opening. At 60\% or higher relative humidity, the opening should be completely open. We formulate a model equation for opening factor as
+
+\begin{equation}
+F_{open} = \begin{array}{ll}
+    0.0 & RH < 25\% \\
+    \frac{RH-25}{60-25} & 25\% \leq RH \leq 60\% \\
+    1.0 & RH > 60\%  
+  \end{array}
+\end{equation}
+
+\subsection{EMS Input Objects}\label{ems-input-objects-005}
+
+EMS-related input objects to solve this problem are listed below and are included in the example file called ``EMSAirflowNetworkOpeningControlByHumidity.idf.''
+
+\begin{lstlisting}
+
+EnergyManagementSystem:Sensor,
+    ZoneRH , ! Name
+    Zone 1 Node, ! Output:Variable or Output:Meter Index Key Name
+    System Node Relative Humidity; ! Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Actuator,
+    MyOpenFactor,                            ! Name
+    Zn001:Wall001:Win001,                  ! Component Name
+    AirFlow Network Window/Door Opening, ! Component Type
+    Venting Opening Factor;    ! Control Type
+
+
+  EnergyManagementSystem:ProgramCallingManager,
+    RH Controlled Open Factor ,    ! Name
+    BeginTimestepBeforePredictor , ! EnergyPlus Model Calling Point
+    RH_OpeningController ;         ! Program Name 1
+
+
+  EnergyManagementSystem:Program,
+    RH_OpeningController ,     ! Name
+    IF ZoneRH < 25,
+      SET MyOpenFactor = 0.0 ,
+    ELSEIF ZoneRH > 60,
+      SET MyOpenFactor = 1.0 ,
+    ELSE,
+      SET MyOpenFactor = (ZoneRH - 25) / (60 - 25),
+    ENDIF;
+
+
+  Output:EnergyManagementSystem,
+    Verbose,
+    Verbose,
+    Verbose;
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-4-halt-program-based-on-constraint.tex b/doc/ems-application-guide/src/ems-examples/example-4-halt-program-based-on-constraint.tex
new file mode 100644
index 00000000000..0463813369e
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-4-halt-program-based-on-constraint.tex
@@ -0,0 +1,58 @@
+\section{Example 4. Halt Program Based on Constraint}\label{example-4.-halt-program-based-on-constraint}
+
+\subsection{Problem Statement}\label{problem-statement-006}
+
+Heavy users of EnergyPlus explore the enormous parameter space associated with building design options. Computational requirements often limit what can be accomplished in a given study. For optimizations and other parametric studies, there is usually a tension between having a very detailed model that is comfortably accurate, and a simpler model that executes faster.
+
+For most studies many trial simulations are discarded because they violate some constraint. To save computation time, you might consider ``fatal--out'' simulations where early calculations show that some predetermined constraints will not be met in the final result. Many studies could save considerable computing resources by prematurely quitting models rather than always letting each simulation run to completion. All types of constraints such as poor comfort, excessive system iterations, and high energy costs could be used to kill a run. You should ask, Is there a way to use the EMS to expedite my optimal searches by stopping models prematurely if they fail some test?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-006}
+
+As an example, let us assume that the criterion for early exit is that the model fails to be sufficiently comfortable. We will start with the Small Hotel Reference Building example file (RefBldgSmallHotelNew2004\_Chicago.idf). Short periods of discomfort are tolerated, but if the space is uncomfortable over time, we want to abandon the simulation and save computational expense. A simulation can be stopped from within an Erl program by calling the built-in function ``@FatalHaltEp.''~ The EMS system has only numeric data types, so we cannot generate text for the error message. Therefore, we choose a particular real-numbered value to use as an error code that provides some detail on which constraint caused early termination. In this example, we choose the value ``1002.50'' to indicate an average PMV exceeds 2.5 and the value ``9001.30'' indicates the average PMV less than 1.3. We will formulate the constraint by using the result of the Fanger comfort model for PMV for the building's core zone named ``Core\_ZN.''~ If the occupants will be too cold, we will call @FatalHaltEp with the error code 9001.30. If the occupants will be too warm during a summer design day, we will fatal out with the error code 1002.50. (These values were chosen arbitrarily to demonstrate EMS; PMV of 1.3 is not necessarily a problem.)
+
+To monitor PMV, we will use a trend variable, which we create by using the EnergyManagementSystem:TrendVariable input object. A trend variable is a log of historical values for Erl variables. A trend log is an array that goes farther and farther back in time. For this example, we assume the constraint is to monitor the average PMV for the previous 2-hour period. The example file has 6 timesteps per hour, so each trend point is 10 minutes and a 2-hour average needs 12 timesteps. So the field Number of Timesteps to be Logged must be 12 or larger. To access the values stored in a trend variable, the built-in functions provided for accessing trends must be used. The @TrendAverage function called with an index of 12 will return the 2-hour running average. To monitor this result of running average PMV, we set up custom output variable using an EnergyManagementSystem:OutputVariable input object.
+
+\subsection{EMS Input Objects}\label{ems-input-objects-006}
+
+The EMS input objects for this example follow and are contained in the example file called ``EMSTestMAthAndKill.idf.''
+
+\begin{lstlisting}
+
+ EnergyManagementSystem:ProgramCallingManager,
+     Average Building Temperature , ! Name
+     EndOfZoneTimestepBeforeZoneReporting , ! EnergyPlus Model Calling Point
+     updateMy_averagePMV; ! Program Name 1
+
+   EnergyManagementSystem:Sensor,
+     PMV5, !Name
+     Core_ZN , ! Output:Variable or Output:Meter Index Key Name
+     Zone Thermal Comfort Fanger Model PMV ; ! Output:Variable Name
+
+   EnergyManagementSystem:TrendVariable,
+     PMVtrendLog1,
+     PMV5,
+     300;
+
+   EnergyManagementSystem:GlobalVariable,
+     PMVrunningAvg;
+
+   EnergyManagementSystem:OutputVariable,
+     Running Two Hour Average PMV [PMVunits], ! Name
+     PMVrunningAvg, ! EMS Variable Name
+     Averaged, ! Type of Data in Variable
+     ZoneTimeStep ; ! Update Frequency
+
+   EnergyManagementSystem:Program,
+     UpdateMy_averagePMV,
+     Set PMVrunningAvg = @TrendAverage PMVtrendLog1 12, ! two hour running average.
+     RUN Kill_Run_if_Uncomfortable;
+
+   EnergyManagementSystem:Subroutine,
+     Kill_Run_if_Uncomfortable,
+     IF PMVrunningAvg > 2.5,
+       SET tmpError = @FatalHaltEp 1002.50, ! error code "1002.50" for comfort avg over 2.5
+     ENDIF,
+     IF PMVrunningAvg < 0.0 - 1.3,
+       SET tmpError = @FatalHaltEp 9001.30, ! error code "9001.30" for comfort avg under - 1.3
+     ENDIF;
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-5-computed-schedule.tex b/doc/ems-application-guide/src/ems-examples/example-5-computed-schedule.tex
new file mode 100644
index 00000000000..5a04a848fa2
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-5-computed-schedule.tex
@@ -0,0 +1,81 @@
+\section{Example 5. Computed Schedule}\label{example-5.-computed-schedule}
+
+\subsection{Problem Statement}\label{problem-statement-007}
+
+Many models have schedule inputs that could be used to control the object, but creating the schedules it is too cumbersome. We need to ask, Can we use the EMS to dynamically calculate a schedule?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-007}
+
+As an example, we will take the model from example 1 and use the EMS to replicate the heating and cooling zone temperature setpoint schedules. The input object Schedule:Constant has been set up to be available as an actuator. We then add EnergyManagementSystem:Actuator objects that set these actuators up as Erl variables.
+
+To devise an Erl program to compute the schedule, we need to use the built-in variables that describe time and day. The built-in variable Hour will provide information about the time of day; DayOfWeek will provide information about whether it is the weekend or a weekday.
+
+\subsection{EMS Input Objects}\label{ems-input-objects-007}
+
+Example EMS input for computing a schedule for heating and cooling setpoints follows and are contained in the example file called ``EMSCustomSchedule.idf.''
+
+\begin{lstlisting}
+
+Schedule:Constant,
+      CLGSETP_SCH,
+      Temperature,
+      24.0;
+
+    EnergyManagementSystem:Actuator,
+      myCLGSETP_SCH_Override,
+      CLGSETP_SCH,Schedule:Constant,Schedule Value;
+
+    EnergyManagementSystem:ProgramCallingManager,
+      My Setpoint Schedule Calculator Example,
+      BeginTimestepBeforePredictor,
+      MyComputedCoolingSetpointProg,
+      MyComputedHeatingSetpointProg;
+
+    EnergyManagementSystem:Program,
+      MyComputedCoolingSetpointProg,
+      IF (DayOfWeek = = 1),
+        Set myCLGSETP_SCH_Override = 30.0  ,
+      ELSEIF (Holiday = = 3.0) && (DayOfMonth = = 21) && (Month = = 1),  !winter design day
+        Set myCLGSETP_SCH_Override = 30.0 ,
+      ELSEIF HOUR < 6       ,
+        Set myCLGSETP_SCH_Override = 30.0  ,
+      ELSEIF (Hour > = 6) && (Hour < 22)  && (DayOfWeek > = 2) && (DayOfWeek < = 6) ,
+        Set myCLGSETP_SCH_Override = 24.0  ,
+      ELSEIF (Hour > = 6) && (hour < 18) && (DayOfWeek = = 7)
+        Set myCLGSETP_SCH_Override = 24.0  ,
+      ELSEIF (Hour > = 6) && (hour > = 18) && (DayOfWeek = = 7)
+        Set myCLGSETP_SCH_Override = 30.0  ,
+      ELSEIF (Hour > = 22)                   ,
+        Set myCLGSETP_SCH_Override = 30.0  ,
+      ENDIF;
+
+    Schedule:Constant,
+      HTGSETP_SCH,
+      Temperature,
+      21.0;
+
+    EnergyManagementSystem:Actuator,
+      myHTGSETP_SCH,
+      HTGSETP_SCH,Schedule:Constant,Schedule Value;
+
+    EnergyManagementSystem:Program,
+     MyComputedHeatingSetpointProg,
+     Set locHour = Hour, ! echo out for debug
+     Set locDay = DayOfWeek, ! echo out for debug
+     Set locHol = Holiday,  ! echo out for debug
+     IF (DayOfWeek = = 1),
+       Set myHTGSETP_SCH = 15.6  ,
+     ELSEIF (Holiday = = 3.0) && (DayOfYear = = 21),  !winter design day
+       Set myHTGSETP_SCH = 21.0 ,
+     ELSEIF HOUR < 5       ,        
+       Set myHTGSETP_SCH = 15.6  ,
+     ELSEIF (Hour > = 5) && (Hour < 19)  && (DayOfWeek > = 2) && (DayOfWeek < = 6) ,
+       Set myHTGSETP_SCH = 21.0  ,
+     ELSEIF (Hour > = 6) && (hour < 17) && (DayOfWeek = = 7),
+       Set myHTGSETP_SCH = 21.0  ,
+     ELSEIF (Hour > = 6) && (hour < = 17) && (DayOfWeek = = 7) ,
+       Set myHTGSETP_SCH = 15.6   ,
+     ELSEIF (Hour > = 19)          ,
+       Set myHTGSETP_SCH = 15.6   ,
+     ENDIF;
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-6-window-shade-control.tex b/doc/ems-application-guide/src/ems-examples/example-6-window-shade-control.tex
new file mode 100644
index 00000000000..1f7dd5bd194
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-6-window-shade-control.tex
@@ -0,0 +1,194 @@
+\section{Example 6. Window Shade Control}\label{example-6.-window-shade-control}
+
+\subsection{Problem Statement}\label{problem-statement-008}
+
+EnergyPlus offers a wide range of control options in the WindowProperty:ShadingControl object, but it is easy to imagine custom schemes for controlling shades or blinds that are not available. We need to ask, Can we use the EMS to override the shading controls?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-008}
+
+We will take the example file PurchAirWindowBlind.idf and use EMS to add a new control scheme. This file has an interior blind that can be either ``on'' or ``off.''~ The control scheme has three parts:
+
+\begin{itemize}
+\item
+  Deploy the blind whenever too much direct sun would enter the zone and cause discomfort for the occupants.
+\item
+  Deploy the blind whenever there is a significant cooling load.
+\item
+  Leave the blind open whenever the first two constraints have not triggered.
+\end{itemize}
+
+We assume that a model for the direct sun control is based on incidence angle, where the angle is defined as zero for normal incidence relative to the plane of the window. When the direct solar incidence angle is less than 45 degrees, we want to draw the blind. EnergyPlus has a report variable called ``Surface Ext Solar Beam Cosine Of Incidence Angle,'' for which we will use a sensor in our EnergyManagementSystem:Sensor input object. This sensor is a cosine value that we turn into an angle value with the built-in function @ArcCos. Then we will use the built-in function @RadToDeg to convert from radians to degrees. This new window/solar incidence angle in degree may be an interesting report variable, so we use an EnergyManagementSystem:OutputVariable input object to create custom output.
+
+Because the transmitted solar is a problem only when there is a cooling load, we also trigger the blind based on the current data for cooling. The report variable called ``Zone/Sys Sensible Cooling Rate'' is used in an EMS sensor to obtain an Erl variable with the most recent data about zone cooling load required to meet setpoint. When this value is positive, we know the zone cannot make good use of passive solar heating, so we close the blind.
+
+The EMS actuator will override the operation of a WindowProperty:ShadingControl input object. Related to this, the EDD file shows
+
+! \textless{}EnergyManagementSystem:Actuator Available\textgreater{}, Component Unique Name, Component Type,~ Control Type
+
+EnergyManagementSystem:Actuator Available,ZN001:WALL001:WIN001,Window Shading Control,Control Status
+
+Although the user-defined name for the WindowProperty:ShadingControl is ``INCIDENT SOLAR ON BLIND,'' the component unique name of the actuator that is available is called ``ZN001:WALL001:WIN001.''~ There could be multiple windows, all with shades, and each is governed by a single WindowProperty:ShadingControl input object. The EMS actuator could override each window separately. The Control Type is called ``Control Status,'' and requires you to set the status to one of a set of possible control flags. For this case, with only an interior shade, there are two states for the actuator to take. The first shows the shade is ``off,'' and corresponds to a value of 0.0. The second shows the interior shade is ``on,'' and corresponds to a value of 6.0.
+
+\subsection{EMS Input Objects}\label{ems-input-objects-008}
+
+The EMS input objects for this example follow and are contained in the example file called ``EMSWindowShadeControl.idf.''
+
+\begin{lstlisting}
+
+Output:EnergyManagementSystem,
+     Verbose,
+     Verbose,
+     Verbose;
+
+
+   EnergyManagementSystem:Sensor,
+     Solar_Beam_Incident_Cos, !Name
+     Zn001:Wall001:Win001,! Output:Variable or Output:Meter Index Key Name
+     Surface Outside Face Beam Solar Incident Angle Cosine Value; ! Var Name
+
+
+   Output:Variable, Zn001:Wall001:Win001,
+      Surface Outside Face Beam Solar Incident Angle Cosine Value, Timestep;
+
+
+   EnergyManagementSystem:Sensor,
+     Zone_Sensible_Cool_Rate, !Name
+     RESISTIVE ZONE,! Output:Variable or Output:Meter Index Key Name
+     Zone Air System Sensible Cooling Rate; ! Var Name
+
+
+   Output:Variable, RESISTIVE ZONE,
+      Zone Air System Sensible Cooling Rate, Timestep;
+
+
+  EnergyManagementSystem:ProgramCallingManager,
+    Window Shading Device EMS Controller,    ! Name
+    BeginTimestepBeforePredictor , ! EnergyPlus Model Calling Point
+    Set_Shade_Control_State ;         ! Program Name 1
+
+
+  EnergyManagementSystem:Actuator,
+    Zn001_Wall001_Win001_Shading_Deploy_Status,   ! Name
+    Zn001:Wall001:Win001,    ! Component Name  Surface name with shade controls
+    Window Shade Control, ! Component Type
+    Control Status;    ! Control Type
+
+
+
+
+  EnergyManagementSystem:Program,
+    Set_Shade_Control_State,     ! Name
+    !
+    Set IncidentAngleRad = @ArcCos Solar_Beam_Incident_Cos,
+    Set IncidentAngle   = @RadToDeg IncidentAngleRad,
+    !
+    IF IncidentAngle < 45 , ! Block intense direct sun
+     Set Zn001_Wall001_Win001_Shading_Deploy_Status = Shade_Status_Interior_Blind_On,
+    ELSEIF Zone_Sensible_Cool_Rate > 20, ! block to reduce cooling loads
+     Set Zn001_Wall001_Win001_Shading_Deploy_Status = Shade_Status_Interior_Blind_On,
+    Else,
+     Set Zn001_Wall001_Win001_Shading_Deploy_Status = Shade_Status_Off ,
+    ENDIF ;
+
+
+
+
+  EnergyManagementSystem:OutputVariable,
+     Erl Shading Control Status, ! Name
+     Zn001_Wall001_Win001_Shading_Deploy_Status, ! EMS Variable Name
+     Averaged, ! Type of Data in Variable
+     ZoneTimeStep ; ! Update Frequency
+
+
+  EnergyManagementSystem:OutputVariable,
+     Erl Zn001:Wall001:Win001 Incident Angle, ! Name
+     IncidentAngle, ! EMS Variable Name
+     Averaged, ! Type of Data in Variable
+     ZoneTimeStep ; ! Update Frequency
+
+
+   EnergyManagementSystem:GlobalVariable,  IncidentAngle;
+
+
+  Output:Variable,
+    *,
+    Erl Shading Control Status,
+    Timestep;
+
+
+  Output:Variable,
+    *,
+    Erl Zn001:Wall001:Win001 Incident Angle,
+    Timestep;
+
+
+
+
+
+
+  EnergyManagementSystem:ProgramCallingManager,
+    Init Window Shading Device Control Constants,    ! Name
+    BeginNewEnvironment , ! EnergyPlus Model Calling Point
+    InitializeShadeControlFlags ;         ! Program Name 1
+
+
+   EnergyManagementSystem:GlobalVariable,    Shade_Status_None;
+   EnergyManagementSystem:GlobalVariable,    Shade_Status_Off ;
+   EnergyManagementSystem:GlobalVariable,    Shade_Status_Interior_Shade_On;
+   EnergyManagementSystem:GlobalVariable,    Shade_Status_Switchable_Dark;
+   EnergyManagementSystem:GlobalVariable,    Shade_Status_Exterior_Shade_On;
+   EnergyManagementSystem:GlobalVariable,    Shade_Status_Interior_Blind_On;
+   EnergyManagementSystem:GlobalVariable,    Shade_Status_Exterior_Blind_On;
+   EnergyManagementSystem:GlobalVariable,    Shade_Status_Between_Glass_Shade_On;
+   EnergyManagementSystem:GlobalVariable,    Shade_Status_Between_Glass_Blind_On;
+
+
+
+
+   EnergyManagementSystem:Program,
+      InitializeShadeControlFlags,
+            ! these are control flag values used inside EnergyPlus for window shades
+            ! EMS control of window shading devices involves setting the control values for shading control actuators with
+            !  one of these values. The variable names can be used or replaced, it is the whole number values that trigger
+            !  changes in the modeling.
+            !  Shades and Blinds are either fully on or fully off, partial positions require multiple windows.
+            ! the window shading control flag values follow
+            !  -1: if window has no shading device
+      Set Shade_Status_None = 0.0 - 1.0,  ! this is how to write a negative number Erl does not have unary "minus,"  only binary subtraction
+            !   0: if shading device is off
+      Set Shade_Status_Off = 0.0,
+            !   1: if interior shade is on
+      Set Shade_Status_Interior_Shade_On = 1.0,
+            !   2: if glazing is switched to darker state
+      Set Shade_Status_Switchable_Dark = 2.0,
+            !   3: if exterior shade is on
+      Set Shade_Status_Exterior_Shade_On = 3.0,
+            !   6: if interior blind is on
+      Set Shade_Status_Interior_Blind_On = 6.0,
+            !   7: if exterior blind is on
+      Set Shade_Status_Exterior_Blind_On = 6.0,
+            !   8: if between-glass shade is on
+      Set Shade_Status_Between_Glass_Shade_On = 8.0,
+            !   9: if between-glass blind is on
+      Set Shade_Status_Between_Glass_Blind_On = 9.0;
+            !  10: window has interior shade that is off but may be triggered on later
+            !       to control daylight glare
+            !  20: window has switchable glazing that is unswitched but may be switched later
+            !       to control daylight glare or daylight illuminance
+            !  30: window has exterior shade that is off but may be triggered on later
+            !       to control daylaight glare or daylight illuminance
+            !  60: window has interior blind that is off but may be triggered on later
+            !       to control daylaight glare or daylight illuminance
+            !  70: window has exterior blind that is off but may be triggered on later
+            !       to control daylaight glare or daylight illuminance
+            !  80: window has between-glass shade that is off but may be triggered on later
+            !       to control daylaight glare or daylight illuminance
+            !  90: window has between-glass blind that is off but may be triggered on later
+            !       to control daylaight glare or daylight illuminance
+            ! A "shading device" may be an exterior, interior or between-glass shade or blind,
+            ! or the lower-transmitting (dark) state of switchable glazing (e.g., electrochromic).
+            ! In all cases, the unshaded condition is represented
+            ! by the construction given by window's Surface()%Construction and
+            ! the shaded condition is represented by the construction given by
+            ! the window's Surface()%ShadedConstruction
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-7-constant-volume-purchased-air.tex b/doc/ems-application-guide/src/ems-examples/example-7-constant-volume-purchased-air.tex
new file mode 100644
index 00000000000..881e0aa5e11
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-7-constant-volume-purchased-air.tex
@@ -0,0 +1,102 @@
+\section{Example 7. Constant Volume Purchased Air System}\label{example-7.-constant-volume-purchased-air-system}
+
+\subsection{Problem Statement}\label{problem-statement-009}
+
+The simplest way to add HVAC control to an EnergyPlus thermal zone is to use the ZoneHVAC:IdealLoadsAirSystem. This was called \emph{purchased air} in older versions. The ideal loads air system is intended for load calculations. You provide input for the supply air conditions of drybulb and humidity ratio, but the flow rate cannot be controlled. The model operates by varying the flow rate to exactly meet the desired setpoints. However, you may want to experiment with various designs in a slightly different way in which, given a prescribed supply air situation, then adjust the design to maximize the thermal comfort. It would be interesting to use the simple-to-input purchased air model to examine how a zone responds to a system, rather than how the system responds to a zone. We should ask, Can we use the EMS to prescribe the supply air flow rates for a purchased air model?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-009}
+
+For this example we begin with the input file from Example 6 (primarily because it already has purchased air). We examine the typical mass flow rates the air system provides to have some data to judge what an appropriate constant flow rate might be. A cursory review of the data indicates that cooling flow rates of 0.3 kg/s are chosen for two zones and 0.4 kg/s is chosen for the third. Heating flow rates of 0.1 and 0.15 kg/s are also chosen.
+
+We want the model to respond differently for heating and cooling. We define two operating states and create global variables to hold that state for each zone. The first state is when the zone calls for heating; we will assign a value of 1.0. The second is when the zone calls for cooling; we assign 2.0.
+
+To sense the state we will use EMS sensors associated with the output variable called ``Zone/Sys Sensible Load Predicted.''~ We will set up one of these for each zone and use it as input data. If this value is less than zero, the zone is in the cooling state. If it is greater than zero, the zone is in the heating state. This predicted load is calculated during the predictor part of the model, so we choose the EMS calling point called ``AfterPredictorAfterHVACManagers.''
+
+An EMS actuator is available for the ideal loads air system that overrides the air mass flow rate (kg/s) delivered by the system when it is on. The override is not absolute in that the model will still apply the limits defined in the input object and overrides only if the system is ``on.''~ The internal logic will turn off the air system if the zone is in the thermostat dead band or scheduled ``off'' by availability managers. This ``off'' state is modeled inside the ideal loads air system so it does not need to be calculated in Erl. This control leads to a constant volume system that cycles in an attempt to control the zone conditions. In practice, it can achieve relatively good control when loads do not exceed the available capacity.
+
+\subsection{EMS Input Objects}\label{ems-input-objects-009}
+
+A set of EMS input objects for a constant volume purchased air system serving three zones follows are contained in the example file called ``EMSConstantVolumePurchAir.idf.''
+
+\begin{lstlisting}
+
+EnergyManagementSystem:ProgramCallingManager,
+    Constant Volume Purchased Air Example,    ! Name
+    AfterPredictorAfterHVACManagers , ! EnergyPlus Model Calling Point
+    Determine_Purch_Air_State,         ! Program Name 1
+    Set_Purch_Air;
+
+
+  EnergyManagementSystem:Program,
+    Determine_Purch_Air_State,     ! Name
+    ! State representation:  1.0 is heating, 2.0 is cooling
+    IF (Sensible_Load_Zone_1 < = 0.0) ,
+      SET Zone_1_State = 2.0,
+    ELSEIF (Sensible_Load_Zone_1 > 0.0) ,
+      SET Zone_1_State = 1.0,
+    ENDIF,
+    IF (Sensible_Load_Zone_2 < = 0.0) ,
+      SET Zone_2_State = 2.0,
+    ELSEIF (Sensible_Load_Zone_2 > 0.0) ,
+      SET Zone_2_State = 1.0,
+    ENDIF,
+    IF (Sensible_Load_Zone_3 < = 0.0) ,
+      SET Zone_3_State = 2.0,
+    ELSEIF (Sensible_Load_Zone_3 > 0.0) ,
+      SET Zone_3_State = 1.0,
+    ENDIF;
+
+
+
+
+   EnergyManagementSystem:Program,
+    Set_Purch_Air,
+    IF (    Zone_1_State = = 2.0),
+      SET ZONE_1_AIR_Mdot = 0.3,
+    ELSEIF (Zone_1_State = = 1.0),
+      SET ZONE_1_AIR_Mdot = 0.1,
+    ENDIF,
+    IF (    Zone_2_State = = 2.0),
+      SET ZONE_2_AIR_Mdot = 0.3,
+    ELSEIF (Zone_2_State = = 1.0),
+      SET ZONE_2_AIR_Mdot = 0.1,
+    ENDIF,
+    IF (    Zone_3_State = = 2.0),
+      SET ZONE_3_AIR_Mdot = 0.4,
+    ELSEIF (Zone_3_State = = 1.0),
+      SET ZONE_3_AIR_Mdot = 0.15,
+    ENDIF;
+
+
+
+
+   EnergyManagementSystem:GlobalVariable,  Zone_1_State;
+   EnergyManagementSystem:GlobalVariable,  Zone_2_State;
+   EnergyManagementSystem:GlobalVariable,  Zone_3_State;
+
+
+   EnergyManagementSystem:Actuator,  ZONE_1_AIR_Mdot,
+    ZONE1AIR,Ideal Loads Air System,Air Mass Flow Rate;
+   EnergyManagementSystem:Actuator, ZONE_2_AIR_Mdot,
+    ZONE2AIR,Ideal Loads Air System,Air Mass Flow Rate;
+   EnergyManagementSystem:Actuator, ZONE_3_AIR_Mdot,
+    ZONE3AIR,Ideal Loads Air System,Air Mass Flow Rate;
+
+
+   EnergyManagementSystem:Sensor,
+    Sensible_Load_Zone_1, !Name
+    RESISTIVE ZONE,! Output:Variable or Output:Meter Index Key Name
+    Zone Predicted Sensible Load to Setpoint Heat Transfer Rate; ! Var Name
+
+
+   EnergyManagementSystem:Sensor,
+    Sensible_Load_Zone_2, !Name
+    EAST ZONE,! Output:Variable or Output:Meter Index Key Name
+    Zone Predicted Sensible Load to Setpoint Heat Transfer Rate; ! Var Name
+
+
+   EnergyManagementSystem:Sensor,
+    Sensible_Load_Zone_3, !Name
+    NORTH ZONE,! Output:Variable or Output:Meter Index Key Name
+    Zone Predicted Sensible Load to Setpoint Heat Transfer Rate; ! Var Name
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-8-system-sizing-with-discrete-package.tex b/doc/ems-application-guide/src/ems-examples/example-8-system-sizing-with-discrete-package.tex
new file mode 100644
index 00000000000..1b9173cdb29
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-8-system-sizing-with-discrete-package.tex
@@ -0,0 +1,251 @@
+\section{Example 8. System Sizing with Discrete Package Sizes}\label{example-8.-system-sizing-with-discrete-package-sizes}
+
+\subsection{Problem Statement}\label{problem-statement-010}
+
+One tension often arises with modeling when options being evaluated have an indirect effect on air system size. In normal autosizing, the changes in sizes are continuous, but in real systems, equipment sizes tend to be discrete. If we start with the Strip Mall Reference Building model (RefBldgStripMallNew2004\_Chicago.idf), we should ask, Could we use the EMS custom calculations to intervene and make the final system sizing results follow the discrete sizes available for a particular product line of equipment?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-010}
+
+Examining the vendor's literature for one line of commercial packaged single-zone HVAC air systems shows that the nominal product sizes include 1200 cfm, 1600 cfm, 2000 cfm, 2400 cfm, 3000 cfm, 3400, cfm, and 4000 cfm. The literature also classifies units by tonnage of cooling capacity; however, in EnergyPlus modeling it is simpler to classify by air flow rate rather than by cooling capacity (because the direct expansion models have a tight range for allowable cooling capacity per air flow rate and size themselves off the flow rate). We construct the following simple model to select the next higher air flow rate product that uses the volume flow determined during the usual autosizing calculations, \(\dot{V}_{size}\) , and threshold values taken from the nominal product sizes (in m\(^{3}\)/s):
+
+\begin{longtable}[c]{p{4.03in}p{1.96in}}
+\toprule 
+Threshold & Selection \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Threshold & Selection \tabularnewline
+\midrule
+\endhead
+
+$0  <  \dot{V}_{size} \leq 0.566$ & $\dot{V} = 0.566$ \tabularnewline
+$0.566  <  \dot{V}_{size} \leq 0.755$ & $\dot{V} = 0.755$ \tabularnewline
+$0.755  <  \dot{V}_{size} \leq 0.944$ & $\dot{V} = 0.944$ \tabularnewline
+$0.944  <  \dot{V}_{size} \leq 1.133$ & $\dot{V} = 1.133$ \tabularnewline
+$1.133  <  \dot{V}_{size} \leq 1.416$ & $\dot{V} = 1.416$ \tabularnewline
+$1.416  <  \dot{V}_{size} \leq 1.604$ & $\dot{V} = 1.604$ \tabularnewline
+$1.604  <  \dot{V}_{size} \leq 1.888$ & $\dot{V} = 1.888$ \tabularnewline
+\bottomrule
+\end{longtable}
+
+The system sizing calculations determine a value for the volume flow rate. To obtain this result for use in an Erl program, we use an EnergyManagementSystem:InternalVariable input object to set up a variable for the data called ``Intermediate Air System Main Supply Volume Flow Rate.''~ We can then use this value in our algorithm to find a discrete system size.
+
+Once we have the new system size, we need to set up an actuator to apply the new size. For this we use an EnergyManagementSystem:Actuator input object to establish control over ``Sizing:System'' type of component using the ``Main Supply Volume Flow Rate'' control type.
+
+The EMS calling point for controlling air system sizing is called ``EndOfSystemSizing.''~ So we enter this into the program calling manager.
+
+For this example, we modify the example file called ``RefBldgStripMallNew2004\_Chicago.idf.''~ This file has 10 separate packaged units, so rather than repeat the algorithm several times, we use a subroutine so the same Erl code can be reused for each air system. The subroutine has two arguments that we will declare as global variables:~ the input for continuous size and the output for the discrete size.
+
+\subsection{EMS Input Objects}\label{ems-input-objects-010}
+
+A set of input objects for EMS control for discrete resizing of 10 air systems follows and is included in the example file called ``EMSDiscreteAirSystemSizes.idf.''
+
+\begin{lstlisting}
+
+Output:EnergyManagementSystem,
+    Verbose,
+    Verbose,
+    Verbose;
+
+
+  EnergyManagementSystem:ProgramCallingManager,
+    Apply Discrete Package Sizes to Air System Sizing , ! Name
+    EndOfSystemSizing ,    ! EnergyPlus Model Calling Point
+    Resize_PSZ_To_Match_Product_Availability;         ! Program Name 1
+
+
+
+
+  EnergyManagementSystem:Program,
+    Resize_PSZ_To_Match_Product_Availability , ! Name
+    SET argMainVdot = PSZ_1_CalcMainSupVdot,
+    RUN Select_Discrete_Nominal_Air_Flow,
+    SET PSZ_1_MainSupVdotSet = argDiscreteMainVdot,
+    SET argMainVdot = PSZ_2_CalcMainSupVdot,
+    RUN Select_Discrete_Nominal_Air_Flow,
+    SET PSZ_2_MainSupVdotSet = argDiscreteMainVdot,
+    SET argMainVdot = PSZ_3_CalcMainSupVdot,
+    RUN Select_Discrete_Nominal_Air_Flow,
+    SET PSZ_3_MainSupVdotSet = argDiscreteMainVdot,
+    SET argMainVdot = PSZ_4_CalcMainSupVdot,
+    RUN Select_Discrete_Nominal_Air_Flow,
+    SET PSZ_4_MainSupVdotSet = argDiscreteMainVdot,
+    SET argMainVdot = PSZ_5_CalcMainSupVdot,
+    RUN Select_Discrete_Nominal_Air_Flow,
+    SET PSZ_5_MainSupVdotSet = argDiscreteMainVdot,
+    SET argMainVdot = PSZ_6_CalcMainSupVdot,
+    RUN Select_Discrete_Nominal_Air_Flow,
+    SET PSZ_6_MainSupVdotSet = argDiscreteMainVdot,
+    SET argMainVdot = PSZ_7_CalcMainSupVdot,
+    RUN Select_Discrete_Nominal_Air_Flow,
+    SET PSZ_7_MainSupVdotSet = argDiscreteMainVdot,
+    SET argMainVdot = PSZ_8_CalcMainSupVdot,
+    RUN Select_Discrete_Nominal_Air_Flow,
+    SET PSZ_8_MainSupVdotSet = argDiscreteMainVdot,
+    SET argMainVdot = PSZ_9_CalcMainSupVdot,
+    RUN Select_Discrete_Nominal_Air_Flow,
+    SET PSZ_9_MainSupVdotSet = argDiscreteMainVdot,
+    SET argMainVdot = PSZ_10_CalcMainSupVdot,
+    RUN Select_Discrete_Nominal_Air_Flow,
+    SET PSZ_10_MainSupVdotSet = argDiscreteMainVdot;
+
+
+  EnergyManagementSystem:Subroutine,
+    Select_Discrete_Nominal_Air_Flow,
+    ! argMainVdot          Input
+    ! argDiscreteMainVdot         Output
+    IF (argMainVdot < = 0.56628) , ! 1200 cfm
+      SET argDiscreteMainVdot = 0.56628 ,
+    ELSEIF (argMainVdot > 0.56628) && (argMainVdot < = 0.75504) , ! 1600 CFM
+      SET argDiscreteMainVdot = 0.75504 ,
+    ELSEIF (argMainVdot > 0.75504) && (argMainVdot < = 0.9438 ) , ! 2000 CFM
+      SET argDiscreteMainVdot = 0.9438 ,
+    ELSEIF (argMainVdot > 0.9438) && (argMainVdot < = 1.13256 ) , ! 2400 CFM
+      SET argDiscreteMainVdot = 1.13256 ,
+    ELSEIF (argMainVdot > 1.13256) && (argMainVdot < = 1.4157 ) , ! 3000 CFM
+      SET argDiscreteMainVdot = 1.4157 ,
+    ELSEIF (argMainVdot > 1.4157) && (argMainVdot < = 1.60446 ) , ! 3400 CFM
+      SET argDiscreteMainVdot = 1.60446 ,
+    ELSEIF (argMainVdot > 1.60446) && (argMainVdot < = 1.8879 ) , ! 4000 CFM
+      SET argDiscreteMainVdot = 1.8879 ,
+    ELSEIF (argMainVdot > 1.8879), ! too high
+      set dummy = @SevereWarnEP 666.0,
+    ENDIF;
+
+
+  EnergyManagementSystem:GlobalVariable, argDiscreteMainVdot;
+  EnergyManagementSystem:GlobalVariable, argMainVdot;
+
+
+  EnergyManagementSystem:InternalVariable,
+     PSZ_1_CalcMainSupVdot,
+     PSZ-AC_1:1 ,
+     Intermediate Air System Main Supply Volume Flow Rate;
+
+
+  EnergyManagementSystem:Actuator,
+     PSZ_1_MainSupVdotSet,                            ! Name
+     PSZ-AC_1:1  ,                  ! Component Name
+     Sizing:System, ! Component Type
+     Main Supply Volume Flow Rate;    ! Control Type
+
+
+
+
+  EnergyManagementSystem:InternalVariable,
+     PSZ_2_CalcMainSupVdot,
+     PSZ-AC_2:2 ,
+     Intermediate Air System Main Supply Volume Flow Rate;
+
+
+  EnergyManagementSystem:Actuator,
+     PSZ_2_MainSupVdotSet,                            ! Name
+     PSZ-AC_2:2  ,                  ! Component Name
+     Sizing:System, ! Component Type
+     Main Supply Volume Flow Rate;    ! Control Type
+
+
+  EnergyManagementSystem:InternalVariable,
+     PSZ_3_CalcMainSupVdot,
+     PSZ-AC_3:3 ,
+     Intermediate Air System Main Supply Volume Flow Rate;
+
+
+  EnergyManagementSystem:Actuator,
+     PSZ_3_MainSupVdotSet,                            ! Name
+     PSZ-AC_3:3  ,                  ! Component Name
+     Sizing:System, ! Component Type
+     Main Supply Volume Flow Rate;    ! Control Type
+
+
+  EnergyManagementSystem:InternalVariable,
+     PSZ_4_CalcMainSupVdot,
+     PSZ-AC_4:4 ,
+     Intermediate Air System Main Supply Volume Flow Rate;
+
+
+  EnergyManagementSystem:Actuator,
+     PSZ_4_MainSupVdotSet,                            ! Name
+     PSZ-AC_4:4  ,                  ! Component Name
+     Sizing:System, ! Component Type
+     Main Supply Volume Flow Rate;    ! Control Type
+
+
+  EnergyManagementSystem:InternalVariable,
+     PSZ_5_CalcMainSupVdot,
+     PSZ-AC_5:5 ,
+     Intermediate Air System Main Supply Volume Flow Rate;
+
+
+  EnergyManagementSystem:Actuator,
+     PSZ_5_MainSupVdotSet,                            ! Name
+     PSZ-AC_5:5  ,                  ! Component Name
+     Sizing:System, ! Component Type
+     Main Supply Volume Flow Rate;    ! Control Type
+
+
+  EnergyManagementSystem:InternalVariable,
+     PSZ_6_CalcMainSupVdot,
+     PSZ-AC_6:6 ,
+     Intermediate Air System Main Supply Volume Flow Rate;
+
+
+  EnergyManagementSystem:Actuator,
+     PSZ_6_MainSupVdotSet,                            ! Name
+     PSZ-AC_6:6  ,                  ! Component Name
+     Sizing:System, ! Component Type
+     Main Supply Volume Flow Rate;    ! Control Type
+
+
+  EnergyManagementSystem:InternalVariable,
+     PSZ_7_CalcMainSupVdot,
+     PSZ-AC_7:7 ,
+     Intermediate Air System Main Supply Volume Flow Rate;
+
+
+  EnergyManagementSystem:Actuator,
+     PSZ_7_MainSupVdotSet,                            ! Name
+     PSZ-AC_7:7  ,                  ! Component Name
+     Sizing:System, ! Component Type
+     Main Supply Volume Flow Rate;    ! Control Type
+
+
+  EnergyManagementSystem:InternalVariable,
+     PSZ_8_CalcMainSupVdot,
+     PSZ-AC_8:8 ,
+     Intermediate Air System Main Supply Volume Flow Rate;
+
+
+  EnergyManagementSystem:Actuator,
+     PSZ_8_MainSupVdotSet,                            ! Name
+     PSZ-AC_8:8  ,                  ! Component Name
+     Sizing:System, ! Component Type
+     Main Supply Volume Flow Rate;    ! Control Type
+
+
+  EnergyManagementSystem:InternalVariable,
+     PSZ_9_CalcMainSupVdot,
+     PSZ-AC_9:9 ,
+     Intermediate Air System Main Supply Volume Flow Rate;
+
+
+  EnergyManagementSystem:Actuator,
+     PSZ_9_MainSupVdotSet,                            ! Name
+     PSZ-AC_9:9  ,                  ! Component Name
+     Sizing:System, ! Component Type
+     Main Supply Volume Flow Rate;    ! Control Type
+
+
+  EnergyManagementSystem:InternalVariable,
+     PSZ_10_CalcMainSupVdot,
+     PSZ-AC_10:10 ,
+     Intermediate Air System Main Supply Volume Flow Rate;
+
+
+  EnergyManagementSystem:Actuator,
+     PSZ_10_MainSupVdotSet,                            ! Name
+     PSZ-AC_10:10  ,                  ! Component Name
+     Sizing:System, ! Component Type
+     Main Supply Volume Flow Rate;    ! Control Type
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-examples/example-9-demand-management.tex b/doc/ems-application-guide/src/ems-examples/example-9-demand-management.tex
new file mode 100644
index 00000000000..a6ec8117ecd
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-examples/example-9-demand-management.tex
@@ -0,0 +1,381 @@
+\section{Example 9. Demand Management}\label{example-9.-demand-management}
+
+\subsection{Problem Statement}\label{problem-statement-011}
+
+Demand management refers to controlling a building to reduce the peak electrical power draws or otherwise improve the load profile from the perspective of the electric utility. Managing electricity demand is an important application for EMS. We should ask, Can we take the model from example 2 and use the EMS to add demand management?
+
+\subsection{EMS Design Discussion}\label{ems-design-discussion-011}
+
+Example 2 is a model of a large office building, but unfortunately the utility tariff is not a demand-based rate. Therefore, we change to a different set of utility rate input objects so the model has demand charges.
+
+For this example, we assume that demand is managed by turning down the lights and increasing the cooling setpoint. The EMS calling point chosen is ``BeginTimestepBeforePredictor'' because it allows you to change the lighting power levels and temperature setpoints before you predict the zone loads.
+
+To manage the demand, we first need to develop some targets based on some a priori idea of what level of demand should be considered ``high.''~ Therefore, we first run the model without demand management and note the simulation results for demand. There are many ways to obtain the demand results, but one method is to obtain them from the tabular report for Tariffs called ``Native Variables.''~ In that report, the row called PeakDemand is the demand used to calculate demand charges and is listed in kW. We will use these values to construct a target level of demand for each month by taking these results and multiplying by 0.85 in an effort to reduce demand by 15\%. For example, the demand for January was 1,154.01 kW, so we make our target level to be 0.85 * 1154.01 = 980.91 kW and the demand for August was 1,555.20 kW, so the target is 0.85 * 1555.20 = 1,321.92 kW.
+
+To develop our Erl program, we separate the overall task into two parts:
+
+1)~~~Determine the current state of demand management control.
+
+2)~~~Set the controls based on that control state.
+
+We then divide the Erl programs into two main programs and give them descriptive names:~ ``Determine\_Current\_Demand\_Manage\_State'';~ ``Dispatch\_Demand\_Changes\_By\_State.''
+
+The Erl program to determine the control state determines the current status for the demand management controls. You can record and manage the control state by setting the value of a global variable called ``argDmndMngrState.''~ For this example, we develop four control states that represent four levels of demand management:
+
+\begin{itemize}
+\item
+  Level 1 is assigned a value of 0.0 and represents no override to implement changes to demand-related controls.
+\item
+  Level 2 is assigned a value of 1.0 and represents moderately aggressive overrides for demand-related controls.
+\item
+  Level 3 is assigned a value of 2.0 and represents more aggressive override.
+\item
+  Level 4 is assigned a value of 3.0 and represents the most aggressive overrides.
+\end{itemize}
+
+We develop an algorithm for choosing the control state by assuming it should be a function of how close the current power level is to the target power level, the current direction for changes in power use, and the recent history of control state. The current demand is obtained by using a sensor that is based on the ``Total Electric Demand'' output variable. This current demand is compared to the target demand levels discussed as well as a ``level 1'' demand level that is set to be 90\% of the target. If the current demand is higher than the level 1 demand but lower than the target, the state will tend to be at level 1. If the current demand is higher than the target, the current state will be either level 2 or level 3 depending on the trend direction. However, we do not want the response to be too quick because it leads to too much bouncing between control states. Therefore, we also introduce some numerical damping with the behavior that once a control state is selected it should be selected for at least two timesteps before dropping down to a lower level. This damping is modeled with the help of a trend variable that records the control state over time so we can retrieve what the control state was during the past two timesteps.
+
+Once the control state is determined, the Erl programs will use EMS actuators to override controls based on the state. The following table summarizes the control adjustments used in our example for each control state.
+
+% table 9
+\begin{longtable}[c]{p{1.5in}p{2.54in}p{1.94in}}
+\caption{Example 9 Demand Management Adjustments by Control State \label{table:example-9-demand-management-adjustments-by}} \tabularnewline
+\toprule 
+Control State & Lighting Power Ahjustment Factor & Cooling Thermostat Offset \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Example 9 Demand Management Adjustments by Control State} \tabularnewline
+\toprule 
+Control State & Lighting Power Ahjustment Factor & Cooling Thermostat Offset \tabularnewline
+\midrule
+\endhead
+
+0 & None & none \tabularnewline
+1 & 0.9 & -   0.8ºC \tabularnewline
+2 & 0.8 & -   1.5ºC \tabularnewline
+3 & 0.7 & -   2.0ºC \tabularnewline
+\bottomrule
+\end{longtable}
+
+For control state level 0, the actuators are all set to Null so they stop overriding controls and return the model to normal operation.
+
+To alter the lighting power density with EMS, you could use either a direct method that employs a Lights actuator or an indirect method that modifies the lighting schedule. For this example we use the direct method with EnergyManagementSystem:Actuator input objects that enable you to override the Electric Power Level for each zone's lights. We also set up internal variables to obtain the Lighting Power Design Level for each Lights object.~ Finally, we set up an EMS sensor to obtain the lighting schedule value to use in Erl programs. If the demand management control state is 1, 2, or 3, we use the following model to determine a new lighting power level:
+
+Power = (Adjustment Factor) × (Lighting Power Design Level) × (Schedule Value)
+
+There are also two ways to alter the cooling setpoint with EMS. To dynamically alter the cooling setpoints, we modify the schedule rather than directly actuating Zone Temperature Control actuators. Changing the schedule allows one actuator to override all the zones; the more direct approach would require actuators for each zone. (This can be used to advantage if different zones are to be managed differently.)~ The algorithm applies an offset depending on the control state. In the input file, the schedule for cooling setpoints is called CLGSETP\_SCH, so we set up an actuator for this Schedule Value. Because the algorithm is a simple offset from the original schedule, we need to keep track of the values in the original schedule. We cannot use the same schedule as an input to the algorithm because once an actuator overrides the schedule value it will corrupt the original schedule. This would be an example of a circular reference problem. Therefore, we make a copy of the cooling setpoint schedule, naming it CLGSETP\_SCH\_Copy, and use the copy in a EnergyManagementSystem:Sensor object to obtain the current scheduled value for the setpoint. When we override the CLGSETP\_SCH schedule, it will not corrupt the values from the CLGSTEP\_SCH\_Copy schedule used as input.
+
+\subsection{EMS Input Objects}\label{ems-input-objects-011}
+
+The main input objects that implement this example of demand management are listed below and are included in the example file called ``EMSDemandManager\_LargeOffice.idf.''~ The results indicate that demand management controls could reduce electricity costs by around \$40,000 or 10\%.
+
+\begin{lstlisting}
+
+EnergyManagementSystem:ProgramCallingManager,
+    Demand Manager Demonstration,
+    BeginTimestepBeforePredictor,
+    Determine_Current_Demand_Manage_State,
+    Dispatch_Demand_Controls_By_State;
+
+
+  EnergyManagementSystem:Program,
+    Determine_Current_Demand_Manage_State,
+    Set localDemand = CurntFacilityElectDemand / 1000.0 ,
+    Set CurrntTrend = @TrendDirection FacilityElectTrend 4,
+    IF (Month = = 1) ,
+      Set argTargetDemand = 0.85 * 1154.01,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ELSEIF (Month = = 2),
+      Set argTargetDemand = 0.85 * 1150.85 ,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ELSEIF (Month = = 3),
+      Set argTargetDemand = 0.85 * 1313.56 ,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ELSEIF (Month = = 4),
+      Set argTargetDemand = 0.85 * 1364.28,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ELSEIF (Month = = 5),
+      Set argTargetDemand = 0.85 * 1506.29  ,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ELSEIF (Month = = 6),
+      Set argTargetDemand = 0.85 * 1516.93  ,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+
+
+    ELSEIF (Month = = 7),
+      Set argTargetDemand = 0.85 * 1545.20  ,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ELSEIF (Month = = 8),
+      Set argTargetDemand = 0.85 * 1555.20  ,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ELSEIF (Month = = 9),
+      Set argTargetDemand = 0.85 * 1491.38  ,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ELSEIF (Month = = 10),
+      Set argTargetDemand = 0.85 * 1402.86  ,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ELSEIF (Month = = 11),
+      Set argTargetDemand = 0.85 * 1418.69  ,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ELSEIF (Month = = 12),
+      Set argTargetDemand = 0.85 * 1440.48  ,
+      Set argCrntDmnd = localDemand,
+      Set argTrendDirection = CurrntTrend,
+    ENDIF,
+    Run Find_Demand_State;
+
+
+
+
+  EnergyManagementSystem:Subroutine,
+    Find_Demand_State,
+    !  argTargetDemand       Input kW level target
+    !  argCrntDmnd           Input  kW level current
+    !  argTrendDirection            Input   J/hour
+    !  argDmndMngrState     Output  value code, 0.0 = no management,
+    !                        1.0 = level 1 demand management
+    !                     2.0 = level 2 demand management
+    !                     3.0 = level 3 demand management
+    Set DmndStateX1 = @TrendValue Demand_Mgr_State_Trend 1,
+    Set DmndStateX2 = @TrendValue Demand_Mgr_State_Trend 2,
+    Set Level1Demand = 0.9 * argTargetDemand,
+    Set argCrntDmnd = argCrntDmnd,
+    Set argTargetDemand = argTargetDemand,
+    SET argDmndMngrState = DmndStateX1, ! initialize to last state then model changes
+    IF (argCrntDmnd > Level1Demand) && (argCrntDmnd <argTargetDemand) && (argTrendDirection > 0.0),
+
+
+      IF DmndStateX1 < = 1.0,
+        SET argDmndMngrState = 1.0,
+      ELSEIF (DmndStateX1 = = 2.0) && (DmndStateX2 < 2.0),
+        SET argDmndMngrState = 2.0,  ! go at least two timesteps at 2.0
+      ELSEIF (DmndStateX1 = = 3.0) && (DmndStateX2 = = 3.0),
+        SET argDmndMngrState = 2.0,
+      ELSEIF (DmndStateX1 = = 3.0) && (DmndStateX2 = = 2.0),
+        SET argDmndMngrState = 3.0,  ! go at least two timesteps at 3.0
+      ENDIF,
+
+
+    ELSEIF (argCrntDmnd > argTargetDemand) && (argTrendDirection < 0.0),
+      IF DmndStateX1 < = 2.0,
+        SET argDmndMngrState = 2.0,
+      ELSEIF (DmndStateX1 = = 3.0) && (DmndStateX2 = = 2.0) , ! go at least two timesteps at 3.0
+        SET argDmndMngrState = 3.0,
+      ELSEIF (DmndStateX1 = = 3.0) && (DmndStateX2 = = 3.0),
+        SET argDmndMngrState = 2.0,
+      ENDIF,
+
+
+    ELSEIF (argCrntDmnd > argTargetDemand) && (argTrendDirection > = 0.0),
+      Set argDmndMngrState = 3.0,
+    ENDIF;
+
+
+
+
+  EnergyManagementSystem:Program,
+    Dispatch_Demand_Controls_By_State,
+    IF     (argDmndMngrState = = 0.0),
+      RUN Unset_Demand_Controls,
+    ELSEIF (argDmndMngrState = = 1.0),
+      RUN Set_Demand_Level1_Controls,
+    ELSEIF (argDmndMngrState = = 2.0),
+      Run Set_Demand_Level2_Controls,
+    ELSEIF (argDmndMngrState = = 3.0),
+      Run Set_Demand_Level3_Controls,
+    ENDIF;
+
+
+
+
+  EnergyManagementSystem:Subroutine,
+    Unset_Demand_Controls,
+    SET Set_Cooling_Setpoint_Sched    = Null,
+    SET Set_Basement_Lights           = Null,
+    SET Set_Core_bottom_Lights        = Null,
+    SET Set_Core_mid_Lights           = Null,
+    SET Set_Core_top_Lights           = Null,
+    SET Set_Perimeter_bot_ZN_3_Lights = Null,
+    SET Set_Perimeter_bot_ZN_2_Lights = Null,
+    SET Set_Perimeter_bot_ZN_1_Lights = Null,
+    SET Set_Perimeter_bot_ZN_4_Lights = Null,
+    SET Set_Perimeter_mid_ZN_3_Lights = Null,
+    SET Set_Perimeter_mid_ZN_2_Lights = Null,
+    SET Set_Perimeter_mid_ZN_1_Lights = Null,
+    SET Set_Perimeter_mid_ZN_4_Lights = Null,
+    SET Set_Perimeter_top_ZN_3_Lights = Null,
+    SET Set_Perimeter_top_ZN_2_Lights = Null,
+    SET Set_Perimeter_top_ZN_1_Lights = Null,
+    SET Set_Perimeter_top_ZN_4_Lights = Null;
+
+
+  EnergyManagementSystem:Subroutine,
+    Set_Demand_Level1_Controls,
+    ! set lighting power to 90% of what it would otherwise be
+    SET Set_Cooling_Setpoint_Sched    = Cooling_Setpoint_Sched + 0.8, ! add 0.8 deg C to cooling setpoint
+    SET Set_Basement_Lights           = 0.90 * Basement_Lights * BLDG_LIGHT_SCH,
+    SET Set_Core_bottom_Lights        = 0.90 * Core_bottom_Lights * BLDG_LIGHT_SCH,
+    SET Set_Core_mid_Lights           = 0.90 * Core_mid_Lights * BLDG_LIGHT_SCH,
+    SET Set_Core_top_Lights           = 0.90 * Core_top_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_3_Lights = 0.90 * Perimeter_bot_ZN_3_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_2_Lights = 0.90 * Perimeter_bot_ZN_2_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_1_Lights = 0.90 * Perimeter_bot_ZN_1_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_4_Lights = 0.90 * Perimeter_bot_ZN_4_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_3_Lights = 0.90 * Perimeter_mid_ZN_3_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_2_Lights = 0.90 * Perimeter_mid_ZN_2_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_1_Lights = 0.90 * Perimeter_mid_ZN_1_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_4_Lights = 0.90 * Perimeter_mid_ZN_4_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_3_Lights = 0.90 * Perimeter_top_ZN_3_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_2_Lights = 0.90 * Perimeter_top_ZN_2_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_1_Lights = 0.90 * Perimeter_top_ZN_1_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_4_Lights = 0.90 * Perimeter_top_ZN_4_Lights * BLDG_LIGHT_SCH;
+
+
+  EnergyManagementSystem:Subroutine,
+    Set_Demand_Level2_Controls,
+    ! set lighting power to 80% of what it would otherwise be
+    SET Set_Cooling_Setpoint_Sched    = Cooling_Setpoint_Sched + 1.5, ! add 1.5 deg C to cooling setpoint
+    SET Set_Basement_Lights           = 0.80 * Basement_Lights * BLDG_LIGHT_SCH,
+    SET Set_Core_bottom_Lights        = 0.80 * Core_bottom_Lights * BLDG_LIGHT_SCH,
+    SET Set_Core_mid_Lights           = 0.80 * Core_mid_Lights * BLDG_LIGHT_SCH,
+    SET Set_Core_top_Lights           = 0.80 * Core_top_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_3_Lights = 0.80 * Perimeter_bot_ZN_3_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_2_Lights = 0.80 * Perimeter_bot_ZN_2_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_1_Lights = 0.80 * Perimeter_bot_ZN_1_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_4_Lights = 0.80 * Perimeter_bot_ZN_4_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_3_Lights = 0.80 * Perimeter_mid_ZN_3_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_2_Lights = 0.80 * Perimeter_mid_ZN_2_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_1_Lights = 0.80 * Perimeter_mid_ZN_1_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_4_Lights = 0.80 * Perimeter_mid_ZN_4_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_3_Lights = 0.80 * Perimeter_top_ZN_3_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_2_Lights = 0.80 * Perimeter_top_ZN_2_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_1_Lights = 0.80 * Perimeter_top_ZN_1_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_4_Lights = 0.80 * Perimeter_top_ZN_4_Lights * BLDG_LIGHT_SCH;
+
+
+
+
+  EnergyManagementSystem:Subroutine,
+    Set_Demand_Level3_Controls,
+    ! set lighting power to 70% of what it would otherwise be
+    SET Set_Cooling_Setpoint_Sched    = Cooling_Setpoint_Sched + 2.0, ! add 2.0 deg C to cooling setpoint
+    SET Set_Basement_Lights           = 0.70 * Basement_Lights * BLDG_LIGHT_SCH,
+    SET Set_Core_bottom_Lights        = 0.70 * Core_bottom_Lights * BLDG_LIGHT_SCH,
+    SET Set_Core_mid_Lights           = 0.70 * Core_mid_Lights * BLDG_LIGHT_SCH,
+    SET Set_Core_top_Lights           = 0.70 * Core_top_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_3_Lights = 0.70 * Perimeter_bot_ZN_3_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_2_Lights = 0.70 * Perimeter_bot_ZN_2_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_1_Lights = 0.70 * Perimeter_bot_ZN_1_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_bot_ZN_4_Lights = 0.70 * Perimeter_bot_ZN_4_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_3_Lights = 0.70 * Perimeter_mid_ZN_3_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_2_Lights = 0.70 * Perimeter_mid_ZN_2_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_1_Lights = 0.70 * Perimeter_mid_ZN_1_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_mid_ZN_4_Lights = 0.70 * Perimeter_mid_ZN_4_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_3_Lights = 0.70 * Perimeter_top_ZN_3_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_2_Lights = 0.70 * Perimeter_top_ZN_2_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_1_Lights = 0.70 * Perimeter_top_ZN_1_Lights * BLDG_LIGHT_SCH,
+    SET Set_Perimeter_top_ZN_4_Lights = 0.70 * Perimeter_top_ZN_4_Lights * BLDG_LIGHT_SCH;
+
+
+
+
+
+
+  EnergyManagementSystem:GlobalVariable,argTargetDemand;
+  EnergyManagementSystem:GlobalVariable,argCrntDmnd;
+  EnergyManagementSystem:GlobalVariable,argTrendDirection;
+  EnergyManagementSystem:GlobalVariable,argDmndMngrState;
+
+
+  EnergyManagementSystem:Sensor,
+    BLDG_LIGHT_SCH, !- Name
+    BLDG_LIGHT_SCH, !- Output:Variable or Output:Meter Index Key Name
+    Schedule Value; !- Output:Variable or Output:Meter Name
+
+
+
+
+  EnergyManagementSystem:Sensor,
+    CurntFacilityElectDemand,  !- Name
+    Whole Building,        !- Output:Variable or Output:Meter Index Key Name
+    Facility Total Electric Demand Power; !- Output:Variable Name
+
+
+
+
+  EnergyManagementSystem:TrendVariable,
+    Demand_Mgr_State_Trend , !- Name
+    argDmndMngrState, !- EMS Variable Name
+    48 ; !- Number of Timesteps to be Logged
+
+
+  EnergyManagementSystem:TrendVariable,
+    FacilityElectTrend , !- Name
+    CurntFacilityElectDemand, !- EMS Variable Name
+    144 ; !- Number of Timesteps to be Logged
+
+
+  EnergyManagementSystem:Sensor,
+    Cooling_Setpoint_Sched,  !- Name
+    CLGSETP_SCH_Copy,        !- Output:Variable or Output:Meter Index Key Name
+    Schedule Value; !- Output:Variable or Output:Meter Name
+
+
+  EnergyManagementSystem:Actuator,
+    Set_Cooling_Setpoint_Sched,  !- Name
+    CLGSETP_SCH ,     !- Actuated Component Unique Name
+    Schedule:Compact,   !- Actuated Component Type
+    Schedule Value    ; !- Actuated Component Control Type
+
+
+  EnergyManagementSystem:OutputVariable,
+    Erl Cooling Setpoint [C],    !- Name
+    Set_Cooling_Setpoint_Sched,  !- EMS Variable Name
+    Averaged   ,                 !- Type of Data in Variable
+    ZoneTimestep;                !- Update Frequency
+
+
+
+
+  Output:Variable,
+    *,
+    Erl Cooling Setpoint,
+    Timestep;
+
+
+  EnergyManagementSystem:Actuator,
+    Set_Basement_Lights,  !- Name
+    Basement_Lights ,     !- Actuated Component Unique Name
+    Lights,               !- Actuated Component Type
+    Electric Power Level; !- Actuated Component Control Type
+
+
+  EnergyManagementSystem:InternalVariable,
+    Basement_Lights , !- Name
+    Basement_Lights , !- Internal Data Index Key Name
+    Lighting Power Design Level ; !- Internal Data Type
+
+
+  EnergyManagementSystem:Actuator,
+    Set_Core_bottom_Lights, !- Name
+    Core_bottom_Lights ,  !- Actuated Component Unique Name
+    Lights,               !- Actuated Component Type
+    Electric Power Level; !- Actuated Component Control Type
+  EnergyManagementSystem:InternalVariable,
+    Core_bottom_Lights , !- Name
+    Core_bottom_Lights , !- Internal Data Index Key Name
+    Lighting Power Design Level ; !- Internal Data Type
+  << Snipped remaining Lights Sensors and Actuators >>
+\end{lstlisting}
diff --git a/doc/ems-application-guide/src/ems-sensors.tex b/doc/ems-application-guide/src/ems-sensors.tex
new file mode 100644
index 00000000000..65c811a10a2
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-sensors.tex
@@ -0,0 +1,7 @@
+\chapter{EMS Sensors}\label{ems-sensors}
+
+This section provides more information about EMS sensors.
+
+The input object EnergyManagementSystem:Sensor is simple but quite powerful. It reuses the normal EnergyPlus output variables to provide a general way of obtaining a wide variety of input data with minimal complications.
+
+One odd result of the approach taken for EMS sensors is that information about the available sensors is derived from what are usually the outputs of EnergyPlus. The RDD file is an important resource for EMS users. The RDD file is an output from running EnergyPlus and is called ``eplusout.rdd'' (but you may rename it to \textless{}your-filename\textgreater{}.rdd with a run manager such as EP-Launch). This output file is often needed to develop EMS input, so you may need to do an initial run of the model with traditional controls to obtain an RDD file. The contents of an RDD file will vary depending on the type of model. Once you have experience and familiarity with the outputs expected from a model, you should not need to prerun models, as you will be able to foresee the available output. The RDD file from a similar model with the same types of components and systems can also be used as a guide for what will be available in a specific model.
diff --git a/doc/ems-application-guide/src/ems-sensors/schedules.tex b/doc/ems-application-guide/src/ems-sensors/schedules.tex
new file mode 100644
index 00000000000..20795fd4703
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-sensors/schedules.tex
@@ -0,0 +1,3 @@
+\section{Schedules}\label{schedules-000}
+
+The EnergyManagementSystem:Sensor object can also provide scheduled data for use in Erl programs. Because schedule values are available as outputs that use the ``Schedule Value'' output, they can also be mapped as sensors. You can use any of the various types of schedule input objects to define a schedule. The schedule does not need to be used elsewhere in the model. The value of the schedule is then mapped to an EMS variable with the Schedule Value report variable. When used with the Schedule:File input object, the sensor object can import time series data into the EMS from an external file. One application might be to test a proposed EMS algorithm with real experimental data.
diff --git a/doc/ems-application-guide/src/ems-sensors/variable-types.tex b/doc/ems-application-guide/src/ems-sensors/variable-types.tex
new file mode 100644
index 00000000000..c1b9d62a8dc
--- /dev/null
+++ b/doc/ems-application-guide/src/ems-sensors/variable-types.tex
@@ -0,0 +1,10 @@
+\section{Variable Types}\label{variable-types}
+
+Various types of output variables in EnergyPlus can be used as sensors in the EMS. It is important to understand some distinctions.
+
+\begin{itemize}
+\item
+  Reported variables have two update frequencies: \textbf{zone} and \textbf{system}. Zone variables are updated for each zone timestep. System variables are updated for each system timestep.
+\item
+  Reported variables have two types of content: \textbf{averaged} and \textbf{summed}. Averaged variables are state variables such as temperature and mass flow rate. Summed variables are quantities of energy such as electricity use.
+\end{itemize}
diff --git a/doc/ems-application-guide/src/energyplus-runtime-language.tex b/doc/ems-application-guide/src/energyplus-runtime-language.tex
new file mode 100644
index 00000000000..2f1c5b6c35a
--- /dev/null
+++ b/doc/ems-application-guide/src/energyplus-runtime-language.tex
@@ -0,0 +1,3 @@
+\chapter{EnergyPlus Runtime Language}\label{energyplus-runtime-language}
+
+Erl is the simplified programming language used to define the EMS control and modeling programs. This section describes the rules and syntax for using Erl to write programs.
diff --git a/doc/ems-application-guide/src/energyplus-runtime-language/built-in-functions.tex b/doc/ems-application-guide/src/energyplus-runtime-language/built-in-functions.tex
new file mode 100644
index 00000000000..0293d538fa1
--- /dev/null
+++ b/doc/ems-application-guide/src/energyplus-runtime-language/built-in-functions.tex
@@ -0,0 +1,231 @@
+\section{Built-In Functions}\label{built-in-functions}
+
+Several useful, built-in functions are available for use in Erl programs. You cannot configure these; they are internal to the language processor inside EnergyPlus. They provide access to a subset of general service routines that are useful inside the main EnergyPlus program or are intrinsic functions available in the underlying Fortran language. The ``@'' character is used to signal to the language processor that the following character string defines a built-in function that is used to assign a result to an Erl variable. The characters appended to the ``@'' operator must be one of the predefined names listed in Table~\ref{table:built-in-math-functions-for-erl}, Table~\ref{table:built-in-energyplus-simulation-management}, Table~\ref{table:built-in-functions-for-trend-variables-in-erl}, or Table~\ref{table:built-in-psychrometric-functions-for-erl}. The syntax of the function call will vary depending on the arguments required by the function, but the general structure is:
+
+SET \textless{}variable\textgreater{} = @\textless{}function name\textgreater{}~ \textless{}argument1\textgreater{}~ \textless{}argument2\textgreater{}~~ \ldots{}~~ \textless{}argumentN\textgreater{}
+
+Where ``argument'' can be either an Erl variable or a numeric constant.
+
+For example, the following two statements can be used to set the value of an Erl variable called mySupplyRH to have percent relative humidity.
+
+SET mySupplyRH = @RhFnTdbWPb mySupplyDryblub mySupplyHumRat mySupplyPress
+
+SET mySupplyRH = mySupplyRH * 100
+
+\subsection{Built-in Math Functions}\label{built-in-math-functions}
+
+Table~\ref{table:built-in-math-functions-for-erl} lists the built-in functions for common mathematical functions. The numerical model for these functions is provided by the underlying Fortran language and the compiler.
+
+% table 4
+\begin{longtable}[c]{p{1.5in}p{3.0in}p{1.5in}}
+\caption{Built-in Math Functions for Erl \label{table:built-in-math-functions-for-erl}} \tabularnewline
+\toprule 
+Function Name & Description & Number of Arguments \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Built-in Math Functions for Erl} \tabularnewline
+\toprule 
+Function Name & Description & Number of Arguments \tabularnewline
+\midrule
+\endhead
+
+@Round & Decreases precision of real number argument to nearest whole number, remains a real number. & 1 \tabularnewline
+@Mod & Returns remainder after dividing the first argument by the second. & 2 \tabularnewline
+@Sin & Sine, returns sine of angle given in radians. & 1 \tabularnewline
+@Cos & Cosine, returns cosine of angle given in radians. & 1 \tabularnewline
+@ArcSin & Arcsine, returns angle in radians from sine of angle. & 1 \tabularnewline
+@ArcCos & ArcCosine, returns angle in radians from cosine of angle. & 1 \tabularnewline
+@DegToRad & Degrees to radians, returns radians from degrees. & 1 \tabularnewline
+@RadToDeg & Radians to degrees, returns degrees from radians. & 1 \tabularnewline
+@Exp & Exponential, e  , returns result. & 1 \tabularnewline
+@Ln & Natural log, log  (x), returns result. & 1 \tabularnewline
+@Max & Maximum, returns largest value of two arguments. & 2 \tabularnewline
+@Min & Minimum, returns smallest value of two arguments. & 2 \tabularnewline
+@Abs & Absolute value, returns positive magnitude of argument. & 1 \tabularnewline
+@RandomUniform & Pseudo-Random Number Generator, returns random number with uniform probability distribution across the range of values passed as the arguments, inclusive. Argument 1 is the lower limit. Argument 2 is the upper limit. & 2 \tabularnewline
+@RandomNormal & Pseudo-Random Number Generator, returns random number with normal (Gaussian) probability distribution as a function of the mean, standard deviation, and limits. Argument 1 is the mean. Argument 2 is the standard deviation. Argument 3 is the lower limit. Argument 4 is the upper limit. & 4 \tabularnewline
+@SeedRandom & Random Seed, controls the seed used in the random number generator for calls to @RandomUniform and @RandomNormal.~ Use is optional and provided for repeatable series of random numbers. The argument is rounded to the nearest whole number and then used to set the size and values of the seed for the number generator.~ & 1 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Built-In Simulation Management Functions}\label{built-in-simulation-management-functions}
+
+% table 5
+\begin{longtable}[c]{p{1.5in}p{3.0in}p{1.5in}}
+\caption{Built-in EnergyPlus Simulation Management Functions for Erl \label{table:built-in-energyplus-simulation-management}} \tabularnewline
+\toprule 
+Function Name & Description & Number of Arguments \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Built-in EnergyPlus Simulation Management Functions for Erl} \tabularnewline
+\toprule 
+Function Name & Description & Number of Arguments \tabularnewline
+\midrule
+\endhead
+
+@FatalHaltEp & Throws fatal error with time of occurrence and stops execution of current model. Argument passes a number that can be used as an error code. & 1 \tabularnewline
+@SevereWarnEp & Throws severe error with time of occurrence and continues execution. Argument passes a number that can be used as an error code. & 1 \tabularnewline
+@WarnEp & Throws warning error and continues execution. Argument passes a number that can be used as an error code. & 1 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Built-in Trend Variable Functions}\label{built-in-trend-variable-functions}
+
+For control algorithms, you often need to be able put a sensor reading into some historical context. The trend variables are provided in Erl as a way to log the time history of data to use in control decisions. To use the trend variables in Erl programs, their values must be extracted and placed into normal Erl variables. Setting up an Erl variable as a trend variable requires an EnergyManagementSystem:TrendVariable input object. The access functions listed in Table~\ref{table:built-in-functions-for-trend-variables-in-erl} are used to obtain data from a trend variable during the execution of an Erl program. These functions act on trend variables and return values into the user's Erl variables for subsequent use in calculations. Each trend function takes the name of the trend variable and an index that identifies how far back in time the function should be applied. Trend variable names are also Erl variables but with special pointers to another data structure with the time series data storage. The trend logs have a first-in, first-out storage array where only the most recent data are retained. Each element in the history corresponds to the result for that value over a zone timestep. The time difference between trend log items is the zone timestep in hours, so that the slope returned by @TrendDirection is in per-hour units.
+
+% table 6
+\begin{longtable}[c]{p{1.5in}p{3.0in}p{1.5in}}
+\caption{Built-in Functions for Trend Variables in Erl \label{table:built-in-functions-for-trend-variables-in-erl}} \tabularnewline
+\toprule 
+Function Name & Description & Number of Arguments \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Built-in Functions for Trend Variables in Erl} \tabularnewline
+\toprule 
+Function Name & Description & Number of Arguments \tabularnewline
+\midrule
+\endhead
+
+@TrendValue & Returns history value for a particular number of timesteps into the past. Dereferences data stored in trend into another Erl variable. Takes trend variable name and the specific timestep into the past to return. & 2 \tabularnewline
+@TrendAverage & Returns historical average (mean) for values in trend variable. Takes trend variable name and number of steps into the past to analyze & 2 \tabularnewline
+@TrendMax & Returns historical maximum for values in trend variable. Takes trend variable name and number of steps into the past to analyze. & 2 \tabularnewline
+@TrendMin & Returns historical minimum for values in trend variable within the index. Takes trend variable name and number of steps into the past to analyze. & 2 \tabularnewline
+@TrendDirection & Returns slope of a linear least squares fit of trend data within the index. Positive if trend is increasing, negative if decreasing. Takes trend variable name and number of steps into the past to analyze. & 2 \tabularnewline
+@TrendSum & Returns sum of elements stored in trend. Takes trend variable name and number of steps into the past to analyze. & 2 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The trend functions all take as their second argument an array index. This number should be considered an integer for locating an array position. (It will be rounded down to the nearest integer using Fortran's FLOOR intrinsic.)~ This index argument tells the trend functions how far back in time they should reach into the history log when they evaluate the function call. This enables you to compare long- and short-range trends.
+
+\subsection{Built-in Psychrometric Functions}\label{built-in-psychrometric-functions}
+
+Building modeling often involves calculations related to moist air. A comprehensive set of built-in functions is available for psychrometric calculations. Table~\ref{table:built-in-psychrometric-functions-for-erl} lists the functions available for use in Erl programs that are related to moist air properties and some physical properties related to water. More discussion of the psychrometric functions is provided in the section ``Pyschrometric services'' in the Module Developer Guide.
+
+% table 7
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Built-in Psychrometric Functions for Erl \label{table:built-in-psychrometric-functions-for-erl}} \tabularnewline
+\toprule 
+Function Name & Arguments & Description & Units \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Built-in Psychrometric Functions for Erl} \tabularnewline
+\toprule 
+Function Name & Arguments & Description & Units \tabularnewline
+\midrule
+\endhead
+
+@RhoAirFnPbTdbW & Result & Density of moist air & kg/m < sup > 3 < /sup > \tabularnewline
+Input 1 & Barometric pressure & Pa \tabularnewline
+Input 2 & Drybulb temperature & °C \tabularnewline
+Input 3 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+@CpAirFnWTdb & Result & Heat capacity of moist air & J/kg-°C \tabularnewline
+Input 1 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 2 & Drybulb temperature & °C \tabularnewline
+@HfgAirFnWTdb` & Result & Heat of vaporization for vapor & J/kg \tabularnewline
+Input 1 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 2 & Drybulb temperature & °C \tabularnewline
+@HgAirFnWTdb & Result & Enthalpy of the gas &  \tabularnewline
+Input 1 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 2 & Drybulb temperature & °C \tabularnewline
+@TdpFnTdbTwbPb & Result & Dew-point temperature & °C \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Wetbulb temperature & °C \tabularnewline
+Input 3 & Barometric pressure & Pa \tabularnewline
+@TdpFnWPb & Result & Dew-point temperature & °C \tabularnewline
+Input 1 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 2 & Barometric pressure & Pa \tabularnewline
+@HFnTdbW & Result & Enthalpy of moist air & J/kg \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+@HFnTdbRhPb & Result & Enthalpy of moist air & J/kg \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Relative humidity & Fraction (0.0 .. 1) \tabularnewline
+Input 3 & Barometric pressure & Pa \tabularnewline
+@TdbFnHW & Result & Drybulb temperature & °C \tabularnewline
+Input 1 & Enthalpy of moist air & J/kg \tabularnewline
+Input 2 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+@RhovFnTdbRh & Result & Vapor density in air & kg/m < sup > 3 < /sup > \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Relative humidity & Fraction (0.0 .. 1) \tabularnewline
+@RhovFnTdbWPb & Result & Vapor density in air & kg/m < sup > 3 < /sup > \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 3 & Barometric pressure & Pa \tabularnewline
+@RhFnTdbRhov & Result & Relative humidity & Fraction (0.0 .. 1) \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Vapor density in air & kg/m < sup > 3 < /sup > \tabularnewline
+@RhFnTdbWPb & Result & Relative humidity & Fraction (0.0 .. 1) \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 3 & Barometric pressure & Pa \tabularnewline
+@TwbFnTdbWPb & Result & Wetbulb temperature & °C \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 3 & Barometric pressure & Pa \tabularnewline
+@VFnTdbWPb & Result & Specific volume & m < sup > 3 < /sup > /kg \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 3 & Barometric pressure & Pa \tabularnewline
+@WFnTdpPb & Result & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 1 & Dew-point temperature & °C \tabularnewline
+Input 2 & Barometric pressure & Pa \tabularnewline
+@WFnTdbH & Result & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Enthalpy of moist air & J/kg \tabularnewline
+@WFnTdbTwbPb & Result & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Wetbulb temperature & °C \tabularnewline
+Input 3 & Barometric pressure & Pa \tabularnewline
+@WFnTdbRhPb & Result & Humidity ratio & kgWater/kgDryAir \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+Input 2 & Relative humidity & Fraction (0.0 .. 1) \tabularnewline
+Input 3 & Barometric pressure & Pa \tabularnewline
+@PsatFnTemp & Result & Saturation pressure & Pa \tabularnewline
+Input 1 & Drybulb temperature & °C \tabularnewline
+@TsatFnHPb & Result & Saturation temperature & °C \tabularnewline
+Input 1 & Enthalpy of moist air & J/kg \tabularnewline
+Input 2 & Barometric pressure & Pa \tabularnewline
+@CpCW & Result & Heat capacity of water & J/kg \tabularnewline
+Input 1 & Temperature & °C \tabularnewline
+@CpHW & Result & Heat capacity of water & J/kg \tabularnewline
+Input 1 & Temperature & °C \tabularnewline
+@RhoH2O & Result & Density of water & kg/m < sup > 3 < /sup > \tabularnewline
+Input 1 & Temperature & °C \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Built-in Curve and Table Functions}\label{built-in-curve-and-table-functions}
+
+EnergyPlus has a number of different generic curve and table input objects that are used to describe the performance characteristics for various component models.~ Table~\ref{table:built-in-function-for-accessing-curves} describes a built-in function called @CurveValue that is available for reusing those curve and table input objects in your Erl programs.~ Although the Erl language could be used to replicate the functionality, reusing those input objects can have advantages because the input may have already been developed for use in traditional component models or the limiting and interpolation methods are helpful.~ The @CurveValue function expects six arguments, although usually only a subset of them will be used depending on the number of independent variables involved with the curve or table.~ Because Erl does not support passing optional arguments, dummy variables do need to be included in the function call for all unused independent variables.~ For example, the Curve:Biquadratric object has only x and y independent variables, so input arguments 4, 5, and 6 will not be used when @CurveValue is evaluated:
+
+~~~~~ Set MyCurveResult = @CurveValue myCurveIndex X1 Y1 dummy dummy dummy;
+
+The first input argument is always an Erl variable that has been declared using an EnergyManagementSystem:CurveOrTableIndexVariable input object.~ This variable identifies the location of a specific curve or table in the program's internal data structures.~ It is important that you do not inadvertently reassign the value held in this variable because it is only filled once at the beginning of the simulation.
+
+% table 8
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Built-in Function for Accessing Curves and Tables \label{table:built-in-function-for-accessing-curves}} \tabularnewline
+\toprule 
+Function Name & Arguments & Description & Notes \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Built-in Function for Accessing Curves and Tables} \tabularnewline
+\toprule 
+Function Name & Arguments & Description & Notes \tabularnewline
+\midrule
+\endhead
+
+@CurveValue & Result & Result from evaluating the curve or table as a function of the input arguments &  \tabularnewline
+Input 1 & Index variable that "points" to a specific curve or table object defined elsewhere in the IDF. & This variable needs to be declared and filled using an EnergyManagementSystem:CurveOrTableIndexVariable object. \tabularnewline
+Input 2 & First independent variable & Typically the "X" input value, always used \tabularnewline
+Input 3 & Second independent variable & Typically the "Y" value, only used if curve/table has two or more independent variables \tabularnewline
+Input 4 & Third independent variable & Typically the "Z" value, only used if curve/table has three or more independent variables. \tabularnewline
+Input 5 & Fourth independent variable & Only used if table has four or more independent variables \tabularnewline
+Input 6 & Fifth independent variable & Only used if table has five independent variables \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/ems-application-guide/src/energyplus-runtime-language/expressions.tex b/doc/ems-application-guide/src/energyplus-runtime-language/expressions.tex
new file mode 100644
index 00000000000..c99d88639af
--- /dev/null
+++ b/doc/ems-application-guide/src/energyplus-runtime-language/expressions.tex
@@ -0,0 +1,68 @@
+\section{Expressions}\label{expressions}
+
+An expression is a sequence of variables and/or constants linked together by operators. An expression is always evaluated to a single value.
+
+The rules for expressions are:
+
+\begin{itemize}
+\item
+  An expression is a sequence of variables and/or constants linked by operators.
+\item
+  Expressions always evaluate to a single value.
+\item
+  Comparison operators evaluate to 1.0 for ``true'' or 0.0 for ``false.''
+\item
+  Compound expressions are allowed and can be organized with parentheses.
+\end{itemize}
+
+The operators shown in Table~\ref{table:operators-for-erl} are available for use in Erl programs.
+
+% table 3
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Operators for Erl \label{table:operators-for-erl}} \tabularnewline
+\toprule 
+Operator Symbol & Description & Evaluation Order & Example \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Operators for Erl} \tabularnewline
+\toprule 
+Operator Symbol & Description & Evaluation Order & Example \tabularnewline
+\midrule
+\endhead
+
+( ) & Parentheses & left-to-right & SET z = 23/(3 + 2) \tabularnewline
++ & Addition & right-to-left & SET a = 4 + 5 \tabularnewline
+- & Subtraction & right-to-left & SET b = a - 3 \tabularnewline
+* & Multiplication & right-to-left & SET c = a * b \tabularnewline
+/ & Division & left-to-right & SET d = b/a \tabularnewline
+\^{} & Raise to a power & left-to-right & SET e = c \^{} 0.5 \tabularnewline
+== & Equality comparison & left-to-right & IF a == b \tabularnewline
+< > ~ & Inequality comparison & left-to-right & IF c  < >  d \tabularnewline
+> ~ & Greater than comparison & left-to-right & IF a  >  e \tabularnewline
+> = & Greater than or equal to comparison & left-to-right & IF a  > = 6 \tabularnewline
+< ~ & Less than comparison & left-to-right & IF b  <  2 \tabularnewline
+< = & Less than or equal to comparison & left-to-right & IF b  < = f \tabularnewline
+\& \& & Logical AND & right-to-left & IF c  \& \&  d \tabularnewline
+|| & Logical OR & right-to-left & IF c || d \tabularnewline
+\bottomrule
+\end{longtable}
+
+Because expressions can be evaluated to a single value, they can be used in SET and IF statements. That means both of the following instructions are allowed:
+
+\begin{lstlisting}
+SET a = c < d
+IF a - 1
+\end{lstlisting}
+
+In the case of the SET example, the value of ``a'' is set to 1 if ``c'' is less than ``d''; otherwise, it is set to 0. For the IF example, the IF block of instructions are executed if a -- 1 is greater than zero.
+
+Compound expressions allow multiple operators to be sequenced or nested. For example:
+
+\begin{lstlisting}
+a + b \* 7 / 4.5
+(a \* 3 + 4) ^ 2
+(a > b) && (c < d)
+\end{lstlisting}
+
+For complicated expressions, it helps to make heavy use of parentheses in your equations.~ By using parentheses with proper algebraic evaluation in mind to group terms, you can help the Erl parser.~ The language processor is simplistic compared to a full-blown programming language and sometimes has problems applying the rules of algebra.~ It is safer to err on the side of extra parentheses and to inspect the results of complex expressions in the EDD output.
diff --git a/doc/ems-application-guide/src/energyplus-runtime-language/statement-keywords.tex b/doc/ems-application-guide/src/energyplus-runtime-language/statement-keywords.tex
new file mode 100644
index 00000000000..491b30c9b1d
--- /dev/null
+++ b/doc/ems-application-guide/src/energyplus-runtime-language/statement-keywords.tex
@@ -0,0 +1,74 @@
+\section{Statement Keywords}\label{statement-keywords}
+
+Every programming language has instructions or commands that tell the processor what to do. Erl supports a few types of program statements. Each line of an Erl program begins with a statement keyword. The syntax for each line depends on the keyword that starts that line. Only those listed in Table 1 are allowed.
+
+\begin{longtable}{@{}ll>{\raggedright}p{3in}@{}}
+
+\caption{Programming Statements in ERL \label{table:programming-statements-in-erl}} \tabularnewline
+\toprule
+Keyword & Syntax & Statement Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Programming Statements in ERL} \tabularnewline
+\toprule
+Keyword & Syntax & Statement Description \tabularnewline
+\midrule
+\endhead
+
+RUN & RUN <program name> & Calls another Erl program or subroutine. Returns to the calling point when completed. Recursive calling is allowed. \tabularnewline
+RETURN & RETURN, & Prematurely exits a subroutine or program and returns control to the caller. \tabularnewline
+SET & SET <variable> = <expression>, & Assigns the right-hand side to the left-hand side. If <variable> has not been used before, it is dynamically declared (with local scope). \textbf{Note: <variables> should NOT start with numerics.} \tabularnewline
+IF & IF <expression>, & Begins an ``IF block.'' Conditional decision. If <expression> evaluates to anything other than zero, the block of statements after the IF is executed. \tabularnewline
+ELSEIF & ELSEIF <expression> & Conditional decision that follows a regular IF block of instructions. If <expression> evaluates to anything other than zero, the block of instructions after the ELSEIF is executed. \tabularnewline
+ELSE & ELSE, & Conditional decision. Associated with an IF statement, the block of statements after the ELSE is executed if <expression> evaluates to zero for preceding IF and ELSEIF statements. \tabularnewline
+ENDIF & ENDIF, & Terminates IF block (required). \tabularnewline
+WHILE & WHILE <expression> & Begins a ``WHILE block.'' Conditional decision. If <expression> evaluates to anything other than zero, the block of statements after the WHILE is repeatedly executed. \tabularnewline
+ENDWHILE & ENDWHILE, & Terminates WHILE block (required). \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Rules for IF blocks:}\label{rules-for-if-blocks}
+
+\begin{itemize}
+\item
+  IF blocks can be nested, but only up to five deep.
+\item
+  ELSE is optional. If omitted, the IF block is terminated by ENDIF.
+\end{itemize}
+
+IF-ELSEIF-ELSE-ENDIF blocks are allowed. If there are many ELSEIF statements, the first in the list that evaluates to true (1.0) is applied and the execution jumps to the ENDIF for that IF block. If no IF or ELSEIF is true, the ELSE condition (if any) is applied. A single IF block currently has a limit of 199 ELSEIF statements plus one ELSE statement.
+
+\subsection{Rules for WHILE blocks:}\label{rules-for-while-blocks}
+
+\begin{itemize}
+\item
+  WHILE blocks cannot be nested.
+\item
+  A WHILE block must be terminated by an ENDWHILE
+\item
+  The block is repeated until the expression following the WHILE statement evaluates to 0.0 (false).
+\item
+  Once the WHILE loop is entered, there is a maximum limit on the number of times the loop can be repeated. The limit is set at one million repetitions to protect against the possibility of an Erl program entering an infinite loop if the WHILE loop's expression is malformed so as to never evaluate to 0.0 (false).
+\end{itemize}
+
+Erl programs are entered into the input data file (IDF) using the input objects called EnergyManagementSystem:Program and EnergyManagementSystem:Subroutine. These objects use individual fields to store the statements for an Erl program. As with most EnergyPlus objects, each field is separated by a comma and typically given a separate line of text for readability. In this case, each field can be considered a separate line of Erl program code. Every input field (line of code) must conform to the following rules:
+
+\begin{itemize}
+\item
+  Every input field contains only one statement.
+\item
+  Every field begins with a statement keyword that identifies what that particular line of code is doing.
+\item
+  The syntax for each statement depends on the keyword.
+\item
+  All field content (keywords, variable names, etc.) is case insensitive.
+\item
+  A comma (or semicolon if it is the last field) marks the end of every statement.
+\item
+  The maximum length for a field is 100 characters. If you enter a longer field, it will be truncated to the first 100 characters. This can have subtle effects if the remaining portion forms a viable expression.
+\item
+  The ``!'' character is for comments.
+\end{itemize}
+
+REMEMBER, every line needs to end in a comma or, if it is the last in the program, a semicolon.
diff --git a/doc/ems-application-guide/src/energyplus-runtime-language/variables.tex b/doc/ems-application-guide/src/energyplus-runtime-language/variables.tex
new file mode 100644
index 00000000000..3831d4befc0
--- /dev/null
+++ b/doc/ems-application-guide/src/energyplus-runtime-language/variables.tex
@@ -0,0 +1,113 @@
+\section{Variables}\label{variables}
+
+Variables are important to any programming language. All Erl variables, except trend variables, are treated the same way in Erl and can be used interchangeably with any instruction.
+
+The rules for selecting names of EMS variables are:
+
+\begin{itemize}
+\item
+  No spaces are allowed in user-defined variable names.
+\item
+  Underscore (``\_'') is the only special character allowed in variable names.
+\item
+  Variable names are \textbf{not} case sensitive.
+\item
+  Names of variables with global scope must be unique.
+\item
+  Variables cannot be declared with the same name as a built-in variable.
+\item
+  Variables can be alpha numeric strings but should NOT start with a numeric.
+\end{itemize}
+
+The rules for using EMS variables are:
+
+\begin{itemize}
+\item
+  All numeric variables are treated as floating point numbers. You use the underlying Fortran language features to handle these as double precision real numbers.
+\item
+  You can use the SET statement to reassign sensor variables and built-in variables.
+\item
+  Actuator variables use SET to perform control actions.
+\end{itemize}
+
+EMS variables can have either local or global scope. Global scope means that the variables can be used across Erl programs and always refer to the same instance of a particular variable. Global variables must have unique names. Local scope means that variables can be used only within a given Erl program.
+
+Erl programs have eight types of variables:
+
+\begin{itemize}
+\item
+  Sensor. Each EnergyManagementSystem:Sensor input object declares a user-defined variable and maps it to a variable elsewhere in EnergyPlus (via output variables). Variables so declared have global scope and are used to \emph{get} time-varying input data from elsewhere in the EnergyPlus model.
+\item
+  Actuator. Each EnergyManagementSystem:Actuator input object declares a user-defined Erl variable and maps it to a variable elsewhere in EnergyPlus. Variables so declared have global scope and are used to \emph{set} control results elsewhere in the EnergyPlus model.
+\item
+  Local. Local variables do not need to be explicitly declared. These undeclared variables will be automatically registered as EMS variables with local scope. This allows you to create new variables ``on the fly.''~ Local variables can be used for temporary storage of intermediate results.
+\item
+  Global. EnergyManagementSystem:GlobalVariable input objects are used to declare variables with a user-defined name and global scope. Global variables can be used to store intermediate results that span across Erl programs. Because the Erl compiler does not support functions or argument passing, global variables have an important role in using subroutines. These variables are global only within Erl and not with respect to code elsewhere in EnergyPlus.
+\item
+  Built-in. The EMS system automatically declares a set of built-in variables with predefined names. These variables have global scope. The built-in variables are always created and cannot be eliminated.
+\item
+  Internal. Each EnergyManagementSystem:InternalVariable input object declares a user-defined Erl variable and maps it to a variable elsewhere in EnergyPlus. Variables so declared have global scope and are used to \emph{get} static input data from elsewhere in EnergyPlus.
+\item
+  Trend. Each EnergyManagementSystem:TrendVariable input object declares a user-defined Erl trend variable and maps it to a global Erl variable for logging. Trend variables are used to store the history of Erl variables. Trend variables differ from other Erl variables in that they can be put to use only through the built-in trend functions (see Table~\ref{table:built-in-functions-for-trend-variables-in-erl}).
+\item
+  Index. Each EnergyManagementSystem:CurveOrTableIndexVariable and/or EnergyManagementSystem:ConstructionIndexVariable declares a user defined Erl variable and maps it to a specific item in the IDF of indicated type.
+\end{itemize}
+
+Built-in variables, internal variables, and sensor variables are primarily used to \emph{get} information about the state of the simulation. However, because all variables are treated alike, built-in variables and sensor variables can also be overwritten by the SET instruction. (This applies within the EMS only; the variables in the rest of EnergyPlus program will not be overwritten.)~ This allows you to reassign constants such as ``on'' and ``off'' as well as the values of the other built-in variables and sensor variables. There is really no problem with this, as long as you know what you are doing. One possible application is to reset a sensor variable that references the outdoor drybulb temperature so it contains the temperature in degrees Fahrenheit instead of Celsius. Regardless of reassignment, sensor variables and the dynamic built-in variables (e.g., date and time) will be cleared and updated with the latest values from EnergyPlus at the next timestep. Resetting a sensor variable does not have a retroactive effect on the report variable to which it is mapped.
+
+The actuator variable is the counterpart of the sensor variable. Sensor variables are used to \emph{get} the state of building systems; actuator variables are used to \emph{set} the state of building systems. When used with actuator variables, the SET instruction performs control actions on the object to which it maps.
+
+\subsection{Built-In Variables}\label{built-in-variables}
+
+A set of built-in variables provides date, time, and weather information that is not available via standard report variables, as well as several handy constant variables such as ``true,'' ``false,'' ``on,'' and ``off.'' Several variables provide access to the time and date information during the course of a simulation.~ The CurrentTime, Hour and Minute variables represent the point in time at end of the timestep currently being simulated. EnergyPlus primarily operates in standard time and these clock values are not adjusted for daylight savings time.~ The built-in variable DaylightSavings time is available for use with the daylight savings time adjustment feature (see RunPeriodControl:DaylightSavingTime). The duration of simulation timesteps are available in the variables ZoneTimeStep and SystemTimeStep. The status of whether or not the simulation is currently during the initial warmup days is available in the variable WarmupFlag.
+
+Table~\ref{table:built-in-unique-variables-for-erl} lists the built-in variables that are always available for use in Erl programs.
+
+% table 2
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Built-In Unique Variables for Erl \label{table:built-in-unique-variables-for-erl}} \tabularnewline
+\toprule 
+Variable Name & Value \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Built-In Unique Variables for Erl} \tabularnewline
+\toprule 
+Variable Name & Value \tabularnewline
+\midrule
+\endhead
+
+Year & 1900–2100 \tabularnewline
+Month & 1–12 \tabularnewline
+DayOfMonth & 1–31 \tabularnewline
+DayOfWeek & 1–7 (1 = Sun, 2 = Mon, …) \tabularnewline
+DayOfYear & 1–365 \tabularnewline
+Holiday & 0 if not. 1.0, 2.0, etc., for each type of holiday in model \tabularnewline
+DaylightSavings & 0 or 1, 0 if not daylight savings time, 1 if daylight savings time \tabularnewline
+CurrentTime & 0.0-24.0, (fractional hours) \tabularnewline
+Hour & 0–23 (whole hours only) \tabularnewline
+Minute & 1.0–60.0 (fractional minutes) \tabularnewline
+True & 1.0 \tabularnewline
+False & 0.0 \tabularnewline
+On & 1.0 \tabularnewline
+Off & 0.0 \tabularnewline
+PI & 3.14159265358979 \tabularnewline
+SunIsUp & 0 (= no) or 1 (= yes) \tabularnewline
+IsRaining & 0 (= no) or 1 (= yes) \tabularnewline
+ZoneTimeStep & Durating of the zone timestep in hours \tabularnewline
+SystemTimeStep & Current duration of the system timestep in hours \tabularnewline
+CurrentEnvironment & Integer index for the current environment period (sizing periods and run periods accumulate throughout the run) \tabularnewline
+Null & Special structure that stops an actuator from overriding control \tabularnewline
+ActualDateAndTime & A simple sum of the values of the date/time function. Could be used in random seeding. \tabularnewline
+ActualTime & A simple sum of the values of the time part of the date/time function. Could be used in random seeding. \tabularnewline
+WarmupFlag & 0 (= not during warmup) or 1 (= during warmup) \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Trend Variables}\label{trend-variables}
+
+Trend variables are used to log data over time. They hold the history of Erl variables from previous zone timesteps. You create trend variables with an EnergyManagementSystem:TrendVariable input object,~ each of which declares a user-defined Erl trend variable and maps it to a global Erl variable for logging.
+
+Trend variables are also used to store the history of Erl variables. The trend input includes the number of timesteps that are to be logged. The logging of data is first-in-first-out, meaning that the oldest data are pushed out the back of the log to make room for the most recent data. The zone timestep is used as the (constant) increment of time between different elements in the log and this value, in fractional hours, is available in the ZoneTimeStep built-in variable.
+
+Trend variables differ from other Erl variables in that they can be used only through the built-in trend functions (see Table~\ref{table:built-in-functions-for-trend-variables-in-erl}). Trend functions provide a number of ways to analyze trend data and extract data from the log. There are functions to obtain the maximum, minimum, average, and sum of logged data. There is a function to obtain the rate of change in the data. All the trend functions include an argument for a log index. This index tells the function how far back in time to go when evaluating.
diff --git a/doc/ems-application-guide/src/internal-variables.tex b/doc/ems-application-guide/src/internal-variables.tex
new file mode 100644
index 00000000000..4ae009cdda0
--- /dev/null
+++ b/doc/ems-application-guide/src/internal-variables.tex
@@ -0,0 +1,5 @@
+\chapter{Internal Variables}\label{internal-variables}
+
+Internal variables form a category of built-in data accessible for EMS. They are internal in that they access information about the input file from inside EnergyPlus. You should already have access to the information contained in these because they depend on other content in the IDF. However, it would be inconvenient to always have to coordinate changes between Erl programs and the rest of the IDF. Internal variables simplify the process of keeping an Erl program in sync with other changes to the model. These differ from the built-in variables in that they may or may not be created in every simulation and have user-defined names that distinguish among different instances of the same type of data. The internal variables differ from sensors in that they are usually static values that do not change over time. The constants might vary from run to run but never within a single run period. Internal variables are read only.
+
+Internal variables are automatically made available whenever an input file includes basic EMS input objects and the model they are associated with is included in the input file. To use an internal variable in an Erl program, you must declare it with an EnergyManagementSystem:InternalVariable input object. This object assigns a specified Erl variable name to contain the value in an internal EnergyPlus data structure. The EDD file lists the specific internal variable types, their unique identifying names, and the units. The rest of this section provides information about specific internal variables.
diff --git a/doc/ems-application-guide/src/internal-variables/hvac-systems.tex b/doc/ems-application-guide/src/internal-variables/hvac-systems.tex
new file mode 100644
index 00000000000..54ac93d5e54
--- /dev/null
+++ b/doc/ems-application-guide/src/internal-variables/hvac-systems.tex
@@ -0,0 +1,75 @@
+\section{HVAC Systems}\label{hvac-systems-000}
+
+\subsection{AirTerminal:SingleDuct:Uncontrolled}\label{airterminalsingleductuncontrolled-000}
+
+An internal variable called ``AirTerminal:SingleDuct:Uncontrolled Maximum Mass Flow Rate'' provides information about the design flow rate for direct air terminals. The units are kg/s. This is the mass flow rate (for dry air at standard conditions) at the volume flow rate entered in the field Maximum Air Flow Rate (m\(^{3}\)/s) in the AirTerminal:SingleDuct:Uncontrolled input object. This internal variable is useful for scaling the flow rates assigned to the ``Mass Flow Rate'' control in the ``AirTerminal:SingleDuct:Uncontrolled'' EMS actuator.
+
+\subsection{Fan Nominal Ratings}\label{fan-nominal-ratings}
+
+\subsubsection{Fan Maximum Mass Flow Rate}\label{fan-maximum-mass-flow-rate}
+
+The input variable ``Fan Maximum Mass Flow Rate'' provides information about the maximum flow rate for a fan. The units are kg/s. This is the mass flow rate (for dry air at standard conditions) associated with the volume flow rate entered into the Maximum Air Flow Rate (m\(^{3}\)/s) in the various fan input objects. This internal variable is useful for scaling the flow rates assigned to the ``Fan Air Mass Flow Rate'' control in the ``Fan'' EMS actuator.
+
+\subsubsection{Fan Nominal Pressure Rise}\label{fan-nominal-pressure-rise}
+
+The input variable ``Fan Nominal Pressure Rise'' provides information about the static pressure rise experienced by a fan. The units are Pascals. This is the value entered into the field called Pressure Rise in the various fan input objects. This internal variable is useful for scaling the pressures assigned to the ``Fan Pressure Rise'' control in the ``Fan'' EMS actuator.
+
+\subsubsection{Fan Nominal Total Efficiency}\label{fan-nominal-total-efficiency}
+
+The input variable ``Fan Nominal Total Efficiency'' provides information about the nominal efficiency of each fan. The value is dimensionless and expressed as a fraction. This is the value entered into the field called Fan Efficiency in the various fan input objects. This internal variable is useful for scaling the value assigned to ``Fan Total Efficiency'' control in the ``Fan'' EMS actuator.
+
+\subsection{Unitary HVAC Nominal Ratings}\label{unitary-hvac-nominal-ratings}
+
+\subsubsection{Unitary HVAC Design Heating Capacity}\label{unitary-hvac-design-heating-capacity}
+
+The internal variable called ``Unitary HVAC Design Heating Capacity'' provides information about the nominal heating capacity of unitary or furnace HVAC equipment. The units are Watts. The source of these data will vary depending on the type of heating coil. This internal variable is useful for scaling the value assigned to ``Sensible Load Request'' control in the ``Unitary HVAC'' EMS actuator.
+
+\subsubsection{Unitary HVAC Design Cooling Capacity}\label{unitary-hvac-design-cooling-capacity}
+
+The internal variable called ``Unitary HVAC Design Cooling Capacity'' provides information about the nominal cooling capacity of unitary or furnace HVAC equipment. The units are Watts. The source of these data will vary depending on the type of cooling coil. This internal variable is useful for scaling the value assigned to ``Sensible Load Request'' control in the ``Unitary HVAC'' EMS actuator.
+
+\subsection{Outdoor Air Mixer Nominal Ratings}\label{outdoor-air-mixer-nominal-ratings}
+
+\subsubsection{Outdoor Air Controller Maximum Mass Flow Rate}\label{outdoor-air-controller-maximum-mass-flow-rate}
+
+The internal variable called ``Outdoor Air Controller Maximum Mass Flow Rate'' provides information about the maximum outdoor air rate for each outdoor air system. The units are kg/s. The sources of these data are inputs in the Controller:OutdoorAir input object. This internal variable is useful for scaling the value assigned to the ``Air Mass Flow Rate'' control in the ``Outdoor Air Controller'' EMS actuator.
+
+\subsubsection{Outdoor Air Controller Minimum Mass Flow Rate}\label{outdoor-air-controller-minimum-mass-flow-rate}
+
+The internal variable called ``Outdoor Air Controller Minimum Mass Flow Rate'' provides information about the minimum outdoor air rate for each outdoor air system. The units are kg/s. The sources of these data are inputs in the Controller:OutdoorAir input object. This internal variable is useful for scaling the value assigned to the ``Air Mass Flow Rate'' control in the ``Outdoor Air Controller'' EMS actuator.
+
+\subsection{Pump Nominal Ratings}\label{pump-nominal-ratings}
+
+The internal variable called ``Pump Maximum Mass Flow Rate'' provides information about the size of the pump. The units are kg/s. This is the mass flow rate associated with the volume flow rate entered into the Rated Flow Rate (m\(^{3}\)/s) in the various pump input objects. This internal variable is useful for scaling the flow rates assigned to the ``Pump Mass Flow Rate'' control in the ``Pump'' EMS actuator.
+
+\subsection{Unitary Systems}\label{unitary-systems}
+
+\subsubsection{Unitary System Control Zone Mass Flow Fraction}\label{unitary-system-control-zone-mass-flow-fraction}
+
+The internal variable called ``Unitary System Control Zone Mass Flow Fraction'' is used to adjust the zone load such that the total load met by the HVAC system, when distributed to the conditioned zones, will meet the controlling zones load. The controlling zone is the zone with the thermostat. See the AirloopHVAC:UnitarySystem input field named ``Controlling Zone or Thermostat Location.''
+
+\subsection{Low Temperature Radiant Hydronic}\label{low-temperature-radiant-hydronic-000}
+
+\subsubsection{Constant Flow Low Temp Radiant Design Water Mass Flow Rate}\label{constant-flow-low-temp-radiant-design-water-mass-flow-rate}
+
+The internal variable called ``Constant Flow Low Temp Radiant Design Water Mass Flow Rate'' provides information about the design water flow rate for radiant systems defined using a ZoneHVAC:LowTemperatureRadiant:ConstantFlow input object. The units are m\(^{3}\)/s. This internal variable is useful for scaling the flow rates assigned to the ``Water Mass Flow Rate'' control in the ``Constant Flow Low Temp Radiant'' EMS actuator.
+
+\subsubsection{Hydronic Low Temp Radiant Design Water Mass Flow Rate for Heating}\label{hydronic-low-temp-radiant-design-water-mass-flow-rate-for-heating}
+
+The internal variable called ``Hydronic Low Temp Radiant Design Water Mass Flow Rate for Heating'' provides information about the heating design water flow rate for radiant systems defined using a ZoneHVAC:LowTemperatureRadiant:VariableFlow input object. The units are m\(^{3}\)/s. This internal variable is useful for scaling the flow rates assigned to the ``Water Mass Flow Rate'' control in the ``Hydronic Low Temp Radiant'' EMS actuator.
+
+\subsubsection{Hydronic Low Temp Radiant Design Water Mass Flow Rate for Cooling}\label{hydronic-low-temp-radiant-design-water-mass-flow-rate-for-cooling}
+
+The internal variable called ``Hydronic Low Temp Radiant Design Water Mass Flow Rate for Heating'' provides information about the cooling design water flow rate for radiant systems defined using a ZoneHVAC:LowTemperatureRadiant:VariableFlow input object. The units are m\(^{3}\)/s. This internal variable is useful for scaling the flow rates assigned to the ``Water Mass Flow Rate'' control in the ``Hydronic Low Temp Radiant'' EMS actuator.
+
+\subsection{Boiler Nominal Ratings}\label{boiler-nominal-ratings}
+
+\subsubsection{Boiler Nominal Capacity}\label{boiler-nominal-capacity}
+
+The internal variable called ``Boiler Nominal Capacity'' provides information about the nominal heating capacity of boiler equipment. The units are Watts.
+
+\subsection{Chiller Nominal Ratings}\label{chiller-nominal-ratings}
+
+\subsubsection{Chiller Nominal Capacity}\label{chiller-nominal-capacity}
+
+The internal variable called ``Chiller Nominal Capacity'' provides information about the nominal cooling capacity of chiller equipment. The units are Watts.
diff --git a/doc/ems-application-guide/src/internal-variables/internal-gains.tex b/doc/ems-application-guide/src/internal-variables/internal-gains.tex
new file mode 100644
index 00000000000..3a0a6458f81
--- /dev/null
+++ b/doc/ems-application-guide/src/internal-variables/internal-gains.tex
@@ -0,0 +1,35 @@
+\section{Internal Gains}\label{internal-gains}
+
+A number of internal variables describe design levels for the various types of internal gains.
+
+\subsection{People Count Design Level}\label{people-count-design-level}
+
+The internal variable ``People Count Design Level'' provides information about the maximum number of people associated with each people input object. The units are number of people. This is the value entered in, or resulting from intermediate calculations using, the inputs in the People object. This variable is useful for scaling the values assigned to the ``Number of People'' control in the ``People'' EMS actuator.
+
+\subsection{Lighting Power Design Level}\label{lighting-power-design-level}
+
+The internal variable ``Lighting Power Design Level'' provides information about the maximum lighting electrical power level associated with each Lights input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the lights object. This variable is useful for scaling the values assigned to the ``Electric Power Level control in the ``Lights'' EMS actuator.
+
+\subsection{Plug and Process Power Design Level}\label{plug-and-process-power-design-level}
+
+The internal variable ``Plug and Process Power Design Level'' provides information about the maximum electrical equipment power level associated with each ElectricEquipment input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the ElectricEquipment object. This variable is useful for scaling the values assigned to the ``Electric Power Level'' control in the ``ElectricEquipment'' EMS actuator.
+
+\subsection{Gas Process Power Design Level}\label{gas-process-power-design-level}
+
+The internal variable ``Gas Process Power Design Level'' provides information about the maximum gas equipment power level associated with each GasEquipment input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the GasEquipment object. This variable is useful for scaling the values assigned to the ``Gas Power Level'' control in the ``GasEquipment'' EMS actuator.
+
+\subsection{Process District Heat Design Level}\label{process-district-heat-design-level}
+
+The internal variable ``Process District Heat Design Level'' provides information about the maximum district heating power level associated with each HotWaterEquipment input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the HotWaterEquipment object. This variable is useful for scaling the values assigned to the ``District Heating Power Level'' control in the ``HotWaterEquipment'' EMS actuator.
+
+\subsection{Process Steam District Heat Design Level}\label{process-steam-district-heat-design-level}
+
+The internal variable ``Process Steam District Heat Design Level'' provides information about the maximum district heating power level associated with each SteamEquipment input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the SteamEquipment object. This variable is useful for scaling the values assigned to the ``District Heating Power Level'' control in the ``SteamEquipment'' EMS actuator.
+
+\subsection{Other Equipment Design Level}\label{other-equipment-design-level}
+
+The internal variable ``Other Equipment Design Level'' provides information about the maximum power level associated with each OtherEquipment input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the OtherEquipment object. This variable is useful for scaling the values assigned to the ``Power Level'' control in the ``OtherEquipment'' EMS actuator.
+
+\subsection{Simple Zone Baseboard Capacity}\label{simple-zone-baseboard-capacity}
+
+The internal variables called ``Simple Zone Baseboard Capacity At Low Temperature'' and ``Simple Zone Baseboard Capacity At High Temperature'' provide information about the power levels associated with each ZoneBaseboard:OutdoorTemperatureControlled object. These value are inputs to that object. The variables are useful for scaling the values assigned to the ``Power Level'' control in the ``ZoneBaseboard:OutdoorTemperatureControlled'' EMS actuator.
diff --git a/doc/ems-application-guide/src/internal-variables/on-site-electricity-production.tex b/doc/ems-application-guide/src/internal-variables/on-site-electricity-production.tex
new file mode 100644
index 00000000000..46edce6e366
--- /dev/null
+++ b/doc/ems-application-guide/src/internal-variables/on-site-electricity-production.tex
@@ -0,0 +1,11 @@
+\section{On-Site Electricity Production}\label{on-site-electricity-production-000}
+
+\subsection{Generator Nominal Ratings}\label{generator-nominal-ratings}
+
+The internal variables called ``Generator Nominal Maximum Power'' and ``Generator Nominal Thermal To Electric Power'' provide information about the nominal capacity of a generator to produce electricity and heat. The values made available here are those listed in the associated ElectricLoadCenter:Generators input object. The power is expressed in Watts.
+
+The thermal-to-electric ratio describes how the nominal thermal output compares to the nominal electrical output and is useful for characterizing combined heat and power (CHP) units.
+
+\subsection{Electrical Storage}\label{electrical-storage-000}
+
+The internal variables called Electrical Storage Simple Maximum Capacity and Electrical Storage Battery Maximum Capacity provide information about the capacity of electrical storage devices. Electrical Storage Simple Maximum Capacity is the value of the field called Maximum Storage Capacity in the ElectricLoadCenter:Storage:Simple input object, the units are in Joules. Electrical Storage Battery Maximum Capacityâ is the value of the field called Maximum Module Capacity in the ElectricLoadCenter:Storage:Battery input object, the units are in amp-hours for just one battery module.
diff --git a/doc/ems-application-guide/src/internal-variables/sizing.tex b/doc/ems-application-guide/src/internal-variables/sizing.tex
new file mode 100644
index 00000000000..c1e5c917158
--- /dev/null
+++ b/doc/ems-application-guide/src/internal-variables/sizing.tex
@@ -0,0 +1,107 @@
+\section{Sizing}\label{sizing-000}
+
+Several internal variables relate to sizing calculations. Although the primary intent for the EMS is to enable custom controls for operation, using internal variables is a prime example of extending the power of user-defined calculations to control certain aspects of sizing calculations.
+
+\subsection{Sizing:Zone}\label{sizingzone-000}
+
+A series of internal variables is available related to zone sizing:
+
+\begin{itemize}
+\item
+  Final Zone Design Heating Air Mass Flow Rate (kg/s)
+\item
+  Intermediate Zone Design Heating Air Mass Flow Rate (kg/s)
+\item
+  Final Zone Design Cooling Air Mass Flow Rate (kg/s)
+\item
+  Intermediate Zone Design Cooling Air Mass Flow Rate (kg/s)
+\item
+  Final Zone Design Heating Load (W)
+\item
+  Intermediate Zone Design Heating Load (W)
+\item
+  Final Zone Design Cooling Load (W)
+\item
+  Intermediate Zone Design Cooling Load (W)
+\item
+  Final Zone Design Heating Air Density (kg/m\(^{3}\))
+\item
+  Intermediate Zone Design Heating Air Density (kg/m\(^{3}\))
+\item
+  Final Zone Design Cooling Air Density (kg/m\(^{3}\))
+\item
+  Intermediate Zone Design Cooling Air Density (kg/m\(^{3}\))
+\item
+  Final Zone Design Heating Volume Flow (m3/s)
+\item
+  Intermediate Zone Design Heating Volume Flow (m3/s)
+\item
+  Final Zone Design Cooling Volume Flow (m3/s)
+\item
+  Intermediate Zone Design Cooling Volume Flow (m3/s)
+\item
+  Zone Outdoor Air Design Volume Flow Rate (m\(^{3}\)/s)
+\end{itemize}
+
+\subsection{Sizing:System}\label{sizingsystem}
+
+A series of internal variables is available related to air system sizing:
+
+\begin{itemize}
+\item
+  Intermediate Air System Main Supply Volume Flow Rate (m\(^{3}\)/s)
+\item
+  Intermediate Air System Coincident Peak Cooling Mass Flow Rate (kg/s)
+\item
+  Intermediate Air System Coincident Peak Heating Mass Flow Rate (kg/s)
+\item
+  Intermediate Air System Noncoincident Peak Cooling Mass Flow Rate (kg/s)
+\item
+  Intermediate Air System Noncoincident Peak Heating Mass Flow Rate (kg/s)
+\item
+  Intermediate Air System Heating Volume Flow Rate (m\(^{3}\)/s)
+\item
+  Intermediate Air System Cooling Volume Flow Rate (m\(^{3}\)/s)
+\item
+  Air System Cooling Design Sensible Capacity (W)
+\item
+  Air System Heating Design Sensible Capacity (W)
+\item
+  Air System Preheating Design Sensible Capacity (W)
+\item
+  Air System Outdoor Air Design Volume Flow Rate (m\(^{3}\)/s)
+\item
+  Air System Cooling Design Mixed Air Temperature (C)
+\item
+  Air System Cooling Design Mixed Air Humidity Ratio (kgWater/kgDryAir)
+\item
+  Air System Cooling Design Return Air Temperature (C)
+\item
+  Air System Cooling Design Return Air Humidity Ratio (kgWater/kgDryAir)
+\item
+  Air System Cooling Design Outdoor Air Temperature (C)
+\item
+  Air System Cooling Design Outdoor Air Humidity Ratio (kgWater/kgDryAir)
+\item
+  Air System Heating Design Mixed Air Temperature (C)
+\item
+  Air System Heating Design Mixed Air Humidity Ratio (kgWater/kgDryAir)
+\item
+  Air System Heating Design Return Air Temperature (C)
+\item
+  Air System Heating Design Return Air Humidity Ratio (kgWater/kgDryAir)
+\item
+  Air System Heating Design Outdoor Air Temperature (C)
+\item
+  Air System Heating Design Outdoor Air Humidity Ratio (kgWater/kgDryAir)
+\end{itemize}
+
+\subsection{Sizing:Plant}\label{sizingplant}
+
+An internal variable is available for plant system sizing.
+
+\begin{itemize}
+\tightlist
+\item
+  Plant Design Volume Flow Rate (m\(^{3}\)/s)
+\end{itemize}
diff --git a/doc/ems-application-guide/src/internal-variables/zone-geometry.tex b/doc/ems-application-guide/src/internal-variables/zone-geometry.tex
new file mode 100644
index 00000000000..b65d845ee8c
--- /dev/null
+++ b/doc/ems-application-guide/src/internal-variables/zone-geometry.tex
@@ -0,0 +1,5 @@
+\section{Zone Geometry}\label{zone-geometry}
+
+The internal variables called ``Zone Air Volume'' and ``Zone Floor Area'' provide basic geometric information about each zone. EnergyPlus calculates these from the geometry in the IDF, or you may input the zone air volume in the zone input object. These internal variables in Erl programming should be useful during a parametric study where the shape of the building is being varied, as for a massing study. For example, you could use the zone floor area to normalize Erl calculations with a per-unit area. Or you could use the zone air volume to convert between air flows in m\(^{3}\)/s to air changes per hour (ACH).
+
+The internal variables called ``Zone Multiplier'' and ``Zone List Multiplier'' indicate the multipliers assigned to zones.~ These can be useful for customizing sizing calculations.
diff --git a/doc/ems-application-guide/src/user-defined-component-models.tex b/doc/ems-application-guide/src/user-defined-component-models.tex
new file mode 100644
index 00000000000..84d9182846e
--- /dev/null
+++ b/doc/ems-application-guide/src/user-defined-component-models.tex
@@ -0,0 +1,7 @@
+\chapter{User-Defined Component Models}\label{user-defined-component-models}
+
+This section provides an overview of how you can use EMS to create your own custom models for HVAC and plant equipment.~ EMS can be used not only for controls and overriding the behavior of existing models, but also to implement entirely new component models of your own formulation.~ Such user-defined component models are implemented by writing Erl programs, setting up internal variables, sensors, actuators and output variables that work in conjunction with a set of special input objects in the group called ``User Defined HVAC and Plant Component Models.''
+
+This system provides a means of modeling new types of equipment that do not yet have models implemented in EnergyPlus.~ The capability to add new custom models should have a wide variety of creative applications such as evaluating the annual energy performance implications of new types of equipment and providing a mechanism for including ``exceptional calculation methods'' in your EnergyPlus models.
+
+This section first introduces common characteristics of the user-defined component models and then goes into more detail on each of available component modeling shells that are used to connect user-defined models and algorithms to the rest of EnergyPlus' HVAC and plant simulations.
diff --git a/doc/ems-application-guide/src/user-defined-component-models/air-coil.tex b/doc/ems-application-guide/src/user-defined-component-models/air-coil.tex
new file mode 100644
index 00000000000..5b8dc347d11
--- /dev/null
+++ b/doc/ems-application-guide/src/user-defined-component-models/air-coil.tex
@@ -0,0 +1,95 @@
+\section{Air Coil}\label{air-coil}
+
+The input object called Coil:UserDefined provides a shell for creating custom models for a coil that processes air as part of an air handler.~ This device is analogous to coils models such as Coil:Cooling:Water, Coil:Heating:Water, and Coil:Cooling:DX:SingleSpeed, but can also be used for heat-exchanger-like devices such as HeatExchanger:AirToAir:SensibleAndLatent or EvaporativeCooler:Indirect:WetCoil.
+
+The user defined coil model can use one or two air connections, one optional plant connection, a water supply tank, a water collection tank, and a separate zone for skin losses.
+
+\subsection{Air Connections}\label{air-connections}
+
+Each of the two air connections that are available include both an inlet and an outlet node that are required for each air connection that is used.~ The Coil:UserDefined object appears directly on a Branch object used to define the supply side of an air handler, or in the AirLoopHVAC:OutdoorAirSystem:EquipmentList object used to define outdoor air systems.~ The following EMS internal variables are made available for each inlet node and should be useful inputs to your own custom models:
+
+\begin{itemize}
+\item
+  An internal variable called ``Inlet Temperature for Air Connection \emph{N},'' provides the current value for the drybulb air temperature at the component's inlet node, in {[}C{]}.
+\item
+  An internal variable called ``Inlet Humidity Ratio for Air Connection \emph{N},'' provides the current value for the moist air humidity ratio at the component's inlet node, in {[}kgWater/kgDryAir{]}
+\item
+  An internal variable called ``Inlet Density for Air Connection \emph{N},'' provides the current value for the density of moist air at the component's main inlet node, in {[}kg/m\(^{3}\){]}.
+\item
+  An internal variable called ``Inlet Specific Heat for Air Connection \emph{N},'' provides the current value for the specific heat of moist air at the component's main inlet node, in {[}J/kg-C{]}.
+\end{itemize}
+
+The following EMS actuators are created for each outlet node and must be used to pass results from the custom model to the rest of EnergyPlus:
+
+\begin{itemize}
+\item
+  An actuator called ``Air Connection \emph{N},'' with the control type ``Outlet Temperature,'' in {[}C{]}, needs to be used.~ This will set the drybulb temperature of the air leaving the coil.
+\item
+  An actuator called ``Air Connection \emph{N},'' with the control type ``Outlet Humidity Ratio,'' in {[}kgWater/kgDryAir{]}, needs to be used.~ This will set the humidity ratio of the air leaving the coil.
+\item
+  An actuator called ``Air Connection \emph{N},'' with the control type ``Outlet Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the flow rate of air leaving the coil.
+\end{itemize}
+
+\subsection{Plant Connections}\label{plant-connections}
+
+The user defined coil can also be connected to one plant loop to provide hydronic-based cooling, heating, or heat source or rejection.
+
+Although the coil actively conditions the air stream passing through it, from the point of view of plant it is a demand component.~ This plant connection is always ``demand'' in the sense that the coil will place loads onto the plant loop serving it and is not configured to be able to meet plant loads in the way that supply equipment could (loading mode is always DemandsLoad).~ This plant connection is always of the type that when flow is requested, the loop will be operated to try and meet the flow request and if not already running, these flow requests can turn on the loop (loop flow request mode is always NeedsFlowAndTurnsLoopOn).
+
+Both the inlet and outlet nodes need to be used is a loop is connected.~ The Coil:UserDefined object appears directly on the Branch object used to describe the plant.~ The central plant routines require that each plant component be properly initialized and registered. Special actuators are provided for these initializations and they should be filled with values by the Erl programs that are called by the program calling manager assigned to the coil for model setup and sizing.~ The following three actuators are created for the plant loop and must be used to properly register the plant connection:
+
+\begin{itemize}
+\item
+  An actuator called ``Plant Connection'' with the control type ``Minimum Mass Flow Rate,'' in {[}kg/s{]}, should be used.~ This will set the so-called hardware limit for component's minimum mass flow rate when operating.~ (If not used, then the limit will be set to zero which may be okay for many if not most models.)
+\item
+  An actuator called ``Plant Connection'' with the control type ``Maximum Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the so-called hardware limit for the component's maximum mass flow rate when operating.
+\item
+  An actuator called ``Plant Connection'' with the control type ``Design Volume Flow Rate,'' in {[}m\(^{3}\)/s{]}, needs to be used.~ This will register the size of the component for use in sizing the plant loop and supply equipment that will need to meet the loads.
+\end{itemize}
+
+When the plant loop connection is used, the following internal variables are available for inputs to the custom component model:
+
+\begin{itemize}
+\item
+  An internal variable called ``Inlet Temperature for Plant Connection'' provides the current value for the temperature of the fluid entering the component, in {[}C{]}.
+\item
+  An internal variable called ``Inlet Mass Flow Rate for Plant Connection'' provides the current value for the mass flow rate of the fluid entering the component, in {[}kg/s{]}.
+\item
+  An internal variable called ``Inlet Density for Plant Connection'' provides the current value for the density of the fluid entering the component, in {[}kg/m\(^{3}\){]}.~ This density is sensitive to the fluid type (e.g.~if using glycol in the plant loop) and fluid temperature at the inlet.
+\item
+  An internal variable called ``Inlet Specific Heat for Plant Connection'' provides the current value for the specific heat of the fluid entering the component, in {[}J/kg-C{]}. This specific heat is sensitive to the fluid type (e.g.~if using glycol in the plant loop) and fluid temperature at the inlet.
+\end{itemize}
+
+When the plant loop connection is used, the following EMS actuators are created and must be used to pass results from the custom model to the rest of EnergyPlus:
+
+\begin{itemize}
+\item
+  An actuator called ``Plant Connection'' with the control type ``Outlet Temperature,'' in {[}C{]}, needs to be used.~ This is the temperature of the fluid leaving the coil.
+\item
+  An actuator called ``Plant Connection'' with the control type ``Mass Flow Rate,'' in kg/s, needs to be used. This actuator registers the component model's request for plant fluid flow.~ The actual mass flow rate through the component may be different than requested if the overall loop situation is such that not enough flow is available to meet all the various requests.~ In general, this actuator is used to lodge a request for flow, but the more accurate flow rate will be the internal variable called ``Inlet Mass Flow Rate for Plant Connection\emph{.}''
+\end{itemize}
+
+\subsection{Water Use}\label{water-use}
+
+The user defined coil can be connected to the water use models in EnergyPlus that allow modeling on-site storage.~ If a supply inlet water storage tank is used, then an actuator called ``Water System'' with the control type ``Supplied Volume Flow Rate,'' in m\(^{3}\)/s, needs to be used.~ This sets up the coil as a demand component for that storage tank.~ If a collection outlet water storage tank is used, then an actuator called ``Water System'' with the control type ``Collected Volume Flow Rate,'' in m\(^{3}\)/s, needs to be used.
+
+\subsection{Ambient Zone}\label{ambient-zone}
+
+The user defined coil can be connected to an ambient zone and provide internal gains to that zone.~ This is for ``skin losses'' that the coil might have that result from inefficiencies and other non-ideal behavior.~ When an ambient zone is specified, the following actuators are created that can be used for different types of internal gains to the named zone:
+
+\begin{itemize}
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Sensible Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for purely convective sensible heat gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Return Air Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for purely convective sensible heat gains (or losses) to the return air duct for a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Thermal Radiation Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for thermal radiation gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Latent Heat Gain Rate,' in {[}W{]}, is available.~ This can be used for latent moisture gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Return Air Latent Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for latent moisture gains (or losses) to a the return air duct for a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Carbon Dioxide Gain Rate,'' in {[}m\(^{3}\)/s{]}, is available.~ This can be used for carbon dioxide gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Gaseous Contaminant Gain Rate,'' in {[}m\(^{3}\)/s{]}, is available.~ This can be used for generic gaseous air pollutant gains (or losses) to a zone.
+\end{itemize}
diff --git a/doc/ems-application-guide/src/user-defined-component-models/air-terminal-unit.tex b/doc/ems-application-guide/src/user-defined-component-models/air-terminal-unit.tex
new file mode 100644
index 00000000000..ce6192e770c
--- /dev/null
+++ b/doc/ems-application-guide/src/user-defined-component-models/air-terminal-unit.tex
@@ -0,0 +1,148 @@
+\section{Air Terminal Unit}\label{air-terminal-unit}
+
+The input object called AirTerminal:SingleDuct:UserDefined provides a shell for creating custom models for an air terminal that connects a multi-zone air handler to a thermal zone.~ This device is analogous to the single-duct terminal units in the Group -- Air Distribution Equipment, such as AirTerminal:SingleDuct:VAV:Reheat or AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction.
+
+In addition to the primary air connection that connects from the air loop to the zone, there are options for additional connections to a second air stream (e.g.~for outdoor ventilation or heat source or sink), up to two separate plant loop connections (e.g.~hot water and chilled water), a water supply tank, a water collection tank, and a separate zone for skin losses.
+
+The air terminal unit is a associated with a thermal zone (by the ZoneHVAC:EquipmentConnections, ZoneHVAC:EquipmentList, and ZoneHVAC:AirDistributionUnit objects).~ In EnergyPlus, when there are controlled thermal zones with thermostat (and humidistat) controls, the central routines predict the loads that zone equipment need to meet in order to maintain control of the zone conditions.~ When there are multiple types of equipment serving a zone, they are sequenced to meet heating or cooling loads in a particular order.~ Rather than the total predicted load, the second or third devices need to know the load that remains after the earlier-sequenced devices have already operated on the zone.~ The following internal variables are useful inputs for controlling zone equipment in your models:
+
+\begin{itemize}
+\item
+  An internal variable called ``Remaining Sensible Load to Heating Setpoint'' provides the current value for the sensible load, in {[}W{]}, that remains for this device that if delivered will allow the zone to reach the heating setpoint under current conditions.
+\item
+  An internal variable called ``Remaining Sensible Load to Cooling Setpoint'' provides the current value for the sensible load, in {[}W{]}, that remains for this device that if delivered will allow the zone to reach the cooling setpoint under current conditions.
+\item
+  An internal variable called ``Remaining Latent Load to Humidifying Setpoint'' provides the current value for the latent load, in {[}kg/s{]}, that remains for this device that if delivered will allow the zone to reach the humidification setpoint under current conditions.
+\item
+  An internal variable called ``Remaining Latent Load to Dehumidifying Setpoint'' provides the current value for the latent load, in {[}kg/s{]}, that remains for this device that if delivered will allow the zone to reach the dehumidification setpoint under current conditions.
+\end{itemize}
+
+\subsection{Primary Air Connection}\label{primary-air-connection}
+
+The primary air connection includes both an inlet and an outlet that are required to be used when using this component.~ This called the primary air connection because it is how the terminal unit is connected from the air handle to the zone.~ The inlet to the custom air terminal unit is a node that is also the outlet from an AirLoopHVAC:ZoneSplitter object.~ The following EMS internal variables are made available for this inlet node and should be useful inputs to your own custom models:
+
+\begin{itemize}
+\item
+  An internal variable called ``Inlet Temperature for Primary Air Connection,'' provides the current value for the drybulb air temperature at the component's inlet node, in {[}C{]}.
+\item
+  An internal variable called ``Inlet Humidity Ratio for Primary Air Connection,'' provides the current value for the moist air humidity ratio at the component's inlet node, in {[}kgWater/kgDryAir{]}
+\item
+  An internal variable called ``Inlet Density for Primary Air Connection,'' provides the current value for the density of moist air at the component's main inlet node, in {[}kg/m\(^{3}\){]}.
+\item
+  An internal variable called ``Inlet Specific Heat for Primary Air Connection,'' provides the current value for the specific heat of moist air at the component's main inlet node, in {[}J/kg-C{]}.
+\end{itemize}
+
+The inlet node also has an actuator associated with it so that the rate of air flow leaving the thermal zone and entering the unit can be passed to the rest of EnergyPlus.
+
+\begin{itemize}
+\tightlist
+\item
+  An actuator called ``Primary Air Connection,'' with the control type ``Inlet Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the flow rate of air leaving the zone splitter and entering the air terminal unit.
+\end{itemize}
+
+The primary outlet for the custom air terminal unit is a node that is also an inlet to the zone.~ The following EMS actuators are created for this outlet node and must be used to pass results from the custom model to the rest of EnergyPlus:
+
+\begin{itemize}
+\item
+  An actuator called ``Primary Air Connection,'' with the control type ``Outlet Temperature,'' in {[}C{]}, needs to be used.~ This will set the drybulb temperature of the air leaving the air terminal unit and entering the zone through the zone air inlet node.
+\item
+  An actuator called ``Primary Air Connection,'' with the control type ``Outlet Humidity Ratio,'' in {[}kgWater/kgDryAir{]}, needs to be used.~ This will set the humidity ratio of the air leaving the air terminal unit and entering the zone through the zone air inlet node.
+\item
+  An actuator called ``Primary Air Connection,'' with the control type ``Outlet Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the flow rate of air leaving the air terminal unit and entering the zone through the zone air inlet node.
+\end{itemize}
+
+It is not required that the primary air connections inlet and outlet mass flow rates be identical.~ However, if there is an imbalance, then the model should use the secondary air connection to balance air mass flows.
+
+\subsection{Secondary Air Connection}\label{secondary-air-connection}
+
+The secondary air connection provides options for an added inlet node, or outlet node, or both depending on the user's needs.~ This separate air stream can be used for outdoor air ventilation or as a source or sink for energy.~ The secondary air inlet node will often be defined to be an outdoor air node (ref. OutdoorAir:Node) but that is not required.~ The secondary air outlet node can be used as relief exhaust when the unit is providing outdoor air ventilation.~ If the secondary air outlet is not really connected to anything else and just releases air to the outdoors, then it isn't necessary that moist air properties be set using actuators because they will not impact anything else in the model.
+
+If the secondary air connection inlet node is used, then the following internal variables and actuator are made available:
+
+\begin{itemize}
+\item
+  An internal variable called ``Inlet Temperature for Secondary Air Connection,'' provides the current value for the drybulb air temperature at the secondary inlet node, in {[}C{]}.
+\item
+  An internal variable called ``Inlet Humidity Ratio for Secondary Air Connection,'' provides the current value for the moist air humidity ratio at the secondary inlet node, in {[}kgWater/kgDryAir{]}
+\item
+  An internal variable called ``Inlet Density for Secondary Air Connection,'' provides the current value for the density of moist air at the secondary inlet node, in {[}kg/m\(^{3}\){]}.
+\item
+  An internal variable called ``Inlet Specific Heat for Secondary Air Connection,'' provides the current value for the specific heat of moist air at the secondary inlet node, in {[}J/kg-C{]}.
+\item
+  An actuator called ``Secondary Air Connection,'' with the control type ``Inlet Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the flow rate of air entering the air terminal unit through the secondary air connection inlet.
+\end{itemize}
+
+If the secondary air connection outlet node is used, then the following actuators are created:
+
+\begin{itemize}
+\item
+  An actuator called ``Secondary Air Connection,'' with the control type ``Outlet Temperature,'' in {[}C{]}, needs to be used.~ This will set the drybulb temperature of the air leaving the air terminal unit through the secondary air outlet node.
+\item
+  An actuator called ``Secondary Air Connection,'' with the control type ``Outlet Humidity Ratio,'' in {[}kgWater/kgDryAir{]}, needs to be used.~ This will set the humidity ratio of the air leaving the air terminal unit through the secondary air outlet node.
+\item
+  An actuator called ``Secondary Air Connection,'' with the control type ``Outlet Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the flow rate of air leaving the air terminal unit through the secondary air outlet node.
+\end{itemize}
+
+\subsection{Plant Connections}\label{plant-connections-000}
+
+The user defined air terminal unit can also be connected to up to two different plants to provide hydronic-based cooling, heating, or heat source or rejection.
+
+Although the air terminal unit actively conditions the zone, from the point of view of plant they are demand components.~ These plant connections are always ``demand'' in the sense that the air terminal unit will place loads onto the plant loops serving it and are not configured to be able to meet plant loads in the way that supply equipment could (loading mode is always DemandsLoad).~ These plant connections are always of the type that when flow is requested, the loop will be operated to try and meet the flow request and if not already running, these flow requests can turn on the loop (loop flow request mode is always NeedsFlowAndTurnsLoopOn).
+
+For plant loops, both the inlet and outlet nodes need to be used for each loop connection.~ The AirTerminal:SingleDuct:UserDefined object appears directly on the Branch object used to describe the plant.~ The central plant routines require that each plant component be properly initialized and registered. Special actuators are provided for these initializations and they should be filled with values by the Erl programs that are called by the program calling manager assigned to the air terminal unit for model setup and sizing.~ The following three actuators are created for each of ``\emph{N}'' plant loops and must be used to properly register the plant connection:
+
+\begin{itemize}
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Minimum Mass Flow Rate,'' in {[}kg/s{]}, should be used.~ This will set the so-called hardware limit for component's minimum mass flow rate when operating.~ (If not used, then the limit will be set to zero which may be okay for many if not most models.)
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Maximum Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the so-called hardware limit for the component's maximum mass flow rate when operating.
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Design Volume Flow Rate,'' in {[}m\(^{3}\)/s{]}, needs to be used.~ This will register the size of the component for use in sizing the plant loop and supply equipment that will need to meet the loads.
+\end{itemize}
+
+For each plant loop connection that is used, the following internal variables are available for inputs to the custom component model:
+
+\begin{itemize}
+\item
+  An internal variable called ``Inlet Temperature for Plant Connection \emph{N}'' provides the current value for the temperature of the fluid entering the component, in {[}C{]}.
+\item
+  An internal variable called ``Inlet Mass Flow Rate for Plant Connection \emph{N}'' provides the current value for the mass flow rate of the fluid entering the component, in {[}kg/s{]}.
+\item
+  An internal variable called ``Inlet Density for Plant Connection \emph{N}'' provides the current value for the density of the fluid entering the component, in {[}kg/m\(^{3}\){]}.~ This density is sensitive to the fluid type (e.g.~if using glycol in the plant loop) and fluid temperature at the inlet.
+\item
+  An internal variable called ``Inlet Specific Heat for Plant Connection \emph{N}'' provides the current value for the specific heat of the fluid entering the component, in {[}J/kg-C{]}. This specific heat is sensitive to the fluid type (e.g.~if using glycol in the plant loop) and fluid temperature at the inlet.
+\end{itemize}
+
+For each plant loop connection that is used, the following EMS actuators are created and must be used to pass results from the custom model to the rest of EnergyPlus:
+
+\begin{itemize}
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Outlet Temperature,'' in {[}C{]}, needs to be used.~ This is the temperature of the fluid leaving the air terminal unit through that particular plant connection.
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Mass Flow Rate,'' in kg/s, needs to be used. This actuator registers the component model's request for plant fluid flow.~ The actual mass flow rate through the component may be different than requested if the overall loop situation is such that not enough flow is available to meet all the various requests.~ In general, this actuator is used to lodge a request for flow, but the more accurate flow rate will be the internal variable called ``Inlet Mass Flow Rate for Plant Connection \emph{N.}''
+\end{itemize}
+
+\subsection{Water Use}\label{water-use-000}
+
+The user defined air terminal unit can be connected to the water use models in EnergyPlus that allow modeling on-site storage.~ If a supply inlet water storage tank is used, then an actuator called ``Water System'' with the control type ``Supplied Volume Flow Rate,'' in m\(^{3}\)/s, needs to be used.~ This sets up the air terminal unit as a demand component for that storage tank.~ If a collection outlet water storage tank is used, then an actuator called ``Water System'' with the control type ``Collected Volume Flow Rate,'' in m\(^{3}\)/s, needs to be used.
+
+\subsection{Ambient Zone}\label{ambient-zone-000}
+
+The user defined air terminal unit can be connected to an ambient zone and provide internal gains to that zone.~ The zone can be different than the one that unit is connected to via the primary air connection if desired.~ This is for ``skin losses'' that the unit might have that result from inefficiencies and other non-ideal behavior.~ When an ambient zone is specified, the following actuators are created that can be used for different types of internal gains to the named zone:
+
+\begin{itemize}
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Sensible Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for purely convective sensible heat gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Return Air Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for purely convective sensible heat gains (or losses) to the return air duct for a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Thermal Radiation Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for thermal radiation gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Latent Heat Gain Rate,' in {[}W{]}, is available.~ This can be used for latent moisture gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Return Air Latent Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for latent moisture gains (or losses) to a the return air duct for a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Carbon Dioxide Gain Rate,'' in {[}m\(^{3}\)/s{]}, is available.~ This can be used for carbon dioxide gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Gaseous Contaminant Gain Rate,'' in {[}m\(^{3}\)/s{]}, is available.~ This can be used for generic gaseous air pollutant gains (or losses) to a zone.
+\end{itemize}
diff --git a/doc/ems-application-guide/src/user-defined-component-models/common-characteristics.tex b/doc/ems-application-guide/src/user-defined-component-models/common-characteristics.tex
new file mode 100644
index 00000000000..095113f9128
--- /dev/null
+++ b/doc/ems-application-guide/src/user-defined-component-models/common-characteristics.tex
@@ -0,0 +1,16 @@
+\section{Common Characteristics}\label{common-characteristics}
+
+In general, each of the user-defined components will:
+
+\begin{itemize}
+\item
+  Setup new EMS internal variables for the state conditions entering the component at each inlet node being used.~ Internal variables serve a similar role as Sensors in terms of obtaining input data.~ The difference is that they are updated just before the component model programs execute and therefore do not suffer the timestep lag issues that can be associated with sensors tied to output variables.~ Whereas most EMS internal variables are constants, those intended for use with user-defined components are filled each time the component is simulated and vary over time with the most current data available.
+\item
+  Setup new EMS actuators for the state conditions at each outlet node being used.~ These actuators are not optional and must be used.~ For each air or plant connection with an active outlet node, the associated actuators must be used and filled with valid values in order for the component model to be properly coupled to the rest of EnergyPlus.~ Some of the components will also set the results at their inlet node, for example to request a mass flow rate.
+\item
+  Trigger one or more specific program calling manager(s) to execute EMS programs that are called to initialize, register, and size the component model.
+\item
+  Trigger one or more specific program calling manager(s) to execute EMS programs that are called to actually model the component when it is called to be simulated.
+\end{itemize}
+
+The various user-defined components have some similar input fields.~ Once the user gains familiarity with one of the components, many of the concepts will carry over to the other user-defined components.~ The separate objects are primarily for the purpose of distinguishing how user-defined components need to vary in order to fit with the rest of EnergyPlus.
diff --git a/doc/ems-application-guide/src/user-defined-component-models/plant-component.tex b/doc/ems-application-guide/src/user-defined-component-models/plant-component.tex
new file mode 100644
index 00000000000..aa1a7e6d65e
--- /dev/null
+++ b/doc/ems-application-guide/src/user-defined-component-models/plant-component.tex
@@ -0,0 +1,133 @@
+\section{Plant Component}\label{plant-component}
+
+The input object called PlantComponent:UserDefined provides a shell for creating custom models of a device that is part of the plant models used for hydronic-type systems.~ This object can be used for primary heating or cooling devices, such as boilers or chillers.
+
+Although the other user-defined component models can also connect to plant, they are always simple ``demand'' components (from the point of view of plant modeling) and their calls to simulate are led by the air side portions of the program's calling tree.~ The plant-centric component here however, is called to simulate along with other plant components (in flow order) by plant's central routines.
+
+The user defined plant component can use up to four different plant loop connections, one optional air connection, a water supply tank, a water collection tank, and an ambient zone for skin losses.
+
+\subsection{Plant Connections}\label{plant-connections-001}
+
+The user defined plant component can be connected to up to four different plant loops.
+
+For plant loops, both the inlet and outlet nodes need to be used for each loop connection.~ The PlantComponent:UserDefined object appears directly on the Branch object used to describe the plant.~ The central plant routines require that each plant component be properly initialized and registered. Special actuators are provided for these initializations and they should be filled with values by the Erl programs that are called by the program calling manager assigned to that particular loop connection for model setup and sizing.~ The following six actuators are created for each of ``\emph{N}'' plant loops and must be used to properly register the plant connection:
+
+\begin{itemize}
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Minimum Mass Flow Rate,'' in {[}kg/s{]}, should be used.~ This will set the so-called hardware limit for component's minimum mass flow rate when operating.~ (If not used, then the limit will be set to zero which may be okay for many if not most models.)
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Maximum Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the so-called hardware limit for the component's maximum mass flow rate when operating.
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Design Volume Flow Rate,'' in {[}m\(^{3}\)/s{]}, needs to be used.~ This will register the size of the component for use in sizing the plant loop and supply equipment that will need to meet the loads.
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Minimum Loading Capacity,'' in {[}W{]}, needs to be used if the device is to be used as a supply component with load-based operation schemes.
+\item
+  An actuator called ``Plant connection \emph{N}'' with the control type ``Maximum Loading Capacity,'' in {[}W{]}, needs to be used if the device is to be used as a supply component with load-based operation schemes.
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Optimal Loading Capacity,'' in {[}W{]}, needs to be used if the device is to be used as a supply component with load-based operation schemes.
+\end{itemize}
+
+For each plant loop connection that is used, the following internal variables are available for inputs to the custom component model:
+
+\begin{itemize}
+\item
+  An internal variable called ``Inlet Temperature for Plant Connection \emph{N}'' provides the current value for the temperature of the fluid entering the component, in {[}C{]}.
+\item
+  An internal variable called ``Inlet Mass Flow Rate for Plant Connection \emph{N}'' provides the current value for the mass flow rate of the fluid entering the component, in {[}kg/s{]}.
+\item
+  An internal variable called ``Inlet Density for Plant Connection \emph{N}'' provides the current value for the density of the fluid entering the component, in {[}kg/m\(^{3}\){]}.~ This density is sensitive to the fluid type (e.g.~if using glycol in the plant loop) and fluid temperature at the inlet.
+\item
+  An internal variable called ``Inlet Specific Heat for Plant Connection \emph{N}'' provides the current value for the specific heat of the fluid entering the component, in {[}J/kg-C{]}. This specific heat is sensitive to the fluid type (e.g.~if using glycol in the plant loop) and fluid temperature at the inlet.
+\item
+  An internal variable called ``Load Request for Plant Connection N'' provides the current value for the desired operating capacity, in {[}W{]}.~ This is the input for how the model is being asked to meet the loads on the supply side.~ This is the result of the central routines for operation schemes and should be useful for controlling a plant model.~ (This internal variable is not made available when this plant connection's loading mode is set to DemandsLoad.)
+\end{itemize}
+
+For each plant loop connection that is used, the following EMS actuators are created and must be used to pass results from the custom model to the rest of EnergyPlus:
+
+\begin{itemize}
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Outlet Temperature,'' in {[}C{]}, needs to be used.~ This is the temperature of the fluid leaving the air terminal unit through that particular plant connection.
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Mass Flow Rate,'' in kg/s, needs to be used. This actuator registers the component model's request for plant fluid flow.~ The actual mass flow rate through the component may be different than requested if the overall loop situation is such that not enough flow is available to meet all the various requests.~ In general, this actuator is used to lodge a request for flow, but the more accurate flow rate will be the internal variable called ``Inlet Mass Flow Rate for Plant Connection \emph{N.}''
+\end{itemize}
+
+For each plant loop connection that is used, there is input required to specify the nature of the connection with respect to loads.~ One of the following choices must be selected depending on the purpose of the component model.
+
+\begin{itemize}
+\item
+  DemandsLoad. This type of loading is used for plant connections that place a load on the loop.~ Connections that use this loading scheme are not set up to meet loads and interact with the operation schemes.~ For example, this loading mode is appropriate for the condenser side of a chiller.
+\item
+  MeetsLoadWithPassiveCapacity.~ This type of loading is used for plant connections where the component has some capacity to meet loads but it is not really of the type that could be controlled.~ For example, a ground heat exchanger is passive because while it can provide some level of heat rejection or source, the amount will vary with current conditions and cannot usually be explicitly controlled.
+\item
+  MeetsLoadWithNominalCapacity.~ This type of loading is used for plant connections where the component has controllable capacity to meet loads and no outlet temperature restrictions.
+\item
+  MeetsLoadWithNominalCapacityLowOutLimit.~ This type of loading is used for plant connections where the component has controllable capacity to meet loads but with a lower limit on the fluid temperature at the outlet node.~ For example, this can be used for a chiller evaporator connection when the chiller is prevented from producing chilled water below a certain temperature limit.~ When this type of loading is selected, an actuator is created to allow setting the low temperature limit for use by the load dispatch routines.~ The actuator is called ``Plant Connection \emph{N}'' with the control type ``Low Outlet Temperature Limit,'' in {[}C{]}, and needs to be used.
+\item
+  MeetsLoadWithNominalCapacityHiOutLimit.~ This type of loading is used for plant connections where the component has controllable capacity to meet loads but with an upper limit on the fluid temperature at the outlet node.~ For example, this can be used for a boiler connection when the boiler is prevented from producing hot water above a certain temperature limit.~ When this type of loading is selected, an actuator is created to allow setting the high temperature limit for use by the load dispatch routines.~ The actuator is called ``Plant Connection \emph{N}'' with the control type ``High Outlet Temperature Limit,'' in {[}C{]}, and needs to be used.
+\end{itemize}
+
+For each plant loop connection, there is input required for the nature of the flow requests made by the component with respect to determining the overall flow for the loop.~ Mass flow request are also important for resolving the flow rates in parallel branches, but the mode here is related to the problem of determining the overall flow rate for the loop, not the flow down one particular branch.~ The overall loop flow rate is a function of all the flow requests made by the different devices on the loop and different types of devices have different implications for the overall loop rate.~ One of the following three choices must be made depending on the nature of the plant component.
+
+\begin{itemize}
+\item
+  NeedsFlowIfLoopOn.~ Devices with this flow request mode will contribute to the overall loop flow rate but will not initiate flow themselves.~ Other devices on the plant loop (of type NeedsFlowAndTurnsLoopOn ) need to make flow requests to get the loop flowing at all, but once it is flowing, this device can affect the overall loop flow rate.~ For example, a chiller may have a lower limit on the allowable chilled water flow rate through its evaporator and if that lower limit is higher than the current request for chilled water by the cooling coils, then the overall loop flow will be that needed by the chiller rather than the coils.
+\item
+  NeedsFlowAndTurnsLoopOn.~ Devices with this flow request mode will contribute to the overall loop flow rate and initiate flow themselves.~ This mode is used for demand component such as coils.~ Devices with this mode will initiate loops to turn on and start moving fluid.
+\item
+  ReceivesWhateverFlowAvailable.~ Devices with this flow request mode will not contribute to the overall loop flow rate and do not initiate flow themselves.~ These are essentially passive devices that take whatever flow is sent to them, such as a ground heat exchanger.
+\end{itemize}
+
+Separate program calling managers are available for each plant loop connection.~ The user defined plant component is called to simulate by the central plant routines (whereas the other user defined components are called by the central HVAC routines).~ The calls to simulate are made for each connection and you may want or need to perform different model calculations depending on which plant loop connection is being simulated at the time.~ There is an Erl program calling manager for initialization, setup, and sizing that needs to be used \emph{for each plant connection} and is only called during the early plant loop initialization phase.~ There is also an Erl program calling manager for the model calculations to perform for each plant connection.
+
+\subsection{Air Connection}\label{air-connection}
+
+An air connection is available that includes both an inlet and an outlet node.~ This can be used for air source or heat rejections. The following EMS internal variables are made available for the inlet node, if it is used, and should be useful inputs to your own custom models:
+
+\begin{itemize}
+\item
+  An internal variable called ``Inlet Temperature for Air Connection,'' provides the current value for the drybulb air temperature at the component's inlet node, in {[}C{]}.
+\item
+  An internal variable called ``Inlet Mass Flow Rate for Air Connection,'' provides the current value for the mass flow rate of air at the component's inlet node, in {[}kg/s{]}.
+\item
+  An internal variable called ``Inlet Humidity Ratio for Air Connection,'' provides the current value for the moist air humidity ratio at the component's inlet node, in {[}kgWater/kgDryAir{]}
+\item
+  An internal variable called ``Inlet Density for Air Connection,'' provides the current value for the density of moist air at the component's main inlet node, in {[}kg/m\(^{3}\){]}.
+\item
+  An internal variable called ``Inlet Specific Heat for Air Connection,'' provides the current value for the specific heat of moist air at the component's main inlet node, in {[}J/kg-C{]}.
+\end{itemize}
+
+The following EMS actuators are created for the outlet air node, if it is used, and must be used to pass results from the custom model to the rest of EnergyPlus:
+
+\begin{itemize}
+\item
+  An actuator called ``Air Connection,'' with the control type ``Outlet Temperature,'' in {[}C{]}, needs to be used.~ This will set the drybulb temperature of the air leaving the component.
+\item
+  An actuator called ``Air Connection,'' with the control type ``Outlet Humidity Ratio,'' in {[}kgWater/kgDryAir{]}, needs to be used.~ This will set the humidity ratio of the air leaving the component.
+\item
+  An actuator called ``Air Connection,'' with the control type ``Outlet Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the flow rate of air leaving the component.
+\end{itemize}
+
+\subsection{Water Use}\label{water-use-001}
+
+The user defined plant component can be connected to the water use models in EnergyPlus that allow modeling on-site storage.~ If a supply inlet water storage tank is used, then an actuator called ``Water System'' with the control type ``Supplied Volume Flow Rate,'' in m\(^{3}\)/s, needs to be used.~ This sets up the plant component as a demand component for that storage tank.~ If a collection outlet water storage tank is used, then an actuator called ``Water System'' with the control type ``Collected Volume Flow Rate,'' in m\(^{3}\)/s, needs to be used.
+
+\subsection{Ambient Zone}\label{ambient-zone-001}
+
+The user defined plant component can be connected to an ambient zone and provide internal gains to that zone.~ This is for ``skin losses'' that the component might have that result from inefficiencies and other non-ideal behavior.~ When an ambient zone is specified, the following actuators are created that can be used for different types of internal gains to the named zone:
+
+\begin{itemize}
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Sensible Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for purely convective sensible heat gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Return Air Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for purely convective sensible heat gains (or losses) to the return air duct for a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Thermal Radiation Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for thermal radiation gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Latent Heat Gain Rate,' in {[}W{]}, is available.~ This can be used for latent moisture gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Return Air Latent Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for latent moisture gains (or losses) to a the return air duct for a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Carbon Dioxide Gain Rate,'' in {[}m\(^{3}\)/s{]}, is available.~ This can be used for carbon dioxide gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Gaseous Contaminant Gain Rate,'' in {[}m\(^{3}\)/s{]}, is available.~ This can be used for generic gaseous air pollutant gains (or losses) to a zone.
+\end{itemize}
diff --git a/doc/ems-application-guide/src/user-defined-component-models/zone-forced-air-unit.tex b/doc/ems-application-guide/src/user-defined-component-models/zone-forced-air-unit.tex
new file mode 100644
index 00000000000..d8992c29046
--- /dev/null
+++ b/doc/ems-application-guide/src/user-defined-component-models/zone-forced-air-unit.tex
@@ -0,0 +1,148 @@
+\section{Zone Forced Air Unit}\label{zone-forced-air-unit}
+
+The input object called ZoneHVAC:ForcedAir:UserDefined provides a shell for creating custom models of a device that serves as a single-zone HVAC unit that operates by circulating air in and out of the zone.~ This device is analogous to those component models in the Group -- Zone Forced Air Units, such as ZoneHVAC:PackagedTerminalAirConditioner or ZoneHVAC:WaterToAirHeatPump.
+
+In addition to the primary air connection that connects to the zone, there are options for additional connections to a second air stream (e.g.~for outdoor ventilation or heat source or sink), up to three separate plant loop connections (e.g.~hot water, chilled water, heat rejection), a water supply tank, a water collection tank, and a separate zone for skin losses.
+
+The zone unit is associated with a thermal zone (by the ZoneHVAC:EquipmentConnections and ZoneHVAC:EquipmentList objects).~ In EnergyPlus, when there are controlled thermal zones with thermostat (and humidistat) controls, the central routines predict the loads that zone equipment need to meet in order to maintain control of the zone conditions.~ When there are multiple types of equipment serving a zone, they are sequenced to meet heating or cooling loads in a particular order.~ Rather than the total predicted load, the second or third devices need to know the load that remains after the earlier-sequenced devices have already operated on the zone.~ The following internal variables are useful inputs for controlling zone equipment in your models:
+
+\begin{itemize}
+\item
+  An internal variable called ``Remaining Sensible Load to Heating Setpoint'' provides the current value for the sensible load, in {[}W{]}, that remains for this device that if delivered will allow the zone to reach the heating setpoint under current conditions.
+\item
+  An internal variable called ``Remaining Sensible Load to Cooling Setpoint'' provides the current value for the sensible load, in {[}W{]}, that remains for this device that if delivered will allow the zone to reach the cooling setpoint under current conditions.
+\item
+  An internal variable called ``Remaining Latent Load to Humidifying Setpoint'' provides the current value for the latent load, in {[}kg/s{]}, that remains for this device that if delivered will allow the zone to reach the humidification setpoint under current conditions.
+\item
+  An internal variable called ``Remaining Latent Load to Dehumidifying Setpoint'' provides the current value for the latent load, in {[}kg/s{]}, that remains for this device that if delivered will allow the zone to reach the dehumidification setpoint under current conditions.
+\end{itemize}
+
+\subsection{Primary Air Connection}\label{primary-air-connection-000}
+
+The primary air connection includes both an inlet and an outlet that are required to be used when using this component.~ This is called the primary air connection because it is how the zone unit is connected to the zone.~ The inlet to the custom zone unit is a node that is also an exhaust outlet from the zone.~ The following EMS internal variables are made available for this inlet node and should be useful inputs to your own custom models:
+
+\begin{itemize}
+\item
+  An internal variable called ``Inlet Temperature for Primary Air Connection,'' provides the current value for the drybulb air temperature at the component's inlet node, in {[}C{]}.
+\item
+  An internal variable called ``Inlet Humidity Ratio for Primary Air Connection,'' provides the current value for the moist air humidity ratio at the component's inlet node, in {[}kgWater/kgDryAir{]}
+\item
+  An internal variable called ``Inlet Density for Primary Air Connection,'' provides the current value for the density of moist air at the component's main inlet node, in {[}kg/m\(^{3}\){]}.
+\item
+  An internal variable called ``Inlet Specific Heat for Primary Air Connection,'' provides the current value for the specific heat of moist air at the component's main inlet node, in {[}J/kg-C{]}.
+\end{itemize}
+
+The inlet node also has an actuator associated with it so that the rate of air flow leaving the thermal zone and entering the unit can be passed to the rest of EnergyPlus.
+
+\begin{itemize}
+\tightlist
+\item
+  An actuator called ``Primary Air Connection,'' with the control type ``Inlet Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the flow rate of air leaving the zone through the zone exhaust air node.
+\end{itemize}
+
+The primary outlet for the custom zone unit is a node that is also an inlet to the zone.~ The following EMS actuators are created for this outlet node and must be used to pass results from the custom model to the rest of EnergyPlus:
+
+\begin{itemize}
+\item
+  An actuator called ``Primary Air Connection,'' with the control type ``Outlet Temperature,'' in {[}C{]}, needs to be used.~ This will set the drybulb temperature of the air leaving the zone unit and entering the zone through the zone air inlet node.
+\item
+  An actuator called ``Primary Air Connection,'' with the control type ``Outlet Humidity Ratio,'' in {[}kgWater/kgDryAir{]}, needs to be used.~ This will set the humidity ratio of the air leaving the zone unit and entering the zone through the zone air inlet node.
+\item
+  An actuator called ``Primary Air Connection,'' with the control type ``Outlet Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the flow rate of air leaving the zone unit and entering the zone through the zone air inlet node.
+\end{itemize}
+
+It is not required that the primary air connections inlet and outlet mass flow rates be identical.~ However, if there is an imbalance, then the model should use the secondary air connection to balance air mass flows.
+
+\subsection{Secondary Air Connection}\label{secondary-air-connection-000}
+
+The secondary air connection provides options for an added inlet node, or outlet node, or both depending on the user's needs.~ This separate air stream can be used for outdoor air ventilation or as a source or sink for energy.~ The secondary air inlet node will often be defined to be an outdoor air node (ref. OutdoorAir:Node) but that is not required.~ The secondary air outlet node can be used as relief exhaust when the unit is providing outdoor air ventilation.~ If the secondary air outlet is not really connected to anything else and just releases air to the outdoors, then it isn't necessary that moist air properties be set using actuators because they will not impact anything else in the model.
+
+If the secondary air connection inlet node is used, then the following internal variables and actuator are made available:
+
+\begin{itemize}
+\item
+  An internal variable called ``Inlet Temperature for Secondary Air Connection,'' provides the current value for the drybulb air temperature at the secondary inlet node, in {[}C{]}.
+\item
+  An internal variable called ``Inlet Humidity Ratio for Secondary Air Connection,'' provides the current value for the moist air humidity ratio at the secondary inlet node, in {[}kgWater/kgDryAir{]}
+\item
+  An internal variable called ``Inlet Density for Secondary Air Connection,'' provides the current value for the density of moist air at the secondary inlet node, in {[}kg/m\(^{3}\){]}.
+\item
+  An internal variable called ``Inlet Specific Heat for Secondary Air Connection,'' provides the current value for the specific heat of moist air at the secondary inlet node, in {[}J/kg-C{]}.
+\item
+  An actuator called ``Secondary Air Connection,'' with the control type ``Inlet Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the flow rate of air entering the zone unit through the secondary air connection inlet.
+\end{itemize}
+
+If the secondary air connection outlet node is used, then the following actuators are created:
+
+\begin{itemize}
+\item
+  An actuator called ``Secondary Air Connection,'' with the control type ``Outlet Temperature,'' in {[}C{]}, needs to be used.~ This will set the drybulb temperature of the air leaving the zone unit through the secondary air outlet node.
+\item
+  An actuator called ``Secondary Air Connection,'' with the control type ``Outlet Humidity Ratio,'' in {[}kgWater/kgDryAir{]}, needs to be used.~ This will set the humidity ratio of the air leaving the zone unit through the secondary air outlet node.
+\item
+  An actuator called ``Secondary Air Connection,'' with the control type ``Outlet Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the flow rate of air leaving the zone unit through the secondary air outlet node.
+\end{itemize}
+
+\subsection{Plant Connections}\label{plant-connections-002}
+
+The user defined zone unit can also be connected to up to three different plants to provide hydronic-based cooling, heating, and/or heat source or rejection.
+
+Although the zone unit actively conditions the zone, from the point of view of plant they are demand components.~ These plant connections are always ``demand'' in the sense that the zone unit will place loads onto the plant loops serving it and are not configured to be able to meet plant loads in the way that supply equipment could (loading mode is always DemandsLoad).~ These plant connections are always of the type that when flow is requested, the loop will be operated to try and meet the flow request and if not already running, these flow requests can turn on the loop (loop flow request mode is always NeedsFlowAndTurnsLoopOn).
+
+For plant loops, both the inlet and outlet nodes need to be used for each loop connection.~ The ZoneHVAC:ForcedAir:UserDefined object appears directly on the Branch object used to describe the plant.~ The central plant routines require that each plant component be properly initialized and registered. Special actuators are provided for these initializations and they should be filled with values by the Erl programs that are called by the program calling manager assigned to the zone unit for model setup and sizing.~ The following three actuators are created for each of ``\emph{N}'' plant loops and must be used to properly register the plant connection:
+
+\begin{itemize}
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Minimum Mass Flow Rate,'' in {[}kg/s{]}, should be used.~ This will set the so-called hardware limit for component's minimum mass flow rate when operating.~ (If not used, then the limit will be set to zero which may be okay for many if not most models.)
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Maximum Mass Flow Rate,'' in {[}kg/s{]}, needs to be used.~ This will set the so-called hardware limit for the component's maximum mass flow rate when operating.
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Design Volume Flow Rate,'' in {[}m\(^{3}\)/s{]}, needs to be used.~ This will register the size of the component for use in sizing the plant loop and supply equipment that will need to meet the loads.
+\end{itemize}
+
+For each plant loop connection that is used, the following internal variables are available for inputs to the custom component model:
+
+\begin{itemize}
+\item
+  An internal variable called ``Inlet Temperature for Plant Connection \emph{N}'' provides the current value for the temperature of the fluid entering the component, in {[}C{]}.
+\item
+  An internal variable called ``Inlet Mass Flow Rate for Plant Connection \emph{N}'' provides the current value for the mass flow rate of the fluid entering the component, in {[}kg/s{]}.
+\item
+  An internal variable called ``Inlet Density for Plant Connection \emph{N}'' provides the current value for the density of the fluid entering the component, in {[}kg/m\(^{3}\){]}.~ This density is sensitive to the fluid type (e.g.~if using glycol in the plant loop) and fluid temperature at the inlet.
+\item
+  An internal variable called ``Inlet Specific Heat for Plant Connection \emph{N}'' provides the current value for the specific heat of the fluid entering the component, in {[}J/kg-C{]}. This specific heat is sensitive to the fluid type (e.g.~if using glycol in the plant loop) and fluid temperature at the inlet.
+\end{itemize}
+
+For each plant loop connection that is used, the following EMS actuators are created and must be used to pass results from the custom model to the rest of EnergyPlus:
+
+\begin{itemize}
+\item
+  An actuator called ``Plant Connection \emph{N}'' with the control type ``Outlet Temperature,'' in {[}C{]}, needs to be used.~ This is the temperature of the fluid leaving the zone unit through that particular plant connection.
+\item
+  An actuator called ``Plant Connection N'' with the control type ``Mass Flow Rate,'' in kg/s, needs to be used. This actuator registers the component model's request for plant fluid flow.~ The actual mass flow rate through the component may be different than requested if the overall loop situation is such that not enough flow is available to meet all the various requests.~ In general, this actuator is used to lodge a request for flow, but the more accurate flow rate will be the internal variable called ``Inlet Mass Flow Rate for Plant Connection \emph{N.}''
+\end{itemize}
+
+\subsection{Water Use}\label{water-use-002}
+
+The user defined zone unit can be connected to the water use models in EnergyPlus that allow modeling on-site storage.~ If a supply inlet water storage tank is used, then an actuator called ``Water System'' with the control type ``Supplied Volume Flow Rate,'' in m\(^{3}\)/s, needs to be used.~ This sets up the zone unit as a demand component for that storage tank.~ If a collection outlet water storage tank is used, then an actuator called ``Water System'' with the control type ``Collected Volume Flow Rate,'' in m\(^{3}\)/s, needs to be used.
+
+\subsection{Ambient Zone}\label{ambient-zone-002}
+
+The user defined zone unit can be connected to an ambient zone and provide internal gains to that zone.~ The zone can be different than the one that unit is connected to via the primary air connection if desired.~ This is for ``skin losses'' that the unit might have that result from inefficiencies and other non-ideal behavior.~ When an ambient zone is specified, the following actuators are created that can be used for different types of internal gains to the named zone:
+
+\begin{itemize}
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Sensible Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for purely convective sensible heat gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Return Air Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for purely convective sensible heat gains (or losses) to the return air duct for a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Thermal Radiation Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for thermal radiation gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Latent Heat Gain Rate,' in {[}W{]}, is available.~ This can be used for latent moisture gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Return Air Latent Heat Gain Rate,'' in {[}W{]}, is available.~ This can be used for latent moisture gains (or losses) to a the return air duct for a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Carbon Dioxide Gain Rate,'' in {[}m\(^{3}\)/s{]}, is available.~ This can be used for carbon dioxide gains (or losses) to a zone.
+\item
+  An actuator called ``Component Zone Internal Gain'' with the control type ``Gaseous Contaminant Gain Rate,'' in {[}m\(^{3}\)/s{]}, is available.~ This can be used for generic gaseous air pollutant gains (or losses) to a zone.
+\end{itemize}
diff --git a/doc/engineering-reference/CMakeLists.txt b/doc/engineering-reference/CMakeLists.txt
new file mode 100644
index 00000000000..ba2207de1db
--- /dev/null
+++ b/doc/engineering-reference/CMakeLists.txt
@@ -0,0 +1,533 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+#  grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's/^/  /g' | sed 's/$/.tex/g'
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/engineering-reference.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/title.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/overview.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/overview/document-overview.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/overview/general-modeling-overview.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/overview/simulation-manager.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/overview/warmup-convergence.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/integrated-solution-manager.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/integrated-solution-manager/basis-for-the-zone-and-air-system-integration.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/integrated-solution-manager/summary-of-predictor-corrector-procedure.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/integrated-solution-manager/air-system-control.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/integrated-solution-manager/moisture-predictor-corrector.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/integrated-solution-manager/carbon-dioxide-predictor-corrector.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/integrated-solution-manager/generic-contaminant-predictor-corrector.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/integrated-solution-manager/zone-air-mass-flow-conservation.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/integrated-solution-manager/summary-of-time-marching-solution.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/surface-heat-balance-manager-processes.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/surface-heat-balance-manager-processes/conduction-through-the-walls.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/surface-heat-balance-manager-processes/conduction-finite-difference-solution.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/surface-heat-balance-manager-processes/inside-heat-balance.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/surface-heat-balance-manager-processes/infrared-radiation-transfer-material.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/surface-heat-balance-manager-processes/surface-heat-balance-with-moveable-insulation.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-c.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-site.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/daylighting-and-window-calculations/daylight-factor-calculation.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/daylighting-and-window-calculations/complex-fenestration-daylighting-calculations.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/daylighting-and-window-calculations/daylighting-devices.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/daylighting-and-window-calculations/window-calculation-module.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/air-heat-balance-manager-processes/convection-from-surfaces.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/air-heat-balance-manager-processes/convection-from-internal-sources.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/air-heat-balance-manager-processes/infiltration-ventilation.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/building-system-simulation-system-manager/air-path-components.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/building-system-simulation-system-manager/plant-load-profile.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/building-system-simulation-system-manager/plant-condenser-loops.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/sizing-manager.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/hvac-sizing-simulation-manager.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/zone-design-loads-and-air-flow-rates.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/system-design-loads-and-air-flow-rates.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/plant-loop-sizing.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/coincident-plant-sizing-using-hvac-sizing.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/demand-limiting.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/alternative-modeling-processes.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/alternative-modeling-processes/airflownetwork-model.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/engineering-reference-encyclopedia.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference/air-system-distribution-terminals.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference/boilers.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference/chillers.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/ice-thermal-storage.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/coils.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/hvac-controllers.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/baseboard-heaters.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/electric-baseboard-heater-with-radiation.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/cooling-towers-and-evaporative-fluid-coolers.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/demand-controlled-ventilation.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-fans.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-compound-component-groups.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/variable-refrigerant-flow-heat-pumps.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/heat-exchangers.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-humidifiers.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/zone-internal-gains.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/indoor-swimming-pool.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/pipes.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/pumps.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/ideal-loads-air-system.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/district-cooling.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/district-heating.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/centralheatpumpsystem.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/chillerheaterperformance-electric-eir.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/plant-temperature-source-component.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/radiant-system-models.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/refrigeration-equipment.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/setpoint-managers.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/solar-collectors.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/system-availability-managers.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/on-site-generation/generators.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/performance-curves-and-lookup-tables/performance-curves.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/performance-curves-and-lookup-tables/performance-tables.tex
+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/economics-calculations.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/economics-calculations/life-cycle-cost-computations.tex
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+  ${CMAKE_SOURCE_DIR}/doc/engineering-reference/src/special-modules-reporting/output-table-annual.tex
+  ${CMAKE_SOURCE_DIR}/doc/title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
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+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/engineering-reference/engineering-reference.tex b/doc/engineering-reference/engineering-reference.tex
new file mode 100644
index 00000000000..cf8df86d212
--- /dev/null
+++ b/doc/engineering-reference/engineering-reference.tex
@@ -0,0 +1,293 @@
+\input{../header}
+
+\title{Engineering Reference}
+
+\hypersetup{unicode=true,
+            pdftitle={Engineering Reference},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+\input{src/title}
+
+\input{src/overview}
+
+\input{src/overview/document-overview}
+
+\input{src/overview/general-modeling-overview}
+
+\input{src/overview/simulation-manager}
+
+\input{src/overview/warmup-convergence}
+
+\input{src/integrated-solution-manager}
+
+\input{src/integrated-solution-manager/basis-for-the-zone-and-air-system-integration}
+
+\input{src/integrated-solution-manager/summary-of-predictor-corrector-procedure}
+
+\input{src/integrated-solution-manager/air-system-control}
+
+\input{src/integrated-solution-manager/moisture-predictor-corrector}
+
+\input{src/integrated-solution-manager/carbon-dioxide-predictor-corrector}
+
+\input{src/integrated-solution-manager/generic-contaminant-predictor-corrector}
+
+\input{src/integrated-solution-manager/zone-air-mass-flow-conservation}
+
+\input{src/integrated-solution-manager/summary-of-time-marching-solution}
+
+\input{src/surface-heat-balance-manager-processes}
+
+\input{src/surface-heat-balance-manager-processes/conduction-through-the-walls}
+
+\input{src/surface-heat-balance-manager-processes/conduction-finite-difference-solution}
+
+\input{src/surface-heat-balance-manager-processes/combined-heat-and-moisture-transfer-hamt}
+
+\input{src/surface-heat-balance-manager-processes/effective-moisture-penetration-depth-empd}
+
+\input{src/surface-heat-balance-manager-processes/outside-surface-heat-balance}
+
+\input{src/surface-heat-balance-manager-processes/inside-heat-balance}
+
+\input{src/surface-heat-balance-manager-processes/adiabatic-boundary-conditions}
+
+\input{src/surface-heat-balance-manager-processes/infrared-radiation-transfer-material}
+
+\input{src/surface-heat-balance-manager-processes/transparent-insulation-material}
+
+\input{src/surface-heat-balance-manager-processes/surface-heat-balance-with-moveable-insulation}
+
+\input{src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-c}
+
+\input{src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-site}
+
+\input{src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-site-001}
+
+\input{src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-finite}
+
+\input{src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-kusuda}
+
+\input{src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-xing}
+
+\input{src/surface-heat-balance-manager-processes/exterior-naturally-vented-cavity}
+
+\input{src/surface-heat-balance-manager-processes/green-roof-model-ecoroof}
+
+\input{src/climate-sky-and-solar-shading-calculations}
+
+\input{src/climate-sky-and-solar-shading-calculations/climate-calculations}
+
+\input{src/climate-sky-and-solar-shading-calculations/design-week-specification}
+
+\input{src/climate-sky-and-solar-shading-calculations/sky-radiance-model}
+
+\input{src/climate-sky-and-solar-shading-calculations/shading-module}
+
+\input{src/solar-radiation-reflected-from-exterior}
+
+\input{src/solar-radiation-reflected-from-exterior/diffuse-reflection-of-beam-solar-and-sky}
+
+\input{src/daylighting-and-window-calculations}
+
+\input{src/daylighting-and-window-calculations/daylighting-calculations}
+
+\input{src/daylighting-and-window-calculations/daylight-factor-calculation}
+
+\input{src/daylighting-and-window-calculations/time-step-daylighting-calculation}
+
+\input{src/daylighting-and-window-calculations/delight-daylighting-calculations}
+
+\input{src/daylighting-and-window-calculations/complex-fenestration-daylighting-calculations}
+
+\input{src/daylighting-and-window-calculations/daylighting-devices}
+
+\input{src/daylighting-and-window-calculations/window-calculation-module}
+
+\input{src/daylighting-and-window-calculations/window-heat-balance-calculation}
+
+\input{src/air-heat-balance-manager-processes}
+
+\input{src/air-heat-balance-manager-processes/convection-from-surfaces}
+
+\input{src/air-heat-balance-manager-processes/convection-from-internal-sources}
+
+\input{src/air-heat-balance-manager-processes/infiltration-ventilation}
+
+\input{src/air-heat-balance-manager-processes/air-exchange}
+
+\input{src/air-heat-balance-manager-processes/calculation-of-zone-air-temperature}
+
+\input{src/building-system-simulation-system-manager}
+
+\input{src/building-system-simulation-system-manager/air-loops}
+
+\input{src/building-system-simulation-system-manager/air-loop-simulation}
+
+\input{src/building-system-simulation-system-manager/primary-air-system-simulation}
+
+\input{src/building-system-simulation-system-manager/outdoor-air-system}
+
+\input{src/building-system-simulation-system-manager/outdoor-air-mixer}
+
+\input{src/building-system-simulation-system-manager/zone-equipment-simulation}
+
+\input{src/building-system-simulation-system-manager/air-path-components}
+
+\input{src/building-system-simulation-system-manager/plant-load-profile}
+
+\input{src/building-system-simulation-system-manager/plant-condenser-loops}
+
+\input{src/building-system-simulation-system-manager/steam-systems-and-component-models}
+
+\input{src/loop-equipment-sizing-and-other-design-data}
+
+\input{src/loop-equipment-sizing-and-other-design-data/sizing-manager}
+
+\input{src/loop-equipment-sizing-and-other-design-data/hvac-sizing-simulation-manager}
+
+\input{src/loop-equipment-sizing-and-other-design-data/zone-design-loads-and-air-flow-rates}
+
+\input{src/loop-equipment-sizing-and-other-design-data/system-design-loads-and-air-flow-rates}
+
+\input{src/loop-equipment-sizing-and-other-design-data/plant-loop-sizing}
+
+\input{src/loop-equipment-sizing-and-other-design-data/coincident-plant-sizing-using-hvac-sizing}
+
+\input{src/loop-equipment-sizing-and-other-design-data/component-sizing}
+
+\input{src/loop-equipment-sizing-and-other-design-data/zone-outdoor-air-design-data}
+
+\input{src/operational-faults}
+
+\input{src/demand-limiting}
+
+\input{src/alternative-modeling-processes}
+
+\input{src/alternative-modeling-processes/airflownetwork-model}
+
+\input{src/engineering-reference-encyclopedia}
+
+\input{src/simulation-models-encyclopedic-reference}
+
+\input{src/simulation-models-encyclopedic-reference/air-system-distribution-terminals}
+
+\input{src/simulation-models-encyclopedic-reference/boilers}
+
+\input{src/simulation-models-encyclopedic-reference/chillers}
+
+\input{src/simulation-models-encyclopedic-reference-001}
+
+\input{src/simulation-models-encyclopedic-reference-001/ice-thermal-storage}
+
+\input{src/simulation-models-encyclopedic-reference-001/coils}
+
+\input{src/simulation-models-encyclopedic-reference-001/hvac-controllers}
+
+\input{src/simulation-models-encyclopedic-reference-001/baseboard-heaters}
+
+\input{src/simulation-models-encyclopedic-reference-001/electric-baseboard-heater-with-radiation}
+
+\input{src/simulation-models-encyclopedic-reference-001/cooling-towers-and-evaporative-fluid-coolers}
+
+\input{src/simulation-models-encyclopedic-reference-001/demand-controlled-ventilation}
+
+\input{src/simulation-models-encyclopedic-reference-001/evaporative-coolers}
+
+\input{src/simulation-models-encyclopedic-reference-001/air-system-fans}
+
+\input{src/simulation-models-encyclopedic-reference-001/air-system-compound-component-groups}
+
+\input{src/simulation-models-encyclopedic-reference-001/variable-refrigerant-flow-heat-pumps}
+
+\input{src/simulation-models-encyclopedic-reference-001/heat-exchangers}
+
+\input{src/simulation-models-encyclopedic-reference-001/air-system-humidifiers}
+
+\input{src/simulation-models-encyclopedic-reference-001/zone-internal-gains}
+
+\input{src/simulation-models-encyclopedic-reference-001/indoor-swimming-pool}
+
+\input{src/simulation-models-encyclopedic-reference-001/pipes}
+
+\input{src/simulation-models-encyclopedic-reference-001/pumps}
+
+\input{src/simulation-models-encyclopedic-reference-001/ideal-loads-air-system}
+
+\input{src/simulation-models-encyclopedic-reference-001/district-cooling}
+
+\input{src/simulation-models-encyclopedic-reference-001/district-heating}
+
+\input{src/simulation-models-encyclopedic-reference-001/centralheatpumpsystem}
+
+\input{src/simulation-models-encyclopedic-reference-001/chillerheaterperformance-electric-eir}
+
+\input{src/simulation-models-encyclopedic-reference-001/plant-temperature-source-component}
+
+\input{src/simulation-models-encyclopedic-reference-002}
+
+\input{src/simulation-models-encyclopedic-reference-002/radiant-system-models}
+
+\input{src/simulation-models-encyclopedic-reference-002/refrigeration-equipment}
+
+\input{src/simulation-models-encyclopedic-reference-002/setpoint-managers}
+
+\input{src/simulation-models-encyclopedic-reference-002/solar-collectors}
+
+\input{src/simulation-models-encyclopedic-reference-002/system-availability-managers}
+
+\input{src/simulation-models-encyclopedic-reference-003}
+
+\input{src/simulation-models-encyclopedic-reference-003/occupant-thermal-comfort}
+
+\input{src/simulation-models-encyclopedic-reference-003/trombe-walls}
+
+\input{src/simulation-models-encyclopedic-reference-003/water-thermal-tanks-includes-water-heaters}
+
+\input{src/simulation-models-encyclopedic-reference-003/water-systems}
+
+\input{src/simulation-models-encyclopedic-reference-003/zone-controls}
+
+\input{src/simulation-models-encyclopedic-reference-003/zone-equipment-and-zone-forced-air-units}
+
+\input{src/on-site-generation}
+
+\input{src/on-site-generation/whole-facility-electric-service}
+
+\input{src/on-site-generation/electric-load-center-distribution-manager}
+
+\input{src/on-site-generation/photovoltaic-arrays}
+
+\input{src/on-site-generation/generators}
+
+\input{src/performance-curves-and-lookup-tables}
+
+\input{src/performance-curves-and-lookup-tables/performance-curves}
+
+\input{src/performance-curves-and-lookup-tables/performance-tables}
+
+\input{src/economics-calculations}
+
+\input{src/economics-calculations/component-costs}
+
+\input{src/economics-calculations/tariff-computation}
+
+\input{src/economics-calculations/life-cycle-cost-computations}
+
+\input{src/special-modules-reporting}
+
+\input{src/special-modules-reporting/environmental-impacts}
+
+\input{src/special-modules-reporting/zone-component-loads-summary}
+
+\input{src/special-modules-reporting/output-table-annual}
+
+\end{document}
diff --git a/doc/src/docs/EngineeringReference/media/ACBussDiagram.png b/doc/engineering-reference/media/ACBussDiagram.png
similarity index 100%
rename from doc/src/docs/EngineeringReference/media/ACBussDiagram.png
rename to doc/engineering-reference/media/ACBussDiagram.png
diff --git a/doc/src/docs/EngineeringReference/media/ACStorageBussDiagram.png b/doc/engineering-reference/media/ACStorageBussDiagram.png
similarity index 100%
rename from doc/src/docs/EngineeringReference/media/ACStorageBussDiagram.png
rename to doc/engineering-reference/media/ACStorageBussDiagram.png
diff --git a/doc/src/docs/EngineeringReference/media/DCInverterBussDiagram.png b/doc/engineering-reference/media/DCInverterBussDiagram.png
similarity index 100%
rename from doc/src/docs/EngineeringReference/media/DCInverterBussDiagram.png
rename to doc/engineering-reference/media/DCInverterBussDiagram.png
diff --git a/doc/src/docs/EngineeringReference/media/DCInverterWithACStorageBussDiagram.png b/doc/engineering-reference/media/DCInverterWithACStorageBussDiagram.png
similarity index 100%
rename from doc/src/docs/EngineeringReference/media/DCInverterWithACStorageBussDiagram.png
rename to doc/engineering-reference/media/DCInverterWithACStorageBussDiagram.png
diff --git a/doc/src/docs/EngineeringReference/media/DCInverterWithDCStorageBussDiagram.png b/doc/engineering-reference/media/DCInverterWithDCStorageBussDiagram.png
similarity index 100%
rename from doc/src/docs/EngineeringReference/media/DCInverterWithDCStorageBussDiagram.png
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diff --git a/doc/src/docs/EngineeringReference/media/SZVAV_Fan_Control_FanCoil.jpg b/doc/engineering-reference/media/SZVAV_Fan_Control_FanCoil.jpg
similarity index 100%
rename from doc/src/docs/EngineeringReference/media/SZVAV_Fan_Control_FanCoil.jpg
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diff --git a/doc/src/docs/EngineeringReference/media/SetPointManager-ResetForReturnControl1.png b/doc/engineering-reference/media/SetPointManager-ResetForReturnControl1.png
similarity index 100%
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diff --git a/doc/src/docs/EngineeringReference/media/SetPointManager-ResetForReturnControl2.png b/doc/engineering-reference/media/SetPointManager-ResetForReturnControl2.png
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diff --git a/doc/src/docs/EngineeringReference/media/SetPointManager-ResetForReturnControl3.png b/doc/engineering-reference/media/SetPointManager-ResetForReturnControl3.png
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diff --git a/doc/src/docs/EngineeringReference/media/StorageOperationControlVolume.png b/doc/engineering-reference/media/StorageOperationControlVolume.png
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diff --git a/doc/src/docs/EngineeringReference/media/TroxDID632A_Tabledata.png b/doc/engineering-reference/media/TroxDID632A_Tabledata.png
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diff --git a/doc/engineering-reference/src/air-heat-balance-manager-processes.tex b/doc/engineering-reference/src/air-heat-balance-manager-processes.tex
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index 00000000000..9c650a0e8cf
--- /dev/null
+++ b/doc/engineering-reference/src/air-heat-balance-manager-processes.tex
@@ -0,0 +1 @@
+\chapter{Air Heat Balance Manager / Processes}\label{air-heat-balance-manager-processes}
diff --git a/doc/engineering-reference/src/air-heat-balance-manager-processes/air-exchange.tex b/doc/engineering-reference/src/air-heat-balance-manager-processes/air-exchange.tex
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index 00000000000..b79f6fde20f
--- /dev/null
+++ b/doc/engineering-reference/src/air-heat-balance-manager-processes/air-exchange.tex
@@ -0,0 +1,138 @@
+\section{Air Exchange}\label{air-exchange}
+
+Air exchange and interchange between zones is treated as a convective gain. Temperature-difference-controlled or constant air mixing can be specified as a one-way or cross-zone phenomenon modeled using the ZoneMixing or ZoneCrossMixing objects. Air exchange through doorways between refrigerated spaces can be modeled using the ZoneRefrigerationMixing object.
+
+For one-way mixing (using ZoneMixing object(s)), the mixing air flow is only used for the energy and mass balance for the receiving zone. The mass referred in this section includes air, water vapor and CO\(_{2}\). The source zone energy and mass balance are not effected, although the user may choose to enter complementary pairs of one-way mixing objects. Multiple mixing flows can be defined for any receiving zone. For cross-zone mixing (using ZoneCrossMixing object(s)), the mixing air flow impacts the mass and energy balances in both the source and receiving zones. No more than one ZoneCrossMixing object can be used for any receiving zone. A separate ZoneCrossMixing object must be used for each of the two zones exchanging air if the mixing flow is bi-directional and based on a temperature difference greater than zero.
+
+For refrigerated space air exchange (using ZoneRefrigerationDoorMixing object(s)), the mixing air flow impacts the mass and energy balances in both the source and receiving zones. A single object accounts for the two-way air flow with the energy and mass exchanges determined by~ the air density difference between the two zones.
+
+\subsection{Temperature Difference Controlled Air Exchange}\label{temperature-difference-controlled-air-exchange}
+
+The volume of air flow into the receiving zone is specified by the user with a number of control parameters and schedules listed in the Input Output Guide. The user can turn this one-way flow on or off based on the temperature difference between the source and receiving zones, or it may be independent of the temperature difference. The density and specific heat of the air flowing into the receiving zone are determined using the average temperature and average humidity ratio in the source and receiving zones. The humidity ratio of the air flowing into the receiving zone is set equal to the humidity ratio of the source zone. The mass, moisture,and energy terms are then used as described in two previous sections, Basis for the Zone and Air System Integration, and Moisture Predictor-Corrector.
+
+\begin{equation}
+ \begin{array}{cl}
+    \rho_{Avg} & = f \left( \frac{T_{ReceivingZone} + T_{SourceZone}}{2},\frac{W_{ReceivingZone} + W_{SourceZone}}{2},P_{Barometric} \right) \\
+    c_{P,Avg} & = f \left( \frac{T_{ReceivingZone} + T_{SourceZone}}{2},\frac{W_{ReceivingZone} + W_{SourceZone}}{2}\right) \\
+    \dot m_{MixingFlowToReceivingZone} & = \sum_{AllSourceZones} \rho_{Avg}\dot V_{Air} \\
+    \dot Q_{MixingFlowToReceivingZone} & = \sum_{AllSourceZones} \rho_{Avg}C_{p,Avg}\dot V_{Air}\left(T_{sourceZone}-T_{receivingZone}\right) \\
+    \text{Moisture}_{MixingFlowToReceivingZone} & = \sum_{AllSourceZones} \rho_{Avg} \dot V_{Air} W_{SourceZone}
+  \end{array}
+\end{equation}
+
+where:
+
+c\(_{P,Avg}\)~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ = Average specific heat of air within the two zones (J/kg.K)
+
+\({\dot m_{{\rm{MixingFlowToReceivingZone}}}}\) ~~~~~~~~~ = Mass of moist air flowing into the receiving zone (kg\(_{air}\)/s)
+
+Moisture\(_{MixingFlowToReceivingZone}\)~~~ = Moisture mass flow rate into the receiving zone (kg\(_{H2O}\)/s)
+
+P\(_{Barometric}\)~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ = Outside barometric pressure (Pa)
+
+�\(_{Avg}\) = Average density of air within the two zones (kg/s)
+
+\({\dot Q_{{\rm{MixingFlowToReceivingZone}}}}\) ~~~~~~~~~ = Energy added to receiving zone air by mixing mass flow (W)
+
+T\(_{ReceivingZone}\) = Temperature in the Receiving Zone (\(^{o}\)C)
+
+T\(_{SourceZone}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ = Temperature in the Source Zone (\(^{o}\)C)
+
+\({\dot V_{Air}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ = Volume rate of air flow defined by the user (m\(^{3}\)/s)
+
+W\(_{ReceivingZone}\) ~~~~~~~~~~~~ = Humidity Ratio in the Receiving Zone (kg\(_{H2O}\)/kg\(_{dry\\ air}\))
+
+W\(_{SourceZone}\)~~~~~~~~~~~~~~~~~~~~~~~~~~~~ = Humidity Ratio in the Source Zone (kg\(_{H2O}\)/kg\(_{dry\\ air}\))
+
+For cross-mixing, the mass of moist air exchanged between the two zones is assumed to be equal.~ Again, the density and specific heat are based on the average conditions in the two zones. Note that the temperature and humidity ratio differences ensure that when the energy and~ moisture terms are used in the Moisture Predictor-Corrector, they correctly reflect a loss or gain in each zone.
+
+\begin{equation}
+  \begin{array}{cl}
+    \dot{m}_{MixingFlowToReceivingZone} & = \dot{m}_{MixingFlowToSourceZone} = \rho_{Avg}\dot{V}_{Air} \\
+    \dot{Q}_{MixingFlowToSourceZone}    & = \rho_{Avg} C_{p,Avg} \dot{V}_{Air} \left( T_{ReceivingZone}-T_{SourceZone} \right) \\
+    \dot{Q}_{MixingFlowToReceivingZone} & = \rho_{Avg} C_{p,Avg} \dot{V}_{Air} \left( T_{SourceZone} - T_{ReceivingZone} \right) \\
+    \text{Moisture}_{MixingFlowToSourceZone} & = \rho_{Avg} \dot{V}_{Air} W_{ReceivingZone} \\
+    \text{Moisture}_{MixingFlowToReceivingZone} & = \rho_{Avg} \dot{V}_{Air} W_{SourceZone}
+  \end{array}
+\end{equation}
+
+where:
+
+\({\dot m_{{\rm{MixingFlowToSourceZone}}}}\) ~~~~~~~~~~~ = Mass of moist air flowing into the source zone (kg\(_{air}\)/s)
+
+Moisture\(_{MixingFlowToSourceZone}\)~~~~~~ = Moisture mass flow rate into the source zone (kg\(_{H2O}\)/s)
+
+\({\dot Q_{{\rm{MixingFlowToSourceZone}}}}\) ~~~~~~~~~~~~ = Sensible energy added to source zone air by mixing mass flow (W)
+
+\({\dot Q_{{\rm{MixingFlowToReceivingZone}}}}\) ~~~~~~~~~ = Sensible energy added to receiving zone air by mixing mass flow, W
+
+\(Moistur{e_{{\rm{MixingFlowToSourceZone}}}}\) = Latent load added to source zone air by mixing mass flow (kg\(_{H2O}\)/s)
+
+\(Moistur{e_{{\rm{MixingFlowToReceivingZone}}}}\) = Latent load added to receiving zone air by mixing mass flow (kg\(_{H2O}\)/s)
+
+\subsection{Density Difference Controlled Air Exchange}\label{density-difference-controlled-air-exchange}
+
+When closed refrigerated spaces exchange air with other closed spaces, the air flow is determined by the difference in air density between the two spaces. The fundamental assumption for this case is that the mass of dry air exchanged between the two spaces is the same.(Gosney and Olama, ~1975{]} This assumption applies to situations where the colder of the two spaces is essentially sealed to other air flows, that is, there are no open doors or exhaust air flows. Multiple refrigeration door mixing objects can be used for the zone, but if there are multiple doors open at the same time for any significant amount of time, the model will not give results appropriate for that condition.
+
+The sensible and latent energy loads are modeled according to the guidance specified in (ASHRAE 2006d, ASHRAE 2009, and Gosney and Olama, 1975).~ Equal dry air exchange is assumed, that is, the mass of dry air infiltrating into the receiving zone is assumed to equal the mass of dry air infiltrating out of the source zone.
+
+\begin{equation}
+  \begin{array}{cl}
+    h_{zoneA},\rho_{zoneA} & = f (T_{zoneA},W_{zoneA},P_{Barometric}) \\
+    h_{zoneB},\rho_{zoneB} & = f (T_{zoneB},W_{zoneB},P_{Barometric}) \\
+    \rho_{zoneA} & > \rho_{zoneB} \\
+    \dot{Q}_{Mixing} & = \dot{Q}_{FullFlow} \times \text{Schedule}_{DoorOpen} \times F_{Flow} \times (1-F_{Protection}) \\
+    \dot{Q}_{FullFlow} & = B (h_{zoneB}-h_{zoneA}) \\
+    B & = 0.221 A_{door} \rho_{zoneA} F_{Density} \sqrt{ \left(1-\frac{\rho_{zoneB}}{\rho_{zoneA}}\right) g H_{Door} } \\
+    F_{Density} & = \left[ \frac{2}{1+\left(\rho_{zoneA}/\rho_{zoneB}\right)^{1/3}} \right]^{1.5} \\
+    \dot{m}_{DryAirZonesAB} & = \frac{\dot{Q}_{Mixing}}{h_{zoneB}-h_{zoneA}} \\
+    \dot{m}_{MixingFlowZoneBtoA} & = \sum_{AllZoneBs} \dot{m}_{DryAirZonesAB}\left(1+W_{ZoneB}\right) \\
+    \dot{Q}_{MixingFlowZoneBtoA} & = \sum_{AllZoneBs} \dot{m}_{ZoneBtoA} C_{p,ZoneB} \left(T_{zoneB}-T_{zoneA}\right) \\
+    \text{Moisture}_{MixingFlowZoneBtoA} & = \sum_{AllZoneBs} \dot{m}_{ZoneBtoA} \left( W_{zoneB}-W_{zoneA} \right) \\
+    \dot{m}_{MixingFlowZoneAtoB} & = \sum_{AllZoneAs} \dot{m}_{DryAirZonesAB}\left(1+W_{ZoneA}\right) \\
+    \dot{Q}_{MixingFlowZoneAtoB} & = \sum_{AllZoneAs} \dot{m}_{ZoneBtoA} C_{p,ZoneA} \left(T_{zoneA}-T_{zoneB}\right) \\
+    \text{Moisture}_{MixingFlowZoneAtoB} & = \sum_{AllZoneAs} \dot{m}_{ZoneBtoA} \left( W_{zoneA}-W_{zoneB} \right) 
+  \end{array}
+\end{equation}
+
+where:
+
+A\(_{door}\)~~~~~~~~~~~ = ~ Area of door between Zones A and B (m\(^{2}\))
+
+F\(_{Flow}\) ~~~~~~~~~~ = ~Doorway flow factor, = 0.8 if ΔT \textgreater{} 11\(^{o}\)C; = 1.1 if ΔT \textless{} = 11\(^{o}\)C
+
+F\(_{Protection}\) ~~~~~~ = Doorway protection factor, = 0 for no protection; = ~ 0.5 for an air curtain; and 0.9 for a strip curtain (dimensionless)
+
+g~~~~~~~~~~~~~~~ = ~ Gravitational constant (m/s\(^{2}\))
+
+h\(_{ZoneA}\) = ~ enthalpy of the air within Zone A (J/kg)
+
+h\(_{ZoneB}\) = ~ enthalpy of the air within Zone B (J/kg)
+
+H\(_{door}\)~~~~~~~~~~~ = ~ Height of door between source and receiving zones (m)
+
+Q\(_{FullFlow}\) ~~~~~~ = Sensible and latent refrigeration load (on Zone A) for fully established flow (W)
+
+Q\(_{Mixing}\) ~~~~~~~~ = Sensible and latent mixing refrigeration load on Zone A for the time step (W)
+
+m\(_{DryAirZoneAB}\) ~ = Mass of dry air exchanged between zones A and B (kg\(_{air}\)/s)
+
+Schedule\(_{DoorOpen}\) ~~~~~~ = Value scheduled by user, fraction of time door open during time step (dimensionless)
+
+W\(_{ZoneA}\) = ~ Humidity ratio of the air within Zone A (kg\(_{H2O}\)/kg\(_{air}\))
+
+W\(_{ZoneB}\) ~~~~~~~~ = ~ Humidity ratio of air within Zone B (kg\(_{H2O}\)/kg\(_{air}\))
+
+Ρ\(_{ZoneA}\) = ~ Density of air within Zone A (kg/m\(^{3}\))
+
+�\(_{ZoneB}\) ~~~~~~~~~ = ~ Density of air within Zone B (kg/m\(^{3}\))
+
+\subsection{References}\label{references}
+
+ASHRAE. 2006d. \emph{Refrigeration Handbook}, Chapter 13. Atlanta: American Society of Heating,
+
+Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2009. \emph{Fundamentals Handbook}, Chapter 1. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Gosney, W.B., Olama, G.A.-L. 1975. Heat and Enthalpy Gains through Cold Room Doorways,~ Proceedings of the Institute of Refrigeration, vol.~72, pp 31-41
diff --git a/doc/engineering-reference/src/air-heat-balance-manager-processes/calculation-of-zone-air-temperature.tex b/doc/engineering-reference/src/air-heat-balance-manager-processes/calculation-of-zone-air-temperature.tex
new file mode 100644
index 00000000000..8f784f37c05
--- /dev/null
+++ b/doc/engineering-reference/src/air-heat-balance-manager-processes/calculation-of-zone-air-temperature.tex
@@ -0,0 +1,3 @@
+\section{Calculation of Zone Air Temperature}\label{calculation-of-zone-air-temperature}
+
+The zone air heat balance is the primary mechanism for linking the loads calculation to the system simulation.~ As such, the zone air temperature becomes the main interface variable.~ Its role in the integration process was described previously (``Basis for the Zone and Air System Integration'').
diff --git a/doc/engineering-reference/src/air-heat-balance-manager-processes/convection-from-internal-sources.tex b/doc/engineering-reference/src/air-heat-balance-manager-processes/convection-from-internal-sources.tex
new file mode 100644
index 00000000000..5971b28a636
--- /dev/null
+++ b/doc/engineering-reference/src/air-heat-balance-manager-processes/convection-from-internal-sources.tex
@@ -0,0 +1,3 @@
+\section{Convection from Internal Sources}\label{convection-from-internal-sources}
+
+This component is the companion part of the radiant contribution from internal gains described previously.~ It is added directly into the air heat balance. Such a treatment also violates the tenets of the heat balance since the surface temperature of the surfaces producing the internal loads exchange heat with the zone air through normal convective processes.~~ However, once again, the details required to include this component in the heat balance are generally not available, and its direct inclusion into the air heat balance is a reasonable approach..
diff --git a/doc/engineering-reference/src/air-heat-balance-manager-processes/convection-from-surfaces.tex b/doc/engineering-reference/src/air-heat-balance-manager-processes/convection-from-surfaces.tex
new file mode 100644
index 00000000000..b4d34b232f7
--- /dev/null
+++ b/doc/engineering-reference/src/air-heat-balance-manager-processes/convection-from-surfaces.tex
@@ -0,0 +1,9 @@
+\section{Convection from Surfaces}\label{convection-from-surfaces}
+
+This contribution is expressed using the convective heat transfer coefficient as follows:
+
+\begin{equation}
+{q_{conv}} = \sum\limits_{i = 1}^{nsurfaces} {{h_{c,i}}{A_i}\left( {{T_a} - {T_{s,i}}} \right)}
+\end{equation}
+
+The inside heat transfer coefficient is modeled from a choice of correlations.
diff --git a/doc/engineering-reference/src/air-heat-balance-manager-processes/infiltration-ventilation.tex b/doc/engineering-reference/src/air-heat-balance-manager-processes/infiltration-ventilation.tex
new file mode 100644
index 00000000000..a55e805bc12
--- /dev/null
+++ b/doc/engineering-reference/src/air-heat-balance-manager-processes/infiltration-ventilation.tex
@@ -0,0 +1,254 @@
+\section{Infiltration/Ventilation}\label{infiltrationventilation}
+
+\subsection{Infiltration}\label{infiltration}
+
+Any outdoor air that enters by way of infiltration is assumed to be immediately mixed with the zone air. The determination of the amount of infiltration air is quite complicated and subject to significant uncertainty. In the most common procedure, the infiltration quantity is converted from a number of air changes per hour (ACH) and included in the zone air heat balance using the outside temperature at the current simulation time step.
+
+EnergyPlus contains three models for infiltration. The first is the ``Design Flow Rate'' model that was inherited from EnergyPlus' predecessor programs. It is accessed through the ZoneInfiltration:DesignFlowRate object and is based on environmental conditions modifying a design flow rate.~ The second is the ``Effective Leakage Area'' model based on Sherman and Grimsrud (1980) and accessed using the ZoneInfiltration:EffectiveLeakageArea input object.~ The third is the ``Flow Coefficient'' model based on Walker and Wilson (1998) and accessed using the ZoneInfiltration:FlowCoefficient input object. The model formulations for the Effective Leakage Area and Flow Coefficient models are from the ASHRAE Handbook of Fundamentals (2001 Chapter 26; 2005 Chapter 27) where they are referred to as ``Basic'' and ``Enhanced'', respectively.
+
+\subsection{Infiltration Design Flow Rate}\label{infiltration-design-flow-rate}
+
+Infiltration (Ref Object: ZoneInfiltration:DesignFlowRate) is the unintended flow of air from the outdoor environment directly into a thermal zone. Infiltration is generally caused by the opening and closing of exterior doors, cracks around windows, and even in very small amounts through building elements. In this model, the user defines a design flow rate that can be modified by temperature differences and windspeed. The basic equation (Coblenz and Achenbach 1963) used to calculate infiltration with this model is:
+
+\begin{equation}
+Infiltration = \left( {{I_{design}}} \right)\left( {{F_{schedule}}} \right)\left[ {A + B\left| {\left( {{T_{zone}} - {T_{odb}}} \right)} \right| + C\left( {WindSpeed} \right) + D\left( {Windspee{d^2}} \right)} \right]
+\end{equation}
+
+More advanced infiltration calculations are possible using the EnergyPlus AirflowNetwork model for natural infiltration driven by wind when the HVAC system does not operate and/or driven by wind and forced air for times when the HVAC system operates. Exfiltration (the leakage of zone air to the outside) is generally handled better as zone exhaust air in the zone equipment description.
+
+The question of typical values for these coefficients is subject to debate. Ideally, one should do a detailed analysis of the infiltration situation and then determine a custom set of coefficients using methods such as those laid out in Chapter 26 of the ASHRAE Handbook of Fundamentals. The EnergyPlus defaults are 1,0,0,0 which gives a constant volume flow of infiltration under all conditions.
+
+BLAST (one of the EnergyPlus predecessors) used the following values as defaults:~ 0.606, 0.03636, 0.1177, 0. These coefficients produce a value of 1.0 at 0C deltaT and 3.35 m/s (7.5 mph) windspeed, which corresponds to a typical summer condition. At a winter condition of 40C deltaT and 6 m/s (13.4 mph) windspeed, these coefficients would increase the infiltration rate by a factor of 2.75.
+
+In DOE-2 (the other EnergyPlus predecessor), the air change method defaults are (adjusted to SI units) 0, 0, 0.224 (windspeed), 0. With these coefficients, the summer conditions above would give a factor of 0.75, and the winter conditions would give 1.34. A windspeed of 4.47 m/s (10 mph) gives a factor of 1.0.
+
+The source of the BLAST defaults is noted in the BLAST documentation as:
+
+``Empirical equation and the coefficient default were determined from ASHRAE journal articles and other data on the effects of outdoor weather conditions.''
+
+The source of the DOE-2 defaults is based on examining the infiltration relationships described in the ASHRAE Handbook of Fundamentals.
+
+The EnergyPlus example files use all of the above, the BLAST defaults in some (e.g., GeometryTest), the DOE-2 defaults in some (e.g., 5ZoneAirCooled), and the EnergyPlus defaults in some (e.g., LgOffVAVDetCoil).
+
+\subsection{Infiltration by Effective Leakage Area}\label{infiltration-by-effective-leakage-area}
+
+The Effective Leakage Area model is based on Sherman and Grimsrud (1980) and accessed using the ZoneInfiltration:EffectiveLeakageArea input object.~ The model formulation used in EnergyPlus is from the ASHRAE Handbook of Fundamentals (2001 Chapter 26; 2005 Chapter 27) where it is referred to as the ``Basic'' model.
+
+The Effective Leakage Area, or Sherman-Grimsrud, model is:
+
+\begin{equation}
+Infiltration = \left( {{F_{Schedule}}} \right)\frac{{{A_L}}}{{1000}}\sqrt {{C_s}\Delta T + {C_w}{{\left( {WindSpeed} \right)}^2}}
+\end{equation}
+
+where,
+
+\({F_{schedule}}\) ~is a value from a user-defined schedule,
+
+\({A_L}\) ~is the effective air leakage area in cm\(^{2}\) that corresponds to a 4 Pa pressure differential,
+
+\({C_s}\) ~is the coefficient for stack-induced infiltration in (L/s)\(^{2}\)/(cm\(^{4}\)·K),
+
+\(\Delta T\) ~is the absolute temperature difference between zone air and outdoor air,
+
+\({C_w}\) ~is the coefficient for wind-induced infiltration in (L/s)\(^{2}\)/(cm\(^{4}\)·(m/s)\(^{2}\)), and
+
+\(WindSpeed\) ~is the local wind speed.
+
+\subsection{Infiltration by Flow Coefficient}\label{infiltration-by-flow-coefficient}
+
+The Flow Coefficient model is based on Walker and Wilson (1998) and accessed using the ZoneInfiltration:FlowCoefficient input object.~ The model formulation used in EnergyPlus is from the ASHRAE Handbook of Fundamentals (2001 Chapter 26; 2005 Chapter 27) where it is referred to as the ``Enhanced'' or ``AIM-2'' model.
+
+The Enhanced, or AIM-2, model is:
+
+\begin{equation}
+Infiltration = \left( {{F_{Schedule}}} \right)\sqrt {{{\left( {c\,{C_s}\Delta {T^n}} \right)}^2} + {{\left( {c\,{C_w}{{\left( {s * WindSpeed} \right)}^{2n}}} \right)}^2}}
+\end{equation}
+
+where,
+
+\({F_{schedule}}\) ~is a value from a user-defined schedule,
+
+\(c\) ~is the flow coefficient in m\(^{3}\)/(s·Pa\(^{n}\)),
+
+\({C_s}\) ~is the coefficient for stack-induced infiltration in (Pa/K)\(^{n}\),
+
+\(n\) ~is the pressure exponent,
+
+\({C_w}\) ~is the coefficient for wind-induced infiltration in (Pa·s\(^{2}\)/m\(^{2}\))\(^{n}\), and
+
+\(s\) ~is the shelter factor.
+
+\subsubsection{References:}\label{references-031}
+
+Coblenz, C. W. and Achenbach, P. R. 1963. Field Measurement of Ten Electrically-Heated Houses. ASHRAE Transactions pp 358-365.
+
+Sherman, M.H. and D.T. Grimsrud. 1980. Infiltration-pressurization correlation: Simplified physical modeling. ASHRAE Transactions 86(2):778
+
+Walker, I.S., and D.J. Wilson. 1998. Field validation of equations for stack and wind driven air infiltration calculations.~ International Journal of HVAC\&R Research 4(2).
+
+ASHRAE Handbook of Fundamentals. 2005. Chapter 27. (and 2001 Chapter 26).
+
+\subsection{Ventilation}\label{ventilation}
+
+EnergyPlus contains two models for ventilation.~ The ``Design Flow Rate'' model, inherited from EnergyPlus' predecessor programs, is accessed through the ZoneVentilation:DesignFlowRate object and is based on environmental conditions modifying a design flow rate.~ The ``Wind and Stack with Open Area'' model, based on equations defined in Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals, is accessed using the ZoneVentilation:WindandStackOpenArea input object. Since the ``Wind and Stack with Open Area'' object requires the height difference between the midpoint of the lower opening and the neutral pressure level, which is difficult to estimate, this object should be used with care (e.g., research only).
+
+These two ventilation objects can be used alone or in combination to determine ventilation air for a zone. If multiple ZoneVentilation:* objects are specified for a zone, then the total zone ventilation flow rate is the sum of the ventilation air flow rates calculated by each ZoneVentilation object.
+
+\subsection{Ventilation Design Flow Rate}\label{ventilation-design-flow-rate}
+
+Ventilation (Ref Object: ZoneVentilation:DesignFlowRate) is the purposeful flow of air from the outdoor environment directly into a thermal zone in order to provide some amount of non-mechanical cooling.~ Ventilation as specified by this input syntax is intended to model ``simple'' ventilation as opposed to the more detailed ventilation investigations that can be performed with the AirflowNetwork model.~ Simple ventilation in EnergyPlus can be controlled by a schedule and through the specification of minimum, maximum and delta temperatures. The temperatures can be either single constant values for the entire simulation or schedules which can vary over time. Specific details are given in the Input/Output reference document. As with infiltration, the actual flow rate of ventilation can be modified by the temperature difference between the inside and outside environment and the wind speed. The basic equation used to calculate ventilation using this model is:
+
+\begin{equation}
+Ventilation = \left( {{V_{design}}} \right)\left( {{F_{schedule}}} \right)\left\lfloor {A + B\left| {{T_{zone}} - {T_{odb}}} \right| + C\left( {WindSpeed} \right) + D\left( {WindSpee{d^2}} \right)} \right\rfloor
+\end{equation}
+
+More advanced ventilation calculations are possible using the EnergyPlus AirflowNetwork model.
+
+The following description is copied from the Infiltration discussion above. The question of typical values for these coefficients is subject to debate. Ideally, one should do a detailed analysis of the ventilation situation and then determine a custom set of coefficients using methods such as those laid out in Chapter 26 of the ASHRAE Handbook of Fundamentals. The EnergyPlus defaults are 1,0,0,0 which gives a constant volume flow of ventilation under all conditions.
+
+BLAST (one of the EnergyPlus predecessors) used the following values as defaults:~ 0.606, 0.03636, 0.1177, 0. These coefficients produce a value of 1.0 at 0C deltaT and 3.35 m/s (7.5 mph) windspeed, which corresponds to a typical summer condition. At a winter condition of 40C deltaT and 6 m/s (13.4 mph) windspeed, these coefficients would increase the ventilation rate by a factor of 2.75.
+
+In DOE-2 (the other EnergyPlus predecessor), the air change method defaults are (adjusted to SI units) 0, 0, 0.224 (windspeed), 0. With these coefficients, the summer conditions above would give a factor of 0.75, and the winter conditions would give 1.34. A windspeed of 4.47 m/s (10 mph) gives a factor of 1.0.
+
+The source of the BLAST defaults is noted in the BLAST documentation as:
+
+``Empirical equation and the coefficient default were determined from ASHRAE journal articles and other data on the effects of outdoor weather conditions.''
+
+The source of the DOE-2 defaults is based on examining the infiltration relationships described in the ASHRAE Handbook of Fundamentals.
+
+The EnergyPlus example files use all of the above, the BLAST defaults in some (e.g., AirflowNetwork\_Simple\_house), the DOE-2 defaults in some (e.g., VentilationSimpleTest -- has all 3), and the EnergyPlus defaults in some (e.g., 5ZoneNightVent2).
+
+\subsection{Ventilation by Wind and Stack with Open Area}\label{ventilation-by-wind-and-stack-with-open-area}
+
+For this model (Ref Object: ZoneVentilation:WindandStackOpenArea), the ventilation air flow rate is a function of wind speed and thermal stack effect, along with the area of the opening being modeled. This object can be used alone or in combination with ZoneVentilation:DesignFlowRate objects. This model is intended for simplified ventilation calculations as opposed to the more detailed ventilation investigations that can be performed with the AirflowNetwork model. Using the ``Wind and Stack with Open Area'' model, the natural ventilation flow rate can be controlled by a multiplier fraction schedule applied to the user-defined opening area and through the specification of minimum, maximum and delta temperatures. The temperatures can be either single constant values for the entire simulation or schedules which can vary over time. The equation used to calculate the ventilation rate driven by wind is given by Eq. 37 in Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals:
+
+\begin{equation}
+{Q_w} = {C_w}{A_{opening}}{F_{schedule}}V
+\end{equation}
+
+where,
+
+\emph{Q\(_{w}\)}~ = Volumetric air flow rate driven by wind {[}m\(^{3}\)/s{]}
+
+\emph{C\(_{w}\)}~ = Opening effectiveness {[}dimensionless{]}
+
+\emph{A\(_{opening}\)}~~~~~~~ = Opening area {[}m\(^{2}\){]}
+
+\emph{F\(_{schedule}\)} = Open area fraction {[}user-defined schedule value, dimensionless{]}
+
+\emph{V}~~~ = Local wind speed {[}m/s{]}
+
+If the user specifies ``Autocalculate'' for the Opening Effectiveness input field, the opening effectiveness is calculated for each simulation time step based on the angle between the actual wind direction and the Effective Angle (a user-defined input) using the following equation:
+
+\begin{equation}
+{C_w} = 0.55 - \frac{{\left| {EffectiveAngle - WindDirection} \right|}}{{180}}*0.25
+\end{equation}
+
+The difference \textbar{}EffectiveAngle -- WindDirection\textbar{} should be between 0 and 180 degrees. If the difference \textbar{}EffectivAngle -- WindDirection\textbar{} is greater than 180, the difference is reset to be minus 180 degrees. This equation is a linear interpolation using the values recommended by the 2009 ASHRAE Handbook of Fundamentals (page 16.13): 0.5 to 0.6 for perpendicular winds and 0.25 to 0.35 for diagonal winds.
+
+The equation used for calculating the ventilation rate due to stack effect is given by Eq. 38 in Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals:
+
+\begin{equation}
+{Q_s} = {C_D}{A_{opening}}{F_{schedule}}\sqrt {2g\Delta {H_{NPL}}(|{T_{zone}} - {T_{odb}}|/{T_{zone}})}
+\end{equation}
+
+where,
+
+\emph{Q\(_{s}\)}~ = Volumetric air flow rate due to stack effect {[}m\(^{3}\)/s{]}
+
+\emph{C\(_{D}\)}~ = Discharge coefficient for opening {[}dimensionless{]}
+
+\emph{A\(_{opening}\)}~~~~~~~ = Opening area {[}m\(^{2}\){]}
+
+\emph{F\(_{schedule}\)} = Open area fraction {[}user-defined schedule value, dimensionless{]}
+
+\emph{ΔH\(_{NPL}\)}~~~~~~~ = Height from midpoint of lower opening to the neutral pressure level {[}m{]}.
+
+Estimation of this value is difficult; refer to Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals for guidance.
+
+\emph{T\(_{zone}\)}~~~~~~~~~~~ = Zone air dry-bulb temperature {[}K{]}
+
+\emph{T\(_{odb}\)} = Local outdoor air dry-bulb temperature {[}K{]}
+
+The following equation, given by Eq. 39 in Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals, is used to calculate the Discharge Coefficient for Opening when the user sets the value for this input field to ``Autocalculate'':
+
+\begin{equation}
+{C_D} = 0.40 + 0.0045\left| {{T_{zone}} - {T_{odb}}} \right|
+\end{equation}
+
+The total ventilation rate calculated by this model is the quadrature sum of the wind and stack air flow components:
+
+\begin{equation}
+Ventilatio{n_{WindAndStack}} = \sqrt {{Q_s}^2 + {Q_w}^2}
+\end{equation}
+
+If desired, a simple summation, instead of quadrature summation, can be realized by inputting two ZoneVentilation:WindAndStackOpenArea objects. One object can be defined with only a wind-driven component by setting C\(_{D}\) = 0, and the other object can have only stack-effect inputs specified and set C\(_{w}\) = 0.
+
+\subsection{Zone Air Balance Outdoor Airflow (ZoneAirBalance:OutdoorAir)}\label{zone-air-balance-outdoor-airflow-zoneairbalanceoutdoorair}
+
+ASHRAE 2009 Handbook of Fundamentals specifies that any unbalanced supply or exhaust ventilation air, Q\(_{u,v}\), to a zone causes pressurization/depressurization that influences the flow of infiltration air and thus should be combined with natural infiltration, Q\(_{n}\), (and, if present, unbalanced duct leakage, Qu,l) in superposition. Balanced ventilation airflow, Q\(_{b,v}\), to a zone (such as an ERV or HRV with balanced exhaust and intake air flows) does not interact with infiltration air and is added in whole:
+
+\begin{equation}
+Q = \sqrt {{Q_n}^2 + {Q_{u,v}}^2 + ({Q_{u,l}}^2)}  + {Q_{b,v}}
+\end{equation}
+
+where,
+
+\emph{Q}~~~ = Combined outdoor airflow with infiltration, balanced and unbalanced outdoor air flows, and unbalanced duct leakage {[}m\(^{3}\)/s{]}
+
+\emph{Q\(_{n}\)}~~ = Natural infiltration airflow {[}m\(^{3}\)/s{]}
+
+\emph{Q\(_{b,v}\)} = Balanced ventilation airflow, excluding infiltration {[}m\(^{3}\)/s{]}
+
+\emph{Q\(_{u,v}\)} = Unbalanced ventilation airflow, excluding infiltration {[}m\(^{3}\)/s{]}
+
+\emph{Q\(_{u,l}\)}~ = Unbalanced duct leakage: the difference between supply and return leaks {[}m\(^{3}\)/s{]}
+
+The natural infiltration airflow includes all outdoor airflows from all ZoneInfiltration:* objects for the same zone.
+
+\begin{equation}
+{Q_n} = \sum\limits_i {{Q_{Infiltration,i}}}
+\end{equation}
+
+where,
+
+\emph{Q\(_{Infiltration,i}\)}~~~~~ = Outdoor airflow rate given in the ith ZoneInfiltration:* objects for the same zone
+
+The balanced ventilation airflow is the sum of outdoor airflows from all ZoneVentilation: DesignFlowRate objects with Ventilation Type = Balanced:
+
+\begin{equation}
+{Q_{b,v}} = \sum\limits_i {{Q_{v,Balanced,i}}}
+\end{equation}
+
+where,
+
+\emph{Q\(_{v,Balanced,i}\)}~~~~ = Ventilation rate with ``Balanced'' ventilation type defined in the ith ZoneVentilation:DesignFlowRate object for the same zone
+
+The unbalanced ventilation airflow is given by the following equation:
+
+{\scriptsize
+\begin{equation}
+{Q_{u,v}} = {\left[ {{{\left( {\sum\limits_i {{Q_{v,Natural,i}}}  + \sum\limits_i {{Q_{v,Wind,i}}} } \right)}^2} + {{\left( {\sum\limits_i {{Q_{v,Intake,i}}} } \right)}^2} + {{\left( {\sum\limits_i {{Q_{v,Exhaust,i}}} } \right)}^2} + {{\left( {\sum\limits_i {Max\left( {0,\;({Q_{ERV,Exh,i}} - {Q_{ERV,Sup,i}})} \right)} } \right)}^2}} \right]^{0.5}}
+\end{equation}}
+
+where
+
+\emph{Q\(_{v,Exhaust,i}\)}~~~~~ = Ventilation rate with ``Exhaust'' type in the ith ZoneVentilation:DesignFlowRate object for the same zone
+
+\emph{Q\(_{v,Intake,i}\)}~~~~~~~ = Ventilation rate with ``Intake'' type in the ith ZoneVentilation:DesignFlowRate object for the same zone
+
+\emph{Q\(_{v,Natural,i}\)}~~~~~~ = Ventilation rate with ``Natural'' type in the ith ZoneVentilation:DesignFlowRate object for the same zone
+
+\emph{Q\(_{v,Wind,v}\)}~~~~~~~ = Ventilation rate in the ith ZoneVentilation:WindandStackOpenArea object for the same zone
+
+\emph{Q\(_{ERV,Sup,i}\)}~~~~~~ = Supply flow rate given in the ith ZoneHVAC:EnergyRecoveryVentilator object
+
+\emph{Q\(_{ERV,Exh,i}\)}~~~~~~ = Exhaust flow rate given in the ith ZoneHVAC:EnergyRecoveryVentilator object
+
+For Ventilation Type = Intake in the ZoneVentilation:DesignFlowRate object, an appropriate amount of fan heat will be ignored and the outdoor temperature will be used in the zone air heat balance equation.
+
+This object provides a simple airflow interaction model without having to use the AirflowNetwork capabilities, when the Air Balance Method is specified as Quadrature.
+
+\subsection{Reference}\label{reference}
+
+ASHRAE. 2009. 2009 ASHRAE Handbook -- Fundamentals, Chapter 16, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
diff --git a/doc/engineering-reference/src/alternative-modeling-processes.tex b/doc/engineering-reference/src/alternative-modeling-processes.tex
new file mode 100644
index 00000000000..0b573ef1b16
--- /dev/null
+++ b/doc/engineering-reference/src/alternative-modeling-processes.tex
@@ -0,0 +1,2010 @@
+\chapter{Alternative Modeling Processes}\label{alternative-modeling-processes}
+
+\subsection{RoomAir Models}\label{roomair-models}
+
+The group of models described in this section is used to account for non-uniform room air temperatures that may occur within the interior air volume of a zone. These models are accessed using the RoomAirModelType input object. RoomAir modeling was added to EnergyPlus starting with Version 1.2. Although there are many types of analyses (comfort, indoor air quality, etc) that might benefit from localized modeling of how room air varies across space, most of the room air models in EnergyPlus only address the distribution of \emph{temperature} within the zone. This allows surface heat transfer and air system heat balance calculations to be made taking into account natural thermal stratification of air and different types of intentional air distribution designs such as under-floor and side-wall displacement ventilation that purport to extract room air at higher-than-mean temperatures. The exception is the RoomAirflowNetwork model, which integrates the AirflowNetwork model and applies the nodal airflow model within zones. Note that EnergyPlus does \textbf{not} have completely general methods of modeling room air that are applicable to every conceivable type of airflow that might occur in a zone. Such models (e.g.~RANS-CFD) are too computationally expensive to use with EnergyPlus for the foreseeable future. The models that are available in EnergyPlus offer only limited modeling capabilities for select room airflow configurations. Also note that because the complete mixing model for room air has long been the standard in building energy simulation, there is not currently a consensus on how to best model non-uniform air temperatures in buildings. Therefore, it is up to the user to have a good understanding of when, where, and how to apply the room air models available in EnergyPlus. The rest of this section provides some guidance in the way of examples and further discussion of the models available in EnergyPlus.
+
+EnergyPlus offers the different types of air models listed in the table below along with the input objects associated with the use of that model.
+
+% table 43
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{3.0in}}
+\caption{Summary of room air models available in EnergyPlus \label{table:summary-of-room-air-models-available-in}} \tabularnewline
+\toprule 
+Air model name & Applicability & Input Objects Required \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Summary of room air models available in EnergyPlus} \tabularnewline
+\toprule 
+Air model name & Applicability & Input Objects Required \tabularnewline
+\midrule
+\endhead
+
+Well-Mixed & All zones & None, default \tabularnewline
+User Defined & Any zone where the user has prior knowledge of the temperature pattern & ‘RoomAirModelType’, ‘RoomAir:TemperaturePattern:UserDefined’, ‘RoomAir:TemperaturePattern: xx’ \tabularnewline
+One-Node Displacement Ventilation (Mundt) & displacement ventilation in typical office-type zones & ‘RoomAirModelType’, ‘RoomAirSettings:OneNodeDisplacementVentilation’, ‘RoomAir:Node’’ \tabularnewline
+Three-Node Displacement Ventilation (UCSD) & displacement ventilation & ‘RoomAirModelType’, ‘RoomAirSettings:ThreeNodeDisplacementVentilation’ \tabularnewline
+Under-Floor Air Distribution Interior Model (UCSD) & Interior zones served by a UFAD system & ‘RoomAirModelType’, ‘RoomAirSettings:UnderFloorAirDistributionInterior’ \tabularnewline
+Under-Floor Air Distribution Exterior Model (UCSD) & Exterior zones served by a UFAD system & ‘RoomAirModelType’, ‘RoomAirSettings:UnderFloorAirDistributionExterior’ \tabularnewline
+UCSD Cross Ventilation & cross ventilation & ‘RoomAirModelType’, ‘RoomAirSettings:CrossVentilation’ \tabularnewline
+RoomAirflowNetwork & Room air model using AirflowNetwork & ‘RoomAirModelType’, ‘RoomAirSettings:AirflowNetwork’ ‘RoomAirflowNetwork:Node’, ‘RoomAirflowNetwork:Node:AdjacentSurfaceList’, ‘RoomAirflowNetwork:Node:InternalGains’, ‘RoomAirflowNetwork:Node:InternalGains’, ‘AirflowNetwork:IntraZone:Node’, ‘AirflowNetwork:IntraZone:Linkage’ \tabularnewline
+\bottomrule
+\end{longtable}
+
+The room air models are coupled to the heat balance routines using the framework described by Griffith and Chen (2004).~ Their framework was modified to include features needed for a comprehensive program for annual energy modeling rather than one for hourly load calculations.~ The formulation is largely shifted from being based on the setpoint temperature to one based on the current mean air temperature.~ This is necessary to allow for floating temperatures and dual setpoint control where there may be times that the mean zone temperatures are inside the dead band.~ The coupling framework was also extended to allow for exhaust air flows (e.g.~bathroom exhaust fans) in addition to air system return flows.
+
+The inside face temperature calculation is modified by rewriting the zone air temperature, \emph{T\(_{a}\)}, with an additional subscript, \emph{i}, for the surface index (\({T_{{a_j}}} \to {T_{{a_{i,j}}}}\) or \({T_{{a_{}}}} \to {T_{{a_i}}}\) ).~ The inside face heat balance is solved for its surface temperature using,
+
+{\scriptsize
+\begin{equation}
+{T_{{s_{i,j}}}} = \frac{{{T_{s{o_{i,j}}}}{Y_{i,o}} + \sum\limits_{k = 1}^{nz} {{T_{s{o_{i,j - k}}}}} {Y_{i,k}} - \sum\limits_{k = 1}^{nz} {{T_{{s_{i,j - k}}}}} {Z_{i,k}} + \sum\limits_{k = 1}^{nq} {{\Phi_{i,k}}{{q''}_{k{i_{i,j - k}}}} + {T_{{a_{i,j}}}}{h_{{c_{i,j}}}} + {{q''}_{LWS}} + {{q''}_{LWX}} + {{q''}_{SW}} + {{q''}_{sol}}} }}{{{Z_{i,o}} + {h_{{c_{i,j}}}}}}
+\end{equation}}
+
+where, ~~~~~~~ \emph{T\(_{s}\)} ~~~~~~~ is the inside face temperature
+
+\emph{i}~~~~~~~~~~ subscript indicates individual surfaces
+
+~~~~~ \emph{j}~~~~~~~~~~ subscript indicates current time step
+
+~~~~~ \emph{k}~~~~~~~~~ subscript indicates time history steps
+
+~~~~~ \emph{T\(_{so}\)} ~~~~~~ is the outside face temperature
+
+~~~~~ \emph{Y\(_{i}\) ~~~~~~~} are the cross CTF coefficients
+
+~~~~~ \emph{Z\(_{i}\)} are the inside CTF coefficients
+
+~~~~~ \(\varphi_{i}\) ~~~~~~~ are the flux CTF coefficients
+
+~~~~~ \({q''_{ki}}\) ~~~~~~ is the conduction heat flux through the surface
+
+~~~~~ \({h_{{c_i}}}\) ~~~~~~ is the surface convection heat transfer coefficient
+
+~~~~~ \emph{T\(_{a}\)}~~~~~~~~ is the near-surface air temperature
+
+~~~~~ \({q''_{LWS}}\) ~~~ is the longwave radiation heat flux from equipment in zone
+
+~~~~~ \({q''_{LWX}}\) ~~~ is the net long wavelength radiation flux exchange between zone surfaces
+
+~~~~~ \({q''_{SW}}\) ~~~~ is the net short wavelength radiation flux to surface from lights
+
+~~~~~ \({q''_{sol}}\) ~~~~~ is the absorbed direct and diffuse solar (short wavelength) radiation
+
+\subsubsection{References:}\label{references-005}
+
+Griffith, B. and Q. Chen. 2004. Framework for coupling room air models to heat balance load and energy calculations (RP-1222). International Journal of Heating, Ventilating, Air-conditioning and Refrigerating Research. ASHRAE, Atlanta GA.~ Vol 10. No 2. April 2004.
+
+\subsection{User Defined RoomAir Temperatures}\label{user-defined-roomair-temperatures}
+
+The input object RoomAir:TemperaturePattern:UserDefined provides a capabity for users to define the sort of air temperature pattern he or she expects in the zone.~ With these models, the pattern is generally set beforehand and does not respond to conditions that evolve during the simulation.~ (Exception: the pattern available through the RoomAir:TemperaturePattern:TwoGradient object will switch between two different pre-defined vertical gradients depending on the current value of certain temperatures or thermal loads. )
+
+The user-defined patterns obtain the mean air temperature, \({T_{MAT}}\) , from the heat balance domain and then produce modified values for:
+
+~~~~~ \({T_{ai}}\) ~~~~~~ the adjacent air temperature which is then used in the calculation of inside face surface temperature during the heat balance calculations,
+
+~~~~~ \({T_{leaving}}\) ~ the temperature of air leaving the zone and entering the air system returns
+
+~~~~~ \({T_{exhaust}}\) ~ the temperature of air leaving the zone and entering the exhaust.
+
+~~~~~ \({T_{stat}}\) ~~~~ the temperature of air ``sensed'' at the thermostat (not currently used in air system control because air system flows use load-based control).
+
+The user defined room air models used indirect coupling so that the patterns provide values for, or ways to calculate, how specific temperatures differ from \({T_{MAT}}\) .~ The various \(\Delta T\) ~values determined from the model are applied to \({T_{MAT}}\) ~as follows:
+
+\begin{equation}
+{T_{ai}} = \Delta {T_{ai}} + {T_{MAT}}
+\end{equation}
+
+(where ``\emph{i's''} represents each surface in the zone that is affected by the model)
+
+\begin{equation}
+{T_{leaving}} = \Delta {T_{return}} + {T_{MAT}}
+\end{equation}
+
+\begin{equation}
+{T_{exhaust}} = \Delta {T_{exhaust}} + {T_{MAT}}
+\end{equation}
+
+\begin{equation}
+{T_{stat}} = \Delta {T_{stat}} + {T_{MAT}}
+\end{equation}
+
+The patterns defined by the object `RoomAir:TemperaturePattern:SurfaceMapping' are fairly straightforward.~ The user directly inputs values for \(\Delta {T_{ai}}\) ~for each surface.~ The pattern ``maps'' specific surfaces, identified by name, to \(\Delta {T_{ai}}\) ~values.~ This provides completely general control (but in practice may be cumbersome to use).~ The other patterns focus on temperature changes in the vertical direction.~ Surfaces do not need to be identified, but all the surfaces with the same height will be assigned the same \(\Delta {T_{ai}}\) ~values.
+
+The patterns defined by the object `RoomAir:TemperaturePattern:NondimensonalHeight' apply a temperature profile based on a non-dimensionalized height, \({\rm Z}\) .~ The height of each surface is defined to be the z-coordinate of the surface's centroid relative to the average z-coordinate of the floor surfaces.~ The zone ceiling height is used as the length scale to non-dimensionalize each surface's height so that,
+
+\begin{equation}
+{{\rm Z}_i} = ({z_{i,centroid}} - {z_{floorAvg}})/Ceiling\;Height
+\end{equation}
+
+(where ``\emph{i's''} represents each surface in the zone that is affected by the model)
+
+The values for \({Z_i}\) ~are constrained to be between 0.01 and 0.99 because the value is meant to describe the air layer near the surface (say approximate 0.1 m from the surface) rather than the surface itself.
+
+The user-defined profile is treated as a look up table or piecewise linear model.~ The values for \(\Delta {T_{ai}}\) ~are determined by searching the \({\rm Z}\) ~values in the user-defined profile and performing linear interpolation on the associated \(\Delta {T_a}\) ~values.
+
+The patterns defined by the object `RoomAir:TemperaturePattern:ConstantGradient' apply a constant temperature gradient in the vertical direction.~ The model assumes that \({T_{MAT}}\) ~occurs at the mid-plane so that \({{\rm Z}_{{T_{MAT}}}} = 0.5\) ~(by definition).~ The surface \({Z_i}\) ~values are compared to \({Z_{{T_{MAT}}}}\) and then scaled with zone ceiling height to obtain values for the change in height (in units of meters), \(\Delta z\) .~ The user defined gradient, \(grad\) , (units of ºC/m) is then used to determine \(\Delta {T_{ai}}\) ~values using
+
+\begin{equation}
+\Delta {T_{ai}} = \Delta z * grad
+\end{equation}
+
+The patterns defined by the object `RoomAir:TemperaturePattern:TwoGradient' are very similar to the constant gradient pattern above but the value of \(grad\) ~used at any given time is selected by interpolating between two user-defined values for \(grad\) .~ Five options are available, three based on temperatures and two based on thermal loads -- see the Input Output Reference.~ The user provides upper and lower bounding values.~ If the current value of the ``sensing'' variable lies between the upper and lower bounds, then \(grad\) ~is determined using linear interpolation.~ If the designated value is above the upper bound then the upper value for \(grad\) ~is used (no extrapolation).~ Similarly, if the designated value is below the lower bound, then the lower value for \(grad\) ~is used.~ Note that ``upper'' and ``lower'' indicate the temperature and heat rate bounds and that the values for \(grad\) ~do not have to follow in the same way; the \(grad\) ~value for the lower bound could be higher than the \(grad\) ~value for the upper bound (providing a something of a reverse control scheme).~ Rather than directly using \(\Delta T\) ~values from the user, the temperatures for the return air, exhaust and thermostat are determined based on user-entered heights (in units of meters from the floor) and applying the current value for \(grad\) .
+
+\subsection{One-Node Displacement Ventilation RoomAir Model}\label{one-node-displacement-ventilation-roomair-model}
+
+The input object RoomAirSettings:OneNodeDisplacementVentilation provides a simple model for displacement ventilation.~ Mundt (1996) points out that a floor air heat balance provides a simple and reasonably accurate method of modeling the temperature near the floor surface. The slope of a linear temperature gradient can then be obtained by adding a second upper air temperature value that comes from the usual overall air system cooling load heat balance.~ The figure below diagrams the temperature distribution versus height being calculated by the model.~ Mundt's floor air heat balance is extended to include convection heat gain from equipment and by ventilation or infiltration that may be introduced near the floor in order to maintain all the terms in the air heat balance of the Heat Balance Model.~ This yields the following heat balance for a floor air node,
+
+\begin{equation}
+\rho \,{c_p}\dot V({T_{AirFloor}} - {T_{Supply}}) = {h_{cFloor}}{A_{Floor}}({T_{Floor}} - {T_{AirFloor}}) + {Q_{ConvSourceFloor}} + {Q_{InfilFloor}}
+\end{equation}
+
+where
+
+\emph{�} is the air density
+
+\emph{c\(_{p}\)} is the air specific heat at constant pressure
+
+\(\mathop V\limits^\cdot\) is the air system flow rate
+
+\emph{T\(_{supply}\)} is the air system's supply air drybulb temperature
+
+\emph{h\(_{cFloor}\)} ~is the convection heat transfer coefficient for the floor
+
+\emph{A\(_{floor}\)} is the surface area of the floor
+
+\emph{T\(_{floor}\)} is the surface temperature of the floor
+
+\emph{Q\(_{convSourceFloor}\)~} is the convection from internal sources near the floor (\textless{} 0.2 m)
+
+\emph{Q\(_{InfilFloor}\)}~ is the heat gain (or loss) from infiltration or ventilation near the floor
+
+``Floor splits'' are the fraction of total convective or infiltration loads that are dispersed so as to add heat to the air located near the floor.~ The user prescribes values for floor splits as input.~ No guidance is known to be available to use in recommending floor splits, but the user could for example account for equipment known to be near the floor, such as tower computer cases, or supplementary ventilation designed to enter along the floor.~ The equation above can be solved directly for \emph{T\(_{AirFloor}\)} and is used in the form of the equation below,
+
+\begin{equation}
+{T_{AirFloor}} = \frac{{\rho \,{c_p}\dot V{T_{Supply}} + \sum {{h_{cFloor}}{A_{Floor}}{T_{Floor}}}  + {{\dot Q}_{ConvSourceFloor}} + {{\dot Q}_{InfilFloor}}}}{{\rho \,{c_p}\dot V + \sum {{h_{cFloor}}{A_{Floor}}} }}
+\end{equation}
+
+The upper air node temperature is obtained by solving the overall air heat balance for the entire thermal zone for the temperature of the air leaving the zone and going into the air system return, \emph{T\(_{leaving}\)}.
+
+\begin{equation}
+{T_{Leaving}} = \frac{{ - {{\dot Q}_{sys}}}}{{p{c_p}\dot V}} + {T_{Supply}}
+\end{equation}
+
+where \({\dot Q_{sys}}\) ~is the air system heat load with negative values indicating a positive cooling load.~ Values for \({\dot Q_{sys}}\) ~are computed by the load calculation routines and passed to the air model.~ The vertical temperature gradient or slope, \emph{dT/dz}, is obtained from,
+
+\begin{equation}
+\frac{{dT}}{{dz}} = \frac{{{T_{Leaving}} - {T_{AirFloor}}}}{{{H_{return}}}}
+\end{equation}
+
+where \emph{H\(_{return}\)} is the distance between the air system return and the floor air node assumed to be 0.1 m from the floor and \emph{z} is the vertical distance.
+
+\begin{figure}[hbtp] % fig 132
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2341.svg.png}
+\caption{Height versus temperature schematic for Mundt model \protect \label{fig:height-versus-temperature-schematic-for-mundt}}
+\end{figure}
+
+The constant slope allows obtaining temperatures at any vertical location using,
+
+\begin{equation}
+{T_{{a_i}}} = {T_{leaving}} - \frac{{dT}}{{dz}}({z_{leaving}} - {z_i})
+\end{equation}
+
+So for example the temperatures near the ceiling can easily be determined. Accounting for the location of the thermostat inside the zone (e.g.~1.1 m) is accomplished by returning the temperature for the appropriate height to the appropriate air node used for control. If the walls are subdivided in the vertical direction as shown in the figure above, then the air model can provide individual values for each surface based on the height and slope.~ However, no additional heat balances are necessarily made (in the air domain) at these points as all the surface convection is passed to the model in the totaled value for \({\dot Q_{sys}}\) .
+
+\subsubsection{References}\label{references-1-001}
+
+Mundt, E. 1996. The performance of displacement ventilation systems-experimental and theoretical studies, Ph. D. Thesis, Royal Institute of Technology, Stockholm.
+
+\subsection{Three-Node Displacement Ventilation RoomAir Model}\label{three-node-displacement-ventilation-roomair-model}
+
+\subsubsection{Overview}\label{overview-005}
+
+The input object RoomAirSettings:ThreeNodeDisplacementVentilation provides a simple model for heat transfer and vertical temperature profile prediction in displacement ventilation. The fully-mixed room air approximation that is currently used in most whole building analysis tools is extended to a three node approach, with the purpose of obtaining a first order precision model for vertical temperature profiles in displacement ventilation systems. The use of three nodes allows for greatly improved prediction of thermal comfort and overall building energy performance in low energy cooling strategies that make use of unmixed stratified ventilation flows.
+
+The UCSD Displacement Ventilation Model is one of the non-uniform zone models provided through the Room Air Manager in EnergyPlus. The intent is to provide a selection of useful non-uniform zone air models to enable the evaluation of air-conditioning techniques that use stratified or partially stratified room air. Such techniques include displacement ventilation (DV) and underfloor air distribution (UFAD) systems. The methodology can also include, in principle, natural displacement ventilation and also wind-driven cross-ventilation (CV).
+
+\subsubsection{Displacement Ventilation}\label{displacement-ventilation}
+
+A DV system is a complete contrast to a conventional forced air system. In a conventional system conditioned air is delivered at ceiling level and the intent is to create a fully mixed space with uniform conditions. In a DV system conditioned air is delivered at floor level and low velocity in order to minimize mixing and to establish a vertical temperature gradient. The incoming air ``displaces'' the air above it which, in turn,~ is exhausted through ceiling level vents. In DV a noticeable interface occurs between the occupied zone of the room and a mixed hot layer near the ceiling of the room(Dominique \& Guitton, 1997). Maintaining the lower boundary of this warm layer above the occupied zone is one of the many unique challenges of displacement ventilation design. Often DV systems use 100\% outside air. The vertical displacement air movement means that convective heat gains introduced near the ceiling will be removed without affecting the occupied region of the room. Also a fraction of the heat gains that occur in the occupied zones rise as plumes into the upper part of the space, thereby reducing the cooling load. Similarly the fresh air will be used more effectively than with a fully mixed system: the fresh air won't be ``wasted'' in the upper, unoccupied region of the room. Finally, the vertical temperature gradient means that the average room temperature can be higher for a DV conditioned room than with a conventionally conditioned room: the occupants feel the lower temperature in the lower region of the room and are unaffected by the higher temperature near the ceiling. However, whenever the outside air temperature is above ≈19°C this advantage is mostly lost: the internal loads must be removed from the space independently of the airflow pattern (during the warmer hours buildings tend to be almost closed to the outside, operating in closed loop). The inflow temperature advantage is then only useful for the minimum outside air that must always be provided (in most cases this remaining advantage is negligible).
+
+DV systems have limitations. In order to avoid chilling the occupants the supply air temperature used for DV is considerably higher than that used in conventional forced-air systems. This can lead to problems in removing both sensible and latent loads. Exterior spaces may have conditions that are not conducive to establishing a vertical temperature gradient. DV systems seem to be best suited to interior spaces with only moderate loads.
+
+\subsubsection{Non-uniform zone models}\label{non-uniform-zone-models}
+
+Several types of models have been proposed as suitable for inclusion in building energy simulation (BES) programs. These models must be simple enough not to impose an undue computational burden on a BES program, yet provide enough predictive capability to produce useful comparisons between conventional and stratified zone operation strategies. ASHRAE RP-1222 (Chen \& Griffith 2002) divides the candidate models into two categories: \emph{nodal} and \emph{zonal}. Nodal models describe the zone air as a network of nodes connected by flow paths; each node couples convectively to one or more surfaces. Zonal models are coarse--grained finite volume models. ASHRAE RP-1222 provides a short history (and examples) of each type of model. In terms of nodal models for displacement ventilation we mention the Mundt model (Mundt 1996), since it is implemented in EnergyPlus, and the Rees-Haves model (Rees \& Haves 2001) since it is a well developed nodal-type model and is implemented in the RP-1222 toolkit. The Rees-Haves model, while successful in predicting the flow and temperature field for geometries similar to those used in its development, can suffer from lack of flexibility and clarity in the modeling approximations. When dealing with diverse geometries it is not clear that the flow coefficients used in the model are applicable or why they can be used since plumes, the fundamental driving mechanisms of the displacement flow, are not explicitly modeled. This is the main difference between the DV models implemented in theRP-1222 toolkit and the model that is described here.
+
+The UCSD DV model is closer to a nodal model than to a zonal model. However, it is best to classify it in a separate category: plume equation based multi-layer models (Linden \emph{et al}. 1990, Morton \emph{et al}. 1956). These models assume that the dominant mechanism is plume-driven flow from discrete internal sources and that other effects (such as buoyancy driven flow at walls or windows) may be neglected. Alternatively, these heat sources also produce plumes that can be included in the model. The result is a zone divided vertically into two or more well separated regions -- each region characterized by a single temperature or temperature profile. This characterization allows the physics of the heat gains and the ventilation flow to be represented in a realistic manner, without the introduction of \emph{ad hoc} assumptions.
+
+\subsubsection{Model Description}\label{model-description-002}
+
+\subsubsection{Single Plume Two Layer Model}\label{single-plume-two-layer-model}
+
+The simplest form of the plume equation based models is the case of a single plume in an adiabatic box with constant supply air flow. For this configuration two layers form in the room: a lower layer with similar density and temperature as the inflow air and a mixed upper layer with the same density / temperature as the outflow air. The main assumption of this model, successfully validated against scaled model experiments (Linden \emph{et al.} 1990), is that the interface between the two layers occurs at the height (h) where the vertical buoyancy driven plume flow rate is the same as the inflow rate. For a point source of buoyancy in a non-stratified environment (a plume) the airflow rate increases with vertical distance from the source according to:
+
+\begin{equation}
+\dot V = C\cdot {B^{1/3}}{z^{5/3}}
+\end{equation}
+
+where
+
+\(\dot V\) = plume volume flux {[}m3/s{]}
+
+\(B\) = buoyancy flux~ {[}m4/s3{]}
+
+\(z\) = vertical distance above source {[}m{]}
+
+\begin{equation}
+C = \frac{6}{5}\alpha {(\frac{9}{{10}}\alpha )^{1/3}}{\pi ^{2/3}}
+\end{equation}
+
+\(\alpha\) = plume entrainment constant; a value of~ 0.127 is used, suitable for top-hat profiles for density and velocity across the plumes.
+
+For an ideal gas
+
+\begin{equation}
+\Delta \rho /\rho  = \Delta {\rm T}/{\rm T}
+\end{equation}
+
+resulting in the following relation between heat input rate and buoyancy flux:
+
+\begin{equation}
+B = \frac{{g\dot Q}}{{\rho {C_p}T}}
+\end{equation}
+
+where
+
+\(\rho\) = density of air {[}kg/m3{]}
+
+\(T\) = air temperature {[}K{]}
+
+\(g\) = acceleration of gravity {[}m/s2{]}
+
+\(\dot Q\) = heat input rate {[}W{]}
+
+\({C_p}\) = specific heat capacity of air {[}J/kgK{]}
+
+Since the plume volume flow rate increases with height with exponent 5/3, for any room inflow rate (F, (m\(^{3}\)/s)) there will always be a height (h,(m)) where the plume driven flow rate matches the inflow rate. This height is obtained by setting (1.1) equal to F and solving for z = h:
+
+\begin{equation}
+h = {F^{3/5}}/({C^{3/5}}{B^{1/5}})
+\end{equation}
+
+Substituting in and introducing air properties at 20 C gives:
+
+\begin{equation}
+h = 24.55\cdot {F^{3/5}}/{\dot Q^{1/5}}
+\end{equation}
+
+\subsubsection{Multiple Plumes and Wall Heat Transfer}\label{multiple-plumes-and-wall-heat-transfer}
+
+Of course, it would be rare for a real world case to consist of a single point-source plume originating on the floor, unaffected by heat gains from walls and windows. For multiple plumes of equal strength a straight-forward extension of the single is possible. N plumes of unequal strength result in the formation of n vertical layers. This case is much more complex but if we are satisfied with a first order precision model the equal strength model can be used by averaging the plume strengths (Carrilho da Graça, 2003). Even in a case where all plumes are of equal strength, nearby plumes may coalesce. Plumes that are less than 0.5 meters apart at their source will coalesce within 2 meters (Kaye \& Linden,2004).
+
+As the complexity of the physical systems modeled increases some limitations must be imposed. In particular, the biggest challenge remains the interaction between wall driven boundary layers (positively and negatively buoyant) and displacement flows. For this reason, the model that is developed below is not applicable when:
+
+1.~~~~Downward moving buoyancy driven airflow rate is of the same order of magnitude as plume driven flow (these airflow currents are typically generated on lateral surfaces or in the ceiling whenever these surfaces are much cooler than the room air).
+
+2.~~~~Upward moving wall or floor generated buoyancy flux in the lower layer is of the same order of magnitude as plume driven flow.
+
+Although these limitations are significant it is important to note that even in the presence of dominant convection from the floor surface, a buoyancy, two layer flow can be established whenever the plume buoyancy flux is more than 1/7 of the horizontal flux (Hunt \emph{et al.} 2002). A two layer structure can also originate when the only heat source is a heated portion of the room floor, as long as the heated area does not exceed 15\% of the room floor (Holford \emph{et al.} 2002).
+
+For the case of multiple non-coalescing plumes (n), with equal strength, the total vertical airflow for a given height is:
+
+\begin{equation}
+  \dot{V} = CnB^{1/3}z^{5/3}
+\end{equation}
+
+resulting in a mixed layer height of:
+
+\begin{equation}
+  h = \frac{24.55F^{3/5}}{{n^3 \dot{Q}}^{1/5}}
+\end{equation}
+
+\subsubsection{Implementation}\label{implementation}
+
+The model predicts three temperatures that characterize the three main levels in the stratification of the room:
+
+1.~~~~a floor level temperature T\(_{floor}\)~to account for the heat transfer from the floor into the supply air
+
+2.~~~~an occupied subzone temperature T\(_{oc}\)~representing the temperature of the occupied region;
+
+3.~~~~an upper level temperature T\(_{mx}\) representing the temperature of the upper, mixed region and the outflow temperature.
+
+We assume that the model for multiple, equal strength plumes (equations and will be adequate for our calculations. The supply air flow rate \(\dot V\) ~is obtained by summing all the air flows entering the zone: supply air, infiltration, ventilation, and inter-zone flow. The heat gain \(\dot Q\) ~is estimated by summing all the convective internal gains located in the occupied subzone -- task lights, people, equipment -- and dividing this power equally among the n plumes. With these assumptions we can describe the implementation.
+
+The UCSD DV model is controlled by the subroutine \emph{ManageUCSDDVModel} which is called from the \emph{RoomAirModelManager}. The \emph{RoomAirModelManager} selects which zone model will be used for each zone.
+
+The calculation is done in subroutine \emph{CalcUCSDDV}. First we calculate the convective heat gain going into the upper and lower regions.
+
+\begin{equation}
+\dot Q_{ocz} = \dot Q_{oc,conv} + \dot Q_{tl,conv} + \dot Q_{eleq,conv} + \dot Q_{gaseq,conv} + \dot Q_{otheq,conv} + \dot Q_{hw,conv} + \dot Q_{stmeq,conv} + \dot Q_{bb,conv}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{mxz}} = {\dot Q_{gl,conv}} + {\dot Q_{ltp}} + {\dot Q_{htrad,conv}}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{tot,conv}} = {\dot Q_{ocz}} + {\dot Q_{mxz}}
+\end{equation}
+
+Next we sum up the inlet air flows in the form of MCP (mass flow rate times the air specific heat capacity) and MCPT (mass flow rate times C\(_{p}\) times air temperature).
+
+\begin{equation}
+MC{P_{zone}} = MC{P_i} + MC{P_{vent}} + MC{P_{mix}}
+\end{equation}
+
+\begin{equation}
+MC{P_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}
+\end{equation}
+
+\begin{equation}
+MC{P_{tot}} = MC{P_{zone}} + MC{P_{sys}}
+\end{equation}
+
+\begin{equation}
+MCP{T_{zone}} = MCP{T_i} + MCP{T_{vent}} + MCP{T_{mix}}
+\end{equation}
+
+\begin{equation}
+MCP{T_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}{T_i}
+\end{equation}
+
+\begin{equation}
+MCP{T_{tot}} = MCP{T_{zone}} + MCP{T_{sys}}
+\end{equation}
+
+The number of plumes per occupant \({N_{plumesperpers}}\) ~is a user input. The total number of plumes in the zone is:
+
+\begin{equation}
+{N_{plumes}} = {N_{occ}} \cdot {N_{plumesperperson}}
+\end{equation}
+
+The gains fraction \(F{r_{gains}}\) is a user input via a schedule. It is the fraction of the convective gains in the occupied subzone that remain in that subzone. Using this we calculate the total power in the plumes and the power per plume.
+
+\begin{equation}
+{\dot Q_{plumes}} = (1 - F{r_{gains}}) \cdot {\dot Q_{tot,conv}}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{perplume}} = {\dot Q_{plumes}}/{N_{plumes}}
+\end{equation}
+
+We now make an initial estimate of the height fraction \emph{Fr\(_{hb}\)} (height of the boundary layer divided by the total zone height).
+
+\begin{equation}
+F{r_{hb}} = \left( {{{24.55} \mathord{\left/ {\vphantom {{24.55} {{H_{ceil}}}}} \right. } {{H_{ceil}}}}} \right){\left( {\frac{{0.000833 \cdot MC{P_{tot}}}}{{{N_{plumes}} \cdot \dot Q_{perplume}^{1/3}}}} \right)^{3/5}}
+\end{equation}
+
+where 0.000833~ = \(1/({\rho_{air}} \cdot {c_{p,air}})\) converts \(MC{P_{tot}}\) ~to a volumetric flow rate. Next we iterate over the following 3 steps.
+
+\subsubsection{Iterative procedure}\label{iterative-procedure}
+
+1.~~~~Call subroutine \emph{HcUCSDDV} to calculate a convective heat transfer coefficient for each surface in the zone, an effective air temperature for each surface, and HA\(_{mx}\), HAT\(_{mx}\), HA\(_{oc}\), HAT\(_{oc}\), HA\(_{fl}\), and HAT\(_{fl}\). Here HA is \(\sum\limits_{surfaces} {{h_{c,i}}} \cdot {A_i}\) ~for a region and HAT is \(\sum\limits_{surfaces} {{h_{c,i}}} \cdot {A_i} \cdot {T_i}\) ~for a region. The sum is over all the surfaces bounding the region; \({h_{c,i}}\) ~is the convective heat transfer coefficient for surface i, \({A_i}\) ~is the area of surface i,~ and \({T_i}\) ~is the surface temperature of surface i.
+
+2.~~~~Recalculate \(F{r_{hb}}\) ~using the equation .
+
+3.~~~~Calculate the three subzone temperatures: \emph{T\(_{floor,}\) T\(_{oc}\)} and \emph{T\(_{mx}\)}.
+
+The h\(_{c}\)'s calculated in step 1 depend on the subzone temperatures and the boundary layer height. In turn the subzone temperatures depend on the HA and HAT's calculated in step 1. Hence the need for iteration
+
+Next we describe each steps 1 and 3 in more detail.
+
+\subsubsection{Step 1}\label{step-1}
+
+Subroutine \emph{HcUCSDDV} is quite straightforward. It loops through all the surfaces in each zone and decides whether the surface is located in the upper, mixed subzone or the lower, occupied subzone, or if the surface is in both subzones. If entirely in one subzone the subzone temperature is stored in the surface effective temperature variable \emph{TempEffBulkAir(SurfNum)} and h\(_{c}\) for the surface is calculated by a call to subroutine \emph{CalcDetailedHcInForDVModel}. This routine uses the ``detailed'' natural convection coefficient calculation that depends on surface tilt and \(\Delta {T^{1/3}}\) . This calculation is appropriate for situations with low air velocity.
+
+For surfaces that bound 2 subzones, the subroutine calculates h\(_{c}\) for each subzone and then averages them, weighting by the amount of surface in each subzone.
+
+During the surface loop, once the h\(_{c}\)~for a surface is calculated, the appropriate subzone HA and HAT sums are incremented. If a surface is in 2 subzones the HA and HAT for each subzone are incremented based on the area of the surface in each subzone.
+
+\subsubsection{Step 3}\label{step-3}
+
+The calculation of~ subzone temperatures follows the method used in the \textbf{\emph{ZoneTempPredictorCorrector}} module and described in the section \textbf{Basis for the System and Zone Integration}. Namely a third order finite difference expansion of the temperature time derivative is used in updating the subzone temperatures. Otherwise the subzone temperatures are obtained straightforwardly by solving an energy balance equation for each subzone.
+
+{\scriptsize
+\begin{equation}
+T_{fl} = (C_{air,fl} \cdot (3 \cdot T_{ - 1,fl} - (3/2) \cdot T_{ - 2,fl} + (1/3) \cdot T_{ - 3,fl}) + HAT_{fl} + MCPT_{tot})  / ((11/6) \cdot C_{air,fl} + HA_{fl} + MCP_{tot})
+\end{equation}}
+
+{\scriptsize
+\begin{equation}
+  \begin{array}{l}
+    T_{oc} = (C_{air,oc} \cdot (3 \cdot T_{ - 1,oc} - (3/2) \cdot T_{ - 2,oc} + (1/3) \cdot T_{ - 3,oc}) + \dot Q_{ocz} \cdot Fr_{gains} + HAT_{oc} + T_{fl} \cdot MCP_{tot}) \\
+    / ((11/6) \cdot C_{air,oc} + HA_{oc} + MCP_{tot})
+\end{array}
+\end{equation}}
+
+{\scriptsize
+\begin{equation}
+  \begin{array}{l}
+    T_{mx} = (C_{air,mx} \cdot (3 \cdot T_{ - 1,mx} - (3/2) \cdot T_{ - 2,mx} + (1/3) \cdot T_{ - 3,mx}) + \dot Q_{ocz} \cdot (1 - Fr_{gains}) + \dot Q_{mxz} + HAT_{mx} + T_{oc} \cdot MCP_{tot}) \\
+    / ((11/6) \cdot C_{air,mx} + HA_{mx} + MCP_{tot})
+  \end{array}
+\end{equation}}
+
+Here \({C_{air,fl}}\) , \({C_{air,oc}}\) , and \({C_{air,mx}}\) ~are the heat capacities of the air volume in each subzone. \({C_{air,mx}}\) ~is calculated by
+
+\begin{equation}
+{R_{air,mx}} = {V_{mx}} \cdot (\Delta {z_{mx}}/{z_{ceil}}) \cdot {\rho_{air,mx}} \cdot {c_{p,air,mx}} \cdot Mu{l_{cap}}/(\Delta {t_z} \cdot 3600)
+\end{equation}
+
+\begin{equation}
+{C_{air,mx}} = {R_{air,mx}} \cdot \Delta {t_z}/\Delta {t_{sys}}
+\end{equation}
+
+The other subzone air heat capacities are calculated in the same manner.
+
+\subsubsection{Mixed calculation}\label{mixed-calculation}
+
+The above iterative procedure assumed that displacement ventilation was taking place: i.e., conditions were favorable temperature stratification in the zone. Now that this calculation is complete and the subzone temperatures and depths calculated, we check to see if this assumption was justified. If not, zone conditions must be recalculated assuming a well-mixed zone.
+
+If \({T_{mx}} < {T_{oc}}\) ~or \(MC{P_{tot}} \le 0\) ~or \({H_{fr}} \cdot {H_{ceil}} < {H_{fl,top}} + \Delta {z_{occ,\min }}\) ~then the following mixed calculation will replace the displacement ventilation calculation.
+
+\textbf{Note:} ~\(\Delta {z_{occ,\min }}\) ~is the minimum thickness of occupied subzone. It is set to 0.2 meters. \({H_{fl,top}}\) is the height of the top of the floor subzone. It is defined to be 0.2 meters; that is, the floor subzone is always 0.2 meters thick and \({T_{fl}}\) ~is the temperature at 0.1 meter above the floor surface.
+
+The mixed calculation iteratively calculates surface convection coefficients and room temperature just like the displacement ventilation calculation described above. In the mixed case however, only one zone temperature \emph{T\(_{avg}\)} is calculated. The 3 subzone temperatures are then set equal to \emph{T\(_{avg}\)}.
+
+First, \emph{Fr\(_{hb}\)}~ is set equal to zero.
+
+Then the code iterates over these steps.
+
+1.~~~~Calculate \emph{T\(_{avg}\)} using
+
+{\scriptsize
+\begin{equation}
+\begin{array}{l}
+T_{avg} = (C_{air,z} \cdot (3 \cdot T_{ - 1,z} - (3/2) \cdot T_{ - 2,z} + (1/3) \cdot T_{ - 3,z}) + \dot Q_{tot,conv} + HAT_{oc} + HAT_{mx} + HAT_{fl} + MCPT_{tot}) \\
+\quad \quad \quad \quad / ((11/6) \cdot C_{air,z} + HA_{oc} + HA_{mx} + HA_{fl} + MCP_{tot})
+\end{array}
+\end{equation}}
+
+\begin{equation}
+{T_{mx}} = {T_{avg}}
+\end{equation}
+
+\begin{equation}
+{T_{oc}} = {T_{avg}}
+\end{equation}
+
+\begin{equation}
+{T_{fl}} = {T_{avg}}
+\end{equation}
+
+2.~~~~Call \emph{HcUCSDDV} to calculate the \emph{h\(_{c}\)}'s.
+
+3.~~~~Repeat step 1
+
+\subsubsection{Final calculations}\label{final-calculations}
+
+The displacement ventilation calculation finishes by calculating some report variables. Using equation , setting the boundary height to 1.5 meters and solving for the flow, we calculate a minimum flow fraction:
+
+\begin{equation}
+{\dot V_{\min }} = {(1.5/{\rm{24}}{\rm{.55)}}^{{\rm{5/3}}}} \cdot {N_{plumes}} \cdot \dot Q_{perplume}^{1/3}
+\end{equation}
+
+\begin{equation}
+F{r_{\min flow}} = .000833 \cdot MC{P_{tot}}/{\dot V_{\min }}
+\end{equation}
+
+We define heights:
+
+\begin{equation}
+{H_{trans}} = F{r_{hb}} \cdot {H_{ceil}}
+\end{equation}
+
+\begin{equation}
+{H_{mxavg}} = ({H_{ceil}} + {H_{trans}})/2
+\end{equation}
+
+\begin{equation}
+{H_{ocavg}} = ({H_{fltop}} + {H_{trans}})/2
+\end{equation}
+
+\begin{equation}
+{H_{flavg}} = {H_{fltop}}/2
+\end{equation}
+
+Using the user defined comfort height we calculate the comfort~ temperature.
+
+If mixing:
+
+\begin{equation}
+{T_{comf}} = {T_{avg}}
+\end{equation}
+
+If displacement ventilation:
+
+If \emph{H\(_{comf}\)} \textless{} \emph{H\(_{flavg}\)}
+
+\begin{equation}
+{T_{comf}} = {T_{fl}}
+\end{equation}
+
+Else if \({H_{comf}} \ge {H_{flavg}}\) ~and \({H_{comf}} < {H_{ocavg}}\)
+
+\begin{equation}
+{T_{comf}} = ({T_{fl}}({H_{ocavg}} - {H_{comf}}) + {T_{mx}}({H_{comf}} - {H_{flavg}})/({H_{ocavg}} - {H_{flavg}})
+\end{equation}
+
+Else if \({H_{comf}} \ge {H_{ocavg}}\) ~and \({H_{comf}} < {H_{mxavg}}\)
+
+\begin{equation}
+{T_{comf}} = ({T_{oc}}({H_{mxavg}} - {H_{comf}}) + {T_{mx}}({H_{comf}} - {H_{ocavg}})/({H_{mxavg}} - {H_{ocavg}})
+\end{equation}
+
+Else if \({H_{comf}} \ge {H_{mxavg}}\) ~and \({H_{comf}} < {H_{ceil}}\)
+
+\begin{equation}
+{T_{comf}} = {T_{mx}}
+\end{equation}
+
+Using the user defined thermostat height we calculate the temperature at the thermostat.
+
+If mixing:
+
+\begin{equation}
+{T_{stat}} = {T_{avg}}
+\end{equation}
+
+If displacement ventilation:
+
+If \emph{H\(_{stat}\)} \textless{} \emph{H\(_{flavg}\)}
+
+\begin{equation}
+{T_{stat}} = {T_{fl}}
+\end{equation}
+
+Else if \({H_{stat}} \ge {H_{flavg}}\) ~and \({H_{stat}} < {H_{ocavg}}\)
+
+\begin{equation}
+{T_{stat}} = ({T_{fl}}({H_{ocavg}} - {H_{stat}}) + {T_{mx}}({H_{stat}} - {H_{flavg}})/({H_{ocavg}} - {H_{flavg}})
+\end{equation}
+
+Else if \({H_{stat}} \ge {H_{ocavg}}\) ~and \({H_{stat}} < {H_{mxavg}}\)
+
+\begin{equation}
+{T_{stat}} = ({T_{oc}}({H_{mxavg}} - {H_{stat}}) + {T_{mx}}({H_{stat}} - {H_{ocavg}})/({H_{mxavg}} - {H_{ocavg}})
+\end{equation}
+
+Else if \({H_{stat}} \ge {H_{mxavg}}\) ~and \({H_{stat}} < {H_{ceil}}\)
+
+\begin{equation}
+{T_{stat}} = {T_{mx}}
+\end{equation}
+
+The average temperature gradient is:
+
+If \({H_{mxavg}} - {H_{flavg}} > 0.1\)
+
+\begin{equation}
+Grad{T_{avg}} = ({T_{mx}} - {T_{fl}})/({H_{mxavg}} - {H_{flavg}})
+\end{equation}
+
+else \[Grad{T_{avg}} =  - 9.999\]
+
+The maximum temperature gradient is:
+
+If~ \({H_{ocavg}} - {H_{flavg}} > 0.1\)
+
+\begin{equation}
+Grad{T_{\max ,1}} = ({T_{oc}} - {T_{fl}})/({H_{ocavg}} - {H_{flavg}})
+\end{equation}
+
+else \(Grad{T_{\max ,1}} = - 9.999\)
+
+If~ \({H_{mxavg}} - {H_{ocavg}} > 0.1\)
+
+\begin{equation}
+Grad{T_{\max ,2}} = ({T_{mx}} - {T_{oc}})/({H_{mxavg}} - {H_{ocavg}})
+\end{equation}
+
+else \(Grad{T_{\max ,2}} = - 9.999\) and
+
+\begin{equation}
+Grad{T_{\max }} = \max (Grad{T_{\max ,1}},Grad{T_{\max ,2}})
+\end{equation}
+
+For reporting purposes, if the zone is deemed to be mixed, the displacement ventilation report variables are set to flag values.
+
+If \({T_{mx}} < {T_{oc}}\) ~or \(MC{P_{tot}} \le 0\) ~or \({H_{fr}} \cdot {H_{ceil}} < {H_{fl,top}} + \Delta {z_{occ,\min }}\) ~or \({T_{mx}} - {T_{oc}} < \Delta {T_{Crit{\mathop{\rm Re}\nolimits} p}}\)
+
+\begin{equation}
+Grad{T_{avg}} =  - 9.999
+\end{equation}
+
+\begin{equation}
+Grad{T_{\max }} =  - 9.999
+\end{equation}
+
+\begin{equation}
+F{R_{\min ,flow}} =  - 1.0
+\end{equation}
+
+\begin{equation}
+{H_{trans}} =  - 9.999
+\end{equation}
+
+Finally, the zone node temperature is set to \emph{T\(_{mx}\)}.
+
+\subsubsection{References}\label{references-2-000}
+
+Carrilho da Graca, G. 2003. Simplified models for heat transfer in rooms. Ph. D. Thesis, University of California, San Diego.
+
+Chen, Q., and B. Griffith. 2002. Incorporating Nodal Room Air Models into Building Energy Calculation Procedures. ASHRAE RP-1222 Final Report.
+
+Cooper, P. and P.F. Linden. 1996. Natural ventilation of an enclosure containing two buoyancy sources. Journal of Fluid Mechanics, Vol. 311, pp.~153-176.
+
+Dominique, M. and P. Guitton. 1997.~ Validation of displacement ventilation simplified models. Proc. of Building Simulation.
+
+Holford, J.M., G.R. Hunt and P.F. Linden. 2002. Competition between heat sources in a ventilated space. Proceedings of RoomVent 2002, pp.~577-580.
+
+Hunt, G.R., J.M. Holford and P.F. Linden. 2002. Characterization of the flow driven by a finite area heat source in a ventilated enclosure. Proceedings of RoomVent 2002, pp.~ 581-584.
+
+Hunt, G.R. and P.F. Linden.~ 2001. Steady-state flows in an enclosure ventilated by buoyancy forces assisted by wind. . Journal of Fluid Mechanics, Vol. 426,~ pp.~355-386.
+
+Kaye, K.N. and P.F. Linden.~ 2004. Coalescing axisymmetric turbulent plumes\emph{.} Journal of Fluid Mechanics, ~Vol. 502, pp.~41--63.
+
+Linden, P.F., G.F. Lane-Serff and D.A. Smeed. 1990. Emptying filling boxes: the fluid mechanics of natural ventilation. Journal of Fluid Mechanics, Vol. 212, pp.~309-335.
+
+Linden, P.F. and P. Cooper. 1996. Multiple sources of buoyancy in a naturally ventilated enclosure. Journal of Fluid Mechanics, Vol. 311, pp.~177-192.
+
+Morton, B.R., G.I. Taylor andJ.S. Turner. 1956. Turbulent gravitational convection from maintained and instantaneous sources. Proceedings of the Royal Society of London, Vol A234, pp.~1-23.
+
+Mundt, E. 1996. The Performance of Displacement Ventilation Systems -- Experimental and Theoretical Studies, Ph. D. Thesis, Bulletin N38, Building Services Engineering KTH, Stockholm.
+
+Rees, S.J., and P. Haves. 2001. A nodal model for displacement ventilation and chilled ceiling systems in office spaces. Building and Environment, Vol. 26, pp.~753-762.
+
+\subsection{Under-Floor Air Distribution Interior Zone Model}\label{under-floor-air-distribution-interior-zone-model}
+
+\subsubsection{Overview}\label{overview-1-001}
+
+The input object RoomAirSettings:UnderFloorAirDistributionInterior provides a simple model for heat transfer and nonuniform vertical temperature profile for interior zones of a UFAD system. These zones are expected to be dominated by internal loads, a portion of which (such as occupants and workstations) will act to generate plumes. The plumes act to potentially create room air stratification, depending on the type \& number of diffusers, the amount and type of load, and the system flowrate. In order to better model this situation the fully-mixed room air approximation that is currently used in most whole building analysis tools is extended to a two node approach, with the purpose of obtaining a first order precision model for vertical temperature profiles for the interior zones of UFAD systems. The use of 2 nodes allows for greatly improved prediction of thermal comfort and overall building energy performance for the increasingly popular UFAD systems.
+
+TheUCSD UFAD Interior Zone Model is one of the non-uniform zone models provided through the Room Air Manager in EnergyPlus. The intent is to provide a selection of useful non-uniform zone air models to enable the evaluation of air-conditioning techniques that use stratified or partially stratified room air. Such techniques include displacement ventilation (DV) and underfloor air distribution (UFAD) systems. The methodology can also include natural displacement ventilation and also wind-driven cross-ventilation (CV).
+
+\subsubsection{Underfloor air distribution systems}\label{underfloor-air-distribution-systems}
+
+UFAD systems represent, in terms of room air stratification, an intermediate condition between a well-mixed zone and displacement ventilation. Air is supplied through an underfloor plenum at low pressure through diffusers in the raised floor. The diffusers can be of various types: e.g., swirl, variable-area, displacement, and produce more or less mixing in the zone. UFAD systems are promoted as saving energy due to: higher supply air temperature; low static pressure; cooler conditions in the occupied subzone than in the upper subzone; and sweeping of some portion of the convective load (from ceiling lights, for instance) into the return air without interaction with the occupied region of the zone.
+
+Modeling a UFAD system is quite complex and involves considerably more than just a non-uniform zone model. The zones' coupling to the supply and return plenums must be modeled accurately (particularly radiative transfer from a warm ceiling to a cool floor and on into the supply plenum by conduction). The supply plenum must be accurately modeled, giving a good estimate of the supply air temperature and conduction heat transfer between supply \& return plenums through the slab. The HVAC system must be modeled including return air bypass and various types of fan powered terminal units.
+
+The UCSD UFAD interior zone model is similar to the UCSD DV model. The most obvious difference is that the UFAD model has no separate near-floor subzone. Like the UCSD DV model it is a plume equation based multi-layer model (2 layers in this case). The zone is modeled as being divided into 2 well separated subzones which we denote as ``occupied'' and ``upper''. Each subzone is treated as having a single temperature. The boundary between the 2 subzones moves up \& down each time step as a function of zone loads and supply air flow rate. Thus at each HVAC time step, the height of the boundary above the floor must be calculated, portions of surfaces assigned to each subzone, and a separate convective heat balance performed on each subzone.
+
+\subsubsection{Model Description}\label{model-description-1-001}
+
+The UFAD interior zone model is based upon non-dimensional analysis of the system and using the non-dimensional description to make a comparison between full-scale UCB test chamber data \& small-scale UCSD salt tank measurements.
+
+In order to do the non-dimensional comparisons, we need to define two dimensionless parameters. One is \(\Gamma\) , and the other is \(\phi\) . Lin \& Linden (Lin \& Linden, 2005) showed that in a UFAD system, the buoyancy flux of the heat source \((B)\) and the momentum flux of the cooling jets \((M)\) are the controlling parameters on the stratification. Since \([B] = {L^4}{T^{ - 3}}\) and\([M] = {L^4}{T^{ - 2}}\) , we can have a length scale as \({M^{3/4}}/{B^{1/2}}\) .
+
+\emph{Definition of} \emph{Gfor the single-plume single-diffuser basic model}
+
+We observed, in our small-scale experiments, that the total room height does not affect the interface position, or the height of the occupied zone. In other words, \emph{H} might not be the critical length scale for the stratification. Therefore, we started to use \(\sqrt A\) ~as the reference length. Then \(\Gamma\) is defined as
+
+\begin{equation}
+\Gamma  = \frac{{{M^{3/4}}}}{{{B^{1/2}}{A^{1/2}}}} = \frac{{{{({Q^2}/A)}^{3/4}}}}{{{B^{1/2}}{A^{1/2}}}} = \frac{{{Q^{3/2}}}}{{{A^{5/4}}{B^{1/2}}}}
+\end{equation}
+
+\emph{Definition for multi-diffuser and multi-source cases}
+
+We only considered single-diffuser, single-source cases in above analysis. Suppose there are \emph{n} equal diffusers and \emph{m} equal heat sources in a UFAD room. We shall divide the number of diffusers up into a number of separate heat sources so that each subsection with \emph{n' = n/m} diffusers per heat source will have the same stratification as other subsections. Further, the air flow and the heat load into the subsection \emph{Q'} and \emph{B'} will be\(Q' = Q/m\) \(B' = B/m\) respectively, where \emph{Q'} and \emph{B'} are the total air flow and the total heat load for the entire UFAD space. Then the momentum flux each diffuser per heat source carries is\({M_d} = {(\frac{1}{{n'}}Q')^2}/A\) . will be modified as
+
+\begin{equation}
+\Gamma  = \frac{{{{(n'{M_d})}^{3/4}}}}{{B{'^{1/2}}\sqrt {n'A} }} = \frac{{Q{'^{3/2}}}}{{{{(n'A)}^{5/4}}B{'^{1/2}}}} = \frac{{{Q^{3/2}}}}{{m{{(n'A)}^{5/4}}{B^{1/2}}}}
+\end{equation}
+
+\emph{Full-scale cases}
+
+Because \emph{B} is the buoyancy flux of the heat sources and \emph{M} is the momentum flux of the cooling jets, in a real full-scale room, we shall consider the total room net heat load (plume heat input, minus the room losses) and the total net flow rate coming from the diffusers (input room air flow, minus the room leakage). Further, if the diffuser is swirl type, the vertical momentum flux should be used.
+
+\begin{equation}
+\Gamma  = \frac{{{{(Q\cos \theta )}^{3/2}}}}{{m{{(n'A)}^{5/4}}{{(0.0281W)}^{1/2}}}}
+\end{equation}
+
+where, \emph{Q} is the net flow rate coming out from all diffusers (m\(^{3}\)/s); \emph{W} is the total net heat load (kW); \emph{A} is the effective area of each diffuser (m\(^{2}\)); \emph{n'} is the number of diffusers per heat source; \emph{q} is the angle between the diffuser slots and the vertical direction and \emph{m} is the number of heat sources
+
+\emph{Definition of} \emph{F}
+
+In our theoretical model, two-layer stratification forms at steady state, provided that each diffuser carries the same momentum flux, and each heat source has the same heat load. We could define a dimensionless parameter \emph{F}, which indicates the strength of stratification.
+
+\emph{Small-scale cases}
+
+In our salt-water tank experiments, fluid density \emph{r} is measured. Define that
+
+\begin{equation}
+\phi  = \frac{{{\rho_u} - {\rho_l}}}{{{\rho_u} - {\rho_o}}}
+\end{equation}
+
+where, \emph{r\(_{u}\)} and \emph{r\(_{l}\)} are the fluid density of the upper layer and lower layer, separately; and \emph{r\(_{o}\)} is the source density at the diffusers.
+
+Therefore, \emph{r\(_{l}\)} = \emph{r\(_{o}\)} gives \emph{f} = \emph{1}, which means the largest stratification (displacement ventilation case); \emph{r\(_{l}\)} = \emph{r\(_{u}\)} leads to \emph{f} = \emph{0}, in which case there is no stratification (mixed ventilation case).
+
+\emph{Full-scale cases}
+
+Similarly, we can define \emph{f} for full-scale cases by using temperature.
+
+\begin{equation}
+\phi  = \frac{{{T_r} - {T_{oz}}}}{{{T_r} - {T_s}}}
+\end{equation}
+
+where \emph{T\(_{r}\)}, \emph{T\(_{oz}\)}, and \emph{T\(_{s}\)} are the return air temperature, the occupied zone temperature and the supply temperature, respectively (K). Again \emph{f = 1} occurs in displacement ventilation; while \emph{f = 0} happens in mixed ventilation.
+
+\emph{Comparisons between full-scale UCB data and small-scale UCSD data}
+
+\begin{figure}[hbtp] % fig 133
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2469.png}
+\caption{Data comparisons in the non-dimensional (a) regular G-fplot \protect \label{fig:data-comparisons-in-the-non-dimensional-a}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 134
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2470.png}
+\caption{(b) log-log G-fplot.\} \protect \label{fig:b-log-log-g-fplot.}}
+\end{figure}
+
+The figures (Figure~\ref{fig:data-comparisons-in-the-non-dimensional-a}. Data comparisons in the non-dimensional (a) regular G-fplot and Figure~\ref{fig:b-log-log-g-fplot.}. (b) log-log G-fplot.\} show the comparisons between UCB's data and the UCSD salt tank data in the \emph{G-f} plot. As seen in the figures, the full-scale and small-scale data are on the same trend curve. This provides the evidence that the salt-tank experiments have included most characteristics of a UFAD system. Note that big \emph{G} (\textgreater{}20) of UCB's experiments all have large DDR (from \emph{1.19} to \emph{2.18}). The largest DDR (\emph{2.18}) even gives a negative\(({T_r} - {T_{oz}})/({T_r} - {T_s})\) , which is NOT shown in the figures.)
+
+We could work out the occupied zone temperature by using the least-square fitting line suggested in Figure~\ref{fig:energyplus-program-schematic}(b). Hence the interface height is needed to determine a entire two-layer stratification. Figure~\ref{fig:non-dimensional-interface-height-of-small} shows the dimensionless interface height\((h/\sqrt {n'A} )\) of the UCSD small-scale experiments plotted against \emph{G}. Note that for the experiments with elevated heat source, the interface heights have been modified by\(h' = h - \frac{1}{2}{h_s}\) ~where \emph{h\(_{s}\)} is the vertical position of the elevated heat source. All data then are located along a line in Figure~\ref{fig:non-dimensional-interface-height-of-small}. Since the salt-tank experiments are concluded to represent important characteristics of a full-scale UFAD room, this figure provides some guidelines for estimate the interface position in a real UFAD room.
+
+\begin{figure}[hbtp] % fig 135
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2474.png}
+\caption{Non-dimensional interface height of small-scale experiments. \protect \label{fig:non-dimensional-interface-height-of-small}}
+\end{figure}
+
+\emph{Formulas for EnergyPlus based on the dimensionless parameter} \emph{G}
+
+If we have input including the supply temperature \emph{T\(_{s}\)} (K); the number of diffusers \emph{n}; the number of heat sources \emph{m}; the vertical position of the heat sources \emph{h\(_{s}\)} (m); the heat load \emph{W} (kW); the effective area of a diffuser \emph{A} (m\(^{2}\)); and the total supply air flow rate \emph{Q} (m\(^{3}\)/s) then the output will be
+
+\begin{equation}
+{T_r} = \frac{{0.0281W}}{{Qg}}{T_s} + {T_s}
+\end{equation}
+
+\begin{equation}
+{T_{oz}} = {T_r} - 1.6{\Gamma ^{ - 0.76}}({T_r} - {T_s})
+\end{equation}
+
+\begin{equation}
+h = \sqrt {\frac{n}{m}A} (7.43ln(\Gamma ) - 1.35) + \frac{1}{2}{h_s}
+\end{equation}
+
+where \emph{T\(_{r}\)} is the return temperature (K); \emph{T\(_{oz}\)} is the occupied subzone temperature (K); \emph{h} is the interface height (m); and \emph{G} is defined above.
+
+\subsubsection{Implementation}\label{implementation-1}
+
+The implementation closely follows the procedure described in the displacement ventilation zone model. The model predicts two temperatures that characterize the two main levels in the stratification of the room:
+
+1.~~~~an occupied subzone temperature T\(_{oc}\)~representing the temperature of the occupied region;
+
+2.~~~~an upper level temperature T\(_{mx}\) representing the temperature of the upper, mixed region and the outflow temperature.
+
+We will use to calculate the interface height and do a heat balance calculation on each subzone. \emph{G} is given by . The supply air flow rate \(\dot V\) ~is obtained by summing all the air flows entering the zone: supply air, infiltration, ventilation, and inter-zone flow. The heat gain \(\dot Q\) ~is estimated by summing all the convective internal gains located in the occupied subzone -- task lights, people, equipment -- and dividing this power equally among the n plumes. With these assumptions we can describe the implementation.
+
+The UCSD UFI model is controlled by the subroutine \emph{ManageUCSDUFModels} which is called from the \emph{RoomAirModelManager}. The \emph{RoomAirModelManager} selects which zone model will be used for each zone.
+
+The calculation is done in subroutine \emph{CalcUCSDUI}. First we calculate the convective heat gain going into the upper and lower regions.
+
+\begin{equation}
+\begin{split}
+\dot Q_{ocz} =& \dot Q_{oc,conv} + \dot Q_{tl,conv} + \dot Q_{eleq,conv} + \dot Q_{gaseq,conv} + \dot Q_{otheq,conv} + \dot Q_{hw,conv} + \dot Q_{stmeq,conv} \\
+&+ \dot Q_{bb,conv} + \dot Q_{waterheater,conv} + \dot Q_{fuelcell,conv}
+\end{split}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{mxz}} = {\dot Q_{gl,conv}} + {\dot Q_{ltp}} + {\dot Q_{htrad,conv}}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{tot,conv}} = {\dot Q_{ocz}} + {\dot Q_{mxz}}
+\end{equation}
+
+Next we sum up the inlet air flows in the form of MCP (mass flow rate times the air specific heat capacity) and MCPT (mass flow rate times C\(_{p}\) times air temperature).
+
+\begin{equation}
+MC{P_{zone}} = MC{P_i} + MC{P_{vent}} + MC{P_{mix}}
+\end{equation}
+
+\begin{equation}
+MC{P_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{systot}} = \sum\limits_{inlets} {{{\dot m}_i}}
+\end{equation}
+
+\begin{equation}
+MC{P_{tot}} = MC{P_{zone}} + MC{P_{sys}}
+\end{equation}
+
+\begin{equation}
+MCP{T_{zone}} = MCP{T_i} + MCP{T_{vent}} + MCP{T_{mix}}
+\end{equation}
+
+\begin{equation}
+MCP{T_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}{T_i}
+\end{equation}
+
+\begin{equation}
+MCP{T_{tot}} = MCP{T_{zone}} + MCP{T_{sys}}
+\end{equation}
+
+The number of plumes per occupant \({N_{plumesperpers}}\) ~is a user input. The total number of plumes in the zone is:
+
+\begin{equation}
+{N_{plumes}} = {N_{occ}} \cdot {N_{plumesperperson}}
+\end{equation}
+
+Using this we calculate the total power in the plumes and the power per plume.
+
+\begin{equation}
+{\dot Q_{plumes}} = {\dot Q_{ocz}}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{perplume}} = {\dot Q_{plumes}}/{N_{plumes}}
+\end{equation}
+
+The number of diffusers per plumes is also a user input. To obtain the number of diffusers in the zone:
+
+\begin{equation}
+{N_{diffusers}} = {N_{plumes}}\cdot {N_{diffusersperplume}}
+\end{equation}
+
+The area \emph{A\(_{diff}\)} is also a user input. For swirl diffusers and for displacement diffusers this area is used as input. For the variable area diffusers, though, we calculate the area. We assume 400 ft/min velocity at the diffuser and a design flow rate per diffuser is 150 cfm (.0708 m\(^{3}\)/s). The design area of the diffuser is 150 ft\(^{3}\)/min /~ 400 ft/min = .575 ft\(^{2}\) = .035 m\(^{2}\). Then the variable area each time step is
+
+\begin{equation}
+{A_{diff}} = {\dot m_{systot}}/(.0708\cdot {N_{diffusers}})
+\end{equation}
+
+We now calculate the height fraction \emph{Fr\(_{hb}\)} (height of boundary layer divided by the total zone height).
+
+\begin{equation}
+\Gamma  = \frac{{{{({{\dot m}_{systot}}\cdot \cos ({\theta_{throw}}))}^{3/2}}}}{{{N_{plumes}}{{({N_{diffusersperplume}}\cdot {A_{diff}})}^{5/4}}{{(0.0281\cdot 0.001\cdot {{\dot Q}_{plumes}})}^{1/2}}}}
+\end{equation}
+
+\begin{equation}
+F{r_{hb}} = \frac{{{{({N_{diffusersperplume}}\cdot {A_{diff}})}^{1/2}}(7.43\ln (\Gamma ) - 1.35 + 0.5{H_s})}}{{{H_{ceil}}}}
+\end{equation}
+
+where \emph{q\(_{throw}\)} is a user input: the angle between the diffuser slots and vertical; and \emph{H\(_{s}\)} is the source height above the floor (m).
+
+Next we iterate over the following 2 steps.
+
+\subsubsection{Iterative procedure}\label{iterative-procedure-1}
+
+1.~~~~Call subroutine \emph{HcUCSDUF} to calculate a convective heat transfer coefficient for each surface in the zone, an effective air temperature for each surface, and HA\(_{mx}\), HAT\(_{mx}\), HA\(_{oc}\), HAT\(_{oc}\). Here HA is \(\sum\limits_{surfaces} {{h_{c,i}} \cdot {A_i}}\) ~for a region and HAT is \(\sum\limits_{surfaces} {{h_{c,i}} \cdot {A_i}} \cdot {T_i}\) ~for a region. The sum is over all the surfaces bounding the region; \({{h_{c,i}}}\) ~is the convective heat transfer coefficient for surface i, \({A_i}\) ~is the area of surface i,~ and \({T_i}\) ~is the surface temperature of surface i.
+
+2.~~~~Calculate the two subzone temperatures: \emph{T\(_{oc}\)} and \emph{T\(_{mx}\)}.
+
+The h\(_{c}\)'s calculated in step 1 depend on the subzone temperatures. In turn the subzone temperatures depend on the HA and HAT's calculated in step 1. Hence the need for iteration
+
+Next we describe each steps 1 and 2 in more detail.
+
+\subsubsection{Step 1}\label{step-1-1}
+
+Subroutine \emph{HcUCSDUF} is quite straightforward. It loops through all the surfaces in each zone and decides whether the surface is located in the upper, mixed subzone or the lower, occupied subzone, or if the surface is in both subzones. If entirely in one subzone the subzone temperature is stored in the surface effective temperature variable \emph{TempEffBulkAir(SurfNum)} and h\(_{c}\) for the surface is calculated by a call to subroutine \emph{CalcDetailedHcInForDVModel}. This routine uses the ``detailed'' natural convection coefficient calculation that depends on surface tilt and \(\Delta {T^{1/3}}\) . This calculation is appropriate for situations with low air velocity.
+
+For surfaces that bound 2 subzones, the subroutine calculates h\(_{c}\) for each subzone and then averages them, weighting by the amount of surface in each subzone.
+
+During the surface loop, once the h\(_{c}\)~for a surface is calculated, the appropriate subzone HA and HAT sums are incremented. If a surface is in 2 subzones the HA and HAT for each subzone are incremented based on the area of the surface in each subzone.
+
+\subsubsection{Step 2}\label{step-2}
+
+The calculation of~ subzone temperatures follows the method used in the \textbf{\emph{ZoneTempPredictorCorrector}} module and described in the section \textbf{Basis for the System and Zone Integration}. Namely a third order finite difference expansion of the temperature time derivative is used in updating the subzone temperatures. Otherwise the subzone temperatures are obtained straightforwardly by solving an energy balance equation for each subzone.
+
+\begin{equation}
+  \begin{array}{cl}
+    T_{oc} & = \frac{(C_{air,oc} \cdot (3 \cdot T_{ - 1,oc} - (3/2) \cdot T_{ - 2,oc} + (1/3) \cdot T_{ - 3,oc}) + \dot Q_{ocz} \cdot Fr_{gains} + HAT_{oc} + MCPT_{tot})} {((11/6) \cdot C_{air,oc} + HA_{oc} + MCP_{tot})} \\
+    T_{mx} & = \frac{(C_{air,mx} \cdot (3 \cdot T_{ - 1,mx} - (3/2) \cdot T_{ - 2,mx} + (1/3) \cdot T_{ - 3,mx}) + \dot Q_{ocz} \cdot (1 - Fr_{gains}) + \dot Q_{mxz} + HAT_{mx} + T_{oc} \cdot MCP_{tot})} {((11/6) \cdot C_{air,mx} + HA_{mx} + MCP_{tot})}
+  \end{array}
+\end{equation}
+
+Here \({C_{air,oc}}\) ~and \({C_{air,mx}}\) ~are the heat capacities of the air volume in each subzone. \({C_{air,mx}}\) ~is calculated by
+
+\begin{equation}
+{R_{air,mx}} = {V_{mx}} \cdot \left( {\Delta {z_{mx}}/{z_{ceil}}} \right) \cdot {\rho_{air,mx}} \cdot {c_{p,air,mx}} \cdot Mu{l_{cap}}/\left( {\Delta {t_z} \cdot 3600} \right)
+\end{equation}
+
+\begin{equation}
+{c_{air,mx}} = {R_{air,mx}} \cdot \Delta {t_z}/\Delta {t_{sys}}
+\end{equation}
+
+The gains fraction \(F{r_{gains}}\) is a user input via a schedule. It is the fraction of the convective gains in the occupied subzone that remain in that subzone.
+
+The other subzone air heat capacities are calculated in the same manner.
+
+\subsubsection{Mixed calculation}\label{mixed-calculation-1}
+
+The above iterative procedure assumed that the UFAD nonuniform zone model was appropriate: i.e., conditions were favorable temperature stratification in the zone. Now that this calculation is complete and the subzone temperatures and depths calculated, we check to see if this assumption was justified. If not, zone conditions must be recalculated assuming a well-mixed zone.
+
+If \({T_{mx}} < {T_{oc}}\) ~or \(MC{P_{tot}} \le 0\) ~or \({H_{fr}} \cdot {H_{ceil}} < \Delta {z_{occ,\min }}\) ~then the following mixed calculation will replace the UFAD interior zone calculation.
+
+\textbf{Note:} ~\(\Delta {z_{occ,min}}\) ~is the minimum thickness of occupied subzone. It is set to 0.2 meters.
+
+The mixed calculation iteratively calculates surface convection coefficients and room temperature just like the displacement ventilation calculation described above. In the mixed case however, only one zone temperature \emph{T\(_{avg}\)} is calculated. The 3 subzone temperatures are then set equal to \emph{T\(_{avg}\)}.
+
+First, \emph{Fr\(_{hb}\)}~ is set equal to zero.
+
+Then the code iterates over these steps.
+
+Calculate \emph{T\(_{avg}\)} using
+
+\begin{equation}
+  \begin{array}{rl}
+    T_{avg} &= ({C_{air,z}} \cdot (3 \cdot {T_{ - 1,z}} - (3/2) \cdot {T_{ - 2,z}} + (1/3) \cdot {T_{ - 3,z}}) \\
+            &+ {{\dot Q}_{tot,conv}} + HA{T_{oc}} + HA{T_{mx}}MCP{T_{tot}})/((11/6) \cdot {C_{air,z}} + H{A_{oc}} + H{A_{mx}} + MC{P_{tot}})
+  \end{array}
+\end{equation}
+
+\begin{equation}
+{T_{mx}} = {T_{avg}}
+\end{equation}
+
+\begin{equation}
+{T_{oc}} = {T_{avg}}
+\end{equation}
+
+Call \emph{HcUCSDUF} to calculate the \emph{h\(_{c}\)}'s.
+
+Repeat step 1
+
+\subsubsection{Final calculations}\label{final-calculations-1}
+
+The UFAD interior zone calculation finishes by calculating some report variables.
+
+We define heights:
+
+\begin{equation}
+{H_{trans}} = F{r_{hb}} \cdot {H_{ceil}}
+\end{equation}
+
+\begin{equation}
+{H_{mxavg}} = \left( {{H_{ceil}} + {H_{trans}}} \right)/2
+\end{equation}
+
+\begin{equation}
+{H_{ocavg}} = {H_{trans}}/2
+\end{equation}
+
+Using the user defined comfort height we calculate the comfort~ temperature.
+
+If mixing:
+
+\begin{equation}
+{T_{comf}} = {T_{avg}}
+\end{equation}
+
+If UFAD:
+
+If~ \({H_{comf}} < {H_{ocavg}}\)
+
+\begin{equation}
+{T_{comf}} = {T_{occ}}
+\end{equation}
+
+Else if \({H_{comf}} \ge {H_{ocavg}}\) ~and \({H_{comf}} < {H_{mxavg}}\)
+
+\begin{equation}
+{T_{comf}} = \left( {{T_{oc}}\left( {{H_{mxavg}} - {H_{comf}}} \right) + {T_{mx}}\left( {{H_{comf}} - {H_{ocavg}}} \right)} \right)/\left( {{H_{mxavg}} - {H_{ocavg}}} \right)
+\end{equation}
+
+Else if \({H_{comf}} \ge {H_{mxavg}}\) ~and \({H_{comf}} < {H_{ceil}}\)
+
+\begin{equation}
+{T_{comf}} < {T_{mx}}
+\end{equation}
+
+Using the user defined thermostat height we calculate the temperature at the thermostat.
+
+If mixing:
+
+\begin{equation}
+{T_{stat}} < {T_{avg}}
+\end{equation}
+
+If UFAD:
+
+If\({H_{stat}} < {H_{ocavg}}\)
+
+\begin{equation}
+{T_{stat}} = {T_{occ}}
+\end{equation}
+
+Else if \({H_{stat}} \ge {H_{ocavg}}\) ~and \({H_{stat}} < {H_{mxavg}}\)
+
+\begin{equation}
+{T_{stat}} = \left( {{T_{oc}}\left( {{H_{mxavg}} - {H_{stat}}} \right) + {T_{mx}}\left( {{H_{stat}} - {H_{ocavg}}} \right)} \right)/\left( {{H_{mxavg}} - {H_{ocavg}}} \right)
+\end{equation}
+
+Else if \({H_{stat}} \ge {H_{mxavg}}\) ~and \({H_{stat}} < {H_{ceil}}\)
+
+\begin{equation}
+{T_{stat}} = {T_{mx}}
+\end{equation}
+
+The average temperature gradient is:
+
+If \({H_{mxavg}} - {H_{occavg}} > 0.1\)
+
+\begin{equation}
+Grad{T_{avg}} = ({T_{mx}} - {T_{occ}})/({H_{mxavg}} - {H_{occavg}})
+\end{equation}
+
+else \(Grad{T_{avg}} = 0.0\)
+
+Finally, the zone node temperature is set to \emph{T\(_{mx}\)}.
+
+Other variables that are reported out are \(\Gamma\) and \(\phi\) .
+
+\begin{equation}
+\phi  = ({T_{mx}} - {T_{occ}})/({T_{mx}} - {T_{sup}})
+\end{equation}
+
+where \({T_{sup}}\) is the zone supply air temperature.
+
+\subsubsection{References}\label{references-3-000}
+
+Lin, Y.J. and P.F. Linden. 2005. A model for an under floor air distribution system. Energy\&Building, Vol. 37, pp.~399-409.
+
+\subsection{Under-Floor Air Distribution Exterior Zone Model}\label{under-floor-air-distribution-exterior-zone-model}
+
+\subsubsection{Overview}\label{overview-2-001}
+
+The input object RoomAirSettings:UnderFloorAirDistributionExterior provides a simple model for heat transfer and a nonuniform vertical temperature profile for exterior zones of a UFAD system. These zones are expected to be dominated by internal loads, a portion of which (such as occupants and workstations) will act to generate plumes, and by window solar and conduction heat gains. The solar radiation penetrating the room is not expected to generate plumes. However, a window plume is likely to be generated in sunny conditions, particularly if an interior blind is deployed. Thus the exterior UFAD zone will have potentially have plumes from people and equipment and plumes arising from the windows. The plumes act to potentially create room air stratification, depending on the type \& number of diffusers, the amount and type of load, and the system flowrate. In order to better model this situation the fully-mixed room air approximation that is currently used in most whole building analysis tools is extended to a two node approach, with the purpose of obtaining a first order precision model for vertical temperature profiles for the exterior zones of UFAD systems. The use of 2 nodes allows for greatly improved prediction of thermal comfort and overall building energy performance for the increasingly popular UFAD systems.
+
+TheUCSD UFAD Exterior Zone Model is one of the non-uniform zone models provided through the Room Air Manager in EnergyPlus. The intent is to provide a selection of useful non-uniform zone air models to enable the evaluation of air-conditioning techniques that use stratified or partially stratified room air. Such techniques include displacement ventilation (DV) and underfloor air distribution (UFAD) systems. The methodology can also include natural displacement ventilation and also wind-driven cross-ventilation (CV).
+
+\subsubsection{Underfloor air distribution systems}\label{underfloor-air-distribution-systems-1}
+
+UFAD systems represent, in terms of room air stratification, an intermediate condition between a well-mixed zone and displacement ventilation. Air is supplied through an underfloor plenum at low pressure through diffusers in the raised floor. The diffusers can be of various types: e.g., swirl, variable-area, displacement, and produce more or less mixing in the zone. UFAD systems are promoted as saving energy due to: higher supply air temperature; low static pressure; cooler conditions in the occupied subzone than in the upper subzone; and sweeping of some portion of the convective load (from ceiling lights, for instance) into the return air without interaction with the occupied region of the zone.
+
+Modeling a UFAD system is quite complex and involves considerably more than just a non-uniform zone model. The zones' coupling to the supply and return plenums must be modeled accurately (particularly radiative transfer from a warm ceiling to a cool floor and on into the supply plenum by conduction). The supply plenum must be accurately modeled, giving a good estimate of the supply air temperature and conduction heat transfer between supply \& return plenums through the slab. The HVAC system must be modeled including return air bypass and various types of fan powered terminal units.
+
+The UCSD UFAD exterior zone model is similar to the UCSD interior zone model. The most obvious difference is that the exterior UFAD has 2 different types of plume sources: people \& equipment and windows. Like the UCSD UFAD interior model it is a plume equation based multi-layer model (2 layers in this case). The zone is modeled as being divided into 2 well separated subzones which we denote as ``occupied'' and ``upper''. Each subzone is treated as having a single temperature. The boundary between the 2 subzones moves up \& down each time step as a function of zone loads and supply air flow rate. Thus at each HVAC time step, the height of the boundary above the floor must be calculated, portions of surfaces assigned to each subzone, and a separate convective heat balance performed on each subzone.
+
+\subsubsection{Model Description}\label{model-description-2-001}
+
+As in the interior zone case, we define 2 dimensionless parameters: \(\Gamma\) and \(\phi\) . The definitions of the 2 parameters are the same as in the previous section (equations , , , , and ). As in the previous case, the experimental data can be plotted versus \(\Gamma\) and lines fitted to the data give the following formulas for occupied subzone temperature and interface height.
+
+\begin{equation}
+{T_{oz}} = {T_r} - 1.4{\Gamma ^{ - 0.6}}({T_r} - {T_s})
+\end{equation}
+
+\begin{equation}
+h = \sqrt {\frac{n}{m}A} (11.03ln(\Gamma ) - 10.73) + \frac{1}{2}{h_s}
+\end{equation}
+
+where \emph{T\(_{oz}\)} is the occupied subzone temperature (K); \emph{T\(_{r}\)}~is the return temperature (K); \emph{G}~is the dimensionless height parameter defined above; \emph{T\(_{s}\)} is the supply temperature (K); \emph{h} is the interface height (m); \emph{n} is the number of diffusers; \emph{m} is the number of heat sources; \emph{A} is the effective area of a diffuser (m\(^{2}\)); and \emph{h\(_{s}\)} is the vertical position of the heat sources (m). The formula for \emph{T\(_{r}\)} is the same as in the previous section.
+
+\subsubsection{Implementation}\label{implementation-2}
+
+The implementation closely follows the procedure described in the UFAD interior zone model. The model predicts two temperatures that characterize the two main levels in the stratification of the room:
+
+1.~~~~an occupied subzone temperature T\(_{oc}\)~representing the temperature of the occupied region;
+
+2.~~~~an upper level temperature T\(_{mx}\) representing the temperature of the upper, mixed region and the outflow temperature.
+
+We will use to calculate the interface height and do a heat balance calculation on each subzone. \emph{G} is given by . The supply air flow rate \(\dot V\) ~is obtained by summing all the air flows entering the zone: supply air, infiltration, ventilation, and inter-zone flow. The heat gain \(\dot Q\) ~is estimated by summing all the convective internal gains located in the occupied subzone -- task lights, people, equipment -- and adding to this the convective gain coming from the window surface. With these assumptions we can describe the implementation.
+
+The UCSD UFE model is controlled by the subroutine \emph{ManageUCSDUFModels} which is called from the \emph{RoomAirModelManager}. The \emph{RoomAirModelManager} selects which zone model will be used for each zone.
+
+The calculation is done in subroutine \emph{CalcUCSDUEI}. First we calculate the convective heat gain going into the upper and lower regions.
+
+\begin{equation}
+\begin{split}
+\dot Q_{ocz} =& \dot Q_{oc,conv} + \dot Q_{tl,conv} + \dot Q_{eleq,conv} + \dot Q_{gaseq,conv} + \dot Q_{otheq,conv} + \dot Q_{hw,conv} + \dot Q_{stmeq,conv} \\
+&+ \dot Q_{bb,conv} + \dot Q_{waterheater,conv} + \dot Q_{fuelcell,conv}
+\end{split}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{mxz}} = {\dot Q_{gl,conv}} + {\dot Q_{ltp}} + {\dot Q_{htrad,conv}}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{tot,conv}} = {\dot Q_{ocz}} + {\dot Q_{mxz}}
+\end{equation}
+
+Next we sum up the inlet air flows in the form of MCP (mass flow rate times the air specific heat capacity) and MCPT (mass flow rate times C\(_{p}\) times air temperature).
+
+\begin{equation}
+MC{P_{zone}} = MC{P_i} + MC{P_{vent}} + MC{P_{mix}}
+\end{equation}
+
+\begin{equation}
+MC{P_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{systot}} = \sum\limits_{inlets} {{{\dot m}_i}}
+\end{equation}
+
+\begin{equation}
+MC{P_{tot}} = MC{P_{zone}} + MC{P_{sys}}
+\end{equation}
+
+\begin{equation}
+MCP{T_{zone}} = MCP{T_i} + MCP{T_{vent}} + MCP{T_{mix}}
+\end{equation}
+
+\begin{equation}
+MCP{T_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}{T_i}
+\end{equation}
+
+\begin{equation}
+MCP{T_{tot}} = MCP{T_{zone}} + MCP{T_{sys}}
+\end{equation}
+
+For exterior zone model, we assume one plume: \({N_{plumes}} = 1\) . The number of diffusers in the zone \({N_{diffusers}}\) is a user input.
+
+The area \emph{A\(_{diff}\)} is also a user input. For swirl diffusers, linear bar grilles, and displacement diffusers this area is used as input. For the variable area diffusers, though, we calculate the area. We assume 400 ft/min velocity at the diffuser and a design flow rate per diffuser is 150 cfm (.0708 m\(^{3}\)/s). The design area of the diffuser is 150 ft\(^{3}\)/min /~ 400 ft/min = .575 ft\(^{2}\) = .035 m\(^{2}\). Then the variable area each time step is
+
+\begin{equation}
+{A_{diff}} = {\dot m_{systot}}/(.0708\cdot {N_{diffusers}})
+\end{equation}
+
+We now make an initial estimate of the convective gain from the windows.
+
+\begin{equation}
+{\dot Q_{win,conv}} = \sum\limits_{i = 1,{n_{win}}} {{h_{c,i}}} {A_{win,i}}{T_{winsurf,i}} - {h_{c,i}}{A_{win,i}}{T_{mat}}
+\end{equation}
+
+Then
+
+\begin{equation}
+{\dot Q_{plumes}} = {\dot Q_{ocz}} + {\dot Q_{win,conv}}
+\end{equation}
+
+We now calculate the height fraction \emph{Fr\(_{hb}\)} (height of boundary layer divided by the total zone height).
+
+\begin{equation}
+\Gamma  = \frac{{{{({{\dot m}_{systot}}\cdot \cos ({\theta_{throw}}))}^{3/2}}}}{{{{({N_{diffusers}}\cdot {A_{diff}})}^{5/4}}{{(0.0281\cdot 0.001\cdot {{\dot Q}_{plumes}})}^{1/2}}}}
+\end{equation}
+
+\begin{equation}
+F{r_{hb}} = \frac{{{{({N_{diffusers}}\cdot {A_{diff}})}^{1/2}}(11.03ln(\Gamma ) - 10.73 + 0.5{H_s})}}{{{H_{ceil}}}}
+\end{equation}
+
+where \emph{q\(_{throw}\)} is a user input: the angle between the diffuser slots and vertical; and \emph{H\(_{s}\)} is the source height above the floor (m).
+
+Next we iterate over the following 2 steps.
+
+\subsubsection{Iterative procedure}\label{iterative-procedure-2}
+
+1.~~~~Call subroutine \emph{HcUCSDUF} to calculate a convective heat transfer coefficient for each surface in the zone, an effective air temperature for each surface, and HA\(_{mx}\), HAT\(_{mx}\), HA\(_{oc}\), HAT\(_{oc}\), HA\(_{mx,win}\),HAT\(_{mx,win}\),HA\(_{oc,win}\),and HAT\(_{oc,win}\). Here HA is \(\sum\limits_{surfaces} {{h_{c,i}} \cdot {A_i}}\) ~for a region and HAT is \(\sum\limits_{surfaces} {{h_{c,i}} \cdot {A_i}} \cdot {T_i}\) ~for a region. The sum is over all the surfaces bounding the region; \({h_{c,i}}\) ~is the convective heat transfer coefficient for surface i, \({A_i}\) ~is the area of surface i,~ and \({T_i}\) ~is the surface temperature of surface i. Variables with the \emph{win} subscript are summed over window surfaces only. Then the convective gain from the window is recalculated:
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \({\dot Q_{win,conv}} = HA{T_{mx,win}} + HA{T_{oc,win}} - H{A_{mx,win}}{T_{mx}} - H{A_{oc,win}}{T_{oc}}\)
+
+and the power in the plume is recalculated: \({\dot Q_{plumes}} = {\dot Q_{ocz}} + {\dot Q_{win,conv}}\) .
+
+2.~~~~Calculate the two subzone temperatures: \emph{T\(_{oc}\)} and \emph{T\(_{mx}\)}.
+
+The h\(_{c}\)'s calculated in step 1 depend on the subzone temperatures. In turn the subzone temperatures depend on the HA and HAT's calculated in step 1. Hence the need for iteration
+
+Next we describe each steps 1 and 3 in more detail.
+
+\subsubsection{Step 1}\label{step-1-2}
+
+Subroutine \emph{HcUCSDUF} is quite straightforward. It loops through all the surfaces in each zone and decides whether the surface is located in the upper, mixed subzone or the lower, occupied subzone, or if the surface is in both subzones. If entirely in one subzone the subzone temperature is stored in the surface effective temperature variable \emph{TempEffBulkAir(SurfNum)} and h\(_{c}\) for the surface is calculated by a call to subroutine \emph{CalcDetailedHcInForDVModel}. This routine uses the ``detailed'' natural convection coefficient calculation that depends on surface tilt and \(\Delta {T^{1/3}}\) . This calculation is appropriate for situations with low air velocity.
+
+For surfaces that bound 2 subzones, the subroutine calculates h\(_{c}\) for each subzone and then averages them, weighting by the amount of surface in each subzone.
+
+During the surface loop, once the h\(_{c}\)~for a surface is calculated, the appropriate subzone HA and HAT sums are incremented. If a surface is in 2 subzones the HA and HAT for each subzone are incremented based on the area of the surface in each subzone. The subroutine calculates a separate HA and HAT for the windows for use in calculating the window convective gain.
+
+\subsubsection{Step 2}\label{step-2-1}
+
+The calculation of~ subzone temperatures follows the method used in the \textbf{\emph{ZoneTempPredictorCorrector}} module and described in the section \textbf{Basis for the System and Zone Integration}. Namely a third order finite difference expansion of the temperature time derivative is used in updating the subzone temperatures. Otherwise the subzone temperatures are obtained straightforwardly by solving an energy balance equation for each subzone.
+
+\begin{equation}
+  \begin{array}{cl}
+    T_{oc} & = \frac{(C_{air,oc} \cdot (3 \cdot T_{ - 1,oc} - (3/2) \cdot T_{ - 2,oc} + (1/3) \cdot T_{ - 3,oc}) + \dot Q_{ocz} \cdot Fr_{gains} + HAT_{oc} + MCPT_{tot})} {((11/6) \cdot C_{air,oc} + HA_{oc} + MCP_{tot})} \\
+    T_{mx} & = \frac{(C_{air,mx} \cdot (3 \cdot T_{ - 1,mx} - (3/2) \cdot T_{ - 2,mx} + (1/3) \cdot T_{ - 3,mx}) + \dot Q_{ocz} \cdot (1 - Fr_{gains}) + \dot Q_{mxz} + HAT_{mx} + T_{oc} \cdot MCP_{tot})} {((11/6) \cdot C_{air,mx} + HA_{mx} + MCP_{tot})}
+  \end{array}
+\end{equation}
+
+Here \({C_{air,oc}}\) ~and \({C_{air,mx}}\) ~are the heat capacities of the air volume in each subzone. \({C_{air,mx}}\) ~is calculated by
+
+\begin{equation}
+{R_{air,mx}} = {V_{mx}} \cdot \left( {\Delta {z_{mx}}/{z_{ceil}}} \right) \cdot {\rho_{air,mx}} \cdot {c_{p,air,mx}} \cdot Mu{l_{cap}}/\left( {\Delta {t_z} \cdot 3600} \right)
+\end{equation}
+
+\begin{equation}
+{c_{air,mx}} = {R_{air,mx}} \cdot \Delta {t_z}/\Delta {t_{sys}}
+\end{equation}
+
+The gains fraction \(F{r_{gains}}\) is a user input via a schedule. It is the fraction of the convective gains in the occupied subzone that remain in that subzone.
+
+The other subzone air heat capacities are calculated in the same manner.
+
+\subsubsection{Mixed calculation}\label{mixed-calculation-2}
+
+The above iterative procedure assumed that the UFAD zone model was applicable: i.e., conditions were favorable temperature stratification in the zone. Now that this calculation is complete and the subzone temperatures and depths calculated, we check to see if this assumption was justified. If not, zone conditions must be recalculated assuming a well-mixed zone.
+
+If \({T_{mx}} < {T_{oc}}\) ~or \(MC{P_{tot}} \le 0\) ~or \({H_{fr}} \cdot {H_{ceil}} < \Delta {z_{occ,\min }}\) ~then the following mixed calculation will replace the UFAD exterior zone calculation.
+
+\textbf{Note:} ~\({\Delta_{occ,min}}\) ~is the minimum thickness of occupied subzone. It is set to 0.2 meters.
+
+The mixed calculation iteratively calculates surface convection coefficients and room temperature just like the displacement ventilation calculation described above. In the mixed case however, only one zone temperature \emph{T\(_{avg}\)} is calculated. The 2 subzone temperatures are then set equal to \emph{T\(_{avg}\)}.
+
+First, \emph{Fr\(_{hb}\)}~ is set equal to zero.
+
+Then the code iterates over these steps.
+
+Calculate \emph{T\(_{avg}\)} using
+
+\begin{equation}
+  \begin{array}{rl}
+    T_{avg} &= ({C_{air,z}} \cdot (3 \cdot {T_{ - 1,z}} - (3/2) \cdot {T_{ - 2,z}} + (1/3) \cdot {T_{ - 3,z}}) \\
+            &+ {{\dot Q}_{tot,conv}} + HA{T_{oc}} + HA{T_{mx}}MCP{T_{tot}})/((11/6) \cdot {C_{air,z}} + H{A_{oc}} + H{A_{mx}} + MC{P_{tot}})
+  \end{array}
+\end{equation}
+
+\begin{equation}
+{T_{mx}} = {T_{avg}}
+\end{equation}
+
+\begin{equation}
+{T_{oc}} = {T_{avg}}
+\end{equation}
+
+Call \emph{HcUCSDUF} to calculate the \emph{h\(_{c}\)}'s.
+
+Repeat step 1
+
+\subsubsection{Final calculations}\label{final-calculations-2}
+
+The UFAD exterior zone calculation finishes by calculating some report variables.
+
+We define heights:
+
+\begin{equation}
+{H_{trans}} = F{r_{hb}} \cdot {H_{ceil}}
+\end{equation}
+
+\begin{equation}
+{H_{mxavg}} = \left( {{H_{ceil}} + {H_{trans}}} \right)/2
+\end{equation}
+
+\begin{equation}
+{H_{ocavg}} = {H_{trans}}/2
+\end{equation}
+
+Using the user defined comfort height we calculate the comfort~ temperature.
+
+If mixing:
+
+\begin{equation}
+{T_{comf}} = {T_{avg}}
+\end{equation}
+
+If UFAD:
+
+If~ \({H_{comf}} < {H_{ocavg}}\)
+
+\begin{equation}
+{T_{comf}} = {T_{occ}}
+\end{equation}
+
+Else if \({H_{comf}} \ge {H_{ocavg}}\) ~and \({H_{comf}} < {H_{mxavg}}\)
+
+\begin{equation}
+{T_{comf}} = \left( {{T_{oc}}\left( {{H_{mxavg}} - {H_{comf}}} \right) + {T_{mx}}\left( {{H_{comf}} - {H_{ocavg}}} \right)} \right)/\left( {{H_{mxavg}} - {H_{ocavg}}} \right)
+\end{equation}
+
+Else if \({H_{comf}} \ge {H_{mxavg}}\) ~and \({H_{comf}} < {H_{ceil}}\)
+
+\begin{equation}
+{T_{comf}} < {T_{mx}}
+\end{equation}
+
+Using the user defined thermostat height we calculate the temperature at the thermostat.
+
+If mixing:
+
+\begin{equation}
+{T_{stat}} = {T_{avg}}
+\end{equation}
+
+If UFAD:
+
+If\({H_{stat}} < {H_{ocavg}}\)
+
+\begin{equation}
+{T_{stat}} = {T_{occ}}
+\end{equation}
+
+Else if \({H_{stat}} \ge {H_{ocavg}}\) ~and \({H_{stat}} < {H_{mcavg}}\)
+
+\begin{equation}
+{T_{stat}} = \left( {{T_{oc}}\left( {{H_{mxavg}} - {H_{stat}}} \right) + {T_{mx}}\left( {{H_{stat}} - {H_{ocavg}}} \right)} \right)/\left( {{H_{mxavg}} - {H_{ocavg}}} \right)
+\end{equation}
+
+Else if \({H_{stat}} \ge {H_{mxavg}}\) ~and \({H_{stat}} < {H_{ceil}}\)
+
+\begin{equation}
+{T_{stat}} = {T_{mx}}
+\end{equation}
+
+The average temperature gradient is:
+
+If \({H_{mxavg}} - {H_{occavg}} > 0.1\)
+
+\begin{equation}
+Grad{T_{avg}} = ({T_{mx}} - {T_{occ}})/({H_{mxavg}} - {H_{occavg}})
+\end{equation}
+
+else \(Grad{T_{avg}} = 0.0\)
+
+Finally, the zone node temperature is set to \emph{T\(_{mx}\)}.
+
+Other variables that are reported out are \(\Gamma\) and \(\phi\) .
+
+\begin{equation}
+\phi  = ({T_{mx}} - {T_{occ}})/({T_{mx}} - {T_{sup}})
+\end{equation}
+
+where \({T_{sup}}\) is the zone supply air temperature.
+
+\subsubsection{References}\label{references-4-000}
+
+Qing Liu. 2006. The Fluid Dynamics of an Underfloor Air Distribution System. A PhD dissertation in Engineering Sciences (Systems Science) at UC San Diego.
+
+\subsection{Cross Ventilation Room Air Model}\label{cross-ventilation-room-air-model}
+
+\subsubsection{Overview}\label{overview-3-001}
+
+The input object RoomAirSettings:CrossVentilation provides a simple model, developed by UCSD, for heat transfer and vertical temperature profile prediction in cross ventilated rooms. This model was developed using scaling analysis, experimental correlations, computational fluid dynamics, and approximate solutions of the Navier-Stokes equations. The model distinguishes two regions in the room, the main jet region and the recirculations, and predicts characteristic airflow velocities and average air temperatures. The model consists of a set of analytical expressions that clearly display the first order effects of room geometry and inflow characteristics on Cross Ventilation airflow and heat transfer.
+
+\subsubsection{Cross-Ventilation}\label{cross-ventilation}
+
+The CV model is developed from analysis of the flow structure inside a cross-ventilated room, which naturally divides into distinct jet and recirculation flow regions. The flows are calculated for different room and opening geometries using CFD. Correlations with room and aperture parameters are then deduced for a characteristic temperature and velocity in the jet and recirculation regions.
+
+The SS 2-opening model is developed from analysis of wind tunnel data for pressure and ventilation rates, correlating the flow rate with the pressure difference between the two openings, with contributions from both the mean and unsteady components. The local velocity estimate is also based on wind tunnel data, and gives the velocity as a function of wind angle.
+
+\subsubsection{Approach}\label{approach}
+
+With the widespread availability of air conditioning, natural ventilation became a rare feature in commercial buildings in the US. The recent resurgence of the use of natural ventilation relies on systems whose performance can be predicted and controlled, often working in conjunction with mechanical ventilation and cooling systems in hybrid ventilation configurations. In this contemporary approach natural ventilation deals with thermal and air renewal requirements in the cold and mild season and often plays a limited role in the warm season (due to the need to control indoor velocities and noise levels). Whereas traditional natural ventilation systems often use large openings (1-4m\(^{2}\)), both recent and expected future examples tend to use smaller openings (0.2-1m\(^{2}\)), often in multiple opening configurations that allow for efficient heat removal with controlled indoor velocities.
+
+The modeling approach used is based on simplified solutions of the Navier Stokes equations that are integrated into scaling formulae that predict relevant flow quantities (characteristic velocities and temperatures) in distinct regions of the flow. The scaling expressions that will be developed use the principle of flow similarity: for a given room geometry and flow regime (either laminar or turbulent), the flow pattern is constant. In the present case, where the goal is to predict internal velocities using as input the inflow velocity (that can be estimated by the airflow rate predicted by the AirflowNetwork model), the principle can be stated as:
+
+(Velocity in a given position in the room) = (Inflow velocity) × (Constant)
+
+The constant is non-dimensional and depends on the position or room zone where the prediction is being made. For a given geometry the constant can be measured experimentally or inferred from a detailed CFD simulation. It is expected that the constant may depend on non-dimensional room geometry parameters that can be inferred from a careful analysis of the flow. The proposed CV model uses a set of CFD simulations, in conjunction with simplified solutions of the Navier Stokes equations, to obtain the constants and their dependence on room geometry features.
+
+The updated CV model proposed in this document was developed using inlet areas \emph{A}\(_{in}\) and room cross-section areas \emph{A}\(_{RM}\) in the following range:
+
+0.5\%~\textless{}~\emph{A}\(_{in}\)/\emph{A}\(_{RM}\)~\textless{}~5\%
+
+whereas the existing model used
+
+3.2\%~\textless{}~\emph{A}\(_{in}\)/\emph{A}\(_{RM}\)~\textless{}~21\%
+
+The room lengths for which these models are expected to be applied range between the smallest room size of 4m and the maximum achievable CV room flushing length of 15-18m.
+
+\begin{figure}[hbtp] % fig 136
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2622.png}
+\caption{Development of an axisymmetric jet from airflow through a window. \protect \label{fig:development-of-an-axisymmetric-jet-from}}
+\end{figure}
+
+Air flows into the room through an inflow window in the form of an approximately axisymmetric jet, with characteristic diameter \emph{L} = \emph{A}\(_{in}\)\(^{1/2}\), that is confined by the room surfaces (see Figure~\ref{fig:top-view-of-a-cross-ventilated-room.-the-air}). The initial portion of the jet (up to six diameters) is called the potential core and is characterized by shear layer development along the perimeter of the jet. After this phase the jet transitions into a self similar profile whose centerline velocity decays as 1/\emph{x}`, where \emph{x}' = \emph{x}/\emph{D} (Awbi, 2003).
+
+For the relevant room length range the geometries used in the two models result in:
+
+~~~~~ New model:~~~~~~ 6~\textless{}~x'~\textless{}~60
+
+~~~~~ Existing model: ~~~~~~~~~~~ 2~\textless{}~x'~\textless{}~18
+
+The smaller openings used in the new model result in significantly more space for jet development along the room length. In all but the shortest rooms the jet will enter the fully developed stage characterized by a 1/\emph{x}' centerline velocity decay rate. For this reason, the updated model uses the average jet velocity profile as opposed to shear layer momentum transfer.
+
+\subsubsection{Components of the flow}\label{components-of-the-flow}
+
+Figure~\ref{fig:development-of-an-axisymmetric-jet-from} shows the schematic development of a free axisymmetric jet in an unconfined environment, and Figure~\ref{fig:top-view-of-a-cross-ventilated-room.-the-air} depicts the confinement effects. The air entrained by the jet is detrained at the outlet, creating two recirculation zones that do not exist in a free jet.
+
+The recirculation flow is similar to the flow in a lid driven cavity, where here the driving force is the confined jet flow. Turbulent lid driven cavity flows have been shown to have self-similar velocity profiles, as shown in Figure~\ref{fig:top-view-of-one-half-of-a-cross-ventilated}.
+
+The model is based on the hypothesis that the flow is composed of:
+
+~~~~~ A -- Lid driven cavity flows (in the recirculation regions).
+
+~~~~~ B -- A confined axisymmetric jet flow.
+
+\begin{figure}[hbtp] % fig 137
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2623.png}
+\caption{Top view of a cross ventilated room. The air entrained by the jet is detrained at the outlet, typically creating two recirculation zones. \protect \label{fig:top-view-of-a-cross-ventilated-room.-the-air}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 138
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2624.png}
+\caption{Top view of one half of a cross ventilated room. The flow is approximately composed of a confined jet and two lid driven cavity flows (one on each side). \protect \label{fig:top-view-of-one-half-of-a-cross-ventilated}}
+\end{figure}
+
+The goal of the model is to obtain the value and functional form of the constant term shown in the scaling laws for the characteristic average velocities in the two flow regions: jet and recirculation regions.
+
+To estimate the average jet velocity we integrate along the depth of the room (including both the core region and the 1/\emph{x}' velocity decay region) to derive an average maximum jet velocity, \emph{V}\(_{J,m}\):∙
+
+\begin{equation}
+{V_{J,m}} = {U_{in}}\sqrt {{A_{in}}} \left\{ {6 + 6.3\ln \left( {{D^*}/6\sqrt {{A_{in}}} } \right)} \right\}/{D^*}
+\end{equation}
+
+(To allow for wind angle effects the room depth \emph{D} has been replaced by \emph{D}* - see a later section.) The lid-driven cavity flow profile that characterizes the recirculation region has a maximum velocity that is approximately one half of the driving velocity, which in this case is due to the jet. For this reason we define the separation between the two regions along the virtual surface where the jet reaches 50\% of its maximum, centerline, velocity.
+
+The analysis of the flow revealed that the room containment effect leads to higher velocities for cases that combine a large inflow opening with a small room cross-section area. In order to account for this effect we propose to use the following non-dimensional scaling parameter:
+
+\begin{equation}
+{C_{RM}} = {\left( {{A_{in}}/{A_{RM}}} \right)^{1/2}}
+\end{equation}
+
+The expression used for the scaling of the average jet velocity is then:
+
+\begin{equation}
+{U_J} = {C_1}{C_{RM}}{V_{J,m}}
+\end{equation}
+
+or
+
+\begin{equation}
+{U_J} = {C_1}\frac{{{Q_{in}}}}{{\sqrt {{A_{in}}{A_{RM}}} }}\left( {{V_{J,m}}/{U_{in}}} \right)
+\end{equation}
+
+where the constant \emph{C}\(_{1}\) will be obtained from the results of a set of CFD simulations shown in the next section.
+
+In addition to the jet velocity the characteristic recirculation flow velocity \({U_R}\) ~is also an interesting parameter that, according to the self-similar flow profile hypothesis shown in Figure~\ref{fig:top-view-of-one-half-of-a-cross-ventilated}, should scale with a similar expression to the one shown above for the jet (although with a different correlation constant, \emph{C}\(_{2}\)). The modeling hypothesis can also be tested by evaluating its capability to predict the maximum recirculation flow rate, which can be predicted by multiplying the average velocity by the room cross-section area:
+
+\begin{equation}
+{Q_R} = {C_3}\frac{{{Q_{in}}}}{{{C_{RM}}}}\left( {{V_{J,m}}/{U_{in}}} \right)
+\end{equation}
+
+Because of the self-similar velocity profile shape that occurs in the recirculation, the near wall velocity (used to predict forced convection) can be estimated simply by multiplying the characteristic recirculation velocity by two.
+
+The expressions obtained apply in the turbulent regime (because the CFD simulations on which they are based are for that regime). Both velocity correlations presented below have the functional form:
+
+\begin{equation}
+V = aX + b
+\end{equation}
+
+where \emph{a} is \emph{C}\(_{1}\), \emph{C}\(_{2}\) or \emph{C}\(_{3}\), X is a velocity scale and \emph{b} is a constant that results from the best fit. The model has a lower limit on the value of \emph{X}: if \emph{X} is too small the flow is no longer turbulent. This limit implies that the point \emph{X}~ = ~0 is never achieved, avoiding the unrealistic prediction of \emph{V}(0) = \emph{b}.
+
+In addition to the velocity and airflow rate predictions described above it is also essential to predict the temperature variations in the two zones of the flow. In most cases these variations will be positive due to the internal sensible heat gains. However`, as a result of room surface heat transfer, in some cases the variations may be negative. Analysis of the CFD simulations that are presented in the next section revealed that approximately all the exhaust air comes from the jet regions. For this reason, the heat gains affect the two regions differently:
+
+·~~~~~~~~Heat gains in the jet region only affect this region (no temperature increase in the recirculation regions)
+
+·~~~~~~~~Heat gains in the recirculations affect both jet and recirculation regions (because they must be exhausted by the jets).
+
+In order to predict the temperature increase, heat gains were inserted into the recirculation regions for different room geometries in the set of simulations presented in the next section. The volume containing the heat gains extended over the whole depth of the room, from floor to ceiling, and in the lateral direction from halfway between the window edge and the wall all the way to the wall. Applying energy conservation principles to predict the temperature increase in the jet and recirculation region as a function of the sensible heat gains in each region (the sum of internal gains and internal surface heat transfer) we can obtain the average value of temperature increase in each region:
+
+\begin{equation}
+\Delta {T_J} = {C_{T,J}}\frac{{q'{'_{RM}}}}{{\rho {c_p}{Q_{in}}}}
+\end{equation}
+
+\begin{equation}
+\Delta {T_R} = {C_{T,R}}\frac{{q'{'_{RM}}}}{{\rho {c_p}{Q_{in}}}}
+\end{equation}
+
+where q''\(_{RM}\) is the total internal heat gain for the room, r and \emph{c}\(_{p}\) are the density and specific heat capacity of air, respectively, and \emph{C}\(_{T,J}\), \emph{C}\(_{T,R}\) are constants.
+
+\subsubsection{Results}\label{results}
+
+Table~\ref{table:test-cases-used-to-develop-correlations} lists the cases used to develop the updated CV model, which predicts the output variables defined in Table~\ref{table:definitions-of-output-variables} (see also Figure~\ref{fig:jet-and-recirculation-regions-in-typical}). Figure 140, Figure 141, and Figure 142 show plots of the data derived from the CFD simulations of these test cases, and the lines giving the best fit to the data. Table~\ref{table:correlation-formulae-in-the-form-y-ax-+-b} summarizes the correlation formulae and constants. Finally, Table~\ref{table:accuracy-of-correlation-formulae-in} provides estimates for the error of the correlation in each test case.
+
+\begin{figure}[hbtp] % fig 139
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2634.png}
+\caption{Jet and recirculation regions in typical vertical cross-section through room (y-z plane). Jet boundary occurs where jet velocity has fallen to 50\% of centerline maximum. Remainder of cross-section is treated as recirculation. Volumetric heat sources ar \protect \label{fig:jet-and-recirculation-regions-in-typical}}
+\end{figure}
+
+% table 44
+\begin{longtable}[c]{@{}lllll@{}}
+\caption{Test cases used to develop correlations \label{table:test-cases-used-to-develop-correlations}} \tabularnewline
+\toprule 
+Case & Opening area & Room width & Room depth & Room height \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Test cases used to develop correlations} \tabularnewline
+\toprule 
+Case & Opening area & Room width & Room depth & Room height \tabularnewline
+\midrule
+\endhead
+
+A in (m 2 ) & W (m) & D (m) & H (m) \tabularnewline
+1 & 0.25 & 6 & 9 & 2.3 \tabularnewline
+2 & 0.25 & 11 & 9 & 2.3 \tabularnewline
+3 & 0.5 & 9 & 4.5 & 2.3 \tabularnewline
+4 & 0.5 & 9 & 6 & 2.3 \tabularnewline
+5 & 0.5 & 6 & 9 & 2.3 \tabularnewline
+6 & 0.5 & 9 & 9 & 2.3 \tabularnewline
+7 & 0.5 & 11 & 9 & 2.3 \tabularnewline
+8 & 0.5 & 13.5 & 9 & 2.3 \tabularnewline
+9 & 0.5 & 9 & 13.5 & 2.3 \tabularnewline
+10 & 0.5 & 9 & 18 & 2.3 \tabularnewline
+11 & 0.5 & 13.5 & 18 & 2.3 \tabularnewline
+12 & 1 & 9 & 9 & 2.3 \tabularnewline
+13 & 1 & 9 & 13.5 & 2.3 \tabularnewline
+14 & 1 & 9 & 18 & 2.3 \tabularnewline
+RANGE (max:min ratio) \tabularnewline
+ & 4 & 2.25 & 4 & 1 \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 45
+\begin{longtable}[c]{p{1.25in}p{0.5in}p{0.5in}p{3.0in}}
+\caption{Definitions of output variables \label{table:definitions-of-output-variables}} \tabularnewline
+\toprule 
+Output variable & Symbol & Units & Definition \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Definitions of output variables} \tabularnewline
+\toprule 
+Output variable & Symbol & Units & Definition \tabularnewline
+\midrule
+\endhead
+Jet velocity & U\(_J\) & m/s & Volume-averaged jet region velocity. The averaging volume is bounded at each x along the room depth by the line in the y-z plane where the jet velocity drops to 50\% of its maximum centerline value. \tabularnewline
+Recirculation zone velocity & U\(_R\) & m/s & Area-averaged velocity in the y-z plane with maximum flow. The averaging area is the recirculation part of the room cross-section. Typically the plane of maximum flow occurs at x~\textbackslash\~{}~2D/3 (D/3 before the outlet). \tabularnewline
+Recirculation zone flow rate & Q\(_R\) & m  /s & Total flow rate for the recirculation regions in the plane of maximum flow (see above). \tabularnewline
+Jet temperature rise & $\Delta$T\(_J\) & °C & Volume-averaged temperature variations in the jet region, over the same volume used to define the jet velocity average. \tabularnewline
+Recirculation zone temperature rise & $\Delta$T\(_R\) & °C & Volume-average temperature variations in the recirculation region. The average is calculated over the cuboidal volume placed in each recirculation containing the volumetric sensible heat gains (see main text). \tabularnewline
+\bottomrule
+\end{longtable}
+
+See also Figure~\ref{fig:jet-and-recirculation-regions-in-typical}. Note the \emph{x}-coordinate is along the room, the \emph{y}-coordinate is across the room and the \emph{z}-coordinate is vertical.
+
+% table 46
+\begin{longtable}[c]{p{1.0in}p{0.5in}p{2.0in}p{0.5in}p{0.5in}p{0.5in}}
+\caption{Correlation formulae in the form Y = aX + b \label{table:correlation-formulae-in-the-form-y-ax-+-b}} \tabularnewline
+\toprule 
+~ & Y & X & a & b & R\(^2\) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Correlation formulae in the form Y = aX + b} \tabularnewline
+\toprule 
+~ & Y & X & a & b & R\(^2\) \tabularnewline
+\midrule
+\endhead
+Jet velocity & U\(_J\)/U\(_{in}\) & $\sqrt{A_{in}/A_{RM}} \cdot \left(V_{J,m}/U_{in}\right)$ & 1.6173 & 0.1466 & 0.8343 \tabularnewline
+Recirculation zone velocity & U\(_R\)/U\(_{in}\) & $\sqrt{A_{in}/A_{RM}} \cdot \left(V_{J,m}/U_{in}\right)$ & 0.8911 & 0.0393 & 0.6464 \tabularnewline
+Recirculation zone flow rate & Q\(_R\)/U\(_{in}\) & $\sqrt{A_{in}/A_{RM}} \cdot \left(V_{J,m}/U_{in}\right)$ & 0.4444 & 0.1751 & 0.6761 \tabularnewline
+Jet temperature rise & $\Delta$T\(_J\) & $\frac{q''_{RM}}{\rho {c_p}{Q_{in}}}$ & 0.8254 & 0 & n/a \tabularnewline
+Recirculation zone temperature rise & $\Delta$T\(_R\) & $\frac{q''_{RM}}{\rho {c_p}{Q_{in}}}$ & 1.2734 & 0 & n/a \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 47
+\begin{longtable}[c]{p{0.5in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}}
+\caption{Accuracy of correlation formulae in predicting test case results \label{table:accuracy-of-correlation-formulae-in}} \tabularnewline
+\toprule 
+Cases & Errors (\%) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Accuracy of correlation formulae in predicting test case results} \tabularnewline
+\toprule 
+Cases & Errors (\%) \tabularnewline
+\midrule
+\endhead
+
+ID & A (m2) & W (m) & D (m) & H (m) & Jet Velocity & Recirculation Velocity & Recirculation Flow Rate & Jet Temperature Rise & Recirculation Temperature Rise \tabularnewline
+1 & 0.25 & 6 & 9 & 2.3 & 16 & 45 & 60 & 1 & 10 \tabularnewline
+2 & 0.25 & 11 & 9 & 2.3 & 5 & 43 & 32 & 5 & 7 \tabularnewline
+3 & 0.5 & 9 & 4.5 & 2.3 & 2 & 18 & 27 & 15 & 2 \tabularnewline
+4 & 0.5 & 9 & 6 & 2.3 & 6 & 32 & 28 & 7 & 1 \tabularnewline
+5 & 0.5 & 6 & 9 & 2.3 & 7 & 6 & 21 & 7 & 0 \tabularnewline
+6 & 0.5 & 9 & 9 & 2.3 & 10 & 4 & 6 & 15 & 17 \tabularnewline
+7 & 0.5 & 11 & 9 & 2.3 & 6 & 7 & 0 & 14 & 20 \tabularnewline
+8 & 0.5 & 13.5 & 9 & 2.3 & 14 & 9 & 5 & 21 & 2 \tabularnewline
+9 & 0.5 & 9 & 13.5 & 2.3 & 10 & 11 & 17 & 7 & 8 \tabularnewline
+10 & 0.5 & 9 & 18 & 2.3 & 10 & 25 & 29 & 8 & 3 \tabularnewline
+11 & 0.5 & 13.5 & 18 & 2.3 & 8 & 2 & 23 & 9 & 6 \tabularnewline
+12 & 1 & 9 & 9 & 2.3 & 2 & 5 & 3 & 3 & 4 \tabularnewline
+13 & 1 & 9 & 13.5 & 2.3 & 8 & 10 & 10 & 3 & 6 \tabularnewline
+14 & 1 & 9 & 18 & 2.3 & 0 & 18 & 6 & 13 & 2 \tabularnewline
+Average & 8 & 17 & 19 & 9 & 6 \tabularnewline
+\bottomrule
+\end{longtable}
+
+In each case the error is the percentage difference between the given correlation prediction and the test case result obtained from CFD, i.e.~100*\textbar{}(correlation prediction -- CFD)/CFD\textbar{}.
+
+\(\sqrt {{A_{in}}/{A_{RM}}} \left( {{V_{J,m}}/{U_{in}}} \right)\) \({U_J}/{U_{in}}\) 
+
+\begin{figure}[hbtp]
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2652.png}
+\caption{Jet velocity correlation. \protect \label{fig:jet-veolicty-correlation}}
+\end{figure}
+
+\(\sqrt {{A_{in}}/{A_{RM}}} \left( {{V_{J,m}}/{U_{in}}} \right)\) \({U_R}/{U_{in}}\) 
+
+\begin{figure}[hbtp]
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2655.png}
+\caption{Recirculation region velocity correlation. \protect \label{fig:recirculation-region-velocity}}
+\end{figure}
+
+\(\sqrt {{A_{in}}{A_{RM}}} \left( {{V_{J,m}}/{U_{in}}} \right)\) \({Q_R}/{U_{in}}\) 
+
+\begin{figure}[hbtp]
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2658.png}
+\caption{Recirculation region flow rate. \protect \label{fig:recirculation-region-flow-rate}}
+\end{figure}
+
+\subsubsection{Wind angle effects}\label{wind-angle-effects}
+
+When the incoming wind is not normal to the façade the jet enters the room at an angle, as shown in Figure~\ref{fig:schematic-of-jet-resulting-from-wind-at-angle}.
+
+\begin{figure}[hbtp] % fig 143
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2659.png}
+\caption{Schematic of jet resulting from wind at angle φ to façade. \protect \label{fig:schematic-of-jet-resulting-from-wind-at-angle}}
+\end{figure}
+
+This oblique geometry has two main effects on the flow and consequent correlation predictions:
+
+The inflow area is reduced, creating a larger inflow velocity for the same flow rate.
+
+The room flow path length is increased, from \emph{D} to \emph{D}*, resulting in a larger apparent depth.
+
+The first effect increases indoor velocities while the second effect decreases the velocities.
+
+\subsubsection{Multiple apertures}\label{multiple-apertures}
+
+CFD simulations for rooms with more than one inflow aperture show that the model can be applied to these configurations with minimal adjustments. As a result of increased dissipation in the central recirculation region, where two distinct recirculation flows collide (Figure~\ref{fig:flow-regions-for-a-room-with-2-inlets-and-2}), the airflow velocities are reduced by 5-10\%, as shown in the charts in Figure~\ref{fig:jet-velocity-and-recirculation-velocity-for}.
+
+\begin{figure}[hbtp] % fig 144
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2660.png}
+\caption{Flow regions for a room with 2 inlets and 2 outlets. \protect \label{fig:flow-regions-for-a-room-with-2-inlets-and-2}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 145
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2662.png}
+\caption{Jet velocity and recirculation velocity for the two halves of 3 different 2-inlet rooms, A-C, compared with the corresponding 1-inlet rooms. \protect \label{fig:jet-velocity-and-recirculation-velocity-for}}
+\end{figure}
+
+\textbf{\emph{Heat transfer in recirculating flows}}
+
+In most cross ventilation flows with recirculations the mixing between recirculation and inflow jet is only partial. Figure~\ref{fig:top-view-of-the-flow-structure-in-case-r.} shows a schematic representation of the heat transfer process (showing a top view of one half of a symmetrical room). The flow is divided into three distinct streams with connected temperature variations:
+
+The main jet (labeled J in the figure).
+
+The part of the recirculation flow that exchanges heat with the jet (label R).
+
+The wall boundary layer part of the recirculation flow (label W).
+
+\begin{figure}[hbtp] % fig 146
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2663.png}
+\caption{Top view of the flow structure in case R. \protect \label{fig:top-view-of-the-flow-structure-in-case-r.}}
+\end{figure}
+
+The light gray arrows show flow direction. The dark gray arrows show heat transfer in the shear layer. The recirculation region coordinate system is shown in the figure, with coordinate \emph{r} varying between 0 and \emph{L}.
+
+\subsubsection{Heat transfer in a shear layer}\label{heat-transfer-in-a-shear-layer}
+
+It is possible to use a formulation with a heat transfer area, a convection heat transfer coefficient and an average shear layer temperature difference to model the heat exchange between jet and recirculation flows:
+
+\({Q_{y = 0}} = {A_{SL}}\,{h_{SL}}\,\Delta {T_{SL}}\) , \({A_{SL}} = L\,\,P\,,\,\,{h_{SL}} = \frac{{\rho \,{C_P}\,F}}{{{C_D}\,\,{A_{IN}}\,\,4\,\sigma \,\sqrt \pi }}\)
+
+Locally, the heat transfer process is driven by the variable, local, temperature difference:
+
+\begin{equation}
+\rho \,{C_P}\,F\,\frac{{\partial \,{T_J}(x)}}{{\partial \,x}} =  - \,\frac{{{A_{SL}}\,{h_{SL}}}}{L}\,\left( {{T_J}(x) - {T_R}(x)} \right) = \frac{{P\,\,\left( {{T_J}(x) - {T_R}(x)} \right)}}{{{C_D}\,{A_{IN}}\,4\,\sigma \,\sqrt \pi  }}
+\end{equation}
+
+\subsubsection{Predicting air temperature in the recirculation region of the flow}\label{predicting-air-temperature-in-the-recirculation-region-of-the-flow}
+
+An accurate representation of system behavior must consider both the local heat transfer in the shear layer (varying along the \emph{x} direction, driven by the temperature profiles \emph{T\(_{J}\)(x)} and \emph{T\(_{R}\)(x)}) and the heat transfer in the wall boundary layers (with temperature \emph{T\(_{W}\)(r)}). Both transfers can be modeled using differential equations, resulting in the following system of equations:
+
+\begin{equation}
+  \begin{array}{rl}
+    \rho C_p F R \frac{\partial T_W \left(r\right)}{\partial r} & = \frac{A_S h_S}{L} \left(T_S - T_W \left(r\right)\right) \\
+    \rho C_p F R \frac{\partial T_R \left(x\right)}{\partial x} & = \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right) \\
+    \rho C_p F \frac{\partial T_J \left(x\right)}{\partial x} & = \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right) 
+  \end{array}
+\end{equation}
+
+The relevant boundary conditions are:
+
+\begin{equation}
+{T_W}({L_{}}) = {T_R}(0)\,,\,{T_W}(0) = {T_R}(L)\,,\,\,{T_J}(0) = {T_{IN}}
+\end{equation}
+
+The first equation in models heat transfer in the wall layer. The second models the temperature variation of the portion of the recirculation flow that is in contact with the jet, it differs from the third equation only in a sign (the temperature variation in \emph{T\(_{R}\)} is symmetric to the variation in \emph{T\(_{J}\)}) and the flow rate (\emph{F.R} for the recirculation and \emph{F} for the main jet). The temperature in the recirculation region is given by:
+
+\begin{equation}
+{T_W}(r) = {T_S} - ({T_S} - {T_{IN}})\,\frac{{{e^{\frac{{{h_S}\,{A_S}}}{{\rho \,{C_P}\,R\,F}}\frac{r}{{{L_{}}}}}}\,({e^{ - \frac{{{A_{SL}}\,{h_{SL}}\,(1 + R)}}{{\rho \,{C_P}\,R\,F}}}} - 1)}}{{{e^{ - \frac{{{A_{SL}}\,{h_{SL}}\,(1 + R)}}{{\rho \,{C_P}\,R\,F}}}} - {e^{\frac{{{h_S}\,{A_S}}}{{\rho \,{C_P}\,R\,F}}}}\,(1 + R) + R}}
+\end{equation}
+
+\subsubsection{Heat transfer in recirculating flows with internal gains}\label{heat-transfer-in-recirculating-flows-with-internal-gains}
+
+Whereas surface heat transfer is an important component of room heat transfer, internal gains often dominate the room temperature field. Referring to the previously used subdivision of the room into jet and recirculation regions we can see that gains can occur exclusively in the jet region, exclusively in the recirculation region or in both regions.
+
+\subsubsection{Heat gains in the jet region}\label{heat-gains-in-the-jet-region}
+
+The effect of gains in the jet region on room air temperature distribution is simple to model and, within the first order accuracy goal, can be characterized as follows:
+
+For gains occurring in the jet region (between the inlet and the room outlet) a change in inflow temperature is an adequate, conservative approximation. From energy conservation we conclude that the altered inflow temperature is given by:
+
+\begin{equation}
+{T_{ING}} = {T_{IN}} + \frac{{{G_J}}}{{\rho {C_P}F}}
+\end{equation}
+
+Gains occurring in the jet region, close to the outlet can be ignored in a first order accuracy model.
+
+Clearly the two approaches described above are only exact when: the gains occur at the inlet and perfectly mix with the inflow jet (for the first case), or whenever the gains occur very close to the outlet (in the second case). In all other situations, the first approach provides a conservative approximation. In the model implementation in EnergyPlus the user will not define the exact location of the heat gains within each region of the flow therefore, heat gains in the jet region, are inserted in two equal parts in two separate points of the jet flow (in the room entrance and before the exit, see points r = 0 and r = L\(_{R}\) in Figure~\ref{fig:top-view-of-the-flow-structure-in-case-r.}).
+
+\subsubsection{Heat gains in the recirculation region}\label{heat-gains-in-the-recirculation-region}
+
+When heat gains occur in the recirculation region significant heat accumulation occurs due to the limited heat transfer ability of the shear layer. Due to this limited ability, the recirculation is partially isolated from the main jet flow and higher temperatures are generated in this region whenever heat gains are present. The concept of a global heat transfer coefficient is not applicable.
+
+In the case of a flow in a room with adiabatic surfaces and heat gains in the recirculation region the indoor air temperatures can be predicted using the solution to the following system of equations:
+
+\begin{equation}
+  \begin{array}{rl}
+    \rho C_p F R \left(T_R\left(0\right) - T_R\left(L\right)\right) & = G_R \\
+    \rho C_p F R \frac{\partial T_R \left(x\right)}{\partial x} & = \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right) \\
+    \rho C_p F \frac{\partial T_J \left(x\right)}{\partial x} & = \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right)
+  \end{array}
+\end{equation}
+
+This system of equations differs from system F16 in several ways. Because there is no wall heat transfer there is no need to split the recirculation flow in two parts (\emph{R} and \emph{W}). The temperature increase in the recirculation flow is simply defined by the internal gains (first equation in ). The second and third equations in model shear layer heat transfer are similar in the two cases ( and ).
+
+The recirculation flow temperature at \emph{x} = 0 is given by:
+
+\begin{equation}
+{T_R}(0) = {T_{IN}} + \left( {\frac{1}{{{e^{\frac{{{A_{SL}}{h_{SL}}\,(1 + R)}}{{\rho \,{C_P}F\,R}}}} - 1}} + 1} \right)\frac{{{G_R}(1 + R)}}{{\rho \,{C_P}F\,R}}
+\end{equation}
+
+The temperature in the recirculation is inversely proportional to the recirculation flow ratio (\emph{R}) and the shear layer area (measured by the product: \emph{A\(_{SL}\) h\(_{SL}\)}). As both of these parameters increase this expression becomes similar to . The recirculation flow temperature at \emph{x = L} is given by:
+
+\begin{equation}
+{T_R}(L) = {T_R}(0) + \Delta {T_R}
+\end{equation}
+
+The temperature variations in the recirculation flow is given by:
+
+\begin{equation}
+\Delta {T_R} = \frac{{{G_R}}}{{\rho \,{C_P}\,F\,R}}
+\end{equation}
+
+\subsubsection{Combined effects of surface heat transfer and internal gains in the recirculation region}\label{combined-effects-of-surface-heat-transfer-and-internal-gains-in-the-recirculation-region}
+
+In this case, the following system of equations must be solved:
+
+\begin{equation}
+\begin{array}{rl}
+    \rho C_p F R \frac{\partial T_W \left(r\right)}{\partial r} & = -\frac{A_S h_S}{L} \left(T_S - T_W \left(r\right)\right) - \frac{G_R}{L_R} \\
+    \rho C_p F R \frac{\partial T_R \left(x\right)}{\partial x} & = \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right) \\
+    \rho C_p F \frac{\partial T_J \left(x\right)}{\partial x} & = \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right) 
+  \end{array}
+\end{equation}
+
+With the boundary conditions: \({T_W}(L) = {T_R}(0)\,,\,{T_W}(0) = {T_R}(L)\,,\,\,{T_J}(0) = {T_{IN}}\)
+
+For simplicity the heat gains are considered to be evenly distributed along the recirculation path. The temperature variation in the recirculation region is given by:
+
+\begin{equation}
+{T_W}(r) = {T_S} + \frac{{{G_R}}}{{{A_S}\,{h_S}}} - \frac{{{e^{\frac{{{h_S}\,{A_S}}}{{\rho \,{C_P}\,R\,F}}\frac{r}{{{L_R}}}}}\,({e^{ - \frac{{{A_{SL}}\,{h_{SL}}\,(1 + R)}}{{\rho \,{C_P}\,R\,F}}}} - 1)\,({G_R} + {A_S}\,{h_S}\,({T_S} + {T_{IN}}))}}{{{e^{ - \frac{{{A_{SL}}\,{h_{SL}}\,(1 + R)}}{{\rho \,{C_P}\,R\,F}}}} + R - {e^{\frac{{{h_S}\,{A_S}}}{{\rho \,{C_P}\,R\,F}}}}\,(1 + R)}}
+\end{equation}
+
+% table 48
+\begin{longtable}[c]{p{1.0in}p{1.0in}p{3.5in}}
+\caption{List of variables for CV model \label{table:list-of-variables-for-cv-model}} \tabularnewline
+\toprule 
+Symbol & Units & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{List of variables for CV model} \tabularnewline
+\toprule 
+Symbol & Units & Description \tabularnewline
+\midrule
+\endhead
+
+a & - & Slope of correlation line of best fit \tabularnewline
+A\(_{in}\) & m\(^2\) & Inlet area \tabularnewline
+A\(_{RM}\) & m\(^2\) & Room cross-sectional area \tabularnewline
+b & - & Intercept of correlation line of best fit \tabularnewline
+c\(_{p}\) & J/kg/K & Specific heat capacity of air \tabularnewline
+C\(_{RM}\) & - & Confinement scaling factor, (A\(_{in}\)/A\(_{RM}\))\(^{1/2}\) \tabularnewline
+C\(_{1}\) & - & Correlation constant for jet velocity \tabularnewline
+C\(_{2}\) & - & Correlation constant for recirculation velocity \tabularnewline
+C\(_{3}\) & - & Correlation constant for recirculation flow rate \tabularnewline
+D & m & Room depth, distance between inlet and outlet facades \tabularnewline
+D* & m & Effective room depth adjusted for wind angle \tabularnewline
+H & m & Room height \tabularnewline
+q\(^{''}_{RM}\) & W & Total heat input from internal heat sources \tabularnewline
+Q\(_{in}\) & m\(^3\)/s & Inlet flow rate, A\(_{in}\)U\(_{in}\) \tabularnewline
+Q\(_R\) & m\(^3\)/s & Maximum recirculation region flow rate \tabularnewline
+U\(_{in}\) & m/s & Inlet velocity, average over inlet area \tabularnewline
+U\(_{m}\) & m/s & Maximum centerline velocity of jet \tabularnewline
+U\(_{o}\) & m/s & Uniform inlet velocity of jet \tabularnewline
+U\(_{J}\) & m/s & Volume-averaged jet velocity \tabularnewline
+U\(_{R}\) & m/s & Average recirculation region velocity over plane of maximum flow \tabularnewline
+V & m/s & Velocity scale \tabularnewline
+V\(_{J,m}\) & m/s & Average of U\(_{m}\) over room depth \tabularnewline
+W & m & Room width \tabularnewline
+x & m & Coordinate along room depth, 0 $\leq$ x $\leq$ D \tabularnewline
+x' & - & Non-dimensional x-coordinate, x/D \tabularnewline
+X & m/s & Velocity correlation parameter \tabularnewline
+Y & m & Lateral coordinate across room width \tabularnewline
+Z & m & Vertical coordinate \tabularnewline
+$\Delta$T\(_{J}\) & °C & Average jet temperature variation \tabularnewline
+$\Delta$T\(_{R}\) & °C & Average recirculation region temperature variation \tabularnewline
+r & kg/m\(^3\) & Density of air \tabularnewline
+$\varphi$ & ° & Wind direction relative to façade normal \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{References}\label{references-5-000}
+
+Awbi, H.B. (2003) \emph{Ventilation of Buildings} (2\(^{nd}\) edition). Routledge, 536pp.
+
+Carrilho da Graca, G. 2003.Simplified models for heat transfer in rooms. Ph. D. Thesis, University of California, San Diego.
+
+Kalema, T., Haapala, T. `995. Effect of interior heat transfer coefficients on thermal dynamics and energy consumption, Energy and Buildings 22 (2) pp.~101-113.
+
+Aynsley, R.M., Melbourne, W., Vickery, B.J. 1977. Architectural Aerodynamics. Applied Science London.
+
+Baturin, V. V. , Billington, N. S. 1972. Fundamentals of Industrial Ventilation, Franklin Book Company 1972, pp.~174-179.
+
+Neiswanger, L., Johnson, G.A., Carey, V.P. 1987. An experimental study of high Raleigh number mixed convection in a rectangular enclosure with restricted inlet and outlet openings. Transactions of ASME, Vol. 109, 446-453.
+
+Ohba, M., Irie, K., Kurabuchi, T. 2001. Study on airflow characteristics inside and outside a CVmodel, and ventilation flow rate using wind tunnel experiments. Journal of Wind Engineering and Industrial Aerodynamics, in press.
+
+Chandra, S., Kerestecioglu, A.A. 1984. Heat transfer in naturally ventilated rooms data from full-scale measurements, ASHRAE Transactions, Volume 90, part 1b 211-224.
+
+Altmayer, E.F., Gadgil, A.J., Bauman, F.S., Kammerud, R.C. Correlations for convective heat transfer from room surfaces. ASHRAE Transactions, No. 2764.
+
+Spitler, J. D., Pedersen, C.O., Fisher, D.E. 1991. Interior Convective Heat Transfer in Buildings with Large Ventilative Flow Rates. ASHRAE Transactions, Vol. 97, Pt.1, pp.~505-515.
+
+Awbi, H.B. \& Hatton, A. 1999. Natural convection from heated room surfaces, Energy and Buildings, 30, 233-244.
+
+Siebers, D. L., Schwind, R. G., Moffat, R. J. 1983. Experimental Mixed Convection Heat Transfer From a Large Vertical Surface in a Horizontal Flow. SAND 83-8225, Sandia National Laboratories, Livermore CA.
+
+Awbi, H.B. \& Hatton, A. 2000. Mixed convection from heated room surfaces, Energy and Buildings, 32, 153-166.
+
+Bejan, A. 1994. Convection Heat Transfer 2nd ed, Wiley, USA.
+
+\subsection{RoomAirflowNetwork Model}\label{roomairflownetwork-model}
+
+\subsubsection{Overview}\label{overview-4-001}
+
+The RoomAirflowNetwork integrates the RoomAir model with the AirflowNetwork model. The model allows multiple Room Air nodes to be associated with AirflowNetwork intra zone nodes. The AirflowNetwork intra zone linkages provide links among the intra zone nodes and users may specify airflow components among these links. The AirflowNetwork model calculates airflows of the links. The incoming airflows are part of the zone heat and moisture balances of intra zone nodes. The model also allows users to specify a node to be connected to surfaces to have convective heat transfer and/or moisture transfer between surfaces and the node, portion of internal gains and supply air and return air fractions from zone equipment and AirLoop terminals.
+
+The input object RoomAirSettings:AirflowNetwork lists multiple RoomAirflowNetwork nodes in a zone. The input object of RoomAirflowNetwork:Node defines a list of connections assigned to a particular RoomAirflowNetwork node so that the connections will be used as components of node heat and moisture balance equations. In addition, the input objects AirflowNetwork:IntraZone:Node and AirflowNetwork:IntraZone:Linkage specify airflow nodes, linkages, and associated flow components, so that the AirflowNetwork model is used to calculate intrazone linkage airflows, which will be a part of loads for the RoomAir node balances.
+
+\subsubsection{Model description}\label{model-description-3-001}
+
+The model calculates each component of the governing equations first. Then heat and moisture balance equations are solved to get the node temperature and humidity ratio at the current time step.
+
+Governing equations for each RoomAirflowNetwork node are described below:
+
+Energy balance equation
+
+\begin{equation}
+\begin{split}
+{F_i}{C_{z,i}}\frac{{d{T_{z,i}}}}{{dt}} =& \sum\limits_{j = 1}^{{N_{i,g}}} {{F_{gain,j}{\dot Q}_{i,j}}}  + \sum\limits_{j = 1}^{{N_{i,sur}}} {{h_{i,j}}} {A_j}\left( {{T_{s,j}} - {T_{z,i}}} \right) + \sum\limits_{j = 1}^{{N_{i,AFN}}} {{{\dot m}_{AFN i,j}}} {C_p}\left( {{T_{z,j}} - {T_{z,i}}} \right)\, \\
+&+ \sum\limits_{j = 1}^{{N_{i,HVAC}}} {{{F_{HVAC,j}}{\dot m}_{sup,i,j}}} {C_p}\left( {{T_{sup_j}} - {T_{z,i}}} \right)
+\end{split}
+\end{equation}
+
+where:
+
+F\(_{i}\) = Fraction of zone air volume for the ith node, defined in the Fraction of Zone Air Volume field of the RoomAir:Node:Airflownetwork
+
+C\(_{z,i}\) = Volumetric heat capacity for the ith node: �\(_{air,i}\)V C\(_{p}\)C\(_{T}\)
+
+�\(_{air,i}\) = Dry air density at the ith zone node
+
+C\(_{p}\) = zone dry air specific heat
+
+C\(_{T}\) = sensible heat capacity multiplier (Detailed description is provided below)
+
+V = Zone air volume
+
+T\(_{z,i}\) = Air temperature at the ith zone RoomAir node
+
+N\(_{i,g}\) = The number of internal gains for the ith node, defined in the RoomAir:Node:Airflownetwork:InternalGains object
+
+F\(_{gain,j}\) = Fraction of internal gain from jth internal gain object defined in the RoomAir:Node:Airflownetwork:InternalGains object
+
+\({\dot Q}_{i,j}\) = The amount of internal sensible gain at the jth internal gain object and ith node.
+
+\({\sum\limits_{j = 1}^{N_{i,g}} F_{gain,j}{\dot Q}_{i,j}}\) = The total amount of internal sensible gains assigned to the ith node
+
+N\(_{i,sur}\) = The number of adjacent surface with convective heat transfer for the ith node, defined in the RoomAir:Node:Airflownetwork:AdjacentSurfaceList object
+
+h\(_{j}\) = Heat transfer coefficient between the jth adjacent surface and ith node
+
+A\(_{j}\) = Area of the jth adjacent surface
+
+T\(_{s,j}\) = Inside temperature at the jth adjacent surface
+
+\({\sum\limits_{j = 1}^{N_{i,sur}} h_{j} A_j \left( T_{s,j} - T_{z,i}\right)}\) = The total amount of convective gains from adjacent surfaces attached to the ith node
+
+N\(_{i,AFN}\) = The number of RoomAir:Node:Airflownetwork objects connected to the ith node. The links are defined in AirflowNetwork:IntraZone:Linkage objects.
+
+\({\dot m}_{AFN,i,j}\) = Mass flow rate from the jth node to the ith node. The flow rates are calculated in the AirflowNetwork model. It should be pointed out that the outgoing flows from the ith node will not be used in the present energy and moisture balance calculations, because they are a part of energy and moisture balances.
+
+T\(_{z,j}\) = Air temperature at the jth zone RoomAir node
+
+\({\sum\limits_{j = 1}^{N_{i,g}} \dot m_{AFN i,j} {C_p}\left( T_{z,j} - T_{z,i} \right)}\) = The total amount of heat transfer driven by intra zonal flows
+
+N\(_{i,HVAC}\) = The number of RoomAir:Node:Airflownetwork:HVACEquipment objects which provide supply air to the ith node.
+
+F\(_{HVAC,j}\) = Fraction of output or supply air to the ith node from jth HVAC equipment defined in RoomAir:Node:Airflownetwork:HVACEquipment objects
+
+\({\dot m}_{sup,i,j}\) = The supply mass flow rate from the jth HVAC equipment
+
+T\(_{sup,j}\) = Supply air temperature at the jth HVAC equipment
+
+\({\sum\limits_{j = 1}^{N_{i,HVAC}} F_{HVAC,j} \dot m_{sup,i,j} \left( T_{sup,j} - T_{z,i}\right)}\) = The total amount of heat transfer from HVAC equipment to the ith node
+
+Moisture balance equation
+
+\begin{equation}
+\begin{split}
+{F_i}{M_{z,i}}\frac{{d{W_{z,i}}}}{{dt}} =& \sum\limits_{j = 1}^{{N_{i,g}}} {{F_{gain,j}{\dot Q}_{i,j}}}  + \sum\limits_{j = 1}^{{N_{i,sur}}} {{h_{M,j}}} {A_j}\left( {{W_{s,j}} - {W_{z,i}}} \right) + \sum\limits_{j = 1}^{{N_{i,AFN}}} {{{\dot m}_{AFN i,j}}} \left( {{W_{z,j}} - {W_{z,i}}} \right)\, \\
+&+ \sum\limits_{j = 1}^{{N_{i,HVAC}}} {{{F_{HVAC,j}}{\dot m}_{sup,i,j}}} \left( {{W_{sup_j}} - {W_{z,i}}} \right)
+\end{split}
+\end{equation}
+
+where:
+
+Fi = Fraction of zone air volume for the ith node, defined in the Fraction of Zone Air Volume of the RoomAir:Node:Airflownetwork
+
+M\(_{z,i}\) = Mass for the ith node: �\(_{air,i}\)V\(_{Cp}\)C\(_{T}\)
+
+�\(_{air,i}\) = Dry air density at the ith zone RoomAir node
+
+V = Zone air volume
+
+W\(_{z,i}\) = Air humidity ratio at the ith zone RoomAir node
+
+N\(_{i,g}\) = The number of internal gains for the ith node, defined in the \\ RoomAir:Node:Airflownetwork:InternalGains object
+
+F\(_{gain,j}\) = Fraction of internal gain from jth internal gain object defined in the RoomAir:Node:Airflownetwork:InternalGains object
+
+\({\dot Q}_{i,j}\) = The amount of internal latent gain at the jth internal gain object and ith node.
+
+\({\sum\limits_{j = 1}^{N_{i,g}} F_{gain,j}{\dot Q}_{i,j}}\) = The total amount of internal latent gains attached to the ith node
+
+N\(_{i,sur}\) = The number of adjacent surface with convective heat transfer for the ith node, defined in the RoomAir:Node:Airflownetwork:AdjacentSurfaceList object
+
+h\(_{M,j}\) = Mass transfer coefficient between the jth adjacent surface and ith node
+
+A\(_{j}\) = Area of the jth adjacent surface
+
+W\(_{s,j}\) = Inside humidity ratio at the jth adjacent surface
+
+\({\sum\limits_{j = 1}^{N_{i,sur}} h_{M,j} A_j \left( W_{s,j} - W_{z,i}\right)}\) = The total amount of convective moisture gains from adjacent surfaces attached to the ith node
+
+N\(_{i,AFN}\) = The number of RoomAir:Node:Airflownetwork objects connected to the ith node. The links are defined in AirflowNetwork:IntraZone:Linkage objects.
+
+\({\dot m}_{AFN,i,j}\) = Mass flow rate from the jth node to the ith node. The flow rates are calculated in the AirflowNetwork model. It should be pointed out that the outgoing flow from the ith node will not be used in the present calculation, because they are a part of energy balance.
+
+W\(_{z,j}\) = Air humidity ratio at the jth zone RoomAir node
+
+\({\sum\limits_{j = 1}^{N_{i,AFN}} \dot m_{AFN,i,j} \left( W_{z,j} - W_{z,i}\right)}\) = The total amount of moisture transfer driven by intra zonal flows
+
+N\(_{i,HVAC}\) = The number of RoomAir:Node:Airflownetwork:HVACEquipment objects which provide supply air to the ith node.
+
+F\(_{HVAC,j}\) = Fraction of output or supply air to the ith node from jth HVAC equipment defined in RoomAir:Node:Airflownetwork:HVACEquipment objects
+
+\({\dot m}_{sup,i,j}\) = The supply mass flow rate from the jth HVAC equipment
+
+W\(_{sup,j}\) = Supply air humidity ratio at the jth HVAC equipment
+
+\({\sum\limits_{j = 1}^{N_{i,HVAC}} F_{HVAC,j} \dot m_{sup,i,j} \left( W_{sup,j} - W_{z,i}\right)}\) = The total amount of moisture transfer from HVAC equipment to the ith node
+
+\subsubsection{Calculation procedures}\label{calculation-procedures}
+
+The AirflowNetwork model is called first to calculate intrazone linkage air flows based on node temperatures and humidity ratios at the previous time step. The linkage loads are summarized based on each node with all incoming airflow, while any outgoing airflows from the node of the interest are excluded in the node energy and moisture balances. When the RoomAirModelAirflowNetowrk module is called, it summarizes internal gains at each node based on specification provided in the RoomAirflowNetwork:Node:InternalGains object, convective heat transfer from adjacent walls specified in the RoomAirflowNetwork:Node:AdjacentSurfaceList object. These load components are used in the predictor to predict system loads based on thermostat setpoint and supply fraction in the controlled zone node. In the corrector, the supply air conditions defined in the RoomAirflowNetwork:Node:HVACEquipment object are added. After all load components are assembled together, the node energy and moisture balance equations are solved. The node temperature and humidity ratio are calculated at the current time step.  
diff --git a/doc/engineering-reference/src/alternative-modeling-processes/airflownetwork-model.tex b/doc/engineering-reference/src/alternative-modeling-processes/airflownetwork-model.tex
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+\section{AirflowNetwork Model}\label{airflownetwork-model}
+
+\subsection{Overview}\label{overview-004}
+
+The AirflowNetwork model provides the ability to simulate the performance of an air distribution system, including supply and return leaks, and calculate multizone airflows driven by outdoor wind and forced air during HVAC system operation. The pressure and airflow model described here was developed based on AIRNET (Walton 1989). This detailed model is used to simulate thermal conduction and air leakage losses for constant volume air distribution systems (e.g., in residential or light commercial buildings). The multizone airflow calculations are performed at the HVAC system time step which, among other benefits,.allows for modeling hybrid ventilation systems.
+
+\subsection{Model Description}\label{model-description-001}
+
+The input object AirflowNetwork:SimulationControl provides access to the airflow network method, which consists of a set of nodes connected by airflow components through linkages. The objects AirflowNetwork:Multizone:Zone, AirflowNetwork:Multizone:ExternalNode, and AirflowNetwork:Distribution:Node represent airflow nodes. The objects AirflowNetwork:Multizone:Surface and AirflowNetwork:Distribution:Linkage represent airflow linkages. The other objects with a relationship between pressure and airflow represent airflow components.
+
+The AirflowNetwork model consists of three sequential steps:
+
+\begin{itemize}
+\item
+  Pressure and airflow calculations
+\item
+  Node temperature and humidity calculations
+\item
+  Sensible and latent load calculations
+\end{itemize}
+
+The pressure and airflow calculations determine pressure at each node and airflow through each linkage given wind pressures and forced airflows. Based on the airflow calculated for each linkage, the model then calculates node temperatures and humidity ratios given zone air temperatures and zone humidity ratios.~ Using these node temperatures and humidity ratios, the sensible and latent loads from duct system conduction and leakage are summed for each zone. The sensible and latent loads obtained in this step are then used in the zone energy balance equations to predict HVAC system loads and to calculate the final zone air temperatures, humidity ratios, and pressures.
+
+The present AirflowNetwork model may only be applied to a single heating and cooling system that uses a single air distribution system (a single AirLoopHVAC object). The model excludes the impact of the air and duct system thermal capacitance. The impact of thermal capacity will be addressed in future upgrades to this model.
+
+\subsection{Pressure and Airflow Calculations}\label{pressure-and-airflow-calculations}
+
+The EnergyPlus airflow network consists of a set of nodes linked by airflow components. Therefore, it is a simplified airflow model, compared to detailed models such as those used in computational fluid dynamics (CFD) models. The node variable is pressure and the linkage variable is airflow rate. A brief description is presented below. A detailed description of the airflow network model may be found in the work of Walton (1989), Dols and Walton (2002), and Walton and Dols (2003).
+
+\subsubsection{Initialization}\label{initialization}
+
+Newton's method is used to solve for node air pressures and it requires an initial set of values for the node pressures. There are two initialization methods available. The first is linear initialization and equivalent to Initialization flag = 0. These initial values may be obtained by including in each airflow component a linear approximation relating airflow to pressure drop:
+
+\begin{equation}
+  \dot{m}_{i} = C_{i}\rho\frac{\Delta P_i}{\mu}
+\end{equation}
+
+where
+
+\(\mathop {{m_i}}\limits^ \bullet\) = Air mass flow rate at i-th linkage {[}kg/s{]}
+
+\emph{C\(_{i}\)}~ = Air mass flow coefficient {[}m\(^{3}\){]}
+
+\(\Delta P\) \(_{i}\) = Pressure difference across the i-th linkage {[}Pa{]}
+
+\emph{µ~~~}~~~~~~~~~~~ = Air viscosity {[}Pa-s{]}
+
+This initialization handles stack effects very well and tends to establish the proper direction for the airflows. The linear approximation is provided by the laminar regime.
+
+The second initialization method assumes the initial pressures are zero and uses Newton's method directly.
+
+\subsubsection{Convergence criteria}\label{convergence-criteria}
+
+Conservation of air mass flow rate at each linkage provides the convergence criterion. When the sum of mass flow rates in all the linkages approaches zero within the convergence tolerance, the solution has converged. The solution is assumed to have converged when the sum is less than the convergence value, in order to reduce the number of iterations and obtain sufficient accuracy. There are two convergence criteria used in the AirflowNetwork model: Relative airflow convergence tolerance and Absolute airflow convergence tolerance.
+
+Relative airflow tolerance = \(\frac{\left| \sum \dot m_i \right|}{\sum \dot m_i}\)
+
+Absolute airflow tolerance = \(\left| \sum \dot m_i \right|\)
+
+The relative airflow tolerance is equivalent to the ratio of the absolute value of the sum of all network airflows to the sum of the network airflow magnitudes.~ The absolute airflow tolerance is the summation of the absolute value of all network airflows. The solution has converged when both of these convergence criteria have been met.
+
+\subsubsection{Linkage models}\label{linkage-models}
+
+A linkage used in the AirflowNetwork model has two nodes, inlet and outlet, and is linked by a component which has a relationship between airflow and pressure.~ The pressure difference across each component in a linkage is assumed to be governed by Bernoulli's equation:
+
+\begin{equation}
+\Delta P = \left( {Pn + \frac{{\rho V_n^2}}{2}} \right) - \left( {Pm + \frac{{\rho V_m^2}}{2}} \right) + \rho g\left( {zn - zm} \right)
+\end{equation}
+
+~where
+
+\emph{ΔP}~~~~~~~~~~~ = Total pressure difference between nodes n and m {[}Pa{]}
+
+\emph{P\(_{n}\), P\(_{m}\)}~~~~~~~ = Entry and exit static pressures {[}Pa{]}
+
+\emph{V\(_{n}\), V\(_{m}\)}~~~~~~~ = Entry and exit airflow velocities {[}m/s{]}
+
+\emph{�~~~}~~~~~~~~~ = Air density {[}kg/m\(^{3}\){]}
+
+\emph{g}~~~~~~~~~~~~~~~ = Acceleration due to gravity {[}9.81 m/s\(^{2}\){]}
+
+\emph{z\(_{n}\), z\(_{m}\)}~~~~~~~~~ = Entry and exit elevations {[}m{]}
+
+By rearranging terms and adding wind pressure impacts, the above equation may be rewritten in the format used by the airflow network model:
+
+\begin{equation}
+\Delta P = {P_n} - {P_m} + {P_S} + {P_W}
+\end{equation}
+
+where
+
+\emph{P\(_{n}\), P\(_{m}\)} = Total pressures at nodes n and m {[}Pa{]}
+
+\emph{P\(_{S}\)}~~~~~~~~~~~~~ = Pressure difference due to density and height differences {[}Pa{]}
+
+\emph{P\(_{W}\)}~~~~~~~~~~~ = Pressure difference due to wind {[}Pa{]}
+
+The Input Output Reference provides the relationship between airflow and pressure for the most of the components (Ref.AirflowNetwork Model). The relationship between airflow and pressure for the AirflowNetwork:Multizone:Component:DetailedOpening, AirflowNetwork:Multizone:Component:SimpleOpening, and Air\-flow\-Net\-work:\-Multi\-zone:\-Com\-ponent:\-Horizontal\-Opening objects are provided in detail in this reference.
+
+\begin{figure}[hbtp] % fig 147
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2691.svg.png}
+\caption{The general problem of gravitational flow through a vertical opening \protect \label{fig:the-general-problem-of-gravitational-flow}}
+\end{figure}
+
+The schematic drawing of a possible air flow pattern through a detailed vertical opening (AirflowNetwork:Multizone:Component:DetailedOpening) is shown in Figure~\ref{fig:the-general-problem-of-gravitational-flow}. The equations used below are extracted from the COMIS Fundamentals manual (1990).
+
+The air density is assumed to be a linear function of height:
+
+\begin{equation}
+{\rho_i}(z) = {\rho_{0i}} + {b_i}z
+\end{equation}
+
+The pressure difference is assumed to be linear and simulate the effect of turbulence:
+
+~\(\Delta {P_t} = {P_{t0}} + {b_t}z\)
+
+The reference pressures on each side are given at the bottom of the opening. By assuming the Bernoulli hypothesis on both sides, the pressure difference can be defined at any level of z as:
+
+\begin{equation}
+{P_1}(z) - {P_2}(z) = ({P_{01}} - {P_{02}}) - g\left[ {({\rho_{01}}z + {b_1}{z^2}/2) - ({\rho_{02}}z + {b_2}{z^2}/2)} \right] + ({P_{t0}} + {b_t}z)
+\end{equation}
+
+The velocity at any level z is given by
+
+\begin{equation}
+v(z) = \sqrt {2\frac{{{P_1}(z) - {P_2}(z)}}{\rho }}
+\end{equation}
+
+The locations of the two possible neutral planes are given by an equilibrium in pressure which leads to a zero velocity point. By assuming the left terms in the equation above to be zero, one may have:
+
+\begin{equation}
+g({b_1} - {b_2}){z^2}/2 + \left[ {g({\rho_{01}} - {\rho_{02}}) - {b_t}} \right]z + ( - {P_{01}} + {P_{02}} - {P_{t0}}) = 0
+\end{equation}
+
+This equation above can have two, one, or zero real solutions.~ The zero solution represents a one-way flow through the opening and may be expressed in the following equation:
+
+\begin{equation}
+\dot m = {C_d}\theta \int\limits_{z = 0}^{z = H} {\rho \nu (z)Wdz}
+\end{equation}
+
+The one real solution represents two-way (bi-directional) flow, which may be written in the following equations.
+
+\begin{equation}
+{\dot m_{0,z1}} = {C_d}\theta \int\limits_{z = 0}^{z = z1} {\rho \nu (z)Wdz}
+\end{equation}
+
+\begin{equation}
+{\dot m_{z1,H}} = {C_d}\theta \int\limits_{z = z1}^{z = H} {\rho \nu (z)Wdz}
+\end{equation}
+
+The two real solutions represent three-way flow, which may be written in the following equations.
+
+\begin{equation}
+{\dot m_{z2,H}} = {C_d}\theta \int\limits_{z = z2}^{z = H} {\rho \nu (z)Wdz}
+\end{equation}
+
+\begin{equation}
+{\dot m_{z1,z2}} = {C_d}\theta \int\limits_{z = z1}^{z = z2} {\rho \nu (z)Wdz}
+\end{equation}
+
+\begin{equation}
+{\dot m_{z2,H}} = {C_d}\theta \int\limits_{z = z2}^{z = H} {\rho \nu (z)Wdz}
+\end{equation}
+
+where
+
+\emph{C\(_{d}\)}~ = discharge coefficient {[}dimensionless{]}
+
+\emph{θ}~~~ = Area reduction factor {[}dimensionless{]}
+
+\emph{W}~~ = Opening width {[}m{]}
+
+The discharge coefficient, opening width, opening height, and start height factor are modulated based on opening factors. A detailed description of opening factor calculations may be found in the Input Output Reference (Ref. AirflowNetwork:Multizone:Zone, AirflowNetwork:Multizone:Surface, and
+
+AirflowNetwork:Multizone:Component:DetailedOpening).
+
+The above calculation procedure is used for a normal rectangular window. For a horizontally pivoted rectangular window, the calculation procedure is slightly different. A schematic drawing of a horizontally-pivoted window is shown in Figure~\ref{fig:schematic-drawing-of-a-horizontally-pivoted}.
+
+\begin{figure}[hbtp] % fig 148
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2703.png}
+\caption{Schematic drawing of a horizontally-pivoted window \protect \label{fig:schematic-drawing-of-a-horizontally-pivoted}}
+\end{figure}
+
+The opening angle α (0-90°) is linearly proportional to the window opening factor (0-1.0). An opening factor of 1.0 is equal to an opening angle of 90°. The heights in the pivoted area are expressed as:
+
+\begin{equation}
+h2 = AxisHeight(1 - \cos (\alpha ))
+\end{equation}
+
+\begin{equation}
+h4 = AxisHeight + (WindowHeight - AxisHeight)\cos (\alpha )
+\end{equation}
+
+When z \textless{} h2 or z \textgreater{} h4, where z is the distance from the bottom of the window, the integration procedure is the same as the procedure for a normal rectangular window. When h2\textless{}z\textless{}h4, the window width W in the above equations is modified as:
+
+~\({W_{pivot}} = \sqrt {\frac{1}{{\frac{1}{{{W^2}}} + \frac{1}{{{{(2(AxisHeight - z)\tan (\alpha ))}^2}}}}}}\)
+
+The mass flow rate in the pivoted area becomes:
+
+\begin{equation}
+{\dot m_{pivot}} = {C_d}\theta \int\limits_{z = h2}^{z = h4} {\rho \nu (z){W_{pivot}}dz}
+\end{equation}
+
+It should be pointed out that the discharge coefficient is modulated based on opening factors, while opening width, opening height, and start height factor do not apply for a horizontally-pivoted window. The actual window width and height are used to calculate airflows for a horizontally-pivoted window.
+
+The schematic drawing of air flow patterns through a simple vertical opening (AirflowNetwork:Multizone:Component:SimpleOpening) is shown in Figure~\ref{fig:schematic-of-large-opening-and-associated}. The equations used below are available from Walton (1989).
+
+\begin{figure}[hbtp] % fig 149
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2708.svg.png}
+\caption{Schematic of large opening and associated three flow patterns \protect \label{fig:schematic-of-large-opening-and-associated}}
+\end{figure}
+
+The air density for each node is assumed to be constant. The hydrostatic equation is used to relate pressures at various heights for each node:
+
+\begin{equation}
+Pn\left( y \right) = {P_{0n}} - {\rho_n}gy
+\end{equation}
+
+\begin{equation}
+{P_m}(y) = {P_{0m}} - {\rho_m}gy
+\end{equation}
+
+where
+
+\emph{P\(_{0n}\), P\(_{0m}\)~ =}pressure at nodes (zones) n and m at y = 0, the reference elevation of the opening {[}Pa{]}
+
+\emph{�\(_{n}\), �\(_{m}\)~ =}air densities of zones n and m {[}kg/m\(^{3}\){]}
+
+\emph{P\(_{n}\), P\(_{m}\)~ =}reference pressures of zones n and m {[}Pa{]}
+
+It is assumed that the velocity of the airflow as a function of height is given by the orifice equation (Brown and Solvason 1962):
+
+\begin{equation}
+v(y) = {C_d}\sqrt {2\frac{{{P_n}(y) - {P_m}(y)}}{\rho }}
+\end{equation}
+
+~where
+
+\emph{C\(_{d}\)} = discharge coefficient {[}dimensionless{]}
+
+\emph{�}~~ = density of the air going through the opening {[}kg/m\(^{3}\){]}
+
+The neutral height, Y, where the velocity of the air is zero, may be calculated in the following equation:
+
+\begin{equation}
+Y = \frac{{{P_{on}} - {P_{0m}}}}{{g({\rho_n} - {\rho_m})}}\,\,\,\,\,\,\,\,or\,\,\,\,\,\,\,\frac{{{P_{om}} - {P_{0n}}}}{{g({\rho_m} - {\rho_n})}}
+\end{equation}
+
+When the neutral plane is within the opening (first pattern in Figure~\ref{fig:schematic-of-large-opening-and-associated}), two-way (bi-directional) flows occur. The total flow through a large opening is the sum of both flows.
+
+\begin{equation}
+{\dot m_{0,Y}} = {C_d}\theta \int\limits_{y = 0}^{y = Y} {\rho \nu (y)Wdy}
+\end{equation}
+
+\begin{equation}
+{\dot m_{Y,H}} = {C_d}\theta \int\limits_{y = Y}^{y = H} {\rho \nu (y)Wdy}
+\end{equation}
+
+When the neutral plane is below or above the large opening (second and third pattern in Figure~\ref{fig:schematic-of-large-opening-and-associated}), one-way flow occurs.
+
+\begin{equation}
+{\dot m_{}} = {C_d}\theta \int\limits_{y = 0}^{y = H} {\rho \nu (y)Wdy}
+\end{equation}
+
+The opening width is modulated based on opening factors. A detailed description of opening factor calculations may be found in the Input Output Reference (Ref. AirflowNetwork:Multizone:Zone, AirflowNetwork:Multizone:Surface, and AirflowNetwork:Multizone:Component:DetailedOpening).
+
+The above two objects are used to simulate airflows across large vertical openings. The simple opening component (AirflowNetwork:Multizone:Component:SimpleOpening) assumes the pressure difference across the opening is a function of height varied from opening bottom to top, so that two-way flow may be obtained if appropriate (Walton 1989). The Detailed Opening component (AirflowNetwork:Multizone:Component:DetailedOpening) assumes both the pressure difference across the opening and air density are a function of height, so that three-way flow may be obtained (COMIS 1990). If these opening models would be used for horizontal openings, the pressure difference across the opening and air density remain constant, so that only one-way flow is possible using the detailed and simple opening components which are meant for vertical or near-vertical openings. In reality, there are two-way flows (air recirculation) across a large horizontal opening caused by buoyancy due to temperature and pressure difference and forced flow driven by air pressure difference only. Therefore, a horizontal opening component (AirflowNetwork:Multizone:Component:HorizontalOpening) is available to simulate airflows across large horizontal openings with the possibility of two-way flow by combining forced and buoyancy airflows together.
+
+The model for horizontal openings consists of forced airflow, buoyancy airflow, purge pressure and sloping plane. The model is mainly from a NIST report presented by Cooper (1989). The sloping plane (Bolmqvist and Sandberg 2004) portion of the model was added to allow for staircase simulations.
+
+For simplicity, a two zone building (upper and lower zones) connected by a large horizontal opening is used to describe the model, as shown in Figure~\ref{fig:air-movements-across-a-horizontal-opening}. Forced and buoyancy airflows are described separately below.
+
+\begin{figure}[hbtp] % fig 150
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2716.png}
+\caption{Air movements across a horizontal opening \protect \label{fig:air-movements-across-a-horizontal-opening}}
+\end{figure}
+
+Forced airflows
+
+The air mass flow rate is determined by the pressure difference across the opening. The relationship between pressure and airflow is the same as AIRNET for a component (see AirflowNetwork:Multizone:Component:SimpleOpening description above). Since the height of the opening is constant, the forced airflow is unidirectional. A positive value for pressure difference indicates flow direction is from the lower zone to the upper zone across the opening, while a negative value represents flow in the opposite direction. The following description addresses forced air mass flow rates and partial derivatives for three possible scenarios of pressure difference:
+
+P\(_{L}\) = P\(_{U}\)
+
+\({\dot m_U}\) = \({\dot m_L}\) = 0
+
+where:
+
+P\(_{L}\)~~~~~~~~~~~~~~ = Air pressure in the lower zone {[}Pa{]}
+
+P\(_{U}\)~~~~~~~~~~~~~ = Air pressure in the upper zone {[}Pa{]}
+
+\({\dot m_U}\) ~~~~~~~~~~~ = Air mass flow rate from the lower zone to the upper zone driven by forced airflow pressure difference {[}kg/s{]}
+
+\({\dot m_L}\) ~~~~~~~~~~~ = Air mass flow rate from the upper zone to the lower zone driven by forced airflow pressure difference {[}kg/s{]}
+
+1)~~~~~~~~~~~P\(_{L}\) \textgreater{} P\(_{U}\)
+
+\({\dot m_U}\) = 0
+
+\begin{equation}
+{\mathop m\limits^ \bullet_L} = {\rho_L}A{C_d}{\left( {\frac{{2\Delta P}}{{{\rho_{ave}}}}} \right)^{0.5}}
+\end{equation}
+
+\begin{equation}
+\frac{{{{\mathop {\partial m}\limits^ \bullet  }_L}}}{{\partial {P_L}}} = {\rho_L}A{C_d}{\left( {\frac{1}{{2\Delta P{\rho_{ave}}}}} \right)^{0.5}}
+\end{equation}
+
+where:
+
+�\(_{L}\)~~ = Air density in the lower zone {[}kg/m\(^{3}\){]}
+
+A~~~ = Opening area {[}m\(^{2}\){]}
+
+C\(_{d}\) = Discharge coefficient {[}Dimensionless{]}
+
+�\(_{ave}\) = Average air density between the lower and upper zones {[}Pa{]}
+
+ΔP~ = Pressure difference P\(_{L}\) - P\(_{U}\) {[}Pa{]}
+
+2)~~~~~~~~~~~P\(_{L}\) \textless{} P\(_{U}\)
+
+\({\mathop m\limits^ \bullet_{_L}}\) = 0
+
+\begin{equation}
+{\mathop m\limits^ \bullet_U} =  - {\rho_U}A{C_d}{\left( {\frac{{2\left| {\Delta P} \right|}}{{{\rho_{ave}}}}} \right)^{0.5}}
+\end{equation}
+
+\begin{equation}
+\frac{{\partial \mathop {{m_U}}\limits^ \bullet  }}{{\partial {P_L}}} = {\rho_U}A{C_d}{\left( {\frac{1}{{2\left| {\Delta P} \right|{\rho_{ave}}}}} \right)^{0.5}}
+\end{equation}
+
+where\textbf{:}
+
+�\(_{U}\)~~ = Air density in the upper zone {[}kg/m\(^{3}\){]}
+
+A~~~ = Opening area {[}m\(^{2}\){]}
+
+C\(_{d}\) = Discharge coefficient {[}Dimensionless{]}
+
+�\(_{ave}\) = Average air density between the lower and upper zones {[}Pa{]}
+
+ΔP~ = Pressure difference P\(_{L}\) - P\(_{U}\) {[}Pa{]}
+
+\paragraph{Buoyancy airflows}\label{buoyancy-airflows}
+
+Buoyancy flow only occurs when the air density in the upper zone is greater than the air density in the lower zone. The flow is bi-directional and the amount of upper flow is equal to the lower flow across the opening. The following discussion assumes the air density in the upper zone is greater than the air density in the lower zone. Otherwise, the buoyancy flow rate is equal to zero. It is also assumed that the maximum buoyancy flow occurs when the pressure difference across the opening due to forced airflows is zero. The maximum buoyancy flow may be expressed as a part of Cooper's model:
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{buo,\max }} = {\rho_{ave}}*0.055{\left( {\frac{{g\left| {\Delta \rho } \right|D_{_H}^5}}{{{\rho_{ave}}}}} \right)^{0.5}}
+\end{equation}
+
+where:
+
+\({\mathop m\limits^ \bullet_{_{buo,\max }}}\) ~ = Buoyancy mass flow rate at zero forced airflow pressure difference {[}kg/s{]}
+
+g~~~ = Gravity acceleration {[}m/s\(^{2}\){]}
+
+D\(_{H}\) = Hydraulic diameter {[}m{]}
+
+�\(_{ave}\) = Average air density between the lower and upper zones {[}kg/m\(^{3}\){]}
+
+Δ�~ = Density difference between the lower and upper zones {[}kg/m\(^{3}\){]}
+
+\paragraph{Combined airflows}\label{combined-airflows}
+
+When forced and buoyancy flows co-exist, it is possible to have either unidirectional or bi-directional flows. For example, when the upward force due to pressure difference is greater than the buoyancy force (downward), unidirectional flow occurs. Bi-directional flow only occurs when the upward imposed force is less than the buoyancy force. The critical pressure between unidirectional and bi-directional flows is called the purge pressure (Tan and Jaluria 1992). The purge pressure is a function of opening geometry and the buoyancy force (ΔP/(gΔ�D\(_{H}\))) and may be expressed as (Cooper 1998):
+
+\begin{equation}
+\Delta {P_{Flood}} = \left| {C_{Shape}^2\frac{{g\Delta \rho D_H^5}}{{2{A^2}}}} \right|
+\end{equation}
+
+where:
+
+ΔP\(_{Flood}\) = Purging pressure {[}Pa{]}
+
+g~~~ = Gravity acceleration {[}m/s\(^{2}\){]}
+
+D\(_{H}\) = Hydraulic diameter {[}m{]}
+
+A~~~ = Opening area {[}m\(^{2}\){]}
+
+Δ�~ = Density difference between the lower and upper zones {[}kg/m\(^{3}\){]}
+
+C\(_{Shape}\) = Shape factor {[}dimensionless{]}
+
+\begin{equation}
+C_{Shape}^{} = \left\{ \begin{array}{l}0.754\;\;\;{\rm{for}}\;{\rm{a}}\;{\rm{circle}}\;{\rm{opening}}\\0.942(w/D)\;{\rm{for}}\;{\rm{a}}\;{\rm{rectangle}}\;{\rm{opening}}\end{array} \right\}
+\end{equation}
+
+where:
+
+w~~~ = Opening width {[}m{]}
+
+D~~~ = Opening depth {[}m{]}
+
+As mentioned above, when the air pressure difference between two zones is zero there is the maximum bi-directional flow due to the buoyancy force. When the pressure difference increases from 0 and is less than \textbar{}ΔP\(_{Flood}\)\textbar{}, there is some bi-directional flow across the opening, but less than the maximum flow. If the pressure difference keeps increasing and exceeds \textbar{}ΔP\(_{Flood}\)\textbar{}, there is no bi-directional flow.~ Cooper's model assumes the buoyancy flow varies linearly with pressure difference.
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{buo}} = \left\{ \begin{array}{l}{\mathop m\limits^ \bullet_{buo,\max }}*\left( {1 - \frac{{\left| {\Delta P} \right|}}{{\left| {\Delta {P_{Flood}}} \right|}}} \right)\;\,\,If\;\Delta \rho  > 0\;and\;\frac{{\left| {\Delta P} \right|}}{{\left| {\Delta {P_{Flood}}} \right|}} < 1\\0\;\,\,\,Otherwise\end{array} \right\}
+\end{equation}
+
+The total air flow across the opening is based on superposition of the forced and buoyancy flows, and may be expressed for three different pressure difference scenarios as follows:
+
+a.~~~~~~~~~~~~~~~~~~~~~~~~~~~~P\(_{L}\) = P\(_{U}\)
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{_U}} = {\mathop m\limits^ \bullet_{buo}}
+\end{equation}
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{_L}} = {\mathop m\limits^ \bullet_{buo}}
+\end{equation}
+
+\begin{equation}
+\frac{{{{\mathop {\partial m}\limits^ \bullet  }_L}}}{{\partial {P_L}}} = 0
+\end{equation}
+
+b.~~~~~~~~~~~~~~~~~~~~~~~~~~~P\(_{L}\) \textgreater{} P\(_{U}\)
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{_U}} = {\mathop m\limits^ \bullet_{buo}}
+\end{equation}
+
+\begin{equation}
+{\mathop m\limits^ \bullet_L} = {\rho_L}A{C_d}{\left( {\frac{{2\Delta P}}{{{\rho_{ave}}}}} \right)^{0.5}} + {\mathop m\limits^ \bullet_{buo}}
+\end{equation}
+
+\begin{equation}
+\frac{{{{\mathop {\partial m}\limits^ \bullet  }_L}}}{{\partial {P_L}}} = {\rho_L}A{C_d}{\left( {\frac{1}{{2\Delta P{\rho_{ave}}}}} \right)^{0.5}} - \frac{{{{\mathop m\limits^ \bullet  }_{buo,\max }}}}{{\left| {\Delta {P_{Flood}}} \right|}}
+\end{equation}
+
+where:
+
+�\(_{L}\)~~ = Air density in the lower zone {[}kg/m\(^{3}\){]}
+
+A~~~ = Opening area {[}m\(^{2}\){]}
+
+C\(_{d}\) = Discharge coefficient {[}dimensionless{]}
+
+Ρ\(_{ave}\) = Average air density between the lower and upper zones {[}Pa{]}
+
+ΔP~ = Pressure difference P\(_{L}\) - P\(_{U}\) {[}Pa{]}
+
+c.~~~~~~~~~~~~~~~~~~~~~~~~~~~~P\(_{L}\) \textless{} P\(_{U}\)
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{_L}} = {\mathop m\limits^ \bullet_{buo}}
+\end{equation}
+
+\begin{equation}
+{\mathop m\limits^ \bullet_U} =  - {\rho_U}A{C_d}{\left( {\frac{{2\left| {\Delta P} \right|}}{{{\rho_{ave}}}}} \right)^{0.5}} + {\mathop m\limits^ \bullet_{buo}}
+\end{equation}
+
+\begin{equation}
+\frac{{\partial \mathop {{m_U}}\limits^ \bullet  }}{{\partial {P_L}}} = {\rho_U}A{C_d}{\left( {\frac{1}{{2\left| {\Delta P} \right|{\rho_{ave}}}}} \right)^{0.5}} + \frac{{{{\mathop m\limits^ \bullet  }_{buo,\max }}}}{{\left| {\Delta {P_{Flood}}} \right|}}
+\end{equation}
+
+\emph{Sloping plane}
+
+\begin{figure}[hbtp] % fig 151
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2741.png}
+\caption{A Staircase is attached to the horizontal opening. \protect \label{fig:a-staircase-is-attached-to-the-horizontal}}
+\end{figure}
+
+When a staircase is introduced as shown in Figure~\ref{fig:a-staircase-is-attached-to-the-horizontal}, the effective opening area will be used to replace A (opening area) in the above equations. The effective area may be estimated as (Bolmqvist and Sandberg 2004):
+
+\begin{equation}
+{A_{eff}} = A\sin \alpha (1 + \cos \alpha )
+\end{equation}
+
+where:
+
+A\(_{eff}\)~ = Effective area of horizontal opening {[}m\(^{2}\){]}
+
+A~~~ = Area of horizontal opening {[}m\(^{2}\){]}
+
+α~~~ = Angle between the stair plane and horizontal opening plane {[}degrees{]}
+
+Note: the hydraulic diameter calculation is based on the effective opening area, while the opening depth remains the same.
+
+Figure~\ref{fig:flow-rates-at-different-pressure-differences} demonstrates possible forced and buoyancy flow rates at different ratios of pressure difference to purging pressure across a horizontal opening when the upper zone air density is greater than the lower zone air density. The pressure difference is the lower zone pressure minus the upper zone pressure. Otherwise, the buoyancy flow is zero. In addition, when the absolute ratio is above 1, the buoyancy flow is also zero. The following table provides a brief description for the legend listed in Figure~\ref{fig:flow-rates-at-different-pressure-differences}.
+
+% table 49
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Legend Description \label{table:legend-description}} \tabularnewline
+\toprule 
+Legend & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Legend Description} \tabularnewline
+\toprule 
+Legend & Description \tabularnewline
+\midrule
+\endhead
+
+Forced downward & Forced flow rate from upper to lower at P  -P    <  0 \tabularnewline
+Forced upward & Forced flow rate from lower to upper at P  -P    >  0 \tabularnewline
+Buoyancy upward & Total upward flow rate due to buoyancy only at P  -P    <  0 \tabularnewline
+Buoyancy downward & Total downward flow rate due to buoyancy only at P  -P    >  0 \tabularnewline
+Combined downward & Total downward flow at P  -P    <  0 (Forced downward + buoyancy upward) \tabularnewline
+Combined upward & Total upward flow at P  -P    >  0 (Forced upward + buoyancy downward) \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{figure}[hbtp] % fig 152
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2743.svg.png}
+\caption{Flow rates at different pressure differences \protect \label{fig:flow-rates-at-different-pressure-differences}}
+\end{figure}
+
+\subsubsection{Wind pressure calculations}\label{wind-pressure-calculations}
+
+The wind pressure is determined by Bernoulli's equation, assuming no height change or pressure losses:
+
+\begin{equation}
+{p_w} = {C_p}\rho \frac{{{V_{ref}}^2}}{2}
+\end{equation}
+
+where:
+
+\emph{p\(_{w}\)}~~~~~~~~~~~ = Wind surface pressure relative to static pressure in undisturbed flow {[}Pa{]}
+
+\emph{�}~~~~~~~~~~~~~~~ = Air density {[}kg/m\(^{3}\){]}
+
+\emph{V\(_{ref}\)}~~~~~~~~~~~~ = Reference wind speed at local height {[}m/s{]}
+
+\emph{C\(_{p}\)}~~~~~~~~~~~~~ = Wind surface pressure coefficient {[}dimensionless{]}
+
+\emph{V\(_{ref}\)} may be expressed as (Ref, Local Wind Speed Calculations):
+
+\begin{equation}
+{V_{ref}} = {V_{met}}{\left( {\frac{{{\delta_{met}}}}{{{z_{met}}}}} \right)^{{\alpha_{met}}}}{\left( {\frac{z}{\delta }} \right)^\alpha }
+\end{equation}
+
+\emph{C\(_{p}\)} is a function of location on the building envelope and wind direction. When Wind Pressure Coefficient Type = ``INPUT'', the\emph{C\(_{p}\)} values are explicitly defined in the input for AirflowNetwork:Multizone:Wind Pressure Coefficient Values. When Wind Pressure Coefficient Type = ``AVERAGE-SURFACE CALCULATION'' and the building shape is rectangular, the program uses the following equations to calculate wind pressure coefficient (\emph{C\(_{p}\)}) values for different wind directions. For a low rise building, the normalized surface pressure coefficient may be written as (Swami and Chandra 1988):
+
+\begin{equation}
+{C_{p,n}} = 0.6*\ln \left[ \begin{array}{l}1.248 - 0.703\sin (\alpha /2) - 1.175{\sin ^2}(\alpha ) + 0.131{\sin ^3}(2\alpha G)\\ + \,0.769\cos (\alpha /2) + 0.07{G^2}{\sin ^2}(\alpha /2) + 0.717{\cos ^2}(\alpha /2)\end{array} \right]
+\end{equation}
+
+where
+
+\emph{C\(_{p,n}\)}~~~~~~~~~~~ = \emph{C\(_{p}\)} value at a given angle between wind direction and the outward normal of the surface under consideration {[}dimensionless{]}
+
+α~~~ ~~~~~~~~~~~ = Angle between wind direction and outward normal of wall under consideration {[}deg{]}
+
+\emph{G}~~ ~~~~~~~~~~~ = Natural log of the ratio of the width of the wall under consideration to the width of the adjacent wall {[}dimensionless{]}
+
+\emph{n} ~~ ~~~~~~~~~~~ = Index of incident angle at 30-degree increments
+
+For walls of a high rise building, a two-dimensional array of surface-averaged wind pressure coefficients is generated based on wind incident angle and side ratio. The wind pressure coefficients are provided in 2001 ASHRAE Fundamentals Handbook, p.~16.5, Fig. 7, ``Surface Averaged Wall Pressure Coefficients for Tall Buildings''. The original work was performed by Atkins et al. (1979). The incident angle has an increment of 30 degrees. The side ratio values are 0.25, 1.0, and 4.0. For a given incident angle and building aspect ratio, the program uses linear interpolation to calculate the corresponding wind pressure coefficient \emph{C\(_{p,n}\)}.
+
+For the roof of a high rise building, a two-dimensional array of surface-averaged wind pressure coefficients is also generated based on wind incident angle and side ratio. The wind pressure coefficients are provided in 2001 ASHRAE Fundamentals Handbook, p.~16.6, Fig. 9, ``Surface Averaged Roof Pressure Coefficients for Tall Buildings''. The original work was performed by Holmes (1986). The incident angle has an increment of 30 degrees. The side ratio values are 0.25, 1.0, and 4.0. At a given wind incident angle and building aspect ratio, the program uses linear interpolation to calculate the corresponding wind pressure coefficient \emph{C\(_{p,n}\)}.
+
+The wind surface pressure at the given incident angle can be calculated by combining the above two equations:
+
+\begin{equation}
+{p_{w,n}} = {C_{p,n}}\rho \frac{{{V_{ref}}^2}}{2}
+\end{equation}
+
+\subsubsection{Solution method}\label{solution-method}
+
+Based on the relationship between airflow rate and pressure drop for each component, a system of equations for all components can be assembled together in an n x n square matrix, where n is the number of nodes. Newton's method is used to iteratively solve for the air pressure at each node. A new estimated vector for all node pressures, \{P\}*, is computed from the current estimated vector of node pressures, \{P\}, by:
+
+\begin{equation}
+{\left\{ P \right\}^*} = \left\{ P \right\} - \left\{ C \right\}
+\end{equation}
+
+where the correction vector, \{C\}, is computed by the matrix relationship:
+
+\begin{equation}
+\left[ J \right]\left\{ C \right\} = \left\{ B \right\}
+\end{equation}
+
+\{B\} is a column vector with each component given by:
+
+\begin{equation}
+{B_n} = \sum\limits_i {\mathop {{m_i}}\limits^ \bullet  }
+\end{equation}
+
+where n is the node number and i indicates all flow paths connecting node n to other nodes, and {[}J{]} is the square Jacobian matrix whose elements are given by:
+
+\begin{equation}
+{J_{n,m}} = \sum\limits_i {\frac{{\partial \mathop m\limits^ \bullet  }}{{\partial {P_m}}}}
+\end{equation}
+
+\subsubsection{Convergence acceleration}\label{convergence-acceleration}
+
+The convergence tolerance is used to check the sum of the mass flow rates by applying mass conservation. The convergence acceleration equation shown below is used to correct the node pressures to more rapidly obtain a solution. By assuming a constant ratio of correction values from one iteration to the next, the following method is applied:
+
+\begin{equation}
+{P_n}^* = {P_n} - {C_n}/(1 - r)
+\end{equation}
+
+where
+
+\emph{r}~~~~ = the ratio of C\(_{n}\) for the current iteration to its value for the previous iteration {[}dimensionless{]}
+
+\emph{C\(_{n}\)}~ = Correction value at the n\(_{th}\) node {[}Pa{]}
+
+\emph{P\(_{n}\)} = Estimated pressure at the n\(_{th}\) node {[}Pa{]}
+
+\emph{P\(_{n}\)\(^{\*}\)} = Corrected pressure at the n\(_{th}\) node used in the next iteration {[}Pa{]}
+
+This method is similar to a Steffensen iteration (Conte and de Boor 1972) which is used as a fixed-point iteration method for individual nonlinear equations.
+
+The iteration correction method presented in the above equation gives a variable factor. When the solution is close to convergence, the solution method converges quadratically. By limiting cases where the value of r is less than some value, such as -0.5, the solution will not interfere with the rapid convergence. It has not been proven that the convergence acceleration equation will always lead to convergence, but it can be shown that it will not prevent convergence. Newton's method converges when the estimated solution values are within some distance, called the radius of convergence, or the correct solution. Applying the convergence acceleration equation when -1 \textless{} r \textless{}0, will cause a smaller correction than Newton's method, which therefore, can not force the iterations outside the radius of convergence. When r\textless{}-1, the solution diverges in an oscillatory fashion. When r\textgreater{}1, the solution also diverges, but in a nonoscillatory manner. For 0\textless{}r\textless{}1, the solution is approached from one direction. In all three cases, the convergence acceleration equation applies as long as r is truly constant over several iterations. However, for the last case, this involves a true extrapolation of correction factor which is very sensitive to the accuracy of r. This is most extreme for the case of r = 1, which would cause an infinite correction.
+
+\subsection{Node Temperature Calculations}\label{node-temperature-calculations}
+
+A brief description of the air node temperature calculation is given below. A detailed description can be found in the work of Swami et al. (1992). The following equation is used to calculate temperature distribution across a duct element at the given airflow rate and inlet air temperature:
+
+\begin{equation}
+\mathop m\limits^ \bullet  {C_p}\frac{{dT}}{{dx}} = UP(T{}_\infty  - T)
+\end{equation}
+
+where
+
+\emph{C\(_{p}\)}~ = Specific heat of airflow {[}J/kg•K{]}
+
+\(\mathop m\limits^ \bullet\) ~ = Airflow rate {[}kg/s{]}
+
+\emph{P}~~~ = Perimeter of a duct element {[}m{]}
+
+\emph{T}~~~ = Temperature as a field variable {[}°C{]}
+
+\(T{}_\infty\) ~~~~~~~~~~~ = Temperature of air surrounding the duct element {[}°C{]}
+
+\emph{U}~~ = Overall heat transfer coefficient {[}W/m\(^{2}\)•K{]}
+
+\begin{equation}
+U = \frac{1}{{\frac{1}{{{h_i}}} + \frac{1}{{{h_o}}} + \sum {\frac{{{t_j}}}{{{k_j}}}} }}
+\end{equation}
+
+\emph{h\(_{i}\)}~~~~~~~~ = Inside heat transfer coefficient {[}W/m\(^{2}\)•K{]}
+
+\emph{h\(_{o}\)} = Outside heat transfer coefficient {[}W/m\(^{2}\)•K{]}
+
+\emph{t\(_{j}\)}~~~~~~~~~ = Thickness at j-th layer {[}m{]}
+
+\emph{k\(_{j}\)}~~~~~~~~~ = Thermal conductivity at j-th layer {[}W/m•K{]}
+
+The outlet air temperature at the end of the duct (x = L) is:
+
+\begin{equation}
+{T_o} = {T_\infty } + ({T_i} - {T_\infty })*\exp \left( { - \frac{{UA}}{{\mathop {m{C_p}}\limits^ \bullet  }}} \right)
+\end{equation}
+
+where
+
+~~~~~ \emph{T\(_{i}\)}~~~~~~~~ = Inlet air temperature {[}°C{]}
+
+~~~~~ \emph{T\(_{o}\)}~~~~~~~~ = Outlet air temperature {[}°C{]}
+
+~~~~~ \emph{T\(_{∞}\)}~~~~~~~ = Temperature of air surrounding the duct element {[}°C{]}
+
+~~~~~ \emph{A}~~~~~~~~~ = Surface area (Perimeter * Length) {[}m\(^{2}\){]}
+
+The heat transfer by convection to ambient, \emph{Q}, is:
+
+\begin{equation}
+Q = \mathop m\limits^ \bullet  {C_p}({T_\infty } - {T_i})\left[ {1 - \exp \left( { - \frac{{UA}}{{\mathop {m{C_p}}\limits^ \bullet  }}} \right)} \right]
+\end{equation}
+
+The outlet air temperature can be calculated using the above equation at the given inlet air temperature. Since the inlet temperature at one linkage is the outlet temperature for the connected linkage, the outlet air temperatures at all nodes are solved simultaneously. A square linear system assembled by the AirflowNetwork model is expressed below:
+
+\begin{equation}
+\{ M\} [T] = [B]
+\end{equation}
+
+where
+
+~~~~~ \{M\}~~~~~~ = Airflow matrix
+
+~~~~~ {[}T{]}~~~~~~~ = Temperature vector
+
+~~~~~ {[}B{]}~~~~~~~ = Given boundary conditions
+
+The zone air temperatures and primary air loop component (fan and coils) outlet conditions are used as prescribed conditions in the AirflowNetwork model. In addition, the temperature difference across zone loop components (terminal units) is held constant during the calculations. For example, thermal zone temperatures calculated during the previous system time step are used as prescribed temperatures when calculating all other node temperatures. The zone air temperature is assumed constant (prescribed) throughout the AirflowNetwork iterative solution. The fan and coil outlet air temperatures, and terminal unit temperature differences are assumed constant within an AirflowNetwork iteration. The sensible heat gains calculated during the AirflowNetwork solution are then used to predict a new zone air temperature.
+
+\subsection{Node Humidity Ratio Calculations}\label{node-humidity-ratio-calculations}
+
+A brief description of the air node humidity ratio calculation is given below. A detailed description can found in the work of Swami et al. (1992). The following equation is used to calculate humidity ratio distribution across a duct element at the given airflow rate and inlet air humidity ratio:
+
+\begin{equation}
+\mathop m\limits^ \bullet  \frac{{dW}}{{dx}} = {U_m}P(W{}_\infty  - W)
+\end{equation}
+
+where
+
+\(\mathop m\limits^ \bullet\) ~~~~~~~~~~~~ = Airflow rate {[}kg/s{]}
+
+\emph{P~~~}~~~~~~~~~~~ = Perimeter of a duct element {[}m{]}
+
+\emph{W~~}~~~~~~~~~~~ = Humidity ratio {[}kg/kg{]}
+
+\(W{}_\infty\) ~~~~~~~~~~ = Humidity ratio of air surrounding the duct element {[}kg/kg{]}
+
+\emph{U\(_{m}\)}~~~~~~~~~~~~ = Overall moisture transfer coefficient {[}kg/m\(^{2}\)•s{]}
+
+\begin{equation}
+{U_m} = \frac{1}{{\frac{1}{{{h_{m,i}}}} + \frac{1}{{{h_{m,o}}}} + \sum {\frac{{{t_j}}}{{{D_j}}}} }}
+\end{equation}
+
+\emph{h\(_{m,i}\)} ~~~~~~~~~~~ = Inside moisture transfer coefficient {[}kg/m\(^{2}\)•s{]}
+
+\emph{h\(_{m,o}\)} = Outside moisture transfer coefficient {[}kg/m\(^{2}\)•s{]}
+
+\emph{t\(_{j}\)}~~~~~~~~~~~~~~~ = Thickness at j-th layer {[}m{]}
+
+D\(_{j}\)~~~~~~~~~~~~~~ = Moisture diffusivity at j-th layer {[}kg/m•s{]}
+
+The outlet air humidity ratio at the end of the duct (x = L) is:
+
+\begin{equation}
+{W_o} = {W_\infty } + ({W_i} - {W_\infty })*\exp \left( { - \frac{{{U_m}A}}{{\mathop m\limits^ \bullet  }}} \right)
+\end{equation}
+
+where
+
+\emph{W\(_{i}\)}~~~~~~~~~~~~~ = Inlet air humidity ratio {[}kg/kg{]}
+
+\emph{W\(_{o}\)}~~~~~~~~~~~ = Outlet air humidity ratio {[}kg/kg{]}
+
+\emph{A}~~~~~~~~~~~~~~~ = Surface area (Perimeter * Length) {[}m\(^{2}\){]}
+
+The moisture transfer by convection to ambient, \emph{Q\(_{m}\)}, is
+
+\begin{equation}
+{Q_m} = \mathop m\limits^ \bullet  ({W_\infty } - {W_i})\left[ {1 - \exp \left( { - \frac{{{U_m}A}}{{\mathop m\limits^ \bullet  }}} \right)} \right]
+\end{equation}
+
+The outlet air humidity ratio can be calculated using the above equation at the given inlet air humidity ratio. Since the inlet humidity ratio at one linkage is the outlet humidity ratio for the connected linkage, the outlet air humidity ratio at all nodes are solved simultaneously. A square linear system assembled by the AirflowNetwork model is expressed below:
+
+\begin{equation}
+\{ {M_m}\} [W] = [{B_m}]
+\end{equation}
+
+where
+
+\{M\(_{m}\)\}~~~~~~~~~~~ = Airflow matrix
+
+{[}W{]}~~~~~~~~~~~~ = Humidity ratio vector
+
+{[}B\(_{m}\){]}~~~~~~~~~~~~~~~~~~~~~~~ = Given boundary conditions
+
+The zone air humidity ratios and primary air loop component (fan and coils) outlet conditions are used as prescribed conditions in the AirflowNetwork model. For example, thermal zone humidity ratios calculated during the previous system time step are used as prescribed humidity ratios when calculating all other node humidity ratios. The zone air humidity ratio is assumed constant (prescribed) throughout the AirflowNetwork iterative solution. The coil outlet air humidity ratio is assumed constant within an AirflowNetwork iteration. The latent heat gains calculated during the AirflowNetwork solution are then used to predict a new zone air humidity ratio.
+
+\subsection{Sensible and Latent Load Calculations}\label{sensible-and-latent-load-calculations}
+
+The zone sensible and latent loads calculated in the AirflowNetwork model consist of multizone, duct conduction and leakage. In addition, the impact of infiltration and mixing is accounted for in this calculation. The multizone load only includes incoming airflows from outside (infiltration) and other adjacent zones (mixing) with and without forced-air fan operation. It is divided into two terms: variable and constant. The constant term is the sum of the mass flow rate multiplied by the specific heat for both infiltration and mixing. The variable term includes the impact of zone and outdoor air temperature. Each of these terms is used in the zone energy balance equation. The sensible load items from the multizone load calculations may be written as follows:
+
+\begin{equation}
+MC{P_{airflow}} = \mathop {{m_{\inf }}}\limits^\cdot  {C_p} + \sum {\left( {\mathop {{m_{mix}}}\limits^\cdot  {C_p}} \right)}
+\end{equation}
+
+\begin{equation}
+MCP{T_{airflow}} = \mathop {{m_{\inf }}}\limits^\cdot  {C_p}{T_{amb}} + \sum {\left( {\mathop {{m_{mix}}}\limits^\cdot  {C_p}{T_{zone}}} \right)}
+\end{equation}
+
+where
+
+\emph{MCP\(_{airflow}\)} = Sum of air mass flow rate multiplied by specific heat for infiltration and mixing {[}W/K{]}
+
+\emph{MCPT\(_{airflow}\)} = Sum of air mass flow rate multiplied by specific heat and temperature for infiltration and mixing {[}W{]}
+
+\({\mathop m\limits^\cdot_{\inf }}\) ~~~~~~~~~~ = Incoming air mass flow rate from outdoors {[}kg/s{]}
+
+\({\mathop m\limits^\cdot_{mix}}\) ~~~~~~~~~ = Incoming air mass flow rate from adjacent zones {[}kg/s{]}
+
+\emph{T\(_{amb}\)}~~~~~~~~~~~ = Outdoor air dry-bulb temperature {[}°C{]}
+
+\emph{T\(_{zone}\)}~~~~~~~~~~ = Adjacent zone air temperature {[}°C{]}
+
+The latent load items from multizone load calculations may be written as follows:
+
+\begin{equation}
+{M_{airflow}} = \mathop {{m_{\inf }}}\limits^\cdot   + \sum {\mathop {{m_{mix}}}\limits^\cdot  }
+\end{equation}
+
+\begin{equation}
+M{W_{airflow}} = \mathop {{m_{\inf }}}\limits^\cdot  {W_{amb}} + \sum {\mathop {{m_{mix}}}\limits^\cdot  } {W_{zone}}
+\end{equation}
+
+where
+
+\emph{M\(_{airflow}\)} = Sum of air mass flow rates for infiltration and mixing {[}kg/s{]}
+
+\emph{MW\(_{airflow}\)} = Sum of air mass flow rate multiplied by humidity ratio for infiltration and mixing {[}kg/s{]}
+
+\({\mathop m\limits^\cdot_{\inf }}\) ~~~~~~~~~~ = Incoming air mass flow rate from outdoors {[}kg/s{]}
+
+\({\mathop m\limits^\cdot_{mix}}\) ~~~~~~~~~ = Incoming air mass flow rate from adjacent zones {[}kg/s{]}
+
+\emph{W\(_{amb}\)}~~~~~~~~~~ = Outdoor air humidity ratio {[}kg/kg{]}
+
+\emph{W\(_{zone}\)}~~~~~~~~~ = Adjacent zone air humidity ratio {[}kg/kg{]}
+
+The air distribution system (ADS) loads due to duct conduction and leakage depend on the air distribution system component (e.g., duct) location. The air distribution system sensible and latent loads are calculated for each zone as follows:
+
+\begin{equation}
+{Q_{ADS,i}} = \sum\limits_j {{Q_{cond(i,j)}} + } \sum\limits_j {{Q_{leak(i,j)}}}
+\end{equation}
+
+\begin{equation}
+{Q_{ADS,m,i}} = \sum\limits_j {{Q_{cond,m(i,j)}} + } \sum\limits_j {{Q_{leak,m(i,j)}}}
+\end{equation}
+
+where
+
+\emph{Q\(_{ADS,i}\)}~~~~~~~~ = Total sensible load in the i-th zone due to ADS losses {[}W{]}
+
+\emph{Q\(_{cond(ij)}\)}~~~~~~ = Duct wall conduction loss at the j-th duct located in the i-th zone {[}W{]}
+
+\emph{Q\(_{leak(ij)}\)}~~~~~~~ = Sensible supply leak loss at the j-th linkage located in the i-th zone {[}W{]}
+
+\emph{Q\(_{ADS,m,i}\)}~~~~~~ = Total latent load in the i-th zone due to ADS losses {[}kg/s{]}
+
+\emph{Q\(_{cond,m(ij)}\)} = Duct wall vapor diffusion loss at the j-th duct located in the i-th zone {[}kg/s{]}
+
+\emph{Q\(_{leak,m(ij)}\)} = Latent supply leak loss at the j-th linkage located in the i-th zone {[}kg/s{]}
+
+\subsection{Impacts of Supply Air Constant Volume Fan Control on Load: Cycling vs.~Continuous}\label{impacts-of-supply-air-constant-volume-fan-control-on-load-cycling-vs.continuous}
+
+The AirflowNetwork model currently allows two types of constant volume fans: Fan:ConstantVolume and Fan:OnOff. The Fan:ConstantVolume object has only one type of supply air fan operation mode: continuous fan, cycling compressor (ContinuousFanWithCyclingCompressor). However, the Fan:OnOff has two types of supply air fan operation modes: cycling fan, cycling compressor (CyclingFanAndCompressor) or continuous fan, cycling compressor (ContinuousFanWithCyclingCompressor). The CyclingFanAndCompressor operation mode is frequently referred to as ``AUTO fan'', where the compressor(s) and supply air fan operate in unison to meet the zone heating or cooling load, and cycle off together when the heating or cooling load has been met. The ContinuousFanWithCyclingCompressor operation mode is often referred to as ``fan ON'', where the compressor(s) cycle on and off to meet the zone heating or cooling load but the supply air fan operates continuously regardless of compressor operation. The supply air fan operation mode is specified in an HVAC system object based on a given fan operation mode schedule (e.g., AirLoopHVAC:UnitaryHeatCool object).
+
+The determination of the zone sensible and latent loads caused by multizone airflows and forced air distribution system operation is dependent on the supply air fan operation mode (see Sensible and Latent Load Calculations section above). The zone loads calculated by the AirflowNetwork model are added to zone sensible and latent balances in the ZonePredictorCorrector module to calculate zone air temperatures and humidity ratios (see Integration of the AirflowNetwork Model section below). For the case of continuous fan/cycling compressor, the zone loads during forced air distribution system operation are calculated with the system design air mass flow rate without modification, since the system air node conditions (temperature and humidity) reflect the average values for the time step considering the coil/fan on and off periods during the time step.
+
+For the case of cycling fan/cycling compressor, where the forced air distribution system can operate for a portion of the simulation time step, the airflows are determined based on the air distribution system part-load ratio (ratio of the average air mass flow rate for the time step divided by the design air mass flow rate). The \textbf{airflows} for the AirflowNetwork:Distribution:Linkage objects are reported during the air distribution system on cycle, since no airflow is assumed during the system off cycle. The \textbf{airflows} for the AirflowNetwork:Multizone:Surface objects are weighted by the air distribution system part-load ratio. The \textbf{zone loads} are the sum of energy losses during both the air distribution system on and off cycle at each system time step. The energy losses when the air distribution system is on are calculated using the system ``on'' air flow rate multiplied by the air distribution system run time fraction. The energy losses when the air distribution system is off are obtained from the multizone airflow calculations (without forced air through the air distribution system) and these losses are multiplied by (1.0 - system run time fraction), assuming no airflows through the air distribution system when the fan is off. The formulas used to calculate airflows and zone loads are given below:
+
+Airflow
+
+Airflow = Airflow during ADS on cycle * ADS Part-load ratio + Airflow during ADS off cycle * (1.0 -- ADS Part-load ratio)
+
+where ADS = Air Distribution System
+
+Zone load
+
+System run time fraction = Maximum run time fraction of coils and fans in the air distribution system
+
+Zone energy losses = Zone energy loss during ADS on cycle * System run time fraction + Zone energy loss during ADS off cycle * (1.0 - System run time fraction)
+
+The calculation of loads due to multizone airflow, without forced air distribution system operation, is performed when the HVAC system is first simulated during a simulation time step (FirstHVACIteration = True). The calculation of loads due to air distribution system operation is performed on subsequent iterations within the same simulation time step when the mass flow rate at the supply air fan inlet is greater than 0.0 (and FirstHVACIteration = False).
+
+\subsection{Airflow Calculation Procedure using A Supply Variable Air Volume Fan}\label{airflow-calculation-procedure-using-a-supply-variable-air-volume-fan}
+
+The AirflowNetwork model currently also allows a variable air volume fan type as Fan:VariableVolume. The allowed terminal type is AirTerminal:SingleDuct:VAV:Reheat only. Other types of terminals will be added later.
+
+In general, the supply fan air flow rate in a VAV central system is determined by a sum of terminal flow rates when the AirflowNetwork model is not applied. When the AirflowNetwork model is applied and the supply air fan flow rate is given, each terminal flow is determined by pressure resistance of each supply air pathway. It is possible that the delivered air flow rate from the pressure resistance at each terminal may be totally different from the desired flow rate determined by terminal units. Therefore, it is not easy to meet both requirements. The following compromised approach, including possible supply and return leaks in an air distribution system, is implemented.
+
+1.~Set up terminal airflows in the AirflowNetwork module based on the SimVAV subroutine in the HVACSingleDuctSystem module.
+
+2.~~~~Require AirflowNetwork:Distribution:Component:LeakageRatio objects to define supply leaks, so that the values of the Effective Leakage Ratio field are used to decide the supply fan flow rates. The base of the ratio will be actual supply fan flow rate, instead of the maximum fan flow rate used in the constant volume fan systems.
+
+3.~~~~Assign the supply fan airflow rate based on the sum of all terminal flow rates and all supply leak ratios until it reaches the maximum fan flow rate
+
+\begin{equation}
+{\dot m_{fan}} = \frac{{\mathop \sum \nolimits_i^n {{\dot m}_{i,terminal}}}}{{1 - \mathop \sum \nolimits_j^k {F_j}}}
+\end{equation}
+
+where
+
+\({\dot m_{fan}}\) ~~~~~~~~~ = The supply fan flow rate
+
+\({\dot m_{i,terminal}}\) ~~~ = The flow rate at the ith terminal, which is determined in the subroutine SimVAV in the HVACSingleDuctSystem module
+
+n~~~ = Number of terminals
+
+\({F_j}\) = The fraction of the supply fan flow rate at the jth supply leak, given in the AirflowNetwork:Distribution:Component:LeakageRatio objects.
+
+k~~~ = Number of supply leaks
+
+4.~~~~If the calculated supply fan flow rate is above the maximum limit of the supply fan flow rate, and the supply leak ratios remain the same, the supply fan flow rate is set to the maximum limit, and the terminal flow rates are reduced proportionally weighted by a ratio of the maximum supply fan flow rate by input to the calculated supply fan flow rate. Therefore, a sum of all terminal rates and all supply leak rates is equal to the maximum supply fan rate. \textbf{\emph{~}}
+
+\begin{equation}
+R = \frac{{{{\dot m}_{fan,max}}}}{{{{\dot m}_{fan,cal}}}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{i,terminal,final}} = {\dot m_{i,terminal}}*R
+\end{equation}
+
+where
+
+R~~~ = The ratio of the maximum fan flow rate given in the inputs to the requested fan flow rate based on the above equation
+
+\({\dot m_{fan,max}}\) ~~~~~ = The maximum supply fan flow rate by input
+
+\({\dot m_{fan,cal}}\) ~~~~~~ = The calculated supply fan flow rate
+
+\({\dot m_{i,terminal,final}}\) ~~~~~~~~~~ = The final flow rate at each terminal adjusted by the ratio
+
+\subsection{Airflow Calculation Procedure using inputs of Intrazone nodes and linkages}\label{airflow-calculation-procedure-using-inputs-of-intrazone-nodes-and-linkages}
+
+The inputs of both AirflowNetwork:IntraZone:Node and AirflowNetwork:IntraZone:Linkage objects are treated as normal model nodes and linkages. Therefore, the calculation procedures are the same as above.
+
+\subsection{Integration of the AirflowNetwork Model}\label{integration-of-the-airflownetwork-model}
+
+The loads calculated by the AirflowNetwork model are integrated into the EnergyPlus heat balance equation in a similar manner as described elsewhere in this document in the section ``Basis for the Zone and System Integration''. The mass flow rate summations and sensible and latent loads described in the previous section are included in the calculation of zone temperature and humidity ratio.
+
+The revised zone temperature update equation becomes:
+
+{\scriptsize
+\begin{equation}
+T_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {\mathop {{Q_i}}\limits^ \bullet  }  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + MCPTairflow + {{\mathop m\limits^ \bullet  }_{sys}}{C_p}{T_{{\rm{supply}}}} + QADS,z - \left( {\frac{{{C_z}}}{{\delta t}}} \right)\left( { - 3T_z^{t - \delta t} + \frac{3}{2}T_z^{t - 2\delta t} - \frac{1}{3}T_z^{t - 3\delta t}} \right)}}{{\left( {\frac{{11}}{6}} \right)\frac{{{C_z}}}{{\delta t}} + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} A + MCPairflow + {{\mathop m\limits^ \bullet  }_{sys}}C}}
+\end{equation}}
+
+Where MCPT\(_{airflow}\) is the sum of mass flow rate multiplied by specific heat and temperature for infiltration and mixing, Q\(_{ADS,z}\) is the added total sensible load in the zone due to Air Distribution System losses, and MCP\(_{airflow}\) is the sum of mass flow rate multiplied by specific heat for infiltration and mixing as calculated in the AirflowNetwork model described above.
+
+The revised coefficient (B) used in the zone humidity ratio calculation is shown below:
+
+\begin{equation}
+B = \sum {k{g_{mas{s_{{\rm{Sched Loads}}}}}}}  + M{W_{airflow}} + {\dot m_{sy{s_{in}}}}{W_{sys}} + \sum\limits_{i = 1}^{surfs} {{A_i}{h_{mi}}{\rho_{ai{r_z}}}{W_{surf{s_i}}}}  + QADS,m,z
+\end{equation}
+
+Where MW\(_{airflow}\) is the sum of mass flow rate multiplied by humidity ratio for infiltration and mixing and Q\(_{ADS,m,z\\}\)is the added total latent (moisture) load in the zone due to Air Distribution System losses from the AirflowNetwork model described above. This coefficient is used in the prediction of moisture as described in the section ``Moisture Predictor-Corrector'' found elsewhere in this document.
+
+\subsection{Model Output}\label{model-output}
+
+The available outputs from the AirflowNetwork model are described in the EnergyPlus Input Output Reference manual.
+
+\subsection{Occupant Ventilation Control}\label{occupant-ventilation-control}
+
+The AirflowNetwork:OccupantVentilationControl object enhances the AirflowNetwork model and provides more practical and advanced controls for window opening and closing operations, based on Marais \& Teichmann (2014). This control includes minimum open and closed time control, indoor thermal comfort control, and opening and closing probability controls.
+
+\subsubsection{Procedures of occupant ventilation control}\label{procedures-of-occupant-ventilation-control}
+
+It should be pointed that the open elapsed time and closed elapsed time are not independent. In other words, when one of the elapsed times value is greater than 0, then other elapsed time value must be equal to 0. The model is either tracking a window as open, in which case the open elapsed time grows, or as closed, in which case the closed elapsed time grows.
+
+The calculation procedures are presented in the following steps:
+
+Step 1: Open elapsed time check
+
+The model checks the open elapsed time first. When the open elapsed time is greater than 0 and less than the minimum opening time, a window will remain open. Otherwise, the model goes to Step 2.
+
+\begin{lstlisting}
+Open elapsed time > minimum open time
+\end{lstlisting}
+
+Step 2: Closed elapsed time check
+
+This step checks the closed elapsed time. When the closed elapsed time is greater than 0 and less than the minimum closed time, a window will remain closed. Otherwise, the model goes to Step 3.
+
+\begin{lstlisting}
+Closed elapsed time > minimum closed time
+\end{lstlisting}
+
+Step 3: Elapsed time only?
+
+When either the open elapsed time or the closed elapsed time is long enough (greater than the minimum time) and no other checks are needed, the model returns to the other ventilation control defined in the Ventilation Control Mode field in AirflowNetwork:MultiZone:Zone or AirflowNetwork:MultiZone:Surface. If other checks are needed, the following steps will be performed.
+
+Step 4: Thermal comfort temperature calculation
+
+The thermal comfort check requires the thermal comfort temperature and the comfort band. The comfort temperature of Tcomf is calculated as a function of the outdoor dry-bulb temperature Tout. The comfort temperature calculation may be based on two curves and a boundary temperature point.
+
+\begin{equation}
+T_{comf} = \left\{ \begin{array}{ll} \rm{Low Temp Curve,} & \min T_{out} < x \leq \rm{Boundary Point} \\ \rm{High Temp Curve,} & \rm{Boundary Point} \leq x < \max T_{out}  \end{array}\right.
+\end{equation}
+
+Step 5: Thermal band calculation
+
+The comfort band is calculated as a function of the design personal dissatisfaction PPD.
+
+\begin{equation}
+\theta = -0.0028 \left(100-\rm{PPD}\right)^2 + 0.3419 \left(100-\rm{PPD}\right) – 6.6275
+\end{equation}
+
+This equation is valid for PPD 0\% to 35\%
+
+Step 6: Upper boundary check of thermal comfort
+
+After calculation of the comfort temperature and band, the thermal comfort check will be performed using the zone air operative temperature Tg. The check consists of upper and lower boundary checks.
+
+The upper boundary check checks window opening status and uses the following logic:
+
+\begin{equation}
+T_g > \left(T_{comf} + \theta\right)
+\end{equation}
+
+If the above logic check is true, the opening probability check will be performed. The detailed description is given in the opening probability section.
+
+If the above logic check is false, no action is needed.
+
+If the opening probability check is true and upper boundary check is satisfied, a window will be opened, regardless of open/closed status at the previous time step. If the opening probability check is false and upper boundary check is satisfied, a window will remain at the status from the previous time step.
+
+\begin{equation}
+T_g > \left(T_{comf} + \theta\right) \&\& \rm{OpeningProbability}
+\end{equation}
+
+Step 7: Lower boundary check of thermal comfort
+
+The lower boundary check will follow the upper boundary check to check the window closing status, using the following logic.
+
+\begin{equation}
+T_g < \left(T_{comf} - \theta\right)
+\end{equation}
+
+If the above logic check is true, the closing probability check will be performed. The detailed description is given in the closing probability section.
+
+If the above logic check is false, no action is needed.
+
+If the closing probability check is true and lower boundary check is satisfied, a window will be closed, regardless of open/closed status at the previous time step. If the closing probability check is false and lower boundary check is satisfied, a window will remain at the status from the previous time step.
+
+\begin{equation}
+T_g < \left(T_{comf} - \theta\right) \&\& \rm{ClosingProbability}
+\end{equation}
+
+The output variables from the model are open status, opening probability status, and closing probability status. The detailed description of opening status is given in the Airflow Network Outputs section in the Input Output Reference.
+
+Note: The upper and lower boundary checks are not independent. In other words, when one of boundary check is satisfied, the other check will be dissatisfied.
+
+\subsubsection{Procedures of opening probability control}\label{procedures-of-opening-probability-control}
+
+Opening probability control provides an optional random number check. The control logic of opening probability is described in the following steps.
+
+Step 1: Closed elapsed time check
+
+This check requires that closed elapsed time is longer than the minimum closing time.
+
+Closed time \textgreater{} minimum closed time
+
+If the time duration is not long enough, the output is false so that a window remains closed.
+
+If the time duration is long enough, an occupancy check is performed.
+
+Step 2: Occupancy check
+
+If a zone is not occupied and the occupancy check is requested, the output is false. If the zone is occupied, the next step is to check the setpoints using zone air temperature at the previous time step as a reference.
+
+Step 3: Setpoint check
+
+There are 5 temperature control types. The following types are available:
+
+\begin{itemize}
+\item
+  No control: Bypass
+\item
+  Single heating setpoint: If Tzon \textgreater{} setpoint, go to next step. Otherwise, return false.
+\item
+  Single cooling setpoint: If Tzon \textless{} setpoint, go to next step. Otherwise, return false.
+\item
+  Single heating and cooling setpoint: no action by returning false
+\item
+  Dual heating and setpoints: If heating setpoint \textless{} Tzon \textless{} Cooling setpoint, go to next step. Otherwise, return false.
+\end{itemize}
+
+Step 4: Select bypass or opening probability check
+
+A choice is provided at this stage so that the opening probability check may be performed or bypassed. If bypassed, the output will be true to open a window. If performed, probability will be determined from a schedule.
+
+Step 5: Perform opening probability check
+
+The opening probability (OP) value is determined from a schedule.
+
+OP = Schedule value or specific function
+
+If the probability value is greater than a random number, the output is true.
+
+OP \textgreater{} random number (random number is between 0 and 1)
+
+Otherwise, the result will be false.
+
+\subsubsection{Procedures of closing probability control}\label{procedures-of-closing-probability-control}
+
+The control logic of closing probability is described as follows.
+
+Step 1: Open elapsed time check
+
+This check requires that open elapsed time is longer than the minimum opening time.
+
+Open time \textgreater{} minimum open time
+
+If the time duration is not long enough, the output is false and the window remains open. Otherwise, Step 2 will be performed.
+
+Step 2: Select by-pass or closing probability check
+
+A choice is provided at this step so that the closing probability check may be performed or bypassed. If bypassed, the output will be true to close a window. If performed, the closing probability will be calculated. The closing probability (CP) value is given from a schedule.
+
+CP = Schedule value or specific function
+
+If the closing probability check is performed and the closing probability is greater than a random number, the output is true.
+
+CP \textgreater{} random number (random number is between 0 and 1)
+
+Otherwise, the result will be false.
+
+\subsection{References}\label{references-004}
+
+Atkins, R. E., J. A. Peterka, and J. E. Cermak. 1979. ``Averaged pressure coefficients for rectangular buildings,'' Wind Engineering, Proceedings of the Fifth International Conference 7:369-80, Fort Collins, CO. Pergamon Press, NY.
+
+Bolmqvist, C. and M. Sandberg, 2004, ``Air Movements through Horizontal Openings in Buildings -- A Model Study,'' International Journal of Ventilation, Vol. 3, No. 1, pp.~1-9
+
+COMIS Fundamentals. 1990. Edited by Helmut E. Feustel and Alison Rayner-Hooson, LBL-28560, Lawrence Berkeley Laboratory, Berkeley, CA
+
+Conte, S. D. and C de Boor. 1972.Elementary Numerical Analysis: an Algorithmic Approach, McGraw-Hill.
+
+Cooper, L., 1989, ``Calculation of the Flow Through a Horizontal Ceiling/Floor Vent,'' NISTIR 89-4052, National Institute of Standards and Technology, Gaithersburg, MD
+
+Dols, W. S. \& G. N. Walton. 2002. ``CONTAMW 2.0 User Manual,'' NISTIR 6921, National Institute of Standards and Technology, Gaithersburg , Maryland
+
+Holmes, J. D. 1986. Wind Loads on low-rise buildings: The structural and environmental effects of wind on buildings and structures, Chapter 12, Faculty of Engineering, Monash University, Melbourne, Australia
+
+Marais, J. M. \& C. Teichmann, ``Window Simulation Methods Required for Manual Window Ventilated Buildings,'' Fifth German-Austrian IBPSA Conference, September 22-24, 2014, RWTH Aachen University, Germany
+
+Swami, M. V. and S. Chandra. 1988. Correlations for pressure distribution on buildings and calculation of natural-ventilation airflow, ASHRAE Transactions 94(1988) (Pt 1), pp.~243-266.
+
+Swami, M. V., L. Gu, \& V. Vasanth. 1992. ``Integration of Radon and Energy Models for Building,'' FSEC-CR-553-92, Florida Solar Energy Center, Cocoa, Florida
+
+Tan, Q. and Y. Jaluria, 1992, ``Flow through Horizontal Vents as Related to Compartment Fire Environments,'' NIST-GCR-92-607, National Institute of Standards and Technology, Gaithersburg, Maryland
+
+Walton, G. N. 1989. ``AIRNET -- A Computer Program for Building Airflow Network Modeling,'' NISTIR 89-4072, National Institute of Standards and Technology, Gaithersburg, Maryland
+
+Walton, G. N. \& W. S. Dols. 2003. ``CONTAM 2.1 Supplemental User Guide and Program Documentation,'' NISTIR 7049, National Institute of Standards and Technology, Gaithersburg, Maryland
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager.tex b/doc/engineering-reference/src/building-system-simulation-system-manager.tex
new file mode 100644
index 00000000000..964792d5638
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@@ -0,0 +1,3 @@
+\chapter{Building System Simulation System Manager / Processes}\label{building-system-simulation-system-manager-processes}
+
+EnergyPlus uses a loop based HVAC system formulation.~ An example of the dual duct VAV system is shown below.
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager/air-loop-simulation.tex b/doc/engineering-reference/src/building-system-simulation-system-manager/air-loop-simulation.tex
new file mode 100644
index 00000000000..9cc4b9959e6
--- /dev/null
+++ b/doc/engineering-reference/src/building-system-simulation-system-manager/air-loop-simulation.tex
@@ -0,0 +1,57 @@
+\section{Air Loop Simulation}\label{air-loop-simulation}
+
+A complete simulation of each primary air system -- zone equipment air loop is done in the following manner.
+
+\begin{itemize}
+\item
+  If this is the first simulation this system time-step, just call \emph{ManageAirLoops} (simulates the primary air systems) and \emph{ManageZoneEquipment} (simulates the zone equipment sets) once and quit. This initial pass is simulated with full design air flow rates and allows the zone equipment to set the flow rates for each zone that will meet the zone loads.
+\item
+  Otherwise loop over primary air systems and zone equipment sets until the temperatures, flow rates, enthalpies, humidity ratios etc. agree to within tolerance at each primary air system -- zone equipment gap. 
+\end{itemize}
+
+\begin{lstlisting}
+DO WHILE ((SimAirLoops .OR. SimZoneEquipment) .AND. (IterAir.LE.MaxAir) )   IF (SimAirLoops) THEN     CALL ManageAirLoops(FirstHVACIteration,SimAirLoops,SimZoneEquipment)     SimPlantDemandLoops = .TRUE     SimElecCircuits = .TRUE.   END IF
+\end{lstlisting}
+
+\begin{lstlisting}
+  IF (SimZoneEquipment) THEN     CALL ResolveAirLoopFlowLimits(IterAir+1)     CALL ManageZoneEquipment(FirstHVACIteration,SimZoneEquipment,SimAirLoops)     SimPlantDemandLoops = .TRUE.     SimElecCircuits = .TRUE.   END IF
+\end{lstlisting}
+
+\begin{lstlisting}
+  IterAir = IterAir + 1
+\end{lstlisting}
+
+\begin{lstlisting}
+END DO
+\end{lstlisting}
+
+\begin{lstlisting}
+CALL ResolveLockoutFlags(SimAirLoops)
+\end{lstlisting}
+
+The logical flags \emph{SimAirLoops} and \emph{SimZoneEquipment} are used to signal whether the primary air systems or the zone equipment sets need to be resimulated. These flags are set by the subroutine \emph{UpdateHVACInterface} which is called~ from within \emph{ManageAirLoops} and \emph{ManageZoneEquipment} at the end of each half-loop simulation. \emph{UpdateHVACInterface} (when called from \emph{ManageAirLoops}) passes the values at the outlet nodes of a primary air system on to the inlet nodes of the corresponding zone equipment half-loop and similarly (when called from \emph{ManageZoneEquipment}) passes the values of the outlet nodes of a zone equipment half-loop on to the inlet nodes of its corresponding~ primary air system. Each time \emph{UpdateHVACInterface} is called it also checks whether the values at the half-loop outlet nodes are in agreement with the values at the downstream half-loop inlet nodes. If they are not it sets the simulate flag of the downstream half-loop to \emph{true}. The values checked by \emph{UpdateHVACInterface} and their tolerances are as follows.
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Quantities & Tolerances \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Quantities & Tolerances \tabularnewline
+\midrule
+\endhead
+
+specific enthalpy [J/kg\} & 10.0 \tabularnewline
+mass flow rate [kg/s] & 0.01 \tabularnewline
+humidity ratio [kg H  O / kg dry air] & 0.0001 \tabularnewline
+quality & 0.01 \tabularnewline
+air pressure [Pa] & 10.0 \tabularnewline
+temperature [C] & 0.01 \tabularnewline
+energy [J] & 10.0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\emph{ResolveAirLoopFlowLimits} is invoked to deal with zone equipment -- primary air system flow mismatches. For instance the zone air terminal units (ATUs) may be asking for more air than the central fan can supply. In this case \emph{ResolveAirLoopFlowLimits} takes the air flow that the fan can supply and apportions it among the ATUs in proportion to their design maximum air flow rates (\emph{ResolveAirLoopFlowLimits} sets the \({\dot m_{\max avail,node}}\) ~at the entering node of each ATU in the system).
+
+At the end of the air loop simulation \emph{ResolveLockoutFlags} is called. This subroutine checks if any air system component has requested that the economizer be locked out. If such a request has been made and if the economizer is active, \emph{ResolveLockoutFlags} sets \emph{SimAirLoops} to \emph{true} and the \emph{EconoLockout} flag to \emph{true} to ensure that the air loop will be resimulated with the economizer forced off.
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager/air-loops.tex b/doc/engineering-reference/src/building-system-simulation-system-manager/air-loops.tex
new file mode 100644
index 00000000000..4675d5474ec
--- /dev/null
+++ b/doc/engineering-reference/src/building-system-simulation-system-manager/air-loops.tex
@@ -0,0 +1,27 @@
+\section{Air Loops}\label{air-loops}
+
+\subsection{Definition of Air Loop}\label{definition-of-air-loop}
+
+In EnergyPlus an air loop is a central forced air HVAC system. The term ``loop'' is used because in most cases some air is recirculated so that the air system forms a fluid loop. The air loop is just the ``air side'' of a full HVAC system.~ The input objects related to these air loops begin ``AirLoopHVAC.''
+
+For simulation purposes the air loop is divided into 2 parts: the primary air system (representing the supply side of the loop) and the zone equipment (representing the demand side of the loop). The primary air system includes supply and return fans, central heating and cooling coils, outside air economizer, and any other central conditioning equipment and controls. The zone equipment side of the loop contains the air terminal units as well as fan coils, baseboards, window air conditioners, and so forth. Supply and return plenums are also included on the zone equipment side of the loop.
+
+\subsection{Simulation Method}\label{simulation-method}
+
+Simulating a forced air system and its associated zones can be done in a number of ways. EnergyPlus uses algebraic energy and mass balance equations combined with steady state component models. When the zone air and the air system are modeled with algebraic equations (steady state) then -- in cases with recirculated air -- there will be one or more algebraic loops. In other words it is not possible to solve the equations directly; instead iterative methods are needed. Typically a humidity ratio and a mass flow rate will be variables involved in the iterative solution.
+
+In EnergyPlus the zone humidity ratios and temperatures are decoupled from the solution of the air system equations. The zone air is assigned heat and moisture storage capacities and the capacity effects are modeled by 1\(^{st}\) order ordinary differential equations. During each system simulation time step new zone temperatures and humidities are predicted using past values. The zone temperatures and humidities are then held constant during the simulation of the air system (and the plant). Then the zone temperatures and humidity ratios are corrected using results from the system simulation. As a result the usual algebraic loops arising in steady state air system simulations are eliminated from the EnergyPlus system simulation. The zone temperatures, humidity ratios, and heating and cooling demands are known inputs to the system simulation.
+
+The need for iteration can be reintroduced by the need for system control. If system setpoints are fixed, externally determined, or lagged and control is local (sensor located at a component outlet, actuator at a component inlet) then iteration can be confined to the components and the overall air system equations can be solved directly. However these requirements are too restrictive to simulate real systems. System setpoints are held fixed during a system time step. But controller sensors are allowed to be remote from the location of the actuator. Consequently EnergyPlus uses iteration over the entire primary air system in order to converge the system controllers.
+
+\subsection{Component Models}\label{component-models}
+
+EnergyPlus component models are algorithmic with fixed inputs and outputs. They are embodied as Fortran90 subroutines within software modules. For each component several choices of inputs and outputs are possible. There is no one choice that will be most usable and efficient for all system configurations and control schemes. For reasons of consistency and comprehensibility the requirement was imposed that all EnergyPlus models be forward models. That is, the component inputs correspond to the inlet conditions and the outputs to the outlet conditions.~ If another choice of inputs and outputs is needed it is obtained by numerical inversion of the forward model.
+
+\subsection{Iteration Scheme}\label{iteration-scheme}
+
+The primary air system simulation uses successive substitution starting at the return air inlet node and proceeding in the flow direction to the supply air outlet nodes. The iteration proceeds until an individual actuator-controller has converged (the sensed value matches the setpoint within the specified tolerance). The system controllers are simulated in sequence. During this sequence of iterative solutions the air mass flow rates are held constant. The controllers are converged by the method of interval halving. This method was chosen (rather than for instance Newton-Raphson) for its robustness.
+
+\subsection{Determination of Air Mass Flow Rates}\label{determination-of-air-mass-flow-rates}
+
+In most cases the air mass flow rate of the central air system is set by zone equipment downstream of the primary air system. The air terminal unit components with their built in dampers and controllers respond to the zone heating and cooling loads by setting air flow rates at their inlet nodes. These flow rates are passed back upstream to the primary air system, establishing the flow rates in the primary air system branches. These flow rates are held fixed while the primary air system is simulated.
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager/air-path-components.tex b/doc/engineering-reference/src/building-system-simulation-system-manager/air-path-components.tex
new file mode 100644
index 00000000000..f415adf49a9
--- /dev/null
+++ b/doc/engineering-reference/src/building-system-simulation-system-manager/air-path-components.tex
@@ -0,0 +1,73 @@
+\section{Air Path Components}\label{air-path-components}
+
+\subsection{Overview}\label{overview}
+
+The air path from the outlet of an AirLoopHVAC (the supply side of a full air loop / central air system) to the zone air distribution units (terminal units) is specified in a AirLoopHVAC:SupplyPath. The AirLoopHVAC:SupplyPath consists of AirLoopHVAC:ZoneSplitters and AirLoopHVAC:SupplyPlenums hooked together outlets to inlet.
+
+The air path from the zone return nodes to the AirLoopHVAC inlet node is described in a AirLoopHVAC:ReturnPath object. The~ AirLoopHVAC:ReturnPath consists of AirLoopHVAC:ZoneMixers and AirLoopHVAC:ReturnPlenums hooked together outlet to inlets.
+
+\subsection{Zone Supply Air Path}\label{zone-supply-air-path}
+
+The AirLoopHVAC:SupplyPaths are simulated just before the zone equipment is simulated and just after the zone equipment is simulated (in module ZoneEquipmentManager, subroutine SimZoneEquipment). In both cases the simulation consists of looping over all the AirLoopHVAC:SupplyPaths and simulating each component (AirLoopHVAC:ZoneSplitter or AirLoopHVAC:SupplyPlenum) in the path. For the ``just before'' simulation a flag \emph{FirstCall} is set to \emph{True} which tells the zone splitter and zone supply plenum models to do a downstream simulation (pass component inlet conditions to component outlets, except for air mass flow rate). For the ``just after'' simulation, \emph{FirstCall} = \emph{False}, which tells the components to do an upstream simulation (set the component inlet air mass flow rate to the sum of the component outlet air mass flow rates, do nothing with other properties).
+
+\subsection{Zone Splitter}\label{zone-splitter}
+
+The AirLoopHVAC:ZoneSplitter divides an inlet air stream into multiple outlet streams. Its data and simulation model are encapsulated in the module \emph{SplitterComponent}. There are two simulation modes. If \emph{SimAirLoopSplitter} is called with input parameter \emph{FirstCall} = \emph{True} then the splitter is simulated in downstream mode. The outlet air streams' humidity ratio, pressure, enthalpy, and temperature are set to the conditions on the inlet air stream.~ If \emph{SimAirLoopSplitter} is called with input parameter \emph{FirstCall} = \emph{False}, the splitter is simulated in the upstream mode. In this case the inlet air stream air mass flow rate is set to the sum of the outlet air mass flow rates. The same calculation is done for the maximum available and minimum available air flow rates.
+
+\subsection{Zone Supply Plenum}\label{zone-supply-plenum}
+
+The AirLoopHVAC:SupplyPlenum acts analogously to the AirLoopHVAC:ZoneSplitter. The only difference is that the AirLoopHVAC:SupplyPlenum is associated with a Zone for which it sets the supply air flow rate and from which it gets its outlet air conditions. The AirLoopHVAC:SupplyPlenum divides an inlet air stream into multiple outlet streams. Its data and simulation model are encapsulated in the module \emph{ZonePlenum}. There are two simulation modes. If \emph{SimAirZonePlenum} is called with input parameter \emph{FirstCall} = \emph{True} then the plenum is simulated in downstream mode. The outlet air streams' humidity ratio, pressure, enthalpy, and temperature are set to the zone conditions.~ If \emph{SimAirZonePlenum} is called with input parameter \emph{FirstCall} = \emph{False}, the plenum is simulated in the upstream mode. In this case the inlet air stream air mass flow rate is set to the sum of the outlet air mass flow rates. The same calculation is done for the maximum available and minimum available air flow rates.
+
+\subsection{Zone Return Air Path}\label{zone-return-air-path}
+
+The AirLoopHVAC:ReturnPaths are simulated after all the zone equipment is simulated (in module ZoneEquipmentManager, subroutine SimZoneEquipment). The simulation is accomplished by a call to \emph{SimReturnAirPath} (in module \emph{ReturnAirPathManager}). The simulation just consists of looping over all the AirLoopHVAC:ReturnPaths and simulating the components (AirLoopHVAC:ZoneMixer or AirLoopHVAC:ReturnPlenum) in each path.
+
+\subsection{Zone Mixer}\label{zone-mixer}
+
+The AirLoopHVAC:ZoneMixer combines multiple inlet air streams into a single outlet air stream. Its data and simulation model are encapsulated in the module \emph{MixerComponent}. The following mass and energy balance equations are used.
+
+\begin{equation}
+{\dot m_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{air,out}}\cdot {W_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}} \cdot {W_{air,in,i}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{air,out}}\cdot {h_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}} \cdot {h_{air,in,i}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{air,out}}\cdot {P_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}} \cdot {P_{air,in,i}}
+\end{equation}
+
+\begin{equation}
+{T_{air,out}} = PsyTdbFnHW({h_{air,out}},{W_{air,out}})
+\end{equation}
+
+Where \(\dot m\) is air mass flow rate, \emph{W} is humidity ratio, \emph{h} is specific enthalpy, \emph{P} is pressure, and \emph{T} is temperature. \emph{PsyTdbFnHW} is the EnergyPlus psychrometric function for drybulb temperature as a function of enthalpy and humidity ratio. The air mass flow rate calculation is also done for the maximum and minimum available mass flow rates.
+
+\subsection{Zone Return Plenum}\label{zone-return-plenum}
+
+The AirLoopHVAC:ReturnPlenum acts analogously to the AirLoopHVAC:ZoneMixer. The only difference is that the AirLoopHVAC:ReturnPlenum is associated with a Zone for which it sets the supply air flow rate and from which it gets its outlet air conditions. The AirLoopHVAC:ReturnPlenum combines multiple inlet air streams into a single outlet air stream. Its data and simulation model are encapsulated in the module \emph{ZonePlenum}. The outlet air mass flow rate is obtained from
+
+\begin{equation}
+{\dot m_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}}
+\end{equation}
+
+The outlet air temperature, enthalpy, humidity ratio and pressure are set to the zone conditions.
+
+In addition to its normal function of acting as an air stream mixer, the return plenum can have 2 types of special connection to upstream air terminal units.
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\item
+  The user can model the effects of duct leakage in VAV single duct systems using the Simplified Duct Leakage Model (see ZoneHVAC:AirDistributionUnit for how to set up this model). After the normal outlet air flow calculation is completed as above, the calculation loops over the air distribution units connected to the zones that feed air to the plenum and adds in to the outlet air mass flow rate the leakage air flow rates from the upstream leaks defined in the ZoneHVAC:AirDistributionUnit inputs. This connection between the leaks and the plenum is not explicit: no extra nodes are defined in the return plenum or in the terminal unit.
+\item
+  The user can model secondary (recirculated) air drawn from the plenum into a fan powered induction unit (AirTerminal:SingleDuct:SeriesPIU:Reheat or AirTerminal:SingleDuct:ParallelPIU:Reheat). In this case the connection is explicit: extra outlet nodes are defined in the return plenum which act as the secondary air inlet nodes for the terminal units. The recirculated air flow rates are set by the terminal units. The outlet return air is then:
+\end{enumerate}
+
+\begin{equation}
+{\dot m_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}}  - \sum\limits_{j = 1,m}^{} {{{\dot m}_{air,recirc,j}}}
+\end{equation}
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager/outdoor-air-mixer.tex b/doc/engineering-reference/src/building-system-simulation-system-manager/outdoor-air-mixer.tex
new file mode 100644
index 00000000000..8fec688e474
--- /dev/null
+++ b/doc/engineering-reference/src/building-system-simulation-system-manager/outdoor-air-mixer.tex
@@ -0,0 +1,7 @@
+\section{Outdoor Air Mixer}\label{outdoor-air-mixer}
+
+The OutdoorAir:Mixer is the fundamental component of the outside air system. There should always be one OutdoorAir:Mixer in an AirLoopHVAC:OutdoorAirSystem. The outside air mixer splits the primary air system (AirLoopHVAC) return air into relief and recirculated air streams. Then it mixes the outside air stream with the recirculated air stream to obtain the mixed air stream. The outdoor air mixer has 2 inlet flow nodes: the return air node and the outside air node. It has 2 outlet flow nodes: the relief air node and the mixed air node.
+
+\subsection{Simulation}\label{simulation-001}
+
+Given the air mass flow rates and conditions (humidity ratio, specific enthalpy) at the return air node, relief air node, and outside air node, the simulation uses mass and energy balance to calculate the air mass flow rate, humidity ratio, and specific enthalpy at the mixed air node. The mixed air temperature is calculated from the mixed air humidity ratio and specific enthalpy using the EnergyPlus psychrometric routine \emph{PsyTdbFnHW}.
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager/outdoor-air-system.tex b/doc/engineering-reference/src/building-system-simulation-system-manager/outdoor-air-system.tex
new file mode 100644
index 00000000000..1dbb100036e
--- /dev/null
+++ b/doc/engineering-reference/src/building-system-simulation-system-manager/outdoor-air-system.tex
@@ -0,0 +1,16 @@
+\section{Outdoor Air System}\label{outdoor-air-system}
+
+The AirLoopHVAC:OutdoorAirSystem is a subsystem of the primary air system (object AirLoopHVAC). To the primary air system it appears to be a single component. Within the subsystem are components and controllers very much like the primary air system. The purpose of the outside air system is to simulate the splitting of the return air into relief and recirculated air; mix the recirculated and outside air to obtain the mixed air (all accomplished by the OutdoorAir:Mixer); simulate the components in the outside air stream; control the components and outside air flow rate (economizer control). The outside air system differs from the primary air system in that it is not described in terms of splitters, mixers, and branches. Instead the components are simply listed in simulation order in an AirLoopHVAC:OutdoorAirSystem:EquipmentList input object. The components other than the OutdoorAir:Mixer are assumed to be in the outside air stream. The connectivity is defined by upstream component's outlet node = downstream component's inlet node. The OutdoorAir:Mixer should be the first component in the AirLoopHVAC:OutdoorAirSystem:EquipmentList object.
+
+\subsection{Simulation}\label{simulation-002}
+
+The data for and simulation of the outside air system are contained in the MixedAir module. This includes the data and simulation of the OutdoorAir:Mixer and the Controller:OutdoorAir. The simulation of the outside air system is straightforward.
+
+\begin{itemize}
+\item
+  All controllers other than Controller:OutdoorAir are moved up to the primary air system level, where they are simulated with the primary air system controllers.
+\item
+  The Controller:OutdoorAir is simulated.
+\item
+  The compnents contained in the outside air system are simulated in the order of their input in the AirLoopHVAC:OutdoorAirSystem:EquipmentList.
+\end{itemize}
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager/plant-condenser-loops.tex b/doc/engineering-reference/src/building-system-simulation-system-manager/plant-condenser-loops.tex
new file mode 100644
index 00000000000..e44bd7a237b
--- /dev/null
+++ b/doc/engineering-reference/src/building-system-simulation-system-manager/plant-condenser-loops.tex
@@ -0,0 +1,543 @@
+\section{Plant/Condenser Loops}\label{plantcondenser-loops}
+
+\subsection{Integration of System and Plant}\label{integration-of-system-and-plant}
+
+In order to integrate the air handling system simulation with the zones simulation, methods were developed to model the system air loop and its interactions with the zones due to temperature controls and the relative difference between the zone and supply air temperatures. A similar situation is encountered when integrating the central plant simulation. Typically, the central plant interacts with the systems via a fluid loop between the plant components and heat exchangers, called either heating or cooling coils. In EnergyPlus the performance of the air systems and plant are interdependent because the simulations are combined. The plant outputs must match the system inputs and vice versa. That is, the temperature of the chilled water leaving the plant must equal the temperature of the water entering the coils, and the chilled water flow rate must satisfy mass continuity. In addition, coil controls are usually necessary to ensure that the values of chilled water flow variables entering and leaving the coil remain in a reasonable range. Plants can also interact with each other so that the operation of a chilled water loop and chiller will affect the operation of a condenser water loop.
+
+\subsection{Current Primary System Modeling Methodology}\label{current-primary-system-modeling-methodology}
+
+There are two main types of loops within the HVAC simulation in EnergyPlus: an air loop and a plant loop. The air loop is assumed to use air as the transport medium as part of an air handling system while the plant loops use a liquid fluid of the user's choosing (typically water).~ Condenser loops are a special case of plant loop that are for heat rejection and are distinguished by slightily different control options and applicable equipment types.~ A user may have any number of each type of loop in a particular input file. There are no explicit limits on the number of loops within the program---the user is only limited by computer hardware. Execution speed will naturally vary with the complexity of the input file.
+
+Plant loops are further divided into ``half-loops'' or ``semi-loops'' for organizational clarity and simulation logistics (see Figure ``Connections between the Main HVAC Simulation Loops and Half-Loops''). These sub-loops, or half-loop sides, are matched pairs that consist of half of a main plant loop. Plant loops are broken into supply and demand sides. The plant demand side half-loop contains equipment that places a load on the primary equipment. This might include coils, baseboards, radiant systems, etc. The load is met by primary equipment such as chillers or boilers on the supply side half-loop. Each supply side half-loop must be connected to a demand side half-loop and vice versa. A similar breakdown is present on condenser loops where the demand side includes the water side of chiller's condensers while the supply side includes condenser equipment such as cooling towers.
+
+\begin{figure}[hbtp] % fig 120
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1957.svg.png}
+\caption{Connections between the Main HVAC Simulation Loops and Half-Loops. \protect \label{fig:connections-between-the-main-hvac-simulation}}
+\end{figure}
+
+The breakdown into two half-loops allows for better handling and control of information and simulation flow throughout the program. Direct connections between the half-loops of the air, plant, and condenser loops are enhanced by components with connections between the various main loop types. For example, coils (heating or cooling) are in reality heat exchangers with an air and a water or refrigerant side. The air side of the coil is handled within the air loop where the control of the device is also maintained. The fluid side of the coil is handled within the plant demand side, which passes the energy requirements of the coil on to the plant supply side. All loops are simulated together by successively modeling each half-loop in a particulary calling order. Overall iterations ensure that the results for the current time step are balanced and updated information has been passed to both sides of the sub-loops as well as across to the other side of air loop connections such as coils.
+
+The plant equipment on a half-loop is described by a set of branches for that half-loop.~ Components can be arranged on a branch in series, and branches can be placed in parallel, with some restrictions. Figure ``Branch Layout for Individual Plant Half-Loops'' provides an overview of the intended branch layout for each plant half-loop. Branches are individual legs within the loop structure. Thus, the segment between point A and point B is defined as a branch, as is the section between points E and F. There may be multiple sections (C1 to D1 through Cn to Dn) in between the splitter and mixer.
+
+Each half-loop may only have one splitter and one mixer. Thus, equipment may be in parallel between the mixer and splitter, however, within any single branch, there can only be components in series and not in parallel. The topology rules for individual half-loops allow a reasonable amount of flexibility without requiring a complicated solver routine to determine the actual flow and temperature conditions. Note that since plant supply and demand are broken up into two separate half-loops, chillers or boilers may be in parallel to each other in the supply side and coils may be in parallel to each other on the demand side. Thus, the restriction of only a single splitter and mixer on a particular half-loop does not unduly limit the allowable configurations. In some cases a single branch can be used to define an entire half-loop, but in general a half-loop should have a splitter and a mixer even if all equipment on the sub-loop is simply in series.
+
+In addition, to avoid the need for overly complex solver routines, there are some restrictions on the placement of pumps within a particular half-loop. There are two general types of pumps, loop pumps and branch pumps. A pump that is the first component on the first branch (between A and B) is termed a ``loop pump'' while any pump in the parallel section (between Ci and Di) is termed a ``branch pump''.~~ The simplest and most common arrangement is to have one loop pump on the supply side inlet.~ In plant demand half-loops pumps can be placed only in the inlet branch. This will allow simulation of primary-secondary systems. For more information on pumps and pump placement rules, see the section on PipingSystem:Underground Simulation Pumps in this document.
+
+\begin{figure}[hbtp] % fig 121
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1958.svg.png}
+\caption{Branch Layout for Individual Plant Half-Loops \protect \label{fig:branch-layout-for-individual-plant-half-loops}}
+\end{figure}
+
+Essentially, each branch is made up of one or more components linked together in series. The branch has system nodes that store properties at a location on the loop (temperature, enthalpy, flow rate, etc.) at the beginning and end of the branch as well as between components. Components on the branch take the conditions of the node at their inlet and use that information as well as overall control information to simulate the component and write the outlet data to the node following the component. This information is then used either by the next component on the branch or establishes the outlet conditions for the branch.
+
+Although the plant model in EnergyPlus is quite flexible, in most cases the topology of the plant system in the model will be somewhat different from the topology of the actual plant system in a building.~ EnergyPlus is focused on modeling building energy performance over long periods of time and is not intended as a completely flexible system that can directly model any actual plant system with its full complexity and exact layout.~ Given the design of an actual complex plant system, the modeler will typically need to develop a simpler system that conforms to EnergyPlus's capabilities and strives to capture the issues important for energy consumption modeling.~ Just like complex geometry should be simplified into thermal zones for energy models, complex plants should to be simplified into sets of pairs of closed half-loops with the allowed branch topologies.
+
+\subsection{Plant Manager}\label{plant-manager}
+
+\subsubsection{Plant Half-Loop Calling Order}\label{plant-half-loop-calling-order}
+
+Because there can be multiple plant loops in a model that depend on each other, one job of the plant manager is to determine an appropriate calling order for the half-loops.~ The intial starting calling order (and the order always used prior to EnergyPlus Version 7) is as follows:
+
+1.~~~~Call all the demand side half-loops of the plant loops (in input object order)
+
+2.~~~~Call all the supply side half-loops of plant loops (in input object order)
+
+3.~~~~Call all the demand side half-loops of condenser loops (in input object order)
+
+4.~~~~Call all the supply side half-loops of the condenser loops (in input object order).
+
+This initial calling order is then revised during a setup phase of program execution when the plant component models are iteratively read in, initialized and sized.~ The algorithm is based on information provided by those component models that connect loops together.~ The components register that two loop-sides are connected and declare which one places demands on the other.~ If a half loop is connected and places demands on anther loop, then the calling order for the independent demanding loop is placed just ahead of the dependent loaded half-loop.~ For example a water cooled chiller component model reports that the supply side of the chilled water loop is connected to the demand side of the condenser loop and that the chilled water loop places demands on the condenser loop.~ The plant manger algorithm is iterative and repeatedly calls all of the half loops a total of four times.~ After this setup phase, the calling order is fixed for the rest of the simulation.
+
+\subsection{Plant Flow Resolver}\label{plant-flow-resolver}
+
+\subsubsection{Overview of the Plant Flow Resolver Concept}\label{overview-of-the-plant-flow-resolver-concept}
+
+An important aspect of the solution procedure within plant loops is the method used to solve for the fluid flow rates throughout the various half-loops. This involves making the supply side meet a particular load and flow situation based on the simulation of the demand side loops. Load distribution is an issue that must be addressed as well as how flow rates are adjusted and temperatures are updated. These issues are discussed in the next several subsections, and the algorithms described are important to how the plant simulation functions.
+
+In the first step, the plant loop manager calls the appropriate module to simulate (in flow order) all of the components on each branch of the loop except for splitters and mixers. In this step, each component would set the conditions at the outlet node including temperature, flow rate, maximum allowed (design) flow rate, minimum allowed (design) flow rate, maximum available flow rate, and minimum available flow rate. This would be based purely on the component's own control scheme and thus each component would be free to request as much (or as little) flow as desired.
+
+In the second step, the loop manager would resolve the flow at all nodes and through all branches of the local loop. The components are then simulated with the corrected flows. For this iteration, the flow resolver sets the flow rate through each loop component.
+
+\subsubsection{Overall Loop Flow Rate}\label{overall-loop-flow-rate}
+
+The plant models determine an overall fluid flow rate for each loop based on the dynamic requests and needs of the components on the loop.~ The flow resolver examines the requests and needs of each half-loop and chooses an overall flow rate.~ As individual plant components are modeled, they register their requests for fluid flow which are stored on the inlet node (variable called MassFlowRateRequest).~~ These requests for flow are used for two purposes, overall loop flows and resolution of parallel flows inside a splitter/mixer.~ For determining the overall loop flow request, the requests by individual components are further qualified into three categories based on the nature of the device.
+
+1.~~~~Need flow and turns loop on
+
+2.~~~~Need flow if loop is already on
+
+3.~~~~Take what ever flow they get.
+
+The loop will only run at all if there are flow requests of type 1.~ If there are flow requests of type 2, they will not turn on the loop but may affect the overall flow rate if it is already on because of some non-zero type 1 requests.~ Flow requests of type 3 will not affect the overall loop flow rate.~ These classifications are hard coded and cannot be altered by the user.
+
+\subsubsection{Pump Control for Plant and Condenser Loops.}\label{pump-control-for-plant-and-condenser-loops.}
+
+The pump is quite simply the component that drives the flow (also see PipingSystem:Underground Simulation Pumps). . How it reacts depends on several different conditions. In total, there are three different decision variables, two of which are defined by user input. These three deciding factors are whether the pump is constant or variable speed, whether the pump operation is continuous or intermittent, and whether or not there is a request for overall loop flow. After the overall loop flow request has been determined the simulation knows what the loop would like to do.~ The next thing it does is simulation all the loop pumps to see what the pumps can actually provide. Then the overall loop flow is bounded by the minimum and maximum that the loop pumps can provide at that time. The operation of a constant speed pump is fairly straightforward. If the user designates a constant speed pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump is constant speed and operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop.
+
+A variable speed pump is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump is operating intermittently, then the pump can shutdown. For any other condition such as the loop having a load and the pump is operating intermittently or the pump is continuously operating (regardless of the loading condition), the pump will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump is running, it will try to meet the flow request for the overall loop.
+
+In many cases, the first estimate of flow requested by the demand side tends to be fairly accurate and the flow rate does not vary in subsequent iterations. However, because there is the possibility that the coils or some other component might request more flow in future iterations during the same time step, the program must not only set flow rates but also maintain a record of the current maximum and minimum flow rate limits. This information is important not only to the pump itself but also to other pieces of equipment which may control their flow rates and thus require knowledge of the limits within which they may work. In general, the decisions on what to set the maximum and minimum flow rates is directly related to the type of pump (constant or variable speed). For constant speed pumps, the maximum and minimum flow rate values are the same and thus if the flow requested does not match this, the other components must either deal with the flow or a bypass branch must be available to handle the excess flow. For variable speed pumps, the maximum and minimum flow rates are set by the user-defined limits.
+
+\subsubsection{Plant/Condenser Supply Side}\label{plantcondenser-supply-side}
+
+Component models, such as boilers, chillers, condensers and cooling towers are simulated on the supply side of the plant and condenser loops. In order to allow specification of realistic configurations, the plant loop managers were designed to support parallel-serial connection of component models on the loop. In addition, loop managers were designed to support both semi-deterministic models (e.g.~the parameter estimation models of the ASHRAE Primary Toolkit {[}Pedersen 2001{]}) and ``demand based'' models (e.g.~the performance map models of BLAST and DOE2.1E). As a result, the loop manager must be able to simulate models that require the mass flow rate as an input and models that calculate the mass flow rate as an output---sometimes in the context of a single loop configuration.
+
+In order to achieve these design criteria without resorting to a pressure based flow network solver in the HVAC portion of the code, a rules-based ``flow resolver'' was developed for the EnergyPlus plant manager. The flow resolver is based on the following assumptions and limitations:
+
+\begin{itemize}
+\item
+  Each loop is only allowed to have a single splitter and a single mixer
+\item
+  Due to the fact that there can only be one splitter and one mixer on a given loop, it follows logically that there can be at most one bypass on each loop side
+\item
+  No other components may be in series with a bypass, i.e., a branch that contains a bypass may have no other equipment on that branch
+\item
+  Equipment may be in parallel only between the splitter and mixer components of a loop
+\item
+  Equipment may be hooked together in series in each branch of the loop
+\item
+  Flow rates on individual branches will be controlled using maximum and minimum available flow rate limits
+\end{itemize}
+
+The flow resolver employs a simple predictor-corrector algorithm to enforce mass continuity across the plant loop splitter as shown in the following figure.
+
+\begin{figure}[hbtp] % fig 122
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1959.png}
+\caption{Plant/Condenser Supply Side Solution Scheme. \protect \label{fig:plantcondenser-supply-side-solution-scheme.}}
+\end{figure}
+
+As previously discussed, the pump establishes the total loop mass flow rate by setting the flow in the first supply side branch. In the second step, a predictor algorithm calls to simulate each piece of equipment on the loop and they update their mass flow rate requests based on the current flow rates, temperatures and load dispatch requests. The loop manager calls the appropriate module to simulate (in flow order) all of the components on each branch of the loop except for splitters and mixers. In this step, each component sets the conditions at its outlet node including temperature and sets component flows on the inlet node.~~ Each component and branch is classified for their type of flow control.~ Prior to version 7 this was input by the user where branch objects were tagged in the user input file as an ACTIVE, SERIESACTIVE, PASSIVE or BYPASS type of model.~ As of version 7 this has been hard coded and the input is no longer used.~ An ACTIVE flow control type describes a demand based plant model that calculates mass flow rate as an output. An ACTIVE component when OFF will shut down the whole branch irrespective of the type of other components on the branch. A SERIESACTIVE branch is like an ACTIVE component except that there are more than one ACTIVE components on the branch so that two components requests may be at odds with each other and so it might not shut down the whole branch when the component is OFF. The flow resolution algorithm is same for both ACTIVE and SERIESACTIVE components and in the rest of the document description of one type will fit the other type too. A PASSIVE type describes a semi-deterministic model that is simulated with the mass flow rate as an input. The BYPASS type designates a loop bypass.
+
+The predictor algorithm first establishes the desired flow rate of each branch by searching for ACTIVE components on the branch. The first ACTIVE component in simulation order sets the desired branch flow. Branches with only PASSIVE components require a flow rate between the minimum and maximum allowable branch flow. Branches with a BYPASS component have a branch flow only when all other branches combined cannot handle the entire loop flow.
+
+The loop flow resolver~ makes any necessary ``corrections'' to the requested branch flows in order to enforce overall continuity on the loop. If mass conservation allows all ACTIVE branches to be satisfied, then the remaining flow is divided between the PASSIVE branches and as a last resort, the BYPASS. If there is insufficient flow to meet the branch demand, ACTIVE branch requests are met first in the order that the branches appear in the branch list in the input file.
+
+The flow rate is resolved first for each individual branch. For every branch, the program cycles through each node on the branch and determines what the flow requests and flow limits are. The most restrictive flow constraints are assumed to be valid for the entire branch regardless of component type. Active components are given highest priority for requesting a particular flow rate. If there is more than one active component on a particular branch, then it is assumed that the active component on the branch with the highest flow request dictates the flow request for the entire branch.
+
+Once all of the branches have set their flow rates and constraints, the splitter and mixer must resolve the various flow requests. The mixer and any branch following the mixer is passive. Thus, all of the flow control happens at the splitter. The splitter first attempts to sum the maximum and minimum constraints from all of the active branches coming out of the device and compares those to the constraints that are valid for the branch leading into the splitter. When there is a mismatch between the outlet constraints and the inlet constraints, the simulation will defer to the inlet constraints due to the fact that the pump is in reality controlling flow on the loop. Since the constraints of the pump would be passed across to the demand side from the supply side, an assumption is made that the coils or other demand side components must live within the bounds of the pump.
+
+Once the flow has been resolved at the splitter, the branch flow rates and constraints between the splitter and mixer can be adjusted, if necessary. In some cases, this will be mandatory to maintain a mass balance at the splitter. When the flow rate coming out of the splitter does not match the active branch requests, individual branch flow rates must be adjusted to provide for the extra flow or the ``flow deficit''. When there is extra flow, the excess flow is sent through any bypass branch first and then is sent to passive branches in reverse order of their appearance in the splitter outlet list. When all of these branches have been exhausted and there is still excess flow, flow will be increased to the active branches, also in reverse order. The reverse order guarantees that the branch appearing first has the highest priority to receive the flow rate it has requested.
+
+if there is not enough flow to meet all active branch requests (i.e., a ``flow deficit''), then the flow rates through the bypass and passive branches are set to zero. The flow rates through the active branches will then be decreased in reverse order until the splitter outlet flow rate matches the available flow at the splitter inlet. For a plant loop flow deficit, the bypass and passive branch flows are also set to zero, and flow rates for each active branch are calculated as follows:
+
+\begin{equation}
+{\dot m_{br}} = \frac{{{{\dot m}_{br_request}}}}{{{{\dot m}_{tot_request}}}}*{\dot m_{tot_available}}
+\end{equation}
+
+where:
+
+\begin{equation}
+  \begin{array}{rl}
+    \dot m_{br} & = \rm{ final resolved branch flow rate} \\
+    \dot m_{br_request} & = \rm{ requested branch flow rate } \\
+    \dot m_{tot_request} & = \rm{ total loop mass flow rate request} \\
+    \dot m_{tot_available} & = \rm{ total loop mass flow rate available}
+  \end{array}
+\end{equation}
+
+It is also necessary to monitor the flow constraints at the branches and components since once the flow rates are changed, the components must be resimulated by the controlling loop (air loop, zone equipment, or plant supply side). The controllers for these components must know if the constraints have been modified so that the simulation does not toggle between a component requesting a flow that the pump cannot meet and the pump then resetting the flow to what it can provide. Note that once a flow rate for any component has changed that this signals the need to resimulate any sub-loop to which it might have an indirect connection. Currently, this means that if a flow rate on the plant demand side changes, the simulation must recalculate the conditions on both the air loop and zone equipment sub-loops since coils and other equipment could be on either side of the main air loop. Similarly, if the condenser demand side simulation results in a change in flow rate through a chiller condenser, then the plant supply side must be triggered to perform its calculations again. Care has been taken to avoid cases where the various half-loops might simply keep triggering the resimulation of their indirect connections in an infinite loop.
+
+\subsubsection{Loop Capacitance and Pump Heat}\label{loop-capacitance-and-pump-heat}
+
+The plant model includes simplified methods of modeling fluid capacitance and the temperature rise because of pumping and friction. The transition from load or energy based plant models to a loop based arrangement makes variables of both the flow rate and the fluid temperature. This means there are more degrees of freedom that must be controlled. The flow resolver concept discussed previously controls the fluid flow rates through the components and maintains an overall mass flow balance through the loop. However, the temperatures still need to be controlled and modeled. A purely iterative procedure can be expected to converge to the appropriate loop temperatures, but the procedure can become slow to converge under conditions where the demand changes rapidly or the supply components may not have enough capacity to meet the system demand. This situation is somewhat analogous to that existing in the link between the zone and the air system. In that case, the convergence and stability of the iterative solution was greatly improved by adding the thermal capacitance of the zone air and other fast responding mass within the zone. Based on that experience, it was decided to add thermal capacitance to the plant loop model to benefit from the added stability. Because the thermal capacitance in the zone/system interaction is relatively small, it was necessary to use a third order numerical solution there. Although the plant loop's fluid thermal capacitance is relatively high, the fluid flows also have high heat capacity and can change temperatures rapidly a simple first order solution was not found to be satisfactory and an exact analytical solution was needed.
+
+In realistic conditions there is often some delay between changes in supply conditions and corresponding changes at demand side components due to the transport of fluid round the loop having a finite velocity.
+
+The act of pumping fluid around a loop adds heat to the fluid through friction.~ The slight warming occurs at the pump and all around the circuit.~ The amount of heat is equal to the work done on the fluid by the pump.~ This so-called pump heat is a complicating factor in plant simulation because the pump heat alters the load on primary equipment.~ A simple method of accounting for pumping heat is needed that doesn't increase the difficulties of the numerical solution and (as of version 7) in EnergyPlus this accomplished by including the pump heat in the loop capacitance model.
+
+Plant loops include a simple loop capacitance model to simulate these effects based on a well-stirred tank model. Each half-loop has a well-stirred tank located at its inlet as indicated in Figure~\ref{fig:loop-capacitance-tank-models}. The temperature of the tank is modeled as a function of the tank mass, inlet fluid flow rate and temperature, and pump heat.~ No energy is lost or gained because of storage in the loop capacitance.
+
+\begin{figure}[hbtp] % fig 123
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1962.png}
+\caption{Loop Capacitance Tank Models \protect \label{fig:loop-capacitance-tank-models}}
+\end{figure}
+
+The total plant loop volume is separated into two tanks, on on each half-loop inlet. For normal loops (without common pipes) each tank is one half of the plant loop volume. For common pipe plant loops, the tank on the supply side inlet has three fourths of the volume and the tank on the demand side inlet has one fourth. Each plant loop is assigned a total fluid volume as user input or an autocalculate routine based on the design flow rate. The size of the thermal capacitance affects the speed of recovery from situations where the setpoint was not maintained. The user must estimate a fluid volume based on the size of the pipes in the loop. Note that rough estimates seem to be sufficient. Loop capacitance (m\(^{3}\)) could be calculated from pipe size data but this is not usually known. If zero capacitance is specified the above formulation reduces to an instantaneous update in demand update temperature and the demand inlet temperature becomes the supply outlet temperature at the previous time step. If a very large capacitance is specified unrealistic time delay may result and there may be poor response to changes in loop setpoint temperature. The loop capacitance `autocalculate' option gives reasonable values and is calculated as follows,
+
+\begin{equation}
+Capacity = \frac{{{{\dot m}_s}*{t_{sys}}*3600}}{{0.8\rho }}
+\end{equation}
+
+The tank temperature is modeled by drawing a control volume and energy balance around the tank and solving for the temperature.~ The temperature of each tank is recalculated whenever the two half-loops are interfaced together. The tank temperature history is stored at the end of the simulation timestep.~ The model equation for tank (and outlet temperature) is formulated as follows:
+
+\begin{equation}
+{T_{tank,new}} = \frac{{\dot m{c_p}{T_{inlet}} + \frac{{{M_{tank}}{c_p}{T_{tank,old}}}}{{{t_{sys}}3600}} + {{\dot Q}_{pumpheat}}}}{{\mathop {m{c_P} + }\limits^ \frac{{{M_{tank}}{c_p}}}{{{t_{sys}}3600}}}}
+\end{equation}
+
+The tank temperature at the end of the simulation timestep is solved by the analytical approach and expressed as
+
+\begin{equation}
+T_{tank}^t = \left( {T_{tank}^{t - \delta t} - \frac{{\dot m{c_p}{T_{inlet}} + {{\dot Q}_{pumpheat}}}}{{\dot m{c_p}}}} \right)\exp \left( { - \frac{{\dot m{c_p}}}{{{M_{tank}}{c_p}}}t} \right) + \frac{{\dot m{c_p}{T_{inlet}} + {{\dot Q}_{pumpheat}}}}{{\dot m{c_p}}}
+\end{equation}
+
+where:
+
+\(T_{tank}^{t - \delta t}\) ~~~~~~~~~ = Previous system time-step tank temperature {[}°C{]}
+
+\(T_{tank}^t\) ~~~~~~~~~~ = Current tank and tank outlet temperature {[}°C{]}
+
+\(\dot m\) ~ ~~~~~~~~~~~ = Current fluid mass flow rate through the tank {[}kg/s{]}
+
+\(\delta t\) ~~~~~~~~~~~~ = Duration of system time step {[}second{]}
+
+\({c_P}\) ~ ~~~~~~~~~~ = Heat capacity of fluid {[}J/kg{]}
+
+\({M_{tank}}\) ~ ~~~~~~ = Mass of the water in the tank {[}kg{]}
+
+\({\dot Q_{pumpheat}}\) ~ ~ = Heat generated by a pump in the tank {[}W{]}
+
+When modeling plants using one of the common pipe modes for plant loops, the same tank model is used but the tanks are situated differently and account for extra connections.~ For common pipe situation, the tanks are located on the outlet of a half loop with common pipe interactions downstream of the tank.
+
+The average temperature is reported as the tank temperature. The average temperature is defined as the value of an integral function of tank temperature on an interval {[}\emph{0},\emph{δt}{]}
+
+\begin{equation}
+\begin{split}
+\mathop T\limits^ -   =& \frac{1}{{\delta t}}\int_0^{\delta t} {T_{tank}^tdt} \;\; = \frac{{{M_{tank}}{c_p}}}{{\dot m{c_p}\delta t}}\left( {T_{tank}^{t - \delta t} - \frac{{\dot m{c_p}{T_{inlet}} + {{\dot Q}_{pumpheat}}}}{{\dot m{c_p}}}} \right)\left( {1 - \exp \left( { - \frac{{\dot m{c_p}}}{{{M_{tank}}{c_p}}}\delta t} \right)} \right) \\
+&+ \frac{{\dot m{c_p}{T_{inlet}} + {{\dot Q}_{pumpheat}}}}{{\dot m{c_p}}}
+\end{split}
+\end{equation}
+
+\subsubsection{Plant Flow Resolver Input}\label{plant-flow-resolver-input}
+
+The input specifically related to the flow resolver consists of the plant BranchList and the plant ConnectorList as shown in the Input Output Reference. User defined names link the plant loop to its branches (contained in the BranchList) and define the loop splitters and mixers contained in the ConnectorList. The Connector:Splitter and Connector:Mixer syntax in turn define the relative connection of the branches to each other on the loop.
+
+The Branch definition is input in simulation and connection order for all of the components on the branch. The simulation assumes that the inlet node of the first component listed on the branch is the branch inlet node and the outlet node of the last component listed on the branch is the branch outlet node. Examples of all the input syntax is shown in the Input/Output Reference for the appropriate object.
+
+\subsection{Summary of Load Distribution Schemes}\label{summary-of-load-distribution-schemes}
+
+Five load distribution schemes are employed in EnergyPlus. The figure below illustrates the plant load distribution algorithm. The total loop demand is calculated and used in the \textbf{ManagePlantLoopOperation} routine to determine which equipment is available based on the supervisory control scheme specified by the user. Once all available components have been identified the loop demand is distributed to the available components based on the user specified load distribution scheme.
+
+~\includegraphics{media/image1974.png}
+
+Figure 124. Load Distribution Scheme
+
+The OPTIMAL scheme first loads each component to its optimal part load ratio (specified in input). Any remaining loop demand is distributed evenly to all the components. The UNIFORMLOAD scheme first divides the load evenly among all available components. If some components do not have the capacity to meet the uniformly distributed load, the remaining load is divided among the remaining components. The SEQUENTIALLOAD scheme loads each component one at a time to capacity until the loop demand is met. The components are loaded up in the order that they appear in the equipment list specified in input. The UNIFORMPLR scheme loads all equipment uniformly by maintaining uniform part load ratios across all equipment on the equipment list. If the load is below the load required by the plant to operate at the largest component minimum part load ratio, the last item is removed from each equipment list. This process is repeated until the plant can operate above the largest component minimum part load ratio. The SEQUENTIALUNIFORMPLR scheme loads all equipment in the order specified on the equipment list to capacity while operating all operational equipment at uniform part load ratios.
+
+\emph{Note:} For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
+
+\subsection{Summary of Plant Loop Demand Calculation Schemes}\label{summary-of-plant-loop-demand-calculation-schemes}
+
+There are two plant loop demand calculations schemes in EnergyPlus. There is a \textbf{SingleSetPoint} and a \textbf{DualSetPointDeadband}; the \textbf{SingleSetPoint} is the default if that field is left blank in the PlantLoop object. In the SingleSetPoint scheme the Plant Loop requires that a Setpoint Manager set a single setpoint value that sets Node\%TempSetPoint. Examples of this Setpoint Manager would be: the objects SetpointManager:Scheduled, SetpointManager:OutdoorAirReset, etc. For the DualSetPointDeadband scheme the Plant Loop requires that a Setpoint Manager that sets the high and low setpoint values for Node\%TempSetPointHi and Node\%TempSetPointLo. Examples of this setpoint manager would be: SetpointManager:Scheduled:DualSetpoint. Look in the Input Output Reference for the correct usage of these SetpointManagers.
+
+The Plant Loop Demand Calculation Scheme determines the amount of heating or cooling necessary to bring the temperature of the Plant Loop to its setpoint(s). When this value is determined then the Load Distribution scheme explained in the previous section takes this value and distributes the load to the appropriate equipment. The demand calculation scheme determines how the load is calculated. In the next section is a summary of the 2 algorithms and how they are used.
+
+\subsubsection{Loop Demand Calculation Scheme SingleSetPoint}\label{loop-demand-calculation-scheme-singlesetpoint}
+
+The SingleSetPoint scheme for the PlantLoop takes the value that is placed on the Node\%TempSetPoint and calculates the heating or cooling load necessary to obtain that setpoint.
+
+~~~~~~~ DeltaTemp~~~ = LoopSetPoint - LoopTempIn
+
+~~~~~~~ LoopDemand = mdot * Cp * DeltaTemp
+
+The sign of the Loop Demand determines if the loop has a cooling or heating load. Then the Load Distribution scheme distributes this calculated load to the appropriate equipment.
+
+\subsubsection{Loop Demand Calculation Scheme DualSetPointDeadband}\label{loop-demand-calculation-scheme-dualsetpointdeadband}
+
+The DualSetPointDeadband scheme for the PlantLoop takes the value that is placed on the Node\%TempSetPointHi and Node\%TempSetPointLo calculates the heating or cooling load necessary to obtain that setpoint; if in the DeadBand then no load is calculated. The pseudo code below shows the basis of the algorithm.
+
+\begin{lstlisting}
+        !Calculate the demand on the loop
+        IF (mdot > 0.0) THEN
+          LoadtoHeatingSetPoint = mdot*Cp*(LoopSetPointLo - LoopTempIn)
+          LoadtoCoolingSetPoint = mdot*Cp*(LoopSetPointHi - LoopTempIn)
+          ! Possible combinations:
+          ! 1  LoadToHeatingSetPoint > 0 & LoadToCoolingSetPoint > 0 -->  Heating required
+          ! 2  LoadToHeatingSetPoint < 0 & LoadToCoolingSetPoint < 0 -->  Cooling Required
+          ! 3  LoadToHeatingSetPoint < 0 & LoadToCoolingSetPoint > 0 -->  Dead Band Operation
+          ! 4  LoadToHeatingSetPoint > 0 & LoadToCoolingSetPoint < 0 -->  Not Feasible
+          IF (LoadToHeatingSetPoint .GT. 0.0 .AND. LoadToCoolingSetPoint .GT. 0.0) THEN
+             LoopDemand = LoadToHeatingSetPoint
+          ELSE IF (LoadToHeatingSetPoint .LT. 0.0 .AND. LoadToCoolingSetPoint .LT. 0.0) THEN
+             LoopDemand = LoadToCoolingSetPoint
+          ELSE IF (LoadToHeatingSetPoint .LT. 0.0 .AND. LoadToCoolingSetPoint .GT. 0.0) THEN
+             LoopDemand = 0.0
+          ELSE
+             CALL ShowSevereError
+          END IF
+        ELSE
+          LoopDemand = 0.0
+        END IF
+\end{lstlisting}
+
+\begin{lstlisting}
+        IF(ABS(LoopDemand) < LoopDemandTol) LoopDemand = 0.0
+\end{lstlisting}
+
+The sign of the Loop Demand determines if the loop has a cooling or heating load. Then the Load Distribution scheme distributes this calculated load to the appropriate equipment, if there is any.
+
+\subsection{Plant and Condenser Equipment Operation Schemes}\label{plant-and-condenser-equipment-operation-schemes}
+
+Plants and condenser loops must have some mechanism for controlling the operation of the loop and which equipment is available under different operating conditions. Once the Loop load is calculated by the return conditions from the demand side and using the loop setpoint, this load needs to be allocated to the supply equipment according to the users input. This is mainly done by the operation schemes.
+
+Each operation scheme must have the type of operation scheme, its identifying name, and the schedule that defines its availability. The first scheme appearing in the list is given the highest priority; the second scheme has second highest priority, etc. In other words, if according to its schedule, the first operation scheme is available, then it is used by the simulation to define how the plant or condenser loop operates. If it is not available, the second operation scheme in the list is checked to see if it is available until the highest priority scheme that is also available is found. See the Input Output Reference for input field details.
+
+\subsection{Plant Operation Schemes}\label{plant-operation-schemes}
+
+See the Input Output Reference for input field details. The options for plant control schemes are:
+
+\subsubsection{Uncontrolled Loop Operation}\label{uncontrolled-loop-operation}
+
+The PlantEquipmentOperation:Uncontrolled scheme takes the full capacity of the supply equipment and cools or heats the loop accordingly. An example would be a cooling tower where the cooling tower would cool the condenser loop with all of its available capacity and not be limioted by a capacity range or setpoint. Uncontrolled loop operation simply specifies a group of equipment that runs `uncontrolled'. If the loop runs, this equipment will run also, unless turned off by the loop flow resolver to maintain continuity in the fluid loop.
+
+\subsubsection{Cooling Load Range Based Operation or Heating Load Range Based Operation}\label{cooling-load-range-based-operation-or-heating-load-range-based-operation}
+
+PlantEquipmentOperation:CoolingLoad (or PlantEquipmentOperation:HeatingLoad) defines the different ranges and which equipment list is valid for each range. In each trio, there is a lower limit for the load range, an upper limit for the load range, and a name that links to an equipment availability list (PlantEquipmentList). Load range operation is used when the loop load is calculated and then the equipment is selected in the proper range. This allows for the most efficient operation of the plant equipment or for the user to determine the most efficient plant configuration. When the equipment list has been deteremined then the load is allocated to the equipment in a manner selected by the user with ``Optimal or Sequential'' load distribution scheme. The load range based operation scheme has two statements associated with it: a main statement that defines the ranges that individual priority settings are valid and the lists of equipment that may be used for each range.
+
+\subsection{Condenser Operation Schemes}\label{condenser-operation-schemes}
+
+This is very similar to the plant operation schemes, but there are several more options avaible with the CondenserLoop. The condenser operation schemes apply to the equipment on the `supply side' of the condenser loop---pumps, cooling towers, ground coupled heat exchangers, etc. The keywords select the algorithm that will be used to determine which equipment is available for each time step. The `\emph{Range Based Operation'} schemes select a user specified set of equipment for each user specified range of a particular simulation variable. `\emph{Load} \emph{Range} \emph{Based'} ~schemes compare the demand on the condenser supply side with specified load ranges and associated equipment lists. `\emph{Outdoor\ldots{}Range Based'} schemes compare the current value of an environmental parameter with user specified ranges of that parameter. See the Input Output Reference for input field details.
+
+\subsubsection{Uncontrolled Loop Operation}\label{uncontrolled-loop-operation-1}
+
+The PlantEquipmentOperation:Uncontrolled scheme takes the full capacity of the supply equipment and cools or heats the loop accordingly. An example would be a cooling tower where the cooling tower would cool the condenser loop with all of its available capacity and not be limioted by a capacity range or setpoint. Uncontrolled loop operation simply specifies a group of equipment that runs `uncontrolled'. If the loop runs, this equipment will run also, unless turned off by the loop flow resolver to maintain continuity in the fluid loop.
+
+\subsubsection{Cooling Load Range Based Operation or Heating Load Range Based Operation}\label{cooling-load-range-based-operation-or-heating-load-range-based-operation-1}
+
+PlantEquipmentOperation:CoolingLoad (or PlantEquipmentOperation:HeatingLoad) statement defines the different ranges and which equipment list is valid for each range. In each trio, there is a lower limit for the load range, an upper limit for the load range, and a name that links to an equipment availability list (CondenserEquipmentList). Load range operation is used when the loop load is calculated and then the equipment is selected in the proper range. This allows for the most efficient operation of the plant equipment or for the user to determine the most efficient plant configuration. When the equipment list has been deteremined then the load is allocated to the equipment in a manner selected by the user with ``Optimal or Sequential'' load distribution scheme. The load range based operation scheme has two statements associated with it: a main statement that defines the ranges that individual priority settings are valid and the lists of equipment that may be used for each range.
+
+\subsubsection{Outdoor Drybulb Range Based Operation, Outdoor Wetbulb Range Based Operation,~ Outdoor RHPercent Range Based Operation}\label{outdoor-drybulb-range-based-operation-outdoor-wetbulb-range-based-operation-outdoor-rhpercent-range-based-operation}
+
+The various ``PlantEquipmentOperation:Outdoor*'' statements define the different ranges of the various environmental parameters and which equipment list is valid for each range. After the keyword and the identifying name, a series of data trios is expected. In each trio, there is a lower limit for the load range, an upper limit for the load range, and a name that links to an equipment availability list (the ``CondenserEquipmentList'').
+
+\subsubsection{Outdoor Drybulb Temperature Difference Based Operation,. Outdoor Wetbulb Temperature Difference Based Operation}\label{outdoor-drybulb-temperature-difference-based-operation.-outdoor-wetbulb-temperature-difference-based-operation}
+
+The various ``PlantEquipmentOperation:Outdoor*Difference'' statements control strategies help to control any condenser equipment based on the difference between a reference node temperature and any environmental temperature. For example a cooling tower can be controlled by a strategy, which looks at the difference between the tower inlet temperature and wet-bulb temperature. A difference range is specified for each equipment list.
+
+\subsection{Primary-Secondary Loop Systems}\label{primary-secondary-loop-systems}
+
+The method to simulate a primary-secondary system in EnergyPlus is termed Common Pipe.
+
+\subsubsection{Common Pipe}\label{common-pipe}
+
+Common pipe feature eliminates the need of specifying two different EnergyPlus loops each for Primary and Secondary half loops. Instead the user can set up the system as it is used in real life applications. A common pipe simulation requires that pumps be placed on both Demand (Secondary) and Supply (Primary) sides of the loop. A typical Common Pipe layout as used in EnergyPlus is shown in Figure~\ref{fig:transmitted-radiation-in-three-directions-for}. The major assumptions in the common pipe implementation are as follows:
+
+\begin{itemize}
+\item
+  Pumps are placed on both demand and supply side of the loop.
+\item
+  Secondary pump flow rate can be less than, equal to or greater than the primary pump flow rate.
+\item
+  The flow at the inlet node of the half loop is equal to the flow at the outlet node of the half loop.
+\item
+  The pumps can have different schedules and any loop can be shut off when the other loop is still running.
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 125
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1975.png}
+\caption{Common Pipe Layout Schematic \protect \label{fig:common-pipe-layout-schematic}}
+\end{figure}
+
+Common pipe simulation is done during the interface update call at both Supply-to-Demand and Demand-to-Supply. Appropriate checks are used to make sure that the effect of flow reversal in between iteration is taken care of. Moreover, the common pipe keeps track of the flow rates and temperatures at all the four nodes linked to it; namely, the inlet and outlet nodes of each sub loop. This record will help to decide if loops have converged or not. In situations where the primary component meets the setpoint and the coil controls does not change its flow request, the common pipe converges quickly. The simple description of the control algorithm for common Pipe implementation is as follows:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  At FirstHVACiteration, the common pipe flow is initialized to zero.
+\item
+  Common pipe is simulated at interfaces and thus we will have 2 different flows handle on either side of interface.
+\item
+  Loops and corresponding flow rates are assigned inlet or outlet (to common pipe) depending on the interface which calls it. So when common pipe is called from demand to supply interface, the inlet loop is demand side and outlet loop is supply side and vice versa.
+\item
+  Inlet flow is compared to outlet flow and the difference is set as the common pipe flow.
+\item
+  At each interface the common pipe flow is assigned a direction which can be into the interface (Inlet flow \textless{} Outlet flow) or away from interface (Inlet flow \textgreater{} Outlet flow).
+\item
+  Outlet temperature is calculated depending on the flow rate and flow direction. When flow is away from interface outlet flow temperature is same as inlet flow temperature. For a common pipe flow into the interface, the outlet flow temperature is calculated as mixed temperature of inlet flow and the common pipe flow.
+\item
+  At demand to supply interface, the supply side inlet node temperature and flow rate are updated every iteration. At supply to demand interface, only flow is updated. The temperature is updated only at the end of timestep.
+\item
+  Loops iterate till the flow and temperatures at all the 4 concerned nodes do not change.
+\end{enumerate}
+
+\subsubsection{Two-Way Common Pipe}\label{two-way-common-pipe}
+
+A model referred to as Two-Way Common Pipe is available which provides a way to model Primary-Secondary systems as a single Plant Loop.~ In a typical EnergyPlus plant loop simulation, the only half loop inlet/outlet node that is controlled is the supply side outlet node. In some cases this requirement becomes a limitation in analyzing different options. A good example is ice thermal storage application, where during charging phase, the coil setpoint can be different from the ice storage equipment setpoint. With this model, the interface between the two half loops includes two additional flow paths that essentially split a single plant loop into both primary and secondary loop sides.~ Though the Two-Way common pipe is designed to be generic some assumptions apply in modeling the component. The assumptions are as follows
+
+\begin{itemize}
+\item
+  The secondary flow may be less than, equal to, or greater than the primary flow.
+\item
+  The mass flow rate at the Primary Side Outlet Node is always equal to the mass flow rate at the Primary Side Inlet Node.
+\item
+  The mass flow rate at the Secondary Side Outlet Node is always equal to the mass flow rate at the Secondary Side Inlet Node.
+\item
+  Only one additional node, either primary-side inlet or secondary-side inlet, (along with the primary-side/supply-side outlet node) can be controlled. The system of equations that describe the loop interface will be under specified if both the Primary and Secondary Inlet nodes have to be controlled.
+\end{itemize}
+
+Figure~\ref{fig:schematic-of-a-two-way-common-pipe-used-in} shows a schematic of the Two-Way Common Pipe. There are two common pipe legs, shown as broken lines, allow for some recirculation at the half loop level.~ The model allows for common pipe flow in either or both directions. The model determines flow rates in the common pipes and temperatures at nodes based on the following:
+
+\begin{itemize}
+\item
+  Which additional node is being controlled to meet a temperature setpoint? If the primary-side inlet node is controlled, then the flows are controlled to deliver the desired temperature at supply side inlet. If the secondary-side inlet node is controlled then the flows are controlled to deliver the desired temperature at the demand side inlet.
+\item
+  Is the specified setpoint achievable with current secondary and primary outlet conditions? If the setpoint is not achievable, then the flow in each common pipe leg is reduced to its minimum possible value.
+\item
+  At the controlled node, with known demand outlet temperature, supply outlet temperature, primary flow rate and secondary flow rate, and energy balance is used to calculate recirculation flows in the common pipes for that particular half loop, so that the desired temperature setpoint is achieved.
+\item
+  With a known flow in one common pipe leg, the flow on Primary to Secondary (or secondary to primary) is easily obtained by mass balance.
+\item
+  When the Two Way Common Pipe is controlling conditions at the secondary-side, or demand side, inlet node, then the loop capacitance model usually used for the conditions at the demand inlet is not used as it would interfere with control.
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 126
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1976.svg.png}
+\caption{Schematic of a Two-Way Common Pipe used in Primary-Secondary System. \protect \label{fig:schematic-of-a-two-way-common-pipe-used-in}}
+\end{figure}
+
+\subsection{Heat Recovery Loop Systems}\label{heat-recovery-loop-systems}
+
+Heat Recovery is accomplished by specifying another set of supply and demand loops. Each of the heat recovery components, i.e.~engine driven and combustion turbine chillers, and internal combustion and combustion turbine generators is designed to use the existing component/loop/solution structure to facilitate the simulation with the existing demand side manager and the supply side manager. Heat recovery normally contains components that produce heat that can be recovered, and the ability to store or use that heat elsewhere in the system. The component that can store the excess heat and allow it to be used elsewhere in the system or for domestic hot water is the Water Heater:Simple and is defined in the Input/Output Reference.
+
+\includegraphics{media/image1977.png}.
+
+Figure 127. Example of a Heat Recovery Loop Simulation
+
+In the example above there is a chilled water Loop with chilled water supplied by a diesel engine driven chiller. There is a hot water Loop that is being supplied by the water heater: simple. There is also scheduled domestic hot water usage on the water heater which excess demand can be met by a number of user-specified heating sources. Then on the demand side of the heat recovery loop there is the engine driven chiller, internal combustion, and combustion turbine electric generators with specified mass flows to recover the heat. This hot water is pump on the supply side by the heat recovery pump and provides the heat to the water heater to meet the water heater setpoint. This is probably one of the more complex configurations and interactions that would take place in heat recovery, but using the Plant supply and demand side configurations this can be extended to meet most user configurations. The plant water heater can also be used to just meet scheduled domestic hot water use, provide a hot water source for PlantLoop equipment, or provide a hot water storage tank for heat recovery as a single function. Or any combination of the above can be configured. Example files of some of these configurations are provided with the installation.
+
+\subsection{Plant Pressure Drop Simulation}\label{plant-pressure-drop-simulation}
+
+As of version 4.0, there is an added feature which allows better calculation of pressure in plant and condenser loops. Without any method, the loops essentially ignore the node pressures. This is suitable for many applications, however may cause inaccuracies in the pump power. This is especially prominent in cases where the loop flow may change drastically over a wide range of configurations, as the pump power is based on a rated power value and rated pump head value. As the loop components turn on and off, the pressure drop will change, and so the pump power should be dynamically updated with these changes.
+
+\subsubsection{Overall model features:}\label{overall-model-features}
+
+Calculates loop pressure drop based on pressure drop information which is placed on branches. These are entered in terms of generic curves (linear, quadratic) or pressure drop information (minor loss/friction factor).
+
+Loop pressure drop is used as the new pump head. No information is entered about the pump curve, so it is assumed that the pump will always be able to meet this operating point. Future enhancements will allow the pump to ride a curve based on the given pressure head.
+
+Model does not resolve flow rates on parallel branches to match pressure drop, this is explained further below, but basically it takes the maximum pressure drop from parallel pressure components and applies that to all parallel components.
+
+Model works for the following configurations:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Pump Location
+\item
+  Loop Pump
+\item
+  Branch Pumps
+\item
+  Loop Types
+\item
+  PlantLoop
+\item
+  CondenserLoop
+\end{enumerate}
+
+The supply side inlet (before the pump) is always set to standard atmospheric pressure. This allows the node pressures around the loop to stay positive. The actual values of pressure are not all that important, it is the delta pressure that is of interest for our calculations, but this makes the pressure values appear realistic if one plots the pressure around the loop.
+
+The pressure drop is at the branch level, not the component level. If multiple components are found on a single branch, the pressure drop is always applied to the last component on the branch. This is coordinated with the rule that a pump must always be the first component if it is found on a branch.
+
+Calculations use the branch flow rate and the branch entering temperature to calculate properties for the whole branch.
+
+\subsubsection{Detailed Restrictions:}\label{detailed-restrictions}
+
+Pressure drop curves must not be placed on branches which only contain a pump. Pressure curves may be placed on the supply inlet branch with a pump as long as there are other components on that same branch, following the pump.
+
+If using branch pumps, pressure drop curves found on the supply inlet branch will be ignored. Put pressure drop information after pumps.
+
+Currently, pressure drop simulations are not allowed with common pipe (demand pump) simulations. A future version of the pressure drop system will allow this by allowing each pump to handle the pressure drop of the given loop side (demand or supply).
+
+\subsubsection{Detailed Calculation Steps:}\label{detailed-calculation-steps}
+
+Before the demand side is simulated, the pressure system is initialized. All node pressures are reset, and pressure drop values for branches are re-initialized.
+
+After all components on a branch are simulated, the pressure drop for that branch is calculated. This pressure drop is registered in the pressure drop system to be used in subsequent loop level calculations.
+
+Once the entire loop (demand then supply sides) is simulated, the loop level pressure drop calculations are performed using the following steps:
+
+Beginning at demand side outlet (linked to supply inlet), and working backwards, the node pressure is updated and loop pressure is summed by ``adding pressure drops'' as they are found around the loop. By working backward, we are able to easily preserve the pump inlet pressure as a realistic value (standard atmospheric pressure).
+
+When a parallel system is encountered, a special operation is performed. Since we are not resolving flows with this version of the pressure simulation, the parallel system is set to use the largest value of pressure drop found on the parallel branches. In this manner, the highest pressure drop component essentially governs the set of parallel branches, and the other components must match the pressure drop in order to achieve their desired flow rate. This is performed by placing ``imaginary'' valves in the splitter. This allows individual branches to report their own pressure information, while the splitter accounts for the required pressure drop to match the governing branch. This is shown graphically in the figure below.
+
+\begin{figure}[hbtp] % fig 128
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1978.png}
+\caption{Explanation of valves inherently built into Splitter object \protect \label{fig:explanation-of-valves-inherently-built-into}}
+\end{figure}
+
+Because the splitter automatically handles the pressure drop required to match the pressures in the parallel system, the mixer will have uniform flow entering from all branches and exiting.
+
+These calculations are performed around the loop and result in a value of pressure drop for the entire loop.
+
+Pump power requires a value of pressure head before it can add heat to the loop, which is done before any components are calculated, and any pressure system calculations are performed. Because of this, the pump power is based on rated head during the first iteration. On subsequent iterations, the pump power is based on the dynamic pressure head calculated by pressure drop information.
+
+If anything drastically changes between one iteration and the next, the loop will be re-simulated, and the latest value of pressure head will be used. By the time the loop is converged, the pressure head between the current and most previous iterations will agree to within simulation tolerance. Thus the pump is using a lagged value of pressure head, but once the loop is converged, the lagged and current values will agree.
+
+\subsubsection{Pressure Drop Calculations:}\label{pressure-drop-calculations}
+
+There are two types of pressure drop curves that can be entered, each with its own calculation engine:
+
+Generic: A curve of any form (single independent variable) such as linear or quadratic may represent the pressure drop in Pascals as a function of current mass flow rate in kg/s. This is common for regressing component pressure drop such as heat pumps into a quadratic best fit form. The branch pressure drop is then calculated by evaluating this curve with the given branch flow rate.
+
+Pressure Information: This calculation involves two types of pressure drop: frictional effects and minor losses. The governing equation is:
+
+\begin{equation}
+\Delta P = \left( {f\frac{L}{D} + K} \right)\frac{{\rho {V^2}}}{2}
+\end{equation}
+
+The user enters value for the minor loss coefficient K to represent all the minor losses on that branch. If the user is entering friction information, the minor loss coefficient may be zero or blank.
+
+The user enters roughness, e, or a fixed value of friction factor to account for frictional losses on the branch, as well as an equivalent length L. If the user enters roughness then the friction factor is calculated from a Moody chart approximation (Haaland, 1983):
+
+\begin{equation}
+f = {\left\{ { - 1.8\log \left[ {{{\left( {\frac{{e/D}}{{3.7}}} \right)}^{1.11}} + \frac{{6.9}}{{{\mathop{\rm Re}\nolimits} }}} \right]} \right\}^{ - 2}}
+\end{equation}
+
+If the user enters minor loss information, then the friction factor information can be left out.
+
+The diameter is an equivalent value and is used to calculate relative roughness for friction calculations as well as velocity for any pressure drop calculation.
+
+\subsubsection{Riding Pump Curves to Determine Loop Operating Point}\label{riding-pump-curves-to-determine-loop-operating-point}
+
+In addition to being able to provide a means of calculating loop pressure drop, EnergyPlus can also perform a ``loop-level'' pump-system flow resolution.~ The pressure drop components that were described in the previous sections are combined with the input of a dimensionless pump pressure-flow curve and at each iteration, these are utilized in determining a proper operating point for the loop.
+
+Some restrictions do apply to this simulation.~ As with the basic pressure drop simulation, common pipes are not valid in the current release.~ For this pump curve phase, the simulation is also restricted to ``loop pumps'' such that pumps should not be used on the parallel branches between a mixer and splitter.
+
+The idea of riding a pump curve, as it is currently implemented, is based on a constant speed pump.~ A variable speed pump in EnergyPlus can already effectively vary its flow/pressure characteristics to meet the demand.~ Thus, this phase is only implemented for the Pump:ConstantSpeed model.
+
+The model works by approximating the loop with a quadratic pressure drop form, then iterating to find an operating point.~ The entire plant loop then iterates to find the operating point that attempts to match the requested flows.~ Note that when doing a pressure based pump simulation, the loop will likely not hit setpoint every timestep, while doing the simpler approach (non-pressure) may result in a tighter-controlled simulation.~ In deciding this, you must consider the realism of the pressure approach vs.~the non-pressure approach which may be more tightly controlled and will have less input requirements.
+
+In the first iteration of the plant, there is not yet enough information to determine a pressure-flow simulation, so flow through the loop is set to the rated flow rate of the pump (irrespective of pump performance curve). For this rated flow rate pressure drop in each branch will be calculated by plant pressure system. So after this first pass through the loop, the pressure system now has a valid system flow-pressure point.~ From this point (pressure drop in the branch and rated mass flow rate) a pressure constant for each branch is calculated assuming quadratic relationship between pressure drop and mass flow rate.
+
+\begin{equation}
+{K_{Branch(i)}} = \Delta {P_{Branch(i)}}/{m_{Rated}}^2
+\end{equation}
+
+If there are parallel branches then equivalent K is calculated from following formula.
+
+\begin{equation}
+\frac{1}{{\sqrt {{K_{ParallelEquivalent}}} }} = \sum\limits_{j = 1}^m {\frac{1}{{\sqrt {{K_{Branch(j)}}} }}}
+\end{equation}
+
+From all these `K' values of the branches a corresponding K value for complete loop is calculated. This representative K value for the loop will lock down a system curve for a single iteration.~ This K value will change throughout the higher-level plant iterations and simulation time steps.
+
+The Non-dimensional pump curve is entered in following way,
+
+\begin{equation}
+\psi  = {C_4} \times {\varphi ^4} + {C_3} \times {\varphi ^3} + {C_2} \times {\varphi ^2} + {C_1} \times \varphi  + {C_0}.
+\end{equation}
+
+C\(_{1-4}\) are curve coefficients with last mandatory non-zero constant term C\(_{0}\) (as pump curve will not pass through origin).
+
+The nondimensional variables in the previous equation are defined in terms of the following expressions:
+
+Ψ -- Non-dimensional pressure rise:~ \(\psi = \frac{{\Delta P}}{{\rho {N^2}{D^2}}}\)
+
+φ - Non-dimensional flow:~ \(\varphi = \frac{{\dot m}}{{\rho N{D^3}}}\)
+
+The user preprocesses mass flow and pressure values into these nondimensional forms in order to generate the curve fit.~ The program then resolves the nondimensional forms into actual values based on the pump speed, diameter, and fluid density.~ This gives the proper pressure-flow relationship for the simulation.
+
+\subsubsection{Pump-System Operating Point Flow Resolver:}\label{pump-system-operating-point-flow-resolver}
+
+The pressure drop components and the pump curve are described in the prior sections.~ The routine which actually uses these curves to resolve to an operating point is described here.~ This routine is called by the pump model as it is determining what flow it should be using.~ The flow resolver reads the non-dimensional pump curve, loop pressure constant (K value) and rated mass flow rate (or mass flow rate from last iteration). The resolver finds the intersection of the two curves by successive substitution with 0.9 as a damping factor. If the flow rate is outside (or if in any iteration move out of) the range for which pump curve-fit is suggested, the resolver will bring the value within range, thus it is important to specify the curve-fit range (in terms of non-dimensional flow rate) for pump curve by the user.~ It was observed that simple successive substitution (sometimes) diverges depending on shape of curves and/or location of operating point. Damping factor provides stability to successive substitution and it was observed that it converges for less number of iteration, speeding up the function. The damping factor was set as 0.9 as it showed full stability during testing, although a more optimum value may be available for a particular set of curves.~ A future version may have an improved selection algorithm for the damping factor itself.
+
+\subsubsection{References}\label{references-037}
+
+Haaland, SE. 1983. ``Simple and Explicit Formulas for the Friction Factor in Turbulent Flow''. Transactions ASIVIE, Journal of Fluids Engineering 103: pp.~89-90.
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager/plant-load-profile.tex b/doc/engineering-reference/src/building-system-simulation-system-manager/plant-load-profile.tex
new file mode 100644
index 00000000000..7a6a938357c
--- /dev/null
+++ b/doc/engineering-reference/src/building-system-simulation-system-manager/plant-load-profile.tex
@@ -0,0 +1,43 @@
+\section{Plant Load Profile}\label{plant-load-profile}
+
+The LoadProfile:Plant object is used to simulate a scheduled demand profile. This can be useful when the building loads are already known. Demanded load and flow rate are schedules specified in the object definition. The load profile can specify heating and cooling loads. Cooling loads are entered as negative numbers. The actual load met is dependent on the performance of the supply loop components.
+
+The LoadProfile:Plant object must be connected on the demand side of the plant loop. If desired, multiple LoadProfile:Plant objects can be combined in series and/or parallel.
+
+\subsection{Calculation Model}\label{calculation-model}
+
+The LoadProfile:Plant object calculates the outlet water temperature based on the inlet water temperature from the plant loop and user inputs for the scheduled plant load and the requested flow rate.~ The calculation can be expressed with the equation:
+
+\begin{equation}
+{T_{out}} = {T_{in}} - \frac{{{Q_{load}}}}{{\dot m{c_p}}}
+\end{equation}
+
+where
+
+\({T_{out}}\) ~ = the outlet water temperature
+
+\({T_{in}}\) ~ = the inlet water temperature
+
+\({Q_{load}}\) ~ = the scheduled plant load
+
+\(\dot m\) ~ = the water mass flow rate
+
+\({c_p}\) ~ = the specific heat of water
+
+The user requested flow rate is not always available from the plant loop.~ The actual flow rate used in the calculation is the lesser of the user requested value and the plant available value.
+
+Note that the LoadProfile:Plant object can still request and receive flow even if the scheduled plant load is zero.~ In this case the outlet temperature will be the same as the inlet temperature.~ This allows users to drive the plant loop flow without necessarily affecting the loop temperature.
+
+For reporting purposes the energy consumption of the object is calculated using the equation:
+
+\begin{equation}
+E = {Q_{load}}\Delta t
+\end{equation}
+
+where
+
+\(E\) ~ = the energy consumption
+
+\({Q_{load}}\) ~ = the scheduled plant load
+
+\(\Delta t\) ~ = the time step interval
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager/primary-air-system-simulation.tex b/doc/engineering-reference/src/building-system-simulation-system-manager/primary-air-system-simulation.tex
new file mode 100644
index 00000000000..bd651351116
--- /dev/null
+++ b/doc/engineering-reference/src/building-system-simulation-system-manager/primary-air-system-simulation.tex
@@ -0,0 +1,245 @@
+\section{Primary Air System Simulation}\label{primary-air-system-simulation}
+
+When the EnergyPlus HVAC simulation manager needs to simulate the primary air system side of the air loop it calls \emph{ManageAirLoops}, the primary air system simulation manager subroutine.
+
+Note that ``air loop'' is used inconsistently in the program: sometimes it means the full loop consisting of both supply \& demand sides -- primary air system and zone equipment; sometimes it means just the supply side -- the primary air system.
+
+Like the other manager routines in EnergyPlus, \emph{ManageAirLoops} has a very simple structure:
+
+Table 39.~ ManageAirLoop Code
+
+\begin{lstlisting}
+IF (GetInputFlag) THEN  !First time subroutine has been entered
+      CALL GetAirPathData ! Get air loop descriptions from input file
+      GetInputFlag = .false.
+  END IF
+\end{lstlisting}
+
+\begin{lstlisting}
+    ! Initialize air loop related parameters
+  CALL InitAirLoops(FirstHVACIteration)
+\end{lstlisting}
+
+\begin{lstlisting}
+    ! Call the AirLoop Simulation
+  IF (SysSizingCalc) THEN
+    CALL SizeAirLoops
+  ELSE
+    CALL SimAirLoops(FirstHVACIteration,SimZoneEquipment)
+  END IF
+\end{lstlisting}
+
+\begin{lstlisting}
+  ! No Update
+\end{lstlisting}
+
+\begin{lstlisting}
+    ! Report information at the Manage Air Loop Level
+  CALL ReportAirLoops
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  ~If the user input data has not been input, get the data and store it in the air loop data structures.
+\item
+  Perform air loop initialization calculations:
+\end{enumerate}
+
+\begin{lstlisting}
+a.  at the beginning of the simulation (one time initializations);
+\end{lstlisting}
+
+\begin{lstlisting}
+b.  at the start of each environment (design day or simulation run period);
+\end{lstlisting}
+
+\begin{lstlisting}
+c.   before each air loop simulation.
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{2}
+\item
+  If automatic sizing of the loop flow rates is called for, do it.
+\item
+  Otherwise perform a simulation of the air loop.
+\end{enumerate}
+
+\subsection{Input data}\label{input-data}
+
+The input data specifying an air loop consists of:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\tightlist
+\item
+  the loop configuration;
+\end{enumerate}
+
+\begin{lstlisting}
+a.  Splitters, Mixers, and Branches;
+\end{lstlisting}
+
+\begin{lstlisting}
+b.  Components on the Branches
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  loop control;
+\end{enumerate}
+
+\begin{lstlisting}
+a.  Controllers;
+\end{lstlisting}
+
+\begin{lstlisting}
+b.  System Availability Managers;
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{2}
+\item
+  connection to zone equipment;
+\item
+  design flow rate.
+\end{enumerate}
+
+These objects and their data are described in the EnergyPlus \emph{Input Output Reference} document. The utility routines used to get and check the data are described in the EnergyPlus \emph{Guide for Module Developers}, section Input Services.
+
+\subsection{Initialization Calculations}\label{initialization-calculations}
+
+\subsubsection{One Time Calculations}\label{one-time-calculations}
+
+\paragraph{Zones Served by System}\label{zones-served-by-system}
+
+The main one time calculation involves figuring out what zones are served by each air loop. The EnergyPlus input does not explicitly describe which zones receive supply air from a given air loop. Instead that knowledge is embedded implicitly in the overall air loop -- zone equipment network description. For sizing calculations it is important to have a data structure that explicitly shows which zones each air loop serves. For instance, the air loop design supply air flow rate is obtained by summing the design heating or cooling air flow rates of the zones connected to the air loop.
+
+For each air loop, the following calculation is performed.
+
+(1)~~For each air loop outlet branch, the corresponding zone equipment inlet node is identified.
+
+(2)~~This node number is compared to the inlet node of all AirLoopHVAC:SupplyPaths. When a match is found, the AirLoopHVAC:ZoneSplitter for this supply path is identified.
+
+(3)~~The outlet nodes of the AirLoopHVAC:ZoneSplitter are compared to the cooling inlet nodes of all the zone ZoneHVAC:AirDistributionUnits. When a match is found this zone is identified as being served by cooling supply air from the air loop.
+
+(4)~~Similarly the outlet nodes of the AirLoopHVAC:ZoneSplitter are compared with the heating inlet nodes of all ZoneHVAC:AirDistributionUnits. A match indicates that this zone is served by heating supply air from the air loop.
+
+(5)~~The case where there is no AirLoopHVAC:ZoneSplitter for a AirLoopHVAC:SupplyPath must be handled. In this case the program looks for a match between the zone equipment inlet node and an ZoneHVAC:AirDistributionUnit heating or cooling inlet node. When a match is found that zone is identified as being served with heating or cooling supply air from the air loop.
+
+(6)~~The list of cooled and heated zones are saved in the air loop data structure AirToZoneNodeInfo.
+
+\paragraph{Branch Sizing}\label{branch-sizing}
+
+If this \emph{not} an air loop sizing calculation, but is the first pass through the HVAC code in a normal simulation, loop over all the branches in all air loops and trigger the branch design air flow auto-sizing calculation. The actual calculation is described in the Sizing section of this document.
+
+\subsubsection{Begin Environment Initializations}\label{begin-environment-initializations}
+
+For each air loop, loop over all the branches in the loop. Initialize each branch mass flow rate:
+
+\begin{equation}
+{\dot m_{br,\max }} = {\rho_{std}} \cdot {\dot V_{br,\max }}
+\end{equation}
+
+\begin{equation}
+{\dot m_{br,\min }} = {\rho_{std}} \cdot {\dot V_{br,\min }}
+\end{equation}
+
+where \({\rho_{std}}\) ~is the density of air at 20 degrees C, humidity ratio = 0, standard pressure.
+
+For each branch, loop over all the nodes on the branch and set the node data to the following values:
+
+\begin{equation}
+{T_{node}} = {20^{\rm{o}}}C
+\end{equation}
+
+\begin{equation}
+{W_{node}} = {W_{oa}}
+\end{equation}
+
+\begin{equation}
+{h_{node}} = {\mathop{\rm PsyHFnTdbW}\nolimits} {\rm{(}}20.0,{W_{oa}}{\rm{)}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{node}} = {\dot m_{br,\max }}
+\end{equation}
+
+\begin{equation}
+{\dot m_{\max ,node}} = {\dot m_{br,\max }}
+\end{equation}
+
+\begin{equation}
+{\dot m_{\max avail,node}} = {\dot m_{br,\max }}
+\end{equation}
+
+\begin{equation}
+{\dot m_{\min ,node}} = 0.0
+\end{equation}
+
+\begin{equation}
+{\dot m_{setpt,node}} = 0.0
+\end{equation}
+
+\begin{equation}
+{\dot m_{\min avail,node}} = 0.0
+\end{equation}
+
+\begin{equation}
+{p_{node}} = {p_{std,baro}}
+\end{equation}
+
+\begin{equation}
+Q{u_{node}} = 0.0
+\end{equation}
+
+where \({W_{oa}}\) ~is the humidity ratio of the outside air; \({\rm{PsyHFnTdbW}}\) is the EnergyPlus psychrometric function for enthalpy \emph{h}, given temperature and humidity ratio; and \emph{Qu} is quality.
+
+\subsubsection{System Time Step Initializations}\label{system-time-step-initializations}
+
+For each branch in each air loop, loop over all the nodes on the branch and set \({\dot m_{setpt,node}} = 0.0\) ; if it is the start of an HVAC solution sequence set \({\dot m_{\max avail,node}} = {\dot m_{\max ,node}}\) . Then set the mass flow rate setpoints for the air loop nodes.
+
+1)~~~~On each air loop, loop over the outlet branches and find the loop outlet nodes. If it is the start of an HVAC solution sequence, set \({\dot m_{setpt,outletnode}} = {\dot m_{outletbr,\max }}\) . This will insure that during the first pass through the full loop that the mass flow rate will be at the maximum. Otherwise, set \({\dot m_{setpt,outletnode}} = {\dot m_{zone{\rm{ }}eq{\rm{ }}inletnode}}\) . This sets the air loop flow rate to the total zone requirement.
+
+2)~~~~Pass the mass flow rate setpoint upstream to the start of the outlet branches; through the splitter, if one exists; and upstream to the beginning node of the splitter inlet branch.
+
+3)~~~~Sum the total return air mass flow rate and save it in the AirLoopFlow data structure.
+
+4)~~~~For each air loop, loop over the inlet nodes and, at the start of each HVAC solution sequence, set the entering node mass flow rate equal to the primary air system design mass flow rate (subject to it not being larger than the entering node mass flow rate setpoint).
+
+\subsection{Central air system simulation}\label{central-air-system-simulation}
+
+The subroutine \emph{SimAirLoops} does the actual simulation the central air system equipment for all the air loops. The simulation of a full air loop (central equipment plus zone terminal units and equipment) requires the interaction of 2 managers: \emph{ManageAirLoops} and \emph{ManageZoneEquipment}. Thus a single call to \emph{SimAirLoops} results in a simulation of all the central air system equipment, but this is one part of a larger iterative simulation of the full air loops involving the zone equipment as well.
+
+\emph{SimAirLoops} accomplishes its task using a set of nested loops.
+
+\begin{itemize}
+\item
+  Loop over all of the central air systems (\emph{Air Primary Loops}).
+\item
+  For each air system, make 1 or 2 simulation passes
+\item
+  Loop over each controller in the \emph{Air Primary Loop}
+\item
+  For each controller, repeat the simulation of all the \emph{Air Primary Loop} components until the controller has converged
+\item
+  Loop over each branch in the \emph{Air Primary Loop}
+\item
+  On each branch, simulate in sequence each component
+\end{itemize}
+
+During and at the end of each loop some tests are performed.
+
+At the end of the first pass of loop 2, a decision is made on whether a second pass is needed. The first pass has been performed assuming that there is a mass flow balance in the central air system simulation. This is usually the case. A call to \emph{ResolveSysFlow} checks the mass balance and imposes a mass balance if there is not a balance. The lack of a system mass balance requires a resimulation of the central air system: i.e., a second pass in loop 2.
+
+In loop 3 a call to \emph{ManageControllers} simulates controller action and checks for controller convergence. If convergence is achieved loop 3 is exited.
+
+After all the controllers on a loop are converged,~ steps 5 \& 6 are repeated one more time to ensure all the components on the loop have final values.
+
+At the end of the primary air system simulation a call to \emph{UpdateHVACInterface} passes the primary air system outlet node data to the zone equipment inlet nodes. If the data across the supply side -- demand side gap doesn't match to within a preset tolerance, the flag \emph{SimZoneEquipment} is set to \emph{true} to ensure that the zone equipment side gets resimulated. Finally a flag indicating whether the economizer is active is set. This flag is used at a higher level to decide whether the primary air system needs to be resimulated if an HVAC component is calling for economizer lockout.
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager/steam-systems-and-component-models.tex b/doc/engineering-reference/src/building-system-simulation-system-manager/steam-systems-and-component-models.tex
new file mode 100644
index 00000000000..b386cf4bffa
--- /dev/null
+++ b/doc/engineering-reference/src/building-system-simulation-system-manager/steam-systems-and-component-models.tex
@@ -0,0 +1,477 @@
+\section{Steam Systems and Component Models}\label{steam-systems-and-component-models}
+
+A steam system uses the vapor phase of water to supply enthalpy or kinetic energy through the piping network.~ In case of EnergyPlus, the steam system is designed to provide energy solely for the building heating requirements.~ Hot steam from the boiler or steam generator in buildings can be used to heat a conditioned space with suitable heat transfer equipment such as fan-coils units, unit-heaters, radiators and convectors or steam can also heat water through shell and tube heat exchangers, and hot water can be supplied to the terminal units to provide the zone heating requirements.
+
+The advantages that steam system offer over hot water or other heating systems are:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Steam flows through the system unaided by external energy source such as pumps; pressure difference moves steam across the system.
+\item
+  Steam, because of its low-density, can be used in high-rise buildings where water systems create excessive pressure.
+\item
+  Terminal units such as heating coils can be added or removed without making any changes to the system.
+\item
+  Steam components can be repaired or replaced by closing the steam supply without the difficulties associated with draining and refilling like in the water systems.
+\item
+  Steam is pressure-temperature dependent, therefore the system temperature can be controlled by varying either steam pressure or temperature.
+\item
+  Steam can be distributed through out the system without any change in temperature.
+\end{enumerate}
+
+In view of the advantages mentioned, the steam systems are suitable for applications where heat is required for process and comfort heating such as in industrial plants, hospitals, restaurants, dry cleaning plants laundries and commercial buildings.~ They are also suitable in places where the heating medium has to travel great distances such as in facilities with scattered building locations or where the building height would result in excessive pressure in a water system, or locations where the load changes occur intermittently.~ Thus steam system is an essential and necessary development step for EnergyPlus.
+
+From EnergyPlus simulation point of view, the advantage associated with a steam system is that steam can be distributed through out the system without change in temperature.~ This means that the boiler outlet temperature can simply be set equal to the heating coil inlet temperature for a steam system.
+
+Another simulation-based advantage associated with the steam system is Steam Quality, which does not change from boiler outlet to coil inlet.~ Actual building steam systems are equipped with condensate drains through out the system, these drains remove, almost immediately any condensate that is formed during steam transportation, thereby maintaining the steam quality at constant value of 1.0 through out the high-pressure steam side.
+
+The HVAC steam system implementation includes simulation models for two phase steam equipment like steam boiler, steam to air heating coils, steam pipes and condensate pumps, which can be connected to the generic loop framework.
+
+\subsection{Steam Loop Assumptions}\label{steam-loop-assumptions}
+
+To replicate the working of an actual building steam system in a satisfactory manner with simulation, it was necessary to make certain assumptions.~ These assumptions help simplify the loop complexity and increase usability.~ The effects of the assumptions made are described in detail below.
+
+The following figure describes the Temperature Entropy Ts diagram based on which the steam system operates in EnergyPlus.~ The steam side of the loop operates on constant saturation pressure of steam: PSteam, the waterside of the loop operates at atmospheric pressure Patm.
+
+\begin{figure}[hbtp] % fig 129
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1986.png}
+\caption{Schematic of Temperature – Entropy Diagram for Steam loop \protect \label{fig:schematic-of-temperature-entropy-diagram-for}}
+\end{figure}
+
+It should be noted that the figure is simply a schematic and not a scaled representation of the process on a Mollier Chart.~ For the following descriptions, please refer to the schematic figure above.
+
+\begin{itemize}
+\item
+  ~Process 1--2 on the Ts diagram, represents condensation of steam in the coil at constant pressure; this is where the steam gives up latent heat to the zone.
+\item
+  ~Process 2--3 represents the subcooling of condensed steam at higher pressure, this subcooling takes place inside the steam coil, just before the steam trap.~ The delta temperature represented by 2-3 is the degree of subcooling in the steam coil, and is a user input to the steam coil.~ This subcool generally accounts for 1 to 2 \% of the total heat transfer in the steam coil.
+\item
+  ~Process 3--4' represents the isenthalpic expansion of water from high-pressure steam side to atmospheric pressure across the steam trap.~ As steam gives up its latent heat at the steam coil the condensate that forms in the steam coil still exists at higher pressure.~ This condensate is discharged to a lower pressure across the steam trap, this condensate contains more heat than necessary to maintain the liquid phase at the lower pressure, this excess heat causes some of the condensate to vaporize or flash to steam at lower pressure at some quality.~ The amount of water that flashes to steam can be calculated by the following equation
+\end{itemize}
+
+\begin{equation}
+\% Flash\,\,Steam\,\, = \frac{{{h_{4'}} - \,{h_4}}}{{{h_{fg}}}}\,\, \times \,\,\,100
+\end{equation}
+
+Where h4' is Enthalpy of liquid at steam pressure just before condensate is supposed to leave the coil.~ Enthalpy at Point 3 is equal to enthalpy at point 4', since it is an isenthalpic process, and~ hfg is the latent enthalpy of the fluid at atmospheric pressure.
+
+For example, water at 102LC and 120 Kpa flashes to steam at at100LC and atmospheric pressure, with quality equal to 0.003.~ This results in loss of some latent capacity of steam and is one of the terms contributing to loop loss in steam system.
+
+\begin{itemize}
+\item
+  ~Process 4'- 4 represents the condensation of the flashed steam, which has exited from steam trap into the condensate drain.~ Condensation occurs at atmospheric pressure Patm, there is loss in latent capacity due to this unavoidable process, only condensate can be returned back to the boiler in a steam system.
+\item
+  ~Process 4-5 represents the loop sub cooling at atmospheric pressure; this is the sub cooling of the condensate that takes place during condensate return to the boiler because the return loop is not insulated, loop sub cooling is of the order of 20LC to 30LC.~ This is a user-defined input in every steam coil, because the variability in location of steam coils in a building will result in different condensate return temperatures for each of the coils.
+\item
+  ~Process 5-6 represents the temperature and pressure rise in condensate due to pump heat addition.~ The pumping process generates heat, which is added to the condensate.~ The condensate is pumped back to the boiler at higher pressure.
+\item
+  ~Process 6-2 represents the sensible heat addition by the boiler to the return condensate.
+\item
+  ~Process 2-1 represents the latent enthalpy of steam, added by the boiler to the water to convert it to steam at saturation pressure.
+\item
+  ~Point 3, which is outlet of the coil and Point 5, which is inlet of the pump are specified directly by the user, subsequently the loop losses in EnergyPlus are directly summed up as the enthalpy difference between point 3 and 5, which is calculated by fluid property routines in EnergyPlus.~ This helps to maintain flexibility and at the same time helps negate the intermediate points calculation in the system.
+\end{itemize}
+
+Aspects of the steam loop such as quality of steam, steam pressure, and steam generation which play an important role in EnergyPlus simulation are described in following sections.
+
+\subsubsection{Constant Pressure Steam loop}\label{constant-pressure-steam-loop}
+
+The steam loop in EnergyPlus is pressure driven and it is assumed to operate at constant pressure on the gaseous-steam part, while the condensate return loop is assumed to operate at atmospheric pressure.~ The steam loop essentially operates at saturation pressure corresponding to the steam temperature; the steam boiler serves to maintain the loop temperature.~ The boiler model determines the amount of energy required to generate the required amount of steam.
+
+Factors such as friction in pipes, which tend to cause small amount of pressure drop in steam loop are neglected in the model.~ It is assumed that the steam pipes are fairly well insulated to prevent heat loss and subsequent condensation of steam in the pipes.~ In actual systems small quantities of steam, which condenses due to heat loss during transportation is removed immediately from the system by steam drains.~ This helps eliminate water hammer, degradation of steam quality and heat transfer capability.
+
+\subsubsection{Steam Generation at Saturated Conditions:}\label{steam-generation-at-saturated-conditions}
+
+Building steam heating systems avoid supplying superheated steam because superheat damages the building HVAC equipment.~ Superheated steam is generated only if there is a cogeneration power system in building such as steam turbine, which requires superheated steam.~ The purpose of having superheated steam is redundant for building steam heating systems because the amount of energy carried by the same is negligible compared to the latent heat. A simple enthalpy calculation, based on each unit of steam mass flow rate (1 kg/s), has been provided in this section to describe the negligible effect of superheat..
+
+Case 1: Loop Operating at Saturation Conditions (no superheat), calculating enthalpy of saturated steam at boiler outlet temperature.
+
+Boiler Outlet Temperature = 105BC,
+
+\begin{equation}
+{h_{Case1:NoSuperheat}} = [{h_f}_{{{105}^ \bullet }C}]
+\end{equation}
+
+\begin{equation}
+{h_{Case1:NoSuperheat}} = \,\,\,\,2684000\,\,\,\,\,\,J
+\end{equation}
+
+Case 2: Loop operating with Superheated steam, calculating enthalpy of superheated steam for 5BC superheat.
+
+Degree of Superheat = 5BC
+
+Boiler Outlet Temperature = 110BC,
+
+\begin{equation}
+{h_{Case2:Superheat}} = [{h_f}_{{{110}^ \bullet }C}]
+\end{equation}
+
+\begin{equation}
+{h_{Case2:Superheat}} = \,\,\,2691000\,\,\,\,\,\,\,\,J
+\end{equation}
+
+The energy difference between the superheated state and the saturated state as calculated in the following equation.~ A 5BC superheat provides only a 0.2608\% increase in heat transfer.~ The advantage of this additional increase in heat transfer is negligible, especially when considering the economic aspect of sizing a bigger heat exchanger to accommodate additional superheat transfer.~ The detrimental effects of superheated steam on the building HVAC system also come into effect once superheat is used.
+
+\begin{equation}
+\Delta {Q_{2 - 1}}\,\,\, = \,\,\,\frac{{2691000\, - 2684000}}{{2684000}}\,\, \times 100\,\,\,\, = \,\,0.2608\,\,\,percent
+\end{equation}
+
+Based on the reasoning above the steam loop in EnergyPlus is designed and implemented to operate at saturated conditions.
+
+\subsubsection{Steam Quality}\label{steam-quality}
+
+The boiler operation is assumed capable to generate steam at quality equal to1.0 every time.~ This is a reasonable assumption, since in practice the variability in generated steam quality would only occur if the boiler operation were not properly controlled.
+
+The steam loop is assumed to have perfect transport mechanism.~ There is no transportation losses due to friction and heat transfer with surroundings.~ This assumption helps maintain the quality of steam through out the system constant value of either 0 or 1.
+
+Steam enters the coils at boiler outlet conditions.~ Steam coils are designed with steam traps, which only allow condensed steam to leave the coil; hence the steam always condenses and leaves the coil at quality of 0.0.
+
+With the above simplifying assumption enables the EnergyPlus steam loop to be solved without problems.
+
+\subsubsection{Steam Traps}\label{steam-traps}
+
+Steam traps are essential part of the steam system; they are indirect flow controllers of the loop.~ Purpose of steam trap is to allow only condensate out of the coil from higher-pressure steam to lower atmospheric pressure condensate return line.~ Points 3-4C, in schematic~ Figure~\ref{fig:schematic-of-temperature-entropy-diagram-for}, represent this process across the steam trap on the Ts diagram.~ The expansion process across the steam trap is assumed to be isenthalpic.~ There is possibility of flashing of high-pressure condensate across the trap because of pressure drop, resulting in generation of steam at lower pressure, this steam generated at lower pressure subsequently condenses in the return piping, and heat is lost to the atmosphere.~ This heat lost is a part of the steam loop losses.
+
+Steam traps are modeled in the EnergyPlus steam coil by assigning the condensate outlet from the coil a quality of 0.0 and sub cooling the condensate at lower pressure.
+
+Although condensate from the steam coil contains valuable heat, attempting to utilize this heat by holding the condensate in the coil reduces the heat transfer area.~ It causes operational problems because it retains air, which further reduces heat transfer and non-condensable gases such as carbon dioxide, which cause slow corrosion of the steam coil.~ Steam moves rapidly in mains and supply piping so when condensate accumulates to the point where the steam can push a slug of it, serious damage can occur from the resulting water hammer, hence the condensate should be immediately removed from the steam coil.~ This is achieved with steam traps.
+
+Hence an ideal steam trap should remove all condensate, air, and non-condensable gases that might be in the system, with little or no loss of steam.
+
+\subsubsection{Loop Losses}\label{loop-losses}
+
+Subcooling of condensate in condensate return piping and flash steam condensing across the steam trap constitute the unavoidable loop losses in the EnergyPlus simulation steam system.~ These losses can be inferred from Figure~\ref{fig:schematic-of-temperature-entropy-diagram-for} and are summed up by calculating enthalpy difference between points 3 and 5 on the schematic Ts diagram.
+
+Unavoidable losses in the EnergyPlus steam loop occur due to pressure drop across the steam trap, which causes flashing of steam and loss in some percentage of latent heat of steam, process 3-4' and 4'-4 on the Ts diagram in Figure~\ref{fig:schematic-of-temperature-entropy-diagram-for}.~ The condensate is pumped backed to the boiler through return pipe network, which is not insulated.~ Sub cooling of the condensate occurs in the return network, represented by process 4-5 on the Ts diagram in Figure~\ref{fig:schematic-of-temperature-entropy-diagram-for}.~ This loop sub cool contributes to significant percentage of loop losses.
+
+In practical systems the return pipeline to the boiler is not insulated despite the condensate containing some valuable heat, however due to low mass flow rate of steam, this amount is negligible and only recovered if separate heat recovery systems are used by coupling them to the loop.~ The condensate is occasionally collected in a receiver and then pumped back to the boiler.~ EnergyPlus simulation mimics practical systems by assumed that the return pipeline is not insulated and accounts for this by calculating loop losses.
+
+The loop losses are calculated in the steam coil simulation model rather that the steam pipe simulation, because the condensate sub cool in the return loop is a direct function of the location of the steam coil in the building.~ In building energy software like EnergyPlus the user would have a fair idea about location of steam coils rather than the location of condensate return piping.
+
+\subsection{Steam To Air Heat Exchanger}\label{steam-to-air-heat-exchanger}
+
+\subsubsection{Description of Model:}\label{description-of-model-001}
+
+The steam to air heat exchanger (Coil:Heating:Steam input object) is the terminal equipment in the steam loop on the demand side that satisfies the heating requirements of the various zones.~ The steam-to-air heat exchanger simulation model in EnergyPlus calculates the mass flow rate of steam desired to meet the heating demand.
+
+A heating coil can be used either as a zone coil or a coil in the air loop depending on the user and application.~ The steam coil simulation model is designed to take these two locations into consideration.~ An air-loop steam heating coil is temperature controlled and the zone coil is zone load controlled.~ This relatively simple and straightforward concept of coil control is preferred over the iterative method to determine mass flow rates using various numeric techniques.~ The assumptions made in the coil model are described in the section below.
+
+This model accounts for the latent heat transfer and sensible cooling of water; the question of superheat is eliminated because steam is assumed to be saturation conditions.~ Steam enters the coil at quality equal to 1.0, at saturation temperature and leaves the coil with desired degree of sub cooling.~ The user inputs the desired degree of subcooling, which determines the condensate outlet condition from the coil.
+
+EnergyPlus heat balance methods determine the amount of heating required in the zone to maintain the zone at the desired conditions.~ Based on this value of heating load, the zone coil determines the mass flow rate of steam required since the heating coil load is the control variable in a zone coil.~ The following equation describes this calculation to determine steam mass flow rate required for the desired heating capacity. The steam latent heat of vaporization, \emph{h}\(_{fg}\) and the condensate heat capacity, \emph{C}\(_{p,w}\) are evaluated at the steam coil inlet node temperature and standard barometric pressure of 101325.0 Pa.
+
+\begin{equation}
+{\dot m_{zc}}\,\,\,\, = \,\,\,\,\,\frac{{{Q_{zc}}}}{{{h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}}}}
+\end{equation}
+
+In case of the air loop-heating coil, the load on the coil is calculated within the coil simulation routine.~ The air loop coil is setpoint controlled and heats the air to maintain the air stream at the desired setpoint, the setpoint is a user input, generally in the range of 12B C to 16BC. The following equation describes the air loop coil load.
+
+\begin{equation}
+{Q_{al}}\,\, = \,\,{\dot m_a}\,\,\, \times \,\,\,\,\,{c_{p,a}}\,\,\, \times \,\,\,\,\,\left[ {{T_{sp}}\,\,\, - \,\,\,{T_a}} \right]
+\end{equation}
+
+The following equation is used to determine the steam mass flow rate required by the air loop coil to meet the heating requirements.
+
+\begin{equation}
+{\dot m_{al}}\,\,\,\, = \,\,\,\,\,\frac{{{Q_{al}}}}{{{h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}}}}
+\end{equation}
+
+Each of the zone coils and air loop coils are simulated independently and the steam mass flow rates for each is added over every time step of simulation.~ This value of total mass flow rate is reported to the boiler, which in turns supplies this required amount of steam.
+
+The control of the steam to air coil is a complex issue.~ The loop splitter-splits total steam flow from the boiler and delivers the required amount of steam to each of the coils connected to the loop through the steam pipe network.~ In cases where the system is undersized, the coils demand more mass flow rate of steam than the boiler can generate.~ The splitter in this case cannot provide all the coils with requested steam mass flow.~ Subsequently the coils are starved of steam and the zone temperatures fall.~ In some cases the user might schedule off the coil, they should then not operate.~ These issues need to be taken care of in the implementation of the steam coil simulation model.~ The control algorithm for the steam coil operation under various situations is best explained with the help of pseudo-code using standard IF THEN ELSE blocks.
+
+*********************PSEUDO CODE SECTION STARTS**************************
+
+\subsubsection{Steam coil is zone load controlled.}\label{steam-coil-is-zone-load-controlled.}
+
+\begin{equation}
+IF\,\,\,\,\,(Coil\, = LoadControlled)\,\,\,\,\,\,THEN\,
+\end{equation}
+
+Check for operational conditions only then continue simulation further.~ The operational conditions are the inlet mass flow rates of steam and air to the coil, the user schedule to the coil and heating load on the coil.~ The coil is simulated only if these conditions are met.
+
+\begin{equation}
+IF\,\,\,\left[ {\,({{\dot m}_s}\,\,\, > \,\,\,0)\,\,.\,\,\,and.\,\,\,({{\dot m}_a} > \,\,\,0)\,\,.and.\,\,(Schedule\,\, = \,\,\,ON)\,.and.\,\,\,({Q_{ZC}}\,\, > \,\,0.0)\,} \right]\,\,\,THEN
+\end{equation}
+
+If the heating demand from the zone-heating coil is greater than coil capacity, then the heating coil is undersized, and the coil can only deliver its maximum heating capacity to the zone.~ In this case the heating demand on the coil is set equal to this lower value of maximum heating capacity.~ If the above is not true then the simulation ignores this statement and proceeds to the next one.
+
+\begin{equation}
+IF\,\,\,\left[ {\,\,\,({Q_{ZC}}\,\, > \,\,{Q_{Z{C_{Max}}}})} \right]\,\,\,\,\,\,THEN\,\,\,\,\,\,\left[ {{Q_{ZC}} = \,\,{Q_{Z{C_{Max}}}}} \right]
+\end{equation}
+
+The following equation calculates the steam mass flow rate required by the coil.~ This flow rate is required to meet the heating requirements for the zone.~ This value of mass flow is requested from the splitter outlet.
+
+\begin{equation}
+{\dot m_{zc}}\,\,\,\, = \,\,\,\,\,\frac{{{Q_{zc}}}}{{{h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}}}}
+\end{equation}
+
+If the calculated value of steam mass flow with the previous equation is greater than the maximum inlet steam flow that the splitter can provide to the coil at that time step.~ Then the requested coil flow rate is set equal to the inlet steam flow rate.~ This is the maximum amount of steam that can be supplied to the coil at this moment.~ The coil can provide heating capacity equal to this limited amount of steam.~ If the requested flow rate is less that what the splitter can provide then the program ignores the logic of the IF Loop Below
+
+\begin{equation}
+IF\,\,({\dot m_{zc}}\,\, > \,\,{\dot m_{in}})\,\,THEN\,\,(\,\,\,{\dot m_{zc}}\,\, = \,\,{\dot m_{in}})
+\end{equation}
+
+Re-Calculating the coil heating capacity with the lower value of steam mass flow rate.
+
+\begin{equation}
+{Q_{ZC}} = {\dot m_{zc}}\,\, \times \,\,({h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}})
+\end{equation}
+
+\begin{equation}
+END\,\,IF
+\end{equation}
+
+The following equations calculate the outlet condensate-water and outlet air temperatures to the zone based on the amount of heating capacity provided by the coil.
+
+~~~~~ \[T{w_{out}} = \,\,T{s_{in}}\,\, - \,\,\,\Delta {T_{sc}}\]
+
+\begin{equation}
+T{a_{out}}\,\,\, = \,\,T{a_{in}}\,\, + \,\,\,\frac{{{Q_{zc}}}}{{\,{{\dot m}_a}\, \times \,\,\,{c_{p,a}}}}
+\end{equation}
+
+\[ELSE\] Else the coil is not running and in this case set outlets to inlets.
+
+\begin{equation}
+{\dot m_s} = 0\,,\,\,\,{\dot m_a} = 0\,,\,\,\,\,\,\,\,\,\,\,\,\,{Q_{zc}} = 0,\,\,\,\,\,\,\,\,\,\,\,\,T{w_{out}} = T{s_{in\,\,,\,\,\,\,}}\,\,\,\,\,\,T{a_{out}} = T{a_{in}}
+\end{equation}
+
+\begin{equation}
+END\,\,IF
+\end{equation}
+
+\(END\,\,IF\) ~End IF for the zone load controlled coil.
+
+\subsubsection{Steam coil is temperature controlled.}\label{steam-coil-is-temperature-controlled.}
+
+\begin{equation}
+IF\,\,\,\,\,(Coil\, = TemperatureControlled)\,\,\,\,\,\,THEN\,
+\end{equation}
+
+Check for operational conditions and continue simulation further.~ The operational conditions are the inlet mass flow rates of steam and air to the coil, the user schedule to the coil and delta temp exists between the setpoint and air inlet temperature.~ The coil is simulated only if these conditions are met.
+
+\begin{equation}
+IF\,\left[ \begin{array}{l}\,({{\dot m}_s}\,\,\, > \,\,\,0)\,\,.\,and.\,({{\dot m}_a} > \,\,\,0)\,\,.and.\,\,(Schedule\,\, = \,\,\,ON)\,.and.\,\\\,\,({T_{SP}} - T{a_{in}})\,\, > \,\,0.0001)\,\end{array} \right]\,THEN
+\end{equation}
+
+Calculate the heating load on the coil using setpoint and inlet air temperatures.
+
+\begin{equation}
+{Q_{al}}\,\, = \,\,\,{\dot m_a}\, \times \,\,\,C{p_a}\,\, \times \,\,\,\,[\,\,{T_{sp}}\,\, - \,\,\,{T_a}]
+\end{equation}
+
+The logic loop for temperature-controlled coil begins here.~ In case the heating load on the coil is negative, which might occur if the setpoint is below the air inlet temperature, the coil operation needs to be shut off.
+
+\begin{equation}
+IF\,\,({Q_{al}}\,\,\, < \,\,\,\,0.0)\,\,\,\,THEN
+\end{equation}
+
+Assigning the inlet to outlet and mass flows to zero shuts off the coil operation.
+
+\begin{equation}
+{\dot m_s} = 0\,,\,\,\,{\dot m_a} = 0\,,\,\,\,\,\,\,\,\,\,\,\,\,{Q_{al}} = 0,\,\,\,\,\,\,\,\,\,\,\,\,T{w_{out}} = T{s_{in\,\,,\,\,\,\,}}\,\,\,\,\,\,T{a_{out}} = T{a_{in}}
+\end{equation}
+
+If air loop coil load is greater than maximum coil load calculated at maximum steam mass flow rate, in such case the coil is undersized, the coil can only deliver to the air loop its maximum heating capacity.~ Setting the air loop coil load equal to maximum load on coil.~ If this is not the case then the program ignores this ELSE IF block and proceeds to the next one.
+
+\begin{equation}
+ELSE\,\,\,IF\,\,\,\,\left[ {\,\,\,({Q_{al}}\,\, > \,\,{Q_{a{l_{Max}}}})} \right]\,\,\,\,\,\,THEN\,\,\,\,\,\,\left[ {{Q_{al}} = \,\,{Q_{a{l_{Max}}}}} \right]
+\end{equation}
+
+If the heating coil is under sized then it can only provide its maximum heating capacity, in this case the air temperature will be below the setpoint, and is calculated based on this maximum allowed value of heat transfer.~ Calculating the air and water outlet temperatures.
+
+\begin{equation}
+T{a_{out}}\,\,\, = \,\,T{a_{in}}\,\, + \,\,\,\frac{{{Q_{al}}}}{{\,\,{{\dot m}_a}\, \times \,\,\,{c_{p,a}}}}
+\end{equation}
+
+\begin{equation}
+T{w_{out}} = \,\,T{s_{in}}\,\, - \,\,\,\Delta {T_{sc}}
+\end{equation}
+
+Determining the mass flow rate of steam required by the undersized coil.~ This value of mass flow is requested from the splitter outlet.
+
+\begin{equation}
+{\dot m_{al}}\,\,\,\, = \,\,\,\,\,\frac{{{Q_{al}}}}{{{h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}}}}
+\end{equation}
+
+A check is introduced to determine if this requested mass flow rate is greater than what the splitter outlet can provide to the coil at that particular time step of simulation.~ In this case the requested value of steam mass flow is greater that what the splitter can provide to that coil, subsequently set the requested coil flow rate equal to the inlet steam flow rate, delivered to the coil by the splitter.~ This is the maximum amount of steam that can be supplied to the coil at this moment.~ If the requested flow rate is less that what the splitter can provide then the program ignores the logic of the IF Loop.
+
+\begin{equation}
+IF\,\,\,({\dot m_{al}}\,\, > \,\,{\dot m_{in}})\,\,THEN\,\,(\,\,\,{\dot m_{al}}\,\, = \,\,{\dot m_{in}})
+\end{equation}
+
+Re-Calculating the coil heating capacity and air outlet temperature with the lower value of steam mass flow rate provided by the splitter.
+
+\begin{equation}
+{Q_{al}}\,\,\,\, = \,\,\,\,{\dot m_{al}}({h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}})
+\end{equation}
+
+\begin{equation}
+T{a_{out}}\,\,\, = \,\,T{a_{in}}\,\, + \,\,\,\frac{{{Q_{al}}}}{{\,\,{{\dot m}_a}\, \times \,\,\,{c_{p,a}}}}
+\end{equation}
+
+\begin{equation}
+End\,\,\,IF
+\end{equation}
+
+If the above two IF ELSE block are not true, then the coil is perfectly sized, the splitter can provide the required mass flow rate to the coil, and the setpoint temperature can be maintained as desired.
+
+\begin{equation}
+ELSE
+\end{equation}
+
+The ideal case where the coils can meet the required setpoint temperature.~ Setting the outlet air temperature to the setpoint, calculating the water outlet temperature and the required steam mass flow rate.
+
+\begin{equation}
+T{a_{out}}\,\,\, = \,\,{T_{SP}}
+\end{equation}
+
+\begin{equation}
+T{w_{out}} = \,\,T{s_{in}}\,\, - \,\,\,\Delta {T_{sc}}
+\end{equation}
+
+\begin{equation}
+{Q_{al}}\,\, = \,\,\,{\dot m_a}\, \times \,\,\,{c_{p,a}}\,\, \times \,\,\,\,[\,\,{T_{sp}}\,\, - \,\,\,{T_a}]
+\end{equation}
+
+\(END\,\,IF\) ~~ End IF statement, for the air coil heating loop.
+
+\(END\,\,IF\) ~~~~~~~~ End IF statement for the operating condition loop
+
+\(END\,\,IF\) ~~ End IF statement for the Temperature Setpoint Controlled Coil
+
+The steam coil model encapsulates the above described control logic along with the other necessary simulation code for reading the user inputs and the code for reporting the simulation results.
+
+*********************PSEUDO CODE SECTION ENDS**************************
+
+The two main types of coil control discussed above are followed by common simulation code in the coil model.~ This code calculates the loop losses occurring due to flashing of steam across the steam trap, isenthalpic expansion occurring across the steam trap due to pressure difference, and loss occurring due to condensate sub cooling returning back to the boiler.~ The above-mentioned two processes are explained in Figure~\ref{fig:schematic-of-temperature-entropy-diagram-for} as process 3-4' and 4-5.
+
+The loop loss calculation is included in the steam coil simulation model, because the degree of subcooling in the return piping for the condensate is solely a function of the coil location.~ In practical applications a coil, which is further away from boiler would return back condensate at much lower temperatures compared to coil, which is closer to boiler.~ Hence for user ease it makes perfect sense to include this input into the coil and calculate the pump inlet conditions in the steam coil simulation model itself.
+
+The loop losses in the EnergyPlus steam system is calculated by determining the enthalpy difference between point 3 and 5.~ The simulation code that determines the loop loss is common to both the coil models, this helps determine the condensate pump inlet conditions.
+
+The following equation is used to calculate condensate enthalpy at coil outlet, point 3 in Figure~\ref{fig:schematic-of-temperature-entropy-diagram-for}.~ Point 2 represents condensed steam; enthalpy at this point is calculated directly by EnergyPlus property routines.
+
+\begin{equation}
+{h_{f3}} = {h_{f2}} - {c_{p,w}} \times \Delta {T_{SC}}
+\end{equation}
+
+Point 4 is at atmospheric pressure, enthalpy at this is calculated directly by EnergyPlus property routines.~ It is saturation enthalpy of steam at quality equal to 0.0 and saturation temperature at atmospheric pressure.
+
+Point 5 is inlet to the pump; enthalpy at this point is calculated with the following equation~ The delta temperature represents the degree of loop subcooling occurring during condensate return back to the pump.
+
+\begin{equation}
+{h_{f5}} = {h_{f4}} - {c_{p,w}} \times \Delta {T_{LSC}}
+\end{equation}
+
+Subsequently loop loss for each coil would be enthalpy difference between 3 and 5 and is calculated using the following equation
+
+\begin{equation}
+\Delta {Q_{loss}} = {\dot m_s}\,\,\, \times \,\,\,\,({h_{f3}} - {h_{f5}})
+\end{equation}
+
+The total loop loss would be a summation of the individual losses occurring for each of the steam coils, this is the unavoidable loss in current steam system.
+
+A simple schematic describing the coil framework, inlet and outlet conditions to the coil and the flow rate resolution is shown in Figure~\ref{fig:schematic-of-steam-coil-connection-to}.~ Five zone coils and one air loop coil are described in the picture, Qzone is calculated by EnergyPlus heat balance and it is the input to the zone coils, while in air loop coil the Qal is calculated within the simulation model
+
+\begin{figure}[hbtp] % fig 130
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2032.png}
+\caption{Schematic of Steam Coil Connection to the Steam Loop \protect \label{fig:schematic-of-steam-coil-connection-to}}
+\end{figure}
+
+As depicted in the figure above the steam condenses on entering the coils, sub cools by the specified amount and leaves the heat exchanger as water.~ The steam in the heat exchanger at any moment has to condense eventually since steam trap at the outlet to coil permits only water to leave the coil.~ Steam traps being an essential part of the loop are modeled by controlling the coil outlet condition at quality equal to 0.0.~ Subsequently the amount of heat transferred to air is a direct function of latent heat and the degree of sub cooling desired by the user.
+
+\subsubsection{Model Assumptions}\label{model-assumptions-001}
+
+The steam coils works on two basic assumptions, firstly, it's assumed that perfect latent heat transfer takes place over every time step, secondly, the user specified degree of subcooling occurs in the coil.~ Steam coils always use steam traps- purpose of which is to only let water out of the coil, hence the modeler knows with certainty the outlet dryness faction of steam coil is at quality equal to 0.0, because water leaves coil.~ Hence the heat transfer is equal to latent heat of steam, which is independent of UA value of coil when averaged over time step of EnergyPlus simulation.
+
+In practice there is 1\% to 2 \% sub cooling of the outlet water stream, the user with desired degree of subcool input accounts for this, subsequently UA calculation for the coil model become superfluous and is neglected in the EnergyPlus model.
+
+Ideally for sub-cooling UA would play an important role, however sub cooling in steam coil constitutes negligible amount of heat transfer, hence this model avoids the UA calculation.~ This is a very reasonable assumption since sensible heat transfer is barely 1\% to 2 \% of the total heat transfer in steam coils, simply due to large latent heat capacity of coil. NOTE in his thesis he gives a little example here which is probably not necessary for the Docs.
+
+\subsection{Condensate Pump}\label{condensate-pump}
+
+The steam loop operates at a pressure differential over the gaseous and liquid part of the loop; subsequently a condensate pump is required to pump the condensed steam back to the boiler at the required pressure.~ Two main reasons for condensed steam to be returned to the boiler is energy savings in reheating water since the water is at high temperature, secondly the water is treated by chemicals to prevent corrosion in the pipes and equipment.~ This is an expensive process and therefore it's economical to reuse the chemically treated water.
+
+\subsubsection{Description of Pump Model}\label{description-of-pump-model}
+
+The pump model designed in EnergyPlus is a variable speed condensate pump.~ Condensation of steam produces water, this takes place at variable rate hence the return water flow rate would be variable but constant when averaged over a time step.~ Condensate pumps operate intermittently; the pump will run at its capacity if a load/flow rate is sensed and will shut off if there is no load on the loop.
+
+The condensate pump essentially operates between maximum and minimum flow rates, which are the physical limits of the device.~ The pump is designed to meet the flow request made by demand side components, which are the coils in case of steam system.
+
+The main difference between the variable volume pump and the constant volume pump is the Part Load Performance Curve.~ The fraction of full load power is determined by the third order equation, which follows:
+
+\begin{equation}
+{P_{Frac}}\,\, = \,\,{C_1} + \,{C_2} \times PLR\,\, + \,\,\,{C_3} \times PL{R^2}\,\, + \,\,{C_4} \times PL{R^3}
+\end{equation}
+
+In preceding equation, PLR stands for part load ratio while C1 to C4 are pump- part load coefficients.~ The following five equations describe the pump operation and calculation of pump output variables such as total power, shaft power and pump heat to fluid etc.
+
+\begin{equation}
+\dot V\,\, = \,\,\frac{{\,\dot m\,}}{{{\rho_w}}}
+\end{equation}
+
+Using the previous equation the pump volume flow rate is determined; the user enters the value of the maximum and minimum volume flow rate.
+
+The pump part load ratio is a function of the pump volume flow rate at any instance determined by the loop and the pump nominal volume flow rate, which is a user input.~ The following equation calculates the Part Load Ratio (PLR).
+
+\begin{equation}
+PLR = \,\frac{{\dot V}}{{{{\dot V}_{nom}}}}
+\end{equation}
+
+The pump power is calculated as described in following equation.~ Pump power is a product of fractional full load power and pump nominal power use.~ Fractional full load power is calculated in a preceding equation while pump nominal power is a user input to the model.
+
+\begin{equation}
+P = {P_{Frac}} \times {P_{Nom}}
+\end{equation}
+
+The shaft power is simply the product of the pump power and motor efficiency, this is required to calculate the heat generated and delivered to the fluid being pumped.~ The following equation is used to calculate pump shaft power.
+
+\begin{equation}
+{P_S}\,\,\, = P\,\,\,\, \times \,\,\,\,{\eta_m}
+\end{equation}
+
+The model assumes that all heat generated and lost ends up in the fluid to the loop, this assumption is necessary since EnergyPlus operates on a closed loop.~ The following equation is used to calculate the pump heat to the fluid, which raises the condensate temperature.~ The pump motor efficiency is defined by the user input and the fractional motor loss to fluid is the amount of heat generated by the pump motor that is added to the fluid loop (as opposed to being lost to the environment where the pump is located).~ FracMotorLossToFluid is also a user input
+
+\begin{equation}
+{P_H} = {P_S}\,\,\, + \,(\,P\,\, - {P_S}) \times {F_{mf}}
+\end{equation}
+
+The shaft power relates to the increase in head through the pump to the loop operating pressure.~ The head lost through the piping network due to frictional heat, represents the heat gain by the fluid throughout the network.~ .~ For model simplicity, this heat is added along with the heat resulting from the pump motor.~ The difference between the pump power and the shaft power is the inefficiency of the pump, or the amount of energy input into the pump that the motor converts to heat rather than mechanical energy.~ Some of this heat is added to the fluid being pumped.~ These two above-mentioned terms are used in the PumpHeatToFluid equation for calculating P\(_{H}\) shown above.
+
+A simple energy balance over the pump based on the pump inlet conditions and flow rate is used to calculate the pump outlet temperature.~ The condensate outlet temperature from the pump is slightly higher than inlet due to the heat dissipation to the fluid steam during pumping action.~ This is calculated in the following equation.~ The pump water outlet temperature is the boiler inlet temperature.
+
+\begin{equation}
+{T_{{w_{out}}}} = {T_{{w_{in}}}}\,\,\, + \,\,\,\,\,\frac{{{P_H}}}{{\,\dot m\,\,\, \times \,\,\,\,{c_{p,w}}}}
+\end{equation}
+
+Pump control is an important part of the steam loop.~ Existing control structure from EnergyPlus has been utilized to operate the condensate pump.~ The pump is simulated first on the supply side of the loop after the demand side loop has determined what the demand on the loop will be.
+
+A simple schematic describing the flow across the pump is shown in the following figure
+
+\begin{figure}[hbtp] % fig 131
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2040.png}
+\caption{Schematic of Condensate Pump in Steam Loop \protect \label{fig:schematic-of-condensate-pump-in-steam-loop}}
+\end{figure}
+
+\subsubsection{Model Assumptions}\label{model-assumptions-1}
+
+Due to the fact that a pump is a mechanical device that acts on the fluid it is circulating, it causes the fluid temperature rise.~ The EnergyPlus model assumes that all pressure increase caused by the pump will eventually be lost due to friction, and that friction will be added as heat to the fluid.~ Although the plant and condenser loops in steam systems are simple pressure-based models, a simplifying assumption has be made in EnergyPlus to assume the heat resulting from the pump itself and from friction throughout the loop is added at the fluid being pumped.~ In case of steam, this assumption is easily justified because the volume flow rate of water is very small in the loop.
+
+\subsection{Steam Pipe}\label{steam-pipe}
+
+\subsubsection{Description of Model}\label{description-of-model-1}
+
+The steam pipe essentially serves as ``energy carrier'' and transfers the node conditions from one point of the pipe to another.~ It's simply a node inlet to node outlet connection, transferring values from inlet to outlet.~ The pipe forms an important part of the framework connecting various equipments from the supply to demand side and inlet and outlets of the equipments.
+
+The steam pipe supports two additional properties, which are pressure and quality, unlike its water counterpart.~ Pipe simulation model in EnergyPlus is hardwired to water as a fluid type; this necessitated the development of similar model supporting pressure and quality for the steam system.
+
+\subsubsection{Model Assumptions}\label{model-assumptions-2}
+
+The piping network in the developed steam system is assumed to perfectly distribute steam, return the condensate, and remove air and non-condensable gases.~ It is also assumed that the pipes are sized to distribute steam not only at full load but also at partial loads and excess loads that can occur during system warm up.
+
+The steam pipe is perfect and there is no losses occurring in transportation.~ This assumption was necessitated since if pipe losses were accounted for, the loss would have to be distributed into the zone, which would be a very complex issue in itself, since in EnergyPlus the pipes are unaware of their locations and simply serve as connectors.
diff --git a/doc/engineering-reference/src/building-system-simulation-system-manager/zone-equipment-simulation.tex b/doc/engineering-reference/src/building-system-simulation-system-manager/zone-equipment-simulation.tex
new file mode 100644
index 00000000000..49fb64e6376
--- /dev/null
+++ b/doc/engineering-reference/src/building-system-simulation-system-manager/zone-equipment-simulation.tex
@@ -0,0 +1,213 @@
+\section{Zone Equipment Simulation}\label{zone-equipment-simulation}
+
+When the EnergyPlus HVAC simulation manager needs to simulate the zone equipment side of the air loop it calls \emph{ManageZoneEquipment}, the zone equipment simulation manager subroutine. Like the other managers, \emph{ManageZoneEquipment} has a very simple structure:
+
+\begin{lstlisting}
+        IF (GetInputFlag) THEN
+          CALL GetZoneEquipment
+          GetInputFlag = .FALSE.
+        END IF
+\end{lstlisting}
+
+\begin{lstlisting}
+        CALL InitZoneEquipment(FirstHVACIteration)
+\end{lstlisting}
+
+\begin{lstlisting}
+        IF (ZoneSizingCalc) THEN
+          CALL SizeZoneEquipment
+        ELSE
+          CALL SimZoneEquipment(FirstHVACIteration, SimAir)
+        END IF
+\end{lstlisting}
+
+\begin{lstlisting}
+        CALL RecordZoneEquipment(SimAir)
+\end{lstlisting}
+
+\begin{lstlisting}
+        CALL ReportZoneEquipment
+\end{lstlisting}
+
+\begin{lstlisting}
+        SimZone = .False.
+\end{lstlisting}
+
+\begin{lstlisting}
+        RETURN
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  If the user input data has not been input, get the data and store it in the zone equipment data structures
+\item
+  Perform zone equipment initialization calculations.
+\item
+  If calculation of the design zone air flow rates and loads needs to be done, do it. The results of this calculation are stored in the zone sizing data structures and used by the component automatic sizing algorithms and the central system sizing calculations.
+\item
+  Otherwise simulate all of the zone equipment.
+\item
+  Transfer the zone equipment outlet node data to the inlet nodes of the primary air systems and check for convergence (done in RecordZoneEquipment by calling UpdateHVACInterface).
+\end{enumerate}
+
+\subsection{Input data}\label{input-data-000}
+
+The input specifying a set of zone equipment consists of:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\tightlist
+\item
+  the ZoneHVAC:EquipmentConnections object data;
+\end{enumerate}
+
+\begin{lstlisting}
+a.  the zone connection to the air loop – air inlet nodes, exhaust nodes, outlet node, zone node;
+\end{lstlisting}
+
+\begin{lstlisting}
+b.  the components serving each zone – air terminal units, fan coils etc.;
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  zone supply air path data;
+\end{enumerate}
+
+\begin{lstlisting}
+a.  zone splitters and supply plenums;
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  zone return air path data;
+\end{enumerate}
+
+\begin{lstlisting}
+a.  zone mixer and return plenums;
+\end{lstlisting}
+
+\subsection{Initialization Calculations}\label{initialization-calculations-000}
+
+\subsubsection{One Time Calculations}\label{one-time-calculations-000}
+
+There are no one time calculations for zone equipment
+
+\subsubsection{Begin Environment Initializations}\label{begin-environment-initializations-000}
+
+For each controlled zone initialize the zone inlet, exhaust and zone nodes to standard conditions. Namely:
+
+\begin{equation}
+{T_{node}} = {20^{\rm{o}}}C
+\end{equation}
+
+\begin{equation}
+{W_{node}} = {W_{oa}}
+\end{equation}
+
+\begin{equation}
+{h_{node}} = {\mathop{\rm PsyHFnTdbW}\nolimits} {\rm{(}}20.0,{W_{oa}}{\rm{)}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{node}} = 0
+\end{equation}
+
+\begin{equation}
+Q{u_{node}} = 1.0
+\end{equation}
+
+\begin{equation}
+{p_{node}} = {p_{oa}}
+\end{equation}
+
+where \emph{W\(_{oa}\)} is the humidity of the outside air; \({\rm{PsyHFnTdbW}}\) is the EnergyPlus psychrometric function for enthalpy \emph{h}, given temperature and humidity ratio; \emph{p\(_{oa}\)} is the pressure of the outside air; and \emph{Qu} is quality.
+
+\subsubsection{System Time Step Initializations}\label{system-time-step-initializations-000}
+
+For each controlled zone, set the exhaust nodes conditions equal to the zone node conditions; except set the exhaust nodes mass flow rate and min and max available mass flow rates to zero.
+
+\subsection{Simulation}\label{simulation-003}
+
+The subroutine \emph{SimZoneEquipment} does the actual simulation of all the zone equipment. Note that this includes components that are part of the demand side of an air loop as well as components that are independent of any air loop.
+
+For zone equipment components that are part of the demand side of an air loop the simulation sequence is effectively performed in the direction of the air flow. First the supply air plenums and zone splitters are simulated in their input order. Then the air terminal units are simulated followed by the zone return plenums and zone mixer. Each air terminal unit sets its inlet node to the air mass flow rate required to satisfy its zone load. These mass flow rates are then passed back upstream to the air loop demand-side inlet nodes at the end of each zone equipment simulation sequence. These demand-side inlet mass flow rates are then used as mass flow rate setpoints in the air loop supply-side simulation.
+
+If multiple air-conditioning components are attached to a zone, the components are simulated in the order specified by the user assigned priority given in the ZoneHVAC:EquipmentList object.
+
+For each full air loop there should be 1 supply air path for each primary air system outlet (i.e.~1 for single duct systems,~ 2 for dual duct systems). For each full air loop there should be one return air path. The supply air paths consist of any combination of zone splitters and zone supply air plenums as long as it forms a tree structure with the supply air path inlet node the root and the air terminal unit inlet nodes as the leaves. The return air path configuration is limited to a single mixer; there may be multiple return plenums.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\tightlist
+\item
+  Loop over all the supply air paths.
+\end{enumerate}
+
+\begin{lstlisting}
+a.  Loop over each component (supply plenum or zone splitter) on the supply air path and simulate each component. The components are simulated in input order.
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Loop over all the controlled zones.
+\end{enumerate}
+
+\begin{lstlisting}
+a.  Set the required system output.
+\end{lstlisting}
+
+\begin{lstlisting}
+b.  Loop over the components serving the zone in the user prioritized order.
+\end{lstlisting}
+
+\begin{lstlisting}
+    i.  Simulate each component.
+\end{lstlisting}
+
+\begin{lstlisting}
+    ii. Increment the required system output.
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Loop over all the supply air paths
+\end{enumerate}
+
+\begin{lstlisting}
+a.  Loop over the components on each supply air path in reverse input order. This reverse order simulation passes the air terminal units inlet mass flows back upstream to the return air path inlet node.
+\end{lstlisting}
+
+\begin{lstlisting}
+b.  Check to see if the supply air path inlet node mass flow rate has changed. If it has set the *SimAir* flag to *true*. This signals the HVAC manager that the supply-side of the air loop needs to be resimulated.
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{3}
+\item
+  Calculate the zone air flow mass balance -- the zone inlet and exhaust mass flow rates are summed and the zone node and return air node mass flow rates are determined by a mass balance for each zone.
+\item
+  Calculate the conditions at each zone return air node. Here energy not included in the zone energy balance such as light-heat-to-return-air is added to the return nodes of the controlled zones.
+\item
+  Loop over all of the return air paths.
+\end{enumerate}
+
+\begin{lstlisting}
+a.  Loop over each component (return plenum or zone mixer) on the return air path and simulate each component.
+\end{lstlisting}
+
+This completes a single simulation sequence of all the zone equipment.
diff --git a/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations.tex b/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations.tex
new file mode 100644
index 00000000000..94dab4b5bc0
--- /dev/null
+++ b/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations.tex
@@ -0,0 +1 @@
+\chapter{Climate, Sky and Solar/Shading Calculations}\label{climate-sky-and-solarshading-calculations}
diff --git a/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/climate-calculations.tex b/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/climate-calculations.tex
new file mode 100644
index 00000000000..954ee9150ca
--- /dev/null
+++ b/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/climate-calculations.tex
@@ -0,0 +1,260 @@
+\section{Climate Calculations}\label{climate-calculations}
+
+The location of the facility under analysis is critical for the determination of energy consumption, heating/cooling loads, daylighting potential, and a host of other calculations. In EnergyPlus, both external (i.e, weather files supplied from others) and internal (i.e., solar position, design day temperature/humidity/solar profiles) data is used during simulations.
+
+The ``Site:Location'' input object includes parameters (Latitude, Longitude, Elevation, Timezone) that allow EnergyPlus to calculate the solar position (using Latitude, Longitude and Timezone) for any day of the year as well as supply the standard barometric pressure (using elevation). Solar position modeling is discussed in more detail in both the Sky Radiance and Shading Calculation sections that directly follow this section.
+
+Weather files have hourly or sub-hourly data for each of the critical elements needed during the calculations (i.e., Dry-Bulb Temperature, Dew-Point Temperature, Relative Humidity, Barometric Pressure, Direct Normal Radiation, Diffuse Horizontal Radiation, Total \& Opaque Sky Cover, Wind Direction, Wind Speed) as well as some auxiliary data such as Rain or Snow that assist in certain calculational aspects. Weather file excerpts such as might be used in sizing calculations also have this breadth of data. The input object ``SizingPeriod:DesignDay'' describes design days (meant to mimic ASHRAE design conditions but in a whole day profile) using certain characteristics for the day and then EnergyPlus supplies the remaining portions to complete outdoor conditions needed for program execution. SizingPeriod:DesignDay are perhaps the best objects for sizing equipment as the ASHRAE specified design conditions can be input AND weather files may or may not have the conditions necessary to size equipment properly.
+
+Two other objects, however, can be used at times: SizingPeriod:WeatherFileDays and SizingPeriod:WeatherFileConditionType.~ With the first of these, one specifies a set of weather file days similar to a RunPeriod (but will be used for the Sizing calculations). In the second, the extreme or typical conditions that are calculated for the weather file during processing can be used by name.~ Of course, either of these can be used as a measure of usage over small periods.
+
+The ASHRAE Handbook of Fundamentals describes their criteria in creating design condition synopses. ``Design data based on dry-bulb temperature represent peak occurrences of the sensible component of ambient outdoor conditions. Design values based on wet-bulb temperature are related to the enthalpy of the outdoor air. Conditions based on dewpoint relate to the peaks of the humidity ratio. The designer, engineer, or other user must decide which set(s) of conditions and probability of occurrence apply to the design situation under consideration.''
+
+\subsection{EnergyPlus Design Day Temperature Calculations}\label{energyplus-design-day-temperature-calculations}
+
+In EnergyPlus, the typical design day input includes a ``high'' and a ``low'' dry-bulb temperature for the day. As these two temperatures are insufficient to represent a full 24 hour period, the program uses a ``range multiplier'' profile to represent the full day's temperatures:
+
+\begin{figure}[hbtp] % fig 36
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image563.svg.png}
+\caption{Default Daily Temperature Range Profile \protect \label{fig:default-daily-temperature-range-profile}}
+\end{figure}
+
+The multipliers are taken from the ASHRAE 2009 HOF, Table \# 6, p.~14.11.. More explicitly, EnergyPlus creates an air temperature for each timestep by using the entered maximum dry-bulb temperature in conjunction with the entered daily range and the above multiplier values. The actual equation used is shown below:
+
+\begin{equation}
+{T_{current}} = {T_{Max}} - {T_{range}}\cdot {T_{Multiplier}}
+\end{equation}
+
+where
+
+T\(_{current}\) = Air temperature of current Hour of Day
+
+T\(_{Max}\) = User supplied Max Dry-bulb Temperature
+
+T\(_{range}\) = User supplied Daily Temperature Range
+
+T\(_{Multiplier}\) = Range multiplier as shown on the above graph
+
+The range multiplier values represent typical conditions of diurnal temperatures (i.e.~the low temperature for the day occurring about 5:00 AM and the maximum temperature for the day occurring about 3:00 PM.~ Note that EnergyPlus does not shift the profile based on the time of solar noon as is optionally allowed by ASHRAE procedures.
+
+ASHRAE research indicates that dry-bulb and wet-bulb temperatures typically follow the same profile, so EnergyPlus can use the default daily temperature profile to generate humidity conditions based on maximum and range of wet-bulb temperature.
+
+Since this default temperature profile may not be applicable to all locations, the user can give a different profile as part of the design day definition.
+
+\subsection{Sky Radiation Modeling}\label{sky-radiation-modeling}
+
+EnergyPlus calculates the Horizontal Infrared Radiation Intensity in Wh/m\(^{2,}\) if it is missing on the weather file or for design days, from the Opaque Sky Cover field as shown in the following explanation.
+
+\begin{equation}
+Horizontal_IR = Sk{y_{emissivity}}\cdot Sigma\cdot Temperature_{drybulb}^4
+\end{equation}
+
+where
+
+Horizontal\_IR = horizontal IR intensity \{W/m\(^{2}\)\}
+
+Sky\(_{emissivity}\) = sky emissivity
+
+Sigma = Stefan-Boltzmann constant = 5.6697e-8 \{W/m\(^{2}\)-K\(^{4}\)\}
+
+Temperature\(_{drybulb}\) = drybulb temperature \{K\}
+
+The sky emissivity is given by
+
+\begin{equation}
+Sk{y_{emissivity}} = \left( {.787 + .764\cdot \ln \left( {\frac{{Temperatur{e_{dewpoint}}}}{{273.}}} \right)} \right)\cdot \left( {1. + .0224N - .0035{N^2} + .00028{N^3}} \right)
+\end{equation}
+
+where
+
+Temperature\(_{dewpoint}\) = dewpoint temperature \{K\}
+
+N = opaque sky cover \{tenths\}
+
+Example: Clear sky (N = 0), Temperature\(_{drybulb}\) = 273+20 = 293 K, Temperature\(_{dewpoint}\) = 273+10 = 283 K:
+
+Sky\(_{emissivity}\) = 0.787 + 0.764*0.036 = 0.815
+
+Horizontal\_IR = 0.815*5.6697e-8*(293**4) = 340.6 W/m\(^{2}\)
+
+References for these calculations are contained in the references section at the end of this list of fields. (Walton, 1983) (Clark and Allen, 1978).
+
+\subsection{EnergyPlus Sky Temperature Calculation}\label{energyplus-sky-temperature-calculation}
+
+The default calculation for sky temperature is:
+
+\begin{equation}
+Sk{y_{Temperature}} = {\left( {\frac{{Horizontal_IR}}{{Sigma}}} \right)^{.25}} - Temperatur{e_{Kelvin}}
+\end{equation}
+
+Where
+
+Sky\(_{Temperature}\) = Sky radiative temperature \{C\}
+
+Horiizontal\_IR = Horizontal Infrared Radiation Intensity as described in the previous section \{Wh/m\(^{2}\)\}
+
+Temperature\(_{Kelvin}\) = Temperature conversion from Kelvin to C, i.e.~273.15
+
+The Sky Temperature can also be set by the user from several options using the \textbf{WeatherProperty:SkyTemperature} object.
+
+\subsection{EnergyPlus Design Day Solar Radiation Calculations}\label{energyplus-design-day-solar-radiation-calculations}
+
+Similarly, calculating solar irradiance (solar modeling) is one of the important effects to be accomplished. Several solar models exist with varying complexity.
+
+\subsubsection{ASHRAE Clear Sky Solar Model}\label{ashrae-clear-sky-solar-model}
+
+The default model used is the ASHRAE Clear Sky model. The ASHRAE clear sky model described in ASHRAE HOF 2005 Chapter 31 can be used to estimate hourly clear-day solar radiation for any month of the year in U.S. or similar temperate climates in the northern hemisphere. EnergyPlus calculations extend the clear sky application to both northern and southern hemispheres.~ Note that the Clear Sky model has been updated in the ASHRAE HOF 2009 (see ASHRAE Revised Clear Sky Model below).
+
+At the earth's surface on a clear day, direct normal irradiation is represented by
+
+\begin{equation}
+Direct\;Normal\;Irradiation = \frac{A}{exp\left( \frac{B}{\sin \beta } \right)}
+\end{equation}
+
+where
+
+\emph{A} = apparent solar irradiation at air mass m = 0 (Table~\ref{table:extraterrestrial-solar-irradiance-and-related})
+
+B = atmospheric extinction coefficient Table~\ref{table:extraterrestrial-solar-irradiance-and-related})
+
+Values of A and B vary during the year because of seasonal changes in the dust and water vapor content of the atmosphere and because of the changing earth-sun distance. Equation does not give the maximum value of direct normal irradiation that can occur in each month but yields values that are representative of conditions on cloudless days for a relatively dry and clear atmosphere. For very clear atmospheres, direct normal irradiation can be 15\% higher than indicated by Equation , using values of A and B in Table~\ref{table:extraterrestrial-solar-irradiance-and-related} below.
+
+% table 20
+\begin{longtable}[c]{p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}}
+\caption{Extraterrestrial Solar Irradiance and Related Data Note: Data are for 21st day of each month during the base year of 1964. \label{table:extraterrestrial-solar-irradiance-and-related}}\\
+\toprule 
+~ & I\(_{o}\)\{W/m\(^{2}\)\} & Equation of Time \{minutes\} & Declination \{degrees\} & A \{W/m\(^{2}\)\} & B \{\} & C \{\} \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Extraterrestrial Solar Irradiance and Related Data Note: Data are for 21st day of each month during the base year of 1964.} \tabularnewline
+\toprule 
+~ & I\(_{o}\)\{W/m\(^{2}\)\} & Equation of Time \{minutes\} & Declination \{degrees\} & A \{W/m\(^{2}\)\} & B \{\} & C \{\} \tabularnewline
+\midrule
+\endhead
+
+Jan & 1416 & -11.2 & -20.0 & 1202 & 0.141 & 0.103 \tabularnewline
+Feb & 1401 & -13.9 & -10.8 & 1187 & 0.142 & 0.104 \tabularnewline
+Mar & 1381 & -7.5 & 0.0 & 1164 & 0.149 & 0.109 \tabularnewline
+Apr & 1356 & 1.1 & 11.6 & 1130 & 0.164 & 0.120 \tabularnewline
+May & 1336 & 3.3 & 20.0 & 1106 & 0.177 & 0.130 \tabularnewline
+Jun & 1336 & -1.4 & 23.45 & 1092 & 0.185 & 0.137 \tabularnewline
+Jul & 1336 & -6.2 & 20.6 & 1093 & 0.186 & 0.138 \tabularnewline
+Aug & 1338 & -2.4 & 12.3 & 1107 & 0.182 & 0.134 \tabularnewline
+Sep & 1359 & 7.5 & 0.0 & 1136 & 0.165 & 0.121 \tabularnewline
+Oct & 1380 & 15.4 & -10.5 & 1166 & 0.152 & 0.111 \tabularnewline
+Nov & 1405 & 13.8 & -19.8 & 1190 & 0.144 & 0.106 \tabularnewline
+Dec & 1417 & 1.6 & -23.45 & 1204 & 0.141 & 0.103 \tabularnewline
+\bottomrule
+\end{longtable}
+
+For locations where clear, dry skies predominate (e.g., at high elevations) or, conversely, where hazy and humid conditions are frequent, values found by using Equation and Table~\ref{table:extraterrestrial-solar-irradiance-and-related} should be multiplied by the clearness numbers in Threlkeld and Jordan (1958), reproduced as Figure \# 5 in Chapter 33 of the 2007 ASHRAE Handbook---HVAC Applications.
+
+The Clear Sky model usually over estimates the amount of solar radiation available to the building.
+
+\subsubsection{\texorpdfstring{ASHRAE Revised Clear Sky Model (``Tau Model'')}{ASHRAE Revised Clear Sky Model (Tau Model)}}\label{ashrae-revised-clear-sky-model-tau-model}
+
+The ASHRAE 2009 HOF introduced a revised clear sky model based on location-specific optical depths for direct and diffuse radiation.~ These values are tabulated by month for all 5564 locations in the ASHRAE design data that accompanies the 2009 HOF.
+
+The model requires air mass, m, calculated as follows --
+
+\begin{equation}
+m = {1 \mathord{\left/ {\vphantom {1 {\left[ {\sin \beta  + 0.50572 \cdot {{\left( {6.07995 + \beta } \right)}^{ - 1.6364}}} \right]}}} \right. } {\left[ {\sin \beta  + 0.50572 \cdot {{\left( {6.07995 + \beta } \right)}^{ - 1.6364}}} \right]}}
+\end{equation}
+
+where \(\beta\) ~ = solar altitude, degrees.
+
+Direct and diffuse irradiance are determined with the following relationships,
+
+\begin{equation}
+{E_b} = {E_o} \cdot \exp \left[ { - {\tau_b} \cdot {m^{ab}}} \right]
+\end{equation}
+
+\begin{equation}
+{E_d} = {E_o} \cdot \exp \left[ { - {\tau_d} \cdot {m^{ad}}} \right]
+\end{equation}
+
+where:
+
+\({E_b}\) ~ = beam normal irradiance, W/m\(^{2}\)
+
+\({E_d}\) ~ = diffuse horizontal irradiance,
+
+\({E_o}\) ~ = extraterrestrial normal irradiance,
+
+\emph{\(m\)}~ = air mass
+
+$\tau$\(_{b}\) and $\tau$\(_{d}\) = beam and diffuse optical depths (from ASHRAE climatic design data)
+
+\(ab\) ~and \(ad\) ~ = beam and diffuse air mass exponents (see below)
+
+Values of $\tau$\(_{b}\) and $\tau$\(_{d}\) are location-specific and vary during the year. They embody the dependence of clear sky solar radiation upon local conditions, such as elevation, precipitable water content, and aerosols.
+
+The air mass exponents \(ab\) ~and \(ad\) ~were correlated to $\tau$\(_{b}\) and $\tau$\(_{d}\) through the following empirical relationships:
+
+\begin{equation}
+ab = 1.219 - 0.043 \cdot {\tau_b} - 0.151 \cdot {\tau_d} - 0.204 \cdot {\tau_b} \cdot {\tau_d}
+\end{equation}
+
+\begin{equation}
+ad = 0.202 + 0.852 \cdot {\tau_b} - 0.007 \cdot {\tau_d} - 0.357 \cdot {\tau_b} \cdot {\tau_d}
+\end{equation}
+
+Studies done as part of ASHRAE research projects show that the revised tau model produces more physically plausible irradiance values than does the traditional clear sky model.~ In particular, diffuse irradiance values are more realistic.
+
+\subsubsection{Zhang-Huang Solar Model}\label{zhang-huang-solar-model}
+
+The Zhang-Huang solar model was developed for initial use in modeling typical meteorological years for China weather sites. This model seems to be good for other locations as well. Using total cloud cover, dry-bulb temperature, relative humidity, and wind speed as the independent variables, the total (global horizontal) solar radiation is estimated by:
+
+\begin{equation}
+I = \frac{{\left[ {{I_0}\cdot \sin (h)\cdot \left( {{c_0} + {c_1}\cdot CC + {c_2}\cdot C{C^2} + {c_3}\left( {{T_n} - {T_{n - 3}}} \right) + {c_4}\cdot \varphi  + {c_5}\cdot {V_w}} \right) + d} \right]}}{k}
+\end{equation}
+
+Where
+
+I = estimated hourly solar radiation, W/m\(^{2}\)
+
+I\(_{0}\) = global solar constant, 1355 W/m\(^{2}\)
+
+h = solar altitude angle, i.e, the angle between the horizontal and the line to the sun
+
+CC = cloud cover
+
+\(\varphi\) ~ = relative humidity, \%
+
+\({T_n},{T_{n - 3}}\) ~ = dry-bulb temperature at hours n (current) and n-3, respectively
+
+\({V_w}\) ~ = Wind speed, m/s
+
+\({c_0},{c_1},{c_2},{c_3},{c_4},{c_5},d,k\) ~ = regression coefficients
+
+The constants were determined by analysis from measured data and are as follows:
+
+c\(_{0}\) = .5598, c\(_{1}\) = .4982, c\(_{2}\) = -.6762, c\(_{3}\) = .02842, c\(_{4}\) = -.00317, c\(_{5}\) = .014, d = -17.853, k = .843.
+
+This is the same model used to estimate the global solar radiation value (when it is absent from the source data) in the Weather Converter. References given in the reference section (Watanabe, Urano, Hayashi, 1983) (Zhang, Huang, 2002).
+
+\subsection{Perez Direct/Diffuse Splitting Model}\label{perez-directdiffuse-splitting-model}
+
+Splitting from global calculated (EnergyPlus) or entered values (WeatherConverter) into direct normal and diffuse horizontal components are done using the Perez direct/diffuse split. References shown in the reference section (Perez et al, 1992) (Perez et al, 1990)
+
+\subsection{Weather File Solar Interpolation}\label{weather-file-solar-interpolation}
+
+The solar values on the weather file are average values over the hour. For interpolation of hourly weather data (i.e., when the specified timestep is greater than 1), the average value is assumed to be the value at the midpoint of the hour.~ The reported values in the output are totals for each reporting period. So, hourly reported values will not match the original values in the weather file, but the total solar for a day should agree. Reference (Ellis, Liesen, Pedersen, 2003)
+
+\subsection{References}\label{references-010}
+
+Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards, p.~21.
+
+Clark, G. and C. Allen, ``The Estimation of Atmospheric Radiation for Clear and Cloudy Skies,'' Proceedings 2nd National Passive Solar Conference (AS/ISES), 1978, pp.~675-678.
+
+Watanabe, T., Urano, Y., and Hayashi, T. 1983. ``Procedures for Separating Direct and Diffuse Insolation on a Horizontal Surface and Prediction of Insolation on Tilted Surfaces'' (in Japanese), Transactions, No. 330, Architectural Institute of Japan, Tokyo, Japan.
+
+Zhang, Q.Y. and Huang, Y.J. 2002. Development of typical year weather files for Chinese locations, LBNL-51436, ASHRAE Transactions, Vol. 108, Part 2.
+
+Perez R., Ineichen P., Maxwell E., Seals, R. and Zelenka, A. 1992. Dynamic Global-to-Direct Irradiance Conversion Models. ASHRAE Transactions-Research Series,354-369.
+
+Perez, R., Ineichen, P., Seals, R., Michalsky, J. and Stewart, R. 1990. Modeling daylight availability and irradiance components from direct and global irradiance. Solar Energy 44, 271-289.
+
+Ellis, P.G., Liesen, R.J. and Pedersen, C.O. 2003. ``Energyplus Experimental Data Validation Work: Development and Validation of the Unvented Trombe Wall Model and Other Heat Balance Components'', CERL Final Report DACA42-01-D-0004, Task 3.
diff --git a/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/design-week-specification.tex b/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/design-week-specification.tex
new file mode 100644
index 00000000000..81c4188d5a5
--- /dev/null
+++ b/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/design-week-specification.tex
@@ -0,0 +1,5 @@
+\section{Design Week Specification}\label{design-week-specification}
+
+A design week (or longer) may be specified in EnergyPlus by selecting a RunPeriod of one week.~ One-week custom weather files may be constructed if extreme design week conditions are desired or one can use the specific dates from the EPW weather files that designate the extreme conditions on the weather file.~ The design week simulation requires that the simulation reach a `steady-periodic' state for the one week time period.~ This is achieved manually by increasing the `number of years of simulation' until the weekly profile does not change from one year to the next.~ The `steady-periodic' output for the last week of the simulation represents the design week simulation results.
+
+Using the SizingPeriod:WeatherFileDays object, one could size equipment from a longer period.
diff --git a/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/shading-module.tex b/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/shading-module.tex
new file mode 100644
index 00000000000..490acc584d8
--- /dev/null
+++ b/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/shading-module.tex
@@ -0,0 +1,754 @@
+\section{Shading Module}\label{shading-module}
+
+\subsection{Shading and Sunlit Area Calculations}\label{shading-and-sunlit-area-calculations}
+
+When assessing heat gains in buildings due to solar radiation, it is necessary to know how much of each part of the building is shaded and how much is in direct sunlight. As an example, the figure below shows a flat roofed, L-shaped structure with a window in each of the visible sides. The sun is to the right so that walls 1 and 3 and windows a and c are completely shaded, and wall 4 and window d are completely sunlit. Wall 2 and window b are partially shaded. The sunlit area of each surface changes as the position of the sun changes during the day. The purpose of the EnergyPlus shadow algorithm is to compute these \textbf{sunlit areas}.~ Predecessors to the EnergyPlus shadowing concepts include the BLAST and TARP shadowing algorithms.
+
+The shadow algorithm is based on coordinate transformation methods similar to Groth and Lokmanhekim and the shadow overlap method of Walton.
+
+Using the \textbf{ShadowCalculation} object, you can set how often the shadowing calculations are performed. Having them calculated each day is obviously the most accurate but may also be the most time consuming.~ Using a greater length of time (number of days) before calculating again can yield speedier results.~ For lengths of time greater than one day, the solar position values (e.g.~equation of time, sun position angles) are averaged over that time period for the shadowing calculations.
+
+\begin{figure}[hbtp] % fig 38
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image601.png}
+\caption{Overall Shadowing Scheme Depiction \protect \label{fig:overall-shadowing-scheme-depiction}}
+\end{figure}
+
+\subsection{Solar Position}\label{solar-position}
+
+Current solar position is described in terms of three direction cosines that are convenient for determining the angle of incidence of the sun's rays on a building surface.~ The following procedure is used to determine the direction cosines.~ The values of the solar declination angle, $\delta$, and the equation of time, $\varepsilon$, are based on \emph{Astronomical Algorithms}, Meeus.~ Solar declination is a function of local/site latitude.
+
+The fractional year is calculated, in radians:
+
+\begin{equation}
+\gamma  = \frac{{2\pi }}{{366}}(day_of_year)
+\end{equation}
+
+From this fractional year, the equation of time and solar declination angle are calculated.~ For each time step (time value = fractional hour), the hour angle is calculated from:
+
+\begin{equation}
+HourAngle = \left( {15\cdot \left( {12 - \left( {TimeValue + EquationOfTime} \right)} \right) + \left( {TimeZoneMeridian - Longitude} \right)} \right)
+\end{equation}
+
+TimeZoneMeridian is the standard meridian for the location's time zone \{GMT +/-\}.
+
+Solar HourAngle (\emph{H}) gives the apparent solar time for the current time period (degrees); HourAngle is positive before noon, negative after noon.~ It is common astronomical practice to express the hour angle in hours, minutes and seconds of time rather than in degrees.~ You can convert the hour angle displayed from EnergyPlus to time by dividing by 15.~ (Note that 1 hour is equivalent to 15 degrees; 360° of the Earth's rotation takes place every 24 hours.)~ The relationship of angles in degrees to time is shown in the following table:
+
+% table 23
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Relationship of Angles (degrees) to Time \label{table:relationship-of-angles-degrees-to-time}} \tabularnewline
+\toprule 
+Unit of Angle & Equivalent time \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Relationship of Angles (degrees) to Time} \tabularnewline
+\toprule 
+Unit of Angle & Equivalent time \tabularnewline
+\midrule
+\endhead
+
+1 radian & 3.819719 hours \tabularnewline
+1 degree & 4 minutes \tabularnewline
+1 arcmin & 4 seconds \tabularnewline
+1 arcsec & 0.066667 seconds \tabularnewline
+\bottomrule
+\end{longtable}
+
+The Solar Altitude Angle ($\beta$) is the angle of the sun above the horizontal (degrees). The Solar Azimuth Angle ($\phi$) is measured from the North (clockwise) and is expressed in degrees.~ This is shown more clearly in the following figure.
+
+\begin{figure}[hbtp] % fig 39
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image604.png}
+\caption{Solar Position Illustration \protect \label{fig:solar-position-illustration}}
+\end{figure}
+
+\subsection{Surface Geometry}\label{surface-geometry}
+
+Shadow calculations first require that the building surfaces be described geometrically. Surfaces are described by the coordinates of their vertices in a three dimensional Cartesian coordinate system. This Right-hand coordinate system has the X-axis pointing east, the Y-axis pointing north, and the Z-axis pointing up (see figure below). The azimuth angle ($\psi$) of a surface is the angle from the north axis to the projection onto the X-Y plane of a normal to the surface (clockwise positive). The surface tilt angle ($\phi$) is the angle between the Z-axis and the normal to the surface. The vertices are recorded in counter-clockwise sequence (as the surface is viewed from outside its zone).
+
+During surface entry, surfaces are checked for convex or non-convex shape. If non-convex and inappropriate (used as a receiving surface) then a severe error is produced telling the user that shadowing calculations may be inaccurate.
+
+Similarly collinear points (or as noted below, points within 1 mm distance) are removed unless removing would make an illegal surface (less than 3 points). But degenerate collinear surfaces \emph{should} be removed -- they make the shadowing routines do extra work which takes extra time.
+
+Collinear -- points that essentially form a ``line'' rather than a surface shape.
+
+Resolution of 1mm or less -- near collinear points.
+
+Note that the resolution on surfaces/shadowing is 1 mm -- using resolution beyond that will result in truncation of the shadowing.
+
+\begin{figure}[hbtp] % fig 40
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image605.png}
+\caption{EnergyPlus Coordinate System \protect \label{fig:energyplus-coordinate-system}}
+\end{figure}
+
+The GlobalGeometryRules object specifies to EnergyPlus how the surface vertices will be presented in the input file.~ Of pertinent interest here is that the user may specify the vertices in either ``relative'' or ``world'' coordinates.~ Regardless of input specifications, when vertices are reported, they are reported in world coordinates, starting at the upper-left-corner (4-sided surface) and are listed counter-clockwise.
+
+\subsubsection{Relative Coordinate Transformation}\label{relative-coordinate-transformation}
+
+When vertices are specified in ``relative'' coordinates, there can be a ``building'' north axis as well as a ``zone'' north axis.~ The building north axis/coordinate system is a rotation of y\(_{b}\) degrees from the global/world coordinate system.~ The global coordinates of zone origins are related to the building relative coordinates by:
+
+\begin{equation}
+{X_{zo}} = {X_{br}}\cdot \cos {\psi_b} - {Y_{br}}\cdot \sin {\psi_b}
+\end{equation}
+
+\begin{equation}
+{Y_{zo}} = {Y_{br}}\cdot \sin {\psi_b} - {Y_{br}}\cdot \cos {\psi_b}
+\end{equation}
+
+\begin{equation}
+{Z_{zo}} = {Z_{br}}
+\end{equation}
+
+Where
+
+zo -- represents Zone Origin
+
+br -- represents the Zone Origin as input (relative to building origin)
+
+The zone may also be rotated $\psi$\(_{z}\) degrees relative to the building coordinates. Origins of zone surfaces are then given relative to the zone coordinate system. The global coordinates of the surface origins are calculated by:
+
+\begin{equation}
+{X_{so}} = {X_{zo}} + {X_{zr}}\cdot \cos {\psi_z} - {Y_{zr}}\cdot \sin {\psi_z}
+\end{equation}
+
+\begin{equation}
+{Y_{so}} = {Y_{zo}} + {X_{zr}}\cdot \sin {\psi_z} - {Y_{zr}}\cdot \cos {\psi_z}
+\end{equation}
+
+\begin{equation}
+{X_{so}} = {X_{zo}} + {X_{zr}}\cdot \cos {\psi_z} - {Y_{zr}}\cdot \sin {\psi_z}
+\end{equation}
+
+A surface azimuth angle relative to the zone coordinate system ($\psi$\(_{s}\)) is converted to a global azimuth by:
+
+\begin{equation}
+\psi  = {\psi_s} + {\psi_z} + {\psi_b}
+\end{equation}
+
+The surface tilt angle ($\phi$) is not changed by these rotations about the Z-axis.
+
+The coordinates of the surface vertices are given in a coordinate system in the plane of the surface relative to the second vertex as shown for surfaces in Figure~\ref{fig:energyplus-coordinate-system}. The X-axis of the surface coordinate system is a horizontal line through the second vertex. The global coordinates of the surface vertices are given by:
+
+\begin{equation}
+X = {X_{so}} + {X_{sr}}\cdot \cos \psi  - {Y_{sr}}\cdot \sin \psi \cdot \cos \phi
+\end{equation}
+
+\begin{equation}
+Y = {Y_{so}} + {X_{sr}}\cdot \sin \psi  - {Y_{sr}}\cdot \cos \psi \cdot \cos \phi
+\end{equation}
+
+\begin{equation}
+Z = {Z_{so}} + {Y_{sr}}\cdot \sin \phi
+\end{equation}
+
+\subsubsection{World Coordinates è Relative Coordinates}\label{world-coordinates-uxe8-relative-coordinates}
+
+Vertices in the global coordinate system can be transformed to the coordinate system relative to a given surface by
+
+\begin{equation}
+{X'} = X - {X_{so}}
+\end{equation}
+
+\begin{equation}
+{Y'} = Y - {Y_{so}}
+\end{equation}
+
+\begin{equation}
+{Z'} = Z - {Z_{so}}
+\end{equation}
+
+\begin{equation}
+{X_{sr}} =  - {X'}\cdot \cos \psi  + {Y'}\cdot \sin \psi
+\end{equation}
+
+\begin{equation}
+{Y_{sr}} =  - {X'}\cdot \sin \psi \cdot \cos \phi  + {Y'}\cdot \cos \psi \cdot \cos \phi  + {Z'}\cdot \sin \phi
+\end{equation}
+
+\begin{equation}
+{Z_{sr}} =  - {X'}\cdot \sin \psi \cdot \sin \phi  + {Y'}\cdot \cos \psi \cdot \sin \phi  + {Z'}\cdot \cos \phi
+\end{equation}
+
+\subsection{Shadow Projection}\label{shadow-projection}
+
+All architectural forms are represented by plane polygons. This can give good accuracy even for curved surfaces: a sphere can be approximated by the 20 nodes of an icosahedron with only 3 percent error in the shadow area cast by the sphere. Consider how a solid object, which is composed of a set of enclosing plane polygons, casts a shadow. Figure~\ref{fig:basic-shadowing-concept-structure} shows a box shaped structure on a horizontal surface. The structure consists of a top (surface 1) and four vertical surfaces (2 and 3 visible to the observer and 4 and 5 not visible). The sun is positioned behind and to the right of the structure and a shadow is cast onto the horizontal surface (the ground).
+
+Surfaces 1, 4, and 5 are in sunlight; 2 and 3 are in shade. It is possible to think of the structure's shadow as the combination of shadows cast by surfaces 1, 2, 3, 4 and 5 or by 1, 4 and 5, or by surfaces 2 and 3.~ This last combination of shadow casting surfaces is the simplest. In the EnergyPlus shadow algorithm every surface is considered to be one of the surfaces that enclose a solid, and only those surfaces that are not sunlit at a given hour are considered shadowing surfaces.
+
+\begin{figure}[hbtp] % fig 41
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image622.png}
+\caption{Basic shadowing concept structure \protect \label{fig:basic-shadowing-concept-structure}}
+\end{figure}
+
+The expressions in equation are the direction cosines of the surface:
+
+\begin{equation}
+C{W_1} = \sin \psi \cdot \cos \phi
+\end{equation}
+
+\begin{equation}
+C{W_2} = \cos \psi \cdot \sin \phi
+\end{equation}
+
+\begin{equation}
+C{W_3} = \cos \phi
+\end{equation}
+
+The cosine of the angle of incidence of the sun's rays on the surface are given by the dot product of surface and sun direction cosines.
+
+\begin{equation}
+\cos \theta  = C{S_1}\cdot C{W_1} + C{S_2}\cdot C{W_2} + C{S_3}\cdot C{W_3}
+\end{equation}
+
+If \(\cos \theta\) ~is less than zero, the sun is behind the surface.
+
+A shadow is projected from the vertices of the shadowing polygon (SP) along the direction of the sun's rays to the plane of the shadow receiving polygon (RP).~ If any vertices of the SP are below the plane of the RP (z \textless{} 0), a false shadow is cast as in Figure~\ref{fig:illustration-of-shadow-clipping}.~ The ``submerged'' portion of the SP must be clipped off before projection.
+
+\begin{figure}[hbtp] % fig 42
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image628.png}
+\caption{Illustration of Shadow Clipping \protect \label{fig:illustration-of-shadow-clipping}}
+\end{figure}
+
+This is done by finding, through linear interpolation, the points on the perimeter of the SP, which intersect the plane of the RP. These points become new vertices of the SP, which together with the other positive vertices define a clipped SP that casts only a real shadow.
+
+A vertex located at (x, y, z) relative to the RP coordinate system casts a shadow to a point in the plane of the RP given by
+
+\begin{equation}
+{x'} = x - \frac{{z\cdot a}}{{\cos \theta }}
+\end{equation}
+
+\begin{equation}
+{y'} = y - \frac{{z\cdot b}}{{\cos \theta }}
+\end{equation}
+
+where
+
+\begin{equation}
+a = \sin \psi \cdot C{S_1} - \cos \psi \cdot C{S_2}
+\end{equation}
+
+and
+
+\begin{equation}
+b =  - \cos \psi \cdot \cos \phi \cdot C{S_1} - \sin \psi \cdot \cos \phi \cdot C{S_2} + \sin \phi \cdot C{S_3}
+\end{equation}
+
+More explicitly, a casting surface -- a shadow casting surface or general casting surface -- is one that casts a shadow on other surfaces. A receiving surface -- a shadow receiving surface -- is one that receives shadows from other surfaces (i.e.~casting surfaces). A back surface -- an inside surface -- is one that may be partially sunlit/receive solar transmission for interior solar distribution.
+
+\subsection{Homogeneous Coordinates}\label{homogeneous-coordinates}
+
+Two-dimensional homogeneous coordinate techniques are used to determine the vertices of shadow overlaps. In homogeneous coordinates, points and lines are represented by a single form that allows simple vector operations between those forms {[}Newman-Sproul{]}.~ A point (X, Y) is represented by a three element vector (x, y, w) where x = w*X, y = w*Y, and w is any real number except zero. A line is also represented by a three element vector (a, b, c). The directed line (a, b, c) from point (x\(_{1}\), y\(_{1}\), w\(_{1}\)) to point (x\(_{2}\), y\(_{2}\), w\(_{2}\)) is given by:
+
+\begin{equation}
+(a,b,c) = ({x_1},{y_1},{z_1}) \otimes ({x_2},{y_2},{z_2})
+\end{equation}
+
+The sequence in the cross product is a convention to determine sign. The condition that a point (x, y, w) lie on a line (a, b, c) is that
+
+\begin{equation}
+(a,b,c) \bullet (x,y,w) = 0
+\end{equation}
+
+The point is normalized by dividing by w. Then if
+
+\begin{equation}
+(a,b,c) \bullet (x/w,y/w,1) > 0
+\end{equation}
+
+the point is to the left of the line.~ If it is less than zero, the point is to the right of the line. The intercept (x, y, w) of line (a\(_{1}\), b\(_{1}\), c\(_{1}\)) and line (a\(_{2}\), b\(_{2}\), c\(_{2}\)) is given by:
+
+\begin{equation}
+(x,y,w) = ({a_1},{b_1},{c_1}) \otimes ({a_2},{b_2},{c_2})
+\end{equation}
+
+Note that the use of homogeneous coordinates as outlined above provides a consistent method and notation for defining points and lines, for determining intercepts, and for determining whether a point lies to the left, to the right, or on a line.~ Normalization provides the means for transforming to and from homogeneous notation and Cartesian coordinates.~ Thus, if (X, Y) is a Cartesian coordinate pair, its homogeneous coordinates are (X, Y, 1).~ Similarly, the homogeneous coordinates (x, y, w) can be transformed to the Cartesian point with coordinates (x/w, y/w).
+
+\subsection{Polygon Clipping Algorithms}\label{polygon-clipping-algorithms}
+
+Two methods for polygon clipping (treating of overlapping shadows) are currently in use in EnergyPlus.
+
+\begin{itemize}
+\item
+  Convex Weiler - Atherton
+\item
+  Sutherland -- Hodgman
+\end{itemize}
+
+The original EnergyPlus method for polygon clipping is a special version of the Weiler-Atherton model (Weiler, Atherton, 1977). It was developed to be sufficiently general to clip concave polygons with holes. The implementation in the current version of EnergyPlus, however, does not support concave shadowing surfaces or holes. The relative computational complexity is preserved -- the algorithm is carried out in four steps. For example, if A and B are polygons (see Figure~\ref{fig:point-a-vertex-of-a-enclosed-by-b}).
+
+1)~~~A call to INCLOS determines which vertices of X lie within Y.
+
+2)~~~A second call determines which vertices of Y lie within X.
+
+3)~~~If neither polygon is contained completely within the other, INTCPT is called to collect points of intersection between X and Y.
+
+4)~~~Since the points are usually gathered out of order, they must then be oriented.
+
+The Sutherland-Hodgman algorithm (Sutherland, Hodgman, 1974) is less complex compared to the Weiler-Atherton method and is well-suited to clipping convex polygons. In actuality, only convex shading surfaces are currently supported by EnergyPlus. Let X be a polygon called the ``subject polygon'' (SP) and Y be a polygon called the ``clipping polygon'' (CP). The method performs the computation by iterating over the edges of the CP and removing points from the SP that fall in the clipping plane, i.e.~points that fall to the left of the edge of the CP. Intersections between the clip edge and the edges of the SP are added appropriately, and points falling outside of the clipping plane, i.e.~to the right of the edge of the CP, are added the output polygon as well. This resultant polygon is stored and the process is repeated for the rest of the clip edges in CP. The process is analogous to cutting off pieces of the SP one-by-one with respect to each edge of the CP. The result is ordered and identical to the polygon produced by the Weiler-Atherton method.
+
+\subsection{Overlapping Shadows}\label{overlapping-shadows}
+
+After transforming the shadows onto the plane of the receiving surface, the basic job of the shadow algorithm is to determine the area of the overlap between the polygons representing the shadows and the polygon representing the receiving surface. Concave surfaces are supported only for exterior wall heat transfer surfaces, when using SutherlandHodgman option. Concave shading devices are not supported by the this option. Neither concave shading devices nor concave exterior wall heat transfer surfaces are supported by the ConvexWeilerAtherton clipping routine.
+
+When only convex shading devices are considered, this provides a great simplification. The overlap between two convex polygons (i.e.~projections of shading devices via the direction of the sun) is another convex polygon. Coordinate and projection transformations of a convex polygon produce another convex polygon. Any non-convex polygon can be constructed as the union of convex ones.
+
+For ConvexWeilerAtherton, there is considerable simplification if only convex (no interior angle \textgreater{} 180 ) polygons are considered. The overlap between two convex polygons is another convex polygon. Coordinate and projection transformations of a convex polygon produce another convex polygon. Any non-convex polygon can be constructed as a sum of convex ones.
+
+The vertices that define the overlap between two convex polygons, A and B, consist of:
+
+\begin{itemize}
+\item
+  the vertices of A enclosed by B
+\item
+  the vertices of B enclosed by A
+\item
+  and the intercepts of the sides of A with the sides of B
+\end{itemize}
+
+In Figure~\ref{fig:point-a-vertex-of-a-enclosed-by-b}, point a is the result of rule 1, point c is the result of rule 2, and points b and d result from rule 3. The overlap of A and B is the polygon a-b-c-d. Figure~\ref{fig:surface-a-totally-overlaps-surface-b.} shows an overlap where all of the vertices of B are enclosed by A.~ Figure~\ref{fig:figure-formed-from-intercept-overlaps-between} shows an overlap defined only by the intercepts of A and B. Figure~\ref{fig:complex-overlapping-condition} shows a more complex overlap.
+
+\begin{figure}[hbtp] % fig 43
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image637.png}
+\caption{Point a – Vertex of A Enclosed by B \protect \label{fig:point-a-vertex-of-a-enclosed-by-b}}
+\end{figure}
+
+Coordinate transformation retains the order of the vertices of a polygon, while a projection reverses the order. The sequence of vertices of the receiving polygons should be reversed so it and all shadow polygons will have the same sequence.
+
+\begin{figure}[hbtp] % fig 44
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image638.png}
+\caption{Surface A Totally Overlaps Surface B. \protect \label{fig:surface-a-totally-overlaps-surface-b.}}
+\end{figure}
+
+A point is enclosed by a clockwise, convex polygon if the point lies to the right of all sides (or does not lie to the left of any side) of the polygon.~ The intercept of two sides may not lie beyond the ends of either side. These are ``line segments'' rather than ``lines''. It is possible to tell if line segments A and B intercept within their end points by noting that the ends of A must lie on both sides of B, and the ends of B must lie on both sides of A. This should be done before the intercept is calculated.
+
+\begin{figure}[hbtp] % fig 45
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image639.png}
+\caption{Figure Formed from Intercept Overlaps Between A and B \protect \label{fig:figure-formed-from-intercept-overlaps-between}}
+\end{figure}
+
+Once the vertices are determined, they must be sorted into clockwise order for the area to be computed.~ Given a closed, planar polygon of n sequential vertices (x\(_{1}\), y\(_{1}\)), (x\(_{2}\), y\(_{2}\)) \ldots{}, (x\(_{n}\), y\(_{n}\)), its \textbf{area} is given:
+
+\begin{equation}
+Area = {\textstyle{1 \over 2}}\sum\limits_{i = 1}^n {({x_i}{y_{i + 1}} - {x_{i + 1}}{y_i})}
+\end{equation}
+
+where (x\(_{n+1}\),y\(_{n+1}\)) = (x\(_{1}\), y\(_{1}\))
+
+The area is positive if the vertices are counter-clockwise and negative if they are clockwise.
+
+\begin{figure}[hbtp] % fig 46
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image641.png}
+\caption{Complex Overlapping Condition \protect \label{fig:complex-overlapping-condition}}
+\end{figure}
+
+If two shadows overlap the receiving surface, they may also overlap each other as in Figure~\ref{fig:multiple-shadow-overlaps}. The vertices of this overlap can be computed.~ The areas of all overlaps can be computed.~ The total sunlit area can be expressed as the sum of all polygon areas given a proper sign on each of the areas.
+
+The following convention was adopted:
+
+% table 24
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Surface / Area Characteristic / Convention \label{table:surface-area-characteristic-convention}} \tabularnewline
+\toprule 
+Surface Characteristic & Area Convention \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Surface / Area Characteristic / Convention} \tabularnewline
+\toprule 
+Surface Characteristic & Area Convention \tabularnewline
+\midrule
+\endhead
+
+receiving surface & positive (A) \tabularnewline
+overlap between shadow and receiving & negative (B  \&  C) \tabularnewline
+overlap between two shadows & positive (D) \tabularnewline
+\bottomrule
+\end{longtable}
+
+and so on through multiple overlaps where the sign of the overlap area is the product of the signs of the overlapping areas.
+
+\begin{figure}[hbtp] % fig 47
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image642.png}
+\caption{Multiple Shadow Overlaps \protect \label{fig:multiple-shadow-overlaps}}
+\end{figure}
+
+Partially transparent shadowing surfaces can also be modeled by giving a transparency ($\tau$) to every shadowing polygon. Let $\tau$ of the receiving polygon be one. Then the $\tau$ of every overlap of polygons i and j is the product of $\tau$\(_{i}\)and $\tau$\(_{j}\). The shaded area is then computed by summing A\(_{i}\)*(1 - $\tau$\(_{i}\)) for all overlap polygons.
+
+It is easy to determine the sunlit area of a window once all the shadow and overlap vertices on the wall have been computed. Consider wall 2 of Figure~\ref{fig:overall-shadowing-scheme-depiction}. First, the wall is considered a simple rectangle and the window on it is ignored. The shadow overlapping is performed and the sunlit portion of the gross wall area is computed. Then the window rectangle is overlapped with the shadow to determine its sunlit area. The sunlit area of the window is subtracted from the gross wall sunlit area to determine the net wall sunlit area. During this calculation it is not necessary to recompute the shadows, because they were precisely determined on the wall.
+
+When the SutherlandHodgman option is selected, the overlap is computed using the Sutherland-Hodgman algorithm for polygon clipping when. Let X be a polygon called the ``subject polygon'' (SP) and Y be a polygon called the ``clipping polygon'' (CP). The method performs the computation by iterating over the edges of the CP and removing points from the SP that fall in the clipping plane, i.e.~points that fall to the left of the edge of the CP. If it is to the left of any edge, it the point does not overlap with the CP. Intersections between the clip edge and the edges of the SP are added appropriately, and points falling outside of the clipping plane, i.e.~to the right of the edge of the CP, are added the output polygon as well. This resultant polygon is stored and the process is repeated for the rest of the clip edges in CP. The process is analogous to cutting off pieces of the SP one-by-one with respect to each edge of the CP. Note that the SP may be concave, but the CP may not. This means that the exterior wall surfaces may be concave, while shading devices may not be concave.
+
+\subsection{Solar Gains}\label{solar-gains-000}
+
+The total solar gain on any exterior surface is a combination of the absorption of direct and diffuse solar radiation given by
+
+\begin{equation}
+{Q_{so}} = \alpha \cdot \left( {{I_b}\cdot \cos \theta \cdot \frac{{{S_s}}}{S} + {I_s}\cdot {F_{ss}} + {I_g}\cdot {F_{sg}}} \right)
+\end{equation}
+
+where
+
+a = solar absorptance of the surface
+
+A = angle of incidence of the sun's rays
+
+S = area of the surface
+
+S\(_{s}\) = sunlit area
+
+I\(_{b}\) = intensity of beam (direct) radiation
+
+I\(_{s}\) = intensity of sky diffuse radiation
+
+I\(_{g}\) = intensity of ground reflected diffuse radiation
+
+F\(_{ss}\) = angle factor between the surface and the sky
+
+F\(_{sg}\) = angle factor between the surface and the ground
+
+For the surface of a building located on a featureless plain
+
+\begin{equation}
+{F_{ss}} = \frac{{1 + \cos \phi }}{2}
+\end{equation}
+
+and
+
+\begin{equation}
+{F_{sg}} = \frac{{1 - \cos \phi }}{2}
+\end{equation}
+
+If the surface is shaded the program modifies \emph{F\(_{ss}\)} by a correction factor that takes into account the radiance distribution of the sky (see ``Shadowing of Sky Diffuse Solar Radiation'').
+
+Shading of ground diffuse solar radiation is not calculated by the program. It is up to the user to estimate the effect of this shading and modify the input value of \emph{F\(_{sg}\)} accordingly.
+
+\subsection{Solar Distribution}\label{solar-distribution}
+
+As discussed in the Input Output Reference (Object: Building), the field Solar Distribution, in the ``Building'' input object, determines how EnergyPlus will treat beam solar radiation entering a zone through exterior windows.~ There are five choices: \textbf{MinimalShadowing}, \textbf{FullExterior}, \textbf{FullInteriorAndExterior, FullExteriorWithReflections}, and \textbf{FullInteriorAndExteriorWithReflections}.
+
+\subsubsection{MinimalShadowing}\label{minimalshadowing}
+
+In this case, there is no exterior shadowing except from window and door reveals. All beam solar radiation entering the zone is assumed to fall on the floor, where it is absorbed according to the floor's solar absorptance. Any reflected by the floor is added to the transmitted diffuse radiation, which is assumed to be uniformly distributed on all interior surfaces. If no floor is present in the zone, the incident beam solar radiation is absorbed on all interior surfaces according to their absorptances. The zone heat balance is then applied at each surface and on the zone's air with the absorbed radiation being treated as a flux on the surface.
+
+\subsubsection{FullExterior}\label{fullexterior}
+
+In this case, shadow patterns on exterior surfaces caused by detached shading, wings, overhangs, and exterior surfaces of all zones are computed. As for MinimalShadowing, shadowing by window and door reveals is also calculated. Beam solar radiation entering the zone is treated as for MinimalShadowing.
+
+\subsubsection{FullExteriorWithReflections}\label{fullexteriorwithreflections}
+
+This case is the same interior distribution as the preceding option but uses exterior reflections as well (see the section Solar Radiation Reflected from Exterior Surfaces for further explanation).
+
+\subsubsection{FullInteriorAndExterior}\label{fullinteriorandexterior}
+
+This is the same as FullExterior except that instead of assuming all transmitted beam solar falls on the floor the program calculates the amount of beam radiation falling on each surface in the zone, including floor, walls and windows, by projecting the sun's rays through the exterior windows, taking into account the effect of exterior shadowing surfaces and window shading devices.
+
+If this option is used, you should be sure that the surfaces of the zone totally enclose a space. This can be determined by viewing the \textbf{eplusout.dxf} file with a program like AutoDesk's Volo View Express. You should also be sure that the zone is \textbf{convex}. Examples of convex and non-convex zones are shown in Figure~\ref{fig:illustration-of-convex-and-non-convex-zones}. The most common non-convex zone is an L-shaped zone. (A formal definition of convex is that any straight line passing through the zone intercepts at most two surfaces.)~ If the zone's surfaces do not enclose a space or if the zone is not convex you should use Solar Distribution = \textbf{FullExterior} instead of \textbf{FullInteriorAndExterior}.
+
+If you use \textbf{FullInteriorAndExterior} the program will calculate how much beam radiation falling on an interior window is absorbed by the window, how much is reflected back into the zone, and how much is transmitted into the adjacent zone. (Interior windows are assumed to have no shading device).
+
+If you use \textbf{FullInteriorAndExterior} the program will also calculate how much beam radiation falling on the inside of an exterior window (from other windows in the zone) is absorbed by the window, how much is reflected back into the zone, and how much is transmitted to the outside. In this calculation the effect of an interior or exterior shading device, if present, is accounted for.
+
+\subsubsection{FulInteriorAndlExteriorWithReflections}\label{fulinteriorandlexteriorwithreflections}
+
+This case is the same interior distribution as the preceding option but uses exterior reflections as well (see Solar Radiation Reflected from Exterior Surfaces for further explanation).
+
+\begin{figure}[hbtp] % fig 48
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image646.png}
+\caption{Illustration of Convex and Non-convex Zones \protect \label{fig:illustration-of-convex-and-non-convex-zones}}
+\end{figure}
+
+\subsection{Details of the Interior Solar Distribution Calculation}\label{details-of-the-interior-solar-distribution-calculation}
+
+EnergyPlus calculates the distribution of short-wave radiation in the interior of each thermal zone. This radiation consists of beam solar radiation, diffuse solar radiation, and short-wave radiation from electric lights. The program determines the amount of this radiation that is (1) absorbed on the inside face of opaque surfaces, (2) absorbed in the glass and shading device layers of the zone's exterior and interior windows, (3) transmitted through the zone's interior windows to adjacent zones, and (4) transmitted back out of the exterior windows. The effects of movable shading devices on the exterior windows are taken into account; \emph{the program does not allow shading devices on interior windows}. Most of this calculation is done in subroutine CalcInteriorSolarDistribution in the SolarShading module.
+
+\subsubsection{Initial Distribution of Diffuse Solar Transmitted through Exterior and Interior Windows}\label{initial-distribution-of-diffuse-solar-transmitted-through-exterior-and-interior-windows}
+
+Diffuse solar (from sky and ground sources) transmitted through exterior windows is first distributed to the interior heat transfer surfaces in the zone containing the exterior windows. This initial distribution apportions the transmitted diffuse solar to interior surfaces using the approximate view factors described above in ``LW Radiation Exchange Among Zone Surfaces.'' The amount of this initially distributed diffuse solar absorbed by each interior surface, and each window material layer, is calculated and later added to the ``short-wave radiation absorbed'' values described below. The amount of this initially distributed diffuse solar that is reflected is accumulated for each zone and redistributed uniformly as part of the QD calculation described below. The amount of this initially distributed diffuse solar that is transmitted by interior windows to adjacent zones is initially distributed to the interior heat transfer surfaces in the adjacent zone in the same manner as just described.
+
+This new treatment of diffuse solar is intended to more accurately account for the initial absorption, transmittance, and reflection of short-wave radiation prior to the uniform distribution described below.
+
+\subsubsection{Interior Solar Radiation Absorbed by Opaque Surfaces}\label{interior-solar-radiation-absorbed-by-opaque-surfaces}
+
+The short-wave radiation absorbed on the inside face of an opaque surface (floor, wall or ceiling) is given by
+
+\begin{equation}
+\begin{array}{l}
+QRadSWInAbs(SurfNum) = QS(ZoneNum)*AbsIntSurf(SurfNum) \\
+\quad \quad \quad \quad+ AISurf(SurfNum)*BeamSolarRad [W/m2]
+\end{array}
+\end{equation}
+
+where
+
+\emph{SurfNum} = surface number
+
+\emph{ZoneNum =}number of zone that surface belongs to
+
+\emph{QS(ZoneNum)} = short-wave diffuse irradiance in the zone {[}W/m\(^{2}\){]}
+
+\emph{AbsIntSurf(SurfNum)} = inside solar absorptance of the surface
+
+\emph{AISurf(SurfNum)} = inside beam solar irradiance factor for the surface {[}-{]}
+
+\emph{BeamSolarRad} = outside beam normal solar irradiance {[}W/m\(^{2}\){]}
+
+\paragraph{Interior Diffuse Radiation}\label{interior-diffuse-radiation}
+
+\emph{QS} is assumed to be uniformly distributed throughout the zone. It is calculated as follows. Let \emph{Q\(_{sw}\)} be the total diffuse short-wave radiation entering the zone or originating in the zone. Since \emph{Q\(_{sw}\)} is ultimately absorbed or transmitted by zone heat transfer surfaces, summing over these surfaces gives the following energy balance equation:
+
+\begin{equation}
+\sum\limits_{i = 1}^{{N_{surf}}} {QS(ZoneNum)*{\alpha_i}{A_i} = {Q_{SW}}(ZoneNum)}
+\end{equation}
+
+where
+
+\emph{i} = zone surface number counter
+
+\emph{N\(_{surf}\)} = number of heat transfer surfaces in zone
+
+\emph{A\(_{i}\)} = surface area {[}m\(^{2}\){]}
+
+\({\alpha_i}\) = inside solar absorptance for an opaque surface, or, for a window, = back diffuse transmittance plus back diffuse system absorptance of glass layers and shading device layers (if present)
+
+Solving this equation for \emph{QS} gives:
+
+\begin{equation}
+QS(ZoneNum) = \frac{{{Q_{SW}}(ZoneNum)}}{{\sum\limits_{i = 1}^{{N_{surf}}} {AbsInsSur{f_i}{A_i}} }} = {Q_{SW}}(ZoneNum)*VMULT(ZoneNum)
+\end{equation}
+
+where
+
+\begin{equation}
+VMULT(ZoneNum) = \frac{1}{{\sum\limits_{i = 1}^{{N_{surf}}} {AbsIntSur{f_i}*{A_i}} }}{\rm{    [}}{{\rm{m}}^{{\rm{ - 2}}}}]
+\end{equation}
+
+\emph{Q\(_{sw}\)} is given by
+
+\begin{equation}
+\begin{array}{l}
+Q{S_{SW}} = QD(ZoneNum) + ZoneIntGain(ZoneNum)\% QLTSW \\
+\quad \quad \quad + ZoneIntGain(ZoneNum)\% T_QLTSW [W]
+\end{array}
+\end{equation}
+
+where
+
+\emph{ZoneIntGain(ZoneNum)\%QLTSW} = short-wave radiation into zone from general (overhead) electric lighting {[}W{]}
+
+\emph{ZoneIntGain(}ZoneNum\emph{)\%T\_QLTSW} = short-wave radiation into zone from task electric lighting {[}W{]}
+
+\emph{QD(ZoneNum)} = diffuse solar radiation entering or originating in zone {[}W{]}
+
+\emph{QD(ZoneNum)} is given by:
+
+\begin{equation}
+\begin{array}{l}
+QD(ZoneNum) = DBZone(ZoneNum)*BeamSolarRad \\
+\quad \quad \quad + InitialDifSolDistReflectedW(ZoneNum)
+\end{array}
+\end{equation}
+
+where
+
+\emph{BeamSolarRad} is the outside beam normal solar irradiance {[}W/m\(^{2}\){]}
+
+\emph{DBZone(ZoneNum)} is the diffuse solar radiation originating from beam solar that passes through the exterior windows in the zone and reflects diffusely from inside zone surfaces plus beam solar entering the zone as diffuse radiation from windows with shading devices or diffusing glass (all divided by BeamSolarRad)~~ {[}m\(^{2}\){]}
+
+\emph{InitialDifSolDistReflectedW(ZoneNum)} is the diffuse solar radiation originating from sky and sun related diffuse solar transmitted through the zone's exterior or interior windows into the zone, and reflected diffusely from inside zone surfaces.
+
+\emph{DBZone(ZoneNum)} is calculated as:
+
+\begin{equation}
+DBZone(ZoneNum) = BTOTZone - BABSZone{\rm{    [}}{{\rm{m}}^{\rm{2}}}]
+\end{equation}
+
+where
+
+\emph{BTOTZone} = total beam solar incident on the zone's exterior windows that is transmitted as beam or diffuse.\protect\hyperlink{ux5fftn1}{{[}1{]}}
+
+\emph{BABSZone =} total beam solar absorbed inside the zone.
+
+\emph{BTOTZone} is given by:
+
+\begin{equation}
+BTOTZone = \sum\limits_{i = 1}^{{N_{extwin}}} {TBmAl{l_i}*SunlitFrac{t_i}*CosIn{c_i}*Are{a_i}*InOutprojSLFracMul{t_i}}
+\end{equation}
+
+\emph{+ Diffuse entering zone from beam reflected by window inside reveal surfaces\protect\hyperlink{ux5fftn2}{\textbf{{[}2{]}}}}
+
+\emph{+ Diffuse transmitted by windows from beam reflected by outside reveal surfaces}
+
+\emph{--~ Beam absorbed by window inside reveal surfaces}
+
+Here,
+
+\emph{TBmAll} = beam-to-beam plus beam-to-diffuse transmittance of window
+
+\emph{SunlitFract} = fraction of window irradiated by sun
+
+\emph{CosInc} = cosine of solar incidence angle on window
+
+\emph{Area} = glazed area of window {[}m\(^{2}\){]}
+
+\emph{InOutProjSLFracMult} = shadowing factor due to inside and outside projections of window frame and/or divider ( = 1.0 if there is no frame or divider).
+
+\emph{BABSZone} is given by the following sum (see Figure~\ref{fig:vertical-section-through-a-two-zone-building}):
+
+\emph{BABSZone} = ~ \emph{Beam absorbed by opaque inside surfaces\protect\hyperlink{ux5fftn3}{\textbf{{[}3{]}}}}
+
+\emph{~~~~~~~~~~~~~~~~~~~~~~~ + Beam transmitted through the zone's interior windows +}
+
+\emph{~~~~~~~~~~~~~~~~~~~~~~~ + Beam transmitted back out of the zone's exterior windows +}
+
+\emph{~~~~~~~~~~~~~~~~~~~~~~~ + Beam absorbed by the zone's exterior and interior windows +}
+
+\emph{~~~~~~~~~~~~~~~~~~~~~~~ + Beam absorbed by inside daylighting shelves}
+
+\begin{figure}[hbtp] % fig 49
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image656.png}
+\caption{Vertical section through a two-zone building showing where transmitted beam solar falls. Some of the beam solar from exterior window EW is absorbed by the floor, D, interior wall, B, and interior window, IW. Some is transmitted by IW to the adjacent zone, Z2. Aoverlap is the irradiated area of a surface projected back onto the plane of EW. Beam reflected by D, B and IW contributes to the interior short-wave radiation flux in Z1. \protect \label{fig:vertical-section-through-a-two-zone-building}}
+\end{figure}
+
+If zone \emph{ZoneNum} shares interior windows with other zones, \emph{QS(ZoneNum)} is modified to take into account short-wave radiation received from the other zones through these windows:
+
+\begin{equation}
+\begin{array}{rl}
+   QS(ZoneNum) & = QS(ZoneNum) \\
+               &+ \sum_{otherZones}\text{FractDifShortZtoZ(OtherZoneNum,ZoneNum)} \\
+               &* [QD(OtherZoneNum) + ZoneIntGain(OtherZoneNum)\% QLTSW \\
+               &\quad + ZoneIntGain(OtherZoneNum)\% T_QLTSW]
+  \end{array}
+\end{equation}
+
+where
+
+\emph{FractDifShortZtoZ(OtherZoneNum,ZoneNum)} = ``diffuse solar exchange factor'' = fraction of short-wave radiation in \emph{OtherZoneNum} that is transmitted to \emph{ZoneNum}. This factor is calculated in subroutine ComputeDifSolExcZonesWIZWindows taking into account multiple reflection between zones. For example, for two zones means that some of the radiation transmitted from Zone1 to Zone2 is reflected back to Zone1, and some of this is in turn reflected back to Zone2, etc.
+
+\paragraph{Interior Beam Radiation}\label{interior-beam-radiation}
+
+The inside beam solar irradiance factor\protect\hyperlink{ux5fftn4}{{[}4{]}} in is given by:
+
+\(AISurf(SurfNum) = \frac{{AbsIntSurf(SurfNum)}}{{A(SurfNum)}}\sum\limits_{i = 1}^{{N_{extwin}}} {TB{m_i}*Aoverla{p_i}(SurfNum)*CosIn{c_i}}\) where
+
+\emph{i} = exterior window number
+
+\emph{N\(_{extwin}\) =} number of exterior windows in zone
+
+\emph{CosInc\(_{i}\)} = cosine of angle of incidence of beam on exterior window \emph{i}
+
+\emph{TBm\(_{i}\)} = beam-to-beam transmittance of exterior window* i\emph{at}CosInc\(_{i}\)* \protect\hyperlink{ux5fftn5}{{[}5{]}}
+
+\emph{Aoverlap\(_{i}\)(SurfNum)} = beam solar irradiated area of surface \emph{SurfNum} projected back onto the plane of exterior window \emph{i} (the \emph{Aoverlap}'s for an exterior window sum up to the glazed area of the window). These overlap areas (Figure~\ref{fig:vertical-section-through-a-two-zone-building}) are determined with the EnergyPlus shadowing routines by considering a zone's exterior window as a ``sending'' surface and the inside faces of the zone's other surfaces as ``receiving'' surfaces (see ``Shading Module''). The overlap areas for a particular exterior window depend on the sun position, the geometry of the window, the geometry of the interior surfaces, and the location of the window with respect to the interior surfaces.
+
+\emph{AbsIntSurf(SurfNum)} = inside face solar absorptance of surface \emph{SurfNum}
+
+\emph{A(SurfNum)} = area of surface \emph{SurfNum} {[}m\(^{2}\){]}
+
+\subsubsection{Interior Solar Radiation Absorbed by Windows}\label{interior-solar-radiation-absorbed-by-windows}
+
+The interior short-wave radiation absorbed by layer \emph{l} (glass, shade or blind) of a window is equal to:
+
+\(\begin{array}{l}QS(ZoneNum)*\alpha_{l,back}^{dif}(SurfNum) + \\BeamSolarRad*\frac{{\alpha_{l,back}^{beam}(SurfNum)}}{{A(SurfNum)}}\sum\limits_{i = 1}^{{N_{extwin}}} {TB{m_i}*Aoverla{p_i}(SurfNum)} *CosIn{c_i}{\rm{ [W/}}{{\rm{m}}^{\rm{2}}}]\end{array}\) where
+
+\(\alpha_{l,back}^{dif}\) = the system diffuse solar absorptance of layer \emph{l} for irradiance from the back side
+
+\(\alpha_{l,back}^{beam}\) = the system beam solar absorptance of layer \emph{l} for irradiance from the back side
+
+\emph{A(SurfNum)} = glazing area {[}m\(^{2}\){]}
+
+Note that as of Version 2.1, the initially distributed diffuse solar absorbed by each surface (as described above under ``Initial Distribution of Diffuse Solar Transmitted through Exterior and Interior Windows'') is added to this uniformly distributed short-wave radiation.
+
+\subsubsection{Interior Solar Radiation Transmitted by Interior Windows}\label{interior-solar-radiation-transmitted-by-interior-windows}
+
+\paragraph{Interior Diffuse Radiation Transmitted by Interior Windows}\label{interior-diffuse-radiation-transmitted-by-interior-windows}
+
+The interior diffuse short-wave radiation transmitted by an interior window to the adjacent zone is given by
+
+\begin{equation}
+QS(ZoneNum)*{\tau ^{dif}}(SurfNum)*A(SurfNum){\rm{    [W]}}
+\end{equation}
+
+where
+
+\({\tau ^{dif}}(SurfNum)\) = diffuse transmittance of the interior window
+
+\paragraph{Interior Beam Radiation Transmitted by Interior Windows}\label{interior-beam-radiation-transmitted-by-interior-windows}
+
+The interior beam solar radiation transmitted by an interior window to the adjacent zone is
+
+\begin{equation}
+BeamSolarRad*{\tau ^{beam}}(SurfNum)\sum\limits_{i = 1}^{{N_{extwin}}} {TB{m_i}*Aoverla{p_i}(SurfNum)*CosIn{c_i}{\rm{    [W}}]}
+\end{equation}
+
+where \({\tau ^{beam}}(SurfNum)\) is the beam-to-beam transmittance of the interior window at the angle of incidence of beam solar from the exterior window on the interior window. The program does not track where this radiation falls in the adjacent zone: it is counted as diffuse radiation in that zone. Therefore,
+
+\begin{equation}
+QS(ZoneNum) \to QS(ZoneNum) + [{\rm{beam solar from adjacent zones]}}*VMULT(ZoneNum)
+\end{equation}
+
+\subsection{Ground Reflectances}\label{ground-reflectances}
+
+Ground reflectance values (Ref Object: Site:GroundReflectance) are used to calculate the ground reflected solar amount.~ This fractional amount (entered monthly) is used in the following equation:
+
+\begin{equation}
+{\rm{GroundReflectedSolar = (BeamSolar}} \bullet {\rm{COS(SunZenithAngle) + DiffuseSolar)}} \bullet {\rm{GroundReflectance}}
+\end{equation}
+
+Of course, the Ground Reflected Solar is never allowed to be negative.~ The Snow Ground Reflectance Modifier can further modify the ground reflectance when snow is on the ground.~ If the user enters 0.0 for each month, no ground reflected solar is used.
+
+\subsection{Ground Reflectances (Snow)}\label{ground-reflectances-snow}
+
+When snow is on the ground, ground reflectances may change. (Ref Object: Site:\-Ground\-Re\-flect\-ance:\-Snow\-Modifier). This object allows the user to specify two values, Ground Reflected Solar Modifier and Daylighting Ground Reflected Solar Modifier.
+
+Ground Reflected Solar Modifier is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values). Values can range from 0.0 to 1.0.
+
+\begin{equation}
+{\rm{GroundReflectanc}}{{\rm{e}}_{{\rm{used}}}} = {\rm{GroundReflectance}} \bullet SolarModifie{r_{Snow}}
+\end{equation}
+
+Daylighting Ground Reflected Solar Modifier is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values). Values can range from 0.0 to 1.0.
+
+\begin{equation}
+{\rm{DaylightingGroundReflectanc}}{{\rm{e}}_{{\rm{used}}}} = {\rm{GroundReflectance}} \bullet DaylightingModifie{r_{Snow}}
+\end{equation}
+
+\subsection{References}\label{references-041}
+
+ASHRAE. 2005. Handbook of Fundamentals, Chapter 31, Atlanta: ASHRAE.
+
+ASHRAE. 2007. HVAC Applications, Chapter 33, Atlanta, ASHRAE.
+
+Zhang, Qingyuan, Joe Huang, and Siwei Lang. 2002. ``Development of Typical Year Weather Data for Chinese Locations'', American Society of Heating Refrigeration and Air-Conditioning Engineers, ASHRAE Transactions, Vol 108, Part 2.
+
+Threlkeld, J.L. and R.C. Jordan. 1958. Direct solar radiation available on clear days. ASHRAE Transactions 64:45.
+
+Groth, C. C., and Lokmanhekim, M. 1969. ``Shadow ‑ A New Technique for the Calculation of Shadow Shapes and Areas by Digital Computer,'' Second Hawaii International Conference on System Sciences, Honolulu, HI, January 22‑24, 1969.
+
+Walton, G.N. 1983. ``The Thermal Analysis Research Program Reference Manual Program (TARP)'', National Bureau of Standards (now National Institute of Standards and Technology).
+
+Walton, G. N. 1978. ``The Application of Homogeneous Coordinates to Shadowing Calculations'', American Society of Heating Refrigeration and Air-Conditioning Engineers, ASHRAE Transactions, Vol 84, Part I.
+
+Meeus, Jean. 2000. Astronomical Algorithms, Willmann-Bell.
+
+Newman, M. W., and Sproul, R. F. 1973. Principles of Interactive Computer Graphics, McGraw‑Hill.
+
+Polygon area derived from Green's Theorem.~ Graphic Gems repository.
+
+Weiler, Kevin, Atherton, Peter. ``Hidden Surface Removal Using Polygon Area Sorting.'' Program of Computer Graphics, Cornell University. Ithaca, NY: 1977.
+
+Sutherland, I.E., and Hodgman, G.W. 1974. ``Reentrant Polygon Clipping'', Communication of Association for Computing Machinery (CACM), vol.~17, pp.~32-42.
+
+Maillot,Patrick-Gilles.** ``**A New, Fast Method For 2D Polygon Clipping: Analysis and Software Implementation.'' Sun Microsystems, inc. Mountain View, CA: 1992.
+
+Wisstein, Eric W. ``Convex Polygon'' From Mathworld- A Wolfram Web Resource.
diff --git a/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/sky-radiance-model.tex b/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/sky-radiance-model.tex
new file mode 100644
index 00000000000..496061dbaf4
--- /dev/null
+++ b/doc/engineering-reference/src/climate-sky-and-solar-shading-calculations/sky-radiance-model.tex
@@ -0,0 +1,257 @@
+\section{Sky Radiance Model}\label{sky-radiance-model}
+
+In EnergyPlus the calculation of diffuse solar radiation from the sky incident on an exterior surface takes into account the anisotropic radiance distribution of the sky. For this distribution, the diffuse sky irradiance on a surface is given by
+
+\begin{equation}
+AnisoSkyMultiplie{r_{surface}}\cdot DiffuseSolarIrradiance
+\end{equation}
+
+Where
+
+Diffuse Solar Irradiance is the diffuse solar irradiance from the sky on the ground.
+
+surface is the surface being analyzed.
+
+AnisoSkyMultiplier is determined by surface orientation and sky radiance distribution, and accounts for the effects of shading of sky diffuse radiation by shadowing surfaces such as overhangs. It does not account for \emph{reflection} of sky diffuse radiation from shadowing surfaces.
+
+The sky radiance distribution is based on an empirical model based on radiance measurements of real skies, as described in Perez et al., 1990. In this model the radiance of the sky is determined by three distributions that are superimposed (see Figure~\ref{fig:schematic-view-of-sky-showing-solar-radiance})
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\item
+  An isotropic distribution that covers the entire sky dome;
+\item
+  A circumsolar brightening centered at the position of the sun;
+\item
+  A horizon brightening.
+\end{enumerate}
+
+\begin{figure}[hbtp] % fig 37
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image589.png}
+\caption{Schematic view of sky showing solar radiance distribution as a superposition of three components: dome with isotropic radiance, circumsolar brightening represented as a point source at the sun, and horizon brightening represented as a line source at the horizon. \protect \label{fig:schematic-view-of-sky-showing-solar-radiance}}
+\end{figure}
+
+The proportions of these distributions depend on the sky condition, which is characterized by two quantities, \emph{clearness factor} and \emph{brightness factor}, defined below, which are determined from sun position and solar quantities from the weather file.
+
+The \emph{circumsolar brightening} is assumed to be concentrated at a point source at the center of the sun although this region actually begins at the periphery of the solar disk and falls off in intensity with increasing angular distance from the periphery.
+
+The \emph{horizon brightening} is assumed to be a linear source at the horizon and to be independent of azimuth. In actuality, for clear skies, the horizon brightening is highest at the horizon and decreases in intensity away from the horizon. For overcast skies the horizon brightening has a negative value since for such skies the sky radiance increases rather than decreases away from the horizon.
+
+% table 21
+\begin{longtable}[c]{p{1.0in}p{2.0in}p{1.0in}p{2.0in}}
+
+\caption{Variables in Anisotropic Sky Model and Shadowing of Sky Diffuse Radiation \label{table:variables-in-anisotropic-sky-model}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Variables in Anisotropic Sky Model and Shadowing of Sky Diffuse Radiation} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+$I_{sky}$ & Solar irradiance on surface from sky & W/m & - \tabularnewline
+$I_{horizon}$ & Solar irradiance on surface from sky horizon & W/m & - \tabularnewline
+$I_{dome}$ & Solar irradiance on surface from sky dome & W/m & - \tabularnewline
+$I_{circumsolar}$ & Solar irradiance on surface from circumsolar region & W/m & - \tabularnewline
+$I_h$ & Horizontal solar irradiance & W/m & - \tabularnewline
+S & Surface tilt & radians & Surface(SurfNum)\%Tilt*DegToRadians \tabularnewline
+a, b & intermediate variables & - & - \tabularnewline
+$F_1$, $F_2$ & Circumsolar and horizon brightening coefficients & - & F1, F2 \tabularnewline
+$\alpha$ & Incidence angle of sun on surface & radians & IncAng \tabularnewline
+Z & Solar zenith angle & radians & ZenithAng \tabularnewline
+$Delta$ & Sky brightness factor & - & Delta \tabularnewline
+$\varepsilon$ & Sky clearness factor & - & Epsilon \tabularnewline
+m & relative optical air mass & - & AirMass \tabularnewline
+$I_o$ & Extraterrestrial solar irradiance & W/m\(^{2}\) & - \tabularnewline
+$I$ & Direct normal solar irradiance & W/m\(^{2}\) & Material\%Thickness \tabularnewline
+$\kappa$ & constant = 1.041 for Z in radians & radians & - \tabularnewline
+$F_{ij}$ & Brightening coefficient factors & - & F11R, F12R, etc. \tabularnewline
+$R_{circumsolar}$ & Shadowing factor for circumsolar radiation & - & SunLitFrac \tabularnewline
+$R_{dome}$ & Shadowing factor for sky dome radiation & - & DifShdgRatioIsoSky \tabularnewline
+$R_{horizon}$ & Shadowing factor for horizon radiation & - & DifShdgRatioHoriz \tabularnewline
+E & Sky radiance & W/m\(^{2}\) & - \tabularnewline
+$\theta$ & Azimuth angle of point in sky & radians & Theta \tabularnewline
+$\varphi$ & Altitude angle of point in sky & radians & Phi \tabularnewline
+$I_i$ & Irradiance on surface from a horizon element & W/m\(^{2}\) & - \tabularnewline
+$I_{ij}$ & Irradiance on surface from a sky dome element & W/m\(^{2}\) & - \tabularnewline
+SF & Sunlit fraction & - & FracIlluminated \tabularnewline
+$I'$ & Sky solar irradiance on surface with shadowing & W/m\(^{2}\) & - \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Sky Diffuse Solar Radiation on a Tilted Surface}\label{sky-diffuse-solar-radiation-on-a-tilted-surface}
+
+The following calculations are done in subroutine AnisoSkyViewFactors in the SolarShading module.
+
+In the absence of shadowing, the sky formulation described above gives the following expression for sky diffuse irradiance, \emph{I\(_{sky}\)}, on a tilted surface:
+
+\begin{equation}
+{I_{sky}} = {I_{horizon}} + {I_{dome}} + {I_{circumsolar}}
+\end{equation}
+
+where
+
+\begin{equation}
+\begin{array}{rcl}
+    I_{horizon} & = \rm{irradiance on surface from sky horizon} & = I_h F_2\sin S \\
+    I_{dome}    & = \rm{irradiance on surface from sky dome}    & = I_h (1 - F_1)(1 + \cos S)/2 \\
+    I_{circumsolar} & = \rm{irradiance on surface from circumsolar region} & = I_h F_1 a/b
+\end{array}
+\end{equation}
+
+AnisoSkyMult is then \emph{I\(_{sky}\)} /DifSolarRad.
+
+In the above equations:
+
+I\(_{horizon}\) = horizontal solar irradiance (W/m\(^{2}\))
+
+\emph{S} = surface tilt (radians)
+
+\emph{a} = max(0,cos\emph{$alpha$})
+
+\emph{b} = max(0.087, cos\emph{Z})
+
+\emph{F\(_{1}\)} = circumsolar brightening coefficient
+
+\emph{F\(_{2}\)} = horizon brightening coefficient
+
+where
+
+\emph{$alpha$} = incidence angle of sun on the surface (radians)
+
+\emph{Z} = solar zenith angle (radians).
+
+The brightening coefficients are a function of sky conditions; they are given by
+
+\begin{equation}
+\begin{array}{rl}
+    F_1 & = F_{11}(\varepsilon ) + F_{12}(\varepsilon )\Delta  + F_{13}(\varepsilon )Z  \\
+    F_2 & = F_{21}(\varepsilon ) + F_{22}(\varepsilon )\Delta  + F_{23}(\varepsilon )Z
+\end{array}
+\end{equation}
+
+Here the sky brightness factor is
+
+\begin{equation}
+\Delta  = {I_h}m/{I_o}
+\end{equation}
+
+where
+
+\emph{m} = relative optical air mass
+
+\emph{I\(_{o}\)} = extraterrestrial irradiance (taken to have an average annual value of 1353 W/m\(^{2}\));
+
+and the sky \emph{clearness factor} is
+
+\begin{equation}
+\varepsilon  = \frac{{({I_h} + I)/{I_h} + \kappa {Z^3}}}{{1 + \kappa {Z^3}}}
+\end{equation}
+
+where
+
+I = direct normal solar irradiance
+
+$\kappa$ = 1.041 for Z in radians
+
+The factors \emph{F\(_{ij}\)} ~are shown in the following table. The F\(_{ij}\) values in this table were provided by R. Perez, private communication, 5/21/99. These values have higher precision than those listed in Table \# 6 of Perez et al., 1990.
+
+% table 22
+{\scriptsize
+\begin{longtable}[c]{p{0.4in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}}
+
+\caption{$F_{ij}$ Factors as a Function of Sky Clearness Range \label{table:fij-factors-as-a-function-of-sky-clearness}} \tabularnewline
+\toprule 
+\endfirsthead
+
+\caption[]{$F_{ij}$ Factors as a Function of Sky Clearness Range} \tabularnewline
+\toprule 
+\endhead
+
+$\varepsilon$~ Range & 1.000-1.065 & 1.065-1.230 & 1.230-1.500 & 1.500-1.950 & 1.950-2.800 & 2.800-4.500 & 4.500-6.200 & >  6.200 \tabularnewline \midrule
+$F_{11}$ & -0.0083117 & 0.1299457 & 0.3296958 & 0.5682053 & 0.8730280 & 1.1326077 & 1.0601591 & 0.6777470 \tabularnewline \midrule
+$F_{12}$ & 0.5877285 & 0.6825954 & 0.4868735 & 0.1874525 & -0.3920403 & -1.2367284 & -1.5999137 & -0.3272588 \tabularnewline \midrule
+$F_{13}$ & -0.0620636 & -0.1513752 & -0.2210958 & -0.2951290 & -0.3616149 & -0.4118494 & -0.3589221 & -0.2504286 \tabularnewline \midrule
+$F_{21}$ & -0.0596012 & -0.0189325 & 0.0554140 & 0.1088631 & 0.2255647 & 0.2877813 & 0.2642124 & 0.1561313 \tabularnewline \midrule
+$F_{22}$ & 0.0721249 & 0.0659650 & -0.0639588 & -0.1519229 & -0.4620442 & -0.8230357 & -1.1272340 & -1.3765031 \tabularnewline \midrule
+$F_{23}$ & -0.0220216 & -0.0288748 & -0.0260542 & -0.0139754 & 0.0012448 & 0.0558651 & 0.1310694 & 0.2506212 \tabularnewline \midrule
+\bottomrule
+\end{longtable}}
+
+\subsection{Shadowing of Sky Diffuse Solar Radiation}\label{shadowing-of-sky-diffuse-solar-radiation}
+
+Sky diffuse solar shadowing on an exterior surface is calculated as follows in subroutine SkyDifSolarShading in the SolarShading module. The sky is assumed to be a superposition of the three Perez sky comp1onents described above.
+
+For the horizon source the following ratio is calculated by dividing the horizon line into 24 intervals of equal length:
+
+\begin{equation}
+{R_{horiz}} = \frac{{{\rm{Irradiance from horizon with obstructions}}}}{{{\rm{Irradiance from horizon without obstructions}}}} = \frac{{\sum\limits_{i = 1}^{24} {{I_i}S{F_i}} }}{{\sum\limits_{i = 1}^{24} {{I_i}} }}
+\end{equation}
+
+where I\(_{i}\) is the unobstructed irradiance on the surface from the i\(^{th}\) interval, SF\(_{i}\) is the sunlit fraction from radiation coming from the \emph{i}\(^{th}\) interval, and the sums are over intervals whose center lies in front of the surface. \emph{SF\(_{i}\)} is calculated using the beam solar shadowing method as though the sun were located at the \emph{i}\(^{th}\) horizon point. Here
+
+\begin{equation}
+{I_i} = E({\theta_i})d\theta \cos {\alpha_i}
+\end{equation}
+
+where
+
+\emph{E} (\emph{$\theta$\(_{i}\)}) = radiance of horizon band (independent of $\theta$)
+
+\emph{d$\theta$} = 2$\pi$/24 = azimuthal extent of horizon interval (radians)
+
+\emph{$\theta$\(_{i}\)} = 0\(^{O}\), 15\(^{O}\), \ldots{} , 345\(^{O}\)
+
+$\alpha$\(_{i}\) = incidence angle on surface of radiation from \emph{$\theta$\(_{i}\)}
+
+The corresponding ratio for the isotropic sky dome is given by
+
+\begin{equation}
+{R_{dome}} = \frac{{{\rm{Irradiance from dome with obstructions}}}}{{{\rm{Irradiance from dome without obstructions}}}} = \frac{{\sum\limits_{i = 1}^{24} {\sum\limits_{j = 1}^6 {{I_{ij}}S{F_{ij}}} } }}{{\sum\limits_{i = 1}^{24} {\sum\limits_{j = 1}^6 {{I_{ij}}} } }}
+\end{equation}
+
+where (\emph{i,j}) is a grid of 144 points (6 in altitude by 24 in azimuth) covering the sky dome, \emph{I\(_{ij}\)} is the unobstructed irradiance on the surface from the sky element at the \emph{ij}\(^{th}\) point, \emph{SF\(_{ij}\)} is the sunlit fraction for radiation coming from the \emph{ij}\(^{th}\) element, and the sum is over points lying in front of the surface. Here
+
+\begin{equation}
+{I_{ij}} = E({\theta_i},{\phi_j})\cos {\phi_j}d\theta d\phi \cos {\alpha_{ij}}
+\end{equation}
+
+where
+
+\emph{E} (\emph{$\theta$\(_{i}\)},\emph{$\phi$\(_{j}\)}) = sky radiance (independent of $\theta$ and $\phi$ for isotropic dome)
+
+\emph{d$\theta$} = 2$\pi$/24 = azimuthal extent of sky element (radians)
+
+\emph{d$\phi$} = ($\pi$/2)/6 = altitude extent of sky element (radians)
+
+\emph{$\theta$\(_{i}\)} = 0\(^{O}\), 15\(^{O}\), \ldots{} , 345\(^{O}\)
+
+\emph{$\phi$\(_{j}\)} = 7.5\(^{O}\), 22.5\(^{O}\), \ldots{} , 82.5\(^{O}\)
+
+$\alpha$\(_{j}\) = incidence angle on surface of radiation from (\emph{$\theta$\(_{i}\)},\emph{$\phi$\(_{j}\)})
+
+Because the circumsolar region is assumed to be concentrated at the solar disk, the circumsolar ratio is
+
+\begin{equation}
+{R_{circumsolar}} = \frac{{{\rm{Irradiance from circumsolar region with obstructions}}}}{{{\rm{Irradiance from circumsolar without obstructions}}}} = S{F_{sun}}
+\end{equation}
+
+where \emph{SF\(_{sun}\)} is the beam sunlit fraction. The total sky diffuse irradiance on the surface with shadowing is then
+
+\begin{equation}
+{I'_{sky}} = {R_{horizon}}{I_{horizon}} + {R_{dome}}{I_{dome}} + {R_{circumsolar}}{I_{circumsolar}}
+\end{equation}
+
+\emph{R\(_{horizon}\)} and \emph{R\(_{dome}\)} are calculated once for each surface since they are independent of sun position.
+
+With shadowing we then have:
+
+AnisoSkyMult = \emph{I'\(_{sky}\)} /DifSolarRad.
+
+\subsection{Shadowing of Sky Long-Wave Radiation}\label{shadowing-of-sky-long-wave-radiation}
+
+EnergyPlus calculates the sky long-wave radiation incident on exterior surfaces assuming that the sky long-wave radiance distribution is isotropic. If obstructions such as overhangs are present the sky long-wave incident on a surface is multiplied by the isotropic shading factor, \emph{R\(_{dome}\)}, described above. The long-wave radiation from these obstructions is added to the long-wave radiation from the ground; in this calculation both obstructions and ground are assumed to be at the outside air temperature and to have an emissivity of 0.9.
diff --git a/doc/engineering-reference/src/daylighting-and-window-calculations.tex b/doc/engineering-reference/src/daylighting-and-window-calculations.tex
new file mode 100644
index 00000000000..ce4eba07cbc
--- /dev/null
+++ b/doc/engineering-reference/src/daylighting-and-window-calculations.tex
@@ -0,0 +1 @@
+\chapter{Daylighting and Window Calculations}\label{daylighting-and-window-calculations}
diff --git a/doc/engineering-reference/src/daylighting-and-window-calculations/complex-fenestration-daylighting-calculations.tex b/doc/engineering-reference/src/daylighting-and-window-calculations/complex-fenestration-daylighting-calculations.tex
new file mode 100644
index 00000000000..41a707c1030
--- /dev/null
+++ b/doc/engineering-reference/src/daylighting-and-window-calculations/complex-fenestration-daylighting-calculations.tex
@@ -0,0 +1,152 @@
+\section{Complex Fenestration Daylighting Calculations}\label{complex-fenestration-daylighting-calculations}
+
+The complex fenestration systems (CFS) daylighting calculation method results in the same Daylighting Factor style output as the it is described in Daylighting Calculations chapter.
+
+Transmitted solar radiation reaches the daylighting sensor in two different ways. The first is an indirect path when solar radiation is reflected from surfaces and uniformly distributed into the space. The second is a direct path when the sensor is directly illuminated by the fenestration system.
+
+For the indirect path, the method performs a one-bounce calculation to determine the diffuse illumination for the zone. For a certain sky condition, including the sun position, the method will calculate which surfaces are illuminated from each of the BSDF directions, taking into account the reflectance of the surfaces. This indirect illumination is calculated from both direct sunlight hitting a window with or without a shading device and diffuse illumination calculated from diffuse light coming into the zone from the sky or the ground. This transmitted light strikes the zone interior surfaces and creates a diffuse component. The CFS daylighting method determines the contribution of each sky patch to the illumination of the zone surfaces based on the BSDF transmittances and then luminance is calculated based on the surface reflection.
+
+For the direct path, the window is subdivided using existing subdivision procedures. From the center of each subdivided element, the angle is calculated to the reference point. The illuminance is calculated based on the BSDF data for the outgoing direction that corresponds to that angle and the incident illumination from sky, ground and sun.
+
+\subsection{Internal Average Reflected Illuminance From Window}\label{internal-average-reflected-illuminance-from-window}
+
+To calculate internal average reflected illumiance from the window it is necessary to calculate transmitted flux at the window.~ Observing an infinitesimal window element, illuminance can originate from the sky or sun, and in both cases the ray can reach the window directly or after reflecting from the ground.~ Based on this, the calculation of luminance at the window is divided into three parts:
+
+\begin{itemize}
+\item
+  Sky-related illuminance and luminous flux
+\item
+  Sun-related illuminance and luminous flux, excluding entering beam
+\item
+  Sun-related illuminance and luminous flux, due to entering beam
+\end{itemize}
+
+where total illuminance will be calculated as a superposition of these three parts.
+
+For any case, illuminace at a window element can be calculated by using the following general approach:
+
+\begin{equation}
+dE{W_{at_window}} = Lu{m_{el}}({\theta_{el}},{\phi_{el}}) \cdot cos({\beta_{el}}) \cdot \cos ({\phi_{el}}) \cdot d{\theta_{el}} \cdot d{\phi_{el}}
+\end{equation}
+
+where \(dE{W_{at_window}}\) ~is the illuminance at a window element, \(Lu{m_{el}}({\theta_{el}},{\phi_{el}})\) ~represents the function of horizontal luminance from the exterior element in the direction \(({\theta_{el}},{\phi_{el}})\) , \({\beta_{el}}\) ~represents the angle at which the ray hits the surface of the window and \(({\theta_{el}},{\phi_{el}})\) ~represents the exterior element azimuth and altitude relative to the window (see Figure~\ref{fig:exterior-luminance-element}).
+
+\begin{figure}[hbtp] % fig 63
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image834.png}
+\caption{Exterior Luminance Element \protect \label{fig:exterior-luminance-element}}
+\end{figure}
+
+This will produce luminous flux at the interior side of the window:
+
+\begin{equation}
+d\phi {W_{inside}} = dE{W_{at_window}} \cdot \tau ({\beta_{el}}) \cdot dA
+\end{equation}
+
+where \(dE{W_{at_window}}\) ~is given by equation , \(\tau ({\beta_{el}})\) ~is the window transmittance at the incoming angle \({\beta_{el}}\) ~and \(dA\) ~is infinitesimal window element surface area.
+
+Integrating luminous flux given by equation over entire window area will give luminous flux on the interior side of the window.
+
+To calculate the interan average reflected illumiance from the window, a simillar approch will be used as described in the chapter ``Internally-Reflected Component of Interior Daylight Illuminance'', which gives the flux balance equation:
+
+\begin{equation}
+A \cdot {E_r} \cdot (1 - \rho ) = {F_1}
+\end{equation}
+
+where \({F_1}\) represents first reflected flux which in the case of non-CFS is calculated by using the split-flux method.~ In the case of CFS, first the reflected flux can be calculated more precisely by using light patches area.~ Since each CFS is described by a BSDF, it is possible to calculate the light patches for each outgoing direction (see Figure~\ref{fig:complex-fenestration-system-light-patches}).
+
+\begin{figure}[hbtp] % fig 64
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image842.png}
+\caption{Complex Fenestration System Light Patches \protect \label{fig:complex-fenestration-system-light-patches}}
+\end{figure}
+
+Considering the total flux passing through the window at the outgoing direction ``k'', the first reflect flux (\({F_{1,k}}\) ) can be calculated as:
+
+\begin{equation}
+{F_{1,k}} = {\phi_k} \cdot \frac{{\sum\limits_{a = 1}^N {({A_{overlap,k,a}} \cdot {\rho_{vis,k,a}})} }}{{\sum\limits_{a = 1}^N {{A_{overlap,k,a}}} }}
+\end{equation}
+
+where \({\phi_k}\) ~is the total flux entering the zone at the BSDF outgoing direction ``k'' and is calculated by integrating equation over the entire window area for a given outgoing direction ``k'', N is the number of interior surfaces hit by the BSDF outgoing direction ``k'' (see Figure~\ref{fig:complex-fenestration-system-light-patches}), \({A_{overlap,k,a}}\) ~is the surface (patch) area which the window from the BSDF outgoing direction ``k'' makes at surface ``a'' and \({\rho_{vis,k,a}}\) ~is the visible reflectance from surface ``a''.
+
+Summing all the outgoing directions will result in total first reflected flux:
+
+\begin{equation}
+{F_1} = \sum\limits_{k = 1}^{{N_{out}}} {{F_{1,k}}}
+\end{equation}
+
+\subsection{Luminance from Exterior Elements}\label{luminance-from-exterior-elements}
+
+The case of CFS luminance from exterior elements can be calculated by using BSDF incoming directions defined for a given CFS.~ Applying equation for a certain incoming BSDF direction will give:
+
+\begin{equation}
+\Delta E{W_{el,i}} = Lum({\theta_i},{\psi_i}) \cdot \cos ({\beta_i}) \cdot \cos ({\phi_i}) \cdot \Delta {\theta_i} \cdot \Delta {\psi_i}
+\end{equation}
+
+This equation can be translated in the BSDF coordinate system where instead of standard azimuth and altitude angles, the equation will be transformed into the BSDF coordinate system.~ In that case, equation becomes:
+
+\begin{equation}
+\Delta E{W_{el,i}} = Lum({\theta_i},{\psi_i}) \cdot {\Lambda_i}
+\end{equation}
+
+where \({\Lambda_i}\) represents the lambda value for the incoming direction ``i''.
+
+\subsection{Luminous Flux and Direct Illuminance at Interior Side of the Window}\label{luminous-flux-and-direct-illuminance-at-interior-side-of-the-window}
+
+In the case of CFS it is of interest to calculate fluxes for each outgoing BSDF direction.~ For a given amount of illuminance at an incoming direction ``i'', flux into direction ``o'' will be calculated as:
+
+\begin{equation}
+\Delta \phi {W_{i,o}} = \Delta E{W_{el}} \cdot {T_{dir - dir,i,o}}
+\end{equation}
+
+where \({T_{dir - dir,i,o}}\) ~is the direct-direct transmittance for given incoming and outgoing directions (``i'' and ``o'').
+
+\begin{figure}[hbtp] % fig 65
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image854.png}
+\caption{Complex Fenestration System Flux Transition - Single Incoming Direction to Single Outgoing Direction \protect \label{fig:complex-fenestration-system-flux-transition}}
+\end{figure}
+
+Total flux from the window at the outgoing direction ``o'' can be calculated by summing over all the incoming directions:
+
+\begin{equation}
+\Delta \phi {W_o} = \sum\limits_{i = 1}^{{N_{inc}}} {(\Delta E{W_{el,i}} \cdot {T_{dir - dir,i,o}})}
+\end{equation}
+
+where \({N_{inc}}\) ~is the number of BSDF incident directions.
+
+Flux transmitted in the outgoing direction ``o'', calculated by equation , can be used for any given distribution of an exterior luminous element.~ Knowing the intensity of the luminous flux, the direct illuminance at a certain point is calculated as:
+
+\begin{equation}
+E{D_o} = \Delta {\Omega_{el}} \cdot \sin ({\phi_{el}}) \cdot \Delta \phi {W_o}
+\end{equation}
+
+where \(E{D_o}\) ~is the direct illuminance at the BSDF outgoing direction ``o'', \(\Delta {\Omega_{el}}\) ~is the spatial angle of the element viewed from a certain reference point and \({\phi_{el}}\) ~is the altitude of the window element viewed from the reference point.
+
+\subsection{Handling Exterior Obstructions}\label{handling-exterior-obstructions}
+
+Exterior obstructions are handled for two different cases.~ The first case is to handle obstructions between the luminous element (sky/ground/sun) and the CFS window element. In that case, the direct illuminance at the window element is modified for the product of all the obstruction transmittances between the luminous and window elements, and equation is modified as:
+
+\begin{equation}
+\Delta E{W_{el,i}} = Lum({\theta_i},{\psi_i}) \cdot {\Lambda_i} \cdot \prod\limits_{p = 1}^{{N_o}} {{\tau_{obs,p}}}
+\end{equation}
+
+where \({N_o}\) ~~is the number of exterior obstructions and \({\tau_{obs,p}}\) ~is the visible transmittance of obstruction ``p''.
+
+The second case is to handle all obstructions between the luminous elements and the ground element.~ The luminance from the ground element is calculated as:
+
+\begin{equation}
+Lu{m_{gnd}} = \frac{{{E_h}}}{\pi } \cdot {\rho_{gnd}}
+\end{equation}
+
+where \({E_h}\) ~is the horizontal illuminance and \({\rho_{gnd}}\) ~is the ground reflectance.~ Horizontal illuminance is obtained by the integration over sky/sun elements and it is of interest to examine if all elements are visible from a certain ground point.~ The integration examines if the ray between the sky and the ground element is hitting an obstruction.~ It does not take into account whether or not the obstruction is transparent, it simply counts the number of hits.~ The sky obstruction multiplier is calculated as:
+
+\begin{equation}
+SOM = \frac{{NumberOfUnobstructedRays}}{{NumberOfRays}}
+\end{equation}
+
+and in case the incoming element is from the ground, the illuminance at the window element (equation ) will be additionally modified from the sky obstruction multiplier:
+
+\begin{equation}
+\Delta E{W_{el,i}} = Lum({\theta_i},{\psi_i}) \cdot {\Lambda_i} \cdot SOM \cdot \prod\limits_{p = 1}^{{N_o}} {{\tau_{obs,p}}}
+\end{equation}
diff --git a/doc/engineering-reference/src/daylighting-and-window-calculations/daylight-factor-calculation.tex b/doc/engineering-reference/src/daylighting-and-window-calculations/daylight-factor-calculation.tex
new file mode 100644
index 00000000000..826dafb0b06
--- /dev/null
+++ b/doc/engineering-reference/src/daylighting-and-window-calculations/daylight-factor-calculation.tex
@@ -0,0 +1,610 @@
+\section{Daylight Factor Calculation}\label{daylight-factor-calculation}
+
+% table 25
+\begin{longtable}[c]{p{1.25in}p{2.0in}p{1.25in}p{1.5in}}
+
+\caption{Variables in Daylighting Calculations \label{table:variables-in-daylighting-calculations}} \tabularnewline
+\toprule 
+Mathematical Variable & Description & Units & Internal Variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Variables in Daylighting Calculations} \tabularnewline
+\toprule 
+Mathematical Variable & Description & Units & Internal Variable \tabularnewline
+\midrule
+\endhead
+
+$E_{h,\text{sky}}$ & Exterior horizontal illuminance due to light from the sky & lux & GILSK \tabularnewline
+$E_{h,\text{sun}}$ & Exterior horizontal illuminance due to light from the sun & lux & GILSU \tabularnewline
+$d_{\text{sky}}$, $d_{\text{sun}}$ & Interior illuminance factor due to sky, sun related light & --- & DFACSK,DFACSU \tabularnewline
+$w_{\text{sky}}$, $w_{\text{sun}}$ & Window luminance factor due to sky, sun related light & cd/lm & SFACSK, SFACSU \tabularnewline
+$b_{\text{sky}}$, $b_{\text{sun}}$ & Window background luminance factor due to sky, sun related light & cd/lm & BFACSK, BFACSU \tabularnewline
+$N$ & Number of exterior windows in a zone & --- & NWD \tabularnewline
+$\theta_{\text{sky}}$, $\varphi_{\text{sky}}$ & Azimuth and altitude angles of a point in the sky & radians & THSKY, PHSKY \tabularnewline
+$\Psi_{cs}$ & Clear sky luminance distribution & $cd/m^2$ & --- \tabularnewline
+$\Psi_{ts}$ & Clear turbid sky luminance distribution & $cd/m^2$ & --- \tabularnewline
+$\Psi_{is}$ & Intermediate sky luminance distribution & $cd/m^2$ & --- \tabularnewline
+$\Psi_{os}$ & Overcast sky luminance distribution & $cd/m^2$ & --- \tabularnewline
+$\varphi_{\text{sun}}$ & Altitude angle of the sun & radians or degrees & PHSUN \tabularnewline
+$\gamma$ & Angle between point in the sky and the sun; or angle between vertical and ray from reference point to window element & radians & G \tabularnewline
+$L_z$ & Sky zenith luminance & cd/m2 & ZENL \tabularnewline
+$m$ & Optical air mass of the atmosphere & m & AM \tabularnewline
+$h$ & Building altitude & m & ELEVATION \tabularnewline
+$E_{h,k}$ & Exterior horizontal illuminance for sky type k & lux & --- \tabularnewline
+$N_{\theta}$, $N_{\varphi}$ & Number of azimuth, altitude steps for sky integration & --- & NTH, NPH \tabularnewline
+$\vec{R}_{ref}$ & Vector from zone origin to reference point & m & RREF \tabularnewline
+$\vec{R}_{win}$ & Vector from zone origin to window element & m & RWIN \tabularnewline
+$\mathrm{d}\Omega$ & Solid angle subtended by window element & steradians & DOMEGA \tabularnewline
+$L_w$ & Luminance of a window element as seen from reference point & $cd/m^2$ & WLUMSK, WLUMSU \tabularnewline
+$L_{w,\text{shade}}$ & Luminance of window element with shade in place & $cd/m^2$ & WLUMSK, WLUMSU \tabularnewline
+$\mathrm{d}E_h$ & Horizontal illuminance at reference point from window element & lux & --- \tabularnewline
+$\mathrm{d}x$, $\mathrm{d}y$ & Size of window element & m & DWX, DWY \tabularnewline
+$D$ & Distance from reference point to window element & m & DIS \tabularnewline
+$B$ & Angle between window element's outward normal and ray from reference point to window element & radians & --- \tabularnewline
+$\hat{R}_{ray}$ & Unit vector from reference point to window element & --- & RAY \tabularnewline
+$\hat{W}_{n}$ & Unit vector normal to window element, pointing away from zone & --- & WNORM \tabularnewline
+$\hat{W}_{21}$ & Unit vector along window y-axis & --- & W21 \tabularnewline
+$\hat{W}_{23}$ & Unit vector along window x-axis & --- & W23 \tabularnewline
+$\tau_{\text{vis}}$ & Glass visible transmittance & --- & TVISB \tabularnewline
+$L$ & Luminance of sky or obstruction & $cd/m^2$ & ELUM, --- \tabularnewline
+$\phi_{FW}$ & Downgoing luminous flux from a window & lm & FLFW --- \tabularnewline
+$\phi_{CW}$ & Upgoing luminous flux from a window & lm & FLCW --- \tabularnewline
+$F_1$ & First-reflected flux & lm & - \tabularnewline
+$\rho_{FW}$ & Area-weighted reflectance of floor and upper part of walls & --- & SurfaceWindow\%RhoFloorWall \tabularnewline
+$\rho_{CW}$ & Area-weighted reflectance of ceiling and upper part of walls & --- & SurfaceWindow\%RhoCeilingWall \tabularnewline
+$E_r$ & Average internally-reflected illuminance & lux & EINTSK, EINTSU \tabularnewline
+$A$ & Total inside surface area of a zone & $m^2$ & ATOT \tabularnewline
+$\rho$ & Area-weighted average reflectance of zone interior surfaces & --- & ZoneDaylight\%AveVisDiffREflect \tabularnewline
+$\theta$, $\varphi$ & Azimuth and altitude angle of a sky or ground element & radians & TH, PH \tabularnewline
+$L(\theta, \varphi)$ & Luminance of sky or ground element at $(\theta, \varphi)$ & $cd/m^2$ & HitPointLum-- \tabularnewline
+$A_w$ & Area of glazed part of window & $m^2$ & Surface\%Area \tabularnewline
+$\beta$ & Angle of incidence, at center of window, of light from a sky or ground element & radians & --- \tabularnewline
+$T(\beta)$ & Glazing visible transmittance at incidence angle $\beta$ & --- & TVISBR \tabularnewline
+$\mathrm{d}\phi_{inc}$ & Luminous flux incident on window from sky or ground element & lm & --- \tabularnewline
+$\mathrm{d}\phi$ & Luminous flux from sky or ground element transmitted through window & lm & --- \tabularnewline
+$\mathrm{d}\phi_{FW}$, $\mathrm{d}\phi_{CW}$ & Luminous flux from sky or ground element transmitted through window and going downward, upward & lm & - \tabularnewline
+$\theta_{\text{min}}$, $\theta_{\text{max}}$ & Azimuth angle integration limits & radians & THMIN, THMAX \tabularnewline
+$\varphi_w$ & Window normal altitude angle & radians & - \tabularnewline
+$\phi_{sh}$, $\phi_{unsh}$ & Transmitted flux through window and shade, without shade & lm & --- \tabularnewline
+$\phi_{CW,sh}$, $\phi_{FW,sh}$ & Upgoing and downgoing portions of transmitted flux through window with shade & lm & --- \tabularnewline
+$\phi_{CW,unsh}$, $\phi_{FW,unsh}$ & Upgoing and downgoing portions of transmitted flux through window without shade & lm & --- \tabularnewline
+$f$ & Fraction of hemisphere seen by the inside of window that lies above the window midplane & --- & SurfaceWindow\%Fraction UpGoing \tabularnewline
+$\phi_{inc}$ & Flux incident on glazing from direct sun & lm & --- \tabularnewline
+$f_{\text{sunlit}}$ & Fraction of glazing that is sunlit & --- & SunLitFrac \tabularnewline
+$\phi$ & Transmitted flux from direct sun & --- & --- \tabularnewline
+$L_{sh}$ & Luminance of window with shade & $cd/m^2$ & --- \tabularnewline
+$L_b$ & Window background luminance & $cd/m^2$ & BLUM \tabularnewline
+$G$ & Discomfort glare constant & --- & GTOT \tabularnewline
+$G_i$ & Discomfort glare constant from window $i$ & --- & --- \tabularnewline
+$\omega$ & Solid angle subtended by window with respect to reference point & steradians & SolidAngAtRefPt \tabularnewline
+$\Omega$ & Solid angle subtended by window with respect to reference point, modified to take direction of occupant view into account & steradians & SolidAngAtRefPtWtd \tabularnewline
+$N_x$, $N_y$ & Number of elements in $x$ and $y$ direction that window is divided into for glare calculation & --- & NWX, NWY \tabularnewline
+$p(x_R, y_R)$ & Position factor for horizontal and vertical displacement ratios $x_R$ and $y_R$ & --- & DayltgGlarePositionFactor \tabularnewline
+$p_H$ & Hopkinson position factor & --- & DayltgGlarePositionFactor \tabularnewline
+$L_b$ & Window background luminance & $cd/m^2$ & BLUM \tabularnewline
+$E_b$ & Illuminance on window background & lm & --- \tabularnewline
+$E_r$ & Total internally-reflected component of daylight illuminance & lm & --- \tabularnewline
+$E_s$ & Illuminance setpoint & lm & IllumSetPoint \tabularnewline
+$G_I$ & Glare Index & --- & GLINDX \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Overview}\label{overview-013}
+
+There are three types of daylight factors: interior illuminance factors, window luminance factors, and window background luminance factors. To calculate these factors the following steps are carried out for each hourly sun position on the sun paths for the design days and for representative days\protect\hyperlink{ux5fftn8}{{[}8{]}} during the simulation run period:
+
+1.~~~~Calculate exterior horizontal daylight illuminance from sky and sun for standard (CIE) clear and overcast skies.
+
+2.~~~~Calculate interior illuminance, window luminance and window background luminance for each window/reference-point combination, for bare and for shaded window conditions (if a shading device has been specified), for overcast sky and for standard clear sky.
+
+3.~~~~Divide by exterior horizontal illuminance to obtain daylight factors.
+
+\subsection{Interior Illuminance Components}\label{interior-illuminance-components}
+
+To calculate daylight factors, daylight incident on a window is separated into two components: (1) light that originates from the \emph{sky} and reaches the window directly or by reflection from exterior surfaces; and (2) light that originates from the \emph{sun} and reaches the window directly or by reflection from exterior surfaces. Light from the window reaches the workplane directly or via reflection from the interior surfaces of the room.
+
+For fixed sun position, sky condition (clear or overcast) and room geometry, the sky-related interior daylight will be proportional to the exterior horizontal illuminance, \emph{E\(_{h,sky}\)}, due to light from the sky. Similarly, the sun-related interior daylight will be proportional to the exterior horizontal solar illuminance, \emph{E\(_{h,sun}\)}.
+
+\subsection{Daylight Factors}\label{daylight-factors}
+
+The following daylight factors are calculated:
+
+\begin{equation}
+{d_{sky}} = \frac{{{\rm{Illuminance at reference point due to sky - related light}}}}{{{E_{h,sky}}}}
+\end{equation}
+
+\begin{equation}
+{d_{sun}} = \frac{{{\rm{Illuminance at reference point due to sun - related light}}}}{{{E_{h,sun}}}}
+\end{equation}
+
+\begin{equation}
+{w_{sky}} = \frac{{{\rm{Average window luminance due to sky - related light}}}}{{{E_{h,sky}}}}
+\end{equation}
+
+\begin{equation}
+{w_{sun}} = \frac{{{\rm{Average window luminance due to sun - related light}}}}{{{E_{h,sun}}}}
+\end{equation}
+
+\begin{equation}
+{b_{sky}} = \frac{{{\rm{Window background luminance due to sky - related light}}}}{{{E_{h,sky}}}}
+\end{equation}
+
+\begin{equation}
+{b_{sun}} = \frac{{{\rm{Window background luminance due to sun - related light}}}}{{{E_{h,sun}}}}
+\end{equation}
+
+For a daylit zone with \emph{N} windows these six daylight factors are calculated for each of the following combinations of reference point, window, sky-condition/sun-position and shading device:
+
+\begin{equation}
+\left[
+    \begin{array}{c}
+      Ref pt 1 \\
+      Ref pt 2
+    \end{array}
+  \right]
+  \left[
+    \begin{array}{c}
+      Window 1 \\
+      Window 2 \\
+      ... \\
+      Window N
+    \end{array}
+  \right]
+  \left[
+    \begin{array}{c}
+      Clear sky, first sun-up hour \\
+      Clear/turbid sky, first sun-up hour \\
+      Intermediate sky, first sun-up hour \\
+      Overcast sky, first sun-up hour \\
+      ...
+      Clear sky, last sun-up hour \\
+      Clear/turbid sky, last sun-up hour \\
+      Intermediate sky, last sun-up hour \\
+      Overcase sky, last sun-up hour
+    \end{array}
+   \right]
+   \left[
+     \begin{array}{c}
+       Unshaded window \\
+       Shaded window \\
+       (if shade assigned)
+     \end{array}
+   \right]
+\end{equation}
+
+\subsection{Sky Luminance Distributions}\label{sky-luminance-distributions}
+
+The luminance distribution of the sky is represented as a superposition of four standard CIE skies using the approach described in (Perez et al. 1990). The standard skies are as follows.
+
+\subsubsection{Clear Sky}\label{clear-sky}
+
+The clear sky luminance distribution has the form (Kittler, 1965; CIE, 1973)
+
+\begin{equation}
+{\psi_{cs}}({\theta_{sky}},{\phi_{sky}}) = {L_z}\frac{{(0.91 + 10{e^{ - 3\gamma }} + 0.45{{\cos }^2}\gamma )(1 - {e^{ - 0.32{\rm{cosec}}{\phi_{sky}}}})}}{{0.27385(0.91 + 10{e^{ - 3(\frac{\pi }{2} - {\phi_{sun}})}} + 0.45{{\sin }^2}{\phi_{sun}})}}
+\end{equation}
+
+Here, \emph{L\(_{z}\)} is the zenith luminance (i.e., the luminance of the sky at a point directly overhead). In the calculation of daylight factors, which are ratios of interior and exterior illumination quantities that are both proportional to \emph{L\(_{z}\)}, the zenith luminance cancels out. For this reason we will use \emph{L\(_{z}\)} = 1.0 for all sky luminance distributions.
+
+The various angles, which are defined in the building coordinate system, are shown in Figure~\ref{fig:illustration-of-convex-and-non-convex-zones}. The angle, $\gamma$, between sun and sky element is given by
+
+\begin{equation}
+\gamma  = {\cos ^{ - 1}}\left[ {\sin {\phi_{sky}}\sin {\phi_{sun}} + \cos {\phi_{sky}}\cos {\phi_{sun}}\cos ({\theta_{sky}} - {\theta_{sun}})} \right]
+\end{equation}
+
+The general characteristics of the clear-sky luminance distribution are a large peak near the sun; a minimum at a point on the other side of~ the zenith from the sun, in the vertical plane containing the sun; and an increase in luminance as the horizon is approached.
+
+\subsubsection{Clear Turbid Sky}\label{clear-turbid-sky}
+
+The clear turbid sky luminance distribution has the form {[}Matsuura, 1987{]}
+
+\begin{equation}
+{\psi_{ts}}({\theta_{sky}},{\phi_{sky}}) = {L_z}\frac{{(0.856 + 16{e^{ - 3\gamma }} + 0.3{{\cos }^2}\gamma )(1 - {e^{ - 0.32{\rm{cosec}}{\phi_{sky}}}})}}{{0.27385(0.856 + 10{e^{ - 3(\frac{\pi }{2} - {\phi_{sun}})}} + 0.3{{\sin }^2}{\phi_{sun}})}}
+\end{equation}
+
+\subsubsection{Intermediate Sky}\label{intermediate-sky}
+
+The intermediate sky luminance distribution has the form {[}Matsuura, 1987{]}
+
+\begin{equation}
+{\psi_{is}}\left( {{\theta_{sky}},{\phi_{sky}}} \right) = {L_z}{Z_1}{Z_2}/({Z_3}{Z_4})
+\end{equation}
+
+where
+
+\begin{equation}
+{Z_1} = \left[ {1.35(\sin (3.59{\phi_{sky}} - 0.009) + 2.31)\sin (2.6{\phi_{sun}} + 0.316) + {\phi_{sky}} + 4.799} \right]/2.326 
+\end{equation}
+
+\begin{equation}
+{Z_2} = \exp \left[ { - 0.563\gamma \{ ({\phi_{sun}} - 0.008)({\phi_{sky}} + 1.059) + 0.812\} } \right]
+\end{equation}
+
+\begin{equation}
+{Z_3} = 0.99224\sin (2.6{\phi_{sun}} + 0.316) + 2.73852
+\end{equation}
+
+\begin{equation}
+{Z_4} = \exp \left[ { - 0.563({\textstyle{\pi  \over 2}} - {\phi_{sun}})\{ 2.6298({\phi_{sun}} - 0.008) + 0.812\} } \right]
+\end{equation}
+
+\begin{figure}[hbtp] % fig 57
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image733.png}
+\caption{Angles appearing in the expression for the clear-sky luminance distribution. \protect \label{fig:angles-appearing-in-the-expression-for}}
+\end{figure}
+
+\subsubsection{Overcast Sky}\label{overcast-sky}
+
+The overcast sky luminance distribution has the form {[}Moon \& Spencer, 1942{]}
+
+\begin{equation}
+{\psi_{os}}({\phi_{sky}}) = {L_z}\frac{{1 + 2\sin {\phi_{sky}}}}{3}
+\end{equation}
+
+Unlike the clear sky case, the overcast sky distribution does not depend on the solar azimuth or the sky azimuth. Note that at fixed solar altitude the zenith (\({\phi_{sky}} = \pi /2\) ) is three times brighter than the horizon (\({\phi_{sky}} = 0\) ).
+
+\subsection{Direct Normal Solar Illuminance}\label{direct-normal-solar-illuminance}
+
+For purposes of calculating daylight factors associated with beam solar illuminance, the direct normal solar illuminance is taken to be 1.0 W/m\(^{2}\). The actual direct normal solar illuminance, determined from direct normal solar irradiance from the weather file and empirically-determined luminious efficacy, is used in the time-step calculation.
+
+\subsection{Exterior Horizontal Illuminance}\label{exterior-horizontal-illuminance}
+
+The illuminance on an unobstructed horizontal plane due to diffuse radiation from the sky is calculated for each of the four sky types by integrating over the appropriate sky luminance distribution:
+
+\begin{equation}
+{E_{h,k}} = \int\limits_0^{2\pi } {\int\limits_0^{\pi /2} {{\psi_k}({\theta_{sky}},{\phi_{sky}})\sin {\phi_{sky}}\cos {\phi_{sky}}d{\theta_{sky}}} } d{\phi_{sky}}
+\end{equation}
+
+where \emph{k} = \emph{cs}, \emph{ts}, \emph{is} or \emph{os}. The integral is evaluated as a double summation:
+
+\begin{equation}
+{E_{h,k}} = \sum\limits_{i = 1}^{{N_\theta }} {\sum\limits_{j = 1}^{{N_\phi }} {{\psi_k}\left( {{\theta_{sky}}(i),{\phi_{sky}}(j)} \right)} } \sin {\phi_{sky}}(j)\cos {\phi_{sky}}(j)\Delta {\theta_{sky}}\Delta {\phi_{sky}}
+\end{equation}
+
+where
+
+\begin{equation}
+\begin{array}{l}
+    \theta_{sky}(i) = (i - 1/2) \Delta \theta_{sky} \\
+    \phi_{sky}(j) = (j - 1/2) \Delta \phi_{sky} \\
+    \Delta \theta_{sky} = 2 \pi / N_{\theta} \\
+    \Delta \phi_{sky} = \pi / 2N_{\phi} 
+\end{array}
+\end{equation}
+
+\({N_\theta } = 18\) ~and \({N_\phi } = 8\) ~were found to give a \(\pm 1\%\) accuracy in the calculation of \({E_h}_{,k}\) .
+
+\subsection{Direct Component of Interior Daylight Illuminance}\label{direct-component-of-interior-daylight-illuminance}
+
+The direct daylight illuminance at a reference point from a particular window is determined by dividing the window into an x-y grid and finding the flux reaching the reference point from each grid element. The geometry involved is shown in Figure~\ref{fig:geometry-for-calculation-of-direct-component}. The horizontal illuminance at the reference point, \({\vec R_{ref}}\) , due to a window element is
+
+\begin{equation}
+d{E_h} = {L_w}d\Omega \cos \gamma
+\end{equation}
+
+where \emph{L\(_{w}\)} is the luminance of the window element as seen from the reference point.
+
+The subtended solid angle is approximated by
+
+\begin{equation}
+d\Omega  = \frac{{dxdy}}{{{D^2}}}\cos B
+\end{equation}
+
+where
+
+\begin{equation}
+D = \left| {{{\bar R}_{win}} - {{\bar R}_{ref}}} \right|
+\end{equation}
+
+\emph{CosB} is found from
+
+\begin{equation}
+\cos B = {\hat R_{ray}} \cdot {\hat W_n}
+\end{equation}
+
+where
+
+\begin{equation}
+{\vec R_{ray}} = ({\vec R_{win}} - {\vec R_{ref}})/D
+\end{equation}
+
+\begin{equation}
+{\hat W_n} = {\rm{ window outward normal }} = {\hat W_{21}} \times {\hat W_{23}} = \frac{{{{\vec W}_1} - {{\vec W}_2}}}{{\left| {{{\vec W}_1} - {{\vec W}_2}} \right|}} \times \frac{{{{\vec W}_3} - {{\vec W}_2}}}{{\left| {{{\vec W}_3} - {{\vec W}_2}} \right|}}
+\end{equation}
+
+Equation becomes exact as \(dx/D\) and \(dy/D \to 0\) and is accurate to better than about 1\% for \(dx \le D/4\) and \(dy \le D/4\) .
+
+The net illuminance from the window is obtained by summing the contributions from all the window elements:
+
+\begin{equation}
+{E_h} = \sum\limits_{\scriptstyle \substack{window \\ elements}} {{L_w}d\Omega \cos \gamma }
+\end{equation}
+
+In performing the summation, window elements that lie below the workplane (\(\cos \gamma < 0\) ) are omitted since light from these elements cannot reach the workplane directly.
+
+\begin{figure}[hbtp] % fig 58
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image755.png}
+\caption{Geometry for calculation of direct component of daylight illuminance at a reference point. Vectors R\(_ref\), W\(_1\), W\(_2\), W\(_3\) and R\(_win\) are in the building coordinate system. \protect \label{fig:geometry-for-calculation-of-direct-component}}
+\end{figure}
+
+\subsubsection{Unshaded Window}\label{unshaded-window}
+
+For the unshaded window case, the luminance of the window element is found by projecting the ray from reference point to window element and determining whether it intersects the sky or an exterior obstruction such as an overhang. If \emph{L} is the corresponding luminance of the sky or obstruction, the window luminance is
+
+\begin{equation}
+{L_w} = L{\tau_{vis}}
+\end{equation}
+
+where \({\tau_{vis}}\) is the visible transmittance of the glass for incidence angle \emph{B}.
+
+Exterior obstructions are generally opaque (like fins, overhangs, neighboring buildings, and the building's own wall and roof surfaces) but can be transmitting (like a tree or translucent awning). Exterior obstructions are assumed to be non-reflecting. If \emph{L\(_{sky}\)} is the sky luminance and \emph{$\tau$\(_{obs}\)} is the transmittance of the obstruction (assumed independent of incidence angle), then \(L = L_{sky} \tau_{obs}\). Interior obstructions are assumed to be opaque ($\tau$\(_{obs}\) = 0).
+
+\subsubsection{Shaded Window}\label{shaded-window}
+
+For the window-plus-shade case the shade is assumed to be a perfect diffuser, i.e., the luminance of the shade is independent of angle of emission of light, position on shade, and angle of incidence of solar radiation falling on the shade. Closely-woven drapery fabric and translucent roller shades are closer to being perfect diffusers than Venetian blinds or other slatted devices, which usually have non-uniform luminance characteristics.
+
+The calculation of the window luminance with the shade in place, \emph{L\(_{w,sh}\)}, is described in {[}Winkelmann, 1983{]}. The illuminance contribution at the reference point from a shaded window element is then given by Eq. (152) with \({L_w} = {L_{w,sh}}\) .
+
+\subsection{Internally-Reflected Component of Interior Daylight Illuminance}\label{internally-reflected-component-of-interior-daylight-illuminance}
+
+Daylight reaching a reference point after reflection from interior surfaces is calculated using the \emph{split-flux} method {[}Hopkinson et al., 1954{]}, {[}Lynes, 1968{]}. In this method the daylight transmitted by the window is split into two parts---a downward-going flux, \({\Phi_{FW}}\) (lumens), which falls on the floor and portions of the walls below the imaginary horizontal plane passing through the center of the window (\emph{window midplane}), and an upward-going flux, \({\Phi_{CW}}\) , that strikes the ceiling and portions of the walls above the window midplane. A fraction of these fluxes is absorbed by the room surfaces. The remainder, the first-reflected flux, \emph{F\(_{1}\)}, is approximated by
+
+\begin{equation}
+{F_1} = {\Phi_{FW}}{\rho_{FW}} + {\Phi_{CW}}{\rho_{CW}}
+\end{equation}
+
+where \emph{$\rho$\(_{FW}\)} is the area-weighted average reflectance of the floor and those parts of the walls below the window midplane, and \emph{$\rho$\(_{CW}\)} is the area-weighted average reflectance of the ceiling and those parts of the walls above the window midplane.
+
+To find the final average internally-reflected illuminance, \emph{E\(_{r}\)}, on the room surfaces (which in this method is uniform throughout the room) a flux balance is used. The total reflected flux absorbed by the room surfaces (or lost through the windows) is \emph{AE\(_{r}\)(1-$\rho$)}, where \emph{A} is the total inside surface area of the floor, walls, ceiling and windows in the room, and \emph{$\rho$} is the area-weighted average reflectance of the room surfaces, including windows. From conservation of energy
+
+\begin{equation}
+A{E_r}(1 - \rho ) = {F_1}
+\end{equation}
+
+or
+
+\begin{equation}
+{E_r} = \frac{{{\Phi_{FW}}{\rho_{FW}} + {\Phi_{CW}}{\rho_{CW}}}}{{A(1 - \rho )}}
+\end{equation}
+
+This procedure assumes that the room behaves like an integrating sphere with perfectly diffusing interior surfaces and with no internal obstructions. It therefore works best for rooms that are close to cubical in shape, have matte surfaces (which is usually the case), and have no internal partitions. Deviations from these conditions, such as would be the case for rooms whose depth measured from the window-wall is more than three times greater than ceiling height, can lead to substantial inaccuracies in the split-flux calculation.
+
+\subsection{Transmitted Flux from Sky and Ground}\label{transmitted-flux-from-sky-and-ground}
+
+The luminous flux incident on the center of the window from a luminous element of sky or ground at angular position \((\theta ,\phi )\) , of luminance \(L(\theta ,\phi )\) , and subtending a solid angle \(\cos \phi d\theta d\phi\) ~is
+
+\begin{equation}
+d{\Phi_{inc}} = {A_w}L(\theta ,\phi )\cos \beta \cos \phi d\theta d\phi
+\end{equation}
+
+The transmitted flux is
+
+\begin{equation}
+d\Phi  = d{\Phi_{inc}}T(\beta )
+\end{equation}
+
+where \emph{T($\beta$)} is the window transmittance for light at incidence angle \emph{$\beta$}. This transmittance depends on whether or not the window has a shade.
+
+For an unshaded window the total downgoing transmitted flux is obtained by integrating over the part of the exterior hemisphere seen by the window that lies above the window midplane. This gives
+
+\begin{equation}
+{\Phi_{FW,unshaded}} = {A_w}\int\limits_{{\theta_{\min }}}^{{\theta_{\max }}} {\int\limits_0^{\pi /2} {L(\theta ,\phi )T(\beta )\cos \beta \cos \phi d\theta d\phi } }
+\end{equation}
+
+The upgoing flux is obtained similarly by integrating over the part of the exterior hemisphere that lies below the window midplane:
+
+\begin{equation}
+{\Phi_{CW,unshaded}} = {A_w}\int\limits_{{\theta_{\min }}}^{{\theta_{\max }}} {\int\limits_{\pi /2 - {\phi_w}}^0 {L(\theta ,\phi )T(\beta )\cos \beta \cos \phi d\theta d\phi } }
+\end{equation}
+
+where \({\phi_w}\) is the angle the window outward normal makes with the horizontal plane.
+
+For a window with a diffusing shade the total transmitted flux is
+
+\begin{equation}
+{\Phi_{sh}} = {A_w}\int\limits_{{\theta_{\min }}}^{{\theta_{\max }}} {\int\limits_{\pi /2 - {\phi_w}}^{\pi /2} {L(\theta ,\phi )T(\beta )\cos \beta \cos \phi d\theta d\phi } }
+\end{equation}
+
+The downgoing and upgoing portions of this flux are
+
+\begin{equation}
+\begin{array}{l}
+    \Phi_{FW,sh} = \Phi (1 - f) \\
+    \Phi_{CW,sh} = \Phi f
+\end{array}
+\end{equation}
+
+where \emph{f}, the fraction of the hemisphere seen by the inside of the window that lies above the window midplane, is given by
+
+\begin{equation}
+f = 0.5 - {\phi_w}/\pi
+\end{equation}
+
+For a vertical window (\({\phi_w} = 0\) ) the up- and down-going transmitted fluxes are equal:
+
+\({\Phi_{FW,sh}} = {\Phi_{CW,sh}} = \Phi /2\) .
+
+For a horizontal skylight (\({\phi_w} = \pi /2\) ):
+
+\begin{equation}
+{\Phi_{FW,sh}} = \Phi ,{\Phi_{CW,sh}} = 0
+\end{equation}
+
+The limits of integration of \emph{θ} in Equations (153), (154) and (155) depend on \(\phi\) . From {[}Figure \# 12 - Winkelmann, 1983{]} we have
+
+\begin{equation}
+\sin \alpha  = \sin (A - \pi /2) = \frac{{\sin \phi \tan {\phi_w}}}{{\cos \phi }}
+\end{equation}
+
+which gives
+
+\begin{equation}
+A = {\cos ^{ - 1}}(\tan \phi \tan {\phi_w})
+\end{equation}
+
+Thus
+
+\begin{equation}
+\begin{array}{rl}
+    \theta_{min} & =  - \left| \cos^{-1}(-\tan\phi\tan\phi_w) \right| \\
+    \theta_{max} & = \left| \cos^{-1}(-\tan\phi\tan\phi_w) \right| 
+\end{array}
+\end{equation}
+
+\subsection{Transmitted Flux from Direct Sun}\label{transmitted-flux-from-direct-sun}
+
+The flux incident on the window from direct sun is
+
+\begin{equation}
+{\Phi_{inc}} = {A_w}{E_{DN}}\cos \beta {f_{sunlit}}
+\end{equation}
+
+The transmitted flux is
+
+\begin{equation}
+\Phi  = T(\beta ){\Phi_{inc}}
+\end{equation}
+
+where T is the net transmittance of the window glazing (plus shade, if present).
+
+For an unshaded window all of the transmitted flux is downward since the sun always lies above the window midplane. Therefore
+
+\begin{equation}
+\begin{array}{l}
+    \Phi_{FW,unsh} = \Phi \\
+    \Phi_{CW,unsh} = 0
+\end{array}
+\end{equation}
+
+For a window with a diffusing shade
+
+\begin{equation}
+  \begin{array}{rl}
+    \Phi_{FW,sh} &= \Phi (1 - f) \\
+    \Phi_{CW,sh} &= \Phi f
+  \end{array}
+\end{equation}
+
+\subsection{Luminance of Shaded Window}\label{luminance-of-shaded-window}
+
+The luminance of a shaded window is determined at the same time that the transmitted flux is calculated. It is given by
+
+\begin{equation}
+{L_{sh}} = \frac{1}{\pi }\int\limits_{{\theta_{\min }}}^{{\theta_{\max }}} {\int\limits_{\pi /2 - {\phi_w}}^{\pi /2} {L(\theta ,\phi )T(\beta )\cos \beta \cos \phi d\theta d\phi } }
+\end{equation}
+
+\subsection{Daylight Discomfort Glare}\label{daylight-discomfort-glare}
+
+The discomfort glare at a reference point due to luminance contrast between a window and the interior surfaces surrounding the window is given by {[}Hopkinson, 1970{]} and {[}Hopkinson, 1972{]}:
+
+\begin{equation}
+G = \frac{{L_w^{1.6}{\Omega ^{0.8}}}}{{{L_b} + 0.07{\omega ^{0.5}}{L_w}}}
+\end{equation}
+
+where
+
+\emph{G} = discomfort glare constant
+
+\emph{L\(_{w}\)} = average luminance of the window as seen from the reference point
+
+\emph{Ω} = solid angle subtended by window, modified to take direction of occupant view into account
+
+\emph{L\(_{b}\)} = luminance of the background area surrounding the window
+
+By dividing the window into \emph{N\(_{x}\)} by \emph{N\(_{y}\)} rectangular elements, as is done for calculating the direct component of interior illuminance, we have
+
+\begin{equation}
+{L_w} = \frac{{\sum\limits_{j = 1}^{{N_y}} {\sum\limits_{i = 1}^{{N_x}} {{L_w}(i,j)} } }}{{{N_x}{N_y}}}
+\end{equation}
+
+where \emph{L\(_{w}\)(i,j)} is the luminance of element \emph{(i,j)} as seen from the reference point.
+
+Similarly,
+
+\begin{equation}
+\omega  = \sum\limits_{j = 1}^{{N_y}} {\sum\limits_{i = 1}^{{N_x}} {d\omega (i,j)} }
+\end{equation}
+
+where \emph{d$\omega$(i,j)} is the solid angle subtended by element \emph{(i,j)} with respect to the reference point.
+
+The modified solid angle is
+
+~\(\Omega = \sum\limits_{j = 1}^{{N_y}} {\sum\limits_{i = 1}^{{N_x}} {d\omega (i,j)} } p({x_R},{y_R})\)
+
+where p is a ``position factor'' {[}Petherbridge \& Longmore, 1954{]} that accounts for the decrease in visual excitation as the luminous element moves away from the line of sight. This factor depends on the horizontal and vertical displacement ratios, \emph{x\(_{R}\)} and \emph{y\(_{R}\)} (Figure~\ref{fig:geometry-for-calculation-of-displacement}),~ given by
+
+\begin{equation}
+\begin{array}{rl}
+    x_R(i,j) & = \frac{\sqrt{A^2-(YD)^2}}{RR} \\
+    y_R(i,j) & = \left|YD/RR\right|
+\end{array}
+\end{equation}
+
+where
+
+\begin{equation}
+\begin{array}{rl}
+    RR & = D (\hat{R}_{ray}\cdot\hat{v}_{view}) \\
+    A^2 & = D^2 - (RR)^2 \\
+    YD = R_{win}(3) - R_{ref}(3)
+\end{array}
+\end{equation}
+
+\begin{figure}[hbtp] % fig 59
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image794.png}
+\caption{Geometry for calculation of displacement ratios used in the glare formula. \protect \label{fig:geometry-for-calculation-of-displacement}}
+\end{figure}
+
+The factor \emph{p} can be obtained from graphs given in {[}Petherbridge \& Longmore, 1954{]} or it can be calculated from tabulated values of \emph{p\(_{H}\)}, the Hopkinson position factor {[}Hopkinson, 1966{]}, since \(p = p_H^{1.25}\) . The values resulting from the latter approach are given in Table~\ref{table:position-factor-for-glare-calculation}. Interpolation of this table is used in EnergyPlus to evaluate \emph{p} at intermediate values of \emph{x\(_{R}\)} and \emph{y\(_{R}\)}.
+
+% table 26
+\begin{longtable}[c]{p{1.0in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}}
+\caption{Position factor for glare calculation \label{table:position-factor-for-glare-calculation}} \tabularnewline
+\toprule 
+            &      & \multicolumn{8}{l}{$x_R$: Horizontal Displacement Factor} \tabularnewline
+\cmidrule(r){2-9}
+\endfirsthead
+
+\caption[]{Position factor for glare calculation} \tabularnewline
+\toprule
+            &      &\multicolumn{8}{l}{$x_R$: Horizontal Displacement Factor} \tabularnewline
+\cmidrule(r){2-9}
+\endhead
+
+            &      & \textbf{0}     & \textbf{0.5}   & \textbf{1.0}   & \textbf{1.5}   & \textbf{2.0}   & \textbf{2.5}   & \textbf{3.0}   & \textbf{>3.0} \tabularnewline
+\textbf{$y_R$:}      & \textbf{0}    & 1.00  & 0.492 & 0.226 & 0.128 & 0.081 & 0.061 & 0.057 & 0 \tabularnewline
+\textbf{Vertical}    & \textbf{0.5}  & 0.123 & 0.119 & 0.065 & 0.043 & 0.029 & 0.026 & 0.023 & 0 \tabularnewline
+\textbf{Displacement}  & \textbf{1.0}  & 0.019 & 0.026 & 0.019 & 0.016 & 0.014 & 0.011 & 0.011 & 0 \tabularnewline
+\textbf{Factor}      & \textbf{1.5}  & 0.008 & 0.008 & 0.008 & 0.008 & 0.008 & 0.006 & 0.006 & 0 \tabularnewline
+            & \textbf{2.0}  & 0     & 0     & 0.003 & 0.003 & 0.003 & 0.003 & 0.003 & 0 \tabularnewline
+            & \textbf{>2.0} & 0     & 0     & 0     & 0     & 0     & 0     & 0     & 0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The background luminance is
+
+\begin{equation}
+{L_b} = {E_b}{\rho_b}
+\end{equation}
+
+where \emph{$\rho$\(_{b}\)} is approximated by the average interior surface reflectance of the entire room and
+
+\begin{equation}
+{E_b} = \max ({E_r},{E_s})
+\end{equation}
+
+where \emph{E\(_{r}\)}is the total internally-reflected component of daylight illuminance produced by all the windows in the room and \emph{E\(_{s}\)} is the illuminance setpoint at the reference point at which glare is being calculated. A precise calculation of \emph{E\(_{b}\)} is not required since the glare index (see next section) is logarithmic. A factor of two variation in \emph{E\(_{b}\)} generally produces a change of only 0.5 to 1.0 in the glare index.
+
+\subsubsection{Glare Index}\label{glare-index}
+
+The net daylight glare at a reference point due to all of the windows in a room is expressed in terms of a \emph{glare index} given by
+
+\begin{equation}
+{G_I} = 10{\log_{10}}\sum\limits_{i = 1}^{\scriptstyle \substack{number of \\ windows}} {{{\rm{G}}_{\rm{i}}}}
+\end{equation}
+
+where \emph{G\(_{i}\)} is the glare constant at the reference point due to the \emph{i\(^{th}\)} window
diff --git a/doc/engineering-reference/src/daylighting-and-window-calculations/daylighting-calculations.tex b/doc/engineering-reference/src/daylighting-and-window-calculations/daylighting-calculations.tex
new file mode 100644
index 00000000000..c47a5c0c63e
--- /dev/null
+++ b/doc/engineering-reference/src/daylighting-and-window-calculations/daylighting-calculations.tex
@@ -0,0 +1,13 @@
+\section{Daylighting Calculations}\label{daylighting-calculations}
+
+The EnergyPlus daylighting model, in conjunction with the thermal analysis, determines the energy impact of daylighting strategies based on analysis of daylight availability, site conditions, window management in response to solar gain and glare, and various lighting control strategies.
+
+The daylighting calculation has three main steps:
+
+1.~~~~\emph{Daylight factors}, which are ratios of interior illuminance or luminance to exterior horizontal illuminance, are calculated and stored. The user specifies the coordinates of one or two reference points in each daylit zone. EnergyPlus then integrates over the area of each exterior window in the zone to obtain the contribution of direct light from the window to the illuminance at the reference points, and the contribution of light that reflects from the walls, floor and ceiling before reaching the reference points. Window luminance and window background luminance, which are used to determine glare, are also calculated. Taken into account are such factors as sky luminance distribution, window size and orientation, glazing transmittance, inside surface reflectances, sun control devices such as movable window shades, and external obstructions. Dividing daylight illuminance or luminance by exterior illuminance yields daylight factors. These factors are calculated for the hourly sun positions on sun-paths for representative days of the run period. To avoid the spikes of daylight and glare factors calculated during some sunrise and/or sunset hours when exterior horizontal illuminance is very low, the daylight and glare factors for those hours are reset to 0.
+
+2.~~~~A daylighting calculation is performed each heat-balance time step when the sun is up. In this calculation the illuminance at the reference points in each zone is found by interpolating the stored daylight factors using the current time step's sun position and sky condition, then multiplying by the exterior horizontal illuminance. If glare control has been specified, the program will automatically deploy window shading, if available, to decrease glare below a specified comfort level. A similar option uses window shades to automatically control solar gain.
+
+3.~~~~The electric lighting control system is simulated to determine the lighting energy needed to make up the difference between the daylighting illuminance level and the design illuminance. Finally, the zone lighting electric reduction factor is passed to the thermal calculation, which uses this factor to reduce the heat gain from lights.
+
+The EnergyPlus daylighting calculation is derived from the daylighting calculation in DOE-2.1E, which is described in {[}Winkelmann, 1983{]} and {[}Winkelmann and Selkowitz, 1985{]}. There are two major differences between the two implementations: (1) In EnergyPlus daylight factors are calculated for four different sky types---clear, clear turbid, intermediate, and overcast; in DOE-2 only two sky types are used---clear and overcast. (2) In EnergyPlus the clear-sky daylight factors are calculated for hourly sun-path sun positions several times a year whereas in DOE-2 these daylight factors are calculated for a set of 20 sun positions that span the annual range of sun positions for a given geographical location.
diff --git a/doc/engineering-reference/src/daylighting-and-window-calculations/daylighting-devices.tex b/doc/engineering-reference/src/daylighting-and-window-calculations/daylighting-devices.tex
new file mode 100644
index 00000000000..2e3eb5188ab
--- /dev/null
+++ b/doc/engineering-reference/src/daylighting-and-window-calculations/daylighting-devices.tex
@@ -0,0 +1,509 @@
+\section{Daylighting Devices}\label{daylighting-devices}
+
+Daylighting devices are used to improve daylighting in a zone.~ Besides their contribution to illuminance, daylighting devices also have a thermal impact on the zone heat balance.~ As a result the simulation of daylighting devices is tightly integrated into both the daylighting model and the zone heat balance.
+
+There are two types of daylighting device in EnergyPlus:~ tubular daylighting devices and daylighting shelves.
+
+\subsection{Tubular Daylighting Devices}\label{tubular-daylighting-devices}
+
+The input object DaylightingDevice:Tubular provides a special model for fenestration components known as Tubular Daylighting Devices (TDDs), also known as tubular skylights or light pipes.~ TDDs are constructed of three components: a dome, a pipe, and a diffuser.
+
+\begin{figure}[hbtp] % fig 66
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image869.png}
+\caption{Tubular Daylighting Devices \protect \label{fig:tubular-daylighting-devices}}
+\end{figure}
+
+The dome is typically a hemisphere made of clear plastic.~ It allows daylight into the pipe while keeping exterior weather out.~ The pipe is assumed to be a smooth cylinder with a highly reflective inside surface.~ The surface is usually either bare polished metal or a special reflective sheet adhered to the inside.~ The pipe channels the daylight from the dome to the diffuser via multiple internal reflections.~ The diffuser is typically a flat frosted plastic cover.~ The diffuser evenly distributes the daylight to the zone.~ The dome/diffuser area and pipe area must be approximately equal (within 2\%) for running the simulation successfully.
+
+In EnergyPlus the TDD model includes three different, but related, phenomena:
+
+\begin{itemize}
+\item
+  Daylighting
+\item
+  Solar gains
+\item
+  Conductive/convective gains
+\end{itemize}
+
+Solar gains and conductive/convective gains are simulated by the zone heat balance.~ Daylighting is simulated independently.
+
+For both daylighting and heat balance simulations, the dome and diffuser are treated as special window surfaces to take advantage of many of the standard daylighting and heat transfer routines.~ Together the dome and diffuser become ``receiver'' and ``transmitter'', i.e.~radiation entering the dome ends up exiting the diffuser.
+
+\begin{figure}[hbtp] % fig 67
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image870.png}
+\caption{Dome and Diffuser Surfaces \protect \label{fig:dome-and-diffuser-surfaces}}
+\end{figure}
+
+The pipe is simulated by a separate code module.~ While several different measures for characterizing TDD performance are in use (Zhang 2002; Harrison 1998), the total transmittance of the TDD is most compatible with the EnergyPlus daylighting and heat balance code.~ Calculation of the transmittance of the pipe and the TDD for different types of radiation is fundamental to all phenomena covered by the model.
+
+\subsubsection{Pipe Beam Transmittance}\label{pipe-beam-transmittance}
+
+The transmittance of beam radiation is derived from the integration of the transmittance of many discrete rays.~ The transmittance of a discrete ray through a pipe is dependent on the reflectivity of the inside pipe surface, the aspect ratio of the pipe, the incident angle of the ray, and the point of entry into the pipe.
+
+\begin{figure}[hbtp] % fig 68
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image871.png}
+\caption{Discrete Ray in a Pipe \protect \label{fig:discrete-ray-in-a-pipe}}
+\end{figure}
+
+For an opaque surface, the reflectivity is:
+
+\begin{equation}
+\rho  = 1 - \alpha
+\end{equation}
+
+where a = surface absorptivity.~ Visible (i.e.~daylighting) and solar absorptivities give visible and solar reflectivities, respectively.~ Measured reflectivities for commercial TDDs range from 0.90 to 0.99.~ Although the actual surface reflectivity is slightly dependent on the incident angle, the model assumes a constant reflectivity for all angles.
+
+The full analytical expression for the transmittance of a beam of light in a highly reflective pipe has been developed by Swift and Smith and verified by experiment (1994).~ By integrating over all rays incident on the pipe entrance, they find the transmittance of a beam of collimated radiation to be:
+
+\begin{equation}
+\tau  = \frac{4}{\pi }\int_{s = 0}^1 {\frac{{{s^2}}}{{\sqrt {1 - {s^2}} }}} {\rho ^{INT\left[ {a\tan \theta /s} \right]}}\left( {1 - \left( {1 - \rho } \right)\left( {a\tan \theta /s - INT\left[ {a\tan \theta /s} \right]} \right)} \right)ds
+\end{equation}
+
+where
+
+a = L/D, the aspect ratio of the TDD
+
+r = surface reflectivity
+
+q = incident angle
+
+s = entry point
+
+This integral does not have an analytical solution and must be calculated numerically.~ It was found that a large number of points (100,000) were necessary to achieve an acceptable accuracy.~ Since the integration is time consuming and the transmittance of the pipe must be utilized many times at every time step, values are calculated over a range of incident angles and stored in a table.~ The tabulated values are interpolated to rapidly give the transmittance at any incident angle.~ A polynomial fit was also considered but it was found that interpolation gave superior results.
+
+In the graph below, interpolated values from EnergyPlus are compared to the results of ray tracing simulations performed at the Florida Solar Energy Center for an incident angle of 30 degrees (McCluney 2003).
+
+\begin{figure}[hbtp] % fig 69
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image874.png}
+\caption{Pipe Transmittance Comparison. \protect \label{fig:pipe-transmittance-comparison.}}
+\end{figure}
+
+During initialization of each unique TDD, the program integrates and tabulates values for the visible and solar transmittance of the pipe.~ The results are subsequently used in the daylighting simulation and heat balance simulation respectively.
+
+The effect of bends in the pipe on beam transmittance is not included in this model.~ Recent research (Zhang 2002) has suggested that a 30 degree bend has a 20\% loss in transmitted light.~ If the effect of bends must be simulated, it can be approximated by the user by appropriately decreasing the transmittance of the diffuser material.
+
+\subsubsection{TDD Beam Transmittance}\label{tdd-beam-transmittance}
+
+The beam transmittance of the TDD takes into account the dome and diffuser transmittances in addition to the pipe transmittance.
+
+\begin{equation}
+{\tau_{TDD}}(\theta ) = {\tau_{dome}}(\theta ){\tau_{pipe}}(\theta ){\tau_{diffuser}}
+\end{equation}
+
+where
+
+\(\tau_{dome}\)(q) = beam transmittance of the dome glazing at the incident angle
+
+\(\tau_{pipe}\)(q) = beam transmittance of the pipe at the incident angle, as described above
+
+\(\tau_{diffuser}\) = diffuse transmittance of the diffuser glazing
+
+The dome transmittance is calculated for a flat window.~ The model does not take into account refraction due to the curvature of the dome surface.
+
+Diffuse transmittance is always assumed for the diffuser because multiple internal reflections in the pipe scatter the beam with a diffusing effect.~ Although the light exiting the pipe is not isotropic, it can be approximated as diffuse.~ The use of a frosted diffuser on the TDD, however, ensures that the light delivered to the zone is very close to isotropic diffuse.
+
+The calculation of TDD diffuse transmittance is considerably more complex and is handled differently in the daylighting simulation and the heat balance simulation.~ The details are discussed in the following sections.
+
+\subsubsection{Daylighting}\label{daylighting}
+
+The daylighting simulation of the TDD treats the diffuser surface as a regular window illuminated from the outside by sun, sky, and ground.~ However, the TDD model replaces the window glazing transmittance with the appropriate TDD transmittance and converts all transmitted light to diffuse.
+
+The illuminance due to the direct beam of the sun is found using the TDD beam transmittance t\(_{TDD}\)(q) as described above.~ The incident angle q is relative to the dome surface.
+
+The illuminance due to sky radiation and ground reflected radiation is calculated with the normal daylighting model integration over the sky and ground within the viewable hemisphere of the dome.~ The transmittance of each sky or ground~ element is also found using the TDD beam transmittance at the incident angle of the sky or ground element relative to the dome.
+
+Light from the diffuser is converted to diffuse inside the zone in the same way as an interior shade.
+
+\subsubsection{Solar Gains}\label{solar-gains}
+
+Solar radiation incident on a window is calculated separately as sun, sky, and ground radiation.~ A different transmittance must be applied for each type of radiation.
+
+For beam radiation the TDD beam transmittance t\(_{TDD}\)(q) for the solar spectrum is used as described above.~ For sky and ground radiation a diffuse transmittance for the TDD must be developed.
+
+The transmittance of diffuse radiation can be defined as the total transmitted flux divided by the total incident flux.
+
+\begin{equation}
+{\tau_{diff}} = \frac{{\sum {{I_{trans}}} }}{{\sum {{I_{inc}}} }}
+\end{equation}
+
+Swift and Smith (1994) suggest a weighted integral of the beam transmittance over the hemisphere for an arbitrary angular distribution:
+
+\begin{equation}
+{\tau_{diff}} = \frac{{\int_{\theta  = 0}^{\pi /2} {\tau (\theta )P(\theta )} \sin \theta d\theta }}{{\int_{\theta  = 0}^{\pi /2} {P(\theta )} \sin \theta d\theta }}
+\end{equation}
+
+where
+
+P(q) = angular distribution function
+
+For isotropic diffuse radiation P(q) is the cosine of the incident angle q.
+
+\begin{equation}
+{\tau_{diff,iso}} = \frac{{\int_{\theta  = 0}^{\pi /2} {\tau (\theta )\cos \theta } \sin \theta d\theta }}{{\int_{\theta  = 0}^{\pi /2} {\cos \theta } \sin \theta d\theta }}
+\end{equation}
+
+For a given pipe or TDD, t\(_{diff,iso}\) is a constant.~ The program calculates t\(_{diff,iso}\) once during initialization using a numerical integration.
+
+The diffuse isotropic transmittance is useful, but not sufficient, for determining the transmittance of sky radiation.~ As described in the \emph{Sky Radiance Model} section, sky radiation has an anisotropic distribution modeled as the superposition of three simple distributions: a diffuse isotropic background, a circumsolar brightening near the sun, and a horizon brightening.~ While the daylighting model is capable of calculating the luminance of any position in the sky, the solar code only calculates the ultimate irradiance on a surface.~ For this reason it is not possible to integrate over an angular distribution function for sky radiance.~ Instead the three sky distributions must be handled piecewise.
+
+\begin{equation}
+{\tau_{diff,aniso}} = \frac{{\sum {{I_{trans,aniso}}} }}{{\sum {{I_{inc,aniso}}} }} = \frac{{{I_{trans,iso}} + {I_{trans,circumsolar}} + {I_{trans,horiz}}}}{{{I_{inc,iso}} + {I_{inc,circumsolar}} + {I_{inc,horiz}}}}
+\end{equation}
+
+Substituting in the appropriate transmittances:
+
+\begin{equation}
+{\tau_{diff,aniso}} = \frac{{{\tau_{diff,iso}}{I_{inc,iso}} + \tau (\theta ){I_{inc,circumsolar}} + {\tau_{diff,horiz}}{I_{inc,horiz}}}}{{{I_{inc,iso}} + {I_{inc,circumsolar}} + {I_{inc,horiz}}}}
+\end{equation}
+
+where
+
+\(\tau_{diff,iso}\) = diffuse isotropic transmittance
+
+t(q) = beam transmittance at incident angle q of sun
+
+\(\tau_{diff,horiz}\) = diffuse transmittance of the horizon, derived below
+
+It is important to note that transmittances above are for the total TDD.~ The transmittance of the dome and diffuser must be included to account for their angular dependences as well.
+
+The beam transmittance is used as an approximation for all circumsolar radiation.
+
+The diffuse horizon transmittance is found by integrating the beam transmittance over the arc of the horizon.
+
+\begin{equation}
+{\tau_{diff,horiz}} = \frac{{\sum {{I_{trans,horiz}}} }}{{\sum {{I_{inc,horiz}}} }} = \frac{{\int_{\theta  =  - \pi /2}^{\pi /2} {\tau (\theta )\cos \theta d\theta } }}{{\int_{\theta  =  - \pi /2}^{\pi /2} {\cos \theta d\theta } }}
+\end{equation}
+
+Since the radiance of the horizon is isotropic, and therefore constant across the entire horizon, the actual value of the radiance cancels out.~ The result is a constant that is calculated once during initialization.
+
+Ground radiation is assumed to be isotropic diffuse.~ The transmittance of ground radiation is the diffuse isotropic transmittance.
+
+\begin{equation}
+{\tau_{diff,gnd}} = {\tau_{diff,iso}}
+\end{equation}
+
+The solar flux transmitted by a TDD due to beam, sky, and ground radiation is calculated as normal for a window but uses the respective transmittances for the TDD.
+
+\begin{equation}
+{q''_{TDD - trans,beam}} = \left( {{I_{sun}}\cos \theta } \right){f_{sunlit}}{\tau_{TDD}}(\theta )
+\end{equation}
+
+\begin{equation}
+{q''_{TDD - trans,sky}} = {I_{h,sky}}{f_{skymult}}{\tau_{TDD,diff,aniso}}
+\end{equation}
+
+\begin{equation}
+{q''_{TDD - trans,gnd}} = \left( {{I_{sun}}\cos \theta  + {I_{h,sky}}} \right){F_{sg}}{\tau_{TDD,diff,iso}}
+\end{equation}
+
+where
+
+I\(_{sun}\) = solar beam intensity of the sun
+
+I\(_{h,sky}\) = total horizontal diffuse solar radiation due to the sky
+
+q = incident angle of the beam on the dome
+
+f\(_{sunlit}\) = sunlit beam fraction of the dome area
+
+f\(_{skymult}\) = anisotropic sky view multiplier (see AnisoSkyMult)
+
+F\(_{sg}\) = view from ground to dome
+
+\(\tau_{TDD}\)(q) = TDD beam transmittance
+
+\(\tau_{TDD,diff,aniso}\) = TDD anisotropic sky transmittance
+
+\(\tau_{TDD,diff,iso}\) = TDD isotropic diffuse transmittance
+
+\subsubsection{Daylighting vs.~Solar}\label{daylighting-vs.solar}
+
+The beam transmittance of a TDD is calculated in the same way for both daylighting and solar gains.~ If the visible and solar properties (i.e.~absorptances in the input file) are the same, the reported TDD beam transmittances are equal.
+
+However, because the daylighting and solar models treat diffuse radiation differently, the TDD diffuse transmittances reported for visible and solar radiation will not necessarily be equal, even though the properties may be the same.
+
+Since the daylighting model calculates the diffuse illuminance using a sky and ground integration of many discrete elements, a visible diffuse transmittance is not required for the TDD daylighting simulation.~ For reporting purposes only, the visible diffuse transmittance is estimated concurrent with the sky and ground integration using:
+
+\begin{equation}
+{\tau_{diff}} = \frac{{\int {{\tau_{TDD}}(\theta )d{\Phi_{inc}}} }}{{\int {d{\Phi_{inc}}} }}
+\end{equation}
+
+\subsubsection{Conductive/Convective Gains}\label{conductiveconvective-gains}
+
+For conductive and convective heat gain, TDDs are treated as one entity with an effective thermal resistance (i.e.~R-value) between the outside and inside surfaces.~ The outside face temperature of the dome and the inside face temperature of the diffuser are calculated as usual by the outside and inside heat balances respectively.~ The temperatures are then copied to the inside face of the dome and the outside face of the diffuser.~ Normal exterior and interior convection and IR radiation exchange occurs for both surfaces.
+
+Although little research has been done on the thermal characteristics of TDDs, one experiment (Harrison 1998) reports an average effective thermal resistance of 0.279 m\(^{2}\) K/W for a commercial TDD measuring 0.33 m in diameter by 1.83 m in length.~ This value, however, reflects a measurement from outdoor air temperature to indoor air temperature.~ The model assumes an effective thermal resistance from outside surface temperature to inside surface temperature.
+
+Solar radiation is inevitably absorbed by the TDD before it reaches the zone.~ Every reflection in the pipe leaves behind some solar radiation according to the surface absorptance.~ Rays incident at a greater angle make more reflections and leave behind more absorbed solar in the pipe wall.
+
+The total absorbed solar radiation in the TDD is the sum of the following gains:
+
+\begin{itemize}
+\item
+  Inward bound solar absorbed by multiple pipe reflections
+\item
+  Outward bound solar absorbed by multiple pipe reflections due to:
+\item
+  Reflection off of diffuser surface (inside of TDD)
+\item
+  Zone diffuse interior shortwave incident on the diffuser from lights, etc.
+\item
+  Inward flowing absorbed solar in dome and diffuser glazing
+\end{itemize}
+
+\begin{equation}
+{Q_{abs,pipe}} = {Q_{abs,in}} + {Q_{abs,out}} + {Q_{abs,glazing}}
+\end{equation}
+
+The inward bound solar absorbed by the pipe is the difference between the solar transmitted by the dome and the solar incident on the diffuser.
+
+\begin{equation}
+{Q_{abs,in}} = {q''_{trans,dome}}{A_{dome}} - {q''_{inc,diffuser}}{A_{diffuser}}
+\end{equation}
+
+The solar transmitted by the dome q``\(_{trans,dome}\) is calculated as usual for a window.~ The solar incident on the diffuser q''\(_{inc,diffuser}\) is more complicated because each component must be treated separately.
+
+\begin{equation}
+{q''_{inc,diffuser}} = {q''_{beam}}\frac{{{\tau_{TDD,beam}}(\theta )}}{{{\tau_{diffuser}}}} + {q''_{sky}}\frac{{{\tau_{TDD,aniso}}(Hour)}}{{{\tau_{diffuser}}}} + {q''_{gnd}}\frac{{{\tau_{TDD,iso}}}}{{{\tau_{diffuser}}}}
+\end{equation}
+
+The outward bound solar absorbed by the pipe is given by:
+
+\begin{equation}
+{Q_{abs,out}} = \left( {{{q''}_{refl,diffuser}}\frac{{\left( {1 - {\tau_{TDD}}} \right)}}{{{\tau_{diffuser}}}} + {{q''}_{zoneSW}}\left( {1 - {\tau_{TDD}}} \right)} \right){A_{diffuser}}
+\end{equation}
+
+where q``\(_{zoneSW}\) is the zone interior diffuse shortwave flux from window, lights, and ambient surface reflections, and
+
+\begin{equation}
+{q''_{refl,diffuser}} = {q''_{inc,diffuser}} - {q''_{abs,diffuser}} - {q''_{trans,diffuser}}
+\end{equation}
+
+The inward flowing portion of solar absorbed in the dome and diffuser glazing is:
+
+\begin{equation}
+{Q_{abs,glazing}} = \frac{{{{q''}_{abs,dome}}{A_{dome}}}}{2} + \frac{{{{q''}_{abs,diffuser}}{A_{diffuser}}}}{2}
+\end{equation}
+
+All absorbed solar radiation in the TDD is distributed among the transition zones that the pipe passes through between dome and diffuser.~ The transition zone heat gain is proportional to the length of the zone.~ Any exterior length of pipe also receives a proportional amount of heat, but this is lost to the outside.
+
+\subsubsection{References}\label{references-016}
+
+Harrison, S. J., McCurdy, G. G., Cooke, R. 1998.~ ``Preliminary Evaluation of the Daylighting and Thermal Performance of Cylindrical Skylights'', Proceedings of International Daylight Conference, Ottawa, Canada, pp.~205-212.
+
+McCluney, R. 2003. ``Rating of Tubular Daylighting Devices for Visible Transmittance and Solar Heat Gain -- Final Report'', FSEC-CR-1385-03, January 15, 2003, Florida Solar Energy Center, 1679 Clearlake Rd., Cocoa, FL 32922.
+
+Swift, P. D., and Smith, G. B. 1995. ``Cylindrical Mirror Light Pipes'', Solar Energy Materials and Solar Cells 36, pp.~159-168.
+
+Zhang, X., Muneer, T., and Kubie, J. 2002.~ ``A Design Guide For Performance Assessment of Solar Light-Pipes'', Lighting Research \& Technology 34, 2, pp.~149-169.
+
+\subsection{Daylighting Shelves}\label{daylighting-shelves}
+
+The input object DaylightingDevice:Shelf provides a special model for light shelves used to augment daylighting.~ Light shelves are constructed from up to three components: a window, an inside shelf, and an outside shelf.~ The inside shelf acts to reflect all transmitted light from the upper window onto the ceiling of the zone as diffuse light.~ The outside shelf changes the amount of light incident on the window.~ All light reflected from the outside shelf also goes onto the zone ceiling.~ The inside shelf and outside shelf are both optional.~ However, if neither shelf is specifed, the daylighting shelf object has no effect on the simulation.
+
+The window is divided into two window surfaces: an upper window and a lower window.~ The upper window interacts with the daylighting shelf but the lower window does not, except to receive shading from the outside shelf.
+
+\begin{figure}[hbtp] % fig 70
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image893.png}
+\caption{Daylighting Shelf Diagram \protect \label{fig:daylighting-shelf-diagram}}
+\end{figure}
+
+Daylighting shelves are simulated separately for daylighting and the zone heat balance.~ The general model is similar in both cases, but the details vary.
+
+\subsubsection{Inside Shelf Daylighting}\label{inside-shelf-daylighting}
+
+The inside shelf is modeled in the daylighting simulation by converting all light transmitted by the upper window into diffuse upgoing flux.~ It is assumed that no beam or downgoing flux can pass the end of the shelf regardless of the shelf's position or orientation.
+
+In the daylighting simulation this is accomplished by forcing all the transmitted flux to be upgoing:
+
+\begin{equation}
+{\Phi_{CW}} = \Phi
+\end{equation}
+
+\begin{equation}
+{\Phi_{FW}} = 0
+\end{equation}
+
+where
+
+F\(_{CW}\) = upgoing flux
+
+F\(_{FW}\) = downgoing flux
+
+F = total flux
+
+Since it is assumed that all light falls on the inside shelf, it is implied that the upper window~ cannot contribute any direct illuminance (i.e.~the upper window cannot be seen from anywhere in the zone).~ The remaining light is entirely interreflected sky-related and interreflected sun-related upgoing flux.
+
+\subsubsection{Inside Shelf Heat Balance}\label{inside-shelf-heat-balance}
+
+In the heat balance simulation the inside shelf is defined as an interzone heat transfer surface, e.g.~partition.~ Since the inside shelf external boundary condition is required to refer to itself, the shelf is essentially equivalent to internal mass.~ Because the shelf surface has two sides that participate in the zone heat balance, the surface area is doubled by the program during initialization.~ Like internal mass, the shelf surface is allowed to interact convectively and radiatively with the zone air and other zone surfaces.
+
+The zone interior solar distribution is modified by the inside shelf.~ Regardless of the solar distribution selected in the input file, all beam solar radiation transmitted by the upper window is incident on one side (half the doubled surface area) of the shelf surface.~ The beam radiation not absorbed is reflected throughout the zone as diffuse shortwave radiation.~ The treatment of sky and ground radiation is unchanged; both are added directly to the zone diffuse shortwave.
+
+The total beam, sky, and ground radiation transmitted by the upper window does not change.
+
+\subsubsection{Outside Shelf Daylighting}\label{outside-shelf-daylighting}
+
+In the daylighting model the luminous flux transmitted by the upper window is determined by integrating over the sky and ground and summing the luminance contribution of each sky or ground element.~ The luminance of any intervening exterior or interior surfaces is assumed to be zero.~ As a shading surface, the effect of the outside shelf during the integration is to block part of the view of the ground, thereby reducing the window transmitted flux due to diffuse ground luminance.~ After the integration is complete, the program calculates the amount of diffuse light that is reflected through the window from the outside shelf and adds it as a lump sum to the upgoing flux transmitted by the window.
+
+The additional shelf upgoing flux is the sum of sun-related and sky-related flux:
+
+\begin{equation}
+{\Phi_{shelf,CW}} = {\Phi_{shelf,sun}} + {\Phi_{shelf,sky}}
+\end{equation}
+
+where
+
+\begin{equation}
+{\Phi_{shelf,sun}} = \left( {{E_{sun}}\cos \theta } \right){f_{sunlit}}{\rho_{vis}}{F_{ws}}{\tau_{diff,vis}}
+\end{equation}
+
+\begin{equation}
+{\Phi_{shelf,sky}} = {E_{h,sky}}{f_{skymult}}{\rho_{vis}}{F_{ws}}{\tau_{diff,vis}}
+\end{equation}
+
+and
+
+E\(_{sun}\) = exterior illuminance due to light from the sun
+
+E\(_{h,\,sky}\) = exterior horizontal illuminance due to light from the sky
+
+q = incident angle of the beam on the shelf
+
+f\(_{sunlit}\) = sunlit beam fraction of the shelf surface area
+
+f\(_{skymult}\) = anisotropic sky view multiplier (see AnisoSkyMult)
+
+r\(_{vis}\) = shelf surface reflectivity in the visible spectrum
+
+F\(_{ws}\) = view factor from window to shelf
+
+t\(_{diff,\, vis}\) = diffuse window transmittance in the visible spectrum
+
+The sunlit beam fraction f\(_{sunlit}\) and the anisotropic sky view multiplier f\(_{skymult}\) are borrowed from the heat balance solar calculations.
+
+The sunlit beam fraction f\(_{sunlit}\) takes into account the effect of shading due to other surfaces.~ Although shadows on the shelf surface change the luminance distribution of the shelf, there is no angular dependence because diffuse properties are assumed.~ Therefore, the flux is simply proportional to the sunlit fraction.
+
+The anisotropic sky view multiplier f\(_{skymult}\) takes into account the anisotropic distribution of sky radiation, the shelf view factor to the sky, and shading.~ This value is utilized in the heat balance simulation for solar calculations but is not currently available in the daylighting simulation.~ A value of 1.0 is assumed until a better model is developed.~ For this reason the sky-related flux may be over-predicted for some building and shelf geometries.~ However, for clear sky conditions the sun-related flux is dominant and the resulting error is small.
+
+The view factor to the outside shelf, F\(_{ws}\), if not specified by the user in the input object, is an exact view factor calculated for adjacent perpendicular rectangles.
+
+\begin{figure}[hbtp] % fig 71
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image899.png}
+\caption{Window and Outside Shelf as Adjacent Perpendicular Rectangles. \protect \label{fig:window-and-outside-shelf-as-adjacent}}
+\end{figure}
+
+For this geometry the view factor is given by (Mills 1995):
+
+\begin{equation}
+{F_{ws}} = \frac{1}{{\pi M}}\left\{ \begin{array}{l}M{\tan ^{ - 1}}\left( {\frac{1}{M}} \right) + N{\tan ^{ - 1}}\left( {\frac{1}{N}} \right) - {\left( {{M^2} + {N^2}} \right)^{1/2}}{\tan ^{ - 1}}\left( {{{\left( {{M^2} + {N^2}} \right)}^{ - 1/2}}} \right)\\ + \frac{1}{4}\ln \left[ {\left( {\frac{{\left( {1 + {M^2}} \right)\left( {1 + {N^2}} \right)}}{{1 + {M^2} + {N^2}}}} \right){{\left( {\frac{{{M^2}\left( {1 + {M^2} + {N^2}} \right)}}{{\left( {1 + {M^2}} \right)\left( {{M^2} + {N^2}} \right)}}} \right)}^{{M^2}}}{{\left( {\frac{{{N^2}\left( {1 + {M^2} + {N^2}} \right)}}{{\left( {1 + {N^2}} \right)\left( {{M^2} + {N^2}} \right)}}} \right)}^{{N^2}}}} \right]\end{array} \right\}
+\end{equation}
+
+where
+
+\begin{equation}
+M = H/W
+\end{equation}
+
+\begin{equation}
+N = L/W
+\end{equation}
+
+\subsubsection{Outside Shelf Heat Balance}\label{outside-shelf-heat-balance}
+
+The heat balance simulation does not do a sky and ground integration.~ View factors to sky and ground are used instead.~ Consequently, the heat balance calculation for the outside shelf is very similar to the daylighting calculation.~ The main difference is that the incident flux on the upper window is calculated first and reported.~ The transmitted and absorbed fractions are subsequently determined.
+
+The solar flux incident on the upper window due to the shelf is given by:
+
+\begin{equation}
+{q''_{shelf - inc}} = {q''_{shelf - inc,sun}} + {q''_{shelf - inc,sky}}
+\end{equation}
+
+where
+
+\begin{equation}
+{q''_{shelf - inc,sun}} = \left( {{I_{sun}}\cos \theta } \right){f_{sunlit}}{\rho_{sol}}{F_{ws}}
+\end{equation}
+
+\begin{equation}
+{q''_{shelf - inc,sky}} = {I_{h,sky}}{f_{skymult}}{\rho_{sol}}{F_{ws}}
+\end{equation}
+
+and
+
+I\(_{sun}\) = solar beam intensity of the sun
+
+I\(_{h,\, sky}\) = total horizontal diffuse solar radiation due to the sky
+
+q = incident angle of the beam on the shelf
+
+f\(_{sunlit}\) = sunlit beam fraction of the surface area
+
+f\(_{skymult}\) = anisotropic sky view multiplier (see AnisoSkyMult)
+
+r\(_{sol}\) = shelf surface reflectivity in the solar spectrum
+
+F\(_{ws}\) = view factor from window to shelf
+
+The view factor F\(_{ws}\) is the same as described above for daylighting.
+
+The total diffuse incident radiation due to the shelf is internally added to the ground diffuse incident radiation on the window.~ For reporting purposes the shelf radiation is included in the \emph{Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area} output variable.
+
+With the incident radiation determined, the remaining window heat balance is calculated normally.~ The resulting transmitted diffuse radiation from the sky, ground, and shelf is:
+
+\begin{equation}
+{q''_{trans}} = \left( {{{q''}_{sky - inc}} + {{q''}_{gnd - inc}} + {{q''}_{shelf - inc}}} \right){\tau_{diff,sol}}
+\end{equation}
+
+where
+
+\(\tau_{diff,\, sol}\) = diffuse window transmittance in the solar spectrum
+
+\subsubsection{References}\label{references-1-006}
+
+Mills, A. F. 1995. Heat and Mass Transfer, p.~499.
+
+\subsection{Window Light Well}\label{window-light-well}
+
+The input object DaylightingDevice:LightWell provides a model for attenuation of light transmitted by windows and skylights that can result from surrounding interior finish surfaces that form a ``light well.''~ The light well model simply attenuates the light transmitted by the exterior window.~ The model does not redirect light distributions or alter the relative mixture of diffuse and beam transmitted by the window.
+
+The attenuation is characterized by the \textbf{well efficiency}, which is the ratio of the amount of light leaving the well to the amount of light entering the well. The well efficiency varies from close to 1.0~ to close to zero if there is high attenuation. The well efficiency is used only in the EnergyPlus detailed daylighting calculation, where it multiplies the beam and diffuse light transmitted by the skylight. (The well efficiency is not used in calculating the solar gain through the skylight.)
+
+\begin{figure}[hbtp] % fig 72
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image907.png}
+\caption{Skylight with light well: (a) perspective view, (b) vertical section. If the bottom of the light well is a rectangle of side lengths c and d, as shown in (a), then the perimeter of the bottom of the well = 2(c+d) and the area = cd (see description of field names for the Light Well object). \protect \label{fig:skylight-with-light-well-a-perspective-view-b}}
+\end{figure}
+
+The well efficiency depends on the visible reflectance of well's side walls and on the well cavity ratio, \textbf{\emph{WCR}}, which is given by:
+
+\begin{equation}
+WCR = \frac{{{\rm{2}}{\rm{.5 x Well Height x Well Perimeter}}}}{{{\rm{Well Area}}}}
+\end{equation}
+
+Well Height, Well Perimeter and Well Area are inputs to the model and are discussed in the figure caption above.
+
+The model in EnergyPlus was implemented by fitting a curve to the data presented as Figure~\ref{fig:illustration-of-zone-air-mass-flow-balance}-21, ``Efficiency factors for various depths of light wells based on well-interreflectance values,'' found in the Lighting Handbook (IES 1993).~ The figure below reproduces that reference data and shows well efficiency vs.~WCR for different side wall reflectances. For use in the EnergyPlus calculation, a fit has been made to this graph that gives the following mathematical expression, where ``Reflectance'' is the user input value of the well-wall reflectance expressed as a fraction:
+
+\begin{equation}
+{\rm{Well efficiency}} = {e^{ - WCR*(0.16368 - 0.144678*{\rm{Reflectance}})}}
+\end{equation}
+
+\begin{figure}[hbtp] % fig 73
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image910.png}
+\caption{Graph showing light well efficiency vs. well cavity ratio (WCR) for well-wall visible reflectances of 80\% (upper curve), 60\% (middle curve) and 40\% (lower curve). Based on Fig. 8-21 of the Lighting Handbook: Reference and Application, 8\(^{th}\) Edition, 1993, Illuminating Engineering Society of North America. \protect \label{fig:graph-showing-light-well-efficiency-vs.-well}}
+\end{figure}
+
+The well efficiency calculated using this curve fit and user inputs is then applied to daylight transmission rates to attenuate daylight as a result of the presence of the light well,
+
+\subsubsection{References}\label{references-2-004}
+
+Lighting Handbook: Reference \& Application, 8th Edition, Illuminating Engineering Society of North America, 1993.
diff --git a/doc/engineering-reference/src/daylighting-and-window-calculations/delight-daylighting-calculations.tex b/doc/engineering-reference/src/daylighting-and-window-calculations/delight-daylighting-calculations.tex
new file mode 100644
index 00000000000..91a043a8e7e
--- /dev/null
+++ b/doc/engineering-reference/src/daylighting-and-window-calculations/delight-daylighting-calculations.tex
@@ -0,0 +1,57 @@
+\section{DElight Daylighting Calculations}\label{delight-daylighting-calculations}
+
+The Daylighting:DELight series of input objects provide an alternative daylighting model.~ The DElight method of analyzing daylighting applies to both simple apertures (i.e., windows and skylights) and complex fenestration systems that include geometrically complicated shading (e.g., roof monitors) and/or optically complicated glazings (e.g., prismatic or holographic glass).~ The DElight daylighting calculation methods are derived from the daylighting calculations in DOE-2.1E (as are the models accessed with Daylighting:Controls input object), and Superlite, with several key modifications.~ The engineering documentation included here focuses on the details of these differences from methods documented elsewhere.~ For the details of the heritage calculations, refer to the section in this documentation entitled ``Daylighting Calculations'' and to {[}Winkelmann, 1983{]}, {[}Winkelmann and Selkowitz, 1985{]}, and~ {[}Modest, 1982{]}.
+
+For each point in time, DElight calculates the interior daylighting illuminance at user specified reference points and then determines how much the electric lighting can be reduced while still achieving a combined daylighting and electric lighting illuminance target.~ The daylight illuminance level in a zone depends on many factors, including exterior light sources; location, size, and visible light transmittance of simple and complex fenestration systems; reflectance of interior surfaces; and location of reference points. The subsequent reduction of electric lighting depends on daylight illuminance level, design illuminance setpoint, fraction of zone controlled by reference point, and type of lighting control.
+
+The DElight daylighting calculation has three main steps:
+
+1.~~~~\emph{Daylight Factor Calculation:}~ Daylight factors, which are ratios of interior illuminance to exterior horizontal illuminance, are pre-calculated and stored for later use. The user spcifies the coordinates of one or more reference points in each daylit zone. DElight first calculates the contribution of light transmitted through all simple and complex fenestration systems in the zone to the illuminance at each reference point, and to the luminance at subdivided nodal patches of interior surfaces, for a given exterior luminous environment (including sky, sun, and exterior reflecting surfaces).~ The effect of inter-reflection of this initial light between interior reflecting surfaces is then calculated, resulting in a final total illuminance at each reference point.~ This total illuminace is then divided by the exterior horizontal illuminance for the given exterior environment to give a daylight factor.~ Daylight factors are calculated for each reference point, for a set of sun positions and sky conditions that are representative of the building location.
+
+2.~~~~\emph{Time-Step Interior Daylighting Calculation}:~ A daylighting calculation is performed for each heat-balance time step when the sun is up. In this calculation the illuminance at the reference points in each zone is found by interpolating the stored daylight factors using the current time step sun position and sky condition, then multiplying by the exterior horizontal illuminance.
+
+3.~~~~\emph{Electric Lighting Control Calculation}:~ The electric lighting control system is simulated to determine the proportion of lighting energy needed to make up the difference between the daylighting illuminance level at the given time step, and the design illuminance level. Finally, the zone lighting electric reduction factor is passed to the thermal calculation, which uses this factor to reduce the heat gain from lights.
+
+\subsection{DElight Daylight Factor Calculation Differences from EnergyPlus Detailed Methods}\label{delight-daylight-factor-calculation-differences-from-energyplus-detailed-methods}
+
+\begin{itemize}
+\item
+  \emph{Initial Interior Illuminance/Luminance Calculation:}~ DElight calculates the total initial contribution of light transmitted through all simple fenestration systems (i.e., windows and skylights) in the zone to the illuminance at each reference point, and to the luminance at each gridded nodal patch of interior surfaces.~ This differs from the models behind the ``Daylighting:Controls'' object (henceforth referred to as ``EnergyPlus Detailed'') in two ways. The first is that EnergyPlus Detailed calculates initial illuminace values at reference points for each pair of reference point and aperture (window/skylight) in the zone, whereas DElight calculates the total contribution from all apertures to each reference point.~ The second difference from EnergyPlus Detailed is that the initial luminance of interior surface nodal patches is calculated to support the inter-reflection calculation described below.~ This calculation uses the same formula as EnergyPlus Detailed modified for arbitrarily oriented surfaces (i.e., non-horizontal), and to calculate luminance rather than illuminance.~ Note however, DElight does not account for interior surface obstructions (e.g., partitions) in this initial interior illuminance/luminance distribution.~ The EnergyPlus Detailed method does account for interior surface obstruction of initial illuminance distribution on reference points.
+\item
+  \emph{Reference Points:}~ DElight allows up to 100 reference points to be arbitrarily positioned with a daylighting zone.~ At this time all reference points are assumed to be oriented on a horizontal virtual surface ``facing'' toward the zenith and ``seeing'' the hemisphere above the horizontal plane.
+\item
+  \emph{Complex Fenestration System Calculation:}~ DElight calculates the contribution to the initial interior illuminance at each reference point, and to the luminance at each gridded nodal patch of interior surfaces, of the light transmitted by complex fenestration systems (CFS).~ The analysis of a CFS within DElight is based on the characterization of the system using bi-directional transmittance distribution functions (BTDF), which must be either pre-calculated (e.g., using ray-tracing techniques) or pre-measured, prior to analysis by DElight.~ A BTDF is a set of data for a given CFS, which gives the ratios of incident to transmitted light for a range of incoming and outgoing directions.~ As illustrated in Figure~\ref{fig:bi-directional-transmittance-data.}, a BTDF can be thought of as collapsing a CFS to a ``black box'' that is represented geometrically as a flat two-dimensional light-transmitting surface that will be treated as an aperture surface in the daylit zone description. For each incoming direction across the exterior hemisphere of the CFS, varying portions of that light are transmitted at multiple outgoing directions across the interior hemisphere of the CFS.~ The two-dimensional CFS ``surface'' and directional hemispheres are ``abstract'' in that they may not literally correspond to actual CFS component geometric details.
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 62
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image827.png}
+\caption{Bi-Directional Transmittance Data. \protect \label{fig:bi-directional-transmittance-data.}}
+\end{figure}
+
+The pre-calculated or pre-measured BTDF for a CFS is independent of its final position and orientation within a building.~ Once a specific instance of a CFS aperture has been positioned within a building, the incident light from all exterior sources across the CFS exterior hemisphere can be integrated over all incident directions for each relevant transmitted direction to determine the light transmitted by the CFS surface in that direction. The light transmitted by the CFS aperture is then distributed to surfaces in the zone according to its non-uniform directionality.~ The algorithms for this BTDF treatment of CFS in DElight are still under development, and are subject to change in the future.
+
+\begin{itemize}
+\tightlist
+\item
+  \emph{Inter-reflected Interior Illuminance/Luminance Calculation:}~ The effect of inter-reflection of the initial interior illuminance/luminance between interior reflecting surfaces is calculated using a radiosity method derived from Superlite {[}Modest, 1982{]}.~ This method subdivides each reflecting surface in the zone into nodal patches and uses view factors between all nodal patch pairs in an iterative calculation of the total contribution of reflected light within the zone.~ This method replaces the split-flux method used in EnergyPlus Detailed, resulting in a more accurate calculation of the varied distribution of inter-reflected light throughout the zone.~ The ability to input up to 100 reference points supports a more complete assessment of this distribution.~ Also, the radiosity method explicitly accounts for interior obstructions between pairs of nodal patches.~ The split-flux method used in the EnergyPlus Detailed approach only implicitly accounts for interior surfaces by including their reflectance and surface area in the zone average surface reflectance calculations.
+\end{itemize}
+
+\subsection{DElight Time-Step Interior Daylighting Calculation Differences from EnergyPlus Detailed Methods}\label{delight-time-step-interior-daylighting-calculation-differences-from-energyplus-detailed-methods}
+
+\begin{itemize}
+\item
+  \emph{Interior Illuminance Calculation:}~ As discussed above, DElight only calculates daylight factors for the total contribution from all windows/skylights and CFS to each defined reference point.~ Thus DElight does not support dynamic control of fenestration shading during the subsequent time-step calculations, as does EnergyPlus Detailed.
+\item
+  \emph{Visual Quality:}~ DElight does not currently calculate a measure of visual quality such as glare due to daylighting.~ DElight does calculate luminance on nodal patches of all interior, reflecting surfaces.~ A variety of visual quality metrics could be calculated from these data in future implementations.
+\item
+  \emph{Electric Lighting Control Calculation:}~ Up to 100 reference points can be defined within a DElight daylighting zone.~ One or more of these reference points must be included in the control of the electric lighting system in the zone.~ Each reference point input includes the fraction of the zone controlled by that point.~ Values of 0.0 are valid, which allows the definition of reference points for which interior illuminance levels are calculated, but which do not control the electric lighting.~ Any non-zero fraction is thus the equivalent of a relative weighting given to that reference point's influence on the overall electric lighting control.~ The sum of all fractions for defined reference points must less than or equal to 1.0 for this relative weighting to make physical sense.~ If the sum is less than 1.0, the remaining fraction is assumed to have no lighting control.
+\end{itemize}
+
+\subsection{References}\label{references-017}
+
+Modest, M. 1982. A General Model for the Calculation of Daylighting in Interior Spaces, Energy and Buildings 5, 66-79, and Lawrence Berkeley Laboratory report no. LBL-12599A.
+
+Winkelmann, F.C. 1983. Daylighting Calculation in DOE-2\emph{.} Lawrence Berkeley Laboratory report no. LBL-11353, January 1983.
+
+Winkelmann, F.C. and S. Selkowitz. 1985. Daylighting Simulation in the DOE-2 Building Energy Analysis Program\emph{.} Energy and Buildings 8, 271-286.
diff --git a/doc/engineering-reference/src/daylighting-and-window-calculations/time-step-daylighting-calculation.tex b/doc/engineering-reference/src/daylighting-and-window-calculations/time-step-daylighting-calculation.tex
new file mode 100644
index 00000000000..84fb59e11a6
--- /dev/null
+++ b/doc/engineering-reference/src/daylighting-and-window-calculations/time-step-daylighting-calculation.tex
@@ -0,0 +1,334 @@
+\section{Time-Step Daylighting Calculation}\label{time-step-daylighting-calculation}
+
+\subsection{Overview}\label{overview-027}
+
+A daylighting calculation is performed each time step that the sun is up for each zone that has one or two daylighting reference points specified. The exterior horizontal illuminance from the sun and sky is determined from solar irradiance data from the weather file. The interior illuminance at each reference point is found for each window by interpolating the daylight illuminance factors for the current sun position, then, for sky-related interior illuminance, multiplying by the exterior horizontal illuminance from the appropriate sky types that time step, and, for sun-related interior illuminance, multiplying by the exterior horizontal solar illuminance that time step. By summation, the net illuminance and glare due to all of the windows in a zone are found. If glare control has been specified window shading (by movable shading devices or switchable glazing) is deployed to reduce glare. Finally the illuminance at each reference point for the final window and shade configuration is used by the lighting control system simulation to determine the electric lighting power required to meet the illuminance setpoint at each reference point.
+
+% table 27
+\begin{longtable}[c]{p{1.0in}p{2.0in}p{1.0in}p{2.0in}}
+\caption{Variables in Time-Step Calculations \label{table:variables-in-time-step-calculations}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Variables in Time-Step Calculations} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+S\(_{norm,dir}\) & Direct normal solar irradiance & W/m\(^{2}\) & BeamSolarRad \tabularnewline
+S\(_{h,dif}\) & Exterior diffuse horizontal solar irradiance & W/m\(^{2}\) & SDIFH, DifSolarRad \tabularnewline
+S\(_{h,dir}\) & Exterior direct horizontal solar irradiance & W/m\(^{2}\) & SDIRH \tabularnewline
+Z & Solar zenith angle & radians & Zeta \tabularnewline
+m & Relative optical air mass & - & AirMass \tabularnewline
+$\Delta$ & Sky brightness & - & SkyBrightness \tabularnewline
+$\varepsilon$ & Sky clearness & - & SkyClearness \tabularnewline
+k, k’ & Sky type index & - & ISky \tabularnewline
+s\(_{k,k'}\) & Interpolation factor for skies k and k’ & - & SkyWeight \tabularnewline
+$\psi$\(_{k,k'}\) & Sky luminance distribution formed from linear interpolation of skies k and k’ & cd/m\(^{2}\) & - \tabularnewline
+f\(_{k}\) & Fraction of sky that is type k & - & - \tabularnewline
+E\(_{h,k}\) & Horizontal illuminance from sky type k & cd/m\(^{2}\) & HorIllSky \tabularnewline
+E\(_{h,sky}\) & Exterior horizontal illuminance from sky & lux & HISKF \tabularnewline
+E\(_{h,sun}\) & Exterior horizontal illuminance from sun & lux & HISUNF \tabularnewline
+$\eta$\(_{dif}\), $\eta$\(_{dir}\) & Luminous efficacy of diffuse and direct solar radiation & lm/W & DiffLumEff, DirLumEff \tabularnewline
+I\(_{win}\) & Interior illuminance from a window & lux & DaylIllum \tabularnewline
+S\(_{win}\) & Window luminance & cd/m\(^{2}\) & SourceLumFromWinAtRefPt \tabularnewline
+B\(_{win}\) & Window background luminance & cd/m\(^{2}\) & BACLUM \tabularnewline
+d\(_{sun}\), d\(_{sky,k}\) & Interior illuminance factor for sun, for sky of type k & - & DaylIllFacSun, DFSUHR, DaylIllFacSky, DFSUHR \tabularnewline
+w\(_{sun}\), w\(_{sky,k}\) & Window luminance factor for sun, for sky of type k & - & DaylSourceFacSun, SFSUHR, DaylSourceFacSky, SFSKHR \tabularnewline
+b\(_{sun}\), b\(_{sky,k}\) & Window background luminance factor for sun, for sky of type k & - & DaylBackFacSun, BFSUHR, DaylBackFacSky, BFSKHR \tabularnewline
+w\(_{j}\) & Weighting factor for time step interpolation & - & WeightNow \tabularnewline
+i\(_{L}\) & Reference point index & - & IL \tabularnewline
+i\(_{S}\) & Window shade index & - & IS \tabularnewline
+I\(_{tot}\) & Total daylight illuminance at reference point & lux & DaylIllum \tabularnewline
+B\(_{tot}\), B & Total window background luminance & cd/m\(^{2}\) & BLUM \tabularnewline
+I\(_{set}\) & Illuminance setpoint & lux & ZoneDaylight\%IllumSetPoint \tabularnewline
+f\(_{L}\) & Fractional electric lighting output & - & FL \tabularnewline
+f\(_{p}\) & Fractional electric lighting input power & - & FP \tabularnewline
+N\(_{L}\) & Number of steps in a stepped control system & - & LightControlSteps \tabularnewline
+M\(_{P}\) & Lighting power multiplier & - & ZonePowerReductionFactor \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Time-Step Sky Luminance}\label{time-step-sky-luminance}
+
+The sky luminance distribution, \emph{$\psi$}, for a particular time step is expressed as a linear interpolation of two of the four standard skies --- \emph{$\psi$\(_{cs}\)}, \emph{$\psi$\(_{ts}\)} , \emph{$\psi$\(_{is}\)} and \emph{$\psi$\(_{os}\)} --- described above under ``Sky Luminance Distributions.'' The two sky types that are interpolated depend on the value of the sky clearness. The interpolation factors are a function of sky clearness and sky brightness (Perez et al., 1990). Sky clearness is given by
+
+\begin{equation}
+\varepsilon  = \frac{{\frac{{{S_{h,dif}} + {S_{norm,dir}}}}{{{S_{h,dif}}}} + \kappa {Z^3}}}{{1 + \kappa {Z^3}}}
+\end{equation}
+
+where \emph{S\(_{h,dif}\)} is the diffuse horizontal solar irradiance, \emph{S\(_{norm,dir}\)} is the direct normal solar irradiance, \emph{Z} is the solar zenith angle and \emph{$\kappa$} is a constant equal to 1.041 for \emph{Z} in radians.
+
+Sky brightness is given by
+
+\begin{equation}
+\Delta  = {S_{h,dif}}m/S_{norm,dir}^{ext}
+\end{equation}
+
+where \emph{m} is the relative optical air mass and \(S_{norm,dir}^{ext}\) is the extraterrestrial direct normal solar irradiance.
+
+If \emph{$\varepsilon$} $≤$ 1.2
+
+\begin{equation}
+{\psi_{is,os}} = {s_{is,os}}{\psi_{is}} + (1 - {s_{is,os}}){\psi_{os}}
+\end{equation}
+
+where \emph{$\psi$\(_{is}\)} is the intermediate sky luminance distribution, \emph{$\psi$\(_{os}\)} is the overcast sky luminance distribution, and
+
+\begin{equation}
+{s_{is,os}} = \min \{ 1,\max [0,(\varepsilon  - 1)/0.2,(\Delta  - 0.05)/0.4]\}
+\end{equation}
+
+If 1.2\textless{}\emph{$\varepsilon$} $≤$ 3
+
+\begin{equation}
+{\psi_{ts,is}} = {s_{ts,is}}{\psi_{ts}} + (1 - {s_{ts,is}}){\psi_{is}}
+\end{equation}
+
+where \emph{$\psi$\(_{ts}\)} is the clear turbid sky luminance distribution and
+
+\begin{equation}
+{s_{ts,is}} = (\varepsilon  - 1.2)/1.8
+\end{equation}
+
+If \emph{$\varepsilon$} \textgreater{} 3
+
+\begin{equation}
+{\psi_{cs,ts}} = {s_{cs,ts}}{\psi_{cs}} + (1 - {s_{cs,ts}}){\psi_{ts}}
+\end{equation}
+
+where \emph{$\psi$\(_{cs}\)} is the clear sky luminance distribution and
+
+\begin{equation}
+{s_{cs,ts}} = \min [1,(\varepsilon  - 3)/3]
+\end{equation}
+
+\subsection{Interior Illuminance}\label{interior-illuminance}
+
+For each time step the interior illuminance, \emph{I\(_{win}\)}, from a window is calculated as follows by multiplying daylight factors and exterior illuminance.
+
+First, the sun- and sky-related daylight illuminance factors for the time step are determined by interpolation of the hourly factors:
+
+\begin{equation}
+{\bar d_{sun}}({i_L},{i_S}) = {w_j}{d_{sun}}({i_L},{i_S},{i_h}) + (1 - {w_j}){d_{sun}}({i_L},{i_S},{i_h} + 1)
+\end{equation}
+
+\begin{equation}
+{\bar d_{sky,k}}({i_L},{i_S}) = {w_j}{d_{sky,k}}({i_L},{i_S},{i_h}) + (1 - {w_j}){d_{sky,k}}({i_L},{i_S},{i_h} + 1)
+\end{equation}
+
+where \emph{i\(_{L}\)} is the reference point index (1 or 2), \emph{i\(_{S}\)} is the window shade index (1 for unshaded window, 2 for shaded window), \emph{i\(_{h}\)} is the hour number, and \emph{k} is the sky type index. For the \emph{j\(^{th}\)} time step in an hour, the time-step interpolation weight is given by
+
+\begin{equation}
+{w_j} = 1 - \min [1,j/{N_t}]
+\end{equation}
+
+where \emph{N\(_{t}\)} is the number of~ time steps per hour.
+
+The interior illuminance from a window is calculated as
+
+\begin{equation}
+{I_{win}}({i_L},{i_S}) = {\bar d_{sun}}{E_{h,sun}} + [{\bar d_{sky,k}}({i_L},{i_S}){f_k} + {\bar d_{sky,k'}}({i_L},{i_S}){f_{k'}}]{E_{h,sky}}
+\end{equation}
+
+where \emph{E\(_{h,sun}\)} and \emph{E\(_{h,sky}\)} are the exterior horizontal illuminance from the sun and sky, respectively, and \emph{f\(_{k}\)} and \emph{f\(_{k’}\)} are the fraction of the exterior horizontal illuminance from the sky that is due to sky type \emph{k} and \emph{k'}, respectively.
+
+The horizontal illuminance from sun and sky are given by
+
+\begin{equation}
+  \begin{array}{rl}
+    E_{h,sun} & = \eta_{dir} S_{norm,dir} \cos Z \\
+    E_{h,sky} & = \eta_{dif} S_{h,dif}
+  \end{array}
+\end{equation}
+
+where \emph{Z} is the solar zenith angle,~ \emph{$\eta$\(_{dif}\)} is the luminous efficacy (in lumens/Watt) of diffuse solar radiation from the sky and \emph{$\eta$\(_{dir}\)} is the luminous efficacy of direct radiation from the sun. The efficacies are calculated from direct and global solar irradiance using a method described in (Perez et al, 1990).
+
+The fractions \emph{f\(_{k}\)} and \emph{f\(_{k’}\)} are given by
+
+\begin{equation}
+  \begin{array}{rl}
+    f_k    & = \frac{ s_{k,k'} E_{h,k} } { s_{k,k'} E_{h,k} + (1 - s_{k,k'})E_{h,k'}} \\
+    f_{k'} & = \frac{ (1 - s_{k,k'} ) E_{h,k'} } { s_{k,k'} E_{h,k} + (1 - s_{k,k'} ) E_{h,k'}}
+  \end{array}
+\end{equation}
+
+where \emph{E\(_{h,k}\)} and \emph{E\(_{h,k’}\)} are the horizontal illuminances from skies \emph{k} and \emph{k'}, respectively (see ``Exterior Horizontal Luminance,'' above), and \emph{s\(_{k,k’}\)} is the interpolation factor for skies \emph{k}and \emph{k'}(see ``Time-Step Sky Luminance,'' above).~ For example, if~ \emph{$\varepsilon$} \textgreater{} 3, \emph{k} = \emph{cs} (clear sky), \emph{k'} = \emph{ts} (clear turbid sky) and
+
+~\(s_{k,k'} = s_{cs,ts} = \min [1,(\varepsilon - 3)/3]\)
+
+Similarly, the window source luminance, \emph{S\(_{win}\)}, and window background luminance, \emph{B\(_{win}\)}, for a window are calculated from
+
+\begin{equation}
+{S_{win}}({i_L},{i_S}) = {\bar w_{sun}}{E_{h,sun}} + [{\bar w_{sky,k}}({i_L},{i_S}){f_k} + {\bar w_{sky,k'}}({i_L},{i_S}){f_{k'}}]{E_{h,sky}}
+\end{equation}
+
+\begin{equation}
+{B_{win}}({i_L},{i_S}) = {\bar b_{sun}}{E_{h,sun}} + [{\bar b_{sky,k}}({i_L},{i_S}){f_k} + {\bar b_{sky,k'}}({i_L},{i_S}){f_{k'}}]{E_{h,sky}}
+\end{equation}
+
+The total illuminance at a reference point from all of the exterior windows in a zone is
+
+\begin{equation}
+{I_{tot}}({i_L}) = \sum\limits_{\scriptstyle{\rm{windows}}\atop\scriptstyle{\rm{in zone}}} {{I_{win}}({i_s},{i_L})}
+\end{equation}
+
+where* i\(_{S}\)* = 1 if the window is unshaded and \emph{i\(_{S}\)} = 2 if the window is shaded that time step. (Before the illuminance calculation is done the window shading control will have been simulated to determine whether or not the window is shaded.)
+
+Similarly, the total background luminance is calculated:
+
+\begin{equation}
+{B_{tot}}({i_L}) = \sum\limits_{\scriptstyle{\rm{windows}}\atop\scriptstyle{\rm{in zone}}} {{B_{win}}({i_s},{i_L})}
+\end{equation}
+
+\subsection{Glare Index}\label{glare-index-000}
+
+The net glare index at each reference point is calculated as
+
+\begin{equation}
+{G_I}({i_L}) = 10{\log_{10}}\sum\limits_{\scriptstyle{\rm{windows}}\atop\scriptstyle{\rm{in zone}}} {\frac{{{S_{win}}{{({i_L},{i_S})}^{1.6}}\Omega {{({i_L})}^{0.8}}}}{{B({i_L}) + 0.07\omega {{({i_L})}^{0.5}}{S_{win}}({i_L},{i_S})}}}
+\end{equation}
+
+where
+
+\begin{equation}
+B\left( {{i_L}} \right) = max\left( {{B_{win}}\left( {{i_L}} \right),{\rho_b}{I_{set}}\left( {{i_L}} \right)} \right)
+\end{equation}
+
+In the last relationship, the background luminance is approximated as the larger of the background luminance from daylight and the average background luminance that would be produced by the electric lighting at full power if the illuminance on the room surfaces were equal to the setpoint illuminance. In a more detailed calculation, where the luminance of each room surface is separately determined, \emph{B(i\(_{L}\))} would be better approximated as an area-weighted luminance of the surfaces surrounding a window, taking into account the luminance contribution from the electric lights.
+
+\subsubsection{Glare Control Logic}\label{glare-control-logic}
+
+If glare control has been specified and the glare index at either reference point exceeds a user-specified maximum value, \emph{G\(_{I,max}\)}, then the windows in the zone are shaded one by one in attempt to bring the glare at both points below \emph{G\(_{I,max}\)}. (Each time a window is shaded the glare and illuminance at each reference point is recalculated.) The following logic is used:
+
+5)~~~If there is only one reference point, shade a window if it is unshaded and shading it decreases the glare, even if it does not decrease the glare below \emph{G\(_{I,max}\)}. Note that if a window~ has already been shaded, say to control solar gain, it will be left in the shaded state.
+
+6)~~~If there are two reference points, then:
+
+*~If glare is too high at both points, shade the window if it decreases glare at both points.
+
+\emph{~If glare is too high only at the first point, shade the window if the glare at the first point decreases, and the glare at the second point stays below}G\(_{I,max}\)*.
+
+\begin{itemize}
+\tightlist
+\item
+  If glare is too high only at the second point, shade the window if the glare at the second point decreases, and the glare at the first point stays below \emph{G\(_{I,max}\)}.
+\end{itemize}
+
+7)~~~Shades are closed in the order of window input until glare at both points is below \emph{G\(_{I,max}\)}, or until there are no more windows left to shade.
+
+\subsection{Lighting Control System Simulation}\label{lighting-control-system-simulation}
+
+Once the final daylight illuminance value at each reference point has been determined, the electric lighting control is simulated. The fractional electric lighting output, \emph{f\(_{L}\)}, required to meet the setpoint at reference point \emph{i\(_{L}\)} is given by
+
+\begin{equation}
+{f_L}({i_L}) = {\rm{max}}\left[ {0,\frac{{{I_{set}}({i_L}) - {I_{tot}}({i_L})}}{{{I_{set}}({i_L})}}} \right]
+\end{equation}
+
+Here, \emph{I\(_{set}\)} is the illuminance setpoint and \emph{I\(_{tot}\)} is the daylight illuminance at the reference point. This relationship assumes that the electric lights at full power produce an illuminance equal to \emph{I\(_{set}\)} at the reference point.
+
+The fractional electric lighting input power, \emph{f\(_{P}\)}, corresponding to \emph{f\(_{L}\)} is then calculated. The relationship between \emph{f\(_{P}\)} and \emph{f\(_{L}\)} depends on the lighting control type.
+
+\subsubsection{Continuous Dimming Control}\label{continuous-dimming-control}
+
+For a continuously-dimmable control system, it is assumed that \emph{f\(_{P}\)} is constant and equal to \emph{f\(_{P,min}\)}for \emph{f\(_{L}\)\textless{}f\(_{L,min}\)} and that f\(_{P}\) increases linearly from \emph{f\(_{P,min}\)} to 1.0 as \emph{f\(_{L}\)} increases from \emph{f\(_{L,min}\)} to 1.0 (Figure~\ref{fig:control-action-for-a-continuous-dimming}). This gives
+
+\begin{equation}
+  f_P = \left\{
+          \begin{array}{cl}
+            f_{P,min} & for: f_L < f_{L,min} \\
+            \frac{f_L + (1 - f_L)f_{P,min} - f_{L,min}}{1 - f_{L,min}} & for: f_{L,min} \le f_L \le 1
+          \end{array}
+        \right.
+\end{equation}
+
+\begin{figure}[hbtp] % fig 60
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image823.png}
+\caption{Control action for a continuous dimming system. \protect \label{fig:control-action-for-a-continuous-dimming}}
+\end{figure}
+
+\subsubsection{Continuous/Off Dimming Control}\label{continuousoff-dimming-control}
+
+A ``continuous/off'' dimming system has the same behavior as a continuous dimming system except that the lights switch off for \emph{f\(_{L}\) \textless{} f\(_{L,min}\)} rather than staying at \emph{f\(_{P,min}\)}.
+
+\subsubsection{Stepped Control}\label{stepped-control}
+
+For a stepped control system, \emph{f\(_{P}\)} takes on discrete values depending on the range of \emph{f\(_{L}\)}and the number of steps, \emph{N\(_{L}\)} (Figure~\ref{fig:stepped-lighting-control-with-three-steps.}). This gives
+
+\begin{equation}
+  f_P = \left\{
+          \begin{array}{cl}
+            0 & for: f_L = 0 \\
+            \frac{\mathop{\rm int} (N_L f_L) + 1}{N_L} & for: 0 < f_L < 1 \\
+            1 & for: f_L = 1
+          \end{array}
+         \right.
+\end{equation}
+
+If a lighting control probability,* p\(_{L}\)\emph{, is specified,} f\(_{P}\)* is set one level higher a fraction of the time equal to \emph{1-p\(_{L}\)}. Specifically, if* f\(_{P}\)* \textless{}1,* f\(_{P}\)\emph{à} f\(_{P}\)\emph{+ 1/}N\(_{L}\)* if a random number between 0 and 1 exceeds \emph{p\(_{L}\)}. This can be used to simulate the uncertainty associated with manual switching of lights.
+
+\begin{figure}[hbtp] % fig 61
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image825.png}
+\caption{Stepped lighting control with three steps. \protect \label{fig:stepped-lighting-control-with-three-steps.}}
+\end{figure}
+
+\subsubsection{Lighting Power Reduction}\label{lighting-power-reduction}
+
+Using the value of \emph{f\(_{P}\)}at each reference point and the fraction \emph{f\(_{Z}\)} of the zone controlled by the reference point, the net lighting power multiplier, \emph{M\(_{P}\)}, for the entire zone is calculated; this value multiplies the lighting power output without daylighting.
+
+\begin{equation}
+{M_P} = \sum\limits_{{i_L} = 1}^2 {{f_P}({i_L})} {f_Z}({i_L}) + \left( {1 - \sum\limits_{{i_L} = 1}^2 {} {f_Z}({i_L})} \right)
+\end{equation}
+
+In this expression, the term to the right in the parentheses corresponds to the fraction of the zone not controlled by either reference point. For this fraction the electric lighting is unaffected and the power multiplier is 1.0.
+
+\subsection{References}\label{references-045}
+
+CIE Technical Committee 4.2. 1973. Standardization of the Luminance Distribution on Clear Skies. CIE Pub. No. 22, Commission Internationale d'Eclairage, Paris.
+
+Hopkinson, R.G., J. Longmore and P. Petherbridge. 1954. An Empirical Formula for the Computation of the Indirect Component of Daylight Factors. Trans. Illum. Eng. Soc. (London) 19, 201.
+
+Hopkinson, R.G., P. Petherbridge and J. Longmore. 1966. Daylighting. Heinnemann, London, p.~322.
+
+Hopkinson, R.G. 1970. Glare from Windows. Construction Research and Development Journal 2, 98.
+
+Hopkinson, R.G. 1972. Glare from Daylighting in Buildings. Applied Ergonomics 3, 206.
+
+Kittler, R. 1965. Standardization of Outdoor Conditions for the Calculation of the Daylight Factor with Clear Skies. Proc. CIE Inter-Session Meeting on Sunlight, Newcastle-Upon-Tyne.
+
+Lynes, J.A. 1968. Principles of Natural Lighting. Applied Science Publishers, Ltd., London, p.~129.
+
+Matsuura, K. 1987. Luminance Distributions of Various Reference Skies. CIE Technical Report of TC 3-09.
+
+Moon, P. and D. Spencer. 1942. Illumination from a Nonuniform Sky. Illuminating Engineering 37, 707-726.
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+\protect\hyperlink{ux5fftnref1}{{[}1{]}} For beam incident on an exterior window we have the following: For transparent glass with no shade or blind there is only beam-to-beam transmission. For diffusing glass, or if a window shade is in place, there is only beam-to-diffuse transmission. If a window blind is in place there is beam-to-diffuse transmission, and, depending on slat angle, solar profile angle, etc., there can also be beam-to-beam transmission.
+
+\protect\hyperlink{ux5fftnref2}{{[}2{]}} See ``Beam Solar Reflection from Window Reveal Surfaces.''
+
+\protect\hyperlink{ux5fftnref3}{{[}3{]}} If Solar Distribution = FullInteriorAndExterior in the Building object, the program calculates where beam solar from exterior windows falls inside the zone. Otherwise, all beam solar is assumed to fall on the floor.
+
+\protect\hyperlink{ux5fftnref4}{{[}4{]}} For the purposes of the surface heat balance calculation, any beam solar radiation absorbed by a surface is assumed to be uniformly distributed over the surface even though in reality it is likely to be concentrated in one or more discrete patches on the surface.
+
+\protect\hyperlink{ux5fftnref5}{{[}5{]}} \emph{TBm\(_{i}\)}is zero if the window has diffusing glass or a shade. \emph{TBm\(_{i}\)} can be \textgreater{} 0 if a blind is present and the slat angle, solar profile angle, etc., are such that some beam passes between the slats.
+
+\protect\hyperlink{ux5fftnref6}{{[}6{]}} A different method from that described here is used for calculating reflections from daylighting shelves (see ``Daylighting Shelves'').
+
+\protect\hyperlink{ux5fftnref7}{{[}7{]}} The ground surface is assumed to be diffusely reflecting so there is no specular reflection from the ground. The program could be improved by adding a ground surface specular component, which could be important for snow-cover conditions.
+
+\protect\hyperlink{ux5fftnref8}{{[}8{]}} The sun positions for which the daylight factors are calculated are the same as those for which the solar shadowing calculations are done.
+
+Perez, R., P. Ineichen, R. Seals, J. Michalsky and R. Stewart. 1990. Modeling Daylight Availability and Irradiance Components from Direct and Global Irradiance. Solar Energy 44, 271-289.
+
+Petherbridge, P. and J. Longmore. 1954. Solid Angles Applied to Visual Comfort Problems. Light and Lighting 47,173.
+
+Winkelmann, F.C.~ 1983. Daylighting Calculation in DOE-2\emph{.} Lawrence Berkeley Laboratory report no. LBL-11353, January 1983.
+
+Winkelmann, F.C. and S. Selkowitz. 1985. Daylighting Simulation in the DOE-2 Building Energy Analysis Program\emph{.} Energy and Buildings 8, 271-286.
diff --git a/doc/engineering-reference/src/daylighting-and-window-calculations/window-calculation-module.tex b/doc/engineering-reference/src/daylighting-and-window-calculations/window-calculation-module.tex
new file mode 100644
index 00000000000..7ce198809c4
--- /dev/null
+++ b/doc/engineering-reference/src/daylighting-and-window-calculations/window-calculation-module.tex
@@ -0,0 +1,2880 @@
+\section{Window Calculation Module}\label{window-calculation-module}
+
+This section describes two potential modeling approaches for Windows.~ The first (layer by layer) is implemented.~ The second, simple approach, reuses the layer-by-layer approach but converts an arbitrary window performance into an equivalent single layer.
+
+The primary Window calculation is a layer-by-layer approach where windows are considered to be composed of the following components, only the first of which, glazing, is required to be present:
+
+\begin{itemize}
+\item
+  \textbf{\emph{Glazing}}, which consists of one or more plane/parallel glass layers. If there are two or more glass layers, the layers are separated by gaps filled with air or another gas. The glazing optical and thermal calculations are based on algorithms from the WINDOW 4 and WINDOW 5 programs {[}Arasteh et al., 1989{]}, {[}Finlayson et al., 1993{]}.~ Glazing layers are described using te input object WindowMaterial:Glazing.
+\item
+  \textbf{\emph{Gap}}, layers filled with air or another gas that separate glazing layers.~ Gaps are described using the input object WindowMaterial:Gas.
+\item
+  \textbf{\emph{Frame}}, which surrounds the glazing on four sides.~ Frames are described using the input object WindowProperty:FrameAndDivider.
+\item
+  \textbf{\emph{Divider}}, which consists of horizontal and/or vertical elements that divide the glazing into individual lites.
+\item
+  \textbf{\emph{Shading device}}, which is a separate layer, such as drapery, roller shade or blind, on the inside or outside of the glazing, whose purpose is to reduce solar gain, reduce heat loss (movable insulation) or control daylight glare.~ Shading layers are described using ``WindowProperty:ShadingControl'' input objects.
+\end{itemize}
+
+In the following, the description of the layer-by-layer glazing algorithms is based on material from Finlayson et al., 1993. The frame and divider thermal model, and the shading device optical and thermal models, are new to EnergyPlus.
+
+A second approch has been developed where windows are modeled in a simplified approach that requires minimal user input that is processed to develop and equivalent layer that then reuses much of the layer-by-model.~ This ``Simple Window Construction: model is described below.
+
+\subsection{Optical Properties of Glazing}\label{optical-properties-of-glazing}
+
+The solar radiation transmitted by a system of glass layers and the solar radiation absorbed in each layer depends on the solar transmittance, reflectance and absorptance properties of the individual layers. The absorbed solar radiation enters the glazing heat balance calculation that determines the inside surface temperature and, therefore, the heat gain to the zone from the glazing (see ``Window Heat Balance Calculation''). The transmitted solar radiation is absorbed by interior zone surfaces and, therefore, contributes to the zone heat balance. In addition, the visible transmittance of the glazing is an important factor in the calculation of interior daylight illuminance from the glazing.
+
+% table 28
+\begin{longtable}[c]{p{1.0in}p{2.5in}p{1.0in}p{1.5in}}
+\caption{Variables in Window Calculations \label{table:variables-in-window-calculations}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Variables in Window Calculations} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+T & Transmittance & - & - \tabularnewline
+R & Reflectance & - & - \tabularnewline
+R\(^{f}\), R\(^{b}\) & Front reflectance, back reflectance & - & - \tabularnewline
+T\(_{i,j}\) & Transmittance through glass layers i to j & - & - \tabularnewline
+T\(^{dir}_{gl}\) & Direct transmittance of glazing & - & - \tabularnewline
+R\(^{f}_{i,j}\), R\(^{b}_{i,j}\) & Front reflectance, back reflectance from glass layers i to j & - & - \tabularnewline
+R\(^{dir}_{gl,f}\), R\(^{dir}_{gl,b}\) & Direct front and back reflectance of glazing & - & - \tabularnewline
+A\(^{f}_{i}\), A\(^{b}_{i}\) & Front~ absorptance, back absorptance of layer i & - & - \tabularnewline
+N & Number of glass layers & - & Nlayer \tabularnewline
+$\lambda$ & Wavelength & microns & Wle \tabularnewline
+E\(_{s}\) ($\lambda$) & Solar spectral irradiance function & W/m\(^{2}\)-micron & E \tabularnewline
+V($\lambda$) & Photopic response function of the eye & - & y30 \tabularnewline
+$\varphi$ & Angle of incidence (angle between surface normal and direction of incident beam radiation) & Rad & Phi \tabularnewline
+$\tau$ & Transmittivity or transmittance & - & tf0 \tabularnewline
+$\rho$ & Reflectivity or reflectance & - & rf0, rb0 \tabularnewline
+$\alpha$ & Spectral absorption coefficient & m\(^{-1}\) & - \tabularnewline
+d & Glass thickness & M & Material\%Thickness \tabularnewline
+n & Index of refraction & - & ngf, ngb \tabularnewline
+$\kappa$ & Extinction coefficient & - & - \tabularnewline
+$\beta$ & Intermediate variable & - & betaf, betab \tabularnewline
+P, p & A general property, such as transmittance & - & - \tabularnewline
+$\tau$\(_{sh}\) & Shade transmittance & - & Material\%Trans \tabularnewline
+$\rho$\(_{sh}\) & Shade reflectance & - & Material\%ReflectShade \tabularnewline
+$\alpha$\(_{sh}\) & Shade absorptance & - & Material\%AbsorpSolar \tabularnewline
+$\tau$\(_{bl}\) $\rho$\(_{bl}\) $\alpha$\(_{bl}\) & Blind transmittance, reflectance, absorptance & - & - \tabularnewline
+Q, G, J & Source, irradiance and radiosity for blind optical properties calculation & W/m\(^{2}\) & - \tabularnewline
+F\(_{ij}\) & View factor between segments i and j & - & - \tabularnewline
+f\(_{switch}\) & Switching factor & - & SwitchFac \tabularnewline
+T & Transmittance & - & - \tabularnewline
+R & Reflectance & - & - \tabularnewline
+R\(^f\), R\(^b\) & Front reflectance, back reflectance & - & - \tabularnewline
+T\(_{i,j}\) & Transmittance through glass layers i to j & - & - \tabularnewline
+R\(^f_{i,j}\), R\(^b_{i,j}\) & Front reflectance, back reflectance from glass layers i to j & - & - \tabularnewline
+A\(^f_i\), A\(^b_i\) & Front~ absorptance, back absorptance of layer i & - & - \tabularnewline
+N & Number of glass layers & - & Nlayer \tabularnewline
+\(\lambda\) & Wavelength & microns & Wle \tabularnewline
+E\(_s (\lambda)\) & Solar spectral irradiance function & W/m\(^2\)-micron & E \tabularnewline
+R($\lambda$) & Photopic response function of the eye & - & y30 \tabularnewline
+$\varphi$' & Relative azimuth angle (angle between screen surface normal and vertical plane through sun, Ref. Figure 87) & Rad & SunAzimuthToScreenNormal \tabularnewline
+$\alpha$' & Relative altitude angle (angle between screen surface horizontal normal plane and direction of incident beam radiation, Ref. Figure 87) & Rad & SunAltitudeToScreenNormal \tabularnewline
+$\rho$\(_{sc}\) & Beam-to-diffuse solar reflectance of screen material & - & Screens\%ReflectCylinder \tabularnewline
+$\gamma$ & Screen material aspect ratio & - & Screens\%ScreenDiameterTo SpacingRatio \tabularnewline
+Α & Spectral absorption coefficient & m\(^{-1}\) & - \tabularnewline
+D & Glass thickness & M & Material\%Thickness \tabularnewline
+N & Index of refraction & - & ngf, ngb \tabularnewline
+Κ & Extinction coefficient & - & - \tabularnewline
+Î’ & Intermediate variable & - & betaf, betab \tabularnewline
+P, p & A general property, such as transmittance & - & - \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Glass Layer Properties}\label{glass-layer-properties}
+
+In EnergyPlus, the optical properties of individual glass layers are given by the following quantities at normal incidence as a function of wavelength:
+
+Transmittance, \emph{T}
+
+Front reflectance, \emph{R\(^{f}\)}
+
+Back reflectance, \emph{R\(^{b}\)}
+
+Here ``front'' refers to radiation incident on the side of the glass closest to the outside environment, and ``back'' refers to radiant incident on the side of the glass closest to the inside environment. For glazing in exterior walls, ``front'' is therefore the side closest to the outside air and ``back'' is the side closest to the zone air. For glazing in interior (i.e., interzone) walls, ``back'' is the side closest to the zone in which the wall is defined in and ``front'' is the side closest to the adjacent zone.
+
+\subsection{Glass Optical Properties Conversion}\label{glass-optical-properties-conversion}
+
+\subsubsection{Conversion from Glass Optical Properties Specified as Index of Refraction and Transmittance at Normal Incidence}\label{conversion-from-glass-optical-properties-specified-as-index-of-refraction-and-transmittance-at-normal-incidence}
+
+The optical properties of uncoated glass are sometimes specified by index of refraction, \emph{n},* * and transmittance at normal incidence, \emph{T}.
+
+The following equations show how to convert from this set of values to the transmittance and reflectance values required by Material:WindowGlass. These equations apply only to uncoated glass, and can be used to convert either spectral-average solar properties or spectral-average visible properties (in general, \emph{n} and \emph{T} are different for the solar and visible). Note that since the glass is uncoated, the front and back reflectances are the same and equal to the \emph{R} that is solved for in the following equations.
+
+Given \emph{n} and \emph{T}, find \emph{R}:
+
+\begin{equation}
+  \begin{array}{l}
+    r = \left( \frac{n - 1}{n + 1} \right)^2 \\
+    \tau  = \frac{\left[ (1 - r)^4 + 4 r^2 T^2 \right]^{1/2} - (1 - r)^2}{2 r^2 T} \\
+    R = r + \frac{(1 - r)^2 r \tau ^2}{1 - r^2 \tau ^2}
+  \end{array}
+\end{equation}
+
+\textbf{Example:}
+
+\emph{T} = 0.86156
+
+\emph{n} = 1.526
+
+\begin{equation}
+  \begin{array}{l}
+    r = \left( \frac{1.526 - 1}{1.526 + 1} \right)^2 \\
+    \tau = 0.93974 \\
+    R = 0.07846
+  \end{array}
+\end{equation}
+
+\subsection{Simple Window Model}\label{simple-window-model}
+
+EnergyPlus includes an alternate model that allows users to enter in simplified window performance indices.~ This model is accessed through the WindowMaterial:SimpleGlazingSystem input object and converts the simple indices into an equivalent single layer window.~ (In addition a special model is used to determine the angular properties of the system -- described below).~ Once the model generates the properties for the layer, the program reuses the bulk of the layer-by-layer model for subsequent calculations.~ The properties of the equivalent layer are determined using the step by step method outlined by Arasteh, Kohler, and Griffith (2009).~ The core equations are documented here.~ The reference contains additional information.
+
+The simplified window model accepts U and SHGC indices and is useful for several reasons:
+
+1)~~~Sometimes, the only thing that is known about the window are its U and SHGC;
+
+2)~~~Codes, standards, and voluntary programs are developed in these terms;
+
+3)~~~A single-layer calculation is faster than multi-layer calculations.
+
+Note: This use of U and SHGC to describe the thermal properties of windows is only appropriate for specular glazings.
+
+While it is important to include the ability to model windows with only U-value and SHGC, we note that any method to use U and SHGC alone in building simulation software will inherently be approximate.~ This is due primarily to the following factors:
+
+\begin{itemize}
+\item
+  SHGC combines directly transmitted solar radiation and radiation absorbed by the glass which flows inward.~ These have different implications for space heating/cooling.~ Different windows with the same SHGC often have different ratios of transmitted to absorbed solar radiation.
+\item
+  SHGC is determined at normal incidence; angular properties of glazings vary with number of layers, tints, coatings.~ So products which have the same SHGC, can have different angular properties.
+\item
+  Window U-factors vary with temperatures.
+\end{itemize}
+
+Thus, for modeling specific windows, we recommend using more detailed data than just the U and SHGC, if at all possible.
+
+The simplified window model determines the properties of an equivalent layer in the following steps.
+
+\subsubsection{Step 1.~ Determine glass-to-glass Resistance.}\label{step-1.-determine-glass-to-glass-resistance.}
+
+Window U-values include interior and exterior surface heat transfer coefficients.~ The resistance of the bare window product, or glass-to-glass resistance is augmented by these film coefficients so that,
+
+\begin{equation}
+\frac{1}{U} = {R_{i,w}} + {R_{o,w}} + {R_{l,w}}
+\end{equation}
+
+Where,
+
+\({R_{i,w}}\) ~is the resistance of the interior film coefficient under standard winter conditions in units of m\(^{2}\)·K/W,
+
+\({R_{o,w}}\) ~is the resistance of the exterior film coefficient under standard winter conditions in units of m\(^{2}\)·K/W, and
+
+\({R_{l,w}}\) ~is the resisance of the bare window under winter conditions (without the film coefficients) in units of m\(^{2}\)·K/W.
+
+The values for \({R_{i,w}}\) ~and \({R_{o,w}}\) ~depend on U and are calculated using the following correlations.
+
+\begin{equation}
+{R_{i,w}} = \frac{1}{{(0.359073\;Ln(U) + 6.949915)}};\quad for\quad U < 5.85
+\end{equation}
+
+\begin{equation}
+{R_{i,w}} = \frac{1}{{(1.788041\;U - 2.886625)}};\quad for\quad U \ge 5.85
+\end{equation}
+
+\begin{equation}
+{R_{o,w}} = \frac{1}{{(0.025342\;U + 29.163853)}}
+\end{equation}
+
+So that the glass-to-glass resistance is calculated using,
+
+\({R_{l,w}} = \frac{1}{U} - {R_{i,w}} - {R_{o,w}}\) .
+
+Because the window model in EnergyPlus is for flat geometries, the models are not necessarily applicable to low-performance projecting products, such as skylights with unisulated curbs.~ The model cannot support glazing systems with a U higher than 7.0 because the thermal resistance of the film coefficients alone can provide this level of performance and none of the various resistances can be negative.
+
+\subsubsection{Step 2.~ Determine Layer Thickness.}\label{step-2.-determine-layer-thickness.}
+
+The thickness of the equivalent layer in units of meters is calculated using,
+
+\begin{equation}
+  Thickness = \left\{
+                \begin{array}{cl}
+                  0.002                             & for \frac{1}{R_{l,w}} > 7.0 \\
+                  0.05914 - \frac{0.00714}{R_{l,w}} & for \frac{1}{R_{l,w}} \leq 7.0
+                \end{array}
+              \right.
+\end{equation}
+
+\subsubsection{Step 3.~ Determine Layer Thermal Conductivity}\label{step-3.-determine-layer-thermal-conductivity}
+
+The effective thermal conductivity, \({\lambda_{eff}}\) , of the equivalent layer is calculated using,
+
+\begin{equation}
+{\lambda_{eff}} = \frac{{Thickness}}{{{R_{l,w}}}}
+\end{equation}
+
+\subsubsection{Step 4.~ Determine Layer Solar Transmittance}\label{step-4.-determine-layer-solar-transmittance}
+
+The layer's solar transmittance at normal incidence, \({T_{sol}}\) , is calculated using correlations that are a function of SHGC and U-Factor.
+
+\begin{equation}
+{T_{sol}} = 0.939998\;SHG{C^2} + 0.20332\;SHGC;\quad U > 4.5;\;SHGC < 0.7206
+\end{equation}
+
+\begin{equation}
+{T_{sol}} = 1.30415SHGC - 0.30515\;;\quad U > 4.5;\;SHGC \ge 0.7206
+\end{equation}
+
+\begin{equation}
+{T_{sol}} = 0.41040\;SHGC;\quad U < 3.4;\;SHGC \le 0.15
+\end{equation}
+
+\begin{equation}
+{T_{sol}} = 0.085775\;SHG{C^2} + 0.963954\;SHGC - 0.084958\;;\;\;U < 3.4;\;SHGC > 0.15
+\end{equation}
+
+And for U-values between 3.4 and 4.5, the value for \({T_{sol}}\) ~is interpolated using results of the equations for both ranges.
+
+\subsubsection{Step 5.~ Determine Layer Solar Reflectance}\label{step-5.-determine-layer-solar-reflectance}
+
+The layer's solar reflectance is calculated by first determining the inward flowing fraction which requires values for the resistance of the inside and outside film coefficients under summer conditions, \({R_{i,s}}\) ~and \({R_{o,s}}\) respectively.~ The correlations are
+
+{\scriptsize
+\begin{equation}
+\begin{split}
+&{R_{i,s}} = \frac{1}{{\left( {29.436546\;{{\left( {SHGC - {T_{Sol}}} \right)}^3} - 21.943415{{\left( {SHGC - {T_{Sol}}} \right)}^2} + 9.945872\left( {SHGC - {T_{Sol}}} \right) + 7.426151} \right)}}; U > 4.5 \\
+&{R_{i,s}} = \frac{1}{{\left( {199.8208128\;{{\left( {SHGC - {T_{Sol}}} \right)}^3} - 90.639733{{\left( {SHGC - {T_{Sol}}} \right)}^2} + 19.737055\left( {SHGC - {T_{Sol}}} \right) + 6.766575} \right)}}; U < 3.4 \\
+&{R_{o,s}} = \frac{1}{{\left( {2.225824(SHGC - {T_{Sol}}) + 20.57708} \right)}}; U > 4.5 \\
+&{R_{o,s}} = \frac{1}{{\left( {5.763355(SHGC - {T_{Sol}}) + 20.541528} \right)}}; U < 3.4
+\end{split}
+\end{equation}}
+
+And for U-values between 3.4 and 4.5, the values are interpolated using results from both sets of equations.
+
+The inward flowing fraction, \(Fra{c_{inward}}\) , is then calculated using
+
+\begin{equation}
+Fra{c_{inward}} = \frac{{\left( {{R_{o,s}} + 0.5\,{R_{l,w}}} \right)}}{{\left( {{R_{o,s}} + {R_{l,w}} + {R_{i,s}}} \right)}}
+\end{equation}
+
+The the solar reflectances of the front face, \({R_{s,f}}\) , and back face, \({R_{s,b}}\) , are calculated using,
+
+\({R_{s,f}} = {R_{s,b}} = 1 - {T_{Sol}} - \frac{{\left( {SHGC - {T_{Sol}}} \right)}}{{Fra{c_{inward}}}}\) .
+
+The thermal absorptance, or emittance, is take as 0.84 for both the front and back and the longwave transmittance is 0.0.
+
+\subsubsection{Step 6.~ Determine Layer Visible Properties}\label{step-6.-determine-layer-visible-properties}
+
+The user has the option of entering a value for visible transmittance as one of the simple performance indices.~ If the user does not enter a value, then the visible properties are the same as the solar properties.~ If the user does enter a value then layer's visible transmittance at normal incidence, \({T_{Vis}}\) ,is set to that value.~ The visible light reflectance for the back surface is calculated using,
+
+\begin{equation}
+{R_{Vis,b}} =  - 0.7409\,T_{Vis}^3 + 1.6531\,T_{Vis}^2 - 1.2299\,{T_{Vis}} + 0.4547
+\end{equation}
+
+The visible light reflectance for the front surface is calculated using,
+
+\begin{equation}
+{R_{Vis,f}} =  - 0.0622\,T_{Vis}^3 + 0.4277\,T_{Vis}^2 - 0.4169\,{T_{Vis}} + 0.2399
+\end{equation}
+
+\subsubsection{Step 7. Determine Angular Performance}\label{step-7.-determine-angular-performance}
+
+The angular properties of windows are important because during energy modeling, the solar incidence angles are usually fairly high.~ Angles of incidence are defined as angles from the normal direction extending out from the window.~ The simple glazing system model includes a range of correlations that are selected based on the values for U and SHGC.~ These were chosen to match the types of windows likely to have such performance levels.~ The matrix of possible combinations of U and SHGC values have been mapped to set of 28 bins shown in the following figure.
+
+\begin{figure}[hbtp] % fig 74
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image947.png}
+\caption{Diagram of Transmittance and Reflectance Correlations Used based on U and SHGC \label{fig:diagram-of-transmittance-and}}
+\end{figure}
+
+There are ten different correlations, A thru J, for both transmission and reflectance.~ The correlations are used in various weighting and interpolation schemes according the figure above.~ The correlations are normalized against the performance at normal incidence.~ EnergyPlus uses these correlations to store the glazing system's angular performance at 10 degree increments and interpolates between them during simulations.~ The model equations use the cosine of the incidence angle, \(\cos (\varphi )\) , as the independent variable.~ The correlations have the form:
+
+\begin{equation}
+T\;or\;R = a\cos {(\varphi )^4} + b\cos {(\varphi )^3} + c\cos {(\varphi )^2} + d\cos (\varphi ) + e
+\end{equation}
+
+The coefficient values for a, b, c, d, and e are listed in the following tables for each of the curves.
+
+\begin{figure}[hbtp] % fig 75
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image950.png}
+\caption{Normalized Transmittance Correlations for Angular Performance \protect \label{fig:normalized-transmittance-correlations-for}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 76
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image951.png}
+\caption{Normalized Reflectanct Correlations for Angular Performance \protect \label{fig:normalized-reflectanct-correlations-for}}
+\end{figure}
+
+\subsubsection{Application Issues}\label{application-issues}
+
+EnergyPlus's normal process of running the detailed layer-by-layer model, with the equivalent layer produced by this model, creates reports (sent to the EIO file) of the overall performance indices and the properties of the equivalent layer. Both of these raise issues that may be confusing.
+
+The simplified window model does not reuse all aspects of the detailed layer-by-layer model, in that the angular solar transmission properties use a different model when the simple window model is in effect. If the user takes the material properties of an equivalent glazing layer from the simple window model and then re-enters them into just the detailed model, then the performance will not be the same because of the angular transmission model will have changed. It is not proper use of the model to re-enter the equivalent layer's properties and expect the exact level of performance.
+
+There may not be exact agreement between the performance indices echoed out and those input in the model. This is expected with the model and the result of a number of factors. For example, although input is allowed to go up to U-7 W/m\(^{2}\)∙K, the actual outcome is limited to no higher than about 5.8W/m\(^{2}\)∙K. This is because the thermal resistance to heat transfer at the surfaces is already enough resistance to provide an upper limit to the conductance of a planar surface. Sometimes there is conflict between the SHGC and the U that are not physical and compromises need to be made. In general, the simple window model is intended to generate a physically-reasonable glazing that approximates the input entered as well as possible. But the model is not always be able to do exactly what is specified when the specifications are not physical.
+
+\subsubsection{References}\label{references-054}
+
+Arasteh, D., J.C. Kohler, B. Griffith, Modeling Windows in EnergyPlus with Simple Performance Indices. Lawrence Berkeley National Laboratory. In Draft. Available at
+
+\subsection{Glazing System Properties}\label{glazing-system-properties}
+
+The optical properties of a glazing system consisting of \emph{N} glass layers separated by nonabsorbing gas layers (Figure~\ref{fig:schematic-of-transmission-reflection}.~ Schematic of transmission, reflection and absorption of solar radiation within a multi-layer glazing system.) are determined by solving the following recursion relations for \emph{T\(_{i,j}\)}, the transmittance through layers* i* to* j\emph{;}R\(^{f}\)\(_{i,j}\)* and \emph{R\(^{b}\)\(_{i,j}\)}, the front and back reflectance, respectively, from layers* i* to* j\emph{; and}A\(_{j}\)\emph{, the absorption in layer} j\emph{. Here layer 1 is the outermost layer and layer}N* is the innermost layer. These relations account for multiple internal reflections within the glazing system. Each of the variables is a function of wavelength.
+
+\begin{equation}
+{T_{i,j}} = \frac{{{T_{i,j - 1}}{T_{j,j}}}}{{1 - R_{j,j}^fR_{j - 1,i}^b}}
+\end{equation}
+
+\begin{equation}
+R_{i,j}^f = R_{i,j - 1}^f + \frac{{T_{i,j - 1}^2R_{j,j}^f}}{{1 - R_{j,j}^fR_{j - 1,i}^b}}
+\end{equation}
+
+\begin{equation}
+R_{j,i}^b = R_{j,j}^b + \frac{{T_{j,j}^2R_{j - 1,i}^b}}{{1 - R_{j - 1,i}^bR_{j,j}^f}}
+\end{equation}
+
+\begin{equation}
+A_j^f = \frac{{{T_{1,j - 1}}(1 - {T_{j,j}} - R_{j,j}^f)}}{{1 - R_{j,N}^fR_{j - 1,1}^b}} + \frac{{{T_{1,j}}R_{j + 1,N}^f(1 - {T_{j,j}} - R_{j,j}^b)}}{{1 - R_{j,N}^fR_{j - 1,1}^b}}
+\end{equation}
+
+In Eq. \emph{T\(_{i,j}\)} = 1 and \emph{R\(_{i,j}\)} = 0 if* i\emph{\textless{}0 or} j\emph{\textgreater{}}N*.
+
+\begin{figure}[hbtp] % fig 77
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image956.png}
+\caption{Schematic of transmission, reflection and absorption of solar radiation within a multi-layer glazing system. \protect \label{fig:schematic-of-transmission-reflection}}
+\end{figure}
+
+As an example, for double glazing (\emph{N} = 2) these equations reduce to
+
+\begin{equation}
+{T_{1,2}} = \frac{{{T_{1,1}}{T_{2,2}}}}{{1 - R_{2,2}^fR_{1,1}^b}}
+\end{equation}
+
+\begin{equation}
+R_{1,2}^f = R_{1,1}^f + \frac{{T_{1,1}^2R_{2,2}^f}}{{1 - R_{2,2}^fR_{1,1}^b}}
+\end{equation}
+
+\begin{equation}
+R_{2,1}^b = R_{2,2}^b + \frac{{T_{2,2}^2R_{1,1}^b}}{{1 - R_{1,1}^bR_{2,2}^f}}
+\end{equation}
+
+\begin{equation}
+A_1^f = (1 - {T_{1,1}} - R_{1,1}^f) + \frac{{{T_{1,1}}R_{2,2}^f(1 - {T_{1,1}} - R_{1,1}^b)}}{{1 - R_{2,2}^fR_{1,1}^b}}
+\end{equation}
+
+\begin{equation}
+A_2^f = \frac{{{T_{1,1}}(1 - {T_{2,2}} - R_{2,2}^f)}}{{1 - R_{2,2}^fR_{1,1}^b}}
+\end{equation}
+
+If the above transmittance and reflectance properties are input as a function of wavelength, EnergyPlus calculates ``spectral average'' values of the above glazing system properties by integrating over wavelength:
+
+The spectral-average solar property is
+
+\begin{equation}
+{P_s} = \frac{{\int {P(\lambda ){E_s}(\lambda )d\lambda } }}{{\int {{E_s}(\lambda )d\lambda } }}
+\end{equation}
+
+The spectral-average visible property is
+
+\begin{equation}
+{P_v} = \frac{{\int {P(\lambda ){E_s}(\lambda )V(\lambda )d\lambda } }}{{\int {{E_s}(\lambda )V(\lambda )d\lambda } }}
+\end{equation}
+
+where \({E_s}(\lambda )\) is the solar spectral irradiance function and \(V(\lambda )\) is the photopic response function of the eye. The default functions are shown in Table~\ref{table:solar-spectral-irradiance-function.} and Table~\ref{table:photopic-response-function.}. They can be overwritten by user defined solar and/or visible spectrum using the objects Site:SolarAndVisibleSpectrum and Site:SpectrumData. They are expressed as a set of values followed by the corresponding wavelengths for values.
+
+If a glazing layer has optical properties that are roughly constant with wavelength, the wavelength-dependent values of \emph{T\(_{i,i}\)} , \emph{R\(^{f}\)\(_{i,i}\)} and \emph{R\(^{b}\)\(_{i,i}\)} in Eqs. to can be replaced with constant values for that layer.
+
+% table 29
+\begin{longtable}[c]{p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}}
+
+\caption{Solar spectral irradiance function. \label{table:solar-spectral-irradiance-function.}} \tabularnewline
+\toprule 
+\endfirsthead
+
+\caption[]{Solar spectral irradiance function.} \tabularnewline
+\toprule 
+\endhead
+
+\multicolumn{10}{l}{Air mass 1.5 terrestrial solar global spectral irradiance values (W/m-micron) on a 37 tilted surface.} \tabularnewline
+\multicolumn{10}{l}{Corresponds to wavelengths in following data block. Based on ISO 9845-1 and ASTM E 892;} \tabularnewline
+\multicolumn{10}{l}{derived from Optics5 data file ISO-9845GlobalNorm.std, 10-14-99.} \tabularnewline
+\midrule
+\endhead
+0.0, & 9.5, & 42.3, & 107.8, & 181.0, & 246.0, & 395.3, & 390.1, & 435.3, & 438.9, \tabularnewline 
+483.7, & 520.3, & 666.2, & 712.5, & 720.7, & 1013.1, & 1158.2, & 1184.0, & 1071.9, & 1302.0, \tabularnewline 
+1526.0, & 1599.6, & 1581.0, & 1628.3, & 1539.2, & 1548.7, & 1586.5, & 1484.9, & 1572.4, & 1550.7, \tabularnewline 
+1561.5, & 1501.5, & 1395.5, & 1485.3, & 1434.1, & 1419.9, & 1392.3, & 1130.0, & 1316.7, & 1010.3, \tabularnewline 
+1043.2, & 1211.2, & 1193.9, & 1175.5, & 643.1, & 1030.7, & 1131.1, & 1081.6, & 849.2, & 785.0, \tabularnewline 
+916.4, & 959.9, & 978.9, & 933.2, & 748.5, & 667.5, & 690.3, & 403.6, & 258.3, & 313.6, \tabularnewline 
+526.8, & 646.4, & 746.8, & 690.5, & 637.5, & 412.6, & 108.9, & 189.1, & 132.2, & 339.0, \tabularnewline 
+460.0, & 423.6, & 480.5, & 413.1, & 250.2, & 32.5, & 1.6, & 55.7, & 105.1, & 105.5, \tabularnewline 
+182.1, & 262.2, & 274.2, & 275.0, & 244.6, & 247.4, & 228.7, & 244.5, & 234.8, & 220.5, \tabularnewline 
+171.5, & 30.7, & 2.0, & 1.2, & 21.2, & 91.1, & 26.8, & 99.5, & 60.4, & 89.1, \tabularnewline 
+82.2, & 71.5, & 70.2, & 62.0, & 21.2, & 18.5, & 3.2 \tabularnewline \midrule
+\multicolumn{10}{l}{Wavelengths (microns) corresponding to above data block} \tabularnewline \midrule
+0.3000, & 0.3050, & 0.3100, & 0.3150, & 0.3200, & 0.3250, & 0.3300, & 0.3350, & 0.3400, & 0.3450, \tabularnewline 
+0.3500, & 0.3600, & 0.3700, & 0.3800, & 0.3900, & 0.4000, & 0.4100, & 0.4200, & 0.4300, & 0.4400, \tabularnewline  
+0.4500, & 0.4600, & 0.4700, & 0.4800, & 0.4900, & 0.5000, & 0.5100, & 0.5200, & 0.5300, & 0.5400, \tabularnewline
+0.5500, & 0.5700, & 0.5900, & 0.6100, & 0.6300, & 0.6500, & 0.6700, & 0.6900, & 0.7100, & 0.7180, \tabularnewline
+0.7244, & 0.7400, & 0.7525, & 0.7575, & 0.7625, & 0.7675, & 0.7800, & 0.8000, & 0.8160, & 0.8237, \tabularnewline
+0.8315, & 0.8400, & 0.8600, & 0.8800, & 0.9050, & 0.9150, & 0.9250, & 0.9300, & 0.9370, & 0.9480, \tabularnewline
+0.9650, & 0.9800, & 0.9935, & 1.0400, & 1.0700, & 1.1000, & 1.1200, & 1.1300, & 1.1370, & 1.1610, \tabularnewline
+1.1800, & 1.2000, & 1.2350, & 1.2900, & 1.3200, & 1.3500, & 1.3950, & 1.4425, & 1.4625, & 1.4770, \tabularnewline
+1.4970, & 1.5200, & 1.5390, & 1.5580, & 1.5780, & 1.5920, & 1.6100, & 1.6300, & 1.6460, & 1.6780, \tabularnewline
+1.7400, & 1.8000, & 1.8600, & 1.9200, & 1.9600, & 1.9850, & 2.0050, & 2.0350, & 2.0650, & 2.1000, \tabularnewline
+2.1480, & 2.1980, & 2.2700, & 2.3600, & 2.4500, & 2.4940, & 2.5370 \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 30
+\begin{longtable}[c]{p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}}
+
+\caption{Photopic response function. \label{table:photopic-response-function.}} \tabularnewline
+\toprule 
+\endfirsthead
+
+\caption[]{Photopic response function.} \tabularnewline
+\toprule 
+\endhead
+
+\multicolumn{10}{l}{Photopic response function values corresponding to wavelengths in following data block.} \tabularnewline 
+\multicolumn{10}{l}{Based on CIE 1931 observer; ISO/CIE 10527, CIE Standard Calorimetric Observers;} \tabularnewline 
+\multicolumn{10}{l}{derived from Optics5 data file "CIE 1931 Color Match from E308.txt",} \tabularnewline 
+\multicolumn{10}{l}{which is the same as WINDOW4 file Cie31t.dat.} \tabularnewline \midrule \endhead
+0.0000, & 0.0001, & 0.0001, & 0.0002, & 0.0004, & 0.0006, & 0.0012, & 0.0022, & 0.0040, & 0.0073, \tabularnewline 
+0.0116, & 0.0168, & 0.0230, & 0.0298, & 0.0380, & 0.0480, & 0.0600, & 0.0739, & 0.0910, & 0.1126, \tabularnewline 
+0.1390, & 0.1693, & 0.2080, & 0.2586, & 0.3230, & 0.4073, & 0.5030, & 0.6082, & 0.7100, & 0.7932, \tabularnewline 
+0.8620, & 0.9149, & 0.9540, & 0.9803, & 0.9950, & 1.0000, & 0.9950, & 0.9786, & 0.9520, & 0.9154, \tabularnewline 
+0.8700, & 0.8163, & 0.7570, & 0.6949, & 0.6310, & 0.5668, & 0.5030, & 0.4412, & 0.3810, & 0.3210, \tabularnewline 
+0.2650, & 0.2170, & 0.1750, & 0.1382, & 0.1070, & 0.0816, & 0.0610, & 0.0446, & 0.0320, & 0.0232, \tabularnewline 
+0.0170, & 0.0119, & 0.0082, & 0.0158, & 0.0041, & 0.0029, & 0.0021, & 0.0015, & 0.0010, & 0.0007, \tabularnewline 
+0.0005, & 0.0004, & 0.0002, & 0.0002, & 0.0001, & 0.0001, & 0.0001, & 0.0000, & 0.0000, & 0.0000, \tabularnewline 
+0.0000 \tabularnewline \midrule
+\multicolumn{10}{l}{Wavelengths (microns) corresponding to above data block} \tabularnewline \midrule
+.380, & .385, & .390, & .395, & .400, & .405, & .410, & .415, & .420, & .425, \tabularnewline 
+.430, & .435, & .440, & .445, & .450, & .455, & .460, & .465, & .470, & .475, \tabularnewline 
+.480, & .485, & .490, & .495, & .500, & .505, & .510, & .515, & .520, & .525, \tabularnewline 
+.530, & .535, & .540, & .545, & .550, & .555, & .560, & .565, & .570, & .575, \tabularnewline 
+.580, & .585, & .590, & .595, & .600, & .605, & .610, & .615, & .620, & .625, \tabularnewline 
+.630, & .635, & .640, & .645, & .650, & .655, & .660, & .665, & .670, & .675, \tabularnewline 
+.680, & .685, & .690, & .695, & .700, & .705, & .710, & .715, & .720, & .725, \tabularnewline 
+.730, & .735, & .740, & .745, & .750, & .755, & .760, & .765, & .770, & .775, \tabularnewline 
+.780 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Calculation of Angular Properties}\label{calculation-of-angular-properties}
+
+Calculation of optical properties is divided into two categories: uncoated glass and coated glass.
+
+\subsubsection{Angular Properties for Uncoated Glass}\label{angular-properties-for-uncoated-glass}
+
+The following discussion assumes that optical quantities such as transmissivity, reflectvity, absorptivity, and index of refraction are a function of wavelength, λ. If there are no spectral data the angular dependence is calculated based on the single values for transmittance and reflectance in the visible and solar range. In the visible range an average wavelength of 0.575 microns is used in the calculations. In the solar range an average wavelength of 0.898 microns is used.
+
+The spectral data include the transmittance, \emph{T}, and the reflectance, \emph{R}. For uncoated glass the reflectance is the same for the front and back surfaces. For angle of incidence, \(\phi\) , the transmittance and reflectance are related to the transmissivity, τ,and reflectivity, �, by the following relationships:
+
+\begin{equation}
+T(\phi ) = \frac{{\tau {{(\phi )}^2}{e^{ - \alpha d/\cos \phi '}}}}{{1 - \rho {{(\phi )}^2}{e^{ - 2\alpha d/\cos \phi '}}}}
+\end{equation}
+
+\begin{equation}
+R(\phi ) = \rho (\phi )\left( {1 + T(\phi ){e^{ - \alpha d/\cos \phi '}}} \right)
+\end{equation}
+
+The spectral reflectivity is calculated from Fresnel's equation assuming unpolarized incident radiation:
+
+\begin{equation}
+\rho (\phi ) = \frac{1}{2}\left( {{{\left( {\frac{{n\cos \phi  - \cos \phi '}}{{n\cos \phi  + \cos \phi '}}} \right)}^2} + {{\left( {\frac{{n\cos \phi ' - \cos \phi }}{{n\cos \phi ' + \cos \phi }}} \right)}^2}} \right)
+\end{equation}
+
+The spectral transmittivity is given by
+
+\begin{equation}
+\tau (\phi ) = 1 - \rho (\phi )
+\end{equation}
+
+The spectral absorption coefficient is defined as
+
+\begin{equation}
+\alpha  = 4\pi \kappa /\lambda
+\end{equation}
+
+where κ is the dimensionless spectrally-dependent extinction coefficient and λ is the wavelength expressed in the same units as the sample thickness.
+
+Solving Eq. at normal incidence gives
+
+\begin{equation}
+n = \frac{{1 + \sqrt {\rho (0)} }}{{1 - \sqrt {\rho (0)} }}
+\end{equation}
+
+Evaluating Eq. at normal incidence gives the following expression for \emph{κ}
+
+\begin{equation}
+\kappa  =  - \frac{\lambda }{{4\pi d}}\ln \frac{{R(0) - \rho (0)}}{{\rho (0)T(0)}}
+\end{equation}
+
+Eliminating the exponential in Eqs. and~ gives the reflectivity at normal incidence:
+
+\begin{equation}
+\rho (0) = \frac{{\beta  - \sqrt {{\beta ^2} - 4(2 - R(0))R(0)} }}{{2(2 - R(0))}}
+\end{equation}
+
+where
+
+\begin{equation}
+\beta  = T{(0)^2} - R{(0)^2} + 2R(0) + 1
+\end{equation}
+
+The value for the reflectivity, \emph{�}(0),from Eq. is substituted into Eqs. and . The result from Eq. is used to calculate the absorption coefficient in Eq. . The index of refraction is used to calculate the reflectivity in Eq. which is then used to calculate the transmittivity in Eq. . The reflectivity, transmissivity and absorption coefficient are then substituted into Eqs. and to obtain the angular values of the reflectance and transmittance.
+
+\subsubsection{Angular Properties for Coated Glass}\label{angular-properties-for-coated-glass}
+
+A regression fit is used to calculate the angular properties of coated glass from properties at normal incidence. If the transmittance of the coated glass is \textgreater{} 0.645, the angular dependence of uncoated clear glass is used. If the transmittance of the coated glass is ≤ 0.645, the angular dependence of uncoated bronze glass is used. The values for the angular functions for the transmittance and reflectance of both clear glass \(({\bar \tau_{clr}},{\bar \rho_{clr}})\) ~and bronze glass \(({\bar \tau_{bnz}},{\bar \rho_{bnz}})\) are determined from a fourth-order polynomial regression:
+
+\begin{equation}
+\bar \tau (\phi ) = {\bar \tau_0} + {\bar \tau_1}\cos (\phi ) + {\bar \tau_2}{\cos ^2}(\phi ) + {\bar \tau_3}{\cos ^3}(\phi ) + {\bar \tau_4}{\cos ^4}(\phi )
+\end{equation}
+
+and
+
+\begin{equation}
+\bar \rho (\phi ) = {\bar \rho_0} + {\bar \rho_1}\cos (\phi ) + {\bar \rho_2}{\cos ^2}(\phi ) + {\bar \rho_3}{\cos ^3}(\phi ) + {\bar \rho_4}{\cos ^4}(\phi ) - \bar \tau (\phi )
+\end{equation}
+
+The polynomial coefficients are given in Table~\ref{table:polynomial-coefficients-used-to-determine}.
+
+% table 31
+\begin{longtable}[c]{p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}}
+
+\caption{Polynomial coefficients used to determine angular properties of coated glass. \label{table:polynomial-coefficients-used-to-determine}} \tabularnewline
+\toprule 
+~ & 0 & 1 & 2 & 3 & 4 \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Polynomial coefficients used to determine angular properties of coated glass.} \tabularnewline
+\toprule 
+~ & 0 & 1 & 2 & 3 & 4 \tabularnewline
+\midrule
+\endhead
+
+$\bar{\tau}_{clr}$ & -0.0015 & 3.355 & -3.840 & 1.460 & 0.0288 \tabularnewline
+$\bar{\rho}_{clr}$ & 0.999 & -0.563 & 2.043 & -2.532 & 1.054 \tabularnewline
+$\bar{\tau}_{bnz}$ & -0.002 & 2.813 & -2.341 & -0.05725 & 0.599 \tabularnewline
+$\bar{\rho}_{bnz}$ & 0.997 & -1.868 & 6.513 & -7.862 & 3.225 \tabularnewline
+\bottomrule
+\end{longtable}
+
+These factors are used as follows to calculate the angular transmittance and reflectance:
+
+For \emph{T}(0) \textgreater{} 0.645:
+
+\begin{equation}
+T(\phi ) = T(0){\bar \tau_{clr}}(\phi )
+\end{equation}
+
+\begin{equation}
+R(\phi ) = R(0)(1 - {\bar \rho_{clr}}(\phi )) + {\bar \rho_{clr}}(\phi )
+\end{equation}
+
+For \emph{T}(0) ≤ 0.645:
+
+\begin{equation}
+T(\phi ) = T(0){\bar \tau_{bnz}}(\phi )
+\end{equation}
+
+\begin{equation}
+R(\phi ) = R(0)(1 - {\bar \rho_{bnz}}(\phi )) + {\bar \rho_{bnz}}(\phi )
+\end{equation}
+
+\subsubsection{Angular Properties for Simple Glazing Systems}\label{angular-properties-for-simple-glazing-systems}
+
+When the glazing system is modeled using the simplified method, an alternate method is used to determine the angular properties.~ The equation for solar transmittance as a function of incidence angle, \(T\left( \phi \right)\) , is,
+
+\begin{equation}
+T\left( \phi  \right) = T\left( {\phi  = 0} \right)\,\cos \left( \phi  \right)\,\,\left( {1 + (0.768 + 0.817\,SHG{C^4})\;{{\sin }^3}\left( \phi  \right)} \right)
+\end{equation}
+
+where,
+
+\(T\left( {\phi = 0} \right)\) ~is the normal incidence solar transmittance, \({T_{Sol}}\) .
+
+The equation for solar reflectance as a function of incidence angle,~ \(R\left( \phi \right)\) , is,
+
+\begin{equation}
+R\left( \phi  \right) = \frac{{R\left( {\phi  = 0} \right)\left( {{f_1}\left( \phi  \right) + {f_2}\left( \phi  \right)\sqrt {SHGC} } \right)}}{{{R_{fit,o}}}}
+\end{equation}
+
+where,
+
+\begin{equation}
+{f_1}\left( \phi  \right) = \left( {\left( {\left( {2.403\cos \left( \phi  \right) - 6.192} \right)\cos \left( \phi  \right) + 5.625} \right)\cos \left( \phi  \right) - 2.095} \right)\cos \left( \phi  \right) + 1
+\end{equation}
+
+\begin{equation}
+{f_2}\left( \phi  \right) = \left( {\left( {\left( { - 1.188\cos \left( \phi  \right) + 2.022} \right)\cos \left( \phi  \right) + 0.137} \right)\cos \left( \phi  \right) - 1.720} \right)\cos \left( \phi  \right)
+\end{equation}
+
+\begin{equation}
+{R_{fit,o}} = 0.7413 - \left( {0.7396\;\sqrt {SHGC} } \right)
+\end{equation}
+
+\subsection{Calculation of Hemispherical Values}\label{calculation-of-hemispherical-values}
+
+The hemispherical value of a property is determined from the following integral:
+
+\begin{equation}
+{P_{hemispherical}} = 2\int_0^{\frac{\pi }{2}} {P(\phi )\cos (\phi )\sin (\phi )d\phi }
+\end{equation}
+
+The integral is evaluated by Simpson's rule for property values at angles of incidence from 0 to 90 degrees in 10-degree increments.
+
+\subsection{Optical Properties of Window Shading Devices}\label{optical-properties-of-window-shading-devices}
+
+Shading devices affect the system transmittance and glass layer absorptance for short-wave radiation and for long-wave (thermal) radiation. The effect depends on the shade position (interior, exterior or between-glass), its transmittance, and the amount of inter-reflection between the shading device and the glazing. Also of interest is the amount of radiation absorbed by the shading device.
+
+In EnergyPlus, shading devices are divided into four categories, ``shades,'' ''blinds,'' ``screens,'' and ``switchable glazing.'' ``Shades'' are assumed to be perfect diffusers. This means that direct radiation incident on the shade is reflected and transmitted as hemispherically uniform diffuse radiation: there is no direct component of transmitted radiation. It is also assumed that the transmittance, \emph{τ\(_{sh}\)}, reflectance, \emph{�\(_{sh}\)}, and absorptance, \emph{α\(_{sh}\)}, are the same for the front and back of the shade and are independent of angle of incidence. Many types of drapery and pull-down roller devices are close to being perfect diffusers and can be categorized as ``shades.''
+
+``Blinds'' in EnergyPlus are slat-type devices such as venetian blinds. Unlike shades, the optical properties of blinds are strongly dependent on angle of incidence. Also, depending on slat angle and the profile angle of incident direct radiation, some of the direct radiation may pass between the slats, giving a direct component of transmitted radiation.
+
+``Screens'' are debris or insect protection devices made up of metallic or non-metallic materials. Screens may also be used as shading devices for large glazing areas where excessive solar gain is an issue. The EnergyPlus window screen model assumes the screen is composed of intersecting orthogonally-crossed cylinders, with the surface of the cylinders assumed to be diffusely reflecting. Screens may only be used on the exterior surface of a window construction. As with blinds, the optical properties affecting the direct component of transmitted radiation are dependent on the angle of incident direct radiation.
+
+With ``Switchable glazing,'' shading is achieved making the glazing more absorbing or more reflecting, usually by an electrical or chemical mechanism. An example is electrochromic glazing where the application of an electrical voltage or current causes the glazing to switch from light to dark.
+
+Shades and blinds can be either fixed or moveable. If moveable, they can be deployed according to a schedule or according to a trigger variable, such as solar radiation incident on the window. Screens can be either fixed or moveable according to a schedule.
+
+\subsubsection{Shades}\label{shades}
+
+\subsubsection{Shade/Glazing System Properties for Short-Wave Radiation}\label{shadeglazing-system-properties-for-short-wave-radiation}
+
+Short-wave radiation includes
+
+1)~~~Beam solar radiation from the sun and diffuse solar radiation from the sky and ground incident on the outside of the window,
+
+2)~~~Beam and/or diffuse radiation reflected from exterior obstructions or the building itself,
+
+3)~~~Solar radiation reflected from the inside zone surfaces and incident as diffuse radiation on the inside of the window,
+
+4)~~~Beam solar radiation from one exterior window incident on the inside of another window in the same zone, and
+
+5)~~~Short-wave radiation from electric lights incident as diffuse radiation on the inside of the window.
+
+\textbf{Exterior Shade}
+
+For an exterior shade we have the following expressions for the system transmittance, the effective system glass layer absorptance, and the system shade absorptance, taking inter-reflection between shade and glazing into account. Here, ``system'' refers to the combination of glazing and shade. The system properties are given in terms of the isolated shade properties (i.e., shade properties in the absence of the glazing) and the isolated glazing properties (i.e., glazing properties in the absence of the shade).
+
+\begin{equation}
+{T_{sys}}(\phi ) = T_{1,N}^{dif}\frac{{{\tau_{sh}}}}{{1 - R_f^{dif}{\rho_{sh}}}}
+\end{equation}
+
+\begin{equation}
+T_{sys}^{dif} = T_{1,N}^{dif}\frac{{{\tau_{sh}}}}{{1 - R_f^{dif}{\rho_{sh}}}}
+\end{equation}
+
+\begin{equation}
+A_{j,f}^{sys}(\phi ) = A_{j,f}^{dif}\frac{{{\tau_{sh}}}}{{1 - {R_f}{\rho_{sh}}}},\quad j = 1{\rm{to}}N
+\end{equation}
+
+\begin{equation}
+A_{j,f}^{dif,sys} = A_{j,f}^{dif}\frac{{{\tau_{sh}}}}{{1 - {R_f}{\rho_{sh}}}},\quad j = 1{\rm{ to }}N
+\end{equation}
+
+\begin{equation}
+A_{j,b}^{dif,sys} = A_{j,b}^{dif}\frac{{T_{1,N}^{dif}{\rho_{sh}}}}{{1 - {R_f}{\rho_{sh}}}},\quad j = 1{\rm{ to }}N
+\end{equation}
+
+\begin{equation}
+\alpha_{sh}^{sys} = {\alpha_{sh}}\left( {1 + \frac{{{\tau_{sh}}{R_f}}}{{1 - {R_f}{\rho_{sh}}}}} \right)
+\end{equation}
+
+\textbf{Interior Shade}
+
+The system properties when an interior shade is in place are the following.
+
+\begin{equation}
+{T_{sys}}(\phi ) = T_{1,N}^{}(\phi )\frac{{{\tau_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}
+\end{equation}
+
+\begin{equation}
+T_{sys}^{dif} = T_{1,N}^{dif}\frac{{{\tau_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}
+\end{equation}
+
+\begin{equation}
+A_{j,f}^{sys}(\phi ) = {A_{j,f}}(\phi ) + {T_{1,N}}(\phi )\frac{{{\rho_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}A_{j,b}^{dif},\quad j = 1{\rm{ to }}N
+\end{equation}
+
+\begin{equation}
+A_{j,f}^{dif,sys} = A_{j,f}^{dif} + T_{1,N}^{dif}\frac{{{\rho_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}A_{j,b}^{dif},\quad j = 1{\rm{ to }}N
+\end{equation}
+
+\begin{equation}
+A_{j,b}^{dif,sys} = \frac{{{\tau_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}A_{j,b}^{dif},{\rm{    }}j = 1{\rm{ to }}N
+\end{equation}
+
+\begin{equation}
+\alpha_{sh}^{sys}(\phi ) = T_{1,N}^{}(\phi )\frac{{{\alpha_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}
+\end{equation}
+
+\begin{equation}
+\alpha_{sh}^{dif,sys} = T_{1,N}^{dif}\frac{{{\alpha_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}
+\end{equation}
+
+\subsubsection{Long-Wave Radiation Properties of Window Shades}\label{long-wave-radiation-properties-of-window-shades}
+
+Long-wave radiation includes
+
+~~~~~~~Thermal radiation from the sky, ground and exterior obstructions incident on the outside of the window,
+
+~~~~~~~Thermal radiation from other room surfaces incident on the inside of the window, and
+
+~~~~~~~Thermal radiation from internal sources, such as equipment and electric lights, incident on the inside of the window.
+
+The program calculates how much long-wave radiation is absorbed by the shade and by the adjacent glass surface. The system emissivity (thermal absorptance) for an interior or exterior shade, taking into account reflection of long-wave radiation between the glass and shade, is given by
+
+\begin{equation}
+\varepsilon_{sh}^{lw,sys} = \varepsilon_{sh}^{lw}\left( {1 + \frac{{\tau_{sh}^{lw}\rho_{gl}^{lw}}}{{1 - \rho_{sh}^{lw}\rho_{gl}^{lw}}}} \right)
+\end{equation}
+
+where \(\rho_{gl}^{lw}\) is the long-wave reflectance of the outermost glass surface for an exterior shade or the innermost glass surface for an interior shade, and it is assumed that the long-wave transmittance of the glass is zero.
+
+The innermost (for interior shade) or outermost (for exterior shade) glass surface emissivity when the shade is present is
+
+\begin{equation}
+\varepsilon_{gl}^{lw,sys} = \varepsilon_{gl}^{lw}\frac{{\tau_{sh}^{lw}}}{{1 - \rho_{sh}^{lw}\rho_{gl}^{lw}}}
+\end{equation}
+
+\subsubsection{Switchable Glazing}\label{switchable-glazing}
+
+For switchable glazing, such as electrochromics, the solar and visible optical properties of the glazing can switch from a light state to a dark state. The switching factor, \emph{f\(_{switch}\)}, determines what state the glazing is in. An optical property, \emph{p}, such as transmittance or glass layer absorptance, for this state is given by
+
+\begin{equation}
+p = (1 - {f_{switch}}){p_{light}} + {f_{switch}}{p_{dark}}
+\end{equation}
+
+where
+
+\emph{p\(_{light}\)}is the property value for the unswitched, or light state, and \emph{p\(_{dark}\)} is the property value for the fully switched, or dark state.
+
+The value of the switching factor in a particular time step depends on what type of switching control has been specified: ``schedule,'' ``trigger,'' or ``daylighting.'' If ``schedule,'' \emph{f\(_{switch}\)} = schedule value, which can be 0 or 1.
+
+\subsection{Thermochromic Windows}\label{thermochromic-windows}
+
+Thermochromic (TC) materials have active, reversible optical properties that vary with temperature. Thermochromic windows are adaptive window systems for incorporation into building envelopes. Thermochromic windows respond by absorbing sunlight and turning the sunlight energy into heat. As the thermochromic film warms it changes its light transmission level from less absorbing to more absorbing. The more sunlight it absorbs the lower the light level going through it. Figure~\ref{fig:variations-of-window-properties-with} shows the variations of window properties with the temperature of the thermochromic glazing layer. By using the suns own energy the window adapts based solely on the directness and amount of sunlight. Thermochromic materials will normally reduce optical transparency by absorption and/or reflection, and are specular (maintaining vision).
+
+\begin{figure}[hbtp] % fig 78
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1015.svg.png}
+\caption{Variations of Window Properties with the Temperature of the Thermochromic Glazing Layer \protect \label{fig:variations-of-window-properties-with}}
+\end{figure}
+
+On cloudy days the window is at full transmission and letting in diffuse daylighting. On sunny days the window maximizes diffuse daylighting and tints based on the angle of the sun relative to the window. For a south facing window (northern hemisphere) the daylight early and late in the day is maximized and the direct sun at mid day is minimized.
+
+The active thermochromic material can be embodied within a laminate layer or a surface film. The overall optical state of the window at a given time is a function primarily of
+
+\begin{itemize}
+\item
+  thermochromic material properties
+\item
+  solar energy incident on the window
+\item
+  construction of the window system that incorporates the thermochromic layer
+\item
+  environmental conditions (interior, exterior, air temperature, wind, etc).
+\end{itemize}
+
+The tinted film, in combination with a heat reflecting, low-e layer allows the window to reject most of the absorbed radiation thus reducing undesirable heat load in a building. In the absence of direct sunlight the window cools and clears and again allows lower intensity diffuse radiation into a building. TC windows can be designed in several ways (Figure~\ref{fig:configurations-of-thermochromic-windows}), with the most common being a triple pane windows with the TC glass layer in the middle a double pane windows with the TC layer on the inner surface of the outer pane or for sloped glazing a double pane with the laminate layer on the inner pane with a low-e layer toward the interior. The TC glass layer has variable optical properties depending on its temperature, with a lower temperature at which the optical change is initiated, and an upper temperature at which a minimum transmittance is reached. TC windows act as passive solar shading devices without the need for sensors, controls and power supplies but their optical performance is dependent on varying solar and other environmental conditions at the location of the window.
+
+\begin{figure}[hbtp] % fig 79
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1017.png}
+\caption{Configurations of Thermochromic Windows \protect \label{fig:configurations-of-thermochromic-windows}}
+\end{figure}
+
+EnergyPlus describes a thermochromic window with a Construction object which references a special layer defined with a WindowMaterial:GlazingGroup:Thermochromic object. The WindowMaterial:GlazingGroup:Thermochromic object further references a series of WindowMaterial:Glazing objects corresponding to each specification temperature of the TC layer. During EnergyPlus run time, a series of TC windows corresponding to each specification temperature is created once. At the beginning of a particular time step calculations, the temperature of the TC glass layer from the previous time step is used to look up the most closed specification temperature whose corresponding TC window construction will be used for the current time step calculations. The current time step calculated temperature of the TC glass layer can be different from the previous time step, but no iterations are done in the current time step for the new TC glass layer temperature. This is an approximation that considers the reaction time of the TC glass layer can be close to EnergyPlus simulation time step say 10 to 15 minutes.
+
+\subsubsection{Blinds}\label{blinds}
+
+Window blinds in EnergyPlus are defined as a series of equidistant slats that are oriented horizontally or vertically. All of the slats are assumed to have the same optical properties. The overall optical properties of the blind are determined by the slat geometry (width, separation and angle) and the slat optical properties (front-side and back-side transmittance and reflectance). Blind properties for direct radiation are also sensitive to the ``profile angle,'' which is the angle of incidence in a plane that is perpendicular to the window plane and to the direction of the slats. The blind optical model in EnergyPlus is based on Simmler, Fischer and Winkelmann, 1996; however, that document has numerous typographical errors and should be used with caution.
+
+The following assumptions are made in calculating the blind optical properties:
+
+\begin{itemize}
+\item
+  The slats are flat.
+\item
+  The spectral dependence of inter-reflections between slats and glazing is ignored; spectral-average slat optical properties are used.
+\item
+  The slats are perfect diffusers. They have a perfectly matte finish so that reflection from a slat is isotropic (hemispherically uniform) and independent of angle of incidence, i.e., the reflection has no specular component. This also means that absorption by the slats is hemispherically uniform with no incidence angle dependence. If the transmittance of a slat is non-zero, the transmitted radiation is isotropic and the transmittance is independent of angle of incidence.
+\item
+  Inter-reflection between the blind and wall elements near the periphery of the blind is ignored.
+\item
+  If the slats have holes through which support strings pass, the holes and strings are ignored. Any other structures that support or move the slats are ignored.
+\end{itemize}
+
+\subsubsection{Slat Optical Properties}\label{slat-optical-properties}
+
+The slat optical properties used by EnergyPlus are shown in the following table.
+
+% table 32
+\begin{longtable}[c]{p{1.5in}p{2.5in}}
+\caption{Slat Optical Properties \label{table:slat-optical-properties}} \tabularnewline
+\toprule 
+\({\tau_{dir,dir}}\) & Direct-to-diffuse transmittance (same for front and back of slat) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Slat Optical Properties} \tabularnewline
+\toprule
+\({\tau_{dir,dir}}\) & Direct-to-diffuse transmittance (same for front and back of slat) \tabularnewline
+\midrule
+\endhead
+
+\({\tau_{dir,dir}}\) & Direct-to-diffuse transmittance (same for front and back of slat) \tabularnewline
+\({\tau_{dif,dir}}\) & Diffuse-to-diffuse transmittance (same for front and back of slat) \tabularnewline
+\(\rho_{dir,dif}^f\), \(\rho_{dir,dif}^b\) & Front and back direct-to-diffuse reflectance \tabularnewline
+\(\rho_{dif,dif}^f\), \(\rho_{dif,dif}^b\) & Front and back diffuse-to-diffuse reflectance \tabularnewline
+\bottomrule
+\end{longtable}
+
+It is assumed that there is no direct-to-direct transmission or reflection, so that \({\tau_{dir,dir}} = 0\), \(\rho_{dir,dir}^f = 0\), and \(\rho_{dir,dir}^b = 0\). It is further assumed that the slats are perfect diffusers, so that \({\tau_{dir,dif}}\), \(\rho_{dir,dif}^f\) and \(\rho_{dir,dif}^b\) are independent of angle of incidence. Until the EnergyPlus model is improved to take into account the angle-of-incidence dependence of slat transmission and reflection, it is assumed that \({\tau_{dir,dif}}\) = \({\tau_{dif,dif}}\), \(\rho_{dir,dif}^f\) = \(\rho_{dif,dif}^f\), and \(\rho_{dir,dif}^b\) = \(\rho_{dif,dif}^b\).
+
+\subsubsection{Direct Transmittance of Blind}\label{direct-transmittance-of-blind}
+
+The direct-to-direct and direct-to-diffuse transmittance of a blind is calculated using the slat geometry shown in Figure~\ref{fig:a-side-view-of-a-cell-formed-by-adjacent} (a), which shows the side view of one of the cells of the blind. For the case shown, each slat is divided into two segments, so that the cell is bounded by a total of six segments, denoted by \emph{s\(_{1}\)} through \emph{s\(_{6}\)} (note in the following that \emph{s\(_{i}\)} refers to both segment \emph{i} and the length of segment \emph{i)}.The lengths of \emph{s\(_{1}\)} and \emph{s\(_{2}\)} are equal to the slat separation, \emph{h}, which is the distance between adjacent slat faces. \emph{s\(_{3}\)} and \emph{s\(_{4}\)} are the segments illuminated by direct radiation. In the case shown in Figure~\ref{fig:a-side-view-of-a-cell-formed-by-adjacent} (a) the cell receives radiation by reflection of the direct radiation incident on \emph{s\(_{4}\)} and, if the slats have non-zero transmittance, by transmission through \emph{s\(_{3}\)}, which is illuminated from above.
+
+The goal of the blind direct transmission calculation is to determine the direct and diffuse radiation leaving the cell through \emph{s\(_{2}\)} for unit direct radiation entering the cell through \emph{s\(_{1}\)}.
+
+\begin{figure}[hbtp] % fig 80
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1034.png}
+\caption{(a) Side view of a cell formed by adjacent slats showing how the cell is divided into segments, \(s_i\),  for the calculation of direct solar transmittance; (b) side view of a cell showing case where some of the direct solar passes between adjacent slats without touching either of them. In this figure \(\phi_s\) is the profile angle and \(\phi_b\) is the slat angle. \label{fig:a-side-view-of-a-cell-formed-by-adjacent}}
+\end{figure}
+
+\subsubsection{Direct-to-Direct Blind Transmittance}\label{direct-to-direct-blind-transmittance}
+
+Figure~\ref{fig:a-side-view-of-a-cell-formed-by-adjacent} (b) shows the case where some of the direct radiation passes through the cell without hitting the slats. From the geometry in this figure we see that
+
+\begin{equation}
+\tau_{bl,f}^{dir,dir} = 1 - \frac{{|w|}}{h},{\rm{       }}|w|{\rm{ }} \le {\rm{ }}h
+\end{equation}
+
+where
+
+\begin{equation}
+w = s\frac{{\cos ({\varphi_b} - {\varphi_s})}}{{\cos {\varphi_s}}}
+\end{equation}
+
+Note that we are assuming that the slat thickness is zero. A correction for non-zero slat thickness is described later.
+
+\subsubsection{Direct-to-Diffuse Blind Transmittance, Reflectance and Absorptance}\label{direct-to-diffuse-blind-transmittance-reflectance-and-absorptance}
+
+The direct-to-diffuse and transmittance and reflectance of the blind are calculated using a radiosity method that involves the following three vector quantities:
+
+\emph{J\(_{i}\)} = the radiosity of segment \emph{s\(_{i}\)}, i.e., the total radiant flux into the cell from~ \emph{s\(_{i}\)}
+
+\emph{G\(_{i}\)} = the irradiance on the cell side of \emph{s\(_{i}\)}
+
+\emph{Q\(_{i}\)} = the source flux from the cell side of s\emph{\(_{i}\)}
+
+Based on these definitions we have the following equations that relate \emph{J}, \emph{G} and \emph{Q} for the different segments:
+
+\begin{equation}
+  \begin{array}{rl}
+    J_1 & = Q_1 \\
+    J_2 & = Q_2 \\
+    J_3 & = Q_3 + \rho_{dif,dif}^b G_3 + \tau_{dif,dif} G_4 \\
+    J_4 & = Q_4 + \tau_{dif,dif} G_3 + \rho_{dif,dif}^f G_4 \\
+    J_5 & = Q_5 + \rho_{dif,dif}^b G_5 + \tau_{dif,dif} G_6 \\
+    J_6 & = Q_6 + \tau_{dif,dif} G_5 + \rho_{dif,dif}^f G_6
+  \end{array}
+\end{equation}
+
+In addition we have the following equation relating \emph{G} and* J*:
+
+\begin{equation}
+{G_i} = \sum\limits_{j = 1}^6 {{J_j}{F_{ji}}{\rm{ ,    }}i = 1,6}
+\end{equation}
+
+where \({F_{ji}}\) is the view factor between \({s_j}\) and \({s_i}\) , i.e., \({F_{ji}}\) is the fraction of radiation leaving \({s_j}\) that is intercepted by \({s_i}\) .
+
+Using \({J_1} = {Q_1} = 0\) and \({J_2} = {Q_2} = 0\) ~and combining the above equations gives the following equation set relating* J* and* Q*:
+
+\begin{equation}
+{J_3} - \rho_{dif,dif}^b\sum\limits_{j = 3}^6 {{J_j}{F_{j3}} - {\tau_{dif,dif}}\sum\limits_{j = 3}^6 {{J_j}{F_{j4}} = {Q_3}} }
+\end{equation}
+
+\begin{equation}
+{J_4} - \tau_{dif,dif}^{}\sum\limits_{j = 3}^6 {{J_j}{F_{j3}} - \rho_{dif,dif}^f\sum\limits_{j = 3}^6 {{J_j}{F_{j4}} = {Q_4}} }
+\end{equation}
+
+\begin{equation}
+{J_5} - \rho_{dif,dif}^b\sum\limits_{j = 3}^6 {{J_j}{F_{j5}} - {\tau_{dif,dif}}\sum\limits_{j = 3}^6 {{J_j}{F_{j6}} = {Q_5}} }
+\end{equation}
+
+\begin{equation}
+{J_6} - \tau_{dif,dif}^{}\sum\limits_{j = 3}^6 {{J_j}{F_{j3}} - \rho_{dif,dif}^f\sum\limits_{j = 3}^6 {{J_j}{F_{j6}} = {Q_6}} }
+\end{equation}
+
+This can be written in the form
+
+\begin{equation}
+Q' = XJ'
+\end{equation}
+
+where \emph{X} is a 4x4 matrix and
+
+\begin{equation}
+J' = \left[ \begin{array}{c}
+   J_3 \\
+   J_4 \\
+   J_5 \\
+   J_6 \end{array} \right]
+\end{equation}
+
+\begin{equation}
+Q' = \left[ \begin{array}{c}
+    Q_3 \\
+    Q_4 \\
+    Q_5 \\
+    Q_6 \end{array} \right]
+\end{equation}
+
+We then obtain \(J'\) ~from
+
+\begin{equation}
+J' = {X^{ - 1}}Q'
+\end{equation}
+
+The view factors, \({F_{ij}}\) , are obtained as follows. The cell we are dealing with is a convex polygon with \emph{n} sides. In such a polygon the view factors must satisfy the following constraints:
+
+\begin{equation}
+\sum\limits_{j = 1}^n {{F_{ij}} = 1{\rm{,  }}i = 1,n}
+\end{equation}
+
+\begin{equation}
+{s_i}{F_{ij}} = {s_j}{F_{ji}}{\rm{,  }}i = 1,n{\rm{;  }}j = 1,n
+\end{equation}
+
+\begin{equation}
+{F_{ii}} = 0{\rm{,  }}i = 1,n
+\end{equation}
+
+These constraints lead to simple equations for the view factors for* n* = 3 and 4. For \emph{n} = 3, we have the following geometry and view factor expression:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image1059.png}
+\caption{WindowHB\_1}
+\end{figure}
+
+For~ \emph{n} = 4~ we have:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image1060.png}
+\caption{WindowHB\_2}
+\end{figure}
+
+Applying these to the slat cell shown in Figure~\ref{fig:slat-cell-showing-geometry-for-calculation-of} we have the following:
+
+\begin{equation}
+{F_{12}} = \frac{{{d_1} + {d_2} - 2s}}{{2h}}
+\end{equation}
+
+\begin{equation}
+{F_{13}} = \frac{{h + {s_3} - {d_3}}}{{2h}}{\rm{ ,  etc}}{\rm{.}}
+\end{equation}
+
+\begin{figure}[hbtp] % fig 81
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1063.png}
+\caption{Slat cell showing geometry for calculation of view factors between the segments of the cell. \protect \label{fig:slat-cell-showing-geometry-for-calculation-of}}
+\end{figure}
+
+The sources for the direct-to-diffuse transmittance calculation are:
+
+\begin{equation}
+{Q_1} = {Q_2} = {Q_5} = {Q_6} = 0 \;  (and therefore) {J_1} = {J_2} = 0
+\end{equation}
+
+\begin{equation}
+\left. 
+    \begin{array}{l}
+      Q_3 = \tau_{dir,dif} \\
+      Q_4 = \rho_{dir,dif}^f 
+    \end{array} 
+  \right\} 
+  \;
+  \varphi_b \le \varphi_s + \frac{\pi }{2} 
+  \;
+  \rm{ (beam hits front of slats)}
+\end{equation}
+
+\begin{equation}
+\left.
+    \begin{array}{l}
+      Q_3 = \rho_{dir,dif}^b \\
+      Q_4 = \tau_{dir,dif}
+    \end{array}
+  \right\}
+  \;
+  \varphi_b > \varphi_s + \frac{\pi }{2}
+  \;
+  \rm{ (beam hits back of slats)}
+\end{equation}
+
+For unit incident direct flux, the front direct-to-diffuse transmittance and reflectance of the blind are:
+
+\begin{equation}
+  \begin{array}{l}
+    \tau_{bl,f}^{dir,dif} = {G_2} \\
+    \rho_{bl,f}^{dir,dif} = {G_1}
+  \end{array}
+\end{equation}
+
+where
+
+\begin{equation}
+  \begin{array}{l}
+    G_2 = \sum_{j = 3}^6 J_j F_{j2} \\
+    G_1 = \sum_{j = 3}^6 J_j F_{j1} 
+  \end{array}
+\end{equation}
+
+and \({J_3}\) to \({J_6}\) are given by Eq. .~
+
+The front direct absorptance of the blind is then
+
+\begin{equation}
+\alpha_{bl,f}^{dir} = 1 - \tau_{bl,f}^{dir,dif} - \tau_{bl,f}^{dir,dir} - \rho_{bl,f}^{dir,dif}
+\end{equation}
+
+The direct-to-diffuse calculations are performed separately for solar and visible slat properties to get the corresponding solar and visible blind properties.
+
+\subsubsection{Dependence on Profile Angle}\label{dependence-on-profile-angle}
+
+The direct-to-direct and direct-to-diffuse blind properties are calculated for direct radiation profile angles (see Figure~\ref{fig:a-side-view-of-a-cell-formed-by-adjacent}) ranging from --90\(^{O}\) to +90\(^{O}\) in 5\(^{O}\) increments. (The ``profile angle'' is the angle of incidence in a plane that is perpendicular to the window \emph{and} perpendicular to the slat direction.) In the time step loop the blind properties for a particular profile angle are obtained by interpolation.
+
+\subsubsection{Dependence on Slat Angle}\label{dependence-on-slat-angle}
+
+All blind properties are calculated for slat angles ranging from --90\(^{O}\) to +90\(^{O}\) in 10\(^{O}\) increments. In the time-step loop the slat angle is determined by the slat-angle control mechanism and then the blind properties at that slat angle are determined by interpolation. Three slat-angle controls are available: (1) slat angle is adjusted to just block beam solar incident on the window; (2) slat angle is determined by a schedule; and (3) slat angle is fixed.
+
+\subsubsection{Diffuse-to-Diffuse Transmittance and Reflectance of Blind}\label{diffuse-to-diffuse-transmittance-and-reflectance-of-blind}
+
+To calculate the diffuse-to-diffuse properties, assuming uniformly distributed incident diffuse radiation, each slat bounding the cell is divided into two segments of equal length (Figure~\ref{fig:slat-cell-showing-arrangement-of-segments}), i.e., \({s_3} = {s_4}\) and \({s_5} = {s_6}\) .~ For front-side properties we have a unit source, \({Q_1} = 1\) .~ All the other \({Q_i}\) are zero. Using this source value, we apply the methodology described above to obtain \emph{G\(_{2}\)}and \emph{G\(_{1}\)}. We then have
+
+\begin{equation}
+\begin{array}{l}\tau_{bl,f}^{dif,dif} = {G_2}\\\rho_{bl,f}^{dif,dif} = {G_1}\\\alpha_{bl,f}^{dif} = 1 - \tau_{bl,f}^{dif,dif} - \rho_{bl,f}^{dif,dif}\end{array}
+\end{equation}
+
+The back-side properties are calculated in a similar way by setting \emph{Q\(_{2}\)} = 1 with the other \({Q_i}\) equal to zero.
+
+The diffuse-to-diffuse calculations are performed separately for solar, visible and IR slat properties to get the corresponding solar, visible and IR blind properties.
+
+\begin{figure}[hbtp] % fig 82
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1078.png}
+\caption{Slat cell showing arrangement of segments and location of source for calculation of diffuse-to-diffuse optical properties. \protect \label{fig:slat-cell-showing-arrangement-of-segments}}
+\end{figure}
+
+\subsubsection{Blind properties for sky and ground diffuse radiation}\label{blind-properties-for-sky-and-ground-diffuse-radiation}
+
+For horizontal slats on a vertical window (the most common configuration) the blind diffuse-to-diffuse properties will be sensitve to whether the radiation is incident upward from the ground or downward from the sky (Figure~\ref{fig:side-view-of-horizontal-slats-in-a-vertical}). For this reason we also calculate the following solar properties for a blind consisting of horizontal slats in a vertical plane:
+
+\(\tau_{bl,f}^{gnd - dif,dif} = {\rm{ }}\) front transmittance for ground diffuse solar
+
+\(\tau_{bl,f}^{sky - dif,dif} = {\rm{ }}\) front transmittance for sky diffuse solar
+
+$\rho_{bl,f}^{gnd - dif,dif} = $ front reflectance for ground diffuse solar
+
+\(\rho_{bl,f}^{sky - dif,dif} = {\rm{ }}\) front reflectance for sky diffuse solar
+
+\(\alpha_{bl,f}^{gnd - dif,dif} = {\rm{ }}\) front absorptance for ground diffuse solar
+
+\(\alpha_{bl,f}^{sky - dif,dif} = {\rm{ }}\) front absorptance for sky diffuse solar
+
+These are obtained by integrating over sky and ground elements, as shown in Figure~\ref{fig:side-view-of-horizontal-slats-in-a-vertical}, treating each element as a source of direct radiation of irradiance \(I({\phi_s})\) ~incident on the blind at profile angle \({\phi_s}\) . This gives:
+
+\begin{equation}
+\tau_{bl,f}^{sky - dif,dif} = \frac{{\int\limits_0^{\pi /2} {\left[ {\tau_{bl,f}^{dir,dir}({\phi_s}) + \tau_{bl,f}^{dir,dif}({\phi_s})} \right]{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}{{\int\limits_0^{\pi /2} {{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}
+\end{equation}
+
+\begin{equation}
+\rho_{bl,f}^{sky - dif,dif} = \frac{{\int\limits_0^{\pi /2} {\rho_{bl,f}^{dir,dif}{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}{{\int\limits_0^{\pi /2} {{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}
+\end{equation}
+
+\begin{equation}
+\alpha_{bl,f}^{sky - dif} = \frac{{\int\limits_0^{\pi /2} {\alpha_{bl,f}^{dir}{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}{{\int\limits_0^{\pi /2} {{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}
+\end{equation}
+
+\begin{figure}[hbtp] % fig 83
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1090.png}
+\caption{Side view of horizontal slats in a vertical blind showing geometry for calculating blind transmission, reflection and absorption properties for sky and ground diffuse radiation. \protect \label{fig:side-view-of-horizontal-slats-in-a-vertical}}
+\end{figure}
+
+We assume that the sky radiance is uniform. This means that \({I_{sky}}\) is independent of \({\phi_s}\) , giving:
+
+\begin{equation}
+\tau_{bl,f}^{sky - dif,dif} = \int\limits_0^{\pi /2} {\left[ {\tau_{bl,f}^{dir,dir} + \tau_{bl,f}^{dir,dif}} \right]\cos {\phi_s}d{\phi_s}}
+\end{equation}
+
+\begin{equation}
+\rho_{bl,f}^{sky - dif,dif} = \int\limits_0^{\pi /2} {\rho_{bl,f}^{dir,dif}\cos {\phi_s}d{\phi_s}}
+\end{equation}
+
+\begin{equation}
+\alpha_{bl,f}^{sky - dif} = \int\limits_0^{\pi /2} {\alpha_{bl,f}^{dir}\cos {\phi_s}d{\phi_s}}
+\end{equation}
+
+The corresponding ground diffuse quantities are obtained by integrating \({\phi_s}\) ~from \(- \pi /2\) ~to 0.
+
+An improvement to this calculation would be to allow the sky radiance distribution to be non-uniform, i.e.,~ to depend on sun position and sky conditions, as is done in the detailed daylighting calculation (see ``Sky Luminance Distributions'' under ``Daylight Factor Calculation'').
+
+\subsubsection{Correction Factor for Slat Thickness}\label{correction-factor-for-slat-thickness}
+
+A correction has to be made to the blind transmittance, reflectance and absorptance properties to account for the amount of radiation incident on a blind that is reflected and absorbed by the slat edges (the slats are assumed to be opaque to radiation striking the slat edges). This is illustrated in Figure~\ref{fig:side-view-of-slats-showing-geometry-for} for the case of direct radiation incident on the blind. The slat cross-section is assumed to be rectangular. The quantity of interest is the fraction, \emph{f\(_{edge}\)}, of direct radiation incident on the blind that strikes the slat edges. Based on the geometry shown in Figure~\ref{fig:side-view-of-slats-showing-geometry-for} we see that
+
+\begin{equation}
+{f_{edge}} = \frac{{t\cos \gamma }}{{\left( {h + \frac{t}{{\cos \xi }}} \right)\cos {\varphi_s}}} = \frac{{t\cos ({\varphi_s} - \xi )}}{{\left( {h + \frac{t}{{\cos \xi }}} \right)\cos {\varphi_s}}} = \frac{{t\sin ({\varphi_b} - {\varphi_s})}}{{\left( {h + \frac{t}{{\sin {\varphi_b}}}} \right)\cos {\varphi_s}}}
+\end{equation}
+
+The edge correction factor for diffuse incident radiation is calculated by averaging this value of \emph{f\(_{edge}\)} over profile angles, \emph{φ\(_{s}\)}, from --90\(^{O}\) to +90\(^{O}\).
+
+As an example of how the edge correction factor is applied, the following two equations show how blind front diffuse transmittance and reflectance calculated assuming zero slat thickness are modified by the edge correction factor. It is assumed that the edge transmittance is zero and that the edge reflectance is the same as the slat front reflectance, \emph{�\(_{f}\)}.
+
+\begin{equation}
+\begin{array}{l}\tau_{bl,f}^{dif,dif} \to \tau_{bl,f}^{dif,dif}\left( {1 - {f_{edge}}} \right)\\\rho_{bl,f}^{dif} \to \rho_{bl,f}^{dif}\left( {1 - {f_{edge}}} \right) + {f_{edge}}{\rho_f}\end{array}
+\end{equation}
+
+\begin{figure}[hbtp] % fig 84
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1100.png}
+\caption{Side view of slats showing geometry for calculation of slat edge correction factor for incident direct radiation. \protect \label{fig:side-view-of-slats-showing-geometry-for}}
+\end{figure}
+
+\subsubsection{Comparison with ISO 15099 Calculation of Blind Optical Properties}\label{comparison-with-iso-15099-calculation-of-blind-optical-properties}
+
+Table~\ref{table:comparison-of-blind-optical-properties} compares EnergyPlus and ISO 15099 {[}2001{]} calculations of blind optical properties for a variety of profile angles, slat angles and slat optical properties. The ISO 15099 calculation method is similar to that used in EnergyPlus, except that the slats are divided into five equal segments. The ISO 15099 and EnergyPlus results agree to within 12\%, except for the solar transmittances for the 10-degree slat angle case. Here the transmittances are small (from 1\% to about 5\%) but differ by about a factor of up to two between ISO 15099 and EnergyPlus. This indicates that the slats should be divided into more than two segments at small slat angles.
+
+% table 33
+\begin{longtable}[c]{p{1.0in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}p{0.4in}}
+\caption{Comparison of blind optical properties calculated with the EnergyPlus and ISO 15099 methods. EnergyPlus values that differ by more than 12\% from ISO 15099 values are shown in bold italics. \label{table:comparison-of-blind-optical-properties}} \tabularnewline
+\toprule 
+\multicolumn{11}{l}{\textbf{Slat Properties}} \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Comparison of blind optical properties calculated with the EnergyPlus and ISO 15099 methods. EnergyPlus values that differ by more than 12\% from ISO 15099 values are shown in bold italics.} \tabularnewline
+\toprule 
+\multicolumn{11}{l}{\textbf{Slat Properties}} \tabularnewline
+\midrule
+\endhead
+
+Separation (m) & \multicolumn{2}{c}{0.012} & \multicolumn{2}{c}{0.012} & \multicolumn{2}{c}{0.012} & \multicolumn{2}{c}{0.012} & \multicolumn{2}{c}{0.012} \tabularnewline
+Width (m) & \multicolumn{2}{c}{0.016} & \multicolumn{2}{c}{0.016} & \multicolumn{2}{c}{0.016} & \multicolumn{2}{c}{0.016} & \multicolumn{2}{c}{0.016} \tabularnewline
+Angle (deg) & \multicolumn{2}{c}{45} & \multicolumn{2}{c}{45} & \multicolumn{2}{c}{45} & \multicolumn{2}{c}{10} & \multicolumn{2}{c}{45} \tabularnewline
+IR transmittance & \multicolumn{2}{c}{0} & \multicolumn{2}{c}{0} & \multicolumn{2}{c}{0} & \multicolumn{2}{c}{0} & \multicolumn{2}{c}{0.4} \tabularnewline
+IR emissivity, front side & \multicolumn{2}{c}{0.9} & \multicolumn{2}{c}{0.9} & \multicolumn{2}{c}{0.9} & \multicolumn{2}{c}{0.9} & \multicolumn{2}{c}{0.55} \tabularnewline
+IR emissivity, back side & \multicolumn{2}{c}{0.9} & \multicolumn{2}{c}{0.9} & \multicolumn{2}{c}{0.9} & \multicolumn{2}{c}{0.9} & \multicolumn{2}{c}{0.55} \tabularnewline
+Solar transmittance & \multicolumn{2}{c}{0} & \multicolumn{2}{c}{0} & \multicolumn{2}{c}{0} & \multicolumn{2}{c}{0} & \multicolumn{2}{c}{0.4} \tabularnewline
+Solar reflectance, front side & \multicolumn{2}{c}{0.7} & \multicolumn{2}{c}{0.55} & \multicolumn{2}{c}{0.7} & \multicolumn{2}{c}{0.7} & \multicolumn{2}{c}{0.5} \tabularnewline
+Solar reflectance, back side & \multicolumn{2}{c}{0.7} & \multicolumn{2}{c}{0.55} & \multicolumn{2}{c}{0.4} & \multicolumn{2}{c}{0.4} & \multicolumn{2}{c}{0.5} \tabularnewline \midrule
+ \tabularnewline \midrule
+Solar Profile angle (deg) & 0 & 60 & 0 & 60 & 0 & 60 & 0 & 60 & 0 & 60 \tabularnewline \midrule
+ \tabularnewline \midrule
+\multicolumn{11}{l}{\textbf{Calculated blind properties} (first row = ISO 15099 calculation,} \tabularnewline
+\multicolumn{11}{l}{second row (in italics) = EnergyPlus calculation)} \tabularnewline \midrule
+Front solar transmittance, direct to Direct & 0.057 \quad \quad \textit{0.057} & 0 \quad \quad \textit{0} & 0.057 \quad \quad \textit{0.057} & 0 \quad \quad \textit{0} & 0.057 \quad \quad \textit{0.057} & 0 \quad \quad \textit{0} & 0 \quad \quad \textit{0} & 0 \quad \quad \textit{0} & 0.057 \quad \quad \textit{0.057} & 0 \quad \quad \textit{0} \tabularnewline
+Back solar transmittance, direct to direct & 0.057 \quad \quad \textit{0.057} & 0.310 \quad \quad \textit{0.309} & 0.057 \quad \quad \textit{0.057} & 0.310 \quad \quad \textit{0.309} & 0.057 \quad \quad \textit{0.057} & 0.310 \quad \quad \textit{0.309} & 0 \quad \quad \textit{0} & 0.088 \quad \quad \textit{0.087} & 0.057 \quad \quad \textit{0.057} & 0.310 \quad \quad \textit{0.309} \tabularnewline
+Front solar transmittance, direct to diffuse & 0.141 \quad \quad \textit{0.155} & 0.073 \quad \quad \textit{0.074} & 0.090 \quad \quad \textit{0.100} & 0.047 \quad \quad \textit{0.048} & 0.096 \quad \quad \textit{0.104} & 0.051 \quad \quad \textit{0.051} & 0.012 \quad \quad \textbf{\textit{0.019}} & 0.005 \quad \quad \textbf{\textit{0.006}} & 0.373 \quad \quad \textit{0.375} & 0.277 \quad \quad \textit{0.275} \tabularnewline
+Back solar transmittance, direct to diffuse & 0.141 \quad \quad \textit{0.155} & 0.288 \quad \quad \textit{0.284} & 0.090 \quad \quad \textit{0.100} & 0.216 \quad \quad \textit{0.214} & 0.076 \quad \quad \textit{0.085} & 0.271 \quad \quad \textit{0.269} & 0.011 \quad \quad \textbf{\textit{0.019}} & 0.027 \quad \quad \textbf{\textit{0.052}} & 0.373 \quad \quad \textit{0.375} & 0.306 \quad \quad \textit{0.304} \tabularnewline
+Front solar reflectance, direct to diffuse & 0.394 \quad \quad \textit{0.389} & 0.558 \quad \quad \textit{0.558} & 0.295 \quad \quad \textit{0.293} & 0.430 \quad \quad \textit{0.431} & 0.371 \quad \quad \textit{0.368} & 0.544 \quad \quad \textit{0.546} & 0.622 \quad \quad \textit{0.636} & 0.678 \quad \quad \textit{0.679} & 0.418 \quad \quad \textit{0.416} & 0.567 \quad \quad \textit{0.568} \tabularnewline
+Back solar reflectance, direct to diffuse & 0.394 \quad \quad \textit{0.389} & 0.103 \quad \quad \textit{0.115} & 0.295 \quad \quad \textit{0.293} & 0.066 \quad \quad \textit{0.074} & 0.216 \quad \quad \textit{0.214} & 0.070 \quad \quad \textit{0.077} & 0.356 \quad \quad \textit{0.363} & 0.273 \quad \quad \textit{0.272} & 0.418 \quad \quad \textit{0.416} & 0.273 \quad \quad \textit{0.275} \tabularnewline
+Front solar transmittance, hemispherical diffuse to diffuse & 0.332 \quad \quad \textit{0.338} &  & 0.294 \quad \quad \textit{0.298} &  & 0.291 \quad \quad \textit{0.295} &  & 0.038 \quad \quad \textbf{\textit{0.053}} &  & 0.495 \quad \quad \textit{0.502} \tabularnewline
+Back solar transmittance, hemispherical diffuse to diffuse & 0.332 \quad \quad \textit{0.338} &  & 0.294 \quad \quad \textit{0.298} &  & 0.291 \quad \quad \textit{0.295} &  & 0.038 \quad \quad \textbf{\textit{0.053}} &  & 0.495 \quad \quad \textit{0.502} &  \tabularnewline
+Front hemispherical IR transmittance & 0.227 \quad \quad \textit{0.227} &  & 0.227 \quad \quad \textit{0.227} &  & 0.227 \quad \quad \textit{0.227} &  & 0.0245 \quad \quad \textit{0.025} &  & 0.385 \quad \quad \textit{0.387} &  \tabularnewline
+Back hemispherical IR transmittance & 0.227 \quad \quad \textit{0.227} &  & 0.227 \quad \quad \textit{0.227} &  & 0.227 \quad \quad \textit{0.227} &  & 0.0245 \quad \quad \textit{0.025} &  & 0.385 \quad \quad \textit{0.387} &  \tabularnewline
+Front hemispherical IR emissivity & 0.729 \quad \quad \textit{0.730} &  & 0.729 \quad \quad \textit{0.730} &  & 0.729 \quad \quad \textit{0.730} &  & 0.890 \quad \quad \textit{0.895} &  & 0.536 \quad \quad \textit{0.534} &  \tabularnewline
+Back hemispherical IR emissivity & 0.729 \quad \quad \textit{0.730} &  & 0.729 \quad \quad \textit{0.730} &  & 0.729 \quad \quad \textit{0.730} &  & 0.890 \quad \quad \textit{0.895} &  & 0.536 \quad \quad \textit{0.534} &  \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Blind/Glazing System Properties for Short-Wave Radiation}\label{blindglazing-system-properties-for-short-wave-radiation}
+
+When a blind is in place we have the following expressions for the system transmittance, the system glass layer absorptance, and the system blind absorptance, taking inter-reflection between blind and glazing into account. The system properties, indicated by ``sys,'' are given in terms of the isolated blind properties (i.e., blind properties in the absence of the glazing)---indicated by ``bl'' ---and the isolated glazing properties (i.e., glazing properties in the absence of the blind)---indicated by ``gl.''
+
+\subsubsection{Interior Blind}\label{interior-blind}
+
+The system properties when an interior blind is in place are the following:
+
+\begin{equation}
+T_{f,sys}^{dir,all}(\phi ,{\phi_s}) = T_{gl}^{dir}(\phi )\left( {\tau_{bl,f}^{dir,dir}({\phi_s}) + \tau_{bl,f}^{dir,dif}({\phi_s}) + \frac{{\tau_{bl,f}^{dif}\rho_{bl,f}^{dir,dif}({\phi_s})R_{gl,b}^{dif}}}{{1 - \rho_{bl,f}^{dif}R_{gl,b}^{dif}}}} \right)
+\end{equation}
+
+\begin{equation}
+A_{gl,j,f}^{dir,sys}(\phi ,{\phi_s}) = A_{gl,j,f}^{dir}(\phi ) + \frac{{T_{gl}^{dir}(\phi )\alpha_{gl,j,b}^{dif}\rho_{bl,f}^{dir}({\phi_s})}}{{1 - \rho_{bl,f}^{dir}({\phi_s})R_{gl,b}^{dif}}}{\rm{,    }}j = 1,N
+\end{equation}
+
+\begin{equation}
+\alpha_{bl,f}^{dir,sys}(\phi ,{\phi_s}) = T_{gl}^{dir}(\phi )\left( {\alpha_{bl,f}^{dir}({\phi_s}) + \frac{{\rho_{bl,f}^{dir}({\phi_s})R_{gl,b}^{dif}\alpha_{bl,f}^{dif}}}{{1 - \rho_{bl,f}^{dif}R_{gl,b}^{dif}}}} \right)
+\end{equation}
+
+\begin{equation}
+T_{f,sys}^{dif,dif} = \frac{{T_{gl}^{dif}\tau_{bl,f}^{dif,dif}}}{{1 - \rho_{bl,f}^{dif}R_{gl,b}^{dif}}}
+\end{equation}
+
+\begin{equation}
+T_{f,sys}^{sky - dif,dif} = \frac{{T_{gl}^{dif}\tau_{bl,f}^{sky - dif,dif}}}{{1 - \rho_{bl,f}^{sky - dif}R_{gl,b}^{dif}}}
+\end{equation}
+
+\begin{equation}
+T_{f,sys}^{gnd - dif,dif} = \frac{{T_{gl}^{dif}\tau_{bl,f}^{gnd - dif,dif}}}{{1 - \rho_{bl,f}^{gnd - dif}R_{gl,b}^{dif}}}
+\end{equation}
+
+\begin{equation}
+A_{gl,j,f}^{dif,sys} = A_{gl,j,f}^{dif} + \frac{{T_{gl}^{dif}\rho_{bl,f}^{dif}A_{gl,j,b}^{dif}}}{{1 - \rho_{bl,f}^{dif}R_{gl,b}^{dif}}}{\rm{,    }}j = 1,N
+\end{equation}
+
+\begin{equation}
+A_{gl,j,f}^{sky - dif,sys} = A_{gl,j,f}^{dif} + \frac{{T_{gl}^{dif}\rho_{bl,f}^{sky - dif}A_{gl,j,b}^{dif}}}{{1 - \rho_{bl,f}^{sky - dif}R_{gl,b}^{dif}}}{\rm{,    }}j = 1,N
+\end{equation}
+
+\begin{equation}
+A_{gl,j,f}^{gnd - dif,sys} = A_{gl,j,f}^{dif} + \frac{{T_{gl}^{dif}\rho_{bl,f}^{gnd - dif}A_{gl,j,b}^{dif}}}{{1 - \rho_{bl,f}^{gnd - dif}R_{gl,b}^{dif}}}{\rm{,    }}j = 1,N
+\end{equation}
+
+\begin{equation}
+\alpha_{bl,f}^{dif,sys} = \frac{{T_{gl}^{dif}\alpha_{bl,f}^{dif}}}{{1 - \rho_{bl,f}^{dif}R_{gl,b}^{dif}}}
+\end{equation}
+
+\begin{equation}
+\alpha_{bl,f}^{sky - dif,sys} = \frac{{T_{gl}^{dif}\alpha_{bl,f}^{sky - dif}}}{{1 - \rho_{bl,f}^{sky - dif}R_{gl,b}^{dif}}}
+\end{equation}
+
+\begin{equation}
+\alpha_{bl,f}^{gnd - dif,sys} = \frac{{T_{gl}^{dif}\alpha_{bl,f}^{gnd - dif}}}{{1 - \rho_{bl,f}^{gnd - dif}R_{gl,b}^{dif}}}
+\end{equation}
+
+\subsubsection{Exterior Blind}\label{exterior-blind}
+
+The system properties when an exterior blind is in place are the following:
+
+\begin{equation}
+T_{f,sys}^{dir,all}(\phi ,{\phi_s}) = \tau_{bl,f}^{dir,dir}({\phi_s})\left( {T_{gl}^{dir}(\phi ) + \frac{{T_{gl}^{dif}R_{gl,f}^{dir}\rho_{bl,b}^{dir,dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}} \right) + \frac{{\tau_{bl}^{dir,dif}({\phi_s})T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}
+\end{equation}
+
+\begin{equation}
+A_{gl,j,f}^{dir,sys}(\phi ,\phi_s) = 
+     \tau_{bl,f}^{dir,dir}(\phi_s) A_{gl,j,f}^{dir}(\phi ) + 
+     \frac{
+       \left(
+         \tau_{bl,f}^{dir,dir}(\phi_s) R_{gl}^{dir}(\phi) \rho_{bl,b}^{dir}(\phi_s)+ \tau_{bl,f}^{dir,dif}(\phi_s)
+       \right) A_{gl,j,f}^{dif}
+     } {
+       1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}
+     },\;j = 1,N
+\end{equation}
+
+\begin{equation}
+\begin{split}
+\alpha_{bl,f}^{dir,sys}(\phi ,\phi_s) =& \alpha_{bl,f}^{dir}(\phi_s) + \alpha_{bl,b}^{dir}(\phi_s) R_{gl,f}^{dir}(\phi) \tau_{bl,f}^{dir,dir}(\phi_s) \\
+&+ \frac{\alpha_{bl,b}^{dif}R_{gl,f}^{dif}}{1 - \rho_{bl,b}^{dif} R_{gl,f}^{dif}}\left(R_{gl,f}^{dir}(\phi) \tau_{bl,f}^{dir,dir}(\phi_s) \rho_{bl,b}^{dir}(\phi_s) + \tau_{bl,f}^{dir,dif}(\phi_s) \right)
+\end{split}
+\end{equation}
+
+\begin{equation}
+T_{f,sys}^{dif,dif} = \frac{{\tau_{bl,f}^{dif,dif}T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}
+\end{equation}
+
+\begin{equation}
+T_{f,sys}^{sky - dif,dif} = \frac{{\tau_{bl,f}^{sky - dif,dif}T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}
+\end{equation}
+
+\begin{equation}
+T_{f,sys}^{gnd - dif,dif} = \frac{{\tau_{bl,f}^{gnd - dif,dif}T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}
+\end{equation}
+
+\begin{equation}
+A_{gl,j,f}^{dif,sys} = \frac{{\tau_{bl,f}^{dif,dif}A_{gl,j,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}},{\rm{    }}j = 1,N
+\end{equation}
+
+\begin{equation}
+A_{gl,j,f}^{sky - dif,sys} = \frac{{\tau_{bl,f}^{sky - dif,dif}A_{gl,j,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}},{\rm{    }}j = 1,N
+\end{equation}
+
+\begin{equation}
+A_{gl,j,f}^{gnd - dif,sys} = \frac{{\tau_{bl,f}^{gnd - dif,dif}A_{gl,j,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}},{\rm{    }}j = 1,N
+\end{equation}
+
+\begin{equation}
+\alpha_{bl,f}^{dif,sys} = \alpha_{bl,f}^{dif} + \frac{{\tau_{bl,f}^{dif,dif}R_{gl,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}\alpha_{bl,b}^{dif}
+\end{equation}
+
+\begin{equation}
+\alpha_{bl,f}^{sky - dif,sys} = \alpha_{bl,f}^{sky - dif} + \frac{{\tau_{bl,f}^{sky - dif,dif}R_{gl,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}\alpha_{bl,b}^{dif}
+\end{equation}
+
+\begin{equation}
+\alpha_{bl,f}^{gnd - dif,sys} = \alpha_{bl,f}^{gnd - dif} + \frac{{\tau_{bl,f}^{gnd - dif,dif}R_{gl,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}\alpha_{bl,b}^{dif}
+\end{equation}
+
+\subsubsection{Blind/Glazing System Properties for Long-Wave Radiation}\label{blindglazing-system-properties-for-long-wave-radiation}
+
+The program calculates how much long-wave radiation is absorbed by the blind and by the adjacent glass surface. The effective emissivity (long-wave absorptance) of an interior or exterior blind, taking into account reflection of long-wave radiation between the glass and blind, is given by
+
+\begin{equation}
+\varepsilon_{bl}^{lw,eff} = \varepsilon_{bl}^{lw}\left( {1 + \frac{{\tau_{bl}^{lw}\rho_{gl}^{lw}}}{{1 - \rho_{bl}^{lw}\rho_{gl}^{lw}}}} \right)
+\end{equation}
+
+where \(\rho_{gl}^{lw}\) is the long-wave reflectance of the outermost glass surface for an exterior blind or the innermost glass surface for an interior blind, and it is assumed that the long-wave transmittance of the glass is zero.
+
+The effective innermost (for interior blind) or outermost (for exterior blind) glass surface emissivity when the blind is present is
+
+\begin{equation}
+\varepsilon_{gl}^{lw,eff} = \varepsilon_{gl}^{lw}\frac{{\tau_{bl}^{lw}}}{{1 - \rho_{bl}^{lw}\rho_{gl}^{lw}}}
+\end{equation}
+
+The effective inside surface emissivity is the sum of the effective blind and effective glass emissivities:
+
+\begin{equation}
+\varepsilon_{ins}^{lw,eff} = \varepsilon_{bl}^{lw,eff} + \varepsilon_{gl}^{lw,eff}
+\end{equation}
+
+The effective temperature of the blind/glazing combination that is used to calculate the window's contribution to the zone's mean radiant temperature (MRT) is given by
+
+\begin{equation}
+T_{}^{eff} = \frac{{\varepsilon_{bl}^{lw,eff}{T_{bl}} + \varepsilon_{gl}^{lw,eff}{T_{gl}}}}{{\varepsilon_{bl}^{lw,eff} + \varepsilon_{gl}^{lw,eff}}}
+\end{equation}
+
+\subsubsection{Solar Radiation Transmitted and Absorbed by a Window/Blind System}\label{solar-radiation-transmitted-and-absorbed-by-a-windowblind-system}
+
+Let the direct solar incident on the window be
+
+\begin{equation}
+{I_{dir,inc}} = {f_{sunlit}}{I_{dir,norm}}\cos \phi {\rm{    }}(W/{m^2})
+\end{equation}
+
+where \({f_{sunlit}}\) is the fraction of the window that is sunlit (determined by the shadowing calculations), \({I_{dir,norm}}\) is the direct normal solar irradiance, and \(\phi\) ~is the angle of incidence.
+
+Let \({I_{sky,inc}}\) be the irradiance on the window due to diffuse solar radiation from the sky (W/m\(^{2}\)) and let \({I_{gnd,inc}}\) be the irradiance on the window due to diffuse solar radiation from the ground (W/m\(^{2}\)).
+
+Then we have the following expressions for different classes of transmitted and absorbed solar radiation for the window/blind system (where \({\phi_s}\) is the direct solar profile angle), all in W/m\(^{2}\):
+
+\emph{Direct solar entering zone from incident direct solar:}
+
+\begin{equation}
+{I_{dir,inc}}T_{f,sys}^{dir,dir}(\phi ,{\phi_s})
+\end{equation}
+
+\emph{Diffuse solar entering zone from incident direct solar:}
+
+\begin{equation}
+{I_{dir,inc}}T_{f,sys}^{dir,dif}(\phi ,{\phi_s})
+\end{equation}
+
+\emph{Direct solar absorbed by blind:}
+
+\begin{equation}
+{I_{dir,inc}}\alpha_{bl,f}^{dir,sys}(\phi ,{\phi_s})
+\end{equation}
+
+\emph{Direct solar absorbed by glass layers:}
+
+\begin{equation}
+{I_{dir,inc}}A_{gl,j,f}^{dir,sys}(\phi ,{\phi_s}),{\rm{    }}j = 1,N
+\end{equation}
+
+\subsubsection{For windows whose blinds have vertical slats:}\label{for-windows-whose-blinds-have-vertical-slats}
+
+\emph{Diffuse solar entering zone from incident diffuse solar:}
+
+\begin{equation}
+({I_{sky,inc}} + {I_{gnd,inc}})T_{f,sys}^{dif,dif}
+\end{equation}
+
+\emph{Diffuse solar absorbed by blind:}
+
+\begin{equation}
+({I_{sky,inc}} + {I_{gnd,inc}})\alpha_{bl,f}^{dif,sys}
+\end{equation}
+
+\emph{Diffuse solar absorbed by glass layers:}
+
+\begin{equation}
+({I_{sky,inc}} + {I_{gnd,inc}})A_{gl,j,f}^{dif,sys},{\rm{   }}j = 1,N{\rm{ }}
+\end{equation}
+
+\subsubsection{\texorpdfstring{For windows of tilt angle \(\gamma\) ~whose blinds have horizontal slats:}{For windows of tilt angle \textbackslash{}gamma ~whose blinds have horizontal slats:}}\label{for-windows-of-tilt-angle-gamma-whose-blinds-have-horizontal-slats}
+
+(vertical windows have tilt = 90\(^{O}\), horizontal windows have tilt = 0\(^{O}\))
+
+\emph{Diffuse solar entering zone from incident diffuse solar:}
+
+\begin{equation}
+\begin{split}
+T_{f,sys}^{sky - dif,dif}\left[ {\left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{sky,inc}} + \frac{{|\cos \gamma |}}{2}{I_{gnd,inc}}} \right] + \\
+T_{f,sys}^{gnd - dif,dif}\left[ {\frac{{|\cos \gamma |}}{2}{I_{sky,inc}} + \left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{gnd,inc}}} \right]
+\end{split}
+\end{equation}
+
+\emph{Diffuse solar absorbed by blind:}
+
+\begin{equation}
+\begin{split}
+\alpha_{bl,f}^{sky - dif,sys}\left[ {\left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{sky,inc}} + \frac{{|\cos \gamma |}}{2}{I_{gnd,inc}}} \right] + \\
+\alpha_{bl,f}^{gnd - dif,sys}\left[ {\frac{{|\cos \gamma |}}{2}{I_{sky,inc}} + \left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{gnd,inc}}} \right]
+\end{split}
+\end{equation}
+
+\emph{Diffuse solar absorbed by glass layers:}
+
+\begin{equation}
+\begin{array}{l}A_{gl,j,f}^{sky - dif,sys}\left[ {\left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{sky,inc}} + \frac{{|\cos \gamma |}}{2}{I_{gnd,inc}}} \right] + \\A_{gl,j,f}^{gnd - dif,sys}\left[ {\frac{{|\cos \gamma |}}{2}{I_{sky,inc}} + \left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{gnd,inc}}} \right],{\rm{    }}j = 1,N\end{array}
+\end{equation}
+
+\subsubsection{Screens}\label{screens}
+
+The model for window screens currently allows placement on the exterior surface of a window system (i.e., between glass and interior window screens can not be modeled). The exterior screen is modeled as a planar semi-transparent sheet having specular transmittance that is dependent on the angle of incidence of beam solar radiation. The screen transmittance algorithm includes two components. The first one, \emph{T\(_{beam}\)} (α', φ'), accounts for the blockage of the sun's rays by the screen material. This component accounts for the beam solar radiation passing through the screen openings without hitting the screen material. The second part, \emph{T\(_{scatt}\)}~ (α', φ'), accounts for the additional flux of transmitted beam solar radiation by diffuse reflectance (scattering) from the screen material. Since the reflected component is small compared with the incident beam and the direction of scattering is highly dependent on incident angle, the component of transmitted beam radiation due to screen material reflectance can be treated in one of three ways based on a user input to the model.
+
+The user may elect not to model the inward reflected beam transmittance due to the uncertainty of the direction of scattering or its low magnitude for low-reflecting screen materials. The user may alternately choose to model the inwardly-reflected transmitted beam as an additive component to the direct beam transmittance in the same solid angle and direction. Finally, the additional flux due to the inward reflection of direct beam radiation may be modeled as hemispherically-diffuse transmittance.
+
+This reflected beam transmittance component depends upon the diffuse (i.e., beam-to-diffuse) reflectance of the screen material, so this reflectance (�\(_{sc}\)) is a required input to the model. Guidance input values for this diffuse reflectance are provided, to account for screens that are dark, medium, or light colored in appearance, in the likely case that more accurate values for the material reflectance are difficult or time-consuming to obtain. If the diffuse reflectance of the screen material is known, use this value in place of the guidance provided.
+
+The model is based on an orthogonal crossed cylinder geometry in which the screen material's cylindrical diameter and spacing are known. The model assumes that the screen material diameter and spacing are the same in both directions. Figure~\ref{fig:screen-model-rendering-of-intersecting} shows a rendering of intersecting orthogonal crossed cylinders used as the basis for the EnergyPlus screen model.
+
+\begin{figure}[hbtp] % fig 85
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1148.png}
+\caption{Screen model rendering of intersecting orthogonal crossed cylinders \protect \label{fig:screen-model-rendering-of-intersecting}}
+\end{figure}
+
+If the required screen material dimensions are not available from the manufacturer, they may be determined using the following procedure:
+
+\begin{itemize}
+\item
+  Lay the screen next to a finely-divided scale or ruler. A magnifying glass may be helpful in determining the screen material dimensions. Alternately, a photograph can be taken and the image enlarged.
+\item
+  Determine the diameter \emph{D} of an individual screen material ``cylinder''. Average the diameter values if different in opposing directions.
+\item
+  Determine the average center-to-center spacing \emph{S} of the screen material or measure from one side of a ``cylinder'' to the same side of the next ''cylinder'' and record the spacing \emph{S}. Average the spacing values if different in opposing directions.
+\item
+  Enter these values as inputs to the exterior window screen model.
+\end{itemize}
+
+The screen material diameter and spacing are then used to determine the screen material aspect ratio for use in the screen model.
+
+\begin{equation}
+\gamma  = {D \mathord{\left/ {\vphantom {D S}} \right. } S}
+\end{equation}
+
+where
+
+\(\gamma\) ~~ = Screen material aspect ratio, dimensionless
+
+\(D\) ~ = Screen material diameter, m
+
+\(S\) ~ = Screen material spacing, m
+
+Figure~\ref{fig:physical-screen-material-properties} below shows the input requirements for material diameter and spacing and the associated calculation for openness factor, the equivalent to \emph{T\(_{beam}\)} at direct normal incidence.
+
+\begin{figure}[hbtp] % fig 86
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1153.png}
+\caption{Physical screen material properties \protect \label{fig:physical-screen-material-properties}}
+\end{figure}
+
+\subsection{Screen Properties and Calculations}\label{screen-properties-and-calculations}
+
+\subsubsection{Screen Beam Transmittance}\label{screen-beam-transmittance}
+
+The first component of the window screen transmittance model is a geometric representation of the open area of the screen material and is dependent on the angle of incident beam radiation. Figure~\ref{fig:schematic-of-a-vertical-window-screen-facing} shows a schematic of a South-facing vertical window screen and the solar angles used in EnergyPlus. The window screen model is based on the relative angles of incidence of the sun's rays with respect the the window screen outward normal. In the figure, the relative solar azimuth and relative solar altitude are represented as φ' and α', respectively.
+
+\begin{figure}[hbtp] % fig 87
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1154.png}
+\caption{Schematic of a vertical window screen facing due South \protect \label{fig:schematic-of-a-vertical-window-screen-facing}}
+\end{figure}
+
+Given the diffuse reflectance �\(_{sc}\) and the screen aspect ratio γ, the model takes the direction of solar incidence, the relative solar altitude angle α' and the relative solar azimuth angle φ', illustrated in Figure~\ref{fig:schematic-of-a-vertical-window-screen-facing}, and calculates the direct beam transmittance \emph{T\(_{beam}\)} (α', φ') as follows. Since the direct beam transmittance is only a function of the incident angle and the screen material aspect ratio, the following applies to both solar and visible radiation.
+
+\begin{equation}
+\alpha '' = {\rm{arctan}}\left( {\tan \alpha '\sec \varphi '} \right)
+\end{equation}
+
+\begin{equation}
+\beta  = \frac{\pi }{2} - \varphi '
+\end{equation}
+
+\begin{equation}
+{T_y} = 1 - \gamma \left[ {\cos \alpha '' + \sin \alpha ''\tan \alpha '{{\left( {1 + {{\cot }^2}\beta } \right)}^{\frac{1}{2}}}} \right]
+\end{equation}
+
+\begin{equation}
+\mu  = \arccos \left( {{{\left[ {{{\cos }^2}\alpha '{{\cos }^2}\varphi ' + {{\sin }^2}\alpha '} \right]}^{\frac{1}{2}}}} \right)
+\end{equation}
+
+\begin{equation}
+  \varepsilon  = \arccos \PB{\frac{\cos \alpha '\cos \varphi '}{\cos \mu}}
+\end{equation}
+
+\begin{equation}
+\eta  = \frac{\pi }{2} - \varepsilon
+\end{equation}
+
+\begin{equation}
+\mu ' = \arctan \left( {\tan \mu \sec \varepsilon } \right)
+\end{equation}
+
+\begin{equation}
+{T_x} = 1 - \gamma \left[ {\cos \mu ' + \sin \mu '\tan \mu {{\left( {1 + {{\cot }^2}\eta } \right)}^{\frac{1}{2}}}} \right]
+\end{equation}
+
+\begin{equation}
+{T_{beam}}\left( {\alpha ',\varphi '} \right) = T_{beam}^{vis}\left( {\alpha ',\varphi '} \right) = {T_x}{T_y}
+\end{equation}
+
+where
+
+\({T_y}\) ~ = vertical component of direct beam transmittance
+
+\({T_x}\) ~ = horizontal component of direct beam transmittance
+
+\({T_{beam}}\) ~ = direct screen transmittance that accounts for beam solar radiation passing through the screen openings without hitting the screen material
+
+\(T_{beam}^{vis}\) ~ = direct visible screen transmittance that accounts for beam solar radiation passing through the screen openings without hitting the screen material
+
+α'~~ = relative solar altitude angle {[}radians{]}
+
+φ'~~ = relative solar azimuth angle {[}radians{]}
+
+\(\gamma\) ~~ = Screen material aspect ratio, dimensionless
+
+\(\alpha '',\beta ,\mu ,\varepsilon ,\eta ,\mu '\) ~ = intermediate variables
+
+This first component of screen direct beam transmittance was developed using geometric principals and was verified using an optical ray tracing software program.
+
+The second component of the window screen transmittance model is an empirical algorithm that accounts for the inward reflection of incident beam radiation off the screen material surface. The calculation procedure for the screen's transmittance via beam reflection, \emph{T\(_{scatt}\)} (α', φ') is as follows:
+
+\begin{equation}
+\begin{array}{l}{T_{scattmax}} = 0.0229\,\gamma  + 0.2971\,{\rho_{sc}} - 0.03624\,{\gamma ^2}\, + \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,0.04763\,{\rho_{sc}}^2 - 0.44416\,\gamma \,{\rho_{sc}}\end{array}
+\end{equation}
+
+\begin{equation}
+\begin{array}{l}T_{scattmax}^{vis} = 0.0229\,\gamma  + 0.2971\,\rho_{sc}^{vis} - 0.03624\,{\gamma ^2}\, + \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,0.04763{\left( {\rho_{sc}^{vis}} \right)^2} - 0.44416\,\gamma \,\rho_{sc}^{vis}\end{array}
+\end{equation}
+
+\begin{equation}
+{\delta_{max}} = 89.7 - {{10\gamma } \mathord{\left/ {\vphantom {{10\gamma } {0.16}}} \right. } {0.16}}
+\end{equation}
+
+\begin{equation}
+\delta  = {\left( {\alpha_d^{'2} + \varphi_d^{'2}} \right)^{\frac{1}{2}}}
+\end{equation}
+
+\begin{equation}
+  Peak_{ratio} = \frac{1}{0.2{\rho_{sc}}\left( {1 - \gamma } \right)}
+\end{equation}
+
+\begin{equation}
+  Peak_{ratio}^{vis} = \frac{1}{0.2\rho_{sc}^{vis}\left( {1 - \gamma } \right)}
+\end{equation}
+
+\begin{equation}
+{T_{scatt}}\left( {\alpha ',\varphi '} \right) = 0.2{\rho_{sc}}{T_{scattmax}}\left( {1 - \gamma } \right)\left( {1 + \left( {Pea{k_{ratio}} - 1} \right){e^{\frac{{ - {{\left| {\delta  - {\delta_{max}}} \right|}^{2.0}}}}{{600}}}}} \right)
+\end{equation}
+
+\begin{equation}
+T_{scatt}^{vis}\left( {\alpha ',\varphi '} \right) = 0.2\rho_{sc}^{vis}T_{scattmax}^{vis}\left( {1 - \gamma } \right)\left( {1 + \left( {Peak_{ratio}^{vis} - 1} \right){e^{\frac{{ - {{\left| {\delta  - {\delta_{max}}} \right|}^{2.0}}}}{{600}}}}} \right)
+\end{equation}
+
+If $\delta > \delta_{max}$, then:
+
+\begin{equation}
+  \begin{array}{rl}
+    T_{scatt} \left( \alpha ',\varphi ' \right) &= 0.2 \rho_{sc} T_{scattmax} \left( 1 - \gamma \right) \left( 1 + \left( Peak_{ratio} - 1 \right) e^{\frac{- \left| \delta - \delta_{max} \right|^{2.5}}{600}} \right) \\
+                                                &- 0.2 \rho_{sc} T_{scattmax} \left( 1 - \gamma \right) \left( \max \left( 0.0, \frac{\delta  - \delta_{max}}{90. - {delta_{max}}} \right) \right) \\
+    T_{scatt}^{vis} \left( \alpha ',\varphi ' \right) &= 0.2 \rho_{sc}^{vis} T_{scattmax}^{vis} \left( 1 - \gamma \right) \left( 1 + \left( Peak_{ratio}^{vis} - 1 \right) e^{\frac{- \left| \delta - \delta_{max} \right|^{2.5}}{600}} \right) \\
+                                                      &- 0.2 \rho_{sc}^{vis} T_{scattmax}^{vis} \left( 1 - \gamma \right) \left( \max \left( 0.0, \frac{\delta  - \delta_{max}}{90. - {delta_{max}}} \right) \right)
+  \end{array}
+\end{equation}
+
+where
+
+\({T_{scattmax}}\) ~ = maximum reflected (scattered) beam transmittance
+
+\(T_{scattmax}^{vis}\) ~ = maximum visible reflected (scattered) beam transmittance
+
+\({\delta_{max}},\delta\) ~ = intermediate variables {[}degrees{]}
+
+\(\alpha_d'\) ~ = relative solar altitude {[}degrees{]}
+
+\(\varphi_d'\) ~ = relative solar azimuth {[}degrees{]}
+
+\(Pea{k_{ratio}}\) = Ratio of peak scattered beam transmittance to scattered beam transmittance at direct normal incidence.
+
+\(Peak_{ratio}^{vis}\) = Ratio of peak scattered visible transmittance to scattered visible transmittance at direct normal incidence.
+
+\({\rho_{sc}}\) = diffuse solar reflectance of the screen material
+
+\(\rho_{sc}^{vis}\) = diffuse visible reflectance of the screen material
+
+\({T_{scatt}}\) ~ = beam solar transmittance due to reflectance (scattering)
+
+\(T_{scatt}^{vis}\) ~ = beam visible transmittance due to reflectance (scattering)
+
+The reflected (scattered) transmittance of incident beam radiation is an empirical model derived by curvefitting results from optical ray trace modeling. Ray traces were performed for a range of screen aspect ratios, diffuse screen reflectances, and relative solar azimuth and altitude angles. The surface of the screen cylinders was assumed to be diffusely reflecting, having the optical properties of a Lambertian surface. The transmitted flux due to reflection was determined by a hemispherical detector on the transmitted side of the screen.
+
+These two components of beam solar transmittance are then used to specify the properties for beam-to-beam and beam-to-diffuse transmittance for the screen based on the user selection for Reflected Beam Transmittance Accounting Method in the WindowMaterial:Screen object. The calculations below apply to both the solar and visible beam solar transmittance.
+
+If the user selects DoNotModel, the direct beam transmittance is set to \emph{T\(_{beam}\)} and the reflected (scattered) portion of the beam solar transmittance is ignored:
+
+\begin{equation}
+T_{sc}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\begin{equation}
+T_{sc}^{dir,dif} = 0.0
+\end{equation}
+
+\begin{equation}
+T_{sc,\,vis}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\begin{equation}
+T_{sc,\,vis}^{dir,dif} = 0.0
+\end{equation}
+
+where
+
+\(T_{sc}^{dir,dir}\) ~ = direct-to-direct beam transmittance of the screen (output report variable Surface Window Screen Beam to Beam Solar Transmittance)
+
+\(T_{sc}^{dir,dif}\) = direct-to-diffuse beam transmittance of the screen (output report variable Surface Window Screen Beam to Diffuse Solar Transmittance)
+
+\(T_{sc,\,vis}^{dir,dir}\) ~ = direct-to-direct visible transmittance of the screen
+
+\(T_{sc,\,vis}^{dir,dif}\) = direct-to-diffuse visible transmittance of the screen
+
+If the user selects Model as Direct Beam, the reflected (scattered) portion of the beam solar transmittance is added to the direct beam transmittance \emph{T\(_{beam}\)} in the same solid angle and direction of the unattenuated solar beam:
+
+\begin{equation}
+T_{sc}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right) + {T_{scatt}}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\begin{equation}
+T_{sc}^{dir,dif} = 0.0
+\end{equation}
+
+\begin{equation}
+T_{sc,\,vis}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right) + T_{scatt}^{vis}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\begin{equation}
+T_{sc,\,vis}^{dir,dif} = 0.0
+\end{equation}
+
+If the user selects Model as Diffuse Beam, the direct beam transmittance is set to \emph{T\(_{beam}\)} and the reflected (scattered) portion of the beam solar transmittance is modeled as diffuse hemispherical radiation:
+
+\begin{equation}
+T_{sc}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\begin{equation}
+T_{sc}^{dir,dif} = {T_{scatt}}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\begin{equation}
+T_{sc,\,vis}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\begin{equation}
+T_{sc,\,vis}^{dir,dif} = T_{scatt}^{vis}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\subsubsection{Screen Beam Reflectance}\label{screen-beam-reflectance}
+
+The screen reflectance (overall value for the screen assembly, accounting for the screen material itself and the open spaces between the screen material) is calculated by first subtracting the direct-to-direct screen transmittance from the unit incident beam. This approximates the fraction of incident beam solar radiation striking the screen that is not inwardly transmitted. The result is then multiplied by the screen material diffuse reflectance �\(_{sc}\). The inwardly scattered transmittance is then subtracted from this quantity to obtain an approximate value for the screen's reflectance R\(_{sc}\) to beam radiation incident as a function of the relative angles of incident radiation. This equation is used for both beam and visible reflectance:
+
+\begin{equation}
+R_{SC}^{dir,dif}\left( {\alpha ',\varphi '} \right) = {\rho_{SC}}\left( {1 - T_{SC}^{dir,dir}} \right) - T_{SC}^{dir,dif}
+\end{equation}
+
+\begin{equation}
+R_{SC,vis}^{dir,dif}\left( {\alpha ',\varphi '} \right) = \rho_{SC}^{vis}\left( {1 - T_{SC,vis}^{dir,dir}} \right) - T_{SC,vis}^{dir,dif}
+\end{equation}
+
+\subsubsection{Screen Beam Absorptance}\label{screen-beam-absorptance}
+
+The screen absorptance(overall value for the screen assembly, accounting for the screen material itself and the open spaces between the screen material) is calculated as the quantity of the unit incident flux (1) less the directly-transmitted component \emph{T\(_{dir,dir}\)} multiplied by the quantity 1 minus the screen material diffuse reflectance.
+
+\begin{equation}
+A_{SC}^{dir}\left( {\alpha ',\varphi '} \right) = \left( {1 - T_{SC}^{dir,dir}} \right)\left( {1 - {\rho_{SC}}} \right)
+\end{equation}
+
+\subsubsection{Screen Diffuse Properties}\label{screen-diffuse-properties}
+
+The transmittance of the screen to half-hemispherical diffuse (sky) radiation is calculated by performing a finite-element-summation, approximately equivalent to an integration over the solid angle of the beam transmittance, assuming uniform radiance. This single-number screen diffuse transmittance is then multiplied by the irradiance incident on the screen from a uniform half-hemisphere of sky- or ground-reflected radiation to determine the level of additional flux transmitted by the screen to the window from the diffuse sky or ground. The sun angles shown in the figure below represent the solar altitude angle (θ) and solar azimuth angle (Ф) in polar coordinates. These angles are used to calculate the average diffuse-to-diffuse properties for screens in the following derivations.
+
+\begin{figure}[hbtp] % fig 88
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1210.png}
+\caption{Sun Angles in Screen Calculations. \protect \label{fig:sun-angles-in-screen-calculations.}}
+\end{figure}
+
+The screen transmittance to diffuse radiation \emph{T\(_{dif,dif}\)} (γ, �\(_{sc}\))~ is computed as the integrated average of the combined beam transmittance \emph{T\(_{tot}\)} (γ, �, θ, Ф) over the directions of incidence using spherical coordinates (θ, Ф) in which the z-axis is perpendicular to the plane of the screen. Using a finite element computation, this is:
+
+\begin{equation}
+{T_{tot}}(\gamma ,{\rho_{sc}},{\theta_j},{\phi_i}) = {T_{beam}}\left( {\alpha ',\varphi '} \right) + {T_{scatt}}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\begin{equation}
+T_{sc}^{dif,dif}(\gamma ,{\rho_{sc}}) = \frac{{\sum\limits_{j = 1}^N {\sum\limits_{i = 1}^M {{T_{tot}}(\gamma ,{\rho_{sc}},{\theta_j},{\phi_i})\sin ({\theta_j})\cos ({\theta_j})} } }}{{\sum\limits_{j = 1}^N {\sum\limits_{i = 1}^M {\sin ({\theta_j})\cos ({\theta_j})} } }}
+\end{equation}
+
+where
+
+\(\theta\) ~ = solar altitude angle in polar coordinates {[}radians{]}
+
+\(\phi\) ~ = solar azimuth angle in polar coordinates {[}radians{]}
+
+\(T_{sc}^{dif,dif}(\gamma ,{\rho_{sc}})\) = diffuse-diffuse transmittance (output report variable Surface Window Screen Diffuse to Diffuse Solar Transmittance)
+
+Similarly, the reflectance of the screen to diffuse radiation is given by
+
+\begin{equation}
+R_{sc}^{dif,dif}(\gamma ,{\rho_{sc}}) = \frac{{\sum\limits_{j = 1}^N {\sum\limits_{i = 1}^M {R_{sc}^{dir,dif}(\gamma ,{\rho_{sc}},{\theta_j},{\phi_i})\sin ({\theta_j})\cos ({\theta_j})} } }}{{\sum\limits_{j = 1}^N {\sum\limits_{i = 1}^M {\sin ({\theta_j})\cos ({\theta_j})} } }}
+\end{equation}
+
+There is an assumption in both of these formulas that the brightness of the sky (or ground) diffuse radiation is the same for all directions. For this reason, the solar azimuth angle Ф and solar altitude angle θ have a range of 0 to \({\pi \mathord{\left/ {\vphantom {\pi 2}} \right. } 2}\) ~(instead of \({{ - \pi } \mathord{\left/ {\vphantom {{ - \pi } 2}} \right. } 2}\) ~to \({{ + \pi } \mathord{\left/ {\vphantom {{ + \pi } 2}} \right. } 2}\) ) because the screen is assumed to have identical optical properties for radiation incident at the same angles on either side of a vertical or horizontal plane perpendicular to the screen.
+
+Since the screen direct transmittance model is derived with respect to a different coordinate axis labeling, a coordinate transform is needed in order to calculate the diffuse optical properties. In these calculations, for each spherical solar coordinates (θ, Ф) we need the corresponding screen relative solar coordinates (α', φ') to evaluate the screen transmittance model for that direction.
+
+For each θ and Ф in the summation, the corresponding values for the relative solar altitude α' and relative solar azimuth φ' needed to calculate screen transmittance are determined with the following coordinate transform equations:
+
+\begin{equation}
+\sin \alpha ' = \sin \theta \cos \phi
+\end{equation}
+
+\begin{equation}
+\tan \varphi ' = \tan \theta \sin \phi
+\end{equation}
+
+The absorptance of the screen to diffuse incident radiation is calculated by subtracting the diffuse transmittance and diffuse reflectance from unity as follows:
+
+\begin{equation}
+A_{sc}^{dif}(\gamma ,{\rho_{sc}}) = 1 - T_{sc}^{dif,dif}(\gamma ,{\rho_{sc}}) - R_{sc}^{dif,dif}(\gamma ,{\rho_{sc}})
+\end{equation}
+
+\subsubsection{Screen/Glass System Properties for Short-Wave Radiation}\label{screenglass-system-properties-for-short-wave-radiation}
+
+The combined system properties of the screen/glass combination are calculated using the properties of the screen in combination with the bare glass material properties. Interreflections of radiation between the screen and glass surfaces are included. The following infinite series serves as an example for calculating the combined screen/glass system properties. The terms of the series are built up as illustrated in the following figure. The terms shown at the right of the figure represent each term in the infinite series for the combined screen/glass property (beam transmittance in this example).
+
+For the example of beam transmittance, the incident solar beam strikes the screen at the incident angle associated with the current relative azimuth and altitude angle. The incident beam splits into reflected and transmitted components at the screen. The transmitted component is attenuated as it passes through the screen material by the screen's beam transmittance (\(T_{sc}^{dir,dir}\) , shown as\(T_{sc}^{dir}\) ~in the figure and equations below) at this incident angle. The reflected (scattered) transmittance of incident solar beam is also shown at this point and will be discussed later in this section. As the attenuated solar beam continues on towards the front glass surface, a portion of the screen-transmitted beam splits at the window surface into transmitted and reflected components. The reflected component reflects off the front surface of the glass material (\(T_{sc}^{dir,dir}R_{gl,f}^{dir}\) ) and the transmitted component continues to travel through the glass material and is further attenuated by the glass beam transmittance. Thus the first term of the combined screen/glass solar beam transmittance is shown as \(T_{sc}^{dir,dir}T_{gl}^{dir}\) . Interreflections are accounted for by following the beam as it continues to reflect off the front surface of the glass material and the back surface of the screen material. Continuing on with the glass-reflected beam (\(T_{sc}^{dir,dir}R_{gl,f}^{dir}\) ) described above, this beam strikes the back surface of the screen material at the same incident angle as the incident solar beam. This reflected beam is also assumed to be a collimated beam (solid lines) which strikes the back surface of the screen material and reflects as hemispherically-diffuse radiation (dotted lines). The reflective property of the screen material used here is the beam reflectance calculated at the incident solar angle (\(R_{sc}^{dir,dif}\) ). A single ray of this diffuse light will be followed through the remaining steps and represents the energy associated with \textbf{all} diffuse rays interreflecting between the screen and glass layers. To determine the second term of the combined screen/glass beam transmittance, the diffusely-reflected ray (\(T_{sc}^{dir,dir}R_{gl,f}^{dir}R_{sc}^{dir,dif}\) ) passes through and is attenuated by the glass layer. Since this ray originates from diffuse reflection, the attenuation of this ray is accounted for using the diffuse transmittance property of the glass. Thus, the second term is shown as \(T_{sc}^{dir,dir}R_{gl,f}^{dir}R_{sc}^{dir,dif}T_{gl}^{dif}\) . Defining the remaining terms continues in a similar fashion using diffuse properties of both the screen and glass material. Notice that the 3\(^{rd}\) and 4\(^{th}\) terms shown below are similar to the 2\(^{nd}\) term, but additional terms are raised to increasing powers.
+
+\begin{figure}[hbtp] % fig 89
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1231.png}
+\caption{Screen/Glass System Transmittance Equation Schematic. \protect \label{fig:screenglass-system-transmittance-equation}}
+\end{figure}
+
+The screen/glass system transmittance equation shown in the figure above is repeated here in an alternate format to emphasize the recurring nature of the infinite series. This equation represents the final solar beam transmittance equation for the screen/glass combination. The recurring terms are shown as a summation of a quantity raised to the n power, with n ranging from 0 to infinity. Since the quantity \(R_{gl}^{dif}R_{sc}^{dif,dif}\) ~is less than 1, the summation \(\sum\limits_{n = 0}^\infty {{{(R_{gl,f}^{dif}R_{sc}^{dif,dif})}^n}}\) converges and can be expressed as $\PB{1-R_{gl,f}^{dif}R_{sc}^{dif,dif}}^{-1}$.  Since the reflected (scattered) transmittance of incident solar beam (\(T_{sc}^{dir,dif}\)) and the diffusely reflecting beam \(T_{sc}^{dir,dir}R_{gl,f}^{dir}R_{sc}^{dir,dif}\) ~are both assumed to be hemispherically diffuse radiation, the reflected (scattered) transmittance of incident solar beam is added to the infinite series as shown below.
+
+\begin{equation}
+\begin{array}{rl}
+  T_{sys}^{dir,all}(\alpha ',\varphi ',\phi ) &= T_{sc}^{dir,dir}(\alpha ',\varphi ')T_{gl}^{dir}\left( \phi  \right) \\
+                                              &+ (T_{sc}^{dir,dir}(\alpha ',\varphi ')R_{gl,f}^{dir}R_{sc}^{dir,dif}(\alpha ',\varphi ') \\
+                                              &+ T_{sc}^{dir,dif}(\alpha ',\varphi '))T_{gl}^{dif}\sum\limits_{n = 0}^\infty  {{{(R_{gl,f}^{dif}R_{sc}^{dif,dif})}^n}} 
+\end{array}
+\end{equation}
+
+or:
+
+\begin{equation}
+T_{sys}^{dir,all}(\alpha ',\varphi ',\phi ) = T_{sc}^{dir,dir}(\alpha ',\varphi ')T_{gl}^{dir}\left( \phi  \right) + \frac{{(T_{sc}^{dir,dir}(\alpha ',\varphi ')R_{gl,f}^{dir}R_{sc}^{dir,dif}(\alpha ',\varphi ') + T_{sc}^{dir,dif}(\alpha ',\varphi '))T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}}}
+\end{equation}
+
+where
+
+\(T_{sys}^{dir,all}(\alpha ',\varphi ',\phi )\) ~ = screen/glass system beam transmittance (output report variable Surface Window Screen and Glazing System Beam Solar Transmittance)
+
+Properties for beam absorptance of the individual glass layers and screen/glass combination are derived in a similar fashion to the transmittance calculation described above. Diffuse transmittance and absorptance of individual glass layers and the screen/glass combination are also shown here.
+
+\begin{equation}
+\begin{array}{l}A_{gl,j,f}^{dir,sys}\left( {\alpha ',\varphi ',\phi } \right) = T_{sc}^{dir,dir}\left( {\alpha ',\varphi '} \right)A_{gl,j,f}^{dir}\left( \phi \right) + \\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\;\;\;\;\;\;\frac{{\left( {T_{sc}^{dir,dir}\left( {\alpha ',\varphi '} \right)R_{gl}^{dir}\left( \phi \right)R_{sc}^{dir,dif}\left( {\alpha ',\varphi '} \right) + T_{sc}^{dir,dif}\left( {\alpha ',\varphi '} \right)} \right)A_{gl,j,f}^{dif}}}{{1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}}},\;j = 1,N\end{array}
+\end{equation}
+
+\begin{equation}
+\begin{array}{l}\alpha_{sc}^{dir,sys}\left( {\alpha ',\varphi ',\phi } \right) = A_{sc}^{dir}\left( {\alpha ',\varphi '} \right)\left( {1 + R_{gl,f}^{dir}\left( \phi \right)T_{sc}^{dir,dir}\left( {\alpha ',\varphi '} \right)} \right) + \\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\frac{{A_{sc}^{dif}R_{gl,f}^{dif}}}{{1 - R_{sc}^{dif,dif}R_{gl,f}^{dif}}}\left( {R_{gl,f}^{dir}\left( \phi \right)T_{sc}^{dir,dir}\left( {\alpha ',\varphi '} \right)R_{sc}^{dir,dif}\left( {\alpha ',\varphi '} \right)} \right)\end{array}
+\end{equation}
+
+\begin{equation}
+T_{sys}^{dif,dif} = \frac{{T_{sc}^{dif,dif}T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}}}
+\end{equation}
+
+\begin{equation}
+A_{gl,j,f}^{dif,sys} = \frac{{T_{sc}^{dif,dif}A_{gl,j,f}^{dif}}}{{1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}}},\;j = 1,N
+\end{equation}
+
+\begin{equation}
+\alpha_{sc}^{dif,\,sys} = A_{sc}^{dif}\left( {1 + \frac{{T_{sc}^{dif,dif}R_{gl,f}^{dif}}}{{1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}}}} \right)
+\end{equation}
+
+where
+
+\(A_{gl,j,f}^{dir,sys}\left( {\alpha ',\varphi ',\phi } \right)\) ~ = glass layer beam absorptance including interreflections with screen material
+
+\(\alpha_{sc}^{dir,sys}\left( {\alpha ',\varphi ',\phi } \right)\) ~ = beam absorptance of screen material including interreflections with glass
+
+\(T_{sys}^{dif,dif}\) ~ = screen/glass system diffuse transmittance (output report variable Surface Window Screen and Glazing System Diffuse Solar Transmittance)
+
+\(A_{gl,j,f}^{dif,sys}\) ~ = glass layer diffuse absorptance including interreflections with screen material
+
+\(\alpha_{sc}^{dif,sys}\) ~ = diffuse absorptance of screen material including interreflections with glass
+
+\subsubsection{Screen/Glazing System Properties for Long-Wave Radiation}\label{screenglazing-system-properties-for-long-wave-radiation}
+
+The program calculates how much long-wave radiation is absorbed by the screen and by the adjacent glass surface. The effective long-wave emissivity (equal to the long-wave absorptance on a wavelength-by-wavelength basis or over the same spectral range) of an exterior screen, taking into account reflection of long-wave radiation between the glass and screen, is given by
+
+\begin{equation}
+\varepsilon_{sc}^{lw,eff} = \varepsilon_{sc}^{lw}\left( {1 + \frac{{T_{sc}^{dif,dif}\rho_{gl}^{lw}}}{{1 - R_{sc}^{dif,dif}\rho_{gl}^{lw}}}} \right)
+\end{equation}
+
+where \(\rho_{gl}^{lw}\) is the long-wave reflectance of the outermost glass surface facing an exterior screen, and it is assumed that the long-wave transmittance of the glass is zero.
+
+The effective outermost (for exterior screen) glass surface emissivity when the screen is present is
+
+\begin{equation}
+\varepsilon_{gl}^{lw,eff} = \varepsilon_{gl}^{lw}\frac{{T_{sc}^{dif,dif}}}{{1 - R_{sc}^{dif,dif}\rho_{gl}^{lw}}}
+\end{equation}
+
+The effective inside surface emissivity is the sum of the effective screen and effective glass emissivities:
+
+\begin{equation}
+\varepsilon_{ins}^{lw,eff} = \varepsilon_{sc}^{lw,eff} + \varepsilon_{gl}^{lw,eff}
+\end{equation}
+
+The effective temperature of the screen/glazing combination that is used to calculate the window's contribution to the zone's mean radiant temperature (MRT) is given by
+
+\begin{equation}
+{T^{eff}} = \frac{{\varepsilon_{sc}^{lw,eff}{T_{sc}} + \varepsilon_{gl}^{lw,eff}{T_{gl}}}}{{\varepsilon_{sc}^{lw,eff} + \varepsilon_{gl}^{lw,eff}}}
+\end{equation}
+
+\subsubsection{Solar Radiation Transmitted and Absorbed by a Window/Screen System}\label{solar-radiation-transmitted-and-absorbed-by-a-windowscreen-system}
+
+Let the direct solar incident on the window be
+
+\begin{equation}
+{I_{dir,inc}} = {f_{sunlit}}{I_{dir,norm}}\cos \phi {\rm{    }}(W/{m^2})
+\end{equation}
+
+where \({f_{sunlit}}\) is the fraction of the window that is sunlit (determined by the shadowing calculations), \({I_{dir,norm}}\) is the direct normal solar irradiance, and \(\phi\) ~is the angle of incidence.
+
+Let \({I_{sky,inc}}\) be the irradiance on the window due to diffuse solar radiation from the sky (W/m\(^{2}\)) and let \({I_{gnd,inc}}\) be the irradiance on the window due to diffuse solar radiation from the ground (W/m\(^{2}\)).
+
+Then we have the following expressions for different classes of transmitted and absorbed solar radiation for the window/screen system, all in W/m\(^{2}\):
+
+\emph{Direct and diffuse solar entering zone from incident direct solar:}
+
+\begin{equation}
+{I_{dir,inc}}T_{sys}^{dir,all}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\emph{Direct solar absorbed by screen:}
+
+\begin{equation}
+{I_{dir,inc}}\alpha_{sc}^{dir,sys}\left( {\alpha ',\varphi '} \right)
+\end{equation}
+
+\emph{Direct solar absorbed by glass layers:}
+
+\begin{equation}
+{I_{dir,inc}}A_{gl,j,f}^{dir,sys}(\phi ,{\phi_s}),{\rm{    }}j = 1,N
+\end{equation}
+
+\emph{Diffuse solar entering zone from incident diffuse solar:}
+
+\begin{equation}
+\left( {{I_{sky,inc}} + {I_{gnd,inc}}} \right)T_{sys}^{dif,dif}
+\end{equation}
+
+\emph{Diffuse solar absorbed by screen:}
+
+\begin{equation}
+\left( {Isky,inc + Ignd,inc} \right)\alpha_{sc}^{dif,sys}
+\end{equation}
+
+\emph{Diffuse solar absorbed by glass layers:}
+
+\begin{equation}
+({I_{sky,inc}} + {I_{gnd,inc}})A_{gl,j,f}^{dif,sys},{\rm{   }}j = 1,N{\rm{ }}
+\end{equation}
+
+\subsection{Complex Fenestration Calculation Module}\label{complex-fenestration-calculation-module}
+
+This section describes detailed method for modeling complex fenestration systems, including shading devices and general fenestration attachments. This detailed method primarily refers to the optical side of modeling complex fenestration systems. Thermal modeling is done according to ISO 15099 standard, which is described in the Window Heat Balance Calculation section with the addition of deflection and vacuum glazing systems modeling and some modifications to shading layer algorithms, which is described in Shading Device Thermal Model section. Optical caclulations in this method are done using Bidirectional Scattering Distribution Function (BSDF) approach.~ The concept behind BSDF is based on the definition of descrete set of incident and outgoing angles, which fully describes optical performance of any system, simple or complex, limited only by the resolution of angular discretization.~ In this method each layer, as well as the whole system is described by a matrix of incident and outgoing angles.
+
+\subsubsection{Complex Fenestration Solar-Optical Calculations}\label{complex-fenestration-solar-optical-calculations}
+
+\paragraph{\texorpdfstring{\textbf{Solar radiation calculation outline}}{Solar radiation calculation outline}}\label{solar-radiation-calculation-outline}
+
+For solar radiation calculations, each of the layers as well as entire glazing system can be represented with the set of Bi-directional Scattering Distribution Functions or BSDF, consisting of Bi-directional Reflectance Distribution Function or BRDF and Bi-directional Transmittance Distribution Function or BTDF.~ Each function is a matrix 145 x 145 that describes reflectance or transmittance distribution in the outgoing hemisphere for each incident angle in the incidence hemisphere.~ For each function there is forward and back matrix, for a total of 4 145 x 145 matrices.~ Depending on the purpose of calculations, description of entire glazing system is divided into solar and visible spectrum, which means that there can be 8 matrices describing visible and complete solar spectrums.~ Reflectance and transmittance being non-dimnsional ratios of reflected or transmitted energy over incident energy, in order to get total reflected and transmitted energy it is necessary to supply vector of incident solar energy, which usually consists of direct and diffuse radition.Specifics of calculations of direct and diffuse solar radiationis be described in some detail in oncoming chapters.
+
+\subparagraph{\texorpdfstring{\textbf{Scattering (Non-Specular) Glazing and Shading Devices}}{Scattering (Non-Specular) Glazing and Shading Devices}}\label{scattering-non-specular-glazing-and-shading-devices}
+
+A general scattering fenestration system is characterized by BTDFs and BRDFs, which were described above.~ Given an incident direction \textbf{\emph{p}}\(^{(I)}\), and an incident irradiance \emph{E}( \textbf{\emph{p}}\(^{(I)}\)), the transmitted radiance in the outgoing direction \textbf{\emph{p}}\(^{(T)}\) is
+
+\begin{equation}
+S({{\bf{p}}^{{\rm{(T)}}}}) = {\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})dE({{\bf{p}}^{{\rm{(I)}}}})
+\end{equation}
+
+where the function T is the BTDF.~ In the absence of a source of effectively plane-parallel incident radiation (such as direct sunlight) d\emph{E(\textbf{p}}\(^{(I)}\)\emph{)} is an infinitesimal quantity, and the right side of the equation must be summed over the irradiance from all incident directions to produce the outgoing radiance:
+
+\begin{equation}
+S({{\bf{p}}^{{\rm{(T)}}}}) = \int {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})\frac{{dE({{\bf{p}}^{{\rm{(I)}}}})}}{{d\Omega }}d\Omega }
+\end{equation}
+
+A similar equation gives the reflected radiance in the direction \textbf{\emph{p}}\(^{(R)}\):
+
+\begin{equation}
+S({{\bf{p}}^{{\rm{(R)}}}}) = \int {{\mathop{\rm R}\nolimits} ({{\bf{p}}^{{\rm{(R)}}}},{{\bf{p}}^{{\rm{(I)}}}})\frac{{dE({{\bf{p}}^{{\rm{(I)}}}})}}{{d\Omega }}d\Omega }
+\end{equation}
+
+We can express the irradiance in terms of the exterior luminance, S, in that direction,
+
+\begin{equation}
+dE({{\bf{p}}^{{\rm{(I)}}}})dA = {S^{{\rm{(I)}}}}({{\bf{p}}^{{\rm{(I)}}}})\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}dA
+\end{equation}
+
+\begin{figure}[hbtp] % fig 90
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1271.png}
+\caption{Irradiance geometry \protect \label{fig:irradiance-geometry}}
+\end{figure}
+
+which allows one to express the transmittance of exterior radiation to produce the total outgoing radiance from the fenestration into the room in a particular direction:
+
+\begin{equation}
+S({{\bf{p}}^{{\rm{(T)}}}}) = \int\limits_{{\Omega ^{{\rm{(I)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(I)}}}}({{\bf{p}}^{{\rm{(I)}}}})\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}}
+\end{equation}
+
+The negative sign is added to account for the fact that \textbf{\emph{p}}\(^{(I)}\) and \textbf{\emph{n}} have opposite sign for incoming radiation.
+
+The radiance in equation is emitted from the back side of the element of area shown in Figure~\ref{fig:irradiance-geometry}.~ Considering a second surface, viewing the back side of the fenestration system, we can use equation to calculate the irradiance on surface 2,
+
+\begin{equation}
+{E^{{\rm{(2)}}}}({{\bf{p}}^{{\rm{(T)}}}})d{A^{{\rm{(2)}}}} = {S^{{\rm{(T)}}}}({{\bf{p}}^{{\rm{(T)}}}})\left( { - {{\bf{p}}^{{\rm{(T)}}}}\cdot {{\bf{n}}^{{\rm{(2)}}}}} \right)d{\Omega ^{{\rm{(I,2)}}}}d{A^{{\rm{(2)}}}}
+\end{equation}
+
+This expression, however, contains a number of new quantities, such as \(d{\Omega ^{{\rm{(I,2)}}}}\) , the element of solid angle for incoming radiation as seen from surface 2.~ We can sort this out by referring to Figure~\ref{fig:radiation-exchange-between-two-surface} and making some changes and clarifications in notation.
+
+\begin{figure}[hbtp] % fig 91
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1275.png}
+\caption{Radiation exchange between two surface elements \protect \label{fig:radiation-exchange-between-two-surface}}
+\end{figure}
+
+In this figure we consider that surface 1 is the back side of the fenestration system, and surface 2 is some other surface in the room that receives the transmitted solar radiation through the fenestration system.~ We consider infinitesimal elements \emph{dA}\(^{(1)}\) and \emph{dA}\(^{(2)}\) of the two surfaces, and define vector surface elements by \emph{d\textbf{A}}\textbf{\(^{(}\)}\(^{1)}\) = \emph{dA}\(^{(1)}\)\textbf{\emph{n}}\(^{(1)}\) and \emph{d\textbf{A}}\textbf{\(^{(}\)}\(^{1)}\) = \emph{dA}\(^{(1)}\)\textbf{\emph{n}}\(^{(1)}\).~ The quantity \textbf{\emph{r}} in the figure denotes a vector pointing from surface 1 to surface 2, the magnitude of which is the distance \emph{r} between the two surface elements.~ This is used to define two unit vectors: \({{\bf{\hat r}}^{{\rm{(1)}}}} = {{\bf{r}} \mathord{\left/ {\vphantom {{\bf{r}} r}} \right. } r}\) ~is a unit vector pointing from surface element 1 to surface element 2, and \({{\bf{\hat r}}^{{\rm{(2)}}}} = - {{\bf{r}} \mathord{\left/ {\vphantom {{\bf{r}} r}} \right. } r}\) ~is a unit vector pointing from surface element 2 back to surface element 1.~ The unit vector \textbf{\emph{p}}\(^{(T)}\) in equation is in fact \({{\bf{\hat r}}^{{\rm{(1)}}}}\) .~ The shaded quadrilaterals in the figure are the projected area elements normal to \textbf{\emph{r}}.~ Since the areas are infinitesimal, all the radiation leaving one surface element and arriving at the other will be in the direction \textbf{\emph{r}}, so that all radiation will be contained within the parallelepiped defined by the dashed lines (parallel to \textbf{\emph{r}}) joining the corners of the two surface elements.~ It follows that the area \emph{dA}\(^{(2)}\)~ is not independent of \emph{dA}\(^{(1)}\).~ The figure also shows the solid angle that has been denoted \emph{d}W\(^{(I,2)}\) above, which is the solid angle subtended by \emph{dA}\(^{(1)}\) as seen from \emph{dA}\(^{(2)}\) and is given by
+
+\begin{equation}
+d{\Omega ^{{\rm{(I,2)}}}} = \frac{{d{{\bf{A}}^{{\rm{(1)}}}} \cdot {{\bf{r}}^{{\rm{(1)}}}}}}{{{r^2}}}
+\end{equation}
+
+The net power from surface element 1 to surface element 2 is
+
+\begin{equation}
+{W^{(1 \to 2)}} = \left( {{S^{{\rm{(1)}}}}({{{\bf{\hat r}}}^{{\rm{(1)}}}}) - {S^{{\rm{(2)}}}}({{{\bf{\hat r}}}^{{\rm{(2)}}}})} \right)\frac{{\left( {d{{\bf{A}}^{{\rm{(1)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(1)}}}}} \right)\left( {d{{\bf{A}}^{{\rm{(2)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(2)}}}}} \right)}}{{{r^2}}}
+\end{equation}
+
+where \({S^{{\rm{(1)}}}}({{\bf{\hat r}}^{{\rm{(1)}}}})\) ~is the radiance leaving surface element 1 in the direction of surface element 2, and vice-versa for \({S^{{\rm{(2)}}}}({{\bf{\hat r}}^{{\rm{(2)}}}})\) .~ In this case, the latter is zero and the former is the quantity called \emph{S}\(^{(T)}\)(\textbf{\emph{p}}\(^{(T)}\)) above.~ Given equation , we can recognize the quantity multiplying the radiance as the solid angle \emph{d}W\(^{(I,2)}\) times the projected area of surface element 2 perpendicular to \textbf{\emph{r}}.~ But the expression is symmetrical in the two surface elements, so we could also express it as
+
+\begin{equation}
+{W^{(1 \to 2)}} = {S^{{\rm{(T)}}}}({{\bf{p}}^{{\rm{(T)}}}})\left( {d{{\bf{A}}^{{\rm{(1)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(1)}}}}} \right)d{\Omega ^{{\rm{(T)}}}}
+\end{equation}
+
+where
+
+\begin{equation}
+d{\Omega ^{{\rm{(T)}}}} = \frac{{\left( {d{{\bf{A}}^{{\rm{(2)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(2)}}}}} \right)}}{{{r^2}}}
+\end{equation}
+
+The superscript (T) is used here because the solid angle element pertains to the direction \textbf{\emph{p}}\(^{(T)}\).~ In the particular case under discussion that restricts attention to those directions for which the outgoing radiation strikes surface element 2.~ We can now rewrite equation as
+
+\begin{equation}
+{E^{{\rm{(2)}}}}({{\bf{p}}^{{\rm{(T)}}}})d{A^{{\rm{(2)}}}} = {S^{{\rm{(T)}}}}({{\bf{p}}^{{\rm{(T)}}}})\left( {{{\bf{n}}^{{\rm{(1)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(1)}}}}} \right)d{\Omega ^{{\rm{(T)}}}}d{A^{{\rm{(1)}}}}
+\end{equation}
+
+and since, as can readily be seen from Figure~\ref{fig:radiation-exchange-between-two-surface}, \(\left( {d{{\bf{A}}^{{\rm{(1)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(1)}}}}} \right) = \left( {d{{\bf{A}}^{{\rm{(2)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(2)}}}}} \right)\) , this becomes
+
+\begin{equation}
+{E^{{\rm{(2)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = {S^{{\rm{(T)}}}}({{\bf{p}}^{{\rm{(T)}}}})\left( { - {{\bf{p}}^{{\rm{(T)}}}} \cdot {{\bf{n}}^{{\rm{(2)}}}}} \right)d{\Omega ^{{\rm{(T)}}}}
+\end{equation}
+
+Substituting equation for \emph{S}\(^{(T)}\)(\textbf{\emph{p}}\(^{(T)}\), we obtain a propagation equation for outside radiation passing through the window and arriving at surface element 2:
+
+\begin{equation}
+E^{(2)}(\bf{p}^{(T)}) = \int_{\Omega^{(I)}} 
+      \rm T (\bf{p}^{(T)},\bf{p}^{(I)}) 
+      S^{(I)}(\bf{p}^{(I)})(-\bf{p}^{(I)}\cdot\bf{n}^{(I)})
+      d\Omega^{(I)}(-\bf{p}^{(T)}\cdot\bf{n}^{(2)})d\Omega^{(T)}
+\end{equation}
+
+or, in terms involving only irradiance,
+
+\begin{equation}
+{E^{{\rm{(2)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = \int\limits_{{\Omega ^{{\rm{(I)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})E({{\bf{p}}^{{\rm{(I)}}}})d{\Omega ^{{\rm{(I)}}}}} \left( { - {{\bf{p}}^{{\rm{(T)}}}} \cdot {{\bf{n}}^{{\rm{(2)}}}}} \right)d{\Omega ^{{\rm{(T)}}}}
+\end{equation}
+
+Comparing these two equations with equations and , we can see that physically they represent the processes of (a) propagation of radiation outgoing at one surface (initially, the sky ``surface''), where it is characterized by radiance, to incidence on a second surface, characterized by irradiance, followed (b) transmittance, which converts incoming radiation traveling in a given direction to outgoing radiation in a different set of directions, characterized again by radiance.~ We can make the former of these processes explicit by defining a propagation function.~ Considering the first surface element to be located at a position specified by the vector \textbf{\emph{x}}\(^{(1)}\) and the second at \textbf{\emph{x}}\(^{(2)}\), then radiation leaving surface 1 in a direction \textbf{\emph{p}}\(^{(1)}\) and arriving at surface 2 in a direction \textbf{\emph{p}}\(^{(2)}\) produces an irradiance given by
+
+\begin{equation}
+{E^{(2)}}({{\bf{p}}^{{\rm{(2)}}}}) = \int {L({{\bf{x}}^{{\rm{(2)}}}},{{\bf{p}}^{{\rm{(2)}}}};{{\bf{x}}^{{\rm{(1)}}}},{{\bf{p}}^{{\rm{(1)}}}}){S^{{\rm{(1)}}}}({{\bf{p}}^{{\rm{(1)}}}})} d{\Omega ^{{\rm{(1)}}}}
+\end{equation}
+
+where the propagation function L is defined by
+
+\begin{equation}
+L({{\bf{x}}^{{\rm{(2)}}}},{{\bf{p}}^{{\rm{(2)}}}};{{\bf{x}}^{{\rm{(1)}}}},{{\bf{p}}^{{\rm{(1)}}}}) = \left( { - {{\bf{p}}^{{\rm{(2)}}}}\cdot {{\bf{n}}^{{\rm{(2)}}}}} \right)d{\Omega ^{{\rm{(2)}}}}\delta ({{\bf{p}}^{{\rm{(2)}}}},{{\bf{p}}^{{\rm{(1)}}}})\delta ({{\bf{x}}^{{\rm{(2)}}}},{{\bf{x}}^{{\rm{(1)}}}} + {\bf{r}})
+\end{equation}
+
+The spatial dependence is inserted to guarantee that the geometrical relations in Figure~\ref{fig:radiation-exchange-between-two-surface} are preserved.~ The delta functions in direction and spatial vectors are the mathematically standard d-distributions defined so that
+
+\begin{equation}
+\int {\delta ({{\bf{p}}^{{\rm{(2)}}}},{{\bf{p}}^{{\rm{(1)}}}})} f({{\bf{p}}^{{\rm{(1)}}}})d{\Omega ^{{\rm{(1)}}}} = f({{\bf{p}}^{{\rm{(2)}}}})
+\end{equation}
+
+\begin{equation}
+\int\limits_\Omega  {\delta ({{\bf{p}}^{{\rm{(2)}}}},{{\bf{p}}^{{\rm{(1)}}}})d{\Omega ^{{\rm{(1)}}}}}  = \left\{ {\begin{array}{*{20}{c}}1&{{{\bf{p}}^{{\rm{(2)}}}} \in \Omega }\\0&{{{\bf{p}}^{{\rm{(2)}}}} \notin \Omega }\end{array}} \right.
+\end{equation}
+
+\begin{equation}
+\int {\delta ({{\bf{x}}^{{\rm{(2)}}}},{{\bf{x}}^{{\rm{(1)}}}})} f({{\bf{x}}^{{\rm{(1)}}}})d{A^{{\rm{(1)}}}} = f({{\bf{x}}^{{\rm{(2)}}}})
+\end{equation}
+
+\begin{equation}
+\int\limits_A {\delta ({{\bf{x}}^{{\rm{(2)}}}},{{\bf{x}}^{{\rm{(1)}}}})d{A^{{\rm{(1)}}}}}  = \left\{ {\begin{array}{*{20}{c}}1&{{{\bf{x}}^{{\rm{(2)}}}} \in A}\\0&{{{\bf{x}}^{{\rm{(2)}}}} \notin A}\end{array}} \right.
+\end{equation}
+
+for an arbitrary function \emph{f}.~ {[}In equations and the integration is assumed to be over all possible values of either direction or position, so that the vectors \textbf{\emph{p}}\(^{(2)}\) and \textbf{\emph{x}}\(^{(2)}\) are necessarily within the domain of integration.{]}
+
+\subparagraph{Physical Caveats}\label{physical-caveats}
+
+In equations and the functions T and R pertain to the overall glazing system, and are assumed to be averaged over both wavelength and polarization with appropriate weightings.~ {[}EnergyPlus considers wavelength only in that it distinguishes between radiation in the longwave thermal IR region and in the shortwave solar/visible region.~ (In considering daylighting, there is a further limitation to the visible region.)~ In this discussion we are concerned solely with the shortwave solar/visible region.{]}~ While fenestration properties may depend on both wavelength and polarization, for externally incident radiation this dependence is taken into account in the calculation and averaging of T and R.~ However, both the wavelength distribution (within the solar region) and the polarization state of the outgoing radiation will generally be different from that of the incident radiation.~ This is not a feature peculiar to non-specular fenestration systems; it is also true of specular ones, and may in fact be more important there.~ For most interior surfaces, where the radiation is either absorbed or diffusely reflected (and where both processes are assumed wavelength and polarization independent), this is of no importance, but in the case of either interior windows or the back-reflectance from exterior windows, it could in principle cause errors, unless proper account is taken in specifying T and R for these cases.
+
+\subparagraph{Discretization: The LBNL Method}\label{discretization-the-lbnl-method}
+
+A series of 6 papers (Papamichael, Klems et al. 1988; Klems 1994A; Klems 1994B; Klems and Warner 1995; Klems and Kelley 1996; Klems, Warner et al. 1996) formulated the LBNL method of characterizing scattering fenestration systems.~ The relevant aspects of that method will be summarized here.~ This method has been incorporated into the WINDOW (from LBNL 2012) computer program.
+
+The method begins by approximating the integrals in equations and by finite sums.~ It does this by defining a set of finite solid angle elements \{\(\Delta {\Omega_i}\) \} that covers the relevant solid angle hemisphere (whether incident, transmitted or reflected directions).~ Each solid angle element is characterized by a direction \textbf{\emph{p}}\emph{\(_{i}\)}, and it is assumed that this may be substituted for any direction within the solid angle element.~ This set of solid angle elements and corresponding directions is termed a basis.~ Note that, since \textbf{\emph{p}}\emph{\(_{i}\)} is a two-dimensional vector, enumerating the solid angle elements with a single index \emph{i} implicitly includes specifying an ordering of the direction vectors.~ Equation then becomes
+
+\begin{equation}
+S({{\bf{p}}_j}^{{\rm{(T)}}}) = \sum\limits_i {{\mathop{\rm T}\nolimits} ({{\bf{p}}_j}^{{\rm{(T)}}},{{\bf{p}}_i}^{{\rm{(I)}}}){S^{{\rm{(I)}}}}({{\bf{p}}_i}^{{\rm{(I)}}})\left( { - {{\bf{p}}_i}^{{\rm{(I)}}}\cdot {\bf{n}}} \right)\Delta {\Omega_i}^{{\rm{(I)}}}}
+\end{equation}
+
+and equation becomes
+
+\begin{equation}
+{E^{(2)}}({{\bf{p}}_j}^{{\rm{(2)}}}) = \sum\limits_i {\int\limits_{\Delta {\Omega_i}} {L({{\bf{x}}^{{\rm{(2)}}}},{{\bf{p}}_j}^{{\rm{(2)}}};{{\bf{x}}^{{\rm{(1)}}}},{{\bf{p}}_i}^{{\rm{(1)}}}){S^{{\rm{(1)}}}}({{\bf{p}}_i}^{{\rm{(1)}}})d{\Omega ^{{\rm{(1)}}}}} }
+\end{equation}
+
+Referring to the definition of the propagation function in equation and properties of the d-distribution in equation , we see that the integrals in the summation will all be zero, except when \textbf{\emph{p}}\emph{\(_{j}\)}\(^{(2)}\) is contained in the solid angle element DW\emph{\(_{i}\)}.~ In that case the integration produces \textbf{\emph{p}}\emph{\(_{i}\)}\(^{(1)}\) = \textbf{\emph{p}}\emph{\(_{j}\)}\(^{(2)}\).~ We can retain the formal summation by utilizing the finite-dimensional form of the d-distribution, known as the Kronicker delta, d\emph{\(_{ij}\)}:
+
+\begin{equation}
+{\delta_{ij}} = \left\{ {\begin{array}{*{20}{c}}1&{i = j}\\0&{i \ne j}\end{array}} \right.
+\end{equation}
+
+Then the integral becomes
+
+\begin{equation}
+\int\limits_{\Delta {\Omega_i}} {L({{\bf{x}}^{{\rm{(2)}}}},{{\bf{p}}_j}^{{\rm{(2)}}};{{\bf{x}}^{{\rm{(1)}}}},{{\bf{p}}_i}^{{\rm{(1)}}}){S^{{\rm{(1)}}}}({{\bf{p}}_i}^{{\rm{(1)}}})d{\Omega ^{{\rm{(1)}}}}}  = \lambda ( - {{\bf{p}}_j}^{{\rm{(2)}}}){\delta_{ij}} \cdot \delta ({{\bf{x}}^{{\rm{(2)}}}},{{\bf{x}}^{{\rm{(1)}}}} + {\bf{r}})
+\end{equation}
+
+where the function \emph{l} is defined as
+
+\begin{equation}
+{\lambda ^{{\rm{(s)}}}}({{\bf{p}}_j}) = \left( {{{\bf{p}}_j}\cdot {{\bf{n}}^{{\rm{(s)}}}}} \right)\Delta {\Omega_j}
+\end{equation}
+
+and the superscript (s) refers to the surface.
+
+The LBNL method, which focuses on glazing systems consisting of plane-parallel layers, makes particular assumptions that allow one to ignore the spatial dependence of L.~ Since the only effect of the function \(\delta ({{\bf{x}}^{{\rm{(2)}}}},{{\bf{x}}^{{\rm{(1)}}}} + {\bf{r}})\) ~in equation is to require that if the expression is formally integrated over two separate surface areas, only the parts of the integration that satisfy the geometric constraints will contribute (in effect, the integration is over only one of the surfaces), we will drop the spatial dependence in the present discussion and replace it later when we consider the total energy transfer between different surfaces.
+
+Equations (without the delta distribution in \textbf{\emph{x}}) and are then considered to define the components of a diagonal matrix,
+
+\begin{equation}
+\begin{array}{*{20}{c}}{{\bf{\Lambda }^{{\rm{(s)}}}} = \left( {{\Lambda ^{{\rm{(s)}}}}_{ij}} \right)}&{{\rm{where}}}&{\Lambda_{ij}^{{\rm{(s)}}} = \left( {{{\bf{p}}_j}\cdot {{\bf{n}}^{{\rm{(s)}}}}} \right)\Delta {\Omega_j}{\delta_{ij}}}\end{array}
+\end{equation}
+
+Considering the radiance in the various basis directions to be the components of a vector,
+
+\begin{equation}
+\bf{S} = \left( 
+    \begin{array}{c}
+      S_1 \\ ... \\ S_j \\ ...
+    \end{array}
+  \right)
+  \text{where}
+  S_j = S(\bf{p}_j)
+\end{equation}
+
+equation becomes
+
+\begin{equation}
+\begin{array}{*{20}{c}}{{S^{{\rm{(T)}}}}_j = \sum\limits_i {{T_{ji}}} \sum\limits_k {{\Lambda_{ik}}} {S_k}}&{{\rm{where}}}&{{T_{ji}} = {\mathop{\rm T}\nolimits} ({{\bf{p}}_j}^{{\rm{(T)}}},{{\bf{p}}_i}^{{\rm{(I)}}})}\end{array}
+\end{equation}
+
+which has the obvious character of a series of matrix multiplications.~ (Note that the superscript (T) here means transmitted, not the matrix operation transpose.)~ Similarly, the reflectance matrix elements are
+
+\begin{equation}
+{R_{ij}} = {\mathop{\rm R}\nolimits} ({{\bf{p}}^{{\rm{(R)}}}},{{\bf{p}}^{{\rm{(I)}}}})
+\end{equation}
+
+The method then identifies the infinitesimal directional irradiances in equation with the components of an irradiance vector,
+
+\begin{equation}
+E = \left( 
+    \begin{array}{c}
+      E_1 \\ ... \\ E_i \\ ...
+    \end{array}
+  \right)
+  \text{where}
+  E_i = \frac{dE(\bf{p}_j)}{d\Omega}
+\end{equation}
+
+and equations - can be rewritten as matrix equations,
+
+\begin{equation}
+{{\bf{S}}^{{\rm{(T)}}}} = {\bf{T}} \cdot {{\bf{E}}^{{\rm{(I)}}}}
+\end{equation}
+
+\begin{equation}
+{{\bf{S}}^{{\rm{(R)}}}} = {\bf{R}} \cdot {{\bf{E}}^{{\rm{(I)}}}}
+\end{equation}
+
+\begin{equation}
+{{\bf{E}}^{{\rm{(I)}}}}{\bf{ = }}{\bf{\Lambda }^{{\rm{(I)}}}} \cdot {{\bf{S}}^{{\rm{(I)}}}}
+\end{equation}
+
+\begin{equation}
+{{\bf{S}}^{{\rm{(T)}}}}{\bf{ = T}} \cdot {\bf{\Lambda }^{{\rm{(I)}}}} \cdot {{\bf{S}}^{{\rm{(I)}}}}
+\end{equation}
+
+(These are for radiation incident on the front surface of the fenestration; there is a similar set of equations for radiation incident on the back surface and propagating in an opposite sense to that in the above equations.)
+
+In the LBNL method, these equations are used extensively to calculate the overall properties of a fenestration system from those of its component layers.~ Here we will assume that the components of the system property matrices are given at input.~ These may be from a calculation by WINDOW or determined by some other method.~ The quantities needed for each fenestration are:
+
+Table 34: Fenestration properties needed for the calculation
+
+Exterior Window
+
+\begin{equation}
+T_{ij}^F
+\end{equation}
+
+Front Transmittance~ matrix elements
+
+\begin{equation}
+R_{ij}^F
+\end{equation}
+
+Back Reflectance matrix elements
+
+\begin{equation}
+{\mathop{\rm A}\nolimits}_i^{F,n}
+\end{equation}
+
+In-situ absorptance of n\(^{th}\) layer for front incidence
+
+\begin{equation}
+{\mathop{\rm A}\nolimits}_i^{B,n}
+\end{equation}
+
+In-situ absorptance of n\(^{th}\) layer for back incidence
+
+Interior Window
+
+\begin{equation}
+T_{ij}^F
+\end{equation}
+
+Front Transmittance matrix elements
+
+\begin{equation}
+T_{ij}^B
+\end{equation}
+
+Back Transmittance matrx elements
+
+\begin{equation}
+R_{ij}^F
+\end{equation}
+
+Front Reflectance matrix elements
+
+\begin{equation}
+R_{ij}^B
+\end{equation}
+
+Back Reflectance matrix elements
+
+\begin{equation}
+{\mathop{\rm A}\nolimits}_i^{F,n}
+\end{equation}
+
+In-situ absorptance of n\(^{th}\) layer for front incidence
+
+\begin{equation}
+{\mathop{\rm A}\nolimits}_i^{B,n}
+\end{equation}
+
+In-situ absorptance of n\(^{th}\) layer for back incidence
+
+The transmittance and reflectance are overall system properties.~ (For daylighting calculations, one also needs the transmittance and reflectance averaged over the visible spectrum only; the quantities indicated in the table pertain to the entire solar spectrum.)~ For the optical calculations we do not need to know anything about the individual layers making up the fenestration.~ However, the thermal calculation of heat flow through the fenestration requires knowledge of the amount of radiation absorbed in each of the fenestration layers.~ As indicated in the table, we therefore need the in-situ layer absorptance for each layer, referenced to the incident surface.~ This is denoted \({\mathop{\rm A}\nolimits}_i^{F,n}\) ~for the fraction of the \emph{i\(^{th}\)} component of the irradiance incident on the front surface of the fenestration that is absorbed in layer \emph{n}, with a similar quantity, \({\mathop{\rm A}\nolimits}_i^{B,n}\) , for irradiance incident on the back surface.~ The term ``in-situ layer absorptance'' is used because these are not simply the absorptance of the layer, but include the transmittance and interreflection by other layers of the system prior to the absorptance in layer \emph{n}.~ The absorptance is a row vector, having possibly a different value for each direction of the incident irradiance, so that for an irradiance \emph{E\(_{i}\)\(^{F}\)} on the front surface of a fenestration and \emph{E\(_{i}\)\(^{B}\)} on the back surface, the power \emph{Q\(^{n}\)} absorbed per unit area in layer \emph{n} would be
+
+\begin{equation}
+{Q^n} = \sum\limits_i {{\mathop{\rm A}\nolimits}_i^{F,n}E_i^F}  + \sum\limits_j {{\mathop{\rm A}\nolimits}_j^{B,n}E_j^B}
+\end{equation}
+
+(In the vector/matrix language, \({Q^n} = {\bf{A}^{F,n}} \cdot {{\bf{E}}^F} + {\bf{A}^{B,n}} \cdot {{\bf{E}}^B}\) )
+
+\subparagraph{Bases and Coordinate Systems}\label{bases-and-coordinate-systems}
+
+The introduction of a basis or multiple bases is a bit more complicated than indicated in the text preceding equation .~ There for transmission we need coordinates describing incoming radiation on one surface of the physical layer and outgoing radiation at the second (opposite) surface, while reflection adds the need for coordinates describing outgoing radiation at the first surface.~ Back transmittance and reflectance add the requirement for coordinates describing incoming radiation at the second surface.~ The usual way of assigning coordinates to radiation involves specifying its line of propagation relative to the local surface normal. This means that there are separate coordinate systems for the first and second surfaces, and that, moreover, the description is different for incoming and outgoing radiation: for incoming radiation one is specifying a unit vector pointing toward the source of the radiation (\emph{i}.\emph{e}., antiparallel to the direction of propagation), while for outgoing radiation one is specifying a unit vector in the direction of propagation of the radiation.~ In principle, then, one needs four coordinate systems or bases (for each physical layer), and the process of transmission or reflection involves a discontinuous transition between an input basis and an output basis.
+
+The LBNL method used by WINDOW uses a particular choice of coordinate systems in which incoming radiation at the first surface and outgoing radiation at the second are described by one coordinate system, while the same coordinate system reflected through the layer is used to describe incoming radiation at the second surface and outgoing radiation at the first.~ The reason for this choice is that it greatly simplifies the matrix representations: specular transmittance or reflectance is always represented by a diagonal matrix, one can mix matrices representing forward or backward incidence processes, and all of the coordinate systems have propagation matrices with the same representation, so in effect there is one \emph{L} matrix rather than four.
+
+The point of this discussion is that the components of the transmittance and reflectance matrices, and the layer absorptance vectors, depend on the definition of these four bases.~ If they were generated by WINDOW, then they assume the particular coordinate system described above.~ (If they were produced by some other means, they may be specified in yet some other coordinate system.)~ While the LBNL coordinate system gives an intuitive description of outgoing radiation, as a description of incoming radiation it is very unintuitive.~ And in any case, the coordinate system is different from that of EnergyPlus.~ It will be necessary to translate the matrices and vectors into the correct EnergyPlus coordinate system.
+
+\subparagraph{Matching the WINDOW6 Calculation to EnergyPlus}\label{matching-the-window6-calculation-to-energyplus}
+
+It is useful to have some sense of how well the basis normally used in WINDOW calculations matches the requirements of EnergyPlus.~ In using a BSDF window, a user would presumably be interested in the directionality of the transmitted radiation; if the size of the solid angle bins in the basis is large compared to the solid angle subtended by the typical surface in a zone, then that directional information will be lost.~ On the other hand, if the bins are very small compared to this solid angle, then (since EnergyPlus does not consider the spatial variations within a surface) the directions are being oversampled.~ Since the calculation time will be proportional to the number of matrix elements, which is the square of the number of basis directions, oversampling is to be avoided.
+
+Because of the great variety of buildings that may be modeled with EnergyPlus, and because the user has control over the basis for the BSDF properties, it is not possible to answer this question in a definitive way.~ Here we consider the effect of the normal WINDOW basis in a typical perimeter office space, 10 ft wide, 15 ft deep and 11 ft high.~ It is assumed to have a window 9 ft wide by 6 ft high, with the sill height 3 ft.~ The window is placed to have a 4 in inner reveal.
+
+The normal WINDOW ``full'' basis has 145 output directions.~ Figure~\ref{fig:transmitted-radiation-in-three-directions-for} shows how the window and the solid angle bin project onto the inner surfaces for three of those directions.~ In each case the solid angle bin is projected from the window center, and the window edges are projected along the central ray.
+
+In general, the basis appears to be reasonably matched to the calculation, with neither a loss of angular detail nor great oversampling.
+
+\begin{figure}[hbtp] % fig 92
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1326.png}
+\caption{Transmitted Radiation in Three Directions for a Perimeter Office. (a) q = 0º; (b) q = 40º, f = 15º; (c) q = 70º, f = 67.5º.  q and f are the normal spherical angle coordinates in a right-handed coordinate system where y points up and z is normal to the window p \protect \label{fig:transmitted-radiation-in-three-directions-for}}
+\end{figure}
+
+\subparagraph{Complex Fenestrations in EnergyPlus}\label{complex-fenestrations-in-energyplus}
+
+Exterior
+
+EnergyPlus models the exterior radiance in two parts, a moving sun radiance \({S^{{\rm{(Sun)}}}}(t)\Delta {\Omega ^{{\rm{(Sun)}}}}\) ~and a constant-shape direction-dependent sky radiance \({S^{{\rm{(Sky)}}}}({\bf{p}},t)\) .~ The intensities of these vary with time.~ For the solar radiation there is a single sky radiance model.~ For daylight calculations the treatment is similar for exterior luminance, except that there are a number of user-selectable sky luminance models.~ Here we will discuss radiance; the treatment of luminance is analogous.
+
+The direct normal solar intensity (at a given time) is
+
+\begin{equation}
+{I^{{\rm{(D)}}}}(t) = {S^{{\rm{(Sun)}}}}(t)\Delta {\Omega ^{{\rm{(Sun)}}}}
+\end{equation}
+
+and if we let
+
+\begin{equation}
+{S^{{\rm{(Sky)}}}}({\bf{p}},t) = {I^{{\rm{(Sky)}}}}(t)s({\bf{p}})
+\end{equation}
+
+where the shape function for the sky radiance model, \emph{s}, is defined so that
+
+\begin{equation}
+\int\limits_{2\pi } {s({\bf{p}})d\Omega }  = 1
+\end{equation}
+
+then the global solar irradiance on a horizontal surface at a given time is
+
+\begin{equation}
+{I^{{\rm{(G)}}}}(t) = {I^{{\rm{(Sky)}}}}(t)\left( {1 - \int\limits_{\Delta {\Omega ^{{\rm{(Sun)}}}}} {s({\bf{p}})d\Omega } } \right) + {I^{{\rm{(D)}}}}(t)\cos {\theta ^{{\rm{(Sun)}}}}(t)
+\end{equation}
+
+It must be understood that in equation the integration region 2p means integration over the sky hemisphere, and that \emph{s(\textbf{p})} is zero for upward-going directions.
+
+With the sky radiance shape \emph{s(\textbf{p})} specified in the EnergyPlus code, the angular size of the sun \(\Delta {\Omega ^{{\rm{(Sun)}}}}\) ~known, and the solar zenith angle \({\theta ^{{\rm{(Sun)}}}}(t)\) ~calculated in the code, the two hourly input quantities \emph{I}\(^{(D*)*}\)\emph{(t)} and \emph{I}\(^{(G)}\)\emph{(t)} determine the exterior radiance for any given hour.
+
+In this context, the transmitted radiance for a complex fenestration system given in equation becomes
+
+\begin{equation}
+\begin{array}{c}S({{\bf{p}}^{{\rm{(T)}}}}) = {I^{({\bf{Sky}})}}(t)\int\limits_{{\Omega ^{{\rm{(Sky)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})s({{\bf{p}}^{{\rm{(I)}}}})\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} \\ + \int\limits_{{\Omega ^{{\rm{(Gnd)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(Gnd)}}}}({{\bf{p}}^{{\rm{(I)}}}},t)\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} \\ + H\left( {\Delta {\Omega ^{{\rm{(Sun)}}}}(t) \not\subset {\Omega ^{{\rm{(Sf)}}}}} \right)\int\limits_{\Delta {\Omega ^{{\rm{(Sun)}}}}(t)} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(Sun)}}}}({{\bf{p}}^{{\rm{(I)}}}},t)\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} \\ + \int\limits_{{\Omega ^{{\rm{(Sf)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(Refl)}}}}({{\bf{p}}^{{\rm{(I)}}}},t)\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} \end{array}
+\end{equation}
+
+where the incoming hemisphere viewed by the fenestration has been broken up into four parts.~ The viewed sky (excluding the part containing the sun) is \({\Omega ^{{\rm{(Sky)}}}}\) , the viewed ground is \({\Omega ^{{\rm{(Gnd)}}}}\) , the part subtended by the sun is DW\(^{(Sun)}\), and the part subtended by one or more exterior surfaces (shading or reflecting objects) is W\(^{(Sf)}\).~ These solid angles must exclude the exterior surfaces.~ The symbol \emph{H} represents a Helmholtz function: Its value is one if its logical argument is true, zero otherwise.~ It has been inserted into the equation to account for those times when the sun is behind an exterior object.~ Where there are multiple exterior shading or reflecting objects, W\(^{(Sf)}\) may consist of several regions that may be disjoint or connected, depending on the exterior geometry.~ As indicated in the equation, DW\(^{(Sun)}\) is time-dependent, to account for the sun's movement; W\(^{(Gnd)}\) and W\(^{(Sf)}\)~ are fixed, but as written \({\Omega ^{{\rm{(Sky)}}}}\) ~has a time dependence induced by the exclusion of the solid angle subtended by the sun.~ So that we can discuss the parts separately, we break the outgoing radiance down by source:
+
+\begin{equation}
+S({{\bf{p}}^{{\rm{(T)}}}}) = {S^{{\rm{(Sky)}}}}({{\bf{p}}^{{\rm{(T)}}}}) + {S^{{\rm{(Gnd)}}}}({{\bf{p}}^{{\rm{(T)}}}}) + {S^{{\rm{(Sun)}}}}({{\bf{p}}^{{\rm{(T)}}}}) + {S^{{\rm{(Sf)}}}}({{\bf{p}}^{{\rm{(T)}}}})
+\end{equation}
+
+By subtracting the radiation from the part of the sky hidden by the sun from \({S^{{\rm{(Sun)}}}}\) ~and adding it back into \emph{S}\(^{(Sky)}\) we can remove the time dependence of W\(^{(Sky)}\):
+
+\begin{equation}
+\begin{array}{c}{S^{{\rm{(Sun)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = H\left( {\Delta {\Omega ^{{\rm{(Sun)}}}}(t) \not\subset {\Omega ^{{\rm{(Sf)}}}}} \right)\\ \times \int\limits_{\Delta {\Omega ^{{\rm{(Sun)}}}}(t)} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})\left[ {{S^{{\rm{(Sun)}}}}({{\bf{p}}^{{\rm{(I)}}}},t) - {I^{({\bf{Sky}})}}(t)s({{\bf{p}}^{{\rm{(I)}}}})} \right]\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} \end{array}
+\end{equation}
+
+\begin{equation}
+{S^{{\rm{(Sky)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = {I^{({\bf{Sky}})}}(t)\int\limits_{{\Omega ^{{\rm{(Sky)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})s({{\bf{p}}^{{\rm{(I)}}}})\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}}
+\end{equation}
+
+Now in equation the integral is to be evaluated without regard to the sun position, and therefore \({\Omega ^{{\rm{(Sky)}}}}\) ~is time-independent.
+
+We can further simplify equation by noting that the angular size of the sun is small, and both \emph{s}(\textbf{\emph{p}}\(^{(I)}\)) and T(\textbf{\emph{p}}\(^{(T)}\), \textbf{\emph{p}}\(^{(I)}\)) can be considered as constant over the range of directions in DW\(^{(Sun)}\).~ We can therefore evaluate them at the direction \textbf{\emph{p}}\(^{(Sun)}\)(t) of the center of the sun and move them out of the integration, resulting in
+
+\begin{equation}
+{S^{{\rm{(Sun)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = {\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(Sun)}}}})\left[ {{I^{{\rm{(D)}}}} - {I^{{\rm{(Sky)}}}}s({{\bf{p}}^{{\rm{(Sun)}}}})\Delta {\Omega ^{{\rm{(Sun)}}}}} \right]\cos {\theta ^{{\rm{(Sun)}}}}H\left( {{{\bf{p}}^{{\rm{(Sun)}}}} \not\subset {\Omega ^{{\rm{(Sf)}}}}} \right)
+\end{equation}
+
+In this equation we have dropped the explicit time dependence, but \textbf{\emph{p}}\(^{(Sun)}\), \emph{q}\(^{(Sun)}\), \emph{I}\(^{(D)}\), and \emph{I}\(^{(Sky)}\) are time-varying, while DW\(^{(Sun)}\) is simply the constant angular size of the sun.
+
+We separate the reflected radiance \emph{S}\(^{(Sf)}\) into separate components for each surface,
+
+\begin{equation}
+{S^{{\rm{(Sf)}}}} = \sum\limits_n {{S^{{\rm{(Sf, n)}}}}}
+\end{equation}
+
+The individual shading surface reflected radiances are then
+
+\begin{equation}
+{S^{{\rm{(Sf, n)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = \int\limits_{{\Omega ^{{\rm{(Sf, n)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(Refl, n)}}}}({{\bf{p}}^{{\rm{(I)}}}},t)\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}}
+\end{equation}
+
+The solid angle of integration in this expression is subtended by the portion of the exterior reflecting surface \emph{n} viewed by the fenestration; if one surface lies behind another, the hidden part of its surface is removed from the solid angle it subtends.~ This is summarized by the requirement
+
+\begin{equation}
+\begin{array}{l}{\Omega ^{{\rm{(Sf)}}}} = \bigcup\limits_n {{\Omega ^{{\rm{(Sf, n)}}}}} \\\bigcap\limits_n {{\Omega ^{{\rm{(Sf, n)}}}}}  = 0\end{array}
+\end{equation}
+
+(This requirement will need to be modified to handle the case of transmitting exterior surfaces.)
+
+\emph{S}\(^{(Refl,n)}\) is time dependent because the incident radiation on the surface depends on the sun position. \emph{~}Equation must be evaluated after the exterior surface shading or reflectance calculations, in order to enforce the requirement that
+
+\begin{equation}
+{\Omega ^{{\rm{(Sky)}}}} \cap {\Omega ^{{\rm{(Sf)}}}} = 0
+\end{equation}
+
+Finally, the transmitted radiance from the ground-reflected exterior radiation is
+
+\begin{equation}
+{S^{{\rm{(Gnd)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = \int\limits_{{\Omega ^{{\rm{(Gnd)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(Gnd)}}}}({{\bf{p}}^{{\rm{(I)}}}},t)\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}}
+\end{equation}
+
+Here, not only is there the requirement that
+
+\begin{equation}
+{\Omega ^{{\rm{(Gnd)}}}} \cap {\Omega ^{{\rm{(Sf)}}}} = 0
+\end{equation}
+
+but also the incident radiation on the ground may be affected by shading or reflection from exterior surfaces.~ Since this is dependent on the sun position, \emph{S}\(^{(Gnd)}\) is time dependent, as indicated in equation .
+
+Applying the discretization of the previous section and the definitions in equations -, we can rewrite equation as
+
+\begin{equation}
+{S_j}^{{\rm{(T,Sky)}}} = {I^{({\bf{Sky}})}}(t)\sum\limits_{i \in {\Omega ^{{\rm{(Sky)}}}}} {{T_{ji}}{\Lambda_{ii}}{s_i}}
+\end{equation}
+
+where
+
+\begin{equation}
+{s_i} = s({{\bf{p}}_i}^{{\rm{(I)}}})
+\end{equation}
+
+is the sky radiance shape factor evaluated at the central direction of the i\(^{th}\) solid angle bin.~ A ``T'' superscript has been added on the left-hand side of the equation to denote that \emph{S} is the transmitted outgoing radiance (due to incident sky radiation for the fenestration under discussion).~ The stipulation \(i \in {\Omega ^{{\rm{(Sky)}}}}\) ~on the summation means that the sum is to include only those solid angle elements for which the sky is viewed by the fenestration.~ This is essentially a shading calculation, in addition to a restriction to downward-going incident directions.~ We anticipate the result of this calculation by defining a sky geometric factor:
+
+\begin{equation}
+V_i^{(Sky)} = \left\{
+    \begin{array}{rl}
+      1                      & \text{all of } \Delta\Omega_i \text{ views sky for all of fenestration} \\
+      \text{viewed fraction} & \text{some of } \Delta\Omega_i \text{, fenestration views sky} \\
+      0                      & \text{none of } \Delta\Omega_i \text{ views sky for any part of fenestration}
+    \end{array}
+  \right.
+\end{equation}
+
+Then we can carry out the summation over all downward directions and write
+
+\begin{equation}
+  S_j^{(T,Sky)} = I^{Sky}(t)\sum_{i down} T_{ji} \Lambda_{ii} V_i^{(Sky)} {s_i}
+\end{equation}
+
+Similarly, equation becomes
+
+\begin{equation}
+{S_j}^{{\rm{(T, Sf, n)}}} = \sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}{S^{{\rm{(Refl, n)}}}}({{\bf{p}}_i}^{{\rm{(I)}}},t)}
+\end{equation}
+
+where \(V_{i}^{(Sf,\, n)}\) is another geometric view factor, defined analogously to equation , giving the fraction of the solid angle \(\Delta {\Omega_i}\) that views the exterior surface \emph{n}. Note that
+
+\begin{equation}
+V_i^{{\rm{(Sky)}}} + \sum\limits_{\rm{n}} {V_i^{{\rm{(Sf, n)}}}}  = 1
+\end{equation}
+
+The quantity \(S^{(Refl,n)} (\bf{p}_i^{(I)},t)\) is in fact the reflected radiance at a particular location on the n\(^{th}\) exterior surface --- the location where the direction \textbf{\emph{p}}\emph{\(_{i}\)}\(^{(I)}\) intersects the surface. (This statement will become more precise when the spatial dependence dropped from equation is re-inserted.) This surface is assumed to have either a diffuse reflectance \emph{r}\(^{(n)}\) or a specular reflectance \emph{r}\(^{(sp,\\ n)}\). (Both properties are possible simultaneously, but EnergyPlus assumes that an exterior surface is either diffusing or specular, but not both.) The reflectance is assumed uniform over the surface, but the particular location (effectively, the image of the fenestration projected onto surface n) may or may not view the sky, or, at a particular time, the sun. We denote the incident irradiance of the surface n by \(E_i^n\). This irradiance pertains only to the surface n (in the present EnergyPlus calculation) and is independent of the fenestration or its basis.~ We attach the subscript i simply as a reminder that (2) the irradiance pertains to the portion of the surface that is viewed by the solid angle element \(\Delta {\Omega_i}\) of the fenestration f (which would become important if the EnergyPlus shading calculations were modified to relax the assumption of uniform incident irradiance on exterior surfaces) and that the irradiance pertains only to those surfaces n that are viewed by the solid angle element i. For specularly reflecting surfaces, we make the following definitions: First, within the set of basis solid angles \(\Delta {\Omega_i}\), let s(\emph{t}) identify the one containing the sun direction at time \emph{t}, and let r(\emph{t}) identify the one containing the specular reflection direction of the sun at time \emph{t}. We then define a contingent direct beam irradiance, which we denote by \(E_{i{\rm{ }}r(t)}^{(D,n)}\) . This irradiance is non-zero only if \(i = r(t)\) this direction is such that i is the specularly reflected direction for the surface n. If this is the case, then \(E_{i = r(t)}^{(D,n)}\) is the incident direct beam irradiance. With this definition,
+
+\begin{equation}
+{S^{{\rm{(Refl, n)}}}}({{\bf{p}}_i}^{{\rm{(I)}}},t) = {\rho ^{{\rm{(sp, n)}}}}E_{i{\rm{ }}r(t)}^{(D,n)} + {\rho ^{{\rm{(n)}}}}E_i^n
+\end{equation}
+
+If we then define normalized irradiance factors \emph{U} by \(E_i^n = U_i^{(Sky,n)}{I^{(Sky)}}(t) + U_{i{\rm{ }}Sun(tsh)}^{(D,n)}{I^{(D)}}(t)\) ~and \(E_{i{\rm{ }}r(t)}^{(D,n)} = U_{i{\rm{ }}r(t)}^{(D,n)}{I^{(D)}}(t)\) , where \(U_{i{\rm{ }}Sun(tsh)}^{(D,n)}\) ~denotes the fraction of the beam solar that irradiates the surface for a given sun direction.~ It is evaluated during the shading calculation, as indicated by the notation \emph{Sun(tsh)}.~ With these definitions we can rewrite the equation as
+
+\begin{equation}
+S^{(Refl,n)}(\bf{p}_i^{(I)},t) = 
+  I^{(D)}(t) U_{i r(t)}^{(D,n)} \rho^{(sp,n)} +
+  I^{(D)}(t) U_{i Sun(tsh)}^{(D,n)} \rho^{(n)} +
+  I^{(sky)}(t) U_i^{(Sky,n)} \rho^{(n)}
+\end{equation}
+
+and equation becomes, in terms of the incident irradiances,
+
+\begin{equation}
+{S_j}^{{\rm{(T, Sf, n)}}} = \sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}\left( {{\rho ^{{\rm{(sp, n)}}}}E_{i{\rm{ }}r(t)}^{(D,n)} + {\rho ^{{\rm{(n)}}}}E_i^n} \right)}
+\end{equation}
+
+and in terms of the normalized irradiance factors,
+
+\begin{equation}
+\begin{array}{c}{S_j}^{{\rm{(T, Sf, n)}}} = \sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}{I^{{\rm{(D)}}}}(t)U_{i{\rm{ r(}}t{\rm{)}}}^{{\rm{(D,n)}}}{\rho ^{{\rm{(sp, n)}}}}} \\ + \sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}\left[ {{I^{{\rm{(D)}}}}(t)U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}}{\rho ^{{\rm{(n)}}}} + {I^{(Sky)}}(t)U_i^{{\rm{(Sky,n)}}}{\rho ^{{\rm{(n)}}}}} \right]} \end{array}
+\end{equation}
+
+The specularly reflected term can be removed from the sum, since only one value of i can contribute:
+
+\begin{equation}
+{S_j}^{{\rm{(T, Sf, n)}}} = {T_{j{\rm{ r(}}t{\rm{)}}}}{\Lambda_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}}V_{{\rm{ r(}}t{\rm{)}}}^{{\rm{(Sf, n)}}}E_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}^{{\rm{(D,n)}}}{\rho ^{{\rm{(sp, n)}}}} + {\rho ^{{\rm{(n)}}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}E_i^n}
+\end{equation}
+
+and
+
+\begin{equation}
+\begin{array}{c}{S_j}^{{\rm{(T, Sf, n)}}} = {T_{j{\rm{ r(}}t{\rm{)}}}}{\Lambda_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}}V_{{\rm{ r(}}t{\rm{)}}}^{{\rm{(Sf, n)}}}U_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}^{{\rm{(D,n)}}}{I^{(D)}}(t){\rho ^{{\rm{(sp, n)}}}}\\ + {\rho ^{{\rm{(n)}}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}\left( {{I^{{\rm{(D)}}}}(t)U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}} + U_i^{(Sky,n)}{I^{(Sky)}}(t)} \right)} \end{array}
+\end{equation}
+
+which separates specular and diffuse reflectance from the exterior surfaces.
+
+With respect to shading and reflection of exterior radiation into the fenestration, the exterior reveal surfaces can be treated as additional diffusely reflecting exterior surfaces.
+
+Ground radiation is treated in the same way as radiation reflected from interior surfaces, except that one sums only over upward-going incident directions, and the ground is assumed to be diffusely reflecting.~ The transmitted radiance from ground reflectance is
+
+\begin{equation}
+{S_j}^{{\rm{(T, Gnd)}}} = {\rho ^{{\rm{(Gnd)}}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}E_i^{(Gnd)}}
+\end{equation}
+
+In this equation, the symbol \(E_i^{(Gnd)}\) ~is shorthand for a spatial calculation.~ The solid angle region \(\Delta {\Omega_i}\) ~views (from various points over the fenestration area) some spatial region of the ground.~ The symbol \(E_i^{(Gnd)}\) ~denotes the incident irradiance on the ground over this spatial region.~ In the absence of shading, this would be simply \({I^{(G)}} = {I^{(Sky)}} + {I^{(D)}}\cos {\theta_{Sun}}\) ; shading requires a more complex calculation.~ Currently the EnergyPlus code does a Monte-Carlo calculation: rays are randomly generated from the window, when they strike the ground a calculation is made to determine whether that point receives direct solar radiation and what portion of the sky it views (reflected radiation from surfaces is neglected).~ Here we would perform that calculation for each region of the ground i viewed by a basis solid angle element, instead of generating random rays from the window.~ We denote the results of that calculation by \(E_i^{(Gnd)} = U_{i{\rm{ }}Sun(tsh)}^{(D,Gnd)}{I^{(D)}}(t) + U_i^{(Sky,Gnd)}{I^{(Sky)}}(t)\) , where the \emph{U}'s are average viewing factors for the sun and sky, calculated as part of the shading calculation (which is indicated by the subscript \emph{tsh}: \emph{Sun(tsh)} is the sun direction as specified by the shading calculation.~ This then gives
+
+\begin{equation}
+{S_j}^{{\rm{(T, Gnd)}}} = {\rho ^{{\rm{(Gnd)}}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}\left( {U_{i{\rm{ }}Sun(tsh)}^{(D,Gnd)}{I^{(D)}}(t) + U_i^{(Sky,Gnd)}{I^{(Sky)}}(t)} \right)}
+\end{equation}
+
+The transmitted radiance from direct beam radiation is
+
+\begin{equation}
+{S_j}^{{\rm{(T, Sun)}}} = {T_{j{\rm{ s}}(t)}}\cos {\theta ^{{\rm{(Sun)}}}}{I^{{\rm{(D)}}}}(t)V_{i{\rm{ s(}}t{\rm{)}}}^{{\rm{(D)}}}
+\end{equation}
+
+This introduces yet one more geometric view factor: $V_{i s(t)}^{(D)}$ is zero if the sun direction s\emph{(t)} is not \emph{i}; if \emph{i} = s(\emph{t}) it is the fraction of the fenestration area irradiated by the direct sun.~ Equation uses the fact that the angular size of the sun is smaller than any basis solid angle element, and that EnergyPlus treats the sun and circumsolar region as a point source {[}hence the absence of the sky correction in equation {]}.
+
+At this point we have developed separate expressions for a fenestration's~ transmitted radiance in a particular direction depending on the exterior source of the radiation.~ These expressions utilize the discretized BTDF of the fenestration in the form of transmittance matrix elements over an angular basis.~ The exterior geometry is re-expressed in the form of geometric view factors in this basis.~ In the process, the explicit time dependence of the exterior radiation has been reduced to the time-varying direct and diffuse solar intensities and the solar position.~ The time dependence of the solar position, however, consists merely in specifying, for a particular time, which of the basis solid angle elements contains the solar direction.~ The entire exterior geometry necessary for the fenestration transmittance calculation can therefore be pre-calculated.
+
+Interior
+
+We begin with the discretized form of equation , in which we also modify the surface notation.~ In that equation, the surfaces involved are termed (1) and (2), where radiation is outgoing from surface 1 and incoming to surface 2.~ Here radiation is outgoing from the inner surface of the fenestration, so we label that surface (f).~ The receiving surface is one of the surfaces of the zone in which the fenestration is located.~ We number those surfaces with the index \emph{k}, so the receiving surface is labeled (\emph{k}).~ Equation then becomes
+
+\begin{equation}
+dW_j^{{\rm{(f}} \to k{\rm{)}}} = {E^{{\rm{(}}k{\rm{)}}}}({{\bf{p}}_j}^{{\rm{(T)}}})d{A^{{\rm{(}}k{\rm{)}}}} = {S_j}^{{\rm{(T)}}} \cdot \left( {{{\bf{n}}^{{\rm{(f)}}}} \cdot {{\bf{p}}_j}^{{\rm{(T)}}}} \right)\Delta {\Omega_j}^{{\rm{(T)}}}d{A^{{\rm{(f)}}}}
+\end{equation}
+
+or, noting that \(\left(\bf{n}^{(f)}\cdot\bf{p}_j^{(T)}\right) \Delta\Omega^{(T)} = \Lambda_{jj}^{(T)}\) ~(where the superscript T is retained in case the incoming and outgoing bases are defined differently),
+
+\begin{equation}
+dW_j^{{\rm{(f}} \to k{\rm{)}}} = {E^{{\rm{(}}k{\rm{)}}}}({{\bf{p}}_j}^{{\rm{(T)}}})d{A^{{\rm{(}}k{\rm{)}}}} = {S_j}^{{\rm{(T)}}}\Lambda_{jj}^{{\rm{(T)}}}d{A^{{\rm{(f)}}}}
+\end{equation}
+
+If we integrate this expression over the fenestration area \emph{A}\(^{(f)}\) we obtain the total power leaving the fenestration surface in direction \emph{j}; however, all of that power may not reach surface \emph{k}: some may strike the inner window reveal or a different zone surface.~ If we define a spatial projection operator by
+
+\begin{equation}
+{{\bf{x}}^{{\rm{(}}k{\rm{)}}}} = {{\mathop{\rm P}\nolimits} ^{{\rm{(}}k{\rm{)}}}}({\bf{p}}_j^{{\rm{(T)}}},{{\bf{x}}^{{\rm{(f)}}}}) \equiv {{\mathop{\rm P}\nolimits}_j}^{{\rm{(}}k{\rm{)}}}({{\bf{x}}^{{\rm{(f)}}}})
+\end{equation}
+
+where \textbf{\emph{x}}\(^{(*k*)}\) is in the plane of surface \emph{k}, and a geometric form factor by
+
+\begin{equation}
+F_j^{{\rm{(}}k{\rm{)}}} = \frac{1}{{{A^{{\rm{(f)}}}}}}\int\limits_{{{\mathop{\rm P}\nolimits}_j}^{{\rm{(}}k{\rm{)}}}({{\bf{x}}^{{\rm{(f)}}}}) \in {A^{{\rm{(}}k{\rm{)}}}}} {d{A^{{\rm{(f)}}}}}
+\end{equation}
+
+then
+
+\begin{equation}
+dW_j^{{\rm{(f}} \to k{\rm{)}}} = {S_j}^{{\rm{(T)}}}\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}{A^{{\rm{(f)}}}}
+\end{equation}
+
+The total power leaving the fenestration (in any direction) and arriving at surface \emph{k} is then
+
+\begin{equation}
+W_j^{{\rm{(f}} \to k{\rm{)}}} = \sum\limits_j {{S_j}^{{\rm{(T)}}}\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}{A^{{\rm{(f)}}}}}
+\end{equation}
+
+Substituting equations , , , , into equation yields a series of expressions for the total power arriving at surface \emph{k} (by transmission through fenestration f) from each of the sources of exterior radiation.~ However, the equations for transmitted radiation describe an infinitesimal region, which means that the radiation in a given direction will always come from one source.~ When one integrates the transmitted power over the fenestration surface, one encounters the problem that for this direction different parts of the fenestration area may receive radiation from different sources.~ Also, for a given outgoing direction, the projection of a receiving surface back onto the fenestration may produce an image that covers only part of the fenestration area, and this image may not be identical with the part of the area that receives incident radiation from a particular source.~ The most important origin of this problem is the existence of inner and outer window reveals, as illustrated in Figure~\ref{fig:mismatch-of-irradiated-and-viewed}.
+
+\begin{figure}[hbtp] % fig 93
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1392.png}
+\caption{Mismatch of irradiated and viewed fenestration areas for different incident and outgoing directions \protect \label{fig:mismatch-of-irradiated-and-viewed}}
+\end{figure}
+
+In this figure, the portion of the fenestration area not viewed by the plane of surface \emph{k} is instead viewed by one or more of the inner window reveals.~ Similarly, the portion of the fenestration not irradiated in the figure is in fact irradiated by diffusely reflected radiation from the outer window reveals.~ We can account for this by replacing the area \emph{A}\(^{(f)}\) in equation with the overlap area \(A_{ji}^{{\rm{(f, Src), }}k}\) \emph{~}(dark shaded in the figure), where ``Src'' stands for the source of the incident radiation.~ This area is defined by
+
+\begin{equation}
+A_{ji}^{\left( {f,Src} \right),k} = \left. {A_i^{\left( {f,Src} \right)}} \right|A_j^{\left( f \right),k}
+\end{equation}
+
+The total power at the interior surface \emph{k} for each source of radiation then becomes
+
+\begin{equation}
+{W^{{\rm{(Sky), }}k}} = {I^{({\bf{Sky}})}}(t)\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sky)}}}A_{ji}^{{\rm{(f, Sky), }}k}{s_i}} }
+\end{equation}
+
+\begin{equation}
+\begin{array}{c}{W^{{\rm{(Sf,n)}},k}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(sp, n)}}}}\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}{T_{j{\rm{ r(}}t{\rm{)}}}}{\Lambda_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}}V_{{\rm{ r(}}t{\rm{)}}}^{{\rm{(Sf, n)}}}A_{j{\rm{ r(}}t{\rm{)}}}^{{\rm{(f, Sf, n), }}k}U_{{\rm{ r(}}t{\rm{) s(}}t{\rm{)}}}^{{\rm{(D,n)}}}} \\ + {I^{(D)}}(t){\rho ^{{\rm{(n)}}}}\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}A_{ji}^{{\rm{(f, Sf, n), }}k}U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}}} } \\ + {I^{(Sky)}}(t){\rho ^{{\rm{(n)}}}}\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}A_{ji}^{{\rm{(f, Sf, n), }}k}U_i^{{\rm{(Sky,n)}}}} } \end{array}
+\end{equation}
+
+\begin{equation}
+\begin{array}{c}{W^{{\rm{(Gnd)}},k}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(Gnd)}}}}\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}A_{ji}^{{\rm{(f, Gnd), }}k}U_{i{\rm{ }}Sky(tch)}^{{\rm{(D, Gnd)}}}} } \\ + {I^{({\bf{Sky}})}}(t){\rho ^{{\rm{(Gnd)}}}}\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}A_{ji}^{{\rm{(f, Gnd), }}k}U_i^{{\rm{( Sky,Gnd)}}}} } \end{array}
+\end{equation}
+
+\begin{equation}
+{W^{{\rm{(Sun)}},k}} = {I^{{\rm{(D)}}}}(t)\sum\limits_j {F_j^{{\rm{(}}k{\rm{)}}}\Lambda_{jj}^{{\rm{(T)}}}{T_{j{\rm{ s}}(t)}}\cos {\theta_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}}}V_{i{\rm{ s(}}t{\rm{)}}}^{{\rm{(D)}}}A_{j{\rm{ s(}}t{\rm{)}}}^{{\rm{(f, Sun), }}k}}
+\end{equation}
+
+If we define a series of solar irradiation factors, Z, that describe the fraction of the radiation incident on the fenestration due to a given exterior radiation source that is ultimately incident on the interior surface \emph{k},
+
+\begin{equation}
+{Z^{{\rm{(Sky), }}k}} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sky)}}}A_{ji}^{{\rm{(f, Sky), }}k}{s_i}} }
+\end{equation}
+
+\begin{equation}
+{Z_{{\rm{r(}}t{\rm{)}}}}^{{\rm{(sp, Sf, n)}},k} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}{T_{j{\rm{ r(}}t{\rm{)}}}}{\Lambda_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}}V_{{\rm{ r(}}t{\rm{)}}}^{{\rm{(Sf, n)}}}A_{j{\rm{ r(}}t{\rm{)}}}^{{\rm{(f, Sf, n), }}k}U_{{\rm{ r(}}t{\rm{) s(}}t{\rm{)}}}^{{\rm{(D,n)}}}}
+\end{equation}
+
+\begin{equation}
+{Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun, Sf, n)}},k} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}A_{ji}^{{\rm{(f, Sf, n), }}k}U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}}} }
+\end{equation}
+
+\begin{equation}
+{Z^{{\rm{(Sky, Sf, n)}},k}} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}A_{ji}^{{\rm{(f, Sf, n), }}k}U_i^{{\rm{(Sky, n)}}}} }
+\end{equation}
+
+\begin{equation}
+{Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(D, Gnd)}},k} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}A_{ji}^{{\rm{(f, Gnd), }}k}U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D, Gnd)}}}} }
+\end{equation}
+
+\begin{equation}
+{Z^{{\rm{(Sky, Gnd)}},k}} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}A_{ji}^{{\rm{(f, Gnd), }}k}U_i^{{\rm{(Sky, Gnd)}}}} }
+\end{equation}
+
+\begin{equation}
+{Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}},k} = \sum\limits_j {F_j^{{\rm{(}}k{\rm{)}}}\Lambda_{jj}^{{\rm{(T)}}}{T_{j{\rm{ s}}(t)}}\cos {\theta_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}}}V_{i{\rm{ s(}}t{\rm{)}}}^{{\rm{(D)}}}A_{j{\rm{ s(}}t{\rm{)}}}^{{\rm{(f, Sun), }}k}}
+\end{equation}
+
+then equations through become
+
+\begin{equation}
+{W^{{\rm{(Sky), }}k}} = {I^{({\bf{Sky}})}}(t){Z^{{\rm{(Sky), }}k}}
+\end{equation}
+
+\begin{equation}
+\begin{array}{c}{W^{{\rm{(Sf,n)}},k}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(sp, n)}}}}{Z_{{\rm{r(}}t{\rm{)}}}}^{{\rm{(sp, Sf, n)}},k} + {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(n)}}}}{Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun, Sf, n)}},k}\\ + {I^{({\bf{Sky}})}}(t){\rho ^{{\rm{(n)}}}}{Z^{{\rm{(Sky, Sf, n)}},k}}\end{array}
+\end{equation}
+
+\begin{equation}
+{W^{{\rm{(Gnd)}},k}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(Gnd)}}}}{Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(D, Gnd)}},k} + {I^{({\bf{Sky}})}}(t){\rho ^{{\rm{(Gnd)}}}}{Z^{{\rm{(Sky, Gnd)}},k}}
+\end{equation}
+
+\begin{equation}
+{W^{{\rm{(Sun)}},k}} = {I^{{\rm{(D)}}}}(t){Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}},k}
+\end{equation}
+
+The notation s(\emph{t}) appearing in a subscript in several of the above equations refers to the basis direction for which the sun direction is contained in the basis solid angle element.~ This is of course time dependent.~ What is meant here is that at any given time the particular basis element containing the sun is to be picked out.~ (If no basis element for the fenestration contains the sun at a given time, then the corresponding view factor---and therefore irradiance or absorption factor---is zero.)~ It is therefore necessary to tabulate those quantities with an s(\emph{t}) subscript for all basis directions \emph{s} that could possibly contain the sun direction (and for \emph{r(t)}, all basis directions that could possibly contain the reflected sun angle for the surface n).~ This is a set considerably smaller than that of all incoming basis directions.~ Figure~\ref{fig:sun-paths-and-incident-basis-for-three-window} illustrates this point for direct irradiation of fenestrations in three different orientations in a building at a particular latitude, using the W6 full basis, which has 145 incoming directions.~ In the worst case (west-facing) one only needs to consider around 50 of these, with much fewer needed in other orientations.~ The specific numbers for a given fenestration will depend on the choice of basis, orientation and latitude.~ The basis direction values can of course be interpolated where greater directional resolution is warranted.~ In equation the specular direction r(\emph{t}) is uniquely determined by the sun direction s(\emph{t}), so the Z factor does not need an additional index for \emph{s}.
+
+\begin{figure}[hbtp] % fig 94
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1410.png}
+\caption{Sun Paths and Incident Basis for Three Window Orientations, 38º N. Latitude. The nodal positions (blue dots) for a W6 full basis are compared with the summer solstice (red curve) and winter solstice (green curve) solar paths. Solar paths for other days of the year will lie between these two extremes. (Note: the basis points are to be interpreted as the direction of a vector pointing from the fenestration to the sun.) (a) South facing. (b) West facing. (c) North facing (the winter path is off the figure (i.e., the window is shaded); allowed paths will be outside the red path. \protect \label{fig:sun-paths-and-incident-basis-for-three-window}}
+\end{figure}
+
+The reason for the definition of the Z factors is that to a great extent they can be precalculated, so that within the hourly calculation only equations - need to be used.~ In addition, there are fewer Z factors to be stored than transmittance matrix elements.~ The storage determinants for the foregoing calculations are summarized in the following table.
+
+% table 35
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+
+\caption{Determination of array sizes \label{table:determination-of-array-sizes}} \tabularnewline
+\toprule
+\multicolumn{2}{c}{Parameters} \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Determination of array sizes} \tabularnewline
+\toprule
+\multicolumn{2}{c}{Parameters} \tabularnewline
+\midrule
+\endhead
+
+N\(_{Basis}\) & Number of elements in the (incoming or outgoing) basis \tabularnewline
+N\(_{Sun}\) & Number of basis directions that may be sun directions (depends on fenestration orientation \tabularnewline
+N\(^{(Gnd)}_{Sun}\) & Number of sun directions that give significantly different ground irradiation conditions, as seen by fenestration \tabularnewline
+N\(_{Sf}\) & Number of reflecting surfaces viewable by fenestration (depends on fenestration orientation) \tabularnewline
+N\(^{(Sf,n)}_{Sun}\) & Number of time steps for which surface \emph{n} is sunlit (depends on orientation of surface \emph{n}; determined during shading calculation) \tabularnewline
+N\(^{(Sf,n)}_{Refl}\) & Number of basis directions that may be reflected sun directions from surface \emph{n} (depends on orientation of fenestration and surface \emph{n}). \tabularnewline
+N\(_{IntSurf}\) & Number of interior surfaces in the zone containing the fenestration \tabularnewline
+N\(_{Layers}\) & Number of thermal layers in the fenestration system \tabularnewline
+\multicolumn{2}{c}{Arrays} \tabularnewline
+A\(^{F,l}_{i}\), A\(^{B,l}_{i}\) & Absorptance vector element; N\(_{Basis}\) \tabularnewline
+T\(_{ij}\) & Transmittance matrix element; N\(_{Basis}\) X N\(_{Basis}\) \tabularnewline
+V\(^{(Sky)}_{i}\) & Sky viewed fraction; one-dimensional, N\(_{Basis}\) \tabularnewline
+V\(^{(Sf,n)}_{i}\) & Fraction of surface \emph{n} viewed; N\(_{Basis}\) X N\(_{Sf}\) \tabularnewline
+$\rho$\(^{(n)}\), $\rho$\(^{(sp,n)}\) & Surface \emph{n} diffuse, specular reflectance; N\(_{Sf}\) (already stored by E+) \tabularnewline
+U\(^{(D,n)}_{i\,Sun(tsh)}\) & Fraction of the image of $\Delta\Omega$\(_{i}\) on surface \emph{n} that views the sun when it is in direction Sun(tsh); N\(_{Basis}\) X N\(_{Sf}\) X N\(^{(Sf,n)}_{Sun}\) \tabularnewline
+V\(^{(Gnd)}_{i}\) & Fraction of $\Delta\Omega$\(_{i}\) that views ground; N\(_{Basis}\) \tabularnewline
+U\(^{(Sky, Gnd)}_{i}\) & Fraction of sky radiation received by the image of $\Delta\Omega$\(_{i}\) on the ground; N\(_{Basis}\) \tabularnewline
+U\(^{(D,Gnd)}_{i\,Sun(tsh)}\) & Fraction of direct solar radiation for sun direction Sun(tsh) received by image of $\Delta\Omega$\(_{i}\) on ground; N\(^{Gnd}_{Sim}\) X N\(_{Basis}\) \tabularnewline
+V\(^{(D)}_{i\,s(t)}\) & Fraction of fenestration area irradiated by direct solar radiation for direction \emph{i}, given that sun angle is s(\emph{t}); N\(_{Sun}\) X N\(_{Basis}\) \tabularnewline
+F\(^{(k)}_{j}\) & Fraction of radiation in direction \emph{j} leaving fenestration interior that arrives at surface \emph{k}; N\(_{Basis}\) X N\(_{IntSurf}\) \tabularnewline
+Z\(^{(Sky), k}\) & Sky irradiation factor; N\(_{IntSurf}\) \tabularnewline
+Z\(^{(sp,Sf,n),k}_{r(t)}\) & Exterior surface specular irradiation factor; N\(^{(Sf,n)}_{Sun}\) X N\(_{Sf}\) X N\(_{IntSurf}\) \tabularnewline
+Z\(^{(Sun,Sf,n),k}_{s(t)}\) & Exterior surface direct-diffuse irradiation factor; N\(^{(Sf,n)}_{Sun}\) X N\(_{Sf}\) X N\(_{IntSurf}\) \tabularnewline
+Z\(^{(Sky,Sf,n),k}\) & Exterior surface sky irradiation factor; N\(_{Sf}\) X N\(_{IntSurf}\) \tabularnewline
+Z\(^{(D,Gnd),k}_{s(t)}\) & Ground-reflected direct solar irradiaton factor (given sun direction s(\emph{t})); N\(^{(Gnd)}_{Sun}\) X N\(_{IntSurf}\) \tabularnewline
+Z\(^{(Sky,Gnd),k}\) & Ground-reflected diffuse solar irradiation factor; N\(_{IntSurf}\) \tabularnewline
+Z\(^{(Sun),k}_{s(t)}\) & Direct solar irradiation factor; N\(_{Sun}\) X N\(_{IntSurf}\) \tabularnewline
+K\(^{(Sky),l}\) & Sky absorption factor; N\(_{Layers}\) \tabularnewline
+K\(^{(sp,Sf,n),l}_{r(t)}\) & Exterior surface specular absorption factor; N\(_{Sf}\) X N\(^{(Sf,n)}_{Refl}\) X N\(_{Layers}\) \tabularnewline
+K\(^{(Sun,Sf,n),l}_{s(t)}\) & Exterior surface diffusely reflected direct sun absorption factor; N\(_{Sf}\) X N\(^{(Sf,n)}_{Sun}\) X N\(_{Layers}\) \tabularnewline
+K\(^{(Sky,Sf,n),l}\) & Exterior surface reflected sky radiation absorption factor; N\(_{Sf}\) X N\(_{Layers}\) \tabularnewline
+K\(^{(D,Gnd),l}_{s(t)}\) & Ground-reflected direct solar absorption factor; N\(^{(Gnd)}_{Sun}\) X N\(_{Layers}\) \tabularnewline
+K\(^{(Sky,Gnd),l}\) & Ground-reflected sky radiation absorption factor; N\(_{Layers}\) \tabularnewline
+K\(^{(Sun),l}_{s(t)}\) & Direct sunlight absorption factor; N\(_{Sun}\) X N\(_{Layers}\) \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subparagraph{Absorption}\label{absorption}
+
+For thermal calculations it is necessary to know the energy absorbed in each layer of the fenestration.~ This depends only on the incident geometry, but otherwise is calculated in the same manner as the solar flux incident on interior surfaces. ~For a given layer l of a fenestration f, we define a source-referenced absorption factor, K(source),l.~ This is the amount of energy absorbed in layer l divided by the relevant solar intensity (which might be beam, diffuse, or reflected beam or diffuse, depending on the source of the radiation).~ These absorption factors and the resultant source-specific absorbed solar powers are calculated by the analogs {[}see equation of equations through :
+
+\begin{equation}
+{K^{{\rm{(Sky), }}l}} = {A^{{\rm{(f)}}}}\sum\limits_{i{\rm{ }}down} {{\mathop{\rm A}\nolimits}_i^{F,l}{\Lambda_{ii}}V_i^{{\rm{(Sky)}}}{s_i}}
+\end{equation}
+
+\begin{equation}
+{Q^{{\rm{(Sky), }}l}} = {I^{({\bf{Sky}})}}(t){K^{{\rm{(Sky), }}l}}
+\end{equation}
+
+\begin{equation}
+{K_{{\rm{r(}}t{\rm{)}}}}^{{\rm{(sp, Sf, n)}},l} = {A^{{\rm{(f)}}}}{\mathop{\rm A}\nolimits}_{r(t)}^{F,l}{\Lambda_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}}V_{{\rm{ r(}}t{\rm{)}}}^{{\rm{(Sf, n)}}}U_{{\rm{ r(}}t{\rm{) s(}}t{\rm{)}}}^{{\rm{(D,n)}}}
+\end{equation}
+
+\begin{equation}
+{K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun, Sf, n)}},l} = {A^{{\rm{(f)}}}}\sum\limits_{i{\rm{ }}down} {{\mathop{\rm A}\nolimits}_i^{F,l}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}}}
+\end{equation}
+
+\begin{equation}
+{K^{{\rm{(Sky, Sf, n)}},l}} = {A^{{\rm{(f)}}}}\sum\limits_{i{\rm{ }}down} {{\mathop{\rm A}\nolimits}_i^{F,l}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}U_i^{{\rm{(Sky, n)}}}}
+\end{equation}
+
+\begin{equation}
+\begin{array}{c}{Q^{{\rm{(Sf,n)}},l}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(sp, n)}}}}{K_{{\rm{r(}}t{\rm{)}}}}^{{\rm{(sp, Sf, n)}},l} + {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(n)}}}}{K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun, Sf, n)}},l}\\ + {I^{({\bf{Sky}})}}(t){\rho ^{{\rm{(n)}}}}{K^{{\rm{(Sky, Sf, n)}},l}}\end{array}
+\end{equation}
+
+\begin{equation}
+{K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(D, Gnd)}},l} = {A^{{\rm{(f)}}}}\sum\limits_{i{\rm{ }}up} {{\mathop{\rm A}\nolimits}_i^{F,l}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D, Gnd)}}}}
+\end{equation}
+
+\begin{equation}
+{K^{{\rm{(Sky, Gnd)}},l}} = {A^{{\rm{(f)}}}}\sum\limits_{i{\rm{ }}up} {{\mathop{\rm A}\nolimits}_i^{F,l}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}U_i^{{\rm{(Sky, Gnd)}}}}
+\end{equation}
+
+\begin{equation}
+{Q^{{\rm{(Gnd)}},l}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(Gnd)}}}}{K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(D, Gnd)}},l} + {I^{({\bf{Sky}})}}(t){\rho ^{{\rm{(Gnd)}}}}{K^{{\rm{(Sky, Gnd)}},l}}
+\end{equation}
+
+\begin{equation}
+{K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}},l} = {A^{{\rm{(f)}}}}{\mathop{\rm A}\nolimits}_{{\rm{s}}(t)}^{F,l}\cos {\theta_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}}}V_{i{\rm{ s(}}t{\rm{)}}}^{{\rm{(D)}}}
+\end{equation}
+
+\begin{equation}
+{Q^{{\rm{(Sun)}},l}} = {I^{{\rm{(D)}}}}(t){K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}},l}
+\end{equation}
+
+\subparagraph{Comment on Bases}\label{comment-on-bases}
+
+Use of the basis in the above discussion has been mostly implicit, but it should nevertheless be clear that the essential feature of the basis is that it is a two-element list (i.e., a 2 X N array): it associates with an incident (i) or outgoing (j) direction index a vector pi (or pj ) that is a unit vector giving the direction of the radiation, the specification of which is two angles in some coordinate system.~ The incident and outgoing bases of course must match the matrix elements of the fenestration properties.~ These bases will (certainly in the case of WINDOW program; probably in the case of other input sources) have a structure: ordering of the elements, etc.~ However, after the initialization of the hourly loop calculation, this structure will be irrelevant:~ EnergyPlus will retain only those incoming and outgoing directions that are essential to the calculation with (one would hope, most of) the others combined into irradiation factors.~ At this point, the basis will truly be an arbitrary list.~ It follows that the specification of the basis in the EnergyPlus input should be determined by (1) the source of fenestration property data, and (2) user convenience.
+
+A related point concerns the specification of a basis for specular glazings, i.e., multiple layers of glass.~ These fenestrations are both specular (input direction = output direction) and axially symmetric.~ These properties have different effects on the calculation.
+
+The specular property means that one should not be using equation at all to describe the transmittance.~ Instead, one should use the equation
+
+\begin{equation}
+S({{\bf{p}}^{{\rm{(T)}}}}) = \tau ({{\bf{p}}^{{\rm{(T)}}}}) \cdot E({{\bf{p}}^{{\rm{(T)}}}})
+\end{equation}
+
+This equation is shoehorned into the integral calculation of equation through the use of a delta function in the incident direction vector, resulting (after the discretization) in a diagonal matrix for the transmittance (or reflectance).~ The outgoing radiance element on the diagonal would be calculated as \emph{T\(_{ii}\)}L\emph{\(_{ii}\)}, where multiplication by L\emph{\(_{ii}\)} substitutes for integration over the basis solid angle element. For a specular glazing, \(T_{ii} = \tau(\bf{p}_i^{(T)})/\Lambda_{ii}\), so one recovers the correct transmittance when one does the multiplication. However, there is still a problem in principle: For a specular fenestration, the angular spread of the outgoing radiation will be that of the source, which for direct sunlight is very small; the calculation, however, assumes the angular spread of the basis element. This problem disappears in the geometric approximation to be used in EnergyPlus: by considering only the central direction of each basis element, the outgoing radiation in that direction is essentially assumed to be specular, so the blurring in the discretization is undone.
+
+The axial symmetry of conventional glazings means that the transmittance (or reflectance) depends on only the incident angle, not the azimuthal angle about the normal to the fenestration plane.~ So if one specifies the diagonal elements of the matrix, all of the terms with the same incident angles but different azimuthal angles will be the same.~ One could alternatively specify only the specular transmittance at each of the incident angle values, provided one also indicated that it was for an axially symmetric fenestration.~ Since expanding this set of values to the equivalent diagonal elements is a trivial calculation, how one specifies a specular glazing is completely a question of user convenience.~ For example, if one were dealing with the WINDOW full basis, would it be more user-friendly to specify
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\item
+  \(T_{ii} = \tau(\bf{p}_i^{(T)})/\Lambda_{ii}\) , for 145 values, 135 of which are repeats of the previous value
+\item
+  \(\tau ({\theta_i})\) ~for 9 values of incident angle, \emph{q\(_{i}\)} ?
+\end{enumerate}
+
+\subparagraph{Interior Solar Radiation Transmitted by Complex Fenestration}\label{interior-solar-radiation-transmitted-by-complex-fenestration}
+
+Diffuse Solar Radiation Transmitted by Complex Fenestration
+
+Distribution of solar radiation transmitted through exterior window is divided on diffuse and direct part.
+
+Diffuse solar transmitted through exterior complex fenestration and absorbed in interor walls is calculated and treated in same way as described in the section on Initial Distribution of Diffuse Solar Transmitted through Exterior and Interior Windows. Even though that BSDF is given for various directions, for purpose of diffuse solar radiation, transmittance and reflectances of fenestration system is integrated over incoming and outgoing hemisphere.~ Because incoming diffuse solar radiation is divided on ground and sky parts, integration of incoming hemisphere is also perfomed over ground and sky part (see equation .
+
+Direct Solar Radiation Transmitted by Complex Fenestration
+
+Direct solar (beam) transmitted through exterior window is using same overlap calculations (see Figure~\ref{fig:vertical-section-through-a-two-zone-building}) for each outgoing basis direction.~ For certain sun position, algorithm calculatates equivalent incoming beam number.~ The inside beam solar irradiance is calculated in similar manner as described in the section titled Interior Beam Radiation.
+
+\begin{equation}
+\begin{split}
+AISurf\left(SurfNum\right) =& \frac{AbsIntSurf\left(SurfNum\right)}{A\left(SurfNum\right)} \\
+&\cdot\sum_{i = 1}^{N_{extwin}} \left( \sum_{j = 1}^{N_{out}} TB{m_{k,j}} \cdot \Lambda_{k,j} \cdot \text{Aoverlap}_{k,j} \left( SurfNum \right)\right) \cdot \text{CosInc}_i
+\end{split}
+\end{equation}
+
+\emph{i} = exterior window number
+
+\emph{N\(_{extwin}\) =} number of exterior windows in zone
+
+\emph{N\(_{out}\) =} Beam number of exterior windows in zone
+
+\emph{CosInc\(_{i}\)} = cosine of angle of incidence of beam on exterior window \emph{i}
+
+\emph{TBm\(_{k,j}\)} = beam-to-beam transmittance of exterior window* i*at incidence direction k outgoing direction j
+
+\emph{Λ\(_{k,j}\)} = lambda value of exterior window* i*at incidence direction k for outgoing direction j
+
+\emph{Aoverlap\(_{k,j}\)(SurfNum)} = beam solar irradiated area of surface \emph{SurfNum} projected back onto the plane of exterior window* i* for incoming direction k and outgoing direction j (the \emph{Aoverlap}'s for an exterior window sum up to the glazed area of the window)
+
+\emph{AbsIntSurf(SurfNum)} = inside face solar absorptance of surface \emph{SurfNum}
+
+\emph{A(SurfNum)} = area of surface \emph{SurfNum} {[}m\(^{2}\){]}
+
+Equation is valid as long as surface which is hit by transmitted solar radiation is not another complex fenestration.~ In that case, for beam which is transmitted from other exterior window and reaches back surface of this window, angle of incidence needs to be taken into account.
+
+\subparagraph{Interior Solar Absorbed by Complex Fenestration}\label{interior-solar-absorbed-by-complex-fenestration}
+
+Solar radiation absorbed in window layers is coming from three sources: Diffuse radiation from sky and ground, direct radiation from the sun and beam radiation coming from the sun and it is transmitted through other exterior windows.
+
+Diffuse Radiation from Sky and Ground
+
+Energy absorbed in the layers and which originates from diffuse radiation from sky and ground is represented by following equation:
+
+\begin{equation}
+\begin{split}
+&\text{QRadSWwinAbs}(Surf, Lay) = \\
+&\sum_{i = 1}^{N_{layers}} \left(\text{WinSkyFtAbs}(Surf, Lay) \cdot \text{SkySolarInc} + \text{WinSkyGndAbs}(Surf, Lay) \cdot \text{GndSolarInc}\right)
+\end{split}
+\end{equation}
+
+where,
+
+\emph{WinSkyFtAbs(Lay)} = front absorptance averaged over sky for layer (Lay) and window belonging to Surf
+
+\emph{WinSkyGndAbs(Lay)} = front absorptance averaged over ground for layer (Lay) and window belonging to Surf
+
+\emph{SkySolarInc =} incident diffuse solar from the sky
+
+\emph{GndSolarInc} = incident diffuse solar from the ground
+
+Direct Radiation from the Sun
+
+Energy absorbed in the layers and which originates from direct solar radiation is given by following equation:
+
+\begin{equation}
+\text{QRadSWwinAbs}(SurfNum, Lay) = \text{AWinSurf}(SurfNum, Lay) \cdot \text{BeamSolar}
+\end{equation}
+
+where,
+
+\emph{AWinSurf(SurfNum,Lay)} -- is time step value of factor for beam absorbed in fenestration glass layers
+
+\emph{BeamSolar} -- Current beam normal solar irradiance
+
+Factor for time step value is given by equation:
+
+\begin{equation}
+\begin{split}
+\text{AWinSurf}(SurfNum,Lay) =& \text{WinBmFtAbs}(Lay,HourOfDay,TimeStep) \cdot \text{CosInc} \\
+&\cdot \text{SunLitFract} \cdot \text{OutProjSLFracMult}(HourOfDay)
+\end{split}
+\end{equation}
+
+where,
+
+\emph{WinBmFtAbs(Lay,HourOfDay,TimeStep)} -- is front directional absorptance for given layer and time
+
+\emph{CosInc} -- cosine of beam solar incident angle
+
+\emph{SunLitFract} -- sunlit fraction without shadowing effects of frame and divider
+
+\emph{OutProjSLFracMult(HourOfDay)} - Multiplier on sunlit fraction due to shadowing of glass by frame and divider outside projections.
+
+Direct Solar Radiation Coming from Sun and it is Transmitted Through Other Windows
+
+Direct solar radiation transmitted through other windows is using solar overlap calculations described in the section on Overlapping Shadows. Overlapping is used to determine amount of energy transferred through the window is hitting certain surface.~ That is used to calculate energy absorbed in walls and same approach will be used to calculate energy absorbed in window layers (equation ).~ In case when receiving surface is complex fenestration, it is not enought just to apply equation because factor AbsIntSurf is now depending of incoming angle which is defined through front and back directional absorptance matrices.~ It would mean that for each outgoing directions of transmitting complex fenestration, algorithm would need to determine what is best matching basis direction of receiving surface.~ Best receiving direction is used to determine absorptance factors which will be used in equation .~ It is important to understand that for basis definition, each unit vector defining one beam is going towards surface, which would mean that best matching directions from surface to surface will actually have minimal dot product.
+
+\begin{equation}
+Bes{t_{in}} = {\rm{min}}\left( {dot\left( {ou{t_p},i{n_1}} \right),dot\left( {ou{t_p},i{n_2}} \right), \ldots ,dot\left( {ou{t_p},i{n_N}} \right)} \right)
+\end{equation}
+
+where,
+
+Best\(_{in}\) -- is best matching receiving direction basis dot product (in\(_{k}\))
+
+out\(_{p}\) -- current transmitting complex fenestration direction
+
+in\(_{1}\), \ldots{}, in\(_{N}\) -- set of receiving complex fenestration basis directions
+
+Result of equation is minimal dot product, which corresponds to best matching direction of receiving surface.~ If we mark that direction with index k, then equation becomes:
+
+\begin{equation}
+  \begin{array}{l}
+    AWinSurf(SurfNum,Lay) = \\
+      \frac{1}{A(SurfNum)} \cdot \\
+      \sum_{i = 1}^{N_{extwin}} (\sum\limits_{j = 1}^{N_{out}} AbsIntSur{f_k}(SurfNum) \cdot TB{m_{k,j}} \cdot \\
+      A_{k,j} \cdot \text{Aoverlap}_{k,j}(SurfNum)) \cdot \text{CosInc}_i
+  \end{array}
+\end{equation}
+
+where,
+
+\emph{AbsIntSurf\(_{k}\)(SurfNum)} -- directional absorptance for the receiving surface for the best matching direction
+
+Everything else is same as described in equation .
+
+\subsubsection{References}\label{references-1-018}
+
+Klems, J. H. 1994A. ``A New Method for Predicting the Solar Heat Gain of Complex Fenestration Systems: I. Overview and Derivation of the Matrix Layer Calculation.''. ASHRAE Transactions. 100(pt.1): 1073-1086.
+
+Klems, J. H. 1994B. ``A New Method for Predicting the Solar Heat Gain of Complex Fenestration Systems: II. Detailed Description of the Matrix Layer Calculation.''. ASHRAE Transactions. 100(pt.1): 1073-1086.
+
+Klems, J. H. 1995. ``Measurements of Bidirectional Optical Properties of Complex Shading Devices.''. ASHRAE Transactions. 101(pt 1; Symposium Paper CH-95-8-1(RP-548)): 791-801.
+
+Klems, J. H. 1996. ``A Comparison between Calculated and Measured SHGC for Complex Glazing Systems.''. ASHRAE Transactions. 102(Pt. 1; Symposium Paper AT-96-16-1): 931-939.
+
+Klems, J. H. 1996. ``Calorimetric Measurements of Inward-Flowing Fraction for Complex Glazing and Shading Systems.''. ASHRAE Transactions. 102(Pt. 1; Symposium Paper AT-96-16-3): 947-954.
+
+Papamichael, K. J. 1998. ``Determination and Application of Bidirectional Solar-Optical Properties of Fenestration Systems.''. Cambridge, MA: 13th National Passive Solar Conference.
diff --git a/doc/engineering-reference/src/daylighting-and-window-calculations/window-heat-balance-calculation.tex b/doc/engineering-reference/src/daylighting-and-window-calculations/window-heat-balance-calculation.tex
new file mode 100644
index 00000000000..755117e7ccc
--- /dev/null
+++ b/doc/engineering-reference/src/daylighting-and-window-calculations/window-heat-balance-calculation.tex
@@ -0,0 +1,2570 @@
+\section{Window Heat Balance Calculation}\label{window-heat-balance-calculation}
+
+% table 36
+\begin{longtable}[c]{p{1.0in}p{2.5in}p{1.0in}p{1.5in}}
+\caption{Fortran Variables used in Window Heat Balance Calculations \label{table:fortran-variables-used-in-window-heat-balance}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Fortran Variables used in Window Heat Balance Calculations} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+N & Number of glass layers & - & nlayer \tabularnewline
+$\alpha$ & Stefan-Boltzmann constant & ~ & sigma \tabularnewline 
+$\varepsilon$\(_{i}\) & Emissivity of face i & - & emis \tabularnewline
+k\(_{i}\) & Conductance of glass layer i & W/m\(^{2}\)-K & scon \tabularnewline
+h\(_{o}\), h\(_{i}\) & Outside, inside air film convective conductance & W/m\(^{2}\)-K & hcout, hcout \tabularnewline
+h\(_{i}\) & Conductance of gap j & W/m\(^{2}\)-K & hgap \tabularnewline
+T\(_{o}\), T\(_{i}\) & Outdoor and indoor air temperatures & K & tout, tin \tabularnewline
+E\(_{o}\), E\(_{i}\) & Exterior, interior long-wave radiation incident on window & W/m\(^{2}\) & outir, rmir \tabularnewline
+$\theta$\(_{i}\) & Temperature of face i & K & thetas \tabularnewline
+S\(_{i}\) & Radiation (short-wave, and long-wave from zone internal sources) absorbed by face i & W/m\(^{2}\) & AbsRadGlassFace \tabularnewline
+I\(^{ext}_{bm}\) & Exterior beam normal solar irradiance & W/m\(^{2}\) & BeamSolarRad \tabularnewline
+I\(^{ext}_{dif}\) & Exterior diffuse solar irradiance on glazing & W/m\(^{2}\) & - \tabularnewline
+I\(^{int}_{sw}\) & Interior short-wave radiation (from lights and from reflected diffuse solar) incident on glazing from inside & W/m\(^{2}\) & QS \tabularnewline
+I\(^{int}_{lw}\) & Long-wave radiation from lights and equipment incident on glazing from inside & W/m\(^{2}\) & QL \tabularnewline
+$\varphi$ & Angle of incidence & radians & - \tabularnewline
+A\(^{f}_{j}\) & Front beam solar absorptance of glass layer j & - & - \tabularnewline
+A\(^{f,diff}_{j}\), A\(^{b,diff}_{j}\) & Front and back diffuse solar absorptance of glass layer j & - & AbsDiff, AbsDiffBack \tabularnewline
+A, B & Matrices used to solve glazing heat balance equations & W/m\(^{2}\), W/m\(^{2}\)-K & Aface, Bface \tabularnewline
+h\(_{r,i}\) & Radiative conductance for face i & W/m\(^{2}\)-K & hr(i) \tabularnewline
+$\Delta\theta$\(_{i}\) & Difference in temperature of face i between successive iterations & K & - \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{The Glazing Heat Balance Equations}\label{the-glazing-heat-balance-equations}
+
+The window glass face temperatures are determined by solving the heat balance equations on each face every time step. For a window with \emph{N} glass layers there are 2\emph{N} faces and therefore 2\emph{N} equations to solve. Figure~\ref{fig:glazing-system-with-two-glass-layers-showing} shows the variables used for double glazing (\emph{N} = 2).
+
+\begin{figure}[hbtp] % fig 95
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1470.png}
+\caption{Glazing system with two glass layers showing variables used in heat balance equations. \protect \label{fig:glazing-system-with-two-glass-layers-showing}}
+\end{figure}
+
+The following assumptions are made in deriving the heat balance equations:
+
+1)~~~~The glass layers are thin enough (a few millimeters) that heat storage in the glass can be neglected; therefore, there are no heat capacity terms in the equations.
+
+2)~~~~The heat flow is perpendicular to the glass faces and is one dimensional. See ``Edge of Glass Corrections,'' below, for adjustments to the gap conduction in multi-pane glazing to account for 2-D conduction effects across the pane separators at the boundaries of the glazing.
+
+3)~~~~The glass layers are opaque to IR. This is true for most glass products. For thin plastic suspended films this is not a good assumption, so the heat balance equations would have to be modified to handle this case.
+
+4)~~~~The glass faces are isothermal. This is generally a good assumption since glass conductivity is very high.
+
+5)~~~~The short wave radiation absorbed in a glass layer can be apportioned equally to the two faces of the layer.
+
+The four equations for double-glazing are as follows. The equations for single glazing (\emph{N} = 1) and for \emph{N} = 3 and \emph{N} = 4 are analogous and are not shown.
+
+\begin{equation}
+{E_o}{\varepsilon_1} - {\varepsilon_1}\sigma \theta_1^4 + {k_1}\left( {{\theta_2} - {\theta_1}} \right) + {h_o}\left( {{T_o} - {\theta_1}} \right) + {S_1} = 0
+\end{equation}
+
+\begin{equation}
+{k_1}\left( {{\theta_1} - {\theta_2}} \right) + {h_1}\left( {{\theta_3} - {\theta_2}} \right) + \sigma \frac{{{\varepsilon_2}{\varepsilon_3}}}{{1 - \left( {1 - {\varepsilon_2}} \right)\left( {1 - {\varepsilon_3}} \right)}}\left( {\theta_3^4 - \theta_2^4} \right) + {S_2} = 0
+\end{equation}
+
+\begin{equation}
+{h_1}({\theta_2} - {\theta_3}) + {k_2}({\theta_4} - {\theta_3}) + \sigma \frac{{{\varepsilon_2}{\varepsilon_3}}}{{1 - \left( {1 - {\varepsilon_2}} \right)\left( {1 - {\varepsilon_3}} \right)}}\left( {\theta_2^4 - \theta_3^4} \right) + {S_3} = 0
+\end{equation}
+
+\begin{equation}
+{E_i}{\varepsilon_4} - {\varepsilon_4}\sigma \theta_4^4 + {k_2}\left( {{\theta_3} - {\theta_4}} \right) + {h_i}\left( {{T_i} - {\theta_4}} \right) + {S_4} = 0
+\end{equation}
+
+\subsubsection{Absorbed Radiation}\label{absorbed-radiation}
+
+\emph{S\(_{i}\)} in Equations to is the radiation (short-wave and long-wave from zone lights and equipment) absorbed on the \emph{i}\(^{th}\) face. Short-wave radiation (solar and short-wave from lights) is assumed to be absorbed uniformly along a glass layer, so for the purposes of the heat balance calculation it is split equally between the two faces of a layer. Glass layers are assumed to be opaque to IR so that the thermal radiation from lights and equipment is assigned only to the inside (room-side) face of the inside glass layer. For \emph{N} glass layers \emph{S\(_{i}\)} is given by
+
+\begin{equation}
+{S_{2j - 1}} = {S_{2j}} = \frac{1}{2}\left( {I_{bm}^{ext}\cos \phi A_j^f(\phi ) + I_{dif}^{ext}A_j^{f,dif} + I_{sw}^{{\mathop{\rm int}} }A_j^{b,dif}} \right),{\rm{     }}j = 1{\rm{ to }}N
+\end{equation}
+
+\begin{equation}
+{S_{2N}} = {S_{2N}} + {\varepsilon_{2N}}I_{lw}^{{\mathop{\rm int}} }
+\end{equation}
+
+Here
+
+\(I_{bm}^{ext}\) = exterior beam normal solar irradiance
+
+\(I_{dif}^{ext}\) = exterior diffuse solar incident on glazing from outside
+
+\(I_{sw}^{{\mathop{\rm int}} }\) = interior short-wave radiation (from lights and from reflected diffuse solar) incident on glazing from inside
+
+\(I_{lw}^{{\mathop{\rm int}} }\) = long-wave radiation from lights and equipment incident on glazing from inside
+
+\({\varepsilon_{2N}}\) = emissivity (thermal absorptance) of the room-side face of the inside glass layer
+
+\subsection{Room-Side Convection}\label{room-side-convection}
+
+The correlation for room-side convection coefficient, \({h_i}\) , is from ISO 15099 section 8.3.2.2.~ (Prior to EnergyPlus version 3.1, the value for \({h_i}\) ~was modeled using the ``Detailed'' algorithm for opaque surface heat transfer, e.g.~for a vertical surface \({h_i} = 1.31{\left| {\Delta T} \right|^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}}\) ; see section Detailed Natural Convection Algorithm).~ The ISO 15099 correlation is for still room air and is determined in terms of the Nusselt number, \(Nu\) , where
+
+\begin{equation}
+{h_i} = Nu\left( {\frac{\lambda }{H}} \right)
+\end{equation}
+
+where,
+
+\(\lambda\) ~is the thermal conductivity of air, and
+
+\(H\) ~is the height of the window.
+
+The Rayleigh number based on height, \(R{a_H}\) , is calculated using,
+
+\begin{equation}
+R{a_H} = \frac{{{\rho ^2}{H^3}g\,{c_p}\left| {{T_{surf,i}} - {T_{air}}} \right|}}{{{T_{m,f}}\mu \lambda }}
+\end{equation}
+
+where,
+
+\(\rho\) ~is the density of air
+
+\(g\) ~is the acceleration due to gravity,
+
+\({c_p}\) ~is the specific heat of air,
+
+\(\mu\) ~is the dynamic viscosity of air, and
+
+\({T_{m,f}}\) ~is the mean film temperature in Kelvin given by,
+
+\begin{equation}
+{T_{m,f}} = {T_{air}} + \frac{1}{4}\left( {{T_{surf,i}} - {T_{air}}} \right)
+\end{equation}
+
+There are four cases for the Nusselt correlation that vary by the tilt angle in degrees, \(\gamma\) , and are based on heating conditions.~ For cooling conditions (where \({T_{surf,i}} > {T_{air}}\) ) the tilt angle is complemented so that \(\gamma = 180 - \gamma\)
+
+Case A. \({0^\circ } \le \gamma < 15^\circ\)
+
+\begin{equation}
+Nu = 0.13Ra_H^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}
+\end{equation}
+
+Case B. \(15^\circ \le \gamma \le 90^\circ\)
+
+\begin{equation}
+R{a_{cv}} = 2.5 \times {10^5}{\left( {\frac{{{e^{0.72\gamma }}}}{{\sin \lambda }}} \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{5}}}}
+\end{equation}
+
+\begin{equation}
+Nu = 0.56{\left( {R{a_H}\sin \gamma } \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{4}}}};\;for\;R{a_H} \le R{a_{CV}}
+\end{equation}
+
+\begin{equation}
+Nu = 0.13\left( {Ra_H^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}} - Ra_{CV}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}} \right) + 0.56{\left( {R{a_{CV}}\sin \gamma } \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{4}}}};\;R{a_H} > R{a_{CV}}
+\end{equation}
+
+Case C. \(90^\circ < \gamma \le 179^\circ\)
+
+\begin{equation}
+Nu = 0.56{\left( {R{a_H}\sin \gamma } \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{4}}}};\;{10^5} \le R{a_H}\sin \gamma  < {10^{11}}
+\end{equation}
+
+Case D. \(179^\circ < \gamma \le 180^\circ\)
+
+\begin{equation}
+Nu = 0.58Ra_H^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{5}}};\;R{a_H} \le {10^{11}}
+\end{equation}
+
+The material properties are evaluated at the mean film temperature.~ Standard EnergyPlus pyschrometric functions are used for \(\rho\) ~and \({c_p}\) .~ Thermal conductivity is calculated using,
+
+\(\lambda = 2.873 \times {10^{ - 3}} + 7.76 \times {10^{ - 5}}{T_{m,f}}\) .
+
+Kinematic viscosity is calculated using,
+
+\(\mu = 3.723 \times {10^{ - 6}} + 4.94 \times {10^{ - 8}}{T_{m,f}}\) .
+
+This correlation depends on the surface temperature of the room-side glazing surface and is therefore included inside the window heat balance interation loop.
+
+\subsection{Solving the Glazing Heat Balance Equations}\label{solving-the-glazing-heat-balance-equations}
+
+The equations are solved as follows:
+
+1)~~~~Linearize the equations by defining \({h_{r,i}} = {\varepsilon_i}\sigma \theta_i^3\) .~ For example, Equation becomes
+
+\begin{equation}
+{E_o}{\varepsilon_1} - {h_{r,1}}{\theta_1} + {k_1}\left( {{\theta_2} - {\theta_1}} \right) + {h_o}\left( {{T_o} - {\theta_1}} \right) + {S_1} = 0
+\end{equation}
+
+2)~~~~Write the equations in the matrix form \(A\theta = B\)
+
+3)~~~~Use previous time step's values of \({\theta_i}\) as initial values for the current time step. For the first time step of a design day or run period the initial values are estimated by treating the layers as a simple RC network.
+
+4)~~~~Save the \({\theta_i}\) ~for use in the next iteration: \({\theta_{prev,i}} = {\theta_i}\)
+
+5)~~~~Using \({\theta_{2N}}\) , reevaluate the room-side face surface convection coefficient \({h_i}\)
+
+6)~~~~Using the \({\theta_i}\) ~to evaluate the radiative conductances \({h_{r,i}}\)
+
+7)~~~~Find the solution \(\theta = {A^{ - 1}}B\) by LU decomposition
+
+8)~~~~Perform relaxation on the the new \({\theta_i}\) \textbf{:} \({\theta_i} \to \left( {{\theta_i} + {\theta_{prev,i}}} \right)/2\)
+
+9)~~~~Go to step 4
+
+Repeat steps 4 to 9 until the difference, \(\Delta {\theta_i}\) , between values of the \({\theta_i}\) ~in successive iterations is less than some tolerance value. Currently, the test is
+
+\begin{equation}
+\frac{1}{{2N}}\sum\limits_{i = 1}^{2N} {|\Delta {\theta_i}|{\rm{ }} < 0.02K}
+\end{equation}
+
+If this test does not pass after 100 iterations, the tolerance is increased to 0.2K. If the test still fails the program stops and an error message is issued.
+
+The value of the inside face temperature, \({\theta_{2N}}\) , determined in this way participates in the zone heat balance solution (see Outdoor/Exterior Convection) and thermal comfort calculation (see Occupant Thermal Comfort).
+
+\subsection{Edge-Of-Glass Effects}\label{edge-of-glass-effects}
+
+% table 37
+\begin{longtable}[c]{p{1.0in}p{2.5in}p{1.0in}p{1.5in}}
+\caption{Fortran Variables used in Edge of Glass calculations \label{table:fortran-variables-used-in-edge-of-glass}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Fortran Variables used in Edge of Glass calculations} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+\(\overline h\) & Area-weighted net conductance of glazing including edge-of-glass effects & W/m\(^{2}\)-K & - \tabularnewline
+A\(_{cg}\) & Area of center-of-glass region & m\(^{2}\) & CenterGlArea \tabularnewline
+A\(_{fe}\) & Area of frame edge region & m\(^{2}\) & FrameEdgeArea \tabularnewline
+A\(_{de}\) & Area of divider edge region & m\(^{2}\) & DividerEdgeArea \tabularnewline
+A\(_{tot}\) & Total glazing area & m\(^{2}\) & Surface\%Area \tabularnewline
+h\(_{cg}\) & Conductance of center-of-glass region (without air films) & W/m\(^{2}\)-K & - \tabularnewline
+h\(_{fe}\) & Conductance of frame edge region (without air films) & W/m\(^{2}\)-K & - \tabularnewline
+h\(_{de}\) & Conductance of divider edge region (without air films) & W/m\(^{2}\)-K & - \tabularnewline
+h\(_{ck}\) & Convective conductance of gap k & W/m\(^{2}\)-K & - \tabularnewline
+h\(_{rk}\) & Radiative conductance of gap k & W/m\(^{2}\)-K & - \tabularnewline
+$\eta$ & Area ratio & - & - \tabularnewline
+$\alpha$ & Conductance ratio & - & FrEdgeToCenterGlCondRatio, DivEdgeToCenterGlCondRatio \tabularnewline
+\bottomrule
+\end{longtable}
+
+Because of thermal bridging across the spacer separating the glass layers in multi-pane glazing, the conductance of the glazing near the frame and divider, where the spacers are located, is higher than it is in the center of the glass. The area-weighted net conductance (without inside and outside air films) of the glazing in this case can be written
+
+\begin{equation}
+\overline h  = \left( {{A_{cg}}{h_{cg}} + {A_{fe}}{h_{fe}} + {A_{de}}{h_{de}}} \right)/{A_{tot}}
+\end{equation}
+
+where
+
+\emph{h\(_{cg}\)} = conductance of center-of-glass region (without air films)
+
+\emph{h\(_{fe}\)} = conductance of frame edge region (without air films)
+
+\emph{h\(_{de}\)} = conductance of divider edge region (without air films)
+
+\emph{A\(_{cg}\)} = area of center-of-glass region
+
+\emph{A\(_{fe}\)} = area of frame edge region
+
+\emph{A\(_{de}\)} = area of divider edge region
+
+\emph{A\(_{tot}\)} = total glazing area = \({A_{cg}} + {A_{fe}} + {A_{de}}\)
+
+The different regions are shown in Figure~\ref{fig:different-types-of-glass-regions.}:
+
+\begin{figure}[hbtp] % fig 96
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1534.png}
+\caption{Different types of glass regions. \label{fig:different-types-of-glass-regions.}}
+\end{figure}
+
+Equation can be rewritten as
+
+\begin{equation}
+\overline h  = {h_{cg}}\left( {{\eta_{cg}} + {\alpha_{fe}}{\eta_{fe}} + {\alpha_{de}}{\eta_{de}}} \right)
+\end{equation}
+
+where
+
+\begin{equation}
+{\eta_{cg}} = {A_{cg}}/{A_{tot}}
+\end{equation}
+
+\begin{equation}
+{\eta_{fe}} = {A_{fe}}/{A_{tot}}
+\end{equation}
+
+\begin{equation}
+{\eta_{de}} = {A_{de}}/{A_{tot}}
+\end{equation}
+
+\begin{equation}
+{\alpha_{fe}} = {h_{fe}}/{h_{cg}}
+\end{equation}
+
+\begin{equation}
+{\alpha_{de}} = {h_{de}}/{h_{cg}}
+\end{equation}
+
+The conductance ratios \({\alpha_{fe}}\) ~and \({\alpha_{de}}\) are user inputs obtained from Window 5. They depend on the glazing construction as well as the spacer type, gap width, and frame and divider type.
+
+In the EnergyPlus glazing heat balance calculation effective gap convective conductances are used to account for the edge-of-glass effects. These effective conductances are determined as follows for the case with two gaps (triple glazing). The approach for other numbers of gaps is analogous.
+
+Neglecting the very small resistance of the glass layers, the center-of-glass conductance (without inside and outside air films) can be written as
+
+\begin{equation}
+{h_{cg}} = {\left( {{{\left( {{h_{r,1}} + {h_{c,1}}} \right)}^{ - 1}} + {{\left( {{h_{r,2}} + {h_{c,2}}} \right)}^{ - 1}}} \right)^{ - 1}}
+\end{equation}
+
+where
+
+\emph{h\(_{c,k}\)} = convective conductance of the \emph{k\(^{h}\)} gap
+
+\emph{h\(_{r,k}\)} = radiative conductance of the \emph{k\(^{h}\)} gap
+
+\begin{equation}
+= \frac{1}{2}\sigma \frac{{{\varepsilon_i}{\varepsilon_j}}}{{1 - \left( {1 - {\varepsilon_i}} \right)\left( {1 - {\varepsilon_j}} \right)}}{\left( {{\theta_i} + {\theta_j}} \right)^3}
+\end{equation}
+
+$\varepsilon$\(_{i}\), $\varepsilon$\(_{j}\) = emissivity of the faces bounding the gap
+
+$\theta$\(_{i}\), $\theta$\(_{j}\) = temperature of faces bounding the gap (K)
+
+Equation then becomes
+
+\begin{equation}
+\overline h  = \left( {{\eta_{cg}} + {\alpha_{fe}}{\eta_{fe}} + {\alpha_{de}}{\eta_{de}}} \right){\left( {{{\left( {{h_{r,1}} + {h_{c,1}}} \right)}^{ - 1}} + {{\left( {{h_{r,2}} + {h_{c,2}}} \right)}^{ - 1}}} \right)^{ - 1}}
+\end{equation}
+
+We can also write \(\overline h\) in terms of effective convective conductances of the gaps as
+
+\begin{equation}
+\overline h  = {\left( {{{\left( {{h_{r,1}} + {{\overline h }_{c,1}}} \right)}^{ - 1}} + {{\left( {{h_{r,2}} + {{\overline h }_{c,2}}} \right)}^{ - 1}}} \right)^{ - 1}}
+\end{equation}
+
+Comparing Eqs. and we obtain
+
+\begin{equation}
+{h_{r,k}} + {\overline h_{c,k}} = \left( {{\eta_{cg}} + {\alpha_{fe}}{\eta_{fe}} + {\alpha_{de}}{\eta_{de}}} \right)\left( {{h_{r,k}} + {h_{c,k}}} \right)
+\end{equation}
+
+Using \({\eta_{cg}} = 1 - {\eta_{fe}} - {\eta_{de}}\) ~gives
+
+\begin{equation}
+{\overline h_{c,k}} = {h_{r,k}}\left( {{\eta_{fe}}\left( {{\alpha_{fe}} - 1} \right) + {\eta_{de}}\left( {{\alpha_{de}} - 1} \right)} \right) + {h_{c,k}}\left( {1 + {\eta_{fe}}\left( {{\alpha_{fe}} - 1} \right) + {\eta_{de}}\left( {{\alpha_{de}} - 1} \right)} \right)
+\end{equation}
+
+This is the expression used by EnergyPlus for the gap convective conductance when a frame or divider is present.
+
+\subsection{Apportioning of Absorbed Short-Wave Radiation in Shading Device Layers}\label{apportioning-of-absorbed-short-wave-radiation-in-shading-device-layers}
+
+If a shading device has a non-zero short-wave transmittance then absorption takes place throughout the shading device layer. The following algorithm is used to apportion the absorbed short-wave radiation to the two faces of the layer. Here \emph{f\(_{1}\)} is the fraction assigned to the face closest to the incident radiation and \emph{f\(_{2}\)} is the fraction assigned to the face furthest from the incident radiation.
+
+~\({f_1} = 1,{\rm{ }}{f_2} = 0{\rm{ if }}{\tau_{sh}} = 0\)
+
+Otherwise
+
+\begin{equation}
+  \begin{array}{cl}
+    f_1 = 0,\;f_2 = 0 &\text{if} \alpha_{sh} \le 0.01 \\
+    f_1 = 1,\;f_2 = 0 &\text{if} \alpha_{sh} > 0.999 \\
+    \left.
+      \begin{array}{l}
+        f_1 = \frac{1 - e^{0.5 \ln (1 - \alpha_{sh}}} {\alpha_{sh}} \\
+        f_2 = 1 - {f_1}
+      \end{array}
+    \right\} &\text{if} 0.01 lt \alpha_{sh} \le 0.999
+  \end{array}
+\end{equation}
+
+\subsection{Window~ Frame and Divider Calculation}\label{window-frame-and-divider-calculation}
+
+For the zone heat balance calculation the inside surface temperature of the frame and that of the divider are needed. These temperatures are determined by solving the heat balance equations on the inside and outside surfaces of the frame and divider.
+
+% table 38
+\begin{longtable}[c]{p{1.0in}p{2.5in}p{1.0in}p{1.5in}}
+\caption{Fortran Variables used in Window/Frame and Divider calculations \label{table:fortran-variables-used-in-windowframe}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Fortran Variables used in Window/Frame and Divider calculations} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+Q\(_{ExtIR,abs}\) & IR from the exterior surround absorbed by outside frame surfaces & W & - \tabularnewline
+Q\(_{IR,emitted}\) & IR emitted by outside frame surfaces & W & - \tabularnewline
+Q\(_{conv}\) & Convection from outside air to outside frame surfaces & W & - \tabularnewline
+Q\(_{cond}\) & Conduction through frame from inside frame surfaces to outside frame surfaces & W & - \tabularnewline
+Q\(_{abs}\) & Solar radiation plus outside glass IR absorbed by outside of frame & W & - \tabularnewline
+Q\(^{dif}_{abs,sol}\) & Diffuse solar absorbed by outside frame surfaces, per unit frame face area & W/m\(^{2}\) & - \tabularnewline
+Q\(^{bm}_{abs,sol}\) & Beam solar absorbed by outside frame surfaces, per unit frame face area & W/m\(^{2}\) & - \tabularnewline
+I\(^{dif}_{ext}\) & Diffuse solar incident on window & W/m\(^{2}\) & - \tabularnewline
+I\(^{bm}_{ext}\) & Direct normal solar irradiance & W/m\(^{2}\) & - \tabularnewline
+$\alpha$\(^{fr}_{sol}\) & Solar absorptance of frame & - & FrameSolAbsorp \tabularnewline
+R\(_{gl}^{f,dif}\) & Front diffuse solar reflectance of glazing & - & ~ \tabularnewline
+R\(_{gl}^{f,bm}\) & Front beam solar reflectance of glazing & - & ~ \tabularnewline
+cos($\beta$\(_{face}\)) & Cosine of angle of incidence of beam solar on frame outside face & ~ & CosIncAng \tabularnewline
+cos($\beta$\(_{h}\)) & Cosine of angle of incidence of beam solar on frame projection parallel to window x-axis & - & CosIncAngHorProj \tabularnewline
+cos($\beta$\(_{v}\)) & Cosine of angle of incidence of beam solar on frame projection parallel to window y-axis & - & CosIncAngVertProj \tabularnewline
+f\(_{sunlight}\) & Fraction of window that is sunlit & - & SunlitFrac \tabularnewline
+A\(_{f}\) & Area of frame’s outside face (same as area of frame’s inside face) & m\(^{2}\) & - \tabularnewline
+A\(_{p1}\), A\(_{p2}\) & Area of frame’s outside and inside projection faces & m\(^{2}\) & - \tabularnewline
+F\(_{f}\) & Form factor of frame’s outside or inside face for IR & - & - \tabularnewline
+F\(_{p1}\), F\(_{p2}\) & Form factor of frame outside projection for exterior IR; form factor of frame inside projection for interior IR & - & - \tabularnewline
+E\(_{o}\) & Exterior IR incident on window plane & W/m\(^{2}\) & outir \tabularnewline
+E\(_{i}\) & Interior IR incident on window plane & W/m\(^{2}\) & SurroundIRfromParentZone \tabularnewline
+$\varepsilon$\(_{1}\), $\varepsilon$\(_{2}\) & Outside, inside frame surface emissivity & - & FrameEmis \tabularnewline
+$\theta$\(_{1}\), $\theta$\(_{2}\) & Frame outside, inside surface temperature & K & FrameTempSurfOut, FrameTempSurfIn \tabularnewline
+T\(_{o}\), T\(_{i}\) & Outdoor and indoor air temperatures & K & tout, tin \tabularnewline
+h\(_{o,c}\), h\(_{i,c}\) & Frame outside and inside air film convective conductance & W/m\(^{2}\)-K & HOutConv, HInConv \tabularnewline
+k & Effective inside-surface to outside-surface conductance of frame per unit area of frame projected onto window plane & W/m\(^{2}\)-K & FrameConductance, FrameCon \tabularnewline
+S\(_{1}\) & Q\(_{abs}\)/A\(_{f}\) & W/m\(^{2}\)-K & FrameQRadOutAbs \tabularnewline
+S\(_{2}\) & Interior short-wave radiation plus interior IR from internal sources absorbed by inside of frame divided by A\(_{f}\) & W/m\(^{2}\)-K & FrameQRadInAbs \tabularnewline
+$\eta$\(_{1}\), $\eta$\(_{2}\) & A\(_{p1}\)/A\(_{f}\), A\(_{p2}\)/A\(_{f}\) & - & - \tabularnewline
+H & Height of glazed portion of window & m & Surface\%Height \tabularnewline
+W & Width of glazed portion of window & m & Surface\%Width \tabularnewline
+w\(_{f}\), w\(_{d}\) & Frame width, divider width & m & FrameWidth, DividerWidth \tabularnewline
+p\(_{f1}\), p\(_{f2}\) & Frame outside, inside projection & m & FrameProjectionOut, FrameProjectionIn \tabularnewline
+N\(_{h}\), N\(_{v}\) & Number of horizontal, vertical dividers & - & HorDividers, VertDividers \tabularnewline
+T\(_{o,r}\), T\(_{i,r}\) & Frame outside, inside radiative temperature & K & TOutRadFr, TInRadFr \tabularnewline
+h\(_{o,r}\), h\(_{i,r}\) & Frame outside, inside surface radiative conductance & W/m\(^{2}\)-K & HOutRad, HInRad \tabularnewline
+A & Intermediate variable in frame heat balance solution & K & Afac \tabularnewline
+C & Intermediate variable in frame heat balance solution & - & Efac \tabularnewline
+B, D & Intermediate variables in frame heat balance solution & - & Bfac, Dfac \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Frame Temperature Calculation}\label{frame-temperature-calculation}
+
+Figure~\ref{fig:cross-section-through-a-window-showing-frame} shows a cross section through a window showing frame and divider. The outside and inside frame and divider surfaces are assumed to be isothermal. The frame and divider profiles are approximated as rectangular since this simplifies calculating heat gains and losses (see ``Error Due to Assuming a Rectangular Profile,'' below).
+
+\begin{figure}[hbtp] % fig 97
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1557.png}
+\caption{Cross section through a window showing frame and divider (exaggerated horizontally). \label{fig:cross-section-through-a-window-showing-frame}}
+\end{figure}
+
+\textbf{~}
+
+\subsubsection{Frame Outside Surface Heat Balance}\label{frame-outside-surface-heat-balance}
+
+The outside surface heat balance equation is
+
+\begin{equation}
+{Q_{ExtIR,abs}} - {Q_{IR,emitted}} + {Q_{conv}} + {Q_{cond}} + {Q_{abs}} = 0
+\end{equation}
+
+where
+
+\({Q_{ExtIR,abs}}\) ~ = IR from the exterior surround (sky and ground) absorbed by outside frame surfaces
+
+\({Q_{IR,emitted}}\) = IR emitted by outside frame surfaces
+
+\({Q_{conv}}\) = convection from outside air to outside frame surfaces
+
+\({Q_{cond}}\) = conduction through frame from inside frame surfaces to outside frame surfaces
+
+\({Q_{abs}}\) = solar radiation (from sun, sky and ground) plus IR from outside window surface absorbed by outside frame surfaces (see ``Calculation of Absorbed Solar Radiation,'' below).
+
+The first term can be written as the sum of the exterior IR absorbed by the outside face of the frame and the exterior IR absorbed by the frame's outside projection surfaces.
+
+\begin{equation}
+{Q_{ExtIR,abs}} = {\varepsilon_1}{E_o}{A_f}{F_f} + {\varepsilon_1}{E_o}{A_{p1}}{F_{p1}}
+\end{equation}
+
+where \emph{ε\(_{1}\)} is the outside surface emissivity.
+
+The exterior IR incident on the plane of the window, \emph{E\(_{o}\)}, is the sum of the IR from the sky, ground and obstructions. For the purposes of the frame heat balance calculation it is assumed to be isotropic. For isotropic incident IR, \emph{F\(_{f}\)} = 1.0 and \emph{F\(_{p1}\)} = 0.5, which gives
+
+\begin{equation}
+{Q_{ExtIR,abs}} = {\varepsilon_1}{E_o}({A_f} + \frac{1}{2}{A_{p1}})
+\end{equation}
+
+The IR emitted by the outside frame surfaces is
+
+\begin{equation}
+{Q_{ExtIR,emitted}} = {\varepsilon_1}\sigma ({A_f} + {A_{p1}})\theta_1^4
+\end{equation}
+
+The convective heat flow from the outside air to the outside frame surfaces is
+
+\begin{equation}
+{Q_{conv}} = {h_{o,c}}({A_f} + {A_{p1}})({T_o} - {\theta_1})
+\end{equation}
+
+The conduction through the frame from inside to outside is
+
+\begin{equation}
+{Q_{cond}} = k{A_f}({\theta_2} - {\theta_1})
+\end{equation}
+
+Note that \emph{A\(_{f}\) ~}is used here since the conductance, \emph{k}, is, by definition, per unit area of frame projected onto the plane of the window.
+
+Adding these expressions for the \emph{Q} terms and dividing by* A\(_{f}\)*~gives
+
+\begin{equation}
+{E_0}{\varepsilon_1}\left( {1 + \frac{1}{2}{\eta_1}} \right) - {\varepsilon_1}\left( {1 + {\eta_1}} \right)\theta_1^4 + {h_{o,c}}\left( {1 + {\eta_1}} \right)\left( {{T_0} - {\theta_1}} \right) + k\left( {{\theta_2} - {\theta_1}} \right) + {S_1} = 0
+\end{equation}
+
+where \emph{S\(_{1}\)} = \emph{Q\(_{abs}\)/A\(_{f}\)}~and
+
+\begin{equation}
+{\eta_1} = \frac{{{A_{p1}}}}{{{A_f}}} = \left( {\frac{{{p_{f,1}}}}{{{w_f}}}} \right)\frac{{H + W - ({N_h} + {N_v}){w_d}}}{{H + W + 2{w_f}}}
+\end{equation}
+
+We linearize Eq. as follows.
+
+Write the first two terms as
+
+\begin{equation}
+{\varepsilon_1}(1 + {\eta_1})[{E_o}(1 + \frac{1}{2}{\eta_1})/(1 + {\eta_1}) - \theta_1^4]
+\end{equation}
+
+and define a radiative temperature
+
+\begin{equation}
+{T_{o,r}} = {[{E_o}(1 + \frac{1}{2}{\eta_1})/(1 + {\eta_1})]^{1/4}}
+\end{equation}
+
+This gives
+
+\begin{equation}
+{\varepsilon_1}(1 + {\eta_1})[T_{o,r}^4 - \theta_1^4]
+\end{equation}
+
+which, within a few percent, equals
+
+\begin{equation}
+{\varepsilon_1}(1 + {\eta_1})\frac{{{{({T_{o,r}} + {\theta_1})}^3}}}{2}({T_{o,r}} - {\theta_1})
+\end{equation}
+
+Defining an outside surface radiative conductance as follows
+
+\begin{equation}
+{h_{o,r}} = {\varepsilon_1}(1 + {\eta_1})\frac{{{{({T_{o,r}} + {\theta_1})}^3}}}{2}
+\end{equation}
+
+then gives
+
+\begin{equation}
+{h_{o,r}}({T_{o,r}} - {\theta_1})
+\end{equation}
+
+The final outside surface heat balance equation in linearized form is then
+
+\begin{equation}
+{h_{o,r}}({T_{o,r}} - {\theta_1}) + {h_{o,c}}(1 + {\eta_1})({T_o} - {\theta_1}) + k({\theta_2} - {\theta_1}) + {S_1} = 0
+\end{equation}
+
+\subsubsection{Frame Inside Surface Heat Balance}\label{frame-inside-surface-heat-balance}
+
+A similar approach can be used to obtain the following linearized \emph{inside} surface heat balance equation:
+
+\begin{equation}
+{h_{i,r}}({T_{i,r}} - {\theta_2}) + {h_{i,c}}(1 + {\eta_2})({T_i} - {\theta_2}) + k({\theta_1} - {\theta_2}) + {S_2} = 0
+\end{equation}
+
+where
+
+\begin{equation}
+{T_{i,r}} = {[{E_i}(1 + \frac{1}{2}{\eta_2})/(1 + {\eta_2})]^{1/4}}
+\end{equation}
+
+\begin{equation}
+{\eta_2} = \frac{{{A_{p2}}}}{{{A_f}}} = \left( {\frac{{{p_{f,2}}}}{{{w_f}}}} \right)\frac{{H + W - ({N_h} + {N_v}){w_d}}}{{H + W + 2{w_f}}}
+\end{equation}
+
+and \emph{E\(_{i}\)} is the interior IR irradiance incident on the plane of the window.
+
+Solving Eqs. and simultaneously gives
+
+\begin{equation}
+{\theta_2} = \frac{{D + CA}}{{1 - CB}}
+\end{equation}
+
+with
+
+\begin{equation}
+A = \frac{{{h_{o,r}}{T_{o,r}} + {h_{o,c}}{T_o} + {S_1}}}{{{h_{o,r}} + k + {h_{o,c}}}}
+\end{equation}
+
+\begin{equation}
+B = \frac{k}{{{h_{o,r}} + k + {h_{o,c}}}}
+\end{equation}
+
+\begin{equation}
+C = \frac{k}{{{h_{i,r}} + k + {h_{i,c}}}}
+\end{equation}
+
+\begin{equation}
+D = \frac{{{h_{i,r}}{T_{i,r}} + {h_{i,c}}{T_i} + {S_2}}}{{{h_{i,r}} + k + {h_{i,c}}}}
+\end{equation}
+
+\subsubsection{Calculation of Solar Radiation Absorbed by Frame}\label{calculation-of-solar-radiation-absorbed-by-frame}
+
+The frame outside face and outside projections and inside projections absorb beam solar radiation (if sunlight is striking the window) and diffuse solar radiation from the sky and ground. For the outside surfaces of the frame, the absorbed diffuse solar per unit frame face area is
+
+\begin{equation}
+Q_{abs,sol}^{dif} = I_{ext}^{dif}{\alpha_{fr,sol}}\left( {{A_f} + {F_{p1}}{A_{p1}}} \right)/{A_f} = I_{ext}^{dif}{\alpha_{fr,sol}}\left( {1 + 0.5\frac{{{A_{p1}}}}{{{A_f}}}} \right)
+\end{equation}
+
+If there is no exterior window shade, \emph{~I\(^{dif}\)\(_{ext}\)} includes the effect of diffuse solar reflecting off of the glazing onto the outside frame projection, i.e.,
+
+\begin{equation}
+I_{ext}^{dif} \to I_{ext}^{dif}\left( {1 + R_{gl}^{f,dif}} \right)
+\end{equation}
+
+The beam solar absorbed by the outside face of the frame, per unit frame face area is
+
+\begin{equation}
+Q_{abs,sol}^{bm,face} = I_{ext}^{bm}{\alpha_{fr,sol}}\cos {\beta_{face}}{f_{sunlit}}
+\end{equation}
+
+The beam solar absorbed by the frame outside projection parallel to the window x-axis is
+
+\begin{equation}
+Q_{abs,sol}^{bm,h} = I_{ext}^{bm}{\alpha_{fr,sol}}\cos {\beta_h}{p_{f1}}\left( {W - {N_v}{w_d}} \right){f_{sunlit}}/{A_f}
+\end{equation}
+
+Here it is assumed that the sunlit fraction, \emph{f\(_{sunlit}\)}, for the window can be applied to the window frame. Note that at any given time beam solar can strike only one of the two projection surfaces that are parallel to the window x-axis. If there is no exterior window shade, \emph{I\(^{bm}\)\(_{ext}\)} includes the effect of beam solar reflecting off of the glazing onto the outside frame projection, i.e.,
+
+\begin{equation}
+I_{ext}^{bm} \to I_{ext}^{bm}\left( {1 + R_{gl}^{f,bm}} \right)
+\end{equation}
+
+The beam solar absorbed by the frame outside projection parallel to the window y-axis is
+
+\begin{equation}
+Q_{abs,sol}^{bm,v} = I_{ext}^{bm}{\alpha_{fr,sol}}\cos {\beta_v}{p_{f1}}\left( {H - {N_h}{w_d}} \right){f_{sunlit}}/{A_f}
+\end{equation}
+
+Using a similar approach, the beam and diffuse solar absorbed by the \emph{inside} frame projections is calculated, taking the transmittance of the glazing into account.
+
+\subsubsection{Error Due to Assuming a Rectangular Profile}\label{error-due-to-assuming-a-rectangular-profile}
+
+Assuming that the inside and outside frame profile is rectangular introduces an error in the surface heat transfer calculation if the profile is non-rectangular. The percent error in the calculation of convection and emitted IR is approximately 100\(\left| {{L_{profile,rect}} - {L_{profile,actual}}} \right|/{L_{profile,rect}}\) , where \emph{L\(_{profile,rect}\)} is the profile length for a rectangular profile (\emph{w\(_{f}\)} +* p\(_{f1}\)* for outside of frame or \emph{w\(_{f}\)} + \emph{p\(_{f2}\)}for inside of frame) and \emph{L\(_{profile,actual}\)} is the actual profile length. For example, for a circular profile \emph{vs} a square profile the error is about 22\%. The error in the calculation of absorbed beam radiation is close to zero since the beam radiation intercepted by the profile is insensitive to the shape of the profile. The error in the absorbed diffuse radiation and absorbed IR depends on details of the shape of the profile. For example, for a circular profile vs.~a square profile the error is about 15\%.
+
+\subsubsection{Divider Temperature Calculation}\label{divider-temperature-calculation}
+
+The divider inside and outside surface temperatures are determined by a heat balance calculation that is analogous to the frame heat balance calculation described above.
+
+\subsection{Beam Solar Reflection from Window Reveal Surfaces}\label{beam-solar-reflection-from-window-reveal-surfaces}
+
+This section describes how beam solar radiation that is reflected from window reveal surfaces is calculated. Reflection from outside reveal surfaces---which are associated with the setback of the glazing from the outside surface of the window's parent wall---increases the solar gain through the glazing. Reflection from inside reveal surfaces---which are associated with the setback of the glazing from the inside surface of the window's parent wall---decreases the solar gain to the zone because some of this radiation is reflected back out of the window.
+
+The amount of beam solar reflected from reveal surfaces depends, among other things, on the extent to which reveal surfaces are shadowed by other reveal surfaces. An example of this shadowing is shown in Figure~\ref{fig:example-of-shadowing-of-reveal-surfaces-by}. In this case the sun is positioned such that the top reveal surfaces shadow the left and bottom reveal surfaces. And the right reveal surfaces shadow the bottom reveal surfaces. The result is that the left/outside, bottom/outside, left/inside and bottom/inside reveal surfaces each have sunlit areas. Note that the top and right reveal surfaces are facing away from the sun in this example so their sunlit areas are zero.
+
+\begin{figure}[hbtp] % fig 98
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1593.png}
+\caption{Example of shadowing of reveal surfaces by other reveal surfaces. \protect \label{fig:example-of-shadowing-of-reveal-surfaces-by}}
+\end{figure}
+
+The size of the shadowed areas, and the size of the corresponding illuminated areas, depends on the following factors:
+
+\begin{itemize}
+\item
+  The sun position relative to the window
+\item
+  The height and width of the window
+\item
+  The depth of the outside and inside reveal surfaces
+\end{itemize}
+
+We will assume that the reveal surfaces are perpendicular to the window plane and that the window is rectangular. Then the above factors determine a unique shadow pattern. From the geometry of the pattern the shadowed areas and corresponding illuminated areas can be determined. This calculation is done in subroutine CalcBeamSolarReflectedFromWinRevealSurface in the SolarShading module. The window reveal input data is specified in the WindowProperty:FrameAndDivider object expect for the depth of the outside reveal, which is determined from the vertex locations of the window and its parent wall.
+
+If an exterior shading device (shade, screen or blind) is in place it is assumed that it blocks beam solar before it reaches outside or inside reveal surfaces. Correspondingly, it is assumed that an interior or between-glass shading device blocks beam solar before it reaches inside reveal surfaces.
+
+Representative shadow patterns are shown in Figure 99 for a window with no shading device, and without and with a frame. The case with a frame has to be considered separately because the frame can cast an additional shadow on the inside reveal surfaces.
+
+The patterns shown apply to both vertical and horizontal reveal surfaces. It is important to keep in mind that, for a window of arbitrary tilt, if the left reveal surfaces are illuminated the right surfaces will not be, and vice versa. And if the bottom reveal surfaces are illuminated the top surfaces will not be, and vice versa. (Of course, for a vertical window, the top reveal surfaces will never be illuminated by beam solar if the reveal surfaces are perpendicular to the glazing, as is being assumed.
+
+For each shadow pattern in Figure 99, equations are given for the shadowed areas \({A_{1,sh}}\) ~and \emph{\({A_{2,sh}}\)}~of the outside and inside reveal surfaces, respectively. The variables in these equations are the following (see also Figure~\ref{fig:vertical-section-through-a-vertical-window}):
+
+\({d_1}\) ~~~~~~~ = depth of outside reveal, measured from the outside plane of the glazing to the edge of the reveal, plus one half of the glazing thickness.
+
+\({d_2}\) ~~ ~~~~~ = depth of inside reveal (or, for illumination on bottom reveal surfaces,~ inside sill depth), measured from the inside plane of the glazing to the edge of the reveal or the sill, plus one half of the glazing thickness.
+
+\(L\) ~~~~~~~ = window height for vertical reveal surfaces or window width for horizontal reveal surfaces
+
+\(\alpha\) ~~~~~~~~~ = vertical solar profile angle for shadowing on vertical reveal surfaces or horizontal solar profile angle for shadowing on horizontal reveal surfaces.
+
+\({p_1}({p_2})\) ~ = distance from outside (inside) surface of frame to glazing midplane.
+
+\({d_2}^\prime\) ~~~~~ = depth of shadow cast by top reveal on bottom reveal, or by left reveal on right reveal, or by right reveal on left reveal.
+
+\({d_2}^{\prime \prime }\) ~~~~ = depth of shadow cast by frame.
+
+For simplicity it is assumed that, for the case without a frame, the shadowed and illuminated areas extend into the glazing region. For this reason, \({d_1}\) and \({d_2}\) are measured from the midplane of the glazing. For the case with a frame, the beam solar absorbed by the surfaces formed by the frame outside and inside projections perpendicular to the glazing is calculated as described in ``Window Frame and Divider Calculation: Calculation of Solar Radiation Absorbed by Frame.''
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image1605.png}
+\caption{Expression for area of shaded regions for different shadow patterns: (a) window without frame, (b) window with frame}
+\end{figure}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image1606.png}
+\caption{Expression for area of shaded regions for different shadow patterns: (a) window without frame, (b) window with frame}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 100
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1607.png}
+\caption{Vertical section through a vertical window with outside and inside reveal showing calculation of the shadows cast by the top reveal onto the inside sill and by the frame onto the inside sill. \protect \label{fig:vertical-section-through-a-vertical-window}}
+\end{figure}
+
+The following logic gives expressions for the shadowed areas for all possible shadow patterns. Here:
+
+d1 = \({d_1}\)
+
+d2 = \({d_2}\)
+
+P1 = \({p_1}\)
+
+P2 = \({p_2}\)
+
+f1 = \({d_1} - {p_1}\)
+
+f2 = \({d_2} - {p_2}\)
+
+d2prime = \({d_2}^\prime\)
+
+d2prime2 = \({d_2}^{\prime \prime }\)
+
+d12 = \({d_1} + {d_2} - {d_2}^\prime\)
+
+TanAlpha = \(\tan \alpha\)
+
+A1sh = \({A_{1,sh}}\)
+
+A2sh = \({A_{2,sh}}\)
+
+L = \(L\)
+
+L1 = average distance to frame of illuminated area of outside reveal (used to calculate view factor to frame).
+
+L2 = average distance to frame of illuminated area of inside reveal (used to calculate view factor to frame).
+
+\begin{lstlisting}
+ IF(window does not have a frame) THEN
+      IF(d2prime < = d2) THEN
+     IF(d12*TanAlpha < = L) THEN
+       A1sh = 0.5*TanAlpha*d1**2
+       A2sh = d2prime*L + 0.5*TanAlpha*d12**2 - A1sh
+     ELSE  ! d12*TanAlpha > L
+       IF(d1*TanAlpha < = L) THEN
+         A1sh = 0.5*TanAlpha*d1**2
+         A2sh = d2*L - 0.5*TanAlpha*(L/TanAlpha - d1)**2
+       ELSE  ! d1*TanAlpha > L
+         A1sh = d1*L - (0.5/TanAlpha)*L**2
+         A2sh = d2*L
+       END IF
+     END IF
+   ELSE  ! d2prime > d2
+     A2sh = d2*L
+     IF(d2prime < d1+d2) THEN
+       IF(d12*TanAlpha < = L) THEN
+         A1sh = L*(d2prime-d2) + 0.5*TanAlpha*d12**2
+       ELSE  ! d12*TanAlpha > L
+         A1sh = d1*L - 0.5*L**2/TanAlpha
+       END IF
+     ELSE  ! d2prime > = d1+d2
+       A1sh = d1*L
+     END IF
+   END IF
+ ELSE  ! Window has a frame
+  f1 = d1-P1
+  f2 = d2-P2
+  d2prime2 = FrameWidth/TanGamma
+  IF(vertical reveal) THEN  ! Vertical reveal
+    IF(InsReveal+0.5*GlazingThickness < = P2) d2 = P2 + 0.001
+  ELSE                      ! Horizontal
+    IF(bottom reveal surfaces may be illuminated) THEN
+      ! Bottom reveal surfaces may be illuminated
+      IF(InsSillDepth+0.5*GlazingThickness< = P2) d2 = P2 + 0.001
+    ELSE
+      ! Top reveal surfaces may be illuminated
+      IF(InsReveal+0.5*GlazingThickness < = P2) d2 = P2 + 0.001
+    END IF
+  END IF
+  IF(d2prime < = f2) THEN
+    ! Shadow from opposing reveal does not go beyond inside
+     !  surface of frame
+    IF(d12*TanAlpha < = L) THEN
+      A1sh = 0.5*TanAlpha*f1**2
+      L1   = f1*(f1*TanAlpha/(6*L)+0.5)
+      IF(d2-(d2prime+d2prime2+P2) > = 0.) THEN
+        A2sh = (d2prime+d2prime2)*L + &
+          0.5*TanAlpha*((d1+d2-d2prime)**2-d1+p2+d2prime2)**2)
+        L2   = d2prime2 + 0.5*(d2-(d2prime+d2prime2+P2))
+      ELSE  ! d2-(d2prime+d2prime2+P2) < 0.
+        ! Inside reveal is fully shadowed by frame and/or
+         !opposing reveal
+        A2sh = f2*L
+        L2   = f2
+      END IF
+    ELSE  ! d12*TanAlpha > = L
+      IF((d1+P2)*TanAlpha < = L) THEN
+        A1sh = 0.5*TanAlpha*f1**2
+        L1 = f1*((f1*TanAlpha)/(6*L) + 0.5)
+        IF((d1+P2+d2prime2)*TanAlpha > = L) THEN
+          A2sh = f2*L
+          L2   = f2
+        ELSE  ! (d1+P2+d2prime2)*TanAlpha < L
+          A2sh = f2*L - 0.5*(L-(d1+P2)*TanAlpha)**2/TanAlpha &
+             + d2prime2*(L-(d1+P2+d2prime2/2)*TanAlpha)
+          L2 = d2prime2 + (L/TanAlpha - (d1+P2+d2prime2))/3
+        END IF
+      ELSE  ! (d1+P2)*TanAlpha > L
+        L2 = f2
+        A2sh = f2*L
+        IF(f1*TanAlpha < = L) THEN
+          A1sh = 0.5*TanAlpha*f1**2
+          L1 = f1*((f1*TanAlpha)/(6*L) + 0.5)
+        ELSE  ! f1*TanAlpha > L
+          A1sh = f1*L - 0.5*L**2/TanAlpha
+          L1 = f1-(L/TanAlpha)/3
+        END IF
+      END IF
+    END IF
+  ELSE
+     ! d2prime > f2 -- Shadow from opposing reveal goes beyond
+     ! inside of frame
+    A2sh = f2*L
+    L2 = f2
+    IF(d2prime > = d1+d2) THEN
+      A1sh = 0.0
+      L1   = f1
+    ELSE  ! d2prime < d1+d2
+      IF(d2prime < = d2+P1) THEN
+        IF(f1*TanAlpha < = L) THEN
+          A1sh = 0.5*TanAlpha*f1**2
+          L1 = f1*((f1*TanAlpha)/(6*L) + 0.5)
+        ELSE  ! f1*TanAlpha > L
+          A1sh = f1*L - 0.5*L**2/TanAlpha
+              L1   = f1 - (L/TanAlpha)/3
+            END IF
+          ELSE  ! d2prime > d2+P1
+            IF(d12*TanAlpha < = L) THEN
+              A1sh = L*(d2prime-(d2+P1)) + 0.5*TanAlpha*d12**2
+              L1   = (L*(f1-d12/2)-d12*TanAlpha* &
+                 (f1/2-d12/3))/(L-d12*TanAlpha/2)
+            ELSE  ! d12*TanAlpha > L
+              A1sh = f1*L - 0.5*L**2/TanAlpha
+              L1   = f1 - (L/TanAlpha)/3
+            END IF
+          END IF
+        END IF
+      END IF
+      FracToGlassOuts = 0.5*(1.0 - ATAN(FrameWidth/L1)/PiOvr2)
+      FracToGlassIns  = 0.5*(1.0 - ATAN(FrameWidth/L2)/PiOvr2)
+    END IF  ! End of check if window has frame
+\end{lstlisting}
+
+The beam solar reflected from a sunlit region of area \(A\) is given by
+
+\begin{equation}
+R = {I_B}A\cos \beta (1 - a){\rm{ }}
+\end{equation}
+
+where
+
+\(R\) = reflected solar radiation {[}W{]}
+
+\({I_B}\) = beam normal irradiance {[}W/m\(^{2}\){]}
+
+\(A\) = sunlit area {[}m\(^{2}\){]}
+
+\(\beta\) = beam solar angle of incidence on reveal surface
+
+\(a\) = solar absorptance of reveal surface
+
+All reflected radiation is assumed to be isotropic diffuse. For outside reveal surfaces it is assumed that \(R/2\) ~goes toward the window and \(R/2\) ~goes to the exterior environment. Of the portion that goes toward the window a fraction \({F_1}\) ~goes toward the frame, if present, and \(1 - {F_1}\) ~goes toward the glazing.
+
+The view factor \({F_1}\) ~to the frame calculated by assuming that the illuminated area can be considered to be a line source. Then the area-weighted average distance, \({L_1}\) , of the source to the frame is calculated from the shape of the illuminated area (see above psuedo-code). Then \({F_1}\) ~is related as follows to the average angle subtended by the frame of width \({w_f}\) :
+
+\begin{equation}
+{F_1} = \frac{{{{\tan }^{ - 1}}({w_f}/{L_1})}}{{\pi /2}}
+\end{equation}
+
+For the portion going towards the frame, \((R/2){F_1}{a_f}\) is absorbed by the frame (where \({a_f}\) is the solar absorptance of the frame) and contributes to the frame heat conduction calculation. The rest, \((R/2){F_1}(1 - {a_f})\) , is assumed to be reflected to the exterior environment.
+
+If the glazing has diffuse transmittance \({\tau_{diff}}\) , diffuse front reflectance \(\rho_{diff}^f\) , and layer front absorptance \(\alpha_{l,diff}^f\) , then, of the portion, \((R/2)(1 - {F_1})\) , that goes toward the glazing, \((R/2)(1 - {F_1}){\tau_{diff}}\) is transmitted to the zone, \((R/2)(1 - {F_1})\alpha_{l,diff}^f\) is absorbed in glass layer \(l\) and contributes to the glazing heat balance calculation, and \((R/2)(1 - {F_1})\rho_{dif{f_{}}}^f\) is reflected to the exterior environment.
+
+The beam solar absorbed by an outside reveal surface is added to the other solar radiation absorbed by the outside of the window's parent wall.
+
+For inside reveal surfaces it is assumed that \(R/2\) ~goes towards the window and \(R/2\) ~goes into the zone. Of the portion that goes toward the window a fraction \((R/2){F_2}\) ~goes toward the frame, if present, and \((R/2)(1 - {F_2})\) goes toward the glazing (\({F_2}\) ~is calculated using a method analogous to that used for \({F_1}\) ). For the portion going towards the frame, \((R/2){F_2}{a_f}\) is absorbed by the frame and contributes to the frame heat conduction calculation. The rest, \((R/2){F_2}(1 - {a_f})\) , is assumed to be reflected back into the zone.
+
+If the glazing has diffuse back reflectance \(\rho_{diff}^b\) , and layer back absorptance \(\alpha_{l,diff}^b\) , then, of the portion \((R/2)(1 - {F_2})\) ~that goes toward the glazing, \((R/2)(1 - {F_2}){\tau_{diff}}\) is transmitted back out the glazing, \((R/2)(1 - {F_2})\alpha_{l,diff}^b\) is absorbed in glass layer \(l\) and contributes to the glazing heat balance calculation, and \((R/2)(1 - {F_2})\rho_{dif{f_{}}}^b\) is reflected into the zone.
+
+The beam solar absorbed by an inside reveal surface is added to the other solar radiation absorbed by the inside of the window's parent wall.
+
+\subsection{Shading Device Thermal Model}\label{shading-device-thermal-model}
+
+Shading devices in EnergyPlus can be on the exterior or interior sides of the window or between glass layers. The window shading device thermal model accounts for the thermal interactions between the shading layer (shade, screen or blind) and the adjacent glass, and between the shading layer and the room (for interior shading) or the shading layer and the outside surround (for exterior shading).
+
+An important feature of the shading device thermal model is calculating the natural convection airflow between the shading device and glass. This flow affects the temperature of the shading device and glazing and, for interior shading, is a determinant of the convective heat gain from the shading layer and glazing to the zone air. The airflow model is based on one described in the ISO Standard 15099, ``Thermal Performance of Windows, Doors and Shading Devices---Detailed Calculations'' {[}ISO15099, 2001{]}. (Between-glass forced airflow is also modeled; see ``Airflow Windows.'')
+
+The following effects are considered by the shading device thermal model:
+
+\begin{itemize}
+\item
+  For interior and exterior shading device: Long-wave radiation (IR) from the surround absorbed by shading device, or transmitted by the shading device and absorbed by the adjacent glass. For interior shading the surround consists of the other zone surfaces. For exterior shading the surround is the sky and ground plus exterior shadowing surfaces and exterior building surfaces ``seen'' by the window.
+\item
+  Inter-reflection of IR between the shading device and adjacent glass.
+\item
+  Direct and diffuse solar radiation absorbed by the shading device.
+\item
+  Inter-reflection of solar radiation between shading layer and glass layers.
+\item
+  Convection from shading layer and glass to the air in the gap (or, for between-glass shading, gaps) between the shading layer and adjacent glass, and convection from interior shading layer to zone air or from exterior shading layer to outside air.
+\item
+  Natural convection airflow in the gap (or, for between-glass shading, gaps) between shading layer and adjacent glass induced by buoyancy effects, and the effect of this flow on the shading-to-gap and glass-to-gap convection coefficients.
+\item
+  For interior shading, convective gain (or loss) to zone air from gap airflow.
+\end{itemize}
+
+In the following it is assumed that the shading device, when in place, covers the glazed part of the window (and dividers, if present) and is parallel to the glazing. For interior and exterior shading devices it is assumed that the shading layer is separated from the glazing by an air gap. A between-glass shading layer is assumed to be centered between two glass layers and separated from the adjacent glass layers by gaps that is filled with the same gas. If the window has a frame, it is assumed that the shading device does \emph{not} cover the frame.
+
+\subsection{Heat Balance Equations for Shading Device and Adjacent Glass}\label{heat-balance-equations-for-shading-device-and-adjacent-glass}
+
+If a window shading device is deployed the heat balance equations for the glass surfaces facing the shading layer are modified, and two new equations, one for each face of the shading layer, are added. Figure~\ref{fig:glazing-system-with-two-glass-layers-and-an} illustrates the case of double glazing with an interior shading device.
+
+\begin{figure}[hbtp] % fig 101
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1663.png}
+\caption{Glazing system with two glass layers and an interior shading layer showing variables used in heat balance equations. \protect \label{fig:glazing-system-with-two-glass-layers-and-an}}
+\end{figure}
+
+The heat balance equation for the glass surface facing the gap between glass and shading layer (called in the following, ``gap'') is
+
+\begin{equation}
+\frac{{{E_i}{\varepsilon_4}{\tau_{sh}}}}{{1 - {\rho_4}{\rho_{sh}}}} + \frac{{\sigma {\varepsilon_4}}}{{1 - {\rho_4}{\rho_{sh}}}}\left[ {\theta_5^4{\varepsilon_{sh}} - \theta_4^4(1 - {\rho_{sh}})} \right] + {k_2}\left( {{\theta_3} - {\theta_4}} \right) + {h_{cv}}\left( {{T_{gap}} - {\theta_4}} \right) + {S_4} = 0
+\end{equation}
+
+where
+
+\emph{$\tau$\(_{sh}\)} = IR diffuse transmittance of shading device
+
+\emph{$\varepsilon$\(_{sh}\)} = diffuse emissivity of shading device
+
+\emph{$\rho$\(_{sh}\)} = IR diffuse reflectance of shading device ( = 1 - ( \emph{$\tau$\(_{sh}\)} + \emph{$\varepsilon$\(_{sh}\)}))
+
+\emph{$\theta$\(_{5}\)} = temperature of the surface of the shading layer that faces the gap (K).
+
+The term 1 - \emph{$\rho$\(_{4}\)$\rho$\(_{sh}\)} accounts for the inter-reflection of IR radiation between glass and shading layer.
+
+The convective heat transfer from glass layer \#2 to the air in the gap is
+
+\begin{equation}
+{q_{c,gl}} = {h_{cv}}({\theta_4} - {T_{gap}})
+\end{equation}
+
+where
+
+\emph{T\(_{gap}\)} = effective mean temperature of the gap air (K).
+
+\emph{h\(_{cv}\)} = convective heat transfer coefficient from glass or shading layer to gap air (W/m\(^{2}\)K).
+
+The corresponding heat transfer from shading layer to gap air is
+
+\begin{equation}
+{q_{c,sh}} = {h_{cv}}({\theta_5} - {T_{gap}})
+\end{equation}
+
+The convective heat transfer coefficient is given by
+
+\begin{equation}
+{h_{cv}} = 2{h_c} + 4v
+\end{equation}
+
+where
+
+\emph{h\(_{c}\)} = surface-to-surface heat transfer coefficient for non-vented (closed) cavities (W/m\(^{2}\)K)
+
+\emph{v} = mean air velocity in the gap (m/s).
+
+The quantities \emph{h\(_{cv}\)} and \emph{T\(_{gap}\)} depend on the airflow velocity in the gap, which in turn depends on several factors, including height of shading layer, glass/shading layer separation (gap depth), zone air temperature for interior shading or outside air temperature for exterior shading, and shading layer and glass face temperatures. The calculation of \emph{h\(_{cv}\)} and \emph{T\(_{gap}\)} is described in the following sections.
+
+The heat balance equation for the shading layer surface facing the gap is
+
+\begin{equation}
+\frac{E_i \tau_{sh} \rho_4 \varepsilon_{sh}} {1 - \rho_4 \rho_{sh}} + 
+  \frac{\sigma \varepsilon_{sh}} {1 - \rho_4 \rho_{sh}} \left[
+    \varepsilon_4 \theta_4^4 - \theta_5^4 (
+      1 - \rho_4( 
+        \varepsilon_{sh} + \rho_{sh}
+      )
+    )
+  \right] + 
+  k_{sh} \left(
+    \theta_6 - \theta_5
+  \right) + 
+  h_{cv} \left(
+    T_{gap} - \theta_5
+  \right) + 
+  S_{sh,1} = 0
+\end{equation}
+
+where
+
+\emph{k\(_{sh}\)} = shading layer conductance (W/m\(^{2}\)K).
+
+\emph{$\theta$\(_{6}\)} = temperature of shading layer surface facing the zone air (K).
+
+\emph{S\(_{sh,l}\)} = solar radiation plus short-wave radiation from lights plus IR radiation from lights and zone equipment absorbed by the gap-side face of the shading layer (W/m\(^{2}\)K).
+
+The heat balance equation for the shading layer surface facing the zone air is
+
+\begin{equation}
+{E_i}{\varepsilon_{sh}} - {\varepsilon_{sh}}\sigma \theta_6^4 + {k_{sh}}\left( {{\theta_5} - {\theta_6}} \right) + {h_i}\left( {{T_i} - {\theta_6}} \right) + {S_{sh,2}} = 0
+\end{equation}
+
+where
+
+\emph{S\(_{sh,2}\)} = solar radiation plus short-wave radiation from lights plus IR radiation from lights and zone equipment absorbed by the zone-side face of the shading layer (W/m\(^{2}\)K).
+
+\subsection{Solving for Gap Airflow and Temperature}\label{solving-for-gap-airflow-and-temperature}
+
+For interior and exterior shading devices a pressure-balance equation is used to determine gap air velocity, gap air mean equivalent temperature and gap outlet air temperature given values of zone air temperature (or outside temperature for exterior shading), shading layer face temperatures and gap geometry. The pressure balance equates the buoyancy pressure acting on the gap air to the pressure losses associated with gap airflow between gap inlet and outlet {[}ISO15099, 2001{]}. The variables used in the following analysis of the interior shading case are shown in Figure~\ref{fig:vertical-section-a-and-perspective-view-b-of}.
+
+\begin{figure}[hbtp] % fig 102
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1670.png}
+\caption{Vertical section (a) and perspective view (b) of glass layer and interior shading layer showing variables used in the gap airflow analysis. The opening areas A\(_{bot}\), A\(_{top}\), A\(_{l}\), A\(_{r}\) and A\(_{h}\) are shown schematically. \protect \label{fig:vertical-section-a-and-perspective-view-b-of}}
+\end{figure}
+
+\subsubsection{Pressure Balance Equation}\label{pressure-balance-equation}
+
+The pressure balance equation for airflow through the gap is
+
+\begin{equation}
+\Delta {p_T} = \Delta {p_B} + \Delta {p_{HP}} + \Delta {p_Z}
+\end{equation}
+
+Here, \emph{Δp\(_{T}\)}is the driving pressure difference between room air and gap air. It is given by
+
+\begin{equation}
+\Delta {p_T} = {\rho_0}{T_0}gH\sin \phi \frac{{\left| {{T_{gap}} - {T_{gap,in}}} \right|}}{{{T_{gap}}{T_{gap,in}}}}
+\end{equation}
+
+where
+
+\emph{$\rho$\(_{0}\)} = density of air at temperature \emph{T\(_{0}\)} (kg/m\(^{3}\))
+
+\emph{T\(_{0}\)} = reference temperature (283K)
+
+\emph{g} = acceleration due to gravity (m/s\(^{2}\))
+
+\emph{H} = height of shading layer (m)
+
+\emph{$\phi$} = tilt angle of window (vertical = 90\(^{o}\))
+
+\emph{T\(_{gap}\)} = effective mean temperature of the gap air (K)
+
+\emph{T\(_{gap,in}\)} = gap inlet temperature ( = zone air temperature for interior shading) (K)
+
+The \emph{Δp\(_{B}\)} term is due to the acceleration of air to velocity \emph{v} (Bernoulli's law). It is given by
+
+\begin{equation}
+\Delta {p_B} = \frac{\rho }{2}{v^2}{\rm{    (Pa)}}
+\end{equation}
+
+where \emph{$\rho$}is the gap air density evaluated at \emph{T\(_{gap}\)} (kg/m\(^{3}\)).
+
+The \emph{Δp\(_{HP}\)} term represents the pressure drop due to friction with the shading layer and glass surfaces as the air moves through the gap. Assuming steady laminar flow, it is given by the Hagen-Poiseuille law for flow between parallel plates {[}Munson et al. 1998{]}:
+
+\begin{equation}
+\Delta {p_{HP}} = 12\mu \frac{H}{{{s^2}}}{v^{}}{\rm{    (Pa)}}
+\end{equation}
+
+where \emph{$\mu$} is the viscosity of air at temperature \emph{T\(_{gap}\)} (Pa-s).
+
+The \emph{Δp\(_{Z}\)} term is the sum of the pressure drops at the inlet and outlet openings:
+
+\begin{equation}
+\Delta {p_Z} = \frac{{\rho {v^2}}}{2}\left( {{Z_{in}} + {Z_{out}}} \right){\rm{    (Pa)}}
+\end{equation}
+
+Here, the inlet pressure drop factor, Z\(_{in}\), and the outlet pressure drop factor, Z\(_{out}\), are given by
+
+\begin{equation}
+  \begin{array}{rl}
+    Z_{in}  & = \left( \frac{A_{gap}}{0.66A_{eq,in}}  - 1 \right)^2 \\
+    Z_{out} & = \left( \frac{A_{gap}}{0.60A_{eq,out}} - 1 \right)^2
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    {Z_{in}}  &= {\left( {\frac{{{A_{gap}}}}{{0.66{A_{eq,in}}}} - 1} \right)^2} \\
+    {Z_{out}} &= {\left( {\frac{{{A_{gap}}}}{{0.60{A_{eq,out}}}} - 1} \right)^2}
+  \end{array}
+\end{equation}
+
+where
+
+\emph{A\(_{eq,in}\)} = equivalent inlet opening area (m\(^{2}\))
+
+\emph{A\(_{eq,out}\)} = equivalent outlet opening area (m\(^{2}\))
+
+\emph{A\(_{gap}\)} = cross-sectional area of the gap = \emph{sW}(m\(^{2}\))
+
+If T\(_{gap}\) \textgreater{} T\(_{gap,in}\)
+
+\begin{equation}
+  \begin{array}{rl}
+    A_{eq,in}  & = A_{bot} + \frac{A_{top}}{2(A_{bot}+A_{top}} \left( A_l + A_r + A_h \right) \\
+    A_{eq,out} & = A_{top} + \frac{A_{bot}}{2(A_{bot}+A_{top}} \left( A_l + A_r + A_h \right) 
+  \end{array}
+\end{equation}
+
+If T\(_{gap}\) ≤ T\(_{gap,in}\)
+
+\begin{equation}
+  \begin{array}{rl}
+    A_{eq,in}  & = A_{top} + \frac{A_{bot}}{2(A_{bot}+A_{top}} \left( A_l + A_r + A_h \right) \\
+    A_{eq,out} & = A_{bot} + \frac{A_{top}}{2(A_{bot}+A_{top}} \left( A_l + A_r + A_h \right) 
+  \end{array}
+\end{equation}
+
+Here, the area of the openings through which airflow occurs (see Figure~\ref{fig:vertical-section-a-and-perspective-view-b-of} and Figure~\ref{fig:examples-of-openings-for-an-interior-shading}) are defined as follows:
+
+A\(_{bot}\) = area of the bottom opening (m\(^{2}\))
+
+A\(_{top}\) = area of the top opening (m\(^{2}\))
+
+A\(_{l}\) = area of the left-side opening (m\(^{2}\))
+
+A\(_{r}\) = area of the right-side opening (m\(^{2}\))
+
+A\(_{h}\) = air permeability of the shading device expressed as the total area of openings (``holes'') in the shade surface (these openings are assumed to be uniformly distributed over the shade) (m\(^{2}\))
+
+Figure~\ref{fig:examples-of-openings-for-an-interior-shading} shows examples of A\(_{bot}\), A\(_{top}\), A\(_{l}\) and A\(_{r}\) for different shading device configurations.~ These areas range from zero to a maximum value equal to the associated shade/screen/blind-to-glass cross-sectional area; i.e., A\(_{bot}\) and A\(_{top}\) ≤ sW,~ A\(_{l}\) and A\(_{r}\) ≤ sH.
+
+\begin{figure}[hbtp] % fig 103
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1679.png}
+\caption{Examples of openings for an interior shading layer covering glass of height H and width W. Not to scale. (a) Horizontal section through shading layer with openings on the left and right sides (top view). (b) Vertical section through shading layer with openings at the top and bottom (side view). \protect \label{fig:examples-of-openings-for-an-interior-shading}}
+\end{figure}
+
+Expression for the Gap Air Velocity
+
+~Expressing Equation in terms of~ v~ yields the following quadratic equation:
+
+\begin{equation}
+\frac{{\rho {v^2}}}{2}\left( {1 + {Z_{in}} + {Z_{out}}} \right) + \frac{{12\mu H}}{{{s^2}}}v - {\rho_0}{T_0}gH\sin \phi \frac{{\left| {{T_{gap,in}} - {T_{gap}}} \right|}}{{{T_{gap,in}}{T_{gap}}}} = 0
+\end{equation}
+
+Solving this gives
+
+\begin{equation}
+v = \frac{{{{\left[ {{{\left( {\frac{{12\mu H}}{{{s^2}}}} \right)}^2} + \frac{{2{\rho ^2}(1 + {Z_{in}} + {Z_{out}}){\rho_0}{T_0}gH\sin \phi \left| {{T_{gap,in}} - {T_{gap}}} \right|}}{{{T_{gap,in}}{T_{gap}}}}} \right]}^{1/2}} - \frac{{12\mu H}}{{{s^2}}}}}{{\rho (1 + {Z_{in}} + {Z_{out}})}}
+\end{equation}
+
+The choice of the root of the quadratic equation is dictated by the requirement that \emph{v} = 0 if \emph{T\(_{gap,in}\)} = \emph{T\(_{gap}\)}.
+
+Gap Outlet Temperature and Equivalent Mean Air Temperature
+
+The temperature of air in the gap as a function of distance, \emph{h}, from the gap inlet (Figure~\ref{fig:variation-of-gap-air-temperature-with}) is
+
+\begin{equation}
+{T_{gap}}(h) = {T_{ave}} - ({T_{ave}} - {T_{gap,in}}){e^{ - h/{H_0}}}
+\end{equation}
+
+where
+
+\begin{equation}
+{T_{ave}} = \frac{{{T_{gl}} + {T_{sh}}}}{2}
+\end{equation}
+
+is the average temperature of the glass and shading layer surfaces facing the gap (K).
+
+\emph{H\(_{0}\)} = characteristic height (m), given by
+
+\begin{equation}
+{H_0} = \frac{{\rho {C_p}s}}{{2{h_{cv}}}}v
+\end{equation}
+
+where \emph{C\(_{p}\)} is the heat capacity of air.
+
+The gap outlet temperature is given by
+
+\begin{equation}
+{T_{gap,out}} = {T_{ave}} - ({T_{ave}} - {T_{gap,in}}){e^{ - H/{H_0}}}
+\end{equation}
+
+The thermal equivalent mean temperature of the gap air is
+
+\begin{equation}
+{T_{gap}} = \frac{1}{H}\int\limits_0^H {{T_{gap}}(h)dh = {T_{ave}} - \frac{{{H_0}}}{H}} \left( {{T_{gap,out}} - {T_{gap,in}}} \right)
+\end{equation}
+
+\begin{figure}[hbtp] % fig 104
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1687.png}
+\caption{Variation of gap air temperature with distance from the inlet for upward flow. \protect \label{fig:variation-of-gap-air-temperature-with}}
+\end{figure}
+
+Solution Sequence for Gap Air Velocity and Outlet Temperature
+
+The routine WinShadeGapFlow is called within the glazing heat balance iterative loop in SolveForWindowTemperatures to determine \emph{v} and \emph{T\(_{gap,out}\)}. The solution sequence in WinShadeGapFlow is as follows:
+
+At start of iteration, guess \emph{T\(_{gap}\)} as ((\emph{T\(_{gl}\)} + \emph{T\(_{sh}\)})/2 + \emph{T\(_{gap,in}\)})/2. Thereafter use value from previous iteration.
+
+Get still-air conductance, \emph{h\(_{c}\)}, by calling WindowGasConductance and NusseltNumber.
+
+Get \emph{v} from Equation
+
+Get \emph{h\(_{cv}\)} from Equation
+
+Get \emph{T\(_{ave}\)}from Equation
+
+Get \emph{T\(_{gap,out}\)} from Equation
+
+Get new value of \emph{T\(_{gap}\)}from Equation
+
+The values of \emph{h\(_{cv}\)} and \emph{T\(_{gap}\)} so determined are then used in the window heat balance equations to find new values of the face temperatures of the glass and shading layers. These temperatures are used in turn to get new values of \emph{h\(_{cv}\)} and \emph{T\(_{gap}\)} until the whole iterative process converges.
+
+Convective Heat Gain to Zone from Gap Airflow
+
+The heat added (or removed) from the air as it passes through the gap produces a convective gain (or loss) to the zone air given by
+
+\begin{equation}
+{q_v} = LW\left[ {{h_{cv}}\left( {{T_{gl}} - {T_{gap}}} \right) + {h_{cv}}\left( {{T_{sh}} - {T_{gap}}} \right)} \right] = 2{h_{cv}}LW\left( {{T_{ave}} - {T_{gap}}} \right){\rm{    (W)}}
+\end{equation}
+
+This can also be expressed as
+
+\begin{equation}
+{q_v} = \dot m{C_p}\left( {{T_{gap,out}} - {T_{gap,in}}} \right){\rm{    (W)}}
+\end{equation}
+
+where the air mass flow rate in the gap is given by
+
+\begin{equation}
+\dot m = \rho {A_{gap}}v{\rm{    (kg/s)}}
+\end{equation}
+
+\subsection{Heat Balance Equations for Between-Glass Shading Device}\label{heat-balance-equations-for-between-glass-shading-device}
+
+In EnergyPlus shading devices are allowed between the two glass panes of double glazing and between the two inner glass panes of triple glazing. Figure~\ref{fig:glazing-system-with-two-glass-layers-and-a} shows the case of a between-glass shading device in double glazing.
+
+\begin{figure}[hbtp] % fig 105
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1691.png}
+\caption{Glazing system with two glass layers and a between-glass shading device showing variables used in the heat balance equations. \protect \label{fig:glazing-system-with-two-glass-layers-and-a}}
+\end{figure}
+
+The heat balance equations for the two glass surfaces facing the shading device are the following.
+
+For face \#2:
+
+\begin{equation}
+h_{cv,1} (T_{gap,1}-\theta_2) + k_1 (\theta_1-\theta_2) +
+    \frac{\sigma \epsilon_2}{1-\rho_2 R_1} \left[
+      \frac{\tau_{sh}}{1-\rho_6\rho_3} (
+        \epsilon_3 \theta_3^4 + \epsilon_6\theta_6^4\rho_3
+      )
+      + \epsilon_5\theta_5^4 + \epsilon_2\theta_2^4R_1
+    \right]
+\end{equation}
+
+where
+
+\begin{equation}
+{R_1} = {\rho_5} + \frac{{\tau_{sh}^2{\rho_3}}}{{1 - {\rho_6}{\rho_3}}}
+\end{equation}
+
+\emph{T\(_{gap,1}\)} = effective mean air temperature in gap 1 (K)
+
+\emph{h\(_{cv,1}\)} = convective heat transfer coefficient from glass or shading layer to gas in gap 1 (W/m\(^{2}\)K)
+
+For face \#3:
+
+\begin{equation}
+h_{cv,2} (T_{gap,2}-\theta_3) + k_2 (\theta_4-\theta_3) +
+    \frac{\sigma \epsilon_3}{1-\rho_3 R_2} \left[
+      \frac{\tau_{sh}}{1-\rho_5\rho_2} (
+        \epsilon_3 \theta_2^4 + \epsilon_5\theta_5^4\rho_2
+      )
+      + \epsilon_6\theta_6^4 + \epsilon_7\theta_3^4R_2
+    \right]
+\end{equation}
+
+where
+
+\begin{equation}
+{R_2} = {\rho_6} + \frac{{\tau_{sh}^2{\rho_2}}}{{1 - {\rho_5}{\rho_2}}}
+\end{equation}
+
+\emph{T\(_{gap,2}\)} = effective mean air temperature in gap 2 (K)
+
+\emph{h\(_{cv,2}\)} = convective heat transfer coefficient from glass or shading layer to gas in gap 2 (W/m\(^{2}\)K)
+
+The heat balance equations for the shading layer faces are:
+
+For face \#5:
+
+\begin{equation}
+h_{cv,1} (T_{gap,1}-\theta_5) + k_sh (\theta_6-\theta_5) +
+    \frac{\sigma \epsilon_5}{1-\rho_2 R_1} \left[
+      \frac{\tau_{sh}\rho_2}{1-\rho_5\rho_3} (
+        \epsilon_3 \theta_3^4 + \epsilon_6\theta_6^4\rho_3
+      )
+      + \epsilon_2\theta_2^4 + \epsilon_5\theta_5^4\rho_2
+    \right]
+\end{equation}
+
+For face \#6:
+
+\begin{equation}
+h_{cv,2} (T_{gap,2}-\theta_3) + k_2 (\theta_4-\theta_3) +
+    \frac{\sigma \epsilon_3}{1-\rho_3 R_2} \left[
+      \frac{\tau_{sh}}{1-\rho_5\rho_2} (
+        \epsilon_2 \theta_2^4 + \epsilon_5\theta_5^4\rho_2
+      )
+      + \epsilon_2\theta_2^4 + \epsilon_7\theta_3^4R_2
+    \right]
+\end{equation}
+
+The convective heat transfer coefficients are given by
+
+\begin{equation}
+  \begin{array}{rl}
+    h_{cv,1} &= 2 h_{c,1} + 4v \\
+    h_{cv,2} &= 2 h_{c,2} + 4v
+  \end{array}
+\end{equation}
+
+where
+
+\emph{h\(_{cv,1}\),h\(_{cv,2}\)} = surface-to-surface heat transfer coefficients for gap \#1 and \#2,~ respectively,~ when these gaps are non-vented (closed).
+
+\emph{v} = air velocity in the gaps (m/s). It is assumed that the gap widths are equal, so that the velocity of flow in the gaps is equal and opposite, i.e., when the airflow is upward in gap \#1 it is downward in gap \#2 and vice-versa.
+
+In analogy to the interior or exterior shading device case, the air velocity is determined by solving the following pressure balance equation:
+
+\begin{equation}
+\Delta {p_{T,1,2}} = \Delta {p_{B,1}} + \Delta {p_{HP,1}} + \Delta {p_{Z,1}} + \Delta {p_{B,2}} + \Delta {p_{HP,2}} + \Delta {p_{Z,2}}
+\end{equation}
+
+where the driving pressure difference between gap \#1 and \#2 is
+
+\begin{equation}
+\Delta {p_{T,1,2}} = {\rho_0}{T_0}gH\sin \phi \frac{{\left| {{T_{gap,1}} - {T_{gap,2}}} \right|}}{{{T_{gap,1}}{T_{gap,2}}}}{\rm{      (Pa)}}
+\end{equation}
+
+The pressure drops on the right-hand side of this equation are:
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta p_{B,i} &= \frac{\rho_{gap,i}}{2} v^2 \\
+    \Delta p_{HP,i} &= 12 \mu_{gap,i} \frac{H}{s^2} \\
+    \Delta p_{Z,i} &= \frac{\rho_{gap,i} v^2}{2}\PB{Z_{in,i} + Z_{out,i}}
+  \end{array}
+\end{equation}
+
+where \emph{i} = gap number (1 or 2).
+
+It can be shown that \({Z_{in,1}} + {Z_{out,1}} = {Z_{in,2}} + {Z_{out,2}}\) . Then, inserting these pressure drop expressions into , we obtain the following expression for the airflow velocity:
+
+\begin{equation}
+v = \frac{{{{\left[ {{{\left( {\frac{{12({\mu_{gap,}}_1 + {\mu_{gap,}}_2)H}}{{{s^2}}}} \right)}^2} + 2\Delta {p_{T,1,2}}({\rho_{gap,1}} + {\rho_{gap,2}})(1 + {Z_{in}} + {Z_{out}})} \right]}^{1/2}} - \frac{{12({\mu_{gap,}}_1 + {\mu_{gap,}}_2)H}}{{{s^2}}}}}{{({\rho_{gap,}}_1 + {\rho_{gap,}}_2)(1 + {Z_{in}} + {Z_{out}})}}
+\end{equation}
+
+The choice of the sign of the square root term is dictated by the requirement that \(v = 0\) ~if \(\Delta {p_{T,1,2}} = 0\) , i.e., \({T_{gap,1}} = {T_{gap,2}}\) .
+
+Given \(v\) ~we can now calculate \({T_{gap,1}}\) and \({T_{gap,2}}\) , which gives \(\Delta {p_{T,1,2}}\) . The procedure is as follows. We have
+
+\begin{equation}
+{T_{gap,1,out}} = {T_{ave,1}} - ({T_{ave,1}} - {T_{gap,1,in}}){\xi_1}
+\end{equation}
+
+where \({T_{ave,1}} = ({\theta_2} + {\theta_5})/2\) ~and \({\xi_1} = {e^{ - \frac{H}{{{H_{0,1}}}}}}\) ~with \({H_{0,1}} = {\rho_{gap,1}}{C_p}sv/(2{h_{cv,1}})\) . Since \({T_{gap,1,in}} = {T_{gap,2,out}}\) ~this gives:
+
+~ \({T_{gap,1,out}} = {T_{ave,1}} - ({T_{ave,1}} - {T_{gap,2,out}}){\xi_1}\)
+
+Similarly,
+
+\begin{equation}
+{T_{gap,2,out}} = {T_{ave,2}} - ({T_{ave,2}} - {T_{gap,1,out}}){\xi_2}
+\end{equation}
+
+Solving these simultaneous equations gives:
+
+\begin{equation}
+  \begin{array}{rl}
+    T_{gap,1,out} &= \frac{T_{ave,1}\PB{1 - \xi_1} + \xi_1 T_{ave,2}\PB{1 - \xi_2}}{1 - \xi_1 \xi_2} \\
+    T_{gap,2,out} &= \frac{T_{ave,2}\PB{1 - \xi_2} + \xi_2 T_{ave,1}\PB{1 - \xi_1}}{1 - \xi_1 \xi_2}
+  \end{array}
+\end{equation}
+
+Using these in
+
+\begin{equation}
+{T_{gap,1}} = {T_{ave,1}} - \frac{{{H_{0,1}}}}{H}\left( {{T_{gap,1,out}} - {T_{gap,2,out}}} \right)
+\end{equation}
+
+gives
+
+~\({T_{gap,1}} = {T_{ave,1}} - \frac{{{H_{0,1}}}}{H}\xi \left( {{T_{ave,1}} - {T_{ave,2}}} \right)\)
+
+with
+
+\begin{equation}
+\xi  = \frac{{(1 - {\xi_1})(1 - {\xi_2})}}{{1 - {\xi_1}{\xi_2}}}
+\end{equation}
+
+Similarly, from
+
+\begin{equation}
+{T_{gap,2}} = {T_{ave,2}} - \frac{{{H_{0,2}}}}{H}\left( {{T_{gap,2,out}} - {T_{gap,1,out}}} \right)
+\end{equation}
+
+we get
+
+\begin{equation}
+{T_{gap,2}} = {T_{ave,2}} - \frac{{{H_{0,2}}}}{H}\xi \left( {{T_{ave,2}} - {T_{ave,1}}} \right)
+\end{equation}
+
+The overall solution sequence is as follows.
+
+At start of iteration guess \({T_{gap,1}} = {T_{ave,1}}\) ~and \({T_{gap,2}} = {T_{ave,2}}\) . Then
+
+1)~~~~Get \({\rho_{gap,1}},{\rho_{gap,2}},{\mu_{gap,1}},{\mu_{gap,2}}\) using \({T_{gap,1}},{T_{gap,2}}\) .
+
+2)~~~~Get still-air conductances \({h_{c,1}},{h_{c,2}}\) by calling WindowGasConductance and NusseltNumber.
+
+3)~~~~Get \(v\) ~from Equation
+
+4)~~~~Get \({h_{cv,1}},{h_{cv,2}}\) from Equation
+
+5)~~~~Get \({T_{ave,1}},{T_{ave,2}}\)
+
+6)~~~~Get \emph{H\(_{o,1}\)}, \emph{H\(_{o,2}\)}, \({\xi_1}\) and \({\xi_2}\) .
+
+7)~~~~Get \({T_{gap,1}}\) ,\({T_{gap,2}}\) from Equations and
+
+The values \({h_{cv,1}}{\rm{, }}{h_{cv,2}}{\rm{, }}{T_{gap,1}}\) ~and \({T_{gap,2}}\) are then used in the face heat balance equations to find new values of the face temperatures \({\theta_2}{\rm{, }}{\theta_3},{\rm{ }}{\theta_5}\) and \({\theta_6}\) . These are used in turn to get new values of \({h_{cv,1}}{\rm{, }}{h_{cv,2}}{\rm{, }}{T_{gap,1}}\) ~and \({T_{gap,2}}\) until the whole iterative process converges.
+
+\subsection{Airflow Windows}\label{airflow-windows}
+
+In airflow windows forced air flows in the gap between adjacent layers of glass. Such windows are also known as ``heat-extract windows'' and ``climate windows.''
+
+Five configurations of airflow windows are modeled (Figure~\ref{fig:gap-airflow-configurations-for-airflow}) that depend on the source and destination of forced air. The allowed combinations of Airflow Source and Airflow Destination are:
+
+InsideAir $\rightarrow$ OutsideAir
+
+InsideAir $\rightarrow$ InsideAir
+
+InsideAir $\rightarrow$ ReturnAir
+
+OutsideAir $\rightarrow$ InsideAir
+
+OutsideAir $\rightarrow$ OutsideAir
+
+\begin{figure}[hbtp] % fig 106
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1748.png}
+\caption{Gap airflow configurations for airflow windows. From “Active facades,� Version no. 1, Belgian Building Research Institute, June 2002. \protect \label{fig:gap-airflow-configurations-for-airflow}}
+\end{figure}
+
+A common application of airflow windows is to reduce the zone cooling load by exhausting indoor air through the window, thereby picking up and rejecting heat from the glazing (Figure~\ref{fig:gap-airflow-configurations-for-airflow}).
+
+Figure~\ref{fig:glazing-system-with-forced-airflow-between} shows the variables used in the heat balance equations for forced airflow in a double-glazed window.
+
+\begin{figure}[hbtp] % fig 107
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1749.png}
+\caption{Glazing system with forced airflow between two glass layers showing variables used in the heat balance equations. \protect \label{fig:glazing-system-with-forced-airflow-between}}
+\end{figure}
+
+The heat balance equation for the left-hand glass surface facing the gap in Figure~\ref{fig:glazing-system-with-forced-airflow-between} is:
+
+\begin{equation}
+{k_1}({\theta_1} - {\theta_2}) + {h_{cv}}({T_{gap}} - {\theta_2}) + \sigma \frac{{{\varepsilon_2}{\varepsilon_3}}}{{1 - (1 - {\varepsilon_2})(1 - {\varepsilon_3})}}\left( {\theta_3^4 - \theta_2^4} \right) + {S_2} = 0
+\end{equation}
+
+The corresponding equation for the right-hand glass surface facing the gap is:
+
+\begin{equation}
+{k_2}({\theta_4} - {\theta_3}) + {h_{cv}}({T_{gap}} - {\theta_3}) + \sigma \frac{{{\varepsilon_2}{\varepsilon_3}}}{{1 - (1 - {\varepsilon_2})(1 - {\varepsilon_3})}}\left( {\theta_2^4 - \theta_3^4} \right) + {S_3} = 0
+\end{equation}
+
+Here,
+
+\emph{T\(_{gap}\)} = effective mean temperature of the gap air (K)
+
+\emph{h\(_{cv}\)} = convective heat transfer coefficient from glass to gap air (W/m2K).
+
+The convective heat transfer coefficient is given by
+
+\begin{equation}
+{h_{cv}} = 2{h_c} + 4v
+\end{equation}
+
+where
+
+\emph{h\(_{c}\)} = glass-to-glass heat transfer coefficient for non-vented (closed) cavity (W/m\(^{2}\)K)
+
+\emph{v} = mean air velocity in the gap (m/s).
+
+The air velocity is determined by the gap cross-sectional area in the flow direction and the air flow rate, which is an input value that is constant or can vary according to a user-specified schedule:
+
+\begin{equation}
+v = \frac{F}{{{A_{gap}}}}{\rm{      (m/s)}}
+\end{equation}
+
+where
+
+\emph{F} = airflow rate (m\(^{3}\)/s)
+
+\emph{A\(_{gap}\)} = gap cross-sectional area in direction of flow (m2)
+
+It is assumed that the airflow is uniform across the width of the window.
+
+The mean temperature of the gap air is given by the following expression, whose derivation follows that for for the case of an interior shading device:
+
+\begin{equation}
+{T_{gap}} = {T_{ave}} - \frac{H}{{{H_0}}}({T_{gap,out}} - {T_{gap,in}})
+\end{equation}
+
+where
+
+\begin{equation}
+{T_{ave}} = \frac{{{\theta_2} + {\theta_3}}}{2}
+\end{equation}
+
+\emph{H} ~ = glazing height (m)
+
+\begin{equation}
+{H_0} = \frac{{\rho {C_p}s}}{{2{h_{cv}}}}v
+\end{equation}
+
+\emph{T\(_{gap,in}\)} = gap air inlet temperature (\emph{T\(_{i}\)} if the airflow source is indoor air, \emph{T\(_{o}\)} if the airflow source is outside air) (K)
+
+The outlet air temperature is given by
+
+\begin{equation}
+{T_{gap,out}} = {T_{ave}} - ({T_{ave}} - {T_{gap,in}}){e^{ - H/{H_0}}}
+\end{equation}
+
+The equations for glass face \#1 and \#4 are the same as those for no airflow in the gap (Equations and ).
+
+The convective heat gain to the zone air due to the gap airflow when the airflow destination is indoor air is
+
+\begin{equation}
+{q_v} = \dot m({C_{p,out}}{T_{gap,out}} - {C_{p,i}}{T_i}){\rm{      (W)}}
+\end{equation}
+
+where
+
+\emph{C\(_{p,i}\)} = heat capacity of the indoor air (J/kg-K)
+
+\emph{C\(_{p,out}\)} = heat capacity of the gap outlet air (J/kg-K)
+
+and where the air mass flow rate in the gap is
+
+\begin{equation}
+\dot m = \rho F{\rm{      (kg/s)}}
+\end{equation}
+
+\subsubsection{Fan Energy}\label{fan-energy}
+
+The fan energy used to move air through the gap is very small and is ignored.
+
+\subsubsection{Airflow Window with Between-Glass Shading Device}\label{airflow-window-with-between-glass-shading-device}
+
+Figure~\ref{fig:airflow-window-with-between-glass-shading} shows the case of a double-glazed airflow window with a between glass shading device. The heat balance equations in this case are the same as those for the between-glass shading device with natural convection (Figure~\ref{fig:glazing-system-with-two-glass-layers-and-a} and following equations) except that now
+
+\begin{equation}
+v = \frac{{F/2}}{{{A_{gap}}}}{\rm{      (m/s)}}
+\end{equation}
+
+where \emph{A\(_{gap}\)} = \emph{sW} is the cross-sectional area of the gap on either side of the shading device. It is assumed that the shading device is centered between the two panes of glass so that the airflow, \emph{F}, is divided equally between the two gaps.
+
+The convective heat gain to the zone air due to the airflow through the two gaps when the airflow destination is indoor air is
+
+\begin{equation}
+{q_v} = \dot m({C_{p,ave,out}}{T_{gap,ave,out}} - {C_{p,i}}{T_i}{\rm{)      (W)}}
+\end{equation}
+
+where the average temperature of the two outlet air streams is
+
+\begin{equation}
+{T_{gap,ave,out}}{\rm{ =  }}({T_{gap,1,out}} + {T_{gap,2,out}})/2
+\end{equation}
+
+and
+
+\emph{C\(_{p,ave,out}\)} = heat capacity of the outlet air evaluated at \emph{T\(_{gap,ave,out}\)} (J/kg-K)
+
+\begin{figure}[hbtp] % fig 108
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1763.png}
+\caption{Airflow window with between-glass shading device showing variables used in the heat balance equations. \protect \label{fig:airflow-window-with-between-glass-shading}}
+\end{figure}
+
+\subsection{Evacuated Glazing Unit (EGU)}\label{evacuated-glazing-unit-egu}
+
+Evacuated glazing Units (EGU) are an emerging technology, developed as a concept some 20-30 years ago, but only now approaching wide-spread commercialization and adoption.
+
+\subsubsection{Evacuated glazing unit (EGU): cavity thermal conductance}\label{evacuated-glazing-unit-egu-cavity-thermal-conductance}
+
+Thermal Conductance of the space in an evacuated glazing unit (EGU) is the sum of the conductance of the low pressure gas (air) and radiation conductance.
+
+\begin{equation}
+{C_{gas}} = {C_{COND}} + {C_{RAD}}
+\end{equation}
+
+\textbf{Conductance of the low-pressure gas}
+
+Conductance of low pressure gasses is calculated using formula by Corrucini (Corruccini, R. (1959)).
+
+\begin{equation}
+{C_{COND}} = \alpha  \cdot \left[ {\frac{{\gamma  + 1}}{{\gamma  - 1}}} \right] \cdot {\left[ {\frac{R}{{8 \cdot \pi  \cdot M \cdot T}}} \right]^{\frac{1}{2}}} \cdot P
+\end{equation}
+
+\begin{equation}
+B = \alpha  \cdot \left[ {\frac{{\gamma  + 1}}{{\gamma  - 1}}} \right] \cdot {\left[ {\frac{R}{{8 \cdot \pi  \cdot M \cdot T}}} \right]^{\frac{1}{2}}}
+\end{equation}
+
+\begin{equation}
+{C_{COND}} = B \cdot P
+\end{equation}
+
+Where:
+
+\begin{equation}
+\alpha  = \frac{{{\alpha_1}{\alpha_2}}}{{{\alpha_2} + {\alpha_1}\left( {1 - {\alpha_2}} \right)}}
+\end{equation}
+
+$\alpha$\(_{1}\), $\alpha$\(_{2}\) = Accommodation coefficients of the gas molecules with the two surfaces.~ These values depend on the temperature, surface conditions, etc.~ For the present configuration and conditions, it is expected that \emph{a} is approximately 0.5.~ If conservative value is needed than value of 1.0 could be used.~ With $\alpha$\(_{1}\), $\alpha$\(_{2}\) = 0.5, $\alpha$ = 0.333
+
+$\gamma$ = Specific heat ratio, $\gamma$\(_{air}\) = 1.40.
+
+\emph{R} = Universal gas constant, \emph{R} = 8,314.462175 J/mol·K
+
+\emph{M} = Molecular Weight, \emph{M}\(_{air}\) = 28.97 {[}mol/g{]}
+
+\emph{T} = (\emph{T}\(_{1}\) + \emph{T}\(_{2}\))/2 {[}K{]}
+
+\emph{P} = Pressure of the gas {[}N/m\(^{2}\){]}
+
+From the paper Collins and Robinson (Collins, R., \& Robinson, S. (1991)), B is set at approximately 50 for Air, if pressure is given in torr.~ Therefore according to Collins and Robinson, for air and approximate conditions of EGU:
+
+\begin{equation}
+  C_{COND} \approx 50 \cdot P
+\end{equation}
+
+Where P is in torr (i.e., mm Hg).
+
+\emph{Note: Conversion from Pa to torr is accomplished by multiplying value in torr by 133.28.}
+
+Using formula 2 and assuming \emph{T}\(_{1}\) to be 20 ºC and \emph{T}\(_{2}\) to be -18 ºC (expected temperatures of glass surfaces in EGU, if one glass surface is low-e and unit is exposed to NFRC standard environmental conditions), and using SI system of units, the B is calculated as 54.4, which is very close to the value of 50, proposed by Collins and Robinson
+
+\begin{equation}
+  C_{COND} \approx 54.4 \cdot P
+\end{equation}
+
+We will use exact value, calculated by the formula, so values of will be input into the calculations, which enables more flexible model that can account for special treatment of glass surfaces.
+
+\subsubsection{Radiation conductance}\label{radiation-conductance}
+
+Radiation conductance for the two parallel plates is given by:
+
+\begin{equation}
+{C_{RAD}} = \frac{1}{{{\varepsilon_1}^{ - 1} + {\varepsilon_2}^{ - 1} - 1}}\sigma \frac{{\left( {{T_1}^4 - {T_2}^4} \right)}}{{{T_1} - {T_2}}}
+\end{equation}
+
+Where:
+
+$\varepsilon$\(_{1}\) = emissivity of the first facing glass surface, {[} - {]}
+
+$\varepsilon$\(_{2}\) = emissivity of the second facing glass surface, {[} - {]}
+
+\(\sigma\) = Stefan-Boltzmann Constant, 5.67 x 10\(^{8}\), {[}W/(m\(^{2}\)·K\(^{4}\)){]}
+
+T\(_{1}\)~~ = Temperature of the first facing glass surface, {[}K{]}
+
+T\(_{2}\)~~ = Temperature of the second facing glass surface. {[}K{]}
+
+Assuming glass surface temperatures of 20 ºC and -18 ºC, respectively, the following radiation conductances are obtained for the three different glass emissivities:
+
+Clear Glass ($\varepsilon$\(_{1}\) = $\varepsilon$\(_{2}\) = 0.84): C\(_{RAD}\) = 3.4 W/m\(^{2}\)K
+
+Hard Coat Low-e ($\varepsilon$\(_{1}\) or $\varepsilon$\(_{2}\) = 0.15): C\(_{RAD}\) = 0.68 W/m\(^{2}\)K
+
+Soft Coat Low-e ($\varepsilon$\(_{1}\) or $\varepsilon$\(_{2}\) = 0.04): C\(_{RAD}\) = 0.19 W/m\(^{2}\)K
+
+\textbf{\emph{Note:}} \emph{C\(_{RAD}\) of 0.09 is theoretically possible using best low-e technology today (i.e.,} \emph{$\varepsilon$\(_{1}\) or} \emph{$\varepsilon$\(_{2}\) = 0.02).}
+
+\textbf{\emph{Note:}} \emph{Low-e values above are typical values, which will vary by manufacturer.~ Some more recent hard coat low-e values are at or below 0.1.}
+
+It should also be noted that values above are based on the fix set of temperatures, while in reality temperatures will depend on the environmental conditions and surface emissivities (e.g., it cannot be expected that clear glass will have same \emph{T\(_{1}\)} and \emph{T\(_{2}\)} as low-e glass).
+
+Equation is precise formulation for two parallel plates at the constant temperature.~ Simplified equation under these conditions is given in the form of:
+
+\begin{equation}
+{C_{RAD}} = 4\sigma \frac{1}{{{\varepsilon_1}^{ - 1} + {\varepsilon_2}^{ - 1} - 1}}{T_m}^3
+\end{equation}
+
+Where:
+
+\emph{T\(_{m}\)} = ~~~~~~~~~~ mean temperature, {[}K{]}
+
+\begin{equation}
+{T_m} = \frac{{\left( {{T_1} + {T_2}} \right)}}{2}
+\end{equation}
+
+Calculation of the U-factor
+
+\begin{equation}
+U = \frac{1}{{{R_{tot}}}} = \frac{1}{{{R_o} + 2 \cdot {R_{glass}} + {R_{gap}} + {R_i}}}
+\end{equation}
+
+\begin{equation}
+{R_{gap}} = \frac{1}{{{C_{gap}}}} = \frac{1}{{{C_{COND}} + {C_{RAD}}}}
+\end{equation}
+
+\begin{equation}
+{R_{glass}} = \frac{{{t_{glass}}}}{{{k_{glass}}}}
+\end{equation}
+
+Where:
+
+\emph{t}\(_{glass}\) = glass thickness; {[}m{]}
+
+\emph{k}\(_{glass}\) = glass conductivity; \emph{k}\(_{glass}\) = 1 W/(m·K)
+
+\emph{R}\(_{glass}\) = 0.003 m\(^{2}\)K/W (for 3 mm glass pane)
+
+\emph{R}\(_{o}\) ≈ 0.033 m\(^{2}\)K/W
+
+\emph{R}\(_{i}\) ≈ 0.14 m\(^{2}\)K/W
+
+U-factor of EGU without any pillars (pretending that this is possible) would be calculated using \emph{C}\(_{RAD}\) only.~ From above radiation conductance calculations:
+
+\emph{Clear Glass: ~~~~~~~~~~ U = 2.64 W/(m\(^{2}\)·K) {[}0.464 Btu/(hr·ft\(^{2}\)·ºF){]}}
+
+\emph{Hard Coat Low-e: ~~~ U = 0.62 W/(m\(^{2}\)·K) {[}0.109 Btu/(hr·ft\(^{2}\)·ºF){]}}
+
+\emph{Soft Coat Low-e:~~~~~ U = 0.19 W/(m\(^{2}\)·K) {[}0.034 Btu/(hr·ft\(^{2}\)·ºF){]}}
+
+Adding conductance of the air at 0.001 torr (\emph{C}\(_{COND}\) = 0.08 W/(m\(^{2}\)·K), these values become:
+
+\emph{Clear Glass: ~~~~~~~~~~ U = 2.66 W/(m\(^{2}\)·K) {[}0.468 Btu/(hr·ft\(^{2}\)·ºF){]}}
+
+\emph{Hard Coat Low-e: ~~~ U = 0.68 W/(m\(^{2}\)·K) {[}0.120 Btu/(hr·ft\(^{2}\)·ºF){]}}
+
+\emph{Soft Coat Low-e:~~~~~ U = 0.27 W/(m\(^{2}\)·K) {[}0.048 Btu/(hr·ft\(^{2}\)·ºF){]}}
+
+In contrast, the U-factor of the same configuration with the air at atmospheric pressure will be (For the space width of 50 mm, C\(_{COND}\) ≈ 450 W/m\(^{2}\)K):
+
+\emph{Clear Glass: ~~~~~~~~~~ U = 5.52 W/(m\(^{2}\)·K) {[}0.468 Btu/(hr·ft\(^{2}\)·ºF){]}}
+
+\emph{Hard Coat Low-e: ~~~ U = 5.52 W/(m\(^{2}\)·K) {[}0.120 Btu/(hr·ft\(^{2}\)·ºF){]}}
+
+\emph{Soft Coat Low-e:~~~~~ U = 5.52 W/(m\(^{2}\)·K) {[}0.048 Btu/(hr·ft\(^{2}\)·ºF){]}}
+
+It is clear that emissivity of the glass surface makes no difference, because of the dominant conductance of the air space.~ Also, it is worth noting that the U-factor of such configuration is very close to the U-factor of single glazing.
+
+\subsubsection{Evacuated glazing unit (EGU): Glass support element thermal conductance}\label{evacuated-glazing-unit-egu-glass-support-element-thermal-conductance}
+
+Glass panes in the EGU are separated by an array of small support elements.~ Typically, these support elements have a cylindrical shape and are often referred to as ``pillars.''~ Typical geometry of the pillar is 0.5-1.0 mm diameter and 0.05 mm (50 mm) height.~ They are typically spaced 1-2 in. apart in a form of square or staggered matrix.
+
+\subsubsection{Calculation of the U-factor}\label{calculation-of-the-u-factor}
+
+The conductance of these elements can be measured or numerically modeled to determine accurate thermal performance.~ Approximate method also exists and is based on the combination of modeling and analytical work for the conduction through small cylinders in contact with infinite parallel plates with thickness much larger than cylinder height.
+
+The following formula can be used to determine conductance of the single pillar, \emph{C}\(_{p}\) (Collins and Fisher-Cripps 1991):
+
+\begin{equation}
+{C_p} = \frac{{2ka}}{{1 + \frac{{2h}}{{\pi a}}}}
+\end{equation}
+
+Where:
+
+\emph{k}~~~ = conductivity of glass, W/(m·K)
+
+\emph{a}~~~ = radius of the pillar (m)
+
+\emph{h}~~~ = pillar height, m
+
+For the square array of support pillars (Collins and Fischer-Cripps 1991) proposes the following formula for their conductance, \emph{C}\(_{pa}\):
+
+\begin{equation}
+{C_{pa}} = \frac{{2ka}}{{{\lambda ^2}\left( {1 + \frac{{2h}}{{\pi a}}} \right)}}
+\end{equation}
+
+Where:
+
+$\lambda$ = pillar spacing, m
+
+This formula is approximate and does not include effect of the conductivity of the pillar, but it gives good approximation for common materials used in this technology, since conductivity of the pillar does not play substantial role for non-insulating pillars (where ``non-insulating'' would mean that conductivity of the pillar is equal or higher than the conductivity of the glass pane.
+
+The U-factor of the EGU with support pillars is then:
+
+\begin{equation}
+U = \frac{1}{{{R_{tot}}}} = \frac{1}{{{R_o} + 2 \cdot {R_{glass}} + {R_{gap}} + {R_i}}}
+\end{equation}
+
+Where:
+
+\begin{equation}
+{R_{gap}} = \frac{1}{{{C_{gap}}}} = \frac{1}{{{C_{COND}} + {C_{RAD}} + {C_{pa}}}}
+\end{equation}
+
+\subsubsection{References}\label{references-055}
+
+Collins, R., \& Fischer-Cripps, A. 1991. ``Design of Support Pillar Arrays in Flat Evacuated Windows.''. Aust. J. Phys.
+
+Collins, R., \& Robinson, S. 1991. \emph{``Evacuated Glazing''.} Solar Energy. Vol. 47, No. 1, pp.~27-38.
+
+Corruccini, R. 1959. ``Gaseous Heat Conduction at Low Pressures and Temperatures''. Vacuum. Vol. 7-8, pp.19-29.
+
+\subsection{Thermal Performance of Deflected Insulated Glazing Unit (IGU)}\label{thermal-performance-of-deflected-insulated-glazing-unit-igu}
+
+\subsubsection{Introduction}\label{introduction-002}
+
+Deflection of insulated glazing unit (IGU) can result in thermal performance degradation or improvement due to the reduction or increase of gap space width. Convection of the gas fill is affected by changed gap space and due to modified convection pattern and shorter or longer thermal path at the center of the glazing unit can result in increased or decreased thermal performance. For the most part, U-factor is mostly affected as a direct result of changed thermal performance; however note that solar heat gain through the window (SHGC) can also be affected because of the effect of inward flowing fraction of absorbed solar radiation, which is affected by thermal performance of the IGU.
+
+Deflection in sealed IGU is caused by the difference in gas pressure in IGU gap vs.~outdoor/indoor pressure. Indoor and outdoor pressure can be considered equal, since indoor building environment is in pretty good contact with outdoor environment. We will call this pressure an atmospheric pressure, \emph{P\(_{a}\)}. The differences in pressure between atmospheric and gap pressure is due to several factors, listed here:
+
+1)~~~Difference in atmospheric pressure between IGU fabrication location and end use location
+
+2)~~~Difference in temperature during fabrication and actual operating conditions for the glazing. It should be noted that initial temperature can be higher than ambient temperature during fabrication process, due to elevated sealant temperatures, which can raise local temperatures within the IGU.
+
+3)~~~Unbalanced gas fill leakage through the sealants, resulting in lower gap pressure and inward deflection.
+
+4)~~~Wind or static load pressure
+
+Effects 1 and 2 will be modeled using equations presented below, while effect 3 does not have credible mathematical model. However, cumulative deflection, resulting from all three effects can be measured in the field and its effect on thermal performance can be modeled by specifying center glazing deflection.
+
+Wind or static load pressure effects on deflection is not included in this model at this time, but will be considered for future versions.
+
+Recognizing that indoor and outdoor air pressure could be different, such as in hot box test environment, future plans for the extension of the model will include option to specify different values for indoor and outdoor pressure. Another future improvement to the model will also include linking certain air gaps with indoor or outdoor environment, meaning that respective pressures in linked spaces will be set to equal.
+
+\subsubsection{Mathematical Model}\label{mathematical-model-000}
+
+Mathematical model described in detail here is based on the research work by Bernier and Bourret (1997) and Timoshenko and Woinowsky-Krieger (1959). Bernier and Bourret (1997) of the Ecole Polytechnique Montréal adopted Timoshenko and Woinowsky-Krieger (1959) model for calculating flat plate deflection subjected to the differential pressure field (static), while their original contribution was to develop correlations for changes in thermal performance, based on IGU deflection at the center of glazing location. In addition to adopting Bernier and Bourret (1997) model here, we have also developed model for calculating change in thermal performance of deflected units when this deflection is measured in the field. Therefore, the mathematical formulation, presented here is divided into two sections; 1) calculation of the deflection and resulting thermal performance caused by pressure and temperature effects and 2) calculation of the thermal performance of the IGU when the deflection is measured.
+
+\subsubsection{Calculation of the deflection and thermal performance caused by pressure and temperature effects}\label{calculation-of-the-deflection-and-thermal-performance-caused-by-pressure-and-temperature-effects}
+
+If coordinate system is set as shown in Figure~\ref{fig:deflection-coordinate-system-2d} and Figure~\ref{fig:deflection-coordinate-system-3d}, it is possible to calculate deflection distribution at each point of pane by using following equation:
+
+\begin{figure}[hbtp] % fig 109
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1779.png}
+\caption{Deflection Coordinate System - 2D \protect \label{fig:deflection-coordinate-system-2d}}
+\end{figure}
+
+\begin{equation}
+{L_{D\left( i \right)}}\left( {x,y} \right) = \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{{\sin \frac{{m\pi x}}{W}\sin \frac{{n\pi y}}{H}}}{{mn{{\left( {{{\left( {\frac{m}{W}} \right)}^2} + {{\left( {\frac{n}{H}} \right)}^2}} \right)}^2}}}
+\end{equation}
+
+Where,
+
+\begin{equation}
+{D_{\left( i \right)}} = \frac{{E\cdot t_{\left( i \right)}^3}}{{12\cdot \left( {1 - {\nu ^2}} \right)}}
+\end{equation}
+
+Where,
+
+\emph{E} = Young's modulus (7.2 x 10\(^{10}\)) {[}Force per unit Area; SI: Pa, IP: psi{]}
+
+\emph{t} = thickness of glazing pane {[}Length; SI: m, IP: in.{]}
+
+$\nu$ = poison's ratio (0.22 for glass) {[}Non-Dimensional{]}
+
+\begin{figure}[hbtp] % fig 110
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1782.png}
+\caption{Deflection Coordinate System - 3D \protect \label{fig:deflection-coordinate-system-3d}}
+\end{figure}
+
+Δ\emph{P\(_{i}\)} = \emph{P\(_{gap(i)}\)} - \emph{P\(_{gap(i-1)}\)} (for i-th pane) {[}Force per unit Area; SI: Pa, IP: psi{]}
+
+Δ\emph{P\(_{i}\)} = \emph{P\(_{gap(1)}\)} - \emph{P\(_{a}\)} (first pane) {[}Force per unit Area; SI: Pa, IP: psi{]}\emph{~~~~~~~~~~~~~~~~~~}
+
+Δ\emph{P\(_{i}\)} = \emph{P\(_{a}\) - P\(_{gap(n-1)}\)} (last pane) {[}Force per unit Area; SI: Pa, IP: psi{]}
+
+Where,
+
+\emph{P\(_{a}\) =} atmospheric pressure. {[}Force per unit Area; SI: Pa, IP: psi{]}
+
+\begin{equation}
+{P_{gap\left( i \right)}} = \frac{{{P_{ini}}{V_{ini\left( i \right)}}{T_{gap\left( i \right)}}}}{{{T_{ini}}{V_{gap\left( i \right)}}}}
+\end{equation}
+
+Where,
+
+\emph{P\(_{ini}\)} = Initial pressure. Applies to all gaps as a single value (input data - measured or otherwise) {[}Force per unit Area; SI: Pa, IP: psi{]}
+
+\emph{T\(_{ini}\)} = Initial temperature. Applies to all gaps as a single value (input data - measured or otherwise) {[}Degree Temperature; SI: K, IP: R{]}
+
+\emph{V\(_{ini(i)}\)} = Initial volume for i-th gap. {[}Length*Length*Length; SI: m\(^{3}\), IP: in\(^{3}\){]}
+
+\begin{equation}
+{V_{ini\left( i \right)}} = {L_i}\cdot W\cdot H
+\end{equation}
+
+Where,
+
+\emph{L\(_{i}\)} = non-deflected glazing gap width (for i-th gap) {[}Length; SI: m, IP: in.{]}
+
+\emph{W} = IGU width {[}Length; SI: m, IP: in.{]}
+
+\emph{H} = IGU height {[}Length; SI: m, IP: in.{]}
+
+\emph{T\(_{gap(i)}\)} = temperature of the gap between two glass panes (calculated using center of glazing thermal calculation algorithm, as described in ISO 15099 (ISO 2003). This value is first calculated using non-deflected state and is recalculated after the resulting deflection is calculated. This process is repeated until temperature at next iteration does not differ by more than 0.1 ºC
+
+\emph{V\(_{gap(i)}\)} = volume of the IGU gap in deflected state {[}Lentgh*Length*Length; SI: m\(^{3}\), IP: in\(^{3}\){]}
+
+\begin{equation}
+{V_{gap\left( i \right)}} = {V_{ini\left( i \right)}} + W\cdot H\cdot \left( {\overline {{L_{D,i}}}  - \overline {{L_{D,i + 1}}} } \right)
+\end{equation}
+
+Where,
+
+\(\overline {{L_{D,i}}}\) ~is mean deflection value for i-th pane. {[}Length; SI: m, IP: in.{]}
+
+Deflection of each pane can be positive or negative and is done solely to establish reference. Current frame of reference is that positive deflection means that pane is deflecting towards left side, while negative deflection means that pane is deflecting towards right side . Whether the deflection is in the direction of reducing the gap width or increasing it, it will be the result of pressure difference, as described in . When pressure in the glazing unit is higher than surrounding environmental pressure, the deflection will be towards increasing gap width (i.e., ballooning), while the opposite situation will result in decreasing gap width (i.e., vacuuming)
+
+\begin{figure}[hbtp] % fig 111
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1787.png}
+\caption{Deflection Direction Convention \protect \label{fig:deflection-direction-convention}}
+\end{figure}
+
+The important part of calculating deflection of the IGU is to determine mean deflection value for each glazing pane. Mean deflection value is used to calculate gap volume in deflected state . Mean deflection of glazing pane can be calculated by integrating :
+
+\begin{equation}
+\overline {{L_{D\left( i \right)}}}  = \mathop \smallint \limits_{x = 0}^W \mathop \smallint \limits_{y = 0}^H \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{{\sin \frac{{m\pi x}}{W}\sin \frac{{n\pi y}}{H}}}{{mn{{\left( {{{\left( {\frac{m}{W}} \right)}^2} + {{\left( {\frac{n}{H}} \right)}^2}} \right)}^2}}}
+\end{equation}
+
+Which is identical with the following expression:
+
+\begin{equation}
+\overline {{L_{D\left( i \right)}}}  = \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{{\mathop \smallint \nolimits_{x = 0}^W \mathop \smallint \nolimits_{y = 0}^H \sin \frac{{m\pi x}}{W}\sin \frac{{n\pi y}}{H}}}{{mn{{\left( {{{\left( {\frac{m}{W}} \right)}^2} + {{\left( {\frac{n}{H}} \right)}^2}} \right)}^2}}}
+\end{equation}
+
+and because integral of sin(x) is equal with --cos(x), above equation will become:
+
+\begin{equation}
+\overline {{L_{D\left( i \right)}}}  = \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{{\left( {1 - cos\left( {m\pi } \right)} \right)\left( {1 - cos\left( {n\pi } \right)} \right)}}{{mn{{\left( {{{\left( {\frac{m}{W}} \right)}^2} + {{\left( {\frac{n}{H}} \right)}^2}} \right)}^2}}}
+\end{equation}
+
+Finally, because \(cos\left( {m\pi } \right)\) ~and \(cos\left( {n\pi } \right)\) ~values are always equal to -1 for the given range of m and n, above equation will became:
+
+\begin{equation}
+\overline {{L_{D\left( i \right)}}}  = \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{4}{{{m^2}{n^2}{\pi ^2}{{\left( {{{\left( {\frac{m}{W}} \right)}^2} + {{\left( {\frac{n}{H}} \right)}^2}} \right)}^2}}}
+\end{equation}
+
+After calculating mean pane deflection the following equation is used to calculate mean gap width:
+
+\begin{equation}
+{L_{r\left( i \right)}} = L + \left( {\overline {{L_{D,\left( i \right)}}}  - \overline {{L_{D,\left( {i + 1} \right)}}} } \right)
+\end{equation}
+
+\emph{Where,}
+
+\emph{L\(_{r(i)}\) = Mean gap ``i'' width after incorporating glazing deflection. This mean gap width is used to recalculate thermal performance of deflected IGU.}
+
+\(\overline {{L_{D,i}}}\) \textbf{\emph{~}}* = mean glazing deflection for each pane ``i''.*
+
+Calculation of the deflection at the center of glazing and mean glazing deflection for each pane is an iterative process, where the initial temperature distribution is calculated for non-deflected state, then deflection is calculated based on this temperature distribution, new temperature distribution is calculated for this deflected state, then temperatures from previous iteration are compared to the current iteration and the process is repeated until the difference is no larger than 0.1 ºC.
+
+At the end of calculations, program will calculate and return maximum deflection value for each pane (i.e., center of glazing deflection). If we label maximum deflection of each pane as \emph{L\(_{D(i),max}\)}, we can calculate this value by substituting \emph{x} = \emph{W}/2 and \emph{y} = \emph{H}/2 in equation to determine deflection at the center point. Therefore,
+
+\begin{equation}
+{L_{D\left( i \right),max}} = \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{{\sin \frac{{m\pi }}{2}\sin \frac{{n\pi }}{2}}}{{mn{{\left( {{{\left( {\frac{m}{2}} \right)}^2} + {{\left( {\frac{n}{2}} \right)}^2}} \right)}^2}}}
+\end{equation}
+
+For glazing systems with more than two glazing layers, meaning multiple gas filled gaps, the deflection will be calculated for each glazing pane assuming that the pressure in a gap is independent from each other and calculated separately, unless spaces are ``linked'' together (e.g., stretched film middle glazing that has hole for equalizing pressure).
+
+\subsubsection{Non-Linked Gaps in 3 or more glazing layer system:}\label{non-linked-gaps-in-3-or-more-glazing-layer-system}
+
+The procedure shown above generally applies to the 3 or more layer glazing system, with the exception that neighboring pressures are no longer \emph{P\(_{a}\)}, but rather could be \emph{P\(_{a}\)} on one side and \emph{P\(_{gap}\)} on the other, or have \emph{P\(_{gap}\)} on both sides, as shown in Figure~\ref{fig:deflection-direction-convention} for gap ``\emph{i}''. Center of glazing thermal calculation will determine new temperature distribution, after deflection is calculated for each glazing and will be used to determine new \emph{P\(_{gap}\)}, as per the procedure above.
+
+\subsubsection{Linked Gaps in 3 or more glazing layer system:}\label{linked-gaps-in-3-or-more-glazing-layer-system}
+
+When one or more gaps are linked together, their pressure is assumed to be identical (e.g., in triple glazing IGU \emph{P\(_{gap,1}\)} = \emph{P\(_{gap,2}\)}.)~ This pressure is calculated from temperatures of bounding glazing for linked gaps (e.g., for triple glazing IGU, glazing 1 and 3) and using neighboring pressures outside of those bounding glazing (e.g., for triple glazed IGU, \emph{P\(_{a}\)} on both sides).
+
+\emph{Note: This feature is not implemented in WINDOW 7.1. It is considered for future enhancements to the program.}
+
+\subsubsection{Gap(s) Linked to Indoor or Outdoor Environment:}\label{gaps-linked-to-indoor-or-outdoor-environment}
+
+If one or more glazing gaps are linked to either indoor or outdoor environment its pressure is fixed to \emph{P\(_{a}\)}. In combination situations, such as two or more gaps linked together with one of them being linked to indoor or outdoor environment, they will all have fixed pressure of \emph{P\(_{a}\)}.
+
+\subsubsection{Calculation of the thermal performance caused by measured deflection}\label{calculation-of-the-thermal-performance-caused-by-measured-deflection}
+
+When deflection is measured, it is normally measured at the point of maximum deflection. Maximum deflection occurs at center of the IGU (at \emph{W}/2 and \emph{H}/2).
+
+Measured value is typically gap width at the point of maximum deflection, which we can label \emph{L\(_{G(i)}\)}. For i-th measured gap the width is equal to:
+
+\begin{equation}
+{L_{G\left( i \right)}} = {L_{\left( i \right)}} + \left( {{L_{D\left( i \right),max}} - {L_{D\left( {i + 1} \right),max}}} \right)
+\end{equation}
+
+\begin{figure}[hbtp] % fig 112
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1798.png}
+\caption{Sketch of the non-symetrically Deflected Glazing Panes \protect \label{fig:sketch-of-the-non-symetrically-deflected}}
+\end{figure}
+
+If we label ratio of mean deflection and maximum deflection as R\(_{(i)}\), then:
+
+\begin{equation}
+{R_{(i)}} = \frac{{\overline {{L_{D(i)}}} }}{{{L_{D(i)}}_{,\max }}} = \sum\limits_{m = 1,3,5,...}^\infty  {\sum\limits_{n = 1,3,5,...}^\infty  {\frac{4}{{{m^2}{n^2}{\pi ^2}{{\left( {{{(\frac{m}{W})}^2} + {{(\frac{n}{H})}^2}} \right)}^2}}}} }
+\end{equation}
+
+Important thing to note is that ratios $\PB{R_{\PB{i}}}$\ for all gaps in glazing system are equal.
+
+\begin{equation}
+{R_{\left( 1 \right)}} = {R_{\left( 2 \right)}} =  \ldots  = {R_{\left( i \right)}} =  \ldots  = {R_{\left( {n - 1} \right)}} = R
+\end{equation}
+
+Replacing and into the following equation is obtained:
+
+\begin{equation}
+{L_{r\left( i \right)}} = {L_{\left( i \right)}} + R\left( {{L_{D\left( i \right),max}} - {L_{D\left( {i + 1} \right),max}}} \right)
+\end{equation}
+
+Combining with we get the following expression for the mean gap width:
+
+\begin{equation}
+{L_{r\left( i \right)}} = {L_{\left( i \right)}} + R\left( {{L_{G\left( i \right)}} - {L_{\left( i \right)}}} \right)
+\end{equation}
+
+Number of equations given in expression is equal to n-1, where n is number of panes. Therefore, we need one more equation to complete the system of equations that would allow us to solve for all independent variables. To get the last equation we can rewrite in slightly different manner:
+
+\begin{equation}
+{L_{D\left( i \right),max}} = \frac{{\Delta {P_{\left( i \right)}}}}{{{D_{\left( i \right)}}}}\cdot K
+\end{equation}
+
+Where coefficient K combines all constant terms, while \({D_{\left( i \right)}}\) ~is given by and \(\Delta {P_{\left( i \right)}}\) ~is calculated by, and . Summing over all deflections, \({L_{D\left( i \right),max}}\) ~the following equation is obtained:
+
+\begin{equation}
+\mathop \sum \limits_{i = 1}^n \frac{{{D_{\left( i \right)}}}}{K}\cdot {L_{D\left( i \right),max}} = \mathop \sum \limits_{i = 1}^n \Delta {P_{\left( i \right)}} = 0
+\end{equation}
+
+Note that sum of all \(\Delta {P_{\left( i \right)}}\) ~is equal to zero since outside pressure is equal to inside. Therefore, the remaining equation that completes the set of equations is:
+
+\begin{equation}
+\mathop \sum \limits_{i = 1}^n {D_{\left( i \right)}}\cdot {L_{D\left( i \right),max}} = 0
+\end{equation}
+
+\subsubsection{Solving system of equations}\label{solving-system-of-equations}
+
+In order to solve system of equations we will present in slightly different manner:
+
+\begin{equation}
+0 = {L_{\left( i \right)}} - {L_{G\left( i \right)}} + {L_{D\left( i \right),max}} - {L_{D\left( {i + 1} \right),max}}
+\end{equation}
+
+Which in developed form will look like this:
+
+\begin{equation}
+0 = {L_{\left( 1 \right)}} - {L_{G\left( 1 \right)}} + {L_{D\left( 1 \right),max}} - {L_{D\left( 2 \right),max}}
+\end{equation}
+
+\begin{equation}
+0 = {L_{\left( 2 \right)}} - {L_{G\left( 2 \right)}} + {L_{D\left( 2 \right),max}} - {L_{D\left( 3 \right),max}}
+\end{equation}
+
+\begin{equation}
+0 = {L_{\left( i \right)}} - {L_{G\left( i \right)}} + {L_{D\left( i \right),max}} - {L_{D\left( {i + 1} \right),max}}
+\end{equation}
+
+\begin{equation}
+0 = {L_{\left( {n - 1} \right)}} - {L_{G\left( {n - 1} \right)}} + {L_{D\left( {n - 1} \right),max}} - {L_{D\left( n \right),max}}
+\end{equation}
+
+In order to express each \({L_{D\left( i \right),max}}\) ~as dependence from \({L_{D\left( n \right),max}}\) ~(deflection of inside/last pane) we will need to make sum from first to last, then from second to last, third to last and so on. This procedure will create following set of equations:
+
+\begin{equation}
+{L_{D\left( 1 \right),max}} = \mathop \sum \limits_{k = 1}^{k = n - 1} \left( {{L_{G\left( k \right)}} - {L_{\left( k \right)}}} \right) + {L_{D\left( n \right),max}}
+\end{equation}
+
+\begin{equation}
+{L_{D\left( 2 \right),max}} = \mathop \sum \limits_{k = 2}^{k = n - 1} \left( {{L_{G\left( k \right)}} - {L_{\left( k \right)}}} \right) + {L_{D\left( n \right),max}}
+\end{equation}
+
+\begin{equation}
+{L_{D\left( i \right),max}} = \mathop \sum \limits_{k = i}^{k = n - 1} \left( {{L_{G\left( k \right)}} - {L_{\left( k \right)}}} \right) + {L_{D\left( n \right),max}}
+\end{equation}
+
+\begin{equation}
+{L_{D\left( {n - 1} \right),max}} = \mathop \sum \limits_{k = n - 1}^{k = n - 1} \left( {{L_{G\left( k \right)}} - {L_{\left( k \right)}}} \right) + {L_{D\left( n \right),max}}
+\end{equation}
+
+Now replacing this set of equations back to :
+
+\begin{equation}
+\mathop \sum \limits_{i = 1}^{n - 1} {D_{\left( i \right)}}\cdot \left( {\mathop \sum \limits_{k = i}^{k = n - 1} \left( {{L_{G\left( k \right)}} - {L_{\left( k \right)}}} \right) + {L_{D\left( n \right),max}}} \right) + {D_{\left( n \right)}}\cdot {L_{D\left( n \right),max}} = 0
+\end{equation}
+
+Which solving by \({L_{D\left( n \right),max}}\) ~leads to the following equation:
+
+\begin{equation}
+{L_{D\left( n \right),max}} = \frac{{\mathop \sum \nolimits_{i = 1}^{n - 1} ({D_{\left( i \right)}}\cdot \mathop \sum \nolimits_{k = i}^{k = n - 1} \left( {{L_{\left( k \right)}} - {L_{G\left( k \right)}}} \right))}}{{\mathop \sum \nolimits_{i = 1}^n {D_{\left( i \right)}}}}
+\end{equation}
+
+Calculating \({L_{D\left( n \right),max}}\) ~value from this equation and substituting it in will enable calculation of the deflection of remaining panes.
+
+\subsubsection{References}\label{references-1-019}
+
+Arasteh, D.K., J.C. Kohler and B.T. Griffith. Draft 2009. Modeling Windows in EnergyPlus with only U, SHGC, and optionally VT. LBNL report.~ Full reference to be determined.
+
+Arasteh, D. J. 2009. Modeling Windows in EnergyPlus with only U, SHGC, and optionally VT. Lawrence Berkeley National Laboratory.
+
+Arasteh, D.K., M.S. Reilly and M.D.~Rubin. 1989. A versatile procedure for calculating heat transfer through windows. American Society of Heating, Refrigeration and Air-Conditioning Engineers, ASHRAE Transactions, Vol. 95, Pt. 2.
+
+Bernier, M., \& Bourret, B. January 1997. ``Effects of Glass Plate Curvature on the U-Factor of Sealed Insulated Glazing Units''. Atlanta, GA: ASHRAE Transactions. Vol. 103, Pt. 1. American Society for Heating, Refrigerating and Air-Conditioning Engineers.
+
+Collins, R., \& Fischer-Cripps, A. 1991. ``Design of Support Pillar Arrays in Flat Evacuated Windows.''. Aust. J. Phys.
+
+Collins, R., \& Robinson, S. 1991. ``Evacuated Glazing''. Solar Energy. Vol. 47, No. 1, pp.~27-38.
+
+Corruccini, R. (1959). ``Gaseous Heat Conduction at Low Pressures and Temperatures''. Vacuum. Vol. 7-8, pp.19-29.
+
+Finlayson, E.U., D.K. Arasteh, C. Huizenga, M.D.~Rubin and M.S. Reilly. 1993. WINDOW 4.0: documentation of calculation procedures. Lawrence Berkeley National Laboratory report no. LBL-33943.
+
+ISO. 2003. ISO 15099:2003. Thermal performance of windows, doors, and shading devices -- Detailed calculations. International Organization for Standardization.
+
+Klems, J. H. 1994A. ``A New Method for Predicting the Solar Heat Gain of Complex Fenestration Systems: I. Overview and Derivation of the Matrix Layer Calculation.''. ASHRAE Transactions. 100 (pt.1): 1073-1086.
+
+Klems, J. H. 1994B. ``A New Method for Predicting the Solar Heat Gain of Complex Fenestration Systems: II. Detailed Description of the Matrix Layer Calculation.''. ASHRAE Transactions. 100 (pt.1): 1073-1086.
+
+Klems, J. H. 1995. ``Measurements of Bidirectional Optical Properties of Complex Shading Devices.''. ASHRAE Transactions. 101 (pt 1; Symposium Paper CH-95-8-1 (RP-548)): 791-801.
+
+Klems, J. H. 1996. ``A Comparison between Calculated and Measured SHGC for Complex Glazing Systems.''. ASHRAE Transactions. 102 (Pt. 1; Symposium Paper AT-96-16-1): 931-939.
+
+Klems, J. H. 1996. ``Calorimetric Measurements of Inward-Flowing Fraction for Complex Glazing and Shading Systems.''. ASHRAE Trans. 102(Pt. 1; Symposium Paper AT-96-16-3): 947-954.
+
+Munson, B.R, D.F. Young and T.H. Okiishi. 1998. ``Fundamentals of Fluid Mechanics,'' Third Edition Update, John Wiley \& Sons, Inc.
+
+Papamichael, K. J. 1998. ``Determination and Application of Bidirectional Solar-Optical Properties of Fenestration Systems.''. Cambridge, MA: 13th National Passive Solar Conference.
+
+Simmler, H., U. Fischer and F. Winkelmann. 1996. Solar-Thermal Window Blind Model for DOE-2. Lawrence Berkeley National Laboratory, Simulation Research Group internal report, (unpublished).
+
+Timoshenko, S., \& Kreiger-Woinowsky, S. 1959. ``Theory of Plates and Shells'' 2nd Edition. McGraw-Hill Company.
+
+\subsection{Equivalent Layer Fenestration Model}\label{equivalent-layer-fenestration-model}
+
+The section describes the equivalent layer fenestration optical and thermal model. The Equivalent Layer fenestration model can have four types of attachments: drapes, venetian blinds, roller blinds and insect screens. In this model shading layers are assumed to be uniform and can be represented by an equivalent homogenous layer that has spatially-averaged ``effective'' optical and thermal properties (ASHRAE 1311-RP). Likewise, venetian blinds can be characterized using effective optical and thermal properties. When solar radiation strikes a window surface some fraction of the incident solar radiation passes unobstructed through openings in a shading layer and the remaining fraction is intercepted by the structure of the layer. The intercepted radiation is partly absorbed, partly reflected and partly transmitted. These reflected and transmitted components of the scattered solar radiation are assumed to be uniformly diffuse. Shading layers, because of their openness, generally transmit longwave radiation, and the effective infrared properties of shades account for that. Using effective optical properties and a beam/diffuse split of solar radiation at each layer, the equivalent layer approach can represent multi-layer systems. This representation provides virtually unlimited flexibility to combine different types of shading layers in a fenestration. The equivalent layer window model requires a few set of optical data to characterize a particular layer and this set of data is used to calculate effective layer properties. For instance, the effective solar optical properties of a venetian blind can be calculated as a function of slats optical properties and geometry. Also, it is possible to adjust slat angle at each time step in response to the changing angular position of the sun. Moreover, the model provides control strategies as a function of slat angle that can be changed at each time step as needed. Likewise, effective properties of a pleated drape are calculated as a function of fabric properties and a specified value of fullness. The only input data needed to fully characterize drapery fabrics, roller blinds and insect screens are material openness as area fraction, and the transmittance and reflectance at normal incidence. Shade openness area fraction is the same as the beam-beam transmittance at normal incidence. In multilayer fenestration, each layer is separated by a gap. A gap in equivalent layer model is defined by specifying the fill gas and the gap spacing. Currently five gas types are allowed: Air, Argon, Xenon, Krypton and Custom. The convective heat transfer coefficient in a gap is calculated depending on the spacing, the temperatures of the layers and the fill gas properties. Equivalent-layer concept -- offers wide range of multiple glazing and shading layers combination and can simulate multi-layer complex fenestration systems. The effective layer properties of venetian blinds, pleated drapes, roller blinds, and insect screens are calculated from geometric layer models and material properties. A set of empirical correlations for estimating off-normal material properties were developed under ASHRAE research project (ASHRAE 1311-RP).
+
+\subsubsection{The Equivalent Layer Analysis}\label{the-equivalent-layer-analysis}
+
+The equivalent layer windows system is treated as a series of parallel layers separated by gaps as shown in Figure~\ref{fig:multi-layer-fenestration-analysis-structure}. This multi-layer structure has been used in several computer programs and the underlying theory has been documented (ASHRAE 1311-RP).
+
+\begin{figure}[hbtp] % fig 113
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1827.svg.png}
+\caption{Multi-layer fenestration analysis structure (ASHRAE 1311-RP) \protect \label{fig:multi-layer-fenestration-analysis-structure}}
+\end{figure}
+
+Equivalent layer fenestration model uses two-step analysis. First, the flux of absorbed solar radiation at each layer, S\(_{i}\), caused by the incident radiation flux, I\(_{sol}\), is determined using net radiation analysis. Second, an energy balance is applied at each layer, accounting for heat transfer and the known set of absorbed solar radiations S\(_{i}\) values, in order to solve for the set of layer temperatures, T\(_{i}\), and the corresponding heat fluxes. The fenestration model also accounts for the diathermanous shade layers in the longwave radiant exchange. The latter can be significant for shading layers. Glass is considered opaque with respect to longwave radiation.
+
+\subsubsection{Equivalent Layer Optical Model}\label{equivalent-layer-optical-model}
+
+The multilayer optical model is based on an algorithm originally developed by Edwards (1977) and extended by Wright and Kotey (2006). The algorithm models the interaction of incident solar radiation with a glazing system composed of any number of parallel, planar, specular glazing layers. The shading layers scatter portion of the incident solar radiation diffusely, and the model tracks the beam and diffuse components of solar radiation as they interact with a multi-layer system of glazing and shading layers. The conceptual arrangement for tracking beam and diffuse solar flux components is illustrated in Figure~\ref{fig:solar-analysis-of-the-multi-layer}.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image1828.svg.png}
+\caption{}
+\end{figure}
+
+Analysis yields beam-beam, beam-diffuse and diffuse-diffuse fluxes, providing full detail concerning the quantities of reflected, transmitted and absorbed radiation.
+
+\begin{figure}[hbtp] % fig 114
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1829.svg.png}
+\caption{Solar analysis of the multi-layer glazing/shading system showing beam and diffuse fluxes (ASHRAE 1311-RP) \protect \label{fig:solar-analysis-of-the-multi-layer}}
+\end{figure}
+
+The beam and diffuse characterization of solar radiation demands an expanded set of solar optical properties (Wright and Kotey 2006). The quantities of interest for single layer are shown inFigure~\ref{fig:twelve-solar-properties-assigned-at-each}.
+
+Where,
+
+\emph{t} ~~~ = ~~~~~~~~~ transmittance of a glazing or a shading layer, (-)
+
+\emph{r} ~~ = ~~~~~~~~~ reflectance of a glazing or a shading layer, (-)
+
+\emph{e} ~~~ = ~~~~~~~~~ thermal emissivity of a glazing or a shading layer, (-)
+
+\emph{q} ~~ = ~~~~~~~~~ incident angle, (degree)
+
+\emph{f} ~~ = ~~~~~~~~~ slat angle, (degree)
+
+\emph{W} ~~ = ~~~~~~~~~ profile angle, (degree)
+
+\emph{J}~~~ = ~~~~~~~~~ radiosity of a layer surface, (W/m2)
+
+\emph{T}~~~ = ~~~~~~~~~ temperature of a layer, (C)
+
+Subscripts
+
+\emph{f}~~~~ = ~~~~~~~~~ front side of a layer
+
+\emph{b}~~~ = ~~~~~~~~~ back side of a layer
+
+\emph{bb}~~ = ~~~~~~~~~ beam-beam optical property. Represents a fraction of the beam radiation incident at a given layer and leaves the layer without being scattered.
+
+\emph{bd}~~ = ~~~~~~~~~ beam-diffuse optical property. Represents a fraction of the beam radiation incident at a given layer and leaves the layer diffusely
+
+\emph{dd}~~ = ~~~~~~~~~ diffuse-diffuse optical property. Represents a diffuse radiation incident at a given layer and leaves the layer as diffuse
+
+\emph{i~~~~ = ~~~~~~~~~} layer index, (-)
+
+Superscripts
+
+\emph{m}~~ = ~~~~~~~~~ represents material property (e.g., fabric material)
+
+\emph{str}~ = ~~~~~~~~~ represents an apparent material structure property of roller blinds
+
+\emph{w}~~~ = ~~~~~~~~~ represents an apparent wire property
+
+\begin{figure}[hbtp] % fig 115
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1830.svg.png}
+\caption{Twelve solar properties assigned at each layer (ASHRAE 1311-RP) \protect \label{fig:twelve-solar-properties-assigned-at-each}}
+\end{figure}
+
+Each glazing or shading layer, in general, require eleven set of solar properties (Wright and Kotey 2006). Only beam-beam properties are needed for common glazing layers. Each shading layer is represented by a few set of component properties and geometries that are converted to the full set of layer optical and thermal properties by equivalent layer models (ASHRAE 1311-RP). The models also make account for off-normal incidence of solar radiation and can calculate the diffuse component from normal incidence values using numerical integration.
+
+\subsubsection{Equivalent Layer Thermal Model}\label{equivalent-layer-thermal-model}
+
+A surface energy balance is applied at each layer and the resulting set of equation is solved for layer temperatures and heat transfer fluxes. A schematic drawing of the multi-layer illustration and variables designation is shown in Figure~\ref{fig:radiosity-model-used-in-thermal-analysis-of}. The net radiation formulation based on the radiosities, Jf,i and Jb,i the radiant flux leaving the front and back surfaces of the i\(^{th}\) layer, respectively, is the used as a solution technique. The net radiant heat flux across a gap can be expressed as the difference between the radiosities of the bounding surfaces. The net radiation model analysis yields the layer temperatures and corresponding heat transfer coefficients that are used to determine U-factor and SHGC. The thermal analysis is done in ``ASHWAT\_Thermal'' routine.
+
+\begin{figure}[hbtp] % fig 116
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1831.svg.png}
+\caption{Radiosity model used in thermal analysis of the multi-layer glazing/shading system (ASHRAE 1311-RP) \protect \label{fig:radiosity-model-used-in-thermal-analysis-of}}
+\end{figure}
+
+\subsubsection{Glazing Layer Analysis}\label{glazing-layer-analysis}
+
+The Equivalent-Layer window model allows a wide range of options regarding the selection of glazing layers and gaps combinations. It also allows mixing glazing and shading layers in any sequence. For instance, it allows placing a venetian blind or a roller blind in between glazing layers. Only beam-beam solar properties at normal incidence, infrared transmittance and infrared emissivity are required for common glazing types. Off-normal solar properties at a given sun position are estimated by adjusting the normal incidence values in ``ASHWAT\_OffNormalProperties'' routine. The model assumes that the ratio between normal and off-normal transmittance is the same for the glazing layer in question and a reference piece of uncoated 6 mm glass with a moderate tint (ASHRAE 1311-RP). A similar procedure is used to convert solar reflectance from normal to off-normal.
+
+\subsubsection{Gap Layer Analysis}\label{gap-layer-analysis}
+
+Gaps can be specified as sealed, vented indoors or vented outdoors. The sealed gap is considered as enclosed cavity. Vented gaps is specified for inner and outer most gaps only and when the gas type is AIR. The vented gap model assumes that air flow at the perimeter of the window is not restricted. Any fill gas can be specified by molecular mass and thermo-physical properties of viscosity, specific heat and thermal conductivity. This is done by providing ``a'', ``b'' and ``c'' coefficients of the quadratic equation of the form, p = a + bT + cT\(^{2}\), where the T (K) is temperature and p is the property being evaluated. EnergyPlus has builtin-data available for common fill gas components including Air, Argon, Krypton and Xenon. Users specify CUSTOM gas by defining the coefficients as an input.
+
+\subsubsection{Shade Layer Analysis}\label{shade-layer-analysis}
+
+Equivalent layer fenestration model has a complete set of solar and longwave models for the four shading layer types: drapes, venetian blinds, roller blinds and insect screens developed under ASHRAE 1311-RP. And semi-empirical models are used to evaluate the off-normal properties of drape, roller blind and insect screen materials. The effective layer properties of venetian blinds and the effect of pleating in drapes are determined using a more fundamental net radiation scheme. The openness fraction, A\(_{o}\) and beam-beam solar transmittance at normal incidence, \emph{t}\(_{bb}\) (q = 0) really represent a geometric quantity and it has been confirmed that they can be used interchangeably (ASHRAE 1311-RP). Openness is simply the fraction of a material, by area, that is open. In equivalent layer fenestration model, beam-beam transmittance at normal incidence (i.e., openness fraction), beam-diffuse transmittance and reflectance at normal incidence are required to characterize drapery fabric, roller blind and insect screen material. A conventional venetian blind in equivalent layer model can be characterized by specifying the geometry, solar reflectance and transmittance, and emissivity of the slats. The off-normal solar properties of drape, roller blind and insect screen materials were formulated based on measurements (ASHRAE 1311-RP). The longwave properties of the of the drape fabrics, roller blinds and insect screens can be calculated from the material emissivity and openness of the fabric (ASHRE 1311-RP). The optical model development for venetian blinds is presented by Yahoda and Wright (2004 and 2005), and Kotey et al. (2008).
+
+\subsubsection{Drapes and Curtains}\label{drapes-and-curtains}
+
+The off-normal optical properties of drapery fabric is determined from user specified optical properties at normal incidence (q = 0) using empirical correlations (Kotey et al., 2009a). The input data required to characterize drapery fabric are the beam-beam transmittance of the material at normal incidence \emph{t}\(_{bb}\) (q = 0) = Ao, the beam-diffuse transmittance of the material at normal incidence\emph{t}\(_{bd}\) (q = 0), and the beam-diffuse (total) reflectance of the materialr\(_{bt}\) (q = 0). The off-normal properties are calculated as follows.
+
+Off-normal Transmittance:
+
+\begin{equation}
+{\rm{\tau }}_{{\rm{bb}}}^{\rm{m}}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bb}}}^{\rm{m}}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}\left( {\rm{\theta }} \right)
+\end{equation}
+
+\begin{equation}
+{\rm{\tau }}_{{\rm{bt}}}^{\rm{m}}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bt}}}^{\rm{m}}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}\left( {\rm{\theta }} \right)
+\end{equation}
+
+\begin{equation}
+{\rm{b}} = {\left[ {\; - 0.5 \cdot \ln \;\left( {\;{{\left[ {{\rm{\tau }}_{{\rm{bb}}}^{\rm{m}}{\rm{(\theta }} = {\rm{0)}}\;{\rm{,}}\;\;{\rm{0}}{\rm{.01}}} \right]}^{\;\max }}\;} \right)\;\;,\;\;0.35\;} \right]^{\;\max }}
+\end{equation}
+
+\begin{equation}
+{\rm{b}} = {\left[ {\; - 0.5 \cdot \ln \;\left( {\;{{\left[ {{\rm{\tau }}_{{\rm{bt}}}^{\rm{m}}{\rm{(\theta }} = {\rm{0)}}\;{\rm{,}}\;\;{\rm{0}}{\rm{.01}}} \right]}^{\;\max }}\;} \right)\;\;,\;\;0.35\;} \right]^{\;\max }}
+\end{equation}
+
+\begin{equation}
+{\rm{\tau }}_{{\rm{bt}}}^{\rm{m}}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bd}}}^{\rm{m}}\left( {\rm{\theta }} \right) + {\rm{\tau }}_{{\rm{bb}}}^{\rm{m}}\left( {\rm{\theta }} \right)
+\end{equation}
+
+The off-normal reflectance:
+
+\begin{equation}
+{\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {\rm{\theta }} \right) = {\rm{\rho }}_{{\rm{bd}}}^{\rm{m}}\left( {\rm{\theta }} \right) = {\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right) + \left( {{\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = 9{\rm{0}}^\circ } \right) - {\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right)} \right) \cdot \left( {1 - {\rm{co}}{{\rm{s}}^{{\rm{0}}{\rm{.6}}}}\left( {\rm{\theta }} \right)} \right)
+\end{equation}
+
+\begin{equation}
+{\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{90}}^\circ } \right) = {\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right) + \left( {{\rm{1}} - {\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right)} \right)\;\left( {\,0.7{{\left( {\;{\rm{\rho }}_{}^{\rm{y}}} \right)}^{\;0.7}}} \right)
+\end{equation}
+
+The apparent yarn reflectance is given by:
+
+\begin{equation}
+{\rho ^y} = \frac{{\rho_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}{{{\rm{1}} - \tau_{{\rm{bb}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right)}} = \frac{{\rho_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}{{{\rm{1}} - {{\rm{A}}_{\rm{o}}}}}
+\end{equation}
+
+The above set of equations for drapery fabrics are used subject to the condition that the solar absorptance of the fabric, at normal incidence, is not less than 1\% (ASHRE 1311-RP). The diffuse-diffuse material properties, for Equivalent layer window model, are determined using Rhomberg integration with 32 panels covering the range from q = 0 to q = 90° (ASHRAE 1311-RP). The subscript ``X'' stands for either front or back side of the layer.
+
+\begin{equation}
+  \tau_{x,dd}^{m} = 2\int_{\theta=0}^{\pi/2}\tau_{x,bt}^{m}\PB{\theta}\cos\theta\sin\theta d\theta
+\end{equation}
+
+\begin{equation}
+  \rho_{x,dd}^{m} = 2\int_{\theta=0}^{\pi/2}\rho_{x,bt}^{m}\PB{\theta}\cos\theta\sin\theta d\theta
+\end{equation}
+
+The above set of equations for drapery fabrics apply to the full range of A\(_{o}\), fabric transmittance and fabric reflectance including that falls within the bounds of Keyes' (1967) fabric chart plus sheer fabrics (ASHRAE 1311-RP). The longwave thermal emissivity and thermal transmittances of drapery fabric are calculated using the following correlations and fabric openness fraction (Kotey et al. 2008).
+
+\begin{equation}
+{\varepsilon ^{\rm{m}}} = {\rm{0}}{\rm{.87}} \cdot \left( {{\rm{1 - }}{{\rm{A}}_{\rm{o}}}} \right)
+\end{equation}
+
+\begin{equation}
+{\tau ^{\rm{m}}} = {\rm{1}} - {\rm{0}}{\rm{.95}} \cdot \left( {{\rm{1}} - {{\rm{A}}_{\rm{o}}}} \right)
+\end{equation}
+
+The optical and thermal properties determined using the above same sets of equations are equally valid for pleated drape shades (Kotey, et. al., 2009a). For pleated drape, the effective beam-beam and beam-diffuse solar properties are determined by tracking both radiation components, for a given incident angle, and interaction with a fabric pleated rectangular geometry shown in Figure~\ref{fig:geometry-used-for-pleated-drape-analysis}. The solar optical properties of the two different pleat planes are evaluated on the basis of the local solar incidence angle. Therefore, the effective layer properties are influenced not just by horizontal solar profile angle, W\(_{H}\), but also by incidence angle (ASHRAE 1311-RP).
+
+\begin{figure}[hbtp] % fig 117
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1844.svg.png}
+\caption{Geometry used for Pleated Drape Analysis \protect \label{fig:geometry-used-for-pleated-drape-analysis}}
+\end{figure}
+
+The solar diffuse-diffuse and long-wave effective properties of the pleated drape are evaluated using a much simpler net-radiation analysis using conventional shape factors (Kotey, et. al., 2009a). Users can chose and apply the pleated drape model to any fabric and any degree of fullness (ASHRAE 1311-RP).
+
+\subsubsection{Venetian Blinds}\label{venetian-blinds}
+
+The effective shortwave optical and longwave optical properties of venetian blind layer is estimated using analytical models (Yahoda and Wright 2004, 2005; Kotey et al. 2008). The model requires properties of venetian blind slats and geometry of the slats shown in Figure~\ref{fig:likewise-the-effective-longwave-properties}.
+
+\begin{figure}[hbtp] % fig 1118
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1845.svg.png}
+\caption{Likewise, the effective longwave properties are obtained for the layer knowing longwave properties of the slats. \protect \label{fig:likewise-the-effective-longwave-properties}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 118
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1846.svg.png}
+\caption{Geometry and properties used for venetian blind analysis \protect \label{fig:geometry-and-properties-used-for-venetian}}
+\end{figure}
+
+The model assumes that venetian blind slats reflect and transmit solar radiation diffusely (ASHRAE 1311-RP). The same assumption is made regarding thermal radiation. The input data required to characterize a venetian blind are: front and back side reflectance and transmittance of the slat, geometry and infrared emissivity and transmittance of the slate. The effective optical properties of the venetian blind are determined by tracking beam and diffuse solar radiation through various interactions with slats positioned at a given slat angle. The model uses simple four-surface model if the slats are fully sunlit and a six-surface model if the slats are partially sunlit (ASHRAE 1311-RP). Slats are assumed to be thin and flat but a correction is applied to account for slat curvature effect (Kotey et al. 2008).
+
+\subsubsection{Roller Blinds}\label{roller-blinds}
+
+The off-normal properties of roller-blind are determined from solar properties of roller blind fabric measured at normal incidence (q = 0) using correlations (Kotey, et. al., 2009b). The off-normal properties for roller blind shades are calculated using the set equations given below:
+
+\begin{equation}
+{{\rm{\tau }}_{bb}}\left( {\rm{\theta }} \right) = \left\{ \begin{array}{l}{{\rm{\tau }}_{bb}}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}{\kern 1pt} \left( {\frac{{\rm{\theta }}}{{{{\rm{\theta }}_{{\rm{cutoff}}}}}} \cdot \frac{\pi }{2}} \right)\quad \theta  < {\theta_{CutOff}}\\0\quad \quad \quad \theta  \ge {\theta_{CutOff}}\end{array} \right.
+\end{equation}
+
+\begin{equation}
+{\rm{b}} = {\rm{0}}{\rm{.6}} \cdot {\rm{co}}{{\rm{s}}^{{\rm{0}}{\rm{.3}}}}\left( {{{\rm{A}}_{\rm{o}}} \cdot \frac{{\rm{\pi }}}{{\rm{2}}}} \right)
+\end{equation}
+
+\begin{equation}
+{{\rm{\theta }}_{{\rm{cutoff}}}} = {\rm{65}}^\circ  + \;\left( {{\rm{90}}^\circ  - {\rm{65}}^\circ } \right) \cdot \left( {{\rm{1}} - {\rm{cos}}\left( {{{\rm{A}}_{\rm{o}}} \cdot \frac{{\rm{\pi }}}{{\rm{2}}}} \right)} \right)
+\end{equation}
+
+\begin{equation}
+{\rm{\tau }}_{{\rm{bt}}}^{}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bt}}}^{}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}{\kern 1pt} \left( {\rm{\theta }} \right)
+\end{equation}
+
+\begin{equation}
+b = \left\{ 
+    \begin{array}{lc}
+      0.133 \cdot \left( \rm{\tau}^{str} + 0.003 \right)^{-0.467} &\text{if} \left( 0 \le \rm{\tau}^{str} \le 0.33 \right) \\
+      0.33 \cdot \left( 1 - \rm{\tau}^{str} \right)               &\text{if} \left( 0.33 < \rm{\tau}^{str} \le 1 \right)
+    \end{array}
+  \right.
+\end{equation}
+
+\begin{equation}
+{\rm{\tau }}_{}^{{\rm{str}}} = \frac{{{\rm{\tau }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right) - {{\rm{\tau }}_{{\rm{bb}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}{{{\rm{1}} - {{\rm{\tau }}_{{\rm{bb}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}
+\end{equation}
+
+\begin{equation}
+{\rm{\tau bt}}\left( {\rm{\theta }} \right) = {\rm{\tau bd}}\left( {\rm{\theta }} \right) + {\rm{\tau bb}}\left( {\rm{\theta }} \right)
+\end{equation}
+
+The off-normal solar property calculation of roller blind is based on a set of correlations developed from measurement data using samples of commonly used commercially produced roller blind material openness range of 0.0 -- 0.14. Thus, these correlations are not applicable for shades with materials openness fraction exceeding 0.20. The mean solar reflectance of a roller blind material was found to be purely diffuse and unaffected by incidence angle and is given by:
+
+\begin{equation}
+{\rm{\rho }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right) = {\rm{\rho }}_{{\rm{bd}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right) = {\rm{\rho }}_{{\rm{bt}}}^{}\left( {\rm{\theta }} \right) = {\rm{\rho }}_{{\rm{bd}}}^{}\left( {\rm{\theta }} \right)
+\end{equation}
+
+The diffuse-diffuse transmittance and reflectance are obtained by Rhomberg numerical integration. The longwave properties of roller blind material determined using the material property and the openness fraction (Kotey et al. 2008) as shown below:
+
+\begin{equation}
+{\varepsilon ^{{\rm{rb}}}} = {\rm{0}}{\rm{.91}} \cdot \left( {{\rm{1 - }}{{\rm{A}}_{\rm{o}}}} \right)
+\end{equation}
+
+\begin{equation}
+{\tau ^{{\rm{rb}}}} = {\rm{1}} - {\rm{0}}{\rm{.95}} \cdot \left( {{\rm{1}} - {{\rm{A}}_{\rm{o}}}} \right)
+\end{equation}
+
+\subsubsection{Insect Screens}\label{insect-screens}
+
+The empirical correlations formulated to obtain the effective off-normal solar and longwave properties of insect screens were based on measurements (Kotey et al. (2009a). Insect screen geometry is shown in Figure~\ref{fig:geometry-used-for-insect-screen-analysis}. The calculation of effective solar properties requires a set of properties measured at normal incidence: \emph{t}\(_{bb}\) (q = 0), \emph{t}\(_{bd}\) (q = 0) and \emph{r}\(_{bt}\) (q = 0).
+
+\begin{figure}[hbtp] % fig 119
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1857.svg.png}
+\caption{Geometry used for insect screen analysis \protect \label{fig:geometry-used-for-insect-screen-analysis}}
+\end{figure}
+
+Openness can be determined by optical measurement at normal incidence, A\(_{o}\) = \emph{t}\(_{bb}\) (q = 0), but in the case of insect screens A\(_{o}\) can reliably be calculated knowing wire diameter (\emph{d}), and wire spacing (\emph{s}) as follows:
+
+\begin{equation}
+{A_o} = {\left( {1 - {d \mathord{\left/ {\vphantom {d s}} \right. } s}} \right)^2}
+\end{equation}
+
+The incidence angle beyond which direct beam transmission is cut off, \emph{q}\(_{CutOff}\), can also be estimated purely from geometry and is given by:
+
+\begin{equation}
+{\theta_{CutOff}} = co{s^{ - 1}}\left( {{d \mathord{\left/ {\vphantom {d S}} \right. } S}} \right)
+\end{equation}
+
+The off-normal properties are calculated as follows.
+
+\begin{equation}
+{\tau_{bb}}\left( {\rm{\theta }} \right) = \left\{ \begin{array}{l}{\tau_{bb}}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}\left( {\frac{{\rm{\theta }}}{{{{\rm{\theta }}_{{\rm{cutoff}}}}}} \cdot \frac{\pi }{{\rm{2}}}} \right)\quad {\rm{\theta }} < {{\rm{\theta }}_{{\rm{cutoff}}}}\\0\quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \;\,{\rm{\theta }} \ge {{\rm{\theta }}_{{\rm{cutoff}}}}\end{array} \right.
+\end{equation}
+
+\begin{equation}
+{\rm{b}} =  - {\rm{0}}{\rm{.45}}\;{\rm{ln}}\;\left( {{\rm{MAX}}\left( {{{\rm{\tau }}_{{\rm{bb}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right){\rm{,}}\;{\rm{0}}{\rm{.01}}} \right)} \right)\; + \;{\rm{0}}{\rm{.1}}
+\end{equation}
+
+\begin{equation}
+{\rm{\tau }}_{{\rm{bt}}}^{}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bt}}}^{}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}\left( {\rm{\theta }} \right)
+\end{equation}
+
+\begin{equation}
+{\rm{b}} =  - {\rm{0}}{\rm{.65}}\;{\rm{ln}}\;\left( {{\rm{MAX}}\left( {{{\rm{\tau }}_{{\rm{bt}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right){\rm{,}}\;{\rm{0}}{\rm{.01}}} \right)} \right)\; + \;{\rm{0}}{\rm{.1}}
+\end{equation}
+
+\begin{equation}
+{\rm{\tau }}_{{\rm{bd}}}^{}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bt}}}^{}\left( {\rm{\theta }} \right) - {\rm{\tau }}_{{\rm{bb}}}^{}\left( {\rm{\theta }} \right)
+\end{equation}
+
+\begin{equation}
+{\rm{\rho }}_{{\rm{bt}}}^{}\left( {\rm{\theta }} \right) = {\rm{\rho }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right) + \left( {{\rm{\rho }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = 9{\rm{0}}^\circ } \right) - {\rm{\rho }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right)} \right) \cdot \left( {1 - {\rm{co}}{{\rm{s}}^{\rm{b}}}\left( {\rm{\theta }} \right)} \right)
+\end{equation}
+
+\begin{equation}
+{\rm{b}} =  - {\rm{0}}{\rm{.45}}\;{\rm{ln}}\;{\left( {{{\rm{\rho }}^{\rm{w}}}} \right)^{}}
+\end{equation}
+
+\begin{equation}
+{\rm{\rho }}_{}^{\rm{w}} = \frac{{{\rm{\rho }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}{{{\rm{1}} - {\rm{\tau }}_{{\rm{bb}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}
+\end{equation}
+
+\begin{equation}
+{\rho_{{\rm{bt}}}}\left( {{\rm{\theta }} = {\rm{90}}^\circ } \right) = {\rho_{{\rm{bt}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right) + \left( {1 - {\rho_{{\rm{bt}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right)} \right)\;\left( {{\rm{0}}{\rm{.35}}{\rho ^{\rm{w}}}} \right)
+\end{equation}
+
+The diffuse-diffuse material properties are obtained by Rhomberg numerical integration. The longwave properties of insect screen are given by expressions similar those formulated for drapery fabrics, and roller blinds (Kotey et al. 2008) is given by:
+
+\begin{equation}
+{\varepsilon ^{screen}} = {\varepsilon ^{\rm{w}}} \cdot \left( {{\rm{1  -  }}{{\rm{A}}_{\rm{o}}}} \right)
+\end{equation}
+
+\begin{equation}
+{\tau ^{{\rm{screen}}}} = {\rm{1 - }}{\tau ^{\rm{w}}} \cdot \left( {{\rm{1  -  }}{{\rm{A}}_{\rm{o}}}} \right)
+\end{equation}
+
+The apparent wire material emissivity can be taken as $\varepsilon^w = 0.93$\ for common insect screens - screens with dark, rough, non-metallic wire surfaces. The corresponding infrared wire material transmittance is $\tau^w = 0.98$. A lower infrared emissivity can be used for screens constructed with shiny metallic wire. For example, to model stainless-steel wire mesh use $\varepsilon^w = 0.32$\ and $\tau^w = 0.81$.
+
+\subsubsection{Integration with Heat Balance Method}\label{integration-with-heat-balance-method}
+
+The solar model calculations are performed surface by surface following the existing structure of EnergyPlus's heat balance algorithm. The optical and thermal calculations are performed for each surface at each time step. The thermal model needs to be updated at each time step during the surface heat balance iteration. Thus, window thermal model is invoked during the surface heat balance but only once. This is consistent with the current EnergyPlus's window model inside surface heat balance iteration scheme. The equivalent layer window thermal model also has internal iteration scheme. The thermal model routine also requires the solar and shortwave radiation flux absorbed by each layer of a fenestration at each time step. The calculation of the absorbed radiation flux is performed using the existing scheme except that the optical properties are calculated by the equivalent layer optical model. The equivalent layer thermal model returns the temperatures and the fluxes at each layer.
+
+\subsubsection{Equivalent Layer Window Solar Model}\label{equivalent-layer-window-solar-model}
+
+The equivalent layer window solar model calculates the transmittance of the window and absorptance of each layer. Separate optical properties calculations are performed for exterior beam and diffuse radiations, and interior diffuse radiation (e.g., lighting and inter-reflected solar gain). The fractions for beam radiations depend on solar incident angle and hence updated for each time step. Diffuse radiation fractions are the same for all time steps unless the shade characteristics are altered; for instance, when the venetian blind slat angle is controlled. Otherwise, the diffuse fractions are constant for a given configuration and time step. The hub of the optical properties calculation routine for Equivalent Layer window model is the routine ``ASHWAT\_Solar''. For beam radiation, at each time step, first the normal incidence optical properties are modified for current incident angle. Using the off-normal properties, then the ASHWAT\_Solar routine sets up the coefficient matrix based on the net radiation concept to determine the effective absorptance of each layer and the window transmittance. The total intensity of shortwave radiation absorbed at each layer is determined by multiplying the incident solar radiation, reflected internal solar radiations, and internal shortwave source components by the appropriate absorbed fractions and summing them.
+
+\subsubsection{Equivalent Layer Window Thermal Model}\label{equivalent-layer-window-thermal-model}
+
+The equivalent layer thermal model is calculated only once for each time step. But the thermal model has internal iterative solutions scheme. During each time step, the procedure initially assumes that room air and means radiant temperatures are known. The surface heat balance loops through all zone surfaces while invoking the Equivalent Layer thermal model only once for each window surface at the first iteration. The window surfaces temperatures from the first iteration are used to complete the heat balances for the indoor (and implicitly the outdoor) face of each surface iteratively. Once indoor surface temperatures are calculated using the surface heat balance, the zone air temperature can be updated and the loads are predicted. Shaded fenestration in general do not have single inside temperature by virture their long-wave radiation transmittance. The equivalent layer window model accounts for this using effective emissivity of the composite layers derived for each fenestration (ASHRAE 1311-RP) as shown below:
+
+\begin{equation}
+{\varepsilon ^{eff}} = \sum\limits_{j = 0}^{nl} {\left[ {{\varepsilon_j} \cdot \prod\limits_{k = j{ + 1}}^{nl + {1}} {{\tau_k}} } \right]}
+\end{equation}
+
+where
+
+\emph{$\varepsilon$\(^{eff}\)}~~ = ~~~~~~~~~ composite indoor (room-side) longwave emissivity, (-)
+
+\emph{$\varepsilon$\(_{j}\)~~~ = ~~~~~~~~~} effective emissivity of layer j, (-)
+
+\emph{$\tau$\(_{k}\)~~~ = ~~~~~~~~~} effective infrared transmittance of layer k (\emph{t\(_{1}\)} = 1)
+
+\emph{nl~~~ = ~~~~~~~~~} number of layers in fenestration system (glazing and shade). Layers are numbered outside to inside (layer 1 is outermost, layer \emph{nl} is innermost).
+
+Each equivalent layer window surafce yields net longwave radiant flux exchanged with the zone surfaces. Net longwave radiation exchange from the window to the zone is recast for a composite surface temperature calculation as follows:
+
+\begin{equation}
+{T^{eff}} = \sqrt[4]{{\frac{{{Q_{lw}}}}{{\sigma {\varepsilon ^{eff}}}}}} + {T_0}
+\end{equation}
+
+where
+
+\emph{T\(^{eff}\)}~ = ~~~~~~~~~ inside surface temperature of the composite layer, °C (°F)
+
+\emph{Q\(_{lw}\)}~ = ~~~~~~~~~ infrared radiant gain from zone, W/m2 (Btu/h-ft2)
+
+\emph{$\sigma$}~~~ = ~~~~~~~~~ Stefan-Boltzmann constant, W/m2-K4 (Btu/h-ft2-R4)
+
+\emph{T\(_{0}\)}~~ = ~~~~~~~~~ Temperature of absolute zero, -273.15 °C (-459.67 °F)
+
+Recalculating effective inside face window temperature may result in extra convection flux. The~ ``extra'' (Other) convective flux is computed; this is the gain in excess of that resulting from the standard surface heat balance model. The net other convection term \emph{QX} calculated below is added to the zone air heat balance (ASHRAE 1311-RP).
+
+\begin{equation}
+QX = {Q_{conv}} - hc \cdot ({T^{eff}} - {T_a})
+\end{equation}
+
+Where,
+
+\emph{h\(_{c}\)~~ = ~~~~~~~~~} inside convective coefficient of the fenestration, W/m\(^{2}\)-K (Btu/h-ft\(^{2}\)-F)
+
+\emph{Q\(_{conv}\)~~~~~~~~~~~ = ~~~~~~~~~} total convective heat flux to zone from equivalent layer window thermal model, W/m\(^{2}\) (Btu/h-ft\(^{2}\)); includes open-channel gains and impact of inside surface convective coefficient
+
+\emph{T\(_{a}\)~~ = ~~~~~~~~~} zone air temperature, °C (°F)
+
+\subsubsection{References:}\label{references-2-009}
+
+Edwards, D.K. 1977. Solar absorption by each element in an absorber-coverglass array, Technical Note, Solar Energy, Vol. 19, pp.~401-402.
+
+Parmelee, G. V., and W. W. Aubele. 1952. The shading of sunlit glass: an analysis of the effect of uniformly spaced flat opaque slats, ASHVE Transactions, Vol. 58, pp.~377-398.
+
+Farber, Erich A.; William A. Smith, C.W. Pennington, John C. Reed. 1963. Theoretical analysis of solar heat gain through insulating glass with inside shading. ASHRAE Transactions, Vol. 69, pp.393-405.
+
+Rheault, S., and E. Bilgen. 1989. Heat transfer analysis in an automated venetian blind system, Journal of Solar Energy, Vol. 111 (Feb.), pp.~89-95.
+
+Pfrommer, P., K. J. Lomas, and C. Kupke. 1996. ``Solar Radiation Transport through Slat-Type Blinds: a New Model and its Application for Thermal Simulation of Buildings,'' Solar Energy, Vol. 57, No. 2, pp.~77-91.
+
+Rosenfeld, J.L.J., W. J. Platzer, H. Van Dijk, and A. Maccari. 2000. ``Modelling the Optical and Thermal Properties of Complex Glazing: Overview of Recent Developments'', Solar Energy, Vol. 69 Supplement, No. 1-6, pp.1-13.
+
+Yahoda, D. S. and J. L. Wright. 2004. ``Methods for Calculating the Effective Longwave Radiative Properties of a Venetian Blind Layer,'' ASHRAE Transactions, Vol. 110, Pt. 1., pp.~463-473.
+
+Yahoda, D. S. and J. L. Wright. 2005. ``Methods for Calculating the Effective Solar-Optical Properties of a Venetian Blind Layer,'' ASHRAE Transactions, Vol. 111, Pt. 1, pp.~572-586.
+
+Yahoda, D. S. and J. L. Wright. 2004. ``Heat Transfer Analysis of a Between-Panes Venetian Blind Using Effective Longwave Radiative Properties,'' ASHRAE Transactions, Vol. 110, Pt. 1., pp.~455-462.
+
+Huang, N.Y.T., J. L. Wright, M. R. Collins. 2006. ``Thermal Resistance of a Window with an Enclosed Venetian Blind: Guarded Heater Plate Measurements,'' ASHRAE Transactions, Vol. 112, Pt. 2. pp.~13-21.
+
+Wright, J. L. 2008. ``Calculating Centre-Glass Performance Indices of Glazing Systems with Shading Devices,'' ASHRAE Transactions, Vol. 114, Pt. 2.
+
+Wright, J. L., N. Y. T. Huang, and M. R. Collins. 2008. ``Thermal Resistance of a Window with an Enclosed Venetian Blind: A Simplified Model,'' ASHRAE Transactions, Vol. 114, Pt. 1.
+
+Kotey, N. A., J. L. Wright, and M. R. Collins. 2008. ``Determining Longwave Radiative Properties of Flat Shading Materials,'' 33rd Annual SESCI / 3rd CSBC Conference Proceedings, Fredericton, NB.
+
+Kotey, N.A., Wright, J.L., M. R. Collins. 2009a. ``Determination of Angle-Dependent Solar Optical Properties of Roller Blind Materials,'' drafted for submission to ASHRAE Transactions, Vol. 115, Pt. 1.
+
+Kotey, N.A., Wright, J.L., M. R. Collins. 2009b. ``Determination of Angle-Dependent Solar Optical Properties of Drapery Fabrics,'' in review, ASHRAE Transactions, Vol. 115, Pt. 2.
+
+Wright, John L., Charles S. Barnaby, Michael R. Collins, and Nathan A. Kotey. Improving Cooling Load Calculations for Fenestration with Shading Devices . ASHRAE 1311-RP, Final Report, February 11, 2009.
diff --git a/doc/engineering-reference/src/demand-limiting.tex b/doc/engineering-reference/src/demand-limiting.tex
new file mode 100644
index 00000000000..fe0f6b1c314
--- /dev/null
+++ b/doc/engineering-reference/src/demand-limiting.tex
@@ -0,0 +1,82 @@
+\chapter{Demand Limiting}\label{demand-limiting}
+
+Demand limiting, or demand management, is a strategy for reducing a building's demand for utilities, e.g., electricity.~ Utility companies typically charge a monthly fee for ``demand charges'' that is based on the peak demand during a certain time period.~ Often the peak demand charge is set by one exceptional day that is much higher than the peak demand for an average day during the month.~ Therefore, to save utility costs, it is in the interest of building owners to find ways to manage the demand on peak days.~ While demand management is generally concerned with the demand for electricity, the future will likely see demand management of other utilities, such as natural gas or water.
+
+Demand limiting controls shut off or reduce the power to non-essential loads in order to reduce the overall building demand.~ Some typical controls:
+
+\begin{itemize}
+\item
+  shut off or dim electric lights, equipment, or HVAC systems
+\item
+  reset the thermostatic setpoints on HVAC systems
+\item
+  reduce ventilation load thus electricity demand
+\item
+  reduce the load of a set of similar components by rotating one or more components ``off'' for a short time interval
+\item
+  turn on generators to meet some or all of the building's demand.
+\end{itemize}
+
+The demand limiting controls implemented in EnergyPlus are intended to allow some of the more common demand limiting strategies.~ The DemandManagerAssignmentList object is a high level control that makes demand limiting decisions based on a list of possible demand limiting strategies.~ Each demand limiting strategy is described in a separate DemandManager object.~ Each DemandManager object controls a group of similar load objects of the same type, such as DemandManager:Lights, DemandManager:ElectricEquipment, DemandManager:Thermostats, or DemandManager:Ventilation objects.
+
+\subsection{Algorithm}\label{algorithm}
+
+In EnergyPlus the DemandManagerAssignmentList and DemandManager objects are simulated by the Demand Manager module.~ The Demand Manager is built into the overall solution method for the program.~ For each zone time step, the program executes three major segments of code:
+
+*~exterior energy use
+
+\begin{itemize}
+\item
+  zone heat balance (surface heat balances, internal gains, and air flows)
+\item
+  HVAC system simulation (air and plant loops)
+\end{itemize}
+
+The exterior energy use segment is completely independent of the zone heat balance and HVAC system simulation.~ Exterior energy use handles energy use accounting for exterior lights and exterior equipment that are outside of the building and are not part of the zone heat balance.~ The zone heat balance segment includes all of the surface heat balances, internal heat gains, and air flows.~ The HVAC system simulation includes air and plant loops with their associated HVAC components.~ The behaviour of the HVAC system depends on the results of the zone heat balance.~ The HVAC system simulation operates on a variable ``system'' time step which is automatically shortened if necessary for stability.
+
+The Demand Manager is called after the first pass through the HVAC system simulation, before the system time step is shortened.~ After evaluating the DemandManagerAssignmentList object, the Demand Manager decides if demand limiting is required.~ If demand limiting is required, the individual DemandManager objects are surveyed to determine which loads can be limited.~ Based on the \emph{Demand Manager Priority} selected, the Demand Manager then decides which DemandManager objects should be activated.~ In turn, the activated DemandManager objects set the demand limiting hooks on their respective load objects.~ Finally, depending on the type of DemandManager objects that were activated, one or more of the major segments of code must be called to be resimulated because the load conditions have changed.~ The code segments depend on the type of DemandManager and the relationship of its load objects to the overall solution method.~ The table below shows the different DemandManager types and the related code segments that must be resimulated.
+
+% table 42
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Demand Manager Types and Resimulation. \label{table:demand-manager-types-and-resimulation.}} \tabularnewline
+\toprule 
+Demand Manager Type & Resimulate Exterior Energy & Resimulate Zone Heat Balance & Resimulate HVAC System \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Demand Manager Types and Resimulation.} \tabularnewline
+\toprule 
+Demand Manager Type & Resimulate Exterior Energy & Resimulate Zone Heat Balance & Resimulate HVAC System \tabularnewline
+\midrule
+\endhead
+
+DemandManager:ExteriorLights & X & ~ & ~ \tabularnewline
+DemandManager:Lights & ~ & X & X \tabularnewline
+DemandManager:ElectricEquipment & ~ & X & X \tabularnewline
+DemandManager:Thermostats & ~ & ~ & X \tabularnewline
+DemandManager:Ventilation & ~ & ~ & X \tabularnewline
+\bottomrule
+\end{longtable}
+
+All demand limiting controls are disabled during warmup days and sizing runs.
+
+\subsubsection{Sequential Priority}\label{sequential-priority}
+
+If the \emph{Demand Manager Priority} field of the DemandManagerAssignmentList object is set to SEQUENTIAL, each DemandManager in the list is activated in sequence from first to last until demand is reduced below the limit or until all managers are activated.~ A DemandManager is skipped if it cannot reduce the demand.~ Possible reasons that a manager cannot reduce demand include:
+
+\begin{itemize}
+\item
+  not enough load to limit
+\item
+  not available because of its \emph{Availability Schedule}
+\item
+  already activated; load limited during a previous time step.
+\end{itemize}
+
+For each DemandManager in the list that is successfully activated, one or more of the major code segments must be called to be resimulated (see above).~ The DemandManagerAssignmentList object is then reevaluated to determine if further demand limiting is required before the next DemandManager is activated.
+
+The implication of sequential priority is that a DemandManagerAssignmentList with many DemandManagers may make many passes through the Demand Manager before all demand limiting decisions are finalized.~ Each pass requires an additional resimulation of the current time step.~ In some cases this could significantly slow down the overall simulation runtime.~ The use of the \emph{Minimum Limit Duration} field can help to ensure that not every DemandManager is being activated at every time step.
+
+\subsubsection{All Priority}\label{all-priority}
+
+If the \emph{Demand Manager Priority} field of the DemandManagerAssignmentList object is set to ALL, all DemandManagers in the list are activated simultaneously to achieve the maximum demand reduction.~ This priority option requires only one final resimulation after all DemandManagers are activated.
diff --git a/doc/engineering-reference/src/economics-calculations.tex b/doc/engineering-reference/src/economics-calculations.tex
new file mode 100644
index 00000000000..ae52fe94117
--- /dev/null
+++ b/doc/engineering-reference/src/economics-calculations.tex
@@ -0,0 +1 @@
+\chapter{Economics Calculations}\label{economics-calculations}
diff --git a/doc/engineering-reference/src/economics-calculations/component-costs.tex b/doc/engineering-reference/src/economics-calculations/component-costs.tex
new file mode 100644
index 00000000000..ae3e9e0698f
--- /dev/null
+++ b/doc/engineering-reference/src/economics-calculations/component-costs.tex
@@ -0,0 +1,236 @@
+\section{Component Costs}\label{component-costs}
+
+EnergyPlus provides simple cost estimating capabilities as an aid to design analysis and for life cycle costs.~ There are three broad steps involved.~ The first involves determining \emph{construction} costs by summing individual ``line items.''~ The second involves determining \emph{project} costs by adjusting construction costs to account for things like profit and design fees.~ The third involves comparing the current simulation to a reference case so that marginal increases can be calculated.~ The reference documentation contained in this section pertains to the following input object names.
+
+\begin{itemize}
+\item
+  \textbf{ComponentCost:LineItem}
+\item
+  \textbf{ComponentCost:Adjustments}
+\item
+  \textbf{ComponentCost:Reference}
+\end{itemize}
+
+\subsection{Line Item Costs}\label{line-item-costs}
+
+Line item cost calculations are generally trivial involving simple multiplication and summation.~ This section documents details of how line item costs are calculated.~ The program code consists mainly of a \textbf{Case} construct where the \textbf{Line Item Type} is used to control the details of how calculations are performed.
+
+The overall philosophy is to provide methods of calculating items using either direct entry of needed data (\textbf{`General'} using object type), or using component descriptive data entered elsewhere in the input file (e.g. \textbf{`Lights'}), or by using quantities that are calculated by the program during the simulation (e.g. \textbf{`Coil:DX'} and \textbf{`Chiller:Electric'}).
+
+The rest of this section provides details by organized by the type of line item.
+
+\subsubsection{General}\label{general}
+
+The line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-Each, \emph{P\(_{e}\)}:
+
+\begin{equation}
+L = N * {P_e}
+\end{equation}
+
+\subsubsection{Construction}\label{construction}
+
+This line item type is called ``Construction'' but is used to estimate the costs of surfaces in the model.~ The Construction attribute of Surface objects is useful for categorizing surfaces.~ The number of units, \emph{N}, is determined by summing the Area, \emph{A}, of Surface objects that have the type of construction specified in the \textbf{Item Name} field.~ Surfaces are screened to eliminate any duplicates that may exist for interior partitions creating a list of 1 to \emph{m} unique surfaces.~ If a surface is associated with a Zone, then zone multiplier, \emph{M\(_{Z}\)}, and list multipliers, \emph{M\(_{G}\)}, are applied (these are usually defaulted to 1).
+
+\begin{equation}
+N = \sum\limits_1^m {(A*{M_Z} * {M_G}} )
+\end{equation}
+
+The line item subtotal, \emph{L}, is calculated by multiplying the number of units (actually units of are here), \emph{N} (m\(^{2}\)) by the Cost-per-Area, \emph{P\(_{a}\)} , (\$/m\(^{2}\)):
+
+\begin{equation}
+L = N * {P_a}
+\end{equation}
+
+\subsubsection{Coil:DX and Coil:Cooling:DX:SingleSpeed}\label{coildx-and-coilcoolingdxsinglespeed}
+
+DX coil costs can be estimated in one of three ways: per-each, per-kW, per-kW-COP.~ The program determines which method to use based on there being non-zero values in appropriate input fields.
+
+If \textbf{cost per each} is greater than 0.0 then the number of units, \emph{N}, is the number of cooling coils.~ This will be 1 if the \textbf{Item Name} is the name of a specific coil described elsewhere.~ If the name is set to the wildcard (*) then this will equal the total number of DX:Coils in the model.~ Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-Each, \emph{P\(_{e}\)}:
+
+\begin{equation}
+L = N * {P_e}
+\end{equation}
+
+If \textbf{cost per kilowatt} is greater than 0.0 then the number of units, \emph{N}, is the number of kilowatts of total, rated, cooling capacity.~ This will be based on all the DX:Coils in the model if \textbf{Item Name} is set to the wildcard (*) and will be that of the named coil if set to a valid coil name.~ Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-kilowatt, \emph{P\(_{kW}\)}:
+
+\begin{equation}
+L = N * {P_{kW}}
+\end{equation}
+
+If \textbf{Cost per kilowatt per coefficient-of-performance} is greater than 0.0 then the number of units, \emph{N}, is the number of kilowatts of total, rated, cooling capacity multiplied by the nominal coefficient of performance (COP) of the DX:Coils.~ This will be based on all the DX:Coils in the model if \textbf{Item Name} is set to the wildcard (*) and will be that of the named coil if set to a valid coil name.~ Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-kilowatt-per-COP, \emph{P\(_{kW-COP}\)}:
+
+\begin{equation}
+L = N * {P_{kW - COP}}
+\end{equation}
+
+\subsubsection{Coil:Heating:Gas}\label{coilheatinggas}
+
+Gas-fired heating coil costs can be estimated in one of three ways: per-each, per-kW, per-kW-COP.~ The program determines which method to use based on there being non-zero values in appropriate input fields.
+
+If \textbf{cost per each} is greater than 0.0 then the number of units, \emph{N}, is the number of heaters.~ This will be 1 if the \textbf{Item Name} is the name of a specific heater described elsewhere.~ If the name is set to the wildcard (*) then this will equal the total number of Coil:Heating:Gas objects in the model.~ Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-Each, \emph{P\(_{e}\)}:
+
+\begin{equation}
+L = N * {P_e}
+\end{equation}
+
+If \textbf{Cost per kilowatt} is greater than 0.0 then the number of units, \emph{N}, is the number of kilowatts of total, rated, heating capacity.~ This will be based on all the Coil:Heating:Gas objects in the model if \textbf{Item Name} is set to the wildcard (*) and will be that of the named coil if set to a valid coil name.~ Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-kilowatt, \emph{P\(_{kW}\)}:
+
+\begin{equation}
+L = N * {P_{kW}}
+\end{equation}
+
+If \textbf{Cost per kilowatt per coefficient-of-performance} is greater than 0.0 then the number of units, \emph{N}, is the number of kilowatts of total, rated, heating capacity multiplied by the theoretical efficiency of the heater(s).~ (Here we are treating gas heating efficiency as a Coefficient of Performance (COP)).~ This will be based on all the Coil:Heating:Gas objects in the model if \textbf{Item Name} is set to the wildcard (*) and will be that of the named coil if set to a valid coil name.~ Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-kilowatt-per-COP, \emph{P\(_{kW-COP}\)}:
+
+\begin{equation}
+L = N * {P_{kW - COP}}
+\end{equation}
+
+\subsubsection{Chiller:Electric}\label{chillerelectric}
+
+Electric chiller costs can be estimated in one of three ways: per-each, per-kW, per-kW-COP.~ The program determines which method to use based on there being non-zero values in appropriate input fields.
+
+If \textbf{cost per each} is greater than 0.0 then the number of units, \emph{N}, is the number of chillers.~ This will be 1 if the \textbf{Item Name} is the name of a specific coil described elsewhere.~ Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-Each, \emph{P\(_{e}\)}:
+
+\begin{equation}
+L = N * {P_e}
+\end{equation}
+
+If \textbf{Cost per kilowatt} is greater than 0.0 then the number of units, \emph{N}, is the number of kilowatts of total, rated, cooling capacity for the specified chiller. Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-kilowatt, \emph{P\(_{kW}\)}:
+
+\begin{equation}
+L = N * {P_{kW}}
+\end{equation}
+
+If \textbf{Cost per kilowatt per coefficient-of-performance} is greater than 0.0, then the number of units, \emph{N}, is the number of kilowatts of total, rated, cooling capacity multiplied by the nominal coefficient of performance (COP) of the chiller. This will be based on the named chiller (if set to a valid coil name). Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-kilowatt-per-COP, \emph{P\(_{kW-COP}\)}:
+
+\begin{equation}
+L = N * {P_{kW - COP}}
+\end{equation}
+
+\subsubsection{Daylighting:Controls}\label{daylightingcontrols}
+
+The costs of controllers for harvesting daylight are determined by the number of reference points.~ The cost for each controller, \emph{P\(_{e}\)} , are input.~ The of units, \emph{N}, is determined from the number of daylight reference points in all the zones if the \textbf{Item Name} is the wildcard (*).~ If \textbf{Item Name} is set to a valid Zone name then N is the number of daylight reference points in just that zone (zones can have more than one daylight controllers).~ Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-Each, \emph{P\(_{e}\)}:
+
+\begin{equation}
+L = N * {P_e}
+\end{equation}
+
+\subsubsection{Shading:Zone:Detailed}\label{shadingzonedetailed}
+
+Shading surfaces need to be handled separately because they do not have the \textbf{Construction} attribute.~ The \textbf{Item Name} must be set to a valid name for a \textbf{Shading:Zone:Detailed} object defined elsewhere in the file.~ The number of units, N, is determined from the area of the named surface multiplied by zone multiplier, \emph{M\(_{Z}\)}, and list multipliers, \emph{M\(_{G}\)}:
+
+\begin{equation}
+N = A*{M_Z} * {M_g}
+\end{equation}
+
+The line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N} (m\(^{2}\)) by the Cost-per-Area, \emph{P\(_{a}\)} , (\$/m\(^{2}\)):
+
+\begin{equation}
+L = N * {P_a}
+\end{equation}
+
+\subsubsection{Lights}\label{lights}
+
+The cost of electric lighting systems can be modeled in two ways: per-each and per-kW.~ The program determines which method to use based on there being non-zero values in appropriate input fields.~ The \textbf{Item Name} must be the name of a valid Zone defined elsewhere in the input.
+
+If \textbf{cost per each} is greater than 0.0, then the number of units, \emph{N}, is the number lighting systems in the zone and is assumed to be 1.~ Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-Each, \emph{P\(_{e}\)}:
+
+\begin{equation}
+L = N * {P_e}
+\end{equation}
+
+If \textbf{Cost per kilowatt} is greater than 0.0 then the number of units, \emph{N}, is the number of kilowatts in the design level for electric lighting systems defined in Lights objects associated with the zone.~ The \textbf{Item Name} must be the name of a valid Zone defined elsewhere in the input.~ \emph{N} is then the sum of all the Lights associated with the named Zone. Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-kilowatt, \emph{P\(_{kW}\)}:
+
+\begin{equation}
+L = N * {P_{kW}}
+\end{equation}
+
+\subsubsection{Generator:Photovoltaic}\label{generatorphotovoltaic}
+
+The costs of simple photovoltaic power systems can be modeled using cost per kilowatt.~ The number of units, N, is the nominal rated peak power of the photovoltaic panels.~ The photovoltaic generator must be modeled using the PhotovoltaicPerformance:Simple input object which is a very simplistic model and does not include input for the nominal rated peak power of the system.~ Therefore a peak power is calculated using the usual 1000 W/m\(^{2}\) of incident solar radiation, \emph{G\(_{p}\)}, multiplied by the active solar cell area, \emph{A} and the efficiency, \emph{E}, and converted to units of kilowatts.
+
+\begin{equation}
+N = \frac{{{G_p} * A * E}}{{1000.0}}
+\end{equation}
+
+Where, the cell area A is calculated by multiplying the area of the surface associated with the simple photovoltaic system and the active area fraction defined in the PhotovoltaicPerformance:Simple. Then the line item subtotal, \emph{L}, is calculated by multiplying the number of units, \emph{N}, by the Cost-per-kilowatt, \emph{P\(_{kW}\)}:
+
+\begin{equation}
+L = N * {P_{kW}}
+\end{equation}
+
+\subsection{Adjustments}\label{adjustments}
+
+Various adjustments are available to model total project costs from the component costs modeled using individual line items.~ These adjustments are provided to allow propagating how changes in component costs are amplified by things like design fees, profit, bonding, and taxes.
+
+The subtotal of individual line items, \emph{S\(_{L}\)}, is obtained by summing all line item subtotals, \emph{L}:
+
+\begin{equation}
+{S_L} = \sum L
+\end{equation}
+
+For the reference building, \emph{S\(_{L,}\)}is user input (typically from a prior run of baseline building model).
+
+The subtotal for miscellaneous construction costs (typically those costs not explicitly included as line items), \emph{S\(_{m}\)}, are calculated by multiplying the \textbf{Miscellaneous Cost Model} (per Square Meter), \emph{C\(_{m}\)},~ by the total conditioned floor area, \emph{A\(_{c}\)}:
+
+\begin{equation}
+{S_m} = {A_c} * {C_m}
+\end{equation}
+
+The subtotal for the amount that the construction costs should be altered because of regional differences in material and labor costs (e.g.~when using national average data), \emph{S\(_{r}\)}, is determined by multiplying the Regional Adjustment Factor, \emph{R\(_{f\, ,}\)} by the sum of \emph{S\(_{L}\)}~and \emph{S\(_{m:}\)}
+
+\begin{equation}
+{S_r} = ({S_L} + {S_m}){R_f}
+\end{equation}
+
+Remaining adjustments are applied to the subtotal for construction costs, \emph{S\(_{c}\)}, which is the sum of \emph{S\(_{L}\)}, \emph{S\(_{m,}\)}, and \emph{S\(_{r:}\)}
+
+\begin{equation}
+{S_C} = {S_L} + {S_m} + {S_r}
+\end{equation}
+
+The \textbf{Design and Engineering Fee Fraction},\emph{F\(_{d}\)},is the fraction of construction costs, \emph{S\(_{c}\)}, attributable to costs associated with architectural and engineering services needed for the project.~ The subtotal for costs associated with these fees, \emph{S\(_{D}\)}, are determined by multiplying \emph{S\(_{C}\)} by \emph{F\(_{d}\)}:
+
+\begin{equation}
+{S_D} = {S_c}*{F_D}
+\end{equation}
+
+The \textbf{Contractor Fee Fraction},\emph{F\(_{c}\)},is the fraction of construction costs, \emph{S\(_{c}\)}, attributable to costs associated with the contractor's profit that should be included in the project.~ The subtotal for costs associated with contracting, \emph{S\(_{P}\)}, are determined by multiplying \emph{S\(_{C}\)} by \emph{F\(_{d}\)}:
+
+\begin{equation}
+{S_P} = {S_c}*{F_C}
+\end{equation}
+
+The \textbf{Contingency Fraction},\emph{F\(_{S}\)},is the fraction of construction costs, \emph{S\(_{c}\)}, which should be included in a cost estimate to provide for contingencies (perhaps related to errors and uncertainty in the estimate and project).~ The subtotal for contingency costs, \emph{S\(_{S}\)}, are determined by multiplying \emph{S\(_{C}\)} by \emph{F\(_{S}\)}:
+
+\begin{equation}
+{S_S} = {S_c}*{F_S}
+\end{equation}
+
+The \textbf{Permits, Bonding, Insurance Fraction,}\emph{F\(_{B}\)},is the fraction of construction costs, \emph{S\(_{c}\)}, which should be included in a cost estimate to provide for things like taxes, bonding, insurance, and permits.~ The subtotal for these extra costs, \emph{S\(_{B}\)}, are determined by multiplying \emph{S\(_{C}\)} by \emph{F\(_{B}\)}:
+
+\begin{equation}
+{S_B} = {S_c}*{F_B}
+\end{equation}
+
+The \textbf{Commissioning Fee Fraction,}\emph{F\(_{CX}\)},is the fraction of construction costs, \emph{S\(_{c}\)}, which should be included in a cost estimate to provide for commissioning the building systems.~ The subtotal for these extra costs, \emph{S\(_{CX}\)}, are determined by multiplying \emph{S\(_{C}\)} by \emph{F\(_{CX}\)}:
+
+\begin{equation}
+{S_{CX}} = {S_c}*{F_{CX}}
+\end{equation}
+
+Finally, the cost estimate total, \emph{T}, is obtained by summing the various subtotals:
+
+\begin{equation}
+T = {S_L} + {S_m} + {S_r} + {S_D} + {S_P} + {S_S} + {S_B} + {S_{CX}}
+\end{equation}
+
+The normalized total cost estimate, C, is calculated by dividing \emph{T} by the total conditioned floor area, \emph{A\(_{c}\)}:
+
+\begin{equation}
+C = \frac{T}{{{A_C}}}
+\end{equation}
+
+\subsection{Comparisons}\label{comparisons}
+
+The capability of comparing the current cost estimate to that of a reference building is provided because is common to consider the marginal increases in costs associated with applying different energy design measures.~ EnergyPlus calculates and reports the difference between the current model and a reference case for all the subtotals and totals discussed above.~ The reported differences are the reference values subtracted from the current value.
diff --git a/doc/engineering-reference/src/economics-calculations/life-cycle-cost-computations.tex b/doc/engineering-reference/src/economics-calculations/life-cycle-cost-computations.tex
new file mode 100644
index 00000000000..1eca9e4ce52
--- /dev/null
+++ b/doc/engineering-reference/src/economics-calculations/life-cycle-cost-computations.tex
@@ -0,0 +1,74 @@
+\section{Life-Cycle Cost Computations}\label{life-cycle-cost-computations}
+
+The objects used for performing a life-cycle cost analysis are:
+
+\begin{itemize}
+\item
+  LifeCycleCost:Parameters
+\item
+  LifeCycleCost:RecurringCosts
+\item
+  LifeCycleCost:NonrecurringCost
+\item
+  LifeCycleCost:UsePriceEscalation
+\item
+  LifeCycleCost:UseAdjustment
+\end{itemize}
+
+The computation of life-cycle costs is broken into three main routines which are described below.
+
+\subsection{ExpressAsCashFlows}\label{expressascashflows}
+
+Step 1. If the input file has ComponentCost:* items, then create an additional instance of a nonrecurring cost to hold the total.
+
+Step 2. Get the costs for each resource that has non-zero utility costs.
+
+Step 3. Compute the inflation on a monthly basis. For cases where the inflation approach is constant dollars, the inflation is set to 1.0 for all months. For current dollar analyses, compute the inflation rate on a monthly basis. Just using 1/12 of the annual inflation is almost correct but introduces a small error so instead the inverse of the formula 4-32 from Newnan (Engineering Economic Analysis Ninth Edition by Donald Newnan, Ted Eschenbach, and Jerome Lavelle):
+
+inflationPerMonth = ((inflation + 1.00) ** (1.0/12.0)) - 1
+
+Then the inflation is applied for each month:
+
+monthlyInflationFactor(jMonth) = (1 + inflationPerMonth) ** (jMonth - 1)
+
+Step 4. Put the nonrecurring, nonrecurring, and utility costs into a monthly array for the entire length of the study period.
+
+Step 5. Multiply the monthly costs by the monthly inflation which was set to 1.0 for constant dollar analyses.
+
+Step 6. Multiply the monthly costs for resources with use adjustments.
+
+Step 7. Sum the monthly costs by category.
+
+Step 8. Based on the base date, accumulate the monthly costs into yearly costs.
+
+\subsection{ComputePresentValue}\label{computepresentvalue}
+
+Step 1. For each year of the study compute the discount factor (SPV) using the following formula:
+
+SPV\(_{yr}\) = 1 / ((1 + curDiscountRate) ** effectiveYear)
+
+This formula is based on formula D.2.1.1 from NIST Handbook 135 Life Cycle Costing Manual for the Federal Energy Management Program by Sieglinde K. Fuller and Stephen R. Petersen.
+
+Where the effectiveYear depends on the discount convention. If end of year discounting is used than the effectiveYear is the year. If middle of the year discounting is used than the effectiveYear is reduced by 0.5. If the beginning of year discounting is used, than the effectiveYear is reduced by 1.0.
+
+For energy costs, the use price escalations are multiplied by the discount factors.
+
+Step 2. Compute the present value for each month by multiply the monthly costs by the discount factor for each year.
+
+Step 3. Sum the costs by category.
+
+\subsection{ComputeTaxAndDepreciation}\label{computetaxanddepreciation}
+
+Step 1. Depending on the depreciation method selected the depreciation factors are set to various constants. Depreciation factors are based on IRS Publication 946 for 2009 ``How to Depreciate Property.'' The MACRS values are based on Modified Accelerated Cost Recovery System GDS for 3, 5, 7, 10 year property are based on 200\% depreciation method shown in Appendix A of IRS Publication 946 using half year. 15 and 20 are based on 150\% (Chart 1 of IRS Publication 946). For Straight Line depreciation GDS is used for 27 years (actually 27.5) 31 years (actually 31.5 years) and 39 years using mid month. For 40 years ADS is used (chart 2) Table A-1 is used for 3, 4, 5, 10, 15 and 20 years. Table A-6 is for 27 years. Table A-7 for 31 years. Table A-7a for 39 years. Table A-13 for 40 years. These years are a classification of property and should not be confused with the length of the study. For 27 years, 31 years, 39 years and 40 years the June value was used. All references in this paragraph are to IRS Publication 946.
+
+Step 2. Apply the annual depreciation factors to the capital costs.
+
+Step 3. For each year the taxable income is the grand total of all costs minus the depreciated capital costs.
+
+Step 4. Taxes are the taxable income times the tax rate.
+
+Step 5. The after tax present value is
+
+AfterTaxPresentValue\(_{yr}\) = GrandTotal\(_{yr}\) - Taxes\(_{yr}\) * SPV\(_{yr}\)
+
+All major results are presented on the tabular report.
diff --git a/doc/engineering-reference/src/economics-calculations/tariff-computation.tex b/doc/engineering-reference/src/economics-calculations/tariff-computation.tex
new file mode 100644
index 00000000000..ddd015c92e9
--- /dev/null
+++ b/doc/engineering-reference/src/economics-calculations/tariff-computation.tex
@@ -0,0 +1,161 @@
+\section{Tariff Computation}\label{tariff-computation}
+
+The EnergyPlus economic (Utility Costs) objects related to computing utility bills include:
+
+\begin{itemize}
+\item
+  UtilityCost:Tariff
+\item
+  UtilityCost:Qualify
+\item
+  UtilityCost:Charge:Simple
+\item
+  UtilityCost:Charge:Block
+\item
+  UtilityCost:Ratchet
+\item
+  UtilityCost:Variable
+\item
+  UtilityCost:Computation
+\end{itemize}
+
+This section builds upon the discussion that appears in the Input Output Reference under the heading ``EnergyPlus Economics.''~ The actual computation of monthly utility bills is not difficult since it is mostly consists of multiplying energy consumptions or demands by the price on a per unit basis and adding different bill components.~ The implementation in EnergyPlus becomes more complex since the objects were crafted to allow a great deal of~ flexibility in specifying a utility tariff while, at the same time, being as simple as possible.
+
+The following discussion on variables and hierarchies is based on the text that appears in the Input Output Reference.
+
+\subsection{Conceptual Framework -- Variables and Hierarchy}\label{conceptual-framework-variables-and-hierarchy}
+
+To understand how to use the utility bill calculation portion of EnergyPlus you first need to understand some important concepts of variables and hierarchy.~ A variable, for the purposes of this section, is simply a named holder of a series of numbers. In most cases, the variable will be a named holder of 12 numbers, one number for each monthly utility bill. Here is a visualization of a variable called Electric Energy Use:
+
+\begin{longtable}[c]{@{}lll@{}}
+\toprule 
+Object & Outputs & Inputs \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Object & Outputs & Inputs \tabularnewline
+\midrule
+\endhead
+
+Qualify & Name & Source \tabularnewline
+~ & ~ & Threshold \tabularnewline
+Charge:Simple & Name & Source \tabularnewline
+~ & Category & Cost Per Unit \tabularnewline
+Charge:Block & Name & Source \tabularnewline
+~ & Category & Block Size Multiplier \tabularnewline
+~ & Remaining & Block Size \tabularnewline
+~ & ~ & Block Cost \tabularnewline
+Ratchet & Name & Baseline \tabularnewline
+~ & ~ & Adjustment \tabularnewline
+~ & ~ & Multiplier \tabularnewline
+~ & ~ & Offset \tabularnewline
+\bottomrule
+\end{longtable}
+
+If you have ever done any computer programming, you can think of a variable as an array.~ Many of the names used in the utility bill calculation portion of EnergyPlus are names of variables.~ In the case of the UtilityCost:Charge objects, the name of the object is also used as a name of a variable.
+
+In many of today's utility rates, the charges for energy or demand are broken into distribution and supply charges.~ To allow for this, more than one charge may to be defined for a particular category.~ The variables assigned to the same category are added together.
+
+The categories are combined in following hierarchy:
+
+
+\begin{figure}[hbtp]
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7909.png}
+\caption{Category Hierarchy \label{fig:category-hierarchy}}
+\end{figure}
+
+Any charges included in the EnergyCharges category are added together. The EnergyCharges, DemandCharges and ServiceCharges are added together to form the Basis. The Basis, Adjustments and Surcharges are added together to form the Subtotal. The Subtotal and Taxes are added together to be the Total.~ The total represents the total monthly charges on that tariff for the energy source used.~ The combining of categories together is performed automatically unless the user specifies the UtilityCost:Computation.~ In addition, each category, which is also a variable, may be used as a source. For example, a tax that is 5\% of the subtotal would be shown as:
+
+\begin{lstlisting}
+
+UtilityCost:Charge:Simple,
+    TaxOfFivePercent,        ! Charge Variable Name
+    TariffExample1,          ! Tariff Name
+    Subtotal,                ! Source Variable
+    Annual,                  ! Season
+    Taxes,                   ! Category Variable Name
+    0.05;                    ! Cost Per Unit Value (or Variable)
+\end{lstlisting}
+
+As you can see, the UtilityCost:Charge:Simple and UtilityCost:Charge:Block objects do most of the ``work'' of computing the annual energy cost.~ The benefit of using this categorization is that totals of each category are shown in the output reports and it organizes the charges in the monthly calculations in a logical way that fits almost all tariffs.~ If no categorization is desired, theoretically, all charges could be assigned to the Total category. The categories themselves are simply variable names. Charges may also be assigned to the ``NotIncluded'' category if the result of the charge is used as an intermediate calculation and should not be included in the Total.
+
+The objects that create variables are:
+
+\begin{itemize}
+\item
+  UtilityCost:Qualify
+\item
+  UtilityCost:Charge:Simple
+\item
+  UtilityCost:Charge:Block
+\item
+  UtilityCost:Ratchet
+\item
+  UtilityCost:Variable
+\end{itemize}
+
+\subsection{Default Order of Computation}\label{default-order-of-computation}
+
+The user has the option of two different ways to determine the order of computation. If an UtilityCost:Computation object is specified for the tariff, the sequence specified in that object is used for computing the various variables. If no UtilityCost:Computation object is specified, a sequence of computational steps is automatically derived and shown as part of the report. The routine that creates this automatic sequence of computation steps is called CreateDefaultComputation as part of the EconomicTariff module.
+
+The order in which the computation should be made is complicated by the fact that the objects can each have variables that are inputs and others that are outputs.~ Since any of the variables can be used as inputs, we must ensure that they are computed prior to being used. In other words, because the objects allow a great deal of flexibility, there is no simple default order that the computations should be made.
+
+Luckily there are known algorithms for sorting though these types of interdependencies.~ In fact, the method that spreadsheets use for sorting through the dependencies of cell formulas referencing other cells with formula is very similar.~ In addition, linkers (used as part of the computer language compiling process) face similar issues of sorting through dependences. Figuring out the optimal path in a complex project represented by a PERT Chart also uses a similar algorithm.
+
+Generically, dependency problems are usually characterized as Directed Acycle Graphs (DAGs). A DAG shows the individual formulas as circles and uses arrows between the circles to show which formula is dependent on which other formulas.~ One of the simplest explanations can be seen at the following website:
+
+(Click on lecture 14 ``Critical Path'').
+
+The lecture and site was created by Alison Cawsey, Department of Computing and Electrical Engineering, Heriot-Watt University Edinburgh EH14 4AS, UK.~ The specific algorithm that was used in EnergyPlus is described at this site and is quoted below:
+
+Calculate, for each node, the in-degree of that node (ie, now many edges end up there). Store these in array D.
+
+Repeat:
+
+-- Remove (output) node such that D{[}n{]} = 0.
+
+-- Decrement D{[}x{]} for all nodes x that are neighbors of n (edge from n to x).
+
+Of course in this case ``node'' has nothing to do with EnergyPlus nodes but is just describing one of the formulas in a DAG.~ This is just one of several different methods to solve a DAG.~ The general method for solving a DAG is called a topological sort. The algorithm used in EnergyPlus is one of the simplest methods available and is appropriate given the number of dependencies.~ More efficient algorithms are known but are probably only appropriate for much larger number of dependencies.
+
+One important note, if after the algorithm is exercised, and some of the formulas still have a count on the number of dependencies, it must be the result of a circular dependency and an error condition is flagged in the ERR file.
+
+The objects have specific variables that are used as inputs and outputs, and thus the outputs are dependent on the inputs, are shown in the following table:
+
+\textbf{\emph{Object Variables Inputs and Outputs}}
+
+\begin{longtable}[c]{@{}lll@{}}
+\toprule 
+Object & Outputs & Inputs \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Object & Outputs & Inputs \tabularnewline
+\midrule
+\endhead
+
+Qualify & Name & Source \tabularnewline
+~ & ~ & Threshold \tabularnewline
+Charge:Simple & Name & Source \tabularnewline
+~ & Category & Cost Per Unit \tabularnewline
+Charge:Block & Name & Source \tabularnewline
+~ & Category & Block Size Multiplier \tabularnewline
+~ & Remaining & Block Size \tabularnewline
+~ & ~ & Block Cost \tabularnewline
+Ratchet & Name & Baseline \tabularnewline
+~ & ~ & Adjustment \tabularnewline
+~ & ~ & Multiplier \tabularnewline
+~ & ~ & Offset \tabularnewline
+\bottomrule
+\end{longtable}
+
+In addition, the hierarchy shown in the first diagram in this section also represents dependencies that are included when determining the order of computation.
+
+The resulting order of computation is shown at the bottom of the economics report.
+
+\subsection{Computation Steps}\label{computation-steps}
+
+Once the order that the formulas should be computed is known, the actual evaluation of the formulas is based on a simple Last In First Out (LIFO) stack.~ This is a common method to compute expressions where values are stored on the stack and operands work off of the top of the stack.
diff --git a/doc/engineering-reference/src/engineering-reference-encyclopedia.tex b/doc/engineering-reference/src/engineering-reference-encyclopedia.tex
new file mode 100644
index 00000000000..764e0b20caf
--- /dev/null
+++ b/doc/engineering-reference/src/engineering-reference-encyclopedia.tex
@@ -0,0 +1,91 @@
+\chapter{Engineering Reference Encyclopedia}\label{engineering-reference-encyclopedia}
+
+The encyclopedic reference of simulation models is a very large document, and so it is split up into multiple pieces. Here is a quick overview with links to each of the pieces:
+
+\begin{itemize}
+\tightlist
+\item
+  \href{13a-EncyclopaedicRefs.md}{Volume 1}
+\end{itemize}
+
+\begin{lstlisting}
+-   Air Terminals
+-   Boilers
+-   Chillers
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  \href{13b-EncyclopaedicRefs.md}{Volume 2}
+\end{itemize}
+
+\begin{lstlisting}
+-   Ice Thermal Storage
+-   Coils
+-   HVAC Controllers
+-   Baseboard Heaters
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  \href{13c-EncyclopaedicRefs.md}{Volume 3}
+\end{itemize}
+
+\begin{lstlisting}
+-   Cooling Towers
+-   Demand Controlled Ventilation
+-   Evap Coolers
+-   Air System Components
+-   VRF Systems
+-   Heat Exchangers
+-   Humidifiers
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  \href{13d-EncyclopaedicRefs.md}{Volume 4}
+\end{itemize}
+
+\begin{lstlisting}
+-   Zone Internal Gains
+-   Indoor Swimming Pool
+-   Pipes
+-   Pumps
+-   Ideal Load Air Systems
+-   District Heating and Cooling
+-   Central HP
+-   ChillerHeater
+-   Plant Components
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  \href{13e-EncyclopaedicRefs.md}{Volume 5}
+\end{itemize}
+
+\begin{lstlisting}
+-   Radiant System Models
+-   Refrigeration
+-   Setpoint Managers
+-   Solar Collectors
+-   System Availability Managers
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  \href{13f-EncyclopaedicRefs.md}{Volume 6}
+\end{itemize}
+
+\begin{lstlisting}
+-   Thermal Comfort
+-   Trombe Walls
+-   Water Tanks
+-   Water Systems
+-   Zone Controls
+-   Zone Equipment
+\end{lstlisting}
diff --git a/doc/engineering-reference/src/integrated-solution-manager.tex b/doc/engineering-reference/src/integrated-solution-manager.tex
new file mode 100644
index 00000000000..3a1cfa9ea10
--- /dev/null
+++ b/doc/engineering-reference/src/integrated-solution-manager.tex
@@ -0,0 +1,21 @@
+\chapter{Integrated Solution Manager}\label{integrated-solution-manager}
+
+EnergyPlus is an integrated simulation. This means that all three of the major parts, building, system, and plant, must be solved simultaneously. In programs with sequential simulation, such as BLAST or DOE-2, the building zones, air handling systems, and central plant equipment are simulated sequentially with no feedback from one to the other. The sequential solution begins with a zone heat balance that updates the zone conditions and determines the heating/cooling loads at all time steps. This information is fed to the air handling simulation to determine the system response; but that response does not affect zone conditions. Similarly, the system information is passed to the plant simulation without feedback. This simulation technique works well when the system response is a well-defined function of the air temperature of the conditioned space. For a cooling situation, a typical supply and demand situation is shown schematically in the Figure~\ref{fig:sequential-simulation-supplydemand}. Here, the operating point is at the intersection of the supply and demand curves.
+
+\begin{figure}[hbtp] % fig 3
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7.png}
+\caption{Sequential Simulation Supply/Demand Relationship. \protect \label{fig:sequential-simulation-supplydemand}}
+\end{figure}
+
+However, in most situations the system capacity is dependent on outside conditions and/or other parameters of the conditioned space. The simple supply and demand situation above becomes a more complex relationship and the system curve is not fixed. The solution should move up and down the demand curve. This doesn't happen in sequential simulation methods and the lack of feedback from the system to the building can lead to nonphysical results. For example, if the system provides too much cooling to a conditioned space the excess is reported by the program as ``overcooling''. Other categories of unmatched loads exist and are similarly reported by the program. While this kind of reporting enables the affected system or plant components to be properly sized, the system designer would, in most cases, prefer to see the actual change in zone temperature. The same mismatches can occur between the system and plant simulations when they are simulated sequentially.
+
+To obtain a simulation that is physically realistic, the elements have to be linked in a simultaneous solution scheme. The entire integrated program can be represented as a series of functional elements connected by fluid loops as shown in Figure ``Schematic of Simultaneous Solution Scheme''. In EnergyPlus all the elements are integrated and controlled by the Integrated Solution Manager. The loops are divided into supply and demand sides, and the solution scheme generally relies on successive substitution iteration to reconcile supply and demand using the Gauss-Seidell philosophy of continuous updating.
+
+\begin{figure}[hbtp] % fig 4
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image8.png}
+\caption{Schematic of Simultaneous Solution Scheme \protect \label{fig:schematic-of-simultaneous-solution-scheme}}
+\end{figure}
+
+In the sections which follow, the various individual functions of the integrated solution will be described.
diff --git a/doc/engineering-reference/src/integrated-solution-manager/air-system-control.tex b/doc/engineering-reference/src/integrated-solution-manager/air-system-control.tex
new file mode 100644
index 00000000000..df96d243216
--- /dev/null
+++ b/doc/engineering-reference/src/integrated-solution-manager/air-system-control.tex
@@ -0,0 +1,127 @@
+\section{Air System Control}\label{air-system-control}
+
+Previously, the formulation of a new heat balance equation with an unsteady zone capacitance term was discussed Equation . In this equation the updated zone temperature was calculated by removing its explicit dependence from the right hand side and lagging, by one time step, the unknown terms on that side. However, the right hand side still contains implicit dependencies on the zone temperature through the air system control logic; the need for heating or cooling in the zones, is based on zone temperature. In real buildings the control system consists of one or more sensing units in the zone, such as a wall thermostat that samples the air temperature and sends signals to a control unit. The controller looks at the difference between the actual zone temperature and the desired temperature to ascertain if heating or cooling is required and then sends appropriate signals to the air system components to drive the zone temperature closer to the desired value.
+
+Although many control systems use only the zone air temperature to control the air system, most modern energy management systems consider many other variables, such as outside environment conditions. Simulating such controllers would seem to be relatively straightforward in a simulation especially since some of the more complex control problems, such as managing duct pressures and flow rates, are not always modeled. However, real controllers have an advantage because they can sample zone conditions, and thus update air system response, on a time scale much shorter than any characteristic time of the air system or zone. Thus the feedback between zone and air system usually results in steady or, at worst, slowly oscillating zone conditions and air system operation unless the air system is grossly oversized. On the other hand, the numerical model is only able to sample zone conditions at discrete time intervals. In the interest of minimizing computation time, these intervals need to be as long as possible. Frequently, they are of the order of, or longer than, the characteristic times of the air system and zones, except in the case of small air system capacity in relation to zone capacitance. This situation has the potential for unstable feedback between the zone and air system, resulting in an oscillatory or diverging solution.
+
+Prior to implementing the new heat balance method (3rdOrderBackwardDifference) in IBLAST, several air system control strategies were considered. The primary objective was selection of a control method that would be numerically stable over a reasonable range of conditions, realistic from the standpoint of looking and operating like an actual air system controller, and flexible enough to be applied to all current and projected systems. The method actually implemented in IBLAST, and later EnergyPlus, took advantage of the computational model's ``knowledge'' of how much energy enters or leaves the zone as a function of zone air temperature i.e., the zone load. The real controller, on the other hand, does not have this information. The net zone load is given by Equation :
+
+\begin{equation}
+{\dot Q_{load}} = \sum\limits_{i = 1}^{{N_{sl}}} {\dot Q_i^{}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}\left( {{T_{zi}} - {T_z}} \right) + {\dot m_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right)
+\end{equation}
+
+This is Equation without the term due to the air system. In addition, Tz is now the \emph{desired} zone temperature as defined by the control system setpoints that must be specified for each zone. An assumption was made that if the air system has sufficient capacity (based on the desired zone air temperature) to meet the zone conditioning requirements (i.e.~Qsys = Qload) at the desired zone air temperature then those requirements will be met. On the other hand, if the air system cannot provide enough conditioning to the zone to maintain the desired temperature, then the air system provides its maximum output to the zone and the zone air temperature is allowed to ``float.'' Equation was used to calculate the air system output required to maintain the desired zone air temperature; the actual zone temperature update was accomplished using Equation . This method was called \emph{predictive system energy balance}. It has many characteristics of a predictor-corrector method since the air system response is first approximated based on a predicted zone temperature and then the actual change in zone temperature is determined from that air system response. The predictive air system energy balance method required that the system controls on air mass flow rate, supply air temperature, etc., be formulated as a function of the zone air temperature. However, this was not a serious drawback. The first example considered was a single zone draw through air system. Typically, such systems have a cooling coil and heating coil in series, and constant air volume flow rate. Single zone draw through systems run at maximum capacity when turned on; so the only way to regulate net air system output and keep the zone air temperature within the desired range is to turn the air system on and off. A simplified schematic of this system type is shown in Figure~\ref{fig:simplified-single-zone-draw-through-air}. Simplified Single Zone Draw Through Air System.
+
+\begin{figure}[hbtp] % fig 5
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image31.svg.png}
+\caption{Simplified Single Zone Draw Through Air System \protect \label{fig:simplified-single-zone-draw-through-air}}
+\end{figure}
+
+The amount of heating or cooling provided by the air system in relation to the desired zone air temperature is given by:
+
+\begin{equation}
+{\dot Q_{sys}} = {\dot m_{sys}}{C_p}\eta \left( {{T_{\sup }} - {T_{z,\,desired}}} \right)
+\end{equation}
+
+where $\eta$ is the fraction of the time step that the air system is turned on and varies between 0 and 1. The supply air temperature is also implicitly limited by the effectiveness of the coils and the operating parameters of the central plant components. These interactions are discussed later.
+
+A far more complex, though again simplified, air system is the variable air volume (VAV) system, shown in Figure~\ref{fig:simplified-variable-volume-air-system.}. Simplified Variable Volume Air System. In VAV systems, the supply air temperature, as well as the supply air volume, are continuous functions of zone air temperature. As shown in Figure~\ref{fig:idealized-variable-volume-system-operation.}. Idealized Variable Volume System Operation., when the zone air temperature is between T\(_{cl}\) and T\(_{cu}\), cooling is required and the air system varies the supply air flow rate while maintaining a constant supply air temperature. When the zone air temperature is between T\(_{hl}\) and T\(_{hu}\), heating is required and air is supplied at a constant minimum flow rate while the supply air temperature is varied.
+
+\begin{figure}[hbtp] % fig 6
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image33.svg.png}
+\caption{Simplified Variable Volume Air System. \protect \label{fig:simplified-variable-volume-air-system.}}
+\end{figure}
+
+The next figure (Idealized variable volume system operation) shows idealized behavior of a VAV system; in practice, the air flow rate and temperature are not exact linear functions of zone air temperature.
+
+\begin{figure}[hbtp] % fig 7
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image34.svg.png}
+\caption{Idealized Variable Volume System Operation. \protect \label{fig:idealized-variable-volume-system-operation.}}
+\end{figure}
+
+As long as a VAV system has sufficient capacity, the zone air temperatures can be expected to vary within the limits defining the range of operation of the air damper, when cooling, or the throttling range of the reheat coil, when the air system is heating. This means that the desired zone air temperature, used to predict the air system response, is variable and must be calculated in order to determine the air system output. For the purposes of this calculation, the following definitions were found useful:
+
+\begin{equation}
+{\dot Q_0} = \sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}} + {\dot m_{\inf }}{C_p}{T_\infty }
+\end{equation}
+
+\begin{equation}
+{\dot Q_{slope}} = \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {\dot m_{\inf }}{C_p}
+\end{equation}
+
+Equations and are derived, respectively, from the numerator and denominator of Equation but with the system related terms omitted. Also excluded from these expressions are the effects of zone capacitance.
+
+When a zone requires cooling, the VAV system is designed to provide air to that zone at a constant supply air temperature. The amount of cooling is matched to the load by dampers in the supply air duct that vary the air volume flow rate of being supplied to the zone. Assuming that the volume flow rate varies linearly with zone air temperature, the volume flow rate of supply air normalized to the maximum flow rate, or supply air fraction, is given by:
+
+\begin{equation}
+{\eta_c} = {\eta_{c,\,\min }} + \left( {1 - {\eta_{c,\,\min }}} \right)\left( {\frac{{{T_z} - {T_{c,\,lower}}}}{{{T_{c,\,upper}} - {T_{c,\,lower}}}}} \right);\,{\eta_{c,\,\min }} \le {\eta_c} \le 1.0
+\end{equation}
+
+Normally, the minimum supply air fraction $\eta$\(_{c,min}\) must be greater than zero to ensure a supply of fresh air sufficient to eliminate contaminants from the zone.
+
+Conversely, when heating is required in a zone, the VAV system becomes a constant volume flow rate system with a variable supply air temperature. The dampers are set to provide air to the zone at the minimum supply air fraction. Throttling the hot water supply to the reheat coil, which effectively alters the coil's heating capacity, modulates the supply air temperature. Again, assuming the heat energy output varies linearly with zone air temperature and normalizing with respect to the maximum coil output gives the following result:
+
+\begin{equation}
+{\eta_h} = \left( {\frac{{{T_{h,\,upper}} - {T_z}}}{{{T_{h,\,upper}} - {T_{h,\,lower}}}}} \right);\,0 \le {\eta_h} \le 1.0
+\end{equation}
+
+Observe that when $\eta$\(_{h}\) is equal to zero, the zone is supplied with air at the cooling coil outlet temperature at the minimum air fraction. Because the control strategies of the VAV system are different whether the air system is heating or cooling, two equations are necessary to describe the air system output in terms of $\eta$\(_{h}\) and $\eta$\(_{c}\). These expressions are as shown in Equations and :
+
+\begin{equation}
+{\dot Q_{sys,h}} = {\eta_h}{\dot Q_{h/c,\,\max }} + {C_p}\rho {\dot V_{\min }}\left( {{T_{c/c}} - {T_{z,pred,heat}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{sys,c}} = {C_p}\rho \left( {{\eta_c}{{\dot V}_{\max }}} \right)\left( {{T_{c/c}} - {T_{z,pred,cool}}} \right)
+\end{equation}
+
+Equation is valid for zone air temperatures below T\(_{h,upper}\), while Equation is valid for all temperatures above this value. Equating the system output to the zone load, as given by Equation , the definitions of $\eta$\(_{c}\) and $\eta$\(_{h}\) were then used to develop expressions for the predicted zone air temperature in the cases of heating and cooling:
+
+\begin{equation}
+{T_{z,pred,heat}} = \frac{{{{\dot Q}_{h/c,\max }}{T_{h,upper}}}}{{{T_{h,upper}} - {T_{h,lower}}}} + {\dot Q_0} + \frac{{{C_p}\rho {{\dot V}_{\min }}{T_{c/c}}}}{{\frac{{{{\dot Q}_{h/c,\max }}}}{{{T_{h,upper}} - {T_{h,lower}}}} + {C_p}\rho {{\dot V}_{\min }} + {{\dot Q}_{slope}}}}
+\end{equation}
+
+\begin{equation}
+{T_{z,pred,cool}} = \frac{{{B_1} + \sqrt {B_1^2 + {B_2}} }}{2}
+\end{equation}
+
+where,
+
+\begin{equation}
+{B_1} = {T_{c/c}} + {T_{c,lower}} - \frac{{{\eta_{c,\min }} - {C_2}}}{{{C_1}}}
+\end{equation}
+
+\begin{equation}
+{B_2} = 4\left( {\frac{{{C_3}}}{{{C_1}}} + {T_{c/c}}\left( {\frac{{{\eta_{c,\min }}}}{{{C_1}}} - {T_{c,lower}}} \right)} \right)
+\end{equation}
+
+and,
+
+\begin{equation}
+{C_1} = \frac{{1 - {\eta_{c,\min }}}}{{{T_{c,upper}} - {T_{c,lower}}}}
+\end{equation}
+
+\begin{equation}
+{C_2} = \frac{{{{\dot Q}_{slope}}}}{{{C_p}\rho {{\dot V}_{\max }}}}
+\end{equation}
+
+\begin{equation}
+{C_3} = \frac{{{{\dot Q}_0}}}{{{C_p}\rho {{\dot V}_{\max }}}}
+\end{equation}
+
+Once the predicted zone air temperature has been calculated from Equations and , the air system response may be determined. When a zone requires cooling the system supply air temperature is constant at the cooling coil outlet temperature and the volume flow rate is given by:
+
+\begin{equation}
+{\dot V_{\sup ply}} = {\eta_c}{\dot V_{\max }}
+\end{equation}
+
+where the supply air fraction $\eta$\(_{c}\) is computed from Equation . When heating is required by the zone, the air system provides air at the minimum volume flow rate and at a temperature given by:
+
+\begin{equation}
+{T_{\sup ply}} = {T_{c/c}} + \frac{{{\eta_h}{{\dot Q}_{h/c,\max }}}}{{{C_p}\rho {{\dot V}_{\min }}}}
+\end{equation}
+
+The reheat coil capacity fraction $\eta$\(_{h}\) is determined by using Equation . Once Equation or , has been used, the supply air flow rate and temperature are known. These values are then used in Equation to calculate the updated zone air temperature. The equations describing VAV system operation may be solved without iteration if the cooling coil outlet temperature is constant, i.e.~if the coil has infinite capacity, and if the reheat coil capacity varies linearly with zone air temperature. This is not the case, either in practice or in simulations, when realistic coil models are used. Therefore, an iteration scheme was developed that solved these equations simultaneously with the coil performance models.
diff --git a/doc/engineering-reference/src/integrated-solution-manager/basis-for-the-zone-and-air-system-integration.tex b/doc/engineering-reference/src/integrated-solution-manager/basis-for-the-zone-and-air-system-integration.tex
new file mode 100644
index 00000000000..a4a6f080899
--- /dev/null
+++ b/doc/engineering-reference/src/integrated-solution-manager/basis-for-the-zone-and-air-system-integration.tex
@@ -0,0 +1,124 @@
+\section{Basis for the Zone and Air System Integration}\label{basis-for-the-zone-and-air-system-integration}
+
+The basis for the zone and air system integration is to formulate energy and moisture balances for the zone air and solve the resulting ordinary differential equations using a predictor-corrector approach. The formulation of the solution scheme starts with a heat balance on the zone air.
+
+\begin{equation}
+{C_z}\frac{{d{T_z}}}{{dt}} = \sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}\left( {{T_{zi}} - {T_z}} \right)\, + {\dot m_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right) + {\dot Q_{sys}}
+\end{equation}
+
+where:
+
+\(\sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}\) = sum of the convective internal loads
+
+\(\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right)\) = convective heat transfer from the zone surfaces
+
+\({\dot m_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right)\) = heat transfer due to infiltration of outside air
+
+\(\sum_{i = 1}^{N_{zones}} \dot m_i C_p\left( T_{zi} - {T_z} \right)\) = heat transfer due to interzone air mixing
+
+\({\dot Q_{sys}}\) = air systems output
+
+${C_z}\frac{dT_z}{dt} =$ energy stored in zone air
+
+C\(_{z}\) = $\rho$\(_{air}\)C\(_{p}\)C\(_{T}\)
+
+$\rho$\(_{air}\) = zone air density
+
+C\(_{p}\) = zone air specific heat
+
+C\(_{T}\) = sensible heat capacity multiplier (Detailed description is provided below)
+
+If the air capacitance is neglected, the steady-state system output must be:
+
+\begin{equation}
+- {\dot Q_{sys}} = \sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}\left( {{T_{zi}} - {T_z}} \right)\, + {\dot m_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right)
+\end{equation}
+
+Air systems provide hot or cold air to the zones to meet heating or cooling loads. The system energy provided to the zone, Qsys, can thus be formulated from the difference between the supply air enthalpy and the enthalpy of the air leaving the zone as in Equation :
+
+\begin{equation}
+{\dot Q_{sys}} = {\dot m_{sys}}{C_p}\left( {{T_{\sup }} - {T_z}} \right)
+\end{equation}
+
+This equation assumes that the zone supply air mass flow rate is exactly equal to the sum of the air flow rates leaving the zone through the system return air plenum and being exhausted directly from the zone. Both air streams exit the zone at the zone mean air temperature. The result of substituting Equation for Qsys in the heat balance Equation is shown in Equation :
+
+\begin{equation}
+\begin{array}{ll}
+    {C_z}\frac{{d{T_z}}}{{dt}} & = \sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}\left( {{T_{zi}} - {T_z}} \right) \\
+                               &+ {{\dot m}_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right) + {{\dot m}_{sys}}{C_p}\left( {{T_{\sup }} - {T_z}} \right)
+  \end{array}
+\end{equation}
+
+The sum of zone loads and air system output now equals the change in energy stored in the zone. Typically, the capacitance Cz would be that of the zone air only. However, thermal masses assumed to be in equilibrium with the zone air could be included in this term.
+
+EnergyPlus provides three different solution algorithms to solve the zone air energy and moisture balance equations. These are defined in the Algorithm field in the ZoneAirHeatBalanceAlgorithm object: 3rdOrderBackwardDifference, EulerMethod and AnalyticalSolution. The first two methods to solve Equation use the finite difference approximation while the third uses an analytical solution. A short description is given below.
+
+In order to calculate the derivative term with respect to time, a finite difference approximation may be used, such as:
+
+\begin{equation}
+\frac{{dT}}{{dt}} = {\left( {\delta t} \right)^{ - 1}}\left( {{T_z}^t - {T_z}^{t - \delta t}} \right) + {\rm O}\left( {\delta t} \right)
+\end{equation}
+
+The use of numerical integration in a long time simulation is a cause for some concern due to the potential build-up of truncation error over many time steps. In this case, the finite difference approximation is of low order that further aggravates the problem. However, the cyclic nature of building energy simulations should cause truncation errors to cancel over each daily cycle so that no net accumulation of error occurs, even over many days of simulation (Walton, 1990). The Euler formula, Equation , was employed in Equation to replace the derivative term. All the terms containing the zone mean air temperature were then grouped on the left hand side of the equation. Since the remaining terms are not known at the current time, they were lagged by one time step and collected on the right hand side. This manipulation resulted in Equation , the formula for updating the zone mean air temperature:
+
+\begin{equation}
+\begin{array}{l}{C_z}\frac{{T_z^t - T_z^{t - \delta t}}}{{dt}} + T_z^t\left( {\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}{C_p}} \right) = \\\sum\limits_{i = 1}^{{N_{sl}}} {\dot Q_i^t}  + {{\dot m}_{sys}}{C_p}T_{{\rm{supply}}}^t + {\left( {\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}} + {{\dot m}_{\inf }}{C_p}{T_\infty }} \right)^{t - \delta t}}\end{array}
+\end{equation}
+
+One final rearrangement was to move the lagged temperature in the derivative approximation to the right side of the equation. The explicit appearance of the zone air temperature was thus eliminated from one side of the equation. An energy balance equation that includes the effects of zone capacitance was then obtained by dividing both sides by the coefficient of Tz:
+
+\begin{equation}
+T_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {\dot Q_i^t}  + {{\dot m}_{sys}}{C_p}T_{{\rm{supply}}}^t + {{\left( {{C_z}\frac{{T_z^{}}}{{\delta t}} + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}} + {{\dot m}_{\inf }}{C_p}{T_\infty }} \right)}^{t - \delta t}}}}{{\frac{{{C_z}}}{{\delta t}} + \left( {\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}{C_p}} \right)}}
+\end{equation}
+
+Equation could be used to estimate zone air temperatures, and is defined as the EulerMethod, one of the three solution algorithms provided in the ZoneAirHeatBalanceAlgorithm object. However, it can severely limit the time step size under some conditions. To improve on this, higher order expressions for the first derivative, with corresponding higher-order truncation errors, were developed. The goal of this approach was to allow for the use of larger time steps in the simulation than would be possible using the first order Euler form, without experiencing instabilities. Approximations from second through fifth order were tried as reported by Taylor, et al. (1990) with the conclusion that the third order finite difference approximation, shown below, gave the best results:
+
+\begin{equation}
+{\left. {\frac{{d{T_z}}}{{dt}}} \right|_t} \approx {\left( {\delta t} \right)^{ - 1}}\left( {\frac{{11}}{6}T_z^t - 3T_z^{t - \delta t} + \frac{3}{2}T_z^{t - 2\delta t} - \frac{1}{3}T_z^{t - 3\delta t}} \right) + O\left( {\delta {t^3}} \right)
+\end{equation}
+
+When this form for the derivative is used, equation changes to:
+
+\begin{equation}
+\begin{array}{l}
+{C_z}{\left( {\delta t} \right)^{ - 1}}\left( {\frac{{11}}{6}T_z^t - 3T_z^{t - \delta t} + \frac{3}{2}T_z^{t - 2\delta t} - \frac{1}{3}T_z^{t - 3\delta t}} \right) = \sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right) \\
+\quad \quad \quad \quad + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}\left( {{T_{zi}} - {T_z}} \right) + {{\dot m}_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right) + {{\dot m}_{sys}}{C_p}\left( {{T_{\sup }} - {T_z}} \right)
+\end{array}
+\end{equation}
+
+and the zone temperature update equation becomes:
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+T_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}}\, + {{\dot m}_{\inf }}{C_p}{T_\infty } + {{\dot m}_{sys}}{C_p}{T_{{\rm{supply}}}} - \left( {\frac{{{C_z}}}{{\delta t}}} \right)\left( { - 3T_z^{t - \delta t} + \frac{3}{2}T_z^{t - 2\delta t} - \frac{1}{3}T_z^{t - 3\delta t}} \right)}}{{\left( {\frac{{11}}{6}} \right)\frac{{{C_z}}}{{\delta t}} + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} A + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}C}}
+\end{equation}
+
+This is the form historically used in EnergyPlus and is the current default referred to as 3rdOrderBackwardDifference in the ZoneAirHeatBalanceAlgorithm object. This algorithm requires zone air temperatures at three previous time steps and uses constant temperature coefficients. The assumption is that three previous time steps lengths are the same.
+
+The AnalyticalSolution algorithm is an integration approach. While the 3\(^{rd}\) order finite difference approximation provides stability without requiring a prohibitively small time step, the method still has truncation errors and requires a fixed time step length for the previous three simulation time steps. Therefore, different time step lengths for the previous three simulation time steps may make the temperature coefficients invalid.
+
+The AnalyticalSolution algorithm provides a possible way to obtain solutions without truncation errors and independent of time step length. In addition, the algorithm only requires the zone air temperature for one previous time step, instead of three previous time steps as required by the 3rdOrderBackwardDifference algorithm. The integrated (analytical) solution for Eq. (4) may be expressed as follows:
+
+\begin{equation}
+\begin{array}{l}T_z^t = \left( {T_z^{t - \delta t} - \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}} + {{\dot m}_{\inf }}{C_p}{T_\infty } + {{\dot m}_{sys}}{C_p}{T_{\sup }}}}{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}{C_p}}}} \right)\\\;\;\;\;\;\;\;*\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}{C_p}}}{{{C_z}}}\delta t} \right)\\\;\;\;\;\;\;\; + \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}} + {{\dot m}_{\inf }}{C_p}{T_\infty } + {{\dot m}_{sys}}{C_p}{T_{\sup }}}}{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}{C_p}}}\end{array}
+\end{equation}
+
+Since the load on the zone drives the entire process, that load is used as a starting point to give a demand to the air system. Then a simulation of the air system provides the actual supply capability and the zone temperature is adjusted if necessary. This process in EnergyPlus is referred to as a Predictor/Corrector process. It is summarized below.
+
+Code Reference: the \textbf{ZoneTempPredictorCorrector} module performs the calculations.
+
+\subsection{Zone Sensible Heat Capacity Multiplier}\label{zone-sensible-heat-capacity-multiplier}
+
+If the Zone Sensible Heat Capacity Multiplier = 1.0, this represents just the sensible heat capacitance of the air volume in the specified zone. If the value is not defined, it is set to 1.0. This multiplier can be greater than 1.0 if the zone air sensible heat capacity needs to be increased for stability of the simulation. This multiplier increases the capacitance of the air volume by increasing the zone volume that is used in the zone predictor-corrector algorithm in the simulation. This can be done for numerical reasons, such as to increase the stability by decreasing the zone air temperature deviations at the time step level. Or it can be increased to try and account for the additional capacitance in the air loop not specified in the zone, i.e.~dampers, diffusers, duct work, etc., to see the effect on the dynamics of the simulation. See the Input/Output Reference for additional information (Object: ZoneCapacitanceMultiplier:ResearchSpecial).
+
+In the source code below we see how the ZoneVolCapMultpSens increases the zone volume used for the air ratio at the time step in the air system. This multiplier is constant throughout the simulation.
+
+\begin{lstlisting}
+    AIRRAT(ZoneNum) = Zone(ZoneNum)%Volume\***ZoneVolCapMultpSens**\* &
+               PsyRhoAirFnPbTdbW(OutBaroPress,MAT(ZoneNum),ZoneAirHumRat(ZoneNum))\* &
+               PsyCpAirFnWTdb(ZoneAirHumRat(ZoneNum),MAT(ZoneNum))/(TimeStepSys\*SecInHour)
+\end{lstlisting}
diff --git a/doc/engineering-reference/src/integrated-solution-manager/carbon-dioxide-predictor-corrector.tex b/doc/engineering-reference/src/integrated-solution-manager/carbon-dioxide-predictor-corrector.tex
new file mode 100644
index 00000000000..306527afe11
--- /dev/null
+++ b/doc/engineering-reference/src/integrated-solution-manager/carbon-dioxide-predictor-corrector.tex
@@ -0,0 +1,156 @@
+\section{Carbon Dioxide Predictor-Corrector}\label{carbon-dioxide-predictor-corrector}
+
+The transient air mass balance equation for the change in zone air carbon dioxide concentration may be expressed as follows:
+
+\begin{equation}
+\begin{array}{l}
+{\rho_{air}}{V_z}{C_{CO2}}\frac{{dC_z^t}}{{dt}} = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{zi}} - C_z^t} \right)\; + {\dot m_{\inf }}\left( {{C_\infty } - C_z^t} \right) \\
+\quad \quad \quad \quad + {\dot m_{sys}}\left( {{C_{\sup }} - C_z^t} \right)
+\end{array}
+\end{equation}
+
+where:
+
+\(\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}\) = sum of scheduled internal carbon dioxide loads. The zone air density is used to convert the volumetric rate of carbon dioxide generation from user input into mass generation rate {[}kg/s{]}.The coefficient of 10\(^{6}\) is used to make the units of carbon dioxide as ppm.
+
+\(\sum_{i = 1}^{N_{zones}} \dot m_i \left( C_{zi} - C_z^t \right)\) = carbon dioxide transfer due to interzone air mixing {[}ppm-kg/s{]}
+
+\({C_{zi}}\) = carbon dioxide concentration in the zone air being transferred into this zone {[}ppm{]}
+
+\({\dot m_{\inf }}\left( {{C_\infty } - C_z^t} \right)\) = carbon dioxide transfer due to infiltration and ventilation of outdoor air {[}ppm-kg/s{]}
+
+\({C_\infty }\) = carbon dioxide concentration in outdoor air {[}ppm{]}
+
+\({\dot m_{sys}}\left( {{C_{\sup }} - C_z^t} \right)\) = carbon dioxide transfer due to system supply {[}ppm-kg/s{]}
+
+\({C_{\sup }}\) = carbon dioxide concentration in the system supply airstream {[}ppm{]}
+
+\({\dot m_{sys}}\) = air system supply mass flow rate {[}kg/s{]}
+
+\({\rho_{air}}{V_z}\frac{{dC_z^t}}{{dt}}\) = carbon dioxide storage term in zone air {[}kg/s{]}
+
+\(C_z^t\) = zone air carbon dioxide concentration at the current time step {[}ppm{]}
+
+\({\rho_{air}}\) = zone air density {[}kg/m\(^{3}\){]}
+
+\({V_z}\) = zone volume {[}m\(^{3}\){]}
+
+C\(_{CO2}\) = carbon dioxide capacity multiplier {[}dimensionless{]} (See the InputOutput Reference for additional information on the object ZoneCapacitanceMultiplier:ResearchSpecial)
+
+In the same manner as described above for zone air temperature (ref. Basis for the Zone and Air System Integration), the solution algorithms provided in the ZoneAirHeatBalanceAlgorithm object are also applied to the zone air carbon dioxide calculations.
+
+In order to calculate the derivative term with respect to time, the first order backward finite difference method, defined as the EulerMethod in the ZoneAirHeatBalanceAlgorithm object, may be used:
+
+\begin{equation}
+\frac{{dC_z^t}}{{dt}} = {\left( {\delta t} \right)^{ - 1}}(C_z^t - C_z^{t - \delta t}) + O(\delta t)
+\end{equation}
+
+The zone air carbon dioxide concentration update at the current time step using the EulerMethod may be expressed as follows:
+
+\begin{equation}
+\begin{array}{l}
+{\rho_{air}}{V_Z}{C_{CO2}}{\left( {\delta t} \right)^{ - 1}}\left( {C_z^t - C_z^{t - \delta t}} \right) = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}} *{10^6} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{zi}} - C_z^t} \right) \\
+\quad \quad \quad \quad + {\dot m_{\inf }}\left( {{C_\infty } - C_z^t} \right) + {\dot m_{sys}}\left( {{C_{\sup }} - C_z^t} \right)
+\end{array}
+\end{equation}
+
+To preserve the stability of the calculation of the zone carbon dioxide concentration, the third order differential approximation, derived by a Taylor Series and used in the calculation of the next time step's zone air temperature, is also applied to the zone air carbon dioxide calculations. This algorithm is the default choice and is defined as ThirdOrderBackwardDifference in the ZoneAirHeatBalanceAlgorithm object.
+
+The third order derivative derived from a Taylor Series expansion is defined as:
+
+\begin{equation}
+\frac{{dC_z^t}}{{dt}} \approx \frac{{\frac{{11}}{6}C_z^t - 3C_z^{t - \delta t} + \frac{3}{2}C_z^{t - 2\delta t} - \frac{1}{3}C_z^{t - 3\delta t}}}{{\delta t}} + O(\delta {t^3})
+\end{equation}
+
+The coefficients of the approximated derivative are very close to the coefficients of the analogous Adams-Bashforth algorithm. Then the approximated derivative is substituted into the mass balance and the terms with the carbon dioxide concentration at past time steps are all put on the right-hand side of the equation. This third order derivative zone carbon dioxide update increases the number of previous time steps that are used in calculating the new zone carbon dioxide concentration, and decreases the dependence on the most recent. The higher order derivative approximations have the potential to allow the use of larger time steps by smoothing transitions through sudden changes in zone operating conditions.
+
+\begin{equation}
+\begin{array}{l}\frac{{{\rho_{air}}{V_z}{C_{CO2}}}}{{\delta t}}\left( {\frac{{11}}{6}} \right)C_z^t + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} C_z^t + {{\dot m}_{\inf }}C_z^t + {{\dot m}_{sys}}C_z^t = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}} *{10^6}\\\;\;\;\;\;\;\; + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}} + {{\dot m}_{\inf }}{C_\infty } + {{\dot m}_{sys}}{C_{\sup }} - \frac{{{\rho_{air}}{V_z}{C_{CO2}}}}{{\delta t}}( - 3C_z^{t - \delta t} + \frac{3}{2}C_z^{t - 2\delta t} - \frac{1}{3}C_z^{t - 3\delta t})\end{array}
+\end{equation}
+
+This gives us the basic air mass balance equation that will be solved two different ways, one way for the predict step and one way for the correct step.
+
+Since the third choice of solution algorithms uses an integration approach, defined as AnalyticalSolution in the ZoneAirHeatBalanceAlgorithm object, it does not require any approximations and has no truncation errors. The solutions in both prediction and correction are provided below in detail.
+
+\subsection{Carbon Dioxide Prediction}\label{carbon-dioxide-prediction}
+
+For the carbon dioxide concentration prediction case, the equation is solved for the anticipated system response as shown below.
+
+\begin{equation}
+{\rm{PredictedSystemLoad}} = {\dot m_{sys}}\left( {{C_{\sup }} - C_z^t} \right)
+\end{equation}
+
+Since the program provides three solution algorithms, the carbon dioxide prediction from each solution algorithm is given below.
+
+\subsubsection{EulerMethod}\label{eulermethod}
+
+For this solution algorithm, the air mass balance for the predicted air system load or response is:
+
+\begin{equation}
+\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = {\rho_{air}}{V_Z}{C_{CO2}}{\left( {\delta t} \right)^{ - 1}}\left( {C_{{\rm{setpoint}}}^t - C_z^{t - \delta t}} \right)\\\;\;\;\; - \left[ {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}} *{{10}^6} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{zi}} - C_{{\rm{setpoint}}}^t} \right) + {{\dot m}_{\inf }}\left( {{C_\infty } - C_{{\rm{setpoint}}}^t} \right)} \right]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\end{array}
+\end{equation}
+
+\subsubsection{ThirdOrderBackwardDifference}\label{thirdorderbackwarddifference}
+
+For this solution algorithm, the air mass balance for the predicted system load or response is given below:
+
+\begin{equation}
+\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = \left[ {\frac{{{\rho_{air}}{V_z}{C_{CO2}}}}{{\delta t}}\left( {\frac{{11}}{6}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }}} \right]*C_{{\rm{setpoint}}}^t\\\;\;\;\; - \left[ {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}} + {{\dot m}_{\inf }}{C_\infty } + \frac{{{\rho_{air}}{V_z}{C_{CO2}}}}{{\delta t}}\left( {3C_z^{t - \delta t} - \frac{3}{2}C_z^{t - 2\delta t} + \frac{1}{3}C_z^{t - 3\delta t}} \right)} \right]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\end{array}
+\end{equation}
+
+\subsubsection{AnalyticalSolution}\label{analyticalsolution}
+
+For this solution algorithm, the air mass balance for the predicted air system load or response is given below:
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = \left[ {\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }}} \right]*\;\left[ {C_{{\rm{setpoint}}}^t - C_z^{t - \delta t}*\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }}}}{{{\rho_{air}}{V_Z}{C_{CO2}}}}\delta t} \right)} \right]*\\\;\;\;{\left[ {1 - \exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }}}}{{{\rho_{air}}{V_Z}{C_{CO2}}}}\delta t} \right)} \right]^{ - 1}} - \;\left( {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}}\; + {{\dot m}_{\inf }}{C_\infty }} \right)\end{array}
+\end{equation}
+
+At the prediction point in the simulation, the system air mass flows are not known; therefore, the system response is approximated. The predicted air system carbon dioxide load is then used in the system simulation to achieve the best results possible. If a central HVAC system provides the outdoor flow rate from a Controller:MechanicalVentilation object, the outdoor airflow rate may be approximated as:
+
+\begin{equation}
+{\rm{PredictedSystemLoad}} = {\dot m_{sys}}\left( {{C_{\sup }} - C_z^t} \right) \approx {\dot m_{OA,z}}\left( {{C_\infty } - C_{{\rm{setpoint}}}^t} \right)
+\end{equation}
+
+where:
+
+\({\dot m_{OA,z}}\) = supply outdoor airflow rate into the controlled zone {[}kg/s{]}
+
+The above approximation is based on the assumption that the carbon dioxide concentration at the outdoor air (OA) mixer inlet is equal to the zone air outlet concentration level, and the carbon dioxide level at the zone supply air inlet is equal to the level at the outlet node of the OA mixer.
+
+After the system simulation is completed the actual response from the air system is used in the carbon dioxide correction step, which is shown next.
+
+\subsection{Carbon Dioxide Correction}\label{carbon-dioxide-correction}
+
+For the correct step the expanded air mass balance equation is solved for the final zone carbon dioxide concentration at the current time step. In the same manner as described above for predicting the carbon dioxide load to be met by the air system, the zone air carbon dioxide correction calculation will be described individually for the three solution algorithms.
+
+\subsubsection{EulerMethod}\label{eulermethod-1}
+
+\begin{equation}
+C_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}} + {{\dot m}_{\inf }}{C_\infty } + {{\dot m}_{sys}}{C_{\sup }} + {\rho_{air}}{V_Z}{C_{CO2}}\frac{{C_z^{t - \delta t}}}{{\delta t}}}}{{\frac{{{\rho_{air}}{V_Z}{C_{CO2}}}}{{\delta t}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}
+\end{equation}
+
+\subsubsection{ThirdOrderBackwardDifference}\label{thirdorderbackwarddifference-1}
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+C_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}} + {{\dot m}_{\inf }}{C_\infty } + {{\dot m}_{sys}}{C_{\sup }} + \frac{{{\rho_{air}}{V_Z}{C_{CO2}}}}{{\delta t}}(3C_z^{t - \delta t} - \frac{3}{2}C_z^{t - 2\delta t} + \frac{1}{3}C_z^{t - 3\delta t})}}{{\frac{{{\rho_{air}}{V_Z}{C_{CO2}}}}{{\delta t}}\left( {\frac{{11}}{6}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}
+\end{equation}
+
+\subsubsection{AnalyticalSolution}\label{analyticalsolution-1}
+
+\begin{equation}
+\begin{array}{l}C_z^t = \left[ {C_z^{t - \delta t} - \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}}\; + {{\dot m}_{\inf }}{C_\infty } + {{\dot m}_{sys}}{C_{sys}}}}{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}} \right]*\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}{{{\rho_{air}}{V_Z}{C_{CO2}}}}\delta t} \right) \\
+\;\;\; + \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}}\; + {{\dot m}_{\inf }}{C_\infty } + {{\dot m}_{sys}}{C_{sys}}}}{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}\end{array}
+\end{equation}
+
+The above solutions are implemented in the Correct Zone Air Carbon Dioxide step in the Zone Contaminant Predictor Corrector module of EnergyPlus.
diff --git a/doc/engineering-reference/src/integrated-solution-manager/generic-contaminant-predictor-corrector.tex b/doc/engineering-reference/src/integrated-solution-manager/generic-contaminant-predictor-corrector.tex
new file mode 100644
index 00000000000..d1a8392625c
--- /dev/null
+++ b/doc/engineering-reference/src/integrated-solution-manager/generic-contaminant-predictor-corrector.tex
@@ -0,0 +1,159 @@
+\section{Generic Contaminant Predictor-Corrector}\label{generic-contaminant-predictor-corrector}
+
+The transient air mass balance equation for the change in zone air generic contaminant concentration may be expressed as follows:
+
+\begin{equation}
+\begin{array}{l}{\rho_{air}}{V_z}{M_{for}}\frac{{dC_{f,z}^t}}{{dt}} = \sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6} - } {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}{C_{f,z}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{f,z,i}} - C_{f,z}^t} \right) \\
+\quad \quad \quad + {{\dot m}_{\inf }}\left( {{C_{f,\infty }} - C_{f,z}^t} \right) + {{\dot m}_{sys}}\left( {{C_{f,\sup }} - C_{f,z}^t} \right) + \sum\limits_j {{h_j}\rho {A_j}(\frac{{{C_{s,j}}}}{{{k_j}}} - {C_{f,z}})}  + {S_f}(C_{f,z}^{t - \delta t})\end{array}
+\end{equation}
+
+where:
+
+\(\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}}\) = Sum of internal generic contaminant loads from sources in a zone or interior surfaces.
+
+The zone air density is used to convert the volumetric rate of generic contaminant generation from user input into mass generation rate {[}kg/s{]}.The coefficient of 10\(^{6}\) is used to make the units of generic contaminant as ppm.
+
+\({\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}{C_{f,z}}}\) = Sum of removal rate from sinks in a zone or interior surfaces {[}ppm-kg/s{]}
+
+\(\sum_{i = 1}^{N_{zones}} \dot m_i \left( C_{f,z,i} - C_{f,z}^t \right)\) = Generic contaminant transfer due to interzone air mixing {[}ppm-kg/s{]}
+
+\({C_{f,z,i}}\) = Generic contaminant concentration in the zone air being transferred into this zone {[}ppm{]}
+
+\({\dot m_{\inf }}\left( {{C_{f,\infty }} - C_{f,z}^t} \right)\) = Generic contaminant transfer due to infiltration and ventilation of outdoor air {[}ppm-kg/s{]}
+
+\({C_{f,\infty }}\) = Generic contaminant concentration in outdoor air {[}ppm{]}
+
+\({\dot m_{sys}}\left( {{C_{f,\sup }} - C_{f,z}^t} \right)\) = Generic contaminant transfer due to system supply {[}ppm-kg/s{]}
+
+\({C_{f,\sup }}\) = Generic contaminant concentration in the system supply airstream {[}ppm{]}
+
+\({\dot m_{sys}}\) = Air system supply mass flow rate {[}kg/s{]}
+
+\({\rho_{air}}{V_z}\frac{{dC_{f,z}^t}}{{dt}}\) = Generic contaminant storage term in zone air {[}ppm-kg/s{]}
+
+\(C_{f,z}^t\) = Zone air generic contaminant concentration at the current time step {[}ppm{]}
+
+\({\rho_{air}}\) = Zone air density {[}kg/m\(^{3}\){]}
+
+\({V_z}\) = Zone volume {[}m\(^{3}\){]}
+
+\(\sum\limits_j {{h_j}\rho {A_j}(\frac{{{C_{s,j}}}}{{{k_j}}} - {C_{f,z}})}\) = Generic contaminant transport through diffusion between interior surfaces and zone air
+
+\({S_f}(C_{f,z}^{t - \delta t})\) = Generic contaminant generation or removal rate as a function of zone air generic contaminant level at the previous time step
+
+Mfor = Generic contaminant capacity multiplier {[}dimensionless{]} (See the InputOutput Reference for additional information on the object ZoneCapacitanceMultiplier:ResearchSpecial)
+
+In the same manner as described above for zone air temperature (ref. Basis for the Zone and Air System Integration), the solution algorithms provided in the ZoneAirHeatBalanceAlgorithm object are also applied to the zone air carbon dioxide calculations.
+
+In order to calculate the derivative term with respect to time, the first order backward finite difference method, defined as the EulerMethod in the ZoneAirHeatBalanceAlgorithm object, may be used:
+
+\begin{equation}
+\frac{{dC_{f,z}^t}}{{dt}} = {\left( {\delta t} \right)^{ - 1}}(C_{f,z}^t - C_{f,z}^{t - \delta t}) + O(\delta t)
+\end{equation}
+
+The zone air generic contaminant concentration update at the current time step using the EulerMethod may be expressed as follows:
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+\begin{array}{l}{\rho_{air}}{V_z}{M_{for}}{\left( {\delta t} \right)^{ - 1}}\left( {C_{f,z}^t - C_{f,z}^{t - \delta t}} \right) = \sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6} - } {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}{C_{f,z}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{f,z,i}} - C_{f,z}^t} \right)\;\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; + {{\dot m}_{\inf }}\left( {{C_{f,\infty }} - C_{f,z}^t} \right) + {{\dot m}_{sys}}\left( {{C_{f,\sup }} - C_{f,z}^t} \right) + \sum\limits_j {{h_j}\rho {A_j}(\frac{{{C_{s,j}}}}{{{k_j}}} - {C_{f,z}})}  + {S_f}\end{array}
+\end{equation}
+
+To preserve the stability of the calculation of the zone generic contaminant concentration, the third order differential approximation, derived by a Taylor Series and used in the calculation of the next time step's zone air temperature, is also applied to the zone air carbon dioxide calculations. This algorithm is the default choice and is defined as ThirdOrderBackwardDifference in the ZoneAirHeatBalanceAlgorithm object.
+
+The third order derivative resulting from a Taylor Series expansion is defined as:
+
+\begin{equation}
+\frac{{dC_{f,z}^t}}{{dt}} \approx \frac{{\frac{{11}}{6}C_{f,z}^t - 3C_{f,z}^{t - \delta t} + \frac{3}{2}C_{f,z}^{t - 2\delta t} - \frac{1}{3}C_{f,z}^{t - 3\delta t}}}{{\delta t}} + O(\delta {t^3})
+\end{equation}
+
+The coefficients of the approximated derivative are very close to the coefficients of the analogous Adams-Bashforth algorithm. Then the approximated derivative is substituted into the mass balance, and the terms with the carbon dioxide concentration at past time steps are all put on the right-hand side of the equation. This third order derivative zone carbon dioxide update increases the number of previous time steps that are used in calculating the new zone generic contaminant concentration and decreases the dependence on the most recent. The higher order derivative approximations have the potential to allow the use of larger time steps by smoothing transitions through sudden changes in zone operating conditions.
+
+\begin{equation}
+\begin{array}{l}\frac{{{\rho_{air}}{V_z}{M_{for}}}}{{\delta t}}\left( {\frac{{11}}{6}} \right)C_{f,z}^t + {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}C_{f,z}^t}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} C_{f,z}^t + {{\dot m}_{\inf }}C_{f,z}^t + {{\dot m}_{sys}}C_{f,z}^t + \sum\limits_j {{h_j}\rho {A_j}C_{f,z}^t} \\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; = \sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{f,z,i}} + {{\dot m}_{\inf }}{C_{f,\infty }} + {{\dot m}_{sys}}{C_{f,\sup }} + \sum\limits_j {{h_j}\rho {A_j}\frac{{{C_{s,j}}}}{{{k_j}}}}  + {S_f}\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; - \frac{{{\rho_{air}}{V_z}{M_{for}}}}{{\delta t}}\left( { - 3C_{f,z}^{t - \delta t} + \frac{3}{2}C_{f,z}^{t - 2\delta t} - \frac{1}{3}C_{f,z}^{t - 3\delta t}} \right)\end{array}
+\end{equation}
+
+This gives us the basic air mass balance equation that will be solved in two different ways, one way for the predict step and one way for the correct step.
+
+Since the third choice of solution algorithms uses an integration approach, defined as AnalyticalSolution in the ZoneAirHeatBalanceAlgorithm object, it does not require any approximations and has no truncation errors. The solutions in both prediction and correction are provided below in detail.
+
+\subsection{Generic Contaminant Prediction}\label{generic-contaminant-prediction}
+
+For the generic contaminant concentration prediction case, the equation is solved for the anticipated system response as shown below.
+
+\begin{equation}
+{\rm{PredictedSystemLoad}} = {\dot m_{sys}}\left( {{C_{f,\sup }} - C_{f,z}^t} \right)
+\end{equation}
+
+Since the program provides three solution algorithms, the generic contaminant prediction from each solution algorithm is given below.
+
+\subsubsection{EulerMethod}\label{eulermethod-000}
+
+For this solution algorithm, the air mass balance for the predicted air system load or response is:
+
+\begin{equation}
+\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = {\rho_{air}}{V_z}{M_{for}}{\left( {\delta t} \right)^{ - 1}}\left( {{C_{{\rm{setpoint}}}} - C_{f,z}^{t - \delta t}} \right)\\\;\;\;\;\;\;\; - \left[ {\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6} - } {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}{C_{{\rm{setpoint}}}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{f,z,i}} - {C_{{\rm{setpoint}}}}} \right) + {S_f}} \right]\\\;\;\;\;\;\; - \left[ {{{\dot m}_{\inf }}\left( {{C_{f,\infty }} - {C_{{\rm{setpoint}}}}} \right) + \sum\limits_j {{h_j}\rho {A_j}(\frac{{{C_{s,j}}}}{{{k_j}}} - {C_{{\rm{setpoint}}}})} } \right]\;\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\end{array}
+\end{equation}
+
+\subsubsection{ThirdOrderBackwardDifference}\label{thirdorderbackwarddifference-000}
+
+For this solution algorithm, the air mass balance for the predicted system load or response is given below:
+
+{\scriptsize
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = \frac{{{\rho_{air}}{V_z}{M_{for}}}}{{\delta t}}\left( {\frac{{11}}{6}} \right){C_{{\rm{setpoint}}}} - \left[ {{\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}{C_{{\rm{setpoint}}}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{{\rm{setpoint}}}} + {{\dot m}_{\inf }}{C_{{\rm{setpoint}}}}} \right]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; - \left[ {\sum\limits_j {{h_j}\rho {A_j}{C_{{\rm{setpoint}}}}}  + \sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{f,z,i}} + {{\dot m}_{\inf }}{C_{f,\infty }} + \sum\limits_j {{h_j}\rho {A_j}\frac{{{C_{s,j}}}}{{{k_j}}} + {S_f}} } \right]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; + \frac{{{\rho_{air}}{V_z}{M_{for}}}}{{\delta t}}\left( { - 3C_{f,z}^{t - \delta t} + \frac{3}{2}C_{f,z}^{t - 2\delta t} - \frac{1}{3}C_{f,z}^{t - 3\delta t}} \right)\end{array}
+\end{equation}}
+
+\subsubsection{AnalyticalSolution}\label{analyticalsolution-000}
+
+For this solution algorithm, the air mass balance for the predicted air system load or response is given below:
+
+\begin{equation}
+\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = \left[ {\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } } \right]*\\\;\;\;\;\;\;\;\;\;\;\;\left[ {C_{{\rm{setpoint}}}^t - C_z^{t - \delta t}*\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } }}{{{\rho_{air}}{V_Z}{M_{FOR}}}}\delta t} \right)} \right]*\\\;\;\;\;\;\;\;\;\;\;\;{\left[ {1 - \exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } }}{{{\rho_{air}}{V_Z}{M_{FOR}}}}\delta t} \right)} \right]^{ - 1}} - \\\;\;\;\;\;\;\;\;\;\;\;\left( {\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{f,z,i}}\; + {{\dot m}_{\inf }}{C_{f,\infty }} + \sum\limits_j {{h_j}\rho {A_j}} \frac{{{C_{s,j}}}}{{{k_j}}} + {S_f}} \right)\end{array}
+\end{equation}
+
+At the prediction point in the simulation, the system air mass flows are not known; therefore, the system response is approximated. The predicted air system generic contaminant load is then used in the system simulation to achieve the best results possible. If a central HVAC system provides the outdoor flow rate from a Controller:MechanicalVentilation object, the outdoor airflow rate may be approximated as:
+
+\begin{equation}
+{\rm{PredictedSystemLoad}} = {\dot m_{sys}}\left( {{C_{f,\sup }} - C_{f,z}^t} \right) \approx {\dot m_{OA,z}}\left( {{C_{f,\infty }} - C_{{\rm{setpoint}}}^t} \right)
+\end{equation}
+
+where:
+
+\({\dot m_{OA,z}}\) = Supply outdoor airflow rate into the controlled zone {[}kg/s{]}
+
+The above approximation is based on the assumption that the generic contaminant concentration at the outdoor air (OA) mixer inlet is equal to the zone air outlet concentration level, and the generic contaminant level at the zone supply air inlet is equal to the level at the outlet node of the OA mixer.
+
+After the system simulation is completed, the actual response from the air system is used in the generic contaminant correction step, which is shown next.
+
+\subsection{Generic Contaminant Correction}\label{generic-contaminant-correction}
+
+For the correct step, the expanded air mass balance equation is solved for the final zone generic contaminant concentration at the current time step. In the same manner as described above for predicting the carbon dioxide load to be met by the air system, the zone air carbon dioxide correction calculation will be described individually for the three solution algorithms.
+
+\subsubsection{EulerMethod}\label{eulermethod-1-000}
+
+\begin{equation}
+\begin{array}{l}C_{f,z}^t = \frac{{\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}{C_{f,z,i}}}  + {{\dot m}_{\inf }}{C_{f,\infty }} + {{\dot m}_{sys}}{C_{f,\sup }} + \sum\limits_j {{h_j}\rho {A_j}\frac{{{C_{s,j}}}}{{{k_j}}} + {\rho_{air}}{V_Z}{M_{FOR}}\frac{{C_{f,z}^{t - \delta t}}}{{\delta t}} + {S_f}} }}{{{\rho_{air}}{V_z}{M_{for}}{{\left( {\delta t} \right)}^{ - 1}} + {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}} + \sum\limits_j {{h_j}\rho {A_j}} }}\\\end{array}
+\end{equation}
+
+\subsubsection{ThirdOrderBackwardDifference}\label{thirdorderbackwarddifference-1-000}
+
+\begin{equation}
+\begin{array}{l}C_{f,z}^t = \frac{\begin{array}{l}\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}{C_{f,z,i}}}  + {{\dot m}_{\inf }}{C_{f,\infty }} + {{\dot m}_{sys}}{C_{f,\sup }}\\ + \sum\limits_j {{h_j}\rho {A_j}\frac{{{C_{s,j}}}}{{{k_j}}} + \frac{{{\rho_{air}}{V_Z}{M_{FOR}}}}{{\delta t}}(3C_{f,z}^{t - \delta t} - \frac{3}{2}C_{f,z}^{t - 2\delta t} + \frac{1}{3}C_{f,z}^{t - 3\delta t}) + {S_f}} \end{array}}{{{\rho_{air}}{V_z}{M_{for}}{{\left( {\delta t} \right)}^{ - 1}}\left( {\frac{{11}}{6}} \right) + {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}} + \sum\limits_j {{h_j}\rho {A_j}} }}\\\end{array}
+\end{equation}
+
+\subsubsection{AnalyticalSolution}\label{analyticalsolution-1-000}
+
+\begin{equation}
+\begin{array}{l}C_{f,z}^t = \left[ {C_{f,z}^{t - \delta t} - \frac{{\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{f,z,i}}\; + {{\dot m}_{\inf }}{C_{f,\infty }} + {{\dot m}_{sys}}{C_{f,sys}} + \sum\limits_j {{h_j}\rho {A_j}} \frac{{{C_{s,j}}}}{{{k_j}}}}}{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } }}} \right]*\\\;\;\;\;\;\;\;\;\;\exp \left[ { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } }}{{{\rho_{air}}{V_Z}{M_{FOR}}}}\delta t} \right] + \\\;\;\;\;\;\;\;\;\frac{{\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{f,z,i}}\; + {{\dot m}_{\inf }}{C_{f,\infty }} + {{\dot m}_{sys}}{C_{f,sys}} + \sum\limits_j {{h_j}\rho {A_j}} \frac{{{C_{s,j}}}}{{{k_j}}} + {S_f}}}{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } }}\end{array}
+\end{equation}
+
+The above solutions are implemented in the Correct Zone Air Generic Contaminant step in the Zone Contaminant Predictor Corrector module of EnergyPlus.
diff --git a/doc/engineering-reference/src/integrated-solution-manager/moisture-predictor-corrector.tex b/doc/engineering-reference/src/integrated-solution-manager/moisture-predictor-corrector.tex
new file mode 100644
index 00000000000..5d1fdebc24e
--- /dev/null
+++ b/doc/engineering-reference/src/integrated-solution-manager/moisture-predictor-corrector.tex
@@ -0,0 +1,197 @@
+\section{Moisture Predictor-Corrector}\label{moisture-predictor-corrector}
+
+The transient air mass balance equation for the change in the zone humidity ratio = sum of internal scheduled latent loads + infiltration + system + multizone airflows + convection to the zone surfaces may be expressed as follows:
+
+\begin{equation}
+\begin{array}{l}
+{\rho_{air}}{V_z}{C_W}\frac{{d{W_z}}}{{dt}} = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}\left( {{W_{surf{s_i}}} - W_z^t} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{W_{zi}} - W_z^t} \right)\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; + {{\dot m}_{\inf }}\left( {{W_\infty } - W_z^t} \right) + {{\dot m}_{sys}}\left( {{W_{\sup }} - W_z^t} \right)
+\end{array}
+\end{equation}
+
+where
+
+C\(_{W}\) = humidity capacity multiplier (See the InputOutput Reference for additional information on the object ZoneCapacitanceMultiplier:ResearchSpecial)
+
+In the same manner as described above for zone air temperature (ref. Basis for the Zone and Air System Integration), the solution algorithms provided in the ZoneAirHeatBalanceAlgorithm object are also applied to zone air moisture calculations.
+
+In order to calculate the derivative term with respect to time, the first order backward finite difference method, defined as the EulerMethod in the ZoneAirHeatBalanceAlgorithm object, may be used:
+
+\begin{equation}
+\frac{{dW}}{{dt}} = {\left( {\delta t} \right)^{ - 1}}(W_z^t - W_z^{t - \delta t}) + O(\delta t)
+\end{equation}
+
+The zone air humidity ratio update at the current time step using the EulerMethod may be expressed as follows:
+
+\begin{equation}
+\begin{array}{l}{\rho_{air}}V{C_W}{\left( {\delta t} \right)^{ - 1}}\left( {W_z^t - W_z^{t - \delta t}} \right) = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}\left( {{W_{surf{s_i}}} - W_z^t} \right) \\
+\quad \quad \quad \quad + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{W_{zi}} - W_z^t} \right) + {{\dot m}_{\inf }}\left( {{W_\infty } - W_z^t} \right) + {{\dot m}_{sys}}\left( {{W_{\sup }} - W_z^t} \right)\end{array}
+\end{equation}
+
+To preserve the stability of the calculation of the zone humidity ratio, the third order differential approximation, derived by a Taylor Series and used in the calculation of the next time step's zone air temperature, is also applied to the zone air humidity ratio calculations. This algorithm is the default choice and is defined as 3rdOrderBackwardDifference in the ZoneAirHeatBalanceAlgorithm object.
+
+The third order derivative derived from a Taylor Series expansion is defined as:
+
+\begin{equation}
+{\left. {\frac{{d{W_z}}}{{dt}}} \right|_t} \approx \frac{{\left( {{\textstyle{\frac{11}{6}}}W_z^t - 3W_z^{t - \delta t} + {\textstyle{\frac{3}{2}}}W_z^{t - 2\delta t} - {\textstyle{frac{1}{3}}}W_z^{t - 3\delta t}} \right)}}{{\delta t}} + O\left( {\delta {t^3}} \right) .
+\end{equation}
+
+The coefficients of the approximated derivative are very close to the coefficients of the analogous Adams-Bashforth algorithm. Then the approximated derivative is substituted into the mass balance and the terms with the humidity ratio at past time steps are all put on the right hand side of the equation. This third order derivative zone humidity ratio update increases the number of previous time steps that are used in calculating the new zone humidity ratio, and decreases the dependence on the most recent. The higher order derivative approximations have the potential to allow the use of larger time steps by smoothing transitions through sudden changes in zone operating conditions.
+
+\begin{equation}
+\begin{array}{l}\frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\left( {\frac{{11}}{6}} \right)W_z^t + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}W_z^t + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} W_z^t + {{\dot m}_{\inf }}W_z^t + {{\dot m}_{sys}}W_z^t = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}} \\
+\quad \quad \quad + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {{\dot m}_{\inf }}{W_\infty } + {{\dot m}_{sys}}{W_{\sup }} \\
+\quad \quad \quad - \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\left( { - 3W_z^{t - \delta t} + \frac{3}{2}W_z^{t - 2\delta t} - \frac{1}{2}W_z^{t - 3\delta t}} \right)\end{array}
+\end{equation}
+
+This gives us the basic air mass balance equation that will be solved two different ways, one way for the predict step and one way for the correct step.
+
+Since the third choice of solution algorithms uses an integration approach, defined as AnalyticalSolution in the ZoneAirHeatBalanceAlgorithm object, it does not require any approximations and has no truncation errors. The solutions in both prediction and correction are provided below in detail.
+
+\subsection{Moisture Prediction}\label{moisture-prediction}
+
+For the moisture prediction case the equation is solved for the anticipated system response as shown below.
+
+\begin{equation}
+\begin{array}{l}
+    \rm{PredictedSystemLoad} = \dot{m}_{sys}*\left(W_z^t - W_{sup}\right) \\
+    \rm{MassFlow * HumRat} = \frac{kg_{air}}{sec}\frac{kg_{water}}{kg_{air}} = \frac{kg_{water}}{sec}
+  \end{array}
+\end{equation}
+
+Since the program provides three solution algorithms, the moisture prediction from each solution algorithm is given below.
+
+\subsubsection{EulerMethod}\label{eulermethod-001}
+
+For this solution algorithm, the air mass balance for the predicted air system load or response is:
+
+{\scriptsize
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+\begin{array}{l}{\rm{PredictedSystemLoad}}\;[k{g_{Water}}/\sec ] = {\rho_{air}}{V_z}{C_W}{\left( {\delta t} \right)^{ - 1}}\left( {W_{{\rm{setpoint}}}^t - W_z^{t - \delta t}} \right) \\
+- \left[ {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}\left( {{W_{surf{s_i}}} - W_{{\rm{setpoint}}}^t} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{W_{zi}} - W_{{\rm{setpoint}}}^t} \right) + {{\dot m}_{\inf }}\left( {{W_\infty } - W_{{\rm{setpoint}}}^t} \right)} \right]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\end{array}
+\end{equation}}
+
+\subsubsection{ThirdOrderBackwardDifference}\label{thirdorderbackwarddifference-001}
+
+For this solution algorithm, the air mass balance for the predicted system load or response is given below:
+
+{\scriptsize
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+\begin{array}{l}{\rm{PredictedSystemLoad}}\;[k{g_{Water}}/\sec ] = \left( {\frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\left( {\frac{{11}}{6}} \right) + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }}} \right)W_z^t - \\\;\;\;\left[ {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {{\dot m}_{\inf }}{W_\infty } + \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\left( {3W_z^{t - \delta t} - \frac{3}{2}W_z^{t - 2\delta t} + \frac{1}{3}W_z^{t - 3\delta t}} \right)} \right]\;\;\end{array}
+\end{equation}}
+
+Then, using the following substitutions, the air mass balance equation becomes:
+
+\begin{equation}
+A = \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {\dot m_{\inf }}
+\end{equation}
+
+\begin{equation}
+B = \;\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {\dot m_{\inf }}{W_\infty }\;
+\end{equation}
+
+\begin{equation}
+C = \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\;
+\end{equation}
+
+\begin{equation}
+\begin{array}{l}{\rm{PredictedSystemLoad}}\;[k{g_{Water}}/\sec ] = \left[ {\frac{{11}}{6}*C + A} \right]\;*{W_{SetPo{\mathop{\rm int}} }} - \\\;\;\;\;\;\;\;\;\;\left[ {B + C*\left( {3W_z^{t - \delta t} - \frac{3}{2}W_z^{t - 2\delta t} + \frac{1}{3}W_z^{t - 3\delta t}} \right)} \right]\end{array}
+\end{equation}
+
+\subsubsection{AnalyticalSolution}\label{analyticalsolution-001}
+
+For this solution algorithm, the air mass balance for the predicted air system load or response is given below:
+
+\begin{equation}
+\begin{array}{l}{\rm{PredictedSystemLoad}}\;[k{g_{Water}}/\sec ] = \left[ {\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}}\; + {{\dot m}_{\inf }}} \right]*\\\;\;\;\left[ {W_{{\rm{setpoint}}}^t - W_z^{t - \delta t}*\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}}\; + {{\dot m}_{\inf }}}}{{{\rho_{air}}{V_z}{C_W}}}\delta t} \right)} \right]*\\\;\;\;{\left[ {1 - \exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }}}}{{{\rho_{air}}{V_z}{C_W}}}\delta t} \right)} \right]^{ - 1}} - \\\;\;\;\left( {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}} \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}}\; + {{\dot m}_{\inf }}{W_\infty }} \right)\end{array}
+\end{equation}
+
+At the prediction point in the simulation, the system air mass flows are not known; therefore, the system response is approximated. The predicted air system moisture load is then used in the system simulation to achieve the best results possible. The system simulation components that have moisture control will try to meet this predicted moisture load. For example, humidifiers will look for positive moisture loads and add moisture at the specified rate to achieve the relative humidity setpoint. Likewise, dehumidification processes will try to remove moisture at the specified negative predicted moisture load to meet the relative humidity setpoint.
+
+After the system simulation is completed the actual response from the air system is used in the moisture correction of step, which is shown next.
+
+\subsection{Moisture Correction}\label{moisture-correction}
+
+For the correct step the expanded air mass balance equation is solved for the final zone humidity ratio at the current time step. When the air system is operating, the mass flow for the system outlet includes the infiltration mass flow rate, therefore the infiltration mass flow rate is not included as a separate term in the air mass balance equation. But when the air system is off, the infiltration mass flow in is then exhausted out of the zone directly.
+
+In the same manner as described above for predicting the moisture load to be met by the air system, the zone air moisture correction calculation will be described individually for the three solution algorithms.
+
+\subsubsection{EulerMethod}\label{eulermethod-1-001}
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+W_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {{\dot m}_{\inf }}{W_\infty } + {{\dot m}_{sys}}{W_{\sup }} + {\rho_{air}}{V_z}{C_W}\frac{{W_z^{t - \delta t}}}{{\delta t}}}}{{\frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}} + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}{\rho_{ai{r_z}}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}
+\end{equation}
+
+\subsubsection{ThirdOrderBackwardDifference}\label{thirdorderbackwarddifference-1-001}
+
+{\scriptsize
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+W_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {{\dot m}_{\inf }}{W_\infty } + {{\dot m}_{sys}}{W_{\sup }} + \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}(3W_z^{t - \delta t} - \frac{3}{2}W_z^{t - 2\delta t} + \frac{1}{3}W_z^{t - 3\delta t})}}{{\frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\left( {\frac{{11}}{6}} \right) + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}{\rho_{ai{r_z}}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}
+\end{equation}}
+
+Using the same A, B, and C parameters from the prediction step modified with actual zone mass flows with the air system ON and OFF result in:
+
+\textbf{If} (ZoneSupplyAirMassFlowRate \textgreater{} 0.0) \textbf{Then}
+
+\begin{equation}
+A = \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {\dot m_{\inf }} + {\dot m_{sys}}
+\end{equation}
+
+\begin{equation}
+B = \;\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {\dot m_{\inf }}{W_\infty }\; + {\dot m_{sys}}{W_{\sup }}
+\end{equation}
+
+\begin{equation}
+C = \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\;
+\end{equation}
+
+\textbf{Else If} (ZoneSupplyAirMassFlowRate \textless{} = 0.0) \textbf{Then}
+
+\begin{equation}
+A = \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {\dot m_{\inf }} + {\dot m_{Exhaust}}
+\end{equation}
+
+\begin{equation}
+B = \;\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {\dot m_{\inf }}{W_\infty }\; + {\dot m_{Exhaust}}{W_\infty }
+\end{equation}
+
+\begin{equation}
+C = \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\;
+\end{equation}
+
+\textbf{End If}
+
+Inserting in the parameters A, B and C above in the air mass balance equation, it simplifies to:
+
+\begin{equation}
+W_z^t = \left[ {\frac{{B + C * \left( {3W_z^{t - \delta t} - {\textstyle{3 \over 2}}W_z^{t - 2\delta t} + {\textstyle{1 \over 3}}W_z^{t - 3\delta t}} \right)}}{{\left( {{\textstyle{{11} \over 6}}} \right) * C + A}}} \right]
+\end{equation}
+
+\subsubsection{AnalyticalSolution}\label{analyticalsolution-1-001}
+
+\begin{equation}
+\begin{array}{l}W_z^t = \left[ \begin{array}{l}W_z^{t - \delta t} - \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}}\; + {{\dot m}_{\inf }}{W_\infty } + {{\dot m}_{sys}}{W_{\sup }}}}{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}\\\end{array} \right]*\\\;\;\;\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}{{{\rho_{air}}{V_z}{C_W}}}\delta t} \right) + \\\;\;\;\frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}}\; + {{\dot m}_{\inf }}{W_\infty } + {{\dot m}_{sys}}{W_{\sup }}}}{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}\end{array}
+\end{equation}
+
+The above solutions are implemented in the Correct Zone Air Humidity Ratio step in EnergyPlus. This moisture update equation is used for the Conduction Transfer Function (CTF) heat balance algorithm, in addition to the effective moisture penetration depth (EMPD) with conduction transfer function heat balance algorithm. The equations are identical except that the convection to the zone surfaces is non-zero for the moisture penetration depth case. This moisture update allows both methods to be updated in the same way, with the only difference being the additional moisture capacitance of the zone surfaces for the Effective Moisture Penetration Depth (EMPD) solution approach.
+
+When the HAMT (Combined Heat And Moisture Finite Element) defined in the HeatBalanceAlgorithm object is applied, the moisture update equations are also the same as the equations used in the effective moisture penetration depth (EMPD) with conduction transfer function solution algorithm.
diff --git a/doc/engineering-reference/src/integrated-solution-manager/summary-of-predictor-corrector-procedure.tex b/doc/engineering-reference/src/integrated-solution-manager/summary-of-predictor-corrector-procedure.tex
new file mode 100644
index 00000000000..42f98a0f267
--- /dev/null
+++ b/doc/engineering-reference/src/integrated-solution-manager/summary-of-predictor-corrector-procedure.tex
@@ -0,0 +1,13 @@
+\section{Summary of Predictor-Corrector Procedure}\label{summary-of-predictor-corrector-procedure}
+
+The predictor-corrector scheme can be summarized as follows:
+
+\begin{itemize}
+\tightlist
+\item
+  Using equation , an estimate is made of the air system energy required to balance the equation with the zone air temperature equal to the setpoint temperature.
+\item
+  With that quantity as a demand, the air system is simulated to determine its actual supply capability at the time of the simulation. This will include a plant simulation if necessary.
+\item
+  The actual air system capability is used in equation to calculate the resulting zone temperature.
+\end{itemize}
diff --git a/doc/engineering-reference/src/integrated-solution-manager/summary-of-time-marching-solution.tex b/doc/engineering-reference/src/integrated-solution-manager/summary-of-time-marching-solution.tex
new file mode 100644
index 00000000000..180500f9285
--- /dev/null
+++ b/doc/engineering-reference/src/integrated-solution-manager/summary-of-time-marching-solution.tex
@@ -0,0 +1,85 @@
+\section{Summary of Time Marching Solution}\label{summary-of-time-marching-solution}
+
+EnergyPlus models building performance over time spans of days to years using a time marching method based on \emph{timesteps}. This section provides more information on issues related to timestep formulation.
+
+\subsection{Summary of Timestep Model Formulation}\label{summary-of-timestep-model-formulation}
+
+An EnergyPlus simulation covers a certain period of time, such as a day or a year, that is broken down into a series of discrete bins of time that are referred to as \emph{timesteps}. The program marches through time by recalculating model equations at each timestep. The figure below diagrams some of these basic concepts.
+
+\begin{figure}[hbtp] % fig 9
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image141.png}
+\caption{Diagram of TimeStep Formulation \protect \label{fig:diagram-of-timestep-formulation}}
+\end{figure}
+
+Most models in EnergyPlus are quasi-steady energy balance equations used to predict the conditions present during each timestep. Various input data and boundary conditions for the models are time-varying and a ``staircase'' approach is used where such values are determined for a particular timestep and then essentially held constant over the entire timestep. Predictions for state variables, such as temperature, are averages over the timestep. Predictions for summed variables, such as energy use, are simple totals over the timestep.
+
+EnergyPlus produces time-series results for selected output variables at selected frequencies. The time values associated with the time-series data, or timestamps, are output for the end of the timestep, but the values of the variables are for the entire bin of time prior to the timestamp. When data are reported at coarser frequencies such as hourly, then the results are averages or simple totals for all the timesteps that are contained within the larger bin of time.
+
+To simplify solutions that would otherwise need to be simultaneous, models sometimes use data that are ``lagged'' which means that the values used in the calculations for the current timestep are actually results from the previous timestep. Many models just use the most current results available and so may use lagged data for a first iteration, but then use current data that are not lagged for subsequent iterations.
+
+\subsection{Zone Update Method}\label{zone-update-method}
+
+A zone is not necessarily a single room but is usually defined as a region of the building or a collection of rooms subject to the same type of thermal control and having similar internal load profiles that, subsequently, can be grouped together. Zones can interact with each other thermally through adjacent surfaces and by intermixing of zone air. In EnergyPlus, the conditions in each zone are updated by Equation , which uses previously calculated values of the zone conditions. This means that EnergyPlus does not have to iterate to find a self-consistent solution of the updated zone conditions. However, because heat transfer through each zone's surfaces and interzone mixing of air still occur, the new space temperatures must be computed at the same simulation time and on the same time step in all zones, even though conditions in one zone may be changing much more rapidly than conditions in the other zones. We have previously documented the method used to update the zone temperature at each time step. This method, called the predictor corrector method, has proved to be satisfactory over a wide range of conditions.
+
+\subsection{Variable Timestep}\label{variable-timestep}
+
+The need for a variable timestep in EnergyPlus was identified during development of its predecessor IBLAST. Prior to the integration of the central plant simulation in IBLAST, a time step Dt for the zone temperature update of 0.25 hours (15 minutes) was found to give stable results without a large increase in computation time. The first step in integrating plant was to implement the detailed coil models and coil control strategies without actually adding the plant models themselves. This meant that the user had to specify the coil water inlet temperature and the maximum coil inlet water flow rate to run the simulation. The real life analogy would be a chiller of very large, though not infinite, capacity. The coil capacity was controlled by adjusting the water flow rate, but the effect of the plant on the chilled water temperature was eliminated. After implementation of this step, experience with the program showed that updating the zone temperatures on a fixed time step frequently resulted in instabilities unless a very short time step was used. However, as the time step got shorter the time required to execute the program got prohibitively high.
+
+Clearly, an adaptive time step was required. This would shorten the time step to maintain stability of the zone air energy balance calculation when zone conditions were changing rapidly and expand it to speed computation when zone conditions were relatively unchanging. But, the adaptive time step could not be applied easily to the surface heat transfer calculations, even using interpolation methods to determine new temperature and flux histories. The problem of updating the zone temperature was resolved by using a two-time-step approach in which the zone air temperature is updated using an adaptive time step that ensures stability. In this two time level scheme, the contributions to the zone loads from the surfaces, and user specified internal loads are updated at the default or user specified time step that is constant. This is often referred to as the ``zone'' time step. The contributions to the zone loads from HVAC system response, infiltration, and air mixing are updated at a second variable time step, referred to as the ``system'' time step. The system time step is limited to between one minute and the zone time step. The lower limit of the system time step can be increased to larger than one minute by the user with a System Convergence Limits object (which may be useful to decrease simulation run times at the expense of some accuracy).
+
+The program's decision to adapt the time step is made by first using the usual zone time step and executing the full predictor-corrector calculations to find resulting zone temperatures. The maximum temperature change experienced by any zone in the model is determined. If this maximum zone temperature change is more than a preset limit of 0.3°C, then the simulation switches to using the shorter system time step. The number of system time steps (within a particular zone time step) is modeled from the results for the maximum zone temperature change (just obtained from the corrector) by assuming that temperature change is linear. The number of system time steps indicated by the temperatures is:
+
+\begin{equation}
+\left( {\frac{{Maximum{\kern 1pt} \;Zone\;Temperature\;Change}}{{Maximum\;Zone\;Temperature\;Difference\;\{ .3C\} }}} \right) + 1.0
+\end{equation}
+
+The limit for the number of system time steps is:
+
+\begin{equation}
+\left( {\frac{{Zone\;Time\;Step}}{{Minimum\;System\;Time\;Step}}} \right)
+\end{equation}
+
+EnergyPlus takes the smallest of these two, truncates them to a whole number and calculates a system time step as:
+
+\begin{equation}
+System\;Time\;Step = \left( {\frac{{Zone\;Time\;Step}}{{Number\;of\;System\;Time\;Steps}}} \right)
+\end{equation}
+
+The same length of time is used for all the system time steps within a particular zone time step, but the system time step length can vary between different zone time steps. Report variables that use the ``detailed'' frequency show results at the system time step time scale.
+
+This approach can be justified because the internal loads and surface temperatures vary on a different and longer time scale than the system response and the zone air temperature.
+
+When the simulation down-steps from using the zone time step to the system time step, linear interpolation is used to generate zone condition history terms:
+
+\begin{equation}
+\begin{array}{l}
+  T_z^{t-\delta t} \\
+  T_z^{t-2\delta t} \\
+  T_z^{t-3\delta t}
+\end{array}
+\end{equation}
+
+for the system time steps using the history data for the zone time step. If two consecutive zone time steps both down-step to have the same number of system time steps, then the system time step history is preserved and used directly rather than being interpolated from zone time step history. The zone temperature update is made for each system time step using the same equation as for the zone time step except that the zone temperature history and time difference (delta-t) terms are for the system time step instead of for the zone time step.
+
+\subsection{Simultaneous Solution of Plant/System Water Loop}\label{simultaneous-solution-of-plantsystem-water-loop}
+
+Simultaneous solution of the system and plant operating parameters required that the temperature of the water entering the coils must be the same as the temperature leaving the chillers or boilers. In addition, the temperature of the return water from the coils must be equal to the chiller or boiler entering water temperature. In practice so long as the plant is not out of capacity the leaving water temperature from chillers and boilers is constant and equal to the design value. No iteration was required to match system and plant boundary conditions. However, if either the chiller or boiler plant was overloaded then the temperature of the water leaving the plant was not equal to the design value and the maximum output of the plant could change because of the off-design conditions. An iterative scheme using the secant method to predict successive updates to the plant leaving water conditions was therefore employed to solve for the water loop conditions with the plant operating at its maximum capacity. The simulation of the system and plant loops is described in greater detail in the later sections.
+
+\subsection{References}\label{references-043}
+
+Ceylan, H. T., and G. E. Myers. 1980. Long-time Solutions to Heat Conduction Transients with Time-Dependent Inputs. ASME Journal of Heat Transfer, Volume 102, No. 1, pp.~115-120.
+
+Hittle, D. C. 1979. Calculating Building Heating and Cooling Loads Using the Frequency Response of Multilayered Slabs, Ph.D.~Thesis, University of Illinois, Urbana, IL.
+
+Hittle, D. C., and R. Bishop. 1983. An Improved Root-Finding Procedure for Use in Calculating Transient Heat Flow Through Multilayered Slabs. International Journal of Heat and Mass Transfer, Vol. 26, No. 11, pp.~1685-1693.
+
+Ouyang, K., and F. Haghighat. 1991. A Procedure for Calculating Thermal Response Factors of Multi-layered Walls--State Space Method. Building and Environment, Vol. 26, No. 2, pp.~173-177.
+
+Seem, J. E. 1987. Modeling of Heat Transfer in Buildings, Ph.D.~Thesis, University of Wisconsin, Madison, WI.
+
+Strand, R. K. 1995. Heat Source Transfer Functions and Their Application to Low Temperature Radiant Heating Systems, Ph.D.~Thesis, University of Illinois, Urbana, IL.
+
+Taylor, R. D., C.O. Pedersen, L.K. Lawrie. 1990. \emph{Simultaneous Simulation of Buildings and Mechanical Systems in Heat Balance Based Energy Analysis Programs}, Proceedings of the 3rd International Conference on System Simulation in Buildings, Liege, Belgium, December 3-5, 1990.
+
+Taylor, R.D., C.O. Pedersen, D.E. Fisher, R. J. Liesen, L.K. Lawrie. 1991. Impact of Simultaneous Simulation of Buildings and Mechanical Systems in Heat Balance Based Energy Analysis Programs on System Response and Control, Conference Proceedings IBPSA Building Simulation '91, Nice, France, August 20-22, 1991.
diff --git a/doc/engineering-reference/src/integrated-solution-manager/zone-air-mass-flow-conservation.tex b/doc/engineering-reference/src/integrated-solution-manager/zone-air-mass-flow-conservation.tex
new file mode 100644
index 00000000000..e7ec017613b
--- /dev/null
+++ b/doc/engineering-reference/src/integrated-solution-manager/zone-air-mass-flow-conservation.tex
@@ -0,0 +1,121 @@
+\section{Zone Air Mass Flow Conservation}\label{zone-air-mass-flow-conservation}
+
+\subsubsection{Overiew}\label{overiew}
+
+The zone air mass flow conservation object, ZoneAirMassFlowConservation, activates zone air mass flow balance calculations. This feature is available only for controlled zones (ZoneVAC:EquipmentConnections) which also have either a zone mixing or infiltration object. The user may specify that zone mixing, infiltration, or both can be overridden to balance the zone air mass flows. The following rules apply:
+
+\begin{itemize}
+\tightlist
+\item
+  If there are no zone mixing flows to adjacent zones, then the zone air mass flow is balanced by setting the Zone Mixing objects mass flow rate to zero.
+\item
+  If there are no zone exhaust fans defined and there are no zone mixing objects specified, then a zone in an air loop is always balanced.
+\item
+  Infiltration mass flow is included in the zone air mass flow balance depending upon one of three options: none (all infiltration is assumed to be self-balanced), all zones, or only zones that serve as a source zone for zone mixing objects.
+\item
+  The base infiltration mass flow rate (calculated based on user inputs) may be controlled one of two ways for zone air mass flow balance purposes: adjust the base infiltration up or down as needed to balance the zone air mass flow, or assume the base infiltration rate is self-balanced and add infiltration if needed to balance the zone air mass flow.
+\item
+  Optional user inputs can override the default return air flow rate.
+\end{itemize}
+
+The zone air mass flow conservation equation always includes: supply air flow rates, return air flow rates, and zone exhaust fan flow rates. Zone mixing and infiltration object flow rates may be included depending upon the selected options. A particular zone can be a source zone, receiving zone, or both depending on the number of ZoneMixing objects specified for that zone.
+
+\subsubsection{Return Air Flow Rate Calculations}\label{return-air-flow-rate-calculations}
+
+The return air flow rate is calculated one of two ways.
+
+The default calculation is:
+
+\begin{equation}
+{\dot m_{R}} = ReturnFlowSchedule*MAX\left( {0.0,\,{{\dot m}_S} + {{\dot m}_{XR}} - {{\dot m}_{EX}} - {{\dot m}_{XS}}} \right)
+\end{equation}
+
+If one or more Zone Return Air Flow Rate Basis Nodes are specified in the ZoneHVAC:EquipmentConnections object, then the base return flow rate is:
+
+\begin{equation}
+{\dot m_{R}} = ReturnFlowSchedule*\sum\nolimits_j {{{\dot m}_{BasisNode,j}}}
+\end{equation}
+
+where,
+
+\({\dot m_{R}}\) = zone return air mass flow rate, (kg/s)
+
+\({\dot m_{Basis Node,j}}\) = zone return air flow basis node mass flow rate, (kg/s)
+
+\({\dot m_{EX}}\) = zone exhaust air mass flow rate from exhaust fans, (kg/s)
+
+\({\dot m_{XR}}\) = zone mixing mass flow rate as a receiving zone, (kg/s)
+
+\({\dot m_{XS}}\) = zone mixing mass flow rate as a source zone, (kg/s)
+
+\({\dot m_S}\) = zone supply air mass flow rate, (kg/s)
+
+ReturnFlowSchedule = optional Zone Return Air Flow Rate Fraction Schedule value
+
+\subsubsection{Zone Mixing Flow Rate Calculations}\label{zone-mixing-flow-rate-calculations}
+
+Figure~\ref{fig:illustration-of-zone-air-mass-flow-balance} illustrates the zone mass flow components for an air loop system providing conditioned air to the two zones connected with a zone mixing object. Since Zone 1 is a source zone only, infiltration object is defined for zone 1 only. The zone mixing object air flow rate depends on the user specified values and the zone air mass flow balance requirements. When required the zone mixing object flow rate is adjusted from the user specified value for balancing purpose.
+
+\begin{figure}[hbtp] % fig 8
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image134.svg.png}
+\caption{Illustration of zone air mass flow balance components \protect \label{fig:illustration-of-zone-air-mass-flow-balance}}
+\end{figure}
+
+An individual zone may be a source zone for multiple receiving zones, and the same source zone may receive mixing flows from multiple adjacent zones in an air loop. The source and receiving mass flow rates of ZoneMixing objects are calculated from user defined mixing flow rates at the first HVAC iteration for each time step and adjusted in subsequent iterations to balance the zone air mass flow. The source zone mixing mass flow rate is calculated by tracking the mass flow rates of ZoneMixing objects connected to a zone and is given by:
+
+\begin{equation}
+{\dot m_{XS}} = \sum\nolimits_j {{{\dot m}_{XS,j}}}
+\end{equation}
+
+Determine the zone return air mass flow rate as shown above, then adjust the zone mixing mass flow rates based on the current zone return air mass flow rate:
+
+\begin{equation}
+{\dot m_{XR,\,new}} = {\dot m_R} + {\dot m_{EX}} + {\dot m_{XS}} - {\dot m_S}
+\end{equation}
+
+This updated receiving zone mixing air mass flow rate is distributed to the mixing objects connected to the current zone proportional to user specified design flow rate. A single zone may be connected to more than one adjacent zone using multiple ZoneMixing objects. Thus, the mixing flow rate of each contributing mixing objects defined in the current zone is updated as follows:
+
+\begin{equation}
+{\dot m_{XR,\,new,j}} = \left( {{{\dot m}_{XR,jDesign}}/{{\dot m}_{XR,Design}}} \right) \cdot {\dot m_{XR,\,new}}
+\end{equation}
+
+\subsubsection{Infiltration Flow Rate Adjustments}\label{infiltration-flow-rate-adjustments}
+
+There are three options for the treatement of infiltration in the zone air mass balance: None, AddInfiltrationFlow, and AdjustInfiltrationFlow. There are also two options to specify which zones are included in the infiltration adjustments: AllZones or MixingSourceZonesOnly.
+
+If a zone is excluded from infiltration adjustments, then the base infiltration rate specified by the Infiltration:* object(s) in the zone is assumed to be self-balanced, and infiltration is not included in the mass flow calculations for that zone.
+
+If a zone is included in the infiltration adjustment, the infiltration air mass flow rate required to balance the zone is determined as follows:
+
+\begin{equation}
+{\dot m_{Inf-required}} = MAX\left( {0.0,\,{{\dot m}_{XS}} + {{\dot m}_{EX}} + {{\dot m}_{R}} - {{\dot m}_S}} \right)
+\end{equation}
+
+This infiltration air mass flow rate calculated is either added to the base infiltration air flow, which is calculated from user inputs, or overrides the base infiltration air flow depending on user choice. For AddInfiltrationFlow, the zoneinfiltration flow rate is:
+
+\begin{equation}
+{\dot m_{Inf}} = {\dot m_{Inf-base}} + {\dot m_{Inf-required}}
+\end{equation}
+
+For AdjustInfiltrationFlow, the zone infiltration flow rate is:
+
+\begin{equation}
+{\dot m_{Inf}} = {\dot m_{Inf-required}}
+\end{equation}
+
+where,
+
+\({\dot m_{Inf}}\) = zone infiltration mass flow rate, (kg/s)
+
+\({\dot m_{Inf-base}}\) = base zone infiltration mass flow rate calculated from Infiltration:* objects, (kg/s)
+
+\({\dot m_{Inf-required}}\) = required zone infiltration mass flow rate to balance the zone, (kg/s)
+
+There is an additional constraint to the return air mass flow rate calculation. The sum of the return air mass flow rates of zones in air loop must satisfy the air loop return air mass flow balance. The above four sets of equations are iterated for each zone in an air loop until the convergence criterion is satisfied or until the maximum iteration limit is exceeded.
+
+The mass conservation calculations are performed in routine CalcZoneMassBalance in the ZoneEquipmentManager module. The latest ZoneMixing and Infiltration object flow rates are communicated back to the zone air heat balance terms. This is done by re-simulating the simple flow objects as zone equipment during each HVAC iteration. This requires calling the routine CalcAirFlowSimple in SimZoneEquipment routine as zone equipment. Both of these routines are also in the ZoneEquipmentManager module.
+
+\emph{Zone Mass Conservation Convergence}
+
+The zone mass conservation calculation convergence criterion is based on the absolute difference of the zone mixing objects mass flow rates between successive iteration. If the difference is above tolerance limits of 0.00001 then the HVAC Air loop is simulated again.
diff --git a/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data.tex b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data.tex
new file mode 100644
index 00000000000..cfb84d14caf
--- /dev/null
+++ b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data.tex
@@ -0,0 +1,17 @@
+\chapter{Loop, Equipment Sizing and other Design Data}\label{loop-equipment-sizing-and-other-design-data}
+
+The importance of correct equipment sizing is often ignored in discussions of building simulation methods. The lack of reliable, efficient and flexible sizing calculations can present a serious barrier to the adoption and acceptance of building simulation programs. This section describes the sizing methodology implemented in EnergyPlus. This method includes:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  A zone by zone heat balance load and air-flow calculation for multiple design days;
+\item
+  Significant user control with modest input requirements;
+\item
+  Zone, system and plant level calculations of design heating and cooling capacities and fluid flow rates;
+\item
+  Modular, component-specific sizing algorithms for each HVAC component.
+\item
+  Options for monitoring how the initial sizes operate over multiple design days and then making adjustments and repeating plant level calculations
+\end{enumerate}
diff --git a/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/coincident-plant-sizing-using-hvac-sizing.tex b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/coincident-plant-sizing-using-hvac-sizing.tex
new file mode 100644
index 00000000000..aaaeccd4e85
--- /dev/null
+++ b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/coincident-plant-sizing-using-hvac-sizing.tex
@@ -0,0 +1,43 @@
+\section{Coincident Plant Sizing using HVAC Sizing Simulation}\label{coincident-plant-sizing-using-hvac-sizing-simulation}
+
+Coincident plant sizing is an advanced sizing method that uses HVAC Sizing Simulations to determine coincident flows. This section describes the algorithm used for sizing plant loop flow rate based on the coincidence of flow requests that actually occur when operating the system. The purpose is to provide a more accurate value for the plant loop design flow rate. This value is held in PlantSizData( PltSizIndex ).DesVolFlowRate. For plant, this flow rate is the main independent variable used by component models in their sizing routines (along with the design temperature difference in Sizing:Plant). The code is contained in a PlantCoinicidentAnalysis object, one for each plant loop that is to be sized using the coincident method using HVAC Sizing Simulation.
+
+The analysis will proceed as follows:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Find the maximum mass flow rate over all Sizing Periods, along with the coinciding return temperature and load. Record which sizing period and timestep. This system node used for logging here is the plant loop supply side inlet node.
+\item
+  Find the maximum load, and the coinciding mass flow and return temperature. Record which sizing period and timestep. For a heating or steam plant loop, the load that is logged is associated with the output variable called Plant Supply Side Heating Demand Rate. For a cooling or condenser plant loop, the load log is as for the output variable called Plant Supply Side Cooling Demand Rate.
+\item
+  Calculate a maximum design flow rate from the maximum load, from step 2, and the temperature difference entered in the Plant:Sizing object and the specific heat (at 5 degC) of the plant fluid.
+\item
+  Compare the flow rate from step 1 to the flow rate from step 3 and take the higher.
+\item
+  Apply a sizing factor to the flow rate from Step 4, if desired. The user can select among different options for which sizing factor use.
+\item
+  Compare the flow rate from step 5 to the current value for plant loop flow rate and calculate a normalized change using
+\end{enumerate}
+
+\begin{lstlisting}
+-   $\rm{Normalized_Change} = \frac{ \left| \rm{NewFlowRate}-\rm{PreviousFlowRate} \right|} \rm{PreviousFlowRate}$
+\end{lstlisting}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{6}
+\tightlist
+\item
+  Normalized\_Change = \(\frac{\left|\text{NewFlowRate}-\text{PreviousFlowRate}\right|}{\text{PreviousFlowRate}}\)
+\end{enumerate}
+
+\begin{lstlisting}
+-   Compare magnitude of Normalized\_Change to a threshold, currently set at 0.005, to determine if it was significant or not.
+-   If change is significant, then alter the size result for that plant loop. Set flags that sizes have changed and sizing calculations need to be called again. Trigger special setup timesteps with flags set so that all plant system and component level sizes will be recomputed. Not this will call and resize all of plant so that if one loop has coincident sizing and it places a load on a loop that has noncoincident sizing, the noncoincident loop might still change size because the loop it depends on changed. Call for another Sizing Pass.
+-   If change is not significant, then leave the sizes alone and do not trigger resizing. Do not call for another Sizing Pass.
+\end{lstlisting}
+
+See OutputDetailsAndExamples documentation for a description of a fairly comprehensive report sent the EIO file called ``Plant Coincident Sizing Algorithm'' which provides the user details for each execution of the algorithm. There is also a predefined summary table
+
+The algorithm described above can have powerful impacts on the sizes of plant loops. It is not uncommon for a hot water plant to size out at around half of what would be determined from the noncoincident sum of the sizes of all the components connected to the loop. The maximum load aspect of the algorithm is able to increase plant flow rates above the size of the pumps, whereas the flow rate aspect of the algorithm is only able to reduce the flow rates. It can happen that load spikes cause sizes to increase after the first Sizing Pass, and then the coincident flow rate bring the sizes back down some during subsequent Sizing Passes. It is worthwhile to explore multiple Sizing Passes, or iterations, because sometimes the algorithm will switch between coincident flow and coincident demand from one Sizing Pass and gradually find a size that just meets conditions. Be aware that all the controls and and EMS are also
diff --git a/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/component-sizing.tex b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/component-sizing.tex
new file mode 100644
index 00000000000..b1410dd4352
--- /dev/null
+++ b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/component-sizing.tex
@@ -0,0 +1,2581 @@
+\section{Component Sizing}\label{component-sizing}
+
+\subsection{Introduction}\label{introduction}
+
+In EnergyPlus each HVAC component sizes itself. Each component module contains a sizing subroutine. When a component is called for the first time in a simulation, it reads in its user specified input data and then calls the sizing subroutine. This routine checks the autosizable input fields for missing data and calculates the data when needed.
+
+A number of high-level variables are used in the sizing subroutines.
+
+\emph{CurDuctType} (in \emph{DataSizing}) contains the information about the current duct type. The types can be \emph{main}, \emph{cooling}, \emph{heating} or \emph{other}.
+
+\emph{CurZoneEqNum} (in \emph{DataSizing}) is the current zone equipment set index and indicates that the component is a piece of zone equipment and should size itself using the zone sizing data arrays.
+
+\emph{CurSysNum} (in \emph{DataSizing}) is the current air loop index and indicates that the component is part of the primary air system and should size itself using the system sizing data arrays.
+
+\subsection{Fan Sizing}\label{fan-sizing}
+
+Fan sizing is done in subroutine \emph{SizeFan}.
+
+\subsubsection{Max Flow Rate}\label{max-flow-rate}
+
+If the fan is part of the central air system then check the duct type.
+
+For duct type = \emph{main, other} or default, \(\dot{V}_{fan,max} = \text{DesMainVolFlowsys}\)
+
+For duct type = \emph{cooling}, \(\dot{V}_{fan,max} = \text{DesCoolVolFlowsys}\)
+
+For duct type = \emph{heating}, \(\dot{V}_{fan,max} = \text{DesHeatVolFlowsys}\)
+
+If the fan is zone equipment then check whether it is part of a component that only does heating.
+
+For heating only \(\dot{V}_{fan,max} = \text{DesHeatVolFlowzone}\) ;
+
+Otherwise \(\dot{V}_{fan,max} = \max\left(\text{DesHeatVolFlowzone},\text{DesCoolVolFlowzone}\right)\)
+
+If the max fan flow rate is less than \emph{SmallAirVolFlow} the max flow rate is set to zero.
+
+\subsection{Coil:Cooling:Water}\label{coilcoolingwater}
+
+The sizing is done in function \emph{SizeWaterCoil} of module \emph{WaterCoils}
+
+\subsubsection{Initial Calculations}\label{initial-calculations}
+
+For central cooling coils, the first step is to determine the design air flow rate, load, and design air entering and exit conditions. The coil design air flow rate is not generally the same as the maximum system air flow rate (used to size the central fans). The cooling coil peak load (either sensible or total) can occur at a different time than the system peak flow rate. Hence the coil air entering conditions can be different than those at the peak system flow rate. Also, the method of controlling the coil's cooling output may also affect coil design flow rate as well as the coil design exit temperature and humidity.
+
+By choosing Type of Load to Size On = \emph{Sensible} or \emph{Total} in Sizing:System the user indicates to the program to save the cooling coil air flow rate and system air conditions (mixed, return, outside) at the time of either the system cooling sensible or total load peak. Note that the choice \emph{VentilationRequirement} uses the time of the sensible peak.
+
+Choosing Central Cooling Capacity Control Method = \emph{VAV}, \emph{Bypass}, \emph{VT}, or \emph{OnOff} indicates which type of cooling output control the program should assume when calculating the design air flow rate. The function \emph{GetCoilDesFlowT} in module \emph{ReportSizingManager} calculates the air flow rate and exit air temperature for each capacity control method.
+
+\begin{longtable}{@{}lp{4in}@{}}
+
+  \caption{Cooling coil calculations for different capacity control methods \label{table:cooling-coil-calculations-for-different-capacity-control-methods}} \tabularnewline
+  \toprule
+  Control Method & Calculations \tabularnewline
+  \midrule
+  \endfirsthead
+
+  \caption[]{Cooling coil calculations for different capacity control methods} \tabularnewline
+  \toprule
+  Control Method & Calculations \tabularnewline
+  \midrule
+  \endhead
+
+  VAV &
+  \(\begin{array}{rl}
+    T_{cc,exit} &= T_{cool,supply} \\ 
+    \dot{V}_{cc,air} &= \frac{\dot{m}_{cc,air,peak}}{\rho_{air}}
+  \end{array}\) \tabularnewline
+  Bypass &
+  \(\begin{array}{rl}
+    T_{cc,exit} &= T_{cool,supply} \\ 
+    \dot{V}_{cc,air} &=
+      \dot{V}_{cc,air,max}\cdot\max \left(0, \min \left(1,
+        \frac{T_{mix,at-peak}-T_{sup,avg}}{T_{mix,at-peak}-T_{cc,exit}} \right) \right)
+  \end{array}\) \tabularnewline
+  VT &
+  \(\begin{array}{rl}
+    T_{cc,exit} &= \max\left(T_{cool,supply}, T_{sup,avg}\right) \\ 
+    \dot{V}_{cc,air} &= \dot{V}_{cc,air,max}
+  \end{array}\) \tabularnewline
+  OnOff &
+  \(\begin{array}{rl}
+    T_{cc,exit} &= T_{cool,supply} \\
+    \dot{V}_{cc,air} &=\dot{V}_{sys,air,max}
+  \end{array}\) \tabularnewline
+\bottomrule
+\end{longtable}
+
+Where:
+
+\begin{equation}
+T_{sup,avg} = T_{zones,avg}-\sum_{zones}\frac{\dot{Q}_{sens,at-peak}}{\rho_{air}c_{p,air}\dot{V}_{cool,air,max}}
+\end{equation}
+
+and:
+
+\begin{itemize}
+\item
+  \(C_{p,air}\) : the specific heat of air (J/kgC)
+\item
+  \(\dot{m}_{cc,air,peak}\) : the air mass flow rate through the cooling coil at the sensible or total system peak cooling load (m3/s)
+\item
+  \(\sum_{zones}\dot{Q}_{sens,at-peak}\) : sum of the zone sensible cooling loads at the time of the peak system cooling load
+\item
+  \(\rho_{air}\) : the density of air (kg/m3)
+\item
+  \(T_{cc,exit}\) : the design cooling coil exit temperature (c)
+\item
+  \(T_{cool,supply}\) : the supply air temperature for cooling specified in Sizing:System (C)
+\item
+  \(T_{mix,at-peak}\) : the mixed air temperature at the time of the system peak cooling load (C)
+\item
+  \(T_{zones,avg}\) : the average zone temperature at the time of the system peak cooling load (C)
+\item
+  \(\dot{V}_{cc,air}\) : the design volumetric air flow rate through the cooling coil (m3/s). This is the flow rate at either the sensible or total cooling load peak from the design period calculations.
+\item
+  \(\dot{V}_{cool,air,max}\) : the maximum cooling volumetric air flow rate from the design calculations (m3/s). This flow rate occurs at the maximum zone cooling demand.
+\item
+  \(\dot{V}_{sys,air,max}\) : the maximum volumetric air flow rate from the design calculations (m3/s). This flow rate occurs at either the maximum zone cooling or heating demand.
+\end{itemize}
+
+\subsubsection{Design Coil Load - System Coils}\label{design-coil-load---system-coils}
+
+Design coil load (cooling capacity) is not an input for Coil:Cooling:Water. It is used for calculating the design water flow rate.
+
+The design load is calculated as:
+
+\begin{equation}
+\dot{Q}_{coil,des} = \dot{m}_{a,coil,des}\left(h_{a,coil,des,in}-h_{a,coil,des,out}\right)
+\end{equation}
+
+Where:
+
+\begin{itemize}
+\item
+  \(h_{a,coil,des,in}\) : is the coil design inlet air enthalpy (J/kg)
+\item
+  \(h_{a,coil,des,out}\) : is the coil design outlet air enthalpy (J/kg), and
+\item
+  \(\dot{m}_{a,coil,des}\) : is the coil design air mass flow rate (kg/s)
+\end{itemize}
+
+The design air mass flow rate depends on the location of the coil. If the coil is in the outside air stream, the flow rate is set to
+
+\[\rho_{air}\dot{V}_{a,coil,oa,des}\] where \(\dot{V}_{a,coil.oa,des}\) is the design outside air volumetric flow rate for the system. Otherwise, it is set to:
+
+\begin{equation}
+\rho_{air}\dot{V}_{cc,air}
+\end{equation}
+
+where \(\dot{V}_{cc,air}\) is calculated above in the Initial Calculations section.
+
+To obtain the inlet and outlet enthalpies, we need the inlet and outlet temperatures and humidity ratios. The inlet and outlet conditions depend on whether the coil is in the outside air stream and if it is not, whether or not there is outside air preconditioning.
+
+\paragraph{\texorpdfstring{\textbf{Coil in outside air stream}:}{Coil in outside air stream:}}\label{coil-in-outside-air-stream}
+
+\begin{itemize}
+\item
+  \(T_{air,in,des} = T_{out,cool,at-peak}\) (the outside air temperature at the design cooling peak)
+\item
+  \(T_{air,out,des} = T_{sys,precool}\) (the specified Precool Design Temperature from the System:Sizing object)
+\item
+  \(W_{air,in,des} = W_{out,cool,at-peak}\) (the outside humidity ratio at the design cooling peak)
+\item
+  \(W_{air,out,des} = W_{sys,precool}\) (the specified Precool Design Humidity Ratio from the System:Sizing object)
+\end{itemize}
+
+\paragraph{\texorpdfstring{\textbf{Coil in main air stream, no preconditioning of outside air} }{Coil in main air stream, no preconditioning of outside air }}\label{coil-in-main-air-stream-no-preconditioning-of-outside-air}
+
+\begin{itemize}
+\item
+  \(T_{air,in,des} = T_{mix,cool,at-peak}\) (the mixed air temperature at the design cooling peak)
+\item
+  \(W_{air,in,des} = W_{mix,cool,at-peak}\) (the mixed humidity ratio at the design cooling peak)
+\item
+  \(T_{air,out,des} = T_{cc,exit}\) (calculated above in the Initial Calculation section)
+\item
+  \(W_{air,out,des} = W_{sup,cool}\) (the specified Central Cooling Design Supply Air Humidity Ratio from the Sizing:System object)
+\end{itemize}
+
+\paragraph{\texorpdfstring{\textbf{Coil in main air stream, outside air preconditioned} }{Coil in main air stream, outside air preconditioned }}\label{coil-in-main-air-stream-outside-air-preconditioned}
+
+The oustide air fraction is calculated as (where V\(_{cc,air}\) is calculated as above)
+
+\begin{itemize}
+\item
+  \(f_{oa} = \frac{\dot V_{air,out,des}}{\dot{V}_{cc,air}}\)
+\item
+  \(T_{air,in,des} = f_{oa}T_{precool} + \left(1-f_{oa}\right)T_{ret,cool,at-peak}\) (Precool temperature is the specified Precool Design Temperature from System:Sizing Manager; T\_ret\_cool\_at-peak is the return temperature at the system cooling peak load)
+\item
+  \(W_{air,in,des} = f_{oa}W_{precool} + \left(1-f_{oa}\right)W_{ret,cool,at-peak}\) (Precool humidity ratio is the specified Precool Design Humidity Ratio from System:Sizing Manager; W\_ret\_cool\_at-peak is the return humidity ratio at the system cooling peak load)
+\item
+  \(T_{air,out,des} = T_{cc,exit}\) (calculated above in the Initial Calculation section)
+\item
+  \(W_{air,out,des} = W_{sup,cool}\) (the specified Central Cooling Design Supply Air Humidity Ratio from the Sizing:System object)
+\end{itemize}
+
+With the inlet and outlet conditions established, we can obtain the inlet and outlet enthalpies:
+
+\begin{equation}
+ \begin{array}{rl}
+  h_{air,coil,des,in} & = \text{PsyHFnTdbW}\left(T_{air,in,des},W_{air,in,des}\right) \\
+  h_{air,coil,des,out} & = \text{PsyHFnTdbW}\left(T_{air,out,des},W_{air,out,des}\right)
+ \end{array}
+\end{equation}
+
+Where PsyHFnTdbW is the EnergyPlus function for calculation air specific enthalpy given the air temperature and humidity ratio. We now have all we need to calculate the design coil capacity, \(\dot{Q}_{coil,des}\) .
+
+\subsubsection{Design Coil Load - Zone Coils}\label{design-coil-load---zone-coils}
+
+If the coil is part of an AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction unit or an ZoneHVAC:FourPipeFanCoil, the cooling load (cooling capacity) is passed down from the terminal unit or fan coil sizing calculations. Otherwise the load is defined as:
+
+\begin{equation}
+\dot{Q}_{coil,des} = \dot{m}_{a,coil,des}\left(h_{a,coil,des,in}-h_{a,coil,des,out}\right)
+\end{equation}
+
+Where:
+
+\begin{itemize}
+\item
+  \(h_{a,coil,des,in}\) : is the coil design inlet air enthalpy (J/kg)
+\item
+  \(h_{a,coil,des,out}\) : is the coil design outlet air enthalpy (J/kg), and
+\item
+  \(\dot{m}_{a,coil,des}\) : is the coil design air mass flow rate (kg/s)
+\end{itemize}
+
+The enthalpies are given by:
+
+\begin{equation}
+ \begin{array}{lr}
+  h_{air,coil,des,in} & = \text{PsyHFnTdbW}\left(T_{air,in,des},W_{air,in,des}\right) \\
+  h_{air,coil,des,out} & = \text{PsyHFnTdbW}\left(T_{air,out,des},W_{air,out,des}\right)
+ \end{array}
+\end{equation}
+Where the inputs to those functions are the coil inlet design conditions. For coils in terminal units these are set at the system level to the system design supply air temperature. For zonal units they are set to design return air, mixed air, or outside air as appropriate to the unit. T\(_{air,out,des}\) is set to the zone cooling design supply air temperature as specified in the \emph{Zone:Sizing} inputs. W\(_{air,out,des}\) is set to the zone cooling design supply air humidity ratio as specified in the \emph{Zone:Sizing} inputs.
+
+\subsubsection{\texorpdfstring{Design Water Flow Rate (m\(^{3}\)/s) - System Coils}{Design Water Flow Rate (m\^{}\{3\}/s) - System Coils}}\label{design-water-flow-rate-m3s---system-coils}
+
+The design water volumetric flow rate is calculated using:
+
+\begin{equation}
+\dot{V}_{w,coil,des} = \frac{\dot{Q}_{coil,des}}{\rho_w c_{p,w} \Delta T_{w,des}}
+\end{equation}
+
+Where \(\Delta T_{w,des}\) is just the \emph{Loop Design Temperature Difference} user input from \emph{Sizing:Plant} (if the coil is in the outside air stream, 1/2 the \emph{Loop Design Temperature Difference} is used). The design coil load \emph{Load\(_{coil,des}\)} is calculated from:
+
+\subsubsection{\texorpdfstring{Design Water Flow Rate (m\(^{3}\)/s) - Zone Coils}{Design Water Flow Rate (m\^{}\{3\}/s) - Zone Coils}}\label{design-water-flow-rate-m3s---zone-coils}
+
+If the coil is part of an AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction unit or an ZoneHVAC:FourPipeFanCoil, the chilled water flow rate is passed down from the terminal unit or fan coil sizing calculations. Otherwise the flow is set to:
+
+\begin{equation}
+\dot{V}_{w,coil,des} = \frac{\dot{Q}_{coil,des}}{\rho_w c_{p,w} \Delta T_{w,des}}
+\end{equation}
+
+Where \(\Delta T_{w,des}\) is just the \emph{Loop Design Temperature Difference} user input from \emph{Sizing:Plant}.
+
+\subsubsection{Design Air Flow Rate - System Coils}\label{design-air-flow-rate---system-coils}
+
+The design air volumetric flow rate for the system cooling coil is set to:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  the design outside air flow rate if the coil is in the outside air stream;
+\item
+  the coil design flow rate from function GetCoilDesFlowT described in section ``Initial Calculations'';
+\item
+  the design flow rate set by the parent component (such as a unitary system) containing the cooling coil.
+\end{enumerate}
+
+\subsubsection{Design Air Flow Rate - Zone Coils}\label{design-air-flow-rate---zone-coils}
+
+Zone chilled water coils are always part of a zone HVAC component. In almost all cases the design flow rate is passed down from the design flow rate of the parent component. Otherwise if the parent component does cooling only the flow rate for the coil is set to the zone design cooling flow rate. And if the parent component does both cooling and heating, the coil flow rate is set to the maximum of the zone design cooling and heating flow rates.
+
+\subsubsection{Design Air Inlet Temperature - System Coils}\label{design-air-inlet-temperature---system-coils}
+
+The inlet air temperature depends on whether the coil is in the outside air stream and if it is not, whether or not there is outside air preconditioning.
+
+\begin{itemize}
+\item
+  Coil in outside air stream: \(T_{air,in,des} = T_{out,cool,at-peak}\) (the outside air temperature set at the design cooling peak).
+\item
+  Coil in main air stream, no preconditioning of outside air: \(T_{air,in,des} = T_{mix,cool,at-peak}\) (the mixed air temperature at the cooling design peak).
+\item
+  Coil in main air stream, outside air preconditioned. The outside air fraction is calculated as \(f_{oa} = \dot V_{air,out,des}/\dot V_{cc,air}\) , where \(\dot V_{cc,air}\) is calculated above. Then \(T_{air,in,des} = f_{oa}T_{precool}+\left(1-f_{oa}\right)T_{ret,cool,at-peak}\) , where \(T_{precool}\) is the specified \emph{Precool Design Temperature} from \emph{System:Sizing}, and \(T_{ret,cool,at-peak}\) is the return temperature at the system cooling peak load.
+\end{itemize}
+
+\subsubsection{Design Air Inlet Temperature - Zone Coils}\label{design-air-inlet-temperature---zone-coils}
+
+The design inlet temperature depends on whether the coil is in a terminal unit or a zonal unit, and where the coil is positioned within the unit.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  For the AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction terminal unit the design inlet temperature is set to the zone temperature at the time of the zone cooling peak, since the coil is located in the induced air stream.
+\item
+  For fan coil units the design inlet temperature is set to the mixed air temperature: \(T_{air,in,des} = f_{oa}T_{oa,coolpeak} + \left(1-f_{oa}\right)T_{z,coolpeak}\) , where \(f_{oa} = \rho_a \dot V_{z,oa,des} / \dot m_{z,cool,des}\)
+\item
+  In all other cases the design inlet temperature is set to the zone design cooling coil inlet temperature which is calculated in the zone sizing simulation and is basically the same calculation as the fan coil unit.
+\end{enumerate}
+
+\subsubsection{Design Air Outlet Temperature - System Coils}\label{design-air-outlet-temperature---system-coils}
+
+The outlet air temperature depends on whether the coil is in the outside air stream.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Coil in outside air stream: T\(_{air,out,des}\) = T\(_{sys,des,precool}\) (the specified Precool Design Temperature from the Sizing:System object).
+\item
+  Coil in main air stream: the design outlet air temperature is set to the temperature calculated in the Initial Calculation section above.
+\end{enumerate}
+
+\subsubsection{Design Air Outlet Temperature - Zone Coils}\label{design-air-outlet-temperature---zone-coils}
+
+If the coil is part of an AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction unit, then:
+
+\begin{equation}
+ \begin{array}{rl}
+  \dot{Q}_{coil,des} & = c_{p,air}\rho_{air}\dot{V}_{w,coil,des}\Delta T_{w,des} \\
+  T_1 & = T_{air,in,des} - \dot{Q}_{coil,des} / \left(\rho_{air}c_{p,air}\dot V_{air,coil,des}\right) \\
+  T_2 & = T_{w,out,des} + 2 \\
+  T_{air,out,des} & = \max \left(T_1,T_2\right)
+ \end{array}
+\end{equation}
+
+For all other cases T\(_{air,out,des}\) is set to T\(_{z,sup,des}\) (the zone design supply air temperature as specified in Sizing:Zone).
+
+\subsubsection{Design Inlet Air Humidity Ratio - System Coils}\label{design-inlet-air-humidity-ratio---system-coils}
+
+The design inlet humidity ratio depends on whether the coil is in the outside air stream and if it is not, whether or not there is outside air preconditioning.
+
+\begin{itemize}
+\item
+  Coil in outside air stream: \(W_{air,in,des} = W_{out,cool,at-peak}\) (the outside air humidity ratio at the design cooling peak).
+\item
+  Coil in main air stream, no preconditioning of outside air: \(W_{air,in,des} = W_{mix,cool,at-peak}\) (the mixed air humidity ratio at the cooling design peak).
+\item
+  Coil in main air stream, outside air preconditioned. The outside air fraction is calculated as \(f_{oa} = \dot V_{air,out,des}/\dot V_{cc,air}\) , where \(\dot V_{cc,air}\) is calculated above. Then \(W_{air,in,des} = f_{oa}W_{precool}+\left(1-f_{oa}\right)W_{ret,cool,at-peak}\) , where \(W_{precool}\) is the specified \emph{Precool Design Humidity Ratio} from \emph{System:Sizing}, and \(W_{ret,cool,at-peak}\) is the return humidity ratio at the system cooling peak load.
+\end{itemize}
+
+\subsubsection{Design Air Inlet Humidity Ratio - Zone Coils}\label{design-air-inlet-humidity-ratio---zone-coils}
+
+The design inlet humidity ratio depends on whether the coil is in a terminal unit or a zonal unit, and where the coil is positioned within the unit.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  For the AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction terminal unit the design inlet humidity ratio is set to the zone humidity ratio at the time of the zone cooling peak, since the coil is located in the induced air stream.
+\item
+  For fan coil units the design inlet humidity ratio is set to the mixed air humidity ratio: \(W_{air,in,des} = f_{oa}W_{oa,coolpeak} + \left(1-f_{oa}\right)W_{z,coolpeak}\) , where \(f_{oa} = \rho_a \dot V_{z,oa,des} / \dot m_{z,cool,des}\)
+\item
+  In all other cases the design inlet humidity ratio is set to the zone design cooling coil inlet hunidity ratio which is calculated in the zone sizing simulation and is basically the same calculation as the fan coil unit.
+\end{enumerate}
+
+\subsubsection{Design Outlet Air Humidity Ratio - System Coils}\label{design-outlet-air-humidity-ratio---system-coils}
+
+The outlet air humidity ratio depends on whether the coil is in the outside air stream.
+
+\begin{itemize}
+\item
+  Coil in outside air stream: W\(_{air,out,des}\) = W\(_{sys,des,precool}\) (the specified Precool Design Humidity Ratio from the Sizing:System object)
+\item
+  Coil in main air stream: W\(_{air,out,des}\) = PsyWFnTdbRhPb(T\(_{air,out,des}\),0.9,P\(_{air,std}\)), where PsyWFnTdbRhPb is the EnergyPlus psychrometric function to calculate humidity ratio from drybulb temperature, relative humidity, and atmospheric pressure. The design outlet humidity ratio is being set to the humidity ratio at 90\% relative humidity and design outlet temperature.
+\end{itemize}
+
+\subsubsection{Design Outlet Air Humidity Ratio - Zone Coils}\label{design-outlet-air-humidity-ratio---zone-coils}
+
+\begin{itemize}
+\tightlist
+\item
+  If the coil is part of an AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction unit, then:
+\end{itemize}
+
+\begin{lstlisting}
+-   Get the dewpoint temperature at W$_{air,in,des}$: $T_{dp,in} = \text{PsyTdpFnWPb}\left(W_{air,in,des},P_{air,std}\right)$
+\end{lstlisting}
+
+\begin{lstlisting}
+-   If T$_{dp,in}$ < = T$_{w,in,des}$ set W$_{air,out,des}$ = W$_{air,in,des}$. Otherwise set W$_{air,out,des}$ = min(PsyWFnTdbRhPb(T$_{air,out,des}$,0.9,P$_{air,std}$),W$_{air,in,des}$)
+\end{lstlisting}
+
+\subsubsection{Design Inlet Water Temperature - System Coils}\label{design-inlet-water-temperature---system-coils}
+
+The Design Inlet Water Temperature is set to the Design Loop Exit Temperature specified in the Sizing:Plant object for the water loop serving this coil.
+
+\subsubsection{Design Inlet Water Temperature - Zone Coils}\label{design-inlet-water-temperature---zone-coils}
+
+The Design Inlet Water Temperature is set to the Design Loop Exit Temperature specified in the Sizing:Plant object for the water loop serving this coil.
+
+\subsection{Coil:Cooling:Water:DetailedGeometry Sizing}\label{coilcoolingwaterdetailedgeometry-sizing}
+
+The sizing is done in subroutine \emph{SizeWaterCoil}
+
+\subsubsection{Max Water Flow Rate of Coil}\label{max-water-flow-rate-of-coil}
+
+The calculation is identical to that done for \emph{Coil:Cooling:Water}.
+
+\subsubsection{Number of Tubes per Row}\label{number-of-tubes-per-row}
+
+\begin{equation}
+Ntube/row = {\mathop{\rm Int}\nolimits} ({\rm{13750}}\cdot \dot Vcoil,water,max)
+\end{equation}
+
+\emph{N\(_{tube/row}\)} = \textbf{Max}(\emph{N\(_{tube/row}\)},3)
+
+\subsubsection{Fin Diameter}\label{fin-diameter}
+
+Depending on the duct type, get the coil design air flow rate.
+
+For duct type = \emph{main, other} or default
+
+\begin{equation}
+\dot mair,des = \rho air\cdot DesMainVolFlowsys
+\end{equation}
+
+for duct type = \emph{cooling}
+
+\begin{equation}
+\dot mair,des = \rho air\cdot DesCoolVolFlowsys
+\end{equation}
+
+for duct type = \emph{heating}
+
+\begin{equation}
+\dot mair,des = \rho air\cdot DesHeatVolFlowsys
+\end{equation}
+
+\begin{equation}
+Dfin = 0.335\cdot \dot mair,des
+\end{equation}
+
+\subsubsection{Minimum Air Flow Area}\label{minimum-air-flow-area}
+
+Depending on the duct type, get the coil design air flow rate.
+
+For duct type = \emph{main, other} or default
+
+\begin{equation}
+\dot mair,des = \rho air\cdot DesMainVolFlowsys
+\end{equation}
+
+for duct type = \emph{cooling}
+
+\begin{equation}
+\dot mair,des = \rho air\cdot DesCoolVolFlowsys
+\end{equation}
+
+for duct type = \emph{heating}
+
+\begin{equation}
+\dot mair,des = \rho air\cdot DesHeatVolFlowsys
+\end{equation}
+
+\begin{equation}
+AMinAirFlow = 0.44\cdot \dot mair,des
+\end{equation}
+
+\subsubsection{Fin Surface Area}\label{fin-surface-area}
+
+Depending on the duct type, get the coil design air flow rate.
+
+For duct type = \emph{main, other} or default
+
+\begin{equation}
+\dot mair,des = \rho air\cdot DesMainVolFlowsys
+\end{equation}
+
+for duct type = \emph{cooling}
+
+\begin{equation}
+\dot mair,des = \rho air\cdot DesCoolVolFlowsys
+\end{equation}
+
+for duct type = \emph{heating}
+
+\begin{equation}
+\dot mair,des = \rho air\cdot DesHeatVolFlowsys
+\end{equation}
+
+\begin{equation}
+AFinSurf = 78.5\cdot \dot mair,des
+\end{equation}
+
+\subsubsection{Total Tube Inside Area}\label{total-tube-inside-area}
+
+\emph{A\(_{tube,total\, inside}\)} = 4.4 *\emph{D\(_{tube,inside}\)} *\emph{N\(_{tube\, rows}\)} *\emph{N\(_{tubes/row}\)}
+
+Where \emph{D\(_{tube,inside}\)} is the tube inside diameter.
+
+\subsubsection{Tube Outside Surf Area}\label{tube-outside-surf-area}
+
+\emph{A\(_{tube,outside}\)} = 4.1 *\emph{D\(_{tube,outside}\)} *\emph{N\(_{tube\, rows}\)} *\emph{N\(_{tubes/row}\)}
+
+Where \emph{D\(_{tube,outside}\)} is the tube outside diameter.
+
+\subsubsection{Coil Depth}\label{coil-depth}
+
+\emph{Depth\(_{coil}\)} = \emph{Depth\(_{tube\, spacing}\)} * \emph{N\(_{tube\, rows}\)}
+
+\subsection{Coil:Cooling:WaterToAirHeatPump:EquationFit Sizing}\label{coilcoolingwatertoairheatpumpequationfit-sizing}
+
+The sizing is done in subroutine \emph{SizeHVACWaterToAir}
+
+\subsubsection{Rated Air Flow Rate}\label{rated-air-flow-rate}
+
+The calculation is identical to that done for \emph{Coil:Cooling:Water}.
+
+\subsubsection{Rated Water Flow Rate}\label{rated-water-flow-rate}
+
+The calculation is identical to that done for \emph{Coil:Cooling:Water}, which is the coil design load divided by the \emph{Loop Design Temperature Difference} user input from \emph{Sizing:Plant.} If there is a companion heating coil, the heating coil design load is used so that both modes will have the same rated water flow rate. For sizing the plant loop serving this coil, only one half of this flow rate is used since both the cooling and heating coil will save a flow rate but only one of these coils will operate at a time.
+
+\subsubsection{Rated Total Cooling Capacity}\label{rated-total-cooling-capacity}
+
+The calculation for coil operating temperatures (inlet and outlet) are identical to that done for \emph{Coil:Cooling:Water}. The following calculations are then performed to determine the rated total cooling capacity.
+
+\begin{equation}
+  T_{WB,ratio} = \frac{T_{WB,air,in,des}+273.15C}{283.15C}
+\end{equation}
+
+\begin{equation}
+  T_{S,ratio} = \frac{29.44C+273.15C}{283.15C}
+\end{equation}
+
+where:
+
+$T_{WB,ratio} = $ ratio of load-side inlet air wet-bulb temperature in Kelvin to a reference temperature
+
+$T_{S,ratio} = $ ratio of source-side inlet water temperature in Kelvin to a reference temperature
+
+TCC1 = user input for Total Cooling Capacity Coefficient 1
+
+TCC2 = user input for Total Cooling Capacity Coefficient 2
+
+TCC3 = user input for Total Cooling Capacity Coefficient 3
+
+TCC4 = user input for Total Cooling Capacity Coefficient 4
+
+TCC5 = user input for Total Cooling Capacity Coefficient 5
+
+\begin{equation}
+TotCapTempModFac = \,TCC1 + TCC2\left( {{T_{WB,ratio}}} \right) + TCC3\left( {{T_{S,ratio}}} \right) + TCC4 + TCC5
+\end{equation}
+
+The 4\(^{th}\) and 5\(^{th}\) coefficient (TCC4 and TCC5) used in the above equation are multipliers for the load-side and source-side flow ratios, respectively. For sizing, these ratios are assumed to be 1.
+
+The enthalpy of the entering air is then compared with the enthalpy of the exiting air. The calculations for air enthalpy are identical to that done for \emph{Coil:Cooling:Water}. If the entering air enthalpy is less than the exiting air enthalpy, a reference value of 48,000 J/kg is used as the entering air enthalpy. If the TotCapTempModFac calculation above yields 0 as the result, a value of 1 is used in the following calculation. If the design air mass flow rate is determined to be less than a very small flow value (0.001 kg/s) or the capacity calculated here is less than 0, the coil total cooling capacity is set equal to 0.
+
+\begin{equation}
+  \dot{Q}_{coil,des,total}   = \left\{
+                                  \begin{array}{cl}
+                                    \frac{\dot{m}_{air,des}\PB{H_{in}-H_{out}}}{TotCapTempModFac}  & if H_{in}>H_{out} \\
+                                    \frac{\dot{m}_{air,des}\PB{48000 -H_{out}}}{TotCapTempModFac}  & otherwise
+                                  \end{array}
+                                \right.
+\end{equation}
+
+\subsubsection{Rated Sensible Cooling Capacity}\label{rated-sensible-cooling-capacity}
+
+The calculation for coil operating temperatures (inlet and outlet) are identical to that done for \emph{Coil:Cooling:Water}. The following calculations are then performed to determine the rated sensible cooling capacity.
+
+\begin{equation}
+  T_{DB,ratio} = \frac{T_{DB,air,in,des}+273.15C}{283.15C}
+\end{equation}
+
+\begin{equation}
+  T_{S,ratio} = \frac{29.44C+273.15C}{283.15C}
+\end{equation}
+
+where:
+
+\$\{T\_\{DB,ratio\}\} = \$ ratio of load-side inlet air dry-bulb temperature in Kelvin to a reference temperature
+
+SCC1 = user input for Sensible Cooling Capacity Coefficient 1
+
+SCC2 = user input for Sensible Cooling Capacity Coefficient 2
+
+SCC3 = user input for Sensible Cooling Capacity Coefficient 3
+
+SCC4 = user input for Sensible Cooling Capacity Coefficient 4
+
+SCC5 = user input for Sensible Cooling Capacity Coefficient 5
+
+SCC6 = user input for Sensible Cooling Capacity Coefficient 6
+
+\begin{equation}
+  \begin{array}{rl}
+    SensCapTempModFac &= SCC1 + SCC2\left( {{T_{DB,ratio}}} \right) + SCC3\left( {{T_{WB,ratio}}} \right) \\
+                      &+ SCC4\left( {{T_{S,ratio}}} \right) + SCC5 + SCC6
+  \end{array}
+\end{equation}
+
+The 5\(^{th}\) and 6\(^{th}\) coefficient (SCC5 and SCC6) used in the above equation are multipliers for the load-side and source-side flow ratios, respectively. For sizing, these ratios are assumed to be 1.
+
+The dry-bulb temperature of the entering air is then compared with the dry-bulb temperature of the exiting air. The calculations for air dry-bulb temperature are identical to that done for \emph{Coil:Cooling:Water}. If the entering air dry-bulb temperature is less than the exiting air dry-bulb temperature, a reference value of 24 C is used as the entering air dry-bulb temperature. If the SensCapTempModFac calculation above yields 0 as the result, a value of 1 is used in the following calculation. If the design air mass flow rate is determined to be less than a very small flow value (0.001 kg/s) or the capacity calculated here is less than 0, the coil sensible cooling capacity is set equal to 0.
+
+\begin{equation}
+  \dot{Q}_{coil,des,sensible} = \left\{
+                                  \begin{array}{cl}
+                                    \frac{\dot{m}_{air,des}C_{p,air,des}\PB{T_{DB,in}-T_{DB,out}}}{SensCapTempModFac}  & if T_{DB,in}>T_{DB,out} \\
+                                    \frac{\dot{m}_{air,des}C_{p,air,des}\PB{24       -T_{DB,out}}}{SensCapTempModFac}  & otherwise
+                                  \end{array}
+                                \right.
+\end{equation}
+
+\subsection{Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit Sizing}\label{coilcoolingwatertoairheatpumpvariablespeedequationfit-sizing}
+
+For the cooling coil of VS WSHP, we specify a nominal speed level. During the sizing calculation, the Rated Air Volume Flow Rate, the Rated Water Volume Flow Rate and the Rated Total Cooling Capacity at the Selected Nominal Speed Level are determined in the same way as the \emph{Coil:Cooling:WaterToAirHeatPump:EquationFit} object. The sensible heat transfer rate is not allowed for auto-sizing, instead, it is a function of the rated air and water flow rates, rated total cooling capacity and the Reference Unit SHR at the nominal speed level. The default nominal speed level is the highest speed. However, the model allows the user to select a nominal speed level rather than the highest.
+
+\subsubsection{Rated Air Flow Rate}\label{rated-air-flow-rate-1}
+
+The calculation is identical to that done for \emph{Coil:Cooling:WaterToAirHeatPump:EquationFit}.
+
+\subsubsection{Rated Water Flow Rate}\label{rated-water-flow-rate-1}
+
+The calculation is identical to that done for \emph{Coil:Cooling:WaterToAirHeatPump:EquationFit} , which is the coil design load divided by the \emph{Loop Design Temperature Difference} user input from \emph{Sizing:Plant.} If there is a companion heating coil, the heating coil design load is used so that both modes will have the same rated water flow rate. For sizing the plant loop serving this coil, only one half of this flow rate is used since both the cooling and heating coil will save a flow rate but only one of these coils will operate at a time.
+
+\subsubsection{Rated Total Cooling Capacity}\label{rated-total-cooling-capacity-1}
+
+The calculation for coil operating temperatures (inlet and outlet) are identical to that done for \emph{Coil:Cooling:WaterToAirHeatPump:EquationFit}. The calculations for air enthalpy are similar to that done for \emph{Coil:Cooling:WaterToAirHeatPump:EquationFit.} The difference is in calculating the total cooling capacity temperature modifier function at the selected nominal speed level, as below:
+
+\begin{equation}
+TotCapTempModFra{c_{NominalSpeed}} = {\rm{a}} + {\rm{b*}}W{B_i} + c*WB_i^2 + {\rm{d*EWT}} + e*EW{T^2} + f*W{B_i}*EWT
+\end{equation}
+
+where
+
+WB\(_{i}\) = wet-bulb temperature of the air entering the heating coil, degC
+
+EWT = entering water temperature, degC
+
+a-f = regression curve-fit coefficients.
+
+If the entering air enthalpy is less than the exiting air enthalpy, a reference value of 48,000 J/kg is used as the entering air enthalpy. If the \emph{TotCapTempModFac} calculation above yields 0 as the result, a value of 1 is used in the following calculation. If the rated air mass flow rate is determined to be less than a very small flow value (0.001 kg/s) or the capacity calculated here is less than 0, the coil total cooling capacity is set equal to 0.
+
+\emph{If H\(_{in}\) \textgreater{} H\(_{out}\) Then}
+
+\begin{equation}
+{\dot Q_{coil,rated,total}} = {m_{air,rated}}({H_{in}} - {H_{out}})/TotCapTempModFra{c_{NominalSpeed}}
+\end{equation}
+
+\emph{Else}
+
+\begin{equation}
+{\dot Q_{coil,rated,total}} = {m_{air,rated}}(48000 - {H_{out}})/TotCapTempModFra{c_{NominalSpeed}}
+\end{equation}
+
+\emph{End If}
+
+\subsection{Coil:Heating:WaterToAirHeatPump:EquationFit Sizing}\label{coilheatingwatertoairheatpumpequationfit-sizing}
+
+The sizing is done in subroutine \emph{SizeHVACWaterToAir.}
+
+\subsubsection{Rated Air Flow Rate}\label{rated-air-flow-rate-2}
+
+The calculation is identical to that done for \emph{Coil:Cooling:Water}.
+
+\subsubsection{Rated Water Flow Rate}\label{rated-water-flow-rate-2}
+
+The calculation is identical to that done for \emph{Coil:Cooling:Water} , which is the coil design load divided by the \emph{Loop Design Temperature Difference} user input from \emph{Sizing:Plant.} For sizing the plant loop serving this coil, only one half of this flow rate is used since both the cooling and heating coil will save a flow rate but only one of these coils will operate at a time.
+
+\subsubsection{Rated Total Heating Capacity}\label{rated-total-heating-capacity}
+
+The rated total heating capacity is set equal to the rated total cooling capacity.
+
+\subsection{Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit Sizing}\label{coilheatingwatertoairheatpumpvariablespeedequationfit-sizing}
+
+For the heating coil of VS WSHP, we specify a nominal speed level. During the sizing calculation, the Rated Air Volume Flow Rate and the Rated Water Volume Flow Rate are determined in the same way as the \emph{Coil:Heating:WaterToAirHeatPump:EquationFit} object. On the other hand, the Rated Heating Capacity at the Selected Nominal Speed Level should be the same as the total cooling capacity of its corresponding cooling coil, which has to be sized first. The default nominal speed level will be the highest speed. However, the model allows the user to select a nominal speed level rather than the highest.
+
+\subsubsection{Rated Air Flow Rate}\label{rated-air-flow-rate-3}
+
+The calculation is identical to that done for Coil:Cooling:WaterToAirHeatPump:EquationFit.
+
+\subsubsection{Rated Water Flow Rate}\label{rated-water-flow-rate-3}
+
+The calculation is identical to that done for Coil:Cooling:WaterToAirHeatPump:EquationFit, which is the coil design load divided by the \emph{Loop Design Temperature Difference} user input from \emph{Sizing:Plant.} For sizing the plant loop serving this coil, only one half of this flow rate is used since both the cooling and heating coil will save a flow rate but only one of these coils will operate at a time.
+
+\subsubsection{Rated Total Heating Capacity}\label{rated-total-heating-capacity-1}
+
+The rated total heating capacity is set equal to the rated total cooling capacity.
+
+\subsection{Coil:Heating:Water Sizing}\label{coilheatingwater-sizing}
+
+The sizing is done in subroutine \emph{SizeWaterCoil}.
+
+\subsubsection{Max Water Flow Rate of Coil}\label{max-water-flow-rate-of-coil-1}
+
+\paragraph{System Coils}\label{system-coils}
+
+With the coil load from the system design data array and the user specified (in a Sizing:Plant object) design hot water temperature fall, calculate the max water flow rate:
+
+\begin{equation}
+\dot Vcoil,water,max = HeatCapsys/(Cp,water\cdot \rho water\cdot \Delta Tplt,hw,des)
+\end{equation}
+
+\paragraph{Zone Coils}\label{zone-coils}
+
+Using the zone design coil inlet and supply air conditions calculate the design coil load.
+
+If the coil is not part of an induction unit then obtain the coil inlet temperature from the zone design data array;
+
+\emph{T\(_{in,air}\) = DesHeatCoilInTemp\(_{zone}\)}
+
+If the coil is part of an induction unit take into account the induced air:
+
+\emph{Frac\(_{minflow}\)} = \emph{MinFlowFrac\(_{zone}\)}
+
+\emph{T\(_{in,air}\)} = \emph{DesHeatCoilInTemp\(_{zone}\)} * \emph{Frac\(_{minflow}\)} +
+
+\emph{ZoneTempAtHeatPeak\(_{zone}\)} *(1- \emph{Frac\(_{minflow}\)})
+
+\emph{T\(_{out,air}\) = HeatDesTemp\(_{zone}\)}
+
+W\emph{\(_{out,air}\) = HeatDesHumRat\(_{zone}\)}
+
+If the coil is part of a terminal unit the mass flow rate is determined by the volumetric flow rate of the terminal unit:
+
+\begin{equation}
+\dot mair,des = \rho air\cdot \dot mair,des,tu
+\end{equation}
+
+Otherwise the design flow is obtained from the zone design data array:
+
+\begin{equation}
+\dot mair,des = DesHeatMassFlowzone
+\end{equation}
+
+\begin{equation}
+Qcoil,des = cp,air\dot mair,des\cdot (Tout,air - Tin,air)
+\end{equation}
+
+Here \emph{c\(_{p,air}\)} is calculated at the outlet humidity and the average of the inlet and outlet temperatures.
+
+With the coil load and the user specified (in a Sizing:Plant object) design hot water temperature decrease, calculate the max water flow rate:
+
+\begin{equation}
+\dot Vcoil,water,max = Qcoil,des/(Cp,water\cdot \rho water\cdot \Delta Tplt,hw,des)
+\end{equation}
+
+\subsubsection{UA of the Coil}\label{ua-of-the-coil}
+
+To obtain the UA of the coil, we specify the model inputs (other than the UA) at design conditions and the design coil load that the coil must meet. Then we numerically invert the coil model to solve for the UA that will enable the coil to meet the design coil load given the specified inputs.
+
+\paragraph{System Coils}\label{system-coils-1}
+
+The design coil load is the system design sensible cooling capacity;
+
+\emph{Q\(_{coil,des}\)} = \emph{HeatCap\(_{sys}\)}
+
+The required inputs for the simple coil model are:
+
+\emph{T\(_{in,air}\)} = \emph{HeatMixTemp\(_{sys}\)}
+
+\emph{W\(_{in,air}\)} = \emph{HeatMixHumRat\(_{sys}\)}
+
+\emph{T\(_{in,water}\)} = \emph{ExitTemp\(_{plt,hw,des}\)}
+
+\begin{equation}
+\dot min,water = \rho water\cdot \dot Vcoil,water,max
+\end{equation}
+
+Depending on the duct type, get the coil design air flow rate.
+
+For duct type = \emph{main, other} or default
+
+\emph{\(\dot min,air = \rho air\cdot DesMainVolFlowsys\)}
+
+for duct type = \emph{cooling}
+
+\emph{\(\dot min,air = \rho air\cdot DesCoolVolFlowsys\)}
+
+for duct type = \emph{heating}
+
+\begin{equation}
+\dot min,air = \rho air\cdot DesHeatVolFlowsys
+\end{equation}
+
+We now have all the data needed to obtain UA. The numerical inversion is carried out by calling subroutine \emph{SolveRegulaFalsi}. This is a general utility routine for finding the zero of a function. In this case it finds the UA that will zero the residual function - the difference between the design coil load and the coil output divided by the design coil load. The residual is calculated in the function \emph{SimpleHeatingCoilUAResidual}.
+
+\paragraph{Zone Coils}\label{zone-coils-1}
+
+If the coil is not part of an induction unit then obtain the coil inlet temperature from the zone design data array;
+
+\emph{T\(_{in,air}\) = DesHeatCoilInTemp\(_{zone}\)}
+
+If the coil is part of an induction unit take into account the induced air:
+
+\emph{Frac\(_{minflow}\)} = \emph{MinFlowFrac\(_{zone}\)}
+
+\emph{T\(_{in,air}\)} = \emph{DesHeatCoilInTemp\(_{zone}\)} * \emph{Frac\(_{minflow}\)} +
+
+\emph{ZoneTempAtHeatPeak\(_{zone}\)} *(1- \emph{Frac\(_{minflow}\)})
+
+\emph{W\(_{in,air}\)} = \emph{DesHeatCoilInHumRat\(_{zone}\)}
+
+\emph{T\(_{in,water}\)} = \emph{ExitTemp\(_{plt,hw,des}\)}
+
+\begin{equation}
+\dot min,water = \rho water\cdot \dot Vcoil,water,max
+\end{equation}
+
+\emph{T\(_{out,air}\) = HeatDesTemp\(_{zone}\)}
+
+W\emph{\(_{out,air}\) = HeatDesHumRat\(_{zone}\)}
+
+If the coil is part of a terminal unit the mass flow rate is determined by the volumetric flow rate of the terminal unit:
+
+\begin{equation}
+\dot mair,des = \rho air\cdot \dot mair,des,tu
+\end{equation}
+
+Otherwise the design flow is obtained from the zone design data array:
+
+\begin{equation}
+\dot mair,des = DesHeatMassFlowzone
+\end{equation}
+
+\begin{equation}
+\dot Qcoil,des = cp,air\cdot \dot mair,des\cdot (Tout,air - Tin,air)
+\end{equation}
+
+Here \emph{c\(_{p,air}\)} is calculated at the outlet humidity and the average of the inlet and outlet temperatures.
+
+We now have all the data needed to obtain UA. The numerical inversion is carried out by calling subroutine \emph{SolveRegulaFalsi}. This is a general utility routine for finding the zero of a function. In this case it finds the UA that will zero the residual function - the difference between the design coil load and the coil output divided by the design coil load. The residual is calculated in the function \emph{SimpleHeatingCoilUAResidual}.
+
+\subsection{Coil:Heating:Steam Sizing}\label{coilheatingsteam-sizing}
+
+The sizing is done in subroutine \emph{SizeSteamCoil}.
+
+\subsubsection{Maximum Steam Flow Rate}\label{maximum-steam-flow-rate}
+
+\paragraph{System Coils}\label{system-coils-2}
+
+The maximum steam volumetric flow rate is calculated using:
+
+\begin{equation}
+{\dot V_{coil,steam,max}}\,\,\, = \,\,\,\,\,\frac{{Loa{d_{coil,des}}}}{{{\rho_{steam}}\left( {{h_{fg}} + {c_{p,w}}\cdot \Delta {T_{sc}}} \right)}}
+\end{equation}
+
+The steam density (\({\rho_{steam}}\) ) is for saturated steam at 100 degC (101325.0 Pa) and \emph{h\(_{fg}\)} is the latent heat of vaporization of water at 100 degC (101325.0 Pa). \emph{C\(_{p,w}\)} is the heat capacity of saturated water (condensate) at 100 degC (101325.0 Pa) and \(\Delta {T_{sc}}\) is the Degree of Subcooling defined in the Coil:Heating:Steam object input. The design coil load \emph{Load\(_{coil,des}\)} is calculated from:
+
+\begin{equation}
+Loa{d_{coil,des}} = {\dot m_{air,des}}({c_{p,air}})({T_{air,coil,des,out}} - {T_{air,coil,des,in}})
+\end{equation}
+
+The design air mass flow rate depends on the location of the coil (duct type). For duct type = \emph{main,} the flow rate is set to \emph{r\(_{air}\)} *\emph{DesMainVolFlow\(_{sys}\)} *\emph{MinSysAirFlowRatio}. If the coil is in a cooling duct the flow rate is set to \emph{r\(_{air}\)} *\emph{DesCoolVolFlow\(_{sys}\)} *\emph{MinSysAirFlowRatio}. If the coil is in a heating duct the flow rate is set to \emph{r\(_{air}\)} *\emph{DesHeatVolFlow\(_{sys}\)}. If the coil is in any other kind of duct, the flow rate is set to \emph{r\(_{air}\)} *\emph{DesMainVolFlow\(_{sys}\)}.
+
+For sizing, the design outlet air temperature (\emph{T\(_{air,coil,des,out}\)}) is the Central Heating Design Supply Air Temperature specified in the Sizing:System object.
+
+The design inlet air temperature depends on whether the coil is being sized for 100\% outdoor air or minimum outdoor air flow (per 100\% Outdoor Air in Heating input field in the Sizing:System object).
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\tightlist
+\item
+  Sizing based on 100\% Outdoor Air in Heating
+\end{enumerate}
+
+\emph{T\(_{air,coil,des,in}\)} = \emph{HeatOutTemp\(_{sys}\)} (the outdoor air temperature at the design heating peak)
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Sizing based on minimum outdoor air flow. The outdoor air fraction is calculated as \emph{Frac}\(_{oa}\) = \emph{DesOutAirVolFlow\(_{sys}\)} / \emph{DesVolFlow}. \emph{DesVolFlow} is \({{{{\mathop m\limits^ \bullet }_{air,des}}} \mathord{\left/ {\vphantom {{{{\mathop m\limits^ \bullet }_{air,des}}} {{\rho_{air}}}}} \right. } {{\rho_{air}}}}\) \emph{.}
+\end{enumerate}
+
+\emph{T\(_{air,coil,des,in}\)} = \emph{Frac}\(_{oa}\)* * HeatOutTemp\(_{sys}\)* + (1.- \emph{Frac\(_{oa}\)}) *\emph{HeatRetTemp\(_{sys}\)} (see Table~\ref{table:system-sizing-data}. System Sizing Data)
+
+\paragraph{Zone Coils}\label{zone-coils-2}
+
+If the coil is part of an \emph{AirTerminal:SingleDuct:*} unit (e.g., \emph{Air\-Terminal:\-Single\-Duct:\-Constant\-Volume\-:Re\-heat, Air\-Terminal:\-Single\-Duct:\-VAV:\-Re\-heat, Air\-Terminal:\-Single\-Duct:\-Series\-PIU:\-Re\-heat, etc.)}, the maximum steam flow rate is set equal to the terminal unit's maximum steam flow rate. Otherwise (e.g., the zone-level coil is part of \emph{Zone\-HVAC:\-Packaged\-Terminal\-Air\-Conditioner, Zone\-HVAC\-:Unit\-Ventilator, Zone\-HVAC\-:Unit\-Heater or Zone\-HVAC:\-Ventilated\-Slab}) the calculation is similar to that at the system level. A design load is calculated:
+
+\begin{equation}
+Loa{d_{coil,des}} = {\dot m_{air,des}}({c_{p,air}})({T_{air,coil,des,out}} - {T_{air,coil,des,in}})
+\end{equation}
+
+where:
+
+\({\dot m_{air,des}}\) = \emph{DesHeatMassFlow\(_{zone}\)} (see Table~\ref{table:zone-sizing-data}. Zone Sizing Data)
+
+\emph{T\(_{air,coil,des,in}\)} = \emph{DesHeatCoilInTemp\(_{zone}\)} (see Table~\ref{table:zone-sizing-data})
+
+\emph{T\(_{air,coil,des,out}\)} = \emph{HeatDesTemp\(_{zone}\)} (user input from Sizing:Zone object)
+
+\({c_{p,air}}\) = Specific heat of air (evaluated at the average of inlet and outlet air temperatures, and at the zone heating design supply air humidity ratio \emph{HeatDesHumRat\(_{zone}\)} {[}user input from Sizing:Zone object{]})
+
+\begin{equation}
+{\dot V_{coil,steam,max}}\,\,\, = \,\,\,\,\,\frac{{Loa{d_{coil,des}}}}{{{\rho_{steam}}\left( {{h_{fg}} + {c_{p,w}}\cdot \Delta {T_{sc}}} \right)}}
+\end{equation}
+
+The terms in the denominator of this equation (\emph{�\(_{steam}\)}, \emph{h\(_{fg}\)}, etc.) are evaluated in the same way as described above for steam System Coils.
+
+\subsection{Sizing of Gas and Electric Heating Coils}\label{sizing-of-gas-and-electric-heating-coils}
+
+The sizing calculation is done in subroutine \emph{SizeHeatingCoil} in module \emph{HeatingCoils}.
+
+\subsubsection{Nominal Capacity of the Coil}\label{nominal-capacity-of-the-coil}
+
+\paragraph{System Coils}\label{system-coils-3}
+
+The value is obtained from the system design array.
+
+\emph{Cap\(_{nom}\)} = \emph{HeatCap\(_{sys}\)}
+
+\paragraph{Zone Coils}\label{zone-coils-3}
+
+The capacity is calculated from the design coil inlet and outlet conditions.
+
+If the coil is not part of an induction unit then obtain the coil inlet temperature from the zone design data array;
+
+\emph{T\(_{in,air}\) = DesHeatCoilInTemp\(_{zone}\)}
+
+If the coil is part of an induction unit take into account the induced air:
+
+\emph{Frac\(_{minflow}\)} = \emph{MinFlowFrac\(_{zone}\)}
+
+\emph{T\(_{in,air}\)} = \emph{DesHeatCoilInTemp\(_{zone}\)} * \emph{Frac\(_{minflow}\)} +
+
+\emph{ZoneTempAtHeatPeak\(_{zone}\)} *(1- \emph{Frac\(_{minflow}\)})
+
+\emph{T\(_{out,air}\) = HeatDesTemp\(_{zone}\)}
+
+W\emph{\(_{out,air}\) = HeatDesHumRat\(_{zone}\)}
+
+\emph{Q\(_{coil,des}\)} = \emph{C\(_{p,air}\)} * \emph{DesHeatMassFlow\(_{zone}\)} *(\emph{T\(_{out,air}\)}-\emph{T\(_{in,air}\)})
+
+Here \emph{c\(_{p,air}\)} is calculated at the outlet humidity and the average of the inlet and outlet temperatures.
+
+\subsection{DX Coil Sizing}\label{dx-coil-sizing}
+
+The sizing calculations are done in subroutine \emph{SizeDXCoil} in module \emph{DXCoils}. This section covers the sizing of the objects
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  Coil:Heating:DX:SingleSpeed
+\item
+  Coil:Cooling:DX:TwoSpeed
+\end{enumerate}
+
+\subsubsection{Rated Air Volume Flow Rate}\label{rated-air-volume-flow-rate}
+
+\subsubsection{System Coils}\label{system-coils-4}
+
+The rated air flow rate is obtained from the system design array.
+
+\begin{equation}
+\dot Vair,rated = DesMainVolFlowsys
+\end{equation}
+
+\subsubsection{Zone Coils}\label{zone-coils-4}
+
+The rated air flow rate is the maximum of the heating and cooling design flow rates from the zone design array.
+
+\begin{equation}
+\dot Vair,rated = Max(DesCoolVolFlowzone,DesHeatVolFlowzone)
+\end{equation}
+
+\subsubsection{Rated Total Cooling Capacity}\label{rated-total-cooling-capacity-2}
+
+\subsubsection{System Coils}\label{system-coils-5}
+
+The rated cooling capacity is obtained by dividing the peak cooling capacity by the \emph{Cooling Capacity Modifier Curve} evaluated at peak mixed wetbulb and outdoor drybulb temperatures.
+
+\emph{T\(_{mix}\)} = \emph{CoolMixTemp\(_{sys}\)}
+
+\emph{W\(_{mix}\)} = \emph{CoolMixHumRat\(_{sys}\)}
+
+\emph{T\(_{sup}\)} = \emph{CoolSupTemp\(_{sys}\)}
+
+\emph{W\(_{sup}\)} = \emph{CoolSupHumRat\(_{sys}\)}
+
+\emph{T\(_{outside}\)} = \emph{CoolOutTemp\(_{sys}\)}
+
+\emph{r\(_{air}\)} = \emph{PsyRhoAirFnPbTdbW}(\emph{p\(_{air,std}\)}, \emph{T\(_{mix}\)},\emph{W\(_{mix}\)})
+
+\emph{h\(_{mix}\)} = \emph{PsyHFnTdbW}(\emph{T\(_{mix}\)},\emph{W\(_{mix}\)})
+
+\emph{h\(_{sup}\)} = \emph{PsyHFnTdbW}(\emph{T\(_{sup}\)},\emph{W\(_{sup}\)})
+
+\emph{T\(_{mix,wb}\)} = \emph{PsyTwbFnTdbWPb}(\emph{T\(_{mix}\)},\emph{W\(_{mix}\)}, \emph{p\(_{air,std}\)})
+
+\emph{CapModFac} = \emph{CurveValue}(CCapFTemp,\emph{T\(_{mix,wb}\)},\emph{T\(_{outside}\)})
+
+\begin{equation}
+CCappeak = \rho air\cdot \dot Vair,rated\cdot (hmix - hsup)
+\end{equation}
+
+\emph{CCap\(_{rated}\)} = \emph{CCap\(_{peak}\)}/ \emph{CapModFac}
+
+We check that the design volume flow per total capacity is within the prescribed range:
+
+\begin{equation}
+FlowCapRatio = \dot Vair,rated/CCaprated
+\end{equation}
+
+If \emph{FlowCapRatio} \textless{} \emph{FlowCapRatio\(_{min}\)} then
+
+\begin{equation}
+CCaprated = \dot Vair,rated/FlowCapRatiomin
+\end{equation}
+
+If \emph{FlowCapRatio} \textgreater{} \emph{FlowCapRatio\(_{max}\)} then
+
+\begin{equation}
+CCaprated = \dot Vair,rated/FlowCapRatiomax
+\end{equation}
+
+where
+
+\emph{FlowCapRatio\(_{min}\)} = 0.00004027 m\(^{3}\)/s per watt (300 cfm/ton)
+
+And
+
+\emph{FlowCapRatio\(_{max}\)} = 0.00006041 m\(^{3}\)/s per watt (450 cfm/ton)
+
+The sizing calculation for DX cooling coils for 100\% dedicated outdor air system (DOAS) are identical to regular DX cooling coils. However, they operate operate at different flow to capacity ratio ranges and are within the prescribed range below:
+
+\emph{FlowCapRatio\(_{min}\)} = 0.00001677 m\(^{3}\)/s per Watt (125 cfm/ton)
+
+And
+
+\emph{FlowCapRatio\(_{max}\)} = 0.00003355 m\(^{3}\)/s per Watt (250 cfm/ton)
+
+\subsubsection{Zone Coils}\label{zone-coils-5}
+
+The rated cooling capacity for zone coils is calculated in the same manner as for system coils.
+
+\emph{T\(_{mix}\)} = \emph{DesCoolCoilInTemp\(_{zone}\)}
+
+\emph{W\(_{mix}\)} = \emph{DesCoolCoilInHumRat\(_{zone}\)}
+
+\emph{T\(_{sup}\)} = \emph{CoolDesTemp\(_{zone}\)}
+
+\emph{W\(_{sup}\)} = \emph{CoolDesHumRat\(_{zone}\)}
+
+\emph{T\(_{outside}\)} = \emph{T\(_{outside}\),\(_{desday,peak}\)}
+
+\emph{r\(_{air}\)} = \emph{PsyRhoAirFnPbTdbW}(\emph{p\(_{air,std}\)}, \emph{T\(_{mix}\)},\emph{W\(_{mix}\)})
+
+\emph{h\(_{mix}\)} = \emph{PsyHFnTdbW}(\emph{T\(_{mix}\)},\emph{W\(_{mix}\)})
+
+\emph{h\(_{sup}\)} = \emph{PsyHFnTdbW}(\emph{T\(_{sup}\)},\emph{W\(_{sup}\)})
+
+\emph{T\(_{mix,wb}\)} = \emph{PsyTwbFnTdbWPb}(\emph{T\(_{mix}\)},\emph{W\(_{mix}\)}, \emph{p\(_{air,std}\)})
+
+\emph{CapModFac} = \emph{CurveValue}(CCapFTemp,\emph{T\(_{mix,wb}\)},\emph{T\(_{outside}\)})
+
+\begin{equation}
+CCappeak = \rho air\cdot \dot Vair,rated\cdot (hmix - hsup)
+\end{equation}
+
+\emph{CCap\(_{rated}\)} = \emph{CCap\(_{peak}\)}/ \emph{CapModFac}
+
+We check that the design volume flow per total capacity is within the prescribed range:
+
+\begin{equation}
+FlowCapRatio = \dot Vair,rated/CCaprated
+\end{equation}
+
+If \emph{FlowCapRatio} \textless{} \emph{FlowCapRatio\(_{min}\)} then
+
+\begin{equation}
+CCaprated = \dot Vair,rated/FlowCapRatiomin
+\end{equation}
+
+If \emph{FlowCapRatio} \textgreater{} \emph{FlowCapRatio\(_{max}\)} then
+
+\begin{equation}
+CCaprated = \dot Vair,rated/FlowCapRatiomax
+\end{equation}
+
+where
+
+\emph{FlowCapRatio\(_{min}\)} = 0.00004027 m\(^{3}\)/s per watt (300 cfm/ton)
+
+And
+
+\emph{FlowCapRatio\(_{max}\)} = 0.00006041 m\(^{3}\)/s per watt (450 cfm/ton)
+
+We check the design flow to the total cooling capacity rato for dedicated zone outdoor unit DX cooling coils to be within the limits prescribed below:
+
+\emph{FlowCapRatio\(_{min}\)} = 0.00001677 m\(^{3}\)/s per Watt (125 cfm/ton)
+
+And
+
+\emph{FlowCapRatio\(_{max}\)} = 0.00003355 m\(^{3}\)/s per Watt (250 cfm/ton)
+
+\subsubsection{Rated Total Heating Capacity}\label{rated-total-heating-capacity-2}
+
+For Coil:Heating:DX:SingleSpeed the rated heating capacity is set equal to the cooling capacity.
+
+\subsubsection{Rated SHR}\label{rated-shr}
+
+The rated sensible heat ratio is calculated to be the sensible cooling (from rated inlet conditions to user specified supply conditions) divided by the total cooling (from rated inlet to specified supply).
+
+\emph{T\(_{in,rated}\)} = 26.6667 \(^{o}\)C (80 \(^{o}\)F)
+
+\emph{W\(_{in,rated}\)} = 0.01125 (corresponds to 80 \(^{o}\)F drybulb, 67 \(^{o}\)F wetbulb)
+
+\emph{C\(_{p,air}\)} = \emph{PsyCpAirFnWTdb}(\emph{W\(_{in,rated}\)}, \emph{T\(_{in,rated}\)})
+
+For system coils
+
+\emph{T\(_{sup}\)} = \emph{CoolSupTemp\(_{sys}\)}
+
+\emph{W\(_{sup}\)} = \emph{CoolSupHumRat\(_{sys}\)}
+
+For zone coils
+
+\emph{T\(_{sup}\)} = \emph{CoolDesTemp\(_{zone}\)}
+
+\emph{W\(_{sup}\)} = \emph{CoolDesHumRat\(_{zone}\)}
+
+Then
+
+\emph{h\(_{rated}\)} = \emph{PsyHFnTdbW}(\emph{T\(_{in,rated}\)}, \emph{W\(_{in,rated}\)})
+
+\emph{h\(_{sup}\)} = \emph{PsyHFnTdbW}(\emph{T\(_{sup}\)}, \emph{W\(_{sup}\)})
+
+\emph{Dh}\(_{rated,sup}\) = \emph{h\(_{rated}\)}-\emph{h\(_{sup}\)}
+
+\emph{DQs\(_{rated,sup}\)} = \emph{C\(_{p,air}\)} *(\emph{T\(_{in,rated}\)}-\emph{T\(_{sup}\)})
+
+\emph{SHR\(_{rated}\)} = \emph{DQs\(_{rated,sup}\)}/\emph{Dh}\(_{rated,sup}\)
+
+\subsubsection{Evaporative Condenser Air Volume Flow Rate}\label{evaporative-condenser-air-volume-flow-rate}
+
+The evaporative condenser air volume flow rate (m\(^{3}\)/s) is set to 0.000114 m\(^{3}\)/s per watt (850 cfm/ton) times the total rated cooling capacity.
+
+\subsubsection{Evaporative Condenser Air Volume Flow Rate, Low Speed}\label{evaporative-condenser-air-volume-flow-rate-low-speed}
+
+The evaporative condenser air volume flow rate, low speed (m\(^{3}\)/s) is set to 1/3 times 0.000114 m\(^{3}\)/s per watt (850 cfm/ton) times the total rated cooling capacity.
+
+\subsubsection{Evaporative Condenser Pump Rated Power Consumption}\label{evaporative-condenser-pump-rated-power-consumption}
+
+The evaporative condenser pump rated power consumption is set equal to the total cooling capacity times 0.004266 watts pump power per watt capacity (15 W/ton).
+
+\subsubsection{Evaporative Condenser Pump Rated Power Consumption, Low Speed}\label{evaporative-condenser-pump-rated-power-consumption-low-speed}
+
+The evaporative condenser pump rated power consumption, low speed, is set equal to 1/3 times the total cooling capacity times 0.004266 watts pump power per watt capacity (15 W/ton).
+
+\subsubsection{Rated Air Volume Flow Rate, low speed}\label{rated-air-volume-flow-rate-low-speed}
+
+The rated air volume flow rate, low speed, is set equal to 1/3 times the full rated air volume flow rate.
+
+\subsubsection{Rated Total Cooling Capacity, Low Speed}\label{rated-total-cooling-capacity-low-speed}
+
+The rated total cooling capacity, low speed, is set equal to 1/3 times the full rated total cooling capacity.
+
+\subsubsection{Rated SHR, low speed}\label{rated-shr-low-speed}
+
+The rated sensible heat ratio, low speed, is set equal to the full speed SHR.
+
+\subsubsection{Resistive Defrost Heater Capacity}\label{resistive-defrost-heater-capacity}
+
+For the heat pump the resistive defrost heat capacity is set equal to the cooling capacity.
+
+\subsection{DX MultiSpeed Coil Sizing}\label{dx-multispeed-coil-sizing}
+
+The sizing calculations are done in subroutine \emph{SizeDXCoil} in module \emph{DXCoils}. This section covers the sizing of the objects
+
+\begin{itemize}
+\item
+  Coil:Heating:DX:MultiSpeed
+\item
+  Coil:Cooling:DX: MultiSpeed
+\end{itemize}
+
+The rated air volume flow rate, rated total cooling capacity, rated heating capacity, rated SHR, evaporative condenser air volume flow rate, evaporative condenser pump rated power consumption at the highest speed are sized in the same ways as DX Coil Sizing.
+
+After the sizes are determined at the highest speed, the sizes in the rest of speeds are assumed to
+
+\begin{equation}
+Valu{e_n} = \frac{n}{{NumberOfSpeed}}*Valu{e_{NumberOfSpeed}}
+\end{equation}
+
+where
+
+Value\(_{n}\) = Any autosizable variable at Speed n, except SHR
+
+SHR\(_{n}\) = SHR\(_{NumberOfSpeed}\)
+
+n = Speed Index number from 1 to NumberOfSpeed-1
+
+NumberOfSpeed = The highest speed number
+
+\subsection{Coil:Cooling:DX:VariableSpeed Sizing}\label{coilcoolingdxvariablespeed-sizing}
+
+For the variable-speed DX cooling coil, we specify a nominal speed level. During the sizing calculation, the Rated Total Cooling Capacity at the Selected Nominal Speed Level is determined in the same way as the Coil:Cooling:DX:SingleSpeed object. If the user chooses to autosize the Rated Air Volume Flow Rate, the flow rate, as compared to the Rated Total Cooling Capacity, is sized to have the same ratio as the air volume flow rate to the total cooling capacity at the nominal speed, of the Reference Unit. The sensible heat transfer rate is not allowed for auto-sizing, instead, it is a function of the rated air flow, rated total cooling capacity and the Reference Unit SHR at the nominal speed level. The default nominal speed level is the highest speed. However, the model allows the user to select a nominal speed level rather than the highest.
+
+\textbf{\emph{Rated Total Cooling Capacity}}
+
+The calculation for coil operating temperatures (inlet and outlet) are identical to that done for Coil:Cooling:DX:SingleSpeed. The calculations for air enthalpy are similar to that done for Coil:Cooling:DX:SingleSpeed\emph{.} The difference is in calculating the total cooling capacity temperature modifier function at the selected nominal speed level, as below:
+
+\begin{equation}
+TotCapTempModFra{c_{NominalSpeed}} = {\rm{a}} + {\rm{b*}}W{B_i} + c*WB_i^2 + {\rm{d*}}D{B_o} + e*D{B_o}{T^2} + f*W{B_i}*D{B_o}
+\end{equation}
+
+where
+
+WB\(_{i}\) = wet-bulb temperature of the air entering thecooling coil, degC
+
+DB\(_{o}\) = condenser entering air temperature, degC
+
+a-f = regression curve-fit coefficients.
+
+If the entering air enthalpy is less than the exiting air enthalpy, a reference value of 48,000 J/kg is used as the entering air enthalpy. If the \emph{TotCapTempModFac} calculation above yields 0 as the result, a value of 1 is used in the following calculation. If the rated air mass flow rate is determined to be less than a very small flow value (0.001 kg/s) or the capacity calculated here is less than 0, the coil total cooling capacity is set equal to 0.
+
+\emph{If H\(_{in}\) \textgreater{} H\(_{out}\) Then}
+
+\begin{equation}
+{\dot Q_{coil,rated,total}} = {m_{air,rated}}({H_{in}} - {H_{out}})/TotCapTempModFra{c_{NominalSpeed}}
+\end{equation}
+
+\emph{Else}
+
+\begin{equation}
+{\dot Q_{coil,rated,total}} = {m_{air,rated}}(48000 - {H_{out}})/TotCapTempModFra{c_{NominalSpeed}}
+\end{equation}
+
+\emph{End If}
+
+The other sizing procedures, e.g.~evaporative condenser pump, etc., are the same as Coil:Cooling:DX:SingleSpeed.
+
+\subsection{Coil:Heating:DX:VariableSpeed Sizing}\label{coilheatingdxvariablespeed-sizing}
+
+For the variable-speed DX heating coil, we specify a nominal speed level. During the sizing calculation, the Rated Heating Capacity at the Selected Nominal Speed Level should be the same as the total cooling capacity of its corresponding cooling coil, which has to be sized first. The default nominal speed level will be the highest speed. However, the model allows the user to select a nominal speed level rather than the highest. If the user chooses to autosize the Rated Air Volume Flow Rate, the flow rate, as compared to the Rated Heating Capacity, is sized to have the same ratio as the air volume flow rate to the heating capacity at the nominal speed, of the Reference Unit. The other sizing procedures are the same as Coil:Heating:DX:SingleSpeed.
+
+\subsection{Pump Sizing}\label{pump-sizing}
+
+The loop pumps' autosizable inputs are design volume flow rate and design power consumption.
+
+\subsubsection{Design Volume Flow Rate}\label{design-volume-flow-rate}
+
+This is set equal to the design flow rate for the loop which is obtained from summing the needs of the components on the demand side of the loop. Each component on the plant loop registers its design flow rate and central routines sum them up.
+
+\subsubsection{Design Power Consumption}\label{design-power-consumption}
+
+There are two methods available for calculating the design flow rate. The pump object has a input field to select which method to use.
+
+The first, and original, method is selected by choosing PowerPerFlowPerPressure. And the design power is calculated using
+
+\begin{equation}
+\dot Q_{nom} = H_{nom} \cdot \dot V_{nom} \cdot ScalingFactor /Eff_{mot}
+\end{equation}
+
+where,
+
+\emph{Eff\(_{mot}\)} is the motor efficiency, often the default value of 0.9. This is defined as the shaft power output in Watts divided by the electric power in Watts.
+
+\emph{V\(_{nom}\)} is the design volume flow rate in m\(^{3}\)/s.
+
+\emph{ScalingFactor} is an input called Design Shaft Power per Unit Flow Rate per Unit Head, with a default of 1.282051 W/((m\(^{3}\)/s)-Pa). (This is the inverse of 0.78 for impeller efficiency that was used prior to version 8.5.)
+
+\emph{H\(_{nom}\)} the nominal head, or pressure rise across the pump, is an input in Pascals.
+
+The second method is selected by choosing PowerPerFlow. Then the power is calculated more simply and does not use head pressure or motor efficiency
+
+\begin{equation}
+\dot Q_{nom} = \dot V_{nom} \cdot ScalingFactor
+\end{equation}
+
+where
+
+\emph{ScalingFactor} is an input called Design Electric Power per Unit Flow Rate, with a default of 348701.1 W/(m\(^{3}\)/s) or 22 W/gpm. The pump motor efficiency and head are still used to model the pump for its fluid heating. This method essentially finds a pump impeller and drive efficiency that when combined with the head and motor efficiency results in the desired power consumption per flow rate.
+
+\subsection{Electric Chiller Sizing}\label{electric-chiller-sizing}
+
+Generally chillers will need nominal cooling capacity, evaporator flow rate and condenser flow rate. All 3 quantities can be straightforwardly obtained using the user specified loop sizing data and the loop design flow rates.
+
+All chillers on a loop are sized to meet the full loop load. If there are multiple chillers on a loop that call for autosizing, they will all be assigned the same cooling capacity and evaporator flow rate.
+
+\subsubsection{Nominal Cooling Capacity}\label{nominal-cooling-capacity}
+
+\begin{equation}
+\dot Qchiller,nom = Cp,w\cdot \rho w\cdot \Delta Tloop,des\cdot \dot Vloop,des
+\end{equation}
+
+where
+
+\emph{C\(_{p,w}\)} is the specific heat of water at 5 \(^{o}\)C;
+
+\emph{r\(_{w}\)} is the density of water at standard conditions (5.05 \(^{o}\)C);
+
+\emph{DT\(_{loop,des}\)} is the chilled water loop design temperature rise;
+
+\(\dot Vloop,des\) is the loop design volumetric flow rate.
+
+\subsubsection{Design Evaporator Volumetric Water Flow Rate}\label{design-evaporator-volumetric-water-flow-rate}
+
+\begin{equation}
+\dot Vevap,des = \dot Vloop,des
+\end{equation}
+
+\subsubsection{Design Condenser Volumetric Water Flow Rate}\label{design-condenser-volumetric-water-flow-rate}
+
+\begin{equation}
+\dot Vcond,des = \dot Qchiller,nom\cdot (1 + 1/COPchiller,nom)/(\Delta Tloop,des\cdot Cp,w\cdot \rho w)
+\end{equation}
+
+where
+
+\emph{C\(_{p,w}\)} is the specific heat of water at design condenser inlet temperature;
+
+\emph{r\(_{w}\)} is the density of water at standard conditions (5.05 \(^{o}\)C);
+
+\emph{DT\(_{loop,des}\)} is the chilled water loop design temperature rise;
+
+\emph{COP\(_{chiller,nom}\)} is the chiller nominal COP.
+
+Boiler Sizing
+
+Generally boilers will need nominal heating capacity and rate. Both quantities can be straightforwardly obtained using the user specified loop sizing data and the loop design flow rates.
+
+All boilers on a loop are sized to meet the full loop load. If there are multiple boilers on a loop that call for autosizing, they will all be assigned the same heating capacity and flow rate.
+
+\subsubsection{Nominal Capacity}\label{nominal-capacity}
+
+\begin{equation}
+\dot Qboiler,nom = Cp,w\cdot \rho w\cdot \Delta Tloop,des\cdot \dot Vloop,des
+\end{equation}
+
+where
+
+\emph{C\(_{p,w}\)} is the specific heat of water at the boiler design outlet temperature;
+
+\emph{r\(_{w}\)} is the density of water at standard conditions (5.05 \(^{o}\)C);
+
+\emph{DT\(_{loop,des}\)} is the hot water loop design temperature decrease;
+
+\(\dot Vloop,des\) is the loop design volumetric flow rate.
+
+\subsubsection{Design Evaporator Volumetric Water Flow Rate}\label{design-evaporator-volumetric-water-flow-rate-1}
+
+\begin{equation}
+\dot Vdes = \dot Vloop,des
+\end{equation}
+
+\subsection{Plant Heat Exchanger Sizing}\label{plant-heat-exchanger-sizing}
+
+The sizing of plant heat exchanger component (object: HeatExchanger:FluidToFluid) involves determining design flow rates for both sides, a UA value, and a nominal capacity for reporting. The component has a sizing factor for fine control and uses the design temperatures defined in the Sizing:Plant object.
+
+The Loop Supply Side design flow rate, \({\dot V_{Sup,des}}\) , is set equal to the design flow rate for that loop, multiplied by the component sizing factor, \({f_{comp}}\) .
+
+\begin{equation}
+{\dot V_{Sup,des}} = {\dot V_{loop,des}}*{f_{comp}}
+\end{equation}
+
+The Loop Demand Side design flow rate,\({\dot V_{Dmd,des}}\) , is set equal to the Loop Supply Side design flow rate.
+
+\begin{equation}
+{\dot V_{Dmd,des}} = {\dot V_{Sup,des}}
+\end{equation}
+
+The design heat transfer capacity and UA for the heat exchanger are calculated using the design temperatures for the two plant loops. The loop design temperature difference for the Loop Supply Side, \(\Delta {T_{SupLoop,Des}}\) , is used to determine a nominal capacity.
+
+\begin{equation}
+\dot Q = {\mathop V\limits^._{Sup,des}}\rho {c_p}\Delta {T_{SupLoop,Des}}
+\end{equation}
+
+A loop-to-loop design temperature difference, \(\Delta {T_{LoopToLoop,Des}}\) , is determined depending on the nature of the plant loop connected to the Loop Supply Side. The Sizing:Plant object includes classifications for the type of loop that include Heating, Steam, Cooling, or Condenser. For Cooling and Condenser loop types, the loop design temperature difference is added to the design exit temperature for the Loop Supply Side, \({T_{SupLoop,Exit}}\) . For Heating and Stem loop types, the loop design temperature difference is subtracted from the design exit temperature. This adjusted supply side temperature is then compared to the design exit temperature for the Loop Demand Side,\({T_{DmdLoop,Exit}}\) .
+
+\(\Delta {T_{LoopToLoop,Des}} = \left( {{T_{SupLoop,Exit}} + \Delta {T_{SupLoop,Des}}} \right) - {T_{DmdLoop,Exit}}\) (Cooling, Condenser)
+
+\(\Delta {T_{LoopToLoop,Des}} = \left( {{T_{SupLoop,Exit}} - \Delta {T_{SupLoop,Des}}} \right) - {T_{DmdLoop,Exit}}\) (Heating, Steam)
+
+\begin{equation}
+\Delta {T_{LoopToLoop,Des}} = MAX\left( {ABS\left( {\Delta {T_{LoopToLoop,Des}}} \right),2.0} \right)
+\end{equation}
+
+The UA (U-Factor Time Area Value) is determined by assuming that the target capacity can be delivered for the loop-to-loop temperature difference which after substituting and rearranging becomes:
+
+\begin{equation}
+UA = \frac{{{{\mathop {V}\limits }_{Sup,des}}\rho {c_p}\Delta {T_{SupLoop,Des}}}}{{\Delta {T_{LoopToLoop,Des}}}}
+\end{equation}
+
+A nominal capacity for the heat exchanger is determined from the design flow rates and UA (regardless of if they were automatically sized or input by the user) and the expected operating temperatures of the two loops. The loop operating temperatures are obtained from the input in Sizing:Plant object if it is present for that loop. If no Sizing:Plant is present then the loop's overall setpoint is used (if the loop's load scheme is DualSetpointDeadband then the average of the high and low setpoints is used). The full heat exchanger model is then calculated for the maximum loop flow rates and expected loop temperatures as inlets to the heat exchanger. The absolute value for the model result for heat transfer rate is then used as the capacity of the heat exchanger. This capacity is reported and may be used for controls based on operation scheme.
+
+\subsection{Humidifier Sizing}\label{humidifier-sizing}
+
+The rated power, or nominal electric power input of an Electric Steam Humidifier (Humidifier:Steam:Electric) is calculated from user specified rated capacity (m\(^{3}\)/s) and the enthalpy change of the water from a reference temperature (20.0 degC) to saturated steam at 100.0 degC. Autosizing procedure assumes that electrical heating element in the humidifier heat the water from the reference temperature and generate saturated steam at 100 degC, and electric to thermal energy conversion efficiency of 100.0\%.
+
+\subsubsection{Rated Power}\label{rated-power}
+
+\begin{equation}
+{P_{rated}} = {\dot V_{rated}} \cdot {\rho_w} \cdot \left( {{h_{fg}} + {C_{p,w}} \cdot \Delta {T_w}} \right)
+\end{equation}
+
+where
+
+\emph{C\(_{p,w}\) is the specific heat of water at average temperature ((100+20)/2 = 60.0} * degC), (J/kgK);*
+
+\emph{r\(_{w}\) is the density of water at standard conditions (5.05} * degC);*
+
+\emph{DT\(_{w}\) is the sensible temperature rise of water (100.0 - 20.0 = 80.0} * degC);*
+
+\emph{\({\dot V_{rated}}\) is the rated capacity of the humidifier in volumetric flow rate.}
+
+\emph{h\(_{fg}\) is the latent heat of vaporization of water at 100.0 degC, (J/kg);}
+
+\subsubsection{Gas Fired Humidifier Sizing}\label{gas-fired-humidifier-sizing}
+
+The rated power, or nominal gas use rate of a gas steam humidifier (Humidifier:Steam:Gas) is calculated from user specified rated volumetric capacity (m3/s) and the enthalpy change of the water from a reference temperature of 20.0 degC to a saturated steam at 100.0 degC. Autosizing procedure assumes that gas heater in the humidifier convert the water from the reference temperature and generate saturated steam at 100 degC, using gas to thermal energy conversion rated thermal efficiency.
+
+Rated Gas Use Rate
+
+The rated or nominal gas use rate is given by:
+
+\begin{equation}
+Q_{NG,nom} = \frac{\dot{V}_{cap,nom}\rho_w\left(h_{fg}+c_{p,w}\Delta T_w\right)}{\eta_{rated}}
+\end{equation}
+
+Where,
+
+\begin{itemize}
+\item
+  Cp,w: specific heat of water at average temperature ((100+20)/2 = 60.0 degC), (J/kgK);
+\item
+  rho\_w: density of water at standard condition (5.05 degC);
+\item
+  DeltaTw: sensible temperature rise of water (100.0 - 20.0 = 80.0 degC);
+\item
+  V\_cap\_nom: rated or nominal capacity of the humidifier, (m3/s)
+\item
+  h\_fg: latent heat of vaporization of water at 100.0 degC, (J/kg);
+\item
+  eta\_rated: thermal efficiency at rated condition;
+\end{itemize}
+
+\subsubsection{Rated Capacity}\label{rated-capacity}
+
+\begin{equation}
+{\dot m_w} = {\dot m_a}\left( {{\omega_o} - {\omega_i}} \right)
+\end{equation}
+
+where
+
+\({\dot m_w}\) * iswater mass flow rate, kg/s;*
+
+\({\dot m_a}\) * is design air mass flow rate, kg/s;*
+
+\emph{ω\(_{o}\) is design outlet humidity ratio, kg-water/kg-air;}
+
+\emph{ω\(_{i}\) is design inlet humidity ratio, kg-water/kg-air.}
+
+The air mass flow rate and humidity ratios are determined based upon zone design conditions. If the unit is part of zone equipment, then:
+
+\begin{equation}
+{\dot m_a} = Max\left( {DesCoolVolFlo{w_{zone}},DesHeatVolFlo{w_{zone}}} \right) \cdot {\rho_a}
+\end{equation}
+
+\begin{equation}
+{\omega_i} = Min\left( {OutHumRatAtCoolPea{k_{zone}},OutHumRatAtHeatPea{k_{zone}}} \right)
+\end{equation}
+
+\begin{lstlisting}
+  ${\omega_o} = Max\left( {ZoneHumRatAtCoolPea{k_{zone}},ZoneHumRatAtHeatPea{k_{zone}}} \right)$ 
+\end{lstlisting}
+
+where
+
+\emph{r\(_{a}\) is the density of air at design conditions, kg/s.}
+
+\begin{itemize}
+\item
+  \begin{itemize}
+  \item
+  \end{itemize}
+\end{itemize}
+
+If the unit is part of the central air system, then check if outdoor air system is present. If outdoor air system is part of the air loop and design outdoor air flow rate is greater than zero, then:
+
+\begin{equation}
+{\dot m_a} = DesOutAirVolFlo{w_{sys}} \cdot {\rho_a}
+\end{equation}
+
+\begin{equation}
+{\omega_i} = Min\left( {CoolOutHumRa{t_{sys}},HeatOutHumRa{t_{sys}}} \right)
+\end{equation}
+
+\begin{lstlisting}
+  ${\omega_o} = Max\left( {CoolSupHumRa{t_{sys}},HeatSupHumRa{t_{sys}}} \right)$ 
+\end{lstlisting}
+
+Otherwise, air mass flow rate is determined as follows:
+
+for duct type = \emph{main}
+
+\begin{equation}
+{\dot m_a} = DesMainAirVolFlo{w_{sys}} \cdot {\rho_a}
+\end{equation}
+
+for duct type = \emph{cooling}
+
+\begin{equation}
+{\dot m_a} = DesCoolVolFlo{w_{sys}} \cdot {\rho_a}
+\end{equation}
+
+for duct type = \emph{heating}
+
+\begin{equation}
+{\dot m_a} = DesHeatVolFlo{w_{sys}} \cdot {\rho_a}
+\end{equation}
+
+for duct type = \emph{other}
+
+\({\dot m_a} = DesMainVolFlo{w_{sys}} \cdot {\rho_a}\) ,
+
+and the humidity ratios are:
+
+\begin{equation}
+{\omega_i} = Min\left( {CoolMixHumRa{t_{sys}},HeatMixHumRa{t_{sys}}} \right)
+\end{equation}
+
+\begin{lstlisting}
+  ${\omega_o} = Max\left( {CoolSupHumRa{t_{sys}},HeatSupHumRa{t_{sys}}} \right)$ 
+\end{lstlisting}
+
+\subsection{Cooling Tower Sizing}\label{cooling-tower-sizing}
+
+The quantities needed to autosize a cooling tower include the design water flow rate, the nominal fan power and air flow rate, and the tower UA. This data may be need to be given at more than one operating point:, for instance - high speed fan, low speed fan and free convection.
+
+EnergyPlus provides two input choices: the user can input the design water flow rate and tower UA at each operating point or the tower nominal capacity (and let the program calculate the water flow rate and UA). Choice of input method will affect the sizing calculations in ways noted below.
+
+\subsubsection{Design Water Flow Rate}\label{design-water-flow-rate}
+
+If \emph{Tower Performance Input Method} = \emph{UFactorTimesAreaAndDesignWaterFlowRate} then
+
+\begin{equation}
+\dot Vtower,w,des = \dot Vloop,des
+\end{equation}
+
+If \emph{Tower Performance Input Method} = \emph{NominalCapacity} then
+
+\begin{equation}
+\dot Vtower,w,des = 5.382E - 8\cdot \dot Qtower,nom
+\end{equation}
+
+where 5.382 *10\(^{-08}\) is m\(^{3}\)/s per watt corresponds to the rule-of-thumb of sizing the tower flow rate at 3 gallons per minute per ton. For the CoolingTower:VariableSpeed:Merkel model with NominalCapacity input method, the user can input the value used to scale design water flow rate from nominal capacity and the default is 5.382 *10\(^{-08}\) m\(^{3}\)/s/W.
+
+\subsubsection{Fan Power at Design Air Flow Rate}\label{fan-power-at-design-air-flow-rate}
+
+The nominal fan power is sized to be 0.0105 times the design load.
+
+If \emph{Tower Performance Input Method} = \emph{UFactorTimesAreaAndDesignWaterFlowRate} then
+
+\begin{equation}
+\dot Qtower,nom = Cp,w\cdot \rho w\cdot \dot Vtower,w,des\cdot \Delta Tloop,des
+\end{equation}
+
+where
+
+\emph{C\(_{p,w}\)} is the specific heat of water at the condenser loop design exit temperature;
+
+\emph{r\(_{w}\)} is the density of water at standard conditions (5.05 \(^{o}\)C);
+
+\emph{DT\(_{loop,des}\)} is the condenser water loop design temperature rise;
+
+Finally
+
+\begin{equation}
+\dot Qfan,nom = 0.0105\cdot \dot Qtower,nom
+\end{equation}
+
+For the CoolingTower:VariableSpeed:Merkel model, the design fan power is determined using a scaling factor, in units of Watts per Watt, that can be input by the user. The default value is 0.0105 which is the same as above.
+
+\subsubsection{Design Air Flow Rate}\label{design-air-flow-rate}
+
+We assume a fan efficiency of 0.5 and a fan pressure rise of 190 Pascals. Then
+
+\begin{equation}
+\dot Vtower,air,des = \dot Qfan,nom\cdot 0.5\cdot \rho air/190
+\end{equation}
+
+where
+
+r\(_{air}\) is the density of air at standard conditions.
+
+For the CoolingTower:VariableSpeed:Merkel model, the design air flow rate is determined from the nominal capacity using a scaling factor, \({f_{airflow/W}}\) ,in units of m\(^{3}\)/s/W. The default value is 2.76316*10\(^{-5}\). When the input field is left blank, the default is used as follows
+
+\begin{equation}
+{\dot V_{tower,air,des}} = {\dot Q_{tower,nom}} \bullet {f_{airflow/W}} \bullet \frac{{101325}}{{{P_{std,altitude}}}}
+\end{equation}
+
+where, \({P_{std,altitude}}\) is the standard barometric pressure for the location's elevation.
+
+When the input field is filled with a hard value, the pressure scaling is not used
+
+\begin{equation}
+{\dot V_{tower,air,des}} = {\dot Q_{tower,nom}} \bullet {f_{airflow/W}}
+\end{equation}
+
+\subsubsection{Tower UA Value at Design Air Flow Rate}\label{tower-ua-value-at-design-air-flow-rate}
+
+To obtain the UA of the tower, we specify the model inputs (other than the UA) at design conditions and the design tower load that the tower must meet. Then we numerically invert the tower model to solve for the UA that will enable the tower to meet the design tower load given the specified inputs.
+
+The design tower load is:
+
+for \emph{Tower Performance Input Method} = \emph{UFactorTimesAreaAndDesignWaterFlowRate}
+
+\begin{equation}
+\dot Qtower,des = Cp,w\cdot \rho w\cdot \dot Vtower,w,des\cdot \Delta Tloop,des
+\end{equation}
+
+for \emph{Tower Performance Input Method} = \emph{NominalCapacity}
+
+\(\dot Qtower,des = 1.25\cdot \dot Qtower,nom\) (to allow for compressor heat)
+
+Where, \({f_{des,heat,ratio}}\) is the ratio of actual heat rejection capacity to nominal capacity. This ratio is available as a user input with a default value of 1.25 (to allow for compressor heat).
+
+Then we assign the inputs needed for the model.
+
+\emph{T\(_{in,air}\)} = 35 \(^{o}\)C (95 \(^{o}\)F design air inlet temperature)
+
+\emph{T\(_{in,air,wb}\)} = 25.6 \(^{o}\)C (78 \(^{o}\)F design air inlet wetbulb temperature)
+
+\emph{W\(_{in}\)} is calculated from the entering air drybulb and wetbulb.
+
+The inlet water mass flow rate is just the design volumetric flow rate times the density of water.
+
+The inlet water temperature is set slightly differently for the 2 input methods. For
+
+\emph{UFactorTimesAreaAndDesignWaterFlowRate}
+
+\emph{T\(_{in,water}\)} = \emph{T\(_{loop,exit,des}\)}+\emph{DT\(_{loop,des}\)}
+
+\emph{NominalCapacity}
+
+\emph{T\(_{in,water}\)} = 35 \(^{o}\)C (95 \(^{o}\)F design inlet water temperature).
+
+We now have all the data needed to obtain UA. The numerical inversion is carried out by calling subroutine \emph{SolveRegulaFalsi}. This is a general utility routine for finding the zero of a function. In this case it finds the UA that will zero the residual function - the difference between the design tower load and the tower output divided by the design tower load. The residual is calculated in the function \emph{SimpleTowerUAResidual.}
+
+\subsubsection{Air Flow Rate at Low Fan Speed}\label{air-flow-rate-at-low-fan-speed}
+
+The nominal air flow rate at low fan speed is set to a fraction of the full speed air flow rate. The fraction is available for user input in the field called Low Fan Speed Air Flow Rate Sizing Factor. The default is 0.5.
+
+\subsubsection{Fan Power at Low Fan Speed}\label{fan-power-at-low-fan-speed}
+
+The fan power at low fan speed is set to a fraction of the fan power at full speed. The fraction is available for user input in the field called Low Fan Speed Fan Power Sizing Factor. The default is 0.16.
+
+\subsubsection{Tower UA Value at Low Fan Speed}\label{tower-ua-value-at-low-fan-speed}
+
+For \emph{Tower Performance Input Method} = \emph{UFactorTimesAreaAndDesignWaterFlowRate} the low speed UA is set to a fraction of the full speed UA. The fraction is available for user input in the field called Low Fan Speed U-Factor Times Area Sizing Factor. The default is 0.6. For \emph{Tower Performance Input Method} = \emph{NominalCapacity} the low speed UA is calculated in the same manner as the full speed UA using \(\dot Qtower,nom,lowspeed\) instead of \(\dot Qtower,nom\) .
+
+\subsubsection{Air Flow Rate in Free Convection Regime}\label{air-flow-rate-in-free-convection-regime}
+
+The free convection air flow rate is set to a fraction of the full air flow rate. The fraction is available for user input in the field called Free Convection Regime Air Flow Rate Sizing Factor. The default is 0.1.
+
+\subsubsection{Tower UA Value in Free Convection Regime}\label{tower-ua-value-in-free-convection-regime}
+
+For \emph{Tower Performance Input Method} = \emph{UA and Design Water Flow Rate} the low speed UA is set to a fraction of the full speed UA. The fraction is available for user input in the field called Free Convection U-Factor Times Area Value Sizing Factor. The default is 0.1. For \emph{Tower Performance Input Method} = \emph{NominalCapacity} the low speed UA is calculated in the same manner as the full speed UA using \(\dot Qtower,nom,freeconv\) instead of \(\dot Qtower,nom\) .
+
+\subsection{Fluid Cooler Sizing}\label{fluid-cooler-sizing}
+
+The quantities needed to autosize a fluid cooler include the design water flow rate, the nominal fan power, air flow rate, and the fluid cooler UA. This data may need to be given at more than one operating point:, for instance - high speed fan and low speed fan.
+
+EnergyPlus provides two input choices: the user can input the design water flow rate and fluid cooler UA at each operating point or the fluid cooler nominal capacity and the water flow rate (and let the program calculate UA). Choice of input method will affect the sizing calculations in ways noted below.
+
+\subsubsection{Design Water Flow Rate}\label{design-water-flow-rate-1}
+
+The design water flow rate is sized as follows
+
+\begin{equation}
+{\dot V_{fluidcooler,w,des}} = {\dot V_{loop,des}}
+\end{equation}
+
+\subsubsection{Fan Power at Design Air Flow Rate}\label{fan-power-at-design-air-flow-rate-1}
+
+The nominal fan power is sized to be 0.0105 times the design load.
+
+If \emph{Performance Input Method} = \emph{UFactorTimesAreaAndDesignWaterFlowRate} then
+
+\begin{equation}
+{\dot Q_{fluidcooler,nom}} = {C_{p,w}} \bullet {\rho_w} \bullet {\dot V_{fluidcooler,w,des}} \bullet \Delta {T_{loop,des}}
+\end{equation}
+
+where
+
+\begin{itemize}
+\item
+  C\(_{p,w}\)* is the specific heat of water at the condenser loop design exit temperature;
+\item
+  \begin{itemize}
+  \tightlist
+  \item
+    \emph{r\(_{w}\)} is the density of water at standard conditions (5.05 \(^{o}\)C);
+  \end{itemize}
+\item
+  \begin{itemize}
+  \tightlist
+  \item
+    \emph{DT\(_{loop,des}\)} is the condenser water loop design temperature rise;
+  \end{itemize}
+\end{itemize}
+
+Finally
+
+\begin{equation}
+{\dot Q_{fan,nom}} = 0.0105 \bullet {\dot Q_{fluidcooler,nom}}
+\end{equation}
+
+\subsubsection{ElseifPerformance Input Method = NominalCapacitythen}\label{elseifperformance-input-method-nominalcapacitythen}
+
+\begin{lstlisting}
+  ${\dot Q_{fan,nom}} = 0.0105 \bullet {\dot Q_{fluidcooler,nom}}$ 
+\end{lstlisting}
+
+Where
+
+\begin{lstlisting}
+  ${\dot Q_{fluidcooler,nom}}$  is provided by the user.
+\end{lstlisting}
+
+\subsubsection{Design Air Flow Rate}\label{design-air-flow-rate-1}
+
+\begin{itemize}
+\tightlist
+\item
+  For Performance Input Method = UFactorTimesAreaAndDesignWaterFlowRate
+\end{itemize}
+
+\({\dot Q_{fluidcooler,nom}} = {C_{p,w}} \bullet {\rho_w} \bullet {\dot V_{fluidcooler,w,des}} \bullet \Delta {T_{loop,des}}\)
+
+\begin{itemize}
+\tightlist
+\item
+  For Performance Input Method = NominalCapacity
+\end{itemize}
+
+\({\dot Q_{fluidcooler,nom}}\) is provided by the user.
+
+\({\dot V_{fluidcooler,air,des}} = {\dot Q_{fluidcooler,nom}}/({T_{in,water}} - {T_{in,air}})*4\)
+
+Where,
+
+\emph{T\(_{in,water}\)} = Design entering water temperature provided by the user
+
+\emph{T\(_{in,air}\)} = Design air inlet temperature provided by the user
+
+\subsubsection{Fluid cooler UA Value at Design Air Flow Rate}\label{fluid-cooler-ua-value-at-design-air-flow-rate}
+
+To obtain the UA of the fluid cooler, we specify the model inputs (other than the UA) at design conditions and the design fluid cooler load that the fluid cooler must meet. Then we numerically invert the fluid cooler model to solve for the UA that will enable the fluid cooler to meet the design fluid cooler load given the specified inputs.
+
+The design fluid cooler load is:
+
+\begin{itemize}
+\tightlist
+\item
+  For Performance Input Method = UFactorTimesAreaAndDesignWaterFlowRate
+\end{itemize}
+
+\({\dot Q_{fluidcooler,nom}} = {C_{p,w}} \bullet {\rho_w} \bullet {\dot V_{fluidcooler,w,des}} \bullet \Delta {T_{loop,des}}\)
+
+\begin{itemize}
+\tightlist
+\item
+  For Performance Input Method = NominalCapacity
+\end{itemize}
+
+\({\dot Q_{fluidcooler,nom}}\) is provided by the user.
+
+Then we assign the inputs needed for the model.
+
+\emph{T\(_{in,air}\)} = Design air inlet temperature provided by the user
+
+\emph{T\(_{in,air,wb}\)} = Design air inlet wetbulb temperature provided by the user
+
+\emph{W\(_{in}\)} is calculated from the entering air drybulb and wetbulb.
+
+The inlet water mass flow rate is just the design entering volumetric flow rate times the density of water.
+
+The inlet water temperature is set slightly differently for the 2 input methods. For
+
+\begin{itemize}
+\tightlist
+\item
+  UFactorTimesAreaAndDesignWaterFlowRate
+\end{itemize}
+
+\begin{equation}
+{T_{in,water}} = {T_{loop,exit,des}} + \Delta {T_{loop,des}}
+\end{equation}
+
+\begin{itemize}
+\tightlist
+\item
+  NominalCapacity
+\end{itemize}
+
+\begin{equation}
+{T_{in,water}} = Provided\,by\,the\,user
+\end{equation}
+
+We now have all the data needed to obtain UA. The numerical inversion is carried out by calling subroutine \emph{SolveRegulaFalsi}. This is a general utility routine for finding the zero of a function. In this case it finds the UA that will zero the residual function - the difference between the design fluid cooler load and the fluid cooler output divided by the design fluid cooler load. The residual is calculated in the function \emph{SimpleFluidCoolerUAResidual.}
+
+\subsubsection{Air Flow Rate at Low Fan Speed}\label{air-flow-rate-at-low-fan-speed-1}
+
+The nominal air flow rate at low fan speed is set to a fraction of the full speed air flow rate. The fraction is available for user input in the field called Low Fan Speed Air Flow Rate Sizing Factor. The default is 0.5.
+
+\subsubsection{Fan Power at Low Fan Speed}\label{fan-power-at-low-fan-speed-1}
+
+The fan power at low fan speed is set to a fraction of the fan power at full speed. The fraction is available for user input in the field called Low Fan Speed Fan Power Sizing Factor. The default is 0.16.
+
+\subsubsection{Fluid cooler UA Value at Low Fan Speed}\label{fluid-cooler-ua-value-at-low-fan-speed}
+
+For \emph{Performance Input Method} = \emph{UFactorTimesAreaAndDesignWaterFlowRate} the low speed UA is set to a fraction of the full speed UA. . The fraction is available for user input in the field called Low Fan Speed U-Factor Times Area Sizing Factor. The default is 0.6. For \emph{Performance Input Method} = \emph{NominalCapacity} the low speed UA is calculated in the same manner as the full speed UA using \({\dot Q_{fluidcooler,nom,lowspeed}}\) instead of \({\dot Q_{fluidcooler,nom}}\) .
+
+\subsection{Evaporative Fluid cooler Sizing}\label{evaporative-fluid-cooler-sizing}
+
+The quantities needed to autosize an evaporative fluid cooler include the design water flow rate, the nominal fan power, air flow rate, and the fluid cooler UA. This data may need to be given at more than one operating point:, for instance - high speed fan and low speed fan.
+
+EnergyPlus provides three input choices: the user can input the design water flow rate and fluid cooler UA at each operating point (\emph{UFactorTimesAreaAndDesignWaterFlowRate}) or the fluid cooler design capacity and the water flow rate and let the program calculate UA (\emph{UserSpecifiedDesignCapacity}) or only the fluid cooler design capacity and let the program calculate UA and the water flow rate (\emph{StandardDesignCapacity}). Choice of input method will affect the sizing calculations in ways noted below.
+
+\subsubsection{Design Water Flow Rate}\label{design-water-flow-rate-2}
+
+If \emph{Performance Input Method} = \emph{StandardDesignCapacity} then
+
+\begin{equation}
+{\dot V_{fluidcooler,w,des}} = 5.382E - 8\cdot {\dot Q_{fluidcooler,standarddesign}}
+\end{equation}
+
+Else
+
+\begin{equation}
+{\dot V_{fluidcooler,w,des}} = {\dot V_{loop,des}}
+\end{equation}
+
+where 5.382 *10\(^{-08}\) is m\(^{3}\)/s per watt corresponds to the rule-of-thumb of sizing the fluid cooler flow rate at 3 gallons per minute per ton.
+
+\subsubsection{Fan Power at Design Air Flow Rate}\label{fan-power-at-design-air-flow-rate-2}
+
+The design fan power is sized to be 0.0105 times the design load.
+
+If \emph{Performance Input Method} = \emph{UFactorTimesAreaAndDesignWaterFlowRate} then
+
+\begin{equation}
+{\dot Q_{fluidcooler,design}} = {C_{p,w}} \bullet {\rho_w} \bullet {\dot V_{fluidcooler,w,des}} \bullet \Delta {T_{loop,des}}
+\end{equation}
+
+where
+
+\emph{C\(_{p,w}\)} is the specific heat of water at the condenser loop design exit temperature;
+
+\emph{r\(_{w}\)} is the density of water at standard conditions (5.05 \(^{o}\)C);
+
+\emph{DT\(_{loop,des}\)} is the condenser water loop design temperature rise;
+
+Finally
+
+\begin{equation}
+{\dot Q_{fan,design}} = 0.0105 \bullet {\dot Q_{fluidcooler,design}}
+\end{equation}
+
+\subsubsection{Else}\label{else}
+
+\begin{equation}
+{\dot Q_{fan,design}} = 0.0105 \bullet {\dot Q_{fluidcooler,design}}
+\end{equation}
+
+Where
+
+\({\dot Q_{fluidcooler,design}}\) is the design capacity provided by the user for the other two performance input methods
+
+\subsubsection{Design Air Flow Rate}\label{design-air-flow-rate-2}
+
+We assume a fan efficiency of 0.5 and a fan pressure rise of 190 Pascals. Then
+
+\begin{equation}
+{\dot V_{fluidcooler,air,des}} = {\dot Q_{fan,design}} \bullet 0.5 \bullet {\rho_{air}}/190
+\end{equation}
+
+where
+
+r\(_{air}\) is the density of air at standard conditions.
+
+\subsubsection{Fluid cooler UA Value at Design Air Flow Rate}\label{fluid-cooler-ua-value-at-design-air-flow-rate-1}
+
+To obtain the UA of the evaporative fluid cooler, we specify the model inputs (other than the UA) at design conditions and the design fluid cooler load that the fluid cooler must meet. Then we numerically invert the fluid cooler model to solve for the UA that will enable the fluid cooler to meet the design fluid cooler load given the specified inputs.
+
+The design fluid cooler load is:
+
+\begin{itemize}
+\tightlist
+\item
+  For Performance Input Method = UFactorTimesAreaAndDesignWaterFlowRate
+\end{itemize}
+
+\begin{equation}
+{\dot Q_{fluidcooler,design}} = {C_{p,w}} \bullet {\rho_w} \bullet {\dot V_{fluidcooler,w,des}} \bullet \Delta {T_{loop,des}}
+\end{equation}
+
+\begin{itemize}
+\tightlist
+\item
+  For Performance Input Method = StandardDesignCapacity
+\end{itemize}
+
+\({\dot Q_{fluidcooler,design}} = 1.25 \bullet {\dot Q_{fluidcooler,standarddesign}}\) (to allow for compressor heat)
+
+Then we assign the inputs needed for the model.
+
+\emph{T\(_{in,air}\)} = 35 \(^{o}\)C (95 \(^{o}\)F design air inlet temperature)
+
+\emph{T\(_{in,air,wb}\)} = 25.6 \(^{o}\)C (78 \(^{o}\)F design air inlet wetbulb temperature)
+
+\emph{W\(_{in}\)} is calculated from the entering air drybulb and wetbulb.
+
+\begin{itemize}
+\tightlist
+\item
+  For Performance Input Method = UserSpecifiedDesignCapacity
+\end{itemize}
+
+\begin{equation}
+{\dot Q_{fluidcooler,design}} = {\dot Q_{fluidcooler,userspecifieddesign}}
+\end{equation}
+
+Where, \({f_{des,heat,ratio}}\) is the ratio of actual heat rejection capacity to nominal capacity. This ratio is available as a user input with a default value of 1.25 (to allow for compressor heat)
+
+Then we assign the inputs needed for the model.
+
+\emph{T\(_{in,air}\)} = Design air inlet temperature provided by the user
+
+\emph{T\(_{in,air,wb}\)} = Design air inlet wetbulb temperature provided by the user
+
+\emph{W\(_{in}\)} is calculated from the entering air drybulb and wetbulb.
+
+The inlet water mass flow rate is just the design entering volumetric flow rate times the density of water.
+
+The inlet water temperature is set slightly differently for the 3 input methods. For
+
+\begin{itemize}
+\tightlist
+\item
+  UFactorTimesAreaAndDesignWaterFlowRate
+\end{itemize}
+
+\begin{equation}
+{T_{in,water}} = {T_{loop,exit,des}} + \Delta {T_{loop,des}}
+\end{equation}
+
+\begin{itemize}
+\tightlist
+\item
+  StandardDesignCapacity
+\end{itemize}
+
+\begin{equation}
+{T_{in,water}} = 35^\circ C\;(95^\circ F\,design\,inlet\,water\,temperature)
+\end{equation}
+
+\begin{itemize}
+\tightlist
+\item
+  UserSpecifiedDesignCapacity
+\end{itemize}
+
+\begin{equation}
+{T_{in,water}} = Provided\,by\,the\,user
+\end{equation}
+
+We now have all the data needed to obtain UA. The numerical inversion is carried out by calling subroutine \emph{SolveRegulaFalsi}. This is a general utility routine for finding the zero of a function. In this case it finds the UA that will zero the residual function - the difference between the design fluid cooler load and the fluid cooler output divided by the design fluid cooler load. The residual is calculated in the function \emph{SimpleEvapFluidCoolerUAResidual.}
+
+\subsubsection{Air Flow Rate at Low Fan Speed}\label{air-flow-rate-at-low-fan-speed-2}
+
+The design air flow rate at low fan speed is set to a fraction of the full speed air flow rate. The fraction is available for user input in the field called Low Fan Speed Air Flow Rate Sizing Factor. The default is 0.5.
+
+\subsubsection{Fan Power at Low Fan Speed}\label{fan-power-at-low-fan-speed-2}
+
+The fan power at low fan speed is set to a fraction of the fan power at full speed. The fraction is available for user input in the field called Low Fan Speed Fan Power Sizing Factor. The default is 0.16.
+
+\subsubsection{Fluid cooler UA Value at Low Fan Speed}\label{fluid-cooler-ua-value-at-low-fan-speed-1}
+
+For \emph{Performance Input Method} = \emph{UFactorTimesAreaAndDesignWaterFlowRate} the low speed UA is set to a fraction of the full speed UA. The fraction is available for user input in the field called Low Fan Speed U-Factor Times Area Sizing Factor. The default is 0.6. For \emph{Performance Input Method} = \emph{StandardDesignCapacity} (and similarly for \emph{UserSpecifiedDesignCapacity method}) the low speed UA is calculated in the same manner as the full speed UA using \({\dot Q_{fluidcooler,standarddesign,lowspeed}}\) instead of \({\dot Q_{fluidcooler,standarddesign}}\) .
+
+\subsection{Fan Coil Unit Sizing}\label{fan-coil-unit-sizing}
+
+Fan Coil units are compound components: each unit contains a fan, hot water coil, chilled water coil and outside air mixer. The inputs that may need to be autosized are the nominal unit air flow rate, the maximum hot and chilled water flow rates, and the design outside air flow rate. The data needed for sizing the units is obtained from the zone design arrays and the user specified plant sizing input.
+
+\subsubsection{Maximum Air Flow Rate}\label{maximum-air-flow-rate}
+
+\begin{equation}
+\dot Vair,max = Max(DesCoolVolFlowzone,DesHeatVolFlowzone)
+\end{equation}
+
+\subsubsection{Maximum Outside Air Flow Rate}\label{maximum-outside-air-flow-rate}
+
+\begin{equation}
+\dot Voutsideair,max = Min(MinOAzone,\dot Vair,max)
+\end{equation}
+
+\subsubsection{Maximum Hot Water Flow}\label{maximum-hot-water-flow}
+
+\emph{T\(_{coil,in}\)} = \emph{DesHeatCoilInTemp\(_{zone}\)}
+
+\begin{equation}
+  T_{coil,out} = HeatDesTemp_{zone}
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{coil,des} = c_{p,air} \cdot DesHeatMassFlow_{zone} \cdot (T_{out,coil} - T_{in,coil})
+\end{equation}
+
+\begin{equation}
+  \dot{V}_{max,hw} = \dot{Q}_{coil,des} / (c_{p,w} \cdot \rho_{w} \cdot \Delta T_{loop,des})
+\end{equation}
+
+where
+
+\emph{c\(_{p,air}\)} is evaluated at the average of the inlet \& outlet temperatures and the coil outlet humidity ratio.
+
+\subsubsection{Maximum Cold Water Flow}\label{maximum-cold-water-flow}
+
+\emph{T\(_{coil,in}\)} = \emph{DesColdCoilInTemp\(_{zone}\)}
+
+\emph{T\(_{coil,out}\)} = \emph{ColdDesTemp\(_{zone}\)}
+
+\emph{W\(_{coil,in}\)} = \emph{DesCoolCoilInHumRat\(_{zone}\)}
+
+\emph{W\(_{coil,out}\)} = \emph{CoolDesHumRat\(_{zone}\)}
+
+\emph{H\(_{coil,in}\)} = \emph{PsyHFnTdbW}(\emph{T\(_{coil,in}\)}, \emph{W\(_{coil,in}\)})
+
+\emph{H\(_{coil,out}\)} = \emph{PsyHFnTdbW}(\emph{T\(_{coil,out}\)}, \emph{W\(_{coil,out}\)})
+
+\begin{equation}
+  \dot{Q}_{coil,des} = DesCoolMassFlow_{zone} \cdot (h_{in,coil} - h_{out,coil})
+\end{equation}
+
+\begin{equation}
+  \dot{V}_{max,hw} = \dot{Q}_{coil,des} / (c_{p,w} \cdot \rho_w \cdot \Delta T_{loop,des})
+\end{equation}
+
+where
+
+\emph{c\(_{p,air}\)} is evaluated at the average of the inlet \& outlet temperatures and the coil outlet humidity ratio.
+
+\subsection{Window Air Conditioner Sizing}\label{window-air-conditioner-sizing}
+
+Window air conditioners are compound components: each unit contains a fan, a DX coil and an outside air mixer. The inputs that may need to be autosized are the nominal unit air flow rate and the design outside air flow rate. The data needed for sizing the units is obtained from the zone design arrays.
+
+\subsubsection{Maximum Air Flow Rate}\label{maximum-air-flow-rate-1}
+
+\begin{equation}
+{\dot V_{air,max}} = DesCoolVolFlo{w_{max}}
+\end{equation}
+
+\subsubsection{Maximum Outside Air Flow Rate}\label{maximum-outside-air-flow-rate-1}
+
+\begin{equation}
+\dot Voutsideair,max = Min(MinOAzone,\dot Vair,max)
+\end{equation}
+
+\subsection{Unit Ventilator Sizing}\label{unit-ventilator-sizing}
+
+Unit ventilators are compound components: each unit contains an outdoor air mixer, a fan, a heating coil, and a cooling coil. The inputs that may need to be autosized are the maximum supply air flow rate and the maximum/minimum outside air flow rates. The data needed for sizing the units is obtained from the zone design arrays.
+
+\subsubsection{Maximum Air Flow Rate}\label{maximum-air-flow-rate-2}
+
+If both the cooling and heating coil are present, then:
+
+\begin{equation}
+{\dot V_{supplyair,max}} = MAX\left( {DesCoolVolFlo{w_{zone}},DesHeatVolFlo{w_{zone}}} \right)
+\end{equation}
+
+If only the heating coil is present, then:
+
+\begin{equation}
+{\dot V_{supplyair,max}} = DesHeatVolFlo{w_{zone}}
+\end{equation}
+
+If only cooling coil is present, then:
+
+\begin{equation}
+{\dot V_{supplyair,max}} = DesCoolVolFlo{w_{zone}}
+\end{equation}
+
+If neither heating nor cooling coil is present, then:
+
+\begin{equation}
+{\dot V_{supplyair,max}} = MinO{A_{zone}}
+\end{equation}
+
+\subsubsection{Maximum Outside Air Flow Rate}\label{maximum-outside-air-flow-rate-2}
+
+\begin{equation}
+{\dot V_{outsideair,max}} = {\dot V_{air,max}}
+\end{equation}
+
+\subsubsection{Minimum Outside Air Flow Rate}\label{minimum-outside-air-flow-rate}
+
+\begin{equation}
+{\dot V_{outsideair,min}} = Min\left( {MinO{A_{zone}},{{\dot V}_{air,max}}} \right)
+\end{equation}
+
+\subsection{Packaged Terminal Heat Pump Sizing}\label{packaged-terminal-heat-pump-sizing}
+
+Packaged terminal heat pumps are compound components: each unit contains a supply air fan, a DX cooling coil, a DX heating coil, a GAS or ELECTRIC supplemental heating coil, and an outside air mixer. The inputs that may need to be autosized are the supply air and outside air volumetric air flow rates during cooling operation, heating operation, and when no cooling or heating is needed. In addition, the maximum supply air temperature from the supplemental heater can also be automatically selected. The data needed for sizing the units are obtained from the zone design arrays.
+
+\subsubsection{Supply air volumetric flow rate during cooling operation}\label{supply-air-volumetric-flow-rate-during-cooling-operation}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{SA\,\,,\,cooling}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)
+\end{equation}
+
+\subsubsection{Supply air volumetric flow rate during heating operation}\label{supply-air-volumetric-flow-rate-during-heating-operation}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{SA\,\,,\,heating}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)
+\end{equation}
+
+\subsubsection{Supply air volumetric flow rate when no cooling or heating is needed}\label{supply-air-volumetric-flow-rate-when-no-cooling-or-heating-is-needed}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{SA\,,\,no\,cool\,or\,heat}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)
+\end{equation}
+
+\subsubsection{Outside air volumetric flow rate during cooling operation}\label{outside-air-volumetric-flow-rate-during-cooling-operation}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{OA\,,\,\,cooling}} = {\rm{MIN}}(MinO{A_{zone}},{\mathop {\,V}\limits^ \cdot_{SA\,,\,\,cooling}})
+\end{equation}
+
+\subsubsection{Outside air volumetric flow rate during heating operation}\label{outside-air-volumetric-flow-rate-during-heating-operation}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{OA\,,\,\,heating}} = {\rm{MIN}}(MinO{A_{zone}},{\mathop {\,V}\limits^ \cdot_{SA\,,\,\,heating}})
+\end{equation}
+
+\subsubsection{Outside air volumetric flow rate when no cooling or heating is needed}\label{outside-air-volumetric-flow-rate-when-no-cooling-or-heating-is-needed}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{OA\,,\,no\,\,cool\,or\,heat}} = {\rm{MIN}}(MinO{A_{zone}},{\mathop {\,V}\limits^ \cdot_{SA\,,\,no\,\,cool\,or\,heat}})
+\end{equation}
+
+\subsubsection{Maximum supply air temperature from supplemental heater}\label{maximum-supply-air-temperature-from-supplemental-heater}
+
+\begin{equation}
+{T_{SA,\max }} = HeatDesTem{p_{zone}}
+\end{equation}
+
+\subsection{MultiSpeed Heat Pump Sizing}\label{multispeed-heat-pump-sizing}
+
+MultiSpeed heat pumps are compound components: each unit contains a supply air fan, a multispeed DX cooling coil, a multispeed DX heating coil, and a GAS or ELECTRIC supplemental heating coil. The inputs that may need to be autosized are the supply air volumetric air flow rates during cooling operation, heating operation, and when no cooling or heating is needed. The data needed for sizing the units are obtained from the controlled zone design arrays.
+
+\subsubsection{Supply air volumetric flow rate during cooling operation at the highest speed}\label{supply-air-volumetric-flow-rate-during-cooling-operation-at-the-highest-speed}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{SA\,\,,\,cooling}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)/ZoneFraction
+\end{equation}
+
+\subsubsection{Supply air volumetric flow rate during heating operation at the highest speed}\label{supply-air-volumetric-flow-rate-during-heating-operation-at-the-highest-speed}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{SA\,\,,\,heating}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)/ZoneFraction
+\end{equation}
+
+\subsubsection{Supply air volumetric flow rate when no cooling or heating is needed}\label{supply-air-volumetric-flow-rate-when-no-cooling-or-heating-is-needed-1}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{SA\,,\,no\,cool\,or\,heat}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)/ZoneFraction
+\end{equation}
+
+where
+
+ZoneFraction = Fraction of the total volume flow that goes through the controlling zone
+
+\subsubsection{Supply air volumetric flow rate during cooling operation at Speed n (1 to NumberOfSpeed-1)}\label{supply-air-volumetric-flow-rate-during-cooling-operation-at-speed-n-1-to-numberofspeed-1}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{SA\,\,,\,cooling,n}} = \frac{n}{{NumberOfSpeed}}{\mathop V\limits^ \cdot_{SA\,\,,\,cooling}}
+\end{equation}
+
+\subsubsection{Supply air volumetric flow rate during heating operation at Speed n (1 to NumberOfSpeed-1)}\label{supply-air-volumetric-flow-rate-during-heating-operation-at-speed-n-1-to-numberofspeed-1}
+
+\begin{equation}
+{\mathop V\limits^ \cdot_{SA\,\,,\,heating,n}} = \frac{n}{{NumberOfSpeed}}{\mathop V\limits^ \cdot_{SA\,\,,\,heating}}
+\end{equation}
+
+where
+
+n = Speed Index number from 1 to NumberOfSpeed-1
+
+NumberOfSpeed = The highest speed number
+
+\subsection{Single Duct Terminal Units}\label{single-duct-terminal-units}
+
+These are all the EnergyPlus components whose names begin with ``\emph{AirTerminal:SingleDuct:}'' (except for Cooled Beam units). This includes \emph{Uncontrolled, ConstantVolume:Reheat, VAV:NoReheat, VAV:Reheat, VAV:Reheat:VariableSpeedFan, VAV:HeatAndCool:NoReheat, VAV:HeatAndCool:Reheat, SeriesPIU:Reheat, ParallelPIU:Reheat,} and \emph{ConstantVolume:FourPipeInduction}. The inputs that may need to be autosized are the various maximum air flow rates through the unit, minimum air flow rates, and maximum hot water and/or chilled water flow rates if heating or cooling coils are present.
+
+\emph{Note:} all zone design flow rates and loads referenced below may have been altered by system sizing inputs. For instance, if the user specifies a \emph{Cooling Design Air Flow Method = Flow/System} and specifies a \emph{Cooling Design Air Flow Rate} the zone cooling design values will be altered to match the specified system flow rate.
+
+\subsubsection{Maximum Air Flow Rate}\label{maximum-air-flow-rate-3}
+
+\begin{equation}
+{\dot V_{air,\max ,{\rm{terminal}}}} = Max(DesCoolVolFlowzone,DesHeatVolFlowzone)
+\end{equation}
+
+\subsubsection{Maximum Heating Air Flow Rate}\label{maximum-heating-air-flow-rate}
+
+\begin{equation}
+{\dot V_{air,max,heat,terminal}} = DesHeatVolFlowzone
+\end{equation}
+
+\subsubsection{Maximum Primary and Secondary Air Flow Rates}\label{maximum-primary-and-secondary-air-flow-rates}
+
+For the PIU terminal units, the maximum primary and secondary air flow rates are sized to the same value as the maximum total air flow rate.
+
+\subsubsection{Minimum Air Flow Rate}\label{minimum-air-flow-rate}
+
+Basically minimum air flow rates are sized to the ventilation air requirement. This may be more or less complicated.
+
+For the PIU's, the minimum primary air flow fraction is set to
+
+\(\mathop {MinOA}\nolimits_{zone} /{\dot V_{air,max,primary,terminal}}\) .
+
+For other VAV terminal units
+
+\begin{equation}
+{\dot V_{air,min,terminal}} = Fra{c_{air,\min }}*DesVolFlowzone
+\end{equation}
+
+where, \emph{Fracair,min}corresponds to the minimum flow fraction of the teminal unit. This value is provided as user input, typically as the field ``Zone Minimum Air Flow Fraction.'' For the VAV terminals that allow scheduling minimum flow fraction (e.g., AirTerminal:SingleDuct:VAV:Reheat), there are two ways that \emph{Fracair,min}can be determined. If a value is entered in the input field Constant Minimum Air Flow Fraction, then it is always used for \emph{Fracair,min}. If the mimimum air flow fraction method is ``Schedule'' and the Constant Minimum Air Flow Fraction is left blank, then the program uses the average of the minimum and maximum values in the schedule for \emph{Fracair,min}.
+
+\subsubsection{Fan On Flow Fraction}\label{fan-on-flow-fraction}
+
+For the parallel PIU, this is set to the minimum primary air flow fraction.
+
+\subsubsection{Max Hot Water Flow}\label{max-hot-water-flow}
+
+\begin{equation}
+{T_{coil,in}} = DesHeatCoilInTem{p_{zone}}
+\end{equation}
+
+\begin{equation}
+{T_{coil,out}} = HeatDesTem{p_{zone}}
+\end{equation}
+
+The coil load and max hot water flow rate are then:
+
+\[\dot Q_{coil,des} = c_{p,air}\cdot \rho_{air}\cdot \dot V_{air,coil,heating}\cdot (T_{out,coil} - T_{in,coil})\] \[\dot V_{max,hw} = \dot Q_{coil,des}/(c_{p,w}\cdot \rho_{w}\cdot \Delta T_{loop,des})\]
+
+where
+
+\emph{c\(_{p,air}\)} is evaluated at the average of the inlet \& outlet temperatures and the coil outlet humidity ratio.
+
+The four-pipe induction unit sizes the heating coil differently: to meet the zone load rather than match the design zone supply temperature. The load on the hot water coil is then the zone load minus whatever the central system does.
+
+\begin{equation}
+{\dot Q_{coil,des}} = {\dot Q_{zone,des}} - {c_{p,air}}{\rho_{air}}{\dot V_{air,primary,des}}({T_{coil,in}} - {T_{zone,heatpeak}})
+\end{equation}
+
+where
+
+\begin{equation}
+{T_{coil,in}} = DesHeatCoilInTem{p_{zone}}
+\end{equation}
+
+\begin{equation}
+{T_{zone,heatpeak}} = ZoneTempAtHeatPea{k_{zone}}
+\end{equation}
+
+\begin{equation}
+{\dot V_{air,primary,des}} = {\dot V_{air,max,terminal}}/(1 + {R_{induc}})
+\end{equation}
+
+\subsubsection{Max Chilled Water Flow}\label{max-chilled-water-flow}
+
+The chilled water flow for the four-pipe induction unit is sized analogously to the hot water flow.
+
+\subsection{Indirect Evaporative Cooler Sizing}\label{indirect-evaporative-cooler-sizing}
+
+The model for the object called EvaporativeCooler:Indirect:ResearchSpecial has a field for the secondary fan flow rate that can be autosized.
+
+\subsubsection{Secondary Fan Flow Rate}\label{secondary-fan-flow-rate}
+
+The secondary fan is not part of an airstream that is directly modeled in EnergyPlus. Because the primary side air flows can be autosized as part of the air system, it is convenent to also scale the size of the secondary flow. If the cooler is part of the main loop of a central air system, then the secondary fan flow rate is sized to equal to the main design flow rate.
+
+\begin{equation}
+\dot Vfan,max = DesMainVolFlowsys
+\end{equation}
+
+If the cooler is part of the outdoor air path of a central air system, then the secondary fan flow rate is sized to be the maximum of either the design minimum outdoor air flow rate or one-half of the main design flow rate.
+
+\begin{equation}
+{\dot V_{fan,\max }} = MAX({\rm{DesOutAirVolFlow, 0}}{\rm{.5*DesMainVolFlow)}}
+\end{equation}
+
+\subsection{Secondary DX Coils Sizing}\label{secondary-dx-coils-sizing}
+
+The secondary DX coils model does not have a standalone object and it is models as add-on feature to the DX Coils. When the secondary DX coil is added to a primary DX cooling coil, the heat rejected to secondary zone is sensible only and is treated as tnternal gain, hence secondary air flow rate is not required in the model. Where as when the secondary DX coil is added to a primary DX heating coil, then the heat removed from secondary zone may have sensible and latent components and is treated as tnternal gain. The sensible/latent component split among other parameters requires secondary coil air flow rate. Hence secondary coil air flow rate sizing is added based on the primary DX cooling coil only.
+
+\begin{equation}
+  \dot{V}_{\rm{SecCoil}} = \dot{V}_{\rm{PriHeatCoil}} \cdot \text{ScalingFactor}
+\end{equation}
+
+where
+
+\begin{itemize}
+\tightlist
+\item
+  \(\dot{V}_\text{SecCoil}\) is the secondary coil design air flow rate (m3/s)
+\item
+  \(\dot{V}_\text{SecCoil}\) is the primary heating DX coil design air flow rate (kg/s)
+\item
+  \(\text{ScalingFactor}\) is the secondary DX coil air flow rarte scaling factor (-)
+\end{itemize}
+
+\subsection{Desiccant Dehumidifier Sizing}\label{desiccant-dehumidifier-sizing}
+
+The sizing of dehumidifier with no fans is done in subroutine SizeDesiccantDehumidifier.
+
+\subsubsection{Nominal Process Air Flow Rate}\label{nominal-process-air-flow-rate}
+
+If the unit is part of zone equipment, then:
+
+\begin{equation}
+{\dot V_p} = Max\left( {DesCoolVolFlo{w_{zone}},DesHeatVolFlo{w_{zone}}} \right)
+\end{equation}
+
+If the unit is part of the central air system, then check if outdoor air system is present. If outdoor air system is part of the air loop and design outdoor air flow rate is greater than zero, then:
+
+\begin{equation}
+{\dot V_p} = DesOutAirVolFlo{w_{sys}}
+\end{equation}
+
+Otherwise, nominal process air flow rate is determined as follows:
+
+for duct type = \emph{main}
+
+\begin{equation}
+{\dot V_p} = DesMainVolFlo{w_{sys}}
+\end{equation}
+
+for duct type = \emph{cooling}
+
+\begin{equation}
+{\dot V_p} = DesCoolVolFlo{w_{sys}}
+\end{equation}
+
+for duct type = \emph{heating}
+
+\begin{equation}
+{\dot V_p} = DesHeatVolFlo{w_{sys}}
+\end{equation}
+
+for duct type = \emph{other}
+
+\begin{equation}
+{\dot V_p} = DesMainVolFlo{w_{sys}}
+\end{equation}
+
+\subsection{Evaporative Cooler Sizing}\label{evaporative-cooler-sizing}
+
+The sizing of evaporative cooler objects is done in subroutine SizeEvapCooler.
+
+\subsubsection{Secondary Fan Flow Rate}\label{secondary-fan-flow-rate-1}
+
+\begin{equation}
+\dot V = DesMainVolFlo{w_{sys}}
+\end{equation}
+
+Note that it is only applicable to indirect CELdek pad object.
+
+\subsubsection{Direct Pad Area}\label{direct-pad-area}
+
+As from the continuity equation, the area of direct pad is directly determined by assuming face air velocity of 3m/s as:
+
+\begin{equation}
+{A_{pad}} = \frac{{DesMainVolFlo{w_{sys}}}}{V}
+\end{equation}
+
+where
+
+\begin{itemize}
+\item
+  (A\_\rm{pad} is area of direct pad, m$^{2}$
+\item
+  (V) is face air velocity, m/s
+\end{itemize}
+
+\subsubsection{Direct Pad Depth}\label{direct-pad-depth}
+
+The solution of the following regression equation is used, assuming saturation effectiveness of 70\% and face air velocity of 3m/s:
+
+\begin{equation}
+\begin{split}
+\epsilon =& 0.792714 + 0.958569D - 0.25193V - 1.03215D^2 + 0.0262659V^2 + 0.914869DV - 1.48241VD^2 \\
+&- 0.018992 D V^3 + 1.13137D^3V + 0.0327622 D^2V^3 - 0.145384D^3 V^2
+\end{split}
+\end{equation}
+
+where
+
+\begin{itemize}
+\tightlist
+\item
+  (D) is depth of pad, m
+\item
+  \(\epsilon\) is saturation effectiveness
+\end{itemize}
+
+\subsection{Heat Recovery Sizing}\label{heat-recovery-sizing}
+
+The sizing of heat exchanger objects is done in subroutine SizeHeatRecovery.
+
+\subsubsection{Nominal Supply Air Flow Rate}\label{nominal-supply-air-flow-rate}
+
+If the unit is part of zone equipment, then:
+
+\begin{equation}
+{\dot V_p} = Max\left( {DesCoolVolFlo{w_{zone}},DesHeatVolFlo{w_{zone}}} \right)
+\end{equation}
+
+If the unit is part of the central air system, then check if outdoor air system is present. If outdoor air system is part of the air loop and design outdoor air flow rate is greater than zero, then:
+
+\begin{equation}
+{\dot V_p} = DesOutAirVolFlo{w_{sys}}
+\end{equation}
+
+Otherwise, nominal supply air flow rate is determined as follows:
+
+for duct type = \emph{main}
+
+\begin{equation}
+{\dot V_p} = DesMainVolFlo{w_{sys}}
+\end{equation}
+
+for duct type = \emph{cooling}
+
+\begin{equation}
+{\dot V_p} = DesCoolVolFlo{w_{sys}}
+\end{equation}
+
+for duct type = \emph{heating}
+
+\begin{equation}
+{\dot V_p} = DesHeatVolFlo{w_{sys}}
+\end{equation}
+
+for duct type = \emph{other}
+
+\begin{equation}
+{\dot V_p} = DesMainVolFlo{w_{sys}}
+\end{equation}
+
+\subsubsection{Nominal Supply Air Flow Rate}\label{nominal-supply-air-flow-rate-1}
+
+It is assumed to be equal to the nominal supply air flow rate.
+
+\subsection{Low Temperature Radiant System Sizing}\label{low-temperature-radiant-system-sizing}
+
+The sizing is done in subroutine \emph{SizeLowTempRadiantSystem}.
+
+\subsubsection{ZoneHVAC:LowTemperatureRadiant:Electric:}\label{zonehvaclowtemperatureradiantelectric}
+
+\paragraph{Nominal Capacity}\label{nominal-capacity-1}
+
+\begin{equation}
+Cap = DesHeatLoa{d_{zone}} \cdot HeatSizingFactor
+\end{equation}
+
+\subsubsection{ZoneHVAC:LowTemperatureRadiant:VariableFlow:}\label{zonehvaclowtemperatureradiantvariableflow}
+
+\paragraph{Maximum Hot Water Flow}\label{maximum-hot-water-flow-1}
+
+\begin{equation}
+{\dot V_h} = \frac{{DesHeatLoa{d_{zone}} \cdot HeatSizingFactor}}{{\Delta {T_h} \cdot {c_{p,h}} \cdot {\rho_h}}}
+\end{equation}
+
+where
+
+\({\dot V_h}\) * is maximum hot water flow rate, m\(^{3}\)/s*
+
+\emph{c\(_{p,h}\) is specific heat of hot water at reference condition (60 degC), J/kgK}
+
+\emph{r\(_{h}\) is the density of water at reference condition (60 degC), kg/m\(^{3}\)}
+
+\paragraph{Maximum Cool Water Flow}\label{maximum-cool-water-flow}
+
+\begin{equation}
+{\dot V_c} = \frac{{DesCoolLoa{d_{zone}} \cdot CoolSizingFactor}}{{\Delta {T_c} \cdot {c_{p,c}} \cdot {\rho_c}}}
+\end{equation}
+
+\({\dot V_c}\) * is maximum chilled water flow rate, m\(^{3}\)/s*
+
+\emph{c\(_{p,c}\) is specific heat of hot water at reference condition (5 degC), J/kgK}
+
+\emph{r\(_{c}\) is the density of chilled water at reference condition (5 degC), kg/m\(^{3}\)}
+
+\paragraph{Hydronic Tubing Length}\label{hydronic-tubing-length}
+
+\begin{equation}
+TubeLength = \frac{{TotalSurfaceArea}}{{TubeSpacing}}
+\end{equation}
+
+Note that tube spacing is assumed to be 0.15m.
+
+\subsubsection{ZoneHVAC:LowTemperatureRadiant:ConstantFlow:}\label{zonehvaclowtemperatureradiantconstantflow}
+
+\paragraph{Rated Flow Rate}\label{rated-flow-rate}
+
+The object provides both cooling and heating, and also operates in a single operating mode such as cooling-only or heating-only mode. Thus, the rated flow rate is determined, depending upon the operating mode of the unit. If the unit operates in a single operating mode, either design chilled water or hot water flow rate is chosen. The larger of the two is chosen if the unit provides both cooling and heating. The flow rates are determined in the same fashion to the variable flow system above.
+
+\paragraph{Hydronic Tubing Length}\label{hydronic-tubing-length-1}
+
+The length of hydronic tube is determined as described in the variable flow radiant system above.
+
+\subsection{Unitary System Sizing}\label{unitary-system-sizing}
+
+The AirloopHVAC:UnitarySystem object incorporates all coils types and fans as a complete packaged system. The fans and coils are optional allowing virtually any system type to be modeled. Sizing of this object depends on the coils selected. For single coil systems, the associated air flow rate is used as the operating flow rate (i.e., cooling or heating). For systems with both a cooling and heating coil, this methodology still applies except for DX systems (Heat Pumps) where the greater of the cooling or heating air flow rate is used. Heat pumps are defined as systems having both a DX cooling and DX heating coil. The inputs that may need to be autosized are the supply air air volumetric air flow rates during cooling operation, heating operation, and when no cooling or heating is needed. The data needed for sizing the units are obtained from the zone design arrays.
+
+\subsubsection{Supply Air volumetric flow rate during cooling operation:}\label{supply-air-volumetric-flow-rate-during-cooling-operation-1}
+
+\begin{equation}
+\dot V_{SA,cooling} = \text{DesCoolVolFlow}_{zone} / \text{ZoneFraction}
+\end{equation}
+
+\subsubsection{Supply Air volumetric flow rate during heating operation:}\label{supply-air-volumetric-flow-rate-during-heating-operation-1}
+
+\begin{equation}
+\dot V_{SA,heating} = \text{DesHeatVolFlow}_{zone} / \text{ZoneFraction}
+\end{equation}
+
+\subsubsection{Supply Air volumetric flow rate when DX coils are used as a system:}\label{supply-air-volumetric-flow-rate-when-dx-coils-are-used-as-a-system}
+
+\begin{equation}
+\dot V_{SA} = \max \left(\text{DesCoolVolFlow}_{zone}, \text{DesHeatVolFlow}_{zone}\right) / \text{ZoneFraction}
+\end{equation}
+
+where:
+
+\begin{itemize}
+\tightlist
+\item
+  ZoneFraction = Fraction of the total volume flow that goes through the controlling zone
+\end{itemize}
+
+The unitary system object also allows scalable sizing as follows:
+
+Flow Per Floor Area:
+
+\begin{equation}
+\dot V_{SA} = \left(\text{FlowPerFloorArea}\right)\left(\text{TotalFloorArea}\right)
+\end{equation}
+
+Fraction of Autosized Cooling Value:
+
+\begin{equation}
+\dot V_{SA,cooling} = \dot V_{SA,des,cooling}\left(\text{FractionOfCoolingValue}\right)
+\end{equation}
+
+Fraction of Autosized Heating Value:
+
+\begin{equation}
+\dot V_{SA,heating} = \dot V_{SA,des,heating}\left(\text{FractionOfHeatingValue}\right)
+\end{equation}
+
+Flow Per Cooling Capacity
+
+\begin{equation}
+\dot V_{SA,cooling} = \dot Q_{coil,des,cooling}\left(\text{FractionOfCoolingValue}\right)
+\end{equation}
+
+Flow Per Heating Capacity
+
+\begin{equation}
+\dot V_{SA,heating} = \dot Q_{coil,des,heating}\left(\text{FractionOfHeatingValue}\right)
+\end{equation}
+
+\subsubsection{Maximum Supply Air Temperature}\label{maximum-supply-air-temperature}
+
+The maximum supply air temperature can also be automatically selected. The value is determined from the Sizing:Zone or Sizing:System object depending on where the object is used in the simulation (i.e., as zone or air loop equipment). Maximum supply air temperature
+
+\begin{equation}
+T_{SA,max} = \text{HeatDesTemp}_{ZoneOrSystem}
+\end{equation}
diff --git a/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/hvac-sizing-simulation-manager.tex b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/hvac-sizing-simulation-manager.tex
new file mode 100644
index 00000000000..20456d43923
--- /dev/null
+++ b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/hvac-sizing-simulation-manager.tex
@@ -0,0 +1,46 @@
+\section{HVAC Sizing Simulation Manager}\label{hvac-sizing-simulation-manager}
+
+After the Sizing Manager has completed its initial pass, all the data needed to complete a running model should be available and the program is ready to run the main simulation(s). However, as of Version 8.3 there is now an option of applying some advanced sizing calculations using what are called HVAC Sizing Simulations.
+
+With this new sizing method we distinguish between different kinds of simulations and introduce some new terminology. The Primary Simulations are the main simulations that are the final version of the model to be run. Prior to Version 8.3, these are just the usual simulations with the final results. When the program is running the zone heat balance model over the sizing periods for zone sizing (for step 3 in the Sizing Manager description above), we call those Ideal Loads Sizing Simulations. When the program is running the zone heat balance model over the sizing periods for component loads calculations we call those Ideal Component Loads Simulations. HVAC Sizing Simulations are a kind of simulation, where the program creates copies of sizing periods and runs them as complete EnergyPlus simulations with the most current equipment sizes and full HVAC systems. The advanced sizing algorithms monitor what occurred during those sizing periods and determines if new size results are needed and signals systems and components to repeat their sizing calculations. The process can repeat in an iterative manner and a Sizing Pass refers to a set of the HVAC Sizing Simulations for each of the sizing periods (e.g.~two design days).
+
+If the user has selected a sizing option that requires HVAC Sizing Simulations the main ManageSimulation will call ManageHVACSizingSimulation before going on to the main simulations.
+
+\begin{itemize}
+\item
+  Instantiate a new HVACSizingSimulationManager object.
+\item
+  Call DetermineSizingAnalysesNeeded(). This checks what user input and decides what, if anything, needs to be done for advanced sizing algorithms. This involves, for example, checking the input in Sizing:Plant object to see if coincident sizing option has been selected.
+\item
+  Call SetupSizingAnalyses(). This method creates the data logging apparatus needed to monitor operation during HVAC Sizing Simulations. Individual sizing algorithms include selecting specific variables, such as system node states or load output variables, that will be recorded.
+\item
+  Loop over some number of Sizing Passes. The set of sizing periods, run as HVAC Sizing Simulations, can iterate up to a maximum limit on the number of passes
+\end{itemize}
+
+\begin{lstlisting}
+-   Loop over all the sizing periods by each day. This runs the HVAC Sizing Simulations which have basically the same set of calls as are used for marching through time and calling of EnergyPlus modeling for the Primary Simulations (in ManageSimulation).
+\end{lstlisting}
+
+\begin{lstlisting}
+    -   Call PostProcessLogs(). This method applies running averages (if desired) and averages system timestep data to fill zone timestep data in the records.
+\end{lstlisting}
+
+\begin{lstlisting}
+    -   Call ProcessCoincidentPlantSizeAdjustments(). This method retrieves data from the logs and calls for the coincident plant sizing algorithm to execute. Set flag if the sizing analyses request another Sizing Pass. (See the section below on Coincident Plant Sizing.)
+\end{lstlisting}
+
+\begin{lstlisting}
+    -   Call RedoKickOffAndResize(). The methods calls SetupSimulation() and sets flag to signal that system and component level sizing methods need to be called again. These are fake timesteps used to initialize and are not part of a Simulation.
+\end{lstlisting}
+
+\begin{lstlisting}
+-   Break out of Sizing Pass loop if size results did not change or the limit on Sizing Passes has been reached.
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  Empty HVACSizingSimulationManager object to free memory
+\end{itemize}
+
+Currently the only application for HVAC Sizing Simulations is to improve the sizing of plant loops using the Coincident sizing option. However this approach may be expanded in the future to extend advanced sizing methods to air-side equipment.
diff --git a/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/plant-loop-sizing.tex b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/plant-loop-sizing.tex
new file mode 100644
index 00000000000..70456f9e8b1
--- /dev/null
+++ b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/plant-loop-sizing.tex
@@ -0,0 +1,33 @@
+\section{Plant Loop Sizing}\label{plant-loop-sizing}
+
+\subsection{Introduction}\label{introduction-000}
+
+The program needs to be able to autosize the fluid flow rate in each plant fluid loop. The design plant loop flow rates are set by the sum of the needs of the demanding components on each loop. For chilled water loops these components will be cooling coils. For hot water loops - hot water coils. And for condenser loops - various types of chiller that use condenser water for cooling. Each component that uses water for heating or cooling stores its design water flow rate (in its sizing routine) in the array \emph{CompDesWaterFlow}, labeled by its inlet water supply node number. These individual component design water flow rates are then accessed, summed for each plant loop, and stored in the \emph{PlantSizingData} array. This array also contains the user specified design values for each plant loop.
+
+\subsection{Hot and Chilled Water Loop Sizing}\label{hot-and-chilled-water-loop-sizing}
+
+\subsubsection{Maximum Loop Volumetric Flow Rate}\label{maximum-loop-volumetric-flow-rate}
+
+The loop maximum volumetric flow rate (m\(^{3}\)) is just set equal to the value stored in the \emph{PlantSizData} array for this loop.
+
+\subsubsection{Volume of the plant loop}\label{volume-of-the-plant-loop}
+
+Since the loop capacitance has a stability requirement of \((\dot V\cdot \Delta tstep/V) \le 1\) the volume is set so that the stability requirement will be 0.8 at the zone time step, which is the largest time step encountered at the max flow rate the loop can reach.
+
+\begin{equation}
+Vloop = (\dot Vloop,max\cdot \Delta tstep,zone\cdot 3600)/0.8
+\end{equation}
+
+\subsection{Condenser Loop Sizing}\label{condenser-loop-sizing}
+
+\subsubsection{Maximum Loop Volumetric Flow Rate}\label{maximum-loop-volumetric-flow-rate-1}
+
+The loop maximum volumetric flow rate (m\(^{3}\)) is just set equal to the value stored in the \emph{PlantSizData} array for this loop.
+
+\subsubsection{Volume of the plant loop}\label{volume-of-the-plant-loop-1}
+
+Since the loop capacitance has a stability requirement of \((\dot V\cdot \Delta tstep/V) \le 1\) the volume is set so that the stability requirement will be 0.8 at the zone time step, which is the largest time step encountered at the max flow rate the loop can reach.
+
+\begin{equation}
+Vloop = (\dot Vloop,max\cdot \Delta tstep,zone\cdot 3600)/0.8
+\end{equation}
diff --git a/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/sizing-manager.tex b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/sizing-manager.tex
new file mode 100644
index 00000000000..b0a3a3eee27
--- /dev/null
+++ b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/sizing-manager.tex
@@ -0,0 +1,78 @@
+\section{Sizing Manager}\label{sizing-manager}
+
+The sizing calculations in EnergyPlus are managed by a sizing manager contained in the software module \emph{SizingManager}. The main sizing manager routine \emph{ManageSizing} is called from \emph{ManageSimulation} before the annual simulation sequence is invoked. \emph{ManageSizing} performs the following tasks.
+
+\begin{itemize}
+\item
+  By calling \emph{GetSizingParams}, \emph{GetZoneSizingInput}, \emph{GetSystemSizingInput} and \emph{GetPlantSizingInput} reads in all the user sizing input contained in objects \emph{Sizing:Parameters}, \emph{Sizing:Zone}, \emph{Sizing:System} and \emph{Sizing:Plant}. These objects and their data are described in the EnergyPlus Input Output Reference, Group Design Objects.
+\item
+  Set the \emph{ZoneSizingCalc} flag equal to \emph{true}.
+\item
+  Loop over all the sizing periods by each day. \textbf{This starts the zone design calculations.}
+\end{itemize}
+
+\begin{lstlisting}
+-   Call *UpdateZoneSizing(BeginDay)* to initialize zone design load and flow rate sequences.
+\end{lstlisting}
+
+\begin{lstlisting}
+-   Loop over hours in the day
+\end{lstlisting}
+
+\begin{lstlisting}
+    -   Loop over zone time steps in each hour
+\end{lstlisting}
+
+\begin{lstlisting}
+        -   Call *ManageWeather* to obtain outside conditions for this time-step.
+\end{lstlisting}
+
+\begin{lstlisting}
+        -   Call *ManageHeatBalance* to do a full heat balance calculation for each zone. The call to *ManageHeatBalance* also brings about an HVAC simulation. *ZoneSizingCalc = true* signals the *HVACManager* to ignore the real HVAC system and instead run the ideal zonal system (described below) used to calculate design loads and flow rates. HVACManager also calls *UpdateZoneSizing(DuringDay)* to save the results of the ideal zonal system calculation in the design load and flow rate sequences.
+\end{lstlisting}
+
+\begin{lstlisting}
+    -   Call *UpdateZoneSizing(EndDay)* to calculate peaks and moving averages from the zone design sequences for each design day.
+\end{lstlisting}
+
+\begin{itemize}
+\item
+  Call \emph{UpdateZoneSizing(EndZoneSizingCalc)} to calculate for each zone the peak heating \& cooling loads and flow rates over all the sizing periods (design days and sizing periods from the weather file, if specified). The corresponding design load and flow rate sequences are saved for use in the system design calculations. \textbf{This ends the zone design calculations.}
+\item
+  Set the \emph{SysSizingCalc} flag equal to \emph{true}.
+\item
+  Call \emph{ManageZoneEquipment} and \emph{ManageAirLoops} to read in the zone and central system inputs needed for the system design calculations. The program needs enough information to be able to figure out the overall air loop connectivity.
+\item
+  Loop over all the sizing periods by each day. \textbf{This starts the system design calculations.}
+\end{itemize}
+
+\begin{lstlisting}
+-   Call *UpdateSysSizing(BeginDay)* to initialize system design load and flow rate sequences.
+\end{lstlisting}
+
+\begin{lstlisting}
+-   Loop over hours in the day
+\end{lstlisting}
+
+\begin{lstlisting}
+    -   Loop over zone time steps in each hour
+\end{lstlisting}
+
+\begin{lstlisting}
+        -   Call *ManageWeather* to obtain outside conditions for this time-step.
+\end{lstlisting}
+
+\begin{lstlisting}
+        -   Call *UpdateSysSizing(DuringDay)* to save the results of the system design calculations in the system design load and flow rate sequences.
+\end{lstlisting}
+
+\begin{lstlisting}
+-   Call *UpdateSysSizing(EndDay)* to calculate peaks and moving averages from the system design sequences for each sizing period.
+\end{lstlisting}
+
+\begin{itemize}
+\item
+  Call \emph{UpdateSysSizing(EndSysSizingCalc))} to calculate for each system the peak heating \& cooling loads and flow rates over all the sizing periods (design days and sizing periods from the weather file, if specified). The corresponding design load and flow rate sequences are saved for use in the component sizing calculations. \textbf{This ends the system design calculations.}
+\item
+  And this ends the tasks of the Sizing Manager.
+\end{itemize}
diff --git a/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/system-design-loads-and-air-flow-rates.tex b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/system-design-loads-and-air-flow-rates.tex
new file mode 100644
index 00000000000..530bd34a1c0
--- /dev/null
+++ b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/system-design-loads-and-air-flow-rates.tex
@@ -0,0 +1,562 @@
+\section{System Design Loads and Air Flow Rates}\label{system-design-loads-and-air-flow-rates}
+
+\subsection{Overview}\label{overview-026}
+
+The purpose of the system design calculation is to estimate design heating and cooling loads and air flow rates for each air loop in the simulation problem. The calculation sequence for system level design loads and air flow rates resembles the calculation sequence for zone loads and air flow rates. There is an update subroutine \emph{UpdateSysSizing} called at the beginning, during, and end of a loop in the Sizing Manager over all the design days. The major difference is that this calculation is done at the zone time-step only. There is no idealized component calculation triggered at the system time-step as in the zone calculation. The system design calculation operates at the zone time step using the design environment weather data and the data stored in the zone sizing arrays. The results of the system design calculation are stored in the system sizing arrays described below.
+
+\subsection{System Design Data Arrays}\label{system-design-data-arrays}
+
+The system design data arrays are:
+
+\emph{SysSizInput(i)} stores the input data from the Sizing:System objects.
+
+\emph{SysSizing(i,j)} stores the results of the system design calculations for all systems and all design days. The index i is for air loops, j for design days.
+
+\emph{CalcSysSizing(i}) stores the results of the system design calculations for the peak heating and cooling cases for each air loop. The index i is for the air loops.
+
+\emph{FinalSysSizing(i}) corresponds to \emph{CalcSysSizing} but includes the effect of the user specified sizing factor or user specified system design flow rate.
+
+The data stored in \emph{SysSizing}, \emph{CalcSysSizing} and \emph{FinalSysSizing} includes the following data items.
+
+% table 41
+\begin{longtable}[c]{p{2.0in}p{4.0in}}
+\caption{System Sizing Data \label{table:system-sizing-data}} \tabularnewline
+\toprule 
+Name & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{System Sizing Data} \tabularnewline
+\toprule
+Name & Description \tabularnewline
+\midrule
+\endhead
+
+All the data from SysSizInput &  \tabularnewline
+CoinCoolMassFlow & coincident peak cooling mass flow rate [kg/s] \tabularnewline
+CoinHeatMassFlow & coincident peak heating mass flow rate [kg/s] \tabularnewline
+NonCoinCoolMassFlow & noncoincident peak cooling mass flow rate [kg/s] \tabularnewline
+NonCoinHeatMassFlow & noncoincident peak heating mass flow rate [kg/s] \tabularnewline
+DesMainVolFlow & design main supply duct volume flow [m  /s] \tabularnewline
+DesHeatVolFlow & design heat supply duct volume flow [m  /s] \tabularnewline
+DesCoolVolFlow & design cool supply duct volume flow [m  /s] \tabularnewline
+SensCoolCap & design sensible cooling capacity [W] \tabularnewline
+TotCoolCap & design total cooling capacity [W] \tabularnewline
+HeatCap & design heating capacity [W] \tabularnewline
+PreheatCap & design preheat capacity [W] \tabularnewline
+MixTempAtCoolPeak & mixed air temperature at the time of the cooling peak [C] \tabularnewline
+MixHumRatAtCoolPeak & mixed air humidity ratio at the time of the cooling peak [kg water/kg dry air] \tabularnewline
+RetTempAtCoolPeak & return air temperature at the time of the cooling peak [C] \tabularnewline
+RetHumRatAtCoolPeak & return air humidity ratio at the time of the cooling peak [kg water/kg dry air] \tabularnewline
+OutTempAtCoolPeak & outside air temperature at the time of the cooling peak [C] \tabularnewline
+OutHumRatAtCoolPeak & outside air humidity ratio at the time of the cooling peak [kg water/kg dry air] \tabularnewline
+HeatMixTemp & design mixed air temperature for heating [C] \tabularnewline
+HeatMixHumRat & design mixed air humidity ratio for heating [kg water/kg dry air] \tabularnewline
+HeatRetTemp & design return air temperature for heating [C] \tabularnewline
+HeatRetHumRat & design return air humidity ratio for heating [kg water/kg dry air] \tabularnewline
+HeatOutTemp & design outside air temperature for heating [C] \tabularnewline
+HeatOutHumRat & design outside air humidity ratio for heating [kg water/kg dry air] \tabularnewline
+HeatFlowSeq(i) & daily sequence of system heating air mass flow rate (zone time step) [kg/s] \tabularnewline
+CoolFlowSeq(i) & daily sequence of system cooling air mass flow rate (zone time step) [kg/s] \tabularnewline
+SumZoneCoolLoadSeq(I) & daily sequence of zones' summed cooling load (zone time step) [W] \tabularnewline
+CoolZoneAvgTempSeq(I) & daily sequence of zones flow weighted average temperature (zone time step) [W] \tabularnewline
+SensCoolCapSeq(I) & daily sequence of system sensible cooling capacity (zone time step) [W] \tabularnewline
+TotCoolCapSeq(I) & daily sequence of system total cooling capacity (zone time step) [W] \tabularnewline
+HeatCapSeq(i) & daily sequence of system heating capacity (zone time step) [W] \tabularnewline
+PreHeatCapSeq(i) & daily sequence of system preheat capacity (zone time step) [W] \tabularnewline
+SysCoolRetTempSeq(i) & daily sequence of system cooling return temperatures (zone time step) [C] \tabularnewline
+SysCoolRetHumRatSeq(I) & daily sequence of system cooling return humidity ratios (zone time step) [kg water/kg dry air] \tabularnewline
+SysHeatRetTempSeq(i) & daily sequence of system heating return temperatures (zone time step) [C] \tabularnewline
+SysHeatRetHumRatSeq(I) & daily sequence of system heating return humidity ratios (zone time step) [kg water/kg dry air] \tabularnewline
+SysCoolOutTempSeq & daily sequence of system cooling outside temperatures (zone time step) [C] \tabularnewline
+SysCoolOutHumRatSeq & daily sequence of system cooling outside humidity ratios (zone time step) [kg water/kg dry air] \tabularnewline
+SysHeatOutTempSeq & daily sequence of system heating outside temperatures (zone time step) [C] \tabularnewline
+SysHeatOutHumRatSeq & daily sequence of system heating outside humidity ratios (zone time step) [kg water/kg dry air] \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{System Design Flow Rate and Load Summation and Adjustment}\label{system-design-flow-rate-and-load-summation-and-adjustment}
+
+There is no system level subroutine corresponding to \emph{SizeZoneEquipment.} Instead the system design loads and flow rates are calculated using the zone level results. The zone design flow rates for the zones served by an air loop are summed to obtain the system level design flow rates. These air flows are mixed with the system level design minimum outside air flow rate to obtain system design coil loads. These activities are all performed within the \emph{UpdateSysSizing} subroutine in the \emph{SimAirServingZones} module. It is called at the start of each design day (\emph{CallIndicator = BeginDay}), at the zone time-step (\emph{CallIndicator = DuringDay}), at the end of the design day (\emph{CallIndicator = EndDay}) and at the end of the zone design calculation (\emph{CallIndicator = EndSysSizingCalc}).
+
+There is a logical flag \emph{SysSizingCalc} corresponding to \emph{ZoneSizingCalc}. It is used to allow the component routines to distinguish a normal simulation call from a being called during a system sizing calculation.
+
+\subsubsection{BeginDay}\label{beginday}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\item
+  The environment (in this case, a design day) name is stored in the system sizing data structures.
+\item
+  Loop over the zones cooled by this air loop: 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\alph{enumi})}
+\tightlist
+\item
+  \emph{NonCoinCoolMassFlow\(_{sys}\)} = \emph{DesCoolMassFlow\(_{zone}\)} 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Loop over the zones heated by this air loop: 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\alph{enumi})}
+\tightlist
+\item
+  \emph{NonCoinHeatMassFlow\(_{sys}\)} = \emph{DesHeatMassFlow\(_{zone}\)}
+\end{enumerate}
+
+\subsubsection{DuringDay}\label{duringday}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\tightlist
+\item
+  Loop over the zones cooled by this air loop:
+\end{enumerate}
+
+\emph{CoolFlowSeq\(_{sys}\)(i)} = \emph{CoolFlowSeq \(_{zone}\)}(i)
+
+\emph{SysCoolRetTemp(i)} = (\emph{CoolZoneRetTempSeq(i) * CoolFlowSeq\(_{zone}\)(i)})\emph{/ CoolFlowSeq\(_{sys}\)(i)}
+
+\emph{SysCoolRetHumRat(i)} = (\emph{CoolZoneHumRatSeq(i) * CoolFlowSeq\(_{zone}\)(i)})\emph{/ CoolFlowSeq\(_{sys}\)(i)}
+
+\emph{FracOA = r\(_{air}\)} * \emph{DesOutAirVolFlow\(_{sys}\)}/ \emph{CoolFlowSeq\(_{sys}\)(i)}
+
+\emph{T\(_{mix}\)} = \emph{T\(_{outside}\)} * \emph{FracOA} + \emph{SysCoolRetTemp(i)}(1 - \emph{FracOA})
+
+\emph{W\(_{mix}\)} = \emph{W\(_{outside}\)} * \emph{FracOA} + \emph{SysCoolRetHumRat (i)}(1 - \emph{FracOA})
+
+\emph{SysCoolOutTempSeq(i)} = \emph{T\(_{outside}\)}
+
+\emph{SysCoolOutHumRatSeq(i)} = \emph{W\(_{outside}\)}
+
+Get the current (zone time-step) system cooling capacity:
+
+\emph{SysSensCoolCap\(_{cur}\)} = \emph{C\(_{p,air}\)} * \emph{CoolFlowSeq\(_{sys}\)(i)} *( \emph{T\(_{mix}\)}-\emph{T\(_{sup}\)})
+
+\emph{SensCoolCapSeq(I)} = \emph{SysSensCoolCap\(_{cur}\)}
+
+If \emph{SysSensCoolCap\(_{cur}\)} is the maximum for the day so far then save \emph{SysSensCoolCap\(_{cur}\)} as the design value:
+
+\emph{SensCoolCap(i )\(_{sys}\)} = \emph{SysSensCoolCap\(_{cur}\)}
+
+And save the corresponding mixed, return and outside conditions:
+
+\emph{CoolMixTemp\(_{sys}\)} = \emph{T\(_{mix}\)}
+
+\emph{CoolMixHumRat\(_{sys}\)} = \emph{W\(_{mix}\)}
+
+\emph{CoolRetTemp\(_{sys}\)} = \emph{SysCoolRetTemp(i)}
+
+\emph{CoolRetHumRat\(_{sys}\)} = \emph{SysCoolRetHumRat(I)}
+
+\emph{CoolOutTemp\(_{sys}\)} = \emph{T\(_{outside}\)}
+
+\emph{CoolOutHumRat\(_{sys}\)} = \emph{W\(_{outside}\)}
+
+Here \emph{r\(_{air}\)} is the density of dry air at 20C and standard elevation corrected pressure, {[}kg/m\(^{3}\){]};
+
+\begin{lstlisting}
+        *FracOA* is the outside air fraction;
+\end{lstlisting}
+
+\begin{itemize}
+\item
+  C\(_{p,air}\)* is the specific heat of dry air at 20C, {[}J/kg-K{]};
+\item
+  T\(_{sup}\)* is the user specified design cooling supply temperature {[}C{]};
+\item
+  T\(_{mix}\)* is the current mixed air temperature {[}C{]};
+\item
+  W\(_{mix}\)* is the current mixed air humidity ratio {[}kg water / kg dry air{]};
+\item
+  \(T_{outside}\) is the current outside air temperature {[}C{]};
+\item
+  \(W_{outside}\) is the current outside air humidity ratio {[}kg water / kg dry air{]}.
+\end{itemize}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Loop over the zones heated by this air loop.
+\end{enumerate}
+
+\emph{HeatFlowSeq\(_{sys}\)(i)} = \emph{HeatFlowSeq \(_{zone}\)}(i)
+
+\emph{SysHeatRetTemp(i)} = (\emph{HeatZoneRetTempSeq(i) * HeatFlowSeq\(_{zone}\)(i)})\emph{/}
+
+\emph{HeatFlowSeq\(_{sys}\)(i)}
+
+\emph{SysHeatRetHumRat(i)} = (\emph{HeatZoneHumRatSeq(i) * HeatFlowSeq\(_{zone}\)(i)})\emph{/}
+
+\begin{itemize}
+\tightlist
+\item
+  HeatFlowSeq\(_{sys}\)(i)*
+\end{itemize}
+
+\emph{FracOA = r\(_{air}\)} * \emph{DesOutAirVolFlow\(_{sys}\)}/ \emph{HeatFlowSeq\(_{sys}\)(i)}
+
+\emph{T\(_{mix}\)} = \emph{T\(_{outside}\)} * \emph{FracOA} + \emph{SysHeatRetTemp(i)}(1 - \emph{FracOA})
+
+\emph{W\(_{mix}\)} = \emph{W\(_{outside}\)} * \emph{FracOA} + \emph{SysHeatRetHumRat (i)}(1 - \emph{FracOA})
+
+\emph{SysHeatOutTempSeq(i)} = \emph{T\(_{outside}\)}
+
+\emph{SysHeatOutHumRatSeq(i)} = \emph{W\(_{outside}\)}
+
+Get the current (zone time-step) system heating capacity:
+
+\emph{SysHeatCap\(_{cur}\)} = \emph{C\(_{p,air}\)} * \emph{MinFlowRat\(_{sys}\)} *\emph{HeatFlowSeq\(_{sys}\)(i)} *( \emph{T\(_{sup}\)}-\emph{T\(_{mix}\)})
+
+\emph{HeatCapSeq(I)} = \emph{SysHeatCap\(_{cur}\)}
+
+If \emph{SysHeatCap\(_{cur}\)} is the maximum for the day so far then save \emph{SysHeatCap\(_{cur}\)} as the design value:
+
+\emph{HeatCap(i )\(_{sys}\)} = \emph{SysHeatCap\(_{cur}\)}
+
+And save the corresponding mixed, return and outside conditions:
+
+\emph{HeatMixTemp\(_{sys}\)} = \emph{T\(_{mix}\)}
+
+\emph{HeatMixHumRat\(_{sys}\)} = \emph{W\(_{mix}\)}
+
+\emph{HeatRetTemp\(_{sys}\)} = \emph{SysHeatRetTemp(i)}
+
+\emph{HeatRetHumRat\(_{sys}\)} = \emph{SysHeatRetHumRat(I)}
+
+\emph{HeatOutTemp\(_{sys}\)} = \emph{T\(_{outside}\)}
+
+\emph{HeatOutHumRat\(_{sys}\)} = \emph{W\(_{outside}\)}
+
+Here \emph{MinFlowRat\(_{sys}\)} is the user specified minimum supply flow ratio.
+
+\subsubsection{EndDay}\label{endday}
+
+If the user has specified \emph{coincident} system sizing then:
+
+\emph{DesCoolVolFlow\(_{sys}\)} = \emph{r\(_{air}\)} *\emph{CoinCoolMassFlow\(_{sys}\)}
+
+\emph{DesHeatVolFlow\(_{sys}\)} = \emph{r\(_{air}\)} *\emph{CoinHeatMassFlow\(_{sys}\)}
+
+\emph{DesMainVolFlow\(_{sys}\)} = \textbf{Max}(\emph{DesCoolVolFlow\(_{sys}\)}, \emph{DesHeatVolFlow\(_{sys}\)})
+
+If the user has specified \emph{noncoincident}system sizing then:
+
+\emph{DesCoolVolFlow\(_{sys}\)} = \emph{r\(_{air}\)} *\emph{NonCoinCoolMassFlow\(_{sys}\)}
+
+\emph{DesHeatVolFlow\(_{sys}\)} = \emph{r\(_{air}\)} *\emph{NonCoinHeatMassFlow\(_{sys}\)}
+
+\emph{DesMainVolFlow\(_{sys}\)} = \textbf{Max}(\emph{DesCoolVolFlow\(_{sys}\)}, \emph{DesHeatVolFlow\(_{sys}\)})
+
+Based on the outdoor air method selected, the \emph{DesCoolVolFlow\(_{sys}\)} and \emph{DesHeatVolFlow\(_{sys}\)} are modified based on the system ventilation effciency calculated based on the maximum outdoor air fraction.
+
+\subsubsection{EndSysSizingCalc}\label{endsyssizingcalc}
+
+At this point all the calculations have been done in \emph{SysSizing(i,j)}: we have results for each design day. Now these results need to be processed to find the heating and cooling design quantities for each system over all the design days.
+
+For coincident sizing the task is quite easy.
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\tightlist
+\item
+  Loop over all of the air loops. 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\alph{enumi})}
+\item
+  Loop over all of the design days.
+\item
+  If the value of \emph{DesCoolVolFlow} in \emph{SysSizing} for the current design day is greater than the value stored in \emph{CalcSysSizing}, then move \emph{DesCoolVolFlow} from \emph{SysSizing} into \emph{CalcSysSizing} along with \emph{CoolDesDay}, \emph{CoinCoolMassFlow}, \emph{SensCoolCap}, \emph{CoolFlowSeq(i)}, \emph{SensCoolCapSeq(i),} \emph{CoolMixTemp}, \emph{CoolRetTemp}, \emph{CoolMixHumRat}, \emph{CoolRetHumRat}, \emph{CoolOutTemp}, \emph{CoolOutHumRat}, \emph{SysCoolRetTempSeq(i)}, \emph{SysCoolRetHumRatSeq(i)}, \emph{SysCoolOutTempSeq(i)} and \emph{SysCoolOutHumRatSeq(i)}. 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\roman{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  If the value of \emph{DesHeatVolFlow} in \emph{SysSizing} for the current design day is greater than the value stored in \emph{CalcSysSizing}, then move \emph{DesHeatVolFlow} from \emph{SysSizing} into \emph{CalcSysSizing} along with \emph{HeatDesDay}, \emph{CoinHeatMassFlow}, \emph{HeatCap}, \emph{PreHeatCap}, \emph{HeatFlowSeq(i)}, \emph{HeatCapSeq(i),} \emph{PreHeatCapSeq(i), HeatMixTemp}, \emph{HeatRetTemp}, \emph{HeatMixHumRat}, \emph{HeatRetHumRat}, \emph{HeatOutTemp}, \emph{HeatOutHumRat}, \emph{SysHeatRetTempSeq(i)}, \emph{SysHeatRetHumRatSeq(i)}, \emph{SysHeatOutTempSeq(i)} and \emph{SysHeatOutHumRatSeq(i)}.
+\end{enumerate}
+
+At the end of each design day loop the peak cooling and the peak heating data will be stored in \emph{CalcSysSizing}. At this point we set \emph{DesMainVolFlow} in \emph{CalcSysSizing} equal to the maximum of \emph{DesCoolVolFlow} and \emph{DesHeatVolFlow.}
+
+For noncoincident sizing the task is harder since we don't have a single time-step during which all the zone peaks occur. So there is no obvious value for outside air temperature at the peak, return air temperature at the peak and so forth. We must return to the zone sizing data and calculate average values for return and outside conditions.
+
+\begin{enumerate}
+\def\labelenumi{(\alph{enumi})}
+\setcounter{enumi}{1}
+\item
+  Loop over all of the zones cooled by this air loop
+\item
+  In \emph{FinalZoneSizing} replace the value in \emph{DesCoolCoilInTemp} with the user specified \emph{CoolSupTemp\(_{sys}\)}. Do the same for \emph{DesCoolCoilInHumRat} and \emph{CoolSupHumRat}. This ensures that zone equipment connected to an air loop will use the system design supply air conditions as coil entering conditions. 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\roman{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  \emph{NonCoinCoolMassFlow\(_{sys}\)} = \emph{DesCoolMassFlow\(_{zone}\)}
+\end{enumerate}
+
+\emph{SysCoolRetTemp} = (\emph{ZoneRetTempAtCoolPeak *DesCoolMassFlow\(_{zone}\)})
+
+/\emph{NonCoinCoolMassFlow\(_{sys}\)}
+
+\emph{SysCoolRetHumRat} = (\emph{ZoneHumRatAtCoolPeak *}
+
+\emph{DesCoolMassFlow\(_{zone}\)})/\emph{NonCoinCoolMassFlow\(_{sys}\)}
+
+\emph{SysCoolOutTemp} = (\emph{T\(_{OA,zone\, peak}\) *DesCoolMassFlow\(_{zone}\)})/
+
+\begin{itemize}
+\tightlist
+\item
+  NonCoinCoolMassFlow\(_{sys}\)*
+\end{itemize}
+
+\emph{SysCoolOutHumRat} = (\emph{W\(_{OA,zone\\ peak}\) *DesCoolMassFlow\(_{zone}\)})/
+
+\begin{itemize}
+\tightlist
+\item
+  NonCoinCoolMassFlow\(_{sys}\)*
+\end{itemize}
+
+At the end of the zone loop calculate mixed air conditions and the system sensible cooling capacity.
+
+\emph{FracOA = r\(_{air}\)} * \emph{DesOutAirVolFlow\(_{sys}\)}/ \emph{NonCoinCoolMassFlow\(_{sys}\)}
+
+\emph{T\(_{mix}\)} = \emph{SysCoolOutTemp} * \emph{FracOA} + \emph{SysCoolRetTemp} * (1 - \emph{FracOA})
+
+\emph{W\(_{mix}\)} = \emph{SysCoolOutHumRat} * \emph{FracOA} + \emph{SysCoolRetHumRat} *
+
+(1 - \emph{FracOA})
+
+\emph{SysSensCoolCap} = \emph{C\(_{p,air}\)} * \emph{NonCoinCoolMassFlow} *( \emph{T\(_{mix}\)}-\emph{T\(_{sup}\)})
+
+Then (for noncoincident sizing) the variables calculated in section (ii) are moved into the \emph{CalcSysSizing} Array.
+
+\begin{enumerate}
+\def\labelenumi{(\alph{enumi})}
+\setcounter{enumi}{2}
+\item
+  Loop over all of the zones heated by this air loop.
+\item
+  In \emph{FinalZoneSizing} replace the value in \emph{DesHeatCoilInTemp} with the user specified \emph{HeatSupTemp\(_{sys}\)}. Do the same for \emph{DesHeatCoilInHumRat} and \emph{HeatSupHumRat}. This ensures that zone equipment connected to an air loop will use the system design supply air conditions as coil entering conditions. 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\roman{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  \emph{NonCoinHeatMassFlow\(_{sys}\)} = \emph{DesHeatMassFlow\(_{zone}\)}
+\end{enumerate}
+
+\emph{SysHeatRetTemp} = (\emph{ZoneRetTempAtHeatPeak *DesHeatMassFlow\(_{zone}\)})
+
+/\emph{NonCoinHeatMassFlow\(_{sys}\)}
+
+\emph{SysHeatRetHumRat} = (\emph{ZoneHumRatAtHeatPeak *}
+
+\emph{DesHeatMassFlow\(_{zone}\)})/\emph{NonCoinHeatMassFlow\(_{sys}\)}
+
+\emph{SysHeatOutTemp} = (\emph{T\(_{OA,zone\\ peak}\) *DesHeatMassFlow\(_{zone}\)})/
+
+\begin{itemize}
+\tightlist
+\item
+  NonCoinHeatMassFlow\(_{sys}\)*
+\end{itemize}
+
+\emph{SysHeatOutHumRat} = (\emph{W\(_{OA,zone\\ peak}\) *DesHeatMassFlow\(_{zone}\)})/
+
+\begin{itemize}
+\tightlist
+\item
+  NonCoinHeatMassFlow\(_{sys}\)*
+\end{itemize}
+
+At the end of the zone loop calculate mixed air conditions and the system sensible cooling capacity.
+
+\emph{FracOA = r\(_{air}\)} * \emph{DesOutAirVolFlow\(_{sys}\)}/ \emph{NonCoinHeatMassFlow\(_{sys}\)}
+
+\emph{T\(_{mix}\)} = \emph{SysHeatOutTemp} * \emph{FracOA} + \emph{SysHeatRetTemp} * (1 - \emph{FracOA})
+
+\emph{W\(_{mix}\)} = \emph{SysHeatOutHumRat} * \emph{FracOA} + \emph{SysHeatRetHumRat} *
+
+(1 - \emph{FracOA})
+
+\emph{SysHeatlCap} = \emph{C\(_{p,air}\)} * \emph{NonCoinHeatlMassFlow} *( \emph{T\(_{sup}\)}-\emph{T\(_{mix}\)})
+
+Then (for noncoincident sizing) the variables calculated in section (ii) are moved into the \emph{CalcSysSizing} Array.
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  We now have the calculated system sizing data. This data needs to be altered to take into account the user input system design flow rates (if any), or the fact that the user may have requested that the system flow rate be sized on the ventilation requirement. Note that user specified sizing ratios have already been applied to the zone sizing data which have been used in out preceding system sizing calculation. Thus the user specified sizing ratios do not have to be explicitly taken into account at the system level.
+\end{enumerate}
+
+First we move the calculated system sizing data from \emph{CalcSysSizing} array into the \emph{FinalSysSizing} array. \emph{FinalSysSizing} will contain the user modified system design data when we are all done.
+
+Loop over the air loops.
+
+\begin{enumerate}
+\def\labelenumi{(\roman{enumi})}
+\tightlist
+\item
+  As in the zone case, the user specified system design flow rates are turned into sizing ratios by dividing the user input value by the calculated value. The same strategy is employed for sizing on the ventilation requirement: the design ventilation flow rate is divided by the calculated design flow rate value. For each air loop this gives us a \emph{SizRat\(_{cool}\)} and \emph{SizRat\(_{heat}\)}.
+\end{enumerate}
+
+\emph{CoinCoolMassFlow} = \emph{SizRat\(_{cool}\)} * \emph{CoinCoolMassFlow\(_{calc}\)}
+
+\emph{NonCoinCoolMassFlow} = \emph{SizRat\(_{cool}\)} * \emph{NonCoinCoolMassFlow\(_{calc}\)}
+
+\emph{DesCoolVolFlow} = \emph{SizRat\(_{cool}\)} * \emph{DesCoolVolFlow\(_{calc}\)}
+
+Since the flow rates have been altered the outside air fraction will change. This will alter the design mixed air conditions and lead to an altered value for the cooling capacity. This must be done for the time-step sequence and for the peak value.
+
+\begin{enumerate}
+\def\labelenumi{(\roman{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Loop over the zone timesteps (index = \emph{i}).
+\end{enumerate}
+
+\emph{CoolFlowSeq\(_{sys}\)(i)} = \emph{SizRat\(_{cool}\)} * \emph{CoolFlowSeq\(_{sys,calc}\)(i)}
+
+\emph{FracOA = r\(_{air}\)} * \emph{DesOutAirVolFlow\(_{sys}\)}/ \emph{CoolFlowSeq\(_{sys}\)(i)}
+
+\emph{T\(_{mix}\)} = \emph{SysCoolOutTempSeq(i) *FracOA +}
+
+\emph{SysCoolRetTempSeq(i) *(}1-FracOA)
+
+\emph{SensCoolCapSeq(i)} = \emph{C\(_{p,air}\)} * \emph{CoolFlowSeq\(_{sys}\)(i)} *( \emph{T\(_{mix}\)}-\emph{T\(_{sup}\)})
+
+\begin{enumerate}
+\def\labelenumi{(\roman{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Do the same calculation for peak cooling.
+\end{enumerate}
+
+\emph{FracOA = r\(_{air}\)} * \emph{DesOutAirVolFlow\(_{sys}\)}/ \emph{DesCoolVolFlow}
+
+\emph{T\(_{mix}\)} = \emph{CoolOutTemp\(_{sys}\) *FracOA + CoolRetTemp\(_{sys}\) *(}1-FracOA)
+
+\emph{W\(_{mix}\)} = \emph{CoolOutHumRat\(_{sys}\) *FracOA + CoolRetHumRat\(_{sys}\) *}
+
+\emph{(}1-FracOA)
+
+\emph{SensCoolCap\(_{sys}\)} = \emph{C\(_{p,air}\)} * \emph{DesCoolVolFlow\(_{sys}\)} *( \emph{T\(_{mix}\)}-\emph{T\(_{sup}\)})
+
+\emph{T\(_{mix}\)} and \emph{W\(_{mix}\)} are saved in \emph{FinalSysSizing} \emph{.}
+
+\begin{enumerate}
+\def\labelenumi{(\roman{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Do the same calculation for the heating case.
+\end{enumerate}
+
+\emph{CoinHeatMassFlow} = \emph{SizRat\(_{heat}\)} * \emph{CoinHeatMassFlow\(_{calc}\)}
+
+\emph{NonCoinHeatMassFlow} = \emph{SizRat\(_{heat}\)} * \emph{NonCoinHeatMassFlow\(_{calc}\)}
+
+\emph{DesHeatVolFlow} = \emph{SizRat\(_{heat}\)} * \emph{DesHeatVolFlow\(_{calc}\)}
+
+\begin{enumerate}
+\def\labelenumi{(\alph{enumi})}
+\setcounter{enumi}{21}
+\tightlist
+\item
+  Loop over the zone timesteps (index = \emph{i}).
+\end{enumerate}
+
+\emph{HeatFlowSeq\(_{sys}\)(i)} = \emph{SizRat\(_{Heat}\)} * \emph{HeatFlowSeq\(_{sys,calc}\)(i)}
+
+\emph{FracOA = r\(_{air}\)} * \emph{DesOutAirVolFlow\(_{sys}\)}/ \emph{HeatFlowSeq\(_{sys}\)(i)}
+
+\emph{T\(_{mix}\)} = \emph{SysHeatOutTempSeq(i) * FracOA +}
+
+\begin{itemize}
+\tightlist
+\item
+  SysHeatRetTempSeq(i) ** \emph{(}1-FracOA)
+\end{itemize}
+
+\emph{HeatCapSeq(i)} = \emph{C\(_{p,air}\)} * \emph{HeatFlowSeq\(_{sys}\)(i)} *(\emph{T\(_{sup}\)}-\emph{T\(_{mix}\)})
+
+\begin{enumerate}
+\def\labelenumi{(\roman{enumi})}
+\setcounter{enumi}{5}
+\tightlist
+\item
+  Do the same calculation for peak heating.
+\end{enumerate}
+
+\emph{FracOA = r\(_{air}\)} * \emph{DesOutAirVolFlow\(_{sys}\)}/ \emph{DesHeatVolFlow}
+
+\emph{T\(_{mix}\)} = \emph{HeatOutTemp\(_{sys}\) *FracOA + HeatRetTemp\(_{sys}\) *} \emph{(}1-FracOA)
+
+\emph{W\(_{mix}\)} = \emph{HeatOutHumRat\(_{sys}\) *FracOA + HeatRetHumRat\(_{sys}\) *}
+
+\emph{(}1-FracOA)
+
+\emph{HeatCap\(_{sys}\)} = \emph{C\(_{p,air}\)} * \emph{DesHeatVolFlow\(_{sys}\)} *( \emph{T\(_{sup}\)}-\emph{T\(_{mix}\)})
+
+\emph{T\(_{mix}\)} and \emph{W\(_{mix}\)} are saved in \emph{FinalSysSizing} \emph{.}
+
+(vii)\emph{DesMainVolFlow\(_{sys}\)} = \textbf{MAX}(\emph{DesCoolVolFlow\(_{sys}\)},\emph{DesHeatVolFlow\(_{sys}\)})
+
+\textbf{This concludes the system design calculation.}
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+\textbf{Scalable System HVAC Sizing}
+
+The scalable system sizing applies to system supply air flow rates and sysyem capacity in coolin and heating modes.
+
+\textbf{Scalable System Air Flow Sizing}
+
+The scalable sizing methods for supply air flow rate allowed are either, \emph{FlowPerFloorArea}, \emph{FractionOfAutosizedCoolingAirflow}, or \emph{FlowPerCoolingCapacity}. The scalable system air flow sizing methods are defined as follows:
+
+\emph{FlowPerFloorArea} means the program calculates the cooling supply air volume flow rate from zone floor area served by the airloop and user specified \emph{Flow Per Floor Area} value.
+
+\emph{FractionOfAutosizedCoolingAirflow} means the program calculates the cooling supply air volume flow rate from user specified fraction and the autosized design cooling supply air volume flow rate value determined by the simulation.
+
+\emph{FractionOfAutosizedHeatingAirflow} means the program calculates the heating supply air volume flow rate from user specified fraction and the autosized design heating supply air volume flow rate value determined by the simulation.
+
+\emph{FlowPerCoolingCapacity} means the supply air volume is calculated from user specified flow per cooling capacity and design cooling capacity determined by the simulation.
+
+\emph{FlowPerHeatingCapacity} means the supply air volume is calculated from user specified flow per heating capacity and design heating capacity determined by the simulation.
+
+\textbf{Scalable System Capacity Sizing}
+
+The scalable sizing methods for system capacity available are: \emph{CapacityPerFloorArea}, \emph{FractionOfAutosizedCoolingCapacity} and \emph{FractionOfAutosizedHeatingCapacity}. The scalable system capacity sizing methods are defined as follows:
+
+\emph{CapacityPerFloorArea} means the program calculates the design capacity from user specified capacity per floor area and floor area of the zones served by the airloop.
+
+\emph{FractionOfAutosizedCoolingCapacity} means the program calculates the design cooling capacity from user specified fraction and the auto-sized design cooling capacity.
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+\emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity.
diff --git a/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/zone-design-loads-and-air-flow-rates.tex b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/zone-design-loads-and-air-flow-rates.tex
new file mode 100644
index 00000000000..bd49621e3dd
--- /dev/null
+++ b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/zone-design-loads-and-air-flow-rates.tex
@@ -0,0 +1,229 @@
+\section{Zone Design Loads and Air Flow Rates}\label{zone-design-loads-and-air-flow-rates}
+
+\subsection{Overview}\label{overview-030}
+
+There is no single best way to establish design HVAC flow rates and size HVAC equipment. Different building designs, climates, and HVAC systems will impose varying constraints on the designer. The method used to size an HVAC system in a hot, moist climate such as Miami will be different than the method used for a building in Albuquerque. The type of building is also relevant - a simple watts per square foot loads estimate could be adequate for a building containing a network server farm while a detailed, dynamic loads simulation would be necessary for a passive solar building. In the end the designer's experience and engineering judgement will play an important role in any sizing calculation.
+
+HVAC equipment sizing begins with the calculation of space heating and cooling loads. A space cooling (heating) load is defined as the rate at which heat must be removed (added) to a space to maintain a constant temperature. The current industry standard method for calculating space loads is the \emph{heat balance method} {[}ASHRAE Fundamentals (2001), page 29.1; Pedersen et al., (1997); Pedersen (2001). Since EnergyPlus is a heat balance based simulation program it is straightforward for the program to use this method for calculating zone loads.
+
+\subsection{Zone Design Data Arrays}\label{zone-design-data-arrays}
+
+The zone design data arrays are:
+
+\emph{ZoneSizingInput(i)} stores the input data from the Sizing:Zone objects.
+
+\emph{CalcZoneSizing(i,j)} stores the results of the zone design calculations for all zones and all design days. The index i is for the controlled zones, j for design days.
+
+\emph{CalcFinalZoneSizing(i)} stores the results of the zone design calculations for the peak heating and cooling cases for each zone. The index i is for the controlled zones.
+
+\emph{ZoneSizing(i,j)} corresponds to \emph{CalcZoneSizing} but includes the effect of the user specified sizing factor or user specified zone design flow rate.
+
+\emph{FinalZoneSizing(i)} corresponds to \emph{CalcFinalZoneSizing} but includes the effect of the user specified sizing factor or user specified zone design flow rate.
+
+The data stored in \emph{CalcZoneSizing}, \emph{CalcFinalZoneSizing}, \emph{ZoneSizing} and \emph{FinalZoneSizing} includes the following data items.
+
+% table 40
+\begin{longtable}[c]{p{1.85in}p{4.13in}}
+\caption{Zone Sizing Data \label{table:zone-sizing-data}} \tabularnewline
+\toprule 
+Name & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Zone Sizing Data} \tabularnewline
+\toprule 
+Name & Description \tabularnewline
+\midrule
+\endhead
+
+All the data from ZoneSizingInput &  \tabularnewline
+DesHeatMassFlow & the zone design heating air mass flow rate in [kg/s] \tabularnewline
+DesCoolMassFlow & the zone design cooling air mass flow rate in [kg/s] \tabularnewline
+DesHeatLoad & the zone design heating load in [W] \tabularnewline
+DesCoolLoad & the zone design cooling load in [W] \tabularnewline
+DesHeatDens & the zone design heating air density [kg/m  ] \tabularnewline
+DesCoolDens & the zone design cooling air density [kg/m  ] \tabularnewline
+DesHeatVolFlow & the zone design heating air volume flow rate [m  /s] \tabularnewline
+DesCoolVolFlow & the zone design cooling air volume flow rate [m  /s] \tabularnewline
+DesHeatCoilInTemp & zone heating coil design air inlet temperature [C] \tabularnewline
+DesCoolCoilInTemp & zone cooling coil design air inlet temperature [C] \tabularnewline
+DesHeatCoilInHumRat & the zone heating coil design air inlet humidity ratio [kg/kg] \tabularnewline
+DesCoolCoilInHumRat & the zone cooling coil design air inlet humidity ratio [kg/kg] \tabularnewline
+HeatMassFlow & current zone heating air mass flow rate at the HVAC time step [kg/s] \tabularnewline
+CoolMassFlow & current zone cooling air mass flow rate at the HVAC time step [kg/s] \tabularnewline
+HeatLoad & Current zone heating load [W] \tabularnewline
+CoolLoad & Current zone cooling load [W] \tabularnewline
+HeatZoneTemp & Current zone temperature during heating [C] \tabularnewline
+HeatZoneRetTemp & current zone return temperature during heating [C] \tabularnewline
+CoolZoneTemp & Current zone temperature during cooling [C] \tabularnewline
+CoolZoneRetTemp & current zone return temperature during cooling [C] \tabularnewline
+HeatZoneHumRat & Current zone humidity ratio during heating [C] \tabularnewline
+CoolZoneHumRat & Current zone humidity ratio during cooling [C] \tabularnewline
+ZoneTempAtHeatPeak & zone temperature at maximum heating [C] \tabularnewline
+ZoneRetTempAtHeatPeak & zone return temperature at maximum heating [C] \tabularnewline
+ZoneTempAtCoolPeak & zone temperature at maximum cooling [C] \tabularnewline
+ZoneRetTempAtCoolPeak & zone return temperature at maximum cooling [C] \tabularnewline
+ZoneHumRatAtHeatPeak & zone humidity ratio at maximum heating [kg/kg] \tabularnewline
+ZoneHumRatAtCoolPeak & zone humidity ratio at maximum cooling [kg/kg] \tabularnewline
+TimeStepNumAtHeatMax & zone time step number (in the day) at the heating peak \tabularnewline
+TimeStepNumAtCoolMax & zone time step number (in the day) at the cooling peak \tabularnewline
+HeatDDNum & design day index of design day causing heating peak \tabularnewline
+CoolDDNum & design day index of design day causing cooling peak \tabularnewline
+MinOA & design minimum outside air [m3/s] \tabularnewline
+HeatFlowSeq(i) & daily sequence of zone heating air mass flow rates (zone time step) [kg/s] \tabularnewline
+CoolFlowSeq(i) & daily sequence of zone cooling air mass flow rates (zone time step) [kg/s] \tabularnewline
+HeatLoadSeq(i) & daily sequence of zone heating loads (zone time step) [W] \tabularnewline
+CoolLoadSeq(i) & daily sequence of zone cooling loads (zone time step) [W] \tabularnewline
+HeatZoneTempSeq(i) & daily sequence of zone temperatures (heating, zone time step) [C] \tabularnewline
+HeatZoneRetTempSeq(i) & daily sequence of zone return temperatures (heating, zone time step) [C] \tabularnewline
+CooltZoneTempSeq(i) & daily sequence of zone temperatures (cooling, zone time step) [C] \tabularnewline
+CoolZoneRetTempSeq(i) & daily sequence of zone return temperatures (cooling, zone time step) [C] \tabularnewline
+HeatZoneHumRatSeq(i) & daily sequence of zone humidity ratios (heating, zone time step) [kg/kg] \tabularnewline
+CoolZoneHumRatSeq(i) & daily sequence of zone humidity ratios (cooling, zone time step) [kg/kg] \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Zone Design Load Calculation}\label{zone-design-load-calculation}
+
+As described in the preceding section, the Sizing Manager initiates the zone design calculation by looping over all of the design days and calling the Heat Balance Manager for each zone time-step in each design day. The Heat Balance manager then causes the HVAC Manager to be called in a manner identical to a normal simulation. The \emph{ZoneSizingCalc} set to \emph{true} signals the HVAC Manager to ignore the actual HVAC system and instead calculate the design zone loads and air flow rates using an ideal zonal system.
+
+In module \emph{HVACManager}, subroutine \emph{ManageHVAC} calls \emph{SimHVAC}. \emph{SimHVAC} checks \emph{ZoneSizingCalc}. If it is \emph{true}, \emph{SimHVAC} calls \emph{ManageZoneEquipment} and returns, rather than simulating the actual system. In turn \emph{ManageZoneEquipment} checks if \emph{ZoneSizingCalc} is \emph{true}; if it is it calls \emph{SizeZoneEquipment} rather than \emph{SimZoneEquipment}.
+
+\emph{SizeZoneEquipment} assumes that each controlled zone is served by an ideal air conditioning unit. This unit supplies heating or cooling air at a fixed, user input temperature and humidity (specified in the Sizing:Zone objects). The units have infinite capacity: the flow rate can be any amount.
+
+Before the ideal zone load is calculated, the function checks whether the user wants to account for the heat gain or loss caused by the ventilation air from a Dedicated Outdoor Air System (DOAS). If the user has selected \emph{Account For Dedicated Outdoor Air = Yes} the function performs an ideal DOAS calculation. The DOAS supply temperature is set according to the user's choice of 1 of 3 possible control strategies: \emph{NeutralSupplyAir}, \emph{NeutralDehumidifiedSupplyAir}, or \emph{ColdSupplyAir}. The different strategies are:
+
+\begin{itemize}
+\item
+  \emph{DOAS Control Strategy = NeutralSupplyAir}. The purpose of this strategy is to cool or heat the outdoor air (OA) to keep it between the \emph{T\(_{l}\)} and \emph{T\(_{h}\)} setpoints.
+\item
+  \emph{DOAS Control Strategy = Neutral Dehumidified Supply Air}. The purpose of this strategy is to cool and dehumidify the outdoor air, then reheat it to a ``neutral'' temperature so that no sensible load is imposed on the space or AHU unit. The DOAS will with this strategy handle some or all of the latent load. If the outdoor air temperature is greater than \emph{T\(_{l}\)} the outdoor air is cooled to \emph{T\(_{l}\)} and reheated to \emph{T\(_{h}\)}. If the outdoor air temperaure is below \emph{T\(_{l}\)} it is heated to \emph{T\(_{h}\)}.
+\item
+  \emph{DOAS Control Strategy = ColdSupplyAir}. The purpose of this strategy is to provide cool, dehumidified ventilation air to the zone. In this case the DOAS can handle part of the sensible zone cooling load as well as meet part or all of the latent load. If the outdoor air temperature is below \emph{T\(_{l}\)} it is heated to \emph{T\(_{h}\)}. If it is above \emph{T\(_{l}\)}, it is heated to \emph{T\(_{l}\)}.
+\end{itemize}
+
+With the DOAS supply temperature set and the air mass flow rate set to the minimum design ventilation flow rate the heat addition rate is just
+
+\begin{equation}
+{\dot Q_{doa}} = {c_{p,air}}{\dot m_{vent,min}}({T_{sup}} - {T_z})
+\end{equation}
+
+\emph{UpdateSSystemOutputRequired} is then invoked to adjust the load to be met by the ideal zone system.
+
+The ideal loads calculation steps are as follows.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Loop over all the controlled zones.
+\item
+  If the system is active (zone temperature not in the deadband and zone load greater than 1 watt) the sign of the zone load is used to determine whether heating or cooling is required and \emph{T\(_{in}\)} and W\emph{\(_{in}\)} are set to the appropriate values from the Sizing:Zone input. When the SupplyTemperature method is specified in the Sizing:Zone object, \emph{T\(_{in}\)} is fixed at the cooling or heating supply temperature. When the TemperatureDifference method is selected, \emph{T\(_{in}\)} is calculated at each time step using the current zone air temperature. The system output \emph{Q\(_{sys}\)} is simply set equal to the zone demand - it is assumed that the ideal system can always meet the zone load. The air flow rate corresponding to the load is just
+\end{enumerate}
+
+\begin{equation}
+{\dot m_{sys}} = {Q_{sys}}/({C_{p,air}} \cdot ({T_{in}} - {T_z}))
+\end{equation}
+
+If the system is not active, the mass flow rate is set to zero and the system output is left at zero.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  The results for each zone are stored in the zone sizing data arrays.
+\end{enumerate}
+
+\subsection{Updating and Adjusting the Zone Results}\label{updating-and-adjusting-the-zone-results}
+
+The results from \emph{SizeZoneEquipment} are at the system time-step and are for all design days. These results then need to be summed or averaged over the zone time-step, peak values calculated for each design day, a heating \& a cooling load sequence chosen for each zone from all the design day results, possible further smoothing of results done, zone coil loads calculated, and user sizing multipliers or user specified design flows taken into account. These tasks are accomplished by the subroutine \emph{UpdateZoneSizing}. It is called at the start of each design day (\emph{CallIndicator = BeginDay}), at the zone time-step (\emph{CallIndicator = DuringDay}), at the end of the design day (\emph{CallIndicator = EndDay}) and at the end of the zone design calculation (\emph{CallIndicator = EndZoneSizingCalc}).
+
+\subsubsection{BeginDay}\label{beginday-000}
+
+The environment (in this case, a design day) name and number are stored in the zone sizing data structures
+
+\subsubsection{DuringDay}\label{duringday-000}
+
+The calculated and stored sequences are summed or averaged over the zone time-step.
+
+\subsubsection{EndDay}\label{endday-000}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\tightlist
+\item
+  Smooth the design sequences by applying a moving, fixed-width averaging window to the sequences. The width of the window is user specified in the \emph{Sizing:Parameters} input object. The sequences that are smoothed are: 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\alph{enumi})}
+\item
+  \emph{CoolFlowSeq}
+\item
+  \emph{CoolLoadSeq}
+\item
+  \emph{HeatFlowSeq}
+\item
+  \emph{HeatLoadSeq}
+\item
+  \emph{CoolZoneRetTempSeq}
+\item
+  \emph{HeatZoneRetTempSeq} 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\setcounter{enumi}{1}
+\item
+  The peak heating and cooling loads and mass \& volume flow rates are extracted from each set of design sequences.
+\item
+  Using the time of the peak and the design outside air fraction the design zone heating and cooling coil inlet temperatures and humidity ratios are calculated.
+\item
+  For each zone, looking at the results for all of the design days, the design days that cause the peak heating and peak cooling for that zone are chosen and the corresponding design sequences and peak loads and flow rates are saved in the CalcFinalZoneSizing array. This finishes the calculated - unmodified by the user - portion of the zone design calculation.
+\end{enumerate}
+
+\subsubsection{EndZoneSizingCalc}\label{endzonesizingcalc}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\item
+  Write out onto a comma-separated file the calculated design sequences for each zone: \emph{HeatLoadSeq}, \emph{CoolLoadSeq}, \emph{HeatFlowSeq}, \emph{CoolFlowSeq} and the corresponding peaks and volumetric flow peaks.
+\item
+  The data in \emph{CalcZoneSizing} and \emph{CalcFinalZoneSizing} is moved to \emph{ZoneSizing} and \emph{FinalZoneSizing}. The user modifications to the calculated sizing will be applied to and stored in \emph{ZoneSizing} and \emph{FinalZoneSizing}.
+\item
+  The user can modify the calculated zone design results by specifying heating and cooling sizing factors at the global or zone level or by specifying and actual design heating or cooling zone design volumetric flow rate. All of this input is treated as a sizing factor. If the user inputs a cooling design volumetric flow rate for a zone it is divided by the calculated cooling design volumetric flow rate for the zone to give a zone cooling sizing factor. Note that the user can input a zone sizing factor or a zone design flow rate - not both - so there is never a conflict.
+\item
+  Once the zone heating and cooling sizing factors are established, the design flow and load sequences as well as peak loads and flows are multiplied by the appropriate sizing factor and stored in \emph{ZoneSizing} and \emph{FinalZoneSizing}. This is the data that will be used for sizing zone HVAC equipment and in the system sizing calculation.
+\item
+  The outside air fractions are recalculated using the new user-modified design flow rates and new design zone coil inlet conditions calculated and stored. At this point the condition that the design flow rates are never allowed to be less than the minimum outside air flow rate is imposed.
+\end{enumerate}
+
+If \emph{outside air method} is \emph{flow/zone}, the input \emph{outside air flow per zone} value will be used, even if it is zero or blank. If \emph{outside air method} is \emph{sum}, the sum of the \emph{outside air flow per person} * \emph{DesignNumberOfPeople} + \emph{outside air flow per area} * \emph{ZoneArea} will be used. If \emph{outside air method} is \emph{maximum}, the maximum of the \emph{outside air flow per person} * \emph{DesignNumberOfPeople} and \emph{outside air flow per area} * \emph{ZoneArea} will be used. If \emph{outside air method} is \emph{flow/person}, \emph{outside air flow per person} will be used to calculate the design minimum outside airflow rate.
+
+If \emph{cooling design air flow method} is \emph{flow/zone}, then \emph{cooling design air flow rate} will be used for the design max cooling air flow rate. If \emph{cooling design air flow method} is \emph{design day}, then the design day calculation will set the design max cooling air flow rate. If \emph{cooling design air flow method} is \emph{design day with limit}, then the maximum from \emph{cooling min flow per area} and \emph{cooling min flow} will set a lower limit on the design max cooling air flow rate. In all cases, the maximum from \emph{cooling min flow per area}, \emph{cooling min flow}, and \emph{cooling min flow fraction} will set a minimum zone cooling air flow rate. In all cases the maximum design cooling air flow rate must be \textgreater{} = to the ventilation requirement.
+
+If \emph{heating design air flow method} is \emph{flow/zone}, then \emph{heating design air flow rate} will be used for the design max heating air flow rate. If \emph{heating design air flow method} is \emph{design day}, then the design day calculation will set the design max heating air flow rate. If \emph{heating design air flow method} is \emph{design day with limit}, then the maximum from \emph{heating max flow per area}, \emph{heating max flow} and \emph{heating max flow fraction} will set an upper limit on the design max heating air flow rate. The design max heating air flow rate must always be \textgreater{} = the ventilation requirement. In each case, the outside airflow will be modified based on zone ventilation effectiveness specified in the zone sizing object.
+
+\textbf{This concludes the calculation of the zone design flow rates and loads.}
+
+\subsection{Zone HVAC Scalable Sizing}\label{zone-hvac-scalable-sizing}
+
+For zone HVAC equipments scalable sizing applies to supply air flow rate and capacity for both cooling and heating. The scalable sizing method allowed for supply air flow rates include: \emph{FractionOfAutosizedCoolingAirflow}, \emph{FractionOfAutosizedHeatingAirflow}, \emph{FlowPerFloorArea, FlowPerCoolingCapacity}, and \emph{FlowPerHeatingCapacity}. The supply air flow rate scalable sizing methods are defined as follows:
+
+\textbf{\emph{FlowPerFloorArea}}: the simulation engine determine the supply air flow rates from the user specified \emph{supply air flow rates per unit floor area} and the zone floor area of the zone served by the zone HVAC equipment.
+
+\textbf{\emph{FractionOfAutosizedCoolingAirflow}}: the simulation engine determines the supply air flow rates from the user specified \emph{flow fraction} and \emph{autosized cooling design supply air flow rate}.
+
+\textbf{\emph{FractionOfAutosizedHeatingAirflow}}: the simulation engine determines the supply air flow rates from the user specified \emph{flow fraction} and \emph{autosized heating design supply air flow rate}.
+
+\textbf{\emph{FlowPerCoolingCapacity}}: he simulation engine determines the supply air flow rates from the user specified \emph{supply air flow per cooling capacity value} and \emph{autosized cooling design capacity}.
+
+\textbf{\emph{FlowPerHeatingCapacity}}: the simulation engine determines the supply air flow rates from the user specified \emph{supply air flow per heating capacity value} and \emph{autosized heating design capacity}.
+
+The scalable capacity sizing may be indirectly impacted by the scalable supply air flow rates sizing values. Moreover, the autosized cold water, hot water and steam flow rates in the parent zone HVAC objects and capacity in child components are determined using the scalable sizing method. Scalable capacity sizing methods allowed for cooling and heating include: \emph{CapacityPerFloorArea, FractionOfAutosizedCoolingCapacity}, \emph{FractionOfAutosizedHeatingCapacity}. The scalable sizing capacity methods are defined as follows:
+
+\textbf{CapacityPerFloorArea}: the simulation engine determines the cooling or heating capacity from user specified capacity per floor area value and the floor area of the zone served by the zone HVAC equipment.
+
+\textbf{FractionOfAutosizedCoolingCapacity}: the simulation engine sizes the cooling capacity from the user specified \emph{capacity fraction} and \emph{autosized cooling design capacity} value.
+
+\textbf{FractionOfAutosizedHeatingCapacity}: the simulation engine sizes the heating capacity from the user specified \emph{capacity fraction} and \emph{autosized heating design capacity} value.
diff --git a/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/zone-outdoor-air-design-data.tex b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/zone-outdoor-air-design-data.tex
new file mode 100644
index 00000000000..d0e702bc541
--- /dev/null
+++ b/doc/engineering-reference/src/loop-equipment-sizing-and-other-design-data/zone-outdoor-air-design-data.tex
@@ -0,0 +1,114 @@
+\section{Zone Outdoor Air Design Data}\label{zone-outdoor-air-design-data}
+
+Outdoor air design data may be required for many aspects of a building computer model. Sizing of HVAC equipment, infiltration and ventilation, and specific outdoor air requirements for different zone types are a few examples where required outdoor air quantities may vary. Since there would be a significant chance for data input errors if each individual aspect of the simulation model allowed for independent input of outdoor air design data, this general object is used to define outdoor air design data and this data set may be used throughout the building simulation model.
+
+The design data is provided as a group of inputs that are recognized by designers as standard practice. This information may be used individually or used as a group to calculate summations or maximums of the entered data. These design data include values for:
+
+\begin{itemize}
+\tightlist
+\item
+  Outdoor air per person
+\item
+  Outdoor air per zone floor area
+\item
+  Outdoor air per zone
+\item
+  Outdoor air changes per hour
+\end{itemize}
+
+This design data is entered in an outdoor air design data object and may be referenced by other objects during the simulation. A single specification for outdoor air design data may be used by all other appropriate objects within EnergyPlus, or multiple outdoor air design data objects may be specified and these design data objects may be used as necessary by other objects when outdoor air design quantaties vary for any reason.
+
+\subsection{Design Outdoor Air Calculation}\label{design-outdoor-air-calculation}
+
+The outdoor air design data is entered as a group and referenced through name association to this group of design data (Ref. DesignSpecification:OutdoorAir). The reference name in the following example is ``ZoneOAData''.
+
+A DesignSpecification:OutdoorAir example:
+
+\begin{lstlisting}
+
+DesignSpecification:OutdoorAir,
+  ZoneOAData,            !- Name
+  Maximum,               !- Outdoor Air Method
+  0.00944,               !- Outdoor Air Flow per Person {m3/s}
+  0.00305;               !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
+  ,                      !- Outdoor Air Flow per Zone
+  ,                      !- Outdoor Air Flow Air Changes per Hour
+  Min OARequirements Sched; !- Outdoor Air Flow Rate Fraction Schedule Name
+\end{lstlisting}
+
+Given this set of data, the quantity of outdoor air is calculated based on the Outdoor Air Method specified in each outdoor air design data object. In this example, the maximum of the per person and per zone floor area is used to establish the outdoor air quantity.
+
+As previously mentioned, this group of outdoor air design data is reference by other objects used in the simulation. The reference is by the \emph{name} of the outdoor air design data object. Any reference to this name by other objects simply means that the object referencing this data set will use the values specified in this common object. Note that a zone name is not included in the list of data and the calculation of occupancy, zone floor area, or zone volume is implied through this named reference and \emph{the connection to a zone via the referencing object}. For example, if a terminal unit references an outdoor air design data object, the zone served by that terminal unit is used to determine the occupancy, zone floor area, and zone volume in the following calculations.
+
+\begin{equation}
+O{A_{people}} = Oc{c_{zone}}\left( {OAFlowperPerson} \right)
+\end{equation}
+
+\begin{equation}
+O{A_{floor\,area}} = {A_{zone}}\left( {OAFlowperFloorArea} \right)
+\end{equation}
+
+\begin{equation}
+O{A_{zone}} = \left( {OAFlowperZone} \right)
+\end{equation}
+
+\begin{equation}
+O{A_{ACH}} = {V_{zone}}\left( {{\raise0.7ex\hbox{{OAFlowAirChangesperHour}} \!\mathord{\left/ {\vphantom {{OAFlowAirChangesperHour} {3600}}}\right.}\!\lower0.7ex\hbox{{3600}}}} \right)
+\end{equation}
+
+where:
+
+\(O{A_{people}}\) = outdoor air volume flow rate based on occupancy, {[}m\(^{3}\)/s{]}
+
+\(Oc{c_{zone}}\) = number of occupants in zone, {[}people{]}
+
+\(OAFlowperPerson\) = outdoor air volume flow rate per person, {[}m\(^{3}\)/s-person{]}
+
+\(O{A_{floor\;area}}\) = outdoor air volume flow rate based on zone floor area, {[}m\(^{3}\)/s{]}
+
+\({A_{zone}}\) = zone floor area, {[}m\(^{2}\){]}
+
+\(OAFlowperFloorArea\) = outdoor air volume flow rate per zone floor area, {[}m\(^{3}\)/s-m\(^{2}\){]}
+
+\(O{A_{zone}}\) = zone outdoor air volume flow rate, {[}m\(^{3}\)/s{]}
+
+\(OAFlowperZone\) = outdoor air volume flow rate per zone, {[}m\(^{3}\)/s{]}
+
+\(O{A_{ACH}}\) = outdoor air volume flow rate based on air changes per hour, {[}m\(^{3}\)/s{]}
+
+\({V_{zone}}\) = zone volume, {[}m\(^{3}\){]}
+
+\(OAFlowAirChangesperHour\) = outdoor air volume flow in air changes per hour, {[}m\(^{3}\)/s-m\(^{3}\){]}
+
+Given the calculations for each specific type of design data, the method used to calculate the outdoor air design data is then based on a user selected method for this specific outdoor air design data object. The outdoor air methods used to calculate the outdoor air quantity and the associated value for outdoor air volume flow rate are shown here.
+
+Flow/Person = \textgreater{} \(O{A_{people}}\)
+
+Flow/Area = \textgreater{} \(O{A_{floor\,area}}\)
+
+Flow/Zone = \textgreater{} \(O{A_{zone}}\)
+
+AirChanges/Hour = \textgreater{} \(O{A_{ACH}}\)
+
+Sum = \textgreater{} \(O{A_{people}}\, + \,O{A_{floor\,area}}\, + \,O{A_{zone}}\, + \,O{A_{ACH}}\)
+
+Maximum = \textgreater{} \(MAX\left( {O{A_{people}}\,,\,O{A_{floor\,area}}\,,\,O{A_{zone}}\,,\,O{A_{ACH}}} \right)\)
+
+If an Outdoor Air Flow Rate Fraction Schedule Name is specified, the flow rate determined above will be multiplied by the current schedule value.
+
+Examples of objects that reference the outdoor air design data object are:
+
+\begin{itemize}
+\item
+  AirTerminal:SingleDuct:VAV:NoReheat
+\item
+  AirTerminal:SingleDuct:VAV:Reheat
+\end{itemize}
+
+\subsection{References}\label{references-058}
+
+ASHRAE Fundamentals 2001. 2001 ASHRAE Fundamentals Handbook. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Pedersen, C.O., D.E. Fisher, and R.J. Liesen. 1997. A heat balance based cooling load calculation procedure. ASHRAE Transactions, Vol. 103(2), pp.~459-468.
+
+Pedersen, C.O. 2001. Toolkit for Building Load Calculations. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
diff --git a/doc/engineering-reference/src/on-site-generation.tex b/doc/engineering-reference/src/on-site-generation.tex
new file mode 100644
index 00000000000..7a19adf89bb
--- /dev/null
+++ b/doc/engineering-reference/src/on-site-generation.tex
@@ -0,0 +1,13 @@
+\chapter{On-Site Generation, Power Conversion, and Storage}\label{on-site-generation}
+
+This section discusses on-site generation, electric storage, and power conversion models related to serving the facility with electric power.  EnergyPlus is usually predicting the electric energy consumed in a building and its HVAC equipment over time.  If this electric power all comes directly from the grid and the building has no power conversion devices (such as a transformer, inverter, battery, generators, solar panels etc.) then only some basic accounting is needed and none of the additional models described here are really needed.  The device models in this section are for when the electric power service system supplying the facility has some added equipment that is considered part of the building being modeled.   The purpose of electric power service modeling in EnergyPlus is to account for the energy performance of such equipment at each timestep of the building and HVAC simulation.  The building and HVAC simulation provides a current prediction of the electric load required by the facility and the electric power service simulation uses that information.   This is simplified power system model with the only goal being to account for power losses (in Watts) and energy consumed (in Joules) by key devices in the balance of system including:
+
+\begin{description}
+  \item[Transformer]: a building may have transformers and they are not 100\% efficient. A facility may own its own transformer and have high voltage utility grid connection. An on-site generation system might have an isolation transformer.  The EnergyPlus model meters electric losses as a function of the power going through each transformer.
+  \item[Fuel-fired generators]: a building may have generators that consume one type of energy resource (natural gas, diesel, etc.) and generate electricity.  These generators need supervisory control to determine when and how hard to run the engine.  The generators may be used for cogeneration and include connections to a hot water plant in the HVAC models.  The generator models determine the efficiency as fuels are converted to electric power and heat. 
+  \item[Renewable generators]: a building may have wind turbines or solar photovoltaic panels.  The generator models determine the efficiency as wind and sun are converted to electricity.
+  \item[Inverters]: the direct current generated by solar photovoltaic or discharged from storage may need to be converted from DC to AC by an inverter.  The EnergyPlus models meter electric losses as a function of the power going through each inverter.
+  \item[Storage]: a building may have on-site electric storage and it is not 100\% efficient.  Storage can be used to adjust utility demand profile or store on-site renewables.
+\end{description}
+
+There is no explicit modeling of voltage and current between devices, just basic power and energy exchanges.  There is no modeling of power loss in conductors and distribution panels throughout the building.  There is no modeling of short term power draws as for a motor start -- power levels are modeled as single-valued averages for the entire system timestep ( 1 minute or longer).
\ No newline at end of file
diff --git a/doc/engineering-reference/src/on-site-generation/electric-load-center-distribution-manager.tex b/doc/engineering-reference/src/on-site-generation/electric-load-center-distribution-manager.tex
new file mode 100644
index 00000000000..de050272509
--- /dev/null
+++ b/doc/engineering-reference/src/on-site-generation/electric-load-center-distribution-manager.tex
@@ -0,0 +1,560 @@
+\section{Electric Load Center Distribution Manager}\label{electric-load-center-distribution-manager}
+
+\subsection{Overview}\label{overview-016}
+
+The electric load center distribution manager (object name: ElectricLoadCenter:Distribution) is used organize power conversion devices and provides supervisory control over generators and storage.   Electric load centers can be thought of as subpanels connected to the facility's main electric panel.  Except for two applications for transformers that are located between the main panel and the utility grid connection, all other devices are associated with a specific load center.  The load center connects the “load� to the generators and “supply� power to the main panel serving the rest of the building.  A load center can have any number of generators but only one storage, (DC to AC) inverter, (AC to DC) converter or (isolation) transformer.  There are two separate operation schemes, one for generators and one for storage.  The generator operation scheme controls the on-site generators connected to a particular load center.  The storage operation scheme controls charging and discharging of electrical storage.  The generator operation is managed before the storage operation.  The internal meters used by EnergyPlus for reporting do all of the tracking. For more details on the individual inputs required see the Input Output Reference document.
+
+The electric load center manager sums all of the building and system electric loads and provides operating schemes for the generators. The electric load center objects are operated in the order they are defined in the input data file (IDF), and generators are dispatched sequentially in the order they are specified within the list referenced by each load center object. The electricity produced from photovoltaic arrays and wind turbines is handled somewhat separately and is always run rather than being dispatched by supervisory control.  What is not provided by the on-site generation equipment, and electric storage units, is met by (purchasing) off-site electricity. It is possible to prescribe a set of ElectricLoadCenter:Distribution objects with inconsistent or conflicting operating schemes, so users need to be careful.
+
+\subsection{Generator Operation Schemes}
+
+The available generator operating schemes are “Baseload�, “DemandLimit�, “TrackElectrical,� “TrackSchedule,� “TrackMeter,� “FollowThermal� and “FollowThermalLimitElectrical.�  These operating schemes affect how loads are dispatched to the generators, in effect telling the generators whether or not to run and requesting power levels.
+
+The Baseload scheme operates the generators at their rated (requested) electric power output when the generator is scheduled ON (ref. ElectricLoadCenter:Generators in the Input Output Reference). The Baseload scheme requests all generators scheduled ON (available) to operate, even if the amount of electric power generated exceeds the total facility electric power demand.
+
+The DemandLimit scheme limits the amount of purchased electricity from the utility to the amount specified in the input. The Demand Limit scheme tries to have the generators meet all of the demand above the purchased electric limit defined by the user.
+
+The TrackElectrical scheme tries to have the generators meet all of the electrical demand for the building.
+
+The TrackMeter scheme tries to have the generators meet all the electrical demand from a meter chosen by the user rather than the usual meter for the entire facility. The meter can be a custom meter so that generators are tied to only certain loads in the building.
+
+The TrackSchedule scheme tries to have the generators meet all of the electrical demand determined by a user-defined schedule.
+
+The FollowThermal and FollowThermalLimitElectrical schemes run the generators to meet thermal demand. The thermal demand is determined from the plant modeling and depends on the flow requested by other components on the demand side of the plant loop, the loop temperatures, and the loop temperature setpoint. The electric load center distribution manager converts the thermal load to an electrical load using a nominal ratio of the thermal to electrical power production for each generator. For these schemes, the generator needs to be connected to the supply side of a plant loop and serve components that use hot water on the demand side of the plant loop. The thermal load request is obtained from the plant data structure (structure location in code is PlantLoop\%LoopSide\%Branch\%Comp\%MyLoad).The distribution manager converts the thermal load, $q_{thermal}$, to an electrical load using:
+
+\begin{equation}
+{q_{Elect}} = \frac{{{q_{thermal}}}}{{ThermElectRatio}}
+\end{equation}
+
+where,
+
+$ThermElectRatio$\ is a nominal, constant, user-defined value for the ratio of thermal production to electrical production for a cogenerator. This ratio is used for supervisory control and dispatch of the electric power request to the generator; however, the cogenerator model may determine that actual performance varies from this nominal value at different times in the simulation when operating conditions differ from those used for the nominal ratio.
+
+For all generator operating schemes except Baseload, a total electric load reduction target (or thermal load converted to electrical equivalent) is established for the load center based on the specific operating scheme. The load center then requests that its generators operate, one-by-one in the order specified in the generator list, until the target is met or exceeded. Generators that are not scheduled as ‘available’ for the simulation time step are not called to operate. The requested power demand to be met by each generator is the **smaller of** the nominal ‘rated’ electric power output (as specified in the ElectricLoadCenter:Generators object) or the remaining total electric load reduction target for the load center. After each electric generator is requested to operate, the actual electric power delivered by the generator, which may be greater than or less than the requested amount due to inputs specified in the generator performance model (e.g., Generator:CombustionTurbine, Generator:MicroTurbine, etc.), is used to update the remaining total electric power target for the other generators associated with this load center.
+
+Most of the operating schemes will sequentially load the available electric load centers and generators. EnergyPlus can accept multiple “ElectricLoadCenter:Distribution� objects with different operating schemes. Because of this, there are two levels of reporting, one for the whole building and a second for each load center. The whole-building results are managed with the internal meters for the entire model. The individual load-center results are summed for those generators connected to a particular load center. The total electricity purchased is reported both in power and energy units. This value is positive when the amount of energy is purchased from the utility. This value can be negative when the total electricity produced is greater than the facility electrical needs. The excess will either be available for storage or to sell back to the electric utility company.
+
+The order of input objects (ElectricLoadCenter:Distribution) in the input file is significant and used to structure how generators are dispatched with the first load centers and generators managed before the later ones. Therefore, load centers listed earlier in the file effectively have a higher priority.
+
+\subsection{Load Center Buss Types}
+
+Electric load centers can have one of five different configurations. Load centers can get fairly complicated and include power conditioning and storage. Separate inverter models are used to condition DC power from photovoltaics into AC power for the building and utility. The other generators may have inverters inside the devices but these are already embedded in the generator models. The load center can also supervise electrical storage controls and depend on the buss configuration. The transformer is optional for all buss types but if included in the load center it can be used to model an isolation or voltage matching transformer acting on the load center.
+
+The most basic configuration is selected with the keyword “AlternatingCurrent� for the Electrical Buss Type, shown in the following diagram.
+
+\begin{figure}[hbtp] % fig 333
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/ACBussDiagram.png}
+\caption{Basic Alternating Current Schematic \protect \label{fig:basic-alternating-current-schematic}}
+\end{figure}
+
+The *AlternatingCurrent* load centers have AC generators with no storage and behave in the following way. All electric demand not met by the sum of the electrical power produced by the available generators will be met by purchased electricity.  If a generator is needed in the simulation for a small load and the load is less than the generator’s minimum part load ratio, the generator will operate at the minimum part load ratio and the excess will either reduce demand or the excess energy will be exported back to the electric utility company. 
+
+A configuration with AC generators with on-site electrical storage is selected with the keyword “AlternatingCurrentWithStorage� and is shown in the following diagram. 
+
+\begin{figure}[hbtp] % fig 334
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/ACStorageBussDiagram.png}
+\caption{AC Generators with On-site Electrical Storage Schematic \protect \label{fig:ac-generators-with-on-site-electrical-storage}}
+\end{figure}
+
+The *AlternatingCurrentWithStorage* load centers attempt to augment the generator electricity production so that the power requests are met. Storage control logic is discussed below under Storage Operation Scheme.
+
+The basic configuration for photovoltaic generators is selected using the “DirectCurrentWithInverter� keyword and is shown in the following diagram.
+
+\begin{figure}[hbtp] % fig 335
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/DCInverterBussDiagram.png}
+\caption{Direct Current With Inverter Photovoltaic Generators Schematic \protect \label{fig:direct-current-with-inverter-photovoltaic}}
+\end{figure}
+
+The *DirectCurrentWithInverter* load centers collect DC power from various generators, usually PV arrays, run the DC power through an inverter and produce AC power. The PV arrays produce DC power based on the availability of sunshine and do not respond to load requests made by the electric load center. 
+
+If the PV-based load center is equipped with DC electrical storage that is connected before the inverter, then the buss type should be “DirectCurrentWithInverterDCStorage� and is shown in the following diagram.
+
+\begin{figure}[hbtp] % fig 336
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/DCInverterWithDCStorageBussDiagram.png}
+\caption{PV based Load Center with DC Electrical Storage Schematic \protect \label{fig:pv-based-load-center-with-dc-electrical}}
+\end{figure}
+
+The *DirectCurrentWithInverterDCStorage* load centers charge or draw DC power to meet the requested electrical load depending on the storage operation scheme.
+
+If the PV-based load center is equipped with AC electrical storage that is connected after the inverter, then the buss type should be “DirectCurrentWithInverterACStorage� and is shown in the following diagram.
+
+\begin{figure}[hbtp] % fig 337
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/DCInverterWithACStorageBussDiagram.png}
+\caption{PV Based Load Center with AC Electrical Storage Schematic \protect \label{fig:pv-based-load-center-with-ac-electrical}}
+\end{figure}
+
+The *DirectCurrentWithInverterACStorage* load centers charge or draw AC power to meet the requested electrical load.  They can also draw power from the main panel into the load center to charge storage from grid-supplied electric power.
+
+\subsection{Electric Load Center Generators}\label{electric-load-center-generators}
+
+The electric load center generators (object name: ElectricLoadCenter:Generators) provide a set of scheduled electric generators for supervisory control over electric power generation. Here is where the user lists what generators and PVs are available at any given time. For more details on the individual inputs required see the EnergyPlus Input Output Reference.
+
+\subsection{Inverters}\label{inverters}
+
+EnergyPlus includes three models for converting Direct Current (DC) electrical power into Alternating Current (AC) electrical power. The DC power into the inverter, \({P_{DC - in}}\) , is converted to AC power out, \({P_{AC - out}}\) , of the inverter using:
+
+\begin{equation}
+{P_{AC - out}} = {P_{DC - in}} \cdot {\varepsilon_{inverter}}
+\end{equation}
+
+The inverter efficiency is determined using one of the three models. For the``Simple'' inveter model, efficiency is constant and input by the user. For the ``Look Up Table'' model, the efficiency is calculated using linear interpolation. For the ``Function of Power'' model, the efficiency is calculating using a single-variable curve object. For both the Look Up Table and Function of Power models, the power production is normalized by \({P_{DC - in}}\) .
+
+The conversion power losses are calculated from the difference between $ {P_{DC,in}} $ and $ {P_{AC,out}} $ and are metered as negative values on PowerConversion:ElectricityProduced.  The thermal losses include the conversion power losses plus any ancillary power consumed during standby.  The ancillary electric power consumption occurs when the inverter is scheduled to be available but it is not conditioning any power flows at the time. 
+
+\subsection{Converter}
+
+EnergyPlus includes a model for converting Alternating Current (AC) electric power into Direct Current (DC) electric power.  This device is used to charge DC electric storage devices with AC drawn from the main panel.  Although the physical device may be a two-way inverter, the modeling is separated so that the converter appears on its own in the modeling. The AC power into the converter, $ {P_{AC,in}} $, is converted to DC power out, $ {P_{DC,out}} $, of the converter using: 
+
+\begin{equation}
+  {P_{DC,out}} = {P_{AC,in}} \cdot {\varepsilon_{converter}}
+\end{equation}
+
+The converter efficiency is determined using one of two method.  For the "SimpleFixed" method the efficiency is constant and input by the user.  For the "FunctionOfPower" method the user defined performance curve or lookup table is evaluated using the normalized power into the converter.
+
+The conversion power losses are calculated from the difference between $ {P_{AC,in}} $ and $ {P_{DC,out}} $ and are metered as negative values on PowerConversion:ElectricityProduced.  The thermal losses include the conversion power losses plus any ancillary power consumed during standby.  The ancillary electric power consumption occurs when the converter is scheduled to be available but it is not conditioning any power flows at the time. 
+
+\subsection{Storage Operation Schemes}
+
+The available storage operation schemes are "TrackFacilityElectricDemandStoreExcessOnSite", "TrackMeterDemandStoreExcessOnSite", "TrackChargeDischargeSchedules", and "FacilityDemandLeveling".  
+
+The following diagram shows the control volume and electrical power flows that are used to model all of the storage operation schemes.  Conservation of energy is used to formulate the calculations based on this control volume and the five terms shown in the diagram.  This control volume is inside a given load center. 
+
+\begin{figure}[hbtp] % fig 337
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/StorageOperationControlVolume.png}
+\caption{Storage operation control volume \protect \label{fig:storage-operation-control-volume}}
+\end{figure}
+
+  $ {P_{gen}}  $  This is the sum of electric power produced by the generators on the load center entering the control volume.  The generator operation is run before the storage operation so that this value is current at the time the storage operation control is evaluated 
+
+  $ {P_{feed}}  $  This is the flow of electric power out of the control volume feeding toward the main panel.  This is power being supplied by the generators and storage and serving the building loads or perhaps being exported.  This power level might be reduced by power conversion losses before it reaches the main panel.  The method used to determine $ {P_{feed}}  $ depends on the operation scheme.
+  
+  $ {P_{draw}}  $  This is the flow of electric power into the control volume drawing from the main panel.  This is power being drawn in order to charge storage as desired by the storage operation scheme.  This power level might be increased by power conversion losses once it is drawn from the main panel.  
+
+  $ {P_{charge}}  $  This is the flow of electric power into the storage device from the control volume.  This is power being supplied by the generators and/or drawn from the main panel and then directed into storage to charge the device.
+
+  $ {P_{discharge}}  $  This is the flow of electric power out of the storage device into the control volume.  This power is being pulled from storage and added to the power from generators to feed toward the main panel. 
+
+The **TrackFacilityElectricDemandStoreExcessOnSite** method tries to run the storage to follow the facility electric demand while storing any excess on-site power production that is above what is needed to run the facility.  This is mainly appropriate for island operation.  This is the intended legacy behavior before version 8.5.  This scheme does not draw from the main panel to charge, so we have  $ {P_{draw}} = 0.0  $.  The value for $ {P_{feed}}  $ is determined from the whole-facility total electric power demand.  (When there is more than one load center in the model, it is actually the portion of the total that remains after previous load centers have been simulated.)  This requested feed in rate is adjusted to be increased by any power conversion losses that may occur in an inverter or a transformer.  This adjusted feed in request is used for $ {P_{feed}}  $. 
+
+If $ {P_{gen}} > {P_{feed}} $ ,  then we have charging, 
+
+\begin{equation}
+  \begin{array}{rl}
+    {P_{charge}} &= {P_{gen}} - {P_{feed}} \\
+    {P_{discharge}} &= 0.0
+  \end{array}
+\end{equation}
+
+If $ {P_{gen}} < {P_{feed}} $ , then we have discharging
+
+\begin{equation}
+  \begin{array}{rl}
+    {P_{discharge}} &=  {P_{feed}} - {P_{gen}} \\
+    {P_{charge}} &= 0.0
+  \end{array}
+\end{equation}
+
+The **TrackMeterDemandStoreExcessOnSite** method is very similar to the TrackFacilityElectricDemandStoreExcessOnSite method except that instead of using the whole-facility total electric demand, the value for $ {P_{feed}}  $ is determined from a user-specified meter.  The same charge and discharge logic is used. 
+
+The **TrackChargeDischargeSchedules** method tries to run the storage to follow user-defined schedules and design power levels for charging and discharging.  The user inputs a design charge rate $ {P_{charge,design}} $, a charge modification schedule $ {f_{sched,charge}} $, a design discharge rate $ {P_{discharge,design}} $, and a discharge modification schedule $ {f_{sched,discharge}} $.  The scheduled power flows will be used to determine charging and discharging as long as other limits on rates or state of charge are not triggered.  The schedules should be arranged to only charge or only discharge at a given time.  
+
+If charging, we have  
+
+\begin{equation}
+  \begin{array}{rl}
+    {P_{charge}} &= {P_{charge,design}} * {f_{sched,charge}} \\
+    {P_{discharge}} &= 0.0
+  \end{array}
+\end{equation}
+
+If $ {P_{gen}} > {P_{charge}} $,  then we have excess to feed toward main panel,
+
+\begin{equation}
+  \begin{array}{rl}
+    {P_{feed}} &= {P_{gen}} - {P_{charge}} \\
+    {P_{draw}} &= 0.0
+  \end{array}
+\end{equation}
+
+If $ {P_{gen}} < {P_{charge}} $, the we have a shortfall and we draw from main panel,
+
+\begin{equation}
+  \begin{array}{rl}
+    {P_{draw}} &= {P_{charge}} - {P_{gen}} \\
+    {P_{feed}} &= 0.0
+  \end{array}
+\end{equation}
+
+If discharging, we have 
+
+\begin{equation}
+  \begin{array}{rl}
+    {P_{discharge}} &= {P_{discharge,design}} * {f_{sched,discharge}} \\
+    {P_{charge}} &= 0.0 \\
+    {P_{feed}} &= {P_{discharge}} + {P_{gen}} \\
+    {P_{draw}} &= 0.0
+  \end{array}
+\end{equation}
+
+The **FacilityDemandLeveling** method tries to run the storage to follow a user-defined schedule for the net purchased power, $ {P_{net,purch}}  $.  This is similar to demand limit operation but instead of just attempting to cap the facility demand, it will also manipulate storage to increase utility grid supply electric to meet the target for net purchased power.  The user inputs a design demand target for net purchase power rate, $ {P_{net,purch,design}}  $, and a demand level modification schedule $ {f_{sched,dmd,target}} $.  
+
+\begin{equation}
+  {P_{net,purch,target}} = {P_{net,purch,design}} *{f_{sched,dmd,target}}
+\end{equation}
+
+This target is compared to an adjusted feed in request, $ {P_{feed, request}}  $, from the (remaining, adjusted) whole-facility total electric power demand. 
+
+\begin{equation}
+  {P_{feed}} = {P_{feed,request}} - {P_{net,purch,target}}
+\end{equation}
+
+If $ {P_{feed}} > 0.0 $, then we have a situation where the facility needs more power that the target demand.  We therefore feed that power toward the main panel, but it is not necessarily the full power request that could be served.  If $ {P_{gen}} < {P_{feed}} $, then we still have some power supply to make up by discharging,
+
+\begin{equation}
+  \begin{array}{rl}
+    {P_{discharge}} &=  {P_{feed}} - {P_{gen}} \\
+    {P_{charge}} &= 0.0
+  \end{array}
+\end{equation}
+
+Or if $ {P_{gen}} > {P_{feed}} $,  then we have excess power we can use for charging.
+
+\begin{equation}
+  \begin{array}{rl}
+    {P_{charge}} &= {P_{gen}} - {P_{feed}} \\
+    {P_{discharge}} &= 0.0
+  \end{array}
+\end{equation}
+
+However, if $ {P_{feed}} < 0.0 $, then the facility needs less power than the target demand.  We therefore draw power from the main panel to increase power purchased to meet target demand level. 
+
+\begin{equation}
+  \begin{array}{rl}
+   {P_{draw}} &= { abs( {P_{feed}} )} \\
+    {P_{feed}} &= 0.0 \\
+    {P_{charge}} &= {P_{draw}} + {P_{gen}}
+  \end{array}
+\end{equation}
+
+\subsection{Electrical Storage - Simple Energy Balance Model}
+
+EnergyPlus includes two models for storing electrical energy: a simple model that is not intended to represent any specific type of storage technology and a battery model that represents the kinetic battery model originally developed by Manwell and McGowan which discussed in the next section.
+
+The simple model treats the battery as a black box, counting energy added and removed, with losses due to charge/discharge inefficiencies. The model is a reasonable starting point for simulation of Li-ion and other battery technologies without significant rate limitations. The simple model might be called constrained bucket with energy losses.  The bucket holds a quantity of Joules of electrical energy, referred to as the state of charge. There are losses and limits to storing and drawing power but otherwise the bucket just holds electricity. The user sets constraints on the rates of charging, ${P_{stor - {\rm{charge - max}}}}$, and drawing, ${P_{stor - {\rm{d}}raw{\rm{ - max}}}}$. The user defines efficiency values for charging, ${\varepsilon_{{\rm{charge}}}}$, and drawing, ${\varepsilon_{draw}}$. 
+
+The user defines an initial state of charge and a maximum state of charge. The storage operation scheme makes supervisory control decisions and determines a value for the charging power, ${P_{stor - ch\arg e}}$, or the discharging power, ${P_{stor - draw}}$ and passes in control limits for the minimum and maximum state of charge fraction.  The maximum state of charge is the physical capacity of the storage device, however the storage control applies a separate layer of minimum and maximum state of charge used to model controller behavior designed to protect the battery from abuse. 
+
+The control requests are constrained by the device's physical limits for how fast it can be charged or discharged, ${P_{stor - {\rm{charge - max}}}}$ and ${P_{stor - {\rm{d}}raw{\rm{ - max}}}}$ are applied.
+
+If charging, the new state of charge, \(Q_{stor}^{t + \Delta t}\) , is determined using:
+
+\begin{equation}
+Q_{stor}^{t + \Delta t} = Q_{stor}^t + {P_{stor - ch\arg e}} \cdot {\varepsilon_{{\rm{charge}}}} \cdot \Delta t
+\end{equation}
+
+If drawing, the new state of charge is:
+
+\begin{equation}
+Q_{stor}^{t + \Delta t} = Q_{stor}^t - \frac{{{P_{stor - draw}} \cdot \Delta t}}{{{\varepsilon_{draw}}}}
+\end{equation}
+
+Where \(\Delta t\) ~is the length of the system time step in seconds.
+
+The storage device has an availability schedule. If it is not available then no power can be drawn or stored.  The state of charge minimum and maximum that are passed into the storage model are used to decide if the device can be further charged or discharged.  The separate control limits allow modeling battery preservation strategies where the full capacity of the storage device is not really used. 
+
+The gross electric power drawn and stored includes losses in the form of heat. These thermal losses are calculated from the user-specified efficiencies for charging and drawing and gross electric power stored and drawn. The thermal (heat) losses are included in a zone heat balance if the user specifies a thermal zone. A user-defined radiative split is used to divide thermal losses into radiation and convection portions. If no zone is specified, then the thermal losses are simply disregarded (e.g., rejected to outdoors and do not impact the zone air heat balance).
+
+\subsection{Electrical Storage -- Kinetic Battery Model with Cycle Life Estimation}\label{electrical-storage-kinetic-battery-model}
+
+The Kinetic Battery Model (KiBaM) (object: ElectricLoadCenter:Storage:Battery) was originally developed by Manwell and McGowan (1993) for use in time series performance models of hybrid energy systems. The model is called kinetic because it is based on a chemical kinetics process to simulate the battery charging and discharging behavior. The model, with different improvements and modifications, has been incorporated into the software Hybrid2 and HOMER as the electrical storage module of hybrid and distributed power systems. In 2005, KiBaM was implemented as a stand-alone application in support of the European Union Benchmarking research project (Bindner et al. 2005). The model is intended to represent technologies such as Pb-acid that encounter significant rate or kinetic limitations.
+
+The Kinetic Battery Model assumes that the battery charge is distributed over two tanks: an available-charge tank and a bound-charge tank. The tank for available charges can supply electrons directly to the load, whereas the tank for chemically bound charges can only supply electrons to the available-charge tank. At any time, the total charge \(q\) ~in the battery is the sum of the available charge (\({q_1}\) ) and bound charge (\({q_2}\) ). That is:
+
+\begin{equation}
+q = {q_1} + {q_2}
+\end{equation}
+
+Based on the governing equations on the change of charge in both tanks (Manwell and McGowan 1993), the battery capacity can be related to a constant charge/discharge current (\(I\) ) as the following equation:
+
+\begin{equation}
+{q_{\max }}(I) = \frac{{{q_{\max }}k \cdot c \cdot t}}{{1 - {e^{ - kt}} + c(kt - 1 + {e^{ - kt}})}}
+\end{equation}
+
+where,
+
+\({q_{\max }}(I)\) ~ : Maximum capacity (Ah) at charge or discharge current I
+
+\({q_{\max }}\) ~~~~~~ : Maximum capacity (Ah) at infinitesimal current
+
+\(t\) ~~~~~~~~~~~ : Charge or discharge time (hr), defined by \(t = \frac{{{q_{\max }}(I)}}{I}\)
+
+\(k\) ~~~~~~~~~~ : Constant coefficient (hr\(^{-1}\))
+
+\(c\) ~~~~~~~~~~ : Parameter indicating the ratio of available charge capacity to total capacity
+
+Assuming that a constant current is used in any time step for charging and discharging, the available charge (\({q_1}\) ) and bound charge (\({q_2}\) ) at any time step are given by:
+
+\begin{equation}
+{q_1} = {q_{1,0}}{e^{ - k\Delta t}} + \frac{{({q_0}kc - I)(1 - {e^{ - k\Delta t}})}}{k} - \frac{{Ic(k\Delta t - 1 + {e^{ - k\Delta t}})}}{k}
+\end{equation}
+
+\begin{equation}
+{q_2} = {q_{2,0}}{e^{ - k\Delta t}} + {q_0}(1 - c)(1 - {e^{ - k\Delta t}}) - \frac{{I(1 - c)(k\Delta t - 1 + {e^{ - k\Delta t}})}}{k}
+\end{equation}
+
+where,
+
+\({q_{1,0}}\) ~ :~ Available charge at the beginning of time step (Ah)
+
+\({q_{2,0}}\) ~:~ Bound charge at the beginning of time step (Ah)
+
+\({q_0}\) ~~ :~ Total charge at the beginning of time step (Ah), \({q_0} = {q_{1,0}} + {q_{2,0}}\)
+
+\(\Delta t\) ~~ :~ Length of time step (hr)
+
+KiBaM views the battery as a voltage source in series with an electric resistance (Figure~\ref{fig:electrical-equivalent-model-for-kibam}). The internal resistance is assumed to be constant and the open circuit voltage varies with current and state of charge.
+
+\begin{figure}[hbtp] % fig 338
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7528.svg.png}
+\caption{Electrical equivalent model for KiBaM \protect \label{fig:electrical-equivalent-model-for-kibam}}
+\end{figure}
+
+The battery's open circuit voltage is modeled in the same form for charging and discharging, but with different coefficients. The open circuit voltage in charging (\({E_c}\) ) and in discharging (\({E_d}\) ) can be respectively expressed as:
+
+\begin{equation}
+{E_c} = {E_{0,d}} + {A_c}{X_c} + \frac{{{C_c}{X_c}}}{{{D_c} - {X_c}}}
+\end{equation}
+
+\begin{equation}
+{E_d} = {E_{0,c}} + {A_d}{X_d} + \frac{{{C_d}{X_d}}}{{{D_d} - {X_d}}}
+\end{equation}
+
+where,
+
+\({E_{0,c}}\) ~~~~~~~~~~~~~~ : Open circuit voltage for a fully charged battery
+
+\({E_{0,d}}\) ~~~~~~~~~~~~~~ : Open circuit voltage for a fully discharged battery
+
+\({A_c}\) , \({C_c}\) , \({D_c}\) ~~~: Constant parameters for charging
+
+\({A_d}\) , \({C_d}\) , \({D_d}\) ~~: Constant parameters for discharging
+
+\({X_c}\) , \({X_d}\) ~~~~~~~~: Normalized maximum capacity at a given charging or discharging current, calculated as:
+
+\begin{equation}
+X = \left\{
+    \begin{array}{cl}
+      q_0 / q_{max}(I) & \; (charging) \\
+      (q_{max}-q_0)/q_{max}(I) & \; (discharging)
+    \end{array}
+  \right.
+\end{equation}
+
+It needs to be noted that the performance curve (Curve:RectangularHyperbola2) used in the model input covers the 2\(^{nd}\) and the 3\(^{rd}\) item of the open circuit voltage equation. Due to the reformatting of performance curve, the voltage function regression coefficients can map to the curve coefficients as follows:
+
+\({C_1} = - C\) ~;\({C_2} = - D\) ;\({C_3} = A\)
+
+With open circuit voltage, the battery terminal voltage (V) can be calculated as:
+
+\begin{equation}
+V = E - IR
+\end{equation}
+
+where, R is the battery internal resistance in Ohms; the current is positive for discharging and negative for charging.
+
+Given desired power in/out of the battery, the desired charge or discharge current can be calculated from the basic power equation: \(P = VI\) . In this calculation, iteration is needed to ensure the electric current has converged and the battery operation satisfies all specified technical constraints such as maximum discharge current and charge rate limit.
+
+KiBaM assumes that battery life is a primary function of charge/discharge cycles. One cycle is defined as the process of starting from a certain state of charge (SOC), the battery is discharged to a lower SOC and then recharged back to the starting SOC. It is regarded that the magnitude of cycle plays more important than the average of SOC during the cycle. This means that in terms of the impact on battery life, the cycle from 90\% to 70\% and then recharge back to 90\% of SOC is equivalent to another cycle from 50\% to 30\% and then recharge back to 50\% of SOC.~ Battery life in terms of the number of cycles is predicted as a function of the cycle range measured by the fractional depth of discharge. A double exponential equation is used to capture the damage to batteries due to cycling. The equation takes the following form where the coefficients need to be derived from battery test data via curve fitting.
+
+\begin{equation}
+{C_F} = {C_1} + {C_2}{e^{{C_3}R}} + {C_4}{e^{{C_5}R}}
+\end{equation}
+
+where,
+
+\({C_F}\) ~~~ :~~~ Cycles to failure
+
+\({C_1}\) -\({C_5}\) :~~~ Regression coefficients
+
+R~~~~~~ :~~~ Cycle range in terms of fractional SOC
+
+Following Hybrid2, the rainflow counting method (Downing and Socie 1982) is used to count battery cycles within a state of charge time series. Based on the number of cycles for each fractional SOC range, the battery damage is estimated as:
+
+\begin{equation}
+D = \sum\limits_{i = 1}^{} {\left( {{N_i}\frac{1}{{{C_{F,i}}}}} \right)}
+\end{equation}
+
+where,
+
+D~~~ : Fractional battery damage. For example, a value of 0.5 at the end of simulation means that half of the battery life is used up after the length of the simulation period.
+
+\({C_{F,i}}\) : Number of cycles to failure for the i-th cycle range
+
+\({N_i}\) ~ : Total number of cycles over the simulation with the i-th cycle range
+
+It needs to be noted that the temperature effects on battery performance and battery self-discharge are not supported in the current model.
+
+\subsubsection{References}\label{references-021}
+
+Bindner H., Cronin T., Lundsager P., Manwell J.F., Abdulwahid U., and Baring-Gould I. 2005. Lifetime Modeling of Lead Acid Batteries. Riso National Laboratory, Roskilde, Denmark.
+
+Downing S. D. and Socie D. F. 1982.~ Simple rainflow counting algorithms, International Journal of Fatigue, 1982.
+
+Manwell J. F. and McGowan J. G. 1993. A lead acid battery storage model for hybrid energy systems, Solar Energy 50(5): 399- 405.
+
+\subsection{Electric Load Center Transformers}\label{electric-load-center-transformers}
+
+Transformers (object name: ElectricLoadCenter:Transformer) are an integral part of the electric distribution system. They have two broad applications closely related to building energy simulation. First, transformers are used to lower the voltage of electricity from utility primary circuits to customer secondary circuits, and in this case they are called distribution transformers. Second, transformers are used to output the surplus power from onsite generators to the electricity grid.
+
+Distribution transformers reduce the voltage on utility distribution lines (34.5 kV or less) to a lower secondary voltage (600 V or less) suitable for customer equipment. Distribution transformers are usually categorized according to the medium used for cooling and insulation (liquid or air), the voltage class that they serve (low or medium), and the number of phases (single phase or three phase).
+
+Liquid-immersed transformers rely on oil or other fire resistant liquid around the coils for cooling. In contrast, dry type transformers rely only on the natural convection of air for insulation and cooling. Medium-voltage transformers step from utility line voltage down to a lower secondary voltage, depending on the application. The secondary voltage from a medium-voltage transformer is usually at 277 V for single phase and 480 V for three phase. This secondary voltage can be directly used as 480 V three-phase power for large motors or as 277 V single-phase power for some fluorescent lighting. However, for most industrial and commercial facilities, low-voltage transformers are needed to reduce the above voltages further to 208/120 V. Common 120 V loads are wall plugs and incandescent lighting.
+
+Most liquid-immersed transformers are owned by utilities and they are of the medium-voltage type. Virtually all dry type transformers are owned by commercial and industrial customers (Barnes et al. 1996). Of the dry type transformers, those of the medium-voltage type are generally special-order items while those of the low-voltage type are commodity items. The efficiency requirement of distribution transformers is covered by the NEMA (National Electrical Manufactures Association) Standard TP 1. ASHRAE 90.1-2010 will cite the NEMA Standard TP 1 to stipulate the efficiency requirement for the low-voltage dry type distribution transformers.
+
+There are two main types of energy losses in transformers: no load loss and load loss. The no load loss comes primarily from the switching of the magnetic fields in the core material. Hence, it is also called the core loss. The no load (core) loss is roughly constant and exists continuously in the core material as long as the transformer is energized. The load loss comes from the electrical resistance in the windings when there is a load on the transformer. Hence, the load loss is also called the winding loss. The load (winding) loss is proportional to the load squared with a small temperature correction.
+
+Given the no load loss (NL) and the load loss (LL) at rated load and conditions, the total energy losses in a transformer at time t is calculated as:
+
+\begin{equation}
+TL(t) = NL + LL(t) = NL + LL*P{(t)^2}*{f_T}(t)
+\end{equation}
+
+where,
+
+\(TL(t)\) ~~~~~~~ Total energy loss at time t (W)
+
+\(LL(t)\) ~~~~~~~ Load loss at time t (W)
+
+\(P(t)\) ~~~~~~~~~ Per unit load at time t
+
+\({f_T}(t)\) ~~~~~~~~ Temperature correction factor for the load loss at time t
+
+The per unit load at time t is calculated as:
+
+\begin{equation}
+P(t) = \frac{{Load(t)}}{{{S_B}}}
+\end{equation}
+
+where,
+
+\(Load(t)\) Transformer load at time t (W)
+
+\({S_B}\) Transformer nameplate rating (VA)
+
+The temperature correction factor at time t is calculated as (NEMA 2002):
+
+\begin{equation}
+{f_T}(t) = {L_{dc}}*\frac{{R(t)}}{{{R_{ref}}}} + {L_{eddy}}*\frac{{{R_{ref}}}}{{R(t)}}
+\end{equation}
+
+where,
+
+\({L_{dc}}\) ~~~~~~~~~~~ Per unit load loss due to electrical resistance
+
+\({L_{eddy}}\) ~~~~~~~~~ Per unit load loss due to eddy currents
+
+\(R(t)\) ~~~~~~~~~ Winding electrical resistance at time t
+
+\({R_{ref}}\) ~~~~~~~~~~ Winding electrical resistance at the full load reference conditions
+
+The ratio of winding electrical resistance is calculated as:
+
+\begin{equation}
+\frac{{R(t)}}{{{R_{ref}}}} = \frac{{F + {T_{winding}}(t) + {T_{amb}}(t)}}{{F + {T_{winding,ref}} + {T_{amb,ref}}}}
+\end{equation}
+
+where,
+
+\(F\) ~ Thermal coefficient of resistance for the winding material ( = 225 for aluminum and 234.5 for copper)
+
+\({T_{winding,ref}}\) Winding temperature rise at the full load reference conditions (°C)
+
+\({T_{winding}}(t)\) Winding temperature rise at time t (°C)
+
+\({T_{amb,ref}}\) ~~~~~~ Ambient temperature at the reference condition ( = 20 °C)
+
+\({T_{amb}}(t)\) ~~~~~ Ambient temperature at time t (°C)
+
+The Ambient temperature \({T_{amb}}(t)\) is equal to the zone temperature if a thermal zone is specified in the input; otherwise, it is assumed equal to 20 °C. The winding temperature rise at time t is calculated as (Barnes et al. 1997):
+
+\begin{equation}
+{T_{winding}}(t) = P{(t)^{1.6}}*{T_{winding.ref}}
+\end{equation}
+
+Based on the derived total energy losses in a transformer, the transformer efficiency at time t can be calculated according to the following equation:
+
+\begin{equation}
+\eta (t) = \frac{{Load(t)}}{{Load(t) + NL + LL(t)}}
+\end{equation}
+
+The above procedure describes how to calculate the total transformer energy losses based on the no load loss and load loss at rated conditions. The transformer model also supports the case when the nominal transformer efficiency is given. In this case, the user needs to provide the nameplate efficiency and the corresponding per unit load, the maximum efficiency and the corresponding per unit load, and the reference conductor temperature at which the nameplate efficiency is measured. Given these information, both no load loss and load loss at rated conditions can be derived as below.
+
+The nameplate efficiency can be expressed as:
+
+\begin{equation}
+{\eta_{np}} = \frac{{{S_B}*{P_{np}}}}{{{S_B}*{P_{np}} + NL + LL*P_{np}^2*{f_{T,np}}}}
+\end{equation}
+
+where,
+
+\({\eta_{np}}\) ~~~~~~~~~~~ Nameplate efficiency
+
+\({S_B}\) Nameplate rating (VA)
+
+\({P_{np}}\) ~~~~~~~~~~~ Per unit load at which the nameplate efficiency is measured
+
+\({f_{T,np}}\) ~~~~~~~~~ Applied temperature correction factor for the nameplate efficiency
+
+Maximum efficiency generally occurs when the load loss is equal to the no-load loss. Because the no-load loss does not vary with the load on the transformer, the following relationship can be established:
+
+\begin{equation}
+NL = L{L_{\max ,\eta }} = LL*P_{\max ,\eta }^2*{f_{T,\max  - \eta }}
+\end{equation}
+
+where,
+
+\({P_{\max ,\eta }}\) ~~~~~~~~ Per unit load at which the maximum efficiency is obtained
+
+\({f_{T,\max - \eta }}\) ~~~~ Applied temperature correction factor for the maximum efficiency
+
+Transformers typically have close per unit loads for the nameplate efficiency and the maximum efficiency. Therefore, it is reasonable to assume that the applied temperature correction factors are equal at those two efficiencies. This implies that:
+
+\begin{equation}
+\frac{{L{L_{np}}}}{{L{L_{\max ,\eta }}}} = \frac{{LL*{P_{np}}^2*{f_{T,np}}}}{{LL*{P_{\max ,\eta }}^2*{f_{T,\max  - \eta }}}} = {\left( {\frac{{{P_{np}}}}{{{P_{\max ,\eta }}}}} \right)^2}
+\end{equation}
+
+Rearranging Equation and combining it with Equation leads to:
+
+\begin{equation}
+L{L_{np}} = L{L_{\max ,\eta }}*{\left( {\frac{{{P_{np}}}}{{{P_{\max ,\eta }}}}} \right)^2} = NL*{\left( {\frac{{{P_{np}}}}{{{P_{\max ,\eta }}}}} \right)^2}
+\end{equation}
+
+Combining Equations and , we can obtain the no load loss as:
+
+\begin{equation}
+NL = \frac{{{S_B}*{P_{np}}*(1 - {\eta_{np}})}}{{{\eta_{np}}*\left[ {1 + {{\left( {\frac{{{P_{ref}}}}{{P{}_{\max ,\eta }}}} \right)}^2}} \right]}}
+\end{equation}
+
+Substitute NL into Equation , we can calculate the load loss at rated conditions as:
+
+\begin{equation}
+LL = \frac{{NL}}{{{f_{T,\max  - \eta }}*P_{\max ,\eta }^2}} = \frac{{NL}}{{{f_{T,np}}*P_{\max ,\eta }^2}}
+\end{equation}
+
+Since both no load and load losses at rated conditions are known, the total energy losses in a transformer at time t can then be calculated according to Equation
+
+\subsubsection{References:}\label{references-1-008}
+
+Barnes, PR., JW. Van Dyke, BW. McConnell, and S. Das. 1996. Determination Analysis of Energy Conservation Standards for Distribution Transformer, ORNL-6847. Oak Ridge National Laboratory, Oak Ridge, TN.
+
+Barnes, PR., S. Das, BW. McConnell, and JW. Van Dyke. 1997. Supplement to the ``Determination Analysis'' (ORNL-6847) and Analysis of the NEMA Efficiency Standard for Distribution Transformer, ORNL-6925. Oak Ridge National Laboratory, Oak Ridge, TN.
+
+NEMA. 2002. NEMA Standards Publication TP 1-2002: Guide for Determining Energy Efficiency for Distribution Transformers. National Electrical Manufactures Association, Rosslyn, VA.
diff --git a/doc/engineering-reference/src/on-site-generation/generators.tex b/doc/engineering-reference/src/on-site-generation/generators.tex
new file mode 100644
index 00000000000..8015953b2d9
--- /dev/null
+++ b/doc/engineering-reference/src/on-site-generation/generators.tex
@@ -0,0 +1,1195 @@
+\section{Generators}\label{generators}
+
+\subsection{Internal Cumbustion Engine}\label{internal-cumbustion-engine}
+
+The engine-driven generator model was originally developed for the BLAST program and was subsequently adapted for use in EnergyPlus. The model uses the following set of equations all of which are quadratic fits to the PLR (Part Load Ratio) of the generator.~ The coefficients must be derived from manufacturers data.
+
+\begin{equation}
+\frac{{electric\,\,energy\,\,output}}{{fuel\,\,energy\,\,input}} = \frac{{electric\,\,energy\,\,output}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {a_1} + {a_2}PLR + {a_3}PL{R^2}
+\end{equation}
+
+The electrical load and engine generator nominal load capacity are used to compute the part load ratio.
+
+\begin{equation}
+PLR = \frac{{Electric energy output}}{{nominal generating capacity}}
+\end{equation}
+
+The exhaust gas temp and flow rate are used if a stack heat exchanger is used to recover waste heat from the exhaust.~ This temperature is the inlet temperature to the heat exchanger which is modeled in a UA-effectiveness form:
+
+\begin{equation}
+\frac{{Total\,Exhaust\,heat}}{{fuel\,energy\,input}} = \frac{{Total\,\,Exhaust\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {d_1} + {d_2}PLR + {d_3}PL{R^2}
+\end{equation}
+
+\begin{equation}
+\frac{{Exhaust\,\,Gas\,\,Temp\,\,\left\{ K \right\}}}{{fuel\,\,energy\,\,input}} = \frac{{Exhaust\,\,Gas\,\,Temp\,\,\left\{ K \right\}}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {e_1} + {e_2}PLR + {e_3}PL{R^2}
+\end{equation}
+
+The exhaust flow rate is then calculated as:
+
+\begin{equation}
+{\dot m_{exhaust}} = \frac{{Total\,\,Exhaust\,\,heat}}{{C{p_{exhaust}} \cdot \left( {{T_{exhaust}} - {T_{reference}}} \right)}}
+\end{equation}
+
+where T\(_{reference}\) is the reference temperature for the fuel lower heating value, and is given as 25°C in manufacturer's data, and
+
+\begin{equation}
+{T_{stack}} = {T_{DesignMinExhaust}} + {\frac{{\left( {{T_{exhaust}} - {T_{DesignMinExhaust}}} \right)}}{{{\rm{exp}}\left( {\frac{{{\rm{UA}}}}{{{{{\rm{\dot m}}}_{{\rm{exhaust}}}}C{p_{exhaust}}}}} \right)}}^2}
+\end{equation}
+
+Finally heat recovered from the lube oil and the water jacket are accounted for as follows:
+
+\begin{equation}
+\frac{{Recoverable\,\,jacket\,\,heat}}{{fuel\,\,energy\,\,input}} = \frac{{Recoverable\,\,jacket\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {b_1} + {b_2}PLR + {b_3}PL{R^2}
+\end{equation}
+
+\begin{equation}
+\frac{{Recoverable\,\,lube\,\,oil\,\,heat}}{{fuel\,\,energy\,\,input}} = \frac{{Recoverable\,\,lube\,\,oil\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {c_1} + {c_2}PLR + {c_3}PL{R^2}
+\end{equation}
+
+The manufacturer must supply the recoverable water jacket heat, lube oil heat and exhaust heat and associated fuel consumption for a range of load conditions.~ This data is then fit to the PLR to obtain the fifteen a,b,c,d, and e coefficients.
+
+\subsection{Turbine Generator}\label{turbine-generator}
+
+The combustion turbine generator model was originally developed for the BLAST program and was subsequently adapted for use in EnergyPlus. The model uses the following set of equations all of which are equation fits to the PLR (Part Load Ratio) of the generator and the entering air temperature. The coefficients must be derived from manufacturers data. For electric power generated in Watts, the fuel input rate is calculated in J/s.
+
+\begin{equation}
+\frac{{{\rm{fuel energy input rate}}}}{{{\rm{electric power output}}}} = \left[ {{a_1} + {a_2}PLR + {a_3}PL{R^2}} \right] * \left[ {{b_1} + {b_2}\Delta T + {b_3}\Delta {T^2}} \right]
+\end{equation}
+
+The electrical load and engine generator nominal load capacity are used to compute the part load ratio.
+
+\begin{equation}
+PLR = \frac{{{\rm{Electric energy output}}}}{{{\rm{nominal generating capacity}}}}
+\end{equation}
+
+The temperature difference shows the deviation of ambient air temperature from the manufacturers design air temperature.
+
+\begin{equation}
+\Delta T = {T_{air}} - {T_{design}}
+\end{equation}
+
+A second curve fit calculates the exhaust temperature (C) by multiplying the exhaust temperature (C) for a particular part load by a correction factor based on the deviation from design temperature.
+
+\begin{equation}
+{{\rm{T}}_{exhaust}} = \left[ {{c_1} + {c_2}PLR + {c_3}PL{R^2}} \right] * \left[ {{d_1} + {d_2}\Delta T + {d_3}\Delta {T^2}} \right]
+\end{equation}
+
+The exhaust gas temp is used if a stack heat exchanger is used to recover waste heat from the exhaust.~ This temperature is the inlet temperature to the heat exchanger which is modeled in a UA-effectiveness form:
+
+\begin{equation}
+{T_{stack}} = {T_{DesignMinExhaust}} + {\frac{{\left( {{T_{exhaust}} - {T_{DesignMinExhaust}}} \right)}}{{{\rm{exp}}\left( {\frac{{{\rm{UA}}}}{{{{{\rm{\dot m}}}_{{\rm{exhaust}}}}C{p_{exhaust}}}}} \right)}}^2}
+\end{equation}
+
+Where the design minimum exhaust temperature is a user input to the model and the exhaust mass flow rate and the UA are fit from manufacturers data as follows:
+
+\begin{equation}
+UA = {e_3}{{\rm{(Nominal Generating Capacity)}}^{e4}}
+\end{equation}
+
+\begin{equation}
+\frac{{{\rm{exhaust gas flow rate}}}}{{{\rm{Nominal Generating Capacity}}}} = \left[ {{f_1} + {f_2}\Delta T + {f_3}\Delta {T^2}} \right]
+\end{equation}
+
+Finally, heat recovered from the lube oil is accounted for as follows:
+
+\begin{equation}
+\frac{{{\rm{Recoverable lube oil heat}}}}{{{\rm{electric power generated}}}} = {g_1} + {g_2}PLR + {g_3}PL{R^2}
+\end{equation}
+
+\subsection{Microturbine Generator}\label{microturbine-generator}
+
+Microturbine generators are small combustion turbines that produce electricity on a relatively small scale (e.g., 25kW to 500kW). This model uses nominal performance at reference conditions along with several modifier curves to determine electrical power output and fuel use at non-reference conditions. The modifier curve coefficients must be derived from manufacturers data. Standby and ancillary power can also be taken into account.
+
+Exhaust air energy recovery for heating water can be also be modeled. Similar to electrical power output, thermal power (heat recovery to water) output is calculated using nominal performance at reference conditions with modifier curves to account for variations at non-reference conditions. The ElectricLoadCenter:Generators and ElectricLoadCenter:Distribution objects are used to define the availability and control of the electric generators included in the simulation (ref. ElectricLoadCenter:Generators and ElectricLoadCenter:Distribution).
+
+For each simulation time step that the generator is being asked to operate (i.e., produce electrical power as determined by the ElectricLoadCenter), the full load electrical output of the generator is determined using the user-defined reference electrical power output along with a bi-quadratic modifier curve to account for differences in the combustion air inlet temperature and elevation for the current simulation time step compared to the reference temperature and elevation (i.e., the modifier curve should evaluate to 1.0 at the reference combustion air inlet temperature and reference elevation).
+
+\begin{equation}
+{P_{Elec,Full\,Load\,}} = {P_{Elec,Ref}}\left( {PowerFTempElev} \right)
+\end{equation}
+
+\begin{equation}
+PowerFTempElev = {a_1} + {a_2}\left( {{T_{a,i}}} \right) + {a_3}{\left( {{T_{a,i}}} \right)^2} + {a_4}\left( {Elev} \right) + {a_5}{\left( {Elev} \right)^2} + {a_6}\left( {{T_{a,i}}} \right)\left( {Elev} \right)
+\end{equation}
+
+where:
+
+\({P_{Elec,Full\,Load}}\) = Full load electrical power output (W)
+
+\({P_{Elec,Ref}}\) = Reference Electrical Power Output, user input (W)
+
+\(PowerFTempElev\) = User-defined Electric Power Modifier Curve (function of temperature and elevation) evaluated at the current combustion air inlet temperature and elevation
+
+\({T_{a,i}}\) = Combustion air inlet temperature (°C)
+
+\(Elev\) = Elevation (m). This value obtained from the Location object or the weather file.
+
+The full load electrical power output of the generator is then checked against the minimum and maximum full load electrical power outputs specified by the user:
+
+\begin{equation}
+{P_{Elec,Full\,Load}} = MIN\left( {{P_{Elec,Full\,Load}},{P_{FL_Max}}} \right)
+\end{equation}
+
+\begin{equation}
+{P_{Elec,Full\,Load}} = MAX\left( {{P_{Elec,Full\,Load}},{P_{FL_Min}}} \right)
+\end{equation}
+
+\({P_{FL_Max}}\) ~ = Maximum Full Load Electrical Power Output, user input (W)
+
+\({P_{FL_Min}}\) ~ = Minimum Full Load Electrical Power Output, user input (W)
+
+The actual (operating) electrical power output from the generator is determined next based on the load requested by the Electric Load Center, the generator's minimum and maximum part-load ratios, and the ancillary power.
+
+\begin{equation}
+{P_{Elec,Operating}} = MAX\left( {0.0,\left( {Load + {P_{Ancillary}}} \right)} \right)
+\end{equation}
+
+\begin{equation}
+{P_{Elec,Operating}} = MIN\left( {{P_{Elec,Operating}},{P_{Elec,Full\,Load}}} \right)
+\end{equation}
+
+\begin{lstlisting}
+ IF (P_elec_fullload > 0) THEN
+   PLR = P_elec_operating / P_elec_fullload
+   PLR = MIN( PLR, PLR_max )
+   PLR = MAX( PLR, PLR_min )
+ ELSE
+   PLR = 0
+ END IF
+ P_elec_operating = P_elec_fullload * PLR
+\end{lstlisting}
+
+where:
+
+\({P_{Elec,Operating}}\) = Actual (operating) electrical power output (W)
+
+\(Load\) ~ = Electrical power output being requested by the Electric Load Center (W)
+
+\({P_{Ancillary}}\) ~ = Ancillary Power, user input (W)
+
+\(PLR\) = Part-load ratio of the electric generator
+
+\(PL{R_{\max }}\) = Maximum part-load ratio of the electric generator (i.e., the maximum value for the independent variable {[}PLR{]} defined in the Curve:Quadratic or Curve:Cubic object for the Electrical Efficiency Modifier Curve {[}function of part-load ratio{]})
+
+\(PL{R_{\min }}\) = Minimum part-load ratio of the electric generator (i.e., the minimum value for the independent variable {[}PLR{]} defined in the Curve:Quadratic or Curve:Cubic object for the Electrical Efficiency Modifier Curve {[}function of part-load ratio{]})
+
+The generator's electrical efficiency is then calculated based on the user-specified reference electrical efficiency (lower heating value {[}LHV{]} basis) and two electrical efficiency modifier curves.
+
+\begin{equation}
+ElecEfficiencyFTemp = {b_1} + {b_2}\left( {{T_{a,i}}} \right) + {b_3}{\left( {{T_{a,i}}} \right)^2}\,\,\,\,or\,\,\,\,\,{b_1} + {b_2}\left( {{T_{a,i}}} \right) + {b_3}{\left( {{T_{a,i}}} \right)^2} + {b_4}{\left( {{T_{a,i}}} \right)^3}
+\end{equation}
+
+\begin{equation}
+ElecEfficiencyFPLR = {c_1} + {c_2}\left( {PLR} \right) + {c_3}{\left( {PLR} \right)^2}\,\,\,\,or\,\,\,\,\,{c_1} + {c_2}\left( {PLR} \right) + {c_3}{\left( {PLR} \right)^2} + {c_4}{\left( {PLR} \right)^3}
+\end{equation}
+
+\begin{equation}
+ElecEf{f_{Operating}} = ElecEf{f_{Ref,LHV}}\left( {ElecEfficiencyFTemp} \right)\left( {ElecEfficiencyFPLR} \right)
+\end{equation}
+
+where:
+
+\(ElecEfficiencyFTemp\) ~ = User-defined Electrical Efficiency Modifier Curve (function of temperature) evaluated at the current combustion air inlet temperature
+
+\(ElecEfficiencyFPLR\) ~ = User-defined Electrical Efficiency Modifier Curve (function of part-load ratio) evaluated at the current operating part-load ratio
+
+\(ElecEf{f_{Operating}}\) ~ = Electrical efficiency at the current operating conditions
+
+\(ElecEf{f_{Ref,LHV}}\) ~ = Reference Electrical Efficiency (LHV {[}lower heating value{]} Basis),~~~~ user input
+
+The fuel energy consumption rate (LHV Basis) is then calculated as follows:
+
+\begin{equation}
+\dot{Q}_{Fuel,LHV} = \frac{P_{Elec,Operating}}{ElecEff_{Operating}}
+\end{equation}
+
+where:
+
+\({\dot Q_{Fuel,LHV}}\) ~ = Fuel energy consumption rate, LHV basis (W)
+
+If \emph{ElecEff\(_{Operating}\)} is equal to zero, then \emph{P\(_{Operating}\)} and \({\dot Q_{Fuel,LHV}}\) are set to zero. The fuel mass flow rate is then calculated.
+
+\begin{equation}
+\dot{m}_{fuel} = \frac{\dot{Q}_{Fuel,LHV}}{LHV*1000}
+\end{equation}
+
+where:
+
+\({\dot m_{fuel}}\) ~ = Mass flow rate of fuel being consumed by the generator (kg/s), report variable ``Generator \textless{}FuelType\textgreater{} Mass Flow Rate {[}kg/s{]}''
+
+\emph{LHV} = Fuel Lower Heating Value, user input (kJ/kg)
+
+The ancillary power is calculated next using the user-specified ancillary power and ancillary power modifier curve. The ancillary power modifier curve is a quadratic function with the generator's fuel mass flow rate as the independent variable. If an ancillary power modifier curve is not specified in the input file, the modifier is assumed to be 1.0 and the ancillary power will be constant throughout the simulation.
+
+\begin{equation}
+AnciPowFMdotFuel = {d_1} + {d_2}\left( {{{\dot m}_{fuel}}} \right) + {d_3}{\left( {{{\dot m}_{fuel}}} \right)^2}
+\end{equation}
+
+\begin{equation}
+{P_{Ancillary,Operating}} = {P_{Ancillary}}\left( {AnciPowFMdotFuel} \right)
+\end{equation}
+
+where:
+
+\(AnciPowFMdotFuel\) ~ = User-defined Ancillary Power Modifier Curve (function of fuel input) evaluated at the actual fuel mass flow rate. This multiplier is assumed to be 1.0 if an ancillary power modifier curve name is not specified in the input.
+
+\({P_{Ancillary}}\) ~ = Ancillary power, user input (W)
+
+\({P_{Ancillary,Operating}}\) ~ = Ancillary electric power at the current fuel mass flow rate (W), report variable ``Generator Ancillary Electric Power {[}W{]}''.
+
+If ancillary power is constant for the simulation (e.g., no modifier curve defined), then the calculations continue as described below. However, if an ancillary power modifier curve has been defined, then the calculations described above for \emph{P\(_{ElecOperating}\)}, \emph{ElecEff\(_{Operating}\)}, \({\dot Q_{Fuel,LHV}}\) and \emph{P\(_{Ancillary,Operating}\)} are recalculated in sequence until the solution converges.
+
+The generator's ``net'' electrical power output is calculated as the difference between the generator's actual power output and the ancillary electric power as follows.
+
+\begin{equation}
+{P_{Elec,Produced}} = {P_{Elec,Operating}} - {P_{Ancillary,Operating}}
+\end{equation}
+
+where:
+
+\({P_{Elec,Produced}}\) ~ = Generator net electric power output, report variable ``Generator Produced Electric Power {[}W{]}''
+
+The fuel energy consumption rate (higher heating value basis) for the generator is then calculated as follows:
+
+\begin{equation}
+{\dot Q_{Fuel,HHV}} = {\dot m_{fuel}}\left( {HHV} \right)\left( {1000} \right)
+\end{equation}
+
+where:
+
+\({\dot Q_{Fuel,HHV}}\) ~ = fuel energy consumption rate (W), report variables ``Generator \textless{}FuelType\textgreater{} HHV Basis Rate {[}W{]}'' and ``Generator Fuel HHV Basis Rate {[}W{]}''
+
+\(HHV\) = Fuel Higher Heating Value, user input (kJ/kg)
+
+Standby electrical power may also be modeled to simulate controls or other parasitics used by the generator. The standby power is calculated only when the generator is not operating (i.e., \emph{Load} from the Electric Load Center is zero). If the generator operates for a given timestep (i.e., \emph{Load} \textgreater{} 0.0), the standby power is set equal to 0.
+
+\begin{equation}
+P_{Standby} = \left\{
+  \begin{array}{cc}
+    P_{Standby,UserInput} &\text{if} Load <= 0 \\
+    0                     &\text{otherwise}
+  \end{array}
+\right.
+\end{equation}
+
+where:
+
+\({P_{Standby,user\,input}}\) ~ = Standby power, user input (W)
+
+\({P_{Standby}}\) ~ = Report variable ``Generator Standby Electric Power'' (W)
+
+Report variables for electric energy produced, electric efficiency (LHV basis), fuel consumption (HHV basis), standby electric consumption and ancillary electric consumption are calculated as follows:
+
+\begin{equation}
+{E_{Elec,Produced}} = {P_{Elec,Produced}}\left( {TimeStepSys} \right)\left( {3600} \right)
+\end{equation}
+
+\begin{equation}
+ElecEff_{Operating,LHV} = \frac{P_{Elec,Produced}}{\dot{Q}_{Fuel,LHV}}
+\end{equation}
+
+\begin{equation}
+{Q_{Fuel,HHV}} = {\dot Q_{Fuel,HHV}}\left( {TimeStepSys} \right)\left( {3600} \right)
+\end{equation}
+
+\begin{equation}
+{E_{Standby}} = {P_{Standby}}\left( {TimeStepSys} \right)\left( {3600} \right)
+\end{equation}
+
+\begin{equation}
+{E_{Ancillary}} = {P_{Ancillary,Operating}}\left( {TimeStepSys} \right)\left( {3600} \right)
+\end{equation}
+
+where:
+
+\({E_{Elec,Produced}}\) ~ = Report variable ``Generator Produced Electric Energy {[}J{]}''
+
+\(ElecEf{f_{Operating,LHV}}\) = Report variable ``Generator LHV Basis Electric Efficiency {[}-{]}''
+
+\({Q_{Fuel,HHV}}\) ~ = Report variables ``Generator \textless{}FuelType\textgreater{} HHV Basis Energy {[}J{]}'' and ``Generator Fuel HHV Basis Energy {[}J{]}''
+
+\({E_{Standby}}\) ~ = Report variable ``Generator Standby Electric Energy {[}J{]}''
+
+\({E_{Ancillary}}\) ~ = ~ Report variable ``Generator Ancillary Electric Energy {[}J{]}''
+
+\emph{TimeStepSys} = HVAC system simulation time step (hr)
+
+In addition to calculating electric power production and fuel usage, the model is able to determine thermal power (heat recovery) output for heating water.~ For this case, the water flow rate through the heat recovery heat exchanger is established first. If the Heat Recovery Water Flow Operating Mode (user input) is set to Plant Control, then the Reference Heat Recovery Water Flow Rate (user input) is requested whenever the generator operates (constant value), but the actual flow rate may be restricted by other plant components (e.g., pump). If the Heat Recovery Water Flow Operating Mode is set to Internal Control, then the requested water flow when the generator operates is determined by the Reference Heat Recovery Water Flow Rate and a flow rate modifier curve.
+
+If \emph{PlantControl}:
+\begin{equation}
+  \dot{m}_w = \dot{V}_{w,ref}\rho_w
+\end{equation}
+
+If \emph{InternalControl}:
+\begin{equation}
+  \text{HeatRecFlowFTempPow} = e_1 + e_2 T_{w,i} + e_3 T_{w,i}^2 + e_4 P_{net} + e_5 P_{net}^2 + e_6 T_{w,i} P_{net}
+\end{equation}
+\begin{equation}
+  \dot{m}_w = \dot{V}_{w,Ref} \rho_w \PB{HeatRecFlowFTempPow}
+\end{equation}
+
+~where:
+
+\({\dot m_w}\) = Report variable ``Generator Heat Recovery Water Mass Flow Rate {[}kg/s{]}''
+
+\({\dot V_{w,Ref}}\) = Reference Heat Recovery Water Flow Rate (m\(^{3}\)/s), user input
+
+\({\rho_w}\) = Density of water (kg/m\(^{3}\)) at 5.05°C
+
+\(HeatRecFlowFTempPow\) = User-defined Heat Recovery Water Flow Rate Modifier Curve (function of temperature and power) evaluated at the current inlet water temperature and net electrical power output. This multiplier is assumed to be 1.0 if a water flow rate modifier curve name is not specified in the input.
+
+\({T_{w,i}}\) = Heat recovery inlet water temperature (°C), report variable ``Generator Heat Recovery Inlet Temperature {[}C{]}''
+
+\({P_{net}}\) = Net electrical power output from the generator (W)
+
+The methodology for determining thermal power (heat recovery to water) is similar to that used for calculating electric power production. The generator's steady-state thermal efficiency is calculated based on the user-specified reference thermal efficiency (LHV basis) and a thermal efficiency modifier curve.
+
+\begin{equation}
+ThermalEf{f_{SS\,}} = ThermalEf{f_{Ref,LHV}}\left( {ThermalEffFTempElev} \right)
+\end{equation}
+
+\begin{equation}
+ThermalEffFTempElev = {f_1} + {f_2}\left( {{T_{a,i}}} \right) + {f_3}{\left( {{T_{a,i}}} \right)^2} + {f_4}\left( {Elev} \right) + {f_5}{\left( {Elev} \right)^2} + {f_6}\left( {{T_{a,i}}} \right)\left( {Elev} \right)
+\end{equation}
+
+where:
+
+\(ThermalEf{f_{SS}}\) = Steady-state thermal efficiency at current conditions
+
+\(ThermalEf{f_{Ref,LHV}}\) = Reference Thermal Efficiency (LHV Basis), user input
+
+\(ThermalEffFTempElev\) = User-defined Thermal Efficiency Modifier Curve (function of temperature and elevation) evaluated at the current combustion air inlet temperature and elevation. This multiplier is assumed to be 1.0 if a thermal efficiency modifier curve name is not specified in the input.
+
+The steady-state thermal power produced (heat recovery rate) is then calculated:
+
+\begin{equation}
+{P_{Thermal,SS}} = ThermalEf{f_{SS}}\left( {{{\dot Q}_{Fuel,LHV}}} \right)
+\end{equation}
+
+The actual (operating) thermal power is then calculated using the steady-state thermal power and three modifier curves:
+
+\begin{equation}
+  P_{Thermal,Operating} = P_{Thermal,SS} \PB{\text{HeatRecRateFPLR}} \PB{\text{HeatRecRateFTemp}} \PB{\text{HeatRecRateFFlow}}
+\end{equation}
+\begin{equation}
+  \begin{array}{cc}
+    \text{HeatRecRateFPLR} &= g_1 + g_2 \PB{PLR} + g_3 \PB{PLR}^2  \\
+                 \text{OR} &= g_1 + g_2 \PB{PLR} + g_3 \PB{PLR}^2 + g_4 \PB{PLR}^3
+  \end{array}
+\end{equation}
+
+\begin{equation}
+HeatRecRateFTemp = {h_1} + {h_2}\left( {{T_{w,i}}} \right) + {h_3}{\left( {{T_{w,i}}} \right)^2}
+\end{equation}
+
+\begin{equation}
+HeatRecRateFFlow = {i_1} + {i_2}\left( {{{\dot m}_w}} \right) + {i_3}{\left( {{{\dot m}_w}} \right)^2}
+\end{equation}
+
+where:
+
+\({P_{Thermal,Operating}}\) = Report variable ``Generator Produced Thermal Rate {[}W{]}''
+
+\(HeatRecRateFPLR\) = User-defined Heat Recovery Rate Modifier Curve (function of part-load ratio) evaluated at the current operating part-load ratio. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
+
+\(HeatRecRateFTemp\) = User-defined Heat Recovery Rate Modifier Curve (function of inlet water temperature) evaluated at the current inlet water temperature. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
+
+\(HeatRecRateFFlow\) = User-defined Heat Recovery Rate Modifier Curve (function of water flow rate) evaluated at the current heat recovery water flow rate. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
+
+The heat recovery output water temperature is then calculated.
+
+\begin{equation}
+  T_{w,o} = T_{w,i} + \frac{P_{Thermal,Operating}}{\dot{m}_w C{p,w}}
+\end{equation}
+
+where:
+
+\({T_{w,o}}\) = Heat recovery outlet water temperature (°C), report variable ``Generator Heat Recovery Outlet Temperature {[}C{]}''
+
+\(C{p_w}\) = Heat capacity of water (J/kg-K)
+
+If the calculated heat recovery outlet water temperature exceeds to Maximum Heat Recovery Water Temperature (user input), then the outlet water temperature is reset to the maximum temperature (user input) and the thermal power is recalculated.
+
+If combustion air inlet and outlet node names are specified in the input, along with exhaust air flow rate and exhaust air temperature information, then the model calculates the exhaust air conditions for each simulation time step. The exhaust air mass flow rate is first calculated based on the Reference Exhaust Air Mass Flow Rate, two modifier curves and an air density adjustment. Since fans are volumetric flow devices, the ratio of the air density at actual inlet air conditions to air density at reference inlet air conditions is used as an adjustment factor.
+
+\begin{equation}
+  \dot{m}_{ExhAir} = \dot{m}_{ExhAir,ref} \PB{\text{ExhFlowFTemp}} \PB{\text{ExhFlowFPLR}} \frac{\rho_{a,i}}{\rho_{a,ref}}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{cc}
+    ExhFlowFTemp     &= j_1 + j_2 T_{a,i} + j_3 T_{a,i}^2 \\
+           \text{OR} &= j_1 + j_2 T_{a,i} + j_3 T_{a,i}^2 + j_4 T_{a,i}^3
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{cc}
+    ExhFlowFPLR      &= k_1 + k_2 T_{PLR} + k_3 T_{PLR}^2 \\
+           \text{OR} &= k_1 + k_2 T_{PLR} + k_3 T_{PLR}^2 + k_4 T_{PLR}^3
+  \end{array}
+\end{equation}
+
+where:
+
+\({\dot m_{ExhAir}}\) = Exhaust air mass flow rate (kg/s)
+
+\({\dot m_{ExhAir,Ref}}\) = Reference Exhaust Air Mass Flow Rate (kg/s), user input
+
+\(ExhFlowFTemp\) = User-defined Exhaust Air Flow Rate Modifier Curve (function of temperature) evaluated at the current combustion air inlet temperature. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
+
+\(ExhFlowFPLR\) ~ = User-defined Exhaust Air Flow Rate Rate Modifier Curve (function of part-load ratio) evaluated at the current operating part-load ratio. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
+
+\({\rho_{a,i}}\) = Density of the combustion inlet air (kg/m\(^{3}\))
+
+\({\rho_{a,Ref}}\) = Density of combustion inlet air at reference conditions (kg/m\(^{3}\))
+
+In an analogous fashion, the exhaust air temperature is calculated using the Nominal (reference) Exhaust Air Outlet Temperature and two modifier curves.
+
+\begin{equation}
+  T_{a,o} = T_{a,o,Nom} \PB{\text{ExhAirTempFTemp}} \PB{\text{ExhAirTempFPLR}}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{cc}
+    ExhAirTempFTemp  &= l_1 + l_2 T_{a,i} + l_3 T_{a,i}^2 \\
+           \text{OR} &= l_1 + l_2 T_{a,i} + l_3 T_{a,i}^2 + l_4 T_{a,i}^3
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{cc}
+    ExhAirTempFPLR   &= m_1 + m_2 T_{PLR} + m_3 T_{PLR}^2 \\
+           \text{OR} &= m_1 + m_2 T_{PLR} + m_3 T_{PLR}^2 + m_4 T_{PLR}^3
+  \end{array}
+\end{equation}
+
+where:
+
+\({T_{a,o}}\) = Exhaust air outlet temperature (°C)
+
+\({T_{a,o,Nom}}\) = Nominal Exhaust Air Outlet Temperature (°C), user input
+
+\(ExhAirTempFTemp\) = User-defined Exhaust Air Temperature Modifier Curve (function of temperature) evaluated at the current combustion air inlet temperature. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
+
+\(ExhAirTempFPLR\) ~ = User-defined Exhaust Air Flow Rate Rate Modifier Curve (function of part-load ratio) evaluated at the current operating part-load ratio. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
+
+The above calculations for exhaust air outlet temperature assume no heat recovery to water is being done.~ If thermal power (water heating) is being produced, then the exhaust air outlet temperature is recalculated as follows:
+
+\begin{equation}
+T_{a,o} = T_{a,i} - \frac{P_{Thermal,Operating}}{\dot{m}_{ExhAir}C_{p,air}}
+\end{equation}
+
+where:
+
+\(C{p_{air}}\) = Heat capacity of air at the actual combustion air inlet conditions (J/kg-K)
+
+The exhaust air outlet humidity ratio is also calculated.
+
+\begin{equation}
+  w_{a,o} = w_{a,i} + \frac{\dot{m}_{fuel} \PB{HHV - LHV} \PB{1000}}{h_{fg,16} \dot{m}_{ExhAir}}
+\end{equation}
+
+where:
+
+\({w_{a,o}}\) = Exhaust air outlet humidity ratio (kg/kg)
+
+\({w_{a,i}}\) = Exhaust air inlet humidity ratio (kg/kg)
+
+\({h_{fg,16}}\) = Enthalpy of vaporization of moisture at 16°C (J/kg)
+
+The remaining report variables are calculated as follows.
+
+\begin{equation}
+{E_{Thermal,Produced}} = {P_{Thermal,Operating}}\left( {TimeStepSys} \right)\left( {3600} \right)
+\end{equation}
+
+\begin{equation}
+ThermalEff_{Operating,LHV} = \frac{P_{Thermal,Operating}}{\dot{Q}_{Fuel,LHV}}
+\end{equation}
+
+where:
+
+\({E_{Thermal,Produced}}\) = Report variable ``Generator Produced Thermal Energy {[}J{]}''
+
+\(ThermalEf{f_{Operating,LHV}}\) = Report variable ``Generator Thermal Efficiency LHV Basis {[}-{]}''
+
+\subsection{Micro-Cogenerator}\label{micro-cogenerator}
+
+The input object Generator:MicroCHP provides a model that is a direct implementation of a model developed by IEA Annex 42 -- The Simulation of Building-Integrated Fuel Cell and Other Cogeneration Systems (FC+COGEN-SIM).~ Annex 42 was formed as a working group within the International Energy Agency (IEA) program on Energy Conservation in Buildings and Community Systems (ECBCS). A full description of the model specification can be found in the report by Subtask B of FC+COGEN-SIM with the title ``Specifications for Modelling Fuel Cell and Combustion-Based Residential Cogeneration Device within Whole-Building Simulation Programs.''~ The ``Micro CHP'' model in EnergyPlus is the one referred to as ``A Generic Model for Combustion-based Residential Cogeneration Devices.''
+
+The Micro CHP model is a straightforward empirical model with the exception that it is dynamic with respect to thermal heat recovery where performance is cast as a function of engine temperature.~ It is also dynamic with respect to possible warm up and cool down periods that may affect the ability of the generator to deliver the requested power.~ The relevant model equations are:
+
+\begin{equation}
+{\eta_e} = f({\dot m_{cw}},{T_{cw,i}},{P_{net,ss}})
+\end{equation}
+
+\begin{equation}
+{\eta_q} = f({\dot m_{cw}},{T_{cw,i}},{P_{net,ss}})
+\end{equation}
+
+\begin{equation}
+{q_{gross}} = {P_{net,ss}}/{\eta_e}
+\end{equation}
+
+\begin{equation}
+{q_{gen,ss}} = {\eta_q}{q_{gross}}
+\end{equation}
+
+\begin{equation}
+{\dot N_{fuel}} = {q_{gross}}/LH{V_{fuel}}
+\end{equation}
+
+\begin{equation}
+\dot m_{fuel}^{t+\Delta t} = \left\{
+    \begin{array}{cl}
+      \dot m_{fuel,demand}^{t+\Delta t}       &\; if d\dot m_{fuel} / dt \le (d\dot m_{fuel}/dt)_{max} \\
+      \dot m_{fuel,demand}^t \pm (d\dot m_{fuel}/dt)_{max}      &\; if d\dot m_{fuel} / dt > (d\dot m_{fuel}/dt)_{max} 
+    \end{array}
+  \right.
+\end{equation}
+
+\begin{equation}
+{\dot m_{air}} = f({P_{net,ss}})
+\end{equation}
+
+\begin{equation}
+P_{net}^{t+\Delta t} = \left\{
+    \begin{array}{cl}
+      P_{net,ss}^{t+\Delta t}                   & \text{if} dP_{net} / dt \le (dP_{net}/dt)_{max} \\
+      P_{net,ss}^t \pm (dP_{net}/dt)_{max}      & \text{if} dP_{net} / dt > (dP_{net}/dt)_{max} 
+    \end{array}
+  \right.
+\end{equation}
+
+\begin{equation}
+{[MC]_{eng}}\frac{{d{T_{eng}}}}{{dt}} = U{A_{HX}}\left( {{T_{cw,p}} - {T_{eng}}} \right) + U{A_{loss}}\left( {{T_{room}} - {T_{eng}}} \right) + {q_{gen,ss}}
+\end{equation}
+
+\begin{equation}
+{[MC]_{cw}}\frac{{d{T_{cw,o}}}}{{dt}} = {[\dot m{c_p}]_{cw}}\left( {{T_{cw,i}} - {T_{cw,o}}} \right) + U{A_{HX}}\left( {{T_{eng}} - {T_{cw,o}}} \right)
+\end{equation}
+
+where,
+
+\({\eta_e}\) ~is the steady-state, part load, electrical conversion efficiency of the engine (-)
+
+\({\eta_q}\) ~is the steady-state part load, thermal conversion efficiency of the engine (-)
+
+\({\dot m_{cw}}\) ~is the mass flow rate of plant fluid through the heat recovery section {[}kg/s{]}
+
+\({T_{cw,i}}\) ~is the bulk temperature of the plant fluid entering the heat recovery section (\(^{o}\)C)
+
+\({T_{cw,o}}\) ~is the bulk temperature of the plant fluid leaving the heat recovery section (\(^{o}\)C)
+
+\({P_{net,ss}}\) is the steady-state electrical output of the system (W),
+
+\({q_{gross}}\) ~is the gross heat input into the engine (W),
+
+\({q_{gen,ss}}\) ~is the steady-state rate of heat generation within the engine (W)
+
+\(LH{V_{fuel}}\) ~is the lower heating value of the fuel used by the system (J/kg or J/kmol),
+
+\({\dot N_{fuel}}\) ~is the molar fuel flow rate (kmol/s)
+
+\({\dot m_{fuel}}\) ~is the mass fuel flow rate (kg/s)
+
+\({\dot m_{air}}\) ~is the mass flow rate of air thru the engine (kg/s)
+
+\({[MC]_{eng}}\) ~is the thermal capacitance of the engine control volume (W/K)
+
+\({T_{eng}}\) ~is the temperature of the engine control volume (C)
+
+\(U{A_{HX}}\) is the effective thermal conductance between the engine control volume and the cooling water control volume (W/K).
+
+\(U{A_{loss}}\) ~is the effective thermal conductance between the engine control volume and the surrounding environment (W/K)
+
+\({T_{room}}\) ~is the air temperature of the surrounding environment (C)
+
+\({[MC]_{cw}}\) ~is the thermal capacitance of the encapsulated cooling water and heat exchanger shell in immediate thermal contact (J/K)
+
+\({[\dot m{c_p}]_{cw}}\) ~is the thermal capacity flow rate associated with the cooling water (W/K)
+
+The functional forms for \({\eta_e}\) ~and \({\eta_q}\) ~are 2\(^{nd}\) order trivariate polynomials with all of the cross terms.
+
+EnergyPlus solves these for state values for the engine mass temperature, \({T_{eng}}\) , and the outlet plant node, \({T_{cw,o}}\) , in the following manner. The last two equations are interrelated but otherwise ordinary differential equations with the general form
+
+\begin{equation}
+\frac{{dT}}{{dt}} = a + bT
+\end{equation}
+
+and have analytical solution
+
+\begin{equation}
+T = \left( {{T_o} + {\raise0.7ex\hbox{a} \!\mathord{\left/ {\vphantom {a b}}\right.}\!\lower0.7ex\hbox{b}}} \right){e^{bt}} - {\raise0.7ex\hbox{a} \!\mathord{\left/ {\vphantom {a b}}\right.}\!\lower0.7ex\hbox{b}}
+\end{equation}
+
+The engine temperature at the current timestep is calculated using
+
+\begin{equation}
+a = \frac{{U{A_{HX}}}}{{{{[MC]}_{eng}}}}*{T_{cw,o}} + \frac{{U{A_{loss}}}}{{{{[MC]}_{eng}}}}*{T_{room}} + \frac{{{q_{gen,ss}}}}{{{{[MC]}_{eng}}}}
+\end{equation}
+
+\begin{equation}
+b =  - \left( {\frac{{U{A_{HX}}}}{{{{[MC]}_{eng}}}} + \frac{{U{A_{loss}}}}{{{{[MC]}_{eng}}}}} \right)
+\end{equation}
+
+The plant node outlet fluid temperature (heat recovered) is solved using
+
+\begin{equation}
+a = \frac{{{{[\dot m{c_p}]}_{cw}}}}{{{{[MC]}_{cw}}}}*{T_{cw,i}} + \frac{{U{A_{HX}}}}{{{{[MC]}_{cw}}}}*{T_{eng}}
+\end{equation}
+
+\begin{equation}
+b =  - \left( {\frac{{{{[\dot m{c_p}]}_{cw}}}}{{{{[MC]}_{cw}}}} + \frac{{U{A_{HX}}}}{{{{[MC]}_{cw}}}}} \right)
+\end{equation}
+
+The interrelation of these two is handled by sequential substitution using an iteration scheme that alternates between calculations of \({T_{eng}}\) ~and \({T_{cw,o}}\) .~ The iteration loop exits once the energy is determined to be balanced using the following criteria:
+
+Number of iterations \textgreater{} 3\textbackslash{}
+
+\begin{equation}
+\frac{{{{\left( {{q_{gen,ss}}} \right)}_{\max }}}}{{10000000}} > U{A_{HX}}\left( {{T_{cw,o}} - {T_{eng}}} \right) + U{A_{loss}}\left( {{T_{room}} - {T_{eng}}} \right) + {q_{gen,ss}} - {[MC]_{eng}}\frac{{d{T_{eng}}}}{{dt}}
+\end{equation}
+
+\begin{equation}
+\frac{{{{\left( {{q_{gen,ss}}} \right)}_{\max }}}}{{10000000}} > {[\dot m{c_p}]_{cw}}\left( {{T_{cw,i}} - {T_{cw,o}}} \right) + U{A_{HX}}\left( {{T_{eng}} - {T_{cw,o}}} \right) - {[MC]_{cw}}\frac{{d{T_{cw,o}}}}{{dt}}
+\end{equation}
+
+The Micro CHP model has a number of different operating modes.~ The operating mode for a given system timestep is determined from the mode during the previous timestep, user inputs, and high-level controls from elsewhere in EnergyPlus.~ The operating mode is reported for the state at the end of each timestep.~ The following table summarizes the various operating modes and the criteria for switching to a new mode for any given timestep.~ The EnergyPlus implementation adds the ``Off'' mode to the modes specified by Annex 42 which corresponds to the unit being scheduled to be unavailable.~ The difference between OFF and Standby modes determines whether or not standby power is consumed.
+
+{\scriptsize
+\begin{longtable}[c]{p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}}
+\toprule 
+Constituent & A & B & C & D & E & F & H & Source \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Constituent & A & B & C & D & E & F & H & Source \tabularnewline
+\midrule
+\endhead
+
+N\(_{2}\) & 26.092 & 8.218801 & -1.976141 & 0.159274 & 0.044434 & -7.98923 & 0.0 & NIST \tabularnewline
+O\(_{2}\) & 29.659 & 6.137261 & -1.186521 & 0.09578 & -0.219663 & -9.861391 & 0.0 & NIST \tabularnewline
+Ar & 20.786 & 2.8259E-7 & -1.4642E-7 & 1.0921E-8 & -3.6614E-8 & -6.19735 & 0.0 & NIST \tabularnewline
+CO\(_{2}\) & 24.99735 & 55.18696 & -33.69137 & 7.948387 & -0.136638 & -403.6075 & -393.5224 & NIST \tabularnewline
+H\(_{2}\)O(gas) & 29.0373 & 10.2573 & 2.81048 & -0.95914 & 0.11725 & -250.569 & -241.8264 & CHEMKIN \tabularnewline
+H\(_{2}\)O(liq) & -203.606 & 1523.29 & -3196.413 & 2474.455 & 3.85533 & -256.5478 & -285.8304 & NIST \tabularnewline
+H\(_{2}\) & 33.066178 & -11.363417 & 11.432816 & -2.772874 & -0.158558 & -9.9808 & 0.0 & NIST \tabularnewline
+CH\(_{4}\) & -0.703029 & 108.4773 & -42.52157 & 5.862788 & 0.678565 & -76.84376 & -74.8731 & NIST \tabularnewline
+C\(_{2}\)H\(_{6}\) & -3.03849 & 199.202 & -84.9812 & 11.0348 & 0.30348 & -90.0633 & -83.8605 & CHEMKIN \tabularnewline
+C\(_{3}\)H\(_{8}\) & -23.1747 & 363.742 & -222.981 & 56.253 & 0.61164 & -109.206 & -103.855 & CHEMKIN \tabularnewline
+C\(_{4}\)H\(_{10}\) & -5.24343 & 426.442 & -257.955 & 66.535 & -0.26994 & -149.365 & -133.218 & CHEMKIN \tabularnewline
+C\(_{5}\)H\(_{12}\) & -34.9431 & 576.777 & -338.353 & 76.8232 & 1.00948 & -155.348 & -146.348 & CHEMKIN \tabularnewline
+C\(_{6}\)H\(_{14}\) & -46.7786 & 711.187 & -438.39 & 103.784 & 1.23887 & -176.813 & -166.966 & CHEMKIN \tabularnewline
+CH\(_{3}\)OH & 14.1952 & 97.7218 & -9.73279 & -12.8461 & 0.15819 & -209.037 & -201.102 & CHEMKIN \tabularnewline
+C\(_{2}\)H\(_{5}\)OH & -8.87256 & 282.389 & -178.85 & 46.3528 & 0.48364 & -241.239 & -234.441 & CHEMKIN \tabularnewline
+\bottomrule
+\end{longtable}}
+
+For timesteps where the generator switches from warm up mode to normal mode in the middle of the timestep, part load ration values are calculated for the portion of the time step that the generator is in normal operation.
+
+The engine and heat recovery thermal conditions are modeled for all modes so, for example, an engine that is off but still warm could provide some hot water recovery.
+
+The engine model can use an arbitray fuel mixture that is defined by the user -- see the entry for Generator:FuelSupply.
+
+\subsubsection{References}\label{references-024}
+
+Kelly, N. and A. Ferguson. 2007. A Generic Model Specification for Combustion-based Residential Cogeneration Devices. In \emph{Specifications for Modelling Fuel Cell and Combustion-Based Residential Cogeneration Device within Whole-Building Simulation Programs}. I. Beausoleil-Morrison and N. Kelly editors.~ Draft report of Annex 42 of the International Energy Agency ECBCS.
+
+\subsection{Fuel Cell Cogenerator}\label{fuel-cell-cogenerator}
+
+The Generator:FuelCell input objects provides a model which is a direct implementation of a model developed by IEA Annex 42 -- The Simulation of Building-Integrated Fuel Cell and Other Cogeneration Systems (FC+COGEN-SIM).~ Annex 42 was formed as a working group within the International Energy Agency (IEA) program on Energy Conservation in Buildings and Community Systems (ECBCS).~ A full description of the model specification can be found in the report by Subtask B of FC+COGEN-SIM with the title ``Specifications for Modelling Fuel Cell and Combustion-Based Residential Cogeneration Device within Whole-Building Simulation Programs.''~ The ``Specifications for Modelling Fuel Cell Cogeneration Devices within Whole-Building Simulation Programs.''
+
+The Annex 42 Fuel Cell model is characterized as a ``grey box'' empirical model where a mixture of thermodynamic principles and empirical performance maps are used to model the cogeneration performance of a fairly complex device with many individual subsystems.~ In EnergyPlus, the individual subsystems are separate into individual input objects such as Generator:FuelCell:PowerModule or Generator:FuelCell:ExhaustGasToWaterHeatExchanger. The resulting model is relatively complex requiring on the order of one hundred inputs.~ The model is not for the faint of heart; this model is far more involved than most component models in building simulation.~ This stems from the fact that fuel cell cogenerators are complicated devices that interact with the built environment in a number of ways.~ Fuel cells could drawn in gas/fuel, air, and water with as many as six separate streams.~ In addition to electricity and heated water, they also give off heat in the form of convection and radiation and exhaust air out of the zone.~ The devices may take a long time to start up and include storage to follow loads rather than attempt to vary the power the fuel cell.~ The fuel cell model allows examining system level interactions over annual timeframes that include all the important interactions with a building's energy and comfort systems.
+
+The Annex 42 fuel cell model is described more thoroughly in the references (see below).~ Here we provide a summary of the relevant model equations which are taken from the Annex 42 model specification.~ The first equation is the main energy balance for the fuel cell power module (includes the fuel reformation and fuel cell stacks).~ This energy balance is used to model the enthalpy of the product gases that leave the fuel cell power module.
+
+\begin{equation}
+  \begin{array}{l}
+    {\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\hat h}_i} - {\Delta_f}\hat h_i^o} \right]} \right)}_{fuel}} + {\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\hat h}_i} - {\Delta_f}\hat h_i^o} \right]} \right)}_{air}} + {{\dot N}_{liq - water}} \cdot \left( {{{\left[ {\hat h - {\Delta_f}{{\hat h}^o}} \right]}_{{H_2}O,liq}} - {\Delta_f}\hat h_{{H_2}O,fg}^o} \right) \\
+    \quad \quad  + {{\dot H}_{dilution - air - in}} + {{\dot N}_{fuel}} \cdot LH{V_{fuel}} + {P_{el,ancillaries - AC}} \\
+    = {P_{el}} + {\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\ddot h}_i} - {\Delta_f}\hat h_i^o} \right]} \right)}_{FCPM - cg}} + {q_{s - cool}} + {q_{skin - loss}} + {{\dot H}_{dilution - air - out}}
+  \end{array}
+\end{equation}
+
+The remaining equations describe various terms and the balance of systems.~ The electrical efficiency is modeled using:
+
+\begin{equation}
+{\varepsilon_{el}} = \left[ {{\varepsilon_0} + {\varepsilon_1} \cdot {P_{el}} + {\varepsilon_2} \cdot P_{el}^2} \right] \cdot \left[ {1 - {N_{stops}} \cdot D} \right] \cdot \left[ {1 - (MAX(\int\limits_{} {dt - {t_{threshold}},0.0))}  \cdot L} \right]
+\end{equation}
+
+\begin{equation}
+{P_{blower - el}} = {b_0} + {b_1} \cdot {\dot N_{air}} + {b_2} \cdot \dot N_{air}^2 + {b_3} \cdot \dot N_{air}^3
+\end{equation}
+
+In several places the model is formulated to offer different options.~ For example, the flow rate of process air can be described either as a function of electrical power produced or the fuel flow rate.
+
+\begin{equation}
+{\dot N_{air}} = \left[ {{a_0} + {a_1} \cdot {P_{el}} + {a_2} \cdot P_{el}^2} \right].\left[ {1 + {a_3} \cdot {T_{air}}} \right]
+\end{equation}
+
+or
+
+\begin{equation}
+{\dot N_{air}} = \left[ {{a_0} + {a_1} \cdot {{\dot N}_{fuel}} + {a_2} \cdot \dot N_{fuel}^2} \right].\left[ {1 + {a_3} \cdot {T_{air}}} \right]
+\end{equation}
+
+\begin{equation}
+{\dot N_{liq - water}} = {w_0} + {w_1} \cdot {\dot N_{fuel}} + {w_2} \cdot \dot N_{fuel}^2
+\end{equation}
+
+\begin{equation}
+{P_{pump - el}} = {p_0} + {p_1} \cdot {\dot N_{water}} + {p_2} \cdot \dot N_{water}^2 + {p_3} \cdot \dot N_{water}^3
+\end{equation}
+
+\begin{equation}
+{P_{comp - el}} = {c_0} + {c_1} \cdot {\dot N_{fuel}} + {c_2} \cdot \dot N_{fuel}^2 + {c_3} \cdot \dot N_{fuel}^3
+\end{equation}
+
+\begin{equation}
+{P_{el,ancillaries - AC}} = an{c_0} + an{c_1} \cdot {\dot N_{fuel}}
+\end{equation}
+
+\begin{equation}
+{P_{el,aux - ancillaries}} = {x_0} + {x_1} \cdot {\dot N_{aux - fuel}}
+\end{equation}
+
+\begin{equation}
+{q_{HX}} = {\varepsilon_{HX}} \cdot {\left( {\dot N{{\hat c}_p}} \right)_{\min }} \cdot \left( {{T_{aux - mix}} - {T_{water,in}}} \right)
+\end{equation}
+
+\begin{equation}
+{q_{HX}} = {\left( {UA} \right)_{eff}} \cdot \frac{{\left( {{T_{aux - mix}} - {T_{water,out}}} \right) - \left( {{T_{HX - exh}} - {T_{water,in}}} \right)}}{{\ln \left( {\frac{{{T_{aux - mix}} - {T_{water,out}}}}{{{T_{HX - exh}} - {T_{water,in}}}}} \right)}}
+\end{equation}
+
+\begin{equation}
+{\left( {UA} \right)_{eff}} = h{x_{s,0}} + h{x_{s,1}} \cdot {\dot N_{water}} + h{x_{s,2}} \cdot \dot N_{water}^2 + h{x_{s,3}} \cdot {\dot N_{aux - mix}} + h{x_{s,4}} \cdot \dot N_{aux - mix}^2
+\end{equation}
+
+or
+
+\begin{equation}
+{\left( {UA} \right)_{eff}} = {\left[ {\frac{1}{{{{\left( {hA} \right)}_{gas}}}} + \frac{1}{{{{(hA)}_{water}}}} + {F_{HX}}} \right]^{ - 1}}
+\end{equation}
+
+where,
+
+\(F_{HX}\) is an adjustment factor,
+
+\begin{equation}
+h_{gas} = h_{gas}^0 \left( \frac{\dot{N}_{gas}}{\dot{N}_{gas}^0} \right)^n
+\end{equation}
+
+\begin{equation}
+{h_{water}} = h_{water}^0 \cdot {\left( {\frac{{{{\dot N}_{water}}}}{{\dot N_{water}^0}}} \right)^m}
+\end{equation}
+
+\begin{equation}
+{q_{HX}} = {\left( {UA} \right)_{eff}} \cdot \frac{{\left( {{T_{aux - mix}} - {T_{water,out}}} \right) - \left( {{T_{HX - exh}} - {T_{water,in}}} \right)}}{{\ln \left( {\frac{{{T_{aux - mix}} - {T_{water,out}}}}{{{T_{HX - exh}} - {T_{water,in}}}}} \right)}} + {\dot N_{{H_2}O - cond}} \cdot {\hat h_{fg}}
+\end{equation}
+
+\begin{equation}
+{\dot N_{{H_2}O - cond}} = \left( {{T_{cond - threshold}} - {T_{water,in}}} \right) \cdot \left[ {h{x_{l,1}} \cdot \left( {\frac{{{{\dot N}_{{H_2}O}}}}{{{{\dot N}_{aux - mix}}}}} \right) + h{x_{l,2}} \cdot {{\left( {\frac{{{{\dot N}_{{H_2}O}}}}{{{{\dot N}_{aux - mix}}}}} \right)}^2}} \right]
+\end{equation}
+
+\begin{equation}
+{q_{aux - skin - losses}} = {(UA)_{aux}} \cdot ({T_{aux - mix}} - {T_{room}})
+\end{equation}
+
+\begin{equation}
+{q_{skin - loss}} = {s_0} + {s_1} \cdot {\dot N_{fuel}} + {s_2} \cdot \dot N_{fuel}^2
+\end{equation}
+
+\begin{equation}
+Q_{battery}^{t + \Delta t} = Q_{battery}^t + {P_{battery - charge}} \cdot {\varepsilon_{charge}} \cdot \Delta t
+\end{equation}
+
+\begin{equation}
+{\eta_{PCU}} = {u_0} + {u_1} \cdot {P_{PCU - in}} + {u_2} \cdot P_{PCU - in}^2
+\end{equation}
+
+\begin{equation}
+{q_{s - cool}} = \left[ {{r_0} + {r_1}\left( {{T_{stack}} - T_{stack}^o} \right)} \right] \cdot \left[ {1 + {r_2}{P_{el}} + {r_3}P_{el}^2} \right]
+\end{equation}
+
+\begin{equation}
+{\left( {UA} \right)_{s - cogen}} = {\left[ {\frac{1}{{{{\left( {hA} \right)}_{s - cogen}}}} + {F_{s - cogen}}} \right]^{ - 1}}
+\end{equation}
+
+\begin{equation}
+{h_{s - cogen}} = h_{s - cogen}^0 \cdot {\left( {\frac{{{{\dot N}_{s - cogen}}}}{{\dot N_{s - cogen}^0}}} \right)^{{n_s}}}
+\end{equation}
+
+\begin{equation}
+{P_{s - air - el}} = {f_0} + {f_1} \cdot {q_{s - air}} + {f_2} \cdot q_{s - air}^2
+\end{equation}
+
+The Annex 42 fuel cell was implemented directly in EnergyPlus.~ A sequential substitution method is used to handle all the interactions between the different subsystems.~ The main energy balance drawn for the fuel cell power module is rearranged to put all the terms on the right hand side.~ The enthalpy of the product gas stream is determined from this energy balance.~ The Shomate equation is used to evaluate the enthalpy and specific heat of the various streams.~ The EnergyPlus implementation evaluates fluid properties using the average temperature of inlet and outlet streams whereas the Annex 42 specification often uses just the inlet temperature.~ The Shomate equation is inverted using the regula falsi numerical method available within EnergyPlus to calculate the temperature of the product gases from their enthalpy.
+
+\subsubsection{References}\label{references-1-009}
+
+Beausoleil-Morrison, I., A. Schatz, and F. Marechal. 2006. A model for simulating the thermal and electrical production of small-scale solid-oxide fuel cell cogeneration systems within building simulation programs.~ \emph{HVAC \& R Research}. Amer. Soc. Heating, Ref. Air-Conditioning Eng. Inc. Atlanta, GA.
+
+Beausoleil-Morrison, I., A. Weber, F. Marechal, and B. Griffith. 2007. Specifications for Modelling Fuel Cell Cogeneration Devices within Whole-Building Simulation Programs. In \emph{Specifications for Modelling Fuel Cell and Combustion-Based Residential Cogeneration Device within Whole-Building Simulation Programs}. I. Beausoleil-Morrison and N. Kelly editors.~ \textbf{Draft} report of Annex 42 of the International Energy Agency ECBCS.
+
+\subsection{Custom Fuel Supply for Generators}\label{custom-fuel-supply-for-generators}
+
+The Generator:FuelSupply input object in EnergyPlus implements a fairly comprehensive capability to calculate properties of fuel mixtures from a description of the molar composition of all the constituents.~ The fuel supply modeling is based on the specifications prepared by IEA Annex 42 for their generator models.~ This modeling capability allows taking into consideration the exact gas composition of local natural gas service.~ Or the user can explore the implications of an various alternative fuels such as alcohols or biogas.~ An unlimited number of possible mixtures can be analyzed.
+
+Gas phase thermochemistry calculations and data are programmed into EnergyPlus to handle the set of constituents listed in the table below.~ The relevant properties of each fuel constituent, \emph{i}, are calculated as a function of temperature using the Shomate equation:
+
+\begin{equation}
+{\hat h_i} - {\Delta_f}\hat h_i^o = A \cdot \left( {\frac{T}{{1000}}} \right) + \frac{B}{2} \cdot {\left( {\frac{T}{{1000}}} \right)^2} + \frac{C}{3} \cdot {\left( {\frac{T}{{1000}}} \right)^3} + \frac{D}{4} \cdot {\left( {\frac{T}{{1000}}} \right)^4} - \frac{E}{{\left( {\frac{T}{{1000}}} \right)}} + F - H
+\end{equation}
+
+where,
+
+\({\hat h_i}\) ~is the enthalpy (J/kmol)
+
+\({\Delta_f}\hat h_i^o\) ~is the molar enthalpy at the standard state (J/kmol)
+
+\(T\) ~is the temperature of the gas (K)
+
+A, B, C, D, E, F, H are the coefficients for the Shomate equation.
+
+The lower heating value (LHV) of a fuel mixture is calculated from the molar fractions using:
+
+\begin{equation}
+LH{V_{fuel}} = \sum\limits_i {\left( {{\chi_i} \cdot LH{V_i}} \right)}
+\end{equation}
+
+Where,
+
+\begin{equation}
+LH{V_i} = \left[ {{\Delta_f}\hat h_{{C_x}{H_y}}^o - x \cdot {\Delta_f}\hat h_{C{O_2}}^o - \frac{y}{2} \cdot {\Delta_f}\hat h_{{H_2}O}^o} \right]
+\end{equation}
+
+\emph{x} is the number of carbon atoms
+
+\emph{y} is the number of hydrogen atoms
+
+Similarly, the higher heating value (HHV) of the fuel mixture is calculated using:
+
+\begin{equation}
+HH{V_{fuel}} = \sum\limits_i {\left( {{\chi_i} \cdot HH{V_i}} \right)}
+\end{equation}
+
+Where,
+
+\begin{equation}
+HH{V_i} = \left[ {{\Delta_f}\hat h_{{C_x}{H_y}}^o - x \cdot {\Delta_f}\hat h_{C{O_2}}^o - \frac{y}{2} \cdot {\Delta_f}\hat h_{{H_2}O}^o + \frac{y}{2} \cdot \left( {{\Delta_f}\hat h_{{H_2}O}^o - {H_{liq}}} \right)} \right]
+\end{equation}
+
+The Shomate coefficients used in EnergyPlus are listed in the table below.~ Data source ``NIST'' indicates the data were directly from Chemistry WebBook.~ Data source ``CHEMKIN'' indicates the data were developed by curve fitting library data for the CHEMKIN commercial program (which uses the Gorden-McBride polynomial rather than the Shomate formulation).
+
+{\scriptsize
+\begin{longtable}[c]{p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}}
+\toprule 
+Constituent & A & B & C & D & E & F & H & Source \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Constituent & A & B & C & D & E & F & H & Source \tabularnewline
+\midrule
+\endhead
+
+N\(_{2}\) & 26.092 & 8.218801 & -1.976141 & 0.159274 & 0.044434 & -7.98923 & 0.0 & NIST \tabularnewline
+O\(_{2}\) & 29.659 & 6.137261 & -1.186521 & 0.09578 & -0.219663 & -9.861391 & 0.0 & NIST \tabularnewline
+Ar & 20.786 & 2.8259E-7 & -1.4642E-7 & 1.0921E-8 & -3.6614E-8 & -6.19735 & 0.0 & NIST \tabularnewline
+CO\(_{2}\) & 24.99735 & 55.18696 & -33.69137 & 7.948387 & -0.136638 & -403.6075 & -393.5224 & NIST \tabularnewline
+H\(_{2}\)O(gas) & 29.0373 & 10.2573 & 2.81048 & -0.95914 & 0.11725 & -250.569 & -241.8264 & CHEMKIN \tabularnewline
+H\(_{2}\)O(liq) & -203.606 & 1523.29 & -3196.413 & 2474.455 & 3.85533 & -256.5478 & -285.8304 & NIST \tabularnewline
+H\(_{2}\) & 33.066178 & -11.363417 & 11.432816 & -2.772874 & -0.158558 & -9.9808 & 0.0 & NIST \tabularnewline
+CH\(_{4}\) & -0.703029 & 108.4773 & -42.52157 & 5.862788 & 0.678565 & -76.84376 & -74.8731 & NIST \tabularnewline
+C\(_{2}\)H\(_{6}\) & -3.03849 & 199.202 & -84.9812 & 11.0348 & 0.30348 & -90.0633 & -83.8605 & CHEMKIN \tabularnewline
+C\(_{3}\)H\(_{8}\) & -23.1747 & 363.742 & -222.981 & 56.253 & 0.61164 & -109.206 & -103.855 & CHEMKIN \tabularnewline
+C\(_{4}\)H\(_{10}\) & -5.24343 & 426.442 & -257.955 & 66.535 & -0.26994 & -149.365 & -133.218 & CHEMKIN \tabularnewline
+C\(_{5}\)H\(_{12}\) & -34.9431 & 576.777 & -338.353 & 76.8232 & 1.00948 & -155.348 & -146.348 & CHEMKIN \tabularnewline
+C\(_{6}\)H\(_{14}\) & -46.7786 & 711.187 & -438.39 & 103.784 & 1.23887 & -176.813 & -166.966 & CHEMKIN \tabularnewline
+CH\(_{3}\)OH & 14.1952 & 97.7218 & -9.73279 & -12.8461 & 0.15819 & -209.037 & -201.102 & CHEMKIN \tabularnewline
+C\(_{2}\)H\(_{5}\)OH & -8.87256 & 282.389 & -178.85 & 46.3528 & 0.48364 & -241.239 & -234.441 & CHEMKIN \tabularnewline
+\bottomrule
+\end{longtable}}
+
+\subsubsection{References}\label{references-2-005}
+
+Beausoleil-Morrison, I., A. Weber, F. Marechal, and B. Griffith. 2007. Specifications for Modelling Fuel Cell Cogeneration Devices within Whole-Building Simulation Programs. In \emph{Specifications for Modelling Fuel Cell and Combustion-Based Residential Cogeneration Device within Whole-Building Simulation Programs}. I. Beausoleil-Morrison and N. Kelly editors.~ Report of Annex 42 of the International Energy Agency ECBCS.
+
+NIST. 2003. Chemistry WebBook, National Institute of Standards and Technology Standard Reference Database Number 69, March 2003 Release, .
+
+Gordon S. and B.J. McBride. 1971. Computer program for calculation of complex chemical equilibrium composition, rocket performance, incident and reflected shocks and Chapman-Jouguet detonations.~ NASA SP-273.
+
+\subsection{Wind Turbine}\label{wind-turbine}
+
+\subsubsection{Overview}\label{overview-017}
+
+The wind turbine (object Generator:WindTurbine) model is intended to estimate the production of electric power of both horizontal and vertical axis wind turbine systems. Due to the cubic relationship between the wind speed and the power produced by a wind turbine, the performance of these systems is highly dependent on local wind conditions. However, differences between typical meteorological year (TMY) wind data attached to the simulation and local wind data at the site where wind turbine system is installed typically appear. The model thus estimates the air density and wind speed at the particular height of the system and factors differences between the wind speed from the TMY weather data and the local wind speed. The weather data file should thus be included in the simulation. The model also requires inputs of both an annual average wind speed that represents accurate wind profile at the location and the height where this annual average wind speed was determined.
+
+The model calculates the power production by both horizontal axis wind turbines (HAWT) and vertical axis wind turbines (VAWT) from generic mathematical equations. Currently, a variable speed control scheme is available in EnergyPlus. The model assumes constant power generation at the rated power and the rated wind speed when the ambient wind speed is between the rated wind speed and cut out wind speed. The model does not attempt to model various types of subsystems of the entire wind turbine system such as shafts, generators and inverters due to computational convergence, time, and usability. Instead, the total system efficiency includes both conversion losses occurring during the DC-AC-DC conversion processes and delivery losses.
+
+\subsubsection{Model Description}\label{model-description-010}
+
+The wind turbine is modeled as a generation component that produces electricity and delivers it directly to buildings. Wind turbine components are executed at the beginning of each time step called by the HVAC manager, and the electric load will be corrected with electricity from the wind turbine. The model calculates electricity production that both HAWTs and VAWTs produce from general mathematical equations. The model then passes the electricity to the electric load center in EnergyPlus at each HVAC system time step. The electric load center then determines the whole building electrical demand, deducting the power output by wind turbine along with any power production by photovoltaic components from the total electrical demand requested in the building. Excessive production of electricity greater than needed from wind turbine along with photovoltaic components is either sold or stored as the user specifies.
+
+\subsubsection{Input and Data}\label{input-and-data}
+
+The user must input the required information according to the IO Reference Manual (ref: Generator:WindTurbine). The wind turbine model in EnergyPlus requires a unique identifying name and an availability schedule. The schedule name must refer to a valid schedule type (range 0-1) and contain values of fractional operation. Various inputs describes wind turbine configuration such as rotor type, control type, rotor diameter, overall height, and number of blades. Rated data provided in the manufacturer's literature determines overall electricity production by using generic equations. These inputs include rated power, rated wind speed, cut in wind speed, cut out wind speed, fraction system efficiency, and maximum tip speed ratio. Two inputs such as annual local average wind speed and height for local average wind speed define local wind conditions at a specific location so that the model predicts wind speed and air density at the height of the wind turbine at the location.
+
+HAWT systems need a maximum power coefficient and empirical power coefficient parameters \emph{C\(_{1}\)} through \emph{C\(_{6}\)}. The maximum power coefficient controls overall performance of the rotor which defines the power extraction efficiency from the ambient air stream. The model predicts power generation more accurately when the user inputs the empirical power coefficients \emph{C\(_{1}\)} through \emph{C\(_{6}\)} for a specific wind turbine. Three additional inputs for VAWT system are required. The model requests blade lift and drag coefficients corresponding to the maximum tip speed ratio so that tangential and normal force coefficients are obtained. Blade chord area is also requested for calculating forces on a single blade.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-003}
+
+Given the inputs needed, the wind turbine model analyzes local wind speed since wind speed is critical to determine the production of electricity of wind turbine systems. To minimize uncertainty involved with wind data, it factors differences between annual average wind speed from weather data and local annual average wind speed at the particular height of the local meteorological station. It reads annual average wind speed from statistical weather file that is automatically copied during the simulation. Note that the user should attach a weather data to the simulation (for a design day simulation, the wind speed data from the design day description is used). This annual average wind speed is converted into a wind speed at the height at which local annual average wind speed that the user inputs is measured and then factored as:
+
+\begin{equation}
+{V_{LocalTMY}} = {V_{AnnualAvg}}{\left( {\frac{{{\delta_{met}}}}{{{H_{met}}}}} \right)^{{a_{met}}}}{\left( {\frac{H}{\delta }} \right)^a}
+\end{equation}
+
+\begin{equation}
+{F_V} = \frac{{{V_{LocalTMY}}}}{{{V_{Local}}}}
+\end{equation}
+
+Note that the wind speed factor \emph{F\(_{v}\)} of 1.0 is assigned, if the user does not input the local wind conditions or the weather data file is not attached to the simulation.
+
+The local air density can be obtained by using EnergyPlus psychrometric functions as follows:
+
+\begin{equation}
+{T_{Local}} = OutDryBulbTempAt(Z)
+\end{equation}
+
+\begin{equation}
+{P_{Local}} = OutBaro\Pr essAt(Z)
+\end{equation}
+
+\begin{equation}
+{\omega_{Local}} = PsyWFnTdbTwbPb({T_{Local}},{T_{wb}},{P_{Local}})
+\end{equation}
+
+\begin{equation}
+{\rho_{Local}} = PsyRhoAirFnPbTdbW({P_{Local}},{T_{Local}},{\omega_{initial}})
+\end{equation}
+
+The model converts TMY wind speed into a wind speed at the specific height of the wind turbine rotor (\emph{V\(_{z}\)}) at the location by using EnergyPlus function as:
+
+\begin{equation}
+{V_Z} = WindSpeedAt(Z)
+\end{equation}
+
+The local wind speed at the rotor height (\emph{V\(_{Local}\)}) at the location is thus:
+
+\begin{equation}
+{V_{Local}} = \frac{{{V_Z}}}{{{F_v}}}
+\end{equation}
+
+The tip speed ratio (TSR) can be obtained as:
+
+\begin{equation}
+\lambda  = \frac{{\omega R}}{{{V_{Local}}}}
+\end{equation}
+
+\subsubsection{Horizontal Axis Wind Turbine}\label{horizontal-axis-wind-turbine}
+
+Once the local wind speed and air density are determined, the model calculates electrical power produced by a wind turbine system according to the rotor type. For HAWT systems, two different approximations are available. The model uses an analytical approximation when the user inputs all six empirical coefficient parameters \emph{C\(_{1}\)} through \emph{C\(_{6}\)}. The equations that define the analytical approximation are:
+
+\begin{equation}
+{C_p} = {C_1}(\frac{{{C_2}}}{{{\lambda_i}}} - {C_3}\theta  - {C_4}{\theta ^x} - {C_5}){e^{ - \frac{{{C_6}(\lambda ,\theta )}}{{{\lambda_i}}}}}
+\end{equation}
+
+\begin{equation}
+\frac{1}{{{\lambda_i}}} = \frac{1}{{\lambda  + 0.08\theta }} - \frac{{0.035}}{{{\theta ^3} + 1}}
+\end{equation}
+
+Note that the model allows changing the rotor speed to meet the maximum tip speed ratio at each time step. That is, the tip speed ratio calculated is limited by the maximum tip speed ratio. Similarly, the power coefficient calculated is also set to the maximum if the calculated is greater than the maximum.
+
+Assuming maximum of rotor angle, i.e.~zero, the power production of the wind turbine is thus obtained by:
+
+\begin{equation}
+{P_W} = \frac{1}{2}{\rho_{Local}}{A_R}V_{_{Local}}^3{C_p}(\lambda ,\theta )
+\end{equation}
+
+The model assumes the simple approximation, if any of empirical power coefficient parameters is not input. The power production of wind turbine is directly obtained from the kinetic energy equation:
+
+\begin{equation}
+{P_W} = \frac{1}{2}{\rho_{Local}}{A_R}V_{_{Local}}^3{C_{p,\max }}(\lambda ,\theta )
+\end{equation}
+
+Here, the model defines \emph{P\(_{W}\)} as rated power output at the rated wind speed, if either the power production of wind turbine or local wind speed is greater than the rated power or rated wind speed, respectively. The power coefficient in this particular case is thus recalculated as:
+
+\begin{equation}
+{C_p} = \frac{{{P_W}}}{{0.5{\rho_{Local}}AV_{_{Local}}^3}}
+\end{equation}
+
+The overall power production that includes conversion loss and delivery loss is thus:
+
+\begin{equation}
+P = \eta {P_W}
+\end{equation}
+
+\subsubsection{Vertical Axis Wind Turbine}\label{vertical-axis-wind-turbine}
+
+\begin{figure}[hbtp] % fig 340
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7837.png}
+\caption{Flow velocities and force diagram of a single blade airfoil (Adapted from Mazharul Islam et al., 2008) \protect \label{fig:flow-velocities-and-force-diagram-of-a-single}}
+\end{figure}
+
+If tip speed ratio at the time step is greater than the maximum tip speed ratio, the model estimates actual rotor speed at the time step as:
+
+\begin{equation}
+\omega R = \lambda {V_{Local}}
+\end{equation}
+
+The model then employs general mathematical expressions for the aerodynamic analysis of straight-bladed Darrieus-type VAWTs to predict the power production by VAWTs. Assuming quasi-steady state, the induced wind speed (\emph{V\(_{a}\)}) on the rotor is defined as:
+
+\begin{equation}
+{V_a} = \frac{2}{3}{V_{Local}}
+\end{equation}
+
+The chordal velocity (\emph{V\(_{c}\)}), normal velocity (\emph{V\(_{n}\)}), and relative flow velocity (\emph{W}) as shown in figure above can be expressed as:
+
+\begin{equation}
+{V_c} = \omega R + {V_a}\cos \theta
+\end{equation}
+
+\begin{equation}
+{V_n} = {V_a}\sin \theta
+\end{equation}
+
+\begin{equation}
+W = \sqrt {V_c^2 + V_n^2}
+\end{equation}
+
+The expression for the non-dimensional angle of attack (\emph{α}) with no consideration of blade pitch is:
+
+\begin{equation}
+\alpha  = {\tan ^{ - 1}}\left[ {\frac{{\sin \theta }}{{{{(\omega R} \mathord{\left/ {\vphantom {{(\omega R} {{V_{Local}})/({{{V_a}} \mathord{\left/ {\vphantom {{{V_a}} {{V_{Local}}}}} \right. } {{V_{Local}}}}}}} \right. } {{V_{Local}})/({{{V_a}} \mathord{\left/ {\vphantom {{{V_a}} {{V_{Local}}}}} \right. } {{V_{Local}}}}}}) + \cos \theta }}} \right]
+\end{equation}
+
+The tangential and normal force coefficients, respectively, are expressed as:
+
+\begin{equation}
+{C_t} = {C_l}\sin \alpha  + {C_d}\cos \alpha
+\end{equation}
+
+\begin{equation}
+{C_n} = {C_l}\cos \alpha  + {C_d}\sin \alpha
+\end{equation}
+
+The net tangential and normal forces are obtained from the following expressions:
+
+\begin{equation}
+{F_t} = {C_t}\frac{1}{2}{\rho_{Local}}{A_c}{W^2}
+\end{equation}
+
+\begin{equation}
+{F_n} = {C_n}\frac{1}{2}{\rho_{Local}}{A_c}{W^2}
+\end{equation}
+
+Average tangential force on a single blade can be defined as:
+
+\begin{equation}
+{F_{ta}} = \frac{1}{{2\pi }}\int_0^{2\pi } {{F_t}(\theta )d\theta }
+\end{equation}
+
+Substituting the values of \emph{F\(_{t}\)} and arranging tangential force on azimuth angle, \(\theta\) , equation above can be written as:
+
+\begin{equation}
+{F_{ta}} = \frac{1}{{4\pi }}{C_t}{\rho_{Local}}{A_c}(\int_0^{2\pi } {{{(\omega R)}^2}}  + \int_0^{2\pi } {V_a^2} )
+\end{equation}
+
+The expression of the total torque for the number of blades is defined as:
+
+\begin{equation}
+Q = N{F_{ta}}
+\end{equation}
+
+The power production of wind turbine is thus:
+
+\begin{equation}
+{P_W} = Q\omega
+\end{equation}
+
+The model also defines \emph{P\(_{W}\)} as the rated power output at the rated wind speed, if either the power production of wind turbine or local wind speed is greater than the rated power.
+
+The overall power production delivered from a wind turbine system is thus:
+
+\begin{equation}
+P = \eta {P_W}
+\end{equation}
+
+% table 92
+\begin{longtable}[c]{p{1.2in}p{3.3in}p{1.5in}}
+\caption{Nomenclature for Wind Turbine model \label{table:nomenclature-for-wind-turbine-model}} \tabularnewline
+\toprule 
+Variable & Description & Units \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature for Wind Turbine model} \tabularnewline
+\toprule 
+Variable & Description & Units \tabularnewline
+\midrule
+\endhead
+
+A\(_{R}\) & swept area of rotor & m\(^{2}\) \tabularnewline
+A\(_{C}\) & blade chord area & m\(^{2}\) \tabularnewline
+a & site wind exponent, 0.22 & ~ \tabularnewline
+a\(_{met}\) & wind exponent, 0.14 & ~ \tabularnewline
+C\(_{d}\) & blade drag coefficient, 0.9 & ~ \tabularnewline
+C\(_{l}\) & blade lift coefficients, 0.05 & ~ \tabularnewline
+C\(_{n}\) & normal force coefficient & ~ \tabularnewline
+C\(_{p}\) & power coefficient (performance coefficient) & ~ \tabularnewline
+C\(_{t}\) & tangential force coefficient & ~ \tabularnewline
+C\(_{1-6}\) & empirical power coefficient parameters & ~ \tabularnewline
+g\(_{o}\) & standard gravity & m/s\(^{2}\) \tabularnewline
+F\(_{n}\) & normal force in radial direction & N.m (J) \tabularnewline
+F\(_{t}\) & tangential force & N.m (J) \tabularnewline
+F\(_{ta}\) & average tangential force & N.m (J) \tabularnewline
+F\(_{v}\) & wind speed factor & ~ \tabularnewline
+H & height of local wind speed measurement & m \tabularnewline
+H\(_{met}\) & height of turbine, 10 & m \tabularnewline
+N & number of blade & ~ \tabularnewline
+P & overall power production delivered to building~ & W \tabularnewline
+P\(_{Local}\) & outdoor static air pressure at rotor height & Pa \tabularnewline
+P\(_{W}\) & wind turbine power produced & W \tabularnewline
+Q & overall torque & N.m \tabularnewline
+R & turbine radius & m \tabularnewline
+T\(_{Local}\) & local air temperature at rotor height & °C \tabularnewline
+v & ambient wind speed & m/s \tabularnewline
+v\(_{1}\) & upstream wind speed & m/s \tabularnewline
+v\(_{2}\) & wind speed on the turbine & m/s \tabularnewline
+v\(_{3}\) & downstream wake velocity & m/s \tabularnewline
+V\(_{a}\) & induced velocity & m/s \tabularnewline
+V\(_{AnnualAvg}\) & annual average wind speed from TMY weather data & m/s \tabularnewline
+V\(_{Local}\) & local wind speed at the location of the system & m/s \tabularnewline
+V\(_{LocalTMY}\) & annual average wind speed converted at the local station height & m/s \tabularnewline
+V\(_{c}\) & chordal velocity component & m/s \tabularnewline
+V\(_{n}\) & normal velocity component & m/s \tabularnewline
+V\(_{Z}\) & wind speed adjusted at rotor height & m/s \tabularnewline
+W & relative flow velocity & m/s \tabularnewline
+Z & height of wind turbine rotor & m \tabularnewline
+$\alpha$ & blade angle of attack & deg \tabularnewline
+$\theta$ & azimuth angle in VAWT and pitch angle in HAWT & deg \tabularnewline
+$\rho$\(_{Local}\) & local density of air at rotor height & kg/m\(^{3}\) \tabularnewline
+$\omega$ & angular velocity of turbine & rad/s \tabularnewline
+$\omega$\(_{Local}\) & local humidity ratio at rotor height & kg-H\(_{2}\)O/kg-air \tabularnewline
+x & exponent, 1.5 & ~ \tabularnewline
+$\lambda$ & tip speed ratio & ~ \tabularnewline
+$\lambda$\(_{i}\) & tip speed ratio at the i\(^{th}\) pitch & ~ \tabularnewline
+$\delta$\(_{met}\) & wind boundary layer thickness of meteorological station, 270 & m \tabularnewline
+$\delta$ & site boundary layer thickness, 370 & m \tabularnewline
+$\eta$ & wind turbine system efficiency & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{References}\label{references-3-002}
+
+Siegfried Heier. 2006. Grid Integration of Wind Energy Conversion Systems, Second Edition. Wiley, Chap. 2, pp.31-44.
+
+Mazharul Islam, David S.K. Ting and Amir Fartaj. 2008. Aerodynamic Models for Darrieus-type Sraight-bladed Vertical Axis Wind Turbines. Renewable \& Sustainable Energy Reviews, Volume 12, pp.1087-1109.
+
+ASHRAE. 2005. Handbook of Fundamentals, pp 16.3-16.4, Atlanta: ASHRAE.
diff --git a/doc/engineering-reference/src/on-site-generation/photovoltaic-arrays.tex b/doc/engineering-reference/src/on-site-generation/photovoltaic-arrays.tex
new file mode 100644
index 00000000000..950c5a8b7c1
--- /dev/null
+++ b/doc/engineering-reference/src/on-site-generation/photovoltaic-arrays.tex
@@ -0,0 +1,411 @@
+\section{Photovoltaic Arrays}\label{photovoltaic-arrays}
+
+The Photovoltaics.f90 module includes three different models referred to as ``Simple'', ``Equivalent One-Diode'' and ``Sandia'' and the choice will determine the mathematical models (and input data) used to determine the energy produced by solar/electric conversion panels. The EnergyPlus photovoltaic array models are called one at a time at the HVAC system timestep along with other electrical generation components such as gas turbines and diesel engines.
+
+All of the photovoltaic models share the same models for predicting incident solar radiation that are also used for the solar thermal calculations and are described in the section Climate, Sky and Solar/Shading Calculations.
+
+Note that some of the terminology used to discussed photovoltaics overlaps with terminology used to discuss Fortran programs. The word \emph{module} may refer to a PV panel or to a fortran90 programming entity. \emph{Model} may refer to a manufacturers production model for a specific type of PV module or to a mathematical model used for engineering analysis. \emph{Array} may refer to a collection of PV modules wired together or to a mathematical variable with multiple elements.
+
+The PV modules are assumed to always run when the total incident solar is greater than 0.3 Watts. If the incident solar is less than 0.3, then the modules produce no power.
+
+PV arrays are managed by an electric load center. The load center is a ``load'' with respect to generating equipment but is a ``supply center'' for the rest of the building. PV arrays need to be connected to ElectricLoadCenter:Distribution objects that have a DC buss type.
+
+\subsection{Simple Model}\label{simple-model}
+
+The Generator:PV:Simple object describes about the simplest model for predicting photovoltaic energy production. In this model the user specifies the efficiency with which surfaces convert incident solar radiation to electricity. (In the other models this efficiency is determined as part of the model.)~ The full geometric model for solar radiation is used, including sky models, shading, and reflections, to determine the incident solar resource. The model accepts arbitrary conversion efficiencies and does not require actual production units be tested to obtain empirical performance coefficients. (The Energy+.idd sets the range of conversion efficiencies to be on {[}0..1{]}, but the user could alter the Energy+.idd to extend this range if desired.)
+
+\subsubsection{Mathematical Description}\label{mathematical-description}
+
+% table 89
+\begin{longtable}[l]{p{1.2in}p{4.8in}}
+\caption{Nomenclature for Simple Photovoltaic model \label{table:nomenclature-for-simple-photovoltaic-model}} \tabularnewline
+\toprule 
+Mathematical variable & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature for Simple Photovoltaic model} \tabularnewline
+\toprule 
+Mathematical variable & Description \tabularnewline
+\midrule
+\endhead
+
+P & Electrical power produced by photovoltaics [W] \tabularnewline
+A\(_{surf}\) & Net area of surface~ [m\(^{2}\)] \tabularnewline
+f\(_{activ}\) & Fraction of surface area with active solar cells [] \tabularnewline
+G\(_{T}\) & Total solar radiation incident on PV array [W/m\(^{2}\)] \tabularnewline
+$\eta$\(_{cell}\) & Module conversion efficiency [] \tabularnewline
+$\eta$\(_{invert}\) & DC to AC conversion efficiency~ [] \tabularnewline
+\bottomrule
+\end{longtable}
+
+The usable electrical power produced by a PV surface are calculated using:
+
+\begin{equation}
+P = {A_{surf}} \cdot {f_{activ}} \cdot {G_T} \cdot {\eta_{cell}} \cdot {\eta_{invert}}
+\end{equation}
+
+On the right hand side of this equation, only G\(_{T}\) is calculated by EnergyPlus and the rest are user inputs. Power levels are assumed constant over the timestep to arrive at energy production.
+
+There are two modes that can be selected by the user that govern how the PV system is coupled to the building surfaces. If the integration mode is selected as `DECOUPLED' then no adjustments are made to account for energy extracted in the form of electricity. If the integration mode is selected as `INTEGRATED' then the energy extracted in the form of electricity is removed from surface heat transfer calculations using a sink term. This sink term is lagged from the previous timestep.
+
+\subsection{Equivalent One-Diode Model}\label{equivalent-one-diode-model}
+
+This model predicts the electrical performance of a photovoltaic (PV) array. This model is also known as the ``TRNSYS PV'' model.
+
+Mathematically speaking, the EnergyPlus PV module employs equations for an empirical equivalent circuit model to predict the current-voltage characteristics of a single module. This circuit consists of a DC current source, diode, and either one or two resistors. The strength of the current source is dependent on solar radiation and the IV characteristics of the diode are temperature-dependent. The results for a single module equivalent circuit are extrapolated to predict the performance of a multi-module array.
+
+The module employs a ``four-parameter'' equivalent circuit to model crystalline (both mono and poly) PV modules developed at the University of Wisconsin -- Madison {[}2{]}. The values of these parameters cannot normally be obtained directly from manufacturers' catalogs. However, the PV module will automatically calculate them from commonly available data. The PV module also includes an optional incidence angle modifier correlation to calculate how the reflectance of the PV module surface varies with the angle of incidence of solar radiation.
+
+The module determines PV current as a function of load voltage. Other OUTPUTS include current and voltage at the maximum power point along the IV curve, open-circuit voltage, short circuit current as well as electrical load met and unmet.
+
+% table 90
+\begin{longtable}[l]{p{1.2in}p{4.8in}}
+\caption{General Nomenclature for the PV model \label{table:general-nomenclature-for-the-pv-model}} \tabularnewline
+\toprule 
+Mathematical variable & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{General Nomenclature for the PV model} \tabularnewline
+\toprule 
+Mathematical variable & Description \tabularnewline
+\midrule
+\endhead
+
+$\beta$ & Slope of PV array [degrees] \tabularnewline
+$\gamma$ & Empirical PV curve-fitting parameter \tabularnewline
+$\varepsilon$\(_{\gamma}\) & Semiconductor bandgap [eV] \tabularnewline
+$\eta$\(_{c}\) & Module conversion efficiency \tabularnewline
+$\mu$\(_{I\alpha\gamma}\) & Temperature coefficient of short-circuit current [A/K] \tabularnewline
+$\mu$\(_{\zeta}\)\(_o\)\(_{\gamma}\) & Temperature coefficient of open-circuit voltage [V/K] \tabularnewline
+$\theta$ & Angle of incidence for solar radiation [degrees] \tabularnewline
+$\tau\alpha$ & Module transmittance-absorptance product \tabularnewline
+$\tau\alpha$\(_{normal}\) & Module transmittance-absorptance product at normal incidence \tabularnewline
+G\(_{T}\) & Total radiation incident on PV array \tabularnewline
+G\(_{T,beam}\) & Beam component of incident radiation \tabularnewline
+G\(_{T,diff}\) & Diffuse component of incident radiation \tabularnewline
+G\(_{T,gnd}\) & Ground-reflected component of incident radiation \tabularnewline
+G\(_{T,NOCT}\) & Incident radiation at NOCT conditions \tabularnewline
+G\(_{T,ref}\) & Incident radiation at reference conditions \tabularnewline
+I & Current \tabularnewline
+I\(_{L}\) & Module photocurrent \tabularnewline
+I\(_{L,ref}\) & Module photocurrent at reference conditions \tabularnewline
+I\(_{o}\) & Diode reverse saturation current \tabularnewline
+I\(_{o,ref}\) & Diode reverse saturation current at reference conditions \tabularnewline
+I\(_{sc}\) & Short-circuit current \tabularnewline
+I\(_{sc,ref}\) & Short-circuit current at reference conditions \tabularnewline
+I\(_{mp}\) & Current at maximum power point along IV curve \tabularnewline
+I\(_{mp,ref}\) & Current at maximum power point along IV curve, reference conditions \tabularnewline
+IAM & Dimensionless incidence angle modifier \tabularnewline
+K & Boltzmann constant [J/K] \tabularnewline
+NP & Number of modules in parallel in array \tabularnewline
+NS & Number of modules in series in array \tabularnewline
+N\(_{s}\) & Number of individual cells in module \tabularnewline
+P & PV output power \tabularnewline
+P\(_{max}\) & PV output power at maximum power point along IV curve \tabularnewline
+Q & Electron charge constant \tabularnewline
+R\(_{s}\) & Module series resistance [$\Omega$] \tabularnewline
+R\(_{sh}\) & Module shunt resistance [$\Omega$] \tabularnewline
+T\(_{c}\)­ & Module temperature [K] \tabularnewline
+T\(_{c,NOCT}\) & Module temperature at NOCT conditions [K] \tabularnewline
+T\(_{c,ref}\) & Module temperature at reference conditions [K] \tabularnewline
+U\(_{L}\) & Array thermal loss coefficient \tabularnewline
+V & Voltage \tabularnewline
+V\(_{mp}\) & Voltage at maximum power point along IV curve \tabularnewline
+V\(_{mp,ref}\) & Voltage at maximum power point along IV curve, reference conditions \tabularnewline
+V\(_{oc}\)­ & Open-circuit voltage \tabularnewline
+V\(_{oc,ref}\) & Open-circuit voltage at reference conditions [V] \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Mathematical Description}\label{mathematical-description-1}
+
+\paragraph{PV Section 1: Four-Parameter Model}\label{pv-section-1-four-parameter-model}
+
+The four-parameter equivalent circuit model was developed largely by Townsend {[}1989{]} and is detailed by Duffie and Beckman {[}1991{]}. The model was first incorporated into a component for the TRNSYS simulation package by Eckstein {[}1990{]}. The EnergyPlus module employs the Eckstein model for crystalline PV modules, using it whenever the short-circuit IV slope is set to zero or a positive value as modified by Ulleberg {[}2000{]}. The four parameter model assumes that the slope of the IV curve is zero at the short-circuit condition:
+
+\begin{equation}
+{\left( {\frac{{dI}}{{dV}}} \right)_{v = 0}} = 0
+\end{equation}
+
+This is a reasonable approximation for crystalline modules. The ``four parameters'' in the model are \emph{I\(_{L,ref}\)}, \emph{I\(_{o,ref,}\)} g, and \emph{R\(_{s}\).} These are empirical values that cannot be determined directly through physical measurement. The EnergyPlus model calculates these values from manufactures' catalog data as discussed in the following section on calculating these parameters
+
+The four-parameter equivalent circuit is shown in the following figure:
+
+\begin{figure}[hbtp] % fig 339
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7592.svg.png}
+\caption{Equivalent circuit in the four parameter model \protect \label{fig:equivalent-circuit-in-the-four-parameter}}
+\end{figure}
+
+\emph{V} is the load voltage and \emph{I} is the current flowing through the load and PV.
+
+\textbf{Determining Performance under Operating Conditions}
+
+The IV characteristics of a PV change with both insolation and temperature. The PV model employs these environmental conditions along with the four module constants \emph{I\(_{L,ref}\)}, \emph{I\(_{o,ref,}\)} g, and \emph{R\(_{s}\)} to generate an IV curve at each timestep.
+
+The current-voltage equation of circuit shown in the previous figure is as follows:
+
+\begin{equation}
+I = {I_L} - {I_o}\left[ {\exp \left( {\frac{q}{{\gamma k{T_c}}}\left( {V + I{R_s}} \right)} \right) - 1} \right]
+\end{equation}
+
+\emph{R\(_{s}\)} and g are constants. The photocurrent \emph{I\(_{L}\)} depends linearly on incident radiation:
+
+\begin{equation}
+{I_L} = {I_{L,ref}}\frac{{{G_T}}}{{{G_{T,ref}}}}
+\end{equation}
+
+The reference insolation \emph{G\(_{ref}\)} ~is nearly always defined as 1000 W/m\(^{2}\). The diode reverse saturation current \emph{I\(_{o}\)} is a temperature dependent quantity:
+
+\begin{equation}
+\frac{{{I_o}}}{{{I_{o,ref}}}} = {\left( {\frac{{{T_c}}}{{{T_{c,ref}}}}} \right)^3}
+\end{equation}
+
+Equation gives the current implicitly as a function of voltage. Once \emph{I\(_{o}\)} and \emph{I\(_{L}\)} are found from Eqs. 3 and 4, Newton's method is employed to calculate the PV current. In addition, an iterative search routine finds the current (\emph{I\(_{mp}\)}) ~and voltage (\emph{V\(_{mp}\)})~ at the point of maximum power along the IV curve.
+
+\textbf{Calculating \emph{I\(_{L,ref}\)}, \emph{I\(_{o,ref,}\)}} \textbf{g, and \emph{R\(_{s}\)}}
+
+The Idf specification for the PV model include several values which must be read from manufacturers' PV module catalogs. The manufactures' values are used to determine the equivalent circuit characteristics \emph{I\(_{L,ref}\)}, \emph{I\(_{o,ref,}\)} g, and \emph{R\(_{s}\)}. These characteristics define an equivalent circuit that is employed to find the PV performance at each timestep, as described previously. This section describes the algebra and calculation algorithms used to solve for the four equivalent circuit characteristics.
+
+Three of these values, \emph{I\(_{L,ref}\)}, \emph{I\(_{o,ref,}\)} g, may be isolated algebraically. The first step is to substitute the current and voltage into Eq. at the open-circuit, short circuit, and maximum power conditions:
+
+\begin{equation}
+0 = {I_{L,ref}} - {I_{o,ref}}\left[ {\exp \left( {\frac{q}{{\gamma k{T_{c,ref}}}}{V_{oc,ref}}} \right) - 1} \right] - \frac{{{V_{oc,ref}}}}{{{R_{sh}}}}
+\end{equation}
+
+\begin{equation}
+{I_{sc,ref}} = {I_{L,ref}} - {I_{o,ref}}\left[ {\exp \left( {\frac{{q{I_{sc,ref}}{R_s}}}{{\gamma k{T_{c,ref}}}}} \right) - 1} \right] - \frac{{{I_{sc,ref}}{R_s}}}{{{R_{sh}}}}
+\end{equation}
+
+\begin{equation}
+{I_{mp,ref}} = {I_{L,ref}} - {I_{o,ref}}\left[ {\exp \left( {\frac{q}{{\gamma k{T_{c,ref}}}}\left( {{V_{mp,ref}} + {I_{mp,ref}}{R_s}} \right)} \right) - 1} \right] - \frac{{{V_{mp,ref}} + {I_{mp,ref}}{R_s}}}{{{R_{sh}}}}
+\end{equation}
+
+In each case the ``-1'' term is may be dropped to simplify the algebra. This approximation has little influence on the right side of the equations since because the magnitude of \emph{I\(_{o}\)} is very small, generally on the order of 10\(^{-6}\) A. Some rearrangement then yields the following three expressions which isolate \emph{I\(_{L,ref}\)}, \emph{I\(_{o,ref,}\)} g:
+
+\begin{equation}
+{I_{L,ref}} \approx {I_{sc,ref}}
+\end{equation}
+
+\begin{equation}
+\gamma  = \frac{{q\left( {{V_{mp,ref}} - {V_{oc,ref}} + I_{mp,ref}^{}{R_s}} \right)}}{{k{T_{c,ref}}\ln \left( {1 - \frac{{{I_{mp,ref}}}}{{{I_{sc,ref}}}}} \right)}}
+\end{equation}
+
+\begin{equation}
+{I_{o,ref}} = \frac{{{I_{sc,ref}}}}{{\exp \left( {\frac{{q{V_{oc,ref}}}}{{\gamma k{T_{c,ref}}}}} \right)}}
+\end{equation}
+
+At this point an additional equation is needed in order to determine the last unknown parameter. Taking the analytical derivative of voltage with respect to temperature at the reference open-circuit condition derives the fourth equation. This analytical value is matched to the open-circuit temperature coefficient, a catalog specification:
+
+\begin{equation}
+\frac{{\partial {V_{oc}}}}{{\partial {T_c}}} = {\mu_{voc}} = \frac{{\gamma k}}{q}\left[ {\ln \left( {\frac{{{I_{sc,ref}}}}{{{I_{o,ref}}}}} \right) + \frac{{{T_c}\mu_{isc}^{}}}{{{I_{sc,ref}}}} - \left( {3 + \frac{{q\varepsilon }}{{Ak{T_{c,ref}}}}} \right)} \right]
+\end{equation}
+
+where
+
+\begin{equation}
+A = \frac{\gamma }{{{N_s}}}
+\end{equation}
+
+The ``TRNSYS PV model'' uses an iterative search routine in these four equations to calculate the equivalent circuit characteristics. The first step is to set upper and lower bounds for the series resistance parameter \emph{R\(_{s}\)}:~ physical constraints require the \emph{R\(_{s}\)} value to lie between 0 and the value such that g = \emph{N\(_{s}\)}. The initial guess for \emph{R\(_{s}\)} is midway between these bounds. g and \emph{I\(_{o,ref}\)} ~are found from Eq. and Eq. , while Eq. gives a trivial solution for \emph{I\(_{L,ref}\)}.~ The model then employs Eq. to compare the analytical and catalog values for m\(_{voc}\). When all other variables are held constant, the analytical value for m\(_{voc}\) increases monotonically with series resistance (Townsend 1989). If the analytical voltage coefficient is less than the catalog value, the lower bound for \emph{R\(_{s}\)} is reset to the present guess value. Likewise, the upper bound is set to the current value if the calculated m\(_{voc}\) is too large. After resetting the upper or lower bound for \emph{R\(_{s}\)}, a new guess value is found by averaging the bounds. This procedure repeats until \emph{R\(_{s}\)} and g converge. Note that for \emph{I\(_{L,ref}\)}, \emph{I\(_{o,ref,}\)} g, and \emph{R\(_{s}\)} are assumed to be constant and are calculated only on the first call in the simulation. Alternatively, the user may enter a known series resistance by entering a \textbf{positive} value in the IDF. In this case the iterative routine described above is skipped and Eqs. , , and find \emph{I\(_{L,ref}\)}, \emph{I\(_{o,ref,}\)} and g directly from the given value of \emph{R\(_{s}\)}.
+
+\paragraph{PV Section 2 : Module Operating Temperature}\label{pv-section-2-module-operating-temperature}
+
+The PV model uses one of five methods for determining cell temperature data. The cell temperature of a PV module is important because the hotter the temperature of the panel, the lower its electrical output. The cell temperature calculation method is chosen by the user in the EnergyPlus IDF file through a parameter choice in the IDD entry called Integration and Cell Temperature Mode.
+
+If the value of this parameter is ``\textbf{Decoupled NOCT Conditions}'' then the cell temperature of the PV is modeled using the method from the Duffie and Beckman (1991) for estimating cell temperature. This is based upon the standard NOCT (Nominal Operating Cell Temperature) measurements to compute the module temperature Tc at each timestep. The NOCT temperature (Tc,NOCT) is the operating temperature of the module with a wind speed of 1 m/s, no electrical load, and a certain specified insolation and ambient temperature {[}Beckman and Duffie, 1991{]}. The values for insolation GT,NOCT ~and ambient temperature \emph{T\(_{a,NOCT}\)} are usually 800 W/m\(^{2}\) and 20º C. \emph{h\(_{c}\)} is the convesion efficiency of the module, which varies with ambient conditions. ta is a user-defined constant.
+
+The equation is:
+
+\begin{equation}
+  T_c = T_a + \frac{1-\frac{\eta_c}{\tau \alpha}}{G_T \tau\alpha/U_L}
+\end{equation}
+
+If the user specifies the ``\textbf{Decoupled Ulleberg Dynamic''} mode for calculating cell temperature, then a method developed by Ulleberg is used:
+
+\begin{equation}
+{\left. {{T_{cell}}} \right|_t} = {T_{ambient}} + \left( {{{\left. {{T_{cell}}} \right|}_{t - 1}} - {T_{ambient}}} \right)*{e^{\frac{{ - UL}}{{Cap}}\Delta t}}
+\end{equation}
+
+In other words, the cell temperature is a function of the privious cell temperature and the thermal capacity of the PV module material.
+
+If the user specifies ``\textbf{Integrated Surface Outside Face''} for this parameter, then the temperature result from EnergyPlus's modeling of surfaces is used for the cell temperature. Also the energy exported from the surface as electricity becomes a sink in the internal source modeling for the heat transfer surface.
+
+If the user specifies ``\textbf{Integrated Transpired Collector''} for this parameter, then the temperature result for the unglazed transpired collector surfaces is used for the cell temperature. Also the energy exported from the collector surface as electricity is deprecated using a source term in the collector's temperature modeling.
+
+If the user specifies ``\textbf{Integrated Exterior Vented Cavity''} for this parameter, then the temperature result for the exterior cavity is used for the cell temperature. Also the energy exported from the baffle surface as electricity is deprecated using a source term in the baffle's temperature modeling.
+
+\paragraph{PV Section 3 : Multi-Array Modules}\label{pv-section-3-multi-array-modules}
+
+The electrical calculations discussed in the sections above deal only with a single module. The EnergyPlus PV component may be used to simulate arrays with any number of modules. The IDF defines the number of modules in series (NS) and modules in parallel (NP) for the entire array. The total number of modules in the array is the product of NS and NP. When simulating a single module only, both NS and NP are set to 1. The single-module values for all currents and voltages discussed in PV Section 1 are multiplied by NP or NS to find values for the entire array. This approach neglects module mismatch losses.
+
+With the above equations, and the assumption that the panels operate at the maximum power point, it is a direct calculation to determine DC power production. The performance of an array of identical modules is assumed to be linear with the number of modules in series and parallel. The inverter efficiency is applied linearly to derate the energy production. The inverter capacity forms a limit for power production from a PV generator. A `load' is passed the PV array acting as a generator and various trivial calculations compare PV production to this load. If the PV array is associated with a surface that is associated with a zone, then if the zone has any multipliers associated with it, electricity production will be multiplied accordingly.
+
+\subsubsection{References}\label{references-035}
+
+Duffie, John A. and William A. Beckman. 1991. \emph{Solar Engineering of Thermal Processes}. New York: John Wiley \& Sons, Inc..
+
+Eckstein, Jürgen Helmut. 1990. \emph{Detailed Modeling of Photovoltaic Components}. M. S. Thesis -- Solar Energy Laboratory, University of Wisconsin, Madison: 1990.
+
+Ulleberg, Øystein. \emph{HYDROGEMS Component Library for TRNSYS 15 User Manual}, Institute for Energy Technology, Kjeller, Norway \emph{~}
+
+\subsection{Sandia Photovoltaic Performance Model}\label{sandia-photovoltaic-performance-model}
+
+The third model available in EnergyPlus for predicting the electricity generated by photovoltaics is referred to as the Sandia model. This model is based on work done at Sandia National Lab, Albuquerque, NM by David King -- with the help of many others. The model consists of a series of empirical relationships with coefficients that are derived from actual testing. Once the coefficients for a particular module are available, it is straightforward matter to use the model equations to calculate five select points on the current-voltage curve.
+
+The implementation in EnergyPlus is also based on work done by Greg Barker (2003) for the National Renewable Energy Lab who implemented the Sandia model in FORTRAN77 as a custom type (Type101) for the TRNSYS computer program.
+
+There are several climate and solar orientation inputs to the model that are managed elsewhere in EnergyPlus including: incident beam solar, incident diffuse solar, incidence angle of beam solar, solar zenith Angle, outdoor drybulb, wind speed, and elevation.
+
+\subsubsection{Mathematical Description}\label{mathematical-description-2}
+
+This section presents the mathematical description of the Sandia model from a draft report by King et, al. (2003). The core of the model predicts the performance of a single PV module. The following nomenclature and equations summarize the Sandia model.
+
+% table 91
+\begin{longtable}[c]{p{1.2in}p{4.8in}}
+\caption{Nomenclature for Sandia PV model \label{table:nomenclature-for-sandia-pv-model}} \tabularnewline
+\toprule 
+Mathematical variable & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature for Sandia PV model} \tabularnewline
+\toprule 
+Mathematical variable & Description \tabularnewline
+\midrule
+\endhead
+
+I\(_{sc}\) & Short-circuit current (A) \tabularnewline
+I\(_{mp}\) & Current at the maximum-power point (A) \tabularnewline
+I\(_{x}\) & Current at module V = 0.5 V\(_{oc}\), defines 4th point on I-V curve \tabularnewline
+I\(_{xx}\) & Current at module V = 0.5 (V\(_{oc}\) + V\(_{mp}\)), defines a 5th point on the I-V curve \tabularnewline
+V\(_{oc}\) & Open-circuit voltage (V) \tabularnewline
+V\(_{mp}\) & Voltage at maximum-power point (V) \tabularnewline
+P\(_{mp}\) & Power at maximum-power point (W) \tabularnewline
+fd & Fraction of diffuse irradiance used by module \tabularnewline
+N\(_{s}\) & Number of cells in series in a module’s cell-string \tabularnewline
+N\(_{p}\) & Number of cell-strings in parallel in module \tabularnewline
+k & Boltzmann’s constant, 1.38066E-23 (J/k) \tabularnewline
+q & Elementary charge, 1.60218E-19 (coulomb) \tabularnewline
+T\(_{c}\) & Cell temperature inside module (°C) \tabularnewline
+$\delta$(T\(_{c}\)) & ‘Thermal voltage’ per cell at temperature T\(_{c}\), approximately 1 volt for a typical 26-cell crystalline silicon module \tabularnewline
+E\(_{e}\) & ‘Effective’ solar irradiance \tabularnewline
+E\(_{b}\) & Beam solar irradiance \tabularnewline
+E\(_{diff}\) & Diffuse solar irradiance \tabularnewline
+C\(_{0}\), C\(_{1}\) & Empirical coefficients relating I\(_{mp}\) to E\(_{e}\), C\(_{0}\) + C\(_{1}\) = 1 (both dimensionless) \tabularnewline
+C\(_{2}\), C\(_{3}\) & Empirical coefficients relating V\(_{mp}\) to E\(_{e}\) (C\(_{2}\) dimensionless, C\(_{3}\) is 1/V) \tabularnewline
+C\(_{4}\), C\(_{5}\) & Empirical coefficients relating I\(_{x}\) to E\(_{e}\), C\(_{4}\) + C\(_{5}\) = 1 (both dimensionless) \tabularnewline
+C\(_{6}\), C\(_{7}\) & Empirical coefficients relating I\(_{xx}\) to E\(_{e}\) C\(_{6}\) + C\(_{7}\) = 1 (both dimensionless) \tabularnewline
+n & Empirically determined ‘diode factor’ for individual cells \tabularnewline
+AMa & Absolute Air Mas \tabularnewline
+AOI & Solar angle-of-incidence (degrees) from normal \tabularnewline
+f\(_{1}\)(AM\(_{a}\)) & Empirical polynomial function used to relate short-circuit current to the solar spectrum via air mass \tabularnewline
+f\(_{2}\)(AOI) & Empirical polynomial function used to relate short-circuit current to the solar angle-of-incidence \tabularnewline
+a\(_{0}\), a\(_{1}\), a\(_{2}\), a\(_{3}\), a\(_{4}\) & Empirical coefficients for f\(_{1}\)(AM\(_{a}\)) polynomial \tabularnewline
+b\(_{0}\), b\(_{1}\), b\(_{2}\), b\(_{3}\), b\(_{4}\),b\(_{5}\),b\(_{6}\) & Empirical coefficients for f\(_{2}\)(AOI) polynomial \tabularnewline
+T\(_{o}\) & Reference cell temperature for rating, typically fixed at 25°C \tabularnewline
+I\(_{sco}\) & Short circuit current at reference conditions \tabularnewline
+I\(_{mpo}\) & Max power point current at reference conditions \tabularnewline
+V\(_{mpo}\) & Voltage at max power at reference conditions \tabularnewline
+V\(_{oco}\) & Open circuit voltage at reference conditions \tabularnewline
+I\(_{xo}\) & Current at V = 0.5 Voc and at reference conditions \tabularnewline
+I\(_{xxo}\) & Current at V = 0.5 (Vmp + Voc) and at reference conditions \tabularnewline
+$\alpha$\(_{Isc}\) & Normalized temperature coefficient for I\(_{sc}\) (1/°C) \tabularnewline
+$\alpha$\(_{Imp}\) & Normalized temperature coefficient for I\(_{mp}\) (1/°C) \tabularnewline
+$\beta$\(_{Voc}\)(E\(_{e}\)) & Temperature coefficient for module open-circuit-voltage as function of E\(_{e}\) \tabularnewline
+$\beta$\(_{Voco}\) & Temperature coefficient for module open-circuit-voltage at reference conditions \tabularnewline
+m\(_{\beta}\)\(_{Voco}\) & Coefficient for irradiance dependence of open-circuit-voltage-temperature coefficient, often zero (V/°C) \tabularnewline
+$\beta$\(_{Vmp}\)(E\(_{e}\)) & Temperature coefficient for module maximum-power-voltage as a function of E \tabularnewline
+$\beta$\(_{Vmpo}\) & Temperature coefficient for module maximum-power-voltage at reference conditions \tabularnewline
+m\(_{\beta}\)\(_{Voco}\) & Cofficient for irradiance dependence of maximum-power-voltage-temperature coefficient, often zero (V/°C) \tabularnewline
+T\(_{m}\) & PV module temperature at back suface (°C) \tabularnewline
+T\(_{a}\) & Ambient outdoor drybulb temperature (°C) \tabularnewline
+E & Solar irradiance incident on module surface (W/m\(^{2}\)) \tabularnewline
+WS & Wind speed at standard 10-m height (m/s) \tabularnewline
+a & Empirical coefficient relating module temperature at low wind and high solar irradiance \tabularnewline
+b & Empirical coefficient relating module temperature decrease with increasing wind speed \tabularnewline
+T\(_{c}\) & Temperature of solar cell inside module (°C) \tabularnewline
+E\(_{o}\) & Reference solar irradiance (1000 W/m\(^{2}\)) \tabularnewline
+$\Delta$T & Temperature difference between T\(_{c}\) and T\(_{m}\) at E\(_{o}\) (°C), (This is d(Tc) in Sandia database) \tabularnewline
+\bottomrule
+\end{longtable}
+
+The current implementation in EnergyPlus focuses on determining performance at the maximum power-point but also calculates, and reports, four other points on the I-V curve so that the data are available for analyses outside of EnergyPlus. The equations below use the module performance parameters that are available in a database provided by Sandia National Laboratory (see www.sandia.gov/pv). The following equations form the basis of the Sandia model implemented in EnergyPlus:
+
+\begin{equation}
+{I_{sc}} = {I_{sco}} \cdot {f_1}\left( {A{M_a}} \right) \cdot \left\{ {\left( {{E_b} \cdot {f_2}\left( {AOI} \right) + {f_d} \cdot {E_{diff}}} \right)/{E_o}} \right\} \cdot \left\{ {1 + {\alpha_{Isc}} \cdot \left( {{T_c} - {T_o}} \right)} \right\}
+\end{equation}
+
+\begin{equation}
+{I_{mp}} = {I_{mpo}} \cdot \left\{ {{C_o} \cdot {E_e} + {C_1} \cdot E_e^2} \right\} \cdot \left\{ {1 + {\alpha_{{\mathop{\rm Im}\nolimits} p}} \cdot ({T_c} - {T_o}} \right\}
+\end{equation}
+
+\begin{equation}
+{V_{oc}} = {V_{oco}} + {N_s} \cdot \delta ({T_c}) \cdot \ln ({E_e}) + {\beta_{Voc}}({E_e}) \cdot \left( {{T_c} - {T_o}} \right)
+\end{equation}
+
+\begin{equation}
+{V_{mp}} = {V_{mpo}} + {C_2} \cdot {N_s} \cdot \delta \left( {T_c^{}} \right) \cdot \ln \left( {{E_e}} \right) + {C_3} \cdot {N_3} \cdot {\left\{ {\delta \left( {T_c^{}} \right) \cdot \ln \left( {{E_e}} \right)} \right\}^2} + {\beta_{Vmp}}({E_e}) \cdot ({T_c} - {T_o})
+\end{equation}
+
+\begin{equation}
+{P_{mp}} = {I_{mp}} \cdot {V_{mp}}
+\end{equation}
+
+\begin{equation}
+{I_x} = {I_{xo}} \cdot \left\{ {{C_4} \cdot {E_e} + {C_5} \cdot E_e^2} \right\} \cdot \left\{ {1 + ({\alpha_{Isc}}) \cdot ({T_c} - {T_o})} \right\}
+\end{equation}
+
+\begin{equation}
+{I_{xx}} = {I_{xxo}} \cdot \left\{ {{C_6} \cdot {E_e} + {C_7} \cdot E_e^2} \right\} \cdot \left\{ {1 + ({\alpha_{{\mathop{\rm Im}\nolimits} p}}) \cdot ({T_c} - {T_{o)}}} \right\}
+\end{equation}
+
+where,
+
+\begin{equation}
+{E_e} = {I_{sc}}/\left[ {{I_{sco}} \cdot \left\{ {1 + {\alpha_{Isc}} \cdot ({T_c} - {T_o})} \right\}} \right]
+\end{equation}
+
+\begin{equation}
+\delta ({T_c}) = n \cdot k \cdot ({T_c} + 273.15)/q
+\end{equation}
+
+\begin{equation}
+{f_1}\left( {A{M_a}} \right) = {a_0} + {a_1}A{M_a} + {a_2}{\left( {A{M_a}} \right)^2} + {a_3}{\left( {A{M_a}} \right)^3} + {a_4}{\left( {A{M_a}} \right)^4}
+\end{equation}
+
+\begin{equation}
+{f_2}\left( {AOI} \right) = {b_0} + {b_1} \cdot AOI + {b_2}{\left( {AOI} \right)^2} + {b_3}{\left( {AOI} \right)^3} + {b_4}{\left( {AOI} \right)^4} + {b_5}{\left( {AOI} \right)^5}
+\end{equation}
+
+\begin{equation}
+{\beta_{Voc}}({E_e}) = {\beta_{Voco}} + {m_{\beta Voc}} \cdot (1 - {E_e})
+\end{equation}
+
+\begin{equation}
+{\beta_{Vmp}}({E_e}) = {\beta_{Vmpo}} + {m_{\beta Vmp}} \cdot (1 - {E_e})
+\end{equation}
+
+\begin{equation}
+{T_m} = E \cdot \left\{ {{e^{a + b \cdot WS}}} \right\} + {T_a}
+\end{equation}
+
+\begin{equation}
+{T_c} = {T_m} + \frac{E}{{{E_o}}} \cdot \Delta T
+\end{equation}
+
+With the above equations, and the assumption that the panels operate at the maximum power point, it is a direct calculation to determine DC power production. The performance of an array of identical modules is assumed to be linear with the number of modules in series and parallel. The inverter efficiency is applied linearly to derate the energy production. The inverter capacity forms a limit for power production from a PV generator. A `load' is passed the PV array acting as a generator and various trivial calculations compare PV production to this load. If the PV array is associated with a surface that is associated with a zone, then if the zone has any multipliers associated with it, electricity production will be multiplied accordingly.
+
+The equation above for T\(_{m}\) is used to predict back-of-module temperature when the mode `SANDIA RACK' is selected. This would be appropriate for most rack mounted PV installations. If the user selects `EPLUS INTEGRATED' then the back-of-module temperature is obtained from the outside face surface temperature calculated by the full complement of Heat Balance models using Conduction Transfer Functions that is native to EnergyPlus. And energy exported from the surface is accounted for using a source/sink term that is lagged from the previous timestep (pingpong).
+
+\subsubsection{References}\label{references-1-014}
+
+King, D.L., Boyson, W.E., Kratochvil J.A. 2003. Photovoltaic Array Performance Model. Sandia National Laboratories, Albuquerque, NM 87185, November 2003~ currently in DRAFT
+
+Barker, G. 2003 (unknown). Predicting Long-Term Performance of Photovoltaic Arrays. Submitted as deliverable for NREL subcontract LAX-1-30480-02. Currently in DRAFT
+
+Davis, M.W., Fanney, A.H., and Dougherty B.P. 2002. Measured Versus Predicted Performance of Building Integrated Photovoltaics. from the conference Solar 2002, Sunrise on the Reliable Energy Economy, June 15-19, 2002, Reno, NV. Available from NIST website.
+
+King, D.L. 1996. Photovoltaic Module and Array Performance Characterization Methods for All System Operating Conditions. Sandia National Laboratory. Albuquerque, NM 87185
diff --git a/doc/engineering-reference/src/on-site-generation/whole-facility-electric-service.tex b/doc/engineering-reference/src/on-site-generation/whole-facility-electric-service.tex
new file mode 100644
index 00000000000..3db4b01c040
--- /dev/null
+++ b/doc/engineering-reference/src/on-site-generation/whole-facility-electric-service.tex
@@ -0,0 +1,58 @@
+\section{Whole-Facility Electric Service}\label{section-whole-facility-electric-service}
+-----------------------------------------
+
+Whenever an EnergyPlus model includes anything that consumes electricity the program will do some basic modeling of what can be thought of as the main panel where utility grid connects to the building and HVAC loads.  The following output variables and meters are created and filled to report on the overall, whole-facility power flows at the main panel: 
+
+\begin{tabular}{c|c|c}
+  $ {P_{purch}}  $ &    Facility Total Purchased Electric Power & [W] \tabularnewline
+  $ {Q_{purch}}  $ &    Facility Total Purchased Electric Energy & [J] \tabularnewline
+  $ {P_{net,purch}}  $ &    Facility Net Purchased Electric Power & [W] \tabularnewline
+  $ {Q_{net,purch}}  $ &    Facility Net Purchased Electric Energy & [J] \tabularnewline
+  $ {P_{surp}}  $ &    Facility Total Surplus Electric Power & [W] \tabularnewline
+  $ {Q_{surp}}  $ &    Facility Total Surplus Electric Energy & [J] \tabularnewline
+  $ {P_{bldg,dmd}}  $ &    Facility Total Building Electric Demand Power & [W] \tabularnewline
+  $ {P_{HVAC,dmd}}  $ &    Facility Total HVAC Electric Demand Power & [W] \tabularnewline
+  $ {P_{dmd}}  $ &    Facility Total Electric Demand Power & [W] \tabularnewline
+  $ {P_{prod}}  $ &    Facility Total Produced Electric Power & [W] \tabularnewline
+  $ {Q_{prod}}  $ &   Facility Total Produced Electric Energy & [J]
+\end{tabular}
+
+The models for electric power service use the meter reporting system inside EnergyPlus to obtain data from all the other models in EnergyPlus for the electric power demand (and maybe power production).  The ElectricPowerServiceManager uses a query routine called "GetInstantMeterValue" which returns the sum for all the metered equipment for the specified meter.  Values for   $P_{bldg,dmd}$ and $P_{HVAC,dmd}$ are both filled from the "Electricity:Facility" meter.  $P_{bldg,dmd}$ is filled by passing an argument that triggers to return the "Building" electric load, which is at the zone timestep, while $P_{HVAC,dmd}$ is filled by passing an argument that returns the "HVAC" electric load, which is at the system timestep.  The modeling is based on average power levels for the duration of the timestep. The return values are converted from energy in Joules to power in Watts by dividing by the number of seconds in the zone timestep for building loads and by the system timestep for the HVAC loads.  Then the total facility power demand is the sum of the building loads and the HVAC loads. 
+
+\begin{equation}
+  P_{dmd} = P_{bldg,dmd} + P_{HVAC,dmd}
+\end{equation}
+
+When the electric power service device models described below are being used, they also make use of the meter reporting system using the components of the ElectricityProduced:Facility ( ResourceType=ElectricityProduced) meter to determine aggregate on-site electricity production rate, $P_{prod}$.  This value rolls up all the power generated and consumed by the on-site generators, storage, and power conversion equipment:
+
+\begin{itemize}
+  \item $P_{prod,cogen}$ is the power from fuel-fired generators, from meter Cogeneration:ElectricityProduced.
+  \item $P_{prod,pv}$ is the power from solar photovoltaics, from meter Photovoltaic:ElectricityProduced.
+  \item $P_{prod,wind}$ is the power from wind generators, from meter WindTurbine:ElectricityProduced.
+  \item $P_{prod,storage}$ is the power from electric storage, from meter ElectricStorage:ElectricityProduced, with storage charging negative and storage discharging positive.
+  \item $P_{prod,conversion}$ is the power loss by converting between different voltages or AC and DC, from meter PowerConversion:ElectricityProduced which are metered as negative values that decrease the amount of electricity produced.
+\end{itemize}
+
+\begin{equation}
+  {P_{prod}}= {P_{prod,cogen}} + {P_{prod,pv}} + {P_{prod,wind}} + {P_{prod,storage}} + {P_{prod,conversion}}
+\end{equation}
+
+Then the net purchased electricity, which can be either positive or negative (for export), is calculated using,
+
+\begin{equation}
+  {P_{net,purch}} = {P_{dmd}} - {P_{prod}}
+\end{equation}
+
+Only the positive portion of the net purchased power is the purchased power.
+
+\begin{equation}
+  {P_{purch}} = { max ( {P_{net,purch}}, 0.0 ) }
+\end{equation}
+
+The surplus electric power is exported out to the grid and is only positive. 
+
+\begin{equation}
+  {P_{surp}} =  { max ( ({P_{prod}} - {P_{dmd}}) , 0.0 ) }
+\end{equation}
+
+The energy versions of the power variables are calculated by multiplying the power level by the number of seconds in the system timestep. 
\ No newline at end of file
diff --git a/doc/engineering-reference/src/operational-faults.tex b/doc/engineering-reference/src/operational-faults.tex
new file mode 100644
index 00000000000..fbb346b16f4
--- /dev/null
+++ b/doc/engineering-reference/src/operational-faults.tex
@@ -0,0 +1,317 @@
+\chapter{Operational Faults}\label{operational-faults}
+
+\subsection{Introduction to Operational Faults Modeling}\label{introduction-to-operational-faults-modeling}
+
+Most of the buildings, either new or old, have operational faults in the sensors, controllers, meters, equipment and systems. Being able to model and simulate these faults and their impact on energy performance of buildings is crucial to improve accuracy of building simulations and to support the retrofit of buildings. To date, the main practitioner use of EnergyPlus has been for new construction design. With the new high priority attached by USDOE to retrofit and improved operation of existing buildings, there is a need to extend the capabilities of EnergyPlus to model existing buildings, including faulty operation:
+
+\begin{itemize}
+\tightlist
+\item
+  Retrofit analysis: starts with calibrated simulation; the ability to estimate the severity of common faults is expected to improve the accuracy and transparency of the calibrated model and hence the increase accuracy of the analysis of different retrofit measures.\\
+\item
+  Commissioning providers can use the fault models to demonstrate the saving to be expected from fixing faults found in retro-commissioning
+\item
+  Support for building operation by using the calibrated model, including unfixed faults, as a real-time reference model to detect, and verify the diagnosis of, newly occurring faults.
+\end{itemize}
+
+The users in these cases are practitioners, not power users, so it is needed to implement the fault models using conventional EnergyPlus objects rather than the EMS, which, in any case, could only be used to model limited types of faults.
+
+EnergyPlus contains a number of objects to model operational faults of sensors, meters, equipment and systems. The current implementation allows the modeling of the following fault types: (1) sensor faults with air economizers, (2) thermostat/humidistat offset faults, and (3) heating and cooling coil fouling faults.
+
+\subsection{Sensor Faults with Air Economizers}\label{sensor-faults-with-air-economizers}
+
+\subsubsection{Symptom}\label{symptom}
+
+The sensor readings deviate from the actual air conditions due to sensor offset, which leads to inappropriate operations of the air economizer and thus undesired resulting indoor conditions.
+
+\subsubsection{Modeling Approach}\label{modeling-approach}
+
+There are a number of sensors installed to support the air economizer operations. The sensors may be of different types. The objects used by EnergyPlus to model the sensor faults are as follows:
+
+\begin{itemize}
+\tightlist
+\item
+  FaultModel:TemperatureSensorOffset:OutdoorAir
+\item
+  FaultModel:HumiditySensorOffset:OutdoorAir
+\item
+  FaultModel:EnthalpySensorOffset:OutdoorAir
+\item
+  FaultModel:TemperatureSensorOffset:ReturnAir
+\item
+  FaultModel:EnthalpySensorOffset:ReturnAir
+\end{itemize}
+
+\subsection{Thermostat/Humidistat Offset}\label{thermostathumidistat-offset}
+
+\subsubsection{Symptom}\label{symptom-1}
+
+The zone air temperature/relative humidity readings deviate from the actual zone air conditions due to thermostat/humidistat offset, and thus leads to inappropriate operations of the HVAC system and undesired resulting indoor conditions.
+
+\subsubsection{Modeling Approach}\label{modeling-approach-1}
+
+The thermostat offset fault is described in the object FaultModel:ThermostatOffset, which refers to the object ZoneControl:Thermostat. The humidistat offset fault is described in the object FaultModel:HumidistatOffset, which refers to the object ZoneControl:Humidistat. The effect of an offset in a thermostat/humidistat whose sole use is for the calculation of difference between the set-points and the design values can be modeled as an equal and opposite offset in the thermostat/humidistat:
+
+\begin{equation}
+T_{s,f} = T_{s,ff}  - \Delta T
+\end{equation}
+
+\begin{equation}
+RH_{s,f} = RH_{s,ff}  - \Delta RH
+\end{equation}
+
+Where,
+
+\(T_{s,f}\) thermostat value in the faulty case, C
+
+\(T_{s,ff}\) thermostat value in the fault-free case (design value), C
+
+\(RH_{s,f}\) humidistat value in the faulty case,
+
+\(RH_{s,ff}\) humidistat value in the fault-free case (design value),
+
+\(\Delta T / \Delta RH\) difference between the thermostat/humidistat readings and the actual zone air conditions. Positive values mean that the readings is higher than the actual air conditions.
+
+For the humidistat that is independent of the thermostat, \(\Delta RH\) can be described by a pre-defined schedule. For the humidistat offset that is caused by the thermostat offset, \(\Delta RH\) is related with both the thermostat offset level as well as the indoor air conditions which are dynamic, and therefore cannot be described with a pre-defined schedule. In this case, the humidistat offset level is calculated each time step.
+
+\begin{equation}
+\Delta RH = RH_{s,ff} - f(T_{real}, W_{s,f})
+\end{equation}
+
+Where,
+
+\(T_{real}\) real-time temperature of the indoor air (real value), C
+
+\(W_{s,f}\) humidistat ratio corresponding to \(T_{real} - \Delta T and RH_{s,ff, kgWater/kgDryAir}\)
+
+Note that the thermostat/humidistat settings are related with two major processes within EnergyPlus: one is the design load calculations and HVAC system sizing, and the other is the HVAC system operations. Only the latter is affected by the thermostat/humidistat offset fault, while the former is not. Therefore, the size of the corresponding HVAC equipment in the faulty cases is the same as that in the fault-free cases.
+
+When EMS is used to overwrite the ZoneControl:Thermostat/ZoneControl:Humidistat values, the offsets are applied to the EMS values rather than the original Thermostat/Humidistat values.
+
+\subsection{Heating and Cooling Coil Fouling}\label{heating-and-cooling-coil-fouling}
+
+\subsubsection{Symptom}\label{symptom-2}
+
+Reduced overall heat transfer coefficient (UA) causes reduced coil capacity, resulting in unmet loads and/or increased water flow rate and decreased water side temperature difference (``low ΔT'' syndrome).
+
+\subsubsection{Modeling Approach}\label{modeling-approach-2}
+
+The coil fouling fault is described in the object FaultModel:Fouling:Coil. The fault model currently applies only to the `simple' water coils: Coil:Heating:Water and Coil:Cooling:Water. The FaultModel:Fouling:Coil object allows the user to describe the fouling information in either of the two methods: FouledUARated or FoulingFactor. Using FouledUARated method, user specifies the value of UAfouled directly. Using FoulingFactor method user specifies air/water side fouling factor, and the UAfouled value is further calculated via the equations shown below.
+
+\begin{equation}
+UA_{fouled} = [UA_{air} - 1  +  R_{foul}  + UA_{water} - 1]-1
+\end{equation}
+
+Where,
+
+\(U_{Aair}\) heat transfer coefficient of the coil on the air side, W/K
+
+\(UA_{fouled}\) overall heat transfer coefficient of the fouled coil, W/K
+
+\(UA_{water}\) heat transfer coefficient of the coil on the water side, W/K
+
+\(R_{foul}\) fouling factor, K/W
+
+\(R_{foul}\) is determined by:
+
+\begin{equation}
+R_{foul} = r_{air}/A_{air} + r_{water} / A_{water}
+\end{equation}
+
+Where,
+
+\(r_{air}\) Air side fouling factor, m2-K/W
+
+\(r_{water}\) Water side fouling factor, m2-K/W
+
+\(A_{air}\) Air side coil surface area, m2
+
+\(A_{water}\) Water side coil surface area, m2
+
+The pressure drop associated with the fouling is ignored in the current implementation.
+
+\subsection{Air Filter Fouling}\label{air-filter-fouling}
+
+\subsubsection{Symptom}\label{symptom-3}
+
+Increased air loop system resistance, resulting in a different system curve. This directly affects the operation of corresponding fans. More specifically, it may lead to variations of the fan pressure rise, fan energy consumption, as well as the enthalpy of the fan outlet air. It may also lead to a reduction in the airflow rate and thus affects the performance of other system components (e.g., heat transfer performance of heating/cooling coils).
+
+\subsubsection{Modeling Approach}\label{modeling-approach-3}
+
+The fouling air filter fault is described in the object FaultModel:Fouling:AirFilter, which refers to the fan objects that describe the associated fan. The fan object can be Fan:ConstantVolume, Fan:OnOff, or Fan:VariableVolume. The design pressure rise variations of the associated fan in the faulty cases are described by the Pressure Fraction Schedule specified in FaultModel:Fouling:AirFilter object, which is used as a multiplier to the fault-free fan design pressure rise specified in the fan object. The variations of the design air flow rate of the fan can then be calculated with the Pressure Fraction Schedule and Fan Curve. When EMS is used to overwrite the the pressure/MassFlow, the EMS values are used.
+
+The effect of the fouling air filter on the fan performance is related with a number of factors, including the fan types, fan curves, and system design and operating conditions. In general, there are three possible situations to be addressed in modeling dirty air filters:
+
+\textbf{(a) The required airflow rate can be maintained by the variable speed fan running at higher speed.}
+
+In this case, the fan operation state changes from point A (intersection of the fan curve corresponding to a lower speed and the system curve with clean filters) to point B (intersection of the fan curve corresponding to a higher speed and the system curve with dirty filters), as shown in Figure~\ref{fig:effect-of-dirty-air-filter-on-variable-speed}. Point B corresponds to a higher fan pressure rise than Point A, and the same air flow rate.
+
+\begin{figure}[hbtp] % fig 345
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image8006.png}
+\caption{Effect of dirty air filter on variable speed fan operation – flow rate maintained \protect \label{fig:effect-of-dirty-air-filter-on-variable-speed}}
+\end{figure}
+
+The required airflow rate m can be maintained while the fan pressure rise \(\Delta P\) is increased to \(\Delta P_{df}\) . This leads to higher fan power \(\dot Q_{tot,df}\) and higher power entering the air \(\dot Q_{toair,df}\) , and thus changes the specific enthalpies of the fan outlet air stream (\(h_{out,df}\) ).
+
+\begin{equation}
+f_{flow,df} = m / m_{design,df}
+\end{equation}
+
+\begin{equation}
+f_{pl,df} = c_{1} + c_{2}*f_{flow,df} + c_{3}*f_{flow,df}^2 + c_{4}*f_{flow,df}^3 + c_{5}*f_{flow,df}^4
+\end{equation}
+
+\begin{equation}
+\dot{Q}_{tot,df} = f_{pl,df} \times m_{design,df} \times \Delta P_{df} / (e_{tot} \times \rho_{air} )
+\end{equation}
+
+\begin{equation}
+\dot{Q}_{shaft,df} = e_{motor} \times \dot{Q}_{tot, df}
+\end{equation}
+
+\begin{equation}
+\dot{Q}_{toair,df} = \dot{Q}_{shaft,df} +( \dot{Q}_{tot,df} - \dot{Q}_{shaft,df}) \times f_{motortoair}
+\end{equation}
+
+\begin{equation}
+h_{out,df} = h_{in} + \dot{Q}_{toair,df} / m
+\end{equation}
+
+Where,
+
+\(e_{tot}\) is the motor efficiency;
+
+\(f_{flow}\) is the flow fraction or part-load ratio;
+
+\(f_{pl}\) is the part load factor;
+
+\(m\) is the air mass flow in kg/s;
+
+\(h_{in}\) is the inlet air stream specific enthalpies in J/kg;
+
+\(h_{out}\) is the outlet air stream specific enthalpies in J/kg;
+
+\(\dot{Q}_{tot}\) is the fan power in watts;
+
+\(\dot{Q}_{toair}\) is the power entering the air in watts;
+
+\(\dot{Q}_{shaft}\) is the fan shaft power in watts;
+
+\(\Delta P\) is the fan pressure increase in Pascal;
+
+\(_{design}\) is for the parameters in the design condition;
+
+\(_{df}\) is for the parameters in the dirty filter case.
+
+\textbf{(b) The variable speed fan cannot increase in speed sufficiently to maintain the required airflow rate.}
+
+In this case, the fan operation state changes from point A (intersection of the fan curve corresponding to a lower speed and the system curve with clean filters) to point B (intersection of the fan curve corresponding to a higher speed and the system curve with dirty filters), as shown in Figure~\ref{fig:effect-of-dirty-air-filter-on-variable-speed-001}. Point B corresponds to a higher fan pressure rise and a lower air flow rate than Point A.
+
+\begin{figure}[hbtp] % fig 346
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image8007.png}
+\caption{Effect of dirty air filter on variable speed fan operation – flow rate reduced \protect \label{fig:effect-of-dirty-air-filter-on-variable-speed-001}}
+\end{figure}
+
+The airflow rate m is reduced to \(m_{df}\) while the fan design pressure rise \(\Delta P\) is increased to \(\Delta P_{df}\). Similarly to case (a), the fan power (\(\dot Q_{tot}\) ), the power entering the air (\(\dot Q_{toair}\) ), and the specific enthalpies of the fan outlet air stream (\(h_{out}\) ) are all affected. Different from case (a), however, the fan power (\(\dot Q_{tot}\) ) may either increase or decrease, depending on the degree of the airflow rate decrease and pressure rise increase. Also note that \(f_{flow,df}\) is always 1 in this case, since the fan runs at its maximum speed.
+
+\begin{equation}
+f_{flow,df} = 1
+\end{equation}
+
+\begin{equation}
+f_{pl,df} = c_{1} + c_{2}*f_{flow,df} + c_{3}*f_{flow,df}^2 + c_{4}*f_{flow,df}^3 + c_{5}*f_{flow,df}^4
+\end{equation}
+
+\begin{equation}
+\dot{Q}_{tot,df} = f_{pl,df} \times m_{design,df} \times \Delta P_{df} / (e_{tot} \times \rho_{air} )
+\end{equation}
+
+\begin{equation}
+\dot{Q}_{shaft,df} = e_{motor} \times \dot{Q}_{tot, df}
+\end{equation}
+
+\begin{equation}
+\dot{Q}_{toair,df} = \dot{Q}_{shaft,df} +( \dot{Q}_{tot,df} - \dot{Q}_{shaft,df}) \times f_{motortoair}
+\end{equation}
+
+\begin{equation}
+h_{out,df} = h_{in} + \dot{Q}_{toair,df} / m_{design,df}
+\end{equation}
+
+Where,
+
+\(e_{tot}\) is the motor efficiency;
+
+\(f_{flow}\) is the flow fraction or part-load ratio;
+
+\(f_{pl}\) is the part load factor;
+
+\(m\) is the air mass flow in kg/s;
+
+\(h_{in}\) is the inlet air stream specific enthalpies in J/kg;
+
+\(h_{out}\) is the outlet air stream specific enthalpies in J/kg;
+
+\(\dot{Q}_{tot}\) is the fan power in watts;
+
+\(\dot{Q}_{toair}\) is the power entering the air in watts;
+
+\(\dot{Q}_{shaft}\) is the fan shaft power in watts;
+
+\(\Delta P\) is the fan pressure increase in Pascal;
+
+\(_{design}\) is for the parameters in the design condition;
+
+\(_{df}\) is for the parameters in the dirty filter case.
+
+\textbf{(c) The constant speed fan cannot maintain the design airflow rate.}
+
+In this case, the fan operation state changes from point A (intersection of the fan curve and the system curve with clean filters) to point B (intersection of the fan curve and the system curve with dirty filters), as shown in Figure~\ref{fig:effect-of-dirty-air-filter-on-constant-speed}. Point B corresponds to a higher fan pressure rise and a lower air flow rate than Point A.
+
+\begin{figure}[hbtp] % fig 347
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image8008.png}
+\caption{Effect of dirty air filter on constant speed fan operation \protect \label{fig:effect-of-dirty-air-filter-on-constant-speed}}
+\end{figure}
+
+Similarly to case (b), the airflow rate m is reduced to \(m_{df}\) while the fan pressure rise \(\Delta P\) is increased to \(\Delta P_{df}\) . This results in the variations of the fan power (\(\dot Q_{tot}\) ), the power entering the air (\(\dot Q_{toair}\) ), and the specific enthalpies of the fan outlet air stream (\(h_{out}\) ).
+
+\begin{equation}
+\dot{Q}_{tot,df} = m_{design,df} \times \Delta P_{df} / (e_{tot} \times \rho_{air} )
+\end{equation}
+
+\begin{equation}
+\dot{Q}_{shaft,df} = e_{motor} \times \dot{Q}_{tot, df}
+\end{equation}
+
+\begin{equation}
+\dot{Q}_{toair,df} = \dot{Q}_{shaft,df} +( \dot{Q}_{tot,df} - \dot{Q}_{shaft,df}) \times f_{motortoair}
+\end{equation}
+
+\begin{equation}
+h_{out,df} = h_{in} + \dot{Q}_{toair,df} / m_{design,df}
+\end{equation}
+
+Where,
+
+\(e_{tot}\) is the motor efficiency;
+
+\(m\) is the air mass flow in kg/s;
+
+\(h_{in}\) is the inlet air stream specific enthalpies in J/kg;
+
+\(h_{out}\) is the outlet air stream specific enthalpies in J/kg;
+
+\(\dot{Q}_{tot}\) is the fan power in watts;
+
+\(\dot{Q}_{toair}\) is the power entering the air in watts;
+
+\(\dot{Q}_{shaft}\) is the fan shaft power in watts;
+
+\(\Delta P\) is the fan pressure increase in Pascal;
+
+\(_{design}\) is for the parameters in the design condition;
+
+\(_{df}\) is for the parameters in the dirty filter case.
diff --git a/doc/engineering-reference/src/overview.tex b/doc/engineering-reference/src/overview.tex
new file mode 100644
index 00000000000..151c54dfc9b
--- /dev/null
+++ b/doc/engineering-reference/src/overview.tex
@@ -0,0 +1 @@
+\chapter{Overview}\label{overview-022}
diff --git a/doc/engineering-reference/src/overview/document-overview.tex b/doc/engineering-reference/src/overview/document-overview.tex
new file mode 100644
index 00000000000..5fcec731fa9
--- /dev/null
+++ b/doc/engineering-reference/src/overview/document-overview.tex
@@ -0,0 +1,8 @@
+\section{Document Overview}\label{document-overview}
+
+This document is organized to give you the best possible look into the EnergyPlus calculations. First, the concepts of modeling in EnergyPlus are presented. These include descriptions of the zone heat balance process, air loop/plant loop processes as well as other important processes for the building simulation.
+
+Discussions during the modeling process may reference specific ``object names'' as found in the Input/Output Reference document.
+
+The remainder of the document focuses on individual models.
+ 
diff --git a/doc/engineering-reference/src/overview/general-modeling-overview.tex b/doc/engineering-reference/src/overview/general-modeling-overview.tex
new file mode 100644
index 00000000000..2766dd10e3a
--- /dev/null
+++ b/doc/engineering-reference/src/overview/general-modeling-overview.tex
@@ -0,0 +1,10 @@
+\section{General Modeling Overview}\label{general-modeling-overview}
+
+The EnergyPlus program is a collection of many program modules that work together to calculate the energy required for heating and cooling a building using a variety of systems and energy sources. It does this by simulating the building and associated energy systems when they are exposed to different environmental and operating conditions. The core of the simulation is a model of the building that is based on fundamental heat balance principles. Since it is relatively meaningless to state: ``based on fundamental heat balance principles'', the model will be described in greater detail in later sections of this document in concert with the FORTRAN code which is used to describe the model. It turns out that the model itself is relatively simple compared with the data organization and control that is needed to simulate the great many combinations of system types, primary energy plant arrangements, schedules, and environments. The next section shows this overall organization in schematic form. Later sections will expand on the details within the blocks of the schematic.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image1.png}
+\caption{EnergyPlus Program Schematic \protect \label{fig:energyplus-program-schematic}}
+\end{figure}
+
diff --git a/doc/engineering-reference/src/overview/simulation-manager.tex b/doc/engineering-reference/src/overview/simulation-manager.tex
new file mode 100644
index 00000000000..bb40f30b63f
--- /dev/null
+++ b/doc/engineering-reference/src/overview/simulation-manager.tex
@@ -0,0 +1,79 @@
+\section{Simulation Manager}\label{simulation-manager}
+
+The simulation manager of EnergyPlus is contained in a single module. The main subroutine is shown below. Flow within the entire program is managed using a series of flags. These paired flags, in order (from the highest to the lowest) are:
+
+% table 1
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Simulation Flags \label{table:simulation-flags}} \tabularnewline
+\toprule
+\endfirsthead
+
+\caption[]{Simulation Flags} \tabularnewline
+\toprule
+\endhead
+
+BeginSimulationFlag & EndSimulationFlag \tabularnewline
+BeginEnvironmentFlag & EndEnvironmentFlag (one to many days) \tabularnewline
+BeginDayFlag & EndDayFlag \tabularnewline
+BeginHourFlag & EndHourFlag \tabularnewline
+BeginTimeStepFlag & EndTimeStepFlag \tabularnewline
+\bottomrule
+\end{longtable}
+
+There is also a \textbf{WarmupFlag} to signal that the program is in warmup state. The operation of these flags can be seen in the following subroutine. The advantage of using the flag system is that any subroutine throughout the code can determine the exact state of the simulation by checking the status of the flags.
+
+\begin{lstlisting}
+SUBROUTINE ManageSimulation     ! Main driver routine for this module
+BeginSimFlag = .TRUE.
+  EndSimFlag = .FALSE.
+  CALL OpenOutputFiles
+  CALL GetProjectData
+  CALL GetEnvironmentInfo                 ! Get the number and type of Environments
+  DO Envrn = 1, NumOfEnvrn        ! Begin environment loop ...
+    BeginEnvrnFlag = .TRUE.
+    EndEnvrnFlag   = .FALSE.
+    WarmupFlag     = .TRUE.
+    DayOfSim       =   0
+    DO WHILE ((DayOfSim.LT.NumOfDayInEnvrn).OR.(WarmupFlag))  ! Begin day loop ...
+      DayOfSim     = DayOfSim + 1
+      BeginDayFlag = .TRUE.
+      EndDayFlag   = .FALSE.
+      DO HourOfDay = 1, 24      ! Begin hour loop ...
+        BeginHourFlag = .TRUE.
+        EndHourFlag   = .FALSE.
+          DO TimeStep = 1, NumOfTimeStepInHour  ! Begin time step (TINC) loop ...
+          BeginTimeStepFlag = .TRUE.
+          EndTimeStepFlag   = .FALSE.
+          ! Set the End_Flag variables to true if necessary. Note that each flag builds on
+          ! the previous level. EndDayFlag cannot be .true. unless EndHourFlag is also .true.,
+          ! etc.
+          ! Note that the EndEnvrnFlag and the EndSimFlag cannot be set during warmup.
+          ! Note also that BeginTimeStepFlag, EndTimeStepFlag, and the
+          ! SubTimeStepFlags can/will be set/reset in the HVAC Manager.
+          IF ((TimeStep.EQ.NumOfTimeStepInHour)) THEN
+            EndHourFlag = .TRUE.
+            IF (HourOfDay.EQ.24) THEN
+              EndDayFlag = .TRUE.
+              IF ((.NOT.WarmupFlag).AND.(DayOfSim.EQ.NumOfDayInEnvrn)) THEN
+                EndEnvrnFlag = .TRUE.
+                IF (Envrn.EQ.NumOfEnvrn) THEN
+                  EndSimFlag = .TRUE.
+                END IF
+              END IF
+            END IF
+          END IF
+          CALL ManageWeather
+          CALL ManageHeatBalance
+          BeginHourFlag  = .FALSE.
+          BeginDayFlag   = .FALSE.
+          BeginEnvrnFlag = .FALSE.
+          BeginSimFlag   = .FALSE.
+        END DO                              ! ... End time step (TINC) loop.
+      END DO                    ! ... End hour loop.
+    END DO                      ! ... End day loop.
+  END DO                        ! ... End environment loop.
+  CALL CloseOutputFiles
+  RETURN
+END SUBROUTINE ManageSimulation
+\end{lstlisting}
+
diff --git a/doc/engineering-reference/src/overview/warmup-convergence.tex b/doc/engineering-reference/src/overview/warmup-convergence.tex
new file mode 100644
index 00000000000..68a58ae6307
--- /dev/null
+++ b/doc/engineering-reference/src/overview/warmup-convergence.tex
@@ -0,0 +1,33 @@
+\section{Warmup Convergence}\label{warmup-convergence}
+
+At the beginning of each new environment (design day or runperiod) zone and surface temperatures are initialized to 23C, and zone humidity ratios are initialized to the outdoor humidity ratio. The first day of the environment is repeated until the loads/temperature convergence tolerance values specified in the Building object are satisfied or until it reaches ``maximum number of warmup days''.
+
+Since everything in EnergyPlus is based on the foundation of the loads simulation, it stands to reason that any inaccuracies in the loads calculation will result in inaccuracies of similar or larger magnitude in the HVAC calculations. In the presumably limited cases where convergence was not truly achieved before the actual simulation began, it is unknown how much error would be introduced into the results. While simulations that last longer (annual vs.~design day) will hopefully have any initial condition problems balanced by the shear number of days in the simulation, shorter simulations---particularly those used for sizing---could result in relatively large errors. The simulation results could be unreliable and inaccurate when steady periodic conditions are not achieved. Therefore, it is important to properly determine when there is enough temperature and flux history terms to start an EnergyPlus simulation since this has a potential economic and energy impact on buildings that use EnergyPlus in design.
+
+EnergyPlus determines warmup convergence in the following manner as shown in the Figure~\ref{fig:flows-of-warmup-convergence-checks} below. The process of the convergence checks begins by tracking four parameters such including the maximum zone air temperature, the minimum zone air temperature, the maximum heating load, and the maximum cooling load for individual zone. It is note that these convergence checks are only in effective in simulations with at least one zone since the criteria is solely based on the maximum and minimum values obtained from an individual zone. Differences in these parameters between two consecutive days are then compared with the convergence tolerance values at the end of the day during the warmup period. For example, the maximum and minimum air temperature and the percentage difference of zone load for each zone at 9:00AM during the second to last warmup is compared to the values at 9:00AM last warmup day as follows:
+
+\begin{equation}
+{T_{\max ,prev}} - {T_{\max }} < {T_{tol}}
+\end{equation}
+
+\begin{equation}
+{T_{\min ,prev}} - {T_{\min }} < {T_{tol}}
+\end{equation}
+
+\begin{equation}
+\frac{{{q_h} - {q_{h,prev}}}}{{{q_h}}} < {q_{tol}}
+\end{equation}
+
+\begin{equation}
+\frac{{{q_c} - {q_{c,prev}}}}{{{q_c}}} < {q_{tol}}
+\end{equation}
+
+where Tmax,prev is the maximum zone temperature of previous day, Tmax is the maximum zone temperature of current day, Ttol is the value of temperature tolerance, qh,prev is the maximum heating load of previous day, qh, is the maximum heating load of current day, qtol is the value of load tolerance, qc,prev is the maximum cooling load of previous day, and qc, is the maximum cooling load of current day.
+
+Note that a minimum load of 100W is used to establish a fraction for the maximum loads when they are less than the minimum. This is done to avoid a false negative indication for the percentage load difference that may appear when zonal loads are very small. The convergence checks are repeated until passed for all zones. EnergyPlus assumes that the warmup period has been reached steady-periodic when these four parameters are within tolerance. Finally, temperature and load differences between the last two warmup days for individual zone at each time step in the last warmup day are reported so that users can easily track whether or not the warmup period has converged. The input parameters and output related to the warmup period are discussed in the Input-Output Reference.
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6.png}
+\caption{Flows of Warmup Convergence Checks \protect \label{fig:flows-of-warmup-convergence-checks}}
+\end{figure}
diff --git a/doc/engineering-reference/src/performance-curves-and-lookup-tables.tex b/doc/engineering-reference/src/performance-curves-and-lookup-tables.tex
new file mode 100644
index 00000000000..ed975c406f7
--- /dev/null
+++ b/doc/engineering-reference/src/performance-curves-and-lookup-tables.tex
@@ -0,0 +1,7 @@
+\chapter{Performance Curves and Lookup Tables}\label{performance-curves-and-lookup-tables}
+
+The following section describes the use of performance curves and lookup tables. Each of these objects may be used in any valid input field where a performance curve name is required.
+
+Performance curves are used directly to simulate the performance of HVAC equipment. The curves are typically created by performing a regression analysis on tabular data for a particular equipment performance metric. The regression analysis determines the equation coefficients which are the primary input to all performance curve objects. Performance tables are similar to performance curves in that they are meant to replicate a particular performance curve. Input to performance tables are made up of data pairs, the same data pairs that would be used to create performance curve coefficients. Performance tables can be interpolated using up to a 4\(^{th}\) order polynomial equation for one independent variable tables or using a 2\(^{nd}\) order polynomial for two independent variable tables. A regression analysis can be performed on performance tables when the simulation is instructed to use the regression analysis during the simulation (i.e., ride the curve). In addition, a performance curve object is created that can be used in future simulations and can be written to the eio file. The performance curve is written to the eio file only when the diagnostics flag is set to DisplayAdvancedReportVariables (ref. Output:Diagnostics, DisplayAdvancedReportVariables;). Lookup tables are similar to performance tables in that tabular data is used for input, however, the input 1) is more compact, 2) a regression analysis may only be performed for one and two independent variable cases, and 3) the tabular data can be read from an external file.
+
+Performance curves and data tables are created using empirical data that are derived from information gathered through observation, experience, or experimental means. Once a curve or table object is defined, these objects can be used to generically describe HVAC equipment performance. Performance curves and performance tables may be used interchangeably in Energyplus objects as required.
diff --git a/doc/engineering-reference/src/performance-curves-and-lookup-tables/performance-curves.tex b/doc/engineering-reference/src/performance-curves-and-lookup-tables/performance-curves.tex
new file mode 100644
index 00000000000..458e6b9c42d
--- /dev/null
+++ b/doc/engineering-reference/src/performance-curves-and-lookup-tables/performance-curves.tex
@@ -0,0 +1,178 @@
+\section{Performance Curves}\label{performance-curves-000}
+
+Performance curves define a polynomial equation which represents a conditional response to a model input. A polynomial is a mathematical expression which uses a sum of powers in one or more variables. The equation below represents an n\(^{th}\) order univariate polynomial. The highest power in the equation represents its order or degree (n).
+
+\begin{equation}
+y = {a_0} + {a_1}x + {a_2}{x^2} + {a_3}{x^3} + ... + {a_n}{x^n}
+\end{equation}
+
+A polynomial in two independent variables (multi-variate) is given by:
+
+\begin{equation}
+z = {a_{00}} + {a_{10}}x + {a_{01}}y + {a_{11}}xy + {a_{21}}{x^2}y + {a_{12}}x{y^2} + {a_{22}}{x^2}{y^2}... + {a_{nm}}{x^n}{y^m}
+\end{equation}
+
+In Energyplus, the result of an equation, the dependent variable, represents the response a system or component has given an input (the independent variable) to the system or component model. This response represents the equipment performance related to the mechanism that causes this change (e.g., the change in capacity or power based on a conditional change in temperature, part-load ratio, or other phenomenon). A variety of performance curves are available to describe the most common forms of engineering equations. The coefficients (a-z) in the following equations are entered in the associated curve object to define a specific phenomenon. Minimum and maximum limits may be applied to both the independent and the dependent variables as necessary.
+
+\subsection{Curves based on a single independent variable}\label{curves-based-on-a-single-independent-variable}
+
+A polynomial having only a single independent variable represents a one-dimensional relationship between a condition (the model input) and response (the model output). The previously described n\(^{th}\) order univariate polynomial is representative of the following performance curves.
+
+\subsubsection{Linear Curves}\label{linear-curves}
+
+A performance curve having an order or degree of 1.
+
+\begin{equation}
+y = a + bx
+\end{equation}
+
+\subsubsection{Quadratic Curves}\label{quadratic-curves}
+
+A performance curve having an order or degree of 2.
+
+\begin{equation}
+y = a + bx + c{x^2}
+\end{equation}
+
+\subsubsection{Cubic Curves}\label{cubic-curves}
+
+A performance curve having an order or degree of 3.
+
+\begin{equation}
+y = a + bx + c{x^2} + d{x^3}
+\end{equation}
+
+\subsubsection{Quartic Curves}\label{quartic-curves}
+
+A performance curve having an order or degree of 4.
+
+\begin{equation}
+y = a + bx + c{x^2} + d{x^3} + e{x^4}
+\end{equation}
+
+\subsubsection{Exponent Curves}\label{exponent-curves}
+
+A performance curve having an order or degree of c.
+
+\begin{equation}
+y = a + b{x^c}
+\end{equation}
+
+\subsection{Curves based on two independent variables}\label{curves-based-on-two-independent-variables}
+
+A polynomial having two independent variables represents a two-dimensional relationship between a condition (the model inputs) and response (the model output). The previously described n\(^{th}\) order multi-variate polynomial is representative of the following performance curves.
+
+\subsubsection{QuadraticLinear Curves}\label{quadraticlinear-curves}
+
+A performance curve having an order or degree of 2 in two independent variables.
+
+\begin{equation}
+z = a + bx + c{x^2} + dy + exy + f{x^2}y
+\end{equation}
+
+\subsubsection{CubicLinear Curves}\label{cubiclinear-curves}
+
+A performance curve having an order or degree of 3 in two independent variables.
+
+\begin{equation}
+z = a + bx + c{x^2} + d{x^3} + ey + fxy
+\end{equation}
+
+\subsubsection{BiQuadratic Curves}\label{biquadratic-curves}
+
+A performance curve having an order or degree of 2 in two independent variables.
+
+\begin{equation}
+z = a + bx + c{x^2} + dy + e{y^2} + fxy
+\end{equation}
+
+\subsubsection{BiCubic Curves}\label{bicubic-curves}
+
+A performance curve having an order or degree of 3 in two independent variables.
+
+\begin{equation}
+z = a + bx + c{x^2} + dy + e{y^2} + fxy + g{x^3} + h{y^3} + i{x^2}y
+\end{equation}
+
+Calulating performance curve coefficients in a spreadsheet is a simple matter of finding the data required to perform the regression analysis. For example, the biquadratic equation shown above is representative of the cooling capacity as a function of temperature performance curve for DX cooling coils. The fundamental equation for DX cooling coil capacity is:
+
+\begin{equation}
+TotCapTempModFac = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d\left( {{T_{c,i}}} \right) + e{\left( {{T_{c,i}}} \right)^2} + f\left( {{T_{wb,i}}} \right)\left( {{T_{c,i}}} \right)
+\end{equation}
+
+where
+
+Twb,i = wet-bulb temperature of the air entering the cooling coil, °C
+
+Tc,i (or Tdb,i) = dry-bulb temperature of the air entering an air-cooled condenser, °C
+
+Given the data set shown in the table below, each of the independent variables would be calculated according to the fundamental equation above (i.e., the T, T\(^{2}\), and cross-product terms would be multiplied out). The data would be converted to degrees celcius and the cooling capacity would be converted to Watts. The data would also be normalized using the ARI rating point shown as highlighted in the table.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image7865.png}
+\caption{DataTable}
+\end{figure}
+
+The fundamental equation would be used to determine the number of independent variables and also the form of the equation. Given the example described here, the spreadsheet would be set up to look like the equation as shown in the following table. A regression analysis could then be performed on the data set. The first five columns are the independent variables and the last column is the dependent variable. A spreadsheet tool is selected to perform the regression analysis, and the coefficients are calculated and displayed in the spreadsheet.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image7866.png}
+\caption{RegressionAnalysis}
+\end{figure}
+
+The regression analysis and summary statistical output is shown below. The equation coefficients are shown highlighted. In this example, the equation coefficents are: a = 0.757382, b = 0.014666, c = 0.000459, d = -0.00095, e = -6.7E-05, and f = -0.00015. These coefficients would be entered in a Curve:BiQuadratic object and used to describe the cooling capacity as a function of temperature for the DX cooling coil model. Minimum and Maximum values from the tabular data are entered as Min/Max values for the curve object. The values may be relaxed slightly with care to allow extrapolation as needed. A performance table may be used to automatically perform the regression analysis as described in the following section.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image7867.png}
+\caption{RegressionSummaryOutput}
+\end{figure}
+
+\begin{lstlisting}
+
+  Curve:Biquadratic,
+      CoolCapFTExample,        !- Name
+      0.757382,                !- Coefficient1 Constant
+      0.014666,                !- Coefficient2 x
+      0.000459,                !- Coefficient3 x**2
+      -0.00095,                !- Coefficient4 y
+      -0.000067,               !- Coefficient5 y**2
+      -0.00015,                !- Coefficient6 x*y
+      17.22222,                !- Minimum Value of x
+      21.66667,                !- Maximum Value of x
+      18.33333,                !- Minimum Value of y
+      46.11111,                !- Maximum Value of y
+      ,                        !- Minimum Curve Output
+      ,                        !- Maximum Curve Output
+      Temperature,             !- Input Unit Type for X
+      Temperature,             !- Input Unit Type for Y
+      Dimensionless;           !- Output Unit Type
+\end{lstlisting}
+
+\subsection{Curves based on three independent variables}\label{curves-based-on-three-independent-variables}
+
+A polynomial having three independent variables represents a three-dimensional relationship between a condition (the model inputs) and response (the model output).
+
+\subsubsection{TriQuadratic Curves}\label{triquadratic-curves}
+
+A performance curve having an order or degree of 2 in three independent variables.
+
+\begin{equation}
+\begin{array}{ll}
+Output &= a + bx^2 + cx + dy^2 + ey + fz^2 + gz + hx^2y^2 + ixy + jxy^2 + kx^2y \\
+       &+ lx^2z^2 + mxz + nxz^2 + ox^2z + py^2z^2 + qyz + ryz^2 + sy^2z + tx^2y^2z^2 \\
+       &+ ux^2y^2z + ux^2yz^2 + vxy^2z^2 + wx^2yz + x\PB{xy^2z} + y\PB{xyz^2} + z\PB{xyz}
+\end{array}
+\end{equation}
+
+\subsection{Pressure drop curve}\label{pressure-drop-curve}
+
+\subsubsection{Functional Pressure Drop Curve}\label{functional-pressure-drop-curve}
+
+A performance curve representing the minor loss and/or friction calculations in plant pressure simulations.
+
+\begin{equation}
+\Delta P = \left[ {K + f\left( {L/D} \right)} \right]\left( {\rho {V^2}} \right)/2
+\end{equation}
diff --git a/doc/engineering-reference/src/performance-curves-and-lookup-tables/performance-tables.tex b/doc/engineering-reference/src/performance-curves-and-lookup-tables/performance-tables.tex
new file mode 100644
index 00000000000..f631888608c
--- /dev/null
+++ b/doc/engineering-reference/src/performance-curves-and-lookup-tables/performance-tables.tex
@@ -0,0 +1,290 @@
+\section{Performance Tables}\label{performance-tables}
+
+Performance tables provide a method to enter specific performance data in tabular form. Tabular data represent equipment performance in a manner similar to performance curves, however, the necessity to formulate the equation coefficient is not required. Tabular data may be used to directly interpolate the actual data within the tables independent variable limits or a regression analysis may be performed to calculate the equation coefficients and use these coefficients for the associated engineering calculations. When direct interpolation is selected, the tabular data is interpolated linearly between the first independent variable and then, if used, the second independent variable. The name of a table object may be used interchangeably in any valid field where a performance curve name is required.
+
+\subsection{Tables based on a single independent variable}\label{tables-based-on-a-single-independent-variable}
+
+The tabular data entered for polynomials with a single independent variable represent x and outupt data pairs as described in the previous section for performance curves.~ The x in each of the previous equations represent the independent variable (model input) and the output represents the dependent variable. The data pairs are organized as the data point for the independent variable followed by the data point for the dependent variable. The data pairs form a one-dimensional array that may either be linearly interpolated, interpolated based on a polynomial equation, or this data may be used to calculate the equation coefficients (a-e) as described in the previous section.
+
+The equation form is user selected as either linear, quadratic, cubic, quartic, or exponent. This choice determines: 1) where this table object may be used (i.e., certain objects may required a specific form of the equation), and 2) the degree or order used to calculate the regression coefficients. The following example describes the methodology used when tabular input data is used in place of common performance curve objects. Although Energyplus does not use a performance curve in the manner described in this example, this example is ideally suited for teaching the basics of tabular data entry.
+
+Given a generic manufacturers fan data for a fan having a maximum flow rate of 5 m3/s and power of 125 W, the power is shown in the table below to be proportional to the cube of flow rate. Since, in this example, the flow rate is not a valid input for calculating fan power, the flow rate will be converted to flow fraction (or PLR). The power data is entered as the actual fan power and will be normalized by the program according to the maximum power of 125W. Also shown here are the performance curve outputs using the regression coefficients calculated by the program. The performance curve outputs represent the fan power ratio as a function of flow fraction. Additional significant digits are included to show the impact a given data set may have on the resulting coefficients (i.e., not quite 0 at the zero crossing, rounding causes slight errors in the actual coefficient values, etc).
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.2in}p{1.8in}}
+\toprule 
+Air Flow (m3/s) & Flow Fraction~ or Fan PLR & Power (W) & Power Ratio Curve Output \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule
+Air Flow (m3/s) & Flow Fraction~ or Fan PLR & Power (W) & Power Ratio Curve Output \tabularnewline
+\midrule
+\endhead
+
+0 & 0 & 0 & -1.1102230246E-16 \tabularnewline
+0.5 & 0.1 & 0.125 & 0.00100000000000018 \tabularnewline
+1 & 0.2 & 1 & 0.00800000000000004 \tabularnewline
+3 & 0.6 & 27 & 0.215999999999995 \tabularnewline
+4 & 0.8 & 64 & 0.51199999999999 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The tabular data can be entered directly into a table object. The data for flow fraction (or fan part-load ratio) and power are entered as data pairs. As this example describes how the fan power changes with changes in air flow, the curve type selected is Cubic and, therefore, the minimum number of data pairs equals 4 (i.e., number of coefficients in a cubic equation) although 5 are used in this example. In addition, since calculating regression coefficients for this data set would yield more accurate results than linearly interpolating this data set, the selection is made to evaluate the curve to the limits specified. In this example, the fan in question is capable of operating up to 5 m3/s at 125 Watts (which is purposely not provided in this set of tabular data). We need this information because we want to create a fan power ratio equation with an input of 0-1 for fan part-load ratio and a table output of 0-1 for fan power ratio. Therefore, the tabular data need to be normalized at a part-load ratio of 1 (i.e., normalized to the power at full flow). The following table object describes the input necessary for this particular data set.
+
+\begin{lstlisting}
+
+Table:OneIndependentVariable,
+  MyFanPower,   !- Name  [Fit from catalog performance data]
+  Cubic,     !- Curve Type
+  EvaluateCurveToLimits,  !- Interpolation Type
+  0,         !- Minimum Value of X1,
+  1,         !- Maximum Value of X1,
+  0,         !- Minimum Table Output
+  64,        !- Maximum Table Output
+  Dimensionless,  !- Input Unit Type for X1
+  Dimensionless,  !- Output Unit Type
+  125,       !- Normalization Point
+  0.8,64,    !- X Value #1, Output Value #1
+  0,0.0,     !- X Value #2, Output Value #2
+  0.2,1,     !- X Value #3, Output Value #3
+  0.1,0.125, !- X Value #4, Output Value #4
+  0.6,27;    !- X Value #5, Output Value #5
+\end{lstlisting}
+
+Notice in this example that:
+
+1)~~~~The data pairs do not need to be entered in ascending order, this data set will automatically be re-ordered in ascending order by the program.
+
+2)~~~~The minimum and maximum table output entered by the user uses the same units as the output values and are subsequently normalized in the same manner as the dependent variable in the data pairs.
+
+3)~~~~For the resulting curve object (see below), the minimum (maximum) limits are based on the lesser (greater) of the user entered value and the lower (upper) limit of the tabular data. When linearly interpolating tabular data, the limits of the data set are used unless the user entered maximum is more restrictive (e.g., 64 W in this example is not more restrictive than the data set).
+
+4)~~~~For the resulting curve object, the calculated coefficients may not perfectly represent the data set (i.e., in this example coefficient 1, 2, and 3 should have been 0). Duplicating the 0,0 data pair four additional times (to weight the 0 crossing) yields constant coefficients of 0. This could also be changed manually in the curve object created by the program.
+
+5)~~~~Referring to the figure below, a selection of LinearInterpolationOfTable would interpolate the tabular data within the limits of the data set (blue circles) resulting in a maximum X and Curve value of 0.8 and 0.512 (i.e., 64/125), respectively. Selecting EvaluateCurveToLimits allows extrapolation of the data set up to a power ratio of 1 had 125 W been entered as the maximum table output in this example.
+
+6)~~~~In the graph below, the linearly interpolated tabular data (blue line) represent a less accurate fan power ratio curve than the performance curve itself (red line). In this specific example, it is more accurate to rely on the performance curve results (i.e., Interpolation Type = EvaluateCurveToLimits in table object). In addition, the performance curve is able to extrapolate outside the limits of the data set since the regression analysis provides a smooth continuous curve through 1. Selecting the LagrangeInterpolationLinearExtrapolation interpolation method with a cubic curve type is similar to the performance curve results.
+
+7)~~~~Including additional data in the table object (e.g., data points for flow fractions = 0.4 and 1) would allow direct linear interpolation of the tabular data without significant loss of accuracy compared to the performance curve or lagrange methods.
+
+Curve output in eio file (when using Output:Diagnostics, DisplayAdvancedReportVariables):
+
+\begin{lstlisting}
+!...GENERATING NEW CURVE OBJECT
+! Input as Table:OneIndependentVariable "MYFANPOWER"
+! RSquared = 1.0000000000
+! Standard Error = 7.3549798168E-016
+! Degrees of Freedom = 5
+Curve:Cubic,
+ MYFANPOWER,         !- Name
+ -1.1102230246E-016, !- Coefficient1 Constant
+ 5.0571599639E-015,  !- Coefficient2 x
+ -2.1582431250E-014, !- Coefficient3 x**2
+ 1.0000000000,       !- Coefficient3 x**3
+ 0.0000000000,       !- Minimum Value of x
+ 1.0000000000,       !- Maximum Value of x
+ 0.0000000000,       !- Minimum Curve Output
+ 1.0000000000;       !- Maximum Curve Output
+!...END GENERATING NEW CURVE OBJECT
+\end{lstlisting}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image7870.png}
+\caption{FanPowerRatioExample}
+\end{figure}
+
+\subsection{Tables based on two independent variables}\label{tables-based-on-two-independent-variables}
+
+The tabular data entered for polynomials with two independent variables represent x, y and output data pairs as described in the previous section for performance curves.~ The x and y in each of the previous equations represent the independent variables (model inputs) and the output represents the dependent variable. The data pairs are organized as the data points for the independent variables followed by the data point for the dependent variable. The order of the data is significant in that the x and y data are entered in the same order as shown in the model's fundamental equation. The data pairs form a two-dimensional array that may either be linearly interpolated, interpolated using a second order polynomial, or this data may be used to calculate the equation coefficients (a-f) as described in the previous section.
+
+The equation order or degree is user selected as biquadratic or quadraticlinear. This choice determines: 1) where this table object may be used (i.e., certain objects may required a specific form of the equation), and 2) the fundamental equation used to calculate the regression coefficients. The following example describes the methodology used when tabular input data is used in place of common performance curve objects.
+
+Given a generic manufacturers air conditioner data for an AC system having a rated total cooling capacity of 7735.1 W, the change in capacity is shown in the table to be a function of both cooling coil entering air wet-bulb temperature and condenser entering air dry-bulb temperature. The tabular data is entered as the actual cooling capacity and will be normalized by the program according to the rated capacity of 7735.1 W. The cooling coil EIR curve could be developed in a similar fashion, except that EIR (Power / TotCap) must first be calculated from the tabular data below BEFORE entering this data into a table object. In this example, only data highlighted in yellow will be used.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image7871.png}
+\caption{NormalizedCapacity}
+\end{figure}
+
+The tabular data can be entered directly into a table object. As an example, for an air-cooled DX cooling coil object in Energyplus, the capacity as a function of temperature has the following fundamental equation (Ref. Single-Speed Electric DX Air Cooling Coil):
+
+\begin{equation}
+TotCapTempModFac = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d\left( {{T_{c,i}}} \right) + e{\left( {{T_{c,i}}} \right)^2} + f\left( {{T_{wb,i}}} \right)\left( {{T_{c,i}}} \right)
+\end{equation}
+
+where
+
+Twb,i = wet-bulb temperature of the air entering the cooling coil, °C
+
+Tc,i = dry-bulb temperature of the air entering an air-cooled condenser, °C
+
+Given this form of the fundamental equation, the data pairs for the cooling coil are entered as entering air wet-bulb temperature, condenser entering dry-bulb temperature, and total cooling capacity. These 3 values, in this precise order, make up each data pair. As this example describes how the DX coil cooling capacity changes with changes in indoor and outdoor temperature, the curve type selected is BiQuadratic and, therefore, the minimum number of data pairs equals 6 (i.e., number of coefficients in the equation above). Evaluating this tabular data based on regression coefficients may be less desirable to the user since the data in the lower right corner of the table is somewhat flat due to controls or other hardware constraints. For the sake of this example, the regression analysis is chosen. In this example, the DX cooling coil total cooling capacity at the ARI rating point is used to normalize the capacity data (e.g., 7735.1 W at 19.4 °C EWB and 35 °C outdoor dry-bulb temperature). In addition, the minimum and maximum limits are chosen such that extrapolation of the performance curve is allowed. Notice in the example below that:
+
+1)~~~~The data pairs do not need to be entered in ascending order, this data set will automatically be re-ordered in ascending order by the program.
+
+2)~~~~As shown in the table object below, only three of the five entries for entering air wet-bulb temperature were entered in the table object and therefore used for the regression analysis. This data entry technique may save time when entering a large data set, however, it may have unforeseen consequences on the resulting regression coefficients (i.e., the coefficients may provide less accuracy than desired). Note in the figure below the difference between the manufacturers data at 19.4 °C entering air wet-bulb temperature vs the prediction made by the regression coefficients. Since this data set (i.e., the 4 data points at 19.4°C entering air wet-bulb temperature from the table above) was left out of the regression analysis, the predicted capacity at this condition is slightly under-estimated.
+
+3)~~~~The minimum and maximum table output entered by the user uses the same units as the output values and are subsequently normalized in the same manner as the dependent variable in the data pairs.
+
+4)~~~~For the resulting curve object, the minimum (maximum) limits are based on the lesser (greater) of the user entered value and the lower (upper) limit of the tabular data. When linearly interpolating tabular data, only the limits of the data set are used.
+
+5)~~~~For the resulting curve object, the calculated coefficients may not perfectly represent the entire data set since all data was not used (i.e., in this example the regressed data do not line up exactly with all the manufacturers data, however, do line up well with the data included in the table object).
+
+6)~~~~Selecting LinearInterpolationOfTable would interpolate the tabular data within the limits of the data set (characters) resulting in a maximum X1, X2 and Curve value of 22.2, 40.8 and 1.25 (i.e., 9206.0/7375.1), respectively. Note how these maximum values compare to the maximum values in the generated curve object below which chose the EvaluateCurveToLimits option instead (i.e., the user min/max inputs were used to generate these fields when creating the curve object). The minimum values would be affected in a similar manner. Selecting Lagrange or EvaluateCurveToLimits allows extrapolation of the data set to values specified by the user.
+
+7)~~~~In the graph below, the linearly interpolated tabular data (character data set representing manufacturers data) may better represent the capacity ratio than the performance curve (lines representing the regressed data) given the non-linear relationship between capacity and temperature shown in the table and/or graph. However, extrapolation of the data set is performed linearly and the second order affects of temperature would be lost when extrapolating. Either the data set would be expanded to include other relevant data (e.g., data at colder outdoor temperatures where cooling may be required) which could then be interpolated or additional existing data could be added to the table object to allow more accurate regression coefficients to be used to predict data outside the table data limits.
+
+\begin{lstlisting}
+
+Table:TwoIndependentVariables,
+  CCoolCapFT,       !- Name  [Fit from catalog performance data]
+  BiQuadratic,      !- Curve Type
+  EvaluateCurveToLimits,  !- Interpolation Type
+  1,                !- Minimum Value of x,
+  30,               !- Maximum Value of x,
+  5,                !- Minimum Value of y,
+  50,               !- Maximum Value of y,
+  4500,             !- Minimum Table Output
+  15000,            !- Maximum Table Output
+  Temperature,      !- Input Unit Type for x
+  Temperature,      !- Input Unit Type for y
+  Dimensionless,    !- Output Unit Type
+  7735.1,           !- Normalization Point
+  17.2,29.4,7462.6, !- X, Y, and Output data pair #1
+  17.2,23.9,7735.1, !- X, Y, and Output data pair #2
+  13.9,29.4,7283.9, !- X, Y, and Output data pair #3
+  13.9,23.9,7474.4, !- X, Y, and Output data pair #4
+  13.9,35,7067.1,   !- X, Y, and Output data pair #5
+  13.9,40.8,6818.0, !- X, Y, and Output data pair #6
+  17.2,35,7157.9,   !- X, Y, and Output data pair #7
+  17.2,40.8,6818.0, !- X, Y, and Output data pair #8
+  22.2,35,8552.6,   !- X, Y, and Output data pair #9
+  22.2,29.4,8898.3, !- X, Y, and Output data pair #10
+  22.2,23.9,9206.0, !- X, Y, and Output data pair #11
+  22.2,40.8,8165.8; !- X, Y, and Output data pair #12
+\end{lstlisting}
+
+Curve output in eio file (when using Output:Diagnostics, DisplayAdvancedReportVariables):
+
+\begin{lstlisting}
+CREATING NEW CURVE OBJECT
+! Input as Table:TwoIndependentVariables "CCOOLCAPFT"
+! RSquared       = 0.9993993101
+! Standard Error = 3.4649248573E-003
+! Sample Size    = 12
+Curve:BiQuadratic,
+FromTable_CCOOLCAPFT,  !- Name
+  1.7214120578,  !- Coefficient1 Constant
+  -0.1011737262,  !- Coefficient2 x
+  3.7738833967E-003,  !- Coefficient3 x**2
+  2.8686934910E-003,  !- Coefficient4 y
+  -5.3785351258E-005,  !- Coefficient5 y**2
+  -3.4086036156E-004,  !- Coefficient6 x*y
+  1.0000000000,  !- Minimum Value of x
+  30.0000000000,  !- Maximum Value of x
+   5.0000000000,  !- Minimum Value of y
+  50.0000000000,  !- Maximum Value of y
+  0.5817636488,  !- Minimum Curve Output
+  1.9392121627;  !- Maximum Curve Output
+END CREATING NEW CURVE OBJECT
+\end{lstlisting}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image7873.png}
+\caption{NormalizedCapacity}
+\end{figure}
+
+\subsection{Lookup Tables}\label{lookup-tables}
+
+Lookup tables provide a method to evaluate a group of data that may or may not conform to a fundamental equation. Only tabular data which conform to existing performance curve equations are currently allowed (i.e., that lookup table name is entered where any valid performance curve is allowed therefore the table data must conform to the models fundamental equation for that specific curve). Efforts to include this lookup table in the energy management system would allow custom use of lookup tables, however, calling lookup tables from the EMS system is not currenly possible. Lookup tables can interpolate the actual data using a non-linear polynomial equation (order higher than 1). As with other table or curve objects, the lookup table can be used anywhere a valid curve object name is allowed. Care must be taken to ensure the table data format is consistent with the associate model that is using the performance curve (e.g., DX cooling coil capacity as a function of temperature where independent variable X1 = indoor wet-bulb temperature and independent variable X2 = outdoor dry-bulb temperature).
+
+The lookup tables are evaluated using the Lagrange form of the interpolation polynomial or the previously described interpolation methods of LinearInterpolationOfTable and EvaluateCurveToLimits. When using the Lagrange method, the number of points used in the interpolation is equal to 1 plus the polynomial order (e.g., a second order interpolation would use 3 points).
+
+\begin{equation}
+{p_n}\left( x \right) = \sum\limits_{i = 0}^n {{y_i}{l_i}\left( x \right)}
+\end{equation}
+
+\begin{equation}
+{l_i}\left( x \right) = \mathop \Pi \limits_{j \ne i} \left( {\frac{{x - {x_j}}}{{{x_i} - {x_j}}}} \right)\,\,\,\,\,\,i = 0,1,...,n
+\end{equation}
+
+First-order Lagrange interpolation polynomial:
+
+\begin{equation}
+{p_1}\left( x \right) = \frac{{\left( {x - {x_1}} \right)}}{{\left( {{x_0} - {x_1}} \right)}}{y_0} + \frac{{\left( {x - {x_0}} \right)}}{{\left( {{x_1} - {x_0}} \right)}}{y_1}
+\end{equation}
+
+Second-order Lagrange interpolation polynomial:
+
+\begin{equation}
+{p_2}\left( x \right) = \frac{{\left( {x - {x_1}} \right)\left( {x - {x_2}} \right)}}{{\left( {{x_0} - {x_1}} \right)\left( {{x_0} - {x_2}} \right)}}{y_0} + \frac{{\left( {x - {x_0}} \right)\left( {x - {x_2}} \right)}}{{\left( {{x_1} - {x_0}} \right)\left( {{x_1} - {x_2}} \right)}}{y_1} + \frac{{\left( {x - {x_0}} \right)\left( {x - {x_1}} \right)}}{{\left( {{x_2} - {x_0}} \right)\left( {{x_2} - {x_1}} \right)}}{y_2}
+\end{equation}
+
+Third-order Lagrange interpolation polynomial:
+
+\begin{equation}
+\begin{array}{ccc}
+  p_3\PB{x} &= \frac{\PB{x-x_{1}}\PB{x-x_{2}}\PB{x-x_{3}}} {\PB{x_{0}-x_{1}}\PB{x_{0}-x_{2}}\PB{x_{0}-x_{3}}} y_0
+            &+ \frac{\PB{x-x_{0}}\PB{x-x_{2}}\PB{x-x_{3}}} {\PB{x_{1}-x_{0}}\PB{x_{1}-x_{2}}\PB{x_{1}-x_{3}}} y_1 \\
+            &+ \frac{\PB{x-x_{0}}\PB{x-x_{1}}\PB{x-x_{3}}} {\PB{x_{2}-x_{0}}\PB{x_{2}-x_{1}}\PB{x_{2}-x_{3}}} y_2
+            &+ \frac{\PB{x-x_{0}}\PB{x-x_{1}}\PB{x-x_{2}}} {\PB{x_{3}-x_{0}}\PB{x_{3}-x_{1}}\PB{x_{3}-x_{2}}} y_3
+\end{array}
+\end{equation}
+
+where:
+
+x = interpolation point
+
+x\(_{n}\) = x value of tabular data
+
+y\(_{n}\) = y value of tabular data
+
+p\(_{i}\)(n) = polynomial (table) output
+
+The lookup table is interpolated using the interpolation polynomial shown above. If the table input value (interpolation point) is near the bottom edge or exceeds the table boundaries, a linear extrapolation is used (2-point extrapolation). The interpolation order is determined by the user entered number of interpolation points.
+
+A regression analysis may be performed on any lookup table having one or two indpenedent variables. As with performance tables, the resulting performance curve coefficients are calculated and used in the simulation only when the interpolation method is selected as EvaluateCurveToLimits. In addition, the performance curve is only written to the eio file when the output diagnostics flag is set to DisplayAdvancedReportVariables (ref. Output:Diagnostics, DisplayAdvancedReportVariables;)..
+
+Using the example provided in the section above for Tables based on two indpendent variables, the lookup table object would be defined as follows:
+
+\begin{lstlisting}
+
+Table:MultiVariableLookup,
+  CCoolCapFT,
+  EvaluateCurveToLimits,
+  3,
+  BiQuadratic,
+  SingleLineIndependentVariableWithMatrix,
+  ,
+  ASCENDING,
+  ASCENDING,
+  7735.1,  !- Normalization reference
+  1,       !- Minimum Value of X1
+  30,      !- Maximum Value of X1
+  5,       !- Minimum Value of X2
+  50,      !- Maximum Value of X2
+  ,        !- Minimum Value of X3
+  ,        !- Maximum Value of X3
+  ,        !- Minimum Value of X4
+  ,        !- Maximum Value of X4
+  ,        !- Minimum Value of X5
+  ,        !- Maximum Value of X5
+  4500,    !- Minimum Table Output
+  15000,   !- Maximum Table Output
+  Temperature,  !- Input Unit Type for X1
+  Temperature,  !- Input Unit Type for X2
+  ,        !- Input Unit Type for X3
+  ,        !- Input Unit Type for X4
+  ,        !- Input Unit Type for X5
+  Dimensionless,    !- Output Unit Type
+     2, 3, 4,
+    13.9, 17.2, 22.2,
+    23.9, 29.4, 35.0, 40.8,
+    7474.4,  7735.1,  9206.0,
+    7283.9,  7462.6,  8898.3,
+    7067.1,  7157.9,  8552.6,
+    6818.0,  6818.0,  8165.8;
+\end{lstlisting}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001.tex
new file mode 100644
index 00000000000..5896360c1b9
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001.tex
@@ -0,0 +1,17 @@
+\chapter{Simulation Models - Encyclopedic Reference}\label{simulation-models---encyclopedic-reference}
+
+The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of ``Heat Balance'', ``HVAC'', and ``Plant''.~ With the integrated solution, these designations signify where the effects of these models have their first impacts.
+
+Main Sections:
+
+\begin{itemize}
+\tightlist
+\item
+  \protect\hyperlink{IceStorage}{Ice Thermal Storage}
+\item
+  \protect\hyperlink{Coils}{Coils}
+\item
+  \protect\hyperlink{Controllers}{HVAC Controllers}
+\item
+  \protect\hyperlink{Baseboards}{Baseboard Heaters} 
+\end{itemize}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-compound-component-groups.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-compound-component-groups.tex
new file mode 100644
index 00000000000..6d89b92115a
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-compound-component-groups.tex
@@ -0,0 +1,2515 @@
+\section{Air System Compound Component Groups }\label{air-system-compound-component-groups}
+
+\subsection{Unitary Systems}\label{unitary-systems}
+
+\subsubsection{Overview}\label{overview-000}
+
+The input object AirLoopHVAC:UnitarySystem provide a ``virtual'' component that collect and control a set of components: fan, heating coil, cooling coil, and/or reheat coil. Reheat coil is modeled for controlling high zone humidity levels. The unit may be configured to have either a blow through or draw through fan. In a blow through configuration, fan is generally the fist component upstream of heating ro cooling coil. In a draw through fan configuration, fan is placed directly after the heating coil and before reheat coil.
+
+\begin{figure}[hbtp] % fig 218
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4930.png}
+\caption{Schematic of the EnergyPlus Unitary System (Blow Through Configuration) \protect \label{fig:schematic-of-the-energyplus-unitary-system}}
+\end{figure}
+
+\subsubsection{Model Description}\label{model-description}
+
+As described previously, the unitary system is a ``virtual'' component consisting of a fan, heating coil, cooling coil and reheat coil. The sole purpose of the unitary system model is to properly coordinate the operation of the various system components. The following sections describe the flow of information within the model, as well as the differences between cycling and continuous supply air fan operation.
+
+\subsubsection{Controls}\label{controls}
+
+There are two types of control types allowed to be specified in the unitary system which are setpoint based and load based. Each control type is described in detail below.
+
+\subsubsection{Setpoint based control:}\label{setpoint-based-control}
+
+The unitary system calculates the current sensible load using the temperature of the inlet node and the System Node Setpoint Temp on the control node. If the control node is not the outlet node, the desired outlet node temperature is adjusted for the current temperature difference between the outlet node and the control node. Likewise, the current latent load is calculated using the humidity ratio of the inlet node and the System Node Humidity Ratio Max on the control node. The controls determine the required coil run-time fraction and dehumidification mode (if applicable) using the steps outlined below.
+
+\paragraph{Step 1 -- Meet Sensible Load Requirement}\label{step-1-meet-sensible-load-requirement}
+
+The controls first attempt to meet the sensible requirement. The specified coil model is called with a part-load ratio (PLR) of 1.0 to determine the full-load output of the coil. This is compared with the desired outlet node temperature and a sensible PLR is calculated. If the PLR is \textless{}1.0, a Regula-Falsi iteration routine is called to determine the coil run-time fraction which results in the desired outlet node temperature. For a variable-speed DX cooling coil, if the load is smaller than the sensible capacity at the lowest speed, the coil run-time fraction is determined in the same way as a single-speed DX cooling coil. Otherwise, its speed number and speed ratio between two neighboring speeds are selected to match the load.
+
+\paragraph{Step 2 -- Meet Latent Load Requirement (if activated)}\label{step-2-meet-latent-load-requirement-if-activated}
+
+If dehumidification controls are active, the leaving humidity ratio resulting from operation to meet the sensible load (Step 1 above) is compared with the desired outlet node humidity ratio. If the humidity requirement is already met, then no further control action is taken. If the humidity requirement has not been met, then the coil is re-simulated depending on the type of humidity control.
+
+\paragraph{Step 2a -- Humidity Control = MultiMode}\label{step-2a-humidity-control-multimode}
+
+If the humidity control type is MultiMode, then the coil's enhanced dehumidification mode is activated when the coil type is Coil:Cooling:DX:TwoStageWithHumidityControlMode and Step 1 above is repeated to meet the sensible load using the coil performance resulting from the enhanced dehumidificaiton mode. This is a semi-passive approach to dehumidification which may fall short or may exceed the dehumidification requirement.
+
+\paragraph{Step 2b -- Humidity Control = CoolReheat}\label{step-2b-humidity-control-coolreheat}
+
+If the humidity control type is CoolReheat, the coil is re-simulated to achieve the desired outlet node humidity ratio. This option is valid for all cooling coil types. When the coil type is Coil:Cooling:DX:TwoStageWithHumidityControlMode, only the cooling performance mode is used for this step and enhanced dehumidification mode is not activated.
+
+\subsubsection{Load based control:}\label{load-based-control}
+
+While the unitary system may be configured to serve multiple zones, system operation is controlled by a thermostat located in a single ``control'' zone. One of the key parameters for the unitary system component is the fraction of the total system air flow that goes through the control zone. This fraction is calculated as the ratio of the maximum air mass flow rate for the air loop's supply inlet node for the control zone (e.g., AirTerminal:SingleDuct:Uncontrolled, field = Maximum Air Flow Rate, converted to mass flow) to the sum of the maximum air mass flow rates for the air loop's supply inlet nodes for all zones served by this air loop. The unitary system module scales the calculated load for the control zone upward based on this fraction to determine the total load to be met by the unitary system. The module then proceeds to calculate the required part-load ratio for the system coil and the supply air fan to meet this total load. The heating or cooling capacity delivered by the unitary system is distributed to all of the zones served by this system via the terminal units that supply air to each zone. The supply air fraction that goes though the control zone is calculated as follows:
+
+\begin{equation}
+Control Zone Air Flow\,Fraction = \frac{{{{\dot m}_{TUMax\,ControlZone}}}}{{\sum\limits_{j = 1}^{NumOfZones} {{{\dot m}_{TUMax\,Zone\,j}}} }}
+\end{equation}
+
+where:
+
+\({\dot m_{TUMax\,ControlledZone}}\) ~~~ = ~~~ maximum air mass flow rate for the air loop's supply inlet node (terminal unit) for the control zone (kg/s)
+
+\({\dot m_{TUMax\,Zone\,j}}\) ~~~~~~~~~~~ = ~~~ maximum air mass flow rate for the air loop's supply inlet node for the jth zone (kg/s)
+
+\(NumOfZones\) ~~~~~~~~~~~~~~~ = ~~~ number of zones, or number of air loop supply air inlet nodes for all zones served by the air loop (-)
+
+The unitary system component is able to model supply air fan operation in two modes: cycling fan -- cycling coil (i.e., AUTO fan) and continuous fan -- cycling coil (i.e., fan ON). Fan:OnOff must be used to model AUTO fan, while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON. The fan operation mode is specified using a supply air fan operating mode schedule where schedule values of 0 denote cycling fan operation and schedule values other than 0 (a 1 is usually used) denote continuous fan operation. Using this schedule, the unitary system fan may be cycled with cooling or heating coil operation or operated continuously based on time of day (e.g., cycling fan operation at night and continuous fan operation during the daytime). If the fan operating mode schedule name field is left blank in the unitary system object, the unitary system assumes cycling or AUTO fan mode operation throughout the simulation.
+
+The unitary system operates based on the user-specified (or autosized) design supply air flow rate(s). The `design' supply air mass flow rate may be different for cooling, heating, and when no cooling or heating is required and the fan operates continuously based on user-specified inputs.
+
+\textbf{Cooling Operation}
+
+If EnergyPlus determines that the unitary system must supply cooling to the control zone to meet the zone air temperature setpoint, then the model computes the total sensible cooling load to be met by the unitary system based on the control zone sensible cooling load and the fraction of the unitary system air flow that goes through the control zone.
+
+\begin{equation}
+UnitarySystemCoolingLoad = \frac{{ControlZoneCoolingLoad}}{{ControlZoneAirFlowFraction}}
+\end{equation}
+
+If the supply air fan operating mode schedule requests cycling fan operation, the model first checks for the presence of an ecomomizer in the outside air system serving the unitary system's air loop (Ref. AirLoopHVAC:OutdoorAirSystem). If an outside air system is not present or if an air-side economizer is not used, the unitary system's compressor is used to meet the unitary system cooling load. If an air-side economizer is used and is active (i.e., economizer controls indicate that conditions are favorable to increase the outside air flow rate), the unitary system will try to meet the cooling load by operating only the supply air fan. If the fan is able to satisfy the unitary system cooling load, the compressor remains off for the entire simulation time step. If the operation of the fan alone is unable to meet the entire cooling load, then the compressor is enabled and additional calculations are performed to determine the compressor's part-load ratio.
+
+The model then calculates the unitary system's sensible cooling energy rate delivered to the zones being served when the system runs at full-load conditions and when the cooling coil is OFF. If the supply air fan cycles with the compressor, then the sensible cooling energy rate is zero when the cooling coil is OFF. However if the fan is configured to run continuously regardless of coil operation, then the sensible cooling energy rate will probably not be zero when the cooling coil is OFF. Calculating the sensible cooling energy rate involves modeling the supply air fan (and associated fan heat), the cooling coil, and the heating and reheat coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and cooling coil OFF), the sensible cooling energy rate delivered by the unitary system is calculated as follows:
+
+\begin{equation}
+Full\;Cool\;Output = (Mass\;Flow\;Rat{e_{full\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}
+\end{equation}
+
+\begin{equation}
+No\;Cool\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}
+\end{equation}
+
+where:
+
+\emph{Mass Flow Rate\(_{full load}\)} = air mass flow rate through unitary system at full-load conditions, kg/s
+
+\emph{h\(_{coil, full load}\)} = enthalpy of air exiting the unitary system at full-load conditions, J/kg
+
+\(h_{\rm{control zone}}\) = enthalpy of air in the control zone (where thermostat is located), J/kg
+
+\emph{HR\(_{min}\)} = enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the unitary system exiting air or the air in the control zone
+
+\emph{Mass Flow Rate\(_{coil off}\)} = air mass flow rate through the unitary system with the cooling coil OFF, kg/s
+
+\emph{h\(_{out,coil off}\)} = enthalpy of air exiting the unitary system with the cooling coil OFF, J/kg
+
+Δ\(_{sen,full load}\) = Sensible load difference between the system output node and the zone inlet node at full-load conditions
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,full load} &= \frac{MassFlowRate_{ZoneInlet}}{Frac} \PB{h_{Out,full load} - h_{ZoneInlet}}_{HR\min} \\
+                           &+ \PB{MassFlowRate_{full load} - \frac{MassFlowRate_{ZoneInlet}}{Frac}} \PB{ h_{Out,full load} - h_{ControlZone}}
+  \end{array}
+\end{equation}
+
+where:
+
+Frac = Control zone air fraction with respect to the system mass flow rate
+
+Δ\(_{sen,coil off}\) = Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,coil off} &= \frac{MassFlowRate_{ZoneInlet}}{Frac} \PB{h_{Out,coil off} - h_{ZoneInlet}}_{HR\min} \\
+                           &+ \PB{MassFlowRate_{coil off} - \frac{MassFlowRate_{ZoneInlet}}{Frac}} \PB{ h_{Out,coil off} - h_{ControlZone}}
+  \end{array}
+\end{equation}
+
+With the calculated sensible cooling energy rates and the total sensible cooling load to be met by the system, the part-load ratio for the unitary system is estimated.
+
+\begin{equation}
+PartLoadRatio = MAX\left( {0.0,\frac{{\left( {UnitarySystemCoolingLoad - NoCoolOutput} \right)}}{{\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)
+\end{equation}
+
+Since the part-load performance of the cooling coil is frequently non-linear, and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the unitary system's cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system's cooling output divided by the load to be met.
+
+\begin{equation}
+Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemCoolingLoad - {Q_{UnitarySystem}}} \right)}}{{UnitarySystemCoolingLoad}}
+\end{equation}
+
+where:
+
+\({Q_{UnitarySystem}}\) = Unitary system delivered sensible capacity (W)
+
+If the unitary system has been specified with cycling fan/cycling coil (AUTO fan), then the unitary system's operating supply air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. In this case, the air conditions at nodes downstream of the cooling coil represent the full-load (steady-state) values when the coil is operating.
+
+If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the unitary system is calculated as the average of the user-specified air flow rate when the cooling coil is ON and the user-specified air flow rate when the cooling coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
+
+\begin{equation}
+{{\mathop m\limits^ \bullet  }_{UnitarySystem}} = PartLoadRatio\left( {{{\mathop m\limits^ \bullet  }_{CoolCoilON}}} \right) + \left( {1 - PartLoadRatio} \right)\left( {{{\mathop m\limits^ \bullet  }_{CoilOFF}}} \right)
+\end{equation}
+
+where: 
+
+$\dot{m}_{HeatCoilON}$ = air mass flow rate through unitary system when the cooling coil is ON (kg/s)
+
+$\dot{m}_{CoilOFF}$ = air mass flow rate through unitary system when no cooling or heating is needed (kg/s)
+
+In this case, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF).
+
+\textbf{Cooling Operation (multi or variable speed coils)}
+
+After the unitary system cooling load is determined as described in Eq. above, the multi or variable speed cooling coil models calculations are described in this section.
+
+The model calculates the unitary system's sensible cooling energy rate delivered to the zones being served when the system runs at full-load conditions at the highest speed and when the DX cooling coil is OFF. If the supply air fan cycles with the compressor, then the sensible cooling energy rate is zero when the cooling coil is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible cooling energy rate will not be zero when the cooling coil is OFF. Calculating the sensible cooling energy rate involves modeling the supply air fan (and associated fan heat) and the multi/variable speed DX cooling coil. The multi/variable speed DX heating coil and the supplemental heating coil are also modeled, but only to pass the air properties and mass flow rate from their inlet nodes to their outlet nodes. For each of these cases (full load at highest cooling speed and DX cooling coil OFF), the sensible cooling energy rate delivered by the unitary system is calculated as follows:
+
+\[FullCoolOutpu{t_{Highest\;Speed}} = ({\dot m_{HighestSpeed}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;HighestSpeed}}\] \[NoCoolOutput = ({\dot m_{CoilOff}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}\]
+
+where:
+
+\({\dot m_{HighestSpeed}}\) = air mass flow rate through unitary system at the highest cooling speed {[}kg/s{]}
+
+\(h_{out,full load}\) = enthalpy of air exiting the unitary system at full-load conditions {[}J/kg{]}
+
+\(h_{control zone}\) = enthalpy of air leaving the control zone (where thermostat is located) {[}J/kg{]}
+
+\(HR_{min}\) = the minimum humidity ratio of the unitary system exiting air or the air leaving the control zone {[}kg/kg{]}
+
+\({\dot m_{CoilOff}}\) = air mass flow rate through the unitary system with the cooling coil OFF {[}kg/s{]}
+
+\(h_{out,coil off}\) = enthalpy of air exiting the unitary system with the cooling coil OFF {[}J/kg{]}
+
+\(\Delta_{sen,\,HighestSpeed}\) = Sensible load difference between the system output node and the zone inlet node at full-load conditions
+
+\(\Delta_{sen,coil off}\) = Sensible load difference between the system output node and the zone inlet node with the cooling coil OFF conditions
+
+\begin{equation}
+\begin{array}{l}
+{\Delta_{sen,\;HighestSpeed}} = \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad \quad  + \left( {{{\dot m}_{_{HighestSpeed}}} - \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;full\;load}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}
+\end{array}
+\end{equation}
+
+\begin{equation}
+\begin{array}{l}
+{\Delta_{sen,\;coil\;off}} = \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {{{\dot m}_{_{coil\;off}}} - \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;coil\;off}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}
+\end{array}
+\end{equation}
+
+where:
+
+Frac = Control zone air fraction with respect to the system mass flow rate
+
+If the unitary system's sensible cooling rate at the highest speed (full load, no cycling) is insufficient to meet the entire cooling load, the controlled zone conditions will not be met. The reported cycling rate and speed ratio are 1, and the speed number is set to the highest index number. If the total sensible cooling load to be met by the system is less than the sensible cooling rate at the highest speed, then the following steps are performed.
+
+·~~~~~~~~Calculate the sensible cooling energy rate at Speed 1
+
+\begin{equation}
+FullCoolOutpu{t_{Speed1}} = ({\dot m_{Speed1}}){({h_{out,fullload}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;Speed1}}
+\end{equation}
+
+where
+
+\emph{\({\dot m_{Speed1}}\)}~ = air mass flow rate through unitary system at Speed 1 {[}kg/s{]}
+
+Δ\(_{*sen,*}\) \(_{*Speed1*}\) = Sensible load difference between the system output node and the zone inlet node at full-load conditions at Speed 1
+
+\begin{equation}
+  \begin{split}
+    \Delta_{sen,Speed1} =& \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,full load} - h_{ZoneInlet}}_{HRmin} \\
+                              &+ \PB{\dot{m}_{Speed1} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,coil off} - h_{ControlZone}}_{HRmin}
+  \end{split}
+\end{equation}
+
+·~~~~~~~~If the sensible cooling energy rate delivered by the unitary system at Speed 1 is greater or equal to the sensible load, the cycling ratio (part-load ratio) for the unitary system is estimated.
+
+\begin{equation}
+  \begin{array}{rl}
+    CyclingRatio &= \frac{ \left| \PB{CoolingCoilSensibleLoad} \right| } {FullCoolingCoilCapacity} \\ 
+                 &= \max \PB{0.0,\frac{UnitarySystemCoolingLoad - AddedFanHeat}{FullCoolOutput_{Speed1} - AddedFanHeat_{Speed1}}}
+  \end{array}
+\end{equation}
+
+where
+
+\emph{AddedFanHeat}~ = generated supply air fan heat, which is a function of part load ratio and as internal component cooling load {[}W{]}.
+
+\emph{AddedFanHeat\(_{Speed1}\)}~~~~~~~ = generated supply air fan heat at Speed 1 (part load ratio = 1) {[}W{]}.
+
+Since the part-load performance of the DX cooling coil is frequently non-linear,and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the unitary system's cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system's cooling output divided by the load to be met.
+
+\begin{equation}
+Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemOutpu{t_{cycling}} - {Q_{UnitarySystem}}} \right)}}{{UnitarySystemCoolingLoad}}
+\end{equation}
+
+where:
+
+Unitary systemOutput\(_{Cycling}\) = unitary system delivered sensible capacity for Speed 1 operating at a specific cycling ratio (W)
+
+\begin{equation}
+UnitarySystemOutpu{t_{cycling}} = {\mathop m\limits^ \bullet_{UnitarySystem}}{\left( {{h_{out}} - {h_{ControlZone}}} \right)_{HR\min }} - {\Delta_{cycling}}
+\end{equation}
+
+where
+
+\({\dot m{_{UnitarySystem}}}\) ~~~~~ = average air mass flow rate defined in the next section {[}kg/s{]}
+
+\emph{h\(_{out,}\)} ~~~~~ ~ = enthalpy of air exiting the unitary system at part load conditions {[}J/kg{]}
+
+Δ\(_{cycling}\) = average sensible load difference between the system output node and the zone inlet node
+
+\begin{equation}
+{\Delta_{cycling}} = \frac{{{{\mathop m\limits^ \bullet  }_{ZoneInlet}}}}{{frac}}\left( {{h_{ZoneInlet}} - {h_{ControlZone}}} \right) + \left( {{{\mathop m\limits^ \bullet  }_{UnitarySystem}} - \frac{{{{\mathop m\limits^ \bullet  }_{ZoneInlet}}}}{{frac}}} \right)\left( {{h_{Out}} - {h_{ControlZone}}} \right)
+\end{equation}
+
+\({\dot m{_{ZoneInlet}}}\) = Air mass flow rate in the supply inlet node in the controlled zone {[}kg/s{]}
+
+For this case where speed 1 operation was able to meet the required cooling load, the speed ratio is set to zero and speed number is equal to 1.
+
+·~~~~~~~~If the unitary system's cooling output at full load for Speed 1 is insufficient to meet the entire cooling load, the Cycling ratio is set equal to 1.0 (compressor and fan are not cycling). Then the cooling speed is increased and the delivered sensible capacity is calculated. If the full load sensible capacity at Speed n is greater than or equal to the sensible load, the speed ratio for the unitary system is estimated:
+
+\begin{equation}
+SpeedRatio = \frac{{ABS\left( {UnitarySystemCoolingLoad - AddedFanHeat - FullCoolOutpu{t_{Speedn - 1}}} \right)}}{{ABS\left( {FullCoolOutpu{t_{Speedn}} - FullCoolOutpu{t_{Speedn - 1}}} \right)}}
+\end{equation}
+
+Although a linear relationship is assumed by applying the speed ratio to obtain the effective capacity and mass flow rate between speed n and n-1, the outlet air node conditions are dependent on the combined outputs and may not be linear. In addition, the supply air fan heat varies with the speed ratio due to different supply mass flow rates between speed n and n-1 . Therefore, the final speed ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the unitary system's cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system's cooling output divided by the load to be met.
+
+\begin{equation}
+Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemCoolingLoad - UnitarySystemOutpu{t_{SpeedRatio}}} \right)}}{{UnitarySystemCoolingLoad}}
+\end{equation}
+
+where:
+
+\emph{UnitarySystemOutput\(_{Speedn}\)} = unitary system delivered sensible capacity between two consecutive speeds at a specific speed ratio (W)
+
+\begin{equation}
+  \begin{array}{rl}
+    UnitarySystemOutput_{SpeedRatio} &= (SpeedRatio)FullCoolOutput_{Speedn} \\
+                                     &+ (1 - SpeedRatio)FullCoolOutput_{Speedn - 1} \\
+                                     &- AddedFanHeat_{SpeedRatio}
+  \end{array}
+\end{equation}
+
+Where
+
+\emph{AddedFanHeat\(_{SpeedRatio}\)} = generated supply air fan heat at a specific speed ratio {[}W{]}
+
+In this case, the reported cycling ratio is 1 and speed number is equal to n.
+
+\paragraph{Air Mass Flow Rate Calculation}\label{air-mass-flow-rate-calculation}
+
+Speed 1 operation
+
+If the unitary system has been specified with cycling fan/cycling coil (AUTO fan), then the unitary system's operating supply air mass flow rate is determined by the cycling ratio (PartLoadRatio) for Speed 1. The supply air mass flow rate is multiplied by the cycling ratio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the cooling coils represent the full-load (steady-state) values when the coil is operating.
+
+\begin{equation}
+{{\mathop m\limits^ \bullet  }_{UnitarySystem}} = \left( {CyclingRatio} \right){{\mathop m\limits^ \bullet  }_{Speed1}}
+\end{equation}
+
+If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the unitary system is calculated as the average of the user-specified air flow rate when the unitary system cooling coil is ON at Speed 1 and the user-specified air flow rate when the unitary system cooling coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
+
+\begin{equation}
+{{\mathop m\limits^ \bullet  }_{UnitarySystem}} = \left( {CyclingRatio} \right){{\mathop m\limits^ \bullet  }_{Speed1}} + \left( {1 - CyclingRatio} \right){{\mathop m\limits^ \bullet  }_{CoilOff}}
+\end{equation}
+
+where:
+
+\({\dot m_{UnitarySystem}}\) ~ = average air mass flow rate through unitary system {[}kg/s{]}
+
+\({\dot m_{Speed1}}\) = air mass flow rate through unitary system when cooling coil is ON at Speed 1 {[}kg/s{]}
+
+\({\dot m_{CoilOff}}\) ~ = air mass flow rate through unitary system when no heating or cooling is needed {[}kg/s{]}
+
+In this case, the air conditions at nodes downstream of the cooling coils are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF).
+
+\paragraph{Higher Speed Operation}\label{higher-speed-operation}
+
+When the unitary system operates at higher speeds to meet the required cooling load, the supply air mass flow rate is linearly interpolated between two consecutive speeds:
+
+\begin{equation}
+{{\mathop m\limits^ \bullet  }_{UnitarySystem}} = \left( {SpeedRatio} \right){{\mathop m\limits^ \bullet  }_{Speedn}} + \left( {1 - SpeedRatio} \right){{\mathop m\limits^ \bullet  }_{Speedn - 1}}
+\end{equation}
+
+where:
+
+\({{\mathop m\limits^ \bullet }_{UnitarySystem}}\) = average air mass flow rate through the unitary system for the time step {[}kg/s{]}
+
+\({\dot m_{Speedn}}\) = air mass flow rate through unitary system when cooling coil is ON at Speed n {[}kg/s{]}
+
+\({\dot m_{Speedn - 1}}\) = air mass flow rate through unitary system when cooling coil is ON at Speed n-1 {[}kg/s{]}
+
+For this case of higher speed operation, the air conditions at nodes downstream of the cooling coils are determined by the delivered cooling capacity and supply air mass flow rates between two consecutive speeds.
+
+Although the above sections present the capacity and air mass flow rate calculation separately, they are dependent and change every iteration until convergence is reached for the time step being simulated.
+
+\textbf{Heating Operation}
+
+Calculations for heating operation are similar to those for cooling operation in most respects. However, due to the inclusion of a supplemental heating coil, additional calculations are necessary to properly meet the total heating load for the zones being served.
+
+If EnergyPlus determines that the unitary system must supply heating to the control zone to meet the zone air temperature setpoint, then the unitary system model computes the total sensible heating load to be delivered to the zones being served based on the control zone sensible heating load and the control zone airflow fraction.
+
+\begin{equation}
+UnitarySystemHeatingLoad = \frac{{ControlZoneHeatingLoad}}{{ControlZoneAirFlowFraction}}
+\end{equation}
+
+The model then calculates the unitary system's sensible heating energy rate delivered to the zones being served when the system runs at full-load conditions and when the heating coil is OFF (without supplemental heater operation in either case). If the supply air fan cycles with the compressor, then the sensible heating energy rate is zero when the compressor is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible heating energy rate will not be zero when the compressor is OFF. Calculating the sensible heating energy rate involves modeling the supply air fan (and associated fan heat), the~ cooling coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node), the~ heating coil, and the supplemental heating coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and~ heating coil OFF, without supplemental heater operation in either case), the sensible heating energy rate delivered by the unitary system is calculated as follows:
+
+\begin{equation}
+Full\;Heat\;Output = (Mass\;Flow\;Rat{e_{ful\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}
+\end{equation}
+
+\begin{equation}
+No\;Heat\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}
+\end{equation}
+
+where:
+
+\emph{Mass Flow Rate \(_{full load}\)} = air mass flow rate through unitary system at full-load conditions, kg/s
+
+\emph{h\(_{out, full load}\)} = enthalpy of air exiting the unitary system at full-load conditions, J/kg
+
+\emph{h\(_{control zone}\)} = enthalpy of air leaving the control zone (where thermostat is located), J/kg
+
+\emph{HR\(_{min}\) =} enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the unitary system exiting air or the air leaving the control zone
+
+\emph{Mass Flow Rate \(_{coil off}\)} = air mass flow rate through the unitary system with the heating coil OFF, kg/s
+
+\emph{h\(_{out, coil off}\)} = enthalpy of air exiting the unitary system with the heating coil OFF, J/kg
+
+Δ\(_{sen,}\) \emph{\(_{full load}\)} = Sensible load difference between the system output node and the zone inlet node at full-load conditions
+
+\begin{equation}
+  \begin{split}
+    \Delta_{sen,full load} =& \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,full load} - h_{ZoneInlet}}_{HRmin} \\
+                              &+ \PB{\dot{m}_{full load} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,full load} - h_{ControlZone}}_{HRmin}
+  \end{split}
+\end{equation}
+
+where:
+
+Frac = Control zone air fraction with respect to the system mass flow rate
+
+Δ\(_{sen,coil off}\) = Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
+
+\begin{equation}
+  \begin{split}
+    \Delta_{sen,coil off} =& \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,coil off} - h_{ZoneInlet}}_{HRmin} \\
+                              &+ \PB{\dot{m}_{coil off} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,coil off} - h_{ControlZone}}_{HRmin}
+  \end{split}
+\end{equation}
+
+With the calculated sensible heating energy rates and the total sensible heating load to be met by the system, the part-load ratio for the unitary system is estimated.
+
+\begin{equation}
+PartLoadRatio = MAX\left( {0.0,\frac{{\left( {UnitarySystemHeatingLoad - NoHeatOutput} \right)}}{{\left( {FullHeatOutput - NoHeatOutput} \right)}}} \right)
+\end{equation}
+
+Since the part-load performance of the~ heating coil is frequently non-linear, and the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the unitary system's heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system's heating output divided by the load to be met.
+
+\begin{equation}
+Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemHeatingLoad - {Q_{UnitarySystem}}} \right)}}{{UnitarySystemHeatingLoad}}
+\end{equation}
+
+where:
+
+\({Q_{UnitarySystem}}\) = Unitary system delivered sensible capacity (W)
+
+If the unitary system's~ heating coil output at full load is insufficient to meet the entire heating load, PartLoadRatio is set equal to 1.0 (compressor and fan are not cycling) and the remaining heating load is passed to the supplemental heating coil. If the unitary system model determines that the outdoor air temperature is below the minimum outdoor air temperature for compressor operation, the compressor is turned off and the entire heating load is passed to the supplemental gas or electric heating coil. The unitary system exiting air conditions and energy consumption are calculated and reported by the individual component models (fan,~ heating coil, and supplemental gas or electric heating coil).
+
+If the unitary system has been specified with cycling fan/cycling coil (AUTO fan), then the unitary system's operating supply air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the heating coils represent the full-load (steady-state) values when the coils are operating. If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the unitary system is calculated as the average of the user-specified air flow rate when the unitary system heating coil is ON and the user-specified air flow rate when the unitary system heating coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
+
+\begin{equation}
+{{\mathop m\limits^ \bullet  }_{UnitarySystem}} = PartLoadRatio\left( {{{\mathop m\limits^ \bullet  }_{HeatCoilON}}} \right) + \left( {1 - PartLoadRatio} \right)\left( {{{\mathop m\limits^ \bullet  }_{CoilOFF}}} \right)
+\end{equation}
+
+where:
+
+\({\dot m_{HeatCoilON}}\) ~ = air mass flow rate through unitary system when the heating coil is ON (kg/s)
+
+\({\dot m_{CoilOFF}}\) ~ = air mass flow rate through unitary system when no heating or cooling is needed (kg/s)
+
+In this case, the air conditions at nodes downstream of the heating coils are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coils are operating and inlet air conditions when the coils are OFF).
+
+\subsubsection{Heating Operation (multi or variable speed coils )}\label{heating-operation-multi-or-variable-speed-coils}
+
+After the unitary system heating load is determined as described in Eq. above, the multi or variable speed heating coil models calculation are described in this section.
+
+The model calculates the unitary system's sensible heating energy rate delivered to the zones being served when the system runs at full-load conditions at the highest speed and when the DX heating coil is OFF (without supplemental heater operation in either case). If the supply air fan cycles with the compressor, then the sensible heating energy rate is zero when the compressor is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible heating energy rate will not be zero when the compressor is OFF. Calculating the sensible heating energy rate involves modeling the supply air fan (and associated fan heat), the DX cooling coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node), the DX heating coil, and the supplemental heating coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and DX heating coil OFF, without supplemental heater operation in either case), the sensible heating energy rate delivered by the unitary system is calculated as follows:
+
+\begin{equation}
+FullHeatOutpu{t_{Highest\;Speed}} = ({\dot m_{HighestSpeed}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;HighestSpeed}}
+\end{equation}
+
+\begin{equation}
+NoHeatOutput = ({\dot m_{CoilOff}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}
+\end{equation}
+
+where:
+
+\emph{\({\dot m_{HighestSpeed}}\)}~ = air mass flow rate through unitary system at the highest heating speed {[}kg/s{]}
+
+\emph{h\(_{out, full load}\)} = enthalpy of air exiting the unitary system at full-load conditions {[}J/kg{]}
+
+\emph{h\(_{control zone}\)} = enthalpy of air leaving the control zone (where thermostat is located) {[}J/kg{]}
+
+\emph{HR\(_{min}\) =} enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the unitary system exiting air or the air leaving the control zone
+
+\({\dot m_{CoilOff}}\) = air mass flow rate through the unitary system with the heating coil OFF {[}kg/s{]}
+
+\emph{h\(_{out,coil off}\)} = enthalpy of air exiting the unitary system with the heating coil OFF {[}J/kg{]}
+
+Δ\(_{sen,}\) \emph{\(_{full load}\)} = Sensible load difference between the system output node and the zone inlet node at full-load conditions
+
+\begin{equation}
+  \begin{split}
+    \Delta_{sen,HighestSpeed} =& \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,full load} - h_{ZoneInlet}}_{HRmin} \\
+                              &+ \PB{\dot{m}_{HighestSpeed} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,coil off} - h_{ControlZone}}_{HRmin}
+  \end{split}
+\end{equation}
+
+where:
+
+Frac = Control zone air fraction with respect to the system mass flow rate
+
+Δ\emph{\(_{sen,coil off}\)} = Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
+
+\begin{equation}
+  \begin{split}
+    \Delta_{sen,coil off} =& \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,coil off} - h_{ZoneInlet}}_{HRmin} \\
+                              &+ \PB{\dot{m}_{coil off} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,coil off} - h_{ControlZone}}_{HRmin}
+  \end{split}
+\end{equation}
+
+If the unitary system's DX heating coil output full load at the highest speed is insufficient to meet the entire heating load, the remaining heating load is passed to the supplemental heating coil. If the unitary system model determines that the outdoor air temperature is below the minimum outdoor air temperature for compressor operation (specified by the user), the compressor is turned off and the entire heating load is passed to the supplemental gas or electric heating coil. The unitary system exiting air conditions and energy consumption are calculated and reported by the individual component models (fan, DX heating coil, and supplemental gas or electric heating coil).
+
+If the total heating load to be met by the system is less than the sensible heating rate at the highest speed, then the following steps are performed.
+
+1. Calculate the sensible heating energy rate at Speed 1
+
+\begin{equation}
+FullHeatOutpu{t_{Speed1}} = ({\dot m_{Speed1}}){({h_{out,fullload}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;Speed1}}
+\end{equation}
+
+where:
+
+\emph{\({\dot m_{Speed1}}\)}~ = air mass flow rate through unitary system at Speed 1 {[}kg/s{]}
+
+Δ\emph{\(_{sen,}\) \(_{Speed1}\)} = Sensible load difference between the system output node and the zone inlet node at full-load conditions at Speed 1
+
+\begin{equation}
+  \begin{split}
+    \Delta_{sen,Speed1} =& \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,full load} - h_{ZoneInlet}}_{HRmin} \\
+                              &+ \PB{\dot{m}_{Speed1} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,coil off} - h_{ControlZone}}_{HRmin}
+  \end{split}
+\end{equation}
+
+2.If the sensible heating energy rate delivered by the unitary system at Speed 1 is greater or equal to the sensible load, the cycling ratio (part-load ratio) for the unitary system is estimated.
+
+\begin{equation}
+  \begin{array}{rl}
+    CyclingRatio &= \frac{\left|\PB{HeatingCoilSensibleLoad}\right|}{FullHeatingCoilCapacity} \\
+                 &= \max \PB{0.0,\frac{UnitarySystemHeatingLoad - AddedFanHeat}{FullHeatOutput_{speed1} - AddedFanHeat_{speed1}}}
+  \end{array}
+\end{equation}
+
+where
+
+\emph{AddedFanHeat}~~~~~~~ = generated supply air fan heat, which is a function of part load ratio and as internal component heating load {[}W{]}.
+
+\emph{AddedFanHeat\(_{Speed1}\)} = generated supply air fan heat at Speed 1 (part load ratio = 1) {[}W{]}.
+
+Since the part-load performance of the DX heating coil is frequently non-linear, and the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the unitary system's heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system's heating output divided by the load to be met.
+
+\begin{equation}
+Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemHeatingLoad - UnitarySystemOutpu{t_{cycling}}} \right)}}{{UnitarySystemHeatingLoad}}
+\end{equation}
+
+where:
+
+\emph{UnitarySystemOutput\(_{cycling}\)} = unitary system delivered sensible capacity for Speed 1 operating at a specific cycling ratio (W)
+
+\begin{equation}
+UnitarySystemOutpu{t_{cycling}} = {{\mathop m\limits^ \bullet  }_{UnitarySystem}}{\left( {{h_{out}} - {h_{ControlZone}}} \right)_{HR\min }} - {\Delta_{cycling}}
+\end{equation}
+
+where
+
+\({{\mathop m\limits^ \bullet }_{UnitarySystem}}\) ~ = average air mass flow rate defined in the next section {[}kg/s{]}
+
+\emph{h\(_{out,}\)} = enthalpy of air exiting the unitary system at part load conditions {[}J/kg{]}
+
+Δ\emph{\(_{cycling}\)} = average sensible load difference between the system output node and the zone inlet node
+
+\begin{equation}
+{\Delta_{cycling}} = \frac{{{{\mathop m\limits^ \bullet  }_{ZoneInlet}}}}{{frac}}\left( {{h_{ZoneInlet}} - {h_{ControlZone}}} \right) + \left( {{{\mathop m\limits^ \bullet  }_{UnitarySystem}} - \frac{{{{\mathop m\limits^ \bullet  }_{ZoneInlet}}}}{{frac}}} \right)\left( {{h_{Out}} - {h_{ControlZone}}} \right)
+\end{equation}
+
+\({\dot m_{ZoneInlet}}\) ~~~~~~ = Air mass flow rate in the supply inlet node in the controlled zone {[}kg/s{]}
+
+For this case where Speed 1 operation was able to meet the required heating load, the speed ratio is set to zero and speed number is equal to 1.
+
+3.~~~~If the unitary system's heating output at full load for Speed 1 is insufficient to meet the entire heating load, the Cycling ratio (PartLoadRatio) is set equal to 1.0 (compressor and fan are not cycling). Then the heating speed is increased and the delivered sensible capacity is calculated. If the full load sensible capacity at Speed n is greater than or equal to the sensible load, the speed ratio for the unitary system is estimated:
+
+\begin{equation}
+SpeedRatio = \frac{{ABS\left( {UnitarySystemHeatingLoad - AddedFanHeat - FullHeatOutpu{t_{Speedn - 1}}} \right)}}{{ABS\left( {FullHeatOutpu{t_{Speedn}} - FullHeatOutpu{t_{Speedn - 1}}} \right)}}
+\end{equation}
+
+Although a linear relationship is assumed by applying the speed ratio to obtain the effective capacity and air mass flow rate between speed n and n-1, the outlet node conditions are dependent on the combined outputs and may not be linear. In addition, the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan). Therefore, the final speed ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the unitary system's heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system's heating output divided by the load to be met.
+
+\begin{equation}
+Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemHeatingLoad - UnitarySystemOutpu{t_{SpeedRatio}}} \right)}}{{UnitarySystemHeatingLoad}}
+\end{equation}
+
+where:
+
+\emph{UnitarySystemOutput\(_{SpeedRatio}\)} = unitary system delivered sensible capacity between two consecutive speeds at a specific ratio {[}W{]}
+
+\begin{equation}
+  \begin{array}{rl}
+    UnitarySystemOutput_{SpeedRatio} &= \PB{SpeedRatio} FullHeatOutput_{speedn} \\
+                                     &+ \PB{1 - SpeedRatio} FullHeatOutput_{speedn - 1} \\ 
+                                     &- AddedFanHeat_{SpeedRatio}
+  \end{array}
+\end{equation}
+
+Where
+
+\emph{AddedFanHeat\(_{SpeedRatio}\)}~~~~~~~~~ = generated supply air fan heat at a specific speed ratio {[}W{]}
+
+In this case, the reported cycling ratio is 1 and speed number is equal to n.
+
+\paragraph{Air Mass Flow Rate Calculation}\label{air-mass-flow-rate-calculation-1}
+
+The air mass flow rate calculations during heating operation are the same as those described above for cooling operation for multi/variable speed.
+
+\subsubsection{High Humidity Control}\label{high-humidity-control}
+
+The specific configuration of the unitary system with supplemental heating coil is shown above (see Figure~\ref{fig:schematic-of-a-blow-through-air-to-air-heat}). This figure shows the fan placement when a blow through fan is specified. If a draw through fan is specified, the fan is located between the heating coil and the supplemental heating coil. The system is controlled to keep the high relative humidity in the control zone from exceeding the setpoint specified in the object ZoneControl:Humidistat. This option is available when the supply air fan operates continuously (i.e., the supply air fan operating mode schedule values are never equal to 0) or the supply air fan cycles with the compressor. In addition, when high humidity control is specified and the compressor operates, the unitary system operates at the cooling air flow rate when a zone heating load is present as determined by the zone thermostat. High humidity control is specified as either None, MultiMode, or CoolReheat in the Dehumidification Control Type input field. MultiMode is specified when a heat exchanger is used to improve the dehumidification performance of the cooling coil. The heat exchanger will be activated when the sensible part-load ratio is insufficient to meet the zone latent load. CoolReheat is specified when a cooling coil is used to over-cool the supply air stream in order to meet the zone latent load. In this case, a supplemental heating coil will ensure the zone temperature does not fall below the zone heating temperature set point. When a heat exchanger is used in conjunction with a cooling coil and CoolReheat is specified as the Dehumidification Control Type, the heat exchanger is ``locked on'' to meet either the sensible or latent cooling load. If the dehumidification control type is selected as None and a heat exchanger assisted cooling coil is used, the heat exchanger is ``locked on'' and the air conditioner runs only to meet the sensible cooling load. A supplemental heating coil is required for all dehumidification control types.
+
+The model first calculates the \emph{PartLoadRatio} required to meet the sensible cooling load.~ The unitary system's sensible cooling load is determined from the control zone sensible cooling load to the cooling setpoint and the control zone air flow fraction to maintain the dry-bulb temperature setpoint in the control zone.:
+
+\begin{equation}
+UnitarySystemCoolingLoad = \frac{{ControlZoneCoolingLoad}}{{ControlZoneAirFlowFraction}}
+\end{equation}
+
+The unitary system's sensible cooling load to be met and the full load cooling output are used to calculate the sensible the part-load ratio iteratively based on user specified convergence criterion.
+
+\begin{equation}
+PartLoadRatio = MAX\left( {0.0,\frac{{\left( {UnitarySystemCoolingLoad - NoCoolOutput} \right)}}{{\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)
+\end{equation}
+
+When the unitary system's sensible cooling capacity meets the system sensible cooling load at a given sensible part load ratio, then the Unitary system meets the controlled zone cooling setpoint temperature. If a moisture (latent) load exists because the control zone humidity has exceeded the setpoint, the total moisture load to be met by the unitary systems (Unitary systemMoistureLoad) is calculated based on the control zone moisture load and the control zone air flow fraction.
+
+\begin{equation}
+UnitarySystemMoistureLoad = \frac{{ControlZoneMoistureLoad}}{{ControlZoneAirFlowFraction}}
+\end{equation}
+
+Then the \emph{LatentPartLoadRatio} required to meet the high humidity setpoint is calculated as follows:
+
+\[LatentPartLoadRatio = MIN\left( {PL{R_{Min}},\frac{{\left( {UnitarySystemMoistureLoad - NoLatentOutput} \right)}}{{\left( {FullLatentOutput - NoLatentOutput} \right)}}} \right)\] The model uses the greater of the two part-load ratios, \emph{PartLoadRatio} or \emph{LatentPartLoadRatio}, to determine the operating part-load ratio of the Unitary system's DX cooling coil.
+
+\begin{equation}
+LatentPartLoadRatio = MAX\left( {PartLoadRatio,LatentPartLoadRatio} \right)
+\end{equation}
+
+As previously described, iterations are performed to converge on the solution within the convergence tolerance.
+
+Where,
+
+\(ControlZoneCoolingLoad\) = the control zone sensible cooling load to the cooling setpoint, (W).
+
+\(ControlZoneMoistureLoad\) ~~~~~~~~~ = the control zone moisture load to the dehumidifying relative humidity setpoint, (W).
+
+\(ControlZoneAirFlowFraction\) ~~~~ = the supply air fraction that goes though the control zone, (-).
+
+\(FullLatentOutput\) = the Unitary system's latent cooling energy rate at full-load conditions, W
+
+\(NoLatentOutput\) ~~ = the Unitary system's latent cooling energy rate with cooling coil OFF, W
+
+\(PartLoadRatio\) ~~~~ = the unitary system's part-load-ratio required to meet system sensible load, (-).
+
+\(LatentPartLoadRatio\) = the unitary system's part-load-ratio required to meet system moisture load, (-).
+
+\(PL{R_{Min}}\) * = *the minimum part-load ratio, which is usually 0.0. For the case when the latent capacity degradation model is used (Ref: DX Cooling Coil Model), this value is the minimum part-load ratio at which the cooling coil will dehumidify the air.
+
+When the predicted zone air temperature is above the heating setpoint and if there is a dehumidification load, the supplemental heating coil load is required to offset the excess cooling as shown in Figure~\ref{fig:supplemental-heating-coil-load-when-predicted-002}. If the model determines that the LatentPartLoadRatio is to be used as the operating part-load ratio of the unitary system's cooling coil, the supplemental heating coil is used to offset the excess sensible capacity provided by the unitary system cooling coil. The model first checks the sensible load that exists for the current simulation time step (predicted zone temperature with no HVAC operation compared to the thermostat setpoint temperatures). If a sensible cooling load or no sensible cooling or heating load exists, the model calculates the difference between the sensible heating load required to reach or maintain the heating dry-bulb temperature setpoint and the actual sensible cooling energy rate delivered by the unit (with LatentPartLoadRatio). In this case, the supplemental heating coil is used to offset the excess sensible cooling energy provided by the cooling coil (if any) that could have caused an overshoot of the heating dry-bulb temperature setpoint. Note that when a humidistat is used and high humidity control is required, the zone dry-bulb temperature will typically move toward the heating temperature setpoint when a high moisture (latent) load exists.
+
+\begin{figure}[hbtp] % fig 219
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5015.png}
+\caption{Supplemental heating coil load when predicted zone air temperature is above the heating Setpoint \protect \label{fig:supplemental-heating-coil-load-when-predicted}}
+\end{figure}
+
+If a heating load exists (Figure~\ref{fig:supplemental-heating-coil-load-when-predicted-003}), the supplementalheating coil is used to meet the heating coil load and at the same time offset the entire sensible cooling energy rate of the cooling coil (to meet the humidistat setpoint). Note that when a heating load exists and high humidity control is required, the unitary system operates at the user-specified cooling air flow rate for the entire simulation time step. As with the fan, and cooling coil, report variables associated with supplemental heating coil performance (e.g., heating coil energy, heating coil rate, heating coil gas or electric energy, heating coil runtime fraction, etc.) are managed in the supplemental (heating) coil object.
+
+\begin{figure}[hbtp] % fig 220
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5016.png}
+\caption{Supplemental heating coil load when predicted zone air temperature is below the heating setpoint \protect \label{fig:supplemental-heating-coil-load-when-predicted-001}}
+\end{figure}
+
+\subsubsection{Waste Heat Calculation}\label{waste-heat-calculation}
+
+Waste heat calculations are done when the multi speed cooling and heating coils are specified in the unitary system and the heat recovery is active (the value of the Design Heat Recovery Water Flow Rate field is greater than 0), the outlet node temperature of heat recovery is calculated based on the recoverable waste heat generated by the child objects Coil:Cooling:DX:MultiSpeed and Coil:Heating:DX:MultiSpeed:
+
+\begin{equation}
+{T_{outlet}} = {T_{inlet}} + \frac{{{Q_{WasteHeat}}}}{{{C_p}{{\dot m}_{hr}}}}
+\end{equation}
+
+where
+
+\emph{T\(_{outlet}\)}~~~~~~~~~~~ = outlet node temperature of heat recovery, C
+
+\emph{T\(_{inlet}\)} = inlet node temperature of heat recovery, C
+
+\emph{Q\(_{WasteHeat}\)}~~~~~ = recoverable waste heat generated by its child objects, W
+
+\emph{C\(_{p}\)}~~~~~~~~~~~~~ = inlet node temperature of heat recovery, C
+
+\({\dot m_{hr}}\) ~~~~~~~~~~~ = mass flow rate of heat recovery, kg/s
+
+If the outlet node temperature is above the value of the Maximum Temp for Heat Recovery field, the outlet node temperature is reset to the value of Maximum Temp for Heat Recovery.
+
+\subsubsection{Multi-Speed Fan with Water Coils In Unitary System}\label{multi-speed-fan-with-water-coils-in-unitary-system}
+
+When modeling multi-speed fan and water coils in unitary system object, the coil's capacity is modulated using speed ratio or part-load ratio. The system load is met by varying the supply air fan speed while operating the coils at maximum water flow. When there is no system load to meet, the water control valve is fully closed. This method of capacity control is called two-position coil control. When the supply fan is cycling between stages, then the speed ratio is calculated, but when the unit cycles between the minimum fan speed and off-position, part-load ratio is calculated. The fan may be off or run at lowest speed continuously to provide ventilation air depending the fan operating schedule. When the fan is operating at the lowest fan speed (Speed = 1), then the water flow rate is reported as the average for the time step by multiplying the maximum water flow by part load ratio. The speed ratio and part-load ratio are calculated iteratively. The set of equations used for the multi-speed fan capacity control in unitary system for water coil AHU modeling are summarized next
+
+\paragraph{Cycling Between Stages:}\label{cycling-between-stages}
+
+When the supply fan is cycling between consecutive speeds, then the speed ratio (SR) and the average mass flow rate are calculated as follows:
+
+\[{SR_{n}} = Abs({SystemLoad} - {FullLoadOutput_{n-1}}) / Abs({FullLoadOutput_{n}} - {FullLoadOutput_{n-1}})\] \[{\dot m} = {\dot m_{on, n}} {SR_{n}} + {\dot m_{on, n-1}} (1 - {SR_{n}})\] \[{\dot m{w}} = {\dot m_{w, max}}\]
+
+\paragraph{Cycling OnOff at Lowest Stage:}\label{cycling-onoff-at-lowest-stage}
+
+The average supply air flow rate calculation when the fan is running at the lowest fan speed level depends on the fan operating schedule and load. The unitary system part load ratio is given by:
+
+\begin{equation}
+{PLR} = Abs({SystemLoad} - {NoLoadOutput}) / Abs({FullLoadOutput_{1}} - {NoLoadOutput})
+\end{equation}
+
+\subparagraph{Continuous Fan:}\label{continuous-fan}
+
+\begin{equation}
+{\dot m} = {\dot m_{on, 1}} {PLR} + {\dot m_{off}} (1 - {PLR})
+\end{equation}
+
+\subparagraph{Cycling Fan:}\label{cycling-fan}
+
+\[{\dot m} = {\dot m_{on, 1}} {PLR}\] \[{\dot m{w}} = {\dot m_{w, max}} * {PLR}\]
+
+where:
+
+\begin{tabular}{clc}
+  $SR_n$ & speed ratio of the water coil unitary system at speed n & (-) \\
+  $PLR$ & part load ratio of the unitary system at speed 1 & (-) \\
+  $\dot{m}$ & average mass flow rate of supply air & (kg/s) \\
+  $\dot{m}_{on, n-1}$ & mass flow rate of supply air at fan speed level n-1 & (kg/s) \\
+  $\dot{m}_{on, n}$ & mass flow rate of supply air at fan speed level n & (kg/s) \\
+  $\dot{m}_{off}$ & mass flow rate of supply air when the coils are off & (kg/s) \\
+  $\dot{m}_{w}$ & average mass flow rate of chilled or hot water & (kg/s) \\
+  $\dot{m}_{w, max}$ & maximum or full mass flow rate of chilled or hot water & (kg/s) \\
+  $SystemLoad$ & system load to be met by the unitary system & (W) \\
+  $FullLoadOutput_{n-1}$ & fully load system output at fan speed level n-1 & (W) \\
+  $FullLoadOutput_{n}$ & fully load system output at fan speed level n & (W)
+\end{tabular}
+
+\subsection{Forced-Air Furnace and Central Air Conditioning}\label{forced-air-furnace-and-central-air-conditioning}
+
+\subsubsection{Overview}\label{overview-1}
+
+The input objects AirLoopHVAC:Unitary:Furnace:HeatOnly and \\
+AirLoopHVAC:Unitary:Furnace:HeatCool provide a ``virtual'' component that collect and control a set of components:~ an on/off or constant volume fan component and a gas or electric heating coil component. If the HeatCool version is selected, then a DX cooling coil is also modeled as part of the system as shown in Figure~\ref{fig:schematic-of-the-energyplus-furnace-blow} below. For the HeatCool version, an optional reheat coil may also be modeled for controlling high zone humidity levels and the furnace's configuration when specifying this option is shown in Figure~\ref{fig:schematic-for-blow-through-furnace-with-high} below. The unit may be configured to have either a blow through or draw through fan. If a blow through fan configuration is specified, the furnace fan is placed before the heating coil for the HeatOnly version, or before the cooling coil for the HeatCool version as shown in the figure below. If a draw through fan configuration is specified, the fan is placed directly after the heating coil.
+
+Note: the coil order shown here has been revised from previous versions of Energyplus to configure the cooling coil upstream of the heating coil. This configuration provides uniformity with all unitary equipment. However, for unitary HeatCool systems that do not use a reheat coil, the heating coil can also be placed upstream of the cooling coil. This optional coil placement is retained to allow compatibility with previous versions of Energyplus. For input files developed using previous versions of Energyplus, it is recommended that the coil order be revised according to the figure below.
+
+\begin{figure}[hbtp] % fig 221
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5019.png}
+\caption{Schematic of the EnergyPlus Furnace (Blow Through Configuration) \protect \label{fig:schematic-of-the-energyplus-furnace-blow}}
+\end{figure}
+
+While the furnace may be configured to serve multiple zones, system operation is controlled by a thermostat located in a single ``control'' zone. One of the key parameters for the furnace component is the fraction of the total system air flow that goes through the control zone. This fraction is calculated as the ratio of the maximum air mass flow rate for the air loop's supply inlet node for the control zone (e.g., AirTerminal:SingleDuct:Uncontrolled, field = Maximum Air Flow Rate, converted to mass flow) to the sum of the maximum air mass flow rates for the air loop's supply inlet nodes for all zones served by this air loop. The furnace module scales the calculated load for the control zone upward based on this fraction to determine the total load to be met by the furnace. The module then proceeds to calculate the required part-load ratio for the system coil and the supply air fan to meet this total load. The heating or cooling capacity delivered by the furnace is distributed to all of the zones served by this system via the terminal units that supply air to each zone. The supply air fraction that goes though the control zone is calculated as follows:
+
+\begin{equation}
+Control Zone Air Flow\,Fraction = \frac{{{{\dot m}_{TUMax\,ControlZone}}}}{{\sum\limits_{j = 1}^{NumOfZones} {{{\dot m}_{TUMax\,Zone\,j}}} }}
+\end{equation}
+
+where:
+
+\({\dot m_{TUMax\,ControlledZone}}\) ~~~ = ~~~ maximum air mass flow rate for the air loop's supply inlet node (terminal unit) for the control zone (kg/s)
+
+\({\dot m_{TUMax\,Zone\,j}}\) ~~~~~~~~~~~ = ~~~ maximum air mass flow rate for the air loop's supply inlet node for the jth zone (kg/s)
+
+\(NumOfZones\) ~~~~~~~~~~~~~~~ = ~~~ number of zones, or number of air loop supply air inlet nodes for all zones served by the air loop (-)
+
+The furnace component is able to model supply air fan operation in two modes: cycling fan -- cycling coil (i.e., AUTO fan) and continuous fan -- cycling coil (i.e., fan ON). Fan:OnOff must be used to model AUTO fan, while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON. The fan operation mode is specified using a supply air fan operating mode schedule where schedule values of 0 denote cycling fan operation and schedule values other than 0 (a 1 is usually used) denote continuous fan operation. Using this schedule, the furnace fan may be cycled with cooling or heating coil operation or operated continuously based on time of day (e.g., cycling fan operation at night and continuous fan operation during the daytime). If the fan operating mode schedule name field is left blank in the furnace object, the furnace assumes cycling or AUTO fan mode operation throughout the simulation.
+
+The only output variables reported by the furnace object are the fan part-load ratio and the compressor part-load ratio (HeatCool only). The fan part-load ratio is defined as the actual air mass flow rate through the system for the time step divided by the design supply air mass flow rate specified for the furnace (\({{{{\dot m}_{actual}}} \mathord{\left/ {\vphantom {{{{\dot m}_{actual}}} {{{\dot m}_{design}}}}} \right. } {{{\dot m}_{design}}}}\) )..The furnace operates based on the user-specified (or autosized) design supply air flow rate(s). The `design' supply air mass flow rate may be different for cooling, heating, and when no cooling or heating is required and the fan operates continuously based on user-specified inputs (HeatCool only). For the HeatCool version, If alternate air flow rates are specified for cooling, heating, and when no cooling or heating is required, the design supply air mass flow rate is the maximum of these specified values. Also for the HeatCool version, the compressor part-load ratio is reported as the ratio of the actual cooling load to the full-load sensible capacity (see Eqn. ). Reporting of other variables of interest for the furnace (heating rate, cooling rate, energy consumption, etc.) is done by the individual system components (fan, heating coil and DX cooling coil).
+
+\subsubsection{Model Description}\label{model-description-1}
+
+As described previously, the furnace is a ``virtual'' component consisting of a fan, heating coil and, for the HeatCool version, a cooling coil with an optional reheat coil. The sole purpose of the furnace model is to properly coordinate the operation of the various system components. The following sections describe the flow of information within the model for both the HeatOnly and HeatCool configurations, as well as the differences between cycling and continuous supply air fan operation. The last section describes the optional control of high zone humidity with a reheat coil for the HeatCool configuration.
+
+\subsubsection{HeatOnly Configuration}\label{heatonly-configuration}
+
+The HeatOnly configuration consists of an on/off or constant volume fan and an electric or gas heating coil. When the model is first called during an EnergyPlus simulation, all of the input data specified for each furnace in the input data file are read into data structures for use throughout the remainder of the simulation.
+
+For each simulation time step when the performance of a heat-only furnace is being modeled, the first step is to retrieve the heating load required to meet the thermostat setpoint for the ``control'' zone (see Figure~\ref{fig:schematic-of-the-energyplus-furnace-blow}. Schematic of the EnergyPlus Furnace). See the section ``Summary of Predictor-Corrector Procedure'' elsewhere in this document for more details regarding load calculations. Since the furnace may be specified to serve several zones but controlled based on the load calculated for the ``control'' zone, the total heating load to be met by the furnace is determined from the following equation:
+
+\begin{equation}
+Furnace\,Heating\,Load\, = \frac{{Control\,Zone\,Heating\,Load}}{{Control\,Zone\,Air\,Flow\,Fraction}}
+\end{equation}
+
+The model then calculates the furnace's sensible heating energy rate delivered to the zones being served when the system runs at full-load conditions and when the heating coil is OFF. If the supply air fan cycles on and off with the heater, then the sensible heating energy rate is zero when the heating coil is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible heating energy rate will not be zero when the heating coil is OFF. Calculating the sensible heating energy rate involves modeling the supply air fan (and associated fan heat) and the heating coil. For each of these cases (full load and heating coil OFF), the sensible heating energy rate delivered by the furnace is calculated as follows:
+
+\begin{equation}
+Full\;Heat\;Output = (Mass\;Flow\;Rat{e_{ful\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}
+\end{equation}
+
+\begin{equation}
+No\;Heat\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}
+\end{equation}
+
+where:
+
+\emph{Mass Flow Rate\(_{full\,load}\)} = air mass flow rate through furnace at full-load conditions, kg/s
+
+\emph{h\(_{out,\,full\,load}\)} = enthalpy of air exiting the furnace at full-load conditions, J/kg
+
+\emph{h\(_{control\, zone}\)} = enthalpy of air in the control zone (where thermostat is located), J/kg
+
+\emph{HR\(_{min}\)~~~~~~ =} enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio
+
+of the furnace exiting air or the air in the control zone
+
+\emph{Mass Flow Rate\(_{coil\, off}\)} = air mass flow rate through the furnace with the heating coil OFF, kg/s
+
+\emph{h\(_{out,\, coil\, off}\)} = enthalpy of air exiting the furnace with the heating coil OFF, J/kg
+
+Δ\(_{sen,}\) \emph{\(_{full\, load}\)} = Sensible load difference between the system output node and the zone inlet node at full-load conditions
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,full load} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,full load} - h_{ZoneInlet}}_{HRmin} \\
+                           &+ \PB{\dot{m}_{full load} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,full load} - h_{ControlZone}}_{HRmin}
+  \end{array}
+\end{equation}
+
+where:
+
+Frac = Control zone air fraction with respect to the system mass flow rate
+
+Δ\(_{sen,coil\, off}\) = Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,coil off} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,coil off} - h_{ZoneInlet}}_{HRmin} \\
+                           &+ \PB{\dot{m}_{coil off} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,full load} - h_{ControlZone}}_{HRmin}
+  \end{array}
+\end{equation}
+
+With the calculated sensible heating energy rates and the total sensible heating load to be met by the system, the part-load ratio for the furnace is estimated.
+
+\begin{equation}
+PartLoadRatio\, = \,MAX\left( {0.0,MIN\left( {1.0,\frac{{ABS\left( {FurnaceHeatingLoad - NoHeatOutput} \right)}}{{ABS(FullHeatOutput - NoHeatOutput)}}} \right)} \right)
+\end{equation}
+
+The part-load ratio calculated above is used to determine the required heating coil capacity as \(Qheating\,coil = Qdesign\,*PartLoadRatio\) where \emph{Q\(_{design}\)} is the nominal heating coil capacity as specified in the heating coil object. If the fan cycles on and off with the heating coil (i.e.,~ when the supply air fan operating mode schedule values are equal to 0), then this part-load ratio is also used to determine the operating mass flow rate of the furnace as
+
+\begin{equation}
+{\dot m_{furnace}} = {\dot m_{design}}*PartLoadRatio
+\end{equation}
+
+~If the fan operates continuously (i.e.~fan ON), the operating mass flow rate is specified as \({\dot m_{design}}\) . The furnace's fan and heating coil are then re-simulated to determine the furnace's delivered sensible heating capacity at the above calculated part-load ratio.
+
+\begin{equation}
+{Q_{furnace}} = \left( {{{\dot m}_{furnace}}} \right){\left( {{h_{out,actual}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,\;actual}}
+\end{equation}
+
+where:
+
+\(Qfurnace\) ~~~~~~ ~~ = sensible heating capacity delivered by the furnace (W)
+
+\({\dot m_{furnace}}\) ~~~~~ ~~~ = air mass flow rate through the furnace (kg/s)
+
+\emph{h\(_{out,\, actual}\)} = enthalpy of air exiting the furnace (J/kg)
+
+\emph{h\(_{out,\, control\, zone}\)} = enthalpy of air in the control zone (J/kg)
+
+\emph{HR\(_{min}\)} = enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio
+
+of the furnace exiting air or the air in the control zone
+
+\(\Delta_{sen,\, actual}\) = Sensible load difference between the system output node and the zone inlet node at the above calculated part-load ratio.
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,actual} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,actual} - h_{ZoneInlet}}_{HRmin} \\
+                           &+ \PB{\dot{m}_{furnace} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,actual} - h_{ControlZone}}_{HRmin}
+  \end{array}
+\end{equation}
+
+Since the part-load performance of the heating coil can be non-linear, and the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the heating coil and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the furnace's heating output matches the heating load to be met within the heating convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the furnace's heating output divided by the load to be met.
+
+\begin{equation}
+  Tolerance \equiv \frac{FurnaceHeatingLoad - Q_{furnace}}{FurnaceHeatingLoad} \leq 0.001
+\end{equation}
+
+If the furnace has been specified with cycling fan/cycling coil (AUTO fan), then the furnace's design air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the heating coil represent the full-load (steady-state) values when the coil is operating. If the supply air fan is specified to run continuously (fan ON), then the air mass flow rate remains at the furnace's design air mass flow rate. In this case, the air conditions at nodes downstream of the heating coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF).
+
+For the case where the furnace is scheduled to operate with continuous supply air fan operation, but no heating load is required to meet the setpoint temperature in the control zone, the supply air fan model is still called to determine the fan exiting air conditions. The heating coil model is also called, but for the case with no heating load the heating coil model simply passes the inlet air conditions and mass flow rate from its inlet node to its outlet node. The air exiting the heating coil is then sent to the direct air units for distribution to each zone served by the furnace, where the zone heat balance is performed to determine the resulting zone air conditions. The furnace exiting air conditions and energy consumption are calculated and reported by the individual component models (fan and heating coil).
+
+\subsubsection{HeatCool Configuration}\label{heatcool-configuration}
+
+The HeatCool configuration consists of an on/off or constant volume fan, a DX cooling coil, and an electric or gas heating coil. For the cases where a heating load is calculated for the control zone or no heating/cooling load is calculated for the control zone, the model follows nearly identical computational steps as described in the HeatOnly Configuration section above. The only difference is the air mass flow rate during no cooling/heating operation with continuous supply air fan operation can be different from the air mass flow rate during heater operation for the HeatCool configuration. If a cooling load is calculated by EnergyPlus for the control zone, the solution methodology is also virtually identical and is described here for completeness.
+
+If EnergyPlus determines that the furnace must supply cooling to the control zone to meet the zone air temperature setpoint, then the model computes the total sensible cooling load to be met by the furnace based on the control zone sensible cooling load and the fraction of the furnace air flow that goes through the control zone.
+
+\begin{equation}
+Furnace\,Cooling\,Load\, = \frac{{Control\,Zone\,Cooling\,Load}}{{Control\,Zone\,Air\,Flow\,Fraction}}
+\end{equation}
+
+If the supply air fan operating mode schedule requests cycling fan operation, the model first checks for the presence of an ecomomizer in the outside air system serving the furnace's air loop (Ref. AirLoopHVAC:OutdoorAirSystem). If an outside air system is not present or if an air-side economizer is not used, the furnace's compressor is used to meet the furnace cooling load. If an air-side economizer is used and is active (i.e., economizer controls indicate that conditions are favorable to increase the outside air flow rate), the furnace will try to meet the cooling load by operating only the supply air fan. If the fan is able to satisfy the furnace cooling load, the compressor remains off for the entire simulation time step. If the operation of the fan alone is unable to meet the entire cooling load, then the compressor is enabled and additional calculations are performed to determine the compressor's part-load ratio.
+
+The model then calculates the furnace's sensible cooling energy rate delivered to the zones being served when the system runs at full-load conditions and when the DX cooling coil is OFF. If the supply air fan cycles with the compressor, then the sensible cooling energy rate is zero when the cooling coil is OFF. However if the fan is configured to run continuously regardless of coil operation, then the sensible cooling energy rate will probably not be zero when the cooling coil is OFF. Calculating the sensible cooling energy rate involves modeling the supply air fan (and associated fan heat), the DX cooling coil, and the heating coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and DX cooling coil OFF), the sensible cooling energy rate delivered by the furnace is calculated as follows:
+
+\begin{equation}
+Full\;Cool\;Output = (Mass\;Flow\;Rat{e_{ful\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}
+\end{equation}
+
+\begin{equation}
+No\;Cool\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}
+\end{equation}
+
+where:
+
+\emph{Mass Flow Rate\(_{full\, load}\)} = air mass flow rate through furnace at full-load conditions, kg/s
+
+\emph{h\(_{out,\, full\, load}\)} = enthalpy of air exiting the furnace at full-load conditions, J/kg
+
+\emph{h\(_{control\, zone}\)} = enthalpy of air in the control zone (where thermostat is located), J/kg
+
+\emph{HR\(_{min}\)} = enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio
+
+of the furnace exiting air or the air in the control zone
+
+\emph{Mass Flow Rate\(_{coil\, off}\)} = air mass flow rate through the furnace with the cooling coil OFF, kg/s
+
+\emph{h\(_{out,\, coil\, off}\)} = enthalpy of air exiting the furnace with the cooling coil OFF, J/kg
+
+Δ\(_{sen,}\) \emph{\(_{full\, load}\)} = Sensible load difference between the system output node and the zone inlet node at full-load conditions
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,full load} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,full load} - h_{ZoneInlet}}_{HRmin} \\
+                           &+ \PB{\dot{m}_{full load} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,full load} - h_{ControlZone}}_{HRmin}
+  \end{array}
+\end{equation}
+where:
+
+Frac = Control zone air fraction with respect to the system mass flow rate
+
+Δ\(_{sen,coil\, off}\)** = Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,coil off} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,coil off} - h_{ZoneInlet}}_{HRmin} \\
+                           &+ \PB{\dot{m}_{coil off} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,coil off} - h_{ControlZone}}_{HRmin}
+  \end{array}
+\end{equation}
+
+With the calculated sensible cooling energy rates and the total sensible cooling load to be met by the system, the part-load ratio for the furnace is estimated.
+
+\begin{equation}
+PartLoadRatio\, = \,MAX\left( {0.0,\frac{{ABS\left( {Furnace\,Cooling\,Load - NoCoolOutput} \right)}}{{ABS\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)
+\end{equation}
+
+Since the part-load performance of the DX cooling coil is frequently non-linear (Ref: DX Cooling Coil Model), and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the furnace's cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the furnace's cooling output divided by the load to be met.
+
+\begin{equation}
+  Tolerance \equiv \frac{FurnaceHeatingLoad - Q_{furnace}}{FurnaceHeatingLoad} \leq 0.001
+\end{equation}
+
+where:
+
+\(Qfurnace\) = Furnace delivered sensible capacity (W)
+
+If the furnace has been specified with cycling fan/cycling coil (AUTO fan) and high humidity control \emph{has not} been specified, then the furnace's operating supply air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the cooling coil represent the full-load (steady-state) values when the coil is operating. If a cycling fan is used and high humidity control \emph{has} been specified, the calculation of average air mass flow rate is based on the greater of the heating or cooling part-load ratio (see following section on high humidity control). When the heating part-load ratio is greater than the cooling part-load ratio, the air conditions at nodes downstream of the cooling coil represent the weighted average of full-load conditions when the cooling coil is operating and inlet air conditions when the cooling coil is off (i.e., the fan continues to operate due to a heating requirement where the heating PLR is greater than the cooling PLR). If the supply air fan is specified to run continuously (fan ON), then the air mass flow rate continues to operate at the user-specified supply air mass flow rate when no cooling or heating is required. In this case, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF). The furnace exiting air conditions and energy consumption are calculated and reported by the individual component models (fan and DX cooling coil).
+
+\subsubsection{High Humidity Control with HeatCool Configuration}\label{high-humidity-control-with-heatcool-configuration}
+
+An optional reheat coil can be specified with the HeatCool configuration to allow the furnace to control high zone humidity levels. The specific configuration of the HeatCool Furnace with high humidity control option is shown in Figure~\ref{fig:schematic-for-blow-through-furnace-with-high}. The figure below shows the fan placement when a blow through fan is specified. If a draw through fan is specified, the fan is located between the heating coil and the reheat coil. The system is controlled to keep the relative humidity in the control zone from exceeding the setpoint specified in the object ZoneControl:Humidistat. This option is available when the supply air fan operates continuously (i.e., the supply air fan operating mode schedule values are never equal to 0) or the supply air fan cycles with the compressor. For the case of cycling fan mode when the high humidity control is specified as CoolReheat \emph{and} the heating part-load ratio is greater than the compressor part-load ratio, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions during the duration of fan operation (i.e., the weighted average of full load conditions when the coil is operating and inlet air conditions when the coil is off and the fan continues to operate to meet the heating load). For the case where cycling fan mode is used \emph{and} the heating part-load ratio is less than the compressor part-load ratio, the air conditions at the nodes downstream of the cooling coil are simply the full load (steady-state) values when the coil is operating. In addition, when high humidity control is specified and the compressor operates, the furnace operates at the cooling air flow rate when a zone heating load is present as determined by the zone thermostat.
+
+High humidity control is specified as either None, MultiMode, or CoolReheat in the Dehumidification Control Type input field. MultiMode is specified when a heat exchanger is used to improve the dehumidification performance of the cooling coil. The heat exchanger will be activated when the sensible part-load ratio is insufficient to meet the zone latent load. CoolReheat is specified when a DX cooling coil is used to over-cool the supply air stream in order to meet the zone latent load. In this case, a reheat coil will ensure the zone temperature does not fall below the zone heating temperature set point. When a heat exchanger is used in conjunction with a DX cooling coil and CoolReheat is specified as the Dehumidification Control Type, the heat exchanger is ``locked on'' to meet either the sensible or latent cooling load. If the dehumidification control type is selected as None and a heat exchanger assisted cooling coil is used, the heat exchanger is ``locked on'' and the air conditioner runs only to meet the sensible cooling load. Although a reheat coil is required when CoolReheat is specified in the Dehumidification Control Type input field, this reheat coil may optionally be present for the other Dehumidification Control Types (e.g., None and Multimode). If the reheat coil is present and the dehumidification control type input is not specified as CoolReheat, the reheat coil will not be active. This allows changing the dehumidification control option without requiring a change in the unit's coil configuration.
+
+The model first calculates the PartLoadRatio required to meet the sensible cooling load as described above (see Eqn. ) to maintain the dry-bulb temperature setpoint in the control zone. If a moisture (latent) load exists because the control zone humidity has exceeded the setpoint, the total moisture load to be met by the HeatCool furnace (SystemMoistureLoad) is calculated based on the control zone moisture load and the control zone air flow fraction. The model then calculates the LatentPartLoadRatio required to meet the humidistat setpoint.
+
+\begin{equation}
+SystemMoistureLoad\, = \frac{{Control\,Zone\,Moisture\,Load}}{{Control\,Zone\,Air\,Flow\,Fraction}}
+\end{equation}
+
+\begin{equation}
+LatentPartLoadRatio\, = \,MAX\left( {MinPLR,\frac{{ABS\left( {SystemMoistureLoad - NoLatentOutput} \right)}}{{ABS\left( {FullLatentOutput - NoLatentOutput} \right)}}} \right)
+\end{equation}
+
+where:
+
+\emph{FullLatentOutput~~} = the furnace's latent cooling energy rate at full-load conditions, W
+
+\emph{NoLatentOutput}~~~~ = the furnace's latent cooling energy rate with the cooling coil OFF, W
+
+\emph{MinPLR}~~~~~~~~~~~~~~~ = the minimum part-load ratio, which is usually 0.0. For the case when the latent capacity degradation model is used (Ref: DX Cooling Coil Model), this value is the minimum part-load ratio at which the cooling coil will dehumidify the air.
+
+The model uses the greater of the two part-load ratios, PartLoadRatio or LatentPartLoadRatio, to determine the operating part-load ratio of the furnace's DX cooling coil. As previously described, iterations are performed to converge on the solution within the convergence tolerance.
+
+\begin{figure}[hbtp] % fig 222
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5049.png}
+\caption{Schematic for Blow Through Furnace with High Humidity Control \protect \label{fig:schematic-for-blow-through-furnace-with-high}}
+\end{figure}
+
+If the model determines that the LatentPartLoadRatio is to be used as the operating part-load ratio of the furnace's cooling coil, the reheat coil is used to offset the excess sensible capacity provided by the unit. The model first checks the sensible load that exists for the current simulation time step (predicted zone temperature with no HVAC operation compared to the thermostat setpoint temperatures). If a sensible cooling load or no sensible cooling or heating load exists (Figure~\ref{fig:reheat-coil-load-when-predicted-zone}), the model calculates the difference between the sensible heating load required to reach or maintain the heating dry-bulb temperature setpoint and the actual sensible cooling energy rate delivered by the unit (with LatentPartLoadRatio). In this case, the reheat coil is used to offset the excess sensible cooling energy provided by the DX cooling coil (if any) that could have caused an overshoot of the heating dry-bulb temperature setpoint. Note that when a humidistat is used and high humidity control is required, the zone dry-bulb temperature will typically move toward the heating temperature setpoint when a high moisture (latent) load exists. If a heating load exists (Figure~\ref{fig:reheat-coil-load-when-predicted-zone-001}), the reheat coil is used to offset the entire sensible cooling energy rate of the DX cooling coil (to meet the humidistat setpoint) and the heating coil is used to meet the entire heating load as described in the HeatOnly configuration section above. Note that when a heating load exists and high humidity control is required, the furnace operates at the user-specified cooling air flow rate for the entire simulation time step. As with the fan, DX cooling coil, and heating coil, report variables associated with reheat coil performance (e.g., heating coil energy, heating coil rate, heating coil gas or electric consumption, heating coil runtime fraction, etc.) are managed in the reheat (heating) coil object.
+
+\begin{figure}[hbtp] % fig 223
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5050.png}
+\caption{Reheat Coil Load when Predicted Zone Temperature is Above Heating Setpoint \protect \label{fig:reheat-coil-load-when-predicted-zone}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 224
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5051.png}
+\caption{Reheat Coil Load when Predicted Zone Temperature is Below Heating Setpoint \protect \label{fig:reheat-coil-load-when-predicted-zone-001}}
+\end{figure}
+
+\subsection{Unitary Systems}\label{unitary-systems-1}
+
+The input objects AirLoopHVAC:UnitaryHeatCool and AirLoopHVAC:UnitaryHeatOnly provides models that are identical to the Furnace and Central Air models described above.~ Please reference the previous section for details.
+
+\subsection{Unitary System with Changeover-Bypass-Variable Air Volume}\label{unitary-system-with-changeover-bypass-variable-air-volume}
+
+\subsubsection{Overview}\label{overview-2}
+
+The input object AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass provides a model for a changeover-bypass variable air volume (CBVAV) unitary system that is a compound object made up of other components. Each CBVAV system consists of an outside air mixer, direct expansion (DX) cooling coil, heating coil, and a supply air fan as shown in the figures below. Zone thermostats and terminal units are required in each zone served by this system. The terminal units are specific to this system type and are either AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat or AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat. A zone humidistat and single zone max humidity setpoint manager may also be specified to help control high humidity levels. These individual components are described elsewhere in this document. The CBVAV unitary system object coordinates the operation of these components and is modeled as a type of air loop equipment (Ref. AirLoopHVAC).
+
+\begin{figure}[hbtp] % fig 225
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5052.png}
+\caption{Schematic of a Changeover Bypass VAV Unitary System with Draw Through Fan \protect \label{fig:schematic-of-a-changeover-bypass-vav-unitary}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 226
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5053.png}
+\caption{Schematic of Changeover Bypass VAV Unitary System with Blow Through Fan \protect \label{fig:schematic-of-changeover-bypass-vav-unitary}}
+\end{figure}
+
+The CBVAV unitary system conditions one or more zones and is controlled by thermostats located in each zone (the use of a single humidistat is also allowed when using multi-mode DX cooling coils). The CBVAV system operates to meet the zone sensible cooling or sensible heating requirements as dictated by the thermostat schedule(s). The priority control input determines the mode of operation and is specified as Cooling Priority, Heating Priority, or Zone Priority. If Cooling Priority is specified, the system operates to meet the cooling load when any zone served by this system (air loop) requires cooling. If Heating Priority is specified, the system operates to meet the heating load when any zone requires heating. If Zone Priority is specified, the system operates based on the maximum number of zones requiring either heating or cooling.
+
+Once the operating mode is determined, the CBVAV model calculates a target supply air temperature required to operate a single terminal unit at its maximum air flow rate. The remaining terminal units will modulate as required to maintain the dry-bulb temperature in the zone they are serving according to the thermostat schedule for their respective zone. The system air flow rate (through the supply air fan, cooling coil and heat coil) remains constant during cooling operation, heating operation, and no cooling/heating mode as specified by the user. Therefore, as the zone terminal units modulate to reduce zone air flow rates, the excess system air flow is ``bypassed'' from the bypass duct splitter node back to the bypass duct mixer node of the CBVAV system (see figures above).
+
+The CBVAV system is able to model supply air fan operation in two modes: cycling fan -- cycling coil (i.e., AUTO fan) and continuous fan -- cycling coil (i.e., fan ON). A Fan:OnOff or Fan:ConstantVolume is used in either case. Since the excess system air flow is bypassed while the zone terminal units modulate, the supply air fan operates the entire simulation time step when heating or cooling is required. For this reason, AUTO fan only allows the supply air fan to turn off when no cooling or heating is required. If fan ON is specified, the supply air fan runs the entire time the system is scheduled to operate (via its availability schedule). The mode of operation for the supply air fan is specified through a fan operating mode schedule where a value of 0 in the schedule indicates cycling fan mode and a value greater than 0 indicates continuous fan mode. If the schedule is not provided, the supply air fan operating mode is considered to be continuous (fan ON).
+
+Output variables reported for the CBVAV system include the supply air fan part-load ratio, the compressor part-load ratio, and the electric consumption of the CBVAV system. Additional output variables report the total heating rate and total cooling rate provided by the CBVAV system. The sensible and latent components for total system cooling and heating are also available as output variables. Reporting of other variables of interest for the CBVAV system (DX coil cooling rate, heating rate, crankcase electric power and energy, supply air fan electric power, etc.) is done by the individual system components (fan, DX cooling coil, and heating coil).
+
+\subsubsection{Model Description}\label{model-description-2}
+
+As described previously, the CBVAV system conditions one or more zones and is controlled by zone thermostats (Ref. ZoneControl:Thermostat). For each simulation time step, EnergyPlus performs a zone air heat balance to determine if cooling or heating is required to meet the zone thermostat setpoints, excluding any impacts from CBVAV system operation. CBVAV system performance is then modeled with all heating/cooling coils off but with the supply air fan operating according to the user specified supply air fan operating mode schedule. If the zone air heat balance plus the impact of CBVAV system operation with coils off results in no requirement for heating or cooling by the CBVAV coils, or if the CBVAV system is scheduled off (via its availability schedule), then the CBVAV coils do not operate and the compressor part-load ratio output variable is set to 0. If the model determines that cooling or heating is required and the CBVAV system is scheduled to operate, the model calculates a target supply air temperature required to maintain a single terminal unit at it's maximum air flow rate, the amount of bypass air returning to the bypass duct mixer node, and the part-load ratio of the cooling or heating coils in order to meet the target supply air temperature.
+
+When high humidity control is desired, a ZoneControl:Humidistat input object and a SetpointManager:SingleZone:Humidity:Maximum, SetpointManager:MultiZone:MaximumHumidity:Average~ ~~or SetpointManager:MultiZone:Humidity:Maximum object are required. The air outlet node of the CBVAV system is used as the control node for the setpoint manager. For this reason, only a single humidistat should be specified for one of the zones being served by this system. If humidistat/setpoint manager objects are specified for more than one zone served by this system, only the last of the SetpointManager:SingleZone:Humidity:Maximum objects is used (the setpoint manager objects are read in order of occurrence in the input file). Since the outlet node of the CBVAV system is always used as the control node, the setpoints calculated by the previous setpoint managers are overwritten by the last setpoint manager in the input. When a heat exchanger is used to improve the dehumidification performance of the cooling coil (i.e.~CoilSystem:Cooling:DX:HeatExchangerAssisted), the heat exchanger is always active and can not be turned on and off based on zone humidity levels.
+
+The remainder of this section describes the calculations performed when cooling or heating coil operation is required. For any HVAC simulation time step, the CBVAV system can only cool or heat the air, not both. Because the CBVAV system bypasses system air flow back to the inlet of the CBVAV unit, the system operates for the entire simulation time step. If the user specifies continuous fan operation, then the supply air fan continues to operate at a user-specified flow rate even during periods when the coils cycle off. If the user specifies AUTO fan operation, then the supply air fan cycles off for the entire simulation time step only when no cooling or heating is required.
+
+\paragraph{Operating Mode}\label{operating-mode}
+
+The first step in modeling a CBVAV system is to obtain the cooling or heating load for each zone as calculated by EnergyPlus based on the zone thermostat setpoint temperature(s). The calculated loads for each zone are used to determine the total cooling and heating requirements for all zones served by this system. In addition to summing the zone cooling and heating loads, the number of zones in cooling and the number of zones in heating are totalized. The priority control mode specified by the user is then used to determine the operating mode for this simulation time step.
+
+If Cooling Priority is specified and the total cooling requirement in all zones is not equal to zero, then cooling is selected as the operating mode. If the total cooling requirement is equal to zero and the total heating requirement is not equal to zero, then heating is selected as the operating mode. If the total cooling requirement and total heating requirement are equal to zero then the zones are allowed to float (no heating or cooling provided).
+
+If Heating Priority is specified and the total heating requirement in all zones is not equal to zero, then heating is selected as the operating mode. If the total heating requirement is equal to zero and the total cooling requirement is not equal to zero, then cooling is selected as the operating mode. If the total cooling requirement and total heating requirement are equal to zero then the zones are allowed to float (no heating or cooling provided).
+
+If Zone Priority is specified and the total number of zones requiring cooling is greater than the total number of zones requiring heating, then cooling is selected as the operating mode. If the total number of zones requiring heating is greater than the total number of zones requiring cooling, then heating is selected as the operating mode. If the total number of zones requiring cooling is equal to the total number of zones requiring heating, then the magnitude of the total cooling and heating requirements for all zones sets the operating mode. In this case, if the magnitudes of the cooling and heating requirements are zero, then the zones are allowed to float (no heating or cooing provided). If the magnitudes of the cooling and heating requirements are non-zero and identical, then cooling is selected as the operating mode.
+
+\paragraph{Calculation of Bypass Duct Mixer Node Conditions}\label{calculation-of-bypass-duct-mixer-node-conditions}
+
+The operation of this system is unique in that it uses constant-air-volume equipment to provide variable air volume to the conditioned zones. This is accomplished with the use of a bypass duct (shown in the figures above) which shunts excess system air flow from the bypass duct splitter node at the system's outlet back to the bypass duct mixer node at the system's inlet. The air conditions at the bypass duct mixer node are based on the inlet air to the CBVAV system, the system outlet air conditions required to meet the zone loads, and the fraction of bypassed air. The following calculations are performed each simulation time step.
+
+\begin{equation}
+BypassFrac = 1.0 - \left( {\frac{{{{\dot m}_{supply}}}}{{{{\dot m}_{system}}}}} \right)
+\end{equation}
+
+\begin{equation}
+{T_{bypassductmixernode}} = \left( {1 - BypassFrac} \right){T_{inlet}} + \left( {BypassFrac} \right){T_{outlet}}
+\end{equation}
+
+\begin{equation}
+{\omega_{bypassductmixernode}} = \left( {1 - BypassFrac} \right){\omega_{inlet}} + \left( {BypassFrac} \right){\omega_{outlet}}
+\end{equation}
+
+\begin{equation}
+{h_{bypassductmixernode}} = PsyHFnTdbW\left( {{T_{mixerinlet}},{\omega_{mixerinlet}}} \right)
+\end{equation}
+
+where:
+
+\(BypassFrac\) ~~~~~ = fraction of system air directed to the bypass duct mixer node
+
+\({\dot m_{supply}}\) ~~~~~~~~~~~~~~~~ = Air mass flow rate at the system's air outlet node, kg/s
+
+\({\dot m_{system}}\) ~~~~~~~~~~~~~~~~ = Air mass flow rate through CBVAV system (coils and supply air fan), kg/s
+
+\({T_{bypassductmixernode}}\) ~~~ = Air temperature at the bypass duct mixer node, °C
+
+\({T_{inlet}}\) ~~~~~~~~~~~~~~~~~~~ = Air inlet node temperature, °C
+
+\({T_{outlet}}\) ~~~~~~~~~~~~~~~~~~ = Air outlet node temperature, °C
+
+\({\omega_{bypassductmixernode}}\) ~~ = Air humidity ratio at the bypass duct mixer node, kg/kg
+
+\({\omega_{inlet}}\) ~~~~~~~~~~~~~~~~~~ = Air inlet node humidity ratio, kg/kg
+
+\({\omega_{outlet}}\) ~~~~~~~~~~~~~~~~~ = Air outlet node humidity ratio, kg/kg
+
+\({h_{bypassductmixernode}}\) ~~~ = Air enthalpy at the bypass duct mixer node, J/kg
+
+\(PsyHFnTdbW\) ~ = Psychrometric function calculating enthalpy given dry-bulb temperature and humidity ratio
+
+\paragraph{Cooling Operation}\label{cooling-operation}
+
+If the model determines that the CBVAV system must supply cooling to the zones, the model first calculates a target outlet air dry-bulb temperature required to operate a single terminal unit at its maximum air flow rate. The minimum target temperature for all zones is used to control the CBVAV system in cooling mode.
+
+\begin{equation}
+  T_{target}^i = T_{Zone}^i + \frac{Q_{Zone}^i}{\dot{m}_{zone,max}^i C_p} \quad \forall i \in \RB{1,n}
+\end{equation}
+
+\begin{equation}
+{T_{target}} = MIN\left( {T_{target}^i} \right);\,\,i = 1,n
+\end{equation}
+
+where:
+
+\(T_{target}^i\) ~~~~~ = Target supply air temperature for zone \emph{i}, °C
+
+\(T_{zone}^i\) ~~~~~~~ = Air temperature in zone \emph{i}, °C
+
+\(Q_{zone}^i\) ~~~~~~ = Cooling or heating load for zone \emph{i} (cooling loads are negative values, ~~~~ heating loads are positive values), W
+
+\(Cp\) ~~~~~~~~~ = Specific heat of supply air with coils off, J/kg-K
+
+\(\dot m_{zone,max}^i\) ~ = Maximum terminal unit mass flow rate in zone \emph{i}, kg/s
+
+\(T_{target}^{}\) ~~~~~ = Target supply (outlet) air temperature for the CBVAV system, °C
+
+The model then calculates the part-load ratio of the DX compressor required to meet the target supply (outlet) air temperature. Since the part-load performance of the DX cooling coil is frequently non-linear (Ref: Coil:Cooling:DX:SingleSpeed model), the actual part-load ratio for the cooling coil compressor is determined through iterative calculations (successive modeling of the DX cooling coil model) until the CBVAV system's outlet air temperature (including on/off cycling effects of the DX coil) matches the target supply (outlet) air temperature within a small temperature convergence tolerance (1E-5 ËšC).
+
+Since the supply air fan operates continuously for each simulation time step (or is OFF for the entire HVAC system time step), the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of coil's outlet node conditions when the coil is operating and the coil's inlet node conditions when the coil is OFF).
+
+\paragraph{Heating Operation}\label{heating-operation}
+
+Modeling the CBVAV system's DX heating coil is identical to the calculations described above for cooling operation except that the maximum target supply air temperature for all zones is used to control the CBVAV system in heating mode.
+
+\begin{equation}
+{T_{target}} = MAX\left( {T_{target}^i} \right);\,\,i = 1,n
+\end{equation}
+
+Iterative calculations (successive modeling of the DX heating coil model) are used to determine the final heating coil part-load ratio to account for the non-linear performance of the DX heating coil at part-load conditions.
+
+When a gas or electric heating coil is used instead of a DX heating coil, the amount of heat required by the coil is calculated based on the target supply (outlet) air temperature and the coil inlet air temperature as follows:
+
+\begin{equation}
+{Q_{heating}} = {\dot m_{system}}{C_p}({T_{target}} - {T_{inlet,heatcoil}})
+\end{equation}
+
+where:
+
+\({Q_{heating}}\) ~~~~~~ = Heating coil load, W
+
+\({C_p}\) ~~~~~~~~~~~~ = Specific heat of heating coil inlet air, J/kg-K
+
+\({T_{inlet,heatcoil}}\) ~ = Heating coil inlet air temperature, °C
+
+\paragraph{Floating Operation (no cooling or heating)}\label{floating-operation-no-cooling-or-heating}
+
+When the zone thermostats determine that there is no cooling or heating requirement in any zone, the CBVAV coils are OFF and the zone temperatures are allowed to float. However, a special case exists where the user specifies continuous supply air fan operation and no cooling or heating requirements exist in any zone. In this case, the outlet air temperature of the CBVAV system (with fan ON and coils OFF) is compared to the target outlet air temperatures required to maintain the zone's cooling and heating setpoint temperatures. If the outlet air temperature with the supply fan ON and coils OFF is below the target outlet air temperature required to maintain the heating setpoint, then heating mode is enabled to avoid overshooting the zone heating setpoint temperature. Conversely, if the outlet air temperature with the supply fan ON and coils OFF is above the target outlet air temperature required to maintain the cooling setpoint, then cooling mode is enabled to avoid overshooting the zone cooling setpoint temperature. This special case is handled at any time a no load condition is reported by the thermostats and overshooting the zone air temperature setpoint is possible regardless of the priority control mode selected by the user.
+
+\paragraph{Minimum and Maximum Outlet Air Temperature in Cooling/Heating Operation}\label{minimum-and-maximum-outlet-air-temperature-in-coolingheating-operation}
+
+The user also specifies a minimum outlet air temperature during cooling operation and a maximum outlet air temperature during heating operation. The target outlet air temperature, as calculated above, is compared to each of these limits during each simulation time step. The resulting target outlet air temperature is used to control the heating and cooling coils.
+
+\begin{equation}
+{T_{target}} = MAX\left( {{T_{target}},\,\,{T_{min,cooling}}} \right)
+\end{equation}
+
+\begin{equation}
+{T_{target}} = MIN\left( {{T_{target}},\,\,{T_{max,heating}}} \right)
+\end{equation}
+
+where:
+
+\({T_{min,cooling}}\) = Minimum outlet air temperature during cooling operation, °C
+
+\({T_{max,heating}}\) = Maximum outlet air temperature during heating operation, °C
+
+\paragraph{Air Flow Calculations}\label{air-flow-calculations}
+
+The changeover-bypass VAV system operates based on user-specified (or autosized) air flow rates. The CBVAV system air flow rate (i.e., air flow through the supply air fan and heating/cooling coils) during cooling operation may be different than the system air flow rate during heating operation. In addition, the system air flow rate when no cooling or heating is required but the supply air fan remains ON can be different than the air flow rates when cooling or heating is required. The outside air flow rates can likewise be different in these various operating modes. The model takes these different air flow rates into account when simulating the performance of the CBVAV system. The system air flow rate for each simulation time step is based on the current operating mode (cooling, heating, or no cooling/heating) and is reported on the inlet/outlet air nodes of the various CBVAV components (e.g.~fan, cooling coil, and heating coil). The supply air flow rate delivered to the individual zones is calculated based on the sum of the air flow rates through each terminal unit and is reported at the air inlet and outlet nodes of the CBVAV system each simulation time step. The difference between the system air mass flow rate and the supply air mass flow rate delivered to all zones is equal to the bypass air mass flow rate which is also reported each simulation time step.
+
+The system and outside air flow rates when a system coil is ON (e.g., system air volumetric flow rate during cooling operation, system air volumetric flow rate during heating operation, outside air volumetric air flow rate during cooling operation, and outside air volumetric air flow rate during heating operation) or the system coils are OFF and the fan operates continuously (e.g., system air volumetric flow rate when no cooling or heating is needed and outside air volumetric air flow rate when no cooling or heating is needed) are specified by the user, or can be autosized, and are converted from volumetric flow rate to mass flow rate at standard conditions. If the user has specified cycling fan operation, then the system air and outside air mass flow rates when the system coils are OFF the entire time step are zero. If the user has specified constant fan operation, then the air flow rates when no cooling or heating is needed are used when the system coils are OFF the entire time step.
+
+There is one special case. If the user has specified constant fan operation and they specify that the system air volumetric flow rate when no cooling or heating is needed is zero (or if the field is left blank), then the model assumes that the system air mass flow rate when the system coils are OFF the entire time step is equal to the corresponding air mass flow rate when any system coil was last operating (ON). This model handles the zero (or blank) entry for outside air volumetric flow rate when no cooling or heating is needed in an analogous fashion.
+
+\begin{equation}
+{\dot m_{system}} = {\rho_{air,std}}*{\dot V_{mode}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{system,OA}} = {\rho_{air,std}}*{\dot V_{mode,OA}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{supply}} = \sum\limits_{i = 1}^n {{{\dot m}_{zone}}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{bypass}} = {\dot m_{system}} - {\dot m_{supply}}
+\end{equation}
+
+where:
+
+\(\rho air,std\) ~~~~~~~~~~~~ = standard air density (1.204 kg/m\(^{3}\)) adjusted for the local barometric pressure (standard barometric pressure corrected for altitude, ASHRAE 1997 HOF pg. 6.1), kg/m\(^{3}\)
+
+\({\dot V_{mode}}\) ~~~~~~~~~~~~~~~ = User-specified system volumetric flow rate in cooling, heating, or no cooling or heating mode, m\(^{3}\)/s
+
+\({\dot m_{system,OA}}\) ~~~~~~~~~ = Outdoor air mass flow rate introduced through the CBVAV system, kg/s
+
+\({\dot V_{mode,OA}}\) ~~~~~~~~~~~ = User-specified outdoor air volumetric flow rate in cooling, heating, or no cooling or heating mode, m\(^{3}\)/s
+
+\paragraph{Calculation of System Heating and Cooling Rates}\label{calculation-of-system-heating-and-cooling-rates}
+
+At the end of each HVAC simulation time step, this object reports the heating or cooling rate and energy delivered by the system, as well as the electric power and consumption by the system. In terms of thermal energy delivered by the system, the sensible, latent and total energy transfer rates for the system are calculated as follows:
+
+\begin{equation}
+{\dot Q_{total}} = ({\dot m_{supply}})({h_{outlet}} - {h_{inlet}})
+\end{equation}
+
+\begin{equation}
+{\dot Q_{sensible}} = ({\dot m_{supply}}){({h_{outlet}} - {h_{inlet}})_{HRmin}}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{latent}} = {\dot Q_{total}} - {\dot Q_{sensible}}
+\end{equation}
+
+where:
+
+\(\dot{Q}_{total}\) = total energy transfer rate by the system, W
+
+\(\dot{Q}_{sensible}\) = sensible energy transfer rate by the system, W
+
+\(\dot{Q}_{latent}\) = latent energy transfer rate by the system, W
+
+\emph{h\(_{inlet}\)} = enthalpy of the air entering the unit at its inlet node, J/kg
+
+\emph{h\(_{outlet}\)} = enthalpy of the air leaving the unit at its outlet node, J/kg
+
+\(H{R_{min}}\) = minimum of the inlet air and outlet air humidity ratio, kg/kg
+
+Since each of these energy transfer rates can be calculated as positive or negative values, individual reporting variables are established for cooling and heating and only positive values are reported. The following calculations are representative of what is done for each of the energy transfer rates:
+
+If $\dot{Q}_{total}<0$, then:
+
+\begin{equation}
+  \begin{array}{rl}
+    \dot{Q}_{total,cooling} &= \left|\dot{Q}_{total}\right| \\
+    \dot{Q}_{total,heating} &= 0
+  \end{array}
+\end{equation}
+
+Else:
+
+\begin{equation} 
+  \begin{array}{rl}
+    \dot{Q}_{total,cooling} &= 0.0 \\
+    \dot{Q}_{total,heating} &= \dot{Q}_{total}
+  \end{array}
+\end{equation}
+
+where:
+
+\(\dot{Q}_{total,cooling}\) = output variable `Unitary System Total Cooling Rate, W'
+
+\(\dot{Q}_{total,heating}\) = output variable `Unitary System Total Heating Rate, W'
+
+In addition to heating and cooling rates, the heating and cooling energy supplied by the system are also calculated for the time step being reported. The following example for total zone cooling energy is representative of what is done for the sensible and latent energy as well as the heating counterparts.
+
+\begin{equation}
+{Q_{total,cooling}} = {\dot Q_{total,cooling}}*TimeStepSys*3600
+\end{equation}
+
+where: \(Q_{total,cooling}\) = output variable `Unitary System Total Cooling Energy, J'
+
+\emph{TimeStepSys}~ = HVAC system simulation time step, hr
+
+3600~~~~~~~~~~~~~ = conversion factor, sec/hr
+
+\subsubsection{Changeover-bypass VAV Unitary System Sizing}\label{changeover-bypass-vav-unitary-system-sizing}
+
+The changeover-bypass VAV system is modeled as an air loop component and is sized according to the methodology described elsewhere in this document (Ref. System Design Loads and Air Flow Rates). The following volumetric air flow rates may be autosized:
+
+·~~~~~~~~system air volumetric flow rate during cooling operation
+
+·~~~~~~~~system air volumetric flow rate during heating operation
+
+·~~~~~~~~system air volumetric flow rate when no cooling or heating is needed
+
+·~~~~~~~~outside air volumetric air flow rate during cooling operation
+
+·~~~~~~~~outside air volumetric air flow rate during heating operation
+
+·~~~~~~~~outside air volumetric air flow rate when no cooling or heating is needed
+
+\subsection{Unitary Air-To-Air Heat Pump}\label{unitary-air-to-air-heat-pump}
+
+\subsubsection{Overview}\label{overview-3}
+
+The input object AirLoopHVAC:UnitaryHeatPump:AirToAir provides a model for an air-to-air heat pump that is a ``virtual'' component that consists of an on/off or constant volume fan component, a DX cooling coil, a DX heating coil, and a gas or electric supplemental heating coil. The specific configuration of the blow through heat pump is shown in the following figure. For a draw through heat pump, the fan is located between the DX heating coil and the supplemental heating coil.
+
+\begin{figure}[hbtp] % fig 227
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5106.png}
+\caption{Schematic of a Blow Through Air-to-Air Heat Pump \protect \label{fig:schematic-of-a-blow-through-air-to-air-heat}}
+\end{figure}
+
+While the heat pump may be configured to serve multiple zones, system operation is controlled by a thermostat located in a single ``control'' zone. One of the key parameters for the heat pump component is the fraction of the total system airflow that goes through the control zone. This fraction is calculated as the ratio of the maximum air mass flow rate for the air loop's supply inlet node for the control zone (e.g., AirTerminal:SingleDuct:Uncontrolled, field = Maximum Air Flow Rate, converted to mass flow) to the sum of the maximum air mass flow rates for the air loop's supply inlet nodes for all zones served by this air loop. The heat pump module scales the calculated load for the control zone upward based on this fraction to determine the total load to be met by the heat pump. The module then proceeds to calculate the required part-load ratio for the system coil and the supply air fan to meet this total load. The heating or cooling capacity delivered by the heat pump is distributed to all of the zones served by this system via the direct air units that supply air to each zone. The supply air fraction that goes though the control zone is calculated as follows:
+
+\begin{equation}
+Control Zone Air Flow\,Fraction = \frac{{{{\dot m}_{TUMax\,ControlZone}}}}{{\sum\limits_{j = 1}^{NumOfZones} {{{\dot m}_{TUMax\,Zone\,j}}} }}
+\end{equation}
+
+where:
+
+\({\dot m_{TUMax\,ControlledZone}}\) ~~~ = ~~~ maximum air mass flow rate for the air loop's supply inlet node (terminal unit) for the control zone (kg/s)
+
+\({\dot m_{TUMax\,Zone\,j}}\) ~~~~~~~~~~~ = ~~~ maximum air mass flow rate for the air loop's supply inlet node for the jth zone (kg/s)
+
+\(NumOfZones\) ~~~~~~~~~~~~~~~ = ~~~ number of zones, or number of air loop supply air inlet nodes for all zones served by the air loop (-)
+
+The heat pump component is able to model supply air fan operation in two modes: cycling fan -- cycling coil (i.e., AUTO fan) and continuous fan -- cycling coil (i.e., fan ON). Fan:OnOff must be used to model AUTO fan, while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON. The fan operation mode is specified using a supply air fan operating mode schedule where schedule values of 0 denote cycling fan operation and schedule values other than 0 (a 1 is usually used) denote continuous fan operation. Using this schedule, the furnace fan may be cycled with cooling or heating coil operation or operated continuously based on time of day (e.g.~cycling fan operation at night and continuous fan operation during the day). If the fan operating mode schedule name field is left blank in the heat pump object, the heat pump assumes cycling or AUTO fan mode operation throughout the simulation.
+
+The output variables reported by the heat pump object are fan part-load ratio and compressor part-load ratio. Fan part-load ratio is defined as the actual air mass flow rate through the system for the time step divided by the operating supply air mass flow rate specified for the heat pump (\({{\mathop m\limits^\cdot actual} \mathord{\left/ {\vphantom {{\mathop m\limits^\cdot actual} {\mathop m\limits^\cdot }}} \right. } {\mathop m\limits^\cdot }}ON\) ). The operating supply air mass flow rate may be different for cooling, heating, and when no cooling or heating is required and the fan operates continuously. Compressor part-load ratio is the actual load for the time step divided by the full-load sensible capacity (see Eqn. or Eqn.). Reporting of other variables of interest for the heat pump (heating rate, cooling rate, energy consumption, etc.) is done by the individual system components (fan, DX cooling coil, DX heating coil, and supplemental heating coil).
+
+\subsubsection{Model Description}\label{model-description-3}
+
+As described previously, the heat pump is a ``virtual'' component consisting of a fan, DX cooling coil, DX heating coil and a supplemental heating coil. The sole purpose of the heat pump model is to properly coordinate the operation of the various system components. The following sections describe the flow of information within the model, as well as the differences between cycling and continuous supply air fan operation.
+
+\subsubsection{Cooling Operation}\label{cooling-operation-1}
+
+If EnergyPlus determines that the heat pump must supply cooling to the control zone to meet the zone air temperature setpoint, then the heat pump model computes the total sensible cooling load to be delivered to the zones being served based on the control zone sensible cooling load and the fraction of the heat pump air flow that goes through the control zone.
+
+\begin{equation}
+Heat\,Pump\,Cooling\,Load\, = \frac{{Control\,Zone\,Cooling\,Load}}{{Control\,Zone\,Air\,Flow\,Fraction}}
+\end{equation}
+
+If the supply air fan operating mode schedule requests cycling fan operation, the model first checks for the presence of an ecomomizer in the outside air system serving the heat pump's air loop (Ref. AirLoopHVAC:OutdoorAirSystem). If an outside air system is not present or if an air-side economizer is not used, the heat pump's compressor is used to meet the heat pump cooling load. If an air-side economizer is used and is active (i.e., economizer controls indicate that conditions are favorable to increase the outside air flow rate), the heat pump will try to meet the cooling load by operating only the supply air fan. If the fan is able to satisfy the heat pump cooling load, the compressor remains off for the entire simulation time step. If the operation of the fan alone is unable to meet the entire cooling load, then the compressor is enabled and additional calculations are performed to determine the compressor's part-load ratio.
+
+The model then calculates the heat pump's sensible cooling energy rate delivered to the zones being served when the system runs at full-load conditions and when the DX cooling coil is OFF. If the supply air fan cycles with the compressor, then the sensible cooling energy rate is zero when the cooling coil is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible cooling energy rate will not be zero when the cooling coil is OFF. Calculating the sensible cooling energy rate involves modeling the supply air fan (and associated fan heat) and the DX cooling coil. The DX heating coil and the supplemental heating coil are also modeled, but only to pass the air properties and mass flow rate from their inlet nodes to their outlet nodes. For each of these cases (full load and DX cooling coil OFF), the sensible cooling energy rate delivered by the heat pump is calculated as follows:
+
+\begin{equation}
+Full\;Cool\;Output = (Mass\;Flow\;Rat{e_{ful\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}
+\end{equation}
+
+\begin{equation}
+No\;Cool\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}
+\end{equation}
+
+where:
+
+\emph{Mass Flow Rate\(_{full \, load}\)} = air mass flow rate through heat pump at full-load conditions, kg/s
+
+\emph{h\(_{out,\, full\, load}\)} = enthalpy of air exiting the heat pump at full-load conditions, J/kg
+
+\emph{h\(_{control \, zone}\)} = enthalpy of air leaving the control zone (where thermostat is located), J/kg
+
+\emph{HR\(_{min}\) =} enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the heat pump exiting air or the air leaving the control zone
+
+\emph{Mass Flow Rate\(_{coil\, off}\)} = air mass flow rate through the heat pump with the cooling coil OFF, kg/s
+
+\(h_{out,coil \, off}\) = enthalpy of air exiting the heat pump with the cooling coil OFF, J/kg
+
+\(\Delta_{sen,full\, load}\) = Sensible load difference between the system output node and the zone inlet node at full-load conditions
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,full load} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,full load} - h_{ZoneInlet}}_{HRmin} \\
+                           &+ \PB{\dot{m}_{full load} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,full load} - h_{ControlZone}}_{HRmin}
+  \end{array}
+\end{equation}
+
+where:
+
+Frac = Control zone air fraction with respect to the system mass flow rate
+
+\(\Delta_{sen,coil\, off}\) = Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,coil off} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,coil off} - h_{ZoneInlet}}_{HRmin} \\
+                           &+ \PB{\dot{m}_{coil off} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,coil off} - h_{ControlZone}}_{HRmin}
+  \end{array}
+\end{equation}
+
+With the calculated sensible cooling energy rates and the total sensible cooling load to be met by the system, the part-load ratio for the heat pump is estimated.
+
+\begin{equation}
+PartLoadRatio\, = \,MAX\left( {0.0,\frac{{ABS\left( {Heat\,Pump\,Cooling\,Load - NoCoolOutput} \right)}}{{ABS\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)
+\end{equation}
+
+Since the part-load performance of the DX cooling coil is frequently non-linear, and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the heat pump's cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump's cooling output divided by the load to be met.
+
+\begin{equation}
+  Tolerance \equiv \frac{HeatPumpCoolingLoad - Q_{HeatPump}}{HeatPumpCoolingLoad} \leq 0.001
+\end{equation}
+
+where:
+
+\(QHeatPump\) = Heat pump delivered sensible capacity (W)
+
+If the heat pump has been specified with cycling fan/cycling coil (AUTO fan), then the heat pump's operating supply air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. In this case, the air conditions at nodes downstream of the cooling coil represent the full-load (steady-state) values when the coil is operating.
+
+If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the heat pump is calculated as the average of the user-specified air flow rate when the cooling coil is ON and the user-specified air flow rate when the cooling coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
+
+\begin{equation}
+\mathop m\limits^ \bullet  furnace = PartLoadRatio\left( {\mathop m\limits^ \bullet  CoolCoilON} \right) + \left( {1 - PartLoadRatio} \right)\left( {\mathop m\limits^ \bullet  CoilOFF} \right)
+\end{equation}
+
+where:
+
+\(\mathop m\limits^ \bullet CoolCoilON\) ~ = air mass flow rate through heat pump when the cooling coil is ON (kg/s)
+
+\(\mathop m\limits^ \bullet CoilOFF\) ~ = air mass flow rate through heat pump when no cooling or heating is needed (kg/s)
+
+In this case, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF).
+
+Heating Operation
+
+Calculations for heating operation are similar to those for cooling operation in most respects. However, due to the inclusion of a supplemental heating coil, additional calculations are necessary to properly meet the total heating load for the zones being served.
+
+If EnergyPlus determines that the heat pump must supply heating to the control zone to meet the zone air temperature setpoint, then the heat pump model computes the total sensible heating load to be delivered to the zones being served based on the control zone sensible heating load and the control zone airflow fraction.
+
+\begin{equation}
+Heat\,Pump\,Heating\,Load\, = \frac{{Control\,Zone\,Heating\,Load}}{{Control\,Zone\,Air\,Flow\,Fraction}}
+\end{equation}
+
+The model then calculates the heat pump's sensible heating energy rate delivered to the zones being served when the system runs at full-load conditions and when the DX heating coil is OFF (without supplemental heater operation in either case). If the supply air fan cycles with the compressor, then the sensible heating energy rate is zero when the compressor is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible heating energy rate will not be zero when the compressor is OFF. Calculating the sensible heating energy rate involves modeling the supply air fan (and associated fan heat), the DX cooling coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node), the DX heating coil, and the supplemental heating coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and DX heating coil OFF, without supplemental heater operation in either case), the sensible heating energy rate delivered by the heat pump is calculated as follows:
+
+\begin{equation}
+Full\;Heat\;Output = (Mass\;Flow\;Rat{e_{ful\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}
+\end{equation}
+
+\begin{equation}
+No\;Heat\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}
+\end{equation}
+
+where:
+
+\emph{Mass Flow Rate \(_{full\, load}\)} = air mass flow rate through heat pump at full-load conditions, kg/s
+
+\emph{h\(_{out,\, full\, load}\)} = enthalpy of air exiting the heat pump at full-load conditions, J/kg
+
+\emph{h\(_{control \, zone}\)} = enthalpy of air leaving the control zone (where thermostat is located), J/kg
+
+\emph{HR\(_{min}\)} = enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the heat pump exiting air or the air leaving the control zone
+
+\emph{Mass Flow Rate \(_{coil \, off}\)} = air mass flow rate through the heat pump with the heating coil OFF, kg/s
+
+\emph{h\(_{out,\, coil \, off}\)} = enthalpy of air exiting the heat pump with the heating coil OFF, J/kg
+
+Δ\(_{sen,}\) \emph{\(_{full\, load}\)} = Sensible load difference between the system output node and the zone inlet node at full-load conditions
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,full load} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,full load} - h_{ZoneInlet}}_{HRmin} \\
+                           &+ \PB{\dot{m}_{full load} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,full load} - h_{ControlZone}}_{HRmin}
+  \end{array}
+\end{equation}
+where:
+
+Frac = Control zone air fraction with respect to the system mass flow rate
+
+\(\Delta_{sen,coil\, off}\) = Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{sen,coil off} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{Out,coil off} - h_{ZoneInlet}}_{HRmin} \\
+                           &+ \PB{\dot{m}_{coil off} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out,coil off} - h_{ControlZone}}_{HRmin}
+  \end{array}
+\end{equation}
+
+With the calculated sensible heating energy rates and the total sensible heating load to be met by the system, the part-load ratio for the heat pump is estimated.
+
+\begin{equation}
+PartLoadRatio\, = \,MAX\left( {0.0,\frac{{ABS\left( {Heat\,Pump\,Heating\,Load - NoHeatOutput} \right)}}{{ABS\left( {FullHeatOutput - NoHeatOutput} \right)}}} \right)
+\end{equation}
+
+Since the part-load performance of the DX heating coil is frequently non-linear (Ref: Single-Speed Electric Heat Pump DX Air Heating Coil), and the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the heat pump's heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump's heating output divided by the load to be met.
+
+\begin{equation}
+  Tolerance \equiv \frac{HeatPumpHeatingLoad - Q_{HeatPump}}{HeatPumpHeatingLoad} \leq 0.001
+\end{equation}
+
+where:
+
+\(QHeatPump\) = Heat pump delivered sensible capacity (W)
+
+If the heat pump's DX heating coil output at full load is insufficient to meet the entire heating load, PartLoadRatio is set equal to 1.0 (compressor and fan are not cycling) and the remaining heating load is passed to the supplemental heating coil. If the heat pump model determines that the outdoor air temperature is below the minimum outdoor air temperature for compressor operation, the compressor is turned off and the entire heating load is passed to the supplemental gas or electric heating coil. The heat pump exiting air conditions and energy consumption are calculated and reported by the individual component models (fan, DX heating coil, and supplemental gas or electric heating coil).
+
+If the heat pump has been specified with cycling fan/cycling coil (AUTO fan), then the heat pump's operating supply air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the heating coils represent the full-load (steady-state) values when the coils are operating. If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the heat pump is calculated as the average of the user-specified air flow rate when the heat pump heating coil is ON and the user-specified air flow rate when the heat pump heating coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
+
+\begin{equation}
+\mathop m\limits^ \bullet  HeatPump = PartLoadRatio\left( {\mathop m\limits^ \bullet  HeatCoilON} \right) + \left( {1 - PartLoadRatio} \right)\left( {\mathop m\limits^ \bullet  CoilOFF} \right)
+\end{equation}
+
+where:
+
+\(\mathop m\limits^ \bullet HeatCoilON\) ~ = air mass flow rate through heat pump when the heating coil is ON (kg/s)
+
+\(\mathop m\limits^ \bullet CoilOFF\) ~ = air mass flow rate through heat pump when no heating or cooling is needed (kg/s)
+
+In this case, the air conditions at nodes downstream of the heating coils are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coils are operating and inlet air conditions when the coils are OFF).
+
+\subsubsection{High Humidity Control with AirToAir HeatPump Model}\label{high-humidity-control-with-airtoair-heatpump-model}
+
+The specific configuration of the AirToAir HeatPump with supplemental heating coil is shown above (see Figure~\ref{fig:schematic-of-a-blow-through-air-to-air-heat}). This figure shows the fan placement when a blow through fan is specified. If a draw through fan is specified, the fan is located between the heating coil and the supplemental heating coil. The system is controlled to keep the high relative humidity in the control zone from exceeding the setpoint specified in the object ZoneControl:Humidistat. This option is available when the supply air fan operates continuously (i.e., the supply air fan operating mode schedule values are never equal to 0) or the supply air fan cycles with the compressor. In addition, when high humidity control is specified and the compressor operates, the heatpump operates at the cooling air flow rate when a zone heating load is present as determined by the zone thermostat. High humidity control is specified as either None, MultiMode, or CoolReheat in the Dehumidification Control Type input field. MultiMode is specified when a heat exchanger is used to improve the dehumidification performance of the cooling coil. The heat exchanger will be activated when the sensible part-load ratio is insufficient to meet the zone latent load. CoolReheat is specified when a DX cooling coil is used to over-cool the supply air stream in order to meet the zone latent load. In this case, a supplemental heating coil will ensure the zone temperature does not fall below the zone heating temperature set point. When a heat exchanger is used in conjunction with a DX cooling coil and CoolReheat is specified as the Dehumidification Control Type, the heat exchanger is ``locked on'' to meet either the sensible or latent cooling load. If the dehumidification control type is selected as None and a heat exchanger assisted cooling coil is used, the heat exchanger is ``locked on'' and the air conditioner runs only to meet the sensible cooling load. A supplemental heating coil is required for all dehumidification control types.
+
+The model first calculates the \emph{PartLoadRatio} required meeting the sensible cooling load.~ The heatpump's sensible cooling load is determined from the control zone sensible cooling load to the cooling setpoint and the control zone air flow fraction to maintain the dry-bulb temperature setpoint in the control zone.:
+
+\begin{equation}
+HeatPumpCoolingLoad = \,\frac{{ControlZoneCoolingLoad}}{{ControlZoneAirFlowFraction}}
+\end{equation}
+
+The heatpump's sensible cooling load to be met and the full load cooling output are used to calculate the sensible the part-load ratio iteratively based on user specified convergence criterion.
+
+\begin{equation}
+PartLoadRatio = MAX\left( {0.0,\,\frac{{ABS\left( {HeatPumpCoolingLoad - NoCoolOutput} \right)}}{{ABS\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)
+\end{equation}
+
+When the heat pump's sensible cooling capacity meets the system sensible cooling load at a given sensible part load ratio, then the Heat pump meets the controlled zone cooling setpoint temperature. If a moisture (latent) load exists because the control zone humidity has exceeded the setpoint, the total moisture load to be met by the heat pumps (HeatPumpMoistureLoad) is calculated based on the control zone moisture load and the control zone air flow fraction.
+
+\begin{equation}
+HeatPumpMoistureLoad = \,\frac{{ControlZoneMoitureLoad}}{{ControlZoneAirFlowFraction}}
+\end{equation}
+
+Then the \emph{LatentPartLoadRatio} required to meet the high humidity setpoint is calculated as follows:
+
+\begin{equation}
+LatentPartLoadRatio = MIN\left( {PL{R_{Min}},\,\frac{{ABS\left( {HeatPumpMoistureLoad - NoLatentOutput} \right)}}{{ABS\left( {FullLatentOutput - NoLatentOutput} \right)}}} \right)
+\end{equation}
+
+The model uses the greater of the two part-load ratios, \emph{PartLoadRatio} or \emph{LatentPartLoadRatio}, to determine the operating part-load ratio of the Heat Pump's DX cooling coil.
+
+\begin{equation}
+LatentPartLoadRatio = MAX\left( {PartLoadRatio,\,LatentPartLoadRatio} \right)
+\end{equation}
+
+As previously described, iterations are performed to converge on the solution within the convergence tolerance.
+
+Where,
+
+\(ControlZoneCoolingLoad\) = the control zone sensible cooling load to the cooling setpoint, (W).
+
+\(ControlZoneMoistureLoad\) ~~~~~~~~ = the control zone moisture load to the dehumidifying relative humidity setpoint, (W).
+
+\(ControlZoneAirFlowFraction\) ~~~~ = the supply air fraction that goes though the control zone, (-).
+
+\emph{FullLatentOutput} ~~~~ = ~~~~~~~~~the Heat Pump's latent cooling energy rate at full-load conditions, W
+
+\emph{NoLatentOutput} ~~~~~ = ~~~~~~~~~ the Heat Pump's latent cooling energy rate with cooling coil OFF, W
+
+\(PartLoadRatio\) ~~~~ = ~~~~~~~~~ the heat pump's part-load-ratio required to meet system sensible load, (-).
+
+\(LatentPartLoadRatio\) ~~~~~ = ~~~~~~~~~ the heat pump's part-load-ratio required to meet system moisture load, (-).
+
+\(PL{R_{MIN}}\) \emph{~~~~~~ = ~~}the minimum part-load ratio, which is usually 0.0. For the case when the latent capacity degradation model is used (Ref: DX Cooling Coil Model), this value is the minimum part-load ratio at which the cooling coil will dehumidify the air.
+
+When the predicted zone air temperature is above the heating setpoint and if there is a dehumidification load, the supplemental heating coil load is required to offset the excess cooling as shown in Figure~\ref{fig:supplemental-heating-coil-load-when-predicted-002}. If the model determines that the LatentPartLoadRatio is to be used as the operating part-load ratio of the heatpump's cooling coil, the supplemental heating coil is used to offset the excess sensible capacity provided by the heat pump DX cooling coil. The model first checks the sensible load that exists for the current simulation time step (predicted zone temperature with no HVAC operation compared to the thermostat setpoint temperatures). If a sensible cooling load or no sensible cooling or heating load exists (see Figure~\ref{fig:flows-of-warmup-convergence-checks}),~ the model calculates the difference between the sensible heating load required to reach or maintain the heating dry-bulb temperature setpoint and the actual sensible cooling energy rate delivered by the unit (with LatentPartLoadRatio). In this case, thesupplemental heating coil is used to offset the excess sensible cooling energy provided by the DX cooling coil (if any) that could have caused an overshoot of the heating dry-bulb temperature setpoint. Note that when a humidistat is used and high humidity control is required, the zone dry-bulb temperature will typically move toward the heating temperature setpoint when a high moisture (latent) load exists.
+
+\begin{figure}[hbtp] % fig 228
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5145.png}
+\caption{Supplemental heating coil load when predicted zone air temperature is above the heating Setpoint \protect \label{fig:supplemental-heating-coil-load-when-predicted-002}}
+\end{figure}
+
+If a heating load exists (Figure~\ref{fig:supplemental-heating-coil-load-when-predicted-003}), the supplementalheating coil is used to meet the heating coil load and at the same time offset the entire sensible cooling energy rate of the DX cooling coil (to meet the humidistat setpoint). Note that when a heating load exists and high humidity control is required, the heat pump operates at the user-specified cooling air flow rate for the entire simulation time step. As with the fan, and DX cooling coil, report variables associated with supplemental heating coil performance (e.g., heating coil energy, heating coil rate, heating coil gas or electric energy, heating coil runtime fraction, etc.) are managed in the supplemental (heating) coil object.
+
+\begin{figure}[hbtp] % fig 229
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5146.png}
+\caption{Supplemental heating coil load when predicted zone air temperature is below the heating setpoint \protect \label{fig:supplemental-heating-coil-load-when-predicted-003}}
+\end{figure}
+
+\subsection{Unitary Multi-Speed Air-To-Air Heat Pump}\label{unitary-multi-speed-air-to-air-heat-pump}
+
+\subsubsection{Overview}\label{overview-4}
+
+The input object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed provides a model for a multispeed air-to-air heat pump that is a ``virtual'' component that consists of an on/off or constant volume fan component, a multispeed DX cooling coil, a multispeed DX heating coil, and a gas or electric supplemental heating coil. The main difference between this heat pump object and other EnergyPlus heat pump objects is that this object allows from two to four discrete compressor speeds for heating and cooling operation (instead of a single speed for each mode). The specific configuration of the blow through heat pump is shown in the following figure. For a draw through heat pump, the fan is located between the DX heating coil and the supplemental heating coil.
+
+\begin{figure}[hbtp] % fig 230
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5147.png}
+\caption{Schematic of a Multispeed Air-to-Air Heat Pump (Blow-through Configuration) \protect \label{fig:schematic-of-a-multispeed-air-to-air-heat}}
+\end{figure}
+
+While the heat pump may be configured to serve multiple zones, system operation is controlled by a thermostat located in a single ``control'' zone. One of the key parameters for the heat pump component is the fraction of the total system airflow that goes through the control zone. This fraction is calculated as the ratio of the maximum air mass flow rate for the air loop's supply inlet node for the control zone (e.g., AirTerminal:SingleDuct:Uncontrolled, field = Maximum Air Flow Rate, converted to mass flow) to the sum of the maximum air mass flow rates for the air loop's supply inlet nodes for all zones served by this air loop. The heat pump module scales the calculated load for the control zone upward based on this fraction to determine the total load to be met by the heat pump. The module then proceeds to calculate the required cycling ratio, speed ratio and speed number for the system coil and determines the supply air mass flow rate to meet this total load based on the speed number. The cycling ratio is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the multispeed heat pump's DX heating or cooling coil at Speed 1 for the entire system time step. It is equivalent to the part load ratio for a single speed DX coil. The value is between 0.0 and 1.0 when the system operates at its lowest speed (Speed 1) and 1.0 when the multispeed heat pump operates at speeds above 1. The speed ratio is the ratio of time in a system time step that the compressor is at rated speed between two consecutive speed numbers ({[}Compressor Speed - Compressor speed at Speed i-1{]} / {[}Compressor speed at Speed i - Compressor speed at Speed i-1{]}). The compressor speed ratio is between 0.0 and 1.0 when the speed number is above 1 and is 0.0 during Speed 1 operation. The speed number is the lowest index number whose corresponding full-load sensible capacity at the given air mass flow rate is greater than or equal to the sensible load (heating or cooling) in a system time step. The heating or cooling capacity delivered by the heat pump is distributed to all of the zones served by this system via the direct air units that supply air to each zone.
+
+The heat pump component is able to model supply air fan operation in two modes: cycling fan -- cycling coil (i.e., AUTO fan) and continuous fan -- cycling coil (i.e., fan ON). Fan:OnOff must be used to model AUTO fan, while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON. The fan operation mode is specified using a supply air fan operating mode schedule where schedule values of 0 denote cycling fan operation and schedule values other than 0 (a 1 is usually used) denote continuous fan operation. Using this schedule, the supply air fan may be cycled with cooling or heating coil operation or operated continuously based on time of day (e.g.~cycling fan operation at night and continuous fan operation during the day).
+
+Several output variables are reported by the heat pump object including fan part-load ratio, compressor part-load ratio, cycling ratio, speed ratio and speed number. Fan part-load ratio is defined as the actual air mass flow rate through the system for the time step divided by the operating supply air mass flow rate specified for the heat pump (\({{{{\dot m}_{actual}}} \mathord{\left/ {\vphantom {{{{\dot m}_{actual}}} {{{\dot m}_{design}}}}} \right. } {{{\dot m}_{ON}}}}\) ) at speed 1. Fan part-load ratio is set to 1.0 when the heat pump operates at speeds above 1. The operating supply air mass flow rate may be different for cooling, heating, and when no cooling or heating is required. Compressor part-load ratio is the actual load for the time step divided by the full-load sensible capacity (see Eqn. or Eqn.). If the defrost strategy is reverse cycle for a DX heating coil, the compressor part-load ratio is the sum of the actual load and the defrost load divided by the full-load sensible capacity. Therefore, the compressor part load ratio for the DX heating coil may be greater than the cycling ratio. This heat pump object also reports the sensible, latent and total cooling and heating rate, as well as the electricity consumption for the unit with separate accounting of auxiliary electric consumption. Furthermore, five report variables related to waste heat recovery are available if the user chooses to model this option.
+
+\subsubsection{Model Description}\label{model-description-4}
+
+As described previously, the heat pump is a ``virtual'' component consisting of a fan, multispeed DX cooling coil, multispeed DX heating coil and supplemental heating coil. The sole purpose of the heat pump model is to properly coordinate the operation of the various system components. The following sections describe the flow of information within the model, as well as the differences between cycling and continuous supply air fan operation.
+
+\subsubsection{Cooling Operation}\label{cooling-operation-2}
+
+The description of heat pump cooling operation is divided in two sections: sensible capacity and average supply air flow rate. Actually, the determinations of capacity and supply air flow rate are related, so these calculations are performed in unison.
+
+\paragraph{Capacity calculation}\label{capacity-calculation}
+
+If EnergyPlus determines that the heat pump must supply cooling to the control zone to meet the zone air temperature setpoint, then the heat pump model computes the total sensible cooling load (negative) to be delivered to the zones being served based on the control zone sensible cooling load and the fraction of the heat pump air flow that goes through the control zone.
+
+\begin{equation}
+Heat\;Pump\;Cooling\;Load = \frac{{Control\;Zone\;Cooling\;Load}}{{Control\;Zone\;Air\;Flow\;Fraction}}
+\end{equation}
+
+The model then calculates the heat pump's sensible cooling energy rate delivered to the zones being served when the system runs at full-load conditions at the highest speed and when the DX cooling coil is OFF. If the supply air fan cycles with the compressor, then the sensible cooling energy rate is zero when the cooling coil is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible cooling energy rate will not be zero when the cooling coil is OFF. Calculating the sensible cooling energy rate involves modeling the supply air fan (and associated fan heat) and the multispeed DX cooling coil. The multispeed DX heating coil and the supplemental heating coil are also modeled, but only to pass the air properties and mass flow rate from their inlet nodes to their outlet nodes. For each of these cases (full load at highest cooling speed and DX cooling coil OFF), the sensible cooling energy rate delivered by the heat pump is calculated as follows:
+
+\begin{equation}
+FullCoolOutpu{t_{Highest\;Speed}} = \left( {{{\dot m}_{HighestSpeed}}} \right){\left( {{h_{out,full\;load}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,HighestSpeed}}
+\end{equation}
+
+\begin{equation}
+NoCoolOutput = \left( {{{\dot m}_{CoilOff}}} \right){\left( {{h_{out,coil\;off}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,coil\;off}}
+\end{equation}
+
+where:
+
+\emph{\({\dot m}_{HighestSpeed}\)} = air mass flow rate through heat pump at the highest cooling speed {[}kg/s{]}
+
+\emph{h\(_{out,\, full\, load}\)} = enthalpy of air exiting the heat pump at full-load conditions {[}J/kg{]}
+
+\emph{h\(_{control \, zone}\)} = enthalpy of air leaving the control zone (where thermostat is located) {[}J/kg{]}
+
+\emph{HR\(_{min}\) =} the minimum humidity ratio of the heat pump exiting air or the air leaving the control zone {[}kg/kg{]}
+
+\({\dot m}_{CoilOff}\) = air mass flow rate through the heat pump with the cooling coil OFF {[}kg/s{]}
+
+\emph{h\(_{out,coil \, off}\)} = enthalpy of air exiting the heat pump with the cooling coil OFF {[}J/kg{]}
+
+Δ\(_{sen,}\) \emph{\(_{full\, load}\)} = Sensible load difference between the system output node and the zone inlet node at full-load conditions
+
+\begin{equation}
+\begin{split}
+{\Delta_{sen,HighestSpeed}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} \\
++ \left( {{{\dot m}_{HighestSpeed}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {h_{Out,full\;load} - {h_{Control\;Zone}}} \right)_{HR\min }}
+\end{split}
+\end{equation}
+
+where:
+
+Frac = Control zone air fraction with respect to the system mass flow rate
+
+Δ\(_{sen,coil\, off}\) = Sensible load difference between the system output node and the zone inlet node with the cooling coil OFF conditions
+
+\begin{equation}
+\begin{split}
+{\Delta_{sen,coil\;off}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} \\ 
++ \left( {{{\dot m}_{coil\;off}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {{h_{Out,coil\;off}} - {h_{Control\;Zone}}} \right)_{HR\min }}
+\end{split}
+\end{equation}
+
+If the heat pump's sensible cooling rate at the highest speed (full load, no cycling) is insufficient to meet the entire cooling load, the controlled zone conditions will not be met. The reported cycling rate and speed ratio are 1, and the speed number is set to the highest index number. If the total sensible cooling load to be met by the system is less than the sensible cooling rate at the highest speed, then the following steps are performed.
+
+·~~~~~~~~Calculate the sensible cooling energy rate at Speed 1
+
+\begin{equation}
+FullCoolOutpu{t_{Speed1}} = \left( {{{\dot m}_{Speed1}}} \right){\left( {{h_{out,fullload}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,Speed1}}
+\end{equation}
+
+where
+
+\emph{\({{{\dot m}_{Speed1}}}\)} = air mass flow rate through heat pump at Speed 1 {[}kg/s{]}
+
+\(\Delta_{sen,\, Speed1}\) = Sensible load difference between the system output node and the zone inlet node at full-load conditions at Speed 1
+
+\begin{equation}
+\begin{split}
+{\Delta_{sen,Speed1}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} \\
++ \left( {{{\dot m}_{Speed1}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {{h_{Out,full\;load}} - {h_{Control\;Zone}}} \right)_{HR\min }}
+\end{split}
+\end{equation}
+
+·~~~~~~~~If the sensible cooling energy rate delivered by the heat pump at Speed 1 is greater or equal to the sensible load, the cycling ratio (part-load ratio) for the heat pump is estimated.
+
+\begin{equation}
+  \begin{array}{rl}
+    CyclingRatio &= \frac{\left|\PB{HeatingCoilSensibleLoad}\right|}{FullHeatingCoilCapacity} \\
+                 &= \max \PB{0.0, \frac{\left|\PB{HeatPumpHeatingLoad-AddedFanHeat}\right|}{\left|\PB{FullHeatOutput_{Speed1}-AddedFanHeat_{Speed1}}\right|} }
+  \end{array}
+\end{equation}
+
+where
+
+AddedFanHeat~ = generated supply air fan heat, which is a function of part load ratio and as internal component cooling load {[}W{]}.
+
+AddedFanHeat\(_{Speed1}\) = generated supply air fan heat at Speed 1 (part load ratio = 1) {[}W{]}.
+
+Since the part-load performance of the DX cooling coil is frequently non-linear,and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the heat pump's cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump's cooling output divided by the load to be met.
+
+\begin{equation}
+  Tolerance \equiv \frac{HeatPumpCoolingLoad - HeatPumpOutput_{Cycling}}{HeatPumpCoolingLoad} \leq 0.001
+\end{equation}
+
+where:
+
+HeatPumpOutput\(_{Cycling}\) = heat pump delivered sensible capacity for Speed 1 operating at a specific cycling ratio (W)
+
+\begin{equation}
+HeatPumpOutpu{t_{cycling}} = {\dot m_{_{HeatPump}}}{\left( {{h_{out}} - {h_{Control\;Zone}}} \right)_{HR\min }} - {\Delta_{cycling}}
+\end{equation}
+
+where
+
+\({\dot m_{HeatPump}}\) = average air mass flow rate defined in the next section {[}kg/s{]}
+
+h\(_{out,}\) = enthalpy of air exiting the heat pump at part load conditions {[}J/kg{]}
+
+Δ\(_{cycling}\) = average sensible load difference between the system output node and the zone inlet node
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{cycling} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{ZoneInlet}-h_{ControlZone}} \\
+                           &+ \PB{\dot{m}_{HeatPump} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out} - h_{ControlZone}}
+  \end{array}
+\end{equation}
+
+\({{{\dot m}_{ZoneInlet}}}\) = Air mass flow rate in the supply inlet node in the controlled zone {[}kg/s{]}
+
+For this case where speed 1 operation was able to meet the required cooling load, the speed ratio is set to zero and speed number is equal to 1.
+
+·~~~~~~~~If the heat pump's cooling output at full load for Speed 1 is insufficient to meet the entire cooling load, the Cycling ratio is set equal to 1.0 (compressor and fan are not cycling). Then the cooling speed is increased and the delivered sensible capacity is calculated. If the full load sensible capacity at Speed n is greater than or equal to the sensible load, the speed ratio for the heat pump is estimated:
+
+\begin{equation}
+Speed{\kern 1pt} Ratio = \frac{{ABS(Heat{\kern 1pt} Pump{\kern 1pt} Cooling{\kern 1pt} Load - AddeFanHeat - Full{\kern 1pt} Cool{\kern 1pt} Outpu{t_{Speed{\kern 1pt} n - 1}})}}{{ABS(Full{\kern 1pt} CoolOutpu{t_{Speed{\kern 1pt} n}} - Full{\kern 1pt} CoolOutpu{t_{Speed{\kern 1pt} n - 1}})}} 
+\end{equation}
+
+Although a linear relationship is assumed by applying the speed ratio to obtain the effective capacity and mass flow rate between speed n and n-1, the outlet air node conditions are dependent on the combined outputs and may not be linear. In addition, the supply air fan heat varies with the speed ratio due to different supply mass flow rates between speed n and n-1 . Therefore, the final speed ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the heat pump's cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump's cooling output divided by the load to be met.
+
+\begin{equation}
+Tolerance = 0.001 \ge \frac{{Heat\,Pump\,Cooling\,Load - HeatPumpOutpu{t_{SpeedRatio}}}}{{Heat\,Pump\,Cooling\,Load}}
+\end{equation}
+
+where:
+
+HeatPumpOutput\(_{Speed,n}\) = heat pump delivered sensible capacity between two consecutive speeds at a specific speed ratio (W)
+
+~~~~~~ \(\begin{array}{l}HeatPumpOutpu{t_{SpeedRatio}} = (SpeedRatio)FullCoolOutpu{t_{Speed\;n}}\\\;\;\;\;\;\;\; = (1 - SpeedRatio)FullCoolOutpu{t_{Speed\;n - 1}} - AddedFanHea{t_{SpeedRatio}}\end{array}\)
+
+Where
+
+AddedFanHeat\(_{SpeedRatio}\)~~~~~~~~~ = generated supply air fan heat at a specific speed ratio {[}W{]}
+
+In this case, the reported cycling ratio is 1 and speed number is equal to n.
+
+\paragraph{Air Mass Flow Rate Calculation}\label{air-mass-flow-rate-calculation-2}
+
+Speed 1 operation
+
+If the heat pump has been specified with cycling fan/cycling coil (AUTO fan), then the heat pump's operating supply air mass flow rate is determined by the cycling ratio (PartLoadRatio) for Speed 1. The supply air mass flow rate is multiplied by the cycling ratio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the cooling coils represent the full-load (steady-state) values when the coil is operating.
+
+\begin{equation}
+{\dot m_{HeatPump}} = (CyclingRatio){\dot m_{Speed1}}
+\end{equation}
+
+If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the heat pump is calculated as the average of the user-specified air flow rate when the heat pump cooling coil is ON at Speed 1 and the user-specified air flow rate when the heat pump cooling coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
+
+\begin{equation}
+{\dot m_{HeatPump}} = (CyclingRatio){\dot m_{Speed1}} + (1.0 - CyclingRatio){\dot m_{CoilOff}}
+\end{equation}
+
+where:
+
+\({\dot m_{HeatPump}}\) ~ = average air mass flow rate through heat pump {[}kg/s{]}
+
+\({{{\dot m}_{Speed1}}}\) = air mass flow rate through heat pump when cooling coil is ON at Speed 1 {[}kg/s{]}
+
+\({{{\dot m}_{CoilOff}}}\) ~ = air mass flow rate through heat pump when no heating or cooling is needed {[}kg/s{]}
+
+In this case, the air conditions at nodes downstream of the cooling coils are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF).
+
+\paragraph{Higher Speed Operation}\label{higher-speed-operation-1}
+
+When the heat pump operates at higher speeds to meet the required cooling load, the supply air mass flow rate is linearly interpolated between two consecutive speeds:
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{HeatPump}} = (SpeedRatio)\mathop m\limits^ \bullet  {{\kern 1pt}_{Speed{\kern 1pt} n}} + (1.0 - SpeedRatio)\mathop m\limits^ \bullet  {{\kern 1pt}_{Speed{\kern 1pt} n - 1}}
+\end{equation}
+
+where:
+
+\({\dot m_{HeatPump}}\) = average air mass flow rate through the heat pump for the time step {[}kg/s{]}
+
+\({\dot m_{Speed\;n}}\) = air mass flow rate through heat pump when cooling coil is ON at Speed n {[}kg/s{]}
+
+\({\dot m_{Speed\;n - 1}}\) = air mass flow rate through heat pump when cooling coil is ON at Speed n-1 {[}kg/s{]}
+
+For this case of higher speed operation, the air conditions at nodes downstream of the cooling coils are determined by the delivered cooling capacity and supply air mass flow rates between two consecutive speeds.
+
+Although the above sections present the capacity and air mass flow rate calculation separately, they are dependent and change every iteration until convergence is reached for the time step being simulated.
+
+\subsubsection{Heating Operation}\label{heating-operation-1}
+
+The description of heat pump heating operation is divided in two sections: total (sensible) capacity and average supply air flow rate. Actually, the determinations of capacity and supply air flow rate are related, so these calculation are performed in unison.
+
+\paragraph{Capacity calculation}\label{capacity-calculation-1}
+
+If EnergyPlus determines that the heat pump must supply heating to the control zone to meet the zone air temperature setpoint, then the heat pump model computes the total sensible heating load (positive) to be delivered to the zones being served based on the control zone sensible heating load and the fraction of the heat pump air flow that goes through the control zone.
+
+\begin{equation}
+Heat\;Pump\;Heating\,Load = \frac{{Control\;Zone\;Heating\,Load}}{{Control\;Zone\;Air\;Flow\;Fraction}}
+\end{equation}
+
+The model then calculates the heat pump's sensible heating energy rate delivered to the zones being served when the system runs at full-load conditions at the highest speed and when the DX heating coil is OFF (without supplemental heater operation in either case). If the supply air fan cycles with the compressor, then the sensible heating energy rate is zero when the compressor is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible heating energy rate will not be zero when the compressor is OFF. Calculating the sensible heating energy rate involves modeling the supply air fan (and associated fan heat), the DX cooling coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node), the DX heating coil, and the supplemental heating coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and DX heating coil OFF, without supplemental heater operation in either case), the sensible heating energy rate delivered by the heat pump is calculated as follows:
+
+\begin{equation}
+FullHeatOutpu{t_{Highest\;Speed}} = \left( {{{\dot m}_{HighestSpeed}}} \right){\left( {{h_{out,full\;load}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,HighestSpeed}}
+\end{equation}
+
+\begin{equation}
+NoHeatOutput = \left( {{{\dot m}_{CoilOff}}} \right){\left( {{h_{out,coil\;off}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,coil\;off}}
+\end{equation}
+
+where:
+
+\emph{\({\dot m}_{HighestSpeed}\)}~ = air mass flow rate through heat pump at the highest heating speed {[}kg/s{]}
+
+\emph{h\(_{out,\, full\, load}\)} = enthalpy of air exiting the heat pump at full-load conditions {[}J/kg{]}
+
+\emph{h\(_{control \, zone}\)} = enthalpy of air leaving the control zone (where thermostat is located) {[}J/kg{]}
+
+\emph{HR\(_{min}\) =} enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the heat pump exiting air or the air leaving the control zone
+
+\({\dot m}_{CoilOff}\) = air mass flow rate through the heat pump with the heating coil OFF {[}kg/s{]}
+
+\emph{h\(_{out,coil \, off}\)} = enthalpy of air exiting the heat pump with the heating coil OFF {[}J/kg{]}
+
+\(\Delta_{sen,full\, load}\) = Sensible load difference between the system output node and the zone inlet node at full-load conditions
+
+\begin{equation}
+\begin{split}
+{\Delta_{sen,HighestSpeed}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} \\
++ \left( {{{\dot m}_{HighestSpeed}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {h_{Out,full\;load} - {h_{Control\;Zone}}} \right)_{HR\min }}
+\end{split}
+\end{equation}
+
+where:
+
+Frac = Control zone air fraction with respect to the system mass flow rate
+
+\(\Delta_{sen,coil\, off}\) = Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
+
+\begin{equation}
+\begin{split}
+{\Delta_{sen,coil\;off}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} \\
++ \left( {{{\dot m}_{coil\;off}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {{h_{Out,coil\;off}} - {h_{Control\;Zone}}} \right)_{HR\min }}
+\end{split}
+\end{equation}
+
+If the heat pump's DX heating coil output full load at the highest speed is insufficient to meet the entire heating load, the remaining heating load is passed to the supplemental heating coil. If the heat pump model determines that the outdoor air temperature is below the minimum outdoor air temperature for compressor operation (specified by the user), the compressor is turned off and the entire heating load is passed to the supplemental gas or electric heating coil. The heat pump exiting air conditions and energy consumption are calculated and reported by the individual component models (fan, DX heating coil, and supplemental gas or electric heating coil).
+
+If the total heating load to be met by the system is less than the sensible heating rate at the highest speed, then the following steps are performed.
+
+1.~~~~Calculate the sensible heating energy rate at Speed 1
+
+\begin{equation}
+FullHeatOutpu{t_{Speed1}} = \left( {{{\dot m}_{Speed1}}} \right){\left( {{h_{out,fullload}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,Speed1}}
+\end{equation}
+
+where:
+
+\emph{\({{{\dot m}_{Speed1}}}\)}~ = air mass flow rate through heat pump at Speed 1 {[}kg/s{]}
+
+\(\Delta_{sen,Speed1}\) = Sensible load difference between the system output node and the zone inlet node at full-load conditions at Speed 1
+
+\begin{equation}
+\begin{split}
+{\Delta_{sen,Speed1}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} \\
++ \left( {{{\dot m}_{Speed1}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {{h_{Out,full\;load}} - {h_{Control\;Zone}}} \right)_{HR\min }}
+\end{split}
+\end{equation}
+
+2.~~~~If the sensible heating energy rate delivered by the heat pump at Speed 1 is greater or equal to the sensible load, the cycling ratio (part-load ratio) for the heat pump is estimated.
+
+\begin{equation}
+  \begin{array}{rl}
+    CyclingRatio &= \frac{\left|\PB{HeatingCoilSensibleLoad}\right|}{FullHeatingCoilCapacity} \\
+                 &= \max \PB{0.0, \frac{\left|\PB{HeatPumpHeatingLoad-AddedFanHeat}\right|}{\left|\PB{FullHeatOutput_{Speed1}-AddedFanHeat_{Speed1}}\right|} }
+  \end{array}
+\end{equation}
+
+where
+
+AddedFanHeat~~~~~~~ = generated supply air fan heat, which is a function of part load ratio and as internal component heating load {[}W{]}.
+
+AddedFanHeat\(_{Speed1}\) = generated supply air fan heat at Speed 1 (part load ratio = 1) {[}W{]}.
+
+Since the part-load performance of the DX heating coil is frequently non-linear (Ref: Single-Speed Electric Heat Pump DX Air Heating Coil), and the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the heat pump's heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump's heating output divided by the load to be met.
+
+\begin{equation}
+  Tolerance \equiv \frac{HeatPumpHeatingLoad - HeatPumpOutput_{Cycling}}{HeatPumpHeatingLoad} \leq 0.001
+\end{equation}
+
+where:
+
+HeatPumpOutput\(_{Cycling}\) = heat pump delivered sensible capacity for Speed 1 operating at a specific cycling ratio (W)
+
+\begin{equation}
+HeatPumpOutpu{t_{cycling}} = {\dot m_{_{HeatPump}}}{\left( {{h_{out}} - {h_{Control\;Zone}}} \right)_{HR\min }} - {\Delta_{cycling}}
+\end{equation}
+
+where
+
+\({\dot m_{HeatPump}}\) ~~~ = average air mass flow rate defined in the next section {[}kg/s{]}
+
+h\(_{out,}\) = enthalpy of air exiting the heat pump at part load conditions {[}J/kg{]}
+
+\(\Delta_{cycling}\) = average sensible load difference between the system output node and the zone inlet node
+
+\begin{equation}
+  \begin{array}{rl}
+    \Delta_{cycling} &= \frac{\dot{m}_{ZoneInlet}}{Frac} \PB{h_{ZoneInlet} - h_{ControlZone}} \\
+                           &+ \PB{\dot{m}_{HeatPump} - \frac{\dot{m}_{ZoneInlet}}{Frac}} \PB{h_{Out} - h_{ControlZone}}
+  \end{array}
+\end{equation}
+
+\({{{\dot m}_{ZoneInlet}}}\) ~~~~~~ = Air mass flow rate in the supply inlet node in the controlled zone {[}kg/s{]}
+
+For this case where speed 1 operation was able to meet the required heating load, the speed ratio is set to zero and speed number is equal to 1.
+
+3.~~~~If the heat pump's heating output at full load for Speed 1 is insufficient to meet the entire heatling load, the Cycling ratio (PartLoadRatio) is set equal to 1.0 (compressor and fan are not cycling). Then the heating speed is increased and the delivered sensible capacity is calculated. If the full load sensible capacity at Speed n is greater than or equal to the sensible load, the speed ratio for the heat pump is estimated:
+
+\begin{equation}
+Speed{\kern 1pt} Ratio = \frac{{ABS(Heat{\kern 1pt} Pump{\kern 1pt} Heating{\kern 1pt} Load - AddeFanHeat - Full{\kern 1pt} Heat{\kern 1pt} Outpu{t_{Speed{\kern 1pt} \;n - 1}})}}{{ABS(Full{\kern 1pt} HeatOutpu{t_{Speed\;n}} - Full{\kern 1pt} HeatOutpu{t_{Speed\;n - 1}})}}
+\end{equation}
+
+Although a linear relationship is assumed by applying the speed ratio to obtain the effective capacity and air mass flow rate between speed n and n-1, the outlet node conditions are dependent on the combined outputs and may not be linear. In addition, the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan). Therefore, the final speed ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the heat pump's heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump's heating output divided by the load to be met.
+
+\begin{equation}
+Tolerance = 0.001 \ge \frac{{Heat\,Pump\,Heating\,Load - HeatPumpOutpu{t_{SpeedRatio}}}}{{Heat\,Pump\,Heating\,Load}}
+\end{equation}
+
+where:
+
+HeatPumpOutput\(_{SpeedRatio}\) = heat pump delivered sensible capacity between two consecutive speeds at a specific ratio {[}W{]}
+
+~~~~~~ \(\begin{array}{l}HeatPumpOutpu{t_{SpeedRatio}} = (SpeedRatio)FullHeatOutpu{t_{Speed\;n}}\\\;\;\;\;\;\;\; = (1 - SpeedRatio)FullHeatOutpu{t_{Speed\;n - 1}} - AddedFanHea{t_{SpeedRatio}}\end{array}\)
+
+Where
+
+AddedFanHeat\(_{SpeedRatio}\) = generated supply air fan heat at a specific speed ratio {[}W{]}
+
+In this case, the reported cycling ratio is 1 and speed number is equal to n.
+
+\paragraph{Air Mass Flow Rate Calculation}\label{air-mass-flow-rate-calculation-3}
+
+The air mass flow rate calculations during heating operation are the same as those described above for cooling operation.
+
+\subsubsection{Fan Placement}\label{fan-placement}
+
+Supply air fan placement impacts the iteration strategy. When the fan placement type is blow through, the air mass flow rate and coil part load factor (PLF) affect the fan outlet conditions. Since the fan is upstream of the coil components with this fan placement, the fan outlet conditions are calculated without knowing the next component's performance at the beginning of each iteration. DX coil performance is strongly dependent on the inlet conditions, so without correct inlet conditions the DX coil components may not be simulated correctly. Therefore, the heat pump components are called twice for each iteration when fan placement is `blow through'. The correct part load factor for the fan component is obtained after the first call, so that the more realistic fan outlet conditions are used to simulate the coil performance in the second call. This extra call to the heat pump components is not required for the draw through fan since the supply air fan is located downstream of the DX coils with this fan placement.
+
+\subsubsection{Waste Heat Calculation}\label{waste-heat-calculation-1}
+
+When the heat recovery is active (the value of the Design Heat Recovery Water Flow Rate field is greater than 0), the outlet node temperature of heat recovery is calculated based on the recoverable waste heat generated by its child objects (Coil:Cooling:DX:MultiSpeed and Coil:Heating:DX:MultiSpeed):
+
+\begin{equation}
+{T_{outlet}} = {T_{inlet}} + \frac{{{Q_{WasteHeat}}}}{{{C_p}{{\dot m}_{hr}}}}
+\end{equation}
+
+where
+
+T\(_{outlet}\) = outlet node temperature of heat recovery, C
+
+T\(_{inlet}\) = inlet node temperature of heat recovery, C
+
+Q\(_{WasteHeat}\) = recoverable waste heat generated by its child objects, W
+
+C\(_{p}\) = inlet node temperature of heat recovery, C
+
+\({{{\dot m}_{hr}}}\) = mass flow rate of heat recovery, kg/s
+
+If the outlet node temperature is above the value of the Maximum Temp for Heat Recovery field, the outlet node temperature is reset to the value of Maximum Temp for Heat Recovery.
+
+\subsection{DX Cooling Package}\label{dx-cooling-package}
+
+\subsubsection{Overview}\label{overview-5}
+
+The DX cooling package subsystem model provides a ``virtual'' component that consists of a DX air cooling coil component as shown in the figure below. The CoilSystem:Cooling:DX input object provides a container component that controls the associated DX cooling coil which is specified in a separate object. This coil can be specified anywhere in the air loop simulation and is controlled by the setpoint(s) on the control node. Optional dehumidification controls may also be specified. CoilSystem:Cooling:DX assumes continuous fan operation for any given time step, because it is not able to control cycling fan operation in the way that other AirLoopHVAC:Unitary* systems can.
+
+This system does not need any plant specification and will provide the electric consumption necessary to operate the compressor and the condenser fan.
+
+\begin{figure}[hbtp] % fig 231
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5198.png}
+\caption{Schematic of Packaged DX Cooling Subsystem in Air Loop for a Blow-Thru Application \protect \label{fig:schematic-of-packaged-dx-cooling-subsystem-in}}
+\end{figure}
+
+\subsubsection{Controls}\label{controls-1}
+
+The system calculates the current sensible load using the temperature of the inlet node and the System Node Setpoint Temp on the control node. If the control node is not the outlet node, the desired outlet node temperature is adjusted for the current temperature difference between the outlet node and the control node. Likewise, the current latent load is calculated using the humidity ratio of the inlet node and the System Node Humidity Ratio Max on the control node. The controls determine the required coil run-time fraction and dehumidification mode (if applicable) using the steps outlined below.
+
+\paragraph{Step 1 -- Meet Sensible Load Requirement}\label{step-1-meet-sensible-load-requirement-1}
+
+The controls first attempt to meet the sensible requirement. The specified DX coil model is called with a part-load ratio (PLR) of 1.0 to determine the full-load output of the coil. This is compared with the desired outlet node temperature and a sensible PLR is calculated. If the PLR is \textless{}1.0, a Regula-Falsi iteration routine is called to determine the coil run-time fraction which results in the desired outlet node temperature. For a variable-speed DX cooling coil, if the load is smaller than the sensible capacity at the lowest speed, the coil run-time fraction is determined in the same way as a single-speed DX cooling coil. Otherwise, its speed level and speed ratio between two neighboring speeds are selected to match the load.
+
+If the cooling coil type is specified as CoilSystem:Cooling:DX:CoolingHeatExchanganerAssisted and the dehumidification control type is specified as CoolReheat, the heat exchanger is active during this attempt to meet the sensible requirement.
+
+\paragraph{Step 2 -- Meet Latent Load Requirement (if activated)}\label{step-2-meet-latent-load-requirement-if-activated-1}
+
+If dehumidification controls are active, the leaving humidity ratio resulting from operation to meet the sensible load (Step 1 above) is compared with the desired outlet node humidity ratio. If the humidity requirement is already met, then no further control action is taken. If the humidity requirement has not been met, then the coil is re-simulated depending on the type of humidity control.
+
+\paragraph{Step 2a -- Humidity Control = MultiMode}\label{step-2a-humidity-control-multimode-1}
+
+If the humidity control type is MultiMode, then the coil's enhanced dehumidification mode is activated when the coil type is Coil:Cooling:DX:TwoStageWithHumidityControlMode or the heat exchanger is activated when the coil type is \\
+CoilSystem:Cooling:DX:CoolingHeatExchangerAssisted and Step 1 above is repeated to meet the sensible load using the coil performance resulting from the enhanced dehumidificaiton mode. This is a semi-passive approach to dehumidification which may fall short or may exceed the dehumidification requirement. If the user has specified Run on Latent Load = Yes in the CoilSystem:Cooling:DX object, and there is no sensible load to be met, then the system will try to meet the entire dehumidification load. If dehumidification mode should not be active when there is no sensible load, then choose Run on Latent Load = No.
+
+\paragraph{Step 2b -- Humidity Control = CoolReheat}\label{step-2b-humidity-control-coolreheat-1}
+
+If the humidity control type is CoolReheat, the coil is re-simulated to achieve the desired outlet node humidity ratio. This option is valid for all cooling coil types. When the coil type is Coil:Cooling:DX:TwoStageWithHumidityControlMode, only the cooling performance mode is used for this step and enhanced dehumidification mode is not activated.
+
+\subsection{DX Heating Package}\label{dx-heating-package}
+
+\subsubsection{Overview}\label{overview-6}
+
+The DX heating package subsystem model provides a ``virtual'' component that consists of a DX air-to-air heating coil component and associated controls. The CoilSystem:Heating:DX input object provides a container component that controls the associated DX heating coil~ which is specified in a separate object. See the entry called Single-Speed and Variable-Speed Electric Heat Pump DX Air Heating Coil for details of the coil model itself.~ This coil can be specified anywhere in the air loop simulation and is controlled by the setpoint on the heating coil's outlet node. This model is analogous to the model for CoilSystem:Cooling:DX which is similar but for cooling.~ The model assumes continuous fan operation for any given time step, because it is not able to control cycling fan operation in the way that other AirLoopHVAC:Unitary* systems can.
+
+This system does not need any plant specification and will provide the electric consumption necessary to operate the compressor and the condenser fan.
+
+\subsubsection{Controls}\label{controls-2}
+
+The DX heating package system calculates how the coil should operate to meet current sensible load using the temperature of the inlet node and the System Node Setpoint Temp on the outlet node. The controls determine the required coil run-time fraction to meet the sensible requirement. The Single-Speed Electric Heat Pump DX Air Heating Coil model is called with a part-load ratio (PLR) of 1.0 to determine the full-load output of the coil. If the PLR is \textless{}1.0, a Regula-Falsi iteration routine is called to determine the coil run-time fraction which results in the desired outlet node temperature. For a variable-speed DX heating coil, if the load is smaller than the heating capacity at the lowest speed, the coil run-time fraction is determined in the same way as a single-speed DX heating coil. Otherwise, its speed level and speed ratio between two neighboring speeds are selected to match the load.
+
+\subsection{Desiccant Dehumidifier Package}\label{desiccant-dehumidifier-package}
+
+\subsubsection{Overview}\label{overview-7}
+
+The input object Dehumidifier:Desiccant:System provides a model that packages components for a desiccant-based subsystem that dehumidifies an air stream, normally called the process air stream. A second heated air stream, called the regeneration air stream, is used to remove the collected moisture from the desiccant heat exchanger and this moisture-laden air is then usually exhausted from the building. This Dehumidifier:Desiccant:System object is similar to the Dehumidifier:Desiccant:NoFans object but has some additional modeling capabilities.
+
+The Dehumidifier:Desiccant:System desiccant dehumidifier object in EnergyPlus is a compound object that can be placed anywhere in an air loop. Common locations for this object are in an AirLoopHVAC:OutdoorAirSystem or in the main air loop downstream of a cooling coil (postcooling desiccant dehumidifier). This compound object coordinates the operation of several `children' objects: a desiccant heat exchanger, a regeneration air fan, and an optional regeneration air heater. If this dehumidifier is placed in the main air loop immediately downstream of a direct expansion (DX) cooling coil, then the dehumidifier's operation can be coordinated with the operation of the companion DX coil and it is also possible to specify that the DX system's condenser waste heat can be used to help regenerate the desiccant heat exchanger. For the case of condenser waste heat regeneration, an optional exhaust fan can also be modeled by this desiccant dehumidifier compound object to help maintain a setpoint temperature for air entering the regeneration side of the desiccant heat exchanger. Refer to the EnergyPlus Input Output Reference for the specific input syntax for this desiccant dehumidifier object.
+
+\begin{figure}[hbtp] % fig 232
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5199.png}
+\caption{Schematic of a Desiccant Dehumidifier with Draw Through Regeneration Fan Placement \protect \label{fig:schematic-of-a-desiccant-dehumidifier-with}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 233
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5200.png}
+\caption{Schematic of a Desiccant Dehumidifier in Blow Through Regeneration Fan Placement \protect \label{fig:schematic-of-a-desiccant-dehumidifier-in-blow}}
+\end{figure}
+
+\subsubsection{Control Logic}\label{control-logic}
+
+The model first decides if the dehumidifier can operate for the simulation time step, based on its availability schedule and if there is air flow detected on the process air inlet node. If available to operate, then the target humidity ratio for the process outlet air is determined based on the maximum humidity ratio setpoint on the control node (System Node Setpoint Humidity Ratio Max). If the control node is not the process air outlet node, the target humidity ratio is adjusted for the current humidity ratio difference between the process air outlet node and the control node. If the humidity ratio of the process inlet air is greater than the target humidity ratio for the process outlet air, then the dehumidifier operates to meet the target to the extent possible.
+
+Once it is determined that the dehumidifier should operate, the components upstream of the desiccant heat exchanger's regeneration inlet are modeled. The actual components that are modeled depend on the configuration specified by the user.
+
+If the waste heat from the companion cooling coil is being used to heat the regeneration air, then this model determines the temperature of the air leaving the cooling coil condenser. The user may also specify a setpoint temperature for the regeneration air entering the desiccant heat exchanger and an optional exhaust fan, which can impact the condenser leaving air temperature. For this case, the exhaust fan is used to control the condenser leaving air temperature by boosting the air flow rate through the condenser to meet the setpoint temperature (minus regeneration fan heat if blow through fan placement).
+
+Note: If the desiccant dehumidifier is OFF for a simulation time step but its companion cooling coil is operating and is specified to provide regeneration air heating, then the exhaust fan operates at the maximum air flow rate (i.e., this fan serves at the condenser fan for the companion cooling coil system when regeneration air heating is specified, so the inputs for the companion cooling coil object should not include the condenser fan energy since the condenser fan energy is modeled by the Dehumidifier:Desiccant:SystemDesiccant Dehumidifier object).
+
+The exhaust fan power is determined as follows:
+
+If dehumidifier is operating:
+
+\begin{equation}
+  \begin{array}{rl}
+    PLR_{exhaust} &= \frac{\dot{m}_{exhaust}}{\rho_{Std}\dot{V}_{exhaust,max}} \\
+    P_{exhaust} &= P_{exhaust,max} \cdot ExhFanModFac
+  \end{array}
+\end{equation}
+
+If dehumidifier is not operating, but companion coil is operating:
+
+\begin{equation}
+  P_{exhaust} = P_{exhaust,max} \cdot PLR_{companion coil}
+\end{equation}
+
+where:
+
+\(PL{R_{exhaust}}\) ~ = part load ratio of the exhaust fan
+
+\({\mathop {\rm{V}}\limits^ \bullet_{exhaust,\,max}}\) ~ = exhaust fan maximum volumetric flow rate, user input (m\(^{3}\)/s)
+
+\({\rho_{Std}}\) ~~~~~~~~~~ = density of air at standard temperature and pressure {[}dry air at 20°C{]} (m\(^{3}\)/kg)
+
+\({P_{exhaust,\,max}}\) ~~ = exhaust fan maximum power, user input (W)
+
+\(ExhFanModFac\) = exhaust fan power modifier curve evaluated at PLR\(_{exhaust}\). If modifier curve not provided by the user, then this factor is assumed to be 1.0.
+
+\(PL{R_{companion\,coil}}\) ~~~~ = part load ratio of the companion cooling coil
+
+\({P_{exhaust}}\) ~~~~~~~ = output variable `Dehumidifier Exhaust Fan Electric Power, W'
+
+The exhaust fan electric consumption is then calculated as:
+
+\begin{equation}
+{E_{exhaust}} = {P_{exhaust}}*\,\,TimeStepSys\,\,*\,\,3600.
+\end{equation}
+
+where:
+
+\({E_{exhaust}}\) ~~~~~~ ~~ = output variable `Dehumidifier Exhaust Fan Electric Energy, J'
+
+\(TimeStepSys\) = HVAC system simulation time step, hr
+
+Once the outlet conditions from the companion coil condenser are determined (if present), then the regeneration air fan (if blow through configuration) and regeneration air heater (if present) are simulated. To the extent possible (e.g., if the heater is available to operate based on its availability schedule and it has sufficient heating capacity), the regeneration air heater operates to raise its outlet air temperature to the specified regeneration inlet air setpoint temperature.
+
+With the inlet air conditions to the regeneration and process sides of the desiccant heat exchanger now known, the performance of the desiccant heat exchanger is modeled. If the desiccant dehumidifier is specified with a companion cooling coil upstream of the heat exchanger's process inlet, then the model assumes that the dehumidifier operates at the same time as the companion coil (same part-load ratio). If not, then the desiccant dehumidifier model calculates the fraction of time it must operate to meet the process outlet air maximum humidity target (setpoint) using the following equation:
+
+\begin{equation}
+  \begin{array}{rl}
+    DDPartLoadRatio &= \frac{w_{Proc,in} - w_{max, setpoint}}{w_{Proc,in} - w_{Proc,out,HXon}} \\
+    DDPartLoadRatio &= \max\PB{0.0,DDPartLoadRatio} \\
+    DDPartLoadRatio &= \min\PB{1.0,DDPartLoadRatio}
+  \end{array}
+\end{equation}
+
+where:
+
+\(\,DDPartLoadRatio\) ~ = output variable `Dehumidifier Part Load Ratio'
+
+\({w_{Proc,\,\,in}}\) ~~~~~ = process inlet air humidity ratio (kg/kg)
+
+\({w_{max, set\,point}}\) = target humidity ratio (setpoint) for the process outlet air (kg/kg)
+
+\({w_{Proc,\,\,out,HXon}}\) = process outlet air humidity ratio when the desiccant heat exchanger operates ~ ~~~~(kg/kg)
+
+After all of the desiccant dehumidifier components are modeled at the appropriate part load ratio, the water removal rate and water removed are calculated.
+
+\begin{equation}
+  \begin{array}{rl}
+    \dot{m}_{water_removed,Proc} & = \dot{m}_{Proc,in} \PB{w_{Proc,in} - w_{Proc,out}} \\
+    m_{water_removed,Proc}       & = \dot{m}_{water_removed,Proc} \cdot TimeStepSys \cdot 3600\dfrac{•}{•}
+  \end{array}
+\end{equation}
+
+where:
+
+\({\mathop m\limits^ \bullet_{water_removed,Proc}}\) ~ = output variable `Dehumidifier Removed Water Mass Flow Rate, kg/s'
+
+\({\mathop m\limits^ \bullet_{Proc,in}}\) ~~~~~~ = air mass flow rate at the process air inlet node (kg/s)
+
+\({w_{Proc,\,\,out}}\) ~~~~ = process outlet air humidity ratio (kg/kg)
+
+\({m_{water_removed,Proc}}\) = output variable `Dehumidifier Removed Water Mass, kg'
+
+\subsubsection{References}\label{references-000}
+
+ASHRAE. 2004. Chapter 22: Desiccant Dehumidification and Pressure-Drying Equipment. 2004 ASHRAE HVAC Systems and Equipment Handbook. Atlanta, GA: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Kosar, D. 2006. Dehumidification Enhancements, ASHRAE Journal, Vol. 48, No. 2, February 2006.
+
+Kosar, D. et al. 2006. Dehumidification Enhancement of Direct Expansion Systems Through Component Augmentation of the Cooling Coil. 15\(^{th}\) Symposium on Improving Building Systems in Hot and Humid Climates, July 24-26, 2006.
+
+\subsection{Unitary Water-To-Air Heat Pump}\label{unitary-water-to-air-heat-pump}
+
+\subsubsection{Overview}\label{overview-8}
+
+The input object AirLoopHVAC:UnitaryHeatPump:WaterToAir provides a model for a water-to-Air heat pump that is a ``virtual'' component that consists of an on/off fan component, a water-to-air heat pump cooling coil, a water-to-air heat pump heating coil, and a gas or electric supplemental heating coil. The specific configuration of the blowthru heat pump is shown in the following figure. For a drawthru heat pump, the fan is located between the water-to-air heat pump heating coil and the supplemental heating coil. The configuration of the water-to-air heat pump in the air loop is similar to an air-to-air heat pump. In addition, a water-to-air heat pump has a water loop connection on its source side. The water loop can be served by a condenser loop (like GHE for Ground source systems), or by a cooling tower/ boiler plant loop (for water loop systems).
+
+\begin{figure}[hbtp] % fig 234
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5222.png}
+\caption{Source Side and Load Side Configuration of a BlowThru WateroToAir Heat Pump \protect \label{fig:source-side-and-load-side-configuration-of-a}}
+\end{figure}
+
+There are two different models for water-to-air heat pump cooling and heating coils. Cooling and heating coils are modeled using a Single Speed or Variable Speed Equation Fit model or a Parameter Estimation model. The parameter estimation procedure is quite detailed and the equation fit model is designed to simplify the user inputs. Each model is discussed in short in the following sections. The Variable-Speed Equation Fit model is described in a separate section, as Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit and Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit.
+
+\subsubsection{Single Speed Equation-Fit Model:}\label{single-speed-equation-fit-model}
+
+This section describes the equation-fit model for Water-to-Air heat pump (Object names: \textbf{Coil:Cooling:WaterToAirHeatPump:EquationFit} and \\ \textbf{Coil:Heating:WaterToAirHeatPump:EquationFit}). This documentation is derived from the M.S. dissertation of Tang (2005) which is available on the Oklahoma State University web site . The model uses five non-dimensional equations or curves to predict the heat pump performance in cooling and heating mode. The methodology involved using the generalized least square method to generate a set of performance coefficients from the catalog data at indicated reference conditions. Then the respective coefficients and indicated reference conditions are used in the model to simulate the heat pump performance. The variables or inlet conditions that influenced the water-to-air heat pump performance are load side inlet water temperature, source side inlet temperature, source side water flow rate and load side water flow rate. The governing equations for the cooling and heating mode are as following:
+
+Cooling Mode:
+
+\begin{equation}
+\frac{{Q{}_{total}}}{{Q{}_{total,ref}}} = A1 + A2\left[ {\frac{{{T_{wb}}}}{{{T_{ref}}}}} \right] + A3\left[ {\frac{{T{}_{w,in}}}{{T{}_{ref}}}} \right] + A4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + A5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]
+\end{equation}
+
+\begin{equation}
+\frac{{{Q_{sens}}}}{{{Q_{sens,ref}}}} = B1 + B2\left[ {\frac{{T{}_{db}}}{{T{}_{ref}}}} \right] + B3\left[ {\frac{{T{}_{wb}}}{{T{}_{ref}}}} \right] + B4\left[ {\frac{{T{}_{w,in}}}{{T{}_{ref}}}} \right] + B5\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + B6\left[ {\frac{{\dot V{}_w}}{{\dot V{}_{w,ref}}}} \right]
+\end{equation}
+
+\begin{equation}
+\frac{{Power{}_c}}{{Power{}_{c,ref}}} = C1 + C2\left[ {\frac{{{T_{wb}}}}{{{T_{ref}}}}} \right] + C3\left[ {\frac{{T{}_{w,in}}}{{T{}_{ref}}}} \right] + C4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + C5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]
+\end{equation}
+
+Heating Mode:
+
+\begin{equation}
+\frac{{{Q_h}}}{{Q{}_{h,ref}}} = E1 + E2\left[ {\frac{{{T_{db}}}}{{{T_{ref}}}}} \right] + E3\left[ {\frac{{T{}_{w,in}}}{{T{}_{ref}}}} \right] + E4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + E5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]
+\end{equation}
+
+\begin{equation}
+\frac{{Powe{r_h}}}{{Power{}_{h,ref}}} = F1 + F2\left[ {\frac{{{T_{db}}}}{{{T_{ref}}}}} \right] + F3\left[ {\frac{{T{}_{w,in}}}{{T{}_{ref}}}} \right] + F4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + F5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]
+\end{equation}
+
+Assuming no losses, the source side heat transfer rate for cooling and heating mode is calculated as following;
+
+\begin{equation}
+{Q_{source,c}} = {Q_{total}} + Powe{r_c}
+\end{equation}
+
+\begin{equation}
+{Q_{source,h}} = {Q_h} - Powe{r_h}
+\end{equation}
+
+where:
+
+\(A1 - F5\) ~ ~~ = Equation fit coefficients for the cooling and heating mode
+
+\({T_{ref}}\) ~~~~~~~~~~~ = 283K
+
+\({T_{w,in}}\) ~~~~~~~~~~ = Entering water temperature, K
+
+\({T_{db}}\) ~~~~~~~~~~~~ = Entering air dry-bulb temperature, K
+
+\({T_{wb}}\) ~~~~~~~~~~~ = Entering air wet-bulb temperature, K
+
+\({\dot V_{air}}\) ~~~~~~~~~~~ = Load side air volumetric flow rate, m\(^{3}\)/s
+
+\({\dot V_w}\) ~~~~~~~~~~~~~~~~~~~~~~~~ = Source side water volumetric flow rate, m\(^{3}\)/s
+
+\({Q_{total}}\) ~~~~~~~~~ = Total cooling capacity, W
+
+\({Q_{sens}}\) ~~~~~~~~~ = Sensible cooling capacity, W
+
+\(Powe{r_c}\) ~~~~ = Power consumption (cooling mode), W
+
+\({Q_{source,c}}\) ~~~~~ = Source side heat transfer rate (cooling mode), W
+
+\({Q_h}\) ~~~~~~~~~~~~~~~~~~~~~~~~ = Total heating capacity, W
+
+\(Powe{r_h}\) ~~~~ = Power consumption (heating mode), W
+
+\({Q_{source,h}}\) ~~~~~ = Source side heat transfer rate (heating mode), W
+
+The inlet conditions or variables are divided by the reference conditions. This formulation allows the coefficients to fall into smaller range of values. Moreover, the value of the coefficient indirectly represents the sensitivity of the output to that particular inlet variable. The reference conditions used when generating the performance coefficients must be the same as the reference conditions used later in the model. The reference temperature \({T_{ref}}\) is fixed at 283K. Temperature unit of Kelvin is used instead of Celsius to keep the ratio of the water inlet temperature and reference temperature positive value should the water inlet temperature drop below the freezing point.
+
+For cooling mode, the reference conditions; reference load side air volumetric flow rate \(\left( {{{\dot V}_{air,ref}}} \right)\) ,reference source side water volumetric flow rate\(\left( {{{\dot V}_{w,ref}}} \right)\) ,reference sensible capacity \(\left( {{Q_{sens,ref}}} \right)\) ~and reference power input \(\left( {Powe{r_{c,ref}}} \right)\) ~are the conditions when the heat pump is operating at the highest cooling capacity or reference cooling capacity\(\left( {{Q_{total,ref}}} \right)\) ~indicated in the manufacturer's catalog. Note that the reference conditions for heating mode might differ from the reference conditions specified for the cooling mode.
+
+\subsubsection{Coefficient estimation procedure:}\label{coefficient-estimation-procedure}
+
+The generalized least square method is used to generate the coefficients. This method utilizes an optimization method which calculates the coefficients that will give the least amount of differences between the model outputs and the catalog data. A set of coefficients for the cooling mode is generated which includes A1-A5 for total cooling capacity, B1-B6 for sensible cooling capacity, and C1-C5 for power consumption. The same procedure is repeated for the heating mode to generate the coefficients E1-E5 and F1-F5. An information flow chart showing the inputs, reference conditions, performance coefficients and outputs are shown in the figure below:
+
+\begin{figure}[hbtp] % fig 235
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5250.png}
+\caption{Information Flow Chart for Water-to-Air Heat Pump Equation Fit Model (Tang 2005) \protect \label{fig:information-flow-chart-for-water-to-air-heat}}
+\end{figure}
+
+\subsubsection{High Humidity Control with WaterToAir HeatPump Equation Fit model}\label{high-humidity-control-with-watertoair-heatpump-equation-fit-model}
+
+The specific configuration of the WaterToAir HeatPump with supplemental heating coil is shown above (see Figure~\ref{fig:source-side-and-load-side-configuration-of-a}). This figure shows the fan placement when a blow through fan is specified. If a draw through fan is specified, the fan is located between the heating coil and the reheat coil. The system is controlled to keep the high relative humidity in the control zone from exceeding the setpoint specified in the object ZoneControl:Humidistat. When high humidity control is specified and the compressor operates, the heatpump always operates at the cooling air flow rate when a zone heating load is present as determined by the zone thermostat. High humidity control is specified as either None, or CoolReheat in the Dehumidification Control Type input field. CoolReheat is specified when a DX cooling coil is used to over-cool the supply air stream in order to meet the zone latent load. In this case, a supplemental heating coil will ensure the zone temperature does not fall below the zone heating temperature set point. If the dehumidification control type is selected as None, the WaterToAir HeatPump uns only to meet the sensible cooling load. A supplemental heating coil is required for all dehumidification control types.
+
+The model first calculates the \emph{PartLoadRatio} required meeting the sensible cooling load.~ The heatpump's sensible cooling load is determined from the control zone sensible cooling load to the cooling setpoint and the control zone air flow fraction to maintain the dry-bulb temperature setpoint in the control zone:
+
+\begin{equation}
+HeatPumpCoolingLoad = \,\frac{{ControlZoneCoolingLoad}}{{ControlZoneAirFlowFraction}}
+\end{equation}
+
+The heatpump's sensible cooling load to be met and the full load cooling output are used to calculate the sensible the part-load ratio iteratively based on user specified convergence criterion.
+
+\begin{equation}
+PartLoadRatio = MAX\left( {0.0,\,\frac{{ABS\left( {HeatPumpCoolingLoad - NoCoolOutput} \right)}}{{ABS\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)
+\end{equation}
+
+When the heat pumps sensible cooling capacity meets the system sensible cooling load at a given sensible part load ratio, then the Heat pump meets the controlled zone cooling setpoint temperature.~ If a moisture (latent) load exists because the control zone humidity has exceeded the setpoint, the total moisture load to be met by the heat pumps (HeatPumpMoistureLoad) is calculated based on the control zone moisture load and the control zone air flow fraction.
+
+\begin{equation}
+HeatPumpMoistureLoad = \,\frac{{ControlZoneMoitureLoad}}{{ControlZoneAirFlowFraction}}
+\end{equation}
+
+Then the \emph{LatentPartLoadRatio} required to meet the high humidity setpoint is calculated as follows:
+
+\begin{equation}
+LatentPartLoadRatio = MIN\left( {PL{R_{Min}},\,\frac{{ABS\left( {HeatPumpMoistureLoad - NoLatentOutput} \right)}}{{ABS\left( {FullLatentOutput - NoLatentOutput} \right)}}} \right)
+\end{equation}
+
+The model uses the greater of the two part-load ratios, \emph{PartLoadRatio} or \emph{LatentPartLoadRatio}, to determine the operating part-load ratio of the Heat Pump's DX cooling coil.
+
+\begin{equation}
+LatentPartLoadRatio = MAX\left( {PartLoadRatio,\,LatentPartLoadRatio} \right)
+\end{equation}
+
+As previously described, iterations are performed to converge on the solution within the convergence tolerance.
+
+Where,
+
+\(ControlZoneCoolingLoad\) = the control zone sensible cooling load to the cooling setpoint, (W).
+
+\(ControlZoneMoistureLoad\) ~~~~~~~~ = the control zone moisture load to the dehumidifying relative humidity setpoint, (W).
+
+\(ControlZoneAirFlowFraction\) ~~~~ = the supply air fraction that goes though the control zone, (-).
+
+\emph{FullLatentOutput} ~~~~ = ~~~~~~~~~the Heat Pump's latent cooling energy rate at full-load conditions, W
+
+\emph{NoLatentOutput} ~~~~~ = ~~~~~~~~~ the Heat Pump's latent cooling energy rate with cooling coil OFF, W
+
+\(PartLoadRatio\) ~~~~ = ~~~~~~~~~ the heat pump's part-load-ratio required to meet system sensible load, (-).
+
+\(LatentPartLoadRatio\) ~~~~~ = ~~~~~~~~~ the heat pump's part-load-ratio required to meet system moisture load, (-).
+
+\(PL{R_{MIN}}\) \emph{~~~~~~ = ~~}the minimum part-load ratio, which is usually 0.0. For the case when the latent capacity degradation model is used (Ref: DX Cooling Coil Model), this value is the minimum part-load ratio at which the cooling coil will dehumidify the air.
+
+When the predicted zone air temperature is above the heating setpoint and if there is a dehumidification load, the supplemental heating coil load is required to offset the excess cooling as shown in Figure~\ref{fig:supplemental-heating-coil-load-when-predicted-004}. If the model determines that the LatentPartLoadRatio is to be used as the operating part-load ratio of the heatpump's cooling coil, the supplemental coil is used to offset the excess sensible capacity provided by the unit. The model first checks the sensible load that exists for the current simulation time step (predicted zone temperature with no HVAC operation compared to the thermostat setpoint temperatures). If a sensible cooling load or no sensible cooling or heating load exists (see Figure~\ref{fig:supplemental-heating-coil-load-when-predicted-004}),~ the model calculates the difference between the sensible heating load required to reach or maintain the heating dry-bulb temperature setpoint and the actual sensible cooling energy rate delivered by the heat pump (with LatentPartLoadRatio). In this case, thesupplemental heating coil is used to offset the excess sensible cooling energy provided by the DX cooling coil (if any) that could have caused an overshoot of the heating dry-bulb temperature setpoint. Note that when a humidistat is used and high humidity control is required, the zone dry-bulb temperature will typically move toward the heating temperature setpoint when a high moisture (latent) load exists.
+
+\begin{figure}[hbtp] % fig 236
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5262.png}
+\caption{Supplemental heating coil load when predicted zone air temperature is above the heating Setpoint \protect \label{fig:supplemental-heating-coil-load-when-predicted-004}}
+\end{figure}
+
+If a heating load exists (Figure~\ref{fig:supplemental-heating-coil-load-when-predicted-005}), the supplementalheating coil is used to meet the heating coil load and at the same time offset the entire sensible cooling energy rate of the DX cooling coil (to meet the humidistat setpoint). Note that when a heating load exists and high humidity control is required, the heat pump operates at the user-specified cooling air flow rate for the entire simulation time step. As with the fan, and DX cooling coil, report variables associated with supplemental heating coil performance (e.g., heating coil energy, heating coil rate, heating coil gas or electric energy, heating coil runtime fraction, etc.) are managed in the supplemental (heating) coil object.
+
+\begin{figure}[hbtp] % fig 237
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5263.png}
+\caption{Supplemental heating coil load when predicted zone air temperature is below the heating setpoint \protect \label{fig:supplemental-heating-coil-load-when-predicted-005}}
+\end{figure}
+
+\subsubsection{Parameter Estimation Model}\label{parameter-estimation-model}
+
+The steady state simulation model (Object: AirLoopHVAC:UnitaryHeatPump:WaterToAir) for a water-to-air vapor compression heat pump is described in this section. The model is implemented under the air-loop manager similar to the algorithm discussed under AirLoopHVAC:UnitaryHeatPump. The heat pump `coil' objects \\
+(Coil:Cooling:WaterToAirHeatPump:ParameterEstimation and Coil:Heating:WaterToAirHeatPump:ParameterEstimation) actually consist of a steady state simulation of the unitary heat pump in cooling or heating mode respectively.~ This documentation is derived from the Ph.D.~dissertation of Hui Jin which is available on the Oklahoma State University web site . ~The model parameters, solution technique and solution algorithm are all identical to that of the water to water heat pump.~ The only difference between the two models is in the modeling of the water to air heat exchanger.
+
+The effectiveness of this heat exchanger is given by
+
+\begin{equation}
+\varepsilon  = 1 - {e^{ - NTU}}
+\end{equation}
+
+Where NTU is defined by
+
+\begin{equation}
+NTU = \frac{{UA}}{{(\dot mC{}_p){}_{water/air}}}
+\end{equation}
+
+UA for the source side and the load side are two of the parameters estimated in the parameter estimation procedure.
+
+Additional model details and a discussion of the parameters and parameter estimation technique are described in the following section on Water to Water Heat Pumps.
+
+\subsection{Water To Water Heat Pumps}\label{water-to-water-heat-pumps}
+
+There are two water-water heat pump models available in EnergyPlus which are \textbf{parameter estimation based model} and \textbf{equation-fit model}. Detailed descriptions of the model are available in the references Tang and Jin
+
+\subsection{Equation Fit Water To Water Heat Pump Model}\label{equation-fit-water-to-water-heat-pump-model}
+
+This section describes the equation-fit model for water-to-water heat pump. (Object names: HeatPump:WaterToWater:EquationFit:Cooling \& HeatPump:WaterToWater:EquationFit:Heating). This documentation is derived from the M.S. dissertation of Tang (2005) which is available on the Oklahoma State University web site . The model uses four non-dimensional equations or curves to predict the heat pump performance in cooling and heating mode. The methodology involved using the generalized least square method to generate a set of performance coefficients from the catalog data at indicated reference conditions. Then the respective coefficients and indicated reference conditions are used in the model to simulate the heat pump performance. The variables that influenced the water-to-water heat pump performance are load side inlet water temperature, source side inlet temperature, source side water flow rate and load side water flow rate. The governing equations for the cooling and heating mode are as following:
+
+Cooling Mode:
+
+\begin{equation}
+\frac{{Q{}_c}}{{Q{}_{c,ref}}} = A1 + A2\left[ {\frac{{T{}_{L,in}}}{{T{}_{ref}}}} \right] + A3\left[ {\frac{{T{}_{S,in}}}{{T{}_{ref}}}} \right] + A4\left[ {\frac{{{{\dot V}_L}}}{{{{\dot V}_{L,ref}}}}} \right] + A5\left[ {\frac{{{{\dot V}_S}}}{{{{\dot V}_{S,ref}}}}} \right]
+\end{equation}
+
+\begin{equation}
+Powe{r_c} = B1 + B2\left[ {\frac{{T{}_{L,in}}}{{T{}_{ref}}}} \right] + B3\left[ {\frac{{T{}_{S,in}}}{{T{}_{ref}}}} \right] + B4\left[ {\frac{{{{\dot V}_L}}}{{{{\dot V}_{L,ref}}}}} \right] + B5\left[ {\frac{{{{\dot V}_S}}}{{{{\dot V}_{S,ref}}}}} \right]
+\end{equation}
+
+Heating Mode:
+
+\begin{equation}
+\frac{{{Q_h}}}{{Q{}_{h,ref}}} = C1 + C2\left[ {\frac{{T{}_{L,in}}}{{T{}_{ref}}}} \right] + C3\left[ {\frac{{T{}_{S,in}}}{{T{}_{ref}}}} \right] + C4\left[ {\frac{{{{\dot V}_L}}}{{{{\dot V}_{L,ref}}}}} \right] + C5\left[ {\frac{{{{\dot V}_S}}}{{{{\dot V}_{S,ref}}}}} \right]
+\end{equation}
+
+\begin{equation}
+Powe{r_h} = D1 + D2\left[ {\frac{{T{}_{L,in}}}{{T{}_{ref}}}} \right] + D3\left[ {\frac{{T{}_{S,in}}}{{T{}_{ref}}}} \right] + D4\left[ {\frac{{{{\dot V}_L}}}{{{{\dot V}_{L,ref}}}}} \right] + D5\left[ {\frac{{{{\dot V}_S}}}{{{{\dot V}_{S,ref}}}}} \right]
+\end{equation}
+
+Assuming no losses, the source side heat transfer rate for cooling and heating mode is calculated as following;
+
+\begin{equation}
+{Q_{source,c}} = {Q_c} + Powe{r_c}
+\end{equation}
+
+\begin{equation}
+{Q_{source,h}} = {Q_h} - Powe{r_h}
+\end{equation}
+
+Where:
+
+\(A1 - D5\) = Equation fit coefficients for the cooling and heating mode
+
+\({T_{ref}}\) = 283.15K
+
+\({T_{L,in}}\) = Entering load side water temperature, K
+
+\({T_{S,in}}\) = Entering source side water temperature, K
+
+\({\dot V_L}\) = Load side volumetric flow rate, m\(^{3}\)/s
+
+\({\dot V_S}\) = Source side volumetric flow rate, m\(^{3}\)/s
+
+\({Q_c}\) = Load side heat transfer rate (cooling mode), W
+
+\(Powe{r_c}\) = Power consumption (cooling mode), W
+
+\({Q_{source,c}}\) ~~~~~ = Source side heat transfer rate (cooling mode), W
+
+\({Q_h}\) = Load side heat transfer rate (heating mode), W
+
+\(Powe{r_h}\) = Power consumption (heating mode), W
+
+\({Q_{source,h}}\) ~~~~~ = Source side heat transfer rate (heating mode), W
+
+\emph{COP\(_{c}\)} = Cooling coefficient of performance, W/W
+
+\emph{COP\(_{h}\)} = Heating coefficient of performance, W/W
+
+If the load side heat transfer rate (\emph{Q\(_{c}\)} or \emph{Q\(_{h}\)}) or power consumption (\emph{Power\(_{c}\)} or \emph{Power\(_{h}\)}) are less than or equal to zero, then the heat pump is turned off for that simulation time step, a warning is issued, and the simulation continues.
+
+The inlet conditions or variables are divided by the reference conditions. This formulation allows the coefficients to fall into smaller range of values. Moreover, the value of the coefficient indirectly represents the sensitivity of the output to that particular inlet variable. The reference conditions used when generating the performance coefficients must be the same as the reference conditions used later in the model. The reference temperature \({T_{ref}}\) is fixed at 283K. Temperature unit of Kelvin is used instead of Celsius to keep the ratio of the water inlet temperature and reference temperature positive value should the water inlet temperature drop below the freezing point.
+
+For cooling mode, the reference conditions; reference load side volumetric flow rate, \({\dot V_{L,ref}}\) , reference source side volumetric flow rate, \({\dot V_{S,ref}}\) , \(Powe{r_{c,ref}}\) ~~and reference source side heat transfer rate, \({Q_{source,c,ref}}\) ~~are the conditions when the heat pump is operating at the highest cooling capacity or reference cooling capacity, \({Q_{c,ref}}\) ~indicated in the manufacturer's catalog. Note that the reference conditions for heating mode might differ from the reference conditions specified for the cooling mode.
+
+\subsubsection{Coefficient estimation procedure:}\label{coefficient-estimation-procedure-1}
+
+The generalized least square method is used to generate the coefficients. This method utilizes an optimization method which calculates for the coefficients that will give the least amount of differences between the model outputs and the catalog data. A set of coefficients for the cooling mode is generated which includes A1-A5 for load side heat transfer. The same procedure is repeated B, C, and D coefficients. An information flow chart showing the inputs, reference conditions, performance coefficients and outputs are shown in the figure below:
+
+\begin{figure}[hbtp] % fig 238
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5290.png}
+\caption{Information Flow Chart for Water-To-Water Heat Pump Equation Fit (Tang 2005) \protect \label{fig:information-flow-chart-for-water-to-water}}
+\end{figure}
+
+\subsection{Parameter Estimation Water-To-Water Heat Pump Model}\label{parameter-estimation-water-to-water-heat-pump-model}
+
+A steady state simulation model for a water-to-water reciprocating vapor compression heat pump (Object names: HeatPump:WaterToWater:ParameterEstimation:Cooling \& HeatPump:WaterToWater:ParameterEstimation:Heating) is described in this section. This documentation is derived from the Ph.D.~dissertation of Hui Jin which is available on the Oklahoma State University web site . The model incorporates a multivariable unconstrained optimization algorithm to estimate several unspecific parameters. The aim of the model is to describe the detailed physical geometry and operation of each component and replicate the performance of the actual unit in operation. Assuming the thermodynamic process in the expansion device and the pressure drop at the suction and discharge valves to be isenthalpic the heat balance equation is given by
+
+\begin{equation}
+{\dot Q_s} = \dot W + {\dot Q_{_L}}
+\end{equation}
+
+Where:
+
+\({\dot Q_s}\) ~ = Source side heat transfer rate
+
+\({\dot Q_L}\) ~ = Load side heat transfer rate
+
+\(\dot W\) = Compressor power input
+
+The compressor model is based on an isentropic process shown in Figure~\ref{fig:schematic-indicator-diagram-for-a} governed by
+
+\(P{V^\gamma }\) ~ = Constant
+
+Where:
+
+P = Pressure
+
+v = Specific volume
+
+\begin{figure}[hbtp] % fig 239
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5296.png}
+\caption{Schematic indicator diagram for a reciprocating Compressor(Jin 2002) \protect \label{fig:schematic-indicator-diagram-for-a}}
+\end{figure}
+
+Since the refrigerant vapor in the clearance volume as shown in the previous figure goes through a re-expansion procedure, the mass flow rate of the compressor refrigerant is a decreasing function of the pressure ratio.
+
+\begin{equation}
+\mathop m\limits^ \bullet   = \frac{{PD}}{{\nu {}_{suc}}}(1 + C - C{(\frac{{P{}_{dis}}}{{P{}_{suc}}})^{\frac{1}{\gamma }}}
+\end{equation}
+
+Where:
+
+\(\mathop m\limits^ \bullet\) ~ = refrigerant mass flow rate
+
+PD = Piston displacement
+
+C~~ = Clearance factor
+
+\(P{}_{dis}\) ~ = discharge pressure
+
+\(P{}_{suc}\) ~ = Suction pressure
+
+\(\gamma\) ~~~~ = Isentropic exponent
+
+\subsubsection{Parameter estimation procedure:}\label{parameter-estimation-procedure}
+
+A set of parameters for the cooling mode is defined on the basis of the equations used in the model. An information flowchart indicating the parameters, inputs to the model and the resulting outputs acquired are shown in Figure~\ref{fig:information-flowchart-for-water-to-water-heat}. The estimation of parameters is conducted using the catalog data.
+
+The parameter definition include:
+
+n~Piston displacement, PD
+
+n~Clearance factor, C
+
+n~Pressure drop across the suction and discharge valves, \({\rm{\Delta P}}\)
+
+n~Loss factor used to define the electromechanical losses supposed to be proportional to the theoretical power, \({\rm{\eta }}\)
+
+n~Superheat in \(^{ο}\)C or F, \({\rm{\Delta T}}{}_{{\rm{sh}}}\)
+
+n~Constant part of the electromechanical losses,\({\rm{W}}{}_{{\rm{loss}}}\)
+
+n~Source side heat transfer coefficient, (UA)\(_{S}\)
+
+n~Load side heat transfer coefficient, (UA)\(_{L}\)
+
+\begin{figure}[hbtp] % fig 240
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5306.png}
+\caption{Information Flowchart for Water-To-Water Heat Pump Parameter Estimation Mmodel implementation (Jin 2002) \protect \label{fig:information-flowchart-for-water-to-water-heat}}
+\end{figure}
+
+Where:
+
+TWiL~~ = Entering water Load side temperature
+
+TWiS~~ = Entering water Source side temperature
+
+\(\mathop {\rm{m}}\limits^ \bullet {}_{{\rm{WiL}}}\) = Entering water Load side mass flow rate
+
+\(\mathop {\rm{m}}\limits^ \bullet {}_{{\rm{WiS}}}\) = Entering water Source side mass flow rate
+
+S~~~~~ = ~ Thermostatic Signal
+
+The parameter estimation procedure incorporates an objective function that computes the difference between the model outputs and the catalog outputs.~ The objective function is then minimized by using a multi variable unconstrained multi modal Nelder Mead optimization algorithm. As the objective function value lowers after each iteration, the model outputs approach the catalog outputs consequently leading to convergence and the correct parameters are estimated for the respective model. The inputs to the model include the entering water temperatures and mass flow rates on the load side and the source side. The calculation of the objective function is shown in the form of a formula flowchart in Figure~\ref{fig:flow-diagram-of-energyplus-water-to-water}. The square of the sum of the errors (SSQE) for a given set of parameter values that will be minimized is given by
+
+\begin{equation}
+SSQE = \sum\limits_{i = 1} {{{\left( {\frac{{\left( {\mathop {W{}_{cat}}\limits^{} } \right) - \left( {\mathop W\limits^{} } \right){}_i}}{{\left( {\mathop {W{}_{cat}}\limits^{} } \right)}}} \right)}^2}}  + \left( {\frac{{\left( {\mathop {QL{}_{cat}}\limits^{} } \right) - \left( {\mathop {QL}\limits^{} } \right){}_i}}{{\left( {\mathop {QL{}_{cat}}\limits^{} } \right)}}} \right)
+\end{equation}
+
+Where
+
+\({\rm{W}}{}_{{\rm{cat}}}\) = Catalog power consumption
+
+\({\rm{W}}{}_{}\) ~ = Model power consumption
+
+\({\rm{QL}}{}_{{\rm{cat}}}\) = Catalog load side heat transfer
+
+\({\rm{QL}}{}_{}\) ~ = Model load side heat transfer
+
+Extrapolation beyond the catalog data grants the parameter estimation model an upper hand in comparison with the equation fit and deterministic models. However, the detailed model is computationally more intensive. Moreover, when the model is implemented within a transient system simulation program, it may come across figures that are random and unplanned by the manufacturer such as low water flow rates or extreme temperatures. This oddity may result in unrealistic set of results.
+
+\begin{figure}[hbtp] % fig 241
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5314.png}
+\caption{Flow diagram of EnergyPlus Water to Water HeatPump implementation \protect \label{fig:flow-diagram-of-energyplus-water-to-water}}
+\end{figure}
+
+\subsubsection{Control Strategy:}\label{control-strategy}
+
+Both water-to-water heat pump models; parameter estimation based model and curve-fit model use the ``cycle time control logic'' developed by Murugappan (2002).
+
+This strategy keeps the heat pump from short-cycling whereby the heat pump will stay on or off for the specified cycle time after switching states. The control logic is identical to the operation of a physical heat pump whereby the heat pump does not switch between on and off instantly. Refer to Muraggapan (2002) for the further details on the control strategy.
+
+\subsubsection{References}\label{references-1}
+
+Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from \href{http://www.hvac.okstate.edu}{http://www.hvac.okstate.edu/})
+
+Tang,C. C. 2005. Modeling Packaged Heat Pumps in Quasi-Steady State Energy Simulation Program. M.S. Thesis. Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from \href{http://www.hvac.okstate.edu}{http://www.hvac.okstate.edu/})
+
+Murugappan, Arun. 2002.~ Implementing Ground Source Heat Pump and Ground Loop Heat Exchanger Models in the EnergyPlus Simulation Environment, M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University (downloadable from \href{http://www.hvac.okstate.edu}{http://www.hvac.okstate.edu/})
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-fans.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-fans.tex
new file mode 100644
index 00000000000..8dd196831aa
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-fans.tex
@@ -0,0 +1,638 @@
+\section{Air System Fans }\label{air-system-fans}
+
+\subsection{Overview}\label{overview-002}
+
+Three input objects (Fan:ConstantVolume, Fan:VariableVolume, and Fan:OnOff) provide models for fans -- the prime movers in most of the air loop and zonal air conditioning systems in EnergyPlus. For these input objects, EnergyPlus uses a simple polynomial-based curve-fit model to describe the relation between the volumetric flow rate and the fan electric power, with no explicit modeling of fan pressure rise. Consequently, duct-static-pressure reset strategies cannot be modeled using this approach. For CAV and VAV central air-handling systems, a fourth input object (Fan:ComponentModel) provides a simple physics-based model for flow-dependent fan pressure rise and detailed models for fan, belt, motor, and variable-frequency-drive efficiencies and energy use. This latter input object provides the capability to analyze the effects of duct-static-pressure reset strategies, as well as changes in fan system element performance. All of these fan models calculate the fan energy usage, which is often a large fraction of HVAC energy use and a significant portion of the building energy consumption. They also calculate the temperature rise in the air stream caused by the static pressure increase as the air goes through the fan. If the motor and belt are in the air stream, waste heat from the motor and belt also acts to raise the air stream temperature.
+
+\subsection{Model}\label{model-000}
+
+Each of the four fan models is a forward type: the model inputs describe the fan characteristics and the conditions of the air at the fan inlet; the outputs are the fan electrical power consumption and the conditions of the air at the fan outlet. The model algorithms and data are contained in the \emph{Fans} module in EnergyPlus.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-000}
+
+For the Fan:ConstantVolume, Fan:VariableVolume, and Fan:OnOff models, the user describes the fan by entering values for the design pressure rise across the fan, the design volumetric flow rate, the fan total efficiency, and the fan motor efficiency. The user also needs to specify the fraction of the fan waste heat that will enter the air stream (usually 0 or 1). For the Fan:VariableVolume model, the user must also enter the coefficients of a 4\(^{th}\) order polynomial that relates the fan mass flow rate to the fan power consumption.The independent variable is the volumetric flow fraction; the dependent variable is the fan power part load ratio. For multi-speed fans, the user must enter a fan power ratio as a function of speed ratio performance curve name. Multi-speed fans can only be simulated in a parent object which allows multiple fan speeds (e.g., AirLoopHVAC:Unitary:Furnace:HeatCool, ZoneHVAC:PackagedTerminalAirConditioner, etc.). An optional efficiency curve may also be used when simulating multi-speed fans to adjust the fan total efficiency as the fan speed changes.
+
+For the Fan:ComponentModel object, the user describes the fan in more detail, and also describes the duct system characteristics as seen by the fan. In particular, the user specifies a pressure rise curve with four coefficients that relates the fan total pressure rise to the volumetric flow through the fan, the duct-static-pressure set-point, and the static pressure of the spaces surrounding the ducts. If duct-static-pressure reset is used, the user enters a linear curve with two coefficients that relates the pressure set-point to the volumetric flow through the fan. For the fan itself, the user specifies the fan geometry (wheel diameter and outlet area), maximum efficiency, the Euler number corresponding to the maximum efficiency, the maximum dimensionless flow, the names of four curves with several coefficients that describe the variation of fan efficiency and dimensionless flow with the Euler number in the normal and stall operation regions of the fan, and a sizing factor (applied to the maximum flow through the fan). For the belt, the user specifies the maximum efficiency (or a curve with five coefficients that defines the maximum efficiency as a function of maximum fan shaft input power), three curves with three coefficients each that relate the belt part-load efficiency to belt fractional output torque, the motor/fan pulley diameter ratio, the belt output torque capacity, and a sizing factor (applied to the maximum output torque of the belt). For the motor, the user specifies the maximum efficiency (or a curve with three coefficients that define the maximum efficiency as a function of maximum belt input power), a curve with three coefficients that relate the motor part-load efficiency to motor fractional output power, and a sizing factor (applied to the maximum output power of the motor). For the variable-frequency-drive (VFD), the user specifies a curve with three coefficients that relate the VFD part-load efficiency to motor fractional input power or to motor fractional speed, and a sizing factor (applied to the maximum output power of the VFD).
+
+\subsubsection{Control}\label{control}
+
+The models must decide whether the fan is on or off. The primary on/off trigger is the fan schedule. This is an on/off schedule associated with each fan: a value of 1 indicates the fan is on; a value of 0 indicates the fan is off. The fan schedule can be overruled by flags set by system availability managers. If the flag \emph{TurnFansOn} is true, a zero fan schedule value will be overridden and the fan will be turned on. If the flag \emph{TurnFansOff} is true the fan will be forced off. The inlet air mass flow rate must be greater than zero for the fan to be on.
+
+Generally the fan is a passive component: it accepts the mass flow on its inlet node, uses it in its calculations of energy consumption and temperature rise, and passes it to the outlet node. However the fan maximum and minimum airflow rates act as absolute limits on the airflow rate.
+
+For multi-speed fans, the parent object determines the fan speed ratio (i.e., the selected speed of the fan motor) and uses this value in conjunction with the fan power ratio performance curve to calculate the full load fan power. This full load fan power is then used to determine the part-load performance of the fan and motor assembly.
+
+\subsubsection{Simulation}\label{simulation}
+
+Simple (Single Speed) Fan Model
+
+The following equations define the model for this fan:
+
+\begin{equation}
+{\dot Q_{tot}} = \dot m\cdot \Delta P/({e_{tot}}\cdot {\rho_{air}})
+\end{equation}
+
+\begin{equation}
+{\dot Q_{shaft}} = {e_{motor}}\cdot {\dot Q_{tot}}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{toair}} = {\dot Q_{shaft}} + ({\dot Q_{tot}} - {\dot Q_{shaft}})\cdot {f_{motortoair}}
+\end{equation}
+
+\begin{equation}
+{h_{out}} = {h_{in}} + {\dot Q_{toair}}/\dot m
+\end{equation}
+
+\begin{equation}
+{w_{out}} = {w_{in}}
+\end{equation}
+
+\begin{equation}
+{T_{out}} = PsyTdbFnHW({h_{out}},{w_{out}})
+\end{equation}
+
+On/Off Fan Model
+
+The on/off fan model is similar to the simple fan model with the exception that the on/off fan may cycle on and off during a simulation time step. The cycling rate of the fan is known as the run time fraction. The calculation of run time fraction accounts for the part-load losses of other equipment used in the HVAC system. A part-load factor (a.k.a. part-load ratio) is first calculated for the fan as the ratio of the actual operating mass flow rate to the maximum fan mass flow rate. The run time fraction is then calculated as the part-load factor divided by the part-load fraction. The part-load fraction is determined by other HVAC equipment in the simulation (Ref. DX coil) for use by this specific fan model.
+
+\begin{equation}
+  f_{flow} = \frac{\dot{m}}{\dot{m}_{max}}
+\end{equation}
+
+\begin{equation}
+  RTF = \frac{f_{flow}}{PLF}
+\end{equation}
+
+The total fan power is then calculated as the maximum fan power multipled by the run time fraction.
+
+\begin{equation}
+{\mathop Q\limits^\cdot_{tot}} = RTF\left[ {\mathop m\limits^\cdot  \cdot \Delta P/\left( {{e_{tot}}\cdot {\rho_{air}}} \right)} \right]
+\end{equation}
+
+The remaining calculations are the same as those described in the simple single-speed fan mode.
+
+Multi-Speed Fan Model
+
+The model used to simulate a multi-speed fan relies on the general fan laws to correct for speed changes in the fan's motor and the corresponding change in fan power and fan total efficiency. Two performance curves are used to define the change in power and efficiency as shown below. The power ratio curve must be used to simulate a multi-speed fan. The power ratio curve modifies the fan power based on a change in fan speed according to the cubic fan law. Exponents other than 3 are allowed. The efficiency ratio curve is used to correct for changes in nominal efficiency at alternate fan speeds. If either or both of these curves are not provided, the ratio is assumed to be 1.
+
+The power ratio term is evaluated using an exponent performance curve. The form of the exponent curve equation is shown below.
+
+\begin{equation}
+ExponentCurveOutput = C1 + C2*{x^{C3}}
+\end{equation}
+
+The exponent performance curve is used to evaluate the power ratio as a function of speed ratio (x in the equation above). For typical fan performance, coefficient C1 = 0 and coefficient C2 = 1. The exponent (C3) is typically equal to 3 (cubed fan law) but other values are allowed.
+
+\begin{equation}
+PowerRatio = f{\left( {{N_{ratio}}} \right)^n} = ExponentCurveOutput
+\end{equation}
+
+The efficiency ratio curve is a quadratic or cubic curve used to evaluate the efficiency ratio as a function of speed ratio (x in the following equation). The cubic equation form is shown below.
+
+\begin{equation}
+EfficiencyCurveOutput = C1 + C2{\left( x \right)^2} + C3{\left( x \right)^3}
+\end{equation}
+
+The curve coefficients are determine by correlating the normalized fan total efficiency (i.e., the actual fan total efficiency divided by the nominal fan total efficiency at a speed ratio of 1) to the speed ratio (i.e., the ratio of actual air flow rate through the fan to the maximum fan air flow rate).
+
+\begin{equation}
+EfficiencyRatio = f\left( {{N_{ratio}}} \right) = EfficiencyCurveOutput
+\end{equation}
+
+To account for the change in fan speed and to ensure that the run time fraction is accurately calculated, an adjustment to the previous calculation for run time fraction is made. This adjusts the calculated run time fraction to account for times when the fan speed has been reduced and the new speed is now considered the fan's maximum speed. The speed adjusted run time fraction is then used in the fan power calculation.
+
+\begin{equation}
+RTF = \frac{RTF}{N_{ratio}}
+\end{equation}
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{tot}} = RTF\left[ {\frac{{\mathop m\limits^ \bullet  \Delta P}}{{{e_{tot}}{\rho_{air}}}}} \right]\left( {\frac{{PowerRatio}}{{EfficiencyRatio}}} \right)
+\end{equation}
+
+Each of the performance curves described above may be used to model the performance of a multi-speed fan motor, however, the power ratio curve must be used to envoke the multi-speed simulation. These curves are used when the fan is used in an HVAC system having multiple flow rates (i.e., different flow rates in cooling and heating mode). If an HVAC system operates at the same speed in either cooling or heating mode, these curves are not required. When these curves are not used, the associated ratio term in the equation above is assumed to be 1. The remaining calculations are identical to the simple single-speed fan model described above.
+
+Variable Speed Fan Model
+
+The model for the variable speed fan is similar to the simple single-speed fan model except for a part load factor that multiplies the fan power consumption.
+
+\begin{equation}
+{f_{flow}} = \dot m/{\dot m_{design}}
+\end{equation}
+
+\begin{equation}
+{f_{pl}} = {c_1} + {c_2} \cdot {f_{flow}} + {c_3} \cdot f_{flow}^2 + {c_4} \cdot f_{flow}^3 + {c_5} \cdot f_{flow}^4
+\end{equation}
+
+\begin{equation}
+{\dot Q_{tot}} = {f_{pl}}\cdot {\dot m_{design}}\cdot \Delta P/\left( {{e_{tot}}\cdot {\rho_{air}}} \right)
+\end{equation}
+
+The rest of the calculation is the same as for the simple fan.
+
+\subsubsection{Nomenclature for Simple Models}\label{nomenclature-for-simple-models}
+
+\({\dot Q_{tot}}\) ~is the fan power in watts;
+
+\(\dot m\) is the air mass flow in kg/s;
+
+\({\dot m_{design}}\) is the design (maximum) air flow in kg/s;
+
+\(\Delta P\) is the fan design pressure increase in Pascals;
+
+\({e_{tot}}\) ~is the fan total efficiency;
+
+\({\rho_{air}}\) is the air density at standard conditions in kg/m\(^{3}\);
+
+\({e_{motor}}\) ~is the motor efficiency;
+
+\({\dot Q_{shaft}}\) is the fan shaft power in watts;
+
+\({\dot Q_{toair}}\) is the power entering the air in watts;
+
+\({N_{ratio}}\) is the ratio of actual fan flow rate (or speed) to maximum fan flow rate (or speed)
+
+\({h_{in}},{h_{out}}\) ~are the inlet and outlet air stream specific enthalpies in J/kg;
+
+\({w_{in}},{w_{out}}\) ~are the inlet and outlet air stream humidity ratios;
+
+\({T_{out}}\) ~is the outlet air temperature in degrees C;
+
+\(PsyTdbFnHW\) is the EnergyPlus psychrometric routine relating enthalpy and humidity ratio to temperature;
+
+\({f_{flow}}\) is the flow fraction or part-load ratio;
+
+\({f_{pl}}\) ~is the part load factor.
+
+Component Fan Model
+
+The Fan:ComponentModel object is based upon combining: modified forms of fan, belt, motor, and variable-frequency-drive (VFD) element models (Stein and Hydeman 2004); a simplified fan pressure rise model with distribution system leakage, duct static pressure, and conditioned space pressure control effects included (Sherman and Wray 2010); and a diagnostic-based simplified duct static-pressure reset (SPR) scheme for air-handling systems (Federspiel 2004, 2005).
+
+Fan \emph{electric} power depends on fan \emph{air} power (product of the airflow through and pressure rise across the fan), mechanical efficiencies (fan and belt), and electrical efficiencies (motor and drive). For systems with variable flows, none of these parameters is constant and all are interrelated. For example, Figure~\ref{fig:example-fan-performance-maps-manufacturers} shows that fan efficiency strongly depends on fan flow \emph{as well as} pressure rise, although this is not obvious from the manufacturer's power and speed performance map (top left). Fan efficiency maps can be derived from the manufacturer's performance map using a commercially-available software-based data extraction tool such as DigitizeIt and by applying the following equation to the extracted data:
+
+\({\eta_{fan}} = \frac{{\Delta {P_{fan}} \cdot {Q_{fan}}}}{{{H_{fan}}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+where \textbf{Δ}\emph{P\(_{fan}\)}is the fan pressure rise (Pa); \emph{Q\(_{fan}\)} is the fan flow at standard conditions (m\(^{3}\)/s); and \emph{H\(_{fan}\)} is the fan shaft power (W). Fan speed values also can be derived from the manufacturer's performance map using a similar software-based data extraction tool.
+
+Fan pressure rise must be sufficient to overcome the air-handling system pressure drop, which depends on duct static pressure, on duct and equipment leakage, and on pressure drops across duct and duct-like elements (e.g., dampers, fittings), coils, and filters that are connected to the fan. Duct and duct-like pressure drops increase approximately as the square of the flow through them. However, pressure drops across coils and filters behave differently: they are proportional to the flow raised to a power n, which can approach one for high-efficiency filters and wet coils (Liu et al. 2003, Trane 1999).
+
+The relation between system pressure drop and flow defines what is commonly called a ``system curve''. When system characteristics change, such as when the duct static pressure set point is varied, a family of system curves results. The intersections of these curves with fan curves (e.g., power as a function of pressure rise and flow) on a pressure versus flow plot define one or more loci of unique fan operating points. Each of these points has an associated fan efficiency, power, and speed.
+
+\begin{figure}[hbtp] % fig 208
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4888.png}
+\caption{Example Fan Performance Maps - Manufacturer’s Data from Loren Cook Company, plus Derived Static Efficiency (Three-Dimensional and Contours) (Dashed Parabolic Curve is “Do Not Select Line�) \protect \label{fig:example-fan-performance-maps-manufacturers}}
+\end{figure}
+
+\emph{Fan Pressure Rise Model}: To calculate fan pressure rise based on flow through the fan, Sherman and Wray (2010) have developed a simple physics-based data-driven four parameter duct system model for the purpose of simulating its system curve. The embodiment of the model for a fixed outdoor air fraction that can be applied to constant- or variable-volume central air-handling systems is:
+
+\(\Delta {P_{fan,tot}} = {A_{fpr}}Q_{fan}^2 + {B_{fpr}}Q_{fan}^{} + {C_{fpr}}Q_{fan}^{}\sqrt {{P_{sm}} - {P_o}} + {D_{fpr}}\left( {{P_{sm}} - {P_o}} \right)\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+where \textbf{Δ}\emph{P\(_{fan,tot}\)} is the fan total pressure rise (Pa); \emph{Q\(_{fan}\)} is the fan flow at standard conditions (m\(^{3}\)/s); \emph{P\(_{sm}\)} is the duct static pressure set point (Pa); \emph{P\(_{o}\)} is the static pressure of the spaces surrounding the ducts (Pa); and \emph{A\(_{fpr}\)}, \emph{B\(_{fpr}\)}, \emph{C\(_{fpr}\)}, and \emph{D\(_{fpr}\)} are constant coefficients that represent different aspects of the fan pressure rise model as described below.
+
+Fan static pressure rise is determined from the total pressure rise by subtracting the outlet velocity pressure:
+
+\(\Delta {P_{fan}} = \Delta {P_{fan,tot}} - \frac{\rho }{2}{\left( {\frac{{{Q_{fan}}}}{{{A_{fan,out}}}}} \right)^2}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+where \emph{A\(_{fan,out}\)} is the fan outlet area (m\(^{2}\)) and \emph{�} is the air density at the fan inlet (kg/m\(^{3}\)).
+
+The first term in Equation looks like the common system curve in which the fan pressure rise is proportional to the square of the fan flow, but here it also depends implicitly on supply and return pressure losses, and in part on the fraction of the fan flow that is outdoor air (essentially ``leaks'' into and out of the return side of the system). Very often it is the only term considered, but that would only be correct with fixed-position dampers, no distribution system leakage, no linear resistance components, and no duct static pressure control.
+
+The second term accounts for significant flow resistances in the system where the pressure difference is linearly proportional to the flow. Some filters and coils in the return may need this term to be adequately described. This term could be ignored if there are no linear components or if their pressure drops are very small compared to the other terms.
+
+The third term, which depends on the fan flow and square root of the supply duct pressure \emph{P\(_{sm}\)}, accounts in part for air leakage from the supply system when damper positions are fixed or are changed independently of static pressure or fan flow. In this case, reducing or eliminating supply leakage results in a different system curve. This, however, might be only a minor ``correction'' to the simple system curves generally used. The third term is zero when VAV box dampers are modulated to control flow. Consequently, with variable-position supply dampers, reducing or eliminating supply leakage does not change the system curve.
+
+The last term also accounts in part for leakage from the supply system when damper positions are fixed or are changed independently of static pressure or fan flow. This term indicates that the same fan pressure rise can be achieved by raising the duct pressure and closing dampers. The only change in the system in such a case is that the leakage flow may increase. The coefficient for this term is equal to one when the VAV box dampers are modulated to control flow. In both cases, this term may be the most important ``correction'' to the simple system curves generally used, especially at low flows.
+
+In principle, especially for research applications of Energy Plus, the four individual fan pressure rise coefficients can be determined using duct design calculation tools for the entire system (e.g., Right-CommDuct, UNI-DUCT, Ductsize, Varitrane Duct Designer, T-Duct). In practice, however, especially for existing buildings, the necessary details may not be known sufficiently. In that case, one can make active measurements at different combinations of fan flows, outside air fractions, damper positions (if they are variable), and duct static pressures and then use non-linear system identification techniques to fit the data and determine the coefficients. If passive measurements can be made over a sufficiently long time so that a wide range of outside air settings, damper positions, and fan flows is obtained, one could instead regress the data to find all of the parameters in the equation. Unfortunately, there are no standardized test procedures available to draw upon, even though some standards appear to be related (e.g., ASHRAE 1999, 2008). Consequently, field test protocols need to be developed to determine the parameters for the new duct system model. These protocols then need to be integrated into standardized data collection and analysis tools such as Pacific Gas and Electric's ``Universal Translator'' tool. The California Energy Commission is funding such a project; data, procedures, and tools from this project will support the EnergyPlus implementation of the fan and duct system models described here.
+
+\emph{SPR Model}: The model for duct-static-pressure reset (SPR) is based on a simple diagnostic procedure and a linear correlation between duct static pressure and supply fan airflow (Federspiel 2004, 2005). The diagnostic method involves measuring the static pressure at the duct static pressure sensor and the velocity pressure at the fan inlet (represents the fan flow) at multiple points over the fan's operating range, while the VAV box dampers attempt to control flow in response to a constant thermostat setpoint. The goal of the test is to define the lowest duct static pressure where all VAV boxes are still in control (dampers modulating). In the model, the correlation between \emph{P\(_{sm}\)} and \emph{Q\(_{fan}\)} is as follows for \emph{Q\(_{fan,min}\)} ≤ \emph{Q\(_{fan}\)} ≤ \emph{Q\(_{fan,max}\)}:
+
+\({P_{sm}} = {P_{sm,\min }} + \left( {{P_{sm,\max }} - {P_{sm,\min }}} \right)*\frac{{\left( {{Q_{fan}} - {Q_{fan,\min }}} \right)}}{{\left( {{Q_{fan,\max }} - {Q_{fan,\min }}} \right)}} = {C_1} + {C_2}*{Q_{fan}}\) ~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+Where
+
+~\({C_1} = {P_{sm,\min }} - {C_2}*{Q_{fan,\min }}\) ~and \({C_2} = \frac{{\left( {{P_{sm,\max }} - {P_{sm,\min }}} \right)}}{{\left( {{Q_{fan,\max }} - {Q_{fan,\min }}} \right)}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+For \emph{Q\(_{fan}\)} \textless{} \emph{Q\(_{fan,min}\)}, \emph{P\(_{sm}\)} = \emph{P\(_{sm,min}\)};for\emph{Q\(_{fan}\)} \textgreater{} \emph{Q\(_{fan,max}\)}, \emph{P\(_{sm}\)} = \emph{P\(_{sm,max}\)}
+
+\emph{Fan Efficiency and Shaft Input Power Model}: A dimensionless parameter in the form of an Euler number can be used to simplify the description of fan static efficiency variations:
+
+\(Eu = \frac{{\left( {\Delta {P_{fan}} * D_{fan}^4} \right)}}{{\left( {\rho * Q_{fan}^2} \right)}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+where \textbf{Δ}\emph{P\(_{fan}\)} is the fan static pressure rise (Pa), \emph{D\(_{fan}\)} is the fan wheel outer diameter (m), \emph{�} is the air density at the fan inlet (kg/m\(^{3}\)), and \emph{Q\(_{fan}\)} is the fan flow at standard conditions (m\(^{3}\)/s). \emph{Eu} is nominally the ratio of pressure forces across the fan to inertial forces at the fan wheel exit.
+
+By plotting the normalized fan static efficiency (\emph{static efficiency / maximum static efficiency}) versus the logarithm base 10 of the normalized Euler number (\emph{Eu} \emph{/} \emph{Eu} \emph{at maximum static efficiency}), the dimensionless performance of various fan sizes is very similar (as one might expect from the ``fan laws''), but so also is the dimensionless performance of different \emph{types} of fans (e.g., single-inlet plenum fans, double-inlet housed centrifugal fans, mixed flow fans, vane axial fans, fans with backward or forward curved blades). An example of this correlation for the ``normal operation'' (non-stall) and stall regions of eight fans is shown in Figure~\ref{fig:normalized-efficiency-curves-for-eight-fans}.
+
+\begin{figure}[hbtp] % fig 209
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4895.png}
+\caption{Normalized Efficiency Curves for Eight Fans in Dimensionless Space *(BC = backward curved, FC = forward curved; SI = single inlet, DI = double inlet)* \protect \label{fig:normalized-efficiency-curves-for-eight-fans}}
+\end{figure}
+
+This model uses a continuous function to represent the normalized fan efficiency (\emph{η\(_{fan}\)}) variation. The normalized exponential-conditioned skew-normal functional relationship is:
+
+\(\frac{{{\eta_{fan}}({x_{fan}})}}{{{\eta_{fan,\max }}}} = \frac{{{e^{( - 0.5*Z_1^2)}}[1 + \frac{{{Z_2}}}{{\left| {{Z_2}} \right|}} \bullet erf\left( {\frac{{\left| {{Z_2}} \right|}}{{\sqrt 2 }}} \right)}}{{{e^{( - 0.5*Z_3^2)}}[1 + \frac{{{Z_3}}}{{\left| {{Z_3}} \right|}} \bullet erf\left( {\frac{{\left| {{Z_3}} \right|}}{{\sqrt 2 }}} \right)}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+where
+
+x\(_{fan}\) = log\(_{10}\)(Eu / Eu\(_{max}\))
+
+Z\(_{1}\) = (x\(_{fan}\) - a\(_{fan}\)) / b\(_{fan}\);~ Z\(_{2}\) = ((e\(^{(c}\)fan\(^{\*x}\)fan\(^{)}\)*d\(_{fan}\)*x\(_{fan}\)) - a\(_{fan}\)) / b\(_{fan}\);~ Z\(_{3}\) = -a\(_{fan}\) / b\(_{fan}\)
+
+For conceptual design when only rough estimates are needed, a generic curve (also shown in Figure~\ref{fig:normalized-efficiency-curves-for-eight-fans}) can be used and then one only needs to know the maximum efficiency (\emph{η\(_{fan,max}\)}) and \emph{Eu} at that maximum (\emph{Eu\(_{max}\)}) to entirely model the fan efficiency and hence fan power. The dimensionless coefficients for the generic normalized fan efficiency curve are as follows:
+
+\emph{a\(_{fan}\)} = -2.732094, \emph{b\(_{fan}\)} = 2.273014,\emph{c\(_{fan}\)} = 0.196344, \emph{d\(_{fan}\)} = 5.267518
+
+In this case, the coefficient of determination R\(^{2}\) is 0.994. Also, the average and RMS differences between the efficiency values based on extracted data and the fitted generic curve are, respectively, about 0.5\% and 1.4\%; maximum differences are about ±9\%.
+
+If more accuracy is needed for a specific fan, a similarly shaped curve can be developed for that fan (using extracted data, Equation , and least-squares regression techniques), segmented into normal operation and stall regions with specific coefficients fitted for each region. Figure~\ref{fig:example-normalized-efficiency-data-for-one} shows an example, using the data from Figure~\ref{fig:example-fan-performance-maps-manufacturers}.
+
+\begin{figure}[hbtp] % fig 210
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4897.svg.png}
+\caption{Example Normalized Efficiency Data for One Fan \protect \label{fig:example-normalized-efficiency-data-for-one}}
+\end{figure}
+
+For this specific fan, the coefficients are:
+
+% table 65
+\begin{longtable}[c]{@{}lllll@{}}
+\caption{Normalized Fan Efficiency Coefficients for Specific Backward-Curved Plenum Fan \label{table:normalized-fan-efficiency-coefficients-for}} \tabularnewline
+\toprule 
+Operating Region & a & b & c & d \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Normalized Fan Efficiency Coefficients for Specific Backward-Curved Plenum Fan} \tabularnewline
+\toprule 
+Operating Region & a & b & c & d \tabularnewline
+\midrule
+\endhead
+
+Normal (Non-Stall) & 0.072613 & 0.833213 & 0 & 0.013911 \tabularnewline
+Stall & -2.354091 & 2.117493 & 0 & 2.753264 \tabularnewline
+\bottomrule
+\end{longtable}
+
+In this case, the average and RMS differences between the efficiency values based on extracted data and fitted specific curve (R\(^{2}\) is 0.999) are, respectively, about -0.1\% and 0.3\%; maximum differences are about ±0.7\%. Field tests are especially needed to determine the coefficients for installed fans because fans are susceptible to ``system effects'' (e.g., inlet obstructions) that are not included in the manufacturer test data (AMCA 1990a).
+
+To determine fan efficiency and fan shaft power at a particular time step, first calculate the fan pressure rise (\textbf{Δ}\emph{P\(_{fan}\)}) using the time step fan flow (\emph{Q\(_{fan}\)}) and Equation (and also using Equations and if there is SPR). Next, calculate \emph{Eu} using Equation and then \emph{x\(_{fan}\)} (log\(_{10}\) normalized \emph{Eu}), which is based on \emph{Eu} and the specified \emph{Eu\(_{max}\)} (\emph{Eu} at maximum efficiency) for the fan. The corresponding normalized efficiency (\emph{η\(_{fan}\)}(\emph{x\(_{fan}\)}) \emph{/ η\(_{fan,max}\)}) is obtained using Equation . The fan efficiency (\emph{η\(_{fan}\)}(\emph{x\(_{fan}\)})) therefore is:
+
+\({\eta_{fan}}\left( {{x_{fan}}} \right) = {\eta_{fan,\max }}\left[ {\frac{{{\eta_{fan}}\left( {{x_{fan}}} \right)}}{{{\eta_{fan,\max }}}}} \right]\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+The fan shaft input power (mechanical, W) is:
+
+\({H_{fan}} = \frac{{\Delta {P_{fan}} \cdot {Q_{fan}}}}{{{\eta_{fan}}\left( {{x_{fan}}} \right)}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+\emph{Fan Shaft Speed and Torque Modeling}: For rotating elements, power (\emph{H}) is the product of torque (\emph{τ}) and rotational speed (ω), or conversely, torque is power divided by rotational speed (\emph{τ = H / ω}).
+
+The Stein and Hydeman variable-frequency-drive (VFD) component model correlates VFD efficiency as a linear function of VFD fractional output power (i.e., motor input power). Available data for about 50 drives from Saftronics were apparently used to develop their model, but those data represent VFD efficiency as a function of motor fractional speed (\emph{ω\(_{motor}\) / ω\(_{motor,max}\)}, or nominally, drive output frequency divided by maximum output frequency, if motor slip is ignored).
+
+To make use of the available data, the Stein and Hydeman linear correlation must intrinsically make an assumption that motor speed and torque have some fixed relationship. Although not documented, their assumption might be the common belief that fractional torque (Ï„/ Ï„\(_{max}\)) for a motor is simply the square of its fractional speed. For fans serving duct systems with components such as filters and coils, with relatively low pressure drops elsewhere in the system, and for systems that have a non-zero controlled duct static pressure, this assumption may be inappropriate. Consequently, to make use of the available data and to avoid such assumptions, one needs to know the fraction of full speed at which fan components operate.
+
+For the fan, dimensionless flow (\emph{φ}) can be defined as (ASHRAE 1993):
+
+\(\varphi = \frac{{{Q_{fan}}}}{{{\omega_{fan}} \cdot D_{fan}^3}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+where \emph{ω\(_{fan}\)} is the fan speed (rad/s). This parameter can be calculated for each operating point on the fan manufacturer's performance map that represents fan speed as a function of flow and fan pressure rise. To simplify the data representation to a single curve (as we have done for fan efficiency), one can plot normalized dimensionless flow (dimensionless flow divided by maximum dimensionless flow, (\emph{φ}(\emph{x\(_{fan}\)}) \emph{/} \emph{φ\(_{max}\)}) as a function of the log base 10 of the normalized Euler (\emph{Eu}) parameter (\emph{x\(_{fan}\)}). Figure~\ref{fig:example-normalized-dimensionless-flow-data} shows an example plot derived from the manufacturer's data in Figure~\ref{fig:example-fan-performance-maps-manufacturers}.
+
+\begin{figure}[hbtp] % fig 211
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4901.svg.png}
+\caption{Example Normalized Dimensionless Flow Data for One Fan \protect \label{fig:example-normalized-dimensionless-flow-data}}
+\end{figure}
+
+Equation describes the sigmoidal functional form for normalized \emph{φ}:
+
+\(\frac{{\varphi \left( {{x_{fan}}} \right)}}{{{\varphi_{\max }}}} = ({A_{spd}} + {B_{spd}}/({(1 + {e^{\left[ {{{({C_{spd}} - {x_{spd}})} \mathord{\left/ {\vphantom {{({C_{spd}} - {x_{spd}})} {{D_{spd}}}}} \right. } {{D_{spd}}}}} \right]}})^{{E_{spd}}}})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+where \emph{A\(_{spd}\)}, \emph{B\(_{spd}\)}, \emph{C\(_{spd}\)}, \emph{D\(_{spd}\)}, and \emph{E\(_{spd}\)} are coefficients for the fan. Separate sets of coefficients for the normal operation and stall regions can be specified. For the curve shown in Figure~\ref{fig:example-normalized-dimensionless-flow-data}, these coefficients are:
+
+% table 66
+\begin{longtable}[c]{@{}llllll@{}}
+\caption{Dimensionless Flow Coefficients – Specific Backward-Curved Fan \label{table:dimensionless-flow-coefficients-specific}} \tabularnewline
+\toprule 
+Operating Region & A & B & C & D & E \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Dimensionless Flow Coefficients – Specific Backward-Curved Fan} \tabularnewline
+\toprule 
+Operating Region & A & B & C & D & E \tabularnewline
+\midrule
+\endhead
+
+Normal (Non-Stall) & 0 & 1.001423 & 0.123935 & -0.476026 & 1 \tabularnewline
+Stall & 0 & 5.924993 & -1.916316 & -0.851779 & 1 \tabularnewline
+\bottomrule
+\end{longtable}
+
+For a generic centrifugal fan with backward-curved blades, the coefficients are:
+
+% table 67
+\begin{longtable}[c]{@{}llllll@{}}
+\caption{Dimensionless Flow Coefficients – Generic Backward-Curved Fan \label{table:dimensionless-flow-coefficients-generic}} \tabularnewline
+\toprule 
+Operating Region & A & B & C & D & E \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Dimensionless Flow Coefficients – Generic Backward-Curved Fan} \tabularnewline
+\toprule 
+Operating Region & A & B & C & D & E \tabularnewline
+\midrule
+\endhead
+
+Normal (Non-Stall) & -0.551396 & 1.551467 & -0.442200 & -0.414006 & 0.234867 \tabularnewline
+Stall & 0.000608 & 0.586366 & 0.021775 & -0.063218 & 0.072827 \tabularnewline
+\bottomrule
+\end{longtable}
+
+For any operating point of flow (\emph{Q\(_{fan}\)}) and fan pressure rise (\textbf{Δ}\emph{P\(_{fan}\)}), one can calculate the corresponding Euler number (\emph{Eu}) for the given fan, and then determine the corresponding normalized dimensionless flow (\emph{φ}(\emph{x\(_{fan}\)}) \emph{/} \emph{φ\(_{max}\)}) from the sigmoidal dimensionless flow function (Equation ). With \emph{φ}(\emph{x\(_{fan}\)}) \emph{/} \emph{φ\(_{max}\)} determined and knowing \emph{φ\(_{max}\)} for the fan, the dimensionless flow is:
+
+\(\varphi \left( {{x_{fan}}} \right) = {\varphi_{\max }}\left[ {\frac{{\varphi \left( {{x_{fan}}} \right)}}{{{\varphi_{\max }}}}} \right]\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+With \emph{φ}(\emph{x\(_{fan}\)}) determined, the fan rotational speed (rad/s) is:
+
+\({\omega_{fan}} = \frac{{{Q_{fan}}}}{{\left( {\varphi ({x_{fan}}) * D_{fan}^3} \right)}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+Fan shaft torque (N∙m), which the belt drive must supply to the fan shaft, is then:
+
+\({\tau_{fan}} = \frac{{{H_{fan}}}}{{{\omega_{fan}}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+The fraction of full-load driven torque for the belt (\emph{Ï„\(_{fan}\) / Ï„\(_{belt,max}\)}), which is typically called ``belt load'', is thus \emph{Ï„\(_{fan}\)} divided by the belt torque capacity (\emph{Ï„\(_{belt,max}\)}). For a particular belt type and cross-section, belt torque capacity can be determined from manufacturer's information such as a shaft speed versus power chart.
+
+Ignoring belt slip, motor shaft speed (\emph{ω\(_{motor}\)}, rad/s) can then be determined using the fan speed (\emph{ω\(_{fan}\)}) and the motor/fan pulley diameter ratio (\emph{D\(_{pulley,motor}\) / D\(_{pulley,fan}\)}), which is typically called the ``drive'' ratio:
+
+\({\omega_{motor}} = \frac{{{\omega_{fan}}}}{{\left( {\frac{{{D_{pulley,motor}}}}{{{D_{pulley,fan}}}}} \right)}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+\emph{Belt, Motor, and Variable-Frequency-Drive Efficiency and Input Power Models -- Overview}: The models for belt drives, motors, and VFDs that Stein and Hydeman included in their air-handling system model represent maximum efficiency as a function of power input to the adjacent downstream component (e.g., the power input to a fan shaft by a belt drive), but they do not include part-load models. The part-load models are needed, because part-load efficiency for these components can fall off rapidly at low load (e.g., to zero at zero load) and many systems operate occasionally (and some much of the time) at low loads, in part because of current practices that result in substantial oversizing of components.
+
+\emph{Belt Efficiency and Input Power Model:} Figure~\ref{fig:belt-maximum-efficiency-vs.-fan-shaft-power} shows three maximum efficiency (\emph{η\(_{belt,max}\)}) curves for belts (low, medium, and high) as a function of maximum fan shaft torque. This set of efficiency curves is based on belt drive loss data from AMCA Publication 203 (1990b), which reportedly is an aggregation of data from over 400 tests.
+
+To determine \emph{η\(_{belt,max}\)} if data for a specific belt are not available, first use the maximum fan shaft input power (\emph{H\(_{fan,max}\)}) for the load spectrum to calculate the natural logarithm of belt power capacity:
+
+\emph{x\(_{belt,max}\) =}ln(\emph{H\(_{fan,max}\)}) with \emph{H\(_{fan,max}\)} expressed in terms of hp~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+Then, use Equations and , along with a choice of low, medium, or high efficiency coefficients from Table~\ref{table:belt-maximum-efficiency-curve-coefficients}, to calculate \emph{η\(_{belt,max}\)}.
+
+\begin{figure}[hbtp] % fig 212
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4907.svg.png}
+\caption{Belt Maximum Efficiency vs. Fan Shaft Power Input \protect \label{fig:belt-maximum-efficiency-vs.-fan-shaft-power}}
+\end{figure}
+
+The quartic polynomial curves in Figure~\ref{fig:belt-maximum-efficiency-vs.-fan-shaft-power} and their coefficients are as follows:
+
+\({\eta_{belt,\max ,\ln }} = {c_1} + {c_2} \cdot {x_{belt,\max }} + {c_3} \cdot x_{_{belt,\max }}^2 + {c_4} \cdot x_{_{belt,\max }}^3 + {c_5} \cdot x_{_{belt,\max }}^4\) ~~~~~~~~~~~~~~~~~~~ ()
+
+% table 68
+\begin{longtable}[c]{p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}}
+\caption{Belt Maximum Efficiency Curve Coefficients \label{table:belt-maximum-efficiency-curve-coefficients}} \tabularnewline
+\toprule 
+Efficiency Class (Loss) & c & c & c & c & c \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Belt Maximum Efficiency Curve Coefficients} \tabularnewline
+\toprule 
+Efficiency Class (Loss) & c & c & c & c & c \tabularnewline
+\midrule
+\endhead
+
+High (Low Loss) & -6.502E-2 & 2.475E-2 & -6.841E-3 & 9.383E-4 & -5.168E-5 \tabularnewline
+Medium (Medium Loss) & -9.504E-2 & 3.415E-2 & -8.897E-3 & 1.159E-3 & -6.132E-5 \tabularnewline
+Low (High Loss) & -1.422E-1 & 5.112E-2 & -1.353E-2 & 1.814E-3 & -9.909E-5 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The belt maximum efficiency is therefore:
+
+\({\eta_{belt,\max }} = {e^{{\eta_{belt,\max ,\ln }}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+The normalized \emph{part-load} belt efficiency model is provided to modify the maximum efficiency of the belt. This model is based on part-load data for belts in ACEEE's handbook on motor systems (Nadel et al. 2002). To determine the normalized belt efficiency at part-load (\emph{η\(_{belt}\)}(\emph{x\(_{belt}\)})/* η\(_{belt,max}\)\emph{), use the fan shaft (belt output) fractional torque (}x\(_{belt}\)* = \emph{τ\(_{belt}\)} / \emph{τ\(_{belt,max;}\) τ\(_{belt}\) = τ\(_{fan}\)}) as the belt fractional load in Equation or (select the equation for the region that contains \emph{x\(_{belt}\)}) and use coefficients from Table~\ref{table:belt-normalized-efficiency-curve-coefficients} that correspond to that region and the belt type: V-Belt or synchronous (toothed). Figure~\ref{fig:belt-normalized-efficiency-vs.-belt} shows a graphical representation of the curves defined by these equations and coefficients.
+
+\begin{figure}[hbtp] % fig 213
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4910.svg.png}
+\caption{Belt Normalized Efficiency vs. Belt Fractional Load) \protect \label{fig:belt-normalized-efficiency-vs.-belt}}
+\end{figure}
+
+The belt normalized (part-load) efficiency curves in Figure~\ref{fig:belt-normalized-efficiency-vs.-belt} for Regions 1 and 3 (single rectangular hyperbola type 2) and Region 2 (exponential decay), respectively, and their coefficients are as follows:
+
+Region 1 (0 \textless{} = \emph{x\(_{belt}\)} \textless{} \emph{x\(_{belt,trans}\)}) and Region 3 (\emph{x\(_{belt}\)} \textgreater{} 1):
+
+\(\frac{{{\eta_{belt}}({x_{belt}})}}{{{\eta_{belt,\max }}}} = \left[ {\frac{{{a_{belt}} \cdot {x_{belt}}}}{{{b_{belt}} + {x_{belt}}}}} \right] + {c_{belt}} \cdot {x_{belt}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+Region 2 (\emph{x\(_{belt,trans}\)} \textless{} = \emph{x\(_{belt}\)} \textless{} = 1):
+
+\(\frac{{{\eta_{belt}}({x_{belt}})}}{{{\eta_{belt,\max }}}} = {a_{belt}} + {b_{belt}} \cdot {e^{\left( {{c_{belt}} \cdot {x_{belt}}} \right)}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+where x\(_{belt}\) = \(\tau\) \(_{belt}\) / \(\tau\) \(_{belt,max}\)
+
+Belt efficiency therefore is:
+
+\({\eta_{belt}}({x_{belt}}) = {\eta_{belt,\max }}\left[ {\frac{{{\eta_{belt}}({x_{belt}})}}{{{\eta_{belt,\max }}}}} \right]\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+Belt input power (mechanical, W) at the motor shaft is:
+
+\({H_{belt}} = \frac{{{H_{fan}}}}{{{\eta_{belt}}({x_{belt}})}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+% table 69
+\begin{longtable}[l]{@{}llllll@{}}
+\caption{Belt Normalized Efficiency Curve Coefficients \label{table:belt-normalized-efficiency-curve-coefficients}} \tabularnewline
+\toprule 
+Belt Type & x\(_{belt,trans}\) & Region & a\(_{belt}\) & b\(_{belt}\) & c\(_{belt}\) \tabularnewline \midrule
+\midrule
+\endfirsthead
+
+\caption[]{Belt Normalized Efficiency Curve Coefficients} \tabularnewline
+\toprule 
+Belt Type & x\(_{belt,trans}\) & Region & a\(_{belt}\) & b\(_{belt}\) & c\(_{belt}\) \tabularnewline \midrule
+\midrule
+\endhead
+
+V-Belt & 0.167 & 1 & 0.920797 & 0.026269 & 0.151594 \tabularnewline
+ & & 2 & 1.011965 & -0.339038 & -3.43626 \tabularnewline
+ & & 3 & 1.037778 & 0.010307 & -0.026815 \tabularnewline
+Synchronous & 0.137 & 1 & 0.982167 & 0.049135 & 0.158164 \tabularnewline
+ & & 2 & 1.002134 & -0.531885 & -5.295707 \tabularnewline
+ & & 3 & 1 & 0 & 0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\emph{Motor Efficiency and Input Power Model:} Figure~\ref{fig:maximum-motor-efficiency-vs.-belt-power-input} shows three maximum efficiency (\emph{η\(_{motor,max}\)}) curves for motors (low, medium, and high) as a function of rated motor output power (belt input power). This set of efficiency curves is based on maximum efficiency data in DOE's MotorMaster+ database (2003) from about 800 tests. It is provided for use in the absence of manufacturer's data.
+
+\begin{figure}[hbtp] % fig 214
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4917.svg.png}
+\caption{Maximum Motor Efficiency vs. Belt Power Input (Motor Output) \protect \label{fig:maximum-motor-efficiency-vs.-belt-power-input}}
+\end{figure}
+
+To determine \emph{η\(_{motor,max}\)} if data for a specific motor are not available (e.g., as listed in Table~\ref{table:example-motor-normalized-efficiency-curve}), first use the maximum belt input power (\emph{H\(_{belt,max}\)}) for the load spectrum (multiplied by whatever oversizing factor may be desired) to calculate the natural logarithm of belt power capacity:
+
+\emph{x\(_{motor,max}\) =}ln(\emph{H\(_{belt,max}\)}) with \emph{H\(_{belt,max}\)} expressed in terms of hp~~~~~~~~~~~~~~~~~~~~ ()
+
+Then, use Equation , along with a choice of low, medium, or high efficiency coefficients from Table~\ref{table:motor-maximum-efficiency-curve-coefficients}, to calculate \emph{η\(_{motor,max}\)}.
+
+The maximum motor efficiency curves in Figure~\ref{fig:maximum-motor-efficiency-vs.-belt-power-input} (single rectangular hyperbola type 1) and their coefficients are as follows:
+
+\({\eta_{motor,\max }} = \left[ {\frac{{{a_{motor,\max }} \cdot {x_{motor,\max }}}}{{{b_{motor,\max }} + {x_{motor,\max }}}}} \right] + {c_{motor,\max }}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+% table 70
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Motor Maximum Efficiency Curve Coefficients \label{table:motor-maximum-efficiency-curve-coefficients}} \tabularnewline
+\toprule 
+Case & a & b & c \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Motor Maximum Efficiency Curve Coefficients} \tabularnewline
+\toprule 
+Case & a & b & c \tabularnewline
+\midrule
+\endhead
+
+High-Efficiency & 0.196205 & 3.653654 & 0.839926 \tabularnewline
+Mid-Efficiency & 0.292280 & 3.368739 & 0.762471 \tabularnewline
+Low-Efficiency & 0.395895 & 3.065240 & 0.674321 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The normalized \emph{part-load} motor efficiency model is provided to modify the maximum efficiency of the motor. This model is based on part-load data for motors from DOE's MotorMaster+ database (2003). To determine the normalized motor efficiency at part-load (\emph{η\(_{motor}\)}(\emph{x\(_{motor}\)})/* η\(_{motor,max}\)\emph{), use the motor fractional power output (}x\(_{motor}\) = H\(_{belt}\)* / \emph{H\(_{belt,max}\)}) as the fraction of motor output power in Equation and use coefficients from Table~\ref{table:example-motor-normalized-efficiency-curve}, or for a specific motor, determined from DOE MotorMaster+ data or from manufacturer's data. Figure~\ref{fig:motor-normalized-efficiency-vs.-motor-load} shows a graphical representation of eight example curves defined by these equations and coefficients.
+
+\begin{figure}[hbtp] % fig 215
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4919.svg.png}
+\caption{Motor Normalized Efficiency vs. Motor Load Fraction \protect \label{fig:motor-normalized-efficiency-vs.-motor-load}}
+\end{figure}
+
+The example motor normalized efficiency curves (single rectangular hyperbola type 2) and their coefficients as a function of motor load fraction in Figure~\ref{fig:motor-normalized-efficiency-vs.-motor-load} are determined from DOE MotorMaster+ data and are as follows:
+
+\(\frac{{{\eta_{motor}}({x_{motor}})}}{{{\eta_{motor,\max }}}} = \left[ {\frac{{{a_{PLmotor}} \cdot {x_{motor}}}}{{{b_{PLmotor}} + {x_{motor}}}}} \right] + {c_{PLmotor}} \cdot {x_{motor}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+% table 71
+\begin{longtable}[c]{p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}}
+\caption{Example Motor Normalized Efficiency Curve Coefficients \label{table:example-motor-normalized-efficiency-curve}} \tabularnewline
+\toprule 
+Poles & Motor Rated Output (hp) & Maximum Efficiency & a\(_{Plmotor}\) & b\(_{Plmotor}\) & c\(_{Plmotor}\) \tabularnewline \midrule
+\midrule
+\endfirsthead
+
+\caption[]{Example Motor Normalized Efficiency Curve Coefficients} \tabularnewline
+\toprule 
+Poles & Motor Rated Output (hp) & Maximum Efficiency & a\(_{Plmotor}\) & b\(_{Plmotor}\) & c\(_{Plmotor}\) \tabularnewline \midrule
+\midrule
+\endhead
+
+8 & 1 & 0.6675 & 1.096694 & 0.097126 & 0.002011 \tabularnewline
+4 & 1 & 0.7787 & 1.092165 & 0.08206 & -0.0072 \tabularnewline
+ & 5 & 0.84 & 1.223684 & 0.08467 & -0.135186 \tabularnewline
+ & 10 & 0.8745 & 1.146258 & 0.045766 & -0.110367 \tabularnewline
+ & 25 & 0.8991 & 1.137209 & 0.050236 & -0.08915 \tabularnewline
+ & 50 & 0.9129 & 1.088803 & 0.029753 & -0.064058 \tabularnewline
+ & 75 & 0.9259 & 1.07714 & 0.029005 & -0.04935 \tabularnewline
+ & 100 & 0.9499 & 1.035294 & 0.012948 & -0.024708 \tabularnewline
+ & 125 & 0.9527 & 1.030968 & 0.010696 & -0.023514 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Motor efficiency therefore is:
+
+\({\eta_{motor}}({x_{motor}}) = {\eta_{motor,\max }}\left[ {\frac{{{\eta_{motor}}({x_{motor}})}}{{{\eta_{motor,\max }}}}} \right]\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+Motor input power (electrical, W) is:
+
+\({H_{motor}} = \frac{{{H_{belt}}}}{{{\eta_{motor}}({x_{motor}})}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+\emph{VFD Efficiency and Input Power Model:} For VFDs, published performance data are limited. Data from DOE (2008) suggest using a functional relation similar to that used for motors to represent VFD efficiency (\emph{η\(_{VFD}\)}) as a function of the fraction of full-load motor input power (\emph{x\(_{VFD}\) = H\(_{motor}\)} / \emph{H\(_{motor,max}\)}), as shown in Figure~\ref{fig:vfd-efficiency-vs.-fraction-of-motor-full}, or as a function of the fraction of full-load speed (\emph{x\(_{VFD}\) = ω\(_{motor}\) / ω\(_{motor,max}\)}), as shown in Figure~\ref{fig:vfd-efficiency-vs.-fraction-of-full-load}.
+
+\begin{figure}[hbtp] % fig 216
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4923.svg.png}
+\caption{VFD Efficiency vs. Fraction of Motor Full-Load Input Power (*Source: DOE 2008*) \protect \label{fig:vfd-efficiency-vs.-fraction-of-motor-full}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 217
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4924.svg.png}
+\caption{VFD Efficiency vs. Fraction of Full-Load Motor Speed (*Courtesy of Saftronics*) \protect \label{fig:vfd-efficiency-vs.-fraction-of-full-load}}
+\end{figure}
+
+The performance curve (single rectangular hyperbola type 2) used here for VFD efficiency is:
+
+\({\eta_{VFD}} = \left[ {\frac{{{a_{VFD}} \cdot {x_{VFD}}}}{{{b_{VFD}} + {x_{VFD}}}}} \right] + {c_{VFD}} \cdot {x_{VFD}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+Example coefficients derived from the DOE data as a function of the fraction of full-load motor input power are listed in Table~\ref{table:example-vfd-efficiency-curve-coefficients}.
+
+% table 72
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Example VFD Efficiency Curve Coefficients \label{table:example-vfd-efficiency-curve-coefficients}} \tabularnewline
+\toprule 
+VFD Rated Output Power (hp) & a\(_{vfd}\) & b\(_{vfd}\) & c\(_{vfd}\) \tabularnewline \midrule
+\midrule
+\endfirsthead
+
+\caption[]{Example VFD Efficiency Curve Coefficients} \tabularnewline
+\toprule 
+VFD Rated Output Power (hp) & a\(_{vfd}\) & b\(_{vfd}\) & c\(_{vfd}\) \tabularnewline \midrule
+\midrule
+\endhead
+
+3 & 0.978856 & 0.034247 & -0.007862 \tabularnewline
+5 & 0.977485 & 0.028413 & -0.002733 \tabularnewline
+10 & 0.978715 & 0.022227 & 0.001941 \tabularnewline
+20 & 0.984973 & 0.017545 & -0.000475 \tabularnewline
+30 & 0.987405 & 0.015536 & -0.005937 \tabularnewline
+50 & 0.987910 & 0.018376 & -0.001692 \tabularnewline
+60 & 0.971904 & 0.014537 & 0.011849 \tabularnewline
+75 & 0.991874 & 0.017897 & -0.001301 \tabularnewline
+100 & 0.982384 & 0.012598 & 0.001405 \tabularnewline
+>= 200 & 0.984476 & 0.009828 & -0.004560 \tabularnewline
+\bottomrule
+\end{longtable}
+
+VFD input power (electrical, W) is:
+
+\({H_{VFD}} = \frac{{{H_{motor}}}}{{{\eta_{VFD}}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+\emph{System Total Efficiency: T}he combined efficiency of the fan system components (i.e., fan, belt, motor, and VFD) is:
+
+\({\eta_{TOTAL}} = {\eta_{fan}} \cdot {\eta_{belt}} \cdot {\eta_{motor}} \cdot {\eta_{VFD}}\) ~~~ \(\left( { = \frac{{{Q_{fan}} \cdot \Delta {P_{fan}}}}{{{H_{VFD}}}}} \right)\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+\emph{Heat Loss to Air}: To calculate the temperature rise from waste heat entering the air stream from the fan, belt, and motor, it is assumed that the user-specified ``motor in air fraction'' applies to the belt and motor but not to the VFD. The power ``lost'' to the air (W) is:
+
+\({\dot Q_{toair}} = {H_{fan}} + \left( {{H_{motor}} - {H_{fan}}} \right) \cdot {f_{motortoair}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ()
+
+\subsection{References}\label{references-002}
+
+AMCA. 1990a. ``Fans and Systems''. Publication 201-90. Arlington Heights, IL: Air Movement and Control Association International.
+
+AMCA. 1990b. ``Field Performance Measurement of Fan Systems''. Publication 203-90. Arlington Heights, IL: Air Movement and Control Association International.
+
+ASHRAE. 1993. HVAC 2 Toolkit: Algorithms and Subroutines for Secondary HVAC System Energy Calculations. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 1999. ``ANSI/ASHRAE Standard 120 Method of Testing to Determine Flow Resistance of HVAC Ducts and Fittings''. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2008. ``ANSI/ASHRAE Standard 126 Method of Testing HVAC Air Ducts and Fittings''. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+DOE. 2003. ``MotorMaster 4.0 User Guide''. U.S. Department of Energy, Industrial Technologies Program.
+
+DOE. 2008. ``Energy Tips -- Motor: Motor Tip Sheet \#11''. U.S. Department of Energy, Industrial Technologies Program. June.
+
+Federspiel, C. 2004. ``Detecting Optimal Fan Pressure''. Final Report of Federspiel Controls to the CEC Energy Innovations Small Grant Program. Grant \#: 02-03.
+
+Federspiel, C. 2005. ``Detecting Critical Supply Duct Pressure''. ASHRAE Transactions, Vol. 111, Part 1. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Heredos, Francis P. 1987. Selection and Application of Multispeed Motors, IEEE Transactions on Industry Applications, Vol. 1A-23, No. 2, March/April.
+
+Liu, M., D.E. Claridge, and S. Deng. 2003. ``An Air Filter Pressure Loss Model for Fan Energy Calculation in Air-Handling Units''. International Journal of Energy Research. Vol. 27, pp.~589-600.
+
+Nadel, S., R.N. Elliot, M. Shepard, S. Greenberg, G. Katz, and A.T. de Almeida. 2002. ``Energy-Efficient Motor Systems: A Handbook on Technology, Program, and Policy Opportunities'' 2nd Edition. Washington, DC: American Council for an Energy Efficient Economy. p.188.
+
+Sherman, M.H. and C.P. Wray. 2010. ``Parametric System Curves: Correlations Between Fan Pressure Rise and Flow for Large Commercial Buildings''. Lawrence Berkeley National Laboratory Report, LBNL-3542E.
+
+Stein, J. and M.M. Hydeman. 2004. ``Development and Testing of the Characteristic Curve Fan Model''. ASHRAE Transactions, Vol. 110, Part 1. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Trane. 1999. ``Delta-Flo Coils: Data Catalog PL-AH-COIL-000-D-2-799''. LaCrosse, WI: The Trane Company. July.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-humidifiers.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-humidifiers.tex
new file mode 100644
index 00000000000..73a186bcce0
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/air-system-humidifiers.tex
@@ -0,0 +1,277 @@
+\section{Air System Humidifiers }\label{air-system-humidifiers}
+
+\subsection{Overview}\label{overview-003}
+
+Air system humidifiers are components that add moisture to the supply air stream. They fall into 2 broad categories: spray type humidifiers which act like direct evaporative coolers, cooling the supply air as well as humidifying it; and dry steam humidifiers, which humidify the supply air stream while causing almost no change to the supply air stream temperature. The EnergyPlus electric and gas fired steam humidifier uses electrical energy and thermal energy, respectively, to convert ordinary tap water to steam which it then injects into the supply air stream by means of a blower fan. The actual electric dry steam unit might be an electrode-type humidifier or a resistance-type humidifier.
+
+\subsection{Electric and Gas Steam Humidifier}\label{electric-and-gas-steam-humidifier}
+
+The electric and gas steam humidifier models (object names: Humidifier:Steam:Electric and Humidifier:Steam:Gas) are based on moisture and enthalpy balance equations plus standard psychrometric relationships. The approach is similar to that taken in the ASHRAE HVAC 2 Toolkit, page 4-112 (ASHRAE 1993). EnergyPlus contains its own module of psychrometric routines; the psychrometric theory and relations are given in the 2001 edition of ASHRAE Fundamentals, Chapter 6 (ASHRAE 2001). The model contains both an ideal controller and the component. The control model assumes that there is a minimum humidity setpoint on the component air outlet node. This setpoint is established by a setpoint manager described elsewhere.
+
+\subsubsection{Model}\label{model-001}
+
+The component model is a forward model: its inputs are its inlet conditions; its outputs are its outlet conditions and its energy consumption. The inputs are the temperature, humidity ratio, and mass flow rate of the inlet air stream, which are known; and the water addition rate (kg/s) which is determined by the controller. The moisture mass balance and psychometric calculations are identical for both gas and electric dry steam humidifiers. The only difference is how a heat source (electric or gas) is used to generate the steam.
+
+\subsubsection{Controller}\label{controller}
+
+The controller first decides whether the humidifier is on or off. For the humidifier to be on:
+
+*~the humidifier schedule value must be nonzero;
+
+*~the inlet air mass flow must be greater than zero;
+
+*~the inlet air humidity ratio must be less than the minimum humidity ratio setpoint.
+
+If the humidifier is off, the water addition rate is set to zero. If the humidifier is on, the water addition rate needed to meet the humidity setpoint is calculated.
+
+\begin{equation}
+{\dot m_a} \cdot {w_{in}} + {\dot m_{w,add,needed}} = {\dot m_a} \cdot {w_{set}}
+\end{equation}
+
+where
+
+\({\dot m_a}\) ~ = the air mass flow rate {[}kg/s{]}
+
+\({w_{in}}\) = the inlet air humidity ratio {[}kg/kg{]}
+
+\({\dot m_{w,add,needed}}\) ~ = water addition rate needed to meet the setpoint {[}kg/s{]}
+
+\({w_{set}}\) = the humidity ratio setpoint {[}kg/kg{]}
+
+Equation is the moisture balance equation for the component. It is solved for \({\dot m_{w,add,needed}}\) ~(the other variables are known) which is passed to the humidifier component model as its desired inlet water addition rate.
+
+\subsubsection{Component}\label{component}
+
+The inputs to the component model are the air inlet conditions and mass flow rate and the water addition rate set by the controller. The outputs are the air outlet conditions. First the desired water addition rate is checked against component capacity.
+
+\begin{equation}
+{\dot m_{w,add,needed,{\rm{max}}}} = Min({\dot m_{w,add}},Ca{p_{nom}})
+\end{equation}
+
+where
+
+\(Ca{p_{nom}}\) ~ = the humidifier nominal capacity {[}kg/s{]}, a user input.
+
+If \({\dot m_{w,add,needed,{\rm{max}}}}\) ~is zero, the outlet conditions are set to the inlet conditions and the water addition rate is set to zero. If the humidifier is scheduled on the component power consumption is set to the standby power consumption: \({W_{hum}} = {W_{stby}}\) . Otherwise \({W_{hum}}\) ~ = 0.
+
+If \({\dot m_{w,add,needed,{\rm{max}}}}\) ~\textgreater{} 0, then the moisture and enthalpy balance equations
+
+\begin{equation}
+{\dot m_a} \cdot {w_{in}} + {\dot m_w} = {\dot m_a} \cdot {w_{out}}
+\end{equation}
+
+\begin{equation}
+{\dot m_a} \cdot {h_{in}} + {\dot m_w} \cdot {h_w} = {\dot m_a} \cdot {h_{out}}
+\end{equation}
+
+with \({\dot m_w}\) ~set equal to \({\dot m_{w,add,needed,{\rm{max}}}}\) ~are solved for \({w_{out}}\) ~and \({h_{out}}\) . Here
+
+\({\dot m_a}\) ~ = the air mass flow rate {[}kg/s{]}
+
+\({w_{in}}\) = the inlet air humidity ratio {[}kg/kg{]}
+
+\({\dot m_w}\) ~ = the inlet water addition rate {[}kg/s{]}
+
+\({w_{out}}\) ~ = the outlet air humidity ratio {[}kg/kg{]}
+
+\({h_{in}}\) ~ = the inlet air specific enthalpy {[}J/kg{]}
+
+\({h_w}\) ~ = the steam specific enthalpy = 2676125.~ {[}J/kg{]} at 100 \(^{o}\)C
+
+\({h_{out}}\) ~ = the outlet air specific enthalpy {[}J/kg{]}
+
+The outlet temperature is obtained from
+
+\begin{equation}
+{T_{out}} = PsyHFnTdbW({h_{out}},{w_{out}})
+\end{equation}
+
+where
+
+\({T_{out}}\) ~ = outlet air temperature {[}\(^{o}\)C{]},
+
+\(PsyHFnTdbW({h_{out}},{w_{out}})\) ~is an EnergyPlus psychrometric function.
+
+The humidity ratio at saturation at the outlet temperature is
+
+\begin{equation}
+{w_{out,sat}} = PsyWFnTdbRhPb({T_{out}},1.0,{P_{atmo}})
+\end{equation}
+
+where
+
+\({P_{atmo}}\) ~ = the barometric pressure {[}Pa{]},
+
+1.0 is the relative humidity at saturation,
+
+\(PsyWFnTdbRhPb\) ~is an EnergyPlus psychrometric function.
+
+IF \({w_{out}} \le {w_{out,sat}}\) ~then the outlet condition is below the saturation curve and the desired moisture addition rate can be met. \({\dot m_{w,add}}\) ~is set to \({\dot m_{w,add,needed,{\rm{max}}}}\) ~and the calculation of outlet conditions is done. But if \({w_{out}} > {w_{out,sat}}\) ~then it is assumed that this condition will be detected and the steam addition rate throttled back to bring the outlet conditions back to the saturation condition. We need to find the point where the line drawn between state 1 (inlet) and state 2 (our desired outlet) crosses the saturation curve. This will be the new outlet condition. Rather than iterate to obtain this point, we find it approximately by solving for the point where 2 lines cross: the first drawn from state 1 to state 2, the second from \({T_1}\) , \({w_{1,sat}}\) ~to \({T_2}\) , \({w_{2,sat}}\) ; where
+
+\({w_{1,sat}}\) ~is the inlet temperature {[}\(^{o}\)C{]},
+
+\({w_{2,sat}}\) ~is the humidity ratio at saturation at temperature \({w_{1,sat}}\) ~{[}kg/kg{]},
+
+\({T_2}\) ~is the desired outlet temperature {[}\(^{o}\)C{]},
+
+\({w_{2,sat}}\) ~is the humidity ratio at saturation at temperature \({T_2}\) ~{[}kg/kg{]}.
+
+The 2 lines are given by the equations:
+
+\begin{equation}
+w = {w_1} + (({w_2} - {w_1})/({T_2} - {T_1})) \cdot (T - {T_1})
+\end{equation}
+
+\begin{equation}
+w = {w_{1,sat}} + (({w_{2,sat}} - {w_{1,sat}})/({T_2} - {T_1})) \cdot (T - {T_1})
+\end{equation}
+
+Solving for the point (state 3) where the lines cross:
+
+\begin{equation}
+{w_3} = {w_1} + (({w_2} - {w_1}) \cdot ({w_{1,sat}} - {w_1}))/({w_2} - {w_{2,sat}} + {w_{1,sat}} - {w_1})
+\end{equation}
+
+\begin{equation}
+{T_3} = {T_1} + ({w_3} - {w_1}) \cdot (({T_2} - {T_1})/({w_2} - {w_1}))
+\end{equation}
+
+This point isn't quite on the saturation curve since we made a linear approximation of the curve, but the temperature should be very close to the correct outlet temperature. We will use this temperature as the outlet temperature and move to the saturation curve for the outlet humidity and enthalpy. Thus we set \({T_{out}}\) ~ = \({T_3}\) ~and
+
+\begin{equation}
+{w_{out}} = PsyWFnTdbRhPb({T_{out}},1.0,{P_{atmo}})
+\end{equation}
+
+\begin{equation}
+{h_{out}} = PsyHFnTdbW({T_{out}},{w_{out}})
+\end{equation}
+
+where \(PsyHFnTdbW\) ~is an EnergyPlus psychrometric function. The water addition rate is set to
+
+\begin{equation}
+{\dot m_{w,add}} = {\dot m_a} \cdot ({w_{out}} - {w_{in}})
+\end{equation}
+
+We now have the outlet conditions and the adjusted steam addition rate for the case where the desired outlet humidity results in an outlet state above the saturation curve. The energy consumption of the electric and gas steam humidifiers is calculated separately.
+
+The electric steam humidifier electric consumption is given by
+
+\begin{equation}
+{W_{hum}} = ({\dot m_{w,add}}/Ca{p_{nom}}) \cdot {W_{nom}} + {W_{fan}} + {W_{stby}}
+\end{equation}
+
+where
+
+\({W_{fan}}\) ~ = nominal fan power {[}W{]}, a user input,
+
+\({W_{stby}}\) ~ = standby power {[}W{]}, a user input.
+
+The gas steam humidifier performance calculation is done for fixed and variable entering water temperature. The calculation procedure for fixed and variable entering water temperature are as follows.
+
+\subsubsection{Fixed Inlet WaterTemperature:}\label{fixed-inlet-watertemperature}
+
+The gas steam humidifier gas consumption rate for fixed entering water temperature is given by:
+
+\begin{equation}
+\dot{Q}_{NG} = \frac{\dot{m}_{w,add}}{\dot{m}_{cap,nom}}Q_{NG,nom}
+\end{equation}
+
+The actual gas use rate accounting for gas fired humidifier thermal efficiency variation with part load ratio is given by:
+
+\begin{equation}
+Q_{NG} = \dot{Q}_{NG}\frac{\eta_{rated}}{\eta_{actual}}
+\end{equation}
+
+\begin{equation}
+\eta_{actual} = \eta_{rated} \times \rm{EffModCurveValue}\left(PLR\right)
+\end{equation}
+
+\begin{equation}
+\rm{PLR} = \frac{\dot{Q}_{NG}}{Q_{NG,nom}}
+\end{equation}
+
+where, EffModCurveValue = thermal efficiency modifier curve value as function of part load ratio. This curve is generated from manufacturer's part load performance data. PLR = part load ratio, (-). Q\_NG\_nom = nominal or rated gas use rate, (Watts). Q\_NG = actual gas use rate, (Watts). eta\_rated = nominal or rated thermal efficiency of gas fired steam humidifier, (-) eta\_actual = actual thermal efficiency of gas fired steam humidifier accounting for part load performance, (-).
+
+\subsubsection{Variable Inlet WaterTemperature:}\label{variable-inlet-watertemperature}
+
+The gas use rate is determined from the theoretical gas input rate and actual thermal efficiency. The actual thermal efficiency is the rated thermal efficiency corrected for part load ratio operation. At steady state the gas use rate is given by:
+
+\begin{equation}
+Q_{NG} = \frac{\dot{m}_w \left(h_{fg}+c_{p,w}\left(100-T_{w,inlet}\right)\right)}{\eta_{rated}}
+\end{equation}
+
+\begin{equation}
+\rm{PLR} = \frac{\dot{Q}_{NG}}{Q_{NG,nom}}
+\end{equation}
+
+\begin{equation}
+\eta_{actual} = \eta_{rated} \times \rm{EffModCurveValue}\left(PLR\right)
+\end{equation}
+
+\begin{equation}
+Q_{NG} = \dot{Q}_{NG}\frac{\eta_{rated}}{\eta_{actual}}
+\end{equation}
+
+where, T\_w\_inlet = temperature of water entering the gas steam humidifier, °C. This value depends on the water source.
+
+If the rated gas use rated input field is not autosized, then user specified thermal efficiency will be overridden with a value calculated from user specified rated gas use rate, nominal capacity (m3/s) and design conditions as follows:
+
+\begin{equation}
+ \eta_{rated} = \frac{\dot{V}_{cap,nom} \rho_w \PB{h_{fg}+c_{p,w}\Delta T_w}}{Q_{NG,nom}}
+\end{equation}
+
+The gas steam humidifier requires electric power input to the blower fan and associated control units. The auxiliary electric power input rate of the gas steam humidifier is given by:
+
+\begin{equation}
+W_{aux} = W_{fan} + W_{controls}
+\end{equation}
+
+where W\_fan = nominal fan power {[}W{]}, a user input, W\_controls = control electric power {[}W{]}, a user input.
+
+The water consumption rate is, in m3/s, for electric and steam humidifier at a reference temperature of 5.05 C is given by.
+
+\begin{equation}
+{\dot V_{cons}} = {\dot m_{w,add}}/{\rho_w}
+\end{equation}
+
+where
+
+\({\dot V_{cons}}\) ~ = the water consumption rate {[}m\(^{3}\){]},
+
+\({\rho_w}\) ~ = water density (998.2 kg/m\(^{3}\)).
+
+\subsubsection{References}\label{references-003}
+
+ASHRAE. 1993. HVAC 2 Toolkit: A Toolkit for Secondary HVAC System Energy Calculations. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2001. 2001 ASHRAE Handbook Fundamentals. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+  Simulation Models -- Encyclopedic Reference = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+
+The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of ``Heat Balance'', ``HVAC'', and ``Plant''.~ With the integrated solution, these designations signify where the effects of these models have their first impacts.
+
+Main Sections:
+
+\begin{itemize}
+\tightlist
+\item
+  \protect\hyperlink{ZoneGains}{Zone Internal Gains}
+\item
+  \protect\hyperlink{IndoorSwimmingPool}{Indoor Swimming Pool}
+\item
+  \protect\hyperlink{Pipes}{Pipes}
+\item
+  \protect\hyperlink{Pumps}{Pumps}
+\item
+  \protect\hyperlink{IdealLoads}{Ideal Loads Air System}
+\item
+  \protect\hyperlink{DistrictCooling}{District Cooling}
+\item
+  \protect\hyperlink{DistrictHeating}{District Heating}
+\item
+  \protect\hyperlink{CentralHeatPumpSystem}{CentralHeatPumpSystem}
+\item
+  \protect\hyperlink{ChillerHeater}{ChillerHeater}
+\item
+  \protect\hyperlink{PlantComponents}{Plant Temperature Source Component} 
+\end{itemize}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/baseboard-heaters.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/baseboard-heaters.tex
new file mode 100644
index 00000000000..bafc4e23c8d
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/baseboard-heaters.tex
@@ -0,0 +1,213 @@
+\section{Baseboard Heaters }\label{baseboard-heaters}
+
+\subsection{Hot Water Baseboard Heater with Only Convection}\label{hot-water-baseboard-heater-with-only-convection}
+
+\subsubsection{Overview}\label{overview-006}
+
+The convective water baseboard heater (Ref. ZoneHVAC:Baseboard:Convective:Water) is a simple model for establishing a convective-only heat addition to a space through a baseboard heater.~ In most situations, the baseboard heater does give a significant amount of heat off via natural convection, but some heat is given off via radiation.~ In this model, the radiant component is ignored and all heat is assumed to be delivered to the space via convection.~ The baseboard heater is supplied with hot water from the primary system which is circulated through the inside of a finned tube within the space.~ Heat is transferred from the water inside the pipe, through the tube and fins, and eventually convected to the surrounding air within the space.~ EnergyPlus then assumes that this heat is evenly spread throughout the space thus having an immediate impact on the zone air heat balance which is used to calculate the mean air temperature (MAT) within the space.
+
+The model requests an effective UA value to handle the heat exchange between the water loop and the zone air.~ From there, it employs an effectiveness-NTU heat exchanger model to determine the heat transfer between the water and the zone air.~ This is necessary because during the simulation only the inlet water and ``inlet air'' (assumed to be zone air) is known.~ As a result, the effectiveness-NTU heat exchanger methodology is better suited to determine the performance of the system.
+
+\subsubsection{Model Description}\label{model-description-003}
+
+\subsubsection{Convective Water Baseboard Heater Inputs}\label{convective-water-baseboard-heater-inputs}
+
+Like many other HVAC components, the convective-only water baseboard model requires a unique identifying name, an availability schedule, and water side inlet and outlet nodes.~ These define the availability of the unit for providing condition to the space and the node connections that relate to the primary system.~ In addition, a convergence tolerance is requested of the user to help define the ability of the local controls to tightly control the system output.~ In almost all cases, the user should simply accept the default value for the convergence tolerance unless engaged in an expert study of controls logic in EnergyPlus.
+
+The input also requires a UA value and a maximum design flow rate for the unit.~ Both of these parameters can be chosen to be auto-sized by EnergyPlus.~ The UA value corresponds to the convective heat transfer from the water to the tube, the conduction through the tube and fin material, and the natural convection from the tube/fins to the zone air.~ The maximum flow rate and UA value define the performance and maximum output of the baseboard unit.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-000}
+
+The simulation of the convective water baseboard unit follows standard effectiveness-NTU methodology.~ It begins by calculating the product of the specific heat and mass flow rate for both the air and water sides of the unit (heat exchanger).~ In the initialization of the model, it is assumed that the air mass flow rate is equal to 2.0 times the water mass flow rate.~ The purpose of this calculation is to provide some reasonable estimate of the air mass flow rate so that the model can calculate system performance correctly.~ This calculation is kept constant throughout the rest of the simulation.
+
+Each system time step, the baseboard attempts to meet any remaining heating requirement of the zone through the following calculations:
+
+\begin{equation}
+{C_{water}} = {c_{p,water}}{\dot m_{water}}
+\end{equation}
+
+\begin{equation}
+{C_{air}} = {c_{p,air}}{\dot m_{air}}
+\end{equation}
+
+\begin{equation}
+{C_{\max }} = MAX\left( {{C_{air}},{C_{water}}} \right)
+\end{equation}
+
+\begin{equation}
+{C_{\min }} = MIN\left( {{C_{air}},{C_{water}}} \right)
+\end{equation}
+
+\begin{equation}
+{C_{ratio}} = {{{C_{\min }}} \mathord{\left/ {\vphantom {{{C_{\min }}} {{C_{\max }}}}} \right. } {{C_{\max }}}}
+\end{equation}
+
+\begin{equation}
+\varepsilon  = 1 - {e^{\left( {\frac{{NT{U^{0.22}}}}{{{C_{ratio}}}}{e^{\left( { - {C_{ratio}}NT{U^{0.78}}} \right)}} - 1} \right)}}
+\end{equation}
+
+Once the effectiveness is determined, the outlet conditions for and output from the unit are determined using the following equations:
+
+\begin{equation}
+{T_{air,outlet}} = {T_{air,inlet}} + \varepsilon {{\left( {{T_{water,inlet}} - {T_{air,inlet}}} \right){C_{\min }}} \mathord{\left/ {\vphantom {{\left( {{T_{water,inlet}} - {T_{air,inlet}}} \right){C_{\min }}} {{C_{air}}}}} \right. } {{C_{air}}}}
+\end{equation}
+
+\begin{equation}
+{T_{water,outlet}} = {T_{water,inlet}} - \left( {{T_{air,outlet}} - {T_{air,inlet}}} \right){{{C_{air}}} \mathord{\left/ {\vphantom {{{C_{air}}} {{C_{water}}}}} \right. } {{C_{water}}}}
+\end{equation}
+
+\begin{equation}
+Output\left( {Convective} \right) = {C_{water}}\left( {{T_{water,inlet}} - {T_{water,outlet}}} \right)
+\end{equation}
+
+If the unit was scheduled off or there is no water flow rate through the baseboard unit, then there will be no convection from the unit.~ The model assumes no heat storage in the baseboard unit itself and thus no residual heat transfer in future system time steps due to heat storage in the water or metal of the baseboard unit.
+
+\subsubsection{References}\label{references-006}
+
+The effectiveness-NTU method is taken from Incropera and DeWitt, Fundamentals of Heat and Mass Transfer, Chapter 11.4, p.~523, eq. 11.33.~ The user can always refer to the ASHRAE Handbook series for general information on different system types as needed.
+
+\subsection{Electric Baseboard Heater with Only Convection}\label{electric-baseboard-heater-with-only-convection}
+
+\subsubsection{Overview}\label{overview-1-002}
+
+The input object ZoneHVAC:Baseboard:Convective:Electric provides a model for electric baseboard heaters that assumes only convective heat addition to a space from a baseboard heater.~ In most situations, the baseboard heater does give a significant amount of heat off via natural convection, but some heat is given off via radiation.~ In this model, the radiant component is ignored and all heat is assumed to be delivered to the space via convection.~ The baseboard heater is transferred to the unit via electric resistance heating.~ EnergyPlus then assumes that this heat is evenly spread throughout the space thus having an immediate impact on the zone air heat balance which is used to calculate the mean air temperature (MAT) within the space.
+
+\subsubsection{Model Description}\label{model-description-1-002}
+
+\subsubsection{Convective Electric Baseboard Heater Inputs}\label{convective-electric-baseboard-heater-inputs}
+
+Like many other HVAC components, the convective-only electric baseboard model requires a unique identifying name and an availability schedule.~ The availability schedule defines the availability of the unit for providing condition to the space.
+
+The input also requires a capacity and efficiency for the unit.~ While the efficiency is a required input that defaults to unity, the capacity can be chosen to be auto-sized by EnergyPlus.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-1-000}
+
+When the unit is available and there is a heating load within a space, the electric baseboard unit will meet the entire remaining provided that it has enough capacity to do so.~ The energy consumption of the baseboard heat is calculated using the user-supplied efficiency and the current load on the baseboard unit as follows:
+
+\begin{equation}
+Energ{y_{electric}} = {{Heatin{g_{baseboard}}} \mathord{\left/ {\vphantom {{Heatin{g_{baseboard}}} {Efficiency}}} \right. } {Efficiency}}
+\end{equation}
+
+If the unit was scheduled off or there is no heating load for the zone, then there will be no convection from the unit.~ The model assumes no heat storage in the baseboard unit itself and thus no residual heat transfer in future system time steps due to heat storage in the metal of the baseboard unit.
+
+\subsubsection{References}\label{references-1-002}
+
+No specific reference.~ Refer to the ASHRAE Handbook series for general information on different system types as needed.
+
+\subsection{Hot Water Baseboard Heater with Radiation and Convection}\label{hot-water-baseboard-heater-with-radiation-and-convection}
+
+\subsubsection{Overview}\label{overview-2-002}
+
+The water baseboard heater model is intended to calculate the mass flow rate of the water by determining the actual system impact not only to the surrounding air via convection but also to the surfaces and people via radiation. The actual system impact by the heater in the zone is the sum of the additional convective heat transfer from the surfaces to the zone air after they have been heated as well as radiant heat transferred to people and the convective heat transfer to the zone. This actual convective power tries to meet any remaining heating requirement in the zone. The model thus improves the accuracy of thermal comfort predictions and system responses.
+
+The radiant components are calculated to interact with the surfaces in the zone through the radiant distribution fractions. Heat is also delivered to the space via convection. The baseboard heater is supplied with hot water from the primary system which is circulated through the inside of a finned tube within the space. This could also be used to model a hot water radiator (convector in the UK). Heat is transferred from the water inside the pipe, through the tube and fins. It is also not only convected to the surrounding air but also radiated to the surfaces within the space. The user is allowed to specify the percentage of radiant heat from the heater to the surfaces. In addition, the user is allowed the ability to define what fraction of radiation leaving the heater is incident directly on a person within the zone for thermal comfort purposes. This amount of heat is then used in the thermal comfort models as the high temperature radiant heater model.
+
+This model calculates the UA values using the log mean temperature difference (LMTD) method. The calculation is based on standard conditions of both fluids obtained in a rating document or manufacturer's literature. Overall energy balances to the hot water and air handle the heat exchange between the water loop and the zone air. Once the UA for the baseboard heater has been determined, the model employs an effectiveness-NTU heat exchanger method to determine the heat transfer between the water and zone air. This is necessary because during the simulation only the inlet water and ``inlet air'' (assumed to be zone air) temperatures are known. As a result, the effectiveness-NTU heat exchanger methodology is suited to determine the performance of the system during the simulation.
+
+\subsubsection{Model Description}\label{model-description-2-002}
+
+\subsubsection{Water Baseboard Heater Inputs}\label{water-baseboard-heater-inputs}
+
+Like many other HVAC components, the water baseboard model requires a unique identifying name, an available schedule, and water inlet and outlet nodes. These define the availability of the unit for providing conditions to the space and the node connections that relate to the primary system. For the calculation of the UA value of the unit, standard conditions of both fluids are necessary. The user can specifies such standard conditions from manufacturers' information such as I = B = R rating document. The user provides the rated capacity, average water temperature, water mass flow rate, and standard inlet air temperature. However, the model also has the ability to autosize the rated capacity, which allows the user simulate and design any baseboard units when manufacturer's data is unavailable.
+
+The UA value corresponds to the convective heat transfer from the water to the tube, the conduction through the tube and fin material, the natural convection from the tube/fins to the zone air, and radiation to the surfaces. In addition, a convergence tolerance is requested of the user to help define the ability of the local controls to tightly control the system output. In almost all cases, the user should simply accept the default value for the convergence tolerance unless engaged in an expert study of controls logic in EnergyPlus.
+
+Many of the inputs for the radiant heat calculation are the same as the high temperature radiant heater model. User inputs of the fraction radiant and of the fraction of radiant energy incident both on people and on surfaces are required to calculate radiant energy distribution from the heater to the people and surfaces. The sum of radiant energy of these distribution fractions must sum to unity, and each water baseboard heater is allowed to distribute energy to up to 20 surfaces.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-2-000}
+
+The simulation of the main algorithm of this water baseboard model with radiation and convection is similar to the convection-only baseboard model. However, this model determines the UA value of the unit based on rated heating capacities available in the manufacturer's literature. Almost all baseboards or radiators are rated under standard conditions such as water flow rate, inlet air temperature and average water temperature. Those standard conditions should thus be obtained from manufacturers' information. The model then determines the UA value of the unit, employing the log mean temperature difference (LMTD) method so that the heating output from the heater can be determined more correctly than other models.
+
+This model initializes all the conditions at the inlet node such as mass flow rates, temperatures, and specific heat capacities. It calculates the UA value once from standard conditions of the air and water during initialization and it is kept throughout the simulation of the unit.
+
+In case that the user has manufacturer's information regarding the rated capacity, the rated water flow rate, and the rated average water temperature, standard conditions such as the rated heating capacity, \emph{q\(_{std}\)}, average water temperature, \({T_{w,avg}}\) , and water mass flow rate, \(\dot m{}_w\) , are known from the user inputs. The standard water inlet temperature, \({T_{w,in}}\) , and outlet temperature, \({T_{w,out}}\) , are thus obtained from expressions
+
+\begin{equation}
+{T_{w,in}} = \frac{{{q_{std}}}}{{2\dot m{}_w{c_{p,w}}}} + {T_{w,avg}}
+\end{equation}
+
+\begin{equation}
+{T_{w,out}} = 2{T_{w,avg}} - {T_{w,in}}
+\end{equation}
+
+where \({c_{p,w}}\) ~is the specific heat capacity of the water.
+
+The model then assumes the air mass flow rate is given by the following expression:
+
+$\dot{m}_{a,std} = 0.0062 + .0000275 \dot{Q}_{design}$
+
+Since the inlet air temperature, \{T\_\{a,in\}\} , of 18°C and the heating capacity of the unit, i.e.~rated capacity, are known, the outlet air temperature, \{T\_\{a,out\}\} , can be obtained from expression
+
+$T_{a,out} = \frac{q_{std}}{\dot{m}_{a,std}c_{p,a}} + T_{a,in}$
+
+where \({c_{p,a}}\) ~is the specific heat capacity of the air.
+
+All temperatures at each node are now known. The mean temperature difference, \(\Delta {T_{lm}}\) , is thus obtained from the following expressions:
+
+\begin{equation}
+\Delta {T_1} = {T_{w,in}} - {T_{a,out}}
+\end{equation}
+
+\begin{equation}
+\Delta {T_2} = {T_{w,out}} - {T_{a,in}}
+\end{equation}
+
+\begin{equation}
+\Delta {T_{lm}} = \frac{{\Delta {T_1} - \Delta {T_2}}}{{\log \left( {\frac{{\Delta {T_1}}}{{\Delta {T_2}}}} \right)}}
+\end{equation}
+
+The UA value of the unit is thus
+
+\begin{equation}
+UA = \frac{{{q_{std}}}}{{\Delta {T_{lm}}}}
+\end{equation}
+
+The model allows the user requests to autosize the rated capacity when the user does not know a particular baseboard unit. It also has the ability to perform parametric study to design the unit based on the design heating load in the zone. The user is also able to modify both rated average water temperature and rated water mass flow rate when manufactures' information is available while the model assumes the default values for both fields if unavailable.
+
+In case that the user requests autosizing the rated capacity, the model employs the design heating load and design water mass flow rate in the zone, so that the standard water inlet and outlet temperatures are estimated as
+
+\begin{equation}
+{T_{w,in}} = \frac{{{q_{design}}}}{{2\dot m{}_{w,design}{c_{p,w}}}} + {T_{w,avg}}
+\end{equation}
+
+\begin{equation}
+{T_{w,out}} = 2{T_{w,avg}} - {T_{w,in}}
+\end{equation}
+
+where \({q_{design}}\) ~is the design heating load estimated by EnergyPlus in the zone.
+
+Similarly, the model estimates the air outlet temperature using the air mass flow rate calculated above:
+
+\begin{equation}
+{T_{a,out}} = \frac{{{q_{design}}}}{{\dot m_{a,std} {c_{p,a}}}} + {T_{a,in}}
+\end{equation}
+
+Temperatures at the nodes are now known and the UA value is determined in the same fashion as the previous case.
+
+Once the UA value is determined, the model employs an effectiveness-NTU heat exchanger method to determine the heat transfer between the water and the zone air as convection-only model does (see ``Hot Water Baseboard Heater with Only Convection'' model). During this calculation the air mass flow rate is proportioned to the water mass flow rate:
+
+$\dot{m}_a = \dot{m}_{a,std} \frac{\dot{m}_w}{\dot{m}_{w,max}}$
+
+The model then determines the radiant heat addition by
+
+$q_{rad} = q \cdot Frac_{rad}$
+
+where \emph{q} is the total heating capacity of the heater and \emph{Frac\(_{rad}\)} is the user-defined fraction.
+
+The model now distributes the radiant heat additions to the appropriate surfaces, people for thermal comfort purpose, and the air in the zone. The surface heat balances are then recalculated to determine all heat sources or sinks for radiant systems in the zone. It is assumed that the radiant heat incident on people in the zone is converted to convection to the zone so that the zone heat balance includes this amount of heat which will be lost (see High Temperature Radiant Heater Model). The load met, the actual convective system impact, for the baseboard heater, \emph{q\(_{req}\)}, is therefore determined as
+
+\begin{equation}
+{q_{req}} = ({q_{surf,c}} - {q_{surf,z}}) + {q_{conv}} + {q_{people}}
+\end{equation}
+
+where \emph{q\(_{surf,c}\)} ~is convection from the surfaces to the air in the zone with radiant systems; \emph{q\(_{surf,z}\)} is zero source convection from the surfaces when radiant systems are unavailable; \emph{q\(_{conv}\)} is the convective heat transfer from the heater to the zone air; and \emph{q\(_{people}\)} is radiant heat to the people.
+
+The radiant heat simulation in the water baseboard heater is very similar to the high temperature radiant system model. The controls are the same as shown in Figure~\ref{fig:variable-flow-low-temperature-radiant-system}.~ Variable Flow Low Temperature Radiant System Controls.~ After all system time steps have been simulated, an ``average'' zone heat balance calculation is done (similar to the radiant systems). If the unit was scheduled off or there is no water flow rate through the baseboard unit, then, there will be no heat transfer from the unit. The model assumes no heat storage in the unit itself and thus no residual heat transfer in future system time steps due to heat storage in the water or metal of the unit.
+
+\subsubsection{References}\label{references-2-001}
+
+I = B = R Ratings for Boilers. 2009. Baseboard Radiation, Finned Tube (Commercial) Radiation, and Indirect Fired Water Heaters, January 2009 Edition
+
+Incropera and DeWitt. Fundamentals of Heat and Mass Transfer, Chapter 11.3 and 11.4, eq. 11.15, 11.17, and 11.33.
+
+Li Lianzhong and M. Zaheeruddin. 2006. Dynamic modeling and simulation of a room with hot water baseboard heater, International Journal of Energy Research; 30, pp.~427--445
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/centralheatpumpsystem.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/centralheatpumpsystem.tex
new file mode 100644
index 00000000000..fb7227e7051
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/centralheatpumpsystem.tex
@@ -0,0 +1,135 @@
+\section{CentralHeatPumpSystem }\label{centralheatpumpsystem}
+
+\subsection{Overview}\label{overview-007}
+
+The CentralHeatPumpSystem object simulates the performance of a central heat pump system containing one or more chiller-heater objects. The main function of the object is to call relevant calculation methods for the chiller-heater objects depending on their operating modes, and to calculate temperatures at the outlet nodes and the total energy transfer. The object can be connected to plant loops and a source loop (see Input-Output Reference document), and the node connections are solely dependent on individual chiller-heaters' operating modes. The central system receives water flows from each plant and source loop and then distributes them to individual chiller-heaters as requested. The conditioned water flows leaving the chiller-heaters are then returned to the system, and in turn flow back to the plant loops and source loop to produce heating and cooling, or exchange heat with the source loop.
+
+\subsection{Model Description}\label{model-description-004}
+
+The model first determines operating modes based on the cooling and heating loads on the system, and then decides which calculation algorithm is called. It calls the cooling calculation subroutine when cooling load is demanded, the heating calculation subroutine when heating load is demanded, and both cooling and heating calculation subroutines when both cooling and heating loads are demanded, i.e., simultaneous cooing-heating mode. It then calculates mass-weighed temperatures and heat transfer energy. Six different operating modes (0 through 5) are possible:
+
+0: off
+
+1: cooling-only mode
+
+2: heating-only mode
+
+3: heat recovery mode
+
+4: cooling dominant simultaneous cooling-heating mode
+
+5: heating dominant simultaneous cooling-heating mode.
+
+The model reads different node information over the operating mode so that outlet water conditions at each node of the system can be appropriately determined.
+
+In cooling-only mode (mode 1), the system is connected to the chilled water loop and source loop. It thus reads the evaporator outlet temperatures and mass flow rates of the chiller-heaters to calculate a mass-weighed chilled water temperature at the system outlet node, and the condenser outlet temperatures and mass flow rates of the chiller-heaters to calculate a mass-weighed source water temperature at the system outlet node. In heating-only mode (mode 2), the system is connected to the hot water loop and source loop. It thus reads the condenser temperatures and mass flow rates of the chiller-heaters to calculate a mass-weighed hot water temperature at the system outlet node, and the evaporator temperatures and mass flow rates of the chiller-heaters to calculate a mass-weighed source temperature at the system outlet node.
+
+In simultaneous cooling-heating mode, three different operating modes (mode 3 through 5) are possible. The model checks which simultaneous cooling-heating mode (3, 4, or 5) each chiller-heater is in, and calculates relevant mass-weighed temperatures. The system may be connected to three loops such as chilled water loop, hot water loop, and source water loop in mode 4 or mode 5.
+
+In heat recovery mode, both evaporator temperatures and condenser temperatures are read and a mass-weighed temperature for both chilled water and hot water is calculated. The chiller-heaters in mode 3 do not exchange heat with source water. At least one of the chiller-heaters within the system is in heat recovery mode during simultaneous cooling-heating mode. The system may be only connected to both chilled water loop and hot water loop if all operating chiller-heaters are in heat recovery mode.
+
+The following nomenclature is used in the following equations:
+
+\({\dot m_{cw,bypass}}\) ~ = chilled water bypass mass flow rate in the system {[}kg/s{]}
+
+\({\dot m_{hw,bypass}}\) = hot water bypass mass flow rate in the system {[}kg/s{]}
+
+\({\dot m_{src,bypass}}\) ~ = source water bypass mass flow rate in the system {[}kg/s{]}
+
+\({\dot m_{cw,CH}}\) ~ = chilled water mass flow rate of i\(^{th}\) chiller-heater's evaporator {[}kg/s{]}
+
+\({\dot m_{hw,CH}}\) ~ = hot water mass flow rate of i\(^{th}\) chiller-heater's condenser {[}kg/s{]}
+
+\({\dot m_{src,CH}}\) ~ = source water mass flow rate of i\(^{th}\) chiller-heater, which varies with operating modes {[}kg/s{]}
+
+\({\dot m_{cw,sys}}\) ~ = chilled water mass flow rate of the system {[}kg/s{]}
+
+\({\dot m_{hw,sys}}\) ~ = hot water mass flow rate of the system {[}kg/s{]}
+
+\({\dot m_{src,sys}}\) ~ = source water mass flow rate of the system {[}kg/s{]}
+
+\({T_{cw,sys}}\) ~ = chilled water outlet temperature of the system {[}C{]}
+
+\({T_{hw,sys}}\) ~ = hot water outlet temperature of the system {[}C{]}
+
+\({T_{src,sys}}\) ~ = source water outlet temperature of the system {[}C{]}
+
+\({T_{cw,bypass}}\) ~ = mass-weighed bypass chilled water temperature in the system {[}C{]}
+
+\({T_{hw,bypass}}\) ~ = mass-weighed bypass hot water temperature in the system {[}C{]}
+
+\({T_{src,bypass}}\) ~ = mass-weighed bypass source water temperature in the system {[}C{]}
+
+\({T_{cw,CH}}\) ~ = mass-weighed chilled water outlet temperature from chiller-heaters {[}C{]}
+
+\({T_{hw,CH}}\) ~ = mass-weighed hot water outlet temperature from chiller-heaters {[}C{]}
+
+\({T_{src,CH}}\) ~ = mass-weighed source water outlet temperature from chiller-heaters {[}C{]}
+
+\({T_{cw,i}}\) ~ = chilled water inlet temperature of the system {[}C{]}
+
+\({T_{hw,i}}\) ~ = hot water inlet temperature of the system {[}C{]}
+
+\({T_{src,i}}\) ~ = source water inlet temperature of the system {[}C{]}
+
+\({T_{cw,out}}\) ~ = chilled water outlet temperature of i\(^{th}\) chiller-heater {[}C{]}
+
+\({T_{hw,out}}\) ~ = hot water outlet temperature of i\(^{th}\) chiller-heater {[}C{]}
+
+\({T_{src,out}}\) ~ = source water outlet temperature of i\(^{th}\) chiller-heater {[}C{]}
+
+The model reads node information and local variables of individual chiller-heaters. The nodes and local variables vary with the operating modes as described above in order to calculate mass-weighed temperatures. In the cooling-only mode, it calculates a mass-weighed chilled water temperature (\emph{T\(_{cw,CH}\)}) and a source water temperature (\emph{T\(_{src,CH}\)}) as follows:
+
+\begin{equation}
+{T_{cw,CH}} = \sum\limits_{CH = 1}^n {{T_{cw,out}}} \frac{{{{\dot m}_{cw,CH}}}}{{{m_{cw,sys}}}}
+\end{equation}
+
+\textbf{\emph{\({T_{src,CH}} = \sum\limits_{CH = 1}^n {{T_{src,out}}} \frac{{{{\dot m}_{src,CH}}}}{{{m_{src,sys}}}}\) ~}}.
+
+In heating-only mode, it calculates a mass-weighed hot water temperature (\emph{T\(_{hw,CH}\)}) and a source water temperature (\emph{T\(_{src,CH}\)}) as follows:
+
+\textbf{\emph{\({T_{hw,CH}} = \sum\limits_{CH = 1}^n {{T_{hw,out}}} \frac{{{{\dot m}_{hw,CH}}}}{{{m_{hw,sys}}}}\) ~}}
+
+\textbf{\emph{\({T_{src,CH}} = \sum\limits_{CH = 1}^n {{T_{src,out}}} \frac{{{{\dot m}_{src,CH}}}}{{{m_{src,sys}}}}\) ~}}.
+
+When all chiller-heaters are in heat recovery mode, it calculates a mass-weighed chilled water temperature (\emph{T\(_{cw,CH}\)}) and hot water temperature (\emph{T\(_{hw,CH}\)}) as follows:
+
+\textbf{\emph{\({T_{cw,CH}} = \sum\limits_{CH = 1}^n {{T_{cw,out}}} \frac{{{{\dot m}_{cw,CH}}}}{{{m_{cw,sys}}}}\)}}
+
+\textbf{\emph{\({T_{hw,CH}} = \sum\limits_{CH = 1}^n {{T_{hw,out}}} \frac{{{{\dot m}_{hw,CH}}}}{{{m_{hw,sys}}}}\) ~}}.
+
+In cooling or heating dominant simultaneous cooling-heating mode (mode 4 and 5), at least one chiller-heater should be in heat recovery mode, and the other(s) are in either mode 4 or mode 5. The system is connected to three loops such as chilled water loop, hot water loop, and source water loop. The model thus calculates a mass-weighed chilled water temperature (\emph{T\(_{cw,CH}\)}), hot water temperature (\emph{T\(_{hw,CH}\)}), and source water temperature (\emph{T\(_{src,CH}\)}) as follows:
+
+\textbf{\emph{\({T_{cw,CH}} = \sum\limits_{CH = 1}^n {{T_{cw,out}}} \frac{{{{\dot m}_{cw,CH}}}}{{{m_{cw,sys}}}}\)}}
+
+\textbf{\emph{\({T_{hw,CH}} = \sum\limits_{CH = 1}^n {{T_{hw,out}}} \frac{{{{\dot m}_{hw,CH}}}}{{{m_{hw,sys}}}}\)}}
+
+\textbf{\emph{\({T_{src,CH}} = \sum\limits_{CH = 1}^n {{T_{src,out}}} \frac{{{{\dot m}_{src,CH}}}}{{{m_{src,sys}}}}\)}}~.
+
+The model then calculates a mass-weighed temperature for the by-pass flows remained in the system as follows:
+
+\begin{equation}
+{T_{cw,bypass}} = {T_{cw,i}}\frac{{{{\dot m}_{cw,bypass}}}}{{{m_{cw,sys}}}}
+\end{equation}
+
+\begin{equation}
+{T_{hw,bypass}} = {T_{hw,i}}\frac{{{{\dot m}_{hw,bypass}}}}{{{m_{hw,sys}}}}
+\end{equation}
+
+\begin{equation}
+{T_{src,bypass}} = {T_{src,i}}\frac{{{{\dot m}_{src,bypass}}}}{{{m_{src,sys}}}}
+\end{equation}
+
+The outlet temperatures at each outlet node of the system are then determined as it sums both mass-weighed temperatures up as follows:
+
+\begin{equation}
+{T_{cw,sys}} = {T_{cw,CH}} + {T_{cw,bypass}}
+\end{equation}
+
+\begin{equation}
+{T_{hw,sys}} = {T_{hw,CH}} + {T_{hw,bypass}}
+\end{equation}
+
+\({T_{src,sys}} = {T_{src,CH}} + {T_{src,bypass}}\) .
+
+The total heat transfer energy of the system is also calculated in the same manner as the temperature calculations. The model simply sums all heat transfer energy of the chiller-heaters depending on their operating modes.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/chillerheaterperformance-electric-eir.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/chillerheaterperformance-electric-eir.tex
new file mode 100644
index 00000000000..ac313d4f22c
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/chillerheaterperformance-electric-eir.tex
@@ -0,0 +1,313 @@
+\section{ChillerHeaterPerformance:Electric:EIR }\label{chillerheaterperformanceelectriceir}
+
+\subsection{Overview}\label{overview-008}
+
+The object simulates the performance of a chiller-heater which can receive pre-cooled or pre-heated water from the source loop, and provide cooling, heating, or simultaneous cooling-heating. The object needs to work with the Central Heat Pump System object to be controlled properly. This model does not simulate the thermal performance or the power consumption of associated pumps or cooling towers. The Central Heat Pump System object holds the input/output nodes connection of the chiller-heater and its control scheme, once the chiller-heater is properly referred.
+
+\subsection{Model Description}\label{model-description-005}
+
+The model uses user-input performance information at design conditions along with three performance curves (curve objects) for cooling capacity and efficiency to determine chiller operation at off-design conditions. Three additional performance curves for heating capacity and efficiency are used when the chiller is operating in a heating-only mode or simultaneous cooling-heating mode.
+
+\subsubsection{Cooling-only mode}\label{cooling-only-mode}
+
+The following nomenclature is used in the cooling equations:
+
+\emph{CompMotorEffic} = compressor motor efficiency
+
+\emph{CompPower\(_{clg}\)} = compressor power {[}W{]}
+
+\emph{CompPower\(_{@PLRmin}\)}~ = compressor power at the minimum part-load ratio {[}W{]}
+
+\({C_{p,cw}}\) ~ = chilled water specific heat~ {[}J/kgK{]}
+
+\emph{CyclingRatio}~ = compressor cycling ratio = \emph{PLR\(_{actual}\)} / \emph{PLR\(_{min}\)}
+
+\emph{EvapCapAvail\(_{clg}\)} = available full-load cooling capacity at current conditions {[}W{]}
+
+\emph{EvapCapFT\(_{clg}\)} = cooling capacity function of temperature curve
+
+\emph{EIRFT\(_{clg}\)} = electric input to cooling output factor for temperature function curve
+
+\emph{EIRFPLR\(_{clg}\)} = electric input to cooling output factor for part-load function curve
+
+\({\dot m_{cw}}\) ~ = chilled water mass flow rate {[}kg/s{]}
+
+\({\dot m_{avail,cw}}\) ~ = chilled water maximum available mass flow rate {[}kg/s{]}
+
+\emph{PLR\(_{clg}\)} = cooling part-load ratio = \emph{CoolingLoad} / \emph{EvapCapAvail\(_{clg}\)}
+
+\emph{PLR\(_{actual}\)} = actual part-load ratio at current conditions
+
+\emph{PLR\(_{min}\)} = minimum part-load ratio
+
+\(QCon{d_{c\lg }}\) ~ = total condenser heat transfer energy {[}J{]}
+
+\(\dot QCon{d_{c\lg }}\) ~ = condenser heat transfer rate {[}W{]}
+
+\(QEva{p_{c\lg }}\) ~ = total evaporator heat transfer energy {[}J{]}
+
+\(\dot QEva{p_{c\lg }}\) ~ = evaporator heat transfer rate {[}W{]}
+
+\({\dot Q_{falseloading,c\lg }}\) ~ = false loading rate {[}W{]}
+
+\emph{RefCOP\(_{clg}\)}~ = reference coefficient of performance {[}W/W{]}
+
+\emph{RefEvapCap\(_{clg}\)}~ = reference evaporator capacity {[}W{]}
+
+\emph{FullLoadPwr\(_{clg}\)}~ = reference full load power = \emph{EvapCapAvail\(_{clg}\)} / \emph{RefCOP\(_{clg}\)} {[}W{]}
+
+\emph{T\(_{cond}\)} = either entering or leaving condenser water temperature depending on user input for condenser water independent variable. \emph{T\(_{cond,l}\)}, if ``LeavingCondenser'' is chosen, or \emph{T\(_{cond,e}\)}, if ``EnteringCondenser'' is chosen.
+
+\emph{T\(_{cond,e}\)} = entering condenser water temperature {[}C{]}
+
+\emph{T\(_{cond,l}\)} = leaving condenser water temperature {[}C{]}
+
+\emph{T\(_{cw,e}\)} = entering chilled water~ temperature {[}W{]}
+
+\emph{T\(_{cw,l}\)} = leaving chilled water~ temperature {[}W{]}
+
+\(\Delta {T_{cw}}\) ~ = chilled water inlet and outlet temperature difference {[}C{]}
+
+\(\Delta {T_{cw}}_{,\max }\) ~ = maximum chilled water inlet and outlet temperature difference {[}C{]}
+
+The model sequentially calls each chiller-heater module in the order defined in the Central Heat Pump System object. It then determines cooling load that each chiller-heater needs to meet and water flow rates delivered to each chiller-heater. Once each chiller-heater is assumed to operate, it determines cooling capacity and efficiency using user-supplied performance information.
+
+Three performance curves are used in the calculation of cooling capacity and efficiency as follows:
+
+1)~~~Cooling mode cooling capacity function of temperature curve (\emph{EvapCapFT\(_{clg}\)})
+
+2)~~~Cooling mode electric input to cooling output ratio function of temperature curve (\emph{EIRFT\(_{clg}\)})
+
+3)~~~Cooling mode electric input to cooling output ratio function of part load ratio curve (\emph{EIRFPLR\(_{clg}\)})
+
+The Cooling Capacity Function of Temperature Curve (\emph{EvapCapFT\(_{clg}\)}) represents the fraction of the cooling capacity of the chiller-heater as it varies by temperature. The curve should have a value of 1.0 at the reference conditions. The output of a bi-quadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature is given by:
+
+\textbf{\emph{\(EvapCapF{T_{c\lg }} = a + b{T_{cw,l}} + c{T_{cw,l}}^2 + d{T_{Cond}} + e{T_{Cond}}^2 + f{T_{cw,l}}{T_{Cond}}\)}}.
+
+The Cooling Mode Electric Input to Cooling Output Ratio Function of Temperature (EIRFT\(_{clg}\)) curve represents the fraction of electricity to the chiller-heater at full load as it varies by temperature. The output of a bi-quadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature is given by:
+
+\textbf{\emph{\(EIRF{T_{c\lg }} = a + b{T_{cw,l}} + c{T_{cw,l}}^2 + d{T_{Cond}} + e{T_{Cond}}^2 + f{T_{cw,l}}{T_{Cond}}\)}}.
+
+The Cooling Mode Electric Input to Cooling Output Ratio Function of Part Load Ratio (EIRFPLR\(_{clg}\)) curve represents the fraction of electricity to the chiller-heater as the load on the chiller varies at a given set of operating temperatures. The curve is normalized so that at full load the value of the curve should be 1.0. Note that the bi-cubic formulation below is generally only valid when LeavingCondenser variable is chosen for the field of Cooling Mode Condenser Water Temperature Curve Input Variable whereas the quadratic curve can be used for both choices, i.e., LeavingCondenser and EnteringCondenser. Bi-cubic may also be used when the chiller-heater uses a variable-speed compressor motor drive. The output of this curve can be determined by one of the following three performance curves:
+
+\begin{equation}
+EIRFPL{R_{c\lg }} = a + b{T_{Cond,l}} + c{T_{Cond,l}}^2 + dPLR + ePL{R^2} + f{T_{Cond,l}}PLR + g \cdot 0 + hPL{R^3} + i \cdot 0 + j \cdot 0
+\end{equation}
+
+\begin{equation}
+EIRFPL{R_{c\lg }} = a + bPLR + cPL{R^2}
+\end{equation}
+
+\begin{equation}
+EIRFPL{R_{c\lg }} = a + bPLR + cPL{R^2} + dPL{R^3}
+\end{equation}
+
+The full-load cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the design temperatures) is then computed as follows:
+
+\textbf{\emph{\(EvapCapAvai{l_{c\lg }} = RefEvapCa{p_{c\lg }} \cdot EvapCapF{T_{c\lg }}\)}}.
+
+The model then determines current chiller-heater's evaporator heat transfer rate based on the total cooling load required a central heat pump system to meet and the maximum available chiller-heater cooling capacity. The maximum evaporator temperature difference between the entering chilled water temperature (\emph{T\(_{cw,e}\)}) and the leaving chilled water temperature (\emph{T\(_{cw,l}\)}) obtained from the plant loop setpoint temperature can also be determined. It then calculates mass flow rate for variable flow control chiller-heaters and the temperature difference for constant flow control chiller-heaters, setting the cooling load each chiller-heater needs to meet equal to the evaporator heat transfer rate.
+
+As for variable flow control chiller-heaters, the chilled water mass flow rate is computed as follows:
+
+\textbf{\emph{\({\dot m_{cw}} = \frac{{\dot QEva{p_{c\lg }}}}{{{C_{p,cw}}\Delta {T_{cw,\max }}}}\)}}.
+
+The chilled water mass flow rate calculated is then compared to the maximum available mass flow rate for individual chiller-heaters. If the calculated one is bigger than the maximum, the model sets the chilled water mass flow rate equal to the maximum. It then adjusts the temperature difference based on the evaporator heat transfer rate and the maximum mass flow rate. If the adjusted temperature difference also exceeds the maximum, the model finally adjusts the evaporator heat transfer rate at the maximum temperature difference and mass flow rate as follows:
+
+\textbf{\emph{\(\dot QEva{p_{c\lg }} = {\dot m_{avail,cw}}{C_{p,cw}}\Delta {T_{cw,\max }}\)}}.
+
+As for constant flow control chiller-heaters, the model calculates chilled water temperature difference as follows:
+
+\textbf{\emph{\(\Delta {T_{cw}} = \frac{{\dot QEva{p_{c\lg }}}}{{{{\dot m}_{avail,cw}}{C_{p,cw}}}}\)}}.
+
+The temperature difference calculated is then compared to the maximum temperature difference allowed. If the calculated one is bigger than the maximum, the model sets the chilled water temperature difference equal the maximum, and then adjusts the evaporator heat transfer rate at the given conditions as follows:
+
+\textbf{\emph{\(\dot QEva{p_{c\lg }} = {\dot m_{avail,cw}}{C_{p,cw}}\Delta {T_{cw,\max }}\)}}.
+
+The model then calculates the part-load ratio as the ratio of the evaporator heat transfer rate to the available chiller-heater capacity as follows:
+
+\textbf{\emph{\(PL{R_{c\lg }} = \frac{{\dot QEva{p_{c\lg }}}}{{\dot QEvapAvai{l_{c\lg }}}}\)}}.
+
+The part-load ratio calculated is set to be between the maximum of 1.0 and the minimum of 0.0 when it is out of the range. Once the part-load ratio is calculated the cycling ratio and false loading rate can be obtained as follows:
+
+\begin{equation}
+CyclingRatio = \frac{{PL{R_{{\rm{actual}}}}}}{{PL{R_{{\rm{min}}}}}}
+\end{equation}
+
+\({\dot Q_{falseloading,c\lg }} = EvapCapAvai{l_{{\rm{clg}}}} \cdot PL{R_{c\lg }} \cdot CyclingRatio - \dot QEva{p_{{\rm{clg}}}}\) .
+
+The compressor power demand is then computed by:
+
+\(CompPowe{r_{c\lg }} = RefFullLoadPowe{r_{{\rm{clg}}}} \cdot {\rm{ }}EIRF{T_{c\lg }}{\rm{ }} \cdot EIRFPL{R_{c\lg }} \cdot CyclingRatio\) .
+
+The heat transfer rate for the chiller-heater condenser can then be computed as follows:
+
+\(\dot QCon{d_{c\lg }} = ComPowe{r_{c\lg }} \cdot CompMotorEffic + \dot QEva{p_{c\lg }} + {\dot Q_{falseloading,c\lg }}\) ~.
+
+The total heat transfer energy by the evaporator and condenser can be calculated as follows:
+
+\begin{equation}
+QEva{p_{c\lg }} = \dot QEva{p_{c\lg }} \cdot TimeStepSys \cdot 3600
+\end{equation}
+
+\(QCon{d_{c\lg }} = \dot QCon{d_{c\lg }} \cdot TimeStepSys \cdot 3600\) ~.
+
+\subsubsection{Heating-only mode and Simultaneous cooling-heating mode}\label{heating-only-mode-and-simultaneous-cooling-heating-mode}
+
+The following nomenclature is used in the heating equations:
+
+\emph{CompMotorEffic} = compressor motor efficiency
+
+\emph{CompPower\(_{htg}\)} = compressor power demand {[}W{]}
+
+\emph{CompPower\(_{@PLRmin}\)}~ = compressor power at the minimum part-load ratio {[}W{]}
+
+\({C_{p,evap}}\) ~ = evaporator water specific heat~ {[}J/kgK{]}
+
+\({C_{p,hw}}\) ~ = hot water specific heat~ {[}J/kgK{]}
+
+\emph{CyclingRatio}~ = compressor cycling ratio = \emph{PLR\(_{actual}\)} / \emph{PLR\(_{min}\)}
+
+\emph{EvapCapAvail\(_{htg}\)} = available full-load cooling capacity at current conditions {[}W{]}
+
+\emph{EvapCapFT\(_{htg}\)} = heating mode cooling capacity function of temperature curve
+
+\emph{EIRFT\(_{htg}\)} = electric input to cooling output factor for temperature function curve
+
+\emph{EIRFPLR\(_{htg}\)} = electric input to cooling output factor for part-load function curve
+
+\({\dot m_{avail,evap}}\) ~ = evaporator water maximum available mass flow rate {[}kg/s{]}
+
+\({\dot m_{avail,hw}}\) ~ = condenser water maximum available mass flow rate {[}kg/s{]}
+
+\({\dot m_{hw}}\) ~ = hot water mass flow rate {[}kg/s{]}
+
+\emph{PLR\(_{htg}\)} = cooling part-load ratio = \emph{RefCap} / \emph{EvapCapAvail\(_{htg}\)}
+
+\emph{PLR\(_{max}\)} = maximum part-load ratio at current conditions
+
+\emph{PLR\(_{min}\)} = minimum part-load ratio
+
+\(QCon{d_{htg}}\) ~ = total condenser heat transfer energy {[}J{]}
+
+\(\dot QCondAvai{l_{htg}}\) ~ = available full-load heating capacity at current conditions {[}W{]}
+
+\(\dot QCon{d_{htg}}\) ~ = condenser heat transfer rate {[}W{]}
+
+\(QEva{p_{htg}}\) ~ = total evaporator heat transfer energy {[}J{]}
+
+\(\dot QEva{p_{htg}}\) ~ = evaporator heat transfer rate {[}W{]}
+
+\({\dot Q_{falseloading,htg}}\) ~ = false loading rate {[}W{]}
+
+\emph{RefCOP\(_{htg}\)}~ = reference coefficient of performance {[}W/W{]}
+
+\emph{RefEvapCap\(_{htg}\)}~ = reference evaporator capacity {[}W{]}
+
+\emph{FullLoadPwr\(_{htg}\)}~ = reference full load power = \emph{EvapCapAvail\(_{htg}\)}/ \emph{RefCOP\(_{htg}\)} {[}W{]}
+
+\emph{T\(_{cond}\)} = either entering or leaving condenser water temperature depending on user input for condenser water independent variable. \emph{T\(_{cond,l}\)}, if ``LeavingCondenser'' is chosen, or \emph{T\(_{cond,e}\)}, if ``EnteringCondenser'' is chosen.
+
+\emph{T\(_{cond,e}\)} = entering condenser water temperature {[}C{]}
+
+\emph{T\(_{cond,l}\)} = leaving condenser water temperature {[}C{]}
+
+\emph{T\(_{cw,l}\)} = leaving chilled water~ temperature {[}C{]}
+
+\emph{T\(_{hw,e}\)} = entering hot water temperature {[}C{]}
+
+\emph{T\(_{hw,l}\)} = leaving hot water temperature {[}C{]}
+
+\(\Delta {T_{evap}}\) ~ = evaporator inlet and outlet water temperature difference {[}C{]}
+
+\(\Delta {T_{hw}}\) ~ = hot water inlet and outlet temperature difference {[}C{]}
+
+\(\Delta {T_{hw}}_{,\max }\) ~ = maximum hot water inlet and outlet temperature difference {[}C{]}
+
+The calculations for the evaporator side are similar to the cooling-only mode calculations. The evaporator capacity and efficiency is determined by a different set of three performance curves read in the cooling-only mode, and the performance curve set is used for both heating-only mode and simultaneous cooling-heating mode. During these modes, the evaporator side is not connected to the chilled water loop, but source water loop. The model thus assumes that each chiller-heater does not meet the plant loop chilled water setpoint temperature while the evaporator operates at the full load capacity to produce heating at a constant water flow rate.
+
+The model sequentially calls each chiller-heater module in the order of the definition in the central heat pump system. It then determines heating load that each chiller-heater needs to meet and water flow rates delivered to each chiller-heater. Once each chiller-heater is assumed to operate, it determines heating capacity and efficiency using the following performance curves:
+
+1)~~~Heating mode cooling capacity function of temperature curve (\emph{EvapCapFT\(_{htg}\)})
+
+2)~~~Heating mode electric input to cooling output ratio function of temperature curve (\emph{EIRFT\(_{htg}\)})
+
+3)~~~Heating mode electric input to cooling output ratio function of part load ratio curve (\emph{EIRFPLR\(_{htg}\)})
+
+The output of a Heating Mode Cooling Capacity Function of Temperature curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature is given by:
+
+\textbf{\emph{\(EvapCapF{T_{htg}} = a + b{T_{cw,l}} + c{T_{cw,l}}^2 + d{T_{Cond}} + e{T_{Cond}}^2 + f{T_{cw,l}}{T_{Cond}}\)}}
+
+The output of a Heating Mode Cooling Output Ratio Function of Temperature curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature is given by:
+
+\textbf{\emph{\(EIRF{T_{htg}} = a + b{T_{cw,l}} + c{T_{cw,l}}^2 + d{T_{Cond}} + e{T_{Cond}}^2 + f{T_{cw,l}}{T_{Cond}}\)}}.
+
+The output of Heating Mode Cooling Output Ratio Function of Part Load Ratio curve can be determined by one of the following three performance curves as follows:
+
+\begin{equation}
+EIRFPL{R_{htg}} = a + b{T_{Cond,l}} + c{T_{Cond,l}}^2 + dPLR + ePL{R^2} + f{T_{Cond,l}}PLR + g \cdot 0 + hPL{R^3} + i \cdot 0 + j \cdot 0
+\end{equation}
+
+\begin{equation}
+EIRFPL{R_{htg}} = a + bPLR + cPL{R^2}
+\end{equation}
+
+\begin{equation}
+EIRFPL{R_{htg}} = a + bPLR + cPL{R^2} + dPL{R^3}
+\end{equation}
+
+The full-load evaporator capacity at specific temperature operating conditions is then given by:
+
+\textbf{\emph{\(EvapCapAvai{l_{htg}} = RefEvapCa{p_{htg}} \cdot EvapCapF{T_{htg}}\)}}.
+
+The part-load ratio is set to be between zero and the maximum, and the evaporator heat transfer rate is computed by:
+
+\textbf{\emph{\(\dot QEva{p_{htg}} = EvapCapAvai{l_{htg}}PL{R_{htg}}\)}}The evaporator inlet and outlet temperature difference is then given by:
+
+\textbf{\emph{\(\Delta {T_{evap}} = \frac{{\dot QEva{p_{htg}}}}{{{{\dot m}_{avail,evap}}{C_{p,evap}}}}\)}}
+
+Once the part-load ratio is calculated the cycling ratio and false loading rate are computed by:
+
+\begin{equation}
+CyclingRatio = \frac{{PL{R_{{\rm{actual}}}}}}{{PL{R_{{\rm{min}}}}}}
+\end{equation}
+
+\({\dot Q_{falseloading,htg}} = EvapCapAvai{l_{{\rm{htg}}}} \cdot PL{R_{htg}} \cdot CyclingRatio - \dot QEva{p_{{\rm{htg}}}}\) .
+
+The compressor power demand is then computed by:
+
+\textbf{\emph{\(CompPowe{r_{htg}} = FullLoadPowe{r_{{\rm{htg}}}} \cdot {\rm{ }}EIRF{T_{htg}}{\rm{ }} \cdot EIRFPL{R_{htg}} \cdot CyclingRatio\)}}
+
+The heat transfer rate of the chiller-heater condenser is then computed as follows:
+
+\begin{equation}
+\dot QCondAvai{l_{htg}} = ComPowe{r_{htg}} \cdot CompMotorEffic + \dot QEva{p_{htg}} + {\dot Q_{falseloading,htg}}
+\end{equation}
+
+Once condenser available heating capacity is determined, the model calculates current chiller-heater's condenser heat transfer rate based on the total heating load required a central heat pump system to meet as well as available heating capacity of the chiller-heater. The maximum condenser temperature difference between the entering hot water temperature (\emph{T\(_{hw,e}\)}) and the leaving hot water temperature (\emph{T\(_{hw,l}\)}) obtained from the plant loop setpoint temperature can also be obtained. It then calculates condenser water mass flow rate for variable flow control chiller-heaters and the hot water temperature difference for constant flow control chiller-heaters, setting the cooling load that each chiller-heater needs to meet equal the evaporator heat transfer rate.
+
+As for variable flow control chiller-heaters, the condenser water mass flow rate is computed as follows:
+
+\textbf{\emph{\({\dot m_{hw}} = \frac{{\dot QCon{d_{htg}}}}{{{C_{p,hw}}\Delta {T_{hw,\max }}}}\)}}.
+
+The condenser water mass flow rate calculated is then compared to the maximum available mass flow rate for individual chiller-heaters. If the calculated one is bigger than the maximum, the model sets the condenser water mass flow rate equal the maximum. It then adjusts the hot water temperature difference at the maximum mass flow rate. If the adjusted temperature difference also exceeds the maximum, the model finally adjusts the condenser heat transfer rate at the maximum allowable conditions as follows:
+
+\textbf{\emph{\(\dot QCon{d_{htg}} = {\dot m_{avail,hw}}{C_{p,hw}}\Delta {T_{hw,\max }}\)}}.
+
+As for constant flow control chiller-heaters, the model calculates condenser temperature difference as follows:
+
+\textbf{\emph{\(\Delta {T_{hw}} = \frac{{\dot QCon{d_{htg}}}}{{{{\dot m}_{avail,hw}}{C_{p,hw}}}}\)}}.
+
+The temperature difference calculated is then compared to maximum hot water temperature difference. If the calculated one is bigger than the maximum, the model sets the hot water temperature difference equal the maximum, and then adjusts the condenser heat transfer rate at the given conditions as follows:
+
+\textbf{\emph{\(\dot QCon{d_{htg}} = {\dot m_{avail,hw}}{C_{p,hw}}\Delta {T_{hw,\max }}\)}}.
+
+Finally, the total heat transfer energy by the evaporator and condenser can then be calculated as follows:
+
+\textbf{\emph{\(QEva{p_{htg}} = \dot QEva{p_{htg}} \cdot TimeStepSys \cdot 3600\)}}
+
+\textbf{\emph{\(QCon{d_{htg}} = \dot QCon{d_{htg}} \cdot TimeStepSys \cdot 3600\)}}.
+
+\subsection{References}\label{references-008}
+
+Central Geothermal Systems, Applications Engineering Manual, Trane Company, April 2010, SYS-APM009-EN.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/coils.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/coils.tex
new file mode 100644
index 00000000000..bbec6bdda91
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/coils.tex
@@ -0,0 +1,7215 @@
+\section{Coils }\label{coils}
+
+\subsection{Chilled-Water-Based Air Cooling Coil}\label{chilled-water-based-air-cooling-coil}
+
+The input object Coil:Cooling:Water is simpler than the detailed geometry model.~ The simple model provides a good prediction of the air and water outlet conditions without requiring the detailed geometric input required for the detailed model.~ A greatly simplified schematic of enthalpy and temperature conditions in a counter flow cooling/dehumidifying coil is shown in the schematic Figure~\ref{fig:simplified-schematic-of-coolingdehumidifying}.~ The input required to model the coil includes only a set of thermodynamic design inputs, which require no specific manufacturer's data.~ The coil simulation model is essentially a modification of one presented by Elmahdy and Mitalas (1977), TRNSYS, 1990 and Threlkeld, J.L. 1970.~ The model calculates the UA values required for a Dry, Wet and Part Wet \& Part Dry Coil and iterates between the Dry and Wet Coil to output the fraction wet.~ There are two modes of flow operation for this model: Cross Flow, which is widely applicable in HVAC systems and the second being Counter flow mode. The default value in program is set up for Counter Flow.~ In addition the coil has two modes of analysis: Simple Analysis and Detailed Analysis. The Simple analysis mode operates the coil as either wet or dry while the detailed mode simulates the coil as part wet part-dry. While the detailed mode provides more accurate results, it is significantly slower than the simple model. The simple mode gives good results for an annual simulation but will not be adequate for a time step performance analysis.
+
+\begin{figure}[hbtp] % fig 162
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3304.svg.png}
+\caption{  Simplified Schematic of Cooling/Dehumidifying Coil \protect \label{fig:simplified-schematic-of-coolingdehumidifying}}
+\end{figure}
+
+\subsubsection{Heat Transfer and Energy Balance}\label{heat-transfer-and-energy-balance}
+
+The cooling coil may be completely dry, completely wet with condensation, or it may have wet and dry sections.~ The actual condition of the coil surface depends on the humidity and temperature of the air passing over the coil and the coil surface temperature.~ The part-dry part-wet case represents the most general scenario for the coil surface conditions.~ There are subroutines present in the model for both the dry and wet regions of the coil, and a subroutine that iterates between the dry and wet subroutines to calculate the fraction of the coil surface that is wet.~ For each region the heat transfer rate from air to water may be defined by the rate of enthalpy change in the air and in the water.~ The rates must balance between each medium for energy to be conserved.
+
+\subsubsection{Model Description}\label{model-description-007}
+
+The Model has two blocks: 1\(^{st}\) = Design Block with the Design Inputs. This block calculates the Design U-Factor Times Area Value (UA) values required by the model. Using these UA values the model simulates the operating conditions.~ The operating block is the one containing the operating conditions, the conditions at which the coil operates. Following is the list of Design and Operating inputs and subsequently the Design and Operating variables used in the model.
+
+% table 52
+\begin{longtable}[c]{p{1.79in}p{4.2in}}
+\caption{Design Inputs (User Inputs) \label{table:design-inputs-user-inputs}} \tabularnewline
+\toprule 
+Input Field & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Design Inputs (User Inputs)} \tabularnewline
+\toprule 
+Input Field & Description \tabularnewline
+\midrule
+\endhead
+
+DesWaterVolFlowRate: & Maximum Water Volume Flow Rate \tabularnewline
+DesAirVolFlowRate: & Maximum Air Volume Flow Rate \tabularnewline
+DesInletWaterTemp: & Inlet Water Temperature at Design Condition \tabularnewline
+DesInletAirTemp: & Inlet Air Temperature at Design Condition \tabularnewline
+DesOutletAirTemp: & Outlet Air Temperature at Design Condition \tabularnewline
+DesInletAirHumRat: & Inlet Air Humidity Ratio at Design Conditions \tabularnewline
+DesOutletAirHumRat: & Outlet Air Humidity Ratio at Design Conditions. \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 53
+\begin{longtable}[c]{p{1.84in}p{4.16in}}
+\caption{Operating Conditions (From Nodes -- not user inputs) \label{table:operating-conditions-from-nodes-not-user}} \tabularnewline
+\toprule 
+Condition Variable & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Operating Conditions (From Nodes -- not user inputs)} \tabularnewline
+\toprule 
+Condition Variable & Description \tabularnewline
+\midrule
+\endhead
+
+InletWaterMassFlowRate: & Entering Water Mass Flow Rate at operating condition \tabularnewline
+InletWaterTemp: & Inlet Water Temperature at operating condition \tabularnewline
+InletAirMassFlowRate: & Entering Air Mass Flow Rate at operating condition \tabularnewline
+InletAirTemp: & Inlet Air Temperature at operating condition \tabularnewline
+InletAirHumRat: & Entering air humidity ratio at operating conditions \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Intermediate calculated U-Factor Times Area Values: The Crux of the Model}\label{intermediate-calculated-u-factor-times-area-values-the-crux-of-the-model}
+
+The various U-Factor Times Area values (UA) required by this model are calculated from the above inputs, which are explained later in the document.~ The various UA are:
+
+% table 54
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{UA Descriptions of Model \label{table:ua-descriptions-of-model}} \tabularnewline
+\toprule 
+UA Variable Name & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{UA Descriptions of Model} \tabularnewline
+\toprule 
+UA Variable Name & Description \tabularnewline
+\midrule
+\endhead
+
+CoilUATotal: & Overall heat transfer coefficient (W/C) \tabularnewline
+CoilUAInternal: & Overall internal UA (W/C) \tabularnewline
+CoilUAExternal: & Overall external UA (W/C) \tabularnewline
+CoilUInternal: & Internal overall heat transfer coefficient (W/m  ∙C) \tabularnewline
+CoilUWetExternal: & Wet part external overall heat transfer coefficient (W/m  ∙C) \tabularnewline
+CoilUDryExternal: & Dry part external overall heat transfer coefficient (W/m  ∙C) \tabularnewline
+\bottomrule
+\end{longtable}
+
+The UA values are calculated assuming a wet coil at the design conditions. Following are a few important calculations to understand the working of the model.~ The model is basically divided into two blocks: the Design Block and the Operating Block.
+
+The Design Block is a one time calculation. The aim of the Design Block is to calculate the Coil UA for use in the operating Block.
+
+\subsubsection{Design Block Calculations:}\label{design-block-calculations}
+
+The design block has the code for calculating the six Coil UA values required by the operating block. Reasonable assumptions have been made in the calculations to maintain the simplicity of the model.
+
+Heat transfer in a wet coil model is based on enthalpy rather than temperature to take into account latent effects. While heat transfer rates are commonly expressed as the product of an overall heat transfer coefficient, UA, and a temperature difference, the use of enthalpy-based heat transfer calculations requires an enthalpy-based heat transfer coefficient which we denote as DesUACoilTotalEnth and hence the equation.
+
+Q = DesUACoilTotalEnth * (H\(_{air,mean}\) - H\(_{water,mean}\)). The value of Q is calculated using product of air mass flow rate and difference in inlet and outlet air enthalpies at design conditions.
+
+The relation between the enthalpy-based UA and the temperature-based UA is DesUACoilTotalEnth = CoilUA / C\(_{p}\). CoilUA is the conventional heat transfer coefficient and C\(_{p}\) = specific heat of the air.
+
+We need the following quantities for our design calculations. The \emph{Psy} functions are the EnergyPlus built-in psychrometric functions.
+
+\begin{equation}
+{\dot m_{air}} = {\rho_{air}}{\dot V_{air}}
+\end{equation}
+
+\begin{equation}
+{h_{air,in}} = {\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{air,in}},{w_{air,in}})
+\end{equation}
+
+\begin{equation}
+{h_{air,out}} = {\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{air,out}},wout)
+\end{equation}
+
+\begin{equation}
+{h_{w,sat,in}} = {\rm{PsyHFnTdbW}}({T_{w,in}},{\rm{PsyWFnTdpPb}}({T_{w,in}},{P_{atm}}))
+\end{equation}
+
+\begin{equation}
+{\dot Q_{coil}} = {\dot m_{air}}({h_{air,in}} - {h_{air,out}})
+\end{equation}
+
+\begin{equation}
+{T_{w,out}} = {T_{w,in}} + {\dot Q_{coil}}/({\dot m_{w,\max }}{C_{p,w}})
+\end{equation}
+
+\begin{equation}
+{h_{w,sat,out}} = {\rm{PsyHFnTdbW}}({T_{w,out}},{\rm{PsyWFnTdpPb}}({T_{w,out}},{P_{atm}}))
+\end{equation}
+
+We now calculate the design coil bypass factor. The bypass factor is not used in subsequent calculations. It is calculated solely to use as check on the reasonableness of the user-input design inlet and outlet conditions. First we make an initial estimate of the apparatus dew point temperature:
+
+\begin{equation}
+{T_{air,dp,app}} = {\rm{PsyTdpFnWPb}}({w_{air,out}},{P_{atm}})
+\end{equation}
+
+we also need the ``slope'' of temperature versus humidity ratio on the psych chart between the inlet and outlet air conditions:
+
+\begin{equation}
+{S_{T,w}} = ({T_{air,in}} - {T_{air,out}})/({w_{air,in}} - {w_{air,out}})
+\end{equation}
+
+We now obtain the actual design apparatus dewpoint temperature by iterating over the following two equations:
+
+\begin{equation}
+{w_{air,dp,app}} = {\rm{PsyWFnTdpPb}}({T_{air,dp,app}},{P_{atm}})
+\end{equation}
+
+\begin{equation}
+{T_{air,dp,app}} = {T_{air,in}} - {S_{T,w}}({w_{air,in}} - {w_{air,dp,app}})
+\end{equation}
+
+The apparatus dewpoint enthalpy is then:
+
+\begin{equation}
+{h_{air,dp,app}} = {\rm{PsyHFnTdbW}}({T_{air,dp,app}},{w_{air,dp,app}})
+\end{equation}
+
+and the coil bypass factor is:
+
+\begin{equation}
+{F_{coilbypass}} = ({h_{air,out}} - {h_{air,dp,app}})/({h_{air,in}} - {h_{air,dp,app}})
+\end{equation}
+
+If the iterative procedure doesn't converge, or the coil bypass factor is too large (greater than 0.5), or the apparatus dewpoint enthalpy is less than the saturated air enthalpy at the water inlet temperature, the design outlet air conditions are reset to 90\% relative humidity at the same outlet enthalpy. The above design calculations are then repeated.
+
+We are now ready to calculate the design coil UA. This will be accomplished by inverting the simple coil calculation routine \emph{CoolingCoil} using the Regula Falsi method. First we make an initial estimate of the coil UA.
+
+\begin{equation}
+\Delta {h_{lmd}} = (({h_{air,in}} - {h_{w,sat,out}}) - ({h_{air,out}} - {h_{w,sat,in}}))/log(({h_{air,in}} - {h_{w,sat,out}}) - ({h_{air,out}} - {h_{w,sat,in}}))
+\end{equation}
+
+\begin{equation}
+U{A_{coil,enthalpy - based}} = {\dot Q_{coil}}/\Delta {h_{lmd}}
+\end{equation}
+
+\begin{equation}
+U{A_{coil,ext}} = {C_{p,air}}U{A_{coil,enthalpy - based}}
+\end{equation}
+
+We set the internal UA to 3.3 times the external UA (as a typical value for a coil). Then the total UA is:
+
+\begin{equation}
+  UA_{coil,tot} = \frac{1}{{(1/U{A_{coil,int}} + 1/U{A_{coil,ext}})}}
+\end{equation}
+
+The next step is to estimate the coil external heat transfer surface area. This is done in the function \emph{EstimateHEXSurfaceArea}:
+
+\begin{equation}
+Are{a_{coil,ext}} = {\rm{EstimateHEXSurfaceArea}}
+\end{equation}
+
+using the following assumptions:
+
+\begin{itemize}
+\item
+  Tube inside diameter = 0.0122 (m)
+\item
+  Tube side water velocity = 2.0 (m/s)
+\item
+  Inside to outside coil surface area ratio (Ai/Ao) = 0.07 (-)
+\item
+  Fins overall efficiency = 0.92 (-)
+\item
+  Aluminum fins, 12 fins per inch with fins to total outside surface area ratio of 90\%.
+\item
+  Airside combined heat and mass transfer coefficient = 140 (W/m2∙°C)
+\end{itemize}
+
+Interior and exterior U values (really UA's per unit exterior surface area) are calculated by dividing the above UA's by the area. The resulting U\(_{coil,ext}\) is assumed to be U\(_{coil,ext,wet}\); U\(_{coil,ext,dry}\) is set equal to U\(_{coil,ext,wet}\). We now have all the starting values needed for inverting the simple coil model using the chosen Regula Falsi iterative method. Once the iteration is completed, we have coil UA's and U's that yield the design outlet air and water enthalpies given the inlet design conditions and flow rates. Note that the simple coil model can not exactly match the specified design outlet air temperature and humidity ratio. It can only match the design air outlet enthalpy. Generally the simple coil model will yield outlet conditions near the saturation curve if any dehumidification is occuring. Typical outlet relative humidities are around 95\%.
+
+\subsubsection{Variable UA}\label{variable-ua}
+
+The above calculations yield coil UA's for the design inlet conditions and air and water flow rates. As the flow rates vary during the time step calculations, the UA's need to be adjusted, since coil UA's are a rather strong function of air and water side flow rates. Each time step the coil UA's are modified using the same formulas as are used in the hot water coil model. Refer to that model for the flow dependences.
+
+\subsubsection{Operating Block Calculations:}\label{operating-block-calculations}
+
+There are two modes of coil analysis in the operating block. They are the Simple analysis mode and the detailed analysis mode. The simple analysis mode assumes the coil to be either all wet or either all dry and execute the model , on the other hand the detailed mode checks for part wet part dry mode of operation and reports surface area wet fraction of coil, however the program execution time in detailed mode is noticeably higher.
+
+The operating block for Detailed Mode Analysis of this coil model is divided into three modes of coil performance. The modes being
+
+n~Coil is completely dry: There is no moisture condensation on the coil surface and the coil is a dry coil. This is an extreme condition when the entering air has very low humidity ratio or is dry air.
+
+n~Coil is completely wet: The entire coil is wet due to complete condensation on the surface of the coil.
+
+n~Part Wet Part Dry Mode: This is the usual/frequent mode of operation of coil, as shown in Figure~\ref{fig:energyplus-program-schematic}, where part of the coil at entry of air is dry and as air cools condensation occurs and part of the coil becomes wet.
+
+The Part Wet Part Dry Mode of operation is essentially a function the Coil Completely Dry and Coil Completely Wet mode. This subroutine iterates between the Dry Coil and the Wet Coil to give outputs, a detailed explanation is given later in the document. The operating block requires 5 inputs, which are mentioned earlier in the document. These inputs are automatically generated from the node connections in Energy Plus. The user does not have to input any information to run this coil model.
+
+The option to identify which mode of operation the coil should perform ie, for a given set of inputs would the coil be Dry, Wet or Part Wet Part Dry, is decided by set of conditions described below.
+
+n~\textbf{IF} (\textbf{Temperature Dewpoint Air \textless{} Water Inlet Temperature}) \textbf{THEN} the coil is Dry and we call the Subroutine Coil Completely Dry. ~In this case outlet temperature of air would be higher than the air dewpoint and hence there would be no condensation.
+
+n~\textbf{IF} (\textbf{Temperature Dewpoint Air \textgreater{} Water Inlet Temperature}) \textbf{THEN} the coil is completely wet, call subroutine Coil Completely Wet, it is assumed that moisture condensation occurs over completely surface of the coil. However we go ahead and check for the coil being partially wet with the following condition.
+
+n~\textbf{IF (AirDewPointTemp \textless{} AirInletCoilSurfTemp) THEN,} the coil is Partially Wet because there is possibility that air temperature will go below its dewpoint and moisture will condense on latter part of the cooling coil.
+
+The Operating Block for Simple Mode Analysis is divided into two modes of coil performance, the two modes being
+
+n~Coil is completely dry: There is no moisture condensation on the coil surface and the coil is a dry coil.
+
+n~Coil is completely wet: The entire coil is wet due to complete condensation on the surface of the coil.
+
+The option to identify which mode of operation the Simple mode analysis should perform ie, for a given set of inputs would the coil be Dry or Wet is decided by set of conditions described below.
+
+n~\textbf{IF} (\textbf{Temperature Dewpoint Air \textless{} Water Inlet Temperature}) \textbf{THEN} the coil is Dry and we call the Subroutine Coil Completely Dry.~ In this case outlet temperature of air would be higher than the air dewpoint and hence there would be no condensation.
+
+n~\textbf{IF} (\textbf{Temperature Dewpoint Air \textgreater{} Water Inlet Temperature}) \textbf{THEN} the coil is completely wet, call subroutine Coil Completely Wet, it is assumed that moisture condensation occurs over completely surface of the coil. However we go ahead and check for the coil being partially wet with the following condition.
+
+The above is a simple mode of analysis and the results are very slightly different from the detailed mode of analysis. The algorithms used in Simple mode and the Detailed mode are identically similar. The surface area wet fraction in the coil is reported as 1.0 or 0.0 for wet or dry coil respectively. The program defaults to simple mode of analysis for enabling higher execution speed.
+
+\subsubsection{Effectiveness Equations:}\label{effectiveness-equations}
+
+There are two modes of flow for the coil, Counter Flow mode or the Cross Flow mode, default set up is as cross flow since most air condition applications have cross flow heat exchangers. According to the mode of flow the following NTU - Effectiveness relationships are used to calculate coil effectiveness, which is used later by all the three modes (Dry, Wet, Part Wet) for calculating air outlet conditions and heat transfer.
+
+Following are the relations used for calculating effectiveness equation for the Heat exchangers.
+
+Counter Flow Heat Exchanger: Effectiveness Equation:
+
+\begin{equation}
+{\eta_{CounterFlow}} = \frac{{(1 - Exp( - NTU \times (1 - Rati{o_{StreamCapacity}})))}}{{1 - Rati{o_{StreamCapacity}} \times Exp( - NTU \times (1 - Rati{o_{StreamCapacity}}))}}
+\end{equation}
+
+In Equation ~ the variable Ratio\_StreamCapacity is defined as below
+
+\begin{equation}
+Rati{o_{StreamCapacity}} = \frac{{MinCapacit{y_{Stream}}}}{{MaxCapacit{y_{Stream}}}}
+\end{equation}
+
+In equation capacity of stream is defined as below in equation
+
+\begin{equation}
+(Min,Max)\,\,Capacit{y_{Stream}} = {(MassFlowRate \times Cp)_{air,water}}
+\end{equation}
+
+NTU in equation , is defined as the Number of Transfer Units, it is a function of Coil UA and the Minimum Capacity of Stream. The Coil UA is a variable in this equation and depends on which mode of the coil operation (Dry, Wet, Part Wet) is calling upon equation , i.e., if it is Coil Completely Dry calling upon the effectiveness equation with the value of Dry UA total, which in our case is defined as CoilUA\_total. Equation gives definition for NTU.
+
+\begin{equation}
+NTU = \frac{{CoilUA}}{{MinStrea{m_{Capacity}}}}
+\end{equation}
+
+Cross Flow Heat Exchanger: Effectiveness Equation:
+
+\begin{equation}
+{\eta_{CrossFlow}} = 1 - EXP\left\{ {\frac{{Exp( - NTU \times Rati{o_{StreamCapacity}} \times NT{U^{ - 0.22}}) - 1}}{{Rati{o_{StreamCapacity}} \times NT{U^{ - 0.22}}}}} \right\}
+\end{equation}
+
+The variables in the above equation have already been defined earlier. Depending on the mode of operation of the coil model the cross or the counter flow equations are used to calculate the effectiveness.
+
+\subsubsection{Coil Outlet Conditions:}\label{coil-outlet-conditions}
+
+Calculating the Outlet Stream Conditions using the effectiveness value from equation ~ or depending on the mode of flow. The energy difference between the outlet and inlet stream conditions gives the amount of heat transfer that has actually take place. Temperature of air and water at outlet to the coil is given as in following equations
+
+\begin{equation}
+TempAi{r_{Out}} = TempAi{r_{inlet}} - {\eta_{cross,counter}} \times \frac{{MaxHeatTransfer}}{{StreamCapacit{y_{Air}}}}
+\end{equation}
+
+\begin{equation}
+TempWate{r_{Out}} = TempWate{r_{Inlet}} + {\eta_{Cross,counter}} \times \frac{{MaxHeatTransfer}}{{StreamCapacit{y_{Water}}}}
+\end{equation}
+
+In the above equations and the maximum heat transfer is calculated as shown in the following equation
+
+\begin{equation}
+MaxHeatTransfer = MinStrea{m_{Capacity}} \times (TempAi{r_{Inlet}} - TempWate{r_{Inlet}})
+\end{equation}
+
+\subsubsection{Coil Completely Dry Calculations: (operating block)}\label{coil-completely-dry-calculations-operating-block}
+
+Since the coil is dry, the sensible load is equal to total load and the same with the humidity ratios at inlet and outlet, as in equations and .
+
+\begin{equation}
+QSensibl{e_{DryCoil}} = QTota{l_{DryCoil}}
+\end{equation}
+
+\begin{equation}
+HumRati{o_{Inlet}} = HumRati{o_{Outlet}}
+\end{equation}
+
+Total Heat Transfer in dry coil is as follows:
+
+\begin{equation}
+{Q_{TotalDryCoil}} = CapacityAir \times (AirTem{p_{In}} - AirTem{p_{Outlet}})
+\end{equation}
+
+The variables in the above equation are calculated earlier in equations and to give the total cooling load on the coil.
+
+\subsubsection{Coil Completely Wet Calculations: (operating block)}\label{coil-completely-wet-calculations-operating-block}
+
+In wet coil we need to account for latent heat transfer, hence calculations are done using enthalpy of air and water instead of stream temperatures Hence we need to define coil UA for the wet coil based on enthalpy of the operating streams and not design streams.
+
+Similar to equations and we calculate the air outlet enthalpy and water outlet enthalpy ie by replacing temperature with enthalpy of the respective streams. The input variable for Coil UA in equation for calculating NTU, in this case it would be enthalpy based and is given as shown in equation
+
+\begin{equation}
+CoilU{A_{\,Enthalpy\,Based}} = \frac{1}{{\left( {\frac{{CpSa{t_{Intermediate}}}}{{CoilU{A_{\,Internal}}}} + \frac{{C{p_{Air}}}}{{CoilU{A_{\,External}}}}} \right)}}
+\end{equation}
+
+Total Coil Load in case of Wet Coil is the product of mass flow rate of air and enthalpy difference between the inlet and outlet streams as given in the following equation
+
+\begin{equation}
+{Q_{Total}} = {\mathop M\limits^ *_{air}} \times (EnthAi{r_{Inlet}} - EnthAi{r_{Outlet}})
+\end{equation}
+
+Once the enthalpy is known the outlet temperatures and outlet humidity ratios of the wet coil are calculated as in equations below.
+
+\textbf{IF (TempCondensation \textless{} PsyTdpFnWPb(InletAirHumRat ,Patm)) THEN}
+
+\begin{equation}
+AirTem{p_{Out}} = AirTem{p_{inlet}} - (AirTem{p_{inlet}} - Condensatio{n_{Temp}}) \times \eta
+\end{equation}
+
+and
+
+\textbf{OutletAirHumdityRatio = PsyWFnTdbH(OutletAirTemp,EnthAirOutlet)}
+
+\textbf{ELSE}
+
+There is no condensation and hence the inlet and outlet Hum Ratios are equal , and outlet temperature is a function of outlet air enthalpy as below
+
+\textbf{OutletAirTemp~~~~~ = ~ PsyTdbFnHW (EnthalpyAirOutlet, OutletAirHumRat)}
+
+\textbf{and}
+
+\textbf{OutletAirHumRat~ = ~ InletAirHumRat}
+
+\textbf{ENDIF}
+
+Effectiveness η used in equation is defined in equation and Condensation Temperature is calculated using psychrometric function as in equation .
+
+\begin{equation}
+\eta  = 1 - Exp\left\{ { - \frac{{CoilU{A_{\,External}}}}{{Capacitanc{e_{Air}}}}} \right\}
+\end{equation}
+
+\begin{equation}
+Condensatio{n_{Temp}} = {\rm{PsyTsatFnHPb(Ent}}{{\rm{h}}_{{\rm{AirCondensateTemp}}}}{\rm{,Patm) }}
+\end{equation}
+
+\begin{equation}
+Ent{h_{\,AirCondensateTemp}} = Ent{h_{\,AirInlet}} - \frac{{\left( {Ent{h_{\,AirInlet}} - Ent{h_{\,AirOutlet}}} \right)}}{\eta }
+\end{equation}
+
+Once the air outlet temperature are known, then sensible load is calculated as a product of capacitance of air and temperature difference at inlet and outlet, as in equation
+
+\begin{equation}
+{Q_{Sensible}} = Capacitanc{e_{Air}} \times \left( {AirTem{p_{Inlet}} - AirTem{p_{Outlet}}} \right)
+\end{equation}
+
+\subsubsection{Coil Part Wet Part Dry Calculations: (operating block)}\label{coil-part-wet-part-dry-calculations-operating-block}
+
+The Coil would perform under part wet part dry conditions when Air Dewpoint Temperature is less than Coil surface temperature at inlet to air. In this case part of the coil used value of Dry UA for heat transfer and part the coil used Wet UA value for heat transfer.
+
+This problem is solved utilizing the fact that the Exit conditions from the Dry Part of the Coil would become the inlet conditions to the wet part of the coil (see Figure~\ref{fig:simplified-schematic-of-coolingdehumidifying}) and the coil model determines by iteration what fraction of the coil is wet and based on that it calculates the areas and subsequently the UA values of that dry and wet part, based on the area of the dry and wet part respectively. Explained below are the steps followed to the estimating the wet dry behavior of the coil.
+
+n~Iterate between the Dry Coil and the Wet Coil. First calculate Coil Completely Dry performance by estimating the wet dry interface water temperature using equation and inputting this variable as the water inlet temperature to dry Coil.
+
+\(WetDryInterfac{e_{WaterTemp}} = {\rm{WaterTem}}{{\rm{p}}_{{\rm{Inlet}}}}{\rm{ + Are}}{{\rm{a}}_{{\rm{WetFraction}}}}{\rm{*(WaterTem}}{{\rm{p}}_{{\rm{Outlet}}}}{\rm{ - WaterTem}}{{\rm{p}}_{{\rm{Inlet}}}}{\rm{)}}\) ~~~
+
+The value of Surface Area Wet fraction is estimated initially as follows
+
+\begin{equation}
+Are{a_{\,WetFractionEstimate}} = \frac{{AirDewP{t_{\,Temp}} - InletWate{r_{\,Temp}}}}{{OutletWate{r_{\,Temp}} - InletWate{r_{\,Temp}}}}
+\end{equation}
+
+For the above mentioned iteration the value of Coil UA for Wet and Dry part need to be varied according to the new respective area of the wet and dry parts. This estimate of Wet and Dry area is a product of the estimated Surface Area Fraction and total coil external area, which keeps varying as will be explained further in the document.
+
+UA value for Dry part of the Coil is estimated as below.
+
+\begin{equation}
+CoilU{A_{Dry\,External}} = \frac{{SurfAre{a_{Dry}}}}{{\frac{1}{{Coil{U_{Dry\,External}}}} + \frac{1}{{Coil{U_{Internal}}}}}}
+\end{equation}
+
+Where Surface Area Dry = (Total Coil Area -- Wet Part Area), where the Wet part area is the product of Surface fraction Wet and Total Coil Area.
+
+UA value for the Wet part of the Coil requires Wet UA external and Wet UA Internal, which are calculated as below.
+
+\begin{equation}
+WetPartUA{\,_{External}} = Coil{U_{Wet\,External}} \times SurfaceAreaWet
+\end{equation}
+
+\begin{equation}
+WetPartUA{\,_{Internal}} = Coil{U_{Internal}} \times SurfaceAreaWet
+\end{equation}
+
+It is essential to remember that the mode of calculation for the coils remains the same as in completely wet and completely dry mode, only the UA values and water, air outlet and inlet values change.
+
+Now Iterate between the Dry Coil and wet Coil with the above respective UA, and usual operating inputs except the variable water inlet temperature for dry Coil is replaced with Wet Dry Interface Water temperature, and in the Wet Coil the Outlet Air Temperature from dry Coil is the inlet air temperature to Wet Coil. The iteration proceeds till the Outlet Water Temperature from Wet Coil equals the Wet Dry Interface Water Temp, which is the input to Dry Coil.
+
+Dry Part Inputs: (changed operating inputs) :Iteration Case 1: Explained In Programming Fashion:
+
+\textbf{CALL CoilCompletelyDry (WetDryInterfcWaterTemp, InletAirTemp, DryCoilUA,~~~~~~~~~~~~~~ \&}
+
+\textbf{~~~~~~~~~~~~~~~~~~~~~~~~~~~~ OutletWaterTemp, WetDryInterfcAirTemp, WetDryInterfcHumRat,~~~~~~~ \&}
+
+\textbf{DryCoilHeatTranfer).}
+
+Input the calculated values calculated by Dry Coil above into Wet Coil below. The variables have been highlighted in color red and blue.
+
+\textbf{CALL}CoilCompletelyWet (InletWaterTemp, \textbf{WetDryInterfcAirTemp}, \textbf{WetDryInterfcHumRat}
+
+WetPartUAInternal,WetPartUAExternal,~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \&
+
+\textbf{EstimateWetDryInterfcWaterTemp}, OutletAirTemp, OutletAirHumRat,~~~ \&
+
+WetCoilTotalHeatTransfer, WetCoilSensibleHeatTransfer,~~~~~~~~~~~~~~~~~~~~~~ \&
+
+EstimateSurfAreaWetFraction, WetDryInterfcSurfTemp)
+
+Iterate Between the above two Wet and Dry Coil calls until the two variables in blue ie \textbf{WetDryInterfcWaterTemp = EstimateWetDryInterfcWaterTemp.}The key is to have the difference between the variables (WetDryInterfcWaterTemp -- OutletWaterTemp) in Dry Coil equal to (InletWaterTemp-EstimatedWetDryInterfcWaterTemp) in Wet Coil. This equality quantized the relative part of coil that is dry and part that is wet on the basis of heat transfer that has occurred.
+
+After the above convergence check for the coil being dry otherwise iterate to calculate surface fraction area wet.
+
+\textbf{IF}
+
+\begin{equation}
+\left\{ {(AreaFractio{n_{Wet}} \le \,0.0)\,\,and(WetDryInterfac{e_{SurfTemp}} > AirDewPt)} \right\}
+\end{equation}
+
+\textbf{THEN CoilCompletelyDry}
+
+If equation is satisfied then Coil is Dry and simply output the value for Dry Coil calculated else the coil is partially wet and then iterate to find the surface fraction area wet. Start with the initially guess value of surface area fraction (equation wet and iterate on the entire loop starting from until the Wet Dry Interface Temperature equals the Air Dewpoint Temperature. The value of Surface Area fraction wet at which the interface air temperature equals is dewpoint is the transition point from wet to dry and gives the \% of coil that is dry and \% that is wet.
+
+Graphs Showing the Performance of the coil model at optimum operating conditions are shown below. All values of variable used have been normalized.
+
+\begin{figure}[hbtp] % fig 163
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3348.png}
+\caption{Air Outlet Temperature Vs Air Mass Flow Rate \protect \label{fig:air-outlet-temperature-vs-air-mass-flow-rate}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 164
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3349.png}
+\caption{Sensible Load variations Vs Air mass Flow Rate \protect \label{fig:sensible-load-variations-vs-air-mass-flow}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 165
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3350.png}
+\caption{Total and Sensible Load variations Vs Air Mass Flow Rate \protect \label{fig:total-and-sensible-load-variations-vs-air}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 166
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3351.png}
+\caption{Surface Area Fraction Wet Vs Air Mass Flow Rate \protect \label{fig:surface-area-fraction-wet-vs-air-mass-flow}}
+\end{figure}
+
+\subsubsection{References}\label{references-011}
+
+IBPSA BuildSim-2004. 2004. Colarado Boulder: An Improvement of Ashrae Secondary HVAC toolkit Simple Cooling Coil Model for Building Simulation, Rahul J Chillar, Richard J Liesen M\&IE ,UIUC.
+
+Stoecker, W.F. \textless{}dates unspecified\textgreater{} Design of Thermal Systems,: ME 423 Class Notes , M\& IE Dept UIUC.
+
+Brandemeuhl, M. J. 1993. HVAC2 Toolkit: Algorithms and Subroutines for Secondary HVAC Systems Energy Calculations, ASHRAE.
+
+Elmahdy, A.H. and Mitalas, G.P.~ 1977. ``A Simple Model for Cooling and Dehumidifying Coils for Use In Calculating Energy Requirements for Buildings ASHRAE Transactions, Vol.83 Part 2, pp.~103-117.
+
+Threlkeld, J.L.~ 1970.~ Thermal Environmental Engineering, 2nd Edition, Englewood Cliffs: Prentice-Hall,Inc. pp.~254-270.
+
+ASHRAE Secondary HVAC Toolkit TRNSYS.~ 1990.~ A Transient System Simulation Program: Reference Manual. Solar Energy Laboratory, Univ. Wisconsin-Madison, pp.~4.6.8-1 - 4.6.8-12.
+
+Kays, W.M. and A.L. London. 1964. Compact Heat Exchangers, 2nd Edition, New York: McGraw-Hill.
+
+Clark, D.R.. 1985. HVACSIM+ Building Systems and Equipment Simulation Program Reference Manual, Pub. No. NBSIR 84-2996, National Bureau of Standards, U.S. Department of Commerce, January, 1985
+
+Elmahdy, A.H. 1975. Analytical and Experimental Multi-Row Finned-Tube Heat Exchanger Performance During Cooling and Dehumidifying Processes, Ph.D.~Thesis, Carleton University, Ottawa, Canada, December, 1975.
+
+Elmahdy, A.H., and Mitalas, G.P. 1977. ``A Simple Model for Cooling and Dehumidifying Coils for Use in Calculating Energy Requirements for Buildings,'' ASHRAE Transactions, Vol.~ 83, Part 2, pp.~103-117.
+
+\subsection{Chilled-Water-Based Detailed Geometry Air Cooling Coil}\label{chilled-water-based-detailed-geometry-air-cooling-coil}
+
+The input object Coil:Cooling:Water:DetailedGeometry provides a coil model that predicts changes in air and water flow variables across the coil based on the coil geometry. A greatly simplified schematic of enthalpy and temperature conditions in a counterflow cooling/dehumidifying coil is shown in the following schematic figure. In addition, the variables required to model a cooling/dehumidifying coils and their definitions are extensively listed in ``Table~\ref{table:coil-geometry-and-flow-variables-for-coils}. Coil Geometry and Flow Variables for Coils''. The input required to model the coil includes a complete geometric description that, in most cases, should be derivable from specific manufacturer's data.~ The coil simulation model is essentially the one presented by Elmahdy and Mitalas (1977) and implemented in HVACSIM+ (Clark 1985), a modular program also designed for energy analysis of building systems. The model solves the equations for the dry and wet sections of the coil using log mean temperature and log mean enthalpy differences between the liquid and the air streams.~ Elmahdy and Mitalas state that crossflow counterflow coils with at four rows or more are approximated well by this model.~ This does not constitute a major limitation since cooling and dehumidifying coils typically have more than four rows.
+
+\begin{figure}[hbtp] % fig 167
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3352.svg.png}
+\caption{Simplified Schematic of Cooling/Dehumidifying Coil \protect \label{fig:simplified-schematic-of-coolingdehumidifying-001}}
+\end{figure}
+
+\subsubsection{Heat Transfer and Energy Balance}\label{heat-transfer-and-energy-balance-1}
+
+The cooling coil may be completely dry, completely wet with condensation, or it may have wet and dry sections.~ The actual condition of the coil surface depends on the humidity and temperature of the air passing over the coil and the coil surface temperature.~ The partly wet-partly dry case represents the most general scenario for the coil surface conditions.~ The all dry and all wet cases can be considered as limiting solutions of the wet or dry areas respectively going to zero.~ In the general case, equations are written for both the dry and wet regions of the coil.~ For each region the heat transfer rate from air to water may be defined by the rate of enthalpy change in the air and in the water.~ The rates must balance between each medium for energy to be conserved.~ Equations through express the energy balance between the water and the air for the case of dry and wet coils respectively.~ Equations and represent the heat transfer rate between water and air based on the actual performance of the coil.~ The UA parameter can be calculated from the parameters in the following table.
+
+% table 55
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Coil Geometry and Flow Variables for Coils \label{table:coil-geometry-and-flow-variables-for-coils}} \tabularnewline
+\toprule 
+A & area & LMHD & log mean enthalpy difference \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Coil Geometry and Flow Variables for Coils} \tabularnewline
+\toprule 
+A & area & LMHD & log mean enthalpy difference \tabularnewline
+\midrule
+\endhead
+
+A & air, air side & LMTD & log mean temperature difference \tabularnewline
+aa, bb & coeff. in enthalpy approximation & $\dot m$ & mass flow rate \tabularnewline
+C1, C2 & coeff. in air side film coeff. & mf & metal and fouling \tabularnewline
+Cp & specific heat & $\mu$ & viscosity \tabularnewline
+D & diameter, effective diameter & o & outside (air side) \tabularnewline
+Dhdr & hydraulic diameter on air side & Pr & Prandtl number \tabularnewline
+D & dry region & $\dot Q$ & heat transfer rate \tabularnewline
+$\delta$ & thickness & R & overall thermal resistance \tabularnewline
+$\Delta$ & spacing & Re & Reynolds number \tabularnewline
+F & heat transfer film coefficient & $\rho$ & ratio of diameters \tabularnewline
+Fai & variable in fin eff. calculation & s & surface, outside of metal \tabularnewline
+fin, fins & air side fin geometry & St & Stanton number \tabularnewline
+H & enthalpy & T & temperature \tabularnewline
+$\eta$ & efficiency & tube & water tube \tabularnewline
+I0() & mod Bessel fn, 1st kind, ord 0 & UAdry & dry heat xfer coeff. * dry area \tabularnewline
+I1() & mod Bessel fn, 1st kind, ord 1 & UcAw & wet heat xfer coeff. * wet area \tabularnewline
+K0() & mod Bessel fn, 2nd kind, ord 0 & ub, ue & variables in fin eff. calculation \tabularnewline
+K1() & mod Bessel fn, 2nd kind, ord 1 & V & average velocity \tabularnewline
+I & inside (water side) & w & water, water side, or wet region \tabularnewline
+K1 & variable in sol'n form of eq. & wa & humidity ratio \tabularnewline
+K & thermal conductivity & Z & variables in sol'n form of eq. \tabularnewline
+L & length & 1, 2, 3 & positions (see diagram) \tabularnewline
+\bottomrule
+\end{longtable}
+
+Equations through represent two sets of three equations with 7 unknowns: \({\dot Q_d}\) , Ta,1, Ta,2, Tw,2, Tw,3, \({\dot m_a}\) , \({\dot m_w}\) .~However, normally at least four of these variables are specified, for example: inlet water temperature, outlet air temperature, water flow rate, air flow rate, so that the system of equations is effectively closed.
+
+\begin{equation}
+{\dot Q_d} = {m_a}C{p_a}\left( {{T_{a,1}} - {T_{a,2}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_d} = {m_w}C{p_w}\left( {{T_{w,3}} - {T_{w,2}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_d} = \left( {U{A_{dry}}} \right)\left( {LMTD} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_w} = {m_a}\left( {{H_{a,2}} - {H_{a,3}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_w} = {m_w}C{p_w}\left( {{T_{w,2}} - {T_{w,1}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_w} = \left( {{U_c}{A_w}} \right)\left( {LMHD} \right)
+\end{equation}
+
+In order to manipulate these equations, the log mean temperature and enthalpy differences are expanded as shown in Equations and .~ Finally, a linear approximation of the enthalpy of saturated air over the range of surface temperature is made using Equation .~ Note that in Equation Hw~refers to the enthalpy of saturated air at the water temperature.
+
+\begin{equation}
+LMTD = \frac{{\left( {{T_{a,1}} - {T_{w,3}}} \right) - \left( {{T_{a,2}} - {T_{w,2}}} \right)}}{{\ln \frac{{{T_{a,1}} - {T_{w,3}}}}{{{T_{a,2}} - {T_{w,2}}}}}}
+\end{equation}
+
+\begin{equation}
+LMHD = \frac{{\left( {{H_{a,2}} - {H_{w,2}}} \right) - \left( {{H_{a,3}} - {H_{w,1}}} \right)}}{{\ln \frac{{{H_{a,2}} - {H_{w,2}}}}{{{H_{a,3}} - {H_{w,1}}}}}}
+\end{equation}
+
+\begin{equation}
+{H_w} = aa + bb {T_w}
+\end{equation}
+
+Equation is derived from the above equations and is used to solve for the coil conditions when all of the inlet conditions are given as input.~ Operating in this manner, the coil does not have a controlled outlet air temperature.
+
+\begin{equation}
+{T_{w,2}} = \frac{{\left( {1 - Z} \right)\left( {{H_{a,1}} - aa - K1 C{p_a} {T_{a,1}}} \right) + Z {T_{w,1}}\left( {bb - \frac{{{m_w}C{p_w}}}{{{m_a}}}} \right)}}{{bb - Z\frac{{{m_w}C{p_w}}}{{{m_a}}} - \left( {1 - Z} \right) K1 C{p_a}}}
+\end{equation}
+
+An alternative solution method is to define the coil leaving air temperature as an input with a variable water flow rate.~ In this case Equations and are more convenient.~ Equations through define terms that are used to simplify Equations , and .
+
+\begin{equation}
+{T_{w,2}} = \frac{{\left( {1 - Z} \right)\left( {{H_{a,3}} - aa} \right) + {T_{w,1}}\left( {\frac{{{m_w}C{p_w}}}{{{m_a}}} - bb Z} \right)}}{{\frac{{{m_w}C{p_w}}}{{{m_a}}} - bb}}
+\end{equation}
+
+\begin{equation}
+{T_{w,2}} = \frac{{\left( {{Z_d} - 1} \right){T_{a1}}C{p_a} + {T_{w,3}}\left( {C{p_a} - {Z_d}\frac{{{m_w}C{p_w}}}{{{m_a}}}} \right)}}{{{Z_d}\left( {C{p_a} - \frac{{{m_w}C{p_w}}}{{{m_a}}}} \right)}}
+\end{equation}
+
+\begin{equation}
+Z = exp\left( {{U_c}{A_w}\left( {\frac{1}{{{m_a}}} - \frac{{bb}}{{{m_w}C{p_w}}}} \right)} \right)
+\end{equation}
+
+\begin{equation}
+K1 = \frac{{{Z_d} - 1}}{{{Z_d} - \frac{{{m_a}C{p_a}}}{{{m_w}C{p_w}}}}}
+\end{equation}
+
+\begin{equation}
+{Z_d} = exp\left( {{U_c}{A_{dry}}\left( {\frac{1}{{{m_a}C{p_a}}} - \frac{1}{{{m_w}C{p_w}}}} \right)} \right)
+\end{equation}
+
+\subsubsection{Underlying Correlations, Properties, and Assumptions}\label{underlying-correlations-properties-and-assumptions}
+
+Overall heat transfer coefficients are calculated from the specified coil geometry and by using empirical correlations from fluid mechanics and heat transfer.~ For the water side, Equation gives the film heat transfer coefficient in SI units:
+
+\begin{equation}
+{f_i} = 1.429\left( {1 + 0.0146 {T_w}} \right)V_w^{0.8}D_i^{ - 0.2}
+\end{equation}
+
+This is valid for Reynolds numbers greater than 3100 based on water flow velocity and pipe inside diameter and is given in Elmahdy and Mitalas(1977) as recommended in the standard issued by the Air-Conditioning and Refrigeration Institute (1972) for air-cooling coils.~ The definition of overall inside thermal resistance follows directly as shown in Equation.
+
+\begin{equation}
+{R_i} = \frac{1}{{{f_i}{A_i}}}
+\end{equation}
+
+Equation gives the film coefficient for the air side.~ Another form of the same equation is Equation , which is familiar from the data presented in Kays and London (1984).~ For coil sections that have a wet surface due to condensation, the air side film coefficient is modified according to Equation .~ The correction term, a function of air Reynolds number, is valid for Reynolds numbers between 400 and 1500.~ The coefficients in Equation and are calculated by Equations and that are functions of the coil geometry.~ Elmahdy (1977)explains the modifier for the wet surface and coefficients for the film coefficient.~ Equations through show definitions and values of common parameters and properties.
+
+\begin{equation}
+  f_o = C_1 Re_a^{C_2} \frac{m_a}{A_{a_min_flow}} C_{p,a} Pr_a^{2/3}
+\end{equation}
+
+\begin{equation}
+  C_1 Re_a^{C_2} = St_a Pr_a^{2/3}
+\end{equation}
+
+\begin{equation}
+{f_{o,w}} = {f_o}\left( {1.425 - 5.1 \times {{10}^{ - 4}}R{e_a} + 2.63 \times {{10}^{ - 7}}Re_a^2} \right)
+\end{equation}
+
+\begin{equation}
+{C_1} = 0.159{\left( {\frac{{{\delta_{fin}}}}{{{D_{hdr}}}}} \right)^{ - 0.065}}{\left( {\frac{{{\delta_{fin}}}}{{{L_{fin}}}}} \right)^{0.141}}
+\end{equation}
+
+\begin{equation}
+{C_2} =  - 0.323{\left( {\frac{{{\Delta_{fins}}}}{{{L_{fin}}}}} \right)^{0.049}}{\left( {\frac{{{D_{fin}}}}{{{\Delta_{tube_rows}}}}} \right)^{0.549}}{\left( {\frac{{{\delta_{fin}}}}{{{\Delta_{fins}}}}} \right)^{ - 0.028}}
+\end{equation}
+
+\begin{equation}
+{D_{hdr}} = \frac{{4{A_{a_min_flow}}{\delta_{coil}}}}{{{A_{s_total}}}}
+\end{equation}
+
+\begin{equation}
+R{e_a} = \frac{{4{\delta_{coil}}\left( {1 + {w_a}} \right){m_a}}}{{{A_{s_total}}{\mu_a}}}
+\end{equation}
+
+\begin{equation}
+P{r_a} = 0.733
+\end{equation}
+
+\begin{equation}
+{\mu_a} = 1.846 \times {10^{ - 5}}
+\end{equation}
+
+The film coefficients above act on the extended surface of the air side, that is the area of the fins and the tubes.~ Therefore, the fin efficiency must also be considered in calculating the overall thermal resistance on the outside.~ Gardner(1945) gives the derivation of Equation , used as a curve fit to find the fin efficiency as a function of film coefficient.~ This equation is based on circular fins of constant thickness.~ To model a coil with flat fins, an effective diameter -- that of circular fins with the same fin area -- is used.~ Equations through define variables used in Equation .~ The overall efficiency of the surface is shown by Equation .~ Note that the efficiency is found by the same equations for the wet surface using the wet surface film coefficient.
+
+\begin{equation}
+{\eta_{fin}} = \frac{{ - 2\rho }}{{fai(1 + \rho )}}\left[ {\frac{{{I_1}({u_b}){K_1}({u_e}) - {K_1}({u_b}){I_1}({u_e})}}{{{I_0}({u_b}){K_1}({u_e}) + {K_0}({u_b}){I_1}({u_e})}}} \right]
+\end{equation}
+
+\begin{equation}
+fai = \frac{{({D_{fin}} - {D_{tube}})}}{2}\sqrt {\frac{{2{f_o}}}{{{k_{fin}}{\delta_{fin}}}}}
+\end{equation}
+
+\begin{equation}
+\rho  = \frac{{{D_{tube}}}}{{{D_{fin}}}}
+\end{equation}
+
+\begin{equation}
+{u_e} = \frac{{fai}}{{1 - \rho }}
+\end{equation}
+
+\begin{equation}
+{u_b} = {u_e}\rho
+\end{equation}
+
+\begin{equation}
+{\eta_o} = 1 - (1 - {\eta_{fin}})\frac{{{A_{fins}}}}{{{A_{s_total}}}}
+\end{equation}
+
+The definition of overall outside thermal resistance is given in Equation as a function of fin efficiency and film coefficient.~ For a wet coil surface the resistance must be defined differently because the heat transfer equations are based on enthalpy rather than temperature differences, as shown in Equation .
+
+\begin{equation}
+{R_o} = \frac{1}{{{f_o}{\eta_o}{A_{s,total}}}}
+\end{equation}
+
+\begin{equation}
+  R_{o,w} = \frac{C_{p,a}/bb}{f_{o,w}\eta_{o,w}A_{s,total}}
+\end{equation}
+
+Equation gives the last two overall components of thermal resistance.~ They represent the metal tube wall and internal fouling.~ The fouling factor, due to deposits of dirt and corrosion of the tube inside surfaces, is assumed to be 5x10-5~m2·K/W.~ All components of thermal resistance are added in series to produce the overall heat transfer coefficients shown in Equations and .
+
+\begin{equation}
+{R_{mf}} = \frac{{{\delta_{tube}}}}{{{k_{tube}}{A_i}}} + \frac{{Fl}}{{{A_i}}}
+\end{equation}
+
+\begin{equation}
+U{A_{dry}} = \frac{{{A_{dry}}}}{{{A_{s,total}}}}\left[ {\frac{1}{{{R_i} + {R_{mf}} + {R_o}}}} \right]
+\end{equation}
+
+\begin{equation}
+{U_c}{A_w} = \frac{{{A_w}}}{{{A_{s,total}}}}\left[ {\frac{{{1 \mathord{\left/ {\vphantom {1 {bb}}} \right. } {bb}}}}{{{R_i} + {R_{mf}} + {R_{o,w}}}}} \right]
+\end{equation}
+
+\subsubsection{Solution Method of Model}\label{solution-method-of-model}
+
+The complicated equations derived above were implemented in a successive substitution solution procedure to calculate the coil performance based on the input parameters.~ The MODSIM implementation of a cooling coil, the TYPE12 subroutine, was the motivation for this approach; the method used there has been retained with modifications for the uncontrolled coil model.~ Clark (1985) contains notes about the MODSIM routine.
+
+In the general case, the cooling coil is only partially wet.~ For an uncontrolled coil, Equation~ is used to find the water temperature at the boundary.~ Several simple equations in the loop adjust the boundary point until the dry surface temperature at the boundary is equal to the dewpoint of the inlet air.~ For the controlled coil, Equations and give two calculations of the boundary temperature, and the water flow rate and boundary position are adjusted until the two equations agree.
+
+Special cases occur when the coil is all wet or all dry.~ The coil is solved as if it were all wet before the general case is attempted.~ If the wet surface temperatures at the coil inlet and outlet are both below the dewpoint, no further solution is required.~ However, to ensure a continuous solution as flow variables are changed, when the surface is all dry or when it is wet with only the dry surface equations yielding a surface temperature below the dewpoint at the water outlet, the general solution is used to calculate the unknowns.~ In the solution of the controlled coil the outlet air enthalpy, given some resulting dehumidification, must correspond to the enthalpy at the specified outlet air temperature.
+
+\subsubsection{Application of Cooling Coil Model to Heating Coils}\label{application-of-cooling-coil-model-to-heating-coils}
+
+The implementation of detailed heating coil models in IBLAST was another important aspect of the system/plant integration.~ The same kind of loops exist to provide hot water to the heating coils from the boilers as exist to supply the cooling coils with chilled water from the chillers.~~ Some simplifications can be made, however, since the enthalpy change of the air flowing over a heating coil is entirely sensible.~ There is no condensation in a heating coil.~ In order to allow heating and cooling coils to be specified using the same geometric parameters, a heating coil simulation was developed from the cooling coil model described above by eliminating the wet surface analysis.
+
+In addition, it was concluded that, since much simpler and less computationally expensive heating coil simulations are possible, an option was provided in IBLAST for a heating coil design using only the UA value of the coil, the product of heat transfer coefficient and coil area.~ This model was largely based on the TYPE10 subroutine implemented in MODSIM.~ The equations used to model the performance of the TYPE10 heating coil are as follows:
+
+\begin{equation}
+  \begin{array}{rl} 
+    T_{a,out} & = T_{a,in} + \left( T_{w,in} - T_{ain} \right) \varepsilon \left( \frac{\min \left( C_{p,a} \dot m_a,C_{p,w}\dot m_w \right)} {C_{p,a}\dot m_a} \right) \\
+    T_{w,out} & = T_{w,in} - \left( T_{a,out} - T_{ain} \right) \left( \frac{C_{p,a}\dot m_a}{C_{p,w}\dot m_w} \right)
+  \end{array}
+\end{equation}
+
+where the coil effectiveness is given by:
+
+\begin{equation}
+\varepsilon  = 1 - \exp \left( {\frac{{\left\{ {\exp \left[ { - \left( {\frac{{\min \left\{ {{C_{p,a}}{{\dot m}_a},{C_{p,w}}{{\dot m}_w}} \right\}}}{{\max \left\{ {{C_{p,a}}{{\dot m}_a},{C_{p,w}}{{\dot m}_w}} \right\}}}} \right){{\left\{ {NTU} \right\}}^{0.78}}} \right] - 1} \right\}}}{{\left( {\frac{{\min \left\{ {{C_{p,a}}{{\dot m}_a},{C_{p,w}}{{\dot m}_w}} \right\}}}{{\max \left\{ {{C_{p,a}}{{\dot m}_a},{C_{p,w}}{{\dot m}_w}} \right\}}}} \right){{\left\{ {NTU} \right\}}^{ - .22}}}}} \right)
+\end{equation}
+
+The parameter NTU is the number of transfer units and is defined as a function of the UA value of the coil as follows:
+
+\begin{equation}
+{\rm{NTU}} = \frac{{{\rm{UA}}}}{{{\rm{min}}\left( {{{\rm{C}}_{{\rm{p,a}}}}{{{\rm{\dot m}}}_{\rm{a}}}{\rm{,}}{{\rm{C}}_{{\rm{p,w}}}}{{{\rm{\dot m}}}_{\rm{w}}}} \right)}}
+\end{equation}
+
+\subsection{Hot-Water-Based Air Heating Coil}\label{hot-water-based-air-heating-coil}
+
+\subsubsection{Overview}\label{overview-010}
+
+The input object Coil:Heating:Water provides a model that uses an NTU--effectiveness model of a static heat exchanger. The model is an inlet -- outlet model: given the inlet conditions and flow rates and the UA, the effectiveness is calculated using the formula for the effectiveness of a cross-flow heat exchanger with both fluid streams unmixed. The effectiveness then allows the calculation of the outlet conditions from the inlet conditions.
+
+The inputs to the model are: (1) the current inlet temperatures and flow rates of the air and water fluid streams and (2) the UA of the coil. Note that the UA is fixed in this model and is not a function of the flow rates.
+
+There are 2 alternative user inputs for the component: the user may input the design water volumetric flow rate and the UA directly; or the user may choose to input the more familiar design heating capacity plus design inlet \& outlet temperatures and let the program calculate the design UA. These alternative user inputs are fully described in the EnergyPlus Input Output Reference document.
+
+\subsubsection{Model Description}\label{model-description-1-004}
+
+The air and water capacitance flows are defined as:
+
+\begin{equation}
+{\dot C_{air}} = {c_{p,air}}\cdot {\dot m_{air}}
+\end{equation}
+
+\begin{equation}
+{\dot C_{water}} = {c_{p,water}}\cdot {\dot m_{water}}
+\end{equation}
+
+The minimum and maximum capacity flows are then:
+
+\begin{equation}
+{\dot C_{\min }} = \min ({\dot C_{air}},{\dot C_{water}})
+\end{equation}
+
+\begin{equation}
+{\dot C_{\max }} = \max ({\dot C_{air}},{\dot C_{water}})
+\end{equation}
+
+The capacitance flow ratio is defined as:
+
+\begin{equation}
+Z = {\dot C_{\min }}/{\dot C_{\max }}
+\end{equation}
+
+The number of transfer units (\emph{NTU}) is:
+
+\begin{equation}
+NTU = UA/{\dot C_{\min }}
+\end{equation}
+
+The effectiveness is:
+
+\begin{equation}
+\varepsilon  = 1 - \exp (\frac{{{e^{ - NTU \cdot Z \cdot \eta }} - 1}}{{Z \cdot \eta }})
+\end{equation}
+
+Where \(\eta = NT{U^{ - 0.22}}\) .
+
+The outlet conditions are then:
+
+\begin{equation}
+{T_{air,out}} = {T_{air,in}} + \varepsilon \cdot {\dot C_{\min }}\cdot ({T_{water,in}} - {T_{air,in}})/{\dot C_{air}}
+\end{equation}
+
+\begin{equation}
+{T_{water,out}} = {T_{water,in}} - {\dot C_{air}}\cdot ({T_{air,out}} - {T_{air,in}})/{\dot C_{water}}
+\end{equation}
+
+The output of the coil in watts is:
+
+\begin{equation}
+{\dot Q_{coil}} = {\dot C_{water}}\cdot ({T_{water,in}} - {T_{water,out}})
+\end{equation}
+
+The UA value is recalculated for each timestep.~ A nominal UA, \emph{UA\(_{0}\)}, at the rating point is calculated by the program using the input for rated conditions and a search routine called regula falsi.
+
+User input for the ratio of convective heat transfers at the nominal or rated operating point, ``\emph{r},'' is used in the model.~ This ratio is defined as
+
+\begin{equation}
+r = \frac{{{\eta_f}{{\left( {hA} \right)}_{air}}}}{{{{\left( {hA} \right)}_{water}}}}
+\end{equation}
+
+where,
+
+~~~~~ \({\eta_f}\) ~is the fin efficiency, (dimensionless)
+
+~~~~~ \emph{h} is the surface convection heat transfer coefficient
+
+\emph{~~~~~ A} is the surface area
+
+The value calculated for \emph{UA\(_{0}\)} is used with the input for \emph{r} to characterize the convective heat transfer on the water sides at the nominal rating operation point using
+
+\begin{equation}
+{\left( {{{\left( {hA} \right)}_w}} \right)_0} = U{A_0}\left( {\frac{{r + 1}}{r}} \right)
+\end{equation}
+
+and on the air side at the nominal rating point using
+
+\begin{equation}
+{\left( {{\eta_f}{{\left( {hA} \right)}_a}} \right)_0} = r{\left( {hA} \right)_{w,0}}
+\end{equation}
+
+Then the following equations are used to calculate a new UA as a function of the flow rates and inlet temperatures at each timestep.
+
+\begin{equation}
+{x_a} = 1 + 4.769\cdot {10^{ - 3}}\left( {{T_{air,in}} - {T_{air,in,0}}} \right)
+\end{equation}
+
+\begin{equation}
+{\eta_f}{\left( {hA} \right)_a} = {x_a}{\left( {\frac{{{{\dot m}_a}}}{{{{\dot m}_{a,0}}}}} \right)^{0.8}}{\left( {{\eta_f}{{\left( {hA} \right)}_a}} \right)_0}
+\end{equation}
+
+\begin{equation}
+{x_w} = 1 + \left( {\frac{{0.014}}{{1 + 0.014{T_{water,in,0}}}}} \right)\;\left( {{T_{water,in}} - {T_{water,in,0}}} \right)
+\end{equation}
+
+\begin{equation}
+{\left( {hA} \right)_w} = {x_w}{\left( {\frac{{{{\dot m}_w}}}{{{{\dot m}_{w,0}}}}} \right)^{0.85}}{\left( {hA} \right)_{w,0}}
+\end{equation}
+
+\begin{equation}
+UA = {\left( {\frac{1}{{{{\left( {hA} \right)}_w}}} + \frac{1}{{{\eta_f}{{\left( {hA} \right)}_a}}}} \right)^{ - 1}}
+\end{equation}
+
+The above formulas are from the following reference, along with further references. The equation for x\(_{w}\) was modified from that published in Wetter (1999) to correct a small error.
+
+\subsubsection{References}\label{references-1-004}
+
+Wetter, M. 1999. Simulation Model: Finned Water-to-Air Coil Without Condensation. LBNL-42355. This document can be downloaded from .
+
+\subsection{Single-Speed Electric DX Air Cooling Coil}\label{single-speed-electric-dx-air-cooling-coil}
+
+\subsubsection{Overview}\label{overview-1-004}
+
+This model (object names Coil:Cooling:DX:SingleSpeed and \\ Coil:Cooling:DX:TwoStageWithHumidityControlMode, with CoilPerformance:DX:Cooling) simulates the performance of an air-cooled or evaporative-cooled direct expansion (DX) air conditioner. The model uses performance information at rated conditions along with curve fits for variations in total capacity, energy input ratio and part-load fraction to determine the performance of the unit at part-load conditions (Henderson et al. 1992, ASHRAE 1993). Sensible/latent capacity splits are determined by the rated sensible heat ratio (SHR) and the apparatus dewpoint (ADP)/bypass factor (BF) approach. This approach is analogous to the NTU-effectiveness calculations used for sensible-only heat exchanger calculations, extended to a cooling and dehumidifying coil.
+
+This model simulates the thermal performance of the DX cooling coil and the power consumption of the outdoor condensing unit (compressor, fan, crankcase heater and evap condenser water pump). The total amount of heat rejected by the condenser is also calculated and stored for use by other waste heat recovery models (e.g., Coil:Heating:Desuperheater). The performance of the indoor supply air fan varies widely from system to system depending on control strategy (e.g., constant fan vs.~AUTO fan, constant air volume vs.~variable air volume, etc.), fan type, fan motor efficiency and pressure losses through the air distribution system. Therefore, this DX system model does not account for the thermal effects or electric power consumption of the indoor supply air fan. EnergyPlus contains separate models for simulating the performance of various indoor fan configurations, and these models can be easily linked with the DX system model described here to simulate the entire DX air conditioner being considered (e.g., see AirLoopHVAC:Unitary:Furnace:HeatCool, AirLoopHVAC:UnitaryHeatCool, ZoneHVAC:WindowAirConditioner or AirLoopHVAC:UnitaryHeatPump:AirToAir).
+
+\subsubsection{Model Description}\label{model-description-2-004}
+
+The user must input the total cooling capacity, sensible heat ratio (SHR), coefficient of performance (COP) and the volumetric air flow rate across the cooling coil at rated conditions. The capacity, SHR and COP inputs should be ``gross'' values, excluding any thermal or energy impacts due to the indoor supply air fan. The rated conditions are considered to be air entering the cooling coil at 26.7°C drybulb/19.4°C wetbulb and air entering the outdoor condenser coil at 35°C drybulb/23.9°C wetbulb. The rated volumetric air flow should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of rated total cooling capacity (300 -- 450 cfm/ton). The rated volumetric air flow to total cooling capacity ratio for 100\% dedicated outdoor air (DOAS) application DX cooling coils should be between 0.00001677 (m3/s)/W (125 cfm/ton) and 0.00003355 (m3/s)/W (250 cfm/ton).
+
+The user must also input five performance curves or performance tables that describe the change in total cooling capacity and efficiency at part-load conditions:
+
+1)~~~~Total cooling capacity modifier curve or table (function of temperature)
+
+2)~~~~Total cooling capacity modifier curve or table (function of flow fraction)
+
+3)~~~~Energy input ratio (EIR) modifier curve or table (function of temperature)
+
+4)~~~~Energy input ratio (EIR) modifier curve or table (function of flow fraction)
+
+5)~~~~Part load fraction correlation curve or table (function of part load ratio)
+
+\begin{itemize}
+\tightlist
+\item
+  The total cooling capacity modifier curve (function of temperature) is a curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the rated total cooling capacity to give the total cooling capacity at the specific entering air temperatures at which the DX coil unit is operating (i.e., at temperatures different from the rating point temperatures). This curve is typically a biquadratic but any curve or table with two independent variables can be used.
+\end{itemize}
+
+Note: The data used to develop the total cooling capacity modifier curve (function of temperature) should represent performance when the cooling coil is `wet' (i.e., coil providing sensible cooling and at least some dehumidification). Performance data when the cooling coil is `dry' (i.e., not providing any dehumidification) should \textbf{not} be included when developing this modifier curve. This model automatically detects and adjusts for `dry coil' conditions (see section ``Dry Coil Conditions'' below).
+
+\begin{equation}
+\text{TotCapTempModFac} = \text{Func}\left(T_{wb,i},T_c,i\right)
+\end{equation}
+
+where
+
+\({T_{wb,i}}\) ~ = x values = wet-bulb temperature of the air entering the cooling coil, °C
+
+\({T_{c,i}}\) ~ = y values = dry-bulb temperature of the air entering an air-cooled condenser or wet-bulb temperature of the air entering an evaporative-cooled condenser, °C
+
+*~The total cooling capacity modifier curve (function of flow fraction) is a curve with one independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the total cooling capacity at the specific temperature and air flow conditions at which the DX unit is operating. This curve is typically a quadratic but any curve or table with one independent variable can be used.
+
+\begin{equation}
+\text{TotCapFlowModFac} = \text{Func}\left(ff\right)
+\end{equation}
+
+where
+
+\begin{equation}
+ff = \text{flow fraction} = \left( \frac{\text{Actual air mass flow rate}}{\text{Rated air mass flow rate}} \right) = \text{x value}
+\end{equation}
+
+\textbf{Note:}~ The actual volumetric air flow rate through the cooling coil for any simulation time step where the DX unit is operating must be between 0.00002684 m\(^{3}\)/s and .00006713 m\(^{3}\)/s per watt of rated total cooling capacity (200 - 500 cfm/ton). The simulation will issue a warning message if this air flow range is exceeded.
+
+\begin{itemize}
+\tightlist
+\item
+  The energy input ratio (EIR) modifier curve (function of temperature) is a curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at the specific entering air temperatures at which the DX coil unit is operating (i.e., at temperatures different from the rating point temperatures). This curve is typically a biquadratic but any curve or table with two independent variables can be used.
+\end{itemize}
+
+Note: The data used to develop the energy input ratio (EIR) modifier curve (function of temperature) should represent performance when the cooling coil is `wet' (i.e., coil providing sensible cooling and at least some dehumidification). Performance data when the cooling coil is `dry' (i.e., not providing any dehumidification) should \textbf{not} be included when developing this modifier curve. This model automatically detects and adjusts for `dry coil' conditions (see section ``Dry Coil Conditions'' below).
+
+\begin{equation}
+\text{EIRTempModFac} = \text{Func}\left(T_{wb,i},T_c,i\right)
+\end{equation}
+
+where
+
+\({T_{wb,i}}\) ~ = x values = wet-bulb temperature of the air entering the cooling coil, °C
+
+\({T_{c,i}}\) ~ = y values = dry-bulb temperature of the air entering an air-cooled condenser or wet-bulb temperature of the air entering an evaporative-cooled condenser, °C
+
+\begin{itemize}
+\tightlist
+\item
+  The energy input ratio (EIR) modifier curve (function of flow fraction) is a curve with one independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the DX unit is operating. This curve is typically a quadratic but any curve or table with one independent variable can be used.
+\end{itemize}
+
+\begin{equation}
+\text{EIRFlowModFrac} = \text{Func}\left(ff\right)
+\end{equation}
+
+where
+
+\begin{equation}
+ff = \text{flow fraction} = \left( \frac{\text{Actual air mass flow rate}}{\text{Rated air mass flow rate}} \right) = \text{x value}
+\end{equation}
+
+\begin{itemize}
+\tightlist
+\item
+  The part load fraction correlation (function of part load ratio) is a curve with one independent variable being part load ratio (sensible cooling load / steady-state sensible cooling capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the ``effective'' EIR for a given simulation time step. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. This curve is typically a linear, quadratic, or cubic but any curve or table with one independent variable can be used.
+\end{itemize}
+
+\begin{equation}
+\text{PartLoadFrac} = \text{PLF} = \text{Func}\left(\text{PLR}\right)
+\end{equation}
+
+where
+
+\begin{equation}
+\text{PLR} = \text{part load ratio} = \left(\frac{\text{actual sensible cooling load}}{\text{steady-state sensible cooling load}}\right) = \text{x values}
+\end{equation}
+
+The part-load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation time step). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+\begin{equation}
+  \begin{array}{rl}
+    \text{PLF} &\geq 0.7 \\
+    \text{PLF} &\geq \text{PLR}
+  \end{array}
+\end{equation}
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential or small commercial unit) would be:
+
+PLF = 0.85 + 0.15(PLR)
+
+All five part-load curves are accessed through EnergyPlus' built-in performance curve equation manager (curve: quadratic, curve:cubic and curve:biquadratic). It is not imperative that the user utilize all coefficients shown in equations (449) through (453) if their performance equation has fewer terms (e.g., if the user's PartLoadFrac performance curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero).
+
+For any simulation time step, the total (gross) cooling capacity of the DX unit is calculated as follows:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{total}} = {\mathop Q\limits^ \bullet_{total,rated}}\left( {TotCapTempModFac} \right)\left( {TotCapFlowModFac} \right)
+\end{equation}
+
+In a similar fashion, the electrical power consumed by the DX unit (compressors plus outdoor condenser fans) for any simulation time step is calculated using the following equation:
+
+\begin{equation}
+Power = \left( {{{\mathop Q\limits^ \bullet  }_{total}}} \right)\left( {EIR} \right)\left( {RTF} \right)
+\end{equation}
+
+where
+
+\({\mathop Q\limits^ \bullet_{total}}\) = Total cooling capacity, W -- ref. equation (455)
+
+\begin{equation}
+EIR = \,Energy\,input\,ratio\, = \,\left( {\frac{1}{{CO{P_{rated}}}}} \right)\left( {EIRTempModFac} \right)\left( {EIRFlowModFac} \right)
+\end{equation}
+
+\(CO{P_{rated}}\) ~ = Coefficient of performance at rated conditions (user input)
+
+\begin{equation}
+RTF{\rm{ }} = {\rm{ }}\left( {{\raise0.7ex\hbox{{PLR}} \!\mathord{\left/ {\vphantom {{PLR} {PartLoadFrac}}}\right.}\!\lower0.7ex\hbox{{PartLoadFrac}}}} \right)\,\, = \,\,runtime fraction of the cooling coil
+\end{equation}
+
+The total amount of heat rejected by the condenser is then calculated and stored for use by other waste heat recovery models (e.g., Coil:Heating:Desuperheater).
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{cond}} = {\mathop Q\limits^ \bullet_{total}}\left( {1 + EIR} \right)
+\end{equation}
+
+where
+
+\({\mathop Q\limits^ \bullet_{cond}}\) ~ = total amount of heat rejected by the condenser (W)
+
+The crankcase heater is assumed to operate when the cooling coil's compressor is OFF and the outdoor dry-bulb temperature is below the maximum outdoor temperature for crankcase heater operation. The average crankcase heater power for the simulation time step is calculated as follows:
+
+\begin{equation}
+{P_{crankcase}} = {\mathop Q\limits^ \bullet_{cap,crankcase}}\left( {1 - RTF} \right)
+\end{equation}
+
+where
+
+\({P_{crankcase}}\) ~ = DX cooling coil crankcase heater power, W
+
+\({\mathop Q\limits^ \bullet_{cap,crankcase}}\) = crankcase heater capacity, W
+
+If this cooling coil is used as part of an air-to-air heat pump (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir), the crankcase heater defined for this DX cooling coil is disregarded and the associated output variable is omitted. Instead, the crankcase heater defined for the DX heating coil (Coil:Heating:DX:SingleSpeed) is enabled during the time that the compressor is not running for either heating or cooling. In this instance, RTF in the above equations would be the runtime fraction of the heat pump's heating coil or cooling coil, whichever is greater.
+
+In addition to calculating the total cooling capacity provided by the DX air conditioner, it is important to properly determine the break down of total cooling capacity into its sensible (temperature) and latent (dehumidification) components. The model computes the sensible/ latent split using the rated SHR and the ADP/BF approach (Carrier et al. 1959). When the DX coil model is initially called during an EnergyPlus simulation, the rated total capacity and rated SHR are used to calculate the coil bypass factor (BF) at rated conditions. The rated total capacity and rated SHR are first used to determine the ratio of change in air humidity ratio to air dry-bulb temperature:
+
+\begin{equation}
+SlopeRated = \,\left( {\frac{{{\omega_{in}} - {\omega_{out}}}}{{{T_{db,in}}\, - {T_{db,out}}}}} \right)\mathop {}\limits_{rated}
+\end{equation}
+
+where
+
+\emph{ω\(_{in}\)} = humidity ratio of the air entering the cooling coil at rated conditions, kg/kg
+
+\emph{ω\(_{out}\)} = humidity ratio of the air leaving the cooling coil at rated conditions, kg/kg
+
+\emph{T\(_{db,in}\)} = dry-bulb temperature of the air entering the cooling coil at rated conditions, °C
+
+\emph{T\(_{db,out}\)} = dry-bulb temperature of the air leaving the cooling coil at rated conditions, °C
+
+Along with the rated entering air conditions, the algorithm then searches along the saturation curve of the psychrometric chart until the slope of the line between the point on the saturation curve and the inlet air conditions matches \emph{SlopeRated}. Once this point, the apparatus dewpoint, is found on the saturation curve the coil bypass factor at rated conditions is calculated as follows:
+
+\begin{equation}
+B{F_{rated}} = \,\frac{{{h_{out,rated}}\,\, - \,{h_{ADP}}}}{{{h_{in,rated}}\,\, - \,{h_{ADP}}}}
+\end{equation}
+
+where
+
+\emph{h\(_{out,rated}\)} = enthalpy of the air leaving the cooling coil at rated conditions, J/kg
+
+\emph{h\(_{in,rated}\)} = enthalpy of the air entering the cooling coil at rated conditions, J/kg
+
+\emph{h\(_{ADP}\)} = enthalpy of saturated air at the coil apparatus dewpoint, J/kg
+
+The coil bypass factor is analogous to the ``ineffectiveness'' (1-ε) of a heat exchanger, and can be described in terms of the number of transfer of unit (NTU).
+
+\begin{equation}
+BF = \,{e^{ - NTU}}\, = \,\,{e^{ - \,{{\left( {\frac{{UA}}{{cp}}} \right)} \mathord{\left/ {\vphantom {{\left( {\frac{{UA}}{{cp}}} \right)} {\dot m}}} \right. } {\dot m}}}}\, = \,{e^{ - \,\,{{Ao} \mathord{\left/ {\vphantom {{Ao} {\dot m}}} \right. } {\dot m}}}}
+\end{equation}
+
+For a given coil geometry, the bypass factor is only a function of air mass flow rate. The model calculates the parameter A\(_{o}\) in equation (460) based on BF\(_{rated}\) and the rated air mass flow rate. With A\(_{o}\) known, the coil BF can be determined for non-rated air flow rates.
+
+For each simulation time step when the DX air conditioner operates to meet a cooling load, the total cooling capacity at the actual operating conditions is calculated using equation (455) and the coil bypass factor is calculated based on equation (460). The coil bypass factor is used to calculate the operating sensible heat ratio (SHR) of the cooling coil using equations (461) and (462).
+
+\begin{equation}
+{h_{ADP}}\,\, = \,{h_{in}}\, - \,\frac{{({{\mathop Q\limits^ \bullet  }_{total}}\,/\dot m)}}{{1 - BF}}
+\end{equation}
+
+\begin{equation}
+SHR\,\, = \,Minimum\,\left( {\left( {\frac{{{h_{Tin,wADP}}\, - \,{h_{ADP}}}}{{{h_{in}} - {h_{ADP}}}}} \right),\,\,1} \right)
+\end{equation}
+
+where
+
+\({h_{in}}\) ~~~~~~~~ = enthalpy of the air entering the cooling coil, J/kg
+
+\({h_{ADP}}\) ~~~~~~ = enthalpy of air at the apparatus dewpoint condition, J/kg
+
+\({h_{Tin,wADP}}\) ~ = enthalpy of air at the entering coil dry-bulb temperature and humidity ratio at ADP, J/kg
+
+\(\dot m\) ~~~~~~~~~~~ = air mass flow rate, kg/s
+
+With the SHR for the coil at the current operating conditions, the properties of the air leaving the cooling coil are calculated using the following equations:
+
+\begin{equation}
+ h_{out} = h_{in} - \frac{\dot{Q}_{total}\cdot PLR}{\dot{m}}
+\end{equation}
+
+\begin{equation}
+{h_{Tin,\omega out}}\, = \,{h_{in}} - \,\left( {1 - SHR} \right)\left( {{h_{in}} - {h_{out}}} \right)
+\end{equation}
+
+\begin{equation}
+{\omega_{out}}\, = \,PsyWFnTdbH({T_{in}},\,\,{h_{Tin,\omega out}})
+\end{equation}
+
+\begin{equation}
+{T_{db,out}}\, = \,PsyTdbFnHW({h_{out}},\,\,\,{\omega_{out}})
+\end{equation}
+
+where
+
+\({h_{out}}\) ~~~~~~~~ = enthalpy of the air leaving the cooling coil, J/kg
+
+\({h_{Tin,\,\omega out}}\) ~ = enthalpy of air at the entering coil dry-bulb temperature and leaving air humidity ratio, J/kg
+
+\(\,{\omega_{out}}\) ~~~~~~~ = leaving air humidity ratio, kg/kg
+
+\(\,{T_{db,out}}\) ~~~ = leaving air dry-bulb temperature, °C
+
+\emph{PsyWFnTdbH} = EnergyPlus psychrometric function, returns humidity ratio given dry-bulb temperature and enthalpy
+
+\emph{PsyTdbFnHW} = EnergyPlus psychrometric function, returns dry-bulb temperature given enthalpy and humidity ratio
+
+\subsubsection{Dry Coil Conditions}\label{dry-coil-conditions}
+
+If the model determines that the cooling coil is dry (ω\(_{in}\) \textless{} ω\(_{ADP}\)), then equations (455) and (456) are invalid since they are functions of entering wet-bulb temperature. Under dry-coil conditions, coil performance is a function of dry-bulb temperature rather than wet-bulb temperature. In this case, the model recalculates the performance of the DX cooling unit using the calculation procedure described above but with ω\(_{in\\ =}\) ω\(_{dry,}\) where ω\(_{dry}\) is the inlet air humidity ratio at the coil dry-out point (SHR = 1.0).
+
+\subsubsection{SHR Calculation Using User Specified SHR Modifier Curves}\label{shr-calculation-using-user-specified-shr-modifier-curves}
+
+This alternative SHR calculation method is based on user specified \emph{SHR} modifying curves for temperature and flow fractions.~ The modifying curves correct the rated \emph{SHR} value for a given DX cooling coil entering air temperatures and air mass flow fraction.~ These \emph{SHR} modifying curves are optional additional curve inputs to the DX cooling coil objects.~ These two curves are a biquadratic \emph{SHR} modifier curve for temperature (\emph{SHRFT}), and a quadratic \emph{SHR} correction curve for flow fraction (\emph{SHRFFF}).
+
+·~~~~~~~~Biquadratic \emph{SHR} modifier normalized curve for DX cooling coil entering air (outdoor) wet-bulb and dry-bulb temperatures. The coil entering conditions can be outdoor air or pretreated outdoor air.
+
+·~~~~~~~~Quadratic SHR modifier curve for flow fraction.
+
+The SHR is given by:
+
+\begin{equation}
+SHR = SH{R_{rated}} \cdot SHRFT\left( {{T_{wb,i}},{T_{db,i}}} \right) \cdot SHRFFF\left( {FF} \right)
+\end{equation}
+
+The cooing coil outlet air enthalpy is given by:
+
+\begin{equation}
+{h_{out}} = {h_{in}} - \frac{{{{\dot Q}_{total}}}}{{\dot m}}
+\end{equation}
+
+The cooling coil outlet air enthalpy at the coil enlet air temperature and coil outlet humidity ratio is given by:
+
+\begin{equation}
+{h_{{T_{in}}{\omega_{out}}}} = {h_{in}} - \left( {1.0 - SHR} \right)\frac{{{{\dot Q}_{total}}}}{{\dot m}}
+\end{equation}
+
+The DX cooling coil outlet air humidity ratio is calculated from the psychometric function as follows:
+
+\begin{equation}
+{\omega_{out}} = PsyWFnTdbH\left( {{T_{db,\,i}},{h_{{T_{in}}{\omega_{out}}}}} \right)
+\end{equation}
+
+The DX cooling coils leaving humidity ratio cannot exceed the DX coil entering air humidity ratio. And for dry air condition entering the cooling coil, the above equation may yield unrealistic (in some cases negative values) coil outlet humidity ratio.~ In this case the coil outlet air humidity is set a small value as follows:
+
+\begin{equation}
+{\omega_{out}} = MIN\left( {0.000010,{\omega_{in}}} \right)
+\end{equation}
+
+The DX cooling coil outlet air dry-bulb temperature is determined as follows:
+
+\begin{equation}
+{T_{db,out}} = PsyTdbFnHW\left( {{h_{out}},{\omega_{out}}} \right)
+\end{equation}
+
+where
+
+\(SHRFT\) ~ = sensible heat ratio modifier normalized biquadratic curve as a function of coil entering air wet-bulb and dry-bulb temperatures, (-). The DX cooling coil entering air temperature can be the outdoor air condition or pretreated outdoor air when the DX cooling coil is placed after an exhaust heat recovery heat exchangers.
+
+\(SHRFFF\) = sensible heat ratio modifier normalized quadratic curve as a function of air mass flow fraction.~ Flow fraction is the ratio of actual to rated mass flow rate of air through the DX cooling coil, (-).
+
+\(SH{R_{rated}}\) ~ = sensible heat ratio at rated condition, (-).
+
+\subsubsection{Condenser Options: AirCooled vs.~EvaporativelyCooled}\label{condenser-options-aircooled-vs.evaporativelycooled}
+
+As described previously, this model can simulate the performance of air-cooled or evaporative-cooled DX air conditioners. The following paragraphs describe three modeling options.
+
+If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) (equations (449) and (451) above) will utilize the outdoor dry-bulb temperature.
+
+If the user wishes to model an evaporatively-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = EvaporativlyCooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) (equations (449) and (451) above) will utilize the outdoor wet-bulb temperature.
+
+If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = EvaporativelyCooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) will utilize the condenser inlet air temperature as calculated below:
+
+\begin{equation}
+{T_{c,i}} = \,\left( {{T_{wb,o}}} \right)\,\, + \,\,\left( {1 - EvapCondEffectiveness} \right)\left( {{T_{db,o}}\,\, - {T_{wb,o}}} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{c,i}\)} = the temperature of the air entering the condenser coil, °C
+
+\emph{T\(_{wb,o}\)} = the wet-bulb temperature of the outdoor air, °C
+
+\emph{T\(_{db,o}\)} = the dry-bulb temperature of the outdoor air, °C
+
+In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
+
+If an evaporatively-cooled condenser is modeled, the power requirements for the water pump are calculated as follows:
+
+\begin{equation}
+{P_{evapcondpump}} = {\mathop Q\limits^ \bullet_{cap,evapcondpump}}\left( {RTF} \right)
+\end{equation}
+
+where
+
+\({P_{evapcondpump}}\) = DX cooling coil evap condenser pump electric power, W
+
+\({\mathop Q\limits^ \bullet_{cap,evapcondpump}}\) = evaporative condenser pump rated power consumption, W
+
+Water consumption for the evaporative-cooled condenser is calculated using the difference in air humidity level across the evaporative media and the condenser air mass flow rate:
+
+\begin{equation}
+{V_{water}} = \frac{{{{\mathop m\limits^ \bullet  }_{_{air}}}\left( {{\omega_{evapcond,out}} - {\omega_{evapcond,in}}} \right)}}{{{\rho_{water}}}}\left( {RTF} \right)\left( {TimeStepSys} \right)\left( {3600.} \right)\,
+\end{equation}
+
+where
+
+\({V_{water}}\) ~~~~~~~~ = DX cooling coil evap condenser water consumption, m\(^{3}\)
+
+\({\mathop m\limits^ \bullet_{_{air}}}\) ~~~~~~~~~ = evaporative condenser air mass flow rate, kg/s
+
+~\({\omega_{evapcond,in}}\) ~ = humidity ratio of outdoor air entering the evap condenser, kg/kg
+
+\({\omega_{evapcond,out}}\) = humidity ratio of air leaving the evap condenser, kg/kg
+
+\({\rho_{water}}\) ~~~~~~~~ = density of water at the outdoor dry-bulb temperature, kg/m\(^{3}\)
+
+\emph{TimeStepSys} = HVAC system simulation time step, hr
+
+\subsubsection{Condenser Inlet Air Temperature}\label{condenser-inlet-air-temperature}
+
+The air temperature entering the outdoor condenser is based on the weather data used during a simulation. This temperature is either taken directly from the weather data, or can be adjusted based on the height of the outdoor condenser. The input for Condenser Air Inlet Node Name can be used to control this optional feature. If this input is left blank, the air temperature entering the condenser is based solely on the weather data. If this input is not blank, then the node name specified must also be listed in an OutdoorAir:Node or OutdoorAir:NodeList object. When the node name is listed in an OutdoorAir:NodeList object, the air temperature entering the condenser is based solely on the weather data. When the node name is listed in an OutdoorAir:Node object, the height of the node determines the air temperature entering the outdoor condenser (see description of Local Outdoor Air Temperature Calculation in the Atmospheric Variation section of this document for further details).
+
+\subsubsection{Supply Air Fan Control: Cycling vs.~Continuous}\label{supply-air-fan-control-cycling-vs.continuous}
+
+The DX cooling coil model simulates two specific supply air fan operation modes: cycling fan, cycling compressor or continuous fan, cycling compressor. The first operation mode is frequently referred to as ``AUTO fan'', where the compressor(s) and supply air fan operate in unison to meet the zone cooling load, and cycle off together when the cooling load has been met. The second operation mode is often referred to as ``fan ON'', where the compressor(s) cycle on and off to meet the zone cooling load but the supply air fan operates continuously regardless of compressor operation.
+
+Since this DX heating coil can only be used in conjunction with a DX cooling coil (i.e.~heat pumps), and these coils are used in AC equipment that specifies a fan operation mode schedule (e.g AirLoopHVAC:UnitaryHeatPump:AirToAir), the fan operation mode schedule value determines the fan operation mode for each time step throughout the simulation. A fan operation mode schedule value of 0 specifies AUTO fan mode operation while values other than 0 (a 1 is usually used) specify fan ON operation. The use of a schedule allows the fan operation mode to change based on time-of-day or with changes in season.
+
+The EnergyPlus methodology for determining the impact that HVAC equipment has on an air stream is to calculate the mass flow rate and air properties (e.g., enthalpy, dry-bulb temperature, humidity ratio) exiting the equipment. These exiting conditions are passed along as inlet conditions to the next component model in the air stream. Eventually the flow rate and properties of the air being supplied to the conditioned zone are used in the zone energy balance to determine the resulting zone air temperature and humidity ratio. With this methodology, the determination of the air mass flow rate and air properties for the two different supply air fan operation modes is slightly different.
+
+Cycling Fan Mode:
+
+For the case of cycling fan/cycling compressor when humidity control is not specified, the conditions of the air leaving the cooling coil are the steady-state values calculated using equations (463), (465) and (466) above. However the air mass flow rate passed along to the next component (and eventually to the conditioned zone) is the average air mass flow rate for the system simulation time step (determined by the cooling system; see ZoneHVAC:WindowAirConditioner, AirLoopHVAC:Unitary:Furnace:HeatCool, AirLoopHVAC:UnitaryHeatCool, or AirLoopHVAC:UnitaryHeatPump:AirToAir).
+
+For the case of cycling fan/cyling compressor when humidity control is specified, the conditions of the air leaving the cooling coil are calculated as the average conditions during the fan operating period. When the compressor operates in tandem with the fan (i.e., compressor part-load ratio {[}PLR{]} is equal to the fan PLR), the outlet conditions are identical to the calculations described above. When the compressor operates for a shorter duration than the fan (i.e., the compressor PLR is less than the heating/fan PLR), the air properties leaving the cooling coil are calculated as the average conditions during the fan operating period. In this case the calculation of exiting air conditions is analogous to the calculations for continuous fan mode described below except that PLR in the equations represents the ratio of the compressor to the fan operating period. For cycling fan systems, the fan will only operate longer than the compressor, and therefore latent degradation may be modeled (user input), when humidity control is specified, a moisture load exists (i.e., the zone air humidistat senses a moisture load), and a heating load exists where the heating PLR is greater than the cooling PLR.
+
+Continuous Fan Mode:
+
+For the case of continuous fan/cycling compressor, the air mass flow rate is constant. However, the air properties leaving the cooling coil are calculated as the average conditions during the system simulation time step. The model assumes that the exiting air conditions are the steady-state values calculated using equations (463), (465) and (466) above when the compressor(s) operate.~ For the remainder of the system simulation time step, it is assumed that the air exiting the DX coil has the same properties as the air entering the coil. For this supply air fan operating strategy, the leaving air properties are calculated as follows:
+
+\begin{equation}
+{h_{out,ContFanCycComp}}\, = \,{h_{out}}\,\left( {PLR} \right) + \,{h_{in}}\,\,\left( {1 - PLR} \right)
+\end{equation}
+
+\begin{equation}
+{\omega_{out,ContFanCycComp}}\, = \,{\omega_{out}}\,\left( {PLR} \right) + \,{\omega_{in}}\,\,\left( {1 - PLR} \right)
+\end{equation}
+
+\begin{equation}
+{T_{db,out,ContFanCycComp}} = \,PsyTdbFnHW({h_{out,\,ContFanCycComp}}\,,\,\,\,\,\,{\omega_{out,ContFanCycComp}})
+\end{equation}
+
+\subsubsection{Latent Capacity Degradation}\label{latent-capacity-degradation}
+
+The latent (dehumidification) capacity of a direct-expansion (DX) cooling coil is strongly affected by part-load, or cyclic, operation. This is especially true in applications where the supply air fan operates continuously while the cooling coil cycles on and off to meet the cooling load. During constant fan operation, moisture condenses on the cooling coil when the compressor operates, but part or all of the moisture that is held by the coil evaporates back into the airstream when the cooling coil is deactivated (Figure~\ref{fig:transient-sensible-and-latent-capacity-of-a}). The net effect is that the amount of moisture removed from the air is degraded at part-load conditions as compared to steady-state conditions when the compressor operates continuously (Figure~\ref{fig:field-data-showing-the-net-impact-of-part}).
+
+EnergyPlus is able to model latent capacity degradation based on algorithms developed by Henderson and Rengarajan (1996). The model is applicable to single-stage cooling units, like residential and small commercial air conditioners or heat pumps with less than 19 kW of nominal cooling capacity. The model inputs are described in the EnergyPlus Input/Output Reference for the object Coil:Cooling:DX:SingleSpeed. The model is enabled only if the four numerical inputs are defined (values greater than zero, see IO Reference).
+
+The following discussion applies to both cycling fan and continuous fan operation when the fan operates for a longer period of time than the compressor and air continues to flow over the moisture laden cooling coil after compressor operation has terminated.
+
+\begin{figure}[hbtp] % fig 168
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3484.png}
+\caption{Transient Sensible and Latent Capacity of a Cooling Coil Over an Operating Cycle \protect \label{fig:transient-sensible-and-latent-capacity-of-a}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 169
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3485.png}
+\caption{Field Data Showing the Net Impact of Part-Load Operation on Sensible Heat Ratio \protect \label{fig:field-data-showing-the-net-impact-of-part}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 170
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3486.png}
+\caption{Concepts of Moisture Buildup and Evaporation \protect \label{fig:concepts-of-moisture-buildup-and-evaporation}}
+\end{figure}
+
+Figure~\ref{fig:concepts-of-moisture-buildup-and-evaporation} graphically depicts the latent degradation concepts and defines several key model parameters. After the cooling coil starts to operate, the coil temperature is eventually reduced below the dewpoint temperature of the entering air. Moisture from the air then builds on the surface of the coil until time t\(_{o}\) has elapsed and the total moisture mass on the coil is M\(_{o}\). After this time (t\(_{o}\)), moisture begins to fall from the coil and all of the latent capacity provided by the coil is ``useful'' since this condensate is collected and removed from the unit. When the coil cycles off and the supply air fan continues to operate, the initial moisture mass buildup on the coil (M\(_{o}\)) evaporates back into the supply air stream. If the cooling coil cycles back on before all of the moisture has evaporated, then the time until the first condensate removal (t\(_{o}\)) is shorter for this cooling cycle since the coil is already partially wetted.
+
+Figure~\ref{fig:concepts-of-moisture-buildup-and-evaporation} also shows several parameters that are used in the latent degradation model. The ratio of the coil's moisture holding capacity (M\(_{o}\)) and the steady-state latent capacity (\({\mathop Q\limits^ \bullet_L}\) ) is defined as \emph{t\(_{wet}\)} : the nominal time for moisture to fall from the coil (ignoring transient effects at startup and starting with a dry coil). The ratio of the initial moisture evaporation rate (\({\mathop Q\limits^ \bullet_e}\) ) and the steady-state latent capacity (\({\mathop Q\limits^ \bullet_L}\) ) is defined as \(\gamma\) . Both \emph{t\(_{wet}\)}and \(\gamma\) ~at the rated air volume flow rate and temperature conditions are required model inputs. Two other model inputs are the Maximum ON/OFF Cycling Rate (cycles per hour, \emph{N\(_{max}\)}) and the time constant (\(\tau\) , in seconds) for the cooling coil's latent capacity to reach steady state after startup. The development of the latent degradation model is fully described by Henderson and Rengarajan (1996). The model implemented in EnergyPlus is for their ``linear decay'' evaporation model.
+
+During the simulation, all of the steady-state calculations described previously in equations (449) through (462) are completed. The latent degradation model then modifies the steady-state sensible heat ratio for the coil as shown below. The value of \emph{t\(_{wet}\)} at the current air volume flow rate and entering air conditions is first calculated based on the rated value of \emph{t\(_{wet}\)} entered by the user:
+
+\begin{equation}
+{t_{wet}} = Minimum\left( {{t_{wet,rated}}\left( {\frac{{{{\mathop Q\limits^ \bullet  }_{latent,rated}}}}{{{{\mathop Q\limits^ \bullet  }_{latent}}}}} \right),\,\,{t_{wet,\max }}} \right)
+\end{equation}
+
+where
+
+\emph{t\(_{wet}\)}~ = nominal time for condensate removal to begin at the current airflow and entering air conditions, starting with a dry coil (sec)
+
+\emph{t\(_{wet,rated}\)} = nominal time for condensate removal to begin at the coil's rated airflow and entering air conditions, starting with a dry coil (sec)
+
+\({\mathop Q\limits^ \bullet_{latent,rated}}\) = cooling coil latent capacity at the rated airflow and temperature conditions, W
+
+\({\mathop Q\limits^ \bullet_{latent}}\) = cooling coil latent capacity at the current airflow and temperature conditions, W
+
+\emph{t\(_{wet,max}\)} = maximum allowed value for \emph{t\(_{wet}\)} (9999.0 sec)
+
+Likewise, the value of \(\gamma\) at the current air volume flow rate and entering air conditions is calculated based on the rated value of \(\gamma\) entered by the user:
+
+\begin{equation}
+  \gamma = {\gamma_{rated}}\left( {\frac{{{{\mathop Q\limits^ \bullet  }_{latent,rated}}}}{{{{\mathop Q\limits^ \bullet  }_{latent}}}}} \right)\left( {\frac{{{T_{db,i}} - {T_{wb,i}}}}{{{T_{db,rated}} - {T_{wb,rated}}}}} \right)
+\end{equation}
+
+where:
+
+\(\gamma\) = ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at the current air volume flow rate and entering air conditions
+
+\({\gamma_{rated}}\) = \(\gamma\) ~at rated air flow and entering air conditions
+
+\emph{T\(_{db,i}\)} = dry-bulb temperature of the air entering the cooling coil, °C
+
+\emph{T\(_{wb,i}\)} = wet-bulb temperature of the air entering the cooling coil, °C
+
+\emph{T\(_{db,rated}\)} = dry-bulb temperature of air entering the cooling coil at rated conditions (26.7°C)
+
+\emph{T\(_{wb,rated}\)} = wet-bulb temperature of air entering the cooing coil at rated conditions (19.4°C)
+
+The cooling coil on and off times are then calculated based on the maximum number of cycles per hour and the calculated run-time fraction for the coil.
+
+\begin{equation}
+{t_{on}} = \frac{{3600}}{{4{N_{\max }}\left( {1 - X} \right)}}
+\end{equation}
+
+\begin{equation}
+{t_{off}} = \frac{{3600}}{{4{N_{max}}X}}
+\end{equation}
+
+where
+
+\emph{t\(_{on}\)} = duration of cooling coil on-cycle (sec)
+
+\emph{N\(_{max}\)} = maximum on/off cycles per hour (cph)
+
+\emph{X} = cooling coil runtime fraction (-)
+
+\emph{t\(_{off}\)} = duration of cooling coil off-cycle (sec)
+
+For cycling fan systems, the duration of the heating coil on and off cycles are also calculated. When the heating coil operates for a longer duration of time than the cooling coil, latent degradation can also occur. For this case, the off-cycle time (i.e., the amount of time the fan operates longer than the cooling coil) is recalculated and based on the difference between the heating coil on-cycle time and the cooling coil on-cycle time. Ton and Toff for the heating coil are calculated in the same manner as shown above except that the heating run-time fraction is used for the calculations. This model assumes that the cycling rate of the cooling and heating coils are the same. In addition, since the heating coil cycling rate may be different than the cooling coil (based on run-time fractions), the heating coil may also turn on again before the next cooling coil on-cycle. The following equations are used when the heating coil operates for a longer time period than does the cooling coil.
+
+\begin{equation}
+ton,heating = \frac{{3600}}{{4Nmax\left( {1 - Xheating} \right)}}
+\end{equation}
+
+\begin{equation}
+toff,heating = \frac{{3600}}{{4Nmax\left( {Xheating} \right)}}
+\end{equation}
+
+{\scriptsize
+\begin{equation}
+ton,heating = ton,heating + MAX\left( {0,MIN\left( {ton,heating,\left( {\left( {ton + toff} \right) - \left( {ton,heating + toff,heating} \right)} \right)} \right)} \right)
+\end{equation}}
+
+\begin{equation}
+toff = MIN\left( {toff,ton,heating - ton} \right)
+\end{equation}
+
+where
+
+\emph{t\(_{on,heating}\)} = duration of heating coil on-cycle (sec)
+
+\emph{X\(_{,heating}\)} = heating coil runtime fraction (-)
+
+\emph{t\(_{off,heating}\)} = duration of heating coil off-cycle (sec)
+
+The equation for calculating the time \emph{t\(_{o}\)} when moisture first begins to fall from the cooling coil is shown below, and is solved iteratively by EnergyPlus:
+
+\begin{equation}
+\mathop t\nolimits_o^{j + 1}  = \gamma {t_{off}} - \left( {\frac{{\mathop \gamma \nolimits^2 }}{{4{t_{wet}}}}} \right)\mathop t\nolimits_{off}^2  - \tau \left( {\mathop e\nolimits^{\frac{{\mathop t\nolimits_o^j }}{\tau }} \,\, - \,\,1} \right)\,\,,\,\,\,\mathop t\nolimits_{off}^{}  \le \,\left( {\frac{{2{t_{wet}}}}{\gamma }} \right)
+\end{equation}
+
+where
+
+\({t_o}\) = time where condensate removal begins (sec)
+
+\(\tau\) = latent capacity time constant at start-up (sec)
+
+\emph{j} = iteration number
+
+The part-load latent heat ratio of the cooling coil is then calculated with \(t_o^{}\) , \emph{t\(_{on}\)} and \(\tau\) , which is in turn used to calculate the ``effective'' sensible heat ratio of the cooling including part-load latent degradation effects.
+
+\begin{equation}
+\frac{{LHR}}{{LH{R_{ss}}}} = Maximum\left( {\left( {\frac{{{t_{on}} - {t_o}}}{{{t_{on}} + \tau \left( {{e^{\left( {\frac{{ - {t_{on}}}}{\tau }} \right)}}\,\, - \,\,1} \right)}}} \right),0.0} \right)
+\end{equation}
+
+\begin{equation}
+SH{R_{eff}} = 1 - \left( {1 - SH{R_{ss}}} \right)\left( {\frac{{LHR}}{{LH{R_{ss}}}}} \right)
+\end{equation}
+
+where
+
+\(LHR\) = part-load latent heat ratio
+
+\(LH{R_{ss}}\) = latent heat ratio at steady-state conditions (\(1 - SH{R_{ss}}\) ~with \(SH{R_{ss}}\) ~from eqn. (462))
+
+\(SH{R_{eff}}\) = part-load sensible heat ratio**(\(SH{R_{ss}}\) \emph{~≤\(SH{R_{eff}}\) ~≤} 1.0)
+
+\(SH{R_{ss}}\) = steady-state sensible heat ratio (from eqn. (462))
+
+With the ``effective'' SHR for the coil at the current operating conditions, including the impacts of latent degradation, equations (463) through (466) are then used to calculate the properties of the air leaving the cooling coil when it operates. Finally, equations (467) through (469) are used to calculate the average leaving air conditions (average when the coil is on and off) for the simulation time step.
+
+\subsubsection{Basin Heater For Single-Speed DX Coil}\label{basin-heater-for-single-speed-dx-coil}
+
+Calculations are also made to estimate the electric power input to the DX coil basin heater. A schedule may be used to disable the basin heater during regular maintenance periods or other time periods (e.g., during summer). If a schedule is not provided, the basin heater is assumed to be available the entire simulation time period. The basin heater operates when it is scheduled on, the outdoor air dry-bulb temperature is below the basin heater setpoint temperature, and the DX coil is not active. The user is required to enter a basin heater capacity (watts per degree Kelvin) and a heater setpoint temperature (\(^{o}\)C) if they want to model basin heater electric power.
+
+\begin{equation}
+ P_{basinheater} = \max\PB{0.0, CAP_{basinheater} \PB{T_{setpoint,basin} - T_{db,outdoor} }\PB{1 - RTF}}
+\end{equation}
+
+\begin{equation}
+  \mathop E\nolimits_{basinheater} = \mathop {(P}\nolimits_{basinheater} )(TimeStepSys)3600
+\end{equation}
+
+where:
+
+\(\mathop P\nolimits_{basinheater}\) = DX coil basin heater electric power (W)
+
+\(\mathop E\nolimits_{basinheater}\) = DX coil basin heater electric consumption (J)
+
+\(\mathop T\nolimits_{setpoint,basin}\) = Basin heater setpoint temperature (\(^{o}\)C)
+
+\(\mathop T\nolimits_{db,outdoor}\) = Outdoor air dry-bulb temperature (\(^{o}\)C)
+
+\(\mathop {CAP}\nolimits_{basinheater}\) = Basin heater capacity (W/K)
+
+\(RTF\) = Run time fraction of DX cooling coil
+
+\subsubsection{Special Calculations for Coil:Cooling:DX:TwoStageWithHumidityControlMode with CoilPerformance:DX:Cooling}\label{special-calculations-for-coilcoolingdxtwostagewithhumiditycontrolmode-with-coilperformancedxcooling}
+
+The multimode DX coil uses 1 to 4 set of performance specifications which all feed into the main DX coil model as described above. The multimode DX coil may have 1 or 2 capacity stages and may have 1 enhanced dehumidification mode in addition to its ``normal'' or base mode performance. Any mode may specify that a portion of the total airflow is bypassed.
+
+\paragraph{Bypass Operation}\label{bypass-operation}
+
+When a mode has coil bypass, the non-bypassed air flow fraction is used to model the DX coil performance as described above. Then the bypassed air stream is mixed with the conditioned air stream and these conditions are place on the coil outlet node.
+
+\paragraph{Multi-Stage Operation}\label{multi-stage-operation}
+
+Multi-stage control is modeled with the DX coil. If 2-stage operation has been specified, stage 1 is assumed to operate first and continue to operate if stage 2 is required. If latent degradation is active, only one of the stages will be degraded. If stage 1 operates for less than the full time step, then latent degradation is applied. If stage 2 operates, then stage 1 is running for the full time step and latent degradation is applied only to the portion of the latent load which is attributed to stage 2 operation.
+
+\paragraph{Enhanced Dehumidification Mode}\label{enhanced-dehumidification-mode}
+
+If enhanced dehumidification mode is available, this is controlled by the parent object of the DX coil, such as DXSystem:AirLoop. A dehumidification mode flag is passed to the coil model which is used to select a different set of performance specifications from a CoilPerformance:DX:Cooling input object. Then the simulation of the DX coil proceeds as described above including any bypass or multi-stage operation.
+
+\subsubsection{Standard Rating of Single-Speed DX Cooling Coils}\label{standard-rating-of-single-speed-dx-cooling-coils}
+
+For small single-speed direct expansion (DX) cooling coils, the industry standard ratings of Standard Rating Cooling Capacity and Seasonal Energy Efficiency Ratio (SEER) are calculated according to ANSI/AHRI Standard 210/240 (AHRI 2008). These ratings apply to unitary air conditioners and air-source unitary heat pumps with air-cooled condensers with standard rating cooling capacities under 19 kW (\textless{}65,000 Btu/hr). For larger DX cooling coils, the industry standard ratings of Standard Rating Cooling Capacity, Energy Efficiency Ratio (EER), and Integrated Energy Efficiency Ratio (IEER) are calculated according to ANSI/AHRI Standard 340/360 (AHRI 2007). These ratings apply to unitary air conditioners and air-source unitary heat pumps with standard rating cooling capacities from 19 kW to below 73.2 kW (65,000 Btu/hr to \textless{}250,000 Btu/hr).
+
+For the Coil:Cooling:DX:SingleSpeed object in EnergyPlus, these standard ratings are not direct inputs to the model. However, these standard ratings can be calculated using user-entered information for the Coil:Cooling:DX:SingleSpeed object. Since users sometimes lump the performance of several smaller DX cooling units into a single larger cooling coil object for simulation purposes, EnergyPlus outputs the Standard Rating Cooling Capacity, SEER, EER, and IEER regardless of the magnitude of the standard rating cooling capacity of the coil. It is up to the user to determine which standard ratings are applicable to the cooling coil(s) they are modeling. These standard rating values are provided in the eplusout.eio output file (Ref. OutputDetailsAndExamples.pdf) and also in the predefined tabular output reports (Output:Table:SummaryReports object, Equipment Summary). Currently, the standard ratings are only calculated and output for single-speed DX cooling coils with air-cooled condensers. If the single-speed DX coling coil is specified with an evaporatively-cooled condenser, then no standard ratings are output from EnergyPlus at this time.
+
+Note: The standard ratings described in this section require that the DX cooling coil model be evaluated at specific operating conditions (i.e., specific wet-bulb temperatures for air entering the cooling coil and dry-bulb temperatures for air entering the air-cooled {[}outdoor{]} condenser). If the cooling coil performance curves can not be evaluated at the required test conditions, then a standard rating value calculated at the curves limit will be output and a warning message will written to eplusout.err. For example, if the curve object (Curve:Biquadratic) for Total Cooling Capacity Function of Temperature Curve has a minimum value of 21C for dry-bulb temperature entering the air-cooled condenser coil, the IEER calculation requires that EER\(_{D}\) be calculated at 18.3C -- so, this would result in IEER calculatd at user specified curve limit as an output and a warning message in the eplusout.err file.
+
+The standard rating cooling capacity (AHRI 2007, AHRI 2008) is calculated as follows:
+
+\begin{equation}
+  \begin{array}{rl}
+    \dot{Q}_{StandardRating} & = \dot{Q}_{Total,Rated}\PB{TotCapTempModFac_{Rated}}\PB{TotCapFlowModFac_{Rated}} \\
+                             & - \PB{FanPowerPerVolFlowRate \cdot \dot{V}_{Rated}}
+  \end{array}
+\end{equation}
+
+where,
+
+\({\dot Q_{StandardRating}}\) = Standard Rating (Net) Cooling Capacity (W)
+
+\({\dot Q_{Total,Rated}}\) = Rated Total (Gross) Cooling Capacity, user input (W)
+
+\(TotCapTempModFa{c_{Rated}}\) = Total Cooling Capacity Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
+
+\(TotCapFlowModFa{c_{Rated}}\) = Total Cooling Capacity Function of Flow Fraction Curve evaluated at a flow fraction of 1.0 (dimensionless)
+
+\(FanPowerPerVolFlowRate\) = Rated Evaporator Fan Power Per Volume Flow Rate, user input ( W/(m\(^{3}\)/s) )
+
+\({\dot V_{Rated}}\) = Rated Air Volume Flow Rate, user input (m\(^{3}\)/s)
+
+The Rated Evaporator Fan Power Per Volume Flow rate is a user-entered value, with a default of 773.3 W/(m\(^{3}\)/s)) if the user leaves this input field blank. The default value is taken from ANSI/AHRI Standards 210/240 and 340/360 where it is defined for systems which do not have a cooling coil fan furnished as part of the system (e.g., a DX cooling coil mounted in the ductwork downstream of a gas furnace where the furnace contains the fan used for air distribution across the gas heating coil and the downstream DX cooling coil). The test conditions in ANSI/AHRI Standards 210/240 and 340/360 vary the external static pressure (i.e., pressure drop associated with ductwork and other devices external to the indoor fan/coil section) seen by the supply air fan based on the standard rating cooling capacity. Note, however, that external static pressure in actual installations is typically much higher. Further details regarding indoor fan power per volume flow rate can be found in Walker and Lutz (2005) and Walker (2007), including differences between Permanent Split Capacitor (PSC) and Brushless Permanent Magnet (BPM) fan motors. Especially at the low external static pressures defined in the ANSI/AHRI Standards, BPM motors (e.g., Electronically Commutated Motors (ECMs)) can draw significantly less power (e.g., 50-75\% less) than PSC motors.
+
+The seasonal energy efficiency ratio (SEER) is calculated as follows:
+
+\begin{equation}
+SEER = PL{F_{0.5}} \cdot EE{R_{TestB}}
+\end{equation}
+
+\begin{equation}
+EE{R_{TestB}} = \frac{{{{\dot Q}_{Total,Net,TestB}}}}{{Powe{r_{Total,TestB}}}}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    \dot{Q}_{Total,Net,TestB} &= \dot{Q}_{Total,Rated} \PB{TotCapTempModFac_{TestB}}\PB{TotCapFlowModFac_{Rated}} \\
+                              &- \PB{FanPowerPerVolFlowRate \cdot \dot{V}_{Rated}}
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    Power_{Total,TestB} &= \dot{Q}_{Total,Rated} \PB{TotCapTempModFac_{TestB}}\PB{TotCapFlowModFac_{Rated}}\cdot EIR_{TestB} \\
+                        &+ \PB{FanPowerPerVolFlowRate \cdot \dot{V}_{Rated}}
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  EIR_{TestB} = \frac{1}{COP_{rated}}\PB{EIRTempModFac_{TestB}}\PB{EIRFlowModFac_{Rated}}
+\end{equation}
+
+where,
+
+\emph{PLF\(_{0.5}\)} = Part Load Fraction Correlation Curve evaluated at a part load ratio (PLR) of 0.5 (dimensionless)
+
+\emph{EER\(_{TestB}\)} = Energy efficiency ratio with 19.44°C wet-bulb temperature air entering the cooling coil, 27.78°C dry-bulb temperature air entering the air-cooled (outdoor) condenser, and rated air volume flow through the cooling coil (W/W)
+
+\({\dot Q_{Total,Net,TestB}}\) = Net total cooling capacity with 19.44°C wet-bulb temperature air entering the cooling coil, 27.78°C dry-bulb temperature air entering the air-cooled (outdoor) condenser, and rated air volume flow through the cooling coil (W)
+
+\(TotCapTempModFa{c_{TestB}}\) = Total Cooling Capacity Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 27.78°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
+
+\(Powe{r_{Total,TestB}}\) = Total electric power (compressors, condenser fans and evaporator fan) with 19.44°C wet-bulb temperature air entering the cooling coil, 27.78°C dry-bulb temperature air entering the air-cooled (outdoor) condenser, and rated air volume flow through the cooling coil (W)
+
+\(CO{P_{rated}}\) = Coefficient of Performance at Rated Conditions, user input (W/W)
+
+\(EIRTempModFa{c_{TestB}}\) = Energy Input Ratio Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 27.78°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
+
+\(EIRFlowModFa{c_{Rated}}\) = Energy Input Ratio Function of Flow Fraction Curve evaluated at a flow fraction of 1.0 (dimensionless).
+
+Energy Efficiency Ratio (EER) is another standard rating (AHRI 2007), and it is defined as the ratio of the total cooling capacity to the total power input at any given set of rating conditions, expressed in W/W (or Btu/W-h). For this class of air-cooled DX cooling coils, EER is calculated at rated test conditions as follows:
+
+\begin{equation}
+EE{R_{}} = \frac{{{{\dot Q}_{Standard\,Rating}}}}{{Powe{r_{Total,Rated}}}}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    Power_{Total,Rated} &= \dot{Q}_{Total,Rated} \PB{TotCapTempModFac_{TestB}}\PB{TotCapFlowModFac_{Rated}}\cdot EIR_{Rated} \\
+                        &+ \PB{FanPowerPerVolFlowRate \cdot \dot{V}_{Rated}}
+  \end{array}
+\end{equation}
+
+\begin{equation}
+EI{R_{Rated}} = \left( {\frac{1}{{CO{P_{Rated}}}}} \right)(EIRTempModFa{c_{Rated}})(EIRFlowModFa{c_{Rated}})
+\end{equation}
+
+where,
+
+\emph{EER} = Energy Efficiency Ratio (W/W)
+
+\(Powe{r_{Total,Rated}}\) = Total electric power (compressors, condenser fans and evaporator fan) with 19.44°C wet-bulb temperature air entering the cooling coil, 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser, and air flow rate across the evaporator at the Rated Air Volume Flow Rate (W).
+
+\(TotCapTempModFa{c_{Rated}}\) = Total Cooling Capacity Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
+
+\(EIRTempModFa{c_{Rated}}\) = Energy Input Ratio Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
+
+The Integrated Energy Efficiency Ratio (IEER) is intended to be a measure of merit for the cooling coil's part-load efficiency. IEER replaced Integrated Part-Load Value (IPLV) as the part-load performance metric in Std. 340/360 as of January 1, 2010. Full details regarding the IEER calculation are available in ANSI/AHRI Std. 340/360 (AHRI 2007). A summary of the IEER calculations made by EnergyPlus for single-speed air-cooled DX cooling coils is provided below:
+
+\begin{equation}
+IEER = \,(0.02 \cdot EE{R_A}) + (0.617 \cdot EE{R_B}) + (0.238 \cdot EE{R_C}) + (0.125 \cdot EE{R_D})
+\end{equation}
+
+where,
+
+\(EE{R_A}\) = \emph{EER} at 100\% net capacity at AHRI standard rating conditions (same as EER calculation shown above)
+
+\(EE{R_B}\) = \emph{EER} at 75\% net capacity and reduced outdoor air temperature
+
+\(EE{R_C}\) = \emph{EER} at 50\% net capacity and reduced outdoor air temperature
+
+\(EE{R_D}\) = \emph{EER} at 25\% net capacity and reduced outdoor air temperature
+
+\begin{equation}
+EE{R_{B - D}} = \frac{{LF \cdot {{\dot Q}_{Total,Net,PartLoad}}}}{{Powe{r_{Total,{\kern 1pt} PartLoad}}}}
+\end{equation}
+
+\begin{equation}
+Powe{r_{Total,{\kern 1pt} PartLoad}} = LF\left( {{C_D} \cdot Powe{r_{CompCondFan,{\kern 1pt} PartLoad}}} \right) + \,\left( {FanPowerPerVolFlowRate \cdot {{\dot V}_{Rated}}} \right)
+\end{equation}
+
+\begin{equation}
+\begin{split}
+Power_{CompCondFan,PartLoad} = \dot{Q}_{Total,Rated}\PB{TotCapTempModFac_{PartLoad}} \\ 
+\cdot \PB{TotCapFlowModFac_{Rated}} \cdot EIR_{PartLoad}
+\end{split}
+\end{equation}
+
+\begin{equation}
+EI{R_{PartLoad}} = \left( {\frac{1}{{CO{P_{Rated}}}}} \right)(EIRTempModFa{c_{PartLoad}})(EIRFlowModFa{c_{Rated}})
+\end{equation}
+
+where,
+
+\({\dot Q_{Total,Net,PartLoad}}\) ~ = ~~~~ Net total cooling capacity with 19.44°C wet-bulb temperature air entering the cooling coil rated air volume flow through the cooling coil (W). The dry-bulb temperature of air entering the air-cooled condenser varies (B = 27.5°C, C = 20.0°C, D = 18.3°C).
+
+\(Powe{r_{Total,PartLoad}}\) ~ = Total electric power (compressors, condenser fans and evaporator fan) with 19.44°C wet-bulb temperature air entering the cooling coil and air flow rate across the evaporator at the Rated Air Volume Flow Rate (W). The dry-bulb temperature of air entering the air-cooled condenser varies (B = 27.5°C, C = 20.0°C, D = 18.3°C).\(Powe{r_{CompCondFan,{\kern 1pt} PartLoad}}\) ~ = Electric power of the compressor and condenser fan at the various part-load ratios, with 19.44°C wet-bulb temperature air entering the cooling coil and rated supply air volume flow rate (W). The dry-bulb temperature of air entering the air-cooled condenser varies per the part-load ratio (B = 27.5°C, C = 20.0°C, D = 18.3°C).
+
+\(EIRTempModFa{c_{PartLoad}}\) ~ = Energy Input Ratio Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and dry-bulb temperature of air entering the air-cooled condenser corresponding to the reduced part-load ratio (B = 27.5°C, C = 20.0°C, D = 18.3°C) (dimensionless).
+
+\({C_D}\) = degradation coefficient to account for cycling of the compressor = 1.13 -- 0.13\emph{LF}.
+
+\(LF\) ~ = fractional ``on'' time at the desired load point
+
+The load factor (\emph{LF}) is the fractional ``on'' time for the desired reduced load points (75\%, 50\%, or 25\%) calculated from the following equation:
+
+\begin{equation}
+LF = \frac{{\left( {{\raise0.7ex\hbox{{\% Load}} \!\mathord{\left/ {\vphantom {{\% Load} {100}}}\right.}\!\lower0.7ex\hbox{{100}}}} \right) \cdot {{\dot Q}_{StandardRating}}}}{{{{\dot Q}_{Total,Net,PartLoad}}}}
+\end{equation}
+
+where,
+
+\emph{\(\% Load\)}~ = Part-load operating points, i.e., 75\% (B), 50\% (C), 25\% (D)
+
+The calculations for \emph{Q\(_{Total,Net,PartLoad}\)} and \emph{Power\(_{Total,PartLoad}\)} are calculated in nearly the same way as \emph{Q\(_{Total,Net,TestB}\)} and \emph{Power\(_{Total,TestB}\)} are calculated for SEER (defined above). The only difference is that these cooling capacity and power values, used for calculating EER\(_{B}\)/EER\(_{C}\)/EER\(_{D}\) for IEER, are calculated for a series of dry-bulb temperatures of air entering the air-cooled condenser (B = 27.5°C, C = 20.0°C, D = 18.3°C) and part-load performance degradiation correction is also applied to the condensing unit electric power calculation.
+
+\subsubsection{ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils}\label{ansiashrae-127---standard-ratings-of-single-speed-dx-cooling-coils}
+
+For computer and data processing room unitary air conditioners single-speed direct expansion (DX) cooling coils, the standard ratings net total cooling capacity and total cooling electric power inputs are calculated according to ANSI/AHRI Standard 127 (ASHRAE 2012). These ratings apply to unitary air conditioners with air-cooled. If the single-speed DX cooling coil is specified with an evaporatively-cooled condenser, then no standard ratings are output from EnergyPlus at this time. These standard ratings are not direct inputs to the model. However, these standard ratings can be calculated using user-entered information for the Coil:Cooling:DX:SingleSpeed object. These standard rating values are provided in the eplusout.eio output file and also in the predefined tabular output reports (Output:Table:SummaryReports object, Equipment Summary).
+
+\textbf{Note}: The standard ratings described in this section require that the DX cooling coil model be evaluated at sixteen different test conditions (i.e., specific wet-bulb temperatures for air entering the cooling coil and dry-bulb temperatures for air entering the air-cooled {[}outdoor{]} condenser) for each of the four standard tests and four application classes (ASHRAE -- 2012). The four test conditions: A, B, C and D are provided in the ANSI/ASHRAE Standard 127. And the test conditions are different for each application classes described in the standard. In total sixteen performance data of net cooling capacity and total electric power inputs are reported. The total cooling electric power includes the supply fan power.
+
+\begin{longtable}[c]{p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}}
+\toprule 
+\multicolumn{6}{l}{Rated Cooling Tests} \tabularnewline \midrule
+\endhead
+& Application Class & A & B & C & D \tabularnewline
+& Class 1 & 23.9°C(75.0°F) & 23.9°C(75.0°F) & 23.9°C(75.0°F) & 23.9°C(75.0°F) \tabularnewline
+Tdb, Indoor & Class 2 & 29.4°C(85.0°F) & 29.4°C(85.0°F) & 29.4°C(85.0°F) & 29.4°C(85.0°F) \tabularnewline
+& Class 3 & 35.0°C(95.0°F) & 35.0°C(95.0°F) & 35.0°C(95.0°F) & 35.0°C(95.0°F) \tabularnewline
+& Class 4 & 40.5°C(105°F) & 40.5°C(105°F) & 40.5°C(105°F) & 40.5°C(105°F) \tabularnewline
+Tdp, Indoor &  & 35.0°C(95.0°F) & 26.7°C(80.0°F) & 18.3°C(65.0°F) & 4.4°C(40.0°F) \tabularnewline
+Tdb, Outdoor &  & 35.0°C(95.0°F) & 26.7°C(80.0°F) & 18.3°C(65.0°F) & 4.4°C(40.0°F) \tabularnewline
+\bottomrule
+\end{longtable}
+
+The standard rating net total cooling capacity is calculated as follows:
+
+\begin{equation}
+\dot{Q}_{StandardRating} = \dot{Q}_{TotalRated}\left(\text{TotCapTempModFac}_{Rated}\right)\left(\text{TotCapFlowModFac}_{Rated}\right)-\left(\text{FanPowerPerVolFlowRate} \cdot \dot{V}_{Rated}\right)
+\end{equation}
+
+where:
+
+\begin{itemize}
+\item
+  \(\dot{Q}_{StandardRating}\) = Standard Rating (Net) Cooling Capacity (W)
+\item
+  \(\dot{Q}_{Total,Rated}\) = Rated Total (Gross) Cooling Capacity, user input (W)
+\item
+  \(\text{TotCapTempModFac}_{Rated}\) = Total Cooling Capacity Function of Temperature Curve evaluated at wet-bulb temperature of air entering the cooling coil and dry-bulb temperature of air entering the air-cooled (outdoor) condenser (dimensionless)
+\item
+  \(\text{TotCapFlowModFac}_{Rated}\) = Total Cooling Capacity Function of Flow Fraction Curve evaluated at a flow fraction of 1.0 (dimensionless)
+\item
+  \(\text{FanPowerPerVolFlowRate}\) = Rated Evaporator Fan Power Per Volume Flow Rate, user input ( W/(m3/s) )
+\item
+  \(\dot{V}_{Rated}\) = Rated Air Volume Flow Rate, user input (m3/s)
+\end{itemize}
+
+The standard rating net total cooling electric power input is calculated as follows:
+
+\begin{equation}
+  \rm{Power}_{Total} = \left[ \dot{Q}_{Total,Rated} \left( \rm{TotCapTempModFac} \right) \left( \rm{TotCapFlowModFac}_{Rated} \right) \right] \cdot \rm{EIR} + \left( \rm{FanPowerPerVolFlowRate} \cdot \dot{V}_{Rated} \right)
+\end{equation}
+
+\begin{equation}
+  \frac{\rm{EIRTempModFac} \rm{EIRFlowModFac_{Rated}}}{COP_{Rated}}
+\end{equation}
+
+where:
+
+\begin{itemize}
+\item
+  \(EER\) = Energy efficiency ratio at wet-bulb temperature of air entering the cooling coil, dry-bulb temperature of air entering the air-cooled (outdoor) condenser, and rated air volume flow through the cooling coil (W/W)
+\item
+  \(\rm{TotCapTempModFac}\) = Total Cooling Capacity Function of Temperature Curve evaluated at the test condition of wet-bulb temperature of air entering the cooling coil and dry-bulb temperature of air entering the air-cooled (outdoor) condenser (dimensionless)
+\item
+  \(\rm{Power}_{Total}\) = Total electric power (compressors, condenser fans and evaporator fan) at the test conditions of wet-bulb temperature of air entering the cooling coil, and dry-bulb temperature of air entering the air-cooled (outdoor) condenser, and rated air volume flow through the cooling coil (W)
+\item
+  \(COP_{Rated}\) = Coefficient of Performance at Rated Conditions, user input (W/W)
+\item
+  \(\rm{EIRTempModFac}\) = Energy Input Ratio Function of Temperature Curve evaluated at the test condition of wet-bulb temperature of air entering the cooling coil and dry-bulb temperature of air entering the air-cooled (outdoor) condenser (dimensionless)
+\item
+  \(\rm{EIRFlowModFac}_{Rated}\) = Energy Input Ratio Function of Flow Fraction Curve evaluated at a flow fraction of 1.0 (dimensionless).
+\end{itemize}
+
+Reference:
+
+ASHRAE 2012. ANSI/ASHRAE Standard 127-2012 Method of Testing for Rating Computer and Data Processing Room Unitary Air Conditioners.
+
+\subsubsection{Basin Heater For Two-Stage DX Coil}\label{basin-heater-for-two-stage-dx-coil}
+
+Basin heater for the object Coil:Cooling:DX:TwoStageWithHumidityControlMode operates in the same manner as for Coil:Cooling:DX:SingleSpeed. Refer to the ``Basin Heater For Single-Speed DX Coil'' description above.
+
+If the number of capacity stages is equal to 1 and the CondenserType for that stage is EvapCooled, then the basin heater power is calculated for (1 - RunTimeFractionStage1) of DX coil.
+
+If the number of capacity stages is greater than 1, then
+
+1)~~~If the CondenserType for stage 1 is EvapCooled, then the basin heater power is calculated for (1 - RunTimeFractionStage1) of DX coil
+
+2)~~~Elseif the CondenserType for stage 2 is EvapCooled, then the basin heater power is calculated for (1 - RunTimeFractionStage2) of DX coil
+
+\subsubsection{References}\label{references-2-002}
+
+AHRI 2008. ANSI/AHRI Standard 210/240: 2008 Standard for Performance Rating of Unitary Air-Conditioning \& Air-Source Heat Pump Equipment.~ Arlington, VA:~ Air-Conditioning, Heating, and Refrigeration Institute.
+
+AHRI 2007. ANSI/AHRI Standard 340/360: 2007 Standard for Performance Rating of Commercial and Industrial Unitary Air-Conditioning and Heat Pump Equipment.~ Arlington, VA:~ Air-Conditioning, Heating, and Refrigeration Institute.
+
+ASHRAE. 1993. HVAC2 Toolkit: A Toolkit for Secondary HVAC System Energy Calculation. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Carrier, W.H., R.E. Cherne, W.A. Grant, and W.H. Roberts. 1959. \emph{Modern air conditioning, heating and ventilating}, 3d ed. New York: Pitman Publishing Corporation.
+
+Henderson, H.I. Jr., K. Rengarajan, and D.B. Shirey III. 1992. The impact of comfort control on air conditioner energy use in humid climates. \emph{ASHRAE Transactions} 98(2): 104-113.
+
+Henderson, H.I. Jr. and K. Rengarajan. 1996. A Model to Predict the Latent Capacity of Air Conditioners and Heat Pumps at Part-Load Conditions with Constant Fan Operation. \emph{ASHRAE Transactions} 102(2): 266-274.
+
+Henderson, H. 1998. The impact of part load air conditioner operation on dehumidification performance: Validating a latent capacity degradation model. Presented at ASHRAE's IAQ \& Energy `98 conference. New Orleans, LA.~ October.
+
+Henderson, H. and D. Shirey. 2003. Understanding the Dehumidification Performance of Air-Conditioning Equipment at Part-Load Conditions. Paper presented at Joint CIBSE/ASHRAE Conference, \emph{Building Sustainability, Value and Profit.} September.~ Edinburgh, Scotland.
+
+Walker, I.S. and Lutz, J.D. 2005. Laboratory Evaluation of Residential Furnace Blower Performance. Berekely, CA:~ Lawrence Berkeley National Laboratory, Report LBNL 58752.
+
+Walker, I.S. 2007. Comparing Residential Furnace Blowers for Rating and Installed Performance. Berkeley, CA:~ Lawrence Berkeley National Laboratory, Environmental Energy Technologies Division Report LBNL 62344.
+
+\subsection{Multi-Speed Electric DX Air Cooling Coil}\label{multi-speed-electric-dx-air-cooling-coil}
+
+\subsubsection{Overview}\label{overview-2-004}
+
+This model (object name Coil:Cooling:DX:MultiSpeed) simulates the performance of an air-to-air direct expansion (DX) cooling system. The main difference compared to the other cooling coil models, such as Coil:Cooling:DX:SingleSpeed, is that this cooling coil allows modeling of two to four discrete compressor speeds. Each speed has a set of corresponding performance information at rated conditions along with curve fits for variations in total capacity, SHR, energy input ratio and part-load fraction to determine the performance of the unit at part-load conditions (DOE 1982).~ The full load supply airflow rate is dependent on the speed number and provided by its parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed). The part-load impact on coil energy use is automatically applied to the lowest speed. A choice is provided to determine whether part-load impacts on coil energy use are applied when the coil is operating at speeds greater than speed 1.
+
+This model simulates the thermal performance of the indoor DX cooling coil, and the power consumption of the outdoor unit (multispeed compressor, fans, and crankcase heaters). The performance of the indoor supply air fan varies widely from system to system depending on control strategy (e.g., constant fan vs.~AUTO fan), fan type, fan motor efficiency and pressure losses through the air distribution system. Therefore, this DX system model does not account for the thermal effects or electric power consumption of the indoor supply air fan. EnergyPlus contains separate models for simulating the performance of various indoor fan configurations, and these models can be easily linked with the DX system model described here to simulate the entire DX system being considered. For the time being, this coil model can only be called by the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
+
+When the model determines performance at Speed 1 (the lowest speed) or cycling between OFF and Speed 1, its performance is almost the same as the performance for the Coil:Cooling:DX:SingleSpeed model. However, the outlet conditions are calculated slightly differently. Therefore, the Coil:Cooling:DX:SingleSpeed model may be considered as a subset of the model described here. When the multispeed coil model determines performance at higher speeds (above 1), the model linearly interpolates the performance at two consecutive speeds (n-1 and n) as needed to meet the cooling load, with the fraction of time at each speed established by the speed ratio.
+
+When single mode operation is specified at higher speeds (above 1), defined in the UnitarySystemPerformance:Multispeed object, a child object of AirLoopHVAC:UnitarySystem, its performance is almost the same as the performance for the Coil:Cooling:DX:SingleSpeed model at different flow rate and capacity with given speed number. No linear interpolation is performed between two adjacent speeds. The highest speed which does not exceed the sensible load is used for each HVAC timestep. This operation does not apply to speed 1 operation and the case when the sensible load is above the highest sensible capacity.
+
+\subsubsection{Model Inputs}\label{model-inputs}
+
+The model inputs are also very similar to the inputs of the Coil:Cooling:DX:SingleSpeed object. The main difference is that this multispeed model requires a set of fields at each speed, such as rated capacity, rated SHR, rated COP, two capacity modifiers, two energy input ratio modifiers, part-load correction, and latent degradation inputs. The inputs also include waste heat fraction at the rated conditions and modifier as a function of temperature to calculate recoverable waste heat for heat recovery, which are not available in the similar Coil:Cooling:DX:SingleSpeed object
+
+\subsubsection{Speed 1 Operation}\label{speed-1-operation}
+
+The calculation procedures in this model, including defrost and crankcase heater, are indentical to the Coil:Heating:DX:SingleSpeed object (Ref: Coil:Heating:DX:SingleSpeed) with one exception: outlet node condition calculation when the supply air fan operates continuously (i.e., supply air fan operating mode schedule value is not equal to 0; Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed).
+
+The following procedure provides the detailed description of the exception.
+
+n~Total delivered cooling capacity
+
+The total delivered cooling capacity for speed 1 operating at the cycling ratio needed to meet the requested cooling load is:
+
+\begin{equation}
+{Q_{coil,cycling}} = {\mathop m\limits^\cdot_{Speed1}}*CycRatio*({h_{inlet}} - {h_{outlet,full}})
+\end{equation}
+
+where,
+
+\emph{Q\(_{coil,cyclingl}\)} = delivered total cooling capacity for Speed 1 operating at a specific cycling ratio {[}W{]}
+
+\({\mathop m\limits^\cdot_{Speed\,\,1}}\) = air mass flow rate through cooling coil at Speed 1 as set by the parent object {[}kg/s{]}
+
+\emph{h\(_{outlet,full}\)} = specific enthalpy of the coil outlet air during full-load operation at Speed 1 (no cycling) {[}J/kg{]}
+
+\emph{h\(_{inlet}\)} = specific enthalpy of the coil inlet air {[}J/kg{]}
+
+\emph{CycRatio} = cycling ratio at Speed 1, ratio of requested heating load to the full-load capacity of the coil at Speed 1 {[}dimensionless{]}
+
+It is assumed that the coil provides no cooling capacity when the coil is OFF, even if the supply air fan continues to operate.
+
+n~Outlet air specific enthalpy
+
+The average specific enthalpy of the coil outlet air is then calculated based on the total delivered cooling capacity and the average air mass flow rate entering the coil:
+
+\begin{equation}
+  h_{outlet,average} = h_{inlet} -  \frac{Q_{coil,cycling}}{{\mathop m\limits^\cdot}_{inlet}}
+\end{equation}
+
+where
+
+h\(_{outlet,average}\) = averaged specific enthalpy at the coil outlet {[}J/kg{]}
+
+h\(_{inlet}\) = specific enthalpy at the coil inlet {[}J/kg{]}
+
+Q\(_{coil,cycling}\) = total capacity at full load {[}W{]}
+
+\({\mathop m\limits^\cdot_{inlet}}\) = mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the cooling coil is ON and the specified flow rate when the cooling coil is OFF for the time step being simulated.
+
+n~Sensible capacity
+
+The minimum humidity ratio (HR\(_{min}\) ) is based on humidity ratios between inlet and full load outlet as:
+
+HR\(_{min}\) = Minimum(HR\(_{inlet}\), HR\(_{full}\))
+
+where
+
+HR\(_{inlet}\) = Humidity ratio at the inlet {[}kg/kg{]}
+
+HR\(_{full}\) = Full load humidity ratio at the outlet {[}kg/kg{]}
+
+The coil sensible capacity may be calculated as:
+
+\begin{equation}
+  Q_{coil,sens} = {\mathop m\limits^\cdot_{Speed1}}*CycRatio*[{h_{inlet}}({T_{inlet}},H{R_{\min }}) - {h_{outlet,full}}({T_{outlet,full}},H{R_{\min }})]
+\end{equation}
+
+where
+
+Q\(_{coil,sens}\) = delivered sensible cooling capacity {[}W{]}
+
+h\(_{outlet,full}\) = full load specific enthalpy at the coil outlet as a function of outlet dry-bulb temperature at the full load, and the minimum humidity ratio {[}J/kg{]}
+
+h\(_{inlet}\) = specific enthalpy at the coil inlet {[}J/kg{]}
+
+n~Latent capacity
+
+The latent capacity is the difference between total and sensible capacities
+
+\begin{equation}
+  Q_{coil,latent} = Q_{coil,cycling} - Q_{coil,sens}
+\end{equation}
+
+where
+
+Q\(_{coil,latent}\) = delivered latent cooling capacity {[}W{]}
+
+n~Average outlet air humidity ratio
+
+The averaged outlet HR can be calculated as:
+
+\begin{equation}
+  HR_{outlet,average} = HR_{inlet} - \frac{Q_{coil,latent}}{\mathop {\lambda m}\limits^\cdot _{inlet}}
+\end{equation}
+
+where
+
+\(\lambda\) = heat of vaporization as a function of HR\(_{min}\) and CycRatio * T\(_{outlet,full}\)+(1-CycRatio) * T\(_{inlet}\) {[}J/kg{]}
+
+n~Average outlet air temperature
+
+Using the above averaged outlet humidity ratio and specific enthalpy, the averaged outlet temperature can be calculated using the psych function of PsyTdbFnHW.
+
+The main reason using the above approach is that outlet conditions are calculated in the same way in low and high speed operation.
+
+The crankcase heater defined for this DX cooling coil is enabled during the time that the compressor is not running for either heating or cooling. The crankcase heater power use from either heating or cooling is reported in the heating coil (Coil:Heating:DX:MultiSpeed).
+
+\subsubsection{Higher Speed Operation}\label{higher-speed-operation-000}
+
+This section describes how higher speed operation is simulated. When the required sensible load is less than the full load sensible capacity at Speed n (Speed Number \textgreater{} 1), the following calculations are performed:
+
+n~Bypass factor at Speed n-1 and Speed n
+
+\begin{equation}
+BypassFacto{r_n} = f(RatedBypassFacto{r_n},RatedFlowRat{e_n},ActualFowRat{e_n})
+\end{equation}
+
+\begin{equation}
+BypassFacto{r_{n - 1}} = f(RatedBypassFacto{r_{n - 1}},RatedFlowRat{e_{n - 1}},ActualFowRat{e_{n - 1}})
+\end{equation}
+
+where
+
+BypassFactor\(_{i}\)~~~~~~~~ = bypass factor at actual flow rate conditions at Speed i {[}dimensionless{]}
+
+RatedBypassFactor\(_{i}\)~~~~~~~~~~~ = bypass factor at the rated conditions at Speed i {[}dimensionless{]}
+
+RatedFowRate\(_{i}\)~~~~~~~ = air mass flow rate at the rated conditions at Speed i {[}kg/s{]}
+
+ActualFowRate\(_{i}\)~~~~~~ = actual air mass flow rate at Speed i {[}kg/s{]}
+
+i~~~~ = Speed n or Speed n-1
+
+The bypass factor at Speed n is a function of the bypass factor at the rated conditions, rated airflow rate, and actual flow rate at Speed n. The calculation is performed by a function, called AdjustCBF in the DXCoil module.
+
+n~Total capacity at Speed n-1 and Speed n
+
+\(TotCa{p_{n - 1}} = f(RatedCa{p_{n - 1}},TotCapTempModFa{c_{n - 1}},TotCapFlowModFa{c_{n - 1}},BypassFacto{r_{n - 1}})\) \(TotCa{p_n} = f(RatedCa{p_n},TotCapTempModFa{c_n},TotCapFlowModFa{c_n},BypassFacto{r_n})\)
+
+where
+
+TotCap\(_{i}\) = total cooling capacity at given temperatures and flow rates at Speed i {[}w{]}
+
+RatedCap\(_{i}\) = cooling capacity at the rated conditions at Speed i {[}W{]}
+
+TotCapTempModFac\(_{i}\) = total cooling capacity modifier as a function of indoor web-bulb temperature and outdoor air dry-bulb temperature at Speed i
+
+TotCapFlowModFac\(_{i}\) = total cooling capacity modifier as a function of the ratio of the actual flow rate across the cooling coil to the rated airflow rate at Speed i
+
+i~~~~ = Speed n or Speed n-1
+
+The calculation is performed by a subroutine, called CalcTotCapSHR in the DXCoil module.
+
+n~EIR at Speed n-1 and Speed n
+
+\begin{equation}
+EI{R_{n - 1}} = RatedEI{R_{n - 1}}*EIRTempModFa{c_{n - 1}}*EIRFlowModFa{c_{n - 1}}
+\end{equation}
+
+\begin{equation}
+EI{R_n} = RateEI{R_n}*EIRTempModFa{c_n}*EIRFlowModFa{c_n}
+\end{equation}
+
+where
+
+EIR\(_{i}\) = Energy input ratio at given temperatures and flow rates at Speed i {[}w{]}
+
+RatedEIR\(_{i}\) = Energy input ratio at the rated conditions at Speed i {[}W{]}
+
+EIRTempModFac\(_{i}\) = Energy input ratio modifier as a function of indoor and outdoor air dry-bulb temperature at Speed i
+
+EIRFlowModFac\(_{i}\) = Energy input ratio modifier as a function of ratio of the actual flow rate across the heating coil to the rated airflow rate at Speed i
+
+i~~~~ = n or n-1
+
+n~Full load outlet conditions at Speed n-1 and Speed n
+
+The calculation procedure of full load outlet conditions at Speed n-1 and Speed n is the same as the calculation procedure used in the Coil:Cooling:DX:SingleSpeed model (Ref. Coil:Cooling:DX:SingleSpeed). The difference is that the outlet conditions at Speed n-1 are calculated based on the total cooling capacity and mass flow rate at Speed n-1, while the outlet conditions at Speed n are calculated based on the total cooling capacity and mass flow rate at Speed n.
+
+n~Effective total cooling capacity
+
+\begin{equation}
+\begin{array}{l}
+{Q_{coil,SpeedRatio}} = (SpeedRatio){\mathop m\limits^\cdot_{Speed{\kern 1pt} n}}({h_{inlet}} - {h_{outlet,full_Speed\;n}}) \\
+\;\;\;\;\;\;\;\;\; + (1 - SpeedRatio){\mathop m\limits^\cdot_{Speed\;n - 1}}({h_{inlet}} - {h_{outlet,full_Speed\;n - 1}})
+\end{array}
+\end{equation}
+
+where
+
+\({Q_{coil,SpeedRatio}}\) = delivered sensible cooling capacity at a given speed ratio between two consecutive speeds {[}W{]}
+
+\({\mathop m\limits^\cdot_{Speed\,n}}\) = air mass flow rate through cooling coil at Speed n as set by the parent object {[}kg/s{]}
+
+\({\mathop m\limits^\cdot_{Speed\,\,n - 1}}\) = air mass flow rate through cooling coil at Speed 1 as set by the parent object {[}kg/s{]}
+
+h\(_{inlet}\) = specific enthalpy at the coil inlet {[}J/kg{]}
+
+h\(_{outlet,full\_Speed\, n}\) = full load specific enthalpy at the coil outlet at Speed n {[}J/kg{]}
+
+h\(_{outlet,full\_Speed\, n-1}\) = full load specific enthalpy at the coil outlet at Speed n-1 {[}J/kg{]}
+
+n~Average outlet air specific enthalpy
+
+\begin{equation}
+  {h_{outlet,average}} = {h_{inlet}} - \frac{Q_{coil,SpeedRatio}}{{\mathop m\limits^\cdot  }_{inlet}}
+\end{equation}
+
+where
+
+h\(_{outlet,average}\) = averaged specific enthalpy at the coil outlet {[}J/kg{]}
+
+h\(_{inlet}\) = specific enthalpy at the coil inlet {[}J/kg{]}
+
+\({\mathop m\limits^\cdot_{inlet}}\) = mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the heating coil is at Speed n and the specified flow rate when the heating coil is at Speed n-1 for the time step being simulated.
+
+n~Effective sensible cooling capacity
+
+The minimum humidity ratio (HR\(_{min}\)) is calculated as
+
+HR\(_{min}\) = Minimum{[}HR\(_{inlet}\), (SpeedRatio)HR\(_{full,n}\)+(1.0-SpeedRatio)HR\(_{full,n-1}\))
+
+The effective sensible cooling capacity is expressed as:
+
+\begin{equation}
+\begin{array}{l}
+{Q_{coil,sens}} = {\mathop m\limits^\cdot_{Speed\;n}}(SpeedRatio)[{h_{inlet}}({T_{inlet}},H{R_{\min }}) - {h_{outlet,full_Speed\,n}}({T_{outlet,n}},H{R_{\min }})] \\
+\;\;\;\;\;\;\;\;\;\;\;\;\;\; + {\mathop m\limits^\cdot_{Speed\;n - 1}}(1 - SpeedRatio)[{h_{inlet}}({T_{inlet}},H{R_{\min }}) - {h_{outlet,full_Speed\;n - 1}}({T_{outlet,n - 1}},H{R_{\min }})]
+\end{array}
+\end{equation}
+
+where
+
+Q\(_{coil,sens}\)~~~~~~~ = effective sensible cooling capacity {[}W{]}
+
+h\(_{outlet,full\_Speed\\ n}\) = full load specific enthalpy at the coil outlet at Speed n as a function of outlet dry-bulb temperature at the full load, and the minimum humidity ratio {[}J/kg{]}
+
+h\(_{outlet,full\_Speed\\ n-1}\) = full load specific enthalpy at the coil outlet at Speed n-1 as a function of outlet dry-bulb temperature at the full load, and the minimum humidity ratio {[}J/kg{]}
+
+h\(_{inlet}\)~~~~~~~~~~~~ = specific enthalpy at the coil inlet {[}J/kg{]}
+
+n~Aaverage outlet air humidity ratio and temperature
+
+The effective latent cooling capacity is the difference between the total and sensible capacity:
+
+\begin{equation}
+{Q_{coil,latent}} = {Q_{coil,SpeedRatio}} - {Q_{coil,sens}}
+\end{equation}
+
+Q\(_{coil,latent}\)~~~~~~~ = effective latent cooling capacity {[}W{]}
+
+The average outlet air HR can be calculated as:
+
+\begin{equation}
+  HR_{outlet,average} = HR_{inlet} - \frac{Q_{coil,latent}}{{\mathop {\lambda m}\limits^\cdot  }_{inlet}}
+\end{equation}
+
+where
+
+\(\lambda\) = heat of vaporization as a function of HR\(_{min}\) and SpeedRatio*T\(_{outlet,n}\)+(1-SpeedRatio)*T\(_{outlet,n-1}\) {[}J/kg{]}
+
+At the given averaged outlet humidity ratio and specific enthalpy, the averaged outlet temperature can be calculated using the psych function of PsyTdbFnHW.
+
+n~Calculate combined energy input
+
+When the input for the field `Apply Part Load Fraction to Speeds Greater than 1' is No in the object (equivalent to a single compressor), the combined energy output is calculated as follows:
+
+\(CoolingPower = (TotCa{p_n})(EI{R_n})(SpeedRatio) + (TotCa{p_{n - 1}})(EI{R_{n - 1}})(1.0 - SpeedRatio)\) ~When the input for the field 'Apply Part Load Fraction to Speeds Greater than 1' is Yes in the object (equivalent to multiple compressors), the combined energy output is calculated as follows:
+
+\begin{equation}
+CoolingPower = (TotCa{p_n})(EI{R_n})(RTF) + (TotCa{p_{n - 1}})(EI{R_{n - 1}})(1.0 - RTF)
+\end{equation}
+
+where
+
+CoolingPower = Power used in Watt
+
+RTF = Run time fraction at Speed n
+
+n~Latent degradation
+
+When the supply fan operation mode is ContinuousFanWithCyclingCompressorand the input of the Apply Latent Degradation to Speeds Greater than 1 is Yes, the latent degradation is included at Speed n. The calculation procedure is the same as one in the Coil:Cooling:DX:SingleSpeed object. The difference is that the rated values and run time fraction at Speed n are used. The adjusted SHR is used to calculate full load outlet conditions at Speed n.
+
+It is expected to have less latent degradation at Speed n than Speed 1. Therefore, smaller values of the latent degradation inputs at Speed n than those at Speed 1 are recommended.
+
+n~Crankcase heater
+
+There is no power need at higher speed operation.
+
+\subsubsection{Higher Speed Operation with Single Mode Operation}\label{higher-speed-operation-with-single-mode-operation}
+
+This section describes how higher speed operation is simulated with single mode operation. When the required sensible load is less than the full load sensible capacity at Speed n (Speed Number \textgreater{} 1), its performance is almost the same as the performance for the Coil:Cooling:DX:SingleSpeed model at different flow rate and capacity with given Speed n. No linear interpolation is performed between two adjacent speeds.
+
+\subsubsection{Waste heat calculation}\label{waste-heat-calculation-000}
+
+The waste heat generated by this coil object is calculated as:
+
+\begin{equation}
+{Q_{WasteHeat}} = (Fraction)(TempModifier)(CoolingPowe)
+\end{equation}
+
+where
+
+Fraction~~~~~~~~~~~~~~~~~ = rated waste heat fraction of the energy input
+
+TempModifer = waste heat modifier as a function of indoor and outdoor air dry-bulb temperature
+
+\subsubsection{Basin Heater For Multi-Speed DX Coil}\label{basin-heater-for-multi-speed-dx-coil}
+
+Basin heater for the object Coil:Cooling:DX:MultiSpeed operates in the same manner as for Coil:Cooling:DX:SingleSpeed. Refer to the Basin Heater For Single-Speed DX Coil description above.
+
+\subsubsection{Standard Rating of Multi-Speed DX Cooling Coils}\label{standard-rating-of-multi-speed-dx-cooling-coils}
+
+For multi-speed direct expansion cooling coils, the industry standard ratings of Standard Rating Seasonal Energy Efficiency Ratio (SEER) are calculated according to ANSI/AHRI Standard 210/240 (AHRI 2008). These standard ratings can be calculated using the user-entered information for the Coil:Cooling:DX:MultiSpeed object. According to Standard 210/240, the Standard Rating SEER applies to air-to-air unitary heat pumps and air conditions with rated cooling capacities under 19,000 Watts (\textless{}65,000 Btu/h). The Cooling Mode Test Conditions for Units Having two-capacity Compressor standard tests A\(_{2}\), B\(_{2}\), B\(_{1}\), and F\(_{1}\) are also provided in Table~\ref{table:cooling-mode-test-conditions-for-units-having}. Cooling Mode Test Conditions for Units Having a Two-Capacity Compressor. The equations required to calculate the net cooling capacity and SEER value are described next.
+
+\subsubsection{Standard Rating Cooling Capacity}\label{standard-rating-cooling-capacity}
+
+The standard net cooling capacity of multi-speed DX cooling coil is reported at the maximum speed and full load A2 test condition only. The Standard Rating (Net) Cooling Capacity calculation is the same as single speed DX cooling coil procedure when calculated at maximum speed.The procedure for calculating the Standard Rating Cooling Capacity is given by:
+
+\begin{equation}
+{\dot Q_{StandardRating}} = \dot Q_{T,\,CRated}^{k = 2} \cdot CAPFT_{TestA2}^{k = 2} \cdot CAPFFF_{TestA2}^{k = 2}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{Standard\,Rating\,Net}} = {\dot Q_{StandardRating}} - Fa{n_{Power,\,CRated}}
+\end{equation}
+
+\begin{equation}
+Fa{n_{Power,\,CRated}} = FanPowerPerVolFlowRat{e^{k = 2}} \cdot \dot V_{CRated}^{k = 2}
+\end{equation}
+
+where,
+
+\({\dot Q_{StandardRating\,Net}}\) ~ = ~~~ total standard \textbf{(net)} cooling capacity (W) of the air-conditioning or heat pump equipment in cooling mode determined from ANSI/AHRI Standard 210/240 and A2 test conditions shown in Table~\ref{table:cooling-mode-test-conditions-for-units-having}. The standard cooling test conditions for air-cooled condenser are: indoor coil entering air dry-bulb and wet-bulb temperatures 26.7°C/19.4°C and outdoor coil entering air dry-bulb and wet-bulb temperatures 35.0°C/23.9°C.
+
+\({\dot Q_{StandardRating}}\) ~ = ~~~~~~~ total standard cooling capacity (W) of the air-conditioning or heat pump equipment determined from ANSI/AHRI Standard 210/240 and A2 test conditions shown in Table~\ref{table:cooling-mode-test-conditions-for-units-having}. The standard cooling test conditions for air-cooled are: indoor coil entering air dry-bulb and wet-bulb temperatures 26.7°C/19.4°C and outdoor coil entering air dry-bulb and wet-bulb temperatures 35.0°C/23.9°C.
+
+\(\dot Q_{T,\,CRated}^{k = 2}\) ~ = Rated total cooling capacity at maximum speed, user input (W)
+
+\(CAPFT_{TestA2}^{k = 2}\) = User-specified bi-quadratic curve evaluated at the indoor coil entering air wet-bulb temperature (19.4°C) and outdoor coil entering air dry-bulb temperature (35.0°C) for air-cooled condenser per A2 test condition as specified in Table~\ref{table:cooling-mode-test-conditions-for-units-having}, (dimensionless).
+
+\(CAPFFF_{TestA2}^{k = 2}\) = User-specified quadratic or cubic curve modifying the total cooling capacity as function of flow fraction, (dimensionless).~ This curve is evaluated at a flow fraction of 1.0.
+
+\(Fa{n_{Power,\,Rated}}\) = Supply air fan power at rated conditions at high (maximum) compressor speed, (W).
+
+\(\dot V_{_{CRated}}^{k = 2}\) = Rated Air Volume Flow Rate at high (maximum) compressor speed, user input (m\(^{3}\)/s)
+
+\(FanPowerPerVolFlowRat{e^{k = 2}}\) = The Rated Indoor Coil Fan Power Per Volume Flow rate is a user-entered value, with a default of 773.3 W/(m\(^{3}\)/s)) if the user leaves this input field blank. The default value is taken from ANSI/ASHRAE Standard 210/240 -2008 where it is defined for systems which do not have an indoor coil fan furnished as part of the system. See the description given below how this value is calculated. User input ( W/(m\(^{3}\)/s)).
+
+The Rated Evaporator (Indoor Coil) Fan Power Per Volume Flow rate is a user-entered value, with a default of 773.3 W/(m\(^{3}\)/s)) if the user leaves this input field blank. The default value is taken from ANSI/ASHRAE Standard 210/240-2008 where it is defined for systems which do not have an Indoor Coil (Evaporator) fan furnished as part of the system. The test conditions in ANSI/AHRI Standard 210/240 vary the external static pressure (i.e., pressure drop associated with ductwork and other devices external to the indoor fan/coil section) seen by the supply air fan based on the standard rating cooling capacity.
+
+\subsubsection{Seasonal Energy Efficiency Ratio (SEER) for Multi-Speed DX Coil}\label{seasonal-energy-efficiency-ratio-seer-for-multi-speed-dx-coil}
+
+The SEER value for multi-speed compressor air conditioner or air-to-air heat pumps per AHRI/ANSI Std. 210/240 -- 2008 is calculated as follows:
+
+\begin{equation}
+SEER = \frac{{\sum\limits_{j = 1}^8 {\frac{{{q_c}({T_j})}}{N}} }}{{\sum\limits_{j = 1}^8 {\frac{{{e_c}({T_j})}}{N}} }}
+\end{equation}
+
+For multi-speed compressor the SEER value is weighted average performance at different outdoor air temperature bins.~ The eight outdoor air temperature bins and the corresponding weight are provided in Table~\ref{table:distribution-of-fractional-hours-with-in}. Distribution of Fractional Hours with in Cooling Season Temperature Bins.
+
+Where,
+
+\emph{q\(_{c}\)}(T\(_{j}\))/N = ~ = the ratio of space cooling capacity provided by the unit during periods of the space cooling season when the outdoor temperature fell within the range represented by bin temperature \emph{T\(_{j}\)} to the total number of hours in the cooling season (N), (W)
+
+\emph{e\(_{c}\)}(T\(_{j}\))/N = the ratio of the electrical energy consumed by the unit during periods of the space cooling season when the outdoor temperature fell within the range represented by bin temperature Tj to the total number of hours in the cooling season (N), W.
+
+\emph{j} ~~~ ~ = the bin number, dimensionless. For cooling season j ranges from 1 to 8.
+
+\emph{T\(_{j}\)}~~~ = ~~~~~~~~ outdoor air bin temperature, °C. Outdoor temperatures are ``binned'' such that calculations are only performed based one temperature within the bin. Bins of 2.8 °C with 8 cooling season bin temperatures being 19.44°C, 22.22°C, 25.0°C, 27.78°C, 30.56°C, 33.33°C, 36.11°C, 38.89°C.
+
+The steady-state cooling capacity delivered and the electric power inputs when the DX coil is operating at minimum compressor speed (\emph{k = 1}), and outdoor air temperature \emph{T\(_{j}\)}, are determined by linear interpolation using the values of B1 and F1 tests as follows:
+
+\begin{equation}
+\dot Q_c^{k = 1}({T_j}) = \dot Q_c^{k = 1}(19.44) + \frac{{\dot Q_c^{k = 1}(27.78) - \dot Q_c^{k = 1}(19.44)}}{{27.78 - 19.44}}\left( {{T_j} - 19.44} \right)
+\end{equation}
+
+\begin{equation}
+\dot E_c^{k = 1}({T_j}) = \dot E_c^{k = 1}(19.44) + \frac{{\dot E_c^{k = 1}(27.78) - \dot E_c^{k = 1}(19.44)}}{{27.78 - 19.44}}\left( {{T_j} - 19.44} \right)
+\end{equation}
+
+The steady-state cooling capacities and electric power inputs at the minimum speed and test condition \emph{B\(_{1}\)} and \emph{F\(_{1}\)} are calculated from the minimum (low) speed performance curves as follows:
+
+\begin{equation}
+\dot Q_c^{k = 1}(27.78) = \dot Q_{T,\,CRated}^{k = 1} \cdot CAPFT_{TestB1}^{k = 1} \cdot CAPFFF_{TestB1}^{k = 1} - FanPower_{CRated}^{k = 1}
+\end{equation}
+
+\begin{equation}
+\dot E_c^{k = 1}(27.78) = \left[ {\frac{{\dot Q_c^{k = 1}(27.78)}}{{COP_{CRated}^{k = 1}}}} \right] \cdot EIRFT_{TestB1}^{k = 1} \cdot EIRFFF_{TestB1}^{k = 1} + FanPower_{CRated}^{k = 1}
+\end{equation}
+
+\begin{equation}
+\dot Q_c^{k = 1}(19.44) = \dot Q_{T,\,CRated}^{k = 1} \cdot CAPFT_{TestF1}^{k = 1} \cdot CAPFFF_{TestF1}^{k = 1} - FanPower_{CRated}^{k = 1}
+\end{equation}
+
+\begin{equation}
+\dot E_c^{k = 1}(19.44) = \left[ {\frac{{\dot Q_c^{k = 1}(19.44)}}{{COP_{CRated}^{k = 1}}}} \right] \cdot EIRFT_{TestF1}^{k = 1} \cdot EIRFFF_{TestF1}^{k = 1} + FanPower_{CRated}^{k = 1}
+\end{equation}
+
+\begin{equation}
+FanPower_{CRated}^{k = 1} = FanPowerPerVolFlowRat{e^{k = 1}} \cdot {\rm{\dot V}}_{CRated}^{k = 1}
+\end{equation}
+
+Where,
+
+\(\dot Q_{T,\,CRated}^{k = 1}\) = ~~ rated total cooling capacity at minimum compressor speed specified by users, (W)
+
+\(COP_{CRated}^{k = 1}\) = ~~~~~~~~~~~ rated gross COP at minimum compressor speed specified by users, (-)
+
+\(CAPFT_{TestB1}^{k = 1}\) = cooling capacities modifier curve for temperature at minimum compressor speed and B1 test condition, (-)
+
+\(CAPFFF_{TestB1}^{k = 1}\) = ~~~~~ cooling capacities modifier curve for flow fraction at minimum compressor speed and B1 test condition, (-)
+
+\(EIRFT_{TestB1}^{k = 1}\) = EIR modifier curve for temperature at minimum compressor speed and B1 test condition, (-)
+
+\(EIRFFF_{TestB1}^{k = 1}\) = EIR modifier curve for flow fraction at minimum compressor speed and B1 test condition, (-)
+
+\(CAPFT_{TestF1}^{k = 1}\) = cooling capacities modifier curve for temperature at minimum compressor speed and F1 test condition, (-)
+
+\(CAPFFF_{TestF1}^{k = 1}\) = cooling capacities modifier curve for flow fraction at minimum compressor speed and F1 test condition, (-)
+
+\(EIRFT_{TestF1}^{k = 1}\) = EIR modifier curve for temperature at minimum compressor speed and F1 test condition, (-)
+
+\(EIRFFF_{TestF1}^{k = 1}\) = EIR modifier curve for flow fraction at minimum compressor speed and F1 test condition, (-)
+
+\(FanPower_{CRated}^{k = 1}\) = the rated supply air fan power when the unit is operating at minimum compressor speed, (W)
+
+\(V_{CRated}^{k = 1}\) = rated cooling supply air volume flow rate at minimum compressor speed specified by users, (-)
+
+\(FanPowerPerVolFlowRat{e^{k = 1}}\) ~ = ~ the rated Indoor Coil fan power per volume flow rate at low (minimum) compressor speed specified value by the user, (W/(m3/s))
+
+The steady-state cooling capacity delivered and the electric power inputs when the DX cooling coil is operating at maximum (high) compressor speed (\emph{k = 2}), and outdoor air temperature \emph{T\(_{j}\)}, are determined as follows:
+
+\begin{equation}
+\dot Q_c^{k = 2}({T_j}) = \dot Q_c^{k = 2}(27.78) + \frac{{\dot Q_c^{k = 2}(35.0) - \dot Q_c^{k = 2}(27.78)}}{{35.0 - 27.78}}\left( {{T_j} - 27.78} \right)
+\end{equation}
+
+\begin{equation}
+\dot E_c^{k = 2}({T_j}) = \dot E_c^{k = 2}(27.78) + \frac{{\dot E_c^{k = 2}(35.0) - \dot E_c^{k = 2}(27.7)}}{{35.0 - 27.78}}\left( {{T_j} - 27.78} \right)
+\end{equation}
+
+The steady-state cooling capacities and electric power input at the maximum speed and test condition \emph{A\(_{2}\)} and \emph{B\(_{2}\)} are determined from the maximum (high) speed performance curves as follows:
+
+\begin{equation}
+\dot Q_c^{k = 2}(35.0) = \dot Q_{T,\,CRated}^{k = 2} \cdot CAPFT_{TestA2}^{k = 2} \cdot CAPFFF_{TestA2}^{k = 2} - FanPower_{CRated}^{k = 2}
+\end{equation}
+
+\begin{equation}
+\dot E_c^{k = 2}(35.0) = \left[ {\frac{{\dot Q_c^{k = 2}(35.0)}}{{COP_{CRated}^{k = 2}}}} \right] \cdot EIRFT_{TestA2}^{k = 2} \cdot EIRFFF_{TestA2}^{k = 2} + FanPower_{CRated}^{k = 2}
+\end{equation}
+
+\(\dot Q_c^{k = 2}(27.78) = \dot Q_{T,\,CRated}^{k = 2} \cdot CAPFT_{TestB2}^{k = 2} \cdot CAPFFF_{TestB2}^{k = 2} - FanPower_{CRated}^{k = 2}\) ~\(\dot E_c^{k = 2}(27.78) = \left[ {\frac{{\dot Q_c^{k = 2}(19.44)}}{{COP_{CRated}^{k = 2}}}} \right] \cdot EIRFT_{TestB2}^{k = 2} \cdot EIRFFF_{TestB2}^{k = 2} + FanPower_{CRated}^{k = 2}\)
+
+\begin{equation}
+FanPower_{CRated}^{k = 2} = FanPowerPerVolFlowRat{e^{k = 2}} \cdot {\rm{\dot V}}_{CRated}^{k = 2}
+\end{equation}
+
+Where,
+
+\(\dot Q_{T,\,CRated}^{k = 2}\) ~ = rated total cooling capacity at maximum (high) compressor speed specified by users, (W)
+
+\(COP_{CRated}^{k = 2}\) ~ = rated gross COP at maximum (high) compressor speed specified by users, (-)
+
+\(CAPFT_{TestA2}^{k = 2}\) ~ = cooling capacity modifier curve for temperature at maximum (high) compressor speed and \emph{A}\(_{2}\) test condition, (-)
+
+\(CAPFFF_{TestA2}^{k = 2}\) ~~~~~~~ = cooling capacity modifier curve for flow fraction at maximum (high) compressor speed and \emph{A}\(_{2}\) test condition, (-)
+
+\(EIRFT_{TestA2}^{k = 2}\) ~ = EIR modifier curve for temperature at maximum (high) compressor speed and \emph{A}\(_{2}\) test condition, (-)
+
+\(EIRFFF_{TestA2}^{k = 2}\) ~ = EIR modifier curve for flow fraction at maximum (high)~ compressor speed and \emph{A}\(_{2}\) test condition, (-)
+
+\(CAPFT_{TestB2}^{k = 2}\) ~ = cooling capacity modifier curve for temperature at maximum (high) compressor speed and \emph{B}\(_{2}\) test condition, (-)
+
+\(CAPFFF_{TestB2}^{k = 2}\) ~~~~~~~ = cooling capacity modifier curve for flow fraction at maximum (high) compressor speed and \emph{B}\(_{2}\) test condition, (-)
+
+\(EIRFT_{TestB2}^{k = 2}\) ~ = EIR modifier curve for temperature at maximum (high) compressor speed and \emph{B}\(_{2}\) test condition, (-)
+
+\(EIRFFF_{TestB2}^{k = 2}\) ~ = EIR modifier curve for flow fraction at maximum (high) compressor speed and \emph{B}\(_{2}\) test condition, (-)
+
+\(FanPower_{CRated}^{k = 2}\) ~ = the rated supply air fan power when the unit is operating at maximum (high) compressor speed, (W)
+
+\(V_{CRated}^{k = 2}\) ~ = rated supply air volume flow rate at maximum (high) compressor speed specified by users, (-)
+
+\(FanPowerPerVolFlowRate{k^{k = 2}}\) ~ = the Rated Evaporator (Indoor Coil) Fan Power Per Volume Flow rate at maximum (high) compressor speed specified value by the user, (W/(m3/s))
+
+The above steps show how the cooling capacity and electric power inputs are determined when the DX cooling coil is operating at minimum (low) and maximum (high) compressor speeds.~ But the unit may operate at minimum (low) speed capacity, cycle on--off, cycle between successiave lower and higher compressor speed capacity, or operate at maximum (high) speed capacity depending on the building cooling load. The operating range of the DX cooling coil is determined based on the building cooling load for each binned outside air temperature. The building cooling load at an outdoor air temperature \emph{T\(_{j}\)}, is calculated as follows:
+
+\begin{equation}
+BL({T_j}) = \left( {\frac{{{T_j} - 18.3}}{{35.0 - 18.3}}} \right)\left( {\frac{{\dot Q_c^{k = 2}(35.0)}}{{1.1}}} \right)
+\end{equation}
+
+Where,
+
+\emph{BL(T\(_{j}\))}~~~~~~~~~ = the building space cooling load corresponding to outdoor temperature of \emph{T\(_{j}\)}, (W).
+
+\(\dot Q_c^{k = 2}(35.0)\) = the cooling capacity determined from the standard A2 test, (W)
+
+The temperatures 35.0 °C and 18.3 °C in the building load calculation equation represent the outdoor design air temperature, and zero-load base temperature, respectively (ANSI/ASHRAE, 2008).~ 1.1 is a sizing factor.
+
+The cooling capacity delivered and the electric power inputs calculations when the DX cooling coil is cycling on-off, operating at minimum (low) compressor speed, cycling between successive minimum (low) and maximum (high) compressor speed, or operating at maximum (high) compressor speed are described next.
+
+\emph{Case 1}:~ The steady state cooling capacity when the unit is operating at or below the minimum (low) speed compressor capacity, i.e., when the building cooling load is less or equal to the minimum (low) compressor speed capacity, is calculated as follows:
+
+\begin{equation}
+\dot Q_c^{k = 1}({T_j}) \ge BL({T_j})
+\end{equation}
+
+\begin{equation}
+\frac{{{q_c}({T_j})}}{N} = \left[ {{X^{k = 1}}({T_j}) \cdot \dot Q_c^{k = 1}({T_j})} \right] \cdot \frac{{{n_j}}}{N}
+\end{equation}
+
+\begin{equation}
+\frac{{{e_c}({T_j})}}{N} = \left[ {\frac{{{X^{k = 1}}({T_j})}}{{PL{F_j}}}\dot E_c^{k = 1}({T_j})} \right] \cdot \frac{{{n_j}}}{N}
+\end{equation}
+
+\begin{equation}
+{X^{k = 1}}({T_j}) = \frac{{BL({T_j})}}{{\dot Q_c^{k = 1}({T_j})}}
+\end{equation}
+
+\begin{equation}
+PL{F_j} = 1 - C_D^c\left[ {1 - {X^{k = 1}}({T_j})} \right]
+\end{equation}
+
+Where,
+
+\emph{X(T\(_{j}\))} = the cooling mode load factor or part-load ratio for temperature bin j, (-)
+
+n\(_{i}\)/N = fractional bin hours for the cooling season; the ratio of the number of hours during the cooling season when the outdoor temperature fell within the range represented by bin temperature \emph{T\(_{j}\)} to the total number of hours in the cooling season, (-). (see Table~\ref{table:distribution-of-fractional-hours-with-in})
+
+\(C_D^c\) ~ = cooling coefficient of degradation, default value is 0.25.
+
+\emph{Case 2}:~ The unit cycles between successive the minimum (low) and maximum (high) compressor speed capacity to meet the building cooling load at outdoor air temperature \emph{T\(_{j}\)}.~ That is, the cooling building load is between the units successive minimum (low) and maximum (high) compressor speed capacities:
+
+\begin{equation}
+\dot Q_c^{k = 1}({T_j}) < BL({T_j}) < \dot Q_c^{k = 2}({T_j})
+\end{equation}
+
+\(\frac{{{q_c}({T_j})}}{N} = \left[ {{X^{k = 1}}({T_j}) \cdot \dot Q_c^{k = 1}({T_j}) + \left( {1 - {X^{k = 1}}({T_j})} \right) \cdot \dot Q_c^{k = 2}({T_j})} \right] \cdot \frac{{{n_j}}}{N}\) \(\frac{{{e_c}({T_j})}}{N} = \left[ {{X^{k = 1}}({T_j}) \cdot \dot E_c^{k = 1}({T_j}) + \left( {1 - {X^{k = 1}}({T_j})} \right) \cdot \dot E_c^{k = 2}({T_j})} \right] \cdot \frac{{{n_j}}}{N}\)
+
+\begin{equation}
+{X^{k = 1}}({T_j}) = \frac{{\dot Q_c^{k = 2}({T_j}) - BL({T_j})}}{{\dot Q_c^{k = 2}({T_j}) - \dot Q_c^{k = 1}({T_j})}}
+\end{equation}
+
+\emph{Case 3}:~ The steady-state cooling capacity when the unit is operating continuously at maximum (high) compressor speed capacity at outdoor air temperature \emph{T\(_{j}\)}. That is the building cooling load is greater or equal to the available capacity at maximum (high) compressor speed:
+
+\begin{equation}
+BL({T_j}) \ge \dot Q_c^{k = 2}({T_j})
+\end{equation}
+
+For units when operating continuously at maximum (high) compressor speed (k = 2) at temperature \emph{T\(_{j}\)}, the delivered cooling capacity and electric power inputs are calculated as follows:
+
+\begin{equation}
+\frac{{{q_c}({T_j})}}{N} = \left[ {\dot Q_c^{k = 2}({T_j})} \right] \cdot \frac{{{n_j}}}{N}
+\end{equation}
+
+\begin{equation}
+\frac{{{e_c}({T_j})}}{N} = \left[ {\dot E_c^{k = 2}({T_j})} \right] \cdot \frac{{{n_j}}}{N}
+\end{equation}
+
+% table 56
+\begin{longtable}[c]{>{\raggedright}p{2.0in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}p{0.5in}>{\raggedright}p{1.5in}}
+\caption{Cooling Mode Test Conditions for Units Having a Two-Capacity Compressor \label{table:cooling-mode-test-conditions-for-units-having}} \tabularnewline
+\toprule 
+Test & \multicolumn{2}{p{1.0in}}{\raggedright Air Entering Indoor Unit Temperature (F / C)} & \multicolumn{2}{p{1.0in}}{\raggedright Air Entering Outdoor Unit Temperature (F / C)} \tabularnewline
+\cmidrule(r){2-3}
+\cmidrule(l){4-5}
+Description & Dry Bulb & Wet Bulb & Dry Bulb & Wet Bulb & Compressor Capacity & Cooling Air Volume Rate \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Cooling Mode Test Conditions for Units Having a Two-Capacity Compressor} \tabularnewline
+\toprule 
+Test & \multicolumn{2}{p{1.0in}}{\raggedright Air Entering Indoor Unit Temperature (F / C)} & \multicolumn{2}{p{1.0in}}{\raggedright Air Entering Outdoor Unit Temperature (F / C)} \tabularnewline
+\cmidrule(r){2-3}
+\cmidrule(l){4-5}
+Description & Dry Bulb & Wet Bulb & Dry Bulb & Wet Bulb & Compressor Capacity & Cooling Air Volume Rate \tabularnewline
+\midrule
+\endhead
+
+A2 Test-required (steady, wet coil) & 80.0/26.7 & 67.0/19.4 & 95.0/35.0 & 75.0/23.9 & High & Cooling Full-load \tabularnewline
+B2 Test-required (steady, wet coil) & 80.0/26.7 & 67.0/19.4 & 82.0/27.8 & 65.0/18.3 & High & Cooling Full-load \tabularnewline
+B1 Test-required (steady, wet coil) & 80.0/26.7 & 67.0/19.4 & 82.0/27.8 & 65.0/18.3 & Low & Cooling Minimum \tabularnewline
+C2 Test-optional (steady, dry coil) & 80.0/26.7 &  & 82.0/27.8 &  & High & Cooling Full-load \tabularnewline
+D2 Test-required (cyclic, dry coil) & 80.0/26.7 &  & 82.0/27.8 &  & High &  \tabularnewline
+C1 Test-optional (steady, dry coil) & 80.0/26.7 &  & 82.0/27.8 &  & Low & Cooling Minimum \tabularnewline
+D1 Test-optional (cyclic, dry coil) & 80.0/26.7 &  & 82.0/27.8 &  & Low &  \tabularnewline
+F1 Test-optional (steady, dry coil) & 80.0/26.7 & 67.0/19.4 & 67.0/19.4 & 53.5/11.9 & High & Cooling Minimum \tabularnewline
+\bottomrule
+\multicolumn{7}{l}{\scriptsize Source: AHRI Standard 210-240, 2008; Table 5, Page 65}
+\end{longtable}
+
+% table 57
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Distribution of Fractional Hours with in Cooling Season Temperature Bins \label{table:distribution-of-fractional-hours-with-in}} \tabularnewline
+\toprule 
+Source: AHRI Standard 210-240, 2008; Table 16, Page 94 \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Distribution of Fractional Hours with in Cooling Season Temperature Bins} \tabularnewline
+\toprule 
+Source: AHRI Standard 210-240, 2008; Table 16, Page 94 \tabularnewline
+\midrule
+\endhead
+
+Bin Number j & Bin Temperature Range (C) & Representative Temperature for bin (C) & Fraction of Total Temperature Bin Hours Nj/N \tabularnewline
+1 & Dry Bulb & Wet Bulb & Dry Bulb \tabularnewline
+2 & 18.33 - 20.56 & 19.44 & 0.214 \tabularnewline
+3 & 21.11 - 23.33 & 22.22 & 0.231 \tabularnewline
+4 & 23.89 - 26.11 & 25 & 0.216 \tabularnewline
+5 & 26.67 - 28.89 & 27.78 & 0.161 \tabularnewline
+6 & 29.44 - 31.67 & 30.56 & 0.104 \tabularnewline
+7 & 32.22 - 34.44 & 33.33 & 0.052 \tabularnewline
+8 & 35.00 - 37.22 & 36.11 & 0.018 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{References}\label{references-3-001}
+
+See the references for the single speed DX cooling coil earlier in this document.
+
+\subsection{Two-Speed Electric DX Air Cooling Coil}\label{two-speed-electric-dx-air-cooling-coil}
+
+\subsubsection{Overview}\label{overview-3-003}
+
+The input object Coil:Cooling:DX:TwoSpeed provides a model that is meant to represent either a 2 speed (fan and compressor) DX cooling unit (compressor, evaporator, condenser) or a variable speed DX cooling unit in which the variation of compressor speed and air flow rate is nearly linear as a function of cooling part load. In EnergyPlus Coil:Cooling:DX:TwoSpeed is used as the cooling coil in packaged variable volume systems (PVAV). The model is based upon the single speed DX unit Coil:Cooling:DX:SingleSpeed. Basically the model for Coil:Cooling:DX:TwoSpeed employs a separate single speed model at high speed (full load) and low speed (minimum load) and interpolates between these 2 states to obtain the needed cooling output. Below minimum load the unit cycles on/off, just like the single speed unit.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-001}
+
+The input is similar to that for Coil:Cooling:DX:SingleSpeed except there needs to be two complete sets of performance data. The user inputs a rated total cooling capacity, rated SHR, rated COP, and rated air volumetric flow rate for the high speed and low speed states. Performance curves -- cooling capacity as a function of entering air wet-bulb temperature and outside dry-bulb temperature (wet-bulb if there is an evaporatively cooled condenser), EIR as a function of the same two temperatures -- must be defined and referenced for both high and low speed states. The performance characteristics of the evaporative condenser, if present, also need to be given at high and low speed states: effectiveness, air volumetric flow rate, and pump power consumption. The full list of inputs is given in the Input/Output Reference document.
+
+The data for Coil:Cooling:DX:TwoSpeed is stored in the array structure \emph{DXCoil} in the program module \emph{DXCoils}
+
+\subsubsection{Calculation}\label{calculation-000}
+
+Calculation is performed in routine \emph{CalcMultiSpeedDXCoil} in module \emph{DXCoils}. The inputs to the calculation are the coil index (denoting a specific coil with its particular performance parameters), the speed ratio, and the cycling ratio. The speed ratio is an artificial parameter between 0 and 1. If the speed ratio (\emph{SR}) is greater than zero, the performance of the unit will be:
+
+\begin{equation}
+SR\cdot HighSpeedPerformance + (1 - SR)\cdot LowSpeedPerformance
+\end{equation}
+
+Here \emph{HighSpeedPerformance} means the electricity consumption, cooling output, and outlet conditions of the unit if the unit were operating at high speed (full load). Similarly \emph{LowSpeed Performance} means the electricity consumption, cooling output, and outlet conditions if the unit were operating at low speed (minimum non-cycling load). The calculations for each state are the same as for the single speed, cycling DX unit Coil:Cooling:DX:SingleSpeed.
+
+If the speed ratio is zero and the cycling ratio is \textgreater{} 0, the unit will be in cycling mode. The unit will be on for \emph{cycling ratio} fraction of the time step, off for the remainder of the time step. While on, the unit will perform according to the low speed performance parameters.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-001}
+
+Coil:Cooling:DX:TwoSpeed is not used by itself; it is used as part of an encompassing component or system that provides control for the unit. In setting up a PVAV system, for instance, Coil:Cooling:DX:TwoSpeed is part of the component CoilSystem:Cooling:DX, which controls Coil:Cooling:DX:TwoSpeed. When used in the CoilSystem:Cooling:DX component, the simulation allows for either temperature \emph{or} temperature and dehumidification control based on a dehumidification control selection in the CoilSystem:Cooling:DX component. If None is selected the simulation runs the DX unit to satisfy a supply air temperature setpoint. It typically varies the speed ratio in an iterative solution process to establish the operating point that will give the desired unit outlet air temperature. If CoolReheat is selected, the simulation first runs the DX unit to satisfy a supply air temperature setpoint. However, in this case if the DX unit outlet air humidity ratio is above the humidity ratio setpoint, the simulation will increase the speed and/or cycling ratio to meet the desired unit outlet air humidity ratio. The humidity ratio setpoint is specified through the use of a humidistat (ref. ZoneControl:Humidistat) and a setpoint manager (ref. SetpointManager:SingleZone:Humidity:Maximum, SetpointManager:MultiZone:MaximumHumidity:Average,~ SetpointManager:MultiZone:Humidity:Maximum or SetpointManager:OudoorAirPretreat). When used with the CoilSystem:Cooling:DX component, the dehumidification control type Multimode is not allowed.
+
+\subsubsection{Basin Heater For Two-Speed DX Coil}\label{basin-heater-for-two-speed-dx-coil}
+
+Basin heater for the object Coil:Cooling:DX:TwoSpeed operates in the same manner as for Coil:Cooling:DX:SingleSpeed. Refer to the ``Basin Heater For Single-Speed DX Coil'' description above.
+
+\subsubsection{Standard Ratings}\label{standard-ratings}
+
+The Coil:Cooling:DX:TwoSpeed object includes industry standard ratings of Standard Rating Cooling Capacity, Energy Efficiency Ratio (EER), and Integrated Energy Efficiency Ratio (IEER) which are calculated according to ANSI/AHRI Standard 340/360-2007 with Addenda 1 and 2 (AHRI 2007). These ratings apply to unitary air conditioners with air-cooled condensers with standard rated cooling capacities from 19 kW (65,000 Btu/h) to below 220 kW (760,000 Btu/h).
+
+For the Coil:Cooling:DX:TwoSpeed object in EnergyPlus, these standard ratings are not direct inputs to the model. However, these standard ratings can be calculated using user-entered information for the Coil:Cooling:DX:TwoSpeed object. These standard rating values are provided in the eplusout.eio output file (Ref. OutputDetailsAndExamples.pdf) and also in the predefined tabular output reports (Output:Table:SummaryReports object, Equipment Summary report, DX Cooling Coil table and VAV DX Cooling Standard Rating Details table). Currently, the standard ratings are only calculated and output for Packaged VAV cooling coils with air-cooled condensers and variable-air-volume fans. If the two-speed DX coling coil is specified with an evaporatively-cooled condenser or along with a constant volume fan, then no standard ratings are output from EnergyPlus at this time.
+
+The standard rating cooling capacity is calculated as follows:
+
+\begin{equation}
+\begin{array}{l}
+{\dot Q}_{StandardRating} = \,\,{\dot Q}_{Total,Rated} \left( TotCapTempModFac_{Rated} \right) \left( TotCapFlowModFac_{Rated} \right) \\
+\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, - \,\left( FanHeatCorrection \right)
+\end{array}
+\end{equation}
+
+where,
+
+\({\dot Q_{StandardRating}}\) = Standard Rating (Net) Cooling Capacity (W)
+
+\({\dot Q_{Total,Rated}}\) = Rated Total (Gross) Cooling Capacity, user input (W)
+
+\(TotCapTempModFa{c_{Rated}}\) = Total Cooling Capacity Function of Temperature Curve evaluated with 19.4°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
+
+\(TotCapFlowModFa{c_{Rated}}\) = Total Cooling Capacity Function of Flow Fraction Curve evaluated at a flow fraction of 1.0 (dimensionless)
+
+\(FanHeatCorrection\) = The rate that air is heated by the supply fan ( W )
+
+\(FanHeatCorrection\) is calculated in one of two ways depending on the user's input for the field called Unit Internal Static Air Pressure.~ If this field was left blank then the fan heat is calculated using
+
+\begin{equation}
+FanHeatCorrection = {\dot V_{RatedHighSpeed}}*773.3
+\end{equation}
+
+where
+
+\({\dot V_{RatedHighSpeed}}\) = Rated Air Volume Flow Rate at high speed, user input (m\(^{3}\)/s)
+
+The value of 773.3 W/(m\(^{3}\)/s) (365 W/1000cfm) is specified by ANSI/AHRI 340/360 for indoor-coil-only units that are not provided with a supply fan.
+
+If an internal static pressure is provided, then the fan heat is modeled by evaluating the full model for Fan:VariableVolume.~ This is different that the ratings calculated for single-speed DX equipment which does not use data from an associated fan object.~ The program detects the VAV fan associated with the two-speed coil and uses the input data for that fan but with a different total air pressure rise.~ The total pressure is the sum of the internal pressure and the external pressure (i.e., pressure drop associated with ductwork and other devices external to the indoor fan/coil section). The test conditions in ANSI/AHRI Standard 340/360 vary the (minimum) external static pressure seen by the supply air fan based on the standard rating cooling capacity (see Table \# 5 in ANSI/AHRI Standard 340/360).~ For the part load test points the supply air flow is reduced and the external pressure varies with the square of the flow ratio (see Note 1 in Table \# 6 in ANSI/AHRI Standard 340/360-2007 with Addenda 1 and 2). The entire VAV fan model in EnergyPlus is evaluated at the specified air flow rate and the total static pressure for rating and the fan heat is calculated using
+
+\begin{equation}
+FanHeatCorrection = Enthalp{y_{leavingFan}} - Enthalp{y_{enteringFan}}
+\end{equation}
+
+Energy Efficiency Ratio (EER) is another standard rating (AHRI 2007), and it is defined as the ratio of the total cooling capacity to the total power input at any given set of rating conditions, expressed in W/W (or Btu/W-h). For this class of air-cooled DX cooling coils, EER is calculated at rated test conditions as follows:
+
+\begin{equation}
+  EER = \frac{{\dot Q}_{Standard\,Rating}}{Power_{Total,Rated}}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{l}
+    Power_{Total,Rated} = \left( {\dot Q}_{Total,Rated} (TotCapTempModFac_{Rated})(TotCapFlowModFac_{Rated}) \right)\, \cdot EIR_{Rated} \\
+    \,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + \,\,\left( FanPowerCorrection \right)
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  EIR_{Rated} = \left( {\frac{1}{{CO{P_{Rated}}}}} \right)(EIRTempModFa{c_{Rated}})(EIRFlowModFa{c_{Rated}})
+\end{equation}
+
+where,
+
+\emph{EER} = Energy Efficiency Ratio (W/W)
+
+\(Power_{Total,Rated}\) = Total electric power (compressors, condenser fans and evaporator fan) with 19.4°C wet-bulb temperature air entering the cooling coil, 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser, and air flow rate across the evaporator at the rated high speed air flow rate. Similar to the fan heat correction, the fan power correction is calculated in one of two ways depending on the input for internal static pressure.~ If no internal static is provided, fan power is calculated using:
+
+\begin{equation}
+  FanPowerCorrection = {\dot V_{RatedHighSpeed}} * 773.3
+\end{equation}
+
+If the internal static pressure is provided, then the entire VAV fan model in EnergyPlus is evaluated at the rated high speed air flow rate and the total static pressure for rating and the then the fan power calculated by the fan model is used for the fan power correction.
+
+\(TotCapTempModFac_{Rated}\) = Total Cooling Capacity Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
+
+\(EIRTempModFa{c_{Rated}}\) = Energy Input Ratio Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
+
+The Integrated Energy Efficiency Ratio (IEER) is intended to be a measure of merit for the cooling coil's part-load efficiency. IEER replaced Integrated Part-Load Value (IPLV) as the part-load performance metric in Std. 340/360 as of January 1, 2010. Full details regarding the IEER calculation are available in ANSI/AHRI Std. 340/360 (AHRI 2007). A summary of the IEER calculations made by EnergyPlus for two-speed air-cooled DX cooling coils is provided below:
+
+\begin{equation}
+  IEER = \,(0.02 \cdot EE{R_A}) + (0.617 \cdot EE{R_B}) + (0.238 \cdot EE{R_C}) + (0.125 \cdot EE{R_D})
+\end{equation}
+
+where,
+
+\(EER_A\) = \emph{EER} at 100\% net capacity at AHRI standard rating conditions (same as EER calculation shown above but in Btu/h)
+
+\(EER_B\) = \emph{EER} at 75\% net capacity and reduced outdoor air temperature Btu/h
+
+\(EER_C\) = \emph{EER} at 50\% net capacity and reduced outdoor air temperature Btu/h
+
+\(EER_D\) = \emph{EER} at 25\% net capacity and reduced outdoor air temperature Btu/h
+
+The following table summarizes the test points.
+
+% table 58
+\begin{longtable}[c]{p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}}
+\caption{Test points for Two-Speed DX Coil Ratings \label{table:test-points-for-two-speed-dx-coil-ratings}} \tabularnewline
+\toprule 
+Point & Net Capacity & Coil inlet wetbulb & Coil inlet drybulb & Condenser inlet drybulb & Supply air flow rate \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Test points for Two-Speed DX Coil Ratings} \tabularnewline
+\toprule 
+Point & Net Capacity & Coil inlet wetbulb & Coil inlet drybulb & Condenser inlet drybulb & Supply air flow rate \tabularnewline
+\midrule
+\endhead
+
+A & 100\% & 19.4C & 26.7C & 35.0C & Rated High speed flow rate \tabularnewline
+B & 75\% & 19.4C & 26.7C & 27.5C & Regula falsi result where coil leaving drybulb matches Point A \tabularnewline
+C & 50\% & 19.4C & 26.7C & 20.0C \tabularnewline
+D & 25\% & 19.4C & 26.7C & 18.3C \tabularnewline
+\bottomrule
+\end{longtable}
+
+The units are assumed to be VAV and Standard 340/360 is be applied as for VAV indoor supply fan.~ Because the standard stipulates ``the airflow rate at part load should be adjusted to maintain the full load measured leaving dry-bulb temperature,'' the part load rating test points ``B'', ``C'', and ``D'' are evaluated by using the entire DX coil model calculations to obtain the supply air conditions leaving the coil and iterating on supply air flow rate to find the supply air flow rate.~ The numerical method called Regula Falsi is used to find the supply flow rate at each of the part load test points.~ Once the supply air flow rate is known, the two-speed DX coil model results are used to determine EER at the part load test points.
+
+When evaluating the two-speed DX coil model, the speed ratio and cycling ratio are specified based on the desired or target net capacity.~ When the low speed net capacity is lower than the target part load net capacity, the speed ratio is calculated using
+
+\begin{equation}
+SpeedRatio = \frac{{DesiredNetCapacity - LowSpeedNetCapacity}}{{HighSpeedNetCapacity - LowSpeedNetCapacity}}
+\end{equation}
+
+When the low speed net capacity is higher than a target part load net capacity then the unit must cycle to meet the lower load.~ The speed ratio is then set to 0.0 (minimum unloading) and the cycling ratio is calculated using
+
+\begin{equation}
+CyclingRatio = \frac{{DesiredNetCapacity}}{{LowSpeedNetCapacity}}
+\end{equation}
+
+The results for EER, COP, and supply air mass flow rate at the part load test points are reported to the EIO file and a predefined table report called VAV DX Cooling Standard Rating Details.
+
+\subsubsection{References}\label{references-4-001}
+
+See the references for the single speed DX cooling coil earlier in this document.
+
+\subsection{Variable Speed DX Cooling Coil}\label{variable-speed-dx-cooling-coil}
+
+\subsubsection{Overview}\label{overview-4-002}
+
+The Coil:Cooling:DX:VariableSpeed object will simulate the performance of a DX cooling coil used in combination with a variable-speed unitary air conditioner and air-to-air heat pump. It fits into the parent objects of AirLoopHVAC:UnitaryHeatCool, ZoneHVAC:PackagedTerminalAirConditioner, AirLoopHVAC:UnitaryHeatPump:AirToAir and ZoneHVAC:PackagedTerminalHeatPump, etc.
+
+The rated conditions for obtaining the capacities, COPs and SHR~ are indoor dry-bulb temperature at 26.67 ËšC (80 ËšF), wet bulb temperature at 19.44 ËšC (67 ËšF),~ and the source side entering air temperature at 35 ËšC (95 ËšF).
+
+Variable-speed cooling coils lead to varied dehumidification behaviors, that the Bypass Factor (BF) is not only dependent on the indoor air flow rate, but also on the refrigerant mass flow rate, i.e.~the compressor speed. The methods of calculating Bypass factor and Sensible Heat Transfer Ratio at each speed are the same as the water source variable-speed cooling coil (object name Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit).
+
+\subsubsection{Model Description}\label{model-description-3-003}
+
+The Coil:Cooling:DX:VariableSpeed object is modeled in a manner similar to Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit. Of course, rather than referencing a water-cooled condenser, the new coil object references to outdoor air-cooled condenser, and has the air entering temperature in place of the condenser water entering temperature.
+
+It shall be noted for the total cooling capacity and flow rate inputs, two fields are autosizable, which are Rated Total Cooling Capacity at Selected Nominal Speed Level and Rated Volumetric Air Flow Rate at Selected Nominal Speed Level. They are used to scale the performances of an actual unit and correlate with the actual loop flow. Except the two fields, all other total cooling capacity and flow rate inputs at individual speed levels should be directly obtained from Reference Unit catalog.
+
+The Rated Total Cooling Capacity at Selected Nominal Speed Level contains the rated total cooling capacity to match the building sensible or latent cooling load.~ The rated cooling capacity is used to determine a capacity scaling factor, as compared to the Reference Unit catalog capacity at the nominal speed level.
+
+\begin{equation}
+{\rm{CapacityScaleFactor}} = \frac{{{\rm{RatedTotalCoolingCapacity}}}}{{{\rm{ReferenceUnitTotalCoolingCapacity}}@{\rm{NominalSpeedLevel}}}}
+\end{equation}
+
+And then, this scaling factor is used to determine capacities at rated condition for other speed levels, as below,
+
+\begin{equation}
+{\rm{RatedTotalCoolingCapacity}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = {\rm{CapacityScaleFactor}} \times {\rm{ReferenceUnitTotalCoolingCapacity}}@{\rm{SpeedLevel}}({\rm{x}})
+\end{equation}
+
+The Rated Volumetric Air Flow Rate is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects, as follows:
+
+\begin{equation}
+{\rm{AirFlowScaleFactor}} = \frac{{{\rm{RatedVolumetricAirFlowRate}}}}{{{\rm{ReferenceUnitVolAirFlowRate}}@{\rm{NominalSpeedLevel}} \times {\rm{CapacityScaleFactor}}}}
+\end{equation}
+
+And the loop volumetric air flow rates in the parent objects are calculated as below,
+
+\begin{equation}
+{\rm{LoopVolumetricAirFlowRate}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = {\rm{AirFlowScaleFactor}} \times {\rm{ReferenceUnitVolAirFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) \times {\rm{CapacityScaleFactor}}
+\end{equation}
+
+If the volumetric air flow rate at one speed level is higher than the flow rate allowed by the fan in the parent object, the flow rate will be set back to the fan flow rate.
+
+If \({\rm{AirFlowScaleFactor}}\) ~equals to unity, the loop air flow rate become the design flow rates of the original unit (after scaled by the rated total cooling capacity). The Rated Volumetric Air Flow Rate is introduced here to correlate with the actual flow rate in the air loop, in case that these differ from the design specifications. Certainly, it is recommended that the Rated Volumetric Air Flow Rate is selected in the way that \({\rm{AirFlowScaleFactor}}\) ~is unity, so as to get more accurate results from the performance curves.
+
+If the condenser is evaporatively cooled, it is necessary to know the condenser air flow rate, so as to calculate the water evaporation rate. We will have fields for specifying the Reference Unit condenser volumetric air flow rates at individual speed levels, and these inputs are optional. If the condenser air flow rates are not inputted by the user, default values of condenser volumetric air flow rate as a function of the rated total cooling capacity will be used. Condenser air flow rates of the simulated unit are calculated as below,
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{CondenserVolumetricAirFlowRate} @ \rm{SpeedLevel} \left( {\rm{x}} \right) = \\
+    \quad \quad \rm{ReferenceUnitCondenserVolAirFlowRate} @ \rm{SpeedLevel} (\rm{x}) \times \\
+    \quad \quad \quad \rm{CapacityScaleFactor}
+  \end{array}
+\end{equation}
+
+\subsubsection{Performance Curves:}\label{performance-curves}
+
+This object includes 4 curve objects at each individual speed level.
+
+1)~ Total cooling capacity modifier curve (function of temperature)
+
+2)~ Total cooling capacity modifier curve (function of air flow fraction)
+
+3)~ Energy input ratio (EIR) modifier curve (function of temperature)
+
+4)~ Energy input ratio (EIR) modifier curve (function of air flow fraction)
+
+The flow fraction modifier curves are used as a placeholder, to account for off-design flow rates if needed. If the manufacturer doesn't provide the off-design performances, we can simply use a default modification multiplier of 1.0.
+
+At the lowest speed, there will be one additional performance curve to correlate the part-load condition, i.e.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{4}
+\tightlist
+\item
+  Part load fraction correlation (function of part load ratio)
+\end{enumerate}
+
+1)~~~~~Total cooling capacity modifier curve (function of temperature)
+
+The total cooling capacity modifier as a function of temperature curve (CAP-FT) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil and the condenser entering air temperature. The output of this curve is multiplied by the rated total cooling capacity at the speed, to give the total cooling capacity at the specific entering air WB and condenser inlet air DB at which the DX unit is operating (i.e., at temperatures different from the rating point temperatures).
+
+Note: The data used to develop the total cooling capacity modifier curve (function of temperature) should represent performance when the cooling coil is `wet' (i.e., coil providing sensible cooling and at least some dehumidification). Performance data when the cooling coil is `dry' (i.e., not providing any dehumidification) should not be included when developing this modifier curve. This model automatically detects and adjusts for `dry coil' conditions.
+
+\begin{equation}
+{\rm{TotCapTempModFac}} = {\rm{a}} + {\rm{b*W}}{{\rm{B}}_{\rm{i}}} + {\rm{c*WB}}_{\rm{i}}^2 + {\rm{d*D}}{{\rm{B}}_{\rm{o}}} + {\rm{e*D}}{{\rm{B}}_{\rm{o}}}^2 + {\rm{f*W}}{{\rm{B}}_{\rm{i}}}{\rm{*D}}{{\rm{B}}_{\rm{o}}}
+\end{equation}
+
+where
+
+WB\(_{i}\) = wet-bulb temperature of the air entering the indoor cooling coil, °C
+
+DB\(_{o}\) = dry-bulb temperature of the air entering the condenser coil, °C
+
+a-f = regression curve-fit coefficients.
+
+2)~~~~~Total cooling capacity modifier curve (function of air flow fraction)
+
+The total cooling capacity modifier curve (function of air flow fraction) is a cubic curve with the independent variable being the ratio of the actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of design flow at the speed).
+
+\begin{equation}
+{\rm{TotCapAirFlowModFac}} = {\rm{a}} + {\rm{b*f}}{{\rm{f}}_{\rm{a}}} + {\rm{c*ff}}_{\rm{a}}^2 + {\rm{d*ff}}_{\rm{a}}^3
+\end{equation}
+
+where
+
+ff\(_{a}\) = actual air mass flow rate/design air mass flow rate, at one speed level.
+
+~~~~~~~~~ \(\begin{array}{l}{\rm{DesignAirMassFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) = {\rm{}}\\\quad \quad \quad {\rm{ReferenceUnitAirMassFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) \times {\rm{CapacityScaleFactor}}\end{array}\)
+
+a-d = regression curve fit coefficients, if no data for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Energy input ratio (EIR) modifier curve (function of temperature)
+\end{enumerate}
+
+The energy input ratio modifier curve as a function of temperature (EIR-FT) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil and the condenser entering air temperature. The output of this curve is multiplied by the rated EIR (inverse of the rated COP) at the speed level, to give the EIR at the specific entering air temperatures at which the DX unit is operating (i.e., at temperatures different from the rating point temperatures).
+
+\begin{equation}
+{\rm{EIRTempModFac}} = {\rm{a}} + {\rm{b*W}}{{\rm{B}}_{\rm{i}}} + {\rm{c*WB}}_{\rm{i}}^2 + {\rm{d*D}}{{\rm{B}}_{\rm{o}}} + {\rm{e*D}}{{\rm{B}}_{\rm{o}}}^2 + {\rm{f*W}}{{\rm{B}}_{\rm{i}}}{\rm{*D}}{{\rm{B}}_{\rm{o}}}
+\end{equation}
+
+where
+
+a-f = regression curve fit coefficients
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Energy input ratio (EIR) modifier curve (function of air flow fraction)
+\end{enumerate}
+
+\begin{equation}
+{\rm{EIRAirFlowModFac}} = {\rm{a}} + {\rm{b*f}}{{\rm{f}}_{\rm{a}}} + {\rm{c*ff}}_{\rm{a}}^2 + {\rm{d*ff}}_{\rm{a}}^3
+\end{equation}
+
+where
+
+a-d = regression curve fit coefficients, if no data available for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{4}
+\tightlist
+\item
+  Part load fraction correlation (function of part load ratio)
+\end{enumerate}
+
+This field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, Sensible or Latent Load/Steady-State Sensible or Latent Capacity~ for Speed 1). The description of the part load fraction correlation for the variable-speed DX cooling coil is similar to the variable-speed DX heating coil.
+
+\subsubsection{Lowest Speed Operation:}\label{lowest-speed-operation}
+
+The lowest speed operation of the variable-speed DX cooling coil is similar to the single speed DX cooling coil. The total (gross) cooling capacity of the variable-speed DX coil is calculated as follows:
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{Q}_{\rm{total},1} = \rm{RatedTotalCoolingCapacity} @ \rm{SpeedLevel} \left( 1 \right) \rm{*} \\
+    \quad \quad \rm{TotCapTempModFa} \rm{c}_1 \rm{*TotCapAirFlowModFa} \rm{c}_1
+  \end{array}
+\end{equation}
+
+And the EIR is calculated as:
+
+\begin{equation}
+\rm{EI} \rm{R}_1 = \frac{1.0}{\rm{ReferenceUnitCOP} @ \rm{Speed}(1)}{\rm{EIRTempModFa}}{\rm{c}_1}{\rm{*EIRAirFlowModFa}}{\rm{c}_1}
+\end{equation}
+
+And the power consumption excluding the indoor fan is,
+
+\begin{equation}
+{\rm{Powe}}{{\rm{r}}_1} = {{\rm{Q}}_{{\rm{total}},1}}{\rm{*EI}}{{\rm{R}}_1}{\rm{*RTF}}
+\end{equation}
+
+At the lowest speed, the dehumidification calculation is exactly the same as the single speed DX coil. That is to use the rated SHR and the design air flow rate at the lowest speed to calculate rated bypass factor of BF\(_{rated,1}\), and the corresponding effective surface area of A\(_{o,1}\). With A\(_{o,1}\)known, the coil BF can be adjusted for non-rated air flow rates.
+
+And the part load ratio for sensible cooling is,
+
+\begin{equation}
+{\rm{PLR}} = {\rm{SensibleCoolingLoad}}/({{\rm{Q}}_{{\rm{total}},1}}{\rm{*SH}}{{\rm{R}}_1})
+\end{equation}
+
+For latent cooling,
+
+\begin{equation}
+{\rm{PLR}} = {\rm{LatentCoolingLoad}}/[{{\rm{Q}}_{{\rm{total}},1}}{\rm{*}}(1.0 - {\rm{SH}}{{\rm{R}}_1})]
+\end{equation}
+
+\subsubsection{Higher Speed Operation:}\label{higher-speed-operation-1-000}
+
+At the speed level between the lowest and the highest, there is no part-load loss. A parameter of speed ratio (SpeedRatio) is used to define the capacity partition between Speed x-1 and Speed x.
+
+The design air flow rate at the speed ratio are given as following:
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{DesignAirFlowRateSpeedRatio} = \rm{ReferenceUnitAirMassFlowRate} @ \rm{SpeedLevel} \left( \rm{x} - 1 \right) \rm{*} \\
+    \quad \quad \quad \rm{CapacityScaleFactor*} \left( 1 - \rm{SpeedRatio} \right) + \\
+    \quad \quad \rm{ReferenceUnitAirMassFlowRate} @ \rm{SpeedLevel} \left( \rm{x} \right) \rm{*} \\
+    \quad \quad \quad \rm{CapacityScaleFactor*SpeedRatio}
+  \end{array}
+\end{equation}
+
+And the fraction of air flow is given:
+
+\({\rm{f}}{{\rm{f}}_{{\rm{a}},{\rm{x}} - 1}}\) = \({\rm{f}}{{\rm{f}}_{{\rm{a}},{\rm{x}}}}\) = actual air mass flow rate/DesignAirFlowRateSpeedRatio
+
+The total cooling capacities and EIRs at Speed x-1 and Speed x are calculated:
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{Q}_{\rm{total},\rm{x} - 1} = \rm{RatedTotalCoolingCapacity} @ \rm{SpeedLevel} \left( \rm{x} - 1 \right) \rm{*} \\
+    \quad \quad \quad \rm{TotCapTempModFa} \rm{c}_{\rm{x} - 1} \rm{*TotCapAirFlowModFa} \rm{c}_{\rm{x} - 1}
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{Q}_{\rm{total},\rm{x}} = \rm{RatedTotalCoolingCapacity} @ \rm{SpeedLevel} \left( \rm{x} \right) \rm{*} \\
+    \quad \quad \quad \rm{TotCapTempModFa} \rm{c}_{\rm{x}} \rm{*TotCapAirFlowModFa} \rm{c}_{\rm{x}}
+  \end{array}
+\end{equation}
+
+\begin{equation}
+{\rm{EI}}{{\rm{R}}_{{\rm{x}} - 1}} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}({\rm{x}} - 1)}}{\rm{EIRTempModFa}}{{\rm{c}}_{{\rm{x}} - 1}}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_{{\rm{x}} - 1}}
+\end{equation}
+
+\begin{equation}
+{\rm{EI}}{{\rm{R}}_{\rm{x}}} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}\left( {\rm{x}} \right)}}{\rm{EIRTempModFa}}{{\rm{c}}_{\rm{x}}}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_{\rm{x}}}
+\end{equation}
+
+The total cooling capacity at the corresponding speed ratio is:
+
+\begin{equation}
+{{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}} = \left( {1.0 - {\rm{SpeedRatio}}} \right){\rm{*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}} + {\rm{SpeedRatio*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}}}}
+\end{equation}
+
+And the power consumption, excluding the indoor fan, is
+
+\begin{equation}
+{\rm{Powe}}{{\rm{r}}_{{\rm{SpeedRatio}}}} = \left( {1.0 - {\rm{SpeedRatio}}} \right){\rm{*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}}{\rm{*EI}}{{\rm{R}}_{{\rm{x}} - 1}} + {\rm{SpeedRatio*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}}}}{\rm{*EI}}{{\rm{R}}_{\rm{x}}}
+\end{equation}
+
+And the net heat discharged from the condenser:
+
+\begin{equation}
+{{\rm{Q}}_{{\rm{cond}},{\rm{SpeedRatio}}}} = {\rm{Powe}}{{\rm{r}}_{{\rm{SpeedRatio}}}} + {{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}}
+\end{equation}
+
+And the effective surface area in the correlations of BF factor is calculated as below:
+
+\begin{equation}
+{{\rm{A}}_{{\rm{o}},{\rm{SpeedRatio}}}} = \left( {1 - {\rm{SpeedRatio}}} \right){\rm{*}}{{\rm{A}}_{{\rm{o}},{\rm{x}} - 1}} + {\rm{SpeedRatio*}}{{\rm{A}}_{{\rm{o}},{\rm{x}}}}
+\end{equation}
+
+Using A\(_{o,SpeedRatio}\) in the same BF and SHR calculation procedure as the single speed DX cooling coil, we can get BF\(_{SpeedRatio}\), and SHR\(_{SpeedRatio}\). And the sensible cooling capacity is calculated:
+
+\begin{equation}
+{{\rm{Q}}_{{\rm{sensible}},{\rm{SpeedRatio}}}} = {{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}}{\rm{*SH}}{{\rm{R}}_{{\rm{SpeedRatio}}}}
+\end{equation}
+
+If the variable-speed DX cooling coil used to match the sensible cooling load,
+
+\begin{equation}
+{{\rm{Q}}_{{\rm{sensible}},{\rm{SpeedRatio}}}} = {\rm{SensibleLoad}}
+\end{equation}
+
+If it intends to match the latent cooling load,
+
+\begin{equation}
+{{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}}{\rm{*}}\left( {1.0 - {\rm{SH}}{{\rm{R}}_{{\rm{SpeedRatio}}}}} \right) = {\rm{LatentLoad}}
+\end{equation}
+
+If the speed reaches the highest level, the speed ratio becomes 1.0, and Speed n represents the highest speed.
+
+\subsubsection{Evaporatively Cooled Condenser:}\label{evaporatively-cooled-condenser}
+
+If using evaporative pre-cooling pad upstream of the condenser, the user must also enter the appropriate evaporative effectiveness for the media at each compressor speed, so as to correlate variation of the effectiveness as a function of compressor speed, i.e.~the variation of condenser air flow rate. The evaporative effectiveness is interpolated between speed levels, i.e.
+
+\begin{equation}
+{\rm{Effectivenes}}{{\rm{s}}_{{\rm{SpeedRatio}}}} = \left( {1.0 - {\rm{SpeedRatio}}} \right){\rm{*Effectivenes}}{{\rm{s}}_{{\rm{x}} - 1}} + {\rm{SpeedRatio*Effectivenes}}{{\rm{s}}_{\rm{x}}}
+\end{equation}
+
+The interpolated effectiveness at the speed ratio is used to calculate the air temperature reduction across the evaporative cooling pad, and the decreased air temperature entering the condenser coil is used in place of the ambient temperature, i.e.
+
+\begin{equation}
+{{\rm{T}}_{{\rm{c}},{\rm{i}}}} = {{\rm{T}}_{{\rm{wb}},{\rm{o}}}} + (1.0 - {\rm{Effectivenes}}{{\rm{s}}_{{\rm{SpeedRatio}}}}){\rm{*}}({{\rm{T}}_{{\rm{db}},{\rm{o}}}} - {{\rm{T}}_{{\rm{wb}},{\rm{o}}}})
+\end{equation}
+
+Where
+
+\({{\rm{T}}_{{\rm{c}},{\rm{i}}}}\) ~is the condenser entering air temperature, °C.
+
+\({{\rm{T}}_{{\rm{wb}},{\rm{o}}}}\) ~is the outdoor air wet bulb temperature, °C.
+
+\({{\rm{T}}_{{\rm{db}},{\rm{o}}}}\) ~is the outdoor air dry bulb temperature, °C.
+
+And the water consumption rate is calculated based on the interpolated condenser air flow rate at the speed ratio, i.e.~the condenser flow rate at the speed ratio,
+
+\begin{equation}
+{\dot m_{condair,{\rm{}}SpeedRatio}} = \left( {1.0 - SpeedRatio} \right){\rm{*}}{\dot m_{condair,{\rm{}}x - 1}} + SpeedRatio{\rm{*}}{\dot m_{condair,{\rm{}}x}}
+\end{equation}
+
+\subsection{Electric Air Heating Coil}\label{electric-air-heating-coil}
+
+The electric air heating coil (object name: Coil:Heating:Electric) is a simple capacity model with a user-input efficiency.~ In many cases, this efficiency for the electric coil will be 100\%.~ This coil only has air nodes to connect it in the system.~ The coil can be used in the air loop simulation or in the zone equipment as a reheat coil.~ Depending on where it is used determines if this coil is temperature or capacity controlled.~ If used in the air loop simulation it will be controlled to a specified temperature on the setpoint node by the SetpointManager.~ If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand.~ See Input Output Reference for additional information.
+
+For a coil that is controlled to meet the zone demand and will meet the capacity necessary for that zone unless it exceeds the capacity of the coil specified by the user.
+
+~ ! Control output to meet load QCoilReq
+
+~ IF((AirMassFlow .GT. 0.0 .AND. HeatingCoil(CoilNum)\%NominalCapacity \textgreater{} 0.0) .and. \&
+
+~~~~ (GetCurrentScheduleValue(HeatingCoil(CoilNum)\%SchedPtr) .gt. 0.0) .and. \&
+
+~~~~ (QCoilReq .gt. 0.0) .and. (TempSetPoint = = 0.0)) THEN
+
+~ ~~~~!check to see if the Required heating capacity is greater than the user! specified capacity.
+
+~~~~~ IF(QCoilReq \textgreater{} HeatingCoil(CoilNum)\%NominalCapacity) Then
+
+~~~~~~~ QCoilCap = HeatingCoil(CoilNum)\%NominalCapacity
+
+~~~~~ Else
+
+~~~~~~~ QCoilCap = QCoilReq
+
+~~~~~ End IF
+
+~~~~~ TempAirOut = TempAirIn + QCoilCap/CapacitanceAir
+
+~~~~~ HeatingCoilLoad = QCoilCap
+
+~~~~ !The HeatingCoilLoad is the change in the enthalpy of the Heating
+
+~~~~~ HeatingCoil(CoilNum)\%ElecUseLoad = HeatingCoilLoad/Effic
+
+For a temperature setpoint coil the delta temperature from the coil inlet temperature to the setpoint is determined and the capacity of the coil is calculated and is met if less than the user specified capacity.
+
+~~ ! Control coil output to meet a setpoint temperature.
+
+~~ Else IF((AirMassFlow .GT. 0.0 .AND. HeatingCoil(CoilNum)\%NominalCapacity \textgreater{} 0.0) .and. \&
+
+~~~~ (GetCurrentScheduleValue(HeatingCoil(CoilNum)\%SchedPtr) .gt. 0.0) .and. \&
+
+~~~~ (QCoilReq = = 0.0) .and. \&
+
+~~~~ (ABS(TempSetPoint-TempAirIn) .gt. TempControlTol) ) THEN
+
+~~~~~ QCoilCap = CapacitanceAir*(TempSetPoint - TempAirIn)
+
+~~~~~ ! check to see if setpoint above enetering temperature. If not, set
+
+~~~~~ ! output to zero.
+
+~~~~~ IF(QCoilCap .LE. 0.0) THEN
+
+~~~~~~~ QCoilCap = 0.0
+
+~~~~~~~ TempAirOut = TempAirIn
+
+~~~~~ !check to see if the Required heating capacity is greater than the user
+
+~~~~~ ! specified capacity.
+
+~~~~~ Else IF(QCoilCap \textgreater{} HeatingCoil(CoilNum)\%NominalCapacity) Then
+
+~~~~~~~ QCoilCap = HeatingCoil(CoilNum)\%NominalCapacity
+
+~~~~~~~ TempAirOut = TempAirIn + QCoilCap/CapacitanceAir
+
+~~~~~ Else
+
+~~~~~~~ TempAirOut = TempSetPoint
+
+~~~~~ End IF
+
+~~~~~ HeatingCoilLoad = QCoilCap
+
+~~~~ !The HeatingCoilLoad is the change in the enthalpy of the Heating
+
+~~~~~ HeatingCoil(CoilNum)\%ElecUseLoad = HeatingCoilLoad/Effic
+
+\subsection{Gas Air Heating Coil}\label{gas-air-heating-coil}
+
+The gas-powered heating coil (object name: Coil:Heating:Gas) is a simple capacity model with user inputted gas burner efficiency.~ The default for the gas burner efficiency is 80\%.~ This coil only has air nodes to connect it in the system.~ The coil can be used in the air loop simulation or in the zone equipment as a reheat coil.~ Depending on where it is used determines if this coil is temperature or capacity controlled.~ If used in the air loop simulation it will be controlled to a specified temperature scheduled from the SetpointManager.~ If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand.~ The gas coil has additional features that can add a part load correction and a parasitic gas or electric load.
+
+The parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.~ This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation time step.
+
+The parasitic gas load associated with the gas coil's operation (Watts), such as a standing pilot light.~ The model assumes that this parasitic load is consumed only for the portion of the simulation time step where the gas heating coil is not operating.
+
+\subsubsection{Field: Part Load Fraction Correlation (function of part load ratio)}\label{field-part-load-fraction-correlation-function-of-part-load-ratio}
+
+The part load correction defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of gas consumption rate by the heating coil as a function of the part load ratio (PLR, sensible heating load/nominal capacity of the heating coil).~ For any simulation time step, the nominal gas consumption rate (heating load/burner efficiency) is divided by the part-load fraction (PLF) if a part-load curve has been defined.~ The part-load curve accounts for efficiency losses due to transient coil operation.
+
+The part-load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the heating coil runs continuously for the simulation time step).~ For PLR values between 0 and 1 ( 0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+\textbf{PLF \textgreater{} = 0.7~~ and~~ PLF \textgreater{} = PLR}
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds.~ The runtime fraction of the heating coil is defined a PLR/PLF. If PLF \textless{} PLR, then a warning message is issues and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional gas heating coil (e.g., residential furnace) would be:
+
+\begin{equation}
+PLF = 0.8 + 0.2\cdot PLR
+\end{equation}
+
+For a better understanding of how the coil meets the temperature setpoint in the air loop or the zone demand as zone equipment, see Coil:Electric:Heating for additional information.~ Also see Input Output Reference for additional input information.
+
+\subsection{Multi-Stage Electric and Gas Air Heating Coil}\label{multi-stage-electric-and-gas-air-heating-coil}
+
+\subsubsection{Overview}\label{overview-5-001}
+
+These models (object names Coil:Heating:Electric:MultiStage and Coil:Heating:Gas:MultiStage) simulate the performance of multi stage electric and gas heating systems with two to four discrete air flow stages. Each stage has a set of user inputted gas burner efficiency, Nominal capacity, and Parasitic electric load (for gas coil only). The full load supply airflow rate is dependent on the stage number and is set by its parent object (Ref: AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed). The part-load impact on coil energy use is automatically applied to the lowest stage.
+
+When the model determines performance at Stage 1 (the lowest stage) or cycling between OFF and Stage 1, its performance is almost the same as the performance for the Coil:Heating:Electric and~ Coil:Heating:Gas models. However, the outlet conditions are calculated slightly differently. Therefore, the Coil:Heating:Electric and~ Coil:Heating:Gas model may be considered as subsets of the multistage model described here. When the multistage coil model determines performance at higher stages (above 1), the model linearly interpolates the performance at two consecutive stages (n-1 and n) as needed to meet the heating load, with the fraction of time at each speed established by the speed ratio. For the time being, this coil model can only be called by the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
+
+\subsubsection{Model Inputs}\label{model-inputs-1}
+
+The model inputs are also very similar to the inputs of the Coil:Heating:Electric and~ Coil:Heating:Gas objects. The main difference is that this multistage model requires a set of fields at each speed, such as nominal capacity, and efficiency.
+
+\subsubsection{Stage 1 Operation}\label{stage-1-operation}
+
+The following procedure provides the detailed description of the exception.
+
+n~Total delivered heating capacity
+
+The total delivered heating capacity for Stage 1 operating at the cycling ratio needed to meet the requested heating load is:
+
+\begin{equation}
+  Q_{coil,cycling} = {\mathop m\limits^\cdot_{Speed\,1}} \left( CycRatio \right) (h_{inlet} - h_{outlet,full})
+\end{equation}
+
+where,
+
+\emph{Q\(_{coil,cycling}\)} = delivered sensible heating capacity for Stage 1 operating at a specific cycling ratio {[}W{]}
+
+\({\mathop m\limits^\cdot_{Speed\,\,1}}\) = air mass flow rate through heating coil at Speed 1 as set by the parent object {[}kg/s{]}
+
+\emph{h\(_{outlet,full}\)} = specific enthalpy of the coil outlet air during full-load operation at Stage 1 (no cycling) {[}J/kg{]}
+
+\emph{h\(_{inlet}\)} = specific enthalpy of the coil inlet air {[}J/kg{]}
+
+\emph{CycRatio} = cycling ratio at Stage 1, ratio of requested heating load to the full-load capacity of the coil at Stage 1 {[}dimensionless{]}
+
+It is assumed that the coil provides no heating capacity when the coil is OFF, even if the supply air fan continues to operate.
+
+n~Outlet air specific enthalpy
+
+The average specific enthalpy of the coil outlet air is then calculated based on the delivered sensible heating capacity and the average air mass flow rate entering the coil:
+
+\begin{equation}
+  h_{outlet,average} = h_{inlet} - \frac{Q_{coil,cycling}}{{\mathop m\limits^\cdot }_{inlet}}
+\end{equation}
+
+where,
+
+\emph{h\(_{outlet,average}\)}~ = average specific enthalpy at the coil outlet {[}J/kg{]}
+
+\({\mathop m\limits^\cdot_{inlet}}\) ~~~~~~~~ = mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiStage, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the heating coil is ON and the specified flow rate when the heating coil is OFF for the time step being simulated.
+
+n~Outlet air temperature
+
+The heating coil's outlet air humidity ratio equals the inlet air humidity ratio since the coil does not change the moisture content of the air. So the average outlet air temperature is calculated based on the inlet air humidity ratio and the average outlet air enthalpy using the psychrometric function PsyTdbFnHW.
+
+The main reason for using the above approach is that outlet air conditions are calculated in the same way for all operating Stages.
+
+\subsubsection{Higher Stage Operation}\label{higher-stage-operation}
+
+This section describes how higher Stage operation is simulated. When the required sensible load is less than the full load sensible capacity at Stage n (Stage Number \textgreater{} 1), the following calculations are performed:
+
+n~Total delivered heating capacity at Stage n-1 and Stage n
+
+\begin{equation}
+TotCa{p_{n - 1}} = MSNominalCa{p_{n - 1}}
+\end{equation}
+
+\begin{equation}
+TotCa{p_n} = MSNominalCa{p_n}
+\end{equation}
+
+where,
+
+\emph{TotCap\(_{i}\)} = total delivered heating capacity at given temperatures and flow rates at Stage i {[}W{]}
+
+\emph{MSNominalCap\(_{i}\)} = heating capacity at the rated conditions at Stage i {[}W{]}
+
+i = Stage n or Stage n-1
+
+n~Full load outlet air specific enthalpy at Stage n-1 and Stage n
+
+\begin{equation}
+{h_{outlet,full_Speed_n}} = {h_{inlet}} - (MSNominalCa{p_n}/{\mathop m\limits^._{inlet}})
+\end{equation}
+
+\begin{equation}
+{h_{outlet,full_Speede_n - 1}} = {h_{inlet}} - (MSNominalCa{p_{n - 1}}/{\mathop m\limits^._{inlet}})
+\end{equation}
+
+where,
+
+\emph{h\(_{outlet,full\_Stage\_n}\)} = specific enthalpy of the coil outlet air during full-load operation at Stage n (no cycling) {[}J/kg{]}
+
+\emph{h\(_{outlet,full\_Stage\_n-1}\)} = specific enthalpy of the coil outlet air during full-load operation at Stage n-1 (no cycling) {[}J/kg{]}
+
+n~Effective total heating capacity
+
+\begin{equation}
+  \begin{array}{l}
+    Q_{coil,SpeedRatio} = \left( SpeedRatio \right){\mathop m\limits^\cdot_{Speed\,n}}(h_{inlet} - h_{outlet,full_Speed\,n}) \\
+    \;\;\;\;\;\;\;\;\;\; + (1 - SpeedRatio) {\mathop m\limits^\cdot_{Speed\,n - 1}}(h_{inlet} - h_{outlet,full_Speed\,n - 1})
+  \end{array}
+\end{equation}
+
+where,
+
+\({{Q_{coil,SpeedRatio}}}\) = delivered sensible heating capacity at a given Stage ratio between two consecutive Stages {[}W{]}
+
+\({\mathop {{\rm{ }}m}\limits_{Speed{\kern 1pt} n}^ \cdot }\) ~~~~~ = air mass flow rate through heating coil at Stage n as set by the parent object {[}kg/s{]}
+
+\({\mathop {{\rm{ }}m}\limits_{Speed{\kern 1pt} n - 1}^ \cdot }\) ~~~ = air mass flow rate through heating coil at Stage 1 as set by the parent object {[}kg/s{]}
+
+n~Average outlet air enthalpy
+
+\begin{equation}
+  h_{outlet,average} = h_{inlet} - \frac{Q_{coil,SpeedRatio}}{{\mathop m\limits^\cdot }_{inlet}}
+\end{equation}
+
+where,
+
+\emph{h\(_{outlet,average}\)} = average specific enthalpy at the coil outlet {[}J/kg{]}
+
+\emph{h\(_{inlet}\)} = specific enthalpy of the coil inlet air {[}J/kg{]}
+
+\({\dot m_{inlet}}\) = Mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiStage, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the heating coil is at Stage n and the specified flow rate when the heating coil is at Stage n-1 for the time step being simulated.
+
+n~Average outlet air temperature
+
+The heating coil's outlet air humidity ratio equals the inlet air humidity ratio since the coil does not change the moisture content of the air. So the average outlet air temperature is calculated based on the inlet air humidity ratio and the average outlet air enthalpy using the psychrometric function PsyTdbFnHW.
+
+n~Full load energy inputs at Stage n-1 and Stage n
+
+\begin{equation}
+HeatingPowe{r_n} = MSNominalCa{p_n}/MSEfficienc{y_n}
+\end{equation}
+
+\begin{equation}
+HeatingPowe{r_{n - 1}} = MSNominalCa{p_{n - 1}}/MSEfficienc{y_{n - 1}}
+\end{equation}
+
+where,
+
+\emph{MSEfficiency\(_{n}\)} = Efficiency at stage n
+
+\emph{MSEfficiency\(_{n-1}\)} = Efficiency at stage n-1
+
+n~Calculate combined energy input
+
+\begin{equation}
+HeatingPower = HeatingPowe{r_n}\left( {SpeedRatio} \right) + HeatingPowe{r_{n - 1}}(1.0 - SpeedRatio)
+\end{equation}
+
+where,
+
+HeatingPower = Power used in Watt
+
+\subsection{Single-Speed Electric Heat Pump DX Air Heating Coil}\label{single-speed-electric-heat-pump-dx-air-heating-coil}
+
+\subsubsection{Overview}\label{overview-6-000}
+
+This model (object name Coil:Heating:DX:SingleSpeed) simulates the performance of an air-to-air direct expansion (DX) heating system. The model uses performance information at rated conditions along with curve fits for variations in total capacity, energy input ratio and part-load fraction to determine the performance of the unit at part-load conditions (DOE 1982).~ Adjustment factors are applied to total capacity and input power to account for frost formation on the outdoor coil.
+
+This model simulates the thermal performance of the indoor DX heating coil, and the power consumption of the outdoor unit (compressors, fans, crankcase heaters and defrost heaters). The performance of the indoor supply air fan varies widely from system to system depending on control strategy (e.g., constant fan vs.~AUTO fan, constant air volume vs.~variable air volume, etc.), fan type, fan motor efficiency and pressure losses through the air distribution system. Therefore, this DX system model does not account for the thermal effects or electric power consumption of the indoor supply air fan. EnergyPlus contains separate models for simulating the performance of various indoor fan configurations, and these models can be easily linked with the DX system model described here to simulate the entire DX system being considered (e.g., see AirLoopHVAC:UnitaryHeatPump:AirToAir).
+
+\subsubsection{Model Inputs}\label{model-inputs-2}
+
+The user must input the total heating capacity, coefficient of performance (COP) and the volumetric airflow rate across the heating coil at rated conditions. The capacity and COP inputs should be ``gross'' values, excluding any thermal or energy impacts due to the indoor supply air fan. The rating condition is considered to be outdoor air at 8.33C dry-bulb and 6.11C wet-bulb temperatures (i.e., air entering the outdoor coil), with air entering the indoor DX heating coil at 21.11C dry-bulb and 15.55C wet-bulb temperatures. The rated volumetric air flow across the DX heating coil should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of rated total heating capacity (300 -- 450 cfm/ton).
+
+Depending on the defrost strategy that is selected, the user must also input up to six performance curves that describe the change in total heating capacity and efficiency at part-load conditions, and efficiency during reverse-cycle defrosting:
+
+n~The total heating capacity modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the rated total heating capacity to give the total heating capacity at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
+
+\begin{equation}
+TotCapTempModFac = \,a + \,b\left( {{T_{db,o}}} \right)\,\, + \,\,c{\left( {{T_{db,o}}} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+TotCapTempModFac = \,a + \,b\left( {{T_{db,o}}} \right)\,\, + \,\,c{\left( {{T_{db,o}}} \right)^2}\,\, + \,\,d{\left( {{T_{db,o}}} \right)^3}
+\end{equation}
+
+\begin{equation}
+TotCapTempModFac = \,a + \,b\left( {{T_{db,i}}} \right)\,\, + \,\,c{\left( {{T_{db,i}}} \right)^2}\,\, + \,\,d\left( {{T_{db,o}}} \right) + e{\left( {{T_{db,o}}} \right)^2} + f\left( {{T_{db,i}}} \right)\left( {{T_{db,o}}} \right)
+\end{equation}
+
+where
+
+\({T_{db,i}}\) ~~~~ = dry-bulb temperature of the air entering the indoor coil, °C
+
+\({T_{db,o}}\) ~~~~ = dry-bulb temperature of the air entering the outdoor coil, °C
+
+n~The total heating capacity modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated total heating capacity and the total heating capacity modifier curve (function of temperature) to give the total heating capacity at the specific temperature and air flow conditions at which the coil is operating.
+
+\begin{equation}
+TotCapFlowModFac = \,a + \,b\left( {ff} \right)\,\, + \,\,c{\left( {ff} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+TotCapFlowModFac = \,a + \,b\left( {ff} \right)\,\, + \,\,c{\left( {ff} \right)^2}\,\, + \,\,d{\left( {ff} \right)^3}
+\end{equation}
+
+where
+
+\begin{equation}
+ff = flow{\rm{ }}fraction = \left( {\frac{{Actual{\rm{ }}air{\rm{ }}mass{\rm{ }}flow{\rm{ }}rate}}{{Rated{\rm{ }}air{\rm{ }}mass{\rm{ }}flow{\rm{ }}rate}}} \right)
+\end{equation}
+
+\textbf{Note:}~ The actual volumetric airflow rate through the heating coil for any simulation time step where the DX unit is operating should be between 0.00002684 m\(^{3}\)/s and .00008056 m\(^{3}\)/s per watt of rated total heating capacity (200 - 600 cfm/ton). The simulation will issue a warning message if this airflow range is exceeded.
+
+n~The energy input ratio (EIR) modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
+
+\begin{equation}
+EIRTempModFac = \,a + \,b\left( {{T_{db,o}}} \right)\,\, + \,\,c{\left( {{T_{db,o}}} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+EIRTempModFac = \,a + \,b\left( {{T_{db,o}}} \right)\,\, + \,\,c{\left( {{T_{db,o}}} \right)^2}\,\, + \,\,d{\left( {{T_{db,o}}} \right)^3}
+\end{equation}
+
+or
+
+\begin{equation}
+EIRTempModFac = \,a + \,b\left( {{T_{db,i}}} \right)\,\, + \,\,c{\left( {{T_{db,i}}} \right)^2}\,\, + \,\,d\left( {{T_{db,o}}} \right) + e{\left( {{T_{db,o}}} \right)^2} + f\left( {{T_{db,i}}} \right)\left( {{T_{db,o}}} \right)
+\end{equation}
+
+n~The energy input ratio (EIR) modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating.
+
+\begin{equation}
+EIRFlowModFac = \,a + \,b\left( {ff} \right)\,\, + \,\,c{\left( {ff} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+EIRFlowModFac = \,a + \,b\left( {ff} \right)\,\, + \,\,c{\left( {ff} \right)^2}\, + \,\,d{\left( {ff} \right)^3}
+\end{equation}
+
+n~The part-load fraction correlation (function of part-load ratio) is a quadratic or cubic curve with the independent variable being part-load ratio (sensible heating load / steady-state heating capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the ``effective'' EIR for a given simulation time step. The part-load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
+
+\begin{equation}
+PartLoadFrac = \,PLF\, = \,a + \,b\left( {PLR} \right)\,\, + \,\,c{\left( {PLR} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+PartLoadFrac = \,a + \,b\left( {PLR} \right)\,\, + \,\,c{\left( {PLR} \right)^2}\,\, + \,\,d{\left( {PLR} \right)^3}
+\end{equation}
+
+where
+
+\begin{equation}
+PLR = part - load\,ratio = \left( {\frac{{sensible\,heating\,load}}{{steady - state\,sensible\,heating\,capacity}}} \right)
+\end{equation}
+
+The part-load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation time step). For PLR values between 0 and 1 ( 0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7~~ and~~ PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined a PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional, single-speed DX heating coil (e.g., residential heat pump) would be:
+
+~~~~~~~~~~~ PLF = 0.85 + 0.15(PLR)
+
+n~The defrost energy input ratio (EIR) modifier curve (function of temperature) is a bi-quadratic curve with two independent variables: outdoor air dry-bulb temperature and the heating coil entering air wet-bulb temperature. The output of this curve is multiplied by the heating coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the coil is operating. This curve is only required when a reverse-cycle defrost strategy is specified.
+
+\begin{equation}
+DefrostEIRTempModFac = \,a + \,b\left( {{T_{wb,i}}} \right)\,\, + \,\,c{\left( {{T_{wb,i}}} \right)^2} + \,\,d\left( {{T_{db,o}}} \right)\,\, + \,\,e{\left( {{T_{db,o}}} \right)^2} + f\left( {{T_{wb,i}}} \right)\left( {{T_{db,o}}} \right)
+\end{equation}
+
+where
+
+\({T_{wb,i}}\) ~~~~ ~ = wet-bulb temperature of the air entering the indoor heating coil, °C
+
+\({T_{db,o}}\) ~~~~ = dry-bulb temperature of the air entering the outdoor coil, °C
+
+All six curves are accessed through EnergyPlus' built-in performance curve equation manager (curve:quadratic, curve:cubic and curve:biquadratic). It is not imperative that the user utilize all coefficients shown in the preceding equations \{ through \} in items (1) through (6) if their performance equation has fewer terms (e.g., if the user's PartLoadFrac performance curve is linear instead of quadratic or cubic, simply enter the appropriate values for the coefficients a and b, and set the remaining coefficients to zero).
+
+The next input item for the Heating DX single speed coil is the supply air fan operation mode. Either the supply air fan runs continuously while the DX coil cycles on/off, or the fan and coil cycle on/off together. The next two inputs define the minimum outdoor dry-bulb temperature that the heat pump compressor will operate and the maximum outdoor dry-bulb temperature for defrost operation. Crankcase heater capacity and crankcase heater cutout temperature are entered in the following two inputs. The final four inputs cover the type of defrost strategy (reverse-cycle or resistive), defrost control (timed or on-demand), the fractional defrost time period (timed defrost control only), and the resistive defrost heater capacity if a resistive defrost strategy is selected.
+
+\subsubsection{Model Description}\label{model-description-4-001}
+
+The general flow of the model is as follows:
+
+1)~~~~If the outdoor air dry-bulb temperature is below the specified minimum temperature for compressor operation or the DX heating coil is not scheduled to operate, simply pass through the heating coil inlet air conditions as the coil outlet conditions, set power and heating rates equal to zero, and set crankcase heater power equal to the crankcase heater capacity value specified by the input file.
+
+2)~~~~If the outdoor air dry-bulb temperature is above the specified minimum temperature for compressor operation and the DX heating coil is scheduled to operate, then:
+
+a.~~~~If the outdoor dry-bulb temperature is below the specified maximum outdoor dry-bulb temperature for defrost operation, calculate a heating capacity multiplier, input power multiplier and fractional defrost time period depending on the defrost strategy and defrost control type specified for the heating coil.
+
+b.~~~Using the rated heating capacity and COP, the part-load curves specified for the DX heating coil, the defrost multipliers calculated above (if applicable), and the part-load ratio that is being requested of the heating coil, determine the following: heating coil exiting air conditions (dry-bulb temperature, humidity ratio and enthalpy), total DX coil heating rate, electric power during heating (compressors and outdoor fans), electric power during defrost, and crankcase heater power.
+
+The following paragraphs give a detailed description of the model calculations that are performed when the DX heating coil is operating (i.e., scenario \# 2 above).
+
+\subsubsection{Frost Adjustment Factors}\label{frost-adjustment-factors}
+
+Frost formation on the outdoor coil, and the need to periodically defrost this coil, has a significant impact on heating capacity and energy use by the DX heating system. If the outdoor air dry-bulb temperature is below the specified maximum temperature for defrost operation, then the model calculates adjustment factors for heating capacity and input power due to frost formation, and the fractional defrost time period, depending on the defrost strategy and defrost control type specified for the heating coil. This method of accounting for the impacts of frosting/defrost was taken from the model used in DOE-2.1E (ESTSC 2001, Miller and Jaster 1985).
+
+The model first estimates the outdoor coil temperature according to a linear empirical relationship with outdoor air dry-bulb temperature as the independent variable.
+
+\begin{equation}
+{T_{coil,out}} = 0.82{T_{db,o}} - 8.589
+\end{equation}
+
+The difference between the outdoor air humidity ratio (from the weather file) and the saturated air humidity ratio at the estimated outdoor coil temperature is then calculated, and this value is used as an indication of frost formation on the outdoor coil.
+
+\begin{equation}
+\Delta {\omega_{\,coil,out}}\, = \,MAX\left[ {1.0E - 6,\,\,\,{\omega_{outdoor}}\, - \,\,{\omega_{sat}}\left( {{T_{coil,out}}\,,{\rm{OutBaroPress}}} \right)} \right]
+\end{equation}
+
+Frost formation on the outdoor coil must be periodically removed. The fraction of compressor runtime when the coil is being defrosted is either entered by the user (for timed defrost) or is calculated by the model (for on-demand defrost) using an empirical equation and \(\Delta {\omega_{\,coil,out}}\) . Adjustment factors to total heating coil capacity and input power due to frost formation on the outdoor coil are also calculated by empirical models with \(\Delta {\omega_{\,coil,out}}\) ~or fractional defrost time period as the independent variable. The defrost time period fraction and adjustment factors due to frost formation on the outdoor coil vary depending on the defrost control type as shown below.
+
+\emph{Timed Defrost}:
+
+\begin{equation}
+Fractional\,Defrost\,Time\, = \,time\,period\,specified\,by\,user = {t_{frac,defrost}}
+\end{equation}
+
+\begin{equation}
+Heating\,Capacity\,Multiplier\, = \,0.909 - \,107.33\left( {\Delta {\omega_{\,coil,out}}} \right)
+\end{equation}
+
+\begin{equation}
+Input\,Power\,Multiplier\, = \,0.9 - \,36.45\left( {\Delta {\omega_{\,coil,out}}} \right)
+\end{equation}
+
+\emph{On-Demand Defrost}:
+
+\begin{equation}
+Fractional\,Defrost\,Time\, = \,\frac{1}{{1 + \left( {\frac{{0.01446}}{{\Delta {\omega_{\,coil,out}}}}} \right)}} = {t_{frac,defrost}}
+\end{equation}
+
+\begin{equation}
+Heating\,Capacity\,Multiplier\, = \,0.875\left( {1 - {t_{frac,defrost}}} \right)
+\end{equation}
+
+\begin{equation}
+Input\,Power\,Multiplier\, = \,0.954\left( {1 - {t_{frac,defrost}}} \right)
+\end{equation}
+
+If the outdoor air dry-bulb temperature is above the specified maximum temperature for defrost operation, the fractional defrost time period is set to zero and the heating capacity/input power multipliers are set to unity.
+
+\subsubsection{Defrost Operation}\label{defrost-operation}
+
+If the fractional defrost time period is greater than zero for the simulation time step, then the model calculates the electrical power used during defrost. The method for calculating defrost power varies based on the defrost strategy specified (i.e., reverse-cycle or resistive). In the case of reverse-cycle defrost, the additional heating load due to defrost (indoor cooling during defrost) is also calculated so that it may be added to the existing heating load when calculating input power for the compressor(s) and outdoor coil fan(s).
+
+\emph{Reverse-Cycle}:
+
+\begin{equation}
+{Q_{defrost}}\, = \,0.01\left( {{t_{frac,defrost}}} \right)\left( {7.222 - {T_{db,o}}} \right)\left( {\frac{{{Q_{total,rated}}}}{{1.01667}}} \right)
+\end{equation}
+
+\begin{equation}
+{P_{defrost}}\, = \,DefrostEIRTempModFac\left( {\frac{{{Q_{total,rated}}}}{{1.01667}}} \right)\left( {{t_{frac,defrost}}} \right)\left( {RTF} \right)
+\end{equation}
+
+\emph{Resistive}:
+
+\begin{equation}
+{Q_{defrost}}\, = \,0.0
+\end{equation}
+
+\begin{equation}
+{P_{defrost}}\, = \,\left( {{Q_{cap,defrost}}} \right)\left( {{t_{frac,defrost}}} \right)\left( {RTF} \right)
+\end{equation}
+
+where:
+
+\({Q_{defrost}}\) ~~~~~~~ = additional indoor heating load due to reverse-cycle defrost (\emph{W})
+
+\({Q_{total,rated}}\) ~~~ = total full-load heating capacity of the coil at rated conditions (W)
+
+\({P_{defrost}}\) ~~~~~~~ = average defrost power for the simulation time step (W)
+
+\({Q_{cap,defrost}}\) ~~ = capacity of the resistive defrost heating element (W)
+
+\emph{DefrostEIRTempModFac} = energy input ratio modifier curve applicable during defrost
+
+\begin{equation}
+{\rm{RTF  =  }}\left( {{\raise0.7ex\hbox{{{\rm{PLR}}}} \!\mathord{\left/ {\vphantom {{{\rm{PLR}}} {{\rm{PartLoadFrac}}}}}\right.}\!\lower0.7ex\hbox{{{\rm{PartLoadFrac}}}}}} \right)\,\,{\rm{ = }}\,\,runtime fraction of the heating coil
+\end{equation}
+
+\subsubsection{Heating Operation}\label{heating-operation-000}
+
+For any simulation time step, the total heating capacity of the DX unit is calculated as follows:
+
+\begin{equation}
+Qtotal = Qtotal,rated\left( {TotCapTempModFac} \right)\left( {TotCapFlowModFac} \right)
+\end{equation}
+
+If the outdoor air dry-bulb temperature is below the maximum temperature for defrost operation, then the total heating capacity is further adjusted due to outdoor coil frost formation based on the results of Equation and Equation or .
+
+\begin{equation}
+Qtotal = Qtotal\left( {HeatingCapacityMultiplier} \right)
+\end{equation}
+
+In a similar fashion, the electrical power draw by the DX unit (compressors plus outdoor coil fans) for any simulation time step is calculated. For a reverse-cycle defrost strategy, the additional heating load (\emph{Q\(_{defrost}\)}) generated during defrost operation is added to the heating load being requested by adjusting the part-load ratio. If a resistive defrost strategy is selected, \emph{Q\(_{defrost}\)} = 0. The part-load fraction correlation for the heating coil (user input, Equation or ) is used in the calculation of electrical power draw to account for efficiency losses due to compressor cycling.
+
+\begin{equation}
+  PLR = \,MIN \left( 1.0\,,\,PLR + \left( \frac{Q_{defrost}}{Q_{total}} \right) \right)
+\end{equation}
+
+\begin{equation}
+PartLoadFrac = \,a + \,b\left( {PLR} \right)\,\, + \,\,c{\left( {PLR} \right)^2}\,\, + \,\,d{\left( {PLR} \right)^3}
+\end{equation}
+
+\begin{equation}
+  P_{heating} = \frac{{\left( {{Q_{total}}} \right)\left( {EIR} \right)\left( {PLR} \right)}}{{PartLoadFrac}} \times InputPowerMultiplier
+\end{equation}
+
+where
+
+\({P_{heating}}\) = average compressor and outdoor fan power for the simulation time step(W)
+
+\({Q_{total}}\) = total heating capacity W, Eqn.
+
+\begin{equation}
+  EIR = \,Energy\,input\,ratio\, = \,\left( {\frac{1}{{CO{P_{rated}}}}} \right)\left( {EIRTempModFac} \right)\left( {EIRFlowModFac} \right)
+\end{equation}
+
+\(CO{P_{rated}}\) ~ = coefficient of performance at rated conditions (user input)
+
+\emph{InputPowerMultiplier} = power adjustment due to frost if applicable -Eqn. or
+
+The crankcase heater is assumed to operate when the heating coil's compressor is OFF, and the average crankcase heater power for the simulation time step is calculated as follows:
+
+\begin{equation}
+  {P_{crankcase}} = {Q_{cap,crankcase}}\left( {1 - RTF} \right)
+\end{equation}
+
+\({\rm{RTF = }}\left( {{\raise0.7ex\hbox{{{\rm{PLR}}}} \!\mathord{\left/ {\vphantom {{{\rm{PLR}}} {{\rm{PartLoadFrac}}}}}\right.}\!\lower0.7ex\hbox{{{\rm{PartLoadFrac}}}}}} \right)\,\,{\rm{ = }}\,\,runtime fraction of the heating coil\)
+
+where
+
+\({P_{crankcase}}\) = average crankcase heater power for the simulation time step (W)
+
+\({Q_{cap,crankcase}}\) = crankcase heater capacity (W)
+
+If this heating coil is used as part of an air-to-air heat pump (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir), the crankcase heater defined for this DX heating coil is enabled during the time that the compressor is not running for either heating or cooling (and the crankcase heater power defined in the DX cooling coil object is disregarded in this case). In this instance, RTF in the above equations would be the runtime fraction of the heat pump's heating coil or cooling coil, whichever is greater.
+
+The properties of the air leaving the heating coil at full-load operation are calculated using the following equations:
+
+\begin{equation}
+  h_{outlet} = h_{inlet} + \frac{Q_{total}}{{\mathop m\limits^ \bullet }}
+\end{equation}
+
+\begin{equation}
+{\omega_{outlet}}\, = \,{\omega_{inlet}}
+\end{equation}
+
+\begin{equation}
+{T_{db,outlet}}\, = \,PsyTdbFnHW({h_{outlet}},\,\,\,{\omega_{outlet}})
+\end{equation}
+
+where
+
+\({h_{outlet}}\) ~~~~~~~~ = enthalpy of the air leaving the heating coil (J/kg)
+
+\(\,{\omega_{outlet}}\) ~~~~~~~ = leaving air humidity ratio (kg/kg)
+
+\(\,{T_{db,outlet}}\) ~~~ = leaving air dry-bulb temperature (°C)
+
+\emph{PsyTdbFnHW} = EnergyPlus psychrometric function, returns dry-bulb temp given enthalpy and humidity ratio
+
+\subsubsection{Condenser Inlet Air Temperature}\label{condenser-inlet-air-temperature-1}
+
+The air temperature entering the outdoor condenser is based on the weather data used during a simulation. This temperature is either taken directly from the weather data, or can be adjusted based on the height of the outdoor condenser. Since this DX heating coil can only be used in conjunction with a DX cooling coil, the input for Condenser Air Inlet Node Name in the DX cooling coil object can be used to control this optional feature. If this input is left blank, the air temperature entering the condenser is based solely on the weather data. If this input is not blank, then the node name specified must also be listed in an OutdoorAir:Node or OutdoorAir:NodeList object. When the node name is listed in an OutdoorAir:NodeList object, the air temperature entering the condenser is based solely on the weather data. When the node name is listed in an OutdoorAir:Node object, the height of the node determines the air temperature entering the outdoor condenser (see description of Local Outdoor Air Temperature Calculation in the Atmospheric Variation section of this document for further details).
+
+\subsubsection{Supply Air Fan Control: Cycling vs.~Continuous}\label{supply-air-fan-control-cycling-vs.continuous-1}
+
+One of the inputs to the DX coil model is the supply air fan operation mode: cycling fan, cycling compressor (CyclingFanAndCompressor) or continuous fan, cycling compressor (ContinuousFanWithCyclingCompressor). The first operation mode is frequently referred to as ``AUTO fan'', where the compressor(s) and supply air fan operate in unison to meet the zone heating load, and cycle off together when the heating load has been met. The second operation mode is often referred to as ``fan ON'', where the compressor(s) cycle on and off to meet the zone heating load but the supply air fan operates continuously regardless of compressor operation.
+
+Since this DX heating coil can only be used in conjunction with a DX cooling coil (i.e.~heat pumps), and these coils are used in AC equipment that specifies a fan operation mode schedule (e.g AirLoopHVAC:UnitaryHeatPump:AirToAir), the selection made in the DX heating coil is currently ignored and the fan operation mode schedule value determines the fan operation mode for each time step throughout the simulation. A fan operation mode schedule value of 0 specifies AUTO fan mode operation while values other than 0 specify fan ON operation. The use of a schedule allows the fan operation mode to change based on time-of-day or with changes in season.
+
+The EnergyPlus methodology for determining the impact that HVAC equipment has on an air stream is to calculate the mass flow rate and air properties (e.g., enthalpy, dry-bulb temperature, humidity ratio) exiting the equipment. These exiting conditions are passed along as inlet conditions to the next component model in the air stream. Eventually the flow rate and properties of the air being supplied to the conditioned zone are used in the zone energy balance to determine the resulting zone air temperature and humidity ratio.
+
+With this methodology, the determination of the air mass flow rate and air properties for the two different supply air fan operation modes is slightly different. For the case of cycling fan/cycling compressor, the conditions of the air leaving the heating coil are the steady-state values calculated using equations , and above. However the air mass flow rate passed along to the next component (and eventually to the conditioned zone) is the average air mass flow rate for the system simulation time step (determined by the heating system; see AirLoopHVAC:UnitaryHeatPump:AirToAir). For this fan control type, the heating coil part-load fraction (Equation or ) is also passed to Fan:OnOff (if used) to properly calculate the supply air fan power and associated fan heat.
+
+For the case of continuous fan/cycling compressor, the air mass flow rate is constant. However, the air properties leaving the heating coil are calculated as the average conditions during the system simulation time step. The model assumes that the exiting air conditions are the steady-state values calculated using equations , and above when the compressor(s) operate. For the remainder of the system simulation time step, it is assumed that the air exiting the DX coil has the same properties as the air entering the coil. For this supply air fan operating strategy, the leaving air properties are calculated as follows:
+
+\begin{equation}
+{h_{outlet,ContFanCycComp}}\, = \,{h_{outlet}}\,\left( {PLR} \right) + \,{h_{inlet}}\,\,\left( {1 - PLR} \right)
+\end{equation}
+
+\begin{equation}
+{\omega_{outlet,ContFanCycComp}}\, = \,{\omega_{outlet}}\,\left( {PLR} \right) + \,{\omega_{inlet}}\,\,\left( {1 - PLR} \right)
+\end{equation}
+
+\begin{equation}
+{T_{db,outlet,ContFanCycComp}} = \,PsyTdbFnHW({h_{outlet,\,ContFanCycComp}}\,,\,\,\,\,\,\,\,{\omega_{outlet,ContFanCycComp}})
+\end{equation}
+
+\subsubsection{References}\label{references-5-001}
+
+DOE. 1982. \emph{DOE-2 engineers manual}, version 2.1A. LBL-11353. Berkeley, CA: Lawrence Berkeley National Laboratory.
+
+ESTSC. 2001. DOE-2.1E Version 110 (source code).Oak Ridge, TN: Energy Science and Technology Software Center.
+
+Miller, R.L. and Jaster, H. 1985. Performance of Air-Source Heat Pumps. EM-4226. Palo Alto, CA: Electric Power Research Institute.
+
+\subsection{Single-Speed DX Heating Coil Standard Ratings}\label{single-speed-dx-heating-coil-standard-ratings}
+
+For single-speed direct expansion (DX) heating coils, the industry standard ratings of High Temperature Heating Standard (Net) Rating Capacity, Low Temperature Heating Standard (Net) Rating Capacity and Heating Seasonal Performance Factor (HSPF) are calculated according to ANSI/AHRI Standard 210/240 (AHRI 2008). The rated Energy Efficiency Ratio (EER) is not calculated for any DX heatings coils at this time.
+
+For the Coil:Heating:DX:SingleSpeed object in EnergyPlus, these standard ratings are not direct inputs to the model. However, these standard ratings can be calculated using user-entered information for the Coil:Heating:DX:SingleSpeed object. These standard rating values are provided in the eplusout.eio output file (Ref. OutputDetailsAndExamples.pdf) and also in the predefined tabular output reports (Output:Table:SummaryReports object, Equipment Summary). Currently, the standard ratings are only calculated and output for single-speed DX heating coils..
+
+Note: The standard ratings described in this section require that the DX heating coil model be evaluated at specific operating conditions (i.e., specific temperatures for air entering the heating coil and for air entering the air-cooled {[}outdoor{]} condenser). If the heating coil performance curves can not be evaluated at the required test conditions, then a standard rating value will be calculated at user specified curve limit as an output and a warning message will written to eplusout.err. For example, if the curve object (Curve:Biquadratic) for Total Heating Capacity Function of Temperature Curve has a minimum value of -5C for dry-bulb temperature entering the condenser coil, the HSPF calculation requires that heating capacity and EIR be calculated at -8.33C, so this would result in HSPF value calculated at -5C as an output and a warning message in the eplusout.err file.
+
+\subsubsection{High Temperature Heating Standard (Net) Rating Capacity}\label{high-temperature-heating-standard-net-rating-capacity}
+
+The procedure for calculating the Standard Rating Heating Capacity is given by:
+
+\begin{equation}
+{\dot Q_{HighStandardRating}} = {\dot Q_{total,Rated}}\left( {TotCapTempModFa{c_{Rated}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{HighStandard\,Rating\,Net}} = {\dot Q_{HighStandardRating}} + Fa{n_{Power,\,Rated}}
+\end{equation}
+
+where,
+
+\({\dot Q_{HighStandardRating\,Net}}\) ~ = Total standard (net) heating capacity (W) of the air-source heat pump equipment in heating mode determined from ANSI/AHRI Standard 210/240 and test conditions shown in Table~\ref{table:heating-mode-test-conditions-for-units-having}. The standard heating test conditions for air-cooled condenser are: indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb 8.33°C.
+
+\({\dot Q_{HighStandardRating}}\) ~ = ~Total standard heating capacity (W) of the air-source heat pump equipment in heating mode determined from ANSI/AHRI Standard 210/240 and test conditions shown in Table~\ref{table:generalized-climatic-region-information}. The standard heating test conditions for air-cooled condenser are: indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb 8.33°C.
+
+\({\dot Q_{total,Rated}}\) ~ = Rated total heating capacity, user input (W)
+
+\(TotCapTempModFa{c_{Rated}}\) = User-specified bi-quadratic curve evaluated at the indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb 8.33°C for air-cooled condenser as specified in Table~\ref{table:heating-mode-test-conditions-for-units-having}, (dimensionless).
+
+\(Fa{n_{Power,Rated}}\) = Supply air fan power at rated conditions, (W). The Rated Indoor Coil Fan Power Per Volume Flow rate is a user-entered value, with a default of 773.3 W/(m3/s)) if the user leaves this input field blank. The default value is taken from ANSI/ASHRAE Standard 210/240-2008 where it is defined for systems which do not have an Indoor Coil fan furnished as part of the system. See the description given at the end of this section for how this value is calculated.
+
+\subsubsection{Low Temperature Heating Standard (Net) Rating Capacity}\label{low-temperature-heating-standard-net-rating-capacity}
+
+The procedure for calculating the Low Temperature Standard Rating Heating Capacity is given by:
+
+\begin{equation}
+{\dot Q_{LowStandardRating}} = {\dot Q_{total,Rated}}\left( {TotCapTempModFa{c_{H3Test}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{LowStandard\,Rating\,Net}} = {\dot Q_{LowStandardRating}} + Fa{n_{Power,\,Rated}}
+\end{equation}
+
+where,
+
+\({\dot Q_{LowStandardRating\,Net}}\) ~ = Total standard (net) heating capacity (W) of the air-source heat pump equipment in heating mode determined from ANSI/AHRI Standard 210/240 and test conditions shown in Table~\ref{table:generalized-climatic-region-information}. The standard heating test conditions for air-cooled condenser are: indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb (-8.33) °C.
+
+\({\dot Q_{LowStandardRating}}\) ~ = ~~~ Total standard heating capacity (W) of the air-source heat pump equipment in heating mode determined from ANSI/AHRI Standard 210/240 and test conditions shown in Table~\ref{table:heating-mode-test-conditions-for-units-having}. The standard heating test conditions for air-cooled condenser are: indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb (-8.33) °C.
+
+\({\dot Q_{total,Rated}}\) ~ = Rated total heating capacity, user input (W)
+
+\(TotCapTempModFa{c_{H3Test}}\) = User-specified bi-quadratic curve evaluated at the indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb (-8.33) °C for air-cooled condenser as specified in Table~\ref{table:generalized-climatic-region-information}, (dimensionless).
+
+\(Fa{n_{Power,Rated}}\) = Supply air fan power at rated conditions, (W). The Rated Indoor Coil Fan Power Per Volume Flow rate is a user-entered value, with a default of 773.3 W/(m3/s)) if the user leaves this input field blank. The default value is taken from ANSI/ASHRAE Standard 210/240-2008 where it is defined for systems which do not have an Indoor Coil fan furnished as part of the system. See the description given at the end of this section for how this value is calculated.
+
+\subsubsection{Heating Seasonal Performance Factor (HSPF)}\label{heating-seasonal-performance-factor-hspf}
+
+Heating Seasonal Performance Factor (HSPF) is defined as the total space heating required during the space heating season, divided by the total electrical energy consumed by the heat pump system during the same season.
+
+Calculations of HSPF of a heat pump having a single-speed compressor that was tested with a fixed speed indoor fan installed, a constant-air-volume-rate indoor fan installed, or with no indoor fan installed is given below.
+
+\begin{equation}
+HSPF = \frac{{\sum\limits_j^J {\left[ {\frac{{{n_j}}}{N} \cdot BL({T_j})} \right]} }}{{\sum\limits_j^J {\left[ {\frac{{{e_h}({T_j})}}{N}} \right]}  + \sum\limits_j^J {\left[ {\frac{{RH({T_j})}}{N}} \right]} }} \cdot {F_{def}}
+\end{equation}
+
+Where,
+
+\(\frac{{{e_h}({T_j})}}{N}\) ~ = The ratio of the electrical energy consumed by the heat pump during periods of the ~space heating season when the outdoor temperature fell within the range represented by bin temperature \({T_j}\) ~to the total number of hours in the heating season (N), W.
+
+\(\frac{{RH({T_j})}}{N}\) = The ratio of the electrical energy used for resistive space heating during periods when the outdoor temperature fell within the range represented by bin temperature \({T_j}\) ~to the total number of hours in the heating season (N),W.
+
+\({T_j}\) = The outdoor bin temperature, °C. Outdoor temperatures are ``binned'' such that calculations are only performed based one temperature within the bin. Bins of 2.78 °C are used.
+
+\(\frac{{{n_j}}}{N}\) = Fractional bin hours for the heating season; the ratio of the number of hours during the heating season when the outdoor temperature fell within the range represented by bin temperature \({T_j}\) ~to the total number of hours in the heating season, dimensionless. Obtain \(\frac{{{n_j}}}{N}\) ~values from Table \# 17 of AHRI Std. 210/240-2008 (Table~\ref{table:generalized-climatic-region-information} below).
+
+\[j\] = The bin number, dimensionless.
+
+\(J\) = For each generalized climatic region, the total number of temperature bins, dimensionless. Referring to Table \# 17, \(J\) ~is the highest bin number (\[j\] ) having a nonzero entry for the fractional bin hours for the generalized climatic region of interest.
+
+\({F_{def}}\) = The demand defrost credit described in section 3.9.2 of AHRI Std. 210/240-2008, dimensionless.~ For simplification, assigned a value of 1 for timed defrost control and a value of 1.03 for demand defrost control.
+
+\(BL({T_j})\) = The building space conditioning load corresponding to an outdoor temperature of\({T_j}\) ; the heating season building load also depends on the generalized climatic region's outdoor design temperature and the design heating requirement, W.
+
+Building heating load can be evaluated by using the following equation
+
+\begin{equation}
+  BL({T_j}) = \frac{{\left( {18.33 - {T_j}} \right)}}{{\left( {18.33 - {T_{OD}}} \right)}} \cdot C \cdot DHR
+\end{equation}
+
+Where,
+
+\(T_{OD}\) = The outdoor design temperature, °C. An outdoor design temperature is specified for each generalized climatic region in Table \# 17 of AHRI Std. 210/240-2008 (Table~\ref{table:generalized-climatic-region-information} below).
+
+\(C\) = 0.77, a correction factor which tends to improve the agreement between calculated and measured building loads, dimensionless.
+
+\(DHR\) = Design Heating Requirement, W. This is the amount of heating required to maintain a given indoor temperature at a particular outdoor design temperature.
+
+For a single speed heat pump with a fixed speed indoor fan installed, a constant-air-volume-rate indoor fan installed, or with no indoor fan installed, the minimum and maximum design heating requirements for each generalized climatic region can be calculated as follows:
+
+\begin{equation}
+  DHR_{\min } =
+  \left\{ 
+    \begin{array}{l}
+      {\mathop Q\limits^ \cdot_h}(8.33) \cdot (1.8) \cdot \left[ {\frac{{18.33 - {T_{OD}}}}{{60.0}}} \right] , {\rm{ for regions I,II,III,IV, and VI}} \\
+      {\mathop Q\limits^ \cdot_h}(8.33),{\rm{                     for regions V}}
+    \end{array}
+  \right\}
+\end{equation}
+
+\begin{equation}
+DH{R_{\max }} = \left\{ \begin{array}{l}2 \cdot {\mathop Q\limits^ \cdot_h}(8.33) \cdot (1.8) \cdot \left[ {\frac{{18.33 - {T_{OD}}}}{{60}}} \right],{\rm{ for regions I,II,III,IV, and VI}}\\\\2.2 \cdot {\mathop Q\limits^ \cdot_h}(8.33),{\rm{                     for regions V}}\end{array} \right\}
+\end{equation}
+
+Both \(DH{R_{\min }}\) and \(DH{R_{\max }}\) above should be rounded to the nearest standardized DHR given in Table~\ref{table:standardized-design-heating-requirements-w}.
+
+The intermediate term used in the calculations of HSPF can be calculated using the equations described below.
+
+\begin{equation}
+\frac{{{e_h}({T_j})}}{N} = \frac{{X({T_j}) \cdot \mathop {{E_h}}\limits^ \cdot  ({T_j}) \cdot \delta ({T_j})}}{{PL{F_j}}} \cdot \frac{{{n_j}}}{N}
+\end{equation}
+
+\begin{equation}
+\frac{{RH({T_j})}}{N} = \left[ {BL({T_j}) - \left( {X({T_j}) \cdot \mathop {{Q_h}}\limits^ \cdot  ({T_j}) \cdot \delta ({T_j})} \right)} \right] \cdot \frac{{{n_j}}}{N}
+\end{equation}
+
+Where,
+
+\begin{equation}
+X({T_j}) = \left\{ 
+    \begin{array}{l}
+      BL({T_J})/\mathop {{Q_h}}\limits^ \cdot  ({T_j}) \\
+      {\rm{Or}} \\
+      1
+    \end{array}
+  \right\}
+\end{equation}
+
+whichever is less; the heating mode load factor for temperature bin \[j\] , dimensionless.
+
+\(\mathop {{Q_h}}\limits^ \cdot ({T_j})\) = the space heating capacity of the heat pump when operating at outdoor temperature \({T_j}\) , ~W.
+
+\(\mathop {{E_h}}\limits^ \cdot ({T_j})\) = the electrical power consumption of the heat pump when operating at outdoor temperature \({T_j}\) , W.
+
+\(\delta ({T_j})\) = the heat pump low temperature cut-out factor, dimensionless.
+
+\(PL{F_j}\) ~ = the part load factor, dimensionless.
+
+Part load factor is determined as follows:
+
+\begin{equation}
+PL{F_j} = 1 - {C_{{D^h}}}[1 - X({T_j})]
+\end{equation}
+
+Where,
+
+\({C_{{D^h}}}\) = Degradation coefficient which is defaulted to the value of 0.25
+
+Low temperature cut-out factor \(\delta ({T_j})\) is determined as follows:
+
+\begin{equation}
+\delta ({T_j}) = \left\{ 
+    \begin{array}{l}
+      {\rm{0, if }}{T_j} \le {T_{off}}{\rm{ or }}\frac{{\mathop {{Q_h}}\limits^ \cdot  ({T_j})}}{{\mathop {{E_h}}\limits^ \cdot  ({T_j})}} < 1 \\
+      {\rm{1/2, if }}{T_{off}} < {T_j} \le {T_{on}}{\rm{ and }}\frac{{\mathop {{Q_h}}\limits^ \cdot  ({T_j})}}{{\mathop {{E_h}}\limits^ \cdot  ({T_j})}} \ge 1 \\
+      {\rm{1, if }}{T_j} > {T_{on}}{\rm{ and }}\frac{{\mathop {{Q_h}}\limits^ \cdot  ({T_j})}}{{\mathop {{E_h}}\limits^ \cdot  ({T_j})}} \ge 1
+    \end{array}
+  \right.
+\end{equation}
+
+where,
+
+\({T_{off}}\) ~ = the outdoor temperature when the compressor is automatically shut off, °C. (If no such temperature exists, \({T_j}\) is always greater than \({T_{off}}\) and\({T_{on}}\) ).
+
+\({T_{on}}\) = the outdoor temperature when the compressor is automatically turned back on, if applicable, following an automatic shut-off, °C.
+
+Calculate \(\mathop {{Q_h}}\limits^ \cdot ({T_j})\) and \(\mathop {{E_h}}\limits^ \cdot ({T_j})\) ~using,
+
+\begin{equation}
+\mathop {{Q_h}}\limits^ \cdot  ({T_j}) = \left\{ \begin{array}{l}\mathop {{Q_h}}\limits^ \cdot  ( - 8.33) + \frac{{\left[ {\mathop {{Q_h}}\limits^ \cdot  (8.33) - \mathop {{Q_h}}\limits^ \cdot  ( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{16.67}}{\rm{, if }}{T_j} \ge 7.22^\circ {\rm{C or }}{T_j} \le  - 8.33^\circ {\rm{C}}\\\mathop {{Q_h}}\limits^ \cdot  ( - 8.33) + \frac{{\left[ {\mathop {{Q_h}}\limits^ \cdot  (1.67) - \mathop {{Q_h}}\limits^ \cdot  ( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{10}}{\rm{, if }} - 8.33^\circ {\rm{C}} < {T_j} < 7.22^\circ {\rm{C}}\end{array} \right.
+\end{equation}
+
+\begin{equation}
+\mathop {{E_h}}\limits^ \cdot  ({T_j}) = \left\{ \begin{array}{l}\mathop {{E_h}}\limits^ \cdot  ( - 8.33) + \frac{{\left[ {\mathop {{E_h}}\limits^ \cdot  (8.33) - \mathop {{E_h}}\limits^ \cdot  ( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{16.67}}{\rm{, if }}{T_j} \ge 7.22^\circ {\rm{C or }}{T_j} \le  - 8.33^\circ {\rm{C}}\\\mathop {{E_h}}\limits^ \cdot  ( - 8.33) + \frac{{\left[ {\mathop {{E_h}}\limits^ \cdot  (1.67) - \mathop {{E_h}}\limits^ \cdot  ( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{10}}{\rm{, if }} - 8.33^\circ {\rm{C}} < {T_j} < 7.22^\circ {\rm{C}}\end{array} \right.
+\end{equation}
+
+\(\mathop {{Q_h}}\limits^ \cdot ( - 8.33),\mathop {{Q_h}}\limits^ \cdot (1.67),\mathop {{Q_h}}\limits^ \cdot (8.33),\mathop {{E_h}}\limits^ \cdot ( - 8.33),\mathop {{E_h}}\limits^ \cdot (1.67)\) ~and \(\mathop {{E_h}}\limits^ \cdot (8.33)\) ~are the \textbf{(net)} values calculated using performance curves entered by the user and supply fan power per rated air flow rate.
+
+% table 59
+{\scriptsize
+\begin{longtable}[c]{>{\raggedright}p{2.0in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}>{\raggedright}p{1.0in}}
+\caption{Heating Mode Test Conditions for Units Having a Single-Speed Compressor and a Fixed-Speed Indoor Fan, a Constant Air Volume Rate Indoor Fan, or No Indoor Fan \label{table:heating-mode-test-conditions-for-units-having}} \tabularnewline
+\toprule 
+Test description & \multicolumn{2}{p{1.5in}}{\raggedright Air Entering Indoor UnitTemperature (°C)} & \multicolumn{2}{p{1.5in}}{\raggedright Air Entering Outdoor UnitTemperature (°C)} & Heating Air Volume Rate \tabularnewline
+\cmidrule(r){2-3}
+\cmidrule(l){4-5}
+& Dry Bulb & Wet Bulb & Dry Bulb & Wet Bulb & \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Heating Mode Test Conditions for Units Having a Single-Speed Compressor and a Fixed-Speed Indoor Fan, a Constant Air Volume Rate Indoor Fan, or No Indoor Fan} \tabularnewline
+\toprule 
+Test description & \multicolumn{2}{p{1.5in}}{\raggedright Air Entering Indoor UnitTemperature (°C)} & \multicolumn{2}{p{1.5in}}{\raggedright Air Entering Outdoor UnitTemperature (°C)} & Heating Air Volume Rate \tabularnewline
+\cmidrule(r){2-3}
+\cmidrule(l){4-5}
+& Dry Bulb & Wet Bulb & Dry Bulb & Wet Bulb & \tabularnewline
+\midrule
+\endhead
+
+H1 Test (Required, Steady) & 21.11 & 15.56 & 8.33 & 6.11 & Heating Full-load \tabularnewline
+H1C Test (Required, Steady) & 21.11 & 15.56 & 8.33 & 6.11 & (2) \tabularnewline
+H2 Test (Required, Steady) & 21.11 & 15.56 & 1.67 & 0.56 & Heating Full-load \tabularnewline
+H3 Test (Required, Steady) & 21.11 & 15.56 & -8.33 & -9.44 & Heating Full-load \tabularnewline
+\bottomrule
+\multicolumn{6}{p{6in}}{\scriptsize \raggedright Notes: 1) Heating air volume arte are defined in section 3.1.4.4 of ANSI/AHRI 210/240-2008  2) Maintain the airflow nozzles static pressure difference ro velocity pressure during the ON periodat the same pressure difference or velocity pressure as measured during the H1 Test} \tabularnewline
+\multicolumn{6}{p{6in}}{\scriptsize Source: Table 9, Page 74, ANSI/AHRI Standard 210/240 -2008}
+\end{longtable}}
+
+% table 60
+{\scriptsize
+\begin{longtable}[c]{p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}}
+\caption{Generalized Climatic Region Information \label{table:generalized-climatic-region-information}} \tabularnewline
+\toprule 
+\multicolumn{2}{p{1.5in}}{\scriptsize \raggedright Region Number} & I & II & III & IV & V & VI \tabularnewline
+\multicolumn{2}{p{1.5in}}{\scriptsize \raggedright Heating Load Hours, HLH} & 750 & 1250 & 1750 & 2250 & 2750 & *2750 \tabularnewline
+\multicolumn{2}{p{1.5in}}{\scriptsize \raggedright Outdoor Design Temperature, \(T_{OD}\) (°C)} & 2.78 & -2.78 & -8.33 & -15 & -23.33 & -1.11 \tabularnewline
+\midrule
+\(j\) & \(T_j\) (°C) & \multicolumn{6}{c}{Fractional Bin Hours \(\frac{n_j}{N}\)} \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Generalized Climatic Region Information} \tabularnewline
+\toprule 
+\(j\) & \(T_j\) (°C) & \multicolumn{6}{c}{Fractional Bin Hours \(\frac{n_j}{N}\)} \tabularnewline
+\midrule
+\endhead
+
+1 & 16.67 & .291 & .215 & .153 & .132 & .106 & .113 \tabularnewline
+2 & 13.89 & 0.239 & 0.189 & 0.142 & 0.111 & 0.092 & 0.206 \tabularnewline
+3 & 11.11 & 0.194 & 0.163 & 0.138 & 0.103 & 0.086 & 0.215 \tabularnewline
+4 & 8.33 & 0.129 & 0.143 & 0.137 & 0.093 & 0.076 & 0.204 \tabularnewline
+5 & 5.56 & 0.081 & 0.112 & 0.135 & 0.1 & 0.078 & 0.141 \tabularnewline
+6 & 2.78 & 0.041 & 0.088 & 0.118 & 0.109 & 0.087 & 0.076 \tabularnewline
+7 & 0 & 0.019 & 0.056 & 0.092 & 0.126 & 0.102 & 0.034 \tabularnewline
+8 & -2.78 & 0.005 & 0.024 & 0.042 & 0.087 & 0.094 & 0.008 \tabularnewline
+9 & -5.56 & 0.001 & 0.008 & 0.021 & 0.055 & 0.074 & 0.003 \tabularnewline
+10 & -8.33 & 0 & 0.002 & 0.009 & 0.036 & 0.055 & 0 \tabularnewline
+11 & -11.11 & 0 & 0 & 0.005 & 0.026 & 0.047 & 0 \tabularnewline
+12 & -13.89 & 0 & 0 & 0.002 & 0.013 & 0.038 & 0 \tabularnewline
+13 & -16.67 & 0 & 0 & 0.001 & 0.006 & 0.029 & 0 \tabularnewline
+14 & -19.44 & 0 & 0 & 0 & 0.002 & 0.018 & 0 \tabularnewline
+15 & -22.22 & 0 & 0 & 0 & 0.001 & 0.01 & 0 \tabularnewline
+16 & -25 & 0 & 0 & 0 & 0 & 0.005 & 0 \tabularnewline
+17 & -27.78 & 0 & 0 & 0 & 0 & 0.002 & 0 \tabularnewline
+18 & -30.56 & 0 & 0 & 0 & 0 & 0.001 & 0 \tabularnewline
+\bottomrule
+\multicolumn{8}{l}{\scriptsize * Pacific Coast Region} \tabularnewline
+\multicolumn{8}{l}{\scriptsize Source: Table 17, Page 99, ANSI/AHRI Standard 210/240 --- 2008}
+\end{longtable}}
+
+% table 61
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Standardized Design Heating Requirements (W) \label{table:standardized-design-heating-requirements-w}} \tabularnewline
+\toprule 
+\tabularnewline
+\endfirsthead
+
+\caption[]{Standardized Design Heating Requirements (W)} \tabularnewline
+\toprule 
+\tabularnewline
+\endhead
+
+1465.356 & 7326.78 & 14653.56 & 26376.41 \tabularnewline
+2930.712 & 8792.136 & 17584.27 & 29307.12 \tabularnewline
+4396.068 & 10257.49 & 20514.98 & 32237.83 \tabularnewline
+5861.424 & 11722.85 & 23445.7 & 38099.26 \tabularnewline
+\bottomrule
+\multicolumn{4}{l}{\scriptsize Source: Table 18, Page 100, ANSI/AHRI Standard 210/240 -2008}
+\end{longtable}
+
+\subsection{Multi-Speed Electric Heat Pump DX Air Heating Coil}\label{multi-speed-electric-heat-pump-dx-air-heating-coil}
+
+\subsubsection{Overview}\label{overview-7-000}
+
+This model (object name Coil:Heating:DX:MultiSpeed:) simulates the performance of an air-to-air direct expansion (DX) heating system. The main difference compared to the other heating coil model (Coil:Heating:DX:SingleSpeed) is that this heating coil allows modeling of two to four discrete compressor speeds. Each speed has a set of corresponding performance information at rated conditions along with curve fits for variations in total capacity, energy input ratio and part-load fraction to determine the performance of the unit at part-load conditions (DOE 1982). The full load supply airflow rate is dependent on the speed number and is set by its parent object (Ref: AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed). The part-load impact on coil energy use is automatically applied to the lowest speed. A choice is provided to determine whether part-load impacts on coil energy use are applied when the coil is operating at speeds greater than Speed 1. Adjustment factors applied to total capacity and input power to account for frost formation on the outdoor coil are calculated at each speed.
+
+This model simulates the thermal performance of the indoor DX heating coil, and the power consumption of the outdoor unit (multispeed compressor, fans, crankcase heaters and defrost heaters). The performance of the indoor supply air fan varies widely from system to system depending on control strategy (e.g., constant fan vs.~AUTO fan), fan type, fan motor efficiency and pressure losses through the air distribution system. Therefore, this DX system model does not account for the thermal effects or electric power consumption of the indoor supply air fan. EnergyPlus contains separate models for simulating the performance of various indoor fan configurations, and these models can be easily linked with the DX system model described here to simulate the entire DX system being considered. For the time being, this coil model can only be called by the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
+
+When the model determines performance at Speed 1 (the lowest speed) or cycling between OFF and Speed 1, its performance is almost the same as the performance for the Coil:Heating:DX:SingleSpeed model. However, the outlet conditions are calculated slightly differently. Therefore, the Coil:Heating:DX:SingleSpeed model may be considered as a subset of the model described here. When the multispeed coil model determines performance at higher speeds (above 1), the model linearly interpolates the performance at two consecutive speeds (n-1 and n) as needed to meet the heating load, with the fraction of time at each speed established by the speed ratio.
+
+When single mode operation is specified at higher speeds (above 1), defined in the UnitarySystemPerformance:Multispeed object, a child object of AirLoopHVAC:UnitarySystem, its performance is almost the same as the performance for the Coil:Heating:DX:SingleSpeed model at different flow rate and capacity with given speed number. No linear interpolation is performed between two adjacent speeds. The highest speed which does not exceed the sensible load is used for each HVAC timestep. This operation does not apply to speed 1 operation and the case when the sensible load is above the highest sensible capacity.
+
+\subsubsection{Model Inputs}\label{model-inputs-3}
+
+The model inputs are also very similar to the inputs of the Coil:Heating:DX:SingleSpeed object. The main difference is that this multispeed model requires a set of fields at each speed, such as rated capacity, rated COP, two capacity modifiers, two energy input ratio modifiers, and part-load correction. The inputs also include waste heat fraction and modifier as a function of temperature to calculate recoverable waste heat for heat recovery, which are not available in the similar Coil:Heating:DX:SingleSpeed object.
+
+\subsubsection{Speed 1 Operation}\label{speed-1-operation-1}
+
+The calculation procedures in this model, including defrost and crankcase heater, are indentical to the Coil:Heating:DX:SingleSpeed object (Ref: Coil:Heating:DX:SingleSpeed) with one exception: outlet node condition calculation when the supply air fan operation mode is ContinuousFanWithCyclingCompressor. The following procedure provides the detailed description of the exception.
+
+n~Total delivered heating capacity
+
+The total delivered heating capacity for speed 1 operating at the cycling ratio needed to meet the requested heating load is:
+
+\begin{equation}
+{Q_{coil,cycling}} = {\mathop m\limits^\cdot_{Speed\,1}}\left( {CycRatio} \right)({h_{inlet}} - {h_{outlet,full}})
+\end{equation}
+
+where,
+
+\emph{Q\(_{coil,cycling}\)}~~~~~ = delivered sensible heating capacity for Speed 1 operating at a specific cycling ratio {[}W{]}
+
+\(\mathop {{\rm{ }}m}\limits_{Speed{\kern 1pt} 1}^ \cdot\) ~~~~~ = air mass flow rate through heating coil at Speed 1 as set by the parent object {[}kg/s{]}
+
+\emph{h\(_{outlet,full}\)}~~~~~ = specific enthalpy of the coil outlet air during full-load operation at Speed 1 (no cycling) {[}J/kg{]}
+
+\emph{h\(_{inlet}\)~~~~~~~~~~~}~~~~~~~~~~~ = specific enthalpy of the coil inlet air {[}J/kg{]}
+
+\emph{CycRatio}~~~ = cycling ratio at Speed 1, ratio of requested heating load to the full-load capacity of the coil at Speed 1 {[}dimensionless{]}
+
+It is assumed that the coil provides no heating capacity when the coil is OFF, even if the supply air fan continues to operate.
+
+n~Outlet air specific enthalpy
+
+The average specific enthalpy of the coil outlet air is then calculated based on the delivered sensible heating capacity and the average air mass flow rate entering the coil:
+
+\begin{equation}
+  h_{outlet,average} = h_{inlet} - \frac{Q_{coil,cycling}}{\dot{m}_{inlet}}
+\end{equation}
+
+where,
+
+\emph{h\(_{outlet,average}\)}~ = average specific enthalpy at the coil outlet {[}J/kg{]}
+
+\({\dot m_{inlet}}\) ~~~~~~~~ = mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the heating coil is ON and the specified flow rate when the heating coil is OFF for the time step being simulated.
+
+n~Outlet air temperature
+
+The heating coil's outlet air humidity ratio equals the inlet air humidity ratio since the coil does not change the moisture content of the air. So the average outlet air temperature is calculated based on the inlet air humidity ratio and the average outlet air enthalpy using the psychrometric function PsyTdbFnHW.
+
+The main reason for using the above approach is that outlet air conditions are calculated in the same way for all operating speeds.
+
+The crankcase heater defined for this DX heating coil is enabled during the time that the compressor is not running for either heating or cooling. The crankcase heater power use from either heating or cooling is reported in the heating coil.
+
+\subsubsection{Higher Speed Operation}\label{higher-speed-operation-2}
+
+This section describes how higher speed operation is simulated. When the required sensible load is less than the full load sensible capacity at Speed n (Speed Number \textgreater{} 1), the following calculations are performed:
+
+n~Total delivered heating capacity at Speed n-1 and Speed n
+
+\(TotCa{p_{n - 1}} = RatedCa{p_{n - 1}}\left( {TotCapTempModFa{c_{n - 1}}} \right)\left( {TotCapFlowModFa{c_{n - 1}}} \right)\) \(TotCa{p_n} = RatedCa{p_n}\left( {TotCapTempModFa{c_n}} \right)\left( {TotCapFlowModFa{c_n}} \right)\)
+
+where,
+
+\emph{TotCap\(_{i}\)} = total delivered heating capacity at given temperatures and flow rates at Speed i {[}W{]}
+
+\emph{RatedCap\(_{i}\)} = heating capacity at the rated conditions at Speed i {[}W{]}
+
+\emph{TotCapTempModFac\(_{i}\)} = total heating capacity modifier as a function of indoor and outdoor air dry-bulb temperature at Speed i
+
+\emph{TotCapFlowModFac\(_{i}\)} = total heating capacity modifier as a function of the ratio of the actual flow rate across the heating coil to the rated airflow rate at Speed i
+
+i~~~~ = Speed n or Speed n-1
+
+n~EIR at Speed n-1 and Speed n
+
+\begin{equation}
+EI{R_{n - 1}} = RatedEI{R_{n - 1}}\left( {EIRTempModFa{c_{n - 1}}} \right)\left( {EIRFlowModFa{c_{n - 1}}} \right)
+\end{equation}
+
+\begin{equation}
+EI{R_n} = RateEI{R_n}\left( {EIRTempModFa{c_n}} \right)\left( {EIRFlowModFa{c_n}} \right)
+\end{equation}
+
+where,
+
+\emph{EIR\(_{i}\)} = energy input ratio at given temperatures and flow rates at Speed i {[}W{]}
+
+\emph{RatedEIR\(_{i}\)} = energy input ratio at the rated conditions at Speed i {[}W{]}
+
+\emph{EIRTempModFac\(_{i}\)} = energy input ratio modifier as a function of indoor and outdoor air dry-bulb temperature at Speed i
+
+\emph{EIRFlowModFac\(_{i}\)} = energy input ratio modifier as a function of the ratio of the actual flow rate across the heating coil to the rated airflow rate at Speed i
+
+i~~~~ = Speed n or Speed n-1
+
+n~Full load outlet air specific enthalpy at Speed n-1 and Speed n
+
+\begin{equation}
+  h_{outlet,full_Speed,n} = h_{inlet} - \frac{TotCap_{n} \cdot HeatingCapacityMultiplier}{\dot{m}_{inlet}}
+\end{equation}
+
+\begin{equation}
+  h_{outlet,full_Speed,n-1} = h_{inlet} - \frac{TotCap_{n-1} \cdot HeatingCapacityMultiplier}{\dot{m}_{inlet}}
+\end{equation}
+
+where,
+
+\emph{HeatingCapacityMultiplier}~~~~~~~~~~~ = frost adjustment factor for heating capacity (See Ref. Coil:Heating:DX:SingleSpeed)
+
+\emph{h\(_{outlet,full\_Speed\\ n}\)}~~~~~~~~ = specific enthalpy of the coil outlet air during full-load operation at Speed n (no cycling) {[}J/kg{]}
+
+\emph{h\(_{outlet,full\_Speed\\ n-1}\)}~~~~~~ = specific enthalpy of the coil outlet air during full-load operation at Speed n-1 (no cycling) {[}J/kg{]}
+
+n~Effective total heating capacity
+
+\begin{equation}
+  \begin{array}{rl}
+    Q_{coil,SpeedRatio} &= \PB{SpeedRatio} \dot{m}_{Speed n} \PB{h_{inlet} - h_{outlet,full_Speed n}} \\
+                        &+ \PB{1 - SpeedRatio} \dot{m}_{Speed n - 1} \PB{h_{inlet} - h_{outlet,full_Speed n - 1}}
+  \end{array}
+\end{equation}
+
+where,
+
+\({{Q_{coil,SpeedRatio}}}\) = delivered sensible heating capacity at a given speed ratio between two consecutive speeds {[}W{]}
+
+\({\mathop {{\rm{ }}m}\limits_{Speed{\kern 1pt} n}^ \cdot }\) ~~~~~ = air mass flow rate through heating coil at Speed n as set by the parent object {[}kg/s{]}
+
+\({\mathop {{\rm{ }}m}\limits_{Speed{\kern 1pt} n - 1}^ \cdot }\) ~~~ = air mass flow rate through heating coil at Speed 1 as set by the parent object {[}kg/s{]}
+
+n~Average outlet air enthalpy
+
+\begin{equation}
+  h_{outlet,average} = h_{inlet} - \frac{Q_{coil,SpeedRatio}}{\dot{m}_{inlet}}
+\end{equation}
+
+where,
+
+\emph{h\(_{outlet,average}\)}~ = average specific enthalpy at the coil outlet {[}J/kg{]}
+
+\emph{h\(_{inlet}\)~~~~~~~~~~~}~~~~~~~~~~~ = specific enthalpy of the coil inlet air {[}J/kg{]}
+
+\({\dot m_{inlet}}\) ~~~~~~~~ = Mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the heating coil is at Speed n and the specified flow rate when the heating coil is at Speed n-1 for the time step being simulated.
+
+n~Average outlet air temperature
+
+The heating coil's outlet air humidity ratio equals the inlet air humidity ratio since the coil does not change the moisture content of the air. So the average outlet air temperature is calculated based on the inlet air humidity ratio and the average outlet air enthalpy using the psychrometric function PsyTdbFnHW.
+
+n~Full load energy inputs at Speed n-1 and Speed n
+
+\begin{equation}
+HeatingPowe{r_n} = TotCa{p_n}\left( {EI{R_n}} \right)\left( {HeatingCapacityMultiplier} \right)\left( {InputPowerMultiplier} \right)
+\end{equation}
+
+\begin{equation}
+HeatingPowe{r_{n - 1}} = TotCa{p_{n - 1}}\left( {EI{R_{n - 1}}} \right)\left( {HeatingCapacityMultiplier} \right)\left( {InputPowerMultiplier} \right)
+\end{equation}
+
+where,
+
+\emph{InputPowerMultiplier}~~~~~~~ = Frost adjustment factor for heating power calculation (Ref. Coil:Heating:DX:SingleSpeed)
+
+n~Calculate combined energy input
+
+When the input for the field `Apply Part Load Fraction to Speeds Greater than 1' is No (equivalent to a single compressor), the combined energy output is calculated as follows:
+
+\begin{equation}
+HeatingPower = HeatingPowe{r_n}\left( {SpeedRatio} \right) + HeatingPowe{r_{n - 1}}(1.0 - SpeedRatio)
+\end{equation}
+
+When the input for the field 'Apply Part Load Fraction to Speeds Greater than 1' is Yes (equivalent to multiple compressors), the combined energy output is calculated as follows:
+
+\begin{equation}
+HeatingPower = HeatingPowe{r_n}\left( {RTF} \right) + HeatingPowe{r_{n - 1}}(1.0 - RTF)
+\end{equation}
+
+where,
+
+HeatingPower~~~~~~~~~ = Power used in Watt
+
+RTF~~~~~~~~~~~~~~~~~~~~~~~ = Run time fraction (SpeedRatio/Part-load Fraction) at Speed n
+
+n~Calculate defrost power
+
+When the defrost strategy is resistive, the power calculation is the same as Speed 1 operation (Ref. Coil:Heating:DX:SingleSpeed). When the defrost strategy is reverse-cycle, the following calculations are performed:
+
+\begin{equation}
+{Q_{defrost,n}} = 0.01({t_{frac,defrost}})(7.222 - {T_{db,o}})\left( {\frac{{{Q_{total,rated,n}}}}{{1.01667}}} \right)
+\end{equation}
+
+\begin{equation}
+{P_{defrost,n - 1}} = DefrostEIRTempModFac\left( {\frac{{{Q_{total,rated,n - 1}}}}{{1.01667}}} \right)({t_{frac,defrost}})
+\end{equation}
+
+\begin{equation}
+{P_{defrost,n}} = DefrostEIRTempModFac\left( {\frac{{{Q_{total,rated,n}}}}{{1.01667}}} \right)({t_{frac,defrost}})
+\end{equation}
+
+where:
+
+\({Q_{defrost,n}}\) ~~~~ = additional indoor heating load due to reverse-cycle defrost at Speed n (\emph{W})
+
+\({Q_{total,rated,n}}\) ~ = total full-load heating capacity of the coil at rated conditions at Speed n (W)
+
+\({P_{defrost,n - 1}}\) ~~~ = full load defrost power for the simulation time step at Speed n-1 (W)
+
+\({P_{defrost,n}}\) ~~~~~ = full load defrost power for the simulation time step at Speed n (W)
+
+\({Q_{total,rated,n - 1}}\) = capacity of the resistive defrost heating element at Speed n-1 (W)
+
+\({Q_{total,rated,n}}\) = capacity of the resistive defrost heating element at Speed n (W)
+
+DefrostEIRTempModFac~~~~ = defrost energy input ratio (EIR) modifier curve (Ref. Coil:Heating:DX:SingleSpeed).
+
+T\(_{frac,defrost}\)~~~~~~ = ~ fractional defrost time (Ref. Coil:Heating:DX:SingleSpeed)
+
+When the input for the field `Apply Part Load Fraction to Speeds Greater than 1' is No (equivalent to a single compressor), the average defrost power is calculated as follows:
+
+\begin{equation}
+{P_{defrost}} = {P_{defrost,n}}(SpeedRatio) + {P_{defrost,n - 1}}(1.0 - SpeedRatio)
+\end{equation}
+
+When the input for the field 'Apply Part Load Fraction to Speeds Greater than 1' is Yes (equivalent to multiple compressors), the combined defrost energy is calculated as follows:
+
+\begin{equation}
+{P_{defrost}} = {P_{defrost,n}}(RTF) + {P_{defrost,n - 1}}(1.0 - RTF)
+\end{equation}
+
+where,
+
+\({P_{defrost}}\) ~~~~~~~ = average defrost power used in Watt
+
+RTF~~~~~~~~~~~ = Run time fraction (SpeedRatio/Part-load Fraction) at Speed n
+
+n~Crankcase heater
+
+There is no power need at higher speed operation.
+
+\subsubsection{Higher Speed Operation with Single Mode Operation}\label{higher-speed-operation-with-single-mode-operation-1}
+
+This section describes how higher speed operation is simulated with single mode operation. When the required sensible load is less than the full load sensible capacity at Speed n (Speed Number \textgreater{} 1), its performance is almost the same as the performance for the Coil:Heating:DX:SingleSpeed model at different flow rate and capacity with given Speed n. No linear interpolation is performed between two adjacent speeds. The highest speed which does not exceed the sensible load is used for each HVAC timestep. This operation does not apply to the case when the sensible load is above the highest sensible capacity.
+
+\subsubsection{Waste heat calculation}\label{waste-heat-calculation-1-000}
+
+The waste heat generated by this coil object is calculated as:
+
+\begin{equation}
+{Q_{WasteHeat}} = (Fraction)(TempModifier)(HeatingPowe)
+\end{equation}
+
+where
+
+Fraction~~~~~~~~~~~~~~~~~ = rated waste heat fraction of the energy input
+
+TempModifier = waste heat modifier as a function of indoor and outdoor air dry-bulb temperature
+
+\subsubsection{Standard Rating of Multi-Speed DX Heating Coils}\label{standard-rating-of-multi-speed-dx-heating-coils}
+
+For multi-speed direct expansion heating coils, the industry standard ratings of Standard Rating Heating Seasonal Performance Factor (HSPF) are calculated according to NSI/AHRI Standard 210/240 (AHRI 2008). These standard ratings can be calculated using the user-entered information for the Coil:Heating:DX:MultiSpeed object.~ According to Standard 210/240, the Standard Rating HSPF applies to air-to-air unitary heat pumps with rated heating capacities under 19,000 watts (65,000 Btu/h). The Heating Mode Test Conditions for Units Having two-capacity Compressor standard tests H0\(_{1}\), H1\(_{1}\), H2\(_{1}\), H3\(_{1}\), H1\(_{2}\), H2\(_{2}\), and H3\(_{2}\) are also provided in Table~\ref{table:heating-mode-test-conditions-for-units-having-001}. The rated Energy Efficiency Ratio (EER) is not calculated for any DX Heating Coils as this time. The equations required to calculate the net heating capacity and HSPF values are described next.
+
+\subsubsection{Standard Ratings Heating Capacity}\label{standard-ratings-heating-capacity}
+
+\emph{The Standard Rating (Net) Heating Capacity calculation is calculated using the same procedure as the single speed DX heating coils except the capacities are evaluated at the maximum speed only.~ Refer to the standard ratings calculation for Coil:DX:Heating:SingelSpeed for description of the procedure.}
+
+The Rated Supply Fan Power Per Volume Flow Rate is a user-entered value, with a default of 773.3 W/(m\(^{3}\)/s)) if the user leaves this input field blank. The default value is taken from ANSI/ASHRAE Standard 210/240-2008 where it is defined for systems which do not have an Indoor Coil (Evaporator) fan furnished as part of the system. The test conditions in ANSI/AHRI Standard 210/240 vary the external static pressure (i.e., pressure drop associated with ductwork and other devices external to the indoor fan/coil section) seen by the supply air fan based on the standard rating cooling capacity. New input field Rated Supply Fan Power Per Volume Flow Rate for each speed will be added to the IDD.
+
+\subsubsection{Heating seasonal performance factors (HSPF) for Multi-Speed DX Coil}\label{heating-seasonal-performance-factors-hspf-for-multi-speed-dx-coil}
+
+The following section describes the test condition for heating mode tests for Air-Source Heat Pumps, including heating-only heat pumps, and the equations required to calculate the HSPF. The HSPF for multi-speed compressor heat pumps in Btu/W-h is given by:
+
+\begin{equation}
+HSPF{\rm{ = }}\frac{{\sum\limits_{\rm{j}}^{\rm{M}} {\frac{{{n_j}}}{N} \cdot BL\left( {{T_j}} \right)} }}{{\sum\limits_{\rm{j}}^{\rm{M}} {\frac{{{e_h}\left( {{T_j}} \right)}}{N}{\rm{ + }}} \sum\limits_{\rm{j}}^{\rm{M}} {\frac{{RH\left( {{T_j}} \right)}}{N}} }} \cdot {F_{def}}
+\end{equation}
+
+Where,
+
+BL(T\(_{j}\))~~~~~~~~~ = ~~~~~~~~~ the building space conditioning load corresponding to an outdoor temperature of T\(_{j}\); the heating season building load also depends on the generalized climatic region's outdoor design temperature and the design heating requirement, Btu/h.
+
+e\(_{h}\)(T\(_{j}\))/N~~~~~~~ = ~~~~~~~~ the ratio of the electrical energy consumed by the heat pump during periods of the space heating season when the outdoor temperature fell within the range represented by bin temperature T\(_{j}\) to the total number of hours in the heating season (N), W. For heat pumps having a heat comfort controller, this ratio may also include electrical energy used by resistive elements to maintain a minimum air delivery temperature.
+
+RH(T\(_{j}\))/N~~~~~ = ~~~~~~~~~ the ratio of the electrical energy used for resistive space heating during periods when the outdoor temperature fell within the range represented by bin temperature T\(_{j}\) to the total number of hours in the heating season (N),W. Resistive space heating is modeled as being used to meet that portion of the building load that the heat pump does not meet because of insufficient capacity or because the heat pump automatically turns off at the lowest outdoor temperatures.
+
+T\(_{j}\)~~~ = ~~~~~~~~~ the outdoor bin temperature, °C. Outdoor temperatures are ``binned'' such that calculations are only performed based one temperature within the bin. Bins of 2.78°C are used.
+
+n\(_{j}\)/N = ~~~~~~~~~ Fractional bin hours for the heating season; the ratio of the number of hours during the heating season when the outdoor temperature fell within the range represented by bin temperature T\(_{j}\) to the total number of hours in the heating season, dimensionless, given in Table~\ref{table:generalized-climatic-region-information}.
+
+j ~~~ = ~~~~~~~~~ the bin number, dimensionless.
+
+M ~ = ~~~~~~~~~ for each generalized climatic region, the total number of temperature bins, dimensionless. Referring to Table~\ref{table:generalized-climatic-region-information}, M is the highest bin number (j) having a nonzero entry for the fractional bin hours for the generalized climatic region of interest.
+
+\({F_{def}}\) = The demand defrost credit described in section 3.9.2 of AHRI Std. 210/240-2008, dimensionless.~ For simplification, assigned a value of 1 for timed defrost control and a value of 1.03 for demand defrost control.
+
+The building heating load is calculated as follows:
+
+\begin{equation}
+BL\left( {{T_j}} \right){\rm{ = }}\frac{{{\rm{18}}{\rm{.33 - }}{T_j}}}{{{\rm{18}}{\rm{.33 - }}{T_{OD}}}} \cdot C \cdot DHR
+\end{equation}
+
+The minimum and maximum design heating requirements for each generalized climate regions are given by:
+
+\begin{equation}
+DHR_{min} = \left\{  \begin{array}{cl}
+                         8.33 \dot{Q}_h^{k = 2} \frac{18.33-T_{OD}}{33.33} & \text{for regions I, II, III, IV, and VI} \\
+                         8.33 \dot{Q}_h^{k = 2} & \text{for region V}
+                     \end{array}
+            \right.
+\end{equation}
+
+and
+
+\begin{equation}
+DHR_{min} = \left\{  \begin{array}{cl}
+                         2 \cdot 8.33 \dot{Q}_h^{k = 2} \frac{18.33-T_{OD}}{33.33} & \text{for regions I, II, III, IV, and VI} \\
+                         2 \cdot 8.33 \dot{Q}_h^{k = 2} & \text{for region V}
+                     \end{array}
+            \right.
+\end{equation}
+
+Where,
+
+C ~~ = ~~~~~~~~~ 0.77, a correction factor which tends to improve the agreement between calculated and measured building loads dimensionless.
+
+DHR ~~~~~~~~~ = ~~~~~~~~~ the design heating requirement for each generalized climate region, Btu/h.
+
+\(\dot Q_h^{k = 2}(8.33)\) = ~~~~~~~~~ the heating capacity determined from H1\(_{2}\) test, (W)
+
+The heating capacity delivered and electric power input of the heat pump when operating at minimum (low) compressor capacity and outdoor air temperature of \emph{T\(_{j}\)} is given by:
+
+\begin{equation}
+{\rm{\dot Q}}_h^{k = 1}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{) = }}\left\{ 
+    \begin{array}{l}
+      {\rm{\dot Q}}_h^{k = 1}(8.33) + \;\frac{{\left[ {{\rm{\dot Q}}_h^{k = 1}{\rm{(16}}{\rm{.67) - \dot Q}}_h^{k = 1}{\rm{(8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} - 8.33} \right)}}{{\left( {16.67 - 8.33} \right)}}\,{\rm{if}}\,{{\rm{T}}_{\rm{j}}} \ge 4.44{\rm{^\circ C}} \\
+      {\rm{\dot Q}}_h^{k = 1}( - 8.33) + \;\frac{{\left[ {{\rm{\dot Q}}_h^{k = 1}{\rm{(1}}{\rm{.67) - \dot Q}}_h^{k = 1}{\rm{( - 8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} + 8.33} \right)}}{{\left( {1.67 + 8.33} \right)}}\,{\rm{if}}\, - 8.33{\rm{^\circ C}} \le {{\rm{T}}_{\rm{j}}} < 4.44{\rm{^\circ C}} \\
+      {\rm{\dot Q}}_h^{k = 1}( - 8.33) + \;\frac{{\left[ {{\rm{\dot Q}}_h^{k = 1}{\rm{(8}}{\rm{.33) - \dot Q}}_h^{k = 1}{\rm{( - 8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} + 8.33} \right)}}{{\left( {8.33 + 8.33} \right)}}\,{\rm{if }}{{\rm{T}}_{\rm{j}}} <  - 8.33{\rm{^\circ C}}\,
+    \end{array}
+  \right\}
+\end{equation}
+
+\begin{equation}
+{\rm{\dot E}}_h^{k = 1}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{) = }}\left\{
+    \begin{array}{l}
+      {\rm{\dot E}}_h^{k = 1}(8.33) + \;\frac{{\left[ {{\rm{\dot E}}_h^{k = 1}{\rm{(16}}{\rm{.67) - \dot E}}_h^{k = 1}{\rm{(8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} - 8.33} \right)}}{{\left( {16.67 - 8.33} \right)}}\,{\rm{if}}\,{{\rm{T}}_{\rm{j}}} \ge 4.44{\rm{^\circ C}} \\
+      {\rm{\dot E}}_h^{k = 1}( - 8.33) + \;\frac{{\left[ {{\rm{\dot E}}_h^{k = 1}{\rm{(1}}{\rm{.67) - \dot E}}_h^{k = 1}{\rm{( - 8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} + 8.33} \right)}}{{\left( {1.67 + 8.33} \right)}}\,{\rm{if}}\, - 8.33{\rm{^\circ C}} \le {{\rm{T}}_{\rm{j}}} < 4.44{\rm{^\circ C}} \\
+      {\rm{\dot E}}_h^{k = 1}( - 8.33) + \;\frac{{\left[ {{\rm{\dot E}}_h^{k = 1}{\rm{(8}}{\rm{.33) - \dot E}}_h^{k = 1}{\rm{( - 8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} + 8.33} \right)}}{{\left( {8.33 + 8.33} \right)}}\,{\rm{if }}{{\rm{T}}_{\rm{j}}} <  - 8.33{\rm{^\circ C}}\,
+    \end{array}
+  \right\}
+\end{equation}
+
+Where,
+
+\({\rm{\dot Q}}_h^{k = 1}\left( {{\rm{16}}{\rm{.67}}} \right),\,{\rm{and}}\,{\rm{\dot E}}_h^{k = 1}\left( {{\rm{16}}{\rm{.67}}} \right)\) are determined from H0\(_{1}\) test and
+
+\({\rm{\dot Q}}_h^{k = 1}\left( {{\rm{8}}{\rm{.33}}} \right),\,{\rm{and}}\,{\rm{\dot E}}_h^{k = 1}\left( {{\rm{8}}{\rm{.33}}} \right)\) are determined from H1\(_{1}\) test and
+
+\({\rm{\dot Q}}_h^{k = 1}\left( {{\rm{1}}{\rm{.67}}} \right),\,{\rm{and}}\,{\rm{\dot E}}_h^{k = 1}\left( {{\rm{1}}{\rm{.67}}} \right)\) are determined from H2\(_{1}\) test, and
+
+\({\rm{\dot Q}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right),\,{\rm{and}}\,{\rm{\dot E}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right)\) are determined from H3\(_{1}\) test.
+
+An alternative to conducting or evaluating the performance at H2\(_{1}\) test is to approximate the capacity and electric power inputs as follows:
+
+\begin{equation}
+{\rm{\dot Q}}_h^{k = 1}\left( {{\rm{1}}{\rm{.67}}} \right) = 0.9 \cdot \left\{ {{\rm{\dot Q}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right) + 0.6\left[ {{\rm{\dot Q}}_h^{k = 1}\left( {{\rm{8}}{\rm{.33}}} \right) - {\rm{\dot Q}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right)} \right]} \right\}
+\end{equation}
+
+\begin{equation}
+{\rm{\dot E}}_h^{k = 1}\left( {{\rm{1}}{\rm{.67}}} \right) = 0.985 \cdot \left\{ {{\rm{\dot E}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right) + 0.6\left[ {{\rm{\dot E}}_h^{k = 1}\left( {{\rm{8}}{\rm{.33}}} \right) - {\rm{\dot E}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right)} \right]} \right\}
+\end{equation}
+
+The heating capacity delivered and electric power input of the heat pump when operating at maximum (high) compressor speed and outdoor air temperature of \emph{T\(_{j}\)} is given by:
+
+\begin{equation}
+\dot Q_h^{k = 2}({T_j}) = \left\{ \begin{array}{l}\dot Q_h^{k = 2}( - 8.33) + \frac{{\left[ {\dot Q_h^{k = 2}(8.33) - \dot Q_h^{k = 2}( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{8.33 + 8.33}},\quad IF\,{T_j} \ge 7.2^\circ C\,or\,{T_j} \le  - 8.33^\circ C\\\dot Q_h^{k = 2}( - 8.33) + \frac{{\left[ {\dot Q_h^{k = 2}(1.67) - \dot Q_h^{k = 2}( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{1.67 + 8.33}},\quad IF\, - 8.33^\circ C < {T_j} < 7.2^\circ C\end{array} \right.
+\end{equation}
+
+\begin{equation}
+\dot E_h^{k = 2}({T_j}) = \left\{ \begin{array}{l}\dot E_h^{k = 2}( - 8.33) + \frac{{\left[ {\dot E_h^{k = 2}(8.33) - \dot E_h^{k = 2}( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{8.33 + 8.33}},\quad IF\,{T_j} \ge 7.2^\circ C\,or\,{T_j} \le  - 8.33^\circ C\\\dot E_h^{k = 2}( - 8.33) + \frac{{\left[ {\dot E_h^{k = 2}(1.67) - \dot E_h^{k = 2}( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{1.67 + 8.33}},\quad IF\, - 8.33^\circ C < {T_j} < 7.2^\circ C\end{array} \right.
+\end{equation}
+
+Where,
+
+\(\dot Q_h^{k = 2}\left( {{\rm{8}}{\rm{.33}}} \right),\,{\rm{and}}\,\dot E_h^{k = 2}\left( {{\rm{8}}{\rm{.33}}} \right)\) are determined from H1\(_{2}\) test
+
+\(\dot Q_h^{k = 2}\left( {{\rm{1}}{\rm{.67}}} \right),\,{\rm{and}}\,\dot E_h^{k = 2}\left( {{\rm{1}}{\rm{.67}}} \right)\) are determined from H2\(_{2}\) test
+
+\(\dot Q_h^{k = 2}\left( {{\rm{ - 8}}{\rm{.33}}} \right),\,{\rm{and}}\,\dot E_h^{k = 2}\left( {{\rm{ - 8}}{\rm{.33}}} \right)\) are determined from H3\(_{2}\) test
+
+The electric energy used by the heat pumps differs depending up on whether the heat pump would operate at low (minimum) capacity, cycle between successive lower and higher speed capacities, or operate at high speed capacity in responding to the building load.~ The procedure for each operation cases is described next.
+
+\emph{Case 1}:~ The steady state heating capacity when the unit is operating at minimum or low capacity, i.e., when the building heating load is less or equal to the low capacity:
+
+\begin{equation}
+\dot Q_c^{k = 1}\left( {{T_j}} \right) \ge BL\left( {{T_j}} \right)
+\end{equation}
+
+\begin{equation}
+\frac{{{{\rm{e}}_h}\left( {{{\rm{T}}_{\rm{j}}}} \right)}}{{\rm{N}}}{\rm{ = }}\frac{{{{\rm{X}}^{k = 1}}\left( {{{\rm{T}}_{\rm{j}}}} \right) \cdot {\rm{\dot E}}_h^{k = 1}\left( {{{\rm{T}}_{\rm{j}}}} \right) \cdot {\rm{\delta }}\left( {{{\rm{T}}_{\rm{j}}}} \right)}}{{PL{F_j}}} \cdot \frac{{{{\rm{n}}_{\rm{j}}}}}{{\rm{N}}}
+\end{equation}
+
+\begin{equation}
+\frac{{RH\left( {{{\rm{T}}_{\rm{j}}}} \right)}}{{\rm{N}}}{\rm{ = }}BL\left( {{{\rm{T}}_{\rm{j}}}} \right) \cdot \left[ {{\rm{1 - }}{{\rm{\delta }}^\prime}\left( {{{\rm{T}}_{\rm{j}}}} \right)} \right] \cdot \frac{{{{\rm{n}}_{\rm{j}}}}}{{\rm{N}}}
+\end{equation}
+
+\begin{equation}
+{{\rm{X}}^{k = 1}}\left( {{{\rm{T}}_{\rm{j}}}} \right){\rm{ = MIN}}\left\{ \begin{array}{l}BL\left( {{{\rm{T}}_{\rm{j}}}} \right){\rm{/\dot Q}}_h^{k = 1}\left( {{{\rm{T}}_{\rm{j}}}} \right)\\1.0\end{array} \right\}
+\end{equation}
+
+\begin{equation}
+{\delta ^\prime}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{) = }}\left\{ \begin{array}{l}0,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{off}}}}\,\\1/2,\quad {\rm{if}}\,{{\rm{T}}_{{\rm{off}}}} < {{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{on}}}}\\1,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, > \,{{\rm{T}}_{{\rm{on}}}}\end{array} \right\}
+\end{equation}
+
+\begin{equation}
+PL{F_{\rm{j}}}{\rm{ = 1 - }}C_D^h \cdot \left[ {{\rm{1 - }}{{\rm{X}}^{k = 1}}{\rm{(}}{T_j}{\rm{)}}} \right]
+\end{equation}
+
+\begin{equation}
+C_D^h{\rm{ = MIN}}\left\{ \begin{array}{l}{\rm{C}}_{\rm{D}}^{\rm{h}},\,{\rm{calculated}}\,{\rm{using}}\,{\rm{Equation}}\,{\rm{24}}\\0.25\end{array} \right\}
+\end{equation}
+
+\emph{Case 2}:~ The unit cycles between the low (minimum) and high (maximum) compressor capacity to meet the building heating load at outdoor air temperature \emph{T\(_{j}\)}.~ That is, the heating building load is between the unit low and high compressor capacities:
+
+\begin{equation}
+\dot Q_h^{k = 1}({T_j}) < BL({T_j}) < \dot Q_h^{k = 2}({T_j})
+\end{equation}
+
+\begin{equation}
+\frac{{{e_c}({T_j})}}{N} = \left[ {{X^{k = 1}}({T_j}) \cdot \dot E_h^{k = 1}({T_j}) + {X^{k = 2}}({T_j}) \cdot \dot E_h^{k = 2}({T_j})} \right] \cdot {\delta ^\prime}({T_j}) \cdot \frac{{{n_j}}}{N}
+\end{equation}
+
+\begin{equation}
+\frac{{RH\left( {{{\rm{T}}_{\rm{j}}}} \right)}}{{\rm{N}}}{\rm{ = BL}}\left( {{{\rm{T}}_{\rm{j}}}} \right) \cdot \left[ {{\rm{1 - }}{{\rm{\delta }}^\prime}\left( {{{\rm{T}}_{\rm{j}}}} \right)} \right] \cdot \frac{{{n_j}}}{N}
+\end{equation}
+
+\begin{equation}
+{\delta ^\prime}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{) = }}\left\{ \begin{array}{l}0,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{off}}}}\,\\ {\textstyle{1 \over 2}},\quad {\rm{if}}\,{{\rm{T}}_{{\rm{off}}}} < {{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{on}}}}\\ 1,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, > \,{{\rm{T}}_{{\rm{on}}}}\end{array} \right\}
+\end{equation}
+
+\begin{equation}
+{X^{k = 1}}({T_j}) = \frac{{\dot Q_h^{k = 2}({T_j}) - BL({T_j})}}{{\dot Q_h^{k = 2}({T_j}) - \dot Q_h^{k = 1}({T_j})}}
+\end{equation}
+
+\begin{equation}
+{X^{k = 2}}({T_j}) = 1 - {X^{k = 1}}({T_j})
+\end{equation}
+
+\emph{Case 3}:~ The steady-state heating capacity when the unit is operating continuously at high or maximum compressor capacity at outdoor air temperature \emph{T\(_{j}\)}. The building heating load is greater than the available capacity at maximum or high compressor capacity:
+
+\begin{equation}
+BL\left( {{T_j}} \right) \ge \dot Q_c^{k = 2}\left( {{T_j}} \right)
+\end{equation}
+
+For units when operating continuously at maximum compressor speed (k = 2) speed at temperature \emph{T\(_{j}\)}, the delivered heating capacity and electric power inputs are calculated as follows:
+
+\begin{equation}
+\frac{{{e_c}({T_j})}}{N} = \left[ {\dot E_h^{k = 2}({T_j}) \cdot {\delta ^``}({T_j})} \right] \cdot \frac{{{n_j}}}{N}
+\end{equation}
+
+\begin{equation}
+\frac{{RH\left( {{T_j}} \right)}}{N}{\rm{ = }}\left\{ {BL\left( {{{\rm{T}}_{\rm{j}}}} \right) - \left[ {{\rm{\dot Q}}_h^{k = 2}\left( {{{\rm{T}}_{\rm{j}}}} \right) \cdot {{\rm{\delta }}^``}\left( {{{\rm{T}}_{\rm{j}}}} \right)} \right]} \right\} \cdot \frac{{{n_j}}}{N}
+\end{equation}
+
+\begin{equation}
+{\delta ^``}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{) = }}\left\{ \begin{array}{l}0,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{off}}}}\,{\rm{or}}\,\frac{{{\rm{\dot Q}}_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}}{{\dot E_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}}\, < \,1\\ {\textstyle{1 \over 2}},\quad {\rm{if}}\,{{\rm{T}}_{{\rm{off}}}} < {{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{on}}}}\,{\rm{and}}\,\frac{{{\rm{\dot Q}}_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}}{{\dot E_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}} \ge \,1\;\\1,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, > \,{{\rm{T}}_{{\rm{on}}}}\,{\rm{and}}\,\frac{{{\rm{\dot Q}}_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}}{{\dot E_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}} \ge \,1\;\end{array} \right\}
+\end{equation}
+
+X(T\(_{j}\))~~~~~~~~~~~ = ~~~~~~~~~ the heating mode load factor for temperature bin j, (-)
+
+\({{\rm{\dot Q}}_{\rm{h}}}\left( {{{\rm{T}}_{\rm{j}}}} \right)\) ~~~~ = ~~~~~~~~~ space heating capacity of the heat pump when operating at outdoor temperature T\(_{j}\), W
+
+\({{\rm{\dot E}}_{\rm{h}}}\left( {{{\rm{T}}_{\rm{j}}}} \right)\) ~~~~~ = ~~~~~~~~~ electrical power consumption of the heat pump when operating at outdoor temperature T\(_{j}\), W
+
+\({\rm{\delta }}\left( {{{\rm{T}}_{\rm{j}}}} \right)\) ~~~~~~~ = ~~~~~~~~~ the heat pump low temperature cut-off factor, (-)
+
+T\(_{off}\)~ = ~~~~~~~~ the outdoor temperature when the compressor is automatically shut off, °C. (If no such temperature exists, Tj is always greater than T\(_{off}\) and T\(_{on}\)).
+
+T\(_{on}\)~ = ~~~~~~~~ the outdoor temperature when the compressor is automatically turned back on, if applicable, following an automatic shut-off, °C.
+
+% table 62
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\caption{Heating Mode Test Conditions for Units Having Two-Capacity Compressor \label{table:heating-mode-test-conditions-for-units-having-001}} \tabularnewline
+\toprule 
+Test & \multicolumn{2}{l}{Air Entering Indoor Unit} & \multicolumn{2}{l}{Air Entering Outdoor Unit} & Compressor & Heating Air \tabularnewline
+Description & Temperature &  & Temperature &  & Speed & Volume Flow Rate \tabularnewline
+\midrule
+& Dry Bulb C (F) & Wet Bulb C (F) & Dry Bulb C (F) & Wet Bulb C (F) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Heating Mode Test Conditions for Units Having Two-Capacity Compressor} \tabularnewline
+\toprule
+Test & \multicolumn{2}{l}{Air Entering Indoor Unit} & \multicolumn{2}{l}{Air Entering Outdoor Unit} & Compressor & Heating Air \tabularnewline
+Description & Temperature &  & Temperature &  & Speed & Volume Flow Rate \tabularnewline
+\midrule
+& Dry Bulb C (F) & Wet Bulb C (F) & Dry Bulb C (F) & Wet Bulb C (F) \tabularnewline
+\midrule
+\endhead
+
+H01 Test (required,steady) & 21.1 (70) & 15.6 (60) (max) & 16.7 (62) & 18.3 (56.5) & Low & Heating Minimum (1) \tabularnewline
+H12 Test (required,steady) & 21.1 (70) & 15.6 (60) (max) & 8.33 (47) & 6.11 (43) & High & Heating Full-Load (2) \tabularnewline
+H1C2 Test (required, cyclic) & 21.1 (70) & 15.6 (60) (max) & 8.33 (47) & 6.11 (43) & High &  \tabularnewline
+H11 Test (required,steady) & 21.1 (70) & 15.6 (60) (max) & 8.33 (47) & 6.11 (43) & Low & Heating Minimum (1) \tabularnewline
+H1C1 Test (required, cyclic) & 21.1 (70) & 15.6 (60) (max) & 8.33 (47) & 6.11 (43) & Low &  \tabularnewline
+H22 Test (required) & 21.1 (70) & 15.6 (60) (max) & 1.67 (35) & 0.56 (33) & High & Heating Full-Load \tabularnewline
+H21 Test (required) & 21.1 (70) & 15.6 (60) (max) & 1.67 (35) & 0.56 (33) & Low & Heating Minimum \tabularnewline
+H32 Test (required,steady) & 21.1 (70) & 15.6 (60) (max) & -8.33 (17) & -9.44 (15) & High & Heating Full-Load \tabularnewline
+H31 Test (required,steady) & 21.1 (70) & 15.6 (60) (max) & -8.33 (17) & -9.44 (15) & Low & Heating Minimum \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{References:}\label{references-6-000}
+
+AHRI 2008. ANSI/AHRI Standard 210/240: 2008 Standard for Performance Rating of Unitary Air-Conditioning \& Air-Source Heat Pump Equipment.~ Arlington, VA:~ Air-Conditioning, Heating, and Refrigeration Institute.
+
+See the references for the single speed DX heating coil earlier in this document.
+
+\subsection{Variable Speed DX Heating Coil}\label{variable-speed-dx-heating-coil}
+
+\subsubsection{Overview}\label{overview-8-000}
+
+The latest technology for commercial air conditioners and air-to-air heat pumps can utilize a variable speed compressor with a variable speed indoor blower and outdoor fan. The indoor and outdoor air flow rates are usually a function of the compressor speed. Refrigerant mass flow rate is a function of compressor speed as well as outdoor heat exchanger entering air temperature and indoor dry bulb or wet bulb. The control system adjusts the equipment capacity based on zone temperature measurements relative to the thermostat set point. The control logic determines what compressor speed is required to control to the zone temperature requirement in response to increased or decreased capacity (heating or cooling load). The compressor, fan and blower speeds are not discrete values and can be considered to vary infinitesimally between the minimum and maximum compressor speed. At the minimum compressor speed (which is different for heating and cooling), for a continuous fan, the supply airflow is fixed and the unit will have to cycle for reduced part loads below this point. For a cycling fan, the fan will cycle with the compressor.
+
+Similar to variable-speed water source heat pump, we expand the number of speed levels and the corresponding curve sets up to ten. The number of speed levels is selectable by the user. The user can provide speed levels at any number from 1 to 10. In the case that the given speed levels are above 1, the model would do linear interpolation between neighboring speeds. The more curves, the more accurate. Furthermore, using linear interpolation and inputting air flow rates at individual speed levels facilitates arbitrary relationships of flow rate as a function of the compressor speed level.
+
+The Coil:Heating:DX:VariableSpeed object will simulate the performance of a DX heating coil used in combination with a variable-speed air-to-air heat pump. It will fit into the parent objects of AirLoopHVAC:UnitaryHeatPump:AirToAir and
+
+ZoneHVAC:PackagedTerminalHeatPump, etc.
+
+The rated conditions for obtaining the capacities and COPs~ are at indoor dry-bulb temperature of 21.1 ËšC (70 ËšF) and the source side entering air temperature of 8.3 ËšC (47 ËšF). Some equations are provided below to help explain the function of the various performance curves and data fields.
+
+\subsubsection{Model Description}\label{model-description-5}
+
+The Coil:Heating:DX:VariableSpeed object is modeled similar to \\ Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit. Of course, rather than referencing a water source evaporator, the new coil object references an air source and has defrosting operation. The evaporator entering air temperature is used in~ lieu of the entering~ water temperature.
+
+It shall be noted for the capacity and flow rate inputs, two fields are autosizable, which are Rated Heating Capacity at the Selected Nominal Speed Level and the Rated Volumetric Air Flow Rate at the Selected Nominal Speed Level. They are used to scale the performances of a specific unit and correlate with the actual loop flow. Except these two fields, all other capacity and flow rate inputs at individual speed levels should be directly obtained from Reference Unit catalog data, specific to an actual unit.
+
+The Rated Heating Capacity at Selected Nominal Speed Level contains the rated capacity to match the building heating load at the design day.~ The rated heating capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
+
+\begin{equation}
+{\rm{CapacityScaleFactor}} = \frac{{{\rm{RatedTotalHeatingCapacity}}}}{{{\rm{ReferenceUnitTotalHeatingCapacity}}@{\rm{NominalSpeedLevel}}}}
+\end{equation}
+
+And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below:
+
+RatedTotalHeatingCapacity @ SpeedLevel (x) = CapacityScaleFactor times ReferenceUnitTotalHeatingCapacity @ SpeedLevel (x)
+
+The Rated Volumetric Air Flow Rate is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects, as follows:
+
+\begin{equation}
+{\rm{AirFlowScaleFactor}} = \frac{{{\rm{RatedVolumetricAirFlowRate}}}}{{{\rm{ReferenceUnitVolAirFlowRate}}@{\rm{NominalSpeedLevel}} \times {\rm{CapacityScaleFactor}}}}
+\end{equation}
+
+And the loop volumetric air flow rates at various speed levels in the parent objects are calculated as below:
+
+LoopVolumetricAirFlowRate @ SpeedLevel (x) = AirFlowScaleFactor times ReferenceUnitVolAirFlowRate @ SpeedLevel (x) times CapacityScaleFactor
+
+If the volumetric air flow rate at one speed level is higher than the flow rate allowed by the fan in the parent object, the flow rate will be set back to the fan flow rate.
+
+If \({\rm{AirFlowScaleFactor}}\) ~equals unity, the loop air flow rate becomes the design flow rate of the Reference Unit (after scaled by the rated heating capacity). The Rated Volumetric Air Flow Rate is introduced here to correlate with the actual flow rate in the air loop, in case that it differs from the design specification. Certainly, it is recommended that the Rated Volumetric Air Flow Rate is selected in the way that \({\rm{AirFlowScaleFactor}}\) ~is unity, so as to get more accurate results from the performance curves.
+
+\subsubsection{Performance curves:}\label{performance-curves}
+
+This object includes 4 curve objects at each individual speed level.
+
+1)~ Total heating capacity modifier curve (function of temperature).
+
+2)~ Total heating capacity modifier curve (function of air flow fraction).
+
+3)~ Energy input ratio (EIR) modifier curve (function of temperature).
+
+4)~ Energy input ratio (EIR) modifier curve (function of air flow fraction).
+
+The flow fraction modifier curves are used as a placeholder, to account for off-design flow rates if needed. If the manufacturer doesn't provide off-design performances, we can simply use a default modification multiplier of 1.0.
+
+At the lowest speed, there will be one additional performance curve to account for the part-load condition, i.e.
+
+5)~ Part load fraction correlation (function of part load ratio).
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\tightlist
+\item
+  Total heating capacity modifier curve (function of temperature)
+\end{enumerate}
+
+The total heating capacity modifier as a function of temperature curve (CAP-FT) is a biquadratic curve with two independent variables: dry-bulb temperature of the air entering the heating coil and the air DB temperature entering the evaporator coil. The output of this curve is multiplied by the rated total heating capacity at the speed, to give the total heating capacity at the specific entering air temperatures at which the ASHP unit is operating (i.e., at temperatures different from the rating point temperatures).
+
+\begin{equation}
+{\rm{TotCapTempModFac}} = {\rm{a}} + {\rm{b*D}}{{\rm{B}}_{\rm{i}}} + {\rm{c*DB}}_{\rm{i}}^2 + {\rm{d*D}}{{\rm{B}}_{\rm{o}}} + {\rm{e*D}}{{\rm{B}}_{\rm{o}}}^2 + {\rm{f*D}}{{\rm{B}}_{\rm{i}}}{\rm{*D}}{{\rm{B}}_{\rm{o}}}
+\end{equation}
+
+where
+
+DB\(_{i}\) = dry-bulb temperature of the air entering the heating coil, °C
+
+DB\(_{o}\) = dry-bulb temperature of the air entering the outdoor coil, °C
+
+a-f = regression curve-fit coefficients
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Total heating capacity modifier curve (function of air flow fraction)
+\end{enumerate}
+
+\begin{equation}
+{\rm{TotCapAirFlowModFac}} = {\rm{a}} + {\rm{b*f}}{{\rm{f}}_{\rm{a}}} + {\rm{c*ff}}_{\rm{a}}^2 + {\rm{d*ff}}_{\rm{a}}^3
+\end{equation}
+
+where
+
+ff\(_{a}\) = actual air mass flow rate/design air mass flow rate, at one speed level;
+
+DesignAirMassFlowRate @ SpeedLevel (x) = ReferenceUnitAirMassFlowRate @ SpeedLevel (x) times CapacityScaleFactor
+
+a-d = regression curve-fit coefficients, if no data available for the correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Energy input ratio (EIR) modifier curve (function of temperature)
+\end{enumerate}
+
+The energy input ratio modifier curve as a function of temperature (EIR-FT) is a biquadratic curve with two independent variables DB\(_{i}\)~ and DB\(_{o}\). The output of this curve is multiplied by the rated EIR at the speed (inverse of the rated COP), to give the EIR at the specific entering air temperatures at which the ASHP coil unit is operating (i.e., at temperatures different from the rating point temperatures).
+
+\begin{equation}
+{\rm{EIRTempModFac}} = {\rm{a}} + {\rm{b*D}}{{\rm{B}}_{\rm{i}}} + {\rm{c*DB}}_{\rm{i}}^2 + {\rm{d*D}}{{\rm{B}}_{\rm{o}}} + {\rm{e*D}}{{\rm{B}}_{\rm{o}}}^2 + {\rm{f*D}}{{\rm{B}}_{\rm{i}}}{\rm{*D}}{{\rm{B}}_{\rm{o}}}
+\end{equation}
+
+where
+
+a-f = regression curve fit coefficients.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Energy input ratio (EIR) modifier curve (function of air flow fraction)
+\end{enumerate}
+
+\begin{equation}
+{\rm{EIRAirFlowModFac}} = {\rm{a}} + {\rm{b*f}}{{\rm{f}}_{\rm{a}}} + {\rm{c*ff}}_{\rm{a}}^2 + {\rm{d*ff}}_{\rm{a}}^3
+\end{equation}
+
+where
+
+a-d = regression curve-fit coefficients, if no data available for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{4}
+\tightlist
+\item
+  Part load fraction correlation (function of part load ratio)
+\end{enumerate}
+
+This field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, heating load/steady-state heating capacity for Speed 1),
+
+\begin{equation}
+{\rm{PartLoadFrac}} = {\rm{a}} + {\rm{b*PLR}} + {\rm{c*PL}}{{\rm{R}}^2} + {\rm{d*PL}}{{\rm{R}}^3}
+\end{equation}
+
+And
+
+RTF = (PLR/PartLoadFrac) = runtime fraction of the heating coil.
+
+The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor runs continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, the runtime fraction of the coil is limited to 1.0. A typical part load fraction correlation would be:
+
+\begin{equation}
+{\rm{PLF}} = 0.85 + 0.15 \times {\rm{PLR}}
+\end{equation}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{equation}
+{\rm{PLF}} = 0.85 + 0.0 \times {\rm{PLR}}
+\end{equation}
+
+\subsubsection{Lowest Speed Operation:}\label{lowest-speed-operation}
+
+The lowest speed operation of the variable-speed DX heating coil is similar to the single speed DX heating coil. The total (gross) heating capacity of the variable-speed DX coil is calculated as follows:
+
+\begin{equation}
+  \begin{array}{rl}
+    Q_{total,1} &= \rm{RatedTotalHeatingCapacity @ SpeedLevel 1} \\
+                &* \rm{TotCapTemModFac}_1 \rm{* TotCapAirFlowModFac}_1
+  \end{array}
+\end{equation}
+
+And the EIR is calculated as:
+
+\begin{equation}
+{\rm{EI}}{{\rm{R}}_1} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}(1)}}{\rm{*EIRTempModFa}}{{\rm{c}}_1}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_1}
+\end{equation}
+
+And the power consumption including the compressor, outdoor fan and accessories (not including indoor fan power) is,
+
+\begin{equation}
+{\rm{Powe}}{{\rm{r}}_1} = {{\rm{Q}}_{{\rm{total}},1}}{\rm{*EI}}{{\rm{R}}_1}{\rm{*RTF}}
+\end{equation}
+
+The fraction of the actual air mass flow to the design air mass flow rate is calculated:
+
+\begin{equation}
+{\rm{f}}{{\rm{f}}_{{\rm{a}},1}} = \frac{{{\rm{actualairmassflowrate}}}}{{({\rm{ReferenceUnitAirMassFlowRate}}@{\rm{SpeedLevel}}(1) \times {\rm{CapacityScaleFactor}})}}{\rm{}}
+\end{equation}
+
+\subsubsection{Higher Speed Operation:}\label{higher-speed-operation-1-000}
+
+At the speed level between the lowest and the highest, there is no part-load loss. A parameter of speed ratio (SpeedRatio) is used to define the capacity partition between Speed x-1 and Speed x.
+
+The design air flow rate at the speed ratio are given as following:
+
+\begin{equation}
+  \begin{array}{rl}
+    \rm{DesignAirFlowRateSpeedRatio} &= \rm{ReferenceUnitAirMassFlowRate @ SpeedLevel} \PB{x-1} \\
+                                     &* \rm{CapacityScaleFactor} * \PB{1 - SpeedRatio} \\
+                                     &+ \rm{ReferenceUnitAirMassFlowRate @ SpeedLevel} \PB{x} \\
+                                     &* \rm{CapacityScaleFactor*SpeedRatio}
+  \end{array}
+\end{equation}
+
+And the fractions of air flow is given:
+
+\({\rm{f}}{{\rm{f}}_{{\rm{a}},{\rm{x}} - 1}}\) = \({\rm{f}}{{\rm{f}}_{{\rm{a}},{\rm{x}}}}\) = actual air mass flow rate/DesignAirFlowRateSpeedRatio
+
+The total heating capacities and EIRs at Speed x-1 and Speed x are given:
+
+\begin{equation}
+\begin{split}
+{{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}} = {\rm{RatedTotalHeatingCapacity}}@{\rm{SpeedLevel}}\left( {{\rm{x}} - 1} \right) \\
+{\rm{*TotCapTempModFa}}{{\rm{c}}_{{\rm{x}} - 1}} {\rm{*TotCapAirFlowModFa}}{{\rm{c}}_{{\rm{x}} - 1}}
+\end{split}
+\end{equation}
+
+\begin{equation}
+\begin{split}
+{{\rm{Q}}_{{\rm{total}},{\rm{x}}}} = {\rm{RatedTotalHeatingCapacity}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) \\
+{\rm{*TotCapTempModFa}}{{\rm{c}}_{\rm{x}}} {\rm{*TotCapAirFlowModFa}}{{\rm{c}}_{\rm{x}}}
+\end{split}
+\end{equation}
+
+\begin{equation}
+{\rm{EI}}{{\rm{R}}_{{\rm{x}} - 1}} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}({\rm{x}} - 1)}}{\rm{EIRTempModFa}}{{\rm{c}}_{{\rm{x}} - 1}}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_{{\rm{x}} - 1}}
+\end{equation}
+
+\begin{equation}
+{\rm{EI}}{{\rm{R}}_{\rm{x}}} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}({\rm{x}})}}{\rm{EIRTempModFa}}{{\rm{c}}_{\rm{x}}}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_{\rm{x}}}
+\end{equation}
+
+The total heating capacity at the corresponding speed ratio is:
+
+\begin{equation}
+{{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}} = \left( {1.0 - {\rm{SpeedRatio}}} \right){\rm{*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}} + {\rm{SpeedRatio*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}}}}
+\end{equation}
+
+And the power consumption is
+
+\begin{equation}
+{\rm{Powe}}{{\rm{r}}_{{\rm{SpeedRatio}}}} = \left( {1.0 - {\rm{SpeedRatio}}} \right){\rm{*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}}{\rm{*EI}}{{\rm{R}}_{{\rm{x}} - 1}} + {\rm{SpeedRatio*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}}}}{\rm{*EI}}{{\rm{R}}_{\rm{x}}}
+\end{equation}
+
+The total amount of heat absorbed by the outdoor evaporator is calculated as:
+
+\begin{equation}
+{{\rm{Q}}_{{\rm{evap}},{\rm{SpeedRatio}}}} = {{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}} - {\rm{Powe}}{{\rm{r}}_{{\rm{SpeedRatio}}}}
+\end{equation}
+
+At last,
+
+\begin{equation}
+{{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}} = {\rm{HeatingLoad}}
+\end{equation}
+
+If the speed reaches the highest level, the speed ratio becomes 1.0, and Speed x represents the highest speed.
+
+\subsubsection{Defrost Operation:}\label{defrost-operation-1}
+
+The defrost operation of a variable-speed DX heating coil is treated the same as the single-speed DX heating coil, except using the total heating capacity at the max speed level to replace the rated heating capacity of the single-speed DX coil, when a reverse-cycle defrost strategy is specified.
+
+We keep the defrost energy input ratio (EIR) modifier curve (function of temperature) as the single speed DX heating coil. It is a biquadratic curve with two independent variables: outdoor air dry-bulb temperature and the heating coil entering air wet-bulb temperature. The output of this curve is multiplied by the heating coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the coil is operating. This curve is only required when a reverse-cycle defrost strategy is specified.
+
+\begin{equation}
+{\rm{DefrostEIRTempModFac}} = {\rm{a}} + {\rm{b*W}}{{\rm{B}}_{\rm{i}}} + {\rm{c*WB}}_{\rm{i}}^2 + {\rm{d*D}}{{\rm{B}}_{\rm{o}}} + {\rm{e*D}}{{\rm{B}}_{\rm{o}}}^2 + {\rm{f*W}}{{\rm{B}}_{\rm{i}}}{\rm{*D}}{{\rm{B}}_{\rm{o}}}
+\end{equation}
+
+where
+
+WB\(_{i}\) = wet-bulb temperature of the air entering the indoor coil, °C
+
+DB\(_{o}\) = dry-bulb temperature of the air entering the outdoor coil, °C
+
+a-f = regression curve-fit coefficients
+
+\subsubsection{Crankcase Heater Operation:}\label{crankcase-heater-operation}
+
+It is the same as the single-speed DX heating coil.
+
+\subsection{Desuperheater-Recovery-Based Air Heating Coil}\label{desuperheater-recovery-based-air-heating-coil}
+
+\subsubsection{Overview}\label{overview-9}
+
+The input object Coil:Heating:Desuperheater provides a model that simulates the thermal performance of a refrigerant-to-air heating coil and the parasitic electric consumption of its control valves or other auxiliary devices. The model assumes that the heating energy provided by this coil is reclaimed from the superheated refrigerant gas leaving a compressor and does not impact the performance of the compressor. The objects from which this coil can obtain its heating energy are:
+
+Coil:Cooling:DX:SingleSpeed
+
+Coil:Cooling:DX:TwoSpeed
+
+Coil:Cooling:DX:TwoStageWithHumidityControlMode
+
+Refrigeration:CompressorRack
+
+Refrigeration:Condenser* (multiple objects)
+
+The heat reclaim recovery efficiency (specified by the user) defines the amount of heat available for use by this coil. Approximately 25-30\% of the energy rejected by typical refrigeration system condensers is to reduce the superheated refrigerant vapor temperature to the condensing temperature. Recovery efficiencies higher than 30\% may cause the refrigerant gas to condense which in turn impacts the performance of the refrigeration compressor rack. For this reason, the maximum heat reclaim recovery efficiency for this coil for all sources except the Refrigeration:Condenser:(Air, Water, or Evap)Cooled is 30\%.For these refrigeration condensers, the amount of waste energy available in the superheat region is explicitly calculated, so for these condensers the maximum heat recovery efficiency is 90\% of this superheat energy. Also, for these refrigeration condensers, an estimate of the temperature of the reclaimed heat source is made and compared to the inlet air temperature for the coil. If the reclaimed heat source is too cool, the amount of available reclaim energy is set to zero.
+
+NOTE: When the heating source is a refrigeration compressor rack, the heat rejection location in the Refrigeration:CompressorRack object must be ``Outdoors''. If the compressor rack heat rejection location is ``Zone'', the total amount of heat rejection available for reclaim (e.g., by this desuperheater heating coil) is set to zero by the compressor rack object and the simulation proceeds.
+
+The sources for the waste heat can also be used to supply other coils.~ To avoid double-counting this waste heat, the amount available is corrected to reflect these other uses. For the three DX Cooling Coil sources, this correction is made within the same time step loop.~ For the two refrigeration system sources, the correction is made using the value from the previous time step.
+
+The desuperheater heating coil can be used in air loop simulations for various air heating applications. For example, it can be used as an air reheat coil for high humidity control in the compound objects AirLoopHVAC:Unitary:Furnace:HeatCool and AirLoopHVAC:UnitaryHeatCool (see High Humidity Control With HeatCool Configuration). For this application, the desuperheater coil is controlled based on the calculated heating load to maintain the zone temperature and humidity setpoints (load-based control). The source of reclaimed heat could be the direct expansion (DX) cooling coil itself (Coil:Cooling:DX:SingleSpeed) or a refrigerated case compressor rack (Refrigeration:CompressorRack).
+
+The desuperheater heating coil can also be used with cooling/heating systems that maintain specific air loop (deck) temperatures. For example, Figure~\ref{fig:desuperheater-heating-coil-used-as-a-reheat} shows a schematic diagram of the desuperheater heating coil used in conjunction with the CoilSystem:Cooling:DX object. The desuperheater heating coil must be placed downstream of the DX cooling coil when reclaiming heat from that cooling coil's compressor(s). Desuperheating heating coil placement is unrestricted when reclaiming heat from a refrigeration compressor rack or refrigeration condenser. The configuration in Figure~\ref{fig:desuperheater-heating-coil-used-as-a-reheat} shows the heating coil being controlled via a temperature-based strategy. In this example, the DX cooling coil could be used to the maintain its discharge air temperature at 11°C for zone dehumidification. The desuperheater heating coil could then raise the air dry-bulb temperature to 16°C providing a dry supply air stream at a temperature which does not require much additional heating by terminal units to meet the zone temperature setpoint.
+
+\begin{figure}[hbtp] % fig 171
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4016.png}
+\caption{Desuperheater Heating Coil Used as a Reheat Coil with CoilSystem:Cooling:DX \protect \label{fig:desuperheater-heating-coil-used-as-a-reheat}}
+\end{figure}
+
+Since the heating provided by the desuperheater coil is based on available waste heat from another system, the selection of fan control for the air loop equipment is essential for proper modeling. When the coil's heating source is a direct expansion cooling coil (Coil:Cooling:DX:SingleSpeed, Coil:Cooling:DX:TwoSpeed, or Coil:Cooling:DX:TwoStageWithHumidityControlMode), the air loop's fan control mode may be auto fan (cycling fan cycling coil), constant fan, or variable volume since the desuperheater heating coil cycles on/off with the DX cooling coil. When the heating source is a compressor rack or condenser for refrigerated cases, the supply air fan control should be either variable volume or constant fan since the desuperheater heating coil will typically be available the entire simulation time step.
+
+NOTE: Use of the desuperheater heating coil in variable air volume systems should be done with caution since the model assumption of a fixed heat reclaim recovery efficiency may not be valid if the air flow rate over the coil varies significantly.
+
+The following sections describe the calculations used for both the load-based and temperature-based strategies that can control the desuperheater heating coil.
+
+\subsubsection{Model Inputs}\label{model-inputs-4}
+
+A minimum of seven inputs must be defined for the desuperheater heating coil. The user must input the coil's name, an availability schedule name, and the heat reclaim recovery efficiency (default of 25\%, with a range of 0\% to 30\% except for detailed refrigeration condensers which have a default of 80\%, with a range of 0\% to 90\%). The next two inputs are the heating coil's inlet and outlet air node names. The user must also enter the desuperheater heat source type and name which are validated when the model inputs are read into the program.
+
+The final two fields are optional. The first of these is the coil temperature setpoint node name. This field is used when the desuperheater heating coil is controlled based on an air loop temperature and a setpoint manager (Ref. SetpointManager:*) is used to place a temperature setpoint on this air node. The latter of these optional fields is the parasitic electric load. This field allows the user to define the electric energy use of parasitic equipment associated with the desuperheater heating coil (e.g.~control valves).
+
+\subsubsection{Model Description}\label{model-description-6}
+
+The model calculates the thermal performance of the heating coil based on the control strategy used. When a temperature setpoint node name is not entered, the control type is assumed to be load-based operation. This method should be used when this coil is specified as the air reheat coil for high humidity control with the compound object AirLoopHVAC:Unitary:Furnace:HeatCool or AirLoopHVAC:UnitaryHeatCool. If the temperature setpoint node name is entered, the control type is temperature-based operation. This method is used when the heating coil is controlled to maintain a dry-bulb temperature setpoint in an air loop.
+
+\subsubsection{Load-Based Operation}\label{load-based-operation}
+
+When load-based operation is selected, a load to be met by the heating coil is requested by the parent object (e.g., AirLoopHVAC:Unitary:Furnace:HeatCool). The model first calculates the heating coil capacity based on the total condenser waste heat rejected by the heating source.
+
+\begin{equation}
+{\dot Q_{coil}} = {\dot Q_{cond}} \times {\varepsilon_{reclaim}}
+\end{equation}
+
+where:
+
+\({\dot Q_{coil}}\) ~~~~~~~~~ = heating capacity of the desuperheater coil (W)
+
+\({\dot Q_{cond}}\) ~~~~~~~~ = total amount of condenser waste heat rejected by the heating source (W)
+
+\({\varepsilon_{reclaim}}\) ~~~~~~ = heat reclaim recovery efficiency
+
+The model then compares the coil's heating capacity to the heating load being requested. If the heating capacity is greater than the heating load, then the amount of reclaimed heat (average heating rate over the simulation time step) is set equal to the requested load and the desuperheater heating coil will cycle off when the requested load is satisfied.
+
+\begin{equation}
+{\dot Q_{reclaim}} = {\dot Q_{load}}
+\end{equation}
+
+Otherwise the amount of reclaimed heat is set equal to the coil's heating capacity and the desuperheater heating coil will operate the entire time that the waste heat source operates.
+
+\begin{equation}
+{\dot Q_{reclaim}} = {\dot Q_{coil}}
+\end{equation}
+
+In either case, the coil's leaving air temperature is then calculated based on the amount of heat recovered and the air mass flow rate through the coil.
+
+\begin{equation}
+{T_{out}} = {T_{in}} + \frac{{{{\dot Q}_{reclaim}}}}{{\dot m{C_p}}}
+\end{equation}
+
+where:
+
+\({T_{out}}\) = coil outlet air temperature (°C)
+
+\({T_{in}}\) = coil inlet air temperature (°C)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \$\$
+
+\(\dot m\) ~ = air mass flow rate through the heating coil (kg/s)
+
+\({C_p}\) = specific heat of air entering the heating coil (J/kg-C)
+
+A final calculation is made to determine the runtime fraction of the desuperheater heating coil. Since the maximum amount of reclaim heat available is dependent on the runtime fraction of the waste heat source, the runtime fraction of the desuperheater heating coil is the product of the waste heat source's runtime fraction and the ratio of the amount of heat reclaimed to the desuperheater coil's heating capacity.
+
+\begin{equation}
+RT{F_{coil}} = RT{F_{source}}\left( {\frac{{{{\dot Q}_{reclaim}}}}{{{{\dot Q}_{coil}}}}} \right)
+\end{equation}
+
+where:
+
+\(RT{F_{coil}}\) ~~~~~ = runtime fraction of the desuperheater heating coil
+
+\(RT{F_{source}}\) ~~~ = runtime fraction of the desuperheater heating source
+
+The heating coil's outlet air humidity ratio and air mass flow rate are simply set equal to the coil inlet air values. The outlet air enthalpy is calculated based on the outlet air dry-bulb temperature and the outlet air humidity ratio.
+
+\begin{equation}
+{h_{out}}\, = \,PsyHFnTdbW({T_{out}},\,\,{\omega_{out}})
+\end{equation}
+
+where
+
+\({h_{out}}\) ~~~~~~~~ = enthalpy of the air leaving the heating coil, J/kg
+
+\(\,{\omega_{out}}\) ~~~~~~~ = humidity ratio of the air leaving the heating coil, kg/kg
+
+\emph{PsyHFnTdbW} = EnergyPlus psychrometric function, returns enthalpy given dry-bulb temperature and humidity ratio
+
+\subsubsection{Temperature-Based Operation}\label{temperature-based-operation}
+
+When temperature-based operation is selected, the model first calculates the heating coil capacity based on the total condenser waste heat rejected by the heating source (same as for load-based operation).
+
+\begin{equation}
+{\dot Q_{coil}} = {\dot Q_{cond}} \times {\varepsilon_{reclaim}}
+\end{equation}
+
+The model then calculates the heating load required to reach the desired setpoint temperature.
+
+\begin{equation}
+{\dot Q_{load}} = \dot m{C_p}\left( {{T_{setpoint}} - {T_{in}}} \right)
+\end{equation}
+
+where:
+
+\({\dot Q_{load}}\) ~~~~~~~~~ = heating load to meet the desired dry-bulb temperature setpoint (W)
+
+\({T_{setpoint}}\) ~~~~~~ = desired dry-bulb temperature setpoint (°C)
+
+A comparison is then made to determine if the desuperheater heating coil should be energized. If the calculated load is less than or equal to 0, the coil's inlet air dry-bulb temperature is at or above the setpoint. In this case the desuperheater heating coil is not active and the outlet air dry-bulb temperature is set equal to the inlet air dry-bulb temperature.
+
+\begin{equation}
+{\dot Q_{reclaim}} = 0
+\end{equation}
+
+\begin{equation}
+{T_{out}}{\rm{ }} = {\rm{ }}{T_{in}}
+\end{equation}
+
+If the amount of heat required to meet the setpoint is larger than the desuperheater coil's heating capacity, then the amount of reclaimed heat is set equal to the coil heating capacity and the outlet air dry-bulb temperature is calculated.
+
+\begin{equation}
+{\dot Q_{reclaim}} = {\dot Q_{coil}}
+\end{equation}
+
+\begin{equation}
+{T_{out}} = {T_{in}} + \frac{{{{\dot Q}_{reclaim}}}}{{\dot m{C_p}}}
+\end{equation}
+
+If the amount of heat required to meet the setpoint is less than the desuperheater coil's heating capacity, the amount of reclaimed heat is set equal to the calculated heating load and the outlet air dry-bulb temperature is set equal to the setpoint temperature. In this case the desuperheater heating coil will cycle off when the requested load is satisfied.
+
+\begin{equation}
+{\dot Q_{reclaim}} = {\dot Q_{load}}
+\end{equation}
+
+\begin{equation}
+{T_{out}}\quad  = \;{T_{setpoint}}
+\end{equation}
+
+A final calculation is made to determine the runtime fraction of the desuperheater heating coil. Since the maximum amount of reclaim heat available is dependent on the runtime fraction of the waste heat source, the runtime fraction of the desuperheater heating coil is the product of the waste heat source's runtime fraction and the ratio of the amount of heat reclaimed to the desuperheater coil's heating capacity.
+
+\begin{equation}
+RT{F_{coil}} = RT{F_{source}}\left( {\frac{{{{\dot Q}_{reclaim}}}}{{{{\dot Q}_{coil}}}}} \right)
+\end{equation}
+
+The heating coil's outlet air humidity ratio and air mass flow rate are simply set equal to the coil inlet air values. The outlet air enthalpy is calculated based on the outlet air dry-bulb temperature and the outlet air humidity ratio.
+
+\begin{equation}
+{h_{out}}\, = \,PsyHFnTdbW({T_{out}},\,\,{\omega_{out}})
+\end{equation}
+
+\subsubsection{Parasitic Electric Load}\label{parasitic-electric-load}
+
+The parasitic electric load attributed to the desuperheater heating coil is calculated using the user-supplied input value (\({P_{parasitic}}\) ) and the desuperheater heating coil runtime fraction calculated above.
+
+\begin{equation}
+{P_{elec}} = {P_{parasitic}} \times RT{F_{coil}}
+\end{equation}
+
+The model assumes that this electric load is small and does not contribute to heating the air stream.
+
+\subsubsection{References}\label{references-7}
+
+Kosar, D. 2006. Dehumidification Enhancements, ASHRAE Journal, Vol. 48, No. 2, February 2006.
+
+Kosar, D. et al. 2006. Dehumidification Enhancement of Direct Expansion Systems Through Component Augmentation of the Cooling Coil. 15\(^{th}\) Symposium on Improving Building Systems in Hot and Humid Climates, July 24-26, 2006.
+
+Nimmo, B.G. et al. 1993.DEAC: Desiccant Enhancement of Cooling-Based Dehumidification. ASHRAE Transactions, Vol.99, Part 1, Paper number CH-93-4-4, pp.~842-848.
+
+\subsection{Desuperheater-Recovery-Based Water Heating Coil}\label{desuperheater-recovery-based-water-heating-coil}
+
+\subsubsection{Overview}\label{overview-10}
+
+The input object Coil:WaterHeating:Desuperheater provides a model that simulates the thermal performance of a refrigerant-to-water heating coil and the electric consumption of its water circulation pump, control valves, and other auxiliary devices. The model assumes that the heating energy provided by this coil is reclaimed from the superheated refrigerant gas leaving a compressor and does not impact the performance of the compressor. The objects from which this coil can obtain its heating energy are:
+
+Coil:Cooling:DX:SingleSpeed
+
+Coil:Cooling:DX:TwoSpeed
+
+Coil:Cooling:DX:TwoStageWithHumidityControlMode
+
+Refrigeration:CompressorRack
+
+Refrigeration:Condenser* (multiple objects)
+
+The heat reclaim recovery efficiency (specified by the user) defines the amount of heat available for use by this coil. Approximately 25-30\% of the energy rejected by typical refrigeration system condensers is to reduce the superheated refrigerant vapor temperature to the condensing temperature. Recovery efficiencies higher than 30\% may cause the refrigerant gas to condense, which in turn impacts the performance of the refrigeration compressor rack. For this reason, the maximum heat reclaim recovery efficiency for this coil for all sources except the Refrigeration:Condenser:(Air, Water, or Evap)Cooled is 30\%.For these refrigeration condensers, the amount of waste energy available in the superheat region is explicitly calculated, so for these condensers the maximum heat recovery efficiency is 90\% of this superheat energy. Also, for these refrigeration condensers, an estimate of the temperature of the reclaimed heat source is made and compared to the inlet air temperature for the coil. If the reclaimed heat source is too cool, the amount of available reclaim energy is set to zero. For all heat sources, the model includes the ability to modify the heat reclaim recovery efficiency based on variations in inlet water temperature and outdoor air dry-bulb temperature.
+
+NOTE: When the heating source is a refrigerated case compressor rack, the heat rejection location in the Refrigeration:CompressorRack object must be ``Outdoors''. If the compressor rack heat rejection location is ``Zone'', the total amount of heat rejection available for reclaim (e.g., by this desuperheater heating coil) is set to zero by the compressor rack object and the simulation proceeds.
+
+To model a desuperheater water heating coil, the input data file must include the following objects:
+
+·~~~~~~~~Coil:WaterHeating:Desuperheater
+
+·~~~~~~~~WaterHeater:Mixed
+
+·~~~~~~~~Coil:Cooling:DX:* or Refrigeration:CompressorRack, or Refrigeration:Condenser:*
+
+A schematic diagram showing the desuperheater water heating coil with its water heater and DX system condenser is shown below.
+
+\begin{figure}[hbtp] % fig 172
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4049.png}
+\caption{Schematic of Desuperheater Water Heating Coil \protect \label{fig:schematic-of-desuperheater-water-heating-coil}}
+\end{figure}
+
+\subsubsection{Model Description}\label{model-description-7}
+
+The desuperheater heating coil input requires a setpoint temperature schedule and dead band temperature difference, which are independent from the setpoint temperature schedule and dead band temperature difference for the heater (element or burner) associated with the water heater tank. The cut-in temperature for the desuperheater coil is defined as the desuperheater coil's setpoint temperature minus its dead band temperature difference.
+
+\begin{equation}
+{T_{cut - in}}\,\, = \,\,{T_{set\,point}}\,\, - \,\,{T_{dead\,band}}
+\end{equation}
+
+where:
+
+\({T_{cut - in}}\) ~~~~~~~~ = Cut-in temperature (°C)
+
+\({T_{set\,point}}\) ~~~~~~ = Setpoint temperature (°C)
+
+\({T_{dead\,band}}\) ~~~~ = Dead band temperature difference (°C)
+
+Desuperheater water heating coils are typically used to offset energy consumption by the water tank's heater (element or burner). Therefore, the cut-in temperature of the desuperheater coil should always be higher than the water heater tank's setpoint temperature. At times when the water heater tank's setpoint temperature is greater than or equal to the cut-in temperature of the desuperheater coil, the desuperheater is disabled and the water heater tank heating element is used to heat the water. An additional input parameter sets the maximum inlet water temperature allowed for desuperheater heat reclaim. Any time the inlet water temperature to the desuperheater coil is above this maximum allowed temperature, heat reclaim is restricted so that the tank water does exceed this temperature.
+
+When the desuperheater coil is scheduled off by its availability schedule, the water heater tank's setpoint temperature is greater than or equal to the desuperheater coil cut-in temperature, or if the DX system's compressor (source of heat reclaim) is off, the water heating capacity and water mass flow rate for the desuperheater coil are set to zero and the water heater tank is simulated with the desuperheater heating coil disabled. Otherwise, the simulation proceeds by first determining the maximum amount of heat available for heat reclaim. If a heat reclaim efficiency modifier curve object is specified by the user, this bi-quadratic curve is evaluated using the desuperheater coil inlet water temperature and the outdoor air dry-bulb temperature; otherwise, the output is assumed to be equal to 1.
+
+If HEffFTemp is specified:
+
+\begin{equation}
+  HEffFTemp = \max\PB{0.0, f\PB{T_{water,inlet},T_{DB,outdoor}}}
+\end{equation}
+
+Else:
+
+\begin{equation}
+  HEffFTemp = 1.0
+\end{equation}
+
+where:
+
+\(HEffFTemp\) = Heat reclaim efficiency modifier
+
+\({T_{water,inlet}}\) ~~~~ = Desuperheater coil inlet water temperature (°C)
+
+\({T_{DB,outdoor}}\) ~~~ = Outdoor air dry-bulb temperature (°C)
+
+Except for the detailed condenser source, heat reclaim recovery efficiencies higher than 30\% may cause the refrigerant gas to condense which in turn impacts the performance of the refrigeration system. The model is unable to account for this refrigeration system impact, so the product of the rated heat reclaim recovery efficiency and heat reclaim efficiency modifier is not allowed to exceed 0.3.~ For the detailed refrigeration condenser, the limit for the heat reclaim efficiency has been set at 0.9 as follows:
+
+\begin{equation}
+{\rm{IF}}\left( {{\varepsilon_{{\rm{reclaim,rated}}}}} \right)\left( {HEfFTemp} \right) > Limit,{\rm{ then }}HeffFTemp = \frac{{Limit}}{{{\varepsilon_{{\rm{reclaim,rated}}}}}}
+\end{equation}
+
+where:
+
+Limit~~~~~~~~~~ = 0.3 for most sources, = 0.9 for detailed condensers
+
+\({\varepsilon_{reclaim,rated}}\) = rated heat reclaim recovery efficiency
+
+The heating capacity of the desuperheater coil is then calculated based on the product of total amount of condenser waste heat rejected by the heating source, the desuperheater coil's rated heat reclaim recovery efficiency, and the heat reclaim efficiency modifier.
+
+\begin{equation}
+{\dot Q_{coil}} = {{\left( {{{\dot Q}_{cond}}} \right)\left( {{\varepsilon_{reclaim,rated}}} \right)HEffFTemp} \mathord{\left/ {\vphantom {{\left( {{{\dot Q}_{cond}}} \right)\left( {{\varepsilon_{reclaim,rated}}} \right)HEffFTemp} {DXSystemPLR}}} \right. } {DXSystemPLR}}
+\end{equation}
+
+where:
+
+\({\dot Q_{coil}}\) ~~~~~~~~~ = water heating capacity of the desuperheater coil (W)
+
+\({\dot Q_{cond}}\) ~~~~~~~~ = average rate of condenser waste heat rejected by the heating source (W)
+
+\(DXSystemPLR\) ~ = part load ratio for the desuperheater coil heating source (1.0 for refrigerated case compressor rack and detailed refrigeration condenser)
+
+The desuperheater is assumed to have a water circulation pump located downstream of the refrigerant-to-water coil. Pump heat is added to the desuperheater water heating capacity based on a user-defined fraction as follows:
+
+\begin{equation}
+{\dot Q_{coil}} = {\dot Q_{coil}} + {P_{pump}}\left( {Fra{c_{pumptowater}}} \right)
+\end{equation}
+
+where:
+
+\({P_{pump}}\) ~~~~~~~~ ~~~~~~~~~~~ = water pump power (W)
+
+\(Fra{c_{pumptowater}}\) ~~~~~~~ = fraction of pump heat to water
+
+The temperature of the water leaving the desuperheater is then calculated as
+
+\({T_{water,outlet}} = {T_{water,inlet}} + \frac{{{Q_{coil}}}}{{{{\dot m}_{water}}\cdot {C_{p,water}}}}\) ~for \({\dot m_{water}}\) ~\textgreater{} 0
+
+\({T_{water,outlet}} = {T_{water,inlet}}\) ~for \({\dot m_{water}}\) ~ = 0
+
+Simulation of the desuperheater heating coil is based on its current mode of operation. This mode of operation is either floating (heating coil off and tank water temperature has not fallen below the heater cut-in temperature) or heating (tank water temperature dropped below the heater cut-in temperature on a previous time step but was unable to reach the heater setpoint temperature). Each mode is handled differently and they will be discussed separately.
+
+\subsubsection{Float Mode}\label{float-mode}
+
+When the water heater tank temperature is floating between the desuperheater coil's cut-in and cut-out temperatures at the end of the previous simulation time step, both the desuperheater coil and the water heater tank's heating element are disabled and a resulting tank temperature is calculated. If the resulting tank temperature is below the desuperheater coil cut-in temperature the desuperheater coil part-load ratio is estimated using a ratio of temperature differences as shown below. The part-load ratio can not be less than zero or greater than the part-load ratio of the DX system from which the desuperheater coil is reclaiming heat.
+
+\begin{equation}
+PLR = \,MIN\left( {DXSystemPLR,MAX\left( {0.0,\,\,\left( {\frac{{{T_{cut - in}} - {T_{tank,float}}}}{{{T_{tank,initial}} - {T_{tank,float}}}}} \right)} \right)} \right)
+\end{equation}
+
+where:
+
+\(PLR\) ~~~~~~~~ = part load ratio of desuperheater heating coil
+
+\({T_{tank,float}}\) ~~~~ = tank temperature in float mode when heating capacity is set to zero (°C)
+
+\({T_{tank,initial}}\) ~~~ = tank water temperature at the beginning of a simulation time step (°C)
+
+Since the water pump is assumed to cycle on and off with the desuperheater coil, the average water mass flow rate through the desuperheater coil is then set proportional to the PLR calculated above:
+
+\begin{equation}
+\dot mwater,avg = \dot mwater\left( {PLR} \right)
+\end{equation}
+
+where:
+
+\(\dot mwater,avg\) ~~~~~~ = average desuperheater water mass flow rate for the time step (kg/s)
+
+The water tank temperature is then calculated based on desuperheater heating coil operation (outlet water temperature and average water mass flow rate as calculated above) and with the water tank's heater element enabled. If the resulting water tank temperature is above the desuperheater coil's setpoint temperature, then the part-load ratio is reduced in the same manner described in the heating mode section below.
+
+\subsubsection{Heating Mode}\label{heating-mode}
+
+When the desuperheater heating coil is in heating mode at the end of the previous simulation time step (i.e., desuperheater coil operated during the previous simulation time step but was unable to achieve the setpoint temperature), both the desuperheater and the water heater tank's heating element are enabled. The desuperheater coil outlet water temperature is calculated (as described above) and the water mass flow rate through the desuperheater coil is set to the maximum operating flow rate:
+
+\textbf{\(\dot mwater,avg = \dot mwater\left( {DXSystemPLR} \right)\)}
+
+If the resulting tank water temperature is above the desuperheater coil's setpoint (cut-out) temperature, the part load ratio of the desuperheater coil is reduced and the water heater tank is simulated again. The process is performed iteratively until the part load ratio of the desuperheater coil achieves the desired setpoint temperature.
+
+\subsubsection{Model Outputs}\label{model-outputs}
+
+After completing the float mode or heating mode calculations and the final desuperheater part load ratio has been determined, the output (report) variables are calculated as follows:
+
+\begin{equation}
+Desuperheater\,Part\,Load\,Ratio = MIN\left( {\frac{{\dot mwater,avg}}{{\dot mwater}},DXSystemPLR} \right)\,\,
+\end{equation}
+
+\begin{equation}
+Desuperheater\,\,Water\,Heating\,Rate\,\,(W) = {\dot Q_{coil}}\left( {PLR} \right)
+\end{equation}
+
+\begin{equation}
+Desuperheater\,\,Water\,Heating\,Energy\,\,(J) = {\dot Q_{coil}}\left( {PLR} \right)(3600)\left( {{t_{sys}}} \right)
+\end{equation}
+
+\begin{equation}
+Desuperheater\,\,Pump\,\,Electric\,\,Power\,\,(W) = {P_{pump}}\left( {PLR} \right)
+\end{equation}
+
+\begin{equation}
+Desuperheater\,\,Pump\,\,Electric\,\,Consumption\,\,(J) = {P_{pump}}\left( {PLR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)
+\end{equation}
+
+\begin{equation}
+Desuperheater Heat Reclaim Efficiency Modifier Curve Output\,\, = \,\,HEffFTemp
+\end{equation}
+
+\begin{equation}
+Desuperheater\,\,On{\rm{ - }}Cycle\,Parasitic\,Electric\,Power\,(W)\,\, = \,\,{P_{parasiticload,on}}\left( {PLR} \right)
+\end{equation}
+
+\begin{equation}
+\begin{split}
+Desuperheater\,\,On{\rm{ - }}Cycle\,Parasitic\,Electric\,Consumption\,(J)\,\, = \\{P_{parasiticload,on}}\left( {PLR} \right)\left( {3600} \right){t_{sys}}
+\end{split}
+\end{equation}
+
+\begin{equation}
+Desuperheater\,\,Off{\rm{ - }}Cycle\,Parasitic\,Electric\,Power\,(W)\,\, = \,\,{P_{parasiticload,off}}\left( {1 - PLR} \right)
+\end{equation}
+
+\begin{equation}
+\begin{split}
+Desuperheater\,\,Off{\rm{ - }}Cycle\,Parasitic\,Electric\,Consumption\,(J)\,\, = \\{P_{parasiticload,off}}\left( {1 - PLR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)
+\end{split}
+\end{equation}
+
+where:
+
+\({P_{parasiticload,on}}\) ~~~~~~~~~~ = on-cycle parasitic electric load (W)
+
+\({P_{parasiticload,off}}\) ~~~~~~~~~ = off-cycle parasitic electric load (W)
+
+\({t_{sys}}\) ~~~~~~~~~~~~~~~~~~~~~~~~ = HVAC system simulation time step (hours)
+
+Note: All output variables, including off cycle parasitic electrical power and energy, equal 0 when the desuperheater heating coil availability schedule equals 0.
+
+\subsection{Heat Exchanger Assisted Air Cooling Coil Systems}\label{heat-exchanger-assisted-air-cooling-coil-systems}
+
+An air-to-air heat exchanger can be used to enhance the dehumidification performance of a conventional cooling coil. EnergyPlus has two compound objects to model this scenario: CoilSystem:Cooling:DX:HeatExchangerAssisted and CoilSystem:Cooling:Water:HeatExchangerAssisted. The input syntax for these compound objects can be found in the EnergyPlus Input/Output Reference.
+
+As shown in Figure~\ref{fig:schematic-of-a-heat-exchanger-assisted}, the air-to-air heat exchanger pre-conditions the air entering the cooling coil, and reuses this energy to post-condition the supply air leaving the cooling coil. This heat exchange process improves the latent removal performance of the cooling coil by allowing it to dedicate more of its cooling capacity toward dehumidification (lower sensible heat ratio).
+
+\begin{figure}[hbtp] % fig 173
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4091.png}
+\caption{Schematic of a Heat Exchanger Assisted Cooling Coil \protect \label{fig:schematic-of-a-heat-exchanger-assisted}}
+\end{figure}
+
+NOTE: Node naming shown in Figure~\ref{fig:schematic-of-a-heat-exchanger-assisted} is representative for \\
+HeatExchanger:AirToAir:SensibleAndLatent. For HeatExchanger:AirToAir:FlatPlate, the exhaust air nodes are referred to as `secondary air' nodes. For HeatExchanger:Desiccant:BalancedFlow (heat exchanger assisted DX coil only), the supply air nodes are referred to as `regeneration air' nodes and the exhaust air nodes as `process air' nodes.
+
+The dehumidification performance of cooling coils can be enhanced using a sensible-only heat exchanger (e.g., heat pipes, runaround coils, cross-flow heat exchangers). For example, a CoilSystem:Cooling:DX:HeatExchangerAssisted object could be used with a HeatExchanger:AirToAir:FlatPlate object or HeatExchanger:AirToAir:SensibleAndLatent object with only sensible effectiveness specified (see resulting psychrometric process in Figure~\ref{fig:psychrometric-process-for-heat-exchanger}). The dehumidification performance of cooling coils can also be enhanced using heat exchangers that transfer both sensible and latent energy (e.g., rotary desiccant heat exchanger). For example, a CoilSystem:Cooling:DX:HeatExchangerAssisted object could be used with a HeatExchanger:Desiccant:BalancedFlow object (see resulting psychrometric process in Figure~\ref{fig:psychrometric-process-for-heat-exchanger-001}).
+
+Note that while the HeatExchanger:AirToAir:SensibleAndLatent and HeatExchanger:Desiccant:BalancedFlow objects can transfer both sensible and latent heat between two air streams, the HeatExchanger:Desiccant:BalancedFlow object with appropriate Performance Data Type object is the proper heat exchanger model to use for the heat exchanger assisted cooling coil described here. The HeatExchanger:AirToAir:SensibleAndLatent object should only be used to model the sensible-only heat exchange case (Figure~\ref{fig:psychrometric-process-for-heat-exchanger}).
+
+\begin{figure}[hbtp] % fig 174
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4092.png}
+\caption{Psychrometric Process for Heat Exchanger Assisted Cooling Coil (Sensible HX Only) \protect \label{fig:psychrometric-process-for-heat-exchanger}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 175
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4093.png}
+\caption{Psychrometric Process for Heat Exchanger Assisted Cooling Coil (Sensible+Latent HX) \protect \label{fig:psychrometric-process-for-heat-exchanger-001}}
+\end{figure}
+
+Modeling of the heat exchanger assisted cooling coil is performed by consecutively modeling the air-to-air heat exchanger and the cooling coil until convergence on a solution is achieved. The detailed modeling calculations for the individual components (air-to-air heat exchangers and cooling coils) are described elsewhere in this document.
+
+Modeling of the heat exchanger assisted cooling coil begins by initializing the air mass flow rate (based on the air mass flow rate placed on the compound object's inlet air node) and passing this value to the exhaust air inlet node of the air-to-air heat exchanger. The heat exchanger and cooling coil are then successively modeled using the calculation routines specific to the type of heat exchanger and cooling coil selected. The air temperature exiting the cooling coil is compared with the air temperature exiting the cooling coil on the previous modeling iteration for this simulation time step. Convergence is reached when the change in this air temperature for successive iterations is within a specified tolerance (0.0005°C). Consecutive modeling of the heat exchanger and cooling coil is terminated and a warning message is issued if the number of modeling iterations exceeds 50.
+
+For the CoilSystem:Cooling:DX:HeatExchangerAssisted object, heat exchanger operation can be controlled based on high humidity levels in a zone. By default, the heat exchanger is assumed to always provide its heat transfer when the associated DX cooling coil is operating and no humidity control mechanism is specified. However, the heat exchanger's energy transfer may be controlled (i.e., turned on and off) based on a zone air humidity level using either a humidistat alone (Figure~\ref{fig:schematic-of-a-heat-exchanger-assisted-dx}) or a humidistat and a maximum humidity setpoint manager (Figure~\ref{fig:schematic-of-heat-exchanger-assisted-dx-coil}) depending on the HVAC system that is utilizing the heat exchanger assisted cooling coil.
+
+The heat exchanger assisted DX cooling coil may be used with furnaces or unitary systems located in an air loop (ref. AirLoopHVAC:Unitary:Furnace:HeatCool or AirLoopHVAC:UnitaryHeatCool). These system objects have three options for dehumidification control (None, Multimode, and CoolReheat). When no dehumidification control is specified in the furnace or unitary system object (None), the heat exchanger is always active when the cooling coil is operating. When multimode or coolreheat dehumidification control is specified, a humidistat is required as shown in Figure~\ref{fig:schematic-of-a-heat-exchanger-assisted-dx}. For the case of multimode dehumidification control, the heat exchanger is only active when the zone air humidity level is above the humidistat setpoint (i.e., the system's cooling coil can't meet the latent cooling load when operating without heat exchanger energy transfer) while the AC system operates to meet the sensible (dry-bulb cooling thermostat) load. For the case of coolreheat dehumidification control, the heat exchanger is always active when the cooling coil operates and this system tries to meet both the sensible (thermostat) and latent (humidistat) loads.
+
+\begin{figure}[hbtp] % fig 176
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4094.png}
+\caption{Schematic of a heat exchanger assisted DX cooling coil with optional humidistat \protect \label{fig:schematic-of-a-heat-exchanger-assisted-dx}}
+\end{figure}
+
+The heat exchanger assisted DX cooling coil may also be used with a DX system located in an air loop (ref. CoilSystem:Cooling:DX). This system object also has three options for dehumidification control (None, Multimode, and CoolReheat). When no dehumidification control is specified (None), the heat exchanger is always active when the cooling coil is operating. When multimode or coolreheat dehumidification control is specified, a humidistat and a maximum humidity setpoint manager are required as shown in Figure~\ref{fig:schematic-of-heat-exchanger-assisted-dx-coil} (setpoint needs to be placed on the DX system's control node). For multimode dehumidification control, the heat exchanger is only active when the zone humidity levels are above the humidistat setpoint (i.e., the system's cooling coil can't meet the maximum humidity ratio setpoint when operating without heat exchanger energy transfer) while the AC system operates to meet the sensible (dry-bulb cooling thermostat) load. For coolreheat dehumidification control, the heat exchanger is always active when the cooling coil operates and this system tries to meet both the sensible (thermostat) and latent (humidistat) loads.
+
+When the heat exchanger assisted cooling coil is used with a furnace or unitary system (ref. AirLoopHVAC:Unitary:Furnace:HeatCool or AirLoopHVAC:UnitaryHeatCool) or DX system (ref. CoilSystem:Cooling:DX) located in an air loop (or DX system used in an outside air system), an ecomizier function may be customized as necessary. For economizer control, an outdoor air controller (ref. Controller:OutdoorAir) is used to define the economizer control inputs and determine when economizer mode is active. The heat exchanger (ref. HeatExchanger:*) object provides an economizer lockout feature which disables heat recovery any time the economizer is active. This feature can be turned on and off using the heat exchanger lockout input. Heat exchanger assisted cooling coils used with the zone equipment described below disregard this economizer control feature.
+
+\begin{figure}[hbtp] % fig 177
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4095.png}
+\caption{Schematic of Heat Exchanger Assisted DX Coil with Humidistat and Setpoint Manager \protect \label{fig:schematic-of-heat-exchanger-assisted-dx-coil}}
+\end{figure}
+
+The heat exchanger assisted DX cooling coil may also be used with the unitary changeover bypass system and the unitary air-to-air heat pump system (ref. AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass and AirLoopHVAC:UnitaryHeatPump:AirToAir); however, the heat exchanger is assumed to always provide its heat transfer when the cooling coil operates and can not be turned on and off based on a zone air humidity setpoint (ref. Figure~\ref{fig:schematic-of-a-heat-exchanger-assisted}). Two zone air conditioners may also use this heat exchanger/coil assembly model for improved dehumidification. The first type is the packaged terminal heat pump (ref. ZoneHVAC:PackagedTerminalHeatPump) where the heat exchanger's heat transfer is always active whenever the cooling coil operates (ref. Figure~\ref{fig:schematic-of-a-heat-exchanger-assisted}). The second type is the window air conditioner (ref. ZoneHVAC:WindowAirConditioner) where the heat exchanger's heat transfer is always active when the cooling coil operates and no humidity control mechanism is specified (ref. Figure~\ref{fig:schematic-of-a-heat-exchanger-assisted}), or the heat exchanger's heat transfer may be controlled based on zone air humidity level when a humidistat and high humidity setpoint manager are specified (maximum humidity ratio setpoint must be placed on the heat exchanger's exhaust air outlet node). For this case, the heat exchanger is only active when the zone air humidity level is above the humidistat setpoint (i.e., the system's cooling coil can't meet the maximum humidity ratio setpoint when operating without heat exchanger energy transfer) while only the sensible (dry-bulb cooling thermostat) load is met by the AC system (ref. Figure~\ref{fig:schematic-of-heat-exchanger-assisted-dx-coil}).
+
+For the CoilSystem:Cooling:Water:HeatExchangerAssisted object, there is currently no method to enable or disable heat exchange based on zone air humidity level. Heat exchange will occur whenever the heat exchanger is available to operate (via its availability schedule) and a temperature difference exists between the two air streams.
+
+\subsubsection{References}\label{references-8}
+
+Kosar, D. 2006. Dehumidification Enhancements, ASHRAE Journal, Vol. 48, No. 2, February 2006.
+
+Kosar, D. et al. 2006. Dehumidification Enhancement of Direct Expansion Systems Through Component Augmentation of the Cooling Coil. 15\(^{th}\) Symposium on Improving Building Systems in Hot and Humid Climates, July 24-26, 2006.
+
+Nimmo, B.G. et al. 1993.DEAC: Desiccant Enhancement of Cooling-Based Dehumidification. ASHRAE Transactions, Vol.99, Part 1, Paper number CH-93-4-4, pp.~842-848.
+
+\subsection{Single-Speed Electric Heat Pump DX Water Heating Coil}\label{single-speed-electric-heat-pump-dx-water-heating-coil}
+
+\subsubsection{Overview}\label{overview-11}
+
+The input object \lstinline!Coil:WaterHeating:AirToWaterHeatPump:\*! provides a model used in a heat pump water heater (HPWH) consisting of a water heater tank (e.g., \lstinline!WaterHeater:Mixed! or \lstinline!WaterHeater:Stratified!), a direct expansion (DX) ``coil'' (i.e., an air-to-water DX compression system which includes a water heating coil, air coil, compressor, and water pump), and a fan to provide air flow across the air coil associated with the DX compression system. These objects work together to model a system which heats water using zone air, outdoor air, or a combination of zone and outdoor air as the primary heat source. The heat pump water heater (Ref. \lstinline!WaterHeater:HeatPump:*!), water heater tank (Ref. \lstinline!WaterHeater:Mixed! and \lstinline!WaterHeater:Stratified!), and fan (Ref. \lstinline!Fan:\*!) objects are described elsewhere in this document.
+
+\begin{figure}[hbtp] % fig 178
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4096.png}
+\caption{Schematic of a Heat Pump Water Heater using Optional Mixer/Splitter Nodes \protect \label{fig:schematic-of-a-heat-pump-water-heater-using}}
+\end{figure}
+
+The heat pump water heater DX coil model described here determines the thermal performance and energy consumption of the DX compression system, which includes a water heating coil (condenser), a coil used to extract heat from air (evaporator), and the compressor. This model also simulates the performance of a condenser water pump that is assumed to cycle on and off with the compressor.
+
+\begin{figure}[hbtp] % fig 179
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4097.png}
+\caption{Schematic of the Heat Pump Water Heater DX Coil \protect \label{fig:schematic-of-the-heat-pump-water-heater-dx}}
+\end{figure}
+
+Virtually all of the inputs to this DX coil model relate to its water heating performance and energy consumption. Model inputs differ between the \lstinline!Coil:WaterHeating:AirToWaterHeatPump:Pumped! and \lstinline!Coil:WaterHeating:AirToWaterHeatPump:Wrapped! to include only the relevant inputs for \lstinline!WaterHeater:HeatPump:PumpedCondenser! and \lstinline!WaterHeater:HeatPump:WrappedCondenser!, respectively. The air-side cooling capacity of this DX system is derived from user inputs and some model assumptions. The sensible/latent cooling capacity split is defined by the user at rated conditions, and the model adjusts this split at off-rated conditions.
+
+\subsubsection{Model Description}\label{model-description-8}
+
+The user must input the heating capacity, coefficient of performance (COP), and the sensible heat ratio (SHR) of the evaporator coil at rated inlet fluid temperatures and flow rates that are also specified by the user. The evaporator SHR should be a ``gross'' value, excluding any thermal impacts due to the indoor supply air fan. The user may also input up to seven performance curves that describe the change in total water heating capacity and efficiency at off-rated and part-load conditions.
+
+1)~~~~Heating capacity modifier curve (function of temperature)
+
+2)~~~~Heating capacity modifier curve (function of air flow fraction)
+
+3)~~~~Heating capacity modifier curve (function of water flow fraction, pumped condenser only)
+
+4)~~~~Heating COP modifier curve (function of temperature)
+
+5)~~~~Heating COP modifier curve (function of air flow fraction)
+
+6)~~~~Heating COP modifier curve~ (function of water flow fraction, pumped condenser only)
+
+7)~~~~Part load fraction correlation (function of part load ratio)
+
+Note: The air dry-bulb or wet-bulb temperature used in the following curve objects is the inlet air temperature to the HPWH evaporator coil/fan assembly. If the fan placement specified in the \lstinline!WaterHeater:HeatPump:*! compound object is draw-through, then the inlet air temperature represents the temperature of the air entering the evaporator coil itself. If blow-through fan placement is specified, then the inlet air temperature represents air conditions entering the fan located immediately in front (upstream) of the evaporator coil.
+
+The heating capacity as a function of temperature modifier curve defines the variation in DX coil heating capacity as a function of inlet fluid (air and water) temperatures. The curve object may use either a bi-quadratic or cubic form. The bi-quadratic curve uses inlet air temperature (dry-bulb or wet-bulb temperature based on the input field Evaporator Air Temperature Type for Curve Objects) and condenser inlet water temperature as the independent variables. The cubic curve uses inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The curve should be normalized to have the value of 1.0 at the rating point temperatures specified by the user.
+
+\begin{equation}
+HCapFTemp = a + b\left( {{T_{evap,in}}} \right) + c{\left( {{T_{evap,in}}} \right)^2} + d\left( {{T_{cond,in}}} \right) + e{\left( {{T_{cond,in}}} \right)^2} + f\left( {{T_{evap,in}}} \right)\left( {{T_{cond,in}}} \right)
+\end{equation}
+
+or
+
+\begin{equation}
+HCapFTemp = a + b\left( {{T_{evap,in}}} \right) + c{\left( {{T_{evap,in}}} \right)^2} + d{\left( {{T_{evap,in}}} \right)^3}
+\end{equation}
+
+where:
+
+\({T_{evap,in}}\) ~ = dry-bulb or wet-bulb temperature of the air entering the evaporator coil/fan assembly based on the Evaporator Air Temperature Type for Curve Objects specified by the user (°C)
+
+\({T_{cond,in}}\) ~ = temperature of the water entering the DX coil condenser (°C)
+
+The heating capacity as a function of air flow fraction modifier curve is a quadratic or cubic curve that defines the variation in DX coil heating capacity as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate (i.e., fraction of full load air flow rate). When used, the output of this curve should be normalized to have the value of 1.0~ at an air flow fraction of 1.
+
+\begin{equation}
+HCapFAirFlow = \,a + \,b\left( {f{f_{air}}} \right)\,\, + \,\,c{\left( {f{f_{air}}} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+HCapFAirFlow = \,a + \,b\left( {f{f_{air}}} \right)\,\, + \,\,c{\left( {f{f_{air}}} \right)^2}\,\, + \,\,d{\left( {f{f_{air}}} \right)^3}
+\end{equation}
+
+where:
+
+\begin{equation}
+f{f_{air}} = air\,flow\,fraction = \left( {\frac{{Actual\,air\,mass\,flow\,rate}}{{Rated\,air\,mass\,flow\,rate}}} \right)
+\end{equation}
+
+Note: The actual volumetric air flow rate through the evaporator coil/fan assembly for any simulation time step where the compressor is operating must be between 0.00002684 m\(^{3}\)/s and .00008056 m\(^{3}\)/s per watt of rated total heating capacity. The simulation will issue a warning message if this air flow range is exceeded, but the simulation will continue.
+
+The heating capacity as a function of water flow fraction modifier curve is a quadratic or cubic curve that defines the variation in DX coil heating capacity as a function of the ratio of actual water flow rate through the condenser to the rated condenser water flow rate (i.e., fraction of full load water flow rate). \emph{It is only used for the pumped condenser configuration.} When used, the output of this curve should be normalized to have the value of 1.0 at a water flow fraction of 1.
+
+\begin{equation}
+HCapFWaterFlow = \,a + \,b\left( {f{f_{water}}} \right)\,\, + \,\,c{\left( {f{f_{water}}} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+HCapFWaterFlow = \,a + \,b\left( {f{f_{water}}} \right)\,\, + \,\,c{\left( {f{f_{water}}} \right)^2}\,\, + \,\,d{\left( {f{f_{water}}} \right)^3}
+\end{equation}
+
+where:
+
+\begin{equation}
+f{f_{water}} = water\,flow\,fraction = \left( {\frac{{Actual\,water\,mass\,flow\,rate}}{{Rated\,water\,mass\,flow\,rate}}} \right)
+\end{equation}
+
+The heating COP as a function of temperature modifier curve defines the variation in DX coil heating COP as a function of inlet fluid (air and water) temperatures. The curve object may use either a bi-quadratic or cubic form. The bi-quadratic curve uses inlet air temperature (dry-bulb or wet-bulb temperature based on the input field Evaporator Air Temperature Type for Curve Objects) and condenser inlet water temperature as the independent variables. The cubic curve uses inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The curve should be normalized to have the value of 1.0 at the rating point temperatures specified by the user.
+
+\begin{equation}
+HCOPFTemp = a + b\left( {{T_{evap,in}}} \right) + c{\left( {{T_{evap,in}}} \right)^2} + d\left( {{T_{cond,in}}} \right) + e{\left( {{T_{cond,in}}} \right)^2} + f\left( {{T_{evap,in}}} \right)\left( {{T_{cond,in}}} \right)
+\end{equation}
+
+or
+
+\begin{equation}
+HCOPFTemp = a + b\left( {{T_{evap,in}}} \right) + c{\left( {{T_{evap,in}}} \right)^2} + d{\left( {{T_{evap,in}}} \right)^3}
+\end{equation}
+
+The heating COP as a function of air flow fraction modifier curve is a quadratic or cubic curve that defines the variation in DX coil heating COP as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate (i.e., fraction of full load air flow rate). When used, the output of this curve should be normalized to have the value of 1.0 at an air flow fraction of 1.
+
+\begin{equation}
+HCOPFAirFlow = \,a + \,b\left( {f{f_{air}}} \right)\,\, + \,\,c{\left( {f{f_{air}}} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+HCOPFAirFlow = \,a + \,b\left( {f{f_{air}}} \right)\,\, + \,\,c{\left( {f{f_{air}}} \right)^2}\,\, + \,\,d{\left( {f{f_{air}}} \right)^3}
+\end{equation}
+
+The heating COP as a function of water flow fraction modifier curve is a quadratic or cubic curve that defines the variation in DX coil heating COP as a function of the ratio of actual water flow rate through the condenser to the rated condenser water flow rate (i.e., fraction of full load water flow rate). \emph{It is only used for the pumped condenser configuration.} When used, the output of this curve should be normalized to have the value of 1.0 at a water flow fraction of 1.
+
+\begin{equation}
+HCOPFWaterFlow = \,a + \,b\left( {f{f_{water}}} \right)\,\, + \,\,c{\left( {f{f_{water}}} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+HCOPFWaterFlow = \,a + \,b\left( {f{f_{water}}} \right)\,\, + \,\,c{\left( {f{f_{water}}} \right)^2}\,\, + \,\,d{\left( {f{f_{water}}} \right)^3}
+\end{equation}
+
+The part load fraction as a function of part load ratio correlation curve parameterizes the variation of electrical power input to the heat pump DX coil as a function of the part load ratio (PLR, heating delivered/steady-state heating capacity). The part load ratio divided by the part load fraction yields the runtime fraction of the DX heating coil for a given simulation time step. The part load fraction correlation accounts for efficiency losses due to compressor cycling.
+
+\begin{equation}
+PartLoadFrac = PLF = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+PartLoadFrac = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2} + d{\left( {PLR} \right)^3}
+\end{equation}
+
+where:
+
+\begin{equation}
+PLR = part\,load\,ratio = \left( {\frac{{water\,heating\,delivered}}{{steady{\rm{ - }}state\,water\,heating\,capacity}}} \right)
+\end{equation}
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor runs continuously for the simulation time step). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7~~ and~~ PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+When the part load fraction correlation for a heat pump water heater DX coil is unknown, the typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential or small commercial unit) may be used:
+
+~~~~~~~~~~~ PLF = 0.85 + 0.15(PLR)
+
+All seven curves are accessed through EnergyPlus' built-in performance curve equation manager (curve:quadratic, curve:cubic and curve:biquadratic). It is not imperative that the user utilize all coefficients shown in the equations above if their performance equation has fewer terms (e.g., if the user's part load fraction correlation curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero).
+
+Note: If any of the above performance curves are not specified by the user, the output of that curve is assumed to be 1 for the entire simulation.
+
+For any simulation time step, the heating capacity of the heat pump water heater DX coil is calculated as follows:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{heating}} = {\mathop Q\limits^ \bullet_{heating,rated}}\left( {HCapFTemp} \right)\left( {HCapFAirFlow} \right)\left( {HCapFWaterFlow} \right)
+\end{equation}
+
+In a similar fashion, the coefficient of performance for the DX coil for any simulation time step is calculated using the following equation:
+
+\begin{equation}
+CO{P_{heating}} = CO{P_{heating,rated}}\left( {HCOPFTemp} \right)\left( {HCOPFAirFlow} \right)\left( {HCOPFWaterFlow} \right)
+\end{equation}
+
+The electric power for the heat pump water heater DX coil is then calculated using the water heating capacity and coefficient of performance calculated above.
+
+\begin{equation}
+{P_{heating}} = \left( {\frac{{{{\mathop Q\limits^ \bullet  }_{heating}}}}{{CO{P_{heating}}}}} \right)
+\end{equation}
+
+where:
+
+\({\mathop Q\limits^ \bullet_{heating}}\) ~~~~~~ = water heating capacity at the current operating conditions (W)
+
+\({\mathop Q\limits^ \bullet_{heating,rated}}\) = water heating capacity at rated conditions, user input (W)
+
+\(CO{P_{heating}}\) ~ = coefficient of performance at the current operating conditions (W/W)
+
+\(CO{P_{heating,rated}}\) = coefficient of performance at rated conditions, user input (W/W)
+
+\({P_{heating}}\) ~~~~~~~ = DX heating coil power (electricity consumption rate) at the current ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ~~~operating conditions (W)
+
+The heating capacity calculated above may or may not include the impact of pump heat. For this reason, the user input Condenser Pump Heat Included in Rated Heating Capacity and Rated COP is used to determine the total water heating capacity including pump heat.
+
+If Condenser Pump Heat Included In Rated Heating Capacity and Rated COP:
+
+\begin{equation}
+  \dot{Q}_{heating,total} = \dot{Q}_{heating}
+\end{equation}
+
+Else:
+
+\begin{equation}
+  \dot{Q}_{heating,total} = \dot{Q}_{heating} + P_{pump}Frac_{PumpToWater}
+\end{equation}
+
+where:
+
+\({\mathop Q\limits^ \bullet_{heating,total}}\) ~ = total water heating capacity including condenser pump heat (W)
+
+\({P_{pump}}\) ~~~~~~~~ = condenser water pump power, user input (W)
+
+\(Fra{c_{pumptowater}}\) = fraction of condenser pump heat to water, user input
+
+Compressor power (electricity consumption rate) is then calculated based on two additional inputs provided by the user. The first input specifies if the condenser pump heat is included in the rated heating capacity and rated COP. If the condenser pump heat is included in the rated heating capacity and COP, then condenser pump power must be subtracted from the DX heating coil power calculated above to determine the compressor power.
+
+The second of these inputs specifies if the evaporator fan power is included in the rated heating COP. If evaporator fan power is included in the rated COP, then fan power must also be subtracted from the DX heating coil power to determine the compressor power as follows:
+
+If Evap Fan Power In COP:
+
+  If Cond Pump Power In COP:
+
+\begin{equation}
+  P_{comp} = P_{heating}-P_{pump}-P_{fan}
+\end{equation}
+
+Else:
+
+\begin{equation}
+  P_{comp} = P_{heating}-P_{fan}
+\end{equation}
+
+where:
+
+\({P_{comp}}\) ~ = Compressor power (electric consumption rate) at the current operating conditions (W)
+
+\({P_{fan}}\) ~ = Fan power, specified in Fan:OnOff object (W)
+
+If fan power is not included in the rated heating COP, then the calculation of compressor power only includes condenser pump power and does not involve the fan:
+
+If Evap Fan Power NOT In COP:
+
+  If Cond Pump Power In COP:
+
+\begin{equation}
+  P_{comp} = P_{heating}-P_{pump}
+\end{equation}
+
+Else:
+
+\begin{equation}
+  P_{comp} = P_{heating}
+\end{equation}
+
+The model assumes that all compressor power is rejected as heat via the DX heating coil. Therefore, the evaporator total cooling capacity at the current operating conditions is determined depending on the user input for pump heat:
+
+If Condenser Pump Heat Included In Rated Heating Capacity and Rated COP:
+
+\begin{equation}
+  \dot{Q}_{Evap} = \dot{Q}_{heating} - P_{comp} - P_{pump}Frac_{pumptowater}
+\end{equation}
+
+Else:
+
+\begin{equation}
+  \dot{Q}_{Evap} = \dot{Q}_{heating} - P_{comp}
+\end{equation}
+
+where:
+
+\({\mathop Q\limits^ \bullet_{evap}}\) ~ = Total evaporator cooling capacity at the current operating conditions (W)
+
+This evaporator cooling capacity is used to calculate the air-side performance of the heat pump water heater DX coil. The sensible heat ratio of the cooling capacity at rated conditions is specified by the user in the input for this DX coil object. The calculation of sensible heat ratio at off-rated conditions uses the ADP/BF approach described for the DX cooling coil model (Ref. Coil Model -- DX Cooling Coil Model). The exiting air conditions for the HPWH DX coil are calculated the same way as they are for the DX cooling coil model (cycling fan, cycling coil). The crankcase heater power and consumption are also calculated using the same equations used for the DX cooling coil model.
+
+The runtime fraction of the DX coil compressor is calculated as the ratio of the compressor part load ratio to the part load fraction correlation entered by the user. The part load ratio of the DX coil is determined by the heat pump water heater compound object (Ref. \lstinline!WaterHeater:HeatPump:*!) and is used by the DX coil to determine the run time fraction of the compressor.
+
+\begin{equation}
+RTF = \left( {{\raise0.7ex\hbox{{PLR}} \!\mathord{\left/ {\vphantom {{PLR} {PartLoadFrac}}}\right.}\!\lower0.7ex\hbox{{PartLoadFrac}}}} \right) = runtime\,fraction\,of\,the\,compressor
+\end{equation}
+
+Finally, the condenser water outlet temperature is calculated based on the total water heating capacity of the DX coil and the actual condenser water mass flow rate.
+
+\begin{equation}
+{T_{cond,out}} = {T_{cond,in}} + \left( {\frac{{{{\mathop Q\limits^ \bullet  }_{heating,total}}}}{{\mathop m\limits^ \bullet  cond\,\,\,{C_p}}}} \right)
+\end{equation}
+
+where:
+
+\({T_{cond,out}}\) ~ = condenser outlet water temperature when the DX coil is operating (ËšC)
+
+\({T_{cond,in}}\) ~ = condenser inlet water temperature (ËšC)
+
+\({C_p}\) ~ = specific heat of water entering the condenser coil (J/kg-C)
+
+\(\mathop m\limits^ \bullet cond\) ~ = actual condenser water mass flow rate when the coil is operating, ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ defined in the WaterHeater:HeatPump:PumpedCondenser parent object (kg/s)
+
+\subsubsection{Model Outputs}\label{model-outputs-1}
+
+After completing the calculations for heating capacity and power and the final compressor part load ratio has been determined, the output (report) variables are calculated as follows:
+
+\begin{equation}
+DX\,Coil\,Total\,Water\,Heating\,Rate\,(W) = {\mathop Q\limits^ \bullet_{heating,total}}\left( {PLR} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Total\,Water\,Heating\,Energy\,(J) = {\mathop Q\limits^ \bullet_{heating,total}}\left( {PLR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Water\,Heating\,Electric\,Power\,(W) = \left( {{P_{comp}} + {P_{pump}}} \right)\left( {RTF} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Water\,Heating\,Electric\,Consumption\,(J) = \left( {{P_{comp}} + {P_{pump}}} \right)\left( {RTF} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Total\,Cooling\,Rate\,(W) = \,{\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Total\,Cooling\,Energy\,\,(J) = \,{\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Sensible\,Cooling\,Rate\,(W) = \,{\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)\left( {SHR} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Sensible\,Cooling\,Energy\,(J) = \,{\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)\left( {SHR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Latent\,Cooling\,Rate\,(W) = \,{\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)\left( {1.0 - SHR} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Latent\,Cooling\,Energy\,\,(J) = {\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)\left( {1.0 - SHR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Runtime\,Fraction = \left( {{\raise0.7ex\hbox{{PLR}} \!\mathord{\left/ {\vphantom {{PLR} {PartLoadFrac}}}\right.}\!\lower0.7ex\hbox{{PartLoadFrac}}}} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Crankcase\,Heater\,Power\,(W) = \,\left( {{P_{crankcase}}} \right)\left( {1.0 - RTF} \right)
+\end{equation}
+
+\begin{equation}
+DX\,Coil\,Crankcase\,Heater\,Consumption\,(J) = \,\left( {{P_{crankcase}}} \right)\left( {1.0 - RTF} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)
+\end{equation}
+
+where:
+
+\emph{t\(_{sys}\)~~~~~~~~~~~~ =} HVAC system simulation time step, hr
+
+\emph{SHR}~~~~~~~~~~ = sensible heat ratio at the current inlet air conditions and air flow rate ~~~~~~~~~~~~~~~~~~~~~~~~~~ (Ref. Coil Model -- DX Cooling Coil Model, ADP/BF approach)
+
+\emph{P\(_{crankcase}\)~~~~~} = Crankcase heater capacity, user input (W)
+
+\subsection{Water Source Electric DX Air Cooling Coil}\label{water-source-electric-dx-air-cooling-coil}
+
+There are two objects for water-to-air heat pumps in cooling mode: \\ Coil:Cooling:WaterToAirHeatPump:EquationFit and Coil:Cooling:WaterToAirHeatPump:ParameterEstimation.~ These are described elsewhere.
+
+\subsection{Water Source Electric Heat Pump DX Air Heating Coil}\label{water-source-electric-heat-pump-dx-air-heating-coil}
+
+There are two objects for water-to-air heat pumps in heating mode: \\ ~Coil:Heating:WaterToAirHeatPump:EquationFit and Coil:Heating:WaterToAirHeatPump:ParameterEstimation.~ These are described elsewhere.
+
+\subsection{Steam-Based Air Heating Coil}\label{steam-based-air-heating-coil}
+
+The steam coils are included in the discussion on steam loops, see: Steam To Air Heat Exchanger.
+
+\subsection{Variable Refrigerant Flow Cooling Coil}\label{variable-refrigerant-flow-cooling-coil}
+
+\subsubsection{Overview}\label{overview-12}
+
+The variable refrigerant flow (VRF) DX cooling coil model is identical to the single-speed DX cooling coil model (Ref. Coil:Cooling:DX:SingleSpeed) when the compressor operates at it's maximum speed. The calculations used when the VRF heat pump operates at part-load are slightly different than the single-speed DX cooling coil model. For this reason, an adaptation of the single-speed DX cooling coil model is used to model the variable-speed compression system used in the VRF model. The difference in model calculations occur when the VRF DX cooling coil's electronic expansion device reduces refrigerant flow through the cooling coil. When the refrigerant flow is reduced, the coil's apparatus dew point (ADP) temperature changes, as well as the coil's sensible heat ratio (SHR). Since the single-speed DX cooling coil model is able to determine the ADP and SHR of a cooling coil at various operating conditions, this same model concept will be used to determine the ADP and SHR of the variable refrigerant flow DX cooling coil.
+
+\subsubsection{Model Description}\label{model-description-9}
+
+The user must input the total cooling capacity and the volumetric air flow rate across the cooling coil at rated conditions. The capacity input should be ``gross'' values, excluding any thermal or energy impacts due to the indoor supply air fan. The rated volumetric air flow should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of rated total cooling capacity (300 -- 450 cfm/ton).
+
+The user is required to input a performance curve in the heat pump object (ref: AirConditioner: VariableRefrigerantFlow) that describes the change in total cooling capacity at various operating conditions (i.e.~at cooling coil inlet air wet-bulb and condenser entering air dry-bulb temperatures different than those used to define total capacity). Each DX cooling coil uses two Cooling Capacity Ratio Modifier curves to define the DX cooling coil performance. The first curve defines the full load performance solely as a function of indoor wet-bulb temperature or uses both indoor wet-bulb temperature and outdoor dry-bulb temperature as the independent variables. The specific performance curves are:
+
+Total cooling capacity modifier curve (function of temperature)
+
+Total cooling capacity modifier curve (function of flow fractionl)
+
+·~~~~~~~~The total cooling capacity modifier curve (function of temperature) defines the performance of the DX cooling coil as a function of operating conditions. These operating conditions may be specified as either a linear, quadratic or cubic equation using coil entering air wet-bulb temperature as the independent variable or as a biquadratic equation using both coil entering air wet-bulb temperature and outdoor dry-bulb temperuate as the independent variables. Since the variable refrigerant flow system modulates the compressor speed to serve the individual cooling coils, the single indpendent variable equation is likely to be sufficient to define the DX cooling coil performance. However, if other more accurate information is available, a biquadratic curve using two independent variables may be used. The output of this curve is multiplied by the rated total cooling capacity to give the total cooling capacity at the specific entering air temperatures at which the DX coil unit is operating (i.e., at temperatures different from the rating point temperatures).
+
+\begin{equation}
+TotCapTempModFac = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d{\left( {{T_{wb,i}}} \right)^3}
+\end{equation}
+
+\begin{itemize}
+\tightlist
+\item
+  or -
+\end{itemize}
+
+\begin{equation}
+TotCapTempModFac = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d\left( {{T_{c,i}}} \right) + e{\left( {{T_{c,i}}} \right)^2} + f\left( {{T_{wb,i}}} \right)\left( {{T_{c,i}}} \right)
+\end{equation}
+
+where
+
+\({{T_{wb,i}}}\) ~ = wet-bulb temperature of the air entering the cooling coil, °C
+
+\({{T_{c,i}}}\) ~ = dry-bulb temperature of the air entering an air-cooled condenser
+
+or wet-bulb temperature of the air entering an evaporative-cooled condenser, °C
+
+The total cooling capacity modifier curve (function of flow fraction) is a linear, quadratic, or cubic curve with the independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the operating (modulated) total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the total cooling capacity at the specific temperature and air flow conditions at which the DX unit is operating. The cubic form of the equation is:
+
+\begin{equation}
+TotCapFlowModFac = \,a + \,b\left( {ff} \right)\,\, + \,\,c{\left( {ff} \right)^2}\,\, + \,\,d{\left( {ff} \right)^3}
+\end{equation}
+
+where
+
+\begin{equation}
+ff = flow{\rm{ }}fraction = \left( {\frac{{Actual{\rm{ }}air{\rm{ }}mass{\rm{ }}flow{\rm{ }}rate}}{{Rated{\rm{ }}air{\rm{ }}mass{\rm{ }}flow{\rm{ }}rate}}} \right)
+\end{equation}
+
+\textbf{Note:}~ The actual volumetric air flow rate through the cooling coil for any simulation time step where the DX unit is operating must be between 0.00002684 m\(^{3}\)/s and .00006713 m\(^{3}\)/s per watt of rated total cooling capacity (200 - 500 cfm/ton). The simulation will issue a warning message if this air flow range is exceeded.
+
+For any simulation time step, the total (gross) cooling capacity of the DX unit is calculated as follows:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{total}} = {\mathop Q\limits^ \bullet_{reference}}\left( {TotCapTempModFac} \right)\left( {TotCapFlowModFac} \right)
+\end{equation}
+
+where
+
+\({\mathop Q\limits^ \bullet_{total}}\) = Total available cooling capacity, W
+
+\({\mathop Q\limits^ \bullet_{reference}}\) = Total reference (rated) cooling capacity, W
+
+In addition to calculating the total cooling capacity provided by the DX cooling coil, it is important to properly determine the break down of total cooling capacity into its sensible (temperature) and latent (dehumidification) components. The model computes the sensible/ latent split using the SHR and ADP/BF approach (Carrier et al. 1959). When the DX coil model is initially called during an EnergyPlus simulation, the rated total capacity and rated SHR are used to calculate the coil bypass factor (BF) at rated conditions. The rated total capacity and rated SHR are first used to determine the ratio of change in air humidity ratio to air dry-bulb temperature:
+
+\begin{equation}
+SlopeRated = {\left( {\frac{{{\omega_{in}} - {\omega_{out}}}}{{{T_{db,in}} - {T_{db,out}}}}} \right)_{rated}}
+\end{equation}
+
+where
+
+\emph{ω\(_{in}\)} = humidity ratio of the air entering the cooling coil at rated conditions, kg/kg
+
+\emph{ω\(_{out}\)} = humidity ratio of the air leaving the cooling coil at rated conditions, kg/kg
+
+\emph{T\(_{db,in}\)} = dry-bulb temperature of the air entering the cooling coil at rated conditions, °C
+
+\emph{T\(_{db,out}\)} = dry-bulb temperature of the air leaving the cooling coil at rated conditions, °C
+
+Along with the rated entering air conditions, the algorithm then searches along the saturation curve of the psychrometric chart until the slope of the line between the point on the saturation curve and the inlet air conditions matches \emph{SlopeRated}. Once this point, the apparatus dew point, is found on the saturation curve the coil bypass factor at rated conditions is calculated as follows:
+
+\begin{equation}
+B{F_{rated}} = \frac{{{h_{out,rated}} - {h_{ADP}}}}{{{h_{in,rated}} - {h_{ADP}}}}
+\end{equation}
+
+where
+
+\emph{h\(_{out,rated}\)} = enthalpy of the air leaving the cooling coil at rated conditions, J/kg
+
+\emph{h\(_{in,rated}\)} = enthalpy of the air entering the cooling coil at rated conditions, J/kg
+
+\emph{h\(_{ADP}\)} = enthalpy of saturated air at the coil apparatus dew point, J/kg
+
+The coil bypass factor is analogous to the ``ineffectiveness'' (1-ε) of a heat exchanger, and can be described in terms of the number of transfer of unit (NTU).
+
+\begin{equation}
+BF = {e^{ - NTU}} = {e^{{{ - \left( {\frac{{UA}}{{{c_p}}}} \right)} \mathord{\left/ {\vphantom {{ - \left( {\frac{{UA}}{{{c_p}}}} \right)} {\dot m}}} \right. } {\dot m}}}} = {e^{ - Ao/\dot m}}
+\end{equation}
+
+For a given coil geometry, the bypass factor is only a function of air mass flow rate. The model calculates the parameter A\(_{o}\) in the equation above based on BF\(_{rated}\) and the rated air mass flow rate. With A\(_{o}\) known, the coil BF can be determined for non-rated air flow rates.
+
+For each simulation time step when the DX cooling coil operates, the total cooling capacity and coil bypass factor at the actual operating conditions are calculated. The coil bypass factor is used to calculate the operating sensible heat ratio (SHR) of the cooling coil using the following equations. Here is where the differnce in models occur for the VRF DX cooling coil and single-speed DX cooling coil. The original coil model (ref: Coil:Cooling:DX:SingleSpeed) calculates the full load outlet air enthalpy and, considering the bypass factor, finds the coil surface temperture (h\(_{ADP}\)) at full load (i.e., PLR = 1). Conversely, the VRF coil model modulates refrigerant flow to the VRF DX cooling coil which is why this model uses the full load coil capacity multipled by the part-load ratio (the modulated refrigerant flow). The effectively finds the coil surface temperature for a variable refrigerant flow DX cooling coil and the operating sensible heat ratio (SHR) can be calculated.
+
+\({h_{ADP}} = {h_{in}} - \frac{{\left( {{{\mathop Q\limits^ \bullet }_{total}}\,\,/\,\mathop m\limits^ \bullet } \right)}}{{1 - BF}}\) ~~~~~~~~~~~ ;~ single-speed DX coil model (h\(_{ADP1}\) in figure below),
+
+\({h_{ADP}} = {h_{in}} - \frac{{\left( {{{\mathop Q\limits^ \bullet }_{total}}\,x\,PLR} \right)\,/\,\mathop m\limits^ \bullet }}{{1 - BF}}\) ~ ;~ variable refrigerant flow DX coil model
+
+\begin{equation}
+SHR = Minimum\left( {\left( {\frac{{{h_{Tin,wADP}} - {h_{ADP}}}}{{{h_{in}} - {h_{ADP}}}}} \right),1} \right)
+\end{equation}
+
+where
+
+\({{h_{in}}}\) ~~~~~~~~ = enthalpy of the air entering the cooling coil, J/kg
+
+\({{h_{ADP}}}\) ~~~~~~ = enthalpy of air at the apparatus dew point condition, J/kg
+
+\({{h_{Tin,wADP}}}\) ~ = enthalpy of air at the entering coil dry-bulb temperature and humidity ratio at ADP, J/kg
+
+\(\dot m\) ~~~~~~~~~~~ = air mass flow rate, kg/s
+
+With the SHR for the coil at the current operating conditions, the properties of the air leaving the cooling coil are calculated using the following equations:
+
+\begin{equation}
+{h_{out}} = {h_{in}} - \left( {\left( {{{\mathop Q\limits^ \bullet  }_{total}}\,xPLR} \right)\,\,/\,\mathop m\limits^ \bullet  } \right)
+\end{equation}
+
+\begin{equation}
+{h_{Tin,\omega out}} = {h_{in}} - \left( {1 - SHR} \right)\left( {{h_{in}} - {h_{out}}} \right)
+\end{equation}
+
+\begin{equation}
+{\omega_{out}} = PsyWFnTdbH\left( {{T_{in}},{h_{Tin,\omega out}}} \right)
+\end{equation}
+
+\begin{equation}
+{T_{db,out}} = PsyTdbFnHW\left( {{h_{out}},{\omega_{out}}} \right)
+\end{equation}
+
+where
+
+\({{h_{out}}}\) ~~~~~~~~ = enthalpy of the air leaving the cooling coil, J/kg
+
+\({{h_{Tin,\omega out}}}\) ~ = enthalpy of air at the entering coil dry-bulb temperature and leaving air humidity ratio, J/kg
+
+\({{\omega_{out}}}\) ~~~~~~~ = leaving air humidity ratio, kg/kg
+
+\({T_{db,out}}\) ~~~ = leaving air dry-bulb temperature, °C
+
+\emph{PsyWFnTdbH} = EnergyPlus psychrometric function, returns humidity ratio given dry-bulb temperature and enthalpy
+
+\emph{PsyTdbFnHW} = EnergyPlus psychrometric function, returns dry-bulb temperature given enthalpy and humidity ratio
+
+The following figure shows this process on a psychrometric chart. This variable refrigerant flow DX cooling coil model follows the dotted process line from h\(_{in}\) towards the outlet air enthalpy (the clear circles, ο) based on the modulated refrigerant flow (PLR). The coil surface temperature (ADP, apparatus dew point) is found by drawing a straight line through these points. The process line from h\(_{in}\) to h\(_{ADP1}\) represents the full load (PLR = 1). This would be what the original DX cooling coil model calculates. At this point the sensible heat ratio is at the design point (assuming h\(_{in}\) is the rating point and the coil operates at the rated air mass flow rate). As the coil load is reduced, the refrigerant flow rate is restricted and the outlet air condition rides up the dotted line. The outlet air condition and associated h\(_{ADP2}\) is shown for a PLR of 0.7 (for example purposes only). Here the sensible heat ratio is higher than that found at full load operation. As the load continues to reduce, the refrigerant flow rate continues to throttle back and there comes a point where the coil's ADP is equal to the inlet air dew point temperature (h\(_{ADP3}\)). At this point, and for all other PLR's less than this value, the coil surface becomes dry (at PLR = 0.4 in this example) and the coil's sensible heat ratio = 1. Between this PLR and PLR = 0, the coil outlet air condition follows the dotted line back towards H\(_{in}\).
+
+\(\cdot\) ~\includegraphics{media/image4182.png}
+
+Figure 180. Process on psychrometric chart
+
+\subsubsection{Dry Coil Conditions}\label{dry-coil-conditions-1}
+
+If the model determines that the cooling coil is dry (ω\(_{in}\) \textless{} ω\(_{ADP}\)), then the equation for total cooling capacity is invalid since it is a function of entering wet-bulb temperature. Under dry-coil conditions, coil performance is a function of dry-bulb temperature rather than wet-bulb temperature. In this case, the model recalculates the performance of the DX cooling unit using the calculation procedure described above but with ω\(_{in\\ =}\) ω\(_{dry,}\) where ω\(_{dry}\) is the inlet air humidity ratio at the coil dry-out point (SHR = 1.0).
+
+\subsubsection{Condenser Options:~ Air Cooled vs.~Evaporative Cooled}\label{condenser-options-air-cooled-vs.evaporative-cooled}
+
+As described previously, this model can simulate the performance of air-cooled or evaporative-cooled DX air conditioners. The choice of condenser type impacts the air dry-bulb temperature entering the heat pump's condenser. Although the actual input for the selection is contained in the variable refrigerant flow air conditioner object, the calculations are repeated here to aid the user in understanding the condenser option choices. The following paragraphs describe three modeling options.
+
+If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) will utilize the outdoor dry-bulb temperature.
+
+If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = EvapCooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) will utilize the outdoor wet-bulb temperature.
+
+If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = EvapCooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) will utilize the condenser inlet air temperature as calculated below:
+
+\begin{equation}
+{T_{c,i}} = \left( {{T_{wb,o}}} \right) + \left( {1 - EvapCondEffectiveness} \right)\left( {{T_{db,o}} - {T_{wb,o}}} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{c,i}\)} = the temperature of the air entering the condenser coil, °C
+
+\emph{T\(_{wb,o}\)} = the wet-bulb temperature of the outdoor air, °C
+
+\emph{T\(_{db,o}\)} = the dry-bulb temperature of the outdoor air, °C
+
+The Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for the variable refrigerant flow air conditioner object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
+
+\subsubsection{Condenser Inlet Air Temperature}\label{condenser-inlet-air-temperature-2}
+
+The air temperature entering the outdoor condenser is based on the weather data used during a simulation. This temperature is either taken directly from the weather data, or can be adjusted based on the height of the outdoor condenser. The input for Condenser Air Inlet Node Name can be used to control this optional feature. If this input is left blank, the air temperature entering the condenser is based solely on the weather data. If this input is not blank, then the node name specified must also be listed in an Outside Air Node or Outside Air Inlet Node List object. When the node name is listed in an Outside Air Inlet Node List object, the air temperature entering the condenser is based solely on the weather data. When the node name is listed in an Outside Air Node object, the height of the node determines the air temperature entering the outdoor condenser (see description of Local Outdoor Air Temperature Calculation in the Atmospheric Variation section of this document for further details).
+
+\subsubsection{Supply Air Fan Control: Cycling vs.~Continuous}\label{supply-air-fan-control-cycling-vs.continuous-2}
+
+One of the inputs to the variable refrigerant flow terminal unit model is the supply air fan operation mode: cycling fan, cycling compressor or continuous fan, cycling compressor. The mode specified in the terminal unit object is passed to the DX cooling coil for use in the model calculations. The first operation mode is frequently referred to as ``AUTO fan'', where the compressor(s) and supply air fan operate in unison to meet the zone cooling load, and cycle off together when the cooling load has been met. The second operation mode is often referred to as ``fan ON'', where the compressor(s) cycle on and off to meet the zone cooling load but the supply air fan operates continuously regardless of compressor operation.
+
+The fan operation mode schedule value determines the fan operation mode for each time step throughout the simulation. A fan operation mode schedule value of 0 specifies AUTO fan mode operation while values other than 0 specify fan ON operation. The use of a schedule allows the fan operation mode to change based on time-of-day or with changes in season.
+
+The EnergyPlus methodology for determining the impact that HVAC equipment has on an air stream is to calculate the mass flow rate and air properties (e.g., enthalpy, dry-bulb temperature, humidity ratio) exiting the equipment. These exiting conditions are passed along as inlet conditions to the next component model in the air stream. Eventually the flow rate and properties of the air being supplied to the conditioned zone are used in the zone energy balance to determine the resulting zone air temperature and humidity ratio.
+
+With this methodology, the determination of the air mass flow rate and air properties for the two different supply air fan operation modes is slightly different. For the case of cycling fan/cycling compressor, the conditions of the air leaving the cooling coil are the steady-state values calculated using the equations described above. However the air mass flow rate passed along to the next component (and eventually to the conditioned zone) is the average air mass flow rate for the system simulation time step.
+
+For the case of continuous fan/cycling compressor, the air mass flow rate is constant. However, the air properties leaving the cooling coil are calculated as the average conditions during the system simulation time step. The model assumes that the exiting air conditions are the steady-state values calculated using the equations described above when the heat pump operates.~ For the remainder of the system simulation time step, it is assumed that the air exiting the DX coil has the same properties as the air entering the coil. For this supply air fan operating strategy, the leaving air properties are calculated as follows:
+
+\begin{equation}
+{h_{out,\,ContFanCycComp}} = {h_{out}}\left( {CyclingRatio} \right) + {h_{in}}\left( {1 - CyclingRatio} \right)
+\end{equation}
+
+\begin{equation}
+{\omega_{out,\,ContFanCycComp}} = {\omega_{out}}\left( {CyclingRatio} \right) + {\omega_{in}}\left( {1 - CyclingRatio} \right)
+\end{equation}
+
+\begin{equation}
+{T_{db,out,ContFanCycComp}} = PsyTdbFnHW\left( {{h_{out,ContFanCycComp}},{\omega_{out,ContFanCycComp}}} \right)
+\end{equation}
+
+\subsubsection{Average Air Flow Calculations}\label{average-air-flow-calculations}
+
+The variable refrigerant flow (VRF) terminal unit operates based on user-specified (or autosized) air flow rates. The VRF terminal unit's supply air flow rate during cooling operation may be different than the supply air flow rate during heating operation. In addition, the supply air flow rate when no cooling or heating is required but the supply air fan remains ON can be different than the air flow rates when cooling or heating is required. The outside air flow rates can likewise be different for cooling and heating operating modes. The model takes these different flow rates into account when modeling the heat pump, and the average air flow rate for each simulation time step is reported on the inlet/outlet air nodes of the various terminal unit components in proportion to the calculated cycling ratio of the coil.
+
+The average supply air and outdoor air mass flow rates through the heat pump for the HVAC simulation time step are calculated based on the cycling ratio of the DX cooling coil or heating coil (whichever coil is operating) as follows:
+
+\begin{equation}
+\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\,\, = \,\,\mathop m\limits^ \bullet  {\,_{SA,coil\,\,on}}\left( {CyclingRatio} \right) + \mathop m\limits^ \bullet  {\,_{SA,\,\,coil\,\,off}}\left( {1 - CyclingRatio} \right)
+\end{equation}
+
+\begin{equation}
+\mathop m\limits^ \bullet  {\,_{OA,\,\,avg\,\,}} = \,\,\mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,on}}\left( {CyclingRatio} \right) + \mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,off}}\left( {1 - CyclingRatio} \right)
+\end{equation}
+
+where:
+
+\(\mathop m\limits^ \bullet {\,_{SA,\,\,avg}}\) ~~~~~ = average supply air mass flow rate during the time step, kg/s
+
+\(\mathop m\limits^ \bullet {\,_{SA,coil\,\,on}}\) ~~ = supply air mass flow rate when the coil is ON, kg/s
+
+\emph{CyclingRatio}~ = cycling ratio of the coil (heating or cooling)
+
+\(\mathop m\limits^ \bullet {\,_{SA,\,\,coil\,\,off}}\) ~ = supply air mass flow rate when the coil is OFF, kg/s
+
+\(\mathop m\limits^ \bullet {\,_{OA,\,\,avg\,\,}}\) ~~~~ = average outside air mass flow rate during the time step, kg/s
+
+\(\mathop m\limits^ \bullet {\,_{OA,\,\,coil\,\,on}}\) ~ = average outside air mass flow rate when the coil is ON, kg/s
+
+\(\mathop m\limits^ \bullet {\,_{OA,\,\,coil\,\,off}}\) = average outside air mass flow rate when the coil is OFF, kg/s
+
+The supply air and outside air flow rates when the DX cooling or DX heating coil is ON are specified by the user (e.g., supply air volumetric flow rate during cooling operation, supply air volumetric flow rate during heating operation, outside air volumetric air flow rate during cooling operation, and outside air volumetric air flow rate during heating operation) and are converted from volumetric to mass flow rate. If the user has specified cycling fan operation, then the supply air and outside air mass flow rates when the coil is OFF are zero. If the user has specified constant fan operation, then the user-defined air flow rates when no cooling or heating is needed are used when the coil is OFF.
+
+There is one special case. If the user has specified constant fan operation and they specify that the supply air volumetric flow rate when no cooling or heating is needed is zero (or field is left blank), then the model assumes that the supply air and outside air mass flow rates when the coil is OFF are equal to the corresponding air mass flow rates when the coil was last operating (ON).
+
+\subsection{Variable Refrigerant Flow Heating Coil}\label{variable-refrigerant-flow-heating-coil}
+
+The variable refrigerant flow (VRF) DX heating coil model uses performance information at rated conditions along with performance curves for variations in total capacity, energy input ratio and part load fraction to determine performance at part-load conditions. The impacts of defrost operation is modeled based a combination of user inputs and empirical models taken from the air-to-air heat pump algorithms in DOE-2.1E. The VRF DX heating coil model is very similar to the DX heating coil model used in the single-speed heat pump. The only difference being that the energy performance curves were moved to the parent object (Ref. AirConditioner:VariableRefrigerantFlow). See the DX Heating Coil model description for further details.
+
+\subsection{Variable Speed Water to Air Heat Pump (Heating \& Cooling)}\label{variable-speed-water-to-air-heat-pump-heating-cooling}
+
+\subsubsection{Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit}\label{coilheatingwatertoairheatpumpvariablespeedequationfit}
+
+\subsubsection{Overview}\label{overview-13}
+
+A Variable Speed Water Source Heat Pump (let's call it VS WSHP) has a system control which dictates the refrigerant flow rate, the design unit supply airflow and the required water flow rate at each compressor speed. The air and water flow rates are usually a function of the compressor speed. Refrigerant mass flow rate is a function of compressor speed as well as entering water temperature and indoor dry bulb or wet bulb. The control system adjusts the equipment capacity based on zone temperature measurements relative to the thermostat set point. The control logic determines what compressor speed is required to control to the zone temperature requirement in response to increased or decreased capacity (heating or cooling load). The compressor, fan and pump speeds are not discrete values and can be considered to vary infinitesimally between the minimum and maximum compressor speed. At the minimum compressor speed (which is different for heating and cooling), for a continuous fan, the supply airflow is fixed and the unit will have to cycle for reduced part loads below this point. For a cycling fan, the fan will cycle with the compressor.
+
+Present EnergyPlus is capable of modeling multiple-speed DX air-to-air coils. The number of speed levels is up to four. In some cases, four sets of performance curves are not sufficient to include all the information for a variable speed equipment. There is a need to expand the space for containing more performance curves. Here, we expand the number of speed levels and the corresponding curve sets up to ten. The number of speed levels is selectable by the user. The user can provide speed levels at any number from 2 to 10. In any case, our model would just do linear interpolation between neighboring speeds. The more curves, the more accurate. Furthermore, using linear interpolation and inputting air and water flow rates at individual speed levels facilitates arbitrary relationships of flow rates as a function of the compressor speed level.
+
+This model (object name Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit) simulates the performance of a variable-speed water-to-air heat pump with heating capability. It fits in the parent objects of \emph{AirLoopHVAC:UnitaryHeatPump:WaterToAir} and \emph{ZoneHVAC:WaterToAirHeatPump}. The rated conditions for obtaining the Reference Unit total heating capacities and COPs~ are indoor dry-bulb temperature at 21.1 ËšC (70 ËšF) and the source side entering water temperature at 21.1 ËšC (70 ËšF).
+
+\subsubsection{Model Description}\label{model-description-10}
+
+The Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit object is modeled in a manner similar to the multi-speed DX heating coil model (Ref. Coil:Heating:DX:MultiSpeed). Of course, rather than referencing an air source evaporator or defrost object, the new coil object references to the water loop, and has the entering water temperature in place of the indoor air entering dry bulb temperature.
+
+It shall be noted for the capacity and flow rate inputs, three fields are autosizable, which are Rated Heating Capacity at the Selected Nominal Speed Level (Numeric Field 3), Rated Volumetric Air Flow Rate (Numeric Field 4) and Rated Volumetric Water Flow Rate (Numeric Field 5). They are used to scale the performances of a specific unit and correlate with the actual loop flows. Except these three fields, all other capacity and flow rate inputs at individual speed levels should be directly obtained from Reference Unit catalog data, specific to an actual unit.
+
+The Rated Heating Capacity at Selected Nominal Speed Level contains the rated capacity to match the building heating load at the design day.~ The rated heating capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
+
+{\scriptsize
+\begin{equation}
+CapacityScaleFactor = \frac{{RatedTotalHeatingCapacity}}{{ReferenceUnitTotalHeatingCapacity@NominalSpeedLevel}}
+\end{equation}}
+
+And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below:
+
+RatedTotalHeatingCapacity@SpeedLevel(x) = CapacityScaleFactor * ReferenceUnitTotalHeatingCapacity@SpeedLevel(x)
+
+The Rated Volumetric Air Flow Rate is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects, as follows:
+
+{\scriptsize
+\begin{equation}
+AirFlowScaleFactor = \frac{{RatedVolumetricAirFlowRate}}{{ReferenceUnitVolAirFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}
+\end{equation}}
+
+And the loop volumetric air flow rates at various speed levels in the parent objects are calculated as below:
+
+LoopVolumetricAirFlowRate@SpeedLevel(x) = AirFlowScaleFactor * ReferenceUnitVolAirFlowRate@SpeedLevel(x) * CapacityScaleFactor
+
+If the volumetric air flow rate at one speed level is higher than the flow rate allowed by the fan in the parent object, the flow rate will be set back to the fan flow rate.
+
+This Rated Volumetric Water Flow Rate is used to determine an internal scaling factor, and calculate the loop water flow rates.
+
+{\scriptsize
+\begin{equation}
+WaterFlowScaleFactor = \frac{{RatedVolumetricWaterFlowRate}}{{ReferenceUnitVolWaterFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}
+\end{equation}}
+
+And the required volumetric water flow rates in the parent objects are calculated as below,
+
+LoopVolumetricWaterFlowRate@SpeedLevel(x) = WaterFlowScaleFactor * ReferenceUnitWaterVolFlowRate@SpeedLevel(x) * CapacityScaleFactor
+
+The required volumetric water flow rate as above should be restricted by the pump in the water loop.
+
+If \(AirFlowScaleFactor\) ~and \(WaterFlowScaleFactor\) ~equal unity, the loop flow rates become the design flow rates of the Reference Unit (after scaled by the rated heating capacity). The Rated Volumetric Air Flow Rate and Rated Volumetric Water Flow Rate are introduced here to correlate with the actual flow rates in the air and water loops, in case that these differ from the design specification. Certainly, it is recommended that the Rated Volumetric Air Flow Rate and Rated Volumetric Water Flow Rate are selected in the way that \(AirFlowScaleFactor\) ~and \(WaterFlowScaleFactor\) ~are unity, so as to get more accurate results from the performance curves.
+
+Performance curves:
+
+This object includes 7 curve objects at each individual speed level.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  ~Total heating capacity modifier curve (function of temperature).
+\item
+  ~Total heating capacity modifier curve (function of air flow fraction).
+\item
+  ~Total heating capacity modifier curve (function of water flow fraction).
+\item
+  ~Energy input ratio (EIR) modifier curve (function of temperature).
+\item
+  ~Energy input ratio (EIR) modifier curve (function of air flow fraction).
+\item
+  ~Energy input ratio (EIR) modifier curve (function of water flow fraction).
+\item
+  Recoverable heat modifier as a function of indoor air dry-bulb and water entering temperatures.
+\end{enumerate}
+
+Curves 3) and 6) are new curves as compared to those used for Multi-Speed Electric DX Air Heating Coil, as to correlate the change in water flow rate at the speed. The flow fraction modifier curves are used as a placeholder, to account for off-design flow rates if needed. If the manufacturer doesn't provide off-design performances, we can simply use a default modification multiplier of 1.0.
+
+At the lowest speed, there will be one additional performance curve to account for the part-load condition, i.e.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{7}
+\item
+  ~Part load fraction correlation (function of part load ratio)
+\item
+  Total heating capacity modifier curve (function of temperature)
+\end{enumerate}
+
+The total heating capacity modifier as a function of temperature curve (CAP-FT) is a biquadratic curve with two independent variables: dry-bulb temperature of the air entering the heating coil and the VS WSHP's entering water temperature. The output of this curve is multiplied by the rated total heating capacity at the speed, to give the total heating capacity at the specific entering air and water temperatures at which the WSHP unit is operating (i.e., at temperatures different from the rating point temperatures).
+
+\begin{equation}
+TotCapTempModFac = a + b*D{B_i} + c*DB_i^2 + d*EWT + e*EW{T^2} + f*D{B_i}*EWT
+\end{equation}
+
+where
+
+DB\(_{i}\) = dry-bulb temperature of the air entering the heating coil, °C
+
+EWT = entering water temperature, °C
+
+a-f = regression curve-fit coefficients
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Total heating capacity modifier curve (function of air flow fraction)
+\end{enumerate}
+
+\begin{equation}
+TotCapAirFlowModFac = a + b*f{f_a} + c*ff_a^2 + d*ff_a^3
+\end{equation}
+
+where
+
+ff\(_{a}\) = actual air mass flow rate/design air mass flow rate, at one speed level;
+
+DesignAirMassFlowRate@SpeedLevel(x) = ReferenceUnitAirMassFlowRate@SpeedLevel(x) * CapacityScaleFactor
+
+a-d = regression curve-fit coefficients, if no data available for the correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Total heating capacity modifier curve (function of water flow fraction)
+\end{enumerate}
+
+\begin{equation}
+TotCapWaterFlowModFac = a + b*f{f_w} + c*ff_w^2 + d*ff_w^3
+\end{equation}
+
+where
+
+ff\(_{w}\) = actual water mass flow rate/design water mass flow rate, at one speed level;
+
+DesignWaterMassFlowRate@SpeedLevel(x) = ReferenceUnitWaterMassFlowRate@SpeedLevel(x) * CapacityScaleFactor
+
+a-d = regression curve-fit coefficients, if no data available for the correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Energy input ratio (EIR) modifier curve (function of temperature)
+\end{enumerate}
+
+The energy input ratio modifier curve as a function of temperature (EIR-FT) is a biquadratic curve with two independent variables: dry-bulb temperature of the air entering the heating coil and the WSHP's entering water temperature. The output of this curve is multiplied by the rated EIR at the speed (inverse of the rated COP), to give the EIR at the specific entering air and water temperatures at which the WSHP coil unit is operating (i.e., at temperatures different from the rating point temperatures).
+
+\begin{equation}
+EIRTempModFac = a + b*D{B_i} + c*DB_i^2 + d*EWT + e*EW{T^2} + f*D{B_i}*EWT
+\end{equation}
+
+where
+
+DB\(_{i}\) = dry-bulb temperature of the air entering the heating coil, °C
+
+EWT = entering water temperature, °C
+
+a-f = regression curve fit coefficients.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{4}
+\tightlist
+\item
+  Energy input ratio (EIR) modifier curve (function of air flow fraction)
+\end{enumerate}
+
+\begin{equation}
+EIRAirFlowModFac = a + b*f{f_a} + c*ff_a^2 + d*ff_a^3
+\end{equation}
+
+where
+
+a-d = regression curve-fit coefficients, if no data available for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{5}
+\tightlist
+\item
+  Energy input ratio (EIR) modifier curve (function of water flow fraction)
+\end{enumerate}
+
+\begin{equation}
+EIRWaterFlowModFac = a + b*f{f_w} + c*ff_w^2 + d*ff_w^3
+\end{equation}
+
+where
+
+a-d = regression curve fit coefficients, if no data available for the correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{6}
+\tightlist
+\item
+  Recoverable heat modifier as a function of indoor dry-bulb and water entering temperatures.
+\end{enumerate}
+
+Recoverable heat modifier function accounts for the recoverable waste heat at the condensing side, as a fraction to the input power. This part of heat doesn't added to the supply side.
+
+\begin{equation}
+WasteHeatTempModFac = a + b*D{B_i} + c*DB_i^2 + d*EWT + e*EW{T^2} + f*D{B_i}*EWT
+\end{equation}
+
+where
+
+a-f = regression curve-fit coefficients.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{7}
+\tightlist
+\item
+  Part load fraction correlation (function of part load ratio)
+\end{enumerate}
+
+This field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, heating load/steady-state heating capacity for Speed 1),
+
+\begin{equation}
+PartLoadFrac = a + b*PLR + c*PL{R^2} + d*PL{R^3}
+\end{equation}
+
+And
+
+RTF = (PLR/PartLoadFrac) = runtime fraction of the heating coil
+
+The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor runs continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, the runtime fraction of the coil is limited to 1.0. A typical part load fraction correlation would be:
+
+\begin{equation}
+{\rm{PLF}} = 0.85 + 0.15 \times {\rm{PLR}}
+\end{equation}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{equation}
+{\rm{PLF}} = 0.85 + 0.0 \times {\rm{PLR}}
+\end{equation}
+
+Lowest Speed Operation:
+
+The lowest speed operation of the VS WSHP is similar to the single speed DX heating coil. The total (gross) heating capacity of the WSHP unit is calculated as follows:
+
+\(\begin{array}{l}{Q_{total,1}} = RatedTotalHeatingCapacity@SpeedLevel\left( 1 \right)\\\quad \quad \quad *TotCapTemModFa{c_1}\\\quad \quad \quad *TotCapAirFlowModFa{c_1}\\\quad \quad \quad *TotCapWaterFlowModFa{c_1}\end{array}\) \emph{~}
+
+And the EIR is calculated as:
+
+\begin{equation}
+  \begin{array}{rl}
+    EIR_1 &= \frac{1.0}{\rm{ReferenceUnitCOP@Speed(1)}} \cdot EIRTempModFac_1 \\
+          &* EIRAirFlowModFac_1 \\
+          &* EIRWaterFlowModFac_1
+  \end{array}
+\end{equation}
+
+And the power consumption including the compressor and accessories (not including pump and indoor fan powers) is,
+
+\begin{equation}
+Powe{r_1} = {Q_{total,1}}*EI{R_1}*RTF
+\end{equation}
+
+The waste heat generated by this coil object is calculated as:
+
+\begin{equation}
+  \begin{array}{rl}
+    Q_{RecoverHeat,1} &= \rm{ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel(1)} \\
+                      &* Power_1 * WasteHeatTempModFac_1
+  \end{array}
+\end{equation}
+
+where
+
+\(ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( 1 \right)\) ~ = waste heat fraction of the energy input at Speed 1, from the Reference Unit data.
+
+The total amount of heat absorbed by the evaporator is calculated as:
+
+\begin{equation}
+{\rm{Q}}{{\rm{}}_{evap,1}} = {Q_{total,1}} + {\rm{}}{Q_{RecoverHeat,1}} - Powe{r_1}
+\end{equation}
+
+The fraction of the actual air mass flow to the design air mass flow rate is calculated:
+
+\begin{equation}
+\begin{split}
+  ff_{a,1} = actualairmassflowrate/(ReferenceUnitAirMassFlowRate@SpeedLevel(1) \\
+  *CapacityScaleFactor)
+\end{split}
+\end{equation}
+
+The fraction of the actual water mass flow to the design water mass flow rate is calculated:
+
+\begin{equation}
+\begin{split}
+  ff_{w,1} = actualwatermassflowrate/(ReferenceUnitWaterMassFlowRate@SpeedLevel(1) \\
+  *CapacityScaleFactor)
+\end{split}
+\end{equation}
+
+Higher Speed Operation:
+
+At the speed level between the lowest and the highest, there is no part-load loss. A parameter of speed ratio (SpeedRatio) is used to define the capacity partition between Speed x-1 and Speed x.
+
+The design air and water flow rate at the speed ratio are given as following:
+
+\begin{equation}
+  \begin{array}{rl}
+  DesignAirFlowRateSpeedRatio &= ReferenceUnitAirMassFlowRate@SpeedLevel\left( {x - 1} \right) \\
+                              &* CapacityScaleFactor \\
+                              &* \left(1-SpeedRatio\right) \\
+                              &+ ReferenceUnitAirMassFlowRate@SpeedLevel\left( x \right) \\
+                              &* CapacityScaleFactor \\
+                              &* SpeedRatio
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    DesignWaterFlowRateSpeedRatio &= ReferenceUnitWaterMassFlowRate@SpeedLevel\left( {x - 1} \right) \\
+                                  &* CapacityScaleFactor \\
+                                  &* \left(1-SpeedRatio\right) \\
+                                  &+ ReferenceUnitWaterMassFlowRate@SpeedLevel\left( x \right) \\
+                                  &* CapacityScaleFactor \\
+                                  &* SpeedRatio
+  \end{array}
+\end{equation}
+
+And the fractions of air flow and water flow are given:
+
+\(f{f_{a,x - 1}}\) = \(f{f_{a,x}}\) = actual air mass flow rate/DesignAirFlowRateSpeedRatio
+
+\(f{f_{w,x - 1}}\) = \(f{f_{w,x}}\) = actual water mass flow rate/DesignWaterFlowRateSpeedRatio
+
+The total heating capacities and EIRs at Speed x-1 and Speed x are given:
+
+\begin{equation}
+  \begin{array}{rl}
+    Q_{total,x - 1} &= RatedTotalHeatingCapacity@SpeedLevel\left( {x - 1} \right) \\
+                    &* TotCapTempModFac_{x - 1} \\
+                    &* TotCapAirFlowModFac_{x - 1} \\
+                    &* TotCapWaterFlowModFac_{x - 1}
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    Q_{total,x} &= RatedTotalHeatingCapacity@SpeedLevel\left( x \right) \\
+                &* TotCapTempModFac_x \\
+                &* TotCapAirFlowModFac_x \\
+                &* TotCapWaterFlowModFac_x 
+ \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    EIR_{x - 1} &= \frac{1.0}{ReferenceUnitCOP@Speed(x - 1)} \\
+                &* EIRTempModFac_{x - 1} \\
+                &* EIRAirFlowModFac_{x - 1} \\
+                &* EIRWaterFlowModFac_{x - 1}
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    EIR_x &= \frac{1.0}{ReferenceUnitCOP@Speed(x)} \\
+                &* EIRTempModFac_{x} \\
+                &* EIRAirFlowModFac_{x} \\
+                &* EIRWaterFlowModFac_{x}
+  \end{array}
+\end{equation}
+
+The total heating capacity at the corresponding speed ratio is:
+
+\begin{equation}
+{Q_{total,SpeedRatio}} = \left( {1.0 - SpeedRatio} \right)*{Q_{total,x - 1}} + SpeedRatio*{Q_{total,x}}
+\end{equation}
+
+And the power consumption is
+
+\begin{equation}
+Powe{r_{SpeedRatio}} = \left( {1.0 - SpeedRatio} \right)*{Q_{total,x - 1}}*EI{R_{x - 1}} + SpeedRatio*{Q_{total,x}}*EI{R_x}
+\end{equation}
+
+The waste heat generated by this coil object is calculated as:
+
+\begin{equation}
+  \begin{array}{rl}
+    Q_{RecoverHeat,SpeedRatio} &= \left( 1.0 - SpeedRatio \right) \\
+                               &* ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( {x - 1} \right) \\
+                               &* WasteHeatTempModFac_{x - 1} * Q_{total,x - 1} * EIR_{x - 1} \\
+                               &+ SpeedRatio \\
+                               &* ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( x \right) \\
+                               &* WasteHeatTempModFac_x \\
+                               &* Q_{total,x} * EIR_x
+  \end{array}
+\end{equation}
+
+The total amount of heat absorbed by the evaporator is calculated as:
+
+\begin{equation}
+{Q_{evap,SpeedRatio}} = {Q_{total,SpeedRatio}} + {\rm{}}{Q_{RecoverHeat,SpeedRatio}} - Powe{r_{SpeedRatio}}
+\end{equation}
+
+At last,
+
+\begin{equation}
+{Q_{total,SpeedRatio}} = HeatingLoad
+\end{equation}
+
+If the speed reaches the highest level, the speed ratio becomes 1.0, and Speed x represents the highest speed.
+
+\subsubsection{Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit}\label{coilcoolingwatertoairheatpumpvariablespeedequationfit}
+
+\subsubsection{Overview}\label{overview-14}
+
+This model (object name Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit) simulates the performance of an variable-speed water-to-air heat pump with cooling capability. It fits in the parent objects of \emph{AirLoopHVAC:UnitaryHeatPump:WaterToAir} and \emph{ZoneHVAC:WaterToAirHeatPump}. It has the same logic for varying the compressor, indoor fan and pump speeds as the \emph{Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit} object. The rated conditions for obtaining the capacities, COPs and SHR~ are indoor dry-bulb temperature at 26.67 ËšC (80 ËšF), wet bulb temperature at 19.44 ËšC (67 ËšF),~ and the source side entering water temperature at 29.4 ËšC (85 ËšF).
+
+Variable-speed cooling coils lead to varied dehumidification behaviors, that the Bypass Factor (BF) is not only dependent on the indoor air flow rate, but also on the refrigerant mass flow rate, i.e.~the compressor speed. It is necessary to assess the BF approach for single-speed DX coil, to be used for the variable-speed systems.
+
+TheDOE/ORNL Heat Pump Design Model(HPDM) is a steady-state vapor compression equipment simulation model, which is able to simulate the performance of a VS WSHP system. We rana calibrated HPDM model to produce performance data of a 2.5-ton, VS WSHPunit in space cooling mode. We ran the model to get the total cooling capacities and SHRs, by specifying the EWT at 65˚F, indoor air DB at 80˚F and relative humidity at 0.5, and then varying the indoor air flow rate from 400 scfm to 1000 scfm, the compressor speed from 30 HZ to 90 HZ in a 7×7 matrix. Based on the performance results, we used EES (Engineering Equation Solver) to back-calculate the corresponding BF factors and the A\(_{o}\) (effective coil surface area) parameters,using the BF equations for the single speed DX cooling coil in EnergyPlus Engineering Reference.
+
+And then, we plotted the resultant A\(_{o}\) as a function of indoor air flow rate and compressor speed, as below:
+
+\begin{figure}[hbtp] % fig 181
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4240.svg.png}
+\caption{Effective Surface Area (Ao) Changing with Compressor Speed and Indoor SCFM \protect \label{fig:effective-surface-area-ao-changing-with}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 182
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4241.svg.png}
+\caption{Bypass Factor (BF) Changing with Compressor Speed and Indoor SCFM \protect \label{fig:bypass-factor-bf-changing-with-compressor}}
+\end{figure}
+
+As indicated in the two figures above, the compressor speed is a significant factor impacting the A\(_{o}\) parameter and the BF factor. So, the current BF factor approach should be upgraded to accommodate variable-speed cooling coils.
+
+As shown in the A\(_{o}\) figure, we can almost assume that the A\(_{o}\) parameter mainly depends on the compressor speed. And thus, for enhancing the VS WSHP model, in the IDF file, we need to input SHRs at individual compressor speeds (this is similar to the current multi-speed DX cooling coil). And then, within the VS WSHP module, we calculate the A\(_{o}\) parameter specific to each compressor speed at the design air flow rates, and then do linear interpolation of A\(_{o}\) between neighboring compressor speeds. For calculating SHRs in energy simulations, we first calculate the A\(_{o}\) parameter related to the actual compressor speed, and then use the simulated A\(_{o}\) parameter in the original BF correlation to correlate effect of the varied indoor air flow rate.
+
+\subsubsection{Model Description}\label{model-description-11}
+
+The Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit object is modeled in a manner similar to the multiple-speed DX cooling coil model (Ref. Coil:Cooling:DX:MultiSpeed). Of course, rather than referencing an air-cooled condenser, the new coil object references the water loop, and have the water entering temperature in place of the condenser air entering dry bulb temperature.
+
+It shall be noted for the total cooling capacity and flow rate inputs, three fields are autosizable, which are Rated Total Cooling Capacity (Numeric Field 3) at Selected Nominal Speed Level, Rated Volumetric Air Flow Rate (Numeric Field 4) ~and Rated Volumetric Water Flow Rate (Numeric Field 5). They are used to scale the performances of an actual unit and correlate with the actual loop flows. Except the three fields, all other total cooling capacity and flow rate inputs at individual speed levels should be directly obtained from Reference Unit catalog data, specific to an actual unit.
+
+The Rated Total Cooling Capacity at Selected Nominal Speed Level contains the rated total cooling capacity to match the building sensible or latent cooling load.~ The rated cooling capacity is used to determine a capacity scaling factor, as compared to the Reference Unit catalog capacity at the nominal speed level.
+
+\begin{equation}
+CapacityScaleFactor = \frac{{RatedTotalCoolingCapacity}}{{ReferenceUnitTotalCoolingCapacity@NominalSpeedLevel}}
+\end{equation}
+
+And then, this scaling factor is used to determine capacities at rated condition for other speed levels, as below,
+
+\begin{equation}
+\begin{split}
+  RatedTotalCoolingCapacity@SpeedLevel(x) = CapacityScaleFactor \\
+  * ReferenceUnitTotalCoolingCapacity@SpeedLevel(x)
+\end{split}
+\end{equation}
+
+The Rated Volumetric Air Flow Rate is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects, as follows:
+
+{\scriptsize
+\begin{equation}
+  AirFlowScaleFactor = \frac{RatedVolumetricAirFlowRate}{ReferenceUnitVolAirFlowRate@NominalSpeedLevel * CapacityScaleFactor}
+\end{equation}}
+
+And the loop volumetric air flow rates in the parent objects are calculated as below,
+
+\begin{equation}
+\begin{split}
+  LoopVolumetricAirFlowRate@SpeedLevel\left( x \right) = AirFlowScaleFactor \\
+  * ReferenceUnitVolAirFlowRate@SpeedLevel(x) * CapacityScaleFactor
+\end{split}
+\end{equation}
+
+If the volumetric air flow rate at one speed level is higher than the flow rate allowed by the fan in the parent object, the flow rate will be set back to the fan flow rate.
+
+This Rated Volumetric Water Flow Rate is used to determine an internal scaling factor, and calculate the loop water flow rates.
+
+{\scriptsize
+\begin{equation}
+  WaterFlowScaleFactor = \frac{{RatedVolumetricWaterFlowRate}}{{ReferenceUnitVolWaterFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}
+\end{equation}}
+
+And the required volumetric water flow rates in the parent objects are calculated as below,
+
+\begin{equation}
+\begin{split}
+  LoopVolumetricWaterFlowRate@SpeedLevel\left( x \right) = WaterFlowScaleFactor \\
+  * ReferenceUnitVolWaterFlowRate@SpeedLevel(x) * CapacityScaleFactor
+\end{split}
+\end{equation}
+
+The required volumetric water flow rate as above is restricted by the pump in the parent object.
+
+If \(AirFlowScaleFactor\) ~and \(WaterFlowScaleFactor\) ~are equal to unity, the loop flow rates become the design flow rates of the original unit (after scaled by the rated total cooling capacity). The Rated Volumetric Air Flow Rate and Rated Volumetric Water Flow Rate are introduced here to correlate with the actual flow rates in the air and water loops, in case that these differ from the design specifications. Certainly, it is recommended that the Rated Volumetric Air Flow Rate and Rated Volumetric Water Flow Rate are selected in the way that \(AirFlowScaleFactor\) ~and \(WaterFlowScaleFactor\) ~are unity, so as to get more accurate results from the performance curves.
+
+Performance Curves:
+
+This object includes 7 curve objects at each individual speed level.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  ~Total cooling capacity modifier curve (function of temperature)
+\item
+  ~Total cooling capacity modifier curve (function of air flow fraction)
+\item
+  ~Total cooling capacity modifier curve (function of water flow fraction)
+\item
+  ~Energy input ratio (EIR) modifier curve (function of temperature)
+\item
+  ~Energy input ratio (EIR) modifier curve (function of air flow fraction)
+\item
+  ~Energy input ratio (EIR) modifier curve (function of water flow fraction)
+\item
+  Recoverable heat modifier as a function of indoor air wet-bulb and water entering temperatures.
+\end{enumerate}
+
+Curves 3) and 6) are new curves as compared to those used for Multi-Speed Electric DX Air Cooling Coil, to correlate the change in water flow rate at the speed. The flow fraction modifier curves are used as a placeholder, to account for off-design flow rates if needed. If the manufacturer doesn't provide the off-design performances, we can simply use a default modification multiplier of 1.0.
+
+At the lowest speed, there will be one additional performance curve to correlate the part-load condition, i.e.
+
+\textbf{8)} Part load fraction correlation (function of part load ratio)
+
+1)~~~~~Total cooling capacity modifier curve (function of temperature)
+
+The total cooling capacity modifier as a function of temperature curve (CAP-FT) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil and the WSHP's entering water temperature. The output of this curve is multiplied by the rated total cooling capacity at the speed, to give the total cooling capacity at the specific entering air WB and water temperatures at which the WSHP unit is operating (i.e., at temperatures different from the rating point temperatures).
+
+Note: The data used to develop the total cooling capacity modifier curve (function of temperature) should represent performance when the cooling coil is `wet' (i.e., coil providing sensible cooling and at least some dehumidification). Performance data when the cooling coil is `dry' (i.e., not providing any dehumidification) should not be included when developing this modifier curve. This model automatically detects and adjusts for `dry coil' conditions.
+
+\begin{equation}
+TotCapTempModFac = a + b*W{B_i} + c*WB_i^2 + d*EWT + e*EW{T^2} + f*W{B_i}*EWT
+\end{equation}
+
+where
+
+WB\(_{i}\) = wet-bulb temperature of the air entering the heating coil, °C
+
+EWT = entering water temperature, °C
+
+a-f = regression curve-fit coefficients.
+
+2)~~~~~Total cooling capacity modifier curve (function of air flow fraction)
+
+The total cooling capacity modifier curve (function of air flow fraction) is a cubic curve with the independent variable being the ratio of the actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of design flow at the speed).
+
+\begin{equation}
+TotCapAirFlowModFac = a + b*f{f_a} + c*ff_a^2 + d*ff_a^3
+\end{equation}
+
+where
+
+ff\(_{a}\) = actual air mass flow rate/design air mass flow rate, at one speed level;
+
+\begin{equation}
+\begin{split}
+  DesignAirMassFlowRate@SpeedLevel(x) = ReferenceUnitAirMassFlowRate@SpeedLevel(x) \\
+  * CapacityScaleFactor
+\end{split}
+\end{equation}
+
+a-d = regression curve fit coefficients, if no data for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+3)~~~~~Total cooling capacity modifier curve (function of water flow fraction)
+
+The total cooling capacity modifier curve (function of water flow fraction) is a cubic curve with the independent variable being the ratio of the actual water flow rate across the water-to-refrigerant heat exchanger to the design water flow rate (i.e., fraction of design flow at the speed).
+
+\begin{equation}
+TotCapWaterFlowModFac = a + b*f{f_w} + c*ff_w^2 + d*ff_w^3
+\end{equation}
+
+where
+
+ff\(_{w}\) = actual water mass flow rate/design water mass flow rate, at one speed level;
+
+\begin{equation}
+\begin{split}
+  DesignWaterMassFlowRate@SpeedLevel(x) = ReferenceUnitWaterMassFlowRate@SpeedLevel(x) \\
+  * CapacityScaleFactor
+\end{split}
+\end{equation}
+
+a-d = regression curve-fit coefficients, if no data available for the correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Energy input ratio (EIR) modifier curve (function of temperature)
+\end{enumerate}
+
+The energy input ratio modifier curve as a function of temperature (EIR-FT) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil and the WSHP's entering water temperature. The output of this curve is multiplied by the rated EIR (inverse of the rated COP) at the speed level, to give the EIR at the specific entering air and water temperatures at which the WSHP unit is operating (i.e., at temperatures different from the rating point temperatures).
+
+\begin{equation}
+EIRTempModFac = a + b*W{B_i} + c*WB_i^2 + d*EWT + e*EW{T^2} + f*W{B_i}*EWT
+\end{equation}
+
+where
+
+WB\(_{i}\) = wet-bulb temperature of the air entering the cooling coil, °C
+
+EWT = entering water temperature, °C
+
+a-f = regression curve fit coefficients
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{4}
+\tightlist
+\item
+  Energy input ratio (EIR) modifier curve (function of air flow fraction)
+\end{enumerate}
+
+\begin{equation}
+EIRAirFlowModFac = a + b*f{f_a} + c*ff_a^2 + d*ff_a^3
+\end{equation}
+
+where
+
+a-d = regression curve fit coefficients, if no data available for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{5}
+\tightlist
+\item
+  Energy input ratio (EIR) modifier curve (function of water flow fraction)
+\end{enumerate}
+
+\begin{equation}
+EIRWaterFlowModFac = a + b*f{f_w} + c*ff_w^2 + d*ff_w^3
+\end{equation}
+
+where
+
+a-d = regression curve fit coefficients, if no data available for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{6}
+\tightlist
+\item
+  Recoverable heat modifier as a function of indoor wet-bulb and water entering temperatures.
+\end{enumerate}
+
+Recoverable heat modifier function is to account for the recoverable heat at the condensing side, as a fraction to the power input, which doesn't discharged to the water side.
+
+\begin{equation}
+WasteHeatTempModFac = a + b*W{B_i} + c*WB_i^2 + d*EWT + e*EW{T^2} + f*W{B_i}*EWT
+\end{equation}
+
+where
+
+a-f = regression curve fit coefficients
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{7}
+\tightlist
+\item
+  Part load fraction correlation (function of part load ratio)
+\end{enumerate}
+
+This field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, Sensible or Latent Load/Steady-State Sensible or Latent Capacity~ for Speed 1). The description of the part load fraction correlation for the VS WSHP cooling coil is similar to the VS WSHP heating coil.
+
+Lowest Speed Operation:
+
+The lowest speed operation of the VS WSHP is similar to the single speed DX cooling coil. The total (gross) cooling capacity of the WSHP unit is calculated as follows:
+
+\begin{equation}
+ \begin{array}{rl}
+  Q_{total,1} &= RatedTotalCoolingCapacity@SpeedLevel\left( 1 \right) \\
+              &* TotCapTempModFac_1 \\
+              &* TotCapAirFlowModFac_1 \\
+              &* TotCapWaterFlowModFac_1
+ \end{array}
+\end{equation}
+
+And the EIR is calculated as:
+
+\begin{equation}
+  \begin{array}{rl}
+    EIR_1 &= \frac{1.0}{ReferenceUnitCOP@Speed(1)} EIRTempModFac_1 \\
+          &* EIRAirFlowModFac_1 \\
+          &* EIRWaterFlowModWaterFac_1 
+  \end{array}
+\end{equation}
+
+And the power consumption excluding the indoor fan and the water pump is,
+
+\begin{equation}
+Powe{r_1} = {Q_{total,1}}*EI{R_1}*RTF
+\end{equation}
+
+Where RTF is the run-time fraction.
+
+The recoverable waste heat is:
+
+\begin{equation}
+  \begin{array}{rl}
+    Q_{RecoverHeat,1} &= ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( 1 \right) \\
+                      &* Power_1 \\
+                      &* WasteHeatTempModFac_1
+  \end{array}
+\end{equation}
+
+And the net heat discharged to the water loop is calculated as following:
+
+\({Q_{cond,1}} = Powe{r_1} + {Q_{total,1}} - {Q_{RecoverHeat,1}}\) .
+
+At the lowest speed, the dehumidification calculation is exactly the same as the single speed DX coil. That is to use the rated SHR and the design air flow rate at the lowest speed to calculate rated bypass factor of BF\(_{rated,1}\), and the corresponding effective surface area of A\(_{o,1}\). Wh A\(_{o,1}\) known, the coil BF can be adjusted for non-rated air flow rates. It shall be noted if choosing to add hot gas reheating to the supply side,~ \({Q_{RecoverHeat,1}}\) ~should be subtracted from bh the total cooling capacity and the sensible cooling capacity.
+
+And the part load ratio for sensible cooling is,
+
+\begin{equation}
+PLR = SensibleCoolingLoad/({Q_{total,1}}*SH{R_1})
+\end{equation}
+
+For latent cooling,
+
+\(PLR = LatentCoolingLoad/[{Q_{total,1}}*(1.0 - SH{R_1})]\) \emph{.}
+
+Higher Speed Operation:
+
+At the speed level between the lowest and the highest, there is no part-load loss. A parameter of speed ratio (SpeedRatio) is used to define the capacity partition between Speed x-1 and Speed x.
+
+the design air and water flow rate at the speed ratio are given as following:
+
+\begin{equation}
+  \begin{array}{rl}
+    {\rm{DesignAirFlowRateSpeedRatio}} &= ReferenceUnitAirMassFlowRate@SpeedLevel\left( {x - 1} \right) \\
+                                       &* CapacityScaleFactor \\
+                                       &* \left( {1-\rm{SpeedRatio}} \right) \\
+                                       &+ ReferenceUnitAirMassFlowRate@SpeedLevel\left( x \right) \\
+                                       &* CapacityScaleFactor \\
+                                       &* SpeedRatio
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    \rm{DesignWaterFlowRateSpeedRatio} &= ReferenceUnitWaterMassFlowRate@SpeedLevel\left( {x - 1} \right) \\
+                                        &* CapacityScaleFactor \\
+                                        &* \left( {1-\rm{SpeedRatio}} \right) \\
+                                        &+ ReferenceUnitWaterMassFlowRate@SpeedLevel\left( x \right) \\
+                                        &* CapacityScaleFactor \\
+                                        &* SpeedRatio
+  \end{array}
+\end{equation}
+
+And the fractions of air flow and water flow are given:
+
+\(f{f_{a,x - 1}}\) . = \(f{f_{a,x}}\) = actual air mass flow rate/DesignAirFlowRateSpeedRatio
+
+\(f{f_{w,x - 1}}\) \(f{f_{w,x}}\) = actual water mass flow rate/DesignWaterFlowRateSpeedRatio
+
+The total cooling capacities and EIRs at Speed x-1 and Speed x are calculated:
+
+\begin{equation}
+  \begin{array}{rl}
+    {Q_{total,x - 1}} &= RatedTotalCoolingCapacity@SpeedLevel\left( {x - 1} \right) \\
+                      &* TotCapTempModFac_{x - 1} \\
+                      &* TotCapAirFlowModFac_{x - 1} \\
+                      &* TotCapWaterFlowModFac_{x - 1}
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    {Q_{total,x}} &= RatedTotalCoolingCapacity@SpeedLevel\left( x \right) \\
+                  &* TotCapTempModFac_x \\
+                  &* TotCapAirFlowModFac_x \\
+                  &* TotCapWaterFlowModFac_x
+  \end{array}
+\end{equation}
+
+\begin{equation}
+  \begin{array}{rl}
+    EIR_{x - 1} &= \frac{{1.0}}{{ReferenceUnitCOP@Speed(x - 1)}}EIRTempModFac_{x - 1} \\
+                &* EIRAirFlowModFac_{x - 1} \\
+                &* EIRWaterFlowModFac_{x - 1}
+  \end{array}
+\end{equation}
+
+The total heating capacity at the corresponding speed ratio is:
+
+\begin{equation}
+{Q_{total,SpeedRatio}} = \left( {1.0 - SpeedRatio} \right)*{Q_{total,x - 1}} + SpeedRatio*{Q_{total,x}}
+\end{equation}
+
+And the power consumption, excluding the fan and pump power consumptions, is
+
+\begin{equation}
+Powe{r_{SpeedRatio}} = \left( {1.0 - SpeedRatio} \right)*{Q_{total,x - 1}}*EI{R_{x - 1}} + SpeedRatio*{Q_{total,x}}*EI{R_x}
+\end{equation}
+
+\emph{The recoverable waste heat is:}
+
+\begin{equation}
+  \begin{array}{rl}
+    Q_{RecoverHeat,SpeedRatio} &= \left( {1.0 - SpeedRatio} \right) \\
+                               &* ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( {x - 1} \right) \\
+                               &* \rm{WasteHeatTempModFac}_{x - 1} * {Q_{total,x - 1}} * EIR_{x - 1} \\
+                               &+ SpeedRatio \\
+                               &* ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( x \right) \\
+                               &* \rm{WasteHeatTempModFac}_x \\
+                               &* Q_{total,x} * EIR_x
+  \end{array}
+\end{equation}
+
+And the net heat discharged to the water loop is calculated as following:
+
+\begin{equation}
+{Q_{cond,SpeedRatio}} = Powe{r_{SpeedRatio}} + {Q_{total,SpeedRatio}} - {Q_{RecoverHeat,SpeedRatio}}
+\end{equation}
+
+And the effective surface area in the correlations of BF factor ~is calculated as below:
+
+\begin{equation}
+{A_{o,SpeedRatio}} = \left( {1 - SpeedRatio} \right)*{A_{o,x - 1}} + SpeedRatio*{A_{o,x}}
+\end{equation}
+
+Using A\(_{o,SpeedRatio}\) in the same BF and SHR calculation procedure as the single speed DX cooling coil, we can get BF\(_{SpeedRatio}\), and SHR\(_{SpeedRatio.}\) And the sensible cooling capacity is calculated:
+
+\begin{equation}
+{Q_{sensible,SpeedRatio}} = {Q_{total,SpeedRatio}}*SH{R_{SpeedRatio}}
+\end{equation}
+
+It should be noted if choosing to add hot gas reheating to the supply side, \({Q_{RecoverHeat,SpeedRatio}}\) ~should be subtracted from both the total cooling capacity and the sensible cooling capacity.
+
+At last, if the VS WSHP is used to match the sensible cooling load,
+
+\begin{equation}
+{Q_{sensible,SpeedRatio}} = SensibleLoad
+\end{equation}
+
+If it intends to match the latent cooling load,
+
+\begin{equation}
+{Q_{total,SpeedRatio}}*\left( {1.0 - SH{R_{SpeedRatio}}} \right) = LatentLoad
+\end{equation}
+
+If the speed reaches the highest level, the speed ratio becomes 1.0, and Speed n represents the highest speed.
+
+\subsubsection{References}\label{references-9}
+
+Keith C. Rice, 2011, DOE/ORNL Heat Pump Design Model:
+
+S.A. Klein 2011, User Manual of Engineering Equation Solver V8
+
+\subsubsection{Secondary Coils of DX Systems and Heat Pumps}\label{secondary-coils-of-dx-systems-and-heat-pumps}
+
+\subsubsection{Overview}\label{overview-15}
+
+Secondary coils reject to or remove heat from a secondary zone. Secondary coil refers to a condenser of a DX system or a heat pump in cooling operating mode or an evaporator of a heat pump in heating mode. The secondary coil (e.g.~condenser) of DX system or heat pumps is commonly installed outdoor but when installed indoor either heat is dumped to or extracted from the secondary zone. A secondary zone is a conditioned or unconditioned zone where the secondary coil is installed. Secondary coils are not standalone DX coil objects but they are add-on features on existing DX coil objects. A secondary DX coil is modelled by specifying additional inputs in single speed and multi speed DX coil objects: The additional inputs allow us to model the heat rejected or extracted by the secondary coil while the primary coil serves another controlled zone as shown in \protect\hyperlink{SchematicDXCoil}{Figure}. A secondary coil is not controlled directly but responds to the requirements of the primary DX coil. The operating mode of a secondary DX coil is determined by the primary DX coil serving the conditioned zone. If the primary DX coil is in cooling mode, then the secondary coil is rejecting heat (heating mode) to the secondary zone, or else if the primary DX coil is in heating mode, then the secondary coil is extracting heat (cooling mode) from the secondary zone. Heat rejected to a secondary zone by a condenser of a DX system or a heat pump is considered as sensible only. Whereas energy extracted from a secondary zone may contain sensible and latent components. The condenser type of the primary DX coils should be AirCooled. There is no need to specify the condenser air inlet node. The model uses zone air node as the secondary coil air inlet node. Air drawn by the secondary coil fan passes through the secondary coil and dumped back into the secondary zone. The previous time step zone condition is used as an inlet condition to the current time for the secondary DX coil model.
+
+\begin{figure}[hbtp]
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image8002.png}
+\caption{Schematic of DX System in cooling operating mode \protect \label{fig:schematic-of-dx-system-in-cooling-operating-mode}}
+\end{figure}
+
+Applications of this technology include: inter-zone heat pump in NTED (Dixon, 2010), and PTAC or PTHP serving Offices attached to a Warehouse, where the office partially or fully enclosed by the warehouse and the condenser is placed inside the Warehouse. The heat rejected or extracted by the secondary DX coil is estimated from the delivered capacity and electric power input of the primary DX coils. And the rejected or extracted heat is treated as internal gain of the secondary zone. Currently secondary DX coil are allowed in single speed, two speed and multi speed DX coil objects: \emph{Coil:Cooling:DX:SingleSpeed}, \emph{Coil:Heating:DX:SingleSpeed}, \emph{Coil:Cooling:DX:TwoSpeed}, \emph{Coil:Cooling:DX:MultiSpeed}, and \emph{Coil:Heating:DX:MultiSpeed}.
+
+\subsubsection{Model Description:}\label{model-description-12}
+
+The secondary coil performance calculation is invoked using inputs in the DX coil objects. The input required for cooling and heating operation of the primary DX coils are different. In the DX cooling coils the only required input is the zone name where the secondary coil is installed. In heating DX coils six inputs are required for single speed coils and a minimum of 11 input fields are required for multispeed DX heating coils. And five more inputs are required for every additional compressor speed. The extensible five input fields are used for splitting the total heat extraction rate into sensible and latent components. These five input fields are: rated sensible heat ratio, secondary air flow rates, scaling factor for auto-sizing secondary air flow rates, sensible heat ratio modifier curves as a function of temperature and sensible heat ratio modifier curves as a function of secondary air flow fraction. The secondary coil model assumes that liquid water from defrosting operation is drained to the outdoor and has no impact on the zone air heat balance.
+
+\textbf{Cooling Operating Mode:} the primary DX cooling coil of a DX system serving a primary zone is on and heat is rejected by the secondary coil (condenser) into a secondary zone. The secondary zone name is specified in DX cooling coil objects. This operating mode applies to a DX cooling system and cooling operating mode of air-to-air single and multi-speed heat pumps. The heat rejected by the secondary coil (condenser) of a DX system or heat pump operating in cooling mode is given by:
+
+\begin{equation}
+  Q_{cond} = Q_{Evap}+P_{CompCondFan}
+\end{equation}
+
+where
+
+\begin{itemize}
+\tightlist
+\item
+  \(Q\_\rm{Evap}\) is the cooling load delivered by the primary DX cooling coil system, W 
+\item
+  \(P\_\rm{CompCondFan}\) is the compressor and evaporator fan electric power input of a heat pump in heating mode, W
+\item
+  \(Q\_\rm{cond}\) is the heat rejected by the secondary coil (condenser) of a DX system or heat pump, W
+\end{itemize}
+
+Heat rejected by a secondary coil (condenser) calculated at each time step becomes internal gain of the secondary zone as shown in \protect\hyperlink{SchematicDXAndSecondary}{Figure}. Whenever a secondary zone name is specified in DX cooling coil objects, the secondary DX coil model calculation is invoked. New input field required as add-on to the DX cooling coil objects is ``\emph{Zone Name for Secondary Coil (condenser) Placement}''.
+
+\begin{figure}[hbtp]
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image8003.png}
+\caption{Schematic of DX system and secondary coil (condenser) \protect \label{fig:schematic-of-dx-system-and-secondary-coil}}
+\end{figure}
+
+\textbf{Heating Operating Mode:} When a heat pump operates in heating mode then energy is extracted from the secondary zone. The total energy extracted is estimated by rearranging the equation above as follows:
+
+\begin{equation}
+Q_\text{Evap} = Q_\text{cond} - P_\text{CompCondFan}
+\end{equation}
+
+where
+
+\begin{itemize}
+\tightlist
+\item
+  (Q\_\text{cond}) is the heat delivered by the primary heating DX coil to the primary zone, W
+\item
+  (P\_\text{CompCondFan}) is the compressor and condenser fan electric power input of a DX system or heat pump in cooling mode, W
+\item
+  (Q\_\text{Evap}) is the energy extracted by secondary coil (evaporator) from the secondary zone, W
+\end{itemize}
+
+The total energy extracted from a secondary zone may contain sensible and latent components. The secondary coil model checks for the coil inlet and full load outlet air condition to determine whether dehumidification will occur. The sensible and latent split of the energy extracted is done using a user specified rated sensible heat ratio (SHR) and SHR modifier curves for temperature and the secondary air flow fraction. If the secondary coil operation is dry, then the SHR is set to 1.0. In addition, the model assumes that defrosting operation is on, then the defrosting melts the frost and the liquid water from the collecting pan is drained to outside. Thus defrosting energy is not included in the zone energy balance. The heat extracted from the secondary zone may contain sensible and latent components and the secondary coil model does the sensible/latent heat split calculation.
+
+\subsubsection{Sensible Heat Ratio Calculation}\label{sensible-heat-ratio-calculation}
+
+The SHR calculation method uses user specified SHR modifying curves for temperature and flow fraction. The modifying curves correct the rated SHR value for a given secondary DX coil (evaporator) entering air temperatures and air mass flow fraction for a given speed. If these SHR modifying curves are not specified a constant SHR will be assumed. These two curves are a biquadratic SHR modifier curve for temperature (SHRFT), and a quadratic SHR correction curve for flow fraction (SHRFFF). The SHR is given by:
+
+\begin{equation}
+SHR = SHR_\text{rated}\cdot SHRFT\left(T_\text{wb,secondaryZone},T_\text{db,primaryCoil}\right)\cdot SHRFFF(FF)
+\end{equation}
+
+where
+
+\begin{itemize}
+\tightlist
+\item
+  (SHRFT) is the sensible heat ratio modifier normalized biquadratic curve as a function of secondary DX coil entering air wet-bulb and primary DX coil entering air dry-bulb temperatures, (-). The secondary DX coil (evaporator) entering air wet-bulb temperature is the secondary zone air wet-bulb temperature.
+\item
+  (SHRFFF) is the sensible heat ratio modifier normalized quadratic curve as a function of air mass flow fraction. Flow fraction is the ratio of actual to rated mass flow rate of air through the secondary DX coil, (-).
+\item
+  (SHR\_\text{rated}) is the sensible heat ratio at rated condition, (-).
+\end{itemize}
+
+For multispeed secondary DX coils when the system is cycling between two speeds of \emph{n} and \emph{n}-1 the operating SHR is weighted using \emph{SpeedRatio} as follows:
+
+\begin{equation}
+SHR = SHR_n \cdot SpeedRatio +  SHR_{n-1} (1 - SpeedRatio)
+\end{equation}
+
+where
+
+\begin{itemize}
+\tightlist
+\item
+  (SHR\_n) is the sensible heat ratio at speed n determined from user specified rated SHR, and SHR modifier curves at speed \emph{n}, (-)
+\item
+  (SHR\_\{n-1\}) is the sensible heat ratio at speed \emph{n}-1 determined from user specified rated SHR, and \emph{SHR} modifier curves at speed \emph{n}-1, (-).
+\item
+  \emph{SpeedRatio} is a parameter that relates performance between successive compressor speeds, (-).
+\end{itemize}
+
+\subsubsection{Sensible and Latent Split}\label{sensible-and-latent-split}
+
+The air enthalpy difference across the secondary DX coil (evaporator) at full load is given by:
+
+\begin{equation}
+h_\text{Delta} = \frac{\left(Q_\text{Evap}/PLR\right)}{\dot{m}_\text{cond}}
+\end{equation}
+
+The coil outlet enthalpy is calculated as follows:
+
+\begin{equation}
+h_\text{Outlet} = h_\text{Inlet}-h_\text{Delta}
+\end{equation}
+
+Using the SHR calculated above and secondary DX coil outlet temperature is given by:
+
+\begin{equation}
+T_\text{OutletNode} = T_\text{ZoneAirNode} -  \frac{\left(Q_\text{Evap}/PLR\right)\cdot SHR}{\dot{m}_\text{cond}c_p}
+\end{equation}
+
+Calculate the saturated outlet temperature at the outlet enthalpy and check the secondary outlet air condition if super-saturation has occurred:
+
+\begin{equation}
+T_\text{OutletNode, Sat} = T_\text{SAT}\left(h_\text{Outlet}, P_\text{Tot}\right)
+\end{equation}
+
+\begin{lstlisting}
+IF(\(T_\text{OutletNode} > T_\text{OutletNode, Sat}\)) Then
+    \(\omega_\text{OutletNode} > \omega_\text{InletNode}\)
+ELSE
+    (\(T_\text{OutletNode} = T_\text{OutletNode, Sat}\)
+    The coil outlet humidity ratio is determined using psychrometric functions as follows.
+    \(\omega_\text{OutletNode} = \omega\left(T_\text{OutletNode,Sat},h_\text{Outlet}\right)\)
+ENDIF
+\end{lstlisting}
+
+where
+
+\(h\_\text{Inlet}\) is the enthalpy of air entering the passive coil (J/kg)
+
+\(h\_\text{Outlet}\) is the enthalpy of air leaving the passive coil, (J/kg) 
+
+\(\dot{m}_{\text{sec}}\) is the secondary DX coil mass flow rate, (kg/s) 
+
+PLR is the primary DX cooling coil compressor part-load ratio, (-)
+
+\(P_{Tot}\) is the total pressure at the inlet of secondary DX coil, (Pa)
+
+\(T\_\text{OutletNode}\) is the secondary coil outlet air temperature, (degC) 
+
+\(T\_\text{OutletNode,Sat}\) is the secondary coil saturated air temperature at the outlet enthalpy, (degC)
+
+\(\omega\_\text{InletNode}\) is the secondary coil inlet node air humidity ratio, (kgH2O/kgDryair) 
+
+\(\omega\_\text{OutletNode}\) is the secondary coil outlet node air humidity ratio, (kgH2O/kgDryair)
+
+Reference: Dixon, Erin Elizabeth, ``Energy Model Development and Heating Energy Investigation of the Nested Thermal Envelope Design (NTED (tm))'' (2010). Theses and dissertations. Paper 974.
+
+\subsection{Packaged Thermal Storage Cooling Coil}\label{packaged-thermal-storage-cooling-coil}
+
+The DX cooling coil model for Coil:Cooling:DX:SingleSpeed:ThermalStorage is described in this section. The following diagram shows the main aspects of the model for packaged thermal energy storage cooling coil. This model allows charging and discharging to shift cooling energy use. The dashed line shows the boundary of the empirical ``black box'' model. The main parts are the Condenser, Evaporator, Compressor, and Thermal Energy Storage (TES) tank. The model interacts with the surroundings via a condenser inlet and outlet nodes, evaporator inlet and outlet nodes, heat transfer between TES tank and surrounding ambient environment, and optional added plant connection to the TES tank.
+
+\begin{figure}[hbtp] % fig 183
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4287.png}
+\caption{Highlights of Packaged Thermal Storage Cooling Coil \protect \label{fig:highlights-of-packaged-thermal-storage}}
+\end{figure}
+
+Depending on the operating mode, different parts are active.~ There are six modes to consider.
+
+\textbf{Off Mode} is when the unit is not running but the TES tank still interacts with ambient and the model needs to track the state of charge in the tank.
+
+\begin{figure}[hbtp] % fig 184
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4288.png}
+\caption{Thermal Storage Cooling Coil Off Mode \protect \label{fig:thermal-storage-cooling-coil-off-mode}}
+\end{figure}
+
+Governing equations for Off Mode include:
+
+\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} = 0\) ~~~~~ (water tank)
+
+\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} = 0\) ~~~~ (ice tank)
+
+\begin{equation}
+{\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{Plant}} = \dot m\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)
+\end{equation}
+
+\textbf{Cooling Only Mode} is when the unit is running but since it is neither charging nor discharging the TES tank, the model is essentially the same as a normal single speed DX cooling coil.~ The latent degradation model is not available.~ The model uses SHR curves~ from user input.
+
+\begin{figure}[hbtp] % fig 185
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4293.png}
+\caption{Thermal Storage Coil Cooling Only Modee \protect \label{fig:thermal-storage-coil-cooling-only-modee}}
+\end{figure}
+
+The governing equations for Cooling Only Mode include:
+
+\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} = 0\) ~~~~~ (water tank)
+
+\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} = 0\) ~~~ (ice tank)
+
+\begin{equation}
+\dot W + {\dot Q_{Evap}} + {\dot Q_{Cond}} = 0
+\end{equation}
+
+\begin{equation}
+{\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{Plant}} = \dot m{c_p}\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)
+\end{equation}
+
+The input correlations are used in the following manner to determine cooling capacity and energy consumption for a given set of operationg conditions.
+
+One total evaporator cooling capacity modifier curve is a function of evaporator inlet wetbulb temperature and condenser inlet drybulb temperature.
+
+\begin{equation}
+EvapCapTempModFac = {f_{}}\left( {{T_{evap,wb}},{\rm{}}{T_{cond,db}}} \right)
+\end{equation}
+
+Another total evaporator cooling capacity modifier curve is a function of air flow fraction through the evaporator section where air flow fraction is the ratio of current air mass flow rate to the rated air mass flow rate.
+
+\begin{equation}
+  EvapCapFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+One energy input ratio modifier curve is a function of evaporator inlet wetbulb temperature and condenser inlet drybulb temperature.
+
+\begin{equation}
+EIRTempModFac = f\left( {{T_{evap,wb}},{\rm{}}{T_{cond,db}}} \right)
+\end{equation}
+
+Another energy input ratio modifier curve is a function of flow fraction.
+
+\begin{equation}
+  EIRFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+Part load degradation curve is a function of part load ratio.
+
+\begin{equation}
+EvapPartLoadFac = f\left( {PLR} \right)
+\end{equation}
+
+The results of the performance curves are applied as follows to determine cooling capacity and energy performance:
+
+\begin{equation}
+{\dot Q_{Evap}} = {\dot Q_{Evap,RatedCoolOnly}}\left( {EvapCapTempModFac} \right)\left( {EvapCapFlowModFac} \right)
+\end{equation}
+
+\begin{equation}
+{\dot W_{elec}} = \frac{{{{\dot Q}_{evap}}\left( {EIRTempModFac} \right)\left( {EIRFlowModFac} \right)\left( {PLR} \right)}}{{\left( {CO{P_{Rated,{\rm{}}CoolOnly}}} \right)\left( {EvapPartLoadFac} \right)}}
+\end{equation}
+
+The sensible heat ratio (SHR) is determined by a rated SHR and two performance curves. The SHR temperature modifying factor is a function of evaporator entering wetbulb and evaporator entering drybulb temperature.
+
+\begin{equation}
+SHRTempModFac = f\left( {{T_{evap,wb}},{T_{evap,db}}} \right)
+\end{equation}
+
+The SHR flow fraction modifying factor is a function of air flow fraction through the evaporator section where air flow fraction is the ratio of current air mass flow rate to the rated air mass flow rate.
+
+\begin{equation}
+  SHRFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+The results of the performance curves are applied as follows to determine SHR:
+
+\begin{equation}
+SHR = SH{R_{rated}}*SHRTempModFac*SHRFlowModFac
+\end{equation}
+
+Cool and Charge Mode is when the unit is both cooling and charging the TES, then all the parts are active. The electric power into the compressor is split into two terms to accommodate devices that actually have dual compressors.
+
+\begin{figure}[hbtp] % fig 186
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4309.png}
+\caption{Thermal Storage Coil Cool and Charge Modes \protect \label{fig:thermal-storage-coil-cool-and-charge-modes}}
+\end{figure}
+
+Governing Equations for ``Cool and Charge Mode''
+
+\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\) ~~~~~ (water tank)
+
+\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\) ~~~ (ice tank)
+
+\begin{equation}
+{\dot W_{Evap}} + {\dot W_{TES}} + {\dot Q_{Evap}} + {\dot Q_{Cond}} + {\dot Q_{TES}} = 0
+\end{equation}
+
+\begin{equation}
+{\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)
+\end{equation}
+
+\({\dot Q_{Plant}} = \dot m{c_p}\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\) \[{\dot Q_{Plant}} = \dot m\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\]
+
+The input correlations are used in the following manner to determine cooling capacity, chargine capacity, and energy consumption for a given set of operationg conditions.
+
+One total evaporator cooling capacity modifier curve is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES, \({S_{TES}}\) ~(temperature of water or fraction of ice).
+
+\begin{equation}
+EvapCapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)
+\end{equation}
+
+Another total evaporator cooling capacity modifier curve is a function of flow fraction.
+
+\begin{equation}
+EvapCapFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+One evaporator energy input ratio modifier curve, function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
+
+\begin{equation}
+EIREvapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)
+\end{equation}
+
+Another energy input ratio modifier curve is a function of flow fraction.
+
+\begin{equation}
+EIREvapFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+Part load degradation curve is a function of evaporator part load ratio.
+
+\begin{equation}
+EvapPartLoadFac = f\left( {PLR} \right)
+\end{equation}
+
+One storage charge capacity modifier curve is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
+
+\begin{equation}
+TESCapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)
+\end{equation}
+
+Another storage charge capacity modifier curve is a function of evaporator part load ratio.
+
+\begin{equation}
+TESCapPartLoadFac = f\left( {PLR} \right)
+\end{equation}
+
+The results of the performance curves are applied as follows to determine cooling capacity and energy performance:
+
+\begin{equation}
+{\dot Q_{Evap}} = {\dot Q_{Evap,RatedCoolAndCharge}}\left( {EvapCapTempModFac} \right)\left( {EvapCapFlowModFac} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{TES}} = {\dot Q_{Charge,Rated}}\left( {TESCapTempModFac} \right)\left( {TESCapPartLoadFac} \right)
+\end{equation}
+
+\begin{equation}
+{\dot W_{Evap,elec}} = \frac{{\left( {{{\dot Q}_{Evap}}} \right)\left( {EIRTempModFac} \right)\left( {EIRFlowModFac} \right)\left( {EvapPLR} \right)}}{{\left( {CO{P_{Rated,Cooling}}} \right)\left( {EvapPartLoadFac} \right)}}
+\end{equation}
+
+\({\dot W_{TES,elec}} = \frac{{\left( {{{\dot Q}_{TES}}} \right)\left( {EIRStorTempModFac} \right)\left( {EIRStorFlowModFac} \right)\left( {StorPLR} \right)}}{{\left( {CO{P_{Rated,Charging}}} \right)\left( {StorPartLoadFac} \right)}}\) .
+
+The sensible heat ratio (SHR) is determined by a rated SHR and two performance curves. There are two options for the SHR temperature modifying factor, it can either be a function of evaporator entering wetbulb and evaporator entering drybulb temperature or it can add a third independent variable for the state of charge of TES.
+
+\begin{equation}
+  SHRTempModFac = \left\{
+    \begin{array}{l}
+      f\PB{T_{evap,wb},T_{evap,db}} \\
+      f\PB{T_{evap,wb},T_{evap,db},S_{TES}}
+    \end{array}
+  \right.
+\end{equation}
+
+The SHR flow fraction modifying factor is a function of air flow fraction through the evaporator section where air flow fraction is the ratio of current air mass flow rate to the rated air mass flow rate.
+
+\begin{equation}
+SHRFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+The results of the performance curves are applied as follows to determine SHR:
+
+\begin{equation}
+SHR = SH{R_{rated}}*SHRTempModFac*SHRFlowModFac
+\end{equation}
+
+\textbf{Cool and Discharge Mode} is when the unit is both cooling and discharging the TES, then all the parts are active. The electric power into the compressor is split into two terms to accommodate devices that actually have dual compressors.
+
+\begin{figure}[hbtp] % fig 187
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4331.png}
+\caption{Thermal Storage Coil Cool and Discharge Modes \protect \label{fig:thermal-storage-coil-cool-and-discharge-modes}}
+\end{figure}
+
+Governing Equations for ``Cool and Discharge Mode''
+
+\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\) ~~~~~ (water tank)
+
+\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\) ~~~ (ice tank)
+
+\begin{equation}
+{\dot W_{Evap}} + {\dot W_{TES}} + {\dot Q_{Evap}} + {\dot Q_{Cond}} + {\dot Q_{TES}} = 0
+\end{equation}
+
+\begin{equation}
+{\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)
+\end{equation}
+
+\({\dot Q_{Plant}} = \dot m{c_p}\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\) \[{\dot Q_{Plant}} = \dot m\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\]
+
+The input correlations are used in the following manner.
+
+One total evaporator cooling capacity modifier curve is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
+
+\begin{equation}
+EvapCapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)
+\end{equation}
+
+Another Total evaporator cooling capacity modifier curve is a function of flow fraction.
+
+\begin{equation}
+EvapCapFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+One evaporator energy input ratio modifier curve is a function of of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
+
+\begin{equation}
+EIREvapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)
+\end{equation}
+
+Another evaporator energy input ratio modifier curve is a function of flow fraction.
+
+\begin{equation}
+EIREvapFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+Evaporator part load degradation curve is a function of evaporator part load ratio.
+
+\begin{equation}
+EvapPartLoadFac = f\left( {EvapPLR} \right)
+\end{equation}
+
+One storage discharge capacity modifier curve is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
+
+\begin{equation}
+TESCapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)
+\end{equation}
+
+Another storage discharge capacity modifier curve is a function of evaporator part load ratio.
+
+\begin{equation}
+TESCapPartLoadFac = f\left( {EvapPLR} \right)
+\end{equation}
+
+One storage energy input ratio modifier curve is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
+
+\begin{equation}
+EIRStorTempModFac = {f_{triquadratic}}\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)
+\end{equation}
+
+Another storage energy input ratio modifier curve is a function of flow fraction.
+
+\begin{equation}
+  EIRStorFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+Storage part load degradation curve is a function of storage discharge part load ratio.
+
+\begin{equation}
+StorPartLoadFac = f\left( {StorPLR} \right)
+\end{equation}
+
+The results of the performance curves are applied as follows to determine cooling capacity and energy performance:
+
+\begin{equation}
+{\dot Q_{Evap}} = {\dot Q_{Evap,RatedCoolAndDischarge}}\left( {EvapCapTempModFac} \right)\left( {EvapCapFlowModFac} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{TES}} =  - {\dot Q_{Discharge,Rated}}\left( {TESCapTempModFac} \right)\left( {TESCapPartLoadFac} \right)
+\end{equation}
+
+\begin{equation}
+{\dot W_{Evap,elec}} = \frac{{\left( {{{\dot Q}_{Evap}}} \right)\left( {EIREvapTempModFac} \right)\left( {EIREvapFlowModFac} \right)\left( {EvapPLR} \right)}}{{\left( {CO{P_{Rated,Cooling}}} \right)\left( {EvapPartLoadFac} \right)}}
+\end{equation}
+
+\begin{equation}
+{\dot W_{TES,elec}} = \frac{{\left( {{{\dot Q}_{TES}}} \right)\left( {EIRStorTempModFac} \right)\left( {EIRStorFlowModFac} \right)\left( {StorPLR} \right)}}{{\left( {CO{P_{Rated,Discharging}}} \right)\left( {StorPartLoadFac} \right)}}
+\end{equation}
+
+The sensible heat ratio (SHR) is determined by a rated SHR and two performance curves. There are two options for the SHR temperature modifying factor, it can either be a function of evaporator entering wetbulb and evaporator entering drybulb temperature or it can add a third independent variable for the state of charge of TES.
+
+\begin{equation}
+  SHRTempModFac = \left\{
+    \begin{array}{l}
+      f\PB{T_{evap,wb},T_{evap,db}} \\
+      f\PB{T_{evap,wb},T_{evap,db},S_{TES}}
+    \end{array}
+  \right.
+\end{equation}
+
+The SHR flow fraction modifying factor is a function of air flow fraction through the evaporator section where air flow fraction is the ratio of current air mass flow rate to the rated air mass flow rate.
+
+\begin{equation}
+SHRFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+The results of the performance curves are applied as follows to determine SHR:
+
+\begin{equation}
+SHR = SH{R_{rated}}*SHRTempModFac*SHRFlowModFac
+\end{equation}
+
+\textbf{Charge Only Mode} is when the unit is only charging, there is no heat flow at the evaporator. ~There is no modulation or part loading, when charging the unit charges at its nominal design rate (adjusted for conditions).
+
+\begin{figure}[hbtp] % fig 188
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4355.png}
+\caption{Thermal Storage Coil Charge Only Mode \protect \label{fig:thermal-storage-coil-charge-only-mode}}
+\end{figure}
+
+The governing equations for ``Charge Only Mode''
+
+\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\) ~~~~~ (water tank)
+
+\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\) ~~~ (ice tank)
+
+\begin{equation}
+\dot W + {\dot Q_{Cond}} + {\dot Q_{TES}} = 0
+\end{equation}
+
+\begin{equation}
+{\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)
+\end{equation}
+
+\({\dot Q_{Plant}} = \dot m{c_p}\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\) \[{\dot Q_{Plant}} = \dot m\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\]
+
+The input correlations are used in the following manner.
+
+Storage charge capacity modifier factor is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
+
+\begin{equation}
+TESCapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)
+\end{equation}
+
+Energy input ratio modifier factor is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
+
+\begin{equation}
+EIRTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{TES}} = \left( {{{\dot Q}_{Charge,Rated}}} \right)\left( {TESCapTempModFac} \right)
+\end{equation}
+
+\begin{equation}
+{\dot W_{elec}} = \left( {{{\dot Q}_{TES}}} \right)\left( {\frac{1}{{CO{P_{Rated,ChargeOnly}}}}} \right)\left( {EIRTempModFac} \right)
+\end{equation}
+
+\textbf{Discharge Only Mode} is when the unit is only discharging, there is no heat flow at the condenser. The rate of discharge will modulate to meet part loading at the evaporator.
+
+\begin{figure}[hbtp] % fig 189
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4366.png}
+\caption{Thermal Storage Coil Discharge Only Mode \protect \label{fig:thermal-storage-coil-discharge-only-mode}}
+\end{figure}
+
+The governing equations for ``Discharge Only Mode''
+
+\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\) ~~~~~ (water tank)
+
+\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\) ~~~ (ice tank)
+
+\begin{equation}
+\dot W + {\dot Q_{Evap}} + {\dot Q_{TES}} = 0
+\end{equation}
+
+\begin{equation}
+{\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)
+\end{equation}
+
+\({\dot Q_{Plant}} = \dot m{c_p}\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\) \({\dot Q_{Plant}} = \dot m\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\)
+
+The input correlations are used in the following manner.
+
+One total evaporator cooling capacity modifier factor is a function of evaporator inlet wetbulb temperature and state of TES.
+
+\begin{equation}
+EvapCapTempModFac = f\left( {{T_{evap,wb}},{S_{TES}}} \right)
+\end{equation}
+
+Another total evaporator cooling capacity modifier factor is a function of flow fraction.
+
+\begin{equation}
+EvapCapFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+One energy input ratio modifier factor is a function of evaporator inlet wetbulb temperature and state of TES.
+
+\begin{equation}
+EIRTempModFac = f\left( {{T_{evap,wb}},{S_{TES}}} \right)
+\end{equation}
+
+Another energy input ratio modifier factor is a function of flow fraction.
+
+\begin{equation}
+EIRFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+Part load degradation curve is a function of evaporator part load ratio.
+
+\begin{equation}
+EvapPartLoadFac = f\left( {EvapPLR} \right)
+\end{equation}
+
+\({\dot Q_{Evap}} = \left( {{{\dot Q}_{Evap,RatedDischargeOnly}}} \right)\left( {EvapCapTempModFac} \right)\left( {EvapCapFlowModFac} \right)\) . \({\dot W_{elec}} = \frac{{\left( {{{\dot Q}_{evap}}} \right)\left( {EIRStorTempModFac} \right)\left( {EIRStorFlowModFac} \right)\left( {EvapPLR} \right)}}{{\left( {CO{P_{Rated,DischargeOnly}}} \right)\left( {EvapPartLoadFac} \right)}}\)
+
+\begin{equation}
+{\dot Q_{TES}} = {\dot Q_{Evap}} + {\dot W_{elec}}
+\end{equation}
+
+The sensible heat ratio (SHR) is determined by a rated SHR and two performance curves. There are two options for the SHR temperature modifying factor, it can either be a function of evaporator entering wetbulb and evaporator entering drybulb temperature or it can add a third independent variable for the state of charge of TES.
+
+\begin{equation}
+  SHRTempModFac = \left\{
+    \begin{array}{l}
+      f\PB{T_{evap,wb},T_{evap,db}} \\
+      f\PB{T_{evap,wb},T_{evap,db},S_{TES}}
+    \end{array}
+  \right.
+\end{equation}
+
+The SHR flow fraction modifying factor is a function of air flow fraction through the evaporator section where air flow fraction is the ratio of current air mass flow rate to the rated air mass flow rate.
+
+\begin{equation}
+SHRFlowModFac = f\PB{\frac{\dot{m}_{evap,air}}{\dot{m}_{evap,air,rated}}}
+\end{equation}
+
+The results of the performance curves are applied as follows to determine SHR:
+
+\begin{equation}
+SHR = SH{R_{rated}}*SHRTempModFac*SHRFlowModFac
+\end{equation}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/cooling-towers-and-evaporative-fluid-coolers.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/cooling-towers-and-evaporative-fluid-coolers.tex
new file mode 100644
index 00000000000..7e833c42889
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/cooling-towers-and-evaporative-fluid-coolers.tex
@@ -0,0 +1,1006 @@
+\section{Cooling Towers and Evaporative Fluid Coolers }\label{cooling-towers-and-evaporative-fluid-coolers}
+
+\subsection{One, Two, and Variable Speed Cooling Towers and Evaporative Fluid Coolers}\label{one-two-and-variable-speed-cooling-towers-and-evaporative-fluid-coolers}
+
+\subsubsection{Overview}\label{overview-012}
+
+The input objects CoolingTower:SingleSpeed, CoolingTower:TwoSpeed, and CoolingTower:VariableSpeed:Merkel provide models for single-speed, two-speed, and variable-speed cooling towers that are based on Merkel's theory (Merkel 1925), which is also the basis for the tower model included in ASHRAE's HVAC1 Toolkit for primary HVAC system energy calculations (ASHRAE 1999, Bourdouxhe et al. 1994). Cooling tower performance is modeled using effectiveness-NTU relationships for counterflow heat exchangers. The model can be used to simulate the performance of both single speed, two speed, and variable speed mechanical-draft cooling towers. The model will also account for tower performance in the ``free convection'' regime, when the tower fan is off but the water pump remains on. For part-load operation, the model assumes a simple linear interpolation between two steady-state regimes without accounting for any cycling losses.
+
+For single speed cooling towers, the capacity control can be fan cycling or fluid bypass. In fluid bypass mode, portion of the water goes through the tower media and gets cooled while the remaining water flow gets bypassed, two water flows then mix together trying to meet the tower exiting water setpoint temperature. In both the free convection cooling when fan is off and normal cooling when fan is on for the entire time step, if the tower exiting water temperature is lower than the setpoint, the tower operates in fluid bypass mode. The model determines the fluid bypass fraction by iterations until the mixed water meets the tower exiting water temperature setpoint. In the fluid bypass mode, except the free convection, the tower fan runs at full speed for the entire time step. The maximum amount of tower water that can be bypassed is bounded by the freezing point of the tower water -- the tower exiting water temperature cannot be lower than the freezing setpoint.
+
+Evaporative fluid coolers are modeled very similar to cooling towers. The main difference between the two is in the ``Performance input method'' input field. Cooling tower has two choices for this field namely ``UFactorTimesAreaAndDesignWaterFlowRate'' and ``Nominal capacity''. The nominal capacity is specified for the standard conditions i.e.~entering water at 35C (95F), leaving water at 29.44C (85F), entering air at 25.56C (78F) wet-bulb temperature and 35C (95F) dry-bulb temperature. On the other hand evaporative fluid cooler has three choices for ``Performance input method'' which are ``UFactorTimesAreaAndDesignWaterFlowRate'', ``StandardDesignCapacity'' and ``UserSpecifiedDesignCapacity''. First method is same for both tower and fluid cooler. Standard design capacity is specified for the same conditions which are used to specify nominal capacity for tower as described above. If the capacity of fluid cooler for conditions other than the standard ones is known then UserSpecifiedDesignCapacity method should be used. In this case, the conditions for which the fluid cooler capacity is known i.e.~entering water temperature, entering air temperature and entering air wet bulb temperature must be specified in the input. To calculate evaporation loss for fluid cooler, spray water flow rate which is different than the process fluid flow rate must be specified for all the performance input methods. This is not required for cooling tower because cooled fluid i.e.~water is in direct contact with the air so the water loss is calculated by using cooled fluid flow rate only. Unlike cooling tower, evaporative fluid cooler model does not account for free convection.
+
+Cooling tower model is described below which holds equally good for evaporative fluid cooler. The differences are mentioned whenever required.
+
+\subsubsection{Model Description}\label{model-description-008}
+
+Based on Merkel's theory, the steady-state total heat transfer between the air and water entering the tower can be defined by the following equation:
+
+\begin{equation}
+d{\dot Q_{total}} = \frac{{UdA}}{{cp}}\left( {{h_s} - {h_a}} \right)
+\end{equation}
+
+where
+
+\emph{h\(_{s}\)} = enthalpy of saturated air at the wetted-surface temperature, J/kg
+
+\emph{h\(_{a}\)} = enthalpy of air in the free stream, J/kg
+
+\emph{c\(_{p}\)} = specific heat of moist air, J/kg-\(^{o}\)C
+
+\emph{U} = cooling tower overall heat transfer coefficient, W/m\(^{2}\)- \(^{o}\)C
+
+\emph{A} = heat transfer surface area, m\(^{2}\)
+
+Equation is based on several assumptions:
+
+n~air and water vapor behave as ideal gases
+
+n~the effect of water evaporation is neglected
+
+n~fan heat is neglected
+
+n~the interfacial air film is assumed to be saturated
+
+n~the Lewis number is equal to 1
+
+In this model, it is also assumed that the moist air enthalpy is solely a function of the wet-bulb temperature and that the moist air can be treated as an equivalent ideal gas with its mean specific heat defined by the following equation:
+
+\begin{equation}
+\bar cpe = \frac{{\Delta h}}{{\Delta {T_{wb}}}}
+\end{equation}
+
+where
+
+Δ\emph{h} = enthalpy difference between the air entering and leaving the tower, J/kg
+
+\(\Delta T_{wb}\) = wet-bulb temperature difference between the air entering and leaving the tower, \(^{o}\)C
+
+Since the liquid side conductance is much greater than the gas side conductance, the wetted-surface temperature is assumed to be equal to the water temperature. Based on this assumption and equations and , the expression for total heat transfer becomes:
+
+\begin{equation}
+d{\dot Q_{total}} = UedA\left( {{T_w} - {T_{wb}}} \right)
+\end{equation}
+
+where
+
+\begin{equation}
+Ue = \frac{{U\,\bar cpe}}{{cp}}
+\end{equation}
+
+\(T_{wb}\) = wet-bulb temperature of the air, \(^{o}\)C
+
+\emph{T\(_{w}\)} = temperature of the water, \(^{o}\)C
+
+An energy balance on the water and air sides of the air/water interface yields the following equations:
+
+\begin{equation}
+d{\dot Q_{total}} = {\dot m_w}cpw\,\,\,dTw
+\end{equation}
+
+\begin{equation}
+d{\dot Q_{total}} = {\dot m_a}\bar cpe\,\,\,dTwb
+\end{equation}
+
+where
+
+\({\dot m_w}\) ~ = mass flow rate of water, kg/s
+
+\({\dot m_a}\) ~ = mass flow rate of air, kg/s
+
+Assuming that the heat capacity rate (\(\dot mcp\) ) for the cooling tower water is less than that for the air,the effectiveness of the cooling tower can be defined by analogy to the effectiveness of a simple heat exchanger:
+
+\begin{equation}
+\varepsilon  = \frac{{{T_{win}} - {T_{wout}}}}{{{T_{win}} - {T_{wbin}}}}
+\end{equation}
+
+where
+
+\emph{ε} = heat exchanger effectiveness
+
+\emph{T\(_{win}\)} = inlet water temperature, \(^{o}\)C
+
+\emph{T\(_{wout}\)} = outlet water temperature, \(^{o}\)C
+
+\emph{T\(_{wbin}\)} = wet-bulb temperature of the inlet air, \(^{o}\)C
+
+Combining equations , , and and integrating over the entire heat transfer surface area, and combining the result with equation provides the following expression for cooling tower effectiveness:
+
+\begin{equation}
+\varepsilon \,\, = \,\frac{{1 - \exp \left\{ { - NTU\left[ {1 - \left( {\frac{{{{\dot C}_w}}}{{{{\dot C}_a}}}} \right)} \right]} \right\}}}{{1 - \left( {\frac{{{{\dot C}_w}}}{{{{\dot C}_a}}}} \right)\exp \left\{ { - NTU\left[ {1 - \left( {\frac{{{{\dot C}_w}}}{{{{\dot C}_a}}}} \right)} \right]} \right\}}}
+\end{equation}
+
+where
+
+\({\dot C_w} = {\dot m_w}c{p_w}\) ~and \({\dot C_a} = {\dot m_a}\bar c{p_e}\)
+
+\begin{equation}
+NTU = Number\,of\,Transfer\,Units = \frac{{UAe}}{{{{\dot C}_w}}}
+\end{equation}
+
+This equation is identical to the expression for effectiveness of an indirect contact (i.e., fluids separated by a solid wall) counterflow heat exchanger (Incropera and DeWitt 1981). Therefore, the cooling tower can be modeled, in the steady-state regime, by an equivalent counterflow heat exchanger as shown in the following figure.
+
+\begin{figure}[hbtp] % fig 194
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4542.png}
+\caption{Cooling Tower Schematic \protect \label{fig:cooling-tower-schematic}}
+\end{figure}
+
+The first fluid is water and the second fluid is an equivalent fluid entering the heat exchanger at temperature T\(_{wbin}\) and specific heat \(\bar cpe\) . The heat exchanger is characterized by a single parameter, its overall heat transfer coefficient-area product UA\(_{e}\). The actual cooling tower heat transfer coefficient-area product is related to UA\(_{e}\) by the following expression:
+
+\begin{equation}
+UA = UAe\frac{{cp}}{{\bar cpe}}
+\end{equation}
+
+This heat transfer coefficient-area product is assumed to be a function of the air mass flow rate only and can be estimated from laboratory test results or manufacturers' catalog data.
+
+The model for the variable speed Merkel tower also includes Scheier's modifications.~ Scheier has extended the Merkel model to also include terms that adjust UA with three factors that model how UA values change when the tower is operating away from its rated conditions.~ The first factor, \({f_{UA,wetbulb}}\) , adjusts UA for the current outdoor wetbulb temperature.~ The user enters a performance curve or lookup table that is a function of one independent variable.~ The independent variable is the difference between the design wetbulb temperature and the current wetbulb temperature, in degrees Celsius.
+
+\begin{equation}
+{f_{UA,wetbulb}} = func\left( {\left( {{T_{des,wetbulb}} - {T_{current,wetbulb}}} \right)} \right)
+\end{equation}
+
+The second factor, \({f_{UA,airflow}}\) , adjusts UA for the current air flow rate.~ The user enters a performance curve or lookup table that is a function of one independent variable.~ The independent variable is the ratio of the current air flow rate to the design air flow rate at full speed.
+
+\begin{equation}
+{f_{UA,airflow}} = func\left( {AirFlowRatio} \right)
+\end{equation}
+
+The third factor, \({f_{UA,waterflow}}\) , adjusts UA for the current water flow rate.~ The user enters a performance curve or lookup table that is a function of one independent variable.~ The independent variable is the ratio of the current water flow rate to the design water flow rate.
+
+\begin{equation}
+{f_{UA,waterflow}} = func\left( {WaterFlowRatio} \right)
+\end{equation}
+
+Then the UA value at any given time is calculated using
+
+\begin{equation}
+U{A_e} = U{A_{design}} \bullet {f_{UA,wetbulb}} \bullet {f_{UA,airflow}} \bullet {f_{UA,waterflow}}
+\end{equation}
+
+\subsubsection{Method for Calculating Steady-State Exiting Water Temperature}\label{method-for-calculating-steady-state-exiting-water-temperature}
+
+The objective of the cooling tower model is to predict the exiting water temperature and the fan power required to meet the exiting water setpoint temperature. Since only the inlet air and inlet water temperatures are known at any simulation time step, an iterative procedure is required to determine the exiting fluid temperatures using the equations defined in the previous section. In the case of the EnergyPlus model, the iterations are performed to determine the exiting wet-bulb temperature of the air. The exiting water temperature is then calculated based on an energy balance that assumes that the energy absorbed by the air is equivalent to the energy removed from the water. The procedure for calculating the steady-state, exiting air wet-bulb temperature is outlined below.
+
+As explained previously, it is assumed that the moist air enthalpy can be defined by the wet-bulb temperature alone. Therefore, the first step in the procedure is to calculate the enthalpy of moist air entering the cooling tower based on the ambient wet-bulb temperature from the weather file. Since an iterative solution is required, a first guess of the outlet air wet-bulb temperature is then made and the enthalpy of this estimated outlet air wet-bulb temperature is calculated. Based on these inlet and outlet air conditions, the mean specific heat of the air is calculated based on equation , repeated here:
+
+\begin{equation}
+\bar cpe = \frac{{\Delta h}}{{\Delta Twb}}
+\end{equation}
+
+With the overall heat transfer coefficient-area product for the cooling tower entered by the user, the effective heat transfer coefficient-area product is calculated by rearranging equation :
+
+\begin{equation}
+UAe = UA\frac{{\bar cpe}}{{cp}}
+\end{equation}
+
+With \(\bar cpe\) ~and \(UAe\) ~known, the effectiveness of the heat exchanger is then calculated:
+
+\begin{equation}
+\varepsilon \,\, = \,\frac{{1 - \exp \left\{ { - NTU\left[ {1 - \left( {\frac{{{{\dot C}_{\min }}}}{{{{\dot C}_{\max }}}}} \right)} \right]} \right\}}}{{1 - \left( {\frac{{{{\dot C}_{\min }}}}{{{{\dot C}_{\max }}}}} \right)\exp \left\{ { - NTU\left[ {1 - \left( {\frac{{{{\dot C}_{\min }}}}{{{{\dot C}_{\max }}}}} \right)} \right]} \right\}}}
+\end{equation}
+
+where
+
+\({\dot C_{\min }} = \,Minimum\,({\dot C_w},\,{\dot C_a})\) ~and \({\dot C_{\max }} = \,Maximum\,({\dot C_w},\,{\dot C_a})\)
+
+\({\dot C_w} = {\dot m_w}c{p_w}\) ~and \({\dot C_a} = {\dot m_a}\bar cpe\)
+
+\begin{equation}
+NTU = Number\,of\,Transfer\,Units = \frac{{UAe}}{{{{\dot C}_{\min }}}}
+\end{equation}
+
+The heat transfer rate is then calculated as follows:
+
+\begin{equation}
+\dot Qtotal = \,\varepsilon \,{\dot C_{\min }}\left( {Twin\, - \,Twbin} \right)
+\end{equation}
+
+The outlet air wet-bulb temperature is then recalculated:
+
+\begin{equation}
+{T_{wbout}} = {T_{wbin}} + \frac{{{{\dot Q}_{total}}}}{{{{\dot C}_a}}}
+\end{equation}
+
+The iterative process of calculating \({T_{wbout}}\) ~continues until convergence is reached.
+
+Finally, the outlet water temperature is calculated as follows:
+
+\begin{equation}
+{T_{wout}} = {T_{win}} + \frac{{{{\dot Q}_{total}}}}{{{{\dot C}_w}}}
+\end{equation}
+
+\subsubsection{Calculating the Actual Exiting Water Temperature and Fan Power}\label{calculating-the-actual-exiting-water-temperature-and-fan-power}
+
+The previous section describes the methodology used for calculating the steady-state temperature of the water leaving the cooling tower. This methodology is used to calculate the exiting water temperature in the free convection regime (water pump on, tower fan off) and with the tower fan operating (including low and high fan speed for the two-speed tower). The exiting water temperature calculations use the fluid flow rates (water and air) and the UA-values entered by the user for each regime.
+
+The cooling tower model seeks to maintain the temperature of the water exiting the cooling tower at (or below) a setpoint. The model obtains the target temperature setpoint from the setpoints placed on either the tower outlet node or the loop's overall setpoint node (typically set to the supply side outlet node). The model checks to see if the outlet node has a setpoint placed on it and uses that if it does.~ If the outlet node does not have a temperature setpoint then the model uses the loop-level outlet node specified in the input field called Loop Temperature Setpoint Node Name in the PlantLoop or CondenserLoop object. The model first checks to determine the impact of ``free convection'', if specified by the user, on the tower exiting water temperature. If free convection is not specified by the user, then the exiting water temperature is initially set equal to the entering tower water temperature. If the user specifies ``free convection'' and the steady-state exiting water temperature based on ``free convection'' is at or below the setpoint, then the tower fan is not turned on.
+
+If the exiting water temperature remains above the setpoint after ``free convection'' is modeled, then the tower fan is turned on to reduce the exiting water temperature to the setpoint. The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (e.g., tower fan on for the entire simulation time step and tower fan off for the entire simulation time step). Cyclic losses are not taken into account.
+
+The fraction of time that the tower fan must operate is calculated based on the following equation:
+
+\begin{equation}
+\omega \,\, = \frac{{{T_{set}} - {T_{wout,off}}}}{{{T_{wout,on}} - {T_{wout,off}}}}
+\end{equation}
+
+where
+
+\({T_{set}}\) ~ = exiting water setpoint temperature, \(^{o}\)C
+
+\({T_{wout,off}}\) ~ = exiting water temperature with tower fan off, \(^{o}\)C
+
+\({T_{wout,on}}\) ~ = exiting water temperature with tower fan on, \(^{o}\)C
+
+The average fan power for the simulation time step is calculated by multiplying \(\omega \,\) by the steady-state fan power specified by the user.
+
+The calculation method for the two-speed tower is similar to that for the single-speed tower example described above. The model first checks to see if ``free convection'' is specified and if the resulting exiting water temperature is below the setpoint temperature. If not, then the model calculates the steady-state exiting water temperature with the tower fan at low speed. If the exiting water temperature at low fan speed is below the setpoint temperature, then the average fan power is calculated based on the result of equation and the steady-state, low speed fan power specified by the user. If low-speed fan operation is unable to reduce the exiting water temperature below the setpoint, then the tower fan is increased to its high speed and the steady-state exiting water temperature is calculated. If this temperature is below the setpoint, then a modified version of equation is used to calculate runtime at high fan speed:
+
+\begin{equation}
+\omega \,\, = \frac{{{T_{set}} - {T_{wout,low}}}}{{{T_{wout,high}} - {T_{wout,low}}}}
+\end{equation}
+
+where
+
+\({T_{set}}\) ~ = exiting water setpoint temperature, \(^{o}\)C
+
+\({T_{wout,low}}\) ~ = exiting water temperature with tower fan at low speed, \(^{o}\)C
+
+\({T_{wout,high}}\) ~ = exiting water temperature with tower fan at high speed, \(^{o}\)C
+
+The average fan power for the simulation time step is calculated for the two-speed cooling tower as follows:
+
+\begin{equation}
+{P_{fan,avg}}\, = \,\omega \,({P_{fan,high}})\, + \,\left( {1 - \omega } \right)\left( {{P_{fan,low}}} \right)
+\end{equation}
+
+The calculation method for the variable-speed Merkel/Scheier model is different from the one- and two-speed models.~ Whereas the other towers are setpoint driven, the variable speed Merkel/Scheier model is driven by the load dispatched from the plant operation scheme, such as PlantEquipmentOperation:CoolingLoad.~ The plant operation scheme provides the cooling tower model with a target load to meet and the tower is controlled to meet that load (as opposed to meeting a leaving setpoint).~ This allows complex configurations with more than one cooling tower to be properly dispatched using all the features available in the various plant operation schemes.~ The model first evaluates the load provided with the fans off using only free convection.~ If the free convection mode meets or exceeds the target load then the tower runs in free convection mode.~ The model then evaluates the load provided by running the fans at full speed.~ If the full fan speed load provided is less than or equal to the target load then the tower runs at full speed.~ The model then evaluates the load provided with the variable speed fan running at the minimum air speed ratio, which is a user input (default is 0.2).~ If the minimum fan speed load provided meets or exceeds the target load, then tower runs at the minimum fan speed.~ If the target load is between the load provided by minimum and maximum fans speeds, then the model solves for an airflow rate ratio that just meets the target load using Regula Falsi numerical method.~ The variable speed Merkel/Scheier model does not model bypass and may provided excess cooling at times when running in free convection or at the minimum fan speed.~ Fan power for the variable speed Merkel/Scheier model is then calculated from the airflow rate ratio using a design fan power and a performance curve or lookup table with one independent variable for the airflow ratio.
+
+\begin{equation}
+{P_{fan}} = {P_{fan,des}} \bullet func\left( {AirFlowRatio} \right)
+\end{equation}
+
+\subsubsection{Tower Basin Heater}\label{tower-basin-heater}
+
+The tower basin heater operates in the same manner as the variable speed cooling tower basin heater. Refer to the variable speed cooling tower basin heater description in the following section.
+
+\subsubsection{Cooling Tower Makeup Water Usage}\label{cooling-tower-makeup-water-usage}
+
+The cooling tower makeup water usage is the same as the variable speed cooling tower makeup water usage. Refer to the variable speed cooling tower makeup water usage description in the following section.
+
+\subsubsection{References}\label{references-015}
+
+Rosaler, Robert C. 1995. Standard Handbook of Plant Engineering, 2\(^{nd}\) Ed. New York, NY: McGraw-Hill, pp.~6-36-37.
+
+\subsection{Variable Speed Cooling Towers Empirical Models}\label{variable-speed-cooling-towers-empirical-models}
+
+\subsubsection{Overview}\label{overview-1-005}
+
+The input object CoolingTower:VariableSpeed provides models for variable speed towers that are based on empirical curve fits of manufacturer's performance data or field measurements. The user specifies tower performance at design conditions, and empirical curves are used to determine the approach temperature and fan power at off-design conditions. The user defines tower performance by entering the inlet air wet-bulb temperature, tower range, and tower approach temperature at the design conditions. The corresponding water flow rate, air flow rate, and fan power must also be specified. The model will account for tower performance in the ``free convection'' regime, when the tower fan is off but the water pump remains on and heat transfer still occurs (albeit at a low level). Basin heater operation and makeup water usage (due to evaporation, drift, and blowdown) are also modeled.
+
+The cooling tower seeks to maintain the temperature of the water exiting the cooling tower at (or below) a setpoint. The setpoint temperature is defined by the setpoints placed on either the tower outlet node or the loop's overall setpoint node (typically set to the supply side outlet node). The model checks to see if the outlet node has a setpoint placed on it and uses that if it does.~ If the outlet node does not have a temperature setpoint then the model uses the loop-level outlet node specified in the input field called Loop Temperature Setpoint Node Name in the PlantLoop or CondenserLoop object. The model simulates the outlet water temperature in four successive steps:
+
+·~~~~~~~~The model first determines the tower outlet water temperature with the tower fan operating at maximum speed. If the outlet water temperature is above the setpoint temperature, the fan runs at maximum speed.
+
+·~~~~~~~~If the outlet water temperature with maximum fan speed is below the setpoint temperature, then the model next determines the impact of ``free convection'' (water flowing through tower with fan off). If the exiting water temperature based on ``free convection'' is at or below the setpoint, then the tower fan is not turned on.
+
+·~~~~~~~~If the outlet water temperature remains above the setpoint after ``free convection'' is modeled, then the tower fan is turned on at the minimum fan speed (minimum air flow rate ratio) to reduce the leaving water temperature. If the outlet water temperature is below the setpoint at minimum fan speed, the tower fan is cycled on and off to maintain the outlet water setpoint temperature.
+
+·~~~~~~~~If the outlet water temperature remains above the setpoint after minimum fan speed is modeled, then the tower fan is turned on and the model determines the required air flow rate and corresponding fan speed to meet the desired setpoint temperature.
+
+\subsubsection{Model Description}\label{model-description-1-005}
+
+The variable speed tower model utilizes user-defined tower performance at design conditions along with empirical curves to determine tower heat rejection and fan power at off-design conditions. Basin heater operation and makeup water usage are also modeled based on user inputs, tower entering air conditions, and tower operation. The following sections describe how each of these tower performance areas is modeled.
+
+\subsubsection{Tower Heat Rejection}\label{tower-heat-rejection}
+
+Heat rejection by the variable speed cooling tower is modeled based on the CoolTools correlation, YorkCalc correlation, or user-defined coefficients for either the CoolTools or YorkCalc correlations. These purely-empirical correlations model the tower approach temperature using a polynomial curve fit with a large number of terms and either three or four independent variables.
+
+The CoolTools correlation has 35 terms with four independent variables:
+
+~~~ Approach = ~~ Coeff(1)~ +~ Coeff(2)•FRair~ +~ Coeff(3)•(FRair)\(^{2}\)~ +
+
+Coeff(4)•(FRair)\(^{3}\)~ +~ Coeff(5)•FRwater~ +
+
+Coeff(6)•FRair•FRwater~ +~ Coeff(7)•(FRair)\(^{2}\)•FRwater~ +
+
+Coeff(8)•(FRwater)\(^{2}\)~ +~ Coeff(9)•FRair•(FRwater)\(^{2}\)~ +
+
+Coeff(10)•(FRwater)\(^{3}\)~ +~ Coeff(11)•Twb~ +~ Coeff(12)•FRair•Twb~ +
+
+Coeff(13)•(FRair)\(^{2}\)•Twb~ +~ Coeff(14)•FRwater•Twb~ +
+
+Coeff(15)•FRair•FRwater•Twb~ +~ Coeff(16)•(FRwater)\(^{2}\)•Twb~ +
+
+Coeff(17)•(Twb)\(^{2}\)~ +~ Coeff(18)•FRair•(Twb)\(^{2}\)~ +
+
+Coeff(19)•FRwater•(Twb)\(^{2}\)~ +~ Coeff(20)•(Twb)\(^{3}\)~ +~ Coeff(21)•Tr~ +
+
+Coeff(22)•FRair•Tr~ +~ Coeff(23)•(FRair)\(^{2}\)•Tr~ +
+
+Coeff(24)•FRwater•Tr~ +~ Coeff(25)•FRair•FRwater•Tr~ +
+
+Coeff(26)•(FRwater)\(^{2}\)•Tr~ +~ Coeff(27)•Twb•Tr~ +
+
+Coeff(28)•FRair•Twb•Tr~ +~ Coeff(29)•FRwater•Twb•Tr~ +
+
+Coeff(30)•(Twb)\(^{2}\)•Tr~ +~ Coeff(31)•(Tr)\(^{2}\) + Coeff(32)•FRair•(Tr)\(^{2}\) +
+
+Coeff(33)•FRwater•(Tr)\(^{2}\) +~ Coeff(34)•Twb•(Tr)\(^{2}\) +~ Coeff(35)•(Tr)\(^{3}\)
+
+where:
+
+Approach = approach temperature (\(^{o}\)C) = outlet water temperature minus inlet air wet-bulb temperature
+
+FRair = air flow rate ratio (actual air flow rate divided by design air flow rate)
+
+FRwater = water flow rate ratio (actual water flow rate divided by design water flow rate)
+
+Tr = range temperature (\(^{o}\)C) = inlet water temperature minus outlet water temperature
+
+Twb = inlet air wet-bulb temperature (\(^{o}\)C)
+
+Coeff(\#) = correlation coefficients
+
+If the user selects Tower Model Type = CoolToolsCrossFlow, then the 35 coefficients derived for the CoolTools simulation model (Benton et al. 2002) are used and these coefficients are already defined within EnergyPlus as shown in Table~\ref{table:approach-temperature-correlation-coefficients}. If the user specifies Tower Model Type = CoolToolsUserDefined, then the user must enter a CoolingTowerPerformance:CoolTools object to define the 35 coefficients that will be used by the CoolTools approach temperature correlation.
+
+% table 63
+\begin{longtable}[c]{p{2.0in}p{2.0in}p{2.0in}}
+
+\caption{Approach Temperature Correlation Coefficients \label{table:approach-temperature-correlation-coefficients}} \tabularnewline
+\toprule 
+Coefficient Number & \multicolumn{2}{c}{Coefficient Value} \tabularnewline
+\cmidrule(r){2-3}
+& CoolTools & YorkCalc \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Approach Temperature Correlation Coefficients} \tabularnewline
+\toprule
+Coefficient Number & \multicolumn{2}{c}{Coefficient Value} \tabularnewline
+\cmidrule(r){2-3}
+& CoolTools & YorkCalc \tabularnewline
+\midrule
+\endhead
+
+Coeff(1) & 0.52049709836241 & -0.359741205 \tabularnewline
+Coeff(2) & -10.617046395344 & -0.055053608 \tabularnewline
+Coeff(3) & 10.7292974722538 & 0.0023850432 \tabularnewline
+Coeff(4) & -2.74988377158227 & 0.173926877 \tabularnewline
+Coeff(5) & 4.73629943913743 & -0.0248473764 \tabularnewline
+Coeff(6) & -8.25759700874711 & 0.00048430224 \tabularnewline
+Coeff(7) & 1.57640938114136 & -0.005589849456 \tabularnewline
+Coeff(8) & 6.51119643791324 & 0.0005770079712 \tabularnewline
+Coeff(9) & 1.50433525206692 & -1.342427256E-05 \tabularnewline
+Coeff(10) & -3.2888529287801 & 2.84765801111111 \tabularnewline
+Coeff(11) & 0.02577861453538 & -0.121765149 \tabularnewline
+Coeff(12) & 0.18246428931525 & 0.0014599242 \tabularnewline
+Coeff(13) & -0.08189472914009 & 1.680428651 \tabularnewline
+Coeff(14) & -0.21501000399629 & -0.0166920786 \tabularnewline
+Coeff(15) & 0.01867413096353 & -0.0007190532 \tabularnewline
+Coeff(16) & 0.053682417759 & -0.025485194448 \tabularnewline
+Coeff(17) & -0.00270968955115 & 4.87491696E-05 \tabularnewline
+Coeff(18) & 0.00112277498589 & 2.719234152E-05 \tabularnewline
+Coeff(19) & -0.00127758497498 & -0.06537662555556 \tabularnewline
+Coeff(20) & 7.60420796601607E-05 & -0.002278167 \tabularnewline
+Coeff(21) & 1.43600088336017 & 0.0002500254 \tabularnewline
+Coeff(22) & -0.5198695909109 & -0.0910565458 \tabularnewline
+Coeff(23) & 0.11733957691051 & 0.00318176316 \tabularnewline
+Coeff(24) & 1.50492810819924 & 3.8621772E-05 \tabularnewline
+Coeff(25) & -0.13589890592697 & -0.0034285382352 \tabularnewline
+Coeff(26) & -0.15257758186651 & 8.56589904E-06 \tabularnewline
+Coeff(27) & -0.05338438281146 & -1.516821552E-06 \tabularnewline
+Coeff(28) & 0.00493294869566 & N/A \tabularnewline
+Coeff(29) & -0.00796260394174 & N/A \tabularnewline
+Coeff(30) & 0.00022261982862 & N/A \tabularnewline
+Coeff(31) & -0.05439520015681 & N/A \tabularnewline
+Coeff(32) & 0.00474266879162 & N/A \tabularnewline
+Coeff(33) & -0.01858546718156 & N/A \tabularnewline
+Coeff(34) & 0.00115667701294 & N/A \tabularnewline
+Coeff(35) & 0.00080737066446 & N/A \tabularnewline
+\bottomrule
+\end{longtable}
+
+Similarly, the YorkCalc correlation has 27 terms with three independent variables:
+
+~~~ Approach = ~~ Coeff(1)~ +~ Coeff(2)•Twb +~ Coeff(3)•Twb\(^{2}\)~ +~ Coeff(4)•Tr~ +
+
+Coeff(5)•Twb•Tr~ +~ Coeff(6)•Twb\(^{2}\)•Tr~ +~ Coeff(7)•Tr\(^{2}\)~ +
+
+Coeff(8)•Twb•Tr\(^{2}\) +~ Coeff(9)•Twb\(^{2}\)•Tr\(^{2}\) +~ Coeff(10)•LGRatio~ +
+
+Coeff(11)•Twb•LGRatio~ + Coeff(12)•Twb\(^{2}\)•LGRatio~ +
+
+Coeff(13)•Tr•LGRatio~ +~ Coeff(14)•Twb•Tr•LGRatio~ +
+
+Coeff(15)•Twb\(^{2}\)•Tr•LGRatio~ +~ Coeff(16)•Tr\(^{2}\)•LGRatio~ +
+
+Coeff(17)•Twb•Tr\(^{2}\)•LGRatio~ + Coeff(18)•Twb\(^{2}\)•Tr\(^{2}\)•LGRatio +
+
+Coeff(19)•LGRatio\(^{2}\) +~ Coeff(20)•Twb•LGRatio\(^{2}\)~ +
+
+Coeff(21)• Twb\(^{2}\)•LGRatio\(^{2}\) +~ Coeff(22)•Tr•LGRatio\(^{2}\) +
+
+Coeff(23)•Twb•Tr•LGRatio\(^{2}\) +~ Coeff(24)•Twb\(^{2}\)•Tr•LGRatio\(^{2}\) +
+
+Coeff(25)•Tr\(^{2}\)•LGRatio\(^{2}\) +~ Coeff(26)•Twb•Tr\(^{2}\)•LGRatio\(^{2}\) +
+
+Coeff(27)•Twb\(^{2}\)•Tr\(^{2}\)•LGRatio\(^{2}\)
+
+where:
+
+~~~~~~~~~~~ Approach = approach temperature (\(^{o}\)C) = outlet water temperature minus inlet air wet-bulb temperature
+
+~~~~~~~~~~~ Tr = range temperature (\(^{o}\)C) = inlet water temperature minus outlet water temperature
+
+~~~~~~~~~~~ Twb = inlet air wet-bulb temperature (\(^{o}\)C)
+
+~~~~~~~~~~~ LGratio = liquid-to-gas ratio = ratio of water flow rate ratio (FRwater) to air flow rate ratio (FRair)
+
+~~~~~ Coeff(\#) = correlation coefficients
+
+If the user selects Tower Model Type = YorkCalc, then the 27 coefficients derived for the YorkCalc simulation model (York International Corp. 2002) are used and these coefficients are already defined within EnergyPlus as shown in Table~\ref{table:approach-temperature-correlation-coefficients}. If the user specifies Tower Model Type = YorkCalcUserDefined, then the user must enter a CoolingTowerPerformance:YorkCalc object to define the 27 coefficients that will be used by the YorkCalc approach temperature correlation.
+
+The approach temperature correlations for the CoolTools and YorkCalc simulation models are valid for a range of conditions defined in Table~\ref{table:minimum-and-maximum-limits-for-approach}. If the user defines their own model coefficients (CoolingTowerPerformance:CoolTools or CoolingTowerPerformance:YorkCalc), then they must also define in that same object the range of conditions for which the model is valid. For all of these correlation variables, the program issues warnings if the actual values are beyond the minimum/maximum values specified for the correlation being used. For inlet air wet-bulb temperature and water mass flow rate ratio, the values of these variables used in the calculation of approach temperature are limited to be within the valid minimum/maximum range. For approach, range, and liquid-to-gas ratio the warnings are issued if the values are beyond the specified minimum/maximum range but the actual values are still used. The warnings issued do not necessarily indicate a poor estimate of tower performance at the condition(s) which caused the warning, but are provided to identify conditions outside the defined correlation limits. Exceeding the defined limits by a small amount may not introduce significant errors, but large deviations may be problematic. It is for this reason that we recommend using a very broad range of cooling tower performance data (i.e., data covering the entire range expected during the simulation) when generating user-defined coefficients for the variable speed tower model.
+
+% table 64
+\begin{longtable}[c]{@{}lll@{}}
+\caption{Minimum and Maximum Limits for Approach Temperature Correlation Variables \label{table:minimum-and-maximum-limits-for-approach}} \tabularnewline
+\toprule 
+Independent Variable Limit & CoolTools & YorkCalc \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Minimum and Maximum Limits for Approach Temperature Correlation Variables} \tabularnewline
+\toprule 
+Independent Variable Limit & CoolTools & YorkCalc \tabularnewline
+\midrule
+\endhead
+
+Minimum Inlet Air Wet-Bulb Temperature & -1.0°C & -34.4°C \tabularnewline
+Maximum Inlet Air Wet-Bulb Temperature & 26.7°C & 26.7°C \tabularnewline
+Minimum Tower Range Temperature & 1.1°C & 1.1°C \tabularnewline
+Maximum Tower Range Temperature & 11.1°C & 22.2°C \tabularnewline
+Minimum Tower Approach Temperature & 1.1°C & 1.1°C \tabularnewline
+Maximum Tower Approach Temperature & 11.1°C & 40°C \tabularnewline
+Minimum Water Flow Rate Ratio & 0.75 & 0.75 \tabularnewline
+Maximum Water Flow Rate Ratio & 1.25 & 1.25 \tabularnewline
+Maximum Liquid-to-Gas Ratio & N/A & 8.0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The approach temperature correlation(s) used to simulate cooling tower heat rejection are based on water and air flow rate ``ratios'' and are not directly dependent on the size of the tower or the actual air and water flow rates through the tower. However, the model correlations are developed based on a reference condition. For Model Types ``CoolToolsCrossFlow'' and ``YorkCalc'', the reference condition is a water flow rate of 0.000043 m\(^{3}\)/s per kW of heat rejected (2.4 gal/min per ton of heat rejected) with 25.6\(^{o}\)C (78\(^{o}\)F) enter air wet-bulb temperature, 35\(^{o}\)C (95\(^{o}\)F) hot water inlet temperature, and 29.4\(^{o}\)C (85\(^{o}\)F) cold water outlet temperature. The reference condition may be different if the user defines tower model coefficients using CoolingTowerPerformance:CoolTools or CoolingTowerPerformance:YorkCalc.
+
+Due to the inherent reference condition used to generate the tower performance curves, the water flow rate at the reference condition must be determined using the design performance information specified by the user and the tower model's approach temperature correlation. This is done by using the model's approach temperature correlation (described earlier in this section) to calculate the water flow rate ratio which yields the user-defined design approach temperature based on an air flow rate ratio of 1.0 (\emph{FR\(_{air}\)} = 1.0), the design inlet air wet-bulb temperature, and the design range temperature. The calculated approach temperature (using the model correlation) must satisfy the following two equations:
+
+\({T_{water,outlet,design}} = {T_{wb,air,design}} + {T_{approach,design}}\quad \{ F{R_{air}} = 1.0\}\) \({T_{water,inlet,design}} = {T_{wb,air,design}} + {T_{approach,design}} + {T_{range,design}}\quad \{ F{R_{air}} = 1.0\}\)
+
+where:
+
+\({T_{water,outlet,design}}\) = design outlet water temperature (\(^{o}\)C)
+
+\({T_{water,inlet,design}}\) = design inlet water temperature (\(^{o}\)C)
+
+\({T_{wb,air,design}}\) = design inlet air wet-bulb temperature (\(^{o}\)C)
+
+\({T_{approach,design}}\) = design approach temperature (\(^{o}\)C)
+
+\({T_{range,design}}\) = design range temperature (\(^{o}\)C)
+
+\(F{R_{air}}\) = air flow rate ratio (actual air flow rate divided by design air flow rate)
+
+The water flow rate ratio used in the approach temperature correlation which satisfies these two equations is the ratio of the design water flow rate (specified by the user) to the water flow rate at the reference condition. This ratio is used to calculate the reference water volumetric flow rate, which is then used throughout the simulation to determine the actual water flow rate ratio used in the approach temperature correlation for each simulation time step.
+
+\begin{equation}
+{\dot V_{reference}} = \frac{{{{\dot V}_{design}}}}{{F{R_{water\;reference}}}}
+\end{equation}
+
+where:
+
+\({\dot V_{reference}}\) = water volumetric flow rate at the reference condition (m\(^{3}\)/s)
+
+\({\dot V_{design}}\) = design water volumetric flow rate specified by the user (m\(^{3}\)/s)
+
+\(F{R_{water,reference}}\) = design water flow rate divided by the reference water flow rate
+
+The cooling tower seeks to maintain the temperature of the water exiting the cooling tower at (or below) a setpoint. The setpoint temperature is defined by the field ``Condenser Loop Temperature Setpoint schedule or reference'' for the CondenserLoop object. The model simulates the outlet water temperature in four successive steps:
+
+·~~~~~~~~The model first determines the tower outlet water temperature with the tower fan operating at maximum speed. If the outlet water temperature is above the setpoint temperature, the fan runs at maximum speed.
+
+·~~~~~~~~If the outlet water temperature with maximum fan speed is below the setpoint temperature, then the model next determines the impact of ``free convection'' (water flowing through tower with fan off). If the exiting water temperature based on ``free convection'' is at or below the setpoint, then the tower fan is not turned on.
+
+·~~~~~~~~If the outlet water temperature remains above the setpoint after ``free convection'' is modeled, then the tower fan is turned on at the minimum fan speed (minimum air flow rate ratio) to reduce the leaving water temperature. If the outlet water temperature is below the setpoint at minimum fan speed, the tower fan is cycled on and off to maintain the outlet water setpoint temperature.
+
+·~~~~~~~~If the outlet water temperature remains above the setpoint after minimum fan speed is modeled, then the tower fan is turned on and the model determines the required air flow rate and corresponding fan speed to meet the desired setpoint temperature.
+
+For each simulation time step, the model first calculates the outlet water temperature with the tower fan operating at maximum speed (FRair = 1.0). The calculated approach temperature (using the correlations described above), inlet air wet-bulb temperature (weather data), and range temperature are used to determine the tower outlet water temperature as follows:
+
+\begin{equation}
+  \begin{array}{rl}
+    T_{water,outlet,fanMAX} &= T_{wb,air} + T_{approach} \quad FR_{air} = 1.0 \\
+                              &= {T_{water,inlet}} + {T_{range}}
+  \end{array}
+\end{equation}
+
+where:
+
+\({T_{water,outlet,fanMAX}}\) ~ = tower outlet water temperature at maximum fan speed (\(^{o}\)C)
+
+\({T_{wb,air}}\) ~ = tower inlet air wet-bulb temperature (\(^{o}\)C)
+
+\({T_{approach}}\) = approach temperature at current operating conditions (\(^{o}\)C)
+
+\({T_{range}}\) = range temperature at current operating conditions (\(^{o}\)C)
+
+Note that the approach temperature correlation as described previously is a function of range temperature, so the equations above must be solved iteratively to converge on a solution. If the resulting outlet water temperature is above the desired setpoint temperature, then the fan runs at maximum speed and does not cycle on/off (fan part-load ratio = FanPLR = 1.0 and \emph{FR\(_{air}\)} = 1.0).
+
+If the outlet water temperature with maximum fan speed is below the setpoint temperature, then the model next determines the impact of ``free convection'' (water flowing through tower with fan off). In the free convection regime, the outlet water temperature is calculated using a fraction of the water temperature difference through the tower when the fan is at its maximum speed. This fraction is defined by the user (Fraction of Tower Capacity in Free Convection Regime).
+
+\begin{equation}
+{T_{water,outlet,fanOFF}} = {T_{water,inlet}}\,\,\,\, - \,\,\left[ {Fra{c_{freeconv}}\left( {{T_{water,inlet}}\,{\rm{ - }}\,\,{T_{water,outlet,fanMAX}}} \right)} \right]
+\end{equation}
+
+where:
+
+\({T_{water,outlet,fanOFF}}\) ~ = tower outlet water temperature in free convection regime (\(^{o}\)C)
+
+\({T_{water,inlet}}\) ~ = tower inlet water temperature (\(^{o}\)C)
+
+\(Fra{c_{freeconv}}\) = fraction of tower capacity in free convection regime (user specified)
+
+If the outlet water temperature in the free convection regime is below the setpoint temperature, the tower fan is not turned on and the fan part-load ratio is set equal to 0. In addition, the air flow rate ratio through the tower is assumed to be equal to the fraction of tower capacity in the free convection regime.
+
+\begin{equation}
+FanPLR\,\, = \,\,FanPL{R_{freeconv}} = 0.0
+\end{equation}
+
+\begin{equation}
+F{R_{air}}\, = F{R_{air,freeconv}} = Fra{c_{freeconv}}
+\end{equation}
+
+where:
+
+\(FanPLR\) = fan part-load ratio
+
+\(FanPL{R_{freeconv}}\) = fan part-load ratio in free convection regime
+
+\(F{R_{air,freeconv}}\) ~ = air flow rate ratio in free convection regime
+
+If the outlet water temperature in the free convection regime is above the setpoint temperature, then the fan is turned on at the minimum fan speed (minimum air flow rate ratio, FR\(_{air,min}\) , entered by the user) and the outlet water temperature is calculated as the inlet air wet-bulb temperature plus the calculated approach temperature:
+
+\begin{equation}
+F{R_{air}} = F{R_{air,\min }}
+\end{equation}
+
+\begin{equation}
+{T_{water,outlet,fanMIN}} = {T_{wb,air}}{\rm{ + }}\,{T_{approach}}\,\,\,\,\{ F{R_{air}}\, = \,F{R_{air,\min }}\}
+\end{equation}
+
+where:
+
+\({T_{water,outlet,FanMIN}}\) ~ = outlet water temperature at minimum fan speed (\(^{o}\)C)
+
+\(F{R_{air,\min }}\) ~ = air flow rate ratio at the minimum fan speed
+
+If the outlet water temperature at minimum fan speed is below the setpoint temperature, the cooling tower fan cycles on and off at the minimum air flow rate ratio in order to meet the setpoint temperature.
+
+\begin{equation}
+FanPLR = \left( {\frac{{{T_{water,outlet,fanOFF}} - {T_{{\rm{setpoint}}}}}}{{{T_{water,outlet,fanOFF}} - {T_{water,outlet,fanMIN}}}}} \right)
+\end{equation}
+
+where:
+
+\({T_{{\rm{setpoint}}}}\) ~ = outlet water setpoint temperature (\(^{o}\)C)
+
+If the outlet water temperature at minimum fan speed is above the outlet water temperature setpoint, then the cooling tower fan speed (\emph{FR\(_{air}\)}) is increased until the calculated approach temperature produces the required outlet water temperature to meet the setpoint.
+
+\begin{equation}
+{T_{approach}} = f\left( {F{R_{air}}} \right)
+\end{equation}
+
+\begin{equation}
+{T_{water,outlet}} = {T_{{\rm{setpoint}}}}\, = {T_{wb,air}}{\rm{ + }}\,{T_{approach}}
+\end{equation}
+
+\(FanPLR = 1.0\) ~\emph{(i.e., fan does not cycle on/off)}
+
+\subsubsection{Fan Power}\label{fan-power}
+
+When the cooling tower fan is operating, fan electric power is calculated based on the air flow rate ratio required to meet the above conditions. If the user has entered a fan power curve object (cubic curve), the output of that curve is multiplied by the design fan power. Otherwise, tower fan power is assumed to be directly proportional to the cube of the air flow rate ratio. In either case, the fan part-load ratio is applied to account for times when the tower fan cycles on/off to meet the setpoint temperature. Fan energy consumption is calculated each simulation time step.
+
+If FanPowerCurveObject is defined, then:
+
+\begin{equation}
+  P_{fan} = \left( {CurveOutput} \right)\left( {FanPLR} \right){P_{fan,design}}
+\end{equation}
+
+Else:
+
+\begin{equation}
+  P_{fan} = \left( {{P_{fan,design}}} \right)\left( {FanPLR} \right){\left( {F{R_{air}}} \right)^{\rm{3}}}
+\end{equation}
+
+\begin{equation}
+{E_{fan}} = \left( {{P_{fan}}} \right)\left( {TimeStepSys} \right)3600.
+\end{equation}
+
+where:
+
+\(FanPowerCurveObject\) ~ = name of fan power ratio as a function of air flow rate ratio curve
+
+\({P_{fan}}\) ~ = tower fan electric power (W)
+
+\({E_{fan}}\) ~ = tower fan electric consumption (J)
+
+\(CurveOutput\) ~ = output of FanPowerCurveObject evaluated at the operating air flow rate ratio (\emph{FR\(_{air}\)})
+
+\({P_{fan,design}}\) ~ = design fan power at design (maximum) air flow through the tower (W)
+
+\emph{TimeStepSys} = HVAC system simulation time step (hr)
+
+\subsubsection{Tower Basin Heater}\label{tower-basin-heater-1}
+
+Calculations are also made to estimate the electric power input to the tower basin heater. A schedule may be used to disable the basin heater during regular maintenance periods or other time periods (e.g., during summer). If a schedule is not provided, the basin heater is assumed to be available the entire simulation time period. The basin heater operates when it is scheduled on, the outdoor air dry-bulb temperature is below the basin heater setpoint temperature, and the cooling tower is not active (i.e., water is not flowing through the tower). The user is required to enter a basin heater capacity (watts per degree Kelvin) and a heater setpoint temperature (\(^{o}\)C) if they want to model basin heater electric power.
+
+\begin{lstlisting}
+P_heater_basin =0.0
+IF (WaterNotFlowingThroughTower) THEN
+  IF (Scheduleheater_basin is Defined) THEN
+    IF (CAPheater_basin > 0 AND Scheduleheater_basin = ON) THEN
+      P_heater_basin = MAX(0.0,CAP_heater_basin*(T_setpoint_basin-T_db_outdoor))
+    ENDIF
+  ELSE
+    IF (CAPheater_basin > 0) THEN
+      P_heater_basin = MAX(0.0,CAP_heater_basin*(T_setpoint_basin-T_db_outdoor))
+    ENDIF
+  ENDIF
+ENDIF
+\end{lstlisting}
+
+\begin{equation}
+{E_{{\rm{heater,basin}}}} = \left( {{P_{{\rm{heater,basin}}}}} \right)\left( {TimeStepSys} \right){\rm{3600}}{\rm{.}}
+\end{equation}
+
+where:
+
+\({P_{{\rm{heater,basin}}}}\) ~ = tower basin heater electric power (W)
+
+\({E_{{\rm{heater,basin}}}}\) ~ = tower basin heater electric consumption (J)
+
+\emph{T\(_{setpoint,basin}\)} = basin heater setpoint temperature (\(^{o}\)C)
+
+\emph{T\(_{db,outdoor}\)}~~~ = outdoor air dry-bulb temperature (\(^{o}\)C)
+
+CAP\emph{\(_{heater,basin}\)} = basin heater capacity (W/K)
+
+\emph{Schedule\(_{heater,basin}\)} = basin heater schedule (schedule value \textgreater{} 0 means ON)
+
+\subsubsection{References}\label{references-1-005}
+
+ASHRAE 1999. HVAC1 Toolkit: A Toolkit for Primary HVAC System Energy Calculations. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Benton, D.J., Bowman, C.F., Hydeman, M., Miller, P. 2002. An Improved Cooling Tower Algorithm for the CoolTools\(^{TM}\) Simulation Model. \emph{ASHRAE Transactions,} Vol. 108, Part 1, pp.760-768.
+
+Bourdouxhe, J.P., M. Grodent, J. Lebrun and C. Silva. 1994. Cooling tower model developed in a toolkit for primary HVAC system energy calculation: part 1. Proceedings of the fourth international conference on system simulation in buildings, Liege (Belgium), December 5-7, 1994.
+
+Incropera, F.P. and D.P. DeWitt. 1981. Fundamentals of Heat Transfer. New York: John Wiley \& Sons.
+
+Merkel, F.~ 1925. Verduftungskuhlung. VDI Forschungarbeiten, No 275, Berlin.
+
+Rosaler, Robert C. 1995. Standard Handbook of Plant Engineering, 2\(^{nd}\) Ed. New York, NY: McGraw-Hill, pp.~6-36-37.
+
+Scheier, L. 2013. Personal communication.
+
+York International Corporation, 2002. ``YORKcalc\(^{TM}\) Software, Chiller-Plant Energy-Estimating Program'', Form 160.00-SG2 (0502).
+
+\subsection{Cooling Towers with Multiple Cells}\label{cooling-towers-with-multiple-cells}
+
+Many towers are constructed to be capable of being grouped together to achieve the desired capacity. Thus, many cooling towers are assemblies of two or more individual cooling towers or ``cells.'' The number of cells they have, e.g., an eight-cell tower, often refers to such towers.
+
+For the operation of multi-cell towers, the first step is to determine the number of cells \emph{n,} which will be operating during the timestep using the calculation logic from DOE-2.1E.
+
+The maximum and minimum flow rates per cell are determined according to the input fractions (\emph{Minimum~ Water Flow Rate Fraction:}\({k_{min}}\) \emph{~}~and \emph{Maximum~ Water Flow Rate Fraction:} \({k_{max}}\) ) as follows:
+
+\begin{equation}
+    \begin{array}{rl}
+      \dot{m}_{w,min} &= \frac{\dot{m}_{w,des}}{n_{tot}} \times k_{min} \\
+      \dot{m}_{w,max} &= \frac{\dot{m}_{w,des}}{n_{tot}} \times k_{max}
+    \end{array}
+\end{equation}
+
+where \({{{\dot m}_{w,des}}}\) ~is the design water flow rate through the entire cooling tower.
+
+Then, we determine the minimum and maximum number of cells that can operate with this water flow rate:
+
+\begin{equation}
+    \begin{array}{rl}
+      n_{min} & = \min\PB{\frac{\dot{m}_{w,tot}}{\dot{m}_{w,max}},n_{tot}} \\
+      n_{max} & = \min\PB{\frac{\dot{m}_{w,tot}}{\dot{m}_{w,min}},n_{tot}}
+    \end{array}
+\end{equation}
+
+where \emph{n\(_{tot}\)} is the total number of cells of the tower, and\({{{\dot m}_{w,tot}}}\) ~is the water flow rate to the tower.
+
+The number of cells operating\emph{n} is set accordingly:
+
+If the \emph{Cell Control} method is \emph{MinimalCell,}
+
+\emph{n =} \({{n_{min}}}\)
+
+If the \emph{Cell Control} method is \emph{MaximalCell,}
+
+\emph{n =} \({{n_{max}}}\)
+
+Finally, the water mass flow rate per cell (\({{\dot m}_w})\) ~will be:
+
+\begin{equation}
+{{\dot m}_w} = \frac{{{{\dot m}_{w,tot}}}}{n}
+\end{equation}
+
+Then we simulate the performance of one cell with this flow rate per cell (calling the SimSimpleTower subroutine for single and two speed cooling tower objects). As we assume that each cell is identical, the UA of one cell is calculated dividing the UA of the whole tower (obtained from the input or from the auto sizing calculations). The air flow rate per cell is also equal to the one of the whole tower divided by the number of cells operating:
+
+\begin{equation}
+U{A_{cell}} = \frac{{U{A_{cell}}}}{{{n_{tot}}}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{air,cell}} = \frac{{{{\dot m}_{air,tot}}}}{n}
+\end{equation}
+
+At the end, the total fan power of the tower operating with a certain number of cells is given by:
+
+\begin{equation}
+FanPower = FanPowe{r_{tot}} \times \frac{n}{{{n_{tot}}}}
+\end{equation}
+
+If the cells operating do not meet the loads, we increase the number of cells if spare cells are available and the water flow through each cell is within the user specified minimum and maximum water flow rate fractions range. This is an iteration process.
+
+\subsection{Cooling Tower Makeup Water Usage}\label{cooling-tower-makeup-water-usage-1}
+
+Makeup water use for all types of cooling towers is made up of three components: evaporation, drift, and blowdown. ~The first is the amount of water evaporated to reduce the water's temperature as it passes through the cooling tower. There are two methods that evaporation makeup water can be modeled in EnergyPlus.~ The first method assumes that the tower outlet air conditions are saturated (which may not always be the case for certain operating conditions). ~For this ``Saturated Exit'' mode, the enthalpy of the tower's outlet air is calculated as the inlet air enthalpy plus the water side heat transfer divided by the air mass flow rate through the tower.
+
+\begin{equation}
+{\dot Q_{water}} = {\dot m_{_{water}}}{C_p}\left( {{T_{{\rm{water,inlet}}}} - {T_{{\rm{water,outlet}}}}} \right)
+\end{equation}
+
+\begin{equation}
+{h_{sat\,air,outlet}} = {h_{air,inlet}} + \left( {\frac{{{{\dot Q}_{water}}}}{{{{\dot m}_{air}}}}} \right)
+\end{equation}
+
+where:
+
+\({\dot Q_{water}}\) ~ = water-side heat transfer (W)
+
+\({\dot m_{_{water}}}\) ~ = mass flow rate of water through the tower (kg/s)
+
+\({C_p}\) ~ = specific heat of water (W/kg-K)
+
+\({h_{sat\,air,outlet}}\) ~ = saturated outlet air enthalpy (J/kg)
+
+\({h_{air,inlet}}\) ~ = inlet air enthalpy (J/kg)
+
+\({\dot m_{air}}\) ~ = mass flow rate of air through the tower (kg/s)
+
+The saturation temperature and humidity ratio are then calculated for the tower's outlet air.
+
+\begin{equation}
+{T_{sat\,air,outlet}} = PsyTsatFnHPb\left( {{h_{sat\,air,outlet}},{\rm{OutBaroPress}}} \right)
+\end{equation}
+
+\begin{equation}
+{\omega_{sat\,air,outlet}} = PsyWFnTdbH\left( {{T_{sat\,air,outlet}},{h_{sat\,air,outlet}}} \right)
+\end{equation}
+
+where:
+
+\({T_{sat\,air,outlet}}\) ~ = saturated outlet air temperature (\(^{o}\)C)
+
+\(PsyTsatFnHPb\) ~ = EnergyPlus psychrometric function, returns saturation temperature given enthalpy and barometric pressure
+
+\({\rm{OutBaroPress}}\) ~ = outdoor barometric pressure (Pa)
+
+\({\omega_{sat\,air,outlet}}\) ~ = saturated outlet air humidity ratio (kg\(_{water}\)/kg\(_{dry\, air}\))
+
+\(PsyWFnTdbH\) ~ = EnergyPlus psychrometric function, returns humidity ratio given dry-bulb temperature and enthalpy
+
+The makeup water quantity required to replenish the water lost due to evaporation is then calculated as the product of the air mass flow rate and the difference between the entering and leaving air humidity ratio divided by the density of water.
+
+\begin{equation}
+{\dot V_{evaporation,makeup}} = \frac{{{{\dot m}_{air}}\left( {{\omega_{sat\,air,outlet}} - {\omega_{air,inlet}}} \right)}}{{{\rho_{water}}}}
+\end{equation}
+
+where:
+
+\({\dot V_{evaporation,makeup}}\) ~ = makeup water usage due to evaporation (m\(^{3}\)/s)
+
+\({\dot m_{air}}\) ~ = mass flow rate of air through tower (kg/s)
+
+\({\omega_{air,inlet}}\) ~ = humidity ratio of tower inlet air (kg\(_{water}\)/kg\(_{dry\, air}\))
+
+\({\rho_{water}}\) ~ = density of water evaluated at the tower inlet air temperature (kg/m\(^{3}\))
+
+The second method available for calculating water makeup for evaporation is for the user to provide a value for a loss factor.~ The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water.~ The value provided by the user is in units of percent-per-degree Kelvin.~ The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water.~ Typical values are from 0.15 to 0.27 {[}percent/K{]}. The default is 0.2.~ The rate of water makeup for evaporation is then calculated by multiplying this factor times the condenser water flow rate and the temperature decrease in the condenser water flow rate. For evaporative fluid coolers, a numerical value of loss factor can be entered in the same manner as for cooling towers. If this field is blank, an empirical correlation will be used to calculate the value based on current outdoor dry bulb temperature and relative humidity. The following correlation from Qureshi and Zubair (2007) is used to calculate the loss factor:
+
+\begin{equation}
+Loss\;Factor = (113 - 8.417\phi  + 1.6147{t_{db}})*{10^{ - 5}}
+\end{equation}
+
+where:
+
+\(\phi\) ~ = relative humidity of inlet air
+
+\({t_{db}}\) ~ = Dry-bulb temperature of inlet air
+
+Additional makeup water usage is modeled as a percentage of design water flow rate through the tower to account for drift, and as a scheduled flow rate to model blowdown. Drift is water loss due to the entrainment of small water droplets in the air stream passing through the tower. Drift is defined by the model user as a percentage of the tower's design water flow rate, and is assumed to vary with tower air flow rate ratio as follows:
+
+\begin{equation}
+{\dot V_{drift,makeup}} = {\dot m_{water,design}}\left( {\frac{{PercentWatertoDrift}}{{100.0}}} \right)F{R_{air}}
+\end{equation}
+
+where:
+
+\({\dot V_{drift,makeup}}\) ~ = makeup water usage due to drift (m\(^{3}\)/s)
+
+\({\dot m_{water,design}}\) ~ = design (volumetric) water flow rate (m\(^{3}\)/s)
+
+\(PercentWatertoDrift\) ~ = percent of design water flow rate lost to drift at the tower design air flow rate
+
+\(F{R_{air}}\) = ratio of actual air flow rate to tower design air flow rate
+
+Blowdown is water flushed from the basin on a periodic basis to purge the concentration of mineral scale or other contaminants. There are two ways that blowdown is calculated in EnergyPlus.~ Blowdown water rates can be scheduled so that we have:.
+
+If ScheduleBlowdown is defined, then:
+
+\begin{equation}
+  \dot{V}_{blowdown,makeup} = ScheduleValue_{blowdown}
+\end{equation}
+
+Else:
+
+\begin{equation}
+  \dot{V}_{blowdown,makeup} = 0.0
+\end{equation}
+
+where:
+
+\({\dot V_{blowdown,makeup}}\) ~ = makeup water usage due to blowdown (m\(^{3}\)/s)
+
+\emph{ScheduleValue\(_{blowdown}\)} = blowdown schedule value for the time step being simulated (m\(^{3}\)/s)
+
+The second (and default) way that blowdown can be calculated is to assume that blowdown water is continually introduced at a rate that will provide a constant concentration ratio.~ As water evaporates it leaves behind minerals and the like causing the concentration of water impurities to be higher in the tower than in the makeup water.~ Acceptable concentration ratios are in the range of 3 to 5 depending on the purity of the make up water.~ Water lost as drift does not evaporate and decrease the water needed for blowdown.~ Using the ``Concentration Ratio'' method, the rate of blowdown can be calculated using:
+
+\begin{equation}
+{\dot V_{blowdown,makeup}} = \frac{{{{\dot V}_{evaporation,makeup}}}}{{{R_{concentration}} - 1}} - {\dot V_{drift,makeup}}
+\end{equation}
+
+where,
+
+\({R_{concentration}}\) ~is the concentration ratio or the ratio of solids in the blowdown water to solids in the makeup water.
+
+The tower makeup water consumption (m\(^{3}\)) for each simulation time step is calculated as the sum of the individual components of makeup water usage multiplied by the simulation time step in hours and the conversion for hours to seconds (3600 sec/hr). Makeup water usage is only calculated when the cooling tower is active and water is flowing through the cooling tower.
+
+\begin{equation}
+{V_{water,\;makeup}} = \left( {{{\dot V}_{evaporation,makeup}} + {{\dot V}_{drift,makeup}} + {{\dot V}_{blowdown,makeup}}} \right)\cdot TimeStepSys\cdot 3600.
+\end{equation}
+
+where:
+
+\({V_{water,makeup}}\) ~ = tower makeup water consumption (m\(^{3}\))
+
+\subsubsection{References}\label{references-2-003}
+
+Robert C. Rosaler. 1995. Standard Handbook of Plant Engineering, 2\(^{nd}\) Ed. McGraw-Hill, New York, NY, pp 6-36-37.
+
+Quereshi, B.A. and S.M.Zubair. 2007. Prediction of evaporation losses in evaporative fluid coolers, Applied Thermal Engineering 27 pp.~520-527
+
+\subsection{One and Two Speed Fluid Coolers}\label{one-and-two-speed-fluid-coolers}
+
+\subsubsection{Overview}\label{overview-2-005}
+
+The input objects FluidCooler:SingleSpeed and FluidCooler:TwoSpeed provide models for dry fluid coolers. Fluid cooler's performance is modeled using effectiveness-NTU relationships for cross flow heat exchanger with both streams unmixed. The model can be used to simulate the performance of both single speed and two speed mechanical-draft fluid coolers. For part-load operation, the model assumes a simple linear interpolation between two steady-state regimes without accounting for any cycling losses.
+
+\subsubsection{Model Description}\label{model-description-2-005}
+
+The expression for fluid cooler effectiveness is as follows:
+
+\begin{equation}
+  \varepsilon = 1-\exp{\CB{ \frac{\exp{\PB{-NTU C_r \eta}}-1}{C_{r}^{\eta}} }}
+\end{equation}
+
+Where
+
+\(\varepsilon\) \(\varepsilon\) \emph{~} = heat exchanger effectiveness
+
+\begin{equation}
+{C_r} = \frac{{{{\dot C}_{\min }}}}{{{{\dot C}_{\max }}}}
+\end{equation}
+
+\({\dot C_a} = {\dot m_a}{c_{pa}}\) \({\dot C_a} = {\dot m_a}{c_{pa}}\) ~and\({\dot C_w} = {\dot m_w}{c_{pw}}\)
+
+\({\dot C_{\max }} = Max({\dot C_a},{\dot C_w})\) \({\dot C_{\max }} = Max({\dot C_a},{\dot C_w})\) ;\({\dot C_{\min }} = Min({\dot C_a},{\dot C_w})\)
+
+\begin{equation}
+NTU = \frac{{UA}}{{{{\dot C}_{\min }}}}
+\end{equation}
+
+\(\eta = NT{U^{( - 0.22)}}\) \(\eta = NT{U^{( - 0.22)}}\)
+
+The first fluid is water and the second fluid is air entering the heat exchanger at temperature \({T_{db,in}}\) \({T_{db,in}}\) ~and specific heat \({c_{pa}}\) \({c_{pa}}\) . The heat exchanger is characterized by a single parameter, its overall heat transfer coefficient-area product UA.
+
+When the user selects the nominal capacity method, the UA is calculated as follows:
+
+The model inputs (other than the UA) and the fluid cooler load that it must meet are specified at design conditions. Then the fluid cooler model converges to a UA value, using the regulafalsi method that will enable it to meet the design fluid cooler load given at the specified inputs.
+
+\subsubsection{Method for Calculating Steady-State Exiting Water Temperature}\label{method-for-calculating-steady-state-exiting-water-temperature-1}
+
+The objective of the fluid cooler model is to predict the exiting water temperature and the fan power required to meet the exiting water setpoint temperature. The exiting water temperature is calculated based on an energy balance that assumes that the energy absorbed by the air is equivalent to the energy removed from the water. The procedure for calculating the steady-state, exiting air dry-bulb temperature is outlined below.
+
+With the overall heat transfer coefficient-area product for the fluid cooler calculated by the nominal capacity information entered by the user, the effectiveness of the heat exchanger is then calculated as:
+
+\begin{equation}
+  \varepsilon = 1-\exp{\CB{ \frac{\exp{\PB{-NTU C_r \eta}}-1}{C_{r}^{\eta}} }}
+\end{equation}
+
+The heat transfer rate is then calculated as follows:
+
+\(\dot Q = \varepsilon {\dot C_{\min }}({T_{w,in}} - {T_{db,in}})\) \(\dot Q = \varepsilon {\dot C_{\min }}({T_{w,in}} - {T_{db,in}})\)
+
+Then the outlet air dry-bulb and outlet water temperature are calculated:
+
+\begin{equation}
+{T_{db,out}} = {T_{db,in}} + \frac{{\mathop Q\limits^. }}{{{{\mathop C\limits^. }_a}}}
+\end{equation}
+
+\begin{equation}
+{T_{w,out}} = {T_{w,in}} - \frac{{\mathop Q\limits^. }}{{{{\mathop C\limits^. }_w}}}
+\end{equation}
+
+\({T_{w,in}}\) = inlet water temperature, \(^{o}\)C
+
+\({T_{w,out}}\) = outlet water temperature, \(^{o}\)C
+
+\({T_{db,in}}\) ~ = dry-bulb temperature of the inlet air, \(^{o}\)C
+
+\({T_{db,out}}\) = dry-bulb temperature of the outlet air, \(^{o}\)C
+
+\subsubsection{Calculating the Actual Exiting Water Temperature and Fan Power}\label{calculating-the-actual-exiting-water-temperature-and-fan-power-1}
+
+The previous section describes the methodology used for calculating the steady-state temperature of the water leaving the fluid cooler. This methodology is used to calculate the exiting water temperature with the fluid cooler fans operating (including low and high fan speed for the two-speed fluid cooler). The exiting water temperature calculations use the fluid flow rates (water and air) and the Nominal capacity information entered by the user for each regime.
+
+The fluid cooler model seeks to maintain the temperature of the water exiting the fluid cooler at (or below) a setpoint. The setpoint schedule is defined by the field ``Loop Temperature Setpoint~ Node or reference'' for the CondenserLoop object.
+
+The fluid cooler fans are turned on to reduce the exiting water temperature to the setpoint. The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (e.g., Fluid cooler fans on for the entire simulation time step and fluid cooler fans off for the entire simulation time step). Cyclic losses are not taken into account. If the outlet water temperature is less than the set-point then the fraction of time for which the fluid cooler must operate to meet the set-point is calculated by using the following equation:
+
+\begin{equation}
+\omega \,\, = \frac{{{T_{set}} - {T_{wout,off}}}}{{{T_{wout,on}} - {T_{wout,off}}}}
+\end{equation}
+
+Where
+
+\({T_{set}}\) ~ = exiting water setpoint temperature, \(^{o}\)C
+
+\({T_{wout,off}}\) ~ = exiting water temperature with all fluid cooler fans off, \(^{o}\)C
+
+\({T_{wout,on}}\) ~ = exiting water temperature with all fluid cooler fans on, \(^{o}\)C
+
+The average fan power for the simulation time step is calculated by multiplying \(\omega \,\) by the steady-state fan power specified by the user.
+
+The calculation method for the two-speed fluid cooler is similar to that for the single-speed fluid cooler example described above. The model first calculates the steady-state exiting water temperature with the fluid cooler fans at low speed. If the exiting water temperature at low fan speed is below the setpoint temperature, then the average fan power is calculated based on the result of previous equation and the steady-state, low speed fan power specified by the user.~ If low-speed fan operation is unable to reduce the exiting water temperature below the setpoint, then the fluid cooler fans' speed is increased to high speed and the steady-state exiting water temperature is calculated. If this temperature is below the setpoint, then a modified version of previous equation is used to calculate runtime at high fan speed:
+
+\begin{equation}
+\omega \,\, = \frac{{{T_{set}} - {T_{wout,low}}}}{{{T_{wout,high}} - {T_{wout,low}}}}
+\end{equation}
+
+where
+
+\({T_{set}}\) ~ = exiting water setpoint temperature, \(^{o}\)C
+
+\({T_{wout,low}}\) ~ = exiting water temperature with fluid cooler fans at low speed, \(^{o}\)C
+
+\({T_{wout,high}}\) ~ = exiting water temperature with fluid cooler fans at high speed, \(^{o}\)C
+
+The average fan power for the simulation time step is calculated for the two-speed fluid cooler as follows
+
+\begin{equation}
+{P_{fan,avg}}\, = \,\omega \,({P_{fan,high}})\, + \,\left( {1 - \omega } \right)\left( {{P_{fan,low}}} \right)
+\end{equation}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/demand-controlled-ventilation.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/demand-controlled-ventilation.tex
new file mode 100644
index 00000000000..5ef70d6b5d9
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/demand-controlled-ventilation.tex
@@ -0,0 +1,363 @@
+\section{Demand Controlled Ventilation }\label{demand-controlled-ventilation}
+
+ASHRAE Standard 62.1, Ventilation for Acceptable Indoor Air Quality, contains provisions that allow building ventilation systems to vary the amount of outdoor ventilation air delivered to occupied zones based on feedback from sensors that monitor various indoor air contaminants (ASHRAE 2007). Although not a contaminant of concern in most buildings, carbon dioxide (CO\(_{2}\)) levels can be monitored as an indicator of building occupancy and the associated human bioeffluent concentration. Demand controlled ventilation (DCV) is being increasingly used to modulate outdoor ventilation air based on real-time occupancy (Emmerich and Persily 1997, Schell et al. 1998, Schell and Int-Hout 2001). Modulating the outdoor ventilation air while maintaining proper indoor air quality has the potential for large energy savings compared to constant rate ventilation systems that are typically designed to provide outdoor ventilation air based on maximum anticipated occupancy.
+
+EnergyPlus can model DCV by the ventilation rate procedure (VRP) defined in ASHRAE Standard 62.1-2007/2010 for single and multiple path systems, and the indoor air quality procedure (IAQP) defined in Standard 62. The VRP first calculates the breathing-zone outdoor air flow rate based on two components -- the zone occupant component and the zone floor area component, then it calculates the zone supply outdoor air flow rate considering the zone air distribution effectiveness and secondary recirculation (for mult-path systems only), and finally calculates the system outdoor air flow rate considering the zone diversity and system ventilation efficiency. The user must include the following five objects in their input data file in order to model DCV (using VRP or IAQP):
+
+n~\textbf{AirLoopHVAC:OutdoorAirSystem} to simulate the mixed air box of the air loop
+
+n~\textbf{Controller:MechanicalVentilation} with the DCV flag set to `Yes' to determine the minimum outdoor air flow rate to be provided by the mixed air box
+
+n~\textbf{Controller:OutdoorAir} to control the outside air flow rate introduced via the mixed air box
+
+n~\textbf{DesignSpecification:OutdoorAir} to describe the outdoor air requirements for each zone
+
+n~\textbf{DesignSpecification:ZoneAirDistribution} to describe air distribution effectiveness and secondary recirculation (for multi-path ventilation systems) for each zone
+
+The outdoor air system (AirLoopHVAC:OutdoorAirSystem) is a subsystem of an AirLoopHVAC which handles the mixed air portion of the primary air system: the system relief air, the outside air inlet, and any components and controllers associated with the system relief air and outside air streams. The inputs for this object are fully described in the EnergyPlus Input Output Reference. Determining the outdoor air ventilation rate and introducing this ventilation via the mixed air box are accomplished by the mechanical ventilation and outdoor air controller objects.
+
+The VRP currently requires outdoor air ventilation rates to be determined based on the floor area of each occupied zone plus the number of people in each zone. The number of people varies based on the setting of the DCV flag in the Controller:MechanicalVentilation object. For using occupancy at every time step, the DCV flag must be set to `Yes'. The outdoor air ventilation rate can then be reset dynamically as operating conditions change (e.g., variations in occupancy). The Controller:MechanicalVentilation object simplifies the procedure for calculating these outdoor air ventilation requirements and resetting them based on varying occupancy levels. This is particularly useful for large air distribution systems that serve a number of different zone types with varying occupancy levels.
+
+The IAQP (ASHRAE 2007) is a design procedure in which outdoor air intake and other system design parameters are based on an analysis of contaminant sources, and contaminant concentration targets. Although carbon dioxide is not considered as an indoor contaminant but is considered as an indicator of indoor air quality in buildings, EnergyPlus uses IAQP to control carbon dioxide. In addition, a generic contaminant may be introduced. The current IAQP in EnergyPlus allows credit to be taken for controls that can be reliably demonstrated to result in indoor carbon dioxide and generic contaminant concentrations equal to or lower that those achieved using the VRP. The IAQP may also be used where the design is intended to attain specific target carbon dioxide and generic contaminant levels.
+
+\subsection{Ventilation Rate Procedure}\label{ventilation-rate-procedure}
+
+\subsubsection{Calculation of zone minimum outdoor air flow}\label{calculation-of-zone-minimum-outdoor-air-flow}
+
+For the i-th zone, first the breathing-zone outdoor air flow is calculated:
+
+\begin{equation}
+{V_{bz,i}} = {R_{p,i}} \times {P_i} + {R_{a,i}} \times {A_i}
+\end{equation}
+
+Where:
+
+\({V_{bz,i}}\) = the breathing-zone outdoor air flow, m³/s
+
+\({R_{p,i}}\) = the ventilation rate per person, m³/s-person
+
+\({P_i}\) ~ = the number of occupants for the zone
+
+\({R_{a,i}}\) = the ventilation rate per floor area, m³/s-m²
+
+\({A_i}\) ~ = the floor area of the zone, m²
+
+\(i\) ~~~ = the index of the zone or zone list
+
+Next, the i-th zone outdoor air flow is calculated:
+
+\begin{equation}
+{V_{oz,i}} = {V_{bz,i}}/{E_i}
+\end{equation}
+
+Where:
+
+\({V_{oz,i}}\) = the zone outdoor air flow, m³/s
+
+\({E_i}\) = the zone air distribution effectiveness, see following figure for ASHRAE recommended values.
+
+\begin{figure}[hbtp] % fig 195
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4716.png}
+\caption{Zone Air Distribution Effectiveness Typical Values (Source: ASHRAE Standard 62.1-2010) \protect \label{fig:zone-air-distribution-effectiveness-typical}}
+\end{figure}
+
+\subsubsection{Calculation of system minimum outdoor air flow}\label{calculation-of-system-minimum-outdoor-air-flow}
+
+For single zone systems, the system outdoor air flow,
+
+\begin{equation}
+{V_{ot}} = {V_{oz}}
+\end{equation}
+
+For 100\% outdoor air multi-zone systems, the system outdoor air flow,
+
+\begin{equation}
+{V_{ot}} = \mathop \sum \limits_{i = 1}^{allzones} {V_{oz,i}}
+\end{equation}
+
+For non 100\% outdoor air multi-zone systems, the system outdoor air flow,
+
+\begin{equation}
+{V_{ot}} = {V_{ou}}/{E_v}
+\end{equation}
+
+Where:
+
+\({V_{ou}}\) ~the uncorrected system outdoor air flow, m³/s
+
+\begin{equation}
+{V_{ou}} = \mathop \sum \limits_{i = 1}^{allzones} ({R_{p,i}} \times {P_i}) + \mathop \sum \limits_{i = 1}^{allzones} ({R_{a,i}} \times {A_i})
+\end{equation}
+
+\({X_s}\) ~ = the uncorrected system outdoor air fraction
+
+\begin{equation}
+{X_s} = {V_{ou}}/{V_{ps}}
+\end{equation}
+
+\({V_{ps}}\) = the system supply air flow, m³/s
+
+\({Z_{d,i}}\) ~ = the zone outdoor air fraction
+
+\begin{equation}
+{Z_{d,i}} = {V_{oz,i}}/{V_{dz,i}}
+\end{equation}
+
+\({V_{dz,i}}\) ~ = the zone supply air flow, m³/s
+
+\({E_v}\) = the system ventilation efficiency, determined as the minimum of the zone ventilation efficiency among all ventilation zones served by the air handler.
+
+\emph{Ev} = minimum (\emph{Evz})
+
+\emph{Evz}~ = the zone ventilation efficiency, determined differently for single-path and multi-path systems.
+
+\textbf{\emph{For single-path systems,}}
+
+Evz = 1+ Xs-- Z\(_{d,i}\)
+
+\textbf{\emph{For multi-path systems,}}
+
+\emph{Evz =} \emph{(Fa+ Xs·Fb-- Z\(_{d,i}\)·Ep·Fc)/Fa}
+
+where system air fractions \emph{Fa}, \emph{Fb}, and \emph{Fc}are determined as follows
+
+\emph{Fa = Ep+} \emph{(1 -- Ep) ·Er}
+
+\emph{Fb = Ep}
+
+\emph{Fc = 1 --} \emph{(1 -- Ez) · (1 -- Er) · (1 -- Ep)}
+
+\emph{Ep~~ =} the zone primary air fraction. For dual-fan dual-duct systems, the zone primary air is the air from the cold duct.
+
+\emph{Ep = Vpz/Vdz,i}
+
+\emph{Er} ~ = the zone secondary recirculation fraction
+
+Single-path systems are special cases of multi-path systems where \emph{Er} = 0, \emph{Ep} = 1, \emph{Fa} = \emph{Fb =} \emph{Fc} = 1.0
+
+The zone secondary recirculation fraction Er is determined by the designer based on system configuration. For plenum return systems with secondary recirculation (e.g., fan-powered VAV with plenum return) Er is usually less than 1.0, although values may range from 0.1 to 1.2 depending upon the location of the ventilation zone relative to other zones and the air handler. For ducted return systems with secondary recirculation (e.g., fan-powered VAV with ducted return), Er is typically 0.0, while for those with system-level recirculation (e.g, dual-fan dual-duct systems with ducted return) Er is typically 1.0. For other system types, Er is typically 0.75.
+
+The program then calculates the minimum outdoor air flow fraction based on the information provided in the object Controller:MechanicalVentilation and the maximum branch air flow rate as follows:
+
+MechVentOutsideAirMinFrac = \({V_{ot}}\) ~RhoStd / \(\dot m{_{maxbranch}}\) here:
+
+MechVentOutsideAirMinFrac = outdoor air minimum fraction based on all zones specified in the Controller:MechanicalVentilation object
+
+Controller:OutdoorAir controls the amount of outdoor ventilation air introduced via the mixed air box based on several user inputs. The user can define the minimum outdoor air flow rate as a percentage of the system's supply air flow rate (e.g., for a variable-air volume system) or a fixed minimum outdoor air flow rate (not as a percentage but a fixed value) (field MinimumLimit). DCV, using the Controller:MechanicalVentilation object in conjunction with the Controller:OutdoorAir object, allows a third option for setting the minimum outdoor air flow. Economizer operation can also be specified to increase the outdoor air flow above the minimum flow rate to provide free cooling when conditions permit (Controller:OutdoorAir, field Economizer Control Type).
+
+EnergyPlus uses the largest outdoor air flow rate calculated by the various methods described above when modeling system performance (as long this rate doesn't exceed the maximum flow rate specified for the main air loop branch or for the outdoor air controller itself).
+
+The method used to calculate the outdoor ventilation air flow rate for each system simulation time step is described in more detail below. The figure below schematically illustrates air flow paths used in the calculation of outdoor air flow rate.
+
+\begin{figure}[hbtp] % fig 196
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4731.png}
+\caption{Demand Control Ventilation -- Air Flow Paths \protect \label{fig:demand-control-ventilation-air-flow-paths}}
+\end{figure}
+
+The minimum outdoor air flow rate is first calculated based on the minimum outdoor air flow rate and the minimum outdoor air schedule value as defined by the user inputs for the object Controller:OutdoorAir:
+
+\begin{equation}
+\dot{m}_{minOA} = \dot{V}_{minOA} \cdot MinOAScheduleValue \cdot RhoStd
+\end{equation}
+
+where:
+
+\({\mathop m\limits^ \bullet_{_{\min OA}}}\) ~~~~~~ = minimum outdoor air flow rate for this time step, kg/s
+
+\({\mathop V\limits^ \bullet_{_{\min OA}}}\) ~~~~~~~ = minimum outdoor air flow rate defined in Controller:OutdoorAir, m\(^{3}\)/s
+
+\emph{MinOAScheduleValue} = minimum outdoor air schedule value defined by the schedule identified in Controller:OutdoorAir
+
+\emph{RhoStd}~~~~~ = standard air density (1.204 kg/m\(^{3}\)) adjusted for the local barometric pressure (standard barometric pressure corrected for altitude, ASHRAE 1997 HOF pg. 6.1).
+
+The outdoor air minimum fraction is then calculated as the ratio of the minimum outdoor air flow rate calculated above to the maximum air flow rate defined in the Branch statement for the main air loop (converted to mass flow rate).
+
+\begin{equation}
+  OutAirMinFrac = \frac{\dot{m}_{minOA}}{\dot{m}_{max,branch}}
+\end{equation}
+
+where:
+
+\({\mathop m\limits^ \bullet_{\max branch}}\) ~~~ = Max branch air volume flow rate times \emph{RhoStd,} kg/s
+
+The program then calculates the minimum outdoor air flow fraction (\emph{MechVentOutsideAirMinFrac}) according to the VRP based on the information provided in the object Controller:MechanicalVentilation and the maximum branch air flow rate.
+
+The algorithm then uses the larger of these outdoor air minimum fractions in subsequent calculations, and also makes sure that the resulting fraction is between 0 and 1.
+
+\begin{equation}
+OutAirMinFrac = \,\,MAX\left( {OutAirMinFrac,MechVentOutsideAirMinFrac} \right)
+\end{equation}
+
+\begin{equation}
+OutAirMinFrac = \,\,MIN\left( {MAX\left( {OutAirMinFrac,0.0} \right),\,1.0} \right)
+\end{equation}
+
+The algorithm goes on to determine if economizer operation is possible based on the user inputs and the current conditions of the outdoor air and return air. If conditions permit economizer operation, the outdoor air flow fraction is increased beyond the minimum fraction to meet the mixed air setpoint temperature (setpoint temperature assigned to the node defined in field ``Control\_Node'' of Controller:OutdoorAir).
+
+\begin{equation}
+OAFrac = \,MAX\,(OutAirMinFrac,\,EconomizerOAFrac)
+\end{equation}
+
+The mass flow rate of outdoor air is then calculated based on the outdoor air fraction determined above and the mixed (supply) air mass flow rate:
+
+\begin{equation}
+{\dot m_{OA}} = OAFrac * {\dot m_{MixedAir}}
+\end{equation}
+
+where:
+
+\({\dot m_{OA}}\) ~~~~~~~~~~ = mass flow rate of outdoor air, kg/s
+
+\(OAFrac\) ~~~ = fraction of outdoor air in the mixed (supply) air stream
+
+\({\mathop m\limits^ \bullet_{MixedAir}}\) ~~~~ = mass flow rate of the mixture of return air and outdoor ventilation air, kg/s
+
+The algorithm checks to make sure the calculated outdoor air mass flow rate is greater than or equal to the air flow rate being exhausted.
+
+\begin{equation}
+{\dot m_{OA}} = MAX\left( {{{\dot m}_{OA}},{{\dot m}_{ExhaustAir}}} \right)
+\end{equation}
+
+If a fixed minimum outdoor air flow rate is specified (field Minimum Limit Type in Controller:OutdoorAir) for a continuous air flow system, the program makes sure that the outdoor air mass flow rate is greater than or equal to the minimum outdoor air flow rate specified by the user.
+
+\begin{equation}
+{\dot m_{OA}} = MAX\left( {{{\dot m}_{OA}},{{\dot m}_{\min OA}}} \right)
+\end{equation}
+
+The outdoor air mass flow rate should be less than or equal to the mixed (supply) air flow rate, and the outdoor air flow rate is reset if necessary.
+
+\begin{equation}
+{\dot m_{OA}} = MIN\left( {{{\dot m}_{OA}},{{\dot m}_{MixedAir}}} \right)
+\end{equation}
+
+The outdoor air mass flow rate should also be less than or equal to the maximum outdoor air flow rate specified by the user, and the outdoor air flow rate is reset if necessary.
+
+\begin{equation}
+{\dot m_{OA}} = MIN\left( {{{\dot m}_{OA}},{{\dot m}_{MaxOA}}} \right)
+\end{equation}
+
+where:
+
+\({\dot m_{MaxOA}}\) = maximum outdoor air mass flow rate, kg/s = maximum outdoor air volume flow rate from Controller:OutdoorAir times \emph{RhoStd}
+
+Finally, the relief air flow rate is calculated as the difference between the outside and exhaust air mass flow rates.
+
+\begin{equation}
+{\dot m_{ReliefAir}} = MAX\left( {{{\dot m}_{OA}} - \,{{\dot m}_{ExhaustAir}}\,,0.0} \right)
+\end{equation}
+
+\subsection{Indoor Air Quality Procedure}\label{indoor-air-quality-procedure}
+
+Like VRP, the user must include the following three objects in their input data file in order to model CO\(_{2}\)-based DCV with IAQP:
+
+n~AirLoopHVAC:OutdoorAirSystem to simulate the mixed air box of the air loop
+
+n~Controller:MechanicalVentilation to determine the minimum outside air flow rate to be provided by the mixed air box
+
+n~Controller:OutdoorAir to control the outside air flow rate introduced via the mixed air box
+
+The outdoor air mass flow rate provided by the air loop is calculated as below:
+
+\begin{equation}
+{\dot m_{OA}} = \sum\limits_i^N {{{\dot m}_{OA,z,i}}}
+\end{equation}
+
+where:
+
+\({\dot m_{OA,z,i}}\) = outdoor air mass flow rate for the ith zone as calculated according to section Carbon Dioxide Prediction located elsewhere in this document.
+
+N = number of zones served by the air loop, which is provided in the input for a Controller:MechanicalVentilation object
+
+\subsection{Proportional Control}\label{proportional-control}
+
+The control has two choices: ProportionalControlBasedonOccupancySchedule and ProportionalControlBasedonDesignOccupancy. The difference is occupancy level. The former uses real time occupancy, while the latter uses design occupancy level. Like Ventilation Rate Procedure and the Indoor Air Quality Procedure, the following three objects must be included in the input data file in order to model CO\(_{2}\)-based DCV with Proportional Control:
+
+n~\textbf{AirLoopHVAC:OutdoorAirSystem} to simulate the mixed air box of the air loop
+
+n~\textbf{Controller:MechanicalVentilation} to determine the minimum outside air flow rate to be provided by the mixed air box
+
+n~\textbf{Controller:OutdoorAir} to control the outside air flow rate introduced via the mixed air box
+
+For the i-th zone, the outdoor air mass flow rate provided by the air loop is calculated as below:
+
+1)~~~The required intake flow of outdoor air for the design zone population, \emph{P\(_{z,i}\)}
+
+\begin{equation}
+{V_{ot - design,i}} = \frac{{\left( {{R_{p,i}}.{P_{z,i}}} \right) + ({R_{a,i}}.{A_{z,i}})}}{{{E_i}}}
+\end{equation}
+
+2)~~~The required intake flow of outdoor air when the zone is unoccupied i.e.~ \emph{P\(_{z,i}\)} = 0
+
+\begin{equation}
+{V_{ot - min,i}} = \frac{{({R_{a,i}}.{A_{z,i}})}}{{{E_i}}}
+\end{equation}
+
+3)~~~The target indoor CO\(_{2}\) concentration at \({V_{ot - design,i}}\)
+
+\begin{equation}
+{C_{s - design,i}} = {C_o} + \frac{N}{{\left( {{V_{ot - design,i}}/{P_{z,i}}} \right)}}
+\end{equation}
+
+4)~~~The target indoor CO\(_{2}\) concentration at \({V_{ot - min}}\) ~is either a user input in the object ZoneControl:ContaminantController or equal to the outdoor CO\(_{2}\) concentration. The default is outdoor CO\(_{2}\) concentration.
+
+\begin{equation}
+{C_{s - min,i}} = {C_o}
+\end{equation}
+
+When the indoor CO\(_{2}\) concentration equals \({C_{s - design,i}}\) , \({V_{ot}}\) ~should equal \({V_{ot - design,i}}\) . When the indoor CO\(_{2}\) concentration equals \({C_{s - min,i}}\) , \({V_{ot}}\) ~should equal \({V_{ot - min,i}}\) . When the indoor CO\(_{2}\) concentration is between \({C_{s - min,i}}\) ~and \({C_{s - design,i}}\) , a controller should adjust outdoor air intake flow \({V_{ot}}\) ~proportionally between \({V_{ot - min,i}}\) ~and \({V_{ot - design,i}}\) :
+
+\begin{equation}
+{V_{ot,i}} = {V_{ot - min,i}} + ({V_{ot - design,i}} - {V_{ot - min,i}})\frac{{({C_{s - actual,i}} - {C_{s - min,i}})}}{{({C_{s - design,i}} - {C_{s - min,i}})}}
+\end{equation}
+
+Where,
+
+\({R_{p,i}}\) ~ = Required outdoor air flow rate per person, (m\(^{3}\)/s)/person
+
+\({R_{a,i}}\) ~ = Required outdoor air flow rate per unit area, (m\(^{3}\)/s)/m\(^{2}\)
+
+\({P_{z,i}}\) ~ = Design zone population, number of people
+
+When ProportionalControlBasedonDesignOccupancy is specified, number of people = design occupancy * current schedule value. When ProportionalControlBasedonDesignOccupancy is specified, number of people = design occupancy.
+
+\({A_{z,i}}\) ~ = Zone floor area, m\(^{2}\)
+
+\({E_i}\) ~ = The zone air distribution effectiveness
+
+\(N\) ~ = CO\(_{2}\) generation rate, (m\(^{3}\)/s)/person (Specified in the People object)
+
+\({C_o}\) ~ = CO\(_{2}\) concentration in the outdoor air, ppm
+
+\({C_{s - design,i}}\) ~ = CO\(_{2}\) concentration in the space for the design conditions, ppm
+
+\({C_{s - min,i}}\) ~ = Minimum CO\(_{2}\) concentration in the space, ppm
+
+\({C_{s - actual,i}}\) ~ = Actual CO\(_{2}\) concentration in the space, ppm
+
+\({V_{ot - design,i}}\) ~ = Required intake of outdoor air flow rate at \({C_{s - design}}\) , (m\(^{3}\)/s)
+
+\({V_{ot - min,i}}\) ~ = Required intake of outdoor air flow rate at \({C_{s - min}}\) , (m\(^{3}\)/s)
+
+\({V_{ot,i}}\) ~ = Required intake of outdoor air flow rate at \({C_{s - actual}}\) , (m\(^{3}\)/s)
+
+Except \({C_{s - min,i}}\) ~above, all other variables are already available in EnergyPlus (See Eng. Reference for ``Ventilation Rate Procedure'' above for further details). \({C_{s - min}}\) ~can be specified in the ZoneControl:ContaminantController object as a schedule. If~ \({C_{s - min}}\) ~is not specified in the ZoneControl:ContaminantController object, then outdoor air CO2 concentration will be used as the minimum. In order for ``ProportionalControl'' to be active, the following conditions must be met, otherwise default ``VentilationProcedure'' will be modeled and a warning will be issued during runtime:
+
+1)~~~``Carbon Dioxide Control Availability Schedule Name'' input field in the ZoneControl:ContaminantController object must be greater than zero.
+
+2)~~~CO2 gain from people in the zone must be greater than zero.
+
+3)~~~``Outdoor air flow per person'' and ``Outdoor air flow per zone floor area'' in the corresponding ``DesignSpecification:OutdoorAir'' object must be greater than zero.
+
+\subsection{References}\label{references-018}
+
+ASHRAE. 2007. \emph{ANSI/ASHRAE Standard 62.1-2007, Ventilation for acceptable indoor air quality}. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2010. \emph{ANSI/ASHRAE Standard 62.1-2010, Ventilation for acceptable indoor air quality}. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Emmerich, S.J. and A.K. Persily. 1997. Literature review on CO\(_{2}\)-based demand-controlled ventilation. \emph{ASHRAE Transactions} 103(2):229-243.
+
+Schell, M.B., S.C. Turner, R.O. Shim. 1998. Application of CO\(_{2}\)-based demand controlled ventilation using ASHRAE Standard 62-1989. \emph{ASHRAE Transactions} 104(2):1213-1225.
+
+Schell, M. and D. Int-Hout. 2001. Demand control ventilation using CO\(_{2}\). \emph{ASHRAE Journal}, February.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/district-cooling.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/district-cooling.tex
new file mode 100644
index 00000000000..b7fb838bc57
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/district-cooling.tex
@@ -0,0 +1,3 @@
+\section{District Cooling }\label{district-cooling}
+
+When the user is not interested in a plant simulation or there is some centralized source of chilled water, the following model can be used in the input.~ This allows the user to achieve a simulation without specifying operating parameters or curve fits for chiller models.~ This model only needs the connections to the loop and the nominal capacity to simulate.~ See the InputOutput Reference for additional information (Object: DistrictCooling).~ This model calculates the output capacity necessary from the inlet temperature to the setpoint temperature for that loop with the given mass flow rate in Watts.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/district-heating.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/district-heating.tex
new file mode 100644
index 00000000000..94311f9bae1
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/district-heating.tex
@@ -0,0 +1,3 @@
+\section{District Heating }\label{district-heating}
+
+When the user is not interested in a plant simulation or there is some centralized source of hot water, the following model can be used in the input.~ This allows the user to achieve a simulation without specifying operating parameters or curve fits for boiler models.~ This model only needs the connections to the loop and the nominal capacity to simulate.~ See the InputOutput Reference for additional information (Object: DistrictHeating).~ This model calculates the output capacity necessary from the inlet temperature to the setpoint temperature for that loop with the given mass flow rate in Watts.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/electric-baseboard-heater-with-radiation.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/electric-baseboard-heater-with-radiation.tex
new file mode 100644
index 00000000000..13ca0fc8c75
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/electric-baseboard-heater-with-radiation.tex
@@ -0,0 +1,135 @@
+\section{Electric Baseboard Heater with Radiation and Convection}\label{electric-baseboard-heater-with-radiation-and-convection}
+
+\subsection{Overview}\label{overview-015}
+
+The input object ZoneHVAC:Baseboard:RadiantConvective:Electric provides a model for electric baseboard heaters that include both convective and radiant heat addition to a space from a baseboard heater. The radiant heat transfer to people as well as surfaces within a space is determined in the same fashion as both hot water and steam baseboard heater with radiation and convection models. The electric baseboard heater transfers energy via electric resistance heating. Radiant heat calculated by the user-defined fraction from the heating capacity of a baseboard unit impacts the surface heat balances and thermal comfort of occupants in a space. EnergyPlus then assumes that the remaining convective gains from the unit are evenly spread throughout the space thus having an immediate impact on the zone air heat balance which is used to calculate the mean air temperature (MAT) within the space.
+
+\subsection{Model Description}\label{model-description-009}
+
+\subsubsection{Convective Electric Baseboard Heater Inputs}\label{convective-electric-baseboard-heater-inputs-000}
+
+Like many other HVAC components, the electric baseboard model requires a unique identifying name and an availability schedule. The availability schedule defines the availability of the unit for providing condition to the space. The input also requires a capacity and efficiency for the unit. While the efficiency is a required input that defaults to unity, the capacity can be chosen to be autosized by EnergyPlus.
+
+All inputs for the radiant heat calculation are the same as the water and steam baseboard heater with radiation and convection models in EnergyPlus. Users are required to input fractions that specify total radiant heat directly delivered to surfaces as well as people in a space. The sum of radiant energy of these distribution fractions must sum to unity, and each baseboard heater is allowed to distribute energy to up to 20 surfaces.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-002}
+
+When the unit is available and there is a heating load within a space, the electric baseboard unit will meet the entire remaining provided that it has enough capacity to do so. The model sets the heating capacity of a baseboard unit to the remaining heating load in the space, which any primary heating system does not meet. Note that it is set to the maximum nominal capacity of the unit, if a heating load in a space is greater than the maximum. The model then determines the radiant heat source through the simulation as
+
+\begin{equation}
+{q_{rad}} = q \cdot Fra{c_{rad}}
+\end{equation}
+
+where \emph{q\(_{rad}\)} is the total radiant heating capacity, \emph{q} is the heating capacity of the unit, and \emph{Frac\(_{rad}\)} is the user-defined fraction for the radiation. The radiant heat additions to people and surfaces are thus
+
+\begin{equation}
+{q_{people}} = {q_{rad}} \cdot Fra{c_{people}}
+\end{equation}
+
+\begin{equation}
+{q_{surface}} = \sum {{q_{rad}} \cdot Fra{c_{surface,i}}}
+\end{equation}
+
+where \emph{q\(_{people}\)} is the radiant heat transfer to people, \emph{q\(_{surface}\)} is the heat radiated to surfaces, \emph{Frac\(_{people}\)} is the fraction of the heat radiated to people, and \emph{Frac\(_{surface,i}\)} is the fraction of the heat radiated to surface i.
+
+Once the radiant heat sources are determined, the model distributes the radiant heat sources to the appropriate surfaces and people for thermal comfort purposes, and EnergyPlus recalculates the surface heat balances. The model then determines differences in convection from the surfaces to the air before and after the surface heat balances are impacted due to radiant heat additions from the unit. Note that the model converts the radiant heat transfer to people to convective energy so that the heat balance includes this amount of energy, which will be lost (see High Temperature Radiant Heater Model). The model calculates the actual convective system impact of an electric baseboard heater unit as
+
+\begin{equation}
+{q_{req}} = ({q_{surf,c}} - {q_{surf,z}}) + {q_{conv}} + {q_{people}}
+\end{equation}
+
+where \emph{q\(_{req}\)} is the actual heating load that the unit should meet, \emph{q\(_{surf,c}\)} is the convection from the surfaces to the air after the radiant heat distribution, \emph{q\(_{surf,z}\)} is the convection from the surfaces to the air before the radiant heat distribution, and \emph{q\(_{conv}\)} is the convective heat transfer to the air.
+
+The energy consumption of the baseboard heater is calculated using the user-supplied efficiency and the actual convective system impact calculated as
+
+\begin{equation}
+{Q_{elec}} = \frac{q}{\eta }
+\end{equation}
+
+where \emph{Q\(_{elec}\)} is the energy consumption and \textbf{\emph{η}} is the efficiency of the unit.
+
+If the unit was scheduled off or there is no heating load for the zone, then there will be no heat transfer from the unit. The model assumes no heat storage in the baseboard unit itself and thus no residual heat transfer in future system time steps due to heat storage in the metal of the baseboard unit.
+
+\subsubsection{References}\label{references-020}
+
+No specific reference. Refer to the ASHRAE Handbook series for general information on different system types as needed.
+
+\subsection{Steam Baseboard Heater with Radiation and Convection}\label{steam-baseboard-heater-with-radiation-and-convection}
+
+\subsubsection{Overview}\label{overview-1-006}
+
+The steam baseboard heater model is intended to calculate the mass flow rate of the steam to meet remaining heating demand by determining the actual system impact not only to the surrounding air via convection but also to the surfaces and people via radiation. The actual system impact by the heater is the sum of the additional convective heat transfer from the surfaces to the zone air after they have been heated as well as radiant heat transferred to people and the convective heat transfer to the zone. This actual convective power tries to meet any remaining heating requirement in the zone. The model thus improves the accuracy of thermal comfort predictions and system responses. The calculation of radiant heat addition is the same as that of water baseboard heater model in EnergyPlus.
+
+This model determines the heating capacity from the sum of the latent heat transfer and sensible cooling of water as current steam coil model in EnergyPlus does. Overall energy balances to the steam and air handle the heat exchange between the steam loop and the zone air. The mass flow rate of steam is determined based on the heating demand in the zone. The model requests the user input the desired degree of subcooling so that it determines the heating rate from the heater due to the cooling of the condensate. The user input is also used to determine the condensate outlet conditions.
+
+\subsubsection{Model Description}\label{model-description-1-006}
+
+\subsubsection{Steam Baseboard Heater Inputs}\label{steam-baseboard-heater-inputs}
+
+The steam baseboard model requires a unique identifying name, an available schedule, and steam inlet and outlet nodes. These define the availability of the unit for providing conditions to the space and the node connections that relate to the primary system. It also requires the desired degree of subcooling to calculate the heating capacity and temperature of the condensate. A maximum design flow rate is required, and the user can request this parameter to be auto-sized by EnergyPlus. In addition, a convergence tolerance is requested of the user to help define the ability of the local controls to tightly control the system output. In almost all cases, the user should simply accept the default value for the convergence tolerance unless engaged in an expert study of controls logic in EnergyPlus.
+
+All of the inputs for the radiant heat calculation are the same as the water baseboard heater model in EnergyPlus. User inputs of the radiant fraction and of the fraction of radiant energy incident both on people and on surfaces are required to calculate radiant energy distribution from the heater to the people and surfaces. The sum of radiant energy of these distribution fractions must sum to unity, and each steam baseboard heater is allowed to distribute energy to up to 20 surfaces.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-1-001}
+
+The simulation of the main algorithm of this steam baseboard model with radiation and convection is similar to steam coil model in EnergyPlus while the simulation of radiant component is the same as the water baseboard models. This model initializes all conditions at the inlet node such as mass flow rate, temperature, enthalpy, and humidity ratio. The model then determines the heating capacity of steam baseboard, \emph{q}, as
+
+\begin{equation}
+q = {\dot m_5}({h_{fg}} + {c_{pw}}\Delta t)
+\end{equation}
+
+where \({\dot m_s}\) is the mass flow rate of steam in kg/s, \({h_{fg}}\) is the heat of vaporization of steam in J/kg, \({c_{pw}}\) is the specific heat of water in J/kg.K, and \(\Delta t\) ~is the degree of subcooling in degree C.
+
+The outlet steam temperature is thus
+
+\begin{equation}
+{T_{s,out}} = {T_{s,in}} - \Delta t
+\end{equation}
+
+Once the heating capacity of the unit is determined, the model determines the radiant heat addition by
+
+\begin{equation}
+{q_{rad}} = q \cdot Fra{c_{rad}}
+\end{equation}
+
+where \emph{q} is the total heating capacity of the heater and \emph{Frac\(_{rad}\)} is the user-defined fraction.
+
+The model now distributes the radiant heat additions to the appropriate surfaces, people for thermal comfort purpose, and the air in the zone. The surface heat balances are then recalculated to determine all heat sources or sinks for radiant systems in the zone. It is assumed that the radiant heat incident on people in the zone is converted to convection to the zone so that the zone heat balance includes this amount of heat which will be lost (see High Temperature Radiant Heater Model). The load met, the actual convective system impact, for the baseboard heater, \emph{q\(_{req}\)}, is therefore determined as
+
+\begin{equation}
+{q_{req}} = ({q_{surf,c}} - {q_{surf,z}}) + {q_{conv}} + {q_{people}}
+\end{equation}
+
+where \emph{q\(_{surf,c}\)} is convection from the surfaces to the air in the zone with radiant systems; \emph{q\(_{surf,z}\)} is zero source convection from the surfaces when radiant systems are unavailable; \emph{q\(_{conv}\)} is the convective heat transfer from the heater to the zone air; and \emph{q\(_{people}\)} is radiant heat to the people.
+
+The simulation of radiant heat addition is the same as the water baseboard heater model. The controls are the same as shown in Figure~\ref{fig:variable-flow-low-temperature-radiant-system}.~ Variable Flow Low Temperature Radiant System Controls. After all system time steps have been simulated, an ``average'' zone heat balance calculation is done (similar to the high temperature radiant system). If the unit was scheduled off or there is no steam flow rate through the baseboard unit, then, there will be no heat transfer from the unit. The model assumes no heat storage in the unit itself and thus no residual heat transfer in future system time steps due to heat storage in the steam or metal of the unit.
+
+\subsubsection{References}\label{references-1-007}
+
+No specific reference.~ Refer to the ASHRAE Handbook series for general information on different system types as needed.
+
+ Simulation Models -- Encyclopedic Reference = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+
+The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of ``Heat Balance'', ``HVAC'', and ``Plant''.~ With the integrated solution, these designations signify where the effects of these models have their first impacts.
+
+Main Sections:
+
+\begin{itemize}
+\tightlist
+\item
+  \protect\hyperlink{TowersAndCoolers}{Cooling Towers and Evaporative Fluid Coolers}
+\item
+  \protect\hyperlink{DCV}{Demand Controlled Ventilation}
+\item
+  \protect\hyperlink{EvapCoolers}{Evap Coolers}
+\item
+  \protect\hyperlink{Fans}{Air System Fans}
+\item
+  \protect\hyperlink{AirComponentGroups}{Air System Component Groups}
+\item
+  \protect\hyperlink{VRF}{VRF Systems}
+\item
+  \protect\hyperlink{HX}{Heat Exchangers}
+\item
+  \protect\hyperlink{Humidifiers}{Humidifiers} 
+\end{itemize}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/evaporative-coolers.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/evaporative-coolers.tex
new file mode 100644
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--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/evaporative-coolers.tex
@@ -0,0 +1,681 @@
+\section{Evaporative Coolers }\label{evaporative-coolers}
+
+This section describes the evaporative coolers models for HVAC in EnergyPlus.
+
+\subsection{Direct Evaporative Cooler}\label{direct-evaporative-cooler}
+
+The input object EvaporativeCooler:Direct:CelDekPad provides a model of a direct stage evaporative cooler, shown in the figure below, that consists of a rigid media evaporative pad, with water recirculated from a reservoir.~ The water is pumped from the reservoir to a water distribution header, for water feed by gravity from above the media.~ The evaporative pad provides the area for the adiabatic saturation of the air.~ While the process provides a lower dry-bulb temperature, the moisture content of the leaving air is higher than the entering condition.~ The direct stage is used for comfort cooling in a building where adding humidity to the air can be tolerated.
+
+\begin{figure}[hbtp] % fig 197
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4789.png}
+\caption{Direct Stage Evaporative Cooler \protect \label{fig:direct-stage-evaporative-cooler}}
+\end{figure}
+
+The thermodynamic process is a simultaneous heat and mass transfer, or adiabatic cooling, and follows a constant enthalpy line on the psychrometric chart; it is shown in the figure below as a process from A to B.~ Since the deviation of the constant wet-bulb line and the constant enthalpy line is small, it is assumed that the wet-bulb temperature is constant across the direct evaporative stage.
+
+\begin{figure}[hbtp] % fig 198
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4790.png}
+\caption{Psychrometric Chart -- Constant Enthalpy \protect \label{fig:psychrometric-chart-constant-enthalpy}}
+\end{figure}
+
+If the direct evaporative process were 100\% efficient, the leaving dry-bulb temperature would equal the entering wet-bulb temperature.~ The efficiency of the direct evaporative process is less than 100\% and by defining saturation efficiency (ese) for the direct stage or evaporative pad, the leaving dry-bulb temperature can be expressed by the following equation.
+
+\begin{equation}
+{T_{dbsupout}} - {T_{dbsupin}} = {\varepsilon_{se}} \cdot \left( {{T_{odb}} - {T_{owb}}} \right)
+\end{equation}
+
+\subsubsection{Saturation Efficiency}\label{saturation-efficiency}
+
+Since the evaporative process is not 100\% efficient the saturation efficiency is defined by.
+
+\begin{equation}
+{\varepsilon_{se}} = \frac{{{T_{dbsupin}} - {T_{dbsupout}}}}{{{T_{odb}} - {T_{owb}}}}
+\end{equation}
+
+The saturation efficiency is determined from manufacturer's data, and the least squares curve fit is discussed in Curve Fitting Evaporative Media section.
+
+Using the saturation efficiency (ese) for the direct stage evaporative pad, the leaving dry-bulb temperature can be determined directly.~ The evaporative process approximately follows a constant wet-bulb line.~ Therefore, with the leaving dry-bulb temperature and assuming adiabatic heat transfer across the direct stage, the outlet conditions for the direct stage are known.
+
+The saturation efficiency of the direct evaporative cooler is a function of the pad geometry and airflow rate.~ The pad geometry is constant throughout the simulation, but the airflow rate can change from hour to hour when the evaporative cooler is used with an air economizer.~ The saturation efficiency would then be determined from the flow for that hour with the geometry of the direct evaporative cooler.~ This gives the dry-bulb temperature leaving the evaporative cooler.~ Assuming adiabatic heat transfer across the direct stage, the evaporative process follows the constant wet-bulb line or the constant enthalpy line on the psychrometric chart, therefore the wet-bulb temperature is constant from inlet to outlet.
+
+Some things that can cause departure from the ideal adiabatic saturation process in the direct evaporative cooler are:
+
+·~~~~~~~~makeup water entering the sump,
+
+·~~~~~~~~friction from water re-circulation,
+
+·~~~~~~~~heat transfer from surroundings,
+
+·~~~~~~~~solar radiation (sun upon a cooler).
+
+Thus, adiabatic saturation in evaporative cooling is only an approximation, however the adiabatic saturation assumption in the rigid-media cooler is good, since the water recirculates rapidly and approximates the wet-bulb temperature at steady state operation.
+
+\subsubsection{Curve Fitting Evaporative Media}\label{curve-fitting-evaporative-media}
+
+The saturation efficiency is usually reported as a function of airflow, pad face velocity, and pad thickness.~ The Figure below shows a typical graph of manufacturer's data for the saturation efficiency.~ A multi-variate least squares curve fit of the data was used to generate saturation efficiency functions for the evaporative models that use the CelDek rigid media pad.
+
+\begin{figure}[hbtp] % fig 199
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4793.png}
+\caption{Graph of Saturation Efficiency \protect \label{fig:graph-of-saturation-efficiency}}
+\end{figure}
+
+The curve fit for saturation efficiency was obtained using the functions listed below.~ The model uses the air velocity (Airvel) through the pad and the depth of the media (Depth).~ The least squares routine produced the following model that is used for the evaporative cooling rigid media pad.~ The least squares routine produced an eleven-term multi-variate fit using a third order quadratic.
+
+ese~ = 0.792714 + 0.958569 (Depth) - 0.25193 (Airvel) - 1.03215 (Depth\(^{2}\)) + 0.0262659~(Airvel\(^{2}\)) + 0.914869 (Depth * Airvel) - 1.48241 (Airvel * Depth\(^{2}\)) - 0.018992 (Airvel\(^{3}\) * Depth) + 1.13137 (Depth\(^{3}\) * Airvel) + 0.0327622~(Airvel\(^{3}\) * Depth\(^{2}\)) - 0.145384 (Depth\(^{3}\) * Airvel\(^{2}\))
+
+Where Airvel is in meters per second and Depth is in meters.~ This curve fit is used for the rigid media in the EvapCooler:Direct:CelDekPad and EvapCooler:InDirect:CelDekPad.
+
+\subsection{Dry Coil Indirect Evaporative Cooler}\label{dry-coil-indirect-evaporative-cooler}
+
+The input object EvaporativeCooler:Indirect:CelDekPad provides a model of a dry coil indirect evaporative cooler, shown in the figure below, that has a rigid media pad, similar to the direct evaporative stage, where the adiabatic cooling takes place.~ The secondary air leaves the rigid media pad and enters an air-to-air heat exchanger where it cools the supply air flowing through the heat exchanger tubes.~ The moist secondary air is then exhausted to the environment.~ The secondary air stream has its own fan and includes consists of a rigid media evaporative pad, with water recirculated from a reservoir.~ The water is pumped from the reservoir to a water distribution header, for water feed by gravity from above the media.~ The evaporative pad provides the area for the adiabatic saturation of the air.
+
+\begin{figure}[hbtp] % fig 200
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4794.png}
+\caption{Evaporative Cooler -- Indirect Dry Coil \protect \label{fig:evaporative-cooler-indirect-dry-coil}}
+\end{figure}
+
+The process that the secondary air goes through, A to C to D, is shown by the dashed lines in~ the following figure.~ Process A to C is adiabatic cooling in the rigid media pad.~ Then the air enters the shell side of the heat exchanger and is sensibly heated from C to D by the warm supply air passing through the tube side.
+
+\begin{figure}[hbtp] % fig 201
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4795.png}
+\caption{Secondary Air Process -- Indirect Dry Coil Evap Cooler \protect \label{fig:secondary-air-process-indirect-dry-coil-evap}}
+\end{figure}
+
+The advantage of the dry coil heat exchanger is that the heat exchanger does not have the evaporation taking place on the outside of the tubes, thus no mineral deposits are left on the heat exchange surface to reduce the efficiency of the heat exchanger.~ The rigid media pads are designed to flush the mineral deposits to the sump, so the saturation efficiency of the pad stays relatively constant.
+
+The following equations are used to determine the dry-bulb temperature leaving the evaporative media, given pad geometry and secondary airflow information.~ The heat transfer in the heat exchanger can be determined with the effectiveness of the heat exchanger according.
+
+Tdb sup out = Tdb sup in - ese*(Todb - Towb )
+
+QHx~ = eHx~* Min( CFMsec~, CFMsupply) * rair~* cp air~* ( Todb~- Tdb sec out)
+
+After the heat transfer for the heat exchanger has been determined, an energy balance is done on the supply airside to determine the dry-bulb temperature leaving the indirect evaporative cooler. ~This assumes all the energy for is provided by the primary air stream so the effectiveness value includes the air-to-air effectiveness of the heat exchanger.
+
+Tdb sup out = ~ Tdb sup in~~ -~ \(\frac{{{Q_{Hx}}}}{{{r_{air}}*{c_{pair}}*CF{M_{\sup ply}}}}\)
+
+The wet-bulb temperature is determined from psychrometric routines using the leaving dry-bulb temperature, humidity ratio, and barometric pressure, since humidity ratio is constant for the supply air across the indirect stage.~ The effectiveness of the heat exchanger is determined from a parameter estimation using manufacturer's performance data.~ For the indirect evaporative cooler it was found that a value of 0.67 represented reasonable default effectiveness.
+
+\subsection{Wet Coil Indirect Evaporative Cooler}\label{wet-coil-indirect-evaporative-cooler}
+
+The input object EvaporativeCooler:Indirect:WetCoil provides a model for a wetted coil evaporative cooler, shown in the figure below, that has water sprayed directly on the tubes of the heat exchanger where latent cooling takes place.~ The vaporization of the water on the outside of the heat exchanger tubes allows the simultaneous heat and mass transfer which removes heat from the supply air on the tube side.~ Then the moist secondary air is exhausted.~ The secondary air stream has its own fan.
+
+\begin{figure}[hbtp] % fig 202
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4797.png}
+\caption{Wet Coil Indirect Evaporative Cooler \protect \label{fig:wet-coil-indirect-evaporative-cooler}}
+\end{figure}
+
+The process that the secondary air goes through, A to C on the following figure, is a path of simultaneous heat and mass transfer, but it does not follow a line of constant enthalpy as in the direct stage.~ The process is not adiabatic due to the heat gain from the supply air flowing through the tubes of the heat exchanger.
+
+\begin{figure}[hbtp] % fig 203
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4798.png}
+\caption{Secondary Air Process – Indirect Wet Coil Evaporative Cooler \protect \label{fig:secondary-air-process-indirect-wet-coil}}
+\end{figure}
+
+The wet coil heat exchanger can have a higher stage efficiency than the dry coil due to a higher heat transfer rate on the outside of the heat exchanger tubes.~ Over the operating lifetime of the heat exchanger, the vaporization taking place on the heat exchange surface can leave mineral deposits that will decrease the effectiveness of the heat exchanger.
+
+\subsubsection{Efficiencies of the Indirect Stage}\label{efficiencies-of-the-indirect-stage}
+
+In an indirect stage of an evaporative cooler, the secondary or wet side air stream acts as a heat sink for the supply air.~ The efficiency of the indirect stage is given as the effectiveness of the sensible heat exchange, eHx, and the saturation efficiency on the wet streamside, ese.~ These are expressed as:
+
+eHx~ = \(\frac{q}{{{q_{max}}}}\) = ~ \(\frac{{{C_{sup}}({T_{supin}} - {T_{supout}})}}{{{C_{min}}({T_{secin}} - {T_{secout}})}}\) ,
+
+ese~ = ~ \(\frac{{{T_{dbsecin}} - {T_{dbsecout}}}}{{{T_{odb}} - {T_{owb}}}}\) ,
+
+where Tdb sup in~ = Tdb sec in~ for the indirect cooler.~ The maximum heat transfer possible would be obtained if the supply stream was cooled all the way to the wet-bulb temperature.~ So the efficiency of the indirect evaporative cooler is defined by:
+
+eind~ = ~ \(\frac{{({T_{dbsupin}} - {T_{dbsupout}})}}{{({T_{odb}} - {T_{owb}})}}\) .
+
+Using the combination of the effectiveness and saturation efficiency, the total efficiency of the indirect stage can be expressed by:
+
+eind~ = eHx~ ese~ \(\frac{{{C_{sup}}}}{{{C_{min}}}}\) .
+
+In many cases Csup = Cmin and the efficiency of the indirect stage reduces to:
+
+eind~ = eHx~ ese.
+
+An intuitive model determining the performance of the wet coil indirect model was developed.~ This model can be used for all indirect models by curve fitting data from the evaporative cooler of interest.~ The model development starts with the total efficiency of the indirect evaporative cooler:
+
+eind~ = ~ \(\frac{{({T_{dbsupin}} - {T_{dbsupout}})}}{{({T_{odb}} - {T_{owb}})}}\)
+
+Solving for T db sup out~gives the leaving conditions of the supply air at a constant humidity ratio:
+
+T db sup out = Tdb sup in - eind * (Todb - Towb)
+
+A form for the efficiency of the indirect stage was devised using a maximum efficiency with a coefficient to reduce the efficiency depending on the ratio of the airflows.
+
+eind~ = emax~- C1~* (\(\frac{{CF{M_{sup}}}}{{CF{M_{sec}}}}\) )
+
+C1~is the ``Flow Efficiency Ratio'' and is determined from performance data.
+
+A check of limits will verify that it makes physical sense.~ As the magnitude of the secondary flow increases, the second term of equation above becomes smaller.~ This would make the efficiency tend to go to the maximum efficiency.~ Physically this would be true since the convective terms for heat and mass transfer would increase on the outside of the tube with the additional mass flow rate.~ Similarly, if the supply air flow goes to zero with a constant secondary air flow, the second term of the equation above again becomes small, and the overall efficiency of the stage would approach the maximum.~ The constant C1~tells how quickly the efficiency of the stage would decrease with a mismatch of the supply and secondary flows.
+
+The maximum efficiency of the stage is a combination of the efficiency due to the simultaneous heat and mass transfer on the outside of the tube and the efficiency of the heat exchanger.~ This value can be higher than the dry coil overall efficiency since the convective coefficients on the outside of the tube are larger.~ For example, a least squares fit for the maximum efficiency showed this value was approximately 0.8 compared to the dry coil indirect value of approximately 0.65 (0.67 * 0.97).~ (The maximum efficiency for the dry coil indirect was determined at the condition where flow through the evaporative pad in the secondary air stream approached zero, for a 12-inch thick pad.)~ It should be noted again that over the operating life of the wet coil heat exchanger, the mineral deposits that are left can decrease the effectiveness of the heat exchanger unless appropriate maintenance has taken place.~ Therefore, if modeling an older system, the manufacturer's data may no longer describe the equipment effectiveness.
+
+\subsection{Two Stage Direct/Indirect Evaporative Cooler}\label{two-stage-directindirect-evaporative-cooler}
+
+A two stage cooler can be modeled by combining either a wet coil or the dry coil indirect evaporative cooler staged with a direct evaporative cooler.~ The figure below shows a dry coil indirect evaporative cooler with a direct evaporative cooler.~ This configuration is mainly used for total comfort cooling for a building and would not normally be used as a pre-cooler for a refrigeration coil, since the direct stage would increase the latent load on a refrigeration coil.
+
+\begin{figure}[hbtp] % fig 204
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4806.png}
+\caption{Two Stage Evaporative Cooler \protect \label{fig:two-stage-evaporative-cooler}}
+\end{figure}
+
+The thermodynamic process for the supply air is shown below, going from A to B to C.~ The process from A to B is sensible cooling in the indirect stage.~ The process from B to C is simultaneous heat and mass transfer following a constant enthalpy line.~ The air leaving the final stage has a lower dry-bulb and wet-bulb temperature, and an increase in moisture from the direct stage.
+
+\begin{figure}[hbtp] % fig 205
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4807.png}
+\caption{Thermodynamic Process for Supply Air Through Two Stage Evaporative Cooler \protect \label{fig:thermodynamic-process-for-supply-air-through}}
+\end{figure}
+
+Two stage evaporative coolers can be accomplished by putting the EvaporativeCooler:Direct:CelDekPad, EvaporativeCooler:Indirect:CelDekPad, EvaporativeCooler:Indirect:WetCoil in series in any combination the user desires in the supply air loop.
+
+\subsection{Indirect Evaporative Cooler Special Research Model}\label{indirect-evaporative-cooler-special-research-model}
+
+This section summarizes the model implemented in the component EvaporativeCooler:Indirect:ResearchSpecial.~ Examples of this evaporative cooler are shown in the following figures, without and with a relief valve. This model differs from the other indirect evaporative coolers in that, under part load conditions, it can modulate so that the air leaving the cooler just meets a drybulb temperature setpoint.
+
+The indirect research special evaporative cooler (IEC) machine provides improved modeling features needed for data center and other hybrid cooling applications. The new model includes performance curves for variable effectiveness, fan power, and pump power. It is intended to be able to model IEC machines that have 1) variable speed secondary fans, 2) variable speed pumps for water recirculation and spraying, and 3) ability to operate in a dry mode. Such IEC machines can modulate the cooling power during operation by varying either the secondary side fan speed or the intensity of water spray or both. To simplify the model it is assumed that the device's internal controls are such that, when it is operating as a ``Wet'' evaporative cooler, secondary fan and spray pump operation are linked together so that there is a one-to-one mapping between them at any given part load situation. This allows formulating the fan and pump power performance curves to be based on the same independent variable, secondary air flow fraction.
+
+\begin{figure}[hbtp] % fig 206
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4808.png}
+\caption{Research Special Indirect Evaporative Cooler \protect \label{fig:research-special-indirect-evaporative-cooler}}
+\end{figure}
+
+\subsubsection{Model Formulation}\label{model-formulation}
+
+Each time the model is called it takes the inputs on the left and produces the outputs on the right as shown in \protect\hyperlink{IndEvapCoolerFig2}{Figure}. ``sys'' is primary air stream and typically sits on an AirLoop HVAC branch. ``sec'' is secondary purge air stream and is typically outdoor air. The model will set node flow rates and ``out\_sec'' state variables on the secondary outlet.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image8005.png}
+\caption{}
+\end{figure}
+
+Figure: Illustration of Inputs-Outputs of Indirect Evaporative Cooler Research Special
+
+The model runs either in dry mode or wet mode depending entering air conditions of the primary and secondary air sides. Different effectiveness values are used depending on the operating modes.
+
+\subsubsection{Wet Mode Operation}\label{wet-mode-operation}
+
+If running ``wet,'' use wet bulb effectiveness and wet bulb temperature depression for delta T:
+
+\begin{equation}
+\begin{array}{rl}
+  \epsilon_{wb,op} & = \epsilon_{wb,design}\cdot f_{wb,mod}\left(\text{flowRatio}\right) \\
+  \text{flowRatio} & = \frac{\dot{m}_{sec}}{\dot{m}_{sys}}
+\end{array}
+\end{equation}
+
+Where:
+
+\begin{itemize}
+\item
+  \(\epsilon_{wb,op}\) = current operation effectiveness with respect to wet bulb temperature depression.
+\item
+  \(\epsilon_{wb,design}\) = user input for effectiveness at design air flow rates and full spray power
+\item
+  \(f_{wb,mod}\) = normalized wet mode operation effectiveness modifier performance curve as a function of flow fraction. The curve value describes how effectiveness varies at different flow rates. When conditions are appropriate, this curve is numerically inverted to find a FlowRatio that just meets a setpoint.
+\item
+  \(\dot{m}_{sys}\) = primary air current time step mass flow rate in kg/s
+\item
+  \(\dot{m}_{sec}\) = secondary air current time step mass flow rate in kg/s
+\end{itemize}
+
+The leaving primary air dry bulb temperature in wet operating mode is calculated as follows:
+
+\begin{equation}
+T_{db,out,sys} = T_{db,in,sys} - \epsilon_{wb,op} \left( T_{db,in,sys} - T_{wb,in,sec} \right)
+\end{equation}
+
+Then check that there is sufficient heat capacitance flux (mcT) in the secondary air stream to provide the conditioning. The following steps are for checking and adjusting for non-physical outcomes that could happen with low secondary flow rates.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\tightlist
+\item
+  Calculate heat transfer rate
+\end{enumerate}
+
+The secondary air entering wet-bulb temperature would be the loswest limit allowed, although this temperature cannot be attained in most practical situations. This is checked as a limiting case.
+
+\begin{equation}
+  \begin{array}{rl}
+    T_{db,out,sys} & = \max\left(T_{db,out,sys},T_{db,out,setpoint}\right) \\
+    \dot{Q}_{HX} & = \left(\dot{m}c_p\right)_{sys,in} \cdot \left(T_{db,in,sys}-T_{db,out,sys}\right)
+  \end{array}
+\end{equation}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Calculate outlet enthalpy of the secondary air
+\end{enumerate}
+
+\begin{equation}
+\text{enahalpy}_{out,sec} = \text{enthalpy}_{in,sec} + \frac{\dot{Q}_{HX}}{\dot{m}_{sec}}
+\end{equation}
+
+One approximation that can be made is the outlet condition of the temperature and humidity ratio combination that produces the outlet enthalpy of the secondary air calculated above. A conservative approach is that the secondary air leaves with water added at such a rate that it results in the secondary air to leave at the same dry bulb temperature and all the total heat transfer results in humidity ratio increases, i.e., latent heat transfer. Following this assumption the secondary air outlet humidity ratio can be calculated in step 3.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Calculate outlet humidity ratio of the secondary air
+\end{enumerate}
+
+\begin{equation}
+  \begin{array}{rl}
+    T_{db,out,sec} & = T_{db,in,sec} \\
+    \text{HumRat}_{out,sec} & = \text{PsyWFnTbH}\left(T_{db,out,sec},\text{enthalpy}_{out,sec}\right) \\
+    \dot{V}_{water} & = \frac{QHX / \left[ \left(\text{HumRat}_{out,sec}-\text{HumRat}_{in,sec}\right) \cdot h_{fg,in,sec}\right]}{\rho_{water,Tdb,in,sec}} \\
+    or & = \\
+    \dot{V}_{water} & = \frac{QHX / \left[ \left(\text{enthalpy}_{out,sec}-\text{enthalpy}_{in,sec}\right) \right]}{\rho_{water,Tdb,in,sec}}
+  \end{array}
+\end{equation}
+
+Dry Operation Mode
+
+Similarly, if running ``dry'' use dry bulb effectiveness and dry bulb based delta T
+
+\begin{equation}
+\epsilon_{db,op} = \epsilon_{db,design} \cdot f_{db,mod}\left(\text{flowRatio}\right)
+\end{equation}
+
+Where:
+
+\begin{itemize}
+\item
+  \(\epsilon_{db,op}\) = current operation effectiveness with respect to dry bulb temperature depression.
+\item
+  \(\epsilon_{db,design}\) = user input for effectiveness at design air flow rates and dry operation mode (no water spray on the secondary air side)
+\item
+  \(f_{db,mod}\) = normalized dry mode operation effectiveness modifier performance curve as a function of flow fraction. The curve value describes how the dry mode effectiveness varies with different flow rates. When conditions are appropriate, this curve is numerically inverted to find a FlowRatio that just meets a setpoint
+\end{itemize}
+
+The leaving primary air dry bulb temperature in dry operating mode is calculated as follows:
+
+\begin{equation}
+T_{db,out,sys} = T_{db,in,sys} - \epsilon{db,op}\left(T_{db,in,sys}-T_{db,in,sec}\right)
+\end{equation}
+
+Then check that there is sufficient heat capacitance flux (mcT) in the secondary air stream to provide the conditioning. For dry operation, it should be sufficient to simply use inlet moist air properties for density and specific heat. The following steps are for checking and adjusting for non-physical outcomes that could happen with low secondary flow rates.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\tightlist
+\item
+  Calculate heat transfer
+\end{enumerate}
+
+\begin{equation}
+\dot{Q}_{HX} = \left(\dot{m}c_{p}\right)_{sys,in} \left(T_{db,in,sys}-T_{db,out,sys}c\right)
+\end{equation}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Calculate secondary/scavenger leaving dry-bulb
+\end{enumerate}
+
+\begin{equation}
+T_{db,out,sec} = T_{db,in,sec} + \frac{\dot{Q}_{HX}}{ \left(\dot{m}c_{p}\right)_{sys,in}}
+\end{equation}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Check for energy imbalance and adjust if need
+\end{enumerate}
+
+\begin{equation}
+\text{IF} \left(T_{db,out,sec}>T_{db,in,sys}\right) \text{THEN} T_{db,out,sec} = T_{db,in,sys}-0.2 C
+\end{equation}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Recalculate heat transfer limit if imbalance found in step 3 using new secondary outlet drybulb
+\end{enumerate}
+
+\begin{equation}
+\dot{Q}_{HX,lim} = \left(\dot{m}c_{p}\right)_{sec,in}\cdot \left( T_{db,out,sec}-T_{db,in,sec} \right)
+\end{equation}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{4}
+\tightlist
+\item
+  Recalculate leaving supply air dryblub using new heat transfer rate from step 4
+\end{enumerate}
+
+\begin{equation}
+T_{db,out,sys} = T_{db,in,sec} + \frac{\dot{Q}_{HX}}{ \left(\dot{m}c_{p}\right)_{sys,in}}
+\end{equation}
+
+The IEC in dry and wet operating mode transfers no moisture to the primary system air, so the humidity ratio remains the same:
+
+\begin{equation}
+\text{HumRat}_{out,sys} = \text{HumRat}_{in,sys}
+\end{equation}
+
+\subsubsection{Secondary Air Flow Fraction}\label{secondary-air-flow-fraction}
+
+The secondary air mass flow rate will either be set to \(\dot{m}_{sec}\) or solved for numerically as described below. The secondary side flow fraction, \(ff_{sec}\) , is defined as. (Note this is another flow ratio that differs from the one used above which combined both streams into one ratio in effectiveness modifier curves.)
+
+\begin{equation}
+ff_{sec} = \frac{\dot{m}_{sec}}{\dot{m}_{sec,design}}
+\end{equation}
+
+The secondary air mass flow rate will either be set to or solved for numerically as described below. The secondary side flow fraction, , is defined as. (Note this is another flow ratio that differs from the one used above which combined both streams into one ratio in effectiveness modifier curves.)
+
+\begin{equation}
+P_{sec,fan} = P_{sec,fan,design}\cdot f_{sec,fan,mod}\left(ff_{sec}\right)
+\end{equation}
+
+Where:
+
+\(P_{sec,fan}\) = secondary air fan electric power value at current secondary air flow rate in W.
+
+\(P_{sec,fan,design}\) = secondary air fan electric power value at design air flow rate in W.
+
+\(f_{sec,fan,mod}\) = secondary air fan power modifier normalized performance curve as a function of secondary air flow fraction.
+
+\(\dot{m}_{sec,design}\) = secondary air design mass flow rate in kg/s
+
+Recirculation and spray pump electric power is calculated using design pump electric power and a normalized pump power modifier performance curve that describes how power varies as a function of the secondary air flow fraction is given by:
+
+\begin{equation}
+P_{pump} = P_{pump,design}\cdot f_{pump,mod}\left(ff_{sec}\right)
+\end{equation}
+
+Where:
+
+\(P_{pump}\) = recirculation and spray pump power value at current operation in W.
+
+\(P_{pump,design}\) = recirculation and spray pump power value at design air flow rate in W.
+
+\(f_{pump,mod}\) = recirculation and spray pump power modifier normalized performance curve as a function of secondary air flow fraction.
+
+User specified three operating temperature limits are included in the model. These allow controlling when operation should shift from wet to dry and when the cooler should just be shut down because the outdoor conditions are too warm or too wet to do anything beneficial.
+
+\(T_{db,evapMinLimit}\) = Evaporative Operation Minimum Limit Outdoor Drybulb Temperature, user input. Shut down wet mode with outdoor temperature is lower than this limit, typically shifting to dry mode.
+
+\(T_{wb,evapMaxLimit}\) = Evaporative Operation Maximum Limit Outdoor Wetbulb Temperature, user input. Shut down fan and pump and don't operate when outdoor Wetbulb is higher than this limit. The wet bulb is maybe warmer than the return air and attempting evaporative cooling is wasteful.
+
+\(T_{db,evapMaxLimit}\) = Dry Operation Maximum Limit Outdoor Drybulb Temperature, user input. Shut down dry operation attempts and don't operate secondary fan when outdoor dry bulb is higher than this limit. The dry bulb is maybe warmer than the return air and attempting to do heat exchange is wasteful.
+
+Algorithm to determine cooler operation proceeds as follows
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Retrieve leaving setpoint, \(T_{db,out,setpoint}\)
+\item
+  Calculate leaving dry bulb for max cooling power available at full secondary air flow rate for dry operation, \(T_{db,out,sys,dry,min}\)
+\item
+  Check if dry operation limit (input field called Evaporative Operation Minimum Limit Outdoor Dry-Bulb Temperature) reached, \(T_{db,in,sec}<T_{db,evapMinLimit}\)
+\item
+  If dry limit not exceeded, then leaving dry bulb for max cooling power available at full secondary air flow rate for wet operation, \(T_{db,out,sys,wet,min}\)
+\item
+  Compare setpoint temperature needed to temperatures available, evaluate limits and choose which case for operation is called for. The following table outlines the five cases in order of increasing cooling power.
+\end{enumerate}
+
+INSERT TABLE
+
+``Modulated'' cases solve for a secondary flow rate using numerical method, such as regula falsi. Residual is formulated by a difference between the dry bulb temperature leaving the cooler and the setpoint. As the solver progress it varies flow rate on the secondary side until the setpoint is met. For each iteration, a new effectiveness is calculated as a function of Flow Ratio. The new flow is used for the \(\left(\dot{m}c_{p}\right)_{min}\) term and the new effectiveness is used to calculate a result for leaving drybulb. The numerical method is the same for dry and wet operation, only the functions will use different curves and state variables to describe performance. The regula falsi solver can vary secondary flow rate, \(\dot{V}_{sec}\) , to drive the following residual to zero:
+
+\begin{equation}
+\text{residual} = T_{db,out,sys} - T_{db,out,setpoint}
+\end{equation}
+
+``Dry or Wet Op Modulated'' is the most complex situation. There is an overlap and the cooler could deliver the setpoint air using either dry operation or wet operation. The model proceeds separately to calculate both wet and dry operation, with separate numerical solvers for modulation in each mode. Then the fan and pump power is calculated for each mode. Select the lowest power mode as the preferred choice. (This doesn't really count the value of water, could bring in a source factor but \ldots{}). Discard results for the unused mode.
+
+The purge air, or secondary airside, is the stream that evaporates water and indirectly cools the primary, or system air.~ The result from Equation is then compared to a lower bound, \({T_{db,out,bound}}\) , determined from the dewpoint of the incoming purge air using Equation .
+
+\begin{equation}
+{T_{db,out,bound}} = {T_{db,in,sys}} - \beta ({T_{db,in,sys}} - {T_{dew,in,purge}})
+\end{equation}
+
+where,
+
+\({T_{dew,in,purge}}\) ~ is the dewpoint of purge air entering the wet side of cooler {[}ºC{]}
+
+\(\beta\) ~~~~~~~~~~~~~ is a factor for how close to dewpoint is possible (eg. 0.9)
+
+The final result (for PLF = 1) is the larger of the results from Equations and .
+
+The indirect cooler has the ability to overcool the air and therefore needs some form of modulation.~ A Part Load Fraction, PLF, is used to model the implications of controlling the amount of cooling.~ It is assumed that through on/off cycling that the cooling power can be varied to exactly meet the desired temperature when PLF is less than unity.
+
+\begin{equation}
+{\dot Q_{Full}} = \dot m\left( {{h_{out,sys}} - {h_{in,sys}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{{\mathop{\rm Re}\nolimits} quired}} = \dot m\left( {{h_{out,desired}} - {h_{in,sys}}} \right)
+\end{equation}
+
+\begin{equation}
+PLF = \frac{{{{\dot Q}_{{\mathop{\rm Re}\nolimits} quired}}}}{{{{\dot Q}_{Full}}}}
+\end{equation}
+
+where,
+
+\(PLF\) ~~~~~~~~~~~~~~~~~~~~ is the Part Load Fraction
+
+When PLF is less than 1.0 it is assumed that the cooler will deliver the desired temperature air (as long as it is less than the inlet; it doesn't need heating).~ The PLF is used to modify the auxiliary fan power when the fan power modifier curve is not specified and find when the unit will overcool.
+
+\begin{equation}
+{P_{fan}} = \Delta P\cdot \dot V\cdot e\cdot PLF
+\end{equation}
+
+Water pump power is also derated using the PLF.
+
+A third air stream input to the cooler was implemented in order to allow mixing building exhaust air with outdoor air on the purge/secondary side of the cooler. The assumption when relief/tertiary air is used is that all of the available relief zone air is used and the remainder made up with outdoor air.~ Moisture and energy balances are drawn to compute humidity ratio and enthalpy of mixed secondary air.~ The volume is determined by the design volume flow rate (from secondary fan size).
+
+\subsubsection{Water Consumption}\label{water-consumption}
+
+Water consumption is an important consideration when evaluating evaporative coolers.~ Water consumption of the evaporative cooler is modeled using Equation .
+
+\begin{equation}
+{\dot V_{water}} = {\dot V_{evap}} + {\dot V_{drift}} + {\dot V_{blowdown}}
+\end{equation}
+
+The three components of water consumption are evaporation, drift, and blowdown.~ Evaporation is the water evaporated as the normal part of the evaporative cooler thermodynamic process and is calculated using:
+
+\begin{equation}
+{\dot V_{evap}} = \frac{{{{\dot Q}_{IEC}}}}{{{\rho_{water}}{h_{fg}}}}
+\end{equation}
+
+where,
+
+\({\dot V_{evap}}\) ~is the volume flow rate of useful water evaporation {[}m\(^{3}\)/s{]}
+
+\({h_{fg}}\) ~is the heat of vaporization of water (taken as 2,500,000 J/kg)
+
+\({\dot Q_{IEC}}\) ~is the rate of heat transfer calculated as by Equation or Equation {[}W{]}
+
+\({\rho_{water}}\) ~is the density of water {[}kg/m3{]}
+
+Drift is water that leaves the secondary side as droplets and does not contribute to the evaporative cooling process in a useful manner.~ It is calculated using a user input factor that describes drift as a fraction of \({\dot V_{evap}}\) .
+
+\begin{equation}
+{\dot V_{drift}} = {\dot V_{evap}} * {f_{drift}}
+\end{equation}
+
+Blowdown is water drained from the sump to counter the build up of solids in the water that would otherwise occur because of evaporation.~ It is calculated using a user input factor for the blowdown concentration ratio ,\({R_{concentration}}\) ~, which is the ratio of solids in in the blowdown water compared to the solids in the fresh makeup water and is limited to values of 2 or higher.~ The make up water needed for blowdown is calculated using:
+
+\begin{equation}
+{\dot V_{blowdown}} = \frac{{{{\dot V}_{evap}}}}{{\left( {{R_{concentration}} - 1.0} \right)}} - {\dot V_{drift}}
+\end{equation}
+
+\begin{figure}[hbtp] % fig 207
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4833.png}
+\caption{Research Special Indirect Evaporative Cooler Using Relief Air \protect \label{fig:research-special-indirect-evaporative-cooler-001}}
+\end{figure}
+
+\subsubsection{Indirect Evaporative Cooler Sizing}\label{indirect-evaporative-cooler-sizing-000}
+
+The model for the object called EvaporativeCooler:Indirect:ResearchSpecial has a field for the secondary fan flow rate that can be autosized.
+
+\paragraph{Secondary Air DesignFan Flow Rate}\label{secondary-air-designfan-flow-rate}
+
+The secondary air design flow rate fan is not part of an airstream that is directly modeled in EnergyPlus. Because the primary side air flows can be autosized as part of the air system, it is convenentconvenient to also scale the size of the secondary flow. If the cooler is part of the main loop of a central air system, then the secondary fan flow rate is sized to equal to the main design flow rate.
+
+User inputs for autosizing scaling factors are included so that when modeling an autosized IEC, all the design values can be scaled off of Primary Design Air Flow Rate. User input for Secondary Air Flow Sizing Factor is multiplied by DesMainVolFlow\(_{sys}\) as follows:
+
+\begin{equation}
+\dot{V}_{sec,design} = \text{DesMainVolFlow}_{sys}\cdot\text{SecAirFlowScalingFactor}
+\end{equation}
+
+If the cooler is part of the outdoor air path of a central air system, then the secondary air design flow rate is sized to be the maximum of either the design minimum outdoor air flow rate or one-half of the main design flow rate.
+
+\begin{equation}
+\dot{V}_{sec,design} = \max\left(\text{DesOutAirVolFlow},0.5\cdot\text{DesMainVolFlow}_{sys}\right)\cdot\text{SecAirFlowScalingFactor}
+\end{equation}
+
+\paragraph{Secondary Fan Design Power}\label{secondary-fan-design-power}
+
+The Secondary Fan Design Power is outosized from secondary air design flow rate and user input for Secondary Fan Sizing Specific Power in units of W/(m3/s) as follows:
+
+\begin{equation}
+P_{sec,fan,design} = \dot{V}_{sec,design}\cdot\text{FanPowerScalingFactor}
+\end{equation}
+
+\paragraph{Recirculating Water Design Pump Power}\label{recirculating-water-design-pump-power}
+
+The Recirculating Water Design Pump Power is sized from secondary air design flow rate and user input for recirculating and spraying Water Pump Power Sizing Factor in units of W/(m3/s) or W-s/m3 and is given by:
+
+\begin{equation}
+P_{pump,design} = \dot{V}_{sec,design}\cdot\text{PumpPowerScalingFactor}
+\end{equation}
+
+Where,
+
+\(\dot{V}_{sys,design}\) = primary air design volume flow rate in m3/s
+
+\(\dot{V}_{sec,design}\) = secondary air design volume flow rate in m3/s
+
+\(\text{SecAirFlowScalingFactor}\) = user specified Secondary air flow sizing factor in units of W/(m3/s) for secondary design air flow rate calculation.
+
+\(\text{FanPowerScalingFactor}\) = user specified secondary air fan sizing specific power in units of W/(m3/s) for design fan power calculation.
+
+\(\text{PumpPowerScalingFactor}\) = user specified recirculating and spraying water pump power sizing factor in units of W/(m3/s) for design pump power calculation.
+
+\subsection{Direct Evaporative Cooler Special Research Model}\label{direct-evaporative-cooler-special-research-model}
+
+This section summarizes the model implemented in the component EvaporativeCooler:Direct:ResearchSpecial.~ This model can use a simple constant effectiveness or a variable effectiveness model that, under part load conditions, can modulate so that the air leaving the cooler just meets a drybulb temperature setpoint.~ The algorithm used to determine the changes to the system air proceeds in four steps:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\tightlist
+\item
+  Calculate the current operation effectiveness using effectiveness modifying curve
+\end{enumerate}
+
+2)~Calculate full load performance using a part load fraction (PLF) = 1 and Equation .
+
+3)~Calculate PLF using Equations , , and .
+
+4)~Recalculate cooler performance using the PLF.
+
+\begin{equation}
+ \begin{array}{rl}
+  \epsilon_{op} & = \epsilon_{design}\cdot f_{mod}\left(flowRatio\right) \\
+  T_{db,out,sys} & = T_{db,in,sys} - \epsilon_{op}\cdot\left(T_{db,in,sys}-T_{wb,in,sys}\right) \\
+  T_{db,out} & = T_{db,in}-\epsilon\left(T_{db,in}-T_{wb,in}\right)
+ \end{array}
+\end{equation}
+
+where,
+
+\begin{itemize}
+\item
+  \({T_{db,out,sys}}\) ~is the drybub temperature of the air leaving the cooler {[}ºC{]},
+\item
+  \({T_{db,in,sys}}\) ~is the drybulb temperature of the air entering the cooler {[}ºC{]},
+\item
+  \({T_{wb,in,sys}}\) ~is the wetbulb temperature of the air entering the cooler {[}ºC{]}, and
+\item
+  \(\epsilon_{design}\) ~is the cooler design effectiveness.
+\item
+  \(\epsilon_{op}\) ~is the cooler current operation effectiveness.
+\item
+  \(f_{mod}\) ~is the effectiveness modifier curve as a function of system air flow fraction
+\end{itemize}
+
+The wetbulb temperature of air leaving a direct cooler is the same as the wetbulb temperature entering the cooler.~ The leaving humidity ratio of the air is calculated using psychrometric functions with leaving drybulb and wetbulb temperatures and outdoor air pressure as inputs.~ The leaving enthalpy of air is calculated using psychrometric functions with leaving drybulb temperature, leaving humidity ratio, and outdoor air pressure as inputs.
+
+The direct cooler sometimes has the ability to overcool the air and therefore some form of modulation is useful for analysis.~ The special research model includes a Part Load Fraction, PLF, used to model the implications of controlling the amount of cooling.~ It is assumed that through some sort of on/off cycling or wetness control that the cooling electric power can be varied to exactly meet the desired temperature when PLF is less than unity.~ The auxiliary water pump power is then varied using pump power modifier curve or linearly using a Part Load Fraction when the pump power modifier curve is not specified.
+
+\begin{equation}
+{\rm{FullOutput}} = {T_{db,out}} - {T_{db,in}}
+\end{equation}
+
+\begin{equation}
+{\rm{RequiredOutput}} = {T_{db,desired}} - {T_{db,in}}
+\end{equation}
+
+\begin{equation}
+PLF = \frac{{{\rm{RequiredOutput}}}}{{{\rm{FullOutput}}}}
+\end{equation}
+
+When PLF is less than 1.0 it is assumed that the cooler will deliver the desired temperature air (as long as it is less than the inlet; it doesn't need heating).~ Water pump power is also derated using the user specified pump modifier curve or using PLF when the pump modifier curve is not specified.
+
+\subsubsection{Water Consumption}\label{water-consumption-1}
+
+Water consumption is an important consideration when evaluating evaporative coolers.~ Water consumption of the evaporative cooler is modeled using Equation .
+
+\begin{equation}
+{\dot V_{water}} = {\dot V_{evap}} + {\dot V_{drift}} + {\dot V_{blowdown}}
+\end{equation}
+
+The three components of water consumption are evaporation, drift, and blowdown.~ Evaporation is the water evaporated as the normal part of the evaporative cooler thermodynamic process and is calculated using:
+
+\begin{equation}
+{\dot V_{evap}} = \frac{{\dot m\left( {{w_{out}} - {w_{in}}} \right)}}{{{\rho_{water}}}}
+\end{equation}
+
+where,
+
+\({\dot V_{evap}}\) ~is the volume flow rate of useful water evaporation {[}m\(^{3}\)/s{]}
+
+\({w_{out}}\) ~is the humidity ratio of the air leaving the cooler {[}kg/kg{]}
+
+\({w_{in}}\) ~is the humidity ratio of air entering the cooler {[}kg/kg{]}
+
+\(\dot m\) ~is the mass flow rate of air moving through the cooler {[}kg/s{]}
+
+\({\rho_{water}}\) ~is the density of water {[}kg/m3{]}
+
+Drift is water that leaves the cooler (and supply air duct) as droplets and does not contribute to the evaporative cooling process in a useful manner.~ It is calculated using a user input factor that describes drift as a fraction of \({\dot V_{evap}}\) .
+
+\begin{equation}
+{\dot V_{drift}} = {\dot V_{evap}} * {f_{drift}}
+\end{equation}
+
+Blowdown is water drained from the sump to counter the build up of solids in the water that would otherwise occur because of evaporation.~ It is calculated using a user input factor for the blowdown concentration ratio ,\({R_{concentration}}\) , which is the ratio of solids in the blowdown water compared to the solids in the fresh makeup water and is limited to values of 2 or higher.~ The make up water needed for blowdown is calculated using:
+
+\begin{equation}
+{\dot V_{blowdown}} = \frac{{{{\dot V}_{evap}}}}{{\left( {{R_{concentration}} - 1.0} \right)}} - {\dot V_{drift}}
+\end{equation}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/heat-exchangers.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/heat-exchangers.tex
new file mode 100644
index 00000000000..ed7acf149a7
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/heat-exchangers.tex
@@ -0,0 +1,1711 @@
+\section{Heat Exchangers }\label{heat-exchangers}
+
+\subsection{Air System Air-To-Air Sensible and Latent Effectiveness Heat Exchanger}\label{air-system-air-to-air-sensible-and-latent-effectiveness-heat-exchanger}
+
+\subsubsection{Overview}\label{overview-019}
+
+The input object HeatExchanger:AirToAir:SensibleAndLatent provides a model for a generic, sensible and latent air-to-air heat exchanger that is an HVAC air system component that consists of a heat exchanger and primary/secondary airflow bypass dampers. The specific configuration of the component is shown in the following figure.
+
+\begin{figure}[hbtp] % fig 250
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5455.png}
+\caption{Schematic of the Sensible and Latent Air-to-Air Heat Exchanger \protect \label{fig:schematic-of-the-sensible-and-latent-air-to}}
+\end{figure}
+
+The sensible and latent air-to-air heat exchanger is typically used for exhaust or relief air heat recovery. Heat exchanger performance can be specified to transfer sensible energy, latent energy or both between the supply and exhaust air streams. The input requires no geometric data. Performance is defined by specifying sensible and/or latent effectiveness at 75\% and 100\% of the nominal (rated) supply air flow rate in both heating and cooling conditions (Table~\ref{table:operating-conditions-for-defining-heat}).
+
+% table 74
+\begin{longtable}[c]{p{3.0in}p{1.5in}p{1.5in}}
+\caption{Operating Conditions for Defining Heat Exchanger Performance \label{table:operating-conditions-for-defining-heat}} \tabularnewline
+\toprule 
+Parameter & Conditions \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Operating Conditions for Defining Heat Exchanger Performance} \tabularnewline
+\toprule 
+Parameter & Conditions \tabularnewline
+\midrule
+\endhead
+Entering supply air temperature: \tabularnewline
+Dry-bulb & 1.7°C (35°F) & 35°C (95°F) \tabularnewline
+Wet-bulb & 0.6°C (33°F) & 26°C (78°F) \tabularnewline
+Entering exhaust air temperature: \tabularnewline
+Dry-bulb & 21°C (70°F) & 24°C (75°F) \tabularnewline
+Wet-bulb & 14°C (58°F) & 17°C (63°F) \tabularnewline
+\multicolumn{3}{l}{Note: Conditions consistent with the Air-Conditioning and Refrigeration Institute’s}  \tabularnewline
+\multicolumn{3}{l}{Standard 1060 (ARI 2001).} \tabularnewline
+\bottomrule
+\end{longtable}
+
+Heat exchange between the supply and exhaust air streams occurs whenever the unit is scheduled to be available (availability schedule) and supply/exhaust air flows are present. This heat exchanger object can be used in conjunction with a conventional air-side economizer (i.e., specify an appropriate economizer control type in the Controller:OutdoorAir object), whereby heat exchange is suspended whenever the air-side economizer is active (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped). This object is also able to suspend heat exchange for the purpose of providing free cooling operation in the absence of a conventional air-side economizer (i.e., specify MinimumFlowWithBypass in the Controller:Outside Air object). Suspension of heat exchange during economizer mode may be customized as necessary using the economizer lockout field. Note that the Economizer Type must be set to something other than NoEconomizer for this control interaction to function.
+
+Several methods of frost control are available to warm the heat exchanger core to prevent frost formation. Available methods are preheat, exhaust only, exhaust air recirculation, and minimum exhaust temperature. Preheat frost control uses a separate heater object placed in the supply inlet air stream to keep the air temperature above the frost threshold temperature. All other frost control methods are modeled within this heat exchanger object.
+
+This heat exchanger object can also control the supply air outlet temperature to a setpoint when a setpoint manager and temperature schedule are used. This temperature control is accomplished through wheel speed modulation or bypassing supply air around the heat exchanger to maintain the desired setpoint and avoid overheating or overcooling the supply air.
+
+\subsubsection{Model Description}\label{model-description-011}
+
+The heat exchanger object models energy transfer between the supply air stream and the exhaust air stream according to the effectiveness values that are specified by the user in the input data file (see IO Reference Document, HeatExchanger:AirToAir:SensibleAndLatent). The operating volumetric air flow rate through the heat exchanger (i.e., the average of the actual supply and exhaust air flow rates for the simulation time step) should be between 50\% and 130\% of the nominal supply air flow rate specified for the heat exchanger. Operating air flow rates outside this range result in a warning message and a recommendation to adjust air flow rates to within the appropriate range.
+
+The user must enter the sensible and latent effectiveness of the heat exchanger for heating and cooling conditions (Table~\ref{table:operating-conditions-for-defining-heat}) with balanced air flow (supply flow equal to the exhaust flow) at two flow rates: 75\% and 100\% of the nominal supply air flow rate. Heat exchanger manufacturers can typically provide this performance information, and it is also available for equipment contained in ARI's Certified Product Directory for Air-to-Air Energy Recovery Ventilation Equipment (ARI 2003). Values may be entered for sensible effectiveness, latent effectiveness, or both. The model assumes default values of 0.0 for sensible and latent effectiveness, thus requiring the user to input representative values for the heat exchanger being modeled.
+
+To obtain the ``operating'' effectiveness of the heat exchanger at different air flow rates, the model first calculates the average volumetric air flow rate through the heat exchanger (average of the supply and exhaust air flow rates) for each simulation time step. Air flows through the heat exchanger may be unbalanced (supply greater than exhaust, or vice versa), but an unbalanced air flow ratio greater than 2:1 is not recommended~ (beyond this range a warning message is issued). The model determines the operating effectiveness of the heat exchanger by linear interpolation or extrapolation of the 100\% flow and 75\% flow effectiveness values specified in the input data file, using the average volumetric air flow rate through the heat exchanger. Extrapolation is allowed down to 50\% and up to 130\% of the nominal supply air flow rate (beyond this range a warning message is issued).
+
+\({\varepsilon_{operating,sensible}} = {\varepsilon_{sensible,75\% \,flow}} + ({\varepsilon_{sensible,100\% \,flow}} - {\varepsilon_{sensible,75\% \,flow}})\left( {\frac{{H{X_{flowratio}} - 0.75}}{{1 - 0.75}}} \right)\) ~
+
+\begin{equation}
+{\varepsilon_{operating,latent}} = {\varepsilon_{latent,75\% \,flow}} + ({\varepsilon_{latent,100\% \,flow}} - {\varepsilon_{latent,75\% \,flow}})\left( {\frac{{H{X_{flowratio}} - 0.75}}{{1 - 0.75}}} \right)
+\end{equation}
+
+\emph{where}:
+
+\({\varepsilon_{operating,sensible}}\) ~ = operating sensible effectiveness of the heat exchanger
+
+\({\varepsilon_{operating,latent}}\) ~~~ = operating latent effectiveness of the heat exchanger
+
+\({\varepsilon_{sensible,75\% \,flow}}\) ~ = ~ sensible effectiveness at 75\% airflow condition
+
+\({\varepsilon_{sensible,100\% \,flow}}\) ~ = ~ sensible effectiveness at 100\% airflow condition
+
+\({\varepsilon_{latent,75\% \,flow}}\) ~ = ~ latent effectiveness at 75\% airflow condition
+
+\({\varepsilon_{latent,100\% \,flow}}\) ~ = ~ latent effectiveness at 100\% airflow condition
+
+\(H{X_{flowratio}}\) ~ = the ratio of the average operating volumetric air flow rate {[}(supply flow plus exhaust flow) / 2.0{]} to the nominal supply air flow rate
+
+If the heat exchanger's supply air inlet temperature is less than the exhaust air inlet temperature, the operating sensible and latent effectivenesses are calculated using the 75\% and 100\% heating condition values; otherwise, the 75\% and 100\% cooling effectiveness values are used in Equations and .
+
+The supply air conditions leaving the heat exchanger are determined using the heat exchanger operating effectiveness calculated above, the ratio of the air stream with the minimum heat capacity rate to the supply air stream heat capacity rate, and the difference in temperature or humidity ratio between the supply and exhaust inlet air:
+
+\begin{equation}
+\mathop m\limits^ \bullet  cp,\min \, = MIN(\mathop m\limits^ \bullet  cp,\sup \,,\,\mathop {\,m}\limits^ \bullet  cp,exh)
+\end{equation}
+
+\begin{equation}
+{T_{SupAirOut}} = {T_{SupAirIn}} + {\varepsilon_{operating,sensible}}\left( {\frac{{\mathop m\limits^ \bullet  cp,\min }}{{\mathop m\limits^ \bullet  cp,\sup }}} \right)({T_{ExhAirIn}} - {T_{SupAirIn}})
+\end{equation}
+
+\begin{equation}
+{\omega_{SupAirOut}} = {\omega_{SupAirIn}} + {\varepsilon_{operating,latent}}\left( {\frac{{\mathop m\limits^ \bullet  cp,\min }}{{\mathop m\limits^ \bullet  cp,\sup }}} \right)({\omega_{ExhAirIn}} - {\omega_{SupAirIn}})
+\end{equation}
+
+\emph{where}:
+
+\(\mathop m\limits^ \bullet cp,\min\) ~~~~~~~~~~ = minimum heat capacity rate (W/K)
+
+\(\mathop m\limits^ \bullet cp,\sup\) ~~~~~~~~~~~ = heat capacity rate of the supply air stream (W/K)
+
+\(\mathop {\,m}\limits^ \bullet cp,exh\) ~~~~~~~~~~ = heat capacity rate of the exhaust air stream (W/K)
+
+\emph{T\(_{SupAirOut}\)} = supply air temperature leaving the heat exchanger (°C)
+
+\emph{T\(_{SupAirIn}\)} = supply air inlet temperature (°C)
+
+\emph{T\(_{ExhAirIn}\)} = exhaust air inlet temperature (°C)
+
+\({\omega_{SupAirOut}}\) ~~~~~~~~~ = supply air humidity ratio leaving the heat exchanger (kg/kg)
+
+\({\omega_{SupAirIn}}\) ~~~~~~~~~~ = supply air inlet humidity ratio (kg/kg)
+
+\({\omega_{ExhAirIn}}\) ~~~~~~~~~~ = exhaust air inlet humidity ratio (kg/kg)
+
+Using the supply air outlet temperature and humidity ratio, the enthalpy of the supply air leaving the heat exchanger is calculated.
+
+\begin{equation}
+{h_{SupAirOut}} = PsyHFnTdbW({T_{SupAirOut}},{\omega_{SupAirOut}})
+\end{equation}
+
+where:
+
+\emph{h\(_{SupAirOut}\)} = enthalpy of the supply air leaving the heat exchanger (J/kg)
+
+\emph{PsyHFnTdbW} = psychrometric routine calculating air enthalpy as a function of
+
+~~~ temperature and humidity ratio
+
+If the predicted conditions of the supply air leaving the heat exchanger exceed the saturation curve (\textgreater{}100\% RH), then the temperature and humidity ratio of the air are reset to saturated conditions ( = 100\% RH) at the enthalpy condition calculated above (\emph{h\(_{SupAirOut}\)).}
+
+Next, the sensible and total heat recovery rates of the heat exchanger are calculated:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Sensible}} = \left( {\mathop m\limits^ \bullet  cp,\sup } \right)({T_{SupAirIn}} - {T_{SupAirOut}})
+\end{equation}
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Total}} = {\mathop m\limits^ \bullet_{SupAir}}({h_{SupAirIn}} - {h_{SupAirOut}})
+\end{equation}
+
+where:
+
+\[{\mathop Q\limits^ \bullet_{Sensible}}\] ~~~~~~~~~~~ = sensible heat recovery rate (W)
+
+\({\mathop Q\limits^ \bullet_{Total}}\) ~~~~~~~~~~~~~~ = total heat recovery rate (W)
+
+\emph{h\(_{SupAirIn}\)}~~~~~~~~~~~ = supply air inlet enthalpy (J/kg)
+
+\({\mathop m\limits^ \bullet_{SupAir}}\) ~~~~~~~~~~~~ = mass flow rate of the supply air stream (kg/s)
+
+The conditions of the exhaust (secondary) air leaving the heat exchanger are then calculated:
+
+\begin{equation}
+{T_{ExhAirOut}} = {T_{ExhAirIn}}\, + \,\,\frac{{{{\mathop Q\limits^ \bullet  }_{Sensible}}}}{{\mathop m\limits^ \bullet  cp,exh}}
+\end{equation}
+
+\begin{equation}
+{h_{ExhAirOut}} = {h_{ExhAirIn}}\, + \,\,\frac{{\mathop Q\limits^ \bullet  {\,_{Total}}}}{{{{\mathop m\limits^ \bullet  }_{_{ExhAir}}}}}
+\end{equation}
+
+\begin{equation}
+{\omega_{ExhAirOut}} = PsyWFnTdbH({T_{ExhAirOut}},{h_{ExhAirOut}})
+\end{equation}
+
+\emph{where}:
+
+\emph{T\(_{ExhAirOut}\)} = exhaust air temperature leaving the heat exchanger (°C)
+
+\emph{h\(_{ExhAirOut}\)}~~~~~~~~~~ = exhaust air enthalpy leaving the heat exchanger (J/kg)
+
+\({\mathop m\limits^ \bullet_{ExhAir}}\) ~~~~~~~~~~~~ = mass flow rate of the exhaust air stream (kg/s)
+
+\({\omega_{ExhAirOut}}\) ~~~~~~~~~ = exhaust air humidity ratio leaving the heat exchanger (kg/kg)
+
+\emph{PsyWFnTdbH} = psychrometric routine calculating air humidity ratio as a function of temperature and enthalpy
+
+As was done for the supply air, calculated exhaust air conditions beyond the saturation curve are reset to saturation conditions at the calculated air enthalpy value.
+
+Once the air conditions leaving each side of the heat exchanger (supply and exhaust) are calculated, this air is blended with any bypass air that was directed around the heat exchanger core to determine the final air conditions leaving the heat exchanger unit. These outlet air conditions are used in Equations and to determine the sensible and total heat recovery rate for the overall heat exchanger unit. The latent heat recovery rate for the overall unit is then calculated as the difference between the total and sensible heat recovery rates:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Latent}} = {\mathop Q\limits^ \bullet_{Total}}\,\, - \,{\mathop {\,Q}\limits^ \bullet_{Sensible}}
+\end{equation}
+
+Heat recovery electric power is the electric consumption rate of the unit in watts. The nominal electric power rate for the heat exchanger is specified in the input data file, and can be used to model controls (transformers, relays, etc.) and/or a motor for a rotary heat exchanger. The model assumes that this electric power is consumed whenever the heat exchanger is scheduled to operate and supply/exhaust air flow rates exist. The electric power is assumed to be zero for all other times or if heat exchange is suspended to provide free cooling (economizer operation). None of this electric power is assumed to contribute thermal load to either of the heat exchanger air streams.
+
+At the end of each HVAC simulation time step, this object reports the sensible, latent and total heat recovery rates for the overall unit as calculated above. The heat recovery rates are reported separately for times when the supply air is heated and when it is cooled (Ref: HeatExchanger:AirToAir:SensibleAndLatent in the EnergyPlus Input Output Reference). The heat recovery electric power is also reported for each simulation time step. In addition to the heat recovery rates and electric power, heating/cooling energy transferred to the supply air and the electric energy consumption by the heat exchanger unit are calculated for the time step being reported as follows:
+
+\begin{equation}
+\,{Q_{SensibleCooling}} = \,\,{\mathop Q\limits^ \bullet_{SensibleCooling}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.
+\end{equation}
+
+\begin{equation}
+\,{Q_{LatentCooling}} = \,\,{\mathop Q\limits^ \bullet_{LatentCooling}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.
+\end{equation}
+
+\begin{equation}
+\,{Q_{TotalCooling}} = \,\,{\mathop Q\limits^ \bullet_{TotalCooling}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.
+\end{equation}
+
+\begin{equation}
+\,{Q_{SensibleHeating}} = \,\,{\mathop Q\limits^ \bullet_{SensibleHeating}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.
+\end{equation}
+
+\begin{equation}
+\,{Q_{LatentHeating}} = \,\,{\mathop Q\limits^ \bullet_{LatentHeating}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.
+\end{equation}
+
+\begin{equation}
+\,{Q_{TotalHeating}} = \,\,{\mathop Q\limits^ \bullet_{TotalHeating}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.
+\end{equation}
+
+\begin{equation}
+\,{E_{HXUnit}} = \,\,{P_{HXUnit}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.
+\end{equation}
+
+where: \(Q_{SensibleCooling}\) = output variable `Heat Exchanger Sensible Cooling Energy, J'
+
+\(\,{\mathop Q\limits^ \bullet_{SensibleCooling}}\) ~~~~~~~~~ = output variable `Heat Exchanger Sensible Cooling Rate, W' = \[{\mathop Q\limits^ \bullet_{Sensible}}\]
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ during times when the supply air is cooled
+
+\emph{TimeStepSys} ~~~~~~~~~ = HVAC system simulation time step, hr \(Q_{LatentCooling}\) = output variable `Heat Exchanger Latent Cooling Energy, J'
+
+\(\,{\mathop Q\limits^ \bullet_{LatentCooling}}\) ~~~~~~~~~~ = output variable `Heat Exchanger Latent Cooling Rate, W' = \[{\mathop Q\limits^ \bullet_{Latent}}\]
+
+~~ during times when the supply air is dehumidified \(Q_{TotalCooling}\) = output variable `Heat Exchanger Total Cooling Energy, J'
+
+\(\,{\mathop Q\limits^ \bullet_{TotalCooling}}\) ~~~~~~~~~~~~ = output variable `Heat Exchanger Total Cooling Rate, W' = \({\mathop Q\limits^ \bullet_{Total}}\) during
+
+~~~ times when the supply air enthalpy is reduced \(Q_{SensibleHeating}\) = output variable `Heat Exchanger Sensible Heating Energy, J'
+
+\(\,{\mathop Q\limits^ \bullet_{SensibleHeating}}\) ~~~~~~~~~ = output variable `Heat Exchanger Sensible Heating Rate, W' = \[{\mathop Q\limits^ \bullet_{Sensible}}\]
+
+~~ during times when the supply air is heated \(Q_{LatentHeating}\) = output variable `Heat Exchanger Latent Heating Energy, J'
+
+\(Q_{LatentHeating}\) = output variable `Heat Exchanger Latent Gain Energy, J'
+
+\(\,{\mathop Q\limits^ \bullet_{LatentHeating}}\) ~~~~~~~~~~ = output variable `Heat Exchanger Latent Gain Rate, W' = \[{\mathop Q\limits^ \bullet_{Latent}}\] ~during times when the supply air is humidified \(Q_{TotalHeating}\) = output variable `Heat Exchanger Total Heating Energy, J'
+
+\(\,{\mathop Q\limits^ \bullet_{TotalHeating}}\) ~~~~~~~~~~~~ = output variable `Heat Exchanger Total Heating Rate, W' = \({\mathop Q\limits^ \bullet_{Total}}\) during times when the supply air enthalpy is increased
+
+\(\,{E_{HXUnit}}\) ~~~~~~~~~~~~~~~~~ = output variable `Heat Exchanger Electric Energy, J'
+
+\({P_{HXUnit}}\) ~~~~~~~~~~~~~~~~~~ = output variable `Heat Exchanger Electric Power, W'
+
+\subsubsection{Frost Control Methods}\label{frost-control-methods}
+
+In cold weather, frost can form on the heat exchanger causing a reduction in air flow and heat recovery performance. Various strategies can be employed to limit frost formation. Heat exchangers that transfer total energy (sensible plus latent) usually have a lower frost threshold temperature than sensible-only heat exchangers. Frost threshold temperatures for sensible-only heat exchangers may be -1°C to -12°C for plate and rotary heat exchangers respectively, while those for comparable total (sensible plus latent) heat exchangers may be 10°C lower. The frost threshold temperature for a specific application is dependent on the exhaust air dry-bulb temperature and relative humidity, heat exchanger type (e.g., sensible-only or total heat exchange, flat plate or rotary), and the heat exchanger effectiveness. Consult manufacturer's literature to obtain specific frost threshold temperatures for the heat exchanger being modeled.
+
+Four frost control strategies can be modeled for this air-to-air heat exchanger unit. Each of these four strategies is discussed in detail below.
+
+\subsubsection{Preheat}\label{preheat}
+
+One method to control frost formation is to preheat the cold outdoor (supply) air entering the heat exchanger. When a preheat coil is used for frost control, a separate heating coil object must be placed in the supply air stream at the inlet to the heat exchanger (Coil:Heating:Water, Coil:Heating:Electric or Coil:Heating:Gas). The preheat coil should be controlled to maintain a minimum supply air inlet temperature thereby eliminating frost buildup on the heat exchanger core. When modeling preheat frost control, specify ``None'' as the frost control method in the heat exchanger object. When modeling this heat exchanger as part of an air loop, refer to the objects AirLoopHVAC:OutdoorAirSystem and SetpointManager:Scheduled the EnergyPlus Input Output Reference for additional information on specifying a preheat coil and controlling its supply air temperature.This frost control method is not currently available when this heat exchanger is being used as part of the compound object ZoneHVAC:EnergyRecoveryVentilator.
+
+\subsubsection{Exhaust Only}\label{exhaust-only}
+
+This method of frost control bypasses the incoming supply air around the heat exchanger core thereby warming the core using the exiting exhaust air. This method is similar to `supply air off' frost control where the supply air fan is turned off for a predetermined period of time while the exhaust air fan continues to operate. For the `supply air off' method, the supply air flow is stopped for a period of time thereby reducing the ventilation air supplied to the zone(s). In addition, the building may be negatively pressurized for the period of time that the supply air flow is stopped since the exhaust air fan continues to operate. On the other hand, the `exhaust only' method of frost control modeled by EnergyPlus continues to provide outdoor ventilation air to the zone(s), but this air is simply bypassed around the heat exchanger core for a portion of the time and the potential problem with negatively pressurizing the building is avoided. Since the supply airflow rate through the heat exchanger core is purposely reduced to control frost formation, average volumetric airflow rates below 50\% of nominal are allowed when this frost control is active and no warning message is issued.
+
+The user enters a threshold temperature, an initial defrost time fraction, and a rate of defrost time fraction increase. When the temperature of the supply air (e.g., outdoor air) entering the heat exchanger is equal to or below the specified threshold temperature, the fractional amount of time that the supply air is bypassed around the heat exchanger core is determined from the following equation:
+
+\begin{equation}
+{X_{DefrostTime}} = {X_{Initial}} + {X_{RateofIncrease}}({T_{Threshold}} - {T_{SupAirIn}})
+\end{equation}
+
+where:
+
+\({X_{DefrostTime}}\) ~ = Fractional time period for frost control \(\left( {0\,\, \le \,\,\,{X_{DefrostTime}}\,\, \le \,\,1} \right)\)
+
+\({X_{Initial}}\) ~~~~~~~ = Initial defrost time fraction
+
+\({X_{RateofIncrease}}\) = Rate of defrost time fraction increase (K\(^{-1}\))
+
+\({T_{Threshold}}\) ~~~~ = Threshold temperature (°C)
+
+\({T_{SupAirIn}}\) ~~~~~~ = Supply air inlet temperature (°C)
+
+During the defrost time, supply air flow is fully bypassed around the heat exchanger core and no heat transfer takes place. For the remainder of the time period, no air is bypassed and full heat exchange is achieved. The average supply air flow bypassed around the heat exchanger core is calculated as follows:
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{_{SupAirBypass}}} = ({X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAir}}}
+\end{equation}
+
+To determine the average heat transfer rates for the simulation time step, the supply air outlet conditions are first calculated as if the heat exchanger were not in defrost mode (see previous section, Model Description). The sensible and total heat transfer rates are then calculated and multiplied by the fractional time period that the heat exchanger is not in defrost mode (1-\emph{X\(_{DefrostTime}\)}).
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Sensible}} = (1 - {X_{DefrostTime}})\left( {\mathop m\limits^ \bullet  cp,\sup } \right)({T_{SupAirIn}} - {T_{SupAirOut}})
+\end{equation}
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Total}} = (1 - {X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAir}}}({h_{SupAirIn}} - {h_{SupAirOut}})
+\end{equation}
+
+Once the average heat transfer rates are determined, the average conditions of the supply air exiting the overall heat exchanger unit are calculated as follows:
+
+\begin{equation}
+{T_{SupAirOut}} = {T_{SupAirIn\,}}\,\,\, - \,\,\,\frac{{{{\mathop Q\limits^ \bullet  }_{Sensible}}}}{{\mathop m\limits^ \bullet  cp,\sup }}
+\end{equation}
+
+\begin{equation}
+{h_{SupAirOut}} = {h_{SupAirIn}}\,\,\, - \,\,\,\frac{{{{\mathop Q\limits^ \bullet  }_{_{Total}}}}}{{{{\mathop m\limits^ \bullet  }_{_{SupAir}}}}}
+\end{equation}
+
+\begin{equation}
+{\omega_{SupAirOut}} = PsyWFnTdbH({T_{SupAirOut}},{h_{SupAirOut}})
+\end{equation}
+
+As described previously, if the predicted conditions of the exiting supply air exceed the saturation curve (\textgreater{}100\% RH), then the temperature and humidity ratio of the air are reset to saturated conditions ( = 100\% RH) at the enthalpy condition calculated above (\emph{h\(_{SupAirOut}\))}. If the supply air temperature is reset, the average sensible heat transfer rate is recalculated before the exhaust air outlet conditions are determined:
+
+\begin{equation}
+{T_{ExhAirOut}} = {T_{ExhAirIn}}\,\,\, + \,\,\,\frac{{{{\mathop Q\limits^ \bullet  }_{Sensible}}}}{{\mathop m\limits^ \bullet  cp,exh}}
+\end{equation}
+
+\begin{equation}
+{h_{ExhAirOut}} = {h_{ExhAirIn}}\,\,\,\, + \,\,\,\frac{{{{\mathop Q\limits^ \bullet  }_{_{Total}}}}}{{{{\mathop m\limits^ \bullet  }_{_{ExhAir}}}}}
+\end{equation}
+
+\begin{equation}
+{\omega_{ExhAirOut}} = PsyWFnTdbH({T_{ExhAirOut}},{h_{ExhAirOut}})
+\end{equation}
+
+\subsubsection{Exhaust Air Recirculation}\label{exhaust-air-recirculation}
+
+This method of frost control routes exhaust (outlet) air back through the supply side of the heat exchanger to warm the core. Since this method routes exhaust air back into the building, the building is typically not depressurized when this frost control is active. However, the incoming supply (outdoor ventilation) air flow is stopped for the fractional period of time that frost control is active. If significant periods of time exist when outdoor temperatures are below the selected threshold temperature and outdoor ventilation air is continuously required, an alternative method of frost control should be considered.
+
+The user enters a threshold temperature, an initial defrost time fraction, and a rate of defrost time fraction increase. When the temperature of the inlet supply air (e.g., outdoor air) is equal to or below the specified threshold temperature, the fractional amount of time that this heat exchanger frost control strategy is active is determined from the following equation:
+
+\begin{equation}
+{X_{DefrostTime}} = {X_{Initial}} + {X_{RateofIncrease}}({T_{Threshold}} - {T_{SupAirIn}})
+\end{equation}
+
+The air mass flow rate of the supply air leaving the heat exchanger unit is then calculated using the defrost time fraction calculated above the mass flow rates of supply and exhaust air entering the unit.
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{_{SupAirOut}}} = (1 - {X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAirIn}}}\,\, + \,\,{X_{DefrostTime}}{\mathop m\limits^ \bullet_{_{ExhAirIn}}}
+\end{equation}
+
+The model assumes that no heat exchange occurs during defrost, and the average supply supply air conditions are simply a blend of the conditions when the unit is not in defrost and the exhaust air inlet conditions during defrost operation:
+
+\begin{equation}
+{T_{SupAirOut}} = \,\,\frac{{(1 - {X_{DefrostTime}}){{\mathop m\limits^ \bullet  }_{_{SupAirIn}}}{T_{SupAirOut,NoDefrost\,}} + \,\,{X_{DefrostTime}}{{\mathop m\limits^ \bullet  }_{_{ExhAirIn}}}{T_{ExhAirIn\,}}}}{{{{\mathop m\limits^ \bullet  }_{_{SupAirOut}}}}}
+\end{equation}
+
+\begin{equation}
+{\omega_{SupAirOut}} = \,\,\frac{{(1 - {X_{DefrostTime}}){{\mathop m\limits^ \bullet  }_{_{SupAirIn}}}{\omega_{SupAirOut,NoDefrost\,}} + \,\,{X_{DefrostTime}}{{\mathop m\limits^ \bullet  }_{_{ExhAirIn}}}{\omega_{ExhAirIn\,}}}}{{{{\mathop m\limits^ \bullet  }_{_{SupAirOut}}}}}
+\end{equation}
+
+\begin{equation}
+{h_{SupAirOut}} = PsyHFnTdbW({T_{SupAirOut}},{\omega_{SupAirOut}})
+\end{equation}
+
+The operating effectivenesses of the heat exchanger are initially calculated according to Equations and assuming no defrost operation. Since the supply air flow across the heat exchanger core is not reduced during defrost operation, the sensible and latent effectiveness are therefore derated (for reporting purposes) in direct proportion to the fraction of time that frost control is not active.
+
+\begin{equation}
+{\varepsilon_{operating,sensible}} = (1 - {X_{DefrostTime}}){\varepsilon_{operating,sensible}}
+\end{equation}
+
+\begin{equation}
+{\varepsilon_{operating,latent}} = (1 - {X_{DefrostTime}}){\varepsilon_{operating,latent}}
+\end{equation}
+
+Since the exhaust outlet air is recirculated through the supply side of the heat exchanger core, the incoming supply air and exiting exhaust air flows are stopped for the fraction of the time when frost control is active. The average air mass flow rate at the supply air inlet and the exhaust air outlet nodes are therefore reduced accordingly.
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{_{SupAirIn}}} = (1 - {X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAirIn}}}
+\end{equation}
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{_{ExhAirOut}}} = (1 - {X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{ExhAirOut}}}
+\end{equation}
+
+The conditions of the exiting (outlet) exhaust air (temperature, humidity ratio and enthalpy) are reported as the values when frost control is not active (i.e., the conditions when exhaust air is actually leaving the unit).
+
+\subsubsection{Minimum Exhaust Temperature}\label{minimum-exhaust-temperature}
+
+With this frost control method, frost formation is avoided by continuously maintaining the temperature of the exhaust air leaving the heat exchanger core above a specified setpoint. The minimum exhaust air temperature is maintained by modulating heat exchanger rotational speed or by bypassing supply air around a plate heat exchanger. For this frost control method, the user must only enter the threshold (minimum) temperature.
+
+For the case of modulating heat exchanger rotation, the operating effectivenesses and outlet air conditions are first calculated as if the heat exchanger is not in defrost mode (see Model Description). If the resulting temperature of the exhaust air leaving the heat exchanger core is below the specified threshold temperature, then the operating effectivenesses are reduced as follows:
+
+\begin{equation}
+{X_{DefrostTime}} = \frac{{({T_{Threshold}} - {T_{ExhAirOut}})}}{{({T_{ExhAirIn}} - {T_{ExhAirOut}})}}
+\end{equation}
+
+\begin{equation}
+{\varepsilon_{operating,sensible}} = (1 - {X_{DefrostTime}}){\varepsilon_{operating,sensible}}
+\end{equation}
+
+\begin{equation}
+{\varepsilon_{operating,latent}} = (1 - {X_{DefrostTime}}){\varepsilon_{operating,latent}}
+\end{equation}
+
+The supply air and exhaust air outlet conditions are then recalculated using these reduced effectiveness values. Finally the sensible, latent and total heat recovery rates are calculated along with the unit's electric power and electric consumption.
+
+The calculation procedure is slightly different for the case of a plate heat exchanger where the supply air is bypassed around the heat exchanger core. Since the volumetric air flow rate through the heat exchanger core is reduced when frost control is active, an iterative process is used to determine the operating effectiveness of the heat exchanger. The operating effectivenesses and outlet air conditions are first calculated as if the heat exchanger is not in defrost mode (see Model Description). If the resulting temperature of the exhaust air leaving the heat exchanger core is below the specified threshold temperature, then the fractional defrost time is calculated as follows:
+
+\begin{equation}
+{X_{DefrostTime}} = \frac{{({T_{Threshold}} - {T_{ExhAirOut}})}}{{({T_{ExhAirIn}} - {T_{ExhAirOut}})}}
+\end{equation}
+
+The iteration process then begins to determine the heat exchanger effectiveness and the exhaust air outlet temperature as if frost control were active. The operating mass flow rate through the supply side of the heat exchanger core is calculated.
+
+\emph{Beginning of iteration process:}
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{_{SupAirCore}}} = (1 - {X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAirIn}}}
+\end{equation}
+
+\begin{equation}
+{\mathop m\limits^ \bullet_{_{SupAirBypass}}} = ({X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAirIn}}}
+\end{equation}
+
+The ratio of average volumetric flow rate through the heat exchanger core to heat exchanger's nominal volumetric flow rate (\emph{HX\(_{flowratio}\)}) is then determined and used to calculate the operating effectiveness of the heat exchanger using Equations and . Since the supply airflow rate through the heat exchanger core is purposely reduced to control frost formation, average volumetric airflow rates below 50\% of nominal are allowed and no warning message is issued. Supply air outlet temperature (leaving the heat exchanger core), sensible heat transfer, and exhaust air outlet temperature are then calculated using the revised heat exchanger effectiveness.
+
+\begin{equation}
+{T_{SupAirOut}} = {T_{SupAirIn}} + {\varepsilon_{operating,sensible}}\left( {\frac{{\mathop m\limits^ \bullet  cp,\min }}{{\mathop m\limits^ \bullet  cp,\sup }}} \right)({T_{ExhAirIn}} - {T_{SupAirIn}})
+\end{equation}
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Sensible}} = (1 - {X_{DefrostTime}})\left( {\mathop m\limits^ \bullet  cp,\sup } \right)({T_{SupAirInlet}} - {T_{SupAirOutlet}})
+\end{equation}
+
+\begin{equation}
+{T_{ExhAirOut}} = {T_{ExhAirIn}} + \frac{{{{\mathop Q\limits^ \bullet  }_{Sensible}}}}{{\mathop m\limits^ \bullet  cp,exh}}
+\end{equation}
+
+The error between the exhaust outlet temperature and the threshold temperature for frost control and a new defrost time fraction are subsequently calculated.
+
+\begin{equation}
+Error = {T_{ExhAirOut}} - {T_{Threshold}}
+\end{equation}
+
+\begin{equation}
+{X_{DefrostTime}} = \,{X_{DefrostTime}}\,\left( {\frac{{{T_{ExhAirIn}} - {T_{ExhAirOut}}}}{{{T_{ExhAirIn}} - {T_{Threshold}}}}} \right)
+\end{equation}
+
+\emph{End of iteration process:}
+
+The iteration process ends when the calculated error is within an error tolerance of 0.001.~ The air streams passing through the heat exchanger core and bypassing the core through the bypass damper are then blended together to provide the air conditions leaving the heat exchanger unit. Finally the sensible, latent and total heat recovery rates are calculated along with the unit's electric power and electric consumption.
+
+\subsubsection{Economizer Operation}\label{economizer-operation}
+
+A conventional air-side economizer may be used in conjunction with this heat exchanger object. The air-side economizer is specified through the use of an outside air controller (see object: Controller:OutdoorAir). Specify the appropriate economizer control type, and provide the required control points and air flow rates as defined in the outside air controller object. Energy transfer provided by the heat exchanger will be suspended whenever free cooling is available (i.e., when the air-side economizer is activated) and \emph{the user specified economizer lockout input is specified as Yes}. For plate heat exchangers, heat transfer is suspended by fully bypassing the supply and exhaust air around the heat exchanger core. For rotary heat exchangers, air flows continue through the core but it is assumed that heat exchanger rotation is stopped.
+
+Heat exchange can also be suspended for the purposes of providing free cooling operation in the absence of a conventional air-side economizer. In this case specify ``MinimumFlowWithBypass'' as the economizer choice and again provide the required control points as defined in the outside air controller object. Energy transfer provided by the heat exchanger will be suspended whenever free cooling is available and \emph{the user specified economizer lockout input is specified as Yes}, however the supply air flow rate will remain at the minimum value specified in the outside air controller object. Note that the Economizer Type must be set to something other than NoEconomizer for this control interaction to function.
+
+If economizer operation is not required, specify ``NoEconomizer'' as the economizer control type in the outside air controller object. The heat exchanger will operate according to its availability schedule and free cooling will not be provided. . If economizer operation \emph{is} required and the heat exchanger \emph{should not} provide free cooling, specify the input for the heat exchanger's economizer lockout as No and heat recovery will remain active during economizer mode.
+
+Heat recovery for this heat exchanger may also be suspended during a high humidity control event (see object Controller:OutdoorAir) in a similar manner. Specifying Yes for economizer lockout will also suspend heat recovery when high humidity control is activated. The default value for economizer lockout is Yes and must be specifically entered as No to disable the economizer or high humidity control lockout feature.
+
+\subsubsection{Supply Air Outlet Temperature Control}\label{supply-air-outlet-temperature-control}
+
+This heat exchanger object can also control the supply air outlet temperature to a setpoint to avoid overheating or overcooling the supply air. This temperature control is accomplished through wheel speed modulation or bypassing supply air around the heat exchanger. To model this temperature control, the user must specify `Yes' for the Supply Air Outlet Temperature Control field in this heat exchanger object, and a separate setpoint manager (see object: SetpointManager:Scheduled) and temperature schedule must be specified for the heat exchanger unit's supply air outlet node.
+
+This control strategy is typically used in conjunction with economizer operation (see object Controller:OutdoorAir), and an example control profile is shown in the figure below. When the outdoor air temperature falls to the specified maximum limit for economizer operation, heat exchange is suspended (air is fully bypassed around the heat exchanger core or heat exchanger rotation is stopped). The figure below shows economizer operation being initiated based on outdoor temperature but other triggers can be used (e.g.~differential temperature {[}outdoor temperature with respect to exhaust air temperature{]}, single point enthalpy or differential enthalpy). Heat exchange remains suspended until the outdoor temperature falls to the minimum temperature (temperature lower limit) for economizer control. The setpoint for the supply air outlet temperature control should match the economizer temperature lower limit.
+
+As the outdoor air temperature falls further below the setpoint for the supply air outlet temperature (same as the economizer lower temperature limit), the heat exchanger bypass dampers will modulate closed to maintain the desired supply air temperature for a plate heat exchanger. For a rotary heat exchanger the rotary heat exchanger speed will gradually increase to maintain the desired supply air temperature. Modulation of heat exchanger performance will continue until the supply air temperature setpoint can no longer be maintained. This control will attempt to achieve the desired temperature set point whether the heat exchanger is cooling or heating the supply air stream. Care should be used to set the supply outlet air temperature set point to the desired value for proper control.
+
+\begin{figure}[hbtp] % fig 251
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5550.png}
+\caption{Air to Air Heat Exchanger with Supply Air Temperature Control \protect \label{fig:air-to-air-heat-exchanger-with-supply-air}}
+\end{figure}
+
+Other types of temperature setpoint control may also be used. For example, the operation described here is used to minimize heating energy and proper control of the supply air temperature set point could also be used to minimize cooling energy or minimize both heating and cooling energy.
+
+\subsubsection{References}\label{references-027}
+
+ARI. 2001. Rating Air-to-Air Heat Exchangers for Energy Recovery Ventilation Equipment. Arlington, Virginia: Air-Conditioning \& Refrigeration Institute.
+
+ARI. 2003. Certified Product Directory for Air-to-Air Energy Recovery Ventilation Equipment. Arlington, Virginia: Air-Conditioning \& Refrigeration Institute.
+
+\subsection{Air System Air-To-Air Flat Plate Heat Exchanger}\label{air-system-air-to-air-flat-plate-heat-exchanger}
+
+\subsubsection{Overview}\label{overview-1-007}
+
+The input object HeatExchanger:AirToAir:FlatPlate provides an NTU -- effectiveness model of a static flat plate air-to-air heat exchanger. Humidity issues are ignored in this model. A full, detailed description of the model can be found in the reference.
+
+The inputs for the model are the design values for the primary air flow rate, primary air inlet and outlet temperature,~ secondary air flow rate, and secondary air inlet temperature. No design UAs are required: instead, the ratio (at design conditions) of the primary \emph{hA} to the secondary \emph{hA} (\emph{r\(_{hA}\)}) is input. The flow configuration is also an input (counter, parallel, or crossflow).
+
+n~An important feature of this model is that the heat exchanger total \emph{UA} is a time varying function of the primary and secondary mass flow rates and inlet temperatures.
+
+\subsubsection{Model Description}\label{model-description-1-007}
+
+The design inlet / outlet conditions determine a design effectiveness \emph{eff}\(_{des}\). From the design capacity flow ratio, the flow arrangement, and \emph{eff}\(_{des,}\) the NTU -- effectiveness formulas give the \emph{NTU\(_{des}\)} and \emph{UA\(_{des}\)}.
+
+The time varying calculations proceed as follows. First the \emph{UA} is determined:
+
+\begin{equation}
+UA = U{A_{des}}({r_{hA}} + 1)/({({\dot m_{p,des}}{T_{p,des}}/{\dot m_p}{T_p})^{.78}} + {r_{hA}}{({\dot m_{s,des}}{T_{s,des}}/{\dot m_s}{T_s})^{.78}})
+\end{equation}
+
+where \emph{des} means \emph{design}, \emph{p} means \emph{primary}, \emph{s} means \emph{secondary}, \emph{T} is air stream temperature, and \(\dot m\) is air stream mass flow rate. From the \emph{UA} and the capacity flow ratio the \emph{NTU} is determined: \(NTU = UA/{C_{\min }}\) . Then the NTU -- effectiveness formulas are used to calculate the effectiveness. From the effectiveness and the inlet conditions, outlet condtions are determined.
+
+\subsubsection{Economizer Operation}\label{economizer-operation-1}
+
+A conventional air-side economizer may be used in conjunction with this heat exchanger object. The air-side economizer is specified through the use of an outside air controller (see object: Controller:OutdoorAir). Specify the appropriate economizer control type, and provide the required control points and air flow rates as defined in the outside air controller object. Energy transfer provided by the heat exchanger will be suspended whenever free cooling is available (i.e., when the air-side economizer is activated) or high humidity control is active and \emph{the user specified economizer lockout input is specified as Yes}. For this flat plate heat exchanger, heat transfer is suspended by fully bypassing the supply and exhaust air around the heat exchanger core. If the economizer lockout is specified as No, the flat plate heat exchanger is operational even when economizer or high humidity mode is active. The default value for economizer lockout is Yes and must be specifically entered as No to disable the economizer or high humidity control lockout feature.
+
+\subsubsection{References}\label{references-1-010}
+
+M. Wetter. 1999. \emph{Simulation Model: Air-To-Air Plate Heat Exchanger}, LBNL-42354. This document can be downloaded from \href{http://simulationresearch.lbl.gov}{\emph{http://simulationresearch.lbl.gov}}.
+
+\subsection{Air System Air-To-Air Balanced Flow Desiccant Heat Exchanger}\label{air-system-air-to-air-balanced-flow-desiccant-heat-exchanger}
+
+\subsubsection{Overview}\label{overview-2-006}
+
+The input object HeatExchanger:Desiccant:BalancedFlow provides a model for a desiccant heat exchanger that is an HVAC component used to model both temperature (sensible) and moisture (latent) heat exchange between two air streams (Figure~\ref{fig:schematic-of-the-balanced-flow-desiccant-heat}). The model assumes balanced air flow through the regeneration and process sides of the heat exchanger (i.e., regeneration and process air volume flow rates and face velocities are the same). Heat exchanger performance is specified through a performance data type object (e.g., Heat Exchanger:Desiccant:BalancedFlow:Performance Data Type 1). Refer to the EnergyPlus Input Output Reference for the specific input syntax for this desiccant heat exchanger object.
+
+\begin{figure}[hbtp] % fig 252
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5554.png}
+\caption{Schematic of the Balanced Flow Desiccant Heat Exchanger \protect \label{fig:schematic-of-the-balanced-flow-desiccant-heat}}
+\end{figure}
+
+EnergyPlus has another air-to-air heat exchanger object for modeling sensible and latent heat transfer between two air streams that uses the input object HeatExchanger:AirToAir:SensibleAndLatent. That heat exchanger model uses effectiveness values specified by the user to determine exiting air conditions from each side of the heat exchanger. In contrast, the balanced flow desiccant heat exchanger references a performance data type object (e.g., HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1) which defines the model equations, user-specified model coefficients, and min/max limits for the model's independent and dependent variables.
+
+\subsubsection{Model Description}\label{model-description-2-006}
+
+This heat exchanger is a simple object that performs three basic functions:
+
+1.~~~~Informs the associated performance data type object (e.g., HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1) if it should calculate heat exchange for a simulation time step, or if heat exchange is suspended for the time step (i.e., bypass air flow around a fixed-plate heat exchanger or stop the rotation of a rotary heat exchanger),
+
+2.~~~~Passes the process and regeneration air inlet conditions (e.g., dry-bulb temperature, humidity ratio, air mass flow rate) to the associated performance data type object, and
+
+3.~~~~Reports the total, sensible and latent cooling/heating rates and electric power based on the results from the performance data type model that is specified.
+
+While the desiccant heat exchanger object's availability to provide heat exchange between the two air streams is determined by the user-specified availability schedule, other objects that call this heat exchanger object can also control its heat exchange during a simulation time step. Currently, this desiccant heat exchanger model can be referenced by two compound objects: CoilSystem:Cooling:DX:HeatExchangerAssisted and Dehumidifier:Desiccant:System, both of which are used to provide enhanced dehumidification over conventional systems. If this heat exchanger is referenced by a compound object, the compound object will control heat exchanger operation (i.e., tell the heat exchanger if heat exchange is needed or not for each simulation time step). Details for how the compound objects control exchanger operation are described elsewhere in this document (ref. CoilSystem:Cooling:DX:HeatExchangerAssisted and Dehumidifier:Desiccant:System).
+
+This desiccant heat exchanger object may also be specified directly in a AirLoopVHAC (air loop BranchList) or in an AirLoopHVAC:OutdoorAirSystem:EquipmentList without being referenced by a compound object. If specified directly in a AirLoopHVAC loop or AirLoopHVAC:OutdoorAirSystem:EquipmentList, then the heat exchanger can be controlled to provide heat exchange based on a maximum and/or minimum humidity setpoint placed on the process air outlet node (ref. SetpointManagers). If no humidity setpoints are provided on this node, then heat exchange will be provided whenever the heat exchanger is available to operate (via its availability schedule) and there is a temperature and/or humidity ratio difference between the two air streams. Further details regarding heat exchanger control via humidity setpoints on the process air outlet node are described in the section for the associated data type object (e.g., HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1).
+
+The balanced flow desiccant heat exchanger model first checks for three conditions to be true before calling the specified performance data type model to calculate heat exchanger performance:
+
+·~~~~~~~~Non-zero air mass flow rates on the process and regeneration inlet air nodes,
+
+·~~~~~~~~Desiccant heat exchanger is available to operate based on its availability schedule,
+
+·~~~~~~~~If a compound object is calling this desiccant heat exchanger, it is requesting that heat exchange be provided.
+
+If any of these conditions is false, then heat exchange is suspended and the model simply passes the air conditions on the process and regeneration air inlet nodes to the respective outlet air nodes. In addition, the heat exchanger electric power is set to zero.
+
+If all of the above conditions are true, then heat exchange is active and the specified performance data type model is called to calculate the process and regeneration outlet air conditions and heat exchanger electric power. Immediately before this call to the performance data type model, a check is made to determine if the operating air flow rates through the heat exchanger (i.e., the actual air flow rates for the simulation time step) are equal (balanced flow). If a difference of more than 2\% exists between the process and regeneration air flow rates at any time during the simulation, a warning is issued.
+
+After the specified performance data type model calculates the process/regeneration air outlet conditions and heat exchanger electric power, the balanced flow desiccant heat exchanger model uses that information to report overall performance. Specifically, the heat exchanger's sensible, latent and total heating and cooling rates are calculated for the process air side of the heat exchanger. Since energy must be conserved, the same heating or cooling rates apply to the regeneration air stream although they are opposite in heat transfer direction (e.g., a sensible cooling rate on the process air side of the heat exchanger would indicate an equivalent sensible heating rate on the regeneration air side).
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Sensible}} = \,{\mathop m\limits^ \bullet_{Proc}}C{p_{Proc,\,\,in}}\left( {{T_{Proc,\,\,out}}\, - \,{T_{Proc,\,\,in}}} \right)
+\end{equation}
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Total}} = \,{\mathop m\limits^ \bullet_{Proc}}\left( {{h_{Proc,\,\,out}}\, - \,{h_{Proc,\,\,in}}} \right)
+\end{equation}
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Latent}} = \,{\mathop Q\limits^ \bullet_{Total}}\, - \,{\mathop Q\limits^ \bullet_{Sensible}}
+\end{equation}
+
+where:
+
+\[{\mathop Q\limits^ \bullet_{Sensible}}\] ~~~~~ = sensible heat transfer rate to the process air stream (W)
+
+\({\mathop Q\limits^ \bullet_{Total}}\) ~~~~~~~~ = total heat transfer rate to the process air stream (W)
+
+\[{\mathop Q\limits^ \bullet_{Latent}}\] ~~~~~~~ = latent heat transfer rate to the process air stream (W)
+
+\({\mathop m\limits^ \bullet_{Proc}}\) ~~~~~~~~ = process air mass flow rate (kg/s)
+
+\(C{p_{Proc,\,\,in}}\) ~~~~ = specific heat of inlet process air (J/kg-K)
+
+\({T_{Proc,\,\,out}}\) ~~~~~ = process air outlet temperature (°C)
+
+\({T_{Proc,\,\,in}}\) ~~~~~~~ = process air inlet temperature (°C)
+
+\({h_{Proc,\,\,out}}\) ~~~~~ = process air outlet enthalpy (J/kg)
+
+\({h_{Proc,\,\,in}}\) ~~~~~~~ = process air inlet enthalpy (J/kg)
+
+To simplify the accounting of heat exchanger performance, the sensible, latent, and total heat transfer rates for the process side of the heat exchanger are stored in cooling and heating report variables. For example, if the sensible heat transfer rate is negative, the absolute value is stored in a ``cooling'' rate report variable. Conversely, if the sensible heat transfer rate is positive, the value is stored in a ``heating'' rate report variable. Similar accounting is performed for the latent and total heat transfer rate variables as follows:
+
+\begin{equation}
+IF\left( {{{\mathop Q\limits^ \bullet  }_{Sensible}} <  = 0} \right){\mathop Q\limits^ \bullet_{SensibleCooling}} = ABS\left( {{{\mathop Q\limits^ \bullet  }_{Sensible}}} \right)
+\end{equation}
+
+\begin{equation}
+IF\left( {{{\mathop Q\limits^ \bullet  }_{Sensible}} > 0} \right){\mathop Q\limits^ \bullet_{SensibleHeating}} = {\mathop Q\limits^ \bullet_{Sensible}}
+\end{equation}
+
+\begin{equation}
+IF\left( {{{\mathop Q\limits^ \bullet  }_{Latent}} <  = 0} \right){\mathop Q\limits^ \bullet_{LatentCooling}} = ABS\left( {{{\mathop Q\limits^ \bullet  }_{Latent}}} \right)
+\end{equation}
+
+\begin{equation}
+IF\left( {{{\mathop Q\limits^ \bullet  }_{Latent}} > 0} \right){\mathop Q\limits^ \bullet_{LatentHeating}} = {\mathop Q\limits^ \bullet_{Latent}}
+\end{equation}
+
+\begin{equation}
+IF\left( {{{\mathop Q\limits^ \bullet  }_{Total}} <  = 0} \right){\mathop Q\limits^ \bullet_{TotalCooling}} = ABS\left( {{{\mathop Q\limits^ \bullet  }_{Total}}} \right)
+\end{equation}
+
+\begin{equation}
+IF\left( {{{\mathop Q\limits^ \bullet  }_{Total}} > 0} \right){\mathop Q\limits^ \bullet_{TotalHeating}} = {\mathop Q\limits^ \bullet_{Total}}
+\end{equation}
+
+At the end of each HVAC simulation time step, this object reports the sensible, latent and total cooling/heating energy and electric consumption for the heat exchanger as follows:
+
+\begin{equation}
+{Q_{SensibleCooling}} = {\dot Q_{SensibleCooling}}*TimeStepSys*3600.
+\end{equation}
+
+\begin{equation}
+{Q_{LatentCooling}} = {\dot Q_{LatentCooling}}*TimeStepSys*3600.
+\end{equation}
+
+\begin{equation}
+{Q_{TotalCooling}} = {\dot Q_{TotalCooling}}*TimeStepSys*3600.
+\end{equation}
+
+\begin{equation}
+{Q_{SensibleHeating}} = {\dot Q_{SensibleHeating}}*TimeStepSys*3600.
+\end{equation}
+
+\begin{equation}
+{Q_{LatentHeating}} = {\dot Q_{LatentHeating}}*TimeStepSys*3600.
+\end{equation}
+
+\begin{equation}
+{Q_{TotalHeating}} = {\dot Q_{TotalHeating}}*TimeStepSys*3600.
+\end{equation}
+
+\begin{equation}
+{E_{HXUnit}} = {P_{HXUnit}}*TimeStepSys*3600.
+\end{equation}
+
+where: \(Q_{SensibleCooling}\) = output variable `Heat Exchanger Sensible Cooling Energy, J'
+
+\({\dot Q_{SensibleCooling}}\) ~~~~~~~~~ = output variable `Heat Exchanger Sensible Cooling Rate, W' = \[{\dot Q_{Sensible}}\]
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ during times when the process air is cooled
+
+\emph{TimeStepSys} ~~~~~~~~~ = HVAC system simulation time step, hr \(Q_{LatentCooling}\) = output variable `Heat Exchanger Latent Cooling Energy, J'
+
+\({\dot Q_{LatentCooling}}\) ~~~~~~~~~~ = output variable `Heat Exchanger Latent Cooling Rate, W' = \({\dot Q_{Latent}}\)
+
+~~ during times when the process air is dehumidified \(Q_{TotalCooling}\) = output variable `Heat Exchanger Total Cooling Energy, J'
+
+\({\dot Q_{TotalCooling}}\) ~~~~~~~~~~~~ = output variable `Heat Exchanger Total Cooling Rate, W' = \({\dot Q_{Total}}\) during
+
+~~~ times when the process air enthalpy is reduced \(Q_{SensibleHeating}\) = output variable `Heat Exchanger Sensible Heating Energy, J'
+
+\({\dot Q_{SensibleHeating}}\) ~~~~~~~~~ = output variable `Heat Exchanger Sensible Heating Rate, W' = \({\dot Q_{Sensible}}\)
+
+~~ during times when the process air is heated \(Q_{LatentHeating}\) = output variable `Heat Exchanger Latent Gain Energy, J'
+
+\({\dot Q_{LatentHeating}}\) ~~~~~~~~~~ = output variable `Heat Exchanger Latent Gain Rate, W' = \({\dot Q_{Latent}}\) ~during times when the process air is humidified \(Q_{TotalHeating}\) = output variable `Heat Exchanger Total Heating Energy, J'
+
+\({\dot Q_{TotalHeating}}\) ~~~~~~~~~~~~ = output variable `Heat Exchanger Total Heating Rate, W' = \({\dot Q_{Total}}\) during times when the process air enthalpy is increased
+
+\({E_{HXUnit}}\) ~~~~~~~~~~~~~~~~~ = output variable `Heat Exchanger Electric Energy, J'
+
+\({P_{HXUnit}}\) ~~~~~~~~~~~~~~~~~~ = output variable `Heat Exchanger Electric Power, W'
+
+\subsubsection{Economizer Operation}\label{economizer-operation-2}
+
+A conventional air-side economizer may be used in conjunction with this heat exchanger object. The air-side economizer is specified through the use of an outside air controller (see object: Controller:OutdoorAir). Specify the appropriate economizer control type, and provide the required control points and air flow rates as defined in the outside air controller object. Energy transfer provided by the heat exchanger will be suspended whenever free cooling is available (i.e., when the air-side economizer is activated) or high humidity control is active and \emph{the user specified economizer lockout input is specified as Yes}. For the desiccant heat exchanger, heat transfer is assumed to be provided by a rotating heat exchanger core. For this reason, air continues to flow through the core when the outdoor air economizer is active but it is assumed that the rotation of the heat exchanger core is stopped. If the economizer lockout is specified as No, the desiccant heat exchanger is operational even when economizer or high humidity mode is active. This specific type of heat exchanger is typically \emph{not} controlled by an outdoor air economizer. For this reason, the default value for economizer lockout is No and must be specifically entered as Yes to enable the economizer or high humidity control lockout feature.
+
+\subsubsection{Desiccant Heat Exchanger Performance Data}\label{desiccant-heat-exchanger-performance-data}
+
+\paragraph{Overview}\label{overview-3-004}
+
+The input object HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 specifies a performance model and model coefficients for a balanced flow desiccant heat exchanger. The HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 object is referenced by a HeatExchanger:Desiccant:BalancedFlow object. This performance data object is used to specify the thermal performance and electric consumption of the heat exchanger. Some representative inputs for this object are provided in the EnergyPlus Reference DataSets (PerfCurves.idf).
+
+This model predicts the regeneration air stream outlet temperature and humidity ratio values based on the entering regeneration and process air stream temperature, humidity ratio and face velocity. The process air stream outlet humidity ratio and temperatures are calculated based on a simple heat and moisture balance. The model requires that the user enter the nominal volumetric flow rate and a nominal face velocity, electric power consumption, empirical model coefficients for the regeneration outlet air temperature and humidity ratio equations, and the applicable minimum and maximum values for both the independent and dependent variables for the empirical model coefficients provided. Refer to the EnergyPlus Input Output Reference for details regarding the input syntax for this object.
+
+\paragraph{Heat Exchanger Face Area and Air Velocity}\label{heat-exchanger-face-area-and-air-velocity}
+
+The user is required to enter a nominal volumetric air flow rate and a nominal face velocity. From these inputs, a heat exchanger face area (applicable for both the regeneration and process sides of the heat exchanger) is calculated and used to determine the operating face velocity during the simulation.
+
+\begin{equation}
+  A_{face} = \frac{V_{face,nom}}{\dot{v}_{face,nom}}
+\end{equation}
+
+\begin{equation}
+  RFV = \frac{\dot{m}_{Reg,in}}{\rho_{std}A_{face}}
+\end{equation}
+
+where:
+
+\({A_{face}}\) ~~~~~~~~~ = heat exchanger face area (m\(^{2}\))
+
+\({V_{face,nom}}\) ~~~~~ = nominal air volume flow rate specified for the heat exchanger (m\(^{3}\)/s)
+
+\({\mathop v\limits^ \bullet_{face,nom}}\) ~~~~~ = nominal air face velocity specified for the heat exchanger (m/s)
+
+\(RFV\) ~~~~~~~~ = face velocity of the regeneration (and process) air stream (m/s)
+
+\({\mathop m\limits^ \bullet_{Reg,in}}\) ~~~~~~ = mass flow rate of the regeneration air stream (kg/s)
+
+\({\rho_{Std}}\) ~~~~~~~~~~ = density of air at standard temperature and pressure {[}dry air at 20°C{]} (m\(^{3}\)/kg)
+
+The face velocity calculated each simulation time step is used in the empirical equations (see `Model Calculations' below) and should be within the minimum and maximum velocity boundaries specified for the model coefficients (see `Empirical Model Boundaries (Minimum and Maximum)` below). When the calculated air velocity exceeds one of the boundaries, a warning is issued and the velocity is reset to the appropriate boundary value before being passed to the empirical equations for calculating regeneration air outlet temperature and humidity ratio. If the user is confident in their empirical model coefficients, the minimum and maximum velocity boundaries may be expanded slightly (caution should be used here) to allow extrapolation of the empirical equations during the simulation.
+
+\paragraph{Model Calculations}\label{model-calculations}
+
+The model coefficients may be obtained by curve fitting field measurements or the results from other computer models that accurately reflect the performance of a balanced flow desiccant heat exchanger. A wide range of data is necessary to properly define the performance of the desiccant heat exchanger such that all operating conditions expected during a simulation are included in the range of data used to obtain the model coefficients. The minimum and maximum boundaries for the independent variables used to generate the empirical model coefficients are used by this model to ensure that model extrapolation does not occur at any point during the simulation. For this reason, it is recommended that the widest possible range of data be used to determine the model coefficients.
+
+The dry-bulb temperature of the regeneration outlet air is determined using the equation shown below.
+
+\begin{equation}
+RTO = B1 + B2*RWI + B3*RTI + B4*\left( {\frac{{RWI}}{{RTI}}} \right) + B5*PWI + B6*PTI + B7*\left( {\frac{{PWI}}{{PTI}}} \right) + B8*RFV
+\end{equation}
+
+where:
+
+\(RTO\) ~ = regeneration outlet air dry-bulb temperature (°C)
+
+\(RWI\) ~ = regeneration inlet air humidity ratio (kg/kg)
+
+\(RTI\) ~ = regeneration inlet air dry-bulb temperature (°C)
+
+\(PWI\) ~ = process inlet air humidity ratio (kg/kg)
+
+\(PTI\) ~ = process inlet air dry-bulb temperature (°C)
+
+\(RFV\) ~ = regeneration (and process) face velocity (m/s)
+
+Similarly, the humidity ratio of the regeneration outlet air is defined using the same empirical equation form; however, different coefficients are used as follows:
+
+\begin{equation}
+RWO = C1 + C2*RWI + C3*RTI + C4*\left( {\frac{{RWI}}{{RTI}}} \right) + C5*PWI + C6*PTI + C7*\left( {\frac{{PWI}}{{PTI}}} \right) + C8*RFV
+\end{equation}
+
+where:
+
+\(RWO\) ~ = regeneration outlet air humidity ratio (kg/kg)
+
+If the regeneration outlet air conditions exceed the saturation curve, RTO and RWO are reset to saturated conditions (100\% RH) at the enthalpy calculated based on the original RTO and RWO values.
+
+Once the regeneration outlet air conditions are determined as described above, the dry-bulb temperature and humidity ratio differences across the regeneration side of the heat exchanger are calculated.
+
+\begin{equation}
+{T_{diff}} = \,RTO - {T_{Reg,\,\,in}}
+\end{equation}
+
+\begin{equation}
+{w_{diff}} = \,RWO - {w_{Reg,\,\,in}}
+\end{equation}
+
+where:
+
+\({T_{Reg,\,\,in}}\) ~~~~~~~~ = actual regeneration inlet air dry-bulb temperature (°C)
+
+\({w_{Reg,\,\,in}}\) ~~~~~~~ = actual regeneration inlet air humidity ratio (kg/kg)
+
+\({T_{diff}}\) ~~~~~~~~~~ = regeneration air temperature difference based on empirical model (°C)
+
+\(wdiff\) ~~~~~~~~~ = regeneration air humidity ratio difference based on empirical model (kg/kg)
+
+The regeneration outlet air conditions described above represent the full load outlet conditions under steady-state operation. However, there are times when the heat exchanger may not operate for the entire simulation time step (i.e., bypass air flow around a fixed-plate heat exchanger or stop the rotation of a rotary heat exchanger for a portion of the time step). For example, the parent object calling this heat exchanger model may request that it only provide heat exchange for a portion of the time step (\emph{HXPartLoadRatio}). Another example would be if this heat exchanger is not called by a parent object but is instead placed directly in a AirLoopHVAC or AirLoopHVAC:OutdoorAirSystem and a setpoint manager is used to place a minimum and/or maximum humidity ratio setpoint on the process air outlet node. For this case the humidity setpoints, if present, are used to calculate a part-load ratio for the heat exchanger assuming the full-load process air humidity ratio difference is equivalent (but opposite in sign) to the regeneration air humidity ratio difference (\emph{w\(_{diff}\)}):
+
+If $w_{diff}>0$, then Regen air humidified, process air dehumidified:
+
+\begin{equation}
+  HXPartLoadRatio = \frac{w_{Proc,in} - w_{max, setpoint}}{w_{diff}}
+\end{equation}
+
+Else, if $w_{diff} <0$, then Regen air dehumidified, process air humidified:
+
+\begin{equation}
+  HXPartLoadRatio = \frac{w_{Proc,in} - w_{min, setpoint}}{w_{diff}}
+\end{equation}
+
+And finally, HXPartLoadRatio is constrained to be within the range 0 to 1.
+
+If this heat exchanger is not being called by a parent object and no humidity setpoints are placed on the process air outlet node, then the model assumes that the heat exchanger operates for the entire simulation time step when it is available to operate (based on its availability schedule) and there is a temperature and/or humidity ratio difference between the two air streams.
+
+EnergyPlus has an established convention for placing information on outlet air nodes. If the air flow rate is continuous but the device only operates for a portion of the simulation time step, then the average outlet conditions (temperature, humidity and enthalpy) are placed on the outlet air node. If the air flow rate cycles on and off during the simulation time step, then the full load outlet conditions are placed on the outlet air node along with the average air mass flow rate for the simulation time step. To account for these cases, this model uses the following logic:
+
+If FanOpMode is equal to CycFanCycComp or if RegAirInletIsOANode is true then:
+
+\begin{equation}
+  \begin{array}{rl}
+    T_{Reg,out} &= T_{Reg,in} + T_{diff} \\
+    w_{Reg,out} &= w_{Reg,in} + w_{diff}
+  \end{array}
+\end{equation}
+
+Otherwise:
+
+\begin{equation}
+  \begin{array}{rl}
+    T_{Reg,out} &= T_{Reg,in} + T_{diff} \cdot HXPartLoadRatio \\
+    w_{Reg,out} &= w_{Reg,in} + w_{diff} \cdot HXPartLoadRatio 
+  \end{array}
+\end{equation}
+
+where:
+
+\({T_{Reg,\,\,out}}\) ~~~~~~ = regeneration outlet air dry-bulb temperature (°C)
+
+\({w_{Reg,\,\,out}}\) ~~~~~ = regeneration outlet air humidity ratio (kg/kg)
+
+\(HXPartLoadRatio\) ~ = heat exchanger part-load ratio (determined by parent object calling this model, or calculated based on a minimum/maximum humidity ratio setpoints as shown above).
+
+In the logic shown above, \emph{RegAirInletIsOANode} is true if the regeneration air inlet node is an outside air node. If so, the model assumes that the air flow through the regeneration side of the heat exchanger cycles on and off as required during the simulation time step. Also, the regeneration outlet air humidity ratio is limited to be between 1E-5 and 1.0.
+
+The regeneration outlet air enthalpy is then calculated using the regeneration outlet air temperature and humidity ratio.
+
+\begin{equation}
+{h_{Reg,\,\,out}} = \,PsyHFnTdbW\left( {{T_{Reg,\,\,out}}\,,\,\,{w_{Reg,\,\,out}}} \right)
+\end{equation}
+
+Using the regeneration outlet air conditions, the heat transfer on the regeneration side of the heat exchanger is then calculated:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Sensible,Reg}} = \,{\mathop m\limits^ \bullet_{Reg}}C{p_{Reg,\,\,in}}\left( {{T_{Reg,\,\,out}}\, - \,{T_{Reg,\,\,in}}} \right)
+\end{equation}
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{Total,Reg}} = \,{\mathop m\limits^ \bullet_{Reg}}\left( {{h_{Reg,\,\,out}}\, - \,{h_{Reg,\,\,in}}} \right)
+\end{equation}
+
+where:
+
+\({\mathop Q\limits^ \bullet_{Sensible,Reg}}\) ~ = sensible heat transfer rate to the regeneration air stream (W)
+
+\({\mathop Q\limits^ \bullet_{Total,Reg}}\) ~~~~ = total heat transfer rate to the regeneration air stream (W)
+
+\({\mathop m\limits^ \bullet_{Reg}}\) ~~~~~~~~~ = regeneration air mass flow rate (kg/s)
+
+\(C{p_{Reg,\,\,in}}\) ~~~~~ = specific heat of inlet regeneration air (J/kg-K)
+
+Since the model assumes that total and sensible heat transfer is conserved, these heat transfer rates are then used to calculate the process air outlet conditions:
+
+\begin{equation}
+{h_{Proc, out}} = \,{h_{Proc,in}} - \left( {\frac{{{{\mathop Q\limits^ \bullet  }_{Total,Reg}}}}{{{{\mathop m\limits^ \bullet  }_{Proc}}}}} \right)
+\end{equation}
+
+\begin{equation}
+{T_{Proc, out}} = \,{T_{Proc,in}} - \left( {\frac{{{{\mathop Q\limits^ \bullet  }_{Sensible,Reg}}}}{{{{\mathop m\limits^ \bullet  }_{Proc}}C{p_{Proc,in}}}}} \right)
+\end{equation}
+
+\begin{equation}
+{w_{Proc,\,\,out}} = \,PsyWFnTdbH\left( {{T_{Proc,\,\,out}}\,,\,\,{h_{Proc,\,\,out}}} \right)
+\end{equation}
+
+where:
+
+\({h_{Proc,\,\,out}}\) ~~~~~ = process outlet air enthalpy (J/kg)
+
+\({T_{Proc,\,\,out}}\) ~~~~~ = process outlet air dry-bulb temperature (°C)
+
+\({w_{Proc,\,\,out}}\) ~~~~~ = process outlet air humidity ratio (kg/kg)
+
+\({\dot m_{Proc}}\) ~~~~~~~~ = process air mass flow rate (kg/s)
+
+\(C{p_{Proc,in}}\) ~~~~ = specific heat of inlet process air (J/kg-K)
+
+Like the regeneration outlet air conditions, the process outlet air conditions are also checked for exceeding saturated conditions and, if detected, the temperature and humidity ratio are reset assuming constant enthalpy.
+
+\begin{equation}
+  T_{sat} = PsyTsatFnHPb \PB{h_{Proc,out},PB}
+\end{equation}
+
+If $T_{sat}>T_{Proc,out}$, then:
+
+\begin{equation}
+  \begin{array}{rl}
+    T_{Proc,out} &= T_{sat} \\
+    w_{Proc,out} &= PsyWFnTdbH \PB{T_{Proc,out},h_{Proc,out}}
+  \end{array}
+\end{equation}  
+
+Heat recovery electric power is the electric consumption rate of the unit in watts. The nominal electric power for the heat exchanger is specified in the input data file, and can be used to model controls (transformers, relays, etc.) and/or a motor for a rotary heat exchanger. The model assumes that this electric power is consumed whenever the heat exchanger operates. The electric power is assumed to be zero for all other times. None of this electric power is assumed to contribute thermal load to either of the heat exchanger air streams. As with the thermal performance of the heat exchanger, the power used by the heat exchanger is also proportional to the heat exchanger part load ratio.
+
+\begin{equation}
+{P_{HXUnit}}\, = \,{P_{HX,\,nom}}\left( {HXPartLoadRatio} \right)
+\end{equation}
+
+where:
+
+\({P_{HXUnit}}\) ~~~~~~ = output variable `Heat Exchanger Electric Power, W' reported by the HeatExchanger:Desiccant:BalancedFlow object.
+
+\({P_{HX,\,nom}}\) ~~~~~~ = user specified `Nominal Electric Power, W'
+
+\paragraph{Empirical Model Boundaries (Minimum and Maximum)}\label{empirical-model-boundaries-minimum-and-maximum}
+
+Since this model uses empirical equations and extrapolation can cause unexpected results, the entering air conditions to both the regeneration and process sides of the heat exchanger are checked during each simulation time step to make sure they are within the valid range defined by the user. If any of the independent variables used in the equations for RTO and RWO above are outside the minimum and maximum limits specified for each independent variable, the values for these specific independent variables are limited to the appropriate boundary (min/max) value for use by the empirical equations and a warning is issued.
+
+Additional model checks occur by testing the regeneration and process inlet air relative humidities. In this case, the process and regeneration inlet air relative humidities are calculated and compared to the minimum/maximum values specified by the user. If the calculated relative humidity exceeds the specified range at any point during the simulation when the heat exchanger is operating, a warning message is issued but the simulation proceeds.
+
+If the user is confident in their empirical model coefficients, the minimum and maximum independent variable boundaries may be expanded (caution should be used here) to allow extrapolation of the empirical equations during the simulation.
+
+In addition to checking the inlet air conditions, the model allows the user to specify limits for the regeneration air outlet conditions (RTO and RWO). If the calculated value for RTO or RWO exceeds the minimum/maximum limits specified by the user, then the calculated value is reset to the appropriate boundary (min/max) value and a warning message is issued.
+
+This model also assumes that the performance of the desiccant heat exchanger (i.e., the output of the empirical equations) conforms to the following two guidelines.
+
+1.~~~~The regeneration outlet air temperature (RTO) is always less than or equal to the regeneration inlet air temperature (\emph{T\(_{RegIn}\)})
+
+2.~~~~The regeneration outlet air humidity ratio (RWO) is always greater than or equal to the regeneration inlet air humidity ratio (\emph{w\(_{RegIn}\)})
+
+When the calculated regeneration outlet air conditions do not follow these guidelines, a warning is issued and the simulation proceeds.
+
+\subsection{Plant Loop Deep-Ground-To-Water Vertical U-Tube Field Heat Exchanger}\label{plant-loop-deep-ground-to-water-vertical-u-tube-field-heat-exchanger}
+
+This model (Object: GroundHeatExchanger:Vertical) documentation is derived from the M.S. thesis of Arunachalam Murugappan, which is available on the Oklahoma State University web site \url{http://www.hvac.okstate.edu/}.~ Eskilson (1987) Yavuzturk and Spitler (1999) developed the long and short time response factors respectively, which are used in determining the borehole temperature responses. Response factors are infinite series of numbers, which relate the current value of a variable to past values of other variables at discrete time intervals.~ These response factors are referred as \emph{g}-functions. The variable time-step model presented here uses both long time-step \emph{g}-functions and short time-step \emph{g}-functions to predict the boreholes response to short term fluctuations in the load.
+
+\subsubsection{Long Time-Step Response Factors}\label{long-time-step-response-factors}
+
+Eskilson developed \emph{g}-functions for various borehole configurations. He plotted the g function curves for different sets of borehole spacing to borehole length ratio \(B/H\) ~typically for .05, 0.1, 0.15, 0.2, 0.3 and ∞ (∞ represents the single borehole configuration. All the plots were for the ratio of 0.0005 between the borehole radius and the borehole length \({r_b}/H\) . For any other radius a simple relation between the two radii as given by Eskilson (1987) can be used. Eskilson gives the \emph{g}-function curves for 38 different configurations.
+
+Figure~\ref{fig:short-time-step-g-function-curve-as-an} shows the \emph{g}-function plotted against the non-dimensional time defined as \(\ln (t/{t_s})\) , \({t_s} = {H^2}/9\alpha\) ~for various configurations of vertical boreholes with \emph{B/H} ratio of .1 along with single borehole. It is seen from this figure that the thermal interaction between boreholes increases with time and with the number of boreholes in field.
+
+\begin{figure}[hbtp] % fig 253
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5651.png}
+\caption{Short Time Step g Function Curve as an Extension of Long Time Step g Function Curves for Different Configuration of Boreholes (Eskilson 1987, Yavuzturk 1999). \protect \label{fig:short-time-step-g-function-curve-as-an}}
+\end{figure}
+
+The \emph{g}-functions developed by Eskilson are valid only after time estimated by Eskilson as \(5r_b^2/\alpha\) . This time varies from 3-6 hours for a typical borehole field. This is because the analytical line source model, based on which the Eskilson's model was developed, does not give a prompt increase in borehole wall temperature at \(r = {r_b}\) . It gives acceptable results only after the non-dimensional times of \(\alpha t/r_b^2 > 5\) . But to model short time responses of a borehole we need response factors, which can give accurate results down to minutes.
+
+\subsubsection{Short Time-Step Response Factors}\label{short-time-step-response-factors}
+
+Yavuzturk and Spitler (1999) developed short time step response factors using a transient, two-dimensional, implicit finite volume model on a polar grid.
+
+The circular u-tube pipe in the ground loop heat exchanger was approximated as a pie sector of equivalent perimeter.~ A constant heat flux for the heat transfer form/to U-tube, a zero heat flux in the angular direction and a constant far field temperature in the radial axis makes up the three boundary condition and undisturbed far field temperature as the initial condition. The numerical model accounts for the thermal resistance due to individual borehole elements; such as resistance of the pipe and grout material and the convection resistance due to the heat transfer fluid in the pipes. The long time step \emph{g}-functions discussed in the previous section do not account for such effects.
+
+The short time-step \emph{g}-functions are the same for different borehole configurations. This is because there is no thermal interaction between the boreholes for times less than 200 hrs during which the short time-step \emph{g}-functions apply. So it is suggested to use the short time-step \emph{g} function for time steps in the range of 2.5 min and 200 hours and the long time-step \emph{g}-functions for time steps longer than 200 hours. The \emph{g} function for any time can be found by linear interpolation between the bounding known values.
+
+\subsubsection{Development of the Variable Short Time Step Model}\label{development-of-the-variable-short-time-step-model}
+
+The variable time step model was developed as an extension of the model presented by Yavuzturk and Spitler (1999). The variable, short time step model uses a similar algorithm and extends it to accommodate sub-hourly responses, variable time steps and explicit equations to calculate the outlet fluid temperature of the ground loop heat exchanger.
+
+The uniform time-steps model developed by Yavuzturk and Spitler (1999) is able to pre-calculate all the g-functions at the beginning of the simulation. The variable time-step model on the other hand must calculate the \emph{g}-functions when the borehole response calculation for each time step is carried out. For every time step a different set of \emph{g}-functions is needed in the variable time step model as the time at which the \emph{g}-function is to be applied for the past loads changes for each time-steps.
+
+This is made clear from the illustration in Figure~\ref{fig:variable-timestep-ground-loop-heat-exchanger}, which shows a simulation in progress. The boxes with numbers represent the sub-hourly loads. The time (in hrs) at which these loads occurred are shown by solid arrows above the respective load boxes. The right-most solid arrow gives the current simulation time, which is 3.31 hrs. The times given below the boxes, pointed by dashed arrows, are the time at which the \emph{g}-functions are to be estimated and applied to the respective sub hourly loads (boxes) for the current time.
+
+For example, let us take the sub hourly loads 1,2 \& 3. These loads occurred at 0 hrs, 0.16 hrs \& 0.28 hrs. The response of the borehole temperature for the current time step is calculated by applying the \emph{g­-}functions at 3.15 hrs, 3.03 hrs \& 2.5 hrs respectively. Thus to calculate the present borehole temperature, the sub hourly loads 1-12 are superposed using the corresponding \emph{g} functions at times given by the dashed lines.~ This gives the borehole temperature at hr 3.31. However, for the previous time step, which occurred at 3.15 hrs, the g-functions for the loads 1, 2 \& 3 are at 2.99 hrs 2.87 hrs and 2.42 hrs, and the over all response is obtained by superposing the loads 1-11.
+
+Thus for each time step since the time step increments are not uniform we need to store the simulation times at which these time-steps occurred, and calculate corresponding \emph{g}-functions at each time-step.
+
+\begin{figure}[hbtp] % fig 254
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5655.png}
+\caption{Variable Timestep Ground Loop Heat Exchanger Model Schematic Explaining the \emph{g} Function Estimation. \protect \label{fig:variable-timestep-ground-loop-heat-exchanger}}
+\end{figure}
+
+Yavuzturk model calculates the outlet fluid temperature by iteration beginning with the undisturbed mean temperature of the surrounding ground as an initial guess. This aggravates the time taken by an already computationally intensive algorithm. To circumvent this a set of explicit equations were formulated to estimate the outlet fluid temperature.
+
+\subsubsection{Description of the Load Aggregation Scheme}\label{description-of-the-load-aggregation-scheme}
+
+A load aggregation scheme was developed for energy simulation software with variable short time steps down to one minute. A major issue in the development was the calculation of the \emph{g}-functions.~ As discussed previously in the variable time step environments, the time step increments are not uniform. As a result, g-functions cannot e pre-calculated. Figure~\ref{fig:schematic-of-variable-time-step-model-g} shows a schematic of the variable time step ground loop heat exchanger model. The figure shows the larger monthly block loads, hourly loads and sub hourly loads and along with the time of occurrence of those loads. The figure also shows the time at which the \emph{g}-functions are applied to different load blocks.
+
+\begin{figure}[hbtp] % fig 255
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5656.png}
+\caption{Schematic of Variable Time Step Model \emph{g} Function Calculation. \protect \label{fig:schematic-of-variable-time-step-model-g}}
+\end{figure}
+
+To calculate the response of a past load on the borehole temperature we apply the \emph{g}-function corresponding to the time elapsed since the load was applied. This is easily understood form the schematic. For example, to calculate the response of the aggregated load 1'' (at the end of 730hrs.) for the current time step (2193.733hrs) we apply a \emph{g}-function at 1463.73hrs. The \emph{g}-function for the same block 1'' at the previous time step, which occurred at 2193.25 hrs, would be at 1463.25hrs. From the schematic it is also seen that for the other two aggregated monthly loads 2'', 3'' the \emph{g}-function are applied at 733.73 hrs and 3.73 hrs for the current time-step and at 733.25 hrs and 3.25 hrs respectively for the previous time-step. The same scheme applies to hourly and sub-hourly. Thus to estimate the time at which the past monthly, hourly or sub-hourly loads occur, we might be tempted to store the simulation times at each time step for the entire simulation, storing load times for the whole length of simulation for a multi year simulation with a variable short time step would require a large amount of memory. But little consideration shows that it is not necessary.~ Since the monthly and hourly loads occur at equal intervals of time 730hrs and 1hr respectively, the \emph{g}-functions can be estimated with the current simulation time and the time at which the load block ends, which is a multiple of the monthly duration of the block size. Only the sub-hourly loads require storage of simulation times.
+
+For example from the schematic (Figure~\ref{fig:schematic-showing-the-calculation-of-hourly}), for the sub hourly load 1, which occurred at the end of 2193.25 a \emph{g}-function at .48 hrs has to be applied and for the next load 2 a \emph{g}-function at 0.34 hrs has to be applied. Since the time intervals are not even for the sub hourly loads, we need to store the time steps at which those loads occurred. These times are required to estimate the time elapsed between the current simulation time and the time at which the sub hourly loads occurred.
+
+Thus, the algorithm keeps track of the sub hourly loads along with their time of occurrence for a user-defined length of time during which the sub hourly calculations are made. The algorithm also estimates the time weighted hourly load from their corresponding sub hourly loads as each hour passes. The sub-hourly loads are time weighted because of the irregular intervals at which the time-step occurs. This is also illustrated in Figure~\ref{fig:schematic-showing-the-calculation-of-hourly}. The sub hourly loads 1,2 \&3 occur for varying length of time. The load 3 occurs for a longer duration than 1 and 2 in that order. This implies that the load 3 has to be given more weight than 1 and 2. So the sub hourly loads for a particular hour are multiplied by the length of their respective period of occurrence and averaged over the hour. This is further explained by the schematic in Figure~\ref{fig:simplified-single-zone-draw-through-air}.
+
+\begin{figure}[hbtp] % fig 256
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5657.png}
+\caption{Schematic Showing the Calculation of Hourly Load from the Sub Houly Loads. \protect \label{fig:schematic-showing-the-calculation-of-hourly}}
+\end{figure}
+
+The bottom text in the boxes represents the magnitude of the sub hourly loads in W/m for each time step. The duration of the occurrence of each time-step for the each block is shown below the respective block. The first hourly load is given by the expression
+
+\begin{equation}
+{\overline q_1} = \left[ \begin{array}{l}\left( {8.36 \times .159} \right) + \left( {6.51 \times .339} \right) + \left( {10.3 \times .107} \right)\\ + \left( {6.92 \times .162} \right) + \left( {9.03 \times .181} \right) + \left( {12 \times .05} \right)\end{array} \right] = 7.993W/m
+\end{equation}
+
+Where \({\overline q_1}\) ~ = the first hourly load in W/m
+
+The algorithm keeps track of enough of these past hourly loads to calculate the monthly load. As each month or user defined time passes, hourly loads over the entire month or user defined time ``blocks'' are averaged and stored in arrays for the respective monthly user defined block of time.
+
+The borehole temperature for any time step is computed by superposing the monthly (larger time block loads) hourly and sub-hourly loads for each time step. To understand more clearly consider the schematic in Figure~\ref{fig:schematic-showing-the-calculation-of-hourly} where the borehole temperature at 2193.733 hour is to be estimated. Here the monthly block time is 730 hrs. We have three monthly aggregated load blocks for 730 hrs, 1460 hrs and 2190 hrs and hourly loads from 2191\(^{st}\) hr to 2193\(^{rd}\) hour. For the remaining 0.733 hours a sub hourly calculation is done. The three monthly aggregated load blocks when superposed using long time \emph{g-}functions, yields the borehole temperature at the end of 2190\(^{th}\) hour. Then the hourly loads from 2191\(^{st}\) to 2193\(^{rd}\) hrs are superposed using the corresponding short time step \emph{g} functions values yielding the borehole temperature at the end of 2193\(^{rd}\) hour. The sub-hourly variations for the current hour are obtained, by superposing the sub-hourly loads. From the schematic, we see there are two sub-hourly loads, 1 and 2. Thus the borehole temperature at the end of 2193.733 is expressed as:
+
+\begin{equation}
+{T_{2193.733}} = {T_{ground}} + \sum\limits_{m = 1}^3 {\left[ {\frac{{{{\overline{\overline q} }_m} - {{\overline{\overline q} }_{m - 1}}}}{{2\pi {k_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_{730(m - 1)}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+\begin{equation}
++ \sum\limits_{n = 2190}^{2193} {\left[ {\frac{{{{\overline q }_n} - {{\overline q }_{n - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_{n - 1}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+\begin{equation}
++ \sum\limits_{p = 2193}^{2193.733} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+Where
+
+\(\overline{\overline q}\) ~ = The average monthly loads
+
+\(\overline q\) ~ = The average hourly loads
+
+\emph{Q} = the sub-hourly loads
+
+\emph{m} = index for monthly aggregated blocks
+
+\emph{p} = array index for sub hourly loads
+
+\emph{t} = time
+
+t\(_{p}\) ~ = ~ the sub hourly time steps over the history period. (here increment is not always unity)
+
+Superposing the temperature responses of monthly (larger) blocks over the shorter, namely the hourly and sub hourly, introduces some error in the borehole temperature calculation at the beginning of every month. Yavuzturk and Spitler suggest a method to reduce the error in borehole temperature prediction by using a minimum hourly history period during which only the short time step superposition is carried out. In our model this idea is extended to sub hourly loads as well. Thus a user specified minimum sub-hourly history period is included along with the minimum hourly history period to model the sub-hourly variations. During this period only sub-hourly and hourly superpositions are made. This guarantees that at any given time step the superposition of temperature responses involves a minimum period of short time responses, which ensures a better estimation of borehole temperature. For example, a minimum hourly history period of 96 hrs and a minimum sub hourly history period of 5 hours would result in only 2 monthly aggregation blocks (1'' and 2''). The last monthly aggregation does not occur because neither of the minimum hourly history period of 96 hours or sub-hourly history period of five hrs is met. So an hourly superposition of the load is carried out for the third month until the minimum sub-hourly history period after which sub hourly superposition is carried out. The equation becomes
+
+\begin{equation}
+{T_{2193.733}} = {T_{ground}} + \sum\limits_{m = 1}^2 {\left[ {\frac{{{{\overline{\overline q} }_m} - {{\overline{\overline q} }_{m - 1}}}}{{2\pi {k_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_{730(m - 1)}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+\begin{equation}
++ \sum\limits_{n = 1460}^{2188} {\left[ {\frac{{{{\overline q }_n} - {{\overline q }_{n - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_{n - 1}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+\begin{equation}
++ \sum\limits_{p = 2188}^{2193.733} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+Yavuzturk and Spitler have done a detailed analysis on the effect of minimum hourly history period. They found that a minimum hourly history period of 192 hrs for an annual simulation would reduce the running time by 90\%.~ They also found that for a 20year simulation, the computation time of the aggregated load scheme is just 1\% of the non-aggregated load scheme.
+
+\subsubsection{Summary of Variable Short Time Step Response Factor Model}\label{summary-of-variable-short-time-step-response-factor-model}
+
+The load aggregation scheme developed in line with the above example is summarized eight steps as follows:
+
+1.~~~~Define monthly load blocks duration (mb) in hrs (generally 730 hrs) and the minimum hourly history period and minimum sub hourly history period.
+
+2.~~~~Read Borehole Geometry Parameters: number of boreholes, borehole length radius thickness of the pipe etc. Read Ground and Fluid thermal properties: Ground conductivity, volumetric specific heat capacity of the ground and heat carrier fluid. Read the short and long time-step \emph{g-}functions into arrays with their respective non-dimensionalized times.
+
+3.~~~~Start Simulation from p = 1 to nts. Here ``nts'' is the number of time steps that have occurred since the start of simulation. (Note that P in not a count of number of hour elapsed in the simulation)
+
+4.~~~~Compute the hourly loads as each hour passes. This is done by averaging the sub hourly loads during the past hour. The monthly loads are calculated by averaging the hourly loads during that month. This is done by summing the hourly loads during that monthly period and dividing the sum by 730 hours NumMonths(the number of months used in aggregation calculations) is set to the number of months of simulation (current number of aggregated load blocks)
+
+5.~~~~If the simulation time is less than the minimum sub hourly history period the borehole temperature is estimated with no aggregation. Only sub hourly loads are superposed as given by the following equation.
+
+\begin{equation}
+{T_{nts}} = {T_{ground}} + \sum\limits_{p = 1}^{nts} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+6.~~~~. If the simulation time is less than sum of minimum hourly history and sub hourly history periods, then decomposed hourly aggregated loads are superposed using their corresponding g function until the sub hourly history required. Then the sub hourly temperature differences are found by superposing the decomposed sub hourly loads with their short time step \emph{g} functions. Average borehole temperature is found by superposing the hourly and sub hourly temperature differences with the following equation
+
+\begin{equation}
+{T_{nts}} = \sum\limits_{n = 1}^{nh - sh} {\left[ {\frac{{{{\overline q }_n} - {{\overline q }_{n - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_{n - 1}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}  + \sum\limits_{p = nts - sh}^{nts} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+7.~~~~If the simulation time is greater then the sum of a monthly period, sub hourly history and the hourly history period. Then monthly load aggregation is performed. Here if the difference between the simulation time and product of a monthly block period and the current number of monthly blocks is greater than the sum of the minimum hourly history and sub hourly history periods then the average borehole temperature is found by the following equation.
+
+\begin{equation}
+{T_{nts}} = {T_{ground}} + \sum\limits_{m = 1}^{calb} {\left[ {\frac{{{{\overline{\overline q} }_m} - {{\overline{\overline q} }_{m - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_{mb[m - 1]}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+\begin{equation}
++ \sum\limits_{n = nh - [calb(mb) + sh]}^{nh - sh} {\left[ {\frac{{{{\overline q }_n} - {{\overline q }_{n - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_{n - 1}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+\textbf{\(+ \sum\limits_{p = nts - sh}^{nts} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~}
+
+8.~~~~If the difference between the simulation time and product of a monthly block period and the current number of monthly blocks is less than the sum of the minimum hourly history and sub hourly history periods, then NumMonths is set to one month less than the actual number of months of simulation completed. The average borehole temperature is calculated by superposing the long and time step temperature differences using the following equation.
+
+\begin{equation}
+{T_{nts}} = {T_{ground}} + \sum\limits_{m = 1}^{calb - 1} {\left[ {\frac{{{{\overline{\overline q} }_m} - {{\overline{\overline q} }_{m - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_{mb[m - 1]}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+\begin{equation}
++ \sum\limits_{n = nh - [(calb - 1)(mb) + sh]}^{nh - sh} {\left[ {\frac{{{{\overline q }_n} - {{\overline q }_{n - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_{n - 1}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}
+\end{equation}
+
+\textbf{\(+ \sum\limits_{p = nts - sh}^{nts} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~}
+
+Define Monthly block duration, minimum hourly history period and minimum sub hourly history period (step 1)
+
+Read Borehole Geometry parameters, Ground and carrier fluid properties and read short and long time-step \emph{g} functions. (Step 2)
+
+\textbf{~}
+
+\textbf{Do until} p = 1 to number of time-steps (nts) (Step 3)
+
+Compute the Ground Load for the current time step using Entering Fluid temperature (For the first time-step \emph{T}\(_{FarField}\) may be used)
+
+Compute the hourly loads as each hour and monthly loads as each month passes. Calculate the number of monthly blocks (NumMonths)(\textbf{Step 4})
+
+\textbf{If} (Current time less than minimum sub hourly history) (\textbf{Step 5})
+
+\textbf{~~~} use Equation
+
+\textbf{Else If} (Current Simulation Time less than sum of minimum hourly history and minimum sub hourly history) (\textbf{step 6})
+
+~~~ use Equation
+
+~~~ \textbf{Else}
+
+\textbf{If} (Difference between current simulation~~~ time and duration of the total number months is Greater than sum of minimum hourly and sub hourly histories) (\textbf{step 7})
+
+~~~ use Equation
+
+~~~~~~~~~~ \textbf{Else} (\textbf{step 8})
+
+~~~~~~~~~~~~~~~~~ use Equation
+
+~~~ ~~~~~~ \textbf{End if}
+
+~~~ \textbf{End if}
+
+\textbf{End do}
+
+\subsubsection{References}\label{references-2-006}
+
+Eskilson, P. 1987. Thermal Analysis of Heat Extraction Boreholes. Ph.D.~Thesis, Department of Mathematical Physics, University of Lund, Lund, Sweden.
+
+Yavuzturk, C. 1999. Modeling of Vertical Ground Loop Heat Exchangers for Ground Source Heat Pump Systems. Ph.D.~Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University, Stillwater, Oklahoma.
+
+Yavuzturk, C., J.D. Spitler. 1999.\href{http://www.hvac.okstate.edu/research/Documents/ASHRAE/Yavuzturk_Spitler_99.pdf}{A Short Time Step Response Factor Model for Vertical Ground Loop Heat Exchangers.} \emph{ASHRAE Transactions}. 105(2):475-485.
+
+\subsection{GroundHeatExchanger:Slinky}\label{groundheatexchangerslinky}
+
+This model reuses much of the same code including the load aggregation and temperature response caluclations which are described above in the GroundHeatExchanger:Vertical model. As a result, that section can also be used as reference material. This model is unique in that it generates it's own temperature response factor g-functions, rather than relying on the other software or data to generate the g-functions. These are generated based on the work by Xiong et al. 2015.
+
+\subsubsection{Horizontal Slinky Temperature Response Functions}\label{horizontal-slinky-temperature-response-functions}
+
+Equation used for calculating the g-function temperature response factors for the horizontal Slinky HX are seen below.
+
+{\scriptsize
+\begin{equation}
+g_s\left(t\right) = \sum_{i = 1}^{N_{ring}} \sum_{j = 1}^{N_{ring}} \frac{R}{4\pi N_{ring}} \int_0^{2\pi} \int_0^{2\pi} 
+            \left[ 
+                \frac{erfc\left(d\left(P_j,P_i\right)/2\sqrt{\alpha t}\right)}{d\left(P_j,P_i\right)} - 
+                \frac{erfc\left(\sqrt{d\left(P_j,P_i\right)^2+4h^2/\left(2\sqrt{\alpha t}\right)}\right)}{\sqrt{d\left(P_j,P_i\right)^2+4h^2} }
+            \right]d\omega d\varphi
+\end{equation}}
+
+Where:
+
+\begin{equation}
+d\left(P_j,P_i\right) = \frac{d\left(P_{ii},P_j\right) + d\left(P_{io},P_j\right)}{2}
+\end{equation}
+
+\begin{equation}
+d\left(P_{ii},P_j\right) = \sqrt{\left[x_{0i} + \left(R-r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i} + \left(R-r\right)\sin \varphi - y_{0j}-R\sin \omega\right]^2}
+\end{equation}
+
+\begin{equation}
+d\left(P_{io},P_j\right) = \sqrt{\left[x_{0i} + \left(R-r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i} + \left(R+r\right)\sin \varphi - y_{0j}-R\sin \omega\right]^2}
+\end{equation}
+
+\subsubsection{Vertical Slinky Temperature Response Functions}\label{vertical-slinky-temperature-response-functions}
+
+Equations used for calculating the g-function temperature response factors for the vertical Slinky HX are seen below.
+
+\begin{equation}
+g_s\left(t\right) = \sum_{i = 1}^{N_{ring}} \sum_{j = 1}^{N_{ring}} \frac{R}{4\pi N_{ring}} \int_0^{2\pi} \int_0^{2\pi} 
+            \left[ 
+                \frac{erfc\left(d\left(P_j,P_i\right)/2\sqrt{\alpha t}\right)}{d\left(P_j,P_i\right)} - 
+                \frac{erfc\left(d\left(P_{j'},P_i\right)/2\sqrt{\alpha t}\right)}{d\left(P_{j'},P_i\right)}
+            \right]d\omega d\varphi
+\end{equation}
+
+Where:
+
+\begin{equation}
+d\left(P_j,P_i\right) = \frac{d\left(P_{ii},P_j\right) + d\left(P_{io},P_j\right)}{2}
+\end{equation}
+
+\begin{equation}
+d\left(P_{j'},P_i\right) = \frac{d\left(P_{ii},P_{j'}\right) + d\left(P_{io},P_{j'}\right)}{2}
+\end{equation}
+
+{\scriptsize
+\begin{equation}
+d\left(P_{ii},P_j\right) = \sqrt{\left[x_{0i} + \left(R-r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i}-y_{0j}\right]^2 + \left[z_{0i} + \left(R-r\right)\sin \varphi - z_{0j}-R\sin \omega\right]^2}
+\end{equation}}
+
+{\scriptsize
+\begin{equation}
+d\left(P_{io},P_j\right) = \sqrt{\left[x_{0i} + \left(R+r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i}-y_{0j}\right]^2 + \left[z_{0i} + \left(R+r\right)\sin \varphi - z_{0j}-R\sin \omega\right]^2}
+\end{equation}}
+
+{\scriptsize
+\begin{equation}
+d\left(P_{ii},P_{j'}\right) = \sqrt{\left[x_{0i} + \left(R-r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i}-y_{0j}\right]^2 + \left[z_{0i} + \left(R-r\right)\sin \varphi - z_{0j} - 2h - R\sin \omega\right]^2}
+\end{equation}}
+
+{\scriptsize
+\begin{equation}
+d\left(P_{io},P_{j'}\right) = \sqrt{\left[x_{0i} + \left(R+r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i}-y_{0j}\right]^2 + \left[z_{0i} + \left(R+r\right)\sin \varphi - z_{0j} - 2h - R\sin \omega\right]^2}
+\end{equation}}
+
+\subsubsection{Model Simplifications for Computational Efficiency}\label{model-simplifications-for-computational-efficiency}
+
+Several simplifications were used to ensure the g-function temperature response factors are computationally efficient. The first simplification is achieved by taking advantage of symmetry. In the \protect\hyperlink{SlinkyGHX1}{Figure} below we can see that by taking advantage of symmettry the temperature response for only one quarter of the rings needs be calculated.
+
+The second simplification occurs by realizing that the effect between two rings decreases exponentially as the distance between the rings increases. Near-field rings are defined as rings whose centers are within 2.5m + D distance from the center of ring i as is seen in \protect\hyperlink{SlinkyGHX1}{Figure}. Far-field rings are defined as rings whose centers are beyond 10m + D, with middle-field rings occupying the space in between the near-field and far-field rings. Near-field ring temperature response factors are determined as indicated above for horzontal or vertical slinkys. Middle-field rings are considerably simplified -- the interaction between ring is approximated as that of two point sources at their centers. Thermal effect of far-field rings are ignored.
+
+The third and final simplification takes advantatge of geometric similarity that ring share. Ring pairs that are geometrically similar do not require recalculation of distances or reponse factors. Thus the calculations for geometrically similar ring pairs can be reused.
+
+For more information, see \protect\hyperlink{SlinkyReferenceXiong}{Xiong et al. 2015}.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image8001.png}
+\caption{}
+\end{figure}
+
+Figure: Schematic of first and second improvements to the algorithm for computational efficiency.
+
+\subsubsection{References}\label{references-3-003}
+
+Xiong, Z., D.E. Fisher, and J.D. Spitler. 2015. Development and Validation of a Slinky(TM) Ground Heat Exchanger Model. Applied Energy 141: 57-69.
+
+\subsection{Plant Loop Pond-To-Water Heat Exchanger}\label{plant-loop-pond-to-water-heat-exchanger}
+
+The pond model (Object: GroundHeatExchanger:Pond) is a `lumped parameter' model where the pond is represented by a single node with thermal mass. The pond surface temperature is the same as the temperature at this node, i.e.~the surface temperature is the same as the bulk temperature. A first order differential equation is solved in the model to calculate the pond temperature at each time step. This type of heat rejecter is modeled as several circuits connected in parallel.
+
+\begin{figure}[hbtp] % fig 257
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5676.png}
+\caption{Heat Transfer Mechanisms in a Pond (Chiasson 1999) \protect \label{fig:heat-transfer-mechanisms-in-a-pond-chiasson}}
+\end{figure}
+
+Rees(2002) implemented the model developed by Chiasson(1999) for the shallow ponds. The model is based on the assumption that thermal gradients in shallow ponds are negligible, especially during times of heat rejection. Using the lumped parameter approach, an overall energy balance for the pond may be devised as
+
+\begin{equation}
+q{}_{in} - q{}_{out} = V\rho C{}_p\frac{{dT}}{{dt}}
+\end{equation}
+
+Where
+
+\(q{}_{in}\) ~~ = ~~ Heat transfer to the pond
+
+\(q{}_{out}\) ~ = ~~ Heat transfer from the pond
+
+\(V\) ~~~~ = ~~ Pond Volume
+
+\(\rho\) ~~~~ = ~~ Density of pond water
+
+\({q_{in}}\) ~ = Heat transfer to the pond
+
+\(C{}_p\) ~ = Specific heat capacity of pond water
+
+\(\frac{{dT}}{{dt}}\) ~ = rate of change of temperature of the pond water
+
+Rate of change in average pond temperature is given as
+
+\begin{equation}
+\frac{{dT}}{{dt}} = \frac{{q{}_{solar} + q{}_{thermal} + q{}_{convection} + q{}_{groundwater} + q{}_{evaporation} + q{}_{fluid}}}{{V\rho C{}_p}}
+\end{equation}
+
+Where
+
+q\(_{solar}\) = Solar radiation heat gain to the pond
+
+q\(_{thermal}\) = Thermal radiation heat transfer at the pond surface.
+
+q\(_{convection}\) = Convection heat transfer at the pond surface
+
+q\(_{ground}\) = Heat transfer to/from ground to the pond
+
+q\(_{groundwater}\) = Heat transfer due to ground water inflow/outflow
+
+q\(_{evaporation}\) = Heat transfer due to evaporation at the pond surface
+
+q\(_{fluid}\) = Total heat transfer to/from the heat exchanging fluid flowing in all spools or~ coils in the pond
+
+A heat balance is calculated at a single node that represents the pond. Heat transfer takes place by surface convection, long-wave radiation to the sky, absorption of solar energy, ground heat transfer and heat exchange with the fluid. A heat exchanger analogy is used to calculate the heat transfer between the heat transfer fluid and the pond. The differential equation defined by the heat balance is solved using a fourth order Runge-Kutta numerical integration method. The implementation along with the model equations are summarized in the figure below.
+
+\begin{figure}[hbtp] % fig 258
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5686.png}
+\caption{Pond Model Component Configuration (Chiasson 1999) \protect \label{fig:pond-model-component-configuration-chiasson}}
+\end{figure}
+
+The model overall pond model consists in a number of sub-models which are enumerated below.
+
+\subsubsection{Solar radiation heat gain to the pond}\label{solar-radiation-heat-gain-to-the-pond}
+
+\begin{equation}
+\rho ' = {\tau_a} - \tau
+\end{equation}
+
+where
+
+\(\rho '\) is the reflectance
+
+\(\tau\) ~is the transmittance of solar radiation by the pond surface and the subscript `a' refers to the absorbed component.
+
+\begin{equation}
+{\tau_a} = {e^{\frac{{ - \mu 'd}}{{\cos {\theta_r}}}}}
+\end{equation}
+
+and
+
+\begin{equation}
+\tau  = \frac{1}{2}\left( {\frac{{1 - {r_{par}}}}{{1 + {r_{par}}}} + \frac{{1 - {r_ \bot }}}{{1 + {r_ \bot }}}} \right){e^{\frac{{ - \mu 'd}}{{\cos {\theta_r}}}}}
+\end{equation}
+
+where
+
+\(\mu '\) is the extinction coefficient for water
+
+\(d\) ~is the pond depth
+
+\({r_{par}}\) represents the parallel component of unpolarized radiation and
+
+\({r_ \bot }\) represents the perpendicular component of unpolarized radiation which are computed by Duffie and Beckman (1991) as:
+
+\begin{equation}
+  r_{par} = \frac{\tan ^2 \left( \theta_r - \theta \right)}{\tan ^2 \left( \theta_r + \theta \right)}
+\end{equation}
+
+\begin{equation}
+  r_{\bot} = \frac{\sin ^2 \left( \theta_r - \theta \right)}{\sin ^2 \left( \theta_r - \theta  \right)}
+\end{equation}
+
+Finally, the amount of solar radiation absorbed by the pond (\({q_{solar}}\) ) is expressed as:
+
+\begin{equation}
+{q_{solar}} = I\left( {1 - \rho '} \right){A_{pond}}
+\end{equation}
+
+where
+
+\(I\) is the solar radiation flux incident on the pond surface (here, the total reflectance is approximated by the beam reflectance)
+
+\({A_{pond}}\) is the area of the pond surface.
+
+The model also accepts solar radiation in the form of beam \(\left( {{I_b}} \right)\) and diffuse \(\left( {{I_d}} \right)\) ~components, in which case \(I\) is computed from:
+
+\begin{equation}
+I = {I_b}\cos \theta  + {I_d}
+\end{equation}
+
+\subsubsection{Thermal radiation heat transfer at the pond surface}\label{thermal-radiation-heat-transfer-at-the-pond-surface}
+
+\begin{equation}
+q{}_{thermal} = \sigma \alpha (T{{}_{surface}^4} - T{{}_{sky}^4})
+\end{equation}
+
+Where
+
+\(\alpha\) = Thermal absorptivity
+
+\(\sigma\) = Stefan Boltzman constant
+
+\subsubsection{Convection heat transfer at the pond surface}\label{convection-heat-transfer-at-the-pond-surface}
+
+\begin{equation}
+q{}_{convection} = h{}_c(T{}_{pond} - T{}_{db})
+\end{equation}
+
+ASHRAE simple convection coefficient model is used to obtain the convection coefficient for external surfaces. Initializing of pond temps to mean of dry-bulb temperature T\(_{db}\) and ground temperatures is useful because repeated warm up days tend to drive the initial pond temperature toward the dry-bulb temperature Hence, for each environment the simulation starts the pond temperature T\(_{pond}\) midway between the dry-bulb and ground temperature.
+
+\subsubsection{Heat transfer to/from ground to the pond}\label{heat-transfer-tofrom-ground-to-the-pond}
+
+Hull et al (1984) expressed the following equation for ground heat losses from any pond. The equations are also based on the assumption that, for all practical purposes, the constant temperature sink is the ground water table (Kishore and Joshi 1984)
+
+\begin{equation}
+q{}_{ground} = U{}_{ground}A{}_{ground}(T{}_{groundwater} - T{}_{pond})
+\end{equation}
+
+\begin{equation}
+U{}_{ground} = 0.999\left( {\frac{{k{}_{ground}}}{{d{}_{groundwater} - d{}_{pond}}}} \right) + 1.37\left( {\frac{{k{}_{ground}P{}_{pond}}}{{A{}_{pond}}}} \right)
+\end{equation}
+
+Where
+
+\(k{}_{ground}\) ~~~~~~~ = Thermal conductivity of the ground
+
+~\(d{}_{groundwater}\) ~ = depth of water table
+
+\(d{}_{pond}\) ~~~~~~~~~ = Pond depth
+
+\(P{}_{pond}\) ~~~~~~~~ = Pond perimeter
+
+\subsubsection{Heat transfer due to evaporation at the pond surface}\label{heat-transfer-due-to-evaporation-at-the-pond-surface}
+
+Evaporation is calculated assuming a fixed Lewis number unlike the Chaisson model.
+
+\begin{equation}
+q{}_{evaporation} = {\left( {\frac{{\Pr }}{{Sc}}} \right)^{2/3}}\left( {\frac{{h{}_c}}{{Cp{}_{air}}}} \right)\left( {HR{}_f - HR{}_a} \right)\left( {q{}_l} \right)
+\end{equation}
+
+Where
+
+Pr = Prandtl number for air
+
+Sc = Schmidt number for air
+
+Hc = convection coefficient
+
+HRf = humidity ratio at pond surface/film temperature
+
+HRa = humidity ratio of air
+
+ql~ = Latent heat of air
+
+Air properties are obtained by applying the existing the psychometric functions of EnergyPlus.
+
+\subsubsection{Total heat transfer to/from the heat exchanging fluid flowing in all spools or coils in the pond}\label{total-heat-transfer-tofrom-the-heat-exchanging-fluid-flowing-in-all-spools-or-coils-in-the-pond}
+
+\begin{equation}
+q{}_{fluid} = UA{}_{pipe}(T{}_{fluid} - T{}_{pond})N{}_{circuit}
+\end{equation}
+
+Where
+
+\(UA{}_{pipe}\) ~ = overall heat transfer coefficient expressed in terms of inside pipe area
+
+\(N{}_{circuit}\) = number of spools installed in the pond
+
+The fluid temperature Tfluid is computed as the average fluid temperatures of the inlet and the outlet node at a given temperature.
+
+\begin{equation}
+U{A_{pipe}} = \frac{{2\pi {r_i}\cdot {L_{spool}}}}{{\sum {{r_t}} }}
+\end{equation}
+
+where
+
+\({r_i}\) = inner pipe radius
+
+\({L_{spool}}\) l = length of one spool
+
+\(\sum {{r_t}}\) = composite thermal resistance defined as
+
+\(\sum {{r_t}}\) = Resistance due to fluid flow in the pipe +external pipe thermal resistance +fouling factor
+
+\subsubsection{References}\label{references-4-002}
+
+Chiasson, A.D. 1999. \emph{Advances in modeling of groundsourceheat pump systems}. Master's thesis,Oklahoma State University, Stillwater, OK
+
+Duffie, J.A., and W.A. Beckman. 1991. \emph{Solar engineering of thermal processes,} 2d ed. New York: John Wiley \& Sons.
+
+Hull, J.R., K.V. Liu, W.T. Sha, J. Kamal, and C.E. Nielsen. 1984. Dependence of ground heat losses upon solar pond size and perimeter insulation---Calculated and experimental results. \emph{Solar Energy} 33(1): 25-33
+
+Kishore, V.V.N., and V. Joshi. 1984. A practical collector efficiency equation for nonconvecting solar ponds. \emph{Solar Energy} 33(5): 391-395.
+
+Rees, S.J., J.D. Spitler and X. Xiao, X 2002.\href{http://www.hvac.okstate.edu/pdfs/Rees_Spitler_Xiao_02.pdf}{Transient Analysis of Snow-melting System Performance}.\emph{ASHRAE Transactions.}108(2):406-423.
+
+\subsection{Plant Loop Surface-Ground-To-Water Heat Exchanger}\label{plant-loop-surface-ground-to-water-heat-exchanger}
+
+This model (Object: GroundHeatExchanger:Surface) is based on the QTF formulation of heat transfer through building elements with embedded heat sources/sinks. The model uses a heat exchanger analogy to relate the inlet fluid temperature to the net heat transfer rate and consequently outlet temperature. The model is entirely passive, i.e.~it does not set any flow rates or incorporate any controls. In order to deal with the non-linear boundary conditions at the top surface due to the presence of ice/snow fluxes have to be calculated by the QTF model and temperature calculated from the surface heat balance. This requires some iteration. Note, top surface variables correspond to `outside' variables in standard CTF/QTF definition. Bottom surface variables correspond to `inside' variables.
+
+For given current surface temperatures the terms of the QTF equations can be grouped into constant terms, and those depending on the current source flux. The surface heat balance may be given by the following equation (Strand,1997)
+
+\begin{equation}
+QS{}_{} = \sum\limits_{m = 1}^M {X{}_{k,m}} T{}_{i,t - m + 1} - \sum\limits_{m = 1}^M {Y{}_{k,m}} T{}_{o,t - m + 1} + \sum\limits_{m = 1}^k {F{}_m} q{}_{i,t - m} + \sum\limits_{m = 1}^M {W{}_m} {q''}{}_{source,t - m + 1}
+\end{equation}
+
+\begin{equation}
+T{}_S{}_{} = \sum\limits_{m = 1}^M {X{}_{k,m}} T{}_{i,t - m + 1} - \sum\limits_{m = 1}^M {Y{}_{k,m}} T{}_{o,t - m + 1} + \sum\limits_{m = 1}^k {F{}_m} q{}_{i,t - m} + \sum\limits_{m = 1}^M {W{}_m} q''{}_{source,t - m + 1}
+\end{equation}
+
+Where
+
+T\(_{s}\)~~~ = temperature of the node where the heat source or sink is present
+
+\(QS\) = Surface heat balance
+
+\({q''}\) = Heat flux
+
+T~~ = Temperature
+
+i~~~ = ~ inside of the building element
+
+o~~ = outside of the building element
+
+t~~~ = current time step
+
+X Y F = Conduction transfer functions
+
+The surface balance equation includes terms for incident solar energy, radiation heat transfer from internal sources, linearized radiation between surfaces using the mean radiation temperature concept and convection to the surrounding air.
+
+The heat balance on the water loop is given by
+
+\begin{equation}
+q = \dot mc{}_p(T{}_{wi} - T{}_{wo})
+\end{equation}
+
+Where
+
+q = heat transferred between the water loop and the building elements.
+
+\(\dot m\) = mass flow rate of water
+
+\(T{}_{wi}\) = Inlet water temperature
+
+\(T{}_{wo}\) = Outlet water temperature
+
+From the second law of thermodynamics the maximum amount of heat transfer is
+
+\begin{equation}
+q{}_{\max } = (\dot mc{}_p){}_{water}(T{}_{wi} - T{}_s)
+\end{equation}
+
+Where
+
+T\(_{s}\) = temperature at the source location
+
+The effectiveness of the heat exchanger is given by
+
+\begin{equation}
+\varepsilon  = 1 - {e^{ - NTU}}
+\end{equation}
+
+Where NTU is defined by
+
+\begin{equation}
+NTU = \frac{{UA}}{{(\dot mC{}_p){}_{water}}}
+\end{equation}
+
+\begin{equation}
+UA = h\pi DL
+\end{equation}
+
+h is the convection coefficient, D is the interior tube diameter and L is the total length of the tube.
+
+The Colburn equation is used to define the Nusselt number Nu
+
+\begin{equation}
+Nu = \frac{{hD}}{k} = 0.023{\mathop{\rm Re}\nolimits} {{}_D^{4/5}}{\Pr ^{1/3}}
+\end{equation}
+
+Pr is the Prandtl number, Re is the Reynolds number and k is the thermal conductivity of the fluid
+
+\begin{equation}
+{\mathop{\rm Re}\nolimits} {}_D = \frac{{4\dot m}}{{\pi \mu D}}
+\end{equation}
+
+with \(\mu\) ~being the absolute viscosity of water
+
+\subsection{Plant Loop Fluid-to-Fluid Heat Exchanger}\label{plant-loop-fluid-to-fluid-heat-exchanger}
+
+This component (Object: HeatExchanger:FluidToFluid) is a simple hydronic heat exchanger that can be used to couple two (hydronic) plant or condenser loops.~ Sizing and nominal capacity calculations are discussed elsewhere in this document, see the section called Plant Heat Exchanger Sizing. This section first discusses the heat transfer modeling and the control issues.
+
+Heat exchanger performance modeling uses classic effectiveness-NTU correlations. The heat exchanger model can be specified as one of seven types: ~cross flow both fluid streams unmixed, cross flow both fluid streams mixed, cross flow maximum capacity flow mixed min), counter flow, parallel flow, or ideal. The model correlations determine a heat transfer effectiveness value, \(\varepsilon\) , which is a function of heat exchanger UA, the mass flow rates through boths sides, and the specific heat of the fluids in the streams.~ The effectiveness of an ideal heat exchanger is set to 1.0 and no correlation is needed.
+
+Because the heat exchanger is intended to be generic, its two sides are distinguished by the nature of loop side being connected.~ One side is called ``Loop Supply Side'' to indicate the heat exchanger is situated on the supply side of a loop. The other side is called ``Loop Demand Side'' to indicate it is on the demand side of a loop.~ The heat exchanger is intended to act as a supply component for the loop connected to it as the ``Loop Supply Side'' and as a demand component for the loop connected to it as the ``Loop Demand Side.''~ From the point of view of the heat exchanger component itself, the Loop Demand Side acts like a supply source/sink for the Loop Supply Side which acts like a demand to the component.
+
+The mass flow rates and specific heat capacity are multiplied together to evaluate flow thermal capacity for each side and the minimum, maximum, and capacity ratio, \({R_C}\) , are determined.
+
+\begin{equation}
+{\left( {\dot m{c_p}} \right)_{SupLoop}} = {\dot m_{SupLoop}}*{c_p}_{SupLoop}
+\end{equation}
+
+\begin{equation}
+{\left( {\dot m{c_p}} \right)_{DmdLoop}} = {\dot m_{DmdLoop}}*{c_p}_{DmdLoop}
+\end{equation}
+
+\begin{equation}
+{\left( {\dot m{c_p}} \right)_{Min}} = MIN\left( {{{\left( {\dot m{c_p}} \right)}_{SupLoop}},{{\left( {\dot m{c_p}} \right)}_{DmdLoop}}} \right)
+\end{equation}
+
+\begin{equation}
+{\left( {\dot m{c_p}} \right)_{Max}} = MAX\left( {{{\left( {\dot m{c_p}} \right)}_{SupLoop}},{{\left( {\dot m{c_p}} \right)}_{DmdLoop}}} \right)
+\end{equation}
+
+\begin{equation}
+{R_C} = \frac{{{{\left( {\dot m{c_p}} \right)}_{Min}}}}{{{{\left( {\dot m{c_p}} \right)}_{Max}}}}
+\end{equation}
+
+NTU, or Number of Transfer Units, is calculated using:
+
+\begin{equation}
+NTU = \frac{{UA}}{{{{\left( {\dot m{c_p}} \right)}_{Min}}}}
+\end{equation}
+
+For a counter flow heat exchanger, effectiveness is calculated using:
+
+\begin{equation}
+\varepsilon  = \frac{{1 - exp\left[ { - NTU\left( {1 - {R_C}} \right)} \right]}}{{1 - {R_C}exp\left[ { - NTU\left( {1 - Rc} \right)} \right]}}
+\end{equation}
+
+For a parallel flow heat exchanger, effectiveness is calculated using:
+
+\begin{equation}
+\varepsilon  = \frac{{1 - exp\left[ { - NTU\left( {1 + {R_C}} \right)} \right]}}{{\left( {1 + {R_C}} \right)}}
+\end{equation}
+
+For a cross flow heat exchanger with both streams unmixed, effectiveness is calculated using:
+
+\begin{equation}
+\varepsilon  = 1 - exp\left\{ {\frac{{NT{U^{0.22}}}}{{{R_C}}}\left[ {exp\left( { - {R_C}NT{U^{0.78}}} \right) - 1} \right]} \right\}
+\end{equation}
+
+For a cross flow heat exchanger with both streams mixed, the effectiveness is calculated using:
+
+\begin{equation}
+\varepsilon  = {\left[ {\frac{1}{{1 - exp\left( { - NTU} \right)}} + \frac{{{R_C}}}{{1 - exp\left( { - {R_C}NTU} \right)}} - \frac{1}{{NTU}}} \right]^{ - 1}}
+\end{equation}
+
+For a cross flow heat exchanger with the stream with the higher capacity mixed and the stream with the lower capacity unmixed, the effectiveness is calculated using:
+
+\begin{equation}
+\varepsilon  = \frac{1}{{{R_C}}}\left\{ {1 - exp\left[ {{R_C}\left( {exp\left( { - NTU} \right) - 1} \right)} \right]} \right\}
+\end{equation}
+
+For a cross flow heat exchanger with the stream with higher capacity unmixed and the stream with lower capacity mixed, the effectiveness is calculated using:
+
+\begin{equation}
+\varepsilon  = 1 - exp\left\{ { - \frac{1}{{{R_C}}}\left[ {1 - exp\left( { - {R_C}NTU} \right)} \right]} \right\}
+\end{equation}
+
+Effectiveness values are always limited to be no higher than 1.0.~ The program code protects from evaluating the exponential with operands that are too large or too small. Once the effectiveness value is determined, the heat transfer rate is calculated using:
+
+\begin{equation}
+\dot Q = \varepsilon {\left( {\dot m{c_p}} \right)_{Min}}\left( {{T_{SupLoop,In}} - {T_{DmdLoop,In}}} \right)
+\end{equation}
+
+Lastly, the fluid temperatures leaving the heat exchanger are calculated using:
+
+\begin{equation}
+{T_{SupLoop,Out}} = {T_{SupLoop,In}} - \frac{{\dot Q}}{{{{\left( {\dot m{c_p}} \right)}_{SupLoop}}}}
+\end{equation}
+
+\begin{equation}
+{T_{DmdLoop,Out}} = {T_{DmdLoop,In}} + \frac{{\dot Q}}{{{{\left( {\dot m{c_p}} \right)}_{DmdLoop}}}}
+\end{equation}
+
+The plant heat exchanger offers a number of control options for a wide variety of applications.~ This section documents the control decision logic. The general goal of the control is to provide appropriate conditioning of the fluid at the Loop Supply Side connection. ~The basic control action is to request the appropriate flow rates for each side of the heat exchanger.~ For all of the control modes, there is also an availability schedule that provides a level of supervisory control to determine if the heat exchange is available to run at all.~ If the device is scheduled off, then zero flow is requested for both connections. All the control modes can also use minimum and maximum temperature limits.~ If the limits are used and either of the two inlet temperatures exceeds the limit, the zero flow is requested for both connections.
+
+\textbf{UncontrolledOn.~} This control type is very simple.~ If scheduled on it requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
+
+\textbf{OperationSchemeModulated.~} This control type uses the plant operation schemes. Any of the various plant (or condenser) operation schemes (e.g.~PlantEquipmentOperation:CoolingLoad or PlantEquipmentOperation:HeatingLoad ). When the heat exchanger is called, the operation scheme will pass a value for the load to be met.~ If the absolute value of the load is less than a small tolerance (1 W), then zero flow is requested for both connections.~ If load is significant and negative, then the heat exchanger will attempt to provide cooling.~ If the load is significant and positive, then it will attempt to provide heating.~ The two inlet fluid temperatures are compared and if their difference exceeds the minimum temperature difference and has the correct sign for heating or cooling as needed, then the heat exchanger is turned ``on.''~ The model requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then a flow rate for the Loop Demand Side is found to attempt to meet the load.~ The load value is converted to a target temperature for the fluid leaving the Loop Supply Side connection.~ The target temperature is then used with the numerical method Regula Falsi to solve for the flow rate.
+
+\textbf{OperationSchemeOnOff}.~ This control type uses the plant operation schemes. Any of the various plant (or condenser) operation schemes (e.g.~PlantEquipmentOperation:CoolingLoad or PlantEquipmentOperation:HeatingLoad). When the heat exchanger is called, the operation scheme will pass a value for the load to be met.~ If the absolute value of the load is less than a small tolerance (1 W), then zero flow is requested for both connections.~ If load is significant and negative, then the heat exchanger will attempt to provide cooling.~ If the load is significant and positive, then it will attempt to provide heating.~ The two inlet fluid temperatures are compared and if their difference exceeds the minimum temperature difference and has the correct sign for heating or cooling as is needed, then the heat exchanger is turned ``on.''~ The model requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
+
+\textbf{HeatingSetpointModulated}.~ This control scheme uses a node setpoint. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible.~ The temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if heating is desired.~ If heating is both desired and possible, then the heat exchanger is turned ``on.''~ The model requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then a flow rate for the Loop Demand Side is found to attempt to meet the setpoint.~ The setpoint temperature is then used with the numerical method Regula Falsi to solve for the flow rate.
+
+\textbf{HeatingSetpointOnOff}.~ This control scheme uses a node setpoint. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible.~ The temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if heating is desired.~ If heating is both desired and possible, then the heat exchanger is turned ``on.''~ The model requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
+
+\textbf{CoolingSetpointModulated}.~ This control scheme uses a node setpoint. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.~ The temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if cooling is desired.~ If cooling is both desired and possible, then the heat exchanger is turned ``on.''~ The model requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then a flow rate for the Loop Demand Side is found to attempt to meet the setpoint.~ The setpoint temperature is then used with the numerical method Regula Falsi to solve for the flow rate.
+
+\textbf{CoolingSetpointOnOff}.~ This control scheme uses a node setpoint. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.~ The temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if cooling is desired.~ If cooling is both desired and possible, then the heat exchanger is turned ``on.''~ The model requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
+
+\textbf{CoolingSetpointOnOffWithComponentOverride}.~ This control scheme uses one of three different control signals, a node setpoint, outdoor air drybulb temperature, or outdoor air wetbulb temperature. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.~ The control signal is compared to the inlet temperature for the Loop Supply Side to see if cooling is desired.~ If cooling is both desired and possible, then the heat exchanger is turned ``on.''~ When the heat exchanger is on, the remote chiller component is turned off.~ The model requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
+
+\textbf{CoolingDifferentialOnOff}.~ This control scheme is based on a simple temperature difference. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.~ If cooling is possible then it is assumed to be desired and the heat exchanger is turned ``on.''~ The model requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
+
+\textbf{DualDeadbandSetpointModulated}.~ This control scheme uses dual setpoints on a node. The basic idea is that the heat exchanger will condition the Loop Supply Side connection to drive its temperature into the deadband whenever its inlet temperature is outside the deadband.~ The model expects dual temperature setpoints to be placed on the setpoint, for example using the object SetpointManager:Scheduled:DualSetpoint.
+
+The heat exchanger will operate to cool the Loop Supply Side fluid when the following three conditions are all met:
+
+1)~ the two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible,
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  the higher temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible, and
+\end{enumerate}
+
+3)~ the higher temperature setpoint on the reference node is compared to the inlet temperature for the Loop Demand Side to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.
+
+The heat exchanger will operate to heat the Loop Supply Side fluid when the following three conditions are all met:
+
+1)~ the two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible,
+
+2)~ the lower temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible, and
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  the lower temperature setpoint on the reference node is compared to the inlet temperature for the Loop Demand Side to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible.
+\end{enumerate}
+
+When the heat exchanger is turned ``on.''~ The model requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then a flow rate for the Loop Demand Side is found to attempt to meet the setpoint.~ The setpoint temperature is then used with the numerical method Regula Falsi to solve for the flow rate.
+
+\textbf{DualDeadbandSetpointOnOff}. This control scheme uses dual setpoints on a node. The basic idea is that the heat exchanger will condition the Loop Supply Side connection to drive its temperature into the deadband whenever its inlet temperature is outside the deadband.~ The model expects dual temperature setpoints to be placed on the setpoint, for example using the object SetpointManager:Scheduled:DualSetpoint.
+
+The heat exchanger will operate to cool the Loop Supply Side fluid when the following three conditions are all met:
+
+1)~ the two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible,
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  the higher temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible, and
+\end{enumerate}
+
+3)~ the higher temperature setpoint on the reference node is compared to the inlet temperature for the Loop Demand Side to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.
+
+The heat exchanger will operate to heat the Loop Supply Side fluid when the following three conditions are all met:
+
+1)~ the two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible,
+
+2)~ the lower temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible, and
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  the lower temperature setpoint on the reference node is compared to the inlet temperature for the Loop Demand Side to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible.
+\end{enumerate}
+
+When the heat exchanger is turned ``on,'' the model requests the full design flow rate on the Loop Supply Side connection.~ If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
+
+\subsection{References}\label{references-5-002}
+
+Strand, R.K. and C.O. Pedersen, 1997.~ Implementation of a Radiant Heating and Cooling Model Into an Integrated Building Energy Analysis Program, ASHRAE Transactions v. 103, n. 1, pp 949-958, 1997.
+
+Incropera, F.P. and D.P. DeWitt. 1981. Fundamentals of Heat Transfer. New York: John Wiley \& Sons.
+
+Mills, A.F.1999. Heat Transfer, Second Edition. Prentice Hall. New Jersey.
+
+Presentation by Taylor Engineering.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/hvac-controllers.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/hvac-controllers.tex
new file mode 100644
index 00000000000..335a0b34715
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+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/hvac-controllers.tex
@@ -0,0 +1,357 @@
+\section{HVAC Controllers }\label{hvac-controllers}
+
+\subsection{Control Valve for Water-Based Air System Coils}\label{control-valve-for-water-based-air-system-coils}
+
+The input object Controller:WaterCoil provides a simple controller model for adjusting water flow rates to meet the desired air side conditions. It is really a solution inverter. For a water coil the simulation cannot be inverted where the mass flow rate of the water through the coil can be solved directly given an air temperature. Thus, this ``controller'' will numerically step through all of the water flow possibilities by a root finding technique until the mass flow rate is determined to meet the specified outlet air temperature within a specified user tolerance.
+
+\subsubsection{Model Description}\label{model-description-012}
+
+The figure below illustrates the use of a simple controller used with a central chilled water coil (control variable Temperature). The controller reads the desired temperature setpoint from the control node (established by a SetpointManager) and modulates the chilled water flow rate at the actuator node in order to meet the desired supply (coil outlet) air temperature.
+
+ % fig 190
+\begin{figure}[hbtp]
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4384.png}
+\caption{Controller:WaterCoil used with Central Chilled Water Coil \protect \label{fig:controller-watercoil-used-with-central}}
+\end{figure}
+
+In this case, the controller simply senses the temperature at the control node and compares this value with the desired temperature setpoint. If the sensed temperature is above the desired setpoint temperature, the chilled water flow rate is increased. This controller may be used for both chilled water and hot water coils. The action parameter input is set to REVERSE for chilled water cooling coils and NORMAL for hot water heating coils.
+
+The simple controller may also be used to control both high temperature and high humidity levels by controlling the water flow rate through a chilled water coil. Setting the controller's control variable to TemperatureAndHumidityRatio enables this feature. In this case, the controller monitors two setpoint values, one for temperature control and the other for high humidity control. Note that two setpoint managers must be used to establish these setpoints as shown in the figure below. The limiting case for either temperature or high humidity control (i.e., the minimum supply air temperature required to meet both setpoints) is used for controlling the water flow rate through the chilled water coil. If high humidity control is the limiting case then colder supply air will be delivered by the cooling coil to achieve proper dehumidification and some form of air reheat may be required to avoid overcooling of the zones being served by this air loop.
+
+\begin{figure}[hbtp] % fig 191
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4385.png}
+\caption{Two Setpoint managers used in Controller:WaterCoil \protect \label{fig:two-setpoint-managers-used-in-controller}}
+\end{figure}
+
+When the control variable TemperatureAndHumidityRatio is used, the controller modulates water flow through a chilled water coil to meet both a temperature and a humidity ratio setpoint. These two setpoints are placed on the control node by setpoint managers.
+
+The model first calculates the approach temperature using the dry-bulb temperature and dewpoint temperature of the air leaving the water coil:
+
+\begin{equation}
+{T_{dp}} = {\rm{PsyTdpFnWPb}}\left( {{\omega_{SA}},P} \right)
+\end{equation}
+
+\begin{equation}
+{T_{approach}} = {T_{SA}} - {T_{dp}}
+\end{equation}
+
+where:
+
+\({T_{approach}}\) = approach temperature, ËšC
+
+\({\omega_{SA}}\) ~ = supply (outlet) air humidity ratio, kg/kg
+
+\(P\) ~~ = outdoor barometric pressure, Pa
+
+\({T_{dp}}\) ~ = supply (outlet) air dewpoint temperature, ËšC
+
+\({T_{SA}}\) ~ = supply (outlet) air dry-bulb temperature, ËšC
+
+\({\rm{PsyTdpFnWPb}}\) = EnergyPlus psychrometric function, returns dewpoint temperature given humidity ratio and barometric pressure
+
+The supply air dewpoint temperature required to meet the humidity ratio setpoint (placed on the control node by SetpointManager:SingleZone:Humidity:Maximum, SetpointManager:MultiZone:MaximumHumidity:Average~ or SetpointManager:MultiZone:Humidity:Maximum) is then calculated as a function of the humidity ratio setpoint and barometric pressure as follows:
+
+\begin{equation}
+{T_{dp,SP}} = {\rm{PsyTdpFnWPb}}\left( {{\omega_{SP}},P} \right)
+\end{equation}
+
+where:
+
+\({T_{dp,SP}}\) = dewpoint temperature corresponding to \emph{w\(_{SP}\)}, ËšC
+
+\({\omega_{SP}}\) = humidity ratio setpoint, kg/kg
+
+In order for the dewpoint temperature of the coil's supply (outlet) air to reach \({T_{dp,SP}}\) ~the dry-bulb temperature of air leaving the cooling coil must be at \({T_{dp,SP}} + {T_{approach}}\) :
+
+\begin{equation}
+{T_{HR,SP}} = {T_{dp,SP}} + {T_{approach}}
+\end{equation}
+
+where:
+
+\({T_{HR,SP}}\) = supply air dry-bulb temperature setpoint required to achieve the specified humidity ratio setpoint, ËšC
+
+The supply air temperature setpoint required to achieve the specified humidity ratio setpoint is then compared to the setpoint temperature required for zone temperature control, and the minimum of these two setpoint values is used as the setpoint temperature for controlling the chilled water coil.
+
+\begin{equation}
+{T_{SP}} = MIN\left( {{T_{Temp,SP}},{T_{HR,SP}}} \right)
+\end{equation}
+
+where:
+
+\({T_{SP}}\) = chilled water coil supply air temperature setpoint, ËšC
+
+\({T_{Temp,SP}}\) = supply air temperature setpoint required for zone temperature control, ËšC
+
+As described previously, the controller varies the chilled water flow rate through the coil using a root finding technique until the actual supply air temperature reaches \emph{T\(_{sp}\)}within the specified tolerance:
+
+\begin{equation}
+{T_{Actual}} - {T_{SP}}\,\, \le \,\,\,Controller\,Convergence\,Tolerance
+\end{equation}
+
+where:
+
+\({T_{Actual}}\) = actual air temperature leaving the cooling coil, ËšC
+
+\subsection{Outdoor Air Damper Controller for Air Systems}\label{outdoor-air-damper-controller-for-air-systems}
+
+When the heat exchanger assisted cooling coil is used with a furnace or unitary system (ref. AirLoopHVAC:Unitary:Furnace:HeatCool or AirLoopHVAC:UnitaryHeatCool) or DX system (ref. CoilSystem:Cooling:DX) located in an air loop (or DX system used in an outside air system), an ecomizier function may be customized as necessary. For economizer control, an outdoor air controller (ref. Controller:OutdoorAir) is used to define the economizer control inputs and determine when economizer mode is active. The heat exchanger (ref. HeatExchanger:*) object provides an economizer lockout feature which disables heat recovery any time the economizer is active. This feature can be turned on and off using the heat exchanger lockout input. Heat exchanger assisted cooling coils used with the zone equipment described below disregard this economizer control feature. The heat recovery bypass control input may also be used to selectively control heat recovery.
+
+\subsubsection{Inputs}\label{inputs}
+
+\begin{itemize}
+\item
+  Controller Name
+\item
+  Relief air node
+\item
+  Return air node
+\item
+  Control node (the mixed air node)
+\item
+  Actuated node (the outside air inlet node)
+\item
+  Minimum outside air flow rate (at design) {[}m\(^{3}\)/s{]}
+\item
+  Maximum outside air flow rate~ (\({\dot V_{oa,\max }}\) ) {[}m\(^{3}\)/s{]}
+\item
+  EconomizerChoice: \emph{FixedDryBulbr} \textbar{} \emph{FixedEnthalpy} \textbar{} \emph{~DifferentialDryBulb~} \textbar{} \emph{~DifferentialEnthalpy} \textbar{} \emph{~~ElectronicEnthalpy} \textbar{} \emph{~~FixedDewPointAndDryBulb~~~} \textbar{} \emph{DifferentialDryBulbAndEnthalpy~} \textbar{} \emph{NoEconomizer}
+\item
+  Bypasschoice: \emph{MinimumFlowWithBypass} \textbar{} \emph{ModulateFlow}
+\item
+  High temperature limit (\({T_{high}}\) ) {[}C{]}
+\item
+  High specific enthalpy limit (\({h_{high}}\) ~) {[}J/kg{]}
+\item
+  High dewpoint temperature limit (\({T_{DP,high}}\) ) {[}C{]}
+\item
+  Electronic Enthalpy limit (quadratic or cubic curve object)
+\item
+  Low temperature limit (\({T_{low}}\) ) {[}C{]}
+\item
+  Lockout: \emph{LockoutWithHeating} \textbar{} \emph{LockoutWithCompressor}
+\item
+  MinimumLimit: \emph{FixedMinimum} \textbar{} \emph{ProportionalMinimum}
+\item
+  Minimum outside air schedule (schedule values multiply the minimum outside air flow rate)
+\item
+  Minimum Outside air flow Schedule(schedule values sets the limit on minimum outside air)
+\item
+  Maximum Outside air flow Schedule(schedule values sets the maximum amount of outside air possible in the system)
+\item
+  Name of Controller:MechanicalVentilation object
+\item
+  Time-of-day economizer control schedule (economizer active when schedule values are greater than 0)
+\item
+  High humidity control flag: \emph{Yes} \textbar{} \emph{No}
+\item
+  Humidstat control zone name (zone name where humidistat is located)
+\item
+  Control high indoor humidity based on outdoor humidity ratio: \emph{Yes} \textbar{} \emph{No}
+\item
+  High humidity outside air flow ratio (this flow ratio is multiplied by the maximum outside air flow rate during periods of high indoor relative humidity)
+\item
+  Heat Recovery Bypass Control Type: BypassWhenWithinEconomizerLimits \textbar{} BypassWhenOAFlowGreaterThanMinimum
+\end{itemize}
+
+\subsubsection{Economizer Limits}\label{economizer-limits}
+
+Economizer limits may be used to create single-point or multi-point controllers. The figure below shows several examples of each type of controller. Single-point economizer controllers use a single independent variable to specify the operation of the economizer. In all cases, the economizer is disabled (OFF) when the outdoor weather condition exceeds the limit. However, when a low temperature limit is used the economizer is disabled when the outdoor temperature is \emph{below} the low dry-bulb temperature limit.
+
+Economizer limits may also be used to create multi-point controllers where two or more limits specify the economizer operating region. The economizer is disabled (OFF) if any single multi-point economizer limit is exceeded.
+
+\begin{figure}[hbtp] % fig 192
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4411.png}
+\caption{Economizer Limit Controls \protect \label{fig:economizer-limit-controls}}
+\end{figure}
+
+\subsubsection{Simulation}\label{simulation-000}
+
+The simulation contains 4 steps.
+
+\subsubsection{Step 1: calculate the minimum outside air flow rate}\label{step-1-calculate-the-minimum-outside-air-flow-rate}
+
+The user inputs the minimum outside air flow rate (or it is automatically calculated by the program from the user's design inputs). This is converted to a mass flow rate \({\dot m_{oa,\min ,des}}\) using the density of dry air at 20 degrees C. If the economizer is on an air loop then the minimum outside air flow fraction is initialized to:
+
+\begin{equation}
+{f_{oa,\min }} = {\dot m_{oa,\min ,des}}/{\dot m_{s,des}}
+\end{equation}
+
+Where \({\dot m_{s,des}}\) is the design supply air mass flow rate. If the economizer is not on an air loop the minimum outside air flow fraction is initialized to:
+
+\begin{equation}
+{f_{oa,\min }} = {\dot m_{oa,\min ,des}}/{\dot m_{oa,\max ,des}}
+\end{equation}
+
+where \({\dot m_{oa,\max ,des}}\) is the user input maximum outside air volumetric flow rate converted to mass flow rate in the same manner as for the minimum outside air flow rate. If a minimum outside air schedule has been input, \({f_{oa,\min }}\) is multiplied by the current schedule value.
+
+\subsubsection{Step 2: calculate an initial outside air signal}\label{step-2-calculate-an-initial-outside-air-signal}
+
+We now define an initial outside air signal \({S_{oa,init}}\) .
+
+If \(\left| {{T_{_r}} - {T_{in}}} \right| > \Delta {T_{small}}\) then:
+
+\({S_{oa,init}} = ({T_r} - {T_{mix,set}})/({T_r} - {T_i})\) .
+
+Otherwise:
+
+if \({T_r} < {T_{mix,set}}\) and \({T_r} \ge {T_i}\) ~, \({S_{oa,init}}\) is set to -1;
+
+if \({T_r} < {T_{mix,set}}\) ~and \({T_r} < {T_i}\) , \({S_{oa,init}}\) ~~is set to 1;
+
+if \({T_r} \ge {T_{mix,set}}\) and \({T_r} \ge {T_i}\) , \({S_{oa,init}}\) ~is set to 1;
+
+if \({T_r} \ge {T_{mix,set}}\) ~and \({T_r} < {T_i}\) , \({S_{oa,init}}\) ~is set to -1.
+
+Finally, \({S_{oa,init}}\) is constrained to be: \({f_{oa,\min }} \le {S_{oa,init}} \le 1\) . Basically, if the outside air can not accomplish cooling, \({S_{oa,init}}\) ~is set to \({f_{oa,\min }}\) . If it can do cooling, \({S_{oa,init}}\) ~is greater than the minimum outside air flow fraction but not greater than1. Here
+
+~~~~~ \emph{T\(_{r}\)} ~is the return air temperature {[}C{]};
+
+\emph{~~~~~ T\(_{i}\)} is the outside air inlet temperature {[}C{]};
+
+\emph{~~~~~ T\(_{mix,set}\)} is the mixed air setpoint {[}C{]};
+
+\emph{~~~~~ \(\Delta {T_{small}}\)}is a small temperature difference {[}delta C{]}, equal to .00001.
+
+\subsubsection{Step 3: do the on/off and limit checks}\label{step-3-do-the-onoff-and-limit-checks}
+
+·~~~~~~~~If \emph{EconomizerChoice} = \emph{No Economizer}, \({S_{oa,init}} = {f_{oa,\min }}\) .
+
+·~~~~~~~~If \({\dot V_{oa,\max }} < {\dot V_{small}}\) , \({S_{oa,init}} = {f_{oa,\min }}\) ; \({\dot V_{small}}\) is.001 m\(^{3}\)/s.
+
+·~~~~~~~~If the economizer is locked out, \({S_{oa,init}} = {f_{oa,\min }}\) .
+
+Note: the above three checks also set the \emph{EconomizerOperationFlag} and \emph{HighHumidityControlFlag} to \emph{false} (economizer and high humidity control not operating).
+
+·~~~~~~~~If \({T_i} > {T_{mix,set}}\) ~, \({S_{oa,init}} = 1\) .
+
+·~~~~~~~~If Differential dry-bulb was input as Economizer choiceand \({T_i} > {T_r}\) , then \({S_{oa,init}} = {f_{oa,\min }}\) .
+
+·~~~~~~~~If Differential Enthalpy was input as Economizer choiceand \({h_i} > {h_r}\) , then \({S_{oa,init}} = {f_{oa,\min }}\) , where \emph{h\(_{i}\)} and \emph{h\(_{r}\)}~are the outside air inlet and return air enthalpies.
+
+Setpoints are checked after this which include check for Fixed dry-bulb temperature~ limit, Enthalpy Limit, Dewpoint Limit and Humidity ratio limit if specified.
+
+·~~~~~~~~If Differential Enthalpy was input as Economizer choiceand \({h_i} > {h_r}\) , then \({S_{oa,init}} = {f_{oa,\min }}\) , where \emph{h\(_{i}\)} and \emph{h\(_{r}\)}~are the outside air inlet and return air enthalpies.
+
+Setpoints are checked after this which include check for Fixed dry-bulb temperature limit, Enthalpy Limit, Dewpoint Limit and Humidity ratio limit if specified.
+
+·~~~~~~~~If a FixedDryBulb / FixedEnthalpy / FixedDewPointAndDryBulb / ElectronicEnthalpy was input as the economizer choice then the limits are checked as before.
+
+·~~~~~~~~Limits are checked as follows
+
+o~~~If a high temperature limit was input and \({T_{oa}} > {T_{high}}\) , \({S_{oa,init}} = {f_{oa,\min }}\) ; where \emph{T\(_{oa}\)} is the outside air temperature.
+
+o~~~If an enthalpy limit was input and \({h_{oa}} > {h_{high}}\) , \({S_{oa,init}} = {f_{oa,\min }}\) ; where \emph{h\(_{oa}\)} is the outside air specific enthalpy.
+
+o~~~If a dewpoint temperature limit was input and \({T_{DP,OA}} > {T_{DP,high}}\) , \({S_{oa,init}} = {f_{oa,\min }}\) ; where T\(_{DP,OA}\) is the outside air dewpoint temperature and T\(_{DP,high}\) is dewpoint temperature limit.
+
+o~~~If an electronic enthalpy curve was input and \({w_{OA}} > {w_{CurveOutput}}\) , \({S_{oa,init}} = {f_{oa,\min }}\) ; where \emph{w}\(_{OA}\) is the outside air humidity ratio and \emph{w}\(_{CurveOutput}\) is the curve's humidity ratio output as a function of outdoor air dry-bulb temperature.
+
+·~~~~~~~~Another Economizer choice called DifferentialDryBulbAndEnthalpy checks the outside air temperature against return temperature and outside air enthalpy against return air enthalpy and also checks the setpoints.
+
+·~~~~~~~~If a low temperature limit was input and \({T_{oa}} < {T_{low}}\) , \({S_{oa,init}} = {f_{oa,\min }}\) .
+
+Note: the above nine cases set the \emph{EconomizerOperationFlag} to \emph{false}~~~~~~ (economizer not operating), otherwise the economizer is active.
+
+·~~~~~~~~If high humidity control is specified and the zone humidistat indicates a moisture load (i.e.~zone relative humidity greater than the relative humidity setpoint), the \emph{HighHumidityOperationFlag} is set to \emph{true.} If high humidity control is based on the outdoor humidity ratio then the \emph{HighHumidityOperationFlag} is set to \emph{true} only when the outdoor air humidity ratio is less than the humidstat's zone humidity ratio. A \emph{true} HIghHumidityOperationFlag also enables economizer operation in the heat exchangers as if the economizer flag used here was also set to \emph{true} (Ref. HeatExchanger:* - field Economizer Lockout).
+
+The economizer schedule is then checked to determine if a ``push-button'' type economizer control is used. When schedule values are greater than 0, the economizer is active (\emph{EconomizerOperationFlag} = \emph{true)}. This test overrides the economizer limit checks described above in Step 3.
+
+\subsubsection{Step 4: calculate the final outside air signal}\label{step-4-calculate-the-final-outside-air-signal}
+
+If \emph{S\(_{oa,init}\)} is greater than \({f_{oa,\min }}\) and less than 1 and the mixed air mass flow rate is greater than \({\dot m_{verysmall}}\) (\({10^{ - 30}}\) ) and night venting is not occuring and \emph{HighHumidityOperationFlag} is false then
+
+·~~~~~~~~we calculate a final outside air signal \emph{S\(_{oa}\)} by using the regula falsi method routine \emph{SolveRegulaFalsi} to zero the residual \({T_{mix,set}} - {T_{mix}}\) by varying the outside air mass flow rate \({S_{oa}}\cdot {\dot m_{mix}}\) . Mass and energy balance are used to obtain the mixed air humidity ratio and enthalpy from the recirculated air and outside air inlet conditions. The psychrometric function \emph{PsyTdbFnHW} is used to obtain \emph{T\(_{mix}\)} from the mixed air enthalpy and humidity ratio.
+
+Otherwise
+
+·~~~~~~~~\({S_{oa}} = {S_{oa,init}}\) .
+
+\subsubsection{Step 5: calculate the outside air flow rate and apply final constraints}\label{step-5-calculate-the-outside-air-flow-rate-and-apply-final-constraints}
+
+·~~~~~~~~If \emph{BypassChoice} = \emph{True and HighHumidityOperationFlag = false}, \({S_{oa}} = {f_{oa,\min }}\) .
+
+1)~~~If the \emph{HighHumidityOperationFlag} is \emph{true} then
+
+\begin{equation}
+  S_{oa} = \max\PB{f_{oa,min},OAFlowRatio_{HighRH}\frac{\dot{m}_{oa,max,des}}{\dot{m}_{mix}}}
+\end{equation}
+
+·~~~~~~~~If night ventilation is occuring, \({S_{oa}} = 1\) .(Night Ventilation has priority over the above constraints)
+
+·~~~~~~~~If the Minimum Outside air flow Schedule and the Maximum outside air flow schedule is available , Out Air signal \emph{S oa},\emph{init} ~is checked against those fractions from the schedule.
+
+~~~~~ S\(_{oa}\)~ = Maximum( Minimum OA fraction, S\(_{oa}\))
+
+~~~~~ S\(_{oa}\)~~~ = Minimum(Maximum OA fraction, S\(_{oa}\))
+
+Now the outside air flow rate is calculated:
+
+\begin{equation}
+{m_{oa}} = {S_{oa}}*{m_{mix}}
+\end{equation}
+
+Calculate the outside air mass flow rate:
+
+If EconomizerOperationFlag is true and HighHumidityOperationFlag is false ~then
+
+\begin{equation}
+{\dot m_{oa}} = {S_{oa}}\cdot {\dot m_{oa,\max ,des}}
+\end{equation}
+
+Otherwise
+
+\begin{equation}
+{\dot m_{oa}} = {S_{oa}}\cdot {\dot m_{mix}}
+\end{equation}
+
+Then the following constraints are applied.
+
+·~~~~~~~~\({\dot m_{oa}}\) ~must be greater than or equal to the air primary loop total exhaust air mass flow rate (\({\dot m_{exhaust}}\) ).
+
+·~~~~~~~~If \emph{MinimumLimit} = \emph{Fixed Minimum}, \({\dot m_{oa}}\) ~must be greater than or equal to the minimum outside air mass flow rate.
+
+·~~~~~~~~\({\dot m_{oa}}\) ~must be \(\le {\dot m_{mix}}\) .
+
+·~~~~~~~~\({\dot m_{oa}}\) ~must be \(\le\) ~the maximum outside air mass flow rate.
+
+If heat recovery bypass control is selected, the type of control determines how heat recovery is simulated. If BypassWhenWithinEconomizerLimits is selected, heat recovery is only active when the EconomizerOperationFlag is false. If BypassWhenOAFlowGreaterThanMinimum is selected \emph{and} the EconomizerOperationFlag is true \emph{and} the outside air mass flow rate is greater than the minimum flow rate, heat recovery is disabled, otherwise heat recovery is active. The heat recovery bypass control option is used to optimize heat recovery in heating mode. Heat recovery is commonly used to reduce the cooling load when outdoor conditions are higher than indoor conditions, however, when outdoor conditions are favorable the heat exchanger can be turned off and the economizer may be used to also reduce the cooling load. Economizer mode is typically involves increasing the outdoor air flow rate. At some point the outdoor air flow rate must be reduced and the heat exchanger should be turned back on to reduce or avoid an indoor heating requirement. This option will typically be used with some form of supply air temperature control used with the heat recovery equipment (Ref. HeatExchanger).
+
+\subsubsection{Step 6: set the relief air mass flow rate}\label{step-6-set-the-relief-air-mass-flow-rate}
+
+\begin{equation}
+{\dot m_{relief}} = \max (0,{\dot m_{oa}} - {\dot m_{exhaust}})
+\end{equation}
+
+\subsection{Outdoor Air Damper Controller for Zone Energy Recovery Ventilator}\label{outdoor-air-damper-controller-for-zone-energy-recovery-ventilator}
+
+The stand alone energy recovery ventilator (ERV) controller is used solely in conjunction with a stand alone energy recovery ventilator (see figure below).
+
+\begin{figure}[hbtp] % fig 193
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image4482.png}
+\caption{Schematic of the ZoneHVAC:EnergyRecoveryVentilator Compound Object \protect \label{fig:schematic-of-the-zonehvac}}
+\end{figure}
+
+This controller object mimics virtually all of the control logic available for a conventional air-side economizer as embodied in the object Controller:OutdoorAir. However, this controller is only used with the stand alone energy recovery ventilator object (dedicated to serving a single zone, without a traditional air distribution system) while the Controller:OutdoorAir is used with systems that utilize an air loop to provide conditioned air to one or more zones. The purpose of this controller is to signal the object HeatExchanger:AirToAir:SensibleAndLatent that favorable conditions are available for free cooling and heat exchange should be suspended (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped). A time-of-day schedule may also be used to simulate a ``push-button'' type economizer. The air flow rate through the stand alone ERV remains the same regardless of whether the controller is signaling for economizer (free cooling) operation or not. In this way, this controller is very similar to Controller:OutdoorAir with the field Economizer Control Action Type set to ``MinimumFlowWithBypass''. However, the supply and exhaust air flow rates may be modified in response to a high indoor humidity condition (i.e., when the zone relative humidity is ``predicted'' to exceed the setpoint, at times the actual zone relative humidity may be slightly below the setpoint. Ref. Zone/Sys Moisture Load Rate Predicted.) and works in a similar fashion to the outside air controller where the air flow rates are adjusted based on a user specified air flow \emph{ratio}.
+
+\subsubsection{Controller Logic}\label{controller-logic}
+
+In many ways, the logic for this controller follows that established for the object Controller:OutdoorAir. Nearly the same computations (source code) are used for this controller as for Controller:OutdoorAir, except the addition of a few calculations that are unique for this stand alone ERV controller. Refer to the \emph{Simulation} discussion for the outdoor air controller to review the calculation procedure. In some instances local variables used in the Controller:OutdoorAir computations are set to specific values for ZoneHVAC:EnergyRecoveryVentilator:Controller to allow the same computations and logic to be used for both controllers. The logic that is being applied for ZoneHVAC:EnergyRecoveryVentilator:Controller is presented below.
+
+As explained above the controller senses when air conditions are such that heat exchange by the air-to-air heat exchanger should be suspended to provide free cooling to the zone, thereby reducing the amount of mechanical cooling that needs to be provided by other equipment. The inputs for this controller specify temperature and/or enthalpy conditions that are used to trigger economizer operation. An economizer lockout input is provided in the heat exchanger object and is used for customizing heat exchanger performance during economizer operation. Heat exchange is suspended only if the heat exchanger's economizer lockout input is set to Yes.
+
+The user can enter a high and low temperature limit for economizer operation. When the supply inlet (outdoor) air is between these two values, heat exchange is suspended while air flow rates remain unchanged. This logic represents a conventional single-point temperature economizer control. If the user wishes to model differential temperature control, EXHAUST AIR TEMP LIMIT should be specified in the proper input field. In this case, heat exchange is suspended whenever the temperature of the exhaust air is greater than the temperature of the outdoor air. The user still needs to set the low temperature limit to restart the heat exchange process when the outdoor temperature falls too low.
+
+A high dewpoint temperature limit may also be specified. When the supply inlet (outdoor) air is below this limit, heat exchange is suspended while air flow rates remains unchanged. The user still needs to set the low temperature limit to restart the heat exchange process when the outdoor temperature falls too low.
+
+Similar logic can be used with air enthalpy. The user can enter a high enthalpy limit, and heat exchange between the supply and exhaust air streams will be suspended when the outdoor air enthalpy falls below this value. This logic represents single-point enthalpy economizer control. If the user wishes to model differential enthalpy control, EXHAUST AIR ENTHALPY LIMIT should be specified in the proper input field. Regardless of modeling single-point enthalpy or differential enthalpy control, the user still needs to set the low temperature limit to restart the heat exchange process when the outdoor temperature falls too low.
+
+The user may also specify an electronic enthalpy curve object to represent a variable enthalpy controller. A quadratic or cubic curve is used in this case. The output of this curve would represent the maximum outdoor humidity ratio allowed as a function of outdoor dry-bulb temperature.
+
+The air flow rates through the stand alone ERV may also be modified based on a high indoor relative humidity condition. The change in air flow rates may occur at any time the indoor relative humidity is high or when the indoor relative humidity is high \emph{and} the outdoor humidity ratio is lower than the indoor humidity ratio. This control mode modifies the air flow rates according to the user specified high humidity outside air flow ratio. When high humidity control is active, heat exchange is suspended in the same manner as if an economizer were used and, as with economizer operation, heat exchange is suspended only if the heat exchanger's economizer lockout input is set to Yes.
+
+The model is flexible, and checks all limits established by the user in the object's input data. The model initially assumes that heat exchange should be suspended, and then checks each one of the limits that the user has set (single-point temperature, differential temperature, single-point enthalpy and differential point enthalpy, single-point dewpoint or electronic (variable) enthalpy). If any of the limits entered by the user is exceeded, then economizer operation is terminated and heat exchange between the supply and exhaust air streams is modeled.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/ice-thermal-storage.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/ice-thermal-storage.tex
new file mode 100644
index 00000000000..e2cc1e82b99
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/ice-thermal-storage.tex
@@ -0,0 +1,217 @@
+\section{Ice Thermal Storage }\label{ice-thermal-storage}
+
+\subsection{Simple Ice Storage Model}\label{simple-ice-storage-model}
+
+\subsubsection{Overview}\label{overview-020}
+
+This model (object name ThermalStorage:Ice:Simple) simulates the performance of an ice storage tank. The model is based on an integrated chiller and storage tank model developed for a special optimization project (Henze and Krarti 2002). This implementation removed the integrated chiller and allows the tank to be charged by any chiller configuration in an EnergyPlus plant loop..
+
+This thermal storage model is based on a simple simulation of an ice storage tank with a fixed capacity.~ The tank is charged, or frozen, in an ice-on-coil configuration where ice builds up on the outside of the tubes carrying the brine or glycol solution from the chiller.~ There are two discharge (melt) options, internal or external.~ Internal melt uses the same fluid tubes for charging and discharging.~ External melt uses a separate fluid path for discharge such that the outer layers of ice melt first.~ The ice storage model includes an implied 3-way valve to control the amount if charge/discharge based on the incoming water temperature and the outlet node setpoint temperature.~ The tank is controlled using the PlantEquipmentOperation:ComponentSetpoint plant operation scheme, and requires that a setpoint be placed by a setpoint manager on the ice storage Plant Outlet Node.~ The model currently does not calculate any tank losses.
+
+\subsubsection{Model Description}\label{model-description-013}
+
+\paragraph{Initialization}\label{initialization-000}
+
+The storage tank is assumed to be fully charged (full of ice) at the beginning of each environment.~ The tank is then allowed to charge and discharge during the warmup days of the environment.
+
+\paragraph{Control}\label{control-000}
+
+The ice storage module is a passive component and will accept any flow rate placed on the inlet node.~ The load on the ice storage tank is determined by the inlet node flow rate, the inlet node temperature, and the outlet node setpoint temperature.~ A positive load indicates a request for cooling and the tank discharges if possible.~ A negative load indicates a request for charging the tank if possible.~ A zero load indicates the tank is dormant in which case all flow bypasses the tank and the outlet node temperature is set to the inlet node temperature.~ The model includes an implied 3-way valve which controls the leaving water temperature to the outlet node setpoint temperature if possible.
+
+\paragraph{Charging}\label{charging}
+
+When charging is requested, the following limits are calculated to determine the actual charging rate:
+
+1)~~~~If the entering water temperature is greater than --1C, the charging rate is zero.
+
+2)~~~~If the entering water temperature is greater than or equal to the outlet setpoint temperature, the charging rate is zero.
+
+3)~~~~If the current fraction of ice stored is 1.0, the tank is fully charge, and the charging rate is zero.
+
+4)~~~~If the requested charging rate times the current system timestep is more than the remaining uncharged storage capacity, the charging rate is limited to that required to completely fill the tank.
+
+5)~~~~The maximum charging rate which the chilled water flow can provide is determined by the entering water temperature and flow rate and an outlet temperature which is the minimum of --1C or the outlet setpoint temperature.
+
+6)~~~~The maximum charging rate which the tank can accept is calculated by the following equations developed in the prior work (Henze and Krarti 2002):
+
+\emph{UAIceCh} = ( 1.3879 - 7.6333*\emph{y} + 26.3423*\emph{y}\(^{2}\) - 47.6084*\emph{y}\(^{3}\) + 41.8498*\emph{y}\(^{4}\) - 14.2948*\emph{y}\(^{5}\) ) * \emph{ITSNomCap} / \emph{TimeInterval} / 10.0
+
+where:
+
+\emph{UAIceCh} ~ = UA rate for charging
+
+\emph{y}~~~~~~~~~~~~~~~ = Current ice fraction stored
+
+\emph{ITSNomCap}~~~~~~~~~ = Nominal storage capacity {[}GJ{]}
+
+TimeInterval = 3600 {[}s{]}
+
+The smallest charging rate determined by the above rules is selected and the corresponding leaving water temperature is calculated.
+
+\paragraph{Discharging}\label{discharging}
+
+When discharging is requested, the following limits are calculated to determine the actual charging rate:
+
+1)~~~~If the entering water temperature is less than 1C, the discharge rate is zero.
+
+2)~~~~If the entering water temperature is less than or equal to the outlet setpoint temperature, the discharge rate is zero.
+
+3)~~~~If the current fraction of ice stored is 0.0, the tank is fully discharged, and the discharge rate is zero.
+
+4)~~~~If the requested discharge rate times the current system timestep is more than the remaining charged storage capacity, the discharge rate is limited to that required to completely deplete the ice in the tank.
+
+5)~~~~The maximum discharge rate which the chilled water flow can accept is determined by the entering water temperature and flow rate and an outlet temperature which is the maximum of 1C or the outlet setpoint temperature.
+
+6)~~~~The maximum discharge rate which the tank can deliver is calculated by the following equations developed in the prior work (Henze and Krarti 2002):
+
+For ice-on-coil internal melt:
+
+\emph{UAIceDisCh} = ( 1.3879 - 7.6333*\emph{y} + 26.3423*\emph{y}\(^{2}\) - 47.6084*\emph{y}\(^{3}\) + 41.8498*\emph{y}\(^{4}\) - 14.2948*\emph{y}\(^{5}\) ) * \emph{ITSNomCap} / \emph{TimeInterval} / 10.0
+
+For ice-on-coil external melt:
+
+\emph{UAIceDisCh} = ( 1.1756 - 5.3689*\emph{y} + 17.3602*\emph{y}\(^{2}\) - 30.1077*\emph{y}\(^{3}\) + 25.6387*\emph{y}\(^{4}\) - 8.5102*\emph{y}\(^{5}\) ) * \emph{ITSNomCap} / \emph{TimeInterval} / 10.0
+
+where:
+
+UAIceDisCh~~~~~~~~~~~ = UA rate for discharging
+
+\emph{y}~~~~~~~~~~~~~~~ = 1 - Current ice fraction stored
+
+\emph{ITSNomCap}~~~~~~~~~ = Nominal storage capacity {[}GJ{]}
+
+TimeInterval = 3600 {[}s{]}
+
+The smallest discharge rate determined by the above rules is selected and the corresponding leaving water temperature is calculated.
+
+\subsubsection{References}\label{references-028}
+
+Henze, Gregor P. and Moncef Krarti. 2002. Predictive Optimal Control of Active and Passive Building Thermal Storage Inventory, Final Report for Phase I:~ Analysis, Modeling, and Simulation.~ U.S. Department of Energy National Energy Technology Laboratory Cooperative Agreement DE-FC-26-01NT41255, December 2002.
+
+\subsection{Detailed Ice Storage Model}\label{detailed-ice-storage-model}
+
+The following section describes how the detailed ice storage model works in EnergyPlus (object name ThermalStorage:Ice:Detailed).
+
+\subsubsection{Charging and Discharging Equation}\label{charging-and-discharging-equation}
+
+The actual performance of the ice storage unit depends on the physical geometry, materials, and characteristics of the ice storage unit.~ In analyzing performance data trends from ice storage manufacturers, it was determined that the following equation would work well for the discharging process:
+
+\begin{equation}
+{q^*} = \left[ {C1 + C2\left( {1 - {P_c}} \right) + C3{{\left( {1 - {P_c}} \right)}^2}} \right] + \left[ {C4 + C5\left( {1 - {P_c}} \right) + C6{{\left( {1 - {P_c}} \right)}^2}} \right]\Delta T_{lm}^*
+\end{equation}
+
+or
+
+\begin{equation}
+{q^*} = \left[ {C1 + C2\left( {{P_d}} \right) + C3{{\left( {{P_d}} \right)}^2}} \right] + \left[ {C4 + C5\left( {{P_d}} \right) + C6{{\left( {{P_d}} \right)}^2}} \right]\Delta T_{lm}^*
+\end{equation}
+
+where:
+
+\begin{equation}
+{q^*} \equiv \frac{{q\Delta t}}{{{Q_{stor}}}}
+\end{equation}
+
+\begin{equation}
+\Delta T_{lm}^* \equiv \frac{{\Delta {T_{lm}}}}{{\Delta {T_{no\min al}}}}
+\end{equation}
+
+\begin{equation}
+\Delta {T_{lm}} \equiv \frac{{{T_{brine,in}} - {T_{brine,out}}}}{{\ln \left( {\frac{{{T_{brine,in}} - {T_{brine,freeze}}}}{{{T_{brine,out}} - {T_{brine,freeze}}}}} \right)}}
+\end{equation}
+
+q is the instantaneous heat transfer rate,
+
+Qstor is the total latent storage capacity,
+
+Dt is a time step used in the curve fit (usually one hour),
+
+DT\(_{nominal}\) is a nominal temperature difference (18°F = 10°C),
+
+T\(_{brine,in}\) is the tank brine inlet temperature,
+
+T\(_{brine,out}\) is the tank brine outlet temperature,
+
+T\(_{freeze}\) is the freezing temperature of water or the latent energy storage material,
+
+P\(_{c}\) is the fraction charged, and
+
+P\(_{d}\) is the fraction discharged.
+
+Likewise, the charging process of the ice storage device can be characterized by the following equation that is similar in form to the discharging equation:
+
+\begin{equation}
+{q^*} = \left[ {C1 + C2\left( {{P_c}} \right) + C3{{\left( {{P_c}} \right)}^2}} \right] + \left[ {C4 + C5\left( {{P_c}} \right) + C6{{\left( {{P_c}} \right)}^2}} \right]\Delta T_{lm}^*
+\end{equation}
+
+Note that the time step might differ from the time step used within the EnergyPlus simulation.~ These are actually two separate time steps and are kept separate.
+
+\subsubsection{Charging Algorithm}\label{charging-algorithm}
+
+During charging, manufacturers have stated that they attempt to charge the unit at the maximum rate until the unit is completely charged.~ This, of course, occurs during off-peak electric hours.~ Thus, once the setpoint has been scheduled for charging, the unit will charge at the maximum possible rate.~ This means that the flow rate through the ice storage device equals the flow to the component (or no bypass).~ The only time flow to the ice storage unit would be reduced is at the end of the charge cycle when more ice making capacity is available in a particular time step than is needed to fully charge the tank.~ In this case, the flow to the tank would be reduced appropriately to top off the tank storage capacity. ~We also have a setpoint goal for the outlet temperature of the ice storage device as defined by the setpoint schedule.
+
+In solving the performance of the ice storage unit, we have effectively two equations (one of which is non-linear) and two unknowns.~ The equations are:
+
+\begin{equation}
+{q^*} = \left[ {C1 + C2\left( {{P_c}} \right) + C3{{\left( {{P_c}} \right)}^2}} \right] + \left[ {C4 + C5\left( {{P_c}} \right) + C6{{\left( {{P_c}} \right)}^2}} \right]\Delta T_{lm}^*
+\end{equation}
+
+from which we can obtain the component load (q) and
+
+\begin{equation}
+q = \dot m{C_p}\left( {{T_i} - {T_o}} \right)
+\end{equation}
+
+Both of these equations have q and T\(_{o}\) as unknowns.~ However, since the setpoint temperature is the goal for T\(_{o}\), we can use this as an initial guess for T\(_{o}\).~ Below is an outline of the algorithm:
+
+n~Initialize T\(_{o}\) = T\(_{set}\)
+
+n~Calculate LMTD*
+
+n~Calculate q* from charging equation for the current percent charged (We will assume that the EnergyPlus time step is sufficiently small so that we do not need to find the average percent charged for the time step.~ This was necessary when one hour time steps were used as in BLAST, but EnergyPlus generally uses relatively short time steps.~ Since there is already some iteration involved in the solution, we would like to avoid another layer of iteration if at all possible.~ One alternative that could be implemented would be to make a second pass with a closer average value based on what happens during the time step.~ This would effectively double the execution time for the model and would need to be justified before implementation.)
+
+n~Calculate T\(_{o,new}\) and compare it to T\(_{o}\)
+
+n~Use T\(_{o,new}\) to calculate a new LMTD* and iterate until T\(_{o}\) converges to some acceptable level
+
+Charging would continue in subsequent time steps until the final state of the ice storage unit at the end of a particular time step is fully charged.~ If running a chiller would ``overcharge'' the tank, then the flow to the tank would be reduced (greater than zero bypass flow) while maintaining the same setpoint temperature coming out of the tank (though not necessarily out of the component).
+
+\subsubsection{Discharging Algorithm}\label{discharging-algorithm}
+
+During discharging, we cannot assume that all of the flow is sent through the ice storage unit and thus some of it may be bypassed around it locally.~ This ice storage model includes a built-in bypass leg to accommodate this without requiring the user to enter this additional information.~ This also allows the bypass leg/valve to be controlled by the ice storage unit.
+
+While we cannot assume that all of the flow is sent through the ice storage unit, we can use that as an initial guess in order to determine the current performance of the ice storage system.~ Most of the discharging algorithm then becomes very similar to the charging process.
+
+In solving the performance of the ice storage unit, we have effectively two equations (one of which is non-linear) and two unknowns.~ The equations are:
+
+\begin{equation}
+{q^*} = \left[ {C1 + C2\left( {{P_d}} \right) + C3{{\left( {{P_d}} \right)}^2}} \right] + \left[ {C4 + C5\left( {{P_d}} \right) + C6{{\left( {{P_d}} \right)}^2}} \right]\Delta T_{lm}^*
+\end{equation}
+
+from which we can obtain the component load (q) and
+
+\begin{equation}
+q = \dot m{C_p}\left( {{T_i} - {T_o}} \right)
+\end{equation}
+
+Both of these equations have q and T\(_{o}\) as unknowns.~ However, since the setpoint temperature is the goal for T\(_{o}\), we can use this as an initial guess for T\(_{o}\).~ Below is an outline of the algorithm:
+
+n~Initialize T\(_{o}\) = T\(_{set}\)
+
+n~Calculate LMTD*
+
+n~Calculate q* from charging equation for the current percent charged (we will assume that the EnergyPlus time step is sufficiently small so that we do not need to find the average percent charged for the time step; this was necessary when one hour time steps were used as in BLAST, but EnergyPlus generally uses relatively short time steps)
+
+n~Calculate T\(_{o,new}\) and compare it to T\(_{o}\)
+
+n~Use T\(_{o,new}\) to calculate a new LMTD* and iterate until T\(_{o}\) converges to some acceptable level
+
+n~Once T\(_{o}\) has converged, we need to compare this value again to T\(_{set}\).~ If T\(_{o}\) is greater than or equal to T\(_{set}\), then we either just met the load (equal) or can't quite meet it (greater than).~ In this case, we simply leave T\(_{o}\) as is because we cannot meet the setpoint temperature.
+
+n~If T\(_{o}\) is less than T\(_{set}\), then we have more capacity available than we need.~ In this case, we need to bypass some of the flow.~ Since the load on the ice storage device and the outlet temperature are not changing (we are just reducing the flow), we only need to split the flow and do not need to recalculate the action of the ice storage device.~ Some systems may be slightly dependent on the actual flow through the device itself.~ However, in an actual application, this only means that a slightly different amount will bypass the device.~ The overall energy impact will be the same and thus it is not necessary to be concerned about flow rate dependence.
+
+Discharging would continue in subsequent time steps until the final state of the ice storage unit at the end of a particular time step is fully discharged.
+
+\subsubsection{References}\label{references-1-011}
+
+Strand, R.K. 1992. ``Indirect Ice Storage System Simulation,'' M.S. Thesis, Department of Mechanical and Industrial Engineering, University of Illinois at Urbana-Champaign.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/ideal-loads-air-system.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/ideal-loads-air-system.tex
new file mode 100644
index 00000000000..1f7587770f8
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/ideal-loads-air-system.tex
@@ -0,0 +1,157 @@
+\section{Ideal Loads Air System }\label{ideal-loads-air-system}
+
+\subsection{Overview}\label{overview-021}
+
+The input object ZoneHVAC:IdealLoadsAirSystem provides a model for an ideal HVAC system. It occupies a place in the program hierarchy corresponding to a zone HVAC unit. It is not connected to a central air system -- instead each ZoneHVAC:IdealLoadsAirSystem object supplies cooling or heating air to a zone in sufficient quantity to meet the zone load or up to its limits, if specified. The supply air conditions are controlled based on specifications in the ZoneHVAC:IdealLoadsAirSystem input. The system has options for humidity control, outdoor air, economizer, demand controlled ventilation, and heat recovery.
+
+\subsection{Model}\label{model-002}
+
+The ZoneHVAC:IdealLoadsAirSystem object is modeled as an ideal VAV terminal unit with variable supply temperature and humidity. The supply air flow rate is varied between zero and the maximum in order to satisfy the zone heating or cooling load, zone humidity controls, outdoor air requirements, and other constraints, if specified.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-002}
+
+The user specifies some or all of the following data for each ZoneHVAC:IdealLoadsAirSystem object:
+
+·~~~~~~~~name of unit availability schedule
+
+·~~~~~~~~name of the zone inlet node;
+
+·~~~~~~~~name of the zone exhaust node;
+
+·~~~~~~~~maximum supply air temperature when in heating mode \emph{T\(_{max,heating}\)} {[}C{]};
+
+·~~~~~~~~minimum supply air temperature when in cooling mode \emph{T\(_{min,cooling}\)} {[}C{]};
+
+·~~~~~~~~maximum supply air humidity ratio when in heating mode \emph{W\(_{max,humid}\)} {[}kg water/kg dry air{]};
+
+·~~~~~~~~minimum supply air humidity ratio when in cooling mode \emph{W\(_{min,dehum}\)} {[}kg water/kg dry air{]};
+
+·~~~~~~~~heating limit type flag (\emph{LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity} or \emph{NoLimit}) \emph{HeatingLimit};
+
+·~~~~~~~~maximum heating air flow rate~ {[}m\(^{3}\)/s{]}
+
+·~~~~~~~~maximum sensible heating capacity~ {[}W{]}
+
+·~~~~~~~~cooling limit type flag (\emph{LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity} or \emph{NoLimit}) \emph{CoolingLimit}
+
+·~~~~~~~~maximum cooling air flow rate~ {[}m\(^{3}\)/s{]}
+
+·~~~~~~~~maximum total cooling capacity~ {[}W{]}
+
+·~~~~~~~~name of heating availability schedule
+
+·~~~~~~~~name of cooling availability schedule
+
+·~~~~~~~~dehumidification control type flag (\emph{ConstantSensibleHeatRatio, Humidistat, None,} or \emph{ConstantSupplyHumidityRatio}) \emph{DehumidCtrlType}
+
+·~~~~~~~~cooling sensible heat ratio
+
+·~~~~~~~~humidification control type flag (\emph{Humidistat, None,} or \emph{ConstantSupplyHumidityRatio}) \emph{HumidCtrlType}
+
+·~~~~~~~~name of a DesignSpecification:OutdoorAir object
+
+·~~~~~~~~outdoor air inlet node name
+
+·~~~~~~~~demand controlled ventilation control type flag (\emph{None, OccupancySchedule or CO2Setpoint})
+
+·~~~~~~~~outdoor air economizer type flag (\emph{NoEconomizer, DifferentialDryBulb, or DifferentialEnthalpy})
+
+·~~~~~~~~heat recovery type flag (\emph{None, Sensible, or Enthalpy})
+
+·~~~~~~~~sensible heat recovery effectiveness
+
+·~~~~~~~~latent heat recovery effectiveness
+
+\subsubsection{All input data for the ZoneHVAC:IdealLoadsAirSystem is stored in the array PurchAir. The model and data are encapsulated in the module PurchasedAirManager.Calculation}\label{all-input-data-for-the-zonehvacidealloadsairsystem-is-stored-in-the-array-purchair.-the-model-and-data-are-encapsulated-in-the-module-purchasedairmanager.calculation}
+
+·~~~~~~~~Set the unit on/off flag \emph{UnitOn}.
+
+The unit is off (\emph{UnitOn} = \emph{False}) if the unit availability schedule value is \textless{} = 0; otherwise the unit is on (\emph{UnitOn} = \emph{True}). If the unit is on, the calculation proceeds through the remaining steps. If the unit is off, the zone inlet node conditions are set to the zone node condition, the inlet node mass flow rate is set to zero, and the unit outputs are set to zero.
+
+·~~~~~~~~Calculate the minimum outdoor air mass flow rate based on the specifications in the DesignSpecification:OutdoorAir object, if specified.
+
+·~~~~~~~~Calculate the sensible and latent impact of the outdoor air flow relative to the zone conditions
+
+·~~~~~~~~Determine if the unit needs to heat or cool
+
+o~~~If outdoor air sensible impact is \textgreater{} = load to zone cooling setpoint and the current thermostat type is not SingleHeatingSetPoint, then unit is in cooling mode
+
+o~~~If outdoor air sensible impact is \textless{} load to zone heating setpoint then unit is in heating mode
+
+o~~~Else if neither condition is true, then unit is in deadband mode (provides outdoor air but shuts off economizer and heat recovery and all humidity control options except \emph{Humidistat} option)
+
+·~~~~~~~~If in cooling mode, simulate outdoor air economizer and adjust outdoor air mass flow rate
+
+·~~~~~~~~Calculate supply air mass flow rate
+
+o~~~If outdoor air flow rate exceeds applicable maximum flow rate (heating or cooling) then reduce outdoor air mass flow rate, issue warning, and set supply air mass flow rate equal to outdoor air mass flow rate
+
+Else
+
+o~~~Calculate supply air mass flow rate required to meet zone sensible load at the applicable (heating or cooling) supply temperature limit (\emph{T\(_{max,heating}\)} or \emph{T\(_{min,cooling}\)})
+
+\begin{equation}
+{\dot m_s} = {\dot Q_z}/({c_{p,air}}\cdot ({T_s} - {T_z}))
+\end{equation}
+
+o~~~If \emph{DehumidCtrlType} = Humidistat (and other conditions are met, see below), then calculate the supply air mass flow rate required to meet the humidistat dehumidification setpoint at \emph{W\(_{min,dehum}\)}
+
+o~~~If \emph{HumidCtrlType} = Humidistat (and other conditions are met, see below), then calculate the supply air mass flow rate required to meet the humidistat humidification setpoint at \emph{W\(_{max,humid}\)}
+
+o~~~Set the supply air mass flow rate to the greatest of these, but limit to the applicable (heating or cooling) maximum flow rate
+
+·~~~~~~~~Calculate the mixed air conditions, modeling heat recovery, if applicable
+
+o~~~The recirculation air conditions are set equal to the zone return air node conditions; if there is no return air node the recirculation air conditions are set equal to the conditions at the zone node.
+
+o~~~The unit entering conditions are then:
+
+If \({\dot m_s}\) \textgreater{} \({\dot m_{oa}}\) ~then
+
+\begin{equation}
+{h_{ma}} = ({\dot m_{oa}} \cdot {h_{oa}} + ({\dot m_s} - {\dot m_{oa}}) \cdot {h_{recirc}})/{\dot m_s}
+\end{equation}
+
+\begin{equation}
+{W_{ma}} = ({\dot m_{oa}} \cdot {W_{oa}} + ({\dot m_s} - {\dot m_{oa}}) \cdot {W_{recirc}})/{\dot m_s}
+\end{equation}
+
+\begin{equation}
+{T_{ma}} = {\mathop{\rm PsyHFnTdbW}\nolimits} ({h_{ma}},{W_{ma}})
+\end{equation}
+
+Otherwise the entering air conditions are set equal to the outside air conditions.
+
+·~~~~~~~~Calculate the supply air temperature required to meet the zone sensible load at the supply air mass flow rate, but limit to the applicable (heating or cooling) supply temperature limit (\emph{T\(_{max,heating}\)} or \emph{T\(_{min,cooling}\)})
+
+\begin{equation}
+{T_s} = {T_z} + {\dot Q_z}/({c_{p,air}}\cdot {\dot m_s})
+\end{equation}
+
+·~~~~~~~~Calculate the supply humidity ratio based on the specified humidity control types, but limit to the applicable (heating or cooling) supply humidity ratio limit
+
+o~~~\emph{DehumidCtrlType = None} sets the supply air humidity ratio equal to the mixed air humidity ratio.
+
+o~~~\emph{DehumidCtrlType = Humidistat,} this will actively dehumidify to the humidistat dehumidification setpoint during cooling and deadband operation, and during heating operation if \emph{HumidCtrlType = Humidistat}
+
+o~~~\emph{DehumidCtrlType = ConstantSensibleHeatRatio} sets the supply air humidity ratio using the cooling sensible heat ratio.
+
+o~~~\emph{DehumidCtrlType = ConstantSupplyHumidityRatio} sets the supply air humidity ratio = \emph{W\(_{min,dehum}\)}.
+
+o~~~\emph{HumidCtrlType = None} sets the supply air humidity ratio equal to the mixed air humidity ratio.
+
+o~~~\emph{HumidCtrlType = Humidistat,} this will actively humidify to the humidistat humidifying setpoint during heating and deadband operation, and during cooling operation if \emph{DehumidCtrlType = Humidistat}
+
+o~~~\emph{HumidCtrlType = ConstantSupplyHumidityRatio} sets the supply air humidity ratio = \emph{W\(_{max,humid}\)}.
+
+·~~~~~~~~Limit supply humidity ratio to saturation at the supply temperature
+
+·~~~~~~~~Check the applicable capacity limits (sensible heating and total cooling) and adjust supply air temperature and humidity if needed.
+
+·~~~~~~~~Set the zone inlet node conditions to the supply air mass flow rate, temperature, and humidity ratio.
+
+·~~~~~~~~Calculate the unit output and load components.
+
+\subsection{References}\label{references-029}
+
+No specific references.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/indoor-swimming-pool.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/indoor-swimming-pool.tex
new file mode 100644
index 00000000000..e150a8ef25f
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/indoor-swimming-pool.tex
@@ -0,0 +1,305 @@
+\section{Indoor Swimming Pool }\label{indoor-swimming-pool}
+
+The modeling of the indoor swimming pool is integrated into the surface heat balance procedures already in EnergyPlus with special modifications for radiation between the pool water surface and the surrounding of the space, convection to the surrounding air, evaporation of water, conduction to the pool bottom, and solar radiation absorbed in the pool water, the pool heating system, the presence of a cover, etc. Effectively, the pool water mass is ``added'' to or lumped into the inside face of the surface to which the pool is ``linked''. Conduction through the floor uses the standard CTF formulation, however the heat balance is modified to include other terms specific to the pool water.
+
+Some assumptions of the model are given below, followed by more details of individual components of the model.
+
+\begin{itemize}
+\tightlist
+\item
+  The pool water is lumped together at the inside face of a surface and follows the standard EnergyPlus heat balance methodology with some modifications based on the pool model details described in this section.
+\item
+  The pool itself must reference a surface that is specifically defined as a floor and it covers the entire floor to which it is linked.
+\item
+  The pool cannot by part of a low temperature radiant system (meaning that the construction of the floor cannot have any embedded pipes for heating or cooling). In addition, the floor/pool cannot be defined with any movable insulation or be defined as a ventilated slab.
+\item
+  The pool/floor surface must use the standard CTF solution algorithm.
+\item
+  The pool may be covered and the fraction covered is defined by user input. This value may vary from 0.0 to 1.0.
+\item
+  The pool cover has an impact on evaporation, convection, short-wavelength radiation, and long-wavelength radiation. Each of these has a separate user input that reduces the heat transfer parameter from the maximum achieved with a cover. While the cover percentage is allowed to vary via a user schedule input, each individual parameter for these four heat transfer modes is a fixed constant. For evaporation and convection, the factors simply reduce the amount of heat transfer proportionally. For the radiation terms, the factors reduce the amount of radiation that impacts the surface (pool) directly. The remaining radiation is assumed to be convected off of the pool cover to the zone air.
+\item
+  Pool water heating is achieved by defining the pool as a component on the demand side of a plant loop.
+\item
+  Makeup water replaces any evaporation of water from the pool surface and the user has control over the temperature of the makeup water.
+\item
+  The pool is controlled to a particular temperature defined by user input.
+\item
+  Evaporation of water from the pool is added to the zone moisture balance and affects the zone humidity ratio.
+\item
+  The pool depth is small in comparison to its surface area. Thus, heat transfer through the pool walls is neglected. This is in keeping with the standard assumption of one-dimensional heat transfer through surfaces in EnergyPlus.
+\end{itemize}
+
+\subsection{Energy Balance of Indoor Swimming Pool}\label{energy-balance-of-indoor-swimming-pool}
+
+Heat losses from indoor swimming pools occur by a variety of mechanisms. Sensible heat transfer by convection, latent heat loss associated with evaporation, and net radiative heat exchange with the surrounding occur at the pool surface. Conductive heat losses take place through the bottom of the pool. Other heat gains/losses are associated with the pool water heating system, the replacement of evaporated water with makeup water The energy balance of the indoor swimming pool estimates the heat gains/losses occurring due to:
+
+\begin{itemize}
+\tightlist
+\item
+  convection from the pool water surface
+\item
+  evaporation from the pool water surface
+\item
+  radiation from the pool water surface
+\item
+  conduction to bottom of pool
+\item
+  fresh pool water supply
+\item
+  pool water heating by the plant
+\item
+  changes in the pool water temperature
+\end{itemize}
+
+Detailed methods for estimating these heat losses and gains of the indoor swimming pools are described in the subsections below.
+
+\subsection{Convection from the pool water surface}\label{convection-from-the-pool-water-surface}
+
+The convection between the pool water and the zone are defined using:
+
+\begin{equation}
+Q_{conv} = h \cdot A \cdot (T_p – T_a)
+\end{equation}
+
+\begin{equation}
+h = 0.22 \cdot (T_p – T_a)1/3
+\end{equation}
+
+where
+
+\(Q_{conv}\) = Convective heat transfer rate (Btu/h·ft2)
+
+\(h\) = Convection heat transfer coefficient (Btu/h· ft2·�F)
+
+\(T_p\) = Pool water temperature (�F)
+
+\(T_a\) = Air temperature over pool (�F)
+
+When a cover is present, the cover and the cover convection factor reduce the heat transfer coefficient proportionally. For example, if the pool is half covered and the pool cover reduces convection by 50\%, the convective heat transfer coefficient is reduced by 25\% from the value calculated using the above equation.
+
+\subsection{Evaporation from the pool water surface}\label{evaporation-from-the-pool-water-surface}
+
+There are 5 main variables used to calculate the evaporation rate (\(Q_{evap}\)):
+
+\begin{itemize}
+\tightlist
+\item
+  Pool water surface area
+\item
+  Pool water temperature
+\item
+  Room air temperature
+\item
+  Room air relative humidity
+\item
+  Pool water agitation and Activity Factor
+\end{itemize}
+
+\begin{equation}
+\dot{m}_{evap} = 0.1 \cdot A \cdot AF \cdot (P_w – P_{dp})
+\end{equation}
+
+where
+
+\(\dot{m}_{evap}\) = Evaporation Rate of pool water (lb/h)
+
+\(A\) = Surface area of pool water (ft²)
+
+\(AF\) = Activity factor
+
+\(P_w\) = Saturation vapor pressure at surface of pool water (in. Hg)
+
+\(P_{dp}\) = Partial vapor pressure at room air dew point (in. Hg)
+
+Typical Activity Factor (AF)
+
+\begin{longtable}[c]{@{}lll@{}}
+\toprule 
+Type of Pool & Air Temperature, �C & Water Temperature, �C \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Type of Pool & Air Temperature, �C & Water Temperature, �C \tabularnewline
+\midrule
+\endhead
+
+Recreational & 24-30 & 24-30 \tabularnewline
+Physical Therapy & 26-30 & 30-32 \tabularnewline
+Competition & 26-29 & 24-28 \tabularnewline
+Diving & 27-29 & 27-32 \tabularnewline
+Elderly Swimmers & 29-32 & 29-32 \tabularnewline
+Hotel & 28-29 & 28-30 \tabularnewline
+Whirlpool / Spa & 27-29 & 36-40 \tabularnewline
+\bottomrule
+\end{longtable}
+
+When a cover is present, the cover and the cover evaporation factor reduce the amount of evaporation proportionally. For example, if the pool is half covered and the pool cover reduces convection by 50\%, the convective heat transfer coefficient is reduced by 25\% from the value calculated using the above equation. The value is converted to a latent gain (loss) through multiplication of the evaporation rate by the heat of vaporization of water.
+
+\subsection{Radiation exchange with the pool water surface}\label{radiation-exchange-with-the-pool-water-surface}
+
+This uses the EnergyPlus internal short- and long-wavelength radiation balances already in place. When a cover is present, it acts to reduce the amount of radiation that arrives at the pool water surface in comparison to the no cover case. Any reduction in either type of radiation is accounted for by adding a convective gain/loss to the zone air. So, in effect, the cover absorbs some radiation and then convects it to the zone air.
+
+\subsection{Conduction through the bottom of the pool}\label{conduction-through-the-bottom-of-the-pool}
+
+The model ignores 2-d effects of pool walls and assume that pool depth is much less than the pool area. Conduction is calculated using the Conduction Transfer Function (CTF) equation with the outside temperature determined by the outside heat balance and the inside surface temperature calculated using the pool water heat balance that is lumped together with the inside surface heat balance.
+
+\subsection{Makeup pool water supply}\label{makeup-pool-water-supply}
+
+\begin{equation}
+Q_{fw} = m_{fw} \cdot cw \cdot (T_p – T_{fw})
+\end{equation}
+
+where
+
+\(m_{fw}\) = Mass flow rate
+
+\(c_w\) = Specific heat of water
+
+\(T_p\) = Pool water temperature
+
+\(T_{fw}\) = Fresh water supply temperature
+
+\subsection{Heat Gain from People}\label{heat-gain-from-people}
+
+The input for the swimming pool requires that the user enter the maximum number of people in the pool, a schedule modifying the maximum number of people for different pool occupancies, and a heat gain per person schedule for differing activities. These three parameters allow for the calculation of a total heat gain from () ̇during a given time. It is assumed that all of the heat gain from people is via convection to the pool water.
+
+\subsection{Heat from auxiliary pool heater}\label{heat-from-auxiliary-pool-heater}
+
+\begin{equation}
+Q_{fw} = m_{hw} \cdot c_w \cdot (T_p – T_{hw})
+\end{equation}
+
+where
+
+\(m_{hw}\) = Mass flow rate (lb·s)
+
+\(c_w\) = Specific heat of water (Btu/lb·�F)
+
+\(T_p\) = Pool water temperature (�F)
+
+\(T_{hw}\) = Heated water supply temperature (�F)
+
+\subsection{Pool Heating to Control the Pool Water Temperature}\label{pool-heating-to-control-the-pool-water-temperature}
+
+The equation used to determine the flow rate request of hot water from the plant is an extremely simplified version of the pool heat balance. This is because the mass of the pool is so much larger than any of the other heat flows. As a result, for the sake of establishing a heated water flow rate, the following equation is used:
+
+\begin{equation}
+\frac{m_w c_p}{\Delta t} (T_{set}-T_{old}) = \dot{m}_p \cdot c_p \cdot (T_{in} - T_{set} )
+\end{equation}
+
+where
+
+\(m_w\) = mass of pool water
+
+\(cp\) = specific heat of water
+
+\(\Delta t\) = time step length
+
+\(T_{set}\) = desired pool water temperature
+
+\(T_{old}\) = temperature of water at the last time step
+
+\(m_p\) = needed mass flow rate of water from the plant
+
+\(T_{in}\) = inlet water temperature from the plant
+
+This equation is rearranged to solve for the needed mass flow rate of water from the plant since all of the other terms are known or given based on user input. This establishes a flow request to the plant and is capped at the maximum value defined in input by the user.
+
+\subsection{Pool/Surface Heat Balance Equation Summary}\label{poolsurface-heat-balance-equation-summary}
+
+The following equation is the basis for the pool/surface heat balance. As has been mentioned previously, the pool water is ``merged'' with the inside surface heat balance which is essentially the same thing as lumping the entire water of the pool in the inside surface heat balance.
+
+\begin{equation}
+\frac{m_w \cdot c_p}{\Delta t} (T_{set} - T_{old}) = Q_{cond} + Q_{conv} + Q_{lwrad} + Q_{swrad} + Q_{damp} + Q_{muw} + Q_{heater} + Q_{evap}
+\end{equation}
+
+where
+
+\(\frac{m_w \cdot c_p}{\Delta t} (T_{set} - T_{old} )\) = the change in energy stored in the pool water
+
+\(Q_{cond}\) = net conduction to/from the pool water to the floor
+
+\(Q_{conv}\) = net convection between the pool water and the zone air
+
+\(Q_{lwrad}\) = net long-wavelength radiation between the pool water/floor and the surrounding surfaces as well as from internal heat gains
+
+\(Q_{swrad}\) = net short-wavelength radiation to the pool water/floor from solar and internal heat gains
+
+\(Q_{damp}\) = standard damping term used in the inside heat balance to avoid large swings in the radiation balance that sometimes cause instability in the solution (see the standard heat balance information for more details)
+
+\(Q_{muw}\) = net gain/loss from replacing water evaporated from the pool with makeup water
+
+\(Q_{heater}\) = net heat added to the pool via the plant loop (controlled to maintain a setpoint temperature as described above)
+
+\(Q_{evap}\) = net heat loss due to evaporation of pool water to the zone air
+
+Details on each of these terms was either provided in previous parts of this section or in the standard EnergyPlus heat balance discussion elsewhere in the Engineering Reference.
+
+\subsection{Other additional information}\label{other-additional-information}
+
+The following subsections are some useful information that those wishing to model a swimming pool in EnergyPlus might find helpful. Further information can be found on-line or in reputable sources such as the ASHRAE Handbooks.
+
+\subsection{Swimming Pool Flow Rate}\label{swimming-pool-flow-rate}
+
+The flow rate of the circulating pump is designed to turn over (circulate) the entire volume of water in the pool in 6 to 8 hours, or 3 or 4 times in 24 hours. About 1 or 2 percent of the pumped circulation rate should be provided as continuous makeup water demand to overcome losses from evaporation, bleed-off, and spillage. To fill the pool initially, a separate quick-fill line should be provided to do the job in 8 to 16 hours; however, filling is usually done at off-peak hours. Thus, the demand flow rate need not be considered in the system demand calculations, unless it out-weighs the demand of all other demands even during the off-peak hours.
+
+\subsection{Comfort and Health}\label{comfort-and-health}
+
+Indoor pools are normally maintained between 50 and 60\% RH for two reasons:
+
+\begin{itemize}
+\tightlist
+\item
+  Swimmers leaving the water feel chilly at lower relative humidity due to evaporation off the body
+\item
+  It is considerably more expensive (and unnecessary) to maintain 40\% RH instead of 50\% RH
+\end{itemize}
+
+\subsection{Air Delivery Rates (Indoor Pool)}\label{air-delivery-rates-indoor-pool}
+
+Most codes require a minimum of 6 ACH, except where mechanical cooling is used. This rate may prove inadequate for some occupancy and use. Where mechanical dehumidification is provided, air delivery rates should be established to maintain appropriate conditions of temperature and humidity. The following rates are typically desired:
+
+\begin{itemize}
+\tightlist
+\item
+  Pools with no spectator areas, 4 \textasciitilde{} 6 ACH
+\item
+  Spectator areas, 6 \textasciitilde{} 8 ACH
+\item
+  Therapeutic pools, 4 \textasciitilde{} 6 ACH
+\end{itemize}
+
+Typical Swimming Pool Design Conditions
+
+\begin{longtable}[c]{@{}lll@{}}
+\toprule 
+Type of Pool & Air Temperature, �C & Water Temperature, �C \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Type of Pool & Air Temperature, �C & Water Temperature, �C \tabularnewline
+\midrule
+\endhead
+
+Recreational & 24-30 & 24-30 \tabularnewline
+Physical Therapy & 26-30 & 30-32 \tabularnewline
+Competition & 26-29 & 24-28 \tabularnewline
+Diving & 27-29 & 27-32 \tabularnewline
+Elderly Swimmers & 29-32 & 29-32 \tabularnewline
+Hotel & 28-29 & 28-30 \tabularnewline
+Whirlpool / Spa & 27-29 & 36-40 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{References}\label{references-030}
+
+ASHRAE (2011). 2011 ASHRAE Handbook -- HVAC Applications. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc., p.5.6-5.9.
+
+Janis, R. and W. Tao (2005). Mechanical and Electrical Systems in Buildings. 3rd ed. Upper Saddle River, NJ: Pearson Education, Inc., p.246.
+
+Kittler, R. (1989). Indoor Natatorium Design and Energy Recycling. ASHRAE Transactions 95(1), p.521-526.
+
+Smith, C., R. Jones, and G. Löf (1993). Energy Requirements and Potential Savings for Heated Indoor Swimming Pools. ASHRAE Transactions 99(2), p.864-874.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/pipes.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/pipes.tex
new file mode 100644
index 00000000000..33048d796b6
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/pipes.tex
@@ -0,0 +1,263 @@
+\section{Pipes }\label{pipes}
+
+\subsection{Heat Transfer Pipes (Objects: Pipe:Indoor \& Pipe:Outdoor)}\label{heat-transfer-pipes-objects-pipeindoor-pipeoutdoor}
+
+\subsubsection{Heat Loss and Time Delay in Pipes}\label{heat-loss-and-time-delay-in-pipes}
+
+The effects of heat loss and time delay in plant loop pipes exposed to air (Pipe:Indoor and Pipe:Outdoor) can be modeled explicitly in EnergyPlus. Users can select the environment with which the pipe transfers heat. Currently users have three options: `OutdoorAir', `Zone' and `Schedule'. Simulation for each of the environments is similar except the way in which the heat transfer between the pipe outer wall and the surrounding environment is calculated. When using the `OutdoorAir' option, the current outdoor dry-bulb temperature and wind velocity from the weather file (or design day input) are used. When the environment is specified as `Zone', the mean air temperature and room air velocity of the corresponding zone are used.
+
+In the case of a pipe in a zone, the heat loss or gain is accounted for in the pipe heat transfer calculation and is also included in the zone air heat balance calculations. When the environment is specified as `Schedule', the user specifies a temperature and velocity schedule which will be used to calculate the heat transfer.
+
+Pipe heat transfer in EnergyPlus is simulated by discretizing the pipe length into a number of nodes (20) and is an implementation of the model by Hanby et al. (2002). A control volume drawn around a node in the pipe is shown in Figure~\ref{fig:control-volume-drawn-around-node-i}. Three nodes are defined at each discrete section of the pipe and represent the fluid, pipe wall and external environment. The fluid and pipe have defined thermal capacitance (mass). The insulation around the pipe is currently modeled as steady-state (no thermal mass), and so the effect of this resistance is accounted for within the h\(_{f}\) term in the following description.~ For the fluid, there is one-dimensional flow from each upstream node.
+
+\begin{figure}[hbtp] % fig 261
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5831.png}
+\caption{Control Volume drawn around node *i* \protect \label{fig:control-volume-drawn-around-node-i}}
+\end{figure}
+
+The model is formulated from the heat balances on the fluid and wall nodes.
+
+\begin{equation}
+{M_{f,i}}{C_{P,f}}\frac{{d{T_{f,i}}}}{{dt}} = \dot m{C_{P,f}}\left( {{T_{f,i - 1}} - {T_{f,i}}} \right) - {h_f}{A_i}\left( {{T_{f,i}} - {T_{w,i}}} \right)
+\end{equation}
+
+\begin{equation}
+{M_{w,i}}{C_{P,w}}\frac{{d{T_{w,i}}}}{{dt}} = {h_f}{A_i}\left( {{T_{f,i}} - {T_{w,i}}} \right) - {h_e}{A_i}\left( {{T_{w,i}} - {T_e}} \right)
+\end{equation}
+
+Where, subscript \emph{w}, \emph{f} and \emph{e} denote the values for pipe wall, fluid and environment respectively. The current node is represented by a subscript of \emph{i}, while the previous node is represented by \emph{i-1}.
+
+\(M\) ~ = Mass
+
+\({C_p}\) ~ = Specific Heat
+
+\(\dot m\) ~ = Mass flow rate of fluid in pipe
+
+\(T\) ~ = Temperature
+
+\(A\) ~ = ~ Heat Transfer Area
+
+\(h\) ~ = Film convective resistance
+
+\(t\) ~~ = time
+
+The exterior film convective resistance is calculated based on either wind speed, room air velocity, or a scheduled value based on the type of pipe heat transfer object. However, when the velocity gets too low, natural convection must be modeled. This is handled within the program by having a lower limit on the Nusselt number. For natural convection from a horizontal cylinder, a constant Nusselt number is assumed based on information from Spang (referenced below). This Nusselt number is 0.36. The Nusselt number used in calculating the exterior convection coefficient (Incropera and Dewitt 1996) is the maximum of the Nusselt number from the forced convection coefficient correlation and this natural convection Nusselt number (0.36).
+
+In addition, the exterior resistance from the pipe wall inner surface to the environment will include resistance values for the pipe wall itself and any insulation specified around the pipe. This is treated as steady state value, so the simulation results are not affected by a change in insulation specific heat. However, the resistance is calculated based on thermal conductivity and thickness (using radial coordinate system), so the simulation results will vary with material conductivity changes. Again, this resistance is added in series with the exterior surface film convective resistance such that h\(_{f}\) contains film and insulation resistance.
+
+Approximating the derivatives using backward differencing enables these equations to be represented as simultaneous algebraic equations. For the fluid, at time step n, the heat balance is:
+
+\begin{equation}
+\frac{{{M_{f,i}}{C_{P,f}}}}{{\Delta t}}\left( {T_{f,i}^n - T_{f,i}^{n - 1}} \right) = \dot m{C_{P,f}}\left( {T_{f,i - 1}^n - T_{f,i}^n} \right) - {h_f}{A_i}\left( {T_{f,i}^n - T_{w,i}^n} \right)
+\end{equation}
+
+Rearranging gives,
+
+\begin{equation}
+T_{f,i}^n\left[ {{M_{f,i}}{C_{P,f}} + \dot m{C_{P,f}}\Delta t + {h_f}{A_i}\Delta t} \right] = \dot m{C_{P,f}}\Delta tT_{f,i - 1}^n + {h_f}{A_i}\Delta tT_{w,i}^n + {M_{f,i}}{C_{P,f}}T_{f,i}^{n - 1}
+\end{equation}
+
+or,
+
+\begin{equation}
+{a_1}T_{f,i}^n = {a_2}T_{f,i - 1}^n + {a_3}T_{w,i}^n + {a_4}T_{f,i}^{n - 1}
+\end{equation}
+
+where,
+
+\begin{equation}
+  \begin{array}{rl}
+    a_1 &= M_{f,i}C_{p,f} + \dot{m}C_{p,f} \Delta t + h_f A_i \Delta t \\
+    a_2 &= \dot{m} C_{p,f} \Delta t \\ 
+    a_3 &= h_f A_i \Delta t \\
+    a_4 &= M_{f,i} C_{p,f}
+  \end{array}
+\end{equation}
+
+Similarly, taking backwards differences for the conduit wall at time step n, the heat balance becomes,
+
+\begin{equation}
+\frac{{{M_{w,i}}{C_{P,w}}}}{{\Delta t}}\left( {T_{w,i}^n - T_{w,i}^{n - 1}} \right) = {h_f}{A_i}\left( {T_{f,i}^n - T_{w,i}^n} \right) - {h_e}{A_i}\left( {T_{w,i}^n - T_e^n} \right)
+\end{equation}
+
+Rearranging gives,
+
+\begin{equation}
+T_{w,i}^n\left[ {{M_{w,i}}{C_{P,w}} + {h_f}{A_i}\Delta t + {h_e}{A_i}\Delta t} \right] = {h_f}{A_i}\Delta tT_{f,i}^n + {h_e}{A_i}\Delta tT_e^n + {M_{w,i}}{C_{P,w}}T_{w,i}^{n - 1}
+\end{equation}
+
+or,
+
+\begin{equation}
+{b_1}T_{w,i}^n = {b_2}T_{f,i}^n + {b_3}T_{e,i}^n + {b_4}T_{w,i}^{n - 1}
+\end{equation}
+
+where,
+
+\begin{equation}
+  \begin{array}{rl}
+    b_1 &= M_{w,i} C_{p,w} + h_f A_i \Delta t + h_e A_i \Delta t \\
+    b_2 &= h_f A_i \Delta t \\
+    b_3 &= h_e A_o \Delta t \\
+    b_4 &= M_{w,i} C_{p,w}
+  \end{array}
+\end{equation}
+
+Substituting into gives an equation for the current fluid temperature:
+
+\begin{equation}
+{a_1}T_{f,i}^n = {a_2}T_{f,i - 1}^n + {a_3}\left( {{b_2}T_{f,i}^n + {b_3}T_{e,i}^n + {b_4}T_{w,i}^{n - 1}} \right)/{b_1} + {a_4}T_{f,i}^{n - 1}
+\end{equation}
+
+\begin{equation}
+T_{f,i}^n = \frac{1}{{\left( {{a_1} - {a_3}{b_2}/{b_1}} \right)}}\left[ {{a_2}T_{f,i - 1}^n + {a_3}\left( {{b_3}T_{e,i}^n + {b_4}T_{w,i}^{n - 1}} \right)/{b_1} + {a_4}T_{f,i}^{n - 1}} \right]
+\end{equation}
+
+The conduit is simulated by solving Eq. followed by Eq. for each of the twenty cells in the model and incrementing the time step. The fluid temperature of the last node is taken to be the pipe outlet temperature.
+
+\subsubsection{References}\label{references-036}
+
+Hanby, V.I., Wright, J.A., Fletcher, D.W and Jones, D.N.T. 2002. Modeling the Dynamic Response of Conduits. International Journal of HVACR\&R, Vol.8, No.1. pp.~1-12.
+
+Incropera, F.P. and Dewitt, D.P. 1996. Fundamentals of Heat Transfer, 4th Edition, pp.~369-370.
+
+Spang, Bernhard. Correlations for Convective Heat Transfer. Chemical Engineers' Resource Page:
+
+\subsection{Underground Pipe (Object: Pipe:Underground)}\label{underground-pipe-object-pipeunderground}
+
+\subsubsection{Description of Model}\label{description-of-model-000}
+
+The buried pipe model in EnergyPlus is similar to the other pipe heat transfer objects (i.e., Pipe:Indoor and Pipe:Outdoor) except for the way in which the pipe boundary condition is developed. For a buried pipe the ground between the pipe and the surface must be modeled. For a shallow buried pipe, the GroundHeatExchanger:Surface object may be used, which uses modified conduction transfer functions to model the ground. However, beyond a certain thickness, the transfer function method fails, and EnergyPlus will respond with a fatal error due to convergence problems. Therefore, when a pipe is buried deeper than about one meter, this new buried pipe model should be used. When the pipe is buried shallower than one meter, either model may be used. Due to the finite difference nature of the Pipe:Underground model, the GroundHeatExchanger:Surface may be slightly faster and therefore more desirable.
+
+The buried model develops a grid around the pipe. The grid was based originally on a model by Piechowski (1999), and still carries the model nomenclature. The grid extends from the ground surface down to a calculated distance below the pipe. The domain extends sideways from the symmetric center of the pipe to a calculated distance from the pipe. The grid stretches along the full length of the pipe. At each cross section, transient 2D Cartesian finite difference equations are used, updating each node except the node centered on the pipe. Axial heat transfer is not modeled in the soil. The large view of the outer Cartesian grid system is shown in Figure~\ref{fig:pipe-underground-outer-finite-difference-grid}.
+
+\begin{figure}[hbtp] % fig 262
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5851.png}
+\caption{Pipe:Underground Outer Finite Difference Grid \protect \label{fig:pipe-underground-outer-finite-difference-grid}}
+\end{figure}
+
+When the model encounters the pipe node, the existing model for Pipe:Interior and Pipe:Exterior pipes is used. The finite difference temperatures neighboring the pipe, grid spacing and soil properties are used to create an average boundary temperature for the pipe along with a conductance value. With a boundary temperature available and a conductance value mimicking the convection coefficient, the simulation continues exactly as with the other pipe heat transfer objects. To avoid redundancy, see the Pipe:Indoor or Pipe:Outdoor objects for a detailed description of the pipe model.
+
+\subsubsection{Boundary Conditions}\label{boundary-conditions-000}
+
+The boundary conditions for this model include a symmetric vertical boundary centered on the pipe, the ground surface, a `far-field', and a `deep ground'. The ground surface boundary uses current simulation outdoor dry-bulb temperature, and the user-entered convection coefficient. The `far-field' and `deep ground' temperatures come from the ``undisturbed'' ground temperature object specified in the input.
+
+Currently, the model is set up to be exposed to open soil above the pipe. If the user intends on simulating this buried pipe under a foundation slab, the effects can be approximating by use of the basement/slab heat transfer preprocessor program. This program takes in general building information, and performs a simulation which generates ground temperatures. Typically these effects are used to generate boundary conditions for the floor zone, but they may also be used in generating the ground surface temperatures for this pipe model. The data from the slab program will be monthly temperatures, so the user can use these as a surface ground temperature object which provides boundary data to the Pipe:Underground model.
+
+\subsubsection{Geometry}\label{geometry}
+
+The model develops the pipe depth and ground thickness from the user-entered construction information. The soil, pipe wall, and optional pipe insulation are entered as materials (with inherent thicknesses). The soil is entered as a standalone material, while the pipe insulation (if applicable) and the pipe wall should be given as a construction containing one or two materials. With knowledge of each individual thickness, the pipe geometry is obtained. The pipe length and inside diameter are the only additional geometry inputs.
+
+\subsubsection{Model Assumptions}\label{model-assumptions-000}
+
+\begin{itemize}
+\item
+  Constant properties throughout domain
+\item
+  Moisture is not directly involved with the model operation, so careful selection of soil thermal conductivity is a priority
+\item
+  Negligible axial heat transfer compared to radial heat transfer
+\item
+  Axisymmetric heat transfer in near pipe region
+\item
+  Surface convection coefficient is constant throughout simulation (does not vary with wind speed)
+\end{itemize}
+
+\subsubsection{References}\label{references-1-015}
+
+Kusuda, T. \& Achenbach, P. 1965. `Earth Temperature and Thermal Diffusivity at Selected Stations in the United States', ASHRAE Transactions Vol. 71, Part 1, pp.~61--75.
+
+Piechowski, M. 1999. `Heat and Mass Transfer Model of a Ground Heat Exchanger: Theoretical Development', Energy Research 23 (7), pp.~571--588.
+
+\subsection{PipingSystem:Underground Simulation}\label{pipingsystemunderground-simulation}
+
+In order to simulate diverse underground piping systems, a generalized model has been implemented which allows placement of pipes in a solid medium (soil).~ The model simulates circuiting effects of multiple pipes by allowing fluid to flow in the pipes in different directions.~ The model also has the capability of simulating interaction with zone surfaces to account for things such as basement heat transfer in a foundation heat exchanger.~ Different aspects of the modelling approach are described in this section which can assist the user in determining if this model is appropriate for a particular application, and determining input parameter values.
+
+An alternative interface is implemented which provides a simpler set of inputs for simulating horizontal trench heat exchangers.~ The key limitations of the simpler inputs include all piping in the domain being on a single circuit, all trenches equidistance apart, and each trench with the same burial depth.~ If this is satisfactory for an application, the GroundHeatExchanger:HorizontalTrench object is a suitable object.~ The object uses the same underlying simulation algorithms and data structures as the detailed piping system model, but with a simpler set of input parameters.~ For other cases and more detailed studies, the PipingSystem:Underground:* objects provide full flexibility.
+
+A dual-coordinate system finite volume heat transfer model of pipes buried in a conducting medium is employed.~ The dual-coordinate system consists of a coarse Cartesian system in the conducting region (the soil, for example) with a refined radial system in the near-pipe region.~ The pipes are connected as objects on the plant loop and are simulated as needed during loop convergence, while the ground itself is only simulated once per system time step.
+
+\subsubsection{Approach:}\label{approach-002}
+
+\subsubsection{General Development and Solution Scheme}\label{general-development-and-solution-scheme}
+
+A new heat transfer model is implemented to handle a diverse set of buried pipe conditions.~ The model uses a dual-coordinate system approach to solve a finite volume domain in a computationally efficient manner.~ The main idea behind the dual coordinate system technique is to focus the computational effort to the region where it is most needed: near the pipe(s).~ To this end, a coarse grid Cartesian coordinate system is used to solve the slow-moving ground heat transfer.~ Then, within one of these cells, a radial coordinate system is configured around the pipe/insulation with a specialized interface cell between the systems.~ Figure~\ref{fig:radial-near-pipe-cell-within-a-cartesian-cell} shows an example of cells surrounding a pipe, including the radial region in the near-pipe cell, while Figure~\ref{fig:close-up-view-of-example-radial-cell} shows a zoomed-in view of the near-pipe cell itself.
+
+\begin{figure}[hbtp] % fig 263
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5852.png}
+\caption{Radial "near-pipe" cell within a Cartesian cell \protect \label{fig:radial-near-pipe-cell-within-a-cartesian-cell}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 264
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5853.png}
+\caption{Close-up view of example radial cell \protect \label{fig:close-up-view-of-example-radial-cell}}
+\end{figure}
+
+The ground heat transfer model can be set up in a fully-3D or quasi-3D manner.~ In either case, there is a three-dimensional grid of Cartesian cells placed in the domain.~ In fully-3D mode, the axial heat transfer is accounted for; in quasi-3D mode, the axial effects are ignored and the result is essentially a set of 2D slices along the length of the domain.~ The determination of which method will be utilized in the final model shall be based upon final testing and on a balance between accuracy vs.~computation time.~ This option could be left to the end-user, but this will likely be unnecessary input overhead.
+
+A fully implicit (and thus numerically stable) formulation is used to describe all cells, which means an iteration loop must be implemented.~ In this solver, an outer iteration loop is used to bring the entire domain to convergence, while an inner iteration loop is used over all the radial cells.~ This is intended to focus the computational effort even further.~ The outer region may converge within one or two iterations, while the ``near-pipe'' cells may take much more iteration.~ For this reason, it does not make sense to iterate over the entire domain a large number of times.
+
+\subsubsection{Boundary Conditions}\label{boundary-conditions-1}
+
+The farfield boundary condition is defined by a Kusuda and Achenbach (1965) correlation, which requires annual ground surface temperature data.~ As with the current Pipe:Underground model, the user will be able to enter the correlation parameters directly, or information from the monthly ground temperature input object will be used to infer the parameters.
+
+The ground surface boundary condition is defined by an energy balance between the surrounding interior cells and the ground surface, including convection and radiation.~ As with the Pipe:Underground object, the ground surface sun exposure may be an optional input to allow for a shaded ground surface.~ In addition to the standard conduction, convection, and both short- and long-wave solar radiation at the surface, the ground surface boundary condition also includes the effects of evapotranspiration in the surface vegetation---the heat loss due to evaporation from soil to plant surface, and transpiration internal to the plant itself.~ The evapotranspiration rate is calculated as a moisture loss by using the Walter et al. (2005) model, and translated into a heat loss by multiplication with the density and latent heat of evaporation of water.~ The evapotranspiration rate is dependent on the type of vegetation at the surface; the user can vary the surface vegetation from anywhere between a concrete surface and a fairly tall grass (about 7'').
+
+Based on the application, an adiabatic boundary condition will also be implemented and employed on particular surfaces of the domain.~ For the case where a basement or under-slab region is present, for example, an adiabatic boundary will represent the vertical line of symmetry.
+
+\subsubsection{\texorpdfstring{``Pipe Cell'' Simulation}{Pipe Cell Simulation}}\label{pipe-cell-simulation}
+
+The ground is discretized into coarse Cartesian cells, some of which will contain a pipe.~ These ``pipe-cells'' are further discretized into a radial system with a specialized interface cell to couple these systems.~ The radial cells consist of a number of ground cells, with an optional insulation cell, then the pipe cell, followed by the fluid itself.
+
+The fluid is modeled as a cylindrical cell interacting with incoming fluid and heat transfer to the pipe.~ When there is no flow in the system, the cell essentially becomes radially adiabatic so that the fluid temperature will float during off periods.~ It will not be equal to ground temperatures, unless it is off for a long time and the transient heat is allowed to dissipate.~ When there is flow in the system, the incoming fluid and heat transfer from the pipe wall balance with the mass of the cell to come up with a new fluid temperature for that cell, to be passed downstream to the next cell.
+
+The fluid within the cells is modeled directionally, so that the flow can be circuited through multiple pipe segments in different directions.~ The flow direction in each pipe is specified by a choice field input.
+
+\subsubsection{Basement Interaction}\label{basement-interaction}
+
+The model can also interact with basement surfaces.~ The interaction is split into two sections: floor surfaces and wall surfaces.~ For each of these, the analysis is lumped, i.e., all walls are treated as one average wall surface and all floors are treated as one average floor surface.~ The distance that the basement impinges within the domain is defined by a simple width and height specification.~ The domain is then \emph{cutaway} for that region.~ Note that these distances then refer to the exterior surface of the wall or floor.
+
+The ground heat transfer model does not perform any transient simulation of the basement surfaces.~ The transient condition through these surfaces are left to the appropriate surface heat balance algorithms.~ Instead, this model interacts directly at the outer boundary through the use of an \emph{OtherSideConditions} model.~ The ground heat transfer model will take the current exterior surface heat flux and use that as the boundary for neighboring cells.~ Once convergence is achieved, the ground model will then effectively apply a constant surface temperature boundary condition by using a very high value of convection coefficient.~ The surface heat balance algorithms will then pick this up during the next zone time step.
+
+\subsubsection{Mesh Development}\label{mesh-development}
+
+The mesh is developed by using a few simple parameters.~ There are two distinct categories, the large-scale Cartesian mesh and the near-pipe refined radial mesh.
+
+\begin{itemize}
+\item
+  X, Y, Z mesh
+\item
+  Mesh Layout
+\item
+  Cell density
+\item
+  Radial mesh
+\item
+  Radial mesh thickness
+\item
+  Cell count
+\end{itemize}
+
+The Cartesian mesh uses a cell density parameter to define the number of cells to use in the simulation.~ Instead of requiring a detailed specification of all cell regions in the domain, this one parameter is used to specify a mesh density and is applied to all domain regions.~ The cell density parameter represents the number of cells within any two domain partitions.~ A domain partition is a basement wall or a pipe placed in the domain.~ Once these partitions are all laid out and validated, the regions between them are populated with the number of cells specified in the cell density parameter.~ Although this may lead to a variation of cell size within the domain, it is assumed that this will help focus computational intensity in the domain. ~Of course, the number of cells (cell density parameter) can be different for each of the X, Y, and Z directions to allow for further fine tuning of the domain.
+
+The Cartesian mesh is laid out in either a uniform or symmetric-geometric fashion.~ In the former, the cells between any two domain partitions are equally sized.~ In the latter, the cells are smaller near the partitions to again help fine-tuning computational intensity.~ If the latter is selected, the amount of non-uniformity is specified by an additional parameter.
+
+The radial coordinate system is always uniform for the soil cells, The two parameters to be specified for this region are the cell count (the number of soil cells to be generated outside of the pipe cell), and the radial mesh thickness (the radial distance from pipe outer wall to the cell boundary).~ Each soil cell will then have a radial thickness equal to the radial mesh thickness divided by the cell count.
+
+\subsubsection{Simulation Methodology}\label{simulation-methodology-001}
+
+The actual simulation of this model is performed in two parts: the ground simulation and the pipe cell simulation.
+
+Since the ground is likely to be slow-moving and easily converging, it is simulated once per system time step.~ This will simulate all the cells in the domain which do not contain a pipe segment.~ The boundary conditions for this step are then the current surface conditions and farfield model along with the previous values for pipe cell temperature.~ This small lag should provide suitable accuracy as the system time step will usually be smaller than the time constant of the pipe cell.~ This decoupling leverages the core of the model development by again placing computational effort where it is needed most, near the pipes.
+
+The ground simulation is performed once per time step, but the pipe cell simulation is performed at each call to the component.~ Each pipe will be placed on a plant loop, but not necessarily on the same plant loop or loop side.~ Thus, at each call to the object, that pipe will use the temperatures of the ground cells near the pipe as boundary conditions to simulate the ``near-pipe'' radial cells and fluid cell.~ In this manner, the pipes will simulate numerous times following the convergence flow of the plant loop system.
+
+\subsubsection{References}\label{references-2-007}
+
+Kusuda, T. \& Achenbach, P. 1965. `Earth Temperature and Thermal Diffusivity at Selected Stations in the United States', ASHRAE Transactions Vol. 71, Part 1, pp.~61--75.
+
+Allen, R.G., Walter, I.A., Elliott, R.L., Howell, T.A., Itenfisu, D., Jensen, M.E., Snyder, R.L. 2005. The ASCE standardized reference evapotranspiration equation. Reston, VA:American Society of Civil Engineers. 59 p.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/plant-temperature-source-component.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/plant-temperature-source-component.tex
new file mode 100644
index 00000000000..25145a2c973
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/plant-temperature-source-component.tex
@@ -0,0 +1,11 @@
+\section{Plant Temperature Source Component }\label{plant-temperature-source-component}
+
+This component (Object: PlantComponent:TemperatureSource) is a simple object used to simulate systems with a known supply temperature.~ This could include a river, well, or other configuration where a known temperature is pumped back into the plant system.~ This fluid could be isolated from chilled water and other loops by using a heat exchanger connection between the loops.
+
+The temperature of the source of this object can be either constant or scheduled.~ If scheduled, it could also be actuated by EMS to allow a calculated temperature at run-time.
+
+The logic of this component is quite simple: if there is flow through the component, the outlet temperature is always the source temperature.~ The component requests flow from the design flow rate, which can be autosized.
+
+\subsubsection{References}\label{references-038}
+
+No specific references. 
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/pumps.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/pumps.tex
new file mode 100644
index 00000000000..4dde087e877
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/pumps.tex
@@ -0,0 +1,216 @@
+\section{Pumps }\label{pumps}
+
+The water pump is quite simply the component that drives the flow in plant and condenser loops. How it reacts depends on several different conditions. In total, there are three different decision variables, two of which are defined by user input. These three deciding factors are whether the pump is constant or variable speed, whether the pump operation is continuous or intermittent, and whether or not there is a load on the loop. The pump is simulated first on the supply side loop after the demand side loop has determined what the demand on the loop will be. For further reference look at sections Pump Control for Plant and Condenser Loops, Plant/Condenser Supply Side, and Plant/Condenser Demand Side in the Plant Flow Resolver of this document.
+
+\subsection{Summary of Pump Rules}\label{summary-of-pump-rules}
+
+\begin{itemize}
+\item
+  Pumps in Plant Loop can be on the supply side or demand side
+\item
+  A Pump, if present, in the demand side of plant loop must be the first component of the inlet branch.
+\item
+  Pumps in Condenser loop must be on supply side
+\item
+  Pumps can operate as constant or variable flow.
+\item
+  Pumps can run continuously or intermittently.
+\item
+  Single boiler/chiller with NO bypass, use Pump:ConstantSpeed
+\item
+  Boiler/chiller should be constant flow
+\item
+  Pump should be intermittent
+\item
+  Single boiler/chiller with NO bypass, Pump:VariableSpeed
+\item
+  Boiler/chiller should be variable flow, regardless of whether pump is intermittent or continuous (runs at the minimum if demand is less than minimum, this includes zero.)
+\item
+  Single boiler/chiller with bypass, Pump:ConstantSpeed
+\item
+  Boiler/chiller can be constant or variable flow
+\item
+  Pump may be intermittent or continuous as long as the bypass can handle the entire pump volume when the boiler is not operating
+\end{itemize}
+
+Multiple branches add more complexity, but it is nothing more than continuity. If the pump is putting out flow then it has to have a branch to flow down whether it is a chiller or a bypass. It can be safer to add the bypass for a simulation. If the active machines require the flow the bypass will be dry. If performing a pressure simulation, and the flow goes through a machine which is off, the pressure drop will be accounted for, but no heat transfer through the machine will be calculated.
+
+If the user designates a pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop. If the pump is scheduled, the schedule modifies the Rated Volumetric Flow Rate of the pump on a time basis. The default is that the pump is ON and runs according to its other operational requirements.
+
+Shown below is the calculation of the total efficiency of the pump and the actual pumping efficiency when the motor efficiency is accounted for either the variable or constant volume pumps.
+
+!~ Total\_Efficiency \% = Rated\_Volume\_Flow\_Rate * Rated\_Pump\_Head / Rated\_Power\_Use
+
+~TotalEffic = ~~ PumpEquip(PumpNum)\%NomVolFlowRate *
+
+~~~~~~~~~~~~~~~~~~ PumpEquip(PumpNum)\%NomPumpHead /
+
+~~~~~~~~~~~~~~~~~~~~ PumpEquip(PumpNum)\%NomPowerUse
+
+!~~~~ Calculated Pump\_Efficiency \% = Total\_Efficiency \% / Motor\_Efficiency \%
+
+~~~~~ PumpEquip(PumpNum)\%PumpEffic = ~ TotalEffic /
+
+~~~~~~~~~~~~~~~~~~ PumpEquip(PumpNum)\%MotorEffic
+
+\subsection{Dynamic Pump Pressure Head}\label{dynamic-pump-pressure-head}
+
+There is an option when performing plant/condenser loop simulations to account for dynamically changing loop pressure drop. For the current implementation, the loop pressure drop is calculated based on pressure drop data on each branch of the loop, then this total pressure drop is set as the pump pressure head. There is no pump curve implemented yet, so it is assumed that the pump can always handle this pressure value. This is a first approximation to actually having the pump ride a curve, and this initial implementation allows the user to enter minimal data, and yet get a more dynamic output for pump power, which is calculated based on current pressure drop and flow rate. The equation for pump power is now:
+
+\begin{equation}
+Pump\;Electric\;Power = Pump\;Volume\;Flow\;Rate*\frac{{Pump\;Head}}{{Total\;Efficiency}}
+\end{equation}
+
+Without the pressure simulation, the pump power is based on the rated value entered with the pump object. For further information, see the input-output reference for Branch objects, and PlantLoop/CondenserLoop objects; as well as the Plant/Condenser loop section of this engineering reference.
+
+\subsection{Variable Speed Pump}\label{variable-speed-pump}
+
+A variable speed pump (object name: Pump:VariableSpeed) is defined with maximum and minimum flow rates that are the physical limits of the device. The pump will operate and select a flow somewhere between the minimum and maximum limits. In the case where the pump is running, the pump will try to meet the flow request made by demand side components.
+
+All of the pump rules and efficiency and power calculations are applicable from the introduction in the pump group section. The main difference between the the variable volume pump and the constant volume pump is the Part Load Performance Curve.The fraction of full load power is determined by the cubic equation:
+
+\begin{equation}
+FractionFullLoadPower = {C_1} + {C_2}PLR + {C_3}PL{R^2} + {C_4}PL{R^3}
+\end{equation}
+
+where C\(_{1}\),C\(_{2}\),C\(_{3}\),and C\(_{4}\) are Coefficients 1 -- 4 and PLR is the Part Load Ratio. In the pseudo code below the FracFullLoadPower modifies the NomPowerUse for the total pump ``Power'' and shows the ``ShaftPower'' and the ``PumpHeattoFluid''.
+
+VolFlowRate = PumpMassFlowRate / LoopDensity
+
+~ PartLoadRatio = VolFlowRate / PumpEquip(PumpNum)\%NomVolFlowRate
+
+~ FracFullLoadPower = ~~ PumpEquip(PumpNum)\%PartLoadCoef(1)~~~~~~~~~~~~~~~~~~~~ \&
+
+~~~~~~~~~~~~~~~~~~~~~ + PumpEquip(PumpNum)\%PartLoadCoef(2) * PartLoadRatio~~~~ \&
+
+~~~~~~~~~~~~~~~~~~~~~ + PumpEquip(PumpNum)\%PartLoadCoef(3) * PartLoadRatio**2~ \&
+
+~~~~~~~~~~~~~~~~~~~~~ + PumpEquip(PumpNum)\%PartLoadCoef(4) * PartLoadRatio**3
+
+~ Power = FracFullLoadPower * PumpEquip(PumpNum)\%NomPowerUse
+
+~ ShaftPower = Power * PumpEquip(PumpNum)\%MotorEffic
+
+! This adds the pump heat based on User input for the pump
+
+! We assume that all of the heat ends up in the fluid eventually since this is a closed loop
+
+!~ PumpHeattoFluid = ShaftPower*(1-PumpEquip(PumpNum)\%PumpEffic)~ \&
+
+~ PumpHeattoFluid = ShaftPower + (Power - ShaftPower)*PumpEquip(PumpNum)\%FracMotorLossToFluid
+
+~ Node(OutletNode)\%Temp = Node(InletNode)\%Temp+PumpHeattoFluid/(PumpMassFlowRate * LoopCp)
+
+~ PumpEquip(PumpNum)\%Power = Power
+
+\subsection{Pressure-based Flow for Variable Speed Pumps}\label{pressure-based-flow-for-variable-speed-pumps}
+
+With the introduction of pressure simulations in plant loops, the variable speed pump object now has the capability to model a more realistic variable speed operation. There are two operation modes which are introduced: differential pressure control is a widely used VFD control method while most VFDs also have a manual control mode in which the user determines the input frequency of the electric motor. The mode can be selected as `ManualControl' or `PressureSetpointControl' in the VFD Control Type input in Pump:VariableSpeed objects.
+
+In manual VFD control mode the specified schedule will determine the current pump rotational speed throughout the simulation. This RPM value will be used to scale the pump curve which is entered by the user in non-dimensional form. Once the pump curve has been fixed then the successive substitution method will use this curve with the system curve to resolve the operating point. VFD manual control mode is implemented in EnergyPlus with the use of the RPM schedule input.
+
+Differential pressure based control will maintain the differential pressure within the specified range. The pressure drop corresponding to the mass flow request will be calculated using the effective pressure constant of the system. This pressure drop will be checked against the pressure set point range. If the pressure drop is within the user specified range, then the mass flow rate will be checked against mass flow rates of operating points corresponding to maximum and minimum rotational speeds. Maximum and minimum differential pressure and rotational speeds are schedule inputs and can be entered as constant schedule.
+
+The allowable mass flow rate range for the Differential pressure control is explained in the figure below:
+
+\begin{figure}[hbtp] % fig 265
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5856.png}
+\caption{Allowable mass flow rate range for the Differential pressure control \protect \label{fig:allowable-mass-flow-rate-range-for}}
+\end{figure}
+
+\subsection{Constant Speed Pump}\label{constant-speed-pump}
+
+The operation of a constant speed pump (object name: Pump:ConstantSpeed) is fairly straightforward. The user designates a maximum flow rate and when this pumpo operates it will run at that capacity. The main difference between the constant speed pump and the variable speed pump is that the fraction of full load power is always = 1. In the pseudo code below the FracFullLoadPower is = 1.0, therefore the Power is always the full power.
+
+VolFlowRate = PumpMassFlowRate / LoopDensity
+
+~ PartLoadRatio = VolFlowRate / PumpEquip(PumpNum)\%NomVolFlowRate
+
+~ FracFullLoadPower = 1.0
+
+~ Power = FracFullLoadPower * PumpEquip(PumpNum)\%NomPowerUse
+
+~ ShaftPower = Power * PumpEquip(PumpNum)\%MotorEffic
+
+! This adds the pump heat based on User input for the pump
+
+! We assume that all of the heat ends up in the fluid eventually since this is a closed loop
+
+! ~PumpHeattoFluid = ShaftPower*(1-PumpEquip(PumpNum)\%PumpEffic)~ \&
+
+~ PumpHeattoFluid = ShaftPower + (Power - ShaftPower)*PumpEquip(PumpNum)\%FracMotorLossToFluid
+
+~ Node(OutletNode)\%Temp = Node(InletNode)\%Temp+PumpHeattoFluid/(PumpMassFlowRate * LoopCp)
+
+~ PumpEquip(PumpNum)\%Power = Power
+
+\subsection{Pressure-based Flow for Constant Speed Pumps}\label{pressure-based-flow-for-constant-speed-pumps}
+
+The constant speed pump can flow can also be overridden dynamically based on a response to the plant loop pressure drop. In ``single-loop-pump'' simulations (no branch pumps, no common pipe), the user can enter a dimensionless pump curve on the Pump:ConstantSpeed (see I/O ref) object which represents the single speed pressure-flow relationship of the pump. In the process of determining the operating flow rate for the pump, the pump will check to see if a valid pressure simulation is being performed. If it is, a flow will be prescribed based on a resolution between system pressure characteristics and the pump pressure curve. This will cause the pump flow to be ``unpredictable,'' meaning that it will not always be a constant, expected value, which is basically what the constant speed pump gives you without the pressure simulation. There is more detail on the pressure based simulation in the Plant/Condenser loop sections of this documentation.
+
+\subsection{Pump Heat Addition to the Loop}\label{pump-heat-addition-to-the-loop}
+
+Due to the fact that a pump is a mechanical device that acts on the fluid it is circulating, it causes the fluid to increase in temperature. The EnergyPlus model assumes that all pressure increase caused by the pump will eventually be lost due to friction, and that friction will be added as heat to the fluid. Since the plant and condenser loops are not yet true pressure-based models, EnergyPlus assumes that all of the heat resulting from the pump itself and from friction throughout the loop. Therefore, as of version 7, the pump heat is added to the plant loop interface by injecting the heat into the mixed tanks used to model loop thermal capacitance(previously it was added at the outlet node of the pump). The amount of heat added to the fluid is calculated using the following two equations:
+
+\begin{equation}
+ShaftPower = PumpPower * PumpMotorEfficiency
+\end{equation}
+
+\begin{equation}
+PumpHeatToFluid = ShaftPower + \left( {PumpPower - ShaftPower} \right) * FracMotorLossToFluid
+\end{equation}
+
+where the pump motor efficiency is defined by the user input and the FracMotorLossToFluid is the amount of heat generated by the pump motor that is added to the fluid loop (as opposed to being lost to the environment where the pump is located). FracMotorLossToFluid is also a user input.
+
+Note that the shaft power relates to the increase in head through the pump. Since all of this head is lost through the piping network due to frictional heat, this represents a heat gain by the fluid throughout the network. For simplicity, this heat is added along with the heat resulting from the pump motor. The difference between the pump power and the shaft power is the inefficiency of the pump---or the amount of energy input into the pump that the motor converts to heat rather than mechanical energy. Some of this heat is added to the fluid being pumped. These two terms are shown in the PumpHeatToFluid equation shown above. As of version 7, this heat is added to the loop capacitance tank(s) rather than at the pump's outlet and so the outlet temperatue is equal to the inlet temperaure.
+
+\subsection{Pump Heat Addition to Surrounding Zone}\label{pump-heat-addition-to-surrounding-zone}
+
+If the user input includes naming a Zone that surrounds the pump, then the pump becomes a source of internal heat gain to that zone.~ The amount of heat transmitted to the surrounding zone is simply the difference between power input and the rate of heat transferred to the fluid. The user can also input a fraction,\({f_{rad}}\) ~, that controls the overall split between thermal radiation and sensible convection.~ The pump's sensible zone gains are determined using the following equations:
+
+\begin{equation}
+TotalZoneGain = PumpPower - PumpHeatToFluid
+\end{equation}
+
+\begin{equation}
+ConvectiveZoneGain = \left( {1 - {f_{rad}}} \right)*TotalZoneGain
+\end{equation}
+
+\begin{equation}
+RadiativeZoneGain = {f_{rad}}*TotalZoneGain
+\end{equation}
+
+\subsection{Headered Pumps}\label{headered-pumps}
+
+The input objects HeaderedPumps:ConstantSpeed and HeaderedPumps:VariableSpeed ~provide models for headered pumps that consist of two or more pumps connected in parallel. The headered pump is simulated as a single component, and it is specified as an integer number of a specific pump. The flow rate provided by the headered pump is determined by the number of pumps in operation and the flow rate of the individual pump. The total flow rate is calculated as
+
+\begin{equation}
+FlowProvided = NumPumpsON*IndividualPumpFlowRate
+\end{equation}
+
+The simulation starts by turning ON all pumps in the group. The pumps are then turned OFF one at a time until the flow provided is less than the flow requested. Finally the last pump is turned back ON to meet the remaining flow (FlowDifference) requested. The flow rate of the last pump depends on the pump bank type. For constant speed headered pumps, the last pump runs at the nominal flow rate, thereby giving a final headered pump flow which is equal to or greater than the flow requested. In a variable speed headered pump the last pump runs at part load so that the flow provided matches the flow requested. The power of the headered pump is then calculated as
+
+\begin{equation}
+Power = (P{R_{FL}}{\rm{*N}}{}_{{\rm{FL}}} + {\rm{P}}{{\rm{R}}_{{\rm{PL}}}}{\rm{*}}{{\rm{N}}_{{\rm{PL}}}}{\rm{)*}}{{\rm{P}}_{{\rm{Nom}}}}{\rm{  }}
+\end{equation}
+
+Where;
+
+\emph{Power} = Power consumed by the pump bank
+
+\emph{PR\(_{FL}\)} = Power ratio at full load (Generally equal to 1)
+
+\emph{N\(_{FL}\)} = Number of pumps running at full load
+
+\emph{PR\(_{PL}\)} = Power ratio at part load
+
+\emph{N\(_{PL}\)} = Number of pumps running at part load
+
+\emph{P\(_{Nom}\)} = Nominal power consumption of individual pumps
+
+For a constant speed headered pump \emph{N\(_{PL}\)} is zero. For a variable speed headered pump \emph{N\(_{PL}\)} is equal to one.
+
+\subsection{Condensate Pumps}\label{condensate-pumps}
+
+The input object Pump:VariableSpeed:Condensate provides a model for steam condensate pumps, see the discussion for steam loops, reference: Condensate Pump.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/variable-refrigerant-flow-heat-pumps.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/variable-refrigerant-flow-heat-pumps.tex
new file mode 100644
index 00000000000..84deb48486a
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/variable-refrigerant-flow-heat-pumps.tex
@@ -0,0 +1,1019 @@
+\section{Variable Refrigerant Flow Heat Pumps }\label{variable-refrigerant-flow-heat-pumps}
+
+A Variable Refrigerant Flow (VRF, or Variable Refrigerant Volume) system is an air-conditioning system that varies the refrigerant flow rate using variable speed compressor(s) in the outdoor unit, and the electronic expansion valves (EEVs) located in each indoor unit. The system meets the space cooling or heating load requirements by maintaining the zone air temperature at the setpoint. The ability to control the refrigerant mass flow rate according to the cooling and/or heating load enables the use of as many as 60 or more indoor units with differing capacities in conjunction with one single outdoor unit. This unlocks the possibility of having individualized comfort control, simultaneous heating and cooling in different zones, and heat recovery from one zone to another. It may also lead to more efficient operations during part-load conditions.
+
+There are two common types of VRF systems.
+
+\begin{itemize}
+\item
+  Heat Pump (HP) type: the most general type that can be used for either cooling or heating, but not simultaneously.
+\item
+  Heat Recovery (HR) type: can deliver simultaneous heating and cooling to different zones by transferring heat between the cooling and heating indoor units. This generally occurs in the winter season in medium-sized to large-sized commercial buildings with a substantial core such as computer rooms.
+\end{itemize}
+
+There are two alternative VRF models availabe in EnergyPlus to simulate the energy performance of Variable Refrigerant Flow (VRF, or Variable Refrigerant Volume) air-conditioning systems:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  \textbf{System Curve based Model (VRF-SysCurve)}. In this model, a number of system level curves are used to describe the VRF system performance. It corresponds to the \emph{AirConditioner:VariableRefrigerantFlow} object.
+\item
+  \textbf{Physics based Model (VRF-FluidTCtrl)}. This model is able to consider the dynamics of more operational parameters and is applicable for fluid temperature control. This model corresponds to the \emph{AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl} object.
+\end{enumerate}
+
+\subsection{Variable Refrigerant Flow Heat Pump Model (System Curve Based Model)}\label{variable-refrigerant-flow-heat-pump-model-system-curve-based-model}
+
+\subsubsection{Overview}\label{overview-028}
+
+This section describes the System Curve based VRF Model (VRF-SysCurve), which can address both the heat pump and heat recovery operating modes and support air-, evaporatively-, or water-cooled condenser equipment ( throughout this section, the term ``condenser'' refers to the outdoor unit where the compressor is located. )
+
+The figure below schematically depicts the AirConditioner:VariableRefrigerantFlow (VRF AC) system. The outdoor unit is connected directly to the zone terminal units using a zone terminal unit list (ref: ZoneTerminalUnitList). The VRF AC system conditions multiple zones and is controlled by thermostats located in each zone. Zone terminal units operate to meet the zone sensible cooling or sensible heating requirements as determined by the zone thermostat schedule.
+
+When the heat pump does not operate to reclaim waste heat, the VRF AC system can only operate in either cooling \emph{or} heating mode. Based on the master thermostat priority control selection, the operating mode is determined by polling the appropriate zone(s) served by the VRF HP system. When the system is operating in cooling mode, the cooling coils will be enabled only in the terminal units where zone cooling is required. When the system is operating in heating mode, the heating coils will be enabled only in the terminal units where zone heating is required. Supply air fans will continue to operate if the zone terminal unit's fan operating mode is set to continuous fan.
+
+When the heat pump does operate to reclaim waste heat, the VRF AC system can simultaneously cool and heat multiple zones. The heat pump will select an operating mode according to the dominant load as reported by the zone thermostat(s). The calculation of the dominant load is based on the master thermostat priority control selection and may either be based on individual zone loads, the number of zones requiring cooling or heating, the master thermostat zone load, or an operating mode schedule. The heat pump will operate in cooling mode, and provide waste heat to zones with a heating load, when the dominant load among all zone terminal units is cooling. The heat pump will operate in heating mode, and absorb heat from zones with a cooling load, when the dominant load among all zone terminal units is heating.
+
+The figure below shows the VRF AC terminal units with draw through fan placement. Blow through fan placement can also be modeled by connecting the supply air fan inlet node to the outside air mixer's mixed air node if an outdoor air mixer is used or to the zone terminal unit inlet node if an outdoor air mixer is not used. The variable refrigerant flow heat pump coordinates the operation of these components and is modeled as a type of zone equipment where the \emph{zone terminal units} are specified in a zone equipment list (Ref. ZoneHVAC: EquipmentList and ZoneHVAC:EquipmentConnections). The AirConditioner: VariableRefrigerantFlow object \emph{is not} specified in an air primary loop or a zone equipment list object.
+
+\begin{figure}[hbtp] % fig 242
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5315.png}
+\caption{Variable Refrigerant Flow Heat Pump (draw through fan placement) \protect \label{fig:variable-refrigerant-flow-heat-pump-draw}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 243
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5316.png}
+\caption{Energyplus object connections for VRF-SysCurve model \protect \label{fig:energyplus-object-connections-for-vrf}}
+\end{figure}
+
+The terminal unit is able to model supply air fan operation in two modes: cycling fan -- cycling coil (i.e., AUTO fan) and continuous fan -- cycling coil (i.e., fan ON). Fan:Simple:OnOff must be used to model AUTO fan, while Fan:Simple:OnOff or Fan:Simple:ConstVolume can be used to model fan ON.
+
+Output variables reported by the VRF AC object include the heat pump's operating capacity (cooling or heating), electric consumption, operating COP, defrost electric consumption, part-load ratio (ratio of actual capacity to available capacity), runtime fraction (when cycling), cycling ratio (actual compressor cycling rate), crankcase heater power, and other report variables associated with an evaporative condenser. Report variables are also available to indicate the maximum available terminal unit cooling or heating capacity (i.e., when the condensers available capacity is insufficient to supply the capacity requested by all terminal units). Reporting of other variables of interest for the VRF AC (fan electric power, DX coil cooling rate, DX coil heating rate, terminal unit total cooling rate, etc.) is done by the individual system components (e.g., fan, DX cooling coil, DX heating coil, and zone terminal unit). For convenience, the total cooling and heating coil capacities (i.e., the coil loads) is also reported.
+
+\subsubsection{Model Description}\label{model-description-015}
+
+As described previously, the VRF AC system conditions multiple zones and is controlled by one or more zone thermostats (ZoneControl:Thermostatic). Each simulation time step, EnergyPlus performs a zone air heat balance to determine if cooling or heating is required to meet each zone's thermostat set point. When heat pump mode is selected (i.e., heat recovery is not selected), an operating mode is chosen based on the master thermostat priority control and all terminal units are operated in that specific mode. When heat recovery mode is selected, the dominant load is determined based on the master thermostat priority control and the outdoor unit operates in this mode. The indoor terminal units operate in either cooling or heating mode based on the individual coil loads The heat pump condenser is then modeled to determine any impact the condensing unit might have on the zone terminal units (i.e., capacity limitations due to oversized terminal units, operating limitations due to allowable operating temperature range, impacts of defrost operation, changes in performance when heat recovery mode is active, etc.). The following sections describe the performance calculations for cooling and heating.
+
+\subsubsection{Cooling Operation}\label{cooling-operation-000}
+
+The operating capacity of the heat pump is calculated based on the user defined input for the heat pump's rated cooling capacity, the ratio of indoor terminal unit capacity to outdoor unit capacity (combination ratio), the actual operating conditions, and whether or not the system's heat recovery mode is active. Performance correction factors are used to correct for off-design performance as follows:
+
+\subsubsection{Cooling Combination Ratio Correction Factor}\label{cooling-combination-ratio-correction-factor}
+
+The cooling combination ratio correction factor is defined as the total terminal unit rated cooling capacity divided by the heat pump's rated cooling capacity. The combination ratio is important when multiple terminal units (or DX coils) are attached to a single variable-speed condensing unit. If the combination ratio is less than 1, the condenser's rated capacity is assumed to be able to meet the indoor terminal unit's demand request. However, if the combination ratio is determined to be greater than 1, the maximum cooling capacity available from the heat pump's condenser may be higher than the user specified rated cooling capacity. The combination ratio capacity correction factor is based on a linear, quadratic or cubic curve and provides a multiplier \textgreater{} 1 to correct for combination ratio's greater than 1. For example, a combination ratio of 1.3 (130\%) may result in a combination ratio capacity correction factor of 1.06 (outdoor condenser can actually provide 106\% of rated capacity) . The cooling combination ratio correction factor is applied to cooling performance calculations. If the cooling combination ratio correction curve name is not specified by the user, the cooling combination ratio correction factor (CR \(_{cooling,\, correction}\)) in the following equation is assumed to be equal to 1.
+
+\begin{equation}
+  CR_{cooling,rated} = \frac{\sum \limits_1^n \dot{Q}_{coil(i),cooling,rated}}{\dot{Q}_{cooling,total,rated}}
+\end{equation}
+
+\begin{equation}
+C{R_{\,cooling\,,\,correction}} = a + b\left( {C{R_{cooling\,,\,rated}}} \right) + c{\left( {C{R_{cooling\,,\,rated}}} \right)^2} + d{\left( {C{R_{cooling\,,\,rated}}} \right)^3}
+\end{equation}
+
+\begin{equation}
+C{R_{\,cooling\,,\,correction}} = MAX\left( {1.0\,\,,\,\,C{R_{\,cooling\,,\,correction}}} \right)
+\end{equation}
+
+where
+
+\({\mathop Q\limits^ \bullet_{coil(i)\,,\,cooling\,,\,rated}}\) ~ = rated total (sensible + latent) cooling capacity in zone \emph{i} (W)
+
+\({\mathop Q\limits^ \bullet_{cooling,\,total\,,\,rated}}\) ~~ = rated total cooling capacity of heat pump (W)
+
+\(C{R_{\,cooling\,,\,correction}}\) ~ = Cooling Combination Ratio capacity correction factor at rated conditions (this value is reported in the eio file)
+
+\(a - d\) ~~~~~~~ ~~~~~~~ = equation coefficients for cooling combination ratio correction factor
+
+\(C{R_{cooling\,,\,rated}}\) ~~ ~~~ = the cooling combination ratio defined as the total indoor terminal unit's rated total cooling capacity divided by the rated total cooling capacity of the heat pump condenser.
+
+The sum of the individual zone total cooling requirements is used to calculate the performance of the outdoor condensing unit. The operating capacities of the indoor cooling coils are calculated based on the indoor cooling coil's rated cooling capacity and the actual operating conditions. The operating capacity of the heat pump condenser is calculated in a similar fashion using a load-weighted average indoor wet-bulb temperature of all operating cooling coils.
+
+\subsubsection{Cooling Capacity Ratio Modifier Function of Low Temperature}\label{cooling-capacity-ratio-modifier-function-of-low-temperature}
+
+The heat pump's cooling capacity correction factor (function of temperature) is determined by averaging the zone cooling coil inlet air wet-bulb temperature for all operating cooling coils. A load-weighted average inlet air wet-bulb temperature is used in the calculations. The weighted average cooling coil inlet air wet-bulb temperature and the outdoor condenser entering air dry-bulb temperature are then used to calculate the temperature correction factor in cooling mode for the heat pump condenser. The actual zone air wet-bulb temperature is used to calculate the operating capacity of the individual zone cooling coils.
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{zone,\,total}} = \sum\limits_1^i {{{\mathop Q\limits^ \bullet  }_{zone(i)}}}
+\end{equation}
+
+\begin{equation}
+  T_{wb,avg} = \sum\limits_1^i {\PB{T_{wb,i}}} \PB{\dot{Q}_{zone(i)}}{\dot{Q}_{zone,total}}
+\end{equation}
+
+The operating capacity of the heat pump is calculated using a bi-quadratic equation using a load-weighted average indoor wet-bulb temperature and outdoor dry-bulb temperature as the independent variables.
+
+\begin{equation}
+CAPF{T_{HP,cooling}} = a + b\left( {{T_{wb,avg}}} \right) + c{\left( {{T_{wb,avg}}} \right)^2} + d\left( {{T_c}} \right) + e{\left( {{T_c}} \right)^2} + f\left( {{T_{wb,avg}}} \right)\left( {{T_c}} \right)
+\end{equation}
+
+The operating capacity of the terminal unit's DX cooling coil is calculated using either a linear, quadratic, or cubic curve. If more information is available to more accurately model the DX cooling coil, a bi-quadratic curve may be used (i.e., if the performance of the DX cooling coil is also a function of outdoor dry-bulb temperature).
+
+\begin{equation}
+CAPF{T_{coil,\,cooling}} = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d{\left( {{T_{wb,i}}} \right)^3}
+\end{equation}
+
+~- or -
+
+\begin{equation}
+CAPF{T_{coil,cooling}} = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d\left( {{T_c}} \right) + e{\left( {{T_c}} \right)^2} + f\left( {{T_{wb,i}}} \right)\left( {{T_c}} \right)
+\end{equation}
+
+where
+
+\({T_{wb,i}}\) ~ = wet-bulb temperature of the air entering the cooling coil in zone \emph{i} (°C)
+
+\({T_{wb,avg}}\) = load-weighted average wet-bulb temperature of the air entering all operating cooling coils (°C)
+
+\({\mathop Q\limits^ \bullet_{zone(i)}}\) ~ = total (sensible + latent) cooling load in zone \emph{i} (W)
+
+\({\mathop Q\limits^ \bullet_{zone,\,total}}\) ~ = total (sensible + latent) cooling load in all zones (W)
+
+\(CAPF{T_{\,HP,cooling}}\) ~ = heat pump Cooling Capacity Ratio Modifier (function of temperature)
+
+\(CAPF{T_{\,coil,cooling}}\) ~ = zone coil Cooling Capacity Ratio Modifier (function of temperature)
+
+\(a - f\) ~ = equation coefficients for Cooling Capacity Ratio Modifier
+
+\({T_c}\) ~~~ = temperature of the air entering an air-cooled or evaporatively-cooled condenser (°C)
+
+\subsubsection{Using multiple curves to define Cooling Capacity Ratio Modifier}\label{using-multiple-curves-to-define-cooling-capacity-ratio-modifier}
+
+The cooling capacity ratio modifier determines the change in total (sensible + latent) capacity with respect to the heat pump rated cooling capacity. This modifier corrects for off-design performance and provides the operating total (sensible + latent) cooling capacity for the heat pump condenser. The performance data for VRF AC systems may be specified using a single curve object, however, if the performance data does not reflect a smooth change in performance as outdoor conditions vary, the overall performance of the system may be described using two cooling capacity ratio modifier curves (i.e., a separate curve at low and high outdoor temperatures) and a boundary curve (i.e., the curve defining the separation at specific outdoor temperatures).
+
+\subsubsection{Application of Dual Performance Curves}\label{application-of-dual-performance-curves}
+
+Two additional inputs are available to more accurately model the cooling performance of a VRF AC system. The first additional input is a boundary curve which is used to distinguish differences in performance at ``low'' and ``high'' outdoor temperature regions and the second input is a cooling capacity performance curve for the ``high'' outdoor temperature region. The boundary curve is a linear, quadratic or cubic curve defining the outdoor temperature as a function of average indoor wet-bulb temperature. The cooling capacity ratio function of high temperature curve is a biquadratic curve using average indoor wet-bulb temperature and outdoor dry-bulb temperature as the two independent variables. These additional curves are used to define the performance over two separate performance regions as shown in Figure 244. The red circles in the figure identify the points at which the performance changes abruptly (i.e., slopes or shapes are significantly different) and are used to create the boundary curve. The performance on either side of the boundary curve can be a smooth curve changing with outdoor condition or a flat plateau where system controls maintain a constant operating condition. This type of performance cannot be accurately simulated using a single performance curve object. For this reason, dual capacity performance curves may be used.
+
+Note: If the cooling performance can be described using a single performance curve object, the boundary and high temperature performance curve objects are not required.
+
+Manufacturers may also provide this information in a tabular format. In this case the data should first be graphically displayed to identify any non-linearities and to also identify where an abrupt change in performance occurs so that a boundary curve can be created.
+
+The cooling capacity ratio boundary curve object is used to differentiate between dual cooling capacity ratio performance curves. This curve defines the outdoor temperature below which the cooling capacity ratio function of low temperature curve object is used, otherwise, the cooling capacity ratio function of high temperature curve object is used.
+
+\begin{equation}
+{T_{OA,DB}} = a + b\left( {{T_{I,WB}}} \right) + c{\left( {{T_{I,WB}}} \right)^2} + d{\left( {{T_{I,WB}}} \right)^3}
+\end{equation}
+
+where
+
+T\(_{OA,DB}\) = Outside air dry-bulb temperature (C)
+
+a-d = coefficients for cooling capacity ratio boundary curve object
+
+T\(_{I,WB}\) = Weighted average indoor wet-bulb temperature (C)
+
+For the performance data shown below, the boundary curve would be created by identifying the outdoor dry-bulb temperature at which the performance changed abruptly for each of the indoor wet-bulb temperature curves shown in the figure. The following example shows the data interpreted from the figure used to regress the cooling capacity ratio boundary curve coefficients. For this example, the regression coefficients were found to be: A1 = 29.87396, B1 = -0.6928, C1 = 0.01928, D1 = -0.000532
+
+\begin{figure}[hbtp] % table 73
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5339.png}
+\caption{Performance Data for Variable Refrigerant Flow Air Conditioner Model \label{fig:performance-data-for-variable-refrigerant-flow-air-conditioner-model}}
+\end{figure}
+
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Find the \(rps\) range that covers the required evaporative capacity \(Q_{rps,modify}\) .
+\end{enumerate}
+
+\begin{equation}
+Q_{rps,modify} = C_{cap,operation}\times(\sum{Q_{in,total}}+Q_{pipe})
+\end{equation}
+
+\begin{equation}
+C_{cap,operation} = C_{cap,density}\times{C_{cap,enthalpy}}
+\end{equation}
+
+\begin{equation}
+C_{cap,density} = \rho_{test}/\rho_{real}
+\end{equation}
+
+\begin{equation}
+C_{cap,enthalpy} = \frac{h_{Evapout,test}-h_{Evapin,test}}{h_{Compin,real}-h_{Evapin,real}}
+\end{equation}
+
+\begin{equation}
+h_{Compin,real} = h_{Hexout,real}+Q_{pipe}/G_{tot}
+\end{equation}
+
+Where
+
+\(C_{cap,operation}\) evaporative capacity correction factor, describing the operational difference between test cases and real cases (i.e., \(SH\) and \(SC\) )
+
+\(C_{cap,density}\) evaporative capacity correction factor, describing the variations of refrigerant density at test conditions and real operational conditions
+
+\(C_{cap,enthalpy}\) evaporative capacity correction factor, describing the variations of refrigerant enthalpy at test conditions and real operational conditions
+
+\(G_{tot}\) refrigerant flow rate in the main loop (kg/s)
+
+\(h_{Evapin,real}\) enthalpy of refrigerant entering the evaporators (IU) at real conditions {[}kJ/kg{]}
+
+\(h_{Evapout,real}\) average enthalpy of refrigerant leaving the evaporators (IU) at real conditions {[}kJ/kg{]}
+
+\(h_{Evapin,test}\) enthalpy of refrigerant entering the evaporator at test conditions (It corresponds to \(SC\) at test condition(e.g., 5 °C) and Tc) (kJ/kg)
+
+\(h_{Evapout,test}\) enthalpy of refrigerant leaving the evaporator at test conditions (It corresponds to \(SH\) at test condition(e.g., 8 °C) and Te) (kJ/kg)
+
+\(h_{Compin}\) enthalpy of refrigerant entering the compressor (kJ/kg)
+
+\(Q_{pipe}\) heat loss through the pipe (W)
+
+For example, if the required capacity is 8 kW, the \(rps\) range is 30 to 36.
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\setcounter{enumi}{2}
+\item
+  Calculate the \(rps\) that meets the required capacity by interpolation. In the above example, the resulting \(rps\) is 34.5 \(rps\) .
+\item
+  If the calculated \(rps\) is lower than the minimum \(rps\) (e.g.~18\(rps\) ), go to Step 2c.5, otherwise skip Step 2c.5 and directly go to Step 2c. 6.
+\end{enumerate}
+
+\paragraph{Step 2c.5: Modify evaporating temperature to further reduce outdoor unit capacity}\label{step-2c.5-modify-evaporating-temperature-to-further-reduce-outdoor-unit-capacity}
+
+If the calculated \(rps\) is lower than the minimum \(rps\) (e.g.~18\(rps\) ), it means that the zone cooling load is even lower than the system evaporative capacity corresponding to the minimum compressor speed. In this situation, the evaporating temperature \(T_e\) as well as the superheating degree \(SH\) is modified to further reduce the outdoor unit capacity. More specifically:
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\item
+  Set \(rps\) at its minimum value (e.g., 18 \(rps\) ).
+\item
+  Update \({T_e}'\) to meet the required evaporative capacity, using equations described in Step 2c.4a.
+\item
+  Update \(T_e\) to meet the updated \({T_e}'\) . Note that due to the \(T_e\) updates, the refrigerant state and flow rate are changed and thus the piping loss analysis should also be repeated (Step 2c.1). So is the calculation of \(C_{cap,operation}\) (Step 2c.2-2c.3).
+\item
+  \(SH\) can be updated based on the updated \(T_e\) , using the equations shown in Step 1.2.
+\end{enumerate}
+
+\paragraph{Step 2c.6: Calculate the compressor power}\label{step-2c.6-calculate-the-compressor-power}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\tightlist
+\item
+  Calculate the compressor power by the following procedures. 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\tightlist
+\item
+  Calculate the compressor power at a variety of loading index using the following equation. The resulting table (Table 2) from the same example used above is shown below.
+\end{enumerate}
+
+\[M_{comp} = c_1+c_2T_c+c_3{T_e}'+c_4T_c^2+c_5T_c{T_e}'+c_6{T_e}'^2\] \[N_{comp,rps} = M_{comp} \times N_{comp,ref}\]
+
+Where
+
+\(c_1\) ,\ldots{},\(c_6\) empirical coefficients corresponding to \(rps\)
+
+\({T_e}'\) suction saturated temperature at the compressor inlet (°C)
+
+\(T_c\) effective condensing temperature (°C)
+
+\(M_{comp}\) multiplier for the compressor power calculation (--)
+
+\(N_{comp,ref}\) rated compressor power (W)
+
+\(N_{comp,rps}\) compressor power corresponding to \(rps\) (W)
+
+Table 2 -- Outdoor unit compressor power at different Loading Index
+
+
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  According to the \(rps\) range determined, calculate the compressor power \(N_{comp}\) by interpolation. In the above example, the compressor power is 1.155 kW. 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Compare the calculated \(N_{comp}\) above with the initialized \({N_{comp}}'\) in Step 2c.2:
+\end{enumerate}
+
+\begin{itemize}
+\item
+  If \({N_{comp}}'-N_{comp}>\delta\) then go to Step 2c.2 for a new round of iteration.
+\item
+  Else, end the iteration and go to Step 2c.7.
+\end{itemize}
+
+\paragraph{Step 2c.7: Total power consumption of the outdoor unit}\label{step-2c.7-total-power-consumption-of-the-outdoor-unit}
+
+Calculate the total electric power consumption by the outdoor unit:
+
+\begin{equation}
+N_{out} = N_{fan}+N_{comp}/e_{inv}
+\end{equation}
+
+Where
+
+\(e_{inv}\) efficiency of the inverter of compressor
+
+\(N_{fan}\) electric power consumption by the outdoor fan (W)
+
+\(N_{out}\) total electric power consumption by the outdoor unit (W)
+
+\subsubsection{\texorpdfstring{\emph{Modeling of the outdoor unit (O/U) - Heating Mode}}{Modeling of the outdoor unit (O/U) - Heating Mode}}\label{modeling-of-the-outdoor-unit-ou---heating-mode}
+
+\paragraph{Step 2h.1: Piping loss calculation in the heating mode}\label{step-2h.1-piping-loss-calculation-in-the-heating-mode}
+
+Similarly to that in the cooling mode, the piping loss analysis in the heating mode needs to address the coupling effect between the piping loss and system operations. However, due to the control strategy difference between the two modes, the piping loss algorithm in the heating mode requires different calculation steps and more numerical iterations, as shown below.
+
+Calculate the refrigerant flow rate for each indoor unit using assumed \(h_{Hexin}\) :
+
+\begin{equation}
+G_i = Q_i/(h_{Hexin}-h_{Hexout,i})
+\end{equation}
+
+Where
+
+\(G_i\) refrigerant flow rate for the i\(^{th}\) indoor unit (kg/s)
+
+\(Q_i\) total heating load of the i\(^{th}\) zone (W)
+
+\(h_{Hexin}\) enthalpy of the refrigerant entering the indoor unit (kJ/kg)
+
+\(h_{Hexout,i}\) enthalpy of the refrigerant leaving a specific indoor unit (kJ/kg)
+
+\(h_{Hexout,i}\) is a function of \(P_c\) , \(T_c\) , and \(SC_i\) . It can be calculated using refrigerant thermodynamic property equations \(f_{g_h}(P_c,T_c-SC_i)\) .
+
+The refrigerant flow rate in the main loop can be obtained by summing up the flow rate in each indoor unit:
+
+\begin{equation}
+G_{tot} = \sum{G_i}
+\end{equation}
+
+Where
+
+\(G_{tot}\) refrigerant flow rate in the main loop (kg/s)
+
+Calculate the average refrigerant pressure and enthalpy within the pipes, using assumed piping pressure loss \(\Delta{P_{pipe}}\) and \(h_{Tdi}\) :
+
+\begin{equation}
+P_{ave} = P_c+\Delta{P_{pipe}}/2
+\end{equation}
+
+\begin{equation}
+h_{ave} = (h_{Hexin}+h_{Tdi})/2
+\end{equation}
+
+Where
+
+\(h_{ave}\) average refrigerant enthalpy within the main pipe (kJ/kg)
+
+\(h_{Hexin}\) enthalpy of the refrigerant entering the indoor unit (kJ/kg)
+
+\(h_{Tdi}\) enthalpy of the refrigerant leaving the compressor (kJ/kg)
+
+\(P_{ave}\) average refrigerant pressure within the main pipe (Pa)
+
+\(P_c\) condensing pressure (Pa)
+
+\(\Delta{P_{pipe}}\) pressure drop in the main pipe (Pa)
+
+The viscosity of the refrigerant within the pipe can be calculated given \(P_{ave}\) and \(h_{ave}\) , using the following equations:
+
+\begin{equation}
+k_{v,1} = P_{ave}/4926000
+\end{equation}
+
+\begin{equation}
+k_{v,2} = h_{ave}/383.55
+\end{equation}
+
+\begin{equation}
+k_{v,3} = (T_{ave}+273.15)/344.39
+\end{equation}
+
+\begin{equation}
+\mu = 10^6\times(4.302\times{k_{v,1}}+0.81622\times{k_{v,1}}^2-120.98\times{k_{v,2}}+139.17\times{k_{v,2}}^2+118.76\times{k_{v,3}}+81.04\times{k_{v,3}}^2+5.7858\times{k_{v,1}}\times{k_{v,2}}-8.3817\times{k_{v,1}}\times{k_{v,3}}-218.48\times{k_{v,2}}\times{k_{v,3}}+21.58)
+\end{equation}
+
+Where
+
+\(\mu\) viscosity of the refrigerant within the pipe (Pa-s)
+
+\(k_{v,i}\) coefficients to calculate the refrigerant viscosity
+
+\(h_{ave}\) average refrigerant enthalpy within the pipes (kJ/kg)
+
+\(P_{ave}\) average refrigerant pressure within the pipes (Pa)
+
+\(T_{ave}\) average temperature of refrigerant leaving indoor units, which corresponds to \(P_{ave}\) and \(h_{ave}\) (°C)
+
+Given \(P_{ave}\) and \(h_{ave}\) , the following dimensionless quantities describing the refrigerant flow state can be obtained:
+
+\begin{equation}
+Re = G_{tot}/3600/(0.25\times\pi\times{D^2})\times{D}/\mu
+\end{equation}
+
+\begin{equation}
+Pr = \mu\times{f_{g_Cp}(P_{ave},h_{ave})}\times{0.001}/f_{g_\lambda}(P_{ave},h_{ave})
+\end{equation}
+
+\begin{equation}
+Nu = 0.023\times{Re^{0.8}\times{Pr^{0.4}}}
+\end{equation}
+
+\begin{equation}
+St = Nu/Re/Pr
+\end{equation}
+
+Where
+
+\(Re\) Reynolds number
+
+\(Pr\) Prandtl number
+
+\(Nu\) Nusselt number
+
+\(St\) Stanton number
+
+\(\mu\) viscosity of the refrigerant within the pipe (Pa-s)
+
+\(f_{g_Cp}\) functions calculating the specific heat of superheating refrigerant
+
+\(f_{g_\lambda}\) functions calculating the conductivity of superheating refrigerant
+
+Then the piping pressure loss \(\Delta{P_{pipe}}\) can be obtained using the above dimensionless quantities:
+
+\begin{equation}
+\Delta{P_{pipe}} = 8\times{St}\times{Pr^{2/3}}\times{L/D}\times{f_{g_\rho}(P_{ave},h_{ave})}\times{V^2}/2-H\times{f_{g_\rho}(P_{ave},h_{ave})}\times9.80665
+\end{equation}
+
+Where
+
+\(f_{g_\rho}\) functions calculating the density of superheating refrigerant
+
+\(D\) main pipe diameter (m)
+
+\(H\) height difference between the outdoor unit node and indoor unit node of the main pipe (m)
+
+\(L\) main pipe length (m)
+
+\(St\) Stanton number
+
+\(Re\) Reynolds number
+
+\(Pr\) Prandtl number
+
+\(\Delta{P_{pipe}}\) pressure drop in the pipe (Pa)
+
+\(V\) refrigerant flow velocity (m/s)
+
+Compare the calculated \(\Delta{P_{pipe}}\) and the one assumed above. If the difference is higher than the assigned tolerance (5\%), a new round of iteration is performed using the calculated \(\Delta{P_{pipe}}\) .
+
+The compressor discharge saturated temperature \(T'_c\) (i.e., saturated vapor temperature corresponding to compressor discharge pressure) can be obtained via:
+
+\begin{equation}
+T'_c = f_{s_t}(P_c+\Delta{P_{pipe}})
+\end{equation}
+
+Where
+
+\(f_{s_t}\) functions calculating the temperature of saturated refrigerant
+
+\(T'_c\) discharge saturated temperature at the compressor outlet (°C)
+
+\(P_c\) condensing pressure (Pa)
+
+\(\Delta{P_{pipe}}\) pressure drop in the pipe (Pa)
+
+The heat loss through the pipe can be obtained via:
+
+\begin{equation}
+k_1 = Nu\times{f_{g_\lambda}(P_{ave},h_{ave})}
+\end{equation}
+
+\begin{equation}
+k_2 = 2\times{\lambda_i}/Ln(1+2\times{W_i}/D)
+\end{equation}
+
+\begin{equation}
+k_3 = h\times(D+2\times{W_i})
+\end{equation}
+
+\begin{equation}
+Q_{pipe} = (\pi\times{L})\times(T_a-T_{Hexin})/(1/k_1+1/k_2+1/k_3)
+\end{equation}
+
+Where
+
+\(f_{g_\lambda}\) functions calculating the conductivity of superheating refrigerant
+
+\(Q_{pipe}\) heat loss through the pipe (W)
+
+\(T_a\) average of outdoor air temperature and indoor temperature (°C)
+
+\(T_{Hexin}\) average of entering indoor units (°C)
+
+\(w_i\) pipe insulation thickness (m)
+
+\(k_i\) coefficients for the piping loss calculation
+
+The enthalpy of the refrigerant entering the indoor unit can be updated using the calculated \(Q_{pipe}\) :
+
+\begin{equation}
+h_{Tdi} = h_{Hexin}+Q_{pipe}/G_{tot}
+\end{equation}
+
+Where
+
+\(h_{Hexin}\) enthalpy of the refrigerant entering the indoor unit (kJ/kg)
+
+\(h_{Tdi}\) enthalpy of the refrigerant leaving the compressor (kJ/kg)
+
+\(G_{tot}\) refrigerant flow rate in the main loop (kg/s)
+
+Compare the calculated \(h_{Tdi}\) and the one assumed above. If the difference is higher than the assigned tolerance (5\%), a new round of iteration is performed using the calculated \(h_{Tdi}\) .
+
+Note that \(Q_{pipe}\) is calculated using an assumed \(h_{Hexin}\) at the beginning of the piping loss algorithm. Its value affects the compressor operation calculations as shown in Step 2h.2\textasciitilde{}2h.6 and may change the value of evaporating temperature \(T_e\) . This leads to an updated \(h_{Hexin} = f(P_e,T_e+SH,N_{comp},G_{tot})\) . If the difference between the calculated result and the assumed value is higher than the assigned tolerance (5\%), a new round of iteration is performed using the calculated \(h_{Hexin}\) .
+
+\paragraph{Step 2h.2: Initialize O/U operation conditions}\label{step-2h.2-initialize-ou-operation-conditions}
+
+Similar to that in cooling mode, an iteration approach is designed to determine the energy consumption of the compressor (Step 2h. 2 to Step 2h. 6).
+
+For the first iteration,
+
+\begin{itemize}
+\item
+  Initialize outdoor unit \(SH\) with the reference value (from IDF input, e.g., 1.5°C)
+\item
+  Iinitialize the compressor power \(N_{comp}\) with the value calculated from the reference \(COP\) (e.g., 3.5):
+\end{itemize}
+
+\begin{equation}
+N'_{comp} = \frac{\sum_iQ_{in,total,i}}{COP}
+\end{equation}
+
+Where
+
+\(N_{comp}\) compressor power (W)
+
+\(N'_{comp}\) assumed compressor power for the first iteration (W)
+
+\(Q_{in,total,i}\) total heating load for zone \(i\) (W)
+
+For the following iterations,
+
+\begin{itemize}
+\item
+  Initialize \(SH\) with the calculated value in the previous iteration
+\item
+  Initialize the compressor power \(N_{comp}\) with the calculated value in the previous iteration
+\end{itemize}
+
+Calculate the heat rate extracted by the outdoor unit by:
+
+\begin{equation}
+Q_{out} = \sum_iQ_{in,total,i}+Q_{pipe}-N_{comp}
+\end{equation}
+
+Where
+
+\(Q_{out}\) heat rate extracted by the outdoor unit (W)
+
+\(Q_{pipe}\) heat loss through the pipe (W)
+
+\paragraph{Step 2h.3: Calculate O/U effective evaporating temperature}\label{step-2h.3-calculate-ou-effective-evaporating-temperature}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\tightlist
+\item
+  Calculate the required coil surface air temperature \({T_{fs}}'\) for the outdoor unit.
+\end{enumerate}
+
+The enthalpy of the air leaving the outdoor unit can be calculated by:
+
+\begin{equation}
+{H_{fs}}' = {H_{in}}'-Q_{out}/({G_{a,rate}}'\times{\rho_o})/(1-BF')
+\end{equation}
+
+The coil surface air temperature \({T_{fs}}'\) can be calculated from the \({H_{fs}}'\) :
+
+\begin{equation}
+if\quad{H_{fs}}'<H_{98\%,W_o}\quad{then}\quad{T_{fs}}' = f({H_{fs}}',98\%)
+\end{equation}
+
+\begin{equation}
+if\quad{H_{fs}}'\ge{H_{98\%,W_o}}\quad{then}\quad{T_{fs}}' = f({H_{fs}}',W_o)
+\end{equation}
+
+Where
+
+\(BF'\) bypass factor for the outdoor unit
+
+\({G_{a,rate}}'\) volumetric flow rate of the air through the outdoor unit, at the rating conditions (m\(^{3}\)/s)
+
+\({H_{fs}}'\) enthalpy of the air leaving the outdoor unit (kJ/kg)
+
+\({H_{in}}'\) enthalpy of the air entering the outdoor unit, i.e., outdoor air (kJ/kg)
+
+\(W_o\) humidity ratio of the outdoor air (kg/kg)
+
+\(\rho_o\) density of the outdoor air (kg/m\(^{3}\))
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Calculate required evaporating temperature for the outdoor unit \(Te_{req}\) and then the effective evaporating temperature \(Te\) .
+\end{enumerate}
+
+\begin{equation}
+Te_{req} = {T_{fs}}'-[{A_c}'\cdot SH^2+{B_c}'\cdot SH+{C_c}']
+\end{equation}
+
+\begin{equation}
+Te = Te_{req}
+\end{equation}
+
+Where
+
+\({A_c}'\) ,\({B_c}'\) ,\({C_c}'\) coefficients (°C)
+
+\(SH\) superheating degrees for the outdoor unit (°C)
+
+\(SH_{ref}\) reference superheating degrees for the outdoor unit (°C)
+
+\(Te_{req}\) required evaporating temperature for the outdoor unit (°C)
+
+\(Te\) effective evaporating temperature (°C)
+
+\paragraph{Step 2h.4: Calculate required compressor Loading Index}\label{step-2h.4-calculate-required-compressor-loading-index}
+
+Calculate the required compressor Loading Index by the following procedures.
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\tightlist
+\item
+  Calculate the evaporative capacity at a variety of speeds:
+\end{enumerate}
+
+\[M_{cap} = C_{cap,system}\times(r_1+r_2{T_c}'+r_3T_e+r_4{T_c}'^2+r_5{T_c}'T_e+r_6T_e^2)\] \[Q_{rps} = C_{cap,system} \times M_{cap} \times Q_{ref}\]
+
+Where
+
+\(C_{cap,system}\) evaporative capacity correction factor, describing the possible system configuration difference between test bed and real system (obtained from manufacturer data)
+
+\(r_1\) ,\ldots{},\(r_6\) empirical coefficients corresponding to \(rps\)
+
+\(rps\) compressor speed (r/s)
+
+\(T_e\) effective evaporating temperature (°C)
+
+\(M_{cap}\) multiplier for the evaporative capacity calculation (--)
+
+\({T_c}'\) discharge saturated temperature at the compressor outlet (°C)
+
+\(Q_{rps}\) evaporative capacity corresponding to \(rps\) (W)
+
+\(Q_{ref}\) rated evaporative capacity (W)
+
+An example of resulting capacity for different \(rps\) (at \({T_c}'\) = 36°C and \(T_e\) = 9°C) is presented in Table 3.
+
+Table 3-- evaporative capacity at different Loading Index
+
+
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Find the \(rps\) range that covers the required evaporative capacity \(Q_{rps,modify}\) .
+\end{enumerate}
+
+\begin{equation}
+Q_{rps,modify} = C_{cap,operation}\times(\sum{Q_{in,total}}+Q_{pipe}-N_{comp})
+\end{equation}
+
+\begin{equation}
+C_{cap,operation} = C_{cap,density}\times{C_{cap,enthalpy}}
+\end{equation}
+
+\begin{equation}
+C_{cap,density} = \rho_{test}/\rho_{real}
+\end{equation}
+
+\begin{equation}
+C_{cap,enthalpy} = \frac{h_{Evapout,test}-h_{Condout,test}}{h_{Compin,real}-h_{Condout,real}}
+\end{equation}
+
+Where
+
+\(C_{cap,operation}\) evaporative capacity correction factor, describing the operational difference between test cases and real cases (i.e., \(SH\) and \(SC\) )
+
+\(C_{cap,density}\) evaporative capacity correction factor, describing the variations of refrigerant density at test conditions and real operational conditions
+
+\(C_{cap,enthalpy}\) evaporative capacity correction factor, describing the variations of refrigerant enthalpy at test conditions and real operational conditions
+
+\(h_{Condout,test}\) enthalpy of refrigerant leaving the condensers (IU) at test conditions (It corresponds to \(SH\) at test condition(e.g., 8°C) and \(Te\) ) (kJ/kg)
+
+\(h_{Condout,real}\) average enthalpy of refrigerant leaving the condensers (IU) at real conditions (kJ/kg)
+
+\(h_{Compin,real}\) enthalpy of refrigerant entering the compressor at real conditions (It corresponds to \(SH\) and \(Te\) at real conditions) (kJ/kg)
+
+\(Q_{pipe}\) heat loss through the pipe (W)
+
+For example, if the required capacity is 8 kW, the \(rps\) range is 30 to 36 \(rps\) based on Table 3.
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\setcounter{enumi}{2}
+\item
+  Calculate the \(rps\) that meets the need by interpolation. In the above example, the resulting \(rps\) is 34.5 \(rps\) .
+\item
+  If the calculated \(rps\) is lower than the minimum \(rps\) (e.g.~18\(rps\) ), go to Step 2h. 5; otherwise, skip Step 2h. 5 and go to Step 2h. 6.
+\end{enumerate}
+
+\paragraph{Step 2h.5: Modify evaporating temperature to further reduce outdoor unit capacity}\label{step-2h.5-modify-evaporating-temperature-to-further-reduce-outdoor-unit-capacity}
+
+If the calculated \(rps\) is lower than the minimum \(rps\) (e.g.~18 \(rps\) ), it means that the zone heating load (indoor unit side) is so low that it leads to an evaporative capacity (outdoor unit side) which is even lower than the system evaporative capacity corresponding to the minimum compressor speed. In this situation, the evaporating temperature \(Te\) as well as the superheating degree \(SH\) is modified to further reduce the outdoor unit capacity. More specifically:
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\item
+  Set \(rps\) at its minimum value (e.g., 18 \(rps\) ).
+\item
+  Update \(Te\) to meet the required evaporative capacity, using equations described in Step 2h.4a.
+\item
+  \(SH\) for each indoor unit can be updated using the equations shown in Step 1.2.
+\end{enumerate}
+
+It should be noted that, different from the corresponding step in the cooling mode (Step 2c.5), the \(Te\) and \(SH\) updates in the heating mode do not affect the refrigerant state and flow rate calculations (as shown in Step 2h.1). Therefore, the piping loss analysis does not need to be repeated here.
+
+\paragraph{Step 2h.6: Calculate the compressor power}\label{step-2h.6-calculate-the-compressor-power}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\tightlist
+\item
+  Calculate the compressor power by the following procedures. 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\tightlist
+\item
+  Calculate the compressor power at a variety of Loading Index using the following equation. The resulting table (Table~\ref{table:atmospheric-variables-at-two-different}) from the same example is shown below.
+\end{enumerate}
+
+\[M_{comp} = c_1+c_2{T_c}'+c_3T_e+c_4{T_c}'^2+c_5{T_c}'T_e+c_6T_e^2\] \[N_{comp,rps} = M_{comp} \times N_{comp,ref}\]
+
+Where
+
+\(c_1\) ,\ldots{},\(c_6\) empirical coefficients corresponding to \(rps\)
+
+\(T_e\) effective evaporating temperature (°C)
+
+\(T_{e,ref}\) reference evaporating temperature (°C)
+
+\({T_c}'\) discharge saturated temperature at the compressor outlet (°C)
+
+\(T_{c,ref}\) reference condensing temperature (°C)
+
+\(M_{comp}\) multiplier for the compressor power calculation (--)
+
+\(N_{comp,ref}\) rated compressor power (W)
+
+\(N_{comp,rps}\) compressor power corresponding to \(rps\) (W)
+
+Table~\ref{table:atmospheric-variables-at-two-different} -- Outdoor unit compressor power at different Loading Index
+
+
+
+\begin{enumerate}
+\def\labelenumi{\alph{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  According to the \(rps\) range determined, calculate the compressor power \(N_{comp}\) by interpolation. In the above example, the compressor power is 1.155 kW. 
+\end{enumerate}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Compare the calculated \(N_{comp}\) above with the initialized \({N_{comp}}'\) in Step 2h.2:
+\end{enumerate}
+
+\begin{itemize}
+\item
+  If \({N_{comp}}'-N_{comp}>\delta\) then go to Step 2h.2 for a new round of iteration.
+\item
+  Else, end the iteration and go to Step 2h.7.
+\end{itemize}
+
+\paragraph{Step 2h.7: Total power consumption of the outdoor unit}\label{step-2h.7-total-power-consumption-of-the-outdoor-unit}
+
+Same as that in the cooling mode (Step 2c. 7)
+
+\subsubsection{\texorpdfstring{\emph{Modeling of the indoor unit (I/U) - Part II - Cooling Mode}}{Modeling of the indoor unit (I/U) - Part II - Cooling Mode}}\label{modeling-of-the-indoor-unit-iu---part-ii---cooling-mode}
+
+\paragraph{Step 3c.1: Update air flow rate for each indoor unit}\label{step-3c.1-update-air-flow-rate-for-each-indoor-unit}
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\tightlist
+\item
+  Calculate coil surface temperature for each indoor unit:
+\end{enumerate}
+
+\begin{equation}
+T_{fs} = T_e+[A_c\cdot SH^2+B_c\cdot SH+C_c]
+\end{equation}
+
+Where
+
+\(T_e\) evaporating temperature decided in the outdoor unit calculations (°C)
+
+\(T_{fs}\) coil surface temperature (°C)
+
+\(SH\) superheating degrees decided in the outdoor unit calculations (°C)
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Calculate the enthalpy of the air at the coil surface, \(H_{fs}\) :
+\end{enumerate}
+
+\begin{equation}
+if\quad{T_{fs}}<T_{98\%,W_{in}}\quad{then}\quad{H_{fs}} = f(T_{fs},98\%)
+\end{equation}
+
+\begin{equation}
+if\quad{T_{fs}}\ge{T_{98\%,W_{in}}}\quad{then}\quad{H_{fs}} = f(T_{fs},W_{in})
+\end{equation}
+
+Where
+
+\(T_{98\%,W_{in}}\) dew point temperature of the indoor air (°C)
+
+\(H_{fs}\) enthalpy of the air at the coil surface (kJ/kg)
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Calculate the required air flow rate \(G_a\) for each indoor unit:
+\end{enumerate}
+
+\begin{equation}
+G_a = Q_{in,total}/[(H_{coil,in}-H_{fs})\times{(1-BF)}\times{\rho_{in}}]
+\end{equation}
+
+Where
+
+\(Q_{in,total}\) total cooling load for the zone (W)
+
+\(H_{coil,in}\) enthalpy of the entering air of the indoor unit (kJ/kg)
+
+\(\rho_{in}\) density of indoor air,\(f_{\rho}(T_{in},W_{in})\) (kg/m\(^{3}\))
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{3}
+\tightlist
+\item
+  Decide whether to modify \(SH\) for further indoor unit capacity reduction.
+\end{enumerate}
+
+\begin{itemize}
+\item
+  If \(G_a\) \textless{} \(G_{a,min}\) (e.g., \(0.7\times\) \(G_{a,rate}\) ) go to Step 3c. 2
+\item
+  Else, directly go to Step 3c. 3
+\end{itemize}
+
+\paragraph{\texorpdfstring{Step 3c.2: Modify \(SH\) to adjust the indoor unit capacity}{Step 3c.2: Modify SH to adjust the indoor unit capacity}}\label{step-3c.2-modify-sh-to-adjust-the-indoor-unit-capacity}
+
+Set \(G_a\) at its minimum value (e.g., \(0.7\times\) \(G_{a,rate}\) ).
+
+The required coil surface temperature \(T_{fs}\) can be determined as described in Step 1.2.
+
+Given \(T_{fs}\) and \(T_e\) , \(SH\) can be determined using the equation shown in Step 1.3.
+
+\begin{itemize}
+\tightlist
+\item
+  If \(SH\) \textgreater{} 15°C, Set \(SH\) as 15°C. On/Off control strategy may be implemented when needed.
+\end{itemize}
+
+\paragraph{Step 3c. 3: Total power consumption of the indoor unit}\label{step-3c.-3-total-power-consumption-of-the-indoor-unit}
+
+The power consumption of the indoor unit comes from the fan operations. This can be calculated using the existing VAV fan model in EnergyPlus. Please refer to the current EnergyPlus Engineering Reference for more details.
+
+\subsubsection{\texorpdfstring{\emph{Modeling of the indoor unit (I/U) - Part II - Heating Mode}}{Modeling of the indoor unit (I/U) - Part II - Heating Mode}}\label{modeling-of-the-indoor-unit-iu---part-ii---heating-mode}
+
+\paragraph{Step 3h.1: Update air flow rate for each indoor unit.}\label{step-3h.1-update-air-flow-rate-for-each-indoor-unit.}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\tightlist
+\item
+  Calculate coil surface temperature for all the indoor units:
+\end{enumerate}
+
+\begin{equation}
+T_{fs} = T_c-[A_h\cdot SC^2+B_h\cdot SC+C_h]
+\end{equation}
+
+Where
+
+\(T_c\) condensing temperature decided in the outdoor unit calculations (°C)
+
+\(T_{fs}\) coil surface temperature (°C)
+
+\(SC\) subcooling degrees decided in the outdoor unit calculations (°C)
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Calculate the required air flow rate \(G_a\) for each indoor unit:
+\end{enumerate}
+
+\begin{equation}
+G_a = Q_{in,total}/[(T_{fs}-T_{coil,in})\times{(1-BF)}\times{\rho_{in}}]
+\end{equation}
+
+Where
+
+\(Q_{in,total}\) total heating load for the zone (W)
+
+\(T_{coil,in}\) temperature of the entering air of the indoor unit (°C)
+
+\(\rho_{in}\) density of indoor air,\(f_{\rho}(T_{in},W_{in})\) (kg/m\(^{3}\))
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Decide whether to modify \(SH\) for further indoor unit capacity reduction
+\end{enumerate}
+
+\begin{itemize}
+\item
+  If \(G_a\) \textless{} \(G_{a,min}\) (e.g., \(0.7\times\) \(G_{a,rate}\) ) go to Step 3h. 2
+\item
+  Else, directly go to Step 3h. 3
+\end{itemize}
+
+\paragraph{\texorpdfstring{Step 3h.2: Modify \(SC\) to modify the indoor unit capacity}{Step 3h.2: Modify SC to modify the indoor unit capacity}}\label{step-3h.2-modify-sc-to-modify-the-indoor-unit-capacity}
+
+Set \(G_a\) at its minimum value (\(0.7\times\) \(G_{a,rate}\) ).
+
+The required coil surface temperature \(T_{fs}\) can be determined as described in Step 2.
+
+Given \(T_{fs}\) and \(T_e\) , \(SC\) can be determined using the equation shown in Step 1.3.
+
+\begin{itemize}
+\tightlist
+\item
+  If \(SC\) \textgreater{} 20°C, Set \(SC\) as 20°C. On/Off control strategy may be implemented when needed.
+\end{itemize}
+
+\paragraph{Step 3h.3: Total power consumption of the indoor unit}\label{step-3h.3-total-power-consumption-of-the-indoor-unit}
+
+Calculate electric power consumption by the indoor unit using the existing VAV fan model in EnergyPlus. Please refer to the current EnergyPlus Engineering Reference for more details.
+
+\subsubsection{Additional energy consumption by defrost and crankcase heater}\label{additional-energy-consumption-by-defrost-and-crankcase-heater}
+
+There may be additional energy consumption due to the defrost operation and crankcase heater operation. These components have no impact on the heat pump operations. The calculation methods in the VRF-FluidTCtrl model are the same as those in VRF-SysCurve model. Please refer to the VRF-SysCurve section for more details.
+
+\subsection{Zone Terminal Unit List}\label{zone-terminal-unit-list}
+
+The zone terminal unit list identifies the terminal units that are connected to a single variable refrigerant flow heat pump. The zone terminal unit list is used exclusively in the variable refrigerant flow (VRF) heat pump object (ref: AirConditioner:VariableRefrigerantFlow) and VRF zone terminal units (ref: ZoneHVAC: TerminalUnit:VariableRefrigerantFlow). Up to 20 terminal units may be connected to a single VRF outdoor condensing unit. This list is extensible if additional indoor terminal units are required. The following figure shows the connection scheme between the zone terminal units, the zone terminal unit list, and finally the VRF AC system. The zone terminal units are connected to the zone through zone inlet and outlet zone nodes. Each zone terminal unit is entered in a list which represents all terminal units connected to a single VRF AC system. And finally, the zone terminal unit list name is entered in the corresponding VRF AC object.
+
+\begin{figure}[hbtp] % fig 249
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5454.png}
+\caption{Zone Terminal List connections in EnergyPlus objects \protect \label{fig:zone-terminal-list-connections-in-energyplus}}
+\end{figure}
+
+\subsubsection{References}\label{references-051}
+
+Raustad R. A variable refrigerant flow heat pump computer model in EnergyPlus, ASHRAE Transactions (2013), 119 (1):1--9.
+
+Hong T, Sun K, Zhang R, Hinokuma R, Kasahara S, Yura Y. Development and Validation of a New VRF Model in EnergyPlus. ASHRAE Winter Conference.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/zone-internal-gains.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/zone-internal-gains.tex
new file mode 100644
index 00000000000..eb52b076848
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-001/zone-internal-gains.tex
@@ -0,0 +1,334 @@
+\section{Zone Internal Gains }\label{zone-internal-gains}
+
+\subsection{Sources and Types of Gains}\label{sources-and-types-of-gains}
+
+Internal heat gains from lights, people, and equipment of various types are often significant elements in the zone thermal balance.~ EnergyPlus allows the user to specify heat gains for several equipment types including people, lights, gas/electric equipment, and several other types.~ The total heat gain is comprised of convective, radiant and latent gains in various proportions from these sources.~ Convective gains are instantaneous additions of heat to the zone air.~ Radiant gains are distributed on the surfaces of the zone, where they are first absorbed and then released back into the room (with some fraction conducted through the surface) according to the surface heat balances. \{See Surface Heat Balance Manager / Processes in this document\}.~ Latent gains must be handled by ventilation or air conditioning equipment.~ Recommended heat gains are given by ASHRAE {[}1{]}.~ These recommendations include the sensible (convective plus radiative) and latent proportions.~ Sensible gains from equipment are primarily radiant.~ The user can specify the heat gains and proportions for any type of equipment.~ Determining the gains from lights, people and baseboard heat are slightly more complicated.
+
+\subsection{Heat Gain from Lights}\label{heat-gain-from-lights}
+
+The input object Lights provides a model for internal gains from lights.~ Radiant gains from lights must be handled differently from other radiant gains for reasons described here (long wavelength description).~ The total radiant gains from lights must be divided into visible and thermal portions.~ For example, the total electric input to typical incandescent lights is converted to 10\% visible radiation, 80\% thermal radiation, and 10\% convective gain.~ In contrast, the electric input to typical fluorescent lights is converted to 20\% visible radiation, 20\% thermal radiation, and 60\% convective gain {[}2{]}.~ These percentage splits are under user control with the Lights input object.
+
+\subsection{Heat Gain from People}\label{heat-gain-from-people-000}
+
+The input object People provides a model for internal gains from occupants.~ Heat is generated in the human body by oxidation at a rate called the metabolic rate (see Thermal Comfort discussion for more details).~ This heat is dissipated from the body surface and respiratory tract by a combination of radiation, convection, and evaporation.~ The relative proportions of sensible (radiation plus convection) and latent (evaporation) heat from people is a complex function of the metabolic rate and the environmental conditions.~ EnergyPlus uses a polynomial function to divide the total metabolic heat gain into sensible and latent portions.~ That function is based on a fit to data {[}3{]} at average adjusted metabolic rates of 350, 400, 450, 500, 750, 850, 1000 and 1450 Btu/h each at temperatures of 70, 75, 78, 80, 82 degrees Fahrenheit.~ Sensible gains of 0 at 96 F and sensible gains equal to the metabolic rate at 30 F were assumed in order to give reasonable values beyond the reported temperature range.
+
+Average adjusted metabolic rate {[}3{]} is the metabolic rate to be applied to a mixed group of people with a typical percent composition based on the following factors:
+
+\begin{itemize}
+  \item Metabolic rate, adult female = Metabolic rate, adult male X 0.85
+  \item Metabolic rate, children = Metabolic rate, adult male X 0.75
+\end{itemize}
+
+The original data was in I-P (Inch-Pound) units, but the following correlation is in SI (Systems-International) units.
+
+\begin{equation}
+  \begin{array}{ll}
+    S &= 6.461927 + .946892 M + .0000255737 M^2 + 7.139322 T - .0627909 T M \\
+      &+ .0000589172 T M^2 - .198550 T^2 + .000940018 T^2 M - .00000149532 T^2 M^2
+  \end{array}
+\end{equation}
+
+where
+
+M = Metabolic Rate (W)
+
+T = Air Temperature (C)
+
+S = Sensible Gain (W)
+
+Latent Gain is simply the total gain (metabolic rate) -- sensible gain:
+
+\begin{equation}
+LatentGain = MetabolicRate - SensibleGain
+\end{equation}
+
+\begin{figure}[hbtp] % fig 259
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5820.png}
+\caption{Sensible Heat Gain from People Correlation \protect \label{fig:sensible-heat-gain-from-people-correlation}}
+\end{figure}
+
+The function for sensible gain calculation is compared to the original data points in the following figure.~ The radiant fraction of the sensible gain is a user input on the People object.
+
+\subsection{Heat Gain from IT Equipment}\label{heat-gain-from-it-equipment}
+
+The input object ElectricEquipment:ITE:AirCooled describes air-cooled electric information technology equipment (ITE) which has variable power consumption as a function of loading and temperature. The calculations are described below.
+
+\subsubsection{Variable Definitions -- User Inputs:}\label{variable-definitions-user-inputs}
+
+\begin{itemize}
+\tightlist
+\item
+  PDesign = Design power input when fully loaded and entering air temperature is at the user-specified design inlet temperature {[}W{]}
+\item
+  PFanFracDesign = Design fan power input fraction of total power input when fully loaded and entering air temperature is at the user-specified design inlet temperature
+\item
+  SchDesignLevel = Scheduled fraction of this equipment which is powered up
+\item
+  SchCPULoading = Scheduled fraction of CPU loading
+\item
+  TAirInDesign = Air inlet temperature at design condition {[}C{]}
+\item
+  VAirDesign = Air volume flow rate at design condition {[}m3/s{]}
+\item
+  VAirfLoadTAir = Air volume flow rate modifier function of TAirIn and SchCPULoading
+\item
+  PCPUfLoadTAir = CPU power input modifier function of TAirIn and SchCPULoading
+\item
+  PFanfFlowFrac = Fan power input modifier function of air flow fraction
+\item
+  RecircFracDesign = Recirculation Fraction at design condition {[}C{]}
+\item
+  RecircfLoadTAir = Recirculation Fraction modifier function of TAirSupply and SchCPULoading
+\item
+  UPSEfficDesign = Design electric power supply efficiency
+\item
+  UPSEfficfPLR = Electric power supply efficiency function of part load ratio
+\item
+  UPSLossFracToZone = Fraction of electric power supply losses to zone
+\end{itemize}
+
+\subsubsection{Variable Definitions -- Simulation Inputs:}\label{variable-definitions-simulation-inputs}
+
+\begin{itemize}
+\tightlist
+\item
+  TAirIn = Air inlet temperature at current conditions {[}C{]}
+\item
+  TAirSupply = Supply air node temperature at current conditions {[}C{]}
+\item
+  TZone = Zone air temperature at current conditions {[}C{]}
+\item
+  TRoomAirNodeIn = Room air model inlet node air temperature at current conditions {[}C{]}
+\item
+  RhoAir = Air density {[}kg/m3{]}
+\item
+  CpAir = Air specific heat {[}J/kg-K{]}
+\end{itemize}
+
+\subsubsection{Variable Definitions -- Intermediate Calculations:}\label{variable-definitions-intermediate-calculations}
+
+\begin{itemize}
+\tightlist
+\item
+  PCPUDesign = Design CPU power input when fully loaded and entering air temperature is at the user-specified design inlet temperature {[}W{]}
+\item
+  PFanDesign = Design fan power input when fully loaded and entering air temperature is at the user-specified design inlet temperature {[}W{]}
+\item
+  UPSPLR = Electric power supply part load ratio (can be greater than 1.0)
+\end{itemize}
+
+\subsubsection{Variable Definitions -- Outputs:}\label{variable-definitions-outputs}
+
+\begin{itemize}
+\tightlist
+\item
+  PCPU = CPU power input {[}W{]}
+\item
+  PFan = Fan power input {[}W{]}
+\item
+  PUPS = Electric power supply net power input {[}W{]}
+\item
+  TAirOut = Air outlet temperature {[}C{]}
+\item
+  VAir = Air volume flow rate {[}m3/s{]}
+\item
+  FlowFrac = Air volume flow rate fraction of design flow rate
+\item
+  RecircFrac = Recirculation fraction
+\item
+  QAir = Air cooling rate {[}W{]}
+\item
+  QUPS = Electric power supply heat loss rate to zone {[}W{]}
+\item
+  QConv = Convective heat gain rate to zone heat balance {[}W{]}
+\item
+  SHI = Supply heat index
+\item
+  SHIZone = Zone average supply heat index
+\end{itemize}
+
+\subsubsection{Calculations}\label{calculations}
+
+The design power input is first split into portions for the CPU (everything in the equipment except the cooling fans) and the fan(s).
+
+PCPUDesign = PDesign * (1 - PFanFracDesign)
+
+PFanDesign = PDesign * PFanFracDesign
+
+For each time step, the air inlet temperature is calculated depending on the type of air node connection.
+
+TAirIn:
+
+\begin{itemize}
+\tightlist
+\item
+  If Air Node Connection Type = AdjustedSupply
+\end{itemize}
+
+\begin{lstlisting}
+-   RecircFrac = RecircFracDesign \* RecircfLoadTAir(SchCPULoading TAirSupply)
+-   TAirIn = TAirSupply \* (1 – RecircFrac) +TAirZone \* RecircFrac
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  If Air Node Connection Type = ZoneAirNode
+\end{itemize}
+
+\begin{lstlisting}
+-   TAirIn = TAirZone
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  If Air Node Connection Type = RoomAirModel
+\end{itemize}
+
+\begin{lstlisting}
+-   TAirIn = TRoomAirNodeIn
+\end{lstlisting}
+
+Using the air inlet temperature, the CPU power consumption, air flow rate, fan power consumption, and power supply power consumption are calculated.
+
+PCPU = PCPUDesign * SchDesignLevel * PfLoadTAir(SchCPULoading, TAirIn)
+
+FlowFrac = VAirfLoadTAir(SchCPULoading, TAirIn)
+
+VAir = VAirDesign * FlowFrac
+
+PFan = PFanDesign * SchDesignLevel * PFanfFlowFrac(FlowFrac)
+
+UPSPLR = (PCPU + PFan) / (PCPUDesign + PFanDesign)
+
+PUPS = (PCPU + PFan) * (1 - UPSEfficDesign * UPSEfficfPLR (UPSPLR))
+
+The convective heat gain to the zone and the air outlet temperature are then calculated. The user specified fration of power supply losses are always added to the general zone heat balace convective heat gain. For air node connection types AdjustedSupply and ZoneAirNode, the CPU and fan power consumption are also added to the zone convective heat gain. For air connection type RoomAirModel, the gains from the CPU and fan power consumption are added to the outlet room air model node.
+
+QAir = PCPU + PFan
+
+QUPS = PUPS * UPSLossFracToZone
+
+QConv:
+
+\begin{itemize}
+\tightlist
+\item
+  If Air Node Connection Type = AdjustedSupply OR ZoneAirNode
+\end{itemize}
+
+\begin{lstlisting}
+-   QConv = QAir + QUPS
+\end{lstlisting}
+
+\begin{itemize}
+\tightlist
+\item
+  If Air Node Connection Type = RoomAirModel
+\end{itemize}
+
+\begin{lstlisting}
+-   QConv = QUPS
+\end{lstlisting}
+
+TAirOut = TAirIn + QAir / (VAir * RhoAir * CpAir)
+
+The individual ITE supply heat index is calculated as shown below.
+
+SHI = (TAirIn -- TAirSupply) / (TAirOut - TAirSupply)
+
+The zone average ITE supply heat index is weighted by the air flow rate of each ITE object.
+
+SHIZone = ∑ {[}VAir * (TAirIn -- TAirSupply){]} / ∑ {[}VAir * (TAirOut - TAirSupply){]}
+
+\subsection{Heat Gain from Baseboard Heat}\label{heat-gain-from-baseboard-heat}
+
+The input object ZoneBaseboard:OutdoorTemperatureControlled provides a model for an outdoor temperature controlled baseboard heater that adds energy to the zone according a control profile as shown in the following figure.~ At TA = T2, the baseboard heat gain is Q2.~ For TA \textgreater{} T2, there is no heat gain.~ For TA \textless{} T1, a maximum amount of energy, Q1, is added to the zone.~ There is proportional control between those two temperatures:
+
+\begin{figure}[hbtp] % fig 260
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5821.png}
+\caption{Control of Outdoor Temperature Controlled Baseboard Heat \protect \label{fig:control-of-outdoor-temperature-controlled}}
+\end{figure}
+
+\begin{equation}
+Q = Q2 - \frac{{(Q2 - Q1)\cdot (T2 - TA)}}{{(T2 - T1)}}
+\end{equation}
+
+These temperature and capacity fields can be autosized based upon envelope, infiltration, and ventilation loads. To autosize these fields, users may set a design zone heating temperature that is assumed to be 20°C if blank.
+
+The capacity at low temperature is the maximum capacity of the unit. It includes external envelope conduction load, infiltration load, and ventilation load in a space where the unit serves. The model first finds the lowest outdoor air temperature throughout design days included in the simulation, and determines the conduction load through external envelop as:
+
+\begin{equation}
+{q_{Cond}} = UA\left( {{T_{Htg}} - {T_L}} \right)
+\end{equation}
+
+where
+
+\emph{q\(_{Cond}\)} is conduction load through external envelope, W
+
+\emph{U} is heat transfer coefficient of external wall, W/m\(^{2}\)K
+
+\emph{A} is area of external wall, m\(^{2}\)
+
+\emph{T\(_{Htg}\)} is baseboard zone heating setpoint temperature, °C
+
+\emph{T\(_{L}\)} is low temperature, °C
+
+The capacity at low temperature that is the maximum capacity of the unit is thus expressed as:
+
+\begin{equation}
+Ca{p_{{T_L}}} = {q_{Cond}} + {q_I} + {q_V}
+\end{equation}
+
+where
+
+\(Ca{p_{{T_L}}}\) is capacity at low temperature, W
+
+\emph{q\(_{I}\)} is design infiltration sensible load, W
+
+\emph{q\(_{V}\)} = design ventilation sensible load, W
+
+The capacity at high temperature is then prorated against the reference low and high temperatures as:
+
+\begin{equation}
+Ca{p_{{T_H}}} = Ca{p_{{T_L}}}\frac{{\left( {{T_{Htg}} - {T_H}} \right)}}{{\left( {{T_{Htg}} - {T_L}} \right)}}
+\end{equation}
+
+where
+
+\(Ca{p_{{T_H}}}\) ~is capacity at high temperature, W
+
+\emph{T\(_{H}\)} is high temperature, °C
+
+\subsection{Distribution of Radiant Gains}\label{distribution-of-radiant-gains}
+
+It is useful to consider the distribution of short wavelength (including visible) radiant energy separate from long wavelength (thermal) radiant energy because many materials have different optical properties at different wavelengths.~ An extreme example is glass that is opaque to the long wavelengths and transparent to the short.~ Properties of materials vary across the entire spectrum of wavelengths.~ In EnergyPlus, all radiant interactions are represented in terms of only two wavelengths: ``short'' and ``long''.~ Short wavelength refers to the distribution given by a \textasciitilde{}6000K black body source such as the sun.~ Long wavelengths refer to radiation from \textasciitilde{}300K sources such as walls or people.~ There is negligible overlap between these two distributions.~ Some sources, such as lights, must be considered as emitting both long and short wavelength radiation in proportions that approximate their actual effects on room surfaces.
+
+Long wavelength radiation from all internal sources, such as people, lights and equipment, is combined and then distributed over surfaces. (see Internal Long-Wave Radiation Exchange).
+
+Some fraction of the beam solar radiation transmitted into the zone is directly absorbed by the interior surfaces according to the solar distribution algorithm (see Solar Distribution) selected by the user.~ The beam radiation not directly absorbed, plus the diffuse sky and ground-reflected radiation, plus the short wavelength radiation from lights are combined and distributed over the surfaces of the zone according to:
+
+\begin{equation}
+QS{I_i} = Q{S_n}\cdot {\alpha_i}/\sum\limits_{i = 1}^{NS} {{S_i}\cdot (1 - {\rho_i})}
+\end{equation}
+
+If all surfaces in the room are opaque, the radiation is distributed in proportion to the area*absorptance product of each surface.~ For surfaces which are transparent,
+
+\begin{equation}
+{\rho_i} = 1 - {\alpha_i} - {\tau_i}
+\end{equation}
+
+That fraction of radiation represented by \({\tau_i}\) ~is lost from the zone.
+
+The transmittance and absorptance of transparent surfaces (windows or glass doors) are calculated as in section Window Calculation Module based on the optical properties of the window material layers.~ The total absorptance of the window is computed for the interior shading device, the inside surface, and the outside surface for diffuse solar radiation incident from outside the zone.~ Those absorptances are used for short wavelength radiation incident from inside the zone.~ In most cases, this should not cause significant error.~ When movable insulation covers the window, the radiation that would have been transmitted is absorbed at the outer surface of the window (thermally equal to the inside surface of the insulation).
+
+\subsection{References}\label{references-057}
+
+ASHRAE. 2001. Handbook of Fundamentals, pp 29.8-29.13, Atlanta: ASHRAE.
+
+Carrier Air Conditioning Company. 1965a. Handbook of Air Conditioning System Design, pp 1-99 to 1-100. New York: McGraw Hill.
+
+Carrier Air Conditioning Company. 1965b. Handbook of Air Conditioning System Design, pp 1-100, Table \# 48. New York: McGraw Hill.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002.tex
new file mode 100644
index 00000000000..c48f467fe79
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002.tex
@@ -0,0 +1,19 @@
+\chapter{Simulation Models -- Encyclopedic Reference}\label{simulation-models-encyclopedic-reference}
+
+The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of ``Heat Balance'', ``HVAC'', and ``Plant''.~ With the integrated solution, these designations signify where the effects of these models have their first impacts.
+
+Main Sections:
+
+\begin{itemize}
+\tightlist
+\item
+  \protect\hyperlink{RadiantSystems}{Radiant System Models}
+\item
+  \protect\hyperlink{Refrigeration}{Refrigeration Equipment}
+\item
+  \protect\hyperlink{SetpointManagers}{Setpoint Managers}
+\item
+  \protect\hyperlink{SolarCollectors}{Solar Collectors}
+\item
+  \protect\hyperlink{AvailManagers}{System Availability Managers} 
+\end{itemize}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/radiant-system-models.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/radiant-system-models.tex
new file mode 100644
index 00000000000..95d204713ab
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/radiant-system-models.tex
@@ -0,0 +1,856 @@
+\section{Radiant System Models }\label{radiant-system-models}
+
+\subsection{Low Temperature Radiant System Model}\label{low-temperature-radiant-system-model}
+
+The input objects ZoneHVAC:LowTemperatureRadiant:ConstantFlow, \\ ZoneHVAC:LowTemperatureRadiant:VariableFlow, and \\
+ZoneHVAC:LowTemperatureRadiant:Electric provide models for low temperature radiant heating and cooling systems that appear, on the surface, to be relatively simple systems.~ The system circulates hot or cold fluid through tubes embedded in a wall, ceiling, or floor or runs current through electric resistance wires embedded in a surface or a panel.~ Energy is thus either added to or removed from the space, and zone occupants are conditioned by both radiation exchange with the system and convection from the surrounding air that is also affected by the system.~ Unless specifically required for indoor air quality considerations, fans, ductwork, dampers, etc. are not needed.
+
+Despite the relative simplicity of the low temperature radiant systems, the integration of such a system within an energy analysis program requires one to overcome several challenges.~ First, for systems with significant thermal mass, the conduction transfer function method for modeling transient conduction must be extended to include embedded heat sources or sinks.~ Second, one must integrate this formulation within an energy analysis program like EnergyPlus.~ Finally, one must overcome the fact that the radiant system is both a zone heat balance element and a conditioning system.~ Each of these issues will be addressed in the next several subsections.
+
+\subsubsection{One Dimensional Heat Transfer Through Multilayered Slabs}\label{one-dimensional-heat-transfer-through-multilayered-slabs}
+
+One of the most important forms of heat transfer in energy analysis is heat conduction through building elements such as walls, floors, and roofs.~ While some thermally lightweight structures can be approximated by steady state heat conduction, a method that applies to all structures must account for the presence of thermal mass within the building elements.~ Transient one dimensional heat conduction through a homogeneous layer with constant thermal properties such as the one shown in Figure~\ref{fig:single-layered-building-element} is governed by the following equation:
+
+\begin{equation}
+\frac{{{\partial ^2}T}}{{\partial {x^2}}} = \frac{1}{\alpha }\frac{{\partial T}}{{\partial t}}
+\end{equation}
+
+where: T is the temperature as a function of position and time,
+
+x is the position,
+
+t is the time,
+
+\(\alpha = \frac{k}{{\rho {c_p}}}\) ~is the thermal diffusivity of the layer material,
+
+k is its thermal conductivity,
+
+r is its density, and
+
+cp~is its specific heat.
+
+This equation is typically coupled with Fourier's law of conduction that relates the heat flux at any position and time to temperature as follows:
+
+\begin{equation}
+q''\left( {x,t} \right) =  - k\frac{{\partial T\left( {x,t} \right)}}{{\partial x}}
+\end{equation}
+
+\begin{figure}[hbtp] % fig 266
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5973.png}
+\caption{Single Layered Building Element \protect \label{fig:single-layered-building-element}}
+\end{figure}
+
+While analytical solutions exist for the single homogeneous layer shown in Figure~\ref{fig:single-layered-building-element}, the solution becomes extremely tedious for the multiple layered slab shown in Figure~\ref{fig:multilayered-building-element}.
+
+\begin{figure}[hbtp] % fig 267
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image5974.png}
+\caption{Multilayered Building Element \protect \label{fig:multilayered-building-element}}
+\end{figure}
+
+\subsubsection{Time Series Solutions:~ Conduction Transfer Functions}\label{time-series-solutions-conduction-transfer-functions}
+
+Equations and can be solved numerically in a variety of ways.~ As mentioned in the previous section, other models have used control theory and numerical methods such as finite difference and finite element.~ However, each of these methods have drawbacks which render them inappropriate for use within an energy analysis program which requires both accuracy and efficiency from the simulation.
+
+Another possible modeling method is a time series solution.~ Several of the detailed energy analysis programs such as EnergyPlus use a time series solution to transient heat conduction.~ The most basic time series solution is the response factor equation which relates the flux at one surface of an element to an infinite series of temperature histories at both sides as shown by:
+
+\begin{equation}
+{q''_{i,t}} = \sum\limits_{m = 1}^\infty  {{X_m}{T_{i,t - m + 1}}}  - \sum\limits_{m = 1}^\infty  {{Y_m}{T_{o,t - m + 1}}}
+\end{equation}
+
+where q'' is heat flux, T is temperature, i signifies the inside of the building element, o signifies the outside of the building element, and t represents the current time step.
+
+While in most cases the terms in the series decay fairly rapidly, the infinite number of terms needed for an exact response factor solution makes it less than desirable.~ Fortunately, the similarity of higher order terms can be used to replace them with flux history terms.~ The new solution contains elements that are called conduction transfer functions (CTFs).~ The basic form of a conduction transfer function solution is shown by the following equation:
+
+\begin{equation}
+{q''_{i,t}} = \sum\limits_{m = 1}^M {{X_m}{T_{i,t - m + 1}}}  - \sum\limits_{m = 1}^M {{Y_m}{T_{o,t - m + 1}}}  + \sum\limits_{m = 1}^k {{F_m}{{q''}_{i,t - m}}}
+\end{equation}
+
+where k is the order of the conduction transfer functions, M is a finite number defined by the order of the conduction transfer functions, and X, Y, and F are the conduction transfer functions.~ This equation states that the heat flux at the interior surface of any generic building element for which the assumption of one dimensional conduction heat transfer is valid is linearly related to the current and some of the previous temperatures at both the interior and exterior surface as well as some of the previous flux values at the interior surface.~ A similar equation holds for the heat flux at the exterior surface.
+
+The final CTF solution form reveals why it is so elegant and powerful.~ With a single, relatively simple equation, the conduction heat transfer through an element can be calculated.~ The coefficients (CTFs) in the equation are constants that only need to be determined once.~ The only storage of data required is the CTFs themselves and a limited number of temperature and flux terms.~ The formulation is valid for any surface type and does not require the calculation or storage of element interior temperatures.
+
+As the next several sections will detail, there are two main methods for calculating conduction transfer functions:~ the Laplace Transform method and the State Space method.~ Both methods are well suited for the main focus of this research, the extension of conduction transfer functions to include heat sources or sinks.
+
+\subsubsection{Laplace Transform Formulation}\label{laplace-transform-formulation}
+
+The traditional method for calculating conduction transfer functions is described in detail by Hittle (1981).~ Beginning with the transient one dimensional heat conduction equation \{Equation \} and Fourier's law of conduction \{Equation \}, the Laplace transform method is used to convert the governing equations into the s-domain for a single layer such as the one shown in Figure~\ref{fig:single-layered-building-element}.
+
+\begin{equation}
+\frac{{{d^2}T\left( {x,s} \right)}}{{d{x^2}}} = \frac{s}{\alpha }T\left( {x,s} \right)
+\end{equation}
+
+\begin{equation}
+q''\left( {x,s} \right) =  - k\frac{{dT\left( {x,s} \right)}}{{dx}}
+\end{equation}
+
+The transformed equations are solved and then put in matrix form as shown below:
+
+\begin{equation}
+\left[ 
+    {\begin{array}{*{20}{c}}
+      {{T_1}\left( s \right)} \\ {{q_1}\left( s \right)}
+    \end{array}}
+  \right] = \left[ 
+    {\begin{array}{*{20}{c}}
+      {{A_1}\left( s \right)}&{{B_1}\left( s \right)} \\
+      {{C_1}\left( s \right)}&{{D_1}\left( s \right)}
+    \end{array}}
+  \right] \left[ 
+    {\begin{array}{*{20}{c}}
+      {{T_2}\left( s \right)} \\
+      {{q_2}\left( s \right)}
+    \end{array}}
+  \right]
+\end{equation}
+
+where: T1(s), T2(s), q1(s), and q2(s) are the temperature and flux terms in the Laplace domain,
+
+\({A_1}\left( s \right) = \cosh \left( {{\ell_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} } \right)\) ,
+
+\({B_1}\left( s \right) = \left( {{1 \mathord{\left/ {\vphantom {1 {{k_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} }}} \right. } {{k_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} }}} \right)\sinh \left( {{\ell_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} } \right)\) ,
+
+\({C_1}\left( s \right) = {k_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} \sinh \left( {{\ell_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} } \right)\) ,
+
+\({D_1}\left( s \right) = \cosh \left( {{\ell_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} } \right)\) ,
+
+k1~is the thermal conductivity of the layer,
+
+a1~is the thermal diffusivity of the layer, and
+
+\({\ell_1}\) ~is the thickness of the layer.
+
+The 2 x 2 matrix consisting of A1(s), B1(s), C1(s), and D1(s) is called the transmission matrix and contains all of the thermophysical properties of the layer necessary to calculate transient conduction heat transfer through it.~ It can easily be shown that a second layer could be characterized in a similar way as:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_2}\left( s \right)}\\ {{q_2}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_3}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+where A2(s), B2(s), C2(s), and D2(s) are calculated using the properties of the second layer.~ This can be substituted into Equation to provide insight how the extension to multilayered slabs is achieved.
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_3}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+Thus, for a multilayered element as shown in Figure~\ref{fig:multilayered-building-element}, each separate layer has a transmission matrix of Ai(s), Bi(s), Ci(s), and Di(s) associated with it.~ The form of the matrix equation for the multilayered element is the same as the equation for a single layer:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{A\left( s \right)}&{B\left( s \right)}\\ {C\left( s \right)}&{D\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_{n + 1}}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+but the transmission matrix is replaced by:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{A\left( s \right)}&{B\left( s \right)}\\ {C\left( s \right)}&{D\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right] \cdots \left[ {\begin{array}{*{20}{c}}{{A_n}\left( s \right)}&{{B_n}\left( s \right)}\\ {{C_n}\left( s \right)}&{{D_n}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+Equation is typically rearranged as follows:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{q_1}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{D\left( s \right)}}{{B\left( s \right)}}}&{\frac{{ - 1}}{{B\left( s \right)}}}\\ {\frac{1}{{B\left( s \right)}}}&{\frac{{ - A\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{T_{n + 1}}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+which relates the flux at either surface of the element to the temperature histories at both surfaces.~ When the temperature histories are formulated as triangular pulses made up of simple ramp functions, the roots of this equation can be found and result in response factors.~ The response factors can be simplified as described above through the introduction of flux history terms to form conduction transfer functions.~ A simplified method of finding the roots of the Laplace domain equations is described by Hittle and Bishop (1983) and is used by the current version of BLAST.
+
+\subsubsection{State Space Formulation}\label{state-space-formulation}
+
+Recently, another method of finding conduction transfer functions starting from a state space representation has begun receiving increased attention (Ceylan and Myers 1980; Seem 1987; Ouyang and Haghighat 1991).~ The basic state space system is defined by the following linear matrix equations:
+
+\begin{equation}
+\frac{{d\left[ x \right]}}{{dt}} = \left[ A \right]\left[ x \right] + \left[ B \right]\left[ u \right]
+\end{equation}
+
+\begin{equation}
+\left[ y \right] = \left[ C \right]\left[ x \right] + \left[ D \right]\left[ u \right]
+\end{equation}
+
+where x is a vector of state variables, u is a vector of inputs, y is the output vector, t is time, and A, B, C, and D are coefficient matrices.~ Through the use of matrix algebra, the vector of state variables (x) can be eliminated from the system of equations, and the output vector (y) can be related directly to the input vector (u) and time histories of the input and output vectors.
+
+This formulation can be used to solve the transient heat conduction equation by enforcing a finite difference grid over the various layers in the building element being analyzed.~ In this case, the state variables are the nodal temperatures, the environmental temperatures (interior and exterior) are the inputs, and the resulting heat fluxes at both surfaces are the outputs.~ Thus, the state space representation with finite difference variables would take the following form:
+
+\begin{equation}
+\frac{{d\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right]}}{{dt}} = \left[ A \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right] + \left[ B \right]\left[ {\begin{array}{*{20}{c}}{{T_i}}\\ {{T_o}}\end{array}} \right]
+\end{equation}
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{{q''}_i}}\\ {{{q''}_o}}\end{array}} \right] = \left[ C \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right] + \left[ D \right]\left[ {\begin{array}{*{20}{c}}{{T_i}}\\ {{T_o}}\end{array}} \right]
+\end{equation}
+
+where T1, T2, \ldots{}, Tn-1, Tn~are the finite difference nodal temperatures, n is the number of nodes, Ti~and To~are the interior and exterior environmental temperatures, and \({q''_i}\) ~and \({q''_o}\) ~are the heat fluxes (desired output).
+
+Seem (1987) shows that for a simple one layer slab with two interior nodes as in Figure~\ref{fig:two-node-state-space-example} and convection at both sides the resulting finite difference equations are given by:
+
+\begin{equation}
+C\frac{{d{T_1}}}{{dt}} = hA\left( {{T_o} - {T_1}} \right) + \frac{{{T_2} - {T_1}}}{R}
+\end{equation}
+
+\begin{equation}
+C\frac{{d{T_2}}}{{dt}} = hA\left( {{T_i} - {T_2}} \right) + \frac{{{T_1} - {T_2}}}{R}
+\end{equation}
+
+\begin{equation}
+{q''_i} = h\left( {{T_i} - {T_2}} \right)
+\end{equation}
+
+\begin{equation}
+{q''_o} = h\left( {{T_1} - {T_o}} \right)
+\end{equation}
+
+where:~~~~~~~~ \(R = \frac{\ell }{{kA}}\) ~ , thermal resistance
+
+\(C = \frac{{\rho {c_p}\ell A}}{2}\) ~, thermal capacitance
+
+\({T_o}\) = outside temperature
+
+\({T_i}\) = inside temperature
+
+\({T_1}\) = temperature of node 1
+
+\({T_2}\) = temperature of node 2
+
+and
+
+A is the area of the surface exposed to the environmental temperatures.
+
+In matrix format:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{\frac{{d{T_1}}}{{dt}}}\\ {\frac{{d{T_2}}}{{dt}}}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{ - 1}}{{RC}} - \frac{{hA}}{C}}&{\frac{1}{{RC}}}\\ {\frac{1}{{RC}}}&{\frac{{ - 1}}{{RC}} - \frac{{hA}}{C}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ {{T_2}}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{\frac{{hA}}{C}}&0\\0&{\frac{{hA}}{C}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\end{array}} \right]
+\end{equation}
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{{q''}_i}}\\ {{{q''}_o}}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}0&{ - h}\\h&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ {{T_2}}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0&h\\ { - h}&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\end{array}} \right]
+\end{equation}
+
+\begin{figure}[hbtp] % fig 268
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6008.svg.png}
+\caption{Two Node State Space Example \protect \label{fig:two-node-state-space-example}}
+\end{figure}
+
+The important aspect of the state space technique is that through the use of relatively simple matrix algebra the state space variables (nodal temperatures) can be eliminated to arrive at a matrix equation that gives the outputs (heat fluxes) as a function of the inputs (environmental temperatures) only.~ This eliminates the need to solve for roots in the Laplace domain.~ In addition, the resulting matrix form has more physical meaning than complex functions required by the Laplace transform method.~ The current version of EnergyPlus uses the state space method for computing CTFs.
+
+The accuracy of the state space method of calculating CTFs has been addressed in the literature.~ Ceylan and Myers (1980) compared the response predicted by the state space method to various other solution techniques including an analytical solution.~ Their results showed that for an adequate number of nodes the state space method computed a heat flux at the surface of a simple one layer slab within 1\% of the analytical solution.~ Ouyang and Haghighat (1991) made a direct comparison between the Laplace and state space methods.~ For a wall composed of insulation between two layers of concrete, they found almost no difference in the response factors calculated by each method.
+
+\subsubsection{Extension of Time Series Solutions to Include Heat Sources and Obtain Internal Temperatures}\label{extension-of-time-series-solutions-to-include-heat-sources-and-obtain-internal-temperatures}
+
+\subsubsection{Laplace Transform Formulation}\label{laplace-transform-formulation-1}
+
+Degiovanni (1988) proposed two methodologies for including sources or sinks in the Laplace Transform Formulation.~ The first method shows how a source that varies as a function of time and location can be incorporated.~ The resulting equations involve some fairly complicated terms including spatial derivatives.
+
+The second method that will be analyzed in more detail involves the addition of a source or sink at the interface between two layers.~ The derivation of the necessary equations is begun by analyzing the simple two layer element shown in Figure 269.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image6009.png}
+\caption{}
+\end{figure}
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_2}\left( s \right)}\\ {{q_2}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_3}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+Figure 269.~ Two Layer Example for Deriving the Laplace Transform Extension to Include Sources and Sinks
+
+For the first layer, it was determined that in the Laplace domain
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_2}\left( s \right)}\\ {{q_2}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+For the second layer:
+
+To link the two layers and include the heat source between them, the following substitution is made:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_2}\left( s \right)}\\ {{q_2}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{T_{2 + }}\left( s \right)}\\ {{q_{2 + }}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+which results in:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left\{ {\left[ {\begin{array}{*{20}{c}}{{T_{2 + }}\left( s \right)}\\ {{q_{2 + }}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]} \right\}
+\end{equation}
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left\{ {\left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_3}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]} \right\}
+\end{equation}
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_3}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+While Degiovanni concludes with this formula, some insight into what the generic equation for an element that has n layers might look like is gained by working with Equation .~ If a layer is added to the left of the first layer, the entire right hand side of Equation is multiplied by the transmission matrix of the new layer.~ Conversely, if a layer is added to the right of the second layer in Figure 269, the vector containing the Laplace transform of the temperature and heat flux at interface 3 is replaced by the product of the transmission matrix of the new layer and the vector for temperature and heat flux at the next interface, and the term dealing with the heat source is not affected.~ The general equation for a building element with n layers and m layers between the left hand surface and the heat source can be derived as:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left( {\prod\limits_{i = 1}^n {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]} } \right)\left[ {\begin{array}{*{20}{c}}{{T_{n + 1}}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right] + \left( {\prod\limits_{i = 1}^m {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]} } \right)\left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+or in more compact form:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{A\left( s \right)}&{B\left( s \right)}\\ {C\left( s \right)}&{D\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_{n + 1}}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{a\left( s \right)}&{b\left( s \right)}\\ {c\left( s \right)}&{d\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]
+\end{equation}
+
+where:~ \(\left[ {\begin{array}{*{20}{c}}{A\left( s \right)}&{B\left( s \right)}\\ {C\left( s \right)}&{D\left( s \right)}\end{array}} \right] = \prod\limits_{i = 1}^n {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]}\) ~~and~ \(\left[ {\begin{array}{*{20}{c}}{a\left( s \right)}&{b\left( s \right)}\\ {c\left( s \right)}&{d\left( s \right)}\end{array}} \right] = \prod\limits_{i = 1}^m {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]}\) ~.
+
+Next, Equation must be rearranged to match the form of Equation , which relates the heat flux at both sides of the element to the temperature at each side.~ The matrix equation that is obtained shows that:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{q_1}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{D\left( s \right)}}{{B\left( s \right)}}}&{\frac{{ - 1}}{{B\left( s \right)}}}\\ {\frac{1}{{B\left( s \right)}}}&{\frac{{ - A\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{T_{n + 1}}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{d\left( s \right) - \frac{{D\left( s \right)b\left( s \right)}}{{B\left( s \right)}}}\\ {\frac{{b\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {{q_{source}}\left( s \right)} \right]
+\end{equation}
+
+This equation bears a striking resemblance to Equation .~ If the source term in Equation is dropped, then the equation is identical to Equation .~ This result conforms with the superposition principle which was used to develop the conduction transfer functions from the summation of a series of triangular pulses or ramp sets.~ Now, the effect of the heat source is simply added to the response to the temperature inputs.
+
+While Equation is correct for any single or multilayered element, the first term in the heat source transmission matrix does not appear to match the compactness of the other terms in the matrix equation.~ It can be shown (see Strand 1995: equations 32 through 42 which detail this derivation) that the heat source transmission term for a two-layer problem reduces to
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{q_1}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{D\left( s \right)}}{{B\left( s \right)}}}&{\frac{{ - 1}}{{B\left( s \right)}}}\\ {\frac{1}{{B\left( s \right)}}}&{\frac{{ - A\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{T_3}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{\frac{{{B_2}\left( s \right)}}{{B\left( s \right)}}}\\ {\frac{{{B_1}\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {{q_{source}}\left( s \right)} \right]
+\end{equation}
+
+If this is extended to a slab with n layers and a source between the m and m+1 layers, the general matrix equation for obtaining heat source transfer functions using the Laplace transform method is:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{q_1}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{D\left( s \right)}}{{B\left( s \right)}}}&{\frac{{ - 1}}{{B\left( s \right)}}}\\ {\frac{1}{{B\left( s \right)}}}&{\frac{{ - A\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{T_{n + 1}}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{\frac{{\bar b\left( s \right)}}{{B\left( s \right)}}}\\ {\frac{{b\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {{q_{source}}\left( s \right)} \right]
+\end{equation}
+
+where: \(\left[ {\begin{array}{*{20}{c}}{A\left( s \right)}&{B\left( s \right)}\\ {C\left( s \right)}&{D\left( s \right)}\end{array}} \right] = \prod\limits_{i = 1}^n {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]}\) ~,
+
+\(\left[ {\begin{array}{*{20}{c}}{a\left( s \right)}&{b\left( s \right)}\\ {c\left( s \right)}&{d\left( s \right)}\end{array}} \right] = \prod\limits_{i = 1}^m {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]}\) ~, and
+
+\(\left[ {\begin{array}{*{20}{c}}{\bar a\left( s \right)}&{\bar b\left( s \right)}\\ {\bar c\left( s \right)}&{\bar d\left( s \right)}\end{array}} \right] = \prod\limits_{i = m + 1}^n {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]}\) ~.
+
+At first glance, the terms in the heat source transmission matrix may appear to be reversed.~ It is expected that only the layers to the left of the source will affect q1(s), but the presence of \(\bar b\left( s \right)\) ~in the element multiplied by qsource(s) to obtain q1(s) seems to be contradictory.~ In fact, the entire term, \({{\bar b\left( s \right)} \mathord{\left/ {\vphantom {{\bar b\left( s \right)} {B\left( s \right)}}} \right. } {B\left( s \right)}}\) , must be analyzed to determine the effect of qsource(s) on q1(s).~ In essence, the appearance of \(\bar b\left( s \right)\) ~removes the effects of the layers to the right of the source from B(s) leaving only the influence of the layers to the left of the source.~ The form displayed by Equation is, however, extremely convenient because the terms in the heat source transmission matrix have the same denominators, and thus roots, as the terms in the temperature transmission matrix.~ Thus, the same roots that are calculated for the CTFs can be used for the QTFs, saving a considerable amount of computer time during the calculation of the transfer functions.
+
+Once Equation is inverted from the Laplace domain back into the time domain, the combined CTF--QTF solution takes the following form:
+
+\begin{equation}
+{q''_{i,t}} = \sum\limits_{m = 1}^M {{X_m}{T_{i,t - m + 1}}}  - \sum\limits_{m = 1}^M {{Y_m}{T_{o,t - m + 1}}}  + \sum\limits_{m = 1}^k {{F_m}{{q''}_{i,t - m}}}  + \sum\limits_{m = 1}^M {{W_m}{q_{source,t - m + 1}}}
+\end{equation}
+
+This relation is identical to Equation except for the presence of the QTF series that takes the heat source or sink into account.
+
+\subsubsection{State Space Formulation}\label{state-space-formulation-1}
+
+The two-node example introduced by Seem (1987) can be utilized to examine the extension of the state space method to include heat sources or sinks.~ Figure~\ref{fig:two-node-state-space-example-with-a-heat} shows the simple two node network with a heat source added at node 1.
+
+The nodal equations for the finite difference network shown in Figure~\ref{fig:two-node-state-space-example-with-a-heat} are:
+
+\begin{equation}
+C\frac{{d{T_1}}}{{dt}} = hA\left( {{T_o} - {T_1}} \right) + \frac{{{T_2} - {T_1}}}{R} + {q_{source}}A
+\end{equation}
+
+\begin{equation}
+C\frac{{d{T_2}}}{{dt}} = hA\left( {{T_i} - {T_2}} \right) + \frac{{{T_1} - {T_2}}}{R}
+\end{equation}
+
+\begin{equation}
+{q''_i} = h\left( {{T_i} - {T_2}} \right)
+\end{equation}
+
+\begin{equation}
+{q''_o} = h\left( {{T_1} - {T_o}} \right)
+\end{equation}
+
+\begin{figure}[hbtp] % fig 270
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6034.svg.png}
+\caption{Two Node State Space Example with a Heat Source \protect \label{fig:two-node-state-space-example-with-a-heat}}
+\end{figure}
+
+In obtaining the matrix equivalent for this set of equations, it should be noted that the source term is not a constant but rather an input that varies with time.~ Thus, it must be grouped with the environmental temperatures as inputs.~ The resulting matrix equations take the following form:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{\frac{{d{T_1}}}{{dt}}}\\ {\frac{{d{T_2}}}{{dt}}}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{ - 1}}{{RC}} - \frac{{hA}}{C}}&{\frac{1}{{RC}}}\\ {\frac{1}{{RC}}}&{\frac{{ - 1}}{{RC}} - \frac{{hA}}{C}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ {{T_2}}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{\frac{{hA}}{C}}&0&{\frac{A}{C}}\\0&{\frac{{hA}}{C}}&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\\ {{q_{source}}}\end{array}} \right]
+\end{equation}
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{{q''}_1}}\\ {{{q''}_2}}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}0&{ - h}\\h&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ {{T_2}}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0&h&0\\ { - h}&0&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\\ {{q_{source}}}\end{array}} \right]
+\end{equation}
+
+Equation appears to suggest that the source term has no direct effect on the heat flux at either side of the element because its coefficients are zero.~ This is not the case.~ Equation only relates variables that have a direct influence on heat flux.~ So, while Ti~has no direct influence on\({q''_o}\) , it does have an indirect influence through the nodal network.~ The same would hold for the influence of qsource.
+
+If this analysis is extended to a finite difference network with n nodes, the corresponding matrix equations can be shown to be:
+
+\begin{equation}
+\frac{{d\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right]}}{{dt}} = \left[ A \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right] + \left[ B \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\\ {{q_{source}}}\end{array}} \right]
+\end{equation}
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{{q''}_i}}\\ {{{q''}_o}}\end{array}} \right] = \left[ C \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right] + \left[ D \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\\ {{q_{source}}}\end{array}} \right]
+\end{equation}
+
+The influence of the heat source is also confirmed by the final solution form, which is identical to the Laplace transform result shown in Equation .~ As with the Laplace solution method, the state space method results in a set of QTFs that relate the heat source at the current time step and several previous time steps to the current heat flux at the surface of the element.
+
+Other similarities between the two solution methods are evident.~ It is interesting to note that as with the Laplace method there is no alteration of the CTFs calculated by the state space method.~ Thus, the principle of superposition is still valid.~ Furthermore, the introduction of the source term did not substantially increase the computing effort required to calculate the additional transfer functions.~ In the Laplace method, this was shown by the common roots, B(s), shared by both the CTFs and the QTFs.~ In the state space method, it can be noted that the A matrices in Equations and are identical.~ Since the state space method requires the inversion and the exponentiation of the A matrix only, the additional QTF terms will not require a substantial amount of additional computing time for their calculation.
+
+\subsubsection{Determination of Internal Temperatures}\label{determination-of-internal-temperatures}
+
+One aspect of low temperature radiant systems that has not been addressed to this point is the appropriateness of specifying the effect of the system on slab response via a heat source term.~ For a heating system that employs electrical resistance heating, the use of a heat source as the input variable is logical.~ The heat produced by such a system can easily be related to the current passing through the heating wire.~ However, for a hydronic heating or cooling system, the known quantity is not heat but rather the temperature of the water being sent to the building element.
+
+The use of a temperature to simulate the presence of a heating or cooling system presents one major obstacle.~ When fluid is not being circulated, there is no readily available temperature value available for use as an input variable.
+
+In a hydronic system, a link between the fluid temperature being sent to the slab and the heat delivered to the slab exist.~ The most effective way of relating these two variables is to consider the slab to be a heat exchanger.~ Using heat exchanger relationships, an equation could then be formulated to obtain the heat delivered to the slab based on the inlet fluid temperature.
+
+Most heat exchangers are used to thermally link two fluids.~ In the case of a hydronic radiant system, there is only one fluid and a stationary solid.~ Presumably, if the inlet fluid temperature, the system geometry, and the solid temperature are known, then the outlet temperature and thus the heat transfer to the building element can be computed.~ This leads to an interesting question:~ what is the solid temperature?
+
+By definition, for one dimensional conduction heat transfer, the solid temperature is the temperature of the building element at the depth where the hydronic loop is located.~ Typically, this temperature is not known because it is not needed.~ The goal of both methods of calculating CTFs was the elimination of internal temperatures that were not needed for the simulation.~ For a hydronic system, it is necessary to extract this information to solve for the heat source term.~ Two methods of accomplishing this are described below.
+
+Returning to the two layer example shown in Figure 269, it can be shown that the final solution form in the time domain for the slab with a source at the interface between the two layers is:
+
+\begin{equation}
+{q''_{1,t}} = \sum\limits_{m = 1}^M {{X_{k,m}}{T_{1,t - m + 1}}}  - \sum\limits_{m = 1}^M {{Y_{k,m}}{T_{3,t - m + 1}}}  + \sum\limits_{m = 1}^k {{F_m}{{q''}_{1,t - m}}}  + \sum\limits_{m = 1}^M {{W_m}{q_{source,t - m + 1}}}
+\end{equation}
+
+A similar equation could be written for the response of the first layer in absence of any source term and is given by:
+
+\begin{equation}
+{q''_{1,t}} = \sum\limits_{m = 1}^M {{x_{k,m}}{T_{1,t - m + 1}}}  - \sum\limits_{m = 1}^M {{y_{k,m}}{T_{2,t - m + 1}}}  + \sum\limits_{m = 1}^k {{f_m}{{q''}_{1,t - m}}}
+\end{equation}
+
+While the current temperature at the interface is not known, presumably the previous values of this parameter will be known.~ In addition, the temperatures and the flux histories at surface 1 are also know.~ The unknowns in Equation are the current heat flux at surface 1 and the temperature at surface 2.~ However, Equation does define the current value of the heat flux at surface 1 based on temperature, heat flux, and heat source histories.~ Thus, if this value is used in Equation , the only remaining unknown in this equation is the current temperature at surface 2, the surface where the heat source or sink is present.~ Rearranging Equation provides an equation from which the temperature at the source location may be calculated:
+
+\begin{equation}
+{T_{2,t}} = \sum\limits_{m = 1}^M {{{\bar X}_{k,m}}{T_{1,t - m + 1}}}  - \sum\limits_{m = 1}^{M - 1} {{{\bar Y}_{k,m}}{T_{2,t - m}}}  + \sum\limits_{m = 1}^{k + 1} {{{\bar F}_m}{{q''}_{1,t - m + 1}}}
+\end{equation}
+
+where the new coefficients are obtained from the standard conduction transfer functions for the first layer via the following equations:
+
+\begin{equation}
+{\bar X_{k,m}} = \frac{{{x_{k,m}}}}{{{y_1}}}\left( {m = 1, \cdots ,M} \right)
+\end{equation}
+
+\begin{equation}
+{\bar Y_{k,m}} = \frac{{{y_{k,m + 1}}}}{{{y_1}}}\left( {m = 1, \cdots ,M - 1} \right)
+\end{equation}
+
+\begin{equation}
+{\bar F_1} = \frac{1}{{{y_1}}}
+\end{equation}
+
+\begin{equation}
+{\bar F_m} = \frac{{{f_{m - 1}}}}{{{y_1}}}\left( {m = 2, \cdots ,k + 1} \right)
+\end{equation}
+
+This system for backing out an internal temperature through the use of a second, rearranged CTF equation is valid regardless of whether the Laplace transform or state space method is utilized to calculate the CTFs and QTFs.~ The state space method, however, offers a more direct method of obtaining an internal temperature through its definition as an additional output variable.
+
+Consider again the state space example shown in Figure~\ref{fig:two-node-state-space-example-with-a-heat}.~ Two output variables were defined for this example: \({q''_i}\) ~and \({q''_o}\) .~ The temperature of the node where the source is present can also be defined as an output variable through the identity equation:
+
+\begin{equation}
+{T_1} = {T_1}
+\end{equation}
+
+When this equation for T1~is added to Equation , the resulting output matrix equation for the heat flux at both surfaces and the internal temperature is:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{{q''}_i}}\\ {{{q''}_o}}\\ {{T_1}}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}0&{ - h}\\h&0\\1&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ {{T_2}}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0&h&0\\ { - h}&0&0\\0&0&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_i}}\\ {{T_o}}\\ {{q_{source}}}\end{array}} \right]
+\end{equation}
+
+The only difference between this relation and Equation is the presence of T1~on both the right and left hand side of the equation.~ The dual role of T1~as a state variable and an output parameter may seem to contradict the goal of the state space method of eliminating the state variables.~ However, due to the flexibility of the formulation, nodal temperatures can be extracted in the same manner that any other output quantity would be obtained.~ For an element with n layers, Equation becomes:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{{{q''}_i}}\\ {{{q''}_o}}\\ {{T_s}}\end{array}} \right] = \left[ C \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right] + \left[ D \right]\left[ {\begin{array}{*{20}{c}}{{T_i}}\\ {{T_o}}\\ {{q_{source}}}\end{array}} \right]
+\end{equation}
+
+where Ts~is the temperature of the node where the heat source or sink is present.~ The transfer function equation for the calculation of Ts~that results from Equation is identical in form to Equation :
+
+\begin{equation}
+{T_{s,t}} = \sum\limits_{m = 1}^M {{x_{k,m}}{T_{i,t - m + 1}}}  - \sum\limits_{m = 1}^M {{y_{k,m}}{T_{o,t - m + 1}}}  + \sum\limits_{m = 1}^k {{f_m}{T_{s,t - m}}}  + \sum\limits_{m = 1}^M {{w_m}{q_{source,t - m + 1}}}
+\end{equation}
+
+Instead of the flux at either side of the element characterized as a function of temperature, flux, and source history terms, the temperature at the source location is related to source and temperature histories including histories of Ts.~ The validity of these internal temperature calculation methods as well as heat source transfer functions in general will be discussed in the next chapter.
+
+\subsubsection{Low Temperature Radiant System Controls}\label{low-temperature-radiant-system-controls}
+
+The use of this equation allows the low temperature radiant system to be handled like any other surface within the heat balance framework.~ Heat balances at the inside and outside surfaces take on the same form as other surfaces, and the participation of the radiant system in the radiation balance within the space and thermal comfort models is automatically included.~ Thus, the radiant system model is fully integrated into the heat balance, and any improvements that are made in areas such as convection coefficients, shading models, etc. are immediately available to the radiant system as part of the overall heat balance solution.
+
+Once the transient nature of the system is accounted for, one must then turn to the next difficult issue: controls.~ Controls are problematic for almost any simulation program.~ The problem is not whether something can be simulated because typically a simulation program offers the ability to experiment with many different control strategies.~ Rather, the problem is typically the diversity of controls that are implemented and keeping the controls that can be simulated up to date.~ EnergyPlus offers two different control schemes: variable flow (ZoneHVAC:LowTemperatureRadiant:VariableFlow) and variable temperature (ZoneHVAC:LowTemperatureRadiant:ConstantFlow).~ The control strategies are different enough that they were developed as separate system types.~ More details of the controls are described below.
+
+The controls for variable flow low temperature radiant systems within EnergyPlus are fairly simple though there is some flexibility through the use of schedules.~ The program user is allowed to define a setpoint temperature as well as a throttling range through which the system varies the flow rate of water (or current) to the system from zero to the user defined maximum flow rate.~ The flow rate is varied linearly with the flow reaching 50\% of the maximum when the controlling temperature reaches the setpoint temperature.~ Setpoint temperatures can be varied on an hourly basis throughout the year if desired.~ The controlling temperature can be the mean air temperature, the mean radiant temperature, or the operative temperature of the zone, and this choice is also left to the user's discretion.~ (Operative temperature for radiant system controls is the average of MAT and MRT.)~ Since flow rate is varied, there is no explicit control on the inlet water temperature or mixing to achieve some inlet water temperature in a hydronic system.~ However, the user does have the ability to specify on an hourly basis through a schedule the temperature of the water that would be supplied to the radiant system.
+
+Graphical descriptions of the controls for the low temperature radiant system model in EnergyPlus are shown in Figure~\ref{fig:variable-flow-low-temperature-radiant-system} for a hydronic system.~ In a system that uses electric resistance heating, the power or heat addition to the system varies in a manner similar to mass flow rate variation shown in Figure~\ref{fig:variable-flow-low-temperature-radiant-system}.
+
+In the constant flow-variable temperature systems, the controls are also considered piecewise linear functions, but in this case the user selects both the control temperatures and the water temperatures via schedules.~ This offers greater flexibility for defining how the radiant system operates though it may not model every situation.~ Figure~\ref{fig:variable-temperature-low-temperature-radiant} shows how the ``desired'' inlet water temperature is controlled based on user schedules.~ The user has the ability to specify the high and low water and control temperature schedules for heating and cooling (separately; a total of eight temperature schedules).~ Note that this inlet temperature is a ``desired'' inlet temperature in that there is no guarantee that the system will provide water to the system at that temperature.~ The model includes a local loop that attempts to meet this demand temperature through mixing and recirculation.
+
+\begin{figure}[hbtp] % fig 271
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6053.png}
+\caption{Variable Flow Low Temperature Radiant System Controls \protect \label{fig:variable-flow-low-temperature-radiant-system}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 272
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6054.png}
+\caption{Variable Temperature Low Temperature Radiant System Controls \protect \label{fig:variable-temperature-low-temperature-radiant}}
+\end{figure}
+
+The constant flow (variable temperature) low temperature radiant system model is actually a combination of mixing valves, a pump (constant speed, but the maximum flow can be modified by a schedule), and the radiant system (surface, panel, or group of surfaces/panels).~ This is connected to the main loop through the standard inlet connections as shown in Figure~\ref{fig:variable-temperature-low-temperature-radiant-001}.~ The system controls determine the desired inlet temperature and system flow rate while loop controls determine the flow rate and temperature of the loop.~ Note that pump heat also factors into the model through a simple constant speed pump model and user input.
+
+There are four possible conditions (separate for heating and cooling).~ First, if the loop has adequate temperature and flow to meet system requests, then the model sets the radiant system inlet temperature and controls to the desired values based on the controls and simulates.~ This is the best condition and recirculation and bypass amounts are adjusted accordingly based on radiant system outlet temperatures.~ Second, if the loop temperature is adequate but the loop flow rate is less than the radiant system flow rate, we may or may not be able to meet the desired inlet temperature since recirculation might lower the temperature below the desired temperature.~ In this second case, the model first simulates the radiant system with the desired conditions and then resimulates it to solve for the actual inlet temperature (see later in this section) if it cannot achieve the desired inlet temperature.~ Third, if the loop flow is greater than the radiant flow but the temperature of the loop is not adequate, then there is no amount of mixing that will solve this problem.~ All of the radiant flow comes from the loop and the loop temperature (after pump heat addition) becomes the radiant system inlet regardless of the temperature controls.~ Finally, if both the temperature and the flow of the loop are inadequate, then the model simply solves for the actual radiant system inlet temperature and does not try to meet the controls (merely tries to get as close as physically possible given the loop conditions).
+
+\begin{figure}[hbtp] % fig 273
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6055.png}
+\caption{Variable Temperature Low Temperature Radiant System Component Details \protect \label{fig:variable-temperature-low-temperature-radiant-001}}
+\end{figure}
+
+One remaining challenge is the merging of the low temperature radiant system model with an integrated building simulation program.~ In the past, most simulation programs have simulated the building envelope, the space conditioning systems, and the central plant equipment in three separate steps.~ While this had some advantages and was partly due to a lack of computing capacity, the large drawback for this arrangement is that there is no feedback from the space conditioning system or central plant response to the building conditions.~ Thus, if the system or plant was undersized, it was reported as an ``unmet load'' and does not affect the temperatures experienced within the building.~ IBLAST, a predecessor (Taylor 1991) to EnergyPlus, resolved this issue by integrating all three major components of a building simulation and thus allowing feedback between the equipment and the building envelope.
+
+This integration was not a trivial task and required that the systems be simulated at shorter time steps in some cases to maintain solution stability.~ In essence, the system simulation will shorten its time step whenever it senses that conditions are changing too rapidly.~ While this is effective in maintaining solution stability, it can present problems for a radiant system.~ The radiant system has either a direct or an indirect impact on the surfaces within a building.~ So, it must be simulated with the building envelope.~ Yet, it is also a space conditioning system that must act on the space like any other system and thus must also be simulated at the system time step, which can be less than the building time step and can also vary within EnergyPlus.
+
+This issue was handled using a multi-step approach.~ In EnergyPlus, the heat balance is always simulated first.~ When this happens, the radiant system is temporarily shut-off to find how the building would respond if there was no heat source/sink.~ Then, as the system and plant are simulated at multiple shorter time steps, the radiant system is allowed to operate per the controls specified by the user.~ Flow rate is allowed to vary at each system time step, and the radiant system model is simulated at each time step as if the current flow rate was being used throughout the entire zone time step.~ This means that each time the heat source/sink in the radiant system is varied during the system simulation the zone heat balance must be recomputed to see what the reaction of the rest of the zone is to this change in the conditions of one (or more) of the surfaces.
+
+In reality, this is not physically correct because each change in the flow rate throughout the system simulation will have an impact on the system time steps remaining before the heat balance is simulated during the next zone time step.~ Yet, other approaches to solving the mismatch between the system and the zone response of radiant systems are not feasible.~ One could force the system to run at the same time step as the zone, but this could result in instabilities in other types of systems that might be present in the simulation.~ On the other hand, one could try to force the zone to run at the shorter time steps of the system, but this could lead to instability within the heat balance due to limits on the precision of the conduction transfer function coefficients.
+
+Despite the fact that the simulation algorithm described above may either over- or under-predict system response dependent on how the system has been controlled in previous system time steps, it is reasonable to expect that the effect of these variations will balance out over time even though it might lead to slightly inaccurate results at any particular system time step.~ The long-term approach is also in view in the final simulation step at each zone time step.~ After the system has simulated through enough system time steps to equal a zone time step, the radiant system will rerun the heat balance using the average heat source/sink over all of the system time steps during the past zone time step.~ This maintains the conservation of energy within the heat balance simulation over the zone time steps and defines more appropriate temperature and flux histories at each surface that are critical to the success of a conduction transfer function based solution.~ A graphical picture of this somewhat complex multiple step simulation is shown in the figure below.
+
+\begin{figure}[hbtp] % fig 274
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6056.png}
+\caption{Resolution of Radiant System Response at Varying Time Steps \protect \label{fig:resolution-of-radiant-system-response-at}}
+\end{figure}
+
+\subsubsection{Heat Exchanger Formulation for Hydronic Systems}\label{heat-exchanger-formulation-for-hydronic-systems}
+
+As has been mentioned previously, the actual heat transferred between the building element and the hydronic loop is related to the temperature of the building element at the source location as well as the water system inlet and outlet temperatures.~ In EnergyPlus, it is assumed that the inlet temperature to the slab (defined by a user schedule and the plant simulation) and the mass flow rate (determined by the control algorithm) are known and that the remaining parameters must be calculated.~ However, the heat balance equations require the heat transferred to the building element from the water loop in order to calculate the heat transferred from the element to the building environment.
+
+Even though systems defined by this model can vary somewhat, the same characteristic link between the system variables exist.~ For modeling purposes, the overall water/slab system can be thought of as a heat exchanger.~ While in principle there are two alternative heat exchanger methodologies, it is more convenient to use the effectiveness-NTU method in this case.
+
+Several assumptions will be incorporated into the heat exchanger analysis.~ It is assumed that the building element that contains the hydronic loop is stationary and that its temperature along the length of the tubing is constant.~ The latter part of this assumption stems from assumptions made in both the one and two dimensional heat source transfer function derivations.~ In either case, the source was added at a single node that was characterized by a single temperature.~ For consistency, this assumption must be made again in the heat exchanger analysis.~ Another assumption for the current EnergyPlus model is that the fluid in the tubing is water.~ Additionally, it is assumed that the thermal properties of the water do not vary significantly over the length of the tubing and that the water flows at a constant flow rate.~ Finally, the temperature at the inside surface of the water tubing is assumed to be equal to the temperature at the source location.~ In other words, it is assumed that the water tubing itself has no appreciable effect on the heat transfer process being modeled.
+
+Using these assumptions and the effectiveness-NTU heat exchanger algorithm, several equations can be defined which establish the relationship between the heat source and the water temperatures.~ First, a heat balance on the water loop results in:
+
+\begin{equation}
+q = {\left( {\dot m{c_p}} \right)_{water}}\left( {{T_{wi}} - {T_{wo}}} \right)
+\end{equation}
+
+where q is the energy transferred between the water loop and the building element, \(\dot m\) ~is the mass flow rate of the water, cp~is the specific heat of the water, Twi~is the inlet water temperature, and Two~is the outlet water temperature.
+
+The maximum amount of heat transfer that is possible according to the Second Law of Thermodynamics is:
+
+\begin{equation}
+{q_{\max }} = {\left( {\dot m{c_p}} \right)_{water}}\left( {{T_{wi}} - {T_s}} \right)
+\end{equation}
+
+where qmax~is the maximum amount of energy transfer that is possible and Ts~is the temperature at the source location.
+
+The effectiveness of the heat exchanger, e, is defined as the ratio of the actual energy transfer to the maximum possible, or:
+
+\begin{equation}
+\varepsilon  \equiv \frac{q}{{{q_{\max }}}}
+\end{equation}
+
+For a heat exchanger where one fluid is stationary, the effectiveness can be related to NTU, the number of transfer units, by the following equation (Incropera and DeWitt 1985):
+
+\begin{equation}
+\varepsilon  = 1 - {e^{ - NTU}}
+\end{equation}
+
+where NTU is defined by:
+
+\begin{equation}
+NTU \equiv \frac{{UA}}{{{{\left( {\dot m{c_p}} \right)}_{water}}}}
+\end{equation}
+
+Since the water tubes were assumed to have no effect on the heat transfer process, the only term present in the overall heat transfer coefficient, UA, is a convection term.~ Thus, the equation for UA is:
+
+\begin{equation}
+UA = h\left( {\pi DL} \right)
+\end{equation}
+
+where h is the convection coefficient, D is the interior tube diameter, and L is the total length of the tube.
+
+The convection coefficient can be obtained from internal flow correlations that relate the Nusselt dimensionless number to other flow properties.~ For laminar flow in a tube of constant surface temperature, the Nusselt number is defined by:
+
+\begin{equation}
+N{u_D} = \frac{{hD}}{k} = 3.66
+\end{equation}
+
+where k is the thermal conductivity of the water.
+
+For turbulent internal flow, the Colburn equation can be used to define the Nusselt number:
+
+\begin{equation}
+N{u_D} = \frac{{hD}}{k} = 0.023{\mathop{\rm Re}\nolimits}_D^{{4 \mathord{\left/ {\vphantom {4 5}} \right. } 5}}{\Pr ^{{1 \mathord{\left/ {\vphantom {1 3}} \right. } 3}}}
+\end{equation}
+
+where Pr is the Prandtl number of water and ReD~is the Reynolds number which is defined by:
+
+\begin{equation}
+{{\mathop{\rm Re}\nolimits}_D} = \frac{{4\dot m}}{{\pi \mu D}}
+\end{equation}
+
+The parameter m is the absolute viscosity of water.~ For internal pipe flow, the flow is assumed to be turbulent for ReD~≥ 2300.
+
+Knowledge of the flow conditions allows Equations through to be calculated.~ This essentially eliminates e as an unknown in Equation .~ The controls and the plant define the water mass flow rate and the inlet water temperature, leaving two equations (Equations and ) and three unknowns.~ The third equation that can be used in conjunction with Equations and is Equation , which is the CTF/QTF equation for the temperature at the source location.
+
+Knowing the inlet water temperature and water mass flow rate, the calculation procedure is somewhat involved and requires, in addition to Equations , , and , the use of a modified form of Equation .~ Equation is the standard conduction transfer function formula for a building element with an embedded source/sink of heat.~ In EnergyPlus, the surface flux on the left hand side of the equation is replaced with a surface heat balance:
+
+\begin{equation}
+\left[ {\begin{array}{*{20}{c}}{Surface}\\ {Heat}\\ {Balance}\end{array}} \right] = \sum\limits_{m = 1}^M {{X_{k,m}}{T_{1,t - m + 1}}}  - \sum\limits_{m = 1}^M {{Y_{k,m}}{T_{3,t - m + 1}}}  + \sum\limits_{m = 1}^k {{F_m}{{q''}_{1,t - m}}}  + \sum\limits_{m = 1}^M {{W_m}{q_{source,t - m + 1}}}
+\end{equation}
+
+The surface heat balance includes terms for incident solar energy, radiation heat transfer from internal heat sources such as lights and electrical equipment, radiation between surfaces using Hottel's Gray Interchange concept, and convection to the surrounding air.~ The presence of the surface temperature in the heat balance does not pose any problems since Equation will be rearranged to solve for this temperature.~ Since the radiation heat balance is dependent on conditions at the other surfaces, an iteration loop is required to provide a more accurate estimate of the radiative exchange within the building.~ This is not the case with the mean air temperature.~ An assumption of the heat balance is that the mean temperature of the surrounding air is equal to the final air temperature of the previous time step.~ Using this estimate in the heat balance avoids a second iterative loop around the radiative iteration loop.
+
+Thus, the terms of the heat balance on the left hand side of the equation have been set with the only unknown quantity being Ti, the inside surface temperature at the current time step.~ On the right hand side of Equation , most of the terms are already defined since they depend on known values from previous time steps (temperature, flux, and source histories).~ The only terms which are not defined are the inside surface temperature (Ti), outside surface temperature (To), and internal heat source/sink (qsource) of the current time step.
+
+The outside surface temperature will depend on the type of environment to which it is exposed.~ For example, if the surface is a slab on grade floor, the outside surface temperature is defined as ground temperature and does not require an outside surface heat balance.~ If the element is an interior surface which has both surfaces exposed to the same air space, the outside surface temperature is redefined to be equal to the inside surface temperature.~ In cases where the outside surface temperature is not simply defined such as a surface exposed to the exterior environment, a heat balance similar to Equation is required to define the outside surface temperature.~ However, to again avoid iteration, the heat balance equation for the outside surface assumes that conditions at the inside surface were the same as the previous time step.~ In most cases, since the influence of the current inside surface temperature on the outside surface temperature is very small, this is a valid assumption.~ In cases were the inside surface temperature has a significant effect, an approximate inside surface heat balance which defines the inside surface temperature is used.~ This approximate inside balance uses mean air and radiant temperatures from the previous time step.
+
+At this point in the simulation algorithm then, all of the terms in Equation have been defined except the value at the current time step of the inside surface temperature and the heat source/sink.~ Thus, Equation can be rewritten in a simpler form:
+
+\begin{equation}
+{T_{i,t}} = {C_1} + {C_2}{q_{source,t}}
+\end{equation}
+
+where the variable C1~includes surface heat balance and past history terms as well as the influence of the current outside temperature.~ The term C2~will depend on the heat source transfer function term and the coefficients of terms linked directly to Ti,t.
+
+Equation , which was the CTF/QTF equation for the temperature at the source location, can be simplified in a similar manner.~ Grouping the temperature and source history terms which are known quantities together with the effect of the outside surface temperature which is defined as described above, the original equation
+
+\begin{equation}
+{T_{s,t}} = \sum\limits_{m = 1}^M {{x_{k,m}}{T_{i,t - m + 1}}}  - \sum\limits_{m = 1}^M {{y_{k,m}}{T_{o,t - m + 1}}}  + \sum\limits_{m = 1}^k {{f_m}{T_{s,t - m}}}  + \sum\limits_{m = 1}^M {{w_m}{q_{source,t - m + 1}}}
+\end{equation}
+
+can be reduced to:
+
+\begin{equation}
+{T_s} = {C_3} + {C_4}{q_{source,t}} + {C_5}{T_{i,t}}
+\end{equation}
+
+where C3~includes all of the history terms and the effect of the current outside temperature, C4~is the heat source transfer function for the current time step, and C5~is the conduction transfer function for the inside surface temperature at the current time step.
+
+Substituting Equation into Equation and noting that qsource,t~is the same quantity as q in Equations and results in:
+
+\begin{equation}
+{T_s} = {C_3} + {C_4}q + {C_5}\left( {{C_1} + {C_2}q} \right)
+\end{equation}
+
+When this equation is combined with Equation , the heat source, which results from a known water inlet temperature, can be shown to be:
+
+\begin{equation}
+q = \frac{{{T_{wi}} - {C_3} - {C_1}{C_5}}}{{\frac{1}{{\varepsilon {{\left( {\dot m{c_p}} \right)}_{water}}}} + {C_4} + {C_2}{C_5}}}
+\end{equation}
+
+With both q and Twi~known, it is a trivial matter to calculate Two~and Ts~from Equations and , respectively.~ Even though the coefficients in Equation are fairly complex, the final equation relating the heat source directly to inlet water temperature is compact and does not require any iteration.~ As with flux control, once the heat source/sink is defined, the inside surface heat balance can be performed to determine the surface temperatures.
+
+It should be noted that Equations through are a slight simplification of the actual implementation in EnergyPlus.~ The development shown above follows the heat balance conventions that assume previous values of the inside temperature to calculate the outside temperature.~ This, in reality, is not necessary and since the radiant system can be significantly influenced by the delay that such an assumption might cause, the initial implementation of radiant systems in EnergyPlus used a development (shown below) that does not lag either the inside or the outside surface temperature.~ In effect, we can establish three basic equations for the temperature at the inside and outside surface as well as at the location of the heat source/sink:
+
+\begin{equation}
+{T_{inside}} = {C_a} + {C_b}{T_{outside}} + {C_C}q''
+\end{equation}
+
+\begin{equation}
+{T_{outside}} = {C_d} + {C_e}{T_{inside}} + {C_f}q''
+\end{equation}
+
+\begin{equation}
+{T_{source}} = {C_g} + {C_h}q'' + {C_i}{T_{inside}} + {C_j}{T_{outside}}
+\end{equation}
+
+where: T\(_{inside}\) is the temperature at the inside surface
+
+T\(_{outside}\) is the temperature at the outside surface
+
+T\(_{source}\) is the temperature within the radiant system at the location of the source/sink
+
+C\(_{a}\) is all of the other terms in the inside heat balance (solar, LW exchange, conduction history terms, etc.)
+
+C\(_{b}\) is the current cross CTF term
+
+C\(_{c}\) is the QTF inside term for the current heat source/sink
+
+C\(_{d}\) is all of the other terms in the outside heat balance (solar, LW exchange, conduction history terms, etc.)
+
+C\(_{e}\) is the current cross CTF term (should be equal to Cb)
+
+C\(_{f}\) is the QTF outside term for the current heat source/sink
+
+C\(_{g}\) is the summation of all temperature and source history terms at the source/sink location
+
+C\(_{h}\) is the QTF term at the source/sink location for the current heat source/sink
+
+C\(_{i}\) is the CTF inside term for the current inside surface temperature
+
+C\(_{j}\) is the CTF outside term for the current outside surface temperature
+
+Equations and above can be solved to remove the other surface temperature. Substituting the new equations for T\(_{inside}\) and T\(_{outside}\) as a function of C and q" into the equation for Tsource and simplifying results in the following equation:
+
+\begin{equation}
+{T_{source}} = {C_k} + {C_l}q''
+\end{equation}
+
+where:~~~~~~~~ \({C_k} = {C_g} + \frac{{{C_i}\left( {{C_a} + {C_b}{C_d}} \right) + {C_j}\left( {{C_d} + {C_e}{C_a}} \right)}}{{1 - {C_e}{C_b}}}\)
+
+\begin{equation}
+{C_l} = {C_h} + \frac{{{C_i}\left( {{C_c} + {C_b}{C_f}} \right) + {C_j}\left( {{C_f} + {C_e}{C_c}} \right)}}{{1 - {C_e}{C_b}}}
+\end{equation}
+
+Combining this with heat exchanger analysis as shown above, we eventually arrive at the following equation to relate the flux to the slab to the water inlet temperature and mass flow rate:
+
+\begin{equation}
+q'' = \frac{{{T_{water,in}} - {C_k}}}{{\frac{{{C_l}}}{A} + \frac{1}{{\varepsilon {{\left( {\dot m{c_p}} \right)}_{water}}}}}}
+\end{equation}
+
+which includes all of the inside and outside heat balance terms (``hidden'' in the C\(_{k}\) and C\(_{l}\) coefficients).~ Once the flux to the slab is known, the remaining terms of interest (outlet water temperature, inside and outside surface temperatures, etc.) can be calculated using the relatively simpler equations shown above.
+
+Note that the above development is valid for both the hydronic (variable flow) low temperature radiant system and for constant flow (variable temperature) low temperature radiant systems where the inlet temperature is known (based on controls).~ However, when due to loop conditions and the presence of recirculation, it is not possible to know the inlet temperature to the radiant system without simulating it, we must either iterate or perform more mathematics to arrive at the inlet temperature.~ The implementation in EnergyPlus chose to avoid iteration and solved for the inlet temperature as shown in the next paragraphs.
+
+The previous equation combines with the following equation which is valid for an surface in the current radiant system:
+
+\begin{equation}
+{{\rm{q}}_{\rm{j}}}{\rm{  =  }}{{\rm{\dot m}}_{\rm{j}}}{{\rm{c}}_{\rm{p}}}{\rm{(}}{{\rm{T}}_{{\rm{water,in}}}}{\rm{  -  }}{{\rm{T}}_{{\rm{water,out,j}}}}{\rm{)}}
+\end{equation}
+
+where q\(_{j}\) is the heat transfer to the jth surface in the radiant system, m\(_{j}\) is the mass flow rate only to this surface, and T\(_{water,out,j}\) is the outlet temperature for the jth surface.~ Combining the previous two equations results in:
+
+\begin{equation}
+{\rm{(}}{{\rm{T}}_{{\rm{water,in}}}}{\rm{  -  }}{{\rm{T}}_{{\rm{water,out,j}}}}{\rm{)}} = \frac{{{\varepsilon_j}\left( {{{\rm{T}}_{{\rm{water,in}}}} - {C_{k,j}}} \right)}}{{1 + \frac{{{\varepsilon_j}{{\dot m}_j}{c_p}{C_{l,j}}}}{A}}}
+\end{equation}
+
+If for each surface in the radiant system, we let:
+
+\begin{equation}
+{{\rm{C}}_{m,j}} = \frac{{{\varepsilon_j}}}{{1 + \frac{{{\varepsilon_j}{{\dot m}_j}{c_p}{C_{l,j}}}}{A}}}
+\end{equation}
+
+then the previous equations because the slightly less complex:
+
+\begin{equation}
+{\rm{(}}{{\rm{T}}_{{\rm{water,in}}}}{\rm{  -  }}{{\rm{T}}_{{\rm{water,out,j}}}}{\rm{)}} = {C_{m,j}}\left( {{{\rm{T}}_{{\rm{water,in}}}} - {C_{k,j}}} \right)
+\end{equation}
+
+Rearranging to obtain the outlet temperature for the jth surface:
+
+\begin{equation}
+{{\rm{T}}_{{\rm{water,out,j}}}} = \left( {1 - {C_{m,j}}} \right){{\rm{T}}_{{\rm{water,in}}}} + {C_{m,j}}{C_{k,j}}
+\end{equation}
+
+The overall outlet temperature from the radiant system is just a simple mixing of all of the surface outlet temperatures based on flow fraction and results in T\(_{water,out}\).
+
+An energy balance on the mixing valve-pump group results in the following equation that relates the radiant system inlet temperature (T\(_{water,in}\)) to the loop inlet water temperature (T\(_{loop,in}\)), the radiant system outlet temperature (T\(_{water,out}\)), and the pump heat addition:
+
+\begin{equation}
+{{\rm{T}}_{{\rm{water,in}}}} = \frac{{{{\dot m}_{loop}}}}{{{{\dot m}_{system}}}}{{\rm{T}}_{{\rm{loop,in}}}} + \frac{{{{\dot m}_{recirc}}}}{{{{\dot m}_{system}}}}{{\rm{T}}_{{\rm{water,out}}}} + \frac{{PumpHeat}}{{{{\dot m}_{system}}{c_p}}}
+\end{equation}
+
+Plugging in the definition of T\(_{water,out}\) based on the summation of T\(_{water,out,j}\) equations results in:
+
+\begin{equation}
+{{\rm{T}}_{{\rm{water,in}}}} = \frac{{LoopTerm + {\mathop{\rm Re}\nolimits} circTerm}}{{TwiCoeff}}
+\end{equation}
+
+where:
+
+\begin{equation}
+{\rm{L}}oopTerm = \frac{{{{\dot m}_{loop}}}}{{{{\dot m}_{system}}}}{{\rm{T}}_{{\rm{loop,in}}}} + \frac{{PumpHeat}}{{{{\dot m}_{system}}{c_p}}}
+\end{equation}
+
+\begin{equation}
+{\mathop{\rm Re}\nolimits} circTerm = \frac{{{{\dot m}_{recirc}}}}{{{{\dot m}_{system}}}}\sum\limits_{\rm{j}} {{\rm{FlowFractio}}{{\rm{n}}_{\rm{j}}}{{\rm{T}}_{{\rm{water,out,j}}}}}
+\end{equation}
+
+\begin{equation}
+TwiCoeff = \left( {1 - \frac{{{{\dot m}_{recirc}}}}{{{{\dot m}_{system}}}}} \right)\sum\limits_{\rm{j}} {\left[ {{\rm{FlowFractio}}{{\rm{n}}_{\rm{j}}}\left( {1 - {C_{m,j}}} \right)} \right]}
+\end{equation}
+
+Once the actual water inlet temperature is calculated with this equation, it is then possible to calculate individual outlet temperatures for each surface, the overall outlet temperature, and finally all of the necessary flow and loop quantities.~ This procedure avoids iteration but is somewhat complex to follow.~ However, this second mathematical process is only needed for select cases of the constant flow radiant system when the inlet temperature is not known explicitly.~ With the proper establishment of input data, it can be avoided.
+
+\textbf{NOTE:} In some ``low-energy'' applications, it is possible that during cooling mode the elevated water temperatures may result in a heat source (or net heating) to the radiant system.~ To avoid heating the slab when cooling is desired, EnergyPlus performs a temperature limit check.~ If heating would result during cooling mode or cooling during heating mode, the model will cut-off the flow rate until the inlet water temperature will produce the proper effect.
+
+\subsection{High Temperature Radiant Heater Model}\label{high-temperature-radiant-heater-model}
+
+The input object ZoneHVAC:HighTemperatureRadiant provides a model for a high temperature radiant heater that is intended to encapsulate an entire class of heating devices that seek to heat the occupants within a zone by direct radiation.~ This encompasses a wide variety of heaters including both gas-fired and electric.~ In most cases, the heater appears much like a lamp or a tube that is suspended from the ceiling of a space, and the surface temperatures are high enough that the heaters must be a safe distance away from the occupied portion of the space for safety concerns.
+
+In EnergyPlus, the high temperature radiant heater model allows the user a reasonable amount of flexibility.~ Rather than specifying an exact location for the radiant heater(s), the user is allowed to specify the percentage of heat leaving the heater as radiation and then on which surfaces this radiation is incident.~ In addition, the user is also allowed the ability to define what fraction of radiation leaving the heater is incident directly on a person within the zone for thermal comfort purposes.~ This amount of heat is then used in the thermal comfort models as shown in Equations for Fanger, for Pierce Two-Node and for KSU Two-node. These equations are similar in form to the equation promoted by Fanger (1970).~ The input parameters for the high temperature radiant heater model are shown in Figure 275.
+
+\begin{equation}
+{T_{radiant}} = {\left[ {\left( {T_{MRT}^4} \right) + \left( {\frac{{{Q_{heater \to person}}}}{{\sigma {A_{person}}}}} \right)} \right]^{0.25}}
+\end{equation}
+
+HIGH TEMP RADIANT SYSTEM,! Program keyword for high temp. radiant heaters
+
+~ Zone 1 Radiant Heater, ! Zone name
+
+~ Radiant Operation,~~~~ ! Availability schedule
+
+~ SHOP ZONE,~~~~~~~~~~~~ ! Zone name (name of zone system is serving)
+
+~ 10000,~~~~~~~~~~~~~~~~ ! maximum power input (in Watts)
+
+~ GAS,~~~~~~~~~~~~~~~~~~ ! type of heater (either gas or electric)
+
+~ 0.85,~~~~~~~~~~~~~~~~~ ! combustion efficiency (ignored for elec. heaters)
+
+~ 0.75,~~~~~~~~~~~ ~~~~~~! fraction radiant
+
+~ 0.05,~~~~~~~~~~~~~~~~~ ! fraction latent
+
+~ 0.05,~~~~~~~~~~~~~~~~~ ! fraction lost
+
+~ OPERATIVE,~~~~~~~~~~~~ ! temperature control type (MAT, MRT also possible)
+
+~ 2.0 ,~~~~~~~~~~~~~~~~~ ! heating throttling range (in C)
+
+~ Heating Setpoints,~~~~ ! schedule of heating setpoint temperatures
+
+~ 0.05,~~~~~~~~~~~~~~~~~ ! fraction of radiant energy to people
+
+~ Zn001:Flr001, 0.75,~~~ ! surface/fraction of radiant energy incident on it
+
+~ Zn001:Wall001, 0.05,~~ ! surface/fraction of radiant energy incident on it
+
+~ Zn001:Wall002, 0.05,~~ ! surface/fraction of radiant energy incident on it
+
+~ Zn001:Wall003, 0.05,~~ ! surface/fraction of radiant energy incident on it
+
+~ Zn001:Wall004, 0.05;~~ ! surface/fraction of radiant energy incident on it
+
+Figure 275.~ Input Description for High Temperature Radiant Heaters
+
+The input for the high temperature radiant heater has two additive relationships that are assumed.~ First, the fractions of radiant, convective, latent, and lost heat must sum to unity.~ The user is required to enter the fractions radiant, latent, and lost with the remainder assumed to be convective energy.~ The fraction latent is added to the latent energy balance and will affect moisture levels within the zone.~ The fraction lost is assumed to have no impact on the energy balance of the zone and is assumed to be lost or vented to the exterior environment.
+
+The second additive relationship is within the distribution of the radiant fraction.~ This energy is distributed to people and to the surfaces within the zone.~ The sum of all of these distribution fractions (the last six lines of input shown in Figure 275) must sum to unity.~ Note that each high temperature radiant heater is allowed to distribute energy to up to 20 surfaces and that radiant energy placed on a surface using these distribution fractions is assumed to be completely absorbed.~ Thus, the distribution fractions should also take into account any differences in long wavelength absorptivity among the surfaces.
+
+Several things should be noted about the fraction of heat that is radiated directly to people.~ This parameter is somewhat sensitive and will have a direct impact on the thermal comfort models.~ This is exactly the intent of the high temperature radiant heaters; however, one must use caution when determining this fraction since overestimation of this number might lead to predictions of thermal comfort where in fact it does not exist.~ In addition, this fraction of radiant energy to people does not have a direct impact on any of the surface heat balances.~ The thermal comfort energy balance is completely separate from and has no bearing on the zone air or the surface heat balances.~ Thus, in order to not ``lose'' this amount of energy from the perspective of the zone air or the surface heat balances, the model assumes that any radiation from the high temperature radiant heater that is incident directly on people is accounted for in the thermal comfort model using Equation but is also assumed to be added to the zone air heat balance via convection from people to the surrounding air.~ This guarantees that the people within the space feel the direct radiative effect of the heaters and that this quantity of energy is not ``lost'' within the heat balance routines.
+
+Many of the control and integration aspects of the high temperature radiant system model in EnergyPlus are very similar to the low temperature radiant system model.~ The controls are the same as shown in ``Figure~\ref{fig:variable-flow-low-temperature-radiant-system}.~ Variable Flow Low Temperature Radiant System Controls'' where the amount of heat generated by the radiant heater varies as a function of the difference between the controlling and the setpoint temperatures.~ As with the low temperature radiant system, the controlling temperature is allowed to be the mean air, the mean radiant, or the operative temperature, and the setpoint temperature is allowed to vary hourly based on a user defined schedule.~ (Operative temperature for radiant system controls is the average of MAT and MRT.)~ Also, since the high temperature radiant heater has a direct impact on the surfaces within a zone, the surface heat balances are recalculated to determine an approximate response to the radiation from the heater.~ A final ``average'' heat balance calculation is done after all of the system time steps have been simulated to maintain continuity within the surface heat balances.~ The algorithm shown in ``Figure~\ref{fig:resolution-of-radiant-system-response-at}.~ Resolution of Radiant System Response at Varying Time Steps is also used for high temperature radiant heaters.
+
+\subsubsection{References}\label{references-039}
+
+Ceylan, H.T. and G.E. Myers.~ 1980.~ Long-time solutions to heat conduction transients with time-dependent inputs.~ ASME Journal of Heat Transfer, Volume 102, Number 1, pp.~115-120.
+
+Degiovanni, A.~ 1988.~ Conduction dans un ``mur'' multicouche avec sources:~ extension de la notion de quadripole.~ International Journal of Heat and Mass Transfer, Volume 31, Number 3, pp.~553-557.
+
+Fanger, P.O. 1970. Thermal Comfort-Analysis and Applications in Environmental Engineering, Danish Technical Press, Copenhagen.
+
+Hittle, D.C.~ 1981.~ Calculating building heating and cooling loads using the frequency response of multilayered slabs.~ Ph.D.~Thesis, Department of Mechanical and Industrial Engineering, University of Illinois at Urbana-Champaign and Technical Manuscript E-169, United States Army Construction Engineering Research Laboratory, Champaign, IL.
+
+Hittle, D.C. and R. Bishop.~ 1983.~ An improved root-finding procedure for use in calculating transient heat flow through multilayered slabs.~ International Journal of Heat and Mass Transfer, Volume 26, Number 11, pp.~1685-1693.
+
+Hottel, H.C. and A.F. Sarofim. 1967. Radiative Transfer, McGraw-Hill, New York.
+
+Incropera, F.P. and D.P. DeWitt.~ 1985.~ Introduction to Heat Transfer.~ New York:~ John Wiley \& Sons.
+
+Lee, J. and R.K. Strand. 2001. ``An Analysis of the Effect of the Building Envelope on Thermal Comfort using the EnergyPlus Program'', submitted for publication in the proceedings of the 2001 ACSA (Association of Collegiate Schools of Architecture) Technology Conference, Austin, TX.
+
+Liesen, R.J. and C.O. Pedersen. 1997. ``An Evaluation of Inside Surface Heat Balance Models for Cooling Load Calculations'', ASHRAE Transactions, Volume 103, Part 2.
+
+Maloney, D. 1987. ``Development of a radiant heater model and the incorporation of thermal comfort considerations into the BLAST energy analysis program'', M.S. thesis, University of Illinois at Urbana-Champaign, Department of Mechanical and Industrial Engineering.
+
+McClellan, T.M. and C.O. Pedersen. 1997. ``Investigation of Outside Heat Balance Models for Use in a Heat Balance Cooling Load Calculation Procedure'', ASHRAE Transactions, Volume 103, Part 2.
+
+Pedersen, C.O., D.E. Fisher, and R.J. Liesen. 1997. ``Development of a Heat Balance Procedure for Cooling Loads'', ASHRAE Transactions, Volume 103, Part 2.
+
+Pedersen, C.O., D.E. Fisher, J.D. Spitler, and R.J. Liesen. 1998. Cooling and Heating Load Calculation Principles, ASHRAE.
+
+Seem, J.E.~ 1987. ~Modeling of heat transfer in buildings.~ Ph.D.~Thesis, University of Wisconsin-Madison.
+
+Strand, R.K., and C.O. Pedersen. 1994. ``Analytical verification of heat source transfer functions'', First Joint Conference of International Simulation Societies, Zürich, Switzerland.
+
+Strand, R.K. 1995. ``Heat source transfer functions and their application to low temperature radiant heating systems'', Ph.D.~dissertation, University of Illinois at Urbana-Champaign, Department of Mechanical and Industrial Engineering.
+
+Strand, R.K. and C.O. Pedersen. 1997. ``Implementation of a Radiant Heating and Cooling Model into an Integrated Building Energy Analysis Program'', ASHRAE Transactions, Volume 103, Part 1.
+
+Strand, R.K. and C.O. Pedersen. 2001. ``Modularization and Simulation Techniques for Heat Balance Based Energy and Load Calculation Programs: the Experience of the ASHRAE LOADS Toolkit and EnergyPlus'', International Building Performance Simulation Association, Conference Proceedings of Building Simulation 2001, Rio de Janeiro, Brazil.
+
+Taylor, R.D., C.O. Pedersen, D. Fisher, R. Liesen, and L. Lawrie. 1991. ``Impact of simultaneous simulation of building and mechanical systems in heat balance based energy analysis programs on system response and control'', International Building Performance Simulation Association, Conference Proceedings of Building Simulation 1991, Nice, France.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/refrigeration-equipment.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/refrigeration-equipment.tex
new file mode 100644
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+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/refrigeration-equipment.tex
@@ -0,0 +1,2122 @@
+\section{Refrigeration Equipment }\label{refrigeration-equipment}
+
+\subsection{Overview}\label{overview-023}
+
+EnergyPlus can model refrigerated case equipment consisting of a compressor rack, multiple refrigerated cases and walk-in coolers, secondary loop equipment, and~ optional heat reclaim air and water heating coils. The refrigerated case equipment models perform four major functions:
+
+n~calculate the electric consumption of refrigerated cases and walk-in coolers connected to a compressor rack
+
+n~determine the impact of refrigerated cases and walk-in coolers on zone cooling and dehumidification loads (i.e., case credits), including the effects of HVAC duct configuration
+
+n~calculate the electric consumption and COP of the compressor rack, and the electric and water (if applicable) consumption related to cooling the compressor rack's condenser.
+
+n~determine the total amount of heat rejected by the compressor rack's condenser and store this information for use by waste heat recovery models (e.g., using Desuperheater heating coil (object: Coil:Heating:Desuperheater) as an air reheat coil for high humidity control in a supermarket)
+
+The case and walk-in models account for nearly all performance aspects of typical supermarket refrigeration equipment. Refrigerated case and walk-in performance are based on the combined effects of evaporator load, fan operation, lighting, defrost type, and anti-sweat heater operation. Optional air and water heating coils can be modeled to reclaim available waste heat (superheat) from the compressor rack.
+
+The user has two options when describing the balance of the system. Energy used to cool the condenser is simulated in both approaches. The simplest option is to use a compressor rack object, combining the compressors and condenser into a single unit with the performance determined by the heat rejection environment and the total case load. An example schematic of a compressor rack system is shown in Figure~\ref{fig:typical-compressor-rack-equipment-schematic} below.
+
+A detailed refrigeration system object models compressor and condenser performance separately. The detailed refrigeration system also includes the ability to transfer refrigeration load from one system to another using subcoolers, cascade condensers, and secondary loops. An example schematic of the detailed refrigeration system is shown in Figure~\ref{fig:typical-detailed-refrigeration-system} below. Subcooler \#2 is shown twice on~ Figure~\ref{fig:typical-detailed-refrigeration-system} because it represents a liquid suction heat exchanger. This type of subcooler uses the cool suction gas to subcool the warmer condensed liquid. Subcoolers \#1 and \#3 on Figure~\ref{fig:typical-detailed-refrigeration-system} represent mechanical subcoolers. These subcoolers are used to subcool the condensate on a lower-temperature system using the cold liquid refrigerant from a higher temperature system. On this example, only subcoolers \#1 and \#2 would be defined as a part of the refrigeration system. However, subcooler \#3 would place a refrigerating load, similar to the load of a refrigerated case, on the system.
+
+\begin{figure}[hbtp] % fig 276
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6091.png}
+\caption{Typical Compressor Rack Equipment Schematic \protect \label{fig:typical-compressor-rack-equipment-schematic}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 277
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6092.png}
+\caption{Typical Detailed Refrigeration System Equipment Schematic \protect \label{fig:typical-detailed-refrigeration-system}}
+\end{figure}
+
+Four classes of secondary refrigeration loops can be modeled:
+
+n~a separate water loop is used to remove heat rejected by the condenser,
+
+n~a lower-temperature refrigeration system rejects heat to a higher-temperature refrigeration system via a cascade condenser,
+
+n~a fluid, such as a brine or glycol solution, is cooled in a secondary evaporator and is then circulated to chill the refrigerated cases and walk-ins, and
+
+n~a refrigerant, such as CO\(_{2}\), is partially evaporated in the refrigerated cases and walk-ins in a liquid-overfeed circuit, and then condensed in a secondary evaporator.
+
+The first two classes of secondary loops are modeled using Refrigeration:System objects with Refrigeration:Condenser:WaterCooled and Refrigeration:Condenser:Cascade objects, respectively.~ Figure~\ref{fig:typical-detailed-refrigeration-system} shows how cascade condensers and secondary evaporators are treated as a refrigeration load on a primary detailed system. The second two classes are modeled with a Refrigeration:SecondarySystem object described later in this section.
+
+The compressor rack, detailed and secondary refrigeration systems, refrigerated case, and other component models are described below. The optional air and water heating coils are described elsewhere in this document (Ref. objects Coil:Heating:Desuperheater and Coil:WaterHeating:Desuperheater).
+
+\subsection{Refrigeration Compressor Racks}\label{refrigeration-compressor-racks}
+
+The refrigerated case compressor rack object works in conjunction with the refrigerated case and walk-in cooler objects (Refrigeration:Case and Refrigeration:WalkIn) to simulate the performance of a simple supermarket-type refrigeration system. This object (Refrigeration:CompressorRack) models the electric consumption of the rack compressors and the cooling of the compressor rack's condenser. Heat removed from the refrigerated cases and walk-ins and compressor/condenser fan heat can be rejected either outdoors or to a zone. Compressor rack condenser waste heat can also be reclaimed for use by an optional air heating coil (Ref. object Coil:Heating:Desuperheater) or by a user-defined plant water loop (Ref. object Coil:WaterHeating:Desuperheater).
+
+The performance of the compressor rack is simulated using the sum of the evaporator loads for all refrigerated cases and walk-ins connected to the rack. Whether a single refrigerated case is connected to a rack (e.g., stand-alone refrigerated case, meat cooler, or produce cooler) or several cases are connected to a rack, the rack electric consumption is calculated based on the total evaporator load for the connected cases and walk-ins and the coefficient of performance (COP) for the compressor rack. At least one refrigerated case or walk-in must be connected to the compressor rack. The model assumes the compressor rack has sufficient capacity to meet the connected refrigeration load for any simulation time step. Additionally, the model neglects compressor cycling losses at part-load conditions.
+
+For condenser heat rejection to the outdoors, condenser cooling can be modeled as dry air cooling, wet evaporative cooling, or water loop cooling. Using evaporative cooling rather than dry air cooling will allow for more efficient condenser heat rejection based on the entering air approaching the wet-bulb temperature rather than the dry-bulb temperature. Analyses under the International Energy Agency's (IEA) Heat Pumping Programme Annex 26 indicates that this measure can improve refrigeration system efficiency by up to 10\% (IEA 2003). The use of an evaporative-cooled condenser requires a water pump and, optionally, a basin sump water heater (to protect against freezing). Makeup water will also be required to replace that lost by evaporation. In colder climates, some evaporative-cooled condensers are drained for the winter months and run as dry air units. This scenario can be modeled by using an optional evaporative condenser availability schedule.
+
+The simulation of the evaporative cooled condenser utilizes an effective air dry-bulb temperature that is assumed to be the result of evaporation of water in the air stream (similar to object EvaporativeCooler:Direct:CelDekPad). As discussed below, this effective temperature is used by performance curves that are a function of temperature. While some designs of evaporative coolers use water film cascading across the condenser coil for evaporative cooling, the current model uses the effective temperature method as a surrogate for the more complex water film on coil calculations.
+
+If the condenser heat rejection is specified as water cooled, an appropriate plant water loop must be defined by the user (see documentation on \emph{Plant/Condenser Loops} for additional details about plant loops).~ This will include defining cooling supply components, such as pumps, water storage tanks, and cooling towers, as well as related branches, nodes, and connectors. The heat rejection from the refrigeration condenser is modeled as a cooling demand, which is satisfied by heat extraction devices (e.g., water tank and cooling tower) on the cooling supply side of a water loop. An example of such an arrangement is shown in Figure~\ref{fig:example-of-condenser-heat-recovery-to-water}.
+
+\begin{figure}[hbtp] % fig 278
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6093.png}
+\caption{Example Of Condenser Heat Recovery To Water Storage Tank \protect \label{fig:example-of-condenser-heat-recovery-to-water}}
+\end{figure}
+
+\subsubsection{Compressor Energy Use}\label{compressor-energy-use}
+
+Calculation of compressor rack electric power uses a simple model based on the total evaporator load (sum of the evaporator loads for all refrigerated cases and walk-ins connected to a rack) and the compressor rack operating COP which accounts for the air temperature entering the condenser:
+
+\begin{equation}
+CO{P_{operating}} = CO{P_{design}}\left( {COPfTemp} \right)
+\end{equation}
+
+where:
+
+\(CO{P_{operating}}\) ~~~~~~~~~~~ ~ = compressor coefficient of performance at actual operating conditions (W/W)
+
+\(CO{P_{design}}\) ~~ ~ = compressor coefficient of performance at design conditions (W/W)
+
+\(COPfTemp\) ~ = output of the normalized ``Compressor Rack COP as a Function of Temperature Curve'' (dimensionless)
+
+Because the COP curve is defined only as a function of the condensing temperature, it is important that this curve definition corresponds to the lowest evaporating temperature served by the compressor rack. The air temperature used to evaluate the ``Compressor Rack COP as a Function of Temperature Curve'' depends on where the compressor rack's condenser is located (Heat Rejection Location). When modeling condenser heat rejected directly to a zone (typical of a stand-alone packaged refrigerated case with integral condenser located in a building zone), the zone air dry-bulb temperature is used to calculate the change in compressor COP from the design value. If more than one refrigerated case and no walk-ins are attached to a compressor rack that rejects its condenser heat to a zone, then all cases served by this rack must reside in the same zone. When modeling a compressor rack serving at least one walk-in, OR with condenser heat rejected to outdoors, the refrigerated cases and walk-ins connected to this rack may be located in different zones. If the condenser type is specified as ``Air Cooled'', the outdoor air dry-bulb temperature is used to evaluate the ``Compressor Rack COP as a Function of Temperature Curve.''~ If the condenser type is specified as ``Evap Cooled'', the air temperature leaving the condenser is related to the effectiveness of the evaporative cooling system. If the evaporative process were 100\% effective, the effective temperature of air leaving the evaporative media would equal the air wet-bulb temperature. However, the efficiency of the direct evaporative process is typically less than 100\%, and the effective temperature leaving the condenser is determined by:
+
+\begin{equation}
+{T_{effective}} = {T_{owb}} + (1 - \varepsilon )*[{T_{odb}} - {T_{owb}}]
+\end{equation}
+
+where:
+
+\({T_{effective}}\) ~~~~~~ = effective dry-bulb temperature of air leaving the condenser cooling coil (°C)
+
+\({T_{owb}}\) ~~~~~~~~~~ = outdoor air wet-bulb temperature (°C)
+
+\({T_{odb}}\) ~~~~~~~~~~ = outdoor air dry-bulb temperature (°C)
+
+\(\varepsilon\) ~~~~~~~~~~~~~~ = evaporative condenser effectiveness.
+
+If the user is modeling an evaporative cooled condenser and is using COPfTemp curve data (e.g., manufacturer's data) based on wet-bulb temperature rather than dry-bulb temperature, the evaporative condenser effectiveness should be set to 1.0 for consistency.
+
+If the condenser is water cooled, the effective temperature experienced by the condenser is based on the return water temperature from the plant loop heat rejection system (e.g., cooling tower) that is defined by the user. This return water temperature is typically related to the outdoor ambient conditions at each time step.
+
+The electric power input to the rack compressor(s) is calculated for each simulation time step as the sum of the connected refrigerated case evaporator loads divided by the operating COP:
+
+\begin{equation}
+{P_{{\rm{rack}}}} = \frac{{\sum {{{\dot Q}_{case}} + \sum {{{\dot Q}_{walkin}}} } }}{{CO{P_{operating}}}}
+\end{equation}
+
+where:
+
+\({P_{rack}}\) ~ = output variable ``Refrigeration Compressor Rack Electric Power {[}W{]}'', electric power input to the rack compressor(s)
+
+\({\dot Q_{case}}\) ~ = evaporator load for each refrigerated case connected to the rack (W)
+
+\({\dot Q_{walkin}}\) = refrigeration load for each walk-in connected to the rack (W)
+
+\subsubsection{Condenser Heat Rejection, Energy Use, and Water Use}\label{condenser-heat-rejection-energy-use-and-water-use}
+
+The compressor rack can reject heat to an air-, water-, or evaporative-cooled condenser. The condenser type determines the heat rejection temperature used for the compressor rack COP calculation. The compressor rack also allows superheat heat reclaim and heat rejection to a conditioned zone.
+
+\paragraph{Condenser Fan Energy Use}\label{condenser-fan-energy-use}
+
+Condenser fan power for any simulation time step is calculated by multiplying the design fan power by the condenser fan power as a function of temperature curve.
+
+\begin{equation}
+{P_{CondFan}}\,\, = {P_{CondFan,design}}\left( {CondFanfTemp} \right)
+\end{equation}
+
+where:
+
+\({P_{CondFan}}\) ~~~~~~~~~~~~~~~~~ = output variable ``Refrigeration Compressor Rack Condenser Fan Electric Energy {[}W{]}''
+
+\({P_{CondFan,design}}\) ~~~~~~~~~~ = design condenser fan power (W)
+
+\(CondFanfTemp\) ~~~ = output of the optional ``Condenser Fan Power as a Function of Temperature Curve''
+
+Similar to the compressor rack energy use described above, the air temperature used to evaluate the ``Condenser Fan Power as a Function of Temperature Curve'' depends on where the condenser rack's condenser is located (i.e., zone air dry-bulb temperature if the condenser is located in a zone, outdoor air dry-bulb temperature if the condenser is located outdoors and is specified as air cooled, or effective temperature if the condenser is outdoors and is specified as evaporative cooled). If the sum of the evaporator loads for the refrigerated cases connected to the rack is equal to zero, the condenser fan power is set equal to zero. If the user does not provide a ``Condenser Fan Power as a Function of Temperature Curve'', then the model assumes the condenser fan power is at the design power level when any of the refrigerated cases connected to this rack are operating.
+
+If the user is modeling an evaporative cooled condenser and is using CondFanfTemp curve data based on wet-bulb temperature rather than dry-bulb temperature, the evaporative condenser effectiveness should be set to 1.0 for consistency.
+
+For a water cooled condenser, there is no fan load at the condenser (i.e., the~ water/refrigerant heat exchanger). Any fan load would be related to and accounted for at the heat rejection object (e.g., cooling tower).
+
+\paragraph{Superheat Reclaim Heating Coil}\label{superheat-reclaim-heating-coil}
+
+EnergyPlus can simulate waste heat being reclaimed from a compressor rack for use by a refrigerant-to-air or refrigerant to water heating coil. Heat reclaimed from the compressor rack is assumed to be recovered from the superheated refrigerant gas leaving the compressor(s) and does not directly impact the performance of the compressor rack or refrigerated cases connected to the rack. The total heat rejected by the condenser (in Watts) is calculated each time step as follows:
+
+\begin{equation}
+{\dot Q_{condenser}} = \left( {\sum {{{\dot Q}_{case}} + \left. {\sum {{{\dot Q}_{walkin}}} } \right)} } \right.\left( {1 + \left. {\frac{1}{{CO{P_{operating}}}}} \right)} \right.
+\end{equation}
+
+The heat reclaim heating coil is able to transfer a fixed percentage of this total amount of rejected energy (not to exceed 30\%) and use it to heat air and water. Refer to objects Coil:Heating:Desuperheater and Coil:WaterHeating:Desuperheater for a complete description of how these coils are modeled.
+
+NOTE: When modeling a heat reclaim coil, the heat rejection location in the Refrigeration:CompressorRack object must be ``Outdoors''. If the compressor rack heat rejection location is ``Zone'', the total amount of waste heat available for reclaim (e.g., by a desuperheater heating coil) is set to zero by the compressor rack object and the simulation proceeds.
+
+\paragraph{Heat Rejection to Zone}\label{heat-rejection-to-zone}
+
+The compressor rack model can simulate condenser heat being rejected to a zone. As explained previously, if this heat rejection option is selected then all refrigerated cases connected to the rack must be located in the same zone and a superheat heat reclaim heating coil can not be modeled (Ref. Superheat Reclaim Heating Coil).
+
+The refrigerated case and walk-in objects (Refrigeration:Case and Refrigeration:WalkIn) already calculate and report the sensible case credits which impact the zone air heat balance (Ref. Sensible Case Credits). When refrigerated cases and/or walk-ins are served by a compressor rack that rejects condenser waste heat directly to the zone (e.g., a stand-alone refrigerated case with integral compressor and condenser), this condenser waste heat also impacts the zone air heat balance and offsets some or all of the sensible case credits.
+
+If only cases are served, the amount of condenser waste heat rejected to the zone and/or the HVAC return air (zone return air path outlet node) is calculated and reported by the refrigerated case compressor rack object as follows:
+
+\begin{equation}
+{\dot Q_{Zone,heating}}\,\,\, = \,\,\,\frac{{\sum {\left( {{{\dot Q}_{case}}[1 - RAF]} \right)} }}{{\sum {\left( {{{\dot Q}_{case}}} \right)} }}\,\left( {{{\dot Q}_{condenser}}\,\, + \,\,{P_{CondFan}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{HVAC,heating}}\,\,\, = \,\,\left( {{{\dot Q}_{condenser}}\,\, + \,\,{P_{CondFan}}} \right) - \,{\dot Q_{zone,heating}}
+\end{equation}
+
+where:
+
+\({\dot Q_{Zone,heating}}\) = output variable ``Refrigeration Compressor Rack Zone Sensible Heating Rate {[}W{]} ``
+
+\emph{RAF}~~~~~~~~~~ = return air factor for each case connected to the rack (Ref. Figure~\ref{fig:return-air-factor-versus-under-case-hvac})
+
+\({\dot Q_{HVAC,heating}}\) = output variable ``Refrigeration Compressor Rack Return Air Sensible Heating Rate {[}W{]} ``
+
+If the HVAC system is off for a simulation time step (no return air mass flow), the rack condenser heat normally attributed to the HVAC return is set equal to zero and all condenser heat energy is applied to the zone air heat balance.
+
+If, however, walk-in cooler(s) are also served by this compressor rack, no condenser heat is rejected to the HVAC return air. For walk-in cooler(s), the user must specify the zone that accepts the condenser heat rejection (because walk-ins can exchange heat with multiple zones). In that case:
+
+\begin{equation}
+{\dot Q_{Zone,heating}} = {\dot Q_{condenser}} + {P_{CondFan}}
+\end{equation}
+
+\paragraph{Water Cooled Condenser}\label{water-cooled-condenser}
+
+If the refrigeration condenser is water cooled, a water plant loop must be defined in the input file. At a minimum, the loop must contain a pump and one or more heat sinks of sufficient capacity to remove the condenser heat load. In the system shown in Figure~\ref{fig:example-of-condenser-heat-recovery-to-water}, the heat sinks are the water heater tank and the cooling tower. The water pump in the loop can be either constant (Ref. Pump:ConstantSpeed)~ or variable speed (Ref. Pump:VariableSpeed). A variable speed pump permits the loop flow to vary and allows for a setpoint to be established on the condenser outlet water temperature. As the refrigeration condenser heat load varies through time, the speed of the pump can be adjusted to achieve a mass flow consistent with a desired outlet water temperature according to
+
+\begin{equation}
+m = \frac{{{Q_{condenser}}}}{{{c_p} \cdot ({T_{out}} - {T_{in}})}}
+\end{equation}
+
+where:
+
+\emph{m} ~~~~~~~~~~~~~ = mass flow in the water loop
+
+\emph{Q\(_{condenser}\)~~~~~~} = heat rejected by the condenser
+
+\emph{c\(_{p}\)~~} ~~~~~~~~~~~ = specific heat of water
+
+\emph{T\(_{out}\)~} ~~~~~~~~~~~ = desired water outlet temperature
+
+\emph{T\(_{in}\)~~~~~~~~~~~~~~ =} return water inlet temperature.
+
+The desired water outlet temperature is specified using a schedule, subject to a maximum water outlet temperature (input specified). The maximum temperature is typically defined by constraints on the refrigerant loop pressures and temperatures. The desired mass flow in the water loop to meet the temperature schedule is also compared to the user-supplied maximum flow rate. If the desired mass flow is greater than the maximum allowed flow, the flow rate is set to the maximum value and the resulting water outlet temperature is determined.
+
+The return water inlet temperature is a function of the cooling system defined by the user. A minimum return water temperature may need to be taken into consideration to prevent lowering the resulting refrigerant condensing pressure to the point that refrigerant expansion valve operation becomes impaired. When ambient conditions produce low temperature warnings based on the minimum return water temperature, an outlet temperature setpoint control may need to be placed on the water heat sink object (e.g., cooling tower) to keep the return water temperature above the minimum.
+
+If the water loop flow is constant (i.e., driven by a constant speed pump), then the outlet water temperature will vary with the amount of heat rejected by the condenser.~~~ Using the equation above, the resulting water outlet temperature is calculated as
+
+\begin{equation}
+{T_{out}} = \frac{{{Q_{condenser}}}}{{{c_p} \cdot m}} + {T_{in}}
+\end{equation}
+
+\paragraph{Evaporative Condenser Water Pump}\label{evaporative-condenser-water-pump}
+
+If the condenser type is specified as ``Evap Cooled'', a water pump is required to circulate water in the evaporative condenser. The pump power can be input directly or be autocalculated using a relationship of 0.004266 W per watt {[}15 W/ton{]} of rated total cooling capacity where the total cooling capacity is the sum of the rated total cooling capacities for the refrigeration load connected to this compressor rack. Following manufacturer's recommendations regarding the avoidance of scaling, the water pump does not cycle when there is no cooling demand (i.e., when the compressors are not running), but rather runs continuously. However, if the evaporative condenser availability schedule is set such that evaporative cooling is not available (e.g., during very cold months to avoid freezing), then the pump power consumption will be zero during that period.
+
+\paragraph{Evaporative Condenser Water Consumption}\label{evaporative-condenser-water-consumption}
+
+With evaporative cooling of the condenser's entering air, makeup water is needed to replenish the water lost due to evaporation. The quantity required is calculated as the product of the air mass flow rate and the difference between the entering and leaving air humidity ratio, divided by the density of water. The air mass flow rate is determined by multiplying the evaporative condenser air volume flow rate times the density of the entering air (i.e., at the condenser air inlet node if provided, or outdoor air conditions {[}e.g., no adjustment for height above ground{]} if the condenser air inlet node field is left blank). The volumetric air flow rate is either specified directly in the user input or is autocalculated using the relationship 0.000144 m\(^{3}\)/s per watt of rated total cooling capacity {[}850 cfm/ton{]} where the total cooling capacity is the sum of the rated total cooling capacities for the refrigerated cases and walk-ins connected to this compressor rack (Ref. Refrigeration:Case and Refrigeration:WalkIn). The air mass flow rate is multiplied by the variable \emph{CondFanfTemp}, described above, to simulate the modulation of air flow by the condenser fans (e.g., staging, multi-speed, or variable speed) as a function of temperature. Mathematically,
+
+\begin{equation}
+{\dot V_{evaporation,makeup}} = \frac{{{{\dot m}_{air}}\left( {CondFanfTemp} \right)({\omega_{air,outlet}} - {\omega_{air,inlet}})}}{{{\rho_{water}}}}
+\end{equation}
+
+where:
+
+\(\mathop {{{\dot V}_{evaporation,makeup}}}\limits^{}\) = Refrigeration Compressor Rack Evaporative Condenser Water Volume Flow Rate (m\(^{3}\)/s)
+
+\(\dot m_{air} = \) ~mass flow rate of air through the evaporative condenser (kg/s)
+
+\({\omega_{air,outlet}}\) ~ = humidity ratio of air leaving the evaporative media (kg\(_{water}\)/kg\(_{dry\\ air}\)) based on the effective dry-bulb temperature \emph{T\(_{effective}\)}, as described above, outdoor air wet-bulb temperature, and outdoor barometric pressure
+
+\({\omega_{air,inlet}}\) ~ = humidity ratio of inlet air (kg\(_{water}\)/kg\(_{dry\\ air}\)) based on conditions at the condenser air inlet node if provided, or outdoor air conditions (e.g., no adjustment for height above ground) if the condenser air inlet node field is left blank
+
+\({\rho_{water}}\) ~ = density of water evaluated at the effective air temperature (kg/m\(^{3}\))
+
+The source of the makeup water may be specified as a water storage tank. If not specified, the makeup water is assumed to come from the building mains (Ref. Water Mains Temperatures).
+
+\paragraph{Evaporative Condenser Basin Heater}\label{evaporative-condenser-basin-heater}
+
+In cold climates, a basin heater may be needed to prevent freezing of the evaporative cooling water. This feature is included in the model whereby an electric basin heater provides heat to the sump water only when the condenser cooling system is idle (i.e., no refrigeration load) and when the outdoor air dry-bulb temperature is below a user-specified setpoint. Since heat balances and basin water temperatures are not explicitly determined, a linear loading relationship, as a function of the difference in outdoor air dry-bulb temperature and the setpoint temperature, is used calculate the power demand at a given time step by the basin heater.
+
+\begin{equation}
+{P_{ba\sinh eater}} = {P_{heatercapacity}}*({T_{setpo{\mathop{\rm int}} }} - {T_{OutDb}})
+\end{equation}
+
+where:
+
+\({P_{ba\sinh eater}}\) = electric power demand for basin heater in current time step (W)
+
+\({P_{heatercapacity}}\) = electric heater capacity as a function of differential temperature (W/deg K)
+
+\({T_{setpo{\mathop{\rm int}} }}\) = setpoint temperature below which the heater turns on (°C)
+
+\({T_{OutDb}}\) ~ = outdoor air dry-bulb temperature (°C)
+
+A default value for the basin heater capacity of 200 W/deg K has been established based on manufacturer data.
+
+\paragraph{Evaporative Condenser Availability Schedule}\label{evaporative-condenser-availability-schedule}
+
+Some manufacturer's evaporative cooling systems for refrigeration condensers permit seasonal draining in the colder months and operation as an air-cooled system during that time. This optional feature is available through an availability schedule. This is important in climates subject to freezing weather in order to avoid excessive ice formation on the condenser surfaces and surroundings. (The Availability Schedule is the correct way to model the use of evaporative condensers in cold climates. However, some users may take a single input description and use it to model a building with a refrigeration system in a variety of climates. To avoid modeling the use of evaporative coolers in freezing weather, the code includes a cutout to switch to dry operation whenever the outdoor drybulb temperature drops below 4C.) During periods when evaporative cooling is not available, the outdoor condenser behaves as an air-cooled system with no water consumption or pump and basin heater loads. The effective temperature of air entering the condenser coil during this period (used to evaluate COPfTemp and CondFanfTemp) is equal to the outdoor air dry-bulb temperature at the condenser air inlet node if provided, or outdoor air conditions (e.g., no adjustment for height above ground) if the condenser air inlet node field is left blank.
+
+\subsection{Refrigerated Cases}\label{refrigerated-cases}
+
+The refrigerated case object (Refrigration:Case) works in conjunction with the compressor rack, detailed refrigeration system, or secondary refrigeration system object (Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem) to simulate the performance of a refrigerated case system. The refrigerated case model uses performance information at rated conditions along with performance curves for latent case credits and defrost heat load to determine performance at off-rated conditions. Energy use for lights, fans and anti-sweat heaters is modeled based on inputs for nominal power, schedules, and control type. The refrigerated case model accounts for the sensible and latent heat exchange with the surrounding environment (termed ``case credits'') which impacts the temperature and humidity in the zone where the case is located. The simplified model described here provides the flexibility to simulate a broad range of refrigerated case types.
+
+The total load on the refrigerated case evaporator is made up of various components:
+
+\begin{equation}
+{\dot Q_{case}} = {\dot Q_{walls}} + {\dot Q_{rad}} + {\dot Q_{{\rm{inf,sens}}}} + {\dot Q_{{\rm{inf,lat}}}} + {\dot Q_{lights}} + {\dot Q_{as}} + {\dot Q_{def}} + {\dot Q_{fan}} + {\dot Q_{restock}}
+\end{equation}
+
+where:
+
+\({\dot Q_{case}}\) ~~~ = total load on the refrigerated case evaporator (W)
+
+\({\dot Q_{walls}}\) ~~ = heat transfer through case walls due to the difference between the refrigerated case operating dry-bulb temperature and the zone air dry-bulb temperature (W)
+
+\({\dot Q_{rad}}\) ~~~~ = radiant heat transfer to the refrigerated case (W)
+
+\({\dot Q_{{\rm{inf,}}sens}}\) = sensible heat transfer by air infiltration to the refrigerated case through the air curtain or via door openings (W)
+
+\({\dot Q_{{\rm{inf,lat}}}}\) ~~ = latent heat transfer by air infiltration to the refrigerated case through the air curtain or via door openings (W)
+
+\({\dot Q_{lights}}\) ~~ = lighting heat load (W)
+
+\({\dot Q_{as}}\) ~~~~~ = anti-sweat heater load (W)
+
+\({\dot Q_{def}}\) ~~~~ = defrost heat load (W)
+
+\({\dot Q_{fan}}\) ~~~~ = fan heat load (W)
+
+\({\dot Q_{restock}}\) = sensible load on the refrigerated case due to restocking of products that are at a higher temperature than the case (W)
+
+The model assumes that these load components are known for a refrigerated case at rated ambient air conditions (typically 23.9ËšC {[}75ËšF{]} and 55\% relative humidity) and the specified case operating temperature. A combination of user input curves and fixed correlations (defined within EnergyPlus) adjust for case performance at off-rated conditions. Several of the load components are typically provided by the case manufacturer (e.g., total rated load, fan, lighting, anti-sweat heater, and defrost loads). The remaining load components are not usually provided by the manufacturer and must be estimated (heat conduction through case walls, radiation heat transfer, sensible/latent air infiltration, and restocking).
+
+For estimating the latent air infiltration load, the model requires that the user provide the latent heat ratio (LHR) for the refrigerated case at rated conditions. Research results are available to provide guidance in selecting this value (ASHRAE 2002, Howell 1993a, Howell 1993b). The rated LHR for refrigerated cases typically ranges from 0.1 to 0.3 depending on case configuration (e.g., glass door reach-in versus multi-deck open case) and case operating temperature.
+
+The case loads due to wall heat conduction, radiation, and sensible air infiltration are estimated by the model as a single lumped value (sensible case credits). The sensible case credits are calculated by subtracting the known loads at rated conditions (fan, lighting, anti-sweat heater, defrost and latent case credits) from the rated total cooling capacity of the case which is provided by the case manufacturer (\({\dot Q_{case,rated}}\) ).
+
+Using these assumptions and the schedule inputs provided by the user, the refrigerated case evaporator load components in Equation are determined for each simulation time step. The variation in certain loads with respect to changes in ambient air temperature and/or humidity (e.g., latent and sensible case credits, defrost load, and anti-sweat heater load) are factored into the calculation based on user-provided inputs or by the model itself.
+
+Whenever the total heat load on the case is greater than the available evaporator capacity, such as during defrost (when the evaporator capacity is set to zero) or restocking, the load is accumulated to be met during subsequent time steps. This accounts for the energy required to bring the case back down to the rated operating temperature even though the rise in case temperature during defrost or restocking is not explicitly modeled. Following defrost, it may take multiple time steps to meet this accumulated load.
+
+The specific calculations for case evaporator load components and electric power for these loads (as applicable) are provided below.
+
+\subsubsection{Case Evaporator Fan}\label{case-evaporator-fan}
+
+The refrigerated case evaporator fan electric power is calculated for each simulation time step as the product of the operating case fan power per unit length of case, the length of the refrigerated case, and the fraction of time that the case is not being defrosted. For cases with hot-gas or electric defrost (with or without temperature termination), the fan is disabled during the entire scheduled defrost drip-down time period. The evaporator fan operates continuously for off-cycle defrost or no defrost.
+
+\begin{equation}
+{P_{fan}}\,\,\,\, = \,\,\,\,{P'}_{fan,oper}\left( {{L_{case}}} \right)\left( {1 - SC{H_{defrost,dripdown}}} \right)
+\end{equation}
+
+where:
+
+\({P_{fan}}\) ~~~~~~~~~~ = output variable ``Refrigerated Case Evaporator Fan Electric Power {[}W{]}''
+
+\({P'}_{fan,oper}\) ~~~~ = operating case fan power per unit length (W/m)
+
+\({L_{case}}\) ~~~~~~~~~ = case length (m)
+
+\(SC{H_{defrost,dripdown}}\) = fraction of time case is being defrosted (0 to 1), including drip-down period (based on the defrost drip-down schedule) for hot-gas or electric defrost. For off-cycle defrost or no defrost, this value is set to zero for this calculation.
+
+The model assumes that the evaporator fan is entirely contained within the thermal envelope of the case, and that all fan power results in a direct heat load on the case evaporator:
+
+\begin{equation}
+{\dot Q_{fan}} = \,{P_{fan}}
+\end{equation}
+
+\subsubsection{Case Lighting}\label{case-lighting}
+
+The refrigerated case lighting electric power is calculated for each simulation time step as the product of the installed case lighting power per unit length of case, the lighting schedule value, and the length of the refrigerated case:
+
+\begin{equation}
+{P_{{\rm{lights}}}} = P{'_{{\rm{lights,  installed}}}}({L_{{\rm{case}}}})(SC{H_{{\rm{lights}}}})
+\end{equation}
+
+where:
+
+\({P_{lights}}\) ~~~~~~~~~ = output variable ``Refrigerated Case Lighting Electric Power {[}W{]}''
+
+\(P{'_{{\rm{lights, installed}}}}\) ~~~~~~~~~ = installed case lighting power per unit length (W/m)
+
+\(SC{H_{lights}}\) ~~~ = case lighting schedule value (0 to 1)
+
+A maximum schedule value of 1.0 means the lights are fully on at the installed case lighting power level. Schedule values of 0.0 indicate the lights are off and 0.5 at half-power.
+
+The user can specify the fraction of lighting energy that directly contributes to the case evaporator heat load:
+
+\begin{equation}
+{\dot Q_{lights}} = \,{P_{lights}}\left( {{F_l}} \right)
+\end{equation}
+
+where:
+
+\({F_l}\) ~ = fraction of lighting energy to case
+
+The remainder of the lighting energy (1 - \emph{F\(_{l}\)}) is a heating load to the zone where the case is located, which is discussed further in section Sensible Case Credits below. This fraction (1 - \emph{F\(_{l}\)}) can be used to represent lighting ballasts and/or bulbs located outside the air curtain of the refrigerated case.
+
+\subsubsection{Anti-Sweat Heater Performance}\label{anti-sweat-heater-performance}
+
+Anti-sweat heaters warm the refrigerated case rails or doors to provide protection from moisture condensation. Different anti-sweat heater control strategies are used depending on the case temperature and the type of anti-sweat heater installed. Several types of anti-sweat heater control strategies can be simulated with this model: constant, linear variation with ambient relative humidity or dewpoint temperature, and a theoretical model that determines the minimum anti-sweat heater power required to maintain the case surface just above the temperature where condensation would occur. Additionally, anti-sweat heater performance can be disregarded if the type of refrigerated case does not warrant its use. For the control strategies described below (except ``None'' and ``Constant Method''), the model does not allow the anti-sweat heater power to be less than the minimum power nor greater than the case anti-sweat heater power specified by the user. Each anti-sweat heater control type is described in detail below.
+
+\paragraph{None}\label{none}
+
+Used for refrigerated cases that do not require an anti-sweat heater.
+
+\begin{equation}
+{\dot Q_{as}} = 0
+\end{equation}
+
+where:
+
+\({\dot Q_{as}}\) ~~~~~~~~~~~ = anti-sweat heater load on the case evaporator (W)
+
+\paragraph{Constant Method}\label{constant-method}
+
+For refrigerated cases requiring constant anti-sweat heater output, the power use is simply calculated as the case anti-sweat heater power per unit length multiplied by the length of the case. This method is used when the manufacturer recommends that cycling of the heaters not occur.
+
+\begin{equation}
+{P_{as}} = {P'}_{as}\,\left( {{L_{case}}} \right)
+\end{equation}
+
+where:
+
+\({P_{as}}\) ~~~~~~~~~~~~ = output variable ``Refrigerated Case Anti-Sweat Heater Electric Power {[}W{]}''
+
+\({P'}_{as}\) ~~~~~~~~~~ = case anti-sweat heater power per unit length (W)
+
+\paragraph{Relative Humidity Method}\label{relative-humidity-method}
+
+Anti-sweat heater power can be reduced at lower ambient relative humidity levels to save energy while still protecting from moisture condensation on cold surfaces. For this control type, anti-sweat heater power use is reduced linearly based on case anti-sweat heater power at the rated ambient relative humidity (typically 55\% RH), the relative humidity specified by the user where no anti-sweat heater power is required, and the relative humidity of the ambient (zone) air surrounding the case.
+
+\begin{equation}
+{P_{as}} = {P'}_{as}\left( {{L_{case}}} \right)\left( {1 - \left[ {\frac{{R{H_{rated}} - R{H_{air}}}}{{R{H_{rated}} - R{H_{\min }}}}} \right]} \right)
+\end{equation}
+
+where:
+
+\(R{H_{air}}\) ~~~~~~~ = relative humidity of the ambient (zone) air (\%)
+
+\(R{H_{rated}}\) ~~~~~ = rated ambient relative humidity (\%)
+
+\(R{H_{\min }}\) ~~~~~~ = relative humidity at zero anti-sweat heater energy (\%)
+
+\paragraph{Dewpoint Method}\label{dewpoint-method}
+
+Anti-sweat heater power can also be reduced as a function of ambient air dewpoint temperature based on a similar correlation to that used by the relative humidity method. This control method varies the anti-sweat heater power linearly based on the ambient air dewpoint temperature, the case operating temperature, and the rated ambient dewpoint temperature (calculated by the model using the rated ambient temperature and rated ambient relative humidity entered by the user).
+
+\begin{equation}
+{P_{as}} = {P'}_{as}\left( {{L_{case}}} \right)\left( {\frac{{{T_{dp,air}} - {T_{case}}}}{{{T_{dp,rated}} - {T_{case}}}}} \right)
+\end{equation}
+
+where:
+
+\({T_{dp,air}}\) ~~~~~~~~ = dewpoint temperature of the ambient (zone) air (ËšC)
+
+\({T_{dp,rated}}\) ~~~~~~ = rated ambient dewpoint temperature (ËšC)
+
+\({T_{case}}\) ~~~~~~~~~~ = case operating temperature (ËšC)
+
+\paragraph{Heat Balance Method}\label{heat-balance-method}
+
+A theoretical model may also be used to simulate the performance of anti-sweat heater operation at various indoor dewpoint temperatures (Henderson and Khattar 1999). The model calculates that amount of heat required to hold the case or door surface at (or slightly above) the dewpoint temperature of the ambient air using the following simple heat balance equation:
+
+\begin{equation}
+{P_{as}} = \,\,\left( {\frac{{\left( {{T_{dp,air}} - {T_{db,air}}} \right){H_{case}}}}{{{R_{air}}}} + \frac{{\left( {{T_{dp,air}} - {T_{case}}} \right){H_{case}}}}{{{R_{case}}}}} \right){L_{case}}
+\end{equation}
+
+where:
+
+\({T_{dp,air}}\) ~~~~~~~~ = dewpoint temperature of the ambient (zone) air (ËšC)
+
+\({T_{db,air}}\) ~~~~~~~~ = dry-bulb temperature of the ambient (zone) air (ËšC)
+
+\({H_{case}}\) ~~~~~~~~ = height of the case (m)
+
+\({R_{air}}\) ~~~~~~~~~~ = air film resistance (assumed constant at 0.3169 m\(^{2}\)-ËšC/W)
+
+\({R_{case}}\) ~~~~~~~~~ = heat transfer resistance of case (m\(^{2}\)-ËšC/W)
+
+\({T_{case}}\) ~~~~~~~~~~ = case operating temperature (ËšC)
+
+\({L_{case}}\) ~~~~~~~~~ = case length (m)
+
+The model above provides a linear relationship of anti-sweat heater power with varying ambient air dewpoint temperature at constant ambient air dry-bulb and case temperatures. By assuming that the `nominal' anti-sweat heater power entered by the user is required to avoid moisture condensation at rated ambient air conditions, the value of \({R_{case}}\) ~can be determined by rearranging the equation and solving as follows:
+
+\begin{equation}
+{R_{case}} = \frac{{\left( {{T_{dp,rated}} - {T_{case}}} \right)}}{{\left( {\frac{{{P'}_{as}}}{{{H_{case}}}}} \right) - \left( {\frac{{{T_{dp,rated}} - {T_{db,rated}}}}{{{R_{air}}}}} \right)}}
+\end{equation}
+
+where:
+
+\({T_{db,rated}}\) ~~~~~~ = rated ambient temperature (ËšC)
+
+With \emph{R\(_{case}\)}known, \emph{P\(_{as}\)} can be calculated for each simulation time step using the actual ambient (zone) air dry-bulb and dewpoint temperatures.
+
+\paragraph{All Anti-Sweat Heater Control Methods}\label{all-anti-sweat-heater-control-methods}
+
+For all control methods, the user can specify the fraction of anti-sweat heater energy that directly contributes to the case evaporator heat load:
+
+\begin{equation}
+{\dot Q_{as}} = \,{P_{as}}\left( {{F_{as}}} \right)
+\end{equation}
+
+where:
+
+\({F_{as}}\) ~~~~~~~~~~~ = fraction of anti-sweat heater energy to case
+
+The remainder of the anti-sweat heater energy (1 - \emph{F\(_{as}\)}) is a heating load to the zone where the case is located, which is discussed further in section Sensible Case Credits below.
+
+\subsubsection{Case Restocking}\label{case-restocking}
+
+The impact of restocking the refrigerated case with product that is not at the case operating temperature is modeled with the case restocking schedule. The schedule is entered as a heat gain rate per unit length of the refrigerated case (W/m). The heat load due to restocking is calculated as the scheduled load multiplied by the length of the refrigerated case. The load due to product restocking is assumed to be only sensible (temperature) heat; a latent (moisture) component is not modeled.
+
+\begin{equation}
+{\dot Q_{restock}} = SC{H_{restock}}\left( {{L_{case}}} \right)
+\end{equation}
+
+where:
+
+\(SC{H_{restock}}\) ~ = refrigerated case restocking schedule value (W/m)
+
+The restocking heat load is removed by the refrigerated case evaporator any time the case is not being defrosted and excess sensible cooling capacity is available. If the evaporator cooling capacity is insufficient to remove the entire restocking load, the unmet portion is carried over to the next simulation time step.
+
+\subsubsection{Case Defrost}\label{case-defrost}
+
+Eight refrigerated case defrost strategies can be simulated: none, off-cycle, electric, electric with temperature termination, hot-gas, hot-gas with temperature termination, hot-brine, and hot-brine with temperature termination. Some research has shown that the defrost times for cases defrosted using hot brine can be significantly shorter than defrost times for electric or hot gas.(Terrell, W. J. Jr., 1999) For each of these strategies, the refrigerated case evaporator is turned off for the required time period to allow accumulated frost to melt. Additional time can be scheduled (drip-down) to allow the water to drip from the evaporator and drain from the case.
+
+Refrigerated cases typically require a specific number of defrost cycles per day for a pre-determined length of time. Refer to manufacturer's recommendations for proper defrost frequency and duration. For example, a refrigerated case may have a single defrost period each day with defrost scheduled from 7:00 -- 7:40 am and defrost drip-down scheduled from 7:00 -- 7:55 am. Notice the drip-down schedule and the defrost schedule start at the same time, and the drip-down schedule is longer than the defrost schedule. These schedules should normally repeat for each day of the year.
+
+For electric, hot gas, and hot brine defrost types, energy use by the defrost heater occurs during the scheduled defrost period. For defrost with temperature termination, the energy is also multiplied by the defrost ratio simulating a defrost duration shorter than the defined (maximum) period. For all non-electric defrost types, defrost electric power is set equal to zero (and is not available as an output variable). For hot gas and hot brine defrost types in cases served by a detailed system, the condenser heat rejection load is reduced by the amount of heat recovered for use in the defrost system. This condenser credit is not applied for the simple compressor rack system.
+
+If DefrostType is electric:
+
+\begin{equation}
+  P_{def} = {P'}_{def} L_{case} SCH_{defrost} 
+\end{equation}
+
+If DefrostType is ElectricWithTempTermination:
+
+\begin{equation}
+  P_{def} = {P'}_{def} L_{case} SCH_{defrost} \PB{DefrostRatio}
+\end{equation}
+
+Otherwise:
+
+\begin{equation}
+  P_{def} = 0.0
+\end{equation}
+
+where:
+
+\({P_{def}}\) ~~~~~~~~~~ = output variable ``Refrigerated Case Defrost Electric Power {[}W{]}''
+
+\({P'}_{def}\) ~~~~~~~~~ = case defrost power per unit length (W)
+
+\({L_{case}}\) ~~~~~~~~~ = case length (m)
+
+\(SC{H_{defrost}}\) ~ = case defrost schedule value (0 to 1)
+
+\(DefrostRatio\) ~ = fraction of maximum defrost time, used with temperature termination
+
+Frost accumulation on the case evaporator will vary with the humidity level in the ambient air surrounding the case. Therefore, defrost heater operation can be reduced when ambient air humidity levels are low. Several methods are used to reduce unnecessary defrost heater operation, including terminating heater operation when the measured evaporator temperature indicates that the accumulated frost has been completely melted. For modeling refrigerated cases with temperature-terminated defrost, EnergyPlus allows the user to specify a defrost energy correction curve to account for variations in defrost energy as ambient air humidity levels change. The user can select from four correction curve types: None, Case Temperature Method, Relative Humidity Method, or Dewpoint Method.
+
+For type None (default):
+
+\begin{equation}
+  DefrostRatio = 1
+\end{equation}
+
+For type Case Temperature Method:
+
+\begin{equation}
+  DefrostRatio = 1 - \PB{RH_{rated} - RH_{air}} \PB{a + b T_{case} + c T_{case}^2 + d T_{case}^3}
+\end{equation}
+
+For type RH Method:
+
+\begin{equation}
+  DefrostRatio = e + f \PB{RH_{air}} + g \PB{RH_{air}^2} + h \PB{RH_{air}^3}
+\end{equation}
+
+For type Dewpoint Method:
+
+\begin{equation}
+  DefrostRatio = i + j T_{dp,air} + k T_{dp,air}^2 + l T_{dp,air}^3
+\end{equation}
+
+where:
+
+\(R{H_{rated}}\) ~~~~~ = rated ambient relative humidity (\%)
+
+\(R{H_{air}}\) ~~~~~~~ = relative humidity of the ambient (zone) air (\%)
+
+\({T_{case}}\) ~~~~~~~~~~ = case operating temperature (ËšC)
+
+\({T_{dp,air}}\) ~~~~~~~~ = dewpoint temperature of the ambient (zone) air (ËšC)
+
+a\ldots{}l~~~~~~~~~~~~~~~~~~~~~~~ = user-defined coefficients using a cubic curve object (Curve:Cubic)
+
+The user specifies the defrost energy correction curve type and the name of the cubic curve object (Curve:Cubic) that defines the curve coefficients. Representative curve coefficients for curve type ``Case Temperature Method'' are provided in Table~\ref{table:representative-defrost-energy-correction}.
+
+% table 75
+\begin{longtable}[c]{p{1.5in}p{2.36in}p{2.13in}}
+\caption{Representative Defrost Energy Correction Curve Coefficients for Case Temperature Method \label{table:representative-defrost-energy-correction}} \tabularnewline
+\toprule 
+Coefficient & Single-shelf horizontal display case & Multi-shelf vertical display case \tabularnewline \midrule
+\endhead
+
+a & 2.3632E-2 & 2.4598E-2 \tabularnewline
+b & 6.2320E-4 & 7.6439E-4 \tabularnewline
+c & 2.8320E-5 & -3.8637E-5 \tabularnewline
+d & 4.4035E-7 & 7.45686E-7 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Note: Coefficients derived for \emph{RH\(_{rated}\)} = 55\% and a rated ambient temperature of 23.9ËšC (75ËšF). Source:~ Howell 1993b.
+
+As mentioned above, the refrigerated case evaporator is turned off while it is being defrosted. Heat gains during defrost must be removed once the defrost period (drip-down schedule) has ended. The model assumes that heat gains due to defrost heater operation are at least partially offset by converting accumulated frost to liquid water (condensate) which drains from the case. Frost accumulation during each simulation time step is estimated by the model using the actual latent heat transfer to the refrigerated case and the heat of vaporization plus the heat of fusion for water. The model assumes that frost is not accumulated on the evaporator during the defrost drip-down time period.
+
+\begin{equation}
+Frost = Frost + \left( {\frac{{{{\dot Q}_{case,rated}}\left( {{L_{case}}} \right)\left( {RT{F_{rated}}} \right)\left( {LH{R_{rated}}} \right)\left( {LatentRatio} \right)\left( {{t_{zn}}} \right)}}{{\left( {{h_f} + {h_{fg}}} \right)}}} \right)\left( {1 - SC{H_{defrost,dripdown}}} \right)
+\end{equation}
+
+where:
+
+\(Frost\) ~~~~~~~ = amount of accumulated frost on the case evaporator (kg)
+
+\({\dot Q_{case,rated}}\) ~~~ = case rated total cooling capacity per unit length (W/m)
+
+\({L_{case}}\) ~~~~~~~~~ = case length (m)
+
+\(RT{F_{rated}}\) ~~~~ = runtime fraction of the refrigerated case at rated conditions
+
+\(LH{R_{rated}}\) ~~~ = latent heat ratio of the refrigerated case at rated conditions
+
+\(LatentRatio\) ~ = ratio of actual latent load to rated latent load on the case, based on latent case credit curve (see section Latent Case Credits below)
+
+\({t_{zn}}\) ~~~~~~~~~~~~ = duration of zone simulation time step (s)
+
+\({h_{fg}}\) ~~~~~~~~~~~~~~~~~~~~~~~ = heat of vaporization of water (assumed constant at 2,498,000 J/kg)
+
+\({h_f}\) ~~~~~~~~~~~~ = heat of fusion of water (335,000 J/kg)
+
+\(SC{H_{defrost,dripdown}}\) ~~~ = defrost drip-down schedule value (0 to 1)
+
+During defrost (SCHdefrost), the model assumes that the hot gas, hot brine, or electric heater energy directly contributes to melting the frost (heat of fusion of water). Defrost energy not attributed to melting frost from the evaporator coil results in a heat load on the refrigerated case evaporator \(Q_{def}\). When the defrost drip-down time period ends, this defrost energy heat load is added to the actual case load (up to the maximum evaporator capacity) until the total defrost energy heat load is removed (which may take several simulation time steps)
+
+If DefrostType is Electric, HotGas, or HotBrine:
+
+\begin{equation}
+  \dot{Q}_{def} = \max\RB{0.0,\PB{P_{def}' L_{case} SCH_{def} - \frac{Frost\PB{h_f}}{t_{zn}}}}
+\end{equation}
+
+Otherwise:
+
+\begin{equation}  
+  \dot{Q}_{def} = 0.0
+\end{equation}
+
+where:
+
+\({\dot Q_{def}}\) ~~~~ = defrost heat load (W)
+
+\subsubsection{Sensible Case Credits}\label{sensible-case-credits}
+
+Refrigerated cases remove sensible energy from the surrounding environment (termed ``sensible case credits''). In this model, the sensible case credits are composed of wall heat conduction, radiation heat transfer, and sensible heat transfer by air infiltration (\({\dot Q_{walls}}\) + \({\dot Q_{rad}}\) + \({\dot Q_{{\rm{inf,sens}}}}\) ~in equation ). To quantify this energy transfer, the model first calculates the rated sensible case credits by subtracting the known loads at rated conditions (fan, lighting, and anti-sweat heater) from the rated sensible cooling capacity of the case. It should be noted that the lighting and fan heat discussed here are for standard-efficiency equipment. Manufacturers typically provide ratings for both standard and high-efficiency fan and lighting equipment; however, the standard equipment is used to determine rated sensible case credits. (Some manufacturers no longer include any lighting in their rated capacity values. For these cases, P'\(_{lights,std}\) will equal zero.)
+
+\begin{equation}
+\dot Qc{c_{sens,rated}} = \left[ {{{\dot Q}_{case,rated}}\left( {RT{F_{rated}}} \right)\left( {1 - LH{R_{rated}}} \right) - {P'}_{lights,std}\left( {{F_l}} \right) - {P'}_{as}\left( {{F_{as}}} \right) - {P'}_{fan,std}} \right]{L_{case}}
+\end{equation}
+
+where:
+
+\(\dot Qc{c_{sens,rated}}\) ~ = sensible case credits at rated conditions (W)
+
+\({\dot Q_{case,rated}}\) ~~~ = case rated total cooling capacity per unit length (W/m)
+
+\(RT{F_{rated}}\) ~~~~ = runtime fraction of the refrigerated case at rated conditions
+
+\(LH{R_{rated}}\) ~~~ = latent heat ratio of the refrigerated case at rated conditions
+
+\({P'}_{lights,std}\) ~~~ = standard case lighting power per unit length (W/m)
+
+\({F_l}\) ~~~~~~~~~~~~~ = fraction of lighting energy to case
+
+\({P'}_{as}\) ~~~~~~~~~~ = case anti-sweat heater power per unit length (W)
+
+\({F_{as}}\) ~~~~~~~~~~~~~~~~~~~~~~~ = fraction of anti-sweat heater energy to case
+
+\({P'}_{fan,std}\) ~~~~~ = standard case fan power per unit length (W/m)
+
+\({L_{case}}\) ~~~~~~~~~ = case length (m)
+
+For every simulation time step, the rated sensible case credits are then adjusted to account for variations at off-rated ambient air temperatures. The model also allows the user to define a case credit fraction using a schedule object. This case credit fraction can be useful for modeling cases that operate differently during specific time periods. For example, metal or plastic coverings may be installed on refrigerated display cases during unoccupied hours which would significantly reduce case credits (e.g., air infiltration) compared to occupied hours when the coverings are removed. If the user does not define a case credit fraction schedule, then the fraction is assumed to be 1 for the entire simulation.
+
+\begin{equation}
+\dot Qc{c_{sens}} = \dot Qc{c_{sens,rated}}\left( {\frac{{{T_{db,air}} - {T_{case}}}}{{{T_{db,rated}} - {T_{case}}}}} \right)\left( {SC{H_{cc}}} \right)
+\end{equation}
+
+where:
+
+\(\dot Qc{c_{sens}}\) ~~~~~ = sensible case credits adjusted for ambient temperature and case credit fraction (W)
+
+\({T_{db,air}}\) ~~~~~~~~ = dry-bulb temperature of the ambient (zone) air (ËšC)
+
+\({T_{case}}\) ~~~~~~~~~~ = case operating temperature (ËšC)
+
+\({T_{db,rated}}\) ~~~~~~ = rated ambient (zone) dry-bulb temperature (ËšC)
+
+\(SC{H_{cc}}\) ~~~~~~ = case credit fraction (schedule value, 0 to 1)
+
+The sensible case credits calculated above are considered heat loads on the refrigerated case evaporator. The \textbf{\emph{net}} impact of the case credits on the surrounding zone includes adjustment for the portion of the lighting and anti-sweat heater power that does not directly contribute to the case evaporator load. Sensible case credits are negative values when heat is removed from the zone load.
+
+\begin{equation}
+\dot Qc{c_{sens,NET}} = {P_{lights}}(1 - {F_l})\,\, + \,\,{P_{as}}(1 - {F_{as}})\,\, - \,\,\dot Qc{c_{sens}}
+\end{equation}
+
+where:
+
+\(\dot Qc{c_{sens,NET}}\) = net impact of the sensible case credits on the surrounding zone, negative for cooling (W)
+
+\({P_{lights}}\) ~~~~~~~~~ = case lighting electric power (W)
+
+\({F_l}\) ~~~~~~~~~~~~~ = fraction of lighting energy to case
+
+\({P_{as}}\) ~~~~~~~~~~~~ = anti-sweat heater electric power (W)
+
+\({F_{as}}\) ~~~~~~~~~~~~~~~~~~~~~~~ = fraction of anti-sweat heater energy to case
+
+When refrigerated cases are served by a compressor rack that rejects condenser waste heat directly to the zone (e.g., a stand-alone refrigerated case with integral compressor and condenser), this condenser waste heat offsets some or all of the sensible case credits. The amount of condenser waste heat rejected to the zone is calculated and reported by the refrigerated case compressor rack object (Ref. Heat Rejection to Zone).
+
+\subsubsection{Latent Case Credits}\label{latent-case-credits}
+
+Refrigerated cases also remove latent energy (moisture) from the surrounding environment (termed ``latent case credits''). In this model, the latent case credit is composed solely of the latent heat transfer by air infiltration \({\dot Q_{inf,lat}}\) in equation . The latent case credits are calculated as the product of the case length and the total cooling capacity per unit length, latent heat ratio, and runtime fraction at rated conditions. As described previously (Ref. Sensible Case Credits), a case credit fraction schedule is used to model cases that operate differently during specific time periods. The same case credit fraction is used to modify both the sensible and latent case credits. If the user does not define a case credit fraction schedule, then the fraction is assumed to be 1 for the entire simulation. The calculation of latent case credits also includes a factor (\emph{LatentRatio}) that accounts for lower ambient humidity levels. Latent case credits are set to zero during the defrost-dripdown periods.
+
+\begin{equation}
+{\dot Q_{{\rm{inf}},lat}} = \,\,\,\, - \dot Qc{c_{lat}}\,\, = \,\,{\dot Q_{case,rated}}\left( {LH{R_{rated}}} \right)\left( {RT{F_{rated}}} \right)\left( {SC{H_{cc}}} \right)\left( {LatentRatio} \right){L_{case}}
+\end{equation}
+
+where:
+
+\({\dot Q_{{\rm{inf,lat}}}}\) ~~~~~~~~ = latent load on the refrigerated case evaporator at current ambient conditions (W)
+
+\(\dot Qc{c_{lat}}\) ~~~~~~~ = latent case credit impact on zone load, negative for dehumidification (W)
+
+\({\dot Q_{case,rated}}\) ~ = case rated total cooling capacity per unit length (W/m)
+
+\(LH{R_{rated}}\) ~ = latent heat ratio of the refrigerated case at rated conditions
+
+\(RT{F_{rated}}\) ~~ = runtime fraction of the refrigerated case at rated conditions
+
+SCH\(_{CC}\)~~~~ = case credit fraction (schedule value, 0 to 1)
+
+\(LatentRatio\) ~ = ratio of actual latent load to rated latent load on the case, based on latent case credit curve
+
+\({L_{case}}\) ~~~~~~~~ = case length (m)
+
+Latent load on the refrigerated case evaporator will vary with ambient humidity levels. Therefore, the refrigerated case model allows the user to specify a latent case credit curve to adjust case credits based on ambient humidity, and the user can select from three curve types: Case Temperature Method, Relative Humidity Method, or Dewpoint Method.
+
+If CurveType is Case Temperature Method:
+
+\begin{equation}
+  LatentRatio = 1-\PB{RH_{rated}-RH_{air}}\PB{m+nT_{case}+oT_{case}^2+pT_{case}^3}
+\end{equation}
+
+Else if CurveType is RH Method:
+
+\begin{equation}
+  LatentRatio = q + r\PB{RH_{air}} + s\PB{RH_{air}^2} + t\PB{RH_{air}^3}
+\end{equation}
+
+Else if CurveType is Dewpoint Method:
+
+\begin{equation}
+  LatentRatio = u + vT_{dp,air} + wT_{dp,air}^2 + xT_{dp,air}^3
+\end{equation}
+
+where:
+
+\(R{H_{rated}}\) ~~~~~ = rated ambient relative humidity (\%)
+
+\(R{H_{air}}\) ~~~~~~~ = relative humidity of the ambient (zone) air (\%)
+
+\({T_{case}}\) ~~~~~~~~~~ = case operating temperature (ËšC)
+
+\({T_{dp,air}}\) ~~~~~~~~ = dewpoint temperature of the ambient (zone) air (ËšC)
+
+m\ldots{}x~~~~~~~~~ = user-defined coefficients using a cubic curve object (Curve:Cubic)
+
+The user specifies the latent case credit curve type and the name of the cubic curve object (Curve:Cubic) that defines the curve coefficients. Representative curve coefficients for curve type ``Case Temperature Method'' are provided in Table~\ref{table:representative-latent-case-credit-curve}.
+
+% table 76
+\begin{longtable}[c]{@{}lll@{}}
+\caption{Representative Latent Case Credit Curve Coefficients for Case Temperature Method \label{table:representative-latent-case-credit-curve}} \tabularnewline
+\toprule 
+Coefficient & Single-shelf horizontal & Multi-shelf vertical \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Representative Latent Case Credit Curve Coefficients for Case Temperature Method} \tabularnewline
+\toprule 
+Coefficient & Single-shelf horizontal & Multi-shelf vertical \tabularnewline
+\midrule
+\endhead
+
+m & 2.0376E-2 & 2.6520E-2 \tabularnewline
+n & 2.4378E-4 & 1.0780E-3 \tabularnewline
+o & 1.1400E-5 & -6.0256E-5 \tabularnewline
+p & 1.8110E-7 & 1.2373E-6 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Note: Coefficients derived for \emph{RH\(_{rated}\)} = 55\% and a rated ambient temperature of 23.9ËšC (75ËšF). Source:~ Howell 1993b.
+
+\subsubsection{Refrigerated Case Credits With Under Case Return Air}\label{refrigerated-case-credits-with-under-case-return-air}
+
+For certain refrigerated case types, the sensible case credits provided to the zone can create an uncomfortably cold environment in the surrounding area. For this reason, return air ducts are frequently placed behind these cases to draw this cold air under the case and direct it back to the HVAC system. This reduces localized over-cooling and improves occupant comfort.
+
+\begin{figure}[hbtp] % fig 279
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6247.png}
+\caption{Return Air Factor Versus Under Case HVAC Return Air Fraction \protect \label{fig:return-air-factor-versus-under-case-hvac}}
+\end{figure}
+
+Since under case return ducts reduce the temperature and humidity of the air being recirculated to the HVAC system, this can impact HVAC system performance. Figure~\ref{fig:return-air-factor-versus-under-case-hvac} shows the relationship that is used by the refrigerated case model to determine the fraction of case credits that directly cool and dehumidify the HVAC system return air. This fraction, referred to as the Return Air Factor (RAF), is a function of the fraction of the HVAC system return air that comes from under the cases. The remaining fraction of the case credits (1-RAF) becomes part of the overall zone air energy balance. If the HVAC system is off for a simulation time step (no return air mass flow), the sensible and latent case credits normally attributed to the HVAC return are set equal to zero (even though they get calculated and reported here as non-zero values) and all case credit energy is applied to the zone air heat balance.
+
+\begin{equation}
+\dot Qc{c_{sens,zone}} = \dot Qc{c_{sens,NET}}\left( {1 - RAF} \right)
+\end{equation}
+
+\begin{equation}
+\dot Qc{c_{lat,zone}} = \dot Qc{c_{lat}}\left( {1 - RAF} \right)
+\end{equation}
+
+\begin{equation}
+\dot Qc{c_{sens,HVAC}} = \dot Qc{c_{sens,NET}}\left( {RAF} \right)
+\end{equation}
+
+\begin{equation}
+\dot Qc{c_{lat,HVAC}} = \dot Qc{c_{lat}}\left( {RAF} \right)
+\end{equation}
+
+where:
+
+\(\dot Qc{c_{sens,zone}}\) = sensible case credit applied to the zone air heat balance (W)
+
+\(\dot Qc{c_{lat,zone}}\) ~~ = latent case credit applied to the zone air heat balance (W)
+
+\(\dot Qc{c_{sens,HVAC}}\) = sensible case credit applied to the HVAC return air (zone return air path outlet node) (W)
+
+\(\dot Qc{c_{lat,HVAC}}\) = latent case credit applied to the HVAC return air (zone return air path outlet node) (W)
+
+RAF~~~~~~~~~~~ = return air factor (see Figure~\ref{fig:return-air-factor-versus-under-case-hvac} above)
+
+\subsubsection{Variable Evaporator Temperature}\label{variable-evaporator-temperature}
+
+Control systems are now available that increase the evaporator temperature to improve compressor efficiency whenever the total loads on a system are less than the system capacity. To model these systems, a variable evaporator temperature is an option available with the detailed refrigeration system object (Refrigeration:System). If this option is selected, the model will compare the refrigeration load on each case to the load at rated conditions. If the case load in a particular time step is less than the rated load, an acceptable elevated evaporator temperature is determined for that case. The evaporator temperature for the whole refrigeration system is then set by the minimum evaporator temperature needed for any particular case.
+
+\begin{equation}
+  LF_{case} = \frac{\dot{Q}_{case,actual}}{\dot{Q}_{case,rated}}
+\end{equation}
+
+\begin{equation} 
+  T_{Evap,Allowed} = T_{case} - LF_{case}\PB{T_{case} - T_{Evap,Design}}
+\end{equation}
+
+where:
+
+LF\(_{case}\)~~~~~~~~~ = Load factor for a particular case
+
+Tevap~~~~~~~~ = Evaporator temperature, C.
+
+\subsection{Walk-In Coolers and Freezers}\label{walk-in-coolers-and-freezers}
+
+The walk-in object (Refrigeration:WalkIn) is another type of refrigeration load that can be placed on either a refrigeration compressor rack, detailed refrigeration system, or secondary refrigeration system object (Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem). Walk-in coolers and freezers differ from refrigerated cases in that they may have surfaces facing more than one zone and in that they are always equipped with doors, that is, they do not have open shelves. Their sensible and latent exchange with zones is therefore calculated in a different manner than for refrigerated cases. Also, the walk-in model does not interact directly with the HVAC system, that is, the return air fraction option available in the refrigerated case model is not included.
+
+The walk-in cooler performance is based on the ASHRAE load model, which includes infiltration through door openings and sensible loss through walls/ceilings described by the user for each zone.(ASHRAE 2006d, ASHRAE 2006e, Gosney, W.B., Olama, G.A.-L. 1975) All equipment loads (fan, light, heaters) are modeled as well.~ Sensible and latent exchange with multiple adjoining zones is included. A master schedule is used for the Walk In operation and~ additional schedules control the lights, defrost, and heater operation. ~Just as for cases, unmet refrigeration loads are accumulated to be met the following time step.~ This usually occurs during defrost and ~restocking.
+
+\subsubsection{Walk-In Sensible and Latent Heat Exchange}\label{walk-in-sensible-and-latent-heat-exchange}
+
+A walk-in can exchange both sensible and latent energy with multiple zones.~ The heat transfer calculations are performed separately for each zone so that the heat transfer impact, or zone credits, can be determined. The area of all walls and ceilings facing each zone are described by the user by their thermal conductance and area. Sensible energy exchange takes place between these surfaces and the surrounding zones.~ Because these walls interface with conditioned zones at relatively constant temperatures, this heat exchange is modeled very simply:
+
+Q\(_{SurfacesZn}\) = U\(_{SurfacesZn}\) x A\(_{SurfacesZn}\) x ΔT\(_{Zn}\)
+
+Q\(_{DoorSensZn}\) ~~~~ = ~U\(_{DoorZn}\)~ x~ Area\(_{DoorZn}\) ~x ΔT\(_{Zn}\)
+
+The heat transfer through the floor is similarly modeled.
+
+Q\(_{Floor}\) = A\(_{Floor}\) x U\(_{Floor}\) x (T\(_{Ground}\) -- T\(_{WalkIn}\))
+
+Where:
+
+A\(_{Floor}\) ~~~~~~~~~ = Area of the walkin floor, m\(^{2}\)
+
+A\(_{SurfacesZn}\) = Area of surfaces facing Zone n, m\(^{2}\)
+
+Q\(_{DoorSensZn}\) ~~~ = Sensible heat transfer through the closed door(s) facing Zone n, W
+
+Q\(_{surfacesZn}\) ~~~~ = Sensible heat transfer through walls and ceilings facing Zone n, W
+
+T\(_{Ground}\) ~~~~~~~~ = Ground temperature, C
+
+T\(_{WalkIn}\)~~~~~~~~~ = Walk-in operating temperature, C
+
+U\(_{Floor}\) ~~~~~~~~~ = Thermal conductance of floor, W/m2-K
+
+U\(_{DoorZn}\) ~~~~~~~ = Thermal conductance of doors facing Zone n, W/m2-K
+
+U\(_{SurfacesZn\\}\) = Thermal conductance of surfaces facing Zone n, W/m2-K
+
+ΔT\(_{Zn}\) ~~~~~~~~~~ = Difference between walk-in operating temperature and Zone n drybulb temperature, C
+
+Infiltration through doorways places both a sensible and a latent load upon the walk-in, and corresponding credits upon the adjacent zone.~ Two types of doors are available, nominally called `stock' and `glass' doors, to enable the user to model doors that differ in thermal conductance, door protection type, and frequency of opening.~ The sensible and latent infiltration loads are modeled according to the guidance specified in (ASHRAE 2006d, ASHRAE 2009, and Gosney and Olama, 1975).~ The air within the cooler is assumed to be at 90\% relative humidity. Equal air exchange is assumed, that is, the mass of dry air infiltrating into the walkin is assumed to equal the mass of dry air infiltrating out of the walkin.
+
+Q\(_{Infiltration}\) = Q\(_{FullFlow}\) ~x~ Factor\(_{DoorOpen}\) ~x Factor\(_{Flow}\) ~x (1 - Factor\(_{Protection}\))
+
+Q\(_{FullFlow}\) = 0.221*A\(_{Door}\)(h\(_{ZoneAir}\)-h\(_{AirWalkIn}\))�\(_{AirWalkIn}\)(1-�\(_{ZoneAir}\)/�\(_{AirWalkIn}\))\(^{0.5}\)(g*H\(_{Door}\))\(^{0.5}\)Factor\(_{Density}\)
+
+Factor\(_{Density}\) = (2 /(1 + (�\(_{AirWalkIn}\) / �\(_{ZoneAir}\))\(^{0.333}\))) \(^{1.5}\)
+
+m\(_{DryAir}\) = Q\(_{Infiltration}\) / (h\(_{ZoneAir}\) - h\(_{AirWalkIn}\))
+
+m\(_{Water}\) = ~m\(_{DryAir}\) ~x (W\(_{ZoneAir}\) - W\(_{AirWalkIn}\))
+
+Q\(_{WalkInLatentZn}\) = m\(_{Water}\) x Δh\(_{IcetoVapor}\) ~x (1 ~- SCH\(_{Defrost,DripDown}\))
+
+Q\(_{WalkInSensInfZn}\) ~ = Q\(_{Infiltration}\) - (m\(_{Water}\) x Δh\(_{IcetoVapor}\))
+
+Where:
+
+A\(_{door}\)~~~~~~~~~~~ = ~ Area of door facing Zone n, m\(^{2}\)
+
+Factor\(_{DoorOpen}\) = Value scheduled by user, fraction of time door open during time step
+
+Factor\(_{Flow}\) ~~ = ~Doorway flow factor, = 0.8 if ΔT\(_{Zn}\) \textgreater{} 11C; = 1.1 if ΔT\(_{Zn}\) \textless{} = 11C
+
+Factor\(_{Protection}\) = Doorway protection factor, = 0 for no protection; = ~ 0.5 for an air curtain; and 0.9 for a strip curtain
+
+g~~~ = ~ Gravitational constant
+
+h\(_{AirWalkIn}\) = ~ enthalpy of the air within the walk in, = ~ f(T\(_{WalkIn}\),P\(_{Oudoor}\), 90\%RH), J/kg
+
+h\(_{ZoneAir}\) = ~ enthalpy of the air in Zone n, J/kg
+
+H\(_{door}\)~~~~~~~~~~~ = ~ Height of door facing Zone n, m
+
+Q\(_{FullFlow}\) ~~~~~~ = Sensible and latent refrigeration load for fully established flow, W
+
+Q\(_{Infiltration}\) ~~~~~ = Average infiltration (sensible and latent) refrigeration load for the time step, W
+
+Q\(_{WalkInLatentZn}\) = Latent load upon the walk in facing Zone n, W
+
+Q\(_{WalkInSensInfZn}\) ~ = Sensible load due to infiltration upon the walkin facing Zone n, W
+
+m\(_{DryAir}\) ~~~~~~~~ = Mass of dry air infiltrating into the walk-in, kg/s
+
+m\(_{Water}\) ~~~~~~~~ = Mass of water removed from the infiltrating air, kg/s
+
+P\(_{Outdoor}\) = ~ Outdoor air pressure, Pa
+
+SCH\(_{Defrost,DripDown}\) = value from 0 to 1 indicating whether the system is in the dripdown period
+
+W\(_{AirWalkIn}\) = ~ Humidity ratio of the air within the walk in, = ~ f(T\(_{WalkIn}\),P\(_{Oudoor}\), 90\%RH), kg/kg
+
+W\(_{ZoneAir}\) ~~~~~~ = ~ Humidity ratio of Zone n air, kg/kg
+
+Δh\(_{IcetoVapor}\) ~~~ = ~ Latent heat absorbed to change ice to vapor, J/kg
+
+�\(_{AirWalkIn}\) = ~ Density of the air within the walk in = ~ f(T\(_{WalkIn}\),P\(_{Oudoor}\), 90\%RH), kg/m\(^{3}\)
+
+�\(_{ZoneAir}\) ~~~~~~~~ = ~ Density of air in Zone n, kg/m\(^{3}\)
+
+The sensible load on the case and the sensible credit to the zone continue throughout the defrost and dripdown periods.~ However, to be consistent with the treatment of refrigerated cases, there is no latent credit to the zone or latent load upon the cooler during the dripdown period. Latent load and latent credit are both based on reducing the infiltrating vapor to ice. The sensible heat exchange between the walk in and the zone is then the total of the heat transfer through the doors and surfaces and the infiltration sensible load. The latent load upon the walkin is converted to the amount of frost added to the coils during each time step.~ This accumulating value is used later to determine the load placed upon the walkin during the defrost cycle.
+
+Q\(_{WalkInSensZn}\) ~ = Q\(_{WalkInSensInfZn}\) + Q\(_{DoorZn}\) + Q\(_{surfacesZn}\)
+
+Q\(_{ZoneLatent}\) ~ = - Q\(_{WalkInLatentZn}\)
+
+Q\(_{ZoneSens}\)~ = - Q\(_{WalkInSensZn}\)
+
+ΔFrost\(_{Zn}\) = (m\(_{Water}\) *Δtime)* (1- SCH\(_{Defrost,DripDown}\))
+
+Where:
+
+Q\(_{WalkInSensZn}\) ~ = Total sensible heat exchange between the walkin and Zone n, W
+
+Q\(_{ZoneLatent}\) ~~~~ = Latent load upon the Zone n, W
+
+Q\(_{ZoneSens}\) ~~~~~ = Sensible load upon Zone n , W
+
+ΔFrost\(_{Zn}\) = Change in frost inventory, kg
+
+Δtime~~~~~~~~~ = Length of time step, s
+
+After the heat exchange with each zone is calculated, the total load on the walkin is calculated:
+
+Q\(_{WalkInLatentTot}\) = ∑Q\(_{WalkInLatentZn}\)
+
+Q\(_{WalkInSensTot}\) = ∑Q\(_{WalkInSensZn}\) + Q\(_{Light}\)+ Q\(_{Fan}\)+ Q\(_{Heater}\) + Q\(_{Defrost\\ +}\) Q\(_{Stocking\\ +}\) Q\(_{Floor}\)
+
+Q\(_{WalkInTotal}\) = Q\(_{WalkInLatentTot}\) + Q\(_{WalkInSensTot}\)
+
+ΔFrost\(_{Tot}\) = ∑ΔFrost\(_{Zn}\)
+
+Where Q\(_{Light}\), Q\(_{Fan}\), Q\(_{Heater}\) , Q\(_{Stocking}\) , and Q\(_{Defrost}\) are described below.
+
+\subsubsection{Walk-In Fans, Heaters, Lighting, and Restocking}\label{walk-in-fans-heaters-lighting-and-restocking}
+
+Sensible heat loads are placed on a walk-in by fans, heaters, and lighting. Unlike refrigerated cases, there is no option to allocate any portion of these heat loads to the surrounding zone(s). Larger walk-ins will have separate fans at the cooling coil and for general circulation. The general circulation fan is assumed to run at all times. The cooling coil fan is assumed to be off for Hot-Fluid and Electric defrost. Lighting, heating, and restocking are modeled according to the schedule values entered by the user. For lighting and heating, the maximum power is entered along with a scheduled ratio (between 0 and 1) to be applied for any point in time.~ The heating power includes all heaters except those used for defrost purposes. The heater power should include anti-sweat, door, floor, and drain-pan heaters. For restocking, the total sensible load in Watts is scheduled for each point in time (the restocking latent load is assumed to be zero).
+
+Q\(_{Light}\) = RatedQ\(_{Lighting}\) * SCH\(_{Lighting}\)
+
+Q\(_{Fan}\) = ~ Power\(_{CircFan}\) + Power\(_{CoilFan}\) * ( 1 - SCH\(_{DripDown}\) )
+
+Q\(_{Heater}\) = Power\(_{Heater}\) * SCH\(_{Heater}\)
+
+Q\(_{Stocking}\) = SCH\(_{Stocking}\)
+
+Where:
+
+Q\(_{Light}\) = Refrigeration load due to lighting during current time step, W
+
+RatedQ\(_{Lighting}\) = Maximum lighting load specified for the walk-in, W
+
+SCH\(_{Lighting}\) = Scheduled value between 0 and 1 for the current time step
+
+Q\(_{Fan}\) ~~~~~~~~~~ = ~ Refrigeration load due to fan power during the current time step, W
+
+Power\(_{CircFan}\) = ~ Rated circulating fan power, W
+
+Power\(_{CoilFan}\) = ~ Rated coil fan power, W
+
+SCH\(_{DripDown}\) = Scheduled value between 0 and 1 for the current time step
+
+Q\(_{Heater}\)~~~~~~~~~ = Refrigeration load due to heaters during current time step, W
+
+Power\(_{Heater}\)~~ = Rated total heater(s) power (including anti-sweat, floor, door, etc.) , W
+
+SCH\(_{Heater}\) = Scheduled value between 0 and 1 for the current time step
+
+Q\(_{Stocking}\)~~~~~~~ = Refrigeration load due to stocking during the time step, W
+
+SCH\(_{Stocking}\)~~~ = Scheduled value of load due to stocking, W
+
+\subsubsection{Defrost}\label{defrost}
+
+The defrost types available for the walk-in model include none, off-cycle, electric, and hot-fluid. Defrosts are started according to scheduled times and can be ended either by schedule or by temperature termination. Dripdown schedules are used to keep the cooling coil off long enough to drain any condensate from the system.
+
+For defrost types none and off-cycle, the refrigeration load on the walk-in due to defrost is zero.~ For off-cycle, the walk-in refrigeration capacity is set to zero during the drip-down scheduled time.
+
+The energy required for hot-fluid defrost is assumed to be reclaimed from the compressor exhaust (for detailed systems, this energy appears as a credit against the heat rejection needed at the condenser). The energy used by electric defrost is available as an output variable.
+
+If the defrost cycle is controlled by the schedule, the refrigeration load placed upon the walk-in is calculated as the product of the defrost capacity and the defrost schedule. The load is then reduced according to the amount of accumulated ice melted during that time step.
+
+Q\(_{Defrost}\) = Capacity\(_{Defrost}\)*SCH\(_{Defrost}\) -- Δfrost x Δh\(_{IceMelt}\) / Δtime
+
+Where:
+
+Q\(_{Defrost}\) ~~~~~~~ = Refrigeration load imposed by defrost heat, W
+
+Capacity\(_{Defrost}\) = Rated defrost power, W
+
+SCH\(_{Defrost}\) = Scheduled value between 0 and 1 for the current time step
+
+Δfrost ~~~~~~~ = amount of frost melted during time step, kg
+
+Δh\(_{IceMelt}\) ~~~~~~ = heat of fusion for ice, J/kg
+
+Δtime ~~~~~~~~ = time in time step, s
+
+If the defrost is controlled by temperature termination, the defrost cycle is assumed to end when all the ice is melted.~ However, we need to recognize not all defrost heat goes to melt ice. Some of the defrost heat goes to raising the temperature of the coil mass to greater than 0C, and some is transferred to the walk-in environment as some of the coils are defrosted before others.~ The user enters a `defrost energy fraction' to specify the portion of the defrost energy that goes directly to melting ice.~ The default for defrost energy fraction is 0.7 for electric defrost and 0.3 for warm fluid defrost.( Baxter, V. D., Mei, V.C., 2002) For this type of defrost control, the model calculates the amount of energy available to melt the ice in each time step. The accumulated amount of ice is then reduced accordingly. When all the ice is melted, the defrost schedule value is set to zero and no further defrost load is placed upon the walk-in cooler.~ If the defrost schedule ends before the ice is melted, the schedule is used and the ice continues to accumulate until the next defrost cycle. The refrigeration capacity is kept at zero until the end of the drip-down schedule. Until the accumulated ice is melted, the defrost heat load upon the walk-in is:
+
+Q\(_{Defrost}\) = Capacity\(_{Defrost}\) x SCH\(_{Defrost}\) x (1- Fraction\(_{DefrostEnergy}\))
+
+\subsection{Air Chillers and Air Chiller Sets}\label{air-chillers-and-air-chiller-sets}
+
+The Air Chiller object (Refrigeration:AirChiller) is another type of refrigeration load that can be placed on either a refrigeration compressor rack, detailed refrigeration system, or secondary refrigeration system object (Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem). Air chillers are used to model the type of equipment typically used in refrigerated warehouses. For that reason, there is a major difference between the air chiller model and those for refrigerated cases or walk-ins. For cases and walk-ins, a portion of the model is directed toward calculating the amount of refrigeration needed to maintain the refrigerated volume at the desired temperature due to heat exchange with the surrounding zone, and that zone is conditioned to a nearly constant temperature.~ In a refrigerated warehouse, the refrigeration load is caused by heat exchange with a variable external environment.~ For that reason, the loads for these zones are calculated by the usual EnergyPlus zone heat balance.~ The amount of refrigeration needed to maintain the specified temperature set points is then passed to the air chiller model, in a similar fashion to the load passed to a window air conditioner model. The air chillers are therefore solved using the system time step, not the zone time step used for cases and walk-ins.
+
+The air chiller performance is based on three types of manufacturers ratings, Unit Load Factor, Total Capacity Map, or a set of European standards. Correction factors for material and refrigerant are applied to all of these ratings.
+
+\subsubsection{Unit Load Factor Capacity}\label{unit-load-factor-capacity}
+
+Bruce Nelson has provided a useful description of the Unit Load Factor approach.(Nelson, B.I., 2010)
+
+*``One well-known method used to calculate the sensible cooling capacity of evaporators is the effectiveness method.(Kays,* \emph{W.M., A.L. London, 1964) ~Heat exchanger effectiveness is defined as the ratio of the actual amount of heat transferred to the maximum possible amount of heat that could be transferred with an infinite area. This method is extremely useful because cooling capacity can be calculated directly knowing only the dimensional characteristics of the coil and the initial temperature difference (entering air temperature minus the evaporating temperature). This initial temperature difference is referred to as ``DT1'' \ldots{} in the refrigeration industry. Sensible cooling capacity is calculated as follows:}
+
+\begin{equation}
+{q_{{\rm{sens}}}} = \dot m \times {c_p} \times \varepsilon  \times ({T_{{\rm{coil inlet}}}} - {T_{{\rm{evap}}}}) = \dot m \times {c_p} \times \varepsilon  \times DT1
+\end{equation}
+
+\emph{For a given size of coil operating with constant airflow rate, the effectiveness can be considered constant over the small op- erating temperature ranges typical of refrigeration applications, and therefore, capacity can be considered to be proportional to the ratio of DT1. Hence, if evaporator coil sensible capac- ity is known for a given DT1, then capacity at a new initial temperature difference, DT1�, can be found by multiplying the original capacity by the ratio DT1�/DT1.''}
+
+Where:
+
+q\(_{sens}\) ~~~~~~~~~~ = Cooling capacity (sensible only), W
+
+\(\dot m\) ~~~~~~~~~~~~~ = mass flow rate of air, kg/s
+
+\({c_p}\) ~~~~~~~~~~~~ = specific heat capacity of moist air, J/kg-C
+
+\(\varepsilon\) ~~~~~~~~~~~~~~ = effectiveness ( = (T\(_{coil\, inlet}\) -- T\(_{coil}\) exit)/(T\(_{coil\, inlet}\) - T\(_{evap}\))
+
+T\(_{coil\, inlet}\)~~~~~~~~ = dry-bulb air temperature entering the coil, C
+
+T\(_{evap}\)~~~~~~~~~~~ = average refrigeratnt evaporating temperature, C
+
+T\(_{coil\, exit}\)~~~~~~~~~ = dry-bulb air temperature leaving the coil, C
+
+DT1~~~~~~~~~~~ = initial temperature difference, C
+
+Using this approach, the manufacturer specifies the Unit Load Factor in terms of sensible capacity per degree of temperature difference.
+
+\begin{equation}
+ULF = Capacit{y_{Rated,Sensible}}/DT{1_{Rated}}
+\end{equation}
+
+\emph{The total capacity is the sum of the sensible and latent capacity. The sensible heat ratio (SHR) is the sensible heat transfer divided by the total (sensible plus latent) heat transfer. Again, from Nelson,} (Nelson, B.I., 2010)
+
+\emph{The mass transfer process is much more ``thermally effective'' than the sensible heat transfer process, that is, the heat flux through the evaporator surfaces during the mass transfer process is extremely high.(AHRI, 2001) Consequently, if the surface effectiveness of the coil were to remain constant, the increase in the evaporator cooling capacity during combined sensible and latent cooling would be equal to the sensible cooling capacity divided by the SHR\ldots{} However, the increase in heat flux through the fin surfaces has the effect of decreasing fin efficiency and overall surface effectiveness due to an increase in the fin surface temperature gradient.7 The result is a slightly lower total cooling capacity.}
+
+\begin{equation}
+  Q_{ideal} = \frac{q_{sens}}{SHR}
+\end{equation}
+
+\begin{equation}
+  SHR = \frac{q_{sens}}{Q_{total}}
+\end{equation}
+
+Where:
+
+\({Q_{{\rm{ideal}}}}\) ~~~~~~~~~ = Cooling capacity (total) if fin efficiency and total effectiveness were constant, W
+
+\({Q_{{\rm{Total}}}}\) ~~~~~~~~ = Cooling capacity (total), actual
+
+The total capacity is therefore a function of the sensible heat ratio, which is a function of the total capacity, and they are both, of course a function of the psychometrics of the air flowing through the chiller. This is handled with a two step estimation process.
+
+\begin{equation}
+  \begin{array}{rl}
+                  \Delta T &= \min{ \Delta T_{max},\PB{T_{coil inlet} - T_{evap}}} \\
+              q_{sens,max} &= ULF \cdot \Delta T \cdot \PB{1 - SCH_{Defrost,DripDown}} \cdot SCH_{Coil} \\ 
+    T_{Coil exit estimate} &= T_{Coil inlet} - \frac{q_{sens,max}}{\dot{m}_{DryAir} C_{p,Coil Inlet Dry Air}} \\
+    h_{Coil exit estimate} &= f\PB{T_{Coil exit estimate},P_{Barometric}}\left.\right|_{at a Relative Humidity of 1} \\
+        Q_{Total estimate} &= \dot{m}_{max}\PB{h_{Coil Inlet} - h_{Coil exit estimate}} \\
+                       SHR &= \frac{q_{sens,max}}{Q_{Total estimate}} \\
+         \text{Correction} &= f(SHR);\,\text{Function input by user, linear or quadratic curve} \\
+                 Q_{Total} &= \text{Correction} \times q_{sens,max}
+  \end{array}
+\end{equation}
+
+Where:
+
+\(\Delta T\) ~~~~~~~~~~~ = Temperature difference between the inlet air and the average evaporating temperature, C
+
+\(\Delta T{}_{Max}\) ~~~~~~ = Maximum temperature difference specified by the user, C
+
+SCH\(_{Coil}\)~~~~~~~ = Coil availability schedule
+
+h\(_{Coil\, exit}\)~~~~~~~~ = Enthalpy of air at the coil exit
+
+h\(_{Coil\, inlet}\)~~~~~~~~ = Enthalpy of air at the coil inlet
+
+P\(_{Barometric}\)~~~~~ = Barometric air pressure,Pa
+
+The ``Correction'' function must be obtained from the chiller manufacturer. Some curves typical of ammonia chillers have been published (see, for example, Fig. 2 in (Nelson, B.I., 2010)). A default linear approximation of this curve is provided as an input option.
+
+\subsubsection{European Standard Ratings}\label{european-standard-ratings}
+
+Five standard rating conditions have been defined in a European rating system. The capacity is reported at the rating condition as either the ``Nominal'' or ``Standard'' capacity. The ``Nominal'' capacity includes both latent and sensible loads and the ``Standard'' capacity includes sensible loads only. ``Wet Coil Factors'' are provided with the ratings to translate between the two, along with a chart giving the impact of Air Inlet Temperature on the Wet Coil Factor. The user identifies the rating condition used and whether the capacity input is ``Nominal'' or ``Standard''. These rating factors, along with the air inlet temperature and evaporating temperature are used to calculate the actual cooling capacity.
+
+\begin{equation}
+{Q_{{\rm{Total}}}} = {Q_{{\rm{Nominal}}}} \times \frac{{WetCoilFactor({T_{{\rm{Coil inlet}}}})}}{{WetCoilFactor({\rm{Standard Condition}})}} \times \frac{{\Delta T}}{{\Delta {T_{{\rm{Rated}}}}}}
+\end{equation}
+
+\subsubsection{Total Capacity Map}\label{total-capacity-map}
+
+Some manufacturers are beginning to provide more comprehensive performance information. For these air chillers, the manufacturers specify a Rated Total Capacity at a given inlet air relative humidity.~ A table or set of curves is then provided to calculate the total capacity Q\(_{Total}\), as a function of the inlet air temperature and relative humidity, and the average evaporating temperature.
+
+\subsubsection{Sensible and Latent Capacity}\label{sensible-and-latent-capacity}
+
+The sensible and latent loads served are then calculated as:
+
+\begin{equation}
+  \begin{array}{rl}
+      h_{Coil exit} &= h_{Coil Inlet} - \frac{Q_{Total}}{\dot{V}_{Air,Max} \rho_{Coil Inlet}} \\
+      T_{Coil exit} &= f\PB{h_{Coil exit}}\left.\right|_{\text{at a Relative Humidity of 1}} \\
+     HR_{Coil exit} &= f\PB{T_{Coil exit},h_{Coil exit}} \\
+    \dot{m}_{Water} &= \dot{m}_{dryair,max} \PB{HR_{Coil exit} - HR_{Coil inlet}} \\
+         q_{latent} &= \dot{m}_{water} h_{icetovapor} \\
+           q_{sens} &= Q_{Total} - q_{latent}
+  \end{array}
+\end{equation}
+
+Where:
+
+\({\dot V_{Air,Max}}\) ~~~~~~ = Maximum air flow, m\(^{3}\)/s
+
+HR~~~~~~~~~~~~~ = Humidity Ratio, kg water/kg dry air
+
+h\(_{ice\, to\, vapor}\) = enthalpy of phase change from vapor to ice
+
+When the sensible capacity provided is greater than the sensible load requested from the zone energy balance, the coil fan speed is varied as described later for the condenser fan. The latent load and amount of water condensed from the air are scaled accordingly.
+
+The frost accumulation and defrost cycles are handled as described previously for walk-in coolers.
+
+The net sensible heat impact on the zone is the difference between the coil's sensible cooling capacity and any energy added during that time step by heaters, fan motors, and defrost.
+
+\subsection{Detailed Refrigeration Systems}\label{detailed-refrigeration-systems}
+
+The detailed refrigeration system object (Refrigeration:System) is an alternative to the refrigeration compressor rack object (Refrigeration:CompressorRack). Either works in conjunction with the refrigerated case and walk-in objects (Refrigeration:Case and Refrigeration:WalkIn) to simulate the performance of a retail refrigeration system. The detailed system model differs from the compressor rack model in that it:
+
+1)~~~~requires performance data for each compressor (see the RefrigerationCompressorCurves dataset),
+
+2)~~~~requires condenser performance curves for air- and evaporative-cooled condensers,
+
+3)~~~~explicitly calculates the amount of superheat available for reclaim in an optional air or water heating coil,
+
+4)~~~~allows the suction temperature to rise when the case loads are less than the design loads, thus improving compressor efficiency,
+
+5)~~~~allows the transfer of loads from one system to another, including cascade condensers and secondary systems typically used to reduce the amount of refrigerant inventory in the primary system, and mechanical subcoolers typically used to transfer a part of the refrigeration load from a lower-temperature system to a more efficient higher-temperature system,
+
+6)~~~~allows the use of liquid suction heat exchangers which will improve the cycle efficiency for some refrigerants,
+
+7)~~~~models three condenser fan types,
+
+8)~~~~allows the user to keep track of refrigerant inventory,
+
+9)~~~~does not assume that the compressor and condenser capacity is sufficient to meet the case loads, but carries unmet load over to the next time step,
+
+10)~provides optional suction piping heat gain for comparison to distribution piping heat gain for secondary systems. {[}Note, these piping heat gains are also reflected in the zone heat balance. This piping heat gain is not to be confused with the pressure change in the suction piping, even though this pressure change is typically expressed in terms of an change in the saturated suction temperature{]}.
+
+\subsubsection{Refrigeration System Loads and Convergence}\label{refrigeration-system-loads-and-convergence}
+
+The refrigeration loads for refrigerated cases and walk-ins are added to provide the first value for the refrigeration load on a detailed system, as well as the evaporating temperature. (If there are no cases or walk-ins served directly by a system, that system is not solved until the energy transfer loads are available.) The user can also choose to include suction pipe heat gain as a load on the system. The performance of refrigeration compressors is dependent upon the condensing and evaporating temperatures. The calculation starts with an estimated condensing temperature, which is used to calculate the compressor power use.
+
+\begin{equation}
+{\dot Q_{{\rm{Refrigeration}}}} = \sum {{{\dot Q}_{case}}}  + \sum {{{\dot Q}_{walkin}}} ( + \sum {{{\dot Q}_{PipeHeatGain}}} )
+\end{equation}
+
+\begin{equation}
+{\dot Q_{System,Estimated}} = {\dot Q_{{\rm{Refrigeration}}}} + {P_{Compressors,Estimated}}
+\end{equation}
+
+These values are in turn used to determine the total heat rejection load on the condenser, which produces a new estimate for the condensing temperature. A few iterations are usually necessary to converge upon the final condensing temperature and compressor power for each time step for each system.
+
+After each detailed refrigeration system has been solved, all energy transfers (subcoolers, secondary loops, and cascade condensers) among the systems are made.
+
+\begin{equation}
+  \begin{array}{rl}
+    \dot{Q}_{Transfer} &= \sum \dot{Q}_{CascadeCondenser} + \sum \dot{Q}_{SecondaryLoop} + \sum \dot{Q}_{MechanicalSubcooler} \\
+    \dot{Q}_{Refrigeration} &= \sum \dot{Q}_{Case} + \sum \dot{Q}_{WalkIn} + \sum \dot{Q}_{Transfer} + \sum \dot{Q}_{PipeHeatGain}
+  \end{array}
+\end{equation}
+
+This two step process is repeated twice to ensure that all the energy transfers among systems are balanced.
+
+Suction piping heat gain is an optional element in the load calculation.~ Typically, the suction pipe heat gain is small compared to the other loads.~ However, when comparing DX systems to secondary systems, this portion of the total load can be very different. (Hinde, D., et al. 2009) ~To calculate the pipe heat gain load, the user must first calculate the U-value and area for the suction piping.~ The U-value is the total conductance from the inside skin coefficient to the outside skin coefficient. This value must be multiplied by the area to provide the ``sum of the UA in W/C,''~ required in the input.
+
+\subsubsection{Compressor Energy Use}\label{compressor-energy-use-1}
+
+The compressor object (Refrigeration:Compressor) calculations start with the determination of the inlet (suction) and outlet (discharge) conditions. The suction pressure is defined by the saturated suction temperature (equal to the evaporating temperature in the refrigeration loads connected to the suction group) minus the pressure drop in the suction pipes. With proper design, this pressure drop typically corresponds to a saturated suction temperature drop of about 1C. The saturated discharge pressure is defined by the condensing temperature plus the pressure drop in the discharge pipes. With proper design, this discharge pipe pressure drop typically corresponds to a saturated discharge temperature increase of about 0.5C (ASHRAE 2006a). These two temperatures are then used with the manufacturer's performance curves for each compressor. The performance curves are defined in ARI Standard 540 and take the following form (ARI 2004):
+
+\begin{equation}
+  \begin{array}{rl}
+    X &= {C_1} + {C_2}(S) + {C_3}(D) + {C_4}({S^2}) + {C_5}(SD) + {C_6}({D^2}) + {C_7}({S^3}) + {C_8}(D{S^2}) + {C_9}(S{D^2}) + {C_{10}}({D^3}) \\
+    S &= {T_{evap}} - 1. \\
+    D &= {T_{condense}} + 0.5
+  \end{array}
+\end{equation}
+
+where:
+
+X~~~ = can represent power input (W), or cooling capacity(W)
+
+C~~~ ~ = compressor performance coefficient (be sure to see the IO Reference guide because the Energy Plus input order for this equation does not match this ARI form)
+
+S~~~ = Saturation temperature corresponding to the suction pressure (C)
+
+D~~~ = Saturation temperature corresponding to the discharge pressure (C)
+
+T\(_{evap}\)~~~~~~~~~~~ = Evaporating temperature (C)
+
+The rated values for the cooling capacity and power consumption from the manufacturer include a specified amount of subcooling before the thermal expansion valve and a certain amount of superheat in the suction gas. Adjustments must be made to these rated values to reflect the actual subcooling and superheat conditions. Actual subcooling is determined by the condenser's rated subcooling and by the subcooling provided by optional subcoolers. The actual superheat is determined by the refrigerated case superheat (usually set to ensure that there is no liquid in the suction lines leading to the compressors), set here at 4C, and the effect from any optional subcoolers(ASHRAE 2006b). These various state points are shown in Figure~\ref{fig:state-points-and-energy-flows-for-detailed}.
+
+\begin{figure}[hbtp] % fig 280
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6275.png}
+\caption{State Points and Energy Flows for Detailed Refrigeration System \protect \label{fig:state-points-and-energy-flows-for-detailed}}
+\end{figure}
+
+Once the corrected capacity is calculated for each compressor, the compressors are dispatched one at a time until the system load is met. The last compressor dispatched is assumed to run at full load for the fraction of the time step necessary to meet the load, That is, the model neglects compressor cycling losses at part-load conditions. Using the state point identification from Figure~\ref{fig:state-points-and-energy-flows-for-detailed}, these corrections are shown in the following equations. If the capacity available from all the compressors is less than the sum of the case loads for that time period, the unmet load is accumulated to be met in succeeding time steps. If this accumulated unmet load becomes too great, a warning message is generated.
+
+\begin{equation}
+  \begin{array}{rl}
+    Cap_{corrected} &= \frac{\rho_{1b}}{\rho_{1c}} \times \frac{h_{1b} - h_4}{h_{1c} - h_{4c}} Cap_{rated} \\
+    \dot{m} &= \frac{Cap_{corrected}}{h_{1b} - h_4}
+  \end{array}
+\end{equation}
+
+where:
+
+\(\dot m\) = mass flow rate of refrigerant, kg/s
+
+�~~~ = density, kg/m\(^{3}\)
+
+h~~~ = enthalpy, J/kg
+
+Cap~~~~~~~~~~~ = refrigeration capacity of an individual compressor, W
+
+Compressor performance can also be improved by allowing the suction pressure to rise whenever the sum of the loads on the refrigerated cases served by the compressors is less than the design load. The calculation of the maximum allowable evaporator temperature is described in ``Variable Evaporator Temperature'' in the discussion of Refrigeration Cases.
+
+\subsubsection{Two-Stage Compression Systems}\label{two-stage-compression-systems}
+
+In addition to the single-stage compression refrigeration system illustrated above, two-stage compression systems can be modeled.~ For low temperature applications where the pressure ratio between the low- and high-pressure sides of the system could be 1:10 or more, it may be beneficial to utilize two stages of compressions (Evans 2008).~ Two smaller compressors in series have a smaller displacement and usually operate more efficiently than one large compressor that covers the entire pressure range from the evaporator to the condenser.~ This is especially true in ammonia refrigeration systems due to the large amount of superheating that occurs during the compression process (ASHRAE 2009b).
+
+Between the two stages of compression, an intercooler is used to cool the discharge gas exiting the low-stage compressor before it enters the high-stage compressor.~ The cooling is performed within the intercooler by refrigerant at an intermediate pressure.~ The degree to which intercooling reduces the power requirement of a refrigeration cycle depends on the refrigerant which is being used as well as the temperature lift between the evaporator and the condenser.
+
+Several methods of two-stage compression and intercooling have been used.~ For large industrial refrigeration systems, typical of ammonia systems used in refrigerated warehouses, both shell-and-coil intercooling (Figure~\ref{fig:two-stage-compression-system-with-a-shell}) and flash intercooling (Figure~\ref{fig:two-stage-compression-system-with-a-flash}) are used.~ The two stages of compression in these systems may be performed by separate low- and high-stage compressors or with a compound compressor containing both the low and high stages within the same compressor body.
+
+\begin{figure}[hbtp] % fig 281
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6278.png}
+\caption{Two-Stage Compression System with a Shell-and-Coil Intercooler. \protect \label{fig:two-stage-compression-system-with-a-shell}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 282
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6279.png}
+\caption{Two-Stage Compression System with a Flash Intercooler. \protect \label{fig:two-stage-compression-system-with-a-flash}}
+\end{figure}
+
+For two-stage compression systems with intercooling, there is an optimum intermediate pressure that minimizes the total power consumption of the system.~ In the case of an ideal intercooler in which the refrigerant gas enters the high-stage compressor at the same temperature as it enters the low-stage compressor, the minimum compressor work is achieved using the same pressure ratio across both compressors (Baek et al. 2005).~ Typically, the optimum intermediate pressure is approximated as the geometric mean pressure of the system as follows:
+
+\begin{equation}
+{P_{{\mathop{\rm int}} ercooler}} = \sqrt {\left( {{P_{evaporator}}} \right)\left( {{P_{condenser}}} \right)}
+\end{equation}
+
+where \emph{P\(_{intercooler}\)} is the pressure within the intercooler shell, \emph{P\(_{evaporator}\)} is the evaporating pressure and \emph{P\(_{condenser}\)} is the condensing pressure.
+
+The low-stage compressors operate between the evaporator pressure and the intercooler pressure while the high-stage compressors operate between the intercooler pressure and the condensing pressure.~ The performance of both the low-stage and high-stage compressors are modeled using the compressors' performance curves defined by ARI Standard 540 (ARI 2004), as discussed previously in the ``Compressor Energy Use'' section.~ In addition, capacity corrections are applied to the compressor performance curves to account for deviations between the actual operating conditions and the rated conditions.
+
+Refering to Figure~\ref{fig:two-stage-compression-system-with-a-shell} for a two-stage system with a shell-and-coil intercooler, the performance of the intercooler is modeled with a ``Shell-and-Coil Intercooler Effectiveness'', defined as follows:
+
+\begin{equation}
+\eta  = \frac{{{T_4} - {T_{5a}}}}{{{T_4} - {T_3}}}
+\end{equation}
+
+where \emph{η} is the shell-and-coil intercooler effectiveness, \emph{T}\(_{4}\) is the inlet temperature of the liquid refrigerant at Location 4, \emph{T}\(_{5*a*}\) is the outlet temperature of the liquid refrigerant at Location 5a, and \emph{T}\(_{3}\) is the saturated refrigerant temperature within the intercooler shell.~ Valid values for the effectiveness range from 0.0 to 1.0.~ An effectiveness of zero indicates that no heat is transferred from the refrigerant in the shell-side of the intercooler to the liquid refrigerant in the coil-side of the the intercooler, and thus, there is no change in the temperature of the liquid refrigerant from Location 4 to Location 5a.~ An effectiveness of 1.0 indicates that the temperature of the liquid exiting the coil-side of the intercooler at Location 5a is equal to the temperature of the saturated refrigerant in the shell-side of the intercooler.~ The user may specify a value for the intercooler effectiveness and a default value of 0.8 is used if no value is specified.~ Furthermore, it is assumed that saturated vapor refrigerant exits the shell-and-coil intercooler at Location 9.
+
+For the flash intercooler shown in Figure~\ref{fig:two-stage-compression-system-with-a-flash}, it is assumed that saturated liquid exits the intercooler at Location 3a and saturated vapor refrigerant exits the intercooler at Location 7.
+
+The two-stage compression refrigeration system may include an optional mechanical subcooler or liquid-suction subcooler.~ These subcoolers cool the liquid refrigerant which exits the intercooler before the refrigerant enters the thermal expansion valve.~ Further details regarding the modeling of mechanical and liquid-suction subcoolers may be found in the ``Subcoolers'' section.
+
+\subsubsection{Condenser Performance}\label{condenser-performance}
+
+Only one condenser is allowed per system. However, multiple refrigeration systems can reject heat through the same condenser. If a single condenser is used by multiple refrigeration systems, the code will iterate just as it does for loads transferred between systems to ensure that the total load on the condenser is accounted for in determining the saturated condensing temperature.
+
+The condenser can be modeled as dry air cooling, wet evaporative cooling, water loop cooling, or cascade cooling. (The detailed system can not be used for a compressor rack discharging heat into a conditioned zone.) The condenser performance is modeled to determine: (1) the condensing temperature and enthalpy of the refrigerant entering the refrigerated cases attached to the suction group, both of which will influence the efficiency of the compressors, (2) auxiliary power consumption for fans and pumps, and (3) water consumption for evaporative and water-cooled condensers.
+
+EnergyPlus can simulate waste heat being reclaimed from a detailed refrigeration system for use by refrigerant-to-air and refrigerant-to-water heating coils. (Refer to objects Coil:Heating:Desuperheater and Coil:WaterHeating:Desuperheater for a complete description of how these coils are modeled.) Heat reclaimed from the detailed refrigeration system is limited to the portion of the rejected heat in the superheat region. Using the state point nomenclature from Figure~\ref{fig:state-points-and-energy-flows-for-detailed}, this value is calculated by the detailed compressor and condenser models each time step as follows:
+
+\$\$ \({\dot Q_{AvailableSuperheat}} = \dot m\left( {{h_{{\rm{2}}a}} - {h_{2b}}} \right)\)
+
+Heat reclaimed for hot gas or hot brine defrost is not limited to the superheat range. However, if an excessive amount of the system rejected heat is diverted for that purpose, a warning is issued advising the user to increase the diversity of the defrost schedules.
+
+The total heat rejection load on the condenser is the sum of the case and walk-in loads, any transfer loads (e.g., mechanical subcooler or secondary system (see object Refrigeration:SecondarySystem)) on the system(s), and the total compressor power. The condenser load is reduced by any heat reclaimed by desuperheating coils for HVAC or water heating purposes and hot gas or hot brine defrost. If a secondary system or cascade condenser is served by the system(s) using this condenser, any defrost heat rejection credits from loads on the secondary system are assigned to this condenser.
+
+\begin{equation}
+{\dot Q_{Rejected}} = \sum {{{\dot Q}_{System}}}  - \sum {{{\dot Q}_{Reclaimed}}}
+\end{equation}
+
+where: \(\dot{Q}_{Rejected}\) = Heat rejected by the condenser (W)
+
+\(\sum {{{\dot Q}_{Reclaimed}}}\) = Sum of all the heat reclaimed by desuperheater coils and hot gas and hot brine defrost (W)
+
+Depending upon the condenser type, the heat rejection environment is set to the ambient conditions, conditions corresponding to a defined ouside air node (sometimes used to represent condensers located above ground level) or zone node, to a temperature specified for a water-cooled condenser, or according to the evaporating temperature for a higher-temperature loop (used for cascade condensers).
+
+The enthalpy of the condensed refrigerant leaving the condenser is equal to:
+
+\begin{equation}
+{h_{condenser,out}} = {h_{sat,liquid}}({T_{condense}}) - {c_{p,sat,liquid}}({T_{condense}}) \times \Delta {T_{RatedSubcooling}}
+\end{equation}
+
+where
+
+h\(_{condenser,out}\)~~~~ = enthalpy leaving the condenser, J/kg
+
+h\(_{sat,liquid}\)~~~~~~~~ = enthalpy of saturated liquid at the condensing temperature, J/kg
+
+c\(_{p,sat,liquid}\) = specific heat of saturated liquid at the condensing temperature, J/kg-C
+
+ΔT\(_{RatedSubcooling}\)~~~~~~~~~~~ = Amount of subcooling included in condenser rated heat rejection, C
+
+A minimum condensing temperature is specified for the detailed refrigeration system, and is usually required to maintain acceptable thermal expansion valve performance. When the calculated condensing temperature is less than this minimum, the air flow for air and evaporative-cooled condensers is reduced to reduce the condenser capacity and maintain the required condensing temperature.
+
+\paragraph{Air-Cooled Condensers}\label{air-cooled-condensers}
+
+The heat rejection capacity of a dry air-cooled condenser object (Refrigeration:Condenser:AirCooled) is directly proportional to the difference between the condensing temperature and the drybulb temperature for the heat rejection environment. The manufacturers typically provide the performance data, at one standard atmosphere, in a linear relationship between heat rejection and temperature difference. A correction factor is applied to account for the variation in air density with elevation (Carrier 1999).
+
+\begin{equation}
+  \begin{array}{rl}
+    Hrej_{Rated} &= C_1 + C_2 \PB{T_{condenser} - T_{drybulb}} \\
+    Hrej_{Rated,corrected} &= Hrej_{Rated} \PB{1 - \PB{7.17E-5 \times Elevation}}
+  \end{array}
+\end{equation}
+
+where:
+
+Hrej\(_{Rated}\) = Manufacturer's rated heat rejected by the condenser (W)
+
+C\(_{1}\) = Intercept taken from manufacturer's condenser performance data (W)
+
+C\(_{2}\) = Coefficient taken from the manufacturer's condenser performance data (W/C)
+
+T\(_{condense}\) = Condensing temperature (C)
+
+T\(_{drybulb}\) = Drybulb temperature for the local environment (C)
+
+Elevation = Local elevation (m)
+
+The manufacturer's form of performance data is used internally to define the condensing temperature as a function of the heat rejection load.
+
+\begin{equation}
+{T_{condense}} = {T_{drybulb}} + \left( {\frac{{Hrej - {C_1}}}{{{C_2}}}} \right) \div (1 - 7.17E - 5 \times Elevation)
+\end{equation}
+
+This calculated condensing temperature is then compared to the minimum condensing temperature allowed for that system. If necessary, the air flow to the condenser is reduced to maintain the condensing temperature at or above that minimum value.
+
+\paragraph{Condenser Fan Energy Use}\label{condenser-fan-energy-use-1}
+
+Condenser fan power for air-cooled condensers is determined by the type of fan control, fixed, variable speed, or two-speed. For all three fan control types, the fan power is set equal to the rated fan power whenever the calculated condensing temperature is greater than or equal to the minimum allowed condensing temperature. If the calculated temperature is less than the minimum allowed, the condenser air flow must be reduced. The reduced rated capacity is calculated using the previous equation for \emph{Hrej\(_{Rated}\)} with the specified minimum condensing temperature. (Note, the minimum condensing temperature is often determined by the expansion valve performance, and is therefore input with the system description, not with the condenser description.) The air flow for the reduced condenser capacity is:
+
+\begin{equation}
+  \begin{array}{rl}
+    Hrej &\propto \text{AirVelocity}^N \\
+    \text{Air Velocity} &\propto Hrej^{1/N} \\
+    \text{Air Volume Ratio} &= \PB{\frac{Hrej}{Hrej_{Rated}}}^{1/N}
+  \end{array}
+\end{equation}
+
+where:
+
+N~~~ = ~~~~~~~~~ 0.633 for turbulent air flow over cylinders (ASHRAE 2005)
+
+The Air Volume Ratio is limited by a minimum value, which may be specified by the user. The default for this value is 0.2,
+
+Four fan curves are built into the condenser fan model to represent four types of fan control, as shown in Figure~\ref{fig:condenser-fan-power-curve-options}. (Lawrence Berkeley Laboratory and Resource Dynamics, April 2003)
+
+\begin{figure}[hbtp] % fig 283
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6291.svg.png}
+\caption{Condenser fan power curve options \protect \label{fig:condenser-fan-power-curve-options}}
+\end{figure}
+
+For a fixed-speed fan, the air flow is reduced through either the use of dampers or by cycling the fan on and off.
+
+For a cycling fan, the power variation with air flow volume is approximately linearabove the minimum air volume ratio as shown in the following equation for the option ``FixedLinear'':
+
+\begin{equation}
+{P_{CondFan}} = ({\rm{Air Volume Ratio}}){P_{CondFan,design}}
+\end{equation}
+
+where:
+
+\({P_{CondFan}}\) ~~~~~~~~~~~~~~~~~ = output variable ``Refrigerated Case Condenser Fan Electric Power {[}W{]}'', not allowed to exceed the design condenser fan power
+
+\({P_{CondFan,design}}\) ~~~~~~~~~~ = design condenser fan power (W)
+
+For a fixed speed fan with damper (corresponding to the option ``Fixed''), the shape of the power fraction curve is as shown above, and calculated using:
+
+\begin{equation}
+{P_{CondFan}} = ({\rm{Air Volume Ratio}}){e^{(1 - {\rm{Air Volume Ratio}})}}{P_{CondFan,design}}
+\end{equation}
+
+For an ideal variable speed fan, the power is proportional to the cube of the air flow. To reflect non-ideal real systems, an exponent of 2.5 is used as shown in the following equation:
+
+\begin{equation}
+{P_{CondFan}} = {({\rm{Air Volume Ratio}})^{2.5}}{P_{CondFan,design}}
+\end{equation}
+
+For a two-speed fan, the fan power is varied as for a constant speed fan with dampers for Air Volume Ratios greater than or equal to 0.6. For lower Air Volume Ratios,~ which correspond to a half-speed fan setting, the power is reduced to the variable fan power value at that point and then varied as for damper control below Air Volume Ratios (AVR) of 0.6.
+
+\begin{equation}
+  P_{CondFan} = \left\{ \begin{array}{cr}
+                          \PB{AVR}\PB{e^{\PB{1-AVR}}}P_{CondFan,Design} & if AVR \geq 0.6 \\
+                          \PB{\frac{AVR+0.4}{2^{2.5}}}\PB{e^{\PB{1-AVR}}}P_{CondFan,Design} & if AVR < 0.6
+                        \end{array}
+                \right.
+\end{equation}
+
+For a water cooled condenser, there is no fan load at the condenser (i.e., the~ water/refrigerant heat exchanger). Any fan load would be related to and accounted for at the heat rejection object (e.g., cooling tower)
+
+\paragraph{Evaporative-Cooled Condensers}\label{evaporative-cooled-condensers}
+
+The input object Refrigeration:Condenser:EvaporativeCooled allows using evaporative cooling rather than dry air cooling which will allow for more efficient condenser heat rejection based on the entering air approaching the wet-bulb temperature rather than the dry-bulb temperature. Analyses under the International Energy Agency's (IEA) Heat Pumping Programme Annex 26 indicates that this measure can improve refrigeration system efficiency by up to 10\% (IEA 2003). The basin heater energy and water pumping power consumption for evaporative condensers in the detailed refrigeration system is modeled as described for the Refrigeration:CompressorRack. Just as for air-dried condensers, an elevation correction is needed to adjust for the variation in density of the air. This correction factor was derived by combining the barometric pressure correction from ARI 490 and a standard correlation for barometric pressure as a function of elevation(ARI 2008, NASA 1976).
+
+\begin{equation}
+  \begin{array}{rl}
+    Hrej_{Rated,Corrected} &= Hrej_{Rated} \RB{ 1 + k_1 B P_{std} \PB{1 - e^{\PB{A \times Elev}}}} \\
+    A &= \frac{g_0 M_0}{R^* T_b} = - 0.00012m^{-1}
+  \end{array}
+\end{equation}
+
+where
+
+k\(_{1}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ 0.0023 for pressure stated in kPa, (ARI 2008)
+
+BP\(_{std}\)~~~~~~~~~~ = ~~~~~~~~~ Standard atmosphere at rating conditions (101.0 kPa)
+
+g\(_{0}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ Gravitational constant (9.80665 m/s\(^{2}\))
+
+R*~~~~~~~~~~~~~~ = ~~~~~~~~~ Universal gas constant (8.31432E3 N-m/kmol-K
+
+M\(_{0}\)~~~~~~~~~~~~~ = ~~~~~~~~~ Molar mass of air (28.9644 kg/kmol)
+
+T\(_{b}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ Standard temperature (288.15 K)
+
+Although based upon an exponential relationship, the resulting correction is very nearly linear within the range of elevations found upon dry land, so the following form of correction is used:
+
+\begin{equation}
+Hre{j_{Rated,Corrected}} = Hre{j_{Rated}} \times (1 - 3.07E - 5 \times Elevation)
+\end{equation}
+
+To calculate the condensing temperature for an evaporative cooled condenser, it is necessary to provide the manufacturer's performance data. The manufacturers typically provide this data as a table of condensing temperature as a function of both entering wet-bulb temperature and the ratio of the heat rejected to the rated heat rejected. This data can be well represented, as shown in Figure~\ref{fig:comparison-of-the-condensing-temperature}, by a regression of the form:
+
+\begin{equation}
+  \begin{array}{rl}
+    \PB{T_{condense} - T_{wetbulb}} &= {C_1} + {C_2} \times HRCF + \frac{C_3}{HRCF} + {C_4}{T_{wetbulb}}\, or: \\
+    T_{condense} &= {C_1} + {C_2} \times HRCF + \frac{C_3}{HRCF} + \PB{1 + C_4}T_{wetbulb}
+  \end{array}
+\end{equation}
+
+Where: $HRCF = \frac{Hrej_{Rated}}{Hrej}$
+
+C\(_{1}\), C\(_{2}\), C\(_{3}\), and C\(_{4}\)~~~~ = ~~~~~~~~~ Coefficients determined by regression from manufacturer's data.
+
+Figure~\ref{fig:comparison-of-the-condensing-temperature} shows a comparison between this equation form, which produced an adjusted R\(^{2}\) of 0.998 and a maximum residual of 0.7C, for one manufacturer of evaporative condensers. Data from two other manufacturers showed similar agreement with this parameterization.
+
+\begin{figure}[hbtp] % fig 284
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6301.svg.png}
+\caption{Comparison of the condensing temperature predicted by four-factor equation to manufacturer's data \protect \label{fig:comparison-of-the-condensing-temperature}}
+\end{figure}
+
+Again, the condensing temperature is not allowed to fall below the system's minimum allowed condensing temperature. Just as with an air-cooled condenser, the air flow through the condenser is controlled to maintain this minimum condensing temperature and the air velocity reduction is a function of the decreased capacity (Manske, 1999). For an evaporative condenser, relevant capacity is not the amount of heat rejected, but the rated capacity at that reduced air flow. That decreased rated capacity must first be calculated based upon the specified minimum condensing temperature. Using Equation , the specified condensing temperature is used to calculate the reduced HRCF, which is used with the current heat rejection to calculate the ``reduced Rated Heat Rejection''.
+
+\begin{equation}
+  \begin{array}{rl}
+    0 = C_2 \times HRCF^2 + \left( \RB{C_1 + C_4 T_{wetbulb} - \left( \PB{T_{condenser} - T_{wetbulb}}}\right) \right) \times HRCF + C_3 \\
+    \text{Reduced Rated Heat Rejection} = HRCF \times Hrej \\
+    \text{Air Volume Ratio} = \left( \PB{\frac{\text{Reduced Rated Heat Rejection}}{Hrej_{Rated}}}\right) ^{1/N}
+  \end{array}
+\end{equation}
+
+where:
+
+N = exponent for evaporative condensers, set to 0.76 (Manske, 1999)
+
+The water consumption for an evaporative condenser is calculated based upon the air flow rate, the total heat rejection, and the heat rejection environment. The amount of water consumption also includes the amount of water that is purged to reduce the concentration of contaminants. The purge water is estimated as proportional to the heat rejection, at a rate of 5.0E-10 m\(^{3}\)/s per Watt of heat rejection (B.A.C., 2007). (This value, which corresponds to 3 gal./min. per 100 tons, is slightly more conservative than the value quoted by ASHRAE, 2004.) For the compressor racks, the condenser effectiveness was input as a function of the environmental wetbulb temperature. For the detailed evaporative condenser, the input data instead describes the capacity as a function of environmental conditions and loading. From that data, the water evaporation is calculated using the effectiveness corresponding to a fully loaded condenser. When the condenser is operating outside the bounds of the manufacturer's data, the effectiveness is limited to a maximum value of 0.9.
+
+\begin{equation}
+  \begin{array}{rl}
+    \eta &= \frac{Hrej}{\dot{V}_{air,rated} \rho_{air} \PB{\left. h \right|_{Tcondense,sat} - h_{air,in}}} \\
+    h_{air,out} &= h_{air,in} + \eta \PB{\left. h \right|_{Tcondense,sat} - h_{air,in}} \\
+    T_{air,out} &= T_{saturated}\PB{h_{air,out},P_{barometric}} \\
+    \dot{V}_{evaporation} &= \frac{\text{AirVolumeRatio} \cdot \dot{V}_{air,rated} \cdot \rho_{air,dry} \cdot \PB{\omega_{air,out} - \omega_{air,in}}}{\rho_{water}} \\
+    \dot{V}_{makeup} = \dot{V}_{evaporation} + \dot{V}_{purge}
+  \end{array}
+\end{equation}
+
+where:
+
+\({\left. h \right|_{Tcondense,sat}}\) = enthalpy of saturated air at the calculated condensing temperature
+
+h\(_{air,out}\) = enthalpy of the air leaving the condenser,
+
+h\(_{air,in}\) = enthalpy of the inlet air, psychometric function of inlet air drybulb temperature and humidity ratio
+
+\({\dot V_{air,rated}}\) = rated volumetric air flow for the evaporative condenser (input value) m\(^{3}\)/s
+
+�\(_{air}\) = density of air evaluated at environmental conditions
+
+�\(_{air,dry}\) = density of dry air evaluated at environmental temperature
+
+T\(_{air,out}\) = air temperature leaving the condenser, psychometric function of saturated air at the enthalpy leaving the condenser and the barometric pressure
+
+\({\dot V_{evaporation}}\) = Volumetric rate of water evaporation in the condenser, m\(^{3}\)/s
+
+ω\(_{air,out}\) = humidity ratio (kg\(_{water}\)/kg\(_{dry\\ air}\)) of the air leaving the condenser, psychometric function of T\(_{air,out}\) and the barometric pressure
+
+ω\(_{air,in}\) = humidity ratio (kg\(_{water}\)/kg\(_{dry\\ air}\)) of the air at environmental conditions
+
+�\(_{water}\) = density of water evaluated at the environmental wetbulb temperature (kg/m\(^{3}\))
+
+\({\dot V_{purge}}\) = Volumetric rate of water purged in the condenser, m\(^{3}\)/s
+
+\({\dot V_{makeup}}\) = Volumetric rate of water makeup in the condenser, m\(^{3}\)/s
+
+The source of the makeup water may be specified as a water storage tank. If not specified, the makeup water is assumed to come from the building mains (Ref. Water Mains Temperatures).
+
+An evaporative condenser can be scheduled, using the Evaporative Condenser Availability Schedule described previously, so that it operates in a dry mode for a portion of the year. This is important in climates subject to freezing weather in order to avoid excessive ice formation on the condenser surfaces and surroundings. (The Availability Schedule is the correct way to model the use of evaporative condensers in cold climates. However, some users may take a single input description and use it to model a building with a refrigeration system in a variety of climates. To avoid modeling the use of evaporative coolers in freezing weather, the code includes a cutout to switch to dry operation whenever the outdoor drybulb temperature drops below 4C.) Dry operation can also reduce water use when the dry heat rejection capacity of the equipment is sufficient to meet the load during times of the year when the outside drybulb temperature is reduced. In dry operation, the condenser heat rejection capacity is approximately one third of the rated wetted heat rejection capacity(Manske, 2000). In dry operation, the condensing temperature is estimated by using the same four-factor equation, but using the air drybulb temperature instead of the wetbulb temperature and using the reduced heat rejection capacity factor.
+
+\begin{equation}
+  \begin{array}{rl}
+    HRCF_{dry operation} &= \frac{HRCF_{wet operation}}{3.0} \\
+    T_{condense,dry operation} &= {C_1} + {C_2} \times HRCF_{dry operation} + \frac{C_3}{HRCF_{dry operation}} + \PB{1 + C_4} T_{drybulb}
+  \end{array}
+\end{equation}
+
+\paragraph{Water-Cooled Condensers}\label{water-cooled-condensers}
+
+If the condenser heat rejection is specified as water cooled (input object Refrigeration:Condenser:WaterCooled), the model uses the same algoithms described above for Refrigeration Compressor Racks. The condensing temperature is set equal to the inlet water temperature plus an approach temperature equal to the difference between the rated values for water inlet temperature and condensing temperature.
+
+\paragraph{Cascade Condensers}\label{cascade-condensers}
+
+A cascade condenser joins two full detailed refrigeration systems; that is, both systems joined by the cascade condenser have loads, compressor(s), and a condenser, as shown in Figure~\ref{fig:a-cascade-condenser-is-used-to-reject-heat}.
+
+\begin{figure}[hbtp] % fig 285
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6310.png}
+\caption{A cascade condenser is used to reject heat from a low-temperature detailed refrigeration system to a higher-temperature detailed refrigeration system \protect \label{fig:a-cascade-condenser-is-used-to-reject-heat}}
+\end{figure}
+
+The input object, Refrigeration:Condenser:Cascade, allows the use of a higher temperature refrigeration system (primary system) to serve as a heat rejection sink for a lower temperature refrigeration system (secondary system). The selection of the condensing temperature represents a trade-off in performance between the primary system absorbing the heat rejection and the secondary system rejecting heat. (Lee et al., 2006) If the condensing temperature control type is `fixed,' then the secondary system condensing temperature is held constant at the temperature specified for that cascade condenser (which should be greater than or equal to the secondary system's specified minimum condensing temperature). If the condensing temperature control type is `float', the condensing temperature is allowed to float according to the minimum required evaporating temperature for other loads served by the primary system.
+
+For fixed control:~ T\(_{condense}\) = T\(_{condense,rated}\)
+
+For floating control: T\(_{condense}\) = ΔT\(_{approach}\) + T\(_{evap,min}\)
+
+where
+
+T\(_{condense,rated}\)~~~ = ~~~~~~~~~ Rated condensing temperature for the cascade condenser, C
+
+ΔT\(_{approach}\)~~~~~ = ~~~~~~~~~ Rated approach temperature difference for the cascade condenser, DeltaC
+
+T\(_{evap,min}\)~~~~~~~~ = ~~~~~~~~~ Evaporating temperature required to meet other loads on the primary system, C.
+
+The approach temperature difference (the difference between the condensing and evaporating temperatures) in the cascade condenser, is held constant at the rated value.~ That is, the approach temperature difference is not varied according to the load on the condenser.
+
+For cases and walk-ins served by cascade condensers, energy needed for hot brine or hot gas defrost is reclaimed from the primary system.~ The refrigeration load the cascade condenser places upon the primary system is classified as a `transfer load', because it transfers load from one system to another. This load is the sum of all case and walk-in loads served by the secondary system, any suction piping heat gains on the secondary loop, plus the secondary loop's compressor power. The same name (Ref. Refrigeration:Condenser:Cascade, field ``Name'') used to identify the condenser in the secondary loop is used to identify the transfer load on the primary system.
+
+\begin{equation}
+{\dot Q_{{\rm{Cascade}}}} = {\sum {\dot Q}_{{\rm{Case}}}} + \sum {{{\dot Q}_{{\rm{Walkin}}}} + } \sum {{{\dot Q}_{{\rm{Compressor}}}}} \left( { + \sum {{{\dot Q}_{{\rm{PipeHeatGain}}}}} } \right)
+\end{equation}
+
+where
+
+\({\dot Q_{Cascade}}\) ~~~~~ = Total refrigeration load the cascade condenser places upon the primary system, W
+
+\({\dot Q_{Case}}\) ~~~~~~~~ = Case load on the secondary loop , W
+
+\({\dot Q_{Walkin}}\) ~~~~~~~ = Walk-in load on the secondary loop, W
+
+\({\dot Q_{Compressor}}\) ~~ = Power input to a compressor on the secondary loop, W
+
+\({\dot Q_{PipeHeatGain}}\) = Heat gain in secondary loop suction pipe, W
+
+\textbf{Even though a cascade condenser is considered to be a part of a secondary loop, that loop is described with the Refrigeration:System object, not with the object, Refrigeration:SecondarySystem, described below.}
+
+\subsubsection{Subcoolers}\label{subcoolers}
+
+Subcooler objects (Refrigeration:Subcooler) reduce the temperature of the liquid refrigerant after it leaves the condenser and before it reaches the thermal expansion valve, corresponding to state point, 3b, on Figure~\ref{fig:state-points-and-energy-flows-for-detailed}. The detailed refrigeration system permits the use of two type of subcoolers, mechanical and liquid suction. A mechanical subcooler is used to transfer refrigeration load from a lower-temperature system to a higher-temperature system. For example, the compressors that are used to provide cooling for dairy products could be used to subcool the refrigerant in another system that is serving frozen food cases. For the system providing the cooling, the mechanical subcooler acts like another refrigerated case load. For the system receiving the cooling, the mechanical subcooler reduces the enthalpy of the refrigerant from point 3a to point 3b on Figure~\ref{fig:state-points-and-energy-flows-for-detailed}, and thus reduces the required refrigerant flow rate. Mechanical subcooler performance is defined by the controlled temperature of the subcooled liquid as follows:
+
+\begin{equation}
+  \begin{array}{rl}
+    \dot{Q} &= \dot{m} C_p \PB{T_{3a} - T_{control}} \\
+    h_{3b}  &= h_{3a} - C_{p,liquid} \PB{T_{3a} - T_{control}}
+  \end{array}
+\end{equation}
+
+where:
+
+\(\dot Q\) = subcooler load, W
+
+\(\dot m\) = mass flow rate of refrigerant, kg/s
+
+c\(_{p,liquid}\)~~~~~~~~~ = specific heat of saturated liquid at the condensing temperature, J/kg-C
+
+T\(_{control}\)~~~~~~~~~~ = control temperature specified for the mechanical subcooler, C
+
+h~~~ = enthalpy, J/kg
+
+A liquid suction heat exchanger (LSHX) subcooler uses the cold gas exiting the refrigerated cases to subcool the condensed liquid refrigerant in the same system. Depending upon the shape of the refrigerant's saturation curve and the operating condensing and evaporating temperature, this can save significant energy by reducing the required refrigerant flow (ASHRAE 2006a). (This model neglects the pressure drop through the suction side of the heat exchanger, although this pressure drop will cause the compressor to operate at a lower suction pressure.) A liquid suction heat exchanger is defined by specifying the design values for: inlet liquid temperature, inlet vapor temperature, and liquid temperature change. A liquid suction heat exchanger subcooler will also increase the superheat of the gas returning to the compressor, as shown by the difference between state points 1a and 1b in Figure~\ref{fig:state-points-and-energy-flows-for-detailed}:
+
+\begin{equation}
+  \begin{array}{rl}
+    \eta_{LSHX} &= \frac{\Delta T_{Design}}{T_{Liquid Design} - T_{Vapor Design}} \\
+    \dot{Q} &= \dot{m} C_{p,liquid} \eta_{LSHX} \PB{T_{3a} - T_{1a}} \\
+    T_{1b} &= T_{1a} + \frac{\dot{Q}}{\dot{m}C_{p,vapor}} \\
+    h_{3b} &= h_{3a} - \frac{\dot{Q}}{\dot{m}}
+  \end{array}
+\end{equation}
+
+where:
+
+ηLSHX~~~~~~~ = subcooler effectiveness, dimensionless
+
+c\(_{p,vapor}\)~~~~~~~~~ = specific heat of saturated vapor at the evaporating temperature, J/kg-C
+
+ΔT\(_{Design}\)~~~~~~~ = design liquid temperature difference, DeltaC
+
+T\(_{LiquidDesign}\)~~~~ = design liquid inlet temperature, C
+
+T\(_{VaporDesign}\)~~~~ = design vapor inlet temperature, C
+
+If a system is subcooled by both a mechanical subcooler and a liquid subcooler, the liquid subcooler will follow the mechanical subcooler and those points labeled `3a' in the liquid suction equations would correspond to the points labeled `3b' in the mechanical subcooler equations, that is, the inlet of the LSHX would be the outlet of the mechanical subcooler.
+
+Any one system can be cooled (i.e., have energy removed between points `3a' and `3b') by at most one liquid suction heat exchanger and one mechanical subcooler. However, a system can provide cooling to multiple mechanical subcoolers. For example if a building had one high temperature refrigeration system (perhaps cooling fresh produce) and three low temperature systems (perhaps cooling frozen foods and meat), each of the three low temperature systems could include a mechanical subcooler with the refrigeration energy for all three absorbed by the one high-temperature system. For the compressors and condenser on the high-temperature system, these three mechanical subcoolers would represent a load very similar to that of the refrigerated cases served by that system.
+
+\subsubsection{Suction Piping Heat Gains}\label{suction-piping-heat-gains}
+
+Suction piping heat gain is an optional element in the load calculation.~ Typically, the suction pipe heat gain is small compared to the other loads.~ However, when comparing DX systems to secondary systems, this portion of the total load can be very different. (Hinde, D., et al. 2009) ~To include the suction pipe heat gain load, the user must first calculate the U-value and outer surface area for the suction piping. The U-value is the total conductance from the inside skin coefficient, through the pipe insulation, to the outside skin coefficient. This value must be multiplied by the external surface area of the pipe insulation to provide the sum of the UA required in the input.~ These piping heat gains are also reflected in the zone heat balance.
+
+\({\dot Q_{PipeHeatGain}}\) ~ = ∑U*A (T\(_{zone}\) -- T\(_{SaturatedSuction}\))
+
+Where:
+
+~~~ \({\dot Q_{PipeHeatGain}}\) ~~ = ~Heat load on the detailed refrigeration system due to suction pipe heat gains (W)
+
+~~~ ∑U*A = ~~Sum of the product of the conductance times the surface area for the suction piping (W/C)
+
+\subsection{Secondary Refrigeration Systems}\label{secondary-refrigeration-systems}
+
+The object, Refrigeration:SecondarySystem, is used to model systems that do not have compressors, but have a circulating pump and a heat exchanger (called the secondary evaporator) where evaporating refrigerant in the primary loop absorbs heat rejected by the secondary loop.~ The purpose of the secondary refrigeration system model is to determine: the refrigerating load placed upon the primary system via the Secondary Evaporator, the required evaporating temperature in the Secondary Evaporator, any heat recovered for defrost purposes, and the total pump power.
+
+If your secondary loop includes compressors and a cascade condenser, do NOT use a Refrigeration:SecondarySystem object.~ Use a Refrigeration:System object with a Refrigeration:Condenser:Cascade object and list that condenser as a transfer load in the input description of the primary system.
+
+In the secondary loop shown in Figure~\ref{fig:secondary-loop-with-brine-or-glycol-solution}, the secondary evaporator serves to chill a brine or glycol solution (single phase) that in turn chills the refrigeration loads on the secondary loop.~ In Figure~\ref{fig:secondary-loop-with-liquid-overfeed}, the secondary evaporator serves as a condenser for a refrigerant that has been partially vaporized(two-phase) while circulating through the refrigeration loads on the secondary loop. Every secondary system includes a refrigeration load made up of refrigerated cases and/or walkins, a heat exchanger (called the Secondary Evaporator), and circulating pump(s). The loop performance at any one time step is determined by the effectiveness of the heat exchanger, the refrigeration load, and the pumping power needed to meet that load. The fluid temperature entering the cases and walk-ins is maintained at a set value.
+
+\begin{figure}[hbtp] % fig 286
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6323.png}
+\caption{Secondary loop with brine or glycol solution circulation \protect \label{fig:secondary-loop-with-brine-or-glycol-solution}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 287
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6324.png}
+\caption{Secondary loop with liquid-overfeed refrigerant circulation \protect \label{fig:secondary-loop-with-liquid-overfeed}}
+\end{figure}
+
+For both types of secondary loops, the primary refrigeration system absorbs the load by providing cold refrigerant that evaporates in the secondary evaporator.~ We classify this secondary load as a `transfer load' because it transfers load from one `system' to another. (Cascade condenser loads are also considered transfer loads.) Just as with any DX refrigeration evaporator, the variable load from the secondary system is served by varying the primary system refrigerant flow to the evaporator side of the secondary evaporator.~ Unmet load will be carried over to the next time step anytime the load on the secondary condenser/evaporator exceeds the rated capacity for the specified temperatures.~ (A warning will be generated if the total unmet energy grows excessively large.) ~The main differences between the single-phase secondary loop model and the two-phase secondary loop model lie in the definition and performance of the secondary evaporator and the way input data is processed to define evaporator capacity.
+
+For a brine system, the secondary loop capacity is matched to the case and walk-in load by varying the brine flow rate. (\emph{Throughout this section, `brine' will be used when referring to the secondary loop heat transfer fluid for systems where the secondary circulating fluid remains in the liquid state.)} When selecting the brine loop design parameters, it is important to consider the performance trade-off between pumping energy and the temperature difference, or range, in the heat exchanger. The circulating fluid selection is also critical in determining the performance of brine loop, with large variations caused by differences in viscosity and density (which impact pumping power requirements) and specific heat (which determines the required fluid flow rate). ~(Kazachki, G. S., and Hinde, D. K., 2006, Faramarzi, R. T., and Walker, D. H. 2004, ASHRAE. 2006c)
+
+For a secondary loop to accommodate a two-phase secondary coolant, additional hardware is required and the system control mode changes. A separator/receiver is required to separate the wet mixture of liquid and gas returning from the refrigeration load, as shown in Figure~\ref{fig:secondary-loop-with-liquid-overfeed}. ~(In the following discussion, we will refer to the secondary fluid in a liquid-overfeed system as CO\(_{2}\).) In Figure~\ref{fig:thermodynamic-cycle-for-a-liquid-overfeed}, which focuses in on the secondary loop alone, the gaseous CO\(_{2}\) moves via thermosiphon effect to the secondary evaporator, where heat is absorbed by the primary system to condense the CO\(_{2}\), which then returns via gravity flow to the separator/revceiver.~ The liquid CO\(_{2}\) is pulled from the bottom of the separator/receiver and pumped to the load. The term `liquid overfeed ratio' refers to the ratio of the total pumped mass flow rate (at the point labeled ``1'' on Figure~\ref{fig:thermodynamic-cycle-for-a-liquid-overfeed}) of CO\(_{2}\) to the mass rate of CO\(_{2}\) evaporated at the load (vapor portion of the flow at the point labled ``5'' on Figure~\ref{fig:thermodynamic-cycle-for-a-liquid-overfeed}). With a variable flow rate(obtained with either a variable-speed pump or multiple constant-speed pumps), the liquid overfeed ratio is maintained at or above the specified value. With a constant flow rate (obtained by specifying a single constant-speed pump), the liquid overfeed ratio will vary to match the capacity of the variable refrigeration load.(Hinde et al 2009) Even though a greater amount of CO\(_{2}\) is circulated than is evaporated, the pumping power requirements are still much less than those for a single-phase secondary coolant.
+
+\begin{figure}[hbtp] % fig 288
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6325.png}
+\caption{Thermodynamic cycle for a liquid overfeed secondary loop \protect \label{fig:thermodynamic-cycle-for-a-liquid-overfeed}}
+\end{figure}
+
+If the defrost type for any of the cases or walkins on the secondary loop is `HotBrine' or `HotGas', the defrost energy is assumed to come from the hot compressed gas leaving the compressors on the primary system, as shown in Figure~\ref{fig:secondary-loop-with-brine-or-glycol-solution} and Figure~\ref{fig:secondary-loop-with-liquid-overfeed}.(Minea, V. 2007) Therefore, the amount of heat rejected by the condenser for that primary system is reduced by the amount needed for defrost. Some research has shown that the defrost times for cases and walk-ins defrosted using hot brine can be significantly shorter than defrost times for electric or hot gas.(Terrell, W. J. Jr., 1999) The user should consider this factor when describing the input data for cases and walk-ins served by a secondary loop.
+
+\subsubsection{Secondary Evaporator in a Single-Phase Secondary Loop (Brine or Glycol Loop)}\label{secondary-evaporator-in-a-single-phase-secondary-loop-brine-or-glycol-loop}
+
+For a single-phase secondary system, the heat exchanger effectiveness is calculated based upon the input rating data, which includes the evaporating temperature, approach and range temperature differences, and heat exchanger capacity. The rated capacity for the heat exchanger can be specified by either providing the capacity in Watts, or the rated mass flow rate. The density and specific heat both correspond to those properties at the average temperature of the heat exchange fluid within the secondary loop heat exchanger.
+
+These variables are specified by the chiller manufacturer at rated conditions:
+
+~ ΔT\(_{Approach}\) ~~~~~~~~~~~~~~ = the approach temperature difference, DeltaC
+
+~ ΔT\(_{Range}\) ~~~~~~~~~~~~~~~~ = range temperature difference, DeltaC
+
+~ T\(_{EvapDesign}\) ~~~~~~~~~~~~~~ = ~heat exchanger evaporating temperature, C
+
+~ Flow\(_{RatedVolume}\) ~~~~~~~~ = brine flow rate through the heat exchanger~ (kg/s)
+
+~ Capacity\(_{Rated}\) ~~~~~~~~ = Heat exchanger cooling capacity (W)
+
+The rated conditions are used to calculate:
+
+~ T\(_{BrineOutRated}\) = T\(_{EvapDesign}\) + ΔT\(_{Approach}\)
+
+~ T\(_{BrineInRated}\) ~ = T\(_{BrineOutRated}\) + ΔT\(_{Range}\)
+
+~ Eta = Capacity\(_{Rated}\) / (Flow\(_{RatedMass}\) * C\(_{pBrine}\) * (T\(_{BrineInRated}\) - T\(_{EvapDesign}\)))
+
+~ T\(_{BrineAverage}\) = (T\(_{BrineOutRated}\) + T\(_{BrineInRated}\))/2
+
+If the capacity is specified and the flow rate is not, then the flow rate is calculated as:
+
+Flow\(_{RatedMass}\) = Capacity\(_{Rated}\)/(C\(_{pBrine}\)*ΔT\(_{Range}\))
+
+Flow\(_{RatedVol}\) = Flow\(_{RatedMass}\) / �\(_{Brine}\)
+
+If the flow rate is specified and the capacity is not, the capacity is calculated as:
+
+Flow\(_{RatedMass}\) = Flow\(_{RatedVol}\)*�\(_{Brine}\)
+
+Capacity\(_{Rated}\) = Flow\(_{RatedMass}\) * C\(_{pBrine}\)*ΔT\(_{Range}\)
+
+Where:
+
+~ Eta~~ ~~~~~~~~~~~~~~~~~~~ = heat exchanger effectiveness, dimensionless and less than one
+
+~ T\(_{BrineInRated\\}\)~~~~~~~~~~~ = heat exchanger brine inlet temperature at rated conditions (C)
+
+~ T\(_{BrineOutRated}\) ~~~~~~~~~~~~ = heat exchanger brine outlet temperature at rated conditions (C)
+
+~ T\(_{BrineAverage}\)~~~ ~~~~~~~~~~ = average brine temperature in the heat exchanger (C)
+
+~ Flow\(_{RatedMass}\) ~~~~~~~~~ = brine flow rate through the heat exchanger~ (kg/s)
+
+~ Flow\(_{RatedVol}\)~~ ~~~~~~~~~ = brine flow rate through the heat exchanger~ (m\(^{3}\)/s)
+
+~ C\(_{pBrine}\)~~~~~~~~~~ ~~~~~~~~ = brine specific heat (J/kg-C)
+
+~ �\(_{Brine}\)~ ~~~~~~~~~~~~~~~~~~~ = brine density (kg/m\(^{3}\))
+
+After the heat exchanger effectiveness has been calculated, the value for the heat exchanger design brine flow rate is compared to the design flow rate for the secondary loop pump(s).~ The maximum flow rate in the loop is limited to the smaller of these two values. The heat transfer capacity corresponding to this maximum flow rate is then calculated and compared to the rated heat exchanger capacity. The maximum load on the heat exchanger is limited to the lesser of these two values, the rated heat exchanger capacity or the capacity corresponding ot the maximum loop flow rate.
+
+Flow\(_{MaxVol}\) = Minimum(Flow\(_{RatedVol}\) ,Flow\(_{RatedPumpVol}\))
+
+Capacity\(_{AtMaxVolFlow}\) = Flow\(_{MaxVol}\) *Eta*( C\(_{pBrine}\) * Density\(_{Brine}\))*( T\(_{BrineInRated}\) -- T\(_{EvapDesign}\))
+
+Capacity\(_{Max}\) = Minmum(Capacity\(_{Rated}\) , Capacity\(_{AtMaxVolFlow}\))
+
+Where:
+
+Flow\(_{MaxVol}\)~ ~~~~~~~~~~~~~~ = Maximum loop volume flow, limited by either the pump rating or the heat exchanger rating (m\(^{3}\)/s)
+
+Capacity\(_{AtMaxVolFlow}\) ~~~ = Secondary loop capacity corresponding to the maximum loop flow rate (W)
+
+Capacity\(_{Max}\) ~~~~~~~~~~~ ~ = Maximum secondary evaporator capacity (W)
+
+\subsubsection{\texorpdfstring{Secondary Evaporator in a Two-Phase Secondary Loop~ (Liquid-Overfeed Loop, e.g., CO\(_{2}\))}{Secondary Evaporator in a Two-Phase Secondary Loop~ (Liquid-Overfeed Loop, e.g., CO\_\{2\})}}\label{secondary-evaporator-in-a-two-phase-secondary-loop-liquid-overfeed-loop-e.g.-coux5f2}
+
+For a two-phase system, the secondary evaporator effectiveness is not calculated. Both the evaporating and condensing sides of the heat exchanger are assumed to operate at fixed temperatures.~ If the capacity of the secondary evaporator is not input, it will be calculated as the sum of the rated loads plus the rated pump power.
+
+\begin{equation}
+  \begin{array}{rl}
+    Capacity_{Rated} &= \text{Input,  OR:} \\
+    Capacity_{Rated} &= \sum \dot{Q}_{Case} + \sum \dot{Q}_{WalkIn} + Power_{Pump} \\
+    Capacity_{Max}   &= Capacity_{Rated}
+  \end{array}
+\end{equation}
+
+If the flow rate through the evaporator is not input, it will be calculated based upon the input value for the Circulating Rate.
+
+\begin{equation}
+Flo{w_{{\rm{RatedVol}}}} = \frac{{\sum {{{\dot Q}_{{\rm{Case}}}} + \sum {{{\dot Q}_{{\rm{WalkIn}}}} + Powe{r_{{\rm{Pump}}}}} } }}{{{\rho_{Liquid}}\Delta {h_{fg}}}}
+\end{equation}
+
+Where:
+
+~ Ρ\(_{Liquid}\)~ ~~~~~~~~~~~~~~~~~~ = liquid density (kg/m\(^{3}\))
+
+Δh\(_{fg}\) ~~~~~~~~~~~~~~~~~~~~~~ = heat of vaporization (J/kg)
+
+\subsubsection{Secondary Loop Distribution Piping and Receiver Shell Heat Gains}\label{secondary-loop-distribution-piping-and-receiver-shell-heat-gains}
+
+Distribution piping and receiver shell heat gains are optional elements in the load calculation.~ Typically, the distribution pipe and receiver shell heat gains are small compared to the other loads.~ However, when comparing direct expansion systems to secondary systems, this portion of the total load can be very different. (Hinde, D., et al. 2009) To calculate the pipe heat gain load, the user must first calculate the U-value and area for the distribution piping. The U-value is the total conductance from the inside skin coefficient to the outside skin coefficient. This value must be multiplied by the piping external surface area to provide the sum of the UA required in the input.~ Note that these piping and receiver shell heat gains are also reflected in the zone heat balance, similar to the zone cooling credits provided by refrigerated cases.
+
+\({\dot Q_{PipeHeatGain}}\) ~ = ∑U*A (T\(_{zone}\) -- T\(_{BrineAverage}\))
+
+Where:
+
+\({\dot Q_{PipeHeatGain}}\) ~~ = ~Heat load on the secondary loop due to pipe heat gains, output variable ``Refrigeration Secondary Loop Pipe Heat Gain Rate {[}W{]}''
+
+∑U*A = ~~Sum of the product of the conductance times the surface area for the piping (W/C)
+
+The receiver shell heat gains are calculated in the same manner.
+
+\subsubsection{Secondary Loop Pumping Power and Secondary Loop Load}\label{secondary-loop-pumping-power-and-secondary-loop-load}
+
+Pump ratings are typically given in the form of curves. The input values for the pumps should correspond to the full-load design conditions, with respect to fluid viscosity, density, and temperature, as well as pressure drop. For these conditions, the user provides either the total pump power or the total head, as well as the flow rate. \emph{These values must be representative of the selected heat transfer fluid at the average loop operating temperature and pressure.} If the pump head at design conditions is specified, the pump power is calculated as:
+
+Power\(_{PumpRated}\) = Flow\(_{RatedPumpVol}\)* Head\(_{Rated}\)/ (Efficiency\(_{PumpImpeller}\)*Efficiency\(_{PumpMotor}\))
+
+Where:
+
+Power\(_{PumpRated}\) ~~~~~~~~~ = ~~Total pumping power for the secondary loop at rated conditions (W)
+
+Head\(_{Rated}\)~~~~~~~~ ~~~~~~~ = ~ Pressure drop through the entire secondary loop circulation at rated conditions, including at the pumps, the chiller, supply and return piping, and through the case and walk-in coils (pipes are typically sized to produce a total head ranging from 0.25E6 to 0.3E6 Pa (ASHRAE. 2006c))(Pa)
+
+Efficiency\(_{PumpImpeller}\) ~ = Pump impeller efficiency, dimensionless
+
+Efficiency\(_{PumpMotor}\)~~ ~ = Pump motor efficiency, dimensionless
+
+The pump impeller efficiency is assumed to be 78\%. (ASHRAE 2006c) The pump motor efficiency is assumed to be 85\%.(ITT 2009)~ If a semi-hermetic motor is specified, all the pump power is translated to heat within the fluid. The total heat load placed upon the loop by the pumps is therefore:
+
+\({\dot Q_{Pump}}\) ~ = Power\(_{PumpRated}\) * Ratio\(_{PowertoHeat}\)
+
+Where:
+
+\({\dot Q_{Pump}}\) ~~~~~~~~~~~~~~~~~~~~ = total heat load placed upon the secondary loop by the pumps (W)
+
+Ratio\(_{PowertoHeat}\) ~~~~~~~~~ = Ratio of total motor energy rejected to the circulating fluid to the total pump power used (input by the user, suggest 1.0 for semi-hermetic motors and 0.85 for others)
+
+A variable speed pump can be modeled by providing a cubic curve for pump power as a function of the ratio of total flow needed to the total flow specified at full load design conditions.
+
+\begin{equation}
+{\dot Q_{Pump}} = \left[ {A{{\left( {L{F_{Pump}}} \right)}^3} + B{{\left( {L{F_{Pump}}} \right)}^2} + C\left( {L{F_{Pump}}} \right) + D} \right] \times {\rm{Powe}}{{\rm{r}}_{{\rm{PumpRated}}}} \times {\rm{Rati}}{{\rm{o}}_{{\rm{PowertoHeat}}}}
+\end{equation}
+
+Where:
+
+LF\(_{Pump}\)~~~~~~~~ = ratio of total flow needed to the total flow specified at full load design conditions
+
+The user may also specify multiple constant-speed pumps.~ Multiple pumps, or pump staging, are often used to reduce the total pumping power requirements while still providing the capacity and constant pressure drop needed to meet peak design loads.(Faramarzi, R. T., and Walker, D. H. 2004) When multiple pumps are specified, the flow rate provided by one pump is compared to the flow rate needed to meet the refrigeration load on the loop during that time step. If that flow rate is insufficient, another pump is added, and the process is continued until the needed flow rate is met or all the pumps are included. The incremental power for each pump is added to determine the total pump power for the loop. Each pump is assumed to operate at full load if it is needed at all.~ A bypass is assumed to carry any fluid flow not needed to meet the load.~ An iterative solution is required for the total pump load on the heat exchanger because the flow rate is determined by the load, which includes the pump power that is determined by the necessary flow rate. For the first estimate, the pump power load is assumed to be zero.
+
+\begin{equation}
+  \begin{array}{rl}
+    \dot{Q}_{Refrigeration} &= \sum \dot{Q}_{Case} + \sum \dot{Q}_{WalkIn} \\
+    \dot{Q}_{TotalSecondary} &= \dot{Q}_{Refrigeration} + \dot{Q}_{Pump} + \sum \dot{Q}_{Pipe and Receiver Shell heat gains} \\
+    \text{FlowNeeded} &= \frac{\dot{Q}_{TotalSecondary}}{\eta C_{p,Brine} \rho_{Brine}\PB{T_{BrineOutRated} - T_{evap}}}
+  \end{array}
+\end{equation}
+
+Where:
+
+\({\dot Q_{{\rm{Refrigeration}}}}\) ~ = output variable ``Refrigeration Secondary Loop Load Heat Transfer Rate''
+
+\({\dot Q_{{\rm{TotalSecondary}}}}\) ~ = Total load the secondary loop transfers to the primary system, output variable ``Refrigeration Secondary Loop Total Heat Transfer Rate {[}W{]}''
+
+\({\dot Q_{{\rm{Pump}}}}\) ~ = Pump power, function of Flow\(_{Needed}\), output variable ``Refrigeration Secondary Loop Pump Electric Power {[}W{]}''
+
+Flow\(_{Needed}\) = Flow rate needed to meet the loop refrigeration load, , output variable ``Refrigeration Secondary Loop Volume Flow Rate {[}m3/{]}s''
+
+The needed flow rate is used to determine the number of pumps required and the total pumping power, which produces a new estimate for the total load. A few iterations converge upon the final secondary loop load for each time step.~ The total load on the heat exchanger is therefore the sum of the refrigeration loads, any pipe heat gains, and the portion of the pump power that is absorbed by the circulating fluid.
+
+\subsection{\texorpdfstring{Transcritical CO\(_{2}\) Refrigeration System}{Transcritical CO\_\{2\} Refrigeration System}}\label{transcritical-coux5f2-refrigeration-system}
+
+The Refrigeration:TranscriticalSystem object allows users to model detailed transcritical carbon dioxide (CO\(_{2}\)) booster refrigeration systems used in supermarkets.~ The object allows for modeling either a single stage system with medium-temperature loads or a two stage system with both medium- and low-temperature loads.
+
+The input objects required to model a detailed transcritical CO\(_{2}\) refrigeration system include the following:
+
+n~One Refrigeration:TranscriticalSystem object,
+
+n~At least one refrigeration load object which may include any combination of the following:
+
+n~Refrigeration:Case,
+
+n~Refrigeration:WalkIn,
+
+n~Refrigeration:CaseAndWalkInList (may include both cases and/or walk-in cooler names),
+
+n~At least one Refrigeration:Compressor object (multiple compressors are entered using a Refrigeration:CompressorList),
+
+n~One Refrigeration:GasCooler:AirCooled object,
+
+Output variables are available to describe the total heat exchange between all the refrigeration objects and the zones containing these objects.
+
+At least one refrigeration load object must be defined which may be one of two types of loads, including a refrigerated display case and a walk-in cooler, (Ref. Refrigeration:Case, and Refrigeration:WalkIn).~ If multiple loads are served by the same system, the user should use the refrigerated case and walk-in list object available to assign all cases and walk-ins cooled directly by this system (Ref. Refrigeration:CaseAndWalkInList).
+
+The name of at least one compressor must be defined and a list object is available if the system is served by more than one compressor (Ref. Refrigeration:Compressor and Refrigeration:CompressorList).
+
+Heat is rejected to the outdoors via an air-cooled gas cooler (Ref. Refrigeration:GasCooler:AirCooled).
+
+The Refrigeration:TranscriticalSystem object coordinates the energy flows between the other refrigeration objects and is used to set system parameters.
+
+The inputs for the refrigeration system object, in addition to the names of the other refrigeration objects described above, include a name for this system, the minimum condensing temperature, and the refrigeration system working fluid.~ Optional input fields are also provided for users seeking to keep track of refrigerant inventory and suction pipe heat gains.
+
+\subsubsection{\texorpdfstring{Transcritical CO\(_{2}\) Refrigeration Cycles}{Transcritical CO\_\{2\} Refrigeration Cycles}}\label{transcritical-coux5f2-refrigeration-cycles}
+
+Transcritical CO\(_{2}\) refrigeration cycles are characterized by a subcritical evaporation process and a supercritical ``gas cooling'' process.~ In the subcritical evaporation process which occurs in the evaporator, the CO\(_{2}\) changes phase from a liquid and vapor mixture to a superheated vapor.~ In doing so, the CO\(_{2}\) absorbs heat, thereby creating the cooling effect.~ This process is similar to the evaporation process in a standard vapor-compression refrigeration cycle.
+
+After the CO\(_{2}\) exits the evaporator and is compressed into the supercritical region, the CO\(_{2}\) gas is cooled.~ This gas cooling process differs from the condensation process which occurs in the standard vapor-compression refrigeration system.~ In the standard refrigeration cycle, the refrigerant vapor is first desuperheated and then condensed to a liquid in the condenser.~ In the transcritical CO\(_{2}\) cycle, a ``gas cooler'' rather than a condenser is used to cool the supercritical CO\(_{2}\) from the compressor discharge temperature to the expansion device inlet temperature.~ No condensation occurs in this process.~ Rather, the temperature and density of the CO\(_{2}\) continuously changes from that at the compressor discharge to that at the expansion device inlet.
+
+EnergyPlus is capable of modeling the transcritical booster refrigeration cycle. Figure~\ref{fig:schematic-of-the-transcritical-co_2-booster} shows a schematic of the booster cycle while Figure~\ref{fig:pressure-enthalpy-p-h-diagram-for} shows the corresponding pressure-enthalpy (\emph{p-H}) diagram of the booster cycle.
+
+\begin{figure}[hbtp] % fig 289
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6337.png}
+\caption{Schematic of the Transcritical CO\$\_\{2\}\$ Booster Refrigeration Cycle. \protect \label{fig:schematic-of-the-transcritical-co_2-booster}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 290
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6338.png}
+\caption{Pressure-Enthalpy (*p-H*) Diagram for the Transcritical CO\$\_\{2\}\$ Booster Refrigeration Cycle. \protect \label{fig:pressure-enthalpy-p-h-diagram-for}}
+\end{figure}
+
+Carbon dioxide exits the gas cooler at Location~1 and passes through the suction line heat exchanger, exiting at Location~2, during which the refrigerant is cooled by the suction gas.~ An intermediate expansion occurs between Locations~2 and~3, and saturated CO\(_{2}\) enters the receiver.~ Saturated liquid CO\(_{2}\) exits the receiver at Location~6, which is then expanded and fed to the medium-temperature loads (between Locations~7 and~8) and the low-temperature loads (between Locations~9 and~10).~ Saturated vapor CO\(_{2}\) exits the receiver bypass at Location~4 and is expanded to the medium-temperature pressure level at Location~5.~ Carbon dioxide vapor exiting the low temperature loads is compressed to the medium-temperature pressure level (Location~10 to 11).~ The CO\(_{2}\) from the discharge of the low pressure compressors, the outlet of the medium-temperature loads and the outlet of the receiver bypass are then combined at Location~13.~ The CO\(_{2}\) suction gas then passes through the suction line heat exchanger where the refrigerant is heated, exiting at Location~14.~ The carbon dioxide is finally compressed to the gas cooler pressure level at Location~15 and heat is rejected to the surroundings in the gas cooler between Locations~15 and~1.
+
+\subsubsection{\texorpdfstring{CO\(_{2}\) Compressor Performance Modeling}{CO\_\{2\} Compressor Performance Modeling}}\label{coux5f2-compressor-performance-modeling}
+
+To model the performance of the CO\(_{2}\) compressors during subcritical and transcritical operation, cubic polynomials are used to curve fit manufacturers' performance data.~ This technique is similar to that described in AHRI Standard 540 (AHRI 2004).~ For subcritical operation, the power consumption and cooling capacity of a CO\(_{2}\) compressor is a function of the saturated suction temperature, \emph{t\(_{ss}\)} (°C), and the saturated discharge temperature, \emph{t\(_{sd}\)} (°C), as follows:
+
+\begin{equation}
+z = {C_1} + {C_2}{t_{ss}} + {C_3}{t_{sd}} + {C_4}t_{ss}^2 + {C_5}{t_{ss}}{t_{sd}} + {C_6}t_{sd}^2 + {C_7}t_{ss}^3 + {C_8}t_{ss}^2{t_{sd}} + {C_9}{t_{ss}}t_{sd}^2 + {C_{10}}t_{sd}^3
+\end{equation}
+
+where \emph{z} is either power consumption (W) or cooling capacity (W) and \emph{C\(_{x}\)} are the corresponding correlation coefficients.
+
+For transcritical operation, the power consumption (in Watts) of a CO\(_{2}\) compressor, \emph{W}, is a function of the saturated suction temperature and the gas cooler pressure, \emph{p\(_{gc}\)} (Pa), as follows (Ge and Tassou 2011):
+
+\begin{equation}
+W = {C_1} + {C_2}{t_{ss}} + {C_3}{p_{gc}} + {C_4}t_{ss}^2 + {C_5}{t_{ss}}{p_{gc}} + {C_6}p_{gc}^2 + {C_7}t_{ss}^3 + {C_8}t_{ss}^2{p_{gc}} + {C_9}{t_{ss}}p_{gc}^2 + {C_{10}}p_{gc}^3
+\end{equation}
+
+The cooling capacity (in Watts) of a transcritical CO\(_{2}\) compressor, \emph{Q}, is a function of the saturated suction temperature and the gas cooler outlet enthalpy, \emph{h\(_{go}\)} (J/kg), as follows (Ge and Tassou 2011):
+
+\begin{equation}
+Q = {C_1} + {C_2}{t_{ss}} + {C_3}{h_{go}} + {C_4}t_{ss}^2 + {C_5}{t_{ss}}{h_{go}} + {C_6}h_{go}^2 + {C_7}t_{ss}^3 + {C_8}t_{ss}^2{h_{go}} + {C_9}{t_{ss}}h_{go}^2 + {C_{10}}h_{go}^3
+\end{equation}
+
+The correlation coefficients, \emph{C\(_{x}\)}, are obtained either directly from CO\(_{2}\) compressor manufacturers or from cubic curve fits performed on their published CO\(_{2}\) compressor performance data.~ For convenience, correlation coefficients for CO\(_{2}\) compressors from several manufacturers have been included in the EnergyPlus refrigeration compressor coefficient database.
+
+The rated values for the cooling capacity and power consumption from the manufacturer include a specified amount of subcooling before the thermal expansion valve and a certain amount of superheat in the suction gas.~ Adjustments must be made to these rated values to reflect the actual subcooling and superheat conditions.~ Actual subcooling is determined by the condenser's rated subcooling and by the subcooling provided by optional subcoolers. The actual superheat is determined by the refrigerated case superheat (usually set to ensure that there is no liquid in the suction lines leading to the compressors), set here at 10°C, and the effect from any optional subcoolers.~ See the section, ``Detailed Refrigeration Systems'', for a description of the compressor corrections.
+
+Once the corrected capacity is calculated for each compressor, the compressors are dispatched one at a time until the system load is met.~ The last compressor dispatched is assumed to run at full load for the fraction of the time step necessary to meet the load.~ That is, the model neglects compressor cycling losses at part-load conditions.~ If the capacity available from all the compressors is less than the sum of the case loads for that time period, the unmet load is accumulated to be met in succeeding time steps.~ If this accumulated unmet load becomes too great, a warning message is generated.
+
+\subsubsection{Gas Cooler Performance}\label{gas-cooler-performance}
+
+Only one gas cooler is allowed per transcritical refrigeration system. However, multiple refrigeration systems can reject heat through the same gas cooler.~ Currently, only air-cooled gas coolers are modeled.~ The gas cooler performance is modeled to determine the gas cooler pressure, gas cooler outlet temperature and outlet enthalpy of the refrigerant, and the auxiliary power consumption for the fans.
+
+\paragraph{\texorpdfstring{Optimal Gas Cooler Pressure for Transcritical CO\(_{2}\) Cycles}{Optimal Gas Cooler Pressure for Transcritical CO\_\{2\} Cycles}}\label{optimal-gas-cooler-pressure-for-transcritical-coux5f2-cycles}
+
+When the compressor discharge conditions are such that the CO\(_{2}\) is in the supercritical region, then the high-side operating pressure is independent of the gas cooler exit temperature (Sawalha 2008).~ Thus, for a given gas cooler exit temperature, there is an optimum pressure to achieve the maximum coefficient of performance (COP).~ Figure~\ref{fig:cop-of-co_2-transcritical-cycle-vs.-discharge} illustrates the variation in COP of a transcritical CO\(_{2}\) cycle with discharge pressure at different gas cooler exit temperatures.
+
+\begin{figure}[hbtp] % fig 291
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6342.png}
+\caption{COP of CO\(_2\) Transcritical Cycle vs. Discharge Pressure at Different Gas Cooler Exit Temperatures (Sawalha 2008). \protect \label{fig:cop-of-co_2-transcritical-cycle-vs.-discharge}}
+\end{figure}
+
+Several researchers have developed correlations to determine the optimum gas cooler pressure in CO\(_{2}\) refrigeration systems (Chen and Gu 2005; Ge and Tassou 2011; Kauf 1998; Liao and Zhao 2000; Sawalha 2008).~ Using a similar curve-fitting procedure, the following optimum gas cooler pressure correlations are used in EnergyPlus:
+
+\begin{equation}
+  p_{gc} = \left\{
+             \begin{array}{cl}
+               7.5 \times 10^6                                & if T_{amb} <    27^{\circ}C \\
+               2.3083 \times 10^5 T_{amb} + 1.190 \times 10^6 & if T_{amb} \geq 27^{\circ}C
+             \end{array}
+           \right.
+\end{equation}
+
+where \emph{p\(_{gc}\)} is the optimum gas cooler pressure (Pa) and \emph{T\(_{amb}\)} (°C) is the ambient temperature surrounding the gas cooler.~ The corresponding gas cooler exit temperature, \emph{T\(_{gco}\)} (°C), is determined as follows:
+
+\begin{equation}
+{T_{gco}} = {T_{amb}} + \Delta {T_{approach}}
+\end{equation}
+
+where Δ\emph{T\(_{approach}\)} is the approach temperature of the gas cooler, defined as the difference between the gas cooler exit temperature and the entering ambient air temperature.
+
+During transcritical operation, the gas cooler outlet pressure is not allowed to fall below 7.5~×~10\(^{6}\)~Pa to ensure proper operation.
+
+\paragraph{Condensing Temperature and Pressure for Subcritical Operation}\label{condensing-temperature-and-pressure-for-subcritical-operation}
+
+During subcritical operation, the gas cooler behaves as a condenser and the condensing pressure is allowed to float with the ambient conditions.~ The condensing temperature, \emph{T\(_{cond}\)} (°C), is determined according to the following:
+
+\begin{equation}
+  T_{cond} = \left\{
+               \begin{array}{cl}
+                 T_{cond,min}                           & if T_{amb} \le T_{cond,min} - \Delta T \\
+                 T_{amb} + \Delta T                     & if T_{cond,min} - \Delta T < T_{amb} \le T_{trans} - \Delta T \\
+                 T_{trans}                              & if T_{trans} - \Delta T < T_{amb} < T_{trans} \\
+                 T_{sat,P = 7.2MPa}                     & if T_{trans} \le {T_{amb}} < 30.978 
+               \end{array}
+             \right.
+\end{equation}
+
+where \emph{T\(_{amb}\)} is the ambient temperature (°C), Δ\emph{T} is the temperature difference between the condensing temperature and the ambient temperature (°C), \emph{T\(_{cond}\)}\(_{,*min*}\) is the minimum allowable condensing temperature (°C), and \emph{T\(_{trans}\)} is the ambient air transition temperature between subcritical and transcritical operation (°C).~ The condensing pressure, \emph{P\(_{cond}\)} (Pa), is determined as the saturation pressure corresponding to the condensing temperature.
+
+\paragraph{Gas Cooler Fan Energy Use}\label{gas-cooler-fan-energy-use}
+
+Gas cooler fan power for air-cooled gas coolers is determined by the type of fan control, which can either be fixed, variable speed, or two-speed.~ For all three fan control types, the gas cooler fan energy is calculated in the same fashion as that for air-cooled condensers, as described in the section, ``Detailed Refrigeration Systems''.
+
+\subsubsection{Suction Line Heat Exchanger}\label{suction-line-heat-exchanger}
+
+The performance of the transcritical CO\(_{2}\) booster system can be enhanced by using a suction line heat exchanger.~ As shown in Figure~\ref{fig:schematic-of-the-transcritical-co_2-booster}, the suction gas entering the heat exchanger at location 13 is used to cool the refrigerant after it leaves the gas cooler at location 1.~ The performance of this heat exchanger is modeled with the heat exchanger effectiveness, ε:
+
+\begin{equation}
+\varepsilon  = \frac{{{h_{14}} - {h_{13}}}}{{{h_{{T_1},{P_{13}}}} - {h_{13}}}} = \frac{{{h_1} - {h_2}}}{{{h_{{T_1},{P_{13}}}} - {h_{13}}}}
+\end{equation}
+
+where \emph{h}\(_{1}\), \emph{h}\(_{2}\), \emph{h}\(_{13}\), and \emph{h}\(_{14}\) are the enthalpies of carbon dioxide at the respective locations in the refrigeration cycle, as shown in Figure~\ref{fig:schematic-of-the-transcritical-co_2-booster} and Figure~\ref{fig:pressure-enthalpy-p-h-diagram-for}, and \({h_{{T_1},{P_{13}}}}\) ~is the enthalpy of carbon dioxide evaluated at temperature \emph{T}\(_{1}\) and pressure \emph{P}\(_{13}\).
+
+In EnergyPlus, the value of the suction line heat exchanger effectiveness, ε, is specified by the user as an input, and the enthalpies at the exit of the heat exchanger, \emph{h}\(_{2}\) and \emph{h}\(_{14}\), are determined from the definition of heat exchanger effectiveness given above.~ In EnergyPlus, the default value of heat exchanger effectiveness is 0.4.
+
+\textbf{Thermodynamic Properties of CO\(_{2}\)}
+
+Modeling of transcritical CO\(_{2}\) booster refrigeration cycles requires the thermodynamic properties of CO\(_{2}\) in the saturated (liquid and vapor), superheated and supercritical regions.~ The refrigerant properties database within EnergyPlus includes saturated, superheated and supercritical thermodynamic data for CO\(_{2}\), including temperature, pressure, density, enthalpy and specific heat.
+
+\subsection{References}\label{references-040}
+
+AHRI, 2001. Standard 410, Forced-Circulation Air-Cooling and Air-Heating Coils, Section 6.2.1, Air-Conditioning Heating \& Refrigeration Institute
+
+ARI. 2003. Standard for Remote Mechanical-Draft Evaporatively-Cooled Refrigerant Condensers, Standard 490, Air-Conditioning \& Refrigeration Institute, Arlington, VA
+
+ARI. 2004. Standard for Performance Rating of Positive Displacement Refrigerant Compressors and Compressor Units, Standard 540, Air-Conditioning \& Refrigeration Institute, Arlington, VA
+
+ARI. 2005. Standard for Performance Rating of Remote Mechanical-Draft Air-Cooled Refrigerant Condensers, Standard 460, Air-Conditioning \& Refrigeration Institute, Arlington, VA
+
+ARI. 2007. Standard for Performance Rating of Water-Cooled Refrigerant Condensers, Remote Type, Standard 450, Air-Conditioning \& Refrigeration Institute, Arlington, VA
+
+ASHRAE. 2002. \emph{Refrigeration Handbook}, Chapter 47. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2004. \emph{HVAC Systems and Equipment Handbook}, Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2006a. \emph{Refrigeration Handbook}, Chapter 2. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2006b. \emph{Refrigeration Handbook}, Chapter 44. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2006c. \emph{Refrigeration Handbook}, Chapter 4. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2006d. \emph{Refrigeration Handbook}, Chapter 13. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2009. \emph{Fundamentals Handbook}, Chapter 1. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2009b. \emph{Fundamentals Handbook}, Chapter 2. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+B.A.C. 2007. Baltimore AirCoil Company Product and Application Handbook, Volume II, Baltimore, MD
+
+Baek, J.S., Groll, E.A., and Lawless, P.B. 2005. Theoretical Perfromance of Transcritical Carbon Dioxide Cycle with Two-Stage Compression and Intercooling. \emph{Proceedings of the Institution of Mechanical Engineers, Part E: Journal of Process Mechanical Engineering} 219, 187-195.
+
+Baxter, V. D., Mei, V.C. 2002.Warm Liquid Defrosting Technology For Supermarket Display Cases, P.S. Hrnjak, Ed., International Conference New Technologies in Commercial Refrigeration, University of Illinois at Urbana-Champaign, Urbana, IL, July 22-23, 2002
+
+Chen, Y., and Gu, J. 2005. The Optimum High Pressure for CO\(_{2}\) Transcritical Refrigeration Systems with Internal Heat Exchangers. \emph{International Journal of Refrigeration} 28(8), 1238-1249.
+
+Evans, J. 2008. Chapter 15, Minimising Energy Consumption Associated with Chilling, Refrigerated Storage and Cooling Systems in the Food Industry. In \emph{Handbook of Water and Energy Management in Food Processing}. Cambridge:~ Woodhead Publishing Limited.
+
+Faramarzi, R. T., and Walker, D. H. 2004. Investigation of Secondary Lop Supermarket Refrigeration Systems, prepared for California Energy Commission Public Interest Energy Research Program, prepared by Southern California Edison and Foster-Miller, PIER 500-04-013
+
+Ge, Y., and Tassou, S. 2011. Performance Evaluation and Optimal Design of Supermarket Refrigeration Systems with Supermarket Model ``Supersim'', Part I: Model Description and Validation. \emph{International Journal of Refrigeration} 34(2), 527-539.
+
+Gosney, W.B., Olama, G.A.-L. 1975. Heat and Enthalpy Gains through Cold Room Doorways,~ Proceedings of the Institute of Refrigeration, vol.~72, pp 31-41
+
+Henderson, H.I. and Khattar, M. 1999. Measured Impacts of Supermarket Humidity Level on Defrost Performance and Refrigerating System Energy Use. \emph{ASHRAE Transactions} 105(1), 508-520. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Hinde, D., Zha, S., and Lan, L. 2009. Carbon Dioxide in North American Supermarkets, ASHRAE Journal, Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.,February 2009
+
+Howell, R.H. 1993. Effects of Store Relative Humidity on Refrigerated Display Case Performance. \emph{ASHRAE Transactions} 99(1), 667-678. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Howell, R.H. 1993. Calculation of Humidity Effects on Energy Requirements of Refrigerated Display Cases. \emph{ASHRAE Transactions} 99(1), 679-693. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+IEA Heat Pump Centre. 2003. \emph{Advanced Supermarket Refrigeration/Heat Recovery Systems Vol. 1 - Executive Summary}, Report HPP-AN26-2, April.
+
+ITT. 2009. Goulds Pumps Industrial~ Products Moter Terms
+
+Kauf, F. 1998. Determination of the Optimum High Pressure for Transcritical CO\(_{2}\)-Refrigeration Cycles. \emph{International Journal of Thermal Sciences} 38(4), 325-330.
+
+Kays, W.M., A.L. London, 1964, compact Heat Exchangers, Second Edition, Chap. 2, pp 15-24, McGraw-Hill Book Company
+
+Kazachki, G. S., and Hinde, D. K. 2006, Secondary Cooplant Systems for Supermarkets, ASHRAE Journal, Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc., September 2006
+
+Lawrence Berkeley Laboratory and Resource Dynamics, Improving Fan Systrem Performance, A Sourcebook for Industry, DOE/GO-102003-1294, April 2003
+
+Lee, T-S., Liu, C-H., and Chen, T-W. 2006. Thermodynamic Analysis of Optimal Condensing Temperature of Cascade-Condenser in CO\(_{2}\)/NH\(_{3}\) Cascade Refrigeration Systems, International Journal of Refrigeration 29 (2006) 1100-1108, Elsevier Ltd.
+
+Liao, S., and Zhao, T. J. 2000. A Correlation of Optimal Heat Rejection Pressures in Transcritical Carbon Dioxide Cycles. \emph{Applied Thermal Engineering} 20(9), 831-841.
+
+Manske, K.A., 2000. Performance Optimization of Industrial Refrigeration Systems, M.S.Thesis Mechanical Engineering, Solar Energy Laboratory, University of Wisconsin-Madison.
+
+Minea, V. 2007. Supermarket Refrigeration System with Completely Secondary Loops, ASHRAE Journal, Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc., ~September 2007
+
+Mitchell, J.W., et al. 1992.Analysis of Supermarket Dehumidification Alternatives. Final Report to Electric Power Research Institute, Report TR-100352, November.
+
+NASA. 1976. U. S. Standard Atmosphere, NASA-TM-74335, National Oceanic and Atmosperic Administration , National Aeronautics and Space Administration
+
+Nelson, B. I., 2010, Refrigeration Air Cooler Rating Methods, ASHRAE Journal, American Society of Heating, Refrigeration and Air-Conditioning Engineers, Inc., August
+
+Sawalha, S. 2008. Theoretical Evaluation of Trans-Critical CO\(_{2}\) Systems in Supermarket Refrigeration. Part I: Modeling, Simulation and Optimization of Two System Solutions. \emph{International Journal of Refrigeration} 31, 516-524.
+
+Terrell, W.J.Jr., Mao, Y., Hrnjak, P.S. 1999. Evaluation of Secondary Fluids for Use in Low-Temperature Supermarket Applications, ACRC CR-15, Air Conditioning and Refrigeration Center, University of Illinois, Urbana, IL, April 1999.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/setpoint-managers.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/setpoint-managers.tex
new file mode 100644
index 00000000000..8fa417ddf28
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/setpoint-managers.tex
@@ -0,0 +1,771 @@
+\section{Setpoint Managers }\label{setpoint-managers}
+
+\subsection{Overview}\label{overview-024}
+
+Setpoint Managers are one of the high-level control constructs in EnergyPlus. A Setpoint Manager is able to access data from any of the HVAC system nodes and use this data to calculate a setpoint (usually a temperature setpoint) for one or more other HVAC system nodes. Setpoints are then used by Controllers as a goal for their control actions.
+
+Setpoint managers are executed at the start of each HVAC time step, and they reside outside the HVAC system iteration loops. Thus, the Setpoint Managers are executed once per HVAC time step, and they use previous time step information (except for zone load) to calculate their setpoints.
+
+All temperatures in the following descriptions are in degrees C, loads are in Watts, mass flow rates are in kg/s.
+
+\subsection{Scheduled}\label{scheduled}
+
+The input object SetpointManager:Scheduled provides the simplest setpoint manager that allows the user to specify a seasonal (or other) scheduled reset, for example, of the supply air temperature setpoint.
+
+\begin{equation}
+{T_{set}} = {T_{sched}}
+\end{equation}
+
+where \({T_{set}}\) is the supply air temperature setpoint and \({T_{sched}}\) is the current value (°C) from the user input temperature schedule. In this case, \({T_{set}}\) will be applied to the node or nodes specified in the input object SetpointManager:Scheduled.~ There are a number of other types of setpoints that can be set, by choosing different control variables in the object, including:
+
+1)~~~Maximum temperature of fluid at node (°C)
+
+2)~~~Minimum temperature of fluid at node (°C)
+
+3)~~~Humidity ratio of fluid at node (kg water/ kg dry air)
+
+4)~~~Maximum humidity ratio of fluid at node (kg water/ kg dry air)
+
+5)~~~Minimum humidity ratio of fluid at node (kg water/ kg dry air)
+
+6)~~~Mass flow rate of fluid at node (kg/s)
+
+7)~~~Maximum mass flow rate of fluid at node (kg/s)
+
+8)~~~Minimum mass flow rate of fluid at node (kg/s)
+
+\subsection{Outdoor Air Reset}\label{outdoor-air-reset}
+
+The input object SetpointManager:OutdoorAirReset provides a setpoint manager that implements an outdoor air reset strategy for the supply air temperature. The user defines a reset rule for this strategy by specifying two setpoint temperatures at two outside drybulb temperatures. Generally the lower setpoint temperature is matched with the higher drybulb temperature and the higher setpoint temperature with the lower drybulb temperature. The user can specify two reset rules and schedule their usage. A schedule value of 1 indicates use of the 1st rule; 2 indicates use of the 2nd.
+
+IF \emph{SchedVal = 2}
+
+\begin{equation}
+{T_{out,low}} = {T_{2,out,low}}
+\end{equation}
+
+\begin{equation}
+{T_{out,high}} = {T_{2,out,high}}
+\end{equation}
+
+\begin{equation}
+{T_{set,atOAlow}} = {T_{2,set,atOAlow}}
+\end{equation}
+
+\begin{equation}
+{T_{set,atOAhigh}} = {T_{2,set,atOAhigh}}
+\end{equation}
+
+otherwise
+
+\begin{equation}
+{T_{out,low}} = {T_{1,out,low}}
+\end{equation}
+
+\begin{equation}
+{T_{out,high}} = {T_{1,out,high}}
+\end{equation}
+
+\begin{equation}
+{T_{set,atOAlow}} = {T_{1,set,atOAlow}}
+\end{equation}
+
+\({T_{set,atOAhigh}} = {T_{1,set,atOAhigh}}\) .
+
+If \({T_{out,low}} < {T_{out,high}}\) and \({T_{set,atOAlow}} > {T_{set,atOAhigh}}\) ~then
+
+~~~~~ If \({T_{out}} \le {T_{out,low}}\) ~then
+
+~~~~~ \({T_{set}} = {T_{out,low}}\)
+
+~~~~~ if \({T_{out}} \ge {T_{out,high}}\) ~then
+
+~~~~~ \({T_{set}} = {T_{out,high}}\)
+
+~~~~~ otherwise
+
+~~~~~ \({T_{set}} = {T_{set,atOAlow}} - (({T_{out}} - {T_{out,low}})/({T_{out,high}} - {T_{out,low}}))\cdot ({T_{set,atOAlow}} - {T_{set,atOAhigh}})\)
+
+otherwise
+
+~~~~~ \({T_{set}} = 0.5({T_{set,atOAlow}} + {T_{set,atOAhigh)}}\) .
+
+\emph{\({T_{set}}\)}will be applied to the node or nodes specified in the \emph{SetpointManager:OutdoorAirReset} object input.
+
+\subsection{Single Zone Reheat Heating and Cooling}\label{single-zone-reheat-heating-and-cooling}
+
+The input object SetpointManager:SingleZone:Reheat provides a setpoint manager that is used to implement a variable supply air setpoint temperature in which the setpoint is varied~ each timestep to meet the heating or cooling load in a control zone. The manager operates in the following manner.
+
+\begin{equation}
+{T_{set}} = {T_z} + {\dot Q_z}/({C_{p,air}}\cdot {\dot m_z})
+\end{equation}
+
+where \({T_z}\) is the control zone temperature, \({\dot Q_z}\) is the zone load (greater than zero for heating, less than zero for cooling), \({\dot m_z}\) is the zone supply air mass flow rate, and \({C_{p,air}}\) is the specific heat of air. If \({\dot m_z}\) is very small (\(\le .001\) ~kg/s) \({T_{set}}\) ~is set equal to \({T_{set,min}}\) ~if the control zone has a cooling load and to \({T_{set,max}}\) if the control zone has a heating load. \({T_{set,min}}\) ~is the user specified minimum setpoint and \({T_{set,max}}\) ~is the user specified maximum setpoint. \({T_{set}}\) will be applied to the node or nodes specified in the SetpointManager:SingleZone:Reheat object input.
+
+\subsection{Single Zone Heating Only}\label{single-zone-heating-only}
+
+The input object SetpointManager:SingleZone:Heating provides a model that detects the control zone load to meet the current heating setpoint (Report Variable ``Zone Predicted Sensible Load to Heating Setpoint Heat Transfer Rate {[}W{]}'', zone inlet node flow rate, and zone node temperature, and calculates a setpoint temperature for the supply air that will satisfy the zone heating load for the control zone.~ ``Zone Predicted Sensible Load to Heating Setpoint Heat Transfer Rate {[}W{]}'' \textgreater{} 0 indicates a heating load.~ The following rules are applied:
+
+·~~~~~~~~If there is no zone heating load, then the setpoint is set at the specified minimum supply air temperature.
+
+·~~~~~~~~If there is a zone heating load~ and the zone supply mass flow rate is less than 0.001 kg/s, then the setpoint is set at the specified maximum supply air temperature.
+
+·~~~~~~~~If there is a zone heating load~ and the zone supply mass flow rate is greater than 0.001 kg/s, then the setpoint is set calculated as follows:
+
+\emph{SetPoint = ZoneTemp + ZoneLoadtoHeatSP/(CpAir*ZoneMassFlow)}
+
+where:
+
+\emph{SetPoint =} Setpoint temperature applied to the specified setpoint node(s)
+
+\emph{ZoneTemp =} Current zone temperature
+
+\emph{ZoneLoadtoHeatSP =} Zone heating load (Report Variable " Zone Predicted Sensible Load to Heating Setpoint Heat Transfer Rate {[}W{]}``)
+
+\emph{CpAir =} Specific heat of zone supply air
+
+\emph{ZoneMassFlow =} Zone supply air mass flow rate
+
+\subsection{Single Zone Cooling Only}\label{single-zone-cooling-only}
+
+The input object SetpointManager:SingleZone:Cooling provides a model that detects the control zone load to meet the current cooling setpoint (Report Variable ``Zone Predicted Sensible Load to Cooling Setpoint Heat Transfer Rate {[}W{]}'', zone inlet node flow rate, and zone node temperature, and calculates a setpoint temperature for the supply air that will satisfy the zone cooling load for the control zone.~ ``Zone Predicted Sensible Load to Cooling Setpoint Heat Transfer Rate {[}W{]}'' \textless{} 0 indicates a cooling load.~ The following rules are applied:
+
+·~~~~~~~~If there is no zone cooling load, then the setpoint is set at the specified maximum supply air temperature.
+
+·~~~~~~~~If there is a zone cooling load~ and the zone supply mass flow rate is less than 0.001 kg/s, then the setpoint is set at the specified minimum supply air temperature.
+
+·~~~~~~~~If there is a zone cooling load~ and the zone supply mass flow rate is greater than 0.001 kg/s, then the setpoint is set calculated as follows:
+
+\emph{SetPoint = ZoneTemp + ZoneLoadtoCoolSP/(CpAir*ZoneMassFlow)}
+
+where:
+
+\emph{SetPoint} = Setpoint temperature applied to the specified setpoint node(s)
+
+\emph{ZoneTemp} = Current zone temeprature
+
+\emph{ZoneLoadtoCoolSP} = Zone cooling load (Report Variable ``Zone Predicted Sensible Load to Cooling Setpoint Heat Transfer Rate {[}W{]}'')
+
+\emph{CpAir} = Specific heat of zone supply air
+
+\emph{ZoneMassFlow} = Zone supply air mass flow rate
+
+\subsection{Single Zone Minimum Humidity}\label{single-zone-minimum-humidity}
+
+The input object SetpointManager:SingleZone:Humidity:Minimum provides a model where the zone moisture load from ZoneTempPredictorCorrector (via DataZoneEnergyDemands) is used to calculate the minimum/maximum supply air humidity ratio needed to meet minimum/maximum zone relative humidity requirement.~ For the Max setpoint manager is currently used in Controller:WaterCoil, when the control variable ``TemperatureAndHumidityRatio''.~ A negative MoistureLoad means a dehumidification load for the coil controller.~ This could be used for any system.
+
+\subsection{Single Zone Maximum Humidity}\label{single-zone-maximum-humidity}
+
+The input object SetpointManager:SingleZone:Humidity:Maximum provides a setpoint manager that allows the control of high air humidity levels in a single zone. This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level in a single control zone and uses air/moisture mass balances to calculate the supply air humidity ratio needed to maintain the zone relative humidity at or below a given setpoint. The calculated supply air humidity ratio is then entered as a setpoint on a designated supply air stream node. A dehumidification component placed upstream of this node can then use the humidity ratio setpoint to control its moisture removal rate (e.g.~desiccant dehumidifiers). In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determine the minimum supply air temperature required to meet both the temperature (sensible) and humidity (latent) load in the control zone. (Ref: Controller:WaterCoil).
+
+\subsubsection{Model Description}\label{model-description-014}
+
+The user must input the required information according to the IO Reference Manual (ref: SetpointManager:SingleZone:Humidity:Maximum). Specific inputs include an object name, control variable (HumidityRatio), name of the schedule defining the maximum relative humidity for the control zone, setpoint node name or list, and the zone air node name associated with the control zone (ref: ZoneHVAC:EquipmentConnections). The schedule name must refer to a valid schedule type (range 0-1) and contain values of fractional relative humidity.
+
+This setpoint manager first converts the desired relative humidity setpoint for the control zone to humidity ratio based on the control zone dry-bulb temperature, the scheduled maximum relative humidity setpoint and outdoor barometric pressure.
+
+\begin{equation}
+{\omega_{sp}} = \,{\rm{PsyWFnTdbRhPb}}\left( {{T_{db}},R{H_{sp}},P} \right)
+\end{equation}
+
+where:
+
+\({\omega_{sp}}\) ~ = humidity ratio setpoint, kg H\(_{2}\)O/kg air
+
+PsyWFnTdbRHPb = EnergyPlus psychrometric function, returns humidity ratio as a function of dry-bulb temperature, relative humidity, and barometric pressure
+
+\({T_{db}}\) = dry-bulb temperature in the control zone, °C
+
+\(R{H_{sp}}\) = maximum relative humidity setpoint, fraction
+
+\(P\) ~ = outdoor barometric pressure, Pa
+
+The model then calculates the supply air humidity ratio required to reduce the control zone relative humidity to the desired level. Using the humidity ratio setpoint (\({\omega_{sp}}\) ) calculated above,
+
+\begin{equation}
+{\omega_{sa}} = \,{\omega_{sp}} + \frac{{{{\mathop Q\limits^ \bullet  }_l}}}{{\mathop m\limits^ \bullet  }}
+\end{equation}
+
+where:
+
+\({\omega_{sa}}\) ~ = maximum supply air humidity ratio setpoint, kg H\(_{2}\)O/kg air
+
+\(\mathop {{Q_l}}\limits^ \bullet\) ~ = control zone latent load, kg H\(_{2}\)O/s (calculated by Zone Control:Humidistat)
+
+\(\mathop m\limits^ \bullet\) ~ = control zone mass flow rate, kg/s
+
+All setpoint managers are executed at the beginning of the simulation time step. Therefore, the calculated setpoint is based on the resulting control zone air temperature and air mass flow rate for the previous simulation time step.
+
+The maximum supply air humidity ratio setpoint is placed on the node(s) specified in the input for this object (using node property Humidity Ratio Maximum).
+
+\subsection{Mixed Air}\label{mixed-air}
+
+The input object SetpointManager:MixedAir provides a setpoint manager that takes an already established setpoint (usually the supply air outlet node setpoint temperature), subtracts the supply fan heat gain, and applies the result as the setpoint temperature at the mixed air node (or any other node the user specifies).
+
+\begin{equation}
+{T_{set}} = {T_{set,ref}} - ({T_{fan,outlet}} - {T_{fan,inlet}})
+\end{equation}
+
+When inputs of optional fields, Cooling Coil Inlet Node Name, Cooling coil Outlet Node Name, and Minimum Temperature at Cooling Coil Outlet Node, are provided, the setpoint temperature at the mixed air node is given below based on supply fan placement and reference node location:
+
+Blow through placement:
+
+\begin{equation}
+{T_{set}} = max(T_{set,ref}, T_{min}) - ({T_{coil,outlet}} - {T_{coil,inlet}}) - ({T_{fan,outlet}} - {T_{fan,inlet}})
+\end{equation}
+
+Draw through placement:
+
+When the reference node is the cooling coil outlet node:
+
+\begin{equation}
+{T_{set}} = max(T_{set,ref}, T_{min}) - ({T_{coil,outlet}} - {T_{coil,inlet}})
+\end{equation}
+
+When the reference node is the unitary system outlet node:
+
+\begin{equation}
+{T_{set}} = max(T_{set,ref} - ({T_{fan,outlet}} - {T_{fan,inlet}}), T_{min}) - ({T_{coil,outlet}} - {T_{coil,inlet}})
+\end{equation}
+
+\subsection{Outdoor Air Pretreat}\label{outdoor-air-pretreat}
+
+The input object SetpointManager:OutdoorAirPretreat provides a setpoint manager that is meant to be used in conjunction with an OutdoorAir:Mixer. The outdoor air pretreat setpoint manager is used to establish a temperature or humidity ratio setpoint in the outdoor air stream flowing into the outdoor air stream node of an outdoor air mixer. This setpoint manager determines the required setpoint in the outdoor air stream to produce the reference setpoint in the mixed air stream after mixing with return air. For example, if the temperature setpoint at the mixed air node is 15C, the return air temperature is 20C, and the outdoor air flow fraction is 0.5, the outdoor air pretreat setpoint would be set to 10C. This setpoint manager references four user-specified nodes to obtain the following values:
+
+·~~~~~~~~Reference setpoint node -- desired mixed flow condition = RefNodeSetPoint
+
+·~~~~~~~~Mixed air stream node -- mixed air flow rate = MixedOutNodeMassFlowRate
+
+·~~~~~~~~Outdoor air stream node -- outdoor air flow rate = OAInNodeMassFlowRate
+
+·~~~~~~~~Return air stream node -- return air condition = ReturnInValue
+
+The following calculations are used to determine the new setpoint value (SetPoint):
+
+\emph{OAFraction = OAInNodeMassFlowRate / MixedOutNodeMassFlowRate}
+
+\emph{SetPoint = ReturnInValue + (RefNodeSetPoint - ReturnInValue)/OAFraction}
+
+Depending on the specified control variable type, the setpoints and conditions may be humidity ratio (max or min) or temperature.~ Note that zero is not allowed as the computed setpoint humidity ratio, because zero is used as a special value to indicate that no humidification or dehumidification is needed.~ If the reference humidity ratio setpoint value is zero, the zero value will be passed directly to the setpoint Node(s).
+
+\subsection{Warmest Zone Supply Air Reset}\label{warmest-zone-supply-air-reset}
+
+The input object SetpointManager:Warmest provides a setpoint manager that attempts to establish a supply air setpoint that will meet the cooling load of the zone needing the coldest air at the maximum zone supply air flowrate. The algorithm loops over all the zones that the system can cool and calculates
+
+\begin{equation}
+{T_{set,z}} = {T_z} + {\dot Q_z}/({C_{p,air}}\cdot {\dot m_{z,max}})
+\end{equation}
+
+Note that for cooling \({\dot Q_z} < 0.\) The lowest \({T_{set,z}}\) is chosen as \({T_{set}}\) . \({T_{set}}\) is constrained to be less than or equal to the maximum setpoint temperature (user input) and greater than or equal to the minimum setpoint temperature (user input). If the sum of the zone cooling loads is very small, the setpoint temperature is set to the maximum. \({T_{set}}\) will be applied to the node or nodes specified in the SetpointManager:Warmest object input.
+
+\subsection{Coldest Zone Supply Air Reset}\label{coldest-zone-supply-air-reset}
+
+The input object SetpointManager:Coldest provides a setpoint manager that attempts to establish a supply air setpoint that will meet the heating load of the zone needing the warmest air at the maximum zone supply air flowrate. The algorithm loops over all the zones that the system can heat and calculates
+
+\begin{equation}
+{T_{set,z}} = {T_z} + {\dot Q_z}/({C_{p,air}}\cdot {\dot m_{z,max}})
+\end{equation}
+
+Note that for heating \({\dot Q_z} > 0.\) The highest \({T_{set,z}}\) is chosen as \({T_{set}}\) . \({T_{set}}\) is constrained to be less than or equal to the maximum setpoint temperature (user input) and greater than or equal to the minimum setpoint temperature (user input). If the sum of the zone heating loads is very small, the setpoint temperature is set to the minimum. \({T_{set}}\) will be applied to the node or nodes specified in the SetpointManager:Coldest object input.
+
+\subsection{Return Air Bypass Flow}\label{return-air-bypass-flow}
+
+The input object SetpointManager:ReturnAirBypassFlow provides a setpoint manager that sets the air flow rate in a bypass duct such that when the bypassed and non-bypassed air are mixed the resutant air stream will be at the user-specified setpoint temperature.
+
+The user specifies the desired setpoint temperature \emph{T\(_{set}\)} through a input temperature schedule.
+
+This temperature is modified to account for any potential fan heat gain:
+
+\begin{equation}
+{T_{set,mod}} = {T_{set}} - ({T_{loop,out}} - {T_{mixer,out}})
+\end{equation}
+
+Here \({T_{loop,out}}\) is the temperature at the air loop outlet node and \({T_{mixer,out}}\) ~is the temperature at the outlet node of the bypass -- nonbypass air mixer. Depending on the system configuration these may be the same node. Then
+
+\begin{equation}
+{\dot m_{bypass}} = ({\dot m_{tot}}\cdot {T_{set,mod}} - {\dot m_{nonbypass}}\cdot {T_{nonbypass}})/{T_{bypass}}
+\end{equation}
+
+where \({\dot m_{tot}}\) is the total supply air flowrate in kg/s sent to the zones, \({\dot m_{nonbypass}}\) is the nonbypassed air flowrate (the conditioned air), \({T_{nonbypass}}\) is the corresponding temperature just before mixing with the bypassed air, and \({T_{bypass}}\) is the temperature of the bypassed (unconditioned) air. The resulting \({\dot m_{bypass}}\) ~is the mass flow rate setpoint for the bypass air branch.
+
+\subsection{Warmest Temp Flow}\label{warmest-temp-flow}
+
+The input object SetpointManager:WarmestTemperatureFlow provides a setpoint manager that attempts to establish a supply air setpoint that will meet the cooling load of the zone needing the coldest air at the maximum zone supply air flowrate. The supply air temperature setpoint is established by SetpointManager:WarmestTemperatureFlow using one of two strategies: `Temp First' sets the supply air temperature to the highest temperature that will meet the cooling load of the coolest zone at minimum cfm. `Flow First' sets the supply air temperature to the highest temperature that will meet the cooling load of the warmest zone at maximum cfm.~ `Temp First' gives higher priority to reducing fan energy whereas `Flow First' gives higher priority to reducing chiller energy.
+
+The algorithm loops over all the zones that the system can cool and calculates according to strategy:
+
+\textbf{Temp First:}
+
+\begin{equation}
+  T_{set,z} = T_z + \frac{\dot{Q}_z}{C_{p,air} \dot{m}_{z,min}}
+\end{equation}
+
+\textbf{Flow First:}
+
+\begin{equation}
+  T_{set,z} = T_z + \frac{\dot{Q}_z}{C_{p,air} \dot{m}_{z,max}}
+\end{equation}
+
+where \({\dot m_{z,\min }}\) is the minimum air flow rate to the zone produced by reducing the capacity of the supply fan or by reducing the opening of the damper in the terminal box, if present, and~ \({\dot m_{z,\max }}\) ~is the design air flow rate to the zone.
+
+Note that for cooling \({\dot Q_z} < 0.\) ~The lowest \({T_{set,z}}\) is chosen as \({T_{set}}\) . \({T_{set}}\) is constrained to be less than or equal to the maximum setpoint temperature (user input) and greater than or equal to the minimum setpoint temperature (user input). If the unconstrained value of \({T_{set}}\) is less than the minimum setpoint temperature and there are no VAV terminal boxes, the fan capacity is increased so as to meet the zone cooling loads with the constrained value of \({T_{set}}\) :
+
+\begin{equation}
+{\dot m_{fan}} = \sum\limits_z {{{\dot m}_{z,\min }}}  = \sum\limits_z {{{\dot Q}_z}/[{C_{p,air}} \cdot ({T_{set}} - {T_z})]}
+\end{equation}
+
+~This is more likely to occur in the `Temp First' case. If the sum of the zone cooling loads is very small, the setpoint temperature is set to the maximum. \({T_{set}}\) will be applied to the node or nodes specified in the SetpointManager:WarmestTemperatureFlow object input.
+
+\subsection{Multizone Heating Average}\label{multizone-heating-average}
+
+The input object SetpointManager:MultiZone:Heating:Average provides a setpoint manager that attempts to establish a supply air heating setpoint that will meet the heating load of multiple zones served by an HVAC air loop. The algorithm aggregates the predicted heating loads for all controlled zones served by an air loop (i.e., zones that have a thermostat object), and calculates the multizone average supply air heating setpoint temperature as follows:
+
+IF ( \({\dot Q_{zj}}\) \textgreater{} 0 ) THEN
+
+\begin{equation}
+\overline {{T_{SP}}}  = \overline {{T_Z}}  + \left( {\frac{{\sum\limits_{j = 1}^{NumControlZones} {{{\dot Q}_{Zi}}} }}{{\sum\limits_{j = 1}^{NumControlZones} {{{\dot m}_{Zi}}\cdot C{p_j}} }}} \right)
+\end{equation}
+
+END IF
+
+\begin{equation}
+{\bar T_z} = {{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{zj}} \bullet } C{p_j} \bullet {T_{zj}}} \right)} \mathord{\left/ {\vphantom {{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{zj}} \bullet } C{p_j} \bullet {T_{zj}}} \right)} {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{zj}} \bullet } C{p_j}} \right)}}} \right. } {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{zj}} \bullet } C{p_j}} \right)}}
+\end{equation}
+
+where,
+
+\({\bar T_{SP}}\) ~~~~~~~~~~~~~~~~~ = average supply air setpoint temperature (°C)
+
+\(NumControlZones\) = number of controlled zones (i.e., zones that contain thermostat objects) served by the air loop (-)
+
+\({\dot Q_{Zj}}\) = sensible heating load required to reach the zone air temperature setpoint for the \emph{j}\(^{th}\) controlled zone at current time step (W)
+
+\({\dot m_{Zj}}\) = air mass flow rate being supplied by the air loop to the \emph{j}\(^{th}\) controlled zone, lagged by one HVAC simulation time step (kg/s)
+
+\(C{p_j}\) = specific heat of supply air for the j\(^{th}\) controlled zone (J/kg-K)
+
+\({T_{Zj}}\) = air node temperature for the \emph{j}\(^{th}\) controlled zone (°C)
+
+\({\overline T_Z}\) = average zone air node temperature weighted by the heat capacity rate of the supply air streams for the controlled zones served by the air loop (°C)
+
+\(TotZones\) = total number of zones served by the air loop (-)
+
+Note that for heating \({\dot Q_{Zj}} > 0.\) ~The average supply air setpoint temperature \({\bar T_{SP}}\) ~is constrained to be less than or equal to the maximum setpoint temperature (user input) and greater than or equal to the minimum setpoint temperature (user input). If the sum of the zone sensible heating loads is extremely small (i.e., no heating load), the setpoint temperature is set to the minimum. \({\bar T_{SP}}\) will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:Heating:Average object.
+
+\subsection{Multizone Cooling Average}\label{multizone-cooling-average}
+
+The input object SetpointManager:MultiZone:Cooling:Average provides a setpoint manager that attempts to establish a supply air cooling setpoint that will meet the cooling load of multiple zones served by an HVAC air loop. The algorithm aggregates the predicted cooling loads for all controlled zones served by an air loop (i.e., zones that have a thermostat object), and calculates the multizone average supply air cooling setpoint temperature as follows:
+
+IF ( \({\dot Q_{zj}}\) \textless{} 0 ) THEN
+
+\begin{equation}
+\overline {{T_{SP}}}  = \overline {{T_Z}}  + \left( {\frac{{\sum\limits_{j = 1}^{NumControlZones} {{{\dot Q}_{Zi}}} }}{{\sum\limits_{j = 1}^{NumControlZones} {{{\dot m}_{Zi}}\cdot C{p_j}} }}} \right)
+\end{equation}
+
+END IF
+
+\begin{equation}
+{\bar T_z} = {{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{Zj}} \bullet } C{p_j} \bullet {T_{zj}}} \right)} \mathord{\left/ {\vphantom {{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{Zj}} \bullet } C{p_j} \bullet {T_{zj}}} \right)} {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{Zj}} \bullet } C{p_j}} \right)}}} \right. } {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{Zj}} \bullet } C{p_j}} \right)}}
+\end{equation}
+
+Note that for cooling \({\dot Q_{Zj}} < 0.\) The average supply air setpoint temperature \({\bar T_{SP}}\) is constrained to be less than or equal to the maximum setpoint temperature (user input) and greater than or equal to the minimum setpoint temperature (user input). If the sum of the zone sensible cooling loads is extremely small (i.e., no cooling load), the setpoint temperature is set to the maximum. \({\bar T_{SP}}\) will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:Cooling:Average object.
+
+\subsection{Multizone Minimum Humidity Average}\label{multizone-minimum-humidity-average}
+
+The input object SetpointManager:MultiZone:MinimumHumidity:Average provides a setpoint manager that attempts to establish a supply air minimum humidity ratio setpoint that will meet the humidification load of multiple zones served by an HVAC air loop.~ This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level for all controlled zones served by an air loop (i.e., zones that have a humidistat object with a humidifying setpoint schedule), and uses moisture mass balances to calculate the average supply air minimum humidity ratio setpoint as follows:
+
+IF ( \({\dot Q_{lzj}}\) \textgreater{} 0 ) THEN
+
+\begin{equation}
+  \bar{\omega}_{SP} = \bar{\omega}_Z + \frac{\sum\limits_{j = 1}^{NumControlZones}\dot{Q}_{l,Zj}}{\sum\limits_{j = 1}^{NumControlZones}\dot{m}_{ZJ}}
+\end{equation}
+
+END IF
+
+\begin{equation}
+  \bar{\omega}_{Z} = \frac{\sum\limits_{j = 1}^{TotZones}\dot{m}_{Zj}\omega_{Zj}}{\sum\limits_{j = 1}^{TotZones}\dot{m}_{ZJ}}
+\end{equation}
+
+where,
+
+\({\bar \omega_{SP}}\) = average supply air minimum humidity ratio setpoint (kg H\(_{2}\)O/kg air)
+
+\(NumControlZones\) = number of controlled zones (i.e., zones that contain humidistat objects with humidifying setpoint schedule) served by the air loop (-)
+
+\({\dot Q_{lZj}}\) = latent (humidification) load required to reach the zone air humidifying setpoint for the \emph{j}\(^{th}\) controlled zone at current time step (kg H\(_{2}\)O/s)
+
+\({\dot m_{Zj}}\) = air mass flow rate being supplied by the air loop to the \emph{j}\(^{th}\) controlled zone, lagged by one HVAC simulation time step (kg/s)
+
+\({\omega_{Zj}}\) = air node humidity ratio for the jth controlled zone (kg H\(_{2}\)O/kg air)
+
+\({\bar \omega_Z}\) = average zone air node humidity ratio weighted by supply air mass flow rate for the controlled zones served by the air loop (kg H\(_{2}\)O/kg air)
+
+\(TotZones\) = total number of zones served by the air loop (-)
+
+Note that a positive latent load means humidification is required. The average supply air minimum humidity ratio setpoint \({\bar \omega_{SP}}\) is constrained to be less than or equal to the maximum setpoint humidity ratio (user input) and greater than or equal to the minimum setpoint humidity ratio (user input). If the sum of the zone latent humidification loads is extremely small (i.e., no humidification load), the humidity ratio setpoint is set to the minimum. \({\bar \omega_{SP}}\) will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:MinimumHumidity:Average object. A humidification component (e.g., an electric humidifier) placed upstream of this node can then use the humidity ratio setpoint to control its moisture addition rate.
+
+All setpoint managers are executed at the beginning of the simulation time step. Therefore, the calculated setpoint is based on the resulting zone air node humidity ratios and supply air mass flow rates for the previous simulation time step.
+
+\subsection{Multizone Maximum Humidity Average}\label{multizone-maximum-humidity-average}
+
+The input object SetpointManager:MultiZone:MaximumHumidity:Average provides a setpoint manager that attempts to establish a supply air maximum humidity ratio setpoint that will meet the dehumidification load of multiple zones served by an HVAC air loop. This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level for all controlled zones served by an air loop (i.e., zones that have a humidistat object with a dehumidifying setpoint schedule), and uses moisture mass balances to calculate the average supply air maximum humidity ratio as follows:
+
+IF ( \({\dot Q_{lzj}}\) \textless{} 0 ) THEN
+
+\begin{equation}
+  \bar{\omega}_{SP} = \bar{\omega}_Z + \frac{\sum\limits_{j = 1}^{NumControlZones}\dot{Q}_{l,Zj}}{\sum\limits_{j = 1}^{NumControlZones}\dot{m}_{ZJ}}
+\end{equation}
+
+END IF
+
+\begin{equation}
+  \bar{\omega}_{Z} = \frac{\sum\limits_{j = 1}^{TotZones}\dot{m}_{Zj}\omega_{Zj}}{\sum\limits_{j = 1}^{TotZones}\dot{m}_{ZJ}}
+\end{equation}
+
+Note that a negative latent load means dehumidification is required. The average supply air maximum humidity ratio setpoint \({\bar \omega_{SP}}\) is constrained to be less than or equal to the maximum setpoint humidity ratio (user input) and greater than or equal to the minimum setpoint humidity ratio (user input). If the sum of the zone latent dehumidification loads is extremely small (i.e., no dehumidification load), the humidity ratio setpoint is set to the maximum. \({\bar \omega_{SP}}\) will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:MaximumHumidity:Average object. A dehumidification component (e.g., an desiccant dehumidifier) placed upstream of this node can then use the humidity ratio setpoint to control its moisture removal rate. In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determines the minimum supply air temperature required to meet both the temperature (sensible) and humidity (latent) load in the control zone (ref: Controller:WaterCoil).
+
+\subsection{MultiZone Minimum Humidity Supply Air Reset}\label{multizone-minimum-humidity-supply-air-reset}
+
+The input object SetpointManager:MultiZone:Humidity:Minimum provides a setpoint manager that attempts to establish a supply air minimum humidity ratio setpoint that will meet the humidification load of zone with the critical humidification requirement at each time step served by an HVAC air loop at the zone actual supply air mass flow rate.~ This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level for all controlled zones served by an air loop (i.e., zones that have a humidistat object with a humidifying setpoint schedule), and uses moisture mass balances to calculate the supply air minimum humidity ratio setpoint.~ The algorithm loops over all the zones that the system can humidify and calculates the setpoint based on a zone with the highest humidity ratio setpoint requirement as follows:
+
+IF (\({\dot Q_{lzj}}\) \textgreater{} 0) THEN
+
+\begin{equation}
+{\omega_{SP\;Zj}} = {\omega_{Zj}} + {{{{\dot Q}_{lZj}}} \mathord{\left/ {\vphantom {{{{\dot Q}_{lZj}}} {{{\dot m}_{Zj}}}}} \right. } {{{\dot m}_{Zj}}}}
+\end{equation}
+
+END IF
+
+\begin{equation}
+{\omega_{SP\;Zj}} = MAX\left( {{\omega_{SP\;Zj}},\;{\omega_{SP\;Min}}} \right)
+\end{equation}
+
+\begin{equation}
+{\omega_{SP}} = MIN\left( {{\omega_{SP\;Zj}},\;{\omega_{SP\;Max}}} \right)
+\end{equation}
+
+where,
+
+\({\omega_{SP}}\) = supply air humidity ratio setpoint (kg/kg)
+
+\({\dot Q_{lzj}}\) = latent load required to reach the zone air setpoint for the \emph{j}\(^{th}\) controlled zone at current time step (kg H\(_{2}\)O/s)
+
+\({\dot m_{Zj}}\) = actual mass flow rate supplied by the air loop to the \emph{j}\(^{th}\) controlled zone, (kg/s)
+
+\({\omega_{Zj}}\) = air node humidity ratio for the j\(^{th}\) controlled zone (kg/kg)
+
+\({\omega_{SP\;Zj}}\) = supply air humidity ratio setpoint for the j\(^{th}\) controlled zones (kg/kg)
+
+\({\omega_{SP\;Min}}\) = user-specified supply air minimum humidity ratio setpoint (kg/kg)
+
+\({\omega_{SP\;Max}}\) = user-specified supply air maximum humidity ratio setpoint (kg/kg)
+
+Note that a positive latent load means humidification is required. The supply air minimum humidity ratio setpoint \({\omega_{SP}}\) is constrained to be less than or equal to the maximum setpoint humidity ratio (user input) and greater than or equal to the minimum setpoint humidity ratio (user input). If the humidification load for all zones in the air loop is extremely small (i.e., no humidification load), the humidity ratio setpoint is set to the user input minimum value. \({\omega_{SP}}\) will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:Humidity:Minimum object. A humidification component (e.g., an electric humidifier) placed upstream of this node can then use the humidity ratio setpoint to control its moisture addition rate.
+
+\subsection{MultiZone Maximum Humidity Supply Air Reset}\label{multizone-maximum-humidity-supply-air-reset}
+
+The input object SetpointManager:MultiZone:Humidity:Maximum provides a setpoint manager that attempts to establish a supply air maximum humidity ratio setpoint that will meet the dehumidification load of the zone with the critical dehumidification requirement at each time step served by an HVAC air loop at the zone actual supply air mass flow rate. This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level for all controlled zones served by an air loop (i.e., zones that have a humidistat object with a dehumidifying setpoint schedule), and uses moisture mass balances to calculate the supply air maximum humidity ratio setpoint.~ The algorithm loops over all the zones that the system can dehumidify and calculates the setpoint based on a zone with the lowest humidity ratio setpoint requirement as follows:
+
+IF (\({\dot Q_{lzj}}\) \textless{} 0) THEN
+
+\begin{equation}
+{\omega_{SP\;Zj}} = {\omega_{Zj}} + {{{{\dot Q}_{lZj}}} \mathord{\left/ {\vphantom {{{{\dot Q}_{lZj}}} {{{\dot m}_{Zj}}}}} \right. } {{{\dot m}_{Zj}}}}
+\end{equation}
+
+END IF
+
+\begin{equation}
+{\omega_{SP\;Zj}} = MAX\left( {{\omega_{SP\;Zj}},\;{\omega_{SP\;Min}}} \right)
+\end{equation}
+
+\begin{equation}
+{\omega_{SP}} = MIN\left( {{\omega_{SP\;Zj}},\;{\omega_{SP\;Max}}} \right)
+\end{equation}
+
+Note that a negative latent load means dehumidification is required. The supply air maximum humidity ratio setpoint \({\omega_{SP}}\) is constrained to be less than or equal to the maximum setpoint humidity ratio (user input) and greater than or equal to the minimum setpoint humidity ratio (user input). If the dehumidification load for all zones in the air loop is extremely small (i.e., no dehumidification load), the humidity ratio setpoint is set to the user input maximum value. \({\omega_{SP}}\) will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:Humidity:Maximum object. A dehumidification component (e.g., an desiccant dehumidifier) placed upstream of this node can then use the humidity ratio setpoint to control its moisture removal rate. In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determines the minimum supply air temperature required to meet both the temperature (sensible) and dehumidification (latent) load in the control zone (ref: Controller:WaterCoil).
+
+\subsection{Follow Outdoor Air Temperature}\label{follow-outdoor-air-temperature}
+
+The input object SetpointManager:FollowOutdoorAirTemperature provides a setpoint manager that is used to place a temperature setpoint on a system node that is derived from the current outdoor air environmental conditions.~ The outdoor air conditions are obtained from the weather information during the simulation.
+
+IF (ReferenceTemperatureType = = OutdoorWetBulb)
+
+~~~ Setpoint = OutdoorWetBulbTemp + OffSet
+
+ELSEIF (ReferenceTemperatureType = = OutdoorDryBulb)
+
+~~~ Setpoint = OutdoorDryBulbTemp + OffSet
+
+ENDIF
+
+Setpoint = MAX(Setpoint, MinSetPoint)
+
+Setpoint = MIN(Setpoint, MaxSetPoint)
+
+MinSetPoint, MaxSetPoint and Offset are specified by the user as the input in object SetpointManager:FollowOutdoorAirTemperature.
+
+\subsection{Follow System Node Temperature}\label{follow-system-node-temperature}
+
+The input object SetpointManager:FollowSystemNodeTemperature provides a temperature setpoint on a system node that is derived from the current temperatures at a separate system node.~ The current value of the temperature at a reference node are obtained and used to generate setpoint on a second system node.~ If the reference node is also designated to be an outdoor air (intake) node, then this setpoint manager can be used to follow outdoor air conditions that are adjusted for altitude.
+
+IF (ReferenceTemperatureType = = NodeWetBulb)
+
+~~~ Setpoint = NodeWetbulbTemp + OffSet
+
+ELSEIF (ReferenceTemperatureType = = NodeDryBulb)
+
+~~~ Setpoint = NodeDrybulbTemp + OffSet
+
+ENDIF
+
+Setpoint = MAX(Setpoint, MinSetPoint)
+
+Setpoint = MIN(Setpoint, MaxSetPoint)
+
+MinSetPoint, MaxSetPoint and Offset are specified by the user as the input in object SetpointManager:FollowSystemNodeTemperature.
+
+\subsection{Follow Ground Temperature}\label{follow-ground-temperature}
+
+The input object SetpointManager:FollowGroundTemperature provides a temperature setpoint on a system node that is derived from a current ground temperature.~ The ground temperatures are specified in different Site:GroundTemperature:* objects and used during the simulation.~ This setpoint manager is primarily intended for condenser or plant loops using some type of ground heat exchanger.
+
+IF (ReferenceGroundTemperatureObjectType = = BuildingSurface)
+
+~~~ Setpoint = GroundTemp + OffSet
+
+ELSEIF (ReferenceGroundTemperatureObjectType = = Shallow)
+
+~~~ Setpoint = GroundTemp\_Surface + OffSet
+
+ELSEIF (ReferenceGroundTemperatureObjectType = = Deep)
+
+~~~ Setpoint = GroundTemp\_Deep + OffSet
+
+ELSEIF (ReferenceTGroundTemperatureObjectType = = FCfactorMethod)
+
+~~~ Setpoint = GroundTemp\_FC + OffSet
+
+ENDIF
+
+Setpoint = MAX(Setpoint, MinSetPoint)
+
+Setpoint = MIN(Setpoint, MaxSetPoint)
+
+\emph{~}
+
+Where,
+
+GroundTemp = Current ground temperature (C)
+
+(Ref: Site:GroundTemperature:BuildingSurface)
+
+GroundTemp\_Surface = Current surface ground temperature~ (C)
+
+(Ref: Site:GroundTemperature:Shallow)
+
+GroundTemp\_Deep~ = Current deep ground temperature~ (C)
+
+(Ref: Site:GroundTemperature:Deep)
+
+GroundTemp\_FC = Current ground temperature defined F or C factor method (C)
+
+(Ref: Site:GroundTemperature:FCfactorMethod)
+
+MinSetPoint, MaxSetPoint and Offset are specified by the user as the input in object SetpointManager:FollowGroundTemperature.
+
+\subsection{Condenser Entering Water Temperature Reset}\label{condenser-entering-water-temperature-reset}
+
+The object resets the condenser entering water temperature to the optimal cooling tower water set point temperature that will result in minimum net energy consumption for the chiller and cooling tower plant. This chiller-tower optimization scheme uses one curve to determine the optimum condenser entering water temperature for a given time step and two other curves to place limit conditions on the ``optimized'' set point value. The optimized condenser entering water temperature may not be valid every timestep then will be limited algorithmically by two boundary curves. The first of these boundary curves is given by:
+
+\emph{MinDsnWB = C1 + C2*OaWb + C3*WPLR + C4*TwrDsnWB + C5*NF}
+
+where:
+
+\emph{C1-C5} = curve coefficients
+
+\emph{OaWb} = outside air wetbulb for current timestep, C
+
+\emph{TwrDsnWB} = Tower design inlet Air Wet-Bulb Temperature, C
+
+\emph{WPLR} = Weighted PLR
+
+~~~ = ChillerCoolingLoadThisTimestep / NominalChillerCapacity
+
+NF = Normalized condenser water flow per unit of tower capacity, m3/W
+
+~~~~~ = Design Tower Flow Rate / Design Tower Capacity \emph{(typically 5.382E-8 m3/s, i.e., 3 gpm/ton)}
+
+MinDsnWB is compared against the design tower wetbulb. This curve is usually a function of Weighted PLR and NF. So if NF is constant at 5.382E-8 m3/s (3 gpm/ton), the curve can be depicted as follows:
+
+\begin{figure}[hbtp] % fig 292
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6482.png}
+\caption{Minimum Tower Design Wet Bulb Boundary Condition \protect \label{fig:minimum-tower-design-wet-bulb-boundary}}
+\end{figure}
+
+The second boundary curve is given by:
+
+\emph{MinActualWb = C1 + C2*MinDsnWB + C3*WPLR + C4*TwrDsnWB + C5*NF}
+
+where,
+
+\emph{C1-C5 = curve coefficients}
+
+\emph{MinDsnWB = from first boundary equation, C}
+
+\emph{TwrDsnWB = Tower design inlet Air Wet-Bulb Temperature, C}
+
+\emph{WPLR = Weighted PLR}
+
+\emph{~~~~~~~~~~ = ChillerCoolingLoadThisTimestep / NominalChillerCapacity}
+
+\emph{NF = Normalized condenser water flow per unit of tower capacity, m3/W}
+
+\emph{~~~~~ = Design Tower Flow Rate / Design Tower Capacity (typically 5.382E-8 m3/s, i.e., 3 gpm/ton)}
+
+MinActualWb is compared against this time step's outside air wet bulb. This curve is usually a function of MinDesignWB, WeightedRatio and TwrDesignWB. So if TwrDesignWB is constant at 25.6 °C (78 °F), and NF = 5.382E-8 m3/s (3 gpm/ton), the curve can be depicted as follows:
+
+\begin{figure}[hbtp] % fig 293
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6483.png}
+\caption{Minimum Wet Bulb Boundary Condition \protect \label{fig:minimum-wet-bulb-boundary-condition}}
+\end{figure}
+
+The Optimized Condenser Entering Water Temperature is calculated with this equation:
+
+\emph{OptCondEntTemp = C1 + C2*OaWb + C3*WPLR + C4*TwrDsnWB + C5*NF}
+
+where,
+
+\emph{C1-C5 = curve coefficients}
+
+\emph{OaWB = this timestep's outside air wetbulb, C}
+
+\emph{TwrDsnWB = Tower design inlet Air Wet-Bulb Temperature, C}
+
+\emph{WPLR = Weighted PLR}
+
+\emph{~~~~~~~~~~ = ChillerCoolingLoadThisTimestep / NominalChillerCapacity}
+
+\emph{NF = Normalized condenser water flow per unit of tower capacity, m3/W}
+
+\emph{~~~~~ = Design Tower Flow Rate / Design Tower Capacity (typically 5.382E-8 m3/s, i.e., 3 gpm/ton)}
+
+A graph of the curve can be depicted as follows:
+
+\begin{figure}[hbtp] % fig 294
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6484.png}
+\caption{Optimum EWT vs PLR \& OaWb \protect \label{fig:optimum-ewt-vs-plr-oawb}}
+\end{figure}
+
+The optimized condenser entering water temperature is calculated but is not necessarily used each timestep. If OptCondEntTemp does not fall within the bounds established by MinDsnWB and MinActualWb, then the value from the Default Condenser Entering Water Temperature Schedule is used for the Condenser Entering Water Set Point instead.
+
+\subsubsection{Special Note for Multiple Towers}\label{special-note-for-multiple-towers}
+
+This control scheme is available for multiple towers by following two steps:
+
+\begin{itemize}
+\tightlist
+\item
+  Use average tower conditions in the curves for the independent variables related to the towers
+\item
+  Make sure the setpoint is applied to either the condenser supply outlet node or use a node list to apply it to each tower outlet node
+\end{itemize}
+
+\subsection{Ideal Condenser Entering Water Temperature Reset}\label{ideal-condenser-entering-water-temperature-reset}
+
+The object determines a ``near-optimal'' condenser water entering set point at each time step that will result in minimum net energy consumption for the chiller and cooling tower plant. The ``ideal'' chiller-tower optimization scheme uses a search algorithm to find the ideal optimal setpoint at a given timestep. This requires resimulating HVAC systems at each timestep until finding an ``optimal'' condenser water entering setpoint (OptSetpoint) which gives the minimum total chiller, cooling tower, chilled water pump and condenser water pump power consumption (TEC). The OptSetpoint falls between realistic minimum and maximum boundaries, which are set by the user. The minimum boundary is determined based on the minimum lift (user input) and evaporator leaving water temperature. The maximum boundary is specified by the user. It is assumed that a single minimum point exists between these boundaries. The following steps are used to find ``optimal'' setpoint:
+
+1)~~~Set an initial setpoint value for the iteration to a user-defined maximum condenser entering water temperature (Toptset\(_{1}\)) and calculate TEC.
+
+2)~~~Decrease the setpoint value by 1ËšC (Toptset\(_{2}\) = Toptset\(_{1}\)--1ËšC) and calculate TEC.
+
+3)~~~Compare the TEC in Step 1 (TEC\(_{1}\)) and TEC in Step 2 (TEC\(_{2}\)), i.e., (dTEC\(_{1}\) = TEC\(_{1}\)--TEC\(_{2}\)).
+
+4)~~~If dTEC\(_{1}\) is negative, stop the iteration and set the ``optimal'' setpoint to Toptset\(_{1}\).
+
+5)~~~If dTEC\(_{1}\) is positive, Decrease the setpoint value by 1ËšC and calculate TEC. Compare the TECs and repeat this step (i.e., dTEC\(_{N}\) = TEC\(_{N}\)--TEC\(_{N+1}\)) until either Toptset\(_{N+1}\) reaches to the minimum boundary value or dTEC\(_{N}\) becomes negative.
+
+6)~~~If Toptset\(_{N}\) reaches to the minimum boundary value and still dTEC\(_{N}\) is positive, set the ``optimal'' setpoint to Toptset\(_{N+1}\).
+
+7)~~~If TEC\(_{N}\) becomes negative, decrease Toptset\(_{N-1}\) by 0.2ËšC and calculate TEC. Compare the TECs and repeat this step (i.e., dTEC\(_{M}\) = TEC\(_{M}\)--TEC\(_{M+1}\)) until dTEC\(_{M}\) becomes negative. Then set the ``optimal'' setpoint to Toptset\(_{M+1}\).
+
+\subsection{Plant Return Water Control Setpoint Reset}\label{plant-return-water-control-setpoint-reset}
+
+The input objects:
+
+\begin{itemize}
+\item
+  SetpointManager:ReturnTemperature:ChilledWater, and
+\item
+  SetpointManager:ReturnTemperature:HotWater
+\end{itemize}
+
+allow for controlling the temperature of the water (or a different fluid defined for the plant) that is returning back to the plant supply equipment. In a typical chilled water loop configuration, this is essentially controlling the temperature of the water entering the chiller. In a typical hot water loop configuration, this is essentially controlling the temperature of the water entering the boiler.
+
+The target return temperature can be specified by:
+
+\begin{itemize}
+\item
+  providing a constant value to use throughout the simulation, or
+\item
+  scheduling the value to vary through the simulation (which then allows custom EMS overriding of the scheduled value), or
+\item
+  using a separate setpoint manager to set the setpoint on the return node itself, which is then retrieved by this reset manager.
+\end{itemize}
+
+\subsubsection{Operation}\label{operation}
+
+The setpoint manager senses conditions on two named nodes, which should correspond to a central plant's supply side inlet and outlet nodes, the return and supply nodes, respectively. The temperature and flow rate information is used in a series of calculations in order to determine a setpoint to specify on the supply outlet node which will in turn provide the target desired return temperature on the supply inlet node. The calculations are summarized for a chilled water loop here:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Use the current supply and demand temperatures to calculate an average temperature for property calculation: \(C_p = f\left(T_{avg}\right) = f\left(\frac{T_{ret}+T_{sup}}{2}\right)\)
+\item
+  Calculate the current loop demand using: \(\dot{Q} = \dot{m} * C_p * \left(T_{ret} - T_{sup}\right)\)
+\item
+  Assuming that this load will be the same moving forward, we can calculate what supply temperature we should target in order to meet the desired return temperature.
+\item
+  So retrieve the current target return temperature, \(T_{ret,target}\) , either from a schedule or constant value.
+\item
+  Then calculate the supply temperature setpoint using: \(T_{sup,sp} = T_{ret,target} - \frac{\dot{Q}}{\dot{m} C_p}\)
+\item
+  Constrain the value to user-specified limiting min/max values
+\end{enumerate}
+
+For a chilled water loop, the user-specified minimum is the default setpoint used in cases of no-load or negative-load. In a hot-water loop the user-specified maximum is used for these situations. Also, in a hot-water loop the sign of the demand will be reversed.
+
+\subsubsection{Key control note}\label{key-control-note}
+
+The setpoint will be reset at the beginning of a system time step, and remain that way through that time step. The setpoint is calculated based on the latest known value of loop demand and loop flow rate. If the demand and flow rate remain the same for the currently calculated time step, the loop will maintain control well. However, if either changes, there will be a lag effect while the loop attempts to maintain control. Consider the following plot, with a short description following:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/SetPointManager-ResetForReturnControl1.png}
+\caption{}
+\end{figure}
+
+Throughout the day, the heat addition (green line) to the loop increases. Each time it increases, there is a small period of time where the loop attempts to regain control of the return temperature. The setpoint is only reset at the beginning of the system time step, so as the plant converges within a single time step, the load will vary and the return temperature may not be exactly on target.
+
+This isn't necessarily a big problem. However, some users may be especially interested in very tight control of the return temperature. This can be done very easily by simply reducing the simulation time step. For example, in the following plot, the time step was reduced from 10 minutes to 1 minute, with some description following the plot:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/SetPointManager-ResetForReturnControl2.png}
+\caption{}
+\end{figure}
+
+With the smaller time step, the reporting frequency is higher. But more importantly, with the smaller time step, the setpoint can be corrected much more often. Because of this, the return temperature regains control much quicker than with the larger time step.
+
+However, these examples are for a jagged demand profile full of discontinuous step changes in loop demand. As a final example, this return water temperature control is applied to the large office reference building chilled water loop. Here is the response:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/SetPointManager-ResetForReturnControl3.png}
+\caption{}
+\end{figure}
+
+Note the control is working properly, maintaining a return temperature around the target of 12 degrees where possible. Since the load profile is a typical -smooth- profile, the control is also much smoother. This should be a good representation of the capabilities of this setpoint manager.
+
+For jagged load profiles, if tight control is highly important, choosing a smaller timestep (\textasciitilde{}1 minute) is recommended. For normal building profiles, the typical range of timesteps (\textasciitilde{}15 minute) should be fully satisfactory.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/solar-collectors.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/solar-collectors.tex
new file mode 100644
index 00000000000..0f75e276183
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-002/solar-collectors.tex
@@ -0,0 +1,1217 @@
+\section{Solar Collectors }\label{solar-collectors}
+
+Solar collectors are devices that convert solar energy into thermal energy by raising the temperature of a circulating heat transfer fluid.~ The fluid can then be used to heat water for domestic hot water usage or space heating.~ Flat-plate solar collectors using water as the heat transfer fluid, Integral-Collector Storage solar collectors using water and unglazed transpired solar collectors using air are currently the only types of collector available in EnergyPlus.
+
+\subsection{Flat-Plate Solar Collectors}\label{flat-plate-solar-collectors}
+
+The input object SolarCollector:FlatPlate:Water provides a model for flat-plate solar collectors that are the most common type of collector.~ Standards have been established by ASHRAE for the performance testing of these collectors (ASHRAE 1989; 1991) and the Solar Rating and Certification Corporation (SRCC) publishes a directory of commercially available collectors in North America (SRCC 2003).
+
+The EnergyPlus model is based on the equations found in the ASHRAE standards and Duffie and Beckman (1991).~ This model applies to glazed and unglazed flat-plate collectors, as well as banks of tubular, i.e.~evacuated tube, collectors.
+
+\subsubsection{Solar and Shading Calculations}\label{solar-and-shading-calculations-000}
+
+The solar collector object uses a standard EnergyPlus surface in order to take advantage of the detailed solar and shading calculations.~ Solar radiation incident on the surface includes beam and diffuse radiation, as well as radiation reflected from the ground and adjacent surfaces.~ Shading of the collector by other surfaces, such as nearby buildings or trees, is also taken into account.~ Likewise, the collector surface can shade other surfaces, for example, reducing the incident radiation on the roof beneath it.
+
+\subsubsection{Thermal Performance}\label{thermal-performance}
+
+The thermal efficiency of a collector is defined as the ratio of the useful heat gain of the collector fluid versus the total incident solar radiation on the gross surface area of the collector.
+
+\begin{equation}
+\eta  = \frac{{(q/A)}}{{{I_{solar}}}}
+\end{equation}
+
+where
+
+q = useful heat gain
+
+A = gross area of the collector
+
+I\(_{solar}\) = total incident solar radiation
+
+Notice that the efficiency h is only defined for I\(_{solar}\) \textgreater{} 0.
+
+An energy balance on a solar collector with double glazing shows relationships between the glazing properties, absorber plate properties, and environmental conditions.
+
+\begin{equation}
+\frac{q}{A} = {I_{solar}}{\tau_{g1}}{\tau_{g2}}{\alpha_{abs}} - \frac{{T_{abs}^4 - T_{g2}^4}}{{{R_{rad}}}} - \frac{{{T_{abs}} - {T_{g2}}}}{{{R_{conv}}}} - \frac{{{T_{abs}} - {T_{air}}}}{{{R_{cond}}}}
+\end{equation}
+
+where
+
+t\(_{g1}\) = transmittance of the first glazing layer
+
+t\(_{g2}\) = transmittance of the second glazing layer
+
+a\(_{abs}\) = absorptance of the absorber plate
+
+R\(_{rad}\) = radiative resistance from absorber to inside glazing
+
+R\(_{conv}\) = convective resistance from absorber to inside glazing
+
+R\(_{cond}\) = conductive resistance from absorber to outdoor air through the insulation
+
+T\(_{abs}\) = temperature of the absorber plate
+
+T\(_{g2}\) = temperature of the inside glazing
+
+T\(_{air}\) = temperature of the outdoor air
+
+The equation above can be approximated with a simpler formulation as:
+
+\begin{equation}
+\frac{q}{A} = {F_R}\left[ {{I_{solar}}(\tau \alpha ) - {U_L}({T_{in}} - {T_{air}})} \right]
+\end{equation}
+
+where
+
+F\(_{R}\) = an empirically determined correction factor
+
+(ta) = the product of all transmittance and absorptance terms
+
+U\(_{L}\) = overall heat loss coefficient combining radiation, convection, and conduction terms
+
+T\(_{in}\) = inlet temperature of the working fluid
+
+Substituting this into Equation ,
+
+\begin{equation}
+\eta  = {F_R}(\tau \alpha ) - {F_R}{U_L}\frac{{({T_{in}} - {T_{air}})}}{{{I_{solar}}}}
+\end{equation}
+
+A linear correlation can be constructed by treating F\(_{R}\)(ta) and -F\(_{R}\)U\(_{L}\) as characteristic constants of the solar collector:
+
+\begin{equation}
+\eta  = {c_0} + {c_1}\frac{{\left( {{T_{in}} - {T_{air}}} \right)}}{{{I_{solar}}}}
+\end{equation}
+
+Similarly, a quadratic correlation can be constructed using the form:
+
+\begin{equation}
+\eta  = {c_0} + {c_1}\frac{{\left( {{T_{in}} - {T_{air}}} \right)}}{{{I_{solar}}}} + {c_2}\frac{{{{\left( {{T_{in}} - {T_{air}}} \right)}^2}}}{{{I_{solar}}}}
+\end{equation}
+
+Both first- and second-order efficiency equation coefficients are listed in the \emph{Directory of SRCC Certified Solar Collector Ratings}.
+
+\subsubsection{Incident Angle Modifiers}\label{incident-angle-modifiers}
+
+As with regular windows the transmittance of the collector glazing varies with the incidence angle of radiation.~ Usually the transmittance is highest when the incident radiation is normal to the glazing surface.~ Test conditions determine the efficiency coefficients for normal incidence.~ For off-normal angles, the transmittance of the glazing is modified by an \emph{incident angle modifier} coefficient.
+
+\begin{equation}
+{K_{\tau \alpha }} = \frac{{\left( {\tau \alpha } \right)}}{{{{\left( {\tau \alpha } \right)}_n}}}
+\end{equation}
+
+Additional testing determines the incident angle modifier as a function of incident angle q.~ This relationship can be fit to a first-order, linear correlation:
+
+\begin{equation}
+{K_{\tau \alpha }} = 1 + {b_0}\left( {\frac{1}{{\cos \theta }} - 1} \right)
+\end{equation}
+
+or a second-order, quadratic correlation:
+
+\begin{equation}
+{K_{\tau \alpha }} = 1 + {b_0}\left( {\frac{1}{{\cos \theta }} - 1} \right) + {b_1}{\left( {\frac{1}{{\cos \theta }} - 1} \right)^2}
+\end{equation}
+
+The incident angle modifier coefficients \emph{b\(_{0}\)} and \emph{b\(_{1}\)} are usually negative, although some collectors have a positive value for \emph{b\(_{0}\)}.~ Both first- and second-order incident angle modifier equation coefficients are listed in the \emph{Directory of SRCC Certified Solar Collector Ratings}.
+
+The SRCC incident angle modifier equation coefficients are only valid for incident angles of 60 degrees or less.~ Because these curves can be valid yet behave poorly for angles greater than 60 degree, the EnergyPlus model cuts off collector gains for incident angles greater than 60 degrees.
+
+For flat-plate collectors, the incident angle modifier is generally symmetrical.~ However, for tubular collectors the incident angle modifier is different depending on whether the incident angle is parallel or perpendicular to the tubes.~ These are called bi-axial modifiers.~ Some special flat-plate collectors may also exhibit this asymmetry.~ The current model cannot yet handle two sets of incident angle modifiers.~ In the meantime it is recommended that tubular collectors be approximated with caution using either the parallel or perpendicular correlation.
+
+Incident angle modifiers are calculated separately for sun, sky, and ground radiation.~ The net incident angle modifier for all incident radiation is calculated by weighting each component by the corresponding modifier.
+
+\begin{equation}
+{K_{\tau \alpha ,net}} = \frac{{{I_{beam}}{K_{\tau \alpha ,beam}} + {I_{sky}}{K_{\tau \alpha ,sky}} + {I_{gnd}}{K_{\tau \alpha ,gnd}}}}{{{I_{beam}} + {I_{sky}} + {I_{gnd}}}}
+\end{equation}
+
+For sky and ground radiation the incident angle is approximated using Brandemuehl and Beckman's equations:
+
+\begin{equation}
+{\theta_{sky}} = 59.68 - 0.1388\phi  + 0.001497{\phi ^2}
+\end{equation}
+
+\begin{equation}
+{\theta_{ground}} = 90.0 - 0.5788\phi  + 0.002693{\phi ^2}
+\end{equation}
+
+where f is the surface tilt in degrees.
+
+The net incident angle modifier is then inserted into the useful heat gain equation :
+
+\begin{equation}
+\frac{q}{A} = {F_R}\left[ {{I_{solar}}{K_{\tau \alpha ,net}}{{(\tau \alpha )}_n} - {U_L}({T_{in}} - {T_{air}})} \right]
+\end{equation}
+
+Equation is also modified accordingly.
+
+\begin{equation}
+\eta  = {F_R}{K_{\tau \alpha ,net}}{(\tau \alpha )_n} - {F_R}{U_L}\frac{{({T_{in}} - {T_{air}})}}{{{I_{solar}}}}
+\end{equation}
+
+\subsubsection{Outlet Temperature}\label{outlet-temperature}
+
+Outlet temperature is calculated using the useful heat gain q as determined by Equation , the inlet fluid temperature T\(_{in}\), and the mass flow rate available from the plant simulation:
+
+\begin{equation}
+\frac{q}{A} = \dot m{c_p}({T_{out}} - {T_{in}})
+\end{equation}
+
+where
+
+\(\dot m\) ~ = fluid mass flow rate through the collector
+
+c\(_{p}\) = specific heat of the working fluid
+
+Solving for T\(_{out}\),
+
+\begin{equation}
+{T_{out}} = {T_{in}} + \frac{q}{{\dot m{c_p}A}}
+\end{equation}
+
+If there is no flow through the collector, T\(_{out}\) is the stagnation temperature of the fluid.~ This is calculated by setting the left side of Equation to zero and solving for T\(_{in}\) (which also equals T\(_{out}\) for the no flow case).
+
+\subsubsection{References}\label{references-042}
+
+ASHRAE.~ 1989.~ ASHRAE Standard 96-1980 (RA 89):~ Methods of Testing to Determine the Thermal Performance of Unglazed Flat-Plate Liquid-Type Solar Collectors.~ Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+ASHRAE.~ 1991.~ ASHRAE Standard 93-1986 (RA 91):~ Methods of Testing to Determine the Thermal Performance of Solar Collectors.~ Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
+
+Duffie, J. A., and Beckman, W. A.~ 1991.~ Solar Engineering of Thermal Processes, Second Edition.~ New York:~ Wiley-Interscience.
+
+Solar Rating and Certification Corporation.~ 2004.~ Directory of SRCC Certified Solar Collector Ratings, OG 100.~ Cocoa, Florida:~ Solar Rating and Certification Corporation.
+
+\subsection{Integral-collector-storage (ICS) Solar Collector}\label{integral-collector-storage-ics-solar-collector}
+
+Solar collectors with integral storage unit models use SolarCollector:IntegralCollectorStorage object, and the characteristics parameter inputs of this collector are provided by the SolarCollectorPerformance:IntegralCollectorStorage object. This model is based on detailed Energy Balance equations of solar collectors that integrates storage in it. This model has two options to represent the collector bottom outside boundary conditions: AmbientAir, and OtherSideConditionsModel. AmbientAir simply applies outside air temperature using combined convection and radiation conductance, and the OtherSideConditionsModel applies combined radiation and convection models that exiats in a naturally ventilated cavity to represent the collector bottom outside boundary condition. The later boundary condition accounts for the shading of the collector on the underlying surface, hence, the ICS collector can be assumed as an integral part of the building envelope. Schematic diagram of a rectangular ICS solar collector is shown in Figure~\ref{fig:schematic-diagram-of-rectangular-integrated} below:
+
+\begin{figure}[hbtp] % fig 295
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6502.png}
+\caption{Schematic diagram of rectangular Integrated Collector Storage unit \protect \label{fig:schematic-diagram-of-rectangular-integrated}}
+\end{figure}
+
+\subsubsection{Solar and Shading Calculations}\label{solar-and-shading-calculations-1}
+
+The solar collector object uses a standard EnergyPlus surface in order to take advantage of the detailed solar and shading calculations. Solar radiation incident on the surface includes beam and diffuse radiation, as well as radiation reflected from the ground and adjacent surfaces. Shading of the collector by other surfaces, such as nearby buildings or trees, is also taken into account. Likewise, the collector surface shades the roof surface beneath it, hence no direct solar radiation incident on the roof surface. The collector and the roof outside boundary conditions should be specified as OtherSideConditionModel to account for solar collector shading impact on the roof surface.
+
+\subsubsection{Mathematical Model}\label{mathematical-model}
+
+The integral-collector-storage (ICS) solar collector is represented using two transient energy balance equations shown below.~ These equations represent the energy balance equation for the absorber plate, and the water in the collector.
+
+\begin{equation}
+{m_p}{C_p}\frac{{d{T_p}}}{{dt}} = A \cdot \left[ {{{\left( {\tau \alpha } \right)}_e} \cdot {I_t} - {h_{pw}}\left( {{T_p} - {T_w}} \right) - {U_t}\left( {{T_p} - {T_a}} \right)} \right]
+\end{equation}
+
+\begin{equation}
+{m_w}{C_w}\frac{{d{T_w}}}{{dt}} = A \cdot \left[ {{h_{pw}}\left( {{T_p} - {T_w}} \right) - {U_b}\left( {{T_w} - {T_{OSC}}} \right) - {U_s}\left( {{T_w} - {T_a}} \right)} \right] - {\dot m_w}{C_w}\left( {{T_w} - {T_{wi}}} \right)
+\end{equation}
+
+Where,
+
+\emph{m\(_{p}\)C\(_{p}\)} = thermal capacity of the absorber surface, J/°C
+
+A~~~~~~~ = collector gross area, m\(^{2}\)
+
+\emph{(ta)}\(_{e}\)~~~ = transmittance-absorptance product of the absorber plate and cover system
+
+\emph{I\(_{t}\)}~~~~~~~ = total solar irradiation, (W/m\(^{2}\))
+
+\emph{h\(_{pw}\)}~~~~~ = convective heat transfer coefficient from absorber plate to water, (W/m2°K)
+
+\emph{U\(_{t}\)}~~~~~~~ = overall heat loss coefficient from absorber to the ambient air, (W/m2 °K)
+
+\emph{T\(_{p}\)}~~~~~~~ = absorber plate average temperature, (°C)
+
+\emph{T\(_{w}\)}~~~~~~ = collector water average temperature, (°C)
+
+\emph{T\(_{a}\)}~~~~~~~ = ambient air temperature, (°C)
+
+\emph{m\(_{w}\)C\(_{pw}\)} = thermal capacity of the water mass in the collector, (J/°C)
+
+\emph{U\(_{s}\)}~~~~~~ = area-weighted conductance of the collector side insulation, (W/m\(^{2}\)×°K)
+
+\emph{U\(_{b}\)}~~~~~~ = conductance of the collector bottom insulation, (W/m\(^{2}\)×°K)
+
+\emph{T\(_{osc}\)}~~~~~ = ~~~ outside temperature of bottom insulation determined from the other side condition model, (°C)
+
+\emph{T\(_{wi}\)}~~~~~~ = Entering makeup or mains water temperature, (°C)
+
+\({\dot m_w}{C_w}\) = water capacity flow through the collector, (W/°C)
+
+The other side condition model boundary condition represented by the \emph{T\(_{osc}\)}, allows us to apply a realistic outside boundary condition for a collector mounted on a building roof.~ This also accounts for the shading impact of the collector on the under-laying surface (roof).~ On the other hand if ambient air boundary condition is specified, then the collector does not shade the underlying surface it is mounted on.
+
+The two energy balance equation can be written as non-homogeneous first order DE with constant coefficients. The initial conditions for these equations are the absorber plate average temperature and the collector water average temperature at previous time steps.
+
+\begin{equation}
+\frac{{d{T_p}}}{{dt}} = {a_1}{T_p} + {a_2}{T_w} + {a_3}
+\end{equation}
+
+\begin{equation}
+\frac{{d{T_w}}}{{dt}} = {b_1}{T_p} + {b_2}{T_w} + {b_3}
+\end{equation}
+
+\begin{equation}
+{a_1} =  - \left( {A \cdot {h_{pw}} + A \cdot {U_t}} \right)/\left( {{m_p} \cdot {C_p}} \right)
+\end{equation}
+
+\begin{equation}
+{a_2} = A \cdot {h_{pw}}{T_w}/\left( {{m_p} \cdot {C_p}} \right)
+\end{equation}
+
+\begin{equation}
+{a_3} = A \cdot {\left( {\tau \alpha } \right)_e} \cdot {I_t} + A \cdot {U_t}{T_a}
+\end{equation}
+
+\begin{equation}
+{b_1} = A \cdot {h_{pw}}{T_p}/\left( {{m_w} \cdot {C_w}} \right)
+\end{equation}
+
+\begin{equation}
+{b_2} =  - \left( {A \cdot {h_{pw}} + A \cdot {U_b} + A \cdot {U_s} + {{\dot m}_w}{C_w}} \right)
+\end{equation}
+
+\begin{equation}
+{{\rm{b}}_{\rm{3}}} = {\rm{ }}\left( {A \cdot {U_b}{T_{osc}} + A \cdot {U_s}{T_a} + {{\dot m}_w}{C_w}{T_{wi}}} \right)
+\end{equation}
+
+The two coupled first order differential equation are solved analytically.~ Auxiliary equation of the the coupled homogeneous differential equation is given by:
+
+\begin{equation}
+{\lambda ^2} - ({a_1} + {b_2}) + ({a_1}{b_2} - {a_2}{b_1}) = 0
+\end{equation}
+
+This auxiliary quadratic equation has always two distinct real roots (l\(_{1}\) and l\(_{2}\)) hence the solution of the homogeneous equation is exponential, and the general solutions of the differential equations are given by:
+
+\begin{equation}
+{T_p} =  {c_1}{e^{{l_1}t}} + {c_2}{e^{{l_2}t}} + A
+\end{equation}
+
+\begin{equation}
+{T_w} =  {r_1}{c_1}{e^{{l_1}t}} + {r_2}{c_2}{e^{{l_2}t}} + B
+\end{equation}
+
+The constant terms \emph{A} and \emph{B} are the particular solution of the non-homogeneous differential equations, the coefficients of the exponential terms (\emph{c\(_{1}\)}, \emph{c\(_{2}\)}, \emph{r\(_{1}\)}, and \emph{r\(_{2}\)}) are determined from the initial conditions of the absorber and collector water temperatures (\emph{T\(_{p0}\)}, \emph{T\(_{w0}\)}) and are given by:
+
+\begin{equation}
+{r_1} =  ({l_1} - {a_1})/{a_2};\quad {r_2} =  ({l_2} - {a_1})/{a_2}
+\end{equation}
+
+\begin{equation}
+A =  ( - {a_3}{b_2} + {b_3}{a_2})/({a_1}{b_2} - {b_1}{a_2});\quad B =  ( - {a_1}{b_3} + {b_1}{a_3})/({a_1}{b_2} - {b_1}{a_2})
+\end{equation}
+
+\begin{equation}
+{c_1} =  ({r_2}{T_{p0}} - {T_{w0}} - {r_2}A + B)/({r_2} - {r_1});\quad {c_2} =  ({T_{w0}} - {r_1}{T_{p0}} + {r_1}A - B)/({r_2} - {r_1})
+\end{equation}
+
+\subsubsection{Thermal Network Model:}\label{thermal-network-model}
+
+The thermal network model requires energy balance for each of the collector covers as well.~ The heat balance equation of the collector covers is assumed to obey steady state formulation by ignoring their thermal mass. The thermal-network representation of the ICS collector is shown in Figure~\ref{fig:thermal-network-diagram-for-ics-solar}. Also, the heat balance at each cover surface requires knowledge of the amount of solar fraction absorbed, which is determined from the ray tracing analysis. For the thermal network model shown above the overall top heat loss coefficient is determined from combination of the resistances in series as follows:
+
+\begin{equation}
+{U_t} = {\left[ {{R_1} + {R_2} + {R_3}} \right]^{ - 1}}
+\end{equation}
+
+Or
+
+\begin{equation}
+{U_t} = {\left[ {\frac{1}{{{h_{c,\,c1 - a}} + {h_{r,\,c1 - a}}}} + \frac{1}{{{h_{c,\,c2 - c1}} + {h_{r,\,c2 - c1}}}} + \frac{1}{{{h_{c,\,p - c2}} + {h_{r,\,p - c2}}}}} \right]^{ - 1}}
+\end{equation}
+
+The convection and radiation heat transfer coefficients in equation above are calculated based on temperatures at the previous time step and determined as described in the \emph{Heat Transfer Coefficients} section.
+
+\begin{figure}[hbtp] % fig 296
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6522.png}
+\caption{Thermal network diagram for ICS Solar Collector \protect \label{fig:thermal-network-diagram-for-ics-solar}}
+\end{figure}
+
+\textbf{\emph{Collector Cover Heat Balance}}
+
+Ignoring the thermal mass of the collector cover, a steady state heat balance equations are formulated for each cover that allow us to determine cover temperatures.~ The cover surface heat balance representation is shown in Figure~\ref{fig:collector-cover-surface-heat-balance} below.
+
+\begin{figure}[hbtp] % fig 297
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6523.png}
+\caption{Collector Cover Surface Heat Balance \protect \label{fig:collector-cover-surface-heat-balance}}
+\end{figure}
+
+The steady state cover heat balance equation is given by:
+
+\begin{equation}
+{q_{LWR,{\kern 1pt} 1}} + {q_{CONV,{\kern 1pt} 1}} + {q_{solar,{\kern 1pt} abs}} + {q_{LWR,{\kern 1pt} 2}} + {q_{CONV,{\kern 1pt} 2}} = 0
+\end{equation}
+
+Linearizing the longwave radiation exchange and representing the convection terms using the classical equation for Newton's law of cooling, the equations for the temperatures of covers 1 and 2 are given by:
+
+\begin{equation}
+{T_{c{\rm{1}}}} = \frac{{{\alpha_{c1}}{I_t} + {h_{r,{\kern 1pt} c1 - a}}{T_a} + {h_{c,{\kern 1pt} c1 - a}}{T_a} + {h_{r,{\kern 1pt} c2 - c1}}{T_{c2}} + {h_{c,{\kern 1pt} c2 - c1}}{T_{c2}}}}{{{h_{r,{\kern 1pt} c1 - a}} + {h_{c,{\kern 1pt} c1 - a}} + {h_{r,{\kern 1pt} c2 - c1}} + {h_{c,{\kern 1pt} c2 - c1}}}}
+\end{equation}
+
+\begin{equation}
+{T_{c2}} = \frac{{{\alpha_{c2}}{I_t} + {h_{r,{\kern 1pt} c2 - c1}}{T_{c1}} + {h_{c,{\kern 1pt} c2 - c1}}{T_{c1}} + {h_{r,{\kern 1pt} p - c2}}{T_p} + {h_{c,{\kern 1pt} p - c2}}{T_p}}}{{{h_{r,{\kern 1pt} c2 - c1}} + {h_{c,{\kern 1pt} c2 - c1}} + {h_{r,{\kern 1pt} p - c2}} + {h_{c,{\kern 1pt} p - c2}}}}
+\end{equation}
+
+Where,
+
+\emph{a\(_{c}\)} ~ = the weighted average solar absorptance of covers \emph{1} and \emph{2}, (-)
+
+\emph{h\(_{r,c1-a}\)}~~~~~~~~~~ = adjusted radiation heat transfer coefficient between cover \emph{1} and the ambient air, (W/m\(^{2}\)×K)
+
+\emph{h\(_{c,c1-a}\)}~~~~~~~~~~ = convection heat transfer coefficient between cover \emph{1} and the ambient, (W/m\(^{2}\)×K)
+
+\emph{h\(_{r,c2-c1}\)}~~~~~~~~~ = radiation heat transfer coefficient between covers \emph{1} and \emph{2}, (W/m\(^{2}\)×K)
+
+\emph{h\(_{c,c2-c1}\)}~~~~~~~~~ = convection heat transfer coefficient between covers \emph{1} and \emph{2}, (W/m\(^{2}\)×K)
+
+\emph{h\(_{r,p-c2}\)}~~~~~~~~~~ = radiation heat transfer coefficient between covers \emph{2} and the absorber plate, (W/m\(^{2}\)×K)
+
+\emph{h\(_{c,p-c2}\)}~~~~~~~~~~ = convection heat transfer coefficient between covers \emph{2} and the absorber plate, (W/m\(^{2}\)×K)
+
+\emph{q\(_{LWR,1}\)}~~~~~~~~~ = longwave radiation exchange flux on side \emph{1} of the collector cover, (W/m\(^{2}\))
+
+\emph{q\(_{CONV,1}\)}~~~~~~~~ = convection heat flux on side \emph{1} of the collector cover, (W/m\(^{2}\))
+
+\emph{q\(_{LWR,2}\)}~~~~~~~~~ = longwave radiation exchange flux on side \emph{2} of the collector cover, (W/m\(^{2}\))
+
+\emph{q\(_{CONV,2}\)}~~~~~~~~ = convection heat flux on side \emph{2} of the collector cover, (W/m\(^{2}\))
+
+\emph{q\(_{solar,abs}\)}~~~~~~~~ = net solar radiation absorbed by the collector cover, (W/m\(^{2}\))
+
+\emph{R}~~~ = thermal resistance for each section along the heat flow path, (m\(^{2}\)K/W)
+
+\subsubsection{Other Side Condition Model}\label{other-side-condition-model}
+
+ICS Solar Collectors are commonly mounted on building heat transfer surfaces hence the collectors shade the underlying heat transfer surface and require a unique boundary condition that reflects the air cavity environment created between the bottom of the collector surface and the underlying surface. The other side condition model that allows us to estimate the other side temperature, \emph{T\(_{osc}\)}, can be determined based on steady state heat balance using the known collector water temperature at the previous time step.
+
+\begin{figure}[hbtp] % fig 298
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6527.png}
+\caption{Illustration for Other Side Condition Model \protect \label{fig:illustration-for-other-side-condition-model}}
+\end{figure}
+
+Ignoring thermal mass of the collector bottom insulation, steady state surface heat balance can be formulated on the outer plane of the collector bottom surface facing the cavity as shown in Figure~\ref{fig:schematic-of-simultaneous-solution-scheme}.~ The heat balance equation on the outer plane of the collector bottom surface is given by:
+
+\begin{equation}
+{q_{cond}} + {q_{conv,{\kern 1pt} cav}} + {q_{rad,{\kern 1pt} cav}} = 0
+\end{equation}
+
+Substituting the equations for each term in the above equation yields:
+
+\begin{equation}
+{U_L}\left( {{T_w} - {T_{osc}}} \right) + {h_{c,{\kern 1pt} cav}}\left( {{T_{a,{\kern 1pt} cav}} - {T_{osc}}} \right) + {h_{r,{\kern 1pt} cav}}\left( {{T_{so}} - {T_{osc}}} \right) = 0
+\end{equation}
+
+Simplifying yields the bottom insulation other side condition temperature:
+
+\begin{equation}
+{T_{osc}} = \frac{{{U_L}{T_w} + {h_{c,{\kern 1pt} cav}}{T_{a,{\kern 1pt} cav}} + {h_{r,{\kern 1pt} cav}}{T_{so}}}}{{{U_L} + {h_{c,{\kern 1pt} cav}} + {h_{r,{\kern 1pt} cav}}}}
+\end{equation}
+
+The cavity air temperature is determined from cavity air heat balance as follows:
+
+\begin{equation}
+{T_{a,{\kern 1pt} cav}} = \frac{{{h_{c,{\kern 1pt} cav}}A{T_{osc}} + {{\dot m}_{vent}}Cp{T_a} + {h_{c,{\kern 1pt} cav}}A{T_{so}}}}{{{h_{c,{\kern 1pt} cav}}A + {{\dot m}_{vent}}Cp + {h_{c,{\kern 1pt} cav}}A}}
+\end{equation}
+
+Where
+
+\emph{h\(_{r,\, cav}\)}~~~~~~~~~~~ = linearized radiation coefficient for underlying surface in the cavity, (W/m\(^{2}\)×K)
+
+\emph{h\(_{c,\, cav}\)}~~~~~~~~~~ = convection coefficient for underlying surface in the cavity, (W/m\(^{2}\)×K)
+
+\emph{T\(_{so}\)} ~ = the outside face temperature of the underlying heat transfer surface, (ºC)
+
+\({\dot m_{vent}}\) ~~~~~~~~~ = air mass flow rate due to natural ventilation, (kg/s)
+
+\emph{q\(_{cond}\)}~~~~~~~~~~~ = conduction heat flux though the insulation bottom and, (W/m\(^{2}\))
+
+\emph{q\(_{conv,cav}\)}~~~~~~~~ = convection heat flux between the collector bottom outside surface and the cavity air, (W/m\(^{2}\))
+
+\emph{q\(_{rad,cav}\)}~~~~~~~~~ = ~~~~~~~~~ longwave radiation exchange flux between the collector bottom outside surface and the outside surface of the underlying surface, (W/m\(^{2}\))
+
+The cavity air temperature is determined from the cavity air energy balance.~ The air heat balance requires the ventilated cavity air natural ventilation rates.~ The calculation of the ventilation rate is described else where in this document. The SurfaceProperty:ExteriorNaturalVentedCavity, object is required to describe the surface properties, the characteristics of the cavity and opening for natural ventilation.
+
+\subsubsection{Heat Transfer Coefficients}\label{heat-transfer-coefficients}
+
+The equations used to determine for the various heat transfer coefficients in the absorber and water heat balance equations are given below. The absorbed solar energy is transferred to the water by convection.~ Assuming natural convection dominated heat transfer for a hot surface facing down and a clod surface facing down the following correlation for Nusselt number by Fujii and Imura (1972).~ The Nusselt number for hot surface facing down ward is given by:
+
+\begin{equation}
+Nu = 0.56{\left( {Gr \cdot \Pr  \cdot cos{\kern 1pt} \theta } \right)^{1/5}}\quad {10^5} < Gr \cdot Pr < {10^{11}}
+\end{equation}
+
+The Nusselt number for hot surface upward and cold surface facing down is given by:
+
+\begin{equation}
+Nu = 0.13{\left( {Gr \cdot \Pr } \right)^{1/3}}\quad Gr \cdot Pr < 5.0 \times {10^8}
+\end{equation}
+
+\begin{equation}
+Nu = 0.16{\left( {Gr \cdot \Pr } \right)^{1/3}}\quad Gr \cdot Pr > 5.0 \times {10^8}
+\end{equation}
+
+\begin{equation}
+Gr = {{g{\beta_{\rm{v}}}\left( {{T_p} - {T_w}} \right)L_c^3} \mathord{\left/ {\vphantom {{g{\beta_{\rm{v}}}\left( {{T_p} - {T_w}} \right)L_c^3} {{\nu ^2}}}} \right. } {{\nu ^2}}}
+\end{equation}
+
+\begin{equation}
+\Pr  = {\nu  \mathord{\left/ {\vphantom {\nu  \alpha }} \right. } \alpha }
+\end{equation}
+
+\begin{equation}
+{T_r} = {T_p} - 0.25\left( {{T_p} - {T_w}} \right)
+\end{equation}
+
+\begin{equation}
+{h_w} = {{Nu \cdot k} \mathord{\left/ {\vphantom {{Nu \cdot k} {{L_c}}}} \right. } {{L_c}}}
+\end{equation}
+
+Where,
+
+\(\theta\) = angle of inclination of the collector to the vertical, radians
+
+\emph{g} ~~ = gravitation force constant, 9.806 (m/s\(^{2}\))
+
+\emph{T\(_{r}\)}~~ = reference properties where the thermo-physical properties are calculated, (°C)
+
+\emph{L\(_{c}\)}~~ = characteristic length for the absorber plate, (m)
+
+\emph{k}~~~ = thermal conductivity of water at reference temperature, (W/m×K)
+
+\emph{n}~~~ = kinematic viscosity of water at reference temperature, (m\(^{2}\)/s)
+
+\emph{a}~~~ = thermal diffusivity of water at reference temperature, (m\(^{2}\)/s)
+
+\emph{β\(_{v}\)}~~ = volumetric expansion coefficient evaluated at Tv, Tv = Tw+0.25(Tp-Tw), (K-1)
+
+\emph{Nu}~ = Nusselt number calculated for water properties at the reference temperature, (-)
+
+\emph{Gr}~~ = Grashof number calculated for water properties at the reference temperature, (-)
+
+\emph{Pr}~~ = Prandtle number calculated for water properties at the reference temperature, (-)
+
+The various radiation and convection heat transfer coefficients are given by the following equations.~ The convection heat transfer coefficients between the covers and the absorber plate are estimated from the empirical correlation for the Nusselt number for air gap between two parallel plates developed by Hollands et al. (1976) is:
+
+\begin{equation}
+N{u_a} = 1 + 1.44\left\{ {1 - \frac{{1708{{\left( {\sin 1.8\beta } \right)}^{1.6}}}}{{Ra\cos \beta }}} \right\}{\left\{ {1 - \frac{{1708}}{{Ra\cos \beta }}} \right\}^ + } + {\left\{ {{{\left( {\frac{{Ra\cos \beta }}{{5830}}} \right)}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}} - 1} \right\}^ + }
+\end{equation}
+
+\begin{equation}
+{h_c} = {{Nu \cdot k} \mathord{\left/ {\vphantom {{Nu \cdot k} L}} \right. } L}
+\end{equation}
+
+\begin{equation}
+{h_{rp - c2}} = \frac{{\sigma \left( {{T_p} + {T_{c2}}} \right)\left( {T_p^2 + T_{c2}^2} \right)}}{{1/{\varepsilon_p} + 1/{\varepsilon_{c2}} - 1}}
+\end{equation}
+
+\begin{equation}
+{h_{rc1 - c2}} = \frac{{\sigma \left( {{T_{c1}} + {T_{c2}}} \right)\left( {T_{c1}^2 + T_{c2}^2} \right)}}{{1/{\varepsilon_{c1}} + 1/{\varepsilon_{c2}} - 1}}
+\end{equation}
+
+The long wave radiation exchange coefficients between the outer collector cover and the sky and ground referencing the ambient air temperature for mathematical simplification are given.
+
+\begin{equation}
+{h_{rc1 - s}} = \frac{{{F_s}{\varepsilon_{c1}}\sigma \left( {{T_{c1}} + {T_s}} \right)\left( {T_{c1}^2 + T_s^2} \right)\left( {{T_{c1}} - {T_s}} \right)}}{{\left( {{T_{c1}} - {T_a}} \right)}}
+\end{equation}
+
+\begin{equation}
+{h_{rc1 - g}} = \frac{{{F_g}{\varepsilon_{c1}}\sigma \left( {{T_{c1}} + {T_g}} \right)\left( {T_{c1}^2 + T_g^2} \right)\left( {{T_{c1}} - {T_g}} \right)}}{{\left( {{T_{c1}} - {T_a}} \right)}}
+\end{equation}
+
+\begin{equation}
+{h_{cc1 - a}} = {h_{cc1 - s}} + {h_{cc1 - g}}
+\end{equation}
+
+The convection heat transfer coefficient from the outer cover to the surrounding air is given by:
+
+\begin{equation}
+{h_{cc1 - a}} = 2.8 + 3.0{V_w}
+\end{equation}
+
+When the bottom surface boundary condition is AmbientAir, the combined conductance from the outer cover to the surrounding is calculated from the equation below (Duffie and Beckman, 1991).
+
+\begin{equation}
+{h_{comb}} = 5.7 + 3.8{V_w}
+\end{equation}
+
+The overall loss coefficient through the bottom and side of the collector-storage is estimated as follows:
+
+\begin{equation}
+{U_b} = {U_{Lb}}\left( {{A_b}/A} \right)
+\end{equation}
+
+\begin{equation}
+{U_s} = {\left[ {\frac{1}{{{U_{Ls}}\left( {{A_s}/A} \right)}} + \frac{1}{{{h_{comb}}}}} \right]^{ - 1}}
+\end{equation}
+
+Where,
+
+\emph{e\(_{c1}\)} ~ = thermal emissivity of collector cover \emph{1}, (-)
+
+\emph{e\(_{c2}\)} ~ = thermal emissivity of collector cover \emph{2}, (-)
+
+\emph{F\(_{s}\)} ~ = view factor from the collector to the sky, (-)
+
+\emph{F\(_{g}\)} ~ = view factor from the collector to the ground, (-)
+
+\emph{T\(_{c1}\)} = temperature of collector cover \emph{1}, (K)
+
+\emph{T\(_{c2}\)} = temperature of collector cover \emph{2}, (K)
+
+\emph{T\(_{s}\)} ~ = sky temperature, (K)
+
+\emph{T\(_{g}\)}~~ = ground temperature, (K)
+
+\emph{k} ~~ = thermal conductivity of air, (W/m K)
+
+\emph{L} ~~ = air gap between the covers, (m)
+
+\emph{β} ~~ = inclination of the plates or covers to the horizontal, (radian)
+
+\emph{V\(_{w}\)} = wind speed, (m/s)
+
+\emph{U\(_{Lb}\)}~ = user specified bottom heat loss conductance, W/m\(^{2}\)×K
+
+\emph{U\(_{Ls}\)}~ = user specified side heat loss conductance, W/m\(^{2}\)×K
+
+\emph{A\(_{b}\)}~~ = collector bottom heat transfer area, m\(^{2}\)
+
+\emph{A\(_{s}\)}~~ = collector side area, m\(^{2}\)
+
+\emph{h\(_{comb}\)}~~~~~~~~~~~ = combined conductance from the outer cover to the ambient air, W/m\(^{2}\)×K
+
+\textbf{\emph{Transmittance-Absorptance Product}}
+
+The transmittance-absorptance product of solar collector is determined using ray tracing method for any incident angle (Duffie and Beckman, 1991).~ This requires optical properties of the cover and absorber materials and the the transmittance-absorptance product for any incident angle is given by:
+
+\begin{equation}
+{\left( {\tau \alpha } \right)_\theta } = \frac{{\tau \alpha }}{{1 - \left( {1 - \alpha } \right){\rho_d}}}
+\end{equation}
+
+The transmittance of the cover system for single and two cover are given by:
+
+\begin{equation}
+\tau  = \frac{1}{2}\left[ {{{\left( {\frac{{{\tau_1} \cdot {\tau_2}}}{{1 - {\rho_1}{\rho_2}}}} \right)}_ \bot } + {{\left( {\frac{{{\tau_1} \cdot {\tau_2}}}{{1 - {\rho_1}{\rho_2}}}} \right)}_\parallel }} \right]
+\end{equation}
+
+\begin{equation}
+\rho  = \frac{1}{2}\left[ {{{\left( {{\rho_1} + \frac{{\tau  \cdot {\rho_2} \cdot {\tau_1}}}{{{\tau_2}}}} \right)}_ \bot } + {{\left( {{\rho_1} + \frac{{\tau  \cdot {\rho_2} \cdot {\tau_1}}}{{{\tau_2}}}} \right)}_\parallel }} \right]
+\end{equation}
+
+The effective transmittance, reflectance and absorptance of a single cover are given by:
+
+\begin{equation}
+\tau  = \frac{{{\tau_a}}}{2}\left\{ {\frac{{1 - {r_ \bot }}}{{1 + {r_ \bot }}}\left[ {\frac{{1 - r_ \bot ^2}}{{1 - {{\left( {{r_ \bot }{\tau_a}} \right)}^2}}}} \right] + \frac{{1 - {r_\parallel }}}{{1 + {r_\parallel }}}\left[ {\frac{{1 - r_\parallel ^2}}{{1 - {{\left( {{r_\parallel }{\tau_a}} \right)}^2}}}} \right]} \right\}
+\end{equation}
+
+\begin{equation}
+\rho  = \frac{1}{2}\left\{ {\left[ {{r_ \bot } + \frac{{{{\left( {1 - {r_ \bot }} \right)}^2}\tau_a^2{r_ \bot }}}{{1 - {{\left( {{r_ \bot }{\tau_a}} \right)}^2}}}} \right] + \left[ {{r_\parallel } + \frac{{{{\left( {1 - {r_\parallel }} \right)}^2}\tau_a^2{r_\parallel }}}{{1 - {{\left( {{r_\parallel }{\tau_a}} \right)}^2}}}} \right]} \right\}
+\end{equation}
+
+\begin{equation}
+\alpha  = \frac{{\left( {1 - {\tau_a}} \right)}}{2}\left\{ {\left( {\frac{{1 - {r_ \bot }}}{{1 - {r_ \bot }{\tau_a}}}} \right) + \left( {\frac{{1 - {r_\parallel }}}{{1 - {r_\parallel }{\tau_a}}}} \right)} \right\}
+\end{equation}
+
+The transmittance of the cover system with absorption only considered \emph{t}\(_{a}\), is defined as:
+
+\begin{equation}
+{\tau_a} = \exp \left( { - \frac{{KL}}{{\cos \,{\theta_2}}}} \right)
+\end{equation}
+
+\begin{equation}
+{\theta_2} = {\sin ^{ - 1}}\left( {\sin {\theta_1} \cdot \frac{{{n_1}}}{{{n_2}}}} \right)
+\end{equation}
+
+The reflectance of un-polarized radiation on passing from medium 1 with reflective index \emph{n}\(_{1}\) to medium 2 with reflective index \emph{n}\(_{2}\) is given by:
+
+~\({r_ \bot } = \frac{{{{\sin }^2}\left( {{\theta_2} - {\theta_1}} \right)}}{{{{\sin }^2}\left( {{\theta_2} + {\theta_1}} \right)}}\)
+
+\begin{equation}
+{r_\parallel } = \frac{{{{\tan }^2}\left( {{\theta_2} - {\theta_1}} \right)}}{{{{\tan }^2}\left( {{\theta_2} + {\theta_1}} \right)}}
+\end{equation}
+
+The sky and ground reflected diffuse radiations average equivalent incident angles are approximated by Brandemuehl and Beckman correlation (Duffie and Beckman, 1991) as follows:
+
+\begin{equation}
+{\theta_{sd}} = 59.68 - 0.1388\beta  + 0.001497{\beta ^2}
+\end{equation}
+
+\begin{equation}
+{\theta_{gd}} = 90 - 0.5788\beta  + 0.002693{\beta ^2}
+\end{equation}
+
+where,
+
+\emph{t} ~~~ = transmittance of the cover system, (-)
+
+\emph{t}\(_{1}\) ~~ = transmittance of the cover 1, (-)
+
+\emph{t}\(_{2}\) ~~ = transmittance of the cover 2, (-)
+
+\emph{a} ~~ = absorptance of the absorber plate, (-)
+
+\emph{r}\(_{d}\) ~~ = diffuse reflectance of the inner cover, (-)
+
+\emph{L} ~~ = thickness of a cover material, (m)
+
+\emph{K} ~~ = extinction coefficient of a cover material, (m\(^{-1}\))
+
+\emph{q}\(_{1}\) ~ = angle of incidence, degree
+
+\emph{q}\(_{2}\) ~~ = angle of refraction, degree
+
+\({r_ \bot }\) ~ = parallel component of reflected un-polarized radiation, (-)
+
+\({r_\parallel }\) ~~ = perpendicular component of reflected un-polarized radiation, (-)
+
+\emph{b} ~~ = slope of the collector, degree
+
+\emph{q}\(_{sd}\) = equivalent incident angle for sky diffuse solar radiation, degree
+
+\emph{q}\(_{gd}\)~ = equivalent incident angle for ground diffuse solar radiation, degree
+
+The integral collector storage unit thermal performance parameters are calculated as follows:
+
+\begin{equation}
+{Q_{delivered}} = {\dot m_w}{C_w}\left( {{T_w} - {T_{wi}}} \right)
+\end{equation}
+
+\begin{equation}
+{Q_{Stored}} = {m_w}{C_w}\frac{{d{T_w}}}{{dt}}
+\end{equation}
+
+\begin{equation}
+{Q_{SkinLoss}} = A \cdot \left[ {{U_t}\left( {{T_p} - {T_w}} \right) + {U_b}\left( {{T_w} - {T_{OSC}}} \right) + {U_s}\left( {{T_w} - {T_a}} \right)} \right]
+\end{equation}
+
+\begin{equation}
+{\eta_{thermal}} = \frac{{{m_w}{C_w}\frac{{d{T_w}}}{{dt}} + {{\dot m}_w}{C_w}\left( {{T_w} - {T_{wi}}} \right)}}{{A \cdot {I_t}}}
+\end{equation}
+
+\subsection{References:}\label{references-1-016}
+
+Duffie, J.A., and W.A. Beckman. 1991. \emph{Solar Engineering of Thermal Processes,} 2d ed. New York: John Wiley \& Sons.
+
+Kumar, R. and M.A.~Rosen. Thermal performance of integrated collector storage solar water heater with corrugated absorber surface. Applied Thermal Engineering:~ 30 (2010) 1764--1768.
+
+Fujii, T., and H. Imura. Natural convection heat transfer from aplate with arbitrary inclination. International Journal of Heat and Mass Transfer: 15(4), (1972), 755-764.
+
+\subsection{Photovoltaic Thermal Flat-Plate Solar Collectors}\label{photovoltaic-thermal-flat-plate-solar-collectors}
+
+Photovoltaic-Thermal solar collectors (PVT) combine solar electric cells and thermal working fluid to collect both electricity and heat.~ Athough there are currently comparatively few commercial products, PVT research has been conducted for the past 30 years and many different types of collectors have been studied.~ Zondag (2008) and Charalambous et. al (2007) provide reviews of the PVT literature.~ Because PVT is much less commercially-mature, there are no standards or rating systems such as for thermal-only, hot-water collectors.~ EnergyPlus currently has one simple model based on user-defined efficiencies but a more detailed model based on first-principles and a detailed, layer-by-layer description is under development.
+
+The PVT models reuse the PV models for electrical production. These are described elsewhere in this document in the section on Photovoltaic Arrays-Simple Model
+
+\subsubsection{Simple PVT Thermal Model}\label{simple-pvt-thermal-model}
+
+The input object SolarCollector:FlatPlate:PhotovoltaicThermal provides a simple PVT model that is provided for quick use during design or policy studies.~ The user simply provides values for a thermal efficiency and the incident solar heats the working fuild.~ The model also includes a cooling mode for air-based systems where a user-provided surface emmittance is used to model cooling of the working fluid to the night sky (water-based cooling will be made available once a chilled water storage tank is available).~ No other details of the PVT collector's construction are required as input data.
+
+The simple model can heat either air or liquid.~ If it heats air, then the PVT is part of HVAC air system loop with air nodes connected to an air system.~ If it heats liquid, then the PVT is part of plant loop with nodes connected to a plant loop and the plant operating scheme determines flows.
+
+Air-system-based PVT modeling include a modulating bypass damper arrangement.~ Control logic decides if the air should bypass the collector to better meet setpoint.~ The model requires a drybulb temperature setpoint be placed on the outlet node.~ The model assume the collector is intended and available for heating when the incident solar is greater than 0.3 W/m\(^{2}\) and otherwise it is intended for cooling.~ The inlet temperature is compare to the setpoint on the outlet node to determine if cooling or heating are beneficial.~ If they are, then the PVT thermal models are applied to condition the air stream.~ If they are not beneficial, then the PVT is completely bypassed and the inlet node is passed directly to the outlet node to model a completely bypassed damper arrangement.~ A report variable is available for bypass damper status.
+
+Plant-based PVT do not include a bypass (although one could be used in the plant loop).~ The collector requests its design flow rate but it otherwise relies on the larger plant loop for control.
+
+When the PVT themal collector is controlled to be ``on,'' in heating mode, and working fluid is flowing, the model calculates the outlet temperature based on the inlet temperature and the collected heat using the following equations.
+
+\begin{equation}
+{Q_{therm}} = {A_{surf}} \cdot {f_{activ}} \cdot {G_T} \cdot {\eta_{thermal}}
+\end{equation}
+
+where,
+
+\({Q_{therm}}\) ~is the thermal energy collected {[}W{]}
+
+\({A_{surf}}\) ~is the net area of the surface {[}m\(^{2}\){]}
+
+\({f_{activ}}\) is the fraction of surface aire with active PV/T collector, and
+
+\({\eta_{thermal}}\) is the thermal conversion efficiency.
+
+\begin{equation}
+{T_{out}} = {T_{in}} + \frac{{{Q_{therm}}}}{{\dot m{c_p}}}
+\end{equation}
+
+where,
+
+\({T_{out}}\) ~is the temperature of the working fluid leaving the PV/T
+
+\({T_{in}}\) ~is the temperature of the working fluid entering the PV/T
+
+\(\dot m\) ~is the entire mass flow of the working fluid through the PV/T
+
+\({c_p}\) ~is the specific heat of the working fluid.
+
+For air-based systems, the value of \({T_{out}}\) is then compared to the temperature setpoint on the outlet node.~ If \({T_{out}}\) ~exceeds the desired outlet temperature, \({T_{set,out}}\) ,then a bypass fraction is calculated to model a modulating bypass damper using:
+
+\begin{equation}
+{f_{bypass}} = \frac{{\left( {{T_{set,out}} - {T_{out}}} \right)}}{{\left( {{T_{in}} - {T_{out}}} \right)}}
+\end{equation}
+
+When the PVT themal collector is controlled to be ``on,'' in cooling mode, and working fluid is flowing, the model calculates the outlet temperature based on the inlet temperature and the heat radiated and convected to the ambient using a heat balance on the outside face of the collector:
+
+\begin{equation}
+\dot m{c_p}\left( {{T_{in}} - {T_{out}}} \right) = {\dot Q_{LWR}} + {\dot Q_{conv}}
+\end{equation}
+
+Where,
+
+\({\dot Q_{LWR}}\) ~is the net rate of long wavelength (thermal) radiation exchange with the air, night sky, and ground.~ See the section ``External Longwave Radiation'' in the Outside Surface Heat Balance, for full discussion of how this modeled in EnergyPlus using linearized radiation coefficients.
+
+\({\dot Q_{conv}}\) ~is the net rate of convective flux exchange with outdoor air. See the section ``Exterior/External Convection'' in the Outside Surface Heat Balance, for full discussion of how this modeled in EnergyPlus.~ The surface roughness is assumed to be ``very smooth.''
+
+The simple model assumes that the effective collector temperature, \({T_{col}}\) , is the average of the working fluid inlet and outlet temperatures so that we can make the following substitution:
+
+\begin{equation}
+{T_{out}} = 2{T_{col}} - {T_{in}}
+\end{equation}
+
+Substituting and solving for \({T_{col}}\) ~we obtain the following model for collector temperatures during a (possible) cooling process :
+
+\begin{equation}
+{T_{col}} = \frac{{2\dot m{c_p}{T_{in}} + {A_{surf}}{f_{activ}}\left( {{h_{r,gnd}}{T_{gnd}} + {h_{r,sky}}{T_{sky}} + {h_{r,air}}{T_{air}} + {h_{c,ext}}{T_{air}}} \right)}}{{2\dot m{c_p} + {A_{surf}}{f_{activ}}\left( {{h_{r,gnd}} + {h_{r,sky}} + {h_{r,air}} + {h_{c,ext}}} \right)}}
+\end{equation}
+
+Then the outlet temperature can be calculated and heat losses determined.~ However, the model allows only sensible cooling of the air stream and limits the outlet temperature to not go below the dewpoint temperature of the inlet.
+
+PVT collectors have a design volume flow rate for the working fluid that is autosizable.~ For air-based systems used as pre-conditioners, the volume flow rate is sized to meet the maximum outdoor air flow rate.~ For water-based systems on the supply side of a plant loop, each of the PVT collectors are sized to the overall loop flow rate.~ For water-based systems on the demand side of a plant loop, the collectors are sized using a rule-of-thumb for typical flow rates per unit of collector area.~ This rule-of-thumb is based on a constant factor of 1.905x10\(^{-5}\) m\(^{3}\)/s-m\(^{2}\) that was developed by analyzing SRCC data set for conventional solar collectors (see data set SolarCollectors.idf) and averaging the ratio for all 171 different collectors.
+
+\subsubsection{References}\label{references-2-008}
+
+Charalambous, P.G., Maidment, G.G., Kalagirou, S.A., and Yiakoumetti, K., Photovoltaic thermal (PV/T) collectors: A review. Applied Thermal Engineering 27 (2007) 275-286.
+
+Zondag, H.A. 2008. Flat-plate PV-Thermal collectors and systems: A review.~ Renewable and Sustainable Energy Reviews 12 (2008) 891-959.
+
+\subsection{Unglazed Transpired Solar Collectors}\label{unglazed-transpired-solar-collectors}
+
+The input object SolarCollector:UnglazedTranspired provides a model for transpired collectors that are perhaps one of the most efficient ways to collect solar energy with demonstrated instantaneous efficiencies of over 90\% and average efficiencies of over 70\%.~ They are used for preheating outdoor air needed for ventilation and processes such as crop drying.
+
+In EnergyPlus, an unglazed transpired solar collector (UTSC) is modeled as a special component attached to the outside face of a heat transfer surface that is also connected to the outdoor air path.~ A UTSC affects both the thermal envelope and the HVAC air system.~ From the air system's point of view, a UTSC is heat exchanger and the modeling needs to determine how much the device raises the temperature of the outdoor air.~ From the thermal envelope's point of view, the presence of the collector on the outside of the surface modifies the conditions experienced by the underlying heat transfer surfaces.~ EnergyPlus models building performance throughout the year and the UTSC will often be ``off'' in terms of forced airflow, but the collector is still present.~ When the UTSC is ``on'' there is suction airflow that is assumed to be uniform across the face.~ When the UTSC is ``off'' the collector acts as a radiation and convection baffle situated between the exterior environment and the outside face of the underlying heat transfer surface.~ We distinguish these two modes of operation as \emph{active} or \emph{passive} and model the UTSC component differently depending on which of these modes it is in.
+
+\subsubsection{Heat Exchanger Effectiveness}\label{heat-exchanger-effectiveness}
+
+The perforated absorber plate is treated as a heat exchanger and modeled using a traditional effectiveness formulation.~ The heat exchanger effectiveness, \({\varepsilon_{HX}}\) , is determined from correlations derived from small-scale experiments.~ Two correlations available in the literature are implemented in EnergyPlus.~ The first is based on research by Kutscher at the National Renewable Energy Laboratory. The second is based on the research by Van Decker, Hollands, and Brunger at the University of Waterloo.~ Because both correlations are considered valid, the choice of which correlation to use is left to the user.
+
+\subsubsection{Kutscher Correlation}\label{kutscher-correlation}
+
+Kutscher's (1994) correlation encompasses surface convection between the collector and the incoming outdoor air stream that occurs on the front face, in the holes, and along the back face of the collector. The correlation uses a Reynolds number based on the hole diameter as a length scale and the mean velocity of air as it passes through the holes as the velocity scale:
+
+\begin{equation}
+{{\mathop{\rm Re}\nolimits}_D} = \frac{{{V_h}D}}{\nu }
+\end{equation}
+
+where,
+
+~~~~~ \({V_h}\) ~is the velocity through the holes {[}m/s{]}
+
+~~~~~ \(D\) ~is the hole diameter {[}m{]}
+
+~~~~~ \(\nu\) ~is the kinematic viscosity of air~ {[}m\(^{2}\)/s{]}
+
+The correlation is a function of Reynolds number, hole geometry, the free stream air velocity, and velocity through the holes:
+
+\begin{equation}
+N{u_D} = 2.75\left[ {{{\left( {\frac{P}{D}} \right)}^{ - 1.2}}{\mathop{\rm Re}\nolimits}_D^{0.43} + 0.011\sigma {{{\mathop{\rm Re}\nolimits} }_D}{{\left( {\frac{{{U_\infty }}}{{{V_h}}}} \right)}^{0.48}}} \right]
+\end{equation}
+
+where,
+
+~~~~~ \(P\) ~is the pitch, or distance between holes, {[}m{]},
+
+~~~~~ \(D\) ~is the diameter of the holes, {[}m{]},
+
+~~~~~ \(\sigma\) ~is the porosity, or area fraction of the holes, {[}dimensionless{]},
+
+~~~~~ \({V_h}\) ~is the mean velocity of air passing through the holes, {[}m/s{]},
+
+~~~~~ \({U_\infty }\) ~is the free stream velocity (local wind speed) {[}m/s{]}.
+
+The Nusselt number is formulated as:
+
+\begin{equation}
+N{u_D} = \frac{{U\;D}}{k}
+\end{equation}
+
+where,
+
+~~~~~ \(U\) is the overall heat transfer coefficient based on log mean temperature difference, {[}W/m\(^{2}\)·K{]}, and
+
+~~~~~ \(k\) ~is the thermal conductivity of air {[}W/m·K{]}.
+
+The heat exchanger effectiveness is:
+
+\begin{equation}
+{\varepsilon_{HX}} = 1 - {e^{\left[ { - \frac{{U\,A}}{{\dot m\,{c_p}}}} \right]}}
+\end{equation}
+
+Kutscher's relation was formulated for triangular hole layout, but based on Van Decker et al. (2001) we allow using the correlation for square hole layout and scale \(P\) ~by a factor of 1.6.
+
+\subsubsection{Van Decker, Hollands, and Brunger Correlation}\label{van-decker-hollands-and-brunger-correlation}
+
+Van Decker et. al. extended Kutscher's measurements to include a wider range of collector parameters including plate thickness, pitch, suction velocities, and square hole patterns.~ Their model formulation differs from Kutscher's in that the model was built up from separate effectiveness models for the front, back, and holes of the collector.~ Their published correlation is:
+
+\begin{equation}
+\begin{split}
+{\varepsilon_{HX}} =& \left[ {1 - \left( {1 + {{{\mathop{\rm Re}\nolimits} }_s}Max{{\left( {1.733{\mathop{\rm Re}\nolimits}_w^{ - {\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 2}}\right.}\!\lower0.7ex\hbox{2}}},0.02136} \right)}^{ - 1}}} \right)} \right] \times \left[ {1 - {{\left( {1 + 0.2273{\mathop{\rm Re}\nolimits}_b^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 2}}\right.}\!\lower0.7ex\hbox{2}}}} \right)}^{ - 1}}} \right] \\
+&\times {e^{\left( { - 0.01895\frac{P}{D} - \frac{{20.62}}{{{{{\mathop{\rm Re}\nolimits} }_D}}}\frac{t}{D}} \right)}}
+\end{split}
+\end{equation}
+
+where,
+
+~~~~~ \({{\mathop{\rm Re}\nolimits}_s} = \frac{{{V_s}P}}{v}\)
+
+~~~~~ \({{\mathop{\rm Re}\nolimits}_w} = \frac{{{U_\infty }P}}{v}\)
+
+~~~~~ \({{\mathop{\rm Re}\nolimits}_b} = \frac{{{V_h}P}}{v}\)
+
+~~~~~ \({V_s}\) ~is the average suction velocity across the front face of the collector {[}m/s{]}
+
+~~~~~ \(t\) ~is the collector plate thickness
+
+\subsubsection{Heat Exchanger Leaving Temperature}\label{heat-exchanger-leaving-temperature}
+
+Using either of the correlations above allows determining the heat exchanger effectiveness from known values.~ By definition the heat exchanger effectiveness is also:
+
+\begin{equation}
+{\varepsilon_{HX}} = \frac{{{T_{a,HX}} - {T_{amb}}}}{{{T_{s,coll}} - {T_{amb}}}}
+\end{equation}
+
+where,
+
+~~~~~ \({T_{{\rm{a,HX}}}}\) ~is the temperature of the air leaving the collector and entering the plenum {[}ºC{]}
+
+~~~~~ \({T_{s,coll}}\) ~is the temperature of the collector's absorber plate, {[}ºC{]}, and
+
+~~~~~ \({T_{amb}}\) ~is the temperature of the ambient outdoor air {[}ºC{]}.
+
+By rewriting equation to solve for \({T_{{\rm{a,HX}}}}\) ~we see that the temperature of the heated outdoor air entering the plenum can be determined once the collector surface temperature is known,
+
+\begin{equation}
+{T_{a,HX}} = {\varepsilon_{HX}}{T_{s,coll}} + \left( {1 - {\varepsilon_{HX}}} \right){T_{amb}}
+\end{equation}
+
+\subsubsection{Collector Heat Balance}\label{collector-heat-balance}
+
+The collector is assumed to be sufficiently thin and high-conductivity so that it can be modeled using a single temperature (for both sides and along its area).~ This temperature \({T_{s,coll}}\) is determined by formulating a heat balance on a control volume that just encapsulates the collector surface.~ The heat balances are formulated separately for active and passive modes and are diagrammed in the following figure.
+
+Observe that for the passive case, we do not use the heat exchanger relations to directly model the interaction of ventilating air with the collector.~ This is because these relations are considered to not apply when the UTSC is in passive mode.~ They were developed for uni-directional flow (rather than the balanced-in-and-out flow expected from natural forces) and for specific ranges of suction face velocity.~ Therefore, this heat transfer mechanism is handled using classical surface convection models (as if the collector was not perforated).~ (Air exchanges are modeled as ventilation in the plenum air heat balance but do not interact with the hole edges in the collector surface.)
+
+\begin{figure}[hbtp] % fig 299
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6620.png}
+\caption{Transpired Collector Heat Balance \protect \label{fig:transpired-collector-heat-balance}}
+\end{figure}
+
+When the UTSC is active, the heat balance on the collector surface control volume is:
+
+\begin{equation}
+{q''_{\alpha sol}} + {q''_{LWR,Env}} + {q''_{conv,wind}} - {q''_{HX}} + {q''_{LWR,plen}} + {q''_{source}} = 0
+\end{equation}
+
+where: \(q''_{\alpha sol}\) is absorbed direct and diffuse solar (short wavelength) radiation heat flux.
+
+\({q''_{LWR,Env}}\) is net long wavelength (thermal) radiation flux exchange with the air and surroundings.
+
+\({q''_{conv,wind}}\) is surface convection flux exchange with outdoor air under high wind and rain conditions.~ Note that this term is usually assumed to be zero in UTSC model development but we add the term to allow for deteriorated performance of the UTSC under poor conditions. \(q''_{HX}\) is heat exchanger flux from collector to incoming outdoor air. \(q''_{LWR,plen}\) is net long wavelength (thermal) radiation flux exchange with the outside face of the underlying surface(s).
+
+\({q''_{source}}\) is a source/sink term that accounts for energy exported out of the control volume when the collecter's absorber plate is a hybrid device such as a photovoltaic panel.
+
+While the heat balance on the passive collector surface control volume is:
+
+\begin{equation}
+{q''_{\alpha sol}} + {q''_{LWR,Env}} + {q''_{conv,Env}} + {q''_{LWR,plen}} + {q''_{conv,plen}} + {q''_{source}} = 0
+\end{equation}
+
+where: \(q''_{conv,Env}\) = surface convection flux exchange with outdoor air. \(q''_{conv,plen}\) = surface convection flux exchange with plenum air.
+
+All terms are positive for net flux to the collector except the heat exchanger term, which is taken to be positive in the direction from collector to incoming air stream.~ Each of these heat balance components is introduced briefly below.
+
+\subsubsection{External SW Radiation}\label{external-sw-radiation-000}
+
+\(q''_{\alpha sol}\) is calculated using procedures presented elsewhere in this manual and includes both direct and diffuse incident solar radiation absorbed by the surface face.~ This is influenced by location, surface facing angle and tilt, shading surfaces, surface face material properties, weather conditions, etc.
+
+\subsubsection{External LW Radiation}\label{external-lw-radiation-000}
+
+\({q''_{LWR,Env}}\) ~is a standard radiation exchange formulation between the surface, the sky, the ground, and the atmosphere.~ The radiation heat flux is calculated from the surface absorptivity, surface temperature, sky, air, and ground temperatures, and sky and ground view factors.~ Radiation is modeled using linearized coefficients.
+
+\subsubsection{External Convection}\label{external-convection-000}
+
+\(q''_{conv,Env}\) is modeled using the classical formulation: \({q''_{conv}}\) ~ = h\(_{co}\)(T\(_{air}\) - T\(_{o}\)) where h\(_{co}\), is the convection coefficient.~ This coefficient will differ depending on whether or not the UTSC is active or passive.~ When the UTSC is passive, h\(_{co}\) is treated in the same way as an outside face with ExteriorEnvironment conditions.~ When the UTSC is active, the special suction airflow situation of a transpired collector during operation means that h\(_{co}\) is often zero because the suction situation can eliminate mass transport away from the collector.~ However when the winds are high, the strong turbulence and highly varying pressures can cause the suction flow situation to breakdown.~ Therefore, we include the \({q''_{conv,wind}}\) ~term in the heat balance and use a special coefficient \({h_{c,wind}}\) ~to model this lost heat transfer.~ In addition, when it is raining outside, we assume the collector gets wet and model the enhanced surface heat transfer using a large value for \({h_{c,wind}}\) .
+
+\subsubsection{Heat Exchanger}\label{heat-exchanger}
+
+\(q''_{HX}\) is modeled using the classical formulation \({q''_{HX}} = \frac{{\dot m{c_p}({T_{a,HX}} - {T_{amb}})}}{A}\) where \({T_{{\rm{a,HX}}}}\) ~is determined using correlations described above.~ When the UTSC is active, the air mass flow is determined from the operation of the outdoor air mixer component.~ When the UTSC is off, this term is zero.
+
+\subsubsection{Plenum LW Radation}\label{plenum-lw-radation}
+
+\({q''_{LWR,plen}}\) is a standard radiation exchange formulation between the collector surface and the underlying heat transfer surface located across the plenum.~ Radiation is modeled using linearized coefficients.
+
+\subsubsection{Plenum Convection}\label{plenum-convection}
+
+\(q''_{conv,plen}\) is modeled using the classical formulation: \({q''_{conv}}\) = h\(_{cp}\)(T\(_{air}\) - T\(_{o}\)) where h\(_{cp}\), is the convection coefficient.~ This coefficient is taken as zero when the UTSC is operating because of the suction airflow situation.~ When the UTSC is off, the value for h\(_{cp}\) is obtained from correlations used for window gaps from ISO (2003) standard 15099.
+
+Substituting models into and solving for \({T_{s,coll}}\) ~yields the following equation when the UTSC is active (``on''):
+
+{\scriptsize
+\begin{equation}
+{T_{s,coll}} = \frac{{\left( {{I_s}\alpha  + {h_{r,atm}}{T_{amb}} + {h_{r,sky}}{T_{sky}} + {h_{r,gnd}}{T_{amb}} + {h_{r,plen}}{T_{so}} + {h_{c,wind}}{T_{amb}} + \frac{{\dot m{c_p}}}{A}{T_{amb}} - \frac{{\dot m{c_p}}}{A}\left( {1 - {\varepsilon_{HX}}} \right){T_{amb}} + {{q''}_{source}}} \right)}}{{\left( {{h_{r,atm}} + {h_{r,sky}} + {h_{r,gnd}} + {h_{r,plen}} + {h_{c,wind}} + \frac{{\dot m{c_p}}}{A}{\varepsilon_{HX}}} \right)}}
+\end{equation}}
+
+and substituting into yields the following equation when the UTSC is passive (``off''):
+
+\begin{equation}
+{T_{s,coll}} = \frac{{\left( {{I_s}\alpha  + {h_{co}}{T_{amb}} + {h_{r,atm}}{T_{amb}} + {h_{r,sky}}{T_{sky}} + {h_{r,gnd}}{T_{amb}} + {h_{r,plen}}{T_{so}} + {h_{c,plen}}{T_{a,plen}} + {{q''}_{source}}} \right)}}{{\left( {{h_{co}} + {h_{r,air}} + {h_{r,sky}} + {h_{r,gnd}} + {h_{r,plen}} + {h_{c,plen}}} \right)}}
+\end{equation}
+
+where,
+
+~~~~~ \({I_s}\) ~is the incident solar radiation of all types {[}W/m\(^{2}\){]},
+
+~~~~~ \(\alpha\) ~is the solar absorptivity of the collector {[}dimensionless{]},
+
+~~~~~ \({h_{r,atm}}\) is the linearized radiation coefficient for the surrounding atmosphere {[}W/m\(^{2}\)·K{]},
+
+~~~~~ \({T_{amb}}\) ~is the outdoor drybulb from the weather data, also assumed for ground surface {[}ºC{]},
+
+~~~~~ \({h_{r,sky}}\) ~is the linearized radiation coefficient for the sky {[}W/m\(^{2}\)·K{]},
+
+~~~~~ \({T_{sky}}\) ~is the effective sky temperature {[}ºC{]},
+
+~~~~~ \({h_{r,gnd}}\) ~is the linearized radiation coefficient for the ground {[}W/m\(^{2}\)·K{]},
+
+~~~~~ \({h_{r,plen}}\) ~is the linearized radiation coefficient for the underlying surface {[}W/m\(^{2}\)·K{]},
+
+~~~~~ \({h_{c,wind}}\) ~is the convection coefficient for the outdoor environment when the UTSC is active and winds are high or it is raining {[}W/m\(^{2}\)·K{]},
+
+~~~~~ \({T_{so}}\) ~is the temperature of the outside face of the underlying heat transfer surface {[}ºC{]},
+
+~~~~~ \(\dot m\) ~is the air mass flow rate when in active mode {[}kg/s{]},
+
+~~~~~ \({c_p}\) ~is the specific heat of air at constant pressure {[}J/kg·K{]},
+
+~~~~~ \(A\) ~is the area of the collector {[}m\(^{2}\){]},
+
+~~~~~ \({h_{co}}\) ~is the convection coefficient for the outdoor environment {[}W/m\(^{2}\)·K{]},
+
+~~~~~ \({h_{c,plen}}\) ~is the convection coefficient for the surfaces facing the plenum {[}W/m\(^{2}\)·K{]}, and
+
+~~~~~ \({T_{a,plen}}\) ~is the air drybulb for air in the plenum and entering the outdoor air system {[}ºC{]}.
+
+\subsubsection{Plenum Heat Balance}\label{plenum-heat-balance}
+
+The \emph{plenum} is the volume of air located between the collector and the underlying heat transfer surface.~ The plenum air is modeled as well-mixed.~ The uniform temperature of the plenum air, \({T_{a,plen}}\) , is determined by formulating a heat balance on a control volume of air as diagrammed below.
+
+Note that we have formulated the control volumes with slight differences for the active and passive cases.~ For the active case, the suction air situation and heat exchanger effectiveness formulations dictate that the collector surface control volume encompass part of the air adjacent to both the front and back surfaces of the collector.~ However for the passive case, the collector surface control volume has no air in it and the plenum air control volume extends all the way to the surface of the collector.
+
+\begin{figure}[hbtp] % fig 300
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6664.png}
+\caption{Transpired Collector Plenum Air Heat Balance \protect \label{fig:transpired-collector-plenum-air-heat-balance}}
+\end{figure}
+
+When the UTSC is active, the heat balance on the plenum air control volume is:
+
+\begin{equation}
+  \dot{Q}_{air} + \dot{Q}_{co} = 0
+\end{equation}
+
+where,
+
+\({\dot Q_{air}}\) is the net rate of energy added by suction air convecting through the control volume. \(\dot{Q}_{co}\) is the net rate of energy added by surface convection heat transfer with the underlying surface.
+
+When the UTSC is passive, the heat balance on the plenum air control volume is:
+
+\begin{equation}
+{\dot Q_{vent}} + {\dot Q_{co}} + {\dot Q_{c,coll}} = 0
+\end{equation}
+
+where,
+
+~~~~~ \({\dot Q_{vent}}\) ~is the net rate of energy added from infiltration -- where outdoor ambient air exchanges with the plenum air.
+
+~~~~~ \({\dot Q_{c,coll}}\) is the net rate of energy added by surface convection heat transfer with the collector.
+
+Substituting into and solving for \({T_{a,plen}}\) ~yields the following equation for when the UTSC is active:
+
+\begin{equation}
+{T_{a,plen}} = \frac{{\left( {\dot m{c_p}{T_{a,HX}} + {h_{c,plen}}A\,{T_{so}}} \right)}}{{\left( {\dot m{c_p} + {h_{c,plen}}A} \right)}}
+\end{equation}
+
+And substituting into yields the following equation when the UTSC is passive:
+
+\begin{equation}
+{T_{a,plen}} = \frac{{\left( {{h_{c,plen}}A\,{T_{so}} + {{\dot m}_{vent}}{c_p}{T_{amb}} + {h_{c,plen}}A\,{T_{s,coll}}} \right)}}{{\left( {{h_{c,plen}}A + {{\dot m}_{vent}}{c_p} + {h_{c,plen}}A} \right)}}
+\end{equation}
+
+where,
+
+~~~~~ \({\dot m_{vent}}\) ~is the air mass flow from natural forces {[}kg/s{]}
+
+The literature on UTSC does not appear to address the passive mode of operation and no models for \({\dot m_{vent}}\) ~have been identified.~ Nevertheless, natural buoyancy and wind forces are expected to drive air exchange between the plenum and ambient and some method of modeling \({\dot m_{vent}}\) ~is needed.~ Reasoning that the configuration is similar to single-side natural ventilation, we elect to use correlations for natural ventilation presented in Chapter 26. of ASHRAE HOF (2001).
+
+\begin{equation}
+{\dot m_{vent}} = \rho \,{{\rm{\rlap{--} \dot V}}_{{\rm{tot}}}}
+\end{equation}
+
+where,
+
+~~~~~ \(\rho\) ~is the density of air {[}kg/m\(^{3}\){]}, and
+
+~~~~~ \({{\rm{\rlap{--} \dot V}}_{{\rm{tot}}}} = {{\rm{\rlap{--} \dot V}}_{{\rm{wind}}}} + \,{{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}}\) ~is the total volumetric flow rate of air ventilating in and out of the plenum.
+
+\begin{equation}
+{{\rm{\rlap{--} \dot V}}_{{\rm{wind}}}} = {C_v}{A_{in}}{U_\infty }
+\end{equation}
+
+\({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}} = {C_D}{A_{in}}\sqrt {2g\Delta {H_{NPL}}\left( {{T_{a,plen}} - {T_{amb}}} \right)/{T_{a,plen}}}\) ~ (if \({T_{a,plen}} > {T_{amb}}\) )
+
+\({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}} = {C_D}{A_{in}}\sqrt {2g\Delta {H_{NPL}}\left( {{T_{amb}} - {T_{a,plen}}} \right)/{T_{amb}}}\) ~ (if \({T_{amb}} > {T_{a,plen}}\) ~and UTSC vertical)
+
+\({C_v}\) ~is the effectiveness of the openings that depends on opening geometry and the orientation with respect to the wind.~ ASHRAE HoF (2001) indicates values ranging from 0.25 to 0.6.~ In the UTSC model, this value is available for user input and defaulted to 0.25.
+
+\({C_D}\) ~is the discharge coefficient for the opening and depends on opening geometry.~ In the UTSC model, this value is available for user input and defaulted to 0.65.
+
+Mass continuity arguments lead to modeling the area of the openings as one half of the total area of the holes, so we have:
+
+\begin{equation}
+{A_{in}} = \frac{{A\,\sigma }}{2}
+\end{equation}
+
+\(g\) ~is the gravitational constant taken as 9.81 {[}m/s\(^{2}\){]}.
+
+\(\Delta {H_{NPL}}\) ~is the height from midpoint of lower opening to the Neutral Pressure Level.~ This is taken as one-fourth the overall height of the UTSC if it is mounted vertically.~ For tilted collectors, the nominal height is modified by the sine of the tilt.~ If the UTSC is mounted horizontally (e.g.~on the roof) then the \(\Delta {H_{NPL}}\) ~is taken as the gap thickness of the plenum.
+
+If the UTSC is horizontal and \({T_{amb}} > {T_{a,plen}}\) ~then \({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}}{\rm{ = 0}}\) ~because this is a stable situation.
+
+\subsubsection{Underlying Heat Transfer Surface}\label{underlying-heat-transfer-surface-000}
+
+The UTSC is applied to the outside of a heat transfer surface.~ This surface is modeled using the usual EnergyPlus methods for handling heat capacity and transients -- typically the CTF method.~ These native EnergyPlus Heat Balance routines are used to calculate \({T_{so}}\) .~ The UTSC model is coupled to the underlying surface using the OtherSideConditionsModel mechanism.~ The UTSC model provides values for \({h_{r,plen}}\) ,\({T_{s,coll}}\) , \({h_{c,plen}}\) , and \({T_{a,plen}}\) ~for use with the Heat Balance Model calculations for the outside face of the underlying surface (described elsewhere in this manual).
+
+\subsubsection{Solar and Shading Calculations}\label{solar-and-shading-calculations-2}
+
+The transpired collector object uses a standard EnergyPlus surface in order to take advantage of the detailed solar and shading calculations.~ Solar radiation incident on the surface includes beam and diffuse radiation, as well as radiation reflected from the ground and adjacent surfaces.~ Shading of the collector by other surfaces, such as nearby buildings or trees, is also taken into account.
+
+\subsubsection{Local Wind Speed Calculations}\label{local-wind-speed-calculations-000}
+
+The outdoor wind speed affects terms used in modeling UTSC components.~ The wind speed in the weather file is assumed to be measured at a meteorological station located in an open field at a height of 10 m.~ To adjust for different terrain at the building site and differences in the height of building surfaces, the local wind speed is calculated for each surface.
+
+The wind speed is modified from the measured meteorological wind speed by the equation (ASHRAE 2001):
+
+\begin{equation}
+{U_\infty } = {V_{met}}{\left( {\frac{{{\delta_{met}}}}{{{z_{met}}}}} \right)^{{a_{met}}}}{\left( {\frac{z}{\delta }} \right)^a}
+\end{equation}
+
+where z is the height of the centroid of the UTSC, z\(_{met}\) is the height of the standard metereological wind speed measurement, and a and d are terrain-dependent coefficients.~ d is the boundary layer thickness for the given terrain type.~ The values of a and d are shown in the following tables:
+
+% table 77
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Terrain-Dependent Coefficients (ASHRAE 2001). \label{table:terrain-dependent-coefficients-ashrae-2001.-001}} \tabularnewline
+\toprule 
+Terrain & Description & Exponent, a & Layer Thickness, $\delta$ (m) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Terrain-Dependent Coefficients (ASHRAE 2001).} \tabularnewline
+\toprule 
+Terrain & Description & Exponent, a & Layer Thickness, $\delta$ (m) \tabularnewline
+\midrule
+\endhead
+
+1 & Flat, open country & 0.14 & 270 \tabularnewline
+2 & Rough, wooded country & 0.22 & 370 \tabularnewline
+3 & Towns and cities & 0.33 & 460 \tabularnewline
+4 & Ocean & 0.10 & 210 \tabularnewline
+5 & Urban, industrial, forest & 0.22 & 370 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The UTSC can be defined such that it has multiple underlying heat transfer surfaces.~ The centroid heights for each surface are area-weighted to determine the average height for use in the local wind calculation.
+
+\subsubsection{Convection Coefficients}\label{convection-coefficients-000}
+
+UTSC modeling requires calculating up to three different coefficients for surface convection heat transfer.~ These coefficients are defined in the classic way by:
+
+\begin{equation}
+{h_c} = \frac{{{T_{air}} - {T_{surf}}}}{{{{q''}_{conv}}}}
+\end{equation}
+
+First, \({h_{co}}\) ~is the convection coefficient for the collector surface facing the outdoors when the UTSC is passive.~ It is modeled in exactly the same way as elsewhere in EnergyPlus and will depend on the user setting for Outside Convection Algorithm -- Outside Surface Heat Balance entry elsewhere in this document.
+
+Second, \({h_{c,plen}}\) ~is the convection coefficient for surfaces facing the plenum.~ This coefficient is applied to just the underlying surface's convection when the UTSC is active and to both the collector and the underlying surface when the UTSC is passive.~ When the UTSC is active, we use the convection correlation for forced air developed by McAdams (1954) as published by ASHRAE HoF (2001):
+
+\begin{equation}
+{h_{c,plen}} = 5.62 + 3.9{V_p}
+\end{equation}
+
+where,
+
+~~~~~ \({V_p}\) ~is the mean velocity in the plenum determined from \({V_p} = \frac{{\dot m}}{{2\rho \,{A_p}}}\) ~where \({A_p}\) ~is the effective cross section area of the plenum perpendicular to the primary flow direction.~ When the UTSC is passive, we model the convection in the same way used in EnergyPlus to model air gaps in windows.~ These correlations vary by Rayleigh number and surface tilt and are based on the work of various research including Hollands et. al., Elsherbiny et. al., Wright, and Arnold.~ The formulations are documented in ISO (2003) standard 15099.~ For the UTSC implementation, the routines were adapted from Subroutine NusseltNumber in WindowManager.f90 (by F. Winkelmann), which itself was derived from Window5 subroutine ``nusselt''.
+
+Third, \({h_{c,wind}}\) ~is the convection coefficient used to degrade the UTSC performance under environmental conditions with high wind or rain.~ If the weather file indicates it is raining, then we set \({h_{c,wind}}\) ~ = 1000.0 which has the effect of making the collector the same temperature as ambient air.~ The heat exchanger effectiveness correlations described above account for a moderate amount of wind, but the correlations appear confined to the range 0 to 5.0 m/s.~ Therefore we set \({h_{c,wind}}\) ~equal to zero if \({U_\infty }\) ~is \textless{} = 5.0 m/s.~ If \({U_\infty }\) ~is \textgreater{} 5.0 m/s then we use the McAdams correlation but with a reduced velocity magnitude:
+
+\$\$ \({h_{c,wind}} = 5.62 + 3.9({U_\infty } - 5.0)\)
+
+\subsubsection{Radiation Coefficients}\label{radiation-coefficients-000}
+
+UTSC modeling requires calculating up to four different linearized coefficients for radiation heat transfer.~ Whereas radiation calculations usually use temperature raised to the fourth power, this greatly complicates solving heat balance equations for a single temperature.~ Linearized radiation coefficients have the same units and are used in the same manner as surface convection coefficients and introduce very little error for the temperature levels involved.
+
+The radiation coefficient, \({h_{r,plen}}\) , is used to model thermal radiation between the collector surface and the outside face of the underlying heat transfer surface.~ We assume a view factor of unity.~ It is calculated using:
+
+\begin{equation}
+{h_{r,plen}} = {\sigma_{SB}}{e_{coll}}{e_{so}}\frac{{\left( {T_{s,coll}^4 - T_{so}^4} \right)}}{{\left( {{T_{s,coll}} - {T_{so}}} \right)}}
+\end{equation}
+
+where,
+
+~~~~~ all temperatures are converted to Kelvin,
+
+~~~~~ \({\sigma_{SB}}\) ~is the Stefan-Boltzmann constant,
+
+~~~~~ \({e_{coll}}\) ~is the longwave thermal emmittance of the collector, and
+
+~~~~~ \({e_{so}}\) ~is the longwave thermal emmittance of the underlying heat transfer surface.
+
+The three other coefficients, \({h_{r,atm}}\) , \({h_{r,sky}}\) , and \({h_{r,gnd}}\) ~are used elsewhere in EnergyPlus for the outside face surface heat balance and are calculated in the same manner as equation for UTSC collectors.~ {[}This is accomplished by calling subroutine InitExteriorConvectionCoeffs in the file HeatBalanceConvectionCoeffs.f90. {]}
+
+\subsubsection{Bypass Control}\label{bypass-control}
+
+The UTSC is assumed to be arranged so that a bypass damper controls whether or not air is drawn directly from the outdoors or through the UTSC.~ The control decision is based on whether or not it will be beneficial to heat the outdoor air.~ There are multiple levels of control including an availability schedule, whether or not the outdoor air is cooler than the mixed air setpoint, or whether or not the zone air temperature is lower than a so-called free heating setpoint.
+
+\subsubsection{Sizing Warnings}\label{sizing-warnings}
+
+Although the design of the transpired collector is left to the user, the program issues warnings when the suction airflow velocity falls outside the range 0.003 to 0.08 m/s.
+
+\subsubsection{Overall Efficiency}\label{overall-efficiency}
+
+The overall thermal efficiency of the UTSC is a useful output report and is defined as the ratio of the useful heat gain of the entire system versus the total incident solar radiation on the gross surface area of the collector.
+
+\begin{equation}
+\eta  = \frac{{(\dot Q/A)}}{{{I_{sc}}}} = \frac{{\dot m\,{c_p}\left( {{T_{a,plen}} - {T_{amb}}} \right)}}{{{I_{sc}}A}}
+\end{equation}
+
+where
+
+\(\dot Q\) ~is useful heat gain
+
+\({I_{sc}}\) ~is total incident solar radiation
+
+Note that the efficiency \(\eta\) ~is only defined for \({I_{solar}} > 0\) .~ This efficiency includes heat recovered from the underlying wall and can exceed 1.0.
+
+\subsubsection{Collector Efficiency}\label{collector-efficiency}
+
+The thermal efficiency of the collector is a useful output report and is defined as the ratio of the useful heat gain of the collector fluid versus the total incident solar radiation on the gross surface area of the collector.
+
+\begin{equation}
+\eta  = \frac{{\dot m\,{c_p}\left( {{T_{a,HX}} - {T_{amb}}} \right)}}{{{I_{sc}}A}}
+\end{equation}
+
+Note that the efficiency \(\eta\) ~is only defined for \({I_{solar}} > 0\)
+
+\subsubsection{References}\label{references-3-004}
+
+Kutscher, C.F. 1994. Heat exchange effectiveness and pressure drop for air flow through perforated plates with and without crosswind. \emph{Journal of Heat Transfer}. May 1994, Vol. 116, p.~391. American Society of Mechanical Engineers.
+
+Van Decker, G.W.E., K.G.T. Hollands, and A.P. Brunger. 2001. Heat-exchange relations for unglazed transpired solar collectors with circular holes on a square of triangular pitch. \emph{Solar Energy}. Vol. 71, No. 1. pp 33-45, 2001.
+
+ISO. 2003. ISO 15099:2003. Thermal performance of windows, doors, and shading devices -- Detailed calculations. International Organization for Standardization.
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@@ -0,0 +1,349 @@
+\section{System Availability Managers }\label{system-availability-managers}
+
+\subsection{Overview}\label{overview-025}
+
+System availability managers, or AvailabilityManagers, are one of the high-level control constructs in EnergyPlus. An AvailabilityManager is able to access data from any of the HVAC system nodes and use this data to set flags telling a central air system or plant loop to turn on or off. Also, some of the HVACZone:* components can use these same availability managers to turn their supply air fan on or off. Each type of availability manager encapsulates a specific high-level on-off control strategy. For instance, the input object AvailabilityManager:NightVentilation allows the user to specify a control strategy for pre-cooling the building with night-time ventilation.
+
+Availability managers are contained in the program module \emph{SystemAvailabilityManager}. The Availability managers are executed at the start of each HVAC time step by a call to \emph{ManageSystemAvailability}, and they reside outside the HVAC system iteration loops. Thus, the availability managers are executed once per HVAC time step, and they use previous time step information to calculate their control actions.
+
+If a given instance of an AvailabilityManager is specific to an AirLoopHVAC or to a PlantLoop, then in the input, each loop references its availability managers through a AvailabilityManagerAssignmentList. Once the data has been read in and processed, the AvailabilityManager data for each loop is stored in array \emph{PriAirSysAvailMgr} in \emph{DataAirLoop} (for AirLoopHVAC) and in array \emph{PlantAvailMgr} ~in \emph{DataPlant} for plant loops.
+
+The availability status for each AirLoopHVAC (\emph{PriAirSysAvailMgr}) is also passed to a zone equipment availability status array (\emph{ZoneEquipAvail}) for possible use by the zones served by that air loop. This sets the availability for certain zone equipment which are assumed to operate in conjunction with the air loop. Specifically, the availability of zone exhaust fans (Ref. Fan:ZoneExhaust) and terminal unit fans (Ref. AirTerminal:SingleDuct:SeriesPIU: Reheat, AirTerminal:SingleDuct: ParallelPIU:Reheat, and AirTerminal:SingleDuct:VAV: Reheat:VariableSpeedFan), if specified in the input, will be the same as the corresponding AirLoopHVAC availability if an AvailabilityManager is specified. Other zone equipment are not affected by the AirLoopHVAC system availability managers (e.g., Window AC, PTAC and PTHP).
+
+However, system availability managers can separately be specified for zone components (currently only allowed for Window AC, PTAC, PTHP, Unit Heater, Unit Ventilator, Zone Water to Air Heat Pump, Zone Terminal Unit (VRF), Standalone Energy Recovery Ventilator, Outdoor Air Unit, Fan Coil Unit, and Ventilated Slab). Similar to AirLoopHVAC or PlantLoop, inputs of these zone components refer to their availability managers through a AvailabilityManagerAssignmentList. System availability managers only operate when zone components are available. If the Window AC (or any other unit) is scheduled off then the system availability manager will not operate until the Window AC is scheduled on. The functioning of the system availability manager for zone components is same as for AirLoopHVAC or PlantLoop. Except night ventilation SAM, all other SAMs can be specified for these zone components.
+
+The actual action of turning on or off a loop is taken by the loop prime movers: fans for AirLoopHVACs and pumps for plant loops. For instance when a fan is deciding whether it is on or off, it checks its on/off schedule and whether the loop availability status flag is \emph{CycleOn} or \emph{ForceOff}. If the schedule is on and the status flag is \emph{ForceOff}, the fan will be off. If the fan schedule says off and the status flag is \emph{CycleOn}, the fan will be on. Thus the availability managers overrule the fan on/off schedule.
+
+\subsection{Scheduled}\label{scheduled-000}
+
+The input object AvailabilityManager:Scheduled provides the simplest availability manager. The sole input for this manager is a schedule name. If the current schedule value is \textgreater{} 0.0, the availability status flag is set to \emph{CycleOn}; otherwise it is set to \emph{ForceOff}.
+
+\subsection{Scheduled On}\label{scheduled-on}
+
+An alternative to the AvailabilityManager:Scheduled object is the \emph{AvailabilityManager:ScheduledOn} that is used specifically to turn equipment on while other availability managers may be used to turn the equipment off. The sole input for this manager is a schedule name. If the current schedule value is \textgreater{} 0.0, the availability status flag is set to \emph{CycleOn}; otherwise it is set to \emph{NoAction}.
+
+\subsection{Scheduled Off}\label{scheduled-off}
+
+An alternative to the AvailabilityManager:Scheduled object is the \emph{AvailabilityManager:ScheduledOff} that is used specifically to turn equipment off while other availability managers may be used to turn the equipment on. The sole input for this manager is a schedule name. If the current schedule value is = 0.0, the availability status flag is set to \emph{ForceOff}; otherwise it is set to \emph{NoAction}.
+
+\subsection{Night Cycle}\label{night-cycle}
+
+The input object AvailabilityManager:NightCycle is to specify when a system that has been scheduled off during unoccupied hours should cycle on to prevent building temperatures from becoming too hot or too cold. This manager can not be used to force a system off. The inputs are:
+
+·~~~~~~~~A manager applicability schedule;
+
+·~~~~~~~~The name of the fan schedule this manager will override;
+
+·~~~~~~~~The control type: \emph{Stay Off}, \emph{Cycle On Any}, \emph{Cycle On Control Zone}, or \emph{Cycle On Any - Zone Fans Only};
+
+·~~~~~~~~Thermostat on/off tolerance \emph{T\(_{tol}\)} (degrees C);
+
+·~~~~~~~~Cycling run time in seconds; used to calculate a stop time (in time steps since the start of the current run period) once the status has become \emph{Cycle On}.
+
+If the fan schedule current value is \textgreater{} 0 or the applicability schedule value is \(\le\) ~0 or if the program is in warmup, \emph{AvailStatus = NoAction}.
+
+Otherwise,
+
+1.~~~~if current time (in time steps since the start of the run period) is greater than the start time and less than the stop time, \emph{AvailStatus = CycleOn} (or \emph{CycleOnZoneFansOnly} if the control type is \emph{Cycle On Any -- Zone Fans only}).
+
+2.~~~~If the current time equals the stop time, \emph{AvailStatus = NoAction} ~and the fan schedule will determine if the system is on.
+
+3.~~~~~If the current time is greater than the stop time, the manager can potentially cycle the system on.
+
+a.~~~~For control types \emph{Cycle On Any} and \emph{Cycle On Any -- Zone Fans Only} the manger looks at each zone served by the air loop and detects whether the zone temperature at the thermostat is greater than the cooling setpoint plus ½\emph{T\(_{tol}\)} or less than the heating setpoint minus ½\emph{T\(_{tol}\)}. If it is, \emph{AvailStatus} is set to \emph{CycleOn} (or \emph{CycleOnZoneFansOnly}). If not, \emph{AvailStatus} is set to \emph{NoAction}.
+
+b.~~~For control type \emph{Cycle On Control Zone}, the manager does the same check just for the control zone.
+
+Lastly if the new status is CycleOn the start time is reset to the current time and the stop time is reset. When this availability manager is specified for a zone component then the only allowed control types are \emph{Stay Off} \emph{and} \emph{Cycle On Control Zone.}
+
+\subsection{Night Ventilation}\label{night-ventilation}
+
+The input object AvailabilityManager:NightVentilation is a manager that looks at indoor and outdoor conditions to see if night ventilation might be beneficial. In addition to being able to cycle the air system on, this manager can specify what the ventilation air flow rate should be.~ The inputs are:
+
+·~~~~~~~~A manager applicability schedule;
+
+·~~~~~~~~The name of the fan schedule this manager will override;
+
+·~~~~~~~~A ventilation temperature schedule;
+
+·~~~~~~~~A ventilation delta T;
+
+·~~~~~~~~A ventilation low limit temperature;
+
+·~~~~~~~~The night ventilation flow fraction;
+
+·~~~~~~~~The name of the control zone.
+
+If the fan schedule current value is \textgreater{} 0 or the applicability schedule value is \(\le\) ~0 or if the program is in warmup, \emph{AvailStatus = NoAction}.
+
+Otherwise, the manager performs 3 limit checks.
+
+1)~~~~If for all the zones connected to the air loop the room temperature at the thermostat of any zone is greater than the ventilation temperature schedule value, this check is true.
+
+2)~~~~If for all the zones connected to the air loop the room temperature at the thermostat of any zone is less than the ventilation low limit temperature, this check is true.
+
+3)~~~~If the difference between the control zone room temperature at the thermostat and the outside temperature is greater than the specified night venting delta T, this check is true.
+
+If 1) and 3) are true and 2) is false, the status is set to \emph{CycleOn}; otherwise the status is \emph{NoAction}.~ If the status is \emph{CycleOn} this manager sets some additional values in the \emph{AirLoopControlInfo} data structure (a flag is set to indicate night ventilation is occurring and a flag is set to indicate that the air system flow rate has been specified by a manager) and in the \emph{~AirLoopFlow} data structure (the system flow fraction is specified). The night ventilation flag indicates to the fan that it should use alternate performance characteristics if they have been specified in a FanPerformance:NightVentilation object.
+
+\subsection{Differential Thermostat}\label{differential-thermostat}
+
+The input object AvailabilityManager:DifferentialThermostat is a manager that overrides fan or pump schedules depending on the temperature difference between two nodes. A typical use would be for one node to be an outdoor air node and the other a zone node. The inputs are:
+
+·~~~~~~~~name of the hot node;
+
+·~~~~~~~~name of the cold node;
+
+·~~~~~~~~temperature difference for turning the system on (\emph{DeltaT\(_{on}\)});
+
+·~~~~~~~~temperature difference for turning the system off (\emph{DeltaT\(_{off}\)}).
+
+Note that there is no applicability schedule for this manager. Also, this manager always returns a status of \emph{CycleOn} or \emph{ForceOff}, never \emph{NoAction}.
+
+\emph{DeltaT} = \emph{T\(_{hot\, node}\)} -- \emph{T\(_{cold\, node}\)}
+
+If \emph{DeltaT} \textgreater{} = \emph{DeltaT\(_{on}\)} ~then
+
+\emph{AvailStatus = CycleOn}
+
+~ ~~~~Else if \emph{DeltaT} \textless{} = \emph{DeltaT\(_{off}\)} ~then
+
+\emph{AvailStatus = ForceOff}
+
+Else
+
+\emph{AvailStatus} remains in its previous state.
+
+\subsection{High Temperature Turn Off}\label{high-temperature-turn-off}
+
+The input object AvailabilityManager:HighTemperatureTurnOff is used to turn off a central air system or a plant loop if a sensed node temperature exceeds a temperature limit. The inputs are:
+
+·~~~~~~~~name of the sensed node;
+
+·~~~~~~~~limit temperature (\emph{T\(_{u}\)}).
+
+If \emph{T\(_{sensed\, node}\)} \textgreater{} = \emph{T\(_{u}\)} then
+
+\emph{AvailStatus} = \emph{ForceOff}
+
+Else
+
+\emph{AvailStatus} = \emph{NoAction}
+
+\subsection{High Temperature Turn On}\label{high-temperature-turn-on}
+
+The input object AvailabilityManager:HighTemperatureTurnOn is used to turn on a central air system or a plant loop if a sensed node temperature exceeds a temperature limit. The inputs are:
+
+·~~~~~~~~name of the sensed node;
+
+·~~~~~~~~limit temperature (\emph{T\(_{u}\)}).
+
+If \emph{T\(_{sensed\, node}\)} \textgreater{} = \emph{T\(_{u}\)} then
+
+\emph{AvailStatus} = \emph{CycleOn}
+
+Else
+
+\emph{AvailStatus} = \emph{NoAction}
+
+\subsection{Low Temperature Turn Off}\label{low-temperature-turn-off}
+
+The input object AvailabilityManager:LowTemperatureTurnOff is used to turn off a central air system or a plant loop if a sensed node temperature is lower than a temperature limit. The inputs are:
+
+·~~~~~~~~name of the sensed node;
+
+·~~~~~~~~limit temperature (\emph{T\(_{l}\)});
+
+·~~~~~~~~applicability schedule name.
+
+If the applicability schedule exists and has a current value of \textless{} = 0, the manager returns an availability status of \emph{NoAction}.
+
+Otherwise,
+
+If \emph{T\(_{sensed\, node}\)} \textless{} = \emph{T\(_{l}\)}~ then
+
+\emph{AvailStatus} = \emph{ForceOff}
+
+Else
+
+\emph{AvailStatus} = \emph{NoAction}
+
+\subsection{Low Temperature Turn On}\label{low-temperature-turn-on}
+
+The input object AvailabilityManager:LowTemperatureTurnOn is used to turn on a central air system or a plant loop if a sensed node temperature is less than a temperature limit. The inputs are:
+
+·~~~~~~~~name of the sensed node;
+
+·~~~~~~~~limit temperature (\emph{T\(_{l}\)}).
+
+If \emph{T\(_{sensed\, node}\)} \textless{} = \emph{T\(_{l}\)}~ then
+
+\emph{AvailStatus} = \emph{CycleOn}
+
+Else
+
+\emph{AvailStatus} = \emph{NoAction}
+
+\subsection{Hybrid Ventilation Control}\label{hybrid-ventilation-control}
+
+The input object AvailabilityManager:HybridVentilation serves two purposes: 1) it prevents simultaneous natural ventilation and HVAC system operation, and 2) it allows users to examine various strategies to maximize natural ventilation in order to reduce heating/cooling loads. This availability manager works with either the AirflowNetwork model or the simple airflow objects to provide controlled natural ventilation. The controlled natural ventilation objects referred to here are either AirflowNetwork:Multizone:ComponentDetailedOpening and AirflowNetwork:Multizone:ComponentSimpleOpening objects, or ZoneVentilation and ZoneMixing objects. The simple airflow objects are not allowed to work with the AirflowNetwork objects simultaneously. If there is no air loop, this availability manager can still be applied to controlled zone specified in the object. In order to apply hybrid ventilation manager to the controlled zone not served by any air loop, the HVAC air loop name input field must be left blank. Currently, zone component objects such as unit heater, unit ventilator, packaged terminal air conditioner, packaged terminal heat pump, zone water source heat pump, window air conditioner, variable refrigerant flow, energy recovery ventilator, outdoor air unit, fan coil unit, and ventilated slab can individually use hybrid ventilation managers to make a decision regarding whether their fan should be on or off. Also, hybrid ventilation manager can be applied to zones served by the ideal load zone component to turn them off when natural ventilation is active. Currently, hybrid ventilation manager is restricted to one per zone. It can either be applied through the air loop or directly to the zone. If hybrid ventilation manager is applied to an air loop and one of the zones served by the air loop also has hybrid ventilation manager, then zone hybrid ventilation manager is disabled. This availability manager performs somewhat differently from the other availability managers:
+
+n~This availability manager is called before the program estimates (predicts) the cooling or heating load that needs to be met by the cooling/heating systems for the simulation time step. On the other hand, the other availability managers are called after the system cooling/heating load prediction. The main reason for calling AvailabilityManager:HybridVentilation early is that this manager determines whether natural ventilation is allowed or not, and the loads from natural ventilation are used to predict system loads.
+
+n~This availability manager has its own control schedule and does not work in tandem with \emph{AvailabilityManager:Scheduled}.
+
+n~AvailabilityManager:HybridVentilation works completely independent of the other system availability managers, so this manager is not a valid system availability manager type in the AvailabilityManagerAssignmentList object.
+
+\subsubsection{Control logic}\label{control-logic-000}
+
+The control logic for each ventilation control mode is described below.
+
+\subsubsection{Temperature control}\label{temperature-control}
+
+This control mode checks whether the outdoor air dry-bulb temperature is between the Minimum Outdoor Temperature and Maximum Outdoor Temperature specified. If the outdoor temperature is between the two values then natural ventilation is allowed, else natural ventilation is not allowed.
+
+When natural ventilation is allowed, the control then checks the temperature difference between the zone temperature and the temperature setpoint(s) in the controlled zone based on the specified temperature control type (four available temperature control types) to make a final decision:
+
+\emph{Single Heating Setpoint:}
+
+If the zone temperature is below the setpoint, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid overcooling a space, which could result in additional heating load.
+
+\emph{Single Cooling Setpoint:}
+
+If the zone temperature is above the setpoint, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid overheating a space, which could result in additional cooling load.
+
+\emph{Single Heating Cooling Setpoint:}
+
+Since this temperature control type requires only a single setpoint, natural ventilation is not allowed. A recurring warning message is issued.
+
+\emph{Dual Setpoint with DeadBand:}
+
+If the zone temperature is beyond the deadband, the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid either overcooling a space, which could result in additional heating load when the zone temperature is below the heating setpoint, or overheating a space, which could result in additional cooling load when the zone temperature is above the cooling setpoint.
+
+\subsubsection{Enthalpy control}\label{enthalpy-control}
+
+This control mode checks whether the outdoor air enthalpy is between the Minimum Outdoor Enthalpy and Maximum Outdoor Enthalpy specified. If the outdoor enthalpy is between the two values then natural ventilation is allowed, else natural ventilation is not allowed.
+
+When natural ventilation is allowed, the control then checks the temperature difference between the zone temperature and the temperature setpoint(s) in the controlled zone based on the specific temperature control type to make a final decision. This procedure is the same as defined above for the temperature control mode.
+
+\emph{Single Heating Setpoint:}
+
+If the zone temperature is below the setpoint, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid overcooling a space, which could result in additional heating load.
+
+\emph{Single Cooling Setpoint:}
+
+If the zone temperature is above the setpoint, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid overheating a space, which could result in additional cooling load.
+
+\emph{Single Heating Cooling Setpoint:}
+
+Since this temperature control type requires only a single setpoint, natural ventilation is not allowed. A recurring warning message is issued.
+
+\emph{Dual Setpoint with DeadBand:}
+
+If the zone temperature is beyond the deadband, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid either overcooling a space, which could result in additional heating load when the zone temperature is below the heating setpoint, or overheating a space, which could result in additional cooling load when the zone temperature is above the cooling setpoint.
+
+\subsubsection{Dew-Point control}\label{dew-point-control}
+
+This control mode checks whether the outdoor air dewpoint temperature is between the Minimum Outdoor Dew-Point and Maximum Outdoor Dew-Point specified. If the outdoor dewpoint temperature is between the two values then natural ventilation is allowed, else national ventilation is not allowed.
+
+When natural ventilation is allowed and a humidistat is available in the controlled zone, the control then checks the humidity ratio difference between the zone air humidity ratio and humidistat setpoint in the controlled zone to make a final decision. It should be pointed out that the humidistat object provides the setpoint of relative humidity, the value of relative humidity has to be converted into the setpoint of humidity ratio using the actual zone air temperature for comparison. Since the humidistat only provides a single value for relative humidity, there are two possible scenarios:
+
+If the actual zone air humidity ratio is below the humidity ratio setpoint and the controlled zone needs humidification as the first scenario, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid dehumidifying a space, which could result in additional humidification load.
+
+If the actual zone air humidity ratio is above the humidity ratio setpoint and the controlled zone needs dehumidification as the second scenario, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid humidifying a space, which could result in additional dehumidification load.
+
+\subsubsection{Outdoor ventilation air control}\label{outdoor-ventilation-air-control}
+
+This control mode does not require any additional checks. The control only works with Airflow Network opening objects only, and is not allowed to work with ZoneVentilation and ZoneMixing objects.
+
+\subsubsection{Availability Status}\label{availability-status}
+
+After the hybrid ventilation control determines whether natural ventilation is allowed or not, the availability status flag is set as follows:
+
+If \emph{Natural Ventilation} then
+
+\emph{AvailStatus} = \emph{CycleOn}
+
+Else
+
+\emph{AvailStatus = ForceOn}
+
+\subsection{\texorpdfstring{\textbf{Optimum Start Controls}}{Optimum Start Controls}}\label{optimum-start-controls}
+
+\subsubsection{Overview}\label{overview-1-008}
+
+Optimum start is often also referred to as optimum recovery time. Commercial buildings are often operated intermittently by lowering heating set-point and increasing cooling set-point during unoccupied period. The building should return to set-point just before occupancy period starts. Therefore it is important to start the operation of heating and cooling plant before building is occupied. If the operation is started too early before the occupants return, energy is wasted. If it is started too late the occupants will be uncomfortable. An optimum start time for operation will save energy without compromising comfort.
+
+\begin{figure}[hbtp] % fig 301
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6731.png}
+\caption{Optimal Start Control \protect \label{fig:optimal-start-control}}
+\end{figure}
+
+In practice a few proprietary algorithms are used to predict this start time value for preheating and precooling operation. ASHRAE Handbook refers to work done by (Seem, Armstrong, \& Hancock, 1989) which compares seven different equations and suggests a set of equations for preheating and precooling time prediction.
+
+\subsubsection{Algorithms}\label{algorithms}
+
+There are a few algorithms to predict the start time for the HVAC system. Among these algorithms following are the promising ones that can be implemented in a simulation environment.
+
+\subsubsection{Constant Start Time}\label{constant-start-time}
+
+This is the simplest format of the optimum start algorithm. The HVAC system will start the HVAC system at a fixed number of hours before occupancy as specified by the user.
+
+\subsubsection{Constant Temperature Gradient}\label{constant-temperature-gradient}
+
+In practice most of the HVAC control manufacturers use a temperature gradient as a thermal capacity factor, in which temperature rise per unit time i.e. °C/hour is measured for the unoccupied building and then the difference between space temperature and set-point temperature is divided by this factor to calculate the actual number of hours before occupancy are needed to start the HVAC system.
+
+\subsubsection{Adaptive Temperature Gradient}\label{adaptive-temperature-gradient}
+
+Adaptive control is used to modify the temperature gradient depending on the time required to meet the set-point on the prior days. The adaptive algorithm takes the arithmetic average of the actual temperature gradients calculated for the specified number of previous days.
+
+\subsubsection{Adaptive ASHRAE Algorithm}\label{adaptive-ashrae-algorithm}
+
+The equations suggested in the ASHRAE Handbook are used in combination with a recursive linear least square method to determine the optimum start/recovery time empirically. Depending on heating or cooling operation the start time is categorized as preheating or precooling time. According to (Seem, Armstrong, \& Hancock, 1989) the preheating time is a strong function of outdoor temperature whereas precooling time is not strong function of outdoor temperature if space temperature is close or less than the setback temperature. Thus, two different equations are suggested for preheating and precooling time.
+
+n~Precooling time
+
+\begin{equation}
+{t_i} = {a_0} + {a_1}{T_{z,i}} + {a_2}T_{z,i}^2
+\end{equation}
+
+Preheating time
+
+\begin{equation}
+{t_i} = {a_0} + \left( {1 - {w_i}} \right)({a_1}{T_{z,i}} + {a_2}T_{z,i}^2) + {w_i}{a_3}{T_{o,i}}
+\end{equation}
+
+Where, on \emph{i}\(^{th}\) day
+
+\emph{t\(_{i}\)} = start/recovery time,
+
+\emph{T\(_{z,i}\)} = ~~~~~~~~~ zone temperature
+
+\emph{T\(_{o,i}\)} = ~~~~~~~~~~ outdoor temperature
+
+`\emph{w\(_{i}\)}' is a weighting factor which determines weighting given to outside and zone temperature.
+
+\begin{equation}
+{w_i} = {1000^{ - \frac{{\left( {{T_{z,i}} - {T_{unocc}}} \right)}}{{\left( {{T_{occ}} - {T_{unocc}}} \right)}}}}
+\end{equation}
+
+\emph{T\(_{unocc}\)} and \emph{T\(_{occ}\)} are setpoint temperatures during unoccupied (setback) and occupied periods.
+
+Coefficients \emph{a\(_{0}\), a\(_{1}\), a\(_{2}\)} (and \emph{a\(_{3}\)}) are separately calculated for heating and cooling operation and are updated from the optimum times from last three days thus; these coefficients carry history and adapt the trend from previous days.
+
+The optimum time for past days is determined using,
+
+\begin{equation}
+{t_{opt,\left( {i - 1} \right)}} = {k_{\left( {i - 1} \right)}}\Delta t - \Delta t\left( {1 - \frac{{{q_{\left( {i - 1} \right)}}}}{{{q_{max}}}}} \right)
+\end{equation}
+
+\emph{k} = time steps required for recovery
+
+Δ\emph{t} = ~~~~~~~~~~~ time-step
+
+\emph{t\(_{opt,(i-1)}\)} = recovery time on (\emph{i}-1)\(^{th}\) day
+
+\emph{q\(_{(i-1)}\)} = ~~~~~~~~~ energy extracted or added during last time step
+
+\emph{q\(_{max}\)} = ~~~~~~~~ maximum capacity of the equipments 
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003.tex
new file mode 100644
index 00000000000..c4ed855e87d
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003.tex
@@ -0,0 +1,21 @@
+\chapter{Simulation Models -- Encyclopedic Reference}\label{simulation-models-encyclopedic-reference-000}
+
+The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of ``Heat Balance'', ``HVAC'', and ``Plant''.~ With the integrated solution, these designations signify where the effects of these models have their first impacts.
+
+Main Sections:
+
+\begin{itemize}
+\tightlist
+\item
+  \protect\hyperlink{ThermalComfort}{Thermal Comfort}
+\item
+  \protect\hyperlink{TrombeWalls}{Trombe Walls}
+\item
+  \protect\hyperlink{WaterTanks}{Water Thermal Tanks}
+\item
+  \protect\hyperlink{WaterSystems}{Water Systems}
+\item
+  \protect\hyperlink{ZoneControls}{Zone Controls}
+\item
+  \protect\hyperlink{ZoneEquip}{Zone Equipment and Zone Forced Air Units} 
+\end{itemize}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/occupant-thermal-comfort.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/occupant-thermal-comfort.tex
new file mode 100644
index 00000000000..006b7debd7c
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/occupant-thermal-comfort.tex
@@ -0,0 +1,1016 @@
+\section{Occupant Thermal Comfort }\label{occupant-thermal-comfort}
+
+The integration of a sophisticated building thermal analysis tool with thermal comfort models allows one to perform an energy analysis on a zone and simultaneously determine if the environmental control strategy will be sufficient for the occupants to be thermally comfortable. This chapter is intended to provide background on thermal comfort, present an overview of state of the art thermal comfort models and present the mathematical models that have been incorporated into Energy Plus.
+
+Thermal comfort modeling is controlled primarily by the People input object. This includes input for selecting the type of thermal comfort model that is desired by the user as well as parameters that serve as inputs to all of the thermal comfort models. This includes the activity level, the work efficiency, the air velocity, and the clothing insulation level for people within the space.~ All four of these parameters can be scheduled. More information on the People input object can be found in the EnergyPlus Input/Output Reference. More information on how each of these parameters is used and the specific modeling equations for the thermal comfort models can be found below.
+
+\subsection{Background on Thermal Comfort Models}\label{background-on-thermal-comfort-models}
+
+Throughout the last few decades, researchers have been exploring the thermal, physiological and psychological response of people in their environment in order to develop mathematical models to predict these responses. Researchers have empirically debated building occupants' thermal responses to the combined thermal effect of the personal, environmental and physiological variables that influence the condition of thermal comfort.
+
+There are two personal variables that influence the condition of thermal comfort: the thermal resistance of the clothing (I\(_{cl}\)), and the metabolic rate (H/A\(_{Du}\)). The thermal resistance of the clothing (I\(_{cl}\)) is measured in units of ``clo.'' The 1985 ASHRAE Handbook of Fundamentals (ASHRAE 1985) suggests multiplying the summation of the individual clothing items clo value by a factor of 0.82 for clothing ensembles.
+
+The metabolic rate (H/A\(_{Du}\)), is a measure of the internal heat production rate of an occupant (H) w/hr. in per unit of ``Dubois'' body surface area (A\(_{Du}\)) in units of m\(^{2}\). The DuBois body surface area is given by :
+
+\begin{equation}
+{A_{Du}} = 0.202{(weight)^{0.425}}{(height)^{0.725}}
+\end{equation}
+
+Using this equation, an area of 1.8 m\(^{2}\) represents the surface area of an average person of weight 70 kg. and height 1.73 m (Fanger 1967). The metabolic rate is measured in mets, where 1 met = 58.2 W/m\(^{2}\).
+
+The environmental variables that influence the conditions of thermal comfort include:
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\item
+  Air Temperature (T\(_{a}\)),
+\item
+  Mean Radiant Temperature (T\(_{r}\)),
+\item
+  Relative air velocity (v),
+\item
+  Water vapor pressure in ambient air (P\(_{a}\))
+\end{enumerate}
+
+The Air Temperature (T\(_{a}\)), a direct environmental index, is the dry-bulb temperature of the environment. The Mean Radiant Temperature (T\(_{r}\)) is a rationally derived environmental index defined as the uniform black-body temperature that would result in the same radiant energy exchange as in the actual environment. The Relative air velocity (v) a direct environmental index is a measure of the air motion obtainable via a hot wire or vane anemometers. The Water vapor pressure in ambient air (P\(_{a}\)) is a direct environmental index.
+
+The physiological variables that influence the conditions of thermal comfort include:
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\item
+  Skin Temperature (T\(_{sk}\)),
+\item
+  Core or Internal Temperature (T\(_{cr}\)),
+\item
+  Sweat Rate,
+\item
+  Skin Wettedness (w),
+\item
+  Thermal Conductance (K) between the core and skin.
+\end{enumerate}
+
+Where the Skin Temperature (T\(_{sk}\)), the Core Temperature (T\(_{cr}\)) and the Sweat Rate are physiological indices. The Skin Wettedness (w) is a rationally derived physiological index defined as the ratio of the actual sweating rate to the maximum rate of sweating that would occur if the skin were completely wet.
+
+One more consideration is important in dealing with thermal comfort - the effect of asymmetrical heating or cooling. This could occur when there is a draft or when there is a radiant flux incident on a person (which is what is of primary interest to us here). Fanger (1967) noted that the human regulatory system is quite tolerant of asymmetrical radiant flux. A reasonable upper limit on the difference in mean radiant temperature (T\(_{r}\)) from one direction to the opposing direction is 15°C. (ASHRAE 1984). This limit is lower if there is a high air velocity in the zone.
+
+% table 78
+\begin{longtable}[c]{p{1.2in}p{2.0in}p{0.8in}p{0.8in}p{1.2in}}
+\caption{General Nomenclature list for Thermal Comfort Models \label{table:general-nomenclature-list-for-thermal-comfort}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units ~ & Range & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{General Nomenclature list for Thermal Comfort Models} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units ~ & Range & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+A\(_{Du}\) & Dubois body surface area & m\(^{2}\) & - & - \tabularnewline
+H & Internal heat production rate of an occupant per unit area = M – W & W/m\(^{2}\) & - & IntHeatProd \tabularnewline
+I\(_{cl}\) & Thermal resistance of the clothing & clo & - & CloUnit \tabularnewline
+M & Metabolic rate per unit area & W/m\(^{2}\) & - & ActLevel \tabularnewline
+P\(_{a}\) & Water vapor pressure in ambient air & Torr & - & VapPress \tabularnewline
+T\(_{a}\) & Air temperature & °C & - & AirTemp \tabularnewline
+T\(_{cr}\) & Core or internal temperature & °C & - & CoreTemp \tabularnewline
+T\(_{r}\) & Mean radiant temperature & °C & - & RadTemp \tabularnewline
+T\(_{sk}\) & Skin temperature & °C & - & - \tabularnewline
+v & Relative air velocity & m/s & - & AirVel \tabularnewline
+W & The rate of heat loss due to the performance of work & W/m\(^{2}\) & - & WorkEff \tabularnewline
+w & Skin wettedness & - & - & - \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Mathematical Models for Predicting Thermal Comfort}\label{mathematical-models-for-predicting-thermal-comfort}
+
+Many researchers have been exploring ways to predict the thermal sensation of people in their environment based on the personal, environmental and physiological variables that influence thermal comfort. From the research done, some mathematical models that simulate occupants' thermal response to their environment have been developed. Most thermal comfort prediction models use a seven or nine point thermal sensation scale, as in the following tables.
+
+% table 79
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Seven point Thermal Sensation Scale \label{table:seven-point-thermal-sensation-scale}} \tabularnewline
+\toprule 
+Sensation & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Seven point Thermal Sensation Scale} \tabularnewline
+\toprule 
+Sensation & Description \tabularnewline
+\midrule
+\endhead
+
+3 & Hot \tabularnewline
+2 & Warm \tabularnewline
+1 & slightly warm \tabularnewline
+0 & neutral \tabularnewline
+-1 & slightly cool \tabularnewline
+-2 & cool \tabularnewline
+-3 & cold \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 80
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Nine point Thermal Sensation Scale \label{table:nine-point-thermal-sensation-scale}} \tabularnewline
+\toprule 
+Sensation Value & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nine point Thermal Sensation Scale} \tabularnewline
+\toprule 
+Sensation Value & Description \tabularnewline
+\midrule
+\endhead
+
+4 & very hot \tabularnewline
+3 & hot \tabularnewline
+2 & warm \tabularnewline
+1 & slightly warm \tabularnewline
+0 & neutral \tabularnewline
+-1 & slightly cool \tabularnewline
+-2 & cool \tabularnewline
+-3 & cold \tabularnewline
+-4 & very cold \tabularnewline
+\bottomrule
+\end{longtable}
+
+The most notable models have been developed by P.O. Fanger (the Fanger Comfort Model), the J. B. Pierce Foundation (the Pierce Two-Node Model), and researchers at Kansas State University (the KSU Two-Node Model). Berglund (1978) presents a detailed description of the theory behind these three models.
+
+Note for all Thermal Comfort reporting:~ Though the published values for thermal comfort ``vote'' have a discrete scale (e.g. --3 to +3 or --4 to +4), the calculations in EnergyPlus are carried out on a continuous scale and, thus, reporting may be ``off the scale'' with specific conditions encountered in the space.~ This is not necessarily an error in EnergyPlus -- rather a different approach that does not take the ``limits'' of the discrete scale values into account.
+
+The main similarity of the three models is that all three apply an energy balance to a person and use the energy exchange mechanisms along with experimentally derived physiological parameters to predict the thermal sensation and the physiological response of a person due to their environment. The models differ somewhat in the physiological models that represent the human passive system (heat transfer through and from the body) and the human control system (the neural control of shivering, sweating and skin blood flow). The models also differ in the criteria used to predict thermal sensation. However, all three models use information from the People statement and the thermal comfort model is selected via the People statement in a user's input file. Scheduled parameters such as the activity level, work efficiency, air velocity, and clothing insulation level all have a direct bearing on the thermal comfort models. For more information on the input of these parameters, see the People statement in the EnergyPlus Input/Output Reference. For more information on how each individual thermal comfort model uses these parameters, please consult the next several sections.
+
+The main similarity of the three models is that all three apply an energy balance to a person and use the energy exchange mechanisms along with experimentally derived physiological parameters to predict the thermal sensation and the physiological response of a person due to their environment. The models differ somewhat in the physiological models that represent the human passive system (heat transfer through and from the body) and the human control system (the neural control of shivering, sweating and skin blood flow). The models also differ in the criteria used to predict thermal sensation.
+
+\subsection{Fanger Comfort Model}\label{fanger-comfort-model}
+
+Fanger's Comfort model was the first one developed. It was published first in 1967 (Fanger 1967) and then in 1970 (Fanger 1970), and helped set the stage for the other two models. The mathematical model developed by P.O. Fanger is probably the most well known of the three models and is the easiest to use because it has been put in both chart and graph form.
+
+\subsubsection{Fanger Model Nomenclature List}\label{fanger-model-nomenclature-list}
+
+% table 81
+\begin{longtable}[c]{p{1.2in}p{2.0in}p{0.8in}p{0.8in}p{1.2in}}
+\caption{Nomenclature list for Fanger model \label{table:nomenclature-list-for-fanger-model}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & Range & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature list for Fanger model} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & Range & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+A\(_{Du}\) & Dubois body surface area & m\(^{2}\) & - & BodySurfaceArea \tabularnewline
+C\(_{res}\) & The rate of dry respiratory heat loss & W/m\(^{2}\) & - & DryRespHeatLoss \tabularnewline
+E\(_{dif}\) & The rate of heat loss from the diffusion of water vapor through the skin & W/m\(^{2}\) & - & EvapHeatLossDiff \tabularnewline
+E\(_{res}\) & The rate of latent respiratory heat loss & W/m\(^{2}\) & - & LatRespHeatLoss \tabularnewline
+E\(_{rsw,req}\) & The rate of heat loss from the evaporation of regulatory sweating at the state of comfort & W/m\(^{2}\) & - & EvapHeatLossRegComf \tabularnewline
+E\(_{sk}\) & Total evaporative heat loss from skin & W/m\(^{2}\) & ~ & EvapHeatLoss \tabularnewline
+f\(_{cl}\) & The ratio of clothed body & - & ~ & CloBodyRat \tabularnewline
+f\(_{eff}\) & The fraction of surface effective for radiation ( = 0.72) & - & - & RadSurfEff \tabularnewline
+H & Internal heat production rate of an occupant per unit area ( = M – W) & W/m\(^{2}\) & - & IntHeatProd \tabularnewline
+h\(_{c}\) & Convective heat transfer coefficient & W/m\(^{2}\)°C & - & Hc \tabularnewline
+L & All the modes of energy loss from body & W/m\(^{2}\) & - & - \tabularnewline
+M & Metabolic rate per unit area & W/m\(^{2}\) & - & ActLevel \tabularnewline
+P\(_{a}\) & Water vapor pressure in ambient air & Torr & - & VapPress \tabularnewline
+PMV & Predicted Mean Vote & - & (-4)-4 & PMV \tabularnewline
+PPD & Predicted Percentage of Dissatisfied & - & 0-100 & PPD \tabularnewline
+Q\(_{c}\) & The rate of convective heat loss & W/m\(^{2}\) & - & ConvHeatLoss \tabularnewline
+Q\(_{dry}\) & Sensible heat flow from skin & W/m\(^{2}\) & ~ & DryHeatLoss \tabularnewline
+Q\(_{r}\) & The rate of radiative heat loss & W/m\(^{2}\) & - & RadHeatLoss \tabularnewline
+Q\(_{res}\) & The rate of respiratory heat loss & W/m\(^{2}\) & - & RespHeatLoss \tabularnewline
+T\(_{a}\) & Air temperature & °C & - & AirTemp \tabularnewline
+T\(_{cl}\) & Clothing surface temperature & °C & - & CloSurfTemp \tabularnewline
+T\(_{cla}\) & Clothing surface temperature (Absolute) & °K & - & AbsCloSurfTemp \tabularnewline
+T\(_{ra}\) & Mean radiant temperature & °K & - & AbsRadTemp \tabularnewline
+W & The rate of heat loss due to the performance of work & W/m\(^{2}\) & - & WorkEff \tabularnewline
+$\varepsilon$ & The emissivity of clothing-skin surface & - & - & SkinEmiss \tabularnewline
+$\sigma$ & The Stefan-Boltzman constant ( = 5.67×10  ) & W/m\(^{2}\)K\(^{4}\) & - & StefanBoltz \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Description of the model and algorithm}\label{description-of-the-model-and-algorithm}
+
+Fanger developed the model based on the research he performed at Kansas State University and the Technical University of Denmark. Fanger used the seven-point form of a thermal sensation scale along with numerous experiments involving human subjects in various environments. He related the subjects in response to the variables, which influence the condition of thermal comfort. Fanger's model is based upon an energy analysis that takes into account all the modes of energy loss (L) from the body, including: the convection and radiant heat loss from the outer surface of the clothing, the heat loss by water vapor diffusion through the skin, the heat loss by evaporation of sweat from the skin surface, the latent and dry respiration heat loss and the heat transfer from the skin to the outer surface of the clothing. The model assumes that the person is thermally at steady state with his environment.
+
+\(M = L\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\(L = {Q_{res}} + {Q_{dry}} + {E_{sk}} + W\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\({Q_{res}} = {E_{res}} + {C_{res}} = 0.000017M(5867 - {P_a}) + 0.0014M(34 - {T_a})\) ~~~~ W/m\(^{2}\)
+
+LatRespHeatLoss = 0.000017*ActLevel*(5867. - VapPress)
+
+DryRespHeatLoss = 0.0014*ActLevel*(34.- AirTemp)
+
+RespHeatLoss = LatRespHeatLoss + DryRespHeatLoss
+
+\({Q_c} = {h_c} \times {f_{cl}}({T_{cl}} - {T_a})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\) 
+
+{Q\(_{r}\) = 3.96*f\(_{l}\)*{[}(0.01*T\(_{a}\))\^{}4 - (0.01*T\(_{a}\))\^{}4{]}}~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\({Q_{dry}} = {Q_c} + {Q_r}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+ConvHeatLos = CloBodyRat*Hc*(CloSurfTemp - AirTemp)
+
+RadHeatLoss = 3.96*CloBodyRat \&
+
+*{[}(0.01*AbsCloSurfTemp)**4 - (0.01*AbsRadTemp)**4{]}
+
+DryHeatLoss = ConvHeatLoss + RadHeatLoss
+
+For\(H > 58.2\) , \({E_{rsw}} = 0.42(H - 58.2)\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+For \(H \le 58.2\) , \({E_{rsw}} = 0\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\) 
+
+{E\(_{f}\) = 0.00305*(5733.0 - 6.99H - P\(_{a}\))}~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\({E_{sk}} = {E_{rsw}} + {E_{diff}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+EvapHeatLossRegComf = 0.42*(IntHeatProd - ActLevelConv)
+
+EvapHeatLossRegComf = 0.0
+
+EvapHeatLossDiff = 0.00305*(5733.0 - 6.99*IntHeatProd - VapPress)
+
+EvapHeatLoss = EvapHeatLossRegComf + EvapHeatLossDiff
+
+The Fanger model was developed using the thermal sensation votes from subjects at KSU and Denmark, and the Predicted Mean Vote (PMV) thermal sensation scale is based on how the energy loss (L) deviates from the metabolic rate (M) in the following form:
+
+\begin{equation}
+PMV = (0.303{e^{ - 0.036M}} + 0.028)(H - L)
+\end{equation}
+
+ThermSensTransCoef = 0.303*EXP(-0.036*ActLevel) + 0.028
+
+PMV = ThermSensTransCoef*(IntHeatProd - EvapHeatLoss - RespHeatLoss - DryHeatLoss)
+
+Predicted Percent of Dissatisfied (PPD) people at each PMV is calculated as follows:
+
+PPD = 100.0 - 95.0*EXP(-0.03353*PMV**4 - 0.2179*PMV**2)
+
+\subsection{Pierce Two-Node Model}\label{pierce-two-node-model}
+
+The Pierce Two-Node model was developed at the John B. Pierce Foundation at Yale University. The model has been continually expanding since its first publication in 1970 (Gagge et.al. 1970). The most recent version on the model appears in the 1986 ASHRAE Transactions (Gagge et.al. 1986).
+
+\subsubsection{Pierce Two-Node Model Nomenclature List}\label{pierce-two-node-model-nomenclature-list}
+
+% table 82
+\begin{longtable}[c]{p{1.2in}p{2.0in}p{0.8in}p{0.8in}p{1.2in}}
+\caption{Nomenclature list for Pierce Two-Node model \label{table:nomenclature-list-for-pierce-two-node-model}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units ~ & Range & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature list for Pierce Two-Node model} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units ~ & Range & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+C\(_{dil}\) & Constant for skin blood flow & ~ & ~ & SkinBloodFlowConst \tabularnewline
+C\(_{res}\) & The rate of dry respiratory heat loss & W/m\(^{2}\) & - & DryRespHeatLoss \tabularnewline
+C\(_{sw}\) & Proportionality constant for sweat control & g/m\(^{2}\)hr & ~ & SweatContConst \tabularnewline
+DISC & Predicted discomfort vote & - & (-5)-5 & DISC \tabularnewline
+E\(_{dif}\) & The rate of heat loss from the diffusion of water vapor through the skin & W/m\(^{2}\) & - & EvapHeatLossDiff \tabularnewline
+E\(_{max}\) & Maximum evaporative heat loss & W/m\(^{2}\) & ~ & EvapHeatLossMax \tabularnewline
+E\(_{sk}\) & Total evaporative heat loss from skin & W/m\(^{2}\) & ~ & EvapHeatLoss \tabularnewline
+E\(_{res}\) & The rate of latent respiratory heat loss & W/m\(^{2}\) & - & LatRespHeatLoss \tabularnewline
+E\(_{rsw}\) & The rate of heat loss from the evaporation of regulatory sweating & W/m\(^{2}\) & - & EvapHeatLossRegSweat \tabularnewline
+E\(_{rsw,req}\) & The rate of heat loss from the evaporation of regulatory sweating at the state of comfort & W/m\(^{2}\) & ~ & EvapHeatLossRegComf \tabularnewline
+ET* & Effective Temperature & °C & - & ET \tabularnewline
+f\(_{cl}\) & The ratio of clothed body & - & ~ & CloBodyRat \tabularnewline
+f\(_{eff}\) & The fraction of surface effective for radiation ( = 0.72) & - & - & RadSurfEff \tabularnewline
+H & Internal heat production rate of an occupant per unit area ( = M – W) & W/m\(^{2}\) & - & IntHeatProd \tabularnewline
+h & Combined heat transfer coefficient & W/m\(^{2}\)°C & ~ & H \tabularnewline
+h\(_{c}\) & Convective heat transfer coefficient & W/m\(^{2}\)°C & - & Hc \tabularnewline
+h\(_{e}\)’ & Combined evaporative heat transfer coefficient & W/(m\(^{2}\)kP\(_{a}\)) & ~ & - \tabularnewline
+h\(_{r}\) & Radiant heat transfer coefficient & W/m\(^{2}\)°C & - & Hr \tabularnewline
+I\(_{cl}\) & Clothing insulation & m\(^{2}\)°C/W & ~ & - \tabularnewline
+L & All the modes of energy loss from body & W/m\(^{2}\) & - & - \tabularnewline
+L\(_{ET*}\) & All the modes of energy loss from body at ET* & W/m\(^{2}\) & ~ & - \tabularnewline
+L\(_{SET*}\) & All the modes of energy loss from body at SET* & W/m\(^{2}\) & ~ & - \tabularnewline
+M & Metabolic rate per unit area & W/m\(^{2}\) & - & ActLevel \tabularnewline
+M\(_{act}\) & Metabolic heat production due to activity & W/m\(^{2}\) & ~ & - \tabularnewline
+M\(_{shiv}\) & Metabolic heat production due to shivering & W/m\(^{2}\) & ~ & ShivResponse \tabularnewline
+P\(_{a}\) & Water vapor pressure in ambient air & Torr & - & VapPress \tabularnewline
+PMV* & Predicted Mean Vote modified by ET* or SET* & - & (-4)-4 & PMVET PMVSET \tabularnewline
+P\(_{SET*}\) & Water vapor pressure at SET* & °C & ~ & StdVapPressSET \tabularnewline
+P\(_{sk}\) & Saturated water vapor pressure at required skin temperature & Torr & - & SatSkinVapPress \tabularnewline
+Q\(_{c}\) & The rate of convective heat loss & W/m\(^{2}\) & - & ConvHeatLoss \tabularnewline
+Q\(_{crsk}\) & Heat flow from core to skin & W/m\(^{2}\) & ~ & HeatFlow \tabularnewline
+Q\(_{dry}\) & Sensible heat flow from skin & W/m\(^{2}\) & ~ & DryHeatLoss \tabularnewline
+Q\(_{r}\) & The rate of radiative heat loss & W/m\(^{2}\) & - & RadHeatLoss \tabularnewline
+Q\(_{res}\) & The rate of respiratory heat loss & W/m\(^{2}\) & - & RespHeatLoss \tabularnewline
+S\(_{cr}\) & Heat storage in core compartment & W/m\(^{2}\) & ~ & CoreheatStorage \tabularnewline
+SET* & Standard Effective Temperature & °C & - & SET \tabularnewline
+SIG\(_{b}\) & Thermal signal of body & °C & ~ & BodyThermSigCold BodyThermSigWarm \tabularnewline
+SIG\(_{cr}\) & Thermal signal of core & °C & ~ & CoreThermSigCold CoreThermSigWarm \tabularnewline
+SIG\(_{sk}\) & Thermal signal of skin & °C & ~ & SkinThermSigCold SkinThermSigWarm \tabularnewline
+SKBF & Skin blood flow & L/m  hr & ~ & SkinBloodFlow \tabularnewline
+S\(_{sk}\) & Heat storage in skin compartment & W/m\(^{2}\) & ~ & SkinHeatStorage \tabularnewline
+S\(_{tr}\) & Constriction constant of skin blood flow for average person & ~ & ~ & Str \tabularnewline
+SW\(_{reg}\) & The rate of regulatory sweating & g/m\(^{2}\)hr & ~ & RegSweat \tabularnewline
+T\(_{a}\) & Air temperature & °C & - & AirTemp \tabularnewline
+T\(_{b}\) & Mean body temperature & ~ & ~ & AvgBodyTemp \tabularnewline
+T\(_{b-c}\) & Mean body temperature when DISC is zero (lower limit) & °C & ~ & AvgBodyTempLow \tabularnewline
+T\(_{b-h}\) & Mean body temperature when HSI is 100 (upper limit) & °C & ~ & AvgBodyTempHigh \tabularnewline
+T\(_{cl}\) & Clothing surface temperature & °C & - & CloSurfTemp \tabularnewline
+T\(_{cr}\) & Core or internal temperature & °C & - & CoreTemp \tabularnewline
+T\(_{r}\) & Mean radiant temperature & °C & - & RadTemp \tabularnewline
+TSENS & Thermal sensation vote & - & (-5)-5 & TSENS \tabularnewline
+T\(_{sk}\) & Skin temperature & °C & ~ & SkinTemp \tabularnewline
+W & The rate of heat loss due to the performance of work & W/m\(^{2}\) & - & WorkEff \tabularnewline
+w\(_{dif}\) & Skin wettedness due to diffusion trough the skin & ~ & ~ & SkinWetDiff \tabularnewline
+w\(_{rsw}\) & Skin wettedness due to regulatory sweating & ~ & ~ & SkinWetSweat \tabularnewline
+$\varepsilon$ & The emissivity of clothing-skin surface & - & - & SkinEmiss \tabularnewline
+$\sigma$ & The Stefan-Boltzman constant ( = 5.67×10  ) & W/m\(^{2}\)K\(^{4}\) & - & StefanBoltz \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Description of the model and algorithm}\label{description-of-the-model-and-algorithm-1}
+
+The Pierce model thermally lumps the human body as two isothermal, concentric compartments, one representing the internal section or core (where all the metabolic heat is assumed to be generated and the skin comprising the other compartment). This allows the passive heat conduction from the core compartment to the skin to be accounted for. The boundary line between two compartments changes with respect to skin blood flow rate per unit skin surface area (SKBF in L/h•m\(^{2}\)) and is described by alpha -- the fraction of total body mass attributed to the skin compartment (Doherty and Arens 1988).
+
+\begin{equation}
+\alpha  = 0.0417737 + 0.7451832/(SKBF + 0.585417)
+\end{equation}
+
+SkinMassRat = 0.0417737 + 0.7451832/(SkinBloodFlow + 0.585417)
+
+Furthermore, the model takes into account the deviations of the core, skin, and mean body temperature weighted by alpha from their respective setpoints. Thermoregulatory effector mechanisms (Regulatory sweating, skin blood flow, and shivering) are defined in terms of thermal signals from the core, skin and body (Doherty and Arens 1988).
+
+\(SI{G_{cr}} = {T_{cr}} - 36.8\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ °C
+
+\(SI{G_{sk}} = {T_{sk}} - 33.7\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ °C
+
+\(SI{G_b} = {T_b} - 36.49\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ °C
+
+SkinThermSigWarm = SkinTemp - SkinTempSet
+
+SkinThermSigCold = SkinTempSet - SkinTemp
+
+CoreThermSigWarm = CoreTemp - CoreTempSet
+
+CoreThermSigCold = CoreTempSet - CoreTemp
+
+BodyThermSigWarm = AvgBodyTemp - AvgBodyTempSet
+
+BodyThermSigCold = AvgBodyTempSet-AvgBodyTemp
+
+\(SKBF = (6.3 + C{}_{dil} \times SI{G_{cr}})/(1 + {S_{tr}} \times ( - SI{G_{sk}}))\) ~~~~~~~~~~~~~~~~~~~~~ L/hr•m\(^{2}\)
+
+VasodilationFac = SkinBloodFlowConst*CoreWarmDelTemp
+
+VasoconstrictFac = Str*SkinColdDelTemp
+
+SkinBloodFlow = (6.3 + VasodilationFac)/(1. + VasoconstrictFac)
+
+\(S{W_{reg}} = {C_{sw}}SI{G_b}{e^{(SI{G_{sk}}/10.7)}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ g/hr•m\(^{2}\)
+
+RegSweat = SweatContConst*BodyWarmDelTemp*EXP(SkinWarmDelTemp/10.7)
+
+\({M_{shiv}} = 19.4( - SI{G_{cr}})( - SI{G_{sk}})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+ShivResponse = 19.4*SkinThermSigCold*CoreThermSigCold
+
+The latest version of the Pierce model (Fountain and Huizenga 1997) discusses the concepts of SET* and ET*. The Pierce model converts the actual environment into a ``standard environment'' at a Standard Effective Temperature, SET*. SET* is the dry-bulb temperature of a hypothetical environment at 50\% relative humidity for subjects wearing clothing that would be standard for the given activity in the real environment. Furthermore, in this standard environment, the same physiological strain, i.e.~the same skin temperature and skin wettedness and heat loss to the environment, would exist as in the real environment. The Pierce model also converts the actual environment into a environment at an Effective Temperature, ET*, that is the dry-bulb temperature of a hypothetical environment at 50\% relative humidity and uniform temperature (Ta = MRT) where the subjects would experience the same physiological strain as in the real environment.
+
+In the latest version of the model it is suggested that the classical Fanged PMV be modified by using ET* or SET* instead of the operative temperature. This gives a new index PMV* which is proposed for dry or humid environments. It is also suggested that PMV* is very responsive to the changes in vapor permeation efficiency of the occupants clothing.
+
+\(M = {M_{act}} + {M_{shiv}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+ActLevel = ActLevel + ActShiv
+
+\(L = {Q_{res}} + {Q_{dry}} + {E_{sk}} + W\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\(\begin{array}{l}{Q_{res}} = {E_{res}} + {C_{res}} = 0.0023M(44 - {P_{a(torr)}}) + 0.0014M(34 - {T_a})\\ = 0.017251M(5.8662 - {P_{a(kPa)}}) + 0.0014M(34 - {T_a})\end{array}\) W/m\(^{2}\)
+
+LatRespHeatLoss = 0.017251*ActLevel*(5.8662 - VapPress)
+
+DryRespHeatLoss = 0.0014*ActLevel*(34.- AirTemp)
+
+RespHeatLoss = LatRespHeatLoss + DryRespHeatLoss
+
+\({Q_c} = {h_c} \times {f_{cl}}({T_{cl}} - {T_a})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\({Q_r} = {h_r} \times {f_{cl}}({T_{cl}} - {T_r})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\({Q_{dry}} = {Q_c} + {Q_r}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+DryHeatLoss = CloBodyRat*(Hc*(CloSurfTemp - AirTemp) + Hr*(CloSurfTemp - RadTemp))
+
+In Pierce model, the convective heat transfer coefficient, h\(_{c}\), varies with the air velocity around body and metabolic rate. The model uses the maximum value of following equations.
+
+\({h_c} = 8.6 \times {v^{_{0.53}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)°C
+
+\({h_c} = 5.66{(M/58.2 - 0.85)^{0.39}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)°C
+
+Hc = 8.6*AirVel**0.53
+
+HcAct = 5.66*(ActMet - 0.85)**0.39
+
+Also, in the model, the radiant heat transfer coefficient, h\(_{r}\), is defined by following equation (Doherty and Arens 1988):
+
+\({h_r} = 4. \times {f_{eff}}\varepsilon \sigma {(({T_{cl}} + {T_r})/2 + 273.15)^3}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)°C
+
+Hr = 4.*RadSurfEff*StefanBoltz*((CloSurfTemp + RadTemp)/2. + TAbsConv)**3
+
+In the Pierce model, T\(_{cl}\) is estimated by each iteration using following equation:
+
+\({T_{cl}} = ({T_{sk}}/{I_{cl}} + {f_{cl}}({h_c}{T_a} - {h_r}{T_r}))/(1/{I_{cl}} + {f_{cl}}({h_c} + {h_r}))\) ~~~~~~~~~~~~~ °C
+
+CloSurfTemp = (CloCond*SkinTemp + CloBodyRat*(Hc*AirTemp \&
+
+\begin{itemize}
+\tightlist
+\item
+  Hr*RadTemp))/(CloCond + CloBodyRat*(Hc + Hr))
+\end{itemize}
+
+Total evaporative heat loss from the skin, E\(_{sk}\), includes evaporation of water produced by regulatory sweating, E\(_{rsw}\), and evaporation of water vapor that diffuses through the skin surface, E\(_{diff}\).
+
+\({E_{sk}} = {E_{rsw}} + {E_{diff}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+EvapHeatLoss = EvapHeatLossRegSweat + EvapHeatLossRegDiff
+
+\({E_{rsw}} = 0.68 \times S{W_{reg}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\({E_{diff}} = {w_{diff}} \times {E_{\max }}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+RegHeatLoss = 0.68*RegSweat
+
+DiffHeatLoss = SkinWetDiff*MaxEvapHeatLoss
+
+Where,
+
+0.68 is the passive water vapor diffusion rate in g/h·m\(^{2}\)·Torr
+
+and,
+
+\begin{equation}
+{w_{diff}} = 0.06(1 - {w_{rsw}})
+\end{equation}
+
+\({E_{\max }} = {h_e}'({P_{sk}} - {P_a})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\begin{equation}
+{w_{rsw}} = {E_{rsw}}/{E_{\max }}
+\end{equation}
+
+SkinWetDiff = (1.-SkinWetSweat)*.06
+
+MaxEvapHeatLoss = (1./TotEvapHeatResist)*(SatSkinVapPress - VapPress)
+
+SkinWetSweat = EvapHeatLossRegSweat/MaxEvapHeatLoss
+
+The Pierce model has one additional heat flow term describing the heat transfer between the internal core compartment and the outer skin shell (Doherty and Arens 1988).
+
+\({Q_{crsk}} = (5.28 + 1.163SKBF)({T_{cr}} - {T_{sk}})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+HeatFlow = (CoreTemp-SkinTemp)*(5.28 + 1.163*SkinBloodFlow)
+
+Where
+
+5.28 is the average body tissue conductance in W/m\(^{2}\)•°C
+
+1.163 is the thermal capacity of blood in W•h/L•°C
+
+Thus, individual heat balance equations for core and skin compartments are expressed using this term, Q\(_{c-s}\). New temperatures of core, skin and body are calculated by each iteration from rates of heat storage in the core and skin.
+
+\({S_{sk}} = {Q_{c - s}} - {Q_c} - {Q_r} - {E_{sk}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)°C
+
+SkinHeatStorage = HeatFlow - DryHeatLoss - EvapHeatLoss
+
+\({S_{cr}} = M - W - {Q_{res}} - {Q_{c - s}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)°C
+
+CoreHeatStorage = IntHeatProd - RespHeatLoss~ - HeatFlow
+
+Thus,
+
+\begin{equation}
+PMVET = (0.303{e^{ - 0.036M}} + 0.028)(H - {L_{ET*}})
+\end{equation}
+
+\begin{equation}
+PMVSET = (0.303{e^{ - 0.036M}} + 0.028)(H - {L_{SET*}})
+\end{equation}
+
+ThermSensTransCoef = 0.303*EXP(-0.036*ActLevel) + 0.028
+
+PMVET = ThermSensTransCoef*(IntHeatProd - EvapHeatLossDiff~ \&
+
+\begin{itemize}
+\tightlist
+\item
+  EvapHeatLossRegComf - RespHeatLoss - DryHeatLossET)
+\end{itemize}
+
+PMVSET = ThermSensTransCoef*(IntHeatProd - EvapHeatLossDiff~ \&
+
+\begin{itemize}
+\tightlist
+\item
+  EvapRegHeatLossReg Comf - RespHeatLoss - DryHeatLossSET)
+\end{itemize}
+
+Besides PMV*, the Pierce Two Node Model uses the indices TSENS and DISC as predictors of thermal comfort. Where TSENS is the classical index used by the Pierce foundation, and is a function of the mean body temperature. DISC is defined as the relative thermoregulatory strain that is needed to bring about a state of comfort and thermal equilibrium. DISC is a function of the heat stress and heat strain in hot environments and equal to TSENS in cold environments. In summary, the Pierce Model, for our purposes, uses four thermal comfort indices; PMVET-a function of ET*, PMVSET- a function of SET*, TSENS and DISC.
+
+\({T_{b - c}} = (0.185/58.2)(M - W) + 36.313\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ °C
+
+\({T_{b - h}} = (0.359/58.2)(M - W) + 36.664\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ °C
+
+\(TSEN{S_c} = 0.68175({T_b} - {T_{b - c}})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \({T_b} \le {T_{b - c}}\)
+
+\(TSEN{S_h} = 4.7({T_b} - {T_{b - c}})/({T_{b - h}} - {T_{b - c}})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \({T_b} > {T_{b - c}}\)
+
+\begin{equation}
+DISC = 5.({E_{rsw}} - {E_{rsw - comf}})/({E_{\max }} - {E_{rsw - comf}} - {E_{diff}})
+\end{equation}
+
+AvgBodyTempLow = (0.185/ActLevelConv)*IntHeatProd + 36.313
+
+AvgBodyTempHigh = (0.359/ActLevelConv)*IntHeatProd + 36.664
+
+TSENS = .68175*(AvgBodyTemp-AvgBodyTempLow)
+
+TSENS = 4.7*(AvgBodyTemp - AvgBodyTempLow)/ \&
+
+(AvgBodyTempHigh - AvgBodyTempLow)
+
+DISC = 5.*(EvapHeatLossRegSweat - EvapHeatLossRegComf)/ \&
+
+(MaxEvapHeatLoss - EvapHeatLossRegComf - DiffHeatLoss)
+
+\subsection{KSU Two-Node Model}\label{ksu-two-node-model}
+
+The KSU two-node model, developed at Kansas State University, was published in 1977 (Azer and Hsu 1977). The KSU model is quite similar to that of the Pierce Foundation. The main difference between the two models is that the KSU model predicts thermal sensation (TSV) differently for warm and cold environment.
+
+\subsubsection{KSU Two Node Model Nomenclature List}\label{ksu-two-node-model-nomenclature-list}
+
+% table 83
+\begin{longtable}[c]{p{1.2in}p{2.0in}p{0.8in}p{0.8in}p{1.2in}}
+\caption{  Nomenclature list for KSU Two-Node model \protect \label{table:nomenclature-list-for-ksu-two-node-model}}\\
+\toprule 
+Mathematical variable & Description & Units ~ & Range & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature list for KSU Two-Node model} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units ~ & Range & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+C\(_{cr}\) & Specific heat of body core & Whr/kg°C & ~ & ~ \tabularnewline
+C\(_{sk}\) & Specific heat of skin & Whr/kg°C & ~ & ~ \tabularnewline
+C\(_{res}\) & The rate of dry respiratory heat loss & W/m\(^{2}\) & - & DryRespHeatLoss \tabularnewline
+E\(_{dif}\) & The rate of heat loss from the diffusion of water vapor through the skin & W/m\(^{2}\) & - & EvapHeatLossDiff \tabularnewline
+E\(_{max}\) & Maximum evaporative heat loss & W/m\(^{2}\) & ~ & EvapHeatLossMax \tabularnewline
+E\(_{sk}\) & Total evaporative heat loss from skin & W/m\(^{2}\) & ~ & EvapHeatLoss \tabularnewline
+E\(_{sw}\) & Equivalent evaporation heat loss from the sweat secreted & W/m\(^{2}\) & ~ & EvapHeatLossSweat \tabularnewline
+E\(_{sw.d}\) & Sweat function for warm and dry skin & W/m\(^{2}\) & ~ & DrySweatRate \tabularnewline
+E\(_{res}\) & The rate of latent respiratory heat loss & W/m\(^{2}\) & - & LatRespHeatLoss \tabularnewline
+F\(_{cl}\) & The Burton thermal efficiency factor for clothing & ~ & - & CloThermEff \tabularnewline
+F\(_{pcl}\) & Permeation efficiency factor for clothing & ~ & - & CloPermeatEff \tabularnewline
+H & Internal heat production rate of an occupant per unit area = M - W & W/m\(^{2}\) & - & IntHeatProd \tabularnewline
+H & Combined heat transfer coefficient & W/m\(^{2}\)°C & ~ & H \tabularnewline
+h\(_{c}\) & Convective heat transfer coefficient & W/m\(^{2}\)°C & - & Hc \tabularnewline
+h\(_{r}\) & Radiant heat transfer coefficient & W/m\(^{2}\)°C & - & Hr \tabularnewline
+KS & Overall skin thermal conductance & W/m\(^{2}\)°C & ~ & ThermCndct \tabularnewline
+KS\(_{o}\) & Skin conductance at thermal neutrality & W/m\(^{2}\)°C & ~ & ThermCndctNeut \tabularnewline
+KS\(_{-4}\) & Skin conductance at thermal sensation very cold & W/m\(^{2}\)°C & ~ & ThermCndctMin \tabularnewline
+M & Metabolic rate per unit area & W/m\(^{2}\) & - & ActLevel \tabularnewline
+M\(_{shiv}\) & Metabolic heat production due to shivering & W/m\(^{2}\) & ~ & ShivResponse \tabularnewline
+P\(_{a}\) & Water vapor pressure in ambient air & Torr & - & VapPress \tabularnewline
+P\(_{sk}\) & Saturated water vapor pressure at required skin temperature & Torr & - & SatSkinVapPress \tabularnewline
+PT\(_{accl}\) & The pattern of acclimation & ~ & ~ & AcclPattern \tabularnewline
+Q\(_{c}\) & The rate of convective heat loss & W/m\(^{2}\) & - & ConvHeatLoss \tabularnewline
+Q\(_{dry}\) & Sensible heat flow from skin & W/m\(^{2}\) & ~ & DryHeatLoss \tabularnewline
+Q\(_{r}\) & The rate of radiative heat loss & W/m\(^{2}\) & - & RadHeatLoss \tabularnewline
+Q\(_{res}\) & The rate of respiratory heat loss & W/m\(^{2}\) & - & RespHeatLoss \tabularnewline
+RH & Relative humidity & ~ & ~ & RelHum \tabularnewline
+T\(_{a}\) & Air temperature & °C & - & AirTemp \tabularnewline
+T\(_{cr}\) & Core or internal temperature & °C & - & CoreTemp \tabularnewline
+T\(_{o}\) & Operative temperature & °C & - & OpTemp \tabularnewline
+T\(_{r}\) & Mean radiant temperature & °C & - & RadTemp \tabularnewline
+T\(_{sk}\) & Skin temperature & °C & ~ & SkinTemp \tabularnewline
+TSV & Thermal sensation vote & ~ & (-4)-4 & TSV \tabularnewline
+V & Relative air velocity & m/s & - & AirVel \tabularnewline
+W & The rate of heat loss due to the performance of work & W/m\(^{2}\) & - & WorkEff \tabularnewline
+W & Skin wettedness & - & - & SkinWet \tabularnewline
+W\(_{cr}\) & Mass of body core per unit body surface & kg/m\(^{2}\) & ~ & - \tabularnewline
+w\(_{rsw}\) & Skin wettedness due to regulatory sweating & ~ & ~ & SkinWetSweat \tabularnewline
+w\(_{rsw-o}\) & Skin wettedness at thermal neutrality & ~ & ~ & SkinWetSweatNeut \tabularnewline
+W\(_{sk}\) & Mass of skin per unit body surface & kg/m\(^{2}\) & ~ & - \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Description of the model and algorithm}\label{description-of-the-model-and-algorithm-2}
+
+The KSU two-node model is based on the changes that occur in the thermal conductance between the core and the skin temperature in cold environments, and in warm environments it is based on changes in the skin wettedness.
+
+In this model metabolic heat production is generated in the core which exchanges energy with the environment by respiration and the skin exchanges energy by convection and radiation. In addition, body heat is dissipated through evaporation of sweat and/or water vapor diffusion through the skin. These principles are used in following passive system equations.
+
+\({W_{cr}}{C_{cr}}d{T_{cr}}/dt = M - W - {Q_{res}} - KS({T_{cr}} - {T_{sk}})\) ~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\({W_{sk}}{C_{sk}}d{T_{sk}}/dt = KS({T_{cr}} - {T_{sk}}) - {Q_{dry}} - {E_{sk}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+Where
+
+\({Q_{res}} = {E_{res}} + {C_{res}} = 0.0023M(44 - {P_{a(torr)}}) + 0.0014M(34 - {T_a})\) ~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+LatRespHeatLoss = 0.0023*ActLevelTot*(44. - VapPress)
+
+DryRespHeatLoss = 0.0014*ActLevelTot*(34. - AirTemp)
+
+RespHeatLoss = LatRespHeatLoss + DryRespHeatLoss
+
+\({Q_{dry}} = {Q_c} + {Q_r} = {h_{}}{f_{cl}}{F_{cl}}({T_{sk}} - {T_o})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+DryHeatLoss = H*CloBodyRat*CloThermEff*(SkinTemp - OpTemp)
+
+\(h = {h_c} + {h_r}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)°C
+
+\({h_c} = 8.3\sqrt v\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)°C
+
+\({h_r} = 3.87 + 0.031{T_r}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)°C
+
+H = Hc + Hr
+
+Hc = 8.3*SQRT(AirVel)
+
+Hr = 3.87 + 0.031*RadTemp
+
+\({T_o} = ({h_c}{T_a} + {h_r}{T_r})/({h_c} + {h_r})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ °C
+
+OpTemp = (Hc*AirTemp + Hr*RadTemp)/H
+
+and
+
+For \({E_{sw}} \le {E_{\max }}\) , \({E_{sk}} = {E_{sw}} + (1 - {w_{rsw}}){E_{diff}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+For \({E_{sw}} > {E_{\max }}\) , \({E_{sk}} = {E_{\max }}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\({E_{diff}} = 0.408({P_{sk}} - {P_a})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+\({E_{\max }} = 2.2{h_c}{F_{pcl}}({P_{sk}} - {P_a})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+EvapHeatLoss = SkinWetSweat*EvapHeatLossMax+(1. - SkinWetSweat)*EvapHeatLossDiff
+
+SkinWetSweat = EvapHeatLossDrySweat/EvapHeatLossMax
+
+EvapHeatLossDiff = 0.408*(SkinVapPress - VapPress)
+
+EvapHeatLossMax = 2.2*Hc*(SkinVapPress - VapPress)*CloPermeatEff
+
+Here, control signals, based on setpoint temperatures in the skin and core, are introduced into passive system equations and these equations are integrated numerically for small time increments or small increments in core and skin temperature. The control signals modulate the thermoregulatory mechanism and regulate the peripheral blood flow, the sweat rate, and the increase of metabolic heat by active muscle shivering. The development of the controlling functions of skin conductance (KS), sweat rate (E\(_{sw}\)), and shivering (M\(_{shiv}\)) is based on their correlation with the deviations in skin and core temperatures from their setpoints.
+
+\begin{equation}
+  KS = 5.3 + \frac{6.75+42.45\PB{T_{cr}-36.98}+8.15\PB{T_{cr}-35.15}^{0.8}\PB{T_{sk}-33.8}}{1+0.4\PB{32.1-T_{sk}}}
+\end{equation}
+
+SkinCndctDilation = 42.45*CoreSignalWarmMax \&
+
+\begin{itemize}
+\tightlist
+\item
+  8.15*CoreSignalSkinSens**0.8*SkinSignalWarmMax
+\end{itemize}
+
+SkinCndctConstriction = 1.0 + 0.4*SkinSignalColdMax
+
+ThermCndct = 5.3+(6.75+SkinCndctDilation)/SkinCndctConstriction
+
+\begin{equation}
+  E_{sw} = \phi \frac{\RB{260\PB{T_{cr} - 36.9} + 26\PB{T_{sk} - 33.8}} \exp\RB{\PB{T_{sk} - 33.8}/8.5}}{1.0 + 0.05\PB{33.37 - T_{sk}}^{2.4}}
+\end{equation}
+
+WeighFac = 260.+70.*AcclPattern
+
+SweatCtrlFac = 1. + 0.05*SkinSignalSweatColdMax**2.4
+
+DrySweatRate = ((WeighFac*CoreSignalSweatMax \&
+
+\begin{itemize}
+\tightlist
+\item
+  0.1*WeighFac*SkinSignalSweatMax) \&
+\end{itemize}
+
+*EXP(SkinSignalSweatMax/8.5))/SweatCtrlFac
+
+Where
+
+\(\phi = 1.0\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \(w \le 0.4\)
+
+\(\phi = 0.5 + 0.5\exp [ - 5.6(w - 0.4)]\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \(w > 0.4\)
+
+SweatSuppFac = 1.
+
+SweatSuppFac = 0.5 + 0.5*EXP(-5.6*SkinWetSignal)
+
+\({M_{shiv}} = 20(36.9 - {T_{cr}})(32.5 - {T_{sk}}) + 5(32.5 - {T_{sk}})\) ~~~~~~~~~~~~~~~~~~~~ W/m\(^{2}\)
+
+ShivResponse = 20.*CoreSignalShivMax*SkinSignalShivMax + 5.*SkinSignalShivMax
+
+In KSU model, two new parameters are introduced and used in correlating thermal sensations with their associated physiological responses. In stead of correlating warm thermal sensations with skin wettedness, it is here correlated with a wettedness factor defined by
+
+\begin{equation}
+{\varepsilon_{wsw}} = ({w_{rsw}} - {w_{rsw - o}})/(1.0 - {w_{rsw - o}})
+\end{equation}
+
+SkinWetFac = (SkinWetSweat - SkinWetNeut)/(1. - SkinWetNeut)
+
+Where
+
+\begin{equation}
+{w_{wsw}} = {E_{sw}}/{E_{\max }}
+\end{equation}
+
+\begin{equation}
+{w_{wsw - o}} = 0.2 + 0.4\{ 1.0 - \exp [ - 0.6(H/58.2 - 1.0)]\}
+\end{equation}
+
+SkinWetSweat = DrySweatRate/EvapHeatLossMax
+
+SkinWetNeut = 0.02 + 0.4*(1.-EXP(-0.6*(IntHeatProdMetMax - 1.)))
+
+and instead of correlating cold thermal sensation with the skin temperature, it is here correlated with a factor identified as vasoconstriction factor defined by
+
+\begin{equation}
+{\varepsilon_{vc}} = (K{S_o} - KS)/(K{S_o} - K{S_{( - 4)}})
+\end{equation}
+
+VasoconstrictFac = (ThermCndctNeut - ThermCndct) \&
+
+/(ThermCndctNeut - ThermCndctMin)
+
+Thus, TSV in the cold is a function of a vasoconstriction factor (ε\(_{vc}\)) as:
+
+\begin{equation}
+TSV =  - 1.46 \times {\varepsilon_{vc}} + 3.75 \times {\varepsilon_{vc}}^2 - 6.17 \times {\varepsilon_{vc}}^3
+\end{equation}
+
+TSV = -1.46153*VasoconstrictFac + 3.74721*VasoconstrictFac**2 \&
+
+~~~~~~~~~~~~~~~~ - 6.168856*VasoconstrictFac**3
+
+and for the warm environments, TSV is defined as:
+
+\begin{equation}
+TSV = [5.0 - 6.56(RH - 0.5)] \times {\varepsilon_{wsw}}
+\end{equation}
+
+TSV = (5. - 6.56*(RelHum - 0.50))*SkinWetFac
+
+The KSU model's TSV was developed from experimental conditions in all temperature ranges and from clo levels between .05 clo to 0.7 clo and from activities levels of 1 to 6 mets (Berglund 1978).
+
+\textbf{Adaptive Comfort Model}
+
+Adaptive comfort model, intended for use in naturally ventilated buildings, determines the acceptability of indoor conditions given the monthly mean outdoor air temperature and the indoor operative temperature. This is used as an index for occupant adaptation to outdoor conditions, and determines the acceptability of indoor conditions. The model also accounts for people's clothing adaptation in naturally conditioned spaces by relating the acceptable range of indoor temperatures to the outdoor climate, so it is not necessary to estimate the clothing values for the space. No humidity or air-speed limits are required when this option is used. This section summarizes the adaptive comfort models based on the ASHRAE Standard 55-2010 and CEN 15251. Details are available in the two standards.
+
+\textbf{Adaptive Comfort Model Based on ASHRAE Standard 55-2010}
+
+In ASHRAE Standard 55, the monthly mean outdoor air temperature, used in the adaptive comfort model, is defined as the simple running average of the previous thirty daily average outdoor air temperatures.
+
+The model defines two comfort regions: 80\% Acceptability, and 90\% Acceptability. If the monthly mean outdoor air temperature is not within the specified domain of 10.0 to 33.5C, the model is not applicable.
+
+\begin{figure}[hbtp] % fig 302
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6814.png}
+\caption{Acceptable operative temperature ranges for naturally conditioned spaces (ASHRAE Standard 55-2010) \protect \label{fig:acceptable-operative-temperature-ranges-for}}
+\end{figure}
+
+The central line of the model (shown in red), or comfort temperature, is defined as
+
+\begin{equation}
+{T_{ot}} = 0.31\cdot {T_o} + 17.8
+\end{equation}
+
+Where
+
+T\(_{ot}\) -- operative temperature (°C), calculated as the average of the indoor air dry-bulb temperature and the mean radiant temperature of zone inside surfaces
+
+T\(_{o}\) -- monthly mean outdoor air dry-bulb temperature (°C).
+
+If the .stat file is provided for the simulation, T\(_{o}\) is drawn directly from the daily average temperatures in the .stat file, which provides a value for each month.~ If no .stat file is provided, the monthly mean outdoor temperature is a simple running average of the previous thirty daily average temperatures, calculated directly from the weather file (.epw):
+
+\begin{equation}
+{T_o} = \frac{{\left( {{T_{od - 1}} + {T_{od - 2}} + ... + {T_{od - 30}}} \right)}}{{30}}
+\end{equation}
+
+\begin{equation}
+{T_o} = (1 - \alpha )\cdot {T_{od - 1}} + \alpha \cdot {T_{od - 1}}
+\end{equation}
+
+\begin{equation}
+\alpha  = \frac{{29}}{{30}}
+\end{equation}
+
+T\(_{od-i}\) is defined as the daily average temperature of the i\(^{th}\) previous day.
+
+Note that the weather file must be a standard .epw containing a full year of data.
+
+The comfort regions for 80\% and 90\% acceptability are symmetric about the central line.
+
+90\% Acceptability Limits: T\(_{ot}\) = 0.31* T\(_{o}\) + 17.8± 2.5
+
+80\% Acceptability Limits: T\(_{ot}\) = 0.31* T\(_{o}\) + 17.8± 3.5
+
+If, using either method, T\(_{o}\) is less than 10°(C) or greater than 33.5°(C), the model is not applicable.
+
+For a detailed description of this model, please see \emph{ASHRAE Standard 55-2010, Thermal Environmental Conditions for Human Occupancy}.
+
+\subsection{Adaptive Comfort Model Based on European Standard EN15251-2007}\label{adaptive-comfort-model-based-on-european-standard-en15251-2007}
+
+The EN15251-2007 is similar to ASHRAE 55-2010, but with slightly different curves of the indoor operative temperature and acceptability limits (Fig. 2). The model, intended for use in naturally ventilated buildings, determines the acceptability of indoor conditions given the 7-day weighted mean outdoor air temperature and the indoor operative temperature. The 7-day weighted mean outdoor air temperature (T\(_{rm}\)) is defined as the weighted running average of the previous 7 daily average outdoor air temperatures.
+
+This weighted running average is calculated from a full annual weather file that must be specified for the simulation. This is used as an index for occupant adaptation to outdoor conditions, and determines the acceptability of indoor conditions. The model also accounts for people's clothing adaptation in naturally conditioned spaces by relating the acceptable range of indoor temperatures to the outdoor climate, so it is not necessary to estimate the clothing values for the space. No humidity or air-speed limits are required when this option is used. The model defines three comfort regions: Category I (90\%) Acceptability, Category II (80\%) Acceptability, and Category III (65\%) Acceptability. If T\(_{rm}\) is not within the specified domain of 10.0 to 30.0C, the model is not applicable.
+
+\begin{figure}[hbtp] % fig 303
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6819.png}
+\caption{Categories for European Standard EN15251-2007 \protect \label{fig:categories-for-european-standard-en15251-2007}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 304
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6820.png}
+\caption{Acceptable operative temperature ranges for naturally conditioned spaces (CEN EN15251-2007) \protect \label{fig:acceptable-operative-temperature-ranges-for-001}}
+\end{figure}
+
+Central line (shown as redFigure~\ref{fig:acceptable-operative-temperature-ranges-for-001}): Tot = 0.33*To + 18.8
+
+Category I, 90\% Acceptability Limits: Tot = 0.33*To + 18.8± 2.0
+
+Category II, 80\% Acceptability Limits: Tot = 0.33*To + 18.8± 3.0
+
+Category III, 65\% Acceptability Limits: Tot = 0.33*To + 18.8± 4.0
+
+For 10°(C) \textless{} T\(_{rm}\) \textless{} 15°(C), the comfort temperature of the lower boundaries of the comfort regions is T\(_{comf}\) = 23.75°(C). That is, the lower boundaries are constant according to the same ranges above:
+
+Category I, 90\% Acceptability Limits: Tot = 23.75- 2.0
+
+Category II, 80\% Acceptability Limits: Tot = 23.75 - 3.0
+
+Category III, 65\% Acceptability Limits: Tot = 23.75 -4.0
+
+Where
+
+Tot -- operative temperature (°C) , calculated as the average of the indoor air dry-bulb temperature and the mean radiant temperature of zone inside surfaces
+
+To -- mean outdoor air dry-bulb temperature (°C), calculated as the weighted mean of the previous 7-day daily mean outdoor air dry-bulb temperature (T\(_{od}\)):
+
+T\(_{o}\) = (1 - α)*\{T\(_{od-1}\) + α *T\(_{od-2}\) + α\(^{2}\) *T\(_{od-3}\) + α\(^{3}\) *T\(_{od-4}\) + α\(^{4}\) *T\(_{od-5}\) + α\(^{5}\) *T\(_{od-6}\) + α\(^{6}\) *T\(_{od-7}\)\}
+
+T\(_{o}\) = (1 - α)*T\(_{od-1}\) + α *T\(_{o-1}\)
+
+α~ = 0.8
+
+\subsection{Dynamic Clothing Model}\label{dynamic-clothing-model}
+
+In most building energy simulations, thermal comfort condition is calculated based on the assumption that the clothing insulation is equal to a constant value of 0.5 clo during the cooling season and 1.0 clo during heating season. Usually those two values are used and the change from 0.5 to 1 or vice-versa is made suddenly from one day to another. In addition, there is no standardized guideline on how to set clothing insulation schedules in the international standards. This simplified assumption may lead to systems that are incorrectly sized and operated and to the incorrect assessment of comfort conditions. In reality, occupants frequently adjust their clothing depending on the thermal conditions around them, as opposed to the assumption of constant clothing values. Therefore, the clothing insulation variation should be captured during the building simulation to realistically model HVAC systems. In order to overcome the limitations of the constant clothing insulation assumption, three new predictive clothing insulation models were developed by Schiavon and Lee (2012) based on 6,333 selected observations taken from ASHRAE RP-884 and RP-921 databases. The first and third models vary the clothing insulation as a function of outdoor air temperature measured at 6 o'clock and the second model takes into account both 6 o'clock outdoor air temperature and indoor operative temperature when adjusting the clothing insulation. The dynamic clothing models should be implemented in dynamic building energy simulation.
+
+The model proposed to ASHRAE 55 is described below.
+
+For t\(_{a(out,6)}\) \textless{} -5°C, \({I_{cl}} = 1\) .00
+
+For -5°C ≤ t\(_{a(out,6)}\) \textless{} 5°C, \({I_{cl}} = 0.818 - 0.0364{\rm{*}}{t_{a\left( {out,6} \right)}}\)
+
+For 5°C ≤ t\(_{a(out,6)}\) \textless{} 26°C \({I_{cl}} = {10^{\left( { - 0.1635 - 0.0066{\rm{*}}{t_{a\left( {out,6} \right)}}} \right)}}\)
+
+or t\(_{a(out,6)}\) ≥ 26°C \({I_{cl}} = 0.46\)
+
+Where, \emph{I\(_{cl}\)} is the clothing insulation value, \emph{t\(_{a(out,\, 6)}\)} is the outdoor air temperature measured at 6 o'clock in the morning. The following figure illustrates the proposed clothing insulation model.
+
+\begin{figure}[hbtp] % fig 305
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6825.png}
+\caption{Clothing Schedule Illustration \protect \label{fig:clothing-schedule-illustration}}
+\end{figure}
+
+In the figure above, clothing insulation schedule for a fixed model (blue) typically used in energy simulation software and for the clothing model based on outdoor air temperature measured at 6 o'clock. Climate data for Chicago O'hare International Airport has been used.
+
+The following figure illustrates the new clothing insulation model.
+
+\begin{figure}[hbtp] % fig 306
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6826.png}
+\caption{Graphical representation of the proposed clothing insulation model \protect \label{fig:graphical-representation-of-the-proposed}}
+\end{figure}
+
+The dynamic predictive clothing insulation model is implemented into EnergyPlus for realistic energy simulation. Addenda A to ASHRAE 55 with the clothing model has been approved by the ASHRAE committee and the chance to be included in ASHRAE 55-2013 is high.
+
+\subsubsection{References}\label{references-033}
+
+Schiavon S, Lee KH. 2013. Dynamic predictive clothing insulation models based on outdoor air and indoor operative temperatures. Building and Environment. Volume 59, 250-260. \url{http://dx.doi.org/10.1016/j.buildenv.2012.08.024} ~(link to the journal) \url{http://escholarship.org/uc/item/3338m9qf} ~(link to the freely available pre-print version)
+
+Lee KH, Schiavon S. 2013. Influence of three dynamic predictive clothing insulation models on building energy use, HVAC sizing and thermal comfort. Submitted to Journal. \url{http://escholarship.org/uc/item/3sx6n876}~ (link to the freely available pre-print version)
+
+\subsection{Mean Radiant Temperature Calculation}\label{mean-radiant-temperature-calculation}
+
+There are three options to calculate mean radiant temperature in the thermal comfort models. One is the zone averaged MRT, another is the surface weighted MRT, and the other is angle factor MRT. The zone averaged MRT is calculated on the assumption that a person is in the center of a space, whereas the surface weighted MRT is calculated in consideration of the surface that a person is closest to, and the angle factor MRT is calculated based on angle factors between a person and the different surfaces in a space. Here, the surface weighted MRT is the average temperature of the selected surface and zone averaged MRT and is intended to represent conditions in the limit as a person gets closer and closer to a particular surface.~ In that limit, half of the person's radiant field will be dominated by that surface and the other half will be exposed to the rest of the zone.~ Note that the surface weighted MRT is only an approximation. The angle factor MRT is the mean temperature of the surrounding surface temperatures weighted according to the magnitude of the respective angle factors and allows the user to more accurately predict thermal comfort at a particular location within a space.
+
+% table 84
+\begin{longtable}[c]{p{1.2in}p{2.0in}p{0.8in}p{0.8in}p{1.2in}}
+\caption{Nomenclature and variable list for MRT calculation \label{table:nomenclature-and-variable-list-for-mrt}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units ~ & Range & FORTRAN variable \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature and variable list for MRT calculation} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units ~ & Range & FORTRAN variable \tabularnewline
+\midrule
+\endhead
+
+T\(_{r}\) & Mean radiant temperature & °C & - & RadTemp \tabularnewline
+T\(_{r-avg}\) & Zone averaged radiant temperature & °C & - & ZoneRadTemp \tabularnewline
+T\(_{surf}\) & Surface temperature & °C & - & SurfaceTemp \tabularnewline
+F\(_{surf}\) & Angle factor between person and surface & - & 0-1 & AngleFactor \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Description of the model and algorithm}\label{description-of-the-model-and-algorithm-3}
+
+The zone averaged MRT is calculated without weighting any surface temperature of the space.
+
+\begin{equation}
+{T_r} = {T_{r - avg}}
+\end{equation}
+
+RadTemp = MRT(ZoneNum)
+
+The surface weighted MRT is the average temperature of the zone averaged MRT and the temperature of the surface that a person is closest to.
+
+\begin{equation}
+{T_r} = ({T_{r - avg}} + {T_{surf}})/2
+\end{equation}
+
+ZoneRadTemp = MRT(ZoneNum)
+
+SurfaceTemp = GetSurfaceTemp(People(PeopleNum)\%SurfacePtr)
+
+RadTemp = (ZoneRadTemp + SurfaceTemp)/2.0
+
+The angle factor MRT is the mean value of surrounding surface temperatures weighted by the size of the respective angle factors between a person and each surface.
+
+\begin{equation}
+{T_r} = {T_{surf - 1}}{F_{surf - 1}} + {T_{surf - 2}}{F_{surf - 2}} + ......... + {T_{surf - n}}{F_{surf - n}}
+\end{equation}
+
+SurfTempAngleFacSummed = SurfTempAngleFacSummed \&
+
+\begin{itemize}
+\tightlist
+\item
+  SurfaceTemp * AngleFactorList(AngleFacNum)\%AngleFactor(SurfNum)
+\end{itemize}
+
+RadTemp = SurfTempAngleFacSummed
+
+\subsection{References}\label{references-1-012}
+
+ASHRAE. 1984. ``High Intensity Infrared Radiant Heating'', 1984 Handbook of Systems and Equipment, American Society of Heating, Refrigerating and Air Conditioning Engineers, Atlanta, GA, Chapter 18.
+
+ASHRAE. 1985. ``Physiological Principles for Comfort and Health,'' 1985 Handbook of Fundamentals, American Society of Heating, Refrigerating and Air Conditioning Engineers, Atlanta, GA, Chapter 8.
+
+ASHRAE. 1993. ``Physiological Principles and Thermal Comfort'', 1993 ASHRAE Handbook of Fundamentals, American Society of Heating, Refrigerating and Air Conditioning Engineers, Atlanta, GA, Chapter 8.
+
+ASHRAE. 2010. ``Standard 55-2010 -- Thermal Environmental Conditions for Human Occupancy (ANSI approved)'', American Society of Heating, Refrigerating and Air Conditioning Engineers, Atlanta, GA.
+
+Azer, N.Z., Hsu, S. 1977. ``The prediction of Thermal Sensation from Simple model of Human Physiological Regulatory Response'', ASHRAE Trans., Vol.83, Pt 1.
+
+Berglund, Larry. 1978. ``Mathematical Models for Predicting the Thermal Comfort Response of Building Occupants'', ASHRAE Trans., Vol.84.
+
+Doherty, T.J., Arens, E. 1988. ``Evaluation of the Physiological Bases of Thermal Comfort Models'', ASHRAE Trans., Vol.94, Pt 1.
+
+Du Bois, D. and E.F. 1916. ``A Formula to Estimate Approximate Surface Area, if Height and Weight are Known'', Archives of internal Medicine, Vol.17.
+
+CEN. 2007. ``Standard EN15251 Indoor environmental input parameters for design and assessment of energy performance of buildings addressing indoor air quality, thermal environment, lighting and acoustics''. Bruxelles: European committee for Standardisation.
+
+Fanger, P.O. 1970. Thermal Comfort-Analysis and Applications in Environmental Engineering, Danish Technical Press, Copenhagen.
+
+Fanger, P.O. 1986. ``Radiation and Discomfort'', ASHRAE Journal. February 1986.
+
+Fanger P.O. 1967. ``Calculation of Thermal Comfort: Introduction of a Basic Comfort Equation'', ASHRE Trans., Vol.73, Pt 2.
+
+Fountain, Marc.E., Huizenga, Charlie. 1997 ``A Thermal Sensation Prediction Tool for Use by the Profession'', ASHRAE Trans., Vol.103, Pt 2.
+
+Gagge, A.P., Stolwijk, J. A. J., Nishi, Y. 1970. ``An Effective Temperature Scale Based on a Simple Model of Human Physiological Regulatory Response'', ASHRAE Trans., Vol.70, Pt 1.
+
+Gagge, A.P., Fobelets, A.P., Berglund, L. G. 1986. ``A Standard Predictive Index of Human Response to the Thermal Environment'',~ ASHRAE Trans., Vol.92, Pt 2.
+
+Hsu, S. 1977. ``A Thermoregulatory Model for Heat Acclimation and Some of its Application'', Ph. D. Dissertation, Kansas State University.
+
+Int-Hout, D. 1990. ``Thermal Comfort Calculation / A Computer Model'', ASHRAE Trans., Vol.96, Pt 1.
+
+ISO. 1983. ``Determination of the PMV and PPD Indices and Specification of the Conditions for Thermal Comfort'', DIS 7730, Moderate Thermal Environment, 1983.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/trombe-walls.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/trombe-walls.tex
new file mode 100644
index 00000000000..47f0f36bcfe
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/trombe-walls.tex
@@ -0,0 +1,69 @@
+\section{Trombe Walls }\label{trombe-walls}
+
+Trombe walls are passive solar devices designed for thermal storage and delivery.~ It consists of a thick wall (150mm to 300mm) {[}8" to 16``{]} faced with a selective surface solar absorber, air gap, and high transmissivity glass pane.~ Trombe walls are usually South facing (in the Northern Hemisphere) for maximum sun exposure.~ An overhang above the wall is used to decrease exposure in the summer when the sun is high in the sky and heating is not required, yet still allows for full exposure in the winter when the sun is low in the sky and heating is desirable.
+
+In EnergyPlus, there is no Trombe wall object per se; rather, it is composed of other existing EnergyPlus objects in the input file (except for a special key choice for Zone Inside Convection Algorithm in the Zone input object).~ This approach provides flexibility in specifying the various wall parameters and allows the freedom to explore unusual configurations.~ On the other hand, this approach puts more of a burden on the user to be sure that all parts of the Trombe wall are correctly specified; otherwise unexpected results may be obtained.
+
+To simulate the Trombe wall, a very narrow zone is coupled to the desired surface via an interzone partition.~ The depth of the zone corresponds to the size of the air space usually 18mm to 150mm (¾" to 6``).~ In most cases the Trombe zone will be a sealed zone with no ventilation.~ The exterior wall of the Trombe zone contains a single or double-pane window.~ Optimally, the window covers nearly all of the wall area and has a very high transmissivity to allow the maximum amount of solar flux into the Trombe zone.~ Frames and dividers can be defined as usual for the window.~ The interior wall is usually constructed of very thick masonry materials with a solar absorber surface as the innermost layer of the wall.~ The absorber is a selective surface material with very high absorptivity and very low emissivity, e.g.~copper with a special black surface treatment.~ It is important to make sure the Solar Distribution field in the \textbf{Building} object is set to FullInteriorAndExterior so that the majority of the solar flux is directed on the absorber surface and not just on the very small area of the Trombe zone floor. ~The Zone Inside Convection Algorithm for the Trombe's Zone object should also be set to TrombeWall to correctly model the air space.~ As is the case for all interzone partitions, the wall construction of the adjoining zone must be the mirror image of the wall construction in the Trombe zone.~ Finally, an overhang is optionally attached to the Trombe zone to control the amount of seasonal sun exposure.~ Since the user selects all of the Trombe wall parameters in the input file, there is considerable freedom to experiment with different materials, sizes, and configurations.
+
+\begin{figure}[hbtp] % fig 307
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6830.png}
+\caption{Building with Trombe Wall \protect \label{fig:building-with-trombe-wall}}
+\end{figure}
+
+\subsection{Passive Trombe Wall}\label{passive-trombe-wall}
+
+Passive Trombe walls perform without the assistance of any additional mechanical equipment.~ Most Trombe walls are passive Trombe walls.~ They can be either sealed or naturally ventilated.
+
+For a sealed or unvented Trombe wall, the \emph{Zone Inside Convection Algorithm} field in the Zone object should be set to ``TrombeWall''.~ This algorithm correctly calculates the convection coefficients for a narrow sealed vertical cavity based on the ISO 15099 standard.~ Refer to the ``Trombe Wall Algorithm'' subsection (under Interior Convection, above) for a complete description of the algorithm.~ The EnergyPlus modeling approach for the sealed passive Trombe wall has been validated with experimental data (Ellis 2003).
+
+For a naturally ventilated Trombe wall, there is no built-in algorithm for calculating the correct convection coefficients on the inside of the cavity walls.~ One option is to use the ``Detailed'' convection algorithm.~ This algorithm takes into account some natural convection effects but is intended for a normal sized room.~ Therefore, some error may be incurred when used with a narrow cavity.~ Another option is to use the SurfaceProperty:ConvectionCoefficients object to schedule coefficients that have been determined beforehand by the user.
+
+\subsubsection{Input File}\label{input-file}
+
+An input file (PassiveTrombeWall.idf) is provided to demonstrate a sample sealed Trombe wall implementation.~ In this file two separated fictional buildings are simulated for summer and winter design days in Zion, Utah.~ The buildings are identical in size and construction except that one has a Trombe wall and the other does not.~ The buildings have uncontrolled zones with no internal loads and heavy insulation.~ All floors use interzone partitions to disconnect them from the ground.~ The window on the Trombe zone is a 3 mm, low iron, single pane glazing with very high transmissivity (0.913 visible, 0.899 solar).~ The absorber surface is a Tabor solar absorber with an emittance of 0.05 and absorptance of 0.85.
+
+\subsubsection{Results}\label{results-000}
+
+The resulting temperature profiles for winter and summer design days are plotted below.
+
+\begin{figure}[hbtp] % fig 308
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6831.png}
+\caption{Passive Trombe Wall Winter \protect \label{fig:passive-trombe-wall-winter}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 309
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6832.png}
+\caption{Passive Trombe Wall Summer \protect \label{fig:passive-trombe-wall-summer}}
+\end{figure}
+
+\subsubsection{References}\label{references-047}
+
+Ellis, Peter G.~ 2003.~ \emph{Development and Validation of the Unvented Trombe Wall Model in EnergyPlus}, Master's Thesis, University of Illinois at Urbana-Champaign.
+
+ISO 15099.~ 2000.~ ``Thermal Performance of Windows, Doors, and Shading Devices-Detailed Calculations''.~ International Standards Organization, Draft, July 18, 2000.
+
+\subsection{Active Trombe Wall}\label{active-trombe-wall}
+
+The active Trombe wall is the same as the passive Trombe wall with the addition of a simple fan system to circulate air between the Trombe zone and the main zone.~ The fan is scheduled to operate only during winter daylight hours to improve the heat transfer from the Trombe zone.
+
+As with the passive Trombe wall, there is no EnergyPlus object for the active Trombe wall; it is simulated using a collection of other EnergyPlus objects.~ Like the passive Trombe wall, the active Trombe wall uses a narrow zone coupled to the main zone with interzone partitions.~ However, the unique part of the active Trombe wall is that the Trombe zone is used to define a zone supply plenum object which allows the Trombe zone to be integrated into the air system.~ A constant volume fan is the main component of the air system.~ To make the zone connections, the Direct Air component is used.
+
+For the active Trombe wall, there is no built-in algorithm for calculating the correct convection coefficients due to forced convection on the inside of the cavity walls.~ One approach is to use the SurfaceProperty:ConvectionCoefficients object to schedule coefficients that have been determined beforehand by the user.
+
+\subsubsection{Input File}\label{input-file-1}
+
+An input file (ActiveTrombeWall.idf) is provided to demonstrate a sample active Trombe wall implementation.~ The building and Trombe wall in this file are identical to the ones described above for PassiveTrombeWall.idf.~ However, this input file adds a system in the form of a low flow rate (0.1 m\(^{3}\)/s) constant volume fan and the necessary duct connections.~ The fan is scheduled to operate October through March from 10 AM to 8 PM.
+
+\subsubsection{Results}\label{results-1}
+
+The resulting temperature profile for the winter design day is plotted below.~ The plot for the summer design day is not shown because it is identical to Figure~\ref{fig:passive-trombe-wall-summer} above since the fan is not scheduled to operate in the summer.
+
+\begin{figure}[hbtp] % fig 310
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6833.png}
+\caption{Active Trombe Wall Winter \protect \label{fig:active-trombe-wall-winter}}
+\end{figure}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/water-systems.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/water-systems.tex
new file mode 100644
index 00000000000..4fd540b5e90
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/water-systems.tex
@@ -0,0 +1,516 @@
+\section{Water Systems }\label{water-systems}
+
+Water systems include a variety of components that simulate water consumption, production, and storage, including:
+
+1.~~~~Water Use Equipment and Connections
+
+2.~~~~Rainwater Collection
+
+3.~~~~Groundwater Well
+
+4.~~~~Water Storage Tanks
+
+\subsection{Water Mains Temperatures}\label{water-mains-temperatures}
+
+The input object Site:WaterMainsTemperature provides a model for the temperature of water mains that deliver water to a building via underground pipes.~ The water mains temperatures are an important input for plant equipment that require make-up water from the water mains, such as for domestic hot water systems.
+
+Water mains temperatures are a function of outdoor climate conditions and vary with time of year.~ A correlation has been formulated to predict water mains temperatures based on two weather inputs:
+
+average annual outdoor air temperature (dry-bulb)
+
+maximum difference in monthly average outdoor air temperatures
+
+These values can be easily calculated from annual weather data using a spreadsheet.
+
+The correlation was developed by Craig Christensen and Jay Burch and is described in Hendron et al. (2004).~ The correlation is:
+
+T\(_{mains}\) = (T\(_{out,avg}\) + 6) + ratio * (ΔT\(_{out,maxdiff}\) / 2) * SIN(0.986 * (day - 15 - lag) - 90)
+
+where
+
+T\(_{mains}\) = water mains temperature (°F)
+
+T\(_{out,avg}\) = average annual outdoor air temperature (°F)
+
+ΔT\(_{out,maxdiff}\) = maximum difference in monthly average outdoor air temperatures (°F)
+
+day = Julian day of the year (1-365)
+
+ratio = 0.4 + 0.01 * (Tamb,avg - 44)
+
+lag = 35 - 1.0 * (Tamb,avg - 44) (°F)
+
+For the Chicago-O'Hare TMY2 weather file, T\(_{out,avg}\) = 9.69 C and ΔT\(_{out,maxdiff}\) = 28.1 C.~ The resulting water mains temperature profile is graphed below.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image6936.png}
+\caption{}
+\end{figure}
+
+\subsubsection{References}\label{references-052}
+
+Hendron, R., Anderson, R., Christensen, C., Eastment, M., and Reeves, P.~ 2004.~ ``Development of an Energy Savings Benchmark for All Residential End-Uses'', Proceedings of SimBuild 2004, IBPSA-USA National Conference, Boulder, CO, August 4 - 6, 2004.
+
+\subsection{Water Use Equipment and Connections}\label{water-use-equipment-and-connections}
+
+Essential parts of most water systems are the end uses where the water is utilized for a purpose.~ These end uses are characterized by familiar pieces of equipment such as sinks, showers, dishwashers, clothes washers, and toilets.~ End uses can also include outdoor uses such as landscape irrigation and agricultural irrigation.
+
+Water end-use modeling in EnergyPlus is accomplished via two input objects:
+
+§~WaterUse:Equipment
+
+§~WaterUse:Connections
+
+The WaterUse:Equipment object simulates all different types of water end uses.~ The WaterUse:Connections object manages multiple pieces of water equipment with a common supply and return, internally providing the services of a splitter and a mixer.~ The WaterUse:Connections object also allows water consuming equipment to be simulated in a closed plant loop by supplying makeup water from the water mains.
+
+\subsection{Unconnected Water Use Equipment}\label{unconnected-water-use-equipment}
+
+Common water equipment, such as sinks and showers, requires mixing of hot and cold water to provide a desired temperature at the tap.~ Water use equipment that is simulated in ``unconnected'' mode, i.e., without being referenced by a WaterUse:Connections object, presents a relatively simple modeling problem illustrated by the diagram below:
+
+\begin{figure}[hbtp] % fig 315
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6937.png}
+\caption{Hot and Cold Water Mixing \protect \label{fig:hot-and-cold-water-mixing}}
+\end{figure}
+
+The variables are defined as:
+
+\({\dot m_{hot}}\) = hot water supply mass flow rate
+
+\({T_{hot}}\) = hot water supply temperature
+
+\({\dot m_{cold}}\) = cold water supply mass flow rate
+
+\({T_{cold}}\) = cold water supply temperature
+
+\({\dot m_{target}}\) = target mass flow rate at the tap
+
+\({T_{target}}\) = target temperature at the tap
+
+The basic physics of the problem are described by two equations representing conservation of mass and conservation of energy respectively:
+
+\begin{equation}
+{\dot m_{target}} = {\dot m_{hot}} + {\dot m_{cold}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{target}}{T_{target}} = {\dot m_{hot}}{T_{hot}} + {\dot m_{cold}}{T_{cold}}
+\end{equation}
+
+The hot and cold water supply temperatures, \({T_{hot}}\) ~and \({T_{cold}}\) , are specified by the user with schedules (or indirectly from the water mains temperatures).~ The target flow rate and target temperature, \({\dot m_{target}}\) ~and \({T_{target}}\) , at the tap are also specified with schedules.~ The target conditions can be thought of as a way to simulate occupant behavior; a person at a sink will adjust the hot and cold flow rates to get the overall water flow and temperature that is desired.
+
+The two equations above are easily solved to calculate the necessary hot and cold flow rates needed to attain the target conditions.
+
+\begin{equation}
+{\dot m_{hot}} = {\dot m_{target}}\left( {\frac{{{T_{target}} - {T_{cold}}}}{{{T_{hot}} - {T_{cold}}}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot m_{cold}} = {\dot m_{target}} - {\dot m_{hot}}
+\end{equation}
+
+Even though hot and cold flow rates are unlimited in ``unconnected'' mode, it is still possible to fail to meet the target conditions if \({T_{target}}\) ~\textgreater{} \({T_{hot}}\) .~ In this case, the actual mixed water temperature at the tap, \({T_{mixed}}\) , is set equal to \({T_{hot}}\) .~ The target flow rate is always met.
+
+Water equipment that omits schedules for the target temperature and/or hot water suppy temperature implies that no hot water is needed.~ The result is all cold water at the target flow rate.
+
+For ``unconnected'' water equipment, the heating rate and energy that is required to supply the hot water is calculated by the following equations.
+
+\begin{equation}
+Q = {\dot m_{hot}}{c_p}\left( {{T_{hot}} - {T_{cold}}} \right)
+\end{equation}
+
+\begin{equation}
+\Delta E = Q\Delta t
+\end{equation}
+
+where
+
+\(Q\) = heating rate
+
+\({c_p}\) = specific heat of water
+
+\(\Delta E\) = heating energy
+
+\(\Delta t\) = time step interval
+
+All heating is assigned to ``Purchased Heating''.
+
+\subsection{Zone Heat Gain from Water Use Equipment}\label{zone-heat-gain-from-water-use-equipment}
+
+Some water use equipment can be a significant source of sensible and latent heat gain when located in a zone.~ Showers, for example, add a noticeable latent gain as some of the hot water evaporates into the zone air (and at the same time adding some sensible gain).~ Other types of equipment may contribute greater sensible gain but less latent gain.
+
+Calculating the amount of sensible and latent heat gain can be extremely complicated and depends on many variables.~ One set of variables is related to the initial conditions of the entering water and the undisturbed zone air, namely:
+
+\begin{itemize}
+\item
+  Entering water temperature
+\item
+  Entering water flow rate
+\item
+  Ambient zone air temperature
+\item
+  Ambient zone humidity
+\item
+  Ambient zone barometric pressure
+\end{itemize}
+
+A second set of variables is tied to the specifics of the water equipment which describe the heat and mass transfer processes that occur as the water passes through the zone.~ These variables might include the velocity of the water in the zone air, the surface area of water exposed to the zone air, the dwell time of water in the zone, and possibly others.~ The complexity of these variables cannot be easily cast into a generalized EnergyPlus input object.~ Consider that in a shower, the velocity of water droplets is increasing as they fall, and the surface area of the spray is increasing.~ How to even determine the surface area of the spray at any point?
+
+The approach taken here is to utilize the first set of initial condition variables and forego the overly-complex second set.~ The initial conditions can be used to calculate a maximum possible change in sensible and latent energy between the entering water conditions and the leaving water conditions at an infinite time later.~ Sensible and latent energy are calculated separately and represent the maximum heat gain, respectively, that could be added to the zone air.~ The user simply specifies a fraction of the maximum heat gain for sensible and latent that is actually added to the zone air.~ The fraction is specified with a schedule to account for different modes of operation.~ The split between sensible and latent will vary depending on the type of equipment that is to be modeled.~ Typically, both fractions should be small numbers.
+
+\begin{figure}[hbtp] % fig 316
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6962.png}
+\caption{Zone Heat Gain from Water Use Equipment \protect \label{fig:zone-heat-gain-from-water-use-equipment}}
+\end{figure}
+
+The maximum sensible heat gain rate is calculated by assuming that all of the water flow is allowed to cool to the zone dry-bulb temperature.~ The actual sensible zone heat gain rate is found by multiplying the maximum by the user fraction.
+
+\begin{equation}
+{Q_{sens}} = {f_{sens}}{\dot m_{target}}{c_p}\left( {{T_{target}} - {T_{zone}}} \right)
+\end{equation}
+
+\begin{equation}
+\Delta {E_{sens}} = {Q_{sens}}\Delta t
+\end{equation}
+
+where
+
+\({Q_{sens}}\) ~ = sensible heat gain rate
+
+\({f_{sens}}\) ~ = user fraction of maximum sensible heat
+
+\({\dot m_{target}}\) = target mass flow rate at the tap
+
+\({c_p}\) = specific heat of water
+
+\({T_{target}}\) = target temperature at the tap
+
+\({T_{zone}}\) ~ = zone dry-bulb air temperature
+
+\(\Delta {E_{sens}}\) = sensible heat gain
+
+\(\Delta t\) = time step interval
+
+The maximum latent heat gain rate is calculated by assuming that the maximum amount of water is evaporated into the zone air during the time step.~ The actual latent zone heat gain rate is found by multiplying the maximum by the user fraction.
+
+\begin{equation}
+{m_{evap,zonemax}} = \left( {{W_{sat}} - {W_{zone}}} \right){\rho_{zone}}{V_{zone}}
+\end{equation}
+
+\begin{equation}
+{m_{evap,flowmax}} = {\dot m_{target}}\Delta t
+\end{equation}
+
+\begin{equation}
+{m_{evap,max}} = MIN({m_{evap,zonemax}},{m_{evap,flowmax}})
+\end{equation}
+
+\begin{equation}
+{m_{evap}} = {f_{lat}}{m_{evap,max}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{evap}} = {m_{evap}}/\Delta t
+\end{equation}
+
+\begin{equation}
+{Q_{lat}} = {h_{fg}}{\dot m_{evap}}
+\end{equation}
+
+\begin{equation}
+\Delta {E_{lat}} = {Q_{lat}}\Delta t
+\end{equation}
+
+where
+
+\({m_{evap,zonemax}}\) = mass of water that can be absorbed by the zone air in one timestep
+
+\({W_{sat}}\) = fully-saturated zone humidity ratio (function of air temperature and pressure)
+
+\({W_{zone}}\) ~ = zone humidity ratio
+
+\({\rho_{zone}}\) ~ = zone dry-air density (function of air temperature and pressure)
+
+\({V_{zone}}\) ~ = zone air volume
+
+\({m_{evap,flowmax}}\) = mass of water available in the flow in one timestep
+
+\({\dot m_{target}}\) = target mass flow rate at the tap
+
+\(\Delta t\) = time step interval
+
+\({m_{evap,max}}\) = maximum mass of water that can be evaporated
+
+\({m_{evap}}\) = actual mass of water evaporated into the zone air
+
+\({f_{lat}}\) ~ = user fraction of maximum latent heat
+
+\({\dot m_{evap}}\) = mass rate of water evaporation into the zone air
+
+\({Q_{lat}}\) ~ = latent heat gain rate
+
+\({h_{fg}}\) = heat of vaporization for water
+
+\(\Delta {E_{lat}}\) = latent heat gain
+
+Sensible and latent heat gains to the zone are lagged by one zone time step.
+
+Note that this method allows the heat gain to vary dynamically according to changing water and zone conditions instead of the fixed or scheduled value that is traditionally used.~ However, sensible and latent fractions may be difficult to estimate.~ Experimental measurement is probably the best way to determine the fractions.
+
+A related result of any zone heat and moisture gain is that the water undergoes an equal heat and moisture loss.~ For a shower the water will generally leave the zone at a cooler temperature and slightly reduced flow rate when compared to the entering water conditions.
+
+\begin{equation}
+{\dot m_{drain}} = {\dot m_{target}} - {\dot m_{evap}}
+\end{equation}
+
+\begin{equation}
+{T_{drain}} = \frac{{{{\dot m}_{target}}{c_p}{T_{target}} - {Q_{sens}} - {Q_{lat}}}}{{{{\dot m}_{drain}}{c_p}}}
+\end{equation}
+
+where
+
+\({\dot m_{drain}}\) = drainwater mass flow rate at the drain
+
+\({\dot m_{target}}\) = target mass flow rate at the tap
+
+\({\dot m_{evap}}\) = mass rate of water evaporation into the zone air
+
+\({T_{drain}}\) = water temperature at the drain
+
+\({c_p}\) = specific heat of water
+
+\({T_{target}}\) = target temperature at the tap
+
+\({Q_{sens}}\) ~ = sensible heat gain rate
+
+\({Q_{lat}}\) ~ = latent heat gain rate
+
+The change in leaving water conditions has implications for drainwater heat recovery and storage tank conditions.
+
+\subsection{Connected Water Use Equipment}\label{connected-water-use-equipment}
+
+Water use equipment referenced by a WaterUse:Connections object is considered to be in ``connected'' mode.~ The WaterUse:Connections object manages multiple pieces of water equipment with a common supply and return, internally providing the services of a splitter and a mixer.~ The connections object also offers three internal configurations for drainwater heat recovery.~ External connections are available for coupling to plant loop nodes or water storage tanks for graywater reuse or reclamation.
+
+Keep in mind that water use equipment in ``connected'' mode does not imply that it is connected to a plant loop.~ WaterUse:Equipment objects are never directly connected to a plant loop; they are connected indirectly through the WaterUse:Connections object.~ WaterUse:Connections can operate either within a plant loop or in stand-alone mode, i.e., without plant loop connections.
+
+The WaterUse:Connections object overrides the hot and cold water supply temperatures of its subordinate WaterUse:Equipment objects based on the specified schedules, plant loop conditions, or water storage tank conditions.~ But the WaterUse:Equipment objects still maintain their individual target flow rates and target temperatures.
+
+Solving the water subsystem described by the WaterUse:Connections object is appreciably more difficult than solving a single, unconnected piece of water use equipment.~ The subsystem is illustrated below.
+
+\begin{figure}[hbtp] % fig 317
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7005.png}
+\caption{Water Use Connections Subsystem \protect \label{fig:water-use-connections-subsystem}}
+\end{figure}
+
+The nomenclature here uses uppercase letters to indicate variables related to the connections object and lowercase letters to indicate variables related to the equipment objects.~ The variables are defined as:
+
+\({\dot M_{hot}}\) = hot water supply mass flow rate
+
+\({T_{hot}}\) = hot water supply temperature
+
+\({\dot M_{cold}}\) = cold water supply mass flow rate
+
+\({T_{cold}}\) = cold water supply temperature
+
+\({\dot M_{drain}}\) = drainwater mass flow rate at the drain
+
+\({T_{drain}}\) = water temperature at the drain
+
+\({T_{waste}}\) = wastewater temperature after the drain
+
+\({\dot M_{return}}\) = return water mass flow rate back to the plant loop
+
+\({T_{return}}\) = return temperature of makeup water back to the plant loop
+
+\subsection{Water Use Equipment Calculations}\label{water-use-equipment-calculations}
+
+The solution method proceeds in steps:
+
+\begin{itemize}
+\item
+  \emph{InitConnectionsTemps}
+\item
+  \emph{CalcConnectionsFlowRates}
+\item
+  \emph{CalcConnectionsDrainTemp}
+\item
+  \emph{UpdateConnectionsNodes}
+\end{itemize}
+
+\subsubsection{Initialize Connections Temperatures}\label{initialize-connections-temperatures}
+
+Initializes the hot and cold supply water temperatures, \({T_{hot}}\) ~and \({T_{cold}}\) , for the common supply to all the equipment.~ If plant-coupled, \({T_{hot}}\) ~is taken from the plant loop inlet node.~ If stand-alone, \({T_{hot}}\) ~is taken from the schedule.
+
+\({T_{cold}}\) ~is taken from the supply water storage tank, if specified.~ Otherwise \({T_{cold}}\) ~is taken from the schedule.~ If a schedule is not specified, \({T_{cold}}\) ~is taken from the water mains.
+
+\subsubsection{Calculate Connections Flow Rates}\label{calculate-connections-flow-rates}
+
+First calls on each piece of equipment to simulate itself with the given supply water temperatures \({T_{hot}}\) ~and \({T_{cold}}\) .~ The desired hot and cold flow rates for \({\dot m_{hot,i}}\) ~and \({\dot m_{cold,i}}\) ~are calculated (as described earlier) and passed back to the connections object.~ The total flow rates for \({\dot M_{hot}}\) ~and \({\dot M_{cold}}\) ~are then calculated:
+
+\({\dot M_{hot}} = \mathop \sum \limits_i {\dot m_{hot,i}}\) ~~~~~~~~~~ \({\dot M_{cold}} = \mathop \sum \limits_i {\dot m_{cold,i}}\)
+
+If plant-coupled, \({\dot M_{hot}}\) ~is compared to the maximum flow rate available in the plant loop (after the first HVAC iteration).~ If \({\dot M_{hot}}\) ~\textgreater{} \({\dot M_{hot,max}}\) , the actual flow rate is reset to equal the maximum:~ \({\dot M_{hot}}\) ~ = \({\dot M_{hot,max}}\) .~ New hot and cold flow rates, \({\dot m'_{hot,i}}\) ~and \({\dot m'_{cold,i}}\) , at the equipment level are then recalculated, decreasing the hot flow rate and increasing the cold flow rate in order to still meet the target flow rate.
+
+\begin{equation}
+\alpha  = \frac{{{{\dot M}_{hot,max}}}}{{{{\dot M}_{hot}}}}
+\end{equation}
+
+\begin{equation}
+{\dot m'_{hot,i}} = \alpha {\dot m_{hot,i}}
+\end{equation}
+
+\begin{equation}
+{\dot m'_{cold,i}} = {\dot m_{target,i}} - {\dot m'_{hot,i}}
+\end{equation}
+
+A new mixed water temperature is also recalculated at the equipment level.
+
+Although water storage tanks can also have a maximum flow rate on the cold side, the cold flow rate is not limited in this implementation.
+
+\subsubsection{Calculate Connections Drain Temperature}\label{calculate-connections-drain-temperature}
+
+At this point zone heat gains are calculated for all equipment in zones.~ The final drainwater temperatures and flow rates are determined for each piece of equipment by subtracting the lost heat and moisture (see above).~ The total drainwater temperature and flow rate for the subsystem are calculated:
+
+\({\dot M_{drain}} = \mathop \sum \limits_i {\dot m_{drain,i}}\) ~~~~~~~~~~ \({T_{drain}} = \frac{{\mathop \sum \limits_i {{\dot m}_{drain,i}}{t_{drain,i}}}}{{{{\dot M}_{drain}}}}\)
+
+In the case of no drainwater heat recovery, the subsystem wastewater temperature, \({T_{waste}}\) , is equal to the drainwater temperature, \({T_{drain}}\) .~ (For drainwater heat recovery, see below.)~ The wastewater temperature and flow rate are propogated to the reclamation water storage tank, if specified.
+
+\subsubsection{Update Connections Nodes}\label{update-connections-nodes}
+
+Finally, if plant-coupled, the return water temperature, \({T_{return}}\) , is passed on to the plant outlet node.~ \({T_{return}}\) ~is taken from the cold water supply schedule or the water mains.~ The return flow rate is equal to the hot water supply flow rate in order to preserve a closed plant loop:~ \({\dot M_{return}}\) ~ = \({\dot M_{hot}}\) .
+
+For ``connected'' water equipment, the heating rate and energy that is required to supply the hot water for individual water equipment is calculated by the following equations.
+
+\begin{equation}
+Q = {\dot m_{hot}}{c_p}\left( {{T_{hot}} - {T_{return}}} \right)
+\end{equation}
+
+\begin{equation}
+\Delta E = Q\Delta t
+\end{equation}
+
+where
+
+\(Q\) = heating rate
+
+\({c_p}\) = specific heat of water
+
+\(\Delta E\) = heating energy
+
+\(\Delta t\) = time interval
+
+The heating rate and energy for the WaterUse:Connections is the sum of the values for its constituent water equipment objects.~ If the WaterUse:Connections object is stand-alone, all heating is assigned to ``Purchased Heating'' by the individual water equipment objects.~ If the WaterUse:Connections object is coupled to a plant loop, all heating is supplied by the plant loop equipment.
+
+\subsection{Drainwater Heat Recovery}\label{drainwater-heat-recovery}
+
+Drainwater heat recovery adds one more complication to the water connections subsystem.~ A heat exchanger is added between the drain and the waste outlet to recover some heat from the water before it leaves the system.~ The heat is usually recovered by preheating the incoming makeup water from the mains.
+
+The heat exchanger can be modeled as ``ideal'', ``counterflow'', or ``crossflow''.~ One common type of drainwater heat exchanger is the gravity-film exchanger (GFX).~ The GFX can be approximated with a counterflow heat exchanger.
+
+The destination of the preheated makeup water can be plumbed in three possible configurations:~ ``plant'', ``equipment'', ``plant and equipment''.~ In the ``plant'' configuration, all preheated water flow is returned to the plant loop to match the makeup water for the hot water supply flow.~ In the ``equipment'' configuration, all preheated water flow is directed internally within the WaterUse:Connections object to provide the makeup water for the cold water supply flow for the local water use equipment.~ In the ``plant and equipment'' configuration, the preheated water is split between both of the previous configurations.~ This is the only configuration where the flow rate is equal on both sides of the heat exchanger.
+
+\begin{figure}[hbtp] % fig 318
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7054.png}
+\caption{Water Use Connections Subsystem with Drainwater Heat Recovery \protect \label{fig:water-use-connections-subsystem-with}}
+\end{figure}
+
+The new variables added here are defined as:
+
+\({\dot M_{recovery}}\) = makeup water mass flow rate in the heat exchanger
+
+\({T_{recovery}}\) = water temperature leaving the heat exchanger
+
+\({T_{makeup}}\) = cold makeup water temperature supplied to various flows
+
+Another subroutine is inserted into the solution method:
+
+\begin{itemize}
+\item
+  \emph{InitConnectionsTemps}
+\item
+  \emph{CalcConnectionsFlowRates}
+\item
+  \emph{CalcConnectionsDrainTemp}
+\item
+  \textbf{\emph{CalcConnectionsHeatRecovery}}
+\item
+  \emph{UpdateConnectionsNodes}
+\end{itemize}
+
+For the ``equipment'' and ``plant and equipment'' configurations, the solution requires iteration to solve because the preheated water leaving the heat exchanger is connected to the cold water supply water, creating a feedback loop.
+
+\subsubsection{Calculate Connections Heat Recovery}\label{calculate-connections-heat-recovery}
+
+Based on the selected configuration, the flow rate through the heat exchanger is first determined.~ For the ``plant'' configuration, \({\dot M_{recovery}} = {\dot M_{hot}}\) .~ For the ``equipment'' configuration, \({\dot M_{recovery}} = {\dot M_{cold}}\) .~ For the ``plant and equipment'' configuration, \({\dot M_{recovery}} = {\dot M_{hot}} + {\dot M_{cold}}\) .
+
+The heat capacity rates on both sides of the heat exchanger are calculated and the minimum and maximum heat capacity rates, \({C_{min}}\) ~and \({C_{max}}\) , are determined.
+
+\begin{equation}
+{C_{drain}} = {\dot M_{drain}}{c_p}
+\end{equation}
+
+\begin{equation}
+{C_{recovery}} = {\dot M_{recovery}}{c_p}
+\end{equation}
+
+\begin{equation}
+{C_{min}} = MIN({C_{drain}},{C_{recovery}})
+\end{equation}
+
+\begin{equation}
+{C_{max}} = MAX({C_{drain}},{C_{recovery}})
+\end{equation}
+
+\begin{equation}
+{R_c} = \frac{{{C_{min}}}}{{{C_{max}}}}
+\end{equation}
+
+where \({R_c}\) ~ = the heat capacity ratio.
+
+The effectiveness \(\varepsilon\) ~is then calculated for the given type of heat exchanger.~ For the ``ideal'' heat exchanger, \(\varepsilon = 1\) .
+
+For the ``counterflow'' and ``crossflow'' heat exchangers, the effectiveness is calculated using the effectiveness-NTU method, where:
+
+\begin{equation}
+NTU = \frac{{UA}}{{{C_{min}}}}
+\end{equation}
+
+For the ``counterflow'' heat exchanger:
+
+\(\varepsilon = \frac{{NTU}}{{1 + NTU}}\) , if \({R_c}\) ~ = 1
+
+\(\varepsilon = \frac{{1 - EXP\left( { - NTU\left( {1 - {R_c}} \right)} \right)}}{{1 - {R_c}EXP\left( { - NTU\left( {1 - {R_c}} \right)} \right)}}\) , if \({R_c}\) ~\textless{} 1
+
+For the ``crossflow'' heat exchanger:
+
+\begin{equation}
+\varepsilon  = 1 - EXP\left( {\frac{{NT{U^{0.22}}}}{{{R_c}}}\left( {EXP\left( { - {R_c}NT{U^{0.78}}} \right) - 1} \right)} \right)
+\end{equation}
+
+The heat recovery rate is then calculated.
+
+\begin{equation}
+{Q_{recovery}} = \varepsilon {C_{min}}\left( {{T_{drain}} - {T_{makeup}}} \right)
+\end{equation}
+
+The outlet water temperatures can then be calculated for both sides of the heat exchanger.
+
+\begin{equation}
+{T_{recovery}} = {T_{makeup}} + \frac{{{Q_{recovery}}}}{{{{\dot M}_{recovery}}{c_p}}}
+\end{equation}
+
+\begin{equation}
+{T_{waste}} = {T_{drain}} - \frac{{{Q_{recovery}}}}{{{{\dot M}_{drain}}{c_p}}}
+\end{equation}
+
+At each iteration the difference between \({T_{recovery}}\) ~and \({T_{cold}}\) is compared and checked for convergence.
+
+\begin{equation}
+\Delta {T_{error}} = \left| {{T_{recovery}} - {T_{cold}}} \right|
+\end{equation}
+
+Once the temperatures have converged, the solution is complete.~ \({T_{waste}}\) ~is then passed on to a storage tank, if specified.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/water-thermal-tanks-includes-water-heaters.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/water-thermal-tanks-includes-water-heaters.tex
new file mode 100644
index 00000000000..3f27f091567
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/water-thermal-tanks-includes-water-heaters.tex
@@ -0,0 +1,848 @@
+\section{Water Thermal Tanks (includes Water Heaters) }\label{water-thermal-tanks-includes-water-heaters}
+
+Water thermal tanks are devices for storing thermal energy in water.~ The most common types are water heaters. devices for storing and heating water.~ Typical water heater applications are for domestic hot water heating, low-temperature radiant space heating, and energy storage for solar hot water systems or waste heat recovery.~ In EnergyPlus, water heater objects can be coupled to a plant loop simulation or used stand-alone.~ There are also chilled water storage tanks that can be used to hold cold water
+
+\subsection{Mixed Water Thermal Tank}\label{mixed-water-thermal-tank}
+
+The input object WaterHeater:Mixed provides a model that simulates a well-mixed water tank, i.e.~non-stratified, and is appropriate for simulating many types of water heaters and storage tanks, including gas and electric residential water heaters, a variety of large commercial water heaters, and also instantaneous, tankless water heaters.~ This model is used for both the mixed water heater and the mixed chilled water storage tanks.
+
+\subsubsection{Energy Balance}\label{energy-balance}
+
+The well-mixed assumption implies that all water in the tank is at the same temperature.~ To calculate the water temperature, the model analytically solves the differential equation governing the energy balance of the water tank:
+
+\begin{equation}
+\rho V{c_p}\frac{{dT}}{{dt}} = {q_{net}}
+\end{equation}
+
+where
+
+\emph{r} = density of water
+
+\emph{V} = volume of the tank
+
+\emph{c\(_{p}\)} = specific heat of water
+
+\emph{T} = temperature of the tank water
+
+\emph{t} = time
+
+\emph{q\(_{net}\)} = net heat transfer rate to the tank water
+
+The density and volume can be replaced with the total mass \emph{m} of water in the tank to get:
+
+\begin{equation}
+m{c_p}\frac{{dT}}{{dt}} = {q_{net}}
+\end{equation}
+
+The net heat transfer rate \emph{q\(_{net}\)} is the sum of gains and losses due to multiple heat transfer pathways.
+
+\begin{equation}
+{q_{net}} = {q_{heater}} + {q_{oncycpara}} + {q_{offcycpara}} + {q_{oncycloss}} + {q_{offcycloss}} + {q_{use}} + {q_{source}}
+\end{equation}
+
+where
+
+\emph{q\(_{heater}\)} = heat added by the heating element or burner
+
+\emph{q\(_{oncycpara}\)} = heat added due to on-cycle parasitic loads (zero when off)
+
+\emph{q\(_{offcycpara}\)} = heat added due to off-cycle parasitic loads (zero when on)
+
+\emph{q\(_{oncycloss}\)} = heat transfer to/from the ambient environment (zero when off)
+
+\emph{q\(_{offcycloss}\)} = heat transfer to/from the ambient environment (zero when on)
+
+\emph{q\(_{use}\)} = heat transfer to/from the use side plant connections
+
+\emph{q\(_{source}\)} = heat transfer to/from the source side plant connections
+
+\emph{q\(_{oncycloss}\)} and \emph{q\(_{offcycloss}\)} are defined as:
+
+\begin{equation}
+{q_{oncycloss}} = U{A_{oncyc}}\left( {{T_{amb}} - T} \right)
+\end{equation}
+
+\begin{equation}
+{q_{offcycloss}} = U{A_{offcyc}}\left( {{T_{amb}} - T} \right)
+\end{equation}
+
+where
+
+\emph{UA\(_{oncyc}\)} = on-cycle loss coefficient to ambient environment (zero when off)
+
+\emph{UA\(_{offcyc}\)} = off-cycle loss coefficient to ambient environment (zero when on)
+
+\emph{T\(_{amb}\)} = temperature of ambient environment
+
+\emph{q\(_{use}\)}, and \emph{q\(_{source}\)} are defined as:
+
+\begin{equation}
+{q_{use}} = {\varepsilon_{use}}{\dot m_{use}}{c_p}\left( {{T_{use}} - T} \right)
+\end{equation}
+
+\begin{equation}
+{q_{source}} = {\varepsilon_{source}}{\dot m_{source}}{c_p}\left( {{T_{source}} - T} \right)
+\end{equation}
+
+where
+
+\emph{e\(_{use}\)} = heat exchanger effectiveness for the use side plant connections
+
+\({\dot m_{use}}\) = mass flow rate for the use side plant connections
+
+\emph{T\(_{use}\)} = inlet fluid temperature of the use side plant connections
+
+\emph{e\(_{source}\)} = heat exchanger effectiveness for the source side plant connections
+
+\({\dot m_{source}}\) = mass flow rate for the source side plant connections
+
+\emph{T\(_{source}\)} = inlet fluid temperature of the use side plant connections
+
+Incorporating all of these equations into the original differential equation,
+
+\begin{equation}
+  \begin{array}{ll}
+    mC_p\frac{dT}{dt} &= q_{heater} + q_{oncyc} + q_{offcyc} + UA_{oncyc} \PB{T_{amb} - T} + UA_{offcyc} \PB{T_{amb} - T} \\ 
+                      &+ \varepsilon_{use}\dot{m}_{use}C_p \PB{T_{use} - T} + \varepsilon_{source}\dot{m}_{source}C_p \PB{T_{source} - T}
+  \end{array}
+\end{equation}
+
+Associating terms not dependent on temperature \emph{T} and terms dependent on temperature \emph{T} yields:
+
+\begin{equation}
+  \begin{array}{ll}
+    \frac{dT}{dt} &= \RB{\frac{1}{mC_p}\PB{\begin{array}{c}
+                                             q_{heater}+q_{oncyc}+q_{offcyc}+UA_{oncyc}T_{amb}+UA_{offcyc}T_{amb} \\
+                                             + \varepsilon_{use}\dot{m}_{use}C_pT_{use} + \varepsilon_{source}\dot{m}_{source}C_pT_{source}
+                                           \end{array}}} \\
+                  &+ \RB{\frac{-1}{mC_p}\PB{UA_{oncyc} + UA_{offcyc}+\varepsilon_{use}\dot{m}_{use}C_p+\varepsilon_{source}\dot{m}_{source}C_p}}T
+  \end{array}
+\end{equation}
+
+The differential equation now has the form
+
+\begin{equation}
+\frac{{dT}}{{dt}} = a + bT
+\end{equation}
+
+where
+
+\begin{equation}
+a = \frac{1}{{m{c_p}}}\left( \begin{array}{l}{q_{heater}} + {q_{oncyc}} + {q_{offcyc}} + U{A_{oncyc}}{T_{amb}} + U{A_{offcyc}}{T_{amb}}\\ + {\varepsilon_{use}}{{\dot m}_{use}}{c_p}{T_{use}} + {\varepsilon_{source}}{{\dot m}_{source}}{c_p}{T_{source}}\end{array} \right)
+\end{equation}
+
+\begin{equation}
+b = \frac{{ - 1}}{{m{c_p}}}\left( {U{A_{oncyc}} + U{A_{offcyc}} + {\varepsilon_{use}}{{\dot m}_{use}}{c_p} + {\varepsilon_{source}}{{\dot m}_{source}}{c_p}} \right)
+\end{equation}
+
+The solution to the differential equation can be written in terms of \emph{a} and \emph{b} as:
+
+\begin{equation}
+T\left( t \right) = \left( {\frac{a}{b} + {T_i}} \right){e^{bt}} - \frac{a}{b}
+\end{equation}
+
+where
+
+\emph{T(t)} = temperature of the tank water at time \emph{t}
+
+\emph{T\(_{i}\)} = initial temperature of the tank water at time \emph{t} = 0
+
+However, if \emph{b} = 0, the solution instead is:
+
+\begin{equation}
+T\left( t \right) = at + {T_i}
+\end{equation}
+
+Since the control algorithm must sometimes calculate the time needed to reach a specified temperature, the equations above can also be rearranged to solve for \emph{t}.
+
+\begin{equation}
+t = \frac{1}{b}\ln \left( {\frac{{{\raise0.7ex\hbox{a} \!\mathord{\left/ {\vphantom {a b}}\right.}\!\lower0.7ex\hbox{b}} + {T_f}}}{{{\raise0.7ex\hbox{a} \!\mathord{\left/ {\vphantom {a b}}\right.}\!\lower0.7ex\hbox{b}} + {T_i}}}} \right)
+\end{equation}
+
+or, if \emph{b} = 0,
+
+\begin{equation}
+t = \frac{{{T_f} - {T_i}}}{a}
+\end{equation}
+
+where
+
+\emph{T\(_{f}\)} = final temperature of the tank water at time t.
+
+In the special case where \emph{b} = 0 and \emph{a} = 0, and \emph{T\(_{f}\)} \textless{}\textgreater{} \emph{T\(_{i}\)}, the time \emph{t} is infinity.
+
+\subsubsection{Water Heater Control Algorithm}\label{water-heater-control-algorithm}
+
+For water heaters, control options allow the heater to cycle or modulate to meet the load.~ When cycling, the heater element or burner is either on or off.~ The heater remains fully on while heating the tank up to the setpoint temperature.~ When the setpoint is reached, the heater turns off.~ The heater remains off until the tank temperature falls below the ``cut-in'' temperature, i.e., the setpoint temperature minus the deadband temperature difference.~ The heater continuously cycles on and off to maintain the tank temperature within the deadband.~ Most storage-tank water heaters cycle.
+
+When modulating, the heater power varies between the maximum and minimum heater capacities.~ The heater stays on as long as the required total demand is above the minimum capacity.~ Below the minimum capacity, the heater will begin to cycle on and off based on the deadband temperature difference.~ Most tankless/instantaneous water heaters modulate.
+
+Within a time step, the differential equation is solved separately for when the heater element or burner is ``on'' (on-cycle) and when it is ``off'' (off-cycle).~ This approach allows ambient losses and parasitic loads to be divided into on-cycle and off-cycle effects and accounted for in detail.
+
+An illustration of how the control algorithm cycles on and off is shown below.~ Ambient losses cool the tank temperature until the bottom of the deadband is reached (50 C) at which point the heater cycles on and reheats the tank back to the setpoint (60 C).~ A water draw causes hot water to be replaced with cold water from the water mains.~ The incoming cold water rapidly cools the tank.~ In this example the heater cannot keep up with the water draw and the tank temperature continues to drop until the water draw ends.
+
+Although the instantaneous tank water temperature may vary considerably within a timestep (due to cycling, etc.), only the average temperature over the timestep is reported.~ The model calculates the average by piece-wise integration of the area under the instantaneous temperature curve for each unique set of conditions.~ The instantaneous temperature is preserved internally by the program and is propogated from the end of one timestep to the beginning of the next.
+
+\begin{figure}[hbtp] % fig 311
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6852.png}
+\caption{Water Heater Cycle Control Algorithm \protect \label{fig:water-heater-cycle-control-algorithm}}
+\end{figure}
+
+\subsubsection{Chilled Water Tank Control Algorithm}\label{chilled-water-tank-control-algorithm}
+
+The input objects ThermalStorage:ChilledWater:Mixed and ThermalStorage:ChilledWater:Stratified provide chilled water tank models that do not include active cooling elements, there is only indirect cooling by remote devices such as a chiller.~ The tank's setpoint controls are used to determine if flow is to be requested through the source side of the tank.~ The setpont and deadband control scheme is similar to the water heater but the logic is flipped around for cooling instead of heating.~ The setpoint temperatue is the ``cut-out'' temperature and the setpoint plus deadband is the ``cut-in'' temperature.~ If the tank temperature ( or tank sensing node for stratified tanks) is above the ``cut-in'' temperature, then flow is requested.~ If temperatures are below the ``cut-out'' temperature, then flow is not requested.~ The chilled water tanks also have separate availability schedules for the use side and source side for additional control options.
+
+\subsubsection{Standard Ratings}\label{standard-ratings-000}
+
+For water heaters, the industry standard ratings of Recovery Efficiency and Energy Factor are calculated according to the 10CFR430 test procedure.~ To emulate the test procedure, a 24-hour simulation of the water heater is performed internally using the specified test conditions:
+
+n~Setpoint Temperature = 57.2 C (135 F)
+
+n~Ambient Temperature = 19.7 C (67.5 F)
+
+n~Ambient Relative Humidity = 50\% (used for heat pump water heaters)
+
+n~Inlet Temperature (Water Mains) = 14.4 C (58 F)
+
+For heat pump water heaters, the water heater tank's heating element and water heater tank parasitic loads are disabled and the user-defined water heating capacity, energy use, and parasitic loads for the heat pump are used to calculate Recovery Efficiency and Energy Factor.
+
+The simulated test procedure performs six equal draws of approximately 0.041 m\(^{3}\) (10.7 gal) in each of the first six hours of the simulation.~ Each draw occurs over the first timestep of the hour.
+
+The Recovery Efficiency is calculated when the water heater recovers to the setpoint after the first draw.
+
+\begin{equation}
+RE = \frac{{{m_1}{c_p}\left( {57.2 - 14.4} \right)}}{{{E_1}}}
+\end{equation}
+
+where
+
+\emph{m\(_{1}\)} = water mass of the first draw
+
+\emph{c\(_{p}\)} = specific heat of water
+
+\emph{E\(_{1}\)} = fuel energy consumed until the setpoint is recovered (including parasitics)
+
+Note: When the standards rating for a heat pump water heater is calculated, the fuel energy consumed refers to the total energy consumed by the heat pump compressor, evaporator fan, condenser pump, and parasitic loads. It is assumed that the parasitic loads for a heat pump water heater do not contribute to heating the water (ref. Heat Pump Water Heater).
+
+The Energy Factor is calculated at the end of the 24-hour simulation period.
+
+\begin{equation}
+EF = \frac{{{m_{total}}{c_p}\left( {57.2 - 14.4} \right)}}{{{E_{total}}}}
+\end{equation}
+
+where
+
+\emph{m\(_{total}\)} = total water mass of all six draws
+
+\emph{c\(_{p}\)} = specific heat of water
+
+\emph{E\(_{total}\)} = total fuel energy consumed over 24 hours (including parasitics)
+
+Under certain input parameters, the rating method will not succeed and a warning message will be generated.~ Problems occur when inputs do not allow the tank to recover to the setpoint temperature within the test period.~ This can occur if the maximum heater capacity is undersized, or if the deadband temperature difference is large enough that the first draw of the test does not trigger the heater to come on.~ In either case, the Recovery Efficiency test will not compute properly because recovery to the setpoint was not achieved.
+
+\subsubsection{References}\label{references-053}
+
+10CFR430.~ \emph{Title 10, Code of Federal Regulations, Part 430 - Energy Conservation Program for Consumer Products, Appendix E to Subpart B - Uniform Test Procedure for Measuring the Energy Consumption of Water Heaters}.
+
+\subsection{Heat Pump Water Heater}\label{heat-pump-water-heater}
+
+\subsubsection{Overview}\label{overview-029}
+
+The input objects \lstinline!WaterHeater:HeatPump:*! provide models for a heat pump water heater (HPWH) that is a compound object consisting of a water heater tank (e.g., \lstinline!WaterHeater:Mixed! or \lstinline!WaterHeater:Stratified!), a direct expansion (DX) ``coil'' (i.e., an air-to-water DX compression system which includes a water heating coil, air coil, compressor, and water pump), and a fan to provide air flow across the air coil associated with the DX compression system. These objects work together to model a system which heats water using zone air, outdoor air, or a combination of zone and outdoor air as the primary heat source.
+
+There are two types of heat pump water heater models available:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\tightlist
+\item
+  \lstinline!WaterHeater:HeatPump:PumpedCondenser!: This model is used to represent a heat pump water heater where water is removed from the tank, pumped through a condenser, and returned to the tank at a higher temperature.
+\item
+  \lstinline!WaterHeater:HeatPump:WrappedCondenser!: This model is used for heat pump water heaters that are more typical in the residential building context where the heating coil is wrapped around or submerged in the tank.
+\end{enumerate}
+
+Each type of \lstinline!WaterHeater:HeatPump:*! object is compatible with certain \lstinline!Coil:WaterHeating:AirToWaterHeatPump:*! objects as shown in the following table:
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+WaterHeater:HeatPump:* & WaterHeater:* \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+WaterHeater:HeatPump:* & WaterHeater:* \tabularnewline
+\midrule
+\endhead
+
+PumpedCondenser & Pumped \tabularnewline
+PumpedCondenser & VariableSpeed \tabularnewline
+WrappedCondenser & Wrapped \tabularnewline
+\bottomrule
+\end{longtable}
+
+Additionally the \lstinline!WaterHeater:HeatPump:WrappedCondenser! object is only compatible with stratified tanks. Therefore \lstinline!WaterHeater:HeatPump:*! has the following tank compatibility matrix:
+
+\begin{longtable}[c]{@{}lll@{}}
+\toprule
+WaterHeater:HeatPump:* & \multicolumn{2}{c}{WaterHeater:*} \tabularnewline
+\cmidrule{2-3}
+& Mixed & Stratified \tabularnewline
+\midrule
+\endhead
+
+Pumped & X & X \tabularnewline
+Wrapped &  & X \tabularnewline
+\bottomrule
+\end{longtable}
+
+Numerous configurations of tank location, inlet air source, and DX coil compressor location can be modeled. The DX coil compressor may be located in a zone, outdoors, or the ambient temperature surrounding the compressor may be scheduled. The location of the compressor controls the operation of its crankcase heater. The water heater tank location is specified in the water heater tank object and is independent of the compressor location. In addition, the inlet air configuration may be specified in one of several ways. The heat pump water heater air coil and fan assembly may draw its inlet air from the zone and outdoor air using an optional mixer and splitter assembly as shown in the first figure below. When used, the mixer and splitter air streams are controlled by a single inlet air mixer schedule. When the HPWH draws its inlet air solely from a zone, the mixer/splitter assembly is not required as shown in the second figure below. In this case, the inlet air to the evaporator and fan assembly is made up entirely of zone air and the heat pump outlet air is directed back to the zone. The final figure illustrates a HPWH that draws its inlet air solely from outdoors and exhausts its outlet air outdoors as well. Each of these configurations may also be connected to a plant hot water loop (via the water heater tank use nodes).
+
+\begin{figure}[hbtp] % fig 312
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6855.png}
+\caption{Schematic of a heat pump water heater using optional mixer/splitter nodes \protect \label{fig:schematic-of-a-heat-pump-water-heater-using-001}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 313
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6856.png}
+\caption{Schematic of a Heat Pump Water Heater with Inlet Air from a Zone \protect \label{fig:schematic-of-a-heat-pump-water-heater-with}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 314
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image6857.png}
+\caption{Schematic of a Heat Pump Water Heater with Inlet Air from Outdoors \protect \label{fig:schematic-of-a-heat-pump-water-heater-with-001}}
+\end{figure}
+
+Note: The water heater tank location shown in the figures above is completely independent of the heat pump water heater's inlet air configuration and its compressor location. The water heater tank may be located outdoors, in a zone, or the ambient temperature surrounding the tank can be scheduled as described in the mixed water heater section below.
+
+\subsubsection{Model Description}\label{model-description-016}
+
+The heat pump water heater input requires a compressor setpoint temperature schedule and dead band temperature difference, which are independent from the setpoint temperature schedule and dead band temperature difference for the heater (element or burner) associated with the water heater tank. The cut-in temperature for the heat pump compressor is defined as the heat pump compressor's setpoint temperature minus its dead band temperature difference.
+
+\begin{equation}
+{T_{HP,\,cut - in}}\,\, = \,\,{T_{HP,set\,point}}\,\, - \,\,{T_{HP,dead\,band}}
+\end{equation}
+
+where:
+
+\({T_{HP,\,cut - in}}\) ~~~~ = Cut-in temperature for the heat pump compressor (°C)
+
+\({T_{HP,set\,point}}\) ~~ = Heat pump compressor setpoint temperature (°C)
+
+\({T_{HP,dead\,band}}\) = Heat pump compressor dead band temperature difference (°C)
+
+In this model, the heat pump water heater's DX compression system is considered the primary heat source and the water tank's heater (element or burner) provides supplemental heat as necessary. Therefore, the cut-in temperature for the heat pump compressor (setpoint minus dead band temperature difference) is usually higher than the setpoint temperature for the heater (element or burner) in the associated water heater tank object. At times when the water heater tank setpoint temperature is greater than the cut-in temperature of the heat pump compressor, the heat pump compressor is disabled and the tank's heater is used to heat the water.
+
+The simulation starts by first calculating the air conditions entering the air coil (evaporator)/fan assembly based on the inlet air configuration of the heat pump water heater and the presence of the optional mixer/splitter nodes. When the HPWH draws its inlet air from the zone and outdoors using the optional mixer/splitter nodes (i.e., Inlet Air Configuration = Zone and Outdoor Air), the inlet air conditions are calculated as follows:
+
+\begin{equation}
+Frac = GetScheduleValue(MixerInletAirSchedule)
+\end{equation}
+
+\begin{equation}
+{T_{inlet}} = {T_{outdoor}}\left( {Frac} \right) + {T_{zone}}\left( {1 - Frac} \right)
+\end{equation}
+
+\begin{equation}
+{\omega_{inlet}} = {\omega_{outdoor}}\left( {Frac} \right) + {\omega_{zone}}\left( {1 - Frac} \right)
+\end{equation}
+
+where:
+
+\(Frac\) ~ = current value of the inlet air mixer schedule (fraction of outdoor air, 0-1)
+
+\({T_{inlet}}\) ~ = inlet air dry-bulb temperature to the HPWH evaporator/fan assembly (°C)
+
+\({T_{outdoor}}\) ~ = outdoor air dry-bulb temperature (°C)
+
+\({T_{zone}}\) ~ = zone (exhaust) air dry-bulb temperature (°C)
+
+\({\omega_{inlet}}\) ~ = inlet air humidity ratio to the HPWH evaporator/fan assembly (kg/kg)
+
+\({\omega_{outdoor}}\) = outdoor air humidity ratio (kg/kg)
+
+\({\omega_{zone}}\) ~ = zone (exhaust) air humidity ratio (kg/kg)
+
+When the heat pump water heater draws its inlet air solely from the zone (i.e., Inlet Air Configuration = Zone Air Only), the inlet air conditions to the evaporator/fan assembly are simply set equal to the zone (exhaust) air conditions. If the heat pump water heater draws its inlet air solely from outdoors (i.e., Inlet Air Configuration = Outdoor Air Only), the inlet air conditions to the evaporator/fan assembly are simply set equal to the outdoor air conditions. When the inlet air to the heat pump water heater evaporator and fan assembly is scheduled (i.e., Inlet Air Configuration = Schedule), the inlet air conditions are determined directly from the user-supplied schedules as follows.
+
+\begin{equation}
+{T_{inlet}} = GetScheduleValue(InletAirTemperatureSchedule)
+\end{equation}
+
+\begin{equation}
+RHinlet = GetScheduleValue(InletAirHumiditySchedule)
+\end{equation}
+
+\begin{equation}
+{\omega_{inlet}} = PsyWFnTdbRhPb({T_{inlet}},R{H_{inlet}},OutBaroPress)
+\end{equation}
+
+where:
+
+\(R{H_{inlet}}\) = inlet air relative humidity to heat pump water heater evaporator/fan assembly (0-1)
+
+\(PsyWFnTdbRhPb\) = psychrometric function returning air humidity ratio given dry-bulb temperature, relative humidity, and barometric pressure
+
+\(OutBaroPress\) = outdoor barometric pressure (Pa)
+
+For each simulation time step, the heat pump water heating capacity, energy use, and air-side/water-side mass flow rates are set to zero and the water heater tank is simulated with the heat pump compressor disabled when any of the following conditions apply:
+
+·~~~~~~~~the HPWH is scheduled off by its availability schedule,
+
+·~~~~~~~~the water heater tank setpoint temperature is greater than or equal to the heat pump compressor cut-in temperature,
+
+·~~~~~~~~the inlet air dry-bulb temperature to the evaporator/fan assembly is less than the Minimum Inlet Air Temperature for Heat Pump Compressor Operation (as specified by the user in the HPWH input object), or
+
+·~~~~~~~~the HPWH setpoint temperature is greater than or equal to the Maximum Temperature Limit (specified in the Water Heater:Mixed object).
+
+Otherwise, simulation of the heat pump water heater is based on its current mode of operation. This mode of operation is either floating (heat pump compressor is off and tank water temperature has not fallen below the heat pump compressor cut-in temperature) or heating (tank water temperature dropped below the compressor cut-in temperature on a previous time step but was unable to reach the compressor setpoint temperature). Each mode is handled differently and they will be discussed separately.
+
+If the heat pump water heater is using the stratified tank model, then there is more than one value for the tank temperature.~ The model includes input for where the heat pump controls detect the temperature. The input data in the associated WaterHeater:Stratified includes up to two heights in the tank where the temperature is measured and a weight associated with each. The associated stratified tank nodes are selected based on these heights. When the heat pump model needs to evaluate the tank temperature of a stratified tank, it evaluates the temperature at the tank nodes associated with these locations.
+
+\subsubsection{Float Mode}\label{float-mode-000}
+
+When the heat pump water heater tank temperature is floating between the heat pump compressor's cut-in and cut-out temperatures at the end of the previous simulation time step, both the heat pump compressor and the water heater tank's heating element are disabled and a resulting tank temperature is calculated. If the resulting tank temperature is below the heat pump compressor's cut-in temperature, the heat pump compressor part-load ratio is estimated using the ratio of the temperature differences shown below. The part-load ratio can not be less than zero or greater than one.
+
+\begin{equation}
+PLR = MIN\left( {1.0,\,\,MAX\left( {0.0,\,\,\left( {\frac{{{T_{HP,\,cut - in}} - {T_{tank,float}}}}{{{T_{tank,initial}} - {T_{tank,float}}}}} \right)} \right)} \right)
+\end{equation}
+
+where:
+
+\(PLR\) ~~~~~~~~ = part-load ratio of the heat pump water heater compressor
+
+\(Ttank,float\) ~~~ = tank temperature in float mode when heating capacity is set to zero(°C)
+
+\({T_{tank,initial}}\) ~~~ = tank temperature at the beginning of the simulation time step (°C)
+
+Since the pump and fan are assumed to cycle on and off with the heat pump compressor, the average condenser water (for pumped condensers only) and evaporator air mass flow rates for the simulation time step are calculated based on the PLR calculated above:
+
+\begin{equation}
+{\dot m_{water,avg}} = \dot Vwater\left( {{\rho_{water}}} \right)\left( {PLR} \right)
+\end{equation}
+
+\begin{equation}
+\dot mair,avg = \dot Vair\left( {{\rho_{air}}} \right)\left( {PLR} \right)
+\end{equation}
+
+where:
+
+\(\dot mwater,avg\) ~~~~~~ = average condenser water mass flow rate for the time step (kg/s)
+
+\(\dot Vwater\) ~~~~~~~~~~~ = condenser water volumetric flow rate, user input (m\(^{3}\)/s)
+
+\({\rho_{water}}\) ~~~~~~~~~~~ = density of condenser inlet water (kg/m\(^{3}\))
+
+\(\dot mair,avg\) ~~~~~~~~ = average evaporator/fan air mass flow rate for the time step (kg/s)
+
+\(\dot Vair\) ~~~~~~~~~~~~~~ = evaporator/fan air volumetric flow rate, user input (m\(^{3}\)/s)
+
+\({\rho_{air}}\) ~~~~~~~~~~~~~ = density of evaporator/fan inlet air (kg/m\(^{3}\))
+
+The water tank temperature is then calculated based on heat pump operation at the part-load ratio estimated above and with the water tank's heating element enabled. If the resulting water tank temperature is above the heat pump compressor's setpoint (cut-out) temperature, then the part-load ratio is reduced and the water heater tank is simulated again. The process is performed iteratively until the part-load ratio of the heat pump compressor achieves the desired setpoint temperature (to the extent possible).
+
+\subsubsection{Heating Mode}\label{heating-mode-000}
+
+When the HPWH is in heating mode at the end of the previous simulation time step (i.e., the heat pump compressor operated during the previous simulation time step but was unable to achieve the setpoint temperature), both the heat pump compressor and the water heater tank's heating element are enabled. The part-load ratio of the heat pump compressor is set to 1, and the condenser water (for pumped condensers) and evaporator air mass flow rates are set to their maximum flow rates.
+
+\begin{equation}
+{\dot m_{water,avg}} = {\dot V_{water}}\left( {{\rho_{water}}} \right)
+\end{equation}
+
+\begin{equation}
+\dot mair,avg = \dot Vair\left( {\rho air} \right)
+\end{equation}
+
+If the resulting tank temperature is above the heat pump compressor's setpoint (cut-out) temperature, the part-load ratio of the heat pump compressor is reduced and the water heater tank is simulated again. The process is performed iteratively until the part-load ratio of the heat pump compressor achieves the desired setpoint temperature (to the extent possible).
+
+The air-side outlet conditions of the HPWH are calculated through simulation of the fan and DX coil with either a blow through or draw through fan placement (user selectable). If mixer/splitter nodes are used, the HPWH model splits the heat pump outlet air mass flow rate with exhaust air flow equaling the outdoor air flow, and the balance of the outlet air being sent to the zone supply air node (i.e., ensures that the heat pump water heater does not contribute to zone pressurization or depressurization). Calculations of heat pump water heating capacity, energy use, air-side performance, and water-side temperature difference are performed in the associated DX Coil object. See the engineering reference section for the Coil:WaterHeating:AirToWaterHeatPump object for details.
+
+\subsubsection{Model Outputs}\label{model-outputs-000}
+
+After completing the float mode or heating mode calculations and the final part-load ratio has been determined, the output (report) variables are calculated as follows:
+
+\begin{equation}
+Heat\,Pump\,Water\,Heater\,Compressor\,Part{\rm{ - }}Load\,Ratio = PLR\,\,
+\end{equation}
+
+\begin{equation}
+Heat\,Pump\,Water\,Heater\,\,On{\rm{ - }}Cycle\,Parasitic\,Electric\,Power\,(W)\,\, = \,\,{P_{parasitic,on}}\left( {PLR} \right)
+\end{equation}
+
+\begin{equation}
+\begin{split}
+Heat\,Pump\,Water\,Heater\,\,On{\rm{ - }}Cycle\,Parasitic\,Electric\,Consumption\,(J)\,\, = \\{P_{parasitic,on}}\left( {PLR} \right)\left( {3600} \right){t_{sys}}
+\end{split}
+\end{equation}
+
+\begin{equation}
+\begin{split}
+Heat\,Pump\,Water\,Heater\,\,Off{\rm{ - }}Cycle\,Parasitic\,Electric\,Power\,(W)\,\, = \\{P_{parasitic,off}}\left( {1 - PLR} \right)
+\end{split}
+\end{equation}
+
+\begin{equation}
+\begin{split}
+Heat\,Pump\,Water\,Heater\,\,Off{\rm{ - }}Cycle\,Parasitic\,Electric\,Consumption\,(J)\,\, = \\{P_{parasitic,off}}\left( {1 - PLR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)
+\end{split}
+\end{equation}
+
+where:
+
+\({P_{parasitic,on}}\) ~~ = on-cycle parasitic electric load, user input (W)
+
+\({P_{parasitic,off}}\) ~ = off-cycle parasitic electric load, user input (W)
+
+\({t_{sys}}\) ~~~~~~~~~~~~ = HVAC system simulation time step (hours)
+
+Note: All heat pump water heater output variables, including off-cycle ancillary electric power and consumption, equal 0 when the heat pump water heater availability schedule equals 0 (i.e., the heat pump water heater is scheduled OFF).
+
+\subsection{Stratified Water Thermal Tank}\label{stratified-water-thermal-tank}
+
+The input objects WaterHeater:Stratified and ThermalStorage:ChilledWater:Stratified provide models for a stratified water thermal tank that divides the water tank into multiple nodes of equal volume.~ This model is used for both the stratified water heater and the stratified chilled water storage tank. The nodes are coupled by vertical conduction effects, internode fluid flow, and temperature inversion mixing.~ The object simultaneously solves the differential equations governing the energy balances on the nodes using the Forward-Euler numerical method.~ The system time step is divided into one second substeps that allow the simulation to capture events that occur on a very short time scale.
+
+\subsubsection{Energy Balance}\label{energy-balance-1}
+
+Similar to the well-mixed model, the stratified model solves the same fundamental differential equation governing the energy balance on a mass of water:
+
+\begin{equation}
+m{c_p}\frac{{dT}}{{dt}} = {q_{net}}
+\end{equation}
+
+where
+
+\emph{m} = mass of water
+
+\emph{c\(_{p}\)} = specific heat of water
+
+\emph{T} = temperature of water
+
+\emph{t} = time
+
+\emph{q\(_{net}\)} = net heat transfer rate
+
+The difference for the stratified model is that it must solve the energy balance on \emph{n} number of nodes simultaneously.~ Node 1 is at the top of the water tank and node \emph{n} is at the bottom of the water tank.
+
+\begin{equation}
+{m_n}{c_p}\frac{{d{T_n}}}{{dt}} = {q_{net,n}}
+\end{equation}
+
+where
+
+\emph{m\(_{n}\)} = mass of water for node \emph{n}
+
+\emph{c\(_{p}\)} = specific heat of water
+
+\emph{T\(_{n}\)} = temperature of water for node \emph{n}
+
+\emph{t} = time
+
+\emph{q\(_{net,n}\)} = net heat transfer rate for node \emph{n}
+
+The net heat transfer rate \emph{q\(_{net}\)} is the sum of gains and losses due to multiple heat transfer pathways.
+
+\begin{equation}
+  \begin{array}{ll}
+    q_{net,n} &= q_{heater,n} + q_{oncycpara,n} + q_{offcycpara,n} + q_{oncycloss,n} + q_{offcycloss,n} \\ 
+              &+ q_{cond,n} + q_{use,n} + q_{source,n} + q_{flow,n} + q_{invmix,n}
+  \end{array}
+\end{equation}
+
+where
+
+\emph{q\(_{heater,n}\)} = heat added by Heater 1 or Heater 2
+
+\emph{q\(_{oncycpara,n}\)} = heat added due to on-cycle parasitic loads (zero when off)
+
+\emph{q\(_{offcycpara,n}\)} = heat added due to off-cycle parasitic loads (zero when on)
+
+\emph{q\(_{oncycloss,n}\)} = heat transfer to/from the ambient environment (zero when off)
+
+\emph{q\(_{offcycloss,n}\)} = heat transfer to/from the ambient environment (zero when on)
+
+\emph{q\(_{cond,n}\)} = heat transfer due to conduction between the node above and below
+
+\emph{q\(_{use,n}\)} = heat transfer to/from the use side plant connections
+
+\emph{q\(_{source,n}\)} = heat transfer to/from the source side plant connections
+
+\emph{q\(_{flow,n}\)} = heat transfer due to fluid flow from the node above and below
+
+\emph{q\(_{invmix,n}\)} = heat transfer due to inversion mixing from the node above and below
+
+\emph{q\(_{oncycloss,n}\)} and \emph{q\(_{offcycloss,n}\)} are defined as:
+
+\begin{equation}
+{q_{oncycloss,n}} = ({UA_{tank}} + UA_add,n)({T_{amb}} - {T_n})
+\end{equation}
+
+\begin{equation}
+{q_{offcycloss,n}} = ({UA_{tank} + UA_{flue}})({T_{amb}} - {T_n})
+\end{equation}
+
+where
+
+\emph{UA\(_{tank}\)} = loss coefficient to ambient environment for the tank
+
+\emph{UA\(_{add,n}\)} = additional node loss coefficient
+
+\emph{UA\(_{flue}\)} = additional off-cycle flue loss coefficient to ambient environment (zero when on)
+
+\emph{T\(_{amb}\)} = temperature of ambient environment
+
+\emph{q\(_{cond,n}\)} is defined as:
+
+\begin{equation}
+{q_{cond,n}} = \frac{{k{A_{n + 1}}}}{{{L_{n + 1}}}}({T_{n + 1}} - {T_n}) + \frac{{k{A_{n - 1}}}}{{{L_{n - 1}}}}({T_{n - 1}} - {T_n})
+\end{equation}
+
+where
+
+\emph{k} = fluid thermal conductivity of water, 0.6 W/m-K
+
+\emph{A\(_{n+1}\)} = shared surface area between node \emph{n} and node \emph{n+1}
+
+\emph{L\(_{n+1}\)} = distance between the center of mass of node \emph{n} and n\emph{+1}
+
+\emph{T\(_{n+1}\)} = temperature of node \emph{n+1}
+
+\emph{A\(_{n-1}\)} = shared surface area between node \emph{n} and node \emph{n-1}
+
+\emph{L\(_{n-1}\)} = distance between the center of mass of node \emph{n} and n\emph{-1}
+
+\emph{T\(_{n-1}\)} = temperature of node \emph{n-1}
+
+\emph{q\(_{use,n}\)}, and \emph{q\(_{source,n}\)} are defined as:
+
+\begin{equation}
+{q_{use}} = {\varepsilon_{use}}{\dot m_{use}}{c_p}\left( {{T_{use}} - T} \right)
+\end{equation}
+
+\begin{equation}
+{q_{source}} = {\varepsilon_{source}}{\dot m_{source}}{c_p}\left( {{T_{source}} - T} \right)
+\end{equation}
+
+where
+
+\emph{e\(_{use}\)} = heat exchanger effectiveness for the use side plant connections
+
+\({\dot m_{use}}\) = mass flow rate for the use side plant connections
+
+\emph{T\(_{use}\)} = inlet fluid temperature of the use side plant connections
+
+\emph{e\(_{source}\)} = heat exchanger effectiveness for the source side plant connections
+
+\({\dot m_{source}}\) = mass flow rate for the source side plant connections
+
+\emph{T\(_{source}\)} = inlet fluid temperature of the source side plant connections
+
+\emph{q\(_{flow,n}\)} is defined as:
+
+\begin{equation}
+{q_{flow,n}} = {\dot m_{n + 1}}{c_p}({T_{n + 1}} - {T_n}) + {\dot m_{n - 1}}{c_p}({T_{n - 1}} - {T_n})
+\end{equation}
+
+where
+
+\({\dot m_{n + 1}}\) = mass flow rate from node \emph{n+1}
+
+\({\dot m_{n - 1}}\) = mass flow rate from node \emph{n-1}
+
+\emph{q\(_{invmix,n}\)} is defined as:
+
+\begin{equation}
+{q_{invmix,n}} = {\dot m_{invmix,n + 1}}{c_p}({T_{n + 1}} - {T_n}) + {\dot m_{invmix,n - 1}}{c_p}({T_{n - 1}} - {T_n})
+\end{equation}
+
+where
+
+\({\dot m_{invmix,n + 1}}\) = mass flow rate from node \emph{n+1} due to temperature inversion mixing
+
+\({\dot m_{invmix,n - 1}}\) = mass flow rate from node \emph{n-1} due to temperature inversion mixing
+
+Inversion mixing occurs when the node below is warmer than the node above.~ The difference in temperatures drives a difference in density that causes the nodes to mix.~ Usually inversion mixing occurs very rapidly.~ In this algorithm, the inversion mixing rate is selected to be the maximum value that will provide a stable solution given the node mass and the substep interval:
+
+\begin{equation}
+{\dot m_{invmix}} = 0.5*{m_n}/\Delta t
+\end{equation}
+
+where
+
+\emph{Dt} = the substep time interval.
+
+The use and source fluid steam outlet temperatures calculation procedure depends on the values of the effectiveness.~ If the effectiveness is 1.0, then complete mixing of these fluid steam and the tank water is assumed.~ In this case the outlet temperatures for the use and source streams will be simply the tank water temperatures at point of the outlet nodes. When the effectiveness is less than 1.0, an indirect heat exchange is assumed between the use or source stream and the water in the stratified thermal storage tank.~ When the effectiveness is less than 1.0, the use and source outlet temperatures are calculated using \emph{Q\(_{use}\)} and \emph{Q\(_{source}\)}, and energy balance equations as follows:
+
+\begin{equation}
+{T_{use\;out,\,n}} = {T_{use,\,n}} + \frac{{{q_{use,n}}}}{{{{\dot m}_{use}}{c_p}}}
+\end{equation}
+
+\begin{equation}
+{T_{source\;out,\,n}} = {T_{source,\,n}} - \frac{{{q_{source,n}}}}{{{{\dot m}_{source}}{c_p}}}
+\end{equation}
+
+~where,
+
+\emph{T\(_{use\, out}\)} = outlet fluid temperature of the use side plant connections
+
+\emph{T\(_{source\, out}\)} = outlet fluid temperature of the source side plant connections
+
+\subsubsection{Numerical Solution}\label{numerical-solution}
+
+The system of simultaneous differential equations is solved using the Forward-Euler numerical method.~ The system time step is divided into one-second substeps.~ The new temperature for a given node is calculated using the following equation:
+
+\begin{equation}
+{T_n} = {T_{n,old}} + \frac{{{q_{net,n}}\Delta t}}{{{m_n}{c_p}}}
+\end{equation}
+
+All node temperatures for \emph{q\(_{net,n}\)} are the old temperatures from the previous substep.
+
+Before each system time step is calculated the following evaluations are made:
+
+§~Use and source inlet flow rates are applied to the inlet nodes
+
+§~Internode flow is determined and net flow rates are determined
+
+Before each substep is calculated, the following evaluations are made:
+
+1)~~~Thermostatic controls for heater 1 and heater 2 are evaluated to determine if the heater elements should turn on or off
+
+2)~~~Node 1 temperature is compared against the maximum limit to determine if venting is necessary
+
+3)~~~Adjoining node temperatures are compared to determine if there are any temperature inversions for which the inversion mixing rate should be used.
+
+The solution continues looping through all substeps until the system time step is completed.
+
+\subsubsection{References}\label{references-1-017}
+
+Duffie, J., and W. Beckman. 1980. \emph{Solar Engineering of Thermal Processes}.~ John Wiley \& Sons.
+
+Newton, B. 1995. \emph{Modeling of Solar Storage Tanks}.~ Master's Dissertation, University of Wisconsin-Madison.
+
+\subsection{Water Heating Sizing}\label{water-heating-sizing}
+
+Some inputs for water heaters can be autosized using the input object WaterHeater:Sizing.~ This section describes the sizing calculations for water heaters.~ There are six general methods for sizing tank volume and heating capacity.
+
+\subsubsection{Autosizing Tank Volume}\label{autosizing-tank-volume}
+
+The volume a water heater can be sized in the following ways depending on the design method chosen by the user.
+
+\begin{itemize}
+  \item Peak Draw. The volume is determined from the loop design flow rate.~ The water heater is positioned on the supply side of a plant loop.~ After the plant sizing routines have run, the model~ obtains the design flow rate for all components on the demand side.~ The tank volume is then: \(V = {\dot V_{loop.des}}*{t_{draw}}\) ,
+
+  \item Residential HUD-FHA Minimum. The volume is determined from a set of rules defined by the table below.~ This is from Chapter 48 of 1999 ASHRAE Handbook HVAC Applications, Americal Society of Heating Refrigeration and Air-conditioning Engineeers, Atlanta GA.~ (also used in the Building America Benchmark).
+\end{itemize}
+
+% table 85
+{\scriptsize
+\begin{longtable}[c]{>{\raggedright}p{0.8in}p{0.35in}p{0.35in}p{0.35in}p{0.35in}p{0.35in}p{0.35in}p{0.35in}p{0.35in}p{0.35in}p{0.35in}p{0.35in}p{0.35in}}
+\caption{Residential HUD-FHA Minimum \label{table:residential-hud-fha-minimum}} \tabularnewline
+\toprule 
+\multicolumn{13}{p{5in}}{\raggedright Residential HUD-FHA Minimum DHW Storage and Burner Capacity (ASHRAE 1999)} \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Residential HUD-FHA Minimum} \tabularnewline
+\toprule 
+\multicolumn{13}{p{5in}}{\raggedright Residential HUD-FHA Minimum DHW Storage and Burner Capacity (ASHRAE 1999)} \tabularnewline
+\midrule
+\endhead
+
+\# Bedrooms & 1 & 2 & 2 & 2 & 3 & 3 & 3 & 4 & 4 & 4 & 5 & 6 \tabularnewline
+\# Bathrooms & All & \(\le 1.5\) & 2-2.5 & \(\ge 3\) & \(\le 1.5\) & 2-2.5 & \(\ge 3\) & \(\le 1.5\) & 2-2.5 & \(\ge 3\) & All & All \tabularnewline
+Gas &  &  &  &  &  &  &  &  &  &  &  &  \tabularnewline
+\;\;Storage (gal) & 20 & 30 & 30 & 40 & 30 & 40 & 40 & 40 & 40 & 50 & 50 & 50 \tabularnewline
+\;\;Burner (kBtu/hr) & 27 & 36 & 36 & 36 & 36 & 36 & 38 & 36 & 38 & 38 & 47 & 50 \tabularnewline
+Electric &  &  &  &  &  &  &  &  &  &  &  &  \tabularnewline
+\;\;Storage (gal) & 20 & 30 & 40 & 50 & 40 & 50 & 50 & 50 & 50 & 66 & 66 & 80 \tabularnewline
+\;\;Burner (kW) & 2.5 & 3.5 & 4.5 & 5.5 & 4.5 & 5.5 & 5.5 & 5.5 & 5.5 & 5.5 & 5.5 & 5.5 \tabularnewline
+\bottomrule
+\end{longtable}}
+
+\begin{itemize}
+  \item Per Person. The tank volume is determined by summing the design level of people in the model and multiplying by a user-entered volume per person factor.
+
+  \item Per Floor Area. The tank volume is determined by summing the floor area in all the zones in the model and multiplying by a user-entered volume per floor area factor.
+
+  \item Per Unit. The tank volume is determined by multiplying a user-entered volume per unit and a user-entered number of units.
+
+  \item Per Solar Collector Area. The tank volume is determined by summing the collector area in all the hot water solar collectors in the model and multiplying by a user-entered volume per collector area factor.
+\end{itemize}
+
+\subsubsection{Autosizing Heater Capacity}\label{autosizing-heater-capacity}
+
+The heater capacity can be sized in the following ways depending on the design method chosen by the user.
+
+\begin{itemize}
+  \item Peak Draw. The heater capacity is determined from the tank volume, assumed start and finish temperatures and a user defined time for recovery.~ The heater capacity is then
+\end{itemize}
+
+\begin{equation}
+  q_{heat} = V\rho C_p \PB{T_{finish} - T_{start}}
+\end{equation}
+
+where,
+
+\begin{equation}
+{T_{finish}} = 57.2C
+\end{equation}
+
+\begin{equation}
+{T_{start}} = 14.4C
+\end{equation}
+
+·~~~~~~~~Residential HUD-FHA Minimum.~ The heater capacity is determined from a set of rules defined by the table above.~ This is from 1999 ASHRAE Handbook HVAC Applications, Americal Society of Heating Refrigeration and Air-conditioning Engineeers, Atlanta GA.~ (also used the Building America Benchmark).
+
+·~~~~~~~~Per Person.~ The heater capacity is determined by summing the design level of people in the model and using a user-entered factor for recovery capacity per person.~ The heater capacity is then:
+
+\begin{equation}
+{q_{heat}} = \frac{{{N_{people}}{f_{{\mathop{\rm Re}\nolimits} {\mathop{\rm cov}} eryPerPerson}}({T_{finish}} - {T_{start}})\rho \,{c_p}}}{{3600}}
+\end{equation}
+
+·~~~~~~~~Per Floor Area.~ The heater capacity is determined by summing the floor area in all the zones in the model and using a user-entered factor for recovery capacity per floor area.~ The heater capacity is then:
+
+\begin{equation}
+  q_{heat} = \frac{A_{floors}f_{RecoveryPerFloorArea}\PB{T_{finish} - T_{start}}\rho C_p}{3600}
+\end{equation}
+
+·~~~~~~~~Per Unit.~ The heater capacity is determined from a user-entered Recovery Capacity per unit and a user-entered number of units.~ The heater capacity is then:
+
+\begin{equation}
+{q_{heat}} = \frac{{{N_{units}}{f_{{\mathop{\rm Re}\nolimits} {\mathop{\rm cov}} eryPerUnit}}({T_{finish}} - {T_{start}})\rho \,{c_p}}}{{3600}}
+\end{equation}
+
+·~~~~~~~~Per Solar Collector Area. The water heater is assumed to be used for solar hot water storage and the heater capacity is set to zero.
+
+\subsubsection{Autosizing Tank Height}\label{autosizing-tank-height}
+
+If the water heater is Stratified, then the geometry is important and the height of the tank can be scaled with changes in volume.~ For tank shapes of Vertical Cylinder, the user defined height aspect ratio, \emph{AR},~ is used to calculate a tank height, \emph{H}, using
+
+\begin{equation}
+H = {\left( {\frac{{4\,V\;A{R^2}}}{\pi }} \right)^{1/3}}
+\end{equation}
+
+\subsubsection{Autosizing Plant Connection Flow Rates}\label{autosizing-plant-connection-flow-rates}
+
+When the water thermal tank is connected to a plant loop, it is convient to autosize the design volume flow rates through the plant connections.~ When the water thermal tank is connected to the supply side of plant loop and flow rates are autosized, the flow rate is the sum of the flow requests of all the various components on the demand side of that plant loop.~ When the water thermal tank is connected on the demand side of a plant loop (e.g.~as for indirect water heating with a boiler) and flow rates are autosized, the design flow rates are calculated with the following equation,
+
+\begin{equation}
+\dot V =  - \left( {\frac{V}{{{t_{{\mathop{\rm Re}\nolimits} {\mathop{\rm cov}} er}} * 3600 * \varepsilon }}} \right) * Ln\left[ {\frac{{\left( {{T_{PlantDesign}} - {T_{Setpo{\mathop{\rm int}} }}} \right)}}{{\left( {{T_{PlantDesign}} - {T_{start}}} \right)}}} \right]
+\end{equation}
+
+where
+
+\emph{V} = volume of the tank
+
+\({t_{{\mathop{\rm Re}\nolimits} {\mathop{\rm cov}} er}}\) ~ = User parameter for the time it takes for the tank to recover from assumed starting temperature to an assumed setpoint temperature.~ For water heaters, the starting temperature is 14.4ºC and the final assumed setpoint temperature is 57.2ºC.~ For chilled water tanks, the starting temperature is 14.4 ºC and the final temperature is 9.0ºC.
+
+\(\varepsilon\) ~ = \emph{e\(_{use}\)} ~~or \emph{e\(_{source}\)}
+
+\({T_{PlantDesign}}\) = the exit temperature specified in the Plant Sizing object
+
+\({T_{setpo{\mathop{\rm int}} }}\) ~ = ~ the final tank temperature of 57.2ºC for heaters and 9.0ºC for chilled water tanks.
+
+\({T_{start}}\) ~ = the initial tank temperature of 14.4ºC
+
+If the demand side connections are autosized and a water heater's tank volume is autosized, then the problem cannot be readily solved in EnergyPlus because the demand side connection flows need to be reported earlier in the simulation and the tank volume is not yet available.~ This situation is resolved by using an interim, nominal tank volume for sizing the connections and the actual volume is calculated later in the simulation.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/zone-controls.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/zone-controls.tex
new file mode 100644
index 00000000000..608ed7f0652
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/zone-controls.tex
@@ -0,0 +1,424 @@
+\section{Zone Controls }\label{zone-controls}
+
+\subsection{Thermostatic Zone Control}\label{thermostatic-zone-control}
+
+The input object ZoneControl:Thermostat provides a way for the zone to be controlled to a specified temperature.~ ZoneControl:Thermostat references a control type schedule and one or more control type objects which in turn reference one or more setpoint schedules.
+
+The control type schedule and the list of control type/name pairs are directly related.~ The schedule defines the type of control that is to be used during for each hour.~ Valid control types are
+
+0 - Uncontrolled (No specification or default)
+
+1 - Single Heating Setpoint
+
+2 - Single Cooling SetPoint
+
+3 - Single Heating/Cooling Setpoint
+
+4 - Dual Setpoint (Heating and Cooling) with deadband
+
+If the schedule referenced in the ZoneControl statement has a value of 4 for a particular hour, this indicates that during that hour ``dual setpoint with deadband control'' is to be used.~ The specific ``dual setpoint with deadband'' control object to be used is specified in the list of control type/name pairs.~ Then the specific control type objects reference the thermostat setpoint temperature schedule to be used.~ Because only one control can be specified for each control type in a ZoneControl statement, there are only four pairs possible in a particular ZoneControl type/name list.~ This is because individual controls can be defined hourly, thus giving the user a full range of flexibility.~ Since putting in the name of the control type directly in the schedule would be very cumbersome, the control types are assigned a number which is used in the hourly schedule profile.
+
+For more information see ZoneControl:Thermostat in the Input Output Reference and succeeding sections in this document.
+
+\subsection{Zone Thermostats}\label{zone-thermostats}
+
+The schema for the current set of four zone thermostats is given below.~ In each case, the keyword is accompanied by an identifying name and either one or two schedule names (depending on whether the control is a single or dual setpoint control).~ The schedule defines a temperature setpoint for the control type.~ The schedule would be defined through the standard schedule syntax described earlier in this document.~ For an uncontrolled zone no thermostat is specified or necessary.~ See the Input Output Reference for more details.
+
+The control type schedule and the list of control type/name pairs are directly related.~ The schedule defines the type of control that is to be used during for each hour.~ Valid Control Types are
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Control Type & Control Type Name/Object \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Control Type & Control Type Name/Object \tabularnewline
+\midrule
+\endhead
+
+0 & No thermal comfort control \tabularnewline
+1 & ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating \tabularnewline
+2 & ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling \tabularnewline
+3 & ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling \tabularnewline
+4 & ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint \tabularnewline
+\bottomrule
+\end{longtable}
+
+For the Uncontrolled case no heating or cooling requirement is calculated for the system to meet.
+
+CASE (0)
+
+~ ! Uncontrolled Zone
+
+~ LoadToHeatingSetPoint = 0.0
+
+~ LoadToCoolingSetPoint = 0.0
+
+~ ZoneSysEnergyDemand(ZoneNum)\%TotalOutputRequired = 0.0
+
+For the Single Heating Setpoint there would be a heating only thermostat.~ The setpoint can be scheduled and varied throughout the simulation but only heating is allowed with this control type.
+
+CASE (SingleHeatingSetPoint)
+
+~ ! Determine zone load based on
+
+~ ! Qload + Qsys = 0 and Qsys = mCp(Tsys-Tzone)
+
+~ ! System Load Sign Convention:
+
+~ !~~~~ - -\textgreater{} Cooling required to reach setpoint
+
+~ !~~~~ + -\textgreater{} Heating required to reach setpoint
+
+~ LoadToHeatingSetPoint = (TempDepZnLd(ZoneNum) *
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ TempZoneThermostatSetPoint(ZoneNum) --
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ TempIndZnLd(ZoneNum))
+
+~ IF ((ZoneSysEnergyDemand(ZoneNum)\%TotalOutputRequired - 1.0) \textless{} 0.0) THEN
+
+~~ ~DeadBandOrSetback(ZoneNum) = .TRUE.
+
+~ ENDIF
+
+For the Single Cooling Setpoint there would be a cooling only thermostat.~ The setpoint can be scheduled and varied throughout the simulation but only cooling is allowed with this control type.
+
+CASE (SingleCoolingSetPoint)
+
+~ LoadToCoolingSetPoint = (TempDepZnLd(ZoneNum) *
+
+~~~~~~~~~~~~~~~~~~~~~~ ~~~~TempZoneThermostatSetPoint(ZoneNum) --
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ TempIndZnLd(ZoneNum))
+
+~ ZoneSysEnergyDemand(ZoneNum)\%TotalOutputRequired = LoadToCoolingSetPoint
+
+~ IF ((ZoneSysEnergyDemand(ZoneNum)\%TotalOutputRequired + 1.0) \textgreater{} 0.0) THEN
+
+~~~ DeadBandOrSetback(ZoneNum) = .TRUE.
+
+~ ENDIF
+
+For the Single Heat Cool Setpoint there would be a cooling only thermostat there would be a heating and cooling thermostat.~ The setpoint can be scheduled and varied throughout the simulation for both heating and cooling. With this control type only 1 setpoint profile is needed or used.
+
+CASE (SingleHeatCoolSetPoint)
+
+~ LoadToHeatingSetPoint = (TempDepZnLd(ZoneNum) *
+
+~~~~~~~~~~~~~~~~~~~~~~~~~ ~TempZoneThermostatSetPoint(ZoneNum) --
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ TempIndZnLd(ZoneNum))
+
+~ LoadToCoolingSetPoint = (TempDepZnLd(ZoneNum) *
+
+~~~~~~~~~~~~~~~~~~~~~~~~~ ~TempZoneThermostatSetPoint(ZoneNum) --
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ TempIndZnLd(ZoneNum))
+
+! Possible combinations:
+
+! 1/~ LoadToHeatingSetPoint \textgreater{} 0 \& LoadToCoolingSetPoint \textgreater{} 0 --\textgreater{}~ Heating required
+
+! 2/~ LoadToHeatingSetPoint \textgreater{} 0 \& LoadToCoolingSetPoint \textless{} 0 --\textgreater{}~ Not Feasible
+
+! 3/~ LoadToHeatingSetPoint \textless{} 0 \& LoadToCoolingSetPoint \textless{} 0 --\textgreater{}~ Cooling Required
+
+! 4/~ LoadToHeatingSetPoint \textless{} 0 \& LoadToCoolingSetPoint \textgreater{} 0 --\textgreater{}~ Dead Band Operation
+
+~ IF (LoadToHeatingSetPoint \textgreater{} 0.0 .AND. LoadToCoolingSetPoint \textgreater{} 0.0) THEN
+
+~~~ ZoneSysEnergyDemand(ZoneNum)\%TotalOutputRequired = LoadToHeatingSetPoint
+
+~~~ ZoneSetPoint = ZoneThermostatSetPointLo(ZoneNum)
+
+~ ELSEIF (LoadToHeatingSetPoint \textless{} 0.0 .AND. LoadToCoolingSetPoint \textless{} 0.0) THEN
+
+~~~ ZoneSysEnergyDemand(ZoneNum)\%TotalOutputRequired = LoadToCoolingSetPoint
+
+~~~ ZoneSetPoint = ZoneThermostatSetPointHi(ZoneNum)
+
+~ ELSEIF (LoadToHeatingSetPoint \textless{} 0.0 .AND. LoadToCoolingSetPoint \textgreater{} 0.0) THEN
+
+~~~ ZoneSysEnergyDemand(ZoneNum)\%TotalOutputRequired = 0.0
+
+~~~ IF(Zone(ZoneNum)\%SystemZoneNodeNumber \textgreater{} 0) THEN
+
+~~~~~ ZoneSetPoint = Node(Zone(ZoneNum)\%SystemZoneNodeNumber)\%Temp
+
+~~~ ENDIF
+
+~~~ DeadBandOrSetback(ZoneNum) = .TRUE.
+
+~ ENDIF
+
+For Dual Setpoint with DeadBand there would be a heating and cooling thermostat.~ For this case both a heating and cooling setpoint can be scheduled for any given time period.~ The setpoint can be scheduled and varied throughout the simulation for both heating and cooling.
+
+CASE (DualSetPointWithDeadBand)
+
+~ LoadToHeatingSetPoint = (TempDepZnLd(ZoneNum) *
+
+~~~~~~~~~~~~~~~~~~~~~~~~~ ~ZoneThermostatSetPointLo(ZoneNum) --
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ TempIndZnLd(ZoneNum))
+
+~ LoadToCoolingSetPoint = (TempDepZnLd(ZoneNum) *
+
+~~~~~~~~~~~~~~~~~~~~~~~~~ ~ZoneThermostatSetPointHi(ZoneNum) --
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ TempIndZnLd(ZoneNum))
+
+! Possible combinations:
+
+! 1/~ LoadToHeatingSetPoint \textgreater{} 0 \& LoadToCoolingSetPoint \textgreater{} 0 --\textgreater{}~ Heating required
+
+! 2/~ LoadToHeatingSetPoint \textgreater{} 0 \& LoadToCoolingSetPoint \textless{} 0 --\textgreater{}~ Not Feasible
+
+! 3/~ LoadToHeatingSetPoint \textless{} 0 \& LoadToCoolingSetPoint \textless{} 0 --\textgreater{}~ Cooling Required
+
+! 4/~ LoadToHeatingSetPoint \textless{} 0 \& LoadToCoolingSetPoint \textgreater{} 0 --\textgreater{}~ Dead Band Operation
+
+~ IF (LoadToHeatingSetPoint \textgreater{} 0.0 .AND. LoadToCoolingSetPoint \textgreater{} 0.0) THEN
+
+~~~ ZoneSysEnergyDemand(ZoneNum)\%TotalOutputRequired = LoadToHeatingSetPoint
+
+~~~ ZoneSetPoint = ZoneThermostatSetPointLo(ZoneNum)
+
+~ ELSEIF (LoadToHeatingSetPoint \textless{} 0.0 .AND. LoadToCoolingSetPoint \textless{} 0.0) THEN
+
+~~~ ZoneSysEnergyDemand(ZoneNum)\%TotalOutputRequired = LoadToCoolingSetPoint
+
+~~~ ZoneSetPoint = ZoneThermostatSetPointHi(ZoneNum)
+
+~ ELSEIF (LoadToHeatingSetPoint \textless{} 0.0 .AND. LoadToCoolingSetPoint \textgreater{} 0.0) THEN
+
+~~~ ZoneSysEnergyDemand(ZoneNum)\%TotalOutputRequired = 0.0
+
+~~~ IF(Zone(ZoneNum)\%SystemZoneNodeNumber \textgreater{} 0) THEN
+
+~~~~~ ZoneSetPoint = Node(Zone(ZoneNum)\%SystemZoneNodeNumber)\%Temp
+
+~~~ ENDIF
+
+~~~ DeadBandOrSetback(ZoneNum) = .TRUE.
+
+~ ENDIF
+
+\subsection{Operative Temperature Control}\label{operative-temperature-control}
+
+The input object ZoneControl:Thermostat:OperativeTemperature provides a model where the behavior of the zone thermostats described above can be modified to accommodate operative temperature control. The ZoneControl:Thermostat:OperativeTemperature input object is used to modify the behavior of any of the thermostatic control types described above.~ When this object is used, the zone can be controlled by a weighted mixture of radiant and air temperatures (rather than just zone air temperatures).
+
+In EnergyPlus, operative temperature, \({T_{OP}}\) , is defined as ,
+
+\begin{equation}
+{T_{OP}} = \gamma {T_{MRT}} + (1 - \gamma ){T_{drybulb}}
+\end{equation}
+
+where,
+
+\(\gamma\) ~ is the radiative fraction,
+
+\({T_{MRT}}\) ~is the mean radiant temperature for the thermal zone, and
+
+\({T_{drybulb}}\) is the mean zone air temperature.
+
+The radiative fraction \(\gamma\) ~is selected by the user and can be scheduled to vary during the simulation.~ A typical value is 0.5.~ The maximum value needs to be less than 0.9 and the minimum is 0.0.~ A value of 0.0 is the same as controlling on only zone air temperature. If air velocities are higher than 0.2 m/s, then lower values for radiative fraction might apply.~ Niu and Burnett (1998) cite International Standard ISO 77300 in recommending the values for this fraction listed in the following table.
+
+% table 86
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Operative Temperature - Radiative Fraction vs Air Velocity \label{table:operative-temperature-radiative-fraction-vs}} \tabularnewline
+\toprule 
+Air Velocity (m/s) & < 0.2 & 0.2 to 0.6 & 0.6 to 1.0 \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Operative Temperature - Radiative Fraction vs Air Velocity} \tabularnewline
+\toprule 
+Air Velocity (m/s) & < 0.2 & 0.2 to 0.6 & 0.6 to 1.0 \tabularnewline
+\midrule
+\endhead
+
+\(\gamma\) & 0.5 & 0.4 & 0.3 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The control is accomplished using the load to setpoint formulation that is fundamental to HVAC system control in EnergyPlus. Although real systems will not know the loads and operate on temperature-based control, EnergyPlus needs to be able to function at zone timesteps up to one hour and this is too long of a timeframe for true temperature-based zone control.~ Load-based control is an important method of determining the average HVAC system response to zone conditions over the time step.~ For operative temperature control, the same methods and routines are used for calculating loads to setpoints but the setpoints are shifted to emulate operative temperature control rather than air temperature control.
+
+The user-defined setpoint for \({T_{OP}}\) ~is an input in degrees Celsius. \({T_{MRT}}\) ~is continually modeled by the full zone heat balance method and includes all the interactions between thermal loads and HVAC systems.~ A new setpoint for the zone's \({T_{drybulb}}\) ~is obtained for each zone timestep by rearranging the definition of \({T_{OP}}\) ~to put \({T_{drybulb}}\) ~on the left hand side.
+
+\begin{equation}
+{T_{drybulb,setpo{\mathop{\rm int}} }} = \frac{{{T_{OP,setpo{\mathop{\rm int}} }} - \gamma {T_{MRT}}}}{{(1 - \gamma )}}
+\end{equation}
+
+This adjustment to the target zone air drybulb temperature is made every timestep for every zone immediately after the setpoints are obtained from the schedule.
+
+Reference: J. Niu and J. Burnett. 1998. Integrating Radiant/Operative Temperature Controls into Building Energy Simulations. ASHRAE Transactions Vol. 104. Part 2. page 210.~ ASHRAE.~ Atlanta, GA.
+
+\subsection{Temperature And Humidity Control}\label{temperature-and-humidity-control}
+
+The input object ZoneControl:Thermostat:TemperatureAndHumidity is used to modify the behavior of ZoneControl:Thermostat objects (control types ThermostatSetpoint:SingleCooling and ThermostatSetpoint:DualSetpoint only) based on zone air humidity conditions. Specifically, this TemperatureAndHumidity zone control resets the ZoneControl:Thermostat's cooling setpoint temperature downward when the zone air relative humidity exceeds the Dehumidifying Relative Humidity Setpoint defined in this object. The reduced cooling setpoint temperature typically results in longer cooling coil runtimes and additional dehumidification. While additional dehumidification (lower absolute humidity level in the zone air) may be achieved, the resulting dry-bulb temperature and absolute humidity of the zone air will determine if the zone air \textbf{relative humidity} is reduced.
+
+The rate at which the cooling setpoint temperature is reduced is dictated by the user-specified Overcool Control Ratio. The maximum reduction in cooling setpoint temperature is defined by the user-entered Overcool Range, although the Overcool Range may be reduced from the user-defined value when this TemperatureAndHumidity control is used in tandem with a dual setpoint thermostat (see discussion below). Note that occupants are sensitive to overcooling and can experience discomfort if the overcool range is too large.
+
+This control is accomplished using the load to setpoint formulation that is fundamental to HVAC system control in EnergyPlus. Although real systems will not know the loads and operate on temperature-based control, EnergyPlus needs to be able to function at zone timesteps up to one hour and this is too long of a timeframe for true temperature-based zone control. Load-based control is an important method of determining the average HVAC system response to zone conditions over the time step. For TemperatureAndHumidity control, the same methods and routines are used for calculating loads to setpoints but the cooling setpoint is shifted to emulate TemperatureAndHumidity control, as described above.
+
+The overcool range limits the extent of the zone air temperature reduction below the cooling setpoint. When a dual setpoint thermostat is being modified by this TemperatureAndHumidity control, the maximum overcool range must be less than or equal to the temperature difference between the dual setpoint thermostat's cooling and heating setpoints:
+
+\begin{equation}
+  \Delta {T_{OvercoolRange,MAX}} = MIN\left( {\Delta {T_{OvercoolRange}},\,\Delta {T_{Setpoints}}} \right)
+\end{equation}
+
+where,
+
+\(\Delta {T_{OvercoolRange,MAX}}\) = maximum overcool range for the zone air (°C)
+
+\(\Delta {T_{OvercoolRange}}\) = overcool range for the zone air (°C).~ User input.
+
+\(\Delta {T_{Setpoints}}\) = temperature difference between the cooling and heating setpoints (°C)
+
+If a single cooling setpoint thermostat is being modified by this control, the maximum overcool range is equal to the user-defined overcool range.
+
+The extent that the zone air relative humidity exceeds the user-entered dehumidifying relative humidity setpoint is given by:
+
+\begin{equation}
+\Delta \phi  = MAX\left( {0.0,{\phi_{ZoneLagged}} - {\phi_{CSP}}} \right)
+\end{equation}
+
+The actual cooling setpoint reduction (overcooling) is calculated for the condition when the zone air relative humidity exceeds the dehumidifying setpoint (i.e., \(\Delta \phi\) \textgreater{}0), as described below:
+
+\begin{equation}
+  \begin{array}{l}
+    IF\,\,(\Delta \phi \, > \,0)\,\,THEN \\
+    ,\,\,\,\,\Delta {T_{Overcool,Actual}} = MIN\left( {\Delta {T_{OvercoolRange,MAX}},\,{{\Delta \phi } \mathord{\left/ {\vphantom {{\Delta \phi } {\Delta {\phi_{adjust}}}}} \right. } {\Delta {\phi_{adjust}}}}} \right) \\
+    ELSE \\
+    ,\,\,\,\,\Delta {T_{Overcool,Actual}} = 0 \\
+    ENDIF
+  \end{array}
+\end{equation}
+
+The cooling setpoint temperature is then adjustedas follows:
+
+\({T_{CSP,adj}} = \left( {{T_{CSP}} - \Delta {T_{Overcool,Actual}}} \right)\) where,
+
+\({T_{CSP,adj}}\) = adjusted cooling setpoint temperature (°C)
+
+\({T_{CSP}}\) = zone air cooling setpoint temperature for the current time step (°C).~ User input.
+
+\(\Delta {\phi_{adjust}}\) = user-defined overcool control ratio (\%/K)
+
+\(\Delta \phi\) = difference between the zone air relative humidity and the user-defined dehumidifying setpoint (\%)
+
+\({\phi_{ZoneLagged}}\) ~ = zone air relative humidity calculated at the last system time step (\%)
+
+\({\varphi_{CSP}}\) = dehumidifying relative humidity setpoint at the current time step (\%).~ User input.
+
+This adjusted cooling setpoint temperature is made every timestep for every zone immediately after the original thermostat setpoint is obtained from the user-defined setpoint schedule.
+
+\subsection{Humidistat}\label{humidistat}
+
+The input object ZoneControl:Humidistat provides a way for the zone to be controlled to a single relative humidity setpoint schedule, or dual humidity schedules (humidifying and dehumidifying with deadband). The schedules consist of relative humidities, expressed as a percentage (0-100), to be used for the zone moisture prediction calculation. Only one control statement can be specified for each zone.~ Individual relative humidity values can be defined for every time step, thus giving the user a full range of flexibility. For a single setpoint humidistat, if the control relative humidity is below the calculated load and the equipment specified can humidify then that equipment will try and meet the requirement.~ The opposite is true if the calculated value is above the setpoint and the equipment can dehumidify. For a dual setpoint humidistat, if the zone relative humidity is below the \textbf{humidifying} relative humidity setpoint and the equipment specified can humidify then that equipment will try and meet the zone's humidification load. The opposite is true if the zone relative humidity is above the \textbf{dehumidifying} relative humidity setpoint and the equipment can dehumidify.
+
+If the ZoneControl:Humidistat is used by a furnace or unitary system then no other objects are required. The signal from the humidistat is used directly by that component. If the Zone Control:Humidistat is used to control a Humidifier or used in conjunction with the Controller:Simple object with control variable ``TemperatureAndHumidityRatio'', then either the ``SetpointManager:SingleZone:Humidity:Minimum'', ``SetpointManager:MultiZone:Humidity:Minimum'',~~ ``SetpointManager:SingleZone:Humidity:Maximum'' or ``SetpointManager:MultiZone:Humidity:Maximum'' objects are required to determine a setpoint for those components to meet for the single setpoint humidistat. For a dual setpoint humidistat, a minimum humidity setpoint manager object~ (``SetpointManager:SingleZone:Humidity:Minimum'' or ``SetpointManager:MultiZone:Humidity:Minimum'') and a maximum humidity setpoint manager object (``SetpointManager:SingleZone:Humidity:Maximum'' or ``SetpointManager:MultiZone:Humidity:Maximum'') are required to determine the setpoints for the corresponding humidification and dehumidification components. Note that the ``SetpointManager:Scheduled'' object can also be used to directly set humidity ratio setpoints on the exit node of the humidifier component.
+
+For the single setpoint humidistat case, the model takes into account all of the moisture gains and/or losses from sources except the HVAC system contribution, and then calculates a moisture removal or addition rate based on the provided setpoint value, like the temperature predictor. The algorithm uses a 3rd Order derivative to predict zone moisture addition or removal to smooth the changes using the zone air capacitance. Positive values of moisture load mean that this amount of moisture must be added to the zone to reach the setpoint. Negative values represent the amount of moisture that must be removed by the system.
+
+\begin{equation}
+{\rm{MoistLoadHumidSetPoint = massflow}}\cdot {\rm{HumidityRatio = kg air/sec}}\cdot {\rm{kg }}{{\rm{H}}_{\rm{2}}}{\rm{O/kg air = kg }}{{\rm{H}}_{\rm{2}}}{\rm{O/sec}}
+\end{equation}
+
+This routine also calculates the zone required humidity ratio, Wsetpoint, which is required and takes into account the zone multiplier. At this time the Wsp is not stored in a derived type to make it available for SetpointManagers. It was setup to be analogous to the temperature thermostat.
+
+For the dual setpoint humidistat case, the model takes into account all of the moisture gains and/or losses from sources except the HVAC system contribution, and then calculates moisture addition and removal rates based on the provided humidifying and dehumidifying setpoint values, like the temperature predictor. The algorithm uses a Third Order Backward Difference , Analytical Solution, or Euler Method in subroutine CalcPredictedHumidityRatio to predict zone moisture addition and removal to smooth the changes using the zone air capacitance. The program calculates the humidifying (addition) and dehumidifying (removal) moisture loads based on the specified humidifying and dehumidifying setpoints, respectively. The calculated humidifying moisture load is passed to subroutine CalcSingZoneMinHumSetPoint and CalcMultiZoneMinHumSetPoint in the SetpointManager module to calculate the requested supply air humidity ratio at the setpoint node (Ref. SetpointManager:SingleZone:Humidity:Minimum and SetpointManager:MultiZone:Humidity:Minimum objects). The calculated dehumidifying moisture load is passed to subroutine CalcSingZoneMaxHumSetPoint and CalcMultiZoneMaxHumSetPoint in the SetpointManager module to calculate the requested supply air humidity ratio at the setpoint node (Ref. SetpointManager:SingleZone:Humidity:Maximum and SetpointManager:MultiZone:Humidity:Maximum objects). At the same time, the dehumidifying load is also passed directly to a furnace or unitary system if it is defined for the simulation, and that system will operate to meet this load based on its configuration and control settings.
+
+\subsection{Thermal Comfort Zone Control}\label{thermal-comfort-zone-control}
+
+The input object ZoneControl:Thermostat:ThermalComfort provides a way for the zone to be controlled to a specified temperature based on a selected thermal comfort model.~ ZoneControl:Thermostat:ThermalComfort references a thermal comfort control type schedule and one or more thermal comfort control type objects which in turn reference one or more setpoint schedules.
+
+The thermal comfort control type schedule and the list of thermal comfort control type/name pairs are directly related.~ The schedule defines the type of thermal comfort control that is to be used during for each simulation time step.~ Valid Control Types are
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Control Type & Control Type Name/Object \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Control Type & Control Type Name/Object \tabularnewline
+\midrule
+\endhead
+
+0 & No thermal comfort control \tabularnewline
+1 & ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating \tabularnewline
+2 & ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling \tabularnewline
+3 & ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling \tabularnewline
+4 & ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint \tabularnewline
+\bottomrule
+\end{longtable}
+
+If the schedule referenced in the ZoneControl statement has a value of 4 for a particular time step, this indicates that during that time step ``ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint'' control is to be used.~ The specific ``ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint'' control object to be used is specified in the list of thermal comfort control type/name pairs.~ Then the specific thermal comfort control type objects reference the thermal comfort PMV setpoint schedule to be used.~ Because only one thermal comfort control can be specified for each thermal comfort control type in a ZoneControl statement, there are only four pairs possible in a particular ZoneControl type/name list.~ This is because individual thermal comfort controls can be defined for specific times, thus giving the user a full range of flexibility.~ Since putting in the name of the thermal comfort control type directly in the schedule would be very cumbersome, the thermal comfort control types are assigned a number which is used in the schedule profile.
+
+For more information see ZoneControl:Thermostat:ThermalComfort in the InputOutput Reference and Zone Fanger Thermal Comfort in the Engineering Documentation.
+
+\subsubsection{Zone Control Based on Fanger Thermal Comfort}\label{zone-control-based-on-fanger-thermal-comfort}
+
+The syntax for the current set (4) of zone thermal comfort control types is given below. In each case, the keyword is accompanied by an identifying name and either one or two schedule names (depending on whether the control type is a single or dual setpoint control). The schedule defines a PMV setpoint for the control type. The schedule would be defined through the standard schedule syntax described earlier in this document. For an uncontrolled thermal comfort zone, no Fanger thermal comfort object is specified or necessary. See the Input Output Reference for more details.
+
+The control type schedule and the list of control type/name pairs are directly related.~ The schedule defines the type of control that is to be used during for each hour.~ Valid Control Types are
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Control Type & Control Type Name/Object \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Control Type & Control Type Name/Object \tabularnewline
+\midrule
+\endhead
+
+0 & No thermal comfort control \tabularnewline
+1 & ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating \tabularnewline
+2 & ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling \tabularnewline
+3 & ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling \tabularnewline
+4 & ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint \tabularnewline
+\bottomrule
+\end{longtable}
+
+For the no thermal comfort control (uncontrolled) case, the control will revert to thermostat control if specified. If the thermal comfort control is specified as ``uncontrolled'' for a particular period and thermostat control is not specified in the input, then conditions will float.
+
+For the ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating case there would be a heating only thermal comfort setpoint temperature.~ The setpoint is calculated based on the selected thermal comfort model and varied throughout the simulation but only heating is allowed with this thermal comfort control type.
+
+~~~~~ CASE (Single Thermal Comfort Heating Setpoint:Fanger)
+
+~~~~~ TempControlType(ZoneNum) = SingleHeatingSetpoint
+
+~~~~~ TempZoneThermostatSetPoint(ZoneNum) = Calculated Zone Setpoint from Fanger heating setpoint PMV
+
+For the ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling case there would be a cooling only thermal comfort setpoint temperature.~ The setpoint is calculated based on the selected thermal comfort model and varied throughout the simulation but only cooling is allowed with this thermal comfort control type.
+
+~~~~~ CASE (Single Thermal Comfort Cooling Setpoint:Fanger)
+
+~~~~~ TempControlType(ZoneNum) = SingleCoolingSetPoint
+
+~~~~~ TempZoneThermostatSetPoint(ZoneNum) = Calculated Zone Setpoint from Fanger cooling setpoint PMV
+
+For the ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling there would be heating and cooling thermal comfort zone control objects.~ The setpoint is calculated based on the selected thermal comfort model and varied throughout the simulation for both heating and cooling. With this thermal comfort control type only 1 setpoint profile is needed or used.
+
+~~~~~ CASE (Single Thermal Comfort Heating Cooling Setpoint:Fanger)
+
+~~~~~ TempControlType(ZoneNum) = SingleHeatCoolSetPoint
+
+~~~~~ TempZoneThermostatSetPoint(ZoneNum) = Calculated Zone Setpoint from Fanger heating and cooling
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ setpoint PMV
+
+For ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint there would be heating and cooling thermal comfort control objects.~ For this case both a heating and cooling setpoint can be calculated based on the selected thermal comfort model for any given time period.~ The thermal comfort setpoint temperature can be varied throughout the simulation for both heating and cooling.
+
+~~~~~ CASE (Dual Thermal Comfort Setpoint with Deadband:Fanger)
+
+~~~~~ TempControlType(ZoneNum) = DualSetPointWithDeadBand
+
+~~~~~ ZoneThermostatSetPointLo(ZoneNum) = Calculated Zone Setpoint from Fanger heating setpoint PMV
+
+~~~~~ ZoneThermostatSetPointHi(ZoneNum) = Calculated Zone Setpoint from Fanger cooling setpoint PMV
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/zone-equipment-and-zone-forced-air-units.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/zone-equipment-and-zone-forced-air-units.tex
new file mode 100644
index 00000000000..19af9e4d93b
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/zone-equipment-and-zone-forced-air-units.tex
@@ -0,0 +1,2337 @@
+\section{Zone Equipment and Zone Forced Air Units }\label{zone-equipment-and-zone-forced-air-units}
+
+\subsection{Air Distribution Terminal Unit}\label{air-distribution-terminal-unit}
+
+\subsubsection{Overview}\label{overview-031}
+
+The ZoneHVAC:AirDistributionUnit is a special piece of zone equipment -- it connects centrally conditioned air with a zone. It encompasses the various types of air terminal units in EnergyPlus: \emph{AirTerminal:DualDuct:ConstantVolume}, \emph{AirTerminal:SingleDuct:VAV:Reheat}, etc. It is a generalized component that accesses the calculations for the different types of air terminal unit.
+
+\subsubsection{Model}\label{model-003}
+
+The air distribution function is encapsulated in the module \emph{ZoneAirEquipmentManager}. The object and module function only to invoke the individual air terminal unit simulations.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-003}
+
+The data for this unit consists of the unit name, the air outlet node name (which should be the same as one of the zone inlet nodes), the type of air terminal unit (air distribution equipment), and the name of the air terminal unit.
+
+All input data for air distribution units is stored in the array \emph{AirDistUnit} in data module \emph{DataDefineEquip}.
+
+\subsubsection{Calculation}\label{calculation-001}
+
+There is no calculation associated with ZoneHVAC:AirDistributionUnit.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-004}
+
+\emph{SimZoneAirLoopEquipment} in module \emph{ZoneAirEquipmentManager} calls the individual air terminal unit simulations.
+
+\subsubsection{References}\label{references-056}
+
+No specific references.
+
+\subsection{Inlet Side Mixer Air Terminal Unit}\label{inlet-side-mixer-air-terminal-unit}
+
+\subsubsection{Overview}\label{overview-1-009}
+
+The input object AirTerminal:SingleDuct:InletSideSideMixer provides a means for using a zonal air conditioning unit as a terminal unit by mixing central system conditioned air with the inlet air stream of the zonal unit. Usually the central system would be a Direct Outside Air System (DOAS) providing centrally conditioned ventilation air to the zones.
+
+\subsubsection{Model}\label{model-1-000}
+
+The inlet side mixer uses the equations for adiabatic mixing of two moist air streams. Namely, dry air mass balance, water mass balance, and enthalpy balance.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-1-000}
+
+The only input data are the name and type of the zonal air conditioning unit plus the node names of the 2 input air nodes and the outlet air node. No flow rate data is needed.
+
+All input data for the inlet side mixer air terminal unit is stored in the data structure \emph{SysATMixer}.
+
+\subsubsection{Calculation}\label{calculation-1-000}
+
+The following equations for the mixing of two moist air streams are used:
+
+\begin{equation}
+{\dot m_{da1}}{h_1} + {\dot m_{da2}}{h_2} = {\dot m_{da3}}{h_3}
+\end{equation}
+
+\begin{equation}
+{\dot m_{da1}} + {\dot m_{da2}} = {\dot m_{da3}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{da1}}{W_1} + {\dot m_{da2}}{W_2} = {\dot m_{da3}}{W_3}
+\end{equation}
+
+where \({\dot m_{da}}\) is dry air mass flow rate in kg/s, \emph{h} is specific enthalpy in J/kg, and W is humidity ratio in (kg of water)/(kg of dry air).
+
+In this case, the outlet air mass flow rate has been set by the zonal unit. The air mass flow rate of one of the inlets - the primary air from the central system - is also known. So the air mass balance equation is used to obtain the secondary air mass flow rate.
+
+The inlet conditions - specific enthalpy and humidity ratio - for both inlet air streams are known. Now that both inlet air streams' mass flow rate is known, the enthalpy and water mass balance equations are used to get the outlet conditions.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-1-002}
+
+The inlet side mixer model is invoked from within the zonal AC model. Basically the inlet side mixer becomes a subcomponent of the zonal unit model. This allows the zonal unit to allow for the mixing of central supply air with its inlet stream in calculating how much cooling or heating it needs to do in order to meet the zone load.
+
+\subsubsection{References}\label{references-1-020}
+
+See Chapter 1, page 1.17 of the 2013 ASHRAE Handbook of Fundamentals
+
+\subsection{Supply Side Mixer Air Terminal Unit}\label{supply-side-mixer-air-terminal-unit}
+
+\subsubsection{Overview}\label{overview-2-007}
+
+The input object AirTerminal:SingleDuct:SupplySideSideMixer provides a means for using a zonal air conditioning unit as a terminal unit by mixing central system conditioned air with the outlet air stream of the zonal unit. Usually the central system would be a Direct Outside Air System (DOAS) providing centrally conditioned ventilation air to the zones.
+
+\subsubsection{Model}\label{model-2-000}
+
+The supply side mixer uses the equations for adiabatic mixing of two moist air streams. Namely, dry air mass balance, water mass balance, and enthalpy balance. In this case the inlet conditions and flow rates are known so the outlet condition and flow rate is calculated.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-2-000}
+
+The only input data are the name and type of the zonal air conditioning unit plus the node names of the 2 input air nodes and the outlet air node. No flow rate data is needed.
+
+All input data for the supply side mixer air terminal unit is stored in the data structure \emph{SysATMixer}.
+
+\subsubsection{Calculation}\label{calculation-2-000}
+
+Given the needed inputs, the output is calculated in subroutine \emph{CalcATMixer}. The input flow rates, humidity ratios, and enthalpies are taken from the inlet nodes' data. The balance equations are then used to calculate the outlet flow rate and conditions:
+
+\begin{equation}
+{\dot m_{da1}}{h_1} + {\dot m_{da2}}{h_2} = {\dot m_{da3}}{h_3}
+\end{equation}
+
+\begin{equation}
+{\dot m_{da1}} + {\dot m_{da2}} = {\dot m_{da3}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{da1}}{W_1} + {\dot m_{da2}}{W_2} = {\dot m_{da3}}{W_3}
+\end{equation}
+
+where \({\dot m_{da}}\) is dry air mass flow rate in kg/s, \emph{h} is specific enthalpy in J/kg, and W is humidity ratio in (kg of water)/(kg of dry air).
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-2-001}
+
+The supply side mixer model is invoked from within the zonal AC model. Basically the supply side mixer becomes a subcomponent of the zonal unit model. This allows the zonal unit to allow for the mixing of central supply air with its outlet stream in calculating how much cooling or heating it needs to do in order to meet the zone load.
+
+\subsubsection{References}\label{references-2-010}
+
+See Chapter 1, page 1.17 of the 2013 ASHRAE Handbook of Fundamentals
+
+\subsection{Simple Duct Leakage Model}\label{simple-duct-leakage-model}
+
+\subsubsection{Overview}\label{overview-3-005}
+
+The input object ZoneHVAC:AirDistributionUnit also provides access to a model for duct leakage that can be a significant source of energy inefficiency in forced-air HVAC systems. Evaluating duct leakage energy losses can involve considerable user effort and computer resources if an airflow network is defined through a detailed description of the system components and airflow paths (including leakage paths). A nonlinear pressure-based solver is used to solve for pressures and flow rates in the network. By making certain assumptions and approximations for certain well defined configurations, however, it is possible to obtain accurate results with a simple mass and energy balance calculation and thus avoid the input and calculation costs of doing a full pressure-based airflow network simulation.
+
+The Simple Duct Leakage Model (SDLM) assumes a central VAV air conditioning system with a constant static pressure setpoint. The model assumes that the leaks are in the supply ducts and that the system returns air through a ceiling plenum that contains the ducts. Thus, the ducts leak into the return plenum, and this part of the supply does not reach the conditioned zones. With the additional assumptions described below, it is possible to model this configuration with heat and mass balance equations and avoid the use of a nonlinear pressure-based solver. In the EnergyPlus context, this means that use of AirflowNetwork is avoided and the leakage calculations are obtained in the course of the normal thermal simulation.
+
+\subsubsection{Principles and Description}\label{principles-and-description}
+
+Constant Flow Rate
+
+The airflow rate through a duct leak is a function of the pressure difference between the duct and the surrounding space:
+
+\begin{equation}
+{\dot V_{leak}} = {C_1} \cdot \Delta p_{duct - space}^n
+\end{equation}
+
+The exponent \emph{n} is 0.5 for leaks that look like orifices (holes that are large relative to the thickness of the duct wall); for leaks that resemble cracks (e.g., lap joints), \emph{n} is approximately 0.6 to 0.65.
+
+For a duct with constant flow rate and a linear pressure drop through the duct, the average static pressure in the duct will equal half of the duct static pressure drop. Assuming turbulent flow in the duct, the duct pressure drop is proportional to the square of the airflow through the duct. This can be expressed as:
+
+\begin{equation}
+\Delta {p_{duct - space}} = \frac{{\Delta {p_{duct}}}}{2} = {C_2}\left( {\frac{{\dot V_{duct}^2}}{2}} \right)
+\end{equation}
+
+Combining equations and and assuming the leaks are large holes (\emph{n} equals 0.5). gives:
+
+\begin{equation}
+{\dot V_{leak}} = {C_1} \cdot \Delta p_{duct - space}^{0.5} = {C_3} \cdot {\dot V_{duct}}
+\end{equation}
+
+where
+
+\begin{equation}
+{C_3} = {C_1} \cdot {({C_2}/2)^{0.5}}
+\end{equation}
+
+Thus the leakage fraction \emph{C}\(_{3}\) remains constant regardless of the duct flow rate or static pressure. This result depends on the following assumptions:
+
+·~~~~~~~~the duct airflow is turbulent;
+
+·~~~~~~~~the duct pressure varies linearly along the duct;
+
+·~~~~~~~~the average duct pressure approximates the pressure drop across the duct;
+
+·~~~~~~~~the leaks are large and have pressure exponent 0.5.
+
+Effects of Constant Pressure Upstream and Variable Flow and Pressure Downstrean
+
+Commonly VAV systems maintain a constant static pressure at some point in the duct system upstream of the VAV terminal units. That is, airflow rate will vary depending on the cooling requirement, but a constant pressure will be maintained at the static pressure sensor. Consequently, the leakage flow for a leak upstream of the VAV boxes will be approximately constant. Or to put it another way, the leakage fraction will vary in proportion to the flow rate.
+
+For leaks downstream of the VAV terminal units, the airflow through the duct and the pressure in the downstream duct will vary as the box damper modulates in response to the differential between the room temperature and the thermostat setpoint. In this case, the situation is similar to the constant flow case: for an orifice-like leak, the pressure difference across the leak will vary linearly with the air speed (or flow rate); i.e., the leakage fraction will be approximately constant.
+
+SDLM
+
+For SDLM, our leakage model is then:
+
+·~~~~~~~~for leaks upstream of the terminal units, the leakage flow rate will be constant;
+
+·~~~~~~~~for leaks downstream of the terminal units, the leakage fraction will be constant.
+
+This model assumes, in addition to the assumptions given above, that the VAV system is controlled to a constant static pressure setpoint. In EnergyPlus SDLM is not currently applicable to systems using static pressure reset. Using SDLM would require knowledge of static pressure as a function of system air flow rate.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-3-000}
+
+User data for the SDLM is entered through The ZoneHVAC:AirDistributionUnit (ADU) object. There are 2 data items per ADU:
+
+1.~~~~the upstream nominal leakage fraction;
+
+2.~~~~the downstream fixed leakage fraction.
+
+Both inputs are leakage fractions. Input (1) is the leakage fraction at design flow rate, which together can be used to determine the constant leakage flow rate upstream of the VAV boxes; this leakage fraction varies with the flow rate. Input (2) is a fixed leakage fraction and is constant as the flow rate varies.
+
+\subsubsection{Implementation}\label{implementation-000}
+
+The various zone mass flow rates are related in the following manner.
+
+\begin{equation}
+{\dot m_{s,us}} = {\dot m_{tu}} + {\dot m_{lk,us}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{tu}} = {\dot m_{lk,ds}} + {\dot m_{s,z}}
+\end{equation}
+
+\begin{equation}
+{\dot m_{lk,us}} = Fra{c_{us}} \cdot {\dot m_{s,us,max}}
+\end{equation}
+
+\({\dot m_{lk,ds}} = Fra{c_{ds}} \cdot {\dot m_{tu}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \$\$
+
+Here
+
+\({\dot m_{s,us}}\) is the constant zone supply air mass flow rate upstream of the leaks {[}kg/s{]};
+
+\({\dot m_{tu}}\) is the air mass flow rate through the terminal unit {[}kg/s{]};
+
+\({\dot m_{lk,us}}\) is the upstream leakage air mass flow rate {[}kg/s{]};
+
+\({\dot m_{lk,ds}}\) is the downstream leakage air mass flow rate {[}kg/s{]};
+
+\({\dot m_{s,us,max}}\) is the maximum upstream supply air mass flow rate (program input) {[}kg/s{]};
+
+\({\dot m_{s,z}}\) is the supply air mass flow rate delivered to the zone {[}kg/s{]};
+
+\(Fra{c_{us}}\) is the design upstream leakage fraction (program input);
+
+\(Fra{c_{ds}}\) is the constant downstream leakage fraction (program input);
+
+\({\dot m_{tu}}\) is calculated in the VAV terminal unit model in the usual manner: the mass flow rate is varied to meet the zone load. The limits on the mass flow rate variation are set by the \({\dot m_{MaxAvail}}\) ~and \({\dot m_{MinAvail}}\) values stored at the terminal unit's air inlet node. To account for upstream leakage the maximum air mass flow rate available is reset to:
+
+\begin{equation}
+{\dot m'_{MaxAvail}} = {\dot m_{MaxAvail}} - {\dot m_{lk,us}}
+\end{equation}
+
+Downstream leakage must also be accounted for because not all of \({\dot m_{tu}}\) will reach the zone. This is done by having \({\dot m_{tu}}\) meet an adjusted zone load:
+
+\begin{equation}
+{\dot Q_{z,adjusted}} = \frac{1}{{1 - Fra{c_{ds}}}}{\dot Q_z}
+\end{equation}
+
+Here \({\dot Q_z}\) {[}watts{]} is the actual zone load (met by \({\dot m_{s,z}}\) ) and \({\dot Q_{z,adjusted}}\) is the load used in the VAV terminal unit model to obtain \({\dot m_{tu}}\) .
+
+Once \({\dot m_{tu}}\) ~is known, all the other flow rates can be calculated. \({\dot m_{s,us}}\) is assigned to the air distribution unit's air inlet node and \({\dot m_{s,z}}\) is assigned to the unit's air outlet node. Thus, air mass flow is not conserved through the unit: the two air leakage flow rates disappear. These two vanished flow rates are stored in the air distribution unit data structure. When the downstream return air plenum mass and energy balances are calculated, the leakage flow rate data is accessed and added back in as inlets to the return air plenum. Thus, the overall air system preserves a mass balance.
+
+\subsubsection{References}\label{references-3-005}
+
+Wray, C.P. 2003. ``Duct Thermal Performance Models for Large Commercial Buildings'', Lawrence Berkeley National Laboratory Report to the California Energy Commission. LBNL-53410.
+
+Wray, C.P. and N.E. Matson. 2003. ``Duct Leakage Impacts on VAV System Performance in California Large Commercial Buildings'', Lawrence Berkeley National Laboratory Report to the California Energy Commission. LBNL-53605.
+
+Wray, C.P., R.C. Diamond, and M.H. Sherman. 2005. ``Rationale for Measuring Duct Leakage Flows in Large Commercial Buildings''. Proceedings -- 26th AIVC Conference, Brussels, Belgium, September. LBNL-58252.
+
+\subsection{Fan Coil Unit}\label{fan-coil-unit}
+
+\subsubsection{Overview}\label{overview-4-003}
+
+The input object ZoneHVAC:FourPipeFanCoil provides a model for a 4 pipe fan coil zonal hydronic unit that can supply heating and cooling to a zone. It contains a hot water or electric heating coil, a chilled water coil, and a fan. It can supply a fixed amount of outdoor air, but cannot operate in an economizer mode. The fan runs at constant speed -- control is achieved by throttling the hot or cold water flow. The fan coil configuration and control is rather limited. The fan position is always \emph{blow-through}, control is always by varying the water flow, never by holding the water flow constant and cycling the fan.
+
+\subsubsection{Model}\label{model-3-000}
+
+The 4 pipe fan coil unit is modeled as a compound component consisting of 4 sub-components: an outdoor air mixer, a fan, a cooling coil, and a heating coil. In terms of EnergyPlus objects these are:
+
+\begin{enumerate}
+  \item \emph{OutdoorAir:Mixer}
+  \item \emph{Fan:ConstantVolume}
+  \item \emph{Coil:Cooling:Water, Coil:Cooling:Water:DetailedGeometry,} or \\ \emph{CoilSystem:Cooling:Water:HeatExchangerAssisted}
+  \item \emph{Coil:Heating:Water or Coil:Heating:Electric}
+\end{enumerate}
+
+The unit is a forward model: its inputs are defined by the state of its inlets: namely its 2 air streams -- recirculated and outdoor air. The outputs of the model are the conditions of the outlet air stream: flow rate, temperature and humidity ratio. The unit data and simulation are encapsulated in the module \emph{FanCoilUnits.}
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-4}
+
+The user describes the 4 pipe fan coil unit by inputting the names of the outdoor air mixer, the fan, the heating coil, and the cooling coil. The heating and cooling coil types must also be specified.
+
+The unit is connected to the overall HVAC system by specifying node names for the unit air inlet (for recirculated air) node, air outlet node, outdoor air node, relief node, inlet hot water node, and inlet chilled water node. The individual components comprising the fan coil must also be input and connected together properly. Specifically the outdoor air mixer mixed air node must be the same as the fan inlet node; the fan outlet node must be the same as the cooling coil air inlet node; the cooling coil air outlet node must be the same as the heating coil air inlet node; and the heating coil air outlet node must be the same as the unit air outlet node; the outdoor air mixer inlet nodes must match the unit inlet nodes; and the outdoor air mixer relief node must match the unit relief node.
+
+The user needs to also specify (unless the unit is autosized) various maximum flow rates: the supply air flow rate, the outdoor air inlet flow rate, the maximum (and minimum) chilled water flow rate, and the maximum (and minimum) hot water flow rate. Heating and cooling convergence tolerances need to be specified or defaulted. And there is an on/off availability schedule for the unit.
+
+All the input data for the fan coil unit is stored in the array \emph{FanCoil}.
+
+\subsubsection{Calculation}\label{calculation-3-000}
+
+Given the needed inputs, the output is calculated in subroutine \emph{Calc4PipeFanCoil}. The temperature, humidity ratio and flow rate of the recirculated and outdoor air streams are taken from the inlet air nodes The inlet hot and chilled water flow rates have been set by local controllers -- temperatures are taken from the inlet water nodes. Then
+
+1.~~~~The outdoor air mixer is simulated (Call \emph{SimOAMixer});
+
+2.~~~~the fan is simulated (Call \emph{SimulateFanComponents});
+
+3.~~~~the cooling coil is simulated (Call \emph{SimulateWaterCoilComponents} or \emph{SimHXAssistedCoolingCoil});
+
+4.~~~~the heating coil is simulated (Call \emph{SimulateWaterCoilComponents or SimulateHeatingCoilComponents}).
+
+The load met (sensible cooling or heating) is calculated and passed back to the calling routine:
+
+\begin{equation}
+  \dot{Q}_{sens,out} = \dot{m}_{tot} \PB{\text{PsyHFnTdbW}\PB{T_{out},W_{in}} - \text{PsyHFnTdbW}\PB{T_{in},W_{in}}}
+\end{equation}
+
+where \emph{PsyHFnTdbW} is the EnergyPlus function for calculating the specific enthalpy of air given the drybulb temperature and the humidity ratio. The subscript \emph{in} indicates the conditions at the inlet recirculated air node.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-3-000}
+
+From the result of the zone simulation we have the current heating/cooling demand on the unit \({\dot Q_{z,req}}\) . The first step is to decide whether the unit is on for the current time step. If the load is less than 1 watt or the flow rate is less than .001 kg/s, the unit is off. If the availability schedule is off, the mass flow rate is set to zero, so the second condition holds. When the unit is off there will be no air flow through the unit and outlet conditions will be equal to inlet conditions.
+
+\({\dot Q_{z,req}}\) ~is not the demand on the heating or cooling coil. To obtain the actual coil load, we need to calculate the unit output with no heating or cooling by the coils (\({\dot Q_{unit,no{\rm{ }}hc}}\) ). We obtain this by calling \emph{Calc4PipeFanCoil} with the water flow rates set to zero. Then the coil loads are calculated:
+
+\begin{equation}
+{\dot Q_{hc}} = {\dot Q_{z,hsp}} - {\dot Q_{unit,no{\rm{ }}hc}}
+\end{equation}
+
+\begin{equation}
+{\dot Q_{cc}} = {\dot Q_{z,csp}} - {\dot Q_{unit,no{\rm{ }}hc}}
+\end{equation}
+
+where \({\dot Q_{hc}}\) is the heating coil load, \({\dot Q_{z,hsp}}\) is the current zone load to the heating setpoint, \({\dot Q_{cc}}\) is the cooling coil load, and \({\dot Q_{z,csp}}\) is the current zone load to the cooling setpoint.
+
+If the unit is on and \({\dot Q_{cc}}\) \textless{} 0 and the thermostat type is not ``single heating setpoint'', \emph{ControlCompOutput} is called with the control node set to the cold water inlet node. \emph{ControlCompOutput} is a general component control routine. In this case calls \emph{Calc4PipeFanCoil} repeatedly while varying the cold water flow rate and minimizing \(({\dot Q_{sens,out}} - {\dot Q_{z,csp}})/{\dot Q_{z,csp}}\) to within the cooling convergence tolerance. Similarly if the unit is on and \({\dot Q_{hc}}\) \textgreater{}0 and the thermostat type is not ``single cooling setpoint'', \emph{ControlCompOutput} is called with the control node set to the hot water inlet node (for hydronic heating coil only). \emph{ControlCompOutput} varies the hot water flow rate or the electric heating coil part-load ratio is varied to minimize \(({\dot Q_{sens,out}} - {\dot Q_{z,hsp}})/{\dot Q_{z,hsp}}\) ~to within the heating tolerance. \emph{ControlCompOutput} executes a slow but safe interval halving algorithm to do its minimization. Once control is achieved, the total cooling/heating output is calculated:
+
+~~~~ \({\dot Q_{tot,out}} = \dot m\cdot ({\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{out}},{W_{out}}) - {\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{in,}}{W_{in}})\)
+
+\paragraph{Multi-Speed Fan In FanCoil}\label{multi-speed-fan-in-fancoil}
+
+When modeling multi-speed fan in FanCoil unit, capacity is modulated using speed ratio or part load ratio. The supply air fan speed is varied while operating the coils at maximum water flow. When there is no system load to meet, the water control valve is fully closed. When the FanCoil fan is cycling between two consecutive fan speed levels a speed ratio is calculated, but when the FanCoil unit cycles between the minimum fan speed and off-position, then part load ratio is calculated. The fan may be off or run continuously at lowest speed to provide ventilation air depending the fan operating schedule specified. When the FanCoil is operating at the lowest fan speed (Speed = 1), the water flow rate is reported as the average for the time step by multiplying the maximum water flow by part load ratio. The speed ratio and part-load ratio are calculated such that the FanCoil unit satisfies the required system zone cooling or heating load.The set of equations used for the multi-speed fan capacity control methods in FanCoil unit are summarized next.
+
+\subparagraph{Cycling Between Speeds}\label{cycling-between-speeds}
+
+When the supply fan is cycling between consecutive speeds, then the speed ratio (SR) and the average mass flow rate are calculated as follows:
+
+\[{SR_{n}} = Abs({SystemLoad} - {FullLoadOutput_{n-1}}) / Abs({FullLoadOutput_{n}} - {FullLoadOutput_{n-1}})\] \[{\dot m} = {\dot m_{on, n}} {SR_{n}} + {\dot m_{on, n-1}} (1 - {SR_{n}})\] \[{\dot m{w}} = {\dot m_{w, max}}\]
+
+\subparagraph{Cycling OnOff at Lowest Speed}\label{cycling-onoff-at-lowest-speed}
+
+The average supply air flow rate calculation when the fan is running at the lowest fan speed level depends on the fan operating schedule and load. The fan coil unit part load ratio is given by:
+
+\begin{equation}
+{PLR} = Abs({SystemLoad} - {NoLoadOutput}) / Abs({FullLoadOutput_{1}} - {NoLoadOutput})
+\end{equation}
+
+Continuous Fan
+
+\begin{equation}
+  \dot{m} = \dot{m}_{on, 1} \text{PLR} + \dot{m}_{off} \PB{1 - \text{PLR}}
+\end{equation}
+
+Cycling Fan:
+
+\begin{equation}
+  \begin{array}{ll}
+    \dot{m}   &= \dot{m}_{on, 1}\text{PLR} \\
+    \dot{m}_w &= \dot{m}_{w, max} \text{PLR}
+  \end{array}
+\end{equation}
+
+where:
+
+$SR_n$ = speed ratio of the fan coil unit at speed n, (-)
+
+$PLR$ = part load ratio of the fan coil uni at speed 1, (-)
+
+$\dot{m}$ = average mass flow rate of supply air, (kg/s
+
+$\dot{m}_{on, n-1}$ = mass flow rate of supply air at fan speed level n-1, (kg/s)
+
+$\dot{m}_{on, n}$ = mass flow rate of supply air at fan speed level n, (kg/s)
+
+$\dot{m}_{off}$ = mass flow rate of supply air when the coils are off, (kg/s)
+
+$\dot{m}_{w}$ = average mass flow rate of chilled or hot water, (kg/s)
+
+$\dot{m}_{w, max}$ = maximum or full mass flow rate of chilled or hot water, (kg/s)
+
+SystemLoad = system load to be met by the fan coil unit, (W)
+
+$FullLoadOutput_{n-1}$ = fully load fan coil unit output at fan speed level n-1, (W)
+
+$FullLoadOutput_{n}$ = fully load fan coil unit output at fan speed level n, (W)
+
+\paragraph{ASHRAE 90.1}\label{ashrae-90.1}
+
+The ASHRAE90.1 control method uses a simple technique to adjust fan speed based on zone design sensible load. The specific section of the Standard is described as:
+
+\begin{lstlisting}
+Section 6.4.3.10 (“Single Zone Variable-Air-Volume Controls�) of ASHRAE Standard 90.1-2010.
+HVAC systems shall have variable airflow controls as follows:
+(a) Air-handling and fan-coil units with chilled-water cooling coils and supply fans with motors 
+    greater than or equal to 5 hp shall have their supply fans controlled by two-speed motors or
+    variable-speed drives. At cooling demands less than or equal to 50%, the supply fan controls
+    shall be able to reduce the airflow to no greater than the larger of the following:
+    • One-half of the full fan speed, or
+    • The volume of outdoor air required to meet the ventilation requirements of Standard 62.1.
+(b) Effective January 1, 2012, all air-conditioning equipment and air-handling units with direct
+    expansion cooling and a cooling capacity at AHRI conditions greater than or equal to 110,000
+    Btu/h that serve single zones shall have their supply fans controlled by two-speed motors or
+    variable-speed drives. At cooling demands less than or equal to 50%, the supply fan controls
+    shall be able to reduce the airflow to no greater than the larger of the following:
+    • Two-thirds of the full fan speed, or
+    • The volume of outdoor air required to meet the ventilation requirements of Standard 62.1.
+\end{lstlisting}
+
+This control method assumes that a simulation sizing run is performed to determine the zone design sensible cooling and heating load \({\dot Q_{z,design}}\) .
+
+For fan coil units, the limit used to determine if reduced zone loads are met with reduced fan speed is the fan coil's Low Speed Supply Air Flow Ratio input.
+
+\begin{equation}
+{\dot Q_{reduced}} = {\dot Q_{z,design}} * {Ratio_{fan,low{\rm{ }}speed}}
+\end{equation}
+
+If the zone load, \({\dot Q_{z,req}}\) , is less than \({Q_{reduced}}\) then the fan is maintained at the reduced speed while the water coils (or electric heating coil) are modulated to meet the zone load.
+
+If the zone load is greater than the design zone sensible load, \({\dot Q_{z,design}}\) , the fan will operate at the maximum supply air flow rate and the water or electric heating coils will modulate to meet the zone load.
+
+If the zone load is between these two extremes, the fan and coil will modulate to meet the zone load.
+
+An example of the ASHRAE 90.1 control method is provided in the following figure. In this figure, the X-axis represents the zone cooling (-) or heating (+) load.
+
+\includegraphics{media/SZVAV_Fan_Control_FanCoil.jpg} Single-Zone VAV Fan Control for Fan Coil Units
+
+\subsubsection{References}\label{references-4-003}
+
+No specific references.
+
+\subsection{Window Air Conditioner}\label{window-air-conditioner}
+
+\subsubsection{Overview}\label{overview-5-002}
+
+The input object ZoneHVAC:WindowAirConditioner provides a model for a window air conditioner unit that is a packaged unit that supplies cooling to a zone (it is part of zone equipment, not part of the air loop equipment). It contains a fan, a DX cooling coil, and an outdoor air inlet. The coil meets the cooling load by cycling on/off. The fan can operate continuously or cycle on/off in conjunction with the coil.
+
+\subsubsection{Model}\label{model-4}
+
+The window air conditioner is modeled as a compound component consisting of 3 sub-components: an outdoor air mixer, a fan, and a DX coil. In terms of EnergyPlus objects these are OutdoorAir:Mixer, Fan:ConstantVolume or Fan:OnOff, and Coil:Coolilng:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted. The unit is a forward model: its inputs are defined by the state of its inlets: namely its 2 air streams -- recirculated and outdoor air. The outputs of the model are the conditions of the outlet air stream: flow rate, temperature and humidity ratio. The model is also an averaged model: the performance of the unit is averaged over the time step. That is, the unit is assumed to cycle on/off during the time step and this on/off cycling is averaged over the simulation time step. The unit data and simulation are encapsulated in the module WindowAC.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-5}
+
+The user describes the window air conditioner by inputting the names of the outdoor air mixer, the fan, and the cooling coil. The user can also choose fan placement -- blow through or draw through; fan operation -- cycling or continuous; and cooling coil type -- normal DX or DX with heat exchanger assistance.
+
+The connectivity of the unit needs to be specified: a recirculated (inlet) air node (same as a zone exhaust node); an air outlet node (same as a zone inlet node); an outdoor air inlet node; and a relief air node. The individual components comprising the window air conditioner must of course also be input and connected together properly. For instance, for a blow through fan configuration the outdoor air mixer mixed air node must be the same as the fan inlet node; the fan outlet node must be the same as the coil inlet node; the coil outlet node must be the same as the unit outlet node; the outdoor air mixer inlet nodes must match the unit inlet nodes; and the outdoor air mixer relief node must match the unit relief node.
+
+The user also specifies the air conditioner flow rate delivered to the zone (when cycled on) and the outdoor air flow rate. The user also needs to specify an availability schedule for the unit (this is an on/off schedule).
+
+Note that there is no input specifying the unit's design cooling capacity. This is an input in the DX coil object and is not repeated here.
+
+All the input data for the window air conditioner is stored in the array \emph{WindAC}.
+
+\subsubsection{Calculation}\label{calculation-4}
+
+Given the needed inputs, the output is calculated in subroutine CalcCyclingWindowAC. The temperature, humidity ratio and flow rate of the recirculated and outdoor air streams are taken from the inlet air nodes. The part load ratio is specified by the calling routine. Then
+
+·~~~~~~~~The outdoor air mixer is simulated (Call SimOAMixer);
+
+·~~~~~~~~For blow-through fan position:
+
+·~~~~~~~~the fan is simulated (Call SimulateFanComponents);
+
+·~~~~~~~~the coil is simulated (Call SimDXCoil or SimHXAssistedCoolingCoil).
+
+For draw-through fan position, the simulation order of the fan and coil is reversed. Note that data is never explicitly passed between the sub-components. This is all handled automatically by the node connections and the data stored on the nodes.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-4-000}
+
+From the result of the zone simulation we have the heating/cooling demand on the unit \({\dot Q_{z,req}}\) . The first step is to decide whether the unit is on for the current time step. For a unit with a cycling fan, the entire unit is assumed to be off if there is no cooling load, the cooling load is very small (less than 1 watt), the unit is scheduled off, or the zone temperature is in the deadband. For a unit with a continuous flow the fan operates if the unit is scheduled on, whether or not there is a cooling demand. The coil however only operates if there is a cooling demand and the zone temperature is not in the deadband.
+
+If the unit is determined to be on, the next step is to find the unit part load fraction that will satisfy the cooling load. This is done in \emph{ControlCycWindACOutput}. In this routine \emph{CalcCyclingWindowAC} ~is first called with part load fraction equal to 0, then with part load fraction equal to 1. These calls establish the minimum and maximum cooling output possible by the unit given the current conditions. An initial estimate of the part load fraction is then made:
+
+\begin{equation}
+PLF = ({\dot Q_{z,req}} - {\dot Q_{out,min}})/|{\dot Q_{out,max}} - {\dot Q_{out,min}}|
+\end{equation}
+
+Since the unit's cooling output is a nonlinear function of the part load fraction, this \emph{PLF} will not give exactly the desired \({\dot Q_{z,req}}\) . To obtain the exact \emph{PLF} that will give \({\dot Q_{z,req}}\) , it is necessary to iteratively call \emph{CalcCyclingWindowAC}, varying \emph{PLF} until the desired cooling output is obtained, within the error tolerance specified by the user in the input.
+
+Once \emph{PLF} is determined, \emph{ControlCycWindACOutput} is exited. One last call to \emph{CalcCyclingWindowAC} is made to establish the final outlet conditions at the unit's air outlet node. Finally, the inlet and outlet node conditions are used to calculate the reporting variables: sensible and total cooling output.
+
+\begin{equation}
+{\dot Q_{sens,out}} = \dot m\cdot ({\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{out}},{W_{in}}) - {\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{in,}}{W_{in}}))
+\end{equation}
+
+\begin{equation}
+{\dot Q_{sens,out}} = \dot m\cdot ({\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{out}},{W_{out}}) - {\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{in,}}{W_{in}})
+\end{equation}
+
+where \emph{PsyHFnTdb} is the EnergyPlus function giving enthalpy as a function of temperature and humidity ratio.
+
+\subsubsection{References}\label{references-5-003}
+
+No specific references.
+
+\subsection{Packaged Terminal Air Conditioner}\label{packaged-terminal-air-conditioner}
+
+\subsubsection{Overview}\label{overview-6-001}
+
+The input object ZoneHVAC:PackagedTerminalAirConditioner provides a model for a packaged terminal air conditioner (PTAC) that is a compound object made up of other components. Each PTAC consists of an outdoor air mixer, direct expansion (DX) cooling coil, heating coil (gas, electric, hot water, or steam) and a supply air fan. While the figure below shows the PTAC with draw through fan placement, blow through fan placement can also be modeled by positioning the supply air fan between the outdoor air mixer and DX cooling coil. The packaged terminal air conditioner coordinates the operation of these components and is modeled as a type of zone equipment (Ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
+
+\begin{figure}[hbtp] % fig 319
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7172.png}
+\caption{Schematic of a Packaged Terminal Air Conditioner with Draw Through Fan Placement \protect \label{fig:schematic-of-a-packaged-terminal-air}}
+\end{figure}
+
+The PTAC conditions a single zone and is controlled by a thermostat located in that zone. The PTAC operates to meet the zone sensible cooling or sensible heating requirements as dictated by the thermostat schedule. The model calculates the required part-load ratio for the air conditioner's coils and the supply air fan to meet the cooling/heating requirements. The heating or cooling energy provided by the PTAC is delivered to the zone via the zone air inlet node.
+
+The PTAC is able to model supply air fan operation in two modes: cycling fan -- cycling coil (i.e., AUTO fan) and continuous fan -- cycling coil (i.e., fan ON). Supply air fan operation is coordinated with the use of a supply air fan operating mode schedule. Schedule values of 0 denote cycling fan operation (AUTO fan). Schedule values other than 0 denote continuous fan operation (fan ON). Fan:OnOff must be used to model AUTO fan (i.e.~if schedule values of 0 occur in the supply air fan operating mode schedule), while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON (i.e.~if schedule values of 0 do not occur in the supply air fan operating mode schedule). The supply air fan operating mode schedule specified for the PTAC overrides the operating mode specified in the DX cooling coil object.
+
+Output variables reported by the PTAC object include the supply air fan part-load ratio, the air conditioner's part-load ratio (cooling or heating), and the electric consumption of the PTAC. Additional output variables report the total zone heating rate and the total zone cooling rate provided by the air conditioner. The sensible and latent components of zone cooling are also available as output variables. Reporting of other variables of interest for the PTAC (DX coil cooling rate, coil heating rate, crankcase heater power, fan power, etc.) is done by the individual system components (fan, DX cooling coil and heating coil).
+
+\subsubsection{Model Description}\label{model-description-017}
+
+As described previously, the PTAC conditions a single zone and is controlled by a zone thermostat (ZoneControl:Thermostatic). Each simulation time step, EnergyPlus performs a zone air heat balance to determine if cooling or heating is required to meet the thermostat setpoints, excluding any impacts from PTAC operation. PTAC performance is then modeled with all heating/cooling coils off but the supply air fan operates as specified by the user. If the zone air heat balance plus the impact of PTAC operation with coils off results in no requirement for heating or cooling by the PTAC coils, or if the PTAC is scheduled off (via its availability schedule), then the PTAC coils do not operate and the air conditioner's part-load ratio output variable is set to 0. If the model determines that cooling or heating is required and the PTAC is scheduled to operate, the model calculates the average air flow rate through the unit and the part-load ratio of the cooling and heating coils in order to meet the thermostat setpoint temperature.
+
+The remainder of this section describes the calculations performed during the latter situation, when cooling or heating coil operation is required. For any HVAC simulation time step, the PTAC can only be cooling or heating, not both. Because the PTAC cycles its coil(s) on and off to meet the required load, the coil(s) operate for a portion of the time step and are off for the rest of the time step. If the user specifies continuous fan operation (i.e.~supply air fan operating mode schedule value is greater than 0), then the supply air fan continues to operate at a user-specified flow rate even during periods when the coils cycle off. If the user specifies AUTO fan operation (i.e.~supply air fan operating mode schedule value is equal to 0), then the supply air fan cycles on and off with the coils. The model accounts for these variations in air flow through the PTAC within a simulation time step when it determines the total cooling or heating energy delivered to the zone, the average supply air conditions and air flow rate, and the energy consumed by the air conditioner.
+
+\subsubsection{Cooling Operation}\label{cooling-operation-001}
+
+If EnergyPlus determines that the air conditioner must supply cooling to the zone in order to meet the zone air temperature setpoint, then the model first calculates the PTAC's sensible cooling rate to the zone under two conditions: when the unit runs at full-load (steady-state) conditions and when the DX cooling coil is OFF. If the supply air fan cycles on/off with the compressor, then the sensible cooling rate is zero when the cooling coil is OFF. However if the fan is configured to run continuously regardless of coil operation, then the sensible cooling rate will not be zero when the cooling coil is OFF. Calculating the sensible cooling rate involves modeling the supply air fan (and associated fan heat), the outdoor air mixer, and the DX cooling coil. The heating coil is also modeled, but only to pass the air properties and mass flow rate from it's inlet node to it's outlet node. For each of these cases (full load and DX cooling coil OFF), the sensible cooling rate delivered to the zone by the PTAC is calculated as follows:
+
+\begin{equation}
+  \dot{Q}_{cooling,\,max} = \left( \dot{m}_{SA,full\,load} \right) \left( h_{out,\,full\,load} - h_{zone\,air} \right)_{HRmin}
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{cooling,\,min} = \left( \dot{m}_{SA,coil\,off} \right) \left( h_{out,\,coil\,off} - h_{zone\,air} \right)_{HRmin}
+\end{equation}
+
+where:
+
+\(\dot{Q}_{cooling,\,max}\) = maximum PTAC sensible cooling rate with cooling coil ON, W
+
+\(\dot{m}_{SA,full\,load}\) = supply air mass flow rate at full-load (steady-state) conditions, kg/s
+
+\emph{h\(_{out,\, full\, load}\)} = enthalpy of air exiting the PTAC at full-load conditions, J/kg
+
+\emph{h\(_{zone\, air}\)} = enthalpy of zone (exhaust) air, J/kg
+
+\emph{HR\(_{min}\)} = enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the PTAC exiting air or the zone (exhaust) air
+
+\(\dot{Q}_{cooling,\,min}\) = minimum PTAC sensible cooling rate with cooling coil OFF, W
+
+\(\dot{m}_{SA,coil\,\,off}\) = supply air mass flow rate with the cooling coil OFF, kg/s
+
+\emph{h\(_{out,\, coil\, off}\)} = enthalpy of air exiting the PTAC with the cooling coil OFF, J/kg
+
+With the calculated PTAC sensible cooling rates and the zone sensible cooling load to be met, the compressor part-load ratio for the PTAC is approximately equal to:
+
+\begin{equation}
+  PartLoadRatio = MAX \left( 0.0, \frac{ABS \left( \dot{Q}_{zone,cooling} - \dot{Q}_{cooling,\,min} \right)}{ABS \left( \dot{Q}_{cooling,\,max} - \dot{Q}_{cooling,\,min} \right)} \right)
+\end{equation}
+
+where:
+
+\(PartLoadRatio\) = compressor part-load ratio required to meet the zone load
+
+\(\dot{Q}_{zone,cooling}\) = required zone sensible cooling rate to meet setpoint, W
+
+Since the part-load performance of the DX cooling coil is frequently non-linear (Ref: DX Cooling Coil Model), and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the actual part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the individual PTAC component models) until the PTAC's cooling output (including on/off cycling effects) matches the zone cooling load requirement.
+
+If the PTAC has been specified with cycling fan/cycling coil (AUTO fan), then the user-defined supply air flow rate during cooling operation (volumetric flow rate converted to mass flow rate) is multiplied by the final PartLoadRatio value to determine the average supply air mass flow rate for the HVAC system simulation time step. For this case, the air conditions (temperature, humidity ratio and enthalpy) at nodes downstream of the cooling coil represent the full-load (steady-state) values when the coil is operating. If the supply air fan is specified to run continuously (fan ON), then the supply air mass flow rate is calculated as the average of the air mass flow rate when the compressor is on and the air mass flow rate when the compressor is off. In this case, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and mixed inlet air conditions when the coil is OFF). Additional discussion regarding the calculation of the average supply air flow and supply air conditions is provided later in this section.
+
+\subsubsection{Heating Operation}\label{heating-operation-001}
+
+Calculations of the PTAC's sensible heating rate delivered to the zone at full load and with the heating coil OFF are identical to the calculations described above for cooling operation.
+
+\begin{equation}
+  \dot{Q}_{heating,\,max} = \left( \dot{m}_{SA,full\,load} \right) \left( h_{out,\,full\,load} - {h_{zone\,air}} \right)_{HRmin}
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{heating,\,min} = \left( \dot{m}_{SA,coil\,off} \right) \left( h_{out,\,coil\,off} - h_{zone\,air} \right)_{HRmin}
+\end{equation}
+
+where:
+
+\(\dot{Q}_{heating,\,max}\) = maximum PTAC sensible heating rate with heating coil ON, W
+
+\(\dot{Q}_{heating,\,min}\) = minimum PTAC sensible heating rate with heating coil OFF, W
+
+With the calculated PTAC sensible heating rates and the zone sensible heating load to be met, the heating coil part-load ratio for the PTAC is approximately equal to:
+
+\begin{equation}
+  PartLoadRatio = MAX \left( 0.0, \frac{ABS \left( \dot{Q}_{zone,heating} - \dot{Q}_{heating,\,min} \right)}{ABS \left( \dot{Q}_{heating,\,max} - \dot{Q}_{heating,\,min} \right)} \right)
+\end{equation}
+
+where:
+
+\(PartLoadRatio\) = heating coil part-load ratio required to meet the zone load
+
+\(\dot{Q}_{zone,heating}\) = required zone sensible heating rate to meet setpoint, W
+
+Iterative calculations (successive modeling of the individual PTAC component models) are used to determine the final heating part-load ratio to account for the non-linear performance of the heating coil at part-load conditions and the variation in supply air fan heat for the case of cycling fan/cycling coil (AUTO fan). If heating coil operation at full load is unable to meet the entire zone heating load (e.g., the heating coil capacity is insufficient or the coil is scheduled OFF), the air conditioner's part-load ratio is set to 1 to meet the zone heating load to the extent possible.
+
+\subsubsection{Average Air Flow Calculations}\label{average-air-flow-calculations-000}
+
+The packaged terminal air conditioner operates based on user-specified (or autosized) air flow rates. The PTAC's supply air flow rate during cooling operation may be different than the supply air flow rate during heating operation. In addition, the supply air flow rate when no cooling or heating is required but the supply air fan remains ON can be different than the air flow rates when cooling or heating is required. The outdoor air flow rates can likewise be different in these various operating modes. The model takes these different flow rates into account when modeling the air conditioner, and the average air flow rate for each simulation time step is reported on the inlet/outlet air nodes of the various PTAC components in proportion to the calculated part-load ratio of the coil.
+
+The average supply air and outdoor air mass flow rates through the air conditioner for the HVAC simulation time step are calculated based on the part-load ratio of the DX cooling coil or heating coil (whichever coil is operating) as follows:
+
+\begin{equation}
+  \dot{m}_{SA,\,avg} = \dot{m}_{SA,coil\,on} \left( PartLoadRatio \right) + \dot{m}_{SA,\,coil\,off} \left( 1 - PartLoadRatio \right)
+\end{equation}
+
+\begin{equation}
+  \dot{m}_{OA,\,avg} = \dot{m}_{OA,\,coil\,on} \left( PartLoadRatio \right) + \dot{m}_{OA,\,coil\,off} \left( 1 - PartLoadRatio \right)
+\end{equation}
+
+where:
+
+\(\dot{m}_{SA,\,avg}\) = average supply air mass flow rate during the time step, kg/s
+
+\(\dot{m}_{SA,coil\,on}\) = supply air mass flow rate when the coil is ON, kg/s
+
+\emph{PartLoadRatio} = part-load ratio of the coil (heating or cooling)
+
+\(\dot{m}_{SA,\,coil\,off}\) = supply air mass flow rate when the coil is OFF, kg/s
+
+\(\dot{m}_{OA,\,avg\,}\) = average outdoor air mass flow rate during the time step, kg/s
+
+\(\dot{m}_{OA,\,coil\,on}\) = average outdoor air mass flow rate when the coil is ON, kg/s
+
+\(\dot{m}_{OA,\,coil\,off}\) = average outdoor air mass flow rate when the coil is OFF, kg/s
+
+The supply air and outdoor air flow rates when the DX cooling coil or the heating coil is ON are specified by the user (i.e., supply air volumetric flow rate during cooling operation, supply air volumetric flow rate during heating operation, outdoor air volumetric air flow rate during cooling operation, and outdoor air volumetric air flow rate during heating operation) and are converted from volumetric to mass flow rate. If the user has specified cycling fan operation (i.e.~supply air fan operating mode schedule value is equal to 0), then the supply air and outdoor air mass flow rates when the coil is OFF are zero. If the user has specified constant fan operation (i.e.~supply air fan operating mode schedule value is greater than 0), then the user-defined air flow rates when no cooling or heating is needed are used when the coil is OFF.
+
+There is one special case. If the supply air fan operating mode schedule value specifies constant fan operation and the user also specifies that the supply air volumetric flow rate when no cooling or heating is needed is zero (or field is left blank), then the model assumes that the supply air and outdoor air mass flow rates when the coil is OFF are equal to the corresponding air mass flow rates when the cooling or heating coil was last operating (ON).
+
+\subsubsection{Calculation of Outlet Air Conditions}\label{calculation-of-outlet-air-conditions}
+
+When the supply air fan cycles on and off with the PTAC coils (AUTO fan), the calculated outlet air conditions (temperature, humidity ratio, and enthalpy) from the heating coil or the DX cooling coil at full-load (steady-state) operation are reported on the appropriate coil outlet air node. The air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the part-load ratio of the coil (see Average Air Flow Calculations above).
+
+When the supply air fan operates continuously while the PTAC coils cycle on and off (fan ON), the air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the part-load ratio of the coil (see Average Air Flow Calculations above). Since the air flow rate can be different when the coil is ON compared to when the coil is OFF, then the average outlet air conditions from the heating coil or the DX cooling coil are reported on the appropriate coil outlet air node.
+
+For hot water or steam coils, the water or steam mass flow rate is also proportional to the part-load ratio of the coil regardless of the supply air fan operating mode. Refer to the sections in the document that describe the heating and DX cooling coils for further explanation on how they report their outlet air (and water or steam) conditions.
+
+\subsubsection{Calculation of Zone Heating and Cooling Rates}\label{calculation-of-zone-heating-and-cooling-rates}
+
+At the end of each HVAC simulation time step, this compound object reports the heating or cooling rate and energy delivered to the zone, as well as the electric power and consumption by the air conditioner. In terms of thermal energy delivered to the zone, the sensible, latent and total energy transfer rate to the zone is calculated as follows:
+
+\begin{equation}
+  \dot{Q}_{Total} = \left( \dot{m}_{SA,\,\,avg} \right) \left( h_{out,\,avg} - h_{zone\,air} \right)
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{Sensible} = \left( \dot{m}_{SA,\,avg} \right) \left( h_{out,\,avg} - h_{zone\,air} \right)_{HRmin}
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{Latent} = \dot{Q}_{Total} - \dot{Q}_{Sensible}
+\end{equation}
+
+where:
+
+\(\dot{Q}_{Total}\) = total energy transfer rate to the zone, W
+
+\(\dot{Q}_{Sensible}\) = sensible energy transfer rate to the zone, W
+
+\(\dot{Q}_{Latent}\) = latent energy transfer rate to the zone, W
+
+\(\dot{m}_{SA,\,avg}\) = average mass flow rate of the supply air stream, kg/s
+
+\emph{h\(_{out,avg}\)} = enthalpy of the air being supplied to the zone, J/kg
+
+Since each of these energy transfer rates can be calculated as positive or negative values, individual reporting variables are established for cooling and heating and only positive values are reported. The following calculations are representative of what is done for each of the energy transfer rates:
+
+IF (\(\dot{Q}_{Total} < 0.0\)) THEN
+
+~~~~~~~~~~~~~~~~~ \(\dot{Q}_{TotalCooling} = ABS(\dot{Q}_{Total})\)
+
+~~~~~~~~~~~~~~~~~ \(\dot{Q}_{TotalHeating} = 0.0\)
+
+ELSE
+
+~~~~~~~~~~~~~~~~~ \(\dot{Q}_{TotalCooling} = 0.0\)
+
+~~~~~~~~~~~~~~~~~ \(\dot{Q}_{TotalHeating} = \dot{Q}_{Total}\)
+
+where:
+
+\(\dot{Q}_{TotalCooling}\) = output variable `Packaged Terminal Air Conditioner Total Zone Cooling Rate, W'
+
+\(\dot{Q}_{TotalHeating}\) = output variable `Packaged Terminal Air Conditioner Total Zone Heating Rate, W'
+
+In addition to heating and cooling rates, the heating and cooling energy supplied to the zone is also calculated for the time step being reported. The following example for total zone cooling energy is representative of what is done for the sensible and latent energy as well as the heating counterparts.
+
+\begin{equation}
+  Q_{TotalCooling} = \dot{Q}_{TotalCooling} \cdot TimeStepSys \cdot 3600
+\end{equation}
+
+where:
+
+\(Q_{TotalCooling}\) = output variable `Packaged Terminal Air Conditioner Total Zone Cooling Energy, J'
+
+\emph{TimeStepSys} = HVAC system simulation time step, hr
+
+\subsection{Packaged Terminal Heat Pump}\label{packaged-terminal-heat-pump}
+
+\subsubsection{Overview}\label{overview-7-001}
+
+The input object ZoneHVAC:PackagedTerminalHeatPump provides a model for a packaged terminal heat pump (PTHP) that is a compound object made up of other components. Each PTHP consists of an outdoor air mixer, direct expansion (DX) cooling coil, DX heating coil, supply air fan, and a supplemental heating coil. While the figure below shows the PTHP with draw through fan placement, blow through fan placement can also be modeled by moving the supply air fan before the DX cooling coil. The packaged terminal heat pump coordinates the operation of these components and is modeled as a type of zone equipment (Ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
+
+\begin{figure}[hbtp] % fig 320
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7215.png}
+\caption{Schematic of a Packaged Terminal Heat Pump (Draw Through Fan Placement) \protect \label{fig:schematic-of-a-packaged-terminal-heat-pump}}
+\end{figure}
+
+The PTHP conditions a single zone and is controlled by a thermostat located in that zone. The PTHP operates to meet the zone sensible cooling or sensible heating requirements as dictated by the thermostat schedule. The model calculates the required part-load ratio for the heat pump's coils and the supply air fan to meet the cooling/heating requirements. The heating or cooling energy provided by the PTHP is delivered to the zone via the zone air inlet node.
+
+The PTHP is able to model supply air fan operation in two modes: cycling fan -- cycling coil (i.e., AUTO fan) and continuous fan -- cycling coil (i.e., fan ON). Fan:OnOff must be used to model AUTO fan, while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON.
+
+Output variables reported by the PTHP object include the supply air fan part-load ratio, the compressor part-load ratio, and the electric consumption of the PTHP. Additional output variables report the total zone heating rate and the total zone cooling rate provided by the heat pump. The sensible and latent components of zone cooling are also available as output variables. Reporting of other variables of interest for the PTHP (DX coil cooling rate, DX coil heating rate, crankcase heater power, fan power, etc.) is done by the individual system components (fan, DX cooling coil, DX heating coil, and supplemental heating coil).
+
+\subsubsection{Model Description}\label{model-description-1-008}
+
+As described previously, the PTHP conditions a single zone and is controlled by a zone thermostat (ZoneControl:Thermostat). Each simulation time step, EnergyPlus performs a zone air heat balance to determine if cooling or heating is required to meet the thermostat setpoints, excluding any impacts from PTHP operation. PTHP performance is then modeled with all heating/cooling coils off but the supply air fan operates as specified by the user. If the zone air heat balance plus the impact of PTHP operation with coils off results in no requirement for heating or cooling by the PTHP coils, or if the PTHP is scheduled off (via its availability schedule), then the PTHP coils do not operate and the compressor part-load ratio output variable is set to 0. If the model determines that cooling or heating is required and the PTHP is scheduled to operate, the model calculates the average air flow rate through the unit and the part-load ratio of the cooling and heating coils in order to meet the thermostat setpoint temperature.
+
+The remainder of this section describes the calculations performed during the latter situation, when cooling or heating coil operation is required. For any HVAC simulation time step, the PTHP can only be cooling or heating, not both. Because the PTHP cycles its coil(s) on and off to meet the required load, the coil(s) operate for a portion of the time step and are off for the rest of the time step. If the user specifies continuous fan operation (supply air fan operating mode schedule value \textgreater{} 0), then the supply air fan continues to operate at a user-specified flow rate even during periods when the coils cycle off. If the user specifies AUTO fan operation (supply air fan operating mode schedule value = 0), then the supply air fan cycles on and off with the coils. The model accounts for these variations in air flow through the PTHP within a simulation time step when it determines the total cooling or heating energy delivered to the zone, the average supply air conditions and air flow rate, and the energy consumed by the heat pump.
+
+\subsubsection{Cooling Operation}\label{cooling-operation-1-000}
+
+If EnergyPlus determines that the heat pump must supply cooling to the zone in order to meet the zone air temperature setpoint, then the model first calculates the PTHP's sensible cooling rate to the zone under two conditions: when the unit runs at full-load (steady-state) conditions and when the DX cooling coil is OFF. If the supply air fan cycles on/off with the compressor, then the sensible cooling rate is zero when the cooling coil is OFF. However if the fan is configured to run continuously regardless of coil operation, then the sensible cooling rate will not be zero when the cooling coil is OFF. Calculating the sensible cooling rate involves modeling the supply air fan (and associated fan heat), the outdoor air mixer, and the DX cooling coil. The DX heating coil and the gas or electric supplemental heating coil are also modeled, but only to pass the air properties and mass flow rate from their inlet nodes to their outlet nodes. For each of these cases (full load and DX cooling coil OFF), the sensible cooling rate delivered to the zone by the PTHP is calculated as follows:
+
+\begin{equation}
+  \dot{Q}_{cooling,\,max} = \left( \dot{m}_{SA,full\,load} \right) \left( h_{out,\,full\,load} - h_{zone\,air} \right)_{HRmin}
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{cooling,\,min} = \left( \dot{m}_{SA,coil\,off} \right) \left( h_{out,\,coil\,off} - h_{zone\,air} \right)_{HRmin}
+\end{equation}
+
+where:
+
+\(\dot{Q}_{cooling,\,max}\) = maximum PTHP sensible cooling rate with cooling coil ON, W
+
+\(\dot{Q}_{SA,full\,load}\) = supply air mass flow rate at full-load (steady-state) conditions, kg/s
+
+\emph{h\(_{out,\, full\, load}\)} = enthalpy of air exiting the PTHP at full-load conditions, J/kg
+
+\emph{h\(_{zone\, air}\)} = enthalpy of zone (exhaust) air, J/kg
+
+\emph{HR\(_{min}\)~~~~~~ ~ =} enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the PTHP exiting air or the zone (exhaust) air
+
+\(\dot{Q}_{cooling,\,min}\) = minimum PTHP sensible cooling rate with cooling coil OFF, W
+
+\(\dot{Q}_{SA,coil\,off}\) = supply air mass flow rate with the cooling coil OFF, kg/s
+
+\emph{h\(_{out,\, coil\, off}\)}~ ~ = enthalpy of air exiting the PTHP with the cooling coil OFF, J/kg
+
+With the calculated PTHP sensible cooling rates and the zone sensible cooling load to be met, the compressor part-load ratio for the PTHP is approximately equal to:
+
+\begin{equation}
+  PartLoadRatio = MAX \left( 0.0, \frac{ABS \left( \dot{Q}_{zone,cooling} - \dot{Q}_{cooling,\,min} \right)}{ABS \left( \dot{Q}_{cooling,\,max} - \dot{Q}_{cooling,\,min} \right)} \right)
+\end{equation}
+
+where:
+
+\(PartLoadRatio\) = compressor part-load ratio required to meet the zone load
+
+\(\dot{Q}_{zone,cooling}\) = required zone sensible cooling rate to meet setpoint, W
+
+Since the part-load performance of the DX cooling coil is frequently non-linear (Ref: DX Cooling Coil Model), and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the actual part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the individual PTHP component models) until the PTHP's cooling output (including on/off cycling effects) matches the zone cooling load requirement within the cooling convergence tolerance that is specified.
+
+If the PTHP is specified to operate with cycling fan/cycling coil (AUTO fan), then the user-defined supply air flow rate during cooling operation (volumetric flow rate converted to mass flow rate) is multiplied by the final PartLoadRatio value to determine the average supply air mass flow rate for the HVAC system simulation time step. For this case, the air conditions (temperature, humidity ratio and enthalpy) at nodes downstream of the cooling coil represent the full-load (steady-state) values when the coil is operating. If the supply air fan is specified to operate continuously (fan ON), then the supply air mass flow rate is calculated as the average of the air mass flow rate when the compressor is on and the air mass flow rate when the compressor is off. In this case, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and mixed inlet air conditions when the coil is OFF). Additional discussion regarding the calculation of the average supply air flow and supply air conditions is provided later in this section.
+
+\subsubsection{Heating Operation}\label{heating-operation-1-000}
+
+Calculations of the PTHP's sensible heating rate delivered to the zone at full load and with the DX heating coil OFF are identical to the calculations described above for cooling operation.
+
+\begin{equation}
+  \dot{Q}_{heating,\,max} = \left( \dot{m}_{SA,full\,load} \right) \left( h_{out,\,full\,load} - h_{zone\,air} \right)_{HRmin}
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{heating,\,min} = \left( \dot{m}_{SA,coil\,off} \right) \left( h_{out,\,coil\,off} - h_{zone\,air} \right)_{HRmin}
+\end{equation}
+
+where:
+
+\(\dot{Q}_{heating,\,max}\) = maximum PTHP sensible heating rate with DX heating coil ON, W
+
+\(\dot{Q}_{heating,\,min}\) = minimum PTHP sensible heating rate with DX heating coil OFF, W
+
+With the calculated PTHP sensible heating rates and the zone sensible heating load to be met, the compressor part-load ratio for the PTHP is approximately equal to:
+
+\begin{equation}
+  PartLoadRatio = MAX \left( 0.0, \frac{ABS \left( \dot{Q}_{zone,heating} - \dot{Q}_{heating,\,min} \right)}{ABS \left( \dot{Q}_{heating,\,max} - \dot{Q}_{heating,\,min} \right)} \right)
+\end{equation}
+
+where:
+
+\(PartLoadRatio\) = compressor part-load ratio required to meet the zone load
+
+\(\dot{Q}_{zone,heating}\) = required zone sensible heating rate to meet setpoint, W
+
+Iterative calculations (successive modeling of the individual PTHP component models) are used to determine the final heating part-load ratio to account for the non-linear performance of the DX heating coil at part-load conditions and the variation in supply air fan heat for the case of cycling fan/cycling coil (AUTO fan). If DX heating coil operating at full load is unable to meet the entire zone heating load (e.g., the DX heating coil capacity is insufficient or the coil is scheduled OFF, or the outdoor temperature is below the PTHP's minimum outdoor dry-bulb temperature for compressor operation), the supplemental heating coil is activated to meet the remaining zone heating load to the extent possible.
+
+\subsubsection{Average Air Flow Calculations}\label{average-air-flow-calculations-1}
+
+The packaged terminal heat pump operates based on user-specified (or autosized) air flow rates. The PTHP's supply air flow rate during cooling operation may be different than the supply air flow rate during heating operation. In addition, the supply air flow rate when no cooling or heating is required but the supply air fan remains ON can be different than the air flow rates when cooling or heating is required. The outdoor air flow rates can likewise be different in these various operating modes. The model takes these different flow rates into account when modeling the heat pump, and the average air flow rate for each simulation time step is reported on the inlet/outlet air nodes of the various PTHP components in proportion to the calculated part-load ratio of the DX coil compressor.
+
+The average supply air and outdoor air mass flow rates through the heat pump for the HVAC simulation time step are calculated based on the part-load ratio of the DX cooling coil or DX heating coil (whichever coil is operating) as follows:
+
+\begin{equation}
+\dot m{\,_{SA,\,\,avg}}\,\, = \,\,\dot m{\,_{SA,comp\,\,on}}\left( {PartLoadRatio} \right) + \dot m{\,_{SA,\,\,comp\,\,off}}\left( {1 - PartLoadRatio} \right)
+\end{equation}
+
+\begin{equation}
+\dot m{\,_{OA,\,\,avg\,\,}} = \,\,\dot m{\,_{OA,\,\,comp\,\,on}}\left( {PartLoadRatio} \right) + \dot m{\,_{OA,\,\,comp\,\,off}}\left( {1 - PartLoadRatio} \right)
+\end{equation}
+
+where:
+
+\(\dot m{\,_{SA,\,\,avg}}\) ~~~~~ = average supply air mass flow rate during the time step, kg/s
+
+\(\dot m{\,_{SA,comp\,\,on}}\) ~ = supply air mass flow rate when the DX coil compressor is ON, kg/s
+
+\emph{PartLoadRatio} = part-load ratio of the DX coil compressor (heating or cooling)
+
+\(\dot m{\,_{SA,\,\,comp\,\,off}}\) ~~~~~~~~~~~ = supply air mass flow rate when the DX coil compressor is OFF, kg/s
+
+\(\dot m{\,_{OA,\,\,avg\,\,}}\) ~~~ = average outdoor air mass flow rate during the time step, kg/s
+
+\(\dot m{\,_{OA,\,\,comp\,\,on}}\) = average outdoor air mass flow rate when the DX coil compressor is ON, kg/s
+
+\(\dot m{\,_{OA,\,\,comp\,\,off}}\) = average outdoor air mass flow rate when the DX coil compressor is OFF, kg/s
+
+The supply air and outdoor air flow rates when the DX cooling or DX heating coil compressor is ON are specified by the user (e.g., supply air volumetric flow rate during cooling operation, supply air volumetric flow rate during heating operation, outdoor air volumetric air flow rate during cooling operation, and outdoor air volumetric air flow rate during heating operation) and are converted from volumetric to mass flow rate. If the user has specified cycling fan operation (supply air fan operating mode schedule value = 0), then the supply air and outdoor air mass flow rates when the DX compressor is OFF are zero. If the user has specified constant fan operation (supply air fan operating mode schedule value \textgreater{} 0), then the user-defined air flow rates when no cooling or heating is needed are used when the DX compressor is OFF.
+
+There is one special case. If the user has specified constant fan operation (supply air fan operating mode schedule value \textgreater{} 0) and they specify that the supply air volumetric flow rate when no cooling or heating is needed is zero (or field is left blank), then the model assumes that the supply air and outdoor air mass flow rates when the DX coil compressor is OFF are equal to the corresponding air mass flow rates when the compressor was last operating (ON).
+
+\subsubsection{Calculation of Outlet Air Conditions}\label{calculation-of-outlet-air-conditions-1}
+
+When the supply air fan cycles on and off with the PTHP coils (AUTO fan), the calculated outlet air conditions (temperature, humidity ratio, and enthalpy) from the DX heating or DX cooling coil at full-load (steady-state) operation are reported on the appropriate coil outlet air node. The air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the part-load ratio of the DX coil compressor (see Average Air Flow Calculations above).
+
+When the supply air fan operates continuously while the PTHP coils cycle on and off (fan ON), the air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the part-load ratio of the DX coil compressor (see Average Air Flow Calculations above). Since the air flow rate can be different when the coil is ON compared to when the coil is OFF, then the average outlet air conditions from the DX heating or DX cooling coil are reported on the appropriate coil outlet air node.
+
+Refer to the sections in the document that describe the DX heating and DX cooling coils for further explanation on how they report their outlet air conditions.
+
+\subsubsection{Calculation of Zone Heating and Cooling Rates}\label{calculation-of-zone-heating-and-cooling-rates-1}
+
+At the end of each HVAC simulation time step, this compound object reports the heating or cooling rate and energy delivered to the zone, as well as the electric power and consumption by the heat pump. In terms of thermal energy delivered to the zone, the sensible, latent and total energy transfer rate to the zone is calculated as follows:
+
+\begin{equation}
+  \dot Q_{Total} = \left( {\dot m{\,_{SA,\,\,avg}}\,\,} \right)\left( {{h_{out,\,avg}} - {h_{zone\,\,air}}} \right)
+\end{equation}
+
+\begin{equation}
+  \dot Q_{Sensible} = \left( {\dot m{\,_{SA,\,\,avg}}\,\,} \right){\left( {{h_{out,\,avg}} - {h_{zone\,\,air}}} \right)_{HRmin}}
+\end{equation}
+
+\begin{equation}
+  \dot Q_{Latent} = \dot Q_{Total} - \dot Q_{Sensible}
+\end{equation}
+
+where:
+
+\(\dot{Q}_{Total}\) = total energy transfer rate to the zone, W
+
+\(\dot{Q}_{Sensible}\) = sensible energy transfer rate to the zone, W
+
+\(\dot{Q}_{Latent}\) = latent energy transfer rate to the zone, W
+
+\(\dot{m}_{SA,\,avg}\) = average mass flow rate of the supply air stream, kg/s
+
+\emph{h\(_{out,avg}\)} = enthalpy of the air being supplied to the zone, J/kg
+
+Since each of these energy transfer rates can be calculated as positive or negative values, individual reporting variables are established for cooling and heating and only positive values are reported. The following calculations are representative of what is done for each of the energy transfer rates:
+
+IF (\({\dot Q_{Total}}\) \emph{\textless{} 0.0 )}THEN
+
+~~~~~~~~~~~~~~~~~ \({\dot Q_{TotalCooling}}\) ~ = ~ ABS (\({\dot Q_{Total}}\) )
+
+~~~~~~~~~~~~~~~~~ \({\dot Q_{TotalHeating}}\) ~ = ~ \emph{0.0}
+
+ELSE
+
+~~~~~~~~~~~~~~~~~ \({\dot Q_{TotalCooling}}\) ~ = ~ \emph{0.0}
+
+~~~~~~~~~~~~~~~~~ \({\dot Q_{TotalHeating}}\) ~ = ~ \({\dot Q_{Total}}\)
+
+where:
+
+\(\dot{Q}_{TotalCooling}\) = output variable `Packaged Terminal Heat Pump Total Zone Cooling Rate, W'
+
+\(\dot{Q}_{TotalHeating}\) = output variable `Packaged Terminal Heat Pump Total Zone Heating Rate, W'
+
+In addition to heating and cooling rates, the heating and cooling energy supplied to the zone is also calculated for the time step being reported. The following example for total zone cooling energy is representative of what is done for the sensible and latent energy as well as the heating counterparts.
+
+\begin{equation}
+  Q_{TotalCooling} = \dot{Q}_{TotalCooling} * TimeStepSys * 3600.
+\end{equation}
+
+where:
+
+\(Q_{TotalCooling}\) = output variable `Packaged Terminal Heat Pump Total Zone Cooling Energy, J'
+
+\emph{TimeStepSys} = HVAC system simulation time step, hr
+
+\subsection{Zone Single Speed Water-To-Air Heat Pump}\label{zone-single-speed-water-to-air-heat-pump}
+
+\subsubsection{Overview}\label{overview-8-001}
+
+The input object ZoneHVAC:WaterToAirHeatPump provides a zone equipment model for a water-to-air heat pump that is a ``virtual'' component consisting of an on/off fan component, a water-to-air heat pump cooling coil, a water-to-air heat pump heating coil, and a gas or electric supplemental heating coil. The specific configuration of the blowthru heat pump is shown in the following figure. For a drawthru heat pump, the fan is located between the water-to-air heat pump heating coil and the supplemental heating coil. In addition, a water-to-air heat pump has a water loop connection on its source side. The water loop can be served by a condenser loop (like GHE for Ground source systems), or by a cooling tower/ boiler plant loop (for water loop systems).
+
+\begin{figure}[hbtp] % fig 321
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7258.png}
+\caption{Source Side and Load Side Configuration of a Zone WaterToAir Heat Pump \protect \label{fig:source-side-and-load-side-configuration-of-a-001}}
+\end{figure}
+
+There are two models for zone water-to-air heat pump cooling and heating coils, i.e.~Single-Speed and Variable-Speed Equation Fit models. Cooling and heating coils are modeled using the Equation Fit model described here.
+
+\subsubsection{Single Speed Equation-Fit Model:}\label{single-speed-equation-fit-model-000}
+
+This section describes the equation-fit model for Water-to-Air heat pump ~(Object names: Coil:Cooling:WaterToAirHeatPump:EquationFit and Coil:Heating:WaterToAirHeatPump:EquationFit). This documentation is derived from the M.S. dissertation of Tang (2005) which is available on the Oklahoma State University web site . The model uses five non-dimensional equations or curves to predict the heat pump performance in cooling and heating mode. The methodology involves using the generalized least square method to generate a set of performance coefficients from the catalog data at indicated reference conditions. Then the respective coefficients and indicated reference conditions are used in the model to simulate the heat pump performance. The variables or inlet conditions that influenced the water-to-air heat pump performance are load side inlet water temperature, source side inlet temperature, source side water flow rate and load side water flow rate. The governing equations for the cooling and heating mode are as following:
+
+Cooling Mode:
+
+\begin{equation}
+\frac{{{Q_{total}}}}{{{Q_{total,ref}}}} = A1 + A2\left[ {\frac{{{T_{wb}}}}{{{T_{ref}}}}} \right] + A3\left[ {\frac{{{T_{w,in}}}}{{{T_{ref}}}}} \right] + A4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + A5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]
+\end{equation}
+
+\begin{equation}
+\frac{{{Q_{sens}}}}{{{Q_{sens,ref}}}} = B1 + B2\left[ {\frac{{{T_{db}}}}{{{T_{ref}}}}} \right] + B3\left[ {\frac{{{T_{wb}}}}{{{T_{ref}}}}} \right] + B4\left[ {\frac{{{T_{w,in}}}}{{{T_{ref}}}}} \right] + B5\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + B6\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]
+\end{equation}
+
+\begin{equation}
+\frac{{Powe{r_c}}}{{Powe{r_{c,ref}}}} = C1 + C2\left[ {\frac{{{T_{wb}}}}{{{T_{ref}}}}} \right] + C3\left[ {\frac{{{T_{w,in}}}}{{{T_{ref}}}}} \right] + C4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + C5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]
+\end{equation}
+
+Heating Mode:
+
+\begin{equation}
+\frac{{{Q_h}}}{{{Q_{h,ref}}}} = E1 + E2\left[ {\frac{{{T_{db}}}}{{{T_{ref}}}}} \right] + E3\left[ {\frac{{{T_{w,in}}}}{{{T_{ref}}}}} \right] + E4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + E5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]
+\end{equation}
+
+\begin{equation}
+\frac{{Powe{r_h}}}{{Powe{r_{h,ref}}}} = F1 + F2\left[ {\frac{{{T_{db}}}}{{{T_{ref}}}}} \right] + F3\left[ {\frac{{{T_{w,in}}}}{{{T_{ref}}}}} \right] + F4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + F5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]
+\end{equation}
+
+Assuming no losses, the source side heat transfer rate for cooling and heating mode is calculated as following;
+
+\begin{equation}
+{Q_{source,c}} = {Q_{total}} + Powe{r_c}
+\end{equation}
+
+\begin{equation}
+{Q_{source,h}} = {Q_h} - Powe{r_h}
+\end{equation}
+
+where:
+
+\(A1 - F5\) ~ ~~ = Equation fit coefficients for the cooling and heating mode
+
+\({{T_{ref}}}\) ~~~~~~~~~~~ = 283K
+
+\({{T_{w,in}}}\) ~~~~~~~~~~ = Entering water temperature, K
+
+\({{T_{db}}}\) ~~~~~~~~~~~~ = Entering air dry-bulb temperature, K
+
+\({{T_{wb}}}\) ~~~~~~~~~~~ = Entering air wet-bulb temperature, K
+
+\({{{\dot V}_{air}}}\) ~~~~~~~~~~~ = Load side air volumetric flow rate, m\(^{3}\)/s
+
+\({{{\dot V}_{w}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~ = Source side water volumetric flow rate, m\(^{3}\)/s
+
+\({{Q_{total}}}\) ~~~~~~~~~ = Total cooling capacity, W
+
+\({{Q_{sens}}}\) ~~~~~~~~~ = Sensible cooling capacity, W
+
+\({Powe{r_c}}\) ~~~~ = Power consumption (cooling mode), W
+
+\({{Q_{source,c}}}\) ~~~~~ = Source side heat transfer rate (cooling mode), W
+
+\({{Q_{h}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~ = Total heating capacity, W
+
+\({Powe{r_h}}\) ~~~~ = Power consumption (heating mode), W
+
+\({{Q_{source,h}}}\) ~~~~~ = Source side heat transfer rate (heating mode), W
+
+The inlet conditions or variables are divided by the reference conditions. This formulation allows the coefficients to fall into smaller range of values. Moreover, the value of the coefficient indirectly represents the sensitivity of the output to that particular inlet variable. The reference conditions used when generating the performance coefficients must be the same as the reference conditions used later in the model. The reference temperature \({{T_{ref}}}\) is fixed at 283K. Temperature unit of Kelvin is used instead of Celsius to keep the ratio of the water inlet temperature and reference temperature positive should the water inlet temperature drop below the freezing point.
+
+For cooling mode, the reference conditions; reference load side air volumetric flow rate \(\left( {{{\dot V}_{air,ref}}} \right)\) ,reference source side water volumetric flow rate\(\left( {{{\dot V}_{w,ref}}} \right)\) ,reference sensible capacity \(\left( {{Q_{sens,ref}}} \right)\) ~and reference power input \(\left( {Powe{r_{c,ref}}} \right)\) ~are the conditions when the heat pump is operating at the highest cooling capacity or reference cooling capacity\(\left( {{Q_{total,ref}}} \right)\) ~indicated in the manufacturer's catalog. Note that the reference conditions for heating mode might differ from the reference conditions specified for the cooling mode.
+
+\subsubsection{Coefficient estimation procedure:}\label{coefficient-estimation-procedure-000}
+
+The generalized least square method is used to generate the coefficients. This method utilizes an optimization method which calculates the coefficients that will give the least amount of differences between the model outputs and the catalog data. A set of coefficients for the cooling mode is generated which includes A1-A5 for total cooling capacity, B1-B6 for sensible cooling capacity, and C1-C5 for power consumption. The same procedure is repeated for the heating mode to generate the coefficients E1-E5 (total heating capacity) and F1-F5 (power consumption). An information flow chart showing the inputs, reference conditions, performance coefficients and outputs are shown in the figure below:
+
+\begin{figure}[hbtp] % fig 322
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7286.png}
+\caption{Information Flow Chart for Water-to-Air Heat Pump Equation Fit Model (Tang 2005) \protect \label{fig:information-flow-chart-for-water-to-air-heat-001}}
+\end{figure}
+
+\subsection{Zone Air DX Dehumidifier}\label{zone-air-dx-dehumidifier}
+
+\subsubsection{Overview}\label{overview-9-000}
+
+This model, object name ZoneHVAC:Dehumidifier:DX, simulates the thermal performance and electric power consumption of conventional mechanical dehumidifiers. These systems use a direct expansion (DX) cooling coil to cool and dehumidify an airstream. Heat from the DX system's condenser section is rejected into the cooled/dehumidified airstream, resulting in warm dry air being supplied from the unit. In EnergyPlus, this object is modeled as a type of zone equipment (ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
+
+\begin{figure}[hbtp] % fig 323
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7287.png}
+\caption{Mechanical Dehumidifier Schematic \protect \label{fig:mechanical-dehumidifier-schematic}}
+\end{figure}
+
+The model assumes that this equipment dehumidifies and heats the air. If used in tandem with another system that cools and dehumidifies the zone air, then the zone dehumidifier should be specified as the lowest cooling priority in the ZoneHVAC:EquipmentList object for best control of zone temperature and humidity levels. With this zone equipment prioritization, the other cooling and dehumidification system would operate first to meet the temperature setpoint (and possibly meet the high humidity setpoint as well). If additional dehumidification is needed, then the zone dehumidifier would operate. The sensible heat generated by the dehumidifier is carried over to the zone air heat balance for the next HVAC time step.
+
+\subsubsection{Model Description}\label{model-description-2-007}
+
+The user must input water removal, energy factor and air flow rate at rated conditions (26.7°C, 60\% RH).~ Three performance curves must also be specified to characterize the change in water removal and energy consumption at part-load conditions:
+
+1)~~~~Water removal curve (function of inlet air temperature and relative humidity)
+
+2)~~~~Energy factor curve (function of inlet air temperature and relative humidity)
+
+3)~~~~Part load fraction correlation (function of part load ratio)
+
+·~~~~~~~~The water removal modifier curve is a biquadratic curve with two independent variables: dry-bulb temperature and relative humidity of the air entering the dehumidifier. The output of this curve is multiplied by the Rated Water Removal to give the water removal rate at the specific entering air conditions at which the dehumidifier is operating (i.e., at temperature/relative humidity different from the rating point conditions). If the output of this curve is negative, then a warning message is issued and it is reset to 0.0.
+
+\begin{equation}
+WaterRemovalModFac = \,a + \,b\left( {{T_{in}}} \right)\,\, + \,\,c{\left( {{T_{in}}} \right)^2}\,\, + \,\,d\left( {R{H_{in}}} \right) + e{(R{H_{in}})^2} + f({T_{in}})(R{H_{in}})
+\end{equation}
+
+where
+
+\emph{T\(_{in}\)}~ = dry-bulb temperature of the air entering the dehumidifier, °C
+
+\emph{RH\(_{in}\)} = relative of the air entering the dehumidifier, \% (0-100)
+
+·~~~~~~~~The energy factor modifier curve is a biquadratic curve with two independent variables: dry-bulb temperature and relative humidity of the air entering the dehumidifier. The output of this curve is multiplied by the Rated Energy Factor to give the energy factor at the specific entering air conditions at which the dehumidifier is operating (i.e., at temperature/relative humidity different from the rating point conditions). If the output of this curve is negative, then a warning message is issued and it is reset to 0.0.
+
+\begin{equation}
+EFModFac = \,a + \,b\left( {{T_{in}}} \right)\,\, + \,\,c{\left( {{T_{in}}} \right)^2}\,\, + \,\,d\left( {R{H_{in}}} \right) + e{(R{H_{in}})^2} + f({T_{in}})(R{H_{in}})
+\end{equation}
+
+·~~~~~~~~The part load fraction (PLF) correlation curve is a quadratic or a cubic curve with the independent variable being part load ratio (PLR = water removal load to be met / dehumidifier steady-state water removal rate). The part load ratio is divided by the output of this curve to determine the dehumidifier runtime fraction. The part load fraction correlation accounts for efficiency losses due to compressor cycling.
+
+\begin{equation}
+PartLoadFrac = PLF = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2}
+\end{equation}
+
+or
+
+\begin{equation}
+PartLoadFrac = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2} + d{\left( {PLR} \right)^3}
+\end{equation}
+
+where
+
+\begin{equation}
+PLR = \,part - load\,ratio\,\, = \left( {\frac{{water\,removal\,load\,to\,be\,met}}{{dehumidifier\,steady - state\,water\,removal\,rate}}} \right)
+\end{equation}
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the dehumidifier runs continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+0.7 \textless{} = PLF \textless{} = 1.0~~ and~~ PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the dehumidifier is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the dehumidifier is set to 1.0.
+
+Mechanical dehumidifier typically have long runtimes with minimal compressor cycling. So, a typical part load fraction correlation might be:
+
+~~~~~ PLF = 0.95 + 0.05(PLR)
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+~~~~~ PLF = 1.0 + 0.0(PLR)
+
+All three part-load curves are accessed through EnergyPlus' built-in performance curve equation manager (Curve:Quadratic, Curve:Cubic and Curve:Biquadratic). It is not imperative that the user utilize all coefficients shown in curve equations above if their performance equation has fewer terms (e.g., if the user's PartLoadFrac performance curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero).
+
+For any simulation time step when there is a water removal load to be met, the dehumidifier is available to operate (via availability schedule), and the inlet air dry-bulb temperature is within the minimum and maximum dry-bulb temperature limits specified in the input file for this object, the water removal rate for the dehumidifier is calculated as follows:
+
+\begin{equation}
+{\dot m_{_{water,ss}}} = \frac{{{\rho_{water}}\left( {{{\dot V}_{_{water,rated}}}} \right)\left( {WaterRemovalModFac} \right)}}{{\left( {24\,hr/dy} \right)\left( {3600sec/hr} \right)\left( {1000L/{m^3}} \right)}}
+\end{equation}
+
+where
+
+\({\dot m_{_{water,ss}}}\) ~ = ~ dehumidifier steady-state water removal rate, kg/s
+
+\({\rho_{water}}\) ~ = density of water, kg/m\(^{3}\)
+
+\({\dot V_{_{water,rated}}}\) ~ = rated water removal rate (user input), L/day
+
+The Zone Dehumidifier Part-Load Ratio (output variable) is then calculated, with the result constrained to be from 0.0 to 1.0:
+
+\begin{equation}
+PLR = \,\frac{{water\,removal\,load\,to\,be\,met}}{{{{\dot m}_{_{water,ss}}}}},\,\,\,0.0 \le PLR \le 1.0
+\end{equation}
+
+The steady-state and average electrical power consumed by the dehumidifier are calculated next using the following equations:
+
+\begin{equation}
+  P_{dehumid,ss} = \frac{\dot{V}_{water,rated}\PB{WaterRemovalModFac}\PB{1000}}{EF_{rated}\PB{EFModFac}\PB{24}}
+\end{equation}
+
+\begin{equation}
+  P_{dehumid,avg} = P_{dehumid,ss} \PB{RTF} + \PB{P_{off-cycle}\PB{1 - RTF}}
+\end{equation}
+
+where the 1000 and 24 are for conversion between kW and W, and days and hours, and:
+
+\({P_{dehumid,ss}}\) = dehumidifier steady-state electric power, W
+
+\({P_{dehumid,avg}}\) = Zone Dehumidifier Electric Power, W (output variable)
+
+\begin{equation}
+RTF = \frac{{PLR}}{{PLF}}\, = \,Zone Dehumidifier\,\,Runtime\,\,Fraction (output variable)
+\end{equation}
+
+\(E{F_{rated}}\) ~ = rated energy factor (user input), L/kWh
+
+\({P_{off - cycle}}\) ~ = off-cycle parasitic electric load (user input), W
+
+If the dehumidifier is unavailable to operate for the time period (via the specified availability schedule) then Zone Dehumidifier Electric Power is set equal to zero.
+
+The average water removal rate (kg/s) for the simulation time step is then calculated:
+
+\begin{equation}
+{\dot m_{water,\,avg}} = {\dot m_{water,\,ss}}\left( {PLR} \right) = {\rm{Zone Dehumidifier Removed Water Mass Flow Rate}},\;{\rm{kg/s}}\,\left( {{\rm{output}}\,{\rm{variable}}} \right)
+\end{equation}
+
+The Zone Dehumidifier Sensible Heating Rate (output variable) is calculated as follows:
+
+\begin{equation}
+{\dot Q_{_{sensible,avg}}} = {\dot m_{_{water,avg}}}\left( {{h_{fg}}} \right) + \,{P_{dehumid,avg}}
+\end{equation}
+
+where
+
+\emph{h\(_{fg}\)} = enthalpy of vaporization of air, J/kg
+
+The Zone Dehumidifier Sensible Heating Rate (W) is calculated during each HVAC simulation time step, and the results are averaged for the timestep being reported. However, this sensible heating is carried over to the zone air heat balance for the next HVAC time step (i.e., it is reported as an output variable for the current simulation time step but actually impacts the zone air heat balance on the following HVAC time step).
+
+The air mass flow rate through the dehumidifier is determined using the Rated Air Flow Rate (m\(^{3}\)/s) entered in the input, PLR, and converting to mass using the density of air at rated conditions (26.7C, 60\% RH) and local barometric pressure accounting for altitude
+
+p = 101325*(1-2.25577E-05*Z)**5.2559~ where p = pressure in Pa and Z = altitude in m:
+
+\begin{equation}
+{\dot m_{_{air,avg}}} = {\rho_{air}}\left( {{{\dot V}_{_{air,rated}}}} \right)\left( {PLR} \right)
+\end{equation}
+
+where
+
+\({\dot m_{_{air,avg}}}\) = average air mass flow rate through dehumidifier, kg/s
+
+\({\dot V_{_{air,rated}}}\) = rated air flow rate (user input), m\(^{3}\)/s
+
+\({\rho_{air}}\) ~ = density of air at 26.7°C , 60\% RH and local barometric pressure, kg/m\(^{3}\)
+
+The dry-bulb temperature and humidity ratio of the air leaving the dehumidifier are calculated as follows:
+
+\begin{equation}
+  T_{out} = T_{in} + \frac{P_{dehumid,ss} + \dot{m}_{water,ss} h_{fg}} {\rho_{air} \dot{V}_{air,rated} C_p}
+\end{equation}
+
+\begin{equation}
+  w_{out} = w_{in} - \frac{\dot{m}_{water,avg}}{\dot{m}_{air,avg}}
+\end{equation}
+
+where
+
+\emph{T\(_{out}\)} = ~~~ Zone Dehumidifier Outlet Air Temperature, C (output variable). Represents the
+
+outlet air temperature when the dehumidifier is operating.
+
+\emph{T\(_{in}\)} = inlet air dry-bulb temperature, C
+
+\({C_p}\) = heat capacity of air, J/kg
+
+\emph{w\(_{in}\)} = inlet air humidity ratio, kg/kg
+
+\emph{w\(_{out}\)} = outlet air humidity ratio, kg/kg
+
+If the dehumidifier does not operate for a given HVAC simulation time step, then the outlet air dry-bulb temperature and humidity ratio are set equal to the corresponding inlet air values.
+
+Since the sensible heating rate impacts the zone air heat balance on the following HVAC time step and is passed to the heat balance via an internal variable, the dry-bulb temperature of the dehumidifier's HVAC outlet air node (System Node Temperature) will always be set equal to the dehumidifier's HVAC inlet air node temperature. Therefore, when the dehumidifier operates the Zone Dehumidifier Outlet Air Temperature (output variable) will not be equal to the System Node Temperature for the dehumidifier's HVAC outlet node.
+
+Finally, the following additional output variables are calculated:
+
+\begin{equation}
+{Q_{_{sensible}}} = {\dot Q_{_{sensible,avg}}}*TimeStepSys*3600.
+\end{equation}
+
+\begin{equation}
+{E_{Dehumid}} = {P_{Dehumid,avg}}*TimeStepSys*3600.
+\end{equation}
+
+\begin{equation}
+{P_{off - cycle,avg}} = {P_{off - cycle}}\left( {1 - RTF} \right)
+\end{equation}
+
+\begin{equation}
+{E_{off - cycle}} = {P_{off - cycle,avg}}*TimeStepSys*3600.
+\end{equation}
+
+\begin{equation}
+{m_{_{water}}} = {\dot m_{_{water,avg}}}*TimeStepSys*3600.
+\end{equation}
+
+\begin{equation}
+\dot{V}_{water,avg} = \frac{\dot{m}_{water,avg}}{\rho_{water}}
+\end{equation}
+
+\begin{equation}
+{V_{_{water}}} = {\dot V_{_{water,avg}}}*TimeStepSys*3600.
+\end{equation}
+
+where
+
+\emph{Q\(_{sensible}\)} = output variable `Zone Dehumidifier Sensible Heating Energy {[}J{]}'
+
+\emph{E\(_{dehumid}\)} ~ = output variable `Zone Dehumidifier Electric Energy {[}J{]}'
+
+\emph{P\(_{off-cycle,avg}\)}~ = output variable `Zone Dehumidifier Off Cycle Parasitic Electric Power {[}W{]}'
+
+\emph{E\(_{off-cycle}\)} = output variable `Zone Dehumidifier Off Cycle Parasitic Electric Energy {[}J{]}'
+
+\emph{m\(_{water}\)} = output variable `Zone Dehumidifier Removed Water Mass {[}kg{]}'
+
+\({\dot V_{_{water,avg}}}\) = output variable `Zone Dehumidifier Condensate Volume Flow Rate {[}m\(^{3}\)/s{]}'
+
+\({V_{_{water}}}\) ~ = output variable `Zone Dehumidifier Condensate Volume {[}m\(^{3}\){]}'
+
+\subsection{Energy Recovery Ventilator}\label{energy-recovery-ventilator}
+
+The input object ZoneHVAC:EnergyRecoveryVentilator provides a model for a stand alone energy recovery ventilator (ERV) that is a single-zone HVAC component used for exhaust air heat recovery (see figure below). This compound object consists of three required components: a generic air-to-air heat exchanger (see object HeatExchanger:AirToAir:SensibleAndLatent), a supply air fan, and an exhaust air fan (see object Fan:OnOff). An optional controller (see object~ ZoneHVAC:EnergyRecoveryVentilator:Controller) may be used to simulate economizer (free cooling) operation.
+
+\begin{figure}[hbtp] % fig 324
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7321.png}
+\caption{Schematic of the Energy Recovery Ventilator:Stand Alone compound object \protect \label{fig:schematic-of-the-energy-recovery-ventilator}}
+\end{figure}
+
+This compound object models the basic operation of supply and exhaust air fans and an air-to-air heat exchanger. The stand alone ERV operates whenever the unit is scheduled to be available (Availability schedule). The stand alone ERV object can be used in conjunction with an economizer feature whereby heat exchange is suspended whenever free cooling is available (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped).
+
+To model a stand alone ERV connected to a single zone, the input data file should include the following objects:
+
+\begin{itemize}
+\item
+  ZoneHVAC:EnergyRecoveryVentilator
+\item
+  HeatExchanger:AirToAir:SensibleAndLatent
+\item
+  Fan:OnOff (supply air)
+\item
+  Fan:OnOff (exhaust air)
+\item
+  ZoneHVAC:EnergyRecoveryVentilator:Controller (if economizer {[}free cooling{]} operation is desired)
+\item
+  SetpointManager:Scheduled (if supply air outlet temperature control is used, Ref. HeatExchanger:AirToAir:SensibleAndLatent)
+\item
+  ZoneHVAC:EquipmentConnections
+\item
+  ZoneHVAC:EquipmentList
+\item
+  OutdoorAir:NodeList
+\end{itemize}
+
+\subsubsection{Model Description}\label{model-description-3-004}
+
+The purpose of this compound component is to simply call the individual component models and optional controller for each energy recovery ventilator. Since this equipment is not associated with an air loop, the compound object sets the supply and exhaust air mass flow rates through the ventilator. This compound object is also used to report the total, sensible and latent energy supplied to the zone, as well as the total electrical energy consumed by all of the individual components (supply air fan, exhaust air fan and heat exchanger parasitics).
+
+During each simulation time step, the air mass flow rate at the supply air and exhaust air inlets is set based on the stand alone ERV's availability schedule and the specified volumetric air flow rates as follows:
+
+IF (availability schedule value \textgreater{} 0) THEN
+
+\(\dot{m}_{Supply} = \rho \dot{V}_{Supply}\)
+
+\begin{equation}
+  \dot{m}_{Exhaust} = \rho \dot{V}_{Exhaust}
+\end{equation}
+
+ELSE
+
+\begin{equation}
+  \dot{m}_{Supply} = \dot{m}_{Exhaust} = 0.0
+\end{equation}
+
+\emph{where}:
+
+\(\dot{m}_{Supply}\) = mass flow rate of the supply air stream, kg/s
+
+\(\dot{m}_{Exhaust}\) = mass flow rate of the exhaust air stream, kg/s
+
+\(\rho\) = density of dry air at local barometric pressure (adjusted for altitude) and 20 ºC, kg/m\(^{3}\)
+
+\(\dot{V}_{Supply}\) = volumetric flow rate of the supply air stream, m\(^{3}\)/s
+
+\({\dot{V}_{Exhaust}}\) = volumetric flow rate of the exhaust air stream, m\(^{3}\)/s
+
+With the supply and exhaust inlet air mass flow rates set, the compound object then calls the generic air-to-air heat exchanger model to determine its supply air and exhaust air exiting conditions based on the inputs specified in the heat exchanger object. The supply air and exhaust air fans are then modeled to determine the final conditions of the air streams exiting the stand alone energy recovery ventilator. The heat exchanger and fan models are described in detail elsewhere in this document (reference: HeatExchanger:AirToAir:SensibleAndLatent and Fan:OnOff).
+
+The sensible heat transfer rate to the zone by the stand alone ventilator is then calculated as follows:
+
+\begin{equation}
+  \dot{Q}_{Sensible} = \dot{m}_{Supply} \left( h_{SupplyOutlet} - h_{ExhaustInlet} \right)_{HR\min }
+\end{equation}
+
+where:
+
+\(\dot{Q}_{Sensible}\) = sensible energy transfer rate to the zone, W
+
+\(\dot{m}_{Supply}\) = mass flow rate of the supply air stream, kg/s
+
+\emph{h\(_{SupplyOutlet}\)} = enthalpy of the air being supplied to the zone, J/kg
+
+\emph{h\(_{ExhaustInlet}\)} = enthalpy of the air being exhausted from the zone through the ventilator, J/kg
+
+\emph{HR\(_{min}\)} = enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the supply air outlet or the exhaust air inlet
+
+The resulting sensible energy transfer rate is passed to the zone equipment manager and added to the zone load to be met by other heating or cooling equipment. Since the stand alone ERV is intended to reduce the outdoor air load through heat exchange and not meet that load completely, the stand alone heat exchanger must be modeled first in the list of zone equipment. This is accomplished by setting the stand alone ERV priority for cooling and heating higher than that of other zone cooling or heating equipment (reference: ZoneHVAC:EquipmentList).
+
+When economizer (free cooling) operation is desired, a controller is coupled to the stand alone ERV by providing the name of the controller object in the ERV controller input field. This controller determines when the air-side economizer is active (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped) based on the controller inputs (Ref. ZoneHVAC:EnergyRecoveryVentilator:Controller).
+
+At the end of each HVAC simulation time step, this compound object reports the heating or cooling rate and energy delivered to the zone, as well as the electric power and consumption by the ventilator. In terms of thermal energy delivered to the zone, the sensible, latent and total energy transfer rate to the zone is calculated as follows:
+
+\begin{equation}
+  \dot{Q}_{Total} = \dot{m}_{Supply} \left( h_{SupplyOutlet} - h_{ExhaustInlet} \right)
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{Sensible} = \dot{m}_{Supply} \left( h_{SupplyOutlet} - h_{ExhaustInlet} \right)_{HR\min }
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{Latent} = \dot{Q}_{Total} - \dot{Q}_{Sensible}
+\end{equation}
+
+where:
+
+\(\dot{Q}_{Total}\) = total energy transfer rate to the zone, W
+
+\(\dot{Q}_{Sensible}\) = sensible energy transfer rate to the zone, W
+
+\(\dot{Q}_{Latent}\) = latent energy transfer rate to the zone, W
+
+\(\dot{m}_{Supply}\) = mass flow rate of the supply air stream, kg/s
+
+\emph{h\(_{SupplyOutlet}\)} = enthalpy of the air being supplied to the zone, J/kg
+
+\emph{h\(_{ExhaustInlet}\)}\(_{\\}\) = enthalpy of the air being exhausted from the zone through the ventilator, J/kg
+
+\emph{HR\(_{min}\)} = enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the supply air outlet or the exhaust air inlet
+
+Since each of these energy transfer rates can be calculated as positive or negative values, individual reporting variables are established for cooling and heating and only positive values are reported. The following calculations are representative of what is done for each of the energy transfer rates:
+
+IF (\({\dot Q_{Total}}\) \emph{~\textless{} 0.0 )}THEN
+
+~~~~~~~~~~~~~~~~~ \({\dot Q_{TotalCooling}}\) ~ = ~ ABS (\({\dot Q_{Total}}\) )
+
+~~~~~~~~~~~~~~~~~ \({\dot Q_{TotalHeating}}\) ~ = ~ \emph{0.0}
+
+ELSE
+
+~~~~~~~~~~~~~~~~~ \({\dot Q_{TotalCooling}}\) ~ = ~ \emph{0.0}
+
+~~~~~~~~~~~~~~~~~ \({\dot Q_{TotalHeating}}\) ~ = ~ \({\dot Q_{Total}}\)
+
+where:
+
+\(\dot{Q}_{TotalCooling}\) = output variable `Zone Ventilator Total Cooling Rate, W'
+
+\(\dot{Q}_{TotalHeating}\) = output variable `Zone Ventilator Total Heating Rate, W'
+
+In addition to heating and cooling rates, the heating and cooling energy supplied to the zone is also calculated for the time step being reported. The following example for total cooling energy is representative of what is done for the sensible and latent energy as well as the heating counterparts.
+
+\begin{equation}
+{Q_{TotalCooling}} = {\dot Q_{TotalCooling}}*TimeStepSys*3600.
+\end{equation}
+
+where:
+
+\(\dot{Q}_{TotalCooling}\) = output variable `Zone Ventilator Total Cooling Energy, J'
+
+\emph{TimeStepSys} = HVAC system simulation time step, hr
+
+\subsection{Zone Evaporative Cooler Unit}\label{zone-evaporative-cooler-unit}
+
+The input object ZoneHVAC:EvaporativeCoolerUnit provides a zone equipment model for evaporative cooling.~ This is a compound object that combines a fan and one or two evaporative coolers in a zone unit.~ The fan and evaporative cooler component models are described elsewhere. In this section we describe how the zone unit is controlled.
+
+\subsubsection{Controls}\label{controls-000}
+
+There are three choices for control methods.
+
+\textbf{ZoneTemperatureDeadbandOnOffCycling}. This control method operates the cooler unit in a manner similar to how a normal, real-world themostat operates.~ The control uses input for throttling temperature range, \(\Delta {T_{throttle}}\) , the most recent result for zone air node temperature, \({T_{zone}}\) , and the current cooling setpoint temperature, \({T_{set}}\) .~ The controller also stores the history of whether or not the unit was operating during the previous timestep to model hysteresis control where the unit retains its mode when it passes through the throttling range (to avoid short cycling).
+
+The following algorithm is used to determine if the unit will operate.
+
+If \(\left[ {{T_{zone}} < \left( {{T_{set}} - 0.5*\Delta {T_{throttle}}} \right)} \right]\) ~is true, then do not operate cooler unit.
+
+If \(\left[ {{T_{zone}} > \left( {{T_{set}} + 0.5*\Delta {T_{throttle}}} \right)} \right]\) ~is true, then operate the cooler unit (at full speed).
+
+If zone air temperature is within the throttling range, $\PB{T_{set}-0.5\Delta T_{throttle}} < T_{zone} < \PB{T_{set}+0.5\Delta T_{throttle}}$, then continue to operate the cooler if it was running during the previous timestep and do not operate the cooler if it was not running during the previous timestep.
+
+Whenever the unit is operating, it runs at the full design air mass flow rate regardless if the fan is constant or variable speed.
+
+\textbf{ZoneCoolingLoadOnOffCycling.} This control method operates the cooler similar to how a thermostat would behave, but instead of using temperatures it uses the predicted zone load to cooling setpoint.~ The control uses input for the threshold value for a load that is considered a significant, \({\dot Q_{thresh}}\) , and the result from the Predictor for the zone's load to cooling setpoint, \({\dot Q_{CoolLoad}}\) . The following algorithm is used to determine if the unit will operate.
+
+If \(\left[ {{{\dot Q}_{CoolLoad}} \le {{\dot Q}_{thresh}}} \right]\) ~is true, then do not operate cooler unit.
+
+If \(\left[ {{{\dot Q}_{CoolLoad}} > {{\dot Q}_{thresh}}} \right]\) ~is true, then operate the cooler unit (at full speed).
+
+Whenever the unit is operating, it runs at the full design air mass flow rate regardless if the fan is constant or variable speed.
+
+\textbf{ZoneCoolingLoadVariableSpeedFan.} This control method also operates the cooler using the predicted zone load to cooling setpoint but instead of on/off cycling, it modulates the fan speed to meet the cooling load.~ This control method is only applicable to cooler units with variable speed supply fans. The control uses input for the threshold value for a load that is considered a significant, \({\dot Q_{thresh}}\) , and the result from the Predictor for the zone's cooling load to setpoint, \({\dot Q_{CoolLoad}}\) . The following algorithm is used to determine if the unit will operate.
+
+If \(\left[ {{{\dot Q}_{CoolLoad}} \le {{\dot Q}_{thresh}}} \right]\) ~is true, then do not operate cooler unit.
+
+If \(\left[ {{{\dot Q}_{CoolLoad}} > {{\dot Q}_{thresh}}} \right]\) ~is true, then operate the cooler unit.
+
+When the unit operates, the model first operates the unit at the highest fan speed, a fan speed ratio of 1.0, and determines the sensible cooling provided by the unit to the zone, $\dot{Q}_{FullOutput}$ . If $\dot{Q}_{FullOutput} \leq \dot Q_{CoolLoad}$ then the unit operates at full fan speed because the cooler cannot meet the entire zone cooling load. If $\dot{Q}_{FullOutput} > \dot{Q}_{CoolLoad}$ then the model solves for a fan speed ratio between 0.0 and 1.0 that satisfies $\left|\PB{\dot{Q}_{Output}-\dot{Q}_{CoolLoad}}\right| < 0.01$ ~using the non-linear numerical method called regula falsi.
+
+\subsection{Unit Heater}\label{unit-heater}
+
+(Note: Some of this information also appears in the Input Output Reference for EnergyPlus.~ It is repeated here for clarity.)
+
+The input object ZoneHVAC:UnitHeater provides a model for unit heaters that are zone equipment units which are assembled from other components and are a simplification of unit ventilators.~ They contain only a fan and a heating coil. These components are described elsewhere in this document. The unit heater input simply requires the names of these components, which have to be described elsewhere in the input. The input also requires the name of an availability schedule, maximum airflow rate, and maximum and minimum hot water volumetric flow rates. The unit is connected to the zone inlet and exhaust nodes by specifying unit inlet and outlet node names. Note that the unit air inlet node should be the same as a zone exhaust node and the unit outlet node should be the same as a zone inlet node.
+
+\subsubsection{Controls}\label{controls-1-000}
+
+While the control of the heating coil is similar to the fan coil units and the unit ventilator, the overall control of the unit heater is much different.~ There are four different modes in which a unit heat can operate based on the user input:
+
+\textbf{OFF:} In this mode, the unit has been scheduled off.~ All flow rates are set to zero, and the temperatures are set to zone conditions.
+
+\textbf{NO LOAD OR COOLING/''NO''} for ``Supply Air Fan Operation During No Heating'' input field \textbf{:} In this mode, the unit is available, but there is no heating load.~ With ``No'' specified for ``Supply Air Fan Operation During No Heating'' and the supply fan operating mode schedule value of 0, the fan will only run when there is a heating load.~ Since there is no heating load in this mode and the fan is in cycling operating mode, all flow rates are set to zero, and the temperatures are set to zone conditions.~ Since the unit heater is designed only to provide heating, the presence of a cooling load signifies that the unit should not be running.
+
+\textbf{NO LOAD OR COOLING/''YES''} for ``Supply Air Fan Operation During No Heating'' input field\textbf{:} In this mode, the unit is available and the fan is controlled to be running continuously. For OnOff fan type the supply fan operating mode schedule value should be greater than 0.~ If it is scheduled to be available and the supply fan operating mode schedule value is greater than 0, then the fan runs and circulates air to the space.~ While no direct heating is provided, any heat added by the fan is introduced into the space with the circulation of the air.~ If the fan is scheduled off, the fan will not run (this is identical to ``NO'' control with no load).
+
+With ``Yes'' specified for ``Supply Air Fan Operation During No Heating'', and the supply fan operating mode schedule value is 0~ (for onOff fan type), then supply fan will not run.~ Since there is no heating load in this mode and the fan is in cycling mode, all flow rates are set to zero. This control mode allows to schedule the supply fan operation by specifying different operating modes during the day regardless of the heating load.
+
+\textbf{HEATING:} In this mode, the unit and fan are on/available, and there is a heating load.~ The heating coil is modulated (constant fan speed) to meet the heating load.~ When the fan is not cycling then the control of the heating coil and its flow rate is identical to the fan coil unit.~ The flow rate of air through the unit is controlled by the user input and schedules. In the case of OnOff fan the fan cycles with heating coil if the current timestep supply fan operating mode schedule value is 0, or the supply fan runs continuously for the entire timestep if the current timestep fan operating mode schedule value is greater than 0.~ When the fan is cycling the average supply air flow rate is proportional to the heating load at current time step, or else when the fan is scheduled to run continuously the fan supplies the maximum flow rate specified.
+
+\subsection{Unit Ventilator}\label{unit-ventilator}
+
+(Note: Some of this information also appears in the Input Output Reference for EnergyPlus.~ It is repeated here for clarity.)
+
+The input object ZoneHVAC:UnitVentilator provides a model for unit ventilators that are zone equipment units which are assembled from other components. They contain a built-in outdoor air mixer, a fan, a heating coil, and a cooling coil. These components are described elsewhere in this document, except the built-in outdoor air mixer which is contained within the unit ventilator statement. The unit ventilator input simply requires the names of these other three components, which have to be described elsewhere in the input. The input also requires the name of an availability schedule, maximum airflow rate, outdoor air control information (control type and schedules), an outdoor airflow rate, and maximum and minimum hot and cold water mass flow rates. The unit is connected to the zone inlet and exhaust nodes and the outdoor air by specifying unit inlet, outlet, outdoor air and exhaust (relief) air node names. Note that the unit air inlet node should be the same as a zone exhaust node and the unit outlet node should be the same as a zone inlet node. In general, the unit ventilator input is very similar to the fan coil unit input, and the unit is connected to a hot water loop (demand side) through its hot water coil and to a chilled water loop (demand side) through its cooling coil.
+
+\subsubsection{Controls and Outdoor Air}\label{controls-and-outdoor-air}
+
+The main difference between the fan coil and unit ventilator input is that the unit ventilator has a built-in outdoor air mixer with its own specialized controls. The outdoor air control type can be selected from one of the following options: ``variable percent'', ``fixed temperature'' or ``fixed amount''. In fixed temperature control, the amount of outdoor air is varied between the minimum outdoor air fraction (specified by a schedule) and 100\% outdoor air to obtain a mixed air temperature as close as possible to the temperature schedule defined in the input. Variable percent control will also vary the amount of outdoor air between the minimum and maximum fractions (both specified in input by the user) to meet the load without the use of a coil if possible. In fixed amount control, the outdoor air flow rate is fixed to the specified value by the user. In this control strategy, the maximum outdoor air flow rate and schedule are automatically set to be equal to the minimum outdoor air flow rate and schedule. These control types are based on the 2004 ASHRAE Systems and Equipment Handbook (pp.~31.1-31.3) description of unit ventilator systems.
+
+The unit is controlled to meet the zone (remaining) heating or cooling demand. If there is a heating demand, the cooling coil is off and the hot water flow through the heating coil is throttled to meet the demand. The hot water control node must be specified (same as the hot water coil inlet node) as well as maximum and minimum possible hot water volumetric flow rates. If there is a cooling demand from the zone, the hot water coil is off and the chilled water flow through the cooling coil is throttled to meet the load. The cooling coil control node must be specified (same as the cooling coil inlet node) and the maximum and minimum chilled water volumetric flow rates must be given. Finally both heating and cooling require a convergence tolerance, which is the tolerance denoting how closely the fan coil unit will meet the heating or cooling load. The tolerance is always relative to the zone load.
+
+Overall, control of the unit must consider the outdoor air for continuously running and cycling fans. For cycling fan operating mode, the outdoor air mass rate is capped by the actual supply air flow rate if the former is greater than the latter; otherwise, uses the amount calculated by the outdoor air control. Here is a more detailed description of the overall unit control:
+
+\textbf{OFF:} Unit is schedule off or there is no load on it. All flow rates are set to zero and the temperatures are set to zone conditions (except for the outdoor air inlet). Outdoor air requirements will not override this condition.
+
+\textbf{HEATING/NO COIL/VARIABLE PERCENT:} The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and variable percent outdoor air control type has been specified. In this case, the variable percent outdoor air controls what happens with the outdoor air. If the outside temperature is greater than the return temperature, then the outdoor air is set to the maximum as defined by the user input. If the outdoor air temperature is less than the return temperature from the zone, then the outdoor air is set to the minimum outdoor air flow rate as defined by the user. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
+
+\textbf{HEATING/NO COIL/FIXED TEMPERATURE:} The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate.
+
+\textbf{HEATING/NO COIL/FIXED AMOUNT:} The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
+
+\textbf{HEATING/WITH COIL/VARIABLE PERCENT:} The unit is on, there is a heating load, and variable percent control is specified. The outdoor air fraction is set to the minimum outdoor air fraction (schedule based), and the heating coil is activated. The heating coil attempts to meet the remaining load on the zone being served by the unit ventilator.
+
+\textbf{HEATING/WITH COIL/FIXED AMOUNT:} The unit is on, there is a heating load, a heating coil is present and is scheduled on, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. The heating coil then attempts to meet any remaining zone heating load.
+
+\textbf{COOLING/NO COIL/VARIABLE PERCENT:} The unit is on, there is a cooling load, no coil is present or it has been scheduled off, and variable percent outdoor air control type has been specified. In this case, the variable percent outdoor air controls what happens with the outdoor air. If the outside temperature is greater than the return temperature, then the outdoor air is set to the minimum as defined by the user input. If the outdoor air temperature is less than the return temperature from the zone, then the outdoor air is set to the maximum outdoor air flow rate as defined by the user. This may be somewhat simplistic in that it could result in overcooling of the space. However, since a temperature goal was not established, this is the best that can be done by the simulation. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
+
+\textbf{COOLING/NO COIL/FIXED TEMPERATURE:} The unit is on, there is a cooling load, no cooling coil is present or it has been scheduled off, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate in the same fashion as the variable percent outdoor air control.
+
+\textbf{COOLING/NO COIL/FIXED AMOUNT:} The unit is on, there is a cooling load, no cooling coil is present or it has been scheduled off, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
+
+\textbf{COOLING/WITH COIL/VARIABLE PERCENT:} The unit is on, there is a cooling load, a coil is present and is scheduled on, and variable percent outdoor air control type has been specified. In this case, the percentage of outdoor air is set to the minimum flow outdoor air flow rate. The coil then attempts to meet any remaining zone load.
+
+\textbf{COOLING/WITH COIL/FIXED TEMPERATURE:} The unit is on, there is a cooling load, a cooling coil is present and is scheduled on, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate in the same fashion as the fixed temperature outdoor air control for the ``no coil'' conditions. The cooling coil then attempts to meet any remaining zone load.
+
+\textbf{COOLING/WITH COIL/FIXED AMOUNT:} The unit is on, there is a cooling load, a cooling coil is present and is scheduled on, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. The cooling coil then attempts to meet any remaining zone cooling load.
+
+Note: the unit ventilator controls are strictly temperature based and do not factor humidity into the equation (not an enthalpy economy cycle but rather a simple return air economy cycle). In addition, temperature predictions are not strict energy balances here in the control routine though in the mixing routine an energy balance is preserved.
+
+\subsection{Variable Refrigerant Flow Terminal Unit}\label{variable-refrigerant-flow-terminal-unit}
+
+Variable refrigerant flow zone terminal units are used exclusively with variable refrigerant flow (VRF) air conditioning systems (ref: AirConditioner:VariableRefrigerantFlow and ZoneTerminalUnitList). The terminal units operate to satisfy a heating or cooling load in a zone based on a zone thermostat temperature set point. A direct-expansion (DX) cooling and/or DX heating coil is specified depending on the operating mode required. Outdoor ventilation air is modeled with the use of an outside air mixer object. Outside air may be provided to the zone only when the coil is operating or can be supplied continuously even when the coil is not operating. A supply air fan is also required and can be modeled as either draw through as shown in the figure below or as blow through where the fan inlet node would be connected to the outside air mixer mixed air node. If an outside air mixer is not used, the fan inlet node would be connected to the zone exhaust node.
+
+\begin{figure}[hbtp] % fig 325
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7369.png}
+\caption{Zone Terminal Unit Schematic \protect \label{fig:zone-terminal-unit-schematic}}
+\end{figure}
+
+\subsubsection{Overview}\label{overview-10-000}
+
+As described previously, the terminal units operate to satisfy a heating or cooling load in a zone based on a zone thermostat temperature set point (Zone Control:Thermostatic). Each simulation time step, EnergyPlus performs a zone air heat balance to determine if cooling or heating is required to meet the zone thermostat set points, excluding any impacts from zone terminal unit operation.
+
+Terminal unit performance is then modeled with all heating/cooling coils off but the supply air fan operates as specified by the user. If the zone air heat balance plus the impact of terminal unit operation with coils off results in no requirement for heating or cooling by the terminal unit coils, or if the terminal unit is scheduled off (via its availability schedule), then the terminal unit coils do not operate and the terminal unit's part-load ratio output variable is set to 0. If the model determines that cooling or heating is required and the terminal unit is scheduled to operate, the model calculates the part-load ratio of the cooling and heating coils in order to meet the thermostat set point temperature.
+
+The following sections describe the performance calculations for cooling-mode and heating-mode.
+
+\subsubsection{Model Description}\label{model-description-4-002}
+
+Zone terminal units meet a zone load as determined by a zone thermostat. The DX coils within a zone terminal unit will operate to meet a sensible zone load and all terminal units are controlled to either meet a zone sensible cooling load or a zone sensible heating load. This model does not provide for simultaneous cooling and heating.
+
+Given a zone load, the model calculates the part-load ratio of the terminal unit such that the terminal unit's ``net'' sensible capacity is equal to the zone load (if sufficient capacity is available). If it is determined that the part-load ratio of the zone terminal unit will be equal to 1, the DX cooling coil's capacity is calculated in the same manner as described for single-speed DX cooling coils (ref: Coil:Cooling:DX:SingleSpeed). When it is determined that the part-load ratio of the zone terminal unit will be less than 1, the DX cooling coil's capacity will be modulated through a reduction in refrigerant flow rate and an iterative solution technique will be used to calculate the performance of the DX cooling coil. For DX heating coils, capacity is calculated in the same manner as described for single-speed DX heating coils (ref: Coil:Heating:DX:SingleSpeed).
+
+The ``net'' sensible full load cooling capacity is then compared to the zone sensible load. If the ``net'' sensible full load capacity is less than or equal to the absolute value of the zone sensible load, the DX coil operates at the \emph{maximum} available capacity and, as a result, the zone air heat balance adjusts the zone air temperature. If the ``net'' sensible full load capacity is greater than the absolute value of the zone sensible load, an iterative solution technique is used to determine the total capacity required to meet the zone sensible load. This iteration loop entails successive modeling of DX coil performance and the loop iterates on the required total capacity until the operating ``net'' sensible capacity is equal to the zone sensible load.
+
+\subsubsection{Average Air Flow Calculations}\label{average-air-flow-calculations-2}
+
+The variable refrigerant flow (VRF) terminal unit operates based on user-specified (or autosized) air flow rates. The VRF terminal unit's supply air flow rate during cooling operation may be different than the supply air flow rate during heating operation. In addition, the supply air flow rate when no cooling or heating is required but the supply air fan remains ON can be different than the air flow rates when cooling or heating is required. The outside air flow rates can likewise be different in these various operating modes. The model takes these different flow rates into account when modeling the terminal unit, and the average air flow rate for each simulation time step is reported on the inlet/outlet air nodes of the various VRF terminal unit components in proportion to the calculated cycling ratio of the heat pump condenser. If the compressor does not cycle for a specific simulation time step then the heating or cooling air flow rate as specified by the user is assumed for the entire time step.
+
+The average supply air and outdoor air mass flow rates through the terminal unit for the HVAC simulation time step are calculated based on the cycling ratio of the heat pump condenser as follows:
+
+\begin{equation}
+  \dot{m}_{SA,\,avg} = \dot{m}_{SA,coil\,on} \left( CyclingRatio \right) + \dot{m}_{SA,\,coil\,off} \left( 1 - CyclingRatio \right)
+\end{equation}
+
+\begin{equation}
+  \dot{m}_{OA,\,avg} = \dot{m}_{OA,\,coil\,on} \left( CyclingRatio \right) + \dot{m}_{OA,\,coil\,off} \left( 1 - CyclingRatio \right)
+\end{equation}
+
+where:
+
+\(\dot{m}_{SA,\,avg}\) = average supply air mass flow rate during the time step, kg/s
+
+\(\dot{m}_{SA,coil\,on}\) = supply air mass flow rate when the coil is ON, kg/s
+
+\emph{CyclingRatio} = cycling ratio of the heat pump condenser (heating or cooling)
+
+\(\dot{m}_{SA,\,coil\,off}\) = supply air mass flow rate when the coil is OFF, kg/s
+
+\(\dot{m}_{OA,\,avg}\) = average outside air mass flow rate during the time step, kg/s
+
+\(\dot{m}_{OA,\,coil\,on}\) = average outside air mass flow rate when the coil is ON, kg/s
+
+\(\dot{m}_{OA,\,coil\,off}\) = average outside air mass flow rate when the coil is OFF, kg/s
+
+The supply air and outside air flow rates when the DX cooling coil or the DX heating coil is ON are specified by the user (i.e., supply air volumetric flow rate during cooling operation, supply air volumetric flow rate during heating operation, outside air volumetric air flow rate during cooling operation, and outside air volumetric air flow rate during heating operation) and are converted from volumetric to mass flow rate. If the user has specified cycling fan/cycling coil operation (i.e.~supply air fan operating mode schedule value is equal to 0), then the supply air and outside air mass flow rates when the coil is OFF are zero. If the user has specified constant fan/cycling coil operation (i.e.~supply air fan operating mode schedule value is greater than 0), then the user-defined air flow rates when no cooling or heating is needed are used when the coil is OFF.
+
+There is one special case. If the supply air fan operating mode schedule value specifies constant fan operation and the user also specifies that the supply air volumetric flow rate when no cooling or heating is needed is zero (or field is left blank), then the model assumes that the supply air and outside air mass flow rates when the coil is OFF are equal to the corresponding air mass flow rates when the cooling or heating coil was last operating (ON).
+
+\subsubsection{Calculation of Outlet Air Conditions}\label{calculation-of-outlet-air-conditions-2}
+
+When the supply air fan cycles on and off with the terminal unit coils (AUTO fan), the calculated outlet air conditions (temperature, humidity ratio, and enthalpy) from the DX heating coil or the DX cooling coil at full-load (steady-state) operation are reported on the appropriate coil outlet air node. The air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the cycling ratio of the coil (see Average Air Flow Calculations above).
+
+When the supply air fan operates continuously while the terminal unit coils cycle on and off (fan ON), the air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the cycling ratio of the coil (see Average Air Flow Calculations above). Since the air flow rate can be different when the coil is ON compared to when the coil is OFF, then the average outlet air conditions from the DX heating coil or the DX cooling coil are reported on the appropriate coil outlet air node.
+
+\subsubsection{Calculation of Zone Heating and Cooling Rates}\label{calculation-of-zone-heating-and-cooling-rates-2}
+
+At the end of each HVAC simulation time step, this compound object reports the heating or cooling rate and energy delivered to the zone. In terms of thermal energy delivered to the zone, the sensible, latent and total energy transfer rate to the zone is calculated as follows:
+
+\begin{equation}
+  \dot{Q}_{Total} = \left( \dot{m}_{SA,\,avg} \right) \left( h_{out,\,avg} - h_{zone\,air} \right)
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{Sensible} = \left( \dot{m}_{SA,\,avg} \right) \left( h_{out,\,avg} - h_{zone\,air} \right)_{HRmin}
+\end{equation}
+
+\begin{equation}
+  \dot{Q}_{Latent} = \dot{Q}_{Total} - \dot{Q}_{Sensible}
+\end{equation}
+
+where:
+
+\(\dot{Q}_{Total}\) = total energy transfer rate to the zone, W
+
+\(\dot{Q}_{Sensible}\) = sensible energy transfer rate to the zone, W
+
+\(\dot{Q}_{Latent}\) = latent energy transfer rate to the zone, W
+
+\(\dot{m}_{SA,\,\,avg}\) = average mass flow rate of the supply air stream, kg/s
+
+\emph{h\(_{out,avg}\)} = enthalpy of the air being supplied to the zone, J/kg
+
+The terminal unit's energy transfer rate is used by the program in the zone air heat balance to determine the final zone air conditions. If the terminal unit is capable of meeting the zone thermostat set point temperature, then these report variables are indicative of the zone loads and may be compared directly to the report variables for predicted zone loads (ref: Output:Variable, e.g., Zone Predicted Sensible Load to Setpoint Heat Transfer Rate).
+
+Since each of these energy transfer rates can be calculated as positive or negative values, individual reporting variables are established for cooling and heating and only positive values are reported. The following calculations are representative of what is done for each of the energy transfer rates:
+
+IF (\({\dot Q_{Total}}\) \emph{~\textless{} 0.0 )} THEN
+
+~~~~~ \({\dot Q_{TotalCooling}}\) ~ = ~ ABS (\({\dot Q_{Total}}\) )
+
+~~~~~ \({\dot Q_{TotalHeating}}\) ~ = ~ \emph{0.0}
+
+ELSE
+
+~~~~~ \({\dot Q_{TotalCooling}}\) ~ = ~ \emph{0.0}
+
+~~~~~ \({\dot Q_{TotalHeating}}\) ~ = ~ \({\dot Q_{Total}}\)
+
+ENDIF
+
+where:
+\(\dot{Q}_{TotalCooling}\) = output variable `Zone VRF Air Terminal Total Cooling Rate, W'
+
+\(\dot{Q}_{TotalHeating}\) = output variable `Zone VRF Air Terminal Total Heating Rate, W'
+
+In addition to heating and cooling rates, the heating and cooling energy supplied to the zone is also calculated for the time step being reported. The following example for total zone cooling energy is representative of what is done for the sensible and latent energy as well as the heating counterparts.
+
+\begin{equation}
+  Q_{TotalCooling} = \dot{Q}_{TotalCooling} * TimeStepSys * 3600.
+\end{equation}
+
+where: \(\dot{Q}_{TotalCooling}\) = output variable `Zone VRF Air Terminal Total Cooling Energy, J'
+
+\emph{TimeStepSys} = HVAC system simulation time step, hr
+
+\subsection{Ventilated Slab}\label{ventilated-slab}
+
+\subsubsection{Model Overview}\label{model-overview}
+
+The input object ZoneHVAC:VentilatedSlab provides a model for ventilated slab systems that in general use outdoor air to ``precool'' slabs with colder nighttime air. This method of precooling the thermal mass of a space can be very effective when nighttime temperatures are low and the mass of the system is high enough to provide a significant amount of cooling potential during the day to counteract internal heat gains within a zone. Nearly all ventilated slabs are simple systems such as that shown in the right side of Figure~\ref{fig:basic-system-for-the-ventilated-slab-module}. The fan is shown in a blow through position, but the model will allow either a blow or draw through configuration.
+
+\begin{figure}[hbtp] % fig 326
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7396.png}
+\caption{Basic System for the Ventilated Slab Module \protect \label{fig:basic-system-for-the-ventilated-slab-module}}
+\end{figure}
+
+It should be noted that in Figure~\ref{fig:basic-system-for-the-ventilated-slab-module} the use of ``unit ventilator'' and ``low temperature radiant system'' do not imply that the user must also specify these elements in the input file. The ventilated slab model combines aspects of these two existing EnergyPlus features into a single model that the user specifies through the input shown in the Input/Output Reference.
+
+The ventilated slab system has been implemented in a fashion that is similar to the ``unit ventilator'' system in EnergyPlus. The unit ventilator is a system that allows the user to bring in outdoor air (ventilation) that may or may not be tempered with a heating or cooling coil as shown the left side of Figure~\ref{fig:basic-system-for-the-ventilated-slab-module}. The air can be delivered to the slab only (Figure~\ref{fig:model-with-air-delivered-to-slab.-slab-only}), to the slab then to the space(Figure~\ref{fig:zone-supply-model-using-ventilated-slab-slab}), and to several slabs in different areas in series (Figure~\ref{fig:multiple-slabs-model-with-several-zones}). The model essentially combines the functionality of the low temperature radiant system (using air as a transport medium rather than water) and the unit ventilator. In some cases, the system may not meet all the zone heating and cooling load because it is operated not by setpoint of the zone but control temperature range and coil outlet air temperature set by user input.**Note that no coils are shown in Figure~\ref{fig:multiple-slabs-model-with-several-zones} for diagram simplicity but the implementation of the system shown in Figure~\ref{fig:multiple-slabs-model-with-several-zones} includes coils as in Figure~\ref{fig:model-with-air-delivered-to-slab.-slab-only} and Figure~\ref{fig:zone-supply-model-using-ventilated-slab-slab}.
+
+\begin{figure}[hbtp] % fig 327
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7397.png}
+\caption{Model with Air Delivered to Slab. (Slab Only Mode) \protect \label{fig:model-with-air-delivered-to-slab.-slab-only}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 328
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7398.png}
+\caption{Zone Supply Model using Ventilated Slab (Slab and Zone mode) \protect \label{fig:zone-supply-model-using-ventilated-slab-slab}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 329
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7399.png}
+\caption{Multiple Slabs model with Several Zones (Series Slabs Mode) \protect \label{fig:multiple-slabs-model-with-several-zones}}
+\end{figure}
+
+\subsubsection{Connections to the Heat Balances}\label{connections-to-the-heat-balances}
+
+The ventilated slab systems shown in the above diagrams connect or will connect to the various EnergyPlus heat balance equations in a variety of ways. All of the systems send outside or conditioned air through a slab or building element. This portion of the system acts in a fashion that is identical to the low temperature radiant systems. These surfaces that have the air being blown through them will impact the zone and air heat balances through the normal surface heat balances that interact with this surface. The ventilated slab will participate in the surface heat balances by exchanging radiation with other surfaces in the zone and in the air heat balances via convection to the zone air. So, the ventilated slab is handled identically to the low temperature radiant systems with respect to the zone and air heat balances. This information is valid for all three of the systems shown in the figures above.
+
+Figure~\ref{fig:zone-supply-model-using-ventilated-slab-slab} shows that the air, instead of being circulated through the slab and then sent back to the ventilation portion of the system, gets circulated through the space after it gets sent through the slab. When this system is selected in EnergyPlus, it will have an additional impact on the zone air heat balance because air will be introduced into the space at conditions different than the zone air. Thus, it will have an energy impact on the air directly through the circulation of air from the slab to the zone and then back to the ventilated slab system. It will still have an impact on the slab surface convection and radiation as with the other systems.
+
+For more information on the impact on the zone and air heat balances by the ventilated slab system, please consult the low temperature radiant system documentation and the EnergyPlus code.
+
+\subsection{CoolTower}\label{cooltower}
+
+\subsubsection{Overview}\label{overview-11-000}
+
+The Cool Tower (object ZoneCoolTower:Shower) is available for modeling a cooltower (which is sometimes referred to as s wind tower or a shower cooling tower) which is a component that is intended to model a passive downdraught evaporative cooling (PDEC) that is designed to capture the wind at the top of a tower and cool the outdoor air using water evaporation before delivering it to a space. The air flow in these systems is natural as the evaporation process increases the density of the air causing it to fall through the tower and into the space without the aid of a fan. A cooltower typically consists of a water spray or an evaporative pad, a shaft, and a water tank or reservoir. Wind catchers to improve the wind-driven performance at the top of the tower are optional. Water is pumped over an evaporative device by water pump which is the only component consumed power for this system. This water cools and humidifies incoming air and then the cool, dense air naturally falls down through shaft and leaves through large openings at the bottom of cooltowers.
+
+The shower cooling tower shown in figure below is controlled by a schedule and the specification of maximum water flow rate and volume flow rate as well as minimum indoor temperature. The actual flow rate of water and air can be controlled as users specify the fractions of water loss and flow schedule. The required input fields include effective tower height and exit area to obtain the temperature and flow rate of the air exiting the tower. A schedule and rated power for the water pump are also required to determine the power consumed. The component typically has a stand-alone water system that is not added to the water consumption from mains. However, users are required to specify the water source through an optional field, the name of water supply storage tank, in case any water comes from a water main.
+
+\begin{figure}[hbtp] % fig 330
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7400.svg.png}
+\caption{Typical Cooltower Configuration \protect \label{fig:typical-cooltower-configuration}}
+\end{figure}
+
+The cooltower model employing a model of the inertial shower cooling tower is intended to establish the actual mass flow rate of the air that leaves the cooltower and the evaporation rate consumed during the processes within the cooltower. Like infiltration, ventilation, and earth tubes, the air is assumed to be immediately mixed with the zone air. The determination of simultaneous heat and mass transfer that occurs during natural evaporative cooling in cooltower is complicated. Therefore, some assumptions have been made to obtain the conditions of the air and water. All cooltowers are executed at the start of each time step called by HVAC manager, and the conditions of air temperature and humidity ratio in the zone will be corrected with any other air that enters the zone.
+
+All temperatures in the following descriptions are in degrees C, mass flow rates are in kg/s, and volume flow rates are in m3/s.
+
+\subsubsection{Model Description}\label{model-description-5-000}
+
+The user must input the required information according to the Input Output Reference Manual (ref: ZoneCoolTower:Shower). The cooltower model requires a unique identifying name, an availability schedule, and the name of the zone being served. The schedule name must refer to a valid schedule type (range 0-1) and contain values of fractional cooltower operation as well as water pump operation. For the determination of the exit temperature and actual air volume flow rate, four additional inputs are required: effective tower height, exit area, fraction of flow schedule, and fraction of water loss. These define the conditions of the exit air, obtaining the conditions of outdoor air from the weather data and thus allow EnergyPlus to correct both the temperature and humidity level in the zone. The power consumed by the water pump can be directly determined by the schedule and rated power that the user inputs. The component is also controlled by the specification of minimum indoor temperature, maximum volume flow rate, and maximum water flow rate. These allow the model to prevent overcooling the zone or overestimation of the air volume flow rate. In addition, the user must input a flow control type according to the information that the user is able to obtain.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-5-000}
+
+The cooltower model first determines the temperature and volume flow rate of the exit air.~ Both parameters can be directly determined in case of water flow schedule control when the water flow rate is known. With the outdoor temperatures obtained from weather data, the exit air temperature (\emph{T\(_{out}\))} can be directly determined as functions of outdoor dry bulb temperature (DB), outdoor wet bulb temperature (WB), effective tower height (\emph{H}) and water flow rate (WF) in l/min by using following equation.
+
+\begin{equation}
+{T_{out}} = DB - (DB - WB)(1 - \exp ( - 0.8H))(1 - \exp ( - 0.15WF)
+\end{equation}
+
+The volume flow rate of the exit air (Q) can also be directly obtained as functions of water flow rate and effective tower height from the following equation.
+
+\begin{equation}
+Q = 0.0125WF \cdot {H^{0.5}}
+\end{equation}
+
+In case of that the calculated air volume flow rate is greater than maximum air volume flow rate in this control, which leads to overestimation of actual volume flow rate of the exit air, the calculated air volume flow rate is replaced with the maximum.
+
+For the simulation of wind-driven flow control where the water flow rate is unknown, the model determines velocity of the outlet air (\emph{V\(_{out}\)}) as functions of effective tower height and wind speed of outdoor air (WS) as
+
+\begin{equation}
+{V_{out}} = 0.7{H^{0.5}} + 0.47(WS - 1)
+\end{equation}
+
+The air volume flow rate (\emph{Q}) is then calculated by
+
+\begin{equation}
+{Q_{estimate}} = A \cdot {V_{out}}
+\end{equation}
+
+where \emph{A} is opening area at the bottom of cooltower.
+
+Substituting the air flow rate to the previous equation for \emph{Q,} water flow rate is obtained as
+
+\begin{equation}
+WF = \frac{Q}{{0.0125 \cdot {H^{0.5}}}}
+\end{equation}
+
+Once water flow rate is determined, the model checks the limit of water flow rate that the user inputs, so that the model prevents overestimation of actual volume flow rate of the exit air. If the calculated water flow rate is greater than the maximum water flow rate, the maximum will be chosen. The model also replaces the calculated air volume flow rate with the maximum volume flow rate from the user input when the calculated is greater than the maximum. Then, the model calculates the air volume flow rate and exit temperature using the previous equation for \emph{Q} and \emph{T\(_{out}\)}.
+
+This cooltower model allows the user to specify water loss due to drift or blow down and the loss of air flow (example: a cooltower which delivers air to both the interior and exterior of the building). If the user inputs the fraction of water loss or flow schedule that means some amount of the air actually goes to outside, the fractional values will be applied to previously calculated ones so that the model calculates both actual water flow rate (\emph{WF\(_{actual}\)}) and air volume flow rate (\emph{Q\(_{actual}\)}) as follows:
+
+\begin{equation}
+W{F_{actual}} = WF(1.0 + Fraction)
+\end{equation}
+
+\begin{equation}
+{Q_{actual}} = Q(1.0 - Fraction)
+\end{equation}
+
+The model then determines the exit humidity ratio (\({\omega_{out}}\) ) from the relation of mass balances below.
+
+\begin{equation}
+{\omega_{in}}({\dot m_{air}} + {\dot m_{water}}) = {\omega_{out}} \cdot {\dot m_{air}}
+\end{equation}
+
+In this case, actual mass flow rate at the inlet and outlet of cooltower cannot be correctly calculated with limited information. Thus, the model estimates initial conditions of the air based on the outdoor temperatures, the calculated exit air temperature, enthalpy of outdoor air (\emph{H\(_{in}\)}) and outdoor barometric pressure (P). Assuming no enthalpy changes and pressure drops between inlet air and the initialized air, the humidity ratio and mass flow of the initialized air can be obtained by using EnergyPlus psychrometric functions and the following equation.
+
+\begin{equation}
+{\omega_{in}} = PsyWRnTdbTwbPb({T_{d{b_{in}}}},{T_{w{b_{in}}}},P)
+\end{equation}
+
+\begin{equation}
+{\omega_{initial}} = PsyWRnTdbH({T_{out}},{H_{in}},P)
+\end{equation}
+
+\begin{equation}
+{\rho_{initial}}_{_{air}} = PsyRhoAirFnPbTdbW({T_{out}},{\omega_{initial}},P)
+\end{equation}
+
+\begin{equation}
+{\dot m_{air}} = {\rho_{initia{l_{air}}}} \cdot {Q_{actual}}
+\end{equation}
+
+where \({\omega_{initial}}\) and \({\rho_{initial}}\) ~are the humidity ratio and air density of the initialized air and \({\omega_{in}}\) is the humidity ratio of outdoor air.
+
+Therefore, the humidity ratio of exit air, \({\omega_{out}}\) , is
+
+\begin{equation}
+{\omega_{out}} = \frac{{{\omega_{in}}({{\dot m}_{air}} + {{\dot m}_{water}})}}{{{{\dot m}_{air}}}}
+\end{equation}
+
+Once the humidity ratio at the exit is determined, the model can obtain the actual density (\({\rho_{air}}\) ), specific heat (\({c_p}_{,air}\) ), and mass flow rate (\({\dot m_{cooltower}}\) ) of the air leaving cooltower by using EnergyPlus psychrometric function and following equation.
+
+\begin{equation}
+{c_p}_{,air} = PsyCpAirFnWtdb({\omega_{out}},{T_{out}})
+\end{equation}
+
+\begin{equation}
+{\rho_{air}} = PsyRhoAirFnPbTdbW({T_{out}},{\omega_{out}},P)
+\end{equation}
+
+\begin{equation}
+{\dot m_{cooltower}} = {\rho_{air}} \cdot {Q_{actual}}
+\end{equation}
+
+Assuming that the water temperature equals to outdoor wet bulb temperature, the model eventually determines density of the water and evaporation rate as bellows.
+
+\begin{equation}
+{\rho_{water}} = RhoH2O({T_{w{b_{in}}}})
+\end{equation}
+
+\begin{equation}
+{Q_{water}} = \frac{{{{\dot m}_a}({\omega_{out}} - {\omega_{in}})}}{{{\rho_{water}}}}
+\end{equation}
+
+\subsection{Earthtube}\label{earthtube}
+
+The earth tube model (input object ZoneEarthtube) provides a simple earth tube model that uses a complex ground heat transfer model to establish the temperature of the soil at the depth of the earth tube.~ The following information defines the basis for the model including the assumptions and mathematical equations.~ It supplements the information for the ZoneEarthtube input object given in the Input/Output Reference for EnergyPlus.
+
+\begin{itemize}
+\tightlist
+\item
+  Input Requirement
+\end{itemize}
+
+Pipe : Pipe radius(m), Pipe thickness(m), Pipe length(m)
+
+Distance between the pipe outer surface and undisturbed soil (m),
+
+Pipe thermal conductivity (W/m-C),
+
+Air velocity inside pipe(m/s), Depth of the radial center of pipe below ground (m)
+
+Soil : Soil density(kg/m\(^{3}\)), Soil specific heat(J/kg°C),
+
+Soil thermal Conductivity(W/m°C), Absorption coefficient,
+
+Fraction of evaporation rate
+
+\begin{itemize}
+\item
+  Assumption(s)
+\item
+  Convection flow inside the pipe is hydrodynamically and thermally developed.
+\item
+  Soil temperature in the pipe vicinity is uniform after the particular distance from the center of the pipe(thickness of the annulus), so that pipe surface temperature is uniform after the distance `r' from the center of the pipe, where `r'is the pipe radius.
+\item
+  The temperature profile in the pipe vicinity is not affected by the presence of the pipe, so that pipe surface temperature is uniform at axial direction.
+\item
+  The soil surrounding the pipe has homogeneous thermal conductivity.
+\item
+  Pipe has uniform cross section area at axial direction.
+\end{itemize}
+
+Wind velocity (m/s), u, is the annual average value. This is calculated from EnergyPlus weather data by averaging individual wind velocity values of the whole year. The convective heat transfer coefficient at the soil surface (W/m\(^{2}\)°C), \emph{h\(_{s}\)}, is function of wind speed u. According to McAdams(1954) \emph{h\(_{s}\)} can be approximated by the following correlation (Krarti, 1995).
+
+\begin{equation}
+{h_s} = 5.7 + 3.8u
+\end{equation}
+
+In case of \emph{h\(_{e}\)} and \emph{h\(_{r}\)}, they can be determined by the following equations.
+
+\begin{equation}
+{h_e} = {h_s}\left( {1 + 0.0168af} \right)
+\end{equation}
+
+\begin{equation}
+{h_r} = {h_s}\left( {1 + 0.0168a{r_a}f} \right)
+\end{equation}
+
+with a = 103 Pa/°C.
+
+Average air temperature (°C), \emph{T\(_{ma}\)}, is also calculated from EnergyPlus weather data by averaging individual air temperature values of the whole year.
+
+The appropriate value of hemispherical emittance of the ground surface, \emph{ε,} is 0.93\textasciitilde{}0.96. Radiation constant (W/m\(^{2}\)), \emph{ΔR,} depends on soil radiative properties, air relative humidity, and effective sky temperature. An appropriate value of \emph{ΔR} according to Krarti (1995) is 63 W/m\(^{2}\).
+
+The absorption coefficient, \emph{β}, depends on the soil absorptance and shading condition. The coefficient \emph{β} is approximately equal to one minus the soil surface albedo. Albedo depends on soil cover and moisture content. Albedo = 0.1 corresponds to wet soils, albedo = 0.2 to moderate soils, and albedo = 0.3 to dry soils.
+
+Average solar radiation (W/m\(^{2}\)), \emph{S\(_{m}\)}, is determined from EnergyPlus weather data by averaging individual global horizontal solar radiation values of the whole year.
+
+The fraction of evaporation rate, \emph{f}, also depends mainly on the soil cover and the soil moisture level. Based on the results reported by Penman, it is recommended to estimate the fraction f as follows. For bare soil, \emph{f} is directly proportional to soil moisture content. For instance, f = 1 corresponds to saturated soils, f = 0.6\textasciitilde{}0.8 to wet soils, f = 0.4\textasciitilde{}0.5 to moist soils, f = 0.1\textasciitilde{}0.2 to arid soils. For dry soils, f = 0, since no evaporation occurs. For covered soils, the fraction f is obtained by multiplying 0.7 by the value of f for bare soil depending on the soil moisture content (Krarti, 1995).
+
+Relative humidity, \emph{r\(_{a}\)}, is also calculated from EnergyPlus weather data by averaging individual relative humidity values of the whole year.
+
+The soil thermal diffusivity (m\(^{2}\)/s), \emph{α\(_{s}\)}, and conductivity (W/m°C), \emph{k\(_{s}\)}, varies with the density and moisture content. From Table 3.3, pg. 26 of ASHRAE's Ground Source Heat Pumpss--Design of Geothermal Systems for Commercial and Institutional Buildings, 1997, the following values are recommended under different conditions.
+
+\begin{longtable}[c]{p{1.2in}p{1.2in}p{1.2in}p{1.2in}p{1.2in}}
+\toprule 
+Soils & Moisture  Content & Density  [kg/m3] & k  [W/m-K] & α   [m\^{}2/s] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Soils & Moisture  Content & Density  [kg/m3] & k  [W/m-K] & α   [m\^{}2/s] \tabularnewline
+\midrule
+\endhead
+
+Heavy clay & 15\% water & 1922 & 1.558 & 5.914E-07 \tabularnewline
+ & 5\% water & 1922 & 1.212 & 6.452E-07 \tabularnewline
+Light clay & 15\% water & 1281 & 0.865 & 4.624E-07 \tabularnewline
+ & 5\% water & 1281 & 0.692 & 4.839E-07 \tabularnewline
+Heavy sand & 15\% water & 1922 & 3.115 & 1.129E-07 \tabularnewline
+ & 5\% water & 1922 & 2.596 & 1.344E-06 \tabularnewline
+Light sand & 15\% water & 1281 & 1.558 & 8.065E-07 \tabularnewline
+ & 5\% water & 1281 & 1.385 & 9.677E-07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The following information is also available for reference from Table~\ref{table:atmospheric-variables-at-two-different}, pg. 34.6 of the ASHRAE Applications Handbook, 2015.
+
+\begin{longtable}[c]{p{1.2in}p{1.2in}p{1.2in}p{1.2in}p{1.2in}}
+\toprule 
+Soils & Moisture  Content & Density  [kg/m3] & k  [W/m-K] & α   [m\^{}2/s] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Soils & Moisture  Content & Density  [kg/m3] & k  [W/m-K] & α   [m\^{}2/s] \tabularnewline
+\midrule
+\endhead
+
+Heavy clay & 15\% water & 1922 & 1.558 & 5.914E-07 \tabularnewline
+ & 5\% water & 1922 & 1.212 & 6.452E-07 \tabularnewline
+Light clay & 15\% water & 1281 & 0.865 & 4.624E-07 \tabularnewline
+ & 5\% water & 1281 & 0.692 & 4.839E-07 \tabularnewline
+Heavy sand & 15\% water & 1922 & 3.115 & 1.129E-07 \tabularnewline
+ & 5\% water & 1922 & 2.596 & 1.344E-06 \tabularnewline
+Light sand & 15\% water & 1281 & 1.558 & 8.065E-07 \tabularnewline
+ & 5\% water & 1281 & 1.385 & 9.677E-07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Annual angular frequency, \emph{w}, is equal to 1.992 x 10\(^{-7}\)rad/s, and dampening depth (m), D, is calculated from the following equation:
+
+\begin{equation}
+D = \sqrt {\frac{{2{\alpha_s}}}{w}}
+\end{equation}
+
+The value of δ is evaluated as follows.
+
+\begin{equation}
+\delta  = \frac{{1 + i}}{D}
+\end{equation}
+
+Amplitude of the air temperature (°C), \emph{T\(_{va}\)}, can be evaluated from EnergyPlus weather data by dividing the difference between the maximum and minimum air temperature value of the whole year by two. Similarly, amplitude of the solar radiation (W/m\(^{2}\)), \emph{S\(_{v}\)}, can also be determined from weather data by dividing the difference between the maximum and minimum solar radiation value of the whole year by two.
+
+Phase angle between the insolation and the air temperature (rad), \emph{φ\(_{I}\)} , is calculated by subtracting insolation phase angle from air temperature phase angle. Phase angle of insolation and air temperature is the point from the beginning of the year at which the insolation and air temperature respectively reaches the minimum value among the whole year.
+
+Phase constant of the air (sec), \emph{t\(_{0a}\)}, is the time elapsed from the beginning of the year at which the air temperature reaches the minimum value in the year.
+
+By using all the input parameters and variables described above, average soil surface temperature (°C), \emph{T\(_{m}\)}, amplitude of the soil surface temperature variation (°C), \emph{A\(_{s}\)}, phase constant of the soil surface (sec), \emph{t\(_{0}\)}, and phase angle difference between the air and soil surface temperature (rad), \emph{Φ\(_{s}\)}, can be evaluated as follows \(^{1)}\):
+
+\begin{equation}
+{T_m} = \frac{1}{{{h_e}}}\left[ {{h_r}{T_{ma}} - \varepsilon \Delta R + \beta {S_m} - 0.0168{h_s}fb\left( {1 - {r_a}} \right)} \right]
+\end{equation}
+
+\begin{equation}
+{A_s} = \left\| {\frac{{{h_r}{T_{va}} - \beta {S_v}{e^{i{\phi_I}}}}}{{\left( {{h_e} + \delta {k_s}} \right)}}} \right\|
+\end{equation}
+
+\begin{equation}
+{t_0} = {t_{0a}} + \frac{{{\phi_s}}}{w}
+\end{equation}
+
+\begin{equation}
+{\phi_s} =  - Arg\left[ {\frac{{{h_r}{T_{va}} - \beta {S_v}{e^{i{\phi_I}}}}}{{\left( {{h_e} + \delta {k_s}} \right)}}} \right]
+\end{equation}
+
+(Note: T\(_{m}\), A\(_{s}\), and t\(_{0}\) are calculated by the CalcSoilSurfTemp program and are inputs to EnergyPlus.~ The remainder of this section describes what has been implemented in EnergyPlus.)
+
+The symbols \textbar{}\textbar{}~ \textbar{}\textbar{} and Arg denote the modulus and the argument of a complex number respectively. In order to calculate \emph{A\(_{s}\)} and \emph{Φ\(_{s}\)}, the complex number under consideration can be rearranged as the following form:
+
+\begin{equation}
+  \begin{array}{ll}
+    \frac{h_r T_{va} - \beta S_v e^{i \phi_I}}{h_e + \delta k_s} 
+           &=  \frac{ \PB{h_e + \frac{k_s}{D}} \PB{ h_r T_{va} - \beta S_v \cos \phi_I} + \frac{k_s}{D} \PB{-\beta S_v \sin \phi_I}}{\PB{h_e + \frac{k_s}{D}}^2 + \PB{\frac{k_s}{D}}^2} \\
+           &+ i\frac{ \PB{h_e + \frac{k_s}{D}} \PB{-\beta S_v \sin \phi_I} - \frac{k_s}{D} \PB{h_r T_{va} - \beta S_v \cos \phi_I}}{\PB{h_e + \frac{k_s}{D}}^2 + \PB{\frac{k_s}{D}}^2}
+  \end{array}
+\end{equation}
+
+Assuming a homogeneous soil of constant thermal diffusivity, the temperature at any depth z and time t can be estimated by the following expression \(^{2)}\).
+
+\begin{equation}
+{T_{z,t}} = {T_m} - {A_s}\exp \left[ { - z{{\left( {\frac{\pi }{{{\rm{365}}{\alpha_s}}}} \right)}^{1/2}}} \right]\cos \left\{ {\frac{{2\pi }}{{{\rm{365}}}}\left[ {t - {t_0} - \frac{z}{2}{{\left( {\frac{{{\rm{365}}}}{{\pi {\alpha_s}}}} \right)}^{1/2}}} \right]} \right\}
+\end{equation}
+
+In this expression, the unit of time, \emph{t}, and phase constant of the soil surface, \emph{t\(_{0}\)}, should be converted into days. Similarly, the unit of soil thermal diffusivity, \emph{α\(_{s}\)}, should also be converted into m\(^{2}\)/days.
+
+By integrating the expression with respect to depth, the average temperature of a vertical soil profile ranging between depth z\(_{1}\) and z\(_{2}\) (°C ) can be determined as follows \(^{2)}\).
+
+{\scriptsize
+\begin{equation}
+{T_{{z_1},{z_2},t}} = {T_m} + \frac{{{A_s}}}{{\left( {{z_2} - {z_1}} \right)\gamma \sqrt 2 }}\left\{ {{e^{ - \gamma {z_1}}}\cos \left[ {\frac{{2\pi }}{{{\rm{365}}}}\left( {t - {t_0} - {z_1}L - 45.6} \right)} \right] - {e^{ - \gamma {z_2}}}\cos \left[ {\frac{{2\pi }}{{{\rm{365}}}}\left( {t - {t_0} - {z_2}L - 45.6} \right)} \right]} \right\}
+\end{equation}}
+
+where,
+
+\begin{equation}
+\gamma  = {\left( {\pi /{\rm{365}}{\alpha_s}} \right)^{1/2}}
+\end{equation}
+
+\begin{equation}
+L = \frac{1}{2}{\left( {{\rm{365}}/\pi {\alpha_s}} \right)^{1/2}}
+\end{equation}
+
+As the final step with regard to the heat transfer between soil and earth tube system, thermal conductivity of air (W/m°C), \emph{k\(_{air}\)}, and kinetic viscosity of air (m\(^{2}\)/s), υ, should calculated first \(^{3)}\).
+
+\begin{equation}
+{k_{air}} = 0.02442 + ({10^{ - 4}}(0.6992{T_a}))
+\end{equation}
+
+\begin{equation}
+\upsilon  = {10^{ - 4}}(0.1335 + 0.000925{T_a})
+\end{equation}
+
+By using the values of thermal conductivity of air, \emph{k\(_{air}\)}, and kinetic viscosity of air, υ, the convective heat transfer coefficient at the inner pipe surface (W/m\(^{2}\)°C), \emph{h\(_{c,}\)} can be evaluated. It is a function of Reynolds number, Re, and Nusselt number, Nu \(^{4)}\), where
+
+\begin{equation}
+{h_c} = \frac{{Nu{k_{air}}}}{{2{r_1}}}
+\end{equation}
+
+\begin{equation}
+Nu = \frac{{({f_a}/2)({\mathop{\rm Re}\nolimits}  - 1000)\Pr }}{{1 + 12.7{{({f_a}/2)}^{1/2}}({{\Pr }^{2/3}} - 1)}}
+\end{equation}
+
+\begin{equation}
+{f_a} = {(1.58\ln {\mathop{\rm Re}\nolimits}  - 3.28)^{ - 2}}
+\end{equation}
+
+\begin{equation}
+  \mathop{\rm Re}\nolimits  = \frac{{2{r_1}{V_a}}}{\nu }
+\end{equation}
+
+\begin{equation}
+\Pr  = \frac{\nu }{{{\alpha_{air}}}}
+\end{equation}
+
+where \emph{r\(_{1}\)} is inner pipe radius (m), and \emph{V\(_{a}\)} is average pipe air velocity (m/s).
+
+After determining the convective heat transfer coefficient, \emph{R\(_{c}\)}, \emph{R\(_{p}\)} and \emph{R\(_{s}\)} are respectively calculated as follows.
+
+\begin{equation}
+{R_c} = \frac{1}{{2\pi {r_1}{h_c}}}
+\end{equation}
+
+\begin{equation}
+{R_p} = \frac{1}{{2\pi {k_p}}}\ln \frac{{{r_1} + {r_2}}}{{{r_1}}}
+\end{equation}
+
+\begin{equation}
+{R_s} = \frac{1}{{2\pi {k_s}}}\ln \frac{{{r_1} + {r_2} + {r_3}}}{{{r_1} + {r_2}}}
+\end{equation}
+
+where \emph{R\(_{c}\)} is thermal resistance due to convection heat transfer between the air in the pipe and the pipe inner surface (m-C/W), \emph{R\(_{p}\)} is thermal resistance due to conduction heat transfer between the pipe inner and outer surface (m-C/W), and \emph{R\(_{s}\)} is thermal resistance due to conduction heat transfer between the pipe outer surface and undisturbed soil (m-C/W). In addition \emph{r\(_{2}\)} is pipe thickness (m), \emph{r\(_{3}\)} is distance between the pipe outer surface and undisturbed soil (m), and \emph{L} is pipe length (m).
+
+Finally, the heat transfer between the soil and the air inside the pipe is equal to the amount of heat losses as air flows along the pipe (Jacovides and Mihalakakou, 1995).
+
+\begin{equation}
+{U_t}\,\,\left[ {{T_a}(y) - {T_{z,t}}} \right]dy =  - {\dot m_a}{C_a}\left[ {d{T_a}(y)} \right]
+\end{equation}
+
+with
+
+\begin{equation}
+{U_t} = \frac{1}{{{R_t}}}
+\end{equation}
+
+\begin{equation}
+{R_t} = {R_c} + {R_p} + {R_s}
+\end{equation}
+
+where \emph{U\(_{t}\)} is overall heat transfer coefficient of the whole earth tube system (W/C-m), \emph{T\(_{a}\)(y)} is air temperature of the pipe at the distance y from the pipe inlet (°C), and \emph{m\(_{a}\)} is mass flow rate of ambient air through pipe (kg/s). \emph{C\(_{a}\)} is specific heat of air (J/kg°C) and \emph{R\(_{t}\)} is total thermal resistance between pipe air and soil (m-C/W).
+
+Initial condition of inlet air temperature is equal to the ambient air temperature. Outlet air temperature is finally evaluated by solving the heat transfer equation above.
+
+% table 87
+\begin{longtable}[c]{p{1.5in}p{3.0in}p{1.5in}}
+\caption{Nomenclature for Earthtube Model \label{table:nomenclature-for-earthtube-model}} \tabularnewline
+\toprule 
+Variable & Description & Units \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature for Earthtube Model} \tabularnewline
+\toprule 
+Variable & Description & Units \tabularnewline
+\midrule
+\endhead
+
+A\(_{s}\) & amplitude of the soil surface temperature variation & (°C) \tabularnewline
+C\(_{a}\) & specific heat of air & (J/kg°C) \tabularnewline
+h\(_{c}\) & convective heat transfer coefficient at the inner pipe surface & (W/m\(^{2}\)°C) \tabularnewline
+h\(_{s}\) & convective heat transfer coefficient at the soil surface & (W/m\(^{2}\)°C) \tabularnewline
+k\(_{air}\) & thermal conductivity of the air & (W/m°C) \tabularnewline
+k\(_{p}\) & pipe thermal conductivity & (W/m°C) \tabularnewline
+k\(_{s}\) & soil thermal conductivity & (W/m°C) \tabularnewline
+L & pipe length & (m) \tabularnewline
+m\(_{a}\) & mass flow rate of ambient air through pipe & (kg/s) \tabularnewline
+r\(_{1}\) & relative humidity & ~ \tabularnewline
+R\(_{c}\) & thermal resistance due to convection heat transfer between the air in the pipe and the pipe inner surface & (m-C/W) \tabularnewline
+R\(_{p}\) & thermal resistance due to conduction heat transfer between the pipe inner and outer surface & (m-C/W) \tabularnewline
+R\(_{s}\) & thermal resistance due to conduction heat transfer between the pipe outer surface and undisturbed soil & (m-C/W) \tabularnewline
+R\(_{t}\) & total thermal resistance between pipe air and soil & (m-C/W) \tabularnewline
+ΔR & radiation constant & (63W/m\(^{2}\)) \tabularnewline
+r\(_{1}\) & inner pipe radius & (m) \tabularnewline
+r\(_{2}\) & pipe thickness & (m) \tabularnewline
+r\(_{3}\) & distance between the pipe outer surface and undisturbed soil & (m) \tabularnewline
+S\(_{m}\) & average solar radiation & (W/m\(^{2}\)) \tabularnewline
+S\(_{v}\) & amplitude of the solar radiation & (W/m\(^{2}\)) \tabularnewline
+t & time elapsed from beginning of calendar year & (days) \tabularnewline
+T\(_{a}\)(y) & air temperature of the pipe at the distance y from the pipe inlet & (°C) \tabularnewline
+T\(_{m}\) & average soil surface temperature & (°C) \tabularnewline
+T\(_{ma}\) & average air temperature & (°C) \tabularnewline
+t\(_{o}\) & phase constant of the soil surface & (sec; days) \tabularnewline
+t\(_{oa}\) & phase constant of the air & (sec; days) \tabularnewline
+T\(_{va}\) & amplitude of the air temperature & (°C) \tabularnewline
+T\(_{z,t}\) & ground temperature at time t and depth z & (°C) \tabularnewline
+T\(_{z1,z2,t}\) & soil profile temperature at time t, averaged over depths between z\(_{1}\) and z\(_{2}\) & (°C) \tabularnewline
+u & ~wind velocity above the ground surface & (m/s) \tabularnewline
+U\(_{t}\) & overall heat transfer coefficient of the whole earth tube system & (W/m-C) \tabularnewline
+V\(_{a}\) & average pipe air velocity & (m/s) \tabularnewline
+z & depth of the radial center of pipe below soil surface & (m) \tabularnewline
+z\(_{1}\) & upper bounds of some vertical profile in soil & (m) \tabularnewline
+z\(_{2}\) & lower bounds of some vertical profile in soil & (m) \tabularnewline
+$\alpha$\(_{s}\) & soil thermal diffusivity & (m\(^{2}\)/s; m\(^{2}\)/days) \tabularnewline
+$\beta$ & soil absorption coefficient ( = 1 – soil albedo) & ~ \tabularnewline
+$\varepsilon$ & hemispherical emittance of the ground surface & ~ \tabularnewline
+$\varphi$\(_{1}\) & phase angle between the insolation and the air temperature & (rad) \tabularnewline
+$\phi$\(_{s}\) & phase angle difference between the air and soil surface temperature & (rad) \tabularnewline
+Ï… & kinetic viscosity of air & (m\(^{2}\)/s) \tabularnewline
+w & annual angular frequency ( = 1.992 x 10\(^{-7}\)rad/s) & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{References}\label{references-6-001}
+
+Krarti M., Lopez-Alonzo C., Claridge D. E. and Kreider J. F. 1995. Analytical model to predict annual soil surface temperature variation. Journal of Solar Energy Engineering 117, 91\textasciitilde{}99
+
+Labs K. In: Cook J., editor. 1989. Passive cooling. Cambridge Massachusetts, London, England: MIT Press
+
+Al-Ajmi F., Loveday D. L. and Hanby V. I. 2005. The Cooling Potential of Earth-air Heat Exchangers for Domestic Buildings in a Desert Climate, Building and Environment
+
+Necati Ozisik M. 1885. Heat transfer: A basic approach, McGraw-Hill Book Company
+
+Jacovides C. P. and Mihalakakou G. 1995. An Underground Pipe Systems as an Energy Source for Cooling/Heating Purposes. Renewable Energy 6, pp.893\textasciitilde{}900
+
+\subsection{Thermal Chimney Model}\label{thermal-chimney-model}
+
+The ZoneThermalChimney input object is available for modeling a thermal chimney which is a device that uses stack driven air movement to ventilate spaces within a building. These systems have been used successfully in buildings as small as the size of an outhouse up to large commercial buildings. The air within a thermal chimney is heated naturally using solar energy. The air increases in temperature which causes its density to drop. This drop in density results in a natural vertical movement of air and a local drop in pressure. The drop in pressure is relieved by drawing air from the building interior, and the heat gained within the thermal chimney does not enter the occupied portion of the building. These systems are often used in support of natural ventilation systems. The EnergyPlus model will seek to model the air heat balance effects of the thermal chimney, balance air movements caused by the thermal chimney, and report other appropriate system variables. The new model will be linked into the air heat balance in a fashion similar to the current infiltration and simple ventilation models but will not be linked to an HVAC air loop.~ Any flow through the thermal chimney will be accounted for in the air mass balance in the HVAC calculations. However, other sophisticated ventilation strategies can be handled by other existing EnergyPlus components.
+
+\begin{itemize}
+\item
+  Thermal Chimney Input Requirements
+\item
+  Distance from the top of thermal chimney to each inlet (m),
+\item
+  Relative ratio of air flow rates passing through each inlet,
+\item
+  Width of the absorber wall (m),
+\item
+  Discharge coefficient,
+\item
+  Cross sectional area of air channel outlet (m\(^{2}\)),
+\item
+  Cross sectional areas of each air channel inlet (m\(^{2}\))
+\item
+  ~Assumptions
+\item
+  Surface temperature of the glass cover is uniformly distributed.
+\item
+  Surface temperature of the absorber wall is uniformly distributed.
+\item
+  The inlet temperature of the air channel in the thermal chimney is equal to the room air temperature.
+\item
+  Resistance to the air flow due to the surface friction is negligible.
+\item
+  The discharged amount of interior air induced by the thermal chimney is replaced by the outdoor air infiltration.
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 331
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7454.png}
+\caption{Basic Composition of Thermal Chimney \protect \label{fig:basic-composition-of-thermal-chimney}}
+\end{figure}
+
+Mathematical model currently available for thermal chimneys has the capability to handle the thermal chimney having only one inlet. In other words, it is unlikely that thermal chimneys with multiple inlets due to multiple stories utilizing the common thermal chimney can be mathematically modeled without computational fluid dynamics. Therefore, if the thermal chimney to be modeled has multiple inlets, it will be assumed that it will have only one inlet. For this assumption, the user will be required to specify the relative ratio of air flow rates passing through each inlet to compute the overall length of the thermal chimney (m), \emph{L}, overall room air temperature (K), \emph{T\(_{r}\)}, and overall cross sectional area of air channel inlet (m\(^{2}\)), \emph{A\(_{i}\)}, as follows:
+
+\begin{equation}
+L = \frac{{{L_1}{r_1}{E_1} + {L_2}{r_2}{E_2} + {L_3}{r_3}{E_3} +  \cdot  \cdot  \cdot  + {L_n}{r_n}{E_n}}}{{{r_1}{E_1} + {r_2}{E_2} + {r_3}{E_3} +  \cdot  \cdot  \cdot  + {r_n}{E_n}}}
+\end{equation}
+
+\begin{equation}
+{T_r} = {T_{r1}}{r_1} + {T_{r2}}{r_2} + {T_{r3}}{r_3} +  \cdot  \cdot  \cdot  + {T_{rn}}{r_n}
+\end{equation}
+
+\begin{equation}
+{A_i} = {A_{i1}} + {A_{i2}} + {A_{i3}} +  \cdot  \cdot  \cdot  + {A_{in}}
+\end{equation}
+
+Where, \emph{A\(_{in}\)} is the cross sectional area of nth air channel inlet (m\(^{2}\)), \emph{L\(_{n}\)} is the distance from the top of thermal chimney to nth inlet (m), \emph{E\(_{n}\)} is the room air specific enthalpy corresponding to nth inlet (J/kg), \emph{r\(_{n}\)} is the relative ratio of air flow rate passing through nth inlet and \emph{T\(_{rn}\)} is the room air temperature corresponding to nth inlet (K). Among them, room air specific enthalpy, \emph{E\(_{n}\)}, and room air temperature corresponding to each inlet, \emph{T\(_{rn}\)}, are directly calculated inside EnergyPlus. In addition, the relative ratios should meet the following expression:
+
+\begin{equation}
+{r_1} + {r_2} + {r_3} +  \cdot  \cdot  \cdot  + {r_n} = 1
+\end{equation}
+
+After merging the multiple inlets into a single inlet condition based on the description above, the following algorithm which is widely used is employed for the modeling of the thermal chimney.
+
+The key output parameter in the thermal chimney model is the enhanced amount of natural ventilation rate caused by the presence of a thermal chimney. In order to determine the enhanced ventilation, the discharge air temperature from a thermal chimney should be calculated, which, in turn, should be computed based on the information on the absorber wall temperature, glass cover temperature and the vertical air temperature distribution within the thermal chimney. Among them, energy balances for the absorber wall and the glass cover are carried out using the existing algorithm currently available in EnergyPlus, which has the similar approach to the Trombe wall. On the other hand, the vertical air temperature distribution and the resultant discharge air temperature of the thermal chimney are computed using the separate thermal chimney algorithm described in the following paragraphs.
+
+Once the glass cover temperature and the absorber wall temperature are computed using the existing modeling algorithm in EnergyPlus, the energy balance for the fluid (air inside the thermal chimney) can be expressed as:
+
+\begin{equation}
+{h_{wf}}({T_w} - \overline {{T_f}} ) = {h_{gf}}(\overline {{T_f}}  - {T_g}) + \frac{{\dot m{C_p}}}{w}\frac{{d{T_f}}}{{dx}}
+\end{equation}
+
+Where, \emph{m} is the total mass flow rate of the air (kg/s), \emph{C\(_{p}\)} is the specific heat of air (J/kg°C), \emph{w} is the width of the absorber wall (m) and \emph{x} is the elemental length of the absorber wall (m).
+
+Since the initial condition of inlet air temperature in this differential equation is equal to the room air temperature (i.e. \emph{x = 0, T\(_{f,i}\) = T\(_{r}\)}), the outlet air temperature, \emph{T\(_{fo}\)}, can be finally evaluated.
+
+Finally, the total air flow rate caused by the thermal chimney (m\(^{3}\)/s), \emph{Q}, can be evaluated from the following expression {[}1{]}:
+
+\begin{equation}
+Q = {C_d}{A_o}\sqrt {\frac{{2(\frac{{{T_{fo}} - {T_r}}}{{{T_r}}})gL}}{{{{(1 + {A_r})}^2}}}}
+\end{equation}
+
+\begin{equation}
+{A_r} = {A_o}/{A_i}
+\end{equation}
+
+Where, \emph{C\(_{d}\)} is the discharge coefficient, \emph{A\(_{o}\)} and \emph{A\(_{i}\)} is the cross sectional areas of air channel outlet and inlet (m\(^{2}\)), respectively, \emph{T\(_{fo}\)} is the outlet air temperature (K), \emph{T\(_{r}\)} is the room air temperature (K) and \emph{L} is the total length of the thermal chimney (m).
+
+Since multiple inlets are merged into a single inlet in the beginning, the air flow rate passing through each inlet due to the existence of the thermal chimney can be finally determined as follows:
+
+\({Q_1} = Q{r_1}\) ,~~~ \({Q_2} = Q{r_2}\) ,~~~ \({Q_3} = Q{r_3}\) ,~~~ ∙∙∙,~~~ \({Q_n} = Q{r_n}\)
+
+Where, \emph{Q\(_{n}\)} is the air flow rate passing through nth inlet (m\(^{3}\)/s) and \emph{r\(_{n}\)} is the relative ratio of air flow rate passing through nth inlet.
+
+The discharged amount of interior air from each zone caused by the presence of the thermal chimney is assumed to be replaced by the outdoor air infiltration.
+
+% table 88
+\begin{longtable}[l]{p{1.5in}p{4.5in}}
+\caption{Nomenclature of Thermal Chimney Model \label{table:nomenclature-of-thermal-chimney-model}} \tabularnewline
+\toprule 
+Model Nomenclature \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature of Thermal Chimney Model} \tabularnewline
+\toprule 
+Model Nomenclature \tabularnewline
+\midrule
+\endhead
+
+Variable & Description \tabularnewline
+A\(_{i}\) & cross sectional area of air channel inlet (m\(^{2}\)) \tabularnewline
+A\(_{o}\) & cross sectional area of air channel outlet (m\(^{2}\)) \tabularnewline
+C\(_{d}\) & discharge coefficient \tabularnewline
+C\(_{p}\) & specific heat of air (J/kg°C) \tabularnewline
+E\(_{n}\) & room air specific enthalpy corresponding to nth inlet (J/kg) \tabularnewline
+g & acceleration due to gravity (9.8 m/s\(^{2}\)) \tabularnewline
+h\(_{gam}\) & convective heat transfer coefficients between the glass and ambient air (W/m\(^{2}\)°C ) \tabularnewline
+h\(_{gf}\) & convective heat transfer coefficients between the glass and the fluid (W/m\(^{2}\)°C ) \tabularnewline
+h\(_{iw}\) & convective heat transfer coefficients between absorber wall inner surface and the room air (W/m\(^{2}\)°C ) \tabularnewline
+h\(_{wf}\) & convective heat transfer coefficients between the absorber wall and the fluid (W/m\(^{2}\)°C ) \tabularnewline
+h\(_{wind}\) & The convective heat transfer coefficient due to the wind (W/m\(^{2}\)°C ) \tabularnewline
+H\(_{sr}\) & incident solar radiation on vertical surface (W/m\(^{2}\)) \tabularnewline
+k\(_{air}\) & thermal conductivity of air (W/m°C) \tabularnewline
+L & total length of the thermal chimney (m) \tabularnewline
+M & mass flow rate of the air (kg/s) \tabularnewline
+r\(_{n}\) & relative ratio of air flow rate passing through nth inlet \tabularnewline
+S\(_{g}\) & solar radiation absorbed by the glass cover (W/m\(^{2}\)) \tabularnewline
+S\(_{w}\) & solar radiation absorbed by the absorber wall (W/m\(^{2}\)) \tabularnewline
+T\(_{am}\) & ambient air temperature (K) \tabularnewline
+T\(_{f}\) & fluid temperature averaged over the entire length of the thermal chimney (K) \tabularnewline
+T\(_{fi}\) & inlet air temperature of the thermal chimney (K) \tabularnewline
+T\(_{fo}\) & outlet air temperature of the thermal chimney (K) \tabularnewline
+T\(_{g}\) & glass cover temperature (K) \tabularnewline
+T\(_{r}\) & room air temperature (K) \tabularnewline
+T\(_{s}\) & surface temperature (K) \tabularnewline
+T\(_{w}\) & absorber wall temperature (K) \tabularnewline
+T\(_{\infty}\) & fluid temperature (K) \tabularnewline
+u & wind speed (m/s) \tabularnewline
+U\(_{w}\) & Overall heat transfer coefficient from the room air and the absorber wall (W/m\(^{2}\)°C ) \tabularnewline
+w & width of the absorber wall (m) \tabularnewline
+x & elemental length of the absorber wall (m) \tabularnewline
+$\alpha$\(_{g}\) & absorptance of glass cover \tabularnewline
+$\alpha$\(_{w}\) & absorptance of absorber wall \tabularnewline
+$\beta$ & air volumetric coefficient of expansion (K\(^{-1}\)) \tabularnewline
+$\varepsilon$\(_{g}\) & emissivity of the glass cover \tabularnewline
+$\sigma$ & Stefan-Boltzmann constant (5.67x10 -8 W/m\(^{2}\)K\(^{4}\)) \tabularnewline
+$\tau$ & transmittance of the glass cover \tabularnewline
+$\nu$ & kinematic viscosity of air (m\(^{2}\)/s) \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{References}\label{references-7-000}
+
+N. K. Bansal, R. Mathur and M. S. Bhandari, Solar Chimney for enhanced Stack Ventilation, Building and Environment, 28, pp.373-377, 1993
+
+K. S. Ong, A Mathematical Model of a Solar Chimney, Renewable Energy, 28, pp.1047-1060, 2003
+
+N. K. Bansal, R. Mathur and M. S. Bhandari, A Study of Solar Chimney Assisted Wind Tower System for Natural Ventilation in Buildings, Building and Environment, 29, pp.495-500, 1994
+
+J. Marti-Herrero and M. R. Heras-Celemin, Dynamic Physical Model for a Solar Chimney, Solar Energy, 81, pp.~614-622, 2007
+
+M. M. Aboulnaga and S. N. Abdrabboh, Improving Night Ventilation into Low-rise Buildings in Hot-arid Climates Exploring a Combined Wall-roof Solar Chimney, Renewable Energy, 19, pp.~47-54, 2000
+
+\subsection{Zone Outdoor Air Unit}\label{zone-outdoor-air-unit}
+
+The zone outdoor air unit (object ZoneHVAC:OutdoorAirUnit) is intended to model systems such as zone make-up air units and dedicated outside air systems.~ These components are ``zone equipment'' meaning that they do not require an air loop but serve a zone directly.~ The system is comprised of a supply fan (in either draw through or blow through configuration), an optional exhaust fan, and a variety of components such as heating coils, cooling coils, heat recovery, etc.~ The object of the zone outdoor air unit is to bring in additional ventilation air into a zone.~ These might be used for high ventilation spaces such as kitchens or laboratories where another system is primarily responsible for space conditioning while the zone outside air unit is primarily responsible for fresh air delivery to the zone.~ Most of the information necessary to configure a zone outdoor air unit is contained in the EnergyPlus Input/Output Reference.~ A diagram of the zone outdoor air unit is shown below.~ As this system is relatively simple and does not contain any unique operating algorithm or equations, the discussion here is limited to the application of the user defined controls and how it relates to the operation of the device.
+
+\begin{figure}[hbtp] % fig 332
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7466.png}
+\caption{Zone Outdoor Air Unit Schematic \protect \label{fig:zone-outdoor-air-unit-schematic}}
+\end{figure}
+
+\subsection{Controls}\label{controls-2-000}
+
+Three input parameters control the operation of the zone outdoor air unit.~ The unit control type has two options: neutral or temperature.~ If the temperature control type is selected, the user must also provide a high and low air temperature control schedule.~ The algorithm for controlling the zone outdoor air unit is dependent on these parameters which are used as described below.
+
+\textbf{\emph{Neutral Control.}}~ If the user selects neutral control, the intent is to provide additional outside air to the zone without imposing any additional thermal load on the zone or any other systems serving the zone.~ In other words, the unit will attempt to provide air to the zone at the zone mean air temperature.~ Mathematically, this means:
+
+\begin{equation}
+{T_{out}} = {T_{MAT}}
+\end{equation}
+
+where:
+
+~~~~~ T\(_{out}\) = the outlet temperature of the zone outdoor air unit
+
+~~~~~ T\(_{MAT}\) = the mean air temperature of the zone being served by the unit
+
+It should be noted that to avoid excessive iteration that the zone mean air temperature that is used is the mean air temperature from the previous time step.~ This will result in a slight lagging that may introduce a slight thermal load, but this should be minimal.
+
+\textbf{\emph{Temperature Control}}.~ If the user selects temperature control, the intent is to limit the outlet temperature of the unit for either heating or cooling or both or perhaps to provide unconditioned air to the space.~ The algorithm used to determine the outlet temperature of the unit is as follows.~ When the outdoor air temperature is at or below the low air temperature control schedule value, the outlet temperature is set to the low air temperature control schedule value and any heating equipment included in the unit description and available will attempt to provide enough heating to produce an outlet temperature equal to the low temperature schedule value.~ When the outdoor air temperature is at or above the high air temperature control schedule value, the outlet temperature of the unit is set to the high air temperature control schedule value and any cooling equipment included in the unit description and available will attempt to provide enough cooling to produce an outlet air temperature equal to the high temperature schedule value.~ When the outdoor air temperature is between the high and low temperature values, the unit will not provide any conditioning of outdoor air and will simply deliver it to the zone.~ Mathematically, this can be summarized as:
+
+\begin{equation}
+{T_{out}} = \left\{ {\begin{array}{*{20}{c}}{{T_{high}}\;if\;{T_{oa}} \ge {T_{high}}}\\ {{T_{oa}}\;if\;{T_{low}} < {T_{oa}} < {T_{high}}}\\ {{T_{low}}\;if\;{T_{oa}} \le {T_{low}}}\end{array}} \right.
+\end{equation}
+
+where:
+
+~~~~~ T\(_{out}\) = the outlet temperature of the zone outdoor air unit
+
+~~~~~ T\(_{oa}\) = the outside air temperature
+
+~~~~~ T\(_{high}\) = the high control air temperature schedule value
+
+~~~~~ T\(_{low}\) = the low control air temperature schedule value
+
+If the user wishes to provide ``unconditioned'' air all of the time, the high and low control temperature values can be set very high and very low, respectively, to always force the unit to provide unconditioned air.~ The same effect can also be realized by not specifying any conditioning components (such as coils) in the unit.~ The user can also limit the device to cooling only by specifying a low control temperature schedule with extremely low values.~ Conversely, the user can limit the device to heating only by specifying a high control temperature schedule with extremely high values.~ The user can also limit the equipment specified as part of the device to either cooling or heating components to get similar effects.~ In essence, the temperature control provides a variety of options in a single control type through the use of the high and low control temperature schedules.
+
+\subsection{Zone Exhaust Fan}\label{zone-exhaust-fan}
+
+The zone exhaust fan (Fan:ZoneExhaust) is a simple model to account for the fan electric energy use and impact on central air handlers from bathroom and hood exhaust.~ Because the fan only extracts air from the zone, it doesn't directly impact the zone itself.
+
+The fan flow rate is either constant or variable depending on if the user input a flow fraction modifier schedule.~~ The value entered for maximum volume flow rate is converted to a design mass flow rate using standard (altitude-adjusted) density and used as the design flow rate.~ If a flow fraction schedule is used, then its values, \({f_{Fract}}\) , are multiplied by the design flow rate to obtain the current mass flow.
+
+\begin{equation}
+{\dot m_{Des}} = {\dot V_{Max}}{\rho_{air,std}}
+\end{equation}
+
+\begin{equation}
+\dot m = {f_{Fract}}{\dot m_{Des}}
+\end{equation}
+
+The exhaust fan model is similar to, but simpler than, the models used for air system fans.~ The electric power calculation is simplified and uses a constant overall efficiency.~ All of the fan power is added to the air stream.
+
+\begin{equation}
+{\dot Q_{fan}} = \frac{{\dot m{\rm{}}\Delta P}}{{{e_{tot}}{\rho_{air}}}}
+\end{equation}
+
+\begin{equation}
+{h_{out}} = {h_{in}} + \frac{{{{\dot Q}_{fan}}}}{{\dot m}}
+\end{equation}
+
+\begin{equation}
+{w_{out}} = {w_{in}}
+\end{equation}
+
+\begin{equation}
+{T_{out}} = PsyTdbFnHW\left( {{h_{out}},{w_{out}}} \right)
+\end{equation}
+
+The controls for determining if the the exhaust fan will operate can be based on a number of factors including: an on/off availability schedule, interaction with system availability managers, minimum zone air temperature control limits and a variable flow fraction schedule.~ When the fan is coupled to the system availability managers then it will operate if either the local availability schedule or the system availability manager's indicate that the fan should run.~ When the fan is not coupled to the system availability manager, then it only uses the local availability schedule and ignores availability managers.~ If using the flow fraction schedule and the resulting flow is zero, then fan will not run.~ If using the minimum zone temperature limit schedule then the fan will only run if the fan inlet temperature is warmer than the limit.
+
+The exhaust fan's interaction with the air system depends on the value, \({f_{Bal}}\) , of the schedule for the fraction of the exhaust that is balanced.~ The model tracks the exhaust flows in two ways, balanced and unbalanced. Balanced exhaust air flow is considered to have been made up from simple airflow from infiltration, ventilation or zone mixing.~ Unbalanced exhaust air flow is considered to not be balanced by simple air flows and needs to be balanced by the air system operation.~ Both of these types of flow are summed at the zone and whole air system level.~~ In a zone, the return air node flow rate is reduced from what it would be with no exhaust by the portion of the zone's exhaust flow that is unbalanced.~ In an air handler with an outdoor air system, the outdoor air flow rate may be increased so as to be sufficient to provide all the unbalanced exhaust air for all the zones on the air handler (when possible).
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference.tex
new file mode 100644
index 00000000000..17326af2b73
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference.tex
@@ -0,0 +1,13 @@
+\chapter{Simulation Models -- Encyclopedic Reference}\label{simulation-models-encyclopedic-reference-001}
+
+The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of ``Heat Balance'', ``HVAC'', and ``Plant''.~ With the integrated solution, these designations signify where the effects of these models have their first impacts. Main Sections:
+
+\begin{itemize}
+\tightlist
+\item
+  \protect\hyperlink{Terminals}{Air Terminals}
+\item
+  \protect\hyperlink{Boilers}{Boilers}
+\item
+  \protect\hyperlink{Chillers}{Chillers} 
+\end{itemize}
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference/air-system-distribution-terminals.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference/air-system-distribution-terminals.tex
new file mode 100644
index 00000000000..27b97cafbb5
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference/air-system-distribution-terminals.tex
@@ -0,0 +1,1033 @@
+\section{Air System Distribution Terminals }\label{air-system-distribution-terminals}
+
+\subsection{Constant Volume Single Duct Uncontrolled Air Terminal}\label{constant-volume-single-duct-uncontrolled-air-terminal}
+
+The input object AirTerminal:SingleDuct:Uncontrolled provides a method for directly connecting a central air system to a thermal zone.~ Central system air is usually supplied to a zone through a terminal unit such as a single duct VAV reheat box.~ Sometimes, however, it is desirable to supply central system air directly to a zone without any zone level control or tempering.~ An example would be Furnace or Central DX equipment.~ AirTerminal:SingleDuct:Uncontrolled is the input object for a component used to pass supply air directly into a zone without any thermostatic control.~ This unit allows the program to know what zone this branch of the air system is attached to and a place to input the maximum air flow rate.~ It is typically used with an AirLoopHVAC running as a constant-volume, variable-temperature system.
+
+The AirTerminal:SingleDuct:Uncontrolled object creates the capability of supplying central system air directly to a zone and only contains the zone inlet node.~ This node is both the zone inlet node and the outlet node of the AirLoopHVAC:ZoneSplitter.~ It can be thought of as a balancing damper in the duct branch going to the zone.~ This inlet flow can be controlled by an availability schedule.~ This can be thought of as a seasonal shut off of the balancing damper.
+
+For the AirTerminal:SingleDuct:Uncontrolled objects to work correctly, it is important in any systems including them for the sum of the maximum zone air flow rates to be equal to the maximum central system flow rate.~ The zone maximum flow rates are specified in the direct air inputs.~ The central air system flow rate is specified in the AirLoopHVAC input and also in the air loop branch and central fan inputs.
+
+\subsection{Constant Volume Single Duct Reheat Air Terminal}\label{constant-volume-single-duct-reheat-air-terminal}
+
+The input object AirTerminal:SingleDuct:ConstantVolume:Reheat provides a model for single duct constant volume systems with reheat that satisfy the cooling load in a zone by changing the inlet air temperature with a reheat coil. The supply air temperature must be low enough to meet the cooling load in the zone having the greatest load. For zones with a smaller cooling load, a reheat coil is used to raise the temperature of the zone inlet air.
+
+This object can be configured with a water, steam, electric or gas reheat coil. Operation is basically the same with all coil types. The coil is controlled to raise the zone supply air temperature (i.e., the Unit Air Outlet Node temperature) to match the zone load.~ If the coil is undersized, the zone setpoint temperature will not be maintained.
+
+\begin{figure}[hbtp] % fig 153
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2788.png}
+\caption{Schematic of AirTerminal:SingleDuct:ConstantVolume:Reheat Unit \protect \label{fig:schematic-of-airterminal-singleduct}}
+\end{figure}
+
+\subsection{Variable Air Volume Single Duct Reheat and No Reheat Air Terminals}\label{variable-air-volume-single-duct-reheat-and-no-reheat-air-terminals}
+
+The VAV Single Duct Reheat and No Reheat terminal units (objects AirTerminal:SingleDuct:VAV:Reheat and AirTerminal:SingleDuct:VAV:NoReheat) provide models for single duct variable-air-volume (VAV) systems that control zone temperature primarily by varying the quantity of supply air rather than by varying the supply air temperature. The supply air temperature must be low enough to meet the cooling load in the zone having the greatest load when the zone terminal device is wide open. For zones with a smaller cooling load, the terminal device damper reduces the flow to match the zone setpoint.. If the lower flow limit on the terminal device is reached and the load is not matched, the inlet air temperature can be moderated if the terminal device has a reheat coil. In that case both the quantity of air and its temperature entering the zone are varied to meet the load. For air terminals using reheat coils, the maximum flow during reheat may be limited. Limiting the maximum flow during reheat occurs only when cooling is required (when any valid air loop cooling coil is active) and the terminal unit must reheat the air. Optional user inputs may also be used to control the amount of outdoor air entering the zone.
+
+\begin{figure}[hbtp] % fig 154
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2789.png}
+\caption{Schematic of AirTerminal:SingleDuct:VAV:NoReheat Unit \protect \label{fig:schematic-of-airterminal-singleduct-vav}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 155
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2790.png}
+\caption{Schematic of AirTerminal:SingleDuct:VAV:Reheat Unit \protect \label{fig:schematic-of-airterminal-singleduct-vav-001}}
+\end{figure}
+
+The operation of the dampers and the control are described in the section AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat and \\ AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat, which follows. The exception is that the section below describes how the air flow rate is varied for both cooling and heating. For the case of AirTerminal:SingleDuct:VAV:NoReheat and AirTerminal:SingleDuct:VAV:Reheat, air flow only varies during cooling operation and the air flow rate is set at the minimum value (minimum air flow fraction) when zone heating is required.
+
+\subsubsection{Minimum Outdoor Air Control}\label{minimum-outdoor-air-control}
+
+The single duct air terminals may also be used to provide a minimum outdoor air quantity. When the air flow rate required to meet the zone load does not provide sufficient outdoor air, the terminal device damper will open to allow sufficient outdoor air to enter the zone. In this case, the terminal damper is controlled based on the air loop's outdoor air fraction. The outdoor air may be specified as a fixed value per person, per floor area, or per zone. The minimum outdoor air may also be specified as air changes per hour. In addition, these values may be added together to provide a combined minimum outdoor air flow rate or the maximum of each of these values may be used. An outdoor air fraction schedule may also be used to modify the calculation for the minimum amount of outdoor air throughout the simulation (Ref. DesignSpecification:OutdoorAir).
+
+\subsection{Variable Air Volume Heating and Cooling Single Duct Reheat and NoReheat Air Terminal}\label{variable-air-volume-heating-and-cooling-single-duct-reheat-and-noreheat-air-terminal}
+
+\subsubsection{Overview}\label{overview-001}
+
+The VAV Heating and Cooling Single Duct Reheat and No Reheat terminal units (objects AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat and Air\-Ter\-minal:\-Single\-Duct:\-VAV:\-Heat\-And\-Cool:\-No\-Re\-heat provide models for variable-air-volume (VAV) terminal units are widely used in commercial and industrial applications. The VAV terminal units contain actuated dampers that vary the amount of central system air supplied to a zone. These terminal units may also contain a heating coil to trim the supply air temperature when overcooling is possible. The heating coil may also serve as the primary air heating source when the central system contains cooling-only equipment.
+
+The VAV terminal units described here are used primarily with central air handling equipment with cooling and heating capability. The terminal unit dampers modulate in \textbf{both} cooling and heating mode to maintain the zone setpoint temperature(s). The central air handling equipment may be either variable air volume or constant volume where a bypass duct is used to shunt excess system air flow back to the inlet of the central air handler as terminal unit dampers modulate to satisfy the zone thermostat (i.e., AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass).
+
+\subsubsection{Model Description}\label{model-description-000}
+
+The no reheat version of the single duct VAV heat and cool terminal unit contains a single virtual damper assembly and requires minimal inputs. The reheat version contains both a virtual damper assembly and an air reheat coil. Multiple reheat coil types are available:
+
+1)~~~Coil:Heating:Water
+
+2)~~~Coil:Heating:Electric
+
+3)~~~Coil:Heating:Gas
+
+4)~~~Coil:Heating:Steam
+
+Both units are simulated to provide an air flow rate sufficient to satisfy the thermostat request. The air flow rate is a function of the terminal unit's inlet air temperature and the load sensed by the thermostat. The output of the models are simply the damper position required to satisfy the zone's thermal load. Other information regarding terminal unit performance may be viewed using node report variables and heating coil report variables.
+
+\begin{figure}[hbtp] % fig 156
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2791.png}
+\caption{Schematic of AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat Unit \protect \label{fig:schematic-of-airterminal-singleduct-vav-002}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 157
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2792.png}
+\caption{Schematic of AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat Unit \protect \label{fig:schematic-of-airterminal-singleduct-vav-003}}
+\end{figure}
+
+\subsubsection{Terminal Unit Inputs}\label{terminal-unit-inputs}
+
+Both terminal unit types share several common input fields. A unique terminal unit name must be entered. A system availability schedule is also defined to allow operational control of the terminal unit. The user must then connect the unit to the air distribution system by defining the unit inlet and outlet node names. Design air flow rates are then specified: maximum total air flow rate (autosizable) and minimum air flow fraction.
+
+The reheat version of this terminal unit requires additional information. The name and type of reheat coil and the damper air outlet node name (same as reheat coil inlet node name). Maximum and minimum water flow rates are entered when a water or steam heating coil is used, as well as a control node name for actuating water-side flow rates and a convergence tolerance for iteration control.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control}
+
+The simulation begins by determining the air mass flow rate required to satisfy the heating/cooling demand.
+
+\begin{equation}
+C{p_{zone}} = PsyCpAirFnWTdb\left( {{\omega_{zone}},{T_{zone}}} \right)
+\end{equation}
+
+\begin{equation}
+C{p_{inlet}} = PsyCpAirFnWTdb\left( {{\omega_{inlet}},{T_{inlet}}} \right)
+\end{equation}
+
+\begin{equation}
+DeltaCpT = \left( {C{p_{inlet}}} \right)\left( {{T_{inlet}}} \right) - \left( {C{p_{zone}}} \right)\left( {{T_{zone}}} \right)
+\end{equation}
+
+\begin{equation}
+  \dot{m} = \min \PB{ \dot{m}_{max}, \max \PB{ \dot{m}_{max}\times MinAirFlowFrac,\frac{\dot{Q}_{zone}}{DeltaCpT} } }
+\end{equation}
+
+where
+
+\(C{p_{zone}}\) ~ = Specific heat of zone air, J/kg-K
+
+\(C{p_{inlet}}\) ~ = Specific heat of terminal unit inlet air, J/kg-K
+
+\({\omega_{zone}}\) ~~~ = Zone air humidity ratio, kg/kg
+
+\({T_{zone}}\) ~~~~ = Zone air dry-bulb temperature, °C
+
+\({\omega_{inlet}}\) ~~~ = Terminal unit inlet air humidity ratio, kg/kg
+
+\({T_{inlet}}\) ~~~~ = Terminal unit inlet air dry-bulb temperature, °C
+
+\({\dot Q_{zone}}\) ~~~ = Zone load, W (positive values denote heating, negative values denote cooling)
+
+\(\dot m\) ~~~~~~~ = Terminal unit air mass flow rate, kg/s
+
+\(PsyCpAirFnWTdb\) ~ = Psychrometric function calculating air specific heat given air humidity ratio and dry-bulb temperature
+
+\(MinAirFlowFrac\) ~~~ = User-specified zone minimum air flow fraction
+
+\({\dot m_{max}}\) ~~~~~~~~~~~~~ = Terminal unit maximum air mass flow rate, kg/s
+
+The outdoor air input fields, if entered, are then used to adjust the terminal unit air mass flow rate to ensure the correct amount of outdoor air enters the zone (within the constraints of the terminal unit maximum and minimum flow rate inputs). The amount of outdoor air is calculated per the outdoor air requirements and is adjusted by the fraction of outdoor air entering the air loop outdoor air system.
+
+\begin{equation}
+\dot m = \max \left( \dot m, \frac{\dot m_{OA}}{OAFrac} \right)
+\end{equation}
+
+where:
+
+\({\mathop m\limits^\cdot_{OA}}\) ~ = zone outdoor air flow rate, kg/s
+
+\(OAFrac\) ~ = fraction of outdoor air entering the air loop outside air system
+
+If the terminal unit is in reheat mode (i.e., the central air loop cooling coil is active, the supply air was overcooled, and the zone thermostat is requesting heating) the maximum air flow rate allowed during reheat mode is adjusted as necessary.
+
+\begin{equation}
+\mathop m\limits^\cdot  \, = \,MIN\left( {\mathop m\limits^\cdot  ,\,{{\mathop m\limits^\cdot  }_{reheat}}} \right)
+\end{equation}
+
+where:
+
+\({\mathop m\limits^\cdot_{reheat}}\) ~ = maximum air mass flow rate during reheat, kg/s
+
+The damper position is then calculated as:
+
+\begin{equation}
+FRAC_{damper} = \frac{\dot m}{\dot m_{max}}
+\end{equation}
+
+And the amount of outdoor air entering the zone is:
+
+\begin{equation}
+\dot V_{OA} = \dot m (OAFrac)
+\end{equation}
+
+where
+
+\(FRAC_{damper}\) ~ = Output variable `Zone Air Terminal VAV Damper Position', fraction of maximum flow
+
+\({\mathop V\limits^\cdot_{OA}}\) ~ = Output variable ``Zone Air Terminal Outdoor Air Volume Flow Rate'' entering the zone, m3/s
+
+Simulation of the reheat coil occurs next when applicable. The heating demand required to maintain the thermostat heating setpoint temperature and the heating capacity of air flowing through the terminal unit are used to determine the amount of reheat required.
+
+\begin{equation}
+{\dot Q_{reheat}} = {\dot Q_{heatSP}} + \dot m C_{p,zone}(T_{inlet}-T_{zone})
+\end{equation}
+
+~where
+
+\({\dot Q_{reheat}}\) ~ = Reheat coil load, W (positive values denote heating)
+
+\({\dot Q_{heatSP}}\) = Load to heating setpoint temperature, W (positive values denote heating)
+
+\subsubsection{References}\label{references-001}
+
+No specific references.
+
+\subsection{Constant Volume Single Duct Four Pipe Induction Air Terminal}\label{constant-volume-single-duct-four-pipe-induction-air-terminal}
+
+The four pipe induction terminal unit (object name: \\ AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction) is a hybrid air-hydronic unit that supplies both centrally conditioned air and local hydronic heating/cooling to a zone. Centrally conditioned air is supplied to the terminal unit at high pressure and constant flow. The central (primary) air is discharged into the terminal unit through a nozzle, inducing a fixed flow of zone (secondary) through a hydronic heating/cooling coil. The primary and secondary air streams mix and are discharged to the zone. Hot or cold water flow through the coil is varied to meet the zone heating or cooling requirement.
+
+\subsubsection{Model}\label{model}
+
+The four pipe induction terminal unit is modeled as a compound component consisting of three sub-components: a hot water coil, a chilled water coil and an air mixer. In terms of EnergyPlus objects these are \emph{Coil:Heating:Water}, \emph{Coil:Cooling:Water}, and \emph{AirLoopHVAC:ZoneSplitter}.~ The terminal unit is a forward model: its inputs are defined by the state of its inlets: namely its 2 air streams -- primary and secondary; and its two water inlets -- hot and cold. The outputs of the model are the conditions of the outlet air stream: flow rate, temperature and humidity ratio. The terminal unit data and simulation are encapsulated in the module \emph{HVACSingleDuctInduc}.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data}
+
+The user describes the terminal unit by inputting the name and type of the heating and cooling coils and the name of the zone mixer. The user must also specify the connectivity of the component by naming the inlet air and water nodes and the air outlet node. Finally maximum and fixed flow rates need to be specified (although these can be autosized): maximum and minimum hot and cold water volumetric flow rates and the total air volumetric flow rate (sum of primary and secondary flow rates). The relative convergence tolerances for the hot and cold water flow rates also need to be input (or allowed to default). Finally the induction ratio needs to be specified: this~ is defined as the ratio of the secondary air flow rate to the primary air flow rate. The relationship between the flow rates is:
+
+\begin{equation}
+{\dot m_{air,tot}} = {\dot m_{air,pri}} + {\dot m_{air,\sec }}
+\end{equation}
+
+\begin{equation}
+{\dot m_{air,sec}} = {R_{induc}}\cdot {\dot m_{air,pri}}
+\end{equation}
+
+so
+
+\begin{equation}
+{\dot m_{air,pri}} = {\dot m_{air,tot}}/(1 + {R_{induc}})
+\end{equation}
+
+\begin{equation}
+{\dot m_{air,sec}} = {\dot m_{air,tot}}\cdot {R_{induc}}/(1 + {R_{induc}})
+\end{equation}
+
+where \emph{R\(_{induc}\)} is the user-input induction ratio.
+
+All input data for the four pipe induction terminal units is stored in the array \emph{IndUnit}.
+
+\subsubsection{Calculation}\label{calculation}
+
+Given the needed inputs, the output is calculated in subroutine \emph{CalcFourPipeIndUnit}. The temperature, humidity ratio and flow rate of the primary and secondary air streams are taken from the inlet air nodes. The inlet hot and chilled water flow rates are passed in as parameters -- temperatures are taken from the inlet water nodes. Then
+
+The hot water coil is simulated (Call \emph{SimulateWaterCoilComponents);}
+
+The chilled water coil is simulated (Call \emph{SimulateWaterCoilComponents});
+
+The two air streams are mixed (Call \emph{SimAirMixer}).
+
+Finally the load met by the terminal unit is calculated and passed back to the calling routine:
+
+\begin{equation}
+{\dot Q_{out}} = {\dot m_{tot}}\cdot {c_{p,air}}\cdot ({T_{air,out}} - {T_{air,zone}})
+\end{equation}
+
+Note that data is never explicitly passed between the sub-components. This is all handled automatically by the node connections and the data stored on the nodes.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-1}
+
+From the result of the zone simulation we have the heating/cooling demand on the terminal unit \({\dot Q_{z,req}}\) . For a given hot and cold water flow \emph{CalcFourPipeIndUnit} will give us the terminal unit heating/cooling output. We need to vary the hot or cold water flow to make the unit output match the demand. To do this we need to numerically invert \emph{CalcFourPipeIndUnit}: given the output, we want one of the inputs -- the hot or cold water flow. The numerical inversion is carried out by calling subroutine \emph{SolveRegulaFalsi}. This is a general utility routine for finding the zero of a function (the \emph{residual} function) of a single independent variable. In this case the residual function calculates \(({\dot Q_{z,req}} - {\dot Q_{out}})/{\dot Q_{z,req}}\) . \emph{SolveRegulaFalsi} varies either the hot water or cold water mass flow rate to zero the residual.
+
+Decide whether the unit is on or off. The unit is off if: a) it is scheduled off; b) the inlet air mass flow rate is zero; c) the zone thermostat is in the deadband; d) or the zone heating/cooling demand is very small.
+
+If the unit is off, call \emph{CalcFourPipeIndUnit} with the hot and cold water flow rates set to their minimum flows and return.
+
+If the unit is on, check whether active heating or cooling by the hydronic coils is needed. Call \emph{CalcFourPipeIndUnit} with minimum water flows to see what how much cooling (or possibly heating) the unit is doing with primary air only. The output for this case is \({\dot Q_{pri}}\) .
+
+If \({\dot Q_{z,req}} > {\dot Q_{pri}}\) ~we need active heating. Set the cold water flow rate to the minimum. Check that the terminal unit can meet the load by setting the hot water flow rate to the maximum and calling \emph{CalcFourPipeIndUnit}. If the output is less than the zone demand we are done -- all the outputs have been calculated. Otherwise call \emph{SolveRegulaFalsi} to obtain the hot water flow rate that will make the unit output match the zone demand. This ends the unit simulation.
+
+If \({\dot Q_{z,req}} < {\dot Q_{pri}}\) we need active cooling. We set the hot water flow rate to the minimum. We check whether the terminal unit can supply the needed output by setting the cold water flow rate to the maximum and calling \emph{CalcFourPipeIndUnit.} If this maximum cooling output is not able to meet the zone cooling demand we are done. Otherwise call \emph{SolveRegulaFalsi} to obtain the cold water flow rate that will make the unit output match the zone demand. This ends the unit simulation.
+
+Note that the terminal unit output is never explicitly passed to another routine. Instead the output is saved as the outlet conditions on the terminal unit outlet air node. The node data is accessed when the terminal unit output is needed elsewhere in the program (in \emph{SimZoneAirLoopEquipment} for instance).
+
+\subsubsection{References}\label{references-1-000}
+
+No specific references.
+
+\subsection{Fan Powered Induction Series and Parallel Single Duct~ Reheat Air Terminal}\label{fan-powered-induction-series-and-parallel-single-duct-reheat-air-terminal}
+
+\subsubsection{Overview}\label{overview-1-000}
+
+The input objects AirTerminal:SingleDuct:SeriesPIU:Reheat and \\ AirTerminal:SingleDuct:ParallelPIU:Reheat provide models for fan powered induction terminal units that occur in a variety of configurations. EnergyPlus models 2 types: \emph{series} (sometimes called \emph{constant}) and \emph{parallel} (sometimes called \emph{intermittent}). The series unit provides a constant flow of air to the zone (the fan is always on at a constant flow) with a variable proportion of primary and secondary air. The parallel unit has an intermittent fan: the fan is off at maximum cooling and does not switch on until primary air flow is significantly reduced from the maximum. Once on it provides a constant flow of secondary air. Both units induce air from the zone or plenum (secondary air) and mix it with centrally conditioned supply air (primary air). Both units are variable volume: the supply air flow rate is varied to match zone conditioning requirement.
+
+\subsubsection{Model}\label{model-1}
+
+Both types of PIU are modeled as compound components. The series unit, in sequence from its inlet, consists of an air mixer, a constant volume fan, and a heating coil. In terms of EnergyPlus objects this is:
+
+1.~~~~AirLoopHVAC:ZoneMixer
+
+2.~~~~Fan:ConstantVolume
+
+3.~~~~Coil:Heating:Water, Coil:Heating:Electric, Coil:Heating:Gas or Coil:Heating:Steam
+
+The parallel unit contains a fan (in the secondary air stream, an air mixer, and a heating coil. In terms of EnergyPlus objects this is:
+
+1.~~~~Fan:ConstantVolume
+
+2.~~~~AirLoopHVAC:ZoneMixer
+
+3.~~~~Coil:Heating:Water, Coil:Heating:Electric, Coil:Heating:Gas or Coil:Heating:Steam
+
+Both units are forward models: their inputs are defined by the state of their inlets: namely the air inlet and the hot water~ inlet. The outputs of the models are the conditions of the outlet air stream: flow rate, temperature and humidity ratio. The PIUs data and simulation are encapsulated in the module \emph{PoweredInductionUnits}. The main simulation routine for the units within the module are \emph{CalcSeriesPIU} and \emph{CalcParallelPIU}.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-1}
+
+The user describes the PIU by inputting the names of the mixer, fan and heating coil sub-components plus the type of the heating coil sub-component. The user must connect the unit to the overall HVAC systems by naming various inlet and outlet nodes: the primary air inlet node, the secondary air inlet node, the unit air outlet node, and the hot water inlet node. One internal node name is needed: the coil air inlet node (same as fan outlet mode for series, mixer outlet node for parallel). Design flow rates need to be specified (although these can be autosized): maximum total air flow rate (series), maximum primary air flow rate, minimum primary air flow fraction, maximum secondary air flow rate (parallel), fan-on flow fraction (parallel), and maximum and minimum hot water flow rates. A convergence tolerance needs to be specified for units with hot water coils. There is an on/off availability schedule that need to be set.
+
+All input data for the powered induction terminal units is stored in the array \emph{PIU}.
+
+\subsubsection{Calculation}\label{calculation-1}
+
+The calculation is performed by simulating the sub-components in the order given above. Most of the code is involved with figuring out what the various flow rates should be before simulating the subcomponents. These calculations are described below.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-2}
+
+\emph{Series}
+
+From the result of the zone simulation we have the heating/cooling demand on the terminal unit \({\dot Q_{tot}}\) . The subroutine \emph{CalcSeriesPIU} needs to determine the flow rates that will allow the unit to meet this load. The first step is to determine the on/off state of the unit and determine the air flow rates.
+
+·~~~~~~~~If the unit is scheduled off, the primary and secondary flow rates are set to zero.
+
+·~~~~~~~~If there is no primary air flow (or less than .001 kg/s), the primary air flow is set to zero and the secondary air flow is set to the constant total air flow input by the user.
+
+·~~~~~~~~If the zone temperature is in the deadband or the zone load is less than 1 watt or the zone needs heating, the primary air flow rate is set to the minimum flow rate specified by the input and the secondary air flow rate is set to the difference between the fixed total air flow rate and the primary air flow rate.
+
+·~~~~~~~~Otherwise, the zone needs cooling and the unit is active.
+
+§~We determine the fan temperature rise: the secondary air flow is set to the max total air flow, primary air flow to zero, and the mixer and fan are simulated. The fan delta T is the difference between the temperature at the fan's outlet node and inlet node.
+
+§~We calculate the unit air outlet temperature needed to meet the zone cooling load: \({T_{out}} = C{p_h} + {\dot Q_{z,req}}/({\dot m_{air,tot}}\cdot {c_{p,air,z}})\)
+
+§~The temperature needed at the outlet of the mixer is then: \({T_{mix}} = {T_{out}} - \Delta {T_{fan}}\)
+
+§~We can then set the primary air flow rate.
+
+·~~~~~~~~If \({T_{mix}} \le {T_{in,pri}}\) then \({\dot m_{pri}} = {\dot m_{pri,max}}\)
+
+·~~~~~~~~else if \({T_{mix}} \ge {T_{in,pri}}\) and \({T_{mix}} \ge {T_{in,sec}}\) then \({\dot m_{pri}} = {\dot m_{pri,min}}\)
+
+·~~~~~~~~otherwise \({\dot m_{pri}} = {\dot m_{air,tot}}\cdot ({T_{in,sec}} - {T_{mix}})/({T_{in,sec}} - {T_{in,pri}})\) , subject to the constraints that the flow rate can't be bigger than the max and min allowed.
+
+The air flow rates are now determined and we can fire the air mixer (Call \emph{SimAir-Mixer}) and fan (Call \emph{SimulateFanComponents}) component simulations. Finally we simulate the heating coil:
+
+·~~~~~~~~for a hot water coil, if the coil is off (no flow, deadband, no load) just fire the coil simulation once (Call \emph{SimulateWaterCoilComponents}). Otherwise call \emph{ControlCompOutput}; \emph{ControlCompOutput} is a general component control routine. In this case it calls \emph{SimulateWaterCoilComponents} repeatedly while varying the hot water flow rate and minimizing
+
+\begin{equation}
+({c_{p,air}}\cdot {\dot m_{air,tot}}\cdot ({T_{out}} - {T_z}) - {\dot Q_{z,req}})/{\dot Q_{z,req}}
+\end{equation}
+
+to within the heating convergence tolerance.
+
+·~~~~~~~~For gas, electric or steam coils, the required coil output is set to \({\dot Q_{coil,req}} = {\dot Q_{z,req}} - {c_{p,air}}\cdot {\dot m_{air,coil}}({T_{air,coil,in}} - {T_z})\) . Then the coil simulation is fired (Call \emph{SimulateHeatingCoilComponent} or \emph{SimulateSteamCoilCompo-nents}).
+
+Finally the unit sensible output is calculated:
+
+\begin{equation}
+{\dot Q_{sens,out}} = {\rm{PsyHFnTdbW}}({T_{air,out}},{W_z}) - {\rm{PsyHFnTdbW(}}{T_z},{W_z})
+\end{equation}
+
+where \emph{PsyHFnTdb} is the EnergyPlus function giving enthalpy as a function of temperature and humidity ratio.
+
+\emph{Parallel}
+
+From the result of the zone simulation we have the heating/cooling demand on the terminal unit \({\dot Q_{tot}}\) . The subroutine \emph{CalcParallelPIU} needs to determine the flow rates that will allow the unit to meet this load. The first step is to determine the on/off state of the unit and determine the air flow rates.
+
+·~~~~~~~~If the unit is scheduled off, the primary and secondary flow rates are set to zero.
+
+·~~~~~~~~If there is no primary air flow (or less than .001 kg/s), the primary air flow is set to zero and the secondary air flow is set to the max secondary air flow input by the user.
+
+·~~~~~~~~If the zone temperature is in the deadband or the zone load is less than 1 watt or the zone needs heating, the primary air flow rate is set to the minimum flow rate specified by the input and the secondary air flow rate is set to max secondary air flow input by the user.
+
+·~~~~~~~~Otherwise, the zone needs cooling and the unit is active.
+
+§~We determine the fan temperature rise: the secondary air flow is set to the max secondary air flow, primary air flow to zero, and the fan and mixer are simulated. The fan delta T is defined as the difference between the temperature at the mixer outlet node and the fan inlet node.
+
+§~Assuming that the fan is off, we calculate the primary air flow needed to meet the cooling demand.
+
+\begin{equation}
+{\dot m_{pri}} = {\dot Q_{z,req}}/({c_{p,air}}\cdot ({T_{in,pri}} - {T_z}))
+\end{equation}
+
+The flow rate is constrained to be between the min and max primary air flow rates. If this calculated primary flow rate is greater than the fan-on flow rate, the secondary flow rate is set to zero and we are done. Otherwise, the fan is on and we need to recalculate the primary air flow rate.
+
+\begin{equation}
+{\dot m_{pri}} = ({\dot Q_{z,req}} - {c_{p,air}}\cdot {\dot m_{sec}}\cdot ({T_{in,sec}} + \Delta {T_{fan}} - {T_z}))/({c_{p,air}}\cdot ({T_{in,pri}} - {T_z}))
+\end{equation}
+
+The secondary flow rate is set to the user input fixed flow rate. The primary air flow rate is constrained to be between the min and max primary flow rated.
+
+The air flow rates are now determined and we can fire the fan (Call \emph{SimulateFanComponents}) and air mixer (Call \emph{SimAirMixer}) component simulations. Finally we simulate the heating coil:
+
+·~~~~~~~~for a hot water coil, if the coil is off (no flow, deadband, no load) just fire the coil simulation once (Call \emph{SimulateWaterCoilComponents}). Otherwise call \emph{ControlCompOutput}; \emph{ControlCompOutput} is a general component control routine. In this case it calls \emph{SimulateWaterCoilComponents} repeatedly while varying the hot water flow rate and minimizing
+
+\begin{equation}
+({c_{p,air}}\cdot {\dot m_{air,tot}}\cdot ({T_{out}} - {T_z}) - {\dot Q_{z,req}})/{\dot Q_{z,req}}
+\end{equation}
+
+to within the heating convergence tolerance.
+
+·~~~~~~~~For gas, electric or steam coils, the required coil output is set to \({\dot Q_{coil,req}} = {\dot Q_{z,req}} - {c_{p,air}}\cdot {\dot m_{air,coil}}({T_{air,coil,in}} - {T_z})\) . Then the coil simulation is fired (Call \emph{SimulateHeatingCoilComponent} or \emph{SimulateSteamCoilCompo-nents}).
+
+Finally the unit sensible output is calculated:
+
+\begin{equation}
+{\dot Q_{sens,out}} = {\rm{PsyHFnTdbW}}({T_{air,out}},{W_z}) - {\rm{PsyHFnTdbW(}}{T_z},{W_z})
+\end{equation}
+
+where \emph{PsyHFnTdb} is the EnergyPlus function giving enthalpy as a function of temperature and humidity ratio.
+
+\subsubsection{References}\label{references-2}
+
+No specific references.
+
+\subsection{Variable Air Volume Fan Powered Single Duct Air Terminal}\label{variable-air-volume-fan-powered-single-duct-air-terminal}
+
+\subsubsection{Overview}\label{overview-2-000}
+
+The input object AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan provides a model for variable speed (VS) fan VAV terminal unit that is a typical VAV reheat unit with the addition of a variable-speed blower fan to assist in moving supply air from the plenum to the conditioned zone. It is typically used with under-floor air distribution systems (UFAD) where the supply air is sent at low static pressure through an under-floor supply plenum. The fan has two maximum flow rate settings: one for cooling and one for heating. The cooling maximum is usually the actual fan maximum while the heating maximum is a lesser flow rate. The fan is upstream of the heating coil (this is a blow-through unit). The heating coil can be hot-water, electric or gas. Cooling control is obtained by varying the supply air flow rate from the cooling maximum to the minimum flow rate. Heating control is established by varying both the heating coil output (or hot water flow rate for hot water coils) and the supply air flow rate. Note that for this unit the minimum supply air flow rate is the flow rate when the fan is off.
+
+\subsubsection{Model}\label{model-2}
+
+The VS fan VAV terminal unit is modeled as a compound component consisting of two sub-components: a fan and a heating coil. In terms of EnergyPlus objects the fan is a \emph{Fan:VariableVolume} object and the heating coil is a \emph{Coil:Heating:Water}, \emph{Coil:Heating:Electric} or a \emph{Coil:Heating:Gas}. The terminal unit is a forward model: its inputs are defined by the state of its inlets: namely its air inlet and its hot water~ inlet, if it has a hot water coil. The outputs of the model are the conditions of the outlet air stream: flow rate, temperature and humidity ratio. The terminal unit data and simulation are encapsulated in the module \emph{SingleDuct}. The main simulation routine for the unit within the module is \emph{SimVAVVS}.
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-2}
+
+The user describes the terminal unit by inputting the name and type of the heating coil and the name and type of the fan. The user must also specify the connectivity of the component by naming the inlet air node; the air node connecting the fan and heating coil (fan outlet, coil inlet); the unit air outlet node (same as the zone inlet node); and hot water inlet node (if any). Maximum flow rates need to be specified (although these can be autosized): maximum cooling and heating air flow rates and the maximum hot water flow rate (if there is a hot water coil). Minimum flow rates are specified by giving by giving a minimum flow fraction for the air flow and a volumetric flow rate minimum for the hot water. For the units with hot water coils the relative convergence tolerance for the hot water flow rate also needs to be input (or allowed to default).
+
+All input data for the VS fan VAV terminal units is stored in the array \emph{Sys}.
+
+\subsubsection{Calculation}\label{calculation-2}
+
+Given the needed inputs, the output is calculated in subroutine \emph{CalcVAVVS}. The temperature and humidity of the supply air stream are taken from the inlet air node. The inlet air flow rate and the hot water flow rate are passed in as parameters. If the coil is electric or gas the coil heating power is passed instead of the hot water flow rate. Then
+
+The fan is simulated (call \emph{SimulateFanComponents}). If the fan is off the fan outlet conditions are set to the inlet conditions.
+
+The heating coil is simulated (call \emph{SimulateWaterCoilComponents} if the coil is a hot water coil; call \emph{SimulateHeatingCoilComponents} if the coil is gas or electric).
+
+Finally the sensible load met by the terminal unit is calculated and passed back to the calling routine:
+
+\begin{equation}
+{\dot Q_{out}} = {\dot m_{air}}\cdot {c_{p,air}}\cdot ({T_{air,out}} - {T_{air,zone}})
+\end{equation}
+
+Note that data is never explicitly passed between the sub-components. This is all handled automatically by the node connections and the data stored on the nodes.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-3}
+
+From the result of the zone simulation we have the heating/cooling demand on the terminal unit \({\dot Q_{tot}}\) . For the given inlet conditions \emph{CalcVAVVS} will give us the terminal unit heating/cooling output. We need to vary the air or hot water flow rate or the heating coil power (for gas or electric coils) to make the unit output match the demand. To do this we need to numerically invert \emph{CalcVAVVS}: given the output, we want one of the inputs -- the air or hot water flow rate or the heating coil power. The numerical inversion is carried out by calling subroutine \emph{SolveRegulaFalsi}. This is a general utility routine for finding the zero of a function (the \emph{residual} function) of a single independent variable. In this case the residual function calculates \(({\dot Q_{tot}} - {\dot Q_{out}})/{\dot Q_{tot}}\) . \emph{SolveRegulaFalsi} varies either the air mass flow rate, the hot water mass flow rate or the heating coil power to zero the residual.
+
+The unit is simulated in the following sequence.
+
+Decide whether the unit is on or off. The unit is off if: a) it is scheduled off; b) the inlet air mass flow rate is zero; or c) the zone thermostat is in the deadband
+
+If the unit is off, call \emph{CalcVAVVS} with flow rates set to their minimum flows and return.
+
+If the unit is on, we need to establish the boundaries of 4 conditioning regions: a) active cooling with fan on; b) active heating with fan on; c) active heating with fan off; d) passive cooling with fan off. The heating/cooling demand will fall into one of these regions. Once the correct region is determined, we will know which model input to vary for control and thus how to invert the calculation.
+
+To establish the boundaries of region a) we call \emph{CalcVAVVS} twice: once with the supply air flow rate set to the cooling maximum, once with the cooling air flow rate set to the minimum. In both cases the heating coil output is at the minimum and the fan is on. Call the 2 cooling outputs \({\dot Q_{cool,max,fanon}}\) and \({\dot Q_{cool,min,fanon}}\) . Remembering that EnergyPlus convention is that cooling loads are negative, then if \({\dot Q_{tot}} < {\dot Q_{cool,max,fanon}}\) the terminal unit can not meet the demand. Set the air mass flow rate to the cooling maximum and call \emph{CalcVAVV} again. This concludes the simulation. If~ \({\dot Q_{cool,max,fanon}} < {\dot Q_{tot}} < {\dot Q_{cool,min,fanon}}\) the cooling demand is in the active cooling region. We hold the heating at the minimum, allow the supply air flow to vary between the cooling maximum and the minimum with the fan on, and call \emph{SolveRegulaFalsi} to obtain the supply air flow rate that will produce the unit sensible cooling output that matches the demand. This concludes the simulation.
+
+To establish the boundaries of region b) call \emph{CalcVAVVS} twice: once with the supply air flow rate set to the heating maximum, once with the supply air flow rate set to the minimum. In both calls, if the heating coil is a hot water coil, the hot water flow rate is at the maximum. For electric and gas coils, the heating power is set to the maximum at maximum supply air flow and to zero at the minimum supply air flow. In both calls the fan is set to be on. Call the 2 heating outputs returned from the two calls to \emph{CalcVAVVS} \({\dot Q_{heat,max,fanon}}\) and \({\dot Q_{heat,min,fanon}}\) . If \({\dot Q_{heat,max,fanon}} < {\dot Q_{tot}}\) the terminal unit can not meet the load. Set the air flow rate to the heating maximum and the hot water flow rate or heating coil power to the maximum and call \emph{CalcVAVVS} again. This concludes the simulation for this case. If \({\dot Q_{heat,min,fanon}} < {\dot Q_{tot}} < {\dot Q_{heat,max,fanon}}\) the heating demand is in the active heating, fan on region. For a hot water coil we call \emph{SolveRegulaFalsi} with the supply air flow rate as the input that is varied and the hot water flow rate set to the maximum. For electric and gas coils the coil power and the supply air flow rate are both varied together from their minimum to maximum in a call to \emph{SolveRegulaFalsi}.~ The call to \emph{SolveRegulaFalsi} concludes the simulation for this case.
+
+This region only applies to terminal units with a hot water coil. To establish the boundaries of region c) the fan is set to off, the supply air flow rate is set to minimum flow and \emph{CalcVAVVS} is called twice: once with the hot water flow at maximum and once with the hot water flow at minimum. Call the two heating outputs \({\dot Q_{heat,max,fanoff}}\)\\
+and \({\dot Q_{tot}}\) . If \({\dot Q_{tot}}\) ~is between these values, the supply air flow rate is set to its minimum, the fan is set to off, and in the call to \emph{SolveRegulaFalsi} the hot water flow rate is varied to meet the load. This concludes the simulation for this case.
+
+If the cooling demand does not fall into cases a) -- c), the unit is assumed to be in the passive cooling state: heating is off or at the minimum, the fan is off, and the minimum supply air flow is delivered to the zone.
+
+Note that the terminal unit output is never explicitly passed to another routine. Instead the output is saved as the outlet conditions on the terminal unit outlet air node. The node data is accessed when the terminal unit output is needed elsewhere in the program (in \emph{SimZoneAirLoopEquipment} for instance).
+
+\subsubsection{References}\label{references-3}
+
+No specific references.
+
+\subsection{Four Pipe Beam Unit (AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam)}\label{four-pipe-beam-unit-airterminalsingleductconstantvolumefourpipebeam}
+
+The four pipe beam air terminal units are ceiling-mounted, beam-type units that are provided with primary air from a central system and additional heating or cooling by inducing room air to flow over a hydronic convector. They are called \emph{four pipe} because the units are connected with two pipes for chilled water supply and return and another two pipes for hot water supply and return. A simple empirical model is used to enable using input data derived from manufacturer's catalog data.
+
+\subsubsection{Model Description}\label{model-description-1-000}
+
+The model assumes that the total conditioning power, \({\dot Q_{Tot}}\) , is the sum of the conditioning provided by the primary air, \({\dot Q_{SA}}\) , and the conditioning provided by the beam convector, \({\dot Q_{Beam}}\) .
+
+\begin{equation}
+{\dot Q_{Tot}} = {{\dot Q_{SA}} + {\dot Q_{Beam}}}
+\end{equation}
+
+The primary air contribution is easily determined using
+
+\begin{equation}
+{\dot Q_{SA}} = {{\dot m_{SA}}\cdot ({c_{p,SA}} \cdot {T_{SA}} - {c_{p,Z}} \cdot {T_{Z}})}
+\end{equation}
+
+The convector power \({\dot Q_{Beam}}\) is coupled directly to the zone air heat balance (using a source code term called \emph{NonAirSysOutput}) in a way that provides only sensible heat transfer directly to the zone air node. We therefore assume that the air terminal's convector is always dry during cooling. Many of the terms used in the performance calculations are normalized by the total length of beam in zones, \({L}\) .
+
+When the unit is operated in cooling mode, the convector power is determined using the rated normalized cooling capacity that is modified by three separate functions.
+
+\begin{equation}
+{\dot Q_{Beam, cool}} = { \dot q_{cool,rated} \cdot f_{ \Delta T_{cool,mod} }() \cdot f_{\dot m_{SA,cool,mod}}() \cdot f_{\dot m_{CW,mod}}() \cdot L }
+\end{equation}
+
+The modification factor \({f_{ \Delta T_{cool,mod} }() }\) describes how the cooling capacity is adjusted to account for the temperature difference between the zone air and the chilled water entering the convector. This empirical correction factor is intended to account for how heat transfer between the chilled water and induced room air flow depends on the temperature difference, both in terms of surface convection heat transfer and the rate of induced air flow. The function can be described using any of the single-variable curves or a lookup table. The single independent variable is the ratio between the current temperature difference, \({\Delta T_{air-CW}}\) , and the temperature difference used to rate beam performance, \({\Delta T_{air-CW,rated}}\) .
+
+\begin{equation}
+{f_{ \Delta T_{cool,mod} }() } = f_{ \Delta T_{cool,mod} }\left(\frac{\Delta T_{air-CW}}{\Delta T_{air-CW,rated}}\right)
+\end{equation}
+
+\begin{equation}
+{\Delta T_{air-CW}} = {T_{Z}}-{T_{CW,in}}
+\end{equation}
+
+The modification factor \({f_{\dot m_{SA,cool,mod}}()}\) describes how the cooling capacity is adjusted to account for the primary air flow rate. This empirical correction factor is intended to account for how varying primary air flow rates will impact the rate that room air is induced to flow across the convector. The function can be described using any of the single-variable curves or a lookup table. The single independent variable is the ratio between the current normalized primary air flow rate, \({\dot m_{SA}}\) , and the normalized flow rate used to rate beam performance, \({\dot m_{SA,rated}}\) . Flow rates are normalized by dividing the total length of all the beam units in the zone. The ratio is calculated using air mass flow rates with the rated flow rate assumed to be for standard temperature and pressure at sea level so that elevation effects appear only in the numerator when the function is evaluated.
+
+\[{f_{\dot m_{SA,cool,mod}}()} = f_{\dot m_{SA,cool,mod}}\left(\frac{{\dot m_{SA}}}{{\dot m_{SA,rated}} }\right)\] \[{\dot m_{SA}} = \frac{\dot M_{SA}}{L}\] \[{\dot m_{SA,rated}} = {\dot v_{SA,rated}} \cdot {\rho_{air,STP}}\]
+
+The modification factor \(f_{\dot m_{CW,mod}}()\) describes how the cooling capacity is adjusted to account for the flow rate of chilled water through the convector. This empirical correction factor is intended to account for how varying chilled water flow rates will impact the velocity of fluid inside the pipes and the corresponding impact on the rate of surface convection heat transfer inside the convector. The function can be described using any of the single-variable curves or a lookup table. The single independent variable is the ratio between the current normalized chilled water flow rate, \({\dot m_{CW}}\) , and the normalized chilled water flow rate at the rating point, \({\dot m_{CW,rated}}\) .
+
+\[{f_{\dot m_{CW,mod}}()} = f_{\dot m_{CW,mod}}\left(\frac{{\dot m_{CW}}}{{\dot m_{CW,rated}}}\right)\] \[{\dot m_{CW}} = \frac{\dot M_{CW}}{L}\] \[{\dot m_{CW,rated}} = {\dot v_{CW,rated}} \cdot {\rho_{CW}}\]
+
+The model for when the unit is operated in heating mode is very similar. The convector power is determined using the rated normalized heating capacity that is modified by three separate functions.
+
+\begin{equation}
+{\dot Q_{Beam, heat}} = {\dot q_{heat,rated}}\cdot f_{ \Delta T_{heat,mod} }() \cdot f_{\dot m_{SA,heat,mod}}()\cdot f_{\dot m_{HW,mod}}() \cdot L
+\end{equation}
+
+The modification factor \(f_{ \Delta T_{heat,mod} }()\) describes how the heating capacity is adjusted to account for the temperature difference between the hot water and the zone air entering the convector. Notice that for heating the temperature difference is defined different from cooling operation so that positive difference values are the result. This empirical correction factor is intended to account for how heat transfer between the hot water and induced room air flow depends on the temperature difference, both in terms of surface convection heat transfer and induced air flow rates. The function can be described using any of the single-variable curves or a lookup table. The single independent variable is the ratio between the current temperature difference, \(\Delta T_{HW-air}\) , and the temperature difference used to rate beam performance, \(\Delta T_{HW-air,rated}\) .
+
+\begin{equation}
+{f_{ \Delta T_{heat,mod} }()} = f_{ \Delta T_{heat,mod} }\left(\frac{\Delta T_{HW-air}}{\Delta T_{HW-air,rated}}\right)
+\end{equation}
+
+\begin{equation}
+{\Delta T_{HW-air}} = {T_{HW,in}} -{T_{Z}}
+\end{equation}
+
+The modification factor \(f_{\dot m_{SA,heat,mod}}()\) describes how the heating capacity is adjusted to account for the primary supply air flow rate. This empirical correction factor is intended to account for how varying primary air flow rates will impact the rate that room air is induced to flow across the convector. The function can be described using any of the single-variable curves or a lookup table. The single independent variable is the same ratio described above for cooling and it is assumed that the unit can be rated using the same primary air flow rate for both heating and cooling operation of the four pipe unit. Flow rates are normalized by dividing the total length of all the beam units in the zone. The ratio is calculated using air mass flow rates with the rated flow rate assumed to be for standard temperature and pressure at sea level so that elevation effects appear only in the numerator when the function is evaluated.
+
+\begin{equation}
+{f_{\dot m_{SA,heat,mod}}()} = f_{\dot m_{SA,heat,mod}}\left(\frac{{\dot m_{SA}}}{{\dot m_{SA,rated}} }\right)
+\end{equation}
+
+The modification factor \(f_{\dot m_{HW,mod}}()\) describes how the heating capacity is adjusted to account for the flow rate of hot water through the convector. This empirical correction factor is intended to account for how varying hot water flow rates will impact the velocity of fluid inside the pipes and the corresponding impact on the rate of surface convection heat transfer inside the convector. The function can be described using any of the single-variable curves or a lookup table. The single independent variable is the ratio between the current normalized hot water flow rate, \({\dot m_{HW}}\) , and the normalized hot water flow rate at the rating point, \({\dot m_{HW,rated}}\) .
+
+\[f_{\dot m_{HW,mod}}() = f_{\dot m_{HW,mod}}\left(\frac{{\dot m_{HW}}}{{\dot m_{HW,rated}}}\right)\] \[{\dot m_{HW}} = \frac{\dot M_{HW}}{L}\] \[{\dot m_{HW,rated}} = {\dot v_{HW,rated}} \cdot {\rho_{HW}}\]
+
+Where,
+
+\({c_{p,SA}}\) Specific heat of primary air entering through the air terminal unit, in J/kg-K.
+
+\({c_{p,Z}}\) Specific heat of zone air, in J/kg-K.
+
+\({c_{p,CW}}\) Specific heat of zone air, in J/kg-K.
+
+\({f_{\dot m_{CW,mod}}()}\) Cooling capacity modification factor function of chilled water flow rate
+
+\({f_{ \Delta T_{cool,mod} }()}\) Cooling capacity modification factor function of air-water temperature difference
+
+\({f_{\dot m_{SA,cool,mod}}()}\) Cooling capacity modification factor function of primary air flow rate
+
+\({f_{\dot m_{HW,mod}}()}\) Heating capacity modification factor function of hot water flow rate
+
+\({f_{ \Delta T_{heat,mod} }()}\) Heating capacity modification factor function of water - air temperature difference
+
+\({f_{\dot m_{SA,heat,mod}}()}\) Heating capacity modification factor function of primary air flow rate
+
+\({L}\) Total length of all beam units serving the zone, in m
+
+\({\dot m_{CW}}\) Mass flow rate of chilled water per meter of length, in kg/s-m
+
+\({\dot m_{CW,rated}}\) Mass flow rate of chilled water per meter of length at rating point, in kg/s-m
+
+\({\dot m_{HW}}\) Mass flow rate of hot water per meter of length, in kg/s-m
+
+\({\dot m_{HW,rated}}\) Mass flow rate of hot water per meter of length at rating point, in kg/s-m
+
+\({\dot m_{SA}}\) Mass flow rate of primary air per meter of length, in kg/s-m
+
+\({\dot m_{SA,rated}}\) Mass flow rate of primary air per meter of length at rating point, kg/s-m
+
+\({\dot M_{SA}}\) Mass flow rate of primary air entering the zone through the air terminal unit, in kg/s
+
+\({\dot M_{CW}}\) Mass flow rate of chilled water, kg/s
+
+\({\dot M_{HW}}\) Mass flow rate of hot water, kg/s
+
+\({\dot q_{cool,rated}}\) Rated beam cooling capacity per meter of length, in W/m.
+
+\({\dot q_{heat,rated}}\) Rated beam heating capacity per meter of length, in W/m.
+
+\({\dot Q_{Beam}}\) Conditioning power delivered to the zone by the beam convector, in W.
+
+\({\dot Q_{SA}}\) Conditioning power delivered to the zone by the primary air mass flow, in W.
+
+\({\dot Q_{Tot}}\) Total (net) conditioning power delivered to zone by the air terminal unit, in W.
+
+\({\rho_{air,STP}}\) Density of air at standard conditions (sea level), in kg/m\(^{3}\)
+
+\({\rho_{air}}\) Density of air at standard conditions adjusted for elevation), in kg/m\(^{3}\)
+
+\({\rho_{CW}}\) Density of chilled water, in kg/m\(^{3}\)
+
+\({T_{SA}}\) Dryblub temperature of the (central) primary air entering the air terminal unit, in degrees C.
+
+\({T_{Z}}\) Dryblub temperature of the zone air, in degrees C.
+
+\({T_{CW,in}}\) Temperature of chilled water entering the convector, in degrees C.
+
+\({\Delta T_{air-CW}}\) Difference between the zone air temperature and chilled water entering the convector, delta degrees C.
+
+\({\Delta T_{HW-air}}\) Difference between the water and zone air temperature entering the convector, delta degrees C.
+
+\({\Delta T_{air-CW,rated}}\) Value of \({\Delta T_{air-CW}}\) at rating conditions for cooling performance, delta degrees C.
+
+\({\Delta T_{HW-air,rated}}\) Value of \({\Delta T_{HW-air}}\) at rating conditions for heating performance, delta degrees C.
+
+\({\dot v_{SA,rated}}\) Volume flow rate of air per meter length at rating point, in m\(^{3}\)/s-m.
+
+\({\dot v_{CW,rated}}\) Volume flow rate of chilled water per meter length at rating point, in m\(^{3}\)/s-m.
+
+\({\dot v_{HW,rated}}\) Volume flow rate of hot water per meter length at rating point, in m\(^{3}\)/s-m.
+
+The performance capacity model described above is controlled to modulate water flow through the beam's convector using the non-linear numerical solver in EnergyPlus called Solve Regula Falsi. The predicted zone load to setpoint \({\dot Q_{Zone, Required}}\) is adjusted by \({\dot Q_{SA}}\) to determine the required beam load.
+
+\begin{equation}
+{\dot Q_{Beam, Required}} = {\dot Q_{Zone, Required}} - {\dot Q_{SA}}
+\end{equation}
+
+When \({\dot Q_{Zone, Required}}\) is negative the beams need to provide cooling and when it is positive the beams need to provide heating. The the solver iterates the water flow rate to find a flow rate that will meet the load.
+
+When cooling, the result for beam capacity (negative for cooling) is used to calculate the leaving temperature of the chilled water using,
+
+\begin{equation}
+{T_{CW,out}} = {T_{CW,in}} - \frac{{\dot Q_{Beam}}}{{\dot m_{CW}} \cdot {c_{p,CW}} }
+\end{equation}
+
+However, to protect from a non-physical result the leaving chilled water temperature is constrained to be no warmer than a 1.0 C approach temperature compared to the zone air or the primary supply air. If the above result is too warm the leaving temperature and beam cooling capacity are adjusted using the following equations, and a recurring warning is issued to alert the user that there may be a problem with the cooliong performance input data.
+
+\[{T_{CW,out}} = { max( {T_{SA}} , {T_{Z}}) - 1.0 }\] \[{\dot Q_{Beam}} = {\dot m_{CW}} \cdot {c_{p,CW}} \cdot {( {T_{CW,in}} - {T_{CW,out}}) }\]
+
+Similarly when heating, the result for beam capacity (positive for heating) is used the calculate the leaving temperature of the hot water using,
+
+\begin{equation}
+{T_{HW,out}} = {T_{HW,in}} - \frac{{\dot Q_{Beam}}}{{\dot m_{HW}} \cdot {c_{p,HW}} }
+\end{equation}
+
+To protect from a non-physical result the leaving hot water temperature is constrained to be no cooler than a 1.0 C approach temperature compared to the zone air or the primary supply air. If the above result is too cool the leaving temperature and beam heating capacity are adjusted using the following equations, and a recurring warning is issued to alert the user that there may be a problem with the heating performance input data.
+
+\[{T_{HW,out}} = { min( {T_{SA}} , {T_{Z}}) + 1.0 }\] \[{\dot Q_{Beam}} = {\dot m_{CW}} \cdot {c_{p,CW}} \cdot {( {T_{HW,in}} - {T_{HW,out}}) }\]
+
+\subsubsection{Four Pipe Beam Sizing}\label{four-pipe-beam-sizing}
+
+The four pipe beam model has four inputs that can be autosized:
+
+\({L}\) Total length of all beam units serving the zone, in m
+
+\({\dot V_{SA,Des}}\) Design primary supply air volume flow rate, in m\(^{3}\)/s
+
+\({\dot V_{CW,Des}}\) Design chilled water volume flow rate, in m\(^{3}\)/s
+
+\({\dot V_{HW,Des}}\) Design hot water volume flow rate, in m\(^{3}\)/s
+
+Because of the way the model is formulated with defaulted inputs for rated, normalized performance data, we can link the four inputs together to ensure an internally consistent set of sizes. If any one of these four inputs is not autosized (given a fixed value at input) then the other three can be computed using the normalized, rated performance data which are either input or have default values. If the total beam length is input, then the following equations are used
+
+\[{\dot V_{SA,Des}} = {{\dot v_{SA,rated}} \cdot {L} }\] \[{\dot V_{CW,Des}} = {{\dot v_{CW,rated}} \cdot {L} }\] \[{\dot V_{HW,Des}} = {{\dot v_{HW,rated}} \cdot {L} }\]
+
+If the design primary supply air flow rate is input then the beam length can be determined as follows and then water flow rates evaluated as above.
+
+\begin{equation}
+{L} = {\frac{{\dot V_{SA,Des}}}{{\dot v_{SA,rated}}}  }
+\end{equation}
+
+If the chilled water flow rate is input, then the beam length can be determined as follows and the other values evaluated as above,
+
+\begin{equation}
+{L} = {\frac{{\dot V_{CW,Des}}}{{\dot v_{CW,rated}}}  }
+\end{equation}
+
+If the hot water flow rate is input, then the beam length can be determined as follows and the other values evaluated as above,
+
+\begin{equation}
+{L} = {\frac{{\dot V_{HW,Des}}}{{\dot v_{HW,rated}}}  }
+\end{equation}
+
+When all four inputs are autosized, which is the usual case, there is no simple way to anchor the sizes and we need to use the results from the zone and system sizing calculations to determine sizes for the four pipe beam unit. The following design data from the zone and system sizing calculations are used when sizing the four pipe beam:
+
+\({\dot V_{TU,Z,final,cool} }\) Final zone terminal unit design volume flow rate for cooling, in m\(^{3}\)/s
+
+\({\dot V_{TU,Z,final,heat} }\) Final zone terminal unit design volume flow rate for heating, in m\(^{3}\)/s
+
+\({\dot V_{Z,final,OA} }\) Final zone design volume flow rate for minimum outdoor air mechanical ventilation, in m\(^{3}\)/s.
+
+\({T_{SA,cool,design } }\) Final design zone terminal unit inlet supply air temperature at cooling peak, in degrees C.
+
+\({w_{SA,cool,design } }\) Final design zone terminal unit inlet supply air humidity ratio at cooling peak, in kg\_H2O/kg\_dryair.
+
+\({T_{Z,cool,design } }\) Final design zone air temperature at cooling peak, in degrees C.
+
+\({w_{Z,cool,design } }\) Final design zone air humidity ratio at cooling peak, in kg\_H2O/kg\_dryair.
+
+\({\dot Q_{Z,cool,design } }\) Final design zone cooling load at cooling peak, in W.
+
+\({T_{CW,design}}\) Chilled water plant loop supply side design exit temperature, in degrees C.
+
+\({T_{SA,heat,design } }\) Final design zone terminal unit inlet supply air temperature at heating peak, in degrees C.
+
+\({w_{SA,heat,design } }\) Final design zone terminal unit inlet supply air humidity ratio at heating peak, in kg\_H2O/kg\_dryair.
+
+\({T_{Z,heat,design } }\) Final design zone air temperature at heating peak, in degrees C.
+
+\({w_{Z,heat,design } }\) Final design zone air humidity ratio at heating peak, in kg\_H2O/kg\_dryair.
+
+\({\dot Q_{Z,heat,design } }\) Final design zone heating load at heating peak, in W.
+
+\({T_{HW,design}}\) Hot water plant loop supply side design exit temperature, in degrees C.
+
+Overhead beam type air terminals induce room air to flow over the convector by the directing primary supply air through special nozzles. Therefore, the cooling and heating capacity of the beam's convector is not separable from the primary flow rate, varying the primary flow rate varies the beam capacity. The design primary flow rate is chosen to be largest value that satisfies three requirements: (1) the ventilation requirement, (2) the design cooling load (if cooling is present), (3) and the design heating load (if heating is present).
+
+The sizing method here uses the non-linear solver inside EnergyPlus, called Solve Regula Falsi, to arrive at a set of sizes that meet the design load. The solver is for a single independent variable and although we have four sizes to solve for, we can reduce the problem to finding a suitable design primary supply air flow rate and then the other sizes can be determined from that as shown above. The solver needs as its input a minimum and a maximum ``x-value,'' which here is the primary supply air flow rate, and then it searches for a solution that minimizes a residual. In general the design primary supply flow rate that meets the load is somewhere between the minimum flow required for ventilation and a maximum flow where the primary supply flow meets all the zone's design load without any help from the beam's convector. For example if the supply air is cold, as it would be for latent control, and there is a cooling load then there will be a relatively large air flow rate that meets all the load without any cooling from chilled water circulating through the beam. This larger air flow serves as the upper bound for the solver.
+
+When sizing for the cooling design load, the following design values are set for use in the model calculations:
+
+\[{T_{CW,in}} = {T_{CW,design}}\] \[{\dot m_{HW}} = 0.0\] \[{T_{Z}} = {T_{Z,cool,design } }\] \[{T_{SA}} = {T_{SA,cool,design } }\] \[{c_{p,Z}} = {PsyCpAirFnWTdb ({w_{Z,cool,design } },  {T_{Z,cool,design } }  ) }\] \[{c_{p,SA}} = {PsyCpAirFnWTdb ( {w_{SA,cool,design } },  {T_{SA,cool,design } }   ) }\] \[{\dot Q_{Zone, Required}} = -1.0 \cdot {\dot Q_{Z,cool,design } }\] \[{\dot m_{SA,max limit}} = { \left(\frac{{\dot Q_{Z,cool,design } }}{{c_{p,SA}} \cdot {( {T_{Z,cool,design } } - {T_{SA,cool,design } } )}}  \right) }\] or if \(( {T_{Z,cool,design }} - {T_{SA,cool,design } } ) < 2.0\) then \[{\dot m_{SA,max limit}} = { \left(\frac{{\dot Q_{Z,cool,design } }}{{c_{p,SA}} \cdot 2.0 } \right) }\] \[{\dot m_{SA,min limit}} = min( {\dot V_{Z,final,OA} }, \frac{{\dot m_{SA,max limit}}}{3.0}, max({\dot V_{TU,Z,final,heat} } , {\dot V_{TU,Z,final,cool} }) )\]
+
+When sizing for the heating design load, the following design values are set for use in the model calculations:
+
+\[{T_{HW,in}} = {T_{HW,design}}\] \[{\dot m_{CW}} = {0.0}\] \[{T_{Z}} = {T_{Z,heat,design } }\] \[{T_{SA}} = {T_{SA,heat,design } }\] \[{c_{p,Z}} = {PsyCpAirFnWTdb ({w_{Z,heat,design } },  {T_{Z,heat,design } }  ) }\] \[{c_{p,SA}} = {PsyCpAirFnWTdb ( {w_{SA,heat,design } },  {T_{SA,heat,design } }   ) }\] \[{\dot Q_{Zone, Required}} = {\dot Q_{Z,heat,design } }\] \[{\dot m_{SA,max limit}} = { \left(\frac{{\dot Q_{Z,heat,design } }}{{c_{p,SA}} \cdot ( {T_{SA,heat,design } } - {T_{Z,heat,design }} ) } \right) }\] or if \(( {T_{SA,heat,design } } - {T_{Z,heat,design } }) < 2.0\) then \[{\dot m_{SA,max limit}} = { \left(\frac{{\dot Q_{Z,heat,design } }}{{c_{p,SA}} \cdot 2.0 } \right) }\] \[{\dot m_{SA,min limit}} = {0.0}\]
+
+The trial value for design primary supply air flow rate is used to calculate design values for length, chilled water flow, and hot water flow. \[{\dot V_{SA,Des}} = { \left(\frac{ {\dot m_{SA,trial}} }{{\rho_{air}} } \right) }\] \[{L} = {\frac{{\dot V_{SA,Des}}}{{\dot v_{SA,rated}}}  }\] \[{\dot V_{CW,Des}} = {{\dot v_{CW,rated}} \cdot {L} }\] \[{\dot V_{HW,Des}} = {{\dot v_{HW,rated}} \cdot {L} }\]
+
+The residual is calculated by evaluating the entire model to determine the total capacity for a trial flow rate (and corresponding design length and maximum water flow rates) and comparing it to the design load. \[{residuum} = \left(\frac{ ({\dot Q_{Zone, Required}} - {\dot Q_{Tot}} )}{{\dot Q_{Zone, Required}}}\right)\]
+
+After the solvers have run and the final sizes for the four pipe beam have been determined, there is one more step taken to make further adjustments in the central sizing data structures for sizing air system components. The usual methods of sizing the main AirLoopHVAC branch and fans are not able account for the methods used to size the four pipe beam. When the Sizing:System object was set to use \emph{VentilationRequirement}, the air handler will be too small. When the Sizing:System object was set to use \emph{Sensible}, the air handler will be too large. The system sizing calculations have already been completed at the time the four pipe beam air terminals are sized so we need to make some adjustments. The final primary supply air flow rate size is compared to the original final zone sizes for the air terminal unit and the air loop sizes adjusted to make up for the difference. A sizing report item called ``AirLoopHVAC Design Supply Air Flow Rate Adjustment {[}m3/s{]}'' is generated for each four pipe beam that shows the magnitude of the adjustment to data structure values used to size central air systems. Therefore when autosizing air handlers with four pipe beams, it is expected that the outcomes for air system sizes will not agree with the system sizing reporting because of the differences introduced by this adjustment.
+
+\subsubsection{Developing Model Input From Catalog Data}\label{developing-model-input-from-catalog-data}
+
+An example is presented showing how manufacturer's data can be converted into the input data for the proposed model. The following example is for a Trox active DID632A product with a type ``H'' nozzle, where the rating point has been chosen based on a 6 foot active length and 140 CFM primary rate with other rating conditions as listed in the catalog data. The EnergyPlus IDF input for this example is show as the example in the in the Input Output reference description of the four pipe beam.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/TroxDID632A_Tabledata.png}
+\caption{FourPipeBeam/tableData}
+\end{figure}
+
+Snippet of catalog data for capacity and primary air flow rate dependence (Trox DID632A)
+
+Choosing a 6 foot beam (with Nozzle type H) at 140 CFM as the rating point, we get 3726 Btu/h = 1092 W, 6 ft = 1.83 m, and 1092/1.83 = 597 W/m for normalized beam cooling capacity at rating point. The associated primary air flow rate of 140 ft\(^{3}\)/min = 0.066 m\^{}3/s and 0.066/1.83 = 0.036 m\(^{2}\)/s is the normalized beam primary air flow rate at the rating point. Note that because the flow rate is normalized by beam length, the units are m\(^{3}\)/s/m (which reduces to m\(^{2}\)/s). The rating heating capacity is listed as a ``net'' heating rate but since this is not well defined in the catalog we go ahead and assume that this represents the beam heating rate where the associated cooling provided by the primary air has already been subtracted. The net heating capacity is 7411 Btu/h = 2172 W. This value need to be increased by the primary cooling provided by 55 F = 12.7 C air entering a zone at 70 F = 21 C. The catalog does not completely define the moist air state of the zone nor the primary air so we assume nominal average moist air density of 1.2 kg/m\(^{3}\) and a specific heat of 1000.0 J/kg-C so that the primary air cooling rate is (21 -- 12.7) * 0.066 * 1.2 * 1000 = 660 W. The beam heating rate is therefore 2172 + 660 = 2832 W. Then normalizing for beam length 2832/1.83 = 1548 W/m is the rated beam heating capacity.\\
+The catalog includes two more data points for capacity at different flow rates, one for 100 ft\(^{3}\)/min and the other for 180 ft\(^{3}\)/min. These are processed in the same way as the rating point data and used to create the modification curves that describe performance as a function of primary air flow rate.
+
+\subsection{Cooled Beam Unit (AirTerminal:SingleDuct:ConstantVolume:CooledBeam)}\label{cooled-beam-unit-airterminalsingleductconstantvolumecooledbeam}
+
+Cooled beam (frequently called chilled beams) systems are usually hybrid water -- air systems. Commonly there is a constant flow, fixed temperature central forced air system for meeting ventilation and latent load requirements.~ Sometimes this forced air system's flow rate is varied according to ventilation demand; and of course its supply air temperature could be reset in various ways. Sensible cooling load is met by the cooled beam units; these are ceiling suspended units with cool water circulating through them. Some types of units are ``passive'' -- they cool by radiation and natural convection. Other types of units are ``active'' and act as supply air terminal units with the supply air inducing room air over the beam cooling elements. These units cool almost entirely by convection. The DOE-2 model (upon which this model is based) is a convection only model -- even the ``passive'' units are assumed to operate 100\% convectively. The cooled beam elements act as an alternative to normal ceiling radiant cooling: they are not coupled to the building mass and they operate more in a convective mode, but they can, like radiant cooling, use fairly warm cooling water.
+
+Heating is accomplished separately from the cooled beam system -- usually baseboards are used on the building perimeter to meet heating loads.
+
+\subsubsection{Model}\label{model-3}
+
+The chilled beam system is modeled as an EnergyPlus terminal unit. In terms of configuration within the overall HVAC system it will resemble a 4 pipe induction terminal unit. The user describes the system as a typical single duct constant volume system (with outside air mixer, fan, heating and cooling coils) on the air loop side, and with cooled beam terminal units on the zone equipment side.
+
+The model is an empirical model developed at the equipment manufacturer Halton Oy. It consists of the following relationships.
+
+\emph{P\(_{beam}\)} = \emph{A·K·DT~~~~~~~} ~~~~~~~~~~~~~~~~~~~~~~~ beam cooling output per unit length W/m
+
+\emph{K = a·DT\(^{n1}\)·vr\(^{n2}\)·w\(^{n3}\)}~~~~~~~~~~~~~~~~~~~~~~~~~~~ coil heat transfer coefficient W/(m\(^{2}\)K)
+
+\emph{vr = (q\(_{in}\)}/a\emph{\(_{0}\))·r\(_{air}\)}~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ room air mass flow rate across coil kg/(m\(^{2}\)s)
+
+\emph{q\(_{in}\) = K\(_{1}\)·DT\(^{n}\)+K\(_{in}\)·q\(_{pr}\)}~~~~~~~~~~~~~~~~ ~~~~~~~~~~~ room air volumetric flow rate across coil per
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ unit length m\(^{3}\)/(s-m)
+
+DT is the room air --water temperature difference (average water temperature is used) in degrees C.
+
+w is the water velocity in m/s.
+
+q\(_{pr}\) is the supply air flow rate per unit length m\(^{3}\)/(s-m)
+
+The other symbols are the model parameters input by the user (see the IO Ref for descriptions).
+
+\subsubsection{Inputs and Data}\label{inputs-and-data-3}
+
+The user describes the unit by inputting the name, referencing an availability schedule, and choosing a type (\emph{active} or \emph{passive}). The user must also specify the connectivity of the component by naming the inlet and outlet air and water nodes. The maximum water and fixed air flow rates need to be specified (although these can be autosized). The design inlet and outlet water temperatures are inputs. Generally the inlet water temperature is quite warm (15C is the default) and the temperature rise is small (design outlet water temperature defaults to 17C). Two key inputs are the number of beams (in the zone) and the beam length. It is generally wise to let these inputs autosize.
+
+The remaining inputs are parameters specific to the product model. Good defaults are supplied and they should not be changed without information from the manufacturer.
+
+\subsubsection{Sizing}\label{sizing}
+
+The Cooled Beam sizing calculations generally follow the procedures used for other terminal units (see \emph{Loop Equipment Sizing}). One difference is that the Cooled Beams use the Cooled Beam inputs \emph{Design Inlet Water Temperature} and \emph{Design Outlet Water Temperature} for the chilled water DT rather than the DT from Plant Sizing. There are also two inputs unique to the Cooled Beam units that are autosized and will be described here.
+
+The input \emph{Number of individual beam units in the zone} is autosized by dividing the beam system zone design chilled water flow rate (either input by the user or autosized) by a nominal chilled water beam flow rate: 0.07 kg/s.
+
+The input \emph{Length of an individual beam unit} is autosized by using the model equations to calculate the length. The inputs to the equations are:
+
+1)~~~~the design load per beam. The design load is calculated from the design water mass flow rate and the design water inlet and outlet temperatures. The design load is divided by the number of beams to obtain the design load per beam.
+
+2)~~~~The design air supply air flow per beam -- obtained by dividing the design supply air flow by the number of beams.
+
+3)~~~~The design water flow per beam (m\(^{3}\)/s) -- obtained by dividing the design water flow by the number of beams.
+
+4)~~~~The design water velocity -- obtained by dividing the design water flow per beam by the cross sectional inside area of a water tube (pD\(^{2}\)/4, where D is the input \emph{Pipe inside diameter}.
+
+5)~~~~Average air to water \emph{DT = T\(_{z,\, cool\, peak}\)} - \emph{0.5(T\(_{w,des\, inlet}\)} \emph{+ T\(_{w,des\, outlet}\))}; where~~~~~~~ \emph{T\(_{z,\, cool\, peak}\)} is the zone air temperature at the cooling peak and the \emph{T\(_{w,des}\)} `s are the water design inlet and outlet temperatures.
+
+With these inputs the model equations can be solve directly for beam length for passive cooled beams, and iteratively for active cooled beams.
+
+\subsubsection{Calculation}\label{calculation-3}
+
+The subroutine \emph{CalcCoolBeam} ~uses the model equations to calculate the cooling power \emph{P\(_{beams,out}\)} delivered to the room air and the outlet water temperature given the water flow rate (and the room air temperature and water inlet temperature). Since the model equations are nonlinear they must be solved iteratively. The subroutine does this by varying the outlet water temperature \emph{T\(_{w,out}\)} and calculating the water-side cooling power
+
+P\(_{w}\) = q\(_{w,beam}\)·c\(_{p,w}\)·(T\(_{w,out}\)-T\(_{w,in}\))
+
+and comparing it to the air-side cooling power
+
+P\(_{air}\) = K·A·DT·L\(_{beam}\)
+
+where \emph{q\(_{w,beam}\)} is the water mass flow rate (kg/s) per beam and \emph{L\(_{beam}\)} is the length of a beam (m). When \emph{P}\(_{w}\) ~and \emph{P\(_{air}\)} match to within 0.1 W the subroutine terminates the iteration.
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-4}
+
+From the result of the zone simulation we have the heating/cooling demand for the zone equipment. For the cooling demand, we use the load to cooling set point \emph{P\(_{c}\)}. Part of the demand may be satisfied by the zone supply air:
+
+P\(_{sup}\) = q\(_{air}\)·(c\(_{p,air,sys}\)·T\(_{sys}\) - c\(_{p,air,z}\)·T\(_{z}\))
+
+The demand on the actual beams is then
+
+P\(_{beams,dem}\) = P\(_{c}\) - P\(_{sup}\)
+
+We want to know the chilled water flow rate that will give a beam cooling output of \emph{P\(_{beams}\)}. To obtain this we need to numerically invert \emph{CalcCoolBeam}: given its desired output, we want to know the chilled water flow rate. This numerical inversion is carried out by calling the subroutine \emph{SolveRegulaFalsi}. This is a general utility routine for finding the zero of a function (the \emph{residual} function) of a single independent variable. In this case the residual function is basically
+
+(P\(_{beams,out}\)-P\(_{beams,dem}\))/P\(_{beams,out,max}\)
+
+\emph{SolveRegulaFalsi} varies the cold water mass flow rate to zero the residual. The water inlet and outlet node flow rates are set to the flow rate found by \emph{SolveRegulaFalsi} and the water outlet node temperature is set to the outlet water temperature from \emph{SolveRegulaFalsi}.
+
+\subsubsection{References}\label{references-4}
+
+Documentation Package Update \#2 for DOE-2.1E, Version 107, page 3.152 describes the input and the model for the DOE-2 cooled beam model.
+
+\subsection{Constant Volume Dual Duct Air Terminal}\label{constant-volume-dual-duct-air-terminal}
+
+\subsubsection{Overview}\label{overview-3-000}
+
+The input object AirTerminal:DualDuct:ConstantVolume provides a model for dual duct constant-air-volume (DDCAV) systems that are typically used in special applications where precise temperature and humidity control are required and energy efficiency is not of primary concern. Thermal control for each zone is achieved by mixing air from the hot deck with air from the cold deck to achieve a supply air temperature that will exactly meet the zone load and satisfy the zone thermostat demand. Each zone has its own mixing box which is connected directly to the hot and cold decks. The mixing box dampers change the relative amount of hot and cold air that will be delivered (at a constant volumetric flow rate) to the zone.
+
+\subsubsection{Model Description}\label{model-description-2-000}
+
+The DDCAV model will attempt to meet all of the thermostatic loads of a particular zone by explicitly calculating the hot and cold deck mass flow rates. For the energy and mass balance equations shown below, the zone load, temperatures, specific heats and the design mass flow rate are all known. These equations can then be solved directly for the hot deck and cold deck mass flow rates.
+
+\begin{equation}
+\dot Q_{zone} = \dot m_c C_{p,c} T_c + \dot m_h C_{p,h}T_h - \dot m_d C_{p,z} T_z
+\end{equation}
+
+\begin{equation}
+\dot m_d = \dot m_c + \dot m_h
+\end{equation}
+
+Where:
+
+\(\dot Q_{zone}\) = Zone load, W (positive = heating, negative = cooling)
+
+\(C{p_z}\) = Specific heat of zone air, J/kg-K
+
+\(C{p_c}\) = Specific heat of cold deck air, J/kg-K
+
+\(C{p_h}\) = Specific heat of hot deck air, J/kg-K
+
+\({T_z}\) = Zone air dry-bulb temperature, °C
+
+\({T_c}\) = Cold deck air dry-bulb temperature, °C
+
+\({T_h}\) = Hot deck air dry-bulb temperature, °C
+
+\({\dot m_d}\) = System design air mass flow rate through both heating or cooling duct, kg/s
+
+\({\dot m_c}\) = Cold deck air mass flow rate, kg/s
+
+\({\dot m_h}\) = Hot deck air mass flow rate, kg/s
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-5}
+
+The simulation first calculates the hot deck and cold deck air mass flow rates required to satisfy the heating/cooling demand on the zone. Once the individual flow rates have been calculated based on temperature control, the zone mixed air conditions are calculated assuming adiabatic mixing of the two air streams.
+
+\subsection{Variable Air Volume Dual Duct Air Terminal}\label{variable-air-volume-dual-duct-air-terminal}
+
+\subsubsection{Overview}\label{overview-4-000}
+
+The input object AirTerminal:DualDuct:VAV provides a model for dual duct variable-air-volume (DDVAV) systems that are typically used in special applications where both temperature and humidity control as well as energy efficiency are of primary concern.~ This system combines the advantages of the standard dual duct system for better thermal control with the possibility to reduce fan energy using a variable speed fan. The DDVAV terminal units contain actuated dampers that vary the amount of central system air supplied to a zone from both the hot and cold deck. Optional user inputs may also be used to control the amount of outdoor air entering the zone.
+
+The DDVAV terminal units described here are used primarily with central air handling equipment with cooling and heating capability. The terminal unit dampers modulate the amount of cold air and hot air as well as the overall flow rate to maintain the zone setpoint temperature(s).
+
+\subsubsection{Model Description}\label{model-description-3-000}
+
+The DDVAV model will attempt to meet all of the thermostatic loads of a particular zone by first sending air through either the heating duct or the cooling duct depending on whether there is a heating or cooling load (respectively).~ Flow rate through the opposite duct is kept at zero and flow through the active duct is varied between the minimum air flow rate (minimum zone air fraction multiplied by the maximum flow rate) and the maximum air flow rate.~ If the flow rate to meet the load through either the heating or cooling duct results in a flow outside these ranges, then air must be passed through the other duct as well to avoid over- or under-heating or --cooling. This is done using a conservation of energy and mass analysis of the terminal unit as well as the known inlet and necessary outlet condition to meet the thermal needs of the zone.
+
+When there is no load on the zone, the system could either be scheduled off or be in a ``no load'' condition.~ If the system is scheduled off, the model keeps the flow rate at zero for both the heating and cooling duct.~ If in a no load condition, the system attempts to throttle back to the minimum possible flow and then find a balance between flow through the heating and cooling duct that will provide no net conditioning to the space.~ This means that the enthalpy of air delivered to the space must be equal to the enthalpy of the (average) air in the zone.
+
+\subsubsection{DDVAV Terminal Unit Inputs}\label{ddvav-terminal-unit-inputs}
+
+Like other terminal units, the DDVAV terminal unit requires an availability schedule and inlet and outlet node designations.~ The DDVAV terminal unit, like the DD terminal unit, has two inlet nodes (one for the heating duct and one for the cooling duct) and one outlet node.
+
+In addition, the DDVAV terminal unit also has a maximum flow rate and a minimum flow fraction like the VAV terminal unit.~ This allows the flow to be throttled back when it is possible to provide the proper amount of conditioning with less flow.~ The maximum flow rate can be auto-sized, if desired.
+
+\subsubsection{Minimum Outdoor Air Control}\label{minimum-outdoor-air-control-1}
+
+This dual duct air terminal may also be used to provide a minimum outdoor air quantity. When the air flow rate required to meet the zone load does not provide sufficient outdoor air, the terminal device damper will open to allow sufficient outdoor air to enter the zone. In this case, the terminal damper is controlled based on the air loop's outdoor air fraction. The outdoor air may be specified as a fixed value per person, per floor area, or per zone or as the required minimum air changes per hour. In addition, these values may be added together to provide a combined minimum outdoor air flow rate or the maximum of each of these values may be used. An outdoor air fraction schedule may also be used to modify the calculation for the minimum amount of outdoor air throughout the simulation (Ref. DesignSpecification:OutdoorAir).
+
+\subsubsection{Simulation and Control}\label{simulation-and-control-6}
+
+The simulation begins by determining the air mass flow rate required to satisfy the heating/cooling demand using either the heating duct or cooling duct.
+
+\begin{equation}
+C{p_{zone}} = \dot m\left( {C{p_{inlet}},{T_{zone}}} \right)
+\end{equation}
+
+\begin{equation}
+C{p_{zone}} = PsyCpAirFnWTdb\left( {{T_{zone}},{T_{inlet}}} \right)
+\end{equation}
+
+\begin{equation}
+DeltaCpT = \left( {C{p_{inlet}}} \right)\left( {{T_{inlet}}} \right) - \left( {C{p_{zone}}} \right)\left( {{T_{zone}}} \right)
+\end{equation}
+
+\begin{equation}
+\dot m = \min \left( \dot m_{max}, \max \left( \dot m_{max}\cdot MinAirFlowFrac,\frac{\dot Q_{zone}}{DeltaCpT} \right) \right)
+\end{equation}
+
+where
+
+\(C{p_{zone}}\) ~ = Specific heat of zone air, J/kg-K
+
+\(C{p_{inlet}}\) ~ = Specific heat of terminal unit inlet air, J/kg-K
+
+\({\omega_{zone}}\) ~~~ = Zone air humidity ratio, kg/kg
+
+\({T_{zone}}\) ~~~~ = Zone air dry-bulb temperature, °C
+
+\({\omega_{inlet}}\) ~~~ = Terminal unit inlet air humidity ratio, kg/kg
+
+\({T_{inlet}}\) ~~~~ = Terminal unit inlet air dry-bulb temperature, °C
+
+\(\dot m\) ~~~ = Zone load, W (positive values denote heating, negative values denote cooling)
+
+\(PsyCpAirFnWTdb\) ~~~~~~~ = Terminal unit air mass flow rate through either heating or cooling duct, kg/s
+
+\(MinAirFlowFrac\) ~~~~~~~~~~ = Psychrometric function calculating air specific heat given air humidity ratio and dry-bulb temperature
+
+\(MinAirFlowFrac\) ~~~ = User-specified zone minimum air flow fraction
+
+\({\dot m_{max}}\) ~~~~~~~~~~~~~ = Terminal unit maximum air mass flow rate, kg/s
+
+The outdoor air input requirements, if entered, are then used to adjust the terminal unit air mass flow rate to ensure the correct amount of outdoor air enters the zone (within the constraints of the terminal unit maximum and minimum flow rate inputs). The amount of outdoor air is calculated per the outdoor air requirements and is adjusted by the fraction of outdoor air entering the air loop outdoor air system.
+
+\begin{equation}
+  \dot{m} = \max\PB{ \dot{m}, \frac{\dot{m}_{OA}}{OAFrac} }
+\end{equation}
+
+where:
+
+\({\mathop m\limits^\cdot_{OA}}\) ~ = zone outdoor air flow rate, kg/s
+
+\(OAFrac\) ~ = fraction of outdoor air entering the air loop outside air system
+
+The damper position is then calculated as:
+
+\begin{equation}
+  FRAC_{damper} = \frac{\dot{m}}{\dot{m}_{max}}
+\end{equation}
+
+where
+
+\(FRA{C_{damper}}\) ~ = Output variable `Zone Air Terminal VAV Damper Position', fraction of maximum flow
+
+If the flow rate was between the maximum flow rate and the minimum flow rate for the terminal unit, then no other calculations are needed.~ However, if the flow was reset to either the maximum or minimum flow rate, then flow through the active duct must be balanced by flow through the other duct to achieve the proper conditioning.
+
+\subsubsection{References}\label{references-5}
+
+No specific references.~ Refer to the ASHRAE Handbook series for general information on different system types as needed.
+
+\subsection{Dual Duct Dedicated Outside Air Terminal with VAV Cooling}\label{dual-duct-dedicated-outside-air-terminal-with-vav-cooling}
+
+\subsubsection{Overview}\label{overview-5-000}
+
+The input object AirTerminal:DualDuct:VAV:OutdoorAir provides a model for dedicated outside air combined with recirculated air for cooling.~ This air terminal has two inlets and one outlet. The outdoor air inlet has one damper that is controlled to meet the air flow requirements for ventilation.~ The second inlet is for cool recirculated air and has a second damper that is controlled to meet the zone's cooling loads.~ The two streams are then mixed and inlet to the zone.~ This unit is for central air systems (using AirLoopHVAC object). ~Because of the limitation in EnergyPlus of allowing only one air terminal per zone, the dual duct approach offers advantages in that it allows modeling dedicated outdoor air systems (DOAS) and central VAV cooling at the same time.~ The original motivation for adding this terminal was to model twin-fan, twin-coil systems.
+
+The recirculated cool air duct is actually optional. If no node name is input for the recirculated air inlet node, then only the outdoor air duct is operational and the air terminal behaves as a single duct.~ This offers additional capabilities for single duct DOAS in that this terminal can request outdoor air flows that change over time but are not controlled to meet zone loads.
+
+\subsubsection{Model Description}\label{model-description-4-000}
+
+The model attempts to meet the ventilation requirements and the cooling loads of a particular zone.~ If the zone requires heating, ancillary heating equipment is needed as this terminal cannot do any heating.~ The model first determines the current required outdoor air flow rate for ventilation and then calculates the flow of cool air needed to reach the cooling setpoint.
+
+The outdoor air rate is controlled by the schedule and specifications contained in a DesignSpecification:OutdoorAir object and can be based on flows per person, per zone, per area, or air changes per hour.~ Using the key CurrentOccupancy, the per person rate can be set to operate based on the current occupancy level to model demand controlled ventilation. Using the key DesignOccupancy it can be set to operate based on the design, or maximum, level of occupancy.~~ The outdoor air inlet side of the terminal is assigned a design maximum flow rate based on the largest flow rates specified by the associated DesignSpecification:OutdoorAir object. This maximum for the outdoor air is used to calculate the damper position and contributes to the overall maximum if that is autosized.
+
+The recirculated cool air flow rate is controlled to meet the zone cooling loads.~ The first step is to calculate the impact that the outdoor air flow has on the loads starting with the specific heats.
+
+\begin{equation}
+{c_{p,zone}} = PsyCpAirFnWTdb\left( {{\omega_{zone}},{T_{zone}}} \right)
+\end{equation}
+
+\begin{equation}
+{c_{p,OA}} = PsyCpAirFnWTdb\left( {{\omega_{OA}},{T_{OA}}} \right)
+\end{equation}
+
+\begin{equation}
+{c_{p,RC}} = PsyCpAirFnWTdb\left( {{\omega_{RC}},{T_{RC}}} \right)
+\end{equation}
+
+where,
+
+\(c_{p,zone}\) = \$ ~specific heat of zone air being served by the terminal unit, J/kg-K
+
+\(c_{p,OA}\) = \$ ~specific heat of outdoor air entering the terminal unit, J/kg-K
+
+\(c_{p,RC}\) = \$ ~specific heat of the recirculated (cool) air entering the terminal unit (if present), J/kg-K
+
+\(\omega_{zone}\) = \$ humidity ratio of the zone air, kg/kg
+
+\(\omega_{OA}\) = \$ humidity ratio of the outdoor air entering the terminal unit, kg/kg
+
+\(\omega_{RC}\) = \$ humidity ratio of the recirculated air entering the terminal unit, kg/kg
+
+\(T_{zone}\) = \$ air drybulb temperature of the zone, ºC
+
+\(T_{OA}\) = \$ air drybulb temperature of the outdoor air entering the terminal unit, ºC
+
+\(T_{RC}\) = \$ air drybulb temperature of the recirculated cool air entering the terminal unit, ºC
+
+\(PsyCpAirFnWTdb\) ~is a psychrometric function for calculating the specific heat of moist air as a function of humidity ratio and drybulb temperature.
+
+The contribution to zone load provided by the outdoor air toward meeting the cooling setpoint, \({\dot Q_{OA}}\) ~(W), is then calculated using:
+
+\begin{equation}
+{\dot Q_{OA}} = {\dot m_{OA}}\left( {{c_{p,OA}}{T_{OA}} - {c_{p,zone}}{T_{zonesetpoint}}} \right)
+\end{equation}
+
+where,
+
+$\dot{m}_{OA} =$ is the mass flow rate of outdoor air determined by the outdoor air requirement, kg/s
+
+$T_{zonesetpoint} =$ is the zone cooling setpoint drybulb temperature, ºC
+
+This is then used to calculate the load that the recirculated cool air should deliver, \({Q_{RC}}\) ~(W):
+
+\begin{equation}
+{\dot Q_{RC}} = {\dot Q_{ToCoolSetpointRemain - }}{\dot Q_{OA}}
+\end{equation}
+
+where,
+
+\({\dot Q_{ToCoolSetpointRemain = }}\) ~is the remaining load to cooling setpoint as determined by Predictor and including the impacts of any other zone equipment sequenced before this terminal. Then the recirculated cool air mass flow rate, \({\dot m_{RC}}\) ~(kg/s), is calculated using:
+
+\begin{equation}
+{\dot m_{RC}} = \frac{{{{\dot Q}_{RC}}}}{{\left( {{c_{p,RC}}{T_{RC}} - {c_{p,zone}}{T_{zone}}} \right)}}
+\end{equation}
+
+The model also includes a form of damping where the last three values for \({\dot m_{RC}}\) ~are stored and used to detect if the solution is oscillating from one iteration to the next and if it is then the new value is not used but rather the value from the previous iteration is used.~ Once the two mass flows are known, the moist air properties of the outlet node are calculated using mass flow weighting.
+
+\subsubsection{References}\label{references-6}
+
+Sekhar, S. C., K. W. Tham, et al. (2004). Development of energy-efficient single-coil twin-fan air-conditioning system with zonal ventilation control, Nashville, TX, United states, Amer. Soc. Heating, Ref. Air-Conditoning Eng. Inc.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference/boilers.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference/boilers.tex
new file mode 100644
index 00000000000..68170d66c72
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference/boilers.tex
@@ -0,0 +1,316 @@
+\section{Boilers }\label{boilers}
+
+\subsection{Simple Hot Water Boiler}\label{simple-hot-water-boiler}
+
+The input object Boiler:HotWater provides a simple model for boilers that only requires the user to supply the nominal boiler capacity and thermal efficiency. An efficiency curve can also be used to more accurately represent the performance of non-electric boilers but is not considered a required input. The fuel type is input by the user for energy accounting purposes.
+
+The model is based the following three equations
+
+\begin{equation}
+OperatingPartLoadRatio = \frac{{BoilerLoad}}{{BoilerNomCapacity}}
+\end{equation}
+
+\begin{equation}
+TheoreticalFuelUse = \frac{{BoilerLoad}}{{NominalThermalEfficiency}}
+\end{equation}
+
+\begin{equation}
+FuelUsed = \frac{{TheoreticalFuelUse}}{{BoilerEfficiencyCurveOuput}}
+\end{equation}
+
+-or-
+
+\begin{equation}
+FuelUsed = \frac{{BoilerLoad}}{{\left( {NominalThermalEfficiency} \right)\left( {BoilerEfficiencyCurveOutput} \right)}}
+\end{equation}
+
+The final equation above includes the impact of the optional boiler efficiency performance curve. To highlight the use of the normalized boiler efficiency curve, the fuel use equation is also shown in an expanded format. The normalized boiler efficiency curve represents the changes in the boiler's nominal thermal efficiency due to loading and changes in operating temperature. If the optional boiler efficiency curve is not used, the boiler's nominal thermal efficiency remains constant throughout the simulation (i.e., BoilerEfficiencyCurveOutput = 1).
+
+When a boiler efficiency performance curve is used, any valid curve object with 1 or 2 independent variables may be used. The performance curves are accessed through EnergyPlus' built-in performance curve equation manager (curve objects). The linear, quadratic, and cubic curve types may be used when boiler efficiency is solely a function of boiler loading, or part-load ratio (PLR). These curve types are used when the boiler operates at the specified setpoint temperature throughout the simulation. Other curve types may be used when the boiler efficiency can be represented by both PLR and boiler operating temperature. Examples of valid single and dual independent variable equations are shown below. For all curve types, PLR is always the x independent variable. When using curve types with 2 independent variables, the boiler water temperature (Twater) is always the y independent variable and can represent either the inlet or outlet temperature depending on user input.
+
+\subsubsection{Single independent variable:}\label{single-independent-variable}
+
+\begin{itemize}
+\item
+  \(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right)\) ~(Linear)
+\item
+  \(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right) + C3{\left( {PLR} \right)^2}\) (Quadratic)
+\item
+  \(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right) + C3{\left( {PLR} \right)^2} + C4{(PLR)^3}\) (Cubic)
+\end{itemize}
+
+\subsubsection{Dual independent variables:}\label{dual-independent-variables}
+
+\begin{itemize}
+\item
+  \(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right) + C3{\left( {PLR} \right)^2} + \left( {C4 + C5\left( {PLR} \right) + C6{{\left( {PLR} \right)}^2}} \right)\left( {Twater} \right)\) (QuadraticLinear)
+\item
+  \(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right) + C3{\left( {PLR} \right)^2} + C4\left( {Twater} \right) + C5{(Twater)^2} + C6(PLR)(Twater)\) ~(Biquadratic)
+\item
+  \(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right) + C3{\left( {PLR} \right)^2} + C4\left( {Twater} \right) + C5{(Twater)^2} + C6\left( {PLR} \right)\left( {Twater} \right) + C7{(PLR)^3} + C8{(Twater)^3} + C9{\left( {PLR} \right)^2}\left( {Twater} \right) + C10\left( {PLR} \right){(Twater)^2}\) (Bicubic)
+\end{itemize}
+
+When a boiler efficiency curve is used, a constant efficiency boiler may be specified by setting C1 = 1 and all other coefficients to 0. A boiler with an efficiency proportional to part-load ratio or which has a non-linear relationship of efficiency with part-load ratio will typically set the coefficients of a linear, quadratic, or cubic curve to non-zero values. Using other curve types allows a more accurate simulation when boiler efficiency varies as a function of part-load ratio and as the boiler outlet water temperature changes over time due to loading or as changes occur in the water temperature setpoint.
+
+The parasitic electric power is calculated based on the user-defined parasitic electric load and the operating part load ratio calculated above. The model assumes that this parasitic power does not contribute to heating the water.
+
+\begin{equation}
+{P_{parasitic}} = {P_{load}}\left( {PLR} \right)
+\end{equation}
+
+where:
+
+\({P_{parasitic}}\) = parasitic electric power (W), average for the simulation time step
+
+\({P_{load}}\) ~~~ = parasitic electric load specified by the user (W)
+
+\subsection{Steam Boiler}\label{steam-boiler}
+
+\subsubsection{Description of Model}\label{description-of-model}
+
+A steam boiler is the essential part of a building steam heating system and can be described as primary driver of the steam loop.~ It is the component that maintains the desired loop temperature.
+
+The emphasis in EnergyPlus was laid on developing a building simulation model for steam boiler with ability to model detailed boiler performance without the cost of exhaustive user inputs to the boiler model.~ The Boiler:Steam input object is used on the plant loop supply side of EnergyPlus with the primary purpose of supplying steam to the heating coils, which constitute the demand side of the loop.
+
+The steam boiler is a variable mass flow rate device.~ The mass flow rate of steam through the boiler is determined by the heating demand on the loop which in turn is determined by the equipment that is hooked to the demand side of the loop, namely the steam coils and hot water heater.~ In short, the steam coil determines the mass flow rate of steam required for heating the zone to its required setpoint, the mixer sums up the total steam demanded by each of the individual coils and reports it to the boiler via the pump.
+
+\begin{figure}[hbtp] % fig 158
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2932.png}
+\caption{Schematic of Steam Boiler in the Steam loop \protect \label{fig:schematic-of-steam-boiler-in-the-steam-loop}}
+\end{figure}
+
+Figure~\ref{fig:schematic-of-steam-boiler-in-the-steam-loop} describes the rudimentary loop structure with steam flowing from coils to boiler.~ It is essential to mention that it is the coils that determine the mass of steam required and the boiler simply delivers the required mass flow at desired temperature provided it is adequately sized.~ The algorithm for determining the mass flow rate is structured on the demand side and the variable flow boiler has no role to play in determining the steam mass flow.
+
+Figure~\ref{fig:schematic-of-steam-boiler-operation} outlines the simple steam boiler model.~ Sub cooled water enters the variable flow boiler through the pump, the boiler inputs energy to water stream consuming fuel, boiler losses are accounted via boiler efficiency.~ The boiler delivers steam at a quality equal to 1.0 at saturated condition.
+
+The advantage of steam heating systems over hot water is the high latent heat carrying capacity of steam, which reduces the mass flow rate of the fluid required.~ The amount of superheated and sub cooled heat transfer in Steam heating systems is negligible, latent heat transfer accounts for almost all of the heat exchange into the zones via steam to air heat exchangers.
+
+\begin{figure}[hbtp] % fig 159
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image2933.png}
+\caption{Schematic of Steam Boiler Operation \protect \label{fig:schematic-of-steam-boiler-operation}}
+\end{figure}
+
+Boiler Load is a summation of sensible and latent heat addition to the water stream as described with the following equation.~ The mass flow rate through the boiler is known, while delta temp is the temperature difference between the boiler inlet and boiler outlet.~ Latent heat of steam is calculated at loop operating temperature.
+
+\begin{equation}
+{Q_B} = \,\dot m\, \times \left[ {({c_{p,w}} \times \Delta T)\,\,\, + \,\,\,{h_{fg}}} \right]
+\end{equation}
+
+Theoretical fuel used is calculated with the following equation.~ Boiler efficiency is a user input and accounts for all the losses in the steam boiler.
+
+\begin{equation}
+{F_t} = \frac{{{Q_B}}}{{{\eta_B}}}
+\end{equation}
+
+The operation part load ratio is calculated with the following equation.~ This is later used to calculate the actual fuel consumption, its ratio of boiler load to boiler nominal capacity.
+
+\begin{equation}
+{O_{PLR}} = \frac{{{Q_B}}}{{{Q_{B,N}}}}
+\end{equation}
+
+The actual fuel consumption by the boiler is calculated as using the following equation, where C1, C2, and C3 are the Part Load Ratio coefficients.
+
+\begin{equation}
+{F_{}} = \frac{{{F_t}}}{{{C_1}\,\, + \,\,{C_2}\,\, \times \,\,{O_{PLR}}\,\, + \,\,{C_3} \times \,{O_{PLR}}^2\,}}
+\end{equation}
+
+Essentially the boiler model provides a first order approximation of performance for fuel oil, gas, and electric boilers.~ Boiler performance is based on theoretical boiler efficiency and a single quadratic fuel use-part load ratio curve represented in the equation above.~ This single curve accounts for all combustion inefficiencies and stack losses.
+
+The control algorithm for a steam boiler is an important issue.~ The user may want the boiler to be undersized and in such a case it will not be able to meet the demand side steam flow request.~ Subsequently the boiler load exceeds the boiler nominal capacity.~ The boiler operates at its nominal capacity but is unable to meet the plant heating demand.~ Pseudo code from EnergyPlus has been used to describe the control logic used in the steam boiler simulation.
+
+*********************PSEUDO CODE SECTION STARTS***********************
+
+At start of simulation an initial value of steam mass flow rate is calculated.~ This is required to start the flow of steam around the loop.
+
+\begin{equation}
+If\,\,\,\,(FirstTimeThrough)\,\,\,THEN
+\end{equation}
+
+Calculate the boiler supply steam mass flow rate at start of simulation.
+
+\begin{equation}
+\,{\dot m_s}\,\, = \,\,\frac{{{Q_B}}}{{{h_{fg\,\,\, + }}\,\,{c_{p,w}}\,\, \times \Delta {T_{loop}}\,\,}}
+\end{equation}
+
+\[ELSE\] ~~ ! Not first time through
+
+Steam boiler calculations rely heavily on the variable \(\dot m\) \(_{b}\), boiler mass flow rate.~ This variable \(\dot m\) \(_{b}\) is the assigned equal to mass flow at boiler inlet node for preliminary calculations.
+
+\begin{equation}
+\,{\dot m_b}\,\,\, = \,\,\,\mathop {\,{{\dot m}_{Inlet_Node}}}\limits^{}
+\end{equation}
+
+Calculating the boiler delta temperature difference between the inlet and outlet nodes.~ This calculation is used to determine various boiler control situation.
+
+\begin{equation}
+\Delta {T_{in_out}}\,\, = \,\,{T_{SP}}\,\, - \,\,{T_{in}}
+\end{equation}
+
+In case the temperature difference calculated with the previous equation equation~ is zero then the boiler just needs to supply latent heat to steam, else the boiler performs its normal load calculations by providing both sensible and latent heat to the inlet stream.
+
+\begin{equation}
+If\,\,(\Delta {T_{in_out}}\,\, < \,\,\,\,0\,\,\,)\,\,\,THEN
+\end{equation}
+
+\begin{equation}
+{Q_B}\,\, = \,\,\,{\dot m_b}\,\,\, \times \,\,{h_{fg}}
+\end{equation}
+
+\begin{equation}
+ELSE
+\end{equation}
+
+\begin{equation}
+{Q_B}\,\, = \,\,\,{\dot m_b}\,\,\, \times \,\,(\,\,\,{h_{fg}} + \,\,{c_{p,w}} \times \Delta {T_{in_out}}\,\,)
+\end{equation}
+
+\begin{equation}
+End\,\,If
+\end{equation}
+
+Sometimes the boiler load Q\(_{B}\) is greater than the demand side requested load at the current time step, which may occur because the boiler inlet conditions is from previous time step.~ There is sudden fall in request of steam mass flow from the demand side.~ The boiler now recalculates its new mass flow and adjusts to these new conditions.
+
+\begin{equation}
+If\,\,({Q_B}\,\, > \,\,{Q_{HeatingDemand}}\,\,\,)\,\,\,THEN
+\end{equation}
+
+Boiler load is set equal to the new boiler heating demand and steam mass flow rate is recalculated.
+
+\begin{equation}
+{Q_B}\,\, = \,\,{Q_{HeatingDemand}}
+\end{equation}
+
+\begin{equation}
+\,{\dot m_s}\,\,\, = \,\,\frac{{{Q_B}}}{{{h_{fg\,\,\, + }}\,\,{c_{p,w}}\,\, \times \Delta {T_{loop}}\,\,}}
+\end{equation}
+
+\begin{equation}
+End\,\,If
+\end{equation}
+
+In case the requested load exceeds the boiler nominal capacity, which is its maximum heating capacity.~ In this case the requested steam mass flow is not met and the zone is not heated adequately.~ This happens if the boiler is undersized.~ The steam mass flow rate is recalculated at nominal capacity.
+
+\begin{equation}
+If\,\,({Q_B}\,\, > \,\,{Q_{No\min al_Capacity}}\,\,\,)\,\,\,THEN
+\end{equation}
+
+Boiler load is set equal to boiler nominal capacity and steam mass flow rate recalculated.
+
+\begin{equation}
+{Q_B}\,\, = \,\,{Q_{No\min al_Capacity}}
+\end{equation}
+
+\begin{equation}
+\,{\dot m_s}\,\,\, = \,\,\frac{{{Q_B}}}{{{h_{fg\,\,\, + }}\,\,{c_{p,w}}\,\, \times \Delta {T_{loop}}\,\,}}
+\end{equation}
+
+\begin{equation}
+End\,\,If
+\end{equation}
+
+\begin{equation}
+End\,\,If
+\end{equation}
+
+End If statement for the boiler load control algorithm.~ This algorithm determines all possible control conditions that might while simulating a system in EnergyPlus.
+
+*********************PSEUDO CODE SECTION STARTS***********************
+
+If the boiler operating pressure exceeds the maximum allowable boiler pressure, the simulation trips and outputs a warning regarding the same.~ This notifies the user about potential system pressure sizing problems.
+
+Integration of the steam boiler simulation model in EnergyPlus required developing number of subroutines, which operate in sequence.~ These subroutines are designed to read inputs from the input file, initialize the variables used in the boiler simulation model, simulate the boiler performance, update the node connections, and report the required variables.~ In case the user has difficulty with boiler inputs, provisions have been made to auto size the boiler nominal capacity and maximum steam flow rate.~ These two values play an important role in sizing the boiler.
+
+\subsubsection{Model Assumptions}\label{model-assumptions}
+
+The EnergyPlus boiler model is ``simple'' in the sense that it requires the user to supply the theoretical boiler efficiency.~ The combustion process is not considered in the model.~ The model is independent of the fuel type, which is input by the user for energy accounting purposes only.~ This is an ideal model for Building Simulation Program such that it utilizes the desired amount of resources in terms of simulation run time, but successfully provides fairly good sizing parameters for an actual boiler.
+
+It is assumed that the steam boiler operates to maintain a desired temperature, the temperature being saturation temperature of steam and corresponding to this saturation temperature there exist a single value of saturation pressure at which the loop operates.~ Hence the boiler could either be saturation pressure controlled or temperature controlled.~ Since users would have better idea of steam temperatures rather than pressure the boiler inputs are designed for temperature control.
+
+\subsubsection{Nomenclature for Steam Loop}\label{nomenclature-for-steam-loop}
+
+% table 50
+\begin{longtable}[c]{p{1.0in}p{4.0in}}
+\caption{Steam Loop Nomenclature \label{table:steam-loop-nomenclature}} \tabularnewline
+\toprule 
+\({Q_{B}}\) & Boiler Heat Transfer. W. \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Steam Loop Nomenclature} \tabularnewline
+\toprule 
+\({Q_{B}}\) & Boiler Heat Transfer. W. \tabularnewline
+\midrule
+\endhead
+
+\({Q_{B,N}}\) & Boiler Nominal Capacity.~ W. \tabularnewline
+\({O_{PLR}}\) & Boiler Operating Part Load Ratio.~ \tabularnewline
+\(\Delta\)T\(_{sc}\) & Degree of subcooling in coil.~ \tabularnewline
+\(\Delta\)T\(_{in_out}\) & Temperature difference across the steam boiler.~ ºC. \tabularnewline
+\(\rho\)\(_{w}\) & Density of condensate entering the pump.~ Kg/m\(^3\).~ \tabularnewline
+\(Q_{Des}\) & Design Load on the steam coil.~ W. \tabularnewline
+\(h_{f,n}\) & Enthalpy of fluid at point n on the Ts diagram.~ J/kg. \tabularnewline
+\(P_{Frac}\) & Fraction of Pump Full Load Power.~ W. \tabularnewline
+\(F_{m,f}\) & Fractional Motor Power Lost to Fluid.~ W. \tabularnewline
+\(Q_{a,l}\) & Heating load on the Air Loop Steam Coil.~ W. \tabularnewline
+\(Q_{z,c}\) & Heating load on the Zone Steam Coil.~ W. \tabularnewline
+\(h_{fg,T_loop}\) & Latent heat of steam at Loop operating Temperature.~ J/kg. \tabularnewline
+\(h_{fg}\) & Latent Heat of Steam.~ J/kg. \tabularnewline
+\(Q_{L,H}\) & Latent Heat Part of the Heating Coil Load.~ W. \tabularnewline
+\(\Delta\)Q\(_{loss}\) & Loop losses in steam coil.~ W. \tabularnewline
+\(\Delta\)T\(_{loop}\) & Loop Temperature Difference. \tabularnewline
+\(\dot m_{a}\) & Mass flow rate for steam coil Kg/s. \tabularnewline
+\(\dot m_{in}\) & Mass flow rate of steam entering the steam coil .Kg/s. \tabularnewline
+\(\dot m_{a,l}\) & Mass flow rate of steam for Air loop steam coil Kg/s \tabularnewline
+\(\dot m_{z,c}\) & Mass flow rate of steam for zone steam coil Kg/s. \tabularnewline
+\(\dot m_{s}\) & Mass flow rate of steam.~ Kg/s. \tabularnewline
+\(\dot m_{loop}\) & Mass flow rate of steam for the steam loop.~ Kg/s. \tabularnewline
+\(\dot m\) & Mass of condensate entering the pump.~ Kg/s. \tabularnewline
+\(\dot m_{a,max}\) & Maximum allowed mass flow rate of air.~ Kg/s \tabularnewline
+\(\dot m_{S,max}\) & Maximum Mass flow rate of steam Kg/s \tabularnewline
+\(\dot m_{B,Supply}\) & Maximum steam mass flow rate supplied by boiler.~ Kg/s. \tabularnewline
+\(\dot V_{w,max}\) & Maximum Volume flow rate of condensate in pump.~ m\(^3\)/s. \tabularnewline
+\(\dot V_{w,loop}\) & Maximum Volume flow rate of condensate in steam loop.~ m\(^3\)/s. \tabularnewline
+\(T_{a,in,min}\) & Minimum inlet air temperature possible.~ ºC. \tabularnewline
+\(P_{n}\) & Nominal Power Capacity for condensate pump.~ W. \tabularnewline
+\(P_{nom}\) & Nominal power of the pump.~ W. \tabularnewline
+\(H_{n}\) & Nominal Pump Head.~ M. \tabularnewline
+\(\dot V_{nom}\) & Nominal volume flow rate through the condensate pump.~ m\(^3\)/s. \tabularnewline
+PLR & Part Load Ratio for condensate pump. \tabularnewline
+\(\eta\)\(_{p}\) & Pump efficiency. \tabularnewline
+\(\eta\)\(_{m}\) & Pump Motor Efficiency. \tabularnewline
+P & Pump Power.~ W. \tabularnewline
+\(Q_{S,H}\) & Sensible Heat Part of the Heating Coil Load.~ W. \tabularnewline
+\(T_{sp}\) & Setpoint Temperature of the zone.~ ºC. \tabularnewline
+\(T_{a,out,SP}\) & Setpoint air outlet temperature for the steam coil.~ ºC. \tabularnewline
+\(P_{S}\) & Shaft power of the pump.~ W. \tabularnewline
+\(c_{p,a}\) & Specific Heat Capacity for Air.~ J/Kg K. \tabularnewline
+\(c_{p,w}\) & Specific Heat Capacity for Water.~ J/Kg K. \tabularnewline
+\(\eta\)\(_{B}\) & Steam Boiler Efficiency. \tabularnewline
+\(T_{a,in}\) & Temperature of air entering the coil.~ ºC. \tabularnewline
+\(T_{a}\) & Temperature of air entering the steam coil.~ ºC. \tabularnewline
+\(T_{a,out}\) & Temperature of air leaving the coil.~ ºC. \tabularnewline
+\(T_{s,in}\) & Temperature of steam entering the coil.~ ºC. \tabularnewline
+\(F_{in}\) & Theoretical Fuel Consumption by the Steam Boiler.~ W. \tabularnewline
+\(\dot m_{coils,R}\) & Total Mass flow rate requested by all the steam coils.~ Kg/s. \tabularnewline
+\(\dot V\) & Volume of condensate entering the pump.~ m\(^3\)/s. \tabularnewline
+\(T_{w,out}\) & Water outlet temperature from pump.~ ºC. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{References}\label{references-007}
+
+ASHRAE Handbook. 1996. HVAC Systems and Equipment, Air Conditioning and Heating Systems.~ Chapter 10, Steam Systems.~ pp.\emph{~} 10.1-10.16. 1996.
+
+\emph{BLAST 3.0 Users Manual}. 1999. Building Systems Laboratory.~ Urbana-Champaign: Building Systems Laboratory, Department of Mechanical and Industrial Engineering, University of Illinois.
+
+Chillar, R.J. 2005. ``Development and Implementation of a Steam Loop In The Building Energy Simulation Program EnergyPlus,'' M.S. Thesis, Department of Mechanical and Industrial Engineering, University of Illinois at Urbana-Champaign.
+
+\emph{TRNSYS 16 User Manual}. 2004. A Transient System Simulation Program. Solar Energy Laboratory, Madison. University of Wisconsin-Madison.
+
+El-Wakil, M. M. 1984. Power Plant Technology, McGraw Hill, New York, pp.~~ 30-72.
+
+Babcock \& Wilcox. 1978. Steam-Its Generation and Use, The Babcock \& Wilcox Company, New York ,Section I, II, IV, and VII.
+
+S.A. Klein. 2004. Engineering Equation Solver EES. University of Wisconsin Madison.
diff --git a/doc/engineering-reference/src/simulation-models-encyclopedic-reference/chillers.tex b/doc/engineering-reference/src/simulation-models-encyclopedic-reference/chillers.tex
new file mode 100644
index 00000000000..f4a65a74ce3
--- /dev/null
+++ b/doc/engineering-reference/src/simulation-models-encyclopedic-reference/chillers.tex
@@ -0,0 +1,1929 @@
+\section{Chillers }\label{chillers}
+
+\subsection{Absorption Chiller}\label{absorption-chiller}
+
+The input object Chiller:Absorption provides a model for absorption chillers that is an empirical model of a standard absorption refrigeration cycle.~ The condenser and evaporator are similar to that of a standard chiller, which are both water-to-water heat exchangers.~ The assembly of a generator and absorber provides the compression operation.~ Low-pressure vapor from the evaporator is absorbed by the liquid solution in the absorber.~ A pump receives low-pressure liquid from the absorber, elevates the pressure of the liquid, and delivers the liquid to the generator.~ In the generator, heat from a high temperature source (hot water or steam) drives off the vapor that has been absorbed by the solution.~ The liquid solution returns to the absorber through a throttling valve whose purpose is to provide a pressure drop to maintain the pressure difference between the generator and absorber.~ The heat supplied to the absorber can be waste heat from a diesel jacket, or the exhaust heat from diesel, gas, and steam turbines.~ For more information on absorption chillers, see the Input/Output Reference Document (Object: Chiller:Absorption).
+
+The part-load ratio of the absoprtion chiller's evaporator is simply the actual cooling effect produced by the chiller divided by the maximum cooling effect available.
+
+\begin{equation}
+PLR = \frac{\dot{Q}_{evap}}{\dot{Q}_{evap,rated}}
+\end{equation}
+
+where
+
+\(PLR\) ~ = part-load ratio of chiller evaporator
+
+\({\dot Q_{evap}}\) ~ = chiller evaporator load {[}W{]}
+
+\({\dot Q_{evap,\,rated}}\) ~ = rated chiller evaporator capacity {[}W{]}
+
+This absorption chiller model is based on a polynomial fit of absorber performance data.~ The Generator Heat Input Part Load Ratio Curve is a quadratic equation that determines the ratio of the generator heat input to the \emph{demand} on the chiller's evaporator (Q\(_{evap}\)).
+
+\begin{equation}
+GeneratorHeatInputRatio = \frac{{C1}}{{PLR}} + C2 + C3\left( {PLR} \right)
+\end{equation}
+
+The Pump Electric Use Part Load Ratio Curve is a quadratic equation that determines the ratio of the actual absorber pumping power to the nominal pumping power.
+
+\begin{equation}
+ElectricInputRatio = C1 + C2 * PLR + C3 * PL{R^2}
+\end{equation}
+
+Thus, the coefficient sets establish the ratio of heat power in-to-cooling effect produced as a function of part load ratio.~ The ratio of heat-power-in to cooling-effect-produced is the inverse of the coefficient of performance.
+
+If the operating part-load ratio is greater than the minimum part-load ratio, the chiller will run the entire time step and cycling will not occur (i.e. \emph{CyclingFrac} = 1). If the operating part-load ratio is less than the minimum part-load ratio, the chiller will be on for a fraction of the time step equal to \emph{CyclingFrac}. Steam (or hot water) and pump electrical energy use are also calculated using the chiller part-load cycling fraction.
+
+\begin{equation}
+CyclingFrac = MIN\left( {1,\frac{{PLR}}{{PL{R_{min}}}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{generator}} = GeneratorHeatInputRatio\left( {{{\dot Q}_{evap}}} \right)\left( {CyclingFrac} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{pump}} = ElectricInputRatio\left( {{P_{pump}}} \right)\left( {CyclingFrac} \right)
+\end{equation}
+
+where
+
+\(CyclingFrac\) ~ = chiller part-load cycling fraction
+
+\(PL{R_{min}}\) ~ = chiller minimum part-load ratio
+
+\({\dot Q_{generator}}\) ~ = generator input power {[}W{]}
+
+\({\dot Q_{pump}}\) ~ = absorbtion chiller pumping power {[}W{]}
+
+The evaporator water mass flow rate is calculated based on the Chiller Flow Mode as follows.
+
+\textbf{Constant Flow Chillers:}
+
+\textbf{\({\dot m_{evap}} = {\dot m_{evap,max}}\)}
+
+\textbf{Variable Flow Chillers:}
+
+\begin{equation}
+\Delta {T_{evap}} = {T_{evap,\,in}} - {T_{evap,\,SP}}
+\end{equation}
+
+\begin{equation}
+  \dot{m}_{evap} = \frac{\dot{Q}_{evap}}{C_{p,evap} \Delta T_{evap}}
+\end{equation}
+
+where
+
+\({\dot m_{evap}}\) ~~~~~~~~~ = chiller evaporator water mass flow rate (kg/s)
+
+\({\dot m_{evap,\,max}}\) ~~~~ = chiller design evaporator water mass flow rate (kg/s)
+
+\(\Delta {T_{evap}}\) ~~~~~~~ = chiller evaporator water temperature difference (ºC)
+
+\({T_{evap,\,in}}\) ~~~~~~~ = chiller evaporator inlet water temperature (ºC)
+
+\({T_{evap,\,SP}}\) ~~~~~~ = chiller evaporator outlet water setpoint temperature (ºC)
+
+\({C_p}\) ~~~~~~~~~~~~~ = specific heat of water entering evaporator (J/kg•ºC)
+
+The evaporator outlet water temperature is then calculated based on the cooling effect produced and the evaporator entering water temperature.
+
+\begin{equation}
+  T_{evap,out} = T_{evap,in} + \frac{\dot{Q}_{evap}}{\dot{m}_{evap}C_{p,evap}}
+\end{equation}
+
+where
+
+\({T_{evap,out}}\) ~ = chiller evaporator outlet water temperature {[}ºC{]}
+
+\({T_{evap,in}}\) ~ = chiller evaporator inlet water temperature {[}ºC{]}
+
+\({C_{p,\,evap}}\) ~ = specific heat of chiller evaporator inlet water {[}J/kg/ºC{]}
+
+\({\dot m_{evap}}\) ~ = chiller evaporator water mass flow rate {[}kg/s{]}
+
+The condenser heat transfer and condenser leaving water temperature are also calculated.
+
+\begin{equation}
+{\dot Q_{cond}} = {\dot Q_{evap}} + {\dot Q_{generator}} + {\dot Q_{pump}}
+\end{equation}
+
+\begin{equation}
+  T_{cond,out} = T_{cond,in} + \frac{\dot{Q}_{cond}}{\dot{m}_{cond}C_{p,cond}}
+\end{equation}
+
+where
+
+\({\dot Q_{cond}}\) ~ = chiller condenser heat transfer rate {[}W{]}
+
+\({T_{cond,out}}\) ~ = chiller condenser outlet water temperature {[}ºC{]}
+
+\({T_{cond,in}}\) ~ = chiller condenser inlet water temperature {[}ºC{]}
+
+\({C_{p,\,cond}}\) ~ = specific heat of chiller condenser inlet water {[}J/kg/ºC{]}
+
+\({\dot m_{cond}}\) ~ = chiller condenser water mass flow rate {[}kg/s{]}
+
+The absorption chiller can model the impact of steam or hot water entering the generator, although the connection of the steam (hot water) nodes to a plant is not actually required. The calculations specific to the generator depend on the type of fluid used and are described here in further detail.
+
+\subsubsection{Steam Loop Calculations}\label{steam-loop-calculations}
+
+When a steam loop is used and the inlet and outlet node names are specified (i.e.~the nodes are connected to a steam loop), the generator outlet node steam mass flow rate and temperature are calculated based on the generator input power, latent heat of steam, the specific heat of water, and the amount of subcooling in the steam generator. The model assumes dry saturated steam enters the absorption chiller's generator and exits the generator as a subcooled liquid. The temperature leaving the generator is calculated based on the user entered amount of liquid subcooling in the generator. The effect of subcooling of the liquid (condensate) in the pipe returning to the boiler is not modeled.
+
+\begin{equation}
+{\dot m_{steam}}\,\,\,\, = \,\,\,\,\,\frac{{{{\dot Q}_{generator}}}}{{{h_{fg}} + {c_{p,\,water}} \times \Delta {T_{sc}}}}
+\end{equation}
+
+\begin{equation}
+{T_{generator,out}} = {T_{generator,in}} - \Delta {T_{sc}}
+\end{equation}
+
+where
+
+\({\dot m_{steam}}\) ~ = chiller steam mass flow rate {[}kg/s{]}
+
+\({h_{fg}}\) ~ = latent heat of steam {[}J/kg{]}
+
+\({c_{p,\,water}}\) ~ = specific heat of saturated water in the generator {[}J/Kg ºK{]}
+
+\(\Delta {T_{sc}}\) ~ = amount of subcooling in steam generator {[}ºC{]}
+
+\({T_{generator,out}}\) ~ = generator steam outlet node temperature {[}ºC{]}
+
+\({T_{generator,in}}\) ~ = generator steam inlet node temperature {[}ºC{]}
+
+\subsubsection{Hot Water Loop Calculations}\label{hot-water-loop-calculations}
+
+When a hot water loop is used and the inlet and outlet node names are specified (i.e.~the nodes are connected to a hot water loop), the generator outlet node temperature is calculated based on the generator input power, mass flow rate of water, and the specific heat of water entering the hot water generator. The calculations are based on the Chiller Flow Mode as follows.
+
+\textbf{Constant Flow Chillers:}
+
+\begin{equation}
+{\dot m_{generator}} = {\dot m_{generator,max}}
+\end{equation}
+
+\textbf{Variable Flow Chillers:}
+
+\begin{equation}
+  \dot{m}_{generator} = \frac{\dot{Q}_{generator}}{C_{p,water}\Delta T_{generator}}
+\end{equation}
+
+\begin{equation}
+{T_{generator,out}} = {T_{generator,in}} - \frac{{{{\dot Q}_{generator}}}}{{{{\dot m}_{generator}}\left( {{C_{p\,,\,water}}} \right)}}
+\end{equation}
+
+where
+
+\({\dot m_{generator}}\) ~ = generator hot water mass flow rate {[}kg/s{]}
+
+\({\dot m_{generator,\,max}}\) = generator design hot water mass flow rate (kg/s)
+
+\(\Delta {T_{generator}}\) ~~ = generator design hot water temperature difference (ºC)
+
+\subsection{Indirect Absorption Chiller}\label{indirect-absorption-chiller}
+
+The Chiller:Absorption:Indirect object is an enhanced version of the absorption chiller model found in the Building Loads and System Thermodynamics (BLAST) program. This enhanced model is nearly identical to the existing absorption chiller model (Ref. Chiller:Absorption) with the exceptions that: 1) the enhanced indirect absorption chiller model provides more flexible performance curves and 2) chiller performance now includes the impact of varying evaporator, condenser, and generator temperatures. Since these absorption chiller models are nearly identical (i.e., the performance curves of the enhanced model can be manipulated to produce similar results to the previous model), it is quite probable that the Chiller:Absorption model will be deprecated in a future release of EnergyPlus.
+
+The indirect absorption chiller's condenser and evaporator are similar to that of a standard chiller, which are both water-to-water heat exchangers. The assembly of a generator and absorber provides the compression operation. A schematic of a single-stage absorption chiller is shown in the figure below. Low-pressure vapor from the evaporator is absorbed by the liquid solution in the absorber. A pump receives low-pressure liquid from the absorber, elevates the pressure of the liquid, and delivers the liquid to the generator. In the generator, heat from a high temperature source (hot water or steam) drives off the vapor that has been absorbed by the solution. The liquid solution returns to the absorber through a throttling valve whose purpose is to provide a pressure drop to maintain the pressure difference between the generator and absorber. The heat supplied to the generator can be either hot water or steam, however, connection to an actual plant loop is not required. For more information on indirect absorption chillers, see the Input/Output Reference Document (Object: Chiller:Absorption:Indirect).
+
+\begin{figure}[hbtp] % fig 160
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3060.png}
+\caption{Schematic Diagram of a Single-Stage Absorption Chiller \protect \label{fig:schematic-diagram-of-a-single-stage}}
+\end{figure}
+
+The chiller cooling effect (capacity) will change with a change in condenser water temperature. Similarly, the chiller cooling effect will change as the temperature of the evaporator water changes. The chiller cooling effect will also change with a change in or generator inlet water temperature and only applies when Hot Water is used as the generator heat source. A quadratic or cubic equation is used to modify the rated chiller capacity as a function of both the condenser and generator inlet water temperatures and the evaporator outlet water temperature. If any or all of the capacity correction factor curves are not used, the correction factors are assumed to be 1.
+
+\begin{equation}
+CAPF{T_{evaporator}} = a + b\left( {{T_{evaporator}}} \right) + c{\left( {{T_{evaporator}}} \right)^2} + d{\left( {{T_{evaporator}}} \right)^3}
+\end{equation}
+
+\begin{equation}
+CAPF{T_{condenser}} = e + f\left( {{T_{condenser}}} \right) + g{\left( {{T_{condenser}}} \right)^2} + h{\left( {{T_{condenser}}} \right)^3}
+\end{equation}
+
+\(CAPF{T_{generator}} = i + j\left( {{T_{generator}}} \right) + k{\left( {{T_{generator}}} \right)^2} + l{\left( {{T_{generator}}} \right)^3}\) ~(\emph{Hot Water only})
+
+\begin{equation}
+{\mathop Q\limits^\cdot_{evap,max}} = {\mathop Q\limits^\cdot_{evap,rated}}\left( {CAPF{T_{evaporator}}} \right)\left( {CAPF{T_{condenser}}} \right)\left( {CAPF{T_{generator}}} \right)
+\end{equation}
+
+where
+
+\(CAPF{T_{evaporator}}\) = Capacity correction (function of evaporator temperature) factor
+
+\$CAPF\{T\_\{condenser\}\} = \$ = Capacity correction (function of condenser temperature) factor
+
+\(CAPF{T_{generator}}\) = Capacity correction (function of generator temperature) factor
+
+\({T_{evaporator}}\) ~ = evaporator outet water temperature {[}C{]}
+
+\({T_{condenser}}\) ~ = condenser inlet water temperature {[}C{]}
+
+\({T_{generator}}\) ~ = generator inlet water temperature {[}C{]}
+
+\({\dot Q_{evap,\,\,max}}\) ~ = maximum chiller capacity {[}W{]}
+
+\({\dot Q_{evap,\,\,rated}}\) ~ = rated chiller capacity {[}W{]}
+
+The part-load ratio of the indirect absoprtion chiller's evaporator is simply the actual cooling effect required (load) divided by the maximum cooling effect available.
+
+\begin{equation}
+  PLR = \frac{\dot{Q}_{evap}}{\dot{Q}_{evap,max}}
+\end{equation}
+
+where
+
+\(PLR\) ~ = part-load ratio of chiller evaporator
+
+\({\dot Q_{evap}}\) ~ = chiller evaporator operating capacity {[}W{]}
+
+The generator's heat input is also a function of several parameters. The primary input for determining the heat input requirements is the Generator Heat Input function of Part-Load Ratio Curve. The curve is a quadratic or cubic equation that determines the ratio of the generator heat input to the chiller's maximum capacity (Q\(_{evap,\, max}\)) and is solely a function of part-load ratio. Typical generator heat input ratios at full load (i.e., PLR = 1) are between 1 and 2. Two additional curves are available to modifiy the heat input requirement based on the generator inlet water temperature and the evaporator outlet water temperature.
+
+\begin{equation}
+GeneratorHIR = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2} + d{\left( {PLR} \right)^3}
+\end{equation}
+
+\begin{equation}
+GenfCondT = e + f\left( {{T_{generator}}} \right) + g{\left( {{T_{generator}}} \right)^2} + h{\left( {{T_{generator}}} \right)^3}
+\end{equation}
+
+\begin{equation}
+GenfEvapT = i + j\left( {{T_{evaporator}}} \right) + k{\left( {{T_{evaporator}}} \right)^2} + l{\left( {{T_{evaporator}}} \right)^3}
+\end{equation}
+
+where
+
+\emph{GeneratorHIR}~ = ratio of generator heat input to chiller operating capacity
+
+\emph{GenfCondT}~ = heat input modifier based on generator inlet water temperature
+
+\emph{GenfEvapT}~ = heat input modifier based on evaporator outlet water temperature
+
+The Pump Electric Use function of Part-Load Ratio Curve is a quadratic or cubic equation that determines the ratio of the actual absorber pumping power to the nominal pumping power.
+
+\begin{equation}
+ElectricInputRatio = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2} + d{\left( {PLR} \right)^3}
+\end{equation}
+
+If the chiller operating part-load ratio is greater than the minimum part-load ratio, the chiller will run the entire time step and cycling will not occur (i.e. \emph{CyclingFrac} = 1). If the operating part-load ratio is less than the minimum part-load ratio, the chiller will be on for a fraction of the time step equal to \emph{CyclingFrac}. Generator heat input and pump electrical energy use are also calculated using the chiller part-load cycling fraction.
+
+\begin{equation}
+CyclingFrac = MIN\left( {1.\frac{{PLR}}{{PL{R_{min}}}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{generator}} = GeneratorHIR\left( {{{\dot Q}_{evap,\,max}}} \right)\left( {GenfCondT} \right)\left( {GenfEvapT} \right)\left( {CyclingFrac} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{generator}} = ElectricInputRatio({P_{pump}})(CyclingFrac)
+\end{equation}
+
+where
+
+\(CyclingFrac\) ~ = chiller part-load cycling fraction
+
+\(PL{R_{min}}\) ~ = chiller minimum part-load ratio
+
+\({\dot Q_{generator}}\) ~ = generator heat input {[}W{]}
+
+\({\dot Q_{pump}}\) ~ = chiller pumping power {[}W{]}
+
+The evaporator water mass flow rate is calculated based on the Chiller Flow Mode as follows.
+
+\textbf{Constant Flow Chillers:}
+
+\begin{equation}
+{\dot m_{evap}} = {\dot m_{evap,max}}
+\end{equation}
+
+\textbf{Variable Flow Chillers:}
+
+\begin{equation}
+\Delta {T_{evap}} = {T_{evap,\,in}} - {T_{evap,\,SP}}
+\end{equation}
+
+\begin{equation}
+  \dot m_{evap} = \frac{\dot{Q}_{evap}}{C_{p,evap}\Delta T_{evap}}
+\end{equation}
+
+where
+
+\({\dot m_{evap}}\) ~~~~~~~~~ = chiller evaporator water mass flow rate (kg/s)
+
+\({\dot m_{evap,\,max}}\) ~~~~ = chiller design evaporator water mass flow rate (kg/s)
+
+\(\Delta {T_{evap}}\) ~~~~~~~ = chiller evaporator water temperature difference (ºC)
+
+\({T_{evap,\,in}}\) ~~~~~~~ = chiller evaporator inlet water temperature (ºC)
+
+\({T_{evap,\,SP}}\) ~~~~~~ = chiller evaporator outlet water setpoint temperature (ºC)
+
+\({C_{p,\,evap}}\) ~~~~~~~~ = specific heat of water entering evaporator (J/kg ºC)
+
+The evaporator outlet water temperature is then calculated based on the cooling effect produced and the evaporator entering water temperature.
+
+\begin{equation}
+  T_{evap,out} = T_{evap,in} + \frac{\dot{Q}_{evap}}{\dot{m}_{evap}C_{p,evap}}
+\end{equation}
+
+where
+
+\({T_{evap,out}}\) ~ = chiller evaporator outlet water temperature {[}ºC{]}
+
+\({T_{evap,in}}\) ~ = chiller evaporator inlet water temperature {[}ºC{]}
+
+\({C_{p,\,evap}}\) ~ = specific heat of chiller evaporator inlet water {[}J/kg/ºC{]}
+
+\({\dot m_{evap}}\) ~ = chiller evaporator water mass flow rate {[}kg/s{]}
+
+The condenser heat transfer and condenser leaving water temperature are also calculated.
+
+\begin{equation}
+{\dot Q_{cond}} = {\dot Q_{evap}} + {\dot Q_{generator}} + {\dot Q_{pump}}
+\end{equation}
+
+\begin{equation}
+  T_{cond,out} = T_{cond,in} + \frac{\dot{Q}_{cond}}{\dot{m}_{cond}C_{p,cond}}
+\end{equation}
+
+where
+
+\({\dot Q_{cond}}\) ~ = chiller condenser heat transfer rate {[}W{]}
+
+\({T_{cond,out}}\) ~ = chiller condenser outlet water temperature {[}ºC{]}
+
+\({T_{cond,in}}\) ~ = chiller condenser inlet water temperature {[}ºC{]}
+
+\({C_{p,\,cond}}\) ~ = specific heat of chiller condenser inlet water {[}J/kg/ºC{]}
+
+\({\dot m_{cond}}\) ~ = chiller condenser water mass flow rate {[}kg/s{]}
+
+The absorption chiller can model the impact of steam or hot water entering the generator, although the connection of the steam (hot water) nodes to a plant is not actually required. The calculations specific to the generator depend on the type of fluid used and are described here in further detail.
+
+\subsubsection{Steam Loop Calculations}\label{steam-loop-calculations-1}
+
+When a steam loop is used and the inlet and outlet node names are specified (i.e.~the nodes are connected to a steam loop), the generator outlet node steam mass flow rate and temperature are calculated based on the generator heat input, latent heat of steam, the specific heat of water, and the amount of subcooling in the steam generator. The model assumes dry saturated steam enters the generator and exits the generator as a subcooled liquid. The temperature leaving the generator is calculated based on the user entered amount of liquid subcooling in the generator. The effect of subcooling of the liquid (condensate) in the pipe returning to the boiler is also modeled using the user entered abount of steam condensate loop subcooling.
+
+\begin{equation}
+{\dot m_{steam}}\,\,\,\, = \,\,\,\,\,\frac{{{{\dot Q}_{generator}}}}{{{h_{fg}} + {c_{p,water}} \times \Delta {T_{sc}}}}
+\end{equation}
+
+\begin{equation}
+{T_{generator,out}} = {T_{generator,in}} - \Delta {T_{sc}}
+\end{equation}
+
+\begin{equation}
+{T_{loop,out}} = {T_{generator,out}} - \Delta {T_{sc,\,\,loop}}
+\end{equation}
+
+where
+
+\({\dot m_{steam}}\) ~ = chiller steam mass flow rate {[}kg/s{]}
+
+\({h_{fg}}\) ~ = latent heat of steam {[}J/kg{]}
+
+\({c_{p,water}}\) ~ = specific heat of water {[}J/Kg ºC{]}
+
+\(\Delta {T_{sc}}\) ~ = amount of subcooling in steam generator {[}ºC{]}
+
+\(\Delta {T_{sc,\,loop}}\) ~ = amount of condensate subcooling in steam loop {[}ºC{]}
+
+\({T_{generator,out}}\) ~ = generator steam outlet node temperature {[}ºC{]}
+
+\({T_{generator,in}}\) ~ = generator steam inlet node temperature {[}ºC{]}
+
+\subsubsection{Hot Water Loop Calculations}\label{hot-water-loop-calculations-1}
+
+When a hot water loop is used and the inlet and outlet node names are specified (i.e.~the nodes are connected to a hot water loop), the generator outlet node temperature is calculated based on the generator heat input, mass flow rate of water, and the specific heat of water entering the hot water generator. The calculations are based on the Chiller Flow Mode as follows.
+
+\textbf{Constant Flow Chillers:}
+
+\begin{equation}
+{\dot m_{generator}} = {\dot m_{generator,\,max}}
+\end{equation}
+
+\textbf{Variable Flow Chillers:}
+
+\begin{equation}
+  \dot{m}_{generator} = \frac{\dot{Q}_{generator}}{C_{p,water}\Delta T_{generator}}
+\end{equation}
+
+\begin{equation}
+{T_{generator,out}} = {T_{generator,in}} - \frac{{{{\dot Q}_{generator}}}}{{{{\dot m}_{generator}}\left( {{C_{p\,,\,water}}} \right)}}
+\end{equation}
+
+where
+
+\({\dot m_{generator}}\) ~ = generator hot water mass flow rate {[}kg/s{]}
+
+\({\dot m_{generator,\,max}}\) = generator design hot water mass flow rate (kg/s)
+
+\(\Delta {T_{generator}}\) ~~ = generator design hot water temperature difference (ºC)
+
+\subsection{Combustion Turbine Chiller}\label{combustion-turbine-chiller}
+
+The input object Chiller:CombustionTurbine provides a chiller model that is the empirical model from the Building Loads and System Thermodynamics (BLAST) program. Fitting catalog data to a third order polynomial equations generates the chiller performance curves.~ Three sets of coefficients are required to model the open centrifugal chiller as discussed in the section, titled, `Electric Chiller Based on Fluid Temperature Differences'.
+
+The gas turbine-driven chiller is an open centrifugal chiller driven directly by a gas turbine.~ The BLAST model of an open centrifugal chiller is modeled as standard vapor compression refrigeration cycle with a centrifugal compressor driven by a shaft power from an engine.~ The centrifugal compressor has the incoming fluid entering at the eye of a spinning impeller that throws the fluid by centrifugal force to the periphery of the impeller.~ After leaving the compressor, the refrigerant is condensed to liquid in a refrigerant to water condenser.~ The heat from the condenser is rejected to a cooling tower, evaporative condenser, or well water condenser depending on which one is selected by the user based on the physical parameters of the plant.~ The refrigerant pressure is then dropped through a throttling valve so that fluid can evaporate at a low pressure that provides cooling to the evaporator.~ The evaporator can chill water that is pumped to chilled water coils in the building.~ For more information, see the Input/Output Reference Document.
+
+This chiller is modeled like the electric chiller with the same numerical curve fits and then some additional curve fits to model the turbine drive.~ Shown below are the definitions of the curves that describe this model.
+
+The chiller's temperature rise coefficient which is defined as the ratio of the required change in condenser water temperature to a given change in chilled water temperature, which maintains the capacity at the nominal value.~ This is calculated as the following ratio:
+
+\begin{equation}
+\frac{{TCEn{t_{required}} - TCEn{t_{rated}}}}{{TEL{v_{required}} - TEL{v_{rated}}}}
+\end{equation}
+
+Where:
+
+TCEnt\(_{required}\) = Required entering condenser air or water temperature to maintain rated capacity.
+
+TCEnt\(_{rated}\) = Rated entering condenser air or water temperature at rated capacity.
+
+TELv\(_{required}\) = Required leaving evaporator water outlet temperature to maintain rated capacity.
+
+TELv\(_{rated}\) = Rated leaving evaporator water outlet temperature at rated capacity.
+
+The Capacity Ratio Curve is a quadratic equation that determines the Ratio of Available Capacity to Nominal Capacity.~ The defining equation is:
+
+\begin{equation}
+AvailToNominalCapacityRatio = {C_1} + {C_2}{\Delta_{temp}} + {C_3}\Delta_{temp}^2
+\end{equation}
+
+Where the Delta Temperature is defined as:
+
+\begin{equation}
+{\Delta_{{\rm{Temp}}}} = \frac{{{\rm{TempCondIn  -  TempCondInDesign }}}}{{{\rm{TempRiseCoefficient}}}} - ({\rm{TempEvapOut  -  TempEvapOutDesign)}}
+\end{equation}
+
+TempCondIn = Temperature entering the condenser (water or air temperature depending on condenser type).
+
+TempCondInDesign = Temp Design Condenser Inlet from User input above.
+
+TempEvapOut = Temperature leaving the evaporator.
+
+TempEvapOutDesign = Temp Design Evaporator Outlet from User input above.
+
+TempRiseCoefficient = User Input from above.
+
+The following three fields contain the coefficients for the quadratic equation.
+
+The Power Ratio Curve is a quadratic equation that determines the Ratio of Full Load to Power.~ The defining equation is:
+
+\begin{equation}
+FullLoadtoPowerRatio = {C_1} + {C_2}AvailToNominalCapRatio + {C_3}AvailToNominalCapRati{o^2}
+\end{equation}
+
+The Full Load Ratio Curve is a quadratic equation that determines the fraction of full load power.~ The defining equation is:
+
+\begin{equation}
+FracFullLoadPower = {C_1} + {C_2}PartLoadRatio + {C_3}PartLoadRati{o^2}
+\end{equation}
+
+The Fuel Input Curve is a polynomial equation that determines the Ratio of Fuel Input to Energy Output.~ The equation combines both the Fuel Input Curve Coefficients and the Temperature Based Fuel Input Curve Coefficients.~ The defining equation is:
+
+\begin{equation}
+\begin{split}
+FuelEnergyInput =& PLoad * (FI{C_1} + FI{C_2}RLoad + FI{C_3}RLoa{d^2}) \\
+&* (TBFI{C_1} + TBFI{C_2}A{T_{air}} + TBFI{C_3}AT_{air}^2)
+\end{split}
+\end{equation}
+
+Where FIC represents the Fuel Input Curve Coefficients, TBFIC represents the Temperature Based Fuel Input Curve Coefficients, Rload is the Ratio of Load to Combustion Turbine Engine Capacity, and AT\(_{air}\) is the difference between the current ambient and design ambient temperatures.
+
+The Exhaust Flow Curve is a quadratic equation that determines the Ratio of Exhaust Gas Flow Rate to Engine Capacity.~ The defining equation is:
+
+\emph{\(ExhaustFlowRate = GTCapacity * ({C_1} + {C_2}A{T_{air}} + {C_3}AT_{air}^2)\) ~}
+
+Where GTCapacity is the Combustion Turbine Engine Capacity, and AT\(_{air}\) is the difference between the current ambient and design ambient temperatures.
+
+The Exhaust Gas Temperature Curve is a polynomial equation that determines the Exhaust Gas Temperature.~ The equation combines both the Exhaust Gas Temperature Curve Coefficients (Based on the Part Load Ratio) and the (Ambient) Temperature Based Exhaust Gas Temperature Curve Coefficients.~ The defining equation is:
+
+~\(ExhaustTemperature = ({C_1} + {C_2}RLoad + {C_3}RLoa{d^2}) * (TB{C_1} + TB{C_2}A{T_{air}} + TB{C_3}AT_{air}^2) - 273.15\)
+
+Where C represents the Exhaust Gas Temperature Curve Coefficients, TBC are the Temperature Based Exhaust Gas Temperature Curve Coefficients, RLoad is the Ratio of Load to Combustion Turbine Engine Capacity, and AT\(_{air}\) is the difference between the actual ambient and design ambient temperatures.
+
+The Recovery Lubricant Heat Curve is a quadratic equation that determines the recovery lube energy.~ The defining equation is:
+
+\begin{equation}
+RecoveryLubeEnergy = PLoad * ({C_1} + {C_2}RL + {C_3}R{L^2})
+\end{equation}
+
+Where Pload is the engine load and RL is the Ratio of Load to Combustion Turbine Engine Capacity
+
+The UA is an equation that determines the overall heat transfer coefficient for the exhaust gasses with the stack.~ The heat transfer coefficient ultimately helps determine the exhaust stack temperature.~ The defining equation is:
+
+\begin{equation}
+UAToCapacityRatio = {C_1}GasTurbineEngineCapacit{y^{{C_2}}}
+\end{equation}
+
+\subsubsection{Chiller Basin Heater}\label{chiller-basin-heater}
+
+This chiller's basin heater (for evaporatively-cooled condenser type) operates in the same manner as the Engine driven chiller's basin heater. The calculations for the chiller basin heater are described in detail at the end of the engine driven chiller description (Ref. Engine Driven Chiller).
+
+\subsection{ChillerHeater:Absorption:DirectFired}\label{chillerheaterabsorptiondirectfired}
+
+\subsubsection{Overview}\label{overview-009}
+
+This model (object name ChillerHeater:Absorption:DirectFired) simulates the performance of a direct fired two-stage absorption chiller with optional heating capability. The model is based on the direct fired absorption chiller model (ABSORG-CHLR) in the DOE-2.1 building energy simulation program. The EnergyPlus model contains all of the features of the DOE-2.1 chiller model, plus some additional capabilities.
+
+This model simulates the thermal performance of the chiller and the fuel consumption of the burner(s). This model does not simulate the thermal performance or the power consumption of associated pumps or cooling towers. This auxiliary equipment must be modeled using other EnergyPlus models (e.g.~Cooling Tower:Single Speed).
+
+\subsubsection{Model Description}\label{model-description-006}
+
+The chiller model uses user-supplied performance information at design conditions along with five performance curves (curve objects) for cooling capacity and efficiency to determine chiller operation at off-design conditions. Two additional performance curves for heating capacity and efficiency are used when the chiller is operating in a heating only mode or simultaneous cooling and heating mode.
+
+\subsubsection{Cooling}\label{cooling}
+
+The following nomenclature is used in the cooling equations:
+
+\emph{AvailCoolCap}~~~~~~~~~ = ~~ available full-load cooling capacity at current conditions {[}W{]}
+
+\emph{CEIR}~~~~~~~~~~~~~~~~~~~~~~~ = ~~ user input ``Electric Input to Cooling Output Ratio''
+
+\emph{CEIRfPLR}~~~~~~~~~~~~~~~ = ~~ electric input to cooling output factor, equal to 1 at full load, user input ``Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name''
+
+\emph{CEIRfT}~~~~~~~~~~~~~~~~~~~~ = ~~ electric input to cooling output factor, equal to 1 at design conditions, user input ``Electric Input to Cooling Output Ratio Function of Temperature Curve Name''
+
+\emph{CFIR}~~~~~~~~~~~~~~~~~~~~~~~ = ~~ user input ``Fuel Input to Cooling Output Ratio''
+
+\emph{CFIRfPLR}~~~~~~~~~~~~~~~ = ~~ fuel input to cooling output factor, equal to 1 at full load, user input ``Fuel Input to Cooling Output Ratio Function of Part Load Ratio Curve Name''
+
+\emph{CFIRfT}~~~~~~~~~~~~~~~~~~~~ = ~~ fuel input to cooling output factor, equal to 1 at design conditions, user input ``Fuel Input to Cooling Output Ratio Function of Temperature Curve Name''
+
+\emph{CondenserLoad~~~~~~~} = ~~ condenser heat rejection load {[}W{]}
+
+\emph{CoolCapfT}~~~~~~~~~~~~~~ = ~~ cooling capacity factor, equal to 1 at design conditions, user input ``Cooling Capacity Function of Temperature Curve Name''
+
+\emph{CoolElectricPower}~~ = ~~ cooling electricity input {[}W{]}
+
+\emph{CoolFuelInput}~~~~~~~~~ = ~~ cooling fuel input {[}W{]}
+
+\emph{CoolingLoad}~~~~~~~~~~~ = ~~ current cooling load on the chiller {[}W{]}
+
+\emph{CPLR}~~~~~~~~~~~~~~~~~~~~~~ = ~~ cooling part-load ratio = \emph{CoolingLoad} / \emph{AvailCoolCap}
+
+\emph{HeatingLoad}~~~~~~~~~~~ = ~~ current heating load on the chiller heater {[}W{]}
+
+\emph{HFIR}~~~~~~~~~~~~~~~~~~~~~~~ = ~~ user input ``Fuel Input to Heating Output Ratio''
+
+\emph{HPLR}~~~~~~~~~~~~~~~~~~~~~~ = ~~ heating part-load ratio = \emph{HeatingLoad} / \emph{AvailHeatCap}
+
+\emph{MinPLR~~~~~~~~~~~~~~~~~~~} = ~~ user input ``Minimum Part Load Ratio''
+
+\emph{NomCoolCap}~~~~~~~~~~ = ~~ user input ``Nominal Cooling Capacity'' {[}W{]}
+
+\emph{RunFrac}~~~~~~~~~~~~~~~~~~ = ~~ fraction of time step which the chiller is running
+
+\emph{T\(_{cond}\)}~~~~~~~~~~~~~~~~~~~~~~~~~ = ~~ entering or leaving condenser fluid temperature {[}C{]}. For a water-cooled condenser this will be the water temperature returning from the condenser loop (e.g., leaving the cooling tower) if the entering condenser fluid temperature option is used. For air- or evap-cooled condensers this will be the entering outdoor air dry-bulb or wet-bulb temperature, respectively, if the entering condenser fluid temperature option is used.
+
+\emph{T\(_{cw,l}\)}~~~~~~~~~~~~~~~~~~~~~~~~~~ = ~~ leaving chilled water temperature {[}C{]}
+
+Five performance curves are used in the calculation of cooling capacity and efficiency:
+
+1)~~~~Cooling Capacity Function of Temperature Curve
+
+2)~~~~Fuel Input to Cooling Output Ratio Function of Temperature Curve
+
+3)~~~~Fuel Input to Cooling Output Ratio Function of Part Load Ratio Curve
+
+4)~~~~Electric Input to Cooling Output Ratio Function of Temperature Curve
+
+5)~~~~Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve
+
+The cooling capacity function of temperature (\emph{CoolCapfT}) curve represents the fraction of the cooling capacity of the chiller as it varies by temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser fluid temperature. The output of this curve is multiplied by the nominal cooling capacity to give the full-load cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the design temperatures). The curve should have a value of 1.0 at the design temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\begin{equation}
+CoolCapfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}
+\end{equation}
+
+The available cooling capacity of the chiller is then computed as follows:
+
+\begin{equation}
+AvailCoolCap = NomCoolCap \cdot CoolCapfT({T_{cw,l}},{T_{cond}})
+\end{equation}
+
+The fuel input to cooling output ratio function of temperature (\emph{CFIRfT}) curve represents the fraction of the fuel input to the chiller at full load as it varies by temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser fluid temperature. The output of this curve is multiplied by the nominal fuel input to cooling output ratio (\emph{CFIR}) to give the full-load fuel input to cooling capacity ratio at specific temperature operating conditions (i.e., at temperatures different from the design temperatures). The curve should have a value of 1.0 at the design temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\begin{equation}
+CFIRfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}
+\end{equation}
+
+The fuel input to cooling output ratio function of part load ratio (\emph{CFIRfPLR}) curve represents the fraction of the fuel input to the chiller as the load on the chiller varies at a given set of~ operating temperatures. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic.
+
+\begin{equation}
+CFIRfPLR = a + b \cdot CPLR + c \cdot CPL{R^2}
+\end{equation}
+
+The fraction of the time step during which the chiller heater is operating is computed as a function of the cooling and heating part-load ratios and the user-input minimum part-load ratio:
+
+\begin{equation}
+RunFrac = {\mathop{\rm MIN}\nolimits} \left( {1.0,{\mathop{\rm MAX}\nolimits} \left( {HPLR,CPLR} \right)/MinPLR} \right)
+\end{equation}
+
+The cooling fuel input to the chiller is then computed as follows:
+
+CoolFuelInput = AvailCoolCap * RunFrac * CFIR * CFIRfT($T_{cw,l}$,$T_{cond}$) * CFIRfPLR(CPLR)
+
+The electric input to cooling output ratio as function of temperature (\emph{CEIRfT}) curve represents the fraction of electricity to the chiller at full load as it varies by temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser fluid temperature.
+
+\begin{equation}
+CEIRfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}
+\end{equation}
+
+The electric input to cooling output ratio function of part load ratio (\emph{CEIRfPLR}) curve represents the fraction of electricity to the chiller as the load on the chiller varies at a given set of operating temperatures. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic.
+
+\begin{equation}
+CEIRfPLR = a + b \cdot CPLR + c \cdot CPL{R^2}
+\end{equation}
+
+The cooling electric input to the chiller is computed as follows:
+
+\begin{equation}
+CoolElectricPower = NomCoolCap \cdot RunFrac \cdot CEIR \cdot CEIRfT({T_{cw,l}},{T_{cond}}) \cdot CEIRfPLR(CPLR)
+\end{equation}
+
+All five of these cooling performance curves are accessed through EnergyPlus' built-in performance curve equation manager (objects Curve:Linear, Curve:Quadratic and Curve:Biquadratic). It is not imperative that the user utilize all coefficients in the performance curve equations if their performance equation has fewer terms (e.g., if the user's \emph{CFIRfPLR} performance curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero).
+
+The condenser load is computed as follows:
+
+\begin{equation}
+CondenserLoad = CoolingLoad + {\raise0.7ex\hbox{{CoolFuelInput}} \!\mathord{\left/ {\vphantom {{CoolFuelInput} {HFIR}}}\right.}\!\lower0.7ex\hbox{{HFIR}}} + CoolElectricPower
+\end{equation}
+
+\subsubsection{Heating}\label{heating}
+
+The following nomenclature is used in the heating equations:
+
+\emph{AvailHeatCap}~~~~~~~~~ = ~~ available full-load heating capacity at current conditions {[}W{]}
+
+\emph{CPLRh}~~~~~~~~~~~~~~~~~~~~ = ~~ cooling part-load ratio for heating curve = \emph{CoolingLoad} / \emph{NomCoolCap}
+
+\emph{HeatCapfCPLR}~~~~~~~ = ~~ heating capacity factor as a function of cooling part load ratio, equal to 1 at zero cooling load, user input ``Heating Capacity Function of Cooling Capacity Curve Name''
+
+\emph{HeatCoolCapRatio~} = ~~ user input ``Heating to Cooling Capacity Ratio''
+
+\emph{HeatElectricPower}~~ = ~~ heating electricity input {[}W{]}
+
+\emph{HeatFuelInput}~~~~~~~~~ = ~~ heating fuel input {[}W{]}
+
+\emph{HeatingLoad}~~~~~~~~~~~ = ~~ current heating load on the chiller {[}W{]}
+
+\emph{HEIR}~~~~~~~~~~~~~~~~~~~~~~~ = ~~ user input ``Electric Input to Heating Output Ratio''
+
+\emph{HFIR}~~~~~~~~~~~~~~~~~~~~~~~ = ~~ user input ``Fuel Input to Heating Output Ratio''
+
+\emph{HFIRfHPLR}~~~~~~~~~~~~ = ~~ fuel input to heating output factor, equal to 1 at full load, user input ``Fuel Input to Heat Output Ratio During Heating Only Operation Curve Name''
+
+\emph{HPLR}~~~~~~~~~~~~~~~~~~~~~~ = ~~ heating part-load ratio = \emph{HeatingLoad} / \emph{AvailHeatCap}
+
+\emph{MinPLR~~~~~~~~~~~~~~~~~~~} = ~~ user input ``Minimum Part Load Ratio''
+
+\emph{NomCoolCap}~~~~~~~~~~ = ~~ user input ``Nominal Cooling Capacity'' {[}W{]}
+
+\emph{RunFrac}~~~~~~~~~~~~~~~~~~ = ~~ fraction of time step which the chiller is running
+
+\emph{TotalElectricPower~} = ~~ total electricity input {[}W{]}
+
+\emph{TotalFuelInput~~~~~~~~} = ~~ total fuel input {[}W{]}
+
+Cooling is the primary purpose of the Direct Fired Absorption Chiller so that function is satisfied first and if energy is available for providing heating that is provided next.
+
+The two performance curves for heating capacity and efficiency are:
+
+1)~~~~Heating Capacity Function of Cooling Capacity Curve
+
+2)~~~~Fuel-Input-to Heat Output Ratio Function
+
+The heating capacity function of cooling capacity curve (\emph{HeatCapfCool}) determines how the heating capacity of the chiller varies with cooling capacity when the chiller is simultaneously heating and cooling. The curve is normalized so an input of 1.0 represents the nominal cooling capacity and an output of 1.0 represents the full heating capacity.~ An output of 1.0 should occur when the input is 0.0.
+
+\begin{equation}
+HeatCapfCPLR = a + b \cdot CPLRh + c \cdot CPLR{h^2}
+\end{equation}
+
+The available heating capacity is then computed as follows:
+
+\begin{equation}
+AvailHeatCap = NomCoolCap \cdot HeatCoolCapRatio \cdot HeatCapfCPLR(CPLRh)
+\end{equation}
+
+The fuel input to heat output ratio curve (\emph{HFIRfHPLR}) function is used to represent the fraction of fuel used as the heating load varies as a function of heating part load ratio. It is normalized so that a value of 1.0 is the full available heating capacity. The curve is usually linear or quadratic and will probably be similar to a boiler curve for most chillers.
+
+\begin{equation}
+HFIRfHPLR = a + b \cdot HPLR + c \cdot HPL{R^2}
+\end{equation}
+
+The fuel use rate when heating is computed as follows:
+
+\begin{equation}
+HeatFuelInput = AvailHeatCap \cdot HFIR \cdot HFIRfHPLR(HPLR)
+\end{equation}
+
+The fraction of the time step during which the chiller is operating is computed as a function of the cooling and heating part-load ratios and the user-input minimum part-load ratio:
+
+\begin{equation}
+RunFrac = {\mathop{\rm MIN}\nolimits} \left( {1.0,{\mathop{\rm MAX}\nolimits} \left( {HPLR,CPLRh} \right)/MinPLR} \right)
+\end{equation}
+
+The heating electric input to the chiller is computed as follows:
+
+\begin{equation}
+HeatElectricPower = NomCoolCap \cdot HeatCoolCapRatio \cdot HEIR \cdot RunFrac
+\end{equation}
+
+If the chiller is delivering heating and cooling simultaneously, the parasitic electric load will be double-counted, so the following logic is applied:
+
+\begin{lstlisting}
+IF ( HeatElectricPower < = CoolElectricPower ) THEN
+  HeatElectricPower = 0.0
+ELSE
+  HeatElectricPower = HeatElectricPower - CoolElectricPower
+ENDIF
+\end{lstlisting}
+
+The total fuel and electric power input to the chiller is computed as shown below:
+
+TotalElectricPower = HeatElectricPower + CoolElectricPower
+
+TotalFuelInput = HeatFuelInput + CoolFuelInput
+
+\subsection{ChillerHeater:Absorption:DoubleEffect}\label{chillerheaterabsorptiondoubleeffect}
+
+\subsubsection{Overview}\label{overview-1-003}
+
+This model (object name ChillerHeater:Absorption:DoubleEffect) simulates the performance of an exhaust~ fired two-stage (double effect) absorption chiller with optional heating capability. The model is based on the direct fired absorption chiller model (ABSORG-CHLR) in the DOE-2.1 building energy simulation program. The EnergyPlus model contains all of the features of the DOE-2.1 chiller model, plus some additional capabilities. The model uses the exhaust gas output from Microturbine.
+
+This model simulates the thermal performance of the chiller and the thermal energy input to the chiller. This model does not simulate the thermal performance or the power consumption of associated pumps or cooling towers. This auxiliary equipment must be modeled using other EnergyPlus models (e.g.~Cooling Tower:Single Speed).
+
+\subsubsection{Model Description}\label{model-description-1-003}
+
+The chiller model uses user-supplied performance information at design conditions along with five performance curves (curve objects) for cooling capacity and efficiency to determine chiller operation at off-design conditions. Two additional performance curves for heating capacity and efficiency are used when the chiller is operating in a heating only mode or simultaneous cooling and heating mode.
+
+\subsubsection{Cooling}\label{cooling-1}
+
+The following nomenclature is used in the cooling equations:
+
+\emph{AvailCoolCap}~~~~~~~~~ = ~~ available full-load cooling capacity at current conditions {[}W{]}
+
+\emph{CEIR}~~~~~~~~~~~~~~~~~~~~~~~ = ~~ user input ``Electric Input to Cooling Output Ratio''
+
+\emph{CEIRfPLR}~~~~~~~~~~~~~~~ = ~~ electric input to cooling output factor, equal to 1 at full load, user input ``Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name''
+
+\emph{CEIRfT}~~~~~~~~~~~~~~~~~~~~ = ~~ electric input to cooling output factor, equal to 1 at design conditions, user input ``Electric Input to Cooling Output Ratio Function of Temperature Curve Name''
+
+\emph{TeFIR}~~~~~~~~~~~~~~~~~~~~~~ = ~~ user input ``Thermal Energy Input to Cooling Output Ratio''
+
+\emph{TeFIRfPLR}~~~~~~~~~~~~~~ = ~~ thermal energy input to cooling output factor, equal to 1 at full load, user input ``Thermal Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve Name''
+
+\emph{TeFIRfT}~~~~~~~~~~~~~~~~~~~ = ~~ thermal energy input to cooling output factor, equal to 1 at design conditions, user input ``Thermal Energy Input to Cooling Output Ratio Function of Temperature Curve Name''
+
+\emph{CondenserLoad~~~~~~~} = ~~ condenser heat rejection load {[}W{]}
+
+\emph{CoolCapfT}~~~~~~~~~~~~~~ = ~~ cooling capacity factor, equal to 1 at design conditions, user input ``Cooling Capacity Function of Temperature Curve Name''
+
+\emph{CoolElectricPower}~~ = ~~ cooling electricity input {[}W{]}
+
+\emph{CoolThermalEnergyInput} = ~~~~~~~~~ cooling thermal energy input {[}W{]}
+
+\emph{CoolingLoad}~~~~~~~~~~~ = ~~ current cooling load on the chiller {[}W{]}
+
+\emph{CPLR}~~~~~~~~~~~~~~~~~~~~~~ = ~~ cooling part-load ratio = \emph{CoolingLoad} / \emph{AvailCoolCap}
+
+\emph{HeatingLoad}~~~~~~~~~~~ = ~~ current heating load on the chiller heater {[}W{]}
+
+\emph{HFIR}~~~~~~~~~~~~~~~~~~~~~~~ = ~~ user input ``Thermal Energy Input to Heating Output Ratio''
+
+\emph{HPLR}~~~~~~~~~~~~~~~~~~~~~~ = ~~ heating part-load ratio = \emph{HeatingLoad} / \emph{AvailHeatCap}
+
+\({\dot m_{ExhAir}}\) ~~~~~~ ~~~~~~~~~~~ ~~ = ~ exhaust air mass flow rate from microturbine (kg/s)
+
+\emph{MinPLR~~~~~~~~~~~~~~~~~~~} = ~~ user input ``Minimum Part Load Ratio''
+
+\emph{NomCoolCap}~~~~~~~~~~ = ~~ user input ``Nominal Cooling Capacity'' {[}W{]}
+
+\emph{RunFrac}~~~~~~~~~~~~~~~~~~ = ~~ fraction of time step which the chiller is running
+
+\({T_{a,o}}\) ~~~~~~~~~~~ ~~~~~~~~~~~~~~~ = ~exhaust air outlet temperature from microturbine entering the chiller
+
+(\(^{o}\)C)
+
+\({T_{abs,gen,o}}\) ~~~~~~~~~~~~~~~~ = ~ Temperature of exhaust leaving the chiller (the generator ~~~~~~~~~~~~~~~~~~~component~ of the absorption chiller)
+
+\emph{T\(_{cond}\)}~~~~~~~~~~~~~~~~~~~~~~~~~ = ~~ entering condenser fluid temperature {[}°C{]}. For a water-cooled condenser this will be the water temperature returning from the condenser loop (e.g., leaving the cooling tower). For air- or evap-cooled condensers this will be the entering outdoor air dry-bulb or wet-bulb temperature, respectively.
+
+\emph{T\(_{cw,l}\)}~~~~~~~~~~~~~~~~~~~~~~~~~~ = ~~ leaving chilled water temperature {[}°C{]}
+
+The selection of entering or leaving condense fluid temperature can be made through the optional field-Temperature Curve Input Variable.
+
+Five performance curves are used in the calculation of cooling capacity and efficiency:
+
+6)~~~~Cooling Capacity Function of Temperature Curve
+
+7)~~~~Thermal Energy Input to Cooling Output Ratio Function of Temperature Curve
+
+8)~~~~Thermal Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve
+
+9)~~~~Electric Input to Cooling Output Ratio Function of Temperature Curve
+
+10)~Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve
+
+The cooling capacity function of temperature (\emph{CoolCapfT}) curve represents the fraction of the cooling capacity of the chiller as it varies with temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and the entering condenser fluid temperature. The output of this curve is multiplied by the nominal cooling capacity to give the full-load cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the design temperatures). The curve should have a value of 1.0 at the design temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\begin{equation}
+CoolCapfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}
+\end{equation}
+
+The available cooling capacity of the chiller is then computed as follows:
+
+\begin{equation}
+AvailCoolCap = NomCoolCap \cdot CoolCapfT({T_{cw,l}} - {T_{cond}})
+\end{equation}
+
+The thermal energy input to cooling output ratio function of temperature (\emph{TeFIRfT}) curve represents the fraction of the thermal energy input to the chiller at full load as it varies with temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and the entering condenser fluid temperature. The output of this curve is multiplied by the nominal thermal energy input to cooling output ratio (\emph{TeFIR}) to give the full-load thermal energy input to cooling capacity ratio at specific temperature operating conditions (i.e., at temperatures different from the design temperatures). The curve should have a value of 1.0 at the design temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\begin{equation}
+TeFIRfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}
+\end{equation}
+
+The thermal energy input to cooling output ratio function of part load ratio (\emph{TeFIRfPLR}) curve represents the fraction of the thermal energy input to the chiller as the load on the chiller varies at a given set of~ operating temperatures. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic.
+
+\begin{equation}
+TeFIRfPLR = a + b \cdot CPLR + c \cdot CPL{R^2}
+\end{equation}
+
+The fraction of the time step during which the chiller heater is operating is computed as a function of the cooling and heating part-load ratios and the user-input minimum part-load ratio:
+
+\begin{equation}
+RunFrac = MIN(1.0,MAX\left( {HPLR,CPLR} \right)/MinPLR)
+\end{equation}
+
+The cooling thermal energy input to the chiller is then computed as follows:
+
+\begin{equation}
+\begin{split}
+CoolThermalEnergyInput =& AvailCoolCap \cdot RunFrac \cdot TeFIR \cdot TeFIRfT\left( {{T_{cw,l}},{T_{cond}}} \right) \\
+&\cdot TeFIRfPLR(CPLR)
+\end{split}
+\end{equation}
+
+To make sure that the exhaust mass flow rate and temperature from microturbine are sufficient to drive the chiller, the heat recovery potential is compared with the cooling thermal energy input to the chiller (CoolThermalEergyInput). The heat recovery potential should be greater than the CoolThermalEnergyInput. Heat recovery potential is calculated as:
+
+\begin{equation}
+{Q_{Recovery}} = {\dot m_{ExhAir}} \cdot {\rm{}}C{p_{Air}} \cdot {\rm{}}({T_{a,o}} - {T_{Abs,gen,o}})
+\end{equation}
+
+T\(_{abs,gen,o}\) is the minimum temperature required for the proper operation of the double-effect chiller. It will be defaulted to 176°C.
+
+The electric input to cooling output ratio as function of temperature (\emph{CEIRfT}) curve represents the fraction of electricity to the chiller at full load as it varies with temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser fluid temperature.
+
+\begin{equation}
+CEIRfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}
+\end{equation}
+
+The electric input to cooling output ratio function of part load ratio (\emph{CEIRfPLR}) curve represents the fraction of electricity to the chiller as the load on the chiller varies at a given set of operating temperatures. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic.
+
+\begin{equation}
+CEIRfPLR = a + b \cdot CPLR + c \cdot CPL{R^2}
+\end{equation}
+
+The cooling electric input to the chiller is computed as follows:
+
+\begin{equation}
+CoolElectricPower = NomCoolCap \cdot RunFrac \cdot CEIR \cdot CEIRfT\left( {{T_{cw,l}},{T_{cond}}} \right) \cdot CEIRfPLR(CPLR)
+\end{equation}
+
+All five of these cooling performance curves are accessed through EnergyPlus' built-in performance curve equation manager (objects Curve:Linear, Curve:Quadratic and Curve:Biquadratic). It is not imperative that the user utilize all coefficients in the performance curve equations if their performance equation has fewer terms (e.g., if the user's \emph{TeFIRfPLR} performance curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero). A set of curves derived from manufacturer's data are also provided in the dataset (ExhaustFiredChiller.idf) is provided with E+ installation.
+
+The condenser load is computed as follows:
+
+\begin{equation}
+CondenserLoad = CoolingLoad + CoolThermalEnergyInput/HFIR + CoolElectricPower
+\end{equation}
+
+\subsubsection{Heating}\label{heating-1}
+
+The following nomenclature is used in the heating equations:
+
+\emph{AvailHeatCap}~~~~~~~~~ = ~~ available full-load heating capacity at current conditions {[}W{]}
+
+\emph{CPLRh}~~~~~~~~~~~~~~~~~~~~ = ~~ cooling part-load ratio for heating curve = \emph{CoolingLoad} / \emph{NomCoolCap}
+
+\emph{HeatCapfCPLR}~~~~~~~ = ~~ heating capacity factor as a function of cooling part load ratio, equal to 1 at zero cooling load, user input ``Heating Capacity Function of Cooling Capacity Curve Name''
+
+\emph{HeatCoolCapRatio~} = ~~ user input ``Heating to Cooling Capacity Ratio''
+
+\emph{HeatElectricPower}~~ = ~~ heating electricity input {[}W{]}
+
+\emph{HeatThermalEnergyInput} = heating thermal energy input {[}W{]}
+
+\emph{HeatingLoad}~~~~~~~~~~~ = ~~ current heating load on the chiller {[}W{]}
+
+\emph{HEIR}~~~~~~~~~~~~~~~~~~~~~~~ = ~~ user input ``Electric Input to Heating Output Ratio''
+
+\emph{HFIR}~~~~~~~~~~~~~~~~~~~~~~~ = ~~ user input ``Thermal Energy Input to Heating Output Ratio''
+
+\emph{HFIRfHPLR}~~~~~~~~~~~~ = ~~ thermal energy input to heating output factor, equal to 1 at full load, user input ``Thermal Energy Input to Heat Output Ratio During Heating Only Operation Curve Name''
+
+\emph{HPLR}~~~~~~~~~~~~~~~~~~~~~~ = ~~ heating part-load ratio = \emph{HeatingLoad} / \emph{AvailHeatCap}
+
+\emph{MinPLR~~~~~~~~~~~~~~~~~~~} = ~~ user input ``Minimum Part Load Ratio''
+
+\emph{NomCoolCap}~~~~~~~~~~ = ~~ user input ``Nominal Cooling Capacity'' {[}W{]}
+
+\emph{RunFrac}~~~~~~~~~~~~~~~~~~ = ~~ fraction of time step which the chiller is running
+
+\emph{TotalElectricPower~} = ~~ total electricity input {[}W{]}
+
+\emph{TotalThermalEnergyInput} = ~~~~~~~~~ total thermal energy input {[}W{]}
+
+Cooling is the primary purpose of the Exhaust Fired Absorption Chiller so that function is satisfied first and if energy is available for providing heating that is provided next.
+
+The two performance curves for heating capacity and efficiency are:
+
+1)~~~~Heating Capacity Function of Cooling Capacity Curve
+
+2)~~~~Thermal-Energy-Input-to Heat Output Ratio Function
+
+The heating capacity function of cooling capacity curve (\emph{HeatCapfCPLR}) determines how the heating capacity of the chiller varies with cooling capacity when the chiller is simultaneously heating and cooling. The curve is normalized so an input of 1.0 represents the nominal cooling capacity and an output of 1.0 represents the full heating capacity.~ An output of 1.0 should occur when the input is 0.0.
+
+\begin{equation}
+HeatCapfCPLR = a + b \cdot CPLRh + c \cdot CPLR{h^2}
+\end{equation}
+
+The available heating capacity is then computed as follows:
+
+\begin{equation}
+AvailHeatCap = NomCoolCap \cdot HeatCoolCapRatio \cdot HeatCapfCPLR(CPLRh)
+\end{equation}
+
+The thermal energy input to heat output ratio curve (\emph{HFIRfHPLR}) function is used to represent the fraction of thermal energy used as the heating load varies as a function of heating part load ratio. It is normalized so that a value of 1.0 is the full available heating capacity. The curve is usually linear or quadratic and will probably be similar to a boiler curve for most chillers.
+
+\begin{equation}
+HFIRfHPLR = a + b \cdot HPLR + c \cdot HPL{R^2}
+\end{equation}
+
+The thermal energy use rate when heating is computed as follows:
+
+\begin{equation}
+HeatThermalEnergyInput = AvailHeatCap.HFIR.HFIRfHPLR(HPLR)
+\end{equation}
+
+The fraction of the time step during which the chiller is operating is computed as a function of the cooling and heating part-load ratios and the user-input minimum part-load ratio:
+
+\begin{equation}
+RunFrac = MIN(1.0,MAX\left( {HPLR,CPLRh} \right)/MinPLR)
+\end{equation}
+
+The heating electric input to the chiller is computed as follows:
+
+\begin{equation}
+HeatElectricPower = NomCoolCap \cdot HeatCoolCapRatio \cdot HEIR.RunFrac
+\end{equation}
+
+If the chiller is delivering heating and cooling simultaneously, the parasitic electric load would be double-counted, so the following logic is applied:
+
+If HeatElectricPower is less than or equal to CoolElectricPower:
+
+\begin{equation}
+  HeatElectricPower = 0.0
+\end{equation}
+
+Else:
+
+\begin{equation}
+  HeatElectricPower = HeatElectricPower - CoolElectricPower
+\end{equation}
+
+The total thermal energy and electric power input to the chiller is computed as shown below:
+
+\begin{equation}
+TotalElectricPower = HeatElectricPower + CoolElectricPower
+\end{equation}
+
+\begin{equation}
+TotalThermalEnergyInput = HeatThermalEnergyInput + CoolThermalEnergyInput
+\end{equation}
+
+\subsubsection{References}\label{references-009}
+
+Personal communications with various absorption chiller manufacturers, March 2011.
+
+Absorption Chillers and Heat Pumps, Keith Herold, Reinhard Radermacher and Sanford A. Klein (Mar 18, 1996).
+
+Absorption systems for combined heat and power: The problem of part-load operation, ASHRAE Transactions, 2003, Vol 109, Part1.
+
+\subsection{Constant COP Chiller}\label{constant-cop-chiller}
+
+The input object Chiller:ConstantCOP provides a chiller model that is based on a simple, constant COP simulation of the chiller.~ In this case, performance does not vary with chilled water temperature or condenser conditions.~ The nominal capacity of the chiller and the COP are user specified along with the connections to the plant and condenser loop and mass flow rates.~ \emph{Such a model is useful when the user does not have access to detailed performance data.}
+
+The chiller power is calculated from the load divided by the COP.~ This chiller will meet the load as long as it does not exceed the nominal capacity specified by the user.
+
+~~~~~~~ QEvaporator = Load
+
+~~~~~~~ Power = Load / ConstCOPChiller(ChillNum)\%COP
+
+Then the evaporator temperatures are calculated from the load
+
+~~~~~~~ EvapDeltaTemp = QEvaporator/EvapMassFlowRate/CPwater
+
+~~~~~~~ EvapOutletTemp = Node(EvapInletNode)\%Temp - EvapDeltaTemp
+
+The condenser load and temperatures are calculated from the evaporator load and the power to the chiller.
+
+~~~~ QCondenser = Power + QEvaporator
+
+~~~~ IF (ConstCOPChiller(ChillNum)\%CondenserType = = WaterCooled) THEN
+
+~~~~~~ IF (CondMassFlowRate \textgreater{} WaterMassFlowTol) THEN
+
+~~~~~~~~ CondOutletTemp = QCondenser/CondMassFlowRate/CPCW(CondInletTemp) + CondInletTemp
+
+~~~~~~ ELSE
+
+~~~~~~~~ CALL ShowSevereError(`CalcConstCOPChillerModel: Condenser flow = 0, for CONST COP Chiller ='//~ \&
+
+~~~~~~ ~~~~~~~~~~~~~~~~~~~~~~~TRIM(ConstCOPChiller(ChillNum)\%Name))
+
+~~~~~~~~ CALL ShowContinueErrorTimeStamp(`')
+
+~~~~~~~~ CALL ShowFatalError(`Program Terminates due to previous error condition.')
+
+~~~~~~ END IF
+
+~~~ ELSE ! Air Cooled or Evap Cooled
+
+~~~~~~~~ !~ Set condenser outlet temp to condenser inlet temp for Air Cooled or Evap Cooled
+
+~~~~~~~~ !~ since there is no CondMassFlowRate and would divide by zero
+
+~~~~~ CondOutletTemp = CondInletTemp
+
+~~~ END IF
+
+See the InputOutput Reference for additional information.
+
+\subsubsection{Chiller Basin Heater}\label{chiller-basin-heater-1}
+
+This chiller's basin heater (for evaporatively-cooled condenser type) operates in the same manner as the Engine driven chiller's basin heater. The calculations for the chiller basin heater are described in detail at the end of the engine driven chiller description (Ref. Engine Driven Chiller).
+
+\subsection{Hot Water Heat Recovery from Chillers}\label{hot-water-heat-recovery-from-chillers}
+
++The electric chillers (e.g., Chiller:Electric, Chiller:EngineDriven, Chiller:CombustionTurbine, Chiller:Electric:EIR, and Chiller:Electric:ReformulatedEIR) all have the option of connecting a third plant loop for heating hot water at the same time the chiller cools the chilled water. The engine and combustion turbine chillers models include curves for heat recovery from oil and or jacket coolers. The other three chillers can model heat recovery where part of its condenser section is connected to a heat recovery loop for what is commonly known as a double bundled chiller, or single condenser with split bundles. The heat recovery chiller is simulated as a standard vapor compression refrigeration cycle with a double bundled condenser. A double bundle condenser involves two separate flow paths through a split condenser. One of these paths is condenser water typically connected to a standard cooling tower; the other path is hot water connected to a heat recovery loop. After leaving the compressor, the refrigerant is condensed to liquid in a refrigerant to water condenser. In a split bundle, the chiller's internal controls will direct a part of the refrigerant to heat recovery condenser bundle and/or to the tower water condenser bundle depending on the chilled water load, the condenser inlet temperatures and internal chiller controls (and possibly a leaving hot water temperature setpoint). The refrigerant pressure is then dropped through a throttling valve so that fluid can evaporate at a low pressure that provides cooling to the evaporator. Note that the heat recovery side of the chiller is placed on the demand-side of a heat recovery loop which will typically supply a hot water storage tank. Heat recovery is a passive benefit when the chiller is dispatched for cooling. The standard plant controls cannot dispatch the chiller based on a heat recovery requirement.
+
+\begin{figure}[hbtp] % fig 161
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image3175.png}
+\caption{Diagram of Chiller:Electric with Heat Recovery \protect \label{fig:diagram-of-chiller-electric-with-heat}}
+\end{figure}
+
+The algorithm for the heat recovery portion of the chiller needs to be determined from relatively simple inputs to estimate the amount of the heat that is recovered and then send the rest of the heat to the cooling tower. For the chiller models associated with the object Chiller:Electric,~ air- or evaporatively-cooled condensers are allowed to be used with heat recovery and, when used, the condenser specific heat, mass flow rate, and temperatures shown below refer to outdoor air. A condenser air volume flow rate must be specified when using heat recovery with air- or evaporatively-cooled chillers.
+
+The basic energy balance for the condenser section of a heat recovery chiller is
+
+\begin{equation}
+{\dot Q_{tot}} = {\dot Q_{Evap}} + {\dot Q_{Elec}} = {\dot Q_{Cond}} + {\dot Q_{HR}}
+\end{equation}
+
+In practice, if the entering temperature of the heat recovery hot fluid is too high, the chiller's internal controls will redirect refrigerant away from the heat recovery bundle.~ A user input is available for declaring the inlet high temperature limit, and if it is exceeded, the chiller will shut down heat recovery and request no flow and will not reject any condenser heat to that fluid.
+
+The heat recovery condenser bundle is often physically smaller than the tower water condenser bundle and therefore may have limited heat transfer capacity.~ User input for the relative capacity of the heat recovery bundle, \({F_{HR,Cap}}\) , is used to define a maximum rate of heat recovery heat transfer using
+
+\begin{equation}
+{\dot Q_{HR,Max}} = {F_{HR,Cap}}\left( {{{\dot Q}_{Evap,Ref}} + \frac{{{{\dot Q}_{Evap,Ref}}}}{{CO{P_{Ref}}}}} \right)
+\end{equation}
+
+This capacity factor is also used to autosize the heat recovery design fluid flow rate when it is set to autosize.~ The design heat recover flow rate is calculated by multiplying \({F_{HR,Cap}}\) ~by the condenser tower water design flow rate.~ If no capacity factor is input, it is assumed to be 1.0.
+
+A heat recovery chiller may control the temperature of heat recovery fluid leaving the device by modulating the flow of refrigerant to the heat recovery condenser bundle.~ There are two different algorithms used depending on if the input has declared a leaving setpoint node.
+
+If no control setpoint node was named, then the model developed by Liesen and Chillar (2004) is used to approximate the relative distribution of refrigerant flow and condenser heat transfer between the bundles.~ This model approximates the heat transfer situation by using average temperatures in and out of the condenser section.
+
+\begin{equation}
+{Q_{Tot}} = ({\dot m_{Heat{\mathop{\rm Re}\nolimits} c}}*C{p_{Heat{\mathop{\rm Re}\nolimits} c}} + {\dot m_{Cond}}*C{p_{Cond}})*({T_{AvgOut}} - {T_{AvgIn}})
+\end{equation}
+
+Then the inlet temperature is flow-weighted to determine lumped inlet and outlet conditions.
+
+\begin{equation}
+{T_{AvgIn}} = \frac{{({{\dot m}_{Heat{\mathop{\rm Re}\nolimits} c}}*C{p_{Heat{\mathop{\rm Re}\nolimits} c}}*{T_{Heat{\mathop{\rm Re}\nolimits} cIn}} + {{\dot m}_{Cond}}*C{p_{Cond}}*{T_{CondIn}})}}{{({{\dot m}_{Heat{\mathop{\rm Re}\nolimits} c}}*C{p_{Heat{\mathop{\rm Re}\nolimits} c}} + {{\dot m}_{Cond}}*C{p_{Cond}})}}
+\end{equation}
+
+\begin{equation}
+{T_{AvgOut}} = \frac{{{Q_{Tot}}}}{{({{\dot m}_{Heat{\mathop{\rm Re}\nolimits} c}}*C{p_{Heat{\mathop{\rm Re}\nolimits} c}} + {{\dot m}_{Cond}}*C{p_{Cond}})}} + {T_{AvgIn}}
+\end{equation}
+
+The lumped outlet temperature is then used for an approximate method of determining the heat recovery rate
+
+\begin{equation}
+{\dot Q_{HR}} = {\dot m_{HR}}{c_p}_{HR}\left( {{T_{Avg,out}} - {T_{HR,in}}} \right)
+\end{equation}
+
+This rate is then limited by the physical size of the heat recovery bundle.
+
+\begin{equation}
+{\dot Q_{HR}} = Min\left( {{{\dot Q}_{HR}},{{\dot Q}_{HR,max}}} \right)
+\end{equation}
+
+If user input for the leaving temperature setpoint is available, then a second model is used to distribute refrigerant flow and condenser heat transfer between the bundles that attempts to meet the heat recovery load implied by the leaving setpoint.~ When setpoint control is used, the desired rate of heat recovery heat transfer is:
+
+\begin{equation}
+{\dot Q_{HR,Setpoint}} = {\dot m_{HR}}{c_p}_{HR}\left( {{T_{HR,set}} - {T_{HR,in}}} \right)
+\end{equation}
+
+\begin{equation}
+{\dot Q_{HR,Setpoint}} = Max\left( {{{\dot Q}_{HR,Setpoint}},0.0} \right)
+\end{equation}
+
+Then the heat recovery rate is simply modeled as the lower of the three different heat flow rates:~ the desired capacity, the maximum capacity, and the current total heat rejection rate.
+
+\begin{equation}
+{\dot Q_{HR}} = Min\left( {{{\dot Q}_{HR,Setpoint}},{{\dot Q}_{HR,max}},{{\dot Q}_{Tot}}} \right)
+\end{equation}
+
+For both models, the condenser heat transfer rate is then
+
+\begin{equation}
+{\dot Q_{Cond}} = {\dot Q_{Tot}} - {\dot Q_{HR}}
+\end{equation}
+
+The outlet temperatures are then calculated using
+
+\begin{equation}
+  T_{HR,out} = T_{HR,in} + \frac{\dot{Q}_{HR}}{\dot{m}_{HR}C_{p,HR}}
+\end{equation}
+
+\begin{equation}
+  T_{Cond,out} = T_{Cond,in} + \frac{\dot{Q}_{Cond}}{\dot{m}_{Cond}C_{p,Cond}}
+\end{equation}
+
+A heat recovery chiller may need to work harder because the refrigeration system faces a higher lift owing to an elevated effective temperature for heat rejection.~ With heat recovery, the condenser temperature used with the chiller's performance curves is determined using one of the following heat-flow-weighted methods. The first is used for the chiller model for the objects Chiller:Electric, and Chiller:Electric:EIR which use the condensing entering temperature for performance.
+
+\begin{equation}
+{T_{Cond,in,Avg}} = \frac{{\left( {{{\dot Q}_{HR}}{T_{HR,in}} + {{\dot Q}_{Cond}}{T_{Cond,in}}} \right)}}{{\left( {{{\dot Q}_{HR}} + {{\dot Q}_{Cond}}} \right)}}
+\end{equation}
+
+The second is used for the chiller model for the object Chiller:Electric:ReformulatedEIR which uses the leaving condenser fluid temperature.
+
+\begin{equation}
+{T_{Cond,out,Avg}} = \frac{{\left( {{{\dot Q}_{HR}}{T_{HR,out}} + {{\dot Q}_{Cond}}{T_{Cond,out}}} \right)}}{{\left( {{{\dot Q}_{HR}} + {{\dot Q}_{Cond}}} \right)}}
+\end{equation}
+
+Both of these are available as an output variable called Chiller Effective Heat Rejection Tempeature, in C.
+
+\subsubsection{Chiller Basin Heater}\label{chiller-basin-heater-2}
+
+This chiller's basin heater (for evaporatively-cooled condenser type) operates in the same manner as the Engine driven chiller's basin heater. The calculations for the chiller basin heater are described in detail at the end of the engine driven chiller description (Ref. Engine Driven Chiller).
+
+\textbf{Reference}
+
+Leisen and Chillar. 2004. Variable Heat Recovery In Double Bundle Electric Chillers. SimBuild 2004, IBPSA-USA National Conference Boulder, CO, August 4-6, 2004.
+
+\subsection{Electric Chiller Model Based on Fluid Temperature Differences}\label{electric-chiller-model-based-on-fluid-temperature-differences}
+
+The centrifugal chiller model (object name Chiller:Electric) was originally developed for the BLAST program.~ The model is based on a `capacity ratio' curve, which is a quadratic equation that determines the Ratio of Available Capacity to Nominal Capacity. The defining equation is:
+
+\begin{equation}
+CapRatio = \frac{{Available Chiller Capacity}}{{Nominal Chiller Capacity}} = {A_1} + {A_2}\Delta {T_{chiller}} + {A_3}\Delta {T_{chiller}}^2
+\end{equation}
+
+Where the Delta Temperature is defined as:
+
+\begin{equation}
+\Delta {T_{chiller}} = \frac{{{T_{cond, in}} - {T_{cond,in,design}}}}{{TempRiseRatio}} - \left( {{T_{evap,out}} - {T_{evap,out,design}}} \right)
+\end{equation}
+
+where the temperature rise coefficient is defined as the ratio of the required change in condenser water temperature to a given change in chilled water temperature, which maintains the capacity at the nominal value.~ If the chiller is a heat recovery chiller,then the condenser inlet temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers. This is calculated as the following ratio:
+
+\begin{equation}
+TempRiseRatio = \frac{{{T_{cond, in,required}} - {T_{cond,in,rated}}}}{{{T_{evap, out,required}} - {T_{evap,out,rated}}}} - \left( {{T_{evap,out}} - {T_{evap,out,design}}} \right)
+\end{equation}
+
+Where:
+
+\emph{T\(_{cond,in,required}\)} = Required entering condenser air or water temperature to maintain rated capacity (C)
+
+\emph{T\(_{cond,in,rated}\)} = Rated entering condenser air or water temperature at rated capacity (C)
+
+\emph{T\(_{evap,out,required}\)} = Required leaving evaporator water outlet temperature to maintain rated capacity (C)
+
+\emph{T\(_{evap,out,rated}\)} = Rated leaving evaporator water outlet temperature at rated capacity (C)
+
+The Power Ratio Curve is a quadratic equation that determines the Ratio of Full Load to Power.~ The defining equation is:
+
+\begin{equation}
+PowerRatio = {B_1} + {B_2}PLR + {B_3}PL{R^2}
+\end{equation}
+
+where the part load ratio, PLR is defined as:
+
+\begin{equation}
+PLR = \frac{{chiller cooling load}}{{nominal chiller capacity}}
+\end{equation}
+
+The Load Ratio Curve is a quadratic equation that determines the Ratio of Actual Cooling Load to Full Cooling Load.~ The defining equation is:
+
+\begin{equation}
+LoadRatio = {C_1} + {C_2}CapRatio + {C_3}CapRati{o^2}
+\end{equation}
+
+The evaporator heat transfer rate and the power required by the chiller are then calculated as:
+
+\begin{equation}
+Qevap = AvailableChillerCap*PLR
+\end{equation}
+
+\begin{equation}
+Power = PowerRatio*LoadRatio*\frac{{AvailableChillerCap}}{{RatedCOP}}
+\end{equation}
+
+\subsection{Electric Chiller Model Based on Condenser Entering Temperature}\label{electric-chiller-model-based-on-condenser-entering-temperature}
+
+\subsubsection{Overview}\label{overview-2-003}
+
+This model (object name Chiller:Electric:EIR) simulates the performance of an electric liquid chiller. The model is based on the compression chiller model (COMREF) in the DOE-2.1 building energy simulation program. The EnergyPlus model contains all of the features of the DOE-2.1 chiller model, plus additional abilities for modeling evaporatively-cooled condensers and heat recovery for water heating.
+
+This model simulates the thermal performance of the chiller and the power consumption of the compressor(s). It also models the power consumption of condenser fans if modeling an air-cooled or evaporatively-cooled condenser. This model does not simulate the thermal performance or the power consumption of associated pumps or cooling towers. This auxiliary equipment must be modeled using other EnergyPlus models (e.g.~CoolingTower:SingleSpeed).
+
+\subsubsection{Model Description}\label{model-description-2-003}
+
+The chiller model uses user-supplied performance information at reference conditions along with three performance curves (curve objects) for cooling capacity and efficiency to determine chiller operation at off-reference conditions. The three performance curves are:
+
+1)~~~~Cooling Capacity Function of Temperature Curve
+
+2)~~~~Energy Input to Cooling Output Ratio Function of Temperature Curve
+
+3)~~~~Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve
+
+·~~~~~~~~The cooling capacity function of temperature curve is a biquadratic performance curve with two independent variables: the leaving chilled water temperature and the entering condenser fluid temperature. The output of this curve is multiplied by the reference capacity to give the full-load cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation. If the chiller is a heat recovery chiller,then the condenser inlet temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers.
+
+\(ChillerCapFTemp = a + b\left( {{T_{cw,l}}} \right) + c{\left( {{T_{cw,l}}} \right)^2} + d\left( {{T_{cond,e}}} \right) + e{\left( {{T_{cond,e}}} \right)^2} + f\left( {{T_{cw,l}}} \right)\left( {{T_{cond,e}}} \right)\) where
+
+\emph{ChillerCapFTemp} = cooling capacity factor, equal to 1 at reference conditions
+
+\emph{T\(_{cw,l}\)}~~~~~~~~~~~ = leaving chilled water temperature, ËšC
+
+\emph{T\(_{cond,e}\)}~~~~~~~~ = entering condenser fluid temperature, ËšC. For a water-cooled condenser this will be the water temperature returning from the condenser loop (e.g., leaving the cooling tower). For air- or evap-cooled condensers this will be the entering outdoor air dry-bulb or wet-bulb temperature, respectively.
+
+·~~~~~~~~The energy input to cooling output ratio function of temperature curve is a biquadratic performance curve that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and the entering condenser fluid temperature. The EIR is the inverse of the COP. The output of this curve is multiplied by the reference EIR (inverse of the reference COP) to give the full-load EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\begin{equation}
+ChillerEIRFTemp = a + b\left( {{T_{cw,l}}} \right) + c{\left( {{T_{cw,l}}} \right)^2} + d\left( {{T_{cond,e}}} \right) + e{\left( {{T_{cond,e}}} \right)^2} + f\left( {{T_{cw,l}}} \right)\left( {{T_{cond,e}}} \right)
+\end{equation}
+
+where
+
+\emph{ChillerEIRFTemp} = energy input to cooling output factor, equal to 1 at reference conditions
+
+\emph{T\(_{cw,l}\)}~~~~~ = leaving chilled water temperature, ËšC
+
+\emph{T\(_{cond,e}\)} = entering condenser fluid temperature, ËšC. For a water-cooled condenser this will be the water temperature returning from the condenser loop (e.g., leaving the cooling tower). For air- or evap-cooled condensers this will be the entering outdoor air dry-bulb or wet-bulb temperature, respectively. If the chiller is a heat recovery chiller,then the condenser inlet temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers.
+
+·~~~~~~~~The energy input to cooling output ratio function of part-load ratio curve is a quadratic performance curve that parameterizes the variation of the chiller input power ratio as a function of the part-load ratio. The part-load ratio is the actual cooling load divided by the chiller's available cooling capacity. The output of this curve is multiplied by the reference EIR (inverse of the reference COP) and the Energy Input to Cooling Output Ratio Function of Temperature Curve to give the EIR at the specific temperatures and part-load ratio at which the chiller is operating. This curve should have a value of 1.0 when the part-load ratio equals 1.0. The quadratic curve should be valid for the range of part-load ratios anticipated for the simulation.
+
+\begin{equation}
+  \begin{array}{rl}
+    ChillerEIRFPLR &= a + b\PB{PLR} + c\PB{PLR}^2\\
+                   &= \frac{P_{chiller}}{P_{ref}}\left( {ChillerCapFTemp} \right)\left( {ChillerEIRFTemp} \right)
+  \end{array}
+\end{equation}
+
+where
+
+\emph{ChillerEIRFPLR} = energy input to cooling output factor, equal to 1 at reference conditions
+
+\emph{PLR} = part-load ratio = (cooling load) / (chiller's available cooling capacity)
+
+\emph{P\(_{chiller}\) = chiller power at specific PLR}
+
+\emph{P\(_{ref}\) = \({\mathop Q\limits^ \bullet_{ref}}\) /COP\(_{ref}\)}
+
+All three of the performance curves are accessed through EnergyPlus' built-in performance curve equation manager (curve:quadratic and curve:biquadratic). It is not imperative that the user utilize all coefficients in the performance curve equations if their performance equation has fewer terms (e.g., if the user's ChillerEIRFPLR performance curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero). Performance curves for more than 160 chillers, including the default DOE-2.1E reciprocating and centrifugal chillers, are provided in the EnergyPlus Reference DataSets (Chillers.idf and AllDataSets.idf).
+
+Note: Chiller:Electric:EIR objects and their associated performance curve objects are developed using performance information for a specific chiller and should normally be used together for an EnergyPlus simulation. Changing the object input values, or swapping performance curves between chillers, should be done with caution.
+
+For any simulation time step, the chiller's available cooling capacity is calculated as follows:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{avail}}\,\, = \,\,{\mathop Q\limits^ \bullet_{ref}}\left( {ChillerCapFTemp} \right)
+\end{equation}
+
+where
+
+\({\mathop Q\limits^ \bullet_{ref}}\) ~~~~ = chiller capacity at reference conditions (reference temperatures and flow rates defined by the user), W
+
+\(\mathop Q\limits^ \bullet avail\) ~ = available chiller capacity adjusted for current fluid temperatures, W
+
+The model then calculates the evaporator heat transfer rate required to bring the entering chilled water temperature down to the leaving chilled water setpoint temperature (established using a SetpointManager object and referenced in the PlantLoop object). If this calculated heat transfer rate is greater than the heat transfer rate being requested by the plant equipment operation scheme, then the evaporator heat transfer rate is reset to the requested cooling rate.
+
+The evaporator heat transfer rate is then compared to the available capacity. If the available chiller capacity is sufficient to meet the evaporator heat transfer rate, the leaving chilled water temperature is set equal to the chilled water setpoint temperature. If the requested evaporator heat transfer rate is larger than the available capacity the chilled water leaving the evaporator is allowed to float upward. For this case, the exiting chilled water temperature is calculated based on the water temperature entering the evaporator, the available cooling capacity, and the evaporator mass flow rate as follows:
+
+\begin{equation}
+  T_{cw,l} = T_{cw,e} - \frac{\dot{Q}_{avail}}{\dot{m}_{evap}C_{p,evap}}
+\end{equation}
+
+where
+
+\emph{T\(_{cw,l}\)}~~~~~~~~~~~ = water temperature leaving the evaporator, ËšC
+
+\emph{T\(_{cw,e}\)}~~~~~~~~~~ = water temperature entering the evaporator, ËšC
+
+\({\mathop m\limits^ \bullet_{evap}}\) ~~~~~~~~ = evaporator mass flow rate, kg/s
+
+\emph{C\(_{p,evap}\)}~~~~~~~~ = specific heat of water entering evaporator at \emph{T\(_{cw,e}\)}, J/kg-ËšC
+
+The part-load ratio is then calculated as the ratio of the evaporator heat transfer rate to the available chiller capacity. The part-load ratio is not allowed to be greater than the maximum part-load ratio specified by the user or less than zero as follows:
+
+\begin{equation}
+  PLR = \max\PB{0.0,\min\PB{\frac{\dot{Q}_{evap}}{\dot{Q}_{avail}},PLR_{max}}}
+\end{equation}
+
+where
+
+\emph{PLR}~~~~~~~~~~ = part-load ratio
+
+\({\mathop Q\limits^ \bullet_{evap}}\) ~~~~~~~~ = load to be met by the chiller, W
+
+\emph{PLR\(_{max}\)} = maximum part-load ratio (specified by the user in the input data file)
+
+The model assumes that the cooling load is met through chiller unloading down to the minimum unloading ratio. False loading (e.g.~hot-gas bypass) is assumed to occur between the minimum unloading ratio and the minimum part load ratio yielding constant electrical power consumption under these conditions. Below the minimum part load ratio, the chiller cycles on and off to meet very small loads and the power consumption during the on cycle is the same as when the chiller is operating at the minimum part load ratio. When the chiller part load ratio is less than the minimum part load ratio, the on-off cycling ratio of the chiller is calculated as follows and is available as an output variable.
+
+\begin{equation}
+  ChillerCyclingRatio = \min\PB{\frac{PLR}{PLR_{min}},1.0}
+\end{equation}
+
+To properly account for chiller electric power consumption when PLR is less than the minimum unloading ratio, the PLR is reset to the greater of the PLR calculated above and the PLR at the minimum unloading ratio. The result is available as the output variable Chiller Part Load Ratio.
+
+\begin{equation}
+PLR = MAX(PLR,PL{R_{MinUnloadRatio}})
+\end{equation}
+
+This revised PLR accounts for the ``false loading'' (e.g., hot gas bypass) that is assumed to occur whenever the PLR (based on cooling load divided by available capacity) is less than the minimum unloading ratio specified. The amount of false loading on the chiller is calculated using this revised PLR and is reported as an output variable as follows:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{falseloading}} = \left( {{{\mathop Q\limits^ \bullet  }_{avail}}} \right)\left( {PLR} \right)\left( {ChillerCyclingRatio} \right) - {\mathop Q\limits^ \bullet_{evap}}
+\end{equation}
+
+The electrical power consumption for the chiller compressor(s) for any simulation time step is then calculated using the following equation:
+
+\({P_{chiller}}\, = \,\,\left( {{{\mathop Q\limits^ \bullet }_{avail}}\,} \right)\,\left( {\frac{1}{{CO{P_{ref}}}}} \right)\,\left( {ChillerEIRFTemp} \right)\left( {ChillerEIRFPLR} \right)\left( {ChillerCyclingRatio} \right)\) where
+
+\emph{P\(_{chiller}\)}~~~~~~~~ = chiller compressor power, W
+
+\emph{COP\(_{ref}\)}~~~~~~ = reference coefficient of performance, W/W
+
+Heat rejected by the chiller condenser includes the heat transferred in the evaporator plus a portion or all of the compressor electrical energy consumption. For electric chillers with hermetic compressors, all compressor energy consumption is rejected by the condenser (compressor motor efficiency = \emph{eff\(_{motor}\)} = 1.0). For chillers with semi-hermetic or open compressors, only a portion of the compressor energy use is rejected by the condenser. The heat transfer rate for the chiller condenser is calculated as follows:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{cond}} = \left( {{P_{chiller}} * ef{f_{motor}}} \right) + {\mathop Q\limits^ \bullet_{evap}} + {\mathop Q\limits^ \bullet_{falseloading}}
+\end{equation}
+
+where
+
+\({\mathop Q\limits^ \bullet_{cond}}\) ~~~~~~~~ = condenser heat transfer rate, W
+
+\(ef{f_{motor}}\) ~~~~~~ = compressor motor efficiency = fraction of compressor electrical energy consumption rejected as condenser heat
+
+For water-cooled chillers, the water temperature leaving the condenser is then calculated as shown below.
+
+\begin{equation} 
+  T_{cond,l} = T_{cond,e} + \frac{\dot{Q}_{cond}}{\dot{m}_{cond}C_{p,cond}}
+\end{equation}
+
+where:
+
+\emph{T\(_{cond,l}\)}~~~~~~~~~ = water temperature leaving the condenser, ËšC
+
+\emph{T\(_{cond,e}\)}~~~~~~~~ = water temperature entering the condenser, ËšC
+
+\({\mathop m\limits^ \bullet_{cond}}\) ~~~~~~~~ = mass flow rate through the condenser, kg/s
+
+\({C_{p,cond}}\) ~~~~~~ = specific heat of water entering the condenser at \emph{T\(_{cond,e}\)}, J/kg-ËšC
+
+For air- and evaporatively-cooled condensers, the exiting air temperature is not calculated and is set equal to the entering air or wet-bulb temperature, respectively.
+
+The model then calculates the condenser fan energy for air- and evaporatively-cooled condensers. The amount of condenser fan energy is assumed to be proportional to the chiller cycling ratio and is calculated as follows:
+
+\begin{equation}
+{P_{cond}}\, = \,{\mathop Q\limits^ \bullet_{ref}}\,\left( {{P_{condfanratio}}} \right)\,\left( {ChillerCyclingRatio} \right)
+\end{equation}
+
+where
+
+\emph{P\(_{cond}\)}~~~~~~~~~~ = chiller condenser fan electric power, W
+
+\emph{P\(_{condfanratio}\)}~~ = condenser fan power ratio, W/W
+
+The final calculations determine the total heat transfer energy for the condenser and evaporator, as well as the total electric energy consumed by the chiller compressor motor(s) and condenser fan(s). The results are available as output variables.
+
+\begin{equation}
+{Q_{cond}} = {\mathop Q\limits^ \bullet_{cond}}*TimeStepSys*3600
+\end{equation}
+
+\begin{equation}
+{Q_{evap}} = {\mathop Q\limits^ \bullet_{evap}}\,\,*\,\,TimeStepSys\,\,*\,\,3600
+\end{equation}
+
+\begin{equation}
+{E_{chiller}} = {P_{chiller}}*\,\,TimeStepSys\,\,*\,\,3600
+\end{equation}
+
+\begin{equation}
+{E_{cond}} = {P_{cond}}\,\, * \,\,TimeStepSys\,\,*\,\,3600
+\end{equation}
+
+where
+
+\emph{Q\(_{cond}\)}~~~~~~~~~ = chiller condenser heat transfer energy, J
+
+\emph{Q\(_{evap}\)}~~~~~~~~~~ = chiller evaporator cooling energy, J
+
+\emph{E\(_{chiller}\)}~~~~~~~~ = chiller (compressor) electric energy, J
+
+\emph{E\(_{cond}\)}~~~~~~~~~~ = chiller condenser fan electric energy, J
+
+\emph{TimeStepSys} = HVAC system simulation time step, hr
+
+\(3600\) ~~~~~~~~ = conversion factor, sec/hr
+
+\subsubsection{Electric EIR Chiller with Heat Recovery Option}\label{electric-eir-chiller-with-heat-recovery-option}
+
+Heat from the electric EIR chiller condenser may be recovered when a water-cooled condenser is selected for simulation. The heat recovery water flow rate is specified by the user along with the input and output nodes connected to the heat recovery loop. The algorithms are identical to those used for Chiller:Electric. Refer to the section entitled Chillers with Plant Heat Recovery for details.
+
+\subsubsection{Standard Rating (Integrated Part Load Value)}\label{standard-rating-integrated-part-load-value}
+
+For the Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR objects in EnergyPlus, the industry standard rating of Integrated Part Load Value (IPLV) is calculated according to ANSI/AHRI Standard 550/590 (2011). This standard rating is not direct input to the model and is calculated using user-entered information for these objects. These standard rating values are provided in the eplusout.eio output file (Ref. Output Details document) and also in the predefined tabular output reports (Output:Table:SummaryReports object, Equipment Summary).
+
+\begin{callout}
+Note: The standard ratings described in this section require that the EIR/Reformulated EIR chiller models be evaluated at specific operating conditions (e.g., specific evaporator outlet temperature (6.67 C) and dry-bulb temperatures for air entering the air-cooled {[}outdoor{]} condenser). If the chiller~ performance curves can not be evaluated at the required test conditions, then the standard rating value will be determined at user specified curve limit and warning error message is provided. For example, if the curve object (Curve:Biquadratic) for Cooling Capacity Function of Temperature Curve has a minimum value of 21C for dry-bulb temperature entering the air-cooled condenser coil, the IPLV calculation requires that EER\(_{D}\) be calculated at 13 C -- so, this would result in IPLV value calculated at 21C and reported in the output and a warning message in the eplusout.err file.
+\end{callout}
+
+The IPLV is a single number part-load performance figure of merit for Water-Chilling Packages. The IPLV equations and procedures described below are taken from Appendix D of ANSI/AHRI Std. 550/590, 2011 and provide a consistent method for calculating IPLV. These equations provide representative average part-load efficiency for a single chiller. ~For equipment covered by this standard, the \emph{IPLV} is calculated using the following formula:
+
+\begin{equation}
+IPLV = (0.01A) + (0.42B) + (0.45C) + (0.12D)
+\end{equation}
+
+where,
+
+\(A\) ~ = ~~ \emph{EER} or \emph{COP} at 100\% capacity at AHRI standard rating conditions
+
+\(B\) ~ = ~~ \emph{EER} or \emph{COP} at 75\% capacity and reduced ambient (see Table~\ref{table:standard-rating-integrated-part-load-value})
+
+\(C\) ~ = ~~ \emph{EER} or \emph{COP} at 50\% capacity and reduced ambient (see Table~\ref{table:standard-rating-integrated-part-load-value})
+
+\(D\) ~ = ~~ \emph{EER} or \emph{COP} at 25\% capacity and reduced ambient (see Table~\ref{table:standard-rating-integrated-part-load-value})
+
+The Coefficient of Performance (\emph{COP}) at the various load capacity points (100\%, 75\%, 50\%, and 25\% part-load ratios) are calculated using the procedure outlined below and applicable test conditions specified in Table~\ref{table:standard-rating-integrated-part-load-value}.
+
+EER at desired reduced capacity (75\%, 50\%, and 25\%) is calculated as follows
+
+\begin{equation}
+COP = \frac{{\rm{1}}}{{EIR}}
+\end{equation}
+
+\begin{equation}
+EIR = EnergyInputRatio = \left( {\frac{{{\rm{Power }}}}{{{\rm{PartLoadRatio * AvailChillerCap}}}}} \right)
+\end{equation}
+
+\begin{equation}
+Power = \left( {\frac{{{\rm{AvailChillerCap}}}}{{CO{P_{reference}}}}} \right)(EIRTempModFa{c_{ReducedTemp}})(EIRPLRModFa{c_{ReducedPLR}})
+\end{equation}
+
+\begin{equation}
+AvailChillerCap = Capacit{y_{reference}}(CAPTempModFa{c_{ReducedTemp}})
+\end{equation}
+
+\(Capacit{y_{reference}}\) = Reference chiller capacity specified by the user, (W).
+
+\(CO{P_{reference}}\) = Reference coefficient of performance specified by the user, (W/W).
+
+\(EIRTempModFa{c_{ReducedTemp}}\) = User-specified bi-quadratic curve for modifying EIR as a function of leaving chilled water temperature (6.7°C) and entering condenser temperature obtained from Table~\ref{table:standard-rating-integrated-part-load-value} for reduced capacities, (dimensionless).
+
+\(EIRPLRModFa{c_{ReducedPLR}}\) = User-specified quadratic curve for modifying EIR as a function of part load ratio.
+
+\(CapTempModFa{c_{ReducedTemp}}\) = Capacity (W) of the chiller determined per the ANSI/AHRI Standard 550/590 reduced ambient test conditions as shown in Table~\ref{table:standard-rating-integrated-part-load-value}.
+
+If the equipment cannot be unloaded to the desired reduced capacity (75\%, 50\%, and 25\%) i.e.~if the minimum unloading ratio of the chiller is greater than desired reduced capacity, then the model is run at the minimum unloading PLR of the equipment at the condenser entering conditions defined in Table~\ref{table:standard-rating-integrated-part-load-value} and the efficiency is adjusted for cyclic performance.
+
+\begin{equation}
+COP = \frac{{\rm{1}}}{{{C_D} \cdot EIRatMinPLR}}
+\end{equation}
+
+~where,
+
+\(EIRatMinPLR\) = EIR of chiller at minimum unloading ratio
+
+\({C_D}\) = degradation coefficient to account for cycling of the compressor for capacity less than the minimum capacity.
+
+Thedegradation coefficient \emph{C\(_{D}\)} for the desired reduced load points (75\%, 50\%, or 25\%) is determined using the following equation:
+
+\begin{equation}
+{C_D} = 1.13 - 0.13LF
+\end{equation}
+
+The load factor (\emph{LF}) for the desired reduced load points (75\%, 50\%, or 25\%) calculated from the following equation:
+
+\begin{equation}
+LF = \frac{{\left( {\frac{{\% Load}}{{100}}} \right) \cdot Full{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity}}{{Part{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity}}
+\end{equation}
+
+Where,
+
+\emph{\(\left( {\frac{{\% Load}}{{100}}} \right)\)}~~~~~~~~~~~ = ~~~~~~~~ standard rating part load ratio (\emph{PLR}) points, 75\%, 50\%, 25\%.
+
+\(Full{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity\) ~ = ~~~~~~~~~~~ Full load heating capacity (W) of the air-source heat pump equipment determined from ANSI/AHRI Standard 550/590 and test conditions shown in Table~\ref{table:standard-rating-integrated-part-load-value} for 100\% load.
+
+\(Part{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity\) ~ = ~~~~~~~~~~ Part load heating capacity (W) of the air-source heat pump units determined from ANSI/AHRI Standard 550/590 at the standard desired reduced ambient test conditions as shown in Table~\ref{table:standard-rating-integrated-part-load-value} ~and the minimum part load capacity of the unit.
+
+\begin{equation}
+Full{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity = {\dot Q_{total,Reference}}\left( {CapTempModFa{c_{Rated}}} \right)
+\end{equation}
+
+\begin{equation}
+Part{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity = MinPLR \cdot {\dot Q_{total,Reference}}\left( {CapTempModFa{c_{ReducedTemp}}} \right)
+\end{equation}
+
+where,
+
+\({\dot Q_{total,Reference}}\) ~ = Reference capacity specified by the user, (W).
+
+\(CapTempModFa{c_{Rated}}\) = User-specified bi-quadratic curve evaluated at full load (100\%) test conditions shown in Table~\ref{table:standard-rating-integrated-part-load-value}, (dimensionless).
+
+\(CapTempModFa{c_{ReducedTemp}}\) = Part load capacity (W) of the chiller determined from ANSI/AHRI Standard 550/590 at the standard desired reduced ambient test conditions as shown in Table~\ref{table:standard-rating-integrated-part-load-value}.
+
+\(MinPLR\) = Minimum PLR up to which chiller can be unloaded
+
+% table 51
+\begin{longtable}[c]{p{1.2in}p{1.2in}p{1.2in}p{1.2in}p{1.2in}}
+\caption{Standard Rating (Integrated Part Load Value) \label{table:standard-rating-integrated-part-load-value}} \tabularnewline
+\toprule
+ & \multicolumn{2}{c}{IPLV} & \multicolumn{2}{c}{NPLV} \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Standard Rating (Integrated Part Load Value)} \tabularnewline
+\toprule
+ & \multicolumn{2}{c}{IPLV} & \multicolumn{2}{c}{NPLV} \tabularnewline
+\midrule
+\endhead
+
+Evaporator (All types)  100 \% Load LWT  0\% Load LWT  Flow Rate (gpm)  F.F.A & 2 44.0°F  44.0°F  3 2.4 gpm/ton  0.0001  h- ft 2 -°F/Btu & 6.7°C  6.7°C  0.043 L/s per  kW  0.000018  m 2 -°C/W & 2 Selected LWT  Same as 100\%  load  3 Selected  gpm/ton  As Specified & 2 Selected  LWT  Same as 100\%  load  3 [L/s per kW]  As Specified \tabularnewline
+1 Condenser (Water  Cooled)  100\% load EWT  75\% load EWT  50\% load EWT  25\% load EWT  0\% load EWT  Flow rate (gpm) [L/s]  F.F.A. & 2 85.0°F  75.0°F  65.0°F  65.0°F  65.0°F  3 3.0 gpm/ton  0.00025  h- ft 2 -°F/Btu & 29.4°C  23.9°C  18.3°C  18.3°C  18.3°C  0.054 L/s per  kW  0.000044  m 2 -°C/W & 2 Selected LWT  4 65.0°F  3 Selected  gpm/ton  As Specified & 2 Selected LWT  4 18.3°C  3 Selected  L/s per kW  As Specified \tabularnewline
+1 Condenser (Air Cooled)  100\% load EDB  75\% load EDB  50\% load EDB  25\% load EDB  0\% load EDB  F.F.A. & 95.0°F  80.0°F  65.0°F  55.0°F  55.0°F  0.0 h- ft 2  -°F/Btu & 35°C  26.7°C  18.3°C  12.8°C  12.8°C  0.0 m 2 -°C/W & \multicolumn{2}{l}{No Rating Requirements} \tabularnewline
+1 Condenser  (Evaporatively Cooled)  100\% load EWB  0\% load EWB  F.F.A. & 75.0°F  50.0°F  0.0 h- ft 2  -°F/Btu & 23.9°C  10.0°C  0.0 m 2 -°C/W & \multicolumn{2}{l}{No Rating Requirements} \tabularnewline
+Air-Cooled Without  Condenser  100\% load SDT  0\% load SDT & 125.0°F  55.0°F & 51.7°C  12.8°C & \multicolumn{2}{l}{No Rating Requirements} \tabularnewline
+Water and Evaporatively-  Cooled Without  Condenser  100\% load SDT  0\% load SDT & 105.0°F  65.0°F & 40.6°C  18.3°C & \multicolumn{2}{l}{No Rating Requirements} \tabularnewline
+\bottomrule
+\multicolumn{5}{l}{1 If the unit Manufacturer’s recommended minimum temperatures are greater than those} \tabularnewline
+\multicolumn{5}{l}{specified in  Table 3, then those may be used in lieu of the specified temperatures.} \tabularnewline
+\multicolumn{5}{l}{2 Correction for Fouling Factor Allowance} \tabularnewline
+\multicolumn{5}{l}{3 The flow rates are to be held constant at full load values for all part-load conditions.} \tabularnewline
+\multicolumn{5}{l}{4 For part-load entering condenser water temperatures, the temperature should vary} \tabularnewline
+\multicolumn{5}{l}{linearly from  the selected} \tabularnewline
+\multicolumn{5}{l}{EWT at 100\% load to 65.0 oF at 50\% loads, and fixed at 65.0°F for 50\% to 0\% loads.} \tabularnewline
+\multicolumn{5}{l}{SDT - saturated discharge temperature} \tabularnewline
+\multicolumn{5}{l}{LWT - leaving water (liquid) temperature} \tabularnewline
+\multicolumn{5}{l}{EWT - entering water (liquid) temperature} \tabularnewline
+\multicolumn{5}{l}{EDB - entering air dry-bulb temperature} \tabularnewline
+\multicolumn{5}{l}{EWB - entering air wet-bulb temperature} \tabularnewline
+\multicolumn{5}{l}{F.F.A. - Fouling Factor Allowance} \tabularnewline
+\multicolumn{5}{c}{\scriptsize Source: Table 3, Page 10, ANSI/AHRI Standard 550/590-2011}
+\end{longtable}
+
+\subsection{Electric Chiller Model Based on Condenser Leaving Temperature}\label{electric-chiller-model-based-on-condenser-leaving-temperature}
+
+\subsubsection{Overview}\label{overview-3-002}
+
+This model (object name Chiller:Electric:ReformulatedEIR) simulates the thermal performance of an electric liquid chiller and the power consumption of its compressor(s). The model, developed by Hydeman et al. (2002) as part of the CoolToolsâ„¢ project sponsored by Pacific Gas and Electric Company (PG\&E), is an empirical model similar to EnergyPlus' Chiller:Electric:EIR model. The model uses performance information at reference conditions along with three curve fits for cooling capacity and efficiency to determine chiller operation at off-reference conditions. The model has the same capabilities as the Chiller:Electric:EIR model, but can potentially provide significant accuracy improvement over the Chiller:Electric:EIR model for chillers with variable-speed compressor motor drives and/or variable condenser water flow applications.
+
+Chiller performance curves can be generated by fitting manufacturer's catalog data or measured data. Performance curves developed primarily from manufacturer's performance data are provided in the EnergyPlus Reference DataSets (Chillers.idf and AllDataSets.idf). This chiller model can be used to predict the performance of various chiller types (e.g., reciprocating, screw, scroll, and centrifugal) with water-cooled condensers. The model does not simulate the thermal performance or the power consumption of associated pumps or cooling towers. This auxiliary equipment must be modeled using other EnergyPlus models (e.g.~CoolingTower:SingleSpeed).
+
+The main difference between this model and the Chiller:Electric:EIR model is the condenser fluid temperature used in the associated performance curves: the Chiller:Electric:ReformulatedEIR model uses the LEAVING condenser water temperature while the Chiller:Electric:EIR model uses the ENTERING condenser water temperature. In addition, the Energy Input to Cooling Output Function of Part Load Ratio curve for this reformulated EIR chiller model includes the condenser leaving water temperature as an independent variable in addition to part-load ratio. Since the leaving condenser water temperature is a function of load, chiller performance, and condenser entering water temperature, EnergyPlus must iterate to converge on a solution for each simulation time step.
+
+\subsubsection{Model Description}\label{model-description-3-002}
+
+The chiller model uses user-supplied performance information at reference conditions along with three performance curves (curve objects) for cooling capacity and efficiency to determine chiller operation at off-reference conditions. The three performance curves are:
+
+1)~~~~Cooling Capacity Function of Temperature Curve
+
+2)~~~~Energy Input to Cooling Output Ratio Function of Temperature Curve
+
+3)~~~~Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve
+
+·~~~~~~~~The cooling capacity function of temperature curve is a biquadratic performance curve with two independent variables: the leaving chilled water temperature and the leaving condenser water temperature. The output of this curve is multiplied by the reference capacity to give the full-load cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation (otherwise the program issues warning messages).
+
+\begin{equation}
+ChillerCapFTemp = a + b({T_{cw,l}}) + c{({T_{cw,l}})^2} + d({T_{cond,l}}) + e{({T_{cond,l}})^2} + f({T_{cw,l}})({T_{cond,l}})
+\end{equation}
+
+where
+
+\emph{ChillerCapFTemp} = Cooling capacity factor, equal to 1 at reference conditions
+
+\emph{T\(_{cw,l}\)}~~~~~~~~~~~ = leaving chilled water temperature, ËšC
+
+\emph{T\(_{cond,l}\)} = leaving condenser water temperature, ËšC. This will be the water temperature entering the condenser loop (e.g., entering the cooling tower). If the chiller is a heat recovery chiller,then the condenser leaving temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers.
+
+·~~~~~~~~The energy input to cooling output ratio function of temperature curve is a biquadratic performance curve that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and the leaving condenser water temperature. The EIR is the inverse of the COP. The output of this curve is multiplied by the reference EIR (inverse of the reference COP) to give the full-load EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation (otherwise the program issues warning messages).
+
+\(ChillerEIRFTemp = a + b({T_{cw,l}}) + c{({T_{cw,l}})^2} + d({T_{cond,l}}) + e{({T_{cond,l}})^2} + f({T_{cw,l}})({T_{cond,l}})\) where
+
+\emph{ChillerEIRFTemp} = Energy input to cooling output factor, equal to 1 at reference conditions
+
+\emph{T\(_{cw,l}\)}~~~~~ = leaving chilled water temperature, ËšC
+
+\emph{T\(_{cond,l}\)} = leaving condenser water temperature, ËšC. This will be the water temperature entering the condenser loop (e.g., entering the cooling tower). If the chiller is a heat recovery chiller,then the condenser leaving temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers.
+
+·~~~~~~~~The energy input to cooling output ratio function of part-load ratio curve parameterizes the variation of the energy input ratio (EIR). The output of this curve is multiplied by the reference EIR (inverse of the reference COP) and the Energy Input to Cooling Output Ratio Function of Temperature Curve to give the EIR at the specific temperatures and part-load ratio at which the chiller is operating. This curve should have a value of 1.0 at the reference leaving condenser water temperature with part-load ratio equal to 1.0. It is recommended that this performance curve be developed using both full- and part-load performance data. The bicubic curve should be valid for the range of condenser water temperatures and part-load ratios anticipated for the simulation (otherwise the program issues warning messages). Either of the following two types of curves can be used.
+
+The first type is a bicubic performance curve that parameterizes the variation of the chiller input power ratio as a function of the leaving condenser water temperature and the part-load ratio. The part-load ratio is the actual cooling load divided by the chiller's available cooling capacity.
+
+\begin{equation}
+ChillerEIRFPLR = a + b({T_{cond,l}}) + c{({T_{cond,l}})^2} + d(PLR) + e{(PLR)^2} + f({T_{cond,l}})(PLR) + g{(PLR)^3}
+\end{equation}
+
+\begin{equation}
+  ChillerEIRFPLR = \frac{P_{chiller}}{P_{ref}}\left( {ChillerCapFTemp} \right)\left( {ChillerEIRFTemp} \right)
+\end{equation}
+
+where
+
+\emph{ChillerEIRFPLR} = Energy input to cooling output factor, equal to 1 at the reference leaving condenser water temperature and PLR = 1.0
+
+\emph{T\(_{cond,l}\)} = leaving condenser water temperature, ËšC. This will be the water temperature entering the condenser loop (e.g., entering the cooling tower). If the chiller is a heat recovery chiller,then the condenser leaving temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers.
+
+\emph{PLR}~~~~~ = Part load ratio = (cooling load) / (chiller's available cooling capacity)
+
+\emph{P\(_{chiller}\) = chiller power at specific PLR}
+
+\emph{P\(_{ref}\) = \({\mathop Q\limits^ \bullet_{ref}}\) /COP\(_{ref}\)}
+
+Note: Although a bicubic curve requires 10 coefficients (ref. Curve:Bicubic), coefficients 7, 9 and 10 are typically not used in the performance curve described here and should be entered as 0 unless sufficient performance data and regression accuracy exist to justify the use of these terms of the bicubic curve.
+
+The second type is a Chiller Part Load Custom Curve that parameterizes the variation of EIR as a function of the normalized dT, normalized Tdev and the PLR.
+
+\begin{equation}
+\begin{split}
+ChillerEIRFPLR = a + b(dT^*) + c(dT^*)^2 + d \cdot PLR + e \cdot PLR^2 + f \cdot (dT^*) \cdot PLR + g \cdot (dT^*)^3 \\
++ h \cdot PLR^3 + i \cdot (dT^*)^2 \cdot PLR + j \cdot (dT^*) \cdot PLR^2 + k \cdot (dT^*)^2 \cdot PLR^2 + l \cdot (T_{dev}^*) \cdot PLR^3
+\end{split}
+\end{equation}
+
+\begin{equation}
+dT^* = dT / dT_{ref}
+\end{equation}
+
+\begin{equation}
+T_{dev}^* = T_{dev} / dT_{ref}
+\end{equation}
+
+where
+
+\(dT\) = the delta of temperature across the leaving condenser water temperature and leaving evaporator water temperature of a chiller (lift)
+
+\(dT^*\) = the normalized fractional lift
+
+\(dT_{ref}\) = the lift under the reference condition
+
+PLR = the part load ratio
+
+\(T_{dev}\) = the deviation of leaving chilled water temperature from the reference condition
+
+\(T_{dev}^*\) = the normalized Tdev term
+
+All three of the performance curves are accessed through EnergyPlus' built-in performance curve equation manager (curve:biquadratic, curve:bicubic, and Curve:ChillerPartLoadWithLift). Note that the above three performance curves use the leaving condenser water temperature as an independent variable, instead of the entering condenser water temperature used in the performance curves for the Chiller:Electric:EIR model. Since the leaving condenser water temperature is calculated based on the condenser heat transfer rate, which is a function of the load to be met by the chiller, chiller compressor power, and the false loading (detailed calculations are given below), iterative calculations are required to determine the actual (converged) leaving condenser water temperature. The program uses the leaving condenser water temperature from the previous iteration to calculate values for each of the three performance curves described above. After obtaining the condenser heat transfer rate, the leaving condenser water temperature is recalculated. When the difference between the leaving condenser water temperature calculated on successive iterations is less than 0.0001\(^{°}\)C, the solution is assumed to have converged. Warning messages are issued if the calculated solution for leaving condenser water temperature and/or part-load ratio falls outside the valid range specified for the chiller's performance curves. If these warnings are issued, the user may choose to extend the range for the performance curves (only if a small extension is required since model extrapolation may produce significant errors) or a different chiller and associated performance curves with extended performance range can be located and used for the simulation.
+
+Note: Chiller:Electric:ReformulatedEIR objects and their associated performance curve objects are developed using performance information for a specific chiller and should almost always be used together for an EnergyPlus simulation. Changing the object input values, or swapping performance curves between chillers, should be done with extreme caution. For example, if the user wishes to model a chiller size that is different from the reference capacity, it is highly recommended that the reference flow rates be scaled proportionately to the change in reference capacity. Although this model can provide more accurate prediction than the Chiller:Electric:EIR model, it requires more performance data to develop the associated performance curves (at least 12 points from full-load performance and 7 points from part-load performance).
+
+Although performance curve data sets for 160 chillers are provided in the EnergyPlus Reference DataSets (Chillers.idf and AllDataSets.idf), they may not meet the requirements for specific applications. One can develop performance curves from performance data using two available techniques (Hydeman and Gillespie 2002). The first technique is called the Least-squares Linear Regression method and is used when sufficient performance data exist to employ standard least-square linear regression techniques. The second technique is called Reference Curve Method and is used when insufficient performance data exist to apply linear regression techniques. A detailed description of both techniques can be found in the reference mentioned above.
+
+For any simulation time step, the chiller's available cooling capacity is calculated as follows:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{avail}}\,\, = \,\,{\mathop Q\limits^ \bullet_{ref}}\left( {ChillerCapFTemp} \right)
+\end{equation}
+
+where
+
+\({\mathop Q\limits^ \bullet_{ref}}\) ~~~~ = chiller capacity at reference conditions (reference temperatures and flow rates defined by the user), W
+
+\({\mathop Q\limits^ \bullet_{avail}}\) ~ = available chiller capacity adjusted for current water temperatures, W
+
+The model then calculates the evaporator heat transfer rate required to bring the entering chilled water temperature down to the leaving chilled water setpoint temperature (established using a SetpointManager object and referenced in the PlantLoop object). If this calculated heat transfer rate is greater than the heat transfer rate being requested by the plant equipment operation scheme, then the evaporator heat transfer rate is reset to the requested cooling rate.
+
+The evaporator heat transfer rate is then compared to the available capacity. If the available chiller capacity is sufficient to meet the evaporator heat transfer rate, the leaving chilled water temperature is set equal to the chilled water setpoint temperature. If the requested evaporator heat transfer rate is larger than the available capacity the chilled water leaving the evaporator is allowed to float upward. For this case, the exiting chilled water temperature is calculated based on the water temperature entering the evaporator, the available cooling capacity, and the evaporator mass flow rate as follows:
+
+\begin{equation}
+  T_{cw,l}  =  T_{cw,e} - \frac{\dot{Q}_{avail}}{\dot{m}_{evap}C_{p,evap}}
+\end{equation}
+
+where
+
+\emph{T\(_{cw,l}\)}~~~~~~~~~~~ = water temperature leaving the evaporator, ËšC
+
+\emph{T\(_{cw,e}\)}~~~~~~~~~~ = water temperature entering the evaporator, ËšC
+
+\({\mathop m\limits^ \bullet_{evap}}\) ~~~~~~~~ = evaporator mass flow rate, kg/s
+
+\emph{C\(_{p,evap}\)}~~~~~~~~ = specific heat of water entering evaporator at \emph{T\(_{cw,e}\)}, J/kg-ËšC
+
+The part-load ratio is then calculated as the ratio of the evaporator heat transfer rate to the available chiller capacity. The part-load ratio is not allowed to be greater than the maximum part-load ratio specified by the user or less than zero as follows:
+
+\begin{equation}
+  PLR = \max\PB{0.0,\min\PB{\frac{\dot{Q}_{evap}}{\dot{Q}_{avail}},PLR_{max}}}
+\end{equation}
+
+where
+
+\emph{PLR}~~~~~~~~~~ = part-load ratio
+
+\({\mathop Q\limits^ \bullet_{evap}}\) ~~~~~~~~ = load to be met by the chiller, W
+
+\emph{PLR\(_{max}\)} = maximum part-load ratio (specified by the user in the input data file)
+
+Note that the maximum part-load ratio (PLR\(_{max}\), specified in the Chiller:Electric:ReformulatedEIR object) used in the equation should be less than or equal to the maximum part-load ratio specified in the ``Energy Input to Cooling Output Ratio Function of Part-Load Ratio'' performance curve object.
+
+The model assumes that the cooling load is met through chiller unloading down to the minimum unloading ratio. False loading (e.g.~hot-gas bypass) is assumed to occur between the minimum unloading ratio and the minimum part-load ratio yielding constant electrical power consumption under these conditions. Below the minimum part-load ratio, the chiller cycles on/off to meet very small loads and the power consumption during the on cycle is the same as when the chiller is operating at the minimum part load ratio. When the chiller part-load ratio is less than the minimum part-load ratio, the on-off cycling ratio of the chiller is calculated as follows and is available as an output variable.
+
+\begin{equation}
+  ChillerCyclingRatio = \min \PB{ \frac{PLR}{PLR_{min}}, 1.0 }
+\end{equation}
+
+To properly account for chiller electric power consumption when PLR is less than the minimum unloading ratio, the PLR is reset to the greater of the PLR calculated above and the PLR at the minimum unloading ratio. The result is available as the output variable Chiller Part Load Ratio.
+
+\begin{equation}
+PLR = MAX(PLR,PL{R_{MinUnloadRatio}})
+\end{equation}
+
+This revised PLR accounts for the ``false loading'' (e.g., hot-gas bypass) that is assumed to occur whenever the PLR (based on cooling load divided by available capacity) is less than the minimum unloading ratio specified. The amount of false loading on the chiller is calculated using this revised PLR and is reported as an output variable as follows:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{falseloading}} = \left( {{{\mathop Q\limits^ \bullet  }_{avail}}} \right)\left( {PLR} \right)\left( {ChillerCyclingRatio} \right) - {\mathop Q\limits^ \bullet_{evap}}
+\end{equation}
+
+The electrical power consumption for the chiller compressor(s) for any simulation time step is then calculated using the following equation:
+
+\({P_{chiller}}\, = \,\,\left( {{{\mathop Q\limits^ \bullet }_{avail}}\,} \right)\,\left( {\frac{1}{{CO{P_{ref}}}}} \right)\,\left( {ChillerEIRFTemp} \right)\left( {ChillerEIRFPLR} \right)\left( {ChillerCyclingRatio} \right)\) where
+
+\emph{P\(_{chiller}\)}~~~~~~~~ = Chiller compressor power, W
+
+\emph{COP\(_{ref}\)}~~~~~~ = Reference coefficient of performance, W/W
+
+Heat rejected by the chiller condenser includes the heat transferred in the evaporator plus a portion or all of the compressor electrical energy consumption. For electric chillers with hermetic compressors, all compressor energy consumption is rejected by the condenser (compressor motor efficiency = \emph{eff\(_{motor}\)} = 1.0). For chillers with semi-hermetic or open compressors, only a portion of the compressor energy use is rejected by the condenser. The heat transfer rate for the chiller condenser is calculated as follows:
+
+\begin{equation}
+{\mathop Q\limits^ \bullet_{cond}} = \left( {{P_{chiller}} * ef{f_{motor}}} \right) + {\mathop Q\limits^ \bullet_{evap}} + {\mathop Q\limits^ \bullet_{falseloading}}
+\end{equation}
+
+where
+
+\({\mathop Q\limits^ \bullet_{cond}}\) ~~~~~~~~ = condenser heat transfer rate, W
+
+\(ef{f_{motor}}\) ~~~~~~ = compressor motor efficiency = fraction of compressor electrical energy consumption rejected as condenser heat
+
+The above curve values are calculated based on the leaving condenser water temperature found through iteration. After obtaining the condenser heat transfer rate, the final leaving condenser water temperature is then calculated as:
+
+\begin{equation}
+  T_{cond,l} = T_{cond,e} + \frac{\dot{Q}_{cond}}{\dot{m}_{cond} C_{p,cond}}
+\end{equation}
+
+where:
+
+\emph{T\(_{cond,l}\)}~~~~~~~~~ = water temperature leaving the condenser, ËšC
+
+\emph{T\(_{cond,e}\)}~~~~~~~~ = water temperature entering the condenser, ËšC
+
+\({\mathop m\limits^ \bullet_{cond}}\) ~~~~~~~~ = mass flow rate through the condenser, kg/s
+
+\({C_{p,cond}}\) ~~~~~~ = specific heat of water entering the condenser at \emph{T\(_{cond,e}\)}, J/kg-ËšC
+
+The final calculations determine the total heat transfer energy for the condenser and evaporator, as well as the total electric energy consumed by the chiller compressor motor(s) and condenser fan(s). The results are available as output variables.
+
+\begin{equation}
+{Q_{cond}} = {\mathop Q\limits^ \bullet_{cond}}*TimeStepSys*3600
+\end{equation}
+
+\begin{equation}
+{Q_{evap}} = {\mathop Q\limits^ \bullet_{evap}}\,\,*\,\,TimeStepSys\,\,*\,\,3600
+\end{equation}
+
+\begin{equation}
+{E_{chiller}} = {P_{chiller}}*\,\,TimeStepSys\,\,*\,\,3600
+\end{equation}
+
+\begin{equation}
+{E_{cond}} = {P_{cond}}\,\, * \,\,TimeStepSys\,\,*\,\,3600
+\end{equation}
+
+where
+
+\emph{Q\(_{cond}\)}~~~~~~~~~ = chiller condenser heat transfer energy, J
+
+\emph{Q\(_{evap}\)}~~~~~~~~~~ = chiller evaporator cooling energy, J
+
+\emph{E\(_{chiller}\)}~~~~~~~~ = chiller (compressor) electric energy, J
+
+\emph{E\(_{cond}\)}~~~~~~~~~~ = chiller condenser fan electric energy, J
+
+\emph{TimeStepSys} = HVAC system simulation time step, hr
+
+\(3600\) ~~~~~~~~ = conversion factor, sec/hr
+
+\subsubsection{Electric Reformulated EIR Chiller with Heat Recovery Option}\label{electric-reformulated-eir-chiller-with-heat-recovery-option}
+
+Heat from the electric reformulated EIR chiller condenser may be recovered. The heat recovery water flow rate is specified by the user along with the input and output nodes connected to the heat recovery loop. The algorithms are identical to those used for Chiller:Electric and Chiller:Electric:EIR. Refer to the section entitled Chillers with Plant Heat Recovery for details.
+
+\subsubsection{Standard Rating (Integrated Part Load Value)}\label{standard-rating-integrated-part-load-value-1}
+
+Integrated Part Laod Value (IPLV) calculations for Reformulated EIR chiller are similar to what are described above for EIR chillers. The only difference with Reformulated EIR chiller is that it calls an iterative subroutine (SolveRegulaFalsi) to obtain a condenser water outlet temperature which corresponds to condenser inlet temperature at reduced capacity conditions as outlined in Table~\ref{table:standard-rating-integrated-part-load-value} above. SolveRegulaFalsi is a general utility routine for finding the zero of a function. In this case it finds the condenser inlet temperature that will zero the residual function -- the difference between calculated condenser inlet temperature and desired condenser inlet temperature per ANSI/AHRE 550/590, 2011 (Table~\ref{table:demand-manager-types-and-resimulation.} above) divided by desired condenser inlet temperature.
+
+\subsubsection{References}\label{references-1-003}
+
+Hydeman, M., N. Webb, P. Sreedharan, and S. Blanc. 2002. Development and Testing of a Reformulated Regression-Based Electric Chiller Model. ASHRAE Transactions HI-02-18-2.
+
+Hydeman, M. and K.L. Gillespie. 2002. Tools and Techniques to Calibrate Electric Chiller Component Models. ASHRAE Transactions AC-02-9-1.
+
+Hydeman, M., K. Gillespie, and R. Kammerud. 1997. PG\&E's CoolTools project: A toolkit to improve evaluation and operation of chilled water plants. Presented at the Cool\$ense National Forum on Integrated Chilled Water Retrofits, Sep. 1997. Berkeley California: Lawrence Berkeley National Laboratory.
+
+\subsection{Engine Driven Chiller}\label{engine-driven-chiller}
+
+The engine driven chiller (Object name: Chiller:EngineDriven) is the empirical model from the Building Loads and System Thermodynamics (BLAST) program. Fitting catalog data to a third order polynomial equations generates the chiller performance curves.~ Three sets of coefficients are required to model the open centrifugal chiller as discussed in the section, titled, `Electric Chiller Based on Fluid Temperature Differences'. Additional curve fits are required to model the engine.~ Because the model inherently involves the lower heating value of the fuel, a reference temperature is also involved in the calculations, which manufacturers present at 25°C.
+
+The engine model was also developed for the BLAST program. It was adapted for use in EnergyPlus. This model is used for both the engine driven generator and the engine driven chiller.~ It uses the following set of equations all of which are quadratic fits to the PLR (Part Load Ratio) of the generator.~ The coefficients must be derived from manufacturers data.
+
+\begin{equation}
+\frac{{chiller\,\,cooling\,\,load}}{{fuel\,\,energy\,\,input}} = \frac{{chiller\,\,cooling\,\,load}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {a_1} + {a_2}PLR + {a_3}PL{R^2}
+\end{equation}
+
+The exhaust gas temp and flow rate are used if a stack heat exchanger is used to recover waste heat from the exhaust.~ This temperature is the inlet temperature to the heat exchanger which is modeled in a UA-effectiveness form:
+
+\begin{equation}
+\frac{{Total\,Exhaust\,heat}}{{fuel\,energy\,input}} = \frac{{Total\,\,Exhaust\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {d_1} + {d_2}PLR + {d_3}PL{R^2}
+\end{equation}
+
+\begin{equation}
+\frac{{Exhaust\,\,Gas\,\,Temp\,\,\left\{ K \right\}}}{{fuel\,\,energy\,\,input}} = \frac{{Exhaust\,\,Gas\,\,Temp\,\,\left\{ K \right\}}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {e_1} + {e_2}PLR + {e_3}PL{R^2}
+\end{equation}
+
+The exhaust flow rate is then calculated as:
+
+\begin{equation}
+{\dot m_{exhaust}} = \frac{{Total\,\,Exhaust\,\,heat}}{{C{p_{exhaust}} \cdot \left( {{T_{exhaust}} - {T_{reference}}} \right)}}
+\end{equation}
+
+where T\(_{reference}\) is the reference temperature for the fuel lower heating value, and is given as 25°C in manufacturer's data, and
+
+\begin{equation}
+{T_{stack}} = {T_{DesignMinExhaust}} + {\frac{{\left( {{T_{exhaust}} - {T_{DesignMinExhaust}}} \right)}}{{{\rm{exp}}\left( {\frac{{{\rm{UA}}}}{{{{{\rm{\dot m}}}_{{\rm{exhaust}}}}C{p_{exhaust}}}}} \right)}}^2}
+\end{equation}
+
+Finally, heat recovered from the lube oil and the water jacket are accounted for as follows:
+
+\begin{equation}
+\frac{{Recoverable\,\,jacket\,\,heat}}{{fuel\,\,energy\,\,input}} = \frac{{Recoverable\,\,jacket\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {b_1} + {b_2}PLR + {b_3}PL{R^2}
+\end{equation}
+
+\begin{equation}
+\frac{{Recoverable\,\,lube\,\,oil\,\,heat}}{{fuel\,\,energy\,\,input}} = \frac{{Recoverable\,\,lube\,\,oil\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {c_1} + {c_2}PLR + {c_3}PL{R^2}
+\end{equation}
+
+\subsubsection{Chiller Basin Heater}\label{chiller-basin-heater-3}
+
+Calculations are also made to estimate the electric power input to the basin heater for chillers with evaporatively-cooled condensers. The chillers which calculate basin heater power are Chiller:Electric:EIR, Chiller:Electric, Chiller:ConstantCOP, Chiller:EngineDriven and Chiller:CombustionTurbine.A schedule may be used to disable the basin heater during regular maintenance periods or other time periods (e.g., during summer). If a schedule is not provided, the basin heater is assumed to be available the entire simulation time period. The basin heater operates when it is scheduled on, the outdoor air dry-bulb temperature is below the basin heater setpoint temperature, and the chiller is not active (i.e., chiller is not operating for the simulation time step --- for example, when there is no cooling load to be met by the chiller, \emph{or if there is no water flow through the chiller due to a chiller or pump availability schedule, etc.}). The user is required to enter a basin heater capacity (watts per degree Kelvin) and a heater setpoint temperature (\(^{o}\)C) if they want to model basin heater electric power.
+
+\begin{lstlisting}
+P_heater_basin = 0.0
+IF (ChillerIsOFF) THEN
+  IF (Scheduleheater_basin is Defined) THEN
+    IF (CAPheater_basin > 0 AND Scheduleheater_basin = ON) THEN
+      P_heater_basin = MAX(0.0,CAP_heater_basin*(T_setpoint_basin-T_db_outdoor))
+    ENDIF
+  ELSE
+    IF (CAPheater_basin > 0) THEN
+      P_heater_basin = MAX(0.0,CAP_heater_basin*(T_setpoint_basin-T_db_outdoor))
+    ENDIF
+  ENDIF
+ENDIF
+\end{lstlisting}
+
+\begin{equation}
+{E_{heater,basin}} = \left( {{P_{heater,basin}}} \right)\left( {TimeStepSys} \right)3600
+\end{equation}
+
+where:
+
+\({P_{heater,basin}}\) ~ = Chiller basin heater electric power (W)
+
+\({E_{heater,basin}}\) = Chiller basin heater electric consumption (J)
+
+\emph{T\(_{setpoint,basin}\)} = Basin heater setpoint temperature, user input (\(^{o}\)C)
+
+\emph{T\(_{db,outdoor}\)}~~~ = Outdoor air dry-bulb temperature (\(^{o}\)C)
+
+\emph{CAP\(_{heater,basin}\)} = Basin heater capacity, user input (W/K)
+
+\emph{Schedule\(_{heater,basin}\)} = Basin heater schedule, user input (schedule value \textgreater{} 0 means ON)
+
+\emph{ChillerIsOFF =}Logical variable denoting that the chiller is not operating for the current simulation time step (e.g.,~ there is no cooling load to be met by the chiller, or if there is no water flow through the chiller due to a chiller or pump availability schedule, etc.) 
diff --git a/doc/engineering-reference/src/solar-radiation-reflected-from-exterior.tex b/doc/engineering-reference/src/solar-radiation-reflected-from-exterior.tex
new file mode 100644
index 00000000000..a0fb02dca96
--- /dev/null
+++ b/doc/engineering-reference/src/solar-radiation-reflected-from-exterior.tex
@@ -0,0 +1,38 @@
+\chapter{Solar Radiation Reflected from Exterior Surfaces}\label{solar-radiation-reflected-from-exterior-surfaces}
+
+EnergyPlus has an option to calculate beam and sky solar radiation that is reflected from exterior surfaces and then strikes the building. This calculation occurs if ``withReflections'' is used on the SolarDistribution option in the Building object. For zones with detailed daylighting, these reflections are also considered in the daylight illuminance calculations.\protect\hyperlink{ux5fftn6}{{[}6{]}}
+
+The reflecting surfaces fall into three categories:
+
+\begin{itemize}
+\item
+  \textbf{Shadowing surfaces}. These are surfaces like overhangs or neighboring buildings entered with objects Shading:Site:Detailed, Shading:Building:Detailed, or Shading:Zone:Detailed Examples are shown in Figure~\ref{fig:examples-of-solar-reflection-from-shadowing}.
+
+These surfaces can have diffuse and/or specular (beam-to-beam)~ reflectance values that are specified with the ShadingProperty:Reflectance object.
+
+\item
+  \textbf{Exterior building surfaces}. In this case one section of the building reflects solar radiation onto another section (and vice-versa). See Figure~\ref{fig:solar-reflection-from-building-surfaces-onto}.
+
+Opaque building surfaces (walls, for example) are assumed to be diffusely reflecting. Windows and glass doors are assumed to be specularly reflecting. The reflectance values for opaque surfaces are calculated by the program from the Solar Absorptance and Visible Absorptance values of the outer material layer of the surface's construction. The reflectance values for windows and glass doors are calculated by the program from the reflectance properties of the individual glass layers that make up surface's construction assuming no shading device is present and taking into account inter-reflections among the layers.
+
+\item
+  \textbf{The ground surface}. Beam solar and sky solar reflection from the ground is calculated even if ``withReflections'' is not used (the default). But in this case the ground plane is considered unobstructed, i.e., the shadowing of the ground by the building itself or by obstructions such as neighboring buildings is ignored. This shadowing is taken into account only if ``WithReflections'' is used in the Solar Distribution field (in ``Building'' input object) (Figure~\ref{fig:shadowing-by-the-building-itself-affects-beam}). In this case the user-input value of ground view factor is not used.
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 50
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image670.png}
+\caption{Examples of solar reflection from shadowing surfaces in the Shading series of input objects. Solid arrows are beam solar radiation; dashed arrows are diffuse solar radiation. (a) Diffuse reflection of beam solar radiation from the top of an overhang. (b) Diffuse reflection of sky solar radiation from the top of an overhang. (c) Beam-to-beam (specular) reflection from the façade of an adjacent highly-glazed building represented by a vertical shadowing surface. \protect \label{fig:examples-of-solar-reflection-from-shadowing}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 51
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image671.png}
+\caption{Solar reflection from building surfaces onto other building surfaces. In this example beam solar reflects from a vertical section of the building onto a roof section. The reflection from the window is specular. The reflection from the wall is diffuse. \protect \label{fig:solar-reflection-from-building-surfaces-onto}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 52
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image672.png}
+\caption{Shadowing by the building itself affects beam solar reflection from the ground. Beam-to-diffuse reflection from the ground onto the building occurs only for sunlit areas, A and C, not for shaded area, B. Shadowing by the building also affects sky solar reflection from ground (not shown). \protect \label{fig:shadowing-by-the-building-itself-affects-beam}}
+\end{figure}
diff --git a/doc/engineering-reference/src/solar-radiation-reflected-from-exterior/diffuse-reflection-of-beam-solar-and-sky.tex b/doc/engineering-reference/src/solar-radiation-reflected-from-exterior/diffuse-reflection-of-beam-solar-and-sky.tex
new file mode 100644
index 00000000000..0b57979dbed
--- /dev/null
+++ b/doc/engineering-reference/src/solar-radiation-reflected-from-exterior/diffuse-reflection-of-beam-solar-and-sky.tex
@@ -0,0 +1,238 @@
+\section{Diffuse Reflection of Beam Solar and Sky Solar Radiation}\label{diffuse-reflection-of-beam-solar-and-sky-solar-radiation}
+
+A ray-tracing method is used to calculate beam solar and sky solar radiation that is diffusely reflected onto each of a building's exterior surfaces (walls, roofs, windows and doors), called here ``receiving surfaces.'' The calculation begins by generating a set of rays proceeding into the outward hemisphere at each receiving point on a receiving surface. Then it determinines whether each ray hits the sky, ground or an obstruction. The radiance at the hit point from reflection of incident beam or sky solar is determined and the contribution of this radiance to the receiving surface is calculated, added to the contribution from other hit points, and averaged over the receiving points. Separate calculations are done for beam-to-diffuse and sky solar reflection from all obstructions and beam-to-diffuse and sky solar reflection from the ground. (For beam-to-beam reflection see ``Beam Solar Radiation Specularly Reflected from Obstructions,'' below.)
+
+\subsection{\texorpdfstring{\emph{Receiving points}}{Receiving points}}\label{receiving-points}
+
+An \emph{N}-sided surface is assigned \emph{N} receiving points with the following coordinates, expressed in terms of the surface vertex coordinates:
+
+\begin{equation}
+{P_{ij}} = \sum\limits_{k = 1}^N {{a_{ki}}{v_{kj}},{\rm{  }}i = 1,3;{\rm{  }}j = 1,3}
+\end{equation}
+
+where
+
+\emph{P\(_{ij}\) = j\(^{th}\)} coordinate of the* i\(^{th}\)* receiving point
+
+\emph{v\(_{kj}\)} = * j\(^{th}\)* coordinate of the \emph{k\(^{th}\)} surface vertex
+
+If \emph{N} = 3:~ \emph{a\(_{kj}\)} = 3/5 if \emph{k} = \emph{i};~ = 1/5 otherwise
+
+If \emph{N} \textgreater{} 3:~ \emph{a\(_{kj}\)} = \(\frac{{N + 1}}{{2N}}\) ~if \emph{k} = \emph{i};~ = \(\frac{1}{{2N}}\) ~otherwise
+
+For example, for a vertical 3m by 5m rectangle with vertices (0,0,3), (0,0,0), (5,0,0) and (5,0,3), this expression gives receiving points at (1.25,0,2.25), (1.25,0,0.75), (3.75,0,0.75) and (3.75,0,2.25), as shown in Figure~\ref{fig:vertical-rectangular-exterior-heat-transfer}.
+
+\begin{figure}[hbtp] % fig 53
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image676.png}
+\caption{Vertical rectangular exterior heat transfer surface showing location of receiving points for calculating incident solar radiation reflected from obstructions. \protect \label{fig:vertical-rectangular-exterior-heat-transfer}}
+\end{figure}
+
+\subsection{\texorpdfstring{\emph{Rays}}{Rays}}\label{rays}
+
+A total of 90 rays are sent out into the exterior hemisphere surrounding each receiving point. An upgoing ray may hit an obstruction or the sky. A downgoing ray may hit an obstruction or the ground. See Figure~\ref{fig:two-dimensional-schematic-showing-rays-going}.
+
+In subroutine InitSolReflRecSurf, the following is determined for each ray, \emph{i,}:
+
+1.~~~~Unit vector in direction of ray
+
+2.~~~~Cosine of angle between ray and plane of receiving surface (\(\cos {\alpha_i}\) )
+
+3.~~~~Element of solid angle associated with ray (\(d{\Omega_i}\) )
+
+4.~~~~If the ray hits one or more obstructions, the coordinates of the hit point on the obstruction nearest the receiving point
+
+5.~~~~For the surface containing the hit point: the surface number, the solar reflectance (\({\rho_{obs,i}}\) if an obstruction), and the surface unit vector at the hit point pointing into the hemisphere containing the receiving point
+
+6.~~~~If the ray is downgoing and hits the ground, the coordinates of the ground hit point
+
+7.~~~~Distance from receiving point to hit point
+
+\begin{figure}[hbtp] % fig 54
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image680.png}
+\caption{Two-dimensional schematic showing rays going outward from a point on a receiving surface. Rays 1-6 hit the ground, rays 7-11 hit an obstruction, and rays 12-15 hit the sky. \protect \label{fig:two-dimensional-schematic-showing-rays-going}}
+\end{figure}
+
+\subsection{Sky Solar Radiation Diffusely Reflected from Obstructions}\label{sky-solar-radiation-diffusely-reflected-from-obstructions}
+
+The factor for reflection of sky radiation from obstructions onto a receiving surface is calculated in subroutine CalcSkySolDiffuseReflFactors. It is given by:
+
+\begin{equation}
+\begin{array}{l}{\rm{ReflFacSkySolObs(RecSurfNum)}} = \\\frac{1}{{{N_{rec}}}}\sum\limits_1^{{N_{rec}}} {\sum\limits_{i = 1}^{{N_{ray}}} {Hi{t_{obs,i}}ViewFacSk{y_{obs,i}}DifShdgRatioIsoSk{y_{obs,i}}{\rho_{obs,i}}\cos {\alpha_i}/\pi } } \end{array}
+\end{equation}
+
+where
+
+RecSurfNum is the receiving surface number,
+
+\({N_{rec}}\) is the number of receiving points,
+
+\({N_{ray}}\) is the number of rays,
+
+``\emph{obs,i}'' denotes the obstruction hit by ray \emph{i},
+
+\emph{Hit\(_{obs,i}\)} = 1 if ray \emph{i} hits an obstruction, = 0 otherwise,
+
+\emph{ViewFacSky\(_{obs,i}\)} = unobstructed sky view factor of the obstruction = \((1 + \cos til{t_{obs}})/2\) ,
+
+\emph{DifShdgRatioIsoSky\(_{obs,i}\)} = (obstructed sky irradiance on obstruction)/(unobstructed sky irradiance on obstruction)
+
+In this equation the product \emph{ViewFacSky*DifShdgRatioIsoSky} is the sky irradiance at the hit point divided by the horizontal sky irradiance taking into account shadowing of sky diffuse radiation on the obstruction by other obstructions, and assuming that the radiance of the sky is uniform. Note that we ignore secondary reflections here and in the following sections. In the present case this means that the irradiance at the hit point due to reflection of sky radiation from the ground or from other obstructions is not considered.
+
+The above reflection factor is used in the timestep calculation to find the irradiance on a receiving surface due to sky radiation reflected from obstructions:
+
+\begin{equation}
+\begin{split}
+QRadSWOutIncSkyDiffReflObs(RecSurfNum) = DifSolarRad \\
+* ReflFacSkySolObs(RecSurfNum) (W/m^{2})
+\end{split}
+\end{equation}
+
+where \emph{DifSolarRad} is the horizontal sky irradiance on an unobstructed horizontal plane (W/m\(^{2}\)).
+
+\subsection{Sky Solar Radiation Diffusely Reflected from the Ground}\label{sky-solar-radiation-diffusely-reflected-from-the-ground}
+
+If a downgoing ray from a receiving point hits the ground (for example, rays 1-6 in Figure~\ref{fig:two-dimensional-schematic-showing-rays-going}), the program calculates the radiance at the ground hit point due to sky diffuse solar reaching that point. To do this, rays are sent upward from the ground hit point and it is determined which of these rays are unobstructed and so go to the sky (for example, rays 6-10 in Figure~\ref{fig:two-dimensional-schematic-showing-rays-going-001}). For this calculation it is assumed that the radiance of the sky is uniform.
+
+\begin{figure}[hbtp] % fig 55
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image685.png}
+\caption{Two-dimensional schematic showing rays going upward from a ground hit point. \protect \label{fig:two-dimensional-schematic-showing-rays-going-001}}
+\end{figure}
+
+The factor for reflection of sky radiation from the ground onto a receiving surface is calculated in subroutine CalcSkySolDiffuseReflFactors. It is given by:
+
+\begin{equation}
+\begin{array}{l}
+{\rm{ReflFacSkySolGnd(RecSurfNum)}} = \\\frac{1}{{{N_{rec}}}}\sum\limits_1^{{N_{rec}}} {\sum\limits_{i = 1}^{{N_{ray}}} {\left[ {(Hi{t_{gnd,i}}d{\Omega_i}\cos {\alpha_i}/\pi )\sum\limits_{j(i)}^{{N_{ray}}} {Hi{t_{sky,j(i)}}\cos {\alpha_{j(i)}}d{\Omega_{j(i)}}/\pi } } \right]} }
+\end{array}
+\end{equation}
+
+where
+
+\emph{\(j(i)\) ~}~denotes an upgoing ray from the ground point hit by ray \emph{i}from the receiving point,
+
+\emph{Hit\(_{skyj(i)}\)} = 1 if ray \emph{\(j(i)\)} hits the sky, = 0 otherwise,
+
+\({\alpha_{j(i)}}\) is the angle of incidence of ray \(j(i)\) with respect to the ground plane,
+
+\(d{\Omega_{j(i)}}\) is the solid angle element associated with ray \(j(i)\) .
+
+This factor is used in the timestep calculation to find the irradiance on a receiving surface due to sky radiation reflected from the ground:
+
+QRadSWOutIncSkyDiffReflGnd(RecSurfNum) = DifSolarRad * \({\rho_{gnd}}\) * ReflFacSkySolGnd(RecSurfNum)~ (W/m\(^{2}\))
+
+where \({\rho_{gnd}}\) is the solar reflectance of the ground, which is assumed to be uniform over the ground plane but may vary monthly (because of snow cover, for example).
+
+\subsection{Beam Solar Radiation Diffusely Reflected from Obstructions}\label{beam-solar-radiation-diffusely-reflected-from-obstructions}
+
+This calculation is similar to that for sky solar reflected from obstructions. However, to find the radiance at a hit point on an obstruction a line is drawn from the hit point to center of the sun. From this line it is determined (1) if there is an obstruction between the hit point and the sun, in which case it is assumed that no beam solar reaches the hit point; and (2) if beam solar does reach the hit point, what the the solar angle of incidence at that point is.
+
+The calculation is done for the hourly sun positions on each of the design days. It is also done for hourly sun positions on selected days during the weather file run period (the same days for which the shadowing calculations are done).
+
+The factor for diffuse reflection of beam solar radiation from obstructions onto a receiving surface is calculated in subroutine CalcBeamSolDiffuseReflFactors. It is given by:
+
+{\scriptsize
+\begin{equation}
+{\rm{ReflFacBmToDiffSolObs(RecSurfNum,IHr)}} = \frac{1}{{{N_{rec}}}}\sum\limits_1^{{N_{rec}}} {\sum\limits_{i = 1}^{{N_{ray}}} {Hi{t_{obs,i}}Hi{t_{obs,i,sun}}d{\Omega_i}\cos {\alpha_i}{\rho_{obs,i}}\cos {\alpha_{sun,obs,i}}} }
+\end{equation}}
+
+where
+
+\emph{IHr} = hour number
+
+\(Hi{t_{obs,i}}\) = 1 if ray \emph{i} from the receiving point hits an obstruction, = 0 otherwise,
+
+\(Hi{t_{obs,i,sun}}\) = 1 if the line from ray \emph{i}'s hit point to the sun is unobstructed, = 0 otherwise,
+
+\({\alpha_{sun,obs,i}}\) is the angle of incidence of the sun on the obstruction.
+
+This factor is used in the timestep calculation to find the diffuse irradiance on a receiving surface due to beam solar diffusely reflected from obstructions:
+
+QRadSWOutIncBmToDiffReflObs(RecSurfNum) = BeamSolarRad * (WeightNow * ReflFacBmToDiffSolObs(RecSurfNum,HourOfDay) + WeightPreviousHour * ReflFacBmToDiffSolObs(RecSurfNum,PreviousHour))
+
+where \emph{BeamSolarRad} is the timestep value of beam normal solar intensity (W/m2), and \emph{WeightNow} and \emph{WeightPreviousHour} are time-averaging factors.
+
+\subsection{Beam Solar Radiation Diffusely Reflected from the Ground}\label{beam-solar-radiation-diffusely-reflected-from-the-ground}
+
+This calculation is the same as that for beam solar diffusely reflected from obstructions except that only rays from a receiving point that hit the ground are considered. The factor for diffuse reflection of beam solar from the ground onto a receiving surface is calculated in subroutine CalcBeamSolDiffuseReflFactors. It is given by:
+
+{\scriptsize
+\begin{equation}
+{\rm{ReflFacBmToDiffSolGnd(RecSurfNum,IHr)}} = \frac{1}{{{N_{rec}}}}\sum\limits_1^{{N_{rec}}} {\sum\limits_{i = 1}^{{N_{ray}}} {Hi{t_{gnd,i}}Hi{t_{gnd,i,sun}}d{\Omega_i}\cos {\alpha_{gnd,i}}\cos {\alpha_{sun,gnd}}} }
+\end{equation}}
+
+where
+
+\(Hi{t_{gnd,i}}\) = 1 if ray \emph{i} hits the ground, = 0 otherwise,
+
+\(Hi{t_{gnd,i,sun}}\) = 1 if the line from ray \emph{i}'s hit point ot the sun is unobstructed, = 0 otherwise,
+
+\({\alpha_{sun,gnd}}\) = angle of incidence of sun on ground ( = solar zenith angle).
+
+This factor is used in the timestep calculation to find the diffuse irradiance on a receiving surface due to beam solar diffusely reflected from the ground:
+
+QRadSWOutIncBmToDiffReflGnd(RecSurfNum) = BeamSolarRad * \({\rho_{gnd}}\) * (WeightNow * ReflFacBmToDiffSolGnd(RecSurfNum,HourOfDay) + WeightPreviousHour * ReflFacBmToDiffSolGnd(RecSurfNum,PreviousHour))
+
+\subsection{Beam Solar Radiation Specularly Reflected from Obstructions}\label{beam-solar-radiation-specularly-reflected-from-obstructions}
+
+Figure~\ref{fig:two-dimensional-schematic-showing-specular} shows schematically how specular (beam-to-beam) reflection from an obstruction is calculated. \protect\hyperlink{ux5fftn7}{{[}7{]}}
+
+\begin{figure}[hbtp] % fig 56
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image703.png}
+\caption{Two-dimensional schematic showing specular reflection from an obstruction such as the glazed façade of a neighboring building. The receiving point receives specularly reflected beam solar radiation if (1) DB passes through specularly reflecting surface EF, (2) CD does not hit any obstructions (such as RS), and (3) AC does not hit any obstructions (such as PQ). \protect \label{fig:two-dimensional-schematic-showing-specular}}
+\end{figure}
+
+The calculation procedure is as follows:
+
+1.~~~~Select receiving point D on receiving surface JK.
+
+2.~~~~Select specularly reflecting surface EF.
+
+3.~~~~Find the mirror image, B, of the sun with respect to the plane of EF and construct ray DB.
+
+4.~~~~Check if DB passes through EF; if yes, find intersection point C and construct ray CD.
+
+5.~~~~Check if CD is obstructed.
+
+6.~~~~If no, construct ray AC and check if it is obstructed.
+
+7.~~~~If no, find reflected beam irradiance (W/m\(^{2}\)) at D:
+
+\begin{equation}
+I_{D,refl}^{bm} = BeamSolarRad*{\rho_{spec}}({\alpha_C})\cos {\alpha_D}
+\end{equation}
+
+where
+
+\({\alpha_C}\) = angle of incidence of beam solar at point C of the obstruction,
+
+\({\rho_{spec}}({\alpha_C})\) = reflectance of obstruction as a function of the angle of incidence,
+
+\({\alpha_D}\) = angle of incidence of ray CD on JK.
+
+The factor for specular reflection of beam solar from obstruction onto a receiving surface is calculated in subroutine CalcBeamSolSpecularReflFactors. It is given by:
+
+\begin{equation}
+{\rm{ReflFacBmToBmSolObs(RecSurfNum,IHr) }} = \sum\limits_{\scriptstyle \substack{specularly \, reflecting \, surfaces}} \left[ {\frac{1}{{{N_{rec}}}}\sum\limits_1^{{N_{rec}}} {{f_{C,glazed}}{\rho_{spec}}({\alpha_C})\cos {\alpha_D}} } \right]
+\end{equation}
+
+The program assumes that specular reflection from a surface is due to glazing. If the reflecting surface is a window belonging to the building itself (as in Figure~\ref{fig:solar-reflection-from-building-surfaces-onto}), then \({f_{C,glazed}}\) is the fraction of the window that is glazed (which is 1.0 unless the window has dividers).
+
+If the surface is a shading surface (that represents, for example, the glazed façade of a neigboring building) the surface reflection information is entered with the Shading Surface Reflectance object. This object contains values for:
+
+1.~~~~Diffuse solar reflectance of the unglazed part of the shading surface
+
+2.~~~~Diffuse visible reflectance of the unglazed part of the shading surface
+
+3.~~~~Fraction of shading surface that is glazed
+
+4.~~~~Name of glazing construction
+
+In this case \({f_{C,glazed}}\) is ``Fraction of shading surface that is glazed'' and \({\rho_{spec}}({\alpha_C})\) is the front reflectance of the indicated glazing construction as a function of beam solar incidence angle.
+
+The above specular reflection factor is used in the timestep calculation to find the beam irradiance on a receiving surface due to beam-beam reflection from obstructions:
+
+QRadSWOutIncBmToBmReflObsRecSurfNum) = BeamSolarRad * (WeightNow * ReflFacBmToBmSolObs(RecSurfNum,HourOfDay) + WeightPreviousHour * ReflFacBmToBmSolObs(RecSurfNum,PreviousHour))
diff --git a/doc/engineering-reference/src/special-modules-reporting.tex b/doc/engineering-reference/src/special-modules-reporting.tex
new file mode 100644
index 00000000000..cb095396235
--- /dev/null
+++ b/doc/engineering-reference/src/special-modules-reporting.tex
@@ -0,0 +1 @@
+\chapter{Special Modules/Reporting}\label{special-modulesreporting}
diff --git a/doc/engineering-reference/src/special-modules-reporting/environmental-impacts.tex b/doc/engineering-reference/src/special-modules-reporting/environmental-impacts.tex
new file mode 100644
index 00000000000..d7fb34e0e2e
--- /dev/null
+++ b/doc/engineering-reference/src/special-modules-reporting/environmental-impacts.tex
@@ -0,0 +1,613 @@
+\section{Environmental Impacts}\label{environmental-impacts}
+
+Typically when a new building technology is evaluated the energy performance of a baseline building is compared to the energy and life-cycle costs of alternatives to determine cost-effectiveness. But what if the lowest energy or life-cycle cost alternative is not the cleanest or lowest environmental impact?~ By calculating environmental impact, designers can compare alternatives not only in terms of their energy performance but also their environmental performance---working towards a more sustainable design (Liesen 1997; Stroot, Nemeth, and Fournier 1996).~ Environmental impacts are quantified, in part, by modeling the amount of emissions and in EnergyPlus this is done using the input objects ``EnvironmentalImpactFactors,'' ``FuelFactors,'' and ``Output:EnvironmentalImpactFactors.''
+
+Based on emissions factors entered by the user, EnergyPlus calculates the mass or volume of thirteen different pollutants: CO\(_{2}\) (carbon dioxide), CO (carbon monoxide), CH\(_{4}\) (methane), NO\(_{x}\) (nitrogen oxides), N\(_{2}\)O (nitrous oxide), SO\(_{2}\) (sulphur dioxide), PM (particulate matter), PM\(_{10}\) (particulate matter 10\textgreater{}PM\(_{10}\)\textgreater{}2.5 microns), PM\(_{2.5}\) (particulate matter\textless{}2.5 microns), NH\(_{3}\) (ammonia), NMVOC (non-methane volatile organic compounds), Hg (mercury), and Pb (lead) as well as water consumed through evaporation in thermo- and hydro-electric generation and high- and low-level nuclear waste from nuclear electricity generation for on- and off-site energy production.~ Note that while these comprise the largest proportion of pollutants, more than one hundred other pollutants are emitted from fossil fuel combustion or electricity generation. Much of the information compiled here for fossil fuel combustion comes from \emph{AP-42 Compilation of Air Pollutant Emission Factors} (EPA 1998a, 1998b, 1996).~ For more information on pollutants, see the U.S. Environmental Protection Agency (EPA) Clearinghouse for Inventories \& Emission Factors (\href{http://www.epa.gov/ttn/chief/efinformation.html}{www.epa.gov/ttn/chief/efinformation.html}).
+
+EnergyPlus models energy performance of on-site fossil fuels and purchased electricity (generated from a variety of fuels including natural gas, oil, gasoline, diesel, coal, hydroelectric, nuclear, wind, solar power, and biomass).~ The energy performance calculated by EnergyPlus is converted into a mass or volume of pollutants emitted.~ From a baseline building, alternative energy and pollution saving technologies can be explored, and the energy savings and pollution reduction can be calculated.~ Figure~\ref{fig:example-annual-atmospheric-pollutants} and Figure~\ref{fig:example-annual-total-carbon-equivalent-for} illustrate a comparison of two buildings simulated using Chicago weather data in EnergyPlus and the calculated pollutant levels (based on U.S. national average pollutants) (Crawley 2003).
+
+To calculate the mass or volume of each pollutant, consumption is multiplied by an emissions factor for each fuel (natural gas, electricity, fuel oil, diesel, or coal). In future versions, users will be able to schedule how the emissions factors by time of day, month, season and year.~ For electricity, the mix of generation fuel sources---whether utility, state or regional---is used to adjust the emission factors. ~If a user has emissions factors specific to the building site and equipment, these can be entered directly.~ \textbf{There are no default emissions factors}.
+
+\subsection{Types of Pollutants}\label{types-of-pollutants}
+
+EPA categorizes pollutants as either Criteria Pollutants or Hazardous Pollutants. Criteria pollutants are the six substances for which EPA has set health-based standards, including carbon monoxide (CO), nitrogen oxides (NO\(_{x}\)), sulfur dioxide (SO\(_{2}\)), and particulate matter (PM10 and PM2.5), ozone (O\(_{3}\)), and lead (Pb).~ Because ozone is created in atmospheric photochemical reactions of volatile organic compounds, ammonia, and other substances rather than direct building-related energy emissions, we do not calculated ozone emissions in EnergyPlus.~ But we do include ozone precursors: methane (CH\(_{4}\)), non-methane volatile organic compounds (NMVOC), and ammonia (NH\(_{3}\)). Hazardous pollutants are substances that are known or suspected to cause serious health problems such as cancer.~ We include typical hazardous substances associated with energy production and use including lead (Pb) and mercury (Hg). We also include CO\(_{2}\) (carbon dioxide) since it is largest greenhouse gas in terms of impact.
+
+\begin{figure}[hbtp] % fig 341
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7910.svg.png}
+\caption{Example Annual Atmospheric Pollutants and Water Consumption \protect \label{fig:example-annual-atmospheric-pollutants}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 342
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7911.svg.png}
+\caption{Example Annual Total Carbon Equivalent for Major Greenhouse Gases \protect \label{fig:example-annual-total-carbon-equivalent-for}}
+\end{figure}
+
+\subsection{Carbon Equivalent}\label{carbon-equivalent}
+
+The Intergovernmental Panel on Climate Change has studied the effects on the relative radiative forcing effects of various greenhouse gases.~ This effect, called Global Warming Potential (GWP), is described in terms of the Carbon Equivalent of a particular greenhouse gas.~ This equivalent is based on a factor of 1.0 for carbon.~ This group of gases includes carbon dioxide (CO\(_{2}\)), carbon monoxide, nitrous oxide, methane, halocarbon emission, hydrofluorocarbons (HFC), perfluorocarbons (PFC), and chlorofluorocarbons (CFC).~ For building energy use, the main gases of concern are carbon dioxide, carbon monoxide, methane, and nitrous oxide.~ Although carbon monoxide has a relatively short life, CO emissions into the atmosphere may have a significant impact on climate forcing due to chemical impact on CH\(_{4}\) lifetime, and tropospheric O\(_{3}\) and CO\(_{2}\) photochemical production normally reacts to produce carbon dioxide, but it can't be ignored since it is produced in incomplete combustion and the carbon remains to interact as CO\(_{2}\) Yet there is no agreement on its carbon equivalent (IPCC 2001). The carbon equivalent of carbon dioxide, methane, and nitrous oxide are calculated and then multiplied by their GWP on a 100 year time frame.~ The Carbon Equivalents of the following gases have been determined and used in the program are shown in the following table.
+
+% table 93
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Carbon Equivalents (IPCC 2001) \label{table:carbon-equivalents-ipcc-2001}} \tabularnewline
+\toprule 
+Gas & Carbon Equivalent \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Carbon Equivalents (IPCC 2001)} \tabularnewline
+\toprule 
+Gas & Carbon Equivalent \tabularnewline
+\midrule
+\endhead
+
+NO & 80.7272 \tabularnewline
+CH & 6.2727 \tabularnewline
+CO & 0.2727 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The resulting carbon equivalents by fuel type are shown in the output of the program along with the individual gas pollutants.
+
+\subsection{Fossil Fuel Emissions Factors}\label{fossil-fuel-emissions-factors}
+
+Emission factors for on-site fossil fuel consumption are based on Section 1.4 Natural Gas Combustion in EPA (1998a) Table~\ref{table:emission-factors-for-natural-gas} shows the greenhouse gas and precursors and criteria pollutant emissions factors for natural gas.~ Similar emissions factors are shown for residual fuel oil (No. 4 and No. 6 fuel oil) {[}Table~\ref{table:emission-factors-for-residual-fuel-oil-no.-4}{]}, distillates (No. 1 and No. 2 fuel oil) {[}Table~\ref{table:emission-factors-for-distillates-no.-1}{]}, residential oil furnace {[}Table~\ref{table:emission-factors-for-residential-oil-furnace}{]}, LPG (butane and propane) {[}Table~\ref{table:emission-factors-for-lpg-butane-and-propane}{]}, gasoline and diesel {[}Table~\ref{table:emission-factors-for-gasoline-and-diesel}{]}, and coal {[}Table~\ref{table:emission-factors-for-coal}{]} in the indicated tables.~ Note that a zero for a pollutant in the table may mean that no data were available, not that there are no emissions of that pollutant.
+
+% table 94
+\begin{longtable}[c]{p{4.5in}p{1.5in}}
+\caption{Emission Factors for Natural Gas \label{table:emission-factors-for-natural-gas}} \tabularnewline
+\toprule 
+Pollutant & Emission Factor  ~~ (g/MJ) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Emission Factors for Natural Gas} \tabularnewline
+\toprule 
+Pollutant & Emission Factor  ~~ (g/MJ) \tabularnewline
+\midrule
+\endhead
+
+Carbon Dioxide (CO  ) & 50.23439 \tabularnewline
+Carbon Monoxide (CO) & 3.51641E-02 \tabularnewline
+Methane (CH  ) & 9.62826E-04 \tabularnewline
+Nitrogen Oxides (NO  ) & 4.18620E-02 \tabularnewline
+Nitrous Oxide (N  O) & 9.20964E-04 \tabularnewline
+Sulphur Dioxide (SO  ) & 2.51172E-04 \tabularnewline
+Particulate Matter (PM) & 3.18151E-03 \tabularnewline
+Particulate Matter (PM10) & 2.38613E-03 \tabularnewline
+Particulate Matter (PM2.5) & 7.95378E-04 \tabularnewline
+Ammonia (NH  ) & 0 \tabularnewline
+Volatile Organic Compounds (NMVOC) & 2.30241E-03 \tabularnewline
+Mercury (Hg) & 1.08841E-07 \tabularnewline
+Lead (Pb) & 2.09310E-07 \tabularnewline
+a Based on data from Tables 1.4-1, 1.4.-2 and 1.4.4~ in EPA (1998a), Natural gas heat value of 1027 Btu/ft3 based on data for 2003 in Table A-4 in DOE (2004) \tabularnewline
+b Values shown are for uncontrolled burner.~ For controlled-low NO   burner, use 0.64 lb/106 ft3, 0.000627 lb/MMBtu, 0.0002679 g/MJ \tabularnewline
+c Based on 100\% conversion of fuel sulfur to SO  . Assumes sulfur content is natural gas of 2,000 grains/106 ft3. The SO2 emission factor can be converted to other natural gas sulfur contents by multiplying the SO   emission factor by the ratio of the site-specific sulfur content (grains/106 ft3) to 2,000 grains/106 ft3. \tabularnewline
+d PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively. \tabularnewline
+e No data \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 95
+\begin{longtable}[c]{p{4.5in}p{1.5in}}
+\caption{Emission Factors for Residual Fuel Oil (No. 4 and No. 6 Fuel Oil) \label{table:emission-factors-for-residual-fuel-oil-no.-4}} \tabularnewline
+\toprule 
+Pollutant & Emission Factor    (g/MJ) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Emission Factors for Residual Fuel Oil (No. 4 and No. 6 Fuel Oil)} \tabularnewline
+\toprule 
+Pollutant & Emission Factor    (g/MJ) \tabularnewline
+\midrule
+\endhead
+
+Carbon Dioxide (CO 2 ) & 50.23439 \tabularnewline
+Carbon Monoxide (CO) & 3.52E-002 \tabularnewline
+Methane (CH 4 ) & 9.63E-004 \tabularnewline
+Nitrogen Oxides (NO X ) & 4.19E-002 \tabularnewline
+Nitrous Oxide (N 2 O) & 9.21E-004 \tabularnewline
+Sulphur Dioxide (SO 2 ) & 2.51E-004 \tabularnewline
+Particulate Matter (PM) & 3.18E-003 \tabularnewline
+Particulate Matter (PM10) & 2.39E-003 \tabularnewline
+Particulate Matter (PM2.5) & 7.95E-004 \tabularnewline
+Ammonia (NH 3 ) & 0 \tabularnewline
+Volatile Organic Compounds (NMVOC) & 2.30E-003 \tabularnewline
+Mercury (Hg) & 1.09E-007 \tabularnewline
+Lead (Pb) & 2.09E-007 \tabularnewline
+Based on data from Tables 1.4-1, 1.4.-2 and 1.4.4 in EPA (1998a), Natural gas heat value of 1027 Btu/ft3 based on data for 2003 in Table A-4 in DOE (2004) \tabularnewline
+Values shown are for uncontrolled burner. For controlled-low NOX burner, use 0.64 lb/106 ft3, 0.000627 lb/MMBtu, 0.0002679 g/MJ \tabularnewline
+Based on 100\% conversion of fuel sulfur to SO2. Assumes sulfur content is natural gas of 2,000 contents by multiplying the SO2 emission factor by the ratio of the site-specific sulfur content (grains/106 ft3) to 2,000 grains/106 ft3. grains/106 ft3. The SO2 emission factor can be converted to other natural gas sulfur \tabularnewline
+PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively. \tabularnewline
+No data. \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 96
+\begin{longtable}[c]{p{3.0in}p{1.5in}p{1.5in}}
+\caption{Emission Factors for Distillates (No. 1 and No. 2 Fuel Oil) \label{table:emission-factors-for-distillates-no.-1}} \tabularnewline
+\toprule 
+Pollutant & No. 1 Fuel Oil Emission Factor   (g/MJ) & No. 2 Fuel Oil Emission Factor   (g/MJ) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Emission Factors for Distillates (No. 1 and No. 2 Fuel Oil)} \tabularnewline
+\toprule 
+Pollutant & No. 1 Fuel Oil Emission Factor   (g/MJ) & No. 2 Fuel Oil Emission Factor   (g/MJ) \tabularnewline
+\midrule
+\endhead
+
+Carbon Dioxide (CO  ) & 66.0233 & 68.47998 \tabularnewline
+Carbon Monoxide (CO) & 1.54E-002 & 1.54E-002 \tabularnewline
+Methane (CH  ) & 6.63E-004 & 6.63E-004 \tabularnewline
+Nitrogen Oxides (NO  ) & 6.14E-002 & 7.37E-002 \tabularnewline
+Nitrous Oxide (N  O) & 3.38E-004 & 3.38E-004 \tabularnewline
+Sulphur Dioxide (SO  ) & 4.36E-001 & 4.82E-001 \tabularnewline
+Particulate Matter (PM) & 6.14E-003 & 6.14E-003 \tabularnewline
+Particulate Matter (PM10) & 3.32E-003 & 3.32E-003 \tabularnewline
+Particulate Matter (PM2.5) & 2.55E-003 & 2.55E-003 \tabularnewline
+Ammonia (NH  ) & 0 & 0 \tabularnewline
+Volatile Organic Compounds (NMVOC) & 1.04E-003 & 1.04E-003 \tabularnewline
+Mercury (Hg) & 3.47E-006 & 3.47E-006 \tabularnewline
+Lead (Pb) & 4.64E-006 & 4.64E-006 \tabularnewline
+a Based on data from Tables 1.3-1, 1.3-3, 1-3.8, 1.3-10 and 1.3-12 in EPA (1998b). &  &  \tabularnewline
+b Based on 100\% conversion of fuel sulfur to SO  . Assumes 1\% sulfur content. The SO   emission factor in this table can be converted to other natural gas sulfur contents by multiplying the SO   emission factor by percentage sulfur content. &  &  \tabularnewline
+c PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively &  &  \tabularnewline
+d No data. &  &  \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 97
+\begin{longtable}[c]{p{4.5in}p{1.5in}}
+\caption{Emission Factors for Residential Oil Furnace \label{table:emission-factors-for-residential-oil-furnace}} \tabularnewline
+\toprule 
+Pollutant & Emission Factor  ~~ (g/MJ) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Emission Factors for Residential Oil Furnace} \tabularnewline
+\toprule 
+Pollutant & Emission Factor  ~~ (g/MJ) \tabularnewline
+\midrule
+\endhead
+
+Carbon Dioxide (CO  ) & 68.48237 \tabularnewline
+Carbon Monoxide (CO) & 1.53543E-02 \tabularnewline
+Methane (CH  ) & 5.46612E-02 \tabularnewline
+Nitrogen Oxides (NO  ) & 5.52753E-02 \tabularnewline
+Nitrous Oxide (N  O) & 1.53543E-04 \tabularnewline
+Sulphur Dioxide (SO  ) & 4.36061E-01 \tabularnewline
+Particulate Matter (PM) & 2.14960E-02 \tabularnewline
+Particulate Matter (PM10) & 1.58763E-02 \tabularnewline
+Particulate Matter (PM2.5) & 5.89603E-03 \tabularnewline
+Ammonia (NH  ) & 0 \tabularnewline
+Volatile Organic Compounds (NMVOC) & 2.18952E-03 \tabularnewline
+Mercury (Hg) & 3.47006E-06 \tabularnewline
+Lead (Pb) & 4.63699E-06 \tabularnewline
+a Based on data from Tables 1.3-1, 1.3-3, 1.3-8, 1.3-10, and 1.3-12 in EPA (1998b). \tabularnewline
+b Based on 100\% conversion of fuel sulfur to SO  . Assumes 1\% sulfur content. The SO   emission factor in this table can be converted to other natural gas sulfur contents by multiplying the SO   emission factor by percentage sulfur content. \tabularnewline
+c PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively. \tabularnewline
+d No data. \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 98
+\begin{longtable}[c]{p{3.0in}p{1.5in}p{1.5in}}
+\caption{Emission Factors for LPG (butane and propane) \label{table:emission-factors-for-lpg-butane-and-propane}} \tabularnewline
+\toprule 
+Pollutant & LPG (butane) Emission Factor    (g/MJ) & Propane Emission Factor    (g/MJ) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Emission Factors for LPG (butane and propane)} \tabularnewline
+\toprule 
+Pollutant & LPG (butane) Emission Factor    (g/MJ) & Propane Emission Factor    (g/MJ) \tabularnewline
+\midrule
+\endhead
+
+Carbon Dioxide (CO  ) & 66.0233 & 68.47998 \tabularnewline
+Carbon Monoxide (CO) & 1.54E-002 & 1.54E-002 \tabularnewline
+Methane (CH  ) & 6.63E-004 & 6.63E-004 \tabularnewline
+Nitrogen Oxides (NO  ) & 6.14E-002 & 7.37E-002 \tabularnewline
+Nitrous Oxide (N  O) & 3.38E-004 & 3.38E-004 \tabularnewline
+Sulphur Dioxide (SO  ) & 4.36E-001 & 4.82E-001 \tabularnewline
+Particulate Matter (PM) & 6.14E-003 & 6.14E-003 \tabularnewline
+Particulate Matter (PM10) & 3.32E-003 & 3.32E-003 \tabularnewline
+Particulate Matter (PM2.5) & 2.55E-003 & 2.55E-003 \tabularnewline
+Ammonia (NH  ) & 0 & 0 \tabularnewline
+Volatile Organic Compounds (NMVOC) & 1.04E-003 & 1.04E-003 \tabularnewline
+Mercury (Hg) & 3.47E-006 & 3.47E-006 \tabularnewline
+Lead (Pb) & 4.64E-006 & 4.64E-006 \tabularnewline
+a Based on data from Table \# 1.5-1 in EPA (1996); Higher Heating value of 1.02 MMBtu/gal for butane and 0.915 MMBtu/gal for propane based on data in EPA (1996). \tabularnewline
+b Based on 100\% conversion of fuel sulfur to SO  . Assumes sulphur content is 0.18 gr/100 ft3.The SO   emission factor can be converted to other LPG sulphur contents by multiplying the SO   emission factor by the ratio of the site-specific sulphur content gr/100 ft3 to 0.18 gr/100 ft3. \tabularnewline
+c PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns; respectively. \tabularnewline
+d No data. \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 99
+\begin{longtable}[c]{p{3.0in}p{1.5in}p{1.5in}}
+\caption{Emission Factors for Gasoline and Diesel \label{table:emission-factors-for-gasoline-and-diesel}} \tabularnewline
+\toprule 
+Pollutant & Gasoline Emission Factor   (g/MJ) & Diesel Emission Factor   (g/MJ) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Emission Factors for Gasoline and Diesel} \tabularnewline
+\toprule 
+Pollutant & Gasoline Emission Factor   (g/MJ) & Diesel Emission Factor   (g/MJ) \tabularnewline
+\midrule
+\endhead
+
+Carbon Dioxide (CO  ) & 66.20808 & 70.50731 \tabularnewline
+Carbon Monoxide (CO) & 2.70E+001 & 4.08E-001 \tabularnewline
+Methane (CH  ) & 0 & 0 \tabularnewline
+Nitrogen Oxides (NO  ) & 7.01E-001 & 1.90E+000 \tabularnewline
+Nitrous Oxide (N  O) & 0 & 0 \tabularnewline
+Sulphur Dioxide (SO  ) & 3.61E-002 & 1.25E-001 \tabularnewline
+Particulate Matter (PM) & 0 & 0 \tabularnewline
+Particulate Matter (PM10) & 4.30E-002 & 1.33E-001 \tabularnewline
+Particulate Matter (PM2.5) & 0 & 0 \tabularnewline
+Ammonia (NH  ) & 0 & 0 \tabularnewline
+Volatile Organic Compounds (NMVOC) & 9.03E-001 & 1.50E-001 \tabularnewline
+Mercury (Hg) & 0 & 0 \tabularnewline
+Lead (Pb) & 0 & 0 \tabularnewline
+a Based on data from Table \# 3.3-1 in EPA (1996); Diesel higher heating value of 19300 Btu/lb and gasoline higher heating value of 20300 Btu/lb based on data in EPA (1996). \tabularnewline
+b PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns; respectively. \tabularnewline
+c No data. \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 100
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Emission Factors for Coal \label{table:emission-factors-for-coal}} \tabularnewline
+\toprule 
+Pollutant & Bituminous Emission Factor   (g/MJ) & Anthracite Emission Factor   (g/MJ) & Lignite Emission Factor   (g/MJ) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Emission Factors for Coal} \tabularnewline
+\toprule 
+Pollutant & Bituminous Emission Factor   (g/MJ) & Anthracite Emission Factor   (g/MJ) & Lignite Emission Factor   (g/MJ) \tabularnewline
+\midrule
+\endhead
+
+Carbon Dioxide (CO  ) & 91.11052 & 99.26669 & 152.12646 \tabularnewline
+Carbon Monoxide (CO) & 8.27E-003 & 1.05E-002 & 8.27E-003 \tabularnewline
+Methane (CH  ) & 6.61E-004 & 0 & 0 \tabularnewline
+Nitrogen Oxides (NO  ) & 1.98E-001 & 3.15E-001 & 2.35E-001 \tabularnewline
+Nitrous Oxide (N  O) & 4.96E-004 & 0 & 0 \tabularnewline
+Sulphur Dioxide (SO  ) & 6.28E-001 & 6.82E-001 & 9.92E-001 \tabularnewline
+Particulate Matter (PM) & 1.65E-001 & 1.75E-001 & 2.18E-001 \tabularnewline
+Particulate Matter (PM10) & 3.80E-002 & 4.02E-002 & 7.61E-002 \tabularnewline
+Particulate Matter (PM2.5) & 9.92E-003 & 1.05E-002 & 2.18E-002 \tabularnewline
+Ammonia (NH  ) & 0 & 0 & 0 \tabularnewline
+Volatile Organic Compounds (NMVOC) & 9.92E-004 & 2.15E-002 & 1.32E-003 \tabularnewline
+Mercury (Hg) & 6.94E-006 & 2.27E-006 & 2.74E-006 \tabularnewline
+Lead (Pb) & 1.37E-006 & 1.56E-004 & 1.39E-005 \tabularnewline
+a Based on data on pulverized coal from Tables 1.1-3, 1.1-6, 1.1-18, 1.1-19 in EPA (1998a), Coal average higher heating value of 26.0 MMBtu/ton based on EPA (1998a). \tabularnewline
+b Based on data on pulverized coal from Tables 1.2-1, 1.2-2, 1.2-3, 1.2-4, 1.2-7 in EPA (1996), Coal average higher heating value of 24.6 MMBtu/ton based on EPA (1996). \tabularnewline
+c Based on data on pulverized coal from Tables 1.7-1, 1.7-3, 1.7-7, 1.7-14 in EPA (1998b), Coal average higher heating value of 13.0 MMBtu/ton based on EPA (1998b). \tabularnewline
+d Based on 100\% conversion of fuel sulfur to SO  . Assumes 1\% sulfur content. The SO   emission factor in this table can be converted to other natural gas sulfur contents by multiplying the SO   emission factor by percentage sulfur content. \tabularnewline
+e PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 are particles smaller than 10 and 2.5 microns, respectively. Expressed in terms of coal ash content, assumes 1\% ash content. Multiply weight \% ash content of coal (as fired) by the value. \tabularnewline
+f No data. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Off-Site Electricity Generation Emissions}\label{off-site-electricity-generation-emissions}
+
+While estimating emissions from on-site fossil fuel combustion can be fairly straight-forward, emissions from off-site electricity is more challenging.~ How the electricity is generated, i.e., from gas, oil, coal, nuclear, renewable sources (wind, PV) or hydroelectric, and the mix of generation determines the resulting level of emissions.~ While data are available at utility and even power plant level (from the sources cited), data are shown here for United States national- and state-level average emissions from electricity generation. Table~\ref{table:united-states-national-average-emission} provides average greenhouse gas and precursors and criteria pollutant emissions factors for the entire United States from electricity generation. Table~\ref{table:u.-s.-state-average-greenhouse-gas-emission} provides average electricity emissions factors by state, for greenhouse gas and precursors, and Table~\ref{table:u.-s.-state-average-criteria-pollutant} for criteria pollutant emission factors. These two tables also include a ratio of heat input to electric output (efficiency of electricity generation) including distribution and transmission losses to allow calculation of source energy.
+
+As mentioned in the introduction to this section, EnergyPlus also calculates water consumed through evaporation in thermo-electric and hydro-electric generation. Torcellini, Long, and Judkoff (2004) provide data on average water consumption by generator type by state.~ These data are summarized in units suitable for EnergyPlus in Table~\ref{table:united-states-national-average-emission}, for national and state average water consumption for thermal-electric, hydro-electric, and Table~\ref{table:u.-s.-state-average-greenhouse-gas-emission} for weighted total electricity generation.
+
+% table 101
+\begin{longtable}[c]{p{4.5in}p{1.5in}}
+\caption{United States National Average Emission Factors for Electricity Generation \label{table:united-states-national-average-emission}} \tabularnewline
+\toprule 
+~ & Efficiency Ratio (J/J) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{United States National Average Emission Factors for Electricity Generation} \tabularnewline
+\toprule 
+~ & Efficiency Ratio (J/J) \tabularnewline
+\midrule
+\endhead
+
+Ratio of Heat Input to Electricity Output & 2.253 \tabularnewline
+~ & ~ \tabularnewline \midrule
+Pollutant & Emission Factor~~ (g/MJ) \tabularnewline \midrule
+Carbon Dioxide (CO  ) & 168.333168 \tabularnewline
+Carbon Monoxide (CO) & 4.20616E-02 \tabularnewline
+Methane (CH  ) & 1.39858E-03 \tabularnewline
+Nitrogen Oxides (NO  ) & 4.10753E-01 \tabularnewline
+Nitrous Oxide (N  O) & 2.41916E-03 \tabularnewline
+Sulphur Dioxide (SO  ) & 8.65731E-01 \tabularnewline
+Particulate Matter (PM) & 2.95827E-02 \tabularnewline
+Particulate Matter (PM10) & 1.80450E-02 \tabularnewline
+Particulate Matter (PM2.5) & 1.15377E-02 \tabularnewline
+Ammonia (NH  ) & 1.10837E-03 \tabularnewline
+Volatile Organic Compounds (NMVOC) & 3.72332E-03 \tabularnewline
+Mercury (Hg) & 3.36414E-06 \tabularnewline
+Lead (Pb) & 0 \tabularnewline
+Data based on 1999 data from *eGRID* version 2.01 (EPA 2003a). \tabularnewline
+Data based on 1998-2000 average data in DOE (2002). \tabularnewline
+Data based on tier emissions report for criteria air pollutants in EPA (2003b). \tabularnewline
+PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively. \tabularnewline
+No data. \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 102
+\begin{longtable}[c]{p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}}
+\caption{U. S. State Average Greenhouse Gas Emission Factors for Electricity Generation, in g/MJ \label{table:u.-s.-state-average-greenhouse-gas-emission}} \tabularnewline
+\toprule 
+ & Ratio of Heat Input to Electric Output & Carbon Dioxide (CO 2 ) b & Carbon Monoxide (CO) c & Methane (CH4) b & Nitrogen Oxides (NO X ) a & Nitrous Oxide (N 2 O) b & Sulphur Dioxide (SO 2 ) a \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{U. S. State Average Greenhouse Gas Emission Factors for Electricity Generation, in g/MJ} \tabularnewline
+\toprule 
+ & Ratio of Heat Input to Electric Output & Carbon Dioxide (CO 2 ) b & Carbon Monoxide (CO) c & Methane (CH4) b & Nitrogen Oxides (NO X ) a & Nitrous Oxide (N 2 O) b & Sulphur Dioxide (SO 2 ) a \tabularnewline
+\midrule
+\endhead
+
+Alabama & 2.23 & 165.30922 & 1.45E+003 & 1.73E-003 & 4.02E-001 & 2.81E-003 & 1.14E+000 \tabularnewline
+Alaska & 2.734 & 173.87708 & 3.72E+002 & 8.57E-004 & 7.29E-001 & 1.12E-003 & 2.38E-001 \tabularnewline
+Arizona & 1.694 & 132.29777 & 8.27E+002 & 8.57E-004 & 2.74E-001 & 1.94E-003 & 2.28E-001 \tabularnewline
+Arkansas & 2.207 & 162.03327 & 6.42E+002 & 1.57E-003 & 2.87E-001 & 2.56E-003 & 4.25E-001 \tabularnewline
+California & 1.422 & 76.35472 & 2.91E+003 & 8.44E-004 & 6.56E-002 & 4.66E-004 & 3.05E-002 \tabularnewline
+Colorado & 3.101 & 242.67192 & 1.51E+003 & 1.60E-003 & 4.74E-001 & 3.64E-003 & 5.84E-001 \tabularnewline
+Connecticut & 1.72 & 118.69 & 3.21E+002 & 2.19E-003 & 1.82E-001 & 1.51E-003 & 3.79E-001 \tabularnewline
+Delaware & 2.736 & 230.57612 & 1.31E+002 & 1.55E-003 & 4.13E-001 & 2.86E-003 & 1.11E+000 \tabularnewline
+District of Columbia & 4.844 & 172.1131 & 8.95E+000 & 1.49E-003 & 7.30E-001 & 2.60E-003 & 1.62E+000 \tabularnewline
+Florida & 2.694 & 175.64105 & 6.13E+003 & 1.89E-003 & 4.73E-001 & 2.27E-003 & 1.01E+000 \tabularnewline
+Georgia & 2.119 & 172.1131 & 1.06E+003 & 1.63E-003 & 4.00E-001 & 2.85E-003 & 1.12E+000 \tabularnewline
+Hawaii & 2.95 & 209.40848 & 1.18E+002 & 2.70E-003 & 7.28E-001 & 2.31E-003 & 5.44E-001 \tabularnewline
+Idaho & 0.213 & 3.52794 & 0 & 1.01E-003 & 1.07E-002 & 4.16E-004 & 1.06E-002 \tabularnewline
+Illinois & 1.694 & 146.66153 & 1.85E+003 & 1.03E-003 & 4.42E-001 & 2.27E-003 & 1.12E+000 \tabularnewline
+Indiana & 3.281 & 261.5716 & 2.14E+003 & 1.80E-003 & 7.30E-001 & 4.07E-003 & 1.89E+000 \tabularnewline
+Iowa & 3.033 & 237.12801 & 7.58E+002 & 1.74E-003 & 5.61E-001 & 3.75E-003 & 1.05E+000 \tabularnewline
+Kansas & 2.826 & 212.18043 & 8.66E+002 & 1.41E-003 & 5.59E-001 & 3.20E-003 & 7.07E-001 \tabularnewline
+Kentucky & 3.234 & 253.00374 & 1.51E+003 & 1.76E-003 & 8.41E-001 & 4.04E-003 & 1.79E+000 \tabularnewline
+Lousiana & 2.624 & 148.4255 & 1.68E+004 & 1.18E-003 & 3.42E-001 & 1.41E-003 & 5.06E-001 \tabularnewline
+Maine & 2.191 & 107.35019 & 4.93E+002 & 7.12E-003 & 1.80E-001 & 3.40E-003 & 4.04E-001 \tabularnewline
+Maryland & 2.277 & 172.1131 & 4.90E+002 & 1.49E-003 & 5.38E-001 & 2.60E-003 & 1.39E+000 \tabularnewline
+Massachusetts & 2.729 & 161.02529 & 7.89E+002 & 2.19E-003 & 2.89E-001 & 2.00E-003 & 8.01E-001 \tabularnewline
+Michigan & 2.616 & 199.07665 & 1.69E+003 & 1.84E-003 & 4.92E-001 & 3.15E-003 & 9.77E-001 \tabularnewline
+Minnesota & 2.331 & 163.04126 & 6.96E+002 & 1.66E-003 & 5.02E-001 & 2.08E-003 & 5.07E-001 \tabularnewline
+Mississippi & 2.404 & 231.8361 & 2.18E+003 & 1.59E-003 & 4.67E-001 & 3.63E-003 & 8.98E-001 \tabularnewline
+Missouri & 2.857 & 192.02077 & 1.30E+003 & 1.98E-003 & 6.42E-001 & 3.11E-003 & 9.07E-001 \tabularnewline
+Montana & 1.936 & 180.68096 & 4.13E+002 & 1.36E-003 & 3.58E-001 & 2.86E-003 & 2.01E-001 \tabularnewline
+Nebraska & 2.195 & 176.39703 & 4.68E+002 & 1.20E-003 & 3.94E-001 & 2.76E-003 & 5.29E-001 \tabularnewline
+Nevada & 2.615 & 191.26478 & 3.82E+002 & 1.13E-003 & 4.02E-001 & 2.46E-003 & 4.03E-001 \tabularnewline
+New Hampshire & 1.394 & 85.93055 & 2.64E+002 & 2.17E-003 & 2.03E-001 & 1.78E-003 & 8.71E-001 \tabularnewline
+New Jersey & 1.451 & 88.9545 & 2.27E+003 & 9.70E-004 & 1.77E-001 & 9.95E-004 & 2.31E-001 \tabularnewline
+New Mexico & 3.307 & 254.26372 & 8.56E+002 & 1.65E-003 & 6.58E-001 & 3.73E-003 & 5.70E-001 \tabularnewline
+New York & 1.808 & 108.10618 & 1.94E+003 & 1.02E-003 & 1.69E-001 & 1.12E-003 & 4.68E-001 \tabularnewline
+North Carolina & 1.969 & 156.48937 & 1.10E+003 & 1.32E-003 & 4.69E-001 & 2.56E-003 & 1.00E+000 \tabularnewline
+North Dakota & 3.244 & 282.48725 & 9.01E+002 & 1.85E-003 & 6.45E-001 & 4.27E-003 & 1.53E+000 \tabularnewline
+Ohio & 2.736 & 226.79619 & 1.59E+003 & 1.64E-003 & 7.68E-001 & 3.63E-003 & 2.34E+000 \tabularnewline
+Oklahoma & 3.024 & 216.96835 & 1.67E+003 & 1.39E-003 & 5.11E-001 & 2.81E-003 & 5.11E-001 \tabularnewline
+Oregon & 0.526 & 35.5314 & 1.87E+002 & 4.16E-004 & 5.27E-002 & 4.28E-004 & 7.51E-002 \tabularnewline
+Pennsylvania & 1.827 & 159.26132 & 1.86E+003 & 1.35E-003 & 3.29E-001 & 2.56E-003 & 1.26E+000 \tabularnewline
+Rhode Island & 2.561 & 132.54977 & 1.68E+002 & 8.57E-004 & 6.21E-002 & 5.92E-004 & 4.54E-003 \tabularnewline
+South Carolina & 1.3 & 105.08223 & 8.39E+002 & 1.15E-003 & 2.54E-001 & 1.83E-003 & 6.05E-001 \tabularnewline
+South Dakota & 1.192 & 100.54631 & 9.79E+001 & 6.68E-004 & 5.45E-001 & 1.52E-003 & 5.81E-001 \tabularnewline
+Tennessee & 1.902 & 163.29325 & 9.10E+002 & 1.32E-003 & 5.10E-001 & 2.67E-003 & 1.18E+000 \tabularnewline
+Texas & 2.749 & 184.4609 & 9.63E+003 & 9.70E-004 & 3.28E-001 & 1.84E-003 & 4.91E-001 \tabularnewline
+Utah & 3.095 & 243.6799 & 5.13E+002 & 1.69E-003 & 5.27E-001 & 3.88E-003 & 2.13E-001 \tabularnewline
+Vermont & 0.306 & 3.52794 & 1.38E+002 & 1.21E-003 & 1.94E-002 & 4.91E-004 & 2.14E-003 \tabularnewline
+Virginia & 1.924 & 146.66153 & 9.13E+002 & 1.73E-003 & 3.65E-001 & 2.42E-003 & 7.87E-001 \tabularnewline
+Washington & 0.414 & 30.99548 & 4.30E+002 & 4.66E-004 & 5.30E-002 & 5.04E-004 & 1.90E-001 \tabularnewline
+West Virginia & 2.917 & 248.97181 & 1.28E+003 & 1.73E-003 & 7.78E-001 & 3.98E-003 & 1.87E+000 \tabularnewline
+Wisconsin & 2.68 & 206.88852 & 1.00E+003 & 1.74E-003 & 4.97E-001 & 3.28E-003 & 9.25E-001 \tabularnewline
+Wyoming & 3.534 & 270.39145 & 9.01E+002 & 1.85E-003 & 5.59E-001 & 4.26E-003 & 5.79E-001 \tabularnewline
+a Data based on 1999 data from eGRID version 2.01 (EPA 2003a). \tabularnewline
+b Data based on 1998-2000 average data in DOE (2002). \tabularnewline
+c Data based on tier emissions report for criteria air pollutants in EPA (2003b). \tabularnewline
+d PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively. \tabularnewline
+e No data. \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 103
+\begin{longtable}[c]{p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}}
+\caption{U. S. State Average Criteria Pollutant Emission Factors for Electricity Generation, in g/MJ \label{table:u.-s.-state-average-criteria-pollutant}} \tabularnewline
+\toprule 
+~ & Particulate Matter (PM) & Particulate Matter (PM10) & Particulate Matter (PM2.5) & Ammonia (NH  ) & Volatile Organic Compounds (NMVOC) & Mercury (Hg) & Lead (Pb) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{U. S. State Average Criteria Pollutant Emission Factors for Electricity Generation, in g/MJ} \tabularnewline
+\toprule 
+~ & Particulate Matter (PM) & Particulate Matter (PM10) & Particulate Matter (PM2.5) & Ammonia (NH  ) & Volatile Organic Compounds (NMVOC) & Mercury (Hg) & Lead (Pb) \tabularnewline
+\midrule
+\endhead
+
+Alabama & 7.91048E-03 & 7.86328E-03 & 4.72023E-05 & 3.55049E-05 & 4.66784E-03 & 5.14071E-06 & 0 \tabularnewline
+Alaska & 8.96502E-03 & 8.85977E-03 & 1.05247E-04 & 6.51454E-06 & 2.82297E-03 & 3.27594E-07 & 0 \tabularnewline
+Arizona & 1.70555E-02 & 1.69322E-02 & 1.23202E-04 & 1.80226E-04 & 2.27385E-03 & 1.88997E-06 & 0 \tabularnewline
+Arkansas & 9.27803E-03 & 9.19307E-03 & 8.49561E-05 & 4.59383E-04 & 3.46429E-03 & 2.73415E-06 & 0 \tabularnewline
+California & 7.16813E-03 & 7.07819E-03 & 8.99402E-05 & 4.02651E-03 & 2.62453E-03 & 1.38598E-07 & 0 \tabularnewline
+Colorado & 7.29822E-03 & 7.23699E-03 & 6.12291E-05 & 9.56430E-05 & 4.36770E-03 & 1.62537E-06 & 0 \tabularnewline
+Connecticut & 1.22734E-02 & 1.21694E-02 & 1.04033E-04 & 2.22944E-03 & 3.93896E-03 & 1.18438E-06 & 0 \tabularnewline
+Delaware & 1.39283E-02 & 1.38287E-02 & 9.96131E-05 & 1.54469E-03 & 4.74441E-03 & 3.62874E-06 & 0 \tabularnewline
+District of Columbia & 2.88269E-02 & 2.84861E-02 & 3.40760E-04 & 8.76496E-03 & 2.30080E-02 & 0 & 0 \tabularnewline
+Florida & 4.33040E-02 & 4.29055E-02 & 3.98460E-04 & 1.58386E-03 & 3.39110E-03 & 1.71357E-06 & 0 \tabularnewline
+Georgia & 2.05237E-02 & 2.03865E-02 & 1.37175E-04 & 7.51637E-05 & 2.16686E-03 & 3.20035E-06 & 0 \tabularnewline
+Hawaii & 5.97339E-03 & 5.90409E-03 & 6.92999E-05 & 3.55697E-03 & 7.01715E-03 & 1.77657E-06 & 0 \tabularnewline
+Idaho & 0 & 0 & 0 & 0 & 0 & 0 & 0 \tabularnewline
+Illinois & 1.53276E-01 & 1.52156E-01 & 1.12047E-03 & 5.93583E-03 & 2.77818E-02 & 4.62412E-06 & 0 \tabularnewline
+Indiana & 2.18862E-02 & 2.17008E-02 & 1.85453E-04 & 5.75861E-04 & 4.87283E-03 & 4.86352E-06 & 0 \tabularnewline
+Iowa & 2.34564E-02 & 2.32698E-02 & 1.86674E-04 & 9.09228E-05 & 4.78644E-03 & 6.19910E-06 & 0 \tabularnewline
+Kansas & 2.41783E-02 & 2.39535E-02 & 2.24799E-04 & 4.19292E-04 & 5.39089E-03 & 4.93912E-06 & 0 \tabularnewline
+Kentucky & 1.69397E-02 & 1.68139E-02 & 1.25825E-04 & 4.35029E-05 & 3.80922E-03 & 4.71232E-06 & 0 \tabularnewline
+Lousiana & 1.79917E-02 & 1.77843E-02 & 2.07304E-04 & 1.66720E-03 & 1.02357E-02 & 1.41118E-06 & 0 \tabularnewline
+Maine & 3.36399E-03 & 3.34131E-03 & 2.26813E-05 & 1.55132E-03 & 9.62614E-03 & 4.53592E-07 & 0 \tabularnewline
+Maryland & 2.13382E-02 & 2.12038E-02 & 1.34391E-04 & 7.21581E-04 & 2.78881E-03 & 4.88872E-06 & 0 \tabularnewline
+Mass-achusetts & 8.85244E-03 & 8.76617E-03 & 8.62772E-05 & 1.70282E-03 & 3.49171E-03 & 1.88997E-06 & 0 \tabularnewline
+Michigan & 9.08755E-03 & 9.00520E-03 & 8.23449E-05 & 2.22140E-04 & 2.79017E-03 & 3.67914E-06 & 0 \tabularnewline
+Minnesota & 4.04781E-02 & 4.01455E-02 & 3.32617E-04 & 6.74889E-05 & 4.13240E-03 & 3.30114E-06 & 0 \tabularnewline
+Mississippi & 5.44446E-02 & 5.37910E-02 & 6.53601E-04 & 4.06289E-02 & 1.54329E-02 & 2.45696E-06 & 0 \tabularnewline
+Missouri & 1.25537E-02 & 1.24368E-02 & 1.16929E-04 & 6.48638E-05 & 4.98085E-03 & 4.67452E-06 & 0 \tabularnewline
+Montana & 3.67504E-03 & 3.64126E-03 & 3.37798E-05 & 4.01020E-05 & 3.14400E-03 & 3.77994E-06 & 0 \tabularnewline
+Nebraska & 1.33751E-02 & 1.32829E-02 & 9.21636E-05 & 6.90470E-05 & 5.23031E-03 & 3.59094E-06 & 0 \tabularnewline
+Nevada & 2.09146E-02 & 2.07657E-02 & 1.48886E-04 & 3.79659E-04 & 3.33440E-03 & 1.36078E-06 & 0 \tabularnewline
+New Hampshire & 3.09503E-02 & 3.06487E-02 & 3.01568E-04 & 7.16019E-04 & 2.45937E-03 & 3.40194E-07 & 0 \tabularnewline
+New Jersey & 3.45712E-02 & 3.41460E-02 & 4.25200E-04 & 1.24216E-04 & 1.52830E-02 & 1.28518E-06 & 0 \tabularnewline
+New Mexico & 5.20754E-02 & 5.16748E-02 & 4.00653E-04 & 4.41665E-04 & 5.12951E-03 & 8.41666E-06 & 0 \tabularnewline
+New York & 5.35802E-03 & 5.31301E-03 & 4.50068E-05 & 2.22325E-03 & 4.26008E-03 & 1.33558E-06 & 0 \tabularnewline
+North Carolina & 3.40955E-02 & 3.38325E-02 & 2.62976E-04 & 3.00504E-05 & 1.73434E-03 & 3.33894E-06 & 0 \tabularnewline
+North Dakota & 5.17162E-02 & 5.13979E-02 & 3.18277E-04 & 6.41672E-05 & 6.88995E-03 & 8.71905E-06 & 0 \tabularnewline
+Ohio & 1.38722E-02 & 1.37957E-02 & 7.64501E-05 & 1.11541E-04 & 2.59201E-03 & 6.24949E-06 & 0 \tabularnewline
+Oklahoma & 1.83971E-02 & 1.82479E-02 & 1.49160E-04 & 9.73713E-04 & 4.68484E-03 & 3.88073E-06 & 0 \tabularnewline
+Oregon & 3.47911E-03 & 3.46199E-03 & 1.71186E-05 & 4.43277E-06 & 5.31933E-04 & 3.77994E-07 & 0 \tabularnewline
+Pennsylvania & 2.21604E-02 & 2.20060E-02 & 1.54356E-04 & 1.47657E-04 & 1.51542E-03 & 6.56449E-06 & 0 \tabularnewline
+Rhode Island & 1.03973E-03 & 1.02744E-03 & 1.22906E-05 & 0 & 2.25247E-03 & 0 & 0 \tabularnewline
+South Carolina & 2.45530E-02 & 2.43803E-02 & 1.72632E-04 & 2.51344E-05 & 1.16735E-03 & 1.54977E-06 & 0 \tabularnewline
+South Dakota & 4.67825E-03 & 4.63562E-03 & 4.26239E-05 & 8.82976E-05 & 4.63562E-03 & 1.22218E-06 & 0 \tabularnewline
+Tennessee & 2.51650E-02 & 2.48944E-02 & 2.70575E-04 & 2.70034E-05 & 2.88396E-03 & 2.98615E-06 & 0 \tabularnewline
+Texas & 1.73147E-02 & 1.71765E-02 & 1.38283E-04 & 1.26310E-03 & 4.32150E-03 & 3.52794E-06 & 0 \tabularnewline
+Utah & 1.47314E-02 & 1.46364E-02 & 9.50155E-05 & 9.59315E-05 & 2.48737E-03 & 9.70184E-07 & 0 \tabularnewline
+Vermont & 1.16247E-03 & 1.14873E-03 & 1.37415E-05 & 1.80704E-05 & 2.12073E-03 & 0 & 0 \tabularnewline
+Virginia & 1.22315E-02 & 1.21362E-02 & 9.53635E-05 & 2.93259E-04 & 2.50975E-03 & 2.21756E-06 & 0 \tabularnewline
+Washington & 5.37627E-04 & 5.32210E-04 & 5.41708E-06 & 6.46409E-06 & 6.87348E-04 & 5.92190E-07 & 0 \tabularnewline
+West Virginia & 2.39677E-03 & 2.38177E-03 & 1.50018E-05 & 4.25792E-05 & 3.09497E-03 & 6.55189E-06 & 0 \tabularnewline
+Wisconsin & 7.34187E-03 & 7.28252E-03 & 5.93472E-05 & 6.45613E-05 & 4.61829E-03 & 4.83832E-06 & 0 \tabularnewline
+Wyoming & 5.08215E-02 & 5.06042E-02 & 2.17349E-04 & 5.19787E-05 & 4.78782E-03 & 5.27931E-06 & 0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 104
+\begin{longtable}[c]{p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}}
+\caption{United States National Average Water Consumption Factorssup{}a \label{table:united-states-national-average-water}} \tabularnewline
+\toprule 
+ & ThermoElectric Generation & HydroElectric Generation & Weighted Total Water Consumption \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{United States National Average Water Consumption Factorssup{}a} \tabularnewline
+\toprule 
+ & ThermoElectric Generation & HydroElectric Generation & Weighted Total Water Consumption \tabularnewline
+\midrule
+\endhead
+
+ & L/MJ & Percent of Total Generation & L/MJ & Percent of Total Generation & L/MJ \tabularnewline
+United States & 0.4960 & 89.4\% & 19.2095 & 8.6\% & 2.1007 \tabularnewline
+a Based on data from Torcellini, Long, and Judkoff (2004). \tabularnewline
+\bottomrule
+\end{longtable}
+
+% table 105
+\begin{longtable}[c]{p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}}
+\caption{U.S. State Average Water Consumption Factors for Electricity Generationsup{}a \label{table:u.s.-state-average-water-consumption-factors}} \tabularnewline
+\toprule 
+ & ThermoElectric Generation & HydroElectric Generation & Weighted Total Water Consumption \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{U.S. State Average Water Consumption Factors for Electricity Generationsup{}a} \tabularnewline
+\toprule 
+ & ThermoElectric Generation & HydroElectric Generation & Weighted Total Water Consumption \tabularnewline
+\midrule
+\endhead
+
+State & L/MJ & Percent of Total Generation & L/MJ & Percent of Total Generation & L/MJ \tabularnewline
+Alabama & 0.1503 & 89.80\% & 38.9053 & 6.4\% & 2.6274 \tabularnewline
+Alaska & 0.3295 & 86.20\% & -- & 13.8\% & 0.2839 \tabularnewline
+Arizona & 0.3313 & 88.30\% & 68.1928 & 11.7\% & 8.2533 \tabularnewline
+Arkansas & 0.3 & 89.50\% & -- & 5.7\% & 0.2684 \tabularnewline
+California & 0.0511 & 74.10\% & 21.943 & 22.0\% & 4.8739 \tabularnewline
+Colorado & 0.5368 & 96.00\% & 18.8333 & 4.0\% & 1.26 \tabularnewline
+Connecticut & 0.086 & 90.80\% & -- & 1.5\% & 0.0781 \tabularnewline
+Delaware & 0.0132 & 99.90\% & -- & 0.0\% & 0.0132 \tabularnewline
+District of Columbia & 1.6959 & 100.00\% & -- & 0.0\% & 1.6959 \tabularnewline
+Florida & 0.1506 & 95.70\% & -- & 0.1\% & 0.1441 \tabularnewline
+Georgia & 0.6267 & 93.60\% & 49.8599 & 2.3\% & 1.7339 \tabularnewline
+Hawaii & 0.044 & 92.40\% & -- & 1.1\% & 0.0407 \tabularnewline
+Idaho & 0 & 2.70\% & 8.9528 & 92.2\% & 8.2501 \tabularnewline
+Illinois & 1.1093 & 99.40\% & -- & 0.1\% & 1.1032 \tabularnewline
+Indiana & 0.435 & 99.60\% & -- & 0.3\% & 0.4331 \tabularnewline
+Iowa & 0.1229 & 97.30\% & -- & 2.5\% & 0.1196 \tabularnewline
+Kansas & 0.6099 & 100.00\% & -- & 0.0\% & 0.6098 \tabularnewline
+Kentucky & 1.1521 & 97.20\% & 162.2884 & 2.8\% & 5.599 \tabularnewline
+Louisiana & 1.6411 & 94.20\% & -- & 0.9\% & 1.5461 \tabularnewline
+Maine & 0.3049 & 40.40\% & -- & 28.7\% & 0.1231 \tabularnewline
+Maryland & 0.0343 & 95.30\% & 7.0617 & 2.7\% & 0.2259 \tabularnewline
+Massachusetts & 0 & 92.40\% & -- & 2.4\% & 0 \tabularnewline
+Michigan & 0.5221 & 95.80\% & -- & 1.4\% & 0.4999 \tabularnewline
+Minnesota & 0.4657 & 93.40\% & -- & 2.4\% & 0.4351 \tabularnewline
+Mississippi & 0.4145 & 94.40\% & -- & 0.0\% & 0.3912 \tabularnewline
+Missouri & 0.3213 & 97.40\% & -- & 2.5\% & 0.313 \tabularnewline
+Montana & 1.0051 & 55.80\% & 38.6619 & 44.1\% & 17.5997 \tabularnewline
+Nebraska & 0.202 & 94.50\% & 2.2888 & 5.5\% & 0.3165 \tabularnewline
+Nevada & 0.5936 & 90.60\% & 77.1023 & 9.2\% & 7.626 \tabularnewline
+New Hampshire & 0.1231 & 83.90\% & -- & 8.6\% & 0.1033 \tabularnewline
+New Jersey & 0.0747 & 97.60\% & -- & 0.0\% & 0.0729 \tabularnewline
+New Mexico & 0.6609 & 99.30\% & 71.507 & 0.7\% & 1.1886 \tabularnewline
+New York & 0.8951 & 81.30\% & 5.8535 & 16.7\% & 1.704 \tabularnewline
+North Carolina & 0.2445 & 95.50\% & 10.9089 & 3.1\% & 0.5751 \tabularnewline
+North Dakota & 0.3809 & 91.70\% & 60.773 & 8.3\% & 5.3968 \tabularnewline
+Ohio & 0.9972 & 99.10\% & -- & 0.3\% & 0.9884 \tabularnewline
+Oklahoma & 0.5378 & 93.70\% & 144.0133 & 5.8\% & 8.8254 \tabularnewline
+Oregon & 0.8633 & 18.40\% & 4.6351 & 80.7\% & 3.899 \tabularnewline
+Pennsylvania & 0.57 & 97.60\% & -- & 1.0\% & 0.5563 \tabularnewline
+Rhode Island & 0 & 98.20\% & -- & 0.1\% & 0 \tabularnewline
+South Carolina & 0.2754 & 97.20\% & -- & 1.9\% & 0.2677 \tabularnewline
+South Dakota & 0.0143 & 36.70\% & 120.7558 & 63.2\% & 76.3811 \tabularnewline
+Tennessee & 0.0026 & 90.80\% & 45.5853 & 8.3\% & 3.7833 \tabularnewline
+Texas & 0.4595 & 99.00\% & -- & 0.3\% & 0.455 \tabularnewline
+Utah & 0.5959 & 96.60\% & 77.115 & 3.4\% & 3.209 \tabularnewline
+Vermont & 0.3642 & 71.50\% & -- & 20.9\% & 0.2605 \tabularnewline
+Virginia & 0.0693 & 94.90\% & -- & 0.9\% & 0.0657 \tabularnewline
+Washington & 0.3013 & 15.70\% & 3.3506 & 83.2\% & 2.8344 \tabularnewline
+West Virginia & 0.618 & 99.00\% & -- & 1.0\% & 0.6119 \tabularnewline
+Wisconsin & 0.5199 & 93.60\% & -- & 3.3\% & 0.4867 \tabularnewline
+Wyoming & 0.519 & 97.10\% & 144.0177 & 2.7\% & 4.3654 \tabularnewline
+a Based on data from Torcellini, Long, and Judkoff (2004). \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Other Energy-Related Pollutants and Sources of Other Information}\label{other-energy-related-pollutants-and-sources-of-other-information}
+
+EnergyPlus (with user entered-data) will also calculate high- and low-level nuclear waste from electricity generation. Few utilities now provide data on nuclear waste resulting from electricity generation and no US national or state-level data are yet available (this will be added as data become available).~ Two Illinois utilities regularly report nuclear waste in terms of pounds per kWh or MWh for high-level waste and cubic feet per kWh or MWh for low-level waste.~ For these two utilities, high level nuclear waste values range from 0.0042 to 0.01 lb/MWh (7000 to 16000 g/MJ); low-level nuclear waste ranges from 0.0001 to 0.0002 ft\(^{3}\)/MWh (0.01 to 0.02 m\(^{3}\)/MJ) depending on relative proportion of nuclear as compared with other electricity generation sources.
+
+IEA (2003) contains carbon dioxide (CO\(_{2}\)) emissions factors for electricity generation by country and region. Carbon dioxide (CO\(_{2}\)) is responsible for over 60\% of the anthropogenic greenhouse effect (UNEP 2002). Because only limited greenhouse gas emissions factors and data (other than CO\(_{2}\)) is available for other countries, an interim method for estimating emission factors would be to compare the CO\(_{2}\) emission factor for the particular country from IEA (2003) and match it to the state with the closest CO\(_{2}\) emission factor in Table~\ref{table:u.-s.-state-average-greenhouse-gas-emission}---using the other emissions factors for that state. Since the Kyoto Protocol (UNFCCC 1997) requires each country to report emissions of the major greenhouse gases {[}carbon dioxide (CO\(_{2}\)), methane (CH\(_{4}\)), and nitrous oxide (N\(_{2}\)O){]} as well as ozone-depleting substances {[}hydrofluorocarbons (HFC), perfluorocarbons (PFC), and sulphur hexafluoride (SF\(_{6}\)){]} and all energy consumption in their annual `national communication', more complete emission factors for a larger number of countries should become available over the next few years. More information and other resources for calculating emissions factors are available in IPCC (2000, 1997).
+
+\subsection{References}\label{references-022}
+
+Crawley, Drury B.~ 2003.~ ``Impact of Climate Change on Buildings,'' in \emph{Proceedings of the CIBSE/ASHRAE International Conference 2003}, September 2003, Edinburgh, Scotland.~ London, England: CIBSE.
+
+Intergovernmental Panel on Climate Change.~ 2001.~ \emph{Climate Change 2001: The Scientific Basis}.~ Cambridge: Cambridge University Press.
+
+Intergovernmental Panel on Climate Change. 2000. \emph{Good Practice Guidance and Uncertainty Management in National Greenhouse Gas Inventories}, Paris, France: IPCC/OECD/IEA.
+
+Intergovernmental Panel on Climate Change. 1997. \emph{Revised 1996 IPCC Guidelines for National Greenhouse Gas Inventories}, J.T. Houghton, L.G. Meira Filho, B. Lim, K. Treanton, I. Mamaty, Y. Bonduki, D.J. Griggs and B.A. Callender (editors).~ Paris, France: IPCC/OECD/IEA.
+
+International Energy Agency.~ 2003. \emph{CO\(_{2}\) Emissions from Fuel Combustion 1971-2001 (2003) -- 2003 Edition}.~ Paris, France: IEA.
+
+Liesen, Richard J. 1997. \emph{Atmospheric Pollution Prediction in a Building Energy Simulation Program}, April 1997, BLAST Support Office, Department of Mechanical Engineering. Champaign, Illinois: University of Illinois.
+
+Stroot, Peter J., Robert J. Nemeth, \& Donald F. Fournier.~ 1996.~ \emph{Pollution Reduction Through Energy Conservation, REEP Model}.~ Champaign, Illinois: U S Army Construction Engineering Research Laboratory.
+
+Torcellini Paul A, Nicholas Long, and Ronald D. Judkoff.~ 2004. ``Consumptive Water Use for U.S. Power Production,'' in \emph{ASHRAE Transactions,} Volume 110, Part 1. Atlanta, Georgia: ASHRAE.
+
+United Nations Environment Programme.~ 2002.~ \emph{Climate Change Information Kit}.~ Châtelaine, Switzerland: UNEP.
+
+United Nations Framework Convention on Climate Change.~ 1997. \emph{Kyoto} \emph{Protocol to the United Nations Framework Convention on Climate Change.}~ Bonn, Germany: UNFCCC.
+
+U.S. Department of Energy.~ 2004. \emph{Monthly Energy Review}. Washington, DC:~ Energy Information Administration, U S Department of Energy.
+
+U.S. Department of Energy.~ 2002. \emph{Updated State-level Greenhouse Gas Emission Coefficients for Electricity Generation 1998-2000}.~ April 2002, Energy Information Administration, Office of Integrated Analysis and Forecasting, Energy Information Administration.~ Washington, DC: U.S. Department of Energy.
+
+U.S. Environmental Protection Agency.~ 2003a. \emph{eGRID Emissions and Generation Resource Integrated Database}, May 2003, Washington, DC:~ U.S. Environmental Protection Agency.
+
+U.S. Environmental Protection Agency.~ 2003b. \emph{AirData,} Tier Emissions Report - Criteria Air Pollutants, 1999 data, May 2003. Washington, DC:~ U.S. Environmental Protection Agency.
+
+U.S. Environmental Protection Agency.~ 1998a. \emph{Compilation of Air Pollutant Emission Factors, AP-42, Fifth Edition, Volume I: Stationary Point and Area Sources}, Chapter 1 External Combustion Sources, Supplement D, July 1998. Research Triangle Park, North Carolina: U. S. Environmental Protection Agency.
+
+U.S. Environmental Protection Agency.~ 1998b. \emph{Compilation of Air Pollutant Emission Factors, AP-42, Fifth Edition, Volume I: Stationary Point and Area Sources,} Chapter 1 External Combustion Sources, Supplement E, September 1998. Research Triangle Park, North Carolina: U. S. Environmental Protection Agency.
+
+U.S. Environmental Protection Agency.~ 1996. \emph{Compilation of Air Pollutant Emission Factors, AP-42, Fifth Edition, Volume I: Stationary Point and Area Sources,} Chapter 1 External Combustion Sources, Supplement B, October 1996. Research Triangle Park, North Carolina: U. S. Environmental Protection Agency.
diff --git a/doc/engineering-reference/src/special-modules-reporting/output-table-annual.tex b/doc/engineering-reference/src/special-modules-reporting/output-table-annual.tex
new file mode 100644
index 00000000000..a0e2b739f9a
--- /dev/null
+++ b/doc/engineering-reference/src/special-modules-reporting/output-table-annual.tex
@@ -0,0 +1,3 @@
+\section{Output:Table:Annual}\label{outputtableannual}
+
+No special algorithms were employed to implement the Output:Table:Annual object.
diff --git a/doc/engineering-reference/src/special-modules-reporting/zone-component-loads-summary.tex b/doc/engineering-reference/src/special-modules-reporting/zone-component-loads-summary.tex
new file mode 100644
index 00000000000..f7d9e252062
--- /dev/null
+++ b/doc/engineering-reference/src/special-modules-reporting/zone-component-loads-summary.tex
@@ -0,0 +1,216 @@
+\section{Zone Component Loads Summary}\label{zone-component-loads-summary}
+
+Many building energy simulation programs provide reports that breakdown the design load into component contributions from~ walls, roofs, floors, underground walls, windows, interior walls, infiltration, ventilation, occupancy, lighting, refrigeration cases, and internal equipment. Some of these components have both sensible and latent subcomponents. It is important to understand the difference between gains and loads. ASHRAE Handbook of Fundamentals 2009 describes the space heat gain as ``.. the rate at which heat enters into and/or is generated within a space'' while the space cooling load is ``the rate at which sensible and latent heat must be removed fro the space to maintain a constant space air temperature and humidity.''~ The difference is that the radiant heat gains which is ``absorbed by walls, floors, furniture, etc., contributed to the space cooling load only after a time lag.''
+
+The heat balance algorithms used by~ EnergyPlus result in a single combined design load for a given zone and some, but not all, of the zone instantaneous heat gains. This section describes the estimation procedure for the Zone Component Loads Summary report that shows an estimated breakdown of load components from each type of of heat gain for each zone.
+
+The Estimated Cooling Peak Load Components and Estimated Heating Peak Load Components subtables of the Zone Component Loads Summary report contain values that are estimated and are not part of the normal heat balance algorithms used in the rest of EnergyPlus.~ In particular, the column described as Sensible-Delayed represents an estimate of the sensible load contributed at the peak time based on radiant contributions from various load components that have radiant portions in previous timesteps. The focus of this section will be on the Sensible-Delayed column.
+
+The columns labeled Sensible-Instant, Sensible-Return Air, and Latent are directly computed for people, lights, equipment, refrigeration, water use equipment,~ HVAC equipment losses, power generation equipment, infiltration, zone ventilation and interzone mixing. For example, Lights objects have inputs for the fractions of the gains that are to return air, radiant, visible and the remainder is convected.~ In this case, the fraction to return air is reported in the Sensible Return Air column and the fraction that is convected is reported in the Sensible-Instant column.
+
+At the time of the peak load, each surface in the zone is contributing a convective heat loss or heat gain depending on the inside surface temperature.
+
+The radiant portion of the internal heat gains from lighting, equipment, and incident solar are radiantly transmitted to the surfaces of the zone. The heat from these radiant gains is stored in the surfaces and retransmitted back into the zone over time as convective gains to the zone. By the time the heat is retransmitted, it is impossible to know the contribution of each possible radiant gain from past time steps on that surface into the convective gain for that timestep. The temperature change of the surface includes the impact of all of these radiant gains as well as any heat transfer through the surface.
+
+To disaggregate the delayed affect of zone radiant (delayed) portions of the peak load, a pulse of radiant internal loads is used to determine custom radiant to convective decay curves for heating and cooling, essentially replicating part of the method used for Radiant Time Series (see Chapter 18 of ASHRAE Handbook of Fundamentals 2009) to isolate the delayed impacts of internal loads. This is performed during the zone sizing routines.
+
+The response of each surface to a pulse of radiant heat is used to estimate the peak load components for solar gains and the radiant portion of internal gains. Subtracting these for each surface then leaves the peak load component from conduction through the surfaces. The approach is described in more detail below:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  When zone sizing is performed for cooling or heating, the heat convected from each opaque surface for each timestep during sizing day is saved to an array.
+\item
+  For each type of internal gain, HVAC equipment gain, and solar energy entering the zone, the radiant and convective portions are saved for every timestep during sizing. In addition, for each type of radiant gain, the amount that lands on each surface in the zone is saved for evergy timestep during sizing.
+\item
+  An additional ``pulse sizing'' run is performed for cooling and heating during zone sizing that includes an additional small, single timestep, pulse of radiant-only heat for each zone but is otherwise the same as a normal zone sizing simulation. This is equivalent to adding an ElectricEquipment object that is scheduled for a single timestep and is 100\% radiant heat. The heat convected from each opaque surface for each timestep during sizing is saved to an array. This run is not used for sizing, but just to gather the impact of the pulse of radiant heat.
+\item
+  For each surface, a ``decay curve'' is developed by subtracting the results from the normal sizing (1) from the ``pulse'' sizing run (3). This represents the delay in converting incoming radiant heat into convected heat for each surface in the zone. The graphs below show the decay curves for an exterior wall (RIGHT-1) and an interior wall (SB23) for a test file.
+\end{enumerate}
+
+\begin{figure}[hbtp] % fig 343
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7912.png}
+\caption{Load Component - Decay Curve of Exterior Wall \protect \label{fig:load-component-decay-curve-of-exterior-wall}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 344
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image7913.png}
+\caption{Load Component - Decay Curve of Interior Wall \protect \label{fig:load-component-decay-curve-of-interior-wall}}
+\end{figure}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{4}
+\item
+  Using the internal and solar gain results saved from the normal sizing period in step (2), for each timestep prior to and including the time of the peak load during the sizing day, the decay curve is applied to each radiant gain on each surface for each timestep to generate a predicted delayed load component for the internal and solar gains for each timestep that comprise the peak load (based on Timesteps in Averaging Window). Timesteps just before the peak have much larger impacts than those just a few timesteps before the peak.~ These results will be the radiant portion of the load for each type of internal and solar gain.
+\item
+  The difference between the sum of the predicted convective loads from internal and solar gains from step (5) and the total convective loads for that surface for the timesteps that comprise the peak load from step (1) is assumed to be the load from heat transfer through that surface.~ This is essentially subtracting out the radiant portions of the internal and solar gains on each surface for the sizing day.
+\end{enumerate}
+
+\subsection{Estimated Component Load Details}\label{estimated-component-load-details}
+
+In HeatBalanceInternalHeatGains, in the InitInternalHeatGains routine, the single timestep pulse is added to the thermal radiation absorbed on the inside surface. It is based on 0.01 W per square meter of the zone area. The time of the pulse and the amount received by each surface is also saved. A new routine GatherComponentLoadsIntGain was also added to that file that gathers the instantenous heat gains from people, lights, equipment, refrigeration equipment, water use, hvac losses, and power generation. Latent gains from people and refrigeration are also gathered along with the radiant portion of the gains from these same sources. EnergyPlus tracks internal gains by type, and these are grouped as follows for the rows of the report:
+
+The gains from ``People'' contain:
+
+\begin{itemize}
+\tightlist
+\item
+  IntGainTypeOf\_People
+\end{itemize}
+
+The gains from ``Lights'' contain:
+
+\begin{itemize}
+\tightlist
+\item
+  IntGainTypeOf\_Lights
+\end{itemize}
+
+The gains from ``Equipment'' contain:
+
+\begin{itemize}
+\item
+  IntGainTypeOf\_ElectricEquipment
+\item
+  IntGainTypeOf\_GasEquipment
+\item
+  IntGainTypeOf\_HotWaterEquipment
+\item
+  IntGainTypeOf\_SteamEquipment
+\item
+  IntGainTypeOf\_OtherEquipment
+\end{itemize}
+
+The gains from ``Refrigeration'' contain:
+
+\begin{itemize}
+\item
+  IntGainTypeOf\_RefrigerationCase
+\item
+  IntGainTypeOf\_RefrigerationCompressorRack
+\item
+  IntGainTypeOf\_RefrigerationSystemAirCooledCondenser
+\item
+  IntGainTypeOf\_RefrigerationSystemSuctionPipe
+\item
+  IntGainTypeOf\_RefrigerationSecondaryReceiver
+\item
+  IntGainTypeOf\_RefrigerationSecondaryPipe
+\item
+  IntGainTypeOf\_RefrigerationWalkIn
+\end{itemize}
+
+The gains from ``Water Use Equipment'' contain:
+
+\begin{itemize}
+\item
+  IntGainTypeOf\_WaterUseEquipment
+\item
+  IntGainTypeOf\_WaterHeaterMixed
+\item
+  IntGainTypeOf\_WaterHeaterStratified
+\end{itemize}
+
+The gains from ``HVAC Equipment Losses'' which are gains to the zone due to the location of the equipment within the zone include:
+
+\begin{itemize}
+\item
+  IntGainTypeOf\_ZoneBaseboardOutdoorTemperatureControlled
+\item
+  IntGainTypeOf\_ThermalStorageChilledWaterMixed
+\item
+  IntGainTypeOf\_ThermalStorageChilledWaterStratified
+\item
+  IntGainTypeOf\_PipeIndoor
+\item
+  IntGainTypeOf\_Pump\_VarSpeed
+\item
+  IntGainTypeOf\_Pump\_ConSpeed
+\item
+  IntGainTypeOf\_Pump\_Cond
+\item
+  IntGainTypeOf\_PumpBank\_VarSpeed
+\item
+  IntGainTypeOf\_PumpBank\_ConSpeed
+\item
+  IntGainTypeOf\_PlantComponentUserDefined
+\item
+  IntGainTypeOf\_CoilUserDefined
+\item
+  IntGainTypeOf\_ZoneHVACForcedAirUserDefined
+\item
+  IntGainTypeOf\_AirTerminalUserDefined
+\end{itemize}
+
+The gains from ``Power Generation Equipment'' include:
+
+\begin{itemize}
+\item
+  IntGainTypeOf\_GeneratorFuelCell
+\item
+  IntGainTypeOf\_GeneratorMicroCHP
+\item
+  IntGainTypeOf\_ElectricLoadCenterTransformer
+\item
+  IntGainTypeOf\_ElectricLoadCenterInverterSimple
+\item
+  IntGainTypeOf\_ElectricLoadCenterInverterFunctionOfPower
+\item
+  IntGainTypeOf\_ElectricLoadCenterInverterLookUpTable
+\item
+  IntGainTypeOf\_ElectricLoadCenterStorageBattery
+\end{itemize}
+
+The ReportSurfaceHeatBalance routine in the HeatBalanceSurfaceManger module gathers the shortwave radiant heat gain from lighting and fenestration solar gains on each surface. In the same module, the CalcHeatBalanceInsideSurf routine gathers the surface by surface convection for both the normal and pulse zone sizing times along with the net radiation on the surface during the normal zone sizing times. In addition, a routine called GatherComponentLoadSurfAbsFact gathers the factors used in distributing the radiant heat from a zone to each surface (TMULT and ITABSF).
+
+The SizingManager module repeats the zone sizing portion of the procedure when this report is requested.~ The pulse occurs at 10am during the zone sizing simulations. The 10am time was chosen after some testing that looked at pulses at different times of the day. It is ~important that the pulse occurs while the system is running and stable not during start up hours. In addition, the plus timing needs to be early enough that the duration of the resulting decay curve can be appropriate applied to as many timesteps as possible during the peak day.
+
+The following subroutines in the OutputReportTabular module produce the report:
+
+\begin{itemize}
+\item
+  ComputeLoadComponentDecayCurve
+\item
+  GatherComponentLoadsSurface
+\item
+  GatherComonentLoadsHVAC
+\item
+  ComputeDelayedComponents
+\item
+  WriteZoneLoadComponentTable
+\end{itemize}
+
+The ComputeLoadComponentDecayCurve routine determines the heating and cooling decay curves using the following (for cooling but repeated also for heating):
+
+\begin{lstlisting}
+  TimeOfPulse = radiantPulseTimestep(ZoneNum,CoolDesSelected)
+  DO TimeStep = TimeOfPulse, NumOfTimeStepInHour* 24
+    IF (radiantPulseReceived(surfNum,CoolDesSelected) .NE. 0.0) THEN
+      diff = loadConvectedWithPulse(surfNum,TimeStep,CoolDesSelected)
+           - loadConvectedNormal(surfNum,TimeStep,CoolDesSelected)
+      decayCurveCool(surfNum, TimeStep - TimeOfPulse + 1) = -diff /
+          radiantPulseReceived(surfNum,CoolDesSelected)
+    ELSE
+      decayCurveCool(surfNum, TimeStep - TimeOfPulse + 1) = 0.0
+    END IF
+  END DO
+\end{lstlisting}
+
+The ComputeDelayedComponents routine applies the decay curve to the load components. It does the following for the heating and cooling sizing period that was selected and for each zone and each surface in the zone
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Determine the heat gain on the surface of people, equipment, hvac losses, power generation and long wave light radiation.
+\item
+  For each time step backwards from the current timestep, estimate the delayed convected heat from people, equipment, HVAC losses, power generation, lighting long wave radiation, lighting short wave radiation, and fenestration solar by multiplying the decay curve with the value determined from (a).
+\item
+  Accumulate the values on a zone basis
+\item
+  Determine the remaining convective heat from surfaces that are not from these gains and remove the net surface radiation (output variable Surface Inside Face Convection Heat Gain Rate)
+\item
+  Store the estimated values in a sequence to be later averaged over the averaging window.
+\end{enumerate}
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes.tex
new file mode 100644
index 00000000000..64161a0fa1c
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes.tex
@@ -0,0 +1 @@
+\chapter{Surface Heat Balance Manager / Processes}\label{surface-heat-balance-manager-processes}
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/adiabatic-boundary-conditions.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/adiabatic-boundary-conditions.tex
new file mode 100644
index 00000000000..98e4a67412e
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/adiabatic-boundary-conditions.tex
@@ -0,0 +1,9 @@
+\section{Adiabatic Boundary Conditions}\label{adiabatic-boundary-conditions}
+
+Adiabatic boundary conditions are applied to two surface types in EnergyPlus:
+
+1)~~~Surfaces with adiabatic outside boundary conditions
+
+2)~~~Internal Mass objects
+
+For both surface types, EnergyPlus will apply the same boundary conditions to each side of the construction so that there is no temperature difference across the surface. In this case, all heat transfer into the surface is a result of the dynamic response of the construction to varying inside boundary conditions. The surface will store and release heat only at the inside face of the surface (it is assumed that the outside face is not within the zone). If both faces are within the zone, this situation can be modeled either by creating another adiabatic or internal mass surface with the reverse construction, or, for symmetric constructions, simply doubling the area of the surface.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/combined-heat-and-moisture-transfer-hamt.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/combined-heat-and-moisture-transfer-hamt.tex
new file mode 100644
index 00000000000..3c1a4f05914
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/combined-heat-and-moisture-transfer-hamt.tex
@@ -0,0 +1,192 @@
+\section{Combined Heat and Moisture Transfer (HAMT) Model}\label{combined-heat-and-moisture-transfer-hamt-model}
+
+\subsection{Overview}\label{overview-011}
+
+The combined heat and moisture transfer finite (HAMT) solution algorithm is a completely coupled, one-dimensional, finite element, heat and moisture transfer model simulating the movement and storage of heat and moisture in surfaces simultaneously from and to both the internal and external environments. As well as simulating the effects of moisture buffering, HAMT is also be able to provide temperature and moisture profiles through composite building walls, and help to identify surfaces with high surface humidity.
+
+\subsection{HAMT Nomenclature}\label{hamt-nomenclature}
+
+Dependencies on moisture content are indicated by a superscript \(^{w}\), on heat by a superscript \(^{h}\) and vapor pressure by a superscript \(^{v}\).
+
+\begin{longtable}[c]{p{1.5in}p{1.0in}p{3.5in}}
+\caption{Combined Heat and Moisture Transfer Model Nomenclature \label{table:combined-heat-and-moisture-transfer-model}} \tabularnewline
+\toprule 
+Symbol & Units & Meaning \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Combined Heat and Moisture Transfer Model Nomenclature} \tabularnewline
+\toprule 
+Symbol & Units & Meaning \tabularnewline
+\midrule
+\endhead
+
+T & °C & Temperature \tabularnewline
+RH,$\varphi$ & \%, fraction & Relative humidity \tabularnewline
+W & $kg/m^3$ & Moisture Content \tabularnewline
+$\partial{H}/\partial{T}$ & $J/m^3C$ & Moisture dependent heat storage capacity \tabularnewline
+$\partial{w}/\partial{\phi}$ & $kg/m^3$ & Moisture dependent moisture storage capacity \tabularnewline
+${k^w}$ & W/mC & Moisture dependent thermal conductivity \tabularnewline
+${h_v}$ & J/kg & Evaporation enthalpy of water (= 2,489,000~J/kg) \tabularnewline
+$\delta$ & kg/msPa & Vapor diffusion coefficient in air \tabularnewline
+$\mu$ & --- & Moisture dependent vapor diffusion resistance factor \tabularnewline
+P & Pa & Vapor pressure \tabularnewline
+$p_{\text{ambient}}$ & Pa & Ambient air pressure \tabularnewline
+C & J/kgC & Specific heat capacity of dry material \tabularnewline
+$c_{w}$ & J/KgC & Specific heat capacity of water (= 4,180~J/kg$^{o}$C@ 20$^{o}$C) \tabularnewline
+$\rho$ & $kg/m^3$ & Material Density \tabularnewline
+${\rho ^w}$ & $kg/m^3$ & Density of water (= 1,000$kg/m^3$) \tabularnewline
+${D^w}$ & $m^2/s$ & Liquid Transport Coefficient \tabularnewline
+A & $m^2$ & Contact Surface area \tabularnewline
+$\Delta {V_i}$ & $m^3$ & Cell Volume \tabularnewline
+$t$ & s & Time \tabularnewline
+$\Delta \tau$ & s & Time step between calculations \tabularnewline
+x & m & Distance between cell centres \tabularnewline
+$C_i^h$ & J/C & Heat Capacitance of cell i \tabularnewline
+$C_i^w$ & kg & Moisture Capacitance of cell i \tabularnewline
+$R_{ij}^h$ & C/W & Heat Resistance between cells i and j \tabularnewline
+$R_{ij}^v$ & sPa/kg & Vapor Resistance between cells i and j \tabularnewline
+$^{R_{ij}^w}$ & s/kg & Liquid Moisture Resistance between cells i and j \tabularnewline
+$^{q_i^v}$ & W & Heat due to Vaporisation \tabularnewline
+$^{q_i^{adds}}$ & W & Heat from additional Sources \tabularnewline
+P & m3/m3 & Material Porosity \tabularnewline
+p(as a superscript) & s & Present Time Step \tabularnewline
+i,j & --- & Cell indices \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{HAMT Model Description}\label{hamt-model-description}
+
+Equations and are derived from heat and moisture balance equations and are taken from {[}Künzel, H.M. (1995){]}. They describe a theoretical model for the transfer of heat and moisture through a material.
+
+\begin{equation}
+\frac{{\partial H}}{{\partial T}}\frac{{\partial T}}{{\partial \tau }} = \frac{\partial }{{\partial x}}\left( {{k^w}\frac{{\partial T}}{{\partial x}}} \right) + {h_v}\frac{\partial }{{\partial x}}\left( {\frac{\delta }{\mu }\frac{{\partial T}}{{\partial x}}} \right)
+\end{equation}
+
+The three terms in equation describe the storage, transport and generation of heat respectively.
+
+\begin{equation}
+\frac{{\partial w}}{{\partial \phi }}\frac{{\partial \phi }}{{\partial \tau }} = \frac{\partial }{{\partial x}}\left( {{D^w}\frac{{\partial w}}{{\partial \phi }}\frac{{\partial \phi }}{{\partial x}}} \right) + \frac{\partial }{{\partial x}}\left( {\frac{\delta }{\mu }\frac{{\partial T}}{{\partial x}}} \right)
+\end{equation}
+
+The three terms in equation describe the storage of moisture, the transport of liquid moisture and the transport of vapor respectively. The equation to calculate the vapor diffusion coefficient in air (\(\delta\)) used in the third term of both equations, is also taken from Künzel,
+
+\begin{equation}
+\delta  = \frac{{\left( {2 \times {{10}^{ - 7}} \times {{\left( {T + 273.15} \right)}^{0.81}}} \right)}}{{{P_{ambient}}}}
+\end{equation}
+
+The heat storage capacity (\(\frac{\partial H}{\partial T}\)) depends on the moisture content w of the material by the following equation.
+
+\begin{equation}
+\frac{{\partial H}}{{\partial T}} = \left( {c\rho  + {c^w}w} \right)
+\end{equation}
+
+The moisture content of the material w and the vapor diffusion resistance factor $\mu$ depend on the relative humidity inside the material. The parameters \(\frac{\partial w}{\partial \phi}\), \({k^w}\) ~and \({D^w}\) are also moisture dependent parameters.
+
+The following sections describe how the above equations are used within the HAMT model.
+
+\subsubsection{Surfaces, Material Layers and Cells}\label{surfaces-material-layers-and-cells}
+
+``Surfaces'' are made of a number of layers of potentially any combination of materials. Each surface is split into its constituent materials and is then split up further into cells through its depth. HAMT will generate no more than 10 cells per material with widths that are thinner near the boundaries of each material where most changes are expected and detail is needed.
+
+\subsubsection{Heat Transfer}\label{heat-transfer}
+
+Equation 1 can be re-written and used to describe the heat storage and transfer through the i\(^{th}\) cell in a surface.
+
+\begin{equation}
+\left( {{c_i}{\rho_i} + {c^w}{w_i}} \right)\Delta {V_i}\frac{{T_i^{p + 1} - T_i^p}}{{\Delta \tau }} = \sum\limits_j {k_{ij}^w{A_{ij}}\frac{{T_j^{p + 1} - T_i^{p + 1}}}{{{x_{ij}}}}}  + \sum\limits_j {{h_v}\frac{{{\delta_{ij}}}}{{{\mu_{ij}}}}{A_{ij}}\frac{{p_j^{p + 1} - p_i^{p + 1}}}{{{x_{ij}}}}}
+\end{equation}
+
+In the one dimensional case there are only two adjacent cells each labelled j. The heat generated due to vaporization \(q_i^v\) can be calculated separately.
+
+\begin{equation}
+q_i^v = \sum\limits_j {{h_v}\frac{{{\delta_{ij}}}}{{{\mu_{ij}}}}{A_{ij}}\frac{{p_j^{p + 1} - p_i^{p + 1}}}{{{x_{ij}}}}}
+\end{equation}
+
+Rearranging equation and including other sources of heat (\(q_i^{adds}\)) such as radiation from other surfaces in the calculation gives the temperature in a cell in the next time step as,
+
+\begin{equation}
+T_i^{p + 1} = \frac{{\sum\nolimits_j {\frac{{T_j^{p + 1}}}{{R_{ij}^h}}}  + q_i^v + q_i^{adds} + C_i^h\frac{{T_i^p}}{{\Delta \tau }}}}{{\frac{{C_i^h}}{{\Delta \tau }} + \sum\nolimits_j {\frac{1}{{R_{ij}^h}}} }}
+\end{equation}
+
+where \(C_i^h = \left( {{c_i}{\rho_i} + {c^w}{w_i}} \right)\Delta {V_i}\) is thermal heat capacitance of cell i and \(R_{ij}^h = \frac{x_{ij}}{k_{ij}A_{ij}}\) ~is the thermal resistance between cells i and j.
+
+This equation can be solved using the Gauss-Seidel iteration technique. The i\(^{th}\) cell temperature is calculated whilst the j\(^{th}\) cell temperatures are kept as up to date as possible. The iteration is stopped when the maximum difference between two consecutive calculations in all cells is less than a threshold of 0.002°C.
+
+\subsubsection{Moisture Content w}\label{moisture-content-w}
+
+The moisture content (w) of a cell is needed for the calculation of the heat transfer through the cell as it affects the thermal resistance and heat capacitance. The moisture content of cells is calculated from the relative humidity (RH) of the material. The relationship between w and the RH for each material is known as the sorption isotherm and measured data points are entered into EnergyPlus as a series of coordinates. HAMT interpolates between the measurements to obtain the moisture content of a material for any RH value. The sorption isotherm input is via the MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm object and is described in the Input Output Reference document.
+
+\subsubsection{Porosity P}\label{porosity-p}
+
+The porosity of a material (P) is an input variable and defined as the maximum fraction, by volume, of a material that can be taken up with moisture. It is used to calculate the maximum point on the sorption isotherm curve. ~The porosity is entered for each material via the MaterialProperty:HeatAndMoistureTransfer:Settings object, as described in the Input Output Reference document.
+
+\subsubsection{\texorpdfstring{Moisture Dependant Thermal Conductivity k\(^{w}\)}{Moisture Dependant Thermal Conductivity k\^{}\{w\}}}\label{moisture-dependant-thermal-conductivity-kw}
+
+The thermal conductivity (k\(^{w}\)) of the cell is determined by interpolating between data points of thermal conductivity versus the moisture content of the material, entered into EnergyPlus via the MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity object. The moisture content is determined via the sorption isotherm which gives the moisture content as a function of Relative Humidity.
+
+\subsubsection{Moisture Dependant Moisture Diffusion Coefficient μ}\label{moisture-dependant-moisture-diffusion-coefficient-ux3bc}
+
+This is used in the third term of equation to describe the heat transfer due to vapor movement. It is determined by interpolating between data points of moisture diffusion coefficient versus the moisture content of the material, entered into EnergyPlus via the MaterialProperty:HeatAndMoistureTransfer:Diffusion object. A simple linear interpolation is used to obtain the conductivity between measured points.
+
+\subsubsection{Moisture Transfer}\label{moisture-transfer}
+
+Moisture, as well as heat, is transported through materials as either liquid (w) or vapor (p). There are two different potentials that control the movement though the material. Liquid transfer is driven by differences in relative humidity whereas vapor transfer is driven by differences in vapor pressure. Materials also have a capacity to store moisture. Equation can be re-written for a discrete cell in a continuous material.
+
+\begin{equation}
+\frac{{dw}}{{d{\phi_i}}}\Delta {V_i}\frac{{\phi_i^{p + 1} - \phi_i^p}}{{\Delta \tau }} = \sum\limits_j {{k_{ij}}{A_{ij}}\frac{{\phi_j^{p + 1} - \phi_i^{p + 1}}}{{{x_{ij}}}}}  + \sum\limits_j {\frac{{{\delta_{ij}}}}{{{\mu_{ij}}}}{A_{ij}}\frac{{p_j^{p + 1} - p_i^{p + 1}}}{{{x_{ij}}}}}
+\end{equation}
+
+Equation can be rearranged to provide the relative humidity of the i\(^{th}\) cell in the next time step.
+
+\begin{equation}
+\phi_i^{p + 1} = \frac{{\sum\nolimits_j {\frac{{\phi_j^{p + 1}}}{{R_{ij}^w}}}  + \sum\nolimits_j {\frac{{p_i^{p + 1}}}{{R_{ij}^v}}}  + C_i^w\frac{{\phi_i^p}}{{\Delta \tau }}}}{{\frac{{C_i^w}}{{\Delta \tau }} + \sum\nolimits_j {\frac{1}{{R_{ij}^w}} + \sum\nolimits_j {\frac{{p_i^{sat}}}{{R_{ij}^v}}} } }}
+\end{equation}
+
+where \(C_i^w = \frac{dw}{d\phi_{i}}\Delta {V_i}\) ~is the ``Moisture Capacitance'' of cell i,
+
+\begin{equation}
+R_{ij}^w = \frac{{{x_{ij}}}}{{{A_{ij}}D_{ij}^w\frac{{dw}}{{d\phi }}}}
+\end{equation}
+
+is the moisture resistance between cells i and j and \(R_{ij}^v = \frac{\mu_{ij}x_{ij}}{A_{ij}\delta_{ij}}\) ~is the vapor resistance~between cells i and j.
+
+Equation can be used together with the heat equation in an alternate step by step fashion to calculate the new temperature and relative humidity profiles for each cell for the next time step.
+
+\subsubsection{\texorpdfstring{Liquid Transport Coefficient D\(^{w}\)}{Liquid Transport Coefficient D\^{}\{w\}}}\label{liquid-transport-coefficient-dw}
+
+The Moisture Dependant Liquid Transport Coefficient is entered as a series of moisture density and liquid transport coefficient data points. There are two different coefficients, one for suction, where the surface is wet due to rain, and one for redistribution where the surface is no longer wet. If the weather file has a rain flag it is used to switch between these two types of coefficient. HAMT-SUCTION and HAMT-REDISTRIBUTION.
+
+\subsubsection{\texorpdfstring{Moisture Dependent Moisture Capacity \(\frac{\partial w}{\partial \phi}\)}{Moisture Dependent Moisture Capacity \textbackslash{}frac\{\textbackslash{}partial w\}\{\textbackslash{}partial \textbackslash{}phi\}}}\label{moisture-dependent-moisture-capacity-fracpartial-wpartial-phi}
+
+This is simply the gradient of moisture sorption isotherm at the RH of the material.
+
+\subsubsection{Convective Heat Transfer}\label{convective-heat-transfer}
+
+The internal and external heat transfer coefficients are used to calculate the thermal resistance of the boundary layer between the zone air and the surface of the surface. They are either supplied by the user via the advanced surface concepts object ``SurfaceProperty:ConvectionCoefficients'' or, if these are not provided, dynamic values are calculated.
+
+\subsubsection{Convective Vapor Transfer}\label{convective-vapor-transfer}
+
+The internal and external vapor transfer coefficients are used to calculate the resistance to vapour transfer of the boundary layer between the zone air and the surface of the surface. They are also either supplied by the user via the advanced surface concept object SurfaceProperties:VaporCoefficients. If these are not provided then dynamic values are calculated based on the convective heat transfer coefficients.
+
+\subsubsection{Initial Moisture Content}\label{initial-moisture-content}
+
+At the start of an EnergyPlus simulation ``warm up'' days are used to ensure that the temperatures of surfaces come to equilibrium with the environment before the simulation starts proper. Moisture content within some building fabrics can take a very long time to come to equilibrium with its environment and it is therefore necessary to set initial or typical values of moisture content for each material to be used at the start of the simulation. These initial values are entered for each material via the MaterialProperty:HeatAndMoistureTransfer:Settings object as described in the Input Output Reference document.
+
+\subsubsection{Using the Model}\label{using-the-model}
+
+As an illustration of the use of the Heat and Moisture Transfer (HAMT) model, the material properties for a small sample of six generic materials have been provided in the EnergyPlus Reference DataSets (MoistureMaterials.idf). The properties were synthesised from the Annex 24 database {[}Kumar Kumaran, M. (1996){]}, supplemented, when required, by data from the database of the WUFI model {[}WUFI (1999){]} and are therefore not related to any unique, measured material. Users should consult material property catalogues and other primary sources when the properties of a specific material are required.
+
+Moisture and heat from the surfaces are used by EnergyPlus to calculate the room air temperature and moisture content. EnergyPlus with HAMT works best with as short a time step as possible. However the optimum time step which gives a good prediction for a short computing time will very much depend on the nature of the weather and type of building. Buildings with frequent and large changes in internal and external temperature will need a small time step, maybe even 60 steps per hour. Slowly evolving temperatures and relative humidity's will not require such a short time step and 20, or even 6, steps per hour may be sufficient.
+
+\subsection{References}\label{references-012}
+
+Künzel, H.M. (1995) Simultaneous Heat and Moisture Transport in Building Components. One- and two-dimensional calculation using simple parameters. IRB Verlag 1995
+
+Holman, J.P. (2002) Heat Transfer, Ninth Edition. McGraw-Hill
+
+Winterton, R.H.S. (1997) Heat Transfer. (Oxford Chemistry Primers; 50) Oxford University Press
+
+Kumar Kumaran, M. (1996) IEA ANNEX 24, Final Report, Volume 3
+
+WUFI (1999) version 2.2 Simultaneous Heat and Moisture Transport in Building components. Fraunhofer IBP, Holzkirchen, Germany
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/conduction-finite-difference-solution.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/conduction-finite-difference-solution.tex
new file mode 100644
index 00000000000..fc3848ad29c
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/conduction-finite-difference-solution.tex
@@ -0,0 +1,195 @@
+\section{Conduction Finite Difference Solution Algorithm}\label{conduction-finite-difference-solution-algorithm}
+
+\subsection{Basic Finite Difference Solution Approach}\label{basic-finite-difference-solution-approach}
+
+EnergyPlus models follow fundamental heat balance principles very closely in almost all aspects of the program. However, the simulation of building surface constructions has relied on a conduction transfer function (CTF) transformation carried over from BLAST. This has all the usual restrictions of a transformation-based solution: constant properties, fixed values of some parameters, and do not produce results for the interior of the surface. As the energy analysis field moves toward simulating more advanced constructions, such as phase change materials (PCM), it becomes necessary to step back from transformations to more fundamental forms. Accordingly, a conduction finite difference (CondFD) solution algorithm has been incorporated into EnergyPlus. This does not replace the CTF solution algorithm, but complements it for cases where the user needs to simulate phase change materials or variable thermal conductivity. It is also possible to use the finite difference algorithm for zone time steps as short as one minute.
+
+EnergyPlus includes two different options for the specific scheme or formulation used for the finite difference model.~ The first scheme is referred to as Crank-Nicholson and was the formulation used in EnergyPlus prior to version 7.~ As of version 7 a second scheme was added and is referred to as fully implicit.~ The selection between the two can be made by the user with the HeatBalanceSettings:ConductionFiniteDifference input object.~ Once selected, the same scheme is used throughout the simulation.~ Although the two different schemes differ in their fundamental heat transfer equations, they share nearly all the same supporting models for material properties, data storage, solution schemes, and spatial discretization algorithms.
+
+The Crank-Nicholson scheme is semi-implicit and based on an Adams-Moulton solution approach. It is considered second-order in time.~ The algorithm uses an implicit finite difference scheme coupled with an enthalpy-temperature function to account for phase change energy accurately. The implicit formulation for an internal node is shown in the equation below.
+
+\begin{equation}
+C_p \rho \Delta x \frac{T_i^{j+1}-T_i^j}{\Delta t} = 
+     \frac{1}{2}\left(k_W\frac{T_{i+1}^{j+1}-T_{i}^{j+1}}{\Delta x} +
+                      k_E\frac{T_{i-1}^{j+1}-T_{i}^{j+1}}{\Delta x} + 
+                      k_W\frac{T_{i+1}^{j}-T_{i}^{j}}{\Delta x} +
+                      k_E\frac{T_{i-1}^{j}-T_{i}^{j}}{\Delta x}\right)
+\end{equation}
+
+Where:
+
+T = node temperature
+
+Subscripts:
+
+i = node being modeled
+
+i+1 = adjacent node to interior of construction
+
+i-1 = adjacent node to exterior of construction
+
+j+1 = new time step
+
+j = previous time step
+
+$\Delta$t = calculation time step
+
+$\Delta$x = finite difference layer thickness (always less than construction layer thickness)
+
+C\(_{p}\) = specific heat of material
+
+k\(_{w}\) = thermal conductivity for interface between i node and i+1 node
+
+k\(_{E}\) = thermal conductivity for interface between i node and i-1 node
+
+$\rho$ = density of material
+
+Then, this equation is accompanied by a second equation that relates enthalpy and temperature.
+
+\begin{equation}
+{h_i} = HTF\left( {{T_i}} \right)
+\end{equation}
+
+where HTF is an enthalpy-temperature function that uses user input data.
+
+The fully implicit scheme is also based on an Adams-Moulton solution approach. It is considered first order in time.~ The model equation for this scheme is show in the following equation.
+
+\begin{equation}
+{C_p}\rho {\rm{\Delta x}}\frac{{T_i^{j + 1} - T_i^j}}{{{\rm{\Delta }}t}} = \left( {{k_W}\frac{{\left( {T_{i + 1}^{j + 1} - T_i^{j + 1}} \right)}}{{{\rm{\Delta x}}}} + {k_E}\frac{{\left( {T_{i - 1}^{j + 1} - T_i^{j + 1}} \right)}}{{{\rm{\Delta x}}}}} \right)
+\end{equation}
+
+For both schemes, EnergyPlus uses the following four types of nodes, as shown in the figure below (1) interior surface nodes, (2) interior nodes, (3) material interface nodes and (4) external surface nodes. The grid for each material is established by specifying a half node for each edge of a material and equal size nodes for the rest of the material. Equations such as are formed for all nodes in a construction. The formulation of all node types is basically the same.
+
+\begin{figure}[hbtp] % fig 15
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image176.png}
+\caption{Node depiction for Conduction Finite Difference Model \protect \label{fig:node-depiction-for-conduction-finite}}
+\end{figure}
+
+In the CondFD model, surface discretization depends on the thermal diffusivity of the material ($\alpha$) and time step ($\Delta$t) selected, as shown in the equation below. The default value of 3 for the space discretization constant, \emph{C}, is basically the inverse of the Fourier Number:
+
+\begin{equation}
+Fo = \frac{\alpha \Delta t}{\Delta x^2}
+\end{equation}
+
+and is based on the stability requirement for the explicit mode that requires values higher than 2, or a Fourier number lower than 0.5. However, CondFD uses implicit schemes that do not have the same stability requirements as the explicit mode. Thus, the default 3 was originally set rather arbitrary.~ As of version 7, the value of this constant can be controlled by the user with the input field called Space Discretization Constant in the HeatBalanceSettings:ConductionFiniteDifference input object.~~ The discretization method allows CondFD to assign different node spacing or grid size to different material layers in a wall or roof, as building walls and roofs typically consist of several layers of different materials having different thermal properties.
+
+\begin{equation}
+{\rm{\Delta x}} = \sqrt {{\rm{C\alpha \Delta t}}}
+\end{equation}
+
+The actual integer number of nodes for each layer is then calculated by rounding off the result from dividing the length of the material layer by the result of the equation above. After this, Δx is recalculated by dividing the length of the material by the number of nodes. A full node is equal to two half nodes. Lower values for the Space Discretization Constant yield more nodes, with higher values yield fewer nodes.
+
+Because the solution is implicit, a Gauss-Seidell iteration scheme is used to update to the new node temperatures in the construction and under-relaxation is used for increased stability.~ The Gauss-Seidell iteration loop is the inner-most solver and is called for each surface.~ It is limited to 30 iterations but will exit early when the sum of all the node temperatures changes between the last call and the current call, normalized by the sum of the temperature values, is below ~0.000001C. This convergence criteria is typically met after 3 iterations, except when PCMs are simulated as it takes an average of 2-3 more iterations when PCM are changing phase. If the number if iterations needed to met convergence criteria start to increase, an automatic internal relaxation factor stabilities the solution and in most cases keep the number of iterations less than 10.
+
+EnergyPlus also uses a separate, outer iteration loop across all the different inside surface heat balances so that internal long-wave radiation exchange can be properly solved.~ For CTF formulations, this iteration is controlled by a maximum allowable temperature difference of 0.002C for inside face surface temperatures from one iteration to the next (or a limit of 100 iterations). CondFD uses the same default value for allowable temperature difference as CTF. However, this parameter was found to often need to be smaller for stability and so the inside surface heat balance manager uses a separate allowable maximum temperature difference when modeling CondFD.~ The user can control the value of the relaxation factor by using the input field called~ Inside Face Surface Temperature Convergence Criteria in the HeatBalanceSettings:ConductionFiniteDifference input object. In addition, if the program detects that there is instability by watching for excessive numbers of iterations in this outer loop and may decrease the relaxation factor. Users can also output the number of iterations inside of CondFD loop for each surface and the outer internal heat balance loop for each zone with ``CondFD Inner Solver Loop Iterations'' and ``Heat Balance Inside Surfaces Calculation Iterations'' respectively.
+
+\begin{equation}
+{T_{i,new}} = {T_{i,old}} + \left( {{T_{i,new}} - {T_{i,old}}} \right)*Relax
+\end{equation}
+
+Because of the iteration scheme used for CondFD,~ the node enthalpies get updated each iteration, and then they are used to develop a variable Cp if a phase change material is being simulated. This is done by including a third equation for Cp.
+
+\begin{equation}
+Cp = \frac{{{h_{i,new}} - {h_{i,old}}}}{{{T_{i,new}} - {T_{i,old}}}}
+\end{equation}
+
+The iteration scheme assures that the correct enthalpy, and therefore the correct Cp is used in each time step, and the enthalpy of the material is accounted for accurately. Of course, if the material is regular, the user input constant Cp is used.
+
+The algorithm also has a provision for including a temperature coefficient to modify the thermal conductivity. The thermal conductivity is obtained from:
+
+\begin{equation}
+k = {k_o} + {k_1}\left( {{T_i} - 20} \right)
+\end{equation}
+
+where:
+
+k\(_{o}\) is the 20°C value of thermal conductivity (normal idf~ input)
+
+k\(_{1}\) is the change in conductivity per degree temperature difference from 20°C
+
+As of Version 7, the CondFD implementation was changed to evaluate the thermal conductivity at the interface between nodes, as shown below. In this case, EnergyPlus uses a linear interpolation between nodal points.
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+{C_p}\rho {\rm{\Delta x}}\frac{{T_i^{j + 1} - T_i^j}}{{{\rm{\Delta }}t}} = \frac{1}{2}\left[ {\left( {{k_W}\frac{{\left( {T_{i + 1}^{j + 1} - T_i^{j + 1}} \right)}}{{{\rm{\Delta x}}}} + {k_E}\frac{{\left( {T_{i - 1}^{j + 1} - T_i^{j + 1}} \right)}}{{{\rm{\Delta x}}}}} \right) + \left( {{k_W}\frac{{\left( {T_{i + 1}^j - T_i^j} \right)}}{{{\rm{\Delta x}}}} + {k_E}\frac{{\left( {T_{i - 1}^j - T_i^j} \right)}}{{{\rm{\Delta x}}}}} \right)} \right]
+\end{equation}
+
+Where,
+
+\begin{equation}
+{k_W} = \frac{{\left( {k_{i + 1}^{j + 1} + k_i^{j + 1}} \right)}}{2}
+\end{equation}
+
+\begin{equation}
+{{\rm{k}}_{\rm{E}}} = \frac{{\left( {{\rm{k}}_{{\rm{i}} - 1}^{{\rm{j}} + 1} + {\rm{k}}_{\rm{i}}^{{\rm{j}} + 1}} \right)}}{2}
+\end{equation}
+
+These additional property information values are put into the input file as explained in the Input/Output Reference Document, but it consists simply of a value for k1 and set of enthalpy temperature pairs that describe the enthalpy of the phase change material in straight line segments with respect to temperature.
+
+A graph showing the effect of a large PCM on the outside surface of a zone is shown below. The phase change temperature was 30°C, and the flat temperature response during the phase change is obvious. This example was run with a zone time step of one minute to show that such small time steps can be done with the finite difference solution technique. It is more efficient to set the zone time step shorter than those used for the CTF solution algorithm. It should be set to 20 time steps per hour or greater, and can range up to 60. The finite difference algorithm actually works better with shorter zone time steps. The computation time has a minimum at a zone time step around two minutes (30 time steps/hr), and increases for shorter or longer zone time steps.
+
+\begin{figure}[hbtp] % fig 16
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image185.png}
+\caption{Effects of Large PCM on Outside Zone Surface \protect \label{fig:effects-of-large-pcm-on-outside-zone-surface}}
+\end{figure}
+
+\subsection{Finite Difference Node Arrangement in Surfaces}\label{finite-difference-node-arrangement-in-surfaces}
+
+The Conduction Finite Difference algorithm determines the number of nodes in each layer of the surface based on the Fourier stability criteria.~ The node thicknesses are normally selected so that the time step is near the explicit solution limit in spite of the fact that the solution is implicit. For very thin, high conductivity layers, a minimum of two nodes is used.~ This means two half thickness nodes with the node temperatures representing the inner and outer faces of the layer. All thicker layers also have two half thickness nodes at their inner and outer faces. These nodes produce layer interface temperatures.
+
+The ConductionFiniteDifferenceSimplified capability was removed as of Version 7.2.
+
+\subsection{Conduction Finite Difference Variable Thermal Conductivity}\label{conduction-finite-difference-variable-thermal-conductivity}
+
+The Conduction Finite Difference algorithm has also been given the capability to use an expanded thermal conductivity function. This function, explained in the input/output document, is similar to the temperature enthalpy function. It consists of pairs of temperature and thermal conductivity values that form a linear segmented function. It is established with the MaterialProperty:VariableThermalConductivity object.
+
+\subsection{Conduction Finite Difference Source Sink Layers}\label{conduction-finite-difference-source-sink-layers}
+
+The Conduction Finite Difference algorithm can also invoke the source/sink layer capability by using the \textbf{Construction:InternalSource} object.
+
+\subsection{Conduction Finite Difference Heat Flux Outputs}\label{conduction-finite-difference-heat-flux-outputs}
+
+The Conduction Finite Difference algorithm can output the heat flux at each node and the heat capacitance of each half-node. During the CondFD solution iterations, the heat capacitance of each half node (CondFD Surface Heat Capacitance Node \textless{} n \textgreater{}) is stored:
+
+\begin{equation}
+{HeatCap_{i} = Cp_{i}*\Delta x_{i}*\rho_{i}/2}
+\end{equation}
+
+For nodes which are at the inside or outside face of the surface, there is only one half-node.
+
+After the CondFD node temperatures have been solved for a given timestep, the heat fluxes (CondFD Surface Heat Flux Node \textless{} i \textgreater{} ) are calculated beginning with the inside face of the surface.
+
+\begin{equation}
+{QDreport_{N} = Q_{inside}}
+\end{equation}
+
+for the remaining nodes
+
+\begin{equation}
+\begin{array}{l}
+QDreport_{i} = QDreport_{i+1}+HeatCap1_{i+1}* \frac{\left(T_{i+1,new}-T_{i+1,old}\right)}{\Delta t}-QSource_{i}+HeatCap2_{i} \\
+\quad \quad \quad \quad * \frac{\left(T_{i,new}-T_{i,old}\right)}{\Delta t}
+\end{array}
+\end{equation}
+
+Where:
+
+HeatCap1\(_{i}\) = heat capacitance associated with a given outer half-node HeatCap2\(_{i}\) = heat capacitance associated with a given inner half-node QDreport\(_{i}\) = CondFD Surface Heat Flux Node \textless{} i \textgreater{} QSource\(_{i}\) = internal source heat flux at node i Q\(_{inside}\) = Surface Inside Face Conduction Heat Transfer Rate per Area {[}W/m\(^{2}\){]}
+
+N = total number of nodes in a surface including the surface inside face node. Note that the variable \emph{TotNodes} used in the source code is actually N-1. The surface inside face node is referenced as \emph{TotNodes+1}.
+
+\subsection{References}\label{references-013}
+
+Pedersen C.O., Enthalpy Formulation of conduction heat transfer problems involving latent heat, Simulation, Vol 18, No. 2, February 1972
+
+Versteeg, H. and Malalasekra, W. 1996. An introduction to computational fluid dynamic: the finite volume method approach. Prentice Hall.
+
+\href{../../../Documents\%20and\%20Settings/ptabares/My\%20Documents/Paulo/CV/Tabares\%20Velasco\%20CV\%20UPDATED2.doc}{Tabares-Velasco, P.C. and Griffith, B. 2012. Diagnostic Test Cases for Verifying Surface Heat Transfer Algorithms and Boundary Conditions in Building Energy Simulation Programs, Journal of Building Performance Simulation, doi:10.1080/19401493.2011.595501}
+
+Tabares-Velasco, P.C., Christensen, C. and Bianchi, M. 2012. Verification and Validation of EnergyPlus Phase Change Material Model for Opaque Wall Assemblies, Building and Environment 54: 186-196.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/conduction-through-the-walls.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/conduction-through-the-walls.tex
new file mode 100644
index 00000000000..6b588ed6641
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/conduction-through-the-walls.tex
@@ -0,0 +1,214 @@
+\section{Conduction Through The Walls}\label{conduction-through-the-walls}
+
+\subsection{Conduction Transfer Function Module}\label{conduction-transfer-function-module}
+
+The most basic time series solution is the response factor equation which relates the flux at one surface of an element to an infinite series of temperature histories at both sides as shown by Equation :
+
+\begin{equation}
+{q''_{ko}}(t) = \sum\limits_{j = 0}^\infty  {{X_j}} {T_{o,t - j\delta }} - \sum\limits_{j = 0}^\infty  {{Y_j}} {T_{i,t - j\delta }}
+\end{equation}
+
+where q'' is heat flux, T is temperature, i signifies the inside of the building element, o signifies the outside of the building element, t represents the current time step, and X and Y are the response factors.
+
+While in most cases the terms in the series decay fairly rapidly, the infinite number of terms needed for an exact response factor solution makes it less than desirable.~ Fortunately, the similarity of higher order terms can be used to replace them with flux history terms.~ The new solution contains elements that are called conduction transfer functions (CTFs).~ The basic form of a conduction transfer function solution is shown by the following equation:
+
+\begin{equation}
+{q''_{ki}}(t) =  - {Z_o}{T_{i,t}} - \sum\limits_{j = 1}^{nz} {{Z_j}} {T_{i,t - j\delta }} + {Y_o}{T_{o,t}} + \sum\limits_{j = 1}^{nz} {{Y_j}} {T_{o,t - j\delta }} + \sum\limits_{j = 1}^{nq} {{\Phi_j}{{q''}_{ki,t - j\delta }}}
+\end{equation}
+
+for the inside heat flux, and
+
+\begin{equation}
+{q''_{ko}}(t) =  - {Y_o}{T_{i,t}} - \sum\limits_{j = 1}^{nz} {{Y_j}} {T_{i,t - j\delta }} + {X_o}{T_{o,t}} + \sum\limits_{j = 1}^{nz} {{X_j}} {T_{o,t - j\delta }} + \sum\limits_{j = 1}^{nq} {{\Phi_j}{{q''}_{ko,t - j\delta }}}
+\end{equation}
+
+for the outside heat flux (q'' = q/A)
+
+where:
+
+X\emph{\(_{j}\)} ~ = Outside CTF coefficient, j = 0,1,\ldots{}nz.
+
+Y\emph{\(_{j}\)} = Cross CTF coefficient, j = 0,1,\ldots{}nz.
+
+Z\emph{\(_{j}\)} = Inside CTF coefficient, j = 0,1,\ldots{}nz.
+
+$\Phi$\emph{\(_{j}\)} = Flux CTF coefficient, j = 1,2,\ldots{}nq.
+
+T\emph{\(_{i}\)} = Inside face temperature
+
+T\emph{\(_{o}\)} = Outside face temperature
+
+\({q''_{ko}}\) ~ = Conduction heat flux on outside face
+
+\(q''\) ~ = Conduction heat flux on inside face
+
+The subscript following the comma indicates the time period for the quantity in terms of the time step d.~ Note that the first terms in the series (those with subscript 0) have been separated from the rest in order to facilitate solving for the current temperature in the solution scheme.~ These equations state that the heat flux at either face of the surface of any generic building element is linearly related to the current and some of the previous temperatures at both the interior and exterior surface as well as some of the previous flux values at the interior surface.
+
+The final CTF solution form reveals why it is so elegant and powerful.~ With a single, relatively simple, linear equation with constant coefficients, the conduction heat transfer through an element can be calculated.~ The coefficients (CTFs) in the equation are constants that only need to be determined once for each construction type.~ The only storage of data required are the CTFs themselves and a limited number of temperature and flux terms.~ The formulation is valid for any surface type and does not require the calculation or storage of element interior temperatures.
+
+\subsection{Calculation of Conduction Transfer Functions}\label{calculation-of-conduction-transfer-functions}
+
+The basic method used in EnergyPlus for CTF calculations is known as the state space method (Ceylan and Myers 1980; Seem 1987; Ouyang and Haghighat 1991).~ Another common, older method used Laplace transformations to reach the solution;~ the Laplace method was~ used in BLAST (Hittle, 1979; Hittle \& Bishop, 1983).~ The basic state space system is defined by the following linear matrix equations:
+
+\begin{equation}
+\frac{{d\left[ {\bf{x}} \right]}}{{dt}} = \left[ {\bf{A}} \right]\left[ {\bf{x}} \right] + \left[ {\bf{B}} \right]\left[ {\bf{u}} \right]
+\end{equation}
+
+\begin{equation}
+\left[ {\bf{y}} \right] = \left[ {\bf{C}} \right]\left[ {\bf{x}} \right] + \left[ {\bf{D}} \right]\left[ {\bf{u}} \right]
+\end{equation}
+
+where x is a vector of state variables, u is a vector of inputs, y is the output vector, t is time, and A, B, C, and D are coefficient matrices.~ Through the use of matrix algebra, the vector of state variables (x) can be eliminated from the system of equations, and the output vector (y) can be related directly to the input vector (u) and time histories of the input and output vectors.
+
+This formulation can be used to solve the transient heat conduction equation by enforcing a finite difference grid over the various layers in the building element being analyzed.~ In this case, the state variables are the nodal temperatures, the environmental temperatures (interior and exterior) are the inputs, and the resulting heat fluxes at both surfaces are the outputs.~ Thus, the state space representation with finite difference variables would take the following form:
+
+\begin{equation}
+\frac{d\left[\begin{array}{c}T_1 \\ \vdots \\ T_n\end{array}\right]}{dt} = \left[\bf{A}\right]\left[\begin{array}{c}T_1 \\ \vdots \\ T_n\end{array}\right]+\left[\bf{B}\right]\left[\begin{array}{c}T_i \\ T_o\end{array}\right]
+\end{equation}
+
+\begin{equation}
+\left[\begin{array}{c}{q''}_i \\ {q''}_o\end{array}\right] = \left[\bf{C}\right]\left[\begin{array}{c}T_1 \\ \vdots \\ T_n\end{array}\right]+\left[\bf{D}\right]\left[\begin{array}{c}T_i \\ T_o\end{array}\right]
+\end{equation}
+
+where T1, T2, \ldots{}, Tn-1, Tn~are the finite difference nodal temperatures, n is the number of nodes, Ti~and To~are the interior and exterior environmental temperatures, and q``i~and q''o~are the heat fluxes (desired output).
+
+Seem (1987) shows that for a simple one layer slab with two interior nodes as in Figure~\ref{fig:idealized-variable-volume-system-operation.} and convection at both sides the resulting finite difference equations are given by:
+
+\begin{equation}
+C\frac{{d{T_1}}}{{dt}} = hA\left( {{T_o} - {T_1}} \right) + \frac{{{T_2} - {T_1}}}{R}
+\end{equation}
+
+\begin{equation}
+C\frac{{d{T_2}}}{{dt}} = hA\left( {{T_i} - {T_2}} \right) + \frac{{{T_1} - {T_2}}}{R}
+\end{equation}
+
+\begin{equation}
+q{``_i} = h\left( {{T_i} - {T_2}} \right)
+\end{equation}
+
+\begin{equation}
+q{``_o} = h\left( {{T_1} - {T_o}} \right)
+\end{equation}
+
+where:
+
+\(R = \frac{\ell }{{kA}}\) ,
+
+\(C = \frac{{\rho {c_p}\ell A}}{2}\) , and
+
+A is the area of the surface exposed to the environmental temperatures.
+
+In matrix format:
+
+\begin{equation}
+\left[\begin{array}{c}\frac{dT_1}{dt} \\ \frac{dT_2}{dt}\end{array}\right] = 
+     \left[\begin{array}{cc}-\frac{1}{RC}-\frac{hA}{C} & \frac{1}{RC} \\ \frac{1}{RC} & -\frac{1}{RC}-\frac{hA}{C}\end{array}\right]\left[\begin{array}{c}T_1 \\ T_2\end{array}\right] + 
+     \left[\begin{array}{cc}\frac{hA}{C} & 0 \\ 0 & \frac{hA}{C}\end{array}\right]\left[\begin{array}{c}T_o \\ T_i\end{array}\right]
+\end{equation}
+
+\begin{equation}
+\left[\begin{array}{c}{q''}_o \\ {q''}_i\end{array}\right] = 
+    \left[\begin{array}{cc}0 & -h \\ h & 0\end{array}\right] \left[\begin{array}{c}T_1 \\ T_2\end{array}\right] +
+    \left[\begin{array}{cc}0 & h \\ -h & 0\end{array}\right] \left[\begin{array}{c}T_o \\ T_i\end{array}\right]
+\end{equation}
+
+\begin{figure}[hbtp] % fig 10
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image168.svg.png}
+\caption{Two Node State Space Example. \protect \label{fig:two-node-state-space-example.}}
+\end{figure}
+
+The important aspect of the state space technique is that through the use of matrix algebra the state space variables (nodal temperatures) can be eliminated to arrive at a matrix equation that gives the outputs (heat fluxes) as a function of the inputs (environmental temperatures) only.~ This eliminates the need to solve for roots in the Laplace domain.~ In addition, the resulting matrix form has more physical meaning than complex functions required by the Laplace transform method.
+
+The accuracy of the state space method of calculating CTFs has been addressed in the literature.~ Ceylan and Myers (1980) compared the response predicted by the state space method to various other solution techniques including an analytical solution.~ Their results showed that for an adequate number of nodes the state space method computed a heat flux at the surface of a simple one layer slab within 1\% of the analytical solution.~ Ouyang and Haghighat (1991) made a direct comparison between the Laplace and state space methods.~ For a wall composed of insulation between two layers of concrete, they found almost no difference in the response factors calculated by each method.
+
+Seem (1987) summarizes the steps required to obtain the CTF coefficients from the A, B, C, and D matrices.~ While more time consuming than calculating CTFs using the Laplace Transform method, the matrix algebra (including the calculation of an inverse and exponential matrix for A) is easier to follow than root find algorithms.~ Another difference between the Laplace and State Space methods is the number of coefficients required for a solution.~ In general, the State Space method requires more coefficients.~ In addition, the number of temperature and flux history terms is identical (nz = nq).~ Note that as with the Laplace method that the actual number of terms will vary from construction to construction.
+
+Two distinct advantages of the State Space method over the Laplace method that are of interest when applying a CTF solution for conduction through a building element are the ability to obtain CTFs for much shorter time steps and the ability to obtain 2- and 3-D conduction transfer functions.~ While not implemented in the Toolkit, both Seem (1987) and Strand (1995) have demonstrated the effectiveness of the State Space method in handling these situations that can have important applications in buildings.
+
+\subsection{Conduction Transfer Function (CTF) Calculations in EnergyPlus}\label{conduction-transfer-function-ctf-calculations-in-energyplus}
+
+Conduction transfer functions are an efficient method to compute surface heat fluxes because they eliminate the need to know temperatures and fluxes within the surface.~ However, conduction transfer function series become progressively more unstable as the time step decreases.~ This became a problem as investigations into short time step computational methods for the zone/system interactions progressed because, eventually, this instability caused the entire simulation to diverge.~ This phenomenon was most apparent for thermally massive constructions with long characteristic times and, correspondingly, requiring a large number of terms in the CTF series. This indicates that the problem is related to round-off and truncation error and is in no way an indictment of the CTF method itself.~ Methods that develop CTF series from finite difference approximations to the heat conduction equation (Meyers, 1980; Seem, 1987) were considered to address this problem.~ Seem's method did give better accuracy and stability at short time steps than the current BLAST technique but, the method still had difficulty computing stable CTF series for time steps of less than 1/4 hour for the heaviest constructions in the BLAST library.
+
+The zone heat gains consist of specified internal heat gains, air exchange between zones, air exchange with the outside environment, and convective heat transfer from the zone surfaces.~ Of these, the surface convection load requires the most complicated calculations because a detailed energy balance is required at the inside and outside surface of each wall, floor, and roof.~ In addition, the transient heat conduction in the material between the surfaces must be solved.~ This solution gives the inside and outside temperatures and heat fluxes that must be known in order to calculate the convection component to the zone load for each zone surface.~ BLAST uses a conduction transfer function CTF method attributed to Hittle (1980) to solve the transient conduction problem for each surface.~ The method results in a time series of weighting factors that, when multiplied by previous values of the surface temperatures and fluxes and the current inside and outside surface temperatures, gives the current inside and outside heat flux.~ The method is easily applied to multilayered constructions for which analytical solutions are unavailable.~ In addition, determining the series of CTF coefficients is a one-time calculation, making the method much faster than finite difference calculations.
+
+A problem with CTF methods is that the series time step is fixed; that is, a CTF series computed for a one hour time step takes information at t-1 hours, t-2 hours, etc. and computes conditions at the current time t.~ As time advances the oldest term in the input series is dropped and the data moved back one time step to allow the newest value to be added to the series.~ For convenience, the time step used to determine the CTF series should be the same as the time step used to update the zone mean air temperature in the zone energy balance.~ But, as the time step used to calculate the CTF series gets shorter, the number of terms in the series grows.~ Eventually, with enough terms, the series becomes unstable due to truncation and round-off error.~ Heavy constructions, such as slab-on-grade floors (12" heavyweight concrete over 18" dirt), have accuracy and stability problems at time steps as large as 0.5 hours when modeled by Hittle's CTF method.~ In an attempt to overcome this problem, Hittle's method was replaced by Seem's method (1987) in IBLAST.~ This resulted in some improvement in stability at shorter time steps, but not enough to allow IBLAST to run at a 0.1 hour time step without restricting the types of surfaces that could be used.
+
+Even though CTF methods require that values of the surface temperatures and fluxes be stored for only a few specific times before the current time, the temperature and flux histories are, actually, continuous functions between those discrete points.~ However, there is no way to calculate information at these intermediate times once a series has been initialized.~ The terms in the temperature and flux histories are out of phase with these points.~ However, they can be calculated by shifting the phase of the temperature and flux histories by only a fraction of a time step.~ This procedure would allow a CTF series computed for a time step Dt, to be used to compute information at times t+Dt/2, t+Dt/3, t+Dt/4, or any other arbitrary fraction of the time step, so long as the surface temperatures and flux values were still Dt apart.~ Several ways of doing this are described below.
+
+The method shown in the Figure~\ref{fig:multiple-staggered-time-history-scheme} maintains two sets of histories out of phase with each other.~ The figure shows how this would work for two sets of histories out of phase by one half of a time step.~ More sets of temperature and flux histories could be used, allowing the simulation time step to take on values: 1/3, 1/4, 1/5, etc., of the minimum time step allowed for the CTF calculations.~ The time step between inputs to the CTF series would be the smallest convenient interval at which the CTF series is stable.~ This scenario is illustrated in this figure for two separate sets of temperature and flux histories.~ Cycling through each history, in order, allowed calculations of the zone energy balance to be performed with updated surface information at a shorter time step than one CTF history series would otherwise allow.~ This method required no interpolation between the series once each set of histories was initialized.~ However, if the smallest time step for a stable CTF series was large compared to the zone temperature update time step, significant memory was required to store all the sets of histories.
+
+\begin{figure}[hbtp] % fig 11
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image169.svg.png}
+\caption{Multiple, staggered time history scheme \protect \label{fig:multiple-staggered-time-history-scheme}}
+\end{figure}
+
+Another method is shown in Figure~\ref{fig:sequential-interpolation-of-new-histories}. Sequential interpolation of new histories that uses successive interpolations to determine the next set of temperature and flux histories.~ The current history is interpolated directly from the previous history set using the required time phase shift between the two.~ This method required permanent storage for only one set of temperature and flux histories at a time, but smoothed out temperature and flux data as more interpolations were performed.~ As a result, at concurrent simulation times current values of history terms were different form previous ``in phase'' history terms.~ This was unacceptable from, a physical point of view, because it allowed current information to change data from a previous time.
+
+\begin{figure}[hbtp] % fig 12
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image170.svg.png}
+\caption{Sequential interpolation of new histories \protect \label{fig:sequential-interpolation-of-new-histories}}
+\end{figure}
+
+A final method, shown in Figure~\ref{fig:master-history-with-interpolation}. Master history with interpolation, was something of a hybrid of the previous two methods.~ One ``master'' history set was maintained and updated for all time; this solved the problem of current events propagating information backwards in time.~ When surface fluxes needed to be calculated at times out of phase with this master history a new, temporary history was interpolated from the master values.~ This method proved to be the best of the three options described because it eliminated propagation of information backwards in time and only required concurrent storage of two sets of temperature and flux histories. This method was subsequently incorporated into the IBLAST program in conjunction with Seem's procedure for calculating the coefficients of the CTF series.
+
+\begin{figure}[hbtp] % fig 13
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image171.svg.png}
+\caption{Master history with interpolation \protect \label{fig:master-history-with-interpolation}}
+\end{figure}
+
+\subsection{Conduction Transfer Function (CTF) Calculations Special Case: R-Value Only Layers}\label{conduction-transfer-function-ctf-calculations-special-case-r-value-only-layers}
+
+Most users will elect to enter materials with four parameters that are of interest for calculating conduction transfer functions: thickness, conductivity, density, and specific heat.~ For these materials, EnergyPlus will divide each material layer within a construction into between 6 and 18 nodes for the application of the state-space method.~ For multi-layered constructions, nodes are also placed at the interface between two layers.~ These interface nodes consist of half a node of the first layer and half a node of the second layer.
+
+In some cases, either due to a lack of information or a desire to simplify input, a user may choose to enter a material layer as a ``no mass'' or ``R-Value only'' material.~ This assumption essentially says that these layers add nothing to the thermal mass of the overall construction and only add to the overall resistance or R-Value of the construction as a whole.~ While this is not recommended, it is allowed and in some cases is not a poor assumption for extremely lightweight materials such as some types of insulation.
+
+In the past, when a user enters such a ``no mass'' material into EnergyPlus, internally the properties of this layer are converted to approximate the properties of air (density, specific heat, and conductivity) with the thickness adjusted to maintain the user's desired R-Value.~ This allowed such layers to be handled internally in the same way as other layers without any additional changes to the code.~ This solution was deemed accurate enough as air has very little thermal mass and it made the coding of the state space method simpler.
+
+It is possible to account for layers that have no thermal mass in the state space solution without resorting to the assignment of fictitious material properties.~ The EnergyPlus internal equations for assigning values to portions of the A, B, C, and D matrices as shown in the previous subsections have been altered to account for the potential presence of R-Value only (or no mass) layers without resorting to assigning these materials the properties of air.~ This is handled by assuming that the ``no mass'' layer is a single node layer.~ As nodes are defined that the interface between material layers, the ``no mass'' layer is essentially two ``half nodes'' that are shared with the surrounding layers.~ This allows the surrounding material layers to provide thermal capacitance for each of the nodes at the material interfaces.
+
+In EnergyPlus, there are two possible cases for the existence of ``no mass'' layers: either between two other solid, thermally massive layers (multiple ``no mass'' layers next to each other are simply combined in this approach) or at the inner or outer most layers of a construction.~ There are potential issues with having a resistance-only layer at either the inner or outer most layers of a construction.~ A little or no mass layer there could receive intense thermal radiation from internal sources or the sun causing the temperature at the inner or outer surface to achieve very high levels.~ This is undesirable from a simulation standpoint as there are limits to temperature levels in EnergyPlus that could be exceeded causing the simulation to terminate and is likely unrealistic from a real-world perspective.~ Thus, for such potentially problematic calculational scenarios, EnergyPlus will continue to convert a ``no mass'' layer at either the inner or outer most layer of a construction into a thermal mass layer using the properties of air as has been done in the past.
+
+The case where a resistance-only layer is defined anywhere except the inner or outer layer of a construction is handled by treating the ``no mass'' layer as a single node layer.~ This will result in a node at each interface as in the standard material layer cases.~ When a ``no mass'' material is present, the R-Value only layer will not add any thermal capacitance to the nodes at the interfaces at either side of the material.~ It will simply add resistance between the two nodes.
+
+\begin{figure}[hbtp] % fig 14
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image172.png}
+\caption{Illustration of no-mass layer between two mass layers \protect \label{fig:illustration-of-no-mass-layer-between-two}}
+\end{figure}
+
+From the EnergyPlus code, the A matrix (AMat) is assigned with values at the interface using the following equations (taken from the actual code):
+
+\begin{lstlisting}
+cap = ( rho(Layer)\*cp(Layer)\*dx(Layer) + rho(Layer+1)\*cp(Layer+1)\*dx(Layer+1) ) \* 0.5D0
+AMat(Node,Node-1) = rk(Layer)/dx(Layer)/cap           ! Assign matrix values for the current node
+AMat(Node,Node)   = -1.0D0 \* ( rk(Layer)/dx(Layer)+rk(Layer+1)/dx(Layer+1) ) / cap
+AMat(Node,Node+1) = rk(Layer+1)/dx(Layer+1)/cap       ! node.
+\end{lstlisting}
+
+Note that these equations do not change.~ For ``no mass'' layers, the density (rho) and the specific heat (cp) variables will be assigned zero values.~ In addition, the thickness (dx) will be equated with the user-defined R-Value and conductivity (rk) will be assigned a value of unity.~ In addition, the number of nodes for the ``no mass'' layer will be set to 1.
+
+This handles resistive layers correctly without resorting to assigning the properties of air to the ``no mass'' layer.~ The only potential problem with this is if two resistive layers are placed next to each other.~ In that case, the interface between the two resistive layers would have no mass (variable ``cap'' would equal zero) and a divide by zero would result.~ To avoid this, adjacent ``no mass'' layers are combined internally so that the user does not have to do this and also to avoid any divide by zero errors.
+
+While from a results standpoint, the difference in output between assigning air properties for specific heat, density, etc. and handling the no mass materials explicitly is negligible, handling the no mass layers properly does provide better code efficiency from a calculation speed standpoint.
+
+\subsection{References}\label{references-014}
+
+Ceylan, H. T., and G. E. Myers. 1980. Long-time Solutions to Heat Conduction Transients with Time-Dependent Inputs. ASME Journal of Heat Transfer, Volume 102, No. 1, pp.~115-120.
+
+Hittle, D. C. 1979. Calculating Building Heating and Cooling Loads Using the Frequency Response of Multilayered Slabs, Ph.D.~Thesis, University of Illinois, Urbana, IL.
+
+Hittle, D. C., and R. Bishop. 1983. An Improved Root-Finding Procedure for Use in Calculating Transient Heat Flow Through Multilayered Slabs. International Journal of Heat and Mass Transfer, Vol. 26, No. 11, pp.~1685-1693.
+
+Ouyang, K., and F. Haghighat. 1991. A Procedure for Calculating Thermal Response Factors of Multi-layered Walls--State Space Method. Building and Environment, Vol. 26, No. 2, pp.~173-177.
+
+Seem, J. E. 1987. Modeling of Heat Transfer in Buildings, Ph.D.~Thesis, University of Wisconsin, Madison, WI.
+
+Strand, R. K. 1995. Heat Source Transfer Functions and Their Application to Low Temperature Radiant Heating Systems, Ph.D.~Thesis, University of Illinois, Urbana, IL.
+
+Taylor, R. D., C.O. Pedersen, D.E. Fisher, R. J. Liesen, L.K. Lawrie. 1990. \emph{Simultaneous Simulation of Buildings and Mechanical Systems in Heat Balance Based Energy Analysis Programs}, Proceedings of the 3rd International Conference on System Simulation in Buildings, Liege, Belgium, December 3-5, 1990.
+
+Taylor, R.D., C.O. Pedersen, D.E. Fisher, R. J. Liesen, L.K. Lawrie. 1991. Impact of Simultaneous Simulation of Buildings and Mechanical Systems in Heat Balance Based Energy Analysis Programs on System Response and Control, Conference Proceedings IBPSA Building Simulation '91, Nice, France, August 20-22, 1991.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/effective-moisture-penetration-depth-empd.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/effective-moisture-penetration-depth-empd.tex
new file mode 100644
index 00000000000..2bdf0c7e777
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/effective-moisture-penetration-depth-empd.tex
@@ -0,0 +1,148 @@
+\section{Effective Moisture Penetration Depth (EMPD) Model}\label{effective-moisture-penetration-depth-empd-model}
+
+\subsection{Overview}\label{overview-014}
+
+Moisture has little effect on heating system performance, but a profound effect on the performance of air conditioning systems.~ In order to accurately describe building performance during periods when cooling is needed, it is very important to know the moisture conditions of the building.~ If one assumes that all building moisture is contained in the room air, then one ignores the fact that the materials that bound the room (e.g.~wall surfaces, furnishings, linens, etc.) store and release moisture.~ Thus, to assume that the only moisture that effects cooling system performance is contained in the room air is a false, and it can lead to significant error in the prediction of room moisture conditions and cooling system loads.
+
+The EMPD (Effective Moisture Penetration Depth) model is a simplified, lumped approach to simulate surface moisture adsorption and desorption.
+
+\subsection{EMPD Model Description}\label{empd-model-description}
+
+The EMPD concept assumes that a thin layer ($\delta$\(_{M}\)) close to the wall surface behaves dynamically and exchanges moisture with the air domain when exposed to cyclic air moisture pulses.~ For short periods where the cyclic integral of the total moisture adsorption and desorption is near zero (i.e.~there is no net moisture storage), the EMPD concept has been shown to be a reasonable approximation of reality (Kerestecioglu et al, 1989).~ In other words, the following constraint must be met:
+
+\begin{equation}
+\int_{{\tau_1}}^{{\tau_2}} {\frac{{dU}}{{d\tau }}} d\tau  = 0
+\end{equation}
+
+where, $\tau$\(_{2}\)-$\tau$\(_{1}\) denotes the finite time interval over which the equation holds.~ The EMPD model assumes no spatial distribution of moisture content across the thickness (L) of the solid; rather, a thin layer ($\delta$\(_{M}\)) of uniform moisture content (U) is assumed to represent the total moisture content of the solid. This may be mathematically stated as:
+
+\begin{equation}
+\int_0^L {U(x)dx = U{\delta_M}}
+\end{equation}
+
+For most building materials, the equilibrium moisture sorption isotherm can be defined by the following general equation (Kerestecioglu et al. 1988):
+
+\begin{equation}
+U = a{\varphi ^b} + c{\varphi ^d}
+\end{equation}
+
+where
+
+\begin{equation}
+\varphi  \approx \frac{{{W^*}}}{{{W_{sat}}^*}}
+\end{equation}
+
+and
+
+\begin{equation}
+{W_{sat}}^* = \frac{1}{{{R_v}{\rho_a}{T^*}}}\exp \left( {23.7093 - \frac{{4111}}{{{T^*} - 35.45}}} \right)
+\end{equation}
+
+~Given that U = U(W\(^{*}\),T\(^{*}\)), the moisture content may be differentiated with respect to time in the following manner:
+
+\begin{equation}
+\frac{{du}}{{d\tau }} = \frac{{\partial U}}{{\partial {W^*}}}\frac{{d{W^*}}}{{d\tau }} + \frac{{\partial U}}{{\partial {T^*}}}\frac{{d{T^*}}}{{d\tau }} = {A_T}\frac{{d{W^*}}}{{d\tau }} - {B_\rho }\frac{{d{T^*}}}{{d\tau }}
+\end{equation}
+
+where A\(_{T}\) and B\(_{\rho}\) are the isothermal moisture capacity and thermo-gradient coefficient, respectively.~ From Eqs. , and , they can be expressed as:
+
+\begin{equation}
+{A_T} = \frac{{ab{\varphi ^b} + cd{\varphi ^d}}}{{{W^*}}}
+\end{equation}
+
+and
+
+\begin{equation}
+{B_\rho } =  - \left[ {\frac{1}{{{T^*}}} - \frac{{4111}}{{{{({T^*} - 35.45)}^2}}}} \right]*(ab{\varphi ^b} + cd{\varphi ^d})
+\end{equation}
+
+The lumped mass transfer equation for the i-th solid domain may be written as
+
+\begin{equation}
+{(A{\rho_b}{\delta_M})_i}\frac{{d{U_i}}}{{d\tau }} = {h_{M,i}}{A_i}({W_r} - {W_i}^*)
+\end{equation}
+
+Using Eqs. , , and , one obtains the final equation needed for closure moisture transfer at internal surface.
+
+\begin{equation}
+{({A_i}{\rho_b}{\delta_M}{A_T})_i}\frac{{d{W_i}^*}}{{d\tau }} = {h_{M,i}}{A_i}({W_r} - {W_i}^*) + {(A{\rho_b}{\delta_M}{B_\rho })_i}\frac{{d{T_i}^*}}{{d\tau }}
+\end{equation}
+
+The energy equation for the envelope contains the surface temperature and is given by the conduction equation
+
+\begin{equation}
+\rho {C_p}\frac{{dT}}{{d\tau }} = \nabla  \cdot (k\nabla T)
+\end{equation}
+
+with the boundary conditions at interior surface
+
+\begin{equation}
+- k\nabla T =  - {q_T}`` + {h_T}({T^*} - {T_r}) + \lambda {h_M}({W^*} - {W_r})
+\end{equation}
+
+A more detailed account of the numerical solution procedure can be found in Kerestecioglu et al. (1988).
+
+\subsection{EMPD Value Determination}\label{empd-value-determination}
+
+An effective moisture penetration depth may be determined from either experimental or detailed simulation data by using actual surface areas and moisture vapor diffusivity.~ An empirical function derived from the detailed simulation may be used to determine the EMPD value (Kerestecioglu et al, 1989):
+
+\begin{equation}
+{\delta_M} = 12.567024 - 12.21373*\exp \left( { - 267.0211*{D_v}^{0.7}*{\xi ^{ - 0.7}}} \right)
+\end{equation}
+
+where
+
+\begin{equation}
+\xi  = \left| {\frac{{\Delta \varphi }}{{\Delta \tau }}} \right|
+\end{equation}
+
+Figure~\ref{fig:limit-of-effective-penetration-depth-values} gives the EMPD values to be used for various vapor diffusivities evaluated at different ambient excitations.
+
+\begin{figure}[hbtp] % fig 17
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image241.svg.png}
+\caption{Limit of Effective Penetration Depth Values for Various Vapor Diffusivities at Different Ambient Excitations. \protect \label{fig:limit-of-effective-penetration-depth-values}}
+\end{figure}
+
+\subsection{EMPD Nomenclature}\label{empd-nomenclature}
+\begin{align*}  
+  A  &= \text{Area} [m^{2}] \\
+  A_{T}  &= \text{Isothermal moisture capacity} [m/(^{3}/kg] \\
+  B_{\rho}  &= \text{Thermo-gradient coefficient} [kg/kg-K] \\
+  C_{p}  &= \text{Specific heat} [J/kg-K] \\
+  h_{M}  &= \text{Convective mass transfer coeff.} [kg/m^{2}-s] \\
+  h_{T}  &= \text{Convective heat transfer coeff.} [W/m^{2}-K] \\
+  k  &= \text{Thermal conductivity} [W/m-K] \\
+  L  &= \text{Length} [m] \\
+  q``_{T}  &= \text{Imposed heat flux} [W/m^{2}] \\
+  R_{v}  &= \text{Ideal gas constant} [461.52 J/kg-K] \\
+  T  &= \text{Temperature} [K] \\
+  U  &= \text{Moisture content} [kg/kg] \\
+  W  &= \text{Humidity ratio} [kg/kg]
+\end{align*}
+
+\subsubsection{Greek letters}\label{greek-letters}
+\begin{align*}  
+  \delta\PB{M}  &= \text{Effective penetration depth for moisture equation} \bracketunits{\meter} \\
+  \lambda       &= \text{Heat of vaporization} \bracketunits{\joule\per\kilogram} \\
+  \rho          &= \text{Density} \bracketunits{\kilogram\per\cubic\meter} \\
+  \tau          &= \text{Time} \bracketunits{\second} \\
+  \varphi       &= \text{Relative humidity - fraction, 0 to 1} \bracketunits{-} \\
+  \xi           &= \text{Ambient moisture excitation rate} \bracketunits{\per\hour}
+\end{align*}
+
+\subsubsection{Subscripts and superscripts}\label{subscripts-and-superscripts}
+\begin{align*}  
+  a             &= \text{Air} \\
+  b             &= \text{Bulk} \\
+  *             &= \text{Surface} \\
+  i             &= \text{i-th surface} \\
+\end{align*}
+
+\subsection{References}\label{references-019}
+
+Kerestecioglu, A., Swami, M., Dabir, R., Razzaq, N., and Fairey, P., 1988, ``Theoretical and Computational Investigation of Algorithms for Simultaneous Heat and Moisture Transport in Buildings,'' FSEC-CR-191-88, Florida Solar Energy Center, Cape Canaveral, FL.
+
+Kerestecioglu, A., M. Swami and A. Kamel, 1989, ``Theoretical and Computational Investigation of Simultaneous Heat and Moisture Transfer in Buildings: Effective Penetration Depth Theory.''~ ASHRAE Winter Meeting, Atlanta, GA.
+
+Kerestecioglu, A., M. V. Swami, P. Brahma, L. Gu, P. Fairey, and S. Chandra, 1989, ``FSEC 1.1 User's Manual,'' Florida Solar Energy Center, Cape Canaveral, FL
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/exterior-naturally-vented-cavity.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/exterior-naturally-vented-cavity.tex
new file mode 100644
index 00000000000..df78cbbad66
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/exterior-naturally-vented-cavity.tex
@@ -0,0 +1,242 @@
+\section{Exterior Naturally Vented~ Cavity}\label{exterior-naturally-vented-cavity}
+
+The input object ``SurfaceProperty:ExteriorNaturalVentedCavity'' allows modeling a special case for the outside boundary conditions of heat transfer surfaces with a multi-skin exterior that is opaque.~ From the thermal envelope's point of view, the presence of a vented cavity on the outside of the surface modifies the conditions experienced by the underlying heat transfer surfaces.~ This exterior cavity acts as a radiation and convection baffle situated between the exterior environment and the outside face of the underlying heat transfer surface.~ The actual outer surface is referred to as the ``baffle''.~ The modeling here assumes that the heat capacity in the outer baffle can be neglected since it is much lower than the underlying mass surface.~ This object is used with the BuildingSurface:Detailed object where the heat transfer surfaces are referred to as the underlying surfaces.~ The constructions and materials for the heat transfer surfaces should reflect the construction of just the underlying surface.~ The SurfaceProperty:ExteriorNaturalVentedCavity object is used to describe the detached layer, or baffle, and the characteristics of the cavity and openings for natural ventilation.~ This model uses the SurfaceProperty:OtherSideConditionsModel object to pass boundary conditions to the heat transfer modeling for the underlying surfaces.
+
+\subsection{Baffle Heat Balance}\label{baffle-heat-balance}
+
+The baffle is assumed to be sufficiently thin and high-conductivity so that it can be modeled using a single temperature (for both sides and along its area).~ This temperature \({T_{s,baff}}\) is determined by formulating a heat balance on a control volume that just encapsulates the baffle surface.~ The baffle is assumed to completely cover the underlying surface such that it is opaque to shortwave and longwave radiation.~ This assumption means that even though the baffle will have some open area for ventilation, no solar energy passes through these openings. The heat balance is diagrammed in the following figure.
+
+\begin{figure}[hbtp] % fig 33
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image438.png}
+\caption{Baffle Surface Heat Balance \protect \label{fig:baffle-surface-heat-balance}}
+\end{figure}
+
+The heat balance on the baffle surface's control volume is:
+
+\begin{equation}
+{q''_{\alpha sol}} + {q''_{LWR,Env}} + {q''_{conv,Env}} + {q''_{LWR,cav}} + {q''_{conv,cav}} + {q''_{source}} = 0
+\end{equation}
+
+where: 
+\(q''_{\alpha sol}\) is absorbed direct and diffuse solar (short wavelength) radiation heat flux.
+\(q''_{LWR,Env}\) is net long wavelength (thermal) radiation flux exchange with the air and surroundings.
+\(q''_{conv,Env}\) = surface convection flux exchange with outside air.
+\(q''_{LWR,cav}\) is net long wavelength (thermal) radiation flux exchange with the outside face of the underlying surface(s).
+\(q''_{conv,cav}\) = surface convection flux exchange with cavity air.
+\({q''_{source}}\) is a source/sink term that accounts for energy exported out of the control volume when the baffle is a hybrid device such as a photovoltaic panel.
+
+All terms are positive for net flux to the baffle.~ Each of these heat balance components is introduced briefly below.
+
+\subsubsection{External SW Radiation}\label{external-sw-radiation}
+
+\(q''_{\alpha sol}\)~is calculated using procedures presented elsewhere in this manual and includes both direct and diffuse incident solar radiation absorbed by the surface face.~ This is influenced by location, surface facing angle and tilt, shading surfaces, surface face material properties, weather conditions, etc.~ The baffle blocks all shortwave radiation from reaching the underlying surface.
+
+\subsubsection{External LW Radiation}\label{external-lw-radiation}
+
+\({q''_{LWR,Env}}\) ~is a standard radiation exchange formulation between the surface, the sky, the ground, and the atmosphere.~ The radiation heat flux is calculated from the surface absorptivity, surface temperature, sky, air, and ground temperatures, and sky and ground view factors.~ Radiation is modeled using linearized coefficients. ~The baffle blocks all longwave radiation.
+
+\subsubsection{External Convection}\label{external-convection}
+
+\(q''_{conv,env}\) is modeled using the classical formulation: \(q''_{conv} = h_{co}(T_{air} - T_{o})\) where h\(_{co}\), is the convection coefficient.~ The h\(_{co}\) is treated in the same way as an outside face with ExteriorEnvironment conditions.~ In addition, when it is raining outside, we assume the baffle gets wet and model the enhanced surface heat transfer using a large value for \({h_{co}}\) .
+
+\subsubsection{Cavity LW Radiation}\label{cavity-lw-radiation}
+
+\({q''_{LWR,cav}}\) is a standard radiation exchange formulation between the baffle surface and the underlying heat transfer surface located across the cavity.~ Radiation is modeled using linearized coefficients.
+
+\subsubsection{Cavity Convection}\label{cavity-convection}
+
+\(q''_{conv,cav}\) is modeled using the classical formulation: \(q''_{conv} = h_{cp}(T_{air} - T_{o})\) where h\(_{cp}\), is the convection coefficient. The value for h\(_{cp}\) is obtained from correlations used for window gaps from ISO (2003) standard 15099.
+
+Substituting models into (113) and solving for \({T_{s,baff}}\) ~yields the following equation:
+
+\begin{equation}
+{T_{s,baff}} = \frac{{\left( {{I_s}\alpha  + {h_{co}}{T_{amb}} + {h_{r,atm}}{T_{amb}} + {h_{r,sky}}{T_{sky}} + {h_{r,gnd}}{T_{amb}} + {h_{r,cav}}{T_{so}} + {h_{c,cav}}{T_{a,cav}} + {{q''}_{source}}} \right)}}{{\left( {{h_{co}} + {h_{r,air}} + {h_{r,sky}} + {h_{r,gnd}} + {h_{r,cav}} + {h_{c,cav}}} \right)}}
+\end{equation}
+
+where,
+
+\({I_s}\) ~is the incident solar radiation of all types {[}W/m\(^{2}\){]},
+
+\(\alpha\) ~is the solar absorptivity of the baffle {[}dimensionless{]},
+
+\({h_{r,atm}}\) is the linearized radiation coefficient for the surrounding atmosphere {[}W/m\(^{2}\)·K{]},
+
+\({T_{amb}}\) ~is the outdoor drybulb from the weather data, also assumed for ground surface {[}ºC{]},
+
+\({h_{r,sky}}\) ~is the linearized radiation coefficient for the sky {[}W/m\(^{2}\)·K{]},
+
+\({T_{sky}}\) ~is the effective sky temperature {[}ºC{]},
+
+\({h_{r,gnd}}\) ~is the linearized radiation coefficient for the ground {[}W/m\(^{2}\)·K{]},
+
+\({h_{r,cav}}\) ~is the linearized radiation coefficient for the underlying surface {[}W/m\(^{2}\)·K{]},
+
+\({T_{so}}\) ~is the temperature of the outside face of the underlying heat transfer surface {[}ºC{]},
+
+\({h_{co}}\) ~is the convection coefficient for the outdoor environment {[}W/m\(^{2}\)·K{]},
+
+\({h_{c,cav}}\) ~is the convection coefficient for the surfaces facing the plenum {[}W/m\(^{2}\)·K{]}, and
+
+\({T_{a,cav}}\) ~is the drybulb temperature for air in the cavity {[}ºC{]}.
+
+\subsection{Cavity Heat Balance}\label{cavity-heat-balance}
+
+The \emph{cavity} is the volume of air located between the baffle and the underlying heat transfer surface.~ The cavity air is modeled as well-mixed.~ The uniform temperature of the cavity air, \({T_{a,cav}}\) , is determined by formulating a heat balance on a control volume of air as diagrammed below.
+
+\begin{figure}[hbtp] % fig 34
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image469.png}
+\caption{Cavity Air Heat Balance \protect \label{fig:cavity-air-heat-balance}}
+\end{figure}
+
+The heat balance on the cavity air control volume is:
+
+\begin{equation}
+{\dot Q_{vent}} + {\dot Q_{co}} + {\dot Q_{c,baff}} = 0
+\end{equation}
+
+where,
+
+\(\dot{Q}_{vent}\) is the net rate of energy added from natural ventilation -- where outdoor ambient air exchanges with the cavity air. \(\dot{Q}_{co}\) is the net rate of energy added by surface convection heat transfer with the underlying surface.
+
+\({\dot Q_{c,baff}}\) is the net rate of energy added by surface convection heat transfer with the collector.
+
+And substituting into yields the following equation:
+
+\begin{equation}
+{T_{a,cav}} = \frac{{\left( {{h_{c,cav}}A\,{T_{so}} + {{\dot m}_{vent}}{c_p}{T_{amb}} + {h_{c,cav}}A\,{T_{s,baff}}} \right)}}{{\left( {{h_{c,cav}}A + {{\dot m}_{vent}}{c_p} + {h_{c,cav}}A} \right)}}
+\end{equation}
+
+where,
+
+\({\dot m_{vent}}\) ~is the air mass flow from natural forces {[}kg/s{]}
+
+Modeling natural ventilation air exchanges in a general way is challenging.~ Simplistic engineering models are used to model \({\dot m_{vent}}\) ~resulting from natural buoyancy and wind forces.~ Reasoning that the configuration is similar to single-side natural ventilation, we elect to use correlations for natural ventilation presented as equations (29) and (30) in Chapter 26. of ASHRAE HOF (2001).
+
+\begin{equation}
+{\dot m_{vent}} = \rho \,{{\rm{\rlap{--} \dot V}}_{{\rm{tot}}}}
+\end{equation}
+
+where,
+
+\(\rho\) ~is the density of air {[}kg/m\(^{3}\){]}, and
+
+\(\rlap{--} \dot{V}_{tot} = \rlap{--} \dot{V}_{wind} + \rlap{--} \dot{V}_{thermal}\) ~is the total volumetric flow rate of air ventilating in and out of the cavity.
+
+\begin{equation}
+\rlap{--} \dot{V}_{wind} = C_{v}A_{in}U_{\infty}
+\end{equation}
+
+\begin{equation}
+\rlap{--} \dot{V}_{thermal} = \left\{
+    \begin{array}{cl}
+      C_{D}A_{in}\sqrt{2g\Delta H_{NPL}\left(T_{a,cav}-T_{amb}\right)/T_{a,cov}} & \; \left(T_{a,cav} > T_{amb}\right) \\
+      C_{D}A_{in}\sqrt{2g\Delta H_{NPL}\left(T_{amb}-T_{a,cav}\right)/T_{amb}} & \; \left(T_{a,cav} < T_{amb}\,\text{and baffle is vertical}\right) 
+    \end{array}
+  \right.
+\end{equation}
+
+\({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}} = {C_D}{A_{in}}\sqrt {2g\Delta {H_{NPL}}\left( {{T_{a,cav}} - {T_{amb}}} \right)/{T_{a,cav}}}\) ~ (if \(T_{a,cav} > T_{amb}\) )
+
+\({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}} = {C_D}{A_{in}}\sqrt {2g\Delta {H_{NPL}}\left( {{T_{amb}} - {T_{a,cav}}} \right)/{T_{amb}}}\) ~ (if \(T_{amb} > T_{a,cav}\) ~and baffle is vertical)
+
+\({C_v}\) ~is the effectiveness of the openings that depends on opening geometry and the orientation with respect to the wind.~ ASHRAE HoF (2001) indicates values ranging from 0.25 to 0.6.~ This value is available for user input.
+
+\({C_D}\) ~is the discharge coefficient for the opening and depends on opening geometry.~ This value is available for user input.
+
+Mass continuity arguments lead to modeling the area of the openings as one half of the total area of the openings, so we have:
+
+\begin{equation}
+{A_{in}} = \frac{{A\,}}{2}
+\end{equation}
+
+\(g\) ~is the gravitational constant taken as 9.81 {[}m/s\(^{2}\){]}.
+
+\(\Delta {H_{NPL}}\) ~is the height from midpoint of lower opening to the Neutral Pressure Level.~ This is value is available for user input.
+
+If the cavity is horizontal and \(T_{amb} > T_{a,cav}\) ~then \({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}}{\rm{ = 0}}\) ~because this is a stable situation.
+
+\subsection{Underlying Heat Transfer Surface}\label{underlying-heat-transfer-surface}
+
+The exterior baffle and cavity are applied to the outside of a heat transfer surface.~ This surface is modeled using the usual EnergyPlus methods for handling heat capacity and transients -- typically the CTF method.~ These native EnergyPlus heat balance routines are used to calculate \({T_{so}}\) .~ The exterior baffle and cavity system is coupled to the underlying surface using the SurfaceProperty:OtherSideConditionsModel mechanism.~ The exterior naturally vented cavity model provides values for \({h_{r,cav}}\) ,\({T_{s,baff}}\) , \({h_{c,cav}}\) , and \({T_{a,cav}}\) ~for use with the heat balance model calculations for the outside face of the underlying surface (described elsewhere in this manual).
+
+\subsection{Solar and Shading Calculations}\label{solar-and-shading-calculations}
+
+The exterior vented cavity model uses standard EnergyPlus surfaces in order to take advantage of the detailed solar and shading calculations.~ Solar radiation incident on the surface includes beam and diffuse radiation, as well as radiation reflected from the ground and adjacent surfaces.~ Shading of the collector by other surfaces, such as nearby buildings or trees, is also taken into account.
+
+\subsection{Local Wind Speed Calculations}\label{local-wind-speed-calculations}
+
+The outdoor wind speed affects terms used in modeling.~ The wind speed in the weather file is assumed to be measured at a meteorological station located in an open field at a height of 10 m.~ To adjust for different terrain at the building site and differences in the height of building surfaces, the local wind speed is calculated for each surface.
+
+The wind speed is modified from the measured meteorological wind speed by the equation (ASHRAE 2001):
+
+\begin{equation}
+{U_\infty } = {V_{met}}{\left( {\frac{{{\delta_{met}}}}{{{z_{met}}}}} \right)^{{a_{met}}}}{\left( {\frac{z}{\delta }} \right)^a}
+\end{equation}
+
+where z is the height of the centroid of the system, z\(_{met}\) is the height of the standard meteorological wind speed measurement, and a and d are terrain-dependent coefficients.~ d is the boundary layer thickness for the given terrain type.~ The values of a and d are shown in the following tables:
+
+% table 19
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Terrain-Dependent Coefficients (ASHRAE 2001). \label{table:terrain-dependent-coefficients-ashrae-2001.}} \tabularnewline
+\toprule 
+Terrain & Description & Exponent, a & Layer Thickness, $\delta$ (m) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Terrain-Dependent Coefficients (ASHRAE 2001).} \tabularnewline
+\toprule 
+Terrain & Description & Exponent, a & Layer Thickness, $\delta$ (m) \tabularnewline
+\midrule
+\endhead
+
+1 & Flat, open country & 0.14 & 270 \tabularnewline
+2 & Rough, wooded country & 0.22 & 370 \tabularnewline
+3 & Towns and cities & 0.33 & 460 \tabularnewline
+4 & Ocean & 0.10 & 210 \tabularnewline
+5 & Urban, industrial, forest & 0.22 & 370 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The exterior vented cavity can be defined such that it has multiple underlying heat transfer surfaces.~ The centroid heights for each surface are area-weighted to determine the average height for use in the local wind calculation.
+
+\subsection{Convection Coefficients}\label{convection-coefficients}
+
+Exterior cavity modeling requires calculating up to three different coefficients for surface convection heat transfer.~ These coefficients are defined in the classic way by:
+
+\begin{equation}
+{h_c} = \frac{{{T_{air}} - {T_{surf}}}}{{{{q''}_{conv}}}}
+\end{equation}
+
+First, \({h_{co}}\) ~is the convection coefficient for the baffle surface facing the outdoors.~ It is modeled in exactly the same way as elsewhere in EnergyPlus and will depend on the user setting for Outside Convection Algorithm -- Outside Surface Heat Balance entry elsewhere in this document.
+
+Second, \({h_{c,cav}}\) ~is the convection coefficient for baffle surfaces facing the cavity.~ This coefficient is applied to both the baffle and the underlying surface.~ The convection coefficient is modeled in the same way used in EnergyPlus to model air gaps in windows.~ These correlations vary by Rayleigh number and surface tilt and are based on the work of various research including Hollands et. al., Elsherbiny et. al., Wright, and Arnold.~ The formulations are documented in ISO (2003) standard 15099.~ The routines were adapted from Subroutine NusseltNumber in WindowManager.f90 (by F. Winkelmann), which itself was derived from Window5 subroutine ``nusselt''.
+
+\subsection{Radiation Coefficients}\label{radiation-coefficients}
+
+Exterior vented cavity modeling requires calculating up to four different linearized coefficients for radiation heat transfer.~ Whereas radiation calculations usually use temperature raised to the fourth power, this greatly complicates solving heat balance equations for a single temperature.~ Linearized radiation coefficients have the same units and are used in the same manner as surface convection coefficients and introduce very little error for the temperature levels involved.
+
+The radiation coefficient, \({h_{r,cav}}\) , is used to model thermal radiation between the collector surface and the outside face of the underlying heat transfer surface.~ We assume a view factor of unity.~ It is calculated using:
+
+\begin{equation}
+{h_{r,cav}} = {\sigma_{SB}}{e_{baff}}{e_{so}}\frac{{\left( {T_{s,baff}^4 - T_{so}^4} \right)}}{{\left( {{T_{s,baff}} - {T_{so}}} \right)}}
+\end{equation}
+
+where,
+
+all temperatures are converted to Kelvin,
+
+\({\sigma_{SB}}\) ~is the Stefan-Boltzmann constant,
+
+\({e_{baff}}\) ~is the longwave thermal emittance of the baffle, and
+
+\({e_{so}}\) ~is the longwave thermal emittance of the underlying heat transfer surface.
+
+The three other coefficients, \({h_{r,atm}}\) , \({h_{r,sky}}\) , and \({h_{r,gnd}}\) ~are used elsewhere in EnergyPlus for the outside face surface heat balance and are calculated in the same manner as equation .~ {[}This is accomplished by calling subroutine InitExteriorConvectionCoeffs in the file HeatBalanceConvectionCoeffs.f90. {]}
+
+\subsection{References}\label{references-023}
+
+ASHRAE HOF 2001.~ 2001 ASHRAE Fundamentals Handbook.~ American Society of Heating Refrigeration and Air-Conditioning Engineers. Altanta GA.
+
+ISO. 2003. ISO 15099:2003. Thermal performance of windows, doors, and shading devices -- Detailed calculations. International Organization for Standardization.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/green-roof-model-ecoroof.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/green-roof-model-ecoroof.tex
new file mode 100644
index 00000000000..8e7e261f425
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/green-roof-model-ecoroof.tex
@@ -0,0 +1,500 @@
+\section{Green Roof Model (EcoRoof)}\label{green-roof-model-ecoroof}
+
+\subsection{Overview}\label{overview-018}
+
+The input object Material:RoofVegetation provides a model for green roofs (aka ecoroofs or vegetated roofs) that are becoming increasingly common for both new and retrofit buildings. There is widespread recognition and a growing literature of measured data that suggest green roofs can reduce building energy consumption. Currently, however, there are few design tools available to assist developers and architects in assessing the likely magnitude of energy savings associated with various implementation options (e.g., soil type/depth, irrigation options, plant type). As a result there is a significant need for a quantitative and physically-based building energy simulation tool that represents the effects of green roof constructions. Such a tool would facilitate more rapid spread of green roof technologies and make it possible to account for green roof benefits in state energy codes and related energy efficiency standards such as LEED.
+
+In response to the need for green roof design tools a computational model of the heat transfer processes involved on a vegetated roof has been developed. This model accounts for:
+
+\begin{itemize}
+\item
+  long wave and short wave radiative exchange within the plant canopy,
+\item
+  plant canopy effects on convective heat transfer,
+\item
+  evapotranspiration from the soil and plants, and
+\item
+  heat conduction (and storage) in the soil layer
+\end{itemize}
+
+The ability to track moisture-dependent thermal properties is not implemented yet due to stability issues in the CTF scheme, but is under development for use with the finite difference solution scheme made available in EnergyPlus starting in version 2.
+
+As implemented in EnergyPlus the green roof module allows the user to specify ``ecoroof'' as the outer layer of a rooftop construction using a ``Material:RoofVegetation'' object. The user can then specify various aspects of the green roof construction including growing media depth, thermal properties, plant canopy density, plant height, stomatal conductance (ability to transpire moisture), and soil moisture conditions (including irrigation).
+
+The model formulation includes the following:
+
+\begin{itemize}
+\item
+  simplified moisture balance that allows precipitation, irrigation, and moisture transport between two soil layers (top and root zone).
+\item
+  soil and plant canopy energy balance based on the Army Corps of Engineers' FASST vegetation models (Frankenstein and Koenig), drawing heavily from BATS (Dickenson et al.) and SiB (Sellers et al.).
+\item
+  soil surface (T\(_{g}\)) and foliage (T\(_{f}\)) temperature equations are solved simultaneously each time step, inverting the CTF to extract heat flux information for the energy balance calculation.
+\end{itemize}
+
+The detailed energy balance analysis and resulting equations, being rather complicated, are summarized here. The interested reader is referred to the FASST documentation cited herein for the complete development. The end result is a set of two simultaneous equations for temperature---one for the soil surface and the other for the foliage.
+
+\subsection{Green Roof Model Description}\label{green-roof-model-description}
+
+As with a traditional roof, the energy balance of an green roof is dominated by radiative forcing from the sun. This solar radiation is balanced by sensible (convection) and latent (evaporative) heat flux from soil and plant surfaces combined with conduction of heat into the soil substrate. This energy balance is illustrated in Figure~\ref{fig:the-energy-balance-for-a-green-roof.}. The variables introduced in this figure are defined in the equations that follow.
+
+\begin{figure}[hbtp] % fig 35
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image509.png}
+\caption{The Energy Balance for a Green Roof. \protect \label{fig:the-energy-balance-for-a-green-roof.}}
+\end{figure}
+
+The energy budget analysis follows the Fast All Season Soil Strength (FASST) model developed by Frankenstein and Koenig for the US Army Corps of Engineers. FASST was developed, in part, to determine the ability of soils to support manned and unmanned vehicles and personnel movement. In order to accomplish this, however, FASST tracks the energy and moisture balance (including ice and snow) within a vegetated soil. It is a one-dimensional model that draws heavily from other plant canopy models including BATS (Dickinson et al.) and SiB (Sellers et al.). We have implemented FASST here with only a few modifications to adapt it for use with a relatively thin soil layer. The sign convention used assumes all heat fluxes are positive when energy is absorbed into the layer.
+
+In the following discussion this energy budget is divided into a budget for the foliage layer (F\(_{f}\)) and a budget for the ground surface (F\(_{g}\)­). The various parameterizations for latent and sensible heat flux are described in some detail and then the equation set is reduced to the simultaneous solution of two equations involving the temperatures of the foliage and ground surface.
+
+\subsubsection{Energy budget in the foliage layer}\label{energy-budget-in-the-foliage-layer}
+
+The foliage energy balance is given by:
+
+\begin{equation}
+{F_f} = {\sigma_f}\left[ {{I_S}^ \downarrow (1 - {\alpha_f}) + {\varepsilon_f}{I_{ir}}^ \downarrow  - {\varepsilon_f}\sigma {T_f}^4} \right] + \frac{{{\sigma_f}{\varepsilon_g}{\varepsilon_f}\sigma }}{{{\varepsilon_1}}}\left( {{T_g}^4 - {T_f}^4} \right) + {H_f} + {L_f}
+\end{equation}
+
+Where $\sigma$\(_{f}\) is calculated as a function of Leaf-Area-Index (LAI):
+
+\begin{equation}
+\sigma_f = 0.9 - 0.7 \exp{-0.75 LAI }
+\end{equation}
+
+In addition to convective and sensible heat transfer this equation accounts for both the short and longwave radiation absorbed by the vegetation, including the effects of multiple reflections. The sensible and latent heat flux terms (H\(_{f}\) and L\(_{f­}\)) are somewhat complicated and therefore discussed in some detail below.
+
+\paragraph{Sensible heat flux in the foliage layer}\label{sensible-heat-flux-in-the-foliage-layer}
+
+The sensible heat transfer between the leaf surface and near-canopy air (H\(_{f}\)) is influenced by the temperature difference between them, wind speed, and Leaf Area Index (LAI). The Leaf Area Index is the dimensionless ratio of the projected leaf area for a unit ground area (Oke). In contrast fractional vegetative cover (s\(_{f}\)) is the ratio of shaded ground surface to total ground surface area. The sensible heat flux is given by:
+
+\begin{equation}
+{H_f} = (1.1*LAI{\rho_{af}}{C_{p,a}}{C_f}{W_{af}})*({T_{af}} - {T_f})
+\end{equation}
+
+In this equation the constant 1.1 accounts for heat transfer from the stems, twigs and limbs (Deardorff). The properties of air near the foliage are modeled using the average from the foliage and instrument conditions:
+
+\begin{equation}
+{\rho_{af}} = 0.5({\rho_a} + {\rho_f})
+\end{equation}
+
+where r\(_{a}\) is the density of air at the instrument height ~and r\(_{f}\) is the density of air at the leaf temperature. The air temperature within the foliage is estimated by:
+
+\begin{equation}
+{T_{af}} = (1 - {\sigma_f})({T_a}) + {\sigma_f}\left( {0.3{T_a} + 0.6{T_f} + 0.1{T_g}} \right)
+\end{equation}
+
+\emph{where, T\(_{a}\)} is the air temperature at the instrument height in Kelvin \emph{T\(_{f}\)}, is leaf temperature in Kelvin and \emph{T\(_{g}\)}, is the ground surface temperature in Kelvin. The foliage wind speed is estimated as:
+
+\begin{equation}
+{W_{af}} = 0.83{\sigma_f}W\sqrt {C_{hn}^f}  + (1 - {\sigma_f})W
+\end{equation}
+
+Here \emph{W} is the larger of 2.0 m/s or the actual wind speed above the canopy (Hughes et al.) and C\(^{f}\)\(_{hn}\) is the transfer coefficient at near-neutral atmospheric stability conditions:
+
+\begin{equation}
+C_{hn}^f = {K_v}^2 \cdot {\left( {\ln \left( {\frac{{{Z_a} - {Z_d}}}{{Z_o^f}}} \right)} \right)^{ - 2}}
+\end{equation}
+
+where \emph{K\(_{v}\),} is von Karmen's constant (0.4), Z\(_{a}\) is the instrument height, Z\(_{d}\) is the zero displacement height in meters (height above soil within which the wind speed is effectively zero), and Z\(^{f}\)\(_{o}\) is the foliage roughness length scale (m). The formulations for zero displacement height, roughness length are based on Balick et al.:
+
+\begin{equation}
+{Z_d} = 0.701Z_{_f}^{0.979}
+\end{equation}
+
+\begin{equation}
+{Z_o} = 0.131Z_{_f}^{0.997}
+\end{equation}
+
+Finally, the bulk transfer coefficient as defined by Deardorff is given by:
+
+\begin{equation}
+{C_f} = 0.01*\left( {1 + \frac{{0.3(m/s)}}{{{W_{af}}(m/s)}}} \right)
+\end{equation}
+
+\paragraph{Latent heat flux in the foliage layer}\label{latent-heat-flux-in-the-foliage-layer}
+
+The process of water loss through plant respiration is known as transpiration. It is controlled by the closing and opening of stomata - the intercellular openings between to epidermal (guard) cells (Gates). The resistance to the diffusion of water vapor from these spaces into the atmosphere is called stomatal resistance. It depends on factors such as light intensity, soil moisture content and vapor pressure difference between inside leaf and the outside atmosphere. It is measured in units of s/m and is formulated as:
+
+\begin{equation}
+{r_s} = \frac{{{r_{s,\min }}}}{{LAI}} \cdot {f_1} \cdot {f_2} \cdot {f_3}
+\end{equation}
+
+Here, r\(_{s,min}\) is the minimum stomatal resistance. The actual stomatal resistance at any time is proportional to this minimum resistance and inversely proportional to LAI. The stomatal resistance is further modified by fractional multiplying factors that relate to incoming solar radiation and atmospheric moisture. As found in Frankenstein and Koenig the inverses of the multiplying factors f\(_{1}\), f\(_{2}\), and f\(_{3}\) are given by:
+
+\begin{equation}
+\begin{array}{l}
+   \frac{1}{f_1} = \min \left[ 1,\frac{{0.004*{I_s}^ \downarrow  + 0.005}}{{0.81*(0.004*{I_s}^ \downarrow  + 1)}} \right] \\
+   \frac{1}{f_2} = \left\{ 
+     \begin{array}{cl}
+       0                                                                 & \text{when} \; \theta_r > \overline \theta \\
+       \frac{ \overline \theta   - \theta_r }{ \theta_{max} - \theta_r } & \text{when} \; \theta_r \leq \overline \theta \leq \theta_{max}
+     \end{array} \right. \\
+   \frac{1}{f_3} = \exp \left[ - {g_d}({e_{f,sat}} - {e_a} \right]
+\end{array}
+\end{equation}
+
+Here, Q\(_{r}\), is the residual moisture content (defined as the amount of moisture in soil when plants begin to wilt), Q\(_{max}\) is the maximum moisture content (defined as the maximum amount of moisture a particular type of soil can hold and above which run off occurs), and \(\overline \Theta\) ~is the average soil moisture in the root zone. The residual moisture content is typically around 0.01 m\(^{3}\)/m\(^{3}\) (Frankenstein and Koenig). The maximum moisture content depends upon the soil, but generally varies from 0.3 to 0.6 m\(^{3}\)/m\(^{3}\) (Guymon et al.). In the expression for f\(_{3}\), g\(_{d}\) is a plant specific characteristic that is only non-zero for trees, e\(_{f,sat}\) is the saturated vapor pressure at the leaf temperature, and e\(_{a}\) is the air vapor pressure.
+
+Resistance to moisture exchange offered by the boundary layer formed on the leaf surface is known as aerodynamic resistance. It is measured in units of (s/m) and is influenced by wind speed, surface roughness and stability of the atmosphere (Oke). It is formulated as:
+
+\begin{equation}
+{r_a} = \frac{1}{{{c_f}{W_{af}}}}
+\end{equation}
+
+The combined effect of aerodynamic and stomatal resistances to vapor diffusion is integrated into a foliage surface wetness factor:
+
+\begin{equation}
+r'' = \frac{{{r_a}}}{{{r_a} + {r_s}}}
+\end{equation}
+
+This surface wetness factor is simply a ratio of the aerodynamic resistance to the total resistance. When the aerodynamic resistance is small the wetness factor approaches zero (leaf surfaces remain dry as surface moisture is readily evaporated). As the aerodynamic resistance increases in importance relative to stomatal resistance the wetness factor approaches 1.0 (moisture readily travels to the leaf surfaces, but is not easily evaporated).
+
+The latent heat flux is then given by:
+
+\begin{equation}
+{L_f} = {l_f} * LAI{\rho_{af}}{C_f}{W_{af}}{r^``}\left( {{q_{af}} - {q_{f,sat}}} \right)
+\end{equation}
+
+Here \emph{l\(_{f}\)} , is the latent heat of vaporization (J/kg), q\(_{f,sat}\) is the saturation mixing ratio at the leaf surface temperature, and q\(_{af}\) is the mixing ratio of the air within the canopy. As developed in Frankenstein and Koenig the mixing ratio within the canopy can be determined from:
+
+\begin{equation}
+{q_{af}} = \left[ {\frac{{\left( {1 - {\sigma_f}} \right){q_a} + {\sigma_f}\left( {0.3{q_a} + 0.6{q_{f,sat}}{r^``} + 0.1{q_{f,sat}}{M_g}} \right)}}{{1 - {\sigma_f}\left[ {0.6\left( {1 - {r^``}} \right) + 0.1\left( {1 - {M_g}} \right)} \right]}}} \right]
+\end{equation}
+
+where the factor \emph{M\(_{g}\)} ~(ranging from 0 to 1) is the ratio of volumetric moisture content to the porosity of the soil (Koenig). The latent heat of vaporization (\emph{l\(_{f}\)}) is the amount of energy required to convert a unit mass of water to vapor. It is measured in units of J/kg and is inversely proportional to the temperature. From Henderson-Sellers it is estimated as:
+
+\begin{equation}
+{l_f} = 1.91846*{10^6}{\left[ {\frac{{{T_f}}}{{{T_f} - 33.91}}} \right]^2}
+\end{equation}
+
+\subsubsection{Soil Energy budget}\label{soil-energy-budget}
+
+The energy budget at the soil surface is mainly influenced by the soil thermal properties, the amount of foliage coverage (s\(_{f}\)) and the amount of moisture in the soil. If the soil surface is densely covered the diurnal range of surface temperature is small. In the soil energy budget the heat released or gained due to phase changes of soil water, precipitation heat flux and heat flux due to vertical transport of water in the soil are ignored. Future refinements to this model will incorporate these phenomena. The sign convention followed here is the same as above (heat flux into the soil is positive). The overall energy balance at the soil surface (as given in Frankenstein and Koenig) is:
+
+\begin{equation}
+{F_g} = (1 - {\sigma_f})\left[ {I_s^ \downarrow (1 - {\alpha_g}) + {\varepsilon_g}I_{ir}^ \downarrow  - {\varepsilon_g}T_g^4} \right] - \frac{{{\sigma_f}{\varepsilon_g}{\varepsilon_f}\sigma }}{{{\varepsilon_1}}}\left( {T_g^4 - T_f^4} \right) + {H_g} + {L_g} + K*\frac{{\partial {T_g}}}{{\partial z}}
+\end{equation}
+
+As with the energy equation for the foliage this equation represents sensible heat flux (H\(_{g}\)), latent heat flux (L\(_{g}\)) and the multiple reflections associated with long and short wave radiation. The final term on the right side gives the conduction of heat into the soil substrate.
+
+\paragraph{Sensible heat flux in the soil layer}\label{sensible-heat-flux-in-the-soil-layer}
+
+Sensible heat flux between the soil surface and air in its vicinity is dependent on the temperature difference between them and the wind speed within the canopy. It is given as
+
+\begin{equation}
+{H_g} = {\rho_{ag}}{C_{p,a}}C_h^g{W_{af}}({T_{af}} - {T_g})
+\end{equation}
+
+where \(C_h^g\) ~is the bulk transfer coefficient and r\(_{ag}\) is the density of air near the soil surface (kg/m\(^{3}\)) given by:
+
+\begin{equation}
+{p_{ag}} = \frac{{{p_a} + {p_g}}}{2}
+\end{equation}
+
+Here r\(_{g}\) is the density of air at the ground surface temperature
+
+The bulk transfer coefficient is given as the linear combination of bulk transfer coefficient near ground (C\(^{f}\)\(_{hn}\)) and near foliage-atmosphere interface (C\(^{g}\)\(_{hn}\)) multiplied by the stability factor (G\(_{h}\)) and is formulated as:
+
+\begin{equation}
+C_h^g = {\Gamma_k}\left[ {\left( {1 - {\sigma_f}} \right)C_{hn}^g + {\sigma_f}C_{hn}^f} \right]
+\end{equation}
+
+The ground and foliage bulk transfer coefficients, in turn, are given by:
+
+\begin{equation}
+C_{hn}^g = r_{ch}^{ - 1}{\left[ {\frac{{{K_v}}}{{\ln \left( \frac{Z_a}{Z_o^g} \right)}}} \right]^2}
+\end{equation}
+
+And
+
+\begin{equation}
+C_{hn}^f = {\left[ {\frac{{K_v}}{{\ln \left( \frac{{Z_a} - {Z_d}}{Z_o^f} \right)}}} \right]^2}
+\end{equation}
+
+where\(Z_o^g\) ~and \(Z_o^f\) ~are the ground and foliage roughness lengths,~ r\(_{ch}\) is turbulent Schmidt number (0.63), and K\(_{v}\) is the von Karman constant (0.4).
+
+The condition of the atmosphere (G\(_{h}\)) is determined as stable or unstable based on the sign of the bulk Richardson number:
+
+\begin{equation}
+{R_{ib}} = \frac{{2g{Z_a}\left( {{T_{af}} - {T_g}} \right)}}{{\left( {{T_{af}} + {T_g}} \right)W_{af}^2}}
+\end{equation}
+
+The atmospheric stability factor is then given by Businger and Lumley and Panofsky as:
+
+\begin{equation}
+\Gamma_h = \left\{ 
+    \begin{array}{cl}
+      \frac{1.0}{\left( 1.0 - 16.0 R_{ib} \right)^{0.5}} & \text{for} \; R_{ib} < 0 \\
+      \frac{1.0}{\left( 1.0 - 5.0  R_{ib} \right)      } & \text{for} \; R_{ib} > 0
+    \end{array}
+  \right.
+\end{equation}
+
+\paragraph{Latent heat flux in the soil layer}\label{latent-heat-flux-in-the-soil-layer}
+
+Removal of water vapor from the soil surface depends on the difference between the mixing ratio of the soil surface and air and the wind speed within the canopy. The resulting latent heat flux is then given by:
+
+\begin{equation}
+{L_R} = C_e^g{l_g}{W_{af}}{\rho_{ag}}\left( {{q_{af}} - {q_g}} \right)
+\end{equation}
+
+Here\(C_e^g\) is the bulk transfer coefficient, l\(_{g}\) is the latent heat of vaporization at the ground surface temperature, q\(_{af}\) is the mixing ratio at the foliage-atmosphere interface, and q\(_{f}\) is the mixing ratio at the ground surface, given by:
+
+\begin{equation}
+{q_g} = {M_g}{q_{g,sat}} + \left( {1 - {M_g}} \right){q_{af}}
+\end{equation}
+
+The bulk transfer coefficient for latent heat exchange is analogous to that for sensible heat exchange and is given by:
+
+\begin{equation}
+C_e^g = {\Gamma_e}\left[ {\left( {1 - {\sigma_f}} \right)C_{en}^g + {\sigma_f}C_{hn}^f} \right]
+\end{equation}
+
+where \(C_{en}^g\) is the near ground bulk transfer coefficient for Latent heat flux and G\(_{e}\) is the latent heat exchange stability correction factor (assumed to be the same as G\(_{h}\)).
+
+\subsection{Linearization}\label{linearization}
+
+In order to solve the foliage and soil heat budget equations, the 4\(^{th}\) order terms T\(_{f}\)\(^{4}\) and T\(_{g}\)\(^{4}\) ~and mixing ratio terms q\(_{g,sat}\) and q\(_{f,sat}\) are linearized as given by Deardorff:
+
+\begin{equation}
+{\left[ {T_f^{\left( {n + 1} \right)}} \right]^4} = {\left[ {T_f^n} \right]^4} + 4{\left[ {T_f^n} \right]^3}\left[ {T_f^{n + 1} - T_f^n} \right]
+\end{equation}
+
+\begin{equation}
+{\left[ {T_g^{\left( {n + 1} \right)}} \right]^4} = {\left[ {T_g^n} \right]^4} + 4{\left[ {T_g^n} \right]^3}\left[ {T_g^{n + 1} - T_g^n} \right]
+\end{equation}
+
+Here T\(_{f}\)\(^{n+1}\) and T\(_{g}\)\(^{n+1}\) are the current time step leaf and ground surface temperatures in Kelvin. T\(_{f}\)\(^{n}\) and T\(_{g}\)\(^{n}\) are the corresponding temperatures at the previous time step.
+
+The saturation mixing ratio at the ground and leaf surface temperatures are given as:
+
+\begin{equation}
+{q_{g,sat}}\left( {T_g^{n + 1}} \right) = {q_{sat}}\left( {T_g^n} \right) + {\left( {\frac{{\partial {q_{sat}}}}{{\partial T}}} \right)_{T_g^n}} * \left( {T_g^{n + 1} - T_g^n} \right)
+\end{equation}
+
+\begin{equation}
+{q_{f,sat}}\left( {T_f^{n + 1}} \right) = {q_{sat}}\left( {T_f^n} \right) + {\left( {\frac{{\partial {q_{sat}}}}{{\partial T}}} \right)_{T_f^n}} * \left( {T_f^{n + 1} - T_f^n} \right)
+\end{equation}
+
+where q\(_{sat}\)(T\(_{g}\)\(^{n}\)) is the saturation mixing ratio at the previous time step and is formulated as given in Garratt:
+
+\begin{equation}
+{q_{sat}}\left( {T_g^n} \right) = \frac{{0.622{e^ * }\left( {T_g^n} \right)}}{{P - {e^ * }\left( {T_g^n} \right)}}
+\end{equation}
+
+Here the saturation vapor pressure e* (Pa) is evaluated at the ground temperature from the previous time step (T\(_{g}\)\(^{n}\)) as:
+
+\begin{equation}
+{e^*} = 611.2\exp \left[ {17.67\left( {\frac{{T_g^n - 273.15}}{{T_g^n - 29.65}}} \right)} \right]
+\end{equation}
+
+The derivative of saturation mixing ratio at the previous time step is given by:
+
+\begin{equation}
+\frac{{d{q^ * }}}{{dT_g^n}} = \left[ {\frac{{0.622 * P}}{{{{\left( {P - 0.378 * {e^ * }} \right)}^2}}}} \right]\left( {\frac{{d{e^ * }}}{{dT_g^n}}} \right)
+\end{equation}
+
+Here, the derivative of the saturation vapor pressure can be calculated from the Clausius-Clapeyron equation:
+
+\begin{equation}
+\frac{{d{e^ * }}}{{dT_g^n}} = \frac{{{l_g} * {e^ * }\left( {T_g^n} \right)}}{{\left( {{R_v} * {{\left( {T_g^n} \right)}^2}} \right)}}
+\end{equation}
+
+Where R\(_{v}\) is the gas constant for water vapor and l\(_{g}\) is the latent heat of vaporization at the soil surface temperature.
+
+The corresponding saturation mixing ratio relations for the leaf surfaces can be obtained by replacing T\(_{g}\) with T\(_{f}\) in the above relations.
+
+\subsection{Final Equations}\label{final-equations}
+
+After linearization the final equations are of the form:
+
+\begin{equation}
+C_1^f + C_2^f{T_g} + C_3^f{T_f} = 0
+\end{equation}
+
+\begin{equation}
+C_1^g + C_2^g{T_g} + C_3^g{T_f} = 0
+\end{equation}
+
+The coefficients in these equations result from the direct combination of the equations from the above development. The interested reader is directed to the papers by Frankenstein and Koenig for the complete and somewhat complicated expressions.
+
+This final set of equations is then solved simultaneously to obtain T\emph{\(_{g}\)} and T\emph{\(_{f}\)} . One key difference in our implementation of the FASST algorithm is that the conduction terms in the equations for \(C_1^g\) and \(C_2^g\) ~are solved by inverting the Conduction Transfer Functions (CTF) within the EnergyPlus solution scheme.
+
+\subsection{Green Roof Nomenclature}\label{green-roof-nomenclature}
+
+C\(_{1}\), C\(_{2}\), C\(_{3}\)~~~ = ~~~~~~~~~ coefficients in linearized temperature equations
+
+\emph{C\(_{e}\)\(^{g}\)~~~~~~~~~~~~~ = ~~~~~~~~~} latent heat flux bulk transfer coefficient at ground layer
+
+\emph{C\(_{f}\)~~ ~~~~~~~~~~~} = ~~~~~~~~~ bulk heat transfer coefficient
+
+C\(_{h}\)\(^{g}\)~~~~~~~~~~~~~ = ~~~~~~~~~ sensible heat flux bulk transfer coefficient at ground layer
+
+C\(_{hn}\)\(^{f}\) ~~~~~~~~~~~ = ~~~~~~~~~ near-neutral transfer coefficient at foliage layer
+
+C\(_{hn}\)\(^{g}\) = ~~~~~~~~~ near-neutral transfer coefficient at ground layer
+
+C\(_{p,a}\)~~~~~~~~~~~~ = ~~~~~~~~~ specific heat of air at constant pressure (1005.6 J/kg k)
+
+e\(^{*}\)~~~~~~~~~~~~~~~ = ~~~~~~~~~ saturation vapor pressure (Pa)
+
+f\(_{1}\)~~~~~~~~~~~~~~~ = ~~~~~~~~~ multiplying factor for radiation effect on stomatal resistance
+
+f\(_{2}\)~~~~~~~~~~~~~~~ = ~~~~~~~~~ multiplying factor for moisture effect on stomatal resistance
+
+f\(_{3}\)~~~~~~~~~~~~~~~ = ~~~~~~~~~ additional multiplying factor for stomatal resistance
+
+F\(_{f}\)~~~~~~~~~~~~~~~ = ~~~~~~~~~ net heat flux to foliage layer (W/m\(^{2}\))
+
+F\(_{g}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ net heat flux to ground surface (W/m\(^{2}\))
+
+g\(_{d}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ plant specific characteristic related to stomatal resistance
+
+H \emph{\(_{f}\)} ~~~~~~~~~~~~~ = ~~~~~~~~~ foliage sensible heat flux (W/m\(^{2}\))
+
+H\(_{g}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ ground sensible heat flux (W/m\(^{2}\))
+
+\(I_s^ \downarrow\) ~~~~~~~~~~~ = ~~~~~~~~~ total incoming short wave radiation (W/m\(^{2}\))
+
+\(I_{i\gamma }^ \downarrow\) ~~~~~~~~~~~~ = ~~~~~~~~~ total incoming longwave radiation (W/m\(^{2}\))
+
+K\(_{v}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ von Karmen constant (0.4)
+
+l\(_{f}\)~~~~~~~~~~~~~~~~ = ~~~~~~~~~ latent heat of vaporization at foliage temperature (J/kg)
+
+l\(_{g}\)~~~~~~~~~~~~~~~ = ~~~~~~~~~ latent heat of vaporization at ground temperature (J/kg)
+
+L\emph{\(_{f}\)}~ ~~~~~~~~~~~~~ = ~~~~~~~~~ foliage latent heat flux (W/m\(^{2}\))
+
+L\(_{g}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ ground latent heat flux (W/m\(^{2}\))
+
+\emph{LAI}~ ~~~~~~~~~~ = ~~~~~~~~~ leaf area index (m\(^{2}\)/m\(^{2}\))
+
+M\(_{g}\)~~~~~~~~~~~~~ = ~~~~~~~~~ moisture saturation factor
+
+q\(_{a}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ mixing ratio for air
+
+q\(_{af}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ mixing ratio for air within foliage canopy
+
+q\(_{f,sat}\)~~~~~~~~~~~~ = ~~~~~~~~~ saturation mixing ratio at foliage temperature
+
+q\(_{g,sat}\)~~~~~~~~~~~ = ~~~~~~~~~ saturation mixing ratio at ground temperature
+
+r\(_{a}\)~~~~~~~~~~~~~~~ = ~~~~~~~~~ aerodynamic resistance to transpiration (s/m)
+
+r\(_{s}\)~~~~~~~~~~~~~~~ = ~~~~~~~~~ foliage leaf stomatal resistance (s/m)
+
+r\(_{s,min}\)~~~~~~~~~~~ = ~~~~~~~~~ minimal leaf stomatal resistance (s/m)
+
+r''~~~~~~~~~~~~~~~ = ~~~~~~~~~ surface wetness factor
+
+R\(_{ib}\)~~~~~~~~~~~~~ = ~~~~~~~~~ bulk Richardson number
+
+R\(_{v}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ gas constant for water vapor (461.53 J/kgK)
+
+\emph{T\(_{a}\)} = ~~~~~~~~~ the air temperature at the instrument height (Kelvin)
+
+T\(_{af}\) ~ ~~~~~~~~~ = ~~~~~~~~~ air temperature with in the canopy (Kelvin)
+
+T\emph{\(_{f}\)}~~ ~~~~~~~~~~~ = ~~~~~~~~~ leaf temperature (Kelvin)
+
+T\(_{g}\) ~~~~~~~~~~~~~~ = ~~~~~~~~~ ground surface temperature (Kelvin)
+
+W~~~~~~~~~~~~~~ = ~~~~~~~~~ wind speed above canopy (m/s)
+
+W\(_{af}\)~ ~~~~~~~~~~~ = ~~~~~~~~~ wind speed with in the canopy (m/s)
+
+z~~~~~~~~~~~~~~~~ = ~~~~~~~~~ height or depth (m)
+
+Z\(_{a}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ instrument height (m)
+
+Z\(_{d}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ displacement height (m)
+
+Z\(_{o}\)\(^{f}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ foliage roughness length scale (m)
+
+\subsubsection{Greek letters}\label{greek-letters-000}
+
+\(\alpha\)\(_{f}\)~~~ ~~~~~~~~~~~ = ~~~~~~~~~ albedo (short wave reflectivity) of the canopy
+
+\(\alpha\)\(_{g}\)~~~~~~~~~~~~~~ = ~~~~~~~~~ albedo (short wave reflectivity) of ground surface
+
+\(\varepsilon\)\(_{1}\)~~~~~~~~~~~~~ = ~~~~~~~~~ \(\varepsilon\)\(_{g}\) + \(\varepsilon\)\(_{f}\)  - \(\varepsilon\)\(_{f}\)\(\varepsilon\)\(_{g}\)
+
+\(\varepsilon\)\(_{f}\) ~~~~~~~~~~~ = ~~~~~~~~~ emissivity of canopy 
+
+\(\varepsilon\)\(_{g}\) ~~~~~~~~~~~ = ~~~~~~~~~ emissivity of the ground surface
+
+\(\Gamma\)\(_{h}\)~~~~~~~~~~~~~~~~~~~ = ~~~~~~~~~~~~~stability factor
+
+\(\rho\)\(_{a}\)~ ~~~~~~~~~~~~ = ~~~~~~~~ density of air at instrument height (kg/m\(^{3}\))
+
+\(\rho\)\(_{f}\)~ ~~~~~~~~~~~~~ = ~~~~~~~~ density of air at foliage temperature (kg/m\(^{3}\))
+
+\(\rho\)\(_{f}\)~ ~~~~~~~~~~~~ = ~~~~~~~~ density of air at foliage temperature (kg/m\(^{3}\))
+
+\(\rho\)\(_{g}\)~~~~~~~~~~~~~ = ~~~~~~~~ density of air at ground surface temperature (kg/m\(^{3}\))
+
+\(\sigma\) ~ ~~~~~~~~~~~ = ~~~~~~~~~ the Stefan-Boltzmann constant (5.699*10\(^{8}\) W/m\(^{2}\) ºK\(^{4}\))
+
+\(\sigma\)\(_f\) ~~~~~~~~~~~ ~~~~~~~~~~~ = ~~~~~~~~~ fractional vegetation coverage
+
+\subsubsection{Subscripts and superscripts}\label{subscripts-and-superscripts-000}
+
+a~~~~~~~~~~~~~~~ = ~~~~~~~~~ air
+
+af~~~~~~~~~~~~~~ = ~~~~~~~~~ air within the foliage layer
+
+e~~~~~~~~~~~~~~~ = ~~~~~~~~~ latent heat flux term
+
+f~~~~~~~~~~~~~~~~ = ~~~~~~~~~ foliage surface
+
+g~~~~~~~~~~~~~~~ = ~~~~~~~~~ ground surface
+
+h~~~~~~~~~~~~~~~ = ~~~~~~~~~ sensible heat flux term
+
+n~~~~~~~~~~~~~~~ = ~~~~~~~~~ current time step
+
+n+1~~~~~~~~~~~~ = ~~~~~~~~~ future time step
+
+ir~~~~~~~~~~~~~~~ = ~~~~~~~~~ infrared (or long-wave)
+
+sat~~~~~~~~~~~~~ = ~~~~~~~~~ saturation value
+
+S~~~~~~~~~~~~~~~ = ~~~~~~~~~ short-wave
+
+\subsection{References}\label{references-025}
+
+ASHRAE. 2005. 2005 ASHRAE Handbook -- Fundamentals. Chapter 16, Air flow Around Buildings, Atlanta: American Society of Heating Refrigerating and Air-Conditioning Engineers, Inc.
+
+Balick, L. R., R. K. Scoggins, and L. E. Link. 1981. Inclusion of a simple vegetation layer in terrain temperature models for thermal IR signature prediction. IEEE Geoscience and Remote Sensing GE-19(3), pp.143-152.
+
+Businger, J. A. 1966. In `Arctic Heat Budget and Atmospheric Circulation', Symposium Proceedings, pp.~305-332. The Rand Corporation.
+
+Deardorff, J.W. 1978. ``Efficient Prediction of ground surface temperature and moisture with inclusion of a layer of vegetation'', Journal Geophysical Research, pp.~1889-1902.
+
+Dickinson, R.E., A. Henderson-Sellers, P.J. Kennedy, and M.F. Wilson. 1986. Biosphere-Atmosphere Transfer Scheme (BATS) for the NCAR community climate model. NCAR Technical Note, TN-275+STR.
+
+ECMWF. 2002. European Centre for Medium-Range Weather Forecasts, Integrated Forecast System. Documentation, CY25R1 (Operational implementation 9 April 2002). .
+
+Frankenstein, S., and G. Koenig. 2004.FASST Vegetation Models. U. S. Army Engineer Research and Development Center, Cold regions Research and Engineering Laboratory, ERDC/CRREL Technical Report TR-04-25.
+
+Frankenstein, S., and G. Koenig. 2004.Fast All-season Soil Strength (FASST). U.S. Army Engineer Research and Development Center, Cold regions Research and Engineering Laboratory, ERDC/CRREL Special Report SR-04-1.
+
+Garratt, J.R. 1992. The Atmospheric Boundary Layer, Cambridge university press.
+
+Gates, D.M. 1980. Biophysical Ecology. New York: Springer-Verlag
+
+Guymon, G.L., R.L. Berg, and T.V. Hromadka. 1993. Mathematical Model of Frost Heave and Thaw Settlement in Pavements. U.S. Army Cold Regions Research and Engineering Laboratory, CRREL Report 93-2.
+
+Henderson-Sellers, B. 1984. ``A New Formula for Latent Heat of Vaporization of water as function of temperature'', Quarterly Journal Royal Meteorological Society, 10 pp.~1186-1190.
+
+Hughes, P.A., T.J.L. McComb, A.B. Rimmer, and K.E. Turver. 1993. ``A mathematical model for the prediction of temperature of man-made and natural surfaces'', International Journal of Remote Sensing 14 (7), pp.~1383-1412.
+
+Koenig, G.G. 1994. Smart Weapons Operability Enhancement (SWOE) Joint Test and Evaluation (JT and E) Program: Final Report. Dr.~James P. Welch, Joint Test Director, SWOE JT and E, SWOE Report 94-10, Annex D.
+
+Lumley, J. L. and Panofsky, H. A. 1964. `The structure of Atmospheric Turbulence'. Interscience Monographs and Texts in Physics and Astronomy, Vol. XII. Wiley, New York.
+
+Oke, T.R. 1987. Boundary Layer Climates, University Press, Cambridge
+
+Sellers, P.J., Y. Mintz, Y.C. Sud, and A. Dalcher. 1986. A simple biosphere model (SiB) for use within general circulation models. Journal of Atmospheric Science, 43 (6), pp.~505-532.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-c.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-c.tex
new file mode 100644
index 00000000000..1bc154c72c4
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-c.tex
@@ -0,0 +1,152 @@
+\section{Ground Heat Transfer Calculations using C and F Factor Constructions}\label{ground-heat-transfer-calculations-using-c-and-f-factor-constructions}
+
+Building energy code and standards like ASHRAE 90.1, 90.2 and California Title 24 require the underground wall constructions and slabs-on-grade or underground floors not to exceed certain maximum values of C-factor and F-factor, which do not specify detailed layer-by-layer materials for the constructions. If using the normal approach (layer by layer) of ground constructions with EnergyPlus, users would need to create a pseudo wall or floor construction to match the thermal performance such as thermal mass effect and U-factor, and rely on the EnergyPlus Basement and Slabs tools to generate the monthly ground temperatures.
+
+A simplified approach is introduced to create equivalent constructions and model the ground heat transfer through underground walls and ground floors for the building energy code compliance calculations. The approach is to create constructions based on the user defined C or F factor with two layers: one concrete layer (0.15 m thick) with thermal mass, and one fictitious insulation layer with no thermal mass.
+
+\begin{itemize}
+\item
+  Three objects are used in the C and F factor calculations:
+\item
+  Construction:CfactorUndergroundWall
+\item
+  Construction:FfactorGroundFloor
+\end{itemize}
+
+Site:GroundTemperature:FCfactorMethod
+
+Site:GroundTemperature:FCfactorMethod is used only by the underground walls or slabs-on-grade or underground floors defined with C-factor (Construction:CfactorUndergroundWall) and F-factor (Construction:FfactorGroundFloor) method for code compliance calculations where detailed construction layers are unknown. Only one such ground temperature object can be included. The monthly ground temperatures for this object are close to the monthly outside air temperatures delayed by three months. If user does not input this object in the IDF file, it will be defaulted to the 0.5m set of monthly ground temperatures from the weather file if they are available.
+
+Detailed description of the three objects is in the Input Output Reference document. The following section describes how the equivalent material layers are created based on the C-factor and F-factor.
+
+\subsubsection{Slab-on-grade and Underground Floors Defined with F-factors}\label{slab-on-grade-and-underground-floors-defined-with-f-factors}
+
+The steady state heat transfer through the floor is calculated as,
+
+Q = Area * U\(_{eff}\) * (T\(_{air,out}\) -- T\(_{air,in}\)) = (T\(_{air,out}\) -- T\(_{air,in}\)) * (P\(_{exp}\) * F-factor)
+
+Where,
+
+Q is the steady state heat transfer through the floor in Watt
+
+Area is the area of the floor in m\(^{2}\)
+
+U\(_{eff}\) is the effective heat transfer coefficient including the floor construction, the soil, and the thermal resistance of the interior and exterior air films.
+
+T\(_{air,in}\) is the indoor air temperature in °C
+
+T\(_{air,out}\) is the outside air temperature in °C
+
+P\(_{exp}\) is the exposed perimeter of the floor in m
+
+F-Factor is the heat transfer through the floor, induced by a unit temperature difference between the outside and inside air temperature, on the per linear length of the exposed perimeter of the floor. The unit is W/m·K.
+
+Therefore,
+
+U\(_{eff}\) = (P\(_{exp}\) * F-factor) / Area
+
+1 / U\(_{eff}\) = R\(_{eff}\) + R\(_{film,in}\) + R\(_{film,out}\)
+
+R\(_{eff}\) = Area / (P\(_{exp}\) * F-factor) - R\(_{film,in}\) - R\(_{film,out}\)
+
+Where,
+
+R\(_{eff}\) is the effective thermal resistance in m\(^{2}\)·K/W, including the soil and the floor construction
+
+R\(_{film,in}\) and R\(_{film,out}\) are the air film resistance of the inside and outside surfaces, respectively.
+
+The outside air film resistance R\(_{film,out}\) = 0.03 m\(^{2}\)·K/W. The inside air film resistance R\(_{film,in}\) = 0.125 m\(^{2}\)·K/W, which is the average of the 0.14 m\(^{2}\)·K/W for heat flow up and 0.11 m\(^{2}\)·K/W for heat flow down.
+
+Approximate the thermal mass of the floor construction with a 6-inch (0.15 m) heavy concrete, and use a fictitious insulation layer with no thermal mass to match the thermal resistance of the construction.
+
+We have,
+
+R\(_{fic}\) = R\(_{eff}\) -- R\(_{con}\)
+
+Where,
+
+R\(_{fic}\) is the thermal resistance of the fictitious insulation layer in m\(^{2}\)·K/W.
+
+R\(_{con}\) is the thermal resistance of the concrete layer in m\(^{2}\)·K/W.
+
+Properties of the concrete layer are:
+
+Thickness = 0.15 m
+
+Conductivity = 1.95 W/m·K
+
+Density = 2240 kg/m\(^{3}\)
+
+Specific heat = 900 J/kg·K
+
+R\(_{con}\) = 0.15/1.95 = 0.077 m\(^{2}\)·K/W
+
+Finally,
+
+R\(_{fic}\) = R\(_{eff}\) -- 0.077
+
+\begin{figure}[hbtp] % fig 32
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image435.png}
+\caption{Schematic for Slab on Grade - Two Spaces \protect \label{fig:schematic-for-slab-on-grade-two-spaces}}
+\end{figure}
+
+For slabs-on-grade as shown in the figure above, the exposed perimeter is (2A + C) for the Dining area, and (2B + C) for the Kitchen area. For underground floors with no exposed perimeter, the R\(_{eff}\) can be assumed a big value such as 1000 hr·ft\(^{2}\)·°F/Btu (177 m\(^{2}\)·K/W).
+
+\textbf{\emph{Underground Walls Defined with C-Factors}}
+
+The steady state heat transfer through the underground wall is calculated as,
+
+Q = Area * U\(_{eff}\) * (T\(_{air,out}\) -- T\(_{air,in}\))
+
+1 / U\(_{eff}\) = R\(_{eff}\) + R\(_{film,out}\) + R\(_{film,in}\)
+
+Where,
+
+Q is the heat transfer through the wall in Watt
+
+Area is the area of the wall in m2
+
+U\(_{eff}\) is the effective heat transfer coefficient including the floor construction, the soil, and the thermal resistance of the interior and exterior air films.
+
+R\(_{eff}\) is the effective thermal resistance in m\(^{2}\)·K/W, including the soil and the wall construction
+
+R\(_{film,in}\) and R\(_{film,out}\) are the air film resistance of the inside and outside surfaces, respectively.
+
+C-factor is the time rate of steady-state heat flow through unit area of the construction, induced by a unit temperature difference between the body surfaces. The C-Factor unit is W/m\(^{2}\)·K. The C-factor does not include soil or air films.
+
+R\(_{eff}\) = 1/C-factor + R\(_{soil}\)
+
+R\(_{soil}\) is the effective R-value of the soil. Reference values from Table C6.10.1 of the SI version of the ASHRAE Standard 90.1-2010 are as follows:
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image436.png}
+\caption{Effective R-Value of Soil for Below-Grade Walls}
+\end{figure}
+
+A fairly good linear regression (R\(^{2}\) = 0.9967) for the above data is,
+
+R\(_{soil}\) = 0.0607 + 0.3479 * Depth
+
+Approximate the thermal mass of the wall construction with a 6-inch (0.15 m) heavy concrete, and use a fictitious insulation layer with no thermal mass to match the thermal resistance of the construction. Then we have the thermal resistance of the insulation layer,
+
+R\(_{fic}\) = R\(_{eff}\) -- R\(_{con}\)
+
+Where,
+
+R\(_{fic}\) is the thermal resistance of the fictitious insulation layer
+
+R\(_{con}\) is the thermal resistance of the concrete layer in m\(^{2}\)·K/W.
+
+Properties of the concrete layer are:
+
+Thickness = 0.15 m
+
+Conductivity = 1.95 W/m·K
+
+Density = 2240 kg/m\(^{3}\)
+
+Specific heat = 900 J/kg·K
+
+R\(_{con}\) = 0.15/1.95 = 0.077 m\(^{2}\)·K/W
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-site-001.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-site-001.tex
new file mode 100644
index 00000000000..68d2b27448f
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-site-001.tex
@@ -0,0 +1,39 @@
+\section{Ground Heat Transfer Calculations using Site:GroundDomain:Basement}\label{ground-heat-transfer-calculations-using-sitegrounddomainbasement}
+
+Basement heat transfer calculations are performed by the same model used by Site:GroundDomain:Slab to simulate zone-ground coupled surfaces. To simulate basements, the previous model is extended to situations where surfaces are below ground.
+
+\subsubsection{Approach}\label{approach-000}
+
+This model is generalized to be able to handle several basement surface and insulation configurations. An implicit finite difference formulation is used to solve for the ground temperatures. As a result the simulation is stable for all timesteps and grid sizes, but an iteration loop must be employed to converge the temperatures in the domain for each domain timestep.
+
+Multiple basement zones can be coupled to each basement domain object. The model determines which floor surfaces are coupled to the basement domain and creates a floor surface of equivalent surface area within the basement domain as a representation of the horizontal surfaces coupled to the domain. The user defined aspect ratio, which is the ratio of basement width to length, along with the total surface area of all surfaces connected to this basement floor will define the size and shape of the basement ground domain.
+
+Vertical basement depth below the ground surface of the domain is user specified. For situations when the ground surface is lower than the first above ground level a separate surface should be employed to bridge the space between the ground domain, and the first above-ground level.
+
+Basement wall and floor surfaces are created normally using the BuildingSurface:Detailed objects, with the outside boundary condition being the OtherSideConditionsModel used for the walls and floor of the basement domain. The interface between the basement walls and floors occurs at the outside surface of the walls and floor. Outside underground insulation is simulated by the ground domain, and therefore should not be included in the basement wall and floor construction objects.
+
+\subsubsection{Boundary Conditions}\label{boundary-conditions}
+
+At the zone interface surfaces, the average surface conduction heat flux from all surfaces connected to the ground domain is imposed as a boundary condition at the Surface/Domain interface cells. Far-field temperatures are applied as boundary temperature at the domain sides and lower surface. The ground temperature profile at the domain sides and lower surface are taken from Kusuda \& Achenbach 1965. The correlation requires annual ground surface temperature data. Ground surface temperature data can be determined by using the CalcSoilSurfTemp preprocessor; or, if the user has average monthly ground surface temperature data available, they can use the Site:GroundTemperature:Shallow object to provide the model monthly ground surface temperatures. From that, the model can then determine the ground temperature model parameters for the Kusuda \& Achenbach (1965) ground temperature model.
+
+Ground surface cells are treated as a heat balance, where long and short wave radiation, conduction, and convection are considered. Evapotranspiration is also considered. The evapotranspiration rate is calculated as a moisture loss by using the Allen et al. (2005) model, and translated into a heat loss by multiplication with the density and latent heat of evaporation of water. The evapotranspiration rate is dependent on the type of vegetation at the surface; the user can vary the surface vegetation from anywhere between a concrete surface and a fairly tall grass (about 7''). The model can be sensitive to variations in this parameter, especially in hot dry climates.
+
+Once the basement model has run, the updated cells with zone surface boundary conditions will update the OtherSideConditionsModel temperatures which are then used at the next timestep in the surface heat balance calculations.
+
+\subsubsection{Simulation Methodology}\label{simulation-methodology}
+
+The ground domain is updated at each zone timestep, or hourly as specified by the user. For situations when the ground domain is updated at each timestep, the domain is simulated by applying the surface heat flux boundary conditions from the previous timestep and calculating a new OthersideConditionsModel temperature. At this point, the surface heat balance algorithms can then take the new outside surface temperatures to update their surface heat fluxes. For situations when the user has elected to have the domain update on an hourly basis, the surface heat flux for each coupled surface is aggregated and passed to the domain as an average surface heat flux from the previous hour, which will then update the outside surface temperatures for the surface heat balance's next iteration.
+
+The basement floor and walls are simulated by standard surface heat balance models within EnergyPlus (CTF, finite difference). The horizontal and vertical insulation are simulated by the ground domain finite difference solver. This is shown in the \protect\hyperlink{BasementGHTFigure1}{Figure} below where the dotted red line defines the OtherSideConditionsModel interface separating the two solution domains. This methodology applies to the basement floor and walls.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image8000.png}
+\caption{Example surface construction.}
+\end{figure}
+
+References
+
+Kusuda, T. \& Achenbach, P. 1965. `Earth Temperature and Thermal Diffusivity at Selected Stations in the United States', ASHRAE Transactions 71(1): 61--75.
+
+Allen, R.G., Walter, I.A., Elliott, R.L., Howell, T.A., Itenfisu, D., Jensen, M.E., Snyder, R.L. 2005. The ASCE standardized reference evapotranspiration equation. Reston, VA: American Society of Civil Engineers.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-site.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-site.tex
new file mode 100644
index 00000000000..12d2430aa53
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/ground-heat-transfer-calculations-using-site.tex
@@ -0,0 +1,60 @@
+\section{Ground Heat Transfer Calculations using Site:GroundDomain:Slab}\label{ground-heat-transfer-calculations-using-sitegrounddomainslab}
+
+In order to simulate heat transfer with horizontal building surfaces in contact with the ground, a general finite difference ground model has been implemented. The model simulates heat transfer with the horizontal building surfaces through the ground domain. The domain can simulate heat transfer for slab-in-grade or slab-on-grade scenarios. In all scenarios, the ground domain must interact with the zone through an OthersideConditionsModel as the horizontal surface's outside boundary condition.
+
+\subsubsection{Approach}\label{approach-001}
+
+This model is generalized to be able to handle a number of different slab and insulation configurations.~ It uses an implicit finite difference formulation to solve for the ground temperatures. As a result the simulation is stable for all timesteps and grid sizes, but an iteration loop must be employed to converge the temperatures in the domain for each domain timestep.
+
+Multiple horizontal surfaces can be coupled to each ground domain object. The model determines which surfaces are coupled to the ground domain and creates a surface of equivalent surface area within the ground domain as a representation of the horizontal surfaces coupled to the ground domain. This surface then interacts with the ground providing updated other side conditions model temperatures to the coupled surfaces for use in their surface heat balance calculations.
+
+\subsubsection{Boudary Conditions}\label{boudary-conditions}
+
+At the interface surface, the average surface conduction heat flux from all surfaces connected to the ground domain is imposed as a GroundDomain boundary condition at the Surface/GroundDomain interface cells. Far-field temperatures are applied as boundary temperature at the GroundDomain sides and lower surface. The ground temperature profile at the domain sides and lower surface are taken from Kusuda \& Achenbach 1965. The correlation requires annual ground surface temperature data.
+
+Ground surface cells are treated as a heat balance, where long and short wave radiation, conduction, and convection are considered. Evapotranspiration is also considered. The evapotranspiration rate is calculated as a moisture loss by using the Allen et al. (2005) model, and translated into a heat loss by multiplication with the density and latent heat of evaporation of water. The evapotranspiration rate is dependent on the type of vegetation at the surface; the user can vary the surface vegetation from anywhere between a concrete surface and a fairly tall grass (about 7'').
+
+Once the ground model has run, the updated cells with zone surface boundary conditions will update the OtherSideConditionsModel temperatures which are the used at the next timestep in the surface heat balance calculations.
+
+\subsubsection{Simulation Methodology}\label{simulation-methodology-000}
+
+The ground domain is updated at each zone timestep, or hourly as specified by the user. For situations when the ground domain is updated at each timestep, the domain is simulated by applying the surface heat flux boundary conditions from the previous timestep and calculating a new OthersideConditionsModeltemperature. At this point, the surface heat balance algorithms can then take the new outside surface temperatures to update their surface heat fluxes. For situations when the user has elected to have the domain update on an hourly basis, the surface heat balance for each coupled surface is aggregated and passed to the domain as an average surface heat flux from the previous hour, which will then update the outside surface temperatures for the surface heat balance's next iteration.
+
+Both in-grade and on-grade scenarios are simulated with the GroundDomain object. The key difference being that for in-grade situations, the slab and horizontal insulation are simulated by the ground domain, whereas for the on-grade situations the slab and horizontal insulation must be included in the floor construction object. All possible insulation/slab configurations are seen in Table~\ref{table:possible-insulationslab-configurations-for}.
+
+% table 18
+\begin{longtable}[c]{@{}lllll@{}}
+\caption{Possible insulation/slab configurations for Site:GroundDomain model. \label{table:possible-insulationslab-configurations-for}} \tabularnewline
+\toprule 
+Situations & Vert. Ins. & Horiz Ins. (Full) & Horiz Ins. (Perim) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Possible insulation/slab configurations for Site:GroundDomain model.} \tabularnewline
+\toprule 
+Situations & Vert. Ins. & Horiz Ins. (Full) & Horiz Ins. (Perim) \tabularnewline
+\midrule
+\endhead
+
+In-Grade & 1 & X &  &  \tabularnewline
+2 & X & X &  \tabularnewline
+3 & X &  & X \tabularnewline
+4 &  &  &  \tabularnewline
+5 &  & X &  \tabularnewline
+6 &  &  & X \tabularnewline
+On-Grade & 7 & X &  &  \tabularnewline
+8* & X & X &  \tabularnewline
+9 &  &  &  \tabularnewline
+10* &  & X &  \tabularnewline
+\bottomrule
+\end{longtable}
+
+* Horizontal insulation must be included in the floor construction
+
+For the slab-in-grade scenarios, a thin surface layer must be included in the floor construction. This can be a very thin layer of the slab or other floor covering materials above the slab. This provides a zone boundary condition for the GroundDomain while still allowing 3-dimensional heat transfer effects to occur within the slab.
+
+\subsubsection{References}\label{references-026}
+
+Kusuda, T. \& Achenbach, P. 1965. Earth Temperature and Thermal Diffusivity at Selected Stations in the United States, ASHRAE Transactions 71(1): 61--75.
+
+Allen, R.G., Walter, I.A., Elliott, R.L., Howell, T.A., Itenfisu, D., Jensen, M.E., Snyder, R.L. 2005. The ASCE Standardized Reference Evapotranspiration Equation. Reston, VA: American Society of Civil Engineers.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/infrared-radiation-transfer-material.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/infrared-radiation-transfer-material.tex
new file mode 100644
index 00000000000..b077dd4e7a7
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/infrared-radiation-transfer-material.tex
@@ -0,0 +1,101 @@
+\section{Infrared Radiation Transfer Material}\label{infrared-radiation-transfer-material}
+
+One of the important technical features of EnergyPlus is that the fundamental zone model includes infrared (IR) radiation exchange among all surfaces within the zone. A zone can consist of a single room or multiple rooms having similar thermal characteristics. The other fundamental characteristic of a zone in EnergyPlus is that the air within the zone is modeled with the assumption that it is well-stirred, so it is characterized by a single uniform air temperature. Normally, this corresponds to the desired physical state of the air within a zone. Practically, this is accomplished with the mixing caused by the air distribution system or even with the addition of ceiling fans. However, there are situations where the well-stirred model condition does not fit the physical conditions within a space (e.g., large atria spaces, displacement ventilation systems, and under floor air distribution systems). In these cases, the air temperature varies spatially within the zone, but the surfaces in the regions that have different air temperatures still exchange IR radiation with the other surfaces in the zone, even those in regions having a different air temperature.
+
+Historically, several approaches have been taken to model such situations. They all involve unrealistically modifying the convective heat transfer characteristics within a single zone to produce reasonable total heat transfer for the zone while maintaining the zone IR radiation in its basic form. The IRT model takes a different, more fundamental approach. The space is divided into subzones, each having the basic well-stirred air model, but surfaces in these subzones are able to exchange IR radiation with other surfaces throughout the original space. Any convective air exchange between subzones is handled using the existing flexible capabilities within EnergyPlus. In other words, the subzones are standard EnergyPlus zones but they have been given the capability of allowing IR radiation to be exchanged with surfaces in adjacent zones.
+
+The IR radiation exchange is accomplished by introducing special IR Transparent (IRT) surfaces to link adjacent zones. These surfaces transmit the IR radiation incident on them to the surfaces in adjacent zone. The special surfaces have no thermal resistance, and they also have zero convective heat transfer coefficients on both sides. Consider a stratified atrium as an example. The atrium would be divided into stacked vertical zones, with each zone having the special IRT surface between it and the next lower zone. All physical surfaces in the two zones exchange radiation with the IRT surface, but it does not impede the transfer of radiation from one zone to the other. On each side it interacts as a black body surface and any radiation incident on it is absorbed. Since it has no other heat transfer mechanisms, it comes to equilibrium with zero net radiation transfer.
+
+Schematic diagrams of the application of the IRT surfaces are shown in Figure~\ref{fig:schematic-view-of-stacked-zones} and Figure~\ref{fig:schematic-model-of-a-ufad-zone}. The first figure shows it applied between two stacked zones that could be part of an atrium. All radiation incident on the IRT in the lower and upper zone is completely absorbed by the surface. It is prevented from participating in the zone air heat balance by fixing the heat transfer coefficients on either side at zero.
+
+\begin{figure}[hbtp] % fig 20
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image390.png}
+\caption{Schematic View of Stacked Zones \protect \label{fig:schematic-view-of-stacked-zones}}
+\end{figure}
+
+The same arrangement can be used for simulating a underfloor air distribution system (UFAD). The two zones represent the lower occupied (mixed) zone and the upper stratified zone. Since the upper zone is being modeled as a mixed EnergyPlus zone, it is not precisely the stratified zone concept. However, if a user has concern about having the entire upper part of the space at a single average temperature, the space could be modeled with two stacked upper zones. In that case the stratified temperature profile would be established by the relative size of the mixing from the convective plumes. The user would have to supply those estimates from external knowledge of the behavior of UFAD systems and plumes.
+
+\begin{figure}[hbtp] % fig 21
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image391.png}
+\caption{Schematic Model of a UFAD Zone \protect \label{fig:schematic-model-of-a-ufad-zone}}
+\end{figure}
+
+\subsection{Radiation Exchange Basics}\label{radiation-exchange-basics}
+
+The behavior of the IRT surface can be analyzed by considering three parallel black plates infinite in extent, as shown in Figure~\ref{fig:radiation-exchange-model}. The outside plates are held at two different temperatures, and the intermediate plate assumes an equilibrium temperature when the net heat flux goes to zero. All plates have black body surface characteristics.
+
+\begin{figure}[hbtp] % fig 22
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image392.png}
+\caption{Radiation Exchange Model \protect \label{fig:radiation-exchange-model}}
+\end{figure}
+
+The radiant exchange between surface 1 and 2 is:
+
+\begin{equation}
+{q_{1 - 2}} = \sigma A\left( {T_1^4 - T_2^4} \right)
+\end{equation}
+
+The exchange between surfaces 2 and 3 is:
+
+\begin{equation}
+{q_{2 - 3}} = \sigma A\left( {T_2^4 - T_3^4} \right)
+\end{equation}
+
+Equating heat fluxes and eliminating T\(_{2}\) gives:
+
+\begin{equation}
+{q_{1 - 3}} = \frac{\sigma }{2}A\left( {T_1^4 - T_3^4} \right)
+\end{equation}
+
+where:
+
+q is the heat flux in W/m\(^{2}\)
+
+$\sigma$ is the Stephan Boltzman constant
+
+A is the plate area in m\(^{2}\), and
+
+T is the temperature in K.
+
+Equation shows that the presence of a black body surface between a source and a sink reduces the heat flux by a factor of two. The same result occurs when the IRT surface is between two zones in EnergyPlus. In that case the adjacent zones behave as black body cavities at some equivalent temperature. In order to account for this reduction, the IRT area must be doubled. This can be done without any difficulty in the EnergyPlus radiant exchange routine because the radiation view factors are determined by an approximate procedure that is based on the areas of the surfaces. Thus, doubling the surface area of the IRT surface results in the correct transfer of radiation through the IRT surface. The doubling will occur automatically in the program as described in the Input Output Reference document.
+
+It should be noted that, because of the black body behavior of the IRT surface, any visible or solar short wavelength radiation incident on the surface will be absorbed and included with the long wavelength (IR) exchange with the adjacent zone. No energy will be lost, but zones with IRT surfaces should not be used in any lighting analyses.
+
+\subsection{Radiation Transfer Surface Details}\label{radiation-transfer-surface-details}
+
+\subsubsection{Specifying an Infrared Transparent (IRT) surface}\label{specifying-an-infrared-transparent-irt-surface}
+
+The Infrared Transparent (IRT) surface is similar to a resistance-only surface. The idd object for this type of surface is shown below. The fields indicate that the surface will actually participate in the transfer of visible and solar radiation by doing a wavelength transformation and making all short wavelength radiation that is incident on the surface into long wavelength radiation and having it participate in the long wavelength radiant exchange. The Material:InfraredTransparent object requires only a name. All other parameters are set internally.
+
+The Infrared Transparent surface should not participate in a convective/conductive exchange between the zones it separates. In order to minimize this effect, the SurfaceProperty:ConvectionCoefficients object must be used. Outside and Inside values for the surface's convection coefficients should be on the order of .1.~ Further examples are given in the Input Output Reference document.
+
+\subsection{Behavior Checks}\label{behavior-checks}
+
+The behavior of multi zones separated with infrared transparent surfaces can be checked with a simple comparison. Begin with a single zone model as shown below. This model has a south-facing window, and four walls exposed to wind and sun, and a roof exposed to wind and sun.
+
+\begin{figure}[hbtp] % fig 23
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image396.png}
+\caption{Single Zone Model \protect \label{fig:single-zone-model}}
+\end{figure}
+
+The single zone model will be compared with a stacked three zone model that has zones separated by interzone infrared transparent surfaces. This model is shown below.
+
+\begin{figure}[hbtp] % fig 24
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image397.png}
+\caption{Stacked Three Zone Model \protect \label{fig:stacked-three-zone-model}}
+\end{figure}
+
+The two upper zones have south facing windows whose total area is the same as the area of the single window in the single zone model. The top and the sides are again exposed to sun and wind. The separating surfaces are modeled as IRT surfaces. All zones in both models are controlled at the same setpoint temperature using purchased air.
+
+The sensible heating results are shown below. The results show the sum of the sensible cooling load for the three stacked zones and the single zone. It is clear that the IRT surfaces are very effective in transmitting infrared radiation between the zones. Some small differences, such as those shown, will occur because of the conversion from short wavelength solar to infrared through the special IRT dividing surfaces.
+
+\begin{figure}[hbtp] % fig 25
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image398.png}
+\caption{Comparison of Single and Three Stacked Zones \protect \label{fig:comparison-of-single-and-three-stacked-zones}}
+\end{figure}
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/inside-heat-balance.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/inside-heat-balance.tex
new file mode 100644
index 00000000000..38efaf60510
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/inside-heat-balance.tex
@@ -0,0 +1,903 @@
+\section{Inside Heat Balance}\label{inside-heat-balance}
+
+The heart of the heat balance method is the internal heat balance involving the inside faces of the zone surfaces.~ This heat balance is generally modeled with four coupled heat transfer components: 1) conduction through the building element, 2) convection to the air, 3) short wave radiation absorption and reflectance and 4) longwave radiant interchange.~ The incident short wave radiation is from the solar radiation entering the zone through windows and emittance from internal sources such as lights.~ The longwave radiation interchange includes the absorption and emittance of low temperature radiation sources, such as all other zone surfaces, equipment, and people.
+
+The heat balance on the inside face can be written as follows:
+
+\begin{equation}
+{q''_{LWX}} + {q''_{SW}} + {q''_{LWS}} + {q''_{ki}} + {q''_{sol}} + {q''_{conv}} = 0
+\end{equation}
+
+where:
+
+\({q''_{LWX}}\) = Net longwave radiant exchange flux between zone surfaces.
+
+\({q''_{SW}}\) ~ = Net short wave radiation flux to surface from lights.
+
+\({q''_{LWS}}\) = Longwave radiation flux from equipment in zone.
+
+\({q''_{ki}}\) ~ = Conduction flux through the wall.
+
+\({q''_{sol}}\) ~ = Transmitted solar radiation flux absorbed at surface.
+
+\({q''_{conv}}\) ~ = Convective heat flux to zone air.
+
+Each of these heat balance components is introduced briefly below.
+
+\begin{figure}[hbtp] % fig 19
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image301.png}
+\caption{Inside Heat Balance Control Volume Diagram \protect \label{fig:inside-heat-balance-control-volume-diagram}}
+\end{figure}
+
+\subsection{Internal Long-Wave Radiation Exchange}\label{internal-long-wave-radiation-exchange}
+
+\subsubsection{LW Radiation Exchange Among Zone Surfaces}\label{lw-radiation-exchange-among-zone-surfaces}
+
+There are two limiting cases for internal LW radiation exchange that are easily modeled:
+
+\begin{itemize}
+\item
+The zone air is completely transparent to LW radiation.
+\item
+The zone air completely absorbs LW radiation from the surfaces within the zone.
+\end{itemize}
+
+The limiting case of completely absorbing air has been used for load calculations and also in some energy analysis calculations.~ This model is attractive because it can be formulated simply using a combined radiation and convection heat transfer coefficient from each surface to the zone air.~ However, it oversimplifies the zone surface exchange problem, and as a result, the heat balance formulation in EnergyPlus treats air as completely transparent.~ This means that it does not participate in the LW radiation exchange among the surfaces in the zone. The model, which considers room air to be completely transparent, is reasonable physically because of the low water vapor concentrations and the short mean path lengths.~ It also permits separating the radiant and convective parts of the heat transfer at the surface, which is an important attribute of the heat balance method.
+
+EnergyPlus uses a grey interchange model for the longwave radiation among zone surfaces.~ This model is based on the ``ScriptF'' concept developed by Hottel (Hottel and Sarofim, Radiative Transfer, Chapter 3, McGraw Hill, 1967).~ This procedure relies on a matrix of exchange coefficients between pairs of surfaces that include all exchange paths between the surfaces.~ In other words all reflections, absorptions and re-emissions~ from other surfaces in the enclosure are included in the exchange coefficient, which is called ScriptF.~ The major assumptions are that all surface radiation properties are grey and all radiation is diffuse.~ Both assumptions are reasonable for building zone interchange.
+
+~The ScriptF coefficients are developed by starting with the traditional direct radiation view factors.~ In the case of building rooms and zones, there are several complicating factors in finding the direct view factors---the main one being that the location of surfaces such as thermal mass representing furniture and partitions are not known.~ The other limitation is that the exact calculation of direct view factors is computationally very intensive even if the positions of all surfaces are known. Accordingly, EnergyPlus uses a procedure to approximate the direct view factors.~ The procedure has two steps:
+
+1)~~~Determine the total area of other surfaces ``seen'' by a surface.
+
+2)~~~Approximate the direct view factor from surface 1 to surface 2 as the ratio of the area of surface 2 to the total area ``seen'' by surface 1.
+
+The determination of the ``seen'' area has several constraints:
+
+\begin{itemize}
+\item
+  No surface sees itself.
+\item
+  All surfaces see thermal mass surfaces.
+\item
+  No surface facing within 10 degrees of another surface is seen by the other surface.
+\item
+  All surfaces see roofs, floors and ceilings (subject to the preceding facing direction constraint).
+\end{itemize}
+
+Because the approximate view factors may not satisfy the basic requirements of reciprocity (two surfaces should exchange equal amounts of heat in each direction), and completeness (every surface should have a direct view factor sum of 1.0), EnergyPlus does a view factor fix operation before they are used in the ScriptF determination.~ Normally both of the requirements are satisfied, but in some special situations they are not, and special rules are applied.
+
+\begin{itemize}
+\item
+  If a user includes less than four surfaces in a zone, only reciprocity is enforced.
+\item
+  If the area of one surface in a zone is greater than the sum of the areas of all other surfaces, reciprocity only is enforced, but sometimes, for very large surfaces, that enforcement becomes impossible, and the view factors are modified so that only the large surface is seen by very small surfaces.
+\end{itemize}
+
+Warning messages are produced for both of these cases, and the results should be examined very carefully to ascertain that they are reasonable.~~ The suggested action for the second case (the extra-large surface) is to divide the large surface into several smaller surfaces; then the enclosure will be treated as normal.
+
+Once the ScriptF coefficients are determined, the longwave radiant exchange is calculated for each surface using:
+
+\begin{equation}
+{q_{i,j}} = {A_i}{F_{i,j}}\left( {T_i^4 - T_j^4} \right)
+\end{equation}
+
+where \textbf{\emph{F}}\(_{i,j}\) is the ScriptF between surfaces i and j.
+
+\subsubsection{Thermal Mass and Furniture}\label{thermal-mass-and-furniture}
+
+Furniture in a zone has the effect of increasing the amount of surface area that can participate in the radiation and convection heat exchanges.~ It also adds participating thermal mass to the zone.~ These two changes both affect the response to temperature changes in the zone and also affect the heat extraction characteristics.
+
+The proper modeling of furniture is an area that needs further research, but the heat balance formulation allows the effect to be modeled in a realistic manner by including the furniture surface area and thermal mass in the heat exchange process.
+
+\subsubsection{LW Radiation From Internal Sources}\label{lw-radiation-from-internal-sources}
+
+The traditional model for this source is to define a radiative/convective split for the heat introduced into a zone from equipment.~ The radiative part is then distributed over the surfaces within the zone in some prescribed manner.~ This, of course, is not a completely realistic model, and it departs from the heat balance principles. However, it is virtually impossible to treat this source in any more detail since the alternative would require knowledge of the placement and surface temperatures of all equipment.
+
+\subsection{Internal Short-Wave Radiation}\label{internal-short-wave-radiation}
+
+\subsubsection{SW Radiation from Lights}\label{sw-radiation-from-lights}
+
+The short wavelength radiation from lights is distributed over the surfaces in the zone in some prescribed manner.
+
+\subsubsection{Transmitted Solar}\label{transmitted-solar}
+
+Transmitted solar radiation is also distributed over the surfaces in the zone in a prescribed manner.~ It would be possible to calculate the actual position of beam solar radiation, but that would involve partial surface irradiation, which is inconsistent with the rest of the zone model that assumes uniform conditions over an entire surface.~ The current procedures incorporate a set of prescribed distributions.~ Since the heat balance approach can deal with any distribution function, it is possible to change the distribution function if it seems appropriate.
+
+\subsubsection{Convection to Zone Air}\label{convection-to-zone-air}
+
+The convection flux is calculated using the heat transfer coefficients as follows:
+
+\({q''_{conv}} = {h_c}({T_s} - {T_a})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ (89)
+
+The inside convection coefficients (\emph{h\(_{c}\)}) can be calculated using one of many different models.~ Currently the implementation uses coefficients based on correlations for natural, mixed, and forced convection.
+
+\subsection{Interior Conduction}\label{interior-conduction}
+
+This contribution to the inside surface heat balance is the wall conduction term, \({q''_{ki}}\) ~shown in Equation (30).~ This represents the heat transfer to the inside face of the building element. Again, a CTF formulation is used to determine this heat flux.
+
+\subsection{Interior Convection}\label{interior-convection}
+
+There are many different modeling options available in EnergyPlus for inside convection coefficients, \emph{h\(_{c}\)}.~ There are four different settings to direct how EnergyPlus managers select \emph{h\(_{c}\)} models during a simulation.~ There are numerous individual model equations for \emph{h\(_{c}\)} in EnergyPlus to cover different situations that arise from surface orientations, room airflow conditions, and heat flow direction.~ Additionally, in many cases multiple researchers have developed competing models for the same situations that differ and there is no way to declare one is better than another.~ An overall default for the simulation is selected in the ``SurfaceConvectionAlgorithm:Inside'' object and can be overridden by selecting a different option in a zone description.~ These models are explained in the following sections. In addition to the correlation choices described below, it is also possible to override the convection coefficients on the inside of any surface by using the ``SurfaceProperty:ConvectionCoefficients'' object in the input file to set the convection coefficient value on the inside of any surface. The values can be specified directly or with schedules. Specific details are given in the Input Output Reference document.
+
+\subsubsection{Adaptive Convection Algorithm}\label{adaptive-convection-algorithm}
+
+Beausoleil-Morrison (2000, 2002) developed a methodology for dynamically managing the selection of \emph{h\(_{c}\)} equations called \emph{adaptive convection algorithm}.~ The algorithm is used to select among the available \emph{h\(_{c}\)} equations for the one that is most appropriate for a given surface at a given time.~ As Beausoleil-Morrison notes, the adaptive convection algorithm is intended to be expanded and altered to reflect different classification schemes and/or new \emph{h\(_{c}\)} equations.~ The implementation in EnergyPlus has been modified from the original in the following ways:
+
+\begin{itemize}
+\item
+  An input mechanism is provided (see the \\
+SurfaceConvectionAlgorithm:Inside:AdapativeModelSelections object) so that the user can customize the specific selections of \emph{h\(_{c}\)} equations that are applied for different flow regimes and surface orientations.~ The changes apply in a general way to the entire model (but can be overridden by setting surface properties).
+\item
+  To avoid requiring additional user input on the position of ZoneHVAC-type equipment within a zone, there is no distinction between zones that have convective zone heater equipment located underneath the windows and those that have convective heaters located away from the windows.~ This applies to the air flow regime associated with convective zone heaters.~ Using Beausoleil-Morrison's terminology, regimes B1 and B2 are combined into just one B regime.
+\item
+  To avoid requiring additional user input on the position of ZoneHVAC-type equipment within a zone, there is no distinction between surfaces that are directly blown on the fan and those that are away from the fan for the air flow regime associated with mechanical circulation from a zone fan (ZoneHVAC type equipment).
+\item
+  The correlation for horizontal free jet developed by Fisher (1995) is not used.~ Ceiling diffuser models are used for all mechanical circulation from central air system.~ This decision was made for two reasons: (1) to avoid requiring additional user input on the position of, and momentum generated by, air terminal units, and (2) because Fisher (1995) found that the Coanda effect is so significant that in practice a free horizontal jet is difficult to maintain and mechanical-driven room airflows generally attach to surfaces and tend to match the flow regime of a ceiling diffuser much more often than a free jet.
+\item
+  EnergyPlus supports arbitrary geometry so surfaces can be tilted with respect to vertical or horizontal.~ Beausoleil-Morrison's adaptive convection algorithm was originally structured to use \emph{h\(_{c}\)} equations that have no functional dependence on surface tilt angle.~ However, tilted surfaces do perform differently than vertical or horizontal surface when buoyancy forces are significant.~ Therefore, the EnergyPlus implementation expands the structure of the algorithm to include additional categories for tilted surfaces.~ The \emph{h\(_{c}\)} equations developed by Walton (1983) are selected as the defaults for tilted surfaces because they have a functional dependence on tilt angle.
+\item
+  Fohanno and Polidari (2006) produced a new \emph{h\(_{c}\)} equation for vertical walls inside buildings with a simple buoyancy flow regime.~ They used a theoretical approach based on integral formalism and uniform heat flux (rather than uniform temperature) that covers both laminar and turbulent flow situations. ~In EnergyPlus, this model is selected as the default in place of the model by Alamdari and Hammond (1983) for vertical walls.
+\item
+  Karadag (2009) produced a new \emph{h\(_{c}\)} equation for ceiling surfaces that are actively chilled.~ He used computation fluid dynamics and various sized rooms and temperature conditions.~ In EnergyPlus, this model is selected as the default for surfaces that have active, in-ceiling cooling (in place of the model by Alamdari and Hammond (1983) for unstable ceilings).
+\item
+  International Standard Organization (ISO) completed Standard 15099-2003 which includes \emph{h\(_{c}\)} equations for the inside face of windows.~ EnergyPlus strives to adhere to formal modeling Standards where possible.~ Therefore the implementation includes a larger structure for the adaptive algorithm that includes additional categories for windows in all flow regimes and ISO 15099-2003 models are used as the default for windows in natural convection flow regimes.~ The ISO 15099 model applies to various tilt angles.
+\item
+  Goldstein and Novosalec (2010) produced new \emph{h\(_{c}\)} equations for forced air situations with ceiling slot diffusers along perimeters with significant glazing fractions.~ They used experiments with full-sized test room.~ These new equations are selected as the default for windows, ceilings and floors when there is an active central air system.
+\item
+  Interior mass surfaces are assigned the \emph{h\(_{c}\)} equation that would apply (stable or unstable) to a horizontal, upward facing surface for each flow regime.
+\item
+  The algorithm switches between forced, mixed, and natural flow regimes by calculating the Richardson number, Ri = Gr/Re\^{}2, for the zone.~ Large values of Ri indicate buoyancy dominates, while small values indicate forced flows dominate. To distinguish between opposing Zone unit type equipment (with fans) are assumed to force air up walls, and central air type equipment (with diffusers) are assumed to force air down walls.
+\end{itemize}
+
+The adaptive convection algorithm implemented in EnergyPlus for the inside face has a total of 45 different categories for surfaces and 29 different options for \emph{h\(_{c}\)} equation selections.~ The following table summarizes the categories and the default assignments for \emph{h\(_{c}\)} equations.~ The individual \emph{h\(_{c}\)} equations are documented below.
+
+{\scriptsize
+\begin{longtable}[c]{p{0.25in}p{1.25in}p{0.25in}p{1.5in}p{2.5in}}
+
+\caption{Inside Convection Categories and Assignments \label{table:table-13.-inside-convection-categories}} \tabularnewline
+\toprule 
+\# & Zone Air Flow Regime & IB-M's \# & Surface orientation and heat flow direction & Keywords for Applicable Model Equation Sources \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Inside Convection Categories and Assignments} \tabularnewline
+\toprule 
+\# & Zone Air Flow Regime & IB-M's \# & Surface orientation and heat flow direction & Keywords for Applicable Model Equation Sources \tabularnewline
+\midrule
+\endhead
+
+1  & & & Vertical Walls & FohannoPolidoriVerticalWall* \tabularnewline
+   & & & & AlamdariHammondVerticalWall \tabularnewline
+   & & & & ASHRAEVerticalWall \tabularnewline
+2  & & & Stable Horizontal & AlamdariHammondStableHorizontal* \tabularnewline
+   & & & & WaltonStableHorizontalOrTilt \tabularnewline
+3  & Simple Buoyancy & A3 & Unstable Horizontal & AlamdariHammondUnstableHorizontal* \tabularnewline
+   & & & & WaltonUnstableHorizontalOrTilt \tabularnewline
+4  & & & Stable Tilted & WaltonStableHorizontalOrTilt* \tabularnewline
+5  & & & Unstable Tilted & WaltonUnstableHorizontalOrTilt* \tabularnewline
+6  & & & Windows & ISO15099Windows* \tabularnewline
+\midrule
+7  & & & Vertical Walls & KhalifaEq3WallAwayFromHeat* \tabularnewline
+   & & & & FohannoPolidoriVerticalWall \tabularnewline
+   & & & & AlamdariHammondVerticalWall \tabularnewline
+   & & & & ASHRAEVerticalWall \tabularnewline
+8  & & & Stable Horizontal & AlamdariHammondStableHorizontal* \tabularnewline
+   & & & & WaltonStableHorizontalOrTilt \tabularnewline
+9  & In-floor Heating or In-ceiling Cooling & A1 & Unstable Horizontal & KhalifaEq4CeilingAwayFromHeat* \tabularnewline
+   & & & & AlamdariHammondUnstableHorizontal \tabularnewline
+   & & & & WaltonUnstableHorizontalOrTilt \tabularnewline
+10 & & & Heated Floor & AwbiHattonHeatedFloor* \tabularnewline
+ & & & & WaltonUnstableHorizontalOrTilt \tabularnewline
+ & & & & AlamdariHammondUnstableHorizontal \tabularnewline
+11 & & & Chilled Ceiling & KaradagChilledCeiling* \tabularnewline
+ & & & & WaltonUnstableHorizontalOrTilt \tabularnewline
+12 & & & Stable Tilted & WaltonStableHorizontalOrTilt* \tabularnewline
+13 & & & Unstable Tilted & WaltonUnstableHorizontalOrTilt* \tabularnewline
+14 & & & Windows & ISO15099Windows* \tabularnewline
+\midrule
+15 & & & Vertical Walls (non-heated) & KhalifaEq6NonHeatedWalls* \tabularnewline
+ & & & & FohannoPolidoriVerticalWall \tabularnewline
+ & & & & ASHRAEVerticalWall \tabularnewline
+16 & & & Heated Wall & AwbiHattonHeatedWall* \tabularnewline
+17 & Wall Panel Heating & A2 & Stable Horizontal & AlamdariHammondStableHorizontal* \tabularnewline
+ & & & & WaltonStableHorizontalOrTilt \tabularnewline
+18 & & & Unstable Horizontal & KhalifaEq7Ceiling* \tabularnewline
+ & & & & AlamdariHammondUnstableHorizontal \tabularnewline
+ & & & & WaltonUnstableHorizontalOrTilt \tabularnewline
+19 & & & Stable Tilted & WaltonStableHorizontalOrTilt* \tabularnewline
+20 & & & Unstable Tilted & WaltonUnstableHorizontalOrTilt* \tabularnewline
+21 & & & Windows & ISO15099Windows* \tabularnewline
+\midrule
+22 & & & Vertical Walls not near heater & FohannoPolidoriVerticalWall* \tabularnewline
+ & & & & KhalifaEq6NonHeatedWalls \tabularnewline
+ & & & & KhalifaEq3WallAwayFromHeat \tabularnewline
+ & & & & AlamdariHammondVerticalWall \tabularnewline
+ & & & & ASHRAEVerticalWall \tabularnewline
+23 & & & Vertical Walls near heater & KhalifaEq5WallNearHeat* \tabularnewline
+24 & Convective Zone Heater & B & Stable Horizontal & AlamdariHammondStableHorizontal* \tabularnewline
+ & & & & WaltonStableHorizontalOrTilt \tabularnewline
+25 & & & Unstable Horizontal & KhalifaEq7Ceiling* \tabularnewline
+ & & & & KhalifaEq4CeilingAwayFromHeat \tabularnewline
+ & & & & WaltonUnstableHorizontalOrTilt \tabularnewline
+26 & & & Stable Tilted & WaltonStableHorizontalOrTilt* \tabularnewline
+27 & & & Unstable Tilted & WaltonUnstableHorizontalOrTilt* \tabularnewline
+28 & & & Windows & ISO15099Windows* \tabularnewline
+\midrule
+29 & & & Walls & GoldsteinNovoselacCeilingDiffuserWalls* \tabularnewline
+ & & & & FisherPedersenCeilingDiffuserWalls \tabularnewline
+30 & & & Ceiling & FisherPedersenCeilingDiffuserCeiling* \tabularnewline
+31 & Mechanical Central Air Diffuser & C & Floor & GoldsteinNovoselacCeilingDiffuserFloor* \tabularnewline
+ & & & & FisherPedersenCeilingDiffuserFloor \tabularnewline
+32 & & & Windows & GoldsteinNovoselacCeilingDiffuserWindow* \tabularnewline
+ & & & & ISO15099Windows \tabularnewline
+\midrule
+33 & & & Walls & KhalifaEq3WallAwayFromHeat * \tabularnewline
+34 & & & Stable Horizontal & AlamdariHammondStableHorizontal* \tabularnewline
+ & & & & WaltonStableHorizontalOrTilt \tabularnewline
+35 & Mechanical Zone Fan Circulation & D & Unstable Horizontal & KhalifaEq4CeilingAwayFromHeat* \tabularnewline
+ & & & & WaltonUnstableHorizontalOrTilt \tabularnewline
+36 & & & Stable Tilted & WaltonStableHorizontalOrTilt* \tabularnewline
+37 & & & Unstable Tilted & WaltonUnstableHorizontalOrTilt* \tabularnewline
+38 & & & Windows & GoldsteinNovoselacCeilingDiffuserWindow* \tabularnewline
+ & & & & ISO15099Windows \tabularnewline
+\midrule
+39 & & & Assisting Flow Walls & BeausoleilMorrisonMixedAssistedWall* \tabularnewline
+40 & & & Opposing Flow Walls & BeausoleilMorrisonMixedOpposingWall* \tabularnewline
+41 & & & Stable Floor & BeausoleilMorrisonMixedStableFloor* \tabularnewline
+42 & Mixed & E & Unstable Floor & BeausoleilMorrisonMixedUnstableFloor* \tabularnewline
+43 & & & Stable Ceiling & BeausoleilMorrisonMixedStableCeiling* \tabularnewline
+44 & & & Unstable Ceiling & BeausoleilMorrisonMixedUnstableCeiling* \tabularnewline
+45 & & & Windows & GoldsteinNovoselacCeilingDiffuserWindow* \tabularnewline
+ & & & & ISO15099Windows \tabularnewline
+\bottomrule
+\end{longtable}}
+
+*Indicates the default selection for \emph{h\(_{c}\)} model equation.
+
+\subsubsection{Inside Face Surface Classification}\label{inside-face-surface-classification}
+
+The adaptive convection algorithm is based on classifying surfaces by flow regime and orientation so that the correct \emph{h\(_{c}\)} equation can be chosen at a particular point in time during the simulation.~ The classification depends on user input with some aspects processed only once at the beginning and others during each timestep.~ There are also various parameters or inputs to the \emph{h\(_{c}\)} equations that need static or dynamic processing.
+
+For each surface, it and the zone it is attached to are processed for the following static characteristics.
+
+\begin{itemize}
+\item
+  Characteristic height for convection is taken as the zone height.
+\item
+  Surfaces listed as receiving heat from Zone HVAC equipment with radiative models are considered ``near'' the heater.
+\item
+  Zones are examined for low temperature radiant systems.~ The surfaces that contain the active elements are examined and the zone characterized to know if it has in-floor heating, in-ceiling cooling, or in-wall heating.
+\item
+  A hydraulic diameter is calculated for horizontal surfaces for the entire zone.
+\end{itemize}
+
+and calculating various parameters needed by \emph{h\(_{c}\)} equations.~ Selecting flow regime is done in the following manner.~ For each surface, we examine the zone on the inside face for the following:
+
+\begin{itemize}
+\item
+  HVAC system type
+\item
+  HVAC operating status
+\item
+  HVAC system ACH
+\end{itemize}
+
+The surfaces are evaluated to determine:
+
+\begin{itemize}
+\item
+  Surface classification: Floor, wall, roof, window, types
+\item
+  Tilt angle
+\item
+  Convective stability (sign of ΔT)
+\end{itemize}
+
+The individual \emph{h\(_{c}\)} model equations and their respective references are listed in next by the keyword used to identify them.
+
+\subsubsection{ASHRAE Vertical Wall}\label{ashrae-vertical-wall}
+
+Walton adopted the following equation for natural convection from ASHRAE .
+
+\begin{equation}
+h = 1.31{\left| {\Delta T} \right|^{\frac{1}{3}}}
+\end{equation}
+
+This is usually bound at a minimum of .1 in EnergyPlus. This is a component of the TARP overall algorithm described below.
+
+\subsubsection{Walton Unstable Horizontal Or Tilt}\label{walton-unstable-horizontal-or-tilt}
+
+Walton (11983) developed the following equation by fitting curves from various sources.
+
+\begin{equation}
+h = \frac{{9.482{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{7.283 - \left| {\cos \Sigma } \right|}}
+\end{equation}
+
+Unstable refers to the direction of heat flow and the associated buoyancy relative to the surfaces. Unstable is when the natural tendency is to enhance flow in the sense that rising warmer air, or falling cooler air, is free to move away from the surface. This is usually bound at a minimum of .1 in EnergyPlus. This is a component of the TARP overall algorithm described below.
+
+\subsubsection{Walton Stable Horizontal Or Tilt}\label{walton-stable-horizontal-or-tilt}
+
+Walton (11983) developed the following equation by fitting curves from various sources.
+
+\begin{equation}
+h = \frac{{1.810{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{1.382 + \left| {\cos \Sigma } \right|}}
+\end{equation}
+
+Stable refers to the direction of heat flow and the associated buoyancy relative to the surfaces. Stable is when the natural tendency is to retard flow in the sense that rising warmer air, or falling cooler air, is driven against the surface. This is usually bound at a minimum of .1 in EnergyPlus. This is a component of the TARP overall algorithm described below.
+
+\subsubsection{Fisher Pedersen Ceiling Diffuser Walls}\label{fisher-pedersen-ceiling-diffuser-walls}
+
+Fisher and Pedersen 1997) developed the following equation from laboratory chamber measurements.
+
+\begin{equation}
+h = 1.208 + 1.012 * AC{H^{0.604}}
+\end{equation}
+
+This is a component of the CeilingDiffuser overall algorithm described below.
+
+\subsubsection{Fisher Pedersen Ceiling Diffuser Ceiling}\label{fisher-pedersen-ceiling-diffuser-ceiling}
+
+Fisher and Pedersen (1997) developed the following equation from laboratory chamber measurements.
+
+\begin{equation}
+h = 2.234 + 4.099 * AC{H^{0.503}}
+\end{equation}
+
+This is a component of the CeilingDiffuser overall algorithm described below.
+
+\subsubsection{Fisher Pedersen Ceiling Diffuser Floor}\label{fisher-pedersen-ceiling-diffuser-floor}
+
+Fisher and Pedersen 1997) developed the following equation from laboratory chamber measurements.
+
+\begin{equation}
+h = 3.873 + 0.082 * AC{H^{0.98}}
+\end{equation}
+
+This is a component of the CeilingDiffuser overall algorithm described below.
+
+\subsubsection{Alamdari Hammond Stable Horizontal}\label{alamdari-hammond-stable-horizontal}
+
+Alamdari and Hammond (1983) developed the following correlation for horizontal surfaces in stable thermal situation.
+
+\begin{equation}
+h = 0.6{\left( {\frac{{\left| {\Delta T} \right|}}{{D_h^2}}} \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{5}}}}
+\end{equation}
+
+where,
+
+\({D_h} = \frac{{4A}}{P}\) , hydraulic diameter of horizontal surface, \emph{A} is area (m\(^{2}\)) and \emph{P} is the perimeter (m) of the entire zone.
+
+\subsubsection{Alamdari Hammond Unstable Horizontal}\label{alamdari-hammond-unstable-horizontal}
+
+Alamdari and Hammond (1983) developed the following correlation for horizontal surfaces in a buoyant thermal situation.
+
+\begin{equation}
+h = {\left\{ {{{\left[ {1.4{{\left( {\frac{{\left| {\Delta T} \right|}}{{{D_h}}}} \right)}^{^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{4}}}}}} \right]}^6} + {{\left[ {1.63{{\left| {\Delta T} \right|}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}}} \right]}^6}} \right\}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 6}}\right.}\!\lower0.7ex\hbox{6}}}}
+\end{equation}
+
+\subsubsection{Alamdari Hammond Vertical Wall}\label{alamdari-hammond-vertical-wall}
+
+Alamdari and Hammond (1983) developed the following correlation for vertical surfaces.
+
+\begin{equation}
+h = {\left\{ {{{\left[ {1.5{{\left( {\frac{{\left| {\Delta T} \right|}}{H}} \right)}^{^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{4}}}}}} \right]}^6} + {{\left[ {1.23{{\left| {\Delta T} \right|}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}}} \right]}^6}} \right\}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 6}}\right.}\!\lower0.7ex\hbox{6}}}}
+\end{equation}
+
+where,
+
+~~~~~ \emph{H} is the characteristic height for the surface.~ In EnergyPlus this is the zone's ceiling height (which could be larger than the height of an individual surface when wall are subdivided into more than one surface).
+
+\subsubsection{Khalifa Eq3 Wall Away From Heat}\label{khalifa-eq3-wall-away-from-heat}
+
+Khalifa (1989) conducted experiments with test chambers and developed correlations for certain types of surfaces.~ One of them, identified as ``Equation 3'' in original reference, is for convectively heated zones and applies to the inside surfaces of walls away from the heat source:
+
+\begin{equation}
+h = 2.07{\left| {\Delta T} \right|^{0.23}}
+\end{equation}
+
+\subsubsection{Khalifa Eq4 Ceiling Away From Heat}\label{khalifa-eq4-ceiling-away-from-heat}
+
+Khalifa (1989) conducted experiments with test chambers and developed correlations for certain types of surfaces.~ One of them, identified as ``Equation 4'' in original reference, is for convectively heated zones and applies to the inside surfaces of ceilings away from the heat source:
+
+\begin{equation}
+h = 2.72{\left| {\Delta T} \right|^{0.13}}
+\end{equation}
+
+\subsubsection{Khalifa Eq5 Wall Near Heat}\label{khalifa-eq5-wall-near-heat}
+
+Khalifa (1989) conducted experiments with test chambers and developed correlations for certain types of surfaces.~ One of them, identified as ``Equation 5'' in original reference, is for convectively heated zones and applies to the inside surfaces of walls near the heat source:
+
+\begin{equation}
+h = 1.98{\left| {\Delta T} \right|^{0.32}}
+\end{equation}
+
+\subsubsection{Khalifa Eq6 Non Heated Walls}\label{khalifa-eq6-non-heated-walls}
+
+Khalifa (1989) conducted experiments with test chambers and developed correlations for certain types of surfaces.~ One of them, identified as ``Equation 6'' in original reference, is for heated zones and applies to the inside surfaces of walls that are not heated:
+
+\begin{equation}
+h = 2.30{\left| {\Delta T} \right|^{0.24}}
+\end{equation}
+
+\subsubsection{Khalifa Eq7 Ceiling}\label{khalifa-eq7-ceiling}
+
+Khalifa (1989) conducted experiments with test chambers and developed correlations for certain types of surfaces.~ One of them, identified as ``Equation 7'' in original reference, is for heated zones and applies to the inside surfaces of ceilings:
+
+\begin{equation}
+h = 3.10{\left| {\Delta T} \right|^{0.17}}
+\end{equation}
+
+\subsubsection{Awbi Hatton Heated Floor}\label{awbi-hatton-heated-floor}
+
+Awbi and Hatton (1999) conducted laboratory measurements using environmental chambers and developed the following correlation for floor surfaces that are being actively heated.
+
+\begin{equation}
+h = \frac{{2.175{{\left| {\Delta T} \right|}^{0.308}}}}{{D_h^{0.076}}}
+\end{equation}
+
+where,
+
+\({D_h} = \frac{{4A}}{P}\), hydraulic diameter of horizontal surface, \emph{A} is area (m\(^{2}\)) and \emph{P} is the perimeter (m) of the entire zone (all of the adjacent floor surfaces if more than one in the zone).
+
+\subsubsection{Awbi Hatton Heated Wall}\label{awbi-hatton-heated-wall}
+
+Awbi and Hatton (1999) developed the following correlation for wall surfaces that are being actively heated.
+
+\begin{equation}
+h = \frac{{1.823{{\left| {\Delta T} \right|}^{0.293}}}}{{D_h^{0.076}}}
+\end{equation}
+
+where,
+
+\({D_h} = \frac{{4A}}{P}\), hydraulic diameter of wall surface, \emph{A} is area (m\(^{2}\)) and \emph{P} is the perimeter (m) of the entire wall (all of the adjacent wall surfaces if more than one along the wall).
+
+\subsubsection{Beausoleil Morrison Mixed Assisted Wall}\label{beausoleil-morrison-mixed-assisted-wall}
+
+Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for walls where the flow driving forces from mechanical forces are augmented by the driving forces from buoyancy.
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+h = \left( 
+\left\{
+\left[1.5\left(\frac{\left|\Delta T\right|}{H}\right)^{1/4}\right]^6 +
+\left[1.23\left|\Delta T\right|^2\right]^{1/6}
+\right\}^{1/2} + 
+\left\{
+\left[\frac{T_{surf}-T_{SAT}}{\left|\Delta T\right|}\right]
+\left[-0.199+0.190\cdot ACH^{0.8}\right]
+\right\}^3
+\right)^{1/3}
+\end{equation}
+
+where,
+
+~~~~~ \emph{T\(_{SAT}\)} is the supply air temperature at the diffuser.
+
+Here the reference temperature is the zone air temperature rather than the diffuser supply air temperature.
+
+\subsubsection{Beausoleil Morrison Mixed Opposing Wall}\label{beausoleil-morrison-mixed-opposing-wall}
+
+Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for walls where the flow driving forces from mechanical forces are opposed by the driving forces from buoyancy.
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+h = \max \left\{
+\begin{array}{l}
+\left(\left\{\left[1.5\left(\frac{\left|\Delta T\right|}{H}\right)^{1/4}\right]^6+\left[1.23\left|\Delta T\right|^2\right]^{1/6}\right\}^{1/2}-\left\{\left[\frac{T_{surf}-T_{SAT}}{\left|\Delta T\right|}\right]\cdot\left[-0.199+0.190\cdot ACH^{0.8}\right]\right\}^3\right)^{1/3} \\
+0.8\cdot \left\{\left[1.5\left(\frac{\left|\Delta T\right|}{H}\right)^{1/4}\right]^6+\left[1.23\left|\Delta T\right|^2\right]\right\}^{1/6} \\
+0.8\cdot \left\{\left[\frac{T_{surf}-T_{SAT}}{\left|\Delta T\right|}\right]\cdot\left[-0.199+0.190\cdot ACH^{0.8}\right]\right\}
+\end{array}
+\right.
+\end{equation}
+
+\subsubsection{Beausoleil Morrison Mixed Stable Floor}\label{beausoleil-morrison-mixed-stable-floor}
+
+Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for floors where the flow driving forces include both mechanical forces and thermally stable buoyancy.
+
+\begin{equation}
+h = {\left( {{{\left\{ {0.6 \cdot {{\left( {\frac{{\left| {\Delta T} \right|}}{{{D_H}}}} \right)}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{5}}}}} \right\}}^3} + {{\left\{ {\left[ {\frac{{{T_{surf}} - {T_{SAT}}}}{{\left| {\Delta T} \right|}}} \right]\cdot\left[ {0.159 + 0.116AC{H^{0.8}}} \right]} \right\}}^3}} \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}}
+\end{equation}
+
+\subsubsection{Beausoleil Morrison Mixed Unstable Floor}\label{beausoleil-morrison-mixed-unstable-floor}
+
+Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for floors where the flow driving forces include both mechanical forces and thermally unstable buoyancy.
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+h = {\left( {{{\left\{ {{{\left[ {1.4{{\left( {\frac{{\left| {\Delta T} \right|}}{{{D_h}}}} \right)}^{^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{4}}}}}} \right]}^6} + {{\left[ {1.63{{\left| {\Delta T} \right|}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}}} \right]}^6}} \right\}}^{{\raise0.7ex\hbox{3} \!\mathord{\left/ {\vphantom {3 6}}\right.}\!\lower0.7ex\hbox{6}}}} + {{\left\{ {\left[ {\frac{{{T_{surf}} - {T_{SAT}}}}{{\left| {\Delta T} \right|}}} \right]\cdot\left[ {0.159 + 0.116AC{H^{0.8}}} \right]} \right\}}^3}} \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}}
+\end{equation}
+
+\subsubsection{Beausoleil Morrison Mixed Stable Ceiling}\label{beausoleil-morrison-mixed-stable-ceiling}
+
+Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for ceilings where the flow driving forces include both mechanical forces and thermally Stable buoyancy.
+
+\begin{equation}
+h = {\left( {{{\left\{ {0.6 \cdot {{\left( {\frac{{\left| {\Delta T} \right|}}{{{D_H}}}} \right)}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{5}}}}} \right\}}^3} + {{\left\{ {\left[ {\frac{{{T_{surf}} - {T_{SAT}}}}{{\left| {\Delta T} \right|}}} \right]\cdot\left[ { - 0.166 + 0.484AC{H^{0.8}}} \right]} \right\}}^3}} \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}}
+\end{equation}
+
+\subsubsection{Beausoleil Morrison Mixed Unstable Ceiling}\label{beausoleil-morrison-mixed-unstable-ceiling}
+
+Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for ceilings where the flow driving forces include both mechanical forces and thermally unstable buoyancy.
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+h = \left(
+   \left(
+    \left[
+     1.4 \left(
+      \frac{
+       \left|
+        \Delta T
+       \right|
+      }{
+       D_h
+      }
+     \right)^{1/4}
+    \right]^6 +
+    \left[
+     1.63 \left|\Delta T\right|^{1/3}
+    \right]^6
+   \right)^{3/6} +
+   \left(
+    \left[
+     \frac{
+      T_{surf}-T_{SAT}
+     }{
+      \left|\Delta T\right|
+     }
+    \right]
+    \cdot
+    \left[
+     -0.166 + 0.484 \cdot ACH^{0.8}
+    \right]
+   \right)^3
+  \right)^{1/3}
+\end{equation}
+
+\subsubsection{Fohanno Polidori Vertical Wall}\label{fohanno-polidori-vertical-wall}
+
+Fohanno and Polidori (2006) developed the following equation for \emph{h\(_{c}\)} for vertical walls under simple buoyancy flow conditions.
+
+\begin{equation}
+h = \left\{ \begin{array}{l}1.332{\left( {\frac{{\left| {\Delta T} \right|}}{H}} \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{4}}}}\quad ,\quad Ra_H^* \le 6.3 \times {10^9}\\1.235{e^{\left( {0.0467H} \right)}}{\left| {\Delta T} \right|^{0.316}}\quad ,\quad Ra_H^* > 6.3 \times {10^9}\end{array} \right.
+\end{equation}
+
+where,
+
+\begin{equation}
+Ra_H^* = \frac{{g{\beta_f}{{q''}_c}{H^4}}}{{{k_f}\nu_f^2}}{\Pr_f}
+\end{equation}
+
+\subsubsection{Karadag Chilled Ceiling}\label{karadag-chilled-ceiling}
+
+Karadag (2009) used numerical methods to develop the following equation for \emph{h\(_{c}\)} for chilled-ceiling surfaces.
+
+\begin{equation}
+h = 3.1{\left| {\Delta T} \right|^{0.22}}
+\end{equation}
+
+\subsubsection{ISO 15099 Windows}\label{iso-15099-windows}
+
+ISO Standard 15099-2003 includes the equations for \emph{h\(_{c}\)} for room-side of windows and surfaces with any tilt angle and heat flow direction.~ The ISO 15099 correlation is for still room air angle and is determined in terms of the Nusselt number, \(Nu\) , where
+
+\begin{equation}
+{h_i} = Nu\left( {\frac{\lambda }{H}} \right)
+\end{equation}
+
+where,
+
+\(\lambda\) ~is the thermal conductivity of air, and
+
+\(H\) ~is the height of the window.
+
+The Rayleigh number based on height, \(R{a_H}\) , is calculated using,
+
+\begin{equation}
+R{a_H} = \frac{{{\rho ^2}{H^3}g\,{c_p}\left| {{T_{surf,i}} - {T_{air}}} \right|}}{{{T_{m,f}}\mu \lambda }}
+\end{equation}
+
+where,
+
+\(\rho\) ~is the density of air
+
+\(g\) ~is the acceleration due to gravity,
+
+\({c_p}\) ~is the specific heat of air,
+
+\(\mu\) ~is the dynamic viscosity of air, and
+
+\({T_{m,f}}\) ~is the mean film temperature in Kelvin given by,
+
+\begin{equation}
+{T_{m,f}} = {T_{air}} + \frac{1}{4}\left( {{T_{surf,i}} - {T_{air}}} \right)
+\end{equation}
+
+There are four cases for the Nusselt correlation that vary by the tilt angle in degrees, \(\gamma\) , and are based on heating conditions.~ For cooling conditions (where \({T_{surf,i}} > {T_{air}}\) ) the tilt angle is complemented so that \(\gamma = 180 - \gamma\)
+
+Case A. \({0^o } \leq \gamma < 15^o\)
+
+\begin{equation}
+Nu = 0.13Ra_H^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}
+\end{equation}
+
+Case B. \(15^o \leq \gamma \leq 90^o\)
+
+\begin{equation}
+R{a_{cv}} = 2.5 \times {10^5}{\left( {\frac{{{e^{0.72\gamma }}}}{{\sin \lambda }}} \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{5}}}}
+\end{equation}
+
+\begin{equation}
+Nu = 0.56{\left( {R{a_H}\sin \gamma } \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{4}}}};\;for\;R{a_H} \le R{a_{CV}}
+\end{equation}
+
+\begin{equation}
+Nu = 0.13\left( {Ra_H^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}} - Ra_{CV}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}} \right) + 0.56{\left( {R{a_{CV}}\sin \gamma } \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{4}}}};\;R{a_H} > R{a_{CV}}
+\end{equation}
+
+Case C. \(90^o < \gamma \leq 179^o\)
+
+\begin{equation}
+Nu = 0.56{\left( {R{a_H}\sin \gamma } \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{4}}}};\;{10^5} \le R{a_H}\sin \gamma  < {10^{11}}
+\end{equation}
+
+Case D. \(179^o < \gamma \leq 180^o\)
+
+\begin{equation}
+Nu = 0.58Ra_H^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{5}}};\;R{a_H} \le {10^{11}}
+\end{equation}
+
+The material properties are evaluated at the mean film temperature.~ Standard EnergyPlus psychrometric functions are used for \(\rho\) ~and \({c_p}\) .~ Thermal conductivity is calculated using,
+
+\(\lambda = 2.873 \times {10^{ - 3}} + 7.76 \times {10^{ - 8}}{T_{m,f}}\) .
+
+Kinematic viscosity is calculated using,
+
+\(\mu = 3.723 \times {10^{ - 6}} + 4.94 \times {10^{ - 8}}{T_{m,f}}\) .
+
+This correlation depends on the surface temperature of the room-side glazing surface and is therefore included inside the window heat balance iteration loop.
+
+\subsubsection{Goldstein Novoselac Ceiling Diffuser Window}\label{goldstein-novoselac-ceiling-diffuser-window}
+
+Goldstein and Novoselac (2010) used laboratory chamber measurements to develop convection correlations for perimeter zones with highly glazed spaces served by overhead slot-diffuser-based air systems. The following are for bare windows in such spaces.
+
+For WWR\textless{}50\% with window in upper part of wall:
+
+\begin{equation}
+h = 0.117{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}
+\end{equation}
+
+For WWR\textless{}50\% with window in lower part of wall
+
+\begin{equation}
+h = 0.093{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}
+\end{equation}
+
+For WWR \textgreater{} 50\%
+
+\begin{equation}
+h = 0.103{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}
+\end{equation}
+
+Where,
+
+~WWR is the window to wall ratio.
+
+~\emph{L} is the length of exterior wall with glazing in the zone.
+
+~\(\dot V\) is the air system flow rate in m\(^{3}\)/s.
+
+\subsubsection{Goldstein Novoselac Ceiling Diffuser Walls}\label{goldstein-novoselac-ceiling-diffuser-walls}
+
+Goldstein and Novoselac (2010) used laboratory chamber measurements to develop convection correlations for perimeter zones with highly glazed spaces served by overhead slot-diffuser-based air systems. The following are for exterior walls in such spaces.
+
+For walls located below a window
+
+\begin{equation}
+h = 0.063{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}
+\end{equation}
+
+For walls located above a window
+
+\begin{equation}
+h = 0.093{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}
+\end{equation}
+
+\subsubsection{Goldstein Novoselac Ceiling Diffuser Floor}\label{goldstein-novoselac-ceiling-diffuser-floor}
+
+Goldstein and Novoselac (2010) used laboratory chamber measurements to develop convection correlations for perimeter zones with highly glazed spaces served by overhead slot-diffuser-based air systems. The following is for floors in such spaces.
+
+\begin{equation}
+h = 0.048{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}
+\end{equation}
+
+Separate from the above model structure, there are also other comprehensive algorithm structures which are described below.
+
+\subsubsection{TARP Algorithm}\label{tarp-algorithm}
+
+The comprehensive natural convection model, accessed using the keyword ``TARP,'' correlates the convective heat transfer coefficient to the surface orientation and the difference between the surface and zone air temperatures (where DT = Surface Temperature - Air Temperature).~ The algorithm is taken directly from Walton (1983).~ Walton derived his algorithm from ASHRAE literature which can now be found for example in the ASHRAE Handbook (HoF 2001), Table 5 on p.~3.12, which gives equations for natural convection heat transfer coefficients in the turbulent range for large, vertical plates and for large, horizontal plates facing upward when heated (or downward when cooled).~~ A note in the text also gives an approximation for large, horizontal plates facing downward when heated (or upward when cooled) recommending that it should be half of the facing upward value.~ Walton adds a curve fit as a function of the cosine of the tilt angle to provide intermediate values between vertical and horizontal.~ The curve fit values at the extremes match the ASHRAE values very well.
+
+For no temperature difference OR a vertical surface the following correlation is used:
+
+\(h = 1.31{\left| {\Delta T} \right|^{\frac{1}{3}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ (90)
+
+For ($\Delta$T \textless{} 0.0 AND an upward facing surface)~ OR~ ($\Delta$T \textgreater{} 0.0 AND an downward facing surface) an enhanced convection correlation is used:
+
+\(h = \frac{{9.482{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{7.283 - \left| {\cos \Sigma } \right|}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ (91)
+
+where $\Sigma$ is the surface tilt angle.
+
+For ($\Delta$T \textgreater{} 0.0 AND an upward facing surface)~ OR~ ($\Delta$T \textless{} 0.0 AND an downward facing surface) a reduced convection correlation is used:
+
+\(h = \frac{{1.810{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{1.382 + \left| {\cos \Sigma } \right|}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ (92)
+
+where $\Sigma$ is the surface tilt angle.
+
+\subsubsection{Simple Natural Convection Algorithm}\label{simple-natural-convection-algorithm}
+
+The simple convection model uses constant coefficients for different heat transfer configurations, using the same criteria as the detailed model to determine reduced and enhanced convection.~ The coefficients are also taken directly from Walton (1983).~ Walton derived his coefficients from the surface conductances for e = 0.90 found in the ASHRAE Handbook (1985) in Table~\ref{table:simulation-flags} on p.~23.2.~ The radiative heat transfer component was estimated at 1.02 * 0.9 = 0.918 BTU/h-ft2-F and then subtracted off.~ Finally the coefficients were converted to SI units to yield the values below.
+
+For a vertical surface:
+
+\begin{equation}
+{\rm{h  =  3}}{\rm{.076}}
+\end{equation}
+
+For a horizontal surface with reduced convection:
+
+\begin{equation}
+{\rm{h  =  0}}{\rm{.948}}
+\end{equation}
+
+For a horizontal surface with enhanced~ convection:
+
+\begin{equation}
+{\rm{h  =  4}}{\rm{.040}}
+\end{equation}
+
+For a tilted surface with reduced convection:
+
+\begin{equation}
+{\rm{h  =  2}}{\rm{.281}}
+\end{equation}
+
+For a tilted surface with enhanced convection:
+
+\begin{equation}
+{\rm{h  =  3}}{\rm{.870}}
+\end{equation}
+
+\subsubsection{Ceiling Diffuser Algorithm}\label{ceiling-diffuser-algorithm}
+
+The ceiling diffuser algorithm is based on empirical correlations developed by Fisher and Pedersen (1997).~ The correlation was reformulated to use the room outlet temperature as the reference temperature.~ The correlations are shown below.
+
+For Floors:
+
+\(h = 3.873 + 0.082 * AC{H^{0.98}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ (93)
+
+The correlation for floors is illustrated in the following figure:
+
+\begin{figure}[hbtp] % fig 1017
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image378.png}
+\caption{Ceiling Diffuser Correlation for Floors \protect \label{fig:ceiling-diffuser-correlation-for-floors}}
+\end{figure}
+
+For ceilings:
+
+\(h = 2.234 + 4.099 * AC{H^{0.503}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ (94)
+
+The correlation for ceilings is illustrated in the following figure:
+
+\begin{figure}[hbtp] % fig 1018
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image380.png}
+\caption{Ceiling Diffuser Correlation for Ceilings \protect \label{fig:ceiling-diffuser-correlation-for-ceilings}}
+\end{figure}
+
+For Walls:
+
+\(h = 1.208 + 1.012 * AC{H^{0.604}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ (95)
+
+The correlation for walls is illustrated in the following figure:
+
+\begin{figure}[hbtp] % fig 1019
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image382.png}
+\caption{Ceiling Diffuser Correlation for Walls \protect \label{fig:ceiling-diffuser-correlation-for-walls}}
+\end{figure}
+
+\subsubsection{Trombe Wall Algorithm}\label{trombe-wall-algorithm}
+
+The Trombe wall algorithm is used to model convection in a ``Trombe wall zone'', i.e.~the air space between the storage wall surface and the exterior glazing.~ (See the later sections on Passive and Active Trombe Walls below for more information about Trombe walls.)~ The algorithm is identical to the convection model (based on ISO 15099) used in Window5 for convection between glazing layers in multi-pane window systems.~ The use of the algorithm for modeling an unvented Trombe wall has been validated against experimental data by Ellis (2003).
+
+This algorithm gives the convection coefficients for air in a narrow vertical cavity that is sealed and not ventilated.~ This applies both to the air gap in between panes of a window or to the air gap between the Trombe wall glazing and the inner surface (often a selective surface).~ These convection coefficients are really the only difference between a normal zone and a Trombe zone.~ The rest of the zone heat balance is the same, e.g., transmitted solar, long-wave radiation between surfaces, etc.
+
+For a vertical cavity, the correlation from ISO 15099 is:
+
+\({\rm{NU1 = 0}}{\rm{.0673838 R}}{{\rm{a}}^{{\textstyle{{\rm{1}} \over {\rm{3}}}}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ for 5E4 \textless{} Ra \textless{} 1E6
+
+\({\rm{NU1 = 0}}{\rm{.028154 R}}{{\rm{a}}^{{\rm{0}}{\rm{.4134}}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ for 1E4 \textless{} Ra \textless{} 5E4
+
+\({\rm{NU1 = 1 + 1}}{\rm{.7596678E - 10 R}}{{\rm{a}}^{{\rm{2}}{\rm{.2984755}}}}\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ for Ra \textless{} = 1E4
+
+\begin{equation}
+{\rm{NU2}} = 0.242{\left( {{\raise0.7ex\hbox{{{\rm{Ra}}}} \!\mathord{\left/ {\vphantom {{{\rm{Ra}}} {\rm{A}}}}\right.}\!\lower0.7ex\hbox{{\rm{A}}}}} \right)^{0.272}}
+\end{equation}
+
+\begin{equation}
+{\rm{NU = MAX(NU1,NU2)}}
+\end{equation}
+
+where
+
+Nu = Nusselt number
+
+Ra = Rayleigh number
+
+A = aspect ratio of cavity
+
+This is then used in EnergyPlus as follows:
+
+Net convection coefficient from glazing to wall is:
+
+\begin{equation}
+{h_{net}} = {\rm{k}}\left( {{\raise0.7ex\hbox{{{\rm{NU}}}} \!\mathord{\left/ {\vphantom {{{\rm{NU}}} {\rm{L}}}}\right.}\!\lower0.7ex\hbox{{\rm{L}}}}} \right)
+\end{equation}
+
+where
+
+k = conductivity of air
+
+L = air gap thickness
+
+Convection coefficient applied to each wall separately and actually used in the zone heat balance is:
+
+\begin{equation}
+{h_c} = 2{h_{net}}
+\end{equation}
+
+\subsubsection{References}\label{references-032}
+
+Alamdari, F. and G.P. Hammond. 1983. Improved data correlations for buoyancy-driven convection in rooms.~ Building Services Engineering Research \& Technology. Vol. 4, No. 3.
+
+ASHRAE. 1985. 1985 ASHRAE Handbook -- Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2001. 2001 ASHRAE Handbook -- Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
+
+Awbi, H.B. and A. Hatton. 1999. Natural convection from heated room surfaces. Energy and Buildings 30 (1999) 233-244.
+
+Beausoleil-Morrison, I. 2000. The adaptive coupling of heat and air flow modeling within dynamic whole-building simulations. PhD. Thesis. University of Strathclyde, Glasgow, UK.
+
+Ellis, Peter G. 2003. Development and Validation of the Unvented Trombe Wall Model in EnergyPlus. Master's Thesis, University of Illinois at Urbana-Champaign.
+
+Fisher, D.E. and C.O. Pedersen. 1997. ``Convective Heat Transfer in Building Energy and Thermal Load Calculations'', ASHRAE Transactions, Vol. 103, Pt. 2.
+
+Fohanno, S., and G. Polidori. 2006. Modelling of natural convective heat transfer at an internal surface. Energy and Buildings 38 (2006) 548 - 553
+
+Goldstein, K. and A. Novoselac. 2010. Convective Heat Transfer in Rooms With Ceiling Slot Diffusers (RP-1416). \emph{HVAC\&R Research Journal} TBD
+
+Karadag, R. 2009. New approach relevant to total heat transfer coefficient including the effect of radiation and convection at the ceiling in a cooled ceiling room. Applied Thermal Engineering 29 (2009) 1561-1565
+
+Khalifa AJN. 1989. Heat transfer processes in buildings. Ph.D.~Thesis, University of Wales College of Cardiff, Cardiff, UK.
+
+ISO. 2003. ISO 15099:2003. Thermal performance of windows, doors, and shading devices -- Detailed calculations. International Organization for Standardization.
+
+Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards (now NIST). This is documentation for ``TARP.''
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/outside-surface-heat-balance.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/outside-surface-heat-balance.tex
new file mode 100644
index 00000000000..11c06b5abbd
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/outside-surface-heat-balance.tex
@@ -0,0 +1,801 @@
+\section{Outside Surface Heat Balance}\label{outside-surface-heat-balance}
+
+\begin{figure}[hbtp] % fig 18
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image242.png}
+\caption{Outside Heat Balance Control Volume Diagram \protect \label{fig:outside-heat-balance-control-volume-diagram}}
+\end{figure}
+
+The heat balance on the outside face is:
+
+\begin{equation}
+{q''_{\alpha sol}} + {q''_{LWR}} + {q''_{conv}} - {q''_{ko}} = 0
+\end{equation}
+
+where:
+\(q''_{\alpha sol}\) = Absorbed direct and diffuse solar (short wavelength) radiation heat flux.
+\(q''_{LWR}\) = Net long wavelength (thermal) radiation flux exchange with the air and surroundings.
+\(q''_{conv}\) = Convective flux exchange with outside air.
+\(q''_{ko}\) = Conduction heat flux (q/A) into the wall.
+
+All terms are positive for net flux to the face except the conduction term, which is traditionally taken to be positive in the direction from outside to inside of the wall.~ Simplified procedures generally combine the first three terms by using the concept of a \emph{sol-air temperature}.~ Each of these heat balance components is introduced briefly below.
+
+\subsection{External Shortwave Radiation}\label{external-shortwave-radiation}
+
+\(q''_{\alpha sol}\) is calculated using procedures presented later in this manual and includes both direct and diffuse incident solar radiation absorbed by the surface face.~ This is influenced by location, surface facing angle and tilt, surface face material properties, weather conditions, etc.
+
+\subsection{External Longwave Radiation}\label{external-longwave-radiation}
+
+\({q''_{LWR}}\) is a standard radiation exchange formulation between the surface, the sky, and the ground. The radiation heat flux is calculated from the surface absorptivity, surface temperature, sky and ground temperatures, and sky and ground view factors.
+
+The longwave radiation heat exchange between surfaces is dependent on surface temperatures, spatial relationships between surfaces and surroundings, and material properties of the surfaces. The relevant material properties of the surface, emissivity e and absorptivity a, are complex functions of temperature, angle, and wavelength for each participating surface. However, it is generally agreed that reasonable assumptions for building loads calculations are (Chapman 1984; Lienhard 1981):
+
+\begin{itemize}
+\item
+  each surface emits or reflects diffusely and is gray and opaque ($\alpha$ = $\varepsilon$, $\tau$ = 0, $\rho$ = 1 - $\varepsilon$)
+\item
+  each surface is at a uniform temperature
+\item
+  energy flux leaving a surface is evenly distributed across the surface,
+\item
+  the medium within the enclosure is non-participating.
+\end{itemize}
+
+These assumptions are frequently used in all but the most critical engineering applications.
+
+\begin{longtable}[c]{p{1.0in}p{3.0in}p{1.0in}p{1.0in}}
+
+\caption{Nomenclature List of Variables \label{table:nomenclature-list-of-variables}} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & Range \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature List of Variables} \tabularnewline
+\toprule 
+Mathematical variable & Description & Units & Range \tabularnewline
+\midrule
+\endhead
+
+$q''_{LWR}$ & Exterior surface longwave radiation flux & $W/m^2$ & --- \tabularnewline
+$h_r$ & Linearized radiative heat transfer coefficient to air temperature & $W/m^2.K$ & --- \tabularnewline
+$T_{surf}$ & Surface Outside face temperatures & $K$ & --- \tabularnewline
+$T_{air}$ & Outside air temperature & $K$ & --- \tabularnewline
+$T_{gnd}$ & Environmental ground surface temperature & $K$ & --- \tabularnewline
+$T_{sky}$ & Sky Effective temperature & $K$ & --- \tabularnewline
+$F_{gnd}$ & view factor of wall surface to ground surface & --- & 0--1 \tabularnewline
+$F_{sky}$ & View factor of wall surface to sky & --- & 0--1 \tabularnewline
+$F_{air}$ & View factor of wall surface to air & --- & 0--1 \tabularnewline
+$\varepsilon$ & Surface long-wave emissivity & --- & 0--1 \tabularnewline
+$\sigma$ & Stefan-Boltzmann constant & $W/m^2.K^4$ & $5.67 \times 10^{-8}$ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Consider an enclosure consisting of building exterior surface, surrounding ground surface, and sky.~ Using the assumptions above, we can determine the longwave radiative heat flux at the building exterior surface (Walton 1983; McClellan and Pedersen 1997).~ The total longwave radiative heat flux is the sum of components due to radiation exchange with the ground, sky, and air.
+
+\begin{equation}
+q_{LWR}^`` = {q''_{gnd}} + {q''_{sky}} + {q''_{air}}
+\end{equation}
+
+Applying the Stefan-Boltzmann Law to each component yields:
+
+\begin{equation}
+q_{_{LWR}}^`` = \varepsilon \sigma {F_{gnd}}(T_{gnd}^4 - T_{surf}^4) + \varepsilon \sigma {F_{sky}}(T_{sky}^4 - T_{surf}^4) + \varepsilon \sigma {F_{air}}(T_{air}^4 - T_{surf}^4)
+\end{equation}
+
+where
+
+$\varepsilon$ = long-wave emittance of the surface
+
+$\sigma$ = Stefan-Boltzmann constant
+
+F\(_{gnd}\) = view factor of wall surface to ground surface temperature
+
+F\(_{sky}\) = view factor of wall surface to sky temperature
+
+F\(_{air}\) = view factor of wall surface to air temperature
+
+T\(_{surf}\) = outside surface temperature
+
+T\(_{gnd}\) = ground surface temperature
+
+T\(_{sky}\) = sky temperature
+
+T\(_{air}\) = air temperature
+
+Linearized radiative heat transfer coefficients are introduced to render the above equation more compatible with the heat balance formulation,
+
+\begin{equation}
+q_{_{LWR}}^`` = {h_{r,gnd}}({T_{gnd}} - {T_{surf}}) + {h_{r,sky}}({T_{sky}} - {T_{surf}}) + {h_{r,air}}({T_{air}} - {T_{surf}})
+\end{equation}
+
+where
+
+\begin{equation}
+{h_{r,gnd}} = \frac{{\varepsilon \sigma {F_{gnd}}(T_{surf}^4 - T_{gnd}^4)}}{{{T_{surf}} - {T_{gnd}}}}
+\end{equation}
+
+\begin{equation}
+{h_{r,sky}} = \frac{{\varepsilon \sigma {F_{sky}}(T_{surf}^4 - T_{sky}^4)}}{{{T_{surf}} - {T_{sky}}}}
+\end{equation}
+
+\begin{equation}
+{h_{r,air}} = \frac{{\varepsilon \sigma {F_{air}}(T_{surf}^4 - T_{air}^4)}}{{{T_{surf}} - {T_{air}}}}
+\end{equation}
+
+The longwave view factors to ground and sky are calculated with the following expressions (Walton 1983):
+
+\begin{equation}
+{F_{ground}} = 0.5(1 - \cos \phi )
+\end{equation}
+
+\begin{equation}
+{F_{sky}} = 0.5(1 + \cos \phi )
+\end{equation}
+
+where \emph{f} is the tilt angle of the surface.~ The view factor to the sky is further split between sky and air radiation by:
+
+\begin{equation}
+\beta  = \sqrt {0.5\left( {1 + \cos \phi } \right)}
+\end{equation}
+
+The ground surface temperature is assumed to be the same as the air temperature.~ The final forms of the radiative heat transfer coefficients are shown here.
+
+\begin{equation}
+{h_{r,gnd}} = \frac{{\varepsilon \sigma {F_{gnd}}(T_{surf}^4 - T_{air}^4)}}{{{T_{surf}} - {T_{air}}}}
+\end{equation}
+
+\begin{equation}
+{h_{r,sky}} = \frac{{\varepsilon \sigma {F_{sky}}\beta (T_{surf}^4 - T_{sky}^4)}}{{{T_{surf}} - {T_{sky}}}}
+\end{equation}
+
+\begin{equation}
+{h_{r,air}} = \frac{{\varepsilon \sigma {F_{sky}}\left( {1 - \beta } \right)(T_{surf}^4 - T_{air}^4)}}{{{T_{surf}} - {T_{air}}}}
+\end{equation}
+
+\subsection{References}\label{references-034}
+
+ASHRAE. 1993. 1993 ASHRAE Handbook -- Fundamentals. Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
+
+Chapman, A. J. 1984. Heat Transfer, 4\(^{th}\) Edition, New York: Macmillan Publishing Company.
+
+Lienhard, J. H. 1981. A Heat Transfer Textbook, Englewood Cliffs, N.J.: Prentice-Hall, Inc.
+
+McClellan, T. M., and C. O. Pedersen. 1997. Investigation of Outside Heat Balance Models for Use in a Heat Balance Cooling Load Calculation. ASHRAE Transactions, Vol. 103, Part 2, pp.~469-484.
+
+Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards.
+
+\subsection{Atmospheric Variation}\label{atmospheric-variation}
+
+All buildings are located in the troposphere, the lowest layer of the atmosphere.~ The troposphere extends from sea level to an altitude of 11 km.~ Throughout the troposphere, air temperature decreases almost linearly with altitude at a rate of approximately 1°C per 150 m.~ Barometric pressure decreases more slowly.~ Wind speed, on the other hand, increases with altitude.
+
+Because the atmosphere changes with altitude (defined as \emph{height above ground} in this case), tall buildings can experience significant differences in local atmospheric properties between the ground floor and the top floor. ~Buildings interact with the atmosphere through convective heat transfer between the outdoor air and the exterior surfaces of the building envelope, and through the exchange of air between the outside and inside of the building via infiltration and ventilation.
+
+Impetus for using this modeling is illustrated in the next table.~ Using a 70 story (284 meters) building as an example, the atmospheric variables are significant.
+
+% table 4
+\begin{longtable}[c]{@{}lllll@{}}
+\caption{Atmospheric Variables at Two Different Altitudes above Ground Level \label{table:atmospheric-variables-at-two-different}} \tabularnewline
+\toprule 
+Variable & 1.5 Meters & 284 meters & Absolute Diff & Percent Diff \tabularnewline \midrule
+\endhead
+
+Air Temperature & 15°C & 13.15°C & 1.85°C & 12.3\% \tabularnewline
+Barometric Pressure & 101,325 Pa & 97,960 Pa & 3,365 Pa & 3.3\% \tabularnewline
+Wind Speed & 2.46 m/s & 7.75 m/s & 5.29 m/s & 215\% \tabularnewline
+\bottomrule
+\end{longtable}
+
+Comparing the annual energy usage between 60 discretely modeled floors of a building, it turns out that the effect due to wind speed change is dominant over the first ten floors.~ But at floor 25, surprisingly, the effect due to air temperature has caught up and is about equal to the effect of wind speed.~ Above floor 25 the effect due to air temperature is now dominant.~ Clearly it is desirable to model air temperature variation with altitude for high-rise buildings.
+
+To accommodate atmospheric variation EnergyPlus automatically calculates the local outdoor air temperature and wind speed separately for each zone and surface that is exposed to the outdoor environment.~ The zone centroid or surface centroid are used to determine the height above ground.~ Only local outdoor air temperature and wind speed are currently calculated because they are important factors for the exterior convection calculation for surfaces (see Exterior Convection below) and can also be factors in the zone infiltration and ventilation calculations.~ Variation in barometric pressure, however, is considered when using the Airflow Network objects.
+
+\subsubsection{Local Outdoor Air Temperature Calculation}\label{local-outdoor-air-temperature-calculation}
+
+Variation in outdoor air temperature is calculated using the U.S. Standard Atmosphere (1976).~ According to this model, the relationship between air temperature and altitude in a given layer of the atmosphere is:
+
+\begin{equation}
+{T_z} = {T_b} + L\left( {{H_z} - {H_b}} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{z}\)} = air temperature at altitude \emph{z}
+
+\emph{T\(_{b}\)} = air temperature at the base of the layer, i.e., ground level for the troposphere
+
+\emph{L} = air temperature gradient, equal to --0.0065 K/m in the troposphere
+
+\emph{H\(_{b}\)} = offset equal to zero for the troposphere
+
+\emph{H\(_{z}\)} = geopotential altitude.
+
+The variable \emph{H\(_{z}\)} is defined by:
+
+\begin{equation}
+{H_z} = \frac{{Ez}}{{\left( {E + z} \right)}}
+\end{equation}
+
+where
+
+\emph{E} = 6,356 km, the radius of the Earth
+
+\emph{z} = altitude.
+
+For the purpose of modeling buildings in the troposphere, altitude \emph{z} refers to the height above ground level, not the height above sea level.~ The height above ground is calculated as the height of the centroid, or area-weighted center point, for each zone and surface.
+
+The air temperature at ground level, \emph{T\(_{b}\)}, is derived from the weather file air temperature by inverting the equation above:
+
+\begin{equation}
+{T_b} = {T_{z,met}} - L\left( {\frac{{E{z_{met}}}}{{E + {z_{met}}}} - {H_b}} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{z,met}\)} = weather file air temperature (measured at the meteorological station)
+
+\emph{z\(_{met}\)} = height above ground of the air temperature sensor at the meteorological station.
+
+The default value for \emph{z\(_{met}\)} for air temperature measurement is 1.5 m above ground.~ This value can be overridden by using the Site:WeatherStation object.
+
+\subsubsection{Local Wind Speed Calculation}\label{local-wind-speed-calculation}
+
+Chapter 16 of the Handbook of Fundamentals (ASHRAE 2005).~ The wind speed measured at a meteorological station is extrapolated to other altitudes with the equation:
+
+\begin{equation}
+{V_z} = {V_{met}}{\left( {\frac{{{\delta_{met}}}}{{{z_{met}}}}} \right)^{{\alpha_{met}}}}{\left( {\frac{z}{\delta }} \right)^\alpha }
+\end{equation}
+
+where
+
+\emph{z} = altitude, height above ground
+
+\emph{V\(_{z}\)} = wind speed at altitude \emph{z}
+
+\emph{$\alpha$} = wind speed profile exponent at the site
+
+\emph{$\delta$} = wind speed profile boundary layer thickness at the site
+
+\emph{z\(_{met}\)} = height above ground of the wind speed sensor at the meteorological station
+
+\emph{V\(_{met}\)} = wind speed measured at the meteorological station
+
+\emph{$\alpha$\(_{met}\)} = wind speed profile exponent at the meteorological station
+
+\emph{$\delta$\(_{met}\)} = wind speed profile boundary layer thickness at the meteorological station.
+
+The wind speed profile coefficients \emph{$\alpha$}, \emph{$\delta$}, \emph{$\alpha$\(_{met}\)}, and \emph{$\delta$\(_{met}\)}, are variables that depend on the roughness characteristics of the surrounding terrain.~ Typical values for \emph{$\alpha$} and \emph{$\delta$} are shown in the following table:
+
+\begin{longtable}[c]{p{3.0in}p{1.5in}p{1.5in}}
+
+\caption{Wind Speed Profile Coefficients (ASHRAE Fundamentals 2005). \label{table:wind-speed-profile-coefficients-ashrae}} \tabularnewline
+\toprule
+Terrain Description       & Exponent, $\alpha$ & Boundary Layer Thickness, $\delta$ (m) \tabularnewline
+\midrule
+\endhead
+
+Flat, open country        & 0.14 & 270 \tabularnewline
+Rough, wooded country     & 0.22 & 370 \tabularnewline
+Towns and cities          & 0.33 & 460 \tabularnewline
+Ocean                     & 0.10 & 210 \tabularnewline
+Urban, industrial, forest & 0.22 & 370 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The terrain types above map to the options in the \emph{Terrain} field of the Building object.~ The \emph{Terrain} field can be overridden with specific values for \emph{$\alpha$} and \emph{$\delta$} by using the Site:HeightVariation object.
+
+The default value for \emph{z\(_{met}\)} for wind speed measurement is 10 m above ground.~ The default values for \emph{$\alpha$\(_{met}\)} and \emph{$\delta$\(_{met}\)} are 0.14 and 270 m, respectively, because most meteorological stations are located in an open field.~ These values can be overridden by using the Site:WeatherStation object.
+
+\subsection{Outdoor/Exterior Convection}\label{outdoorexterior-convection}
+
+Heat transfer from surface convection is modeled using the classical formulation:
+
+\begin{equation}
+{Q_c} = {h_{c,ext}}A\left( {{T_{surf}} - {T_{air}}} \right)
+\end{equation}
+
+where
+
+\emph{Q\(_{c}\)} = rate of exterior convective heat transfer
+
+\emph{h\(_{c,ext}\)} = exterior convection coefficient
+
+\emph{A} = surface area
+
+\emph{T\(_{surf}\)} = surface temperature
+
+\emph{T\(_{air}\)} = outdoor air temperature
+
+Substantial research has gone into the formulation of models for estimating the exterior convection coefficient. Since the 1930's there have been many different methods published for calculating this coefficient, with much disparity between them (Cole and Sturrock 1977; Yazdanian and Klems 1994).~ More recently Palyvos (2008) surveyed correlations cataloging some 91 different correlations into four categories based on functional form of the model equation.~ EnergyPlus therefore offers a wide selection of different methods for determining values for \emph{h\(_{c,ext}\)}. The selection of model equations for \emph{h\(_{c,ext}\)} can be made at two different levels. The first is the set of options available in the input object SurfaceConvectionAlgorithm:Outside that provides a way of broadly selecting which model equations are applied throughout the model.~ The input objects SurfaceProperty:ConvectionCoefficients and SurfaceProperty:ConvectionCoefficients:MultipleSurface also provide ways of selecting which model equations or values are applied for specific surfaces.~ These basic options are identified by the key used for input and include:
+
+\begin{itemize}
+\item
+  SimpleCombined
+\item
+  TARP
+\item
+  MoWiTT
+\item
+  DOE-2
+\item
+  AdaptiveConvectionAlgorithm
+\end{itemize}
+
+Note that when the outside environment indicates that it is raining, the exterior surfaces (exposed to wind) are assumed to be wet.~ The convection coefficient is set to a very high number (1000) and the outside temperature used for the surface will be the wet-bulb temperature.~ (If you choose to report this variable, you will see 1000 as its value.)
+
+When the AdaptiveConvectionAlgorithm is used, there is a second, deeper level of control available for selecting among a larger variety of \emph{h\(_{c,ext}\)} equations and also defining custom equations using curve or table objects.~ These options are described in this section.
+
+In addition to the correlation choices described below, it is also possible to override the convection coefficients on the outside of any surface by other means:
+
+\begin{itemize}
+\item
+  Use the SurfaceProperty:ConvectionCoefficients object in the input file to set the convection coefficient value on either side of any surface.
+\item
+  Use the SurfaceProperty:OtherSideCoefficients object in the input file to set heat transfer coefficients and temperatures on surfaces.
+\item
+  Use the EnergyManagementSystem Actuators that are available for overriding h\(_{c}\) values.
+\end{itemize}
+
+These options can also use schedules to control values over time. Specific details are given in the Input Output Reference document.
+
+\subsubsection{Simple Combined}\label{simple-combined}
+
+The simple algorithm uses surface roughness and local surface windspeed to calculate the exterior heat transfer coefficient (key:SimpleCombined).~ The basic equation used is:
+
+\begin{equation}
+h = D + E{V_z} + F{V_z}^2
+\end{equation}
+
+where
+
+\emph{h} = heat transfer coefficient
+
+\emph{V\(_{z}\)} = local wind speed calculated at the height above ground of the surface centroid
+
+D, E, F = material roughness coefficients
+
+The roughness correlation is taken from Figure~\ref{fig:energyplus-program-schematic}, Page 22.4, ASHRAE Handbook of Fundamentals (ASHRAE 1989).~ The roughness coefficients are shown in the following table:
+
+% table 6
+\begin{longtable}[c]{@{}lllll@{}}
+\caption{Roughness Coefficients D, E, and F. \label{table:roughness-coefficients-d-e-and-f.}} \tabularnewline
+\toprule 
+Roughness Index & D & E & F & Example Material \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Roughness Coefficients D, E, and F.} \tabularnewline
+\toprule 
+Roughness Index & D & E & F & Example Material \tabularnewline
+\midrule
+\endhead
+
+1 (Very Rough) & 11.58 & 5.894 & 0.0 & Stucco \tabularnewline
+2 (Rough) & 12.49 & 4.065 & 0.028 & Brick \tabularnewline
+3 (Medium Rough) & 10.79 & 4.192 & 0.0 & Concrete \tabularnewline
+4 (Medium Smooth) & 8.23 & 4.0 & -0.057 & Clear pine \tabularnewline
+5 (Smooth) & 10.22 & 3.1 & 0.0 & Smooth Plaster \tabularnewline
+6 (Very Smooth) & 8.23 & 3.33 & -0.036 & Glass \tabularnewline
+\bottomrule
+\end{longtable}
+
+Note that the simple correlation yields a combined convection and radiation heat transfer coefficient.~ Radiation to sky, ground, and air is included in the exterior convection coefficient for this algorithm.
+
+All other algorithms yield a \emph{convection only} heat transfer coefficient.~ Radiation to sky, ground, and air is calculated automatically by the program.
+
+\subsubsection{TARP ALGORITHM}\label{tarp-algorithm-000}
+
+TARP, or Thermal Analysis Research Program, is an important predecessor of EnergyPlus (Walton 1983).~ Walton developed a comprehensive model for exterior convection by blending correlations from ASHRAE and flat plate experiments by Sparrow et. al. In older versions of EnergyPlus, prior to version 6, the ``TARP'' model was called ``Detailed.''~ The model was reimplemented in version 6 to use Area and Perimeter values for the group of surfaces that make up a facade or roof, rather than the single surface being modeled.
+
+% table 7
+\begin{longtable}[c]{p{1.5in}p{2.5in}p{1.0in}p{1.0in}}
+
+\caption{Nomenclature List of Variables. \label{table:nomenclature-list-of-variables.-001}} \tabularnewline
+\toprule 
+Variable & Description & Units & Range \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature List of Variables.} \tabularnewline
+\toprule 
+Variable & Description & Units & Range \tabularnewline
+\midrule
+\endhead
+
+A & Surface area of the surface & m\(^{2}\) & /=0 \tabularnewline
+h\(_{c}\) & Surface exterior convective heat transfer coefficient & W/(m\(^{2}\)K) & - \tabularnewline
+h\(_{f}\) & Forced convective heat transfer coefficient & W/(m\(^{2}\)K) & - \tabularnewline
+h\(_{n}\) & Natural convective heat transfer coefficient & W/(m\(^{2}\)K) & - \tabularnewline
+P & Perimeter of surface & m & - \tabularnewline
+R\(_{f}\) & Surface roughness multiplier & - & - \tabularnewline
+T\(_{air}\) & Local outdoor air temperature calculated at the height above ground of the surface centroid & °C & - \tabularnewline
+T\(_{so}\) & Outside surface temperature & °C & - \tabularnewline
+$\Delta$T & Temperature difference between the surface and air, & °C & - \tabularnewline
+V\(_{z}\) & Local wind speed calculated at the height above ground of the surface centroid & m/s & - \tabularnewline
+W\(_{f}\) & Wind direction modifier & - & - \tabularnewline
+$\phi$ & Angle between the ground outward normal and the surface outward normal & degree & - \tabularnewline
+Roughness Index & Surface roughness index (6=very smooth, 5=smooth, 4=medium smooth, 3=medium rough, 2=rough, 1=very rough) & - & 1-6 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The Detailed, BLAST, and TARP convection models are very similar.~ In all three models, convection is split into forced and natural components (Walton 1981).~ The total convection coefficient is the sum of these components.
+
+\begin{equation}
+{h_c} = {h_f} + {h_n}
+\end{equation}
+
+The forced convection component is based on a correlation by Sparrow, Ramsey, and Mass (1979):
+
+\begin{equation}
+{h_f} = 2.537{W_f}{R_f}{\left( {\frac{{P{V_z}}}{A}} \right)^{1/2}}
+\end{equation}
+
+where
+
+W\(_{f}\) ~ = ~ 1.0 for windward surfaces
+
+or
+
+W\(_{f}\) = 0.5 for leeward surfaces
+
+Leeward is defined as greater than 100 degrees from normal incidence (Walton 1981).
+
+The surface roughness multiplier Rf~is based on the ASHRAE graph of surface conductance (ASHRAE 1981) and may be obtained from the following table:
+
+% table 8
+\begin{longtable}[c]{@{}lll@{}}
+\caption{Surface Roughness Multipliers (Walton 1981). \label{table:surface-roughness-multipliers-walton-1981.}} \tabularnewline
+\toprule 
+Roughness Index & Rf & Example Material \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Surface Roughness Multipliers (Walton 1981).} \tabularnewline
+\toprule 
+Roughness Index & Rf & Example Material \tabularnewline
+\midrule
+\endhead
+
+1 (Very Rough) & 2.17 & Stucco \tabularnewline
+2 (Rough) & 1.67 & Brick \tabularnewline
+3 (Medium Rough) & 1.52 & Concrete \tabularnewline
+4 (Medium Smooth) & 1.13 & Clear pine \tabularnewline
+5 (Smooth) & 1.11 & Smooth Plaster \tabularnewline
+6 (Very Smooth) & 1.00 & Glass \tabularnewline
+\bottomrule
+\end{longtable}
+
+The natural convection component \emph{h\(_{n}\)} is calculated in the same way as the interior ``Detailed'' model.~ The detailed natural convection model correlates the convective heat transfer coefficient to the surface orientation and the difference between the surface and zone air temperatures (where $\Delta$T = Air Temperature - Surface Temperature).~ The algorithm is taken directly from Walton (1983).~ Walton derived his algorithm from the ASHRAE Handbook (2001), Table 5 on p.~3.12, which gives equations for natural convection heat transfer coefficients in the turbulent range for large, vertical plates and for large, horizontal plates facing upward when heated (or downward when cooled).~~ A note in the text also gives an approximation for large, horizontal plates facing downward when heated (or upward when cooled) recommending that it should be half of the facing upward value.~ Walton adds a curve fit as a function of the cosine of the tilt angle to provide intermediate values between vertical and horizontal.~ The curve fit values at the extremes match the ASHRAE values very well.
+
+For no temperature difference OR a vertical surface the following correlation is used:
+
+\begin{equation}
+h = 1.31{\left| {\Delta T} \right|^{\frac{1}{3}}}
+\end{equation}
+
+For ($\Delta$T \textless{} 0.0 AND an upward facing surface)~ OR~ ($\Delta$T \textgreater{} 0.0 AND an downward facing surface) an enhanced convection correlation is used:
+
+\begin{equation}
+h = \frac{{9.482{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{7.283 - \left| {\cos \Sigma } \right|}}
+\end{equation}
+
+where $\Sigma$ is the surface tilt angle.
+
+For ($\Delta$T \textgreater{} 0.0 AND an upward facing surface)~ OR~ ($\Delta$T \textless{} 0.0 AND an downward facing surface) a reduced convection correlation is used:
+
+\begin{equation}
+h = \frac{{1.810{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{1.382 + \left| {\cos \Sigma } \right|}}
+\end{equation}
+
+where $\Sigma$ is the surface tilt angle.
+
+\subsubsection{MoWiTT Algorithm}\label{mowitt-algorithm}
+
+% table 9
+\begin{longtable}[c]{p{0.5in}p{3.0in}p{1.5in}p{1.0in}}
+
+\caption{Nomenclature List of Variables. \label{table:nomenclature-list-of-variables.-002}} \tabularnewline
+\toprule 
+Variable & Description & Units & Range \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature List of Variables.} \tabularnewline
+\toprule 
+Variable & Description & Units & Range \tabularnewline
+\midrule
+\endhead
+
+A & Constant & W/(m\(^{2}\)K(m/s)\(^{b}\) & - \tabularnewline
+B & Constant & - & - \tabularnewline
+C\(_{t}\) & Turbulent natural convection constant & W/(m\(^{2}\)K\(^{4/3}\)) & - \tabularnewline
+h\(_{c}\) & Surface exterior convective heat transfer coefficient & W/(m\(^{2}\)K) & - \tabularnewline
+T\(_{so}\) & Outside surface temperature & °C/K & - \tabularnewline
+$\Delta$T & Temperature difference between the surface and air & °C/K & - \tabularnewline
+\bottomrule
+\end{longtable}
+
+The MoWiTT model is based on measurements taken at the Mobile Window Thermal Test (MoWiTT) facility (Yazdanian and Klems 1994).~ The correlation applies to very smooth, vertical surfaces (e.g.~window glass) in low-rise buildings and has the form:
+
+\begin{equation}
+{h_c} = \sqrt {{{\left[ {{C_t}{{\left( {\Delta T} \right)}^{\frac{1}{3}}}} \right]}^2} + {{\left[ {aV_z^b} \right]}^2}}
+\end{equation}
+
+Constants a, b and turbulent natural convection constant C\(_{t}\) are given in Table~\ref{table:mowitt-coefficients-yazdanian-and-klems-1994}.~ The original MoWiTT model has been modified for use in EnergyPlus so that it is sensitive to the local suface's wind speed which varies with the height above ground.~ The original MoWiTT model was formulated for use with the air velocity at the location of the weather station.~ As of Version 7.2, EnergyPlus uses the ``a'' model coefficients derived by Booten et al. (2012) rather than the original values from Yazdanian and Klems (1994).
+
+NOTE:~ The MoWiTT algorithm may not be appropriate for rough surfaces, high-rise surfaces, or surfaces that employ movable insulation.
+
+% table 10
+\begin{longtable}[c]{@{}llll@{}}
+\caption{MoWiTT Coefficients (Yazdanian and Klems 1994, Booten et al. 2012) \label{table:mowitt-coefficients-yazdanian-and-klems-1994}} \tabularnewline
+\toprule 
+Wind Direction & C\(_t\) & a & b \tabularnewline
+(Units) & W/(m\(^{2}\)K\(^{4/3}\)) & W/(m\(^{2}\)K(m/s)\(^{b}\) & - \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{MoWiTT Coefficients (Yazdanian and Klems 1994, Booten et al. 2012)} \tabularnewline
+\toprule 
+Wind Direction & C\(_t\)t & a & b \tabularnewline
+(Units) & W/(m\(^{2}\)K\(^{4/3}\)) & W/(m\(^{2}\)K(m/s)\(^{b}\) & - \tabularnewline
+\midrule
+\endhead
+
+Windward & 0.84 & 3.26 & 0.89 \tabularnewline
+Leeward & 0.84 & 3.55 & 0.617 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{DOE-2 Model}\label{doe-2-model}
+
+% table 11
+\begin{longtable}[c]{p{0.5in}p{3.0in}p{1.5in}p{1.0in}}
+
+\caption{Nomenclature List of Variables. \label{table:nomenclature-list-of-variables.-003}} \tabularnewline
+\toprule 
+Variable & Description & Units & Range \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Nomenclature List of Variables.} \tabularnewline
+\toprule 
+Variable & Description & Units & Range \tabularnewline
+\midrule
+\endhead
+
+a & Constant & W/(m\(^{2}\)K(m/s)\(^{b}\) & - \tabularnewline
+b & Constant & - & - \tabularnewline
+h\(_{c}\) & Surface exterior convective heat transfer coefficient & W/(m\(^{2}\)K) & - \tabularnewline
+h\(_{c,glass}\) & Convective heat transfer coefficient for very smooth surfaces (glass) & W/(m\(^{2}\)K) & - \tabularnewline
+h\(_{n}\) & Natural convective heat transfer coefficient & W/(m\(^{2}\)K) & - \tabularnewline
+R\(_{f}\) & Surface roughness multiplier & - & - \tabularnewline
+T\(_{so}\) & Outside surface temperature & °C/K & - \tabularnewline
+$\Delta$T & Temperature difference between the surface and air, & °C/K & - \tabularnewline
+$\Phi$ & Angle between the ground outward normal and the surface outward normal & radian & - \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{}\label{section}
+
+The DOE-2 convection model is a combination of the MoWiTT and BLAST Detailed convection models (LBL 1994). The convection coefficient for very smooth surfaces (e.g.~glass) is calculated as:
+
+\begin{equation}
+{h_{c,glass}} = \sqrt {h_n^2 + {{\left[ {aV_z^b} \right]}^2}}
+\end{equation}
+
+h\(_{n}\) is calculated using Equation or Equation .~ Constants a and b are given in Table~\ref{table:mowitt-coefficients-yazdanian-and-klems-1994}.
+
+For less smooth surfaces, the convection coefficient is modified according to the equation
+
+\begin{equation}
+{h_c} = {h_n} + {R_f}({h_{c,glass}} - {h_n})
+\end{equation}
+
+where R\(_{f}\) is the roughness multiplier given by Table~\ref{table:surface-roughness-multipliers-walton-1981.}.
+
+\subsubsection{Adaptive Convection Algorithm}\label{adaptive-convection-algorithm-000}
+
+This algorithm has a structure that allows for finer control over the models used for particular surfaces.~ The algorithm for the outside face was developed for EnergyPlus but it borrows concepts and its name from the research done by Beausoleil-Morrison (2000, 2002) for convection at the inside face (see the description below for interior convection).
+
+The adaptive convection algorithm implemented in EnergyPlus for the outside face is much simpler than that for the inside face. The surface classification system has a total of 4 different categories for surfaces that depend on current wind direction and heat flow directions.~ However it is more complex in that the \emph{h\(_{c}\)} equation is split into two parts and there are separate model equation selections for forced convection, \emph{h\(_{f}\)}, and natural convection, \emph{h\(_{n}\)}. The following table summarizes the categories and the default assignments for \emph{h\(_{c}\)} equations. The individual \emph{h\(_{c}\)} equations are documented below.
+
+% table 12
+{\scriptsize
+\begin{longtable}[c]{p{0.25in}p{0.75in}p{0.5in}p{0.5in}p{1.75in}p{1.75in}}
+
+\caption{Adaptive Convection Algorithm Details \label{table:adaptive-convection-algorithm-details}} \tabularnewline
+\toprule 
+\# & Surface Classification & Heat Flow Direction & Wind Direction & h\(_f\) Models & h\(_n\) Models \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Adaptive Convection Algorithm Details} \tabularnewline
+\toprule 
+\# & Surface Classification & Heat Flow Direction & Wind Direction & h\(_f\) Models & h\(_n\) Models \tabularnewline
+\midrule
+\endhead
+
+1 & Roof Stable & Down & Any & TARPWindward MoWiTTWindward DOE2Windward NusseltJurges BlockenWindward EmmelRoof ClearRoof & WaltonStableHorizontalOrTilt AlamdariStableHorizontal \tabularnewline
+2 & Roof Unstable & Up & Any & TARPWindward MoWiTTWindward DOE2Windward NusseltJurges BlockenWindward EmmelRoof ClearRoof & WaltonUnstableHorizontalOrTilt AlamdariUnstableHorizontal \tabularnewline
+3 & Vertical Wall Windward & Any & Windward & TARPWindward DOE2Windward MoWiTTWindward NusseltJurges McAdams Mitchell BlockenWindward EmmelVertical & ASHRAEVerticalWall AlamdariHammondVerticalWall FohannoPolidoriVerticalWall ISO15099Windows \tabularnewline
+4 & Vertical Wall Leeward & Any & Leeward & TARPLeeward MoWiTTLeeward DOE2Leeward EmmelVertical NusseltJurges McAdams Mitchell & ASHRAEVerticalWall AlamdariHammondVerticalWall FohannoPolidoriVerticalWall ISO15099Windows \tabularnewline
+\bottomrule
+\end{longtable}}
+
+\paragraph{Outside Face Surface Classification}\label{outside-face-surface-classification}
+
+During an initial setup phase, all the heat transfer surfaces in the input file are analyzed in groups to determine appropriate values for geometry scales used in many of the convection correlations.~ Eight separate groups are assembled for nominally vertical exterior surfaces for eight bins of azimuth: north, northeast, east, southeast, south, southwest, west, northwest.~ Surfaces with the same range of azimuth are grouped together and analyzed for overall geometry parameters.~ A ninth group is assembled for nominally horizontal exterior surfaces for a roof bin that is also analyzed for geometry.~ These geometry routines find bounds and limits of all the surfaces in the group and then model geometric parameters from these limits.
+
+\paragraph{Sparrow Windward}\label{sparrow-windward}
+
+As discussed above for the TARP algorithm, a Sparrow et al. (1979) conducted flat plate measurements and develop the following correlation for finite-size flat plates oriented to windward.
+
+\begin{equation}
+{h_f} = 2.53{R_f}{\left( {\frac{{P{V_z}}}{A}} \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 2}}\right.}\!\lower0.7ex\hbox{2}}}}
+\end{equation}
+
+\paragraph{Sparrow Leeward}\label{sparrow-leeward}
+
+Sparrow et al. (1979) conducted flat plate measurements and develop the following correlation for finite-size flat plates oriented to leeward.
+
+\begin{equation}
+{h_f} = \frac{{2.53}}{2}{R_f}{\left( {\frac{{P{V_z}}}{A}} \right)^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 2}}\right.}\!\lower0.7ex\hbox{2}}}}
+\end{equation}
+
+\paragraph{MoWITT Windward}\label{mowitt-windward}
+
+As discussed above, Yazdanian and Klems (1994) used outdoor laboratory measurements to develop the following correlation for smooth surfaces oriented to windward. Booten et al. (2012) developed revised coefficients for use with local surface wind speeds.
+
+\begin{equation}
+{h_c} = \sqrt {{{\left[ {0.84{{\left| {\Delta T} \right|}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}}} \right]}^2} + {{\left[ {2.38{\kern 1pt} {\kern 1pt} V_z^{0.89}} \right]}^2}}
+\end{equation}
+
+This model equation is for the total film coefficient and includes the natural convection portion. Therefore it should not be used in conjunction with a second natural convection model equation.
+
+\paragraph{MoWITT Leeward}\label{mowitt-leeward}
+
+Yazdanian and Klems (1994) used outdoor laboratory measurements to develop the following correlation for smooth surfaces oriented to leeward. Booten et al. (2012) developed revised coefficients for use with local surface wind speeds.
+
+\begin{equation}
+{h_c} = \sqrt {{{\left[ {0.84{{\left| {\Delta T} \right|}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}}} \right]}^2} + {{\left[ {2.86{\kern 1pt} {\kern 1pt} V_z^{0.617}} \right]}^2}}
+\end{equation}
+
+This model equation is for the total film coefficient and includes the natural convection portion. Therefore it should not be used in conjunction with a second natural convection model equation.
+
+\paragraph{Blocken}\label{blocken}
+
+Blocken et al. (2009) developed a set of correlations for windward facing outdoor surfaces using numerical methods (key: BlockenWindward).
+
+\begin{equation}
+\begin{array}{lcl}
+    h_f = 4.6V^{0.89}_{10m} & : & \theta \leq 11.25 \\
+    h_f = 5.0V^{0.80}_{10m} & : & 11.25 < \theta \leq 33.75 \\
+    h_f = 4.6V^{0.84}_{10m} & : & 33.75 < \theta \leq 56.25 \\
+    h_f = 4.5V^{0.81}_{10m} & : & 56.25 < \theta \leq 100.0
+\end{array}
+\end{equation}
+
+Where \emph{V\(_{10m}\)} is the air velocity at the location of the weather station and θ is the angle of incidence between the wind and the surface in degrees.~ This model is only applicable to windward surfaces and lacks a natural convection component and therefore cannot be used on its own but only within the adaptive convection algorithm for the outside face.
+
+\paragraph{Clear}\label{clear}
+
+Clear et al. (2003) developed correlations from measurements for horizontal roofs on two commercial buildings. In EnergyPlus the implementation uses the model for natural convection plus turbulent forced convection (eq. 8A in the reference) and applies it to the center point of each surface section that makes up the roof.
+
+\begin{equation}
+{h_c} = \eta \frac{k}{{{L_n}}}0.15Ra_{{L_n}}^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}} + \frac{k}{x}{R_f}0.0296{\mathop{\rm Re}\nolimits}_x^{{\raise0.7ex\hbox{4} \!\mathord{\left/ {\vphantom {4 5}}\right.}\!\lower0.7ex\hbox{5}}}{\Pr ^{{\raise0.7ex\hbox{1} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{3}}}}
+\end{equation}
+
+Where
+
+\begin{itemize}
+\item
+  \emph{x} is the distance to the surface centroid from where the wind begins to intersect the roof. In EnergyPlus this is currently simplified to half the square root of the roof surface.
+\item
+  \({L_n} = \frac{{Area}}{{Perimeter}}\) ~of overall roof
+\item
+  \(k\) ~is the thermal conductivity of air
+\item
+  $\eta  = \frac{ln \left( 1 + \frac{Gr_{L,x}}{Re_x^2} \right)}{1 + ln \left( 1 + \frac{Gr_{L,x}}{Re_x^2} \right)}$ is the weighting factor for natural convection (suppressed at high forced convection rates)
+\item
+  $Ra_{L_n} = Gr_{L_n} Pr$ is the Rayleigh number
+\item
+  \(G{r_{{L_n}}} = \frac{{g{\rho ^2}{L_n}^3\Delta T}}{{{T_f}{\mu ^2}}}\) is the Grashof number
+\item
+  \({{\mathop{\rm Re}\nolimits}_x} = \frac{{{V_z}\rho x}}{\mu }\) is the Reynolds number at x
+\item
+  Pr is the Prandtl number
+\end{itemize}
+
+This model only claims to be applicable to horizontal roof surfaces so it may not be applicable to tilted roofs. It combines natural and forced convection and therefore should not be used in conjunction with yet another natural convection model.
+
+\paragraph{Emmel}\label{emmel}
+
+Emmel et al. (2007) developed a set of correlations for outdoor surfaces using numerical methods.~ The following equations are for vertical surfaces (key: EmmelVertical):
+
+\begin{equation}
+\begin{array}{lcl}
+    h_f = 5.15V^{0.81}_{10m} & : & \theta \leq 22.5 \\
+    h_f = 3.34V^{0.84}_{10m} & : & 22.5 < \theta \leq 67.5 \\
+    h_f = 4.78V^{0.71}_{10m} & : & 67.5 < \theta \leq 112.5 \\
+    h_f = 4.05V^{0.77}_{10m} & : & 112.5 < \theta \leq 157.5 \\
+    h_f = 3.54V^{0.76}_{10m} & : & 157.5 < \theta \leq 180.0
+\end{array}
+\end{equation}
+
+Where \emph{V\(_{10m}\)} is the air velocity at the location of the weather station and \(\theta\) is the angle of incidence between the wind and the surface in degrees.~ The following equations are used for horizontal (roof) surfaces (key: EmmelRoof):
+
+\begin{equation}
+\begin{array}{lcl}
+    h_f = 5.11V^{0.78}_{10m} & : & \theta \leq 22.5 \\
+    h_f = 4.60V^{0.79}_{10m} & : & 22.5 < \theta \leq 67.5 \\
+    h_f = 3.67V^{0.85}_{10m} & : & 67.5 < \theta \leq 90
+\end{array}
+\end{equation}
+
+Where $\theta$ is the angle of incidence between the wind and the longest edge of the roof surface in degrees.
+
+This model is for all wind directions but lacks a natural convection component.~ The model was developed for simple, rectangular low-rise buildings.~ It is available only within the adaptive convection algorithm for the outside face
+
+\paragraph{Nusselt Jurges}\label{nusselt-jurges}
+
+Perhaps the oldest equation for wind-driven convection was developed by Nusselt and Jurges (1922).~ Palyvos (2008) casts their model in simplified form in SI units as:
+
+\begin{equation}
+{h_c} = 5.8 + 3.94\;{V_z}
+\end{equation}
+
+Where \emph{V\(_{z}\)} is the wind velocity in m/s, in EnergyPlus that velocity is adjusted for height above ground using the z axis coordinate of the surface's centroid and the site wind model.~ This model can be applied to all surfaces and the relatively large constant is assumed to represent the natural convection portion of a total convection coefficient.~ The model is not sensitive to wind direction nor surface roughness.
+
+\paragraph{McAdams}\label{mcadams}
+
+A venerable equation for wind-driven convection was developed by McAdams (1954) which Palyvos (2008) casts in SI units as:
+
+\begin{equation}
+{h_c} = 5.7 + 3.8\;{V_z}
+\end{equation}
+
+Where \emph{V\(_{z}\)} is the wind velocity in m/s that has been adjusted for height above ground using the z axis coordinate of the surface's centroid.~ This model can be applied to all surfaces and the relatively large constant is assumed to represent the natural convection portion of a total convection coefficient.~ The model is not sensitive to wind direction nor surface roughness.
+
+\paragraph{Mitchell}\label{mitchell}
+
+A useful geometric scale based on building volume is used in an equation developed by Mitchell (1976).~ The wind-driven convection equation is cast by Palyvos as:
+
+\begin{equation}
+{h_f} = \frac{{8.6\;V_z^{0.6}}}{{{L^{0.4}}}}
+\end{equation}
+
+Where \emph{V\(_{z}\)} is the wind velocity in m/s that has been adjusted for height above ground using the z axis coordinate of the surface's centroid and \emph{L} is the cube root of the building's total volume. EnergyPlus interprets this as the sum of the volume of all the zones in the input file.
+
+\subsection{Exterior/External Conduction}\label{exteriorexternal-conduction}
+
+The conduction term, \({q''_{ko}}\) \(_{,}\) can in theory be calculated using a wide variety of heat conduction formulations. Typically in EnergyPlus, the Conduction Transfer Function (CTF) method is used. The available models are described in this section: Conduction Through The Walls.
+
+\subsection{References}\label{references-1-013}
+
+ASHRAE. 1981. 1981 ASHRAE Handbook -- Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 1989. 1989 ASHRAE Handbook -- Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 1993. 1993 ASHRAE Handbook -- Fundamentals, Chapter 3, Heat Transfer, I-P \& S-I Editions, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2001. 2001 ASHRAE Handbook -- Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
+
+ASHRAE. 2005. 2005 ASHRAE Handbook -- Fundamentals, Chapter 16, Air Flow Around Buildings, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
+
+Booten, C., N. Kruis, and C. Christensen. 2012. Identifying and Resolving Issues in EnergyPlus and DOE-2 Window Heat Transfer Calculations. National Renewable Energy Laboratory. NREL/TP-5500-55787. Golden, CO.
+
+Cole, R. J., and N. S. Sturrock. 1977. The Convective Heat Exchange at the External Surface of Buildings. Building and Environment, Vol. 12, p.~207.
+
+Ellis, P.G., and P.A. Torcellini. 2005. ``Simulating Tall Buildings Using EnergyPlus'', Proceedings of the Ninth International IBPSA Conference, Building Simulation 2005, Montreal, Canada, August 15-18, 2005.
+
+Lawrence Berkeley Laboratory (LBL). 1994. DOE2.1E-053 source code.
+
+Sparrow, E. M., J. W. Ramsey, and E. A. Mass. 1979. Effect of Finite Width on Heat Transfer and Fluid Flow about an Inclined Rectangular Plate. Journal of Heat Transfer, Vol. 101, p.~204.
+
+U.S. Standard Atmosphere. 1976. U.S. Government Printing Office, Washington, D.C.
+
+Walton, G. N. 1981. Passive Solar Extension of the Building Loads Analysis and System Thermodynamics (BLAST) Program, Technical Report, United States Army Construction Engineering Research Laboratory, Champaign, IL.
+
+Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards.
+
+Yazdanian, M. and J. H. Klems. 1994. Measurement of the Exterior Convective Film Coefficient for Windows in Low-Rise Buildings. ASHRAE Transactions, Vol. 100, Part 1, p.~1087.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/surface-heat-balance-with-moveable-insulation.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/surface-heat-balance-with-moveable-insulation.tex
new file mode 100644
index 00000000000..060628e68c7
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/surface-heat-balance-with-moveable-insulation.tex
@@ -0,0 +1,296 @@
+\section{Surface Heat Balance With Moveable Insulation}\label{surface-heat-balance-with-moveable-insulation}
+
+\subsection{Basic Heat Balance Cases}\label{basic-heat-balance-cases}
+
+A heat balance must exist at the outside surface-air interface. The incoming conductive, convective, and radiative fluxes must sum up to zero:
+
+\begin{equation}
+Conductive + Convective + Radiative = 0
+\end{equation}
+
+In contrast to the internal surface heat balance that treats all surfaces simultaneously, the external thermal balance for each surface is performed independent of all other surfaces. This implies that there is no direct interaction between the individual surfaces.
+
+TARP includes four possible representations for the basic outside surface heat balance. The first two depend on which of the optimal surface conductance algorithms the user selects. The simple outside surface conductance that includes both the convective and thermal interchange between the surface and the environment in a single coefficient, is represented by the thermal network in Figure~\ref{fig:thermal-network-for-simple-outside-surface}. Equation can also be expressed as:
+
+\begin{equation}
+\left[ {{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {{\rm{Y}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{I}}_t} - {{\rm{X}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{O}}_{\rm{t}}}} \right]{\rm{ + }}\left[ {{\rm{HO}}\cdot \left( {{{\rm{T}}_{\rm{a}}} - {\rm{T}}{{\rm{O}}_t}} \right)} \right]{\rm{  + QSO  =  0}}
+\end{equation}
+
+This can be solved for the outside surface temperature.
+
+\begin{equation}
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{\rm{t}}}{\rm{ + HO}}\cdot {{\rm{T}}_{\rm{a}}}}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HO}}}}} \right]{\rm{  }}
+\end{equation}
+
+The detailed outside surface conductance model considers convection and radiant interchange with the sky and with the ground as separate factors. Its use in the outside thermal balance is shown in Figure~\ref{fig:thermal-network-for-detailed-outside-surface}.In this case, equation can be expanded to give
+
+\begin{equation}
+\left[ {{\rm{KO}}{{\rm{P}}_{\rm{t}}}{\rm{ + }}{{\rm{Y}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{I}}_{\rm{t}}}{\rm{ - }}{{\rm{X}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{O}}_{\rm{t}}}} \right]{\rm{ + }}\left[ {{\rm{HA}}\cdot \left( {{{\rm{T}}_{\rm{a}}}{\rm{ - T}}{{\rm{O}}_{\rm{t}}}} \right){\rm{ + HS}}\cdot \left( {{{\rm{T}}_{\rm{s}}}{\rm{ - T}}{{\rm{O}}_{\rm{t}}}} \right){\rm{ + HG}}\cdot \left( {{{\rm{T}}_{\rm{g}}}{\rm{ - T}}{{\rm{O}}_{\rm{t}}}} \right)} \right]{\rm{  + QSO  =  0  }}
+\end{equation}
+
+This can be solved for the outside surface temperature:
+
+\begin{equation}
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{\rm{t}}}{\rm{ + HA}}\cdot {{\rm{T}}_{\rm{a}}}{\rm{ + HS}}\cdot {{\rm{T}}_{\rm{s}}}{\rm{ + HG}}\cdot {{\rm{T}}_{\rm{g}}}}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HA + HS + HG}}}}} \right]{\rm{  }}
+\end{equation}
+
+The third and fourth representations occur when the outside surface has been covered with movable insulation. The insulation has a conductance of UM. The thermal network in Figure~\ref{fig:thermal-network-for-outside-moveable} represents this case.The insulation must be mass-less because it is not generally possible to perform a correct thermal balance at the juncture of two surfaces each modeled by CTF.
+
+The equation for the thermal balance between the surface and the insulation is
+
+\begin{equation}
+\left[ {{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {{\rm{Y}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{I}}_t} - {{\rm{X}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{O}}_{\rm{t}}} + {\rm{UM}}\cdot \left( {{\rm{TM - T}}{{\rm{O}}_{\rm{t}}}} \right)} \right]{\rm{ + QSO  =  0}}
+\end{equation}
+
+Which can be rewritten to solve for TO :
+
+\begin{equation}
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{\rm{t}}}{\rm{ + UM}}\cdot {\rm{TM}}}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + UM}}}}} \right]{\rm{  }}
+\end{equation}
+
+Depending on whether or not the detailed or simple algorithm for surface conductance is being used, there are two expressions for TM, the outside temperature of the insulation. For the simple conductance:
+
+\begin{equation}
+{\rm{TM}} = \left[ {\frac{{{\rm{QSM + UM}}\cdot {\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ + HO}}\cdot {{\rm{T}}_{\rm{a}}}}}{{{\rm{UM + HO}}}}} \right]
+\end{equation}
+
+For the detailed conductance:
+
+\begin{equation}
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{QSM}} + {\rm{UM}}\cdot {\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ + HA}}\cdot {{\rm{T}}_{\rm{a}}}{\rm{ + HS}}\cdot {{\rm{T}}_{\rm{s}}}{\rm{ + HG}}\cdot {{\rm{T}}_{\rm{g}}}}}{{{\rm{UM + HA + HS + HG}}}}} \right]{\rm{  }}
+\end{equation}
+
+In this case the values of HA, HS and HG must be found by using an estimated value of TM in place of TO.
+
+\begin{figure}[hbtp] % fig 29
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image420.png}
+\caption{Thermal Network for Simple Outside Surface Coefficient \protect \label{fig:thermal-network-for-simple-outside-surface}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 30
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image421.png}
+\caption{Thermal Network for Detailed Outside Surface Coefficient \protect \label{fig:thermal-network-for-detailed-outside-surface}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 31
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image422.png}
+\caption{Thermal Network for Outside Moveable Insulation \protect \label{fig:thermal-network-for-outside-moveable}}
+\end{figure}
+
+\subsection{Heat Balance Cases}\label{heat-balance-cases}
+
+TO\(_{t}\) and TI\(_{t}\) are related through the Y\(_{0}\)CTF. However TI\(_{t}\) is also unknown. While it is possible to combine the outside and the inside surface heat balances to compute TO\(_{t}\) and TI\(_{t}\) simultaneously, TARP uses a simpler procedure where TO\(_{t}\) is based on a previous value of TI. When Y\(_{0}\) is small, as occurs in well insulated or very massive surfaces, TI\(_{t}\) can be replaced by TI\(_{t-1}\) (which is known for the previous hour's heat balance) without significantly effecting the value of TO\(_{t}\) When Y\(_{0}\) is large, TO and TI can so strongly be coupled that separate outside and inside heat balances do not work because the environment and zone temperatures have negligible influence on the heat balances. The TARP uses the inside surface heat balance to couple TO\(_{t}\) with TZ and TR. These two temperatures are less strongly influenced by TO and allow a reasonable heat balance. On the first heat balance iteration, TZ and TR are the values at time t-1. The user may optionally require that TO\(_{t}\) be recomputed with every iteration of TI\(_{t}\). ~In this case TZ and TR have values from the previous iteration and a true simultaneous solution is achieved. In most conventional constructions, recomputing TO\(_{t}\) does not significantly change the computed zone loads and temperatures. The inside surface heat balance is given by
+
+\begin{equation}
+{\rm{T}}{{\rm{I}}_{\rm{t}}} = \left[ {\frac{{KI{P_t} + QSI + HC\cdot TZ + HR\cdot TR + {Y_0}\cdot TO}}{{{Z_0} + HC + HR}}} \right]
+\end{equation}
+
+The surface heat balances can be combined in eight ways according to conditions for calculations of the outside surface temperature
+
+\begin{equation}
+{F_1} = \left[ {\frac{{{Y_0}}}{{{Z_0} + HI + HR}}} \right]
+\end{equation}
+
+\begin{equation}
+{F_2} = \left[ {\frac{{UM}}{{UM + HO}}} \right]
+\end{equation}
+
+\begin{equation}
+{F_3} = \left[ {\frac{{UM}}{{UM + HA + HS + HG}}} \right]
+\end{equation}
+
+\subsubsection{\texorpdfstring{Case1: Y\(_{0}\)~ small, simple conductance, no movable insulation:}{Case1: Y\_\{0\}~ small, simple conductance, no movable insulation:}}\label{case1-yux5f0-small-simple-conductance-no-movable-insulation}
+
+From Equation
+
+\begin{equation}
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{{\rm{t - 1}}}}{\rm{ + HO}}\cdot {{\rm{T}}_{\rm{a}}}}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HO}}}}} \right]{\rm{  }}
+\end{equation}
+
+\subsubsection{\texorpdfstring{Case2: Y\(_{0}\) not small, simple conductance, no movable insulation:}{Case2: Y\_\{0\} not small, simple conductance, no movable insulation:}}\label{case2-yux5f0-not-small-simple-conductance-no-movable-insulation}
+
+From Equations and
+
+\begin{equation}
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {\rm{HO}}\cdot {{\rm{T}}_{\rm{a}}} + {{\rm{F}}_1}\cdot \left( {{\rm{KI}}{{\rm{P}}_{\rm{t}}}{\rm{ + QSI + HI}}\cdot {\rm{TZ + HR}}\cdot {\rm{TR}}} \right)}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HO - }}{{\rm{F}}_{\rm{1}}}\cdot {{\rm{Y}}_0}}}} \right]{\rm{  }}
+\end{equation}
+
+\subsubsection{\texorpdfstring{Case3: Y\(_{0}\)~ small, detailed conductance, no movable insulation:}{Case3: Y\_\{0\}~ small, detailed conductance, no movable insulation:}}\label{case3-yux5f0-small-detailed-conductance-no-movable-insulation}
+
+From Equation
+
+\begin{equation}
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{{\rm{t - 1}}}}{\rm{ + HA}}\cdot {{\rm{T}}_{\rm{a}}} + {\rm{HS}}\cdot {{\rm{T}}_{\rm{s}}} + {\rm{HG}}\cdot {{\rm{T}}_{\rm{g}}}}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HA + HS + HG}}}}} \right]{\rm{  }}
+\end{equation}
+
+\subsubsection{\texorpdfstring{Case4: Y\(_{0}\) not small, detailed conductance, no movable insulation:}{Case4: Y\_\{0\} not small, detailed conductance, no movable insulation:}}\label{case4-yux5f0-not-small-detailed-conductance-no-movable-insulation}
+
+From Equations and
+
+\begin{equation}
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {\rm{HA}}\cdot {{\rm{T}}_{\rm{a}}} + {\rm{HS}}\cdot {{\rm{T}}_{\rm{s}}} + {\rm{HG}}\cdot {{\rm{T}}_{\rm{g}}} + {{\rm{F}}_{\rm{1}}}\cdot \left( {{\rm{KI}}{{\rm{P}}_{\rm{t}}}{\rm{ + QSI + HI}}\cdot {\rm{TZ + HR}}\cdot {\rm{TR}}} \right)}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HA + HS + HG - }}{{\rm{F}}_1}\cdot {{\rm{Y}}_0}}}} \right]{\rm{  }}
+\end{equation}
+
+\subsubsection{\texorpdfstring{Case5: Y\(_{0}\)~ small, simple conductance, with movable insulation:}{Case5: Y\_\{0\}~ small, simple conductance, with movable insulation:}}\label{case5-yux5f0-small-simple-conductance-with-movable-insulation}
+
+From Equations and \(TO_t = \left[ \frac{ KOP_t + QSO + HA \cdot T_a + HS \cdot T_s + HG \cdot T_g + F_1 \cdot \left( KIP_t QS1 + HI \cdot TZ + HR \cdot TR \right) } { X_0 + HA + HS + HG - F_1 \cdot Y_0 } \right]\)
+
+\subsubsection{\texorpdfstring{Case6: Y\(_{0}\) not small, simple conductance, with movable insulation:}{Case6: Y\_\{0\} not small, simple conductance, with movable insulation:}}\label{case6-yux5f0-not-small-simple-conductance-with-movable-insulation}
+
+From Equations , and
+
+\begin{equation}
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{F}}_2}\cdot \left( {{\rm{QSM + HO}}\cdot {{\rm{T}}_{\rm{a}}}} \right) + {{\rm{F}}_1}\cdot \left( {{\rm{KI}}{{\rm{P}}_{\rm{t}}}{\rm{ + QSI + HI}}\cdot {\rm{TZ + HR}}\cdot {\rm{TR}}} \right)}}{{{{\rm{X}}_{\rm{0}}} + {\rm{UM - }}{{\rm{F}}_{\rm{2}}}\cdot {\rm{UM - }}{{\rm{F}}_{\rm{1}}}\cdot {{\rm{Y}}_{\rm{0}}}}}} \right]{\rm{  }}
+\end{equation}
+
+\subsubsection{\texorpdfstring{Case7: Y\(_{0}\)~ small, detailed conductance, with movable insulation:}{Case7: Y\_\{0\}~ small, detailed conductance, with movable insulation:}}\label{case7-yux5f0-small-detailed-conductance-with-movable-insulation}
+
+From Equations and
+
+\begin{equation}
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{{\rm{t - 1}}}}{\rm{ + }}{{\rm{F}}_{\rm{3}}}\left( {{\rm{QSM + HA}}\cdot {{\rm{T}}_{\rm{a}}}{\rm{ + HS}}\cdot {{\rm{T}}_{\rm{s}}}{\rm{ + HG}}\cdot {{\rm{T}}_{\rm{g}}}} \right)}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + UM - }}{{\rm{F}}_{\rm{3}}}\cdot {\rm{UM}}}}} \right]{\rm{  }}
+\end{equation}
+
+\subsubsection{\texorpdfstring{Case8: Y\(_{0}\) not small, detailed conductance, with movable insulation:}{Case8: Y\_\{0\} not small, detailed conductance, with movable insulation:}}\label{case8-yux5f0-not-small-detailed-conductance-with-movable-insulation}
+
+From Equations , and
+
+\begin{equation}
+\medmuskip=0mu
+\thinmuskip=0mu
+\thickmuskip=0mu
+\nulldelimiterspace=0pt
+\scriptspace=0pt
+{\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{F}}_1}\cdot \left( {{\rm{KI}}{{\rm{P}}_{\rm{t}}}{\rm{ + QSI + HI}}\cdot {\rm{TZ + HR}}\cdot {\rm{TR}}} \right){\rm{ + }}{{\rm{F}}_{\rm{3}}}\left( {{\rm{QSM + HA}}\cdot {{\rm{T}}_{\rm{a}}}{\rm{ + HS}}\cdot {{\rm{T}}_{\rm{s}}}{\rm{ + HG}}\cdot {{\rm{T}}_{\rm{g}}}} \right)}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + UM - }}{{\rm{F}}_{\rm{3}}}\cdot {\rm{UM - }}{{\rm{F}}_{\rm{1}}}\cdot {{\rm{Y}}_{\rm{0}}}}}} \right]{\rm{  }}
+\end{equation}
+
+\subsection{Fortran Algorithm Examples}\label{fortran-algorithm-examples}
+
+\subsubsection{\texorpdfstring{Case5: Y\(_{0}\)~ small, simple conductance, with movable insulation:}{Case5: Y\_\{0\}~ small, simple conductance, with movable insulation:}}\label{case5-yux5f0-small-simple-conductance-with-movable-insulation-1}
+
+From Equation
+
+\begin{lstlisting}
+! Outside heat balance case: Movable insulation, slow conduction, simple convection
+ F2 = DBLE(HmovInsul) / ( DBLE(HmovInsul) + DBLE(HExtSurf(SurfNum)) )
+ TH(SurfNum,1,1) = (-CTFConstOutPart(SurfNum)                       &
+                    +DBLE(QRadSWOutAbs(SurfNum) )                   &
+           +Construct(ConstrNum)\%CTFCross(0)*TempSurfIn(SurfNum)   &
+           +F2* ( DBLE(QRadSWOutMvIns(SurfNum))                     &
+           + DBLE(HExtSurf(SurfNum))* DBLE(TempExt) ) )             &
+           /( Construct(ConstrNum)\%CTFOutside(0) + DBLE(HmovInsul) &
+          - F2* DBLE(HMovInsul))
+\end{lstlisting}
+
+\subsubsection{\texorpdfstring{Case6: Y\(_{0}\) not small, simple conductance, with movable insulation:}{Case6: Y\_\{0\} not small, simple conductance, with movable insulation:}}\label{case6-yux5f0-not-small-simple-conductance-with-movable-insulation-1}
+
+From Equation
+
+\begin{lstlisting}
+! Outside heat balance case: Movable insulation, quick conduction, simple convection
+F2 = DBLE(HmovInsul) / ( DBLE(HmovInsul) + DBLE(HExtSurf(SurfNum)) )
+TH(SurfNum,1,1) = (-CTFConstOutPart(SurfNum)              &
+DBLE(QRadSWOutAbs(SurfNum))                               &
++F2*( DBLE(QRadSWOutMvIns(SurfNum))                       &
++DBLE(HExtSurf(SurfNum))* DBLE(TempExt) )                 &
++F1*( CTFConstInPart(SurfNum)                             &
++ DBLE(QRadSWInAbs(SurfNum))                              &
++ DBLE(QRadThermInAbs(SurfNum))                           &
++ DBLE(HConvIn(SurfNum))*MAT(ZoneNum)                     &
++ DBLE(NetLWRadToSurf(SurfNum)) ) )                       &
+/( Construct(ConstrNum)\%CTFOutside(0) + DBLE(HmovInsul)  &
+-F2* DBLE(HMovInsul )- F1*Construct(ConstrNum)\%CTFCross(0) )
+\end{lstlisting}
+
+\subsubsection{\texorpdfstring{Case7: Y\(_{0}\)~ small, detailed conductance, with movable insulation:}{Case7: Y\_\{0\}~ small, detailed conductance, with movable insulation:}}\label{case7-yux5f0-small-detailed-conductance-with-movable-insulation-1}
+
+From Equation
+
+\begin{lstlisting}
+! Outside heat balance case: Movable insulation, slow conduction, detailed convection
+F2 = DBLE(HMovInsul)/ ( DBLE(HMovInsul) + DBLE(HExtSurf(SurfNum))  &
+           +DBLE(HSky) + DBLE(HGround) )
+TH(SurfNum,1,1) = (-CTFConstOutPart(SurfNum)                       &
++DBLE(QRadSWOutAbs(SurfNum))                                       &
++Construct(ConstrNum)\%CTFCross(0)*TempSurfIn(SurfNum)             &
++F2*( DBLE(QRadSWOutMvIns(SurfNum))                                &
++DBLE(HExtSurf(SurfNum))*DBLE(TempExt)                             &
++DBLE(HSky)*DBLE(SkyTemp)                                          &
++DBLE(HGround)*DBLE(OutDryBulbTemp) ) )                            &
+/( Construct(ConstrNum)\%CTFOutside(0)                             &
++DBLE(HMovInsul) - F2*DBLE(HMovInsul) )
+\end{lstlisting}
+
+\subsubsection{\texorpdfstring{Case8: Y\(_{0}\) not small, detailed conductance, with movable insulation:}{Case8: Y\_\{0\} not small, detailed conductance, with movable insulation:}}\label{case8-yux5f0-not-small-detailed-conductance-with-movable-insulation-1}
+
+From Equation
+
+\begin{lstlisting}
+! Outside heat balance case: Movable insulation, quick conduction, detailed convection
+F2 = DBLE(HMovInsul)/ ( DBLE(HMovInsul) + DBLE(HExtSurf(SurfNum)) &
+           +DBLE(HSky) + DBLE(HGround) )
+TH(SurfNum,1,1) = (-CTFConstOutPart(SurfNum)                      &
++DBLE(QRadSWOutAbs(SurfNum))                                      &
++F1*( CTFConstInPart(SurfNum)                                     &
++DBLE(QRadSWInAbs(SurfNum))                                       &
++DBLE(QRadThermInAbs(SurfNum))                                    &
++DBLE(HConvIn(SurfNum))*MAT(ZoneNum)                              &
++DBLE(NetLWRadToSurf(SurfNum)) )                                  &
++F2*( DBLE(QRadSWOutMvIns(SurfNum))                               &
++DBLE(HExtSurf(SurfNum))*DBLE(TempExt)                            &
++DBLE(HSky)*DBLE(SkyTemp)                                         &
++DBLE(HGround)*DBLE(OutDryBulbTemp) )                             &
+/( Construct(ConstrNum)\%CTFOutside(0)                            &
++DBLE(HMovInsul) - F2*DBLE(HMovInsul)                             &
+-F1*Construct(ConstrNum)\%CTFCross(0) )
+\end{lstlisting}
+
+\subsection{Fortran Variable Descriptions}\label{fortran-variable-descriptions}
+
+% table 16
+{\scriptsize
+\begin{longtable}[c]{p{1.8in}p{1.2in}p{0.9in}p{0.9in}p{1.2in}}
+
+\caption{Fortran Variables and Descriptions \label{table:fortran-variables-and-descriptions}} \tabularnewline
+\toprule 
+FORTRAN Variable & Description & Tarp Variable & Units & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Fortran Variables and Descriptions} \tabularnewline
+\toprule 
+FORTRAN Variable & Description & Tarp Variable & Units & Description \tabularnewline
+\midrule
+\endhead
+
+TH(SurfNum,1,1) & Temperature History(SurfNum,Hist Term,In/Out), where: Hist Term (1 = Current Time, 2-MaxCTFTerms = previous times), In/Out (1 = Outside, 2 = Inside) & TO & C & Temperature of outside of surface I at time t \tabularnewline
+Construct(ConstrNum) \% CTFCross(0) & Cross or Y term of the CTF equation & Y0 & W/m  K & Cross CTF term \tabularnewline
+Construct(ConstrNum) \% CTFInside(0) & Inside or Z terms of the CTF equation & Z0 & W/m  K & Inside CTF term \tabularnewline
+Construct(ConstrNum) \% CTFOutside(0) & Outside or X terms of the CTF equation & X0 & W/m  K & Outside CTF term \tabularnewline
+CTFConstInPart(SurfNum) & Constant inside portion of the CTF calculation & KIP & W/m & Portion of inward conductive flux based on previous temperature and flux history terms \tabularnewline
+CTFConstOutPart(SurfNum) & Constant Outside portion of the CTF calculation & KOP & W/m & Portion of outward conductive flux based on previous temperature and flux history terms \tabularnewline
+F1, F2, F3 & Intermediate calculation variables & F1, F2, F3 & ~ & Radiation interchange factor between surfaces \tabularnewline
+GroundTemp & Ground surface temperature & T & C & Temperature of ground at the surface exposed to the outside environment \tabularnewline
+HConvIn(SurfNum) & Inside convection coefficient & HI & W/m  K & Inside convection coefficient \tabularnewline
+HExtSurf(SurfNum) & Outside Convection Coefficient & HO, HA & W/m  K & Overall outside surface conductance \tabularnewline
+HGround & Radiant exchange (linearized) coefficient & HG & W/m  K & Radiative conductance (outside surface to ground temperature \tabularnewline
+HmovInsul & Conductance or "h" value of movable insulation & UM & W/m  K & Conductance of Movable insulation \tabularnewline
+HSky & Radiant exchange (linearized) coefficient & HS & W/m  K & Radiative conductance (outside surface to sky radiant temperature \tabularnewline
+MAT(ZoneNum) & Zone temperature & TZ & C & Temperature of zone air \tabularnewline
+NetLWRadToSurf(SurfNum) & Net interior longwave radiation to a surface from other surfaces & HR*TR & W/m & Net surface to surface radiant exchange \tabularnewline
+QRadSWInAbs(SurfNum) & Short-wave radiation absorbed on inside of opaque surface & QSI & W/m & Short wave radiant flux absorbed at inside of surface \tabularnewline
+QRadSWOutAbs(SurfNum) & Short wave radiation absorbed on outside opaque surface & QSO & W/m & Short wave radiant flux absorbed at outside of surface \tabularnewline
+QRadSWOutMvIns(SurfNum) & Short wave radiation absorbed on outside of movable insulation & QSM & W/m & Short wave radiant flux absorbed at surface of movable insulation \tabularnewline
+QRadThermInAbs(SurfNum) & Thermal Radiation absorbed on inside surfaces & ~ & W/m & Longwave radiant flux from internal gains \tabularnewline
+SkyTemp & Sky temperature & T & C & Sky temp \tabularnewline
+TempExt & Exterior surface temperature or exterior air temperature & TM, T & C & Temperature of external surface of movable insulation or outside ambient air temperature \tabularnewline
+TempSurfIn(SurfNum) & Temperature of inside surface for each heat transfer surface & TI & C & Temperature of inside of surface I at time t-1 \tabularnewline
+\bottomrule
+\end{longtable}}
+
+\subsection{References}\label{references-044}
+
+Walton, G.N. 1983. ``The Thermal Analysis Research Program Reference Manual Program (TARP)'', National Bureau of Standards (now National Institute of Standards and Technology).
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/transparent-insulation-material.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/transparent-insulation-material.tex
new file mode 100644
index 00000000000..88d410592d8
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/transparent-insulation-material.tex
@@ -0,0 +1,271 @@
+\section{Transparent Insulation Material (TIM)}\label{transparent-insulation-material-tim}
+
+\subsection{Introduction}\label{introduction-001}
+
+The input object ``SurfaceControl:MovableInsulation'' allows modeling Transparent Insulation Materials (TIM) that were originally designed for use in solar collector systems, where there was a need to increase the insulation in the solar collector without dramatically reducing solar energy transmittance.~ Transparent Insulation provides both these properties, insulation from heat loss and transmittance of solar energy.~ The combination of these properties is achieved, because Transparent Insulation is a transmitter of short wave radiation but a barrier to longwave radiation.~ Therefore short wave solar radiation passes through the Transparent Insulation and longwave heat radiation is insulated by the transparent insulation. Incident solar energy falling on the transparent insulation is reflected and re-reflected within the material and eventually falls on the absorber.~ In addition, transparent insulation materials also have increase thermal resistance due to conduction in comparison to standard glass.
+
+Transparent Insulation is now used in the housing industry as a passive solar feature. It is attached to the walls of houses for insulation and solar energy gains are transmitted to the house during the right ambient conditions. The walls of the house act as a thermal mass, absorbing the sunlight at the surface and converting it into heat which is slowly transmitted to the inside of the house.
+
+\subsection{Comparison of Opaque and Transparent Insulation}\label{comparison-of-opaque-and-transparent-insulation}
+
+A qualitative comparison between the performance of Transparent Insulation and opaque insulation is shown diagrammatically in the figure below. The upper half of the figure represents approximate heat transfer through the wall cross-section for both transparent and opaque insulation cases.~ The lower half of this figure shows representative temperature variations through the wall cross-sections for different solar conditions.
+
+\begin{figure}[hbtp] % fig 26
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image399.png}
+\caption{Energy Flows of Opaquely and Transparently Insulated Walls (Wood and Jesch 1993). \protect \label{fig:energy-flows-of-opaquely-and-transparently}}
+\end{figure}
+
+While both types of insulation reduce energy losses from the building via conduction through the building surfaces, transparent insulation allows solar radiation to penetrate deeper into the surface construction.~ This increases the construction internal temperature and can result in heat being conducted into the building under the proper weather conditions.~ This can be seen in the lower half of the above figure during a sunny day.~ The temperature plot shows a maximum between the transparent insulation and the rest of the surface construction.~ As a result, the temperature gradient results in heat transfer from this point into the interior space, causing a heating effect on the zone.~ Thus, the advantage of transparent insulation is that, like opaque insulation, it reduces winter heat transfer losses during low or no solar conditions and has the possibility of providing heating during sunny winter days.~ It should be noted that this same effect in summer could be detrimental to the cooling loads of a building since the introduction of solar radiation closer to the space will increase the solar heating within the zone.~ Most systems counteract this with a shading device or with sophisticated transparent insulation systems.
+
+\subsection{Types of Transparent Insulation Materials}\label{types-of-transparent-insulation-materials}
+
+Transparent insulation can be classified into four general categories:
+
+Absorber Parallel Covers
+
+Cavity Structures
+
+Absorber Vertical Covers
+
+Quasi-Homogeneous Structures
+
+Cross-sections of each of these types is shown in the figure below.~ The arrows in these diagrams indicate solar rays and the path these rays trace as they are transmitted through the transparent insulation layer.~ The most advantageous set-up (see absorber-parallel below) would send most of the rays downward towards the interior of the building while minimizing the rays that are reflected back to the exterior environment.
+
+\begin{figure}[hbtp] % fig 27
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image400.png}
+\caption{Geometrical Categories of Classification for Transparent Insulation Material (Wood and Jesch 1993). \protect \label{fig:geometrical-categories-of-classification-for}}
+\end{figure}
+
+\subsection{TIM- Basic Mathematical Model}\label{tim--basic-mathematical-model}
+
+\begin{figure}[hbtp] % fig 28
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image401.png}
+\caption{Cross Section of TIM and wall, showing energy flow \protect \label{fig:cross-section-of-tim-and-wall-showing-energy}}
+\end{figure}
+
+Mathematical model to calculate amount of energy absorbed at the surface of moveable insulation (TIM) and at the Outside surface of the Wall.
+
+\begin{equation}
+QSM = {\alpha_{TIM}}\cdot Incident\;Solar
+\end{equation}
+
+The total solar gain on any exterior surface is a combination of the absorption of direct and diffuse solar radiation given by
+
+\textbf{\emph{\(Incident\;Solar = ({I_b}\cdot \cos \theta \cdot \frac{{{S_s}}}{S} + {I_s}\cdot {F_{ss}} + {I_g}\cdot {F_{sg}})\) ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~}}
+
+Where,
+
+$\alpha$ = solar absorptance of the surface
+
+$\theta$ = angle of incidence of the sun's rays
+
+S = area of the surface
+
+S\(_{s}\) = sunlit area of the surface
+
+I\(_{b}\) = intensity of the beam (direct) radiation
+
+I\(_{s}\) = intensity of the sky diffuse radiation
+
+I\(_{g}\) = intensity of the beam (direct) radiation
+
+F\(_{ss}\) = angle factor between the surface and the sky
+
+F\(_{sg}\) = angle factor between the surface and the ground
+
+Now,
+
+\begin{equation}
+{\alpha_{wall}} + {\rho_{wall}} = 1
+\end{equation}
+
+The model for TIM is simplified in that it assumes that absorption of solar radiation takes place at the inside and outside of the TIM only, not throughout the material.~ In addition, the model assumes that the solar radiation absorbed during the first pass through the TIM affects the outside surface of the TIM while the solar radiation reflected at the outer wall surface that gets absorbed during the back reflection will affect the inside TIM surface (which is also the outside surface of the wall).~ Thus, the heat absorbed at the outside of the TIM is as shown in Equation .
+
+The heat absorbed at the inside of the TIM/outside of the wall includes two components.~ The first component is the amount of solar that is transmitted through the TIM and absorbed at the inside of the wall.~ This is characterized by the following equation:
+
+\begin{equation}
+First\,pass\,solar\,absorbed\,by\,wall = \left( {{\tau_{TIM}}\cdot Incident\,Solar} \right)\cdot \left( {{\alpha_{wall}}} \right)
+\end{equation}
+
+The amount of solar absorbed by the TIM and aggregated at the inside surface of the TIM (outside wall surface) is:
+
+\begin{equation}
+Amount\,of\,back\,reflection\,absorbed\,by\,TIM = \left( {{\tau_{TIM}}\cdot Incident\,Solar} \right)\cdot \left( {1 - {\alpha_{wall}}} \right)\cdot {\alpha_{TIM}}
+\end{equation}
+
+The heat absorbed at the interface between the wall and the TIM includes both of these components.~ Thus, QSO is equal to:
+
+\begin{equation}
+QSO = \left( {{\tau_{TIM}}\cdot Incident\,Solar} \right)\cdot \left\{ {{\alpha_{wall}} + \left( {1 - {\alpha_{wall}}} \right)\cdot \alpha {}_{TIM}} \right\}
+\end{equation}
+
+Substituting the definition for QSM into this equation and rearranging results in:
+
+\begin{equation}
+QSO = \left\{ {\frac{{{\tau_{TIM}}\cdot QSM}}{{{\alpha_{TIM}}}}} \right\}\cdot \left\{ {{\alpha_{wall}} + \left( {1 - {\alpha_{wall}}} \right)\cdot {\alpha_{TIM}}} \right\}
+\end{equation}
+
+\begin{equation}
+QSO = \left( {{\tau_{TIM}}\cdot QSM} \right)\cdot \left\{ {\left( {\frac{{{\alpha_{wall}}}}{{{\alpha_{TIM}}}}} \right) + \left( {1 - {\alpha_{wall}}} \right)} \right\}
+\end{equation}
+
+Where,
+
+\emph{QSM}~~~~~~~~~~ = Short wave radiant flux absorbed at surface of Movable Insulation
+
+\emph{QSO}~~~~~~~~~~ = Short wave radiant flux absorbed at surface of Wall.
+
+$\alpha$\(_{TIM}\) = Absorptance of TIM
+
+$\tau$\(_{TIM}\) = Transmittance of TIM.
+
+$\alpha$\(_{WALL}\) = Absorptance of Wall.
+
+$\rho$\(_{WALL}\) = Reflectance of Wall surface
+
+Following is the FORTRAN Code used in the HeatBalanceSurfaceManager module, to determine the short wave radiation absorbed on outside of movable insulation and the short wave radiation absorbed on outside of opaque surface of the wall.
+
+\begin{lstlisting}
+IF (Surface(SurfNum)\%MaterialMovInsulExt.GT.0)                                           &
+
+    CALL EvalOutsideMovableInsulation(SurfNum,HMovInsul,RoughIndexMovInsul,AbsExt)
+
+    IF (HMovInsul \textgreater{} 0) THEN    ! Movable outside insulation in place
+
+      QRadSWOutMvIns(SurfNum) = QRadSWOutAbs(SurfNum)*AbsExt                              &
+
+                       /Material(Construct(ConstrNum)\%LayerPoint(1))\%AbsorpSolar
+
+!   For Transparent Insulation
+
+      QRadSWOutAbs(SurfNum) = Material(Surface(SurfNum)\%MaterialMovInsulExt)\%Trans      &
+
+             *QRadSWOutMvIns(SurfNum)*                                                    &
+
+                 (  (Material(Construct(ConstrNum)\%LayerPoint(1))\%AbsorpSolar/AbsExt)   &
+
+                        +(1-Material(Construct(ConstrNum)\%LayerPoint(1))\%AbsorpSolar)~ )
+\end{lstlisting}
+
+\subsection{Sample Test Run Cases: -- Comparison}\label{sample-test-run-cases-comparison}
+
+A series of test cases were run in EnergyPlus to test the TIM model.~ The building was a very simple box with walls facing north, south, east, and west, all of which are exterior walls.~ Transparent Insulation Material has been applied to the south wall (except as noted in the table below).~ The program was run for this fictional 1 zone building located in Chanute AFB IL, for two design days, (21\(^{st}\) June and 21\(^{st}\) January).~ The main purpose of these runs was to verify that the transparent insulation model was predicting results that were reasonable using a simple test case.~ The winter design day was also modified in some runs to have a clearness of 1.0 so that the effect that solar radiation during winter-time conditions could be studied.
+
+The Transparent Insulation material is conceived by applying a SurfaceControl:MoveableInsulation on the exterior.~ In the test cases, the TIM had the following thermal properties:
+
+~~~ 0.05, ! Thickness \{m\}
+
+~~~ 0.90,~ ! Solar transmittance at normal incidence
+
+~~~ 0.031,~ ! Solar reflectance at normal incidence: front side
+
+~~~ 0.031,~ ! Solar reflectance at normal incidence: back side
+
+~~~ 0.90,~ ! Visible transmittance at normal incidence
+
+~~~ 0.05,~ ! Visible reflectance at normal incidence: front side
+
+~~~ 0.05,~ ! Visible reflectance at normal incidence: back side
+
+~~~ 0.0,~~ ! IR transmittance at normal incidence
+
+~~~ 0.84,~ ! IR emissivity: front side
+
+~~~ 0.84,~ ! IR emissivity: back side
+
+~~~ 0.04;~~ ! Conductivity \{W/m-K\}
+
+The Wall Construction is defined as an EXTWALL80 composed of 1'' Stucco, 4'' Common Brick and ¾'' Plaster or Gypboard.
+
+The following two tables shows data for two series of runs.~ The first ``summer table'' illustrates the execution of a summer design day.~ The second ``winter table'' shows winter conditions with clearness = 0 (the typical default for a winter design day) and clearness = 1 (to illustrate solar radiation with other winter conditions).~ Test cases included no movable insulation, moveable opaque insulation, and TIM on the exterior (south wall unless otherwise noted).~ Savings reported are heating and cooling loads for the design days only.~ The results showed that the TIM model was performing reasonably well and was producing results that were within expectations.
+
+% table 14
+{\scriptsize
+\begin{longtable}[c]{p{2.5in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}}
+\caption{TIM with Summer Conditions \label{table:tim-with-summer-conditions-000}} \tabularnewline
+\toprule 
+EXTWALL80 Construction & Conductivity & Thickness & Sensible Cooling Energy & Energy Saved \tabularnewline
+~ & [W/m-K] & [m] & [J] & [J] \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{TIM with Summer Conditions} \tabularnewline
+\toprule
+EXTWALL80 Construction & Conductivity & Thickness & Sensible Cooling Energy & Energy Saved \tabularnewline
+~ & [W/m-K] & [m] & [J] & [J] \tabularnewline
+\midrule
+\endhead
+
+Normal case Without any Insulation & 0.000 & 0.000 & 3.37E+08 & 0.00E+00 \tabularnewline
+With Dense Insulation Present & 0.040 & 0.025 & 3.17E+08 & 2.05E+07 \tabularnewline
+With Dense Insulation Present & 0.040 & 0.050 & 3.09E+08 & 2.84E+07 \tabularnewline
+With Dense Insulation Present & 0.040 & 0.100 & 3.02E+08 & 3.53E+07 \tabularnewline
+With TIM Present & 0.040 & 0.025 & 4.27E+08 & -9.01E+07 \tabularnewline
+With TIM Present & 0.040 & 0.050 & 4.63E+08 & -1.26E+08 \tabularnewline
+With TIM Present & 0.040 & 0.100 & 4.89E+08 & -1.52E+08 \tabularnewline
+With TIM Present R value = (0.05m,0.04W/m-K) & 0.035 & 0.044 & 4.63E+08 & -1.26E+08 \tabularnewline
+With TIM Present (EAST WALL) & 0.040 & 0.050 & 5.49E+08 & -2.12E+08 \tabularnewline
+With TIM Present (NORTH WALL) & 0.040 & 0.050 & 3.63E+08 & -2.57E+07 \tabularnewline
+With TIM Present (WEST WALL) & 0.040 & 0.050 & 5.64E+08 & -2.27E+08 \tabularnewline
+\bottomrule
+\end{longtable}}
+
+% table 15
+{\scriptsize
+\begin{longtable}[c]{p{1.0in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}p{0.75in}}
+\caption{TIM with Winter Conditions \label{table:tim-with-winter-conditions-000}} \tabularnewline
+\toprule 
+EXTWALL80 Construction & Conductivity & Thickness & Sensible Heating Energy & Energy Saved Winter Clearness = 0 & Sensible Heating Energy & Energy Saved Winter Clearness = 1 \tabularnewline
+~ & [W/m-K] & [m] & [J] & [J] & [J] & [J] \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{TIM with Winter Conditions} \tabularnewline
+\toprule 
+EXTWALL80 Construction & Conductivity & Thickness & Sensible Heating Energy & Energy Saved Winter Clearness = 0 & Sensible Heating Energy & Energy Saved Winter Clearness = 1 \tabularnewline
+~ & [W/m-K] & [m] & [J] & [J] & [J] & [J] \tabularnewline
+\midrule
+\endhead
+
+Normal case Without any Insulation & 0.000 & 0.000 & 1.47E+09 & 0.00E+00 & 1.05E+09 & 0.00E+00 \tabularnewline
+With Dense Insulation Present & 0.040 & 0.025 & 1.30E+09 & 1.70E+08 & 9.76E+08 & 7.40E+07 \tabularnewline
+With Dense Insulation Present & 0.040 & 0.050 & 1.26E+09 & 2.10E+08 & 9.73E+08 & 7.70E+07 \tabularnewline
+With Dense Insulation Present & 0.040 & 0.100 & 1.22E+09 & 2.50E+08 & 9.74E+08 & 7.60E+07 \tabularnewline
+With TIM Present & 0.040 & 0.025 & 1.30E+09 & 1.70E+08 & 5.66E+08 & 4.84E+08 \tabularnewline
+With TIM Present & 0.040 & 0.050 & 1.26E+09 & 2.10E+08 & 4.41E+08 & 6.09E+08 \tabularnewline
+With TIM Present & 0.040 & 0.100 & 1.22E+09 & 2.50E+08 & 3.57E+08 & 6.93E+08 \tabularnewline
+With TIM Present R value = (0.05m,0.04W/m-K) & 0.035 & 0.044 & 1.26E+09 & 2.10E+08 & 4.40E+08 & 6.10E+08 \tabularnewline
+With TIM Present (EAST WALL) & 0.040 & 0.050 & 1.26E+09 & 2.10E+08 & 7.36E+08 & 3.14E+08 \tabularnewline
+With TIM Present (NORTH WALL) & 0.040 & 0.050 & 1.24E+09 & 2.30E+08 & 8.31E+08 & 2.19E+08 \tabularnewline
+With TIM Present (WEST WALL) & 0.040 & 0.050 & 1.24E+09 & 2.30E+08 & 7.07E+08 & 3.43E+08 \tabularnewline
+\bottomrule
+\end{longtable}}
+
+\subsection{References}\label{references-046}
+
+P.O. Braun, A. Goetzberger, J. Schmid, and W.Stahl. Transparent Insulation of Building Facades- Steps from Research to Commercial applications, Fraunhofer Institute for Solar Energy Systems, Oltmannsstrasse 22, D-7800 Freiburg, Germany.
+
+Thermotropic materials and Systems for Overheating Protection.
+
+Robert Hausner. Arbeitsgemeinschaft Erneuerbare energie, Transparent Insulation- Areas of Application, Society for Renewable Energy.
+
+Werner J.Platzer. Transparent Insulation materials: a review, Fraunhofer Institute for Solar Energy Systems, Oltmannsstr. 5, D-79100 Freiburg, Germany.
+
+Volker Wittwer. The use of Transparent Insulation Materials and Optical Switching Layers in Window Systems, Fraunhofer Institute for Solar Energy Systems, Oltmannsstr. 5, D-79100 Freiburg, Germany.
+
+M. Wood and L.F. Jesch. 1993. Transparent insulation technology: a technical note, Ambient Press Limited.
+
+Façade Modules with back-ventilated Transparent Insulation- Research and Development toward Series Application.
+
+Two 0-Energy Houses,
+
+Advanced Building Technologies -- Transparent Insulation Materials ( TIM ).
+
+Transparent Insulation,
+
+G. Verbeeck, H. Hens. Transparent Insulation: an alternative solution for summer discomfort. Die neue Transparenz: Warmedamm-Verbund- system StoTherm Solar.
+
+E.Lindauer, H.Leonhardt. Brauchwasservorerwarmmung mit transparent gedammten Bauteilen ( Hybridsystem ), Fraunhofer- Institut fur Bauphysik.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-finite.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-finite.tex
new file mode 100644
index 00000000000..8f38b76444b
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-finite.tex
@@ -0,0 +1,21 @@
+\section{Undisturbed Ground Temperature Model: Finite Difference}\label{undisturbed-ground-temperature-model-finite-difference}
+
+\subsubsection{Approach}\label{approach-003}
+
+This model uses a 1D implicit finite difference heat transfer model to determine the steady-periodic annual ground temperature. The model, which uses a daily timestep, is run through an annual simulation using the user provided weather file to determine daily averages for global horizontal radiation, air temperature, relative humidity, and wind speed. Once the steady-periodic ground temperature has been determined, the temperatures are cached for use later in the simulation. The basis for the model was taken from Xing, 2014, however, the numerical methods were adapted from those described in Lee, 2013; the latter uses an implicit numerically stable finite difference method, whereas the former utilized an explicit, conditionally stable method.
+
+Surface heat balance boundary conditions are similar what is described in Herb et al., 2008. Evapotranspiration is considered as described by Allen et al., 1998. Soil freezing given the assumed stagnant soil moisture content is also considered.
+
+\subsubsection{Limitations}\label{limitations}
+
+The model does not consider the effects of vegitative canopy layers, snow cover, ground water flow, ground moisture transport, or surface runoff.
+
+\subsubsection{References}\label{references-048}
+
+Allen, R.G., L.S. Pereira, D. Raes, M. Smith. 1998. \emph{Crop Evapotranspiration - Guidelines for Computing Crop Water Requirements.} Food and Agriculture Organization of the United Nations.
+
+Herb, W.R., B. Janke, O. Mohseni, \& H.G. Stefan. 2008. `Ground Surface Temperature Simulation for Different Land Covers.' Journal of Hydrology, 356: pp 327-343.
+
+Lee, E.S. 2013. An Improved Hydronic Loop System Solution Algorithm with a Zone-Coupled Horizontal Ground Heat Exchanger Model for Whole Building Energy Simulation. Ph.D.~Diss. Oklahoma State University, Stillwater, OK.
+
+Xing, L. 2014. Estimations of Undisturbed Ground Temperatures using Numerical and Analytical Modeling. Ph.D.~Diss. Oklahoma State University, Stillwater, OK.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-kusuda.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-kusuda.tex
new file mode 100644
index 00000000000..fe8882a3627
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-kusuda.tex
@@ -0,0 +1,15 @@
+\section{Undisturbed Ground Temperature Model: Kusuda-Achenbach}\label{undisturbed-ground-temperature-model-kusuda-achenbach}
+
+\subsubsection{Approach}\label{approach-004}
+
+The model uses the correlation developed by Kusuda \& Achenbach, 1965 which is shown below. The average soil surface temperature, amplitude of the soil surface temperature, and day of minimum surface temperature are all required inputs. These can be determined by using the CalcSoilSurfTemp preprocessor. They can also automatically be generated by leaving the parameters blank and including a Site:GroundTemperature:Shallow object in the input file.
+
+\begin{equation}
+T(z,t) = \bar{T}_{s} - \Delta\bar{T}_{s} \cdot e^{-z \cdot \sqrt{\frac{\pi}{\alpha\tau}}} \cdot cos\left( \frac{2\pi t}{\alpha t} - \theta \right)
+\end{equation}
+
+Where: \[T(z,t)\] is the undisturbed ground temperature as a function of time and depth \[\bar{T}_{s}\] is the average annual soil surface temperature, in deg C \[\Delta\bar{T}_{s}\] is the amplitude of the soil temperature change throughout the year, in deg C \[\theta\] is the phase shift, or day of minimum surface temperature \[\alpha\] is the themal diffusivity of the ground \[\tau\] is time constant, 365.
+
+\subsubsection{References}\label{references-049}
+
+Kusuda, T. and P.R. Achenbach. 1965. `Earth Temperatures and Thermal Diffusivity at Selected Stations in the United States.' \emph{ASHRAE Transactions}. 71(1): 61-74.
diff --git a/doc/engineering-reference/src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-xing.tex b/doc/engineering-reference/src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-xing.tex
new file mode 100644
index 00000000000..a255b43caeb
--- /dev/null
+++ b/doc/engineering-reference/src/surface-heat-balance-manager-processes/undisturbed-ground-temperature-model-xing.tex
@@ -0,0 +1,15 @@
+\section{Undisturbed Ground Temperature Model: Xing}\label{undisturbed-ground-temperature-model-xing}
+
+\subsubsection{Approach}\label{approach-005}
+
+This model uses the correlation developed by Xing, 2014 to predict undisturbed ground temperature. The correlation parameters for 4000+ international locations can be found in Xing, 2014. The parameters were first determined by creating and validating a finite difference numerical model which used local weather data for boundary conditions. From the numerical model, the correlation parameters were determined to provide for this simplified design model.
+
+\begin{equation}
+T(z,t) = \bar{T}_{s} - \sum_{n = 1}^{2} \Delta\bar{T}_{s,n} \cdot e^{-z \cdot \sqrt{\frac{n\pi}{\alpha\tau}}} \cdot cos\left[ \frac{2 \pi n}{\tau} \left(t - \theta_{n} \right) - z \sqrt{\frac{n \pi}{\alpha \tau}} \right]
+\end{equation}
+
+\[T(z,t)\] is the undisturbed ground temperature as a function of time and depth \[\bar{T}_{s}\] is the average annual soil surface temperature, in deg C \[\Delta\bar{T}_{s,n}\] is the n-th amplitude of the soil temperature change throughout the year, in deg C \[\theta_{n}\] is the n-th phase shift, or day of minimum surface temperature \[\alpha\] is the themal diffusivity of the ground \[\tau\] is time constant, 365.
+
+\subsubsection{References}\label{references-050}
+
+Xing, L. 2014. Estimations of Undisturbed Ground Temperatures using Numerical and Analytical Modeling. Ph.D.~Diss. Oklahoma State University, Stillwater, OK. Advanced Surface Concepts = = = = = = = = = = = = = = = = = = = = = = = = =
diff --git a/doc/engineering-reference/src/title.tex b/doc/engineering-reference/src/title.tex
new file mode 100644
index 00000000000..63f37402bb8
--- /dev/null
+++ b/doc/engineering-reference/src/title.tex
@@ -0,0 +1 @@
+\input{../title}
diff --git a/doc/external-interfaces-application-guide/CMakeLists.txt b/doc/external-interfaces-application-guide/CMakeLists.txt
new file mode 100644
index 00000000000..98305813b14
--- /dev/null
+++ b/doc/external-interfaces-application-guide/CMakeLists.txt
@@ -0,0 +1,47 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/external-interfaces-application-guide.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/src/external-interfaces-application-guide.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/src/external-interface-s.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/src/external-interface-s/introduction.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/src/external-interface-s/coupling-energyplus-with-the-building.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/src/external-interface-s/bcvtb-examples.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/src/external-interface-s/coupling-energyplus-with-functional-mock-up.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/src/external-interface-s/fmu-examples.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/src/external-interface-s/exporting-energyplus-as-a-functional-mock-up.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/src/references.tex
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/../title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image004.png
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image005.png
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image006.png
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image007.png
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image008.png
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image016.png
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image033.png
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image034.png
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image035.png
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image036.png
+  ${CMAKE_SOURCE_DIR}/doc/external-interfaces-application-guide/media/image037.png
+) 
+
+SET( SOURCE_FILENAME "external-interfaces-application-guide" )
+SET( OUTPUT_FILENAME "ExternalInterfacesApplicationGuide" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/external-interfaces-application-guide/external-interfaces-application-guide.tex b/doc/external-interfaces-application-guide/external-interfaces-application-guide.tex
new file mode 100644
index 00000000000..2c7a43b2ae3
--- /dev/null
+++ b/doc/external-interfaces-application-guide/external-interfaces-application-guide.tex
@@ -0,0 +1,36 @@
+\input{../header}
+
+\title{External Interface(s) Application Guide}
+
+\hypersetup{unicode=true,
+            pdftitle={External Interface(s) Application Guide},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/external-interfaces-application-guide}
+
+\input{src/external-interface-s}
+
+\input{src/external-interface-s/introduction}
+
+\input{src/external-interface-s/coupling-energyplus-with-the-building}
+
+\input{src/external-interface-s/bcvtb-examples}
+
+\input{src/external-interface-s/coupling-energyplus-with-functional-mock-up}
+
+\input{src/external-interface-s/fmu-examples}
+
+\input{src/external-interface-s/exporting-energyplus-as-a-functional-mock-up}
+
+\input{src/references}
+
+\end{document}
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/ep.gif b/doc/external-interfaces-application-guide/media/ep.gif
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/ep.gif
rename to doc/external-interfaces-application-guide/media/ep.gif
diff --git a/doc/external-interfaces-application-guide/media/ep.png b/doc/external-interfaces-application-guide/media/ep.png
new file mode 100644
index 00000000000..a808760c870
Binary files /dev/null and b/doc/external-interfaces-application-guide/media/ep.png differ
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image004.png b/doc/external-interfaces-application-guide/media/image004.png
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image004.png
rename to doc/external-interfaces-application-guide/media/image004.png
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image005.png b/doc/external-interfaces-application-guide/media/image005.png
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image005.png
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diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image006.png b/doc/external-interfaces-application-guide/media/image006.png
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image006.png
rename to doc/external-interfaces-application-guide/media/image006.png
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image007.png b/doc/external-interfaces-application-guide/media/image007.png
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image007.png
rename to doc/external-interfaces-application-guide/media/image007.png
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image008.png b/doc/external-interfaces-application-guide/media/image008.png
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image008.png
rename to doc/external-interfaces-application-guide/media/image008.png
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image016.png b/doc/external-interfaces-application-guide/media/image016.png
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rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image016.png
rename to doc/external-interfaces-application-guide/media/image016.png
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image033.png b/doc/external-interfaces-application-guide/media/image033.png
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image033.png
rename to doc/external-interfaces-application-guide/media/image033.png
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image034.png b/doc/external-interfaces-application-guide/media/image034.png
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image034.png
rename to doc/external-interfaces-application-guide/media/image034.png
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image035.png b/doc/external-interfaces-application-guide/media/image035.png
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image035.png
rename to doc/external-interfaces-application-guide/media/image035.png
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image036.png b/doc/external-interfaces-application-guide/media/image036.png
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image036.png
rename to doc/external-interfaces-application-guide/media/image036.png
diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/media/image037.png b/doc/external-interfaces-application-guide/media/image037.png
similarity index 100%
rename from doc/src/docs/ExternalInterfaces_Application_Guide/media/image037.png
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diff --git a/doc/external-interfaces-application-guide/src/external-interface-s.tex b/doc/external-interfaces-application-guide/src/external-interface-s.tex
new file mode 100644
index 00000000000..647f4788d7f
--- /dev/null
+++ b/doc/external-interfaces-application-guide/src/external-interface-s.tex
@@ -0,0 +1 @@
+\chapter{External Interface(s)}\label{external-interfaces}
diff --git a/doc/external-interfaces-application-guide/src/external-interface-s/bcvtb-examples.tex b/doc/external-interfaces-application-guide/src/external-interface-s/bcvtb-examples.tex
new file mode 100644
index 00000000000..da428f3a55d
--- /dev/null
+++ b/doc/external-interfaces-application-guide/src/external-interface-s/bcvtb-examples.tex
@@ -0,0 +1,567 @@
+\section{BCVTB Examples}\label{bcvtb-examples}
+
+\subsection{Architecture of System}\label{architecture-of-system}
+
+The figure below shows the architecture of the connection between EnergyPlus and the BCVTB. The black objects are explained in this application guide, whereas the grey items are not specific to EnergyPlus and are explained in the BCVTB documentation. The BCVTB connects to the external interface in EnergyPlus. In the external interface, the input/output signals that are exchanged between the BCVTB and EnergyPlus are mapped to EnergyPlus objects. The subject of this External Interface Application Guide is how to configure this mapping and how to use these objects. For a detailed explanation of the grey items, we refer to the BCVTB documentation.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image004.png}
+\caption{Architecture of the BCVTB with the EnergyPlus client (black) and other clients (grey). \protect \label{fig:architecture-of-the-bcvtb-with-the-energyplus}}
+\end{figure}
+
+The external interface can map to three EnergyPlus input objects called ExternalInterface:Schedule, ExternalInterface:Actuator and ExternalInterface:Variable. The ExternalInterface:Schedule can be used to overwrite schedules, and the other two objects can be used in place of Energy Management System (EMS) actuators and EMS variables. The objects have similar functionality as the objects Schedule:Compact, EnergyManagementSystem:Actuator and EnergyManagementSystem:GlobalVariable, except that their numerical value is obtained from the external interface at the beginning of each zone time step, and will remain constant during this zone time step.
+
+Compared to EnergyManagementSystem:Actuator, the object ExternalInterface:Actuator has an optional field called ``initial value.'' If a value is specified for this field, then this value will be used during the warm-up period and the system sizing. If unspecified, then the numerical value for this object will only be used during the time stepping. Since actuators always overwrite other objects (such as a schedule), all these objects have values that are defined during the warm-up and the system sizing even if no initial value is specified. For the objects~ ExternalInterface:Schedule and ExternalInterface:Variable, the field ``initial value'' is required, and its value will be used during the warm-up period and the system-sizing.
+
+ExternalInterface:Variable is a global variable from the point of view of the EMS language. Thus, it can be used within any EnergyManagementSystem:Program in the same way as an EnergyManagementSystem:GlobalVariable or an EnergyManagementSystem:Sensor can be used.
+
+Although variables of type ExternalInterface:Variable can be assigned to EnergyManagmentSystem:Actuator objects, for convenience, there is also an object called ExternalInterface:Actuator. This object behaves identically to EnergyManagmentSystem:Actuator, with the following exceptions:
+
+\begin{itemize}
+\item
+  Its value is assigned by the external interface.
+\item
+  Its value is fixed during the zone time step because this is the synchronization time step for the external interface.
+\end{itemize}
+
+The external interface can also map to the EnergyPlus objects Output:Variable and EnergyManagementSystem:OutputVariable. These objects can be used to send data from EnergyPlus to the BCVTB at each zone time step.
+
+We will now present examples that use all of these objects. The following table shows which EnergyPlus features are used in the examples, which are all distributed with the BCVTB installation that can be obtained from the LBNL web site. Note -- these examples are NOT distributed with EnergyPlus installation because you need the special software to make them work.
+
+% table 1
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Overview of the EnergyPlus objects used in Examples \label{table:overview-of-the-energyplus-objects-used-in}} \tabularnewline
+\toprule 
+~ & Example 1 & Example 2 & Example 3 \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Overview of the EnergyPlus objects used in Examples} \tabularnewline
+\toprule 
+~ & Example 1 & Example 2 & Example 3 \tabularnewline
+\midrule
+\endhead
+
+ExternalInterface:Schedule & x & ~ & ~ \tabularnewline
+ExternalInterface:Actuator & ~ & X & ~ \tabularnewline
+ExternalInterface:Variable & ~ & ~ & x \tabularnewline
+Output:Variable & x & X & x \tabularnewline
+EnergyManagementSystem:OutputVariable & ~ & ~ & x \tabularnewline
+\bottomrule
+\end{longtable}
+
+To configure the data exchange, the following three steps are required from the user:
+
+1)~~~Create an EnergyPlus idf file.
+
+2)~~~Create an xml file that defines the mapping between EnergyPlus and BCVTB variables.
+
+3)~~~Create a Ptolemy model.
+
+These steps are described in the examples below. Prior to discussing the examples, we will explain the syntax of the xml configuration file that defines how data are mapped between the external interface and EnergyPlus.
+
+\subsection{XML Syntax}\label{xml-syntax}
+
+This section describes the syntax of the xml file that configures the data mapping between EnergyPlus and the external interface.
+
+The data mapping between EnergyPlus and the external interface is defined in an xml file called variables.cfg. This file needs to be in the same directory as the EnergyPlus idf file.
+
+The file has the following header:
+
+\textless{}?xml version = ``1.0'' encoding = ``ISO-8859-1''?\textgreater{}
+
+\textless{}!DOCTYPE BCVTB-variables SYSTEM ``variables.dtd''\textgreater{}
+
+Following the header is an element of the form
+
+\textless{}BCVTB-variables\textgreater{}
+
+\textless{}/BCVTB-variables\textgreater{}
+
+This element will contain child elements that define the variable mapping. In between the element tags, a user needs to specify how the exchanged data is mapped to EnergyPlus objects. Hence, the order of these elements matter, and it need to be the same as the order of the elements in the input and output signal vector of the BCVTB actor that calls EnergyPlus. The exchanged variables are declared in elements that are called ``variable'' and have an attribute ``source.'' As described above, the external interface can send data to ExternalInterface:Schedule, ExternalInterface:Actuator, ExternalInterface:Variable. For these objects, the ``source'' attribute needs to be set to ``Ptolemy,'' because they are computed in Ptolemy. The xml elements for these objects look as follows:
+
+For ExternalInterface:Schedule, use
+
+\textless{}variable source = ``Ptolemy''\textgreater{}
+
+~~~ \textless{}EnergyPlus schedule = ``NAME''/\textgreater{}
+
+~ \textless{}/variable\textgreater{}
+
+where NAME needs to be the EnergyPlus schedule name. For ExternalInterface:Actuator, use
+
+\textless{}variable source = ``Ptolemy''\textgreater{}
+
+~~~ \textless{}EnergyPlus actuator = ``NAME'' /\textgreater{}
+
+~ \textless{}/variable\textgreater{}
+
+where NAME needs to be the EnergyPlus actuator name. For ExternalInterface:Variable, use
+
+~ \textless{}variable source = ``Ptolemy''\textgreater{}
+
+~~~ \textless{}EnergyPlus variable = ``NAME''/\textgreater{}
+
+~ \textless{}/variable\textgreater{}
+
+where NAME needs to be the EnergyPlus Energy Runtime Language (Erl) variable name.
+
+The external interface can also read data from any Output:Variable and EnergyManagementSystem:OutputVariable. For these objects, set the ``source'' attribute to ``EnergyPlus,'' because they are computed by EnergyPlus. The read an Output:Variable, use
+
+~ \textless{}variable source = ``EnergyPlus''\textgreater{}
+
+~~~ \textless{}EnergyPlus name = ``NAME'' type = ``TYPE''/\textgreater{}
+
+~ \textless{}/variable\textgreater{}
+
+where NAME needs to be the EnergyPlus ``Variable Name'' (such as ZONE/SYS AIR TEMP) and TYPE needs to be the EnergyPlus ``Key Value'' (such as ZONE ONE). To read an EnergyManagementSystem:OutputVariable, use
+
+\textless{}variable source = ``EnergyPlus''\textgreater{}
+
+~~~ \textless{}EnergyPlus name = ``EMS'' type = ``TYPE''/\textgreater{}
+
+\textless{}/variable\textgreater{}
+
+i.e., the attribute ``name'' must be EMS, and the attribute ``type'' must be set to the EMS variable name.
+
+Complete examples of these xml files are presented below.
+
+\subsection{Example 1: Interface using ExternalInterface:Schedule}\label{example-1-interface-using-externalinterfaceschedule}
+
+In this example, a controller that is implemented in the BCVTB computes the room temperature set points for cooling and heating. The example can be found in the BCVTB distribution in the folder examples/ePlusX-schedule, where X stands for the EnergyPlus version number.
+
+Suppose we need to send from the BCVTB to EnergyPlus a schedule value, and from EnergyPlus to the BCVTB an output variable at each zone time step. This can be accomplished by using an object of type ExternalInterface:Schedule and an object of type Output:Variable.
+
+To interface EnergyPlus using the EMS feature, the following three items are needed:
+
+\begin{itemize}
+\item
+  An object that instructs EnergyPlus to activate the external interface.
+\item
+  EnergyPlus objects that write data from the external interface to the EMS.
+\item
+  A configuration file to configure the data exchange.
+\end{itemize}
+
+\subsubsection{Creating the EnergyPlus idf file}\label{creating-the-energyplus-idf-file}
+
+The EnergyPlus idf file contains the following objects to activate and use the external interface:
+
+\begin{itemize}
+\item
+  An object that instructs EnergyPlus to activate the external interface.
+\item
+  An object of type ExternalInterface:Schedule. The external interface will write its values to these objects at each zone time-step.
+\item
+  Objects of type Output:Variable. Any EnergyPlus output variable can be read by the external interface.
+\end{itemize}
+
+The code below shows how to declare these objects.
+
+To activate the external interface, we use:
+
+\begin{lstlisting}
+
+ExternalInterface,           !- Object to activate the external interface
+   PtolemyServer;              !- Name of external interface
+\end{lstlisting}
+
+To enter schedules to which the external interface writes, we use:
+
+\begin{lstlisting}
+
+! Cooling schedule. This schedule is set directly by the external interface.
+  ! During warm-up and system-sizing, it is fixed at 24 degC.
+    ExternalInterface:Schedule,
+      TSetCoo,                 !- Name
+      Temperature,             !- ScheduleType
+      24;                      !- Initial value, used during warm-up
+
+
+  ! Heating schedule. This schedule is set directly by the external interface.
+  ! During warm-up and system-sizing, it is fixed at 20 degC.
+    ExternalInterface:Schedule,
+      TSetHea,                 !- Name
+      Temperature,             !- ScheduleType
+      20;                      !- Initial value, used during warm-up
+\end{lstlisting}
+
+These schedules can be used as other EnergyPlus schedules. In this example, they are used to change a thermostat setpoint:
+
+\begin{lstlisting}
+
+ThermostatSetpoint:DualSetpoint,
+      DualSetPoint,            !- Name
+      BCVTB-SP-TH,             !- Heating Setpoint Temperature Schedule Name
+      BCVTB-SP-TC;             !- Cooling Setpoint Temperature Schedule Name
+\end{lstlisting}
+
+We also want to read from EnergyPlus output variables, which we declare as
+
+\begin{lstlisting}
+
+Output:Variable,
+      TSetHea,        !- Key Value
+      Schedule Value, !- Variable Name
+      TimeStep;       !- Reporting Frequency
+
+
+  Output:Variable,
+      TSetCoo,        !- Key Value
+      Schedule Value, !- Variable Name
+      TimeStep;       !- Reporting Frequency
+\end{lstlisting}
+
+To specify that data should be exchanged every 15 minutes of simulation time, enter in the idf file the section
+
+\begin{lstlisting}
+
+  Timestep,
+      4;          !- Number of Timesteps per Hour
+\end{lstlisting}
+
+\subsubsection{Creating the configuration file}\label{creating-the-configuration-file}
+
+Note that we have not yet specified the order of the elements in the signal vector that is exchanged between EnergyPlus and the BCVTB. This information is specified in the file variables.cfg. The file variables.cfg needs to be in the same directory as the EnergyPlus idf file. For the objects used in the section above, the file looks like
+
+\begin{lstlisting}
+
+<?xml version = "1.0" encoding = "ISO-8859-1"?>
+  <!DOCTYPE BCVTB-variables SYSTEM "variables.dtd">
+  <BCVTB-variables>
+    <!-- The next two elements send the set points to E+ -->
+    <variable source = "Ptolemy">
+      <EnergyPlus schedule = "TSetHea"/>
+    </variable>
+    <variable source = "Ptolemy">
+      <EnergyPlus schedule = "TSetCoo"/>
+    </variable>
+    <!-- The next two elements receive the outdoor and zone air temperature from E+ -->
+    <variable source = "EnergyPlus">
+     <EnergyPlus name = "ENVIRONMENT" type = "SITE OUTDOOR AIR DRYBULB TEMPERATURE"/>
+    </variable>
+    <variable source = "EnergyPlus">
+      <EnergyPlus name = "ZSF1" type = "ZONE AIR TEMPERATURE"/>
+    </variable>
+    <!-- The next two elements receive the schedule value as an output from E+ -->
+    <variable source = "EnergyPlus">
+      <EnergyPlus name = "TSetHea" type = "Schedule Value"/>
+    </variable>
+    <variable source = "EnergyPlus">
+      <EnergyPlus name = "TSetCoo" type = "Schedule Value"/>
+    </variable>
+  </BCVTB-variables>
+\end{lstlisting}
+
+This file specifies that the actor in the BCVTB that calls EnergyPlus has an input vector with two elements that are computed by Ptolemy (Ptolemy is the name of the software on which the BCVTB is based) and sent to EnergyPlus, and that it has an output vector with four elements that are computed by EnergyPlus and sent to Ptolemy. The order of the elements in each vector is determined by the order in the above XML file. Hence, the input vector that contains the signals sent to EnergyPlus has elements
+
+TSetHea
+
+~ TSetCoo
+
+and the output vector that contains values computed by EnergyPlus has elements
+
+Environment (Site Outdoor Air Drybulb Temperature)
+
+~ ZSF1 (ZONE AIR TEMPERATURE)
+
+~ TSetHea (Schedule Value)
+
+~ TSetCoo (Schedule Value)
+
+\paragraph{\texorpdfstring{\textbf{Creating the Ptolemy model}}{Creating the Ptolemy model}}\label{creating-the-ptolemy-model}
+
+To start EnergyPlus from the BCVTB, you will need to create a Ptolemy model.
+
+The model bcvtb/example/ePlus40-schedule/system-windows.xml that is part of the BCVTB installation and that is shown below may be used as a starting point. (For Mac and Linux, use the file system.xml.) In this example, the time step is 15 minutes and the simulation period is four days.
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image005.png}
+\caption{System model in the BCVTB. \protect \label{fig:system-model-in-the-bcvtb.}}
+\end{figure}
+
+In this model, the Simulator actor that calls EnergyPlus is configured for Windows as follows:
+
+\begin{figure}[hbtp] % fig 3
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image006.png}
+\caption{Configuration of the Simulator actor that calls EnergyPlus on Windows. \protect \label{fig:configuration-of-the-simulator-actor-that}}
+\end{figure}
+
+Hence, it calls the file ``RunEPlus.bat,'' with arguments ``EMSWindowShadeControl USA\_IL\_Chicago-OHare.Intl.AP.725300\_TMY3.'' The working directory is the current directory and the console output is written to the file simulation.log. If EnergyPlus does not communicate with the BCVTB within 10 seconds, the BCVTB will terminate the connection. (See \url{http://simulationresearch.lbl.gov/bcvtb} for more detailed documentation about how to configure a BCVTB model that communicates with other programs.)
+
+For Mac OS X and Linux, the configuration is similar:
+
+\begin{figure}[hbtp] % fig 4
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image007.png}
+\caption{Configuration of the Simulator actor that calls EnergyPlus on Mac OS X and on Linux. \protect \label{fig:configuration-of-the-simulator-actor-that-001}}
+\end{figure}
+
+This completes the configuration.
+
+\subsection{Example 2: Interface using ExternalInterface:Actuator}\label{example-2-interface-using-externalinterfaceactuator}
+
+In this example, a shading controller with a finite state machine is implemented in the BCVTB. Inputs to the controller are the outside temperature and the solar radiation that is incident on the window. The output of the controller is the shading actuation signal.
+
+This example describes how to set up EnergyPlus to exchange data between the BCVTB and EnergyPlus, using an Energy Management System (EMS) actuator. The example can be found in the BCVTB distribution in the folder examples/ePlusX-actuator, where X stands for the EnergyPlus version number.
+
+The object of type ExternalInterface:Actuator behaves identically to EnergyManagmentSystem:Actuator, with the following exceptions:
+
+\begin{itemize}
+\item
+  Its value is assigned by the external interface.
+\item
+  Its value is fixed during the zone time step because this is the synchronization time step for the external interface.
+\end{itemize}
+
+To interface EnergyPlus using the EMS feature, the following three items are needed:
+
+1)~~~An object that instructs EnergyPlus to activate the external interface.
+
+2)~~~EnergyPlus objects that write data from the external interface to the EMS.
+
+3)~~~A configuration file to configure the data exchange.
+
+\subsubsection{Creating the EnergyPlus idf file}\label{creating-the-energyplus-idf-file-1}
+
+The code below shows how to set up an EnergyPlus file that uses EnergyManagmentSystem:Actuator. To activate the external interface, we use:
+
+\begin{lstlisting}
+
+ExternalInterface,           !- Object to activate the external interface
+   PtolemyServer;              !- Name of external interface
+\end{lstlisting}
+
+To declare an actuator that changes the control status of the window with name ``Zn001:Wall001:Win001'', we use:
+
+\begin{lstlisting}
+
+ExternalInterface:Actuator,
+      Zn001_Wall001_Win001_Shading_Deploy_Status,  !- Name
+      Zn001:Wall001:Win001,    !- Actuated Component Unique Name
+      Window Shading Control,  !- Actuated Component Type
+      Control Status,          !- Actuated Component Control Type
+       ;                       ! initial value
+\end{lstlisting}
+
+Thus, the entry is identical with EnergyManagmentSystem:Actuator, except for the additional optional field that specifies the initial value. If unspecified, then the actuator will only be used during the time stepping, but not during the warm-up and the system sizing. Since actuators always overwrite other objects (such as a schedule), all these objects have values that are defined during the warm-up and the system sizing even if no initial value is specified.
+
+We also want to read from EnergyPlus the outdoor temperature, the zone air temperature, the solar radiation that is incident on the window, and the fraction of time that the shading is on. Thus, we declare the output variables
+
+\begin{lstlisting}
+
+Output:Variable,
+     Environment,                            !- Key Value
+     Site Outdoor Air Drybulb Temperature,   !- Variable Name
+     timestep;                               !- Reporting Frequency
+
+
+  Output:Variable,
+     *,                                      !- Key Value
+     Zone Mean Air Temperature,              !- Variable Name
+     timestep;                               !- Reporting Frequency
+
+
+  Output:Variable,
+     Zn001:Wall001:Win001,                   !- Key Value
+     Surface Outside Face Incident Solar Radiation Rate per Area, !- Var Name
+     timestep;                               !- Reporting Frequency
+
+
+  Output:Variable,
+     *,                                      !- Key Value
+     Surface Shading Device Is On Time Fraction,  !- Variable Name
+     timestep;                               !- Reporting Frequency
+\end{lstlisting}
+
+To specify that data should be exchanged every 10 minutes of simulation time, we enter in the idf file the section
+
+\begin{lstlisting}
+
+  Timestep,
+      6;          !- Number of Timesteps per Hour
+\end{lstlisting}
+
+\paragraph{\texorpdfstring{\textbf{Creating the configuration file}}{Creating the configuration file}}\label{creating-the-configuration-file-1}
+
+Note that we have not yet specified the order of the elements in the signal vector that is exchanged between EnergyPlus and the BCVTB. This information is specified in the file variables.cfg. The file variables.cfg needs to be in the same directory as the EnergyPlus idf file. For the objects used in the section above, the file looks like
+
+\begin{lstlisting}
+
+<?xml version = "1.0" encoding = "ISO-8859-1"?>
+  <!DOCTYPE BCVTB-variables SYSTEM "variables.dtd">
+  <BCVTB-variables>
+    <variable source = "EnergyPlus">
+     <EnergyPlus name = "ENVIRONMENT" type = "SITE OUTDOOR AIR DRYBULB TEMPERATURE"/>
+    </variable>
+    <variable source = "EnergyPlus">
+      <EnergyPlus name = "WEST ZONE" type = "Zone Mean Air Temperature"/>
+    </variable>
+    <variable source = "EnergyPlus">
+      <EnergyPlus name = "Zn001:Wall001:Win001" type = "Surface Outside Face Incident Solar Radiation Rate per Area"/>
+    </variable>
+    <variable source = "EnergyPlus">
+      <EnergyPlus name = "Zn001:Wall001:Win001" type = "Surface Shading Device Is On Time Fraction"/>
+    </variable>
+    <variable source = "Ptolemy">
+      <EnergyPlus actuator = "Zn001_Wall001_Win001_Shading_Deploy_Status" />
+    </variable>
+  </BCVTB-variables>
+\end{lstlisting}
+
+This file specifies that the actor in the BCVTB that calls EnergyPlus has an input vector with one element that will be written to the actuator, and that it has an output vector with four elements that are computed by EnergyPlus and sent to Ptolemy. The order of the elements in each vector is determined by the order in the above XML file. Hence, the output vector that contains the signals computed by EnergyPlus has elements
+
+\begin{lstlisting}
+  ENVIRONMENT (SITE OUTDOOR AIR DRYBULB TEMPERATURE)
+  WEST ZONE (Zone Mean Air Temperature)
+  Zn001:Wall001:Win001 (Surface Outside Face Incident Solar Radiation Rate per Area)
+  Zn001:Wall001:Win001 (Surface Shading Device Is On Time Fraction)
+\end{lstlisting}
+
+The configuration of the Ptolemy model is identical to the configuration in Example 1.
+
+\subsection{Example 3: Interface using ExternalInterface:Variable}\label{example-3-interface-using-externalinterfacevariable}
+
+This example implements the same controller as the Example 2. However, the interface with EnergyPlus is done using an external interface variable instead of an external interface actuator. In addition, the example uses an EnergyManagementSystem:OutputVariable to set up data that will be read by the external interface.
+
+Similarly to EnergyManagementSystem:GlobalVariable, an ExternalInterface:Variable can be used in any EnergyManagementSystem:Program. The subject of this example is to illustrate how an ExternalInterface:Variable can be set up for use in an EnergyManagementSystem:Program. The example can be found in the BCVTB distribution in the folder examples/ePlusX-variable, where X stands for the EnergyPlus version number.
+
+To interface EnergyPlus using an external interface variable, the following items are needed:
+
+\begin{itemize}
+\item
+  An object that instructs EnergyPlus to activate the external interface.
+\item
+  EnergyPlus objects that write data from the external interface to the EMS.
+\item
+  A configuration file to configure the data exchange.
+\end{itemize}
+
+\subsubsection{Creating the EnergyPlus idf file}\label{creating-the-energyplus-idf-file-2}
+
+To write data from the external interface to an EnergyPlus EMS variable, an EnergyPlus object of the following entry may be used in the idf file:
+
+\begin{lstlisting}
+
+ExternalInterface,           !- Object to activate the external interface
+     PtolemyServer;            !- Name of external interface
+
+
+    ExternalInterface:Variable,
+      yShade,                  !- Name of Erl variable
+      1;                       !- Initial value
+\end{lstlisting}
+
+During the warm-up period and the system-sizing, the variable will be set to its initial value. Afterwards, the value will be assigned from the external interface at each beginning of a zone time step and kept constant during the zone time step. From the point of view of the EMS language, ExternalInterface:Variable can be used like any global variable. Thus, it can be used within any EnergyManagementSystem:Program in the same way as an EnergyManagementSystem:GlobalVariable or an EnergyManagementSystem:Sensor.
+
+This idf section above activates the external interface and declares a variable with name yShade that can be used in an Erl program to actuate the shading control of the window ``Zn001:Wall001:Win001'' as follows:
+
+\begin{lstlisting}
+
+! EMS program. The first assignments sets the shading status and converts it into the
+  !              EnergyPlus signal (i.e., replace 1 by 6).
+  !              The second assignment sets yShade to
+  !              an EnergyManagementSystem:OutputVariable
+  !              which will be read by the external interface.
+    EnergyManagementSystem:Program,
+      Set_Shade_Control_State,          !- Name
+      Set Shade_Signal = 6*yShade,      !- Program Line 1
+      Set Shade_Signal_01 = yShade+0.1; !- Program Line 2
+
+
+  ! Declare an actuator to which the EnergyManagementSystem:Program will write
+    EnergyManagementSystem:Actuator,
+      Shade_Signal,  !- Name
+      Zn001:Wall001:Win001,             !- Actuated Component Unique Name
+      Window Shading Control,           !- Actuated Component Type
+      Control Status;                   !- Actuated Component Control Type
+
+
+  ! Declare a global variable to which the EnergyManagementSystem:Program will write
+    EnergyManagementSystem:GlobalVariable,
+      Shade_Signal_01;                  !- Name of Erl variable
+\end{lstlisting}
+
+We want to read from EnergyPlus the outdoor temperature, the zone air temperature and the solar radiation that is incident on the window. Thus, we declare
+
+\begin{lstlisting}
+
+Output:Variable,
+     Environment,                 !- Key Value
+     Site Outdoor Air Drybulb Temperature,            !- Variable Name
+     timestep;                    !- Reporting Frequency
+
+
+    Output:Variable,
+    *,                          !- Key Value
+    Zone Mean Air Temperature,  !- Variable Name
+    timestep;                   !- Reporting Frequency
+
+
+    Output:Variable,
+    Zn001:Wall001:Win001,       !- Key Value
+    Surface Outside Face Incident Solar Radiation Rate per Area, !- Var Name
+    timestep;                   !- Reporting Frequency
+\end{lstlisting}
+
+In addition, we want to output the variable ``Erl Shading Control Status'' that has been set up as
+
+\begin{lstlisting}
+
+! Declare an output variable. This variable is equal to the shahing signal + 0.1
+  ! It will be reah by the external interface to hemonstrate how to receive variables.
+    EnergyManagementSystem:OutputVariable,
+      Erl Shahing Control Status,  !- Name
+      Shahe_Signal_01,             !- EMS Variable Name
+      Averageh,                    !- Type of Data in Variable
+      ZoneTimeStep;                !- Uphate Frequency
+\end{lstlisting}
+
+To specify that data should be exchanged every 10 minutes of simulation time, enter in the idf file the section
+
+\begin{lstlisting}
+
+  Timestep,
+      6;          !- Number of Timesteps per Hour
+\end{lstlisting}
+
+\subsubsection{Creating the configuration file}\label{creating-the-configuration-file-2}
+
+Note that we have not yet specified the order of the elements in the signal vector that is exchanged between EnergyPlus and the BCVTB. This information is specified in the file variables.cfg. The file variables.cfg needs to be in the same directory as the EnergyPlus idf file. For the objects used in the section above, the file looks like
+
+\begin{lstlisting}
+
+<?xml version = "1.0" encoding = "ISO-8859-1"?>
+  <!DOCTYPE BCVTB-variables SYSTEM "variables.dtd">
+  <BCVTB-variables>
+    <variable source = "Ptolemy">
+      <EnergyPlus variable = "yShade"/>
+    </variable>
+    <variable source = "EnergyPlus">
+      <EnergyPlus name = "ENVIRONMENT" type = "SITE OUTDOOR AIR DRYBULB TEMPERATURE"/>
+    </variable>
+    <variable source = "EnergyPlus">
+      <EnergyPlus name = "WEST ZONE" type = "Zone Mean Air Temperature"/>
+    </variable>
+    <variable source = "EnergyPlus">
+      <EnergyPlus name = "Zn001:Wall001:Win001" type = "Surface Outside Face Incident Solar Radiation Rate per Area"/>
+    </variable>
+    <variable source = "EnergyPlus">
+      <EnergyPlus name = "EMS" type = "Erl Shading Control Status"/>
+    </variable>
+  </BCVTB-variables>
+\end{lstlisting}
+
+This file specifies that the actor in the BCVTB that calls EnergyPlus has an input vector with one element that will be written to the actuator, and that it has an output vector with four elements that are computed by EnergyPlus and sent to Ptolemy. The order of the elements in each vector is determined by the order in the above XML file. Note that the fourth element has the name ``EMS'' because it is an EnergyManagementSystem:OutputVariable. Hence, the output vector that contains the signals computed by EnergyPlus has elements
+
+\begin{lstlisting}
+  ENVIRONMENT (SITE OUTDOOR AIR DRYBULB TEMPERATURE)
+  WEST ZONE (Zone Mean Air Temperature)
+  Zn001:Wall001:Win001 (Surface Outside Face Incident Solar Radiation Rate per Area)
+  EMS (Erl Shading Control Status)
+\end{lstlisting}
+
+The configuration of the Ptolemy model is identical to the configuration in the previous examples.
diff --git a/doc/external-interfaces-application-guide/src/external-interface-s/coupling-energyplus-with-functional-mock-up.tex b/doc/external-interfaces-application-guide/src/external-interface-s/coupling-energyplus-with-functional-mock-up.tex
new file mode 100644
index 00000000000..e2a06392671
--- /dev/null
+++ b/doc/external-interfaces-application-guide/src/external-interface-s/coupling-energyplus-with-functional-mock-up.tex
@@ -0,0 +1,175 @@
+\section{Coupling EnergyPlus with Functional Mock-up Units for co-simulation}\label{coupling-energyplus-with-functional-mock-up-units-for-co-simulation}
+
+The Functional Mock-up Unit (FMU) for co-simulation import for EnergyPlus allows EnergyPlus to conduct co-simulation with various programs that are packaged as FMUs. A FMU is a component which implements the Functional Mock-up Interface (FMI) standard (http://www.modelisar.com).
+
+A FMU is distributed in the form of a zip file that may contain physical models, model descriptions, source code, and executable programs for various platforms. The FMU for co-simulation import provides EnergyPlus with a standard interface to conduct and control co-simulation with an arbitrary number of FMUs without any middle-ware, such as the Building Controls Virtual Test Bed (BCVTB Documentation, 2011).
+
+The FMU for co-simulation import allows coupling of continuous-time and discrete-time models exported from different simulation programs. In the current implementation, EnergyPlus is implemented as the co-simulation master. It controls the data exchange between the subsystems and the synchronization of all slave simulation programs.
+
+The FMU for co-simulation import enables the direct link between the EnergyPlus kernel and other simulation tools. It will make the co-simulation easier to conduct as no middle-ware is involved. This direct link will decrease run-time by eliminating the transaction layer. In addition, by separating the co-simulation interface from the EnergyPlus kernel, the FMU interface is reusable when EnergyPlus is updated. Furthermore, the FMU contains executable files that have the same interface to EnergyPlus regardless of their original programming environment. Some commercial tools allow running their FMU without licensing requirement.
+
+\textbf{Notes:}
+
+1)~~~The current implementation of FMU for co-simulation is only supported on Windows and Linux.
+
+2)~~~FMUs must be in a folder to which the user has \emph{write} access.
+
+\subsection{Data exchange between EnergyPlus and FMUs}\label{data-exchange-between-energyplus-and-fmus}
+
+Prior to describing the data exchange between EnergyPlus and FMUs, some definitions and terminologies used in the remainder of this document will be introduced.
+
+A variable of a system described by a system of differential algebraic equations (DAE) is defined as differential variable if its derivatives are present in the DAE. A variable of a system described by a system of DAE is defined as algebraic if its derivatives do not appear explicitly in the DAE (Fabian et al., 2008).
+
+\begin{figure}[hbtp] % fig 5
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image008.png}
+\caption{System with two variables that could be either differential or algebraic variables. \protect \label{fig:system-with-two-variables-that-could-be}}
+\end{figure}
+
+Because in subsequent discussions, it will be distinguished between algebraic and differential variables, a notation for different system of equations that involve algebraic and differential variables will be introduced. Let \(q\in\mathbf{N}\) , then
+
+\begin{itemize}
+\tightlist
+\item
+  If x\(_{1}\) and x\(_{2}\)~are differential variables, then the system is
+\end{itemize}
+
+\(F\left(\dot x_1,x_1,\dot x_2,x_2,u,t\right) = 0\) ~with \emph{F}: �\(^{n}\) x �\(^{n}\) x �\(^{m}\) x �\(^{m}\) x �\(^{q}\) x � → �\(^{n+m}\).
+
+\begin{itemize}
+\tightlist
+\item
+  If x\(_{1}\) is a differential variable and x\(_{2}\)~is an algebraic variable, then the system is
+\end{itemize}
+
+\(G\left(\dot x_1,x_1,x_2,u,t\right) = 0\) ~with \emph{G}: �\(^{n}\) x �\(^{n}\) x �\(^{m}\) x �\(^{q}\) x � → �\(^{n+m}\).
+
+\begin{itemize}
+\tightlist
+\item
+  If x\(_{1}\)~is an algebraic variable and x\(_{2}\)~is a differential variable, then the system is
+\end{itemize}
+
+\(H\left(x_1,\dot x_2,x_2,u,t\right) = 0\) ~with \emph{H:} �\(^{n}\) x�\(^{m}\) x�\(^{m}\) x�\(^{q}\) x� →�\(^{n+m}\).
+
+\begin{itemize}
+\tightlist
+\item
+  If x\(_{1}\)~is an algebraic variable and x\(_{2}\)~is an algebraic variable, then the system is
+\end{itemize}
+
+\(I\left(x_1,x_2,u,t\right) = 0\) with \emph{I}: �\(^{n}\) x�\(^{m}\) x�\(^{q}\) x� →�\(^{n+m}\).
+
+Figure~\ref{fig:system-with-one-fmu-linked-to-energyplus.}~shows a case where a FMU is linked to an EnergyPlus model for co-simulation. The FMU and EnergyPlus could be linked through differential or algebraic variables.
+
+\begin{figure}[hbtp] % fig 6
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image016.png}
+\caption{System with one FMU linked to EnergyPlus. HERHERHEHERHERHERHERH Table 2 shows the different system configurations that are possible. \protect \label{fig:system-with-one-fmu-linked-to-energyplus.}}
+\end{figure}
+
+\begin{itemize}
+\item
+  In the first case, the variable x\(_{1}\)~and x\(_{2}\)~are differential variables in both systems.
+\item
+  In the second case, the variable x\(_{1}\)~is a differential variable and the variable x\(_{2}\)~is an algebraic variable.
+\item
+  In the third case, the variable x\(_{1}\)~is an algebraic variable and the variable x\(_{2}\) is a differential variable.
+\item
+  In the fourth case, the variable x\(_{1}\)~is an algebraic variable and the variable x\(_{2}\) is an algebraic variable.
+\end{itemize}
+
+In the current implementation, it will be focused on the first and the second cases since the third and the fourth cases will constrain the FMU to be solved numerically in the iteration solver loop of EnergyPlus. This will necessitate the ability of the FMU to reject time steps (Modelisar, 2010) which is currently not implemented in the EnergyPlus FMU for co-simulation import. Applications for case 1 and 2 are described in the next sections.
+
+Table 2:~Use cases with different system configurations
+
+\begin{longtable}[c]{@{}lll@{}}
+\toprule 
+Case & EnergyPlus & FMU (e.g. from Modelica) \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Case & EnergyPlus & FMU (e.g. from Modelica) \tabularnewline
+\midrule
+\endhead
+
+(1) & Model1 (Differential variable) & Model2 (Differential variable) \tabularnewline
+(2) & Model1 (Differential variable) & Model2 (Algebraic variable) \tabularnewline
+(3) & Model1 (Algebraic variable) & Model2 (Differential variable) \tabularnewline
+(4) & Model1 (Algebraic variable) & Model2 (Algebraic variable) \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Case 1: Linking two systems through differential variables}\label{case-1-linking-two-systems-through-differential-variables}
+
+This case could be for an application where a wall with a phase change material (PCM) is modeled in a FMU and is linked to a room model in EnergyPlus. The room air temperature is the differential variable in EnergyPlus and the temperature of the wall with PCM is the differential variable in the FMU. Each system solves a differential equation that is connected~to the differential equation of the other system. For simplicity, we assume that \emph{y\(_{1}\)(.)} = \emph{x\(_{1}\)(.) and y\(_{2}\)(.)} = \emph{x\(_{2}\)(.).}The systems are described by the ordinary differential equations
+
+dx\(_{1}\)/dt = f\(_{1}\)(x\(_{1}\), x\(_{2}\)), with x\(_{1}\)(0) = x\(_{1,0}\) ,
+
+dx\(_{2}\)/dt = f\(_{2}\)(x\(_{2}\), x\(_{1}\)), with x\(_{2}\)(0) = x\(_{2,0\\ .}\)
+
+Let \(N\in\textbf{N}\) ~denote the number of time steps and let \emph{t\(_{k}\)} with \(k\in\left\{1,...,N\right\}\) denote the time steps. We will use the subscripts \emph{1} and \emph{2} to denote the variables and the functions that compute the next state variable of the simulator \emph{1} and \emph{2}, respectively.
+
+The first system computes, for \(k\in\left\{0,...,N-1\right\}\) and some \(\tilde{F}_1\) : �\(^{n}\) x �\(^{m}\) x � x � → �\(^{n}\), the sequence
+
+x\(_{1}\)(t\(_{k+1}\)) = \(\tilde{F}_1\) (x\(_{1}\)(t\(_{k}\)), x\(_{2}\)(t\(_{k}\)), t\(_{k}\), t\(_{k+1}\))
+
+and, similarly, the simulator \emph{2} computes for some \(\tilde{F}_2\) : �\(^{m}\) x �\(^{n}\) x � x � → �\(^{m}\) the sequence
+
+x\(_{2}\)(t\(_{k+1}\)) = \(\tilde{F}_2\) (x\(_{2}\)(t\(_{k}\)), x\(_{1}\)(t\(_{k}\)), t\(_{k}\), t\(_{k+1}\))
+
+with initial conditions \emph{x\(_{1}\)(0) = x\(_{1,0}\)} and \emph{x\(_{2}\)(0) = x\(_{2,0.}\)} \(\tilde{F}_1\) ~and \(\tilde{F}_2\) ~*are the functions that are used to compute the value of the state variables at the new time step
+
+To advance from time \emph{t\(_{k}\)} to \emph{t\(_{k+1}\)}, each system uses its own time integration algorithm. At the end of the time step, EnergyPlus sends the new state \emph{x\(_{1}\)(t\(_{k+1}\))} to the FMU and it receives the state \emph{x\(_{2}\)(t\(_{k+1}\))} from the FMU. The same procedure is done with the FMU.
+
+\subsection{Case 2: Linking two systems through algebraic and differential variables}\label{case-2-linking-two-systems-through-algebraic-and-differential-variables}
+
+This case could be for an application where a fan is modeled in a FMU and is linked to a room model in EnergyPlus. The room temperature is the differential variable in EnergyPlus and the pressure difference of the fan is the algebraic variable in the FMU. For simplicity, we assume that \emph{y\(_{1}\)(.)} = \emph{x\(_{1}\)(.) and y\(_{2}\)(.)} = \emph{x\(_{2}\)(.).} In this application, the systems are described by the following equations
+
+dx\(_{1}\)/dt = g\(_{1}\)(x\(_{1}\), x\(_{2}\)), with x\(_{1}\)(0) = x\(_{1,0,}\)
+
+0 = g\(_{2}\)(x\(_{2}\), x\(_{1}\)).
+
+Let \(N\in\mathbf{N}\) ~denote the number of time steps and let \emph{t\(_{k}\)} with \(k\in\left\{1,...,N\right\}\) ~denote the time steps. We use the same subscripts \emph{1} and \emph{2} as for the first case to denote the variable and the function that computes the next variable of the simulator \emph{1} and \emph{2}, respectively.
+
+The first system computes, for \(k\in\left\{0,...,N-1\right\}\) and some \(\tilde{G}_1\) : �\(^{n}\) x �\(^{m}\) x � x � → �\(^{n}\), the sequence
+
+x\(_{1}\)(t\(_{k+1}\)) = \(\tilde{G}_1\) (x\(_{1}\)(t\(_{k}\)), x\(_{2}\)(t\(_{k}\)), t\(_{k}\), t\(_{k+1}\))
+
+and, similarly, the simulator \emph{2} computes for some \(\tilde{G}_2\) : �\(^{m}\) x �\(^{n}\) x � → �\(^{m}\) the sequence
+
+x\(_{2}\)(t\(_{k+1}\)) = \(\tilde{G}_2\) (x\(_{2}\)(t\(_{k+1}\)), x\(_{1}\)(t\(_{k+1}\)), t\(_{k+1}\))
+
+with initial condition \emph{x\(_{1}\)(0) = x\(_{1,0}\)}. \(\tilde{G}_1\) and \(\tilde{G}_2\) are the functions that compute the value of the variables at the new time step.
+
+To advance from time \emph{t\(_{k}\)} to \emph{t\(_{k+1}\)}, each system uses its own time integration algorithm. At the end of the time step, EnergyPlus sends the new value \emph{x\(_{1}\)(t\(_{k+1}\))} to the FMU and it receives the value \emph{x\(_{2}\)(t\(_{k+1}\))} from the FMU. The same procedure is done with the FMU.
+
+\subsection{Requirements}\label{requirements}
+
+The current implementation for linking EnergyPlus with the FMUs has the following requirements:
+
+\begin{itemize}
+\item
+  The data exchange between EnergyPlus and the FMUs is done at the zone time step of EnergyPlus.
+\item
+  Each FMU is linked to EnergyPlus only through a differential variable in EnergyPlus (see Figure~\ref{fig:system-with-one-fmu-linked-to-energyplus.-001} for one FMU).
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 7
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image033.png}
+\caption{System with one FMU linked to EnergyPlus. \protect \label{fig:system-with-one-fmu-linked-to-energyplus.-001}}
+\end{figure}
+
+\begin{itemize}
+\tightlist
+\item
+  Two or multiple FMUs are linked together only through differential variables in EnergyPlus (see Figure~\ref{fig:system-with-two-fmus-linked-to-energyplus.} for two FMUs).
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 8
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image034.png}
+\caption{System with two FMUs linked to EnergyPlus. \protect \label{fig:system-with-two-fmus-linked-to-energyplus.}}
+\end{figure}
diff --git a/doc/external-interfaces-application-guide/src/external-interface-s/coupling-energyplus-with-the-building.tex b/doc/external-interfaces-application-guide/src/external-interface-s/coupling-energyplus-with-the-building.tex
new file mode 100644
index 00000000000..a889da5e881
--- /dev/null
+++ b/doc/external-interfaces-application-guide/src/external-interface-s/coupling-energyplus-with-the-building.tex
@@ -0,0 +1,60 @@
+\section{Coupling EnergyPlus with the Building Controls Virtual Test Bed}\label{coupling-energyplus-with-the-building-controls-virtual-test-bed}
+
+\subsection{Algorithm for data exchange}\label{algorithm-for-data-exchange}
+
+The process in which at least two simulators solve initial-value differential equations that are coupled to each other is called co-simulation. Various algorithms are possible for the data exchange. In the BCVTB, data are exchanged between its client programs, including EnergyPlus, using a fixed synchronization time step. There is no iteration between the clients. In the co-simulation literature, this coupling scheme is referred to as \emph{quasi-dynamic coupling}, \emph{loose coupling} or \emph{ping-pong coupling} (Hensen 1999, Zhai and Chen 2005).
+
+The algorithm for exchanging data is as follows: Suppose we have a system with two clients, with client 1 being EnergyPlus and client 2 being, for example, the Simulink program from Mathworks. Suppose each client solves an initial-value ordinary differential equation that is coupled to the differential equation of the other client. Let \(N\in\mathbf{N}\) ~denote the number of time steps and let \(k\in\left\{1,...,N\right\}\) ~denote the time steps. We will use the subscripts \emph{1} and \emph{2} to denote the state variable and the function that computes the next state variable of the simulator \emph{1} and \emph{2}, respectively.
+
+The simulator \emph{1} computes, for \(k\in\left\{1,...,N-1\right\}\) the sequence
+
+\emph{x\(_{1}\)(k+1) = f\(_{1}\)(x\(_{1}\)(k), x\(_{2}\)(k))}
+
+and, similarly, the simulator \emph{2} computes the sequence
+
+\emph{x\(_{2}\)(k+1) = f\(_{2}\)(x\(_{2}\)(k), x\(_{1}\)(k))}
+
+with initial conditions \emph{x\(_{1}\)(0) = x\(_{1,0}\)} and \emph{x\(_{2}\)(0) = x\(_{2,0}\)}.
+
+To advance from time \emph{k} to \emph{k+1}, each simulator uses its own time integration algorithm. At the end of the time step, the simulator \emph{1} sends the new state \emph{x\(_{1}\)(k+1)} to the BCVTB and it receives the state \emph{x\(_{2}\)(k+1)} from the BCVTB. The same procedure is done with the simulator \emph{2}. The BCVTB synchronizes the data in such a way that it does not matter which of the two simulators is called first.
+
+In comparison to numerical methods of differential equations, this scheme is identical to an explicit Euler integration, which is an integration algorithm that computes for an ordinary differential equation with specified initial values,
+
+\emph{dx/dt = h(x),}
+
+\emph{x(0)~ = x\(_{0}\),}
+
+on the time interval \emph{t} \emph{∈ {[}0, 1{]}}, the following sequence:
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Step 0: & Initialize counter k = 0 and number of steps $N \in \mathbf{N}$ . \tabularnewline \midrule
+\endhead
+~ & Set initial state x(k) = x   and set time step Dt = 1/N. \tabularnewline
+Step 1: & Compute new state x(k+1) = x(k) + h(x(k)) Dt. \tabularnewline
+~ & Replace k by k+1. \tabularnewline
+Step 2: & If k = N stop, else go to Step 1. \tabularnewline
+\bottomrule
+\end{longtable}
+
+In the situation where the differential equation is solved using co-simulation, the above algorithm becomes
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Step 0: & Initialize counter k=0 and number of steps $N \in \mathbf{N}$ . \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Step 0: & Initialize counter k=0 and number of steps $N \in \mathbf{N}$ . \tabularnewline
+\midrule
+\endhead
+
+~ & Set initial state x  (k) = x   and x  (k) = x  . Set the time step Dt = 1/N. \tabularnewline
+Step 1: & Compute new states ~ x  (k+1) = x  (k) + f  (x  (k), x  (k)) Dt, and ~ x  (k+1) = x  (k) + f  (x  (k), x  (k)) Dt. \tabularnewline
+~ & Replace k by k+1. \tabularnewline
+Step 2: & If k=N stop, else go to Step 1. \tabularnewline
+\bottomrule
+\end{longtable}
+
+This algorithm is implemented in the BCVTB. Note that there is no iteration between the two simulators.
diff --git a/doc/external-interfaces-application-guide/src/external-interface-s/exporting-energyplus-as-a-functional-mock-up.tex b/doc/external-interfaces-application-guide/src/external-interface-s/exporting-energyplus-as-a-functional-mock-up.tex
new file mode 100644
index 00000000000..11b10a4d5ff
--- /dev/null
+++ b/doc/external-interfaces-application-guide/src/external-interface-s/exporting-energyplus-as-a-functional-mock-up.tex
@@ -0,0 +1,7 @@
+\section{Exporting~ EnergyPlus as a Functional Mock-up Unit for co-simulation}\label{exporting-energyplus-as-a-functional-mock-up-unit-for-co-simulation}
+
+The FMU export of EnergyPlus allows EnergyPlus to be accessed from other simulation environments, as a FMU for co-simulation.
+
+FMUs are formally specified in the Functional Mock-up Interface (FMI) standard, an open standard designed to enable links between disparate simulation programs. The standard is available from \href{http://www.functional-mockup-interface.org/.\%20}{http://www.functional-mockup-interface.org/}.
+
+To export EnergyPlus as a FMU for co-simulation, the Lawrence Berkeley National Laboratory has developed a utility which exports EnergyPlus as a FMU for co-simulation. This utility is freely available from http://SimulationResearch.lbl.gov.
diff --git a/doc/external-interfaces-application-guide/src/external-interface-s/fmu-examples.tex b/doc/external-interfaces-application-guide/src/external-interface-s/fmu-examples.tex
new file mode 100644
index 00000000000..a48baa1677d
--- /dev/null
+++ b/doc/external-interfaces-application-guide/src/external-interface-s/fmu-examples.tex
@@ -0,0 +1,458 @@
+\section{FMU Examples}\label{fmu-examples}
+
+\subsection{Architecture of the FMU for co-simulation Import}\label{architecture-of-the-fmu-for-co-simulation-import}
+
+Figure~\ref{fig:architecture-of-the-fmu-for-co-simulation} shows the architecture of the connection between EnergyPlus and two FMUs. EnergyPlus imports the FMUs that connect to its external interface. These FMUs are generated by external simulation environments that implement the FMI Application Programming Interface (API) for co-simulation. See http://www.modelisar.com/tools.html for a list of programs that export FMUs. In the external interface, the input/output signals that are exchanged between the FMUs and EnergyPlus are mapped to EnergyPlus objects. The subject of this External Interface Application Guide is how to configure this mapping and how to use these objects.
+
+\begin{figure}[hbtp] % fig 9
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image035.png}
+\caption{Architecture of the FMU for co-simulation import. \protect \label{fig:architecture-of-the-fmu-for-co-simulation}}
+\end{figure}
+
+The external interface can map to three EnergyPlus input objects called
+
+\begin{itemize}
+\item
+  ExternalInterface:FunctionalMockupUnitImport:To:Schedule
+\item
+  ExternalInterface:FunctionalMockupUnitImport:To:Actuator
+\item
+  ExternalInterface:FunctionalMockupUnitImport:To:Variable.
+\end{itemize}
+
+The ExternalInterface:FunctionalMockupUnitImport:To:Schedule can be used to overwrite schedules, and the other two objects can be used in place of Energy Management System (EMS) actuators and EMS variables. The objects have similar functionality as the objects Schedule:Compact, EnergyManagementSystem:Actuator and EnergyManagementSystem:GlobalVariable, except that their numerical value is obtained from the external interface at the beginning of each zone time step, and will remain constant during this zone time step.
+
+The external interface also uses the ExternalInterface:FunctionalMockupUnitImport:From:Variable object which~ maps to EnergyPlus objects Output:Variable and EnergyManagementSystem:OutputVariable to send data from EnergyPlus to FMUs at each zone time step.
+
+We will now present examples that use all of these objects. The following table shows which EnergyPlus features are used in the examples.
+
+% table 3
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Overview of the EnergyPlus objects used in Examples \label{table:overview-of-the-energyplus-objects-used-in-001}} \tabularnewline
+\toprule 
+~ & Example 1 & Example 2 & Example 3 \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Overview of the EnergyPlus objects used in Examples} \tabularnewline
+\toprule 
+~ & Example 1 & Example 2 & Example 3 \tabularnewline
+\midrule
+\endhead
+
+ExternalInterface:FunctionalMockupUnitImport:From:Variable & x & x & x \tabularnewline
+ExternalInterface:FunctionalMockupUnitImport:To:Schedule & x & ~ & ~ \tabularnewline
+ExternalInterface:FunctionalMockupUnitImport:To:Actuator & ~ & x & ~ \tabularnewline
+ExternalInterface:FunctionalMockupUnitImport:To:Variable & ~ & ~ & x \tabularnewline
+Output:Variable & x & x & x \tabularnewline
+\bottomrule
+\end{longtable}
+
+Prior to discussing the examples, we will explain the pre-processing steps that are required to prepare EnergyPlus to be linked to FMUs for co-simulation.
+
+\subsection{Workflow of the FMU for co-simulation import}\label{workflow-of-the-fmu-for-co-simulation-import}
+
+To use the FMU for co-simulation import, there are two important steps: pre-processing and co-simulation.~ The pre-processing step generates a section of an EnergyPlus input file (*.idf) that can be used to configure the FMU for co-simulation import. The input file defines the input and output variables for both EnergyPlus and FMUs. The co-simulation step performs co-simulation.
+
+Figure~\ref{fig:work-flow-for-pre-processing.} shows the work flow for pre-processing. First, a FMU Parser parses the FMU files (i.e.~xxx.fmu) and generates a temporary EnergyPlus input file (i.e.~xxxtmp.idf). The temporary EnergyPlus input file is not complete as it just contains information related to the FMU, such as names of the FMU and properties of each FMU variable including variable name, associated FMU name, input/output type, data type, units and definitions. The user will need to manually copy the FMU information from xxxtmp.idf into the EnergyPlus input file xxx.idf. The user then needs to modify the xxx.idf file to link the FMU variables with EnergyPlus variables.
+
+\begin{figure}[hbtp] % fig 10
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image036.png}
+\caption{Work flow for pre-processing. \protect \label{fig:work-flow-for-pre-processing.}}
+\end{figure}
+
+\subsection{FMU Parser}\label{fmu-parser}
+
+The FMU parser is a code written in C. It includes Expat (Expat XML Parser, 2011) which is a XML parser library written in C. The low level implementation of the function (\emph{parser}) that is used to process a FMU is \emph{parser {[}options{]} xxx.fmu}, where \emph{options} are as follows:
+
+\begin{itemize}
+\item
+  \emph{--printidf}, prints a temporary xxxtmp.idf with FMU information to be printed,
+\item
+  \emph{--unpack}, unpacks a FMU to be unpacked, and
+\item
+  \emph{--delete}, deletes temporary files related to FMUs.
+\end{itemize}
+
+A FMU is a zip file which may contain executable programs for specific platforms, description files and source code. In the pre-processing step, the FMU Parser will be called with the command option \emph{--printidf.} This will cause the parser to parse the XML file with the model description of the FMU and write the FMU information in a format of the EnergyPlus input file (*.idf). The parser will check if all the required fields from FMU (see next section for details) in the *.idf file are correctly specified. If the check succeeds, the parser will successfully close. If the check fails, the parser will close with an error message. After the EnergyPlus executable (such as EnergyPlus.exe) terminates, the EnergyPlus batch file will delete all the temporary files that may have been generated.~~ The FMU Parser is distributed with EnergyPlus and can be found in the PreProcess folder (FMUParser) of the EnergyPlus installation.
+
+\textbf{~}
+
+\begin{figure}[hbtp] % fig 11
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image037.png}
+\caption{Workflow of FMU parser for pre-processing. \protect \label{fig:workflow-of-fmu-parser-for-pre-processing.}}
+\end{figure}
+
+\subsection{Example 1: Interface using ExternalInterface:FunctionalMockupUnitImport:To:Schedule}\label{example-1-interface-using-externalinterfacefunctionalmockupunitimporttoschedule}
+
+In this example, an HVAC system implemented in a FMU (MoistAir.fmu) is linked to a room model in EnergyPlus. The HVAC system computes sensible and latent heat gain required for maintaining a set point temperature. The FMU needs as input the outdoor dry-bulb (TDryBul) temperature, outdoor air relative humidity (outRelHum), the room dry-bulb temperature (TRooMea) and the room air relative humidity (rooRelHum). The outputs of the FMU are the latent (QLatent) and sensible (QSensible) heat transported across the thermodynamic boundary of air inlet and outlet of the thermal zone.
+
+To link the FMU with EnergyPlus, we need to send from the FMU to EnergyPlus two schedule values for the latent and sensible heat gain and from EnergyPlus to the FMU four output variables for outdoor dry-bulb temperature, outdoor air relative humidity, room dry-bulb temperature and room air relative humidity at each zone time step. This can be accomplished by using two objects of type ExternalInterface:FunctionalMockupUnitImport:To:Schedule and four objects of type ExternalInterface:FunctionalMockupUnitImport:From:Variable.
+
+To interface EnergyPlus, the following four items are needed:
+
+\begin{itemize}
+\item
+  An object that instructs EnergyPlus to activate the external interface.
+\item
+  An object that specifies the FMU and its instances.
+\item
+  EnergyPlus objects that read data from EnergyPlus and send to FMU.
+\item
+  EnergyPlus objects that read data from FMU and send to EnergyPlus.
+\end{itemize}
+
+\subsubsection{Creating the EnergyPlus idf file}\label{creating-the-energyplus-idf-file-000}
+
+To create the EnergyPlus idf file the user should:
+
+\begin{itemize}
+\item
+  Use the \emph{parser} to generate a temporary idf.
+\item
+  Copy the FMU information from the temporary idf into the full idf file.
+\item
+  Modify the full idf file to link the FMU variables with EnergyPlus variables.
+\end{itemize}
+
+The code below shows how the objects will be in the idf.
+
+To activate the external interface, we use:
+
+\begin{lstlisting}
+
+ExternalInterface,           !- Object to activate the external interface
+   FunctionalMockupUnitImport; !- Name of external interface
+\end{lstlisting}
+
+To define the FMU that will be linked to EnergyPlus, we use:
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport,
+      MoistAir.fmu,            !- FMU Filename
+      15,                       !- FMU Timeout
+      0;                        !- FMU LoggingOn
+\end{lstlisting}
+
+To enter output variables from which the external interface read and send to FMUs, we use:
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+      Environment,                      !- EnergyPlus Key Value
+      Site Outdoor Air Drybulb Temperature,     !- EnergyPlus Variable Name
+      MoistAir.fmu,                     !- FMU Filename
+      Model1,                           !-FMU Model Name
+      TDryBul;                          !- FMU Model Variable Name
+
+
+  ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+      ZONE ONE,                         !- EnergyPlus Key Value
+      Zone Mean Air Temperature,        !- EnergyPlus Variable Name
+      MoistAir.fmu,                     !- FMU Filename
+      Model1,                           !- FMU Model Name
+      TRooMea;                          !- FMU Model Variable Name
+
+
+  ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+      Environment,                      !- EnergyPlus Key Value
+      Site Outdoor Air Relative Humidity,      !- EnergyPlus Variable Name
+      MoistAir.fmu,                     !- FMU Filename
+      Model1,                           !- FMU Model Name
+      outRelHum;                        !- FMU Model Variable Name
+
+
+  ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+      ZONE ONE,                         !- EnergyPlus Key Value
+      Zone Air Relative Humidity,       !- EnergyPlus Variable Name
+      MoistAir.fmu,                     !- FMU Filename
+      Model1,                           !- FMU Model Name
+      rooRelHum;                        !- FMU Model Variable Name
+\end{lstlisting}
+
+These output variables need to be specified in the idf file:
+
+\begin{lstlisting}
+
+Output:Variable,
+      Environment,                 !- Key Value
+      Site Outdoor Air Drybulb Temperature,            !- Variable Name
+      TimeStep;                    !- Reporting Frequency
+
+
+  Output:Variable,
+      ZONE ONE,                    !- Key Value
+      Zone Mean Air Temperature,   !- Variable Name
+      TimeStep;                    !- Reporting Frequency
+
+
+  Output:Variable,
+      Environment,                 !- Key Value
+      Site Outdoor Air Relative Humidity,   !- Variable Name
+      TimeStep;                    !- Reporting Frequency
+
+
+  Output:Variable,
+      ZONE ONE,                    !- Key Value
+      Zone Air Relative Humidity,  !- Variable Name
+      TimeStep;                    !- Reporting Frequency
+\end{lstlisting}
+
+To enter schedules to which the external interface writes, we use:
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport:To:Schedule,
+      FMU_OthEquSen_ZoneOne,   !- EnergyPlus Variable Name
+      Any Number,              !- Schedule Type Limits Names
+      MoistAir.fmu,            !- FMU Filename
+      Model1,                  !- FMU Model Name
+      QSensible,               !- FMU Model Variable Name
+      0;                       !- Initial Value
+
+
+  ExternalInterface:FunctionalMockupUnitImport:To:Schedule,
+      FMU_OthEquLat_ZoneOne,   !- EnergyPlus Variable Name
+      Any Number,              !- Schedule Type Limits Names
+      MoistAir.fmu,            !- FMU Filename
+      Model1,                  !- FMU Model Name
+      QLatent,                 !- FMU Model Variable Name
+      0;                       !- Initial Value
+\end{lstlisting}
+
+This completes the configuration that is required to simulate EnergyPlus with the FMU.
+
+\subsection{Example 2: Interface using ExternalInterface:FunctionalMockupUnitImport:To:Actuator}\label{example-2-interface-using-externalinterfacefunctionalmockupunitimporttoactuator}
+
+In this example, a shading controller with a finite state machine is implemented in a FMU (ShadingController.fmu). Inputs of the FMU are the outside temperature (TRoo) and the solar irradiation (ISolExt) that is incident on the window. The output of the FMU is the shading actuation signal (yShade).This example describes how to set up EnergyPlus to exchange data between the FMU and EnergyPlus, using an Energy Management System (EMS) actuator.
+
+To interface EnergyPlus using the EMS feature, the following four items are needed:
+
+\begin{itemize}
+\item
+  An object that instructs EnergyPlus to activate the external interface.
+\item
+  An object that specifies the FMU and its instances.
+\item
+  EnergyPlus objects that read data from EnergyPlus and send to FMU.
+\item
+  EnergyPlus objects that read data from FMU and send to EnergyPlus.
+\end{itemize}
+
+\subsubsection{Creating the EnergyPlus idf file}\label{creating-the-energyplus-idf-file-1-000}
+
+To create the EnergyPlus idf file the user should:
+
+\begin{itemize}
+\item
+  Use the \emph{parser} to generate a temporary idf.
+\item
+  Copy the FMU information from the temporary idf into the full idf file.
+\item
+  Modify the full idf file to link the FMU variables with EnergyPlus variables
+\end{itemize}
+
+The code below shows how the objects will be in the idf.
+
+To activate the external interface, we use:
+
+\begin{lstlisting}
+
+ExternalInterface,           !- Object to activate the external interface
+   FunctionalMockupUnitImport; !- Name of external interface
+\end{lstlisting}
+
+To define the FMU that will be linked to EnergyPlus, we use:
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport,
+      ShadingController.fmu,            !- FMU Filename
+      15,                       !- FMU Timeout in milli-seconds
+      0;                        !- FMU LoggingOn
+\end{lstlisting}
+
+To enter the two output variables from which the external interface read from and send to FMUs, we use:
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+      Zn001:Wall001:Win001,             !- EnergyPlus Key Value
+      Surface Outside Face Incident Solar Radiation Rate per Area,
+      ShadingController.fmu,            !- FMU Filename
+      Model1,                           !- FMU Model Name
+     ISolExt;                          !- FMU Model Variable Name
+
+
+  ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+      WEST ZONE,                        !- EnergyPlus Key Value
+      Zone Mean Air Temperature,        !- EnergyPlus Variable Name
+      ShadingController.fmu,            !- FMU Filename
+      Model1,                           !- FMU Model Name
+      TRoo;                             !- FMU Model Variable Name
+\end{lstlisting}
+
+These output variables need to be specified in the idf file:
+
+\begin{lstlisting}
+
+Output:Variable,
+      Zn001:Wall001:Win001,               !- Key Value
+      Surface Outside Face Incident Solar Radiation Rate per Area,  !- Var Name
+      TimeStep;                           !- Reporting Frequency
+
+
+  Output:Variable,
+      WEST ZONE,                          !- Key Value
+      Zone Mean Air Temperature,          !- Variable Name
+      TimeStep;                           !- Reporting Frequency
+\end{lstlisting}
+
+To enter the actuator that changes the control status of the window with name ``Zn001:Wall001:Win001'', we use:
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport:To:Actuator,
+  Zn001_Wall001_Win001_Shading_Deploy_Status,  !- EnergyPlus Variable Name
+      Zn001:Wall001:Win001,                !- Actuated Component Unique Name
+      Window Shading Control,                  !- Actuated Component Type
+      Control Status,                      !- Actuated Component Control Type
+      ShadingController.fmu,                   !- FMU Filename
+      Model1,                                  !- FMU Model Name
+      yShade,                                  !- FMU Model Variable Name
+      6;                                       !- Initial Value
+\end{lstlisting}
+
+~~~~~ This completes the configuration that is required to simulate EnergyPlus with the FMU.
+
+\subsection{Example 3: Interface using ExternalInterface:FunctionalMockupUnitImport:To:Variable}\label{example-3-interface-using-externalinterfacefunctionalmockupunitimporttovariable}
+
+This example implements the same controller as the Example 2. However, the interface with EnergyPlus is done using an external interface variable instead of an external interface actuator. Inputs of the FMU are the outside temperature (TRoo) and the solar irradiation (ISolExt) that is incident on the window. The output of the FMU is the shading actuation signal (yShade).
+
+To interface EnergyPlus using an external interface variable, the following items are needed:
+
+\begin{itemize}
+\item
+  An object that instructs EnergyPlus to activate the external interface.
+\item
+  An object that specifies the FMU and its instances.
+\item
+  EnergyPlus objects that read data from EnergyPlus and send to FMU.
+\item
+  EnergyPlus objects that read data from FMU and send to EnergyPlus.
+\end{itemize}
+
+\subsubsection{Creating the EnergyPlus idf file}\label{creating-the-energyplus-idf-file-2-000}
+
+To create the EnergyPlus idf file the user should:
+
+\begin{itemize}
+\item
+  Use the \emph{parser} to generate a temporary idf.
+\item
+  Copy the FMU information from the temporary idf into the full idf file.
+\item
+  Modify the full idf file to link the FMU variables with EnergyPlus
+\end{itemize}
+
+The code below shows how the objects will be in the idf.
+
+To activate the external interface, we use:
+
+\begin{lstlisting}
+
+ExternalInterface,           !- Object to activate the external interface
+   FunctionalMockupUnitImport; !- Name of external interface
+\end{lstlisting}
+
+To define the FMU that will be linked to EnergyPlus, we use:
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport,
+      ShadingController.fmu,            !- FMU Filename
+      15,                       !- FMU Timeout in milli-seconds
+      0;                        !- FMU LoggingOn
+\end{lstlisting}
+
+To enter the two output variables from which the external interface read from and send to FMUs, we use:
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+      Zn001:Wall001:Win001,             !- EnergyPlus Key Value
+      Surface Outside Face Incident Solar Radiation Rate per Area,
+      ShadingController.fmu,            !- FMU Filename
+      Model1,                           !- FMU Model Name
+     ISolExt;                          !- FMU Model Variable Name
+
+
+  ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+      WEST ZONE,                        !- EnergyPlus Key Value
+      Zone Mean Air Temperature,        !- EnergyPlus Variable Name
+      ShadingController.fmu,            !- FMU Filename
+      Model1,                           !- FMU Model Name
+      TRoo;                             !- FMU Model Variable Name
+\end{lstlisting}
+
+These output variables need to be specified in the idf file:
+
+\begin{lstlisting}
+
+Output:Variable,
+      Zn001:Wall001:Win001,               !- Key Value
+      Surface Outside Face Incident Solar Radiation Rate per Area,  !- Var Name
+      TimeStep;                           !- Reporting Frequency
+
+
+  Output:Variable,
+      WEST ZONE,                          !- Key Value
+      Zone Mean Air Temperature,          !- Variable Name
+      TimeStep;                           !- Reporting Frequency
+\end{lstlisting}
+
+To write data from the external interface to an EnergyPlus EMS variable, we use the following item in idf file:
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport:To:Variable,
+      Shade_Signal,            !- EnergyPlus Variable Name
+      ShadingController.fmu,   !- FMU Filename
+      Model1,                  !- FMU Model Name
+      yShade,                  !- FMU Model Variable Name
+      1;                       !- Initial Value
+\end{lstlisting}
+
+which declares a variable with name yShade that can be used in an Erl program to actuate the shading control of the window ``Zn001:Wall001:Win001'' as follows:
+
+\begin{lstlisting}
+
+! EMS program. The first assignments sets the shading status and converts it into the
+  !              EnergyPlus signal (i.e., replace 1 by 6).
+  !              The second assignment sets yShade to
+  !              an EnergyManagementSystem:OutputVariable
+  !              which will be read by the external interface.
+    EnergyManagementSystem:Program,
+      Set_Shade_Control_State,          !- Name
+      Set Shade_Signal = 6*yShade,      !- Program Line 1
+      Set Shade_Signal_01 = yShade+0.1; !- Program Line 2
+
+
+  ! Declare an actuator to which the EnergyManagementSystem:Program will write
+    EnergyManagementSystem:Actuator,
+      Shade_Signal,  !- Name
+      Zn001:Wall001:Win001,             !- Actuated Component Unique Name
+      Window Shading Control,           !- Actuated Component Type
+      Control Status;                   !- Actuated Component Control Type
+
+
+  ! Declare a global variable to which the EnergyManagementSystem:Program will write
+    EnergyManagementSystem:GlobalVariable,
+      Shade_Signal_01;                  !- Name of Erl variable
+\end{lstlisting}
+
+This completes the configuration that is required to simulate EnergyPlus with the FMU.
diff --git a/doc/external-interfaces-application-guide/src/external-interface-s/introduction.tex b/doc/external-interfaces-application-guide/src/external-interface-s/introduction.tex
new file mode 100644
index 00000000000..12243fd6cda
--- /dev/null
+++ b/doc/external-interfaces-application-guide/src/external-interface-s/introduction.tex
@@ -0,0 +1,3 @@
+\section{Introduction}\label{introduction}
+
+The ExternalInterface allows coupling EnergyPlus to the Building Controls Virtual Test Bed (BCVTB). It supports the import of Functional Mock-up Units (FMUs) for co-simulation as well as the export of EnergyPlus as a FMU for co-simulation. BCVTB is a software environment that allows expert users to couple different simulation programs for distributed simulation or for a real-time simulation that is connected to a building control system. For example, the BCVTB allows simulation of the building envelope and HVAC system in EnergyPlus and the control logic in MATLAB/Simulink, while exchanging data between the two programs as they simulate. The BCVTB can be downloaded from http://simulationresearch.lbl.gov/bcvtb. A FMU is a component which implements the Functional Mock-up Interface (FMI) standard (http://www.modelisar.com).
diff --git a/doc/external-interfaces-application-guide/src/external-interfaces-application-guide.tex b/doc/external-interfaces-application-guide/src/external-interfaces-application-guide.tex
new file mode 100644
index 00000000000..63f37402bb8
--- /dev/null
+++ b/doc/external-interfaces-application-guide/src/external-interfaces-application-guide.tex
@@ -0,0 +1 @@
+\input{../title}
diff --git a/doc/external-interfaces-application-guide/src/references.tex b/doc/external-interfaces-application-guide/src/references.tex
new file mode 100644
index 00000000000..74a2ca45493
--- /dev/null
+++ b/doc/external-interfaces-application-guide/src/references.tex
@@ -0,0 +1,13 @@
+\chapter{References}\label{references}
+
+Hensen, Jan L. M. 1999. ``A comparison of coupled and de-coupled solutions for temperature and air flow in a building.'' \emph{ASHRAE Transactions 105 (2): 962--969}.
+
+Zhai, Zhiqiang John, and Qingyan Yan Chen. 2005. ``Performance of coupled building energy and CFD simulations.'' \emph{Energy and Buildings 37 (4): 333--344}.
+
+BCVTB Documentation. 2011. Online available at: \url{http://simulationresearch.lbl.gov/bcvtb/releases/1.0.0/doc/manual/index.xhtml} {[}last accessed: 06/13/2011{]}.
+
+Expat XML Parser. 2011. http://sourceforge.net/projects/expat/ \emph{{[}Last accessed: 06/20/2011{]}}.
+
+G. Fábián, D.A. van Beek, J.E. Rooda. 2008. Substitute equations for index reduction and discontinuity handling.~ In Proc. of the Third International Symposium on Mathematical Modeling, Vienna, Austria.
+
+Modelisar. 2010. ``Functional Mock-up Interface for Co-Simulation.'' \href{http://www.modelisar.com/specifications/FMI_for_CoSimulation_v1.0.pdf}{\emph{http://www.modelisar.com/specifications/FMI\_for\_CoSimulation\_v1.0.pdf}} \emph{{[}Last accessed: 06/06/2011{]}}.
diff --git a/doc/getting-started/CMakeLists.txt b/doc/getting-started/CMakeLists.txt
new file mode 100644
index 00000000000..5295f28317a
--- /dev/null
+++ b/doc/getting-started/CMakeLists.txt
@@ -0,0 +1,87 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/getting-started.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/title.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/energyplus-overview.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/energyplus-overview/what-is-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/energyplus-overview/why-does-energyplus-exist-and-what-were-its.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/energyplus-overview/energyplus-documentation-library.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/getting-started-with-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/running-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/running-energyplus/introduction.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/running-energyplus/ep-launch-program.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/running-energyplus/energyplus-file-extensions.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/tutorial-example-for-running-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/tutorial-example-for-running-energyplus/running-energyplus-building-envelope-internal.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/tutorial-example-for-running-energyplus/instructions.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/overall-scheme-methodology-for-running.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/overall-scheme-methodology-for-running/building-simulation.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/overall-scheme-methodology-for-running/a-methodology-for-using-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/tutorial-exercise-2.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/tutorial-exercise-2/unitary-system-and-vav-using-hvactemplate.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/tutorial-exercise-2/instructions-001.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/idf-editor-brief-introduction.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/hvactemplate-objects.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/data-sets.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/slab-and-basement-programs.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/coefficient-curve-generation.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/useful-programs.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/weatherdata.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/results-processing.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/hvac-diagram.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/csvproc.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/convertesomtr.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/datafiles.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/other-useful-programs-information/library-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/energy-meters.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/energy-meters/standard-energy-meters.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/energy-meters/custom-meters.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/src/standard-energyplus-units.tex
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/../title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image001.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image002.jpg
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image004.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image005.jpg
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image006.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image007.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image008.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image009.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image010.jpg
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image011.jpg
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image012.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image013.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image014.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image015.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image016.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image017.jpg
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image018.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image019.jpg
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image020.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image021.jpg
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image022.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image023.png
+  ${CMAKE_SOURCE_DIR}/doc/getting-started/media/image024.jpg
+) 
+
+SET( SOURCE_FILENAME "getting-started" )
+SET( OUTPUT_FILENAME "GettingStarted" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/getting-started/getting-started.tex b/doc/getting-started/getting-started.tex
new file mode 100644
index 00000000000..e0c21e3448e
--- /dev/null
+++ b/doc/getting-started/getting-started.tex
@@ -0,0 +1,92 @@
+\input{../header}
+
+\title{Getting Started}
+
+\hypersetup{unicode=true,
+            pdftitle={Getting Started},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/title}
+
+\input{src/energyplus-overview}
+
+\input{src/energyplus-overview/what-is-energyplus}
+
+\input{src/energyplus-overview/why-does-energyplus-exist-and-what-were-its}
+
+\input{src/energyplus-overview/energyplus-documentation-library}
+
+\input{src/getting-started-with-energyplus}
+
+\input{src/running-energyplus}
+
+\input{src/running-energyplus/introduction}
+
+\input{src/running-energyplus/ep-launch-program}
+
+\input{src/running-energyplus/energyplus-file-extensions}
+
+\input{src/tutorial-example-for-running-energyplus}
+
+\input{src/tutorial-example-for-running-energyplus/running-energyplus-building-envelope-internal}
+
+\input{src/tutorial-example-for-running-energyplus/instructions}
+
+\input{src/overall-scheme-methodology-for-running}
+
+\input{src/overall-scheme-methodology-for-running/building-simulation}
+
+\input{src/overall-scheme-methodology-for-running/a-methodology-for-using-energyplus}
+
+\input{src/tutorial-exercise-2}
+
+\input{src/tutorial-exercise-2/unitary-system-and-vav-using-hvactemplate}
+
+\input{src/tutorial-exercise-2/instructions-001}
+
+\input{src/idf-editor-brief-introduction}
+
+\input{src/other-useful-programs-information}
+
+\input{src/other-useful-programs-information/hvactemplate-objects}
+
+\input{src/other-useful-programs-information/data-sets}
+
+\input{src/other-useful-programs-information/slab-and-basement-programs}
+
+\input{src/other-useful-programs-information/coefficient-curve-generation}
+
+\input{src/other-useful-programs-information/useful-programs}
+
+\input{src/other-useful-programs-information/weatherdata}
+
+\input{src/other-useful-programs-information/results-processing}
+
+\input{src/other-useful-programs-information/hvac-diagram}
+
+\input{src/other-useful-programs-information/csvproc}
+
+\input{src/other-useful-programs-information/convertesomtr}
+
+\input{src/other-useful-programs-information/datafiles}
+
+\input{src/other-useful-programs-information/library-files}
+
+\input{src/energy-meters}
+
+\input{src/energy-meters/standard-energy-meters}
+
+\input{src/energy-meters/custom-meters}
+
+\input{src/standard-energyplus-units}
+
+\end{document}
diff --git a/doc/src/docs/GettingStarted/media/ep.gif b/doc/getting-started/media/ep.gif
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diff --git a/doc/getting-started/src/energy-meters.tex b/doc/getting-started/src/energy-meters.tex
new file mode 100644
index 00000000000..4fedd8d970f
--- /dev/null
+++ b/doc/getting-started/src/energy-meters.tex
@@ -0,0 +1 @@
+\chapter{Energy Meters}\label{energy-meters}
diff --git a/doc/getting-started/src/energy-meters/custom-meters.tex b/doc/getting-started/src/energy-meters/custom-meters.tex
new file mode 100644
index 00000000000..d8539e202f9
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+++ b/doc/getting-started/src/energy-meters/custom-meters.tex
@@ -0,0 +1,3 @@
+\section{Custom Meters}\label{custom-meters}
+
+You can also define your own ``custom meters'' from variable names that are summed during the simulation.~ You assign the proper fuel type during the definition (review Input Output Reference, objects: \textbf{Meter:Custom} and \textbf{Meter:CustomDecrement}) for further requirements.
diff --git a/doc/getting-started/src/energy-meters/standard-energy-meters.tex b/doc/getting-started/src/energy-meters/standard-energy-meters.tex
new file mode 100644
index 00000000000..24fd5d9fa3b
--- /dev/null
+++ b/doc/getting-started/src/energy-meters/standard-energy-meters.tex
@@ -0,0 +1,144 @@
+\section{Standard Energy Meters}\label{standard-energy-meters}
+
+Meters provide one way for EnergyPlus to report energy use in a form that is pallatable to the users. The primary implemented method for output gives very fine detail (down to the variable level) for results from EnergyPlus. However, to get the required energy use, there may be several variables that need to be polled and accumulated. The meter implementation for EnergyPlus accomplishes this reporting.
+
+\begin{figure}[hbtp] % fig 24
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image024.jpg}
+\caption{Illustration of Energy Metering \protect \label{fig:illustration-of-energy-metering}}
+\end{figure}
+
+Meters can be used to typify energy use by type and by component. The diagrams and tables illustrate how the meters have been incorporated into EnergyPlus.
+
+As shown in the figure above, energy use for the facility is grouped according to fuel type (see Table~\ref{table:table-of-metered-fuel-types}. Table of Metered Fuel Types), by meter type (see Table~\ref{table:overall-meter-types}. Overall Meter Types) and by end use category type (see Table~\ref{table:end-use-category-types}. End Use Category Types).
+
+% table 7
+\begin{longtable}[c]{@{}l@{}}
+\caption{Overall Meter Types \label{table:overall-meter-types}} \tabularnewline
+\toprule 
+Meters \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Overall Meter Types} \tabularnewline
+\toprule 
+Meters \tabularnewline
+\midrule
+\endhead
+
+Facility \tabularnewline
+Building \tabularnewline
+Zone \tabularnewline
+System \tabularnewline
+Plant \tabularnewline
+\bottomrule
+\end{longtable}
+
+Both the fuel types and enduse types are set within the program by the developers. Current Fuel types are shown in the table below. There is also a special category called ``EnergyTranser''.
+
+% table 8
+\begin{longtable}[c]{@{}l@{}}
+\caption{Table of Metered Fuel Types \label{table:table-of-metered-fuel-types}} \tabularnewline
+\toprule 
+Utility/Fuel Types \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table of Metered Fuel Types} \tabularnewline
+\toprule 
+Utility/Fuel Types \tabularnewline
+\midrule
+\endhead
+
+Electricity \tabularnewline
+Gas \tabularnewline
+Gasoline \tabularnewline
+Diesel \tabularnewline
+Coal \tabularnewline
+FuelOil\#1 \tabularnewline
+FuelOil\#2 \tabularnewline
+Propane \tabularnewline
+Water \tabularnewline
+Steam \tabularnewline
+DistrictCooling \tabularnewline
+DistrictHeating \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{longtable}[c]{@{}l@{}}
+\toprule 
+AdditionalTypes \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+AdditionalTypes \tabularnewline
+\midrule
+\endhead
+
+HeatingCoils \tabularnewline
+CoolingCoils \tabularnewline
+Chillers \tabularnewline
+Boilers \tabularnewline
+Baseboard \tabularnewline
+HeatRecoveryForCooling \tabularnewline
+HeatRecoveryForHeating \tabularnewline
+\bottomrule
+\end{longtable}
+
+The end use types are shown in the following table:
+
+% table 9
+\begin{longtable}[c]{@{}l@{}}
+\caption{End Use Category Types \label{table:end-use-category-types}} \tabularnewline
+\toprule 
+End Use Types \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{End Use Category Types} \tabularnewline
+\toprule 
+End Use Types \tabularnewline
+\midrule
+\endhead
+
+InteriorLights \tabularnewline
+ExteriorLights \tabularnewline
+InteriorEquipment \tabularnewline
+ExteriorEquipment \tabularnewline
+Fans \tabularnewline
+Pumps \tabularnewline
+Heating \tabularnewline
+Cooling \tabularnewline
+HeatRejection \tabularnewline
+Humidifier \tabularnewline
+HeatRecovery \tabularnewline
+DHW \tabularnewline
+Cogeneration \tabularnewline
+Refrigeration \tabularnewline
+Miscellaneous \tabularnewline
+\bottomrule
+\end{longtable}
+
+Additional End Use Types Only Used for EnergyTransfer:
+
+\begin{longtable}[c]{@{}l@{}}
+\toprule 
+AdditionalTypes \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+AdditionalTypes \tabularnewline
+\midrule
+\endhead
+
+HeatingCoils \tabularnewline
+CoolingCoils \tabularnewline
+Chillers \tabularnewline
+Boilers \tabularnewline
+Baseboard \tabularnewline
+HeatRecoveryForCooling \tabularnewline
+HeatRecoveryForHeating \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/getting-started/src/energyplus-overview.tex b/doc/getting-started/src/energyplus-overview.tex
new file mode 100644
index 00000000000..ccce5884e02
--- /dev/null
+++ b/doc/getting-started/src/energyplus-overview.tex
@@ -0,0 +1,3 @@
+\chapter{EnergyPlus Overview}\label{energyplus-overview}
+
+Welcome to EnergyPlus! This section offers a big picture view of what EnergyPlus is, what it does, why it exists, and what its goals are AND provides an overview to the \textbf{EnergyPlus documentation library}. While this document does not provide every detail on the program, it does give the reader a macroscopic view of EnergyPlus and how it is intended to fit into the energy analysis and thermal load simulation software continuum.
diff --git a/doc/getting-started/src/energyplus-overview/energyplus-documentation-library.tex b/doc/getting-started/src/energyplus-overview/energyplus-documentation-library.tex
new file mode 100644
index 00000000000..79091e8bd82
--- /dev/null
+++ b/doc/getting-started/src/energyplus-overview/energyplus-documentation-library.tex
@@ -0,0 +1,77 @@
+\section{EnergyPlus Documentation Library}\label{energyplus-documentation-library}
+
+The documentation library for EnergyPlus has historically been provided in the form of pdf's packaged with the release. As of the 8.3.0 release, a major conversion was completed where the source of the docs was changed to Markdown. This allows for numerous improvements:
+
+\begin{itemize}
+\tightlist
+\item
+  Easy to automatically translate in between other markup languages, including html, thus making it easy to host as a web page.
+\item
+  Merging can be done automatically so the documentation source can stay alongside the source code, idd, and idfs, and all be merged at once. With the ever-increasing visibility of EnergyPlus development, it is becoming key that documentation is directly in sync with the rest of the program files.
+\item
+  Since Markdown is clear text, it is platform-independent and maximizes the possibility for outside contributions to EnergyPlus.
+\end{itemize}
+
+The Markdown source for the latest major release is converted to html which is then available at http://energyplus.net/documentation. The current, or ``daily'' documentation is available at http://nrel.github.io/EnergyPlus, but since this is a moving target within a release cycle, it is recommended that users view the .net documentation page.
+
+Two key aspects of the documentation that are currently in development and should be completed soon are:
+
+\begin{itemize}
+\tightlist
+\item
+  Search: the ability to search the online html docs easily
+\item
+  Download as pdf: the ability to download pdfs for local/offline access
+\end{itemize}
+
+The Markdown based documentation is structured similarly to the pdfs, though the larger files are broken into smaller pieces for faster load times due to the dynamic nature of the math, especially in the engineering reference. Each of the main documentation pieces are described here.
+
+\subsection{User Information Documents}\label{user-information-documents}
+
+The following documents relate to using EnergyPlus, the engine. These documents cover a full range of questions and should be the first place a beginning or even experienced user would go to find out how the program works, what it expects as input, what it produces as output, etc. In general, the information in these documents is not highly technical, but it is detailed enough to use the basic capabilities of the program.
+
+\textbf{\emph{Getting Started with EnergyPlus -- the Basics Manual:}} You are currently reading the Overview section of this document. The overview contains a ``big picture'' description of the EnergyPlus program as well as background of its development and the goals to which it ascribes. The remainder of the Getting Started document provides beginning users with an introduction into how to run EnergyPlus, what files are needed for EnergyPlus to execute, and what files are produced when EnergyPlus runs successfully. It also provides some guidance as to how to determine what potential sources of errors are when EnergyPlus runs into problems and how serious those problems might be.
+
+\textbf{\emph{Input and Output Reference:}} This document is a thorough description of the various input and output files related to EnergyPlus, the format of these files, and how the files interact and interrelate.
+
+\textbf{\emph{Output Details, Examples and Data Sets:}} While the Input and Output Reference document touch on some of the outputs from EnergyPlus, this document has more details and specific examples. It also addresses the reference data sets that are included.
+
+\textbf{\emph{Auxiliary Programs}:}~This document contains information for the auxiliary programs that are part of the EnergyPlus package. For example, this document contains the user manual for the Weather Converter program, descriptions on using Ground Heat Transfer auxiliary programs with EnergyPlus, Compact HVAC descriptions, the Transition program/package and other assorted documents.
+
+\subsection{Engineering Reference Document}\label{engineering-reference-document}
+
+The Engineering Reference provides more in-depth knowledge into the theoretical basis behind the various calculations contained in the program. This reference includes more information on modeling equations, limitations, literature references, etc. The document contains the following information and is structured along the lines of the above illustration (Figure~\ref{fig:energyplus-internal-elements}. EnergyPlus -- Internal elements).
+
+\textbf{\emph{Heat Balance Overview and Reference:}}~ This section describes the heat balance calculations that form the basis of the EnergyPlus building model. It includes descriptions of shadowing calculations and other pieces of the model.
+
+\textbf{\emph{HVAC Overview and Reference:}}This section contains a description of the loop-based approach used by EnergyPlus to model the HVAC systems: air loops, water loops, etc. It includes a description of the higher-level managers that control the simulation flow as well as some information on the various components that can be linked together to comprise an HVAC system.
+
+\textbf{\emph{HVAC Branch Based Input Description:}}This section is a special extension of both the input document and the HVAC overview document. It contains more detail on the various HVAC input objects and how these different object link together to form an HVAC description. It contains vital information mainly for the interface developer but also provides users with an in-depth look at the inner workings of the loop approach adopted by EnergyPlus.
+
+\textbf{\emph{Encyclopedic Reference:}}If the information did not fit in the above categories, then the last part of the Engineering Reference is a detailed description of the various models.
+
+\subsection{Application Guides}\label{application-guides}
+
+The application guides are intended to address specific applications using EnergyPlus where the other documents may not provide cohesive examples of intended usage; that is, the techniques for doing certain things may be spread throughout other documents but warrant a more ``how to'' approach that will be present in these documents. The application guides are intended to become more prolific over time, specifically targeted to questions users have sent to the helpdesk support site.
+
+\textbf{\emph{Current Application Guides:}}
+
+\textbf{\emph{EMS Application Guide:}} This guide contains information useful to use the advanced feature of EnergyPlus: Energy Management System tweaks. The Erl language is described and examples for use are given.
+
+\textbf{\emph{External Interface Application Guide:}} This guide contains information specific to using the external interface feature of EnergyPlus to connect other simulation systems.
+
+\textbf{\emph{Plant Application Guide:}} This guide details the methods for simulating real chilled and hot water plant systems within EnergyPlus.
+
+\textbf{\emph{Using EnergyPlus for Compliance Guide:}} This guide contains information specific to using EnergyPlus in Compliance and Standard Rating systems.
+
+\textbf{\emph{External Interface(s) Application Guide:}} This guide contains information about external interfaces (through the Building Controls Virtual Test Bed link) to EnergyPlus.
+
+\textbf{\emph{Tips \& Tricks for Using EnergyPlus:}} This guide contains short tips and tricks for using various parts of EnergyPlus.
+
+\subsection{Developer Menu and Developer Information Documents}\label{developer-menu-and-developer-information-documents}
+
+The following documents will be most useful to potential developers of EnergyPlus, both Interface Developers and Module Developers. Interface Developers will be creating input and output wraps on EnergyPlus so that is it is usable to the architect, design engineers, and others. Module developers will be creating new modules within the EnergyPlus structure and framework.
+
+\textbf{\emph{Interface Developer's Guide:}} This document is critically important to persons interested in developing an interface that provides input to and read output from EnergyPlus. It is a comprehensive guide to the input data dictionary and the input data files that contain a user's building data. Each piece of input syntax is described in detail. In addition, the mechanism for obtaining output and the format in which output will be produced are discussed. This document also contains sections on weather files and units. Numerous samples and examples are given throughout the document with a full file length example provided in the appendix.
+
+\textbf{\emph{Module Developer's Guide:}} This document contains a wealth of information that is intended to provide as much assistance as possible to persons interested in adding modules to the EnergyPlus program. It reviews the module concept as outlined in the programming standard and how they have been implemented in EnergyPlus. It provides a description of how the various modules work together and how the program is structured from a module tree (inverted tree) perspective. One of the most important features of this document is a list of standard EnergyPlus service subroutines and modules that greatly simplify the developers' task of integrating their work into the program. Input and output issues are also addressed from the perspective of how modules actually obtain data from the input file and how each section of the code sends data to the output files.
diff --git a/doc/getting-started/src/energyplus-overview/what-is-energyplus.tex b/doc/getting-started/src/energyplus-overview/what-is-energyplus.tex
new file mode 100644
index 00000000000..119120ed907
--- /dev/null
+++ b/doc/getting-started/src/energyplus-overview/what-is-energyplus.tex
@@ -0,0 +1,51 @@
+\section{What is EnergyPlus?}\label{what-is-energyplus}
+
+EnergyPlus has its roots in both the BLAST and DOE--2 programs. BLAST (Building Loads Analysis and System Thermodynamics) and DOE--2 were both developed and released in the late 1970s and early 1980s as energy and load simulation tools. Their intended audience is a design engineer or architect that wishes to size appropriate HVAC equipment, develop retrofit studies for life cycling cost analyses, optimize energy performance, etc. Born out of concerns driven by the energy crisis of the early 1970s and recognition that building energy consumption is a major component of the American energy usage statistics, the two programs attempted to solve the same problem from two slightly different perspectives. Both programs had their merits and shortcomings, their supporters and detractors, and solid user bases both nationally and internationally.
+
+Like its parent programs, EnergyPlus is an energy analysis and thermal load simulation program. Based on a user's description of a building from the perspective of the building's physical make-up, associated mechanical systems, etc., EnergyPlus will calculate the heating and cooling loads necessary to maintain thermal control setpoints, conditions throughout an secondary HVAC system and coil loads, and the energy consumption of primary plant equipment as well as many other simulation details that are necessary to verify that the simulation is performing as the actual building would. Many of the simulation characteristics have been inherited from the legacy programs of BLAST and DOE--2. Below is list of some of the features of the first release of EnergyPlus. While this list is not exhaustive, it is intended to give the reader and idea of the rigor and applicability of EnergyPlus to various simulation situations.
+
+\begin{itemize}
+\item
+  \textbf{Integrated, simultaneous solution} where the building response and the primary and secondary systems are tightly coupled (iteration performed when necessary)
+\item
+  \textbf{Sub-hourly, user-definable time steps} for the interaction between the thermal zones and the environment; variable time steps for interactions between the thermal zones and the HVAC systems (automatically varied to ensure solution stability)
+\item
+  \textbf{ASCII text based weather, input, and output files} that include hourly or sub-hourly environmental conditions, and standard and user definable reports, respectively
+\item
+  \textbf{Heat balance based solution} technique for building thermal loads that allows for simultaneous calculation of radiant and convective effects at both in the interior and exterior surface during each time step
+\item
+  \textbf{Transient heat conduction} through building elements such as walls, roofs, floors, etc. using conduction transfer functions
+\item
+  \textbf{Improved ground heat transfer modeling} through links to three-dimensional finite difference ground models and simplified analytical techniques
+\item
+  \textbf{Combined heat and mass transfer} model that accounts for moisture adsorption/desorption either as a layer-by-layer integration into the conduction transfer functions or as an effective moisture penetration depth model (EMPD)
+\item
+  \textbf{Thermal comfort models} based on activity, inside dry bulb, humidity, etc.
+\item
+  \textbf{Anisotropic sky model} for improved calculation of diffuse solar on tilted surfaces
+\item
+  \textbf{Advanced fenestration calculations} including controllable window blinds, electrochromic glazings, layer-by-layer heat balances that allow proper assignment of solar energy absorbed by window panes, and a performance library for numerous commercially available windows
+\item
+  \textbf{Daylighting controls} including interior illuminance calculations, glare simulation and control, luminaire controls, and the effect of reduced artificial lighting on heating and cooling
+\item
+  \textbf{Loop} \textbf{based configurable HVAC systems} (conventional and radiant) that allow users to model typical systems and slightly modified systems without recompiling the program source code
+\item
+  \textbf{Atmospheric pollution calculations} that predict CO\(_{2}\), SO\(_{x}\), NO\(_{x}\), CO, particulate matter, and hydrocarbon production for both on site and remote energy conversion
+\item
+  \textbf{Links to other popular simulation environments/components} such as WINDOW5, WINDOW6 and DElight to allow more detailed analysis of building components
+\end{itemize}
+
+More details on each of these features can be found in the various parts of the EnergyPlus documentation library.
+
+No program is able to handle every simulation situation. However, it is the intent of EnergyPlus to handle as many building and HVAC design options either directly or indirectly through links to other programs in order to calculate thermal loads and/or energy consumption on for a design day or an extended period of time (up to, including, and beyond a year). While the first version of the program contained mainly features directly linked to the thermal aspects of buildings, later versions of the program also included other issues that are important to the built environment: water, electrical systems, etc.
+
+\emph{Although it is important to note what EnergyPlus is, it is also important to remember what it is not.}
+
+\begin{itemize}
+\item
+  EnergyPlus is not a user interface. It is intended to be the simulation engine around which a third-party interface can be wrapped. Inputs and outputs are simple ASCII text that is decipherable but best left to a GUI (graphical user interface). This approach allows interface designers to do what they do best---produce quality tools specifically targeted toward individual markets and concerns. The availability of EnergyPlus frees up resources previously devoted to algorithm production and allows them to be redirected interface feature development in order to keep pace with the demands and expectations of building professionals.
+\item
+  EnergyPlus is currently not a life cycle cost analysis tool. It produces results that can then be fed into an LCC program. In general, calculations of this nature are better left to smaller ``utility'' programs which can respond more quickly to changes in escalation rates and changes to methodologies as prescribed by state, federal, and defense agencies.
+\item
+  EnergyPlus is not an architect or design engineer replacement. It does not check input, verify the acceptability or range of various parameters (expect for a limited number of very basic checks), or attempt to interpret the results. While many GUI programs assist the user in fine-tuning and correcting input mistakes, EnergyPlus still operates under the ``garbage in, garbage out'' standard. Engineers and architects will always be a vital part of the design and thermal engineering process.
+\end{itemize}
diff --git a/doc/getting-started/src/energyplus-overview/why-does-energyplus-exist-and-what-were-its.tex b/doc/getting-started/src/energyplus-overview/why-does-energyplus-exist-and-what-were-its.tex
new file mode 100644
index 00000000000..17c6191d3ae
--- /dev/null
+++ b/doc/getting-started/src/energyplus-overview/why-does-energyplus-exist-and-what-were-its.tex
@@ -0,0 +1,48 @@
+\section{Why does EnergyPlus exist and what were its original goals?}\label{why-does-energyplus-exist-and-what-were-its-original-goals}
+
+The existence of EnergyPlus is directly related to some of the increasingly obvious shortcomings of its predecessor programs---BLAST and DOE--2. Both programs, though still valid tools that will continue to have utility in various environments, have begun to show their age in a variety of ways. Both BLAST and DOE--2 were written in older version of FORTRAN and used features that will eventually be obsolete in new compilers. Both programs consisted of a significant amount of ``spaghetti code'' and outdated structures that made it difficult to maintain, support, and enhance. Neither BLAST nor DOE--2 is able to correctly handle feedback from the HVAC system to the zone conditions.
+
+Finally, the speed with which new technology in the HVAC field is developed has far outpaced the ability of the support and development groups of both programs to keep the programs current and viable. This is really the key issue in the existence of EnergyPlus: there simply are not enough researchers worldwide who have enough experience with the complex code of the programs to keep pace with new technology. In addition, due to the years of experience necessary to make modifications to either BLAST or DOE--2, it is extremely expensive and time consuming to produce models or train someone to become proficient in either program's code. The following paragraphs address how the goals of EnergyPlus have been carefully selected to solve the problems of the legacy programs and to make EnergyPlus an international repository for algorithms that can be made available to all interested parties.
+
+\textbf{\emph{Structure and Simulation Management:}} The ``spaghetti code'' nature of the parent programs resulted in great confusion as to how information flowed within the program, when data was modified or should be modified, and what was happening when. Thus, one of the goals of EnergyPlus development was to eliminate the interconnections between various program sections and the need to understand all parts of the code just to make an addition to a very limited part of the program. This goal was achieved through a program structure that implemented a ``manager'' philosophy. In effect, the program consists of many pieces (i.e., modules---see next paragraph) which when viewed graphically resemble an inverted tree. Instead of allowing lower level pieces of the program and calls to those sections of the code to infiltrate up to the highest level of the simulation, each branch exercises control over when its sub-branches are called. Thus, this is much like an organization chart where management over employees proceeds up a chain of command until it reaches the ``CEO'' of the simulation. In EnergyPlus, a subroutine called ManageSimulation serves the ``CEO'' role. This single subroutine controls four of the five main simulation loops (environment, day, hour, sub-hour time step; the system time step is controlled by the HVAC manager). In addition, this subroutine also sets global flags that are used by other subroutines and modules to determine the state of the simulation so that each part of the program knows whether to read input, initialize, simulate, report, etc. The manager philosophy makes the links between program modules simple and explicit. Typically, each module is accessible only through a call to its manager routine. Developers no longer have to worry about hidden and unexpected connections between and among program subroutines.
+
+\textbf{\emph{Modularity:}} One of the benefits of the structural improvements over the legacy programs is that the code can now be much more object-oriented and modular in nature. A result of the goal for improved structure in EnergyPlus was the definition of a well-organized, module concept that would facilitate adding features and links to other programs. It was decided that FORTRAN90 would be used for the initial release of EnergyPlus due to the fact that it:
+
+\begin{itemize}
+\item
+  is a modern, modular language with good compilers on many platforms
+\item
+  allows C-like data structures and mixed language modules
+\item
+  provides structure that begins to be object-based
+\item
+  allows long variable names (up to 32 characters)
+\item
+  provides backward compatibility with legacy code during the development process
+\end{itemize}
+
+The key benefit of modularity is that researchers can develop modules concurrently without interfering with other modules under development and with only a limited knowledge of the entire program structure. This feature is critical to promoting both widespread use and broad development of program models. EnergyPlus can only be successful if the pool of potential model developers increases significantly so that interest and economics drives what models are added to the program rather than have its extensions limited by a lack of intellectual resources. Thus, modularity and structure improvements in EnergyPlus solve the problems of not having enough experts to keep up with technology and the large start-up time and expense previously needed to bring someone up to speed on program additions.
+
+Since the original version (2001), EnergyPlus code and structure continued to evolve and adopt the ever changing Fortran Standard. However, in 2014, a full conversion of the simulation code to C++ was completed. The development team also adapted workflows and open sourced the code and posted it on \href{https://github.com/NREL/EnergyPlus}{Github}. Just like how the Fortran simulation code utilized modern Fortran standard capabilities, the C++ code utilizes modern (C++11\ldots{}) C++ standard capabilities.
+
+\textbf{\emph{Established Links:}} The modularity of EnergyPlus makes it easier for other developers to quickly add other component simulation modules. This means that it will be significantly easier to establish links to other programming elements. Since initially the EnergyPlus code will contain a significant number of existing modules, there will be many places within the HVAC code where natural links to new programming elements can be established. These are fully documented to assist other developers in a swift integration of their research into EnergyPlus. In addition to these more natural links in the HVAC section of the code, EnergyPlus will also have other more fluid links in areas such as the heat balance that will allow for interaction where the modules might be more complex or less component based. Again, the goal of this feature of EnergyPlus is maximize the number of developers who can quickly integrate their work into EnergyPlus for the minimum investment of resources. The following diagram depicts how other programs have already been linked to EnergyPlus and a big picture view of how future work can impact the program.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image001.png}
+\caption{EnergyPlus -- the big picture \protect \label{fig:energyplus-the-big-picture}}
+\end{figure}
+
+\textbf{\emph{Integration of Loads, Systems, and Plants:}} One of the strong points of EnergyPlus is the integration of all aspects of the simulation---loads, systems, and plants. Based on a research version of the BLAST program called IBLAST, system and plant output is allowed to directly impact the building thermal response rather than calculating all loads first, then simulating systems and plants. The simulation is coupled allowing the designer to more accurately investigate the effect of undersizing fans and equipment and what impact that might have on the thermal comfort of occupants within the building. The diagram below shows a basic overview of the integration of these important elements of a building energy simulation.
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image002.jpg}
+\caption{EnergyPlus -- Internal elements \protect \label{fig:energyplus-internal-elements}}
+\end{figure}
+
+\textbf{\emph{``Open'' Source Code:}} Another advantage of EnergyPlus that it shares with both BLAST and DOE--2 is that the source code of the program will be available and open for public inspection, revision, etc. The program is not intended to be a black box that is unintelligible to the users and developers around the world. While there are many conflicting ideas on what is meant by ``open'', EnergyPlus is certainly not closed since this would be counter to the goals that have already been stated. The hope is that this access to source code will improve the accuracy and usability of the program over the long term and allow many developers to work on the program simultaneously. This ``developer friendly'' stance is critical to keeping EnergyPlus current and in step with technological advances.
+
+In summary, the goals of EnergyPlus are ambitious but achievable via the path described above. EnergyPlus aims to be a program that is relatively simple to work with from the perspective of both the users and the developer. The development team made tremendous efforts to keep simulation code and algorithms as separate as possible and as modular as possible to minimize the overall knowledge that someone would need to have to add models to the program. This will minimize the resource investment and maximize the impact of current research in the field of building energy analysis and thermal load calculations. Finally, the full coupling of building envelopes, systems, and plants will provide a better understanding of how a building responds not only to the environmental factors that impact the building but also the HVAC system as it attempts to meet the thermal loads on the building.
+
+It is also important to note that testing and verification are key issues in the development of any new program such as EnergyPlus. While there are large sections of EnergyPlus that consist of brand new code, the majority of the heat balance code can be traced back to the original parent programs. It should be noted that while this code has been significantly reengineered the team used what has been termed an ``evolutionary reengineering'' (ER) process. In ER, program code is modified stepwise in an effort to restructure it, modularize it, replace old obsolete data structures, etc. The ultimate goal is to bring it up to current programming standards without starting over with new code. At each step along the way, the program is exercised over a variety of input files and parameters to insure that what were intended to be algorithm neutral changes in the program have not resulted in changes to the output. This process was very successful and bolstered confidence in the program. In addition, comparisons could be made back to legacy programs to show that the new program is at a minimum as accurate as its predecessors. Beyond this, EnergyPlus has also been subjected to a lengthy and rigorous testing plan by an outside agency as well as numerous beta testers. This level of effort and collaboration is unprecedented in the history of energy analysis and thermal load calculation programs and has resulted in a much higher level of confidence in the results produced by EnergyPlus.
diff --git a/doc/getting-started/src/getting-started-with-energyplus.tex b/doc/getting-started/src/getting-started-with-energyplus.tex
new file mode 100644
index 00000000000..b59245899ec
--- /dev/null
+++ b/doc/getting-started/src/getting-started-with-energyplus.tex
@@ -0,0 +1,41 @@
+\chapter{Getting Started with EnergyPlus}\label{getting-started-with-energyplus}
+
+The remainder of this document is intended to give you a start on using the program with a few simple tools (EP-Launch to help run the simulation; IDFEditor to help create or look at input files) as well as some of the features (such as energy meters, simulation results) of using the program.
+
+For learning about a specific input file, or a specific input object, the install includes two documents in the ExampleFiles folder:
+
+\begin{itemize}
+\item
+  Example Files Summary (highlights of each example file)
+\item
+  Example Files Links to Objects (for any object, up to 3 files using that object are shown)
+\end{itemize}
+
+The standard Windows install procedure has put the following information on your computer, in the directories/folders shown.
+
+The main EnergyPlus folder contains: * Energy+.idd * EnergyPlus.exe and dependent shared libraries (dll files) * RunEPlus.bat and other batch files for running EnergyPlus * readme file(s), license, etc. * EP-Macro.exe and other support binaries * bugreprt.txt~
+
+The general layout of folders from the install looks like:
+
+\begin{lstlisting}
+. EnergyPlus main folder
++-- Documentation
+|   +-- A link to find the documentation online, and any additional docs packaged with the installation
++-- DataSets
+|   +-- Reference Data Sets (libraries)
++-- MacroDataSets
+|   +-- Macroized Reference Data Sets (libraries)
++-- PreProcess
+|   +-- FMUParser              Tool for external interface specific applications
+|   +-- IDFEditor              Program files for the IDFEditor
+|   +-- GrndTempCalc           Special program to calculate ground temperatures.
+|   +-- DOE2Translator         Simple translator for DOE-2 files
+|   +-- WeatherConverter       Tool for performing weather file creation and conversion
+|   +-- ParametricPreprocessor Parametric simulation tool
+|   +-- IDFVersionUpdater      Graphical tool for updating old EnergyPlus files to the latest version
++-- PostProcess
+|   +-- ReadVarsEso            The simple post processor exe.
+|   +-- EPCompare              A graphical tool for comparing two EnergyPlus output sets
++-- ExampleFiles               Sample input, output, results files shipped with the program.
++-- WeatherData                Sample weather files shipped with the program.
+\end{lstlisting}
diff --git a/doc/getting-started/src/idf-editor-brief-introduction.tex b/doc/getting-started/src/idf-editor-brief-introduction.tex
new file mode 100644
index 00000000000..2bb93c5c8cf
--- /dev/null
+++ b/doc/getting-started/src/idf-editor-brief-introduction.tex
@@ -0,0 +1,93 @@
+\chapter{IDF Editor -- Brief Introduction}\label{idf-editor-brief-introduction}
+
+EnergyPlus has several options for the user to create input files. For the purposes of this document, we will describe briefly the workings of the IDF Editor that is supplied with the EnergyPlus Installation.~ The IDF Editor is a simple, ``intelligent'' editor that reads the EnergyPlus Data Dictionary (IDD) and allows creation/revision of EnergyPlus Input Files (IDF). It can be run from a shortcut in the main EnergyPlus directory (created as part of the install) or directly from EP-Launch.
+
+Full details of the IDF Editor can be found in the Auxiliary Programs document.~ IDD Conventions (to be able to read the IDD) are found in the Input Output Reference document. EnergyPlus standard units are described in several places, including later in this document.
+
+IDF Editor is an optional component of the EnergyPlus installation. For users who want a simple way of creating or editing EnergyPlus input data files (IDF), IDF Editor provides this service.~ The IDF Editor does not check inputs for validity, although some numeric fields are highlighted if out of range and some text fields are highlighted if they contain an invalid reference. For instructions and rules that must be followed when creating an IDF file the user should refer to the \href{../../EnergyPlusFromStarTeam/EnergyPlusFromStarTeam/Documentation/sources/InputOutputReference.pdf}{\emph{Input/Output Reference}} document.
+
+\begin{figure}[hbtp] % fig 21
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image021.jpg}
+\caption{IDF Editor Screen. \protect \label{fig:idf-editor-screen.}}
+\end{figure}
+
+\subsection{Start IDF Editor}\label{start-idf-editor}
+
+IDF Editor should be located in the EnergyPlus\textbackslash{}PreProcessor\textbackslash{}IDFEditor directory where you installed EnergyPlus. By double clicking on the IDF Editor icon you will get a screen similar to the one shown above. IDF Editor works in conjunction with the current EnergyPlus Input Data Directory (IDD) file that resides in the directory where EnergyPlus is installed. Another way to start the IDF Editor is from EP-Launch. Multiple IDF files can be opened at once.
+
+\subsection{Creating or Selecting an Input Data File}\label{creating-or-selecting-an-input-data-file}
+
+Creating a new input data file or selecting an existing input data file can be accomplished either through use of the File menu on the menu bar at the top of the screen or through use of the New File icon button or Open File icon button on the tool bar.
+
+\subsection{Class List}\label{class-list}
+
+The class list shows how the items for the IDF are grouped.~ This class list follows the Data Dictionary (IDD) description. Select a class from the list by clicking on and highlighting the class. The field to the left of the selected class in the `Class List' will either contain {[}------{]} to indicate that this class has no objects in the IDF file or it will contain a number like {[}0003{]} to indicate the number of times the object currently appears in the IDF file. For example, for the BuildingSurface:Detailed class selected in the screen above under the Thermal Zone Description/Geometry group, there are 40 objects in the IDF file. The details for these 40 objects or any new object that is defined are displayed in columns within the grid. Each object is made up of fields and can be used to further define the object. Any units attached to each field are shown in the second column. You may need to scroll down the `field' list or maximize the application to see all of the fields. Likewise, you may need to scroll to the right of the main grid to see other objects.
+
+Options under the view menu can change how you use the Class List. To display only classes that contain objects select the ``show classes with objects only'' option on the ``View'' menu. You can also toggle this feature on and off with CTRL+L. If the file is empty and has no objects, this toggle does not impact the display.
+
+The ``Show Quick Select Dropdowns'' view menu option adds two new input fields to the main screen. The input fields can be used to go quickly to different classes in the main list of classes. By typing in the top input field, the group that start with those letters are displayed. After selecting one and pressing the tab button, classes in that group are shown and by typing the first few letters, you can easily select a specific class. Pressing tab again displays that class and it objects. This method allow for quick selection of classes if you remember the group name and class name.
+
+\subsection{Changing Values}\label{changing-values}
+
+By clicking and highlighting a value within an object, several things happen:
+
+1)~~~Any user comments from the IDF file will be displayed in the `Comments from IDF' portion of the screen
+
+2)~~~Any notes contained in the IDD for this input field will be displayed in the `Explanation of Keyword' portion of the screen
+
+3)~~~The value can be edited. Depending on the field, a drop down list may display the default value, maximum and minimum, or other keywords that can be used with the field.
+
+4)~~~Numeric fields that can be autosized will include ``autosize'' as a selection in the drop down list.
+
+5)~~~Some numeric fields have a maximum and/or minimum value specified in the IDD. If the value entered is outside this range, the cell will be highlighted in pale orange.
+
+6)~~~For values that are names of nodes, a new dialog box titled ``Edit or Select Node Name'' can be shown when the small button is pressed that is on the right side in each node name cell.
+
+\subsection{Working with Objects}\label{working-with-objects}
+
+To delete an object, first click on any value for the object and then click on the ``Del Obj'' button. To add a new object, click on the ``New Obj'' button and a new object column with fields set to blanks, zeros, or default values will be added to the far right of the grid. The ``Dup Obj'' button is similar to ``New Obj'', but copies the values of the fields of the currently selected object. Copying and pasting an object or groups of objects is also possible using the ``Copy Obj'' and ``Paste Obj'' buttons.~ These allow objects to be copied between files are also good for copying from files in the DataSets subdirectory. (Also see the Edit menu to perform these functions.)
+
+\subsection{File Menu}\label{file-menu-000}
+
+The File menu can be used for creating or selecting input files just like the buttons on the IDF Editor screen (see the \emph{Creating or Selecting an Input File} section above). In addition, the File menu is used to save a file or exit the IDF Editor. More than one file can be opened at a time.
+
+The ``File'', ``Save Options'' screen is shown below.
+
+~\includegraphics{media/image022.png}
+
+Figure 22. IDF Editor Save Options Screen.
+
+The save options allow the order of the objects in the file to be sorted by type of object or to keep the original order of the objects (for an existing file). The placement of new objects when the original order is specified can be either at the top or bottom of the file.
+
+In addition, the Save Options also allow certain objects to be written to the file using a specific format that some users prefer. Selecting this option will format the following objects on a single line: Report, Report Meter, Report Variable, Version, Timestep in Hour, Inside Convection Algorithm, Outside Convection Algorithm, Solution Algorithm, Shadowing Calculations, Ground Reflectances, and GroundTemperatures:Deep. In addition, Schedule:Compact objects will be formatted to have two field for some lines. With this option, objects with geometric vertices are formatted to have the X, Y, and Z values on the same line. Those objects include: Surface:HeatTransfer, Surface:HeatTransfer:Sub, Surface:Shading:Detached:Fixed, Surface:Shading:Detached:Building and Surface:Shading:Attached.
+
+The settings for the save options are kept for each file saved from the IDF Editor.
+
+Also on the File menu is the Open DataSet menu and submenu. This allows you to open any input file that appears in the DataSet subdirectory and copy objects from them into another file. This is required because EnergyPlus does not read the DataSet files, it is up to you to include objects from them.
+
+\subsection{Edit Menu}\label{edit-menu-000}
+
+The Edit Menu offers options to create a new object, duplicate an object, and delete an object as well as finding and searching. The object options are the same operations as can be accomplished by using the `New Obj', `Dup Obj' and `Del Obj' buttons (see the \emph{Working with Objects} section above). In addition, the ``Next Row after Enter'' option can be toggled. When this option is on, the selection moves down one row after pressing Enter. The copy and paste object commands allow a single object to be copied within a file or between files. The pasted object appears as the last object in the class. This capability makes it easier to utilize the data in the DataSets directory. The Find Class and Search and Replace options can be used to search through the list of classes or the values of a file quickly. If renaming objects, the recommended approach is to rename the object and select the cell again and open the Search and Replace dialog. This will show other places in the file that use that object name that also may need to be changed.
+
+\subsection{View Menu}\label{view-menu-000}
+
+The View menu offers options for units and column widths. The Narrow/Medium/Wide Column options set the standard column width for items in the object grid. Individual columns can also be resized by dragging the column separator. The displayed value is rounded and/or expressed in scientific notation to fit within the column width.
+
+EnergyPlus input files must always be in SI units. Selecting ``Inch-Pound'' (IP) units in the View menu displays and edits values in IP units.
+
+1)~~~The IP unit will be displayed in the units column of the object grid. Some SI units convert to multiple IP units. For example, W becomes Btu/hr for heating and cooling capacity but remains as W for lighting and electrical equipment.
+
+2)~~~All conversion factors used in the IDF editor are documented in a block of comments near the top of the Energy+.IDD file.
+
+3)~~~Schedules, fluid properties and curves now support IP unit conversions. For curves, the minimum and maximum values are converted but the coefficients are not.
+
+To display only classes that contain objects select the ``show classes with objects only'' option on the ``View'' menu. You can also toggle this feature on and off with CTRL+L. If the file is empty and has no objects, this toggle does not impact the display.
+
+The ``Show Quick Select Dropdowns'' view menu option adds two new input fields to the main screen. The input fields can be used to go quickly to different classes in the main list of classes.
+
+The ``Validity Check'' function has replaced and expanded upon the old~ ``Check Out-of-Range'' function. It can also be started by using CTRL-R. The ``Validity Check'' function performs three kinds of validity checks. It displays the values and locations for objects with values that are either above the maximum or below the minimum values.~ It also displays fields that contain invalid references. The ``Validity Check'' dialog also shows when an entry for a field is not one of the possible lists of choices. The Perform Validity Check When Saving File can be turned on and off and automatically performs the check whenever the file is saved.
+
+\subsection{Help Menu}\label{help-menu-000}
+
+The Help menu offers options to open the EnergyPlus documentation files.
diff --git a/doc/getting-started/src/other-useful-programs-information.tex b/doc/getting-started/src/other-useful-programs-information.tex
new file mode 100644
index 00000000000..0143797b621
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information.tex
@@ -0,0 +1 @@
+\chapter{Other Useful programs/information}\label{other-useful-programsinformation}
diff --git a/doc/getting-started/src/other-useful-programs-information/coefficient-curve-generation.tex b/doc/getting-started/src/other-useful-programs-information/coefficient-curve-generation.tex
new file mode 100644
index 00000000000..0b96acae67b
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/coefficient-curve-generation.tex
@@ -0,0 +1,3 @@
+\section{Coefficient Curve Generation}\label{coefficient-curve-generation}
+
+The CoeffConv and CoeffConv utility programs can be used to convert DOE-2 temperature dependent curves (Fahrenheit) to EnergyPlus temperature curves (Centigrade/Celsius). These programs are described in the Auxiliary Programs document.
diff --git a/doc/getting-started/src/other-useful-programs-information/convertesomtr.tex b/doc/getting-started/src/other-useful-programs-information/convertesomtr.tex
new file mode 100644
index 00000000000..783ddaaa098
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/convertesomtr.tex
@@ -0,0 +1,3 @@
+\section{convertESOMTR}\label{convertesomtr}
+
+This simple post processing program can be used seamlessly with EP-Launch to provide IP (inch-pound) unit output files rather than SI units. This program is described more fully in the Auxiliary Programs document.
diff --git a/doc/getting-started/src/other-useful-programs-information/csvproc.tex b/doc/getting-started/src/other-useful-programs-information/csvproc.tex
new file mode 100644
index 00000000000..41f2a6a7273
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/csvproc.tex
@@ -0,0 +1,3 @@
+\section{CSVProc}\label{csvproc}
+
+This simple post processing program uses .csv files (such as created by ReadVarsESO) and performs some simple statistics on the contents. This program is described more fully in the Auxiliary Programs document.
diff --git a/doc/getting-started/src/other-useful-programs-information/data-sets.tex b/doc/getting-started/src/other-useful-programs-information/data-sets.tex
new file mode 100644
index 00000000000..66be04b17c0
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/data-sets.tex
@@ -0,0 +1,3 @@
+\section{Data Sets}\label{data-sets}
+
+EnergyPlus uses snippets of IDF files to create the library of data that may be useful for you. Two folders are created upon installation: DataSets -- which contains IDF snippets and MacroDataSets -- which also contain IDF snippets but are in a form such that they can be easily used with the EPMacro program.
diff --git a/doc/getting-started/src/other-useful-programs-information/datafiles.tex b/doc/getting-started/src/other-useful-programs-information/datafiles.tex
new file mode 100644
index 00000000000..e380054840f
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/datafiles.tex
@@ -0,0 +1,3 @@
+\section{DataFiles}\label{datafiles}
+
+Some example files are installed during installation (Sample Files option). Each sample input file should contain comments about its purpose at the start of the file. Other example files are made available from the website (http://www.energyplus.gov/).
diff --git a/doc/getting-started/src/other-useful-programs-information/hvac-diagram.tex b/doc/getting-started/src/other-useful-programs-information/hvac-diagram.tex
new file mode 100644
index 00000000000..0dcf1c27d4e
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/hvac-diagram.tex
@@ -0,0 +1,3 @@
+\section{HVAC-Diagram}\label{hvac-diagram}
+
+Another post processing program (EnergyPlus versions 1.2 and later) is the HVAC-Diagram application. It reads one of the EnergyPlus output files (eplusout.bnd and produces a Scalable Vector Graphics (SVG) file. More information on the HVAC Diagram program is found in the \href{file:///E:/Docs4PDFs/AuxiliaryPrograms.pdf}{Auxiliary Programs} document.
diff --git a/doc/getting-started/src/other-useful-programs-information/hvactemplate-objects.tex b/doc/getting-started/src/other-useful-programs-information/hvactemplate-objects.tex
new file mode 100644
index 00000000000..b324797613d
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/hvactemplate-objects.tex
@@ -0,0 +1,3 @@
+\section{HVACTemplate Objects}\label{hvactemplate-objects}
+
+HVAC Template objects are available. These are intended to allow for several ``usual'' HVAC types to be expanded into EnergyPlus HVAC inputs with minimal user entries. These are described in the ``Input/Output Reference'' document under the Group ``HVACTemplates'' and the expansion process is described in the Auxiliary Programs document under ``ExpandObjects''.
diff --git a/doc/getting-started/src/other-useful-programs-information/library-files.tex b/doc/getting-started/src/other-useful-programs-information/library-files.tex
new file mode 100644
index 00000000000..a33cc4a0284
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/library-files.tex
@@ -0,0 +1,5 @@
+\section{Library Files}\label{library-files}
+
+Library files for EnergyPlus are embodied in the DataSets and MacroDataSets folders. DataSets are IDF excerpts -- you must cut and paste from them in order to use them. Items in MacroDataSets can be used in conjunction with the EPMacro preprocessor program. All files are in the necessary form for processing with EnergyPlus.
+
+The files in the DataSets and MacroDataSets folders are described in more detail in the ``\href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details and Examples}'' document.
diff --git a/doc/getting-started/src/other-useful-programs-information/results-processing.tex b/doc/getting-started/src/other-useful-programs-information/results-processing.tex
new file mode 100644
index 00000000000..a21181e73a3
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/results-processing.tex
@@ -0,0 +1,45 @@
+\section{Results Processing}\label{results-processing}
+
+Results from EnergyPlus (using EP-Launch) appear in several possible formats.~ The most basic are the csv files for the time oriented output and the meter output.~ These will appear as \textless{}filename\textgreater{}.csv and \textless{}filename\textgreater{}Meter.csv.~ These can be quite detailed files (ref: Output:Variable, Output:Meter commands).~ Other formats (such as Tabular outputs) can yield more summarized results.~ These files and contents are described in more detail in the ``\href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details and Examples}'' document.
+
+As an example, here is what the normal ``csv'' file might look like in Excelâ„¢:
+
+\begin{figure}[hbtp] % fig 23
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image023.png}
+\caption{Results in Spreadsheet format \protect \label{fig:results-in-spreadsheet-format}}
+\end{figure}
+
+Likewise, a tabular output (usually in HTML format -- which can be read by any web browser) might look like:
+
+\textbf{End Uses}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Electricity (GJ) & Natural Gas (GJ) & Other Fuel (GJ) & Purchaseh Cooling (GJ) & Purchaseh Heating (GJ) & Water (m3) \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Electricity (GJ) & Natural Gas (GJ) & Other Fuel (GJ) & Purchaseh Cooling (GJ) & Purchaseh Heating (GJ) & Water (m3) \tabularnewline
+\midrule
+\endhead
+
+Heating & 0.00 & 95.17 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Cooling & 56.78 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Interior Lighting & 124.39 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Exterior Lighting & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Interior Equipment & 28.27 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Exterior Equipment & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Fans & 73.52 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Pumps & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Heat Rejection & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Humidification & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Heat Recovery & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Water Systems & 0.08 & 85.39 & 0.00 & 0.00 & 0.00 & 363.07 \tabularnewline
+Refrigeration & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+Generators & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 & 0.00 \tabularnewline
+~ & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+Total End Uses & 283.03 & 180.56 & 0.00 & 0.00 & 0.00 & 363.07 \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/getting-started/src/other-useful-programs-information/slab-and-basement-programs.tex b/doc/getting-started/src/other-useful-programs-information/slab-and-basement-programs.tex
new file mode 100644
index 00000000000..5a300ca99b3
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/slab-and-basement-programs.tex
@@ -0,0 +1,3 @@
+\section{Slab and Basement Programs}\label{slab-and-basement-programs}
+
+The Slab and Basement programs can be used to create accurate Ground Temperature profiles for your runs using minimal input about your building. These are used prior to an actual simulation. The programs are described in the Auxiliary Programs document.
diff --git a/doc/getting-started/src/other-useful-programs-information/useful-programs.tex b/doc/getting-started/src/other-useful-programs-information/useful-programs.tex
new file mode 100644
index 00000000000..91b53988eff
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/useful-programs.tex
@@ -0,0 +1,3 @@
+\section{Useful Programs}\label{useful-programs}
+
+Several useful programs, not described fully here can be found in the Auxiliary Programs document.
diff --git a/doc/getting-started/src/other-useful-programs-information/weatherdata.tex b/doc/getting-started/src/other-useful-programs-information/weatherdata.tex
new file mode 100644
index 00000000000..ae12f2206d5
--- /dev/null
+++ b/doc/getting-started/src/other-useful-programs-information/weatherdata.tex
@@ -0,0 +1,5 @@
+\section{WeatherData}\label{weatherdata}
+
+The E/E+ format is very flexible (as well as being ASCII and somewhat readable). In addition to the usual weather data (temperatures, solar radiation data), the format embodies other information from the location and weather data (e.g.~design conditions, calculated ground temperatures, typical and extreme weather periods). The EPW (weather data format)~ is described in \href{file:///E:/Docs4PDFs/AuxiliaryPrograms.pdf}{Auxiliary Programs} Document. Other details including statistical reports, backgrounds on data sources and formats, use of the Weather Converter program (used both for processing data and reporting) are also provided in the Auxiliary Programs document.
+
+The web site for EnergyPlus (http://www.energyplus.gov) provides downloadable weather data for many sites throughout the world from several different formats. In addition, we are amenable to posting more weather data from users.
diff --git a/doc/getting-started/src/overall-scheme-methodology-for-running.tex b/doc/getting-started/src/overall-scheme-methodology-for-running.tex
new file mode 100644
index 00000000000..d4849170395
--- /dev/null
+++ b/doc/getting-started/src/overall-scheme-methodology-for-running.tex
@@ -0,0 +1 @@
+\chapter{Overall scheme/methodology for running EnergyPlus}\label{overall-schememethodology-for-running-energyplus}
diff --git a/doc/getting-started/src/overall-scheme-methodology-for-running/a-methodology-for-using-energyplus.tex b/doc/getting-started/src/overall-scheme-methodology-for-running/a-methodology-for-using-energyplus.tex
new file mode 100644
index 00000000000..35ef4e3c808
--- /dev/null
+++ b/doc/getting-started/src/overall-scheme-methodology-for-running/a-methodology-for-using-energyplus.tex
@@ -0,0 +1,496 @@
+\section{A Methodology for Using Energyplus}\label{a-methodology-for-using-energyplus}
+
+This section provides a step by step outline that will help you streamline creating your building models for using EnergyPlus.
+
+\subsection{\texorpdfstring{\emph{Step 1}: Plan Ahead}{Step 1: Plan Ahead}}\label{step-1-plan-ahead}
+
+Some preliminary steps will facilitate the construction of your input file. EnergyPlus requires some information in specified, externally available formats; other information may require some lead time to obtain. The following checklist should be completed before you start to construct your input file.
+
+\begin{itemize}
+\item
+  Obtain location and design climate information for the city in which your building is located. If possible, use one of the weather files available for your weather period run.
+\item
+  Obtain sufficient \emph{building} \emph{construction} information to allow specification of overall building geometry and surface constructions (including exterior walls, interior walls, partitions, floors, ceilings, roofs, windows and doors).
+\item
+  Obtain sufficient \emph{building} \emph{use} information to allow specification of the lighting and other equipment (e.g.~electric, gas, etc.) and the number of people in each area of the building.
+\item
+  Obtain sufficient \emph{building} \emph{thermostatic} \emph{control} information to allow specification of the temperature control strategy for each area of the building.
+\item
+  Obtain sufficient \emph{HVAC} \emph{operation} information to allow specification and scheduling of the fan systems.
+\item
+  Obtain sufficient \emph{central plant} information to allow specification and scheduling of the boilers, chillers and other plant equipment.
+\end{itemize}
+
+\subsection{*Step 2: ``*Zone" the Building}\label{step-2-zone-the-building}
+
+A building ``surface'' is the fundamental element in the building model. In the general sense, there are two types of ``surfaces'' in EnergyPlus. These are:
+
+1.~~ heat transfer surfaces~ and
+
+2.~~ heat storage surfaces
+
+The first rule of building modeling is, ``\emph{Always define a surface as a heat storage surface unless it must be defined as a heat transfer surface}''. Any surface, which is expected to separate spaces of significantly different temperatures, must be defined as a \emph{heat transfer surface.} Thus, exterior surfaces, such as outside walls, roofs and floors, are \emph{heat transfer surfaces}. Interior surfaces (partitions) are \emph{heat storage surfaces} if they separate spaces maintained at the same temperature and \emph{heat transfer surfaces} if they separate spaces maintained at different temperatures. A discussion of how to define heat transfer and heat storage surfaces will occur in later steps. In order to correctly ``zone'' the building it is necessary only to distinguish between the two.
+
+A ``zone'' is a \emph{thermal,} not a \emph{geometric,} concept. A ``zone'' is an air volume at a uniform temperature plus all the heat transfer and heat storage surfaces bounding or inside of that air volume. EnergyPlus calculates the energy required to maintain each zone at a specified temperature for each hour of the day. Since EnergyPlus performs a zone heat balance, the first step in preparing a building description is to break the building into zones. The objective of this exercise is to define as \emph{few} zones as possible without significantly compromising the integrity of the simulation.
+
+Although defining building zones is somewhat of an art, a few general rules will keep the new simulation user out of trouble. Consider the following figure, which shows the floor plan of an Adult Education Center.
+
+\begin{figure}[hbtp] % fig 12
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image012.png}
+\caption{Adult Education Center \protect \label{fig:adult-education-center}}
+\end{figure}
+
+The question is, ``How many \emph{thermal} zones should be used to model this building?''~ The inexperienced building modeler may be tempted to define each room in the building as a zone, but the thermal zone is defined as a volume of air at a uniform temperature. The general rule then is to \emph{use the number of fan systems (and radiant systems) not the number of rooms to determine the number of zones in the building.} The minimum number of zones in a general simulation model will usually be equal to the number of systems serving the building. The collection of heat transfer and heat storage surfaces defined within each zone will include all surfaces bounding or inside of the space conditioned by the system.
+
+\subsection{Zoning -- Concept 1 - Simple}\label{zoning-concept-1---simple}
+
+Complete estimates of the total building load (magnitude only) may be obtained with very simple models. For example the total building load calculated using a one-zone model of the Education Center (Figure~\ref{fig:single-zone-model-of-the-adult-education}) will \textbf{NOT} be significantly different from the total building load calculated using a more detailed model. The \emph{distribution} of the load within the building cannot be estimated with the simplified building model, but its \emph{magnitude} (such as would be used in sizing the central plant equipment) can be quickly estimated using a very simple model. For simplicity, assume there is no ground heat transfer; if you want to simulate ground heat transfer, you should use the slab and/or basement programs as described in the Auxiliary Programs document.
+
+\begin{figure}[hbtp] % fig 13
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image013.png}
+\caption{Single Zone Model of the Adult Education Center. \protect \label{fig:single-zone-model-of-the-adult-education}}
+\end{figure}
+
+\subsection{Zoning -- Concept 2 - Detailed}\label{zoning-concept-2---detailed}
+
+A more detailed model will allow you to determine more accurately the actual distribution of loads/energy within the building. In a more detailed model of the education center, five systems were designed to serve the Adult Education Center. These systems with the thermal zones they serve are shown in the table below. The location of each zone is shown in accompanying figure.
+
+% table 2
+\begin{longtable}[c]{@{}lllll@{}}
+\caption{Zoning the Building by System Type. \label{table:zoning-the-building-by-system-type.}} \tabularnewline
+\toprule 
+System Number & System Name & CFM & m/s & Zone Served \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Zoning the Building by System Type.} \tabularnewline
+\toprule 
+System Number & System Name & CFM & m/s & Zone Served \tabularnewline
+\midrule
+\endhead
+
+1 & Four Pipe Fan Coil & 3900 & 19.812 & Zone 1 \tabularnewline
+1 & Four Pipe Fan Coil & 2500 & 12.7 & Zone 2 \tabularnewline
+2 & Single Zone Draw Through & 1400 & 7.112 & Zone 3 \tabularnewline
+3 & Single Zone Draw Through & 2250 & 11.43 & Zone 5 \tabularnewline
+4 & Single Zone Draw Through & 2450 & 12.446 & Zone 6 \tabularnewline
+5 & Unit Heater & 185 & .9398 & Zone 4 \tabularnewline
+5 & Unit Heater & 41 & .20828 & Zone 7 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{figure}[hbtp] % fig 14
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image014.png}
+\caption{Thermal Zones in the Education Center \protect \label{fig:thermal-zones-in-the-education-center}}
+\end{figure}
+
+Take note of Zone 1, Zone 2, Zone 4, and Zone 7. The two important zoning concepts can be demonstrated with the zoning to reinforce the idea of a thermal zone and encourage the use of simplified models.
+
+1.~~ Notice that Zones 4 and 7 include two rooms that are not adjacent to one another but are served by the same system. Because the air temperature in the two spaces is maintained at the same uniform temperature, the two spaces, though separated spatially, may be defined as a single zone. For our purposes, we will define them as separate zones.
+
+2.~~ Notice that Zone 1 and Zone 2 are served by the same fan system and could be defined as a single zone with 7650 cfm of conditioned air supplied to the space. The space was split into two zones because the designer expected higher solar loads on the South and West sides of the wing and wanted to examine the \emph{distribution} as well as the \emph{magnitude} of the load in the space.
+
+\subsection{\texorpdfstring{\emph{Step 3:} Prepare to Construct the Building Model}{Step 3: Prepare to Construct the Building Model}}\label{step-3-prepare-to-construct-the-building-model}
+
+Working from blueprints or sketches and following the guidelines in Step 2, the building zones were determined. It is recommended that the engineer sketch the building with its zones. Surface dimensions should be included in the sketch. Additional geometric and surface information is required before an input file describing the building can be constructed. Specifically the building model must:
+
+1.~~ Determine \emph{heat transfer} and \emph{heat storage} surfaces.
+
+2.~~ Define equivalent surfaces.
+
+3.~~ Specify surfaces and subsurfaces (windows, doors, etc.) construction and materials.
+
+4.~~ Compile surface and subsurface information.
+
+By the way, the file for this example, the 1 zone model are contained in your EnergyPlus installation ExampleFiles\textbackslash{}BasicFiles folder.
+
+\subsubsection{Step 3.1.~~~~~ Determine heat transfer and heat storage surfaces.}\label{step-3.1.-determine-heat-transfer-and-heat-storage-surfaces.}
+
+The surfaces of the building can be described in any order; grouping surfaces by zone may help you read the input file. Specifics of the describing surfaces help categorize the surface's heat transfer/storage as well as identify the surface construction information.
+
+The details of inputting surfaces are described in the Input/Output Reference document. The allowable surface types are shown in the following table:
+
+% table 3
+\begin{longtable}[c]{p{1.61in}p{4.38in}}
+\caption{Surface types and categorization \label{table:surface-types-and-categorization}} \tabularnewline
+\toprule 
+Surface Type & Applicability \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Surface types and categorization} \tabularnewline
+\toprule 
+Surface Type & Applicability \tabularnewline
+\midrule
+\endhead
+
+BuildingSurface:Detailed & Wall, Roof, Ceiling, Floor \tabularnewline
+FenestrationSurface:Detailed & Window, Door, Glassdoor \tabularnewline
+InternalMass & Areas internal to a zone \tabularnewline
+Shading:Site:Detailed & Shading devices external to the building face (other buildings, trees, etc.) \tabularnewline
+Shading:Zone:Detailed & Shading devices attached to the building (overhang, fin) \tabularnewline
+\bottomrule
+\end{longtable}
+
+The pieces of the definition that designate BuildingSurface:Detailed surfaces as either \emph{heat transfer} or \emph{heat storage} surfaces are:
+
+\begin{lstlisting}
+
+  A5 , \field Outside Boundary Condition
+         \required-field
+         \type choice
+         \key Surface
+         \key Zone
+         \key Outdoors
+         \key Ground
+         \key OtherSideCoefficients
+         \key OtherSideConditionsModel
+    A6,  \field Outside Boundary Condition Object
+         \type object-list
+         \object-list OutFaceEnvNames
+         \note Non-blank only if the field Outside Boundary Condition is Surface, Zone, OtherSideCoefficients,
+         \note or OtherSideConditionsModel
+         \note If Surface, specify name of corresponding surface in adjacent zone or
+         \note specify current surface name for internal partition separating like zones
+         \note If Zone, specify the name of the corresponding zone and
+         \note the program will generate the corresponding interzone surface
+         \note If OtherSideCoefficients, specify name of SurfaceProperty:OtherSideCoefficients
+         \note If OtherSideConditionsModel, specify name of SurfaceProperty:OtherSideConditionsModel
+    A7 , \field Sun Exposure
+         \required-field
+         \type choice
+         \key SunExposed
+         \key NoSun
+         \default SunExposed
+    A8,  \field Wind Exposure
+         \required-field
+         \type choice
+         \key WindExposed
+         \key NoWind
+         \default WindExposed
+\end{lstlisting}
+
+Note that subsurfaces (windows, doors) on these base surfaces will inherit the base surface properties listed above. The following examples will use a bit more of the Surface definition to give context.
+
+Surfaces that specify ``themselves'' as the outside boundary condition are ceilings, floors and partitions that divide temperature-controlled spaces. The program assumes that the surface temperatures on both sides of the surface are the same. This means that even though heat may be stored in a partition, ceiling, or floor, no heat flows \emph{through} it.
+
+Heat Storage Surfaces (Use current Surface name for ExteriorEnvironment), e.g.:
+
+\begin{lstlisting}
+
+BuildingSurface:Detailed,Zn005:Wall006,  !- Base Surface Name
+    Wall,INTERIOR,  !- Class and Construction Name
+    MAINE WING,  !- Zone
+    Surface, Zn005:Wall006,  !- Exterior Conditions and Target
+     NoSun,  !- Solar Exposure
+     NoWind,  !- Wind Exposure
+    0.5000000    ,  !- VF to Ground
+             4, !-Rectangle
+     57.90000    ,   57.79000    ,   10.00000    ,
+     57.90000    ,   57.79000    ,  0.0000000E+00,
+     57.90000    ,   47.79000    ,  0.0000000E+00,
+     57.90000    ,   47.79000    ,   10.00000    ;
+\end{lstlisting}
+
+Some surfaces divide the temperature controlled space from the outside environment. Surfaces that are both sun and wind exposed (e.g.~exterior walls, exposed floors, roofs) feel the full effect of both solar radiation and outside temperature, and the outside air film resistance for these surfaces changes with wind speed and wind direction. Surfaces that are not sun or wind exposed (a wall to an ``uncontrolled'' space) are not affected by solar radiation, wind speed or direction and have a constant outside convective air film resistance.
+
+Heat Transfer Surfaces Exposed to the Outside Environment, such as Exterior Walls, Roofs, Exposed Floors:
+
+\begin{lstlisting}
+
+BuildingSurface:Detailed,Zn005:Wall002,  !- Base Surface Name
+    Wall,EXTERIOR,  !- Class and Construction Name
+    MAINE WING,  !- Zone
+    Outdoors,,  !- Exterior Conditions and Target (if applicable)
+     SunExposed,  !- Solar Exposure
+     WindExposed,  !- Wind Exposure
+    0.5000000    ,  !- VF to Ground
+             4, !-Rectangle
+     77.90000    ,   47.79000    ,   10.00000    ,
+     77.90000    ,   47.79000    ,  0.0000000E+00,
+     77.90000    ,   67.79000    ,  0.0000000E+00,
+     77.90000    ,   67.79000    ,   10.00000    ;
+\end{lstlisting}
+
+Surfaces such as basement walls and slab floors separate the space from the earth surrounding the surfaces. Therefore, the outside surface temperatures become the ground temperatures.
+
+Heat Transfer Surfaces in Contact with the Ground, such as Basement Walls or Slab Floors:
+
+\begin{lstlisting}
+
+BuildingSurface:Detailed,Zn004:Flr001,  !- Base Surface Name
+    Floor,SLAB FLOOR,  !- Class and Construction Name
+    ARIZONA WING,  !- Zone
+    Ground,,  !- Exterior Conditions and Target (if applicable)
+     NoSun,  !- Solar Exposure
+     NoWind,  !- Wind Exposure
+     1.000000    ,  !- VF to Ground
+             4, !-Rectangle
+     38.01000    ,   8.510000    ,  0.0000000E+00,
+     18.01000    ,   8.510000    ,  0.0000000E+00,
+     18.01000    ,   28.51000    ,  0.0000000E+00,
+     38.01000    ,   28.51000    ,  0.0000000E+00;
+\end{lstlisting}
+
+Other surfaces separate zones that may be at different temperatures. These surface types allow heat transfer (by conduction through the walls) from a zone at a higher temperature to a zone at a lower temperature. The location of the heat storage surface in the zone is not important except in specialized solar studies. The surface above (wall to uncontrolled space) would be more correctly modeled as an interzone surface.
+
+Heat Transfer Surfaces Exposed to Another Zone, such as Interzone walls, ceilings or floors:
+
+\begin{lstlisting}
+
+BuildingSurface:Detailed,Zn005:Wall005,  !- Base Surface Name
+    Wall,INTERIOR,  !- Class and Construction Name
+    MAINE WING,  !- Zone
+    Surface,Zn001:Wall009,  !- Exterior Conditions and Target
+     NoSun,  !- Solar Exposure
+     NoWind,  !- Wind Exposure
+    0.5000000    ,  !- VF to Ground
+             4, !-Rectangle
+     57.90000    ,   47.79000    ,   10.00000    ,
+     57.90000    ,   47.79000    ,  0.0000000E+00,
+     67.90000    ,   47.79000    ,  0.0000000E+00,
+     67.90000    ,   47.79000    ,   10.00000    ;
+   
+\end{lstlisting}
+
+\subsubsection{Step 3.2.~~~~ Define equivalent surfaces as desired.}\label{step-3.2.-define-equivalent-surfaces-as-desired.}
+
+When the building was zoned, our objective was to define as \emph{few} zones as possible. Now we would like to extend this objective to include defining as \emph{few} surfaces as possible without significantly compromising the integrity of the simulation. We reduce the number and complexity of surfaces in our input file by defining \emph{equivalent} surfaces.
+
+Before dealing with equivalent surfaces, it is appropriate to take the concept of a thermal zone one step further. EnergyPlus performs heat balances on individual zone surfaces and on the zone air. For purposes of the heat transfer calculations, a \emph{geometrically} correct rendering of the zone surfaces is not required. The surfaces do not even have to be connected. As long as the program knows to which thermal zone (mass of air) each surface transfers heat, it will calculate all heat balances correctly. For example, all heat storage surfaces of the same construction within a zone may be defined as a single rectangular surface. The size of this \emph{equivalent} surface will equal the sum of all the areas of all the heat storage surfaces in the zone. A few simple rules will further explain what we mean by \emph{equivalent} surfaces and how these surfaces may be used. Remember that these are guidelines for optional simplification of input. Each simplification must be evaluated to determine if it would significantly impact certain shading, interior solar gains, or daylighting features. The goal is to seek an adequate level of detail to capture the key features of the building envelope without spending excess time describing and computing results for details that are insignificant.
+
+1.~~ \emph{Define all roofs and floors as rectangles regardless of the shape of the zone.} Each zone may have one rectangular roof and one rectangular floor of a given construction.
+
+2.~~ \emph{Define all heat storage surfaces of the same construction within a zone as a single surface}. The size of the single surface is obtained by summing the individual surface areas exposed to the zone. Thus, if a partition is completely within a zone (both sides of the partition are exposed to the zone), the area of each side must be added to the area of the equivalent surface. On the other hand, if the partition separates two zones, the area of only one side should be added to the equivalent surface.
+
+3.~~ \emph{Combine all windows on a given exterior surface into a single window}. Usually each exterior surface should have only one window of each type. Overhangs or other shading devices may require that more windows be specified or combined together. By using the WindowMaterial:Glazing construction for your glass door, they will be correctly modeled in EnergyPlus with sunlight transferring into the zone.
+
+The following figure shows the surfaces and subsurfaces required for a one-zone model, i.e., the education center. Since there were two types of partitions in the building, two heat storage surfaces (``internal mass'') of different constructions were defined.
+
+\begin{figure}[hbtp] % fig 15
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image015.png}
+\caption{Simplifications Using Equivalent Surfaces \protect \label{fig:simplifications-using-equivalent-surfaces}}
+\end{figure}
+
+\subsubsection{Step 3.3. Specify construction elements}\label{step-3.3.-specify-construction-elements}
+
+BLAST, DOE-2 and other programs often have ``libraries'' of constructions, schedules, and other aspects of simulating the building. In EnergyPlus, we have a special set of files in the DataSets folder that represent many facets of building simulation. Data sets are usually IDF snippets or macro files. For constructions, using the guidelines in the ASHRAE Handbook of Fundamentals (2005), the file ASHRAE\_2005\_HOF\_Materials.idf contains materials and constructions from Chapters 30 and 25. Since Chapter 30 discusses heating and cooling loads, it includes constructions for light, medium and heavy weight buildings -- these constructions are represented in the dataset file. For the education center, ``medium'' constructions are used. For the windows, we will use the Double Pane Window from the previous exercise.
+
+% table 4
+\begin{longtable}[c]{@{}lll@{}}
+\caption{Building Elements \label{table:building-elements}} \tabularnewline
+\toprule 
+Type (1) & Name (2) & Material (3) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Building Elements} \tabularnewline
+\toprule 
+Type (1) & Name (2) & Material (3) \tabularnewline
+\midrule
+\endhead
+
+Wall & Medium Exterior Wall & M01 100mm brick \tabularnewline
+~ & ~ & I02 50mm insulation board \tabularnewline
+~ & ~ & F04 Wall air space resistance \tabularnewline
+~ & ~ & G01a 19mm gypsum board \tabularnewline
+Window & Double Pane Window & Clear 6MM \tabularnewline
+~ & ~ & Air 3MM \tabularnewline
+~ & ~ & Clear 6MM \tabularnewline
+Partition & Medium/Heavy Partitions & G01a 19mm gypsum board \tabularnewline
+~ & ~ & M01 100mm brick \tabularnewline
+~ & ~ & M05 200mm concrete block \tabularnewline
+~ & ~ & G01a 19mm gypsum board \tabularnewline
+Partition & Medium Partitions & G01a 19mm gypsum board \tabularnewline
+~ & ~ & F04 Wall air space resistance \tabularnewline
+~ & ~ & G01a 19mm gypsum board \tabularnewline
+Wall & Heavy/Medium Partitions & G01a 19mm gypsum board \tabularnewline
+~ & ~ & M05 200mm concrete block \tabularnewline
+~ & ~ & M01 100mm brick \tabularnewline
+~ & ~ & G01a 19mm gypsum board \tabularnewline
+Roof & Medium Roof/Ceiling & M14a 100mm heavyweight concrete \tabularnewline
+~ & ~ & F05 Ceiling air space resistance \tabularnewline
+~ & ~ & F16 Acoustic tile \tabularnewline
+Floor & Medium Floor & F16 Acoustic tile \tabularnewline
+~ & ~ & F05 Ceiling air space resistance \tabularnewline
+~ & ~ & M14a 100mm heavyweight concrete \tabularnewline
+\bottomrule
+\end{longtable}
+
+Notes:
+
+(1)~ The surface type is a wall, floor, roof, window or door.
+
+\begin{enumerate}
+\def\labelenumi{(\arabic{enumi})}
+\setcounter{enumi}{1}
+\item
+  User supplies name for the element. For this example use name from the DataSet: \textbf{ASHRAE\_2005\_HOF\_Materials.idf}. Similarly, the window was constructed from the \textbf{Windows.idf} dataset.
+\item
+  Material's full name is as found in the ASHRAE\_2005\_HOF\_Materials.idf dataset.
+\end{enumerate}
+
+\subsubsection{Step 3.4.~~~~ Compile surface and subsurface information.}\label{step-3.4.-compile-surface-and-subsurface-information.}
+
+\emph{Building information:}
+
+\emph{Building North Axis:} This syntax simplifies building geometry specification by designating one wall of the building as the building's north pointing axis. The building model North axis is measured from true (compass) North. Surface facing angles (see surface information below) are then specified relative to the building north axis. The \emph{North Axis} entry in the Input Output Reference (duplicated here) illustrates specification of the building north axis.
+
+\begin{figure}[hbtp] % fig 16
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image016.png}
+\caption{Illustration of Building North Axis \protect \label{fig:illustration-of-building-north-axis}}
+\end{figure}
+
+\emph{Zone information:}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\tightlist
+\item
+  \emph{Wall height}: In a simple model, one should make all the walls the same height. Then, the simple, 1 zone model can entirely enclose the space. In more complex models, you may resize each wall accordingly.
+\end{enumerate}
+
+\emph{Surface information:}
+
+1.~~ \emph{Base} \emph{Surface Type:} Heat Transfer/Heat Storage Surfaces may be of the following types: wall, floor, roof, internal mass, or subsurface
+
+2.~~ \emph{Construction:} The type of construction of the surface (see previous table).
+
+\emph{Subsurface information:}
+
+1.~~~~\emph{Subsurfaces} are Windows, Doors or GlassDoors
+
+2.~~ \emph{Area:} Area of the subsurface.
+
+3.~~ \emph{Reveal:} For windows only, the distance it is inset from the outside surface of a wall. For simplicity, put all the windows in the same physical plane as the wall they are on.
+
+For the single zone model, the following figure is a schematic representation of a one zone representation. The figure shows the length of all ``base'' surfaces and the areas of all ``subsurfaces'' (windows). Doors are shown and may be entered, if desired. In the table (Table~\ref{table:compilation-of-surface-information-for}), the surfaces are numbered counter-clockwise around the zone beginning at the lower left corner of the figure. ~This table is the minimum required zone information compiled by the user. A few simple conventions should be followed to facilitate the construction of zone information tables:
+
+1.~~ Number all surfaces in order counter-clockwise around the zone.
+
+2.~~ Keep the subsurfaces with the base surface on which they are located.
+
+3.~~ Specify \emph{lengths} for base surfaces and areas for subsurfaces and internal mass.
+
+4.~~~~Specify the roof and floor as rectangles of the correct size.
+
+\begin{figure}[hbtp] % fig 17
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image017.jpg}
+\caption{Schematic of One Zone Model with Exterior Wall length and Window Areas. \protect \label{fig:schematic-of-one-zone-model-with-exterior}}
+\end{figure}
+
+\textbf{Full Building -- 1 Zone model}
+
+% table 5
+\begin{longtable}[c]{p{1.2in}p{1.2in}p{1.2in}p{1.2in}p{1.2in}}
+\caption{Compilation of Surface Information for the One Zone Model \label{table:compilation-of-surface-information-for}} \tabularnewline
+\toprule 
+Surface & type & construction & Length \{m\} & Area \{m  \} \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Compilation of Surface Information for the One Zone Model} \tabularnewline
+\toprule 
+Surface & type & construction & Length \{m\} & Area \{m  \} \tabularnewline
+\midrule
+\endhead
+
+1 & exterior wall & Medium Exterior Wall & 15.25 & ~ \tabularnewline
+2 & window & Double Pane Window & ~ & 5.62 \tabularnewline
+3 & exterior wall & Medium Exterior Wall & 4.9 & ~ \tabularnewline
+4 & window & Double Pane Window & ~ & 3.9 \tabularnewline
+5 & exterior wall & Medium Exterior Wall & 34.44 & ~ \tabularnewline
+6 & window & Double Pane Window & ~ & 33.7 \tabularnewline
+7 & exterior wall & Medium Exterior Wall & 13.2 & ~ \tabularnewline
+8 & window & Double Pane Window & ~ & 9.44 \tabularnewline
+9 & exterior wall & Medium Exterior Wall & 10.4 & ~ \tabularnewline
+10 & window & Double Pane Window & ~ & 7.58 \tabularnewline
+11 & exterior wall & Medium Exterior Wall & 20 & ~ \tabularnewline
+12 & window & Double Pane Window & ~ & 10.5 \tabularnewline
+13 & exterior wall & Medium Exterior Wall & 12 & ~ \tabularnewline
+14 & window & Double Pane Window & ~ & 7.58 \tabularnewline
+15 & exterior wall & Medium Exterior Wall & 20 & ~ \tabularnewline
+16 & window & Double Pane Window & ~ & 17.66 \tabularnewline
+17 & exterior wall & Medium Exterior Wall & 6.1 & ~ \tabularnewline
+18 & window & Double Pane Window & ~ & 4.7 \tabularnewline
+19 & exterior wall & Medium Exterior Wall & 3.1 & ~ \tabularnewline
+20 & exterior wall & Medium Exterior Wall & 6.1 & ~ \tabularnewline
+21 & window & Double Pane Window & ~ & 3.71 \tabularnewline
+22 & exterior wall & Medium Exterior Wall & 23 & ~ \tabularnewline
+23 & window & Double Pane Window & ~ & 19.39 \tabularnewline
+24 & exterior wall & Medium Exterior Wall & 15.24 & ~ \tabularnewline
+25 & window & Double Pane Window & ~ & 7.8 \tabularnewline
+26 & exterior wall & Medium Exterior Wall & 38 & ~ \tabularnewline
+27 & window & Double Pane Window & ~ & 31 \tabularnewline
+28 & roof & Medium Roof/Ceiling & Equivalent area (square) & 1250.1 \tabularnewline
+29 & floor & Medium Floor & Equivalent area (square) & 1250.1 \tabularnewline
+30 & internal mass & Medium Partitions & ~ & 956.9 \tabularnewline
+31 & internal mass & Medium/Heavy Partitions & ~ & 1757.7 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The column headings in the previous table have the following meanings:
+
+\textbf{Type:}~ A shortened notation for the surface type in EnergyPlus to differentiate between heat storage surfaces and various types of heat transfer surfaces.
+
+\textbf{Construction:}~ A name for the surface construction types.
+
+\textbf{Length:}~ The length of base surfaces (i.e.~Exterior Walls).
+
+\textbf{Area:}~ The area of subsurfaces (windows), roofs, floors.
+
+\subsection{Step 4: Compile Internal Space Gain Data}\label{step-4-compile-internal-space-gain-data}
+
+People, lights, equipment, outside air infiltration and ventilation all constitute ``internal gains'' for the thermal zone. These gains are described to EnergyPlus as a \emph{design or} \emph{peak} level with a \emph{schedule} that specifies a fraction of the peak for each hour. The peak level is calculated by the user. Table~\ref{table:internal-gain-data}. Internal Gain Data shows the internal loads for a single zone model of Ft. Monmouth and the schedule named to specify the hourly load.
+
+% table 6
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Internal Gain Data \label{table:internal-gain-data}} \tabularnewline
+\toprule 
+Zone & Gain Type & Size & Schedule \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Internal Gain Data} \tabularnewline
+\toprule 
+Zone & Gain Type & Size & Schedule \tabularnewline
+\midrule
+\endhead
+
+1 & People & 205 & Office occupancy \tabularnewline
+~ & Lights & 26360 W & Office lighting \tabularnewline
+~ & ZoneInfiltration & .75 m  /sec & Constant \tabularnewline
+\bottomrule
+\end{longtable}
+
+The column headings in the table have the following meanings:
+
+\textbf{Gain Type:}~ The code used to differentiate between various types of internal gains.
+
+\textbf{Size:}~ The peak load. This is the actual size of the load for every hour that the schedule specifies ``100\%''.
+
+\textbf{Schedule:}~ The hourly schedule that specifies the percentage of peak load for each hour of the day.
+
+\textbf{HVAC:} Using the Compact HVAC models, purchased air can be used to calculate the energy needs of the building.
+
+As the following figure shows, the equivalent area floor/roof does not fit in the building perimeter. As an exercise, you might reconfigure both floor and roof to be a polygonal shape and compare results.
+
+\begin{figure}[hbtp] % fig 18
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image018.png}
+\caption{Full Building - Adult Education Center \protect \label{fig:full-building-adult-education-center}}
+\end{figure}
+
+As an adjunct to the previous schematic layout for the one zone approach, the following figure shows the same building but with IP units:
+
+\begin{figure}[hbtp] % fig 19
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image019.jpg}
+\caption{Schematic for One Zone Building - IP Units \protect \label{fig:schematic-for-one-zone-building-ip-units}}
+\end{figure}
diff --git a/doc/getting-started/src/overall-scheme-methodology-for-running/building-simulation.tex b/doc/getting-started/src/overall-scheme-methodology-for-running/building-simulation.tex
new file mode 100644
index 00000000000..c5fd9f1bbd0
--- /dev/null
+++ b/doc/getting-started/src/overall-scheme-methodology-for-running/building-simulation.tex
@@ -0,0 +1,3 @@
+\section{Building Simulation}\label{building-simulation}
+
+If you are already familiar with modeling buildings, particularly modeling buildings for energy consumption, you may wish to skip to ``IDF Editor -- Brief Introduction''. The following steps are general guidelines for using any building simulation program.
diff --git a/doc/getting-started/src/running-energyplus.tex b/doc/getting-started/src/running-energyplus.tex
new file mode 100644
index 00000000000..abc567a4c9b
--- /dev/null
+++ b/doc/getting-started/src/running-energyplus.tex
@@ -0,0 +1 @@
+\chapter{Running EnergyPlus}\label{running-energyplus}
diff --git a/doc/getting-started/src/running-energyplus/energyplus-file-extensions.tex b/doc/getting-started/src/running-energyplus/energyplus-file-extensions.tex
new file mode 100644
index 00000000000..bd490161fb3
--- /dev/null
+++ b/doc/getting-started/src/running-energyplus/energyplus-file-extensions.tex
@@ -0,0 +1,127 @@
+\section{EnergyPlus File Extensions}\label{energyplus-file-extensions}
+
+This section will present a list of common EnergyPlus file extensions and what they mean. This will help you after the EP-Launch program finishes.
+
+\subsection{Input Files}\label{input-files}
+
+The following files are input to the EnergyPlus program.
+
+\subsubsection{IDD}\label{idd}
+
+The \emph{input data dictionary} (IDD) is an ASCII (text) file containing a list of all possible EnergyPlus objects and a specification of the data each object requires. This file is analogous to the DOE-2 keyword file. The \emph{Guide for Interface Developers} contains a full description of the input data dictionary.
+
+\subsubsection{idf}\label{idf}
+
+The \emph{input data file} (IDF) is an ASCII file containing the data describing the building and HVAC system to be simulated. Many example files are installed as part of the EnergyPlus installation. Additionally, a spreadsheet file ``ExampleFiles.xls'' ~contains columnar descriptions of each file's features.
+
+\subsubsection{imf}\label{imf}
+
+The \emph{input macro file} (IMF) is an ascii file containing the data describing the building and HVAC system to be simulated and will have some contents of ``macro'' commands. The Auxiliary programs document describes use of the macro commands and the program that processes them -- EP-Macro. ~~Many example files are installed as part of the EnergyPlus installation.
+
+\subsubsection{ini}\label{ini}
+
+This is the EnergyPlus initialization file. It is an optional ascii input file that allows the user to specify the path for the directory containing Energy+.idd. This file, using the actual directories of the install, will be created during the install. Unless you change where the EnergyPlus.exe file resides, you will not need to change this file.
+
+\subsubsection{epw}\label{epw}
+
+The \emph{EnergyPlus weather} file is an ascii file containing the hourly or sub-hourly weather data needed by the simulation program. The data format is described in detail in the Auxiliary Programs Document. It is also described succinctly in the Input Output Reference document.
+
+\subsection{Primary Output Files}\label{primary-output-files}
+
+The following output files are the most important for beginning users.~ Then, there is the section on ``other output'' files.~ And, more information about output files (complete list) is shown in the \href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details and Examples} Document.
+
+\subsubsection{err}\label{err}
+
+A text file containing the error messages issued by EnergyPlus. \textbf{This is the first output that should be examined after a simulation.}Error messages may be issued by EnergyPlus during its input phase or during the simulation. There are three levels of error severity: \emph{fatal}, \emph{severe}, and \emph{warning} as well as simple \emph{``information''} lines. A fatal error causes the program to terminate immediately. The following table illustrates the necessary actions.
+
+% table 1
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Error Message Levels – Required Actions \label{table:error-message-levels-required-actions}} \tabularnewline
+\toprule 
+Error Level & Action \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Error Message Levels – Required Actions} \tabularnewline
+\toprule 
+Error Level & Action \tabularnewline
+\midrule
+\endhead
+
+Information, shown as ********* & Informative, usually a follow-on to one of the others. No action required. \tabularnewline
+**~~ \~{}\textbackslash\~{}\~{}~~** & This is a continuation of a previous message.~ String all the words/sentences together to form the complete message. \tabularnewline
+Warning & Take note. Fix as applicable. \tabularnewline
+Severe & Should Fix \tabularnewline
+Fatal & Program will abort, Must Fix \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{csv}\label{csv}
+
+When run normally, EP-Launch and EnergyPlus automatically creates post-processed standard output (eso) and meter output (mtr) files into columnar csv (comma separated variable) files.~ These files are ready to be read by spreadsheet programs (such as Excelâ„¢).
+
+\subsubsection{htm/html}\label{htmhtml}
+
+Several of the report options produce html files that can be read in standard Web browsers.~ These are very powerful, information packed files.~ Though wary of information overload, the easiest way to see ``everything'' is to enter the following in your input file:
+
+\begin{lstlisting}
+
+OutputControl:Table,
+     HTML;                    !- ColumnSeparator
+
+  Output:Table:SummaryReports,
+     All Summary;
+\end{lstlisting}
+
+Note that you can also get this file in other formats (the OutputControl:Table option).
+
+\subsection{Other Output Files}\label{other-output-files}
+
+\subsubsection{audit}\label{audit}
+
+This is an text file which echoes the IDD and IDF files, flagging syntax errors in either file. Note that both \emph{err} and \emph{audit} will show most of the error messages caused by input syntax errors; however only \emph{err} will show errors issued during the actual simulation. The \emph{audit} can be used when you need to see the context of the error message to fully ascertain the cause. The \emph{audit} file also contains potentially extra information that may be useful from the input scan.
+
+\subsubsection{eso}\label{eso}
+
+The \emph{EnergyPlus Standard Output} (ESO) is a text file containing the time varying simulation output. The format of the file is discussed in the \emph{Guide for Interface Developers} and the \emph{InputOutputReference}. The contents of the file are controlled by \emph{Output:Variable} commands in the IDF file. Although the ESO is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
+
+\subsubsection{mtr}\label{mtr}
+
+The \emph{EnergyPlus Meter Output} (MTR) is a text file containing the time varying simulation output. The format of the file is similar to the ESO file. As described in a later section of this document (see Energy Meters), meters are a powerful reporting tool in EnergyPlus. Values are grouped onto logical meters and can be viewed the same way that the ESO variables are used. The contents of the file are controlled by \emph{Output:Meter} commands in the IDF file. Although the MTR is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
+
+\subsubsection{mtd}\label{mtd}
+
+This file contains all the details (i.e., which report variables are on a meter and, conversely, what meters contain) about meters.
+
+\subsubsection{eio}\label{eio}
+
+The \emph{EnergyPlus Invariant Output} (EIO) is a text file containing output that does not vary with time. For instance, location information (latitude, longitude, time zone, altitude) appears on this file.
+
+\subsubsection{rdd}\label{rdd}
+
+\subsubsection{mdd}\label{mdd}
+
+The \emph{Report (variable) Data Dictionary} (RDD) is a text file listing those variables available for reporting (on the ESO) for this particular simulation. Which variables are available for output depends on the actual simulation problem described in the IDF. The \emph{Report (meter) Data Dictionary} (MDD) is a text file listing those variables available for reporting (on the MTR) for this particular simulation. Which meters are available for output depends on the actual simulation problem described in the IDF. A simulation with no chiller does not permit the output of any chiller report variables. The user may need to examine the RDD or MDD to find out which report variables are available in a particular simulation. The RDD and MDD are written only if the following is included in the IDF file.
+
+\begin{lstlisting}
+
+Output:Reports, VariableDictionary;
+\end{lstlisting}
+
+A variant produces the same files in a IDF ``ready'' format.
+
+\begin{lstlisting}
+
+Output:Reports, VariableDictionary, IDF;
+\end{lstlisting}
+
+\subsubsection{dxf}\label{dxf}
+
+This is a file in AutoCadâ„¢ DXF format showing all the surfaces defined in the IDF file. It provides a means of viewing the building geometry. The DXF file from EnergyPlus highlights different building elements (shading, walls, subsurfaces) in differing colors. A number of programs can read and display DXF files. Output of this file is triggered by
+
+\begin{lstlisting}
+
+Output:Reports, Surfaces, DXF;
+\end{lstlisting}
+
+in the IDF.
diff --git a/doc/getting-started/src/running-energyplus/ep-launch-program.tex b/doc/getting-started/src/running-energyplus/ep-launch-program.tex
new file mode 100644
index 00000000000..2764dab22ed
--- /dev/null
+++ b/doc/getting-started/src/running-energyplus/ep-launch-program.tex
@@ -0,0 +1,291 @@
+\section{EP-Launch Program}\label{ep-launch-program}
+
+EP-Launch is an optional component of the EnergyPlus Windows installation (it is not available for Linux and Mac platforms). For users that want a simple way of selecting files and running EnergyPlus, EP-Launch provides this and more. In addition, EP-Launch can help open a text editor for the input and output files, open a spreadsheet for the postprocessor results files, a web browser for the tabular results file, and start up a viewer for the selected drawing file.
+
+\begin{figure}[hbtp] % fig 4
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image004.png}
+\caption{EP-Launch Screen \protect \label{fig:ep-launch-screen}}
+\end{figure}
+
+\subsection{Start EP-Launch}\label{start-ep-launch}
+
+EP-Launch is located in the main directory/folder for EnergyPlus. In addition, it is available on the shortcut menu for EnergyPlus.~ By double clicking on the EP-Launch icon you get the screen shown above (Figure~\ref{fig:ep-launch-screen}) for running a single input file. The EP-Launch program simply starts other programs and allows you to avoid having to use the DOS command line prompt to run EnergyPlus. More help is provided for the program under the ``Help'' menu.
+
+\subsection{Selecting Input and Weather Files}\label{selecting-input-and-weather-files}
+
+The input file and weather files can be selected on the Single Input File tab from the two pull down lists which show recently used files or you can press the ``Browse\ldots{}'' buttons to locate an input or weather file that you have created yourself. If this is your first time using EP-Launch, the pull down lists will show some files from the ExampleFiles subdirectory. These are not the only examples, use browse to open other example files from the ExampleFiles subdirectory or other EnergyPlus input files.
+
+\subsection{Running a Single Input File}\label{running-a-single-input-file}
+
+On the Single Input File tab, after you select the weather and input files simply push the ``Simulate\ldots{}'' button to start the EnergyPlus building energy simulation engine. At this point a black DOS window should pop up on your screen and show the progress of your simulation. The simulation is complete when the black DOS box closes. The EnergyPlus program black DOS window will show scrolling text as the simulation procedure progresses. If you would like to see these messages more slowly you have two options:
+
+1)~~~Press the ``Control-S'' key combination to try to stop the progress and any key to continue.
+
+2)~~~Under the ``View'' menu on the EP-Launch program, select ``Options'' then ``Command Window'' then check ``Pause During Simulation'' and this will pause the process immediately after EnergyPlus executes. To continue after the pause, press any key.
+
+If the file contains Parametric objects, the single input file may cause multiple simulations to be performed. If multiple simulations are performed, the output files will be listed on the History tab and will be named with either the file suffixes defined in the input file or with a serial number.
+
+Multiple single input file and group simulations can be started at the same time. On a computer with multiple-processors or multiple-cores, this will enable the simulations to complete more quickly than starting one after another.
+
+\subsection{Looking at the Results}\label{looking-at-the-results}
+
+After you have run a simulation and the black DOS window closes, EnergyPlus has completed, and a status message is displayed see Figure~\ref{fig:ep-launch-finish-status}:
+
+\begin{figure}[hbtp] % fig 5
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image005.jpg}
+\caption{EP-Launch Finish Status \protect \label{fig:ep-launch-finish-status}}
+\end{figure}
+
+This status gives you a quick overview of whether there were warning (\textbf{should look at}), severe (\textbf{should probably fix}) or fatal (\textbf{must fix}) errors in the run as well as the time it took for the simulation to complete.~ After pressing ``OK'' from this box, selecting ``ERR/EIO/BND Output Files Only'' from the ``View'' menu will display the ERR, EIO, and BND files -- useful when errors may have occurred. Alternatively, pressing the F2 function key will display the same three files.
+
+Another way to open files easily is by using the View Results buttons shown in Figure~\ref{fig:ep-launch-with-the-sets-tab-of-view-results}. Two different panels of buttons can be used under View Results, one shown by using the ``All'' tab on the left edge and by using the ``Sets'' tab on the left edge. The ``All'' tab shows all the various files by file extension that can be viewed individually.~ Files available for view~ based on the current input file name are ``enabled'' (extension names clearly readable). The contents of each file extension is listed below.
+
+\begin{figure}[hbtp] % fig 6
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image006.png}
+\caption{EP-Launch with the Sets tab of View Results \protect \label{fig:ep-launch-with-the-sets-tab-of-view-results}}
+\end{figure}
+
+The figure above shows the same main screen of EP-Launch but with the ``Sets'' tab selected on the left edge of the View Results section. The buttons on this tab can open many files at the same time and are a shortcut to opening the files that may be commonly used. The Text Output Files, Drawing Files, and Spreadsheets buttons cause several different results files to open at once based on the currently selected Input File. The HTML file opens just the tabular results file if that file was produced (see \emph{OutputContol:Table:Style}).
+
+The contents (along with examples) are discussed in the \href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details} document.
+
+You can also view the results using one of the three buttons (``Text Output Files,'' ``Drawing File'' and ``Spreadsheets'') in the ``View Results'' area of the main EP-Launch screen.
+
+By pressing the ``Text Output Files'' button, a text editor will open each of the text output files. Up to 29 files will open, if they exist. Selecting ``Single File'' from the `View `` menu displays a menu of all available output files from which any file can be opened individually. Each file may also be opened with an associated function key. The output files and function key shortcuts are listed below:
+
+1.~Variable -- tabulated results in comma, tab or space delimited format (generated by the ReadVarsESO postprocessor) (F4)
+
+2.~ESO -- raw report variable output (F5),
+
+3.~RDD -- list of output variables available from the run (F6).
+
+4.~MDD -- list of output meters available from the run (Shift-Ctrl-F3)
+
+5.~EIO -- additional EnergyPlus results (F7),
+
+6.~ERR -- list of errors and warnings (F8),
+
+7.~BND -- HVAC system node and component connection details (F9),
+
+8.~MTR -- raw report meter output (F11),
+
+9.~MTD -- list of meter component variables (F12)
+
+10.~METER File -- tabulated meter report in comma, tab or space delimited format (generated by the ReadVarsESO postprocessor) (Ctrl-F4)
+
+11.~ZSZ -- zone sizing details in comma, tab or space delimited format (Ctrl+F5)
+
+12.~SSZ -- system sizing details in comma, tab or space delimited format (Ctrl+F6)
+
+13.~AUDIT -- input file echo with input processor errors and warnings (Ctrl+F8)
+
+14.~SLN -- output from ``report, surfaces, lines'' (Ctrl+F9)
+
+15.~DBG -- output from the debug command (Ctrl+F11)
+
+16.~SHD -- output related to shading (Ctrl+F12)
+
+17.~SVG - HVAC Diagram (Shift+ F4)
+
+18.~EPMIDF -- clean idf file after EP-Macro processing (Shift+F5)
+
+19.~EPMDET -- EP-Macro detailed output with errors and warnings (Shift+F6)
+
+20.~MAP -- daylighting illuminance map (Shift+F7)
+
+21.~TABLE -- tabulated report of bin and monthly data in comma, tab or space delimited or HTML format~ (Shift+F8)
+
+22.~VMRL -- drawing file in VRML (Virtual Reality Markup Language) format (Shift F+F11)
+
+23.~DXF -- drawing file in AutoCAD DXF format (Shift+F12)
+
+24.~Delight IN - DElight input generated from EnergyPlus processed input (Shift+Ctrl+F4)
+
+25.~Delight OUT -- Detailed DElight output (Shift+Ctrl+F5)
+
+26.~Delight ELDMP -- DElight reference point illuminance per time step (Shift+Ctrl+F6)
+
+27.~Delight DFDMP -- DElight warning and error messages (Shift+Ctrl+F7)
+
+28.~EXPIDF -- Expanded IDF when using HVACTemplate objects (Shift+Ctrl+F8)
+
+29.~Group Error -- combined error files for a group run. (Shift+Ctrl+F9)
+
+30.~VCpErr -- Transition program error file (Shift+Ctrl+F11)
+
+31.~Screen (Shift+Ctrl+f12)
+
+32.~Proc CSV -- Simple statistiscs generated from CSVProc (also see Create Statistics File option under View-Options).
+
+33.~EDD -- Energy Management System details.
+
+Clicking on the ``Drawing File'' button will open the generated DXF file if an appropriate viewer has been configured (see \emph{Selecting Viewers and Editors} below). The DXF file is a CAD format that displays the physical shape of the building being modeled in three dimensions. The ``Drawing File'' button also opens the HVAC diagram generated with the HVAC-Diagram utility (see Auxiliary Programs).
+
+Clicking on the ``Spreadsheets'' buttons will open any generated CSV files if an appropriate viewer has been configured (see \emph{Selecting Viewers and Editors} below).
+
+\subsection{Viewing the Drawing File without Running a Simulation}\label{viewing-the-drawing-file-without-running-a-simulation}
+
+The ``Drawing'' button (or the View menu Drawing File option) will automatically run EPDrawGUI if the DXF file does not exist or it is older than the input file. This allows the building geometry to be viewed without running a full simulation. For more information about EPDrawGUI, see the \href{file:///E:/Docs4PDFs/AuxiliaryPrograms.pdf}{\emph{Auxiliary Programs}} document.
+
+\subsection{Editing the Input Files}\label{editing-the-input-files}
+
+The input file, called IDF file that is selected from the top pull-down list, can be edited by pressing one of two buttons in the ``Input File'' area. The ``Edit - Text Editor'' button will start a text editor and the ``Edit - IDF Editor'' will start the separate program called the IDF Editor. Remember to save any changes you make in either editor before returning to EP-Launch to run the simulations again.
+
+\subsection{File Menu}\label{file-menu}
+
+The File menu can be used for selecting input and weather files just like the ``Browse\ldots{}'' buttons (see the \emph{Selecting Input and Weather Files} section above).
+
+If you are upgrading from the previous version of EnergyPlus you can use the ``File'', ``Transition'' menu option to upgrade your EnergyPlus input files (IDF and IMF) to the most recent version (see the \href{file:///E:/Docs4PDFs/AuxiliaryPrograms.pdf}{AuxiliaryPrograms} document for more information about the Transition program). This EP-Launch option only works for upgrading input files one version.
+
+\subsection{Edit Menu}\label{edit-menu}
+
+No cutting or pasting is used in this program so the edit menu shows options that duplicate the functions of the ``Edit -- Text Editor'' and ``Edit -- IDF Editor'' buttons. In addition, the weather file and the postprocessor command file (rvi) may be opened in the text editor.
+
+\subsection{View Menu}\label{view-menu}
+
+The View menu (Figure~\ref{fig:ep-launch-view-menu}) duplicates the options in the ``View Results'' area of the main screen (see the \emph{Looking at the Results} section above) and allows opening of selected output files. You can also open the folders that contain the active input and weather files. Opening a single file is under a submenu and is very similar to the Quick Open Panel for Single Simulation described above. Selecting ``HTML File'' from the ``View'' menu will open any user created files saved in the format: \textless{}filename\textgreater{}table.html (see \emph{OutputControl:Table:Style}).
+
+\begin{figure}[hbtp] % fig 7
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image007.png}
+\caption{EP-Launch View Menu \protect \label{fig:ep-launch-view-menu}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 8
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image008.png}
+\caption{EP-Launch Options Screen. \protect \label{fig:ep-launch-options-screen.}}
+\end{figure}
+
+The ``View'' menu also accesses the ``Options'' menu item shown in Figure~\ref{fig:ep-launch-options-screen.} that is used to control many of the optional features of EP-Launch. These optional features are described below:
+
+\subsubsection{Command Window Options}\label{command-window-options}
+
+\textbf{Pause During Simulation (Unless Minimized)} -- Stops the progress of the EnergyPlus run at different points. This does not stop the simulation itself but pauses before or after important events as files are copied or utility programs are run. It is usually used only for diagnosing problems with the EPL-RUN batch file. The feature is also described in the \emph{Running a Single Input File} section above.
+
+\textbf{Minimize Single Simulation Command Window} -- For a single input file, minimizes the Command Window that EP-Launch uses to run EnergyPlus. The command window will appear only in the Windows taskbar and the command window will not be visible. You can restore the command window be clicking on the taskbar item labeled ``EnergyPlus Process''. This option should be used with caution since you will not see any indication of the simulation being complete other than the ``EnergyPlus Process'' taskbar item will disappear.
+
+\textbf{Minimum Group Simulation Command Window} -- For a group of input files, minimizes the Command Window that EP-Launch uses to run EnergyPlus. This is a good option when working on something else on your computer at the same time as the group of simulations is running since the command window normally becomes the front window each time a new simulation starts. This option prevents the command window coming to the front for each simulation. The command window will appear only in the Windows taskbar and the command window will not be visible. You can restore the command window be clicking on the taskbar item labeled ``EnergyPlus Process''. This option should be used with caution since you will not see any indication of the simulation being complete other than the ``EnergyPlus Process'' taskbar item will not be present.
+
+\textbf{Number of Simultaneous Processes} -- Select the maximum number of simulations that should be able to be run at the same time. For a computer with multiple processors or multiple cores, this will allow better utilization of the computers power. The value selected should correspond to the number of processors/cores but higher or lower number can be used as well.
+
+\textbf{Disable Multi-Threading} -- Check this box if you wish to disable the built in multi-threading capabilities of EnergyPlus. Portions of EnergyPlus have been programmed to use more than one processor, or CPU core, at the same time during a single simulation. This multithreading may not be desirable when running more than one simulation at a time on the same computer (because it can actually run more slowly). When this check box is checked multi-threading is turned off. The check box sets the \textbf{EP\_OMP\_NUM\_THREADS} environmental variable to 1. The multi-threading capability of EnergyPlus can also be controlled using the \textbf{ProgramControl} object field called Number of Threads Allowed. That field takes precedence over the setting of the checkbox. Also note that when multiple simulations are started from EP-Launch, this automatically disables multithreading by setting the EP\_OMP\_NUM\_THREADS environmental variable to 1 whether this box is checked or not. The ProgramControl object is described in the Input Output Reference document.
+
+\subsubsection{Interface Options}\label{interface-options}
+
+\textbf{Extra Wide Window} -- Select this option to make the main EP-Launch window wider. This is useful when files are used with very long file path names.
+
+\textbf{Alternative layout} -- Changes the layout of the EP-Launch window to an alternative arrangement of buttons.
+
+\subsubsection{Miscellaneous Options}\label{miscellaneous-options}
+
+\textbf{Tab Delimited Open with Spreadsheet} -- Selecting ''Single File'' and then ``Main Results File'' from the ``View'' menu or pressing the F4 function key will open TAB files with the default spreadsheet application rather than the text editor. Comma-separated variable (CSV) is the default setting for viewing tabulated results set in the RVI file. If the user changes the setting for viewing tabulated results to TAB or TXT format, selecting ''Single File'' and then ``Main Results File'' from the ``View'' menu or pressing the F4 function key will open the files in the default text editor.~ TAB files, when selected, will also be opened by the text editor when the ``Text Output Files'' button is pressed after a successful run.
+
+\textbf{Allow More Than 250 Columns} -- Tabulated data that exceeds 250 columns, the MS Excel maximum, will be truncated to that limit unless ``Allow \textgreater{}250 Columns'' is selected. Excel versions prior to 2007 were limited to 255 columns in a sheet; later versions allow unlimited number of columns. This limitation may not be true for other spreadsheet programs.
+
+\textbf{Check VERSION Prior to Simulation} -- Automatically check the VERSION object in the selected EnergyPlus input file prior to simulation and if it is an older version than the current version will run the Transition program to update the file.
+
+\textbf{Convert ESO/MTR to IP Units} -- Runs the convertESOMTR utility program (see AuxiliaryPrograms documentation for more information). This utility will convert the ESO and MTR files into Inch-Pound units. The CSV file created from these files will also be in Inch-Pound units.
+
+\textbf{Create Statistics File} -- Runs the CSVProc utility program (see the AuxiliaryPrograms documentation for more information) and creates the --Proc.csv file. This file contains some simple statistics on each variable in the normal CSV file.
+
+\textbf{Create Batch File to Run EnergyPlus} -- Traditionally EP-Launch has created a batch file in order to execute EnergyPlus with the various options chosen. This can cause problems with some operating systems, such as Windows Vista, when set to a higher security setting.~ This option can be unchecked and a batch file is not created when running EnergyPlus instead parameters are passed to an existing batch file.
+
+\textbf{Run ParametricPreprocessor} -- When this option is checked, if Parametric objects are present in the file, the ParametricPreprocessor will be run prior to the first simulation and if multiple simulations are needed they will all be executed. See the Auxiliary Programs documentation for details.
+
+\textbf{Check for Updates to EnergyPlus} -- When this option is checked, EP-Launch will check every seven days if an update to EnergyPlus or any of the files distributed with EnergyPlus are available to download. If they are available a message will be shown upon start up.~ You can also manually check by going to HELP .. CHECK FOR UPDATES.
+
+\subsubsection{Text Editor Options}\label{text-editor-options}
+
+EP-Launch will start a text editor when editing a IDF file or when viewing many of the results files.~ The text editor that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the text editor of your choice. The Auto Find button will automatically find the program that is associated with the TXT file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a text editor is available immediately. The most common text editor is NOTEPAD.EXE and is built into Windows but many other text editors are also available.
+
+\subsubsection{Drawing Viewer Options}\label{drawing-viewer-options}
+
+The default drawing viewer is the application associated with DXF files. This can be changed to your favorite drawing program by using the Select button then locating the executable file for your favorite drawing software capable of reading a DXF file. The Auto Find button will automatically find the program that is associated with the DXF file extension and use that program. A variety of programs (free of charge) can render DXF files for viewing.~ The \href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details} document lists some of these programs as well as displaying what a DXF rendered file looks like on the screen.
+
+\subsubsection{VRML Viewer Options}\label{vrml-viewer-options}
+
+EP-Launch will start a VRML Viewer when a building drawing is created using the Report, Surfaces, VRML option in your IDF file.~ The VRML Viewer that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the VRML Viewer of your choice. The Auto Find button will automatically find the program that is associated with the WRL file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a VRML Viewer is available immediately. Many other VRML Viewers are available.
+
+\subsubsection{Spreadsheet Options}\label{spreadsheet-options}
+
+EP-Launch will start a spreadsheet program when viewing many of the results files.~ The spreadsheet that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the spreadsheet program of your choice. The Auto Find button will automatically find the program that is associated with the CSV file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a spreadsheet program is available immediately.
+
+\subsubsection{Diagramming Options}\label{diagramming-options}
+
+EP-Launch will start a diagramming program to view SVG files from HVAC Diagram.~ The diagramming program that will be used is shown but can be changed by either pressing the Select button, the Auto Find button, the Use Firefox button or the Use Opera button. The Select button allows you to find the diagramming program of your choice but make sure it is capable of opening SVG files. The Auto Find button will automatically find the program that is associated with the SVG file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a spreadsheet program is available immediately.~ Since both Firefox and Opera web browsers can view SVG files, those buttons will select those respective browsers if available.
+
+\subsubsection{HTML Browser Options}\label{html-browser-options}
+
+EP-Launch will start a HTML browser program when viewing the tabular results file when HTML is chosen in OutputControl:Table:Style object. The HTML browser that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the HTML browser of your choice. The Auto Find button will automatically find the program that is associated with the HTML file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a HTML browser is available immediately.
+
+\subsubsection{ESO Viewer Options}\label{eso-viewer-options}
+
+By default, ESO files are opened with a text editor. ESO files are the raw output file containing results from EnergyPlus for Output:Variable objects. They are often processed into CSV files to make it easier to view them. At least one utility program has been developed to view ESO files directly (see the EnergyPlus.gov web site under ``Interfaces \& Other Tools'', ``Third-party EnergyPlus Tools).~ The Auto Find and Select buttons work the same way as other viewer selectors. If no special ESO viewer is selected the box will be shown as empty. It can also be emptied by using the Clear button.
+
+\subsubsection{PDF Viewer Options}\label{pdf-viewer-options}
+
+EP-Launch will start a PDF viewer program when opening the EnergyPlus documentation under the Help menu.~ The PDF Viewer that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the PDF Viewer of your choice. The Auto Find button will automatically find the program that is associated with the PDF file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a PDF Viewer is available immediately.
+
+\subsubsection{File Association Options}\label{file-association-options}
+
+When installing EnergyPlus, you are given an option if you want IDF, IMF, and EPG files associated with EP-Launch. This allows double clicking on files with those extensions and having EP-Launch start automatically with those files. If during the install that option is not selected or if you have changed the program that opens IDF, IMF and EPG files and want to change it back to EP-Launch, the button for this option will do that.
+
+\subsubsection{Reset Options}\label{reset-options}
+
+Two reset options are available here.
+
+The \textbf{Auto Find All File Viewers} button will autofind all the file viewers in one step. This is equivalent to pressing the Auto Find button for each viewer program.
+
+The \textbf{Reset All Options and Exit} button will clear all options and restore the default values used when first invoking EP-Launch for the first time. This also clears the list of recently used IDF and weather files.~ This option will exit EP-Launch and you will have to start EP-Launch again.
+
+\subsection{Help Menu}\label{help-menu}
+
+The Help menu can be used to open the EnergyPlus documentation files and the EP-Launch help file. In addition, you can check for updates to the EnergyPlus program and other files in the EnergyPlus distribution.
+
+\subsection{Recently Used Files}\label{recently-used-files}
+
+The recently used input, weather and group file pull down lists can hold a maximum of twenty items. These lists, like the viewers selected, are saved between times you use the EP-Launch program.
+
+\subsection{Utilities Tab}\label{utilities-tab}
+
+The utilities tab shown in the following figure allows several utility programs that come with EnergyPlus to be used directly. More information on each utility is also available in the AuxiliaryPrograms documentation.
+
+\begin{figure}[hbtp] % fig 9
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image009.png}
+\caption{EP-Launch Utilities Tab. \protect \label{fig:ep-launch-utilities-tab.}}
+\end{figure}
+
+For each utility, input files can be selected by using the Browse Button. The input file can be opened using a text editor and, for certain utilities, the IDF Editor. If a weather file is needed for a utility it can also be selected. For other utilities, no weather file is needed and that portion of the screen is not shown. The appropriate output files can be opened by the ``Open'' button near the bottom of the screen. To run the utility, use the ``Run'' button in the lower left corner of the screen above the ``Exit'' button.
+
+In addition, for each utility, a brief description of the function of the utility is shown in the about box but much more information is available in the AuxiliaryPrograms documentation.
+
+\subsection{Caveats}\label{caveats}
+
+Remember to save changes made in the editor before you run another simulation.
+
+The simulation cannot write new results to open files which are locked by another application.
+
+You will need to close the spreadsheet program that views the resulting CSV files prior to another simulation and you may need to close the text editor windows also (depending on your editor).
+
+The EPL-RUN.BAT batch file is used to run EnergyPlus from the EP-Launch program. It can be edited with care if other postprocessors or preprocessors are to be used.
+
+\subsection{When things go wrong}\label{when-things-go-wrong}
+
+Though EnergyPlus has had several releases (including beta releases prior to initial release), there still may be problems when input files meet with EnergyPlus. If you are using EP-Launch when this happens, you will see a window appear as in the figure below (Figure~\ref{fig:energyplus-crash-within-ep-launch.}). Follow the instructions listed on the screen.
+
+\begin{figure}[hbtp] % fig 10
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image010.jpg}
+\caption{EnergyPlus crash within EP-Launch. \protect \label{fig:energyplus-crash-within-ep-launch.}}
+\end{figure}
+
+\subsection{Bugs}\label{bugs}
+
+The EP-Launch program has been through several ``releases'' but there is still a chance you will find bugs. Please report them to the energyplus-support@gard.com address so that we can fix them prior to the release.
+
+If the pull-down lists ever are shown as blank the ``reset'' button may be used. This unlabeled button is very small in the lower left-hand corner of the main screen. It removes the items shown in the recently used file list and causes the program to forget the selected viewers and text editors; and exits the program. When you start EP-Launch again, you will need to make these selections (viewers and text editors) again.
diff --git a/doc/getting-started/src/running-energyplus/introduction.tex b/doc/getting-started/src/running-energyplus/introduction.tex
new file mode 100644
index 00000000000..68972043597
--- /dev/null
+++ b/doc/getting-started/src/running-energyplus/introduction.tex
@@ -0,0 +1,7 @@
+\section{Introduction}\label{introduction}
+
+EnergyPlus is a simulation program designed for modeling buildings with all their associated heating, ventilating, and air conditioning equipment. EnergyPlus is a simulation \emph{engine}: it was designed to be an element within a system of programs that would include a graphical user interface to describe the building. However, it can be run \emph{stand alone} without such an interface. This document describes how to run EnergyPlus in such a stand alone fashion. This section will introduce you to the EP-Launch program, which helps you run EnergyPlus.~ EP-Launch looks and acts pretty much like a standard Windowsâ„¢ program, so if you just want to get started with some exercises, you can skip to the section ``Tutorial Example for running EnergyPlus'' first and come back to this section if you run into problems with EP-Launch.
+
+Like all simulation programs, EnergyPlus consists of more than just an executable file. EnergyPlus needs various input files that describe the building to be modeled and the environment surrounding it. The program produces several output files, which need to be described or further processed in order to make sense of the results of the simulation. Finally, even in stand-alone mode, EnergyPlus is usually not executed ``by hand'', but rather by running a procedure file which takes care of finding input files and storing or further processing the output files.
+
+To assist those in the Windows environment, we have included the EP-Launch program. Review the next section for basic instructions. More advanced techniques of executing the program are contained in the Auxiliary Programs document under ``Technical Details of running EnergyPlus'', including some advanced uses of the EP-Launch program. If you wish to learn about DOS/Command Line use for EnergyPlus, you will need to read that section in the Auxiliary Programs document.
diff --git a/doc/getting-started/src/standard-energyplus-units.tex b/doc/getting-started/src/standard-energyplus-units.tex
new file mode 100644
index 00000000000..27ea4aa9a4d
--- /dev/null
+++ b/doc/getting-started/src/standard-energyplus-units.tex
@@ -0,0 +1,63 @@
+\chapter{Standard EnergyPlus Units}\label{standard-energyplus-units}
+
+EnergyPlus has adopted the standard SI units for input and output.
+
+ASCII with no spaces is used for abbreviations. Note that exponents appear without any indication of exponentiation: i.e., kg/m3 not kg/m\^{}3 or kg/m**3. Also note the use of dashes. We have W/m2-K not W/m2*K or W/(m2*K).
+
+At the end we note the ``problem'' variables -- the inputs that have non-standard units. Inputs using these units will have to be changed and the code checked to see how the quantities are used internally.
+
+% table 10
+\begin{longtable}[c]{p{1.59in}p{2.9in}p{1.5in}}
+\caption{Standard EnergyPlus Units \label{table:standard-energyplus-units}} \tabularnewline
+\toprule 
+Quantity & unit & abbreviation \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Standard EnergyPlus Units} \tabularnewline
+\toprule 
+Quantity & unit & abbreviation \tabularnewline
+\midrule
+\endhead
+
+angular degrees & degree & deg \tabularnewline
+Length & meter & m \tabularnewline
+Area & square meter & m2 \tabularnewline
+Volume & cubic meter & m3 \tabularnewline
+Time & seconds & s \tabularnewline
+frequency & Hertz & Hz \tabularnewline
+temperature & Celsius & C \tabularnewline
+absolute temperature & Kelvin & K \tabularnewline
+temperature difference & Celsius & deltaC \tabularnewline
+Speed & meters per second & m/s \tabularnewline
+energy (or work) & Joules & J \tabularnewline
+Power & Watts & W \tabularnewline
+Mass & kilograms & kg \tabularnewline
+Force & Newton & N \tabularnewline
+mass flow & kilograms per second & kg/s \tabularnewline
+volume flow & cubic meters per second & m3/s \tabularnewline
+Pressure & Pascals & Pa \tabularnewline
+pressure difference & Pascals & Pa \tabularnewline
+specific enthalpy & Joules per kilogram & J/kg \tabularnewline
+Density & kilograms per cubic meter & kg/m3 \tabularnewline
+heat flux & watts per square meter & W/m2 \tabularnewline
+specific heat & ------------------------------------------------------------------------ & J/kg-K \tabularnewline
+conductivity & ------------------------------------------------------------------------ & W/m-K \tabularnewline
+Diffusivity & ------------------------------------------------------------------------ & m2/s \tabularnewline
+heat transfer coefficient & ------------------------------------------------------------------------ & W/m2-K \tabularnewline
+R-value & ------------------------------------------------------------------------ & m2-K/W \tabularnewline
+heating or cooling capacity & Watts & W \tabularnewline
+electric potential & volts & V \tabularnewline
+electric current & Amperes & A \tabularnewline
+illuminace & lux & lx \tabularnewline
+luminous flux & lumen & lm \tabularnewline
+luminous intensity & candelas & cd \tabularnewline
+luminance & candelas per square meter & cd/m2 \tabularnewline
+vapor diffusivity & m2/s & ~ \tabularnewline
+Viscosity & ------------------------------------------------------------------------ & kg/m-s \tabularnewline
+Dynamic Viscosity & ------------------------------------------------------------------------ & N-s/m2 \tabularnewline
+Porosity & ------------------------------------------------------------------------ & m3/m3 \tabularnewline
+thermal gradient coeff for moisture capacity & ------------------------------------------------------------------------ & kg/kg-K \tabularnewline
+isothermal moisture capacity & ------------------------------------------------------------------------ & m3/kg \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/getting-started/src/title.tex b/doc/getting-started/src/title.tex
new file mode 100644
index 00000000000..63f37402bb8
--- /dev/null
+++ b/doc/getting-started/src/title.tex
@@ -0,0 +1 @@
+\input{../title}
diff --git a/doc/getting-started/src/tutorial-example-for-running-energyplus.tex b/doc/getting-started/src/tutorial-example-for-running-energyplus.tex
new file mode 100644
index 00000000000..1a23b5482f9
--- /dev/null
+++ b/doc/getting-started/src/tutorial-example-for-running-energyplus.tex
@@ -0,0 +1,3 @@
+\chapter{Tutorial Example for running EnergyPlus}\label{tutorial-example-for-running-energyplus}
+
+The following example is taken directly from the training course ``Introduction to EnergyPlus'', Exercise 1.~ Of course, it is presented here without the benefit of classroom presentation and discussion but when followed step by step, should provide an introduction of actually using EnergyPlus.
diff --git a/doc/getting-started/src/tutorial-example-for-running-energyplus/instructions.tex b/doc/getting-started/src/tutorial-example-for-running-energyplus/instructions.tex
new file mode 100644
index 00000000000..fcc3923832c
--- /dev/null
+++ b/doc/getting-started/src/tutorial-example-for-running-energyplus/instructions.tex
@@ -0,0 +1,365 @@
+\section{Instructions}\label{instructions-000}
+
+\subsection{Exercise 1A. Run Pre-Defined Building with no Windows}\label{exercise-1a.-run-pre-defined-building-with-no-windows}
+
+Objective:~ Learn to use EP-Launch to run an EnergyPlus input file and view output files.
+
+1.~Open EP-Launch.
+
+2.~Under ``Input File'', browse for input file Exercise1A.idf.~ This input file contains the 1-zone model described above without the windows and lights. This is located under the install folder \textless{}root\textgreater{}\textbackslash{}ExampleFiles\textbackslash{}BasicsFiles,
+
+3.~Under ``Weather File'', select ``No Weather File'' (at the top of the pull-down list).
+
+4.~Press ``Simulate''.
+
+5.~When the simulation is complete, review output files:
+
+\begin{itemize}
+\item
+  Press ``Text Output Files'' to see all text output.~ Look especially at the eio and err output files.
+\item
+  Press ``Drawing Files'' to see a dxf drawing of the building envelope.~ (If using Voloview Express, right-click to switch between wireframe and shaded orbit view.~ In DWG True View, use ``View'' -\textgreater{} ``Visual Styles'' to switch between wireframe and solid views. In both programs, use ``View'' à``Named Views'' to select isometric views.)
+\item
+  An empty svg drawing file will also open (this will show HVAC system components in later exercises).~ Note that the Adobe SVG viewer is a ``plug-in'' for Internet Explorer (IE), so IE will open when viewing an SVG file.~ Depending on the security settings in IE, you may be prompted with a warning about ``active'' content.
+\item
+  Press ``Spreadsheets'' to open the numeric csv output files.~ In Exercise1a.csv, review the pattern of outdoor conditions and loads.~ (To make it easier to read the column headings, select Row 1, format cells, and turn on wrap text; then select cell B2 and select ``freeze panes''.) ~In Exercise1aMeter.csv, review the facility district heating and cooling meters.
+\item
+  Zone/Sys Air Temperature -- the zone air temperatures are already being reported.
+\item
+  Outdoor Dry Bulb -- is being reported (so you can compare to outside temperature)
+\item
+  The meter for the heating in the facility - DistrictHeating:Facility -- is being reported. Facility is the entire building.
+\item
+  The meter for the cooling in the facility - DistrictCooling:Facility -- is being reported.
+\end{itemize}
+
+\subsection{Exercise 1B. Add Windows}\label{exercise-1b.-add-windows}
+
+Objective:~ Learn how to add materials, constructions, and a surface using 3-D coordinates.
+
+1.~In EP-Launch, with input file Exercise1A.idf still selected, press ``Edit -- IDF Editor''.~ This will open Exercise1A.idf in the IDF Editor, a tool that assists in editing EnergyPlus input files (idf).
+
+2.~In IDF Editor, select File -\textgreater{} Save Options . . . and set ``Saved Order'' to ``Original with New at Top'', and ``Special Format for Some Objects'' to ``Yes.''~ Check the ``Set as Default'' box.
+
+3.~In IDF Editor, Select File -\textgreater{} Save As . . . and save this file as Exercise1B.idf.
+
+4.~Create the construction definition for the windows which are double-pane clear gas with an air space:
+
+\begin{itemize}
+\item
+  Using File -\textgreater{} Open Dataset, open the window glass materials dataset file, WindowGlassMaterials.idf
+\item
+  Scroll down the Class list and select ``\textbf{WindowMaterial:Glazing}''.
+\end{itemize}
+
+\begin{lstlisting}
+-Hint:  In IDF Editor, View -> Show Classes with Objects Only (or ctl-L) will hide all empty object types from the class list.
+\end{lstlisting}
+
+\begin{itemize}
+\item
+  Locate the object which defines the material properties for ``CLEAR 6MM''.~ Select this object (by clicking on the column heading).
+\item
+  Using Edit -\textgreater{} Copy Object (or the toolbar button, or ctl-C), copy this object.
+\item
+  Switch windows to file Exercise1B.idf and paste the window material into this file.~ (Verify that is had been added by going to \textbf{WindowMaterial:Glazing} to view the object.)
+\item
+  Open dataset file WindowGasMaterials.idf.
+\item
+  Locate ``AIR 3MM'', copy it and paste it into Exercise1B.idf.
+\item
+  In Exercise1B.idf, select the ``\textbf{Construction}'' class.~ There are three constructions pre-defined for the walls, roof, and floor.
+\item
+  Press ``New Obj'' to create a new blank \textbf{Construction} object.
+\item
+  Name this new construction ``DOUBLE PANE WINDOW''.
+\item
+  Use the pulldown list to select ``CLEAR 6MM'' for the outside layer, then press ``Enter'' or ``Return'' to save this entry and move to the next field.
+\item
+  Select ``AIR 3MM'' for Layer 2, and ``CLEAR 6MM'' for Layer 3.
+\end{itemize}
+
+5.~Add the east window (3m wide by 2m high, centered on wall, \emph{see the drawing in} \emph{Figure~\ref{fig:schematic-for-exercise-1}} \emph{to determine coordinates):}
+
+\begin{itemize}
+\item
+  Select ``\textbf{FenestrationSurface:Detailed}'' class.
+\item
+  Add a new object named ``EAST WINDOW''.
+\item
+  Set the remaining fields as listed:
+\item
+  Surface Type \ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{} = Window
+\item
+  Construction Name \ldots{}\ldots{}\ldots{}\ldots{} = DOUBLE PANE WINDOW
+\item
+  Base Surface Name \ldots{}\ldots{}\ldots{}\ldots{}\ldots{} = ZONE SURFACE EAST
+\item
+  OutsideFaceEnvironment Object \ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}. = \textless{}blank\textgreater{}
+\item
+  View Factor to Ground \ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}.. = autocalculate
+\item
+  Name of shading control \ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{} = \textless{}blank\textgreater{}
+\item
+  WindowFrameAndDivider Name \ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}.. = \textless{}blank\textgreater{}
+\item
+  Multiplier \ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}. = 1
+\item
+  Number of Surface Vertex Groups \ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{}\ldots{} = 4
+\item
+  Vertex coordinates = \emph{as determined from the drawing} \emph{Figure~\ref{fig:schematic-for-exercise-1}}.~ Coordinates in this input are in World Coordinates (all relative to the global origin of 0,0,0).~ Coordinates are specified as viewed from the outside of the surface, using the rules specified in the SurfaceGeometry object.
+\end{itemize}
+
+6.~Add the west window, similar to the east window.
+
+7.~Add a new \textbf{Output:Surfaces:List} object, type = Details.~ This report produces a list of all surfaces in the eio output summarizing area, azimuth, tilt, etc.
+
+8.~Save and close the IDF file, select Exercise1B.idf in EP-Launch, run the simulation and view outputs.
+
+\begin{itemize}
+\item
+  Always review the err file for errors and warnings.~ Fix problems if needed and re-run.
+\item
+  Are the windows in the right place in the dxf drawing file. (Use the Drawing File button or select the DXF file from View -\textgreater{} Single File or from the Quick-Open panel).
+\item
+  Review the surface details report in the eio file, search for ``Zone/Shading Surfaces'' to find this report. (Use the Text Output button, Quick Open ``eio'' button, or select from the single file menu, or use F7).~ This report is easier to read by pasting this section into a spreadsheet and using the text to columns function with comma as a delimiter).
+\item
+  Open the csv output file and compare the heating and cooling loads with the results from Exercise1A.csv.
+\end{itemize}
+
+\subsection{Exercise 1C. Add Internal Loads}\label{exercise-1c.-add-internal-loads}
+
+Objective:~ Learn how to add schedules, internal loads, and report variables.
+
+1.~Save Exercise1B.idf as Exercise1C.idf.
+
+2.~Open the dataset file Schedules.idf:
+
+\begin{itemize}
+\item
+  Copy the \textbf{Schedule:Compact} object named ``Office Lighting'', and paste it into Exercise1C.idf.
+\item
+  Copy the \textbf{ScheduleTypeLimits} object named ``Fraction'', and paste it into Exercise1C.idf.
+\end{itemize}
+
+3.~In Exercise1C.idf, add a LIGHTS object named ZONE ONE Lights, using the Office Lighting schedule, peak input is 1000W.~ Consult the EnergyPlus Input Output Reference section on \textbf{Lights} for values for the return, radiant, and visible fractions.~ Assume the lights are surface mounted fluorescents.
+
+4.~Save and close the IDF file, select Exercise1C.idf in EP-Launch, run the simulation and review outputs.
+
+5.~Open the rdd file (the report variable data dictionary) and find report variable names related to \textbf{Lights}.~ Add a new \textbf{Output:Variable} object to report the lighting electric consumption.
+
+6.~Run the simulation and review outputs.
+
+\begin{itemize}
+\item
+  Check the err file.
+\item
+  Find the lighting electric consumption in the csv output file.
+\end{itemize}
+
+7.~Compare heating and cooling loads with Exercise1A and Exercise1B.
+
+8.~Add more \textbf{Output:Variable} objects as desired.
+
+\subsection{Exercise 1D. Annual Simulation and Predefined Reports}\label{exercise-1d.-annual-simulation-and-predefined-reports}
+
+Objective:~ Learn how to run an annual simulation using a weather data file and add table reports.
+
+1.~Save Exercise1C.idf as Exercise1D.idf.
+
+2.~Edit the \textbf{SimulationControl} object to turn off the design day simulations by setting ``Run Simulation for Sizing Periods'' to \textbf{No} and turn on the weather file (annual) simulation by setting ``Run Simulation for Weather File Run Periods'' to \textbf{Yes}..
+
+3.~Add a RunPeriod object to run a full annual simulation, let other fields default or remain blank.
+
+4.~Add a \textbf{Output:Table:SummaryReports} object, and select the following reports:~ ``Annual Building Performance Summary'' (ABUPS), ``Input Verification and Results Summary'' (IVRS), ``Climate Summary'', and ``Envelope Summary''.
+
+5.~Add a \textbf{OutputControl:Table:Style} object, and select HTML format (ColumnSeparator).
+
+6.~Edit existing \textbf{Output:Variable} and \textbf{Output:Meter} objects and change the reporting frequency from Hourly to Monthly.
+
+7.~Save and close the IDF file, select Exercise1D.idf in EP-Launch.
+
+8.~Select Chicago TMY2 weather file (or the weather file of your choice) and run the simulation.
+
+9.~Review outputs.
+
+\begin{itemize}
+\item
+  Check the err file.
+\item
+  Look at the monthly results in the csv output.
+\item
+  Press the Table output button to view the predefined reports.
+\end{itemize}
+
+\subsection{Solution: Exercise 1}\label{solution-exercise-1}
+
+\emph{Try not to look at this section until you have completed the Exercise.}
+
+\subsubsection{List of New Objects}\label{list-of-new-objects}
+
+This is a listing of new and modified objects created in this Exercise.
+
+\begin{lstlisting}
+WindowMaterial:Glazing,
+    CLEAR 6MM,               !- Name
+    SpectralAverage,         !- Optical Data Type
+    ,                        !- Name of Window Glass Spectral Data Set
+    0.006,                   !- Thickness {m}
+    0.775,                   !- Solar Transmittance at Normal Incidence
+    0.071,                   !- Solar Reflectance at Normal Incidence: Front Side
+    0.071,                   !- Solar Reflectance at Normal Incidence: Back Side
+    0.881,                   !- Visible Transmittance at Normal Incidence
+    0.080,                   !- Visible Reflectance at Normal Incidence: Front Side
+    0.080,                   !- Visible Reflectance at Normal Incidence: Back Side
+    0.0,                     !- IR Transmittance at Normal Incidence
+    0.84,                    !- IR Hemispherical Emissivity: Front Side
+    0.84,                    !- IR Hemispherical Emissivity: Back Side
+    0.9;                     !- Conductivity {W/m-K}
+\end{lstlisting}
+
+\begin{lstlisting}
+WindowMaterial:Gas,
+    AIR 3MM,                 !- Name
+    Air    ,                 !- Gas Type
+    0.0032;                  !- Thickness {m}
+\end{lstlisting}
+
+\begin{lstlisting}
+Construction,
+    DOUBLE PANE WINDOW,      !- Name
+    CLEAR 6MM,               !- Outside Layer
+    AIR 3MM,                 !- Layer #2
+    CLEAR 6MM;               !- Layer #3
+\end{lstlisting}
+
+\begin{lstlisting}
+FenestrationSurface:Detailed,
+    EAST WINDOW,             !- User Supplied Surface Name
+    WINDOW,                  !- Surface Type
+    DOUBLE PANE WINDOW,      !- Construction Name of the Surface
+    ZONE SURFACE EAST,       !- Base Surface Name
+    ,                        !- OutsideFaceEnvironment Object
+    autocalculate,           !- View Factor to Ground
+    ,                        !- Name of shading control
+    ,                        !- WindowFrameAndDivider Name
+    1,                       !- Multiplier
+    4,                       !- Number of vertices
+    8, 1.5, 2.35,            !- X,Y,Z  1 {m}
+    8, 1.5, 0.35,            !- X,Y,Z  2 {m}
+    8, 4.5, 0.35,            !- X,Y,Z  3 {m}
+    8, 4.5, 2.35;            !- X,Y,Z  4 {m}
+\end{lstlisting}
+
+\begin{lstlisting}
+FenestrationSurface:Detailed,
+    WEST WINDOW,             !- User Supplied Surface Name
+    WINDOW,                  !- Surface Type
+    DOUBLE PANE WINDOW,      !- Construction Name of the Surface
+    ZONE SURFACE WEST,       !- Base Surface Name
+    ,                        !- OutsideFaceEnvironment Object
+    autocalculate,           !- View Factor to Ground
+    ,                        !- Name of shading control
+    ,                        !- WindowFrameAndDivider Name
+    1,                       !- Multiplier
+    4,                       !- Number of Vertices
+    0, 4.5, 2.35,            !- X,Y,Z  1 {m}
+    0, 4.5, 0.35,            !- X,Y,Z  2 {m}
+    0, 1.5, 0.35,            !- X,Y,Z  3 {m}
+    0, 1.5, 2.35;            !- X,Y,Z  4 {m}
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Surfaces:List,Details;
+\end{lstlisting}
+
+\begin{lstlisting}
+Schedule:Compact,
+    Office Lighting,         !- Name
+    Fraction,                !- ScheduleType
+    Through: 12/31,          !- Complex Field #1
+    For: Weekdays SummerDesignDay,  !- Complex Field #2
+    Until: 05:00, 0.05,      !- Complex Field #4
+    Until: 07:00, 0.1,       !- Complex Field #6
+    Until: 08:00, 0.3,       !- Complex Field #8
+    Until: 17:00, 0.9,       !- Complex Field #10
+    Until: 18:00, 0.5,       !- Complex Field #12
+    Until: 20:00, 0.3,       !- Complex Field #14
+    Until: 22:00, 0.2,       !- Complex Field #16
+    Until: 23:00, 0.1,       !- Complex Field #18
+    Until: 24:00, 0.05,      !- Complex Field #20
+    For: Saturday WinterDesignDay,  !- Complex Field #21
+    Until: 06:00, 0.05,      !- Complex Field #23
+    Until: 08:00, 0.1,       !- Complex Field #25
+    Until: 12:00, 0.3,       !- Complex Field #27
+    Until: 17:00, 0.15,      !- Complex Field #29
+    Until: 24:00, 0.05,      !- Complex Field #31
+    For: Sunday Holidays AllOtherDays,  !- Complex Field #32
+    Until: 24:00, 0.05;      !- Complex Field #34
+\end{lstlisting}
+
+\begin{lstlisting}
+ScheduleTypeLimits,
+    Fraction,                !- ScheduleType Name
+    0.0,                     !- Lower Limit Value
+    1.0,                     !- Upper Limit Value
+    CONTINUOUS;              !- Numeric Type
+\end{lstlisting}
+
+\begin{lstlisting}
+Lights,
+    ZONE ONE Lights,         !- Name
+    ZONE ONE,                !- Zone Name
+    Office Lighting,         !- Schedule Name
+    LightingLevel,           !- Design Level Calculation Method
+    1000,                    !- Lighting Level {W}
+    ,                        !- Watts per Zone Floor Area {W/m2}
+    ,                        !- Watts per Person {W/person}
+    0,                       !- Return Air Fraction
+    0.72,                    !- Fraction Radiant
+    0.18,                    !- Fraction Visible
+    1,                       !- Fraction Replaceable
+    General,                 !- End-Use Subcategory
+    No;                      !- Return Air Fraction Calculated from Plenum Temperature
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,*,Lights Electric Consumption ,hourly;
+\end{lstlisting}
+
+\begin{lstlisting}
+RunPeriod,
+    1,                       !- Begin Month
+    1,                       !- Begin Day Of Month
+    12,                      !- End Month
+    31,                      !- End Day Of Month
+    UseWeatherFile,          !- Day Of Week For Start Day
+    Yes,                     !- Use WeatherFile Holidays/Special Days
+    Yes,                     !- Use WeatherFile DaylightSavingPeriod
+    No,                      !- Apply Weekend Holiday Rule
+    Yes,                     !- Use WeatherFile Rain Indicators
+    Yes,                     !- Use WeatherFile Snow Indicators
+    1;                       !- Number of years of simulation
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Table:SummaryReports,
+    Annual Building Utility Performance Summary,  !- ReportName1
+    Input Verification and Results Summary,  !- ReportName2
+    Climate Summary,         !- ReportName3
+    Envelope Summary;        !- ReportName4
+\end{lstlisting}
+
+\begin{lstlisting}
+OutputControl:Table,
+    HTML;                    !- ColumnSeparator
+\end{lstlisting}
+
+\begin{lstlisting}
+SimulationControl,
+    No,                      !- Do the zone sizing calculation
+    No,                      !- Do the system sizing calculation
+    No,                      !- Do the plant sizing calculation
+    No,                      !- Do the design day simulations
+    Yes;                     !- Do the weather file simulation
+\end{lstlisting}
diff --git a/doc/getting-started/src/tutorial-example-for-running-energyplus/running-energyplus-building-envelope-internal.tex b/doc/getting-started/src/tutorial-example-for-running-energyplus/running-energyplus-building-envelope-internal.tex
new file mode 100644
index 00000000000..bf98291d7b0
--- /dev/null
+++ b/doc/getting-started/src/tutorial-example-for-running-energyplus/running-energyplus-building-envelope-internal.tex
@@ -0,0 +1,95 @@
+\section{Running EnergyPlus, Building Envelope, Internal Loads, Reports}\label{running-energyplus-building-envelope-internal-loads-reports}
+
+\subsection{Overview}\label{overview}
+
+\begin{itemize}
+\item
+  Rectangular single story building
+\item
+  Windows in east and west walls
+\item
+  Single zone with no interior partitions
+\item
+  Lightweight construction
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 11
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image011.jpg}
+\caption{Schematic for Exercise 1 \protect \label{fig:schematic-for-exercise-1}}
+\end{figure}
+
+The details of the building construction and operation are shown in the following tables and description. For tutorial purposes, the building is located in Chicago Illinois, one of the weather files supplied with EnergyPlus. These details are listed in a fashion to make for easy entry into EnergyPlus.
+
+\subsection{Details of the exercise}\label{details-of-the-exercise}
+
+\subsubsection{Surface Constructions}\label{surface-constructions}
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Additional Model Details \label{table:additional-model-details}} \tabularnewline
+\toprule 
+Type & Details \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Additional Model Details} \tabularnewline
+\toprule 
+Type & Details \tabularnewline
+\midrule
+\endhead
+
+Internal Loads & Lights (1000 W), Office Lighting schedule, surface mount fluorescent \tabularnewline
+Space Conditioning & Heating setpoint 20C, cooling setpoint 24C, no setback \tabularnewline
+Location & Chicago, Illinois, USA; Summer and Winter design days \tabularnewline
+Simulation Period & Annual, Jan 1 - Dec 31 \tabularnewline
+Ground Temperatures & 18.2 C to 22.5 C (from Slab preprocessor, vary monthly) \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Window Properties}\label{window-properties}
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Additional Model Details \label{table:additional-model-details}} \tabularnewline
+\toprule 
+Type & Details \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Additional Model Details} \tabularnewline
+\toprule 
+Type & Details \tabularnewline
+\midrule
+\endhead
+
+Internal Loads & Lights (1000 W), Office Lighting schedule, surface mount fluorescent \tabularnewline
+Space Conditioning & Heating setpoint 20C, cooling setpoint 24C, no setback \tabularnewline
+Location & Chicago, Illinois, USA; Summer and Winter design days \tabularnewline
+Simulation Period & Annual, Jan 1 - Dec 31 \tabularnewline
+Ground Temperatures & 18.2 C to 22.5 C (from Slab preprocessor, vary monthly) \tabularnewline
+\bottomrule
+\end{longtable}
+
+Refers to specific glass type included in the EnergyPlus datasets directory
+
+~(\textbf{WindowGlassMaterials.idf})
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Additional Model Details \label{table:additional-model-details}} \tabularnewline
+\toprule 
+Type & Details \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Additional Model Details} \tabularnewline
+\toprule 
+Type & Details \tabularnewline
+\midrule
+\endhead
+
+Internal Loads & Lights (1000 W), Office Lighting schedule, surface mount fluorescent \tabularnewline
+Space Conditioning & Heating setpoint 20C, cooling setpoint 24C, no setback \tabularnewline
+Location & Chicago, Illinois, USA; Summer and Winter design days \tabularnewline
+Simulation Period & Annual, Jan 1 - Dec 31 \tabularnewline
+Ground Temperatures & 18.2 C to 22.5 C (from Slab preprocessor, vary monthly) \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/getting-started/src/tutorial-exercise-2.tex b/doc/getting-started/src/tutorial-exercise-2.tex
new file mode 100644
index 00000000000..334e7d90651
--- /dev/null
+++ b/doc/getting-started/src/tutorial-exercise-2.tex
@@ -0,0 +1,3 @@
+\chapter{Tutorial Exercise 2}\label{tutorial-exercise-2}
+
+The following example is taken directly from the training course ``Introduction to EnergyPlus'', Exercise 2.~ Of course, it is presented here without the benefit of classroom presentation and discussion but when followed step by step, should provide an introduction of actually using EnergyPlus.
diff --git a/doc/getting-started/src/tutorial-exercise-2/instructions-001.tex b/doc/getting-started/src/tutorial-exercise-2/instructions-001.tex
new file mode 100644
index 00000000000..e42e3fb1650
--- /dev/null
+++ b/doc/getting-started/src/tutorial-exercise-2/instructions-001.tex
@@ -0,0 +1,510 @@
+\section{Instructions}\label{instructions}
+
+\subsection{Exercise 2A. Add Unitary System with DX Cooling and Gas Heating (Furnace) Serving a Single Zone}\label{exercise-2a.-add-unitary-system-with-dx-cooling-and-gas-heating-furnace-serving-a-single-zone}
+
+Objective:~ Learn how to describe a thermostat and unitary equipment using HVACTemplate objects.
+
+1)~~~Open Exercise2.idf and save it as Exercise2A.idf.~ (Exercise2.idf contains the building envelope, internal loads, and some extra schedules to support the HVAC system descriptions which will be added in this Exercise.)
+
+2)~~~Add a \textbf{HVACTemplate:Thermostat} object to define the thermostat setpoints for this simulation.
+
+\begin{itemize}
+\item
+  Choose a name for the thermostat.~ This name will be referenced in the next step.
+\item
+  For heating setpoints, use pre-defined schedule named ``Office Heating Setpoints''.
+\item
+  For cooling setpoints, use pre-defined schedule named ``Office Cooling Setpoints''.
+\end{itemize}
+
+3)~~~Add a \textbf{HVACTemplate:Zone:Unitary} object serving the ``NORTH PERIMETER'' zone.~ Choose a name for the air handling system which will be added in Step 4. Use the thermostat name from step 2 for the thermostat field. Retain the defaults for the remaining fields.
+
+4)~~~Add a \textbf{HVACTemplate:System:Unitary} object.~ The name of this system object must be the same name used in the zone object for ``Air Handling System Name'' field (See Step 3).~ Retain the defaults for all fields except the following:
+
+\begin{itemize}
+\item
+  Availability Schedule = Office HVAC (predefined)
+\item
+  Control Zone Name or Thermostat Location = NORTH PERIMETER
+\item
+  Supply Fan Operating Mode Schedule Name = Continuous
+\item
+  Heating Coil Type = Gas
+\item
+  Minimum Outdoor Air Schedule Name = Office Minimum OA (predefined)
+\end{itemize}
+
+5)~~~Add a \textbf{Sizing:Parameters} object and set the sizing factor to 1.2 (for 20\% oversizing).
+
+6)~~~Edit the \textbf{SimulationControl} object and set the Zone and System sizing flags to ``Yes''.
+
+7)~~~Run the simulation and review output files, especially:
+
+\begin{itemize}
+\item
+  err, there will be some warnings about meters that do no exist and the ABUPS report not being a full year.~ These will go away as more features are added and an annual run is simulated.
+\item
+  DXF , drawing of building surfaces.~ (Try selecting the Southwest Isometric named view, then see how each zone is a separate drawing layer.~ In Voloview open the View -\textgreater{} Layers dialog.~ Click on the light bulbs to toggle display of each zone.~ In TrueView click on the Layer Properties Manager toolbar button.~ To toggle display of a layer, single-click a layer light bulb, then click apply.)
+\item
+  SVG, block diagram of the HVAC system components. (HINT: right-click in the drawing and read the Help to learn how to navigate in the SVG viewer.)
+\item
+  Main Results File (csv) and Meter File (Meter.csv).
+\item
+  eio, zone and system sizing results
+\item
+  Add output variables to report operation of the system (furnace) fan, heating coil, and cooling coil.~ Reference the RDD output file for variable names.
+\end{itemize}
+
+8)~~~Re-run the simulation and review results again.
+
+\begin{itemize}
+\tightlist
+\item
+  Note during hour 7 of the summer design day that ``NORTH PERIMETER:Zone/Sys Sensible Heating Rate\href{Hourly}{W}'' is nonzero, but the heating coil is off and the DX cooling coil shows a load.~ Why?~ This report variable reports the impact of the system on the zone (not the zone's demand for heating or cooling), averaged over the hour.~ The system fan is scheduled on at 6 a.m., but the outside air dampers are closed.~ The zone is not warm enough from the night to require cooling, so the circulating fan heat warms the zone slightly for a portion of the hour until the zone temperature exceeds the cooling setpoint and the DX coil comes on for the remainder of the hour.~ If the economizer were active, this would not occur.
+\end{itemize}
+
+\subsection{Exercise 2B. Add VAV System with Reheat Serving Four Zones with Chiller and Boiler Plant}\label{exercise-2b.-add-vav-system-with-reheat-serving-four-zones-with-chiller-and-boiler-plant}
+
+Objective:~ Learn how to describe a VAV system with central plant using HVACTemplate objects.
+
+1)~~~Save Exercise2A.idf as Exercise2B.idf.
+
+2)~~~Add a \textbf{HVACTemplate:System:VAV} object.~ Retain the defaults for all fields except the following:
+
+\begin{itemize}
+\item
+  Air Handling System Name = \textless{}assign a name\textgreater{}
+\item
+  System Availability Schedule = Office HVAC (predefined)
+\item
+  Cooling Coil Design Setpoint = 13C (55.4F)
+\item
+  Minimum Outdoor Air Schedule Name = Office Minimum OA (predefined)
+\item
+  Economizer Type = FixedDryBulb
+\item
+  Return Plenum Name = PLENUM
+\end{itemize}
+
+3)~~~Add four \textbf{HVACTemplate:Zone:VAV} objects serving the four remaining zones (South Perimeter, East Perimeter, West Perimeter, and Core).~ Retain the defaults for all fields except the following:
+
+\begin{itemize}
+\item
+  Specify the same air handler name added in Step 2 (use the dropdown list)
+\item
+  Specify the same thermostat control added in Exercise 2A Step 2 (again, use the dropdown list).
+\item
+  Supply Air Minimum Flow Fraction = 0.2
+\item
+  Reheat Coil Type = Hot Water
+\item
+  Heating Damper Action = Reverse
+\item
+  HINT:~ Define one \textbf{HVACTemplate:Zone:VAV} object, make the above changes to defaults, then press ``Dup Obj'' three times to duplicate the object, then edit the remaining three zone names.
+\end{itemize}
+
+4)~~~Add a \textbf{HVACTemplate:Plant:ChilledWaterLoop} object and assign a name.~~~ Retain the defaults for all fields except the following:
+
+\begin{itemize}
+\tightlist
+\item
+  Condenser Water Temperature Control Type = Specified Setpoint
+\end{itemize}
+
+5)~~~Add a \textbf{HVACTemplate:Plant:Chiller} object, type Electric Reciprocating Chiller with a nominal COP of 3.6, water cooled.
+
+6)~~~Add a \textbf{HVACTemplate:Plant:Tower} object, type Two Speed.
+
+7)~~~Add a \textbf{HVACTemplate:Plant:HotWaterLoop} object and assign a name.~ Retain the defaults for all fields.
+
+8)~~~Add a natural gas fired hot water boiler using \textbf{HVACTemplate:Plant:Boiler}.
+
+9)~~~Run the simulation, add desired report variables, and re-run the simulation.~ Review results and compare with results from Exercise 2A:
+
+\begin{itemize}
+\item
+  Note how the heating and cooling rates for the NORTH PERIMETER zone are smaller than before.~ Why?
+\item
+  Review the SVG drawing to see the components of the VAV system and water loops.
+\item
+  Browse the expidf file in a text editor (or open in IDF Editor from File, Open, setting file type to expidf) to see the full detailed description of the HVAC systems using native EnergyPlus objects (the expanded result of the HVACTemplate preprocessor).
+\end{itemize}
+
+\subsection{Exercise 2C. Annual Simulation}\label{exercise-2c.-annual-simulation}
+
+Objective:~ Learn how to schedule report variables and create a monthly table report.
+
+1)~~~Save Exercise2B.idf as Exercise2C.idf.
+
+2)~~~Edit the \textbf{SimulationControl} object to turn off the design day simulations by setting ``Run Simulation for Sizing Periods'' to \textbf{No} and turn on the weather file (annual) simulation by setting ``Run Simulation for Weather File Run Periods'' to \textbf{Yes}..
+
+3)~~~Edit existing \textbf{Output:Variable} and \textbf{Output:Meter} objects and change the reporting frequency from Hourly to Monthly.
+
+4)~~~Locate the \textbf{Output:Variable} object for ``Zone/Sys Air Temp'' and duplicate it.~ Edit the new object and add a schedule ``Office Occupancy 2''.~ This object will report zone temperatures averaged only during occupied periods (when ``Office Occupancy 2'' is greater than zero).~ The original instance of this report variable will average the zone temperatures over all hours.
+
+5)~~~Add a new \textbf{Output:Table:Monthly} object:
+
+\begin{itemize}
+\item
+  Name = Zone Temperature Report
+\item
+  Open the rdd output file for Exercise2B in the text editor and find the following report variable names to copy and paste into the fields of the Report:Table:Monthly object in IDF Editor.~ Variable name and aggregation type are listed in pairs.
+\item
+  Zone Mean Air Temperature, SumOrAverage
+\item
+  Zone Mean Air Temperature, Maximum
+\item
+  Zone Mean Air Temperature, Minimum
+\item
+  Zone People Number of Occupants, HoursPositive
+\item
+  Zone Mean Air Temperature, SumOrAverageDuringHoursShown
+\item
+  Zone Mean Air Temperature, MaximumDuringHoursShown
+\item
+  Zone Mean Air Temperature, MinimumDuringHoursShown
+\end{itemize}
+
+6)~~~Edit \textbf{Output:Table:SummaryReports} to add the ``Equipment Summary'' report.
+
+7)~~~Select Chicago TMY2 weather file and run the simulation.
+
+8)~~~Review outputs.~ (Note the ABUPS report in the HTML file will now show a full year of results.)~ Especially review the Zone Temperatures table report in the HTML file.~ There will be a warning regarding \textbf{Output:Table:Monthly}, because there are no people in the PLENUM zone; this is normal.
+
+\subsection{Solution: Exercise 2}\label{solution-exercise-2}
+
+This is a listing of new objects added in this Exercise.
+
+\textbf{\emph{Try not to look at this section until you have completed the Exercise.}}
+
+\subsubsection{Solution: Exercise 2A}\label{solution-exercise-2a}
+
+\begin{lstlisting}
+
+HVACTemplate:Thermostat,
+      Office Thermostat,       !- Thermostat Name
+      Office Heating Setpoints,!- Thermostat Heating Setpoint Schedule
+      ,                        !- Thermostat Constant Heating Setpoint {C}
+      Office Cooling Setpoints,!- Thermostat Cooling Setpoint Schedule
+      ;                        !- Thermostat Constant Cooling Setpoint {C}
+
+
+  HVACTemplate:Zone:Unitary,
+      NORTH PERIMETER,         !- Zone Name
+      North Zone Unitary,      !- Air Handling System Name
+      Office Thermostat,       !- Thermostat Name
+      autosize,                !- Zone Supply Air Max Flow Rate {m3/s}
+      ,                        !- Zone Supply Air Sizing Factor
+      Flow/Person,             !- Zone Outside Air Method
+      0.00944,                 !- Zone Outside Air Flow Rate per Person {m3/s}
+      0.0,                     !- Zone Outside Air Flow per Zone Area {m3/s-m2}
+      0.0,                     !- Zone Outside Air Flow per Zone {m3/s}
+      ,                        !- Zone Supply Plenum Name
+      ,                        !- Zone Return Plenum Name
+      None,                    !- Baseboard Heating Type
+      ,                        !- Baseboard Heating Availability Schedule
+      autosize;                !- Baseboard Heating Capacity {W}
+
+
+  HVACTemplate:System:Unitary,
+      North Zone Unitary,      !- Air Handling System Name
+      Office HVAC,             !- System Availability Schedule
+      NORTH PERIMETER,         !- Control Zone Name or Thermostat Location
+      autosize,                !- Supply Fan Max Flow Rate {m3/s}
+      Continuous,              !- Supply Fan Operating Mode Schedule Name
+      0.7,                     !- Supply Fan Total Efficiency
+      600,                     !- Supply Fan Delta Pressure {Pa}
+      0.9,                     !- Supply Fan Motor Efficiency
+      1,                       !- Supply Fan Motor in Air Stream Fraction
+      Single-speed DX,         !- Cooling Coil Type
+      ,                        !- Cooling Coil Availability Schedule
+      autosize,                !- Cooling Coil Capacity {W}
+      autosize,                !- Cooling Coil Rated SHR
+      3,                       !- Cooling Coil Rated COP
+      Gas,                     !- Heating Coil Type
+      ,                        !- Heating Coil Availability Schedule
+      autosize,                !- Heating Coil Capacity {W}
+      0.8,                     !- Gas Heating Coil Efficiency
+      ,                        !- Gas Heating Coil Parasitic Electric Load {W}
+      autosize,                !- Maximum Outside Air Flow Rate {m3/s}
+      autosize,                !- Minimum Outside Air Flow Rate {m3/s}
+      Office Minimum OA,       !- Minimum Outside Air Schedule Name
+      NoEconomizer,            !- Economizer Type
+      NoLockout,               !- Economizer Lockout
+      ,                        !- Economizer Upper Temperature Limit {C}
+      ,                        !- Economizer Lower Temperature Limit {C}
+      ,                        !- Economizer Upper Enthalpy Limit {J/kg}
+      ,                        !- Supply Plenum Name
+      ,                        !- Return Plenum Name
+      BlowThrough,             !- Supply Fan Placement
+      StayOff,                 !- Night Cycle Control
+      ,                        !- Night Cycle Control Zone Name
+      None,                    !- Heat Recovery Type
+      0.7,                     !- Sensible Heat Recovery Effectiveness
+      0.65,                    !- Latent Heat Recovery Effectiveness
+      ,                        !- Dehumidification Control Type
+      ,                        !- Dehumidification Control Zone Name
+      ,                        !- Dehumidification Setpoint {percent}
+      ,                        !- Humidifier Type
+      ,                        !- Humidifier Availability Schedule
+      ,                        !- Humidifier Rated Capacity {m3/s}
+      ,                        !- Humidifier Rated Electric Power {W}
+      ,                        !- Humidifier Control Zone Name
+      ;                        !- Humidifier Setpoint {percent}
+
+
+  Sizing:Parameters,
+      1.2;                     !- sizing factor
+
+
+  Output:Variable,*,Furnace Fan Part-Load Ratio,hourly;
+  Output:Variable,*,DX Cooling Coil Runtime Fraction,hourly;
+  Output:Variable,*,Heating Coil Runtime Fraction,hourly;
+\end{lstlisting}
+
+\subsubsection{Solution: Exercise 2B}\label{solution-exercise-2b}
+
+\begin{lstlisting}
+
+HVACTemplate:System:VAV,
+     VAV with Reheat,         !- Air Handling System Name
+      Office HVAC,             !- System Availability Schedule
+      autosize,                !- Supply Fan Max Flow Rate {m3/s}
+      autosize,                !- Supply Fan Min Flow Rate {m3/s}
+      0.7,                     !- Supply Fan Total Efficiency
+      1000,                    !- Supply Fan Delta Pressure {Pa}
+      0.9,                     !- Supply Fan Motor Efficiency
+      1,                       !- Supply Fan Motor in Air Stream Fraction
+      ChilledWater,            !- Cooling Coil Type
+      ,                        !- Cooling Coil Availability Schedule
+      ,                        !- Cooling Coil Setpoint Schedule
+      13,                      !- Cooling Coil Design Setpoint {C}
+      None,                    !- Heating Coil Type
+      ,                        !- Heating Coil Availability Schedule
+      ,                        !- Heating Coil Setpoint Schedule
+      10.0,                    !- Heating Coil Design Setpoint {C}
+      0.8,                     !- Gas Heating Coil Efficiency
+      ,                        !- Gas Heating Coil Parasitic Electric Load {W}
+      None,                    !- Preheat Coil Type
+      ,                        !- Preheat Coil Availability Schedule
+      ,                        !- Preheat Coil Setpoint Schedule
+      7.2,                     !- Preheat Coil Design Setpoint {C}
+      0.8,                     !- Gas Preheat Coil Efficiency
+      ,                        !- Gas Preheat Coil Parasitic Electric Load {W}
+      autosize,                !- Maximum Outside Air Flow Rate {m3/s}
+      autosize,                !- Minimum Outside Air Flow Rate {m3/s}
+      ProportionalMinimum,     !- Minimum Outside Air Control Type
+      Office Minimum OA,       !- Minimum Outside Air Schedule Name
+      FixedDryBulb,            !- Economizer Type
+      NoLockout,               !- Economizer Lockout
+      ,                        !- Economizer Upper Temperature Limit {C}
+      ,                        !- Economizer Lower Temperature Limit {C}
+      ,                        !- Economizer Upper Enthalpy Limit {J/kg}
+      ,                        !- Supply Plenum Name
+      PLENUM,                  !- Return Plenum Name
+      DrawThrough,             !- Supply Fan Placement
+      InletVaneDampers,        !- Supply Fan Part-Load Power Coefficients
+      StayOff,                 !- Night Cycle Control
+      ,                        !- Night Cycle Control Zone Name
+      None,                    !- Heat Recovery Type
+      0.7,                     !- Sensible Heat Recovery Effectiveness
+      0.65,                    !- Latent Heat Recovery Effectiveness
+      None,                    !- Cooling Coil Setpoint Reset Type
+      None,                    !- Heating Coil Setpoint Reset Type
+      ,                        !- Dehumidification Control Type
+      ,                        !- Dehumidification Control Zone Name
+      ,                        !- Dehumidification Setpoint {percent}
+      ,                        !- Humidifier Type
+      ,                        !- Humidifier Availability Schedule
+      ,                        !- Humidifier Rated Capacity {m3/s}
+      ,                        !- Humidifier Rated Electric Power {W}
+      ,                        !- Humidifier Control Zone Name
+      ;                        !- Humidifier Setpoint {percent}
+
+
+  HVACTemplate:Zone:VAV,
+      SOUTH PERIMETER,         !- Zone Name
+      VAV with Reheat,         !- Air Handling System Name
+      Office Thermostat,       !- Thermostat Name
+      autosize,                !- Zone Supply Air Max Flow Rate {m3/s}
+      ,                        !- Zone Supply Air Sizing Factor
+      0.2,                     !- Zone Supply Air Min Flow Fraction
+      Flow/Person,             !- Zone Outside Air Method
+      0.00944,                 !- Zone Outside Air Flow Rate per Person {m3/s}
+      0.0,                     !- Zone Outside Air Flow per Zone Area {m3/s-m2}
+      0.0,                     !- Zone Outside Air Flow per Zone {m3/s}
+      HotWater,                !- Reheat Coil Type
+      ,                        !- Reheat Coil Availability Schedule
+      Reverse,                 !- Zone Damper Heating Action
+      ,                        !- Zone Supply Plenum Name
+      ,                        !- Zone Return Plenum Name
+      None,                    !- Baseboard Heating Type
+      ,                        !- Baseboard Heating Availability Schedule
+      autosize;                !- Baseboard Heating Capacity {W}
+
+
+  HVACTemplate:Zone:VAV,
+      EAST PERIMETER,          !- Zone Name
+      VAV with Reheat,         !- Air Handling System Name
+      Office Thermostat,       !- Thermostat Name
+      autosize,                !- Zone Supply Air Max Flow Rate {m3/s}
+      ,                        !- Zone Supply Air Sizing Factor
+      0.2,                     !- Zone Supply Air Min Flow Fraction
+      Flow/Person,             !- Zone Outside Air Method
+      0.00944,                 !- Zone Outside Air Flow Rate per Person {m3/s}
+      0.0,                     !- Zone Outside Air Flow per Zone Area {m3/s-m2}
+      0.0,                     !- Zone Outside Air Flow per Zone {m3/s}
+      HotWater,                !- Reheat Coil Type
+      ,                        !- Reheat Coil Availability Schedule
+      Reverse,                 !- Zone Damper Heating Action
+      ,                        !- Zone Supply Plenum Name
+      ,                        !- Zone Return Plenum Name
+      None,                    !- Baseboard Heating Type
+      ,                        !- Baseboard Heating Availability Schedule
+      autosize;                !- Baseboard Heating Capacity {W}
+
+
+  HVACTemplate:Zone:VAV,
+      WEST PERIMETER,          !- Zone Name
+      VAV with Reheat,         !- Air Handling System Name
+      Office Thermostat,       !- Thermostat Name
+      autosize,                !- Zone Supply Air Max Flow Rate {m3/s}
+      ,                        !- Zone Supply Air Sizing Factor
+      0.2,                     !- Zone Supply Air Min Flow Fraction
+      Flow/Person,             !- Zone Outside Air Method
+      0.00944,                 !- Zone Outside Air Flow Rate per Person {m3/s}
+      0.0,                     !- Zone Outside Air Flow per Zone Area {m3/s-m2}
+      0.0,                     !- Zone Outside Air Flow per Zone {m3/s}
+      HotWater,                !- Reheat Coil Type
+      ,                        !- Reheat Coil Availability Schedule
+      Reverse,                 !- Zone Damper Heating Action
+      ,                        !- Zone Supply Plenum Name
+      ,                        !- Zone Return Plenum Name
+      None,                    !- Baseboard Heating Type
+      ,                        !- Baseboard Heating Availability Schedule
+      autosize;                !- Baseboard Heating Capacity {W}
+
+
+  HVACTemplate:Zone:VAV,
+      CORE,                    !- Zone Name
+      VAV with Reheat,         !- Air Handling System Name
+      Office Thermostat,       !- Thermostat Name
+      autosize,                !- Zone Supply Air Max Flow Rate {m3/s}
+      ,                        !- Zone Supply Air Sizing Factor
+      0.2,                     !- Zone Supply Air Min Flow Fraction
+      Flow/Person,             !- Zone Outside Air Method
+      0.00944,                 !- Zone Outside Air Flow Rate per Person {m3/s}
+      0.0,                     !- Zone Outside Air Flow per Zone Area {m3/s-m2}
+      0.0,                     !- Zone Outside Air Flow per Zone {m3/s}
+      HotWater,                !- Reheat Coil Type
+      ,                        !- Reheat Coil Availability Schedule
+      Reverse,                 !- Zone Damper Heating Action
+      ,                        !- Zone Supply Plenum Name
+      ,                        !- Zone Return Plenum Name
+      None,                    !- Baseboard Heating Type
+      ,                        !- Baseboard Heating Availability Schedule
+      autosize;                !- Baseboard Heating Capacity {W}
+
+
+  HVACTemplate:Plant:ChilledWaterLoop,
+    Chilled Water Plant,     !- Plant Loop Name
+    ,                        !- Pump Schedule
+    Intermittent,            !- Pump Control Type
+    Default,                 !- Chiller Plant Operation Scheme Type
+    ,                        !- Chiller Plant Operation Scheme Name
+    ,                        !- Chilled Water Setpoint Schedule
+    7.22,                    !- Chilled Water Design Setpoint {C}
+    ConstantPrimaryNoSecondary,  !- Chilled Water Pump Configuration
+    179352,                  !- Primary Chilled Water Pump Rated Head {Pa}
+    179352,                  !- Secondary Chilled Water Pump Rated Head {Pa}
+    Default,                 !- Condenser Plant Operation Scheme Type
+    ,                        !- Condenser Plant Operation Scheme List Name
+    SpecifiedSetpoint,       !- Condenser Water Temperature Control Type
+    ,                        !- Condenser Water Setpoint Schedule
+    29.4,                    !- Condenser Water Design Setpoint {C}
+    179352,                  !- Condenser Water Pump Rated Head {Pa}
+    None,                    !- Chilled Water Setpoint Reset Type
+    12.2,                    !- Chilled Water Setpoint at Outdoor Dry Bulb Low {C}
+    15.6,                    !- Chilled Water Reset Outdoor Dry Bulb Low {C}
+    6.7,                     !- Chilled Water Setpoint at Outdoor Dry Bulb High {C}
+    26.7;                    !- Chilled Water Reset Outdoor Dry Bulb High {C}
+
+
+  HVACTemplate:Plant:Chiller,
+      Chiller 1,               !- Chiller Name
+      ElectricReciprocatingChiller,  !- Chiller Type
+      autosize,                !- Capacity {W}
+      3.6,                     !- COP {W/W}
+      WaterCooled,             !- Condenser Type
+      ;                        !- Priority
+
+
+  HVACTemplate:Plant:Tower,
+      Tower 1,                 !- Tower Name
+      TwoSpeed,                !- Tower Type
+      autosize,                !- High-Speed Nominal Capacity {W}
+      autosize,                !- High-Speed Fan Power {W}
+      autosize,                !- Low-Speed Nominal Capacity {W}
+      autosize,                !- Low-Speed Fan Power {W}
+      autosize,                !- Free Convection Capacity {W}
+      ;                        !- Priority
+
+
+  HVACTemplate:Plant:HotWaterLoop,
+    Hot Water Plant,         !- Plant Loop Name
+    ,                        !- Pump Schedule
+    Intermittent,            !- Pump Control Type
+    Default,                 !- Hot Water Plant Operation Scheme Type
+    ,                        !- Hot Water Plant Operation Scheme List Name
+    ,                        !- Hot Water Setpoint Schedule
+    82,                      !- Hot Water Design Setpoint {C}
+    ConstantFlow,            !- Hot Water Pump Configuration
+    179352,                  !- Hot Water Pump Rated Head {Pa}
+    None,                    !- Hot Water Setpoint Reset Type
+    82.2,                    !- Hot Water Setpoint at Outdoor Dry Bulb Low {C}
+    -6.7,                    !- Hot Water Reset Outdoor Dry Bulb Low {C}
+    65.6,                    !- Hot Water Setpoint at Outdoor Dry Bulb High {C}
+    10;                      !- Hot Water Reset Outdoor Dry Bulb High {C}
+
+
+  HVACTemplate:Plant:Boiler,
+    Boiler 1,                !- Boiler Name
+    HotWaterBoiler,          !- Boiler Type
+    autosize,                !- Capacity {W}
+    0.8,                     !- Efficiency
+    NaturalGas,              !- Fuel Type
+    ;                        !- Priority
+
+
+  Output:Variable,*,Damper Position,hourly;
+  Output:Variable,*,Chiller Evap Heat Trans Rate,hourly;
+  Output:Variable,*,Chiller COP,hourly;
+  Output:Variable,*,Boiler Heating Output Rate,hourly;
+  Output:Variable,*,Tower Heat Transfer,hourly;
+\end{lstlisting}
+
+\subsubsection{Exercise 2C}\label{exercise-2c}
+
+\begin{lstlisting}
+
+Output:Variable,*,Zone/Sys Air Temperature,monthly,Office Occupancy 2;
+
+
+  Output:Table:Monthly,
+      Zone Temperature Report, !- Name
+      2,                       !- DigitsAfterDecimal
+      Zone Mean Air Temperature,  !- VariableOrMeterName01
+      SumOrAverage,            !- AggregationType01
+      Zone Mean Air Temperature,  !- VariableOrMeterName02
+      Maximum,                 !- AggregationType02
+      Zone Mean Air Temperature,  !- VariableOrMeterName03
+      Minimum,                 !- AggregationType03
+      Zone People Number of Occupants,  !- VariableOrMeterName04
+      HoursPositive,           !- AggregationType04
+      Zone Mean Air Temperature,  !- VariableOrMeterName05
+      SumOrAverageDuringHoursShown,  !- AggregationType05
+      Zone Mean Air Temperature,  !- VariableOrMeterName06
+      MaximumDuringHoursShown, !- AggregationType06
+      Zone Mean Air Temperature,  !- VariableOrMeterName07
+      MinimumDuringHoursShown; !- AggregationType07
+\end{lstlisting}
diff --git a/doc/getting-started/src/tutorial-exercise-2/unitary-system-and-vav-using-hvactemplate.tex b/doc/getting-started/src/tutorial-exercise-2/unitary-system-and-vav-using-hvactemplate.tex
new file mode 100644
index 00000000000..bfe8c1f95be
--- /dev/null
+++ b/doc/getting-started/src/tutorial-exercise-2/unitary-system-and-vav-using-hvactemplate.tex
@@ -0,0 +1,89 @@
+\section{Unitary System and VAV using HVACTemplate Inputs}\label{unitary-system-and-vav-using-hvactemplate-inputs}
+
+\subsection{Overview}\label{overview-000}
+
+\begin{itemize}
+\item
+  Rectangular single story building with 5 occupied zones and a ceiling plenum
+\item
+  Packaged DX cooling with gas heat serving one zone
+\item
+  VAV with reheat and return plenum serving the other 4 zones
+\item
+  All equipment autosized using summer and winter design days
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 20
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image020.png}
+\caption{Schematic for Exercise 2. \protect \label{fig:schematic-for-exercise-2.}}
+\end{figure}
+
+\subsection{Details of the Exercise}\label{details-of-the-exercise-000}
+
+\subsubsection{Building Description}\label{building-description}
+
+\begin{itemize}
+\item
+  Single floor rectangular building 30.5 m (100 ft) by 15.2 m (50 ft) by 3m (10 ft) high.
+\item
+  Building is oriented with the long axis running east-west.
+\item
+  Floor Area 463.6 m2 (5000 ft2).
+\item
+  5 occupied zones - 4 exterior, 1 interior, zone height 2.4 m (8 ft). Exterior zone depth is 3.7 m (12 ft).
+\item
+  1 plenum zone 0.6 m (2 ft) high.
+\item
+  Windows on all 4 facades
+\item
+  South and north facades have glass doors.
+\item
+  South facing glass is shaded by overhangs.
+\item
+  Walls are wood shingle over plywood, insulation, and gypsum board.
+\item
+  Roof is gravel built up roof with mineral board insulation and plywood sheathing.
+\item
+  Floor slab is 0.1 m (4 in) heavy concrete.
+\item
+  Windows and glass doors are double pane Low-e clear glass with argon gap.
+\item
+  Window to wall ratio is approximately 0.3.
+\item
+  Lighting is 16 W/m2 (1.5 W/ft2).
+\item
+  Office electric equipment is 10.8 W/m2 (1.0 W/ft2).
+\item
+  1 occupant per 9.3 m2 (100 ft2) of floor area.
+\item
+  Infiltration is 0.25 air changes per hour (always on, proportional to wind speed).
+\item
+  * Refers to specific glass type included in the EnergyPlus datasets directory
+\item
+  ~~~~~~~~~~~ (WindowGlassMaterials.idf)
+\end{itemize}
+
+\subsubsection{Space Conditioning}\label{space-conditioning}
+
+\begin{itemize}
+\item
+  Heating setpoints:~~ 21.1C (70F) occupied, 12.8C (55F) unoccupied
+\item
+  Cooling setpoints:~~ 23.9C (75F) occupied, 40.0C (104F, system off) unoccupied
+\item
+  Plenum zone not controlled
+\end{itemize}
+
+\subsubsection{Environment}\label{environment}
+
+\begin{itemize}
+\item
+  Location:~~~~~~~~~~~~~~~~~~ Chicago, Illinois, USA
+\item
+  Design Days:~~~~~~~~~~~~ Summer, Winter
+\item
+  Annual Simulation Period:~~~ Jan 1 -- Dec 31
+\item
+  Ground Temperatures:~~~~~~~~ from Slab preprocessor (20.4 to 23.0 C)
+\end{itemize}
diff --git a/doc/header.tex b/doc/header.tex
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+++ b/doc/header.tex
@@ -0,0 +1,86 @@
+\documentclass[12pt,twoside,letterpaper,titlepage]{report}
+
+\usepackage{amssymb,amsmath}
+\usepackage{mathspec}
+\defaultfontfeatures{Ligatures=TeX,Scale=MatchLowercase}
+\usepackage[margin=1.0in]{geometry}
+% fixltx2e has been merged into LaTeX2e proper
+% see: https://latex-project.org/ltnews/ltnews22.pdf
+% \usepackage{fixltx2e}
+\usepackage{graphicx,grffile}
+\makeatletter
+\def\maxwidth{\ifdim\Gin@nat@width>\linewidth\linewidth\else\Gin@nat@width\fi}
+\def\maxheight{\ifdim\Gin@nat@height>\textheight\textheight\else\Gin@nat@height\fi}
+\makeatother
+% Scale images if necessary, so that they will not overflow the page
+% margins by default, and it is still possible to overwrite the defaults
+% using explicit options in \includegraphics[width, height, ...]{}
+\setkeys{Gin}{width=\maxwidth,height=\maxheight,keepaspectratio}
+\usepackage[table,svgnames]{xcolor}
+\usepackage{framed}
+\usepackage{longtable,booktabs}
+\usepackage{listings}
+\PassOptionsToPackage{hyphens}{url}\usepackage[breaklinks=true]{hyperref}
+
+% Background Color for Note/Admonition Boxes
+\definecolor{shadecolor}{rgb}{0.9,0.9,0.9}
+
+% Band the Color of Rows in Tables
+% unfortunately, doesn't seem to work across the board. Turning off for now
+%\rowcolors{1}{white}{lightgray!25!white}
+
+\newenvironment{callout}{\begin{shaded*}\small}{\end{shaded*}}
+\newcommand{\warning}[1]{\small{\textbf{\textcolor[rgb]{0.8,0.2,0.2}{#1}}}}
+
+% Font Settings
+%\setmainfont[]{Calibri}
+%\setmonofont[Mapping=tex-ansi]{Inconsolata}
+%\usepackage{newtxtext,newtxmath}
+
+% The depth of numbering for sections
+\setcounter{secnumdepth}{4}
+
+% Listing Settings
+\lstset{
+  backgroundcolor=\color{BlanchedAlmond!20!white},
+  basicstyle=\ttfamily\scriptsize,
+  breakatwhitespace=false,
+  breaklines=true,
+  frame=bottomline,
+  keepspaces=true,
+}
+
+% Provide better table spacing
+% From https://www.inf.ethz.ch/personal/markusp/teaching/guides/guide-tables.pdf
+\renewcommand{\arraystretch}{1.2} 
+
+\graphicspath{{media/}}
+
+\pagestyle{headings}
+
+% Define custom commands from Pandoc
+\setlength{\emergencystretch}{3em}  % prevent overfull lines
+\providecommand{\tightlist}{%
+  \setlength{\itemsep}{0pt}\setlength{\parskip}{0pt}}
+
+% Redefine (sub)paragraphs to behave more like sections
+\ifx\paragraph\undefined\else
+\let\oldparagraph\paragraph
+\renewcommand{\paragraph}[1]{\oldparagraph{#1}\mbox{}}
+\fi
+\ifx\subparagraph\undefined\else
+\let\oldsubparagraph\subparagraph
+\renewcommand{\subparagraph}[1]{\oldsubparagraph{#1}\mbox{}}
+\fi
+
+% this is a great package for printing units in a standard way, we should move this way
+\usepackage{siunitx}
+
+% some additional macros
+\newcommand{\PB}[1]{\left(#1\right)}
+\newcommand{\RB}[1]{\left[#1\right]}
+\newcommand{\CB}[1]{\left\{#1\right\}}
+\newcommand{\bracketunits}[1]{\RB{\si[per-mode=fraction]{#1}}}
+
+\author{U.S. Department of Energy}
+\date{March 31, 2016}
diff --git a/doc/index.html b/doc/index.html
deleted file mode 100644
index 4a69cf7735f..00000000000
--- a/doc/index.html
+++ /dev/null
@@ -1,12 +0,0 @@
-<!DOCTYPE html PUBLIC "-//W3C//DTD HTML 4.0 Transitional//EN">
-<html>
-<head>
-  <title>EnergyPlus Documentation</title>
-</head>
-<body>
-  <p>
-EnergyPlus documentation is available online at the <a href=http://energyplus.net/documentation>EnergyPlus website</a>.
-  </p>
-</body>
-</html>
-
diff --git a/doc/input-output-reference/CMakeLists.txt b/doc/input-output-reference/CMakeLists.txt
new file mode 100644
index 00000000000..219ba9dfb8a
--- /dev/null
+++ b/doc/input-output-reference/CMakeLists.txt
@@ -0,0 +1,322 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/input-output-reference.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/title.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/hvac-template-objects.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/parametric-objects.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/input-for-output.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/output.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/standard-output-reports.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/weather-data.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/running-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/appendix-a-units-and-abbreviations.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/appendix-a-units-and-abbreviations/standard-energyplus-conditions.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/appendix-a-units-and-abbreviations/standard-energyplus-units.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/group-economics.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/introduction-to-economics.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/conceptual-framework-variables-and-hierarchy.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/utilitycost-qualify.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/utilitycost-charge-simple.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/utilitycost-charge-block.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/utilitycost-ratchet.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/utilitycost-variable.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/utilitycost-computation.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff-examples.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff-reporting.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/economic-results-summary-report.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/complex-tariff-modeling.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/cost-estimating.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/life-cycle-costing.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/lifecyclecost-parameters.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/lifecyclecost-recurringcosts.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/lifecyclecost-nonrecurringcost.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/lifecyclecost-usepriceescalation.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/energyplus-economics/lifecyclecost-useadjustment.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/hvac-template-objects/hvactemplate-processing.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/hvac-template-objects/group-hvac-templates.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/output/using-readvarseso.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/what-s-different-about-energyplus-input.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/idd-conventions.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/input-output-descriptions.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-simulation-parameters.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-compliance-objects.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-location-climate-weather-file-access.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-schedules.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-surface-construction-elements.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-thermal-zone-description-geometry.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-advanced-surface-concepts.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-detailed-ground-heat-transfer.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-room-air-models.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-internal-gains-people-lights-other.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-daylighting.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-exterior-energy-use-equipment.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-airflow.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-design-objects.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/hvac-primary-and-secondary-systems.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-node-branch-management.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-plant-condenser-loops.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-plant-condenser-control.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-plant-equipment.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-water-heaters.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-condenser-equipment.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-plant-condenser-flow-control.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-air-distribution.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-airflow-network.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-zone-equipment.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-air-distribution-equipment.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-zone-forced-air-units.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-unitary-equipment.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-variable-refrigerant-flow-equipment.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-radiative-convective-units.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-refrigeration.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-zone-controls-thermostats.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-air-path.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-non-zone-equipment.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-solar-collectors.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-pumps.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-heating-and-cooling-coils.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-fans.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-humidifiers.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-desiccant-dehumidifiers.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-energy-management-system-ems.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-externalinterface.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-user-defined-hvac-and-plant-component.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-system-availability-managers.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-setpoint-managers.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-controllers.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-evaporative-coolers.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-heat-recovery.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-demand-limiting-controls.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-electric-load-center-generator.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-water-systems.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-operational-faults.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-performance-curves.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-performance-tables.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/overview/group-fluid-properties.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/running-energyplus/energy-ini.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/running-energyplus/errors.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/running-energyplus/energyplus-execution-time.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/standard-output-reports/output-table-timebins.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/standard-output-reports/output-table-monthly.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/standard-output-reports/output-table-annual.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/standard-output-reports/output-table-summaryreports.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/standard-output-reports/outputcontrol-table-style.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/../title.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/weather-data/missing-weather-file-data.tex
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/src/weather-data/weather-data-hourly-interpolation.tex
+  ${CMAKE_SOURCE_DIR}/doc/title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/ACBussDiagram.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/ACStorageBussDiagram.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/AirLoopComponentMatrix.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/DCInverterBussDiagram.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/DCInverterWithACStorageBussDiagram.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/DCInverterWithDCStorageBussDiagram.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/ElectPowerServiceOverview.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/OASysComponentMatrix.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/ZoneComponentMatrix.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/calculation-of-dtop-for-a-shading-device-collage.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/three-cases-for-the-dtop-calculation-for-an-indoor-outdoor-shade-collage.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image001.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image002.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image003.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image004.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image005.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image010.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image012.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image013.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image020.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image024.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image025.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image029.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image033.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image034.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image035.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image041.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image042.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image043.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image044.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image045.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image046.svg
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image047.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image048.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image050.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image051.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image052.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image053.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image054.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image055.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image056.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image057.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image058.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image059.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image060.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image061.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image062.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image063.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image064.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image065.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image066.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image069.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image070.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image078.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image079.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image080.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image081.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image082.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image083.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image084.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image085.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image087.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image095.png
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+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image097.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image098.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image099.png
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+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image101.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image102.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image103.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image104.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image105.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image106.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image107.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image108.png
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+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image263.png
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+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image265.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image267.png
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+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image269.png
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+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image289.svg
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+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image292.png
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+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image298.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image299.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image300.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image301.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image302.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image303.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image304.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image305.svg
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image306.svg
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image307.svg
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image308.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image309.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image310.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image311.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image312.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image313.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image321.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image322.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image337.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image338.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image339.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image340.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image341.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image349.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image353.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image354.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image368.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image369.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image370.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image409.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image410.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image414.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image415.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image416.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image419.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image420.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image421.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image422.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image423.svg
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image424.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image467.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image579.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image603.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image604.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image605.svg
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image606.svg
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image607.svg
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image608.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image609.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image611.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image612.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image613.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image614.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image615.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image616.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image900.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image901.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image902.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image903.png
+  ${CMAKE_SOURCE_DIR}/doc/input-output-reference/media/image904.png
+) 
+
+SET( SOURCE_FILENAME "input-output-reference" )
+SET( OUTPUT_FILENAME "InputOutputReference" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/input-output-reference/input-output-reference.tex b/doc/input-output-reference/input-output-reference.tex
new file mode 100644
index 00000000000..e2dfa71f63a
--- /dev/null
+++ b/doc/input-output-reference/input-output-reference.tex
@@ -0,0 +1,39 @@
+\input{../header}
+
+\title{Input Output Reference}
+
+\hypersetup{unicode=true,
+            pdftitle={Input Output Reference},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+\input{src/title}
+
+\input{src/overview}
+
+\input{src/hvac-template-objects}
+
+\input{src/energyplus-economics}
+
+\input{src/parametric-objects}
+
+\input{src/input-for-output}
+
+\input{src/output}
+
+\input{src/standard-output-reports}
+
+\input{src/weather-data}
+
+\input{src/running-energyplus}
+
+\input{src/appendix-a-units-and-abbreviations}
+
+\end{document}
diff --git a/doc/src/docs/InputOutputReference/media/ACBussDiagram.png b/doc/input-output-reference/media/ACBussDiagram.png
similarity index 100%
rename from doc/src/docs/InputOutputReference/media/ACBussDiagram.png
rename to doc/input-output-reference/media/ACBussDiagram.png
diff --git a/doc/src/docs/InputOutputReference/media/ACStorageBussDiagram.png b/doc/input-output-reference/media/ACStorageBussDiagram.png
similarity index 100%
rename from doc/src/docs/InputOutputReference/media/ACStorageBussDiagram.png
rename to doc/input-output-reference/media/ACStorageBussDiagram.png
diff --git a/doc/src/docs/InputOutputReference/media/AirLoopComponentMatrix.png b/doc/input-output-reference/media/AirLoopComponentMatrix.png
similarity index 100%
rename from doc/src/docs/InputOutputReference/media/AirLoopComponentMatrix.png
rename to doc/input-output-reference/media/AirLoopComponentMatrix.png
diff --git a/doc/src/docs/InputOutputReference/media/DCInverterBussDiagram.png b/doc/input-output-reference/media/DCInverterBussDiagram.png
similarity index 100%
rename from doc/src/docs/InputOutputReference/media/DCInverterBussDiagram.png
rename to doc/input-output-reference/media/DCInverterBussDiagram.png
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similarity index 100%
rename from doc/src/docs/InputOutputReference/media/DCInverterWithACStorageBussDiagram.png
rename to doc/input-output-reference/media/DCInverterWithACStorageBussDiagram.png
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similarity index 100%
rename from doc/src/docs/InputOutputReference/media/DCInverterWithDCStorageBussDiagram.png
rename to doc/input-output-reference/media/DCInverterWithDCStorageBussDiagram.png
diff --git a/doc/src/docs/InputOutputReference/media/ElectPowerServiceOverview.png b/doc/input-output-reference/media/ElectPowerServiceOverview.png
similarity index 100%
rename from doc/src/docs/InputOutputReference/media/ElectPowerServiceOverview.png
rename to doc/input-output-reference/media/ElectPowerServiceOverview.png
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rename from doc/src/docs/InputOutputReference/media/OASysComponentMatrix.png
rename to doc/input-output-reference/media/OASysComponentMatrix.png
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similarity index 100%
rename from doc/src/docs/InputOutputReference/media/ZoneComponentMatrix.png
rename to doc/input-output-reference/media/ZoneComponentMatrix.png
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rename to doc/input-output-reference/media/ep.gif
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diff --git a/doc/input-output-reference/src/appendix-a-units-and-abbreviations.tex b/doc/input-output-reference/src/appendix-a-units-and-abbreviations.tex
new file mode 100644
index 00000000000..41629cd4a89
--- /dev/null
+++ b/doc/input-output-reference/src/appendix-a-units-and-abbreviations.tex
@@ -0,0 +1,5 @@
+\chapter{Appendix A. Units and Abbreviations}\label{appendix-a.-units-and-abbreviations}
+
+\input{src/appendix-a-units-and-abbreviations/standard-energyplus-conditions}
+
+\input{src/appendix-a-units-and-abbreviations/standard-energyplus-units}
diff --git a/doc/input-output-reference/src/appendix-a-units-and-abbreviations/standard-energyplus-conditions.tex b/doc/input-output-reference/src/appendix-a-units-and-abbreviations/standard-energyplus-conditions.tex
new file mode 100644
index 00000000000..25442f11892
--- /dev/null
+++ b/doc/input-output-reference/src/appendix-a-units-and-abbreviations/standard-energyplus-conditions.tex
@@ -0,0 +1,15 @@
+\section{Standard EnergyPlus Conditions}\label{standard-energyplus-conditions}
+
+\subsection{Standard Temperature and Pressure}\label{standard-temperature-and-pressure}
+
+Several objects specify inputs at ``standard temperature and pressure''. Standard Temperature~ is dry air at 20\(^{o}\) C drybulb. The program uses local barometric pressure to account for altitude using the equation for ``standard atmospheric'' pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
+
+\begin{equation}
+Stdpressure = 101325\cdot {\left( {1.0 - Z\cdot {{2.25577}^{ - 5}}} \right)^{5.2559}}
+\end{equation}
+
+where
+
+StdPressure = pressure \{Pa\}
+
+Z = altitude/elevation \{m\}
diff --git a/doc/input-output-reference/src/appendix-a-units-and-abbreviations/standard-energyplus-units.tex b/doc/input-output-reference/src/appendix-a-units-and-abbreviations/standard-energyplus-units.tex
new file mode 100644
index 00000000000..a047dfdc83e
--- /dev/null
+++ b/doc/input-output-reference/src/appendix-a-units-and-abbreviations/standard-energyplus-units.tex
@@ -0,0 +1,61 @@
+\section{Standard EnergyPlus Units}\label{standard-energyplus-units}
+
+EnergyPlus expects information in a single unit system (SI). This requires interface developers to convert user inputs from those preferred by architects and engineers into the standard metric units of EnergyPlus. EnergyPlus will not perform any units conversions and will not have any unit conversion routines.
+
+ASCII with no spaces is used for abbreviations. Note that exponents appear without any indication of exponentiation: i.e., kg/m3 not kg/m\^{}3 or kg/m**3. Also note the use of dashes. We have W/m2-K not W/m2*K or W/(m2*K).
+
+At the end we note the ``problem'' variables -- the inputs that have non-standard units. Inputs using these units will have to be changed and the code checked to see how the quantities are used internally.
+
+\begin{longtable}[c]{p{1.59in}p{2.9in}p{1.5in}}
+\caption{Standard EnergyPlus Units \label{table:standard-energyplus-units}} \tabularnewline
+\toprule 
+Quantity & unit & abbreviation \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Standard EnergyPlus Units} \tabularnewline
+\toprule 
+Quantity & unit & abbreviation \tabularnewline
+\midrule
+\endhead
+
+angular degrees & degree & deg \tabularnewline
+Length & meter & m \tabularnewline
+Area & square meter & m2 \tabularnewline
+Volume & cubic meter & m3 \tabularnewline
+Time & seconds & s \tabularnewline
+Frequency & Hertz & Hz \tabularnewline
+Temperature & Celsius & C \tabularnewline
+absolute temperature & Kelvin & K \tabularnewline
+temperature difference & Kelvin & deltaC \tabularnewline
+speed & meters per second & m/s \tabularnewline
+energy (or work) & Joules & J \tabularnewline
+power & Watts & W \tabularnewline
+mass & kilograms & kg \tabularnewline
+force & Newton & N \tabularnewline
+mass flow & kilograms per second & kg/s \tabularnewline
+volume flow & cubic meters per second & m3/s \tabularnewline
+pressure & Pascals & Pa \tabularnewline
+pressure difference & Pascals & Pa \tabularnewline
+specific enthalpy & Joules per kilogram & J/kg \tabularnewline
+density & kilograms per cubic meter & kg/m3 \tabularnewline
+heat flux & watts per square meter & W/m2 \tabularnewline
+specific heat & ------- & J/kg-K \tabularnewline
+conductivity & ------- & W/m-K \tabularnewline
+diffusivity & ------- & m2/s \tabularnewline
+heat transfer coefficient & ------- & W/m2-K \tabularnewline
+R-value & ------- & m2-K/W \tabularnewline
+heating or cooling capacity & Watts & W \tabularnewline
+electric potential & volts & V \tabularnewline
+electric current & Amperes & A \tabularnewline
+illuminace & lux & lx \tabularnewline
+luminous flux & lumen & lm \tabularnewline
+luminous intensity & candelas & cd \tabularnewline
+luminance & candelas per square meter & cd/m2 \tabularnewline
+vapor diffusivity & meters squared per second & m2/s \tabularnewline
+viscosity & ------- & kg/m-s \tabularnewline
+dynamic Viscosity & ------- & N-s/m2 \tabularnewline
+thermal gradient coeff for moisture capacity & ------- & kg/kg-K \tabularnewline
+isothermal moisture capacity & ------- & m3/kg \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/input-output-reference/src/energyplus-economics.tex b/doc/input-output-reference/src/energyplus-economics.tex
new file mode 100644
index 00000000000..c8a0e45ea91
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics.tex
@@ -0,0 +1,43 @@
+\chapter{EnergyPlus Economics}\label{energyplus-economics}
+
+\input{src/energyplus-economics/group-economics}
+
+\input{src/energyplus-economics/introduction-to-economics}
+
+\input{src/energyplus-economics/conceptual-framework-variables-and-hierarchy}
+
+\input{src/energyplus-economics/utilitycost-tariff}
+
+\input{src/energyplus-economics/utilitycost-qualify}
+
+\input{src/energyplus-economics/utilitycost-charge-simple}
+
+\input{src/energyplus-economics/utilitycost-charge-block}
+
+\input{src/energyplus-economics/utilitycost-ratchet}
+
+\input{src/energyplus-economics/utilitycost-variable}
+
+\input{src/energyplus-economics/utilitycost-computation}
+
+\input{src/energyplus-economics/utilitycost-tariff-examples}
+
+\input{src/energyplus-economics/utilitycost-tariff-reporting}
+
+\input{src/energyplus-economics/economic-results-summary-report}
+
+\input{src/energyplus-economics/complex-tariff-modeling}
+
+\input{src/energyplus-economics/cost-estimating}
+
+\input{src/energyplus-economics/life-cycle-costing}
+
+\input{src/energyplus-economics/lifecyclecost-parameters}
+
+\input{src/energyplus-economics/lifecyclecost-recurringcosts}
+
+\input{src/energyplus-economics/lifecyclecost-nonrecurringcost}
+
+\input{src/energyplus-economics/lifecyclecost-usepriceescalation}
+
+\input{src/energyplus-economics/lifecyclecost-useadjustment}
diff --git a/doc/input-output-reference/src/energyplus-economics/complex-tariff-modeling.tex b/doc/input-output-reference/src/energyplus-economics/complex-tariff-modeling.tex
new file mode 100644
index 00000000000..53458404884
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/complex-tariff-modeling.tex
@@ -0,0 +1,182 @@
+\section{Complex Tariff Modeling}\label{complex-tariff-modeling}
+
+Much can be accomplished with the UtilityCost:Charge:Simple and UtilityCost:Charge:Block objects. In almost all cases, these structures are flexible enough to model the tariff. At times the built in approach is not sufficient to model a particular rate. In those cases, the rate may be modeled by using the UtilityCost:Computation object. For most rates this object can be omitted but for difficult to model rates, they may be used to modify the normal way the rate computation is performed.
+
+Each ComputeStep is performed in order and can be either a variable followed by an expression or simply a variable.
+
+\begin{itemize}
+\item
+  demandMod SUM demand1 demand2
+\item
+  chargeSummer1
+\end{itemize}
+
+The normal calculations associated with the UtilityCost:Qualify, UtilityCost:Charge:Simple, UtilityCost:Charge:Block, or UtilityCost:Ratchet are performed the first time that object is called. Subsequent times are not recomputed but use the value stored in the appropriate variable. The result of the computation for those objects is available in the expression for further computation. The expressions allow the manipulation of variables directly using simple mathematical functions. Only variable names may be entered along with operators. Numbers may not be entered and should be entered with UtilityCost:Variable. Multiple operators are allowed per step. Variables names do not include spaces. If spaces are found in a variable name then an error is shown. Unused variables are flagged with a warning. All expressions are in the form:
+
+\begin{itemize}
+\tightlist
+\item
+  assignedToVariable OPERATOR variable1 variable2
+\end{itemize}
+
+Each step is performed for each of the months before the next step is taken. The same operation is performed for each step as specified.
+
+The actual evaluation of the expression is performed from the end of the line to the beginning using stack based operations. Some operators pull all values from the stack (SUM, MAXIMUM, MINIMUM) while most use just one or two values from the stack. All operations return a single value to the stack. This stack based approach to expressions is sometimes called Polish Notation. While multiple operators are allowed per line, it reduces confusion if each line has only a single operator.
+
+When the UtilityCost:Computation object is used, it must contain references to all objects involved in the rate in the order that they should be computed. No checking is performed for objects that should or should not be included; instead, the computational process is driven completely by the input of this object.
+
+A typical rate will have a simple series of steps. For example F the following steps would be created automatically by the software:
+
+\begin{lstlisting}
+
+UtilityCost:Computation,
+    SpecialStepsForF,             !- Name
+    ExampleF,                     !- Tariff Name
+    EnergyCharges SUM SummerOnPeak SummerOffPeak WinterOnPeak WinterOffPeak, Compute Step 1
+    Basis SUM EnergyCharges DemandCharges ServiceCharges, Compute Step 2
+    SubTotal SUM Basis Adjustments Surcharges, Compute Step 3
+    Total SUM SubTotal Taxes, Compute Step 4
+    MinDemand; Compute Step 5
+\end{lstlisting}
+
+This example does not have any dependency of different charges that are summed on the same line but if it did the charges could appear by themselves on lines and this would indicate the order that they should be computed. Here is the same example again showing that form.
+
+\begin{lstlisting}
+
+UtilityCost:Computation,
+    SpecialStepsForF,            !- Name
+    ExampleF,                    !- Tariff Name
+    SummerOnPeak,                !- Compute Step 1
+    SummerOffPeak,               !- Compute Step 2
+    WinterOnPeak,                !- Compute Step 3
+    WinterOffPeak,               !- Compute Step 4
+    EnergyCharges SUM SummerOnPeak SummerOffPeak WinterOnPeak WinterOffPeak,  !- Compute Step 5
+    Basis SUM EnergyCharges DemandCharges ServiceCharges,                     !- Compute Step 6
+    SubTotal SUM Basis Adjustments Surcharges,   !- Compute Step 7
+    Total SUM SubTotal Taxes,                    !- Compute Step 8
+    MinDemand;                   !- Compute Step 9
+\end{lstlisting}
+
+This second expanded format is generated automatically when no UtilityCost:Computation object is provided.
+
+The functions built in are (number of arguments in parentheses):
+
+\subsubsection{Operator:~~ SUM (unlimited)}\label{operator-sum-unlimited}
+
+Adds together all of the variable values for each month for as many variables that are used.
+
+\subsubsection{Operator:~~ ADD (2)}\label{operator-add-2}
+
+Adds together the first variable value with the second variable value.
+
+\subsubsection{Operator:~~ MULTIPLY (2)}\label{operator-multiply-2}
+
+Multiplies the first variable value with the second variable value. MULT may also be used.
+
+\subsubsection{Operator:~ SUBTRACT (2)}\label{operator-subtract-2}
+
+Subtracts the second variable value from the first variable value. SUBT may also be used.
+
+\subsubsection{Operator:~ DIVIDE (2)}\label{operator-divide-2}
+
+Divides the first variable value by the second variable value. DIV may also be used.
+
+\subsubsection{Operator:~ ABSOLUTE (1)}\label{operator-absolute-1}
+
+Takes the absolute value of the variable value. This turns negative values into positive ones. ABS may also be used.
+
+\subsubsection{Operator:~ INTEGER (1)}\label{operator-integer-1}
+
+Removes non-integer portions of the variable values. INT may also be used.
+
+\subsubsection{Operator:~ SIGN (1)}\label{operator-sign-1}
+
+Returns a 1 for positive values, -1 for negative values and 0 for zero values.
+
+\subsubsection{Operator:~ MAXIMUM (unlimited)}\label{operator-maximum-unlimited}
+
+Selects the maximum value across variables for each of the months. Two or more variables may be used. MAX may also be used.
+
+\subsubsection{Operator:~ MINIMUM (unlimited)}\label{operator-minimum-unlimited}
+
+Selects the minimum value across variables for each of the months. Two or more variables may be used. MIN may also be used.
+
+\subsubsection{Operator:~ EXCEEDS (2)}\label{operator-exceeds-2}
+
+Returns the difference between the first and second variable if the first variable is greater than the second. If the second variable is greater or equal to the first variable returns a zero.
+
+\subsubsection{Operator:~ ANNUALMINIMUM (1)}\label{operator-annualminimum-1}
+
+Returns the minimum value of the twelve months in the variable. Zero values are ignored (see also ANNUALMINZERO). If all values are zero then zero is returned. ANMIN may also be used.
+
+\subsubsection{Operator:~ ANNUALMAXIMUM (1)}\label{operator-annualmaximum-1}
+
+Returns the maximum value of the twelve months in the variable. Zero values are ignored (see also ANNUALMAXZERO). If all values are zero then zero is returned. ANMAX may also be used.
+
+\subsubsection{Operator:~ ANNUALSUM (1)}\label{operator-annualsum-1}
+
+Returns the sum of the twelve months in the variable. ANSUM may also be used.
+
+\subsubsection{Operator:~ ANNUALAVERAGE (1)}\label{operator-annualaverage-1}
+
+Returns the sum of the twelve monthly values divided by the number of non-zero monthly values. If all values are zero than zero is returned. If an average is desired that includes zero valued elements the SUM() function should be used divided by 12. ANAVG may also be used.
+
+\subsubsection{Operator:~ ANNUALOR (1)}\label{operator-annualor-1}
+
+Returns 1 for all monthly values if any of the monthly values are non-zero. ANOR may also be used.
+
+\subsubsection{Operator:~ ANNUALAND (1)}\label{operator-annualand-1}
+
+Returns 1 for all monthly values if all of the monthly values are non-zero. ANAND may also be used.
+
+\subsubsection{Operator:~ ANNUALMAXIMUMZERO (1)}\label{operator-annualmaximumzero-1}
+
+Returns the maximum value of the twelve monthly values in x. Zeros are counted so if a zero is the largest value (the rest would be negative) a zero may be returned. ANMAXZ may also be used.
+
+\subsubsection{Operator:~ ANNUALMINIMUMZERO (1)}\label{operator-annualminimumzero-1}
+
+Returns the minimum value of the twelve monthly values in x. Zeros are counted. ANMINZ may also be used.
+
+\subsubsection{Operator:~ IF (3)}\label{operator-if-3}
+
+Returns the value of the second variable if the first variable is non-zero otherwise returns the value of the third variable. Usually used with GT, GE, LT, LE, EQ, NE operators.
+
+\subsubsection{Operator:~ GREATERTHAN (2)}\label{operator-greaterthan-2}
+
+1 if the first variable value is greater than the second variable value otherwise 0. GT may also be used.
+
+\subsubsection{Operator:~ GREATEREQUAL (2)}\label{operator-greaterequal-2}
+
+1 if the first variable value is greater than or equal to the second variable value otherwise 0. GE may also be used.
+
+\subsubsection{Operator:~ LESSTHAN (2)}\label{operator-lessthan-2}
+
+1 if the first variable value is less than the second variable value otherwise 0. LT may also be used.
+
+\subsubsection{Operator:~ LESSEQUAL (2)}\label{operator-lessequal-2}
+
+1 if the first variable value is less than or equal to the second variable value otherwise 0. LE may also be used.
+
+\subsubsection{Operator:~ EQUAL (2)}\label{operator-equal-2}
+
+1 if the first variable value is equal to the second variable value otherwise 0. EQ may also be used.
+
+\subsubsection{Operator:~ NOTEQUAL (2)}\label{operator-notequal-2}
+
+1 if the first variable value is not equal to the second variable value otherwise 0. NE may also be used.
+
+\subsubsection{Operator:~ AND (2)}\label{operator-and-2}
+
+1 if the first variable value and second variable values are both not zero otherwise 0.
+
+\subsubsection{Operator:~ OR (2)}\label{operator-or-2}
+
+1 if the first variable value and second variable values are either not zero, otherwise 0 if both the first and second variable value are both zero.
+
+\subsubsection{Operator:~ NOT (2)}\label{operator-not-2}
+
+1 if the first variable value and only variable value is zero otherwise 0 if the first variable value is not zero.
+
+\subsubsection{Operator:~ FROM (Unlimited)}\label{operator-from-unlimited}
+
+Indicates what variables a variable is dependant on (or derived from). No computation is performed. The algorithm that creates the automatic sequence of equations uses these to indicate when variables are dependant on other variables so that they can be sorted into the correct order.
diff --git a/doc/input-output-reference/src/energyplus-economics/conceptual-framework-variables-and-hierarchy.tex b/doc/input-output-reference/src/energyplus-economics/conceptual-framework-variables-and-hierarchy.tex
new file mode 100644
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--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/conceptual-framework-variables-and-hierarchy.tex
@@ -0,0 +1,61 @@
+\section{Conceptual Framework -- Variables and Hierarchy}\label{conceptual-framework-variables-and-hierarchy}
+
+To understand how to use the utility bill calculation portion of EnergyPlus you first need to understand some important concepts of variables and hierarchy. A variable, for the purposes of this section, is simply a named holder of a series of numbers. In most cases, the variable will be a named holder of 12 numbers, one number for each monthly utility bill. Here is a visualization of a variable called Electric Energy Use:
+
+% table 35
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Example Electric Energy Use (for Economics Calculation) \label{table:example-electric-energy-use-for-economics}} \tabularnewline
+\toprule 
+Month & Electric Energy Use \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Example Electric Energy Use (for Economics Calculation)} \tabularnewline
+\toprule 
+Month & Electric Energy Use \tabularnewline
+\midrule
+\endhead
+
+January & 12143 \tabularnewline
+February & 13454 \tabularnewline
+March & 14178 \tabularnewline
+April & 14876 \tabularnewline
+May & 15343 \tabularnewline
+June & 16172 \tabularnewline
+July & 16105 \tabularnewline
+August & 15762 \tabularnewline
+September & 14543 \tabularnewline
+October & 13987 \tabularnewline
+November & 13287 \tabularnewline
+December & 12403 \tabularnewline
+\bottomrule
+\end{longtable}
+
+If you have ever done any computer programming, you can think of a variable as an array. Many of the names used in the utility bill calculation portion of EnergyPlus are names of variables. In the case of the UtilityCost:Charge objects, the name of the object is also used as a name of a variable.
+
+In many of today's utility rates, the charges for energy or demand are broken into distribution and supply charges. To allow for this, more than one charge may to be defined for a particular category. The variables assigned to the same category are added together.
+
+The categories are combined in following hierarchy:
+
+\begin{figure}[hbtp] % fig 162
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image615.png}
+\caption{Hierarchy for Economics Charges \protect \label{fig:hierarchy-for-economics-charges}}
+\end{figure}
+
+Any charges included in the EnergyCharges category are added together. The EnergyCharges, DemandCharges and ServiceCharges are added together to form the Basis. The Basis, Adjustments and Surcharges are added together to form the Subtotal. The Subtotal and Taxes are added together to be the Total. The total represents the total monthly charges on that tariff for the energy source used. The combining of categories together is performed automatically unless the user specifies the UtilityCost:Computation. In addition, each category, which is also a variable, may be used as a source. For example, a tax that is 5\% of the subtotal would be shown as:
+
+\begin{lstlisting}
+
+UtilityCost:Charge:Simple,
+    TaxOfFivePercent,        ! Charge Variable Name
+    TariffExample1,          ! Tariff Name
+    Subtotal,                ! Source Variable
+    Annual,                  ! Season
+    Taxes,                   ! Category Variable Name
+    0.05;                    ! Cost Per Unit Value or Variable Name
+\end{lstlisting}
+
+As you can see, the UtilityCost:Charge:Simple and UtilityCost:Charge:Block objects do most of the ``work'' of computing the annual energy cost. The benefit of using this categorization is that totals of each category are shown in the output reports and it organizes the charges in the monthly calculations in a logical way that fits almost all tariffs. If no categorization is desired, theoretically, all charges could be assigned to the Total category. The categories themselves are simply variable names. Charges may also be assigned to the ``NotIncluded'' category if the result of the charge is used as an intermediate calculation and should not be included in the Total.
+
+The rest of this section is divided into a reference of the objects and the fields, a set of examples, discussion of the reporting, and a description of Complex Tariff Modeling. For most tariffs, simply using a variety of UtilityCost:Charge:Simple's and UtilityCost:Charge:Block's will result in a good model but for some more complex tariffs, especially ones with complex block sizes, variables may be computed using a very simple programming language that may appear in the UtilityCost:Computation object. This will be described more in the Complex Tariff Modeling section.
diff --git a/doc/input-output-reference/src/energyplus-economics/cost-estimating.tex b/doc/input-output-reference/src/energyplus-economics/cost-estimating.tex
new file mode 100644
index 00000000000..941d44cd5d8
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/cost-estimating.tex
@@ -0,0 +1,295 @@
+\section{Cost Estimating}\label{cost-estimating}
+
+In order to understand how to include cost estimates, it may be helpful to first define some terminology and provide an overview of the process used in EnergyPlus. There are three broad steps involved. The first involves determining \emph{construction} costs by summing individual ``line items.''~ The second involves determining \emph{project} costs by adjusting construction costs to account for things like profit and design fees. The third involves comparing the current simulation to a reference case so that marginal increases can be calculated. Each of these steps involves using one of the three `ComponentCost' objects described below.
+
+\subsection{ComponentCost:LineItem}\label{componentcostlineitem}
+
+Each instance of this object creates a cost line item and will contribute to the total for a cost estimate. Each line item is reported in table form in the tabular report file. The user must request that this report be generated by including a Output:Table:SummaryReports object with the Component Cost Economics Summary option selected. The style of a tabular report can be controlled using the OutputControl:Table:Style object.
+
+Cost estimates are not currently general in that they cannot be performed for every type of component that could be included in an EnergyPlus model. Although a ``General'' option is available where all information needed for the cost line item is input by the user, the usefulness of cost modeling within EnergyPlus is expected to be enhanced when quantities are obtained from elsewhere in the input file or computed during a simulation. The cost computations are programmed in selected ways for selected objects. The objects available and the type of cost modeling that may be performed are discussed in detail in the discussion of Reference Object Type field. A particular instance of this object will always have many blank fields. Entering values in too many fields may cause an error because the program may determine how a particular cost is to be calculated based on the presence of non-zero values in particular fields. The input object includes fields that are reserved for future use in expanded cost estimate and investment analyses planned for future versions of EnergyPlus. If you would like to request additional objects or different methods of modeling component costs, feel free to describe your needs and submit a request via email to energyplus-support@gard.com.
+
+\subsubsection{Inputs}\label{inputs}
+
+\paragraph{Field: Name}\label{field-name}
+
+This field is a user-selected name that will appear in the line item description of the cost report. It is not used in the calculation but allows identifying a line item in the subsequent report.
+
+\paragraph{Field: Type}\label{field-type}
+
+This field is not yet used and may be left blank.
+
+\paragraph{Field: Line Item Type}\label{field-line-item-type}
+
+The cost estimate line item calculation will be controlled by the name entered in this field. The requirements for the remaining input, and the cost calculations performed, will vary depending on the object referenced here. Only selected objects can be entered here. The objects available for cost estimating are listed in the following table showing the active fields and options available for each.
+
+% table 37
+\begin{longtable}[c]{p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}}
+\caption{Cost Line Item Types (ref Objects) \label{table:cost-line-item-types-ref-objects}} \tabularnewline
+\toprule 
+Object Types available (choice keys) & Cost per each & Cost per m & Cost per kW & Cost per kW *COP & Cost per m & Cost per m  /s & Cost per W/K & Qty & Wildcard for Name \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Cost Line Item Types (ref Objects)} \tabularnewline
+\toprule 
+Object Types available (choice keys) & Cost per each & Cost per m & Cost per kW & Cost per kW *COP & Cost per m & Cost per m  /s & Cost per W/K & Qty & Wildcard for Name \tabularnewline
+\midrule
+\endhead
+
+General & X & ~ & ~ & ~ & ~ & ~ & ~ & X & ~ \tabularnewline
+Construction & ~ & X & ~ & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+Coil:DX Coil:Cooling:DX: SingleSpeed & X & ~ & X & X & ~ & ~ & ~ & ~ & X \tabularnewline
+Chiller:Electric & X & ~ & X & X & ~ & ~ & ~ & ~ & ~ \tabularnewline
+~ & ~ & ~ & ~ & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+Coil:Heating:Gas & X & ~ & X & X & ~ & ~ & ~ & ~ & X \tabularnewline
+Daylighting:Controls & X & ~ & ~ & ~ & ~ & ~ & ~ & ~ & X \tabularnewline
+Shading:Zone:Detailed & ~ & X & ~ & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+Lights & X & ~ & X & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+Generator:Photovoltaic & ~ & ~ & X & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+General
+
+This choice of object is used to calculate costs in a general way. No quantities from internal calculations are used. All information needed for the cost line item is input by the user. The Cost per Each and the Quantity fields that follow need to have values.
+
+\subparagraph{~Construction}\label{construction}
+
+This choice of object type is used to calculate the costs associated with surfaces based on the type of Construction used for the surface. Costs are entered on a per-square-meter basis. The program finds all the surfaces that have the type of Construction named in the Reference Object Name field that follows and determines the total area. If the model includes duplicate surfaces, as for interior partitions or floors, these will be detected and not double-counted. The cost per area should include all the material layers defined in the Construction.
+
+\subparagraph{Coil:DX or Coil:Cooling:DX:SingleSpeed}\label{coildx-or-coilcoolingdxsinglespeed}
+
+This choice of object type is used to calculate the cost of direct expansion cooling equipment. Cost can be entered in three different ways, (1) per each, (2) per kW total cooling capacity, or (3) per kW total cooling capacity per COP (coefficient of performance). The program will determine which method to use by examining which input fields have non-zero values. It is an error to specify costs in more than one way. The per-each approach is most useful for discrete packages. The per-kW approach is useful for autosizing DX coils with the same COP. The per-kW-per-COP approach is convenient for modeling autosized DX coils with differing COPs as long as a linear relationship is sufficient.
+
+The wildcard character ``*'' may be used in the object name field that follows to allow a single line item to include all of the DX coils in the model.
+
+Chiller:Electric
+
+This choice of object type is used to calculate the cost of a central chiller. The object name entered in following field must correspond to a Chiller:Electric object name defined elsewhere in the input file. Cost can be entered in three different ways, (1) per each, (2) per kW total cooling capacity or (3) per kW total cooling capacity per COP (coefficient of performance). The program will determine which method to use by examining which input fields have non-zero values. It is an error to specify costs in more than one way. The per-each approach is most useful for discrete chillers. The per-kW approach is useful for autosizing chillers with the same COP. The per-kW-per-COP approach is convenient for modeling autosized chillers with differing COPs as long as a linear relationship is sufficient.
+
+\subparagraph{Coil:Heating:Gas}\label{coilheatinggas}
+
+This choice of object type is used to calculate the cost of gas-fired heating equipment. Cost can be entered in three different ways, (1) per each, (2) per kW of heating capacity, or (3) per kW total cooling capacity per nominal efficiency (actually uses the per kW per COP field). The program will determine which method to use by examining which input fields have non-zero values. It is an error to specify costs in more than one way. The per-each approach is most useful for discrete packages. The per-kW approach is useful for autosizing heating coils with the same efficiency. The per-kW-per-Eff approach is convenient for modeling autosized heating coils with differing efficiencies as long as a linear relationship is sufficient.
+
+The wildcard character ``*'' may be used in the object name field that follows to allow a single line item to include all of the gas heating coils in the model.
+
+\subparagraph{Daylighting:Controls}\label{daylightingcontrols}
+
+These choices of object type are used to include the cost of controllers needed to control electric lighting in response to daylight. The only option for entering costs is ``per each''. The wildcard character ``*'' may be used in the following object name field to allow a single line item to include all of the simple and detailed daylighting controls in the cost model.
+
+\subparagraph{Shading:Zone:Detailed}\label{shadingzonedetailed}
+
+This choice of object type is used to calculate the costs associated with attached shading surfaces. Costs are entered on a per-square-meter basis. The cost calculations are similar to those for heat transfer surfaces but are handled separately because ``Construction'' is not defined for a shading surface. The object name entered in the following field must correspond to a Shading:Zone:Detailed object name defined elsewhere in the input file.
+
+\subparagraph{Lights}\label{lights}
+
+This choice of object is used to calculate the costs associated with electric lighting. Costs are entered on either a cost-per-each basis or as a cost-per-kilowatt-of-design-level. (This design level is an input in the Lights object.). The object name entered into the following field must match the name of a Zone object defined elsewhere in the input file.
+
+\subparagraph{Generator:Photovoltaic}\label{generatorphotovoltaic}
+
+This choice of object is used to calculate the costs associated with a photovoltaic system. Costs are entered on a cost-per-kilowatt-of-rated-capacity. The rated capacity of a photovoltaic generator is calculated for cost modeling by exposing the surface to a 1000 W/m2 incident radiation using the area fraction and nominal fixed efficiency input by the user (from the Generator:Photovoltaic object). The object name entered into the following field must match the name of a Generator:Photovoltaic ~object defined elsewhere in the input file.
+
+\paragraph{Field: Item Name}\label{field-item-name}
+
+This field is used to refer to a specific instance of an object. The wildcard character ``*'' is acceptable for some objects as described above for the previous field.
+
+\paragraph{Field: Object End Use Key}\label{field-object-end-use-key}
+
+This field is not yet used and may be left blank.
+
+\paragraph{Field: Cost per Each}\label{field-cost-per-each}
+
+This field is used to enter cost information on a per-each basis. The units are dollars (\$).
+
+\paragraph{Field: Cost per Area}\label{field-cost-per-area}
+
+This field is used to enter cost information on a per-area basis. The units are dollars per square meter (\$/m\(^{2}\)).
+
+\paragraph{Field: Cost per Unit of Output Capacity}\label{field-cost-per-unit-of-output-capacity}
+
+This field is used to enter cost information on a per-kilowatt basis. The units are dollars per kilowatt (\$/kW).
+
+\paragraph{Field: Cost per Unit of Output Capacity per COP}\label{field-cost-per-unit-of-output-capacity-per-cop}
+
+This field is used to enter cost information on a per-kilowatt-per-COP basis. The units are dollars per kilowatt per non-dimensional COP (\$/kW-COP).~ Note that this field can be used for Coil:Heating:Gas cost modeling in which case the better terminology would be per-kilowatt-per-non-dimensional-efficiency.
+
+\paragraph{Field: Cost per Volume}\label{field-cost-per-volume}
+
+This field is not yet used but will be used to enter cost information on a per-cubic-meter basis. The units are dollars per cubic meter (\$/m\(^{3}\)).
+
+\paragraph{Field: Cost per Volume Rate}\label{field-cost-per-volume-rate}
+
+This field is not yet used but will be used to enter cost information on a per-cubic-meter-per-second basis. The units are dollars per cubic meter (\$/(m\(^{3}\)/s)).
+
+\paragraph{Field: Cost per Energy per Temperature Difference}\label{field-cost-per-energy-per-temperature-difference}
+
+This field is not yet used but will be used to enter cost information on a per-watt-per-Kelvin basis. These units will be used to represent a UA description of coils and the like. The units are dollars per watt per delta K (\$/(W/K)).
+
+\paragraph{Field: Quantity}\label{field-quantity}
+
+This field is used to directly enter the line item quantity. The units should correspond to what is used in the Per Each field.
+
+Some examples of this object in an IDF:
+
+\begin{lstlisting}
+
+  ComponentCost:LineItem,
+     PSZ Equipment from scaling , !- Name
+     ,                            !- Type
+     Coil:DX,                     !- Line Item Type
+     ACDXCoil ZN1 ,               !- Item Name
+     ,                            !- Object End Use Key
+     ,                            !- Cost per Each {$}
+     ,                            !- Cost per Area {$/m2}
+     ,                            !- Cost per Unit of Output Capacity {$/kW}
+     82.5;                   !- Cost per Unit of Output Capacity per COP {$/kW}
+
+
+    ComponentCost:LineItem,
+      Lighting Equip: ZN2_E_Space_1, ,
+      Lights,!- Line Item Type
+      ZN2_E_Space_1, ,
+      ,!- Cost per Each {$}
+      ,!- Cost per Area {$/m2}
+      3300.000;!- Cost per Unit of Output Capacity {$/kW}
+
+
+
+
+    ComponentCost:LineItem, DL controls: ZN4_W_Space_1, ,
+      Daylighting:Detailed, !- Line Item Type
+      ZN4_W_Space_1, ,!- Item Name
+      125.000, !- Cost per Each {$}
+      ,!- Cost per Area {$/m2}
+      ;!- Cost per Unit of Output Capacity {$/kW}
+\end{lstlisting}
+
+\subsection{ComponentCost:Adjustments}\label{componentcostadjustments}
+
+This object can be used to perform various modifications to the construction costs to arrive at an estimate for total project costs. This object allows extending the line item model so that the overall costs of the project will reflect various profit and fees. Only one object of this type can be included in the input file. The results are included in the Construction Cost Estimate Summary table by request using the Output:Table:SummaryReports object with the Component Cost Economics Summary option selected.
+
+\subsubsection{Inputs}\label{inputs-1}
+
+\paragraph{Field: Miscellaneous Cost per Conditioned Area}\label{field-miscellaneous-cost-per-conditioned-area}
+
+This optional field can be used to enter a cost model for miscellaneous project costs that are not included in the line item modeling. Miscellaneous costs are entered in dollars per square meter of conditioned floor area. This field allows including the costs of project elements that go beyond what can be modeled using ``ComponentCost:LineItem'' input objects including such things as structural components, site preparation, finishes, etc. The value input in this field will be multiplied by the conditioned floor area and listed in the Construction Cost Estimate Summary table. The miscellaneous project costs are added to the line item model total to determine the ``modeled and miscellaneous Construction costs'' that will be multiplied by the fractions in the following five fields.
+
+\paragraph{Field: Design and Engineering Fees}\label{field-design-and-engineering-fees}
+
+This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for design and engineering fees. Note that is not the same as a fraction of the total cost estimate.
+
+\paragraph{Field: Contractor Fee}\label{field-contractor-fee}
+
+This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for Contractor fees. Note that is not the same as a fraction of the total cost estimate.
+
+\paragraph{Field: Contingency}\label{field-contingency}
+
+This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added for contingency. Note that is not the same as a fraction of the total cost estimate.
+
+\paragraph{Field: Permits, Bonding and Insurance}\label{field-permits-bonding-and-insurance}
+
+This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for permitting, bonding, and insurance costs to the project. Note that is not the same as a fraction of the total cost estimate.
+
+\paragraph{Field: Commissioning Fee}\label{field-commissioning-fee}
+
+This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for commissioning services. Note that is not the same as a fraction of the total cost estimate.
+
+\paragraph{Field: Regional Adjustment Factor}\label{field-regional-adjustment-factor}
+
+This optional field can be used to enter an adjustment factor to account for regional differences is construction costs. The factor will be applied to the modeled and miscellaneous construction costs to determine and amount that should be added, or subtracted, to account for local variations in construction costs. The default factor is 1.0. The additive adjustment is calculated by subtracting 1.0 from the value entered in this field. This field is useful for using national average data in the line item and miscellaneous construction cost models and then altering the results based on regional differences.
+
+An example of this object in an IDF is:
+
+\begin{lstlisting}
+ComponentCost:Adjustments,
+            467, !- Miscellaneous Cost per Conditioned Area
+           0.07, !- Design and Engineering Fees
+           0.07, !- Contractor Fee
+           0.10, !- Contingency
+           0.04, !- Permits, Bonding and Insurance
+           0.015,!- Commissioning Fee
+          1.136; !- Regional Adjustment Factor
+\end{lstlisting}
+
+\subsection{ComponentCost:Reference}\label{componentcostreference}
+
+This object can be used to allow comparing the current cost estimate to the results of a previous estimate for a reference building. This object parallels the ComponentCost:Adjustment object but adds a field for entering the cost line item model result for the reference building. All the various adjustments to the project cost estimate are available here to allow using factors that differ between the current and the reference building models. The factors entered in the field associated with this object are applied to the reference building while the factors listed in the ComponentCost:Adjustment object are applied to the current building model cost estimate. Only one object of this type can be included in the input file. The results are included in the Construction Cost Estimate Summary table by request using the Output:Table:SummaryReports object with the Component Cost Economics Summary option selected.
+
+\subsubsection{Inputs}\label{inputs-2}
+
+\paragraph{Field: Reference Building Line Item Costs}\label{field-reference-building-line-item-costs}
+
+This field is used to enter a dollar amount representing the total for the reference building that the user would like to compare to the line item cost model for the current building model. A typical source of data for this would be the ``Line Item Subtotal'' from a previous EnergyPlus simulation.
+
+\paragraph{Field: Reference Building Miscellaneous Cost per Conditioned Area}\label{field-reference-building-miscellaneous-cost-per-conditioned-area}
+
+This optional field can be used to enter a cost model for miscellaneous project costs that are not included in the line item modeling. Miscellaneous costs are entered in dollars per square meter of conditioned floor area. This field allows including the costs of project elements that go beyond what can be modeled using ``ComponentCost:LineItem'' input objects including such things as structural components, site preparation, finishes, etc. The value input in this field will be multiplied by the conditioned floor area and listed in the Construction Cost Estimate Summary table. The miscellaneous project costs are added to the reference building line item subtotal to determine the ``modeled and miscellaneous construction costs'' that will be multiplied by the fractions in the following five fields.
+
+\paragraph{Field: Reference Building Design and Engineering Fees}\label{field-reference-building-design-and-engineering-fees}
+
+This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for design and engineering fees. Note that is not the same as a fraction of the total cost estimate.
+
+\paragraph{Field: Reference Building Contractor Fee}\label{field-reference-building-contractor-fee}
+
+This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for Contractor fees. Note that is not the same as a fraction of the total cost estimate.
+
+\paragraph{Field: Reference Building Contingency}\label{field-reference-building-contingency}
+
+This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added for contingency. Note that is not the same as a fraction of the total cost estimate.
+
+\paragraph{Field: Reference Building Permits, Bonding and Insurance}\label{field-reference-building-permits-bonding-and-insurance}
+
+This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for permitting, bonding, and insurance costs to the project. Note that is not the same as a fraction of the total cost estimate.
+
+\paragraph{Field: Reference Building Commissioning Fee}\label{field-reference-building-commissioning-fee}
+
+This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for commissioning services. Note that is not the same as a fraction of the total cost estimate.
+
+\paragraph{Field: Reference Building Regional Adjustment Factor}\label{field-reference-building-regional-adjustment-factor}
+
+This optional field can be used to enter an adjustment factor to account for regional differences is construction costs. The factor will be applied to the modeled and miscellaneous construction costs to determine and amount that should be added, or subtracted, to account for local variations in construction costs. The default factor is 1.0. The additive adjustment is calculated by subtracting 1.0 from the value entered in this field. This field is useful for using national average data in the line item and miscellaneous construction cost models and then altering the results based on regional differences.
+
+An example of this object in an IDF is:
+
+\begin{lstlisting}
+
+ComponentCost:Reference,
+    683060.000, !- Reference Building Line Item Costs {$}
+    467.0, !- Reference Building Miscellaneous Cost per Conditioned Area {$/m2}
+    0.060, !- Reference Building Design and Engineering Fees {dimensionless}
+    0.070, !- Reference Building Contractor Fee {dimensionless}
+    0.100, !- Reference Building Contingency
+    0.04,  !- Reference Building Permits, Bonding and Insurance {dimensionless}
+    0.0075,!- Reference Building Commissioning Fee {dimensionless}
+    1.136; !- Reference Building Regional Adjustment Factor {dimensionless}
+\end{lstlisting}
+
+\subsection{Economics Cost Estimate Reporting}\label{economics-cost-estimate-reporting}
+
+Cost estimate results are only output to tabular reports; they are not available in the standard output file (.eso). The results are included in the Construction Cost Estimate Summary table by request using the object Output:Table:SummaryReports object with the Component Cost Economics Summary option selected. The figure below shows an example of summary output using html style for tabular reporting. A second table is produced that provides the line item details with one line for every line item object. Per-area cost modeling and cost normalization are based on total conditioned floor area which is also provided in the tabular report.
+
+\begin{figure}[hbtp] % fig 163
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image616.png}
+\caption{Economics Cost Modeling \protect \label{fig:economics-cost-modeling}}
+\end{figure}
+
+``Line Item Subtotal'' is the sum of items explicitly modeled in the cost estimate. For the reference building, this value is input by the user. For the current building, this value is the sum of line items which are detailed in Cost Line Item Details table that follows.
+
+``Misc. Cost'' is the product of the user-defined Miscellaneous Cost Model (per Square Meter) and the conditioned floor area.
+
+``Regional Adjustment'' is the produce of the user-defined Regional Adjustment Factor and the conditioned floor area.
+
+``Design Fee'' is the product of the user-defined Design and Engineering Fee Fraction and the subtotal for construction costs (which includes the Line Item Subtotal, Misc. Cost, and Regional Adjustment).
+
+``Contractor Fee'' is the product of the user-defined Contractor Fee Fraction and the subtotal for construction costs (which includes the Line Item Subtotal, Misc. Cost, and Regional Adjustment).
+
+``Contingency'' is the product of the user-defined Contingency Fraction and the subtotal for construction costs (which includes the Line Item Subtotal, Misc. Cost, and Regional Adjustment).
+
+``Permits, Bonds, and Insurance'' is the product of the Permits, Bonding, Insurance Fraction and the subtotal for construction costs (which includes the Line Item Subtotal, Misc. Cost, and Regional Adjustment).
+
+``Commissioning'' is the product of the user-defined Commissioning Fee Fraction and the subtotal for construction costs (which includes the Line Item Subtotal, Misc. Cost, and Regional Adjustment).
+
+``Cost Estimate Total'' is the sum of eight items above and represents the total project cost estimate.
+
+``Cost per Conditioned Building Area'' is the Cost Estimate Total divided by the total conditioned floor area. This represents a normalized cost intensity.
diff --git a/doc/input-output-reference/src/energyplus-economics/economic-results-summary-report.tex b/doc/input-output-reference/src/energyplus-economics/economic-results-summary-report.tex
new file mode 100644
index 00000000000..dd5ea71baf3
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/economic-results-summary-report.tex
@@ -0,0 +1,31 @@
+\section{Economic Results Summary Report}\label{economic-results-summary-report}
+
+\begin{itemize}
+\item
+  Annual Cost -- Shows the annual cost for qualified and selected electric and gas tariffs and the total cost
+\item
+  Tariff Summary -- For each tariff included shows if that tariff was selected, if it was qualified, what meter it was connected to, what group it was part of, and the annual cost. The qualified tariff with the lowest annual cost for each of the meters is indicated as ``selected'' and shown in the Annual Cost section of the report. If multiple groups are defined, a tariff is selected from each group.
+\end{itemize}
+
+\textbf{Tariff Summary}
+
+\begin{itemize}
+\item
+  Summary table -- Shows the if that tariff was selected, if it was qualified, which qualifier disqualified the tariff, what meter it was connected to, what group it was part of, if the computation was based on a user defined computation or was automatic.
+\item
+  Categories -- Shows the monthly results of all the category variables.
+\item
+  Charges -- Shows the monthly results for all of the simple and block charges.
+\item
+  Ratchets -- Shows the monthly results for all ratchets.
+\item
+  Qualifies -- Shows the monthly results for all qualifies.
+\item
+  Native Variables -- Shows the monthly values for the native variables such as TotalEnergy and TotalDemand.
+\item
+  Other Variables -- Shows the monthly values for any other variables not appearing in the other tables.
+\item
+  Computation -- Shows the computational steps used including those generated automatically.
+\end{itemize}
+
+The report is part of the tabular report and is created using the same style as specified for the tabular reports.
diff --git a/doc/input-output-reference/src/energyplus-economics/group-economics.tex b/doc/input-output-reference/src/energyplus-economics/group-economics.tex
new file mode 100644
index 00000000000..39fc8cd6509
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/group-economics.tex
@@ -0,0 +1,56 @@
+\section{Group -- Economics}\label{group-economics}
+
+EnergyPlus contains a number of objects to model construction cost and utility bill calculations.
+
+The objects used by EnergyPlus for construction cost calculations are as follows:
+
+\begin{itemize}
+\item
+  ComponentCost:Adjustments
+\item
+  ComponentCost:Reference
+\item
+  ComponentCost:LineItem
+\end{itemize}
+
+The objects used by EnergyPlus for utility bill calculations are as follows:
+
+\begin{itemize}
+\item
+  UtilityCost:Tariff
+\item
+  UtilityCost:Qualify
+\item
+  UtilityCost:Charge:Simple
+\item
+  UtilityCost:Charge:Block
+\item
+  UtilityCost:Ratchet
+\item
+  UtilityCost:Variable
+\item
+  UtilityCost:Computation
+\end{itemize}
+
+The objects used for performing a life-cycle cost analysis are:
+
+\begin{itemize}
+\item
+  LifeCycleCost:Parameters
+\item
+  LifeCycleCost:RecurringCosts
+\item
+  LifeCycleCost:NonrecurringCost
+\item
+  LifeCycleCost:UsePriceEscalation
+\item
+  LifeCycleCost:UseAdjustment
+\end{itemize}
+
+The object used for specifying the currency symbol of the monetary unit used is:
+
+\begin{itemize}
+\tightlist
+\item
+  CurrencyType
+\end{itemize}
diff --git a/doc/input-output-reference/src/energyplus-economics/introduction-to-economics.tex b/doc/input-output-reference/src/energyplus-economics/introduction-to-economics.tex
new file mode 100644
index 00000000000..810c59199fd
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/introduction-to-economics.tex
@@ -0,0 +1,39 @@
+\section{Introduction to Economics}\label{introduction-to-economics}
+
+While it is true that monthly utility bills are often directly related to monthly energy consumption and monthly peak demand, due to the elaborate regulatory environment and the changing value of the energy based on load factor, the calculations involved are often complicated. The EnergyPlus approach is to allow you to model the individual component charges that make up the utility bill and report the results on a monthly basis.
+
+To show you how simple the specification of a rate can be here is a simple example for a flat charge of 8 cents for every kWh sold.
+
+\begin{lstlisting}
+
+UtilityCost:Tariff,
+    TariffExample1,          ! Name
+    Electricity:Facility,    ! Output Meter Name
+    kWh;               ! Conversion Factor Choice
+
+
+  UtilityCost:Charge:Simple,
+    ChargeExample1,          ! Charge Variable Name
+    TariffExample1,          ! Tariff Name
+    totalEnergy,             ! Source Variable
+    Annual,                   ! Season
+    EnergyCharges,           ! Category Variable Name
+    0.08;                    ! Cost Per Unit Value or Variable Name
+\end{lstlisting}
+
+Overall, the goals of the economics section of EnergyPlus are to make simple tariffs easy to model and complex tariffs possible to model.
+
+The cost implications of alternative, energy-related design options may be important in determining the whether or not a particular design is viable. Although the main purpose of EnergyPlus is to determine the energy performance of a building, component cost modeling is provided to allow estimating initial construction costs associated with the building and HVAC system being modeled. This is provided in order to ensure that cost estimates are consistent with the EnergyPlus model and it allows using results calculated during a simulation such as equipment sizes and surface areas. The cost estimating capabilities are not comprehensive and are not intended to duplicate all the types of analyses included in cost estimating software. Economics modeling is being implemented in stages. Future versions of EnergyPlus will add other investment related analyses such as life-cycle cost. The objects used by EnergyPlus for calculating first costs for construction projects are as follows:
+
+\begin{itemize}
+\item
+  ComponentCost:Adjustments
+\item
+  ComponentCost:Reference
+\item
+  ComponentCost:LineItem
+\end{itemize}
+
+The results of the cost estimate are reported in a Construction Cost Estimate Summary table provided that the user requests the results using the object Output:Table:SummaryReports object with the Component Cost Economics Summary option selected. The style of this predefined report can be controlled using the OutputControl:Table:Style object. If the Annual Building Performance Report Summary is also requested, then cost estimate results will follow that data in the same output file.
+
+The rest of this Economics section is organized to first present reference material on tariff calculations followed by construction cost estimating.
diff --git a/doc/input-output-reference/src/energyplus-economics/life-cycle-costing.tex b/doc/input-output-reference/src/energyplus-economics/life-cycle-costing.tex
new file mode 100644
index 00000000000..a493f424495
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/life-cycle-costing.tex
@@ -0,0 +1,30 @@
+\section{Life-Cycle Costing}\label{life-cycle-costing}
+
+Life-cycle costing is used with building energy simulation in order to justify energy efficiency upgrades. Many alterative building technologies that result in energy savings cost more initially, or may cost more to maintain, than traditional solutions. In order to justify selecting these energy savings technologies, it is essential to combine both initial and future costs in the decision process. Using life-cycle costs provides a framework to combine initial costs and future costs into a single combined measure, called the ``present value.'' Present value is a metric that combines all costs and reduces (or discounts) those costs that occur in the future. Discounting future costs is based on the principal of the time value of money.
+
+The calculations are based on discounting the future values according to normal life-cycle costing techniques as described in NIST Handbook 135 ``Life-Cycle Costing Manual for the Federal Energy Management Program.''
+
+The following is a list of life-cycle costing related objects that provide a way to describe the parameters and costs associated with the life-cycle of a building or building system:
+
+\begin{itemize}
+\item
+  LifeCycleCost:Parameters
+\item
+  LifeCycleCost:RecurringCosts
+\item
+  LifeCycleCost:NonrecurringCost
+\item
+  LifeCycleCost:UsePriceEscalation
+\item
+  LifeCycleCost:UseAdjustment
+\end{itemize}
+
+The utility costs (see UtilityCost:Tariff) and first costs (see ComponentCost:LineItem) are~ calculated by EnergyPlus are used along with other current and future costs input using the LifeCycleCost:RecurringCosts and LifeCycleCost:NonrecurringCost objects and these are combined these into the present value life-cycle cost metric. The LifeCycleCost:Parameters object establishes the set of assumptions for the analysis along with LifeCycleCost:UsePriceEscalation (often from a DataSet) and LifeCycleCost:UseAdjustment.
+
+It is important to understand that the comparison of different simulation results and their present values is not performed by EnergyPlus. Instead, EnergyPlus provides the present value calculations for a specific simulation combining the energy costs, first costs, and future costs and you need to make the comparison between the results of multiple simulations.
+
+The results of using the LifeCycleCost objects are included automatically in the tabular report file whenever the LifeCycleCost:Parameters object is present. The report appearing in the tabular report file is titled ``Life Cycle Cost Report.'' This report shows the costs and the timing of costs, often called ``cash flows,'' along with the present value in several different tables. The tabular results would show the present value of all current and future costs.
+
+The datasets file ``LCCusePriceEscalationDataSetXXXX.idf'' includes the energy escalation factors from the NIST Handbook 135 annual supplement for the year indicated. These are necessary to use because the expected change in price for electricity and various fuels does not change at the same rate as inflation.
+
+Life-cycle costing should not be confused with life-cycle analysis. With life-cycle costing the result is an economic evaluation of current and future expenditures in order to make a decision on alternative investments. In life cycle analysis, the environmental impact such as equivalent CO2 production involved in the materials, delivery, manufacturing, and construction are combined with environmental impacts of the building in operation and the eventual removal of the building and is used to understand the overall environmental impact or embodied energy.
diff --git a/doc/input-output-reference/src/energyplus-economics/lifecyclecost-nonrecurringcost.tex b/doc/input-output-reference/src/energyplus-economics/lifecyclecost-nonrecurringcost.tex
new file mode 100644
index 00000000000..07547c4488c
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/lifecyclecost-nonrecurringcost.tex
@@ -0,0 +1,64 @@
+\section{LifeCycleCost:NonrecurringCost}\label{lifecyclecostnonrecurringcost}
+
+A non-recurring cost happens only once during the study period. For costs that occur more than once during the study period on a regular schedule, use the LifeCycleCost:RecurringCost object.
+
+\subsection{Inputs}\label{inputs-057}
+
+\paragraph{Field: Name}\label{field-name-055}
+
+The identifier used for the object. The name is used in identifying the cash flow equivalent in the output results in the Life-Cycle Cost Report.
+
+\paragraph{Field: Category}\label{field-category}
+
+Enter the category of the non-recurring costs. Choose the closest category. The options include:
+
+\begin{itemize}
+\item
+  Construction
+\item
+  Salvage
+\item
+  OtherCapital
+\end{itemize}
+
+The default is Construction.
+
+For recommendations on estimating capital and salvage (residual) costs, see NIST 135 Section 4.5.
+
+\paragraph{Field: Cost}\label{field-cost}
+
+Enter the non-recurring cost value. For construction and other capital costs the value entered is typically a positive value. For salvage costs, the value entered is typically a negative value which represents the money paid to the investor for the equipment at the end of the study period.
+
+\paragraph{Field: Start of Costs}\label{field-start-of-costs}
+
+Enter when the costs start. The First Year of Cost is based on the number of years past the Start of Costs. For most non-recurring costs the Start of Costs should be Base Period which begins at the base month and year. The options are:
+
+\begin{itemize}
+\item
+  ServicePeriod
+\item
+  BasePeriod
+\end{itemize}
+
+The default value is BasePeriod
+
+\paragraph{Field: Years From Start}\label{field-years-from-start}
+
+This field and the Months From Start field together represent the time from either the start of the Service Period, on the service month and year, or start of the Base Period, on the base month and year (depending on the Start of Cost field) that the costs start to occur. Normally, for most capital costs the Start of Costs is the Base Period and the Years from Start will be 0. These would be first costs for the building equipment or system. Salvage costs are usually shown as happening in the last year of the analysis. Only integers should be entered representing whole years. The default value is 0.
+
+\paragraph{Field: Months From Start}\label{field-months-from-start}
+
+This field and the Years From Start field together represent the time from either the start of the Service Period, on the service month and year, or start of the Base Period, on the base month and year (depending on the Start of Cost field) that the costs start to occur. Normally, for most capital costs the Start of Costs is the Base Period and the Months from Start will be 0. Only integers should be entered representing whole months. The Years From Start (times 12) and Months From Start are added together. The default value is 0.
+
+An example of this object in an IDF:
+
+\begin{lstlisting}
+
+LifeCycleCost:NonrecurringCost,
+      EstimatedSalvage,        !- Name
+      Salvage,                 !- Category
+      -2000,                   !- Cost
+      ServicePeriod,           !- Start of Costs
+      20,                      !- Years from Start
+      0;                       !- Months from Start
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/energyplus-economics/lifecyclecost-parameters.tex b/doc/input-output-reference/src/energyplus-economics/lifecyclecost-parameters.tex
new file mode 100644
index 00000000000..1cfcbeb2897
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/lifecyclecost-parameters.tex
@@ -0,0 +1,198 @@
+\section{LifeCycleCost:Parameters}\label{lifecyclecostparameters}
+
+Provides inputs related to the overall life-cycle analysis. It establishes many of the assumptions used in computing the present value. It is important that when comparing the results of multiple simulations that the fields in the LifeCycleCost:Parameters objects are the same for all the simulations. To aide in this comparison, the first table in the Life-Cycle Cost Report shows the inputs to this object. Only one LifeCycleCost:Parameters object is permitted for a file. When this object is present the tabular report file will contain the Life-Cycle Cost Report.
+
+\subsection{Inputs}\label{inputs-058}
+
+\paragraph{Field: Name}\label{field-name-056}
+
+An identifying name used for the LifeCycleCost:Parameters object.
+
+\paragraph{Field: Discounting Convention}\label{field-discounting-convention}
+
+The field specifies if the discounting of future costs should be computed as occurring at the end of each year, the middle of each year, or the beginning of each year. The most common discounting convention uses the end of each year. Without a specific reason, the end of each year should be used. Some military projects may specifically require using the middle of each year. The year being used starts with the base year and month and repeats every full year. All costs assumed to occur during that duration are accumulated and shown as an expense either at the beginning, middle or end of the year.~ The options are:
+
+\begin{itemize}
+\item
+  BeginningOfYear
+\item
+  MidYear
+\item
+  EndOfYear
+\end{itemize}
+
+\paragraph{Field: Inflation Approach}\label{field-inflation-approach}
+
+This field is used to determine if the analysis should use constant dollars or current dollars which is related to how inflation is treated. The two options are:
+
+\begin{itemize}
+\item
+  ConstantDollar
+\item
+  CurrentDollar
+\end{itemize}
+
+The default option is ConstantDollars
+
+If ConstantDollar is selected, then the Real Discount Rate input is used and it excludes the rate of inflation. If CurrentDollar is selected, then the Nominal Discount Rate input is used and it includes the rate of inflation. From NIST Handbook 135:
+
+``The constant dollar approach has the advantage of avoiding the need to project future rates of inflation or deflation. The price of a good or service stated in constant dollars is not affected by the rate of general inflation. For example, if the price of a piece of equipment is \$1,000 today and \$1,050 at the end of a year in which prices in general have risen at an annual rate of 5 percent, the price stated in constant dollars is still \$1,000; no inflation adjustment is necessary. In contrast, if cash flows are stated in current dollars, future amounts include general inflation, and an adjustment is necessary to convert the current-dollar estimate to its constant-dollar equivalent. This adjustment is important because constant- and current-dollar amounts must not be combined in an LCCA {[}life cycle cost analysis{]}.''
+
+For most analyses, using the ConstantDollar option will be easier since the effect of inflation may be ignored.
+
+\paragraph{Field: Real Discount Rate}\label{field-real-discount-rate}
+
+Enter the real discount rate as a decimal. For a 3\% rate, enter the value 0.03. This input is used when the Inflation Approach is ConstantDollar. The real discount rate reflects the interest rates needed to make current and future expenditures have comparable equivalent values when general inflation is ignored. When Inflation Approach is set to CurrentDollar this input is ignored. If this field is blank and Inflation Approach is ConstantDollar, a warning is issued.
+
+\paragraph{Field: Nominal Discount Rate}\label{field-nominal-discount-rate}
+
+Enter the nominal discount rate as a decimal. For a 5\% rate, enter the value 0.05. This input is used when the Inflation Approach is CurrentDollar. The real discount rate reflects the interest rates needed to make current and future expenditures have comparable equivalent values when general inflation is included. When Inflation Approach is set to ConstantDollar this input is ignored. If this field is blank and Inflation Approach is CurrentDollar, a warning is issued.
+
+\paragraph{Field: Inflation Rate}\label{field-inflation-rate}
+
+Enter the rate of inflation for general goods and services as a decimal. For a 2\% rate, enter the value 0.02. If this field is not blank and Inflation Approach is ConstantDollar, a warning is issued.
+
+\paragraph{Field: Base Date Month}\label{field-base-date-month}
+
+Enter the month that is the beginning of study period, also known as the beginning of the base period. According to NIST 135 ``the base date is the point in time to which all project-related costs are discounted in an LCCA {[}life cycle cost analysis{]}. The base date is usually the first day of the study period for the project, which in turn is usually the date that the LCCA is performed. In a constant dollar analysis, the base date usually defines the time reference for the constant dollars (e.g.~1995 constant dollars). It is essential that you use the same base data and constant-dollar year for all of the project alternatives to be compared. If you set the base date to the date that the LCCA is performed, then the constant dollar basis for the analysis will be the current date, and you can use actual costs as of that date without adjusting for general inflation.''
+
+The choices are:
+
+\begin{itemize}
+\item
+  January
+\item
+  February
+\item
+  March
+\item
+  April
+\item
+  May
+\item
+  June
+\item
+  July
+\item
+  August
+\item
+  September
+\item
+  October
+\item
+  November
+\item
+  December
+\end{itemize}
+
+The default value is January.
+
+This field could also be referred to as part of ``the date of study.'' It is used as the date for constant dollars.
+
+\paragraph{Field: Base Date Year}\label{field-base-date-year}
+
+Enter the four digit year that is the beginning of study period, such as~ a year expressed in four digits like ``2013''. The study period is also known as the base period. See more details in the previous field.
+
+\paragraph{Field: Service Date Month}\label{field-service-date-month}
+
+Enter the month that is the beginning of building occupancy. Energy costs computed by EnergyPlus are assumed to occur during the year following the service date. The service date must be the same or later than the Base Date. The choices are:
+
+\begin{itemize}
+\item
+  January
+\item
+  February
+\item
+  March
+\item
+  April
+\item
+  May
+\item
+  June
+\item
+  July
+\item
+  August
+\item
+  September
+\item
+  October
+\item
+  November
+\item
+  December
+\end{itemize}
+
+The default value is January. According to NIST Handbook 135:
+
+``The service date is the date on which the project is expected to be implemented; operating and maintenance costs (including energy- and water-related costs) are generally incurred after this date, not before.''
+
+This field could also be referred to as part of ``beneficial occupancy date.''
+
+\paragraph{Field: Service Date Year}\label{field-service-date-year}
+
+Enter the four digit year that is the beginning of occupancy, such as~ two years after the previously entered year expressed in four digits like ``2013''. See more details in the previous field.
+
+\paragraph{Field: Length of Study Period in Years}\label{field-length-of-study-period-in-years}
+
+Enter the number of years of the study period. It is the number of years that the study continues based on the start at the base date. The default value is 25 years. Only integers may be used indicating whole years.~ According to NIST Handbook 135, ``the study period for an LCCA is the time over which the costs and benefits related to a capital investment decision are of interest to the decision maker. Thus, the study period begins with the base date and includes both the {[}planning/construction{]} period (if any) and the relevant service period for the project. The service period begins with the service date and extends to the end of the study period.''
+
+\paragraph{Field: Tax rate}\label{field-tax-rate}
+
+Enter the overall marginal tax rate for the project costs. This does not include energy or water taxes. The single tax rate entered here is not intended to be a replacement of the complex calculations necessary to compute personal or corporate taxes; instead it is an approximate that may be used for a simple analysis assuming a constant tax rate is applied on all costs. The tax rate entered should be based on the marginal tax rate for the entity and not the average tax rate. Enter the tax rate results in present value calculations after taxes. Most analyses do not factor in the impact of taxes and assume that all options under consideration have roughly the same tax impact. Due to this, many times the tax rate can be left to default to zero and the present value results before taxes are used to make decisions. The value should be entered as a decimal value. For 15\% enter 0.15. For an analysis that does not include tax impacts, enter 0.0. The default is 0.
+
+\paragraph{Field: Depreciation Method}\label{field-depreciation-method}
+
+For an analysis that includes income tax impacts, this entry describes how capital costs are depreciated. According to IRS Publication 946 -- How to Depreciate Property ``Depreciation is an annual income tax deduction that allows you to recover the cost or other basis of certain property over the time you use the property. It is an allowance for Fair market value the wear and tear, deterioration, or obsolescence of the Intangible property.'' Details on which depreciation method to choose depends on the property being depreciated and IRS Publication 946 and your accountant are the best sources of information in determining which depreciation method to choose. Only one depreciation method may be used for an analysis and is applied to all capital expenditures. Only analyses that include tax impacts need to select a depreciation method.
+
+The options are:
+
+\begin{itemize}
+\item
+  ModifiedAcceleratedCostRecoverySystem-3year
+\item
+  ModifiedAcceleratedCostRecoverySystem-5year
+\item
+  ModifiedAcceleratedCostRecoverySystem-7year
+\item
+  ModifiedAcceleratedCostRecoverySystem-10year
+\item
+  ModifiedAcceleratedCostRecoverySystem-15year
+\item
+  ModifiedAcceleratedCostRecoverySystem-20year
+\item
+  StraightLine-27year
+\item
+  StraightLine-31year
+\item
+  StraightLine-39year
+\item
+  StraightLine-40year
+\item
+  None
+\end{itemize}
+
+Depreciation allowances reduce the actual/nominal tax dollars paid by the owner.~ Thus, analyses using depreciation should be conducted in nominal dollars. For an analysis that does not include tax effects, None should be selected.
+
+The default value is None.
+
+An example of this object in an IDF:
+
+\begin{lstlisting}
+
+LifeCycleCost:Parameters,
+      TypicalLCC,              !- Name
+      EndOfYear,               !- Discounting Convention
+      ConstantDollar,          !- Inflation Approach
+      0.034314,                !- Real Discount Rate
+      ,                        !- Nominal Discount Rate
+      ,                        !- Inflation
+      January,                 !- Base Date Month
+      2010,                    !- Base Date Year
+      January,                 !- Service Date Month
+      2010,                    !- Service Date Year
+      25,                      !- Length of Study Period in Years
+      0.39,                    !- Tax rate
+      StraightLine-39year;     !- Depreciation Method
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/energyplus-economics/lifecyclecost-recurringcosts.tex b/doc/input-output-reference/src/energyplus-economics/lifecyclecost-recurringcosts.tex
new file mode 100644
index 00000000000..47e7497e347
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/lifecyclecost-recurringcosts.tex
@@ -0,0 +1,87 @@
+\section{LifeCycleCost:RecurringCosts}\label{lifecyclecostrecurringcosts}
+
+Recurring costs are costs that repeat over time on a regular schedule during the study period. If costs associated with equipment do repeat but not on a regular schedule, use LifeCycleCost:NonrecurringCost objects instead. Costs related to energy usage are not included here. The UtilityCost:Tariff and other UtilityCost objects can be used to compute energy costs that are automatically included in the life-cycle cost calculations
+
+\subsection{Inputs}\label{inputs-059}
+
+\paragraph{Field: Name}\label{field-name-057}
+
+The identifier used for the object. The name is used in identifying the cash flow equivalent in the output results in the Life-Cycle Cost Report.
+
+\paragraph{Field: Category}\label{field-category-000}
+
+Enter the category of the recurring costs. Choose the closest category. The options include:
+
+\begin{itemize}
+\item
+  Maintenance
+\item
+  Repair
+\item
+  Operation
+\item
+  Replacement
+\item
+  MinorOverhaul
+\item
+  MajorOverhaul
+\item
+  OtherOperational
+\end{itemize}
+
+The default value is Maintenance.
+
+For recommendations on estimating other operational costs, see NIST 135 Section 4.6.3.
+
+\paragraph{Field: Cost}\label{field-cost-000}
+
+Enter the cost in dollars (or the appropriate monetary unit) for the recurring costs. Enter the cost for each time it occurs. For example, if the annual maintenance cost is \$500, enter 500 here.
+
+\paragraph{Field: Start of Costs}\label{field-start-of-costs-000}
+
+Enter when the costs start. The First Year of Cost is based on the number of years past the Start of Costs. For most maintenance costs, the Start of Costs should be Service Period. The options are:
+
+\begin{itemize}
+\item
+  ServicePeriod
+\item
+  BasePeriod
+\end{itemize}
+
+The default value is ServicePeriod.
+
+\paragraph{Field: Years From Start}\label{field-years-from-start-000}
+
+This field and the Months From Start field together represent the time from either the start of the Service Period, on the service month and year, or start of the Base Period, on the base month and year (depending on the Start of Costs field) that the costs start to occur. Normally, for most maintenance costs that begin in the first year that the equipment is in service the Start of Costs is the Service Period and the Years from Start will be 0. Only integers should be entered representing whole years. The default value is 0.
+
+\paragraph{Field: Months From Start}\label{field-months-from-start-000}
+
+This field and the Years From Start field together represent the time from either the start of the Service Period, on the service month and year, or start of the Base Period, on the base month and year (depending on the Start of Costs field) that the costs start to occur. Normally, for most maintenance costs the Start of Costs is the Service Period and the Months from Start will be 0. Only integers should be entered representing whole months. The Years From Start (times 12) and Months From Start are added together. The default value is 0.
+
+\paragraph{Field: Repeat Period Years}\label{field-repeat-period-years}
+
+This field and the Repeat Period Months field indicate how much time elapses between reoccurrences of the cost. For costs that occur every year, such as annual maintenance costs, the Repeat Period Years should be 1 and Repeat Period Months should be 0. Only integers should be entered representing whole years. The default value is 1.
+
+\paragraph{Field: Repeat Period Months}\label{field-repeat-period-months}
+
+This field and the Repeat Period Years field indicate how much time elapses between reoccurrences of the cost. For costs that occur every year the Repeat Period Years should be 1 and Repeat Period Months should be 0. For, costs that occur every eighteen months, the Repeat Period Years should be 1 and the Repeat Period Months should be 6. Only integers should be entered representing whole years. The Repeat Period Years (times 12) and Repeat Period Months are added together. The default value is 0.
+
+\paragraph{Field: Annual Escalation Rate}\label{field-annual-escalation-rate}
+
+Enter the annual escalation rate as a decimal. For a 1\% rate, enter the value 0.01. This input is used when the Inflation Approach is CurrentDollar. When Inflation Approach is set to ConstantDollar this input is ignored. The default value is 0.
+
+An example of this object in an IDF:
+
+\begin{lstlisting}
+
+LifeCycleCost:RecurringCosts,
+      AnnualMaint,             !- Name
+      Maintenance,             !- Category
+      2000,                    !- Cost
+      ServicePeriod,           !- Start of Costs
+      0,                       !- Years from Start
+      0,                       !- Months from Start
+      1,                       !- Repeat Period Years
+      0,                       !- Repeat Period Months
+      0;                       !- Annual escalation rate
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/energyplus-economics/lifecyclecost-useadjustment.tex b/doc/input-output-reference/src/energyplus-economics/lifecyclecost-useadjustment.tex
new file mode 100644
index 00000000000..799bbc01852
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/lifecyclecost-useadjustment.tex
@@ -0,0 +1,77 @@
+\section{LifeCycleCost:UseAdjustment}\label{lifecyclecostuseadjustment}
+
+Used by advanced users to adjust the energy or water use costs for future years. This should not be used for compensating for inflation but should only be used to increase the costs of energy or water based on assumed changes to the actual use of water or energy, such as due to changes in the future function of the building or the impact of future adjacent buildings on energy use. This object is not commonly used and should be used with caution. The adjustments begin at the start of the service period.
+
+\subsection{Inputs}\label{inputs-060}
+
+\paragraph{Field: Name}\label{field-name-058}
+
+The identifier used for the object.
+
+\paragraph{Field: Resource}\label{field-resource}
+
+Enter the resource such as:
+
+\begin{itemize}
+\item
+  Electricity
+\item
+  NaturalGas
+\item
+  Steam
+\item
+  Gasoline
+\item
+  Diesel
+\item
+  Coal
+\item
+  FuelOil \#1
+\item
+  FuelOil \#2
+\item
+  Propane
+\item
+  Water
+\end{itemize}
+
+\paragraph{Field: Year 1 multiplier}\label{field-year-1-multiplier}
+
+The multiplier to be applied to the end use cost for the first year in the service period. The total utility costs for the selected end use is multiplied by this value. For no change enter 1.0.
+
+\paragraph{Field: Year N multiplier}\label{field-year-n-multiplier}
+
+The multiplier to be applied to the end use cost for each following year. The total utility costs for the selected end use is multiplied by this value. For no change enter 1.0.~ This object is extensible and often includes 25 to 50 years of values.
+
+An example of this object in an IDF:
+
+\begin{lstlisting}
+LifeCycleCost:UseAdjustment,
+  ElecAdjustment,       !- Name
+  Electricity,          !- Resource
+  1.0000,               !- Year 1 Multiplier
+  1.0022,               !- Year 2 Multiplier
+  1.0023,               !- Year 3 Multiplier
+  1.0024,               !- Year 4 Multiplier
+  1.0025,               !- Year 5 Multiplier
+  1.0026,               !- Year 6 Multiplier
+  1.0027;               !- Year 7 Multiplier
+\end{lstlisting}
+
+\subsubsection{CurrencyType}\label{currencytype}
+
+By default, the predefined reports related to economics use the \$ symbol. If a different symbol should be shown in the predefined reports to represent the local currency this object can be used. If the object is not used, the \$ sign is used in the reports. Only one CurrencyType object is allowed in the input file.
+
+\paragraph{Field: Monetary Unit}\label{field-monetary-unit}
+
+The commonly used three letter currency code for the units of money for the country or region. Based on ISO 4217 currency codes. Common currency codes are USD for the U.S. Dollar represented with `\$' and EUR for Euros represented with `€'. The three letter currency codes can be seen at the following web sites (as of 2008):
+
+http://www.iso.org/iso/support/faqs/faqs\_widely\_used\_standards/widely\_used\_standards\_other/currency\_codes/currency\_codes\_list-1.htm
+
+http://www.xe.com/symbols.php
+
+When a three letter currency code is specified, the HTML file will use either an ASCII character if available or one or more UNICODE characters. Since not all browsers and all fonts used by browsers completely support UNICODE, not all currency symbols may be rendered correctly. If a box or a box with four small letters appears, this indicates that the browser and its fonts do not support a specific UNICODE character.
+
+For text reports, an ASCII representation of the currency code will be used. Since ASCII is much more limited than UNICODE, many times the three letter currency code will be shown in the reports.
+
+Since forms of currency change, please contact EnergyPlus support if a new currency code and symbol are needed.
diff --git a/doc/input-output-reference/src/energyplus-economics/lifecyclecost-usepriceescalation.tex b/doc/input-output-reference/src/energyplus-economics/lifecyclecost-usepriceescalation.tex
new file mode 100644
index 00000000000..e6e124de2df
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/lifecyclecost-usepriceescalation.tex
@@ -0,0 +1,132 @@
+\section{LifeCycleCost:UsePriceEscalation}\label{lifecyclecostusepriceescalation}
+
+The LifeCycleCost:UsePriceEscalation object will commonly be part of a dataset on life cycle costs. The values for this object may be found in the annual supplement to NIST Handbook 135 in Tables Ca-1 to Ca-5. A dataset file comes with EnergyPlus in the DataSet directory and includes the LCCusePriceEscalationDataSetXXXX.idf file which includes the value for the supplement to NIST 135 from the year indicated. The object provides inputs for the escalations of energy and water costs assuming that they change differently than inflation. According to the NIST 135 supplement the values are ``present projected fuel price indices for the four Census regions and for the United States. These indices, when multiplied by annual energy costs computed at base-date prices provide estimates of future-year costs in constant base-date dollars. Constant-dollar cost estimates are needed when discounting is performed with a real discount rate (i.e., a rate that does not include general price inflation).''
+
+The LCCusePriceEscalationDataSetXXXX.idf is periodically updated by the EnergyPlus development team using data available from NIST along with a spreadsheet to convert that data into an IDF dataset file. The NIST 135 annual supplement is available from NIST or through US DOE FEMP program.
+
+http://www1.eere.energy.gov/femp/program/lifecycle.html
+
+If requested, NIST personnel will provide a file called ENCOSTxx.TXT which contains the data used to create Table Ca-1 to Table Ca-5 in the supplement. To convert the data in the ENCOSTxx.TXT file to an IDF file, open the ENCOSTxx.TXT file in a text editor and copy the entire contents into the first tab called ``Step 1'' of the conversion spreadsheet. The conversion spreadsheet file named ConvertENCOSTtoEnergyPlusLifeCycleCost.xls is available upon request from the EnergyPlus development team. The ``Step 2'' tab separates the data into columns. The ``Step 3'' tab computes ratios that are the same as Table Ca-1 to Table C1-6 in the supplement. Checking these values against what appears in the printed supplement is recommended. The ``Step 4'' and ``Step 5'' tabs rearrange the data and the ``Step 6'' tab shows the data in a format that can be easily copied and pasted into a new idf dataset file. The final step requires using your text editor to replace the fuel names with those used by EnergyPlus. The replacement names are listed on the ``FuelNameConversion'' tab.
+
+\subsection{Inputs}\label{inputs-061}
+
+\paragraph{Field: Name}\label{field-name-059}
+
+The identifier used for the object. The name usually identifies the location (such as the state, region, country or census area) that the escalations apply to. In addition the name should identify the building class such as residential, commercial, or industrial and the use type such as electricity, natural gas, or water.
+
+\paragraph{Field: Resource}\label{field-resource-000}
+
+Enter the resource such as:
+
+\begin{itemize}
+\item
+  Electricity
+\item
+  FuelOil\#1
+\item
+  NaturalGas
+\item
+  PropaneGas
+\item
+  FuelOil\#2
+\item
+  Coal
+\item
+  Steam
+\item
+  Gasoline
+\item
+  Diesel
+\item
+  Water
+\end{itemize}
+
+\paragraph{Field: Escalation Start Year}\label{field-escalation-start-year}
+
+This field and the Escalation Start Month define the time that corresponds to ``Year 1 Escalation'' such as a year expressed in four digits like ``2013'', when the escalation rates are applied. This field and the Escalation Start Month define the time that escalation begins.
+
+\paragraph{Field: Escalation Start Month}\label{field-escalation-start-month}
+
+This field and the Escalation Start Year define the time that corresponds to ``Year 1 Escalation'' such as~ a year expressed in four digits such as ``2013'', when the escalation rates are applied. This field and the Escalation Start Year define the time that escalation begins.
+
+The choices are:
+
+\begin{itemize}
+\item
+  January
+\item
+  February
+\item
+  March
+\item
+  April
+\item
+  May
+\item
+  June
+\item
+  July
+\item
+  August
+\item
+  September
+\item
+  October
+\item
+  November
+\item
+  December
+\end{itemize}
+
+The default value is January. According to NIST Handbook 135:
+
+\paragraph{Field: Year 1 Escalation}\label{field-year-1-escalation}
+
+The escalation in price of the energy or water use for the first year expressed as a decimal.
+
+\paragraph{Field: Year n Escalation}\label{field-year-n-escalation}
+
+The escalation in price of the energy or water use for the n-th year expressed as a decimal. This object is extensible and often includes 25 to 50 years of projected values.
+
+If the number of years in LifeCycleCost:UsePriceEscalation is less than the number of years in the analysis period, the remaining years will assume no escalation. Normal inflation will be the only affect for these years.
+
+An example of this object in an IDF:
+
+\begin{lstlisting}
+
+LifeCycleCost:UsePriceEscalation,
+      NorthEast  Residential-Electricity,  !- Name
+      Electricity,                         !- Resource
+      2010,                                !- Escalation Start Year
+      January,                             !- Escalation Start Month
+      0.9374,                              !- Year 1 Escalation
+      0.9790,                              !- Year 2 Escalation
+      1.0138,                              !- Year 3 Escalation
+      1.0127,                              !- Year 4 Escalation
+      1.0096,                              !- Year 5 Escalation
+      1.0177,                              !- Year 6 Escalation
+      1.0279,                              !- Year 7 Escalation
+      1.0334,                              !- Year 8 Escalation
+      1.0327,                              !- Year 9 Escalation
+      1.0382,                              !- Year 10 Escalation
+      1.0454,                              !- Year 11 Escalation
+      1.0494,                              !- Year 12 Escalation
+      1.0564,                              !- Year 13 Escalation
+      1.0587,                              !- Year 14 Escalation
+      1.0549,                              !- Year 15 Escalation
+      1.0566,                              !- Year 16 Escalation
+      1.0630,                              !- Year 17 Escalation
+      1.0707,                              !- Year 18 Escalation
+      1.0857,                              !- Year 19 Escalation
+      1.0953,                              !- Year 20 Escalation
+      1.1063,                              !- Year 21 Escalation
+      1.1165,                              !- Year 22 Escalation
+      1.1227,                              !- Year 23 Escalation
+      1.1292,                              !- Year 24 Escalation
+      1.1349,                              !- Year 25 Escalation
+      1.1414,                              !- Year 26 Escalation
+      1.1480,                              !- Year 27 Escalation
+      1.1550,                              !- Year 28 Escalation
+      1.1617,                              !- Year 29 Escalation
+      1.1686;                              !- Year 30 Escalation
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/energyplus-economics/utilitycost-charge-block.tex b/doc/input-output-reference/src/energyplus-economics/utilitycost-charge-block.tex
new file mode 100644
index 00000000000..e06d5a37070
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/utilitycost-charge-block.tex
@@ -0,0 +1,79 @@
+\section{UtilityCost:Charge:Block}\label{utilitycostchargeblock}
+
+The UtilityCost:Charge:Block objects is also used extensively for tariff calculation. It is used to compute energy and demand charges that are structured in blocks of charges. It may also be used for taxes, surcharges and any other charges that occur on a utility bill but those are more commonly simple flat charges so UtilityCost:Charge:Simple ~is more commonly used for those functions. As many UtilityCost:Charge:Block objects as needed may be defined for a single tariff and they will be added together. Blocks are a structure used by almost all utilities for calculating energy and demand charges and they allow the utility to charge more or less per unit of energy or demand if more units are used.
+
+\subsection{Inputs}\label{inputs-067}
+
+\paragraph{Field: Charge Variable Name}\label{field-charge-variable-name}
+
+This is the name associated with the UtilityCost:Charge:Block object and will appear in the report. In addition, the results of the UtilityCost:Charge:Block are stored in a variable with the same name. That way, the results may be used for further calculation.
+
+\paragraph{Field: Tariff Name}\label{field-tariff-name}
+
+The name of the tariff that this UtilityCost:Charge:Block is associated with.
+
+\paragraph{Field: Source Variable}\label{field-source-variable}
+
+The name of the source used by the UtilityCost:Charge:Block. This is usually the name of the variable holding the energy or demand but may also be the name of any variable including the subtotal or basis if other charges are based on those.
+
+\paragraph{Field: Season}\label{field-season}
+
+This is the name (or number) of a season for which the ~UtilityCost:Charge:Block is calculated. If this is set to annual, the calculations are performed for the UtilityCost:Charge:Block for the entire year (all months) otherwise it is calculated only for those months in the season defined. The season is defined by the Season Schedule in the UtilityCost:Tariff object. The choices for seasons are the following names or numbers may be used:
+
+\begin{itemize}
+\item
+  Annual
+\item
+  Summer
+\item
+  Winter
+\item
+  Spring
+\item
+  Fall
+\end{itemize}
+
+\paragraph{Field: Category Variable Name}\label{field-category-variable-name}
+
+All charges get added somewhere in the hierarchy described in the introduction to EnergyPlus economics above. This field shows where the charge should be added. The reason to enter this field appropriately is so that the charge gets reported in a reasonable category. The charge automatically gets added to the variable that is the category. The choices for this field are limited to:
+
+\begin{itemize}
+\item
+  EnergyCharges
+\item
+  DemandCharges
+\item
+  ServiceCharges
+\item
+  Basis
+\item
+  Adjustment
+\item
+  Surcharge
+\item
+  Subtotal
+\item
+  Taxes
+\item
+  Total
+\item
+  NotIncluded
+\end{itemize}
+
+\paragraph{Field: Remaining Into Variable}\label{field-remaining-into-variable}
+
+If the blocks do not use all of the energy or demand from the source, some energy and demand remains, then the remaining amount should be assigned to a variable. If no variable is assigned and some amount of energy or demand is not used in the block structure a warning will be issued.
+
+\paragraph{Field: Block Size Multiplier Value or Variable Name}\label{field-block-size-multiplier-value-or-variable-name}
+
+The sizes of the blocks are usually used directly but if a value or a variable is entered here, the block sizes entered in the rest of the charge are first multiplied by the entered value prior to being used. This is common for rates that are kWh/kW rates and in that case the variable that holds the monthly total electric demand would be entered. If no value is entered, a default value of one is assumed so that the block sizes remain exactly as entered. This field is unusual for the EnergyPlus syntax because it can be either a number or a name of a variable.
+
+\paragraph{Field: Block Size 1 Value or Variable Name}\label{field-block-size-1-value-or-variable-name}
+
+The size of the first block of the charges is entered here. For most rates that use multiple blocks, this will be the value for the first block size. Additional block sizes are entered with every other field. A default variable named ``remaining'' contains a large value and this may be used when the remaining amount should be included in that block. This field and the next field may be repeated in groups of two for as many blocks as are defined. This field is unusual for the EnergyPlus syntax because it can be either a number or a name of a variable.
+
+\paragraph{Field: Block 1 Cost per Unit Value or Variable Name}\label{field-block-1-cost-per-unit-value-or-variable-name}
+
+The cost of the first block. This value is also repeated for every other field in the charge. As many blocks may be entered as are needed. This field and the previous field may be repeated in groups of two for as many blocks as are defined. This field is unusual for the EnergyPlus syntax because it can be either a number or a name of a variable. For SellToUtility tariffs, the values in this field are usually expressed as negative numbers.
+
+These last two fields may be repeated fifteen times. If more blocks are defined by the utility, the computation can be continued using another UtilityCost:Charge:Block and using the variable from Remaining Into Variable as the source variable.
diff --git a/doc/input-output-reference/src/energyplus-economics/utilitycost-charge-simple.tex b/doc/input-output-reference/src/energyplus-economics/utilitycost-charge-simple.tex
new file mode 100644
index 00000000000..0fe7d634750
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/utilitycost-charge-simple.tex
@@ -0,0 +1,65 @@
+\section{UtilityCost:Charge:Simple}\label{utilitycostchargesimple}
+
+The UtilityCost:Charge:Simple is one of the most often used objects for tariff calculation. It is used to compute energy and demand charges that are very simple. It may also be used for taxes, surcharges and any other charges that occur on a utility bill. As many UtilityCost:Charge:Simple objects as needed may be defined for a single tariff and they will be added together.
+
+\subsection{Inputs}\label{inputs-068}
+
+\paragraph{Field: Charge Variable Name}\label{field-charge-variable-name-000}
+
+This is the name associated with the UtilityCost:Charge:Simple object and will appear in the report. In addition, the results of the UtilityCost:Charge:Simple calculation are stored in a variable with the same name. That way, the results may be used for further calculation. Spaces are not significant in Charge Variable Names. They are removed during the utility bill calculation process.
+
+\paragraph{Field: Tariff Name}\label{field-tariff-name-000}
+
+The name of the tariff that this UtilityCost:Charge:Simple is associated with.
+
+\paragraph{Field: Source Variable}\label{field-source-variable-000}
+
+The name of the source used by the UtilityCost:Charge:Simple. This is usually the name of the variable holding the energy or demand but may also be the name of any variable including the subtotal or basis if other charges are based on those.
+
+\paragraph{Field: Season}\label{field-season-000}
+
+This is the name (or number) of a season for which the UtilityCost:Charge:Simple is calculated. If this is set to Annual, the calculations are performed for the UtilityCost:Charge:Simple for the entire year (all months) otherwise it is calculated only for those months in the season defined. The season is defined by the Season Schedule in the UtilityCost:Tariff object. The choices for seasons are the following names or numbers may be used:
+
+\begin{itemize}
+\item
+  Annual
+\item
+  Winter
+\item
+  Spring
+\item
+  Summer
+\item
+  Fall
+\end{itemize}
+
+\paragraph{Field: Category Variable Name}\label{field-category-variable-name-000}
+
+All charges get added somewhere in the hierarchy described in the introduction to EnergyPlus economics above. This field shows where the charge should be added. The reason to enter this field appropriately is so that the charge gets reported in a reasonable category. The charge automatically gets added to the variable that is the category. The choices for this field are limited to:
+
+\begin{itemize}
+\item
+  EnergyCharges
+\item
+  DemandCharges
+\item
+  ServiceCharges
+\item
+  Basis
+\item
+  Adjustment
+\item
+  Surcharge
+\item
+  Subtotal
+\item
+  Taxes
+\item
+  Total
+\item
+  NotIncluded
+\end{itemize}
+
+\paragraph{Field: Cost per Unit Value or Variable Name}\label{field-cost-per-unit-value-or-variable-name}
+
+This field contains either a single number or the name of a variable. The number is multiplied with all of the energy or demand or other source that is specified in the source field. If a variable is used, then the monthly values of the variable are multiplied against the variable specified in the source field. This field makes it easy to include a simple charge without specifying block sizes. It is added to any of the block calculations (see later fields) but is most often used by itself. If no value or variable is entered, a zero is assumed. This is a good way to include a tax or cost adjustment. For SellToUtility tariffs, the values in this field are usually expressed as negative numbers.
diff --git a/doc/input-output-reference/src/energyplus-economics/utilitycost-computation.tex b/doc/input-output-reference/src/energyplus-economics/utilitycost-computation.tex
new file mode 100644
index 00000000000..2f495c15d2d
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/utilitycost-computation.tex
@@ -0,0 +1,19 @@
+\section{UtilityCost:Computation}\label{utilitycostcomputation}
+
+The UtilityCost:Computation object lists a series of computations that are used to perform the bill calculation. The object is only used for complex tariffs that cannot be modeled any other way. For 95\% of the utility tariffs, using UtilityCost:Computation is unnecessary and should be avoided. If the UtilityCost:Computation object is used, it must contain references to all objects involved in the rate in the order that they should be computed.
+
+\subsection{Inputs}\label{inputs-069}
+
+\paragraph{Field: Name}\label{field-name-062}
+
+The name of the UtilityCost:Computation.
+
+\paragraph{Field: Tariff Name}\label{field-tariff-name-001}
+
+The name of the tariff that this UtilityCost:Charge:Simple is associated with.
+
+\paragraph{Field: Compute Step N}\label{field-compute-step-n}
+
+The Compute Step fields contain a simple language that describes the steps used in the computation process similar to a programming language. If no entry is made to any Compute Step fields (as usually the case) a default method of computing the rates shall be used. Compute Step is described later in this section under Complex Tariff Modeling.
+
+Remember, this object should be omitted for almost all tariffs.
diff --git a/doc/input-output-reference/src/energyplus-economics/utilitycost-qualify.tex b/doc/input-output-reference/src/energyplus-economics/utilitycost-qualify.tex
new file mode 100644
index 00000000000..e12a29cc819
--- /dev/null
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@@ -0,0 +1,63 @@
+\section{UtilityCost:Qualify}\label{utilitycostqualify}
+
+Many utilities provide a large number of tariffs and separate their customers by the amount of energy use they have or by the amount of demand. The qualify object allows only certain tariffs that are modeled to be used. If the results of the simulation fall outside of the range of qualifications, that tariff is still calculated but the ``Qualified'' entry will say ``No'' and the UtilityCost:Qualify that caused its exclusion is shown. When multiple tariffs from the same utility are modeled and only one of them should be used, make sure that the qualifiers are consistent especially within the same GroupName (see UtilityCost:Tariff). Multiple UtilityCost:Qualify objects can appear for a specific rate and they can be based on any variable.
+
+The energy used and demands for each month vary. Since it is possible that they vary across the minimum and maximum values defined by this object, a choice in how to treat the thresholds is necessary. Say that a utility has two tariffs, a small tariff that has a maximum demand requirement of 50kW and a large tariff that has a minimum demand requirement of 50kW. If the use for a building goes above the 50kW threshold during some summer months and the rest of the time is below 50kW, then how does the utility choose which rate would qualify. The utility probably has very specific requirements about which months or consecutive months can be above or below a threshold to qualify for the rate.
+
+\subsection{Inputs}\label{inputs-070}
+
+\paragraph{Field: Name}\label{field-name-063}
+
+The name used for the UtilityCost:Qualify and displayed if the tariff does not qualify. It is also treated as a variable and contains:
+
+\begin{itemize}
+\item
+  1 for each month that does qualify,
+\item
+  0 for months that do not qualify, and
+\item
+  -1 for months that are not part of the season selected.
+\end{itemize}
+
+\paragraph{Field: Tariff Name}\label{field-tariff-name-002}
+
+The name of the UtilityCost:Tariff object that is associated with this UtilityCost:Qualify object.
+
+\paragraph{Field: Variable Name}\label{field-variable-name-001}
+
+The name of the variable used. For energy and demand, the automatically created variables, totalEnergy and totalDemand should be used, respectively.
+
+\paragraph{Field: Qualify Type}\label{field-qualify-type}
+
+Enter either ``Minimum'' or ``Maximum''.
+
+\paragraph{Field: Threshold Value or Variable Name}\label{field-threshold-value-or-variable-name}
+
+The minimum or maximum value for the qualify. If the variable has values that are less than this value when the qualify type is minimum then the tariff may be disqualified. If the variable has values that are greater than this value when the qualify type is maximum then the tariff may be disqualified. For demand, it is still the minimum of the demands set each month even though the demands are, by definition, the peak value for the month. Depending on the threshold test entry (see below) this minimum applies to all months, some of the months, or just a single month.
+
+\paragraph{Field: Season}\label{field-season-001}
+
+If the UtilityCost:Qualify only applies to a season, enter the season name from the following list:
+
+\begin{itemize}
+\item
+  Annual
+\item
+  Winter
+\item
+  Spring
+\item
+  Summer
+\item
+  Fall
+\end{itemize}
+
+If this field is left blank, it defaults to Annual.
+
+\paragraph{Field: Threshold Test}\label{field-threshold-test}
+
+Enter either ``Count'' or ``Consecutive''. Uses the number in Number of Months in one of two different ways depending on the Threshold Test. If the Threshold Test is set to ``Count'' then the qualification is based on the count of the total number of months per year. If the Threshold Test is set to ``Consecutive'' then the qualification is based on a consecutive number of months. If left blank this field defaults to count and it should be allowed to default for most cases.
+
+\paragraph{Field: Number of Months}\label{field-number-of-months}
+
+A number from 1 to 12. If no value entered, 12 is assumed when the qualify type is minimum and 1 when the qualify type is maximum. This is the number of months that the threshold test applies to determine if the rate qualifies or not. If the season is less than 12 months (if it is not annual) then the value is automatically reduced to the number of months of the season.
diff --git a/doc/input-output-reference/src/energyplus-economics/utilitycost-ratchet.tex b/doc/input-output-reference/src/energyplus-economics/utilitycost-ratchet.tex
new file mode 100644
index 00000000000..4b52e1e9550
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/utilitycost-ratchet.tex
@@ -0,0 +1,109 @@
+\section{UtilityCost:Ratchet}\label{utilitycostratchet}
+
+The UtilityCost:Ratchet command allows the modeling of tariffs that include some type of seasonal ratcheting. Ratchets are most common when used with electric demand charges. A ratchet is when a utility requires that the demand charge for a month with a low demand may be increased to be more consistent with a month that set a higher demand charge.
+
+While the details of the UtilityCost:Ratchet command are described further in this section, an example is probably the easiest way to learn the basic functions.
+
+Ratchet Example: A utility has a single ratchet that says that the billing demand for each month of the year is the higher value of the actual demand or 60\% of the peak summer demand
+
+\begin{lstlisting}
+
+UtilityCost:Ratchet,
+    BillingDemand1,   ! Ratchet Variable Name
+    ExampleTariff1,   ! Tariff Name
+    TotalDemand,      ! Baseline Source Variable
+    TotalDemand,      ! Adjustment Source Variable
+    Summer,           ! Season From
+    Annual,           ! Season To
+    0.60,             ! Multiplier Value or Variable Name
+    0;                ! Offset Value or Variable Name
+\end{lstlisting}
+
+The Ratchet Variable Name (the first field) should be used wherever the ratchet should be applied and is often the source variable for UtilityCost:Charge:Simple or UtilityCost:Charge:Block.
+
+The detailed steps taken for the ratchet are the following:
+
+\begin{itemize}
+\item
+  AdjSeasonal contains either:
+\item
+  When SeasonFrom is not set to Monthly, the maximum for all months in Season From in the Adjustment Source Variable. This is a single value.
+\item
+  When SeasonFrom is set to Monthly, the monthly values of the Adjustment Source Variable.
+\item
+  AdjPeak = (AdjSeasonal + Offset) * Multiplier
+\item
+  MaxAdjBase = maximum value of either AdjPeak or Baseline Source Variable
+\item
+  The resulting Ratchet Variable contains:
+\item
+  For months not in SeasonTo, the values of Baseline Source Variable
+\item
+  For months in SeasonTo, the values of MaxAdjBase
+\end{itemize}
+
+If multiple ratchets occur in the same tariff, multiple UtilityCost:Ratchet commands should be ``chained'' together with the Baseline Source Variable subsequent ratchets referencing the Ratchet Variable Name of the previous UtilityCost:Ratchet.
+
+Since the ratchet command can add together two variables, mutliply two variables, or take the maximum value between two variables, it may be used for other difficult to model tariffs without needing to use UtilityCost:Computation. Clever use of UtilityCost:Ratchet should be well documented with comments.
+
+\subsection{Inputs}\label{inputs-071}
+
+\paragraph{Field: Ratchet Variable Name}\label{field-ratchet-variable-name}
+
+The name of the ratchet and the name of the result of this single ratchet.
+
+\paragraph{Field: Tariff Name}\label{field-tariff-name-003}
+
+The name of the tariff that this UtilityCost:Ratchet is associated with.
+
+\paragraph{Field: Baseline Source Variable}\label{field-baseline-source-variable}
+
+The name of the variable used as the baseline value. When the ratcheted value exceeds the baseline value for a month the ratcheted value is used but when the baseline value is greater then the ratcheted value the baseline value is used. Usually the electric demand charge is used. The baseline source variable can be the results of another ratchet object. This allows utility tariffs that have multiple ratchets to be modeled.
+
+\paragraph{Field: Adjustment Source Variable}\label{field-adjustment-source-variable}
+
+The variable that the ratchet is calculated from. It is often but not always the same as the baseline source variable. The ratcheting calculations using offset and multiplier are using the values from the adjustment source variable. If left blank, the adjustment source variable is the same as the baseline source variable.
+
+\paragraph{Field: Season From}\label{field-season-from}
+
+The name of the season that is being examined. The maximum value for all of the months in the named season is what is used with the multiplier and offset. This is most commonly Summer or Annual. When Monthly is used, the adjustment source variable is used directly for all months.
+
+\begin{itemize}
+\item
+  Annual
+\item
+  Winter
+\item
+  Spring
+\item
+  Summer
+\item
+  Fall
+\item
+  Monthly
+\end{itemize}
+
+\paragraph{Field: Season To}\label{field-season-to}
+
+The name of the season when the ratchet would be calculated. This is most commonly Winter. The ratchet only is applied to the months in the named season. The resulting variable for months not in the Season To selection will contain the values as appear in the baseline source variable.
+
+\begin{itemize}
+\item
+  Annual
+\item
+  Winter
+\item
+  Spring
+\item
+  Summer
+\item
+  Fall
+\end{itemize}
+
+\paragraph{Field: Multiplier Value or Variable Name}\label{field-multiplier-value-or-variable-name}
+
+Often the ratchet has a clause such as ``the current month demand or 90\% of the summer month demand''. For this case a value of 0.9 would be entered here as the multiplier. This value may be left blank if no multiplier is needed and a value of one will be used as a default.
+
+\paragraph{Field: Offset Value or Variable Name}\label{field-offset-value-or-variable-name}
+
+A less common strategy is to say that the ratchet must be all demand greater than a value, in this case an offset that is added to the demand may be entered here. If entered, it is common for the offset value to be negative representing that the demand be reduced.~ If no value is entered it is assumed to be zero and not affect the ratchet.
diff --git a/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff-examples.tex b/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff-examples.tex
new file mode 100644
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--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff-examples.tex
@@ -0,0 +1,589 @@
+\section{UtilityCost:Tariff Examples}\label{utilitycosttariff-examples}
+
+One of the best ways to learn the details of EnergyPlus Economics is to see some example tariffs and how they translate into objects. To do this, several different rates of increasing complexity are shown in the following examples.
+
+Another source of examples is the large set of tariff input objects provided with EnergyPlus in the macro data set file called ``UtilityTariffObjects.imf'' located in the ``MacroDataSets'' folder where EnergyPlus is installed. This file contains sets of objects that fully define tariffs for commercial customers from a collection of U.S. utility companies.
+
+\subsubsection{Example A -- Flat Energy Charge}\label{example-a-flat-energy-charge}
+
+As an example of the simplest type of tariff.
+
+Customer Charge: \$2.51 per month
+
+Energy Charge:~~~ 5.5342 cents/kWh
+
+This tariff would use a single UtilityCost:Charge:Simple object. The monthly charge is part of the UtilityCost:Tariff object.
+
+\begin{lstlisting}
+
+UtilityCost:Tariff,
+    ExampleA,                     ! Name
+    Electricity:Facility,         ! Output Meter Name
+    kWh,                          ! Conversion Factor Choice
+    ,                             ! Energy Conversion Factor
+    ,                             ! Demand Conversion Factor
+    ,                             ! Time of Use Period Schedule Name
+    ,                             ! Season Schedule Name
+    ,                             ! Month Schedule Name
+    ,                             ! Demand Window Length
+    2.51;                         ! Monthly Charge or Variable Name
+
+
+  UtilityCost:Charge:Simple,
+    FlatEnergyCharge,             ! Charge Variable Name
+    ExampleA,                     ! Tariff Name
+    totalEnergy,                  ! Source Variable
+    Annual,                       ! Season
+    EnergyCharges,                ! Category Variable Name
+    0.055342;                     ! Cost Per Unit Value or Variable Name
+\end{lstlisting}
+
+\subsubsection{Example B -- Block Energy Charge}\label{example-b-block-energy-charge}
+
+Another simple type of tariff is one where the energy charges vary by the amount of energy consumed each month.
+
+Customer Charge:~~~ \$5.75 per month
+
+Energy Charge:~~~~~~~ 7.231 cents/kWh for first 200 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 6.656 cents/kWh for next 1000 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 5.876 cents/kWh for over 1200 kWh
+
+This tariff would use a single UtilityCost:Charge:Block object. The monthly charge is part of the UtilityCost:Tariff object. Note that the block sizes are every other field at the bottom of the object and the that final block size references a built in variable called ``remaining'' that contains a very large number.
+
+\begin{lstlisting}
+
+UtilityCost:Tariff,
+    ExampleB,                     ! Name
+    Electricity:Facility,         ! Output Meter Name
+    kWh,                          ! Conversion Factor Choice
+    ,                             ! Energy Conversion Factor
+    ,                             ! Demand Conversion Factor
+    ,                             ! Time of Use Period Schedule Name
+    ,                             ! Season Schedule Name
+    ,                             ! Month Schedule Name
+    ,                             ! Demand Window Length
+    5.75;                         ! Monthly Charge or Variable Name
+
+
+  UtilityCost:Charge:Block,
+    BlockEnergyCharge,            ! Charge Variable Name
+    ExampleB,                     ! Tariff Name
+    totalEnergy,                  ! Source Variable
+    Annual,                       ! Season
+    EnergyCharges,                ! Category Variable Name
+    ,                             ! Remaining Into Variable
+    ,                             ! Block Size Multiplier Value or Variable Name
+    200,                          ! Block Size 1 Value or Variable Name
+    0.07231,                      ! Block 1 Cost per Unit Value or Variable Name
+    1000,                         ! Block Size 2 Value or Variable Name
+    0.06656,                      ! Block 2 Cost per Unit Value or Variable Name
+    remaining,                    ! Block Size 3 Value or Variable Name
+    0.05876;                      ! Block 3 Cost per Unit Value or Variable Name
+\end{lstlisting}
+
+\subsubsection{Example C -- Block Energy and Demand Charges}\label{example-c-block-energy-and-demand-charges}
+
+This example contains both a block for energy and a block for demand and is very similar to the previous example except it now includes demand charges as well. The energy and demand charges vary by the amount of energy and demand consumed each month.
+
+Energy Charge:~~~~~~~ 4.74 cents/kWh for first 20,000 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 4.24 cents/kWh for next 180,000 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 3.83 cents/kWh for additional kWh
+
+Demand Charge:~~~~~ 5.38 dollars per kW for first 20 kW
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 4.23 dollars per kW for next 80 kW
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 3.60 dollars per kW for additional kW
+
+This tariff would use two UtilityCost:Charge:Block objects. No monthly charge is shown so the UtilityCost:Tariff object can include just the first four fields. Note that the block sizes are every other field at the bottom of the object and the that final block size references a built in variable called ``remaining'' that contains a very large number.
+
+\begin{lstlisting}
+
+UtilityCost:Tariff,
+    ExampleC,                     ! Name
+    Electricity:Facility,         ! Output Meter Name
+    KWh;                          ! Conversion Factor Choice
+
+
+  UtilityCost:Charge:Block,
+    BlockEnergyCharge,            ! Charge Variable Name
+    ExampleC,                     ! Tariff Name
+    totalEnergy,                  ! Source Variable
+    Annual,                       ! Season
+    EnergyCharges,                ! Category Variable Name
+    ,                             ! Remaining Into Variable
+    ,                             ! Block Size Multiplier Value or Variable Name
+    20000,                        ! Block Size 1 Value or Variable Name
+    0.0474,                       ! Block 1 Cost per Unit Value or Variable Name
+    180000,                       ! Block Size 2 Value or Variable Name
+    0.0424,                       ! Block 2 Cost per Unit Value or Variable Name
+    remaining,                    ! Block Size 3 Value or Variable Name
+    0.0383;                       ! Block 3 Cost per Unit Value or Variable Name
+
+
+  UtilityCost:Charge:Block,
+    BlockDemandCharge,            ! Charge Variable Name
+    ExampleC,                     ! Tariff Name
+    totalDemand,                  ! Source Variable
+    Annual,                       ! Season
+    DemandCharges,                ! Category Variable Name
+    ,                             ! Remaining Into Variable
+    ,                             ! Block Size Multiplier Value or Variable Name
+    20,                           ! Block Size 1 Value or Variable Name
+    5.38,                         ! Block 1 Cost per Unit Value or Variable Name
+    80,                           ! Block Size 2 Value or Variable Name
+    4.23,                         ! Block 2 Cost per Unit Value or Variable Name
+    remaining,                    ! Block Size 3 Value or Variable Name
+    3.60;                         ! Block 3 Cost per Unit Value or Variable Name
+\end{lstlisting}
+
+\subsubsection{Example D - Seasonal Energy Charges with Minimum Charge}\label{example-d---seasonal-energy-charges-with-minimum-charge}
+
+Another type of tariff is one where the energy charges vary by the amount of energy consumed each month and are different for the summer and winter. In addition, this example demonstrates the minimum charge field.
+
+Minimum Charge:~~~~ \$7.00 per month
+
+Winter -- October through May
+
+Energy Charge:~~~~~~~ 4.385 cents/kWh for first 650 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 3.763 cents/kWh for next 350 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 3.704 cents/kWh for over 1000 kWh
+
+Summer -- June through September
+
+Energy Charge:~~~~~~~ 8.385 cents/kWh for first 650 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 7.588 cents/kWh for next 350 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 7.103 cents/kWh for over 1000 kWh
+
+This tariff would use two UtilityCost:Charge:Block objects. The monthly charge is part of the UtilityCost:Tariff object. Note that the block sizes are every other field at the bottom of the object and the that final block size references a built in variable called ``remaining'' that contains a very large number.
+
+\begin{lstlisting}
+
+UtilityCost:Tariff,
+    ExampleD,                     ! Name
+    Electricity:Facility,         ! Output Meter Name
+    KWh,                          ! Conversion Factor Choice
+    ,                             ! Energy Conversion Factor
+    ,                             ! Demand Conversion Factor
+    ,                             ! Time of Use Period Schedule Name
+    TwoSeasonSchedule,            ! Season Schedule Name
+    ,                             ! Month Schedule Name
+    ,                             ! Demand Window Length
+    ,                             ! Monthly Charge or Variable Name
+    7.00;                         ! Minimum Monthly Charge or Variable Name
+
+
+  UtilityCost:Charge:Block,
+    WinterEnergyCost,             ! Charge Variable Name
+    ExampleD,                     ! Tariff Name
+    totalEnergy,                  ! Source Variable
+    Winter,                       ! Season
+    EnergyCharges,                ! Category Variable Name
+    ,                             ! Remaining Into Variable
+    ,                             ! Block Size Multiplier Value or Variable Name
+    650,                          ! Block Size 1 Value or Variable Name
+    0.04385,                      ! Block 1 Cost per Unit Value or Variable Name
+    350,                          ! Block Size 2 Value or Variable Name
+    0.03763,                      ! Block 2 Cost per Unit Value or Variable Name
+    remaining,                    ! Block Size 3 Value or Variable Name
+    0.03704;                      ! Block 3 Cost per Unit Value or Variable Name
+
+
+  UtilityCost:Charge:Block,
+    SummerEnergyCost,             ! Charge Variable Name
+    ExampleD,                     ! Tariff Name
+    totalEnergy,                  ! Source Variable
+    Summer,                       ! Season
+    EnergyCharges,                ! Category Variable Name
+    ,                             ! Remaining Into Variable
+    ,                             ! Block Size Multiplier Value or Variable Name
+    650,                          ! Block Size 1 Value or Variable Name
+    0.08385,                      ! Block 1 Cost per Unit Value or Variable Name
+    350,                          ! Block Size 2 Value or Variable Name
+    0.07588,                      ! Block 2 Cost per Unit Value or Variable Name
+    remaining,                    ! Block Size 3 Value or Variable Name
+    0.07103;                      ! Block 3 Cost per Unit Value or Variable Name
+
+
+  Schedule:Compact, TwoSeasonSchedule, number,
+  Through: 5/31, For: AllDays, Until: 24:00, 1,
+  Through: 9/30, For: AllDays, Until: 24:00, 3,
+  Through: 12/31, For: AllDays, Until: 24:00, 1;
+\end{lstlisting}
+
+\subsubsection{Example E -- kWh/kW Energy Charges}\label{example-e-kwhkw-energy-charges}
+
+A more advanced rate varies the size of the blocks based on amount of demand for the month. This creates an effective demand charge if the blocks have declining values.
+
+Customer Charge:~ \$14.00 per month
+
+Energy Charge:~~ 8.756 cents/kWh for all consumption not greater than 200 hours times the demand
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ 6.812 cents/kWh for all consumption in excess of 200 hours and not greater than 400 hours times the demand
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ 5.029 cents/kWh for all consumption in excess of 400 hours times the demand.
+
+This tariff would use a single ~UtilityCost:Charge:Block object. The monthly charge is part of the ~UtilityCost:Tariff object. In this case the Block Size Multiplier Value (or Variable) is set to the totalDemand variable.
+
+\begin{lstlisting}
+
+UtilityCost:Tariff,
+    ExampleE,                     ! Name
+    Electricity:Facility,         ! Output Meter Name
+    KWh,                          ! Conversion Factor Choice
+    ,                             ! Energy Conversion Factor
+    ,                             ! Demand Conversion Factor
+    ,                             ! Time of Use Period Schedule Name
+    ,                             ! Season Schedule Name
+    ,                             ! Month Schedule Name
+    ,                             ! Demand Window Length
+    14;                           ! Monthly Charge or Variable Name
+
+
+  UtilityCost:Charge:Block,
+    BlockEnergyCharge,            ! Charge Variable Name
+    ExampleE,                     ! Tariff Name
+    totalEnergy,                  ! Source Variable
+    Annual,                       ! Season
+    EnergyCharges,                ! Category Variable Name
+    ,                             ! Remaining Into Variable
+    totalDemand,                  ! Block Size Multiplier Value or Variable Name
+    200,                          ! Block Size 1 Value or Variable Name
+    0.08756,                      ! Block 1 Cost per Unit Value or Variable Name
+    200,                          ! Block Size 2 Value or Variable Name
+    0.06812,                      ! Block 2 Cost per Unit Value or Variable Name
+    remaining,                    ! Block Size 3 Value or Variable Name
+    0.05029;                      ! Block 3 Cost per Unit Value or Variable Name
+\end{lstlisting}
+
+\subsubsection{Example F -- Seasonal Time of Use Energy}\label{example-f-seasonal-time-of-use-energy}
+
+Tariffs sometimes have higher costs for energy consumed during the daytime than at night. This example includes energy charges that vary by the time of day and by the season.
+
+Monthly Charge:~~~~~~ \$37.75 per month
+
+Winter -- October through May
+
+On Peak:~~~~~~~~~~~~~~~~~~ 8.315 cents/kWh
+
+Off-Peak:~~~~~~~~~~~~~~~~~~ 2.420 cents/kWh
+
+Summer -- June through September
+
+On Peak:~~~~~~~~~~~~~~~~~~ 14.009 cents/kWh
+
+Off-Peak:~~~~~~~~~~~~~~~~~~ 6.312 cents/kWh
+
+The on-peak period is defined as the hours starting at 10am and ending at 7pm, Monday through Friday for June through September and 3pm to 10pm Monday through Friday for October through May. All other hours are considered off-peak.
+
+The tariff is only applicable for customers that use 50KW for at least one month of the year.
+
+This tariff uses four different UtilityCost:Charge:Simple objects to capture the variation with time of the energy cost. The monthly charge is part of the UtilityCost:Tariff object.
+
+\begin{lstlisting}
+
+UtilityCost:Tariff,
+    ExampleF,                     ! Name
+    Electricity:Facility,         ! Output Meter Name
+    kWh,                          ! Conversion Factor Choice
+    ,                             ! Energy Conversion Factor
+    ,                             ! Demand Conversion Factor
+    TimeOfDaySchedule,            ! Time of Use Period Schedule Name
+    TwoSeasonSchedule,            ! Season Schedule Name
+    ,                             ! Month Schedule Name
+    ,                             ! Demand Window Length
+    37.75;                        ! Monthly Charge or Variable Name
+
+
+  UtilityCost:Charge:Simple,
+    SummerOnPeak,                 ! Charge Variable Name
+    ExampleF,                     ! Tariff Name
+    peakEnergy,                   ! Source Variable
+    Summer,                       ! Season
+    EnergyCharges,                ! Category Variable Name
+    0.14009;                      ! Cost per Unit Value or Variable Name
+
+
+  UtilityCost:Charge:Simple,
+    SummerOffPeak,                ! Charge Variable Name
+    ExampleF,                     ! Tariff Name
+    offPeakEnergy,                ! Source Variable
+    Summer,                       ! Season
+    EnergyCharges,                ! Category Variable Name
+    0.06312;                      ! Cost per Unit Value or Variable Name
+
+
+  UtilityCost:Charge:Simple,
+    WinterOnPeak,                 ! Charge Variable Name
+    ExampleF,                     ! Tariff Name
+    peakEnergy,                   ! Source Variable
+    Winter,                       ! Season
+    EnergyCharges,                ! Category Variable Name
+    0.08315;                      ! Cost per Unit Value or Variable Name
+
+
+  UtilityCost:Charge:Simple,
+    WinterOffPeak,                ! Charge Variable Name
+    ExampleF,                     ! Tariff Name
+    offPeakEnergy,                ! Source Variable
+    Winter,                       ! Season
+    EnergyCharges,                ! Category Variable Name
+    0.02420;                      ! Cost per Unit Value or Variable Name
+
+
+  UtilityCost:Qualify,
+    MinDemand,                    ! Name
+    ExampleF,                     ! Tariff Name
+    TotalDemand,                  ! Variable Name
+    Minimum,                      ! Qualify Type
+    50,                           ! Threshold Value or Variable Name
+    Annual,                       ! Season
+    Count,                        ! Threshold Test
+    1;                            ! Number of Months
+
+
+  Schedule:Compact, TwoSeasonSchedule, number,
+  Through: 5/31, For: AllDays,  Until: 24:00, 1,
+  Through: 9/30, For: AllDays,  Until: 24:00, 3,
+  Through: 12/31, For: AllDays, Until: 24:00, 1;
+
+
+  Schedule:Compact, TimeOfDaySchedule, number,
+  Through: 5/31, For: AllDays,  Until: 15:00, 3,
+                                Until: 22:00, 1,
+                                Until: 24:00, 3,
+  Through: 9/30, For: AllDays,  Until: 10:00, 3,
+                                Until: 19:00, 1,
+                                Until: 24:00, 3,
+  Through: 12/31, For: AllDays, Until: 15:00, 3,
+                                Until: 22:00, 1,
+                                Until: 24:00, 3;
+\end{lstlisting}
+
+\subsubsection{Example G -- Blocks within Blocks}\label{example-g-blocks-within-blocks}
+
+Utilities have come up with many different ways to encourage certain load factors and discourage other load factors. One method that has been used is blocks defined within other blocks. In the following example standard kWh blocks exist within the energy allocated for the first of several kWh/kW blocks.
+
+Monthly Charge:~~ \$35 per month
+
+Energy Charge:~~~ For all consumption not greater than 200 hours times the demand use
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 10.32 cents/kWh for the first 1000 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 7.43 cents/kWh for the next 4000 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 6.23 cents/kWh for the next 5000 kWh
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 4.27 cents/kWh for the remaining kWh less than 200 hours times the demand
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 6.82 cents/kWh for all consumption in excess of 200 hours and not greater than 400 hours times the demand
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 5.03 cents/kWh for all consumption in excess of 400 hours times the demand.
+
+To set up this ``block within a block'' a UtilityCost:Charge:Block is first used to separate out the first 200 kWh/kW. The ``EnergyFirst200kWhPerkW'' charge performs this. It uses demand to multiply the first block size by 200 and the ``cost'' for the block is simply 1 since it passes through the energy to the variable ``EnergyFirst200kWhPerkW''. The remaining energy goes into the ``restOfEnergy'' variable as specified as the ``Remaining Into Variable'' field. After this is evaluated we have two new variables that hold energy. Each of these variables are then separately used in UtilityCost:Charge:Block objects to evaluate the different parts of the example tariff. By using the ``Remaining Into Variable'' along with the concept of variables, many very complex tariffs may be modeled.
+
+\begin{lstlisting}
+
+  UtilityCost:Tariff,
+      ExampleG,                !- Name
+      ElectricityPurchased:Facility,  !- Output Meter Name
+      KWh,                     !- Conversion Factor Choice
+      ,                        !- Energy Conversion Factor
+      ,                        !- Demand Conversion Factor
+      ,                        !- Time of Use Period Schedule Name
+      ,                        !- Season Schedule Name
+      ,                        !- Month Schedule Name
+      ,                        !- Demand Window Length
+      35;                      !- Monthly Charge or Variable Name
+
+
+    UtilityCost:Charge:Block,
+      EnergyFirst200kWhPerkW,  !- Charge Variable Name
+      ExampleG,                !- Tariff Name
+      totalEnergy,             !- Source Variable
+      Annual,                  !- Season
+      NotIncluded,             !- Category Variable Name
+      restOfEnergy,            !- Remaining Into Variable
+      totalDemand,             !- Block Size Multiplier Value or Variable Name
+      200,                     !- Block Size 1 Value or Variable Name
+      1;                       !- Block 1 Cost Per Unit Value or Variable Name
+
+
+    UtilityCost:Charge:Block,
+      CostOfFirst200kWhPerkW,  !- Charge Variable Name
+      ExampleG,                !- Tariff Name
+      EnergyFirst200kWhPerkW,  !- Source Variable
+      Annual,                  !- Season
+      EnergyCharges,           !- Category Variable Name
+      ,                        !- Remaining Into Variable
+      ,                        !- Block Size Multiplier Value or Variable Name
+      1000,                    !- Block Size 1 Value or Variable Name
+      0.1032,                  !- Block 1 Cost Per Unit Value or Variable Name
+      4000,                    !- Block Size 2 Value or Variable Name
+      0.0743,                  !- Block 2 Cost Per Unit Value or Variable Name
+      5000,                    !- Block Size 3 Value or Variable Name
+      0.0623,                  !- Block 3 Cost Per Unit Value or Variable Name
+      remaining,               !- Block Size 4 Value or Variable Name
+      0.0427;                  !- Block 4 Cost Per Unit Value or Variable Name
+
+
+    UtilityCost:Charge:Block,
+      CostOfRestOfEnergy,      !- Charge Variable Name
+      ExampleG,                !- Tariff Name
+      restOfEnergy,            !- Source Variable
+      Annual,                  !- Season
+      EnergyCharges,           !- Category Variable Name
+      ,                        !- Remaining Into Variable
+      totalDemand,             !- Block Size Multiplier Value or Variable Name
+      200,                     !- Block Size 1 Value or Variable Name
+      0.0682,                  !- Block 1 Cost Per Unit Value or Variable Name
+      remaining,               !- Block Size 2 Value or Variable Name
+      0.0503;                  !- Block 2 Cost Per Unit Value or Variable Name
+\end{lstlisting}
+
+\subsubsection{Example H -- Real Time Pricing}\label{example-h-real-time-pricing}
+
+Some utilities have tariffs that can have different prices every hour of the year called Real Time Pricing tariffs. Often the utility will inform the customer of the prices for each hour of the day just one day in advance. To model this type of utility rate a normal schedule is used that contains the prices on an hourly basis.~ The ``Charge Schedule'' field is where the Schedule object containing the prices is referenced.~ In addition, the ``Baseline Use Schedule'' field is used to set the schedule for the customer baseline load. Not all utilities use a customer baseline load so the field can be left blank if none is needed. The Period, Season and Month Schedules are not needed for these tariffs unless UtilityCost:Charge's are used.~ The Schedule:File object can be especially useful to input a complex schedule that changes throughout the year.
+
+Example H, shown below, is an example of how to use the UtilityCost:Tariff object with a schedule to calculate a utility tariff using real time prices.~ The example real time pricing schedule results in the same energy cost as Example F -- Seasonal Time of Use Energy. This is only an example and usually for real time pricing the schedule values would vary throughout the year.
+
+!~ EXAMPLE H - Real Time Pricing (RTP)
+
+\begin{lstlisting}
+
+  UtilityCost:Tariff,
+      ExampleH,                !- Name
+      ElectricityPurchased:Facility,  !- Output Meter Name
+      kWh,                     !- Conversion Factor Choice
+      ,                        !- Energy Conversion Factor
+      ,                        !- Demand Conversion Factor
+      ,                        !- Time of Use Period Schedule Name
+      ,                        !- Season Schedule Name
+      ,                        !- Month Schedule Name
+      ,                        !- Demand Window Length
+      37.75,                   !- Monthly Charge or Variable Name
+      ,                        !- Minimum Monthly Charge or Variable Name
+      RTPpriceSchedule-H,      !- Real Time Pricing Charge Schedule Name
+      ,                        !- Customer Baseline Load Schedule Name
+      ,                        !- Group Name
+      buyFromUtility;          !- Buy Or Sell
+
+
+    Schedule:Compact,
+      RTPpriceSchedule-H,      !- Name
+      Any Number,              !- Schedule Type Limits Name
+      Through: 5/31,           !- Field 1
+      For: AllDays,            !- Field 2
+      Until: 15:00,            !- Field 3
+      0.02420,                 !- Field 4
+      Until: 22:00,            !- Field 5
+      0.08315,                 !- Field 6
+      Until: 24:00,            !- Field 7
+      0.02420,                 !- Field 8
+      Through: 9/30,           !- Field 9
+      For: AllDays,            !- Field 10
+      Until: 10:00,            !- Field 11
+      0.06312,                 !- Field 12
+      Until: 19:00,            !- Field 13
+      0.14009,                 !- Field 14
+      Until: 24:00,            !- Field 15
+      0.06312,                 !- Field 16
+      Through: 12/31,          !- Field 17
+      For: AllDays,            !- Field 18
+      Until: 15:00,            !- Field 19
+      0.02420,                 !- Field 20
+      Until: 22:00,            !- Field 21
+      0.08315,                 !- Field 22
+      Until: 24:00,            !- Field 23
+      0.02420;                 !- Field 24
+\end{lstlisting}
+
+\subsubsection{Example I -- Selling and Net-Metering}\label{example-i-selling-and-net-metering}
+
+When the building contains a generator, photovoltaics, or other sources of electrical power, there is an opportunity for the building generator to produce more power than the building uses. The excess power can either be sold to the utility or offset the energy purchased.
+
+When the excess power is sold, two utility rates need to be defined. The first can be defined just as in any of the previous examples. Since the ``Buy or Sell'' field of the UtilityCost:Tariff object defaults to ``buyFromUtility'' it does not even need to be specified. The meter specified in the ``Output Meter'' is usually set to ``ElectricityPurchased:Facility.''
+
+The second tariff needs to be defined with the ``Buy or Sell'' field set to ``sellToUtility.'' The ``Output Meter'' is usually set to ``ElectricitySurplusSold:Facility.'' It is important to set the appropriate meters that correspond with the ``Buy or Sell'' field.~ The example below shows an tariff that sells the excess electricity back to utility. The UtilityCost:Charge:Simple object contains a ``Cost Per Value'' with a negative number. A negative number is critical if a credit for selling this electricity is expected.
+
+!~ EXAMPLE I - Selling
+
+\begin{lstlisting}
+
+  UtilityCost:Charge:Simple,
+      GeneratedElectricSold,   !- Charge Variable Name
+      ExampleI-Sell,           !- Tariff Name
+      totalEnergy,             !- Source Variable
+      Annual,                  !- Season
+      EnergyCharges,           !- Category Variable Name
+      -0.02;                   !- Cost Per Unit Value (or Variable)
+
+
+    UtilityCost:Tariff,
+      ExampleI-Sell,           !- Name
+      ElectricitySurplusSold:Facility,  !- Output Meter Name
+      kWh,                     !- Conversion Factor Choice
+      ,                        !- Energy Conversion Factor
+      ,                        !- Demand Conversion Factor
+      ,                        !- Time of Use Period Schedule Name
+      ,                        !- Season Schedule Name
+      ,                        !- Month Schedule Name
+      ,                        !- Demand Window Length
+      ,                        !- Monthly Charge or Variable Name
+      ,                        !- Minimum Monthly Charge or Variable Name
+      ,                        !- Real Time Pricing Charge Schedule Name
+      ,                        !- Customer Baseline Load Schedule Name
+      ,                        !- Group Name
+      sellToUtility;           !- Buy Or Sell
+
+
+    UtilityCost:Charge:Simple,
+      GeneratedElectricSold,   !- Charge Variable Name
+      ExampleI-Sell,           !- Tariff Name
+      totalEnergy,             !- Source Variable
+      Annual,                  !- Season
+      EnergyCharges,           !- Category Variable Name
+      -0.02;                   !- Cost Per Unit Value or Variable Name
+\end{lstlisting}
+
+The next part of this example is a rate that uses net-metering. With net metering the meter conceptually turns backwards when the energy is being sold to the utility directly reducing the energy consumption being charged.~ Effectively, the rate charge for purchased electricity is the same as the rate credited for electricity sold to the utility. In this the ``Buy or Sell'' field should be set to ``netMetering.''~ It is also important the ``Output Meter'' is set to a meter that represents net metering such as ``ElectricityNet:Facility.'' The following example shows a simple example tariff using net metering with a single UtilityCost:Charge:Simple:
+
+\begin{lstlisting}
+
+!  EXAMPLE I – Net Metering
+
+
+    UtilityCost:Tariff,
+      ExampleI-NetMeter,       !- Name
+      ElectricityNet:Facility, !- Output Meter Name
+      kWh,                     !- Conversion Factor Choice
+      ,                        !- Energy Conversion Factor
+      ,                        !- Demand Conversion Factor
+      ,                        !- Time of Use Period Schedule Name
+      ,                        !- Season Schedule Name
+      ,                        !- Month Schedule Name
+      ,                        !- Demand Window Length
+      30.00,                   !- Monthly Charge or Variable Name
+      ,                        !- Minimum Monthly Charge or Variable Name
+      ,                        !- Real Time Pricing Charge Schedule Name
+      ,                        !- Customer Baseline Load Schedule Name
+      ,                        !- Group Name
+      netMetering;             !- Buy Or Sell
+
+
+    UtilityCost:Charge:Simple,
+      NetMeteredCharge,        !- Charge Variable Name
+      ExampleI-NetMeter,       !- Tariff Name
+      totalEnergy,             !- Source Variable
+      Annual,                  !- Season
+      EnergyCharges,           !- Category Variable Name
+      0.065;                   !- Cost Per Unit Value or Variable Name
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff-reporting.tex b/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff-reporting.tex
new file mode 100644
index 00000000000..83f05b92012
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff-reporting.tex
@@ -0,0 +1,3 @@
+\section{UtilityCost:Tariff Reporting}\label{utilitycosttariff-reporting}
+
+A standardized tabular output report is created which shows all components of all categories in the calculation sequence on a variable basis (usually 12 numbers, one for each month). The economics report is automatically created if any UtilityCost:Tariff objects are present. The values reported are in the units specified in the UtilityCost:Tariff object. The report includes:
diff --git a/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff.tex b/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff.tex
new file mode 100644
index 00000000000..5de28ee4429
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/utilitycost-tariff.tex
@@ -0,0 +1,276 @@
+\section{UtilityCost:Tariff}\label{utilitycosttariff}
+
+Defines the name of the tariff, the type of tariff, and other details about the overall tariff. Each other object that is part of the tariff model references the tariff name including the UtilityCost:Charge:Simple, UtilityCost:Charge:Block, UtilityCost:Ratchet, UtilityCost:Qualify, UtilityCost:Variable and UtilityCost:Computation objects.
+
+Multiple UtilityCost:Tariff objects can appear in the same IDF file. It is common that electric and gas utilities have more than one rate that may be used. Only one UtilityCost:Tariff for each Output:Meter object and Group Name is shown in the Economics Summary Report. The one that is shown in that report is chosen by first eliminating UtilityCost:Tariff objects that are not qualified due to their UtilityCost:Qualify objects. If more than one UtilityCost:Tariff object remains, the one that has the lowest cost for a combination of a Meter and Group Name will be selected. If the Group Name field is not used, then the lowest cost UtilityCost:Tariff is chosen for each Meter.
+
+Part of the tariff description is used to transform the annual energy use of any fuel under any meter into a group of named variables containing the values for each of the periods that the bills are calculated (usually monthly). The schedules create a variable for energy use and for demand. If specified it also creates a variable for energy and a variable for demand for the ``on-peak'', ``off-peak'', and ``shoulder'' periods for use in time-of-use tariffs. It performs this allocation prior to other calculations for the tariff. The variables that are always created are:
+
+\begin{itemize}
+\item
+  totalEnergy
+\item
+  totalDemand
+\end{itemize}
+
+\subsection{Inputs}\label{inputs-072}
+
+\paragraph{Field: Name}\label{field-name-064}
+
+The name of the tariff. Tariffs are sometimes called rates. The name is used in identifying the output results and in associating all of the charges and other objects that make up a tariff.
+
+\paragraph{Field: Output Meter Name}\label{field-output-meter-name}
+
+The name of any meter defined but usually set to either Electricity:Facility or Gas:Facility.
+
+\paragraph{Field: Conversion Factor Choice}\label{field-conversion-factor-choice}
+
+A choice that allows several different predefined conversion factors to be used; otherwise, user defined conversion factors are used as defined in the next two fields.
+
+\begin{itemize}
+\item
+  UserDefined
+\item
+  kWh
+\item
+  Therm
+\item
+  MMBtu
+\item
+  MJ
+\item
+  KBtu
+\item
+  MCF
+\item
+  CCF
+\end{itemize}
+
+The following table shows the conversion factors when specifying one of the predefined choices:
+
+% table 36
+\begin{longtable}[c]{@{}lll@{}}
+\caption{Built in UtilityCost:Tariff Conversion Factors \label{table:built-in-utilitycost-tariff-conversion}} \tabularnewline
+\toprule 
+Choice & Energy Conversion Factor & Demand Conversion Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Built in UtilityCost:Tariff Conversion Factors} \tabularnewline
+\toprule 
+Choice & Energy Conversion Factor & Demand Conversion Factor \tabularnewline
+\midrule
+\endhead
+
+kWh & 0.0000002778 & 0.001 \tabularnewline
+Therm & 9.4781712E-09 & 0.00003412 \tabularnewline
+MMBtu & 9.4781712E-10 & 0.000003412 \tabularnewline
+MJ & 0.000001 & 0.0036 \tabularnewline
+KBtu & 9.4781712E-07 & 0.003412 \tabularnewline
+MCF & 9.4781712E-10 & 0.000003412 \tabularnewline
+CCF & 9.4781712E-09 & 0.00003412 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Field: Energy Conversion Factor}\label{field-energy-conversion-factor}
+
+Is a multiplier used to convert energy into the units specified by the utility in their tariff. If left blank, it defaults to 1 (no conversion). This field will be used only if Conversion Factor Choice is set to UserDefined. Within EnergyPlus energy always has units of J (joules). For conversion from J to kWh use the value of 0.0000002778. This is also used for all objects that reference the UtilityCost:Tariff.
+
+\paragraph{Field: Demand Conversion Factor}\label{field-demand-conversion-factor}
+
+Is a multiplier used to convert demand into the units specified by the utility in their tariff. If left blank, it defaults to 1 (no conversion). This field will be used only if Conversion Factor Choice is set to UserDefined. Within EnergyPlus demand always has units of J/s (joules/sec) which equivalent to W (watts). For conversion from W to kW use the value of 0.001. This is also used for all objects that reference the UtilityCost:Tariff.
+
+\paragraph{Field: Time of Use Period Schedule Name}\label{field-time-of-use-period-schedule-name}
+
+The name of the schedule that defines the time-of-use periods that occur each day. The period schedule is used to determine which variables are defined. The values for the different variables are:
+
+\begin{itemize}
+\item
+  1 is Peak
+\item
+  2 is Shoulder
+\item
+  3 is OffPeak
+\item
+  4 is MidPeak
+\end{itemize}
+
+The following variables are created automatically if these different periods are used in the schedule and include:
+
+\begin{itemize}
+\item
+  peakEnergy
+\item
+  peakDemand
+\item
+  shoulderEnergy
+\item
+  shoulderDemand
+\item
+  offPeakEnergy
+\item
+  offPeakDemand
+\item
+  midPeakEnergy
+\item
+  midPeakDemand
+\end{itemize}
+
+Some special variables are created that include only demand from one period that exceeds the demand from another period. For other months that do not exceed, the values are zero. These variables are seldom used but are available for the occasional rate that includes a clause looking at demands during one period that exceed another period.
+
+\begin{itemize}
+\item
+  PeakExceedsOffPeak
+\item
+  OffPeakExceedsPeak
+\item
+  PeakExceedsMidPeak
+\item
+  MidPeakExceedsPeak
+\item
+  PeakExceedsShoulder
+\item
+  ShoulderExceedsPeak
+\end{itemize}
+
+If no Period Schedule is specified then no peak, offPeak, midPeak or shoulder variables are defined.
+
+\paragraph{Field: Season Schedule Name}\label{field-season-schedule-name}
+
+The name of a schedule that defines the seasons. The seasons are
+
+\begin{itemize}
+\item
+  1 is Winter
+\item
+  2 is Spring
+\item
+  3 is Summer
+\item
+  4 is Autumn
+\end{itemize}
+
+The change in the season schedule must occur at the same time as the change in the Monthly Schedule. In other words, a season must end at the same time as a billing month. Variables are automatically created if a season schedule is used. These variables are set to 1 within the season and 0 for the months that are not in the season. The variables are:
+
+\begin{itemize}
+\item
+  isWinter
+\item
+  isNotWinter
+\item
+  isSpring
+\item
+  isNotSpring
+\item
+  isSummer
+\item
+  isNotSummer
+\item
+  isAutumn
+\item
+  isNotAutumn
+\end{itemize}
+
+\paragraph{Field: Month Schedule Name}\label{field-month-schedule-name}
+
+The name of the schedule that defines the billing periods of the year. Normally this entry is allowed to default and a schedule will be internally used that has the breaks between billing periods occurring at the same time as the breaks between months, i.e., at midnight prior to the first day of the month. If other billing periods are used such as two month cycles or a single bill for an entire season, such as some natural gas companies do in the summer, then the month schedule may be used to redefine it. Make sure that the month schedule and season schedule are consistent, otherwise an error will be issued.
+
+\begin{itemize}
+\item
+  1 is the first month, usually January
+\item
+  2 is the second month, usually February
+\item
+  3 is the third month, usually March
+\item
+  4 is the fourth month, usually April
+\item
+  5 is the fifth month, usually May
+\item
+  6 is the sixth month, usually June
+\item
+  7 is the seventh month, usually July
+\item
+  8 is the eighth month, usually August
+\item
+  9 is the ninth month, usually September
+\item
+  10 is the tenth month, usually October
+\item
+  11 is the eleventh month, usually November
+\item
+  12 is the twelfth month, usually December
+\end{itemize}
+
+Thus, the schedule that represents this would look like the following. If no schedule is specified the following Month Schedule is used which defines the months of the year as the normal calendar months.
+
+\begin{lstlisting}
+
+Schedule:Compact, defaultMonths, number,
+  Through: 1/31, For: AllDays, Until: 24:00, 1,
+  Through: 2/28, For: AllDays, Until: 24:00, 2,
+  Through: 3/31, For: AllDays, Until: 24:00, 3,
+  Through: 4/30, For: AllDays, Until: 24:00, 4,
+  Through: 5/31, For: AllDays, Until: 24:00, 5,
+  Through: 6/30, For: AllDays, Until: 24:00, 6,
+  Through: 7/31, For: AllDays, Until: 24:00, 7,
+  Through: 8/31, For: AllDays, Until: 24:00, 8,
+  Through: 9/30, For: AllDays, Until: 24:00, 9,
+  Through: 10/31, For: AllDays, Until: 24:00, 10,
+  Through: 11/30, For: AllDays, Until: 24:00, 11,
+  Through: 12/31, For: AllDays, Until: 24:00, 12;
+\end{lstlisting}
+
+\paragraph{Field: Demand Window Length}\label{field-demand-window-length-000}
+
+The determination of demand can vary by utility. Some utilities use the peak instantaneous demand measured but most use a fifteen minute average demand or a one hour average demand. Some gas utilities measure demand as the use during the peak day or peak week. The choices for demand window are:
+
+\begin{itemize}
+\item
+  QuarterHour
+\item
+  HalfHour
+\item
+  FullHour
+\item
+  Day
+\item
+  Week
+\end{itemize}
+
+If no value is entered, QuarterHour is assumed. The choice may be overridden based on the value of Timestep so that they are consistent. If the Timestep is 6, i.e.~10 minute timesteps, then QuarterHour is not used and instead HalfHour is used instead. If Timestep is 3, i.e.~20 minute timesteps, then QuarterHour and HalfHour are not used and instead FullHour is used instead. Day and Week are primarily used by fuel utilities.
+
+\paragraph{Field: Monthly Charge or Variable Name}\label{field-monthly-charge-or-variable-name}
+
+The fixed monthly service charge that many utilities have. The entry may be numeric and gets added to the ServiceCharges variable or if a variable name is entered here, its values for each month are used.
+
+\paragraph{Field: Minimum Monthly Charge or Variable Name}\label{field-minimum-monthly-charge-or-variable-name}
+
+The minimum total charge for the tariff or if a variable name is entered here, its values for each month are used.~ The sum of the subtotal and taxes usually equals the total unless you have specified the minimum monthly charge. If the minimum monthly charge does not apply to the entire bill, a UtilityCost:Computation object can be specified using a Minimum function for the appropriate variables.
+
+\paragraph{Field: Real Time Pricing Charge Schedule Name}\label{field-real-time-pricing-charge-schedule-name}
+
+Used with real time pricing rates. The name of a schedule that contains the cost of energy for that particular time period of the year. Real time rates can be modeled using a charge schedule with the actual real time prices entered in the schedule. The charges should be consistent with the conversion factor specified in the tariff.
+
+\paragraph{Field: Customer Baseline Load Schedule Name}\label{field-customer-baseline-load-schedule-name}
+
+Used with real time pricing rates and often described as the CBL or customer baseline load. The name of a schedule that contains the baseline energy use for the customer. Many real time rates apply the charges as a credit or debit only to the difference between the baseline use and the actual use. The baseline use is established between the customer and the utility using a contract. If this field is used the baseline use schedule will be used for establishing the totalEnergy and totalDemand instead of the metered value and the real time rate charge is added or subtracted to the rate calculation using the real time charge schedule. If this field is not used, the real time charge schedule applies to all energy from the meter and totalEnergy and totalDemand is based on metered value as usual.
+
+\paragraph{Field: Group Name}\label{field-group-name}
+
+The group name of the tariff such as distribution, transmission, supplier, etc. If more than one tariff with the same group name is present and qualifies, only the lowest cost tariff is used. Usually the group name field is left blank which results in all tariffs using the same meter variable being compared and the lowest cost one being selected.
+
+\paragraph{Field: Buy Or Sell}\label{field-buy-or-sell}
+
+Sets whether the tariff is used for buying, selling or both to the utility. This should be allowed to default to BuyFromUtility unless a power generation system is included in the building that may generate more power than the building needs during the year. The choices are:
+
+\begin{itemize}
+\item
+  BuyFromUtility -- The values from the metered variable are used and are shown as being purchases from the utility.
+\item
+  SellToUtility -- The values from the metered variable are used for a ``sell back'' rate to the utility. The charges in the rate should be expressed as negative values.
+\item
+  NetMetering -- Negative values are used to reduce any positive values during the specific period on the tariff when negative values occur.
+\end{itemize}
+
+A warning will be issued if the selection of this field does not match the type of meter.
diff --git a/doc/input-output-reference/src/energyplus-economics/utilitycost-variable.tex b/doc/input-output-reference/src/energyplus-economics/utilitycost-variable.tex
new file mode 100644
index 00000000000..231f72b4dc2
--- /dev/null
+++ b/doc/input-output-reference/src/energyplus-economics/utilitycost-variable.tex
@@ -0,0 +1,32 @@
+\section{UtilityCost:Variable}\label{utilitycostvariable}
+
+The UtilityCost:Variable object allows for the direct entry of monthly values into a variable.
+
+\subsection{Inputs}\label{inputs-073}
+
+\paragraph{Field: Name}\label{field-name-065}
+
+The name of the variable.
+
+\paragraph{Field: Tariff Name}\label{field-tariff-name-004}
+
+The name of the tariff that is using the variable.
+
+\paragraph{Field: Variable Type}\label{field-variable-type-000}
+
+This field is used to indicate the kind of units that may be associated with the variable. It is used by IDF Editor to display the appropriate SI and IP units for the January through December values. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion\textbf{.}
+
+\begin{itemize}
+\item
+  Energy
+\item
+  Demand
+\item
+  Currency
+\item
+  Dimensionless
+\end{itemize}
+
+\paragraph{Field: January through December Values}\label{field-january-through-december-values}
+
+An entry (up to 24 are available) of the monthly values of the variable. Normally 12 months are used for most utility rates and so 12 values should be entered. If any values are not entered, the value of the previous entry is used. This allows a variable that is constant for an entire year to be entered using only the first value.
diff --git a/doc/input-output-reference/src/hvac-template-objects.tex b/doc/input-output-reference/src/hvac-template-objects.tex
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@@ -0,0 +1,5 @@
+\chapter{HVAC Template Objects}\label{hvac-template-objects}
+
+\input{src/hvac-template-objects/hvactemplate-processing}
+
+\input{src/hvac-template-objects/group-hvac-templates}
diff --git a/doc/input-output-reference/src/hvac-template-objects/group-hvac-templates.tex b/doc/input-output-reference/src/hvac-template-objects/group-hvac-templates.tex
new file mode 100644
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@@ -0,0 +1,8292 @@
+\section{Group -- HVAC Templates}\label{group-hvac-templates}
+
+This group of objects allows for the specification of simple zone thermostats and HVAC systems with automatically generated node names. The combinations of HVACTemplate objects are shown below.
+
+For a simple ideal loads system to use for sizing and loads oriented simulations:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:IdealLoadsAirSystem
+\end{itemize}
+
+For baseboard heating systems with optional hot water boiler:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:BaseboardHeat
+\item
+  HVACTemplate:Plant:HotWaterLoop (optional)
+\item
+  HVACTemplate:Plant:Boiler (optional)
+\end{itemize}
+
+For fan coil systems with boilers and chillers:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:FanCoil
+\item
+  HVACTemplate:Plant:ChilledWaterLoop
+\item
+  HVACTemplate:Plant:HotWaterLoop
+\item
+  HVACTemplate:Plant:Chiller
+\item
+  HVACTemplate:Plant:Boiler
+\item
+  HVACTemplate:Plant:Tower
+\end{itemize}
+
+For packaged terminal air conditioner (PTAC) systems with optional hot water boiler:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:PTAC
+\item
+  HVACTemplate:Plant:HotWaterLoop (optional)
+\item
+  HVACTemplate:Plant:Boiler (optional)
+\end{itemize}
+
+For packaged terminal air-to-air heat pump (PTHP) systems:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:PTHP
+\end{itemize}
+
+For water to air heat pumps with boiler and cooling tower:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:WaterToAirHeatPump
+\item
+  HVACTemplate:Plant:MixedWaterLoop
+\item
+  HVACTemplate:Plant:Boiler
+\item
+  HVACTemplate:Plant:Tower
+\end{itemize}
+
+For variable refrigerant flow heat pumps (air-to-air):
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:VRF
+\item
+  HVACTemplate:System:VRF
+\end{itemize}
+
+For variable refrigerant flow heat pumps (water-to-air)with boiler and cooling tower:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:VRF
+\item
+  HVACTemplate:System:VRF
+\item
+  HVACTemplate:Plant:MixedWaterLoop
+\item
+  HVACTemplate:Plant:Boiler
+\item
+  HVACTemplate:Plant:Tower
+\end{itemize}
+
+For direct-expansion cooling, packaged and split system simulations:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:Unitary
+\item
+  HVACTemplate:System:Unitary or
+\item
+  HVACTemplate:System:UnitarySystem
+\end{itemize}
+
+For direct-expansion heat pump systems:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:Unitary
+\item
+  HVACTemplate:System:UnitaryHeatPump:AirToAir or
+\item
+  HVACTemplate:System:UnitarySystem
+\end{itemize}
+
+For packaged variable air volume systems using direct-expansion cooling:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:VAV or
+\item
+  HVACTemplate:Zone:VAV:FanPowered or
+\item
+  HVACTemplate:Zone:VAV:HeatAndCool
+\item
+  HVACTemplate:System:PackagedVAV
+\end{itemize}
+
+For variable air volume systems with boilers and air-cooled chillers:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:VAV or
+\item
+  HVACTemplate:Zone:VAV:FanPowered or
+\item
+  HVACTemplate:Zone:VAV:HeatAndCool
+\item
+  HVACTemplate:System:VAV
+\item
+  HVACTemplate:Plant:ChilledWaterLoop
+\item
+  HVACTemplate:Plant:HotWaterLoop
+\item
+  HVACTemplate:Plant:Chiller
+\item
+  HVACTemplate:Plant:Boiler
+\end{itemize}
+
+For variable air volume systems with boilers and water-cooled chillers, an object related to towers is added:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:VAV or
+\item
+  HVACTemplate:Zone:VAV:FanPowered or
+\item
+  HVACTemplate:Zone:VAV:HeatAndCool
+\item
+  HVACTemplate:System:VAV
+\item
+  HVACTemplate:Plant:ChilledWaterLoop
+\item
+  HVACTemplate:Plant:HotWaterLoop
+\item
+  HVACTemplate:Plant:Chiller
+\item
+  HVACTemplate:Plant:Boiler
+\item
+  HVACTemplate:Plant:Tower
+\end{itemize}
+
+For constant air volume systems with boilers and water-cooled chillers:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:ConstantVolume
+\item
+  HVACTemplate:System:ConstantVolume
+\item
+  HVACTemplate:Plant:ChilledWaterLoop
+\item
+  HVACTemplate:Plant:HotWaterLoop
+\item
+  HVACTemplate:Plant:Chiller
+\item
+  HVACTemplate:Plant:Boiler
+\item
+  HVACTemplate:Plant:Tower
+\end{itemize}
+
+For dual-duct systems (constant or variable air volume) with boilers and water-cooled chillers:
+
+\begin{itemize}
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:DualDuct
+\item
+  HVACTemplate:System:DualDuct
+\item
+  HVACTemplate:Plant:ChilledWaterLoop
+\item
+  HVACTemplate:Plant:HotWaterLoop
+\item
+  HVACTemplate:Plant:Chiller
+\item
+  HVACTemplate:Plant:Boiler
+\item
+  HVACTemplate:Plant:Tower
+\end{itemize}
+
+For dedicated outdoor air systems (DOAS) combined with a zonal template system:
+
+\begin{itemize}
+\item
+  HVACTemplate:System:DedicatedOutdoorAir
+\item
+  HVACTemplate:Thermostat
+\end{itemize}
+
+One of the following for each zone served by the (DOAS) --
+
+\begin{itemize}
+\item
+  HVACTemplate:Zone:BaseboardHeat
+\item
+  HVACTemplate:Zone:PTAC
+\item
+  HVACTemplate:Zone:PTHP
+\item
+  HVACTemplate:Zone:FanCoil
+\item
+  HVACTemplate:Zone:WaterToAirHeatPump
+\item
+  HVACTemplate:Zone:VRF
+\item
+  HVACTemplate:Plant:* objects as needed (depending on the type of zonal system and the type of coils specified in the DOAS system:WaterToAirHeatPump).
+\end{itemize}
+
+The \emph{only} other HVAC related objects besides the HVACTemplate objects that need to be specified related to HVAC systems are:
+
+\begin{itemize}
+\item
+  Schedule:Year or Schedule:Compact
+\item
+  SizingPeriod objects (one for heating and one for cooling) Note: all SizingPeriod objects can be used but for simplicity in the following descriptions, we will only reference SizingPeriod:DesignDay
+\item
+  SimulationControl
+\item
+  Sizing:Parameters
+\end{itemize}
+
+This makes the input requirements much smaller but sacrifices some of the flexibility normally found in EnergyPlus.
+
+\subsection{HVACTemplate:Thermostat}\label{hvactemplatethermostat}
+
+Each type of HVAC template zone object may reference one of these HVAC template thermostat objects. Multiple HVAC template zones can reference the same HVAC template thermostat object. The object allows the setpoints to be specified either as a constant for the entire simulation or as schedules. Referenced schedules must be defined elsewhere in the idf. Thermostat control type is dual setpoint with deadband. This object may be omitted and the user may define zone thermostat controls directly using standard EnergyPlus objects (ZoneControl:Thermostat and related objects).
+
+\subsubsection{Inputs}\label{inputs-024}
+
+\paragraph{Field: Name}\label{field-name-023}
+
+A name used to reference this object. This name is referenced by HVACTemplate:Zone objects: i.e., HVACTemplate:Zone:IdealLoadsAirSystem, HVACTemplate:Zone:FanCoil, HVACTemplate:Zone:Unitary, HVACTemplate:Zone:VAV or HVACTemplate:Zone:VAV:FanPowered objects.
+
+\paragraph{Field: Heating Setpoint Schedule Name}\label{field-heating-setpoint-schedule-name}
+
+Enter the name of a heating setpoint schedule that has values that change at different times of the day or year. If a constant set point is needed simply leave this field blank and use the next field. The values in the schedule are in degrees C.
+
+\paragraph{Field: Constant Heating Setpoint}\label{field-constant-heating-setpoint}
+
+Enter the heating setpoint temperature in degrees C if constant throughout the year. If the previous field is used this field should be left blank and will be ignored.
+
+\paragraph{Field: Cooling Setpoint Schedule Name}\label{field-cooling-setpoint-schedule-name}
+
+Enter the name of a cooling setpoint schedule that has values that change at different times of the day or year. If a constant set point is needed simply leave this field blank and use the next field. The values in the schedule are in degrees C.
+
+\paragraph{Field: Constant Cooling Setpoint}\label{field-constant-cooling-setpoint}
+
+Enter the cooling setpoint temperature in degrees C if constant throughout the year. If the previous field is used this field should be left blank and will be ignored.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Thermostat,
+  Office Thermostat,     !- Thermostat Name
+  Htg-SetP-Sch,          !- Heating Setpoint Schedule
+  ,                      !- Constant Heating Setpoint {C}
+  Clg-SetP-Sch,          !- Cooling Setpoint Schedule
+  ;                      !- Constant Cooling Setpoint {C}
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:IdealLoadsAirSystem}\label{hvactemplatezoneidealloadsairsystem}
+
+This object provides an ideal system to supply conditioned air to the zone that meets all the load requirements and consumes no energy. It is often used for load calculations, an evaluation where the load components of the building are all that is being investigated, or as the first step to a more realistic model of a building.
+
+This component can be operated with infinite or finite heating and cooling capacity. For either mode -- infinite or limited capacity -- the user can also specify on/off schedules for heating and cooling and outdoor air controls. There are also optional controls for dehumidification, humidification, economizer, and heat recovery. This component may be used in combination with other HVAC equipment serving the same zone.
+
+This component can be thought of as an ideal unit that mixes air at the zone exhaust condition with the specified amount of outdoor air and then adds or removes heat and moisture at 100\% efficiency in order to produce a supply air stream at the specified conditions. The energy required to condition the supply air is metered and reported as DistrictHeating and DistrictCooling.
+
+\subsubsection{Inputs}\label{inputs-1-022}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-006}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:IdealLoadsAirSystem objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. There are additional schedules fields for heating and cooling operation.
+
+\paragraph{Field: Maximum Heating Supply Air Temperature}\label{field-maximum-heating-supply-air-temperature}
+
+The maximum air temperature (degrees C) of the air used for heating the zone. The default is 50C (122F).
+
+\paragraph{Field: Minimum Cooling Supply Air Temperature}\label{field-minimum-cooling-supply-air-temperature}
+
+The minimum air temperature (degrees C) of the air used for cooling the zone. The default is 13C (55.4F).
+
+\paragraph{Field: Maximum Heating Supply Air Humidity Ratio}\label{field-maximum-heating-supply-air-humidity-ratio}
+
+The maximum humidity ratio (kg of water per kg of dry air) of the hot supply air. The default is 0.0156 kgWater/kgDryAir which corresponds to a 20\%RH at 50C (122F) dry bulb.
+
+\paragraph{Field: Minimum Cooling Supply Air Humidity Ratio}\label{field-minimum-cooling-supply-air-humidity-ratio}
+
+The minimum humidity ratio (kg of water per kg of dry air) of the cool supply air. The default is 0.0077 kgWater/kgDryAir which corresponds to a 10C (50F) dew point.
+
+\paragraph{Field: Heating Limit}\label{field-heating-limit}
+
+The input must be either \emph{LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity} or \emph{NoLimit}. \emph{LimitFlowRate} means that the heating supply air flow rate will be limited to the value specified in the next input field. \emph{LimitCapacity} means that the sensible heating capacity will be limited to the value specified in the Maximum Sensible Heating Capacity field. \emph{LimitFlowRateAndCapacity} means that both flow rate and capacity will be limited. \emph{NoLimit} (the default) means that there will not be any limit on the heating supply air flow rate or capacity and the subsequent two fields will be ignored.
+
+\paragraph{Field: Maximum Heating Air Flow Rate}\label{field-maximum-heating-air-flow-rate-000}
+
+The maximum heating supply air flow rate in cubic meters per second if heating limit is set to \emph{LimitFlowRate or LimitFlowRateAndCapacity} \emph{.} This field may be autosized. This field is ignored if heating limit is set to \emph{NoLimit} or \emph{LimitCapacity}. If blank, there is no limit.
+
+\paragraph{Field: Maximum Sensible Heating Capacity}\label{field-maximum-sensible-heating-capacity}
+
+The maximum allowed sensible heating capacity in Watts if Heating Limit is set to \emph{LimitCapacity} or \emph{LimitFlowRateAndCapacity}. This field may be autosized. If blank, there is no limit. If Heating Limit \emph{is set to NoLimit} or \emph{LimitFlowRate}, this field is ignored.
+
+\paragraph{Field: Cooling Limit}\label{field-cooling-limit}
+
+The input must be either \emph{LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity} or \emph{NoLimit}. \emph{LimitFlowrate} means that the cooling supply air flow rate will be limited to the value specified in the next input field. \emph{LimitCapacity} means that the total cooling capacity will be limited to the value specified in the Maximum Total Cooling Capacity field. \emph{LimitFlowRateAndCapacity} means that both flow rate and capacity will be limited. \emph{NoLimit} (the default) means that there will not be any limit on the cooling supply air flow rate or capacity and the subsequent two fields will be ignored.
+
+\paragraph{Field: Maximum Cooling Air Flow Rate}\label{field-maximum-cooling-air-flow-rate-000}
+
+The maximum cooling supply air flow rate in cubic meters per second if Cooling Limit is set to \emph{LimitFlowRate} or \emph{LimitFlowRateAndCapacity.} This field may be autosized. This field is ignored if cooling limit is set to \emph{NoLimit} or \emph{LimitCapacity}. If blank, there is no limit. If \emph{Cooling Limit is set to NoLimit,} this field is ignored\emph{.} This field is required if Outdoor Air Control Type is \emph{TemperatureEconomizer} in order to establish an upper limit on outdoor air flow when the economizer is active\emph{.}
+
+\paragraph{Field: Maximum Total Cooling Capacity}\label{field-maximum-total-cooling-capacity}
+
+The maximum allowed total (sensible plus latent) cooling capacity in Watts if Cooling Limit is set to \emph{LimitCapacity} or \emph{LimitFlowRateAndCapacity}. This field may be autosized. If blank, there is no limit. If Cooling Limit \emph{is set to NoLimit} or \emph{LimitFlowRate,} this field is ignored\emph{.}
+
+\paragraph{Field: Heating Availability Schedule Name}\label{field-heating-availability-schedule-name-000}
+
+The name of a schedule (ref: Schedule) that denotes whether heating is available. A schedule value greater than 0 (usually 1 is used) indicates that heating and humidification are available. A value less than or equal to 0 (usually 0 is used) denotes that heating and humidification are not available. If blank, heating and humidification are always available.
+
+\paragraph{Field: Cooling Availability Schedule Name}\label{field-cooling-availability-schedule-name-000}
+
+The name of a schedule (ref: Schedule) that denotes whether cooling is available. A schedule value greater than 0 (usually 1 is used) indicates that cooling and dehumidification are available. A value less than or equal to 0 (usually 0 is used) denotes that cooling and dehumidification is not available. If blank, cooling and dehumidification are always available.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-000}
+
+Select from \emph{ConstantSensibleHeatRatio}, \emph{Humidistat, None, or ConstantSupplyHumidityRatio}. \emph{ConstantSensibleHeatRatio} (the default) means that the ideal loads system will be controlled to meet the sensible cooling load, and the latent cooling rate will be computed using a constant sensible heat ratio (SHR) (see next field). \emph{Humidistat} means that there is a ZoneControl:Humidistat for this zone and the ideal loads system will attempt to meet the humidistat request (i.e.~will dehumidify according to the Dehumidifying Relative Humidity Schedule in the ZoneControl:Humidistat object). \emph{None} means that there is no dehumidification. \emph{ConstantSupplyHumidityRatio} means that during cooling the supply air will always be at the Minimum Cooling Supply Humidity Ratio. For \emph{ConstantSensibleHeatRatio} and \emph{Humidistat}, if the mixed air humidity ratio is less than the target humidity ratio, then the mixed air humidity ratio will be used. For all options, the supply air humidity ratio will never be allowed to exceed saturation at the supply dry bulb temperature.
+
+The selected dehumidification control type is always applied when the unit is in cooling mode. If the unit is in deadband mode (not actively heating the supply air) control type \emph{Humidistat} will be active. If the unit is in heating mode, control type \emph{Humidistat} will be active if the Humidification Control Type field below is set to \emph{Humidistat} or \emph{None}.
+
+This allows the ideal loads system to heat and dehumidify at the same time.
+
+\paragraph{Field: Cooling Sensible Heat Ratio}\label{field-cooling-sensible-heat-ratio}
+
+When the Dehumidification Control Type is set to \emph{ConstantSensibleHeatRatio} the ideal loads system will be controlled to meet the sensible cooling load, and the latent cooling rate will be computed using the value of Cooling Sensible Heat Ratio (SHR), where SHR = Sensible Cooling divided by Total Cooling (sensible plus latent). The default is 0.7. If Dehumidification Control Type is set to something other than \emph{ConstantSensibleHeatRatio} then this field will be ignored.
+
+\paragraph{Field: Dehumidification Setpoint}\label{field-dehumidification-setpoint}
+
+This field specifies the zone humidistat relative humidity setpoint for dehumidification in percent (0 to 100). The default is 60\%. This field is used only when the Dehumidification Control Type = \emph{Humidistat.}
+
+\paragraph{Field: Humidification Control Type}\label{field-humidification-control-type}
+
+Select from \emph{None}, \emph{Humidistat, or ConstantSupplyHumidityRatio}. \emph{None} means that there is no humidification. \emph{Humidistat} means that there is a ZoneControl:Humidistat for this zone and the ideal loads system will attempt to meet the humidistat request (i.e., humidify according to the Humidifying Relative Humidity Setpoint Schedule in the ZoneControl:Humidistat object). \emph{ConstantSupplyHumidityRatio} means that during heating the supply air will always be at the Maximum Heating Supply Humidity Ratio. The default is \emph{None}. For \emph{Humidistat}, if the mixed air humidity ratio is greater than the target humidity ratio, then the mixed air humidity ratio will be used. For all options, the supply air humidity ratio will never be allowed to exceed saturation at the supply dry bulb temperature.
+
+The selected humidification control type is always applied when the unit is in heating mode. If the unit is in deadband mode (not actively heating the supply air) control type \emph{Humidistat} will be active. If the unit is in cooling mode, control type \emph{Humidistat} will be active if the Dehumidification Control Type field above is set to \emph{Humidistat} or \emph{None}.
+
+This allows the ideal loads system to cool and humidify at the same time.
+
+\paragraph{Field: Humidification Setpoint}\label{field-humidification-setpoint}
+
+This field specifies the zone humidistat relative humidity setpoint for humidification in percent (0 to 100). The default is 30\%. This field is used only when the Humidification Control Type = \emph{Humidistat.}
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-000}
+
+The input must be either \emph{None, Flow/Zone}, \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{None} means there is no outdoor air provided by this system. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{None.}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object referenced in the Design Specification Outdoor Air Object Name field below.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if Outdoor Air Method is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum.}
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if Outdoor Air Method is \emph{Flow/Area, Sum} or \emph{Maximum}. The default is 0.0.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if Outdoor Air Method is \emph{Flow/Zone, Sum} or \emph{Maximum}. The default is 0.0.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-001}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the outdoor air requirements and schedule for this system. The outdoor air flow rate may also be affected by the next two fields, Demand Controlled Ventilation Type and Outdoor Air Economizer Type. If this field is blank, this system will have no outdoor air, and all outdoor air control and heat recovery options will be ignored..
+
+\paragraph{Field: Demand Controlled Ventilation Type}\label{field-demand-controlled-ventilation-type}
+
+This field, along with the Design Specification Outdoor Air Object (if used) specifies how the minimum outdoor air flow rate is calculated. The choices are: \emph{None, OccupancySchedule or CO2Setpoint}. The default is \emph{None}.
+
+\begin{itemize}
+\item
+  None means that the design occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field).
+\item
+  OccupancySchedule means that the current occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field).
+\item
+  CO2Setpoint means that the design occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field). In addition, the minimum outdoor air flow rate may be increased if necessary to maintain the level of indoor air carbon dioxide at or below the setpoint defined in a ZoneControl:ContaminantController object (the user must add this to the idf file along with other related inputs).
+\end{itemize}
+
+\paragraph{Field: Outdoor Air Economizer Type}\label{field-outdoor-air-economizer-type}
+
+This field specifies if there is an outdoor air economizer. The choices are: \emph{NoEconomizer, DifferentialDryBulb,} or \emph{DifferentialEnthalpy}. The default is \emph{NoEconomizer}. \emph{DifferentialDryBulb} and \emph{DifferentialEnthalpy} mean that the economizer will increase the outdoor air flow rate above the minimum outdoor air flow (see fields Design Specification Outdoor Air Object Name and Demand Controlled Ventilation Type) when there is a cooling load and the outdoor air temperature or enthalpy is below the zone exhaust air temperature or enthalpy. The \emph{DifferentialDryBulb} and \emph{DifferentialEnthalpy} options require that the Maximum Cooling Air Flow Rate be specified which will be used as the limit for maximum outdoor air flow rate.
+
+\paragraph{Field: Heat Recovery Type}\label{field-heat-recovery-type}
+
+Select from \emph{None}, \emph{Sensible}, or \emph{Enthalpy}. \emph{None} means that there is no heat recovery. \emph{Sensible} means that there is sensible heat recovery whenever the zone exhaust air temperature is more favorable than the outdoor air temperature. \emph{Enthalpy} means that there is latent and sensible heat recovery whenever the zone exhaust air enthalpy is more favorable than the outdoor air enthalpy. The default is \emph{None}.
+
+\paragraph{Field: Sensible Heat Recovery Effectiveness}\label{field-sensible-heat-recovery-effectiveness}
+
+The sensible heat recovery effectiveness, where effectiveness is defined as the change in supply temperature divided by the difference in entering supply and relief air temperatures. The default is 0.70.
+
+\paragraph{Field: Latent Heat Recovery Effectiveness}\label{field-latent-heat-recovery-effectiveness}
+
+The latent heat recovery effectiveness, where effectiveness is defined as the change in supply humidity ratio divided by the difference in entering supply and relief air humidity ratios. The default is 0.65.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:IdealLoadsAirSystem,
+  Zone 1,                  !- Zone Name
+  All Zones,               !- Thermostat Name
+  FanAvailSched,           !- System Availability Schedule Name
+  50,                      !- Maximum Heating Supply Air Temperature {C}
+  13,                      !- Minimum Cooling Supply Air Temperature {C}
+  0.0156,         !- Maximum Heating Supply Air Humidity Ratio {kgWater/kgDryAir}
+  0.0077,         !- Minimum Cooling Supply Air Humidity Ratio {kgWater/kgDryAir}
+  NoLimit,                 !- Heating Limit
+  ,                        !- Maximum Heating Air Flow Rate {m3/s}
+  ,                        !- Maximum Sensible Heating Capacity {W}
+  NoLimit,                 !- Cooling Limit
+  ,                        !- Maximum Cooling Air Flow Rate {m3/s}
+  ,                        !- Maximum Total Cooling Capacity {W}
+  ,                        !- Heating Availability Schedule Name
+  ,                        !- Cooling Availability Schedule Name
+  ConstantSensibleHeatRatio,  !- Dehumidification Control Type
+  0.7,                     !- Cooling Sensible Heat Ratio
+  60,                      !- Dehumidification Setpoint {percent}
+  None,                    !- Humidification Control Type
+  30,                      !- Humidification Setpoint {percent}
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  0.0,                     !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
+  ,                        !- Design Specification Outdoor Air Object Name
+  None,                    !- Demand Controlled Ventilation Type
+  NoEconomizer,            !- Outdoor Air Economizer Type
+  None,                    !- Heat Recovery Type
+  0.70,                    !- Sensible Heat Recovery Effectiveness
+  0.65;                    !- Latent Heat Recovery Effectiveness
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:BaseboardHeat}\label{hvactemplatezonebaseboardheat}
+
+This object simulates a hot water or electric thermostatically controlled baseboard heating system. This object includes optional fields to combine the baseboard heat with a dedicated outdoor air system. If the zone is also served by another HVAC system, such as a PTAC or unitary air handler, then do not use this object. Instead, use the HVACTemplate:Zone:* object for the forced air system and use the baseboard heating fields in that object.
+
+\subsubsection{Inputs}\label{inputs-2-020}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-004}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-1}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:IdealLoadsAirSystem objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that detailed thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-000}
+
+This input is the zone level heating sizing ratio. The zone design heating load will be multiplied by the number input in this field when the Baseboard Heating Capacity is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type}
+
+This field specifies the type of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\end{itemize}
+
+The default choice is \emph{HotWater}.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the fan coil system. The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the fan coil system.
+
+\paragraph{Field: Dedicated Outdoor Air System Name}\label{field-dedicated-outdoor-air-system-name}
+
+Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the DOAS will provide ventilation air to the zone based on the outdoor air specifications in this object. If this field is blank, then the following outdoor air fields are ignored.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-1}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-1}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if Outdoor Air Method is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum.}
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-1}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if Outdoor Air Method is \emph{Flow/Area, Sum} or \emph{Maximum}. The default is 0.0.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-1}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if Outdoor Air Method is \emph{Flow/Zone, Sum} or \emph{Maximum}. The default is 0.0.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-1-000}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when Outdoor Air Method * = DetailedSpecification*.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-000}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when Outdoor Air Method * = DetailedSpecification*.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:BaseboardHeat,
+  SPACE1-1,          !- Zone Name
+  All Zones,         !- Template Thermostat Name
+  ,                  !- Zone Heating Sizing Factor
+  HotWater,          !- Baseboard Heating Type
+  ,                  !- Baseboard Heating Availability Schedule Name
+  Autosize;          !- Baseboard Heating Capacity {W}
+  ,                  !- Dedicated Outdoor Air System Name
+  flow/person,       !- Outdoor Air Method
+  0.00944,           !- Outdoor Air Flow Rate per Person {m3/s}
+  0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  0.0,               !- Outdoor Air Flow Rate per Zone {m3/s}
+  ,                  !- Design Specification Outdoor Air Object Name
+  ;                  !- Design Specification Zone Air Distribution Object Name
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:FanCoil}\label{hvactemplatezonefancoil}
+
+This object simulates a 4 pipe fan coil unit with hot water heating coil, chilled water cooling coil, and an outdoor air mixer. The coils are served directly by HVACTemplate:Plant:ChilledWaterLoop and HVACTemplate:Plant:HotWaterLoop objects. No HVACTemplate:System object is required. Reference ZoneHVAC:FourPipeFanCoil for more details about the fan coil model.
+
+\subsubsection{Inputs}\label{inputs-3-018}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-2-002}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-2}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Supply Air Maximum Flow Rate}\label{field-supply-air-maximum-flow-rate}
+
+By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. Note that the zone must have a thermostat specified in order to autosize the flow rate. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-1}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-000}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-2}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-2}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-2}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-2}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-1}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. Fan coil systems are modeled with continuous fan operation, so this is also the supply fan operating schedule. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Supply Fan Delta Pressure}\label{supply-fan-delta-pressure}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Supply Fan Motor in Air Stream Fraction}\label{field-supply-fan-motor-in-air-stream-fraction}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type}
+
+There are two coil types available:
+
+\begin{itemize}
+\item
+  ChilledWater
+\item
+  ChilledWaterDetailedFlatModel
+\end{itemize}
+
+\emph{Chilled Water} uses theCoil:Cooling:Water object with the DetailedAnalysis option. This is the preferred coil model for most applications. \emph{ChilledWaterDetailedFlatModel} uses the Coil:Cooling:Water:DetailedGeometry object. This option is available for special applications. The default is \emph{ChilledWater}.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of one indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Coil Design Setpoint}\label{field-cooling-coil-design-setpoint}
+
+This is the design supply air temperature in C used to size the cooling supply air flow and the cooling coil. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 14\(^{o}\)C.
+
+\paragraph{Field: Heating Coil Type}\label{field-heating-coil-type}
+
+Only one possible value may be entered here:
+
+\begin{itemize}
+\tightlist
+\item
+  HotWater
+\end{itemize}
+
+Future versions may have additional heating coil types.
+
+\paragraph{Field: Heating Coil Availability Schedule Name}\label{field-heating-coil-availability-schedule-name}
+
+Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period
+
+\paragraph{Field: Heating Coil Design Setpoint}\label{field-heating-coil-design-setpoint}
+
+This is the design supply air temperature in C used to size the heating supply air flow and the heating coil. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50\(^{o}\)C.
+
+\paragraph{Field: Dedicated Outdoor Air System Name}\label{field-dedicated-outdoor-air-system-name-1}
+
+Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the outdoor air flow rate for this zone equipment object will be set to zero and the DOAS will provide the ventilation air to the zone based on the outdoor air specifications in this object. For this fancoil system (ref. ZoneHVAC:FourPipeFanCoil):, the ``Capacity Control Method'' will be set to CyclingFan if a DOAS system is specified. If this field is blank, then the zone served by this fancoil system will not be served by a DOAS, and the fancoil Capacity Control Method will be ConstantFanVariableFlow.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-000}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Cooling Coil Design Setpoint will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-000}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-000}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Heating Coil Design Setpoint will be used for sizing the zone heating design air flow rate and the heating coil. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-000}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-2-000}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-1}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Fan Coil Capacity Control Method}\label{field-fan-coil-capacity-control-method}
+
+This input denotes how the unit's output is controlled in order to meet zone heating or cooling requirement. The choices are \emph{ConstantFanVariableFlow}, \emph{CyclingFan}, \emph{VariableFanVariableFlow} or \emph{VariableFanConstantFlow}. For \emph{ConstantFanVariableFlow}, the fan speed is held constant to produce a fixed air flow rate whenever the unit is scheduled on. The hot water or chilled flow rate is varied so that the unit output matches the zone heating or cooling requirement. For \emph{CyclingFan}, the fan speed is chosen so that the unit capacity is greater than or equal to the heating / cooling load and the fan is cycled to match unit output with the load. For \emph{VariableFanVariableFlow} both air and water flow rates are varied to match the load. For \emph{VariableFanConstantFlow,} the water flow rate is at full flow and the fan speed varies to meet the load. If this field is left blank, it will default to \emph{CyclingFan} if a Dedicated Outdoor Air System is specified (see above), otherwise it will default to \emph{ConstantFanVariableFlow.}
+
+\paragraph{Field: Low Speed Supply Air Flow Ratio}\label{field-low-speed-supply-air-flow-ratio}
+
+This numerical field specifies the ratio of the low speed flow rate to the maximum supply air flow rate. Its value should be less than \emph{Medium Speed Supply Air Flow Ratio.} If left blank, the default value is 0.33. This field is ignored if the capacity control method selected is not \emph{CyclingFan}.
+
+\paragraph{Field: Medium Speed Supply Air Flow Ratio}\label{field-medium-speed-supply-air-flow-ratio}
+
+This numerical field specifies the ratio of the medium speed flow rate to the maximum supply air flow rate. Its value should be greater than the \emph{Low Speed Supply Air Flow Ratio} but less than 1.If left blank, the default value is 0.66. This field is ignored if the capacity control method selected is not \emph{CyclingFan}.
+
+\paragraph{Field: Outdoor Air Schedule Name}\label{field-outdoor-air-schedule-name}
+
+\paragraph{The name of a schedule whose values (0.0 to 1.0) are used as multipliers to alter the outdoor air flow rate. If this field is left blank, the values will default to 1.0. This schedule is ignored if the zone is served by an HVACTemplate dedicated outdoor air system.}\label{the-name-of-a-schedule-whose-values-0.0-to-1.0-are-used-as-multipliers-to-alter-the-outdoor-air-flow-rate.-if-this-field-is-left-blank-the-values-will-default-to-1.0.-this-schedule-is-ignored-if-the-zone-is-served-by-an-hvactemplate-dedicated-outdoor-air-system.}
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-1}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-1}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-1}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the fan coil system. The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the fan coil system.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:FanCoil,
+  SPACE1-1,                !- Zone Name
+  All Zones,               !- Template Thermostat Name
+  autosize,                !- Supply Air Maximum Flow Rate {m3/s}
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
+  FanAvailSched,           !- System Availability Schedule Name
+  0.7,                     !- Supply Fan Total Efficiency
+  75,                      !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  1,                       !- Supply Fan Motor in Air Stream Fraction
+  ChilledWater,            !- Cooling Coil Type
+  ,                        !- Cooling Coil Availability Schedule Name
+  12.5,                    !- Cooling Coil Design Setpoint {C}
+  HotWater,                !- Heating Coil Type
+  ,                        !- Heating Coil Availability Schedule Name
+  50,                      !- Heating Coil Design Setpoint {C}
+  ,                        !- Dedicated Outdoor Air System Name
+  SupplyAirTemperature, !- Zone Cooling Design Supply Air Temperature Input Method
+  ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
+  SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
+  ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
+  ,            !- Design Specification Outdoor Air Object Name
+  ,            !- Design Specification Zone Air Distribution Object Name
+  ConstantFanVariableFlow, !- Fan Coil Capacity Control Method
+  ,                        !- Low Speed Supply Air Flow Ratio
+  ,                        !- Medium Speed Supply Air Flow Ratio
+  OUTAIRFANCOILSCHEDULE,   !- Outdoor Air Schedule Name
+  None,        !- Baseboard Heating Type
+  ,            !- Baseboard Heating Availability Schedule Name
+  Autosize;    !- Baseboard Heating Capacity {W}
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:PTAC}\label{hvactemplatezoneptac}
+
+This object simulates a packaged terminal air conditioner (PTAC) with a DX cooling coil, a heating coil (electric, gas, or hot water), and an outdoor air mixer. The optional hot water heating coil is served directly by HVACTemplate:Plant:HotWaterLoop and HVACTemplate:Plant:Boiler objects. No HVACTemplate:System object is required. Reference ZoneHVAC:PackagedTerminalAirConditioner for more details about the PTAC model.
+
+\begin{figure}[hbtp] % fig 154
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image603.png}
+\caption{Schematic of a packaged terminal air conditioner with draw through fan placement \protect \label{fig:schematic-of-a-packaged-terminal-air}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-4-016}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-3-001}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-3}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-000}
+
+This field specifies the supply air flow rate when the DX cooling coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-000}
+
+This field specifies the supply air flow rate when the heating coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate}
+
+This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner's supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation). By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will \emph{not} be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers.The units are in m3/s. The default is autosize.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-2}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Heating Supply Air Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-1}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Cooling Supply Air Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-3}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-3}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-3}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-3}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-2}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. When the fan operating mode schedule indicates continuous fan operation, the fan will operate whenever this schedule is 1.0. If the fan operating schedule indicates cycling fan operation, then fan will only cycle on as needed to meet a load.
+
+\paragraph{Field: Supply Fan Operating Mode Schedule Name}\label{field-supply-fan-operating-mode-schedule-name}
+
+This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{DrawThrough}.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-1}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 75.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency-1}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. The default is 0.9.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-1}
+
+Enter the type of cooling coil. There is currently only one choices for this field, SingleSpeedDX.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-1}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Coil Gross Rated Total Capacity}\label{field-cooling-coil-gross-rated-total-capacity}
+
+Enter autosize to let the automatic sizing algorithm determine the cooling coil gross capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the ``gross'', i.e., the effect of supply air fan heat is NOT accounted for. The units are in W. The default is autosize.
+
+\paragraph{Field: Cooling Coil Gross Rated Sensible Heat Ratio}\label{field-cooling-coil-gross-rated-sensible-heat-ratio}
+
+Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the rated capacity and air flow rate. Otherwise, enter the value of the ratio of the sensible capacity divided by total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be ``gross'', i.e., the effect of supply air fan heat is not accounted for. The default is autosize.
+
+\paragraph{Field: Cooling Coil Gross Rated Cooling COP}\label{field-cooling-coil-gross-rated-cooling-cop}
+
+Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 3.0.
+
+\paragraph{Field: Heating Coil Type}\label{field-heating-coil-type-1}
+
+Enter the type of heating coil. The choices for this field are
+
+\begin{itemize}
+\item
+  Electric
+\item
+  HotWater
+\item
+  Gas
+\end{itemize}
+
+If HotWater is specified, then a HVACTemplate:Plant:HotWaterLoop and a HVACTemplate:Plant:Boiler must be included in the input file to serve this hot water coil. The default is Electric.
+
+\paragraph{Field: Heating Coil Availability Schedule Name}\label{field-heating-coil-availability-schedule-name-1}
+
+Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of 1.0 indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period
+
+\paragraph{Field: Heating Coil Capacity}\label{field-heating-coil-capacity}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the coil can deliver in Watts. The default is autosize.
+
+\paragraph{Field: Gas Heating Coil Efficiency}\label{field-gas-heating-coil-efficiency}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default. This field applies only if the heating coil type is gas.
+
+\paragraph{Field: Gas Heating Coil Parasitic Electric Load}\label{field-gas-heating-coil-parasitic-electric-load}
+
+Enter the parasitic electric load associated with the gas heating coil operation, such as a combustion fan. The units are in W. This field applies only if the heating coil type is gas.
+
+\paragraph{Field: Dedicated Outdoor Air System Name}\label{field-dedicated-outdoor-air-system-name-2}
+
+Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the outdoor air flow rate for this zone equipment object (ref. ZoneHVAC: PackagedTerminalAirConditioner) will be set to zero and the DOAS will provide the ventilation air to the zone based on the outdoor air specifications in this object. If this field is blank, then the zone served by this PTAC system will not be served by a DOAS.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-1}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature-000}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 14\(^{o}\)C.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-1}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-1}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Heating Coil Design Setpoint will be used for sizing the zone heating design air flow rate and the heating coil. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature-000}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50\(^{o}\)C.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-1}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-3-000}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-2}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-2}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-2}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-2}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the PTAC system. The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the PTAC system.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:PTAC,
+  SPACE1-1,                !- Zone Name
+  All Zones,               !- Template Thermostat Name
+  autosize,                !- Cooling Supply Air Flow Rate {m3/s}
+  autosize,                !- Heating Supply Air Flow Rate {m3/s}
+  ,                        !- No Load Supply Air Flow Rate {m3/s}
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  ,                  !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  ,                        !- Outdoor Air Flow Rate per Zone {m3/s}
+  ,                        !- System Availability Schedule Name
+  ,                        !- Supply Fan Operating Mode Schedule Name
+  DrawThrough,             !- Supply Fan Placement
+  0.7,                     !- Supply Fan Total Efficiency
+  75,                      !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  SingleSpeedDX,           !- Cooling Coil Type
+  ,                        !- Cooling Coil Availability Schedule Name
+  autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
+  autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
+  3,                       !- Cooling Coil Gross Rated COP
+  Electric,                !- Heating Coil Type
+  ,                        !- Heating Coil Availability Schedule Name
+  autosize,                !- Heating Coil Capacity {W}
+  0.8,                     !- Gas Heating Coil Efficiency
+  ,                        !- Gas Heating Coil Parasitic Electric Load {W}
+  ,                        !- Dedicated Outdoor Air System Name
+  SupplyAirTemperature, !- Zone Cooling Design Supply Air Temperature Input Method
+  14.0,        !- Zone Cooling Design Supply Air Temperature {C]
+  ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
+  SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
+  50.0,        !- Zone Heating Design Supply Air Temperature {C]
+  ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
+  ,            !- Design Specification Outdoor Air Object Name
+  ,            !- Design Specification Zone Air Distribution Object Name
+  None,        !- Baseboard Heating Type
+  ,            !- Baseboard Heating Availability Schedule Name
+  Autosize;    !- Baseboard Heating Capacity {W}
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:PTHP}\label{hvactemplatezonepthp}
+
+This object simulates a packaged terminal air-to-air heat pump (PTHP) with a DX cooling coil, a DX air-to-air heat pump heating coil, a supplemental heating coil (electric or gas), and an outdoor air mixer. No HVACTemplate:System object is required. Reference ZoneHVAC:PackagedTerminalHeatPump for more details about the PTHP model.
+
+\begin{figure}[hbtp] % fig 155
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image604.png}
+\caption{Schematic of a packaged terminal heat pump (draw through fan placement) \protect \label{fig:schematic-of-a-packaged-terminal-heat-pump}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-5-014}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-4-001}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-4}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-1}
+
+This field specifies the supply air flow rate when the DX cooling coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-1}
+
+This field specifies the supply air flow rate when the heating coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-1}
+
+This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner's supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation). By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will \emph{not} be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-3}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Heating Supply Air Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-2}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Cooling Supply Air Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-4}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-4}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-4}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-4}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-3}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. When the fan operating mode schedule indicates continuous fan operation, the fan will operate whenever this schedule is 1.0. If the fan operating schedule indicates cycling fan operation, then fan will only cycle on as needed to meet a load.
+
+\paragraph{Field: Supply Fan Operating Mode Schedule Name}\label{field-supply-fan-operating-mode-schedule-name-1}
+
+This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement-1}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{DrawThrough}.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-2}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure-1}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 75.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency-2}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. The default is 0.9.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-2}
+
+Enter the type of cooling coil. There is currently only one choices for this field, SingleSspeedDX.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-2}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Coil Gross Rated Total Capacity}\label{field-cooling-coil-gross-rated-total-capacity-1}
+
+Enter autosize to let the automatic sizing algorithm determine the gross cooling coil total capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize.
+
+\paragraph{Field: Cooling Coil Gross Rated Sensible Heat Ratio}\label{field-cooling-coil-gross-rated-sensible-heat-ratio-1}
+
+Enter Autosize to allow the sizing algorithm to determine the gross sensible heat ratio based on the gross rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by the gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be ``gross'', i.e., the effect of supply air fan heat is not accounted for. The default is autosize.
+
+\paragraph{Field: Cooling Coil Gross Rated COP}\label{field-cooling-coil-gross-rated-cop}
+
+Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The default is 3.0. The gross COP should not account for the supply air fan.
+
+\paragraph{Field: Heat Pump Heating Coil Type}\label{field-heat-pump-heating-coil-type}
+
+Enter the type of heat pump heating coil. There is currently only one choices for this field, SingleSpeedDXHeatPump.
+
+\paragraph{Field: Heat Pump Heating Coil Availability Schedule Name}\label{field-heat-pump-heating-coil-availability-schedule-name}
+
+Usually set to blank, which allows the heat pump heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. A schedule value of 1.0 indicates that the heat pump heating coil can be on during a given time period. A value of zero denotes that the heat pump heating coil cannot be used during that time period.
+
+\paragraph{Field: Heat Pump Heating Coil Gross Rated Capacity}\label{field-heat-pump-heating-coil-gross-rated-capacity}
+
+Enter autosize to let the automatic sizing algorithm determine the heat pump heating coil gorss rated capacity based on the maximum heating loads during the heating design day. If a value is entered, it represents the full load gross heating capacity, in watts of the DX heat pump unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize.
+
+\paragraph{Field: Heat Pump Heating Coil Gross Rated COP}\label{field-heat-pump-heating-coil-gross-rated-cop}
+
+Enter the coefficient of performance defined as the gross heating coil capacity in watts divided by electrical power input in watts of the DX heating coil unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 2.75.
+
+\paragraph{Field: Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature}\label{field-heat-pump-heating-minimum-outdoor-dry-bulb-temperature}
+
+This numeric field defines the minimum outdoor dry-bulb temperature in degrees Celsius for PTHP compressor operation. The compressor will not operate (for DX heating or DX cooling) when outdoor dry-bulb temperatures fall below this value. The minimum value must be greater than or equal to -20 °C. The default value is -8°C.
+
+\paragraph{Field: Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature}\label{field-heat-pump-defrost-maximum-outdoor-dry-bulb-temperature}
+
+This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 C and less than or equal to 7.22 C. If this input field is left blank, the default value is 5 C.
+
+\paragraph{Field: Heat Pump Defrost Strategy}\label{field-heat-pump-defrost-strategy}
+
+This alpha field has two choices: \emph{ReverseCycle} or \emph{Resistive}. If the \emph{ReverseCycle} strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a \emph{Resistive} defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is \emph{ReverseCycle}.
+
+\paragraph{Field: Heat Pump Defrost Control}\label{field-heat-pump-defrost-control}
+
+This alpha field has two choices: \emph{Timed} or \emph{OnDemand}. If \emph{Timed} control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For \emph{Timed} defrost control, the fractional amount of time the unit is in defrost is entered in the input field ``Defrost Time Period Fraction'' described below. If \emph{OnDemand} defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field ``Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature'' described above. If this input field is left blank, the default defrost control is \emph{Timed}.
+
+\paragraph{Field: Heat Pump Defrost Time Period Fraction}\label{field-heat-pump-defrost-time-period-fraction}
+
+This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to ``timed'' defrost (see Heat Pump Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
+
+\paragraph{Field: Supplemental Heating Coil Type}\label{field-supplemental-heating-coil-type}
+
+Enter the type of supplemental heating coil. The choices for this field are
+
+\begin{itemize}
+\item
+  Electric
+\item
+  Gas
+\item
+  HotWater
+\end{itemize}
+
+The default is Electric.
+
+\paragraph{Field: Supplemental Heating Coil Availability Schedule Name}\label{field-supplemental-heating-coil-availability-schedule-name}
+
+Usually set to blank, which allows the supplemental heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when supplemental heating is only available seasonally. The schedule values denote whether the supplemental heating coil can run during a given time period. A schedule value of 1.0 indicates that the supplemental heating coil can be on during a given time period. A value of zero denotes that the supplemental heating coil cannot be used during that time period
+
+\paragraph{Field: Supplemental Heating Coil Capacity}\label{field-supplemental-heating-coil-capacity}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the supplemental heating coil can deliver in Watts. The default is autosize.
+
+\paragraph{Field: Supplemental Heating Coil Maximum Outdoor Dry-Bulb Temperature}\label{field-supplemental-heating-coil-maximum-outdoor-dry-bulb-temperature}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
+
+\paragraph{Field: Supplemental Gas Heating Coil Efficiency}\label{field-supplemental-gas-heating-coil-efficiency}
+
+Enter supplemental heating coil gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default. This field applies only if the supplemental heating coil type is gas.
+
+\paragraph{Field: Supplemental Gas Heating Coil Parasitic Electric Load}\label{field-supplemental-gas-heating-coil-parasitic-electric-load}
+
+Enter the parasitic electric load associated with the gas supplemental heating coil operation, such as a combustion fan. The units are in W. The default is 0.0. This field applies only if the supplemental heating coil type is gas.
+
+\paragraph{Field: Dedicated Outdoor Air System Name}\label{field-dedicated-outdoor-air-system-name-3}
+
+Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the outdoor air flow rate for this zone equipment object (ref. ZoneHVAC:PackagedTerminalHeatPump) will be set to zero and the DOAS will provide the ventilation air to the zone based on the outdoor air specifications in this object. If this field is blank, then the zone served by this PTHP system will not be served by a DOAS.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-2}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature-1}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 14\(^{o}\)C.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-2}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-2}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Heating Coil Design Setpoint will be used for sizing the zone heating design air flow rate and the heating coil. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature-1}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50\(^{o}\)C.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-2}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-4}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-3}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-3}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-3}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-3}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the PTHP system. The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the PTHP system.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:PTHP,
+  SPACE1-1,                !- Zone Name
+  All Zones,               !- Template Thermostat Name
+  autosize,                !- Cooling Supply Air Flow Rate {m3/s}
+  autosize,                !- Heating Supply Air Flow Rate {m3/s}
+  ,                        !- No Load Supply Air Flow Rate {m3/s}
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  ,                  !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  ,                        !- Outdoor Air Flow Rate per Zone {m3/s}
+  ,                        !- System Availability Schedule Name
+  ,                        !- Supply Fan Operating Mode Schedule Name
+  DrawThrough,             !- Supply Fan Placement
+  0.7,                     !- Supply Fan Total Efficiency
+  75,                      !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  SingleSpeedDX,           !- Cooling Coil Type
+  ,                        !- Cooling Coil Availability Schedule Name
+  autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
+  autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
+  3,                       !- Cooling Coil Gross Rated COP
+  SingleSpeedDXHeatPump,   !- Heat Pump Heating Coil Type
+  ,                    !- Heat Pump Heating Coil Availability Schedule Name
+  autosize,                !- Heat Pump Heating Coil Gross Rated Capacity {W}
+  2.75,                    !- Heat Pump Heating Coil Gross Rated COP
+  -8,         !- Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature {C}
+  5,          !- Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature {C}
+  ReverseCycle,            !- Heat Pump Defrost Strategy
+  Timed,                   !- Heat Pump Defrost Control
+  0.058333,                !- Heat Pump Defrost Time Period Fraction
+  Electric,                !- Supplemental Heating Coil Type
+  ,           !- Supplemental Heating Coil Availability Schedule Name
+  autosize,                !- Supplemental Heating Coil Capacity {W}
+  21,     !- Supplemental Heating Coil Max Outdoor Dry-Bulb Temperature {C}
+  0.8,                     !- Supplemental Gas Heating Coil Efficiency
+  ,          !- Supplemental Gas Heating Coil Parasitic Electric Load {W}
+  ,                        !- Dedicated Outdoor Air System Name
+  SupplyAirTemperature, !- Zone Cooling Design Supply Air Temperature Input Method
+  14.0,        !- Zone Cooling Design Supply Air Temperature {C]
+  ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
+  SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
+  50.0,        !- Zone Heating Design Supply Air Temperature {C]
+  ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
+  ,            !- Design Specification Outdoor Air Object Name
+  ,            !- Design Specification Zone Air Distribution Object Name
+  None,        !- Baseboard Heating Type
+  ,            !- Baseboard Heating Availability Schedule Name
+  Autosize;    !- Baseboard Heating Capacity {W}
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:WaterToAirHeatPump}\label{hvactemplatezonewatertoairheatpump}
+
+This object simulates the zone portion of a water source heat pump system. Often many HVACTemplate:Zone:WaterToAirHeatPump objects will be used in a building along with a single HVACTemplate:Plant:MixedWaterLoop that contains a cooling tower and boiler.
+
+\subsubsection{Inputs}\label{inputs-6-011}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-5-001}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-5}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-2}
+
+This field specifies the supply air flow rate when the unit is operating in cooling mode. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-2}
+
+This field specifies the supply air flow rate when the unit is operating in heating mode. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-2}
+
+This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., the coil is off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation). . By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will \emph{not} be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-4}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Heating Supply Air Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-3}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Cooling Supply Air Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-5}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-5}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-5}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-5}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-4}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. When the fan operating mode schedule indicates continuous fan operation, the fan will operate whenever this schedule is 1.0. If the fan operating schedule indicates cycling fan operation, then fan will only cycle on as needed to meet a load.
+
+\paragraph{Field: Supply Fan Operating Mode Schedule Name}\label{field-supply-fan-operating-mode-schedule-name-2}
+
+This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement-2}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{DrawThrough}.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-3}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure-2}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 75.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency-3}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. The default is 0.9.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-3}
+
+Enter the type of cooling coil. There is currently only one choices for this field, Coil:Cooling:WaterToAirHeatPump:EquationFit.
+
+\paragraph{Field: Cooling Coil Gross Rated Total Capacity}\label{field-cooling-coil-gross-rated-total-capacity-2}
+
+Enter autosize to let the automatic sizing algorithm determine the cooling coil gross rated total capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions (26.7C (80F) entering air dry-bulb temperature, 19.4C (67F) entering air wet-bulb temperature, and 29.4C (85F) entering water temperature). Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize. If a value is specified for this field, it is recommended that the Cooling Coil Rated Sensible Heat Ratio also be specified (see below for more details).
+
+\paragraph{Field: Cooling Coil Gross Rated Sensible Heat Ratio}\label{field-cooling-coil-gross-rated-sensible-heat-ratio-2}
+
+Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by gross total cooling capacity of the DX cooling coil at rated conditions (26.7C (80F) entering air dry-bulb temperature, 19.4C (67F) entering air wet-bulb temperature, and 29.4C (85F) entering water temperature). Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be ``gross'' , i.e., the effect of supply air fan heat is not accounted for. The default is autosize. If the Cooling Coil Rated Capacity is autosized, this field should also be autosized (any value specified for Cooling Coil Rate Sensibe Heat Ratio will be ignored). If the Cooling Coil Rated Capacity has a specified value, then this field should also have a specified value. This is because the Coil:Cooling:WaterToAirHeatPump:EquationFit object has fields for Rated Total Cooling Capacity and Rated Sensible Cooling Capacity. If this field is autosized, a specified value for Cooling Coil Rated Capacity will not be used when the coil object sensible capacity is autosized.
+
+\paragraph{Field: Cooling Coil Gross Rated COP}\label{field-cooling-coil-gross-rated-cop-1}
+
+Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions (26.7C (80F) entering air dry-bulb temperature, 19.4C (67F) entering air wet-bulb temperature, and 29.4C (85F) entering water temperature). The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 3.5.
+
+\paragraph{Field: Heat Pump Heating Coil Type}\label{field-heat-pump-heating-coil-type-1}
+
+Enter the type of heat pump heating coil. There is currently only one choices for this field, Coil:Heating:WaterToAirHeatPump:EquationFit.
+
+\paragraph{Field: Heat Pump Heating Coil Gross Rated Capacity}\label{field-heat-pump-heating-coil-gross-rated-capacity-1}
+
+Enter autosize to let the automatic sizing algorithm determine the heat pump heating coil gross capacity based on the maximum heating loads during the heating design day. If a value is entered, it represents the full load heating capacity, in watts of the DX heat pump unit at rated conditions (21.11C (70F) entering air dry-bulb temperature and 21.11C (70F) entering water temperature). Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize.
+
+\paragraph{Field: Heat Pump Heating Coil Gross Rated COP}\label{field-heat-pump-heating-coil-gross-rated-cop-1}
+
+Enter the coefficient of performance defined as the gross heating coil capacity in watts divided by electrical power input in watts of the DX heating coil unit at rated conditions (21.11C (70F) entering air dry-bulb temperature and 21.11C (70F) entering water temperature). The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 4.2.
+
+\paragraph{Field: Supplemental Heating Coil Availability Schedule Name}\label{field-supplemental-heating-coil-availability-schedule-name-1}
+
+Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when supplemental heating is only available seasonally. The schedule values denote whether the supplemental heating coil can run during a given time period. A schedule value of 1.0 indicates that the supplemental heating coil can be on during a given time period. A value of zero denotes that the supplemental heating coil cannot be used during that time period
+
+\paragraph{Field: Supplemental Heating Coil Capacity}\label{field-supplemental-heating-coil-capacity-1}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the supplemental heating coil can deliver in Watts. The default is autosize.
+
+\paragraph{Field: Maximum Cycling Rate}\label{field-maximum-cycling-rate-000}
+
+This numeric field contains the maximum on-off cycling rate for the compressor, which occurs at 50\% run time fraction. Suggested values are shown below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image605.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Heat Pump Time Constant}\label{field-heat-pump-time-constant}
+
+This numeric field contains the time constant for the cooling coil's capacity to reach steady state after startup. Suggested values are shown below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image606.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Fraction of On-Cycle Power Use}\label{field-fraction-of-on-cycle-power-use}
+
+This numeric field contains the fraction of on-cycle power use to adjust the part load fraction based on the off-cycle power consumption due to crankcase heaters, controls, fans, and etc. Suggested value values are below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image607.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Heat Pump Fan Delay Time}\label{field-heat-pump-fan-delay-time}
+
+This numeric field contains the time delay in seconds for the heat pump supply air fan to shut off after compressor cycle off. This value can be obtained from the manufacturer or the heat pump catalog. Suggested value is 60 seconds. This value is disregared at times when the WaterToAirHeatPump's fan operating mode schedule value is greater than 0 (i.e., continuous fan mode).
+
+\paragraph{Field: Dedicated Outdoor Air System Name}\label{field-dedicated-outdoor-air-system-name-4}
+
+Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the outdoor air flow rate for this zone equipment object (ref. ZoneHVAC:WaterToAirHeatPump) will be set to zero and the DOAS will provide the ventilation air to the zone based on the outdoor air specifications in this object. If this field is blank, then the zone served by this water-to-air heat pump system will not be served by a DOAS.
+
+\paragraph{Field: Supplemental Heating Coil Type}\label{field-supplemental-heating-coil-type-1}
+
+Enter the type of supplemental heating coil. The choices for this field are
+
+\begin{itemize}
+\item
+  Electric
+\item
+  HotWater
+\end{itemize}
+
+The default is Electric.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-3}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature-2}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 14\(^{o}\)C.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-3}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-3}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Heating Coil Design Setpoint will be used for sizing the zone heating design air flow rate and the heating coil. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature-2}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50\(^{o}\)C.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-3}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+\paragraph{Field: Heat Pump Coil Water Flow Mode}\label{field-heat-pump-coil-water-flow-mode}
+
+This field specifies the way in which water flow through the heat pump coils will be modeled. For this template, WatertoAirHeatPump:EquationFit coil objects are generated and, therefore, there are three options:
+
+\begin{itemize}
+\item
+  Cycling
+\item
+  Constant
+\item
+  ConstantOnDemand
+\end{itemize}
+
+\textbf{Cycling} varies water flow through the coil based on the heat pump Part Load Ratio. This control method is appropriate for modeling heat pumps that are outfitted with a soleniod valve which allows water to flow through the coil only when the compressor is active. This is the \textbf{default} for EnergyPlus V8 and later.
+
+\textbf{Constant} provides a constant water flow regardless of heat pump operation. Remember that EnergyPlus has two coils (a heating coil and a cooling coil) to approximate the operation of one coil that can operate in either heating mode or cooling mode. Therefore, when the water flow mode is constant, there will be full flow through either the heating coil or the cooling coil, but not both at the same time.
+
+\textbf{ConstantOnDemand} provides full flow through the coil whenever there is a load. When there is no load, there is zero flow through the coil. This control strategy represents the way EnergyPlus modeled heat pump water flow prior to Version 8.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-5}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-4}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-4}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-4}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-4}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the heat pump system. The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the heat pump system.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:WaterToAirHeatPump,
+  SPACE1-1,                !- Zone Name
+  All Zones,               !- Template Thermostat Name
+  autosize,                !- Cooling Supply Air Flow Rate {m3/s}
+  autosize,                !- Heating Supply Air Flow Rate {m3/s}
+  ,                        !- No Load Supply Air Flow Rate {m3/s}
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  Flow/Person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  ,                !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  ,                        !- Outdoor Air Flow Rate per Zone {m3/s}
+  ,                        !- System Availability Schedule Name
+  ,                        !- Supply Fan Operating Mode Schedule Name
+  DrawThrough,             !- Supply Fan Placement
+  0.7,                     !- Supply Fan Total Efficiency
+  75,                      !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  Coil:Cooling:WaterToAirHeatPump:EquationFit,  !- Cooling Coil Type
+  autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
+  autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
+  3,                       !- Cooling Coil Gross Rated COP
+  Coil:Heating:WaterToAirHeatPump:EquationFit,  !- HPump Heating Coil Type
+  autosize,                !- Heat Pump Heating Coil Gross Rated Capacity {W}
+  2.75,                    !- Heat Pump Heating Coil Gross Rated COP
+  ,                !- Supplemental Heating Coil Availability Schedule Name
+  autosize,                !- Supplemental Heating Coil Capacity {W}
+  2.5,                     !- Maximum Cycling Rate {cycles/hr}
+  60,                      !- Heat Pump Time Constant {s}
+  0.01,                    !- Fraction of On-Cycle Power Use
+  60,                      !- Heat Pump Fan Delay Time {s}
+  ,                        !- Dedicated Outdoor Air System Name
+  Electric,                !- Supplemental Heating Coil Type
+  SupplyAirTemperature, !- Zone Cooling Design Supply Air Temperature Input Method
+  14.0,        !- Zone Cooling Design Supply Air Temperature {C]
+  ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
+  SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
+  50.0,        !- Zone Heating Design Supply Air Temperature {C]
+  ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
+  ,            !- Design Specification Outdoor Air Object Name
+  !- Design Specification Zone Air Distribution Object Name
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:VRF}\label{hvactemplatezonevrf}
+
+This object simulates a variable refrigerant flow (VRF) zone terminal unit which is served by an HVACTemplate:System:VRF condenser unit. Reference ZoneHVAC:TerminalUnit:VariableRefrigerantFlow for more details about the VRF terminal unit model.
+
+\subsubsection{Inputs}\label{inputs-7-011}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-6-001}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-6}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-5}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Heating Supply Air Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-4}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Cooling Supply Air Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Rated Total Heating Capacity Sizing Ratio}\label{field-rated-total-heating-capacity-sizing-ratio}
+
+This numeric field defines the ratio of the heating coil to cooling coil size when autosizing is used. The model assumes that when used, this value will be greater than 1. This field supersedes the Rated Total Heating Capacity Sizing Ratio entered in the AirConditioner:VariableRefrigerantFlow object. If this field is left blank, the value entered in the parent object is used for sizing. If neither field is used, the sizing ratio is assumed to be 1.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-3}
+
+This field specifies the supply air flow rate when the terminal unit is operating in cooling mode. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: No Cooling Supply Air Flow Rate}\label{field-no-cooling-supply-air-flow-rate}
+
+This field specifies the supply air flow rate when the terminal unit's cooling coil is not operating and the previous mode was cooling.. This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner's supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation). By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will \emph{not} be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-3}
+
+This field specifies the supply air flow rate when the heating coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: No Heating Supply Air Flow Rate}\label{field-no-heating-supply-air-flow-rate}
+
+This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner's supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation). By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will \emph{not} be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is autosize.
+
+\paragraph{Field: Cooling Outdoor Air Flow Rate}\label{field-cooling-outdoor-air-flow-rate}
+
+This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in cooling mode. If this field is set to autosize it will be sized based on the outdoor air inputs below, unless a dedicated outdoor air system is specified for this zone and then it will be set to zero.
+
+\paragraph{Field: Heating Outdoor Air Flow Rate}\label{field-heating-outdoor-air-flow-rate}
+
+This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in heating mode. If this field is set to autosize it will be sized based on the outdoor air inputs below, unless a dedicated outdoor air system is specified for this zone and then it will be set to zero.
+
+\paragraph{Field: No Load Outdoor Air Flow Rate}\label{field-no-load-outdoor-air-flow-rate}
+
+This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is not operating in cooling or heating mode. If this field is set to autosize it will be sized based on the outdoor air inputs below, unless a dedicated outdoor air system is specified for this zone and then it will be set to zero.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-6}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-6}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-6}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-6}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-6}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-5}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-5}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. When the fan operating mode schedule indicates continuous fan operation, the fan will operate whenever this schedule is 1.0. If the fan operating schedule indicates cycling fan operation, then fan will only cycle on as needed to meet a load.
+
+\paragraph{Field: Supply Fan Operating Mode Schedule Name}\label{field-supply-fan-operating-mode-schedule-name-3}
+
+This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement-3}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{DrawThrough}.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-4}
+
+Enter the total efficiency of the supply fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure-3}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 75.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency-4}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. The default is 0.9.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-4}
+
+Enter the type of cooling coil. The options are \emph{VariableRefrigerantFlowDX} or None. The default is \emph{VariableRefrigerantFlowDX}.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-3}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Coil Gross Rated Total Capacity}\label{field-cooling-coil-gross-rated-total-capacity-3}
+
+Enter autosize to let the automatic sizing algorithm determine the gross cooling coil total capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize.
+
+\paragraph{Field: Cooling Coil Gross Rated Sensible Heat Ratio}\label{field-cooling-coil-gross-rated-sensible-heat-ratio-3}
+
+Enter Autosize to allow the sizing algorithm to determine the gross sensible heat ratio based on the gross rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by the gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be ``gross'', i.e., the effect of supply air fan heat is not accounted for. The default is autosize.
+
+\paragraph{Field: Heat Pump Heating Coil Type}\label{field-heat-pump-heating-coil-type-2}
+
+Enter the type of heat pump heating coil. The options are \emph{VariableRefrigerantFlowDX} or None. The default is \emph{VariableRefrigerantFlowDX}.
+
+\paragraph{Field: Heat Pump Heating Coil Availability Schedule Name}\label{field-heat-pump-heating-coil-availability-schedule-name-1}
+
+Usually set to blank, which allows the heat pump heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. A schedule value of 1.0 indicates that the heat pump heating coil can be on during a given time period. A value of zero denotes that the heat pump heating coil cannot be used during that time period.
+
+\paragraph{Field: Heat Pump Heating Coil Gross Rated Capacity}\label{field-heat-pump-heating-coil-gross-rated-capacity-2}
+
+Enter autosize to let the automatic sizing algorithm determine the heat pump heating coil gorss rated capacity based on the maximum heating loads during the heating design day. If a value is entered, it represents the full load gross heating capacity, in watts of the DX heat pump unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize.
+
+\paragraph{Field: Zone Terminal Unit On Parasitic Electric Energy Use}\label{field-zone-terminal-unit-on-parasitic-electric-energy-use}
+
+This numeric field defines the parasitic electrical energy use of the zone terminal unit when either terminal unit coil is operating. When in cooling mode, this electric energy use is reported in a zone terminal unit cooling electric consumption output variable. When in heating mode, this electric energy use is reported in a zone terminal unit heating electric consumption output variable.
+
+\paragraph{Field: Zone Terminal Unit Off Parasitic Electric Energy Use}\label{field-zone-terminal-unit-off-parasitic-electric-energy-use}
+
+This numeric field defines the parasitic electrical energy use of the zone terminal unit when the terminal unit coil(s) is not operating. When the previous mode was cooling, this electric energy use is reported in a zone terminal unit cooling electric consumption output variable. When the previous mode was heating, this electric energy use is reported in a zone terminal unit heating electric consumption output variable.
+
+\paragraph{Field: Dedicated Outdoor Air System Name}\label{field-dedicated-outdoor-air-system-name-5}
+
+Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the outdoor air flow rate for this zone equipment object (ref. ZoneHVAC: TerminalUnit:VariableRefrigerantFlow) will be set to zero and the DOAS will provide the ventilation air to the zone based on the outdoor air specifications in this object. If this field is blank, then the zone served by this VRF terminal unit will not be served by a DOAS.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-4}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature-3}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 14\(^{o}\)C.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-4}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-4}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Heating Coil Design Setpoint will be used for sizing the zone heating design air flow rate and the heating coil. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature-3}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50\(^{o}\)C.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-4}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-5}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-5}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-5}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the PTHP system. The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the PTHP system.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:VRF,
+  SPACE1-1,                !- Zone Name
+  All Zones,               !- Template Thermostat Name
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  ,                        !- Rated Total Heating Capacity Sizing Ratio
+  autosize,                !- Cooling Supply Air Flow Rate{m3/s}
+  autosize,                !- No Cooling Supply Air Flow Rate{m3/s}
+  autosize,                !- Heating Supply Air Flow Rate{m3/s}
+  autosize,                !- No Heating Supply Air Flow Rate{m3/s}
+  autosize,                !- Cooling Outdoor Air Flow Rate{m3/s}
+  autosize,                !- Heating Outdoor Air Flow Rate{m3/s}
+  autosize,                !- No Load Outdoor Air Flow Rate{m3/s}
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  ,            !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  ,                        !- Outdoor Air Flow Rate per Zone {m3/s}
+  ,            !- Design Specification Outdoor Air Object Name
+  ,            !- Design Specification Zone Air Distribution Object Name
+  ,                        !- System Availability Schedule Name
+  ,                        !- Supply Fan Operating Mode Schedule Name
+  DrawThrough,             !- Supply Fan Placement
+  0.7,                     !- Supply Fan Total Efficiency
+  75,                      !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  VariableRefrigerantFlowDX,  !- Cooling Coil Type
+  ,                        !- Cooling Coil Availability Schedule Name
+  autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
+  autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
+  VariableRefrigerantFlowDX,  !- Heat Pump Heating Coil Type
+  ,                        !- Heat Pump Heating Coil Availability Schedule Name
+  autosize,                !- Heat Pump Heating Coil Gross Rated Capacity {W}
+  0,           !- Zone Terminal Unit On Parasitic Electric Energy Use {W}
+  0,           !- Zone Terminal Unit Off Parasitic Electric Energy Use {W}
+  ,                        !- Dedicated Outdoor Air System Name
+  SupplyAirTemperature, !- Zone Cooling Design Supply Air Temperature Input Method
+  14.0,        !- Zone Cooling Design Supply Air Temperature {C}
+  ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
+  SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
+  50.0,        !- Zone Heating Design Supply Air Temperature {C}
+  ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC}
+  None,        !- Baseboard Heating Type
+  ,            !- Baseboard Heating Availability Schedule Name
+  Autosize;    !- Baseboard Heating Capacity {W}
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:Unitary}\label{hvactemplatezoneunitary}
+
+This object simulates the zone portion of a constant volume direct-expansion based HVAC configuration with several different heating options. Often a single HVACTemplate:Zone:Unitary object will be used with a single HVACTemplate:System:Unitary (or HVACTemplate:System:UnitaryHeatPump:AirToAir , or HVACTemplate:System:UnitarySystem) object to simulate single zone direct-expansion based air conditioning systems. In addition, multiple HVACTemplate:Zone:Unitary objects may appear that all reference the same HVACTemplate:System object in a multiple zone version. For a multizone system, only one zone is specified as the control zone (see HVACTemplate:System:Unitary, HVACTemplate:System:UnitaryHeatPump:AirToAir , or HVACTemplate:System:UnitarySystem for more information). Direct expansion includes single packaged rooftop systems commonly seen in commercial applications and split systems commonly seen in residential applications.
+
+\subsubsection{Inputs}\label{inputs-8-009}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-7-001}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template Unitary System Name}\label{field-template-unitary-system-name}
+
+Enter the name of the HVACTemplate:System:Unitary, HVACTemplate:System:UnitaryHeatPump:AirToAir , or HVACTemplate:System:UnitarySystem object serving this zone.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-7}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Supply Air Maximum Flow Rate}\label{field-supply-air-maximum-flow-rate-1}
+
+By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. Note that the zone must have a thermostat specified in order to autosize the flow rate, even if it is not the control zone in a multiple zone unitary system. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The template unitary system object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-6}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-5}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-7}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
+
+If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-7}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-7}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-7}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name}
+
+This field allows the user to specify a supply plenum which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name}
+
+This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-6}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-6}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-6}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the unitary air handling system. The baseboard heating will be set to heating priority 2, which means it will meet any remaining heating load not met by the unitary system. Prior to v7.1, the capacity was only applied to electric baseboard. Starting with v7.1, the capacity will be used for both hot water and electric baseboard.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-5}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. \emph{SystemSupplyAirTemperature} means that the Cooling Design Supply Air Temperature from the template unitary system serving this zone will be used. The default is \emph{SystemSupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature-4}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 12.8°C.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-5}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-5}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Heating Design Supply Air Temperature will be used for sizing the zone heating design air flow rate. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. \emph{SystemSupplyAirTemperature} means that the Heating Design Supply Air Temperature from the template unitary system serving this zone will be used. The default is \emph{SystemSupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature-4}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50°C.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-5}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-7}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-6}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:Unitary,
+  SPACE1-1,                !- Zone Name
+  Furnace DX 1-1,          !- Template Unitary System Name
+  All Zones,               !- Template Thermostat Name
+  autosize,                !- Supply Air Maximum Flow Rate {m3/s}
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
+  ,                        !- Supply Plenum Name
+  ,                        !- Return Plenum Name
+  None,                    !- Baseboard Heating Type
+  ,                        !- Baseboard Heating Availability Schedule Name
+  Autosize,                !- Baseboard Heating Capacity {W}
+  SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
+  ,            !- Zone Cooling Design Supply Air Temperature {C]
+  ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
+  SystemSupplyAirTemperature, !- Zone Heating Design Supply Air . . . Input Method
+  ,            !- Zone Heating Design Supply Air Temperature {C]
+  ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
+  ,            !- Design Specification Outdoor Air Object Name
+  ;            !- Design Specification Zone Air Distribution Object Name
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:VAV}\label{hvactemplatezonevav}
+
+This object simulates the zone portion of a variable air volume HVAC configuration with several different heating options. When heating is required, this terminal unit will activate the reheat coil first, and then increase airflow if reverse action is specified. Multiple HVACTemplate:Zone:VAV, HVACTemplate:Zone:VAV:FanPowered or HVACTemplate:Zone:VAV:HeatAndCool objects are usually specified for each HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object. Reheat is specified at the zone level. Reference AirTerminal:SingleDuct:VAV:Reheat and AirTerminal:SingleDuct:VAV:NoReheat for more details about VAV terminal units.
+
+\subsubsection{Inputs}\label{inputs-9-008}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-8-001}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template VAV System Name}\label{field-template-vav-system-name}
+
+Enter the name of the HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object serving this zone.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-8}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Supply Air Maximum Flow Rate}\label{field-supply-air-maximum-flow-rate-2}
+
+By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-7}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-6}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Minimum Air Flow Method}\label{field-zone-minimum-air-flow-method-000}
+
+This field is used to select how the program will determine the minimum flow rate to the zone while the system is operating. There are three choices for selecting how the minimum flow rate is specified: Constant, FixedFlowRate, and Scheduled. If Constant is entered, then the program will use the value for the constant minimum air flow fraction entered in the following field. If FixedFlowRate is entered, then the program will use the value entered in the field below called Fixed Minimum Air Flow Rate.If Scheduled is entered, then the program will obtain the value for minimum flow fraction from the schedule named in the field below called Minimum Air Flow Fraction Schedule Name.
+
+\paragraph{Field: Constant Minimum Air Flow Fraction}\label{field-constant-minimum-air-flow-fraction-000}
+
+The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default). This field is used if the previous field is set to Constant. If the previous field is set to Scheduled (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then this field is optional and can be used to separately control the air flow rate used for sizing normal-action reheat coils. If this field and the following field have values, the greater of the two is used for sizing.
+
+\paragraph{Field: Fixed Minimum Air Flow Rate}\label{field-fixed-minimum-air-flow-rate-000}
+
+The minimum flow rate to the zone while the system is operating, specified as a fixed minimum air flow rate in meters cubed per second. The minimum air flow rate is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default). This field is used if the Zone Minimum Air Flow Method field is set to FixedFlowRate. If the Zone Minimum Air Flow Method field is set to Scheduled (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then this field is optional and can be used to separately control the air flow rate used for sizing normal-action reheat coils. Only one of these two minimum air flow fields (i.e., this field and the previous field) should be used at any time. If this field and the previous field have values, the greater of the two is used for sizing.
+
+\paragraph{Field: Minimum Air Flow Fraction Schedule Name}\label{field-minimum-air-flow-fraction-schedule-name-000}
+
+The name of a schedule that determines the value of the minimum air flow fraction. The schedule should contain fractions from 0.0 to 1.0. These values will define the minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default). This field is used if the previous field is set to Scheduled. If the previous field is left blank (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then the air flow rate usedfor sizing normal-action reheat coils is the average of the minimum and maximum values in this schedule. The air flow rate used for reheat coil sizing is reported with other component sizing information as ``Reheat Coil Sizing Air Volume Flow Rate.''
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-8}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name for Sizing and Design Specification Zone Air Distribution Object Name fields below.
+
+If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-8}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-8}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-8}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Reheat Coil Type}\label{field-reheat-coil-type}
+
+A reheat coil may be added to the VAV box with this field. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Reheat Coil Availability Schedule Name}\label{field-reheat-coil-availability-schedule-name}
+
+Leave this field blank if you want the reheat coil to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the coil is available should be specified as 1.0. Those times that the coil is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the coil is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Damper Heating Action}\label{field-damper-heating-action-000}
+
+The VAV box flow rate can be controlled in one of two ways during heating operation:
+
+\begin{itemize}
+\item
+  Normal
+\item
+  Reverse
+\end{itemize}
+
+Under ``Normal'' operation, the supply air flow into the zone is the minimum air flow rate of the VAV system during heating, essentially acting like a constant volume system during heating. Under ``Reverse'' the air flow rate through the VAV box may increase above the minimum air flow when the heating demand cannot be satisfied unless greater air flow is provided. The default value is Normal. Reverse action only applies when Reheat Coil Type is HotWater. For electric reheat coils, Normal and Reverse behave the same. For more details, please see the section for AirTerminal:SingleDuct:VAV:Reheat.
+
+\paragraph{Control Fields for Maximum Flow During Reheat:}\label{control-fields-for-maximum-flow-during-reheat-000}
+
+The following two fields are used only when Reheat Coil Object Type = Coil:Heating:Water and Damper Heating Action = Reverse. Maximum Flow per Zone Floor Area During Reheat and Maximum Flow Fraction During Reheat are two optional methods to calculate the maximum allowable air flow rate during reheat operation. If both are entered, the greater resulting flow rate is used. If Design Specification Outdoor Air Object Name is also specified, it may increase this limit to meet the outdoor air flow rate requirement. At no time will the maximum flow rate calculated here exceed the value for Maximum Air Flow Rate. This limit is active only when the zone thermostat requests heating and the VAV box damper is reverse acting.
+
+\paragraph{Field: Maximum Flow per Zone Floor Area During Reheat}\label{field-maximum-flow-per-zone-floor-area-during-reheat-000}
+
+This factor (m\(^{3}\)/s-m\(^{2}\)) is multiplied by the zone area, to determine the maximum volume flow rate (m\(^{3}\)/s) allowed during reheat operation (see detailed explanation above). This field is autocalculatable. If autocalculate is selected, the value is set to 0.002032 m\(^{3}\)/s-m\(^{2}\) (0.4 cfm/ft\(^{2}\)). If this field and the following field are entered, the greater of the two inputs is used. If this field and the following field are left blank, the maximum flow will not be limited.
+
+\paragraph{Field: Maximum Flow Fraction During Reheat}\label{field-maximum-flow-fraction-during-reheat-000}
+
+This fraction is multiplied by the Maximum Air Flow Rate to determine the maximum volume flow rate (m\(^{3}\)/s) allowed during reheat operation (see detailed explanation above). This field is autocalculatable. If autocalculate is selected, the value is set to 0.002032 m\(^{3}\)/s-m\(^{2}\) (0.4 cfm/ft\(^{2}\)) multiplied by the zone floor area divided by the Maximum Air Flow Rate. If this field and the previous field are entered, the greater of the two inputs is used. If this field and the previous field are left blank, the maximum flow will not be limited.
+
+\paragraph{Field: Maximum Reheat Air Temperature}\label{field-maximum-reheat-air-temperature-000}
+
+This field specifies the maximum allowable supply air temperature (°C) leaving the reheat coil in a VAV terminal unit during heating operation. If left blank, there is no limit, and the supply air temperature to the space may become unrealistically high during heating operation. If unknown, a value of 35C (95F) is recommended. There is no default in order to maintain consistency with prior results.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name for Control}\label{field-design-specification-outdoor-air-object-name-for-control}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object. When this field is used, the terminal unit will increase flow as needed to meet this outdoor air requirement. If Outdoor Air Flow per Person is non-zero (in the specified DesignSpecification:OutdoorAir object), then the outdoor air requirement will be computed based on the current number of occupants in the zone. At no time will the supply air flow rate exceed the value for Maximum Air Flow Rate. If this field is blank, then the terminal unit will not be controlled for outdoor air flow. See documentation for the zone HVAC outdoor air object for further information (Ref DesignSpecification:OutdoorAir object).
+
+Note that this field is used only for specifying the design outdoor air flow rate used for controlling the terminal unit air flow rate. The field \emph{Design Specification Outdoor Air Object Name for Sizing} (see below) is used to specify the design outdoor air flow rate.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name-1}
+
+This field allows the user to specify a supply plenum which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-1}
+
+This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-7}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-7}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-7}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the VAV air handling system. The baseboard heating will be set to heating priority 2, which means it will meet any remaining heating load not met by the VAV system. Prior to v7.1, the capacity was only applied to electric baseboard. Starting with v7.1, the capacity will be used for both hot water and electric baseboard.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-6}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. \emph{SystemSupplyAirTemperature} means that the Cooling Design Supply Air Temperature from the template VAV system serving this zone will be used (Ref. HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV). The default is \emph{SystemSupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature-5}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 12.8°C.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-6}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-6}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Heating Design Supply Air Temperature will be used for sizing the zone heating design air flow rate and the heating or reheat coil. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature-5}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50\(^{o}\)C.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-6}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name for Sizing}\label{field-design-specification-outdoor-air-object-name-for-sizing}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}. Note that this field is used only for specifying the design outdoor air flow rate used for sizing. The field \emph{Design Specification Outdoor Air Object Name for Sizing} (see above) is used to actively control the VAV terminal air flow rate.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-7}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:VAV,
+  SPACE1-1,                !- Zone Name
+  VAV Sys 1,               !- Template VAV System Name
+  All Zones,               !- Template Thermostat Name
+  autosize,                !- Supply Air Maximum Flow Rate {m3/s}
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  Constant,                !- Zone Minimum Air Flow Input Method
+  0.3,                     !- Constant Minimum Air Flow Fraction
+  ,                        !- Fixed Minimum Air Flow Rate {m3/s}
+  ,                        !- Minimum Air Flow Fraction Schedule Name
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
+  HotWater,                !- Reheat Coil Type
+  ,                        !- Reheat Coil Availability Schedule Name
+  Reverse,                 !- Heating Damper Action
+  ,             !- Maximum Flow per Zone Floor Area During Reheat {m3/s-m2}
+  ,                        !- Maximum Flow Fraction During Reheat
+  ,                        !- Maximum Reheat Air Temperature
+  ,             !- Design Specification Outdoor Air Object Name for Control
+  ,                        !- Supply Plenum Name
+  ,                        !- Return Plenum Name
+  None,                    !- Baseboard Heating Type
+  ,                        !- Baseboard Heating Availability Schedule Name
+  autosize;                !- Baseboard Heating Capacity {W}
+  SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
+  ,            !- Zone Cooling Design Supply Air Temperature {C]
+  ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
+  SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
+  50.0,        !- Zone Heating Design Supply Air Temperature {C]
+  ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
+  ,            !- Design Specification Outdoor Air Object Name for Sizing
+  ;            !- Design Specification Zone Air Distribution Object Name
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:VAV:FanPowered}\label{hvactemplatezonevavfanpowered}
+
+This object simulates the zone portion of a variable air volume HVAC configuration with a series or parallel fan powered terminal unit (also know as a powered induction unit or PIU) and several different heating options. Multiple HVACTemplate:Zone:VAV, HVACTemplate:Zone:VAV:FanPowered or HVACTemplate:Zone:VAV:HeatAndCool objects are usually specified for each HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object. Reheat is specified at the zone level.
+
+The series powered induction unit is an air system terminal unit that mixes varying amounts of secondary (recirculated) air and primary (conditioned supply) air to produce a fixed flow of air to a zone. The unit contains a small fan that acts to induce the secondary air and a heating coil for heating the mixed secondary and primary air. The fan runs at a constant volume flow rate whenever the unit is on (and the fan's availability schedule is on or it is activated by an availability manager). With HVACTemplate:Zone:VAV:FanPowered, the secondary fan will operate according to the Zone PIU Fan Schedule and any Night Cycle Control specified in the system it is served by.) The fan is downstream of the primary and secondary air inlets. The variable mixing is accomplished by a damper in the unit's primary air supply inlet duct. This damper can move from fully open (100\% primary air. 0\% secondary air) to a minimum stop that is specified in the input description. At full cooling the damper will be fully open. At minimum cooling and for heating the damper will be at the minimum stop and the secondary air flow will be at its maximum. Reference object AirTerminal:SingleDuct:SeriesPIU:Reheat for more details.
+
+\begin{figure}[hbtp] % fig 156
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image608.png}
+\caption{Series PIU Terminal Unit \protect \label{fig:series-piu-terminal-unit-001}}
+\end{figure}
+
+The parallel powered induction unit is an air system terminal unit that mixes varying amounts of secondary (recirculated) air and primary (conditioned supply) air to produce a variable total flow of air to a zone. The unit contains a small fan that acts to induce the secondary air and a heating coil for heating the mixed secondary and primary air. The secondary and primary air streams enter the unit in parallel. The fan sits in the secondary air stream and runs only when the primary air flow is below the Parallel Fan On Flow Fraction and the fan's availability schedule is on or it is activated by an availability manager. With HVACTemplate:Zone:VAV:FanPowered, the secondary fan will operate according to the Zone PIU Fan Schedule and any Night Cycle Control specified in the system it is served by.). The primary air inlet contains a damper that can move from fully open (maximum primary air) to a minimum stop (minimum primary air). At full cooling load the primary air damper is fully open and the fan is off. The primary air flow is at maximum and there is little or no secondary air flow. As the cooling load decreases, the primary air damper gradually closes and the secondary air flow remains close to zero. At some point, usually when the primary air flow has reached the minimum, the fan switches on and secondary air is induced. The heating coil will switch on as needed to meet any heating demand. Reference object AirTerminal:SingleDuct:ParallelPIU:Reheat for more details.
+
+\begin{figure}[hbtp] % fig 157
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image609.png}
+\caption{Parallel PIU Terminal Unit \protect \label{fig:parallel-piu-terminal-unit-001}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-10-008}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-9-000}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template VAV System Name}\label{field-template-vav-system-name-1}
+
+Enter the name of the HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object serving this zone.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-9}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Primary Supply Air Maximum Flow Rate}\label{field-primary-supply-air-maximum-flow-rate}
+
+In a fan powered VAV terminal unit, the primary air flow is the air supplied by the central air handler. By entering Autosize, the maximum primary supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified and cooling SizingPeriod:DesignDay. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-8}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Primary Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-7}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Primary Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Primary Supply Air Minimum Flow Fraction}\label{field-primary-supply-air-minimum-flow-fraction}
+
+Enter the fraction that the VAV box can reduce to based on the primary supply air maximum flow rate. This field may be sized automatically by entering Autosize.
+
+\paragraph{Field: Secondary Supply Air Maximum Flow Rate}\label{field-secondary-supply-air-maximum-flow-rate}
+
+In a fan powered VAV terminal unit, the secondary air flow is the air taken from the zone by the terminal unit fan. By entering Autosize, the maximum secondary supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s.
+
+\paragraph{Field: Flow Type}\label{field-flow-type}
+
+This field specifies the type of fan powered unit (PIU). The choices for this field are:
+
+\begin{itemize}
+\item
+  Series -- Series configuration with recirculation directly from the zone
+\item
+  Parallel -- Parallel configuration with recirculation directly from the zone
+\item
+  SeriesFromPlenum -- Series configuration with recirculation from the return plenum
+\item
+  ParallelFromPlenum -- Parallel configuration with recirculation from the return plenum
+\end{itemize}
+
+See descriptions of these configurations in the general description for this object, above. For all types, the secondary fan will run according to the Zone PIU Fan Schedule (see below) and any Night Cycle Control specified in the system which serves this terminal unit (see Template VAV System Name above). For Parallel PIU, there is an additional secondary fan control based on the primary air flow fraction (see Parallel Fan On Flow Fraction below). For recirculation from plenum, a Return Plenum Name must be specificed in this object or in the system object (HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV) which serves this terminal unit. The default is Parallel.
+
+\paragraph{Field: Parallel Fan On Flow Fraction}\label{field-parallel-fan-on-flow-fraction}
+
+For parallel PIUs, this field specifies the fraction of the primary air flow at which fan turns on. In the parallel PIU the fan operation is intermittent. If the primary air flow is above this fraction of the maximum, the fan is off. Otherwise the secondary fan will run according to the System Availability Schedule and Night Cycle Control specified in the HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV which serves this terminal unit. This field does not apply to series PIUs.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-9}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
+
+If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-9}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-9}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-9}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Reheat Coil Type}\label{field-reheat-coil-type-1}
+
+A reheat coil may be added to the VAV box with this field. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\end{itemize}
+
+The default choice is Electric.
+
+\paragraph{Field: Reheat Coil Availability Schedule Name}\label{field-reheat-coil-availability-schedule-name-1}
+
+Leave this field blank if you want the reheat coil to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the coil is available should be specified as 1.0. Those times that the coil is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the coil is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Fan Total Efficiency}\label{field-fan-total-efficiency-001}
+
+Enter the total efficiency of the zone induction fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Fan Delta Pressure}\label{field-fan-delta-pressure}
+
+Enter the pressure rise of the zone induction fan in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa.
+
+\paragraph{Field: Fan Motor Efficiency}\label{field-fan-motor-efficiency}
+
+Enter the shaft power of the zone induction fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. Note that the zone fan motor is assumed to be 100\% in the air stream.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name-2}
+
+This field allows the user to specify a supply plenum which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-2}
+
+This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-8}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-8}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-8}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the VAV air handling system. The baseboard heating will be set to heating priority 2, which means it will meet any remaining heating load not met by the VAV system. Prior to v7.1, the capacity was only applied to electric baseboard. Starting with v7.1, the capacity will be used for both hot water and electric baseboard.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-7}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. \emph{SystemSupplyAirTemperature} means that the Cooling Design Supply Air Temperature from the template VAV system serving this zone will be used (Ref. HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV). The default is \emph{SystemSupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature-6}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 12.8°C.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-7}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-7}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Heating Design Supply Air Temperature will be used for sizing the zone heating design air flow rate and the heating or reheat coil. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature-6}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50\(^{o}\)C.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-7}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+\paragraph{Field: Zone PIU Fan Schedule Name}\label{field-zone-piu-fan-schedule-name}
+
+This is the operating schedule for the zone PIU fan. For a parallel PIU, the zone fan operates only when the primary air flow is below the Parallel Fan On Flow Fraction and the Zone PIU Fan Schedule is on, or when it is activated by an availability manager. For a series PIU, the zone fan operates whenever the Zone PIU Fan Schedule is on, or it is activated by an availability manager. If this field is left blank, the System Availability Schedule for the HVACTemplate:System serving this zone will be used.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-8}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-8}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:VAV:FanPowered,
+  SPACE1-1,                !- Zone Name
+  VAV Sys 1,               !- Template VAV System Name
+  All Zones,               !- Template Thermostat Name
+  autosize,                !- Primary Supply Air Maximum Flow Rate {m3/s}
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  autosize,                !- Primary Supply Air Minimum Flow Fraction
+  autosize,                !- Secondary Supply Air Maximum Flow Rate {m3/s}
+  Series,                  !- Flow Type
+  autosize,                !- Parallel Fan On Flow Fraction
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
+  HotWater,                !- Reheat Coil Type
+  ,                        !- Reheat Coil Availability Schedule Name
+  0.7,                     !- Fan Total Efficiency
+  1000,                    !- Fan Delta Pressure {Pa}
+  0.9,                     !- Fan Motor Efficiency
+  ,                        !- Supply Plenum Name
+  ,                        !- Return Plenum Name
+  None,                    !- Baseboard Heating Type
+  ,                        !- Baseboard Heating Availability Schedule Name
+  autosize;                !- Baseboard Heating Capacity {W}
+  SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
+  ,            !- Zone Cooling Design Supply Air Temperature {C]
+  ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
+  SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
+  50.0,        !- Zone Heating Design Supply Air Temperature {C]
+  ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
+  ,            !- Zone PIU Fan Schedule Name
+  ,            !- Design Specification Outdoor Air Object Name
+  ;            !- Design Specification Zone Air Distribution Object Name
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:VAV:HeatAndCool}\label{hvactemplatezonevavheatandcool}
+
+This object simulates the zone portion of a variable air volume HVAC configuration with several different heating options. When heating is required, this terminal unit will increase airflow first and then activate the optional reheat coil. Multiple HVACTemplate:Zone:VAV, HVACTemplate:Zone:VAV:FanPowered, or HVACTemplate:Zone:VAV:HeatAndCool objects are usually specified for each HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object. Reheat is specified at the zone level. Reference AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat and AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat for more details about these VAV terminal units.
+
+\subsubsection{Inputs}\label{inputs-11-006}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-10}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template VAV System Name}\label{field-template-vav-system-name-2}
+
+Enter the name of the HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object serving this zone.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-10}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Supply Air Maximum Flow Rate}\label{field-supply-air-maximum-flow-rate-3}
+
+By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-9}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-8}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Constant Minimum Air Flow Fraction}\label{field-constant-minimum-air-flow-fraction-1-000}
+
+The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default). This field is used if the previous field is set to Constant. If the previous field is set to Scheduled (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then this field is optional and can be used to separately control the air flow rate used for sizing normal-action reheat coils. If this field and the following field have values, the greater of the two is used for sizing.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-10}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name for Sizing and Design Specification Zone Air Distribution Object Name fields below.
+
+If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-10}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-10}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-10}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name for Sizing}\label{field-design-specification-outdoor-air-object-name-for-sizing-1}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}. Note that this field is used only for specifying the design outdoor air flow rate used for sizing. The field \emph{Design Specification Outdoor Air Object Name for Sizing} (see above) is used to actively control the VAV terminal air flow rate.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-9}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Reheat Coil Type}\label{field-reheat-coil-type-2}
+
+A reheat coil may be added to the VAV box with this field. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Reheat Coil Availability Schedule Name}\label{field-reheat-coil-availability-schedule-name-2}
+
+Leave this field blank if you want the reheat coil to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the coil is available should be specified as 1.0. Those times that the coil is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the coil is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Maximum Reheat Air Temperature}\label{field-maximum-reheat-air-temperature-1-000}
+
+This field specifies the maximum allowable supply air temperature (°C) leaving the reheat coil in a VAV terminal unit during heating operation. If left blank, there is no limit, and the supply air temperature to the space may become unrealistically high during heating operation. If unknown, a value of 35C (95F) is recommended. There is no default in order to maintain consistency with prior results.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name-3}
+
+This field allows the user to specify a supply plenum which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-3}
+
+This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-9}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-9}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-9}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the VAV air handling system. The baseboard heating will be set to heating priority 2, which means it will meet any remaining heating load not met by the VAV system. Prior to v7.1, the capacity was only applied to electric baseboard. Starting with v7.1, the capacity will be used for both hot water and electric baseboard.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-8}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. \emph{SystemSupplyAirTemperature} means that the Cooling Design Supply Air Temperature from the template VAV system serving this zone will be used (Ref. HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV). The default is \emph{SystemSupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature-7}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 12.8°C.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-8}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-8}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Heating Design Supply Air Temperature will be used for sizing the zone heating design air flow rate and the heating or reheat coil. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is \emph{SupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature-7}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50\(^{o}\)C.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-8}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:VAV:HeatAndCool,
+  SPACE1-1,                !- Zone Name
+  VAV Sys 1,               !- Template VAV System Name
+  All Zones,               !- Template Thermostat Name
+  autosize,                !- Supply Air Maximum Flow Rate {m3/s}
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  0.3,                     !- Constant Minimum Air Flow Fraction
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
+  ,            !- Design Specification Outdoor Air Object Name for Sizing
+  ,            !- Design Specification Zone Air Distribution Object Name
+  HotWater,                !- Reheat Coil Type
+  ,                        !- Reheat Coil Availability Schedule Name
+  ,                        !- Maximum Reheat Air Temperature
+  ,                        !- Supply Plenum Name
+  ,                        !- Return Plenum Name
+  None,                    !- Baseboard Heating Type
+  ,                        !- Baseboard Heating Availability Schedule Name
+  autosize;                !- Baseboard Heating Capacity {W}
+  SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
+  ,            !- Zone Cooling Design Supply Air Temperature {C]
+  ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
+  SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
+  50.0,        !- Zone Heating Design Supply Air Temperature {C]
+  ;            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:ConstantVolume}\label{hvactemplatezoneconstantvolume}
+
+This object simulates the zone portion of a constant volume HVAC configuration with or without reheat. One or more HVACTemplate:Zone:ConstantVolume objects will be used with a single HVACTemplate:System:ConstantVolume which has optional chilled water cooling and several types of heating. Reference AirTerminal:SingleDuct:Uncontrolled and AirTerminal:SingleDuct:ConstantVolume:Reheat for more details about the terminal units.
+
+\subsubsection{Inputs}\label{inputs-12-006}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-11}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template Constant Volume System Name}\label{field-template-constant-volume-system-name}
+
+Enter the name of the HVACTemplate:System:ConstantVolume object serving this zone.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-11}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Supply Air Maximum Flow Rate}\label{field-supply-air-maximum-flow-rate-4}
+
+By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. Note that the zone must have a thermostat specified in order to autosize the flow rate, even if it is not the control zone in a multiple zone unitary system. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The HVACTemplate:System:ConstantVolume object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-10}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-9}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-11}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
+
+If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-11}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-11}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-11}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-9}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-10}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Reheat Coil Type}\label{field-reheat-coil-type-3}
+
+A reheat coil may be added to the terminal unit with this field. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Reheat Coil Availability Schedule Name}\label{field-reheat-coil-availability-schedule-name-3}
+
+Leave this field blank if you want the reheat coil to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the coil is available should be specified as 1.0. Those times that the coil is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the coil is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Maximum Reheat Air Temperature}\label{field-maximum-reheat-air-temperature-2-000}
+
+This field specifies the maximum allowable supply air temperature (°C) leaving the reheat coil during heating operation. If left blank, there is no limit, and the supply air temperature to the space may become unrealistically high during heating operation. If unknown, a value of 35C (95F) is recommended. There is no default in order to maintain consistency with prior results.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name-4}
+
+This field allows the user to specify a supply plenum which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-4}
+
+This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-10}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-10}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-10}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the air handling system. The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the air handling system.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-9}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. \emph{SystemSupplyAirTemperature} means that the Cooling Coil Design Setpoint Temperature from the template system serving this zone will be used (Ref. HVACTemplate:System:ConstantVolume). The default is \emph{SystemSupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature-8}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 12.8°C.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-9}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-9}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Heating Design Supply Air Temperature will be used for sizing the zone heating design air flow rate. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. \emph{SystemSupplyAirTemperature} means that the Heating Coil Design Setpoint Temperature from the template system serving this zone will be used (Ref. HVACTemplate:System:ConstantVolume). The default is \emph{SystemSupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature-8}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50\(^{o}\)C.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-9}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:ConstantVolume,
+  SPACE1-1,                !- Zone Name
+  CAV Sys 1,               !- Template Constant Volume System Name
+  All Zones,               !- Template Thermostat Name
+  autosize,                !- Supply Air Maximum Flow Rate {m3/s}
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  0.0,                     !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
+  ,                        !- Design Specification Outdoor Air Object Name
+  ,                       !- Design Specification Zone Air Distribution Object Name
+  HotWater,                !- Reheat Coil Type
+  ,                        !- Reheat Coil Availability Schedule Name
+  ,                        !- Maximum Reheat Air Temperature {C}
+  ,                        !- Supply Plenum Name
+  ,                        !- Return Plenum Name
+  None,                    !- Baseboard Heating Type
+  ,                        !- Baseboard Heating Availability Schedule Name
+  autosize;                !- Baseboard Heating Capacity {W}
+  SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
+  12.8,                    !- Zone Cooling Design Supply Air Temperature {C]
+  11.11,          !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
+  SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
+  50,                      !- Zone Heating Design Supply Air Temperature {C]
+  30;             !- Zone Heating Design Supply Air Temperature Difference {deltaC]
+\end{lstlisting}
+
+\subsection{HVACTemplate:Zone:DualDuct}\label{hvactemplatezonedualduct}
+
+This object simulates the zone portion of a constant volume or variable volume dual-duct HVAC system. One or more HVACTemplate:Zone:DualDuct objects may be used with a single HVACTemplate:System:DualDuct object which has optional chilled water cooling and several types of heating. A constant air volume dual duct system is simulated by setting the Zone Minimum Air Flow Fraction = 1.0. A variable air volume duct duct system is simulated by setting the Zone Minimum Air Flow Fraction \textless{}1.0. . Reference AirTerminal:DualDuct:ConstantVolume and AirTerminal:DualDuct:VAV for more details about the terminal units.
+
+\subsubsection{Inputs}\label{inputs-13-005}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-12}
+
+Enter the name of the zone. The name must match a building zone name used in the ZONE object.
+
+\paragraph{Field: Template Dual Duct System Name}\label{field-template-dual-duct-system-name}
+
+Enter the name of the HVACTemplate:System:DualDuct object serving this zone.
+
+\paragraph{Field: Template Thermostat Name}\label{field-template-thermostat-name-12}
+
+Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
+
+When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
+
+\paragraph{Field: Supply Air Maximum Flow Rate}\label{field-supply-air-maximum-flow-rate-5}
+
+By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. Note that the zone must have a thermostat specified in order to autosize the flow rate, even if it is not the control zone in a multiple zone unitary system. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The HVACTemplate:System:DualDuct object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor-11}
+
+This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor-10}
+
+This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized. If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
+
+\paragraph{Field: Zone Minimum Air Flow Fraction}\label{field-zone-minimum-air-flow-fraction-000}
+
+The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. This field is ignored is the system serving this zone is constant volume.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method-12}
+
+The input must be either \emph{Flow/Zone}, or \emph{Flow/Person}, \emph{Flow/Area}, \emph{Sum}, \emph{Maximum or DetailedSpecification}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow} as the zone design outdoor air flow rate. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the maximum occupancy to calculate a zone design outdoor air flow rate. \emph{Flow/Area} means the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} to calculated a zone design outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be added to obtain the zone design outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area} and \emph{Outdoor Air Flow per Zone} will be used for the zone design outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\emph{DetailedSpecification} means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
+
+If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
+
+\paragraph{Field: Outdoor Air Flow Rate per Person}\label{field-outdoor-air-flow-rate-per-person-12}
+
+The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone Floor Area}\label{field-outdoor-air-flow-rate-per-zone-floor-area-12}
+
+The design outdoor air volumetric flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is multiplied by the zone area to obtain a flow rate. This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow Rate per Zone}\label{field-outdoor-air-flow-rate-per-zone-12}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name for Sizing}\label{field-design-specification-outdoor-air-object-name-for-sizing-2}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}. Note that this field is used only for specifying the design outdoor air flow rate used for sizing. The field \emph{Design Specification Outdoor Air Object Name for Control} (see below) is used to actively control the VAV terminal air flow rate.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name-11}
+
+This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone. This field is used only when \emph{Outdoor Air Method = DetailedSpecification}.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name for Control}\label{field-design-specification-outdoor-air-object-name-for-control-1}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object. When this field is used, the terminal unit will increase flow as needed to meet this outdoor air requirement. If Outdoor Air Flow per Person (in the specified DesignSpecification:OutdoorAir object) is non-zero, then the outdoor air requirement will be computed based on the current number of occupants in the zone. At no time will the supply air flow rate exceed the value for Maximum Air Flow Rate. If this field is blank, then the terminal unit will not be controlled for outdoor air flow. See documentation for the zone HVAC outdoor air object for further information (Ref DesignSpecification:OutdoorAir object).
+
+Note that this field is used only for specifying the design outdoor air flow rate used for controlling the terminal unit air flow rate. The field \emph{Design Specification Outdoor Air Object Name for Sizing} (see above) is used to specify the design outdoor air flow rate.
+
+\paragraph{Field: Cold Supply Plenum Name}\label{field-cold-supply-plenum-name}
+
+This field allows the user to specify a cold supply plenum zone which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Hot Supply Plenum Name}\label{field-hot-supply-plenum-name}
+
+This field allows the user to specify a hot supply plenum zone which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-5}
+
+This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
+
+\paragraph{Field: Baseboard Heating Type}\label{field-baseboard-heating-type-11}
+
+This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  None
+\end{itemize}
+
+The default choice is None.
+
+\paragraph{Field: Baseboard Heating Availability Schedule Name}\label{field-baseboard-heating-availability-schedule-name-11}
+
+Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
+
+\paragraph{Field: Baseboard Heating Capacity}\label{field-baseboard-heating-capacity-11}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts. Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the VAV air handling system. The baseboard heating will be set to heating priority 2, which means it will meet any remaining heating load not met by the VAV system. Prior to v7.1, the capacity was only applied to electric baseboard. Starting with v7.1, the capacity will be used for both hot water and electric baseboard.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method-10}
+
+This field selects the method for specifying the cooling design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. \emph{TemperatureDifference} means that the field Zone Cooling Design Supply Air Temperature Difference will be used. \emph{SystemSupplyAirTemperature} means that the Cooling Design Supply Air Temperature from the template system serving this zone will be used (Ref. HVACTemplate:System:DualDuct). The default is \emph{SystemSupplyAirTemperature.}
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature-9}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 12.8°C.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference-10}
+
+The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 11.11 deltaC.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method-10}
+
+This field selects the method for specifying the heating design supply air temperature. \emph{SupplyAirTemperature} means that the field Zone Heating Design Supply Air Temperature will be used for sizing the zone heating design air flow rate. \emph{TemperatureDifference} means that the field Zone Heating Design Supply Air Temperature Difference will be used. \emph{SystemSupplyAirTemperature} means that the Heating Coil Design Setpoint Temperature from the template system serving this zone will be used (Ref. HVACTemplate:System:DualDuct). The default is \emph{SystemSupplyAirTemperature.}
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature-9}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{SupplyAirTemperature.} The default is 50\(^{o}\)C.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference-10}
+
+The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is \emph{TemperatureDifference.} The default is 30 deltaC.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Zone:DualDuct,
+  SPACE1-1,                !- Zone Name
+  DD Sys 1,                !- Template Dual Duct System Name
+  All Zones,               !- Template Thermostat Name
+  autosize,                !- Supply Air Maximum Flow Rate {m3/s}
+  ,                        !- Zone Heating Sizing Factor
+  ,                        !- Zone Cooling Sizing Factor
+  0.2,                     !- Zone Minimum Air Flow Fraction
+  flow/person,             !- Outdoor Air Method
+  0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
+  0.0,                     !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
+  0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
+  ,                    !- Design Specification Outdoor Air Object Name for Sizing
+  ,                      !- Design Specification Zone Air Distribution Object Name
+  ,                    !- Design Specification Outdoor Air Object Name for Control
+  ,                        !- Cold Supply Plenum Name
+  ,                        !- Hot Supply Plenum Name
+  ,                        !- Return Plenum Name
+  None,                    !- Baseboard Heating Type
+  ,                        !- Baseboard Heating Availability Schedule Name
+  autosize;                !- Baseboard Heating Capacity {W}
+  SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
+  12.8,                    !- Zone Cooling Design Supply Air Temperature {C]
+  11.11,          !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
+  SystemSupplyAirTemperature, !- Zone Heating Design Supply Air . . . Input Method
+  50,                      !- Zone Heating Design Supply Air Temperature {C]
+  30;             !- Zone Heating Design Supply Air Temperature Difference {deltaC]
+\end{lstlisting}
+
+\subsection{HVACTemplate:System:VRF}\label{hvactemplatesystemvrf}
+
+This model simulates a variable-refrigerant-flow (or variable-refrigerant-volume) air-conditioning system. This system type models direct-expansion cooling and/or heating coils configured in a zone terminal unit (ref. HVACTemplate:Zone:VRF). For more details about this system type see AirConditioner:VariableRefrigerantFlow.
+
+\subsubsection{Inputs}\label{inputs-14-005}
+
+\paragraph{Field: Name}\label{field-name-1-021}
+
+Enter a name for the HVACTemplate:System:VRF object. This name is used in the HVACTemplate:Zone:VRF object to reference this system.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-6}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump operates during a given time period. A schedule value equal to 0 denotes that the heat pump must be off for that time period. A value other than 0 denotes that the heat pump is available to operate during that time period. This schedule may be used to completely disable the heat pump (and all of its terminal units) as required. If this field is blank, the unit is enabled the entire simulation.
+
+\paragraph{Field: Gross Rated Total Cooling Capacity}\label{field-gross-rated-total-cooling-capacity-000}
+
+This numeric field defines the gross rated total cooling capacity of the DX cooling coil in watts. The total cooling capacity should be a ``gross'', i.e., the effect of supply air fan heat NOT accounted for.
+
+\paragraph{Field: Gross Rated Cooling COP}\label{field-gross-rated-cooling-cop-000}
+
+This numeric field defines the cooling coefficient of performance at rated conditions. The cooling coefficient of performance includes compressor power and condenser fan power. This COP value does not account for impacts due to the supply air fan. The nominal heat pump cooling COP must be greater than 0. If this field is left blank, a default coefficient of performance of 3.3 is assumed.
+
+\paragraph{Field: Minimum Outdoor Temperature in Cooling Mode}\label{field-minimum-outdoor-temperature-in-cooling-mode}
+
+This numeric field defines the minimum outdoor dry-bulb temperature allowed for cooling operation. Below this temperature, cooling is disabled. If this field is left blank, the default value is -6ºC.
+
+\paragraph{Field: Maximum Outdoor Temperature in Cooling Mode}\label{field-maximum-outdoor-temperature-in-cooling-mode}
+
+This numeric field defines the maximum outdoor dry-bulb temperature allowed for cooling operation. Above this temperature, cooling is disabled. If this field is left blank, the default value is 43ºC.
+
+\paragraph{Field: Gross Rated Heating Capacity}\label{field-gross-rated-heating-capacity-000}
+
+This numeric field defines the gross total heat pump heating capacity at rated conditions in watts. The nominal heat pump heating capacity must be greater than 0 or set to autosize.
+
+\paragraph{Field: Rated Heating Capacity Sizing Ratio}\label{field-rated-heating-capacity-sizing-ratio}
+
+This numeric field defines the ratio of gross heating to gross cooling capacity. The model assumes that when used, this value will be greater than 1. A similar input is available in the ZoneHVAC:TerminalUnit:VariableRefrigerantFlow object. When the heating capacity is autosized, if this field is non-blank, this ratio is used to scale the heating capacity to the gross rated total cooling capacity regardless of the value entered in the terminal unit objects. When the heating capacity is not autosized, the gross rated heating capacity will be equal to the sum of the terminal unit heating coil size. If this field is blank and the terminal unit sizing ratio input is also blank, then the heating capacity sizing ratio is assumed to be 1. If this field is not blank and the heating capacity sizing ratio in the terminal unit object(s) is blank, then this ratio also applies to each heating coil. If this field is not blank and the heating capacity sizing ratio in the terminal units is also not blank, then the terminal unit heating coil capacity sizing ratio input applies to each heating coil.
+
+\paragraph{Field: Gross Rated Heating COP}\label{field-gross-rated-heating-cop-000}
+
+This numeric field defines the heating coefficient of performance at rated conditions. The heating coefficient of performance includes compressor power and condenser fan power. This gross COP value does NOT account for the supply air fan. The nominal heat pump heating COP must be greater than 0. If this field is left blank, a coefficient of performance of 3.4 is assumed.
+
+\paragraph{Field: Minimum Outdoor Temperature in Heating Mode}\label{field-minimum-outdoor-temperature-in-heating-mode}
+
+This numeric field defines the minimum outdoor temperature allowed for heating operation. Below this temperature, heating is disabled. If this field is left blank, the default value is -20ºC.
+
+\paragraph{Field: Maximum Outdoor Temperature in Heating Mode}\label{field-maximum-outdoor-temperature-in-heating-mode}
+
+This numeric field defines the maximum outdoor temperature allowed for heating operation. Above this temperature, heating is disabled. If this field is left blank, the default value is 16ºC.
+
+\paragraph{Field: Minimum Heat Pump Part-Load Ratio}\label{field-minimum-heat-pump-part-load-ratio}
+
+This numeric field specifies the minimum operating part-load ratio (PLR) of the heat pump. When the heat pump operates at a PLR below this value, the heat pump's compressor will cycle to meet the cooling or heating demand. Above this value, the heat pump's compressor operates the entire time step to meet the cooling or heating demand. The minimum value for this field is 0. If this field is left blank, the default value is 0.15. When the heat pump compressor cycles, the previous field is used to determine cycling losses.
+
+\paragraph{Field: Zone Name for Master Thermostat Location}\label{field-zone-name-for-master-thermostat-location}
+
+This alpha field defines the name of the zone where the ``master'' thermostat is located. When the heat pump is connected to multiple zone terminal units, one terminal unit must be selected as the master thermostat. The remaining thermostats are slaves and can operate only in the same mode as the master thermostat.
+
+\paragraph{Field: Master Thermostat Priority Control Type}\label{field-master-thermostat-priority-control-type}
+
+This choice field determines the logic used to simulate the ``master'' thermostat. Valid choices are LoadPriority, ZonePriority, ThermostatOffsetPriority, MasterThermostatPriority, and Scheduled. The default value is MasterThermostatPriority. When LoadPriority is selected, the total zone load is used to choose the operating mode as either cooling or heating. When ZonePriority is selected, the number of zones requiring cooling or heating determines the operating mode. When ThermostatOffsetPriority is selected, the zone farthest from the thermostat set point determines the operating mode. The MasterThermostatPriority choice operates the system according the zone load where the master thermostat is located. The heat pump can also be scheduled to operate in either cooling or heating mode. For scheduled operation, a schedule name is entered in the following field.
+
+\paragraph{Field: Thermostat Priority Schedule Name}\label{field-thermostat-priority-schedule-name}
+
+This alpha field identifies the schedule used when the previous field is set to Scheduled. Schedule values of 0 denote cooling mode while values of 1 denote heating mode. Any other values will force the system off.
+
+\paragraph{Field: Heat Pump Waste Heat Recovery}\label{field-heat-pump-waste-heat-recovery}
+
+This choice field defines the configuration of the heat pump refrigeration system. Valid choices are \textbf{Yes} and \textbf{No}. If Yes is selected, heat recovery is enabled and the heat pump can independently cool and heat different zones. If No is selected, the heat pump is only able to cool or heat for any given time step.
+
+\paragraph{Field: Equivalent Piping Length used for Piping Correction Factor in Cooling Mode}\label{field-equivalent-piping-length-used-for-piping-correction-factor-in-cooling-mode}
+
+This numeric field defines the equivalent pipe length in meters between the farthest terminal unit and the heat pump condenser. This value includes the gas refrigerant line length (for both horizontal and vertical distances), fitting losses, pipe bends, and other connections that contribute to piping losses. This field is used to calculate the piping correction factor in cooling mode. This value defines the head losses due to the pipe length between the farthest terminal unit and the heat pump condenser and impacts the maximum available capacity in cooling mode.
+
+\paragraph{Field: Vertical Height used for Piping Correction Factor}\label{field-vertical-height-used-for-piping-correction-factor}
+
+This numeric field defines the vertical pipe height in meters between the highest or lowest terminal unit and the heat pump condenser. This value defines the gravitational losses due to a change in height between the highest (positive value), or lowest (negative value) terminal unit and the heat pump condenser. The distance specified here is applied to the piping correction factor calculation for both cooling and heating. If the distance between the highest terminal unit above the heat pump condenser is greater than the distance between the lowest terminal unit below the condenser enter the difference between the highest and lowest terminal units as a positive distance, otherwise enter this difference as a negative distance. Example: if the distance from the heat pump condenser to the highest terminal unit above the condenser is 10 m and the distance from the heat pump condenser to the lowest terminal unit below the condenser is -15 m, then enter a value of -5 m in this field. This head loss impacts the maximum available capacity in cooling mode.
+
+\paragraph{Field: Equivalent Piping Length used for Piping Correction Factor in Heating Mode}\label{field-equivalent-piping-length-used-for-piping-correction-factor-in-heating-mode}
+
+This numeric field defines the equivalent pipe length in meters between the farthest terminal unit and the heat pump condenser. This value includes the liquid refrigerant line length (for both horizontal and vertical distances), fitting losses, pipe bends, and other connections that contribute to piping losses. This field is used to calculate the piping correction factor in heating mode. This value defines the head losses due to the pipe length between the farthest terminal unit and the heat pump condenser and impacts the maximum available capacity in heating mode.
+
+\paragraph{Field: Crankcase Heater Power per Compressor}\label{field-crankcase-heater-power-per-compressor}
+
+This numeric field defines the electrical power consumed by the crankcase heater in watts for \emph{each} compressor. This crankcase heater power is consumed when the outdoor temperature is below the maximum outdoor dry-bulb temperature for crankcase heater operation. The minimum value for this field is 0. If this field is left blank, the default value is 33 watts. Crankcase heater electrical consumption is applied only when the compressor is off or is applied during the off cycle when the compressor is cycling below the Minimum Heat Pump Part-Load Ratio. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Number of Compressors}\label{field-number-of-compressors}
+
+This numeric field defines the number of compressors in the heat pump condensing unit and is used exclusively to determine the operating characteristics of the crankcase heater. For example, if the number of compressors is 3, one crankcase heater will operate when the heat pump condensing unit's part-load ratio is less than or equal to 0.67 (when the ratio of compressor size to total compressor capacity input is 0.33) and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. Similarly, two crankcase heaters will operate when the heat pump condensing unit's PLR is less than or equal to 0.33 and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. If the heat pump condensing unit is off, all 3 crankcase heaters will operate if the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. The minimum value for this field is 1. If this field is left blank, the default value is 2. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Ratio of Compressor Size to Total Compressor Capacity}\label{field-ratio-of-compressor-size-to-total-compressor-capacity}
+
+This numeric field defines the size of the first stage compressor to the total compressor capacity and is used exclusively for calculating crankcase heater energy. If this field and the previous field are left blank, the default value is 0.5. If this field is left blank and the previous field is not blank, the compressors are assumed to be equally sized. When the number of compressors is greater than 2, the 2\(^{nd}\) stage compressor and all additional compressors are assumed to be equally sized. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Maximum Outdoor Dry-bulb Temperature for Crankcase Heater}\label{field-maximum-outdoor-dry-bulb-temperature-for-crankcase-heater}
+
+This numeric field defines the maximum outdoor temperature, in degrees Celsius, below which the crankcase heater will operate. If this field is left blank, the default value is 0°C. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Defrost Strategy}\label{field-defrost-strategy-000}
+
+This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse-cycle. Defrost can be disabled by entering a resistive defrost strategy using a timed defrost control, a 0 defrost time period fraction and a 0 resistive defrost heater capacity in the following inputs fields. This method is used when the Maximum Outdoor Dry-Bulb Temperature for Defrost Operation field value is greater than the expected minimum outdoor dry-bulb temperature simulated in the weather file.
+
+\paragraph{Field: Defrost Control}\label{field-defrost-control-000}
+
+This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value of compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field ``Defrost Time Period Fraction'' described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field ``Maximum Outdoor Dry-bulb Temperature for Defrost Operation'' described above. If this input field is left blank, the default defrost control is timed.
+
+\paragraph{Field: Defrost Time Period Fraction}\label{field-defrost-time-period-fraction-000}
+
+This numeric field defines the fraction of compressor runtime when the defrost cycle is active. For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
+
+\paragraph{Field: Resistive Defrost Heater Capacity}\label{field-resistive-defrost-heater-capacity-000}
+
+This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is `resistive' (see input field ``Defrost Strategy'' above). The value for this input field must be greater than or equal to 0 and it is auotsizable. If this input field is left blank, the default is autosize.
+
+\paragraph{Field: Maximum Outdoor Dry-bulb Temperature for Defrost Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-defrost-operation-000}
+
+This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. If this input field is left blank, the default value is 5 C. Defrost can be completely eliminated by selecting a temperature lower than the minimum expected outdoor temperature found in the weather file.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-000}
+
+This choice field defines the configuration of the heat pump condenser. Valid choices are \textbf{AirCooled}, \textbf{EvaporativelyCooled}, and \textbf{WaterCooled}. If WaterCooled is specified, then this unit will be served by an HVACTemplate:Plant:MixedWaterLoop.
+
+\paragraph{Field: Water Condenser Volume Flow Rate}\label{field-water-condenser-volume-flow-rate}
+
+This numeric field defines the condenser water volume flow rate in cubic meters per second. This field is autosizable and only used for water-cooled systems.
+
+\paragraph{Field: Evaporative Condenser Effectiveness}\label{field-evaporative-condenser-effectiveness-000}
+
+The effectiveness of the evaporative condenser, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
+
+\begin{equation}
+Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectiveness} \right)\left( {Tdb,o\,\, - Twb,o} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{cond\\ inlet}\)} = the temperature of the air entering the condenser coil (C)
+
+\emph{T\(_{wb,o}\)} = the wet-bulb temperature of the outdoor air (C)
+
+\emph{T\(_{db,o}\)} = the dry-bulb temperature of the outdoor air (C)
+
+The resulting condenser inlet air temperature is used by the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled and the simulation is calculating heating performance.
+
+If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
+
+If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = EvapCooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
+
+If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = EvapCooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Cooling Capacity and Cooling EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
+
+\paragraph{Field: Evaporative Condenser Air Flow Rate}\label{field-evaporative-condenser-air-flow-rate-000}
+
+The air volume flow rate, in m\(^{3}\) per second, entering the evaporative condenser. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000144 m\(^{3}\)/s per watt of rated total cooling capacity {[}850 cfm/ton{]}). This field is not used when Condenser Type = AirCooled.
+
+\paragraph{Field: Evaporative Condenser Pump Rated Power Consumption}\label{field-evaporative-condenser-pump-rated-power-consumption-000}
+
+The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt {[}15 W/ton{]} of rated total cooling capacity). This field is not used when Condenser Type = AirCooled.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-001}
+
+This numeric field contains the capacity of the heat pump's electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the heat pump compressor(s) is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-001}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the heat pump is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-001}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the heat pump is off.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-001}
+
+This alpha field determines the type of fuel that this variable refrigerant flow system uses. This field has seven choices: Electricity, NaturalGas, PropaneGas, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1, and OtherFuel2. The default is Electricity. The use of alternate fuel types assumes an engine drives the variable speed compression system and also accounts for condenser air flow (i.e., a fan attached to the engine provides air flow through the outdoor condenser.
+
+\paragraph{Field: Minimum Outdoor Temperature in Heat Recovery Mode}\label{field-minimum-outdoor-temperature-in-heat-recovery-mode}
+
+This numeric field defines the minimum outdoor dry-bulb temperature allowed for heat recovery operation. Below this temperature, heat recovery is disabled. This input must be greater than the larger of the minimum outdoor temperature in cooling or heating mode. If this field is left blank, the default value is the higher of the Minimum Outdoor Temperature in Cooling Mode or Minimum Outdoor Temperature in Heating Mode inputs. This system may still operate in cooling or heating only mode when outdoor temperatures are below the minimum outdoor temperature in heat recovery mode. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes.
+
+\paragraph{Field: Maximum Outdoor Temperature in Heat Recovery Mode}\label{field-maximum-outdoor-temperature-in-heat-recovery-mode}
+
+This numeric field defines the maximum outdoor dry-bulb temperature allowed for heat recovery operation. Above this temperature, heat recovery is disabled. This input must be less than the smaller of the maximum outdoor temperature in cooling or heating mode. If this field is left blank, the default value is the lower of the Maximum Outdoor Temperature in Cooling Mode or Maximum Outdoor Temperature in Heating Mode inputs.. This system may still operate in cooling or heating only mode when outdoor temperatures are above the maximum outdoor temperature in heat recovery mode. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes.
+
+Following is an example input for a AirConditioner:VariableRefrigerantFlow system.
+
+\begin{lstlisting}
+
+HVACTemplate:System:VRF,
+  VRF Heat Pump,        !- Name
+  VRFCondAvailSched,    !- Availability Schedule Name
+  autosize,             !- Gross Rated Total Cooling Capacity {W}
+  3.16038,              !- Gross Rated Cooling COP {W}
+  -5,                   !- Minimum Outdoor Temperature in Cooling Mode {C}
+  43,                   !- Maximum Outdoor Temperature in Cooling Mode {C}
+  autosize,             !- Gross Rated Heating Capacity {W}
+  ,                     !- Rated Heating Capacity Sizing Ratio (W/W)
+  3.40909,              !- Gross Rated Heating COP
+  -20,                  !- Minimum Outdoor Temperature in Heating Mode {C}
+  15.5,                 !- Maximum Outdoor Temperature in Heating Mode {C}
+  0.25,                 !- Minimum Heat Pump Part-Load Ratio
+  SPACE1-1,             !- Zone Name for Master Thermostat Location
+  LoadPriority,         !- Master Thermostat Priority Control Type
+  ,                     !- Thermostat Priority Schedule Name
+  No,                   !- Heat Pump Waste Heat Recovery
+  30,  !- Equivalent Piping Length . . . Factor in Cooling Mode {m}
+  10,  !- Vertical Height used for Piping Correction Factor {m}
+  30,  !- Equivalent Piping Length . . . Factor in Heating Mode {m}
+  15,  !- Crankcase Heater Power per Compressor {W}
+  3,   !- Number of Compressors
+  0.33,!- Ratio of Compressor Size to Total Compressor Capacity
+  7,   !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater {C}
+  Resistive,            !- Defrost Strategy
+  Timed,                !- Defrost Control
+  ,                     !- Defrost Time Period Fraction
+  autosize,             !- Resistive Defrost Heater Capacity {W}
+  7,   !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation {C}
+  EvaporativelyCooled,  !- Condenser Type
+  MyVRFOANode,          !- Condenser Inlet Node Name
+  ,                     !- Condenser Outlet Node Name
+  ,                     !- Water Condenser Volume Flow Rate
+  ,             !- Evaporative Condenser Effectiveness {dimensionless}
+  autosize,     !- Evaporative Condenser Air Flow Rate {m3/s}
+  autosize,     !- Evaporative Condenser Pump Rated Power Consumption {W}
+  ,                     !- Supply Water Storage Tank Name
+  200,                  !- Basin Heater Capacity {W/K}
+  ,                     !- Basin Heater Set Point Temperature (C)
+  ,                     !- Basin Heater Operating Schedule Name
+  ,                     !- Fuel Type
+  ,    !- Minimum Outdoor Temperature in Heat Recovery Mode (C)
+  ;    !- Maximum Outdoor Temperature in Heat Recovery Mode (C)
+\end{lstlisting}
+
+\subsection{HVACTemplate:System:Unitary}\label{hvactemplatesystemunitary}
+
+This object simulates the system portion of a constant volume air handler with electric, gas, or hot water heating and optional direct-expansion (DX) cooling. This system may serve one or more HVACTemplate:Zone:Unitary objects. If this system serves more than one zone, only one zone is specified as the control zone. Common names for this sytem type include packaged rooftop systems commonly seen in commercial buildings and split systems (furnace with air conditioner) commonly seen in residential buildings.
+
+\subsubsection{Inputs}\label{inputs-15-005}
+
+\paragraph{Field: Name}\label{field-name-2-019}
+
+Enter a name for the HVACTemplate:System:Unitary object. This name is used in the HVACTemplate:Zone:Unitary object to reference this system.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-7}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. If the ``Supply Fan Operating Mode'' (see below) is set to Cycling, then this is the supply fan operating schedule. If the fan mode is Cycling this is not a schedule of when the system is providing heating, cooling or air flow but a schedule of when it can provide either heating, cooling, or air flow.
+
+\paragraph{Field: Control Zone or Thermostat Location Name}\label{field-control-zone-or-thermostat-location-name}
+
+Enter the name of the HVACTemplate:Zone:Unitary object that contains the thermostat. While multiple HVACTemplate:Zone:Unitary objects can be part of a HVACTemplate:System:Unitary system, only one of the zones contains a thermostat that controls heating and cooling operation. For a single zone system, this field should contain the name of that zone.
+
+\paragraph{Field: Supply Fan Maximum Flow Rate}\label{field-supply-fan-maximum-flow-rate}
+
+Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m3/s.
+
+\paragraph{Field: Supply Fan Operating Mode Schedule Name}\label{field-supply-fan-operating-mode-schedule-name-4}
+
+This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-5}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure-4}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency-5}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Supply Fan Motor in Air Stream Fraction}\label{field-supply-fan-motor-in-air-stream-fraction-1}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-5}
+
+Enter the type of cooling coil. The choices for this field are:
+
+\begin{itemize}
+\item
+  None
+\item
+  SingleSpeedDX
+\end{itemize}
+
+Set this value to ``SingleSpeedDX'' if you want to simulate a system that provides cooling. You may set this value to ``None'' if no cooling is desired. The default value is SingleSpeedDX. Future versions may have additional cooling coil types.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-4}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Design Supply Air Temperature}\label{field-cooling-design-supply-air-temperature}
+
+Enter the cooling supply air temperature in °C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8°C.
+
+\paragraph{Field: Cooling Coil Gross Rated Total Capacity}\label{field-cooling-coil-gross-rated-total-capacity-4}
+
+Enter autosize to let the automatic sizing algorithm determine the cooling coil gross capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for. The units are in W.
+
+\paragraph{Field: Cooling Coil Gross Rated Sensible Heat Ratio}\label{field-cooling-coil-gross-rated-sensible-heat-ratio-4}
+
+Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the gross rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by the gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be ``gross'', i.e., the effect of supply air fan heat is not accounted for.
+
+\paragraph{Field: Cooling Coil Gross Rated COP}\label{field-cooling-coil-gross-rated-cop-2}
+
+Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan.
+
+\paragraph{Field: Heating Coil Type}\label{field-heating-coil-type-2}
+
+Enter the type of heating used in the unitary system. The choices for this field are
+
+\begin{itemize}
+\item
+  Electric
+\item
+  Gas
+\item
+  HotWater
+\end{itemize}
+
+\paragraph{Field: Heating Coil Availability Schedule Name}\label{field-heating-coil-availability-schedule-name-2}
+
+Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of 1.0 indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period
+
+\paragraph{Field: Heating Design Supply Air Temperature}\label{field-heating-design-supply-air-temperature}
+
+Enter the heating supply air temperature in °C to be used for sizing the heating coil and zone supply air flow rates. The default is 50°C.
+
+\paragraph{Field: Heating Coil Capacity}\label{field-heating-coil-capacity-1}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the coil can deliver in Watts.
+
+\paragraph{Field: Gas Heating Coil Efficiency}\label{field-gas-heating-coil-efficiency-1}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default
+
+\paragraph{Field: Gas Heating Coil Parasitic Electric Load}\label{field-gas-heating-coil-parasitic-electric-load-1}
+
+Enter the parasitic electric load associated with the gas heating coil operation, such as a combustion fan. The units are in W.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-000}
+
+Enter autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100\% of the full supply flow may be taken from outdoor air. If a value is entered, it is used instead of the autosize value. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Flow Rate}\label{field-minimum-outdoor-air-flow-rate-000}
+
+Enter autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Schedule Name}\label{field-minimum-outdoor-air-schedule-name-000}
+
+Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 -- 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours.
+
+\paragraph{Field: Economizer Type}\label{field-economizer-type}
+
+The options for this field are
+
+\begin{itemize}
+\item
+  `FixedDryBulb'
+\item
+  `DifferentialDryBulb'
+\item
+  `FixedEnthalpy'
+\item
+  `DifferentialEnthalpy'
+\item
+  `ElectronicEnthalpy' (i.e., humidity ratio curve strategy)
+\item
+  `FixedDewPointAndDryBulb'
+\item
+  `DifferentialDryBulbAndEnthalpy'
+\item
+  `NoEconomizer'
+\end{itemize}
+
+Choosing \textbf{NoEconomizer} means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
+
+Choosing \textbf{FixedDryBulb} means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
+
+Choosing \textbf{DifferentialDryBulb} will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
+
+\textbf{FixedEnthalpy} checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
+
+\textbf{DifferentialEnthalpy} does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
+
+Choosing \textbf{ElectronicEnthalpy} enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
+
+Choosing \textbf{FixedDewPointAndDryBulb} compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
+
+Another option \textbf{DifferentialDryBulbAndEnthalpy} enables the control strategy to be based on both the \textbf{DifferentialDryBulb} and \textbf{DifferentialEnthalpy} economizer control strategies.
+
+In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
+
+The default for this field is \textbf{NoEconomizer}.
+
+\paragraph{Field: Economizer Lockout}\label{field-economizer-lockout-000}
+
+Enter one of the following choices for this field:
+
+\begin{itemize}
+\item
+  NoLockout
+\item
+  LockoutWithHeating
+\item
+  LockoutWithCompressor
+\end{itemize}
+
+The default value is \textbf{NoLockout}. The \textbf{LockoutWithHeating} means that if the packaged unit is in heating mode, the economizer is locked out -- i.e., the economizer dampers are closed and there is minimum outdoor air flow. \textbf{LockoutWithCompressor} means that in addition to locking out the economizer when the unit is in heating mode the economizer is locked out when the DX unit compressor is on. In other words, when the DX coil is off, the economizer must meet the entire cooling load -- it isn't allowed to operate in conjunction with the DX cooling coil. Similarly, when the DX coil is operating, the economizer is not allowed to operate. The \textbf{LockoutWithCompressor} option is sometimes called a ``nonintegrated'' economizer.
+
+\paragraph{Field: Economizer Upper Temperature Limit}\label{field-economizer-upper-temperature-limit}
+
+Enter the outdoor air temperature high limit (\(^{o}\)C) for economizer operation. If the outdoor air temperature is above this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature high limit control.
+
+\paragraph{Field: Economizer Lower Temperature Limit}\label{field-economizer-lower-temperature-limit}
+
+Enter the outdoor air temperature low limit (\(^{o}\)C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
+
+\paragraph{Field: Economizer Upper Enthalpy Limit}\label{field-economizer-upper-enthalpy-limit}
+
+Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
+
+\paragraph{Field: Economizer Maximum Limit Dewpoint Temperature}\label{field-economizer-maximum-limit-dewpoint-temperature-000}
+
+Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type `FixedDewPointAndDryBulb' has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name-5}
+
+Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any supply plenums have been specified, the outlet from the system supply plenum will flow through the supply plenum to the zone terminal unit.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-6}
+
+Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement-4}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{BlowThrough}.
+
+\paragraph{Field: Night Cycle Control}\label{field-night-cycle-control}
+
+Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are \emph{StayOff}, \emph{CycleOnAny}, or \emph{CycleOnControlZone}. \emph{StayOff} means the system will remain off, no matter how hot or cold the zones may be. \emph{CycleOnAny} means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. \emph{CycleOnControlZone} means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. The default is \emph{StayOff}.
+
+\paragraph{Field: Night Cycle Control Zone Name}\label{field-night-cycle-control-zone-name}
+
+For the Night Cycle Control option \emph{CycleOnControlZone} enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
+
+\paragraph{Field: Heat Recovery Type}\label{field-heat-recovery-type-1}
+
+Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
+
+\begin{itemize}
+\item
+  None
+\item
+  Sensible
+\item
+  Enthalpy
+\end{itemize}
+
+The default is \textbf{None}\emph{.}
+
+\paragraph{Field: Sensible Heat Recovery Effectiveness}\label{field-sensible-heat-recovery-effectiveness-1}
+
+Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
+
+\paragraph{Field: Latent Heat Recovery Effectiveness}\label{field-latent-heat-recovery-effectiveness-1}
+
+Enter the latent heat recovery effectiveness if Heat Recovery Type is \emph{Enthalpy}. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-1}
+
+There are three dehumidification control type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  CoolReheatHeatingCoil
+\item
+  CoolReheatDesuperheater
+\end{itemize}
+
+The \emph{CoolReheatHeatingCoil} option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so. Reheat is provided as required by the heating coil. In the simulation, two instances of the heating coil are modeled, one for heating, and one for reheat. The two coil objects represent the same physical coil and never operate simultaneously.
+
+The \emph{CollReheatDesuperheater} option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so. Reheat is provided by a desuperheater coil (see object Coil:Heating:Desuperheater).
+
+The default is \emph{None} which meets the sensible cooling load only. The humidistat is located in the same zone that is specified above as the Control Zone or Thermostat Location Name.
+
+\paragraph{Field: Dehumidification Control Zone Name}\label{field-dehumidification-control-zone-name}
+
+This field is deprecated and will be removed. The humidistat is located in the same zone that is specified above as the Control Zone or Thermostat Location Name.
+
+\paragraph{Field: Dehumidification Setpoint}\label{field-dehumidification-setpoint-1}
+
+This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100). The default is 60\%.
+
+\paragraph{Field: Humidifier Type}\label{field-humidifier-type}
+
+There are two humidifier type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  ElectricSteam
+\end{itemize}
+
+The \emph{ElectricSteam} humidifier option uses the Humidifier:Steam:Electric object. The default is \emph{None.}
+
+\paragraph{Field: Humidifier Availability Schedule Name}\label{field-humidifier-availability-schedule-name}
+
+If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
+
+\paragraph{Field: Humidifier Rated Capacity}\label{field-humidifier-rated-capacity}
+
+Enter the rated moisture output rate in m3/s. The humidifier does not currently autosize, so the default is very large to allow for adequate capacity. The default is 0.000001 m3/s.
+
+\paragraph{Field: Humidifier Rated Electric Power}\label{field-humidifier-rated-electric-power}
+
+Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
+
+\paragraph{Field: Humidifier Control Zone Name}\label{field-humidifier-control-zone-name}
+
+This field specifies the zone name where the humidistat is located for controlling humidification.
+
+\paragraph{Field: Humidifier Setpoint}\label{field-humidifier-setpoint}
+
+This field specifies the zone humidistat setpoint for humidification in percent (0 to 100). The default is 30\%.
+
+\paragraph{Field: Return Fan Delta Pressure}\label{field-return-fan-delta-pressure}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 300 Pa.
+
+\paragraph{Field: Return Fan Motor efficiency}\label{field-return-fan-motor-efficiency}
+
+Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. Default is 0.9.
+
+\paragraph{Field: Return Fan Motor in Air Stream Fraction}\label{field-return-fan-motor-in-air-stream-fraction}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. Default is 1.0.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:System:Unitary,
+  AHU 1,                   !- Air Handling System Name
+  FanAndCoilAvailSched,    !- System Availability Schedule
+  EAST ZONE,               !- Control Zone Name or Thermostat Location
+  autosize,                !- Supply Fan Max Flow Rate {m3/s}
+  Fan Mode Schedule,       !- Supply Fan Operating Mode Schedule
+  .7,                      !- Supply Fan Total Efficiency
+  600,                     !- Supply Fan Delta Pressure {Pa}
+  .9,                      !- Supply Fan Motor Efficiency
+  1,                       !- Supply Fan Motor in Air Stream Fraction
+  SingleSspeedDX,          !- Cooling Coil Type
+  FanAndCoilAvailSched,    !- Cooling Coil Availability Schedule
+  14.0,                    !- Cooling Design Supply Air Temperature {C}
+  autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
+  autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
+  3,                       !- Cooling Coil Gross Rated COP
+  Gas,                     !- Heating Coil Type
+  FanAndCoilAvailSched,    !- Heating Coil Availability Schedule
+  50.0,                    !- Heating Design Supply Air Temperature {C}
+  autosize,                !- Heating Coil Capacity {W}
+  .8,                      !- Gas Heating Coil Efficiency
+  0,                       !- Gas Heating Coil Parasitic Electric Load {W}
+  autosize,                !- Maximum Outdoor air Flow Rate {m3/s}
+  autosize,                !- Minimum Outdoor air Flow Rate {m3/s}
+  ,                        !- Minimum Outdoor air Schedule Name
+  NoEconomizer,            !- Economizer Type
+  NoLockout,               !- Economizer Lockout
+  ,                        !- Economizer Upper Temperature Limit {C}
+  ,                        !- Economizer Lower Temperature Limit {C}
+  ,                        !- Economizer Upper Enthalpy Limit {J/kg}
+  ,                        !- Economizer Maximum Limit Dewpoint Temperature {C}
+  ,                        !- Supply Plenum Name
+  ,                        !- Return Plenum Name
+  BlowThrough,             !- Supply Fan Placement
+  CycleOnAny,              !- Night Cycle Control
+  ,                        !- Night Cycle Control Zone Name
+  None,                    !- Heat Recovery Type
+  ,                        !- Sensible Heat Recovery Effectiveness
+  ,                        !- Latent Heat Recovery Effectiveness
+  None,                    !- Dehumidification Control Type
+  ,                        !- Dehumidification Control Zone Name
+  60,                      !- Dehumidification Setpoint {percent}
+  ElectricSteam,           !- Humidifier Type
+  ,                        !- Humidifier Availability Schedule
+  0.000001,                !- Humidifier Rated Capacity {m3/s}
+  2690,                    !- Humidifier Rated Electric Power {W}
+  EAST ZONE,               !- Humidifier Control Zone Name
+  30,                      !- Humidifier Setpoint {percent}
+  No,                      !- Return Fan
+  0.7,                     !- Return Fan Total Efficiency
+  300,                     !- Return Fan Delta Pressure {Pa}
+  0.9,                     !- Return Fan Motor Efficiency
+  1.0;                     !- Return Fan Motor in Air Stream Fraction
+\end{lstlisting}
+
+\subsection{HVACTemplate:System:UnitaryHeatPump:AirToAir}\label{hvactemplatesystemunitaryheatpumpairtoair}
+
+This object simulates the system portion of a constant volume air handler with a direct-expansion (DX) air-to-air heat pump and supplemental heating (electric, gas, or hot water). This system may serve one or more HVACTemplate:Zone:Unitary objects. If this system serves more than one zone, only one zone is specified as the control zone. Common names for this sytem type include packaged rooftop heat pumps commonly seen in commercial buildings and split system heat pumps commonly seen in residential buildings.
+
+\subsubsection{Inputs}\label{inputs-16-004}
+
+\paragraph{Field: Name}\label{field-name-3-016}
+
+Enter a name for the HVACTemplate:System:UnitaryHeatPump:AirToAir object. This name is used in the HVACTemplate:Zone:Unitary object to reference this system.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-8}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. During times when the system is available, the supply fan operating mode controls fan operation. (See ``Supply Fan Operating Mode Schedule Name'' below)
+
+\paragraph{Field: Control Zone or Thermostat Location Name}\label{field-control-zone-or-thermostat-location-name-1}
+
+Enter the name of the HVACTemplate:Zone:Unitary object that contains the thermostat. While multiple HVACTemplate:Zone:Unitary objects can be part of a HVACTemplate:System:UnitaryHeatPump:AirToAir system, only one of the zones contains a thermostat that controls heating and cooling operation. For a single zone system, this field should contain the name of that zone.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-4}
+
+This field specifies the supply air flow rate when the DX cooling coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are in m3/s. The default is Autosize.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-4}
+
+This field specifies the supply air flow rate when the heating coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are in m3/s. The default is Autosize.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-3}
+
+This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner's supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation). By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will \emph{not} be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is Autosize.
+
+\paragraph{Field: Supply Fan Operating Mode Schedule Name}\label{field-supply-fan-operating-mode-schedule-name-5}
+
+This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement-5}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the dx cooling/heating coil and before the supplemental heating coil. \emph{BlowThrough} models a system where the supply air fan is before the dx cooling/heating coil and the supplemental heating coil. The default is \emph{BlowThrough}.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-6}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure-5}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20 C at sea level, 101325 Pa. The default is 600 Pa.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency-6}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater or equal to the Supply Fan Total Efficiency and less than or equal to 1. The default is 0.9.
+
+\paragraph{Field: Supply Fan Motor in Air Stream Fraction}\label{field-supply-fan-motor-in-air-stream-fraction-2}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-6}
+
+Enter the type of cooling coil. There is currently only one choices for this field,
+
+SingleSpeedDX. Future versions may have additional cooling coil types.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-5}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Design Supply Air Temperature}\label{field-cooling-design-supply-air-temperature-1}
+
+Enter the cooling supply air temperature in °C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8°C.
+
+\paragraph{Field: Cooling Coil Gross Rated Total Capacity}\label{field-cooling-coil-gross-rated-total-capacity-5}
+
+Enter Autosize to let the automatic sizing algorithm determine the cooling coil capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the ``gross'' capacity where the effect of supply air fan heat is not accounted for. The units are in W. The default is Autosize.
+
+\paragraph{Field: Cooling Coil Gross Rated Sensible Heat Ratio}\label{field-cooling-coil-gross-rated-sensible-heat-ratio-5}
+
+Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by the gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be ``gross'' capacity where the effect of supply air fan heat is not accounted for. The default is Autosize.
+
+\paragraph{Field: Cooling Coil Gross Rated COP}\label{field-cooling-coil-gross-rated-cop-3}
+
+Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 3.0.
+
+\paragraph{Field: Heat Pump Heating Coil Type}\label{field-heat-pump-heating-coil-type-3}
+
+Enter the type of heat pump heating coil. There is currently only one choice for this field, SingleSpeedDXHeatPump.
+
+\paragraph{Field: Heating Design Supply Air Temperature}\label{field-heating-design-supply-air-temperature-1}
+
+Enter the heating supply air temperature in °C to be used for sizing the heating coil and zone supply air flow rates. The default is 50°C.
+
+\paragraph{Field: Heat Pump Heating Coil Availability Schedule Name}\label{field-heat-pump-heating-coil-availability-schedule-name-2}
+
+Usually set to blank, which allows the heat pump heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. A schedule value of 1.0 indicates that the heat pump heating coil can be on during a given time period. A value of zero denotes that the heat pump heating coil cannot be used during that time period.
+
+\paragraph{Field: Heat Pump Heating Coil Gross Rated Capacity}\label{field-heat-pump-heating-coil-gross-rated-capacity-3}
+
+Enter Autosize to let the automatic sizing algorithm determine the heat pump heating coil gross capacity based on the maximum heating loads during the heating design day. If a value is entered, it represents the full load gross heating capacity, in watts of the DX heat pump unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. Capacity should be the ``gross'' capacity where the effect of supply air fan heat is not accounted for. The units are in W. The default is Autosize.
+
+\paragraph{Field: Heat Pump Heating Coil Gross Rated COP}\label{field-heat-pump-heating-coil-gross-rated-cop-2}
+
+Enter the coefficient of performance defined as the gross heating coil capacity in watts divided by electrical power input in watts of the DX heating coil unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 2.75.
+
+\paragraph{Field: Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature}\label{field-heat-pump-heating-minimum-outdoor-dry-bulb-temperature-1}
+
+This numeric field defines the minimum outdoor dry-bulb temperature in degrees Celsius for compressor operation. The compressor will not operate (for DX heating or DX cooling) when outdoor dry-bulb temperatures fall below this value. The minimum value must be greater than or equal to -20 °C. The default value is -8°C.
+
+\paragraph{Field: Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature}\label{field-heat-pump-defrost-maximum-outdoor-dry-bulb-temperature-1}
+
+This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 C and less than or equal to 7.22 C. If this input field is left blank, the default value is 5 C.
+
+\paragraph{Field: Heat Pump Defrost Strategy}\label{field-heat-pump-defrost-strategy-1}
+
+This alpha field has two choices: \emph{ReverseCycle} or \emph{Resistive}. If the \emph{ReverseCycle} strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a \emph{Resistive} defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is \emph{ReverseCycle}.
+
+\paragraph{Field: Heat Pump Defrost Control}\label{field-heat-pump-defrost-control-1}
+
+This alpha field has two choices: \emph{Timed} or \emph{OnDemand}. If \emph{Timed} control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For \emph{Timed} defrost control, the fractional amount of time the unit is in defrost is entered in the input field ``Defrost Time Period Fraction'' described below. If \emph{OnDemand} defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field ``Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature'' described above. If this input field is left blank, the default defrost control is \emph{Timed}.
+
+\paragraph{Field: Heat Pump Defrost Time Period Fraction}\label{field-heat-pump-defrost-time-period-fraction-1}
+
+This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to ``timed'' defrost (see Heat Pump Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
+
+\paragraph{Field: Supplemental Heating Coil Type}\label{field-supplemental-heating-coil-type-2}
+
+Enter the type of supplemental heating coil. The choices for this field are
+
+\begin{itemize}
+\item
+  Electric
+\item
+  Gas
+\item
+  HotWater
+\end{itemize}
+
+The default is Electric.
+
+\paragraph{Field: Supplemental Heating Coil Availability Schedule Name}\label{field-supplemental-heating-coil-availability-schedule-name-2}
+
+Usually set to blank, which allows the supplemental heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when supplemental heating is only available seasonally. The schedule values denote whether the supplemental heating coil can run during a given time period. A schedule value of 1.0 indicates that the supplemental heating coil can be on during a given time period. A value of zero denotes that the supplemental heating coil cannot be used during that time period
+
+\paragraph{Field: Supplemental Heating Coil Capacity}\label{field-supplemental-heating-coil-capacity-2}
+
+Enter Autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the supplemental heating coil can deliver in Watts. The default is Autosize.
+
+\paragraph{Field: Supplemental Heating Coil Maximum Outdoor Dry-Bulb Temperature}\label{field-supplemental-heating-coil-maximum-outdoor-dry-bulb-temperature-1}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
+
+\paragraph{Field: Supplemental Gas Heating Coil Efficiency}\label{field-supplemental-gas-heating-coil-efficiency-1}
+
+Enter supplemental heating coil gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default. This field applies only if the supplemental heating coil type is gas.
+
+\paragraph{Field: Supplemental Gas Heating Coil Parasitic Electric Load}\label{field-supplemental-gas-heating-coil-parasitic-electric-load-1}
+
+Enter the parasitic electric load associated with the gas supplemental heating coil operation, such as a combustion fan. The units are in W. The default is 0.0. This field applies only if the supplemental heating coil type is gas.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-1}
+
+Enter Autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100\% of the full supply flow may be taken from outdoor air. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Flow Rate}\label{field-minimum-outdoor-air-flow-rate-1}
+
+Enter Autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Schedule Name}\label{field-minimum-outdoor-air-schedule-name-1}
+
+Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 -- 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate during unoccupied or start up hours.
+
+\paragraph{Field: Economizer Type}\label{field-economizer-type-1}
+
+The options for this field are
+
+\begin{itemize}
+\item
+  `FixedDryBulb'
+\item
+  `DifferentialDryBulb'
+\item
+  `FixedEnthalpy'
+\item
+  `DifferentialEnthalpy'
+\item
+  `ElectronicEnthalpy' (i.e., humidity ratio curve strategy)
+\item
+  `FixedDewPointAndDryBulb'
+\item
+  `DifferentialDryBulbAndEnthalpy'
+\item
+  `NoEconomizer'
+\end{itemize}
+
+Choosing \textbf{NoEconomizer} means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
+
+Choosing \textbf{FixedDryBulb} means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
+
+Choosing \textbf{DifferentialDryBulb} will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
+
+\textbf{FixedEnthalpy} checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
+
+\textbf{DifferentialEnthalpy} does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
+
+Choosing \textbf{ElectronicEnthalpy} enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
+
+Choosing \textbf{FixedDewPointAndDryBulb} compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
+
+Another option \textbf{DifferentialDryBulbAndEnthalpy} enables the control strategy to be based on both the \textbf{DifferentialDryBulb} and \textbf{DifferentialEnthalpy} economizer control strategies.
+
+In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
+
+The default for this field is \textbf{NoEconomizer}
+
+\paragraph{Field: Economizer Lockout}\label{field-economizer-lockout-1-000}
+
+Enter one of the following choices for this field:
+
+\begin{itemize}
+\item
+  NoLockout
+\item
+  LockoutWithHeating
+\item
+  LockoutWithCompressor
+\end{itemize}
+
+The default value is \textbf{NoLockout}. The \textbf{LockoutWithHeating} means that if the packaged unit is in heating mode, the economizer is locked out -- i.e., the economizer dampers are closed and there is minimum outdoor air flow. \textbf{LockoutWithCompressor} means that in addition to locking out the economizer when the unit is in heating mode the economizer is locked out when the DX unit compressor is on. In other words, when the DX coil is off, the economizer must meet the entire cooling load -- it isn't allowed to operate in conjunction with the DX cooling coil. Similarly, when the DX coil is operating, the economizer is not allowed to operate. The \textbf{LockoutWithCompressor} option is sometimes called a ``nonintegrated'' economizer.
+
+\paragraph{Field: Economizer Maximum Limit Dry-Bulb Temperature}\label{field-economizer-maximum-limit-dry-bulb-temperature-000}
+
+Input for this field is the outdoor air temperature high limit (ºC) for economizer operation. If the outdoor air temperature is above this limit, the outdoor airflow rate will be set to the minimum. This field is required if Economizer Control Type `FixedDryBulb' or `FixedDewPointAndDryBulb' has been specified. No input (blank) in this field means that there is no outdoor air temperature high limit control.
+
+\paragraph{Field: Economizer Maximum Limit Enthalpy}\label{field-economizer-maximum-limit-enthalpy-000}
+
+Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
+
+\paragraph{Field: Economizer Maximum Limit Dewpoint Temperature}\label{field-economizer-maximum-limit-dewpoint-temperature-1}
+
+Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type `FixedDewPointAndDryBulb' has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
+
+\paragraph{Field: Economizer Minimum Limit Dry-Bulb Temperature}\label{field-economizer-minimum-limit-dry-bulb-temperature-000}
+
+Enter the outdoor air temperature low limit (C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name-6}
+
+Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any zone supply plenums have been specified, the outlet from the system supply plenum will flow through the zone supply plenum to the zone terminal unit.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-7}
+
+Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
+
+\paragraph{Field: Night Cycle Control}\label{field-night-cycle-control-1}
+
+Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are \emph{StayOff}, \emph{CycleOnAny}, or \emph{CycleOnControlZone}. \emph{StayOff} means the system will remain off, no matter how hot or cold the zones may be. \emph{CycleOnAny} means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. \emph{CycleOnControlZone} means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. The default is \emph{StayOff}.
+
+\paragraph{Field: Night Cycle Control Zone Name}\label{field-night-cycle-control-zone-name-1}
+
+For the Night Cycle Control option \emph{CycleOnControlZone} enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
+
+\paragraph{Field: Heat Recovery Type}\label{field-heat-recovery-type-2}
+
+Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
+
+\begin{itemize}
+\item
+  None
+\item
+  Sensible
+\item
+  Enthalpy
+\end{itemize}
+
+The default is \textbf{None}\emph{.}
+
+\paragraph{Field: Sensible Heat Recovery Effectiveness}\label{field-sensible-heat-recovery-effectiveness-2}
+
+Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
+
+\paragraph{Field: Latent Heat Recovery Effectiveness}\label{field-latent-heat-recovery-effectiveness-2}
+
+Enter the latent heat recovery effectiveness if Heat Recovery Type is \emph{Enthalpy}. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
+
+\paragraph{Field: Humidifier Type}\label{field-humidifier-type-1}
+
+There are two humidifier type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  ElectricSteam
+\end{itemize}
+
+The \emph{ElectricSteam} humidifier option uses the Humidifier:Steam:Electric object. The default is \emph{None.}
+
+\paragraph{Field: Humidifier Availability Schedule Name}\label{field-humidifier-availability-schedule-name-1}
+
+If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
+
+\paragraph{Field: Humidifier Rated Capacity}\label{field-humidifier-rated-capacity-1}
+
+Enter the rated moisture output rate in m3/s. The humidifier does not currently autosize, so the default is very large to allow for adequate capacity. The default is 0.000001 m3/s.
+
+\paragraph{Field: Humidifier Rated Electric Power}\label{field-humidifier-rated-electric-power-1}
+
+Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
+
+\paragraph{Field: Humidifier Control Zone Name}\label{field-humidifier-control-zone-name-1}
+
+This field specifies the zone name where the humidistat is located for controlling humidification.
+
+\paragraph{Field: Humidifier Setpoint}\label{field-humidifier-setpoint-1}
+
+This field specifies the zone humidistat setpoint for humidification in percent (0 to 100). The default is 30\%.
+
+\paragraph{Field: Return Fan Delta Pressure}\label{field-return-fan-delta-pressure-1}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 300 Pa.
+
+\paragraph{Field: Return Fan Motor efficiency}\label{field-return-fan-motor-efficiency-1}
+
+Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. Default is 0.9.
+
+\paragraph{Field: Return Fan Motor in Air Stream Fraction}\label{field-return-fan-motor-in-air-stream-fraction-1}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. Default is 1.0.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:System:UnitaryHeatPump:AirToAir,
+  Heat Pump 1,             !- Name
+  FanAvailSched,           !- System Availability Schedule Name
+  SPACE1-1,                !- Control Zone or Thermostat Location Name
+  autosize,                !- Cooling Supply Air Flow Rate {m3/s}
+  autosize,                !- Heating Supply Air Flow Rate {m3/s}
+  autosize,                !- No Load Supply Air Flow Rate {m3/s}
+  ,                        !- Supply Fan Operating Mode Schedule Name
+  BlowThrough,             !- Supply Fan Placement
+  0.7,                     !- Supply Fan Total Efficiency
+  600,                     !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  1,                       !- Supply Fan Motor in Air Stream Fraction
+  SingleSpeedDX,           !- Cooling Coil Type
+  ,                        !- Cooling Coil Availability Schedule Name
+  14,                      !- Cooling Design Supply Air Temperature {C}
+  autosize,                !- Cooling Coil Gross Rated TotalCapacity {W}
+  autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
+  3,                       !- Cooling Coil Gross Rated COP
+  SingleSpeedDXHeatPump,   !- Heat Pump Heating Coil Type
+  ,                    !- Heat Pump Heating Coil Availability Schedule Name
+  50.0,                    !- Heating Design Supply Air Temperature {C}
+  autosize,            !- Heat Pump Heating Coil Gross Rated Capacity {W}
+  2.75,                    !- Heat Pump Heating Coil Gross Rated COP
+  -8,         !- Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature {C}
+  5,          !- Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature {C}
+  ReverseCycle,            !- Heat Pump Defrost Strategy
+  Timed,                   !- Heat Pump Defrost Control
+  0.058333,                !- Heat Pump Defrost Time Period Fraction
+  Electric,                !- Supplemental Heating Coil Type
+  ,           !- Supplemental Heating Coil Availability Schedule Name
+  autosize,                !- Supplemental Heating Coil Capacity {W}
+  21,    !-  Supplemental Heating Coil Max Outdoor Dry-Bulb Temperature {C}
+  0.8,                     !- Supplemental Gas Heating Coil Efficiency
+  ,           !- Supplemental Gas Heating Coil Parasitic Electric Load {W}
+  autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
+  autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}
+  Min OA Sched,            !- Minimum Outdoor Air Schedule Name
+  DifferentialDryBulb,     !- Economizer Type
+  NoLockout,               !- Economizer Lockout
+  19,                 !- Economizer Maximum Limit Dry-Bulb Temperature {C}
+  ,                        !- Economizer Maximum Limit Enthalpy {J/kg}
+  ,                   !- Economizer Maximum Limit Dewpoint Temperature {C}
+  4,                  !- Economizer Minimum Limit Dry-Bulb Temperature {C}
+  ,                        !- Supply Plenum Name
+  ,                        !- Return Plenum Name
+  CycleOnAny,              !- Night Cycle Control
+  ,                        !- Night Cycle Control Zone Name
+  None,                    !- Heat Recovery Type
+  0.7,                     !- Sensible Heat Recovery Effectiveness
+  0.65,                    !- Latent Heat Recovery Effectiveness
+  None,                    !- Humidifier Type
+  ,                        !- Humidifier Availability Schedule Name
+  0.000001,                !- Humidifier Rated Capacity {m3/s}
+  2690,                    !- Humidifier Rated Electric Power {W}
+  ,                        !- Humidifier Control Zone Name
+  30,                      !- Humidifier Setpoint {percent}
+  No,                      !- Return Fan
+  0.7,                     !- Return Fan Total Efficiency
+  300,                     !- Return Fan Delta Pressure {Pa}
+  0.9,                     !- Return Fan Motor Efficiency
+  1.0;                     !- Return Fan Motor in Air Stream Fraction
+\end{lstlisting}
+
+\subsection{HVACTemplate:System:UnitarySystem}\label{hvactemplatesystemunitarysystem}
+
+This object simulates a unitary system with option cooling coil (air-cooled DX, water-cooled DX, and chilled water), options heating coil (gas, electric, hot water, air-to-air heat pump, and water-to-air heat pump) with cycling or continous fan controls. Often a single HVACTemplate:Zone:Unitary object will be used with a single HVACTemplate:System:UnitarySystem object to simulate single zone system. In addition, multiple HVACTemplate:Zone:Unitary objects may reference the same HVACTemplate:System:UnitarySystem object in a multiple zone version. For a multiple zone system, only one zone is specified as the control zone. The model can simulate chilled water or heat pump systems seen in commercial buildings and split systems commonly seen in residential buildings. HVACTemplate:System:UnitarySystem is similar to HVACTemplate:System:Unitary and HVACTemplate:System:UnitaryHeatPump:AirToAir, but it offers more flexilbility by using the more general AirLoopHVAC:UnitarySystem object instead of the more specific unitary furnace and heat pump objects.
+
+\subsubsection{Inputs}\label{inputs-17-003}
+
+\paragraph{Field: Name}\label{field-name-4-013}
+
+Enter a name for the HVACTemplate:System:UnitarySystem object. This name is used in the HVACTemplate:Zone:Unitary object to reference this system.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-9}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. During times when the system is available, the supply fan operating mode controls fan operation. (See ``Supply Fan Operating Mode Schedule Name'' below)
+
+\paragraph{Field: Control Type}\label{field-control-type-002}
+
+This alpha field contains control type i.e.~load based or setpoint based for the unitary system. Valid choices are \emph{Load} and \emph{SetPoint}. \emph{Load} control requires a Controlling Zone name and \emph{SetPoint} control is an advanced option which requires set points at each coil outlet node. A single set point at the outlet of the system is allowed but not recommended. The user must add the desired setpoint managers to the idf file. The default is \emph{Load}.
+
+\paragraph{Field: Control Zone or Thermostat Location Name}\label{field-control-zone-or-thermostat-location-name-2}
+
+Enter the name of the HVACTemplate:Zone:Unitary object that contains the thermostat. While multiple HVACTemplate:Zone:Unitary objects can be part of a HVACTemplate:System:UnitarySystem system, only one of the zones contains a thermostat that controls heating and cooling operation. For a single zone system, this field should contain the name of that zone.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-5}
+
+This field specifies the supply air flow rate when the cooling coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are in m3/s. The default is Autosize.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-5}
+
+This field specifies the supply air flow rate when the heating coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are in m3/s. The default is Autosize.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-4}
+
+This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner's supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation). By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will \emph{not} be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is Autosize.
+
+\paragraph{Field: Supply Fan Operating Mode Schedule Name}\label{field-supply-fan-operating-mode-schedule-name-6}
+
+This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement-6}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils and before the supplemental heating (or reheat) coil. \emph{BlowThrough} models a system where the supply air fan is before all of the coils. The default is \emph{BlowThrough}.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-7}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure-6}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20 C at sea level, 101325 Pa. The default is 600 Pa.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency-7}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater or equal to the Supply Fan Total Efficiency and less than or equal to 1. The default is 0.9.
+
+\paragraph{Field: Supply Fan Motor in Air Stream Fraction}\label{field-supply-fan-motor-in-air-stream-fraction-3}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-7}
+
+There are seven coil types available:
+
+\begin{itemize}
+\item
+  SingleSpeedDX (the default)
+\item
+  TwoSpeedDX
+\item
+  MultiSpeedDX
+\item
+  TwoStageDX
+\item
+  TwoStageHumidityControlDX
+\item
+  HeatExchangerAssistedDX
+\item
+  SingleSpeedDXWaterCooled
+\item
+  ChilledWater
+\item
+  ChilledWaterDetailedFlatModel
+\item
+  HeatExchangerAssistedChilledWater
+\item
+  None
+\end{itemize}
+
+\emph{SingleSpeedDX} uses the Coil:Cooling:DX:SingleSpeed object.
+
+\emph{TwoSpeedDX} uses the Coil:Cooling:DX:TwoSpeed object.
+
+\emph{MultiSpeedDX} uses the Coil:Cooling:DX:MultiSpeed object.
+
+\emph{TwoStageDX} and \emph{TwoStageHumidityControlDX} use the Coil:Cooling:DX:TwoStageWithHumidityControlMode object.
+
+\emph{HeatExchangerAssistedDX} uses the CoilSystem:Cooling:DX:HeatExchangerAssisted, HeatExchanger:AirToAir:SensibleAndLatent, and Coil:Cooling:DX:SingleSpeed objects.
+
+\emph{SingleSpeedDXWaterCooled} uses the Coil:Cooling:WaterToAirHeatPump:EquationFit object. This option requires an HVACTemplate:Plant:MixedWaterLoop to serve as the water source.
+
+The default type is \emph{SingleSpeedDX}
+
+\emph{ChilledWater} uses the Coil:Cooling:Water object with the DetailedAnalysis option. This is the preferred coil model for most chilled water applications.
+
+\emph{ChilledWaterDetailedFlatModel} uses the Coil:Cooling:Water:DetailedGeometry object. This option is available for special applications.
+
+\emph{HeatExchangerAssistedChilledWater} uses the CoilSystem:Cooling:DX:HeatExchangerAssisted, HeatExchanger:AirToAir:SensibleAndLatent, and Coil:Cooling:Water objects.
+
+\paragraph{Field: Number of Speeds for Cooling}\label{field-number-of-speeds-for-cooling}
+
+This field defines the number of cooling speeds is a multi-speed cooling coil is specifiedl. The default is 1, and the maximum allowed is 10. This field only applies if Cooling Coil Type is MultiSpeedDX.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-6}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Design Supply Air Temperature}\label{field-cooling-design-supply-air-temperature-2}
+
+Enter the cooling supply air temperature in °C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8°C.
+
+\paragraph{Field: DX Cooling Coil Gross Rated Total Capacity}\label{field-dx-cooling-coil-gross-rated-total-capacity}
+
+Enter Autosize to let the automatic sizing algorithm determine the cooling coil gross total cooling capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb. Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is Autosize. This field is only used when the cooling coil type is set to one of the DX options. For two-speed DX coils, the low-speed capacity is assumed to be 0.33 times this value. For two-stage DX coils, the stage 1 capacity is assumed to be 0.5 times this value.
+
+\paragraph{Field: DX Cooling Coil Gross Rated Sensible Heat Ratio}\label{field-dx-cooling-coil-gross-rated-sensible-heat-ratio}
+
+Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the gross rated cooling total capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by gross total cooling capacity of the DX cooling coil at rated conditions. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be ``gross'', i.e., the effect of supply air fan heat is not accounted for. This field is only used when the cooling coil type is set to one of the DX options. The default is Autosize.
+
+For air-cooled DX coils the rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb.
+
+For water-cooled DX coilst the rated conditions are 26.7C (80F) entering air dry-bulb temperature, 19.4C (67F) entering air wet-bulb temperature, and 29.4C (85F) entering water temperature.
+
+For two-speed DX coils, the low-speed SHR is assumed to be equal to this value. For two-stage DX coils, the stage 1 SHR is assumed to be equal to this value. For two-stage DX coil with humidity control, the humidity control mode SHR is assumed to be 0.9 times this value (for both stage 1 and stage 2).
+
+\paragraph{Field: DX Cooling Coil Gross Rated COP}\label{field-dx-cooling-coil-gross-rated-cop}
+
+Enter the coefficient of performance defined as the gross cooling coil total capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The default is 3.0. This field is only used when the cooling coil type is set to one of the DX options. For two-speed DX coils, the low-speed COP is assumed to be 1.5 times this value. For two-stage DX coils, the stage 1 COP is assumed to be this this value. For two-stage DX coil with humidity control, the humidity control mode COP is assumed to be 0.9 times this value (for both stage 1 and stage 2). The gross COP should not account for the supply air fan.
+
+\paragraph{Field: Heating Coil Type}\label{field-heating-coil-type-3}
+
+The heating coil is located in the supply air stream, downstream of the cooling coil. The choices for this field are
+
+\begin{itemize}
+\item
+  Electric
+\item
+  Gas
+\item
+  HotWater
+\item
+  SingleSpeedDXHeatPumpAirSource (air-to-air heat pump)
+\item
+  MultiSpeedDXHeatPumpAirSource (air-to-air heat pump)
+\item
+  SingleSpeedDXHeatPumpWaterSource (water-to-air heat pump). This option requires an HVACTemplate:Plant:MixedWaterLoop to serve as the water source.
+\item
+  MultiStageElectric (uses coil object type Coil:Heating:Electric:MultiStage)
+\item
+  MultiStageGas (uses coil object type Coil:Heating:Gas:MultiStage)
+\item
+  None
+\end{itemize}
+
+The default value is Gas.
+
+\paragraph{Field: Number of Speeds or Stages for Heating}\label{field-number-of-speeds-or-stages-for-heating}
+
+This field defines the number of heating speeds or stages if a multi-speed heatpump or multi-stage heating coil is specifiedl. The default is 1. For heating coil type MultiSpeedDXHeatPumpAirSource, the maximum number of speeds allowed is 10. For heating coil types MultiStageElectric and MultiStageGas, the maximum number of stages allowed is 4. For other heating coil types, this field is ignored.
+
+\paragraph{Field: Heating Coil Availability Schedule Name}\label{field-heating-coil-availability-schedule-name-3}
+
+Usually left blank, which allows the heating coil to be available as needed anytime the system is operating. If a schedule name is specified, it defines when the heating coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period.
+
+\paragraph{Field: Heating Design Supply Air Temperature}\label{field-heating-design-supply-air-temperature-2}
+
+Enter the heating supply air temperature in °C to be used for sizing the heating coil and zone supply air flow rates. The default is 50°C.
+
+\paragraph{Field: Heating Coil Gross Rated Capacity}\label{field-heating-coil-gross-rated-capacity}
+
+Enter Autosize to let the automatic sizing algorithm determine the heating coil gross capacity based on the maximum heating loads during the heating design day. The units are in W. The default is Autosize.
+
+If the Heating Coil Type is Electric or Gas, this field is the rated output of the heating coil not including any effect of the supply air fan.
+
+If the Heating Coil Type is HotWater, this field is the rated output of the heating coil not including any effect of the supply air fan at the following conditions: inlet water temperature is is 82.2 degrees C (180 degrees F), output water temperature is 71.1 degrees C (160 degrees F), inlet air temperature is 16.6 degrees C (60 degrees F), and outlet air temperature is 32.2 degrees C (90 degrees F).
+
+If the Heating Coil Type is SingleSpeedDXHeatPumpAir this field represents the full load gross heating capacity, in watts of the DX heat pump unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. Capacity should be the ``gross'' capacity where the effect of supply air fan heat is not accounted for.
+
+If the Heating Coil Type is SingleSpeedDXHeatPumpWater this field represents the full load heating capacity, in watts of the DX heat pump unit at rated conditions (21.11C (70F) entering air dry-bulb temperature and 21.11C (70F) entering water temperature). Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for.
+
+\paragraph{Field: Gas Heating Coil Efficiency}\label{field-gas-heating-coil-efficiency-2}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default. This field applies only if the heating coil type is gas.
+
+\paragraph{Field: Gas Heating Coil Parasitic Electric Load}\label{field-gas-heating-coil-parasitic-electric-load-2}
+
+Enter the parasitic electric load associated with the gas heating coil operation, such as a combustion fan. The units are in W. This field applies only if the heating coil type is gas.
+
+\paragraph{Field: Heat Pump Heating Coil Gross Rated COP}\label{field-heat-pump-heating-coil-gross-rated-cop-3}
+
+Enter the coefficient of performance defined as the gross heating coil capacity in watts divided by electrical power input in watts of the DX heat pump heating coil unit at rated conditions. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 2.75 which is appropriate for an air-to-air heat pump. This value should be changed for a water-to-air heat pump. The rated conditions are described above under Heating Coil Gross Rated Capacity.
+
+\paragraph{Field: Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature}\label{field-heat-pump-heating-minimum-outdoor-dry-bulb-temperature-2}
+
+This numeric field defines the minimum outdoor dry-bulb temperature in degrees Celsius for compressor operation. The compressor will not operate (for DX heating or DX cooling) when outdoor dry-bulb temperatures fall below this value. The minimum value must be greater than or equal to -20 °C. The default value is -8°C.
+
+\paragraph{Field: Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature}\label{field-heat-pump-defrost-maximum-outdoor-dry-bulb-temperature-2}
+
+This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 C and less than or equal to 7.22 C. If this input field is left blank, the default value is 5 C.
+
+\paragraph{Field: Heat Pump Defrost Strategy}\label{field-heat-pump-defrost-strategy-2}
+
+This alpha field has two choices: \emph{ReverseCycle} or \emph{Resistive}. If the \emph{ReverseCycle} strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a \emph{Resistive} defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is \emph{ReverseCycle}.
+
+\paragraph{Field: Heat Pump Defrost Control}\label{field-heat-pump-defrost-control-2}
+
+This alpha field has two choices: \emph{Timed} or \emph{OnDemand}. If \emph{Timed} control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For \emph{Timed} defrost control, the fractional amount of time the unit is in defrost is entered in the input field ``Defrost Time Period Fraction'' described below. If \emph{OnDemand} defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field ``Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature'' described above. If this input field is left blank, the default defrost control is \emph{Timed}.
+
+\paragraph{Field: Heat Pump Defrost Time Period Fraction}\label{field-heat-pump-defrost-time-period-fraction-2}
+
+This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to ``timed'' defrost (see Heat Pump Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
+
+\paragraph{Field: Supplemental Heating or Reheat Coil Type}\label{field-supplemental-heating-or-reheat-coil-type}
+
+Enter the type of supplemental heating coil or reheat coil. The choices for this field are
+
+\begin{itemize}
+\item
+  Electric
+\item
+  Gas
+\item
+  HotWater
+\item
+  DesuperHeater (applicable only if cooling coil type is air-cooled DX)
+\item
+  None
+\end{itemize}
+
+The default is None.
+
+\paragraph{Field: Supplemental Heating or Reheat Coil Availability Schedule Name}\label{field-supplemental-heating-or-reheat-coil-availability-schedule-name}
+
+Usually set to blank, which allows the supplemental heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when supplemental heating is only available seasonally. The schedule values denote whether the supplemental heating coil can run during a given time period. A schedule value of 1.0 indicates that the supplemental heating coil can be on during a given time period. A value of zero denotes that the supplemental heating coil cannot be used during that time period
+
+\paragraph{Field: Supplemental Heating or Reheat Coil Capacity}\label{field-supplemental-heating-or-reheat-coil-capacity}
+
+Enter Autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the supplemental heating coil can deliver in Watts. The default is Autosize.
+
+\paragraph{Field: Supplemental Heating or Reheat Coil Maximum Outdoor Dry-Bulb Temperature}\label{field-supplemental-heating-or-reheat-coil-maximum-outdoor-dry-bulb-temperature}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
+
+\paragraph{Field: Supplemental Gas Heating Coil Efficiency}\label{field-supplemental-gas-heating-coil-efficiency-2}
+
+Enter supplemental heating coil gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default. This field applies only if the supplemental heating coil type is gas.
+
+\paragraph{Field: Supplemental Gas Heating Coil Parasitic Electric Load}\label{field-supplemental-gas-heating-coil-parasitic-electric-load-2}
+
+Enter the parasitic electric load associated with the gas supplemental heating coil operation, such as a combustion fan. The units are in W. The default is 0.0. This field applies only if the supplemental heating coil type is gas.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-2}
+
+Enter Autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100\% of the full supply flow may be taken from outdoor air. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template. The default is Autosize.
+
+\paragraph{Field: Minimum Outdoor Air Flow Rate}\label{field-minimum-outdoor-air-flow-rate-2}
+
+Enter Autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Schedule Name}\label{field-minimum-outdoor-air-schedule-name-2}
+
+Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 -- 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate during unoccupied or start up hours.
+
+\paragraph{Field: Economizer Type}\label{field-economizer-type-2}
+
+The options for this field are
+
+\begin{itemize}
+\item
+  `FixedDryBulb'
+\item
+  `DifferentialDryBulb'
+\item
+  `FixedEnthalpy'
+\item
+  `DifferentialEnthalpy'
+\item
+  `ElectronicEnthalpy' (i.e., humidity ratio curve strategy)
+\item
+  `FixedDewPointAndDryBulb'
+\item
+  `DifferentialDryBulbAndEnthalpy'
+\item
+  `NoEconomizer'
+\end{itemize}
+
+Choosing \textbf{NoEconomizer} means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
+
+Choosing \textbf{FixedDryBulb} means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
+
+Choosing \textbf{DifferentialDryBulb} will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
+
+\textbf{FixedEnthalpy} checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
+
+\textbf{DifferentialEnthalpy} does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
+
+Choosing \textbf{ElectronicEnthalpy} enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
+
+Choosing \textbf{FixedDewPointAndDryBulb} compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
+
+Another option \textbf{DifferentialDryBulbAndEnthalpy} enables the control strategy to be based on both the \textbf{DifferentialDryBulb} and \textbf{DifferentialEnthalpy} economizer control strategies.
+
+In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
+
+The default for this field is \textbf{NoEconomizer}
+
+\paragraph{Field: Economizer Lockout}\label{field-economizer-lockout-2-000}
+
+Enter one of the following choices for this field:
+
+\begin{itemize}
+\item
+  NoLockout
+\item
+  LockoutWithHeating
+\item
+  LockoutWithCompressor
+\end{itemize}
+
+The default value is \textbf{NoLockout}. The \textbf{LockoutWithHeating} means that if the packaged unit is in heating mode, the economizer is locked out -- i.e., the economizer dampers are closed and there is minimum outdoor air flow. \textbf{LockoutWithCompressor} means that in addition to locking out the economizer when the unit is in heating mode the economizer is locked out when the DX unit compressor is on. In other words, when the DX coil is off, the economizer must meet the entire cooling load -- it isn't allowed to operate in conjunction with the DX cooling coil. Similarly, when the DX coil is operating, the economizer is not allowed to operate. The \textbf{LockoutWithCompressor} option is sometimes called a ``nonintegrated'' economizer.
+
+\paragraph{Field: Economizer Maximum Limit Dry-Bulb Temperature}\label{field-economizer-maximum-limit-dry-bulb-temperature-1}
+
+Input for this field is the outdoor air temperature high limit (ºC) for economizer operation. If the outdoor air temperature is above this limit, the outdoor airflow rate will be set to the minimum. This field is required if Economizer Control Type `FixedDryBulb' or `FixedDewPointAndDryBulb' has been specified. No input (blank) in this field means that there is no outdoor air temperature high limit control.
+
+\paragraph{Field: Economizer Maximum Limit Enthalpy}\label{field-economizer-maximum-limit-enthalpy-1}
+
+Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
+
+\paragraph{Field: Economizer Maximum Limit Dewpoint Temperature}\label{field-economizer-maximum-limit-dewpoint-temperature-2}
+
+Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type `FixedDewPointAndDryBulb' has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
+
+\paragraph{Field: Economizer Minimum Limit Dry-Bulb Temperature}\label{field-economizer-minimum-limit-dry-bulb-temperature-1}
+
+Enter the outdoor air temperature low limit (C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name-7}
+
+Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any zone supply plenums have been specified, the outlet from the system supply plenum will flow through the zone supply plenum to the zone terminal unit.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-8}
+
+Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
+
+\paragraph{Field: Heat Recovery Type}\label{field-heat-recovery-type-3}
+
+Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
+
+\begin{itemize}
+\item
+  None
+\item
+  Sensible
+\item
+  Enthalpy
+\end{itemize}
+
+The default is \textbf{None}\emph{.}
+
+\paragraph{Field: Sensible Heat Recovery Effectiveness}\label{field-sensible-heat-recovery-effectiveness-3}
+
+Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
+
+\paragraph{Field: Latent Heat Recovery Effectiveness}\label{field-latent-heat-recovery-effectiveness-3}
+
+Enter the latent heat recovery effectiveness if Heat Recovery Type is \emph{Enthalpy}. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
+
+\paragraph{Field: Heat Recovery Heat Exchanger Type}\label{field-heat-recovery-heat-exchanger-type}
+
+This alpha field denotes the type of heat exchanger being modeled: Plate (e.g., fixed plate) or Rotary (e.g., rotating cylinder or wheel). The default choice for this field is ``Plate''. The heat exchanger type affects the modeling of frost control options and supply air outlet temperature control. For rotary heat exchangers, rotational speed is varied to control frost formation or the supply air outlet temperature. For plate exchangers, air bypass around the heat exchanger is used to obtain the desired effect.
+
+\paragraph{Field: Heat Recovery Frost Control Type}\label{field-heat-recovery-frost-control-type}
+
+This alpha field has four choices: None, ExhaustAirRecirculation, ExhaustOnly and MinimumExhaustTemperature. If this field is left blank, the default frost control type is ``None''. For modeling preheat frost control, specify ``None'' for this input field and insert a separate heating coil object in the supply inlet air stream to keep the air temperature above the desired frost threshold temperature.
+
+\emph{ExhaustAirRecirculation}: dampers are used to direct exhaust air back into the zone through the supply side of the heat exchanger when the supply (outdoor) air inlet temperature falls below a threshold temperature. The fraction of time that exhaust air is circulated through the supply side of the heat exchanger is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When exhaust air is being recirculated, no supply (outdoor ventilation) air is being provided through the heat exchanger unit (which may or may not be acceptable regarding ventilation for occupants).
+
+\emph{ExhaustOnly (supply air bypass)}: this control cycles off the supply air flow through the heat exchanger for a certain period of time while the exhaust air continues to flow through the exhaust side of the heat exchanger. The fraction of time that the supply flow through the heat exchanger is cycled off is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When implemented in real applications, provisions are usually made to avoid building depressurization when this frost control is operating (automatic or pressure-operated dampers, or a bypass air damper around the supply side of the heat exchanger). For this frost control type, it is assumed that the supply air is bypassed around the heat exchanger during frost control operation (i.e., the total supply flow is not reduced during defrost, but merely bypassed around the heat exchanger).
+
+\emph{MinimumExhaustTemperature}: the temperature of the exhaust air leaving the heat exchanger is monitored and the heat exchanger effectiveness is decreased (by slowing heat exchanger rotation or bypassing supply air around the plate exchanger) to keep the exhaust air from falling below the threshold temperature.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-2}
+
+There are three dehumidification control type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  CoolReheat
+\item
+  Multimode
+\end{itemize}
+
+The \emph{CoolReheat} option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so. Reheat is provided as required by the reheat coil. In the simulation, two instances of the heating coil are modeled, even if the main heating coil acts as the reheat coil in the actual system.
+
+\emph{Multimode} is only applicable for cooling coil type \emph{TwoStageHumidityControlDX}. In this case, the enhanced dehumidification mode is activated as needed, but the system operates to meet the sensible dry-bulb temperature cooling setpoint.
+
+The default is \emph{None} which meets the sensible cooling load only. The humidistat is located in the same zone that is specified above as the Control Zone or Thermostat Location Name.
+
+\paragraph{Field: Dehumidification Control Zone Name}\label{field-dehumidification-control-zone-name-1}
+
+This field specifies the zone name where the humidistat is located for controlling dehumidification.
+
+\paragraph{Field: Dehumidification Relative Humidity Setpoint}\label{field-dehumidification-relative-humidity-setpoint}
+
+This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100). The default is 60\%. This field is ignored if a Dehumidification Relative Humidity Setpoint Schedule Name is specified.
+
+\paragraph{Field: Dehumidification Relative Humidity Setpoint Schedule Name}\label{field-dehumidification-relative-humidity-setpoint-schedule-name}
+
+Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint, The values in the schedule are in percent (0 to 100).
+
+\paragraph{Field: Humidifier Type}\label{field-humidifier-type-2}
+
+There are two humidifier type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  ElectricSteam
+\end{itemize}
+
+The \emph{ElectricSteam} humidifier option uses the Humidifier:Steam:Electric object. The default is \emph{None.}
+
+\paragraph{Field: Humidifier Availability Schedule Name}\label{field-humidifier-availability-schedule-name-2}
+
+If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
+
+\paragraph{Field: Humidifier Rated Capacity}\label{field-humidifier-rated-capacity-2}
+
+Enter the rated moisture output rate in m3/s. The humidifier does not currently autosize, so the default is very large to allow for adequate capacity. The default is 0.000001 m3/s.
+
+\paragraph{Field: Humidifier Rated Electric Power}\label{field-humidifier-rated-electric-power-2}
+
+Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
+
+\paragraph{Field: Humidifier Control Zone Name}\label{field-humidifier-control-zone-name-2}
+
+This field specifies the zone name where the humidistat is located for controlling humidification.
+
+\paragraph{Field: Humidifier Relative Humidity Setpoint}\label{field-humidifier-relative-humidity-setpoint}
+
+This field specifies the zone humidistat setpoint for humidification in percent (0 to 100). The default is 30\%. This field is ignored if a Humidifier Relative Humidity Setpoint Schedule Name is specified.
+
+\paragraph{Field: Humidifier Relative Humidity Setpoint Schedule Name}\label{field-humidifier-relative-humidity-setpoint-schedule-name}
+
+Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint, The values in the schedule are in percent (0 to 100).
+
+\paragraph{Field: Sizing Option}\label{field-sizing-option-000}
+
+This field specifies the sizing method for the system supply air flow rate. \emph{Coincident} sizes on the sum of the coincident zone supply air flow rates. \emph{NonCoincident} sizes on sum of the noncoincident zone design supply air flow rates. The default is \emph{NonCoincident}.
+
+\paragraph{Field: Return Fan}\label{field-return-fan}
+
+Enter \emph{Yes} if the system has a return fan. The default is \emph{No}.
+
+\paragraph{Field: Return Fan Total Efficiency}\label{field-return-fan-total-efficiency}
+
+Enter the total efficiency of the return fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1. Default is 0.7.
+
+\paragraph{Field: Return Fan Delta Pressure}\label{field-return-fan-delta-pressure-2}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 300 Pa.
+
+\paragraph{Field: Return Fan Motor efficiency}\label{field-return-fan-motor-efficiency-2}
+
+Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. Default is 0.9.
+
+\paragraph{Field: Return Fan Motor in Air Stream Fraction}\label{field-return-fan-motor-in-air-stream-fraction-2}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. Default is 1.0.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:System:UnitarySystem,
+  AHU 1,                   !- Name
+  FanAvailSched,           !- System Availability Schedule Name
+  Load,                    !- Control Type
+  SPACE1-1,                !- Control Zone or Thermostat Location Name
+  autosize,                !- Cooling Supply Air Flow Rate {m3/s}
+  autosize,                !- Heating Supply Air Flow Rate {m3/s}
+  autosize,                !- No Load Supply Air Flow Rate {m3/s}
+  FanModeSchedule,         !- Supply Fan Operating Mode Schedule Name
+  BlowThrough,             !- Supply Fan Placement
+  0.7,                     !- Supply Fan Total Efficiency
+  600,                     !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  1,                       !- Supply Fan Motor in Air Stream Fraction
+  SingleSpeedDX,           !- Cooling Coil Type
+  1,                       !- Number of Speeds for Cooling
+  ,                        !- Cooling Coil Availability Schedule Name
+  12.8,                    !- Cooling Design Supply Air Temperature {C}
+  autosize,                !- DX Cooling Coil Gross Rated Total Capacity{W}
+  autosize,            !- DX Cooling Coil Gross Rated Sensible Heat Ratio
+  3,                       !- DX Cooling Coil Gross Rated COP
+  Gas,                     !- Heating Coil Type
+  1,                       !- Number of Speeds for Heating
+  ,                        !- Heating Coil Availability Schedule Name
+  50.0,                    !- Heating Design Supply Air Temperature {C}
+  autosize,                !- Heating Coil Gross Rated Capacity{W}
+  .8,                      !- Gas Heating Coil Efficiency
+  0,                       !- Gas Heating Coil Parasitic Electric Load {W}
+  2.75,                    !- Heat Pump Heating Coil Gross Rated COP
+  -8,         !- Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature {C}
+  5,          !- Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature {C}
+  ReverseCycle,            !- Heat Pump Defrost Strategy
+  Timed,                   !- Heat Pump Defrost Control
+  0.058333,                !- Heat Pump Defrost Time Period Fraction
+  Electric,                !- Supplemental Heating or Reheat Coil Type
+  ,     !- Supplemental Heating  or ReheatCoil Availability Schedule Name
+  autosize,         !- Supplemental Heating or Reheat Coil Capacity {W}
+  21,   !-  Supplemental Heating or Reheat Coil Max . . . Temperature {C}
+  0.8,  !- Supplemental Gas Heating or Reheat Coil Efficiency
+  ,     !- Supplemental Gas Heating or Reheat Coil Parasitic . . . Load {W}
+  autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
+  autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}
+  Min OA Sched,            !- Minimum Outdoor Air Schedule Name
+  DifferentialDryBulb,     !- Economizer Type
+  NoLockout,               !- Economizer Lockout
+  19,                 !- Economizer Maximum Limit Dry-Bulb Temperature {C}
+  ,                   !- Economizer Maximum Limit Enthalpy {J/kg}
+  ,                   !- Economizer Maximum Limit Dewpoint Temperature {C}
+  4,                  !- Economizer Minimum Limit Dry-Bulb Temperature {C}
+  ,                        !- Supply Plenum Name
+  ,                        !- Return Plenum Name
+  None,                    !- Heat Recovery Type
+  0.7,                     !- Sensible Heat Recovery Effectiveness
+  0.65,                    !- Latent Heat Recovery Effectiveness
+  ,                        !- Heat Recovery Heat Exchanger Type
+  ,                        !- Heat Recovery Frost Control Type
+  None,                    !- Dehumidification Control Type
+  ,                        !- Dehumidification Control Zone Name
+  60.0,       !- Dehumidification Relative Humidity Setpoint {percent}
+  ,           !- Dehumidification Relative Humidity Setpoint Schedule Name
+  None,                    !- Humidifier Type
+  ,                        !- Humidifier Availability Schedule Name
+  0.000001,                !- Humidifier Rated Capacity {m3/s}
+  2690.0,                  !- Humidifier Rated Electric Power {W}
+  ,                        !- Humidifier Control Zone Name
+  30.0,       !- Humidifier Relative Humidity Setpoint {percent}
+  ,           !- Humidifier Relative Humidity Setpoint Schedule Name
+  No,                      !- Return Fan
+  0.7,                     !- Return Fan Total Efficiency
+  300,                     !- Return Fan Delta Pressure {Pa}
+  0.9,                     !- Return Fan Motor Efficiency
+  1.0;                     !- Return Fan Motor in Air Stream Fraction
+\end{lstlisting}
+
+\subsection{HVACTemplate:System:VAV}\label{hvactemplatesystemvav}
+
+This object simulates the system portion of a variable air volume HVAC configuration with chilled water cooling and several different heating options. Multiple HVACTemplate:Zone:VAV objects are usually specified for each HVACTemplate:System:VAV object.
+
+\subsubsection{Inputs}\label{inputs-18-002}
+
+\paragraph{Field: Name}\label{field-name-5-010}
+
+Enter a name for the HVACTemplate:System:VAV object. This name is used in the HVACTemplate:Zone:VAV object to reference this system.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-10}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. Please note that for this system type, this is a schedule of when the system is providing air flow.
+
+\paragraph{Field: Supply Fan Maximum Flow Rate}\label{field-supply-fan-maximum-flow-rate-1}
+
+Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m\(^{3}\)/s.
+
+\paragraph{Field: Supply Fan Minimum Flow Rate}\label{field-supply-fan-minimum-flow-rate}
+
+Enter the minimum supply air volume that may be provided. This field may be set to autosize. The units are in m\(^{3}\)/s.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-8}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure-7}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 1000 Pa.
+
+\paragraph{Field: Supply Fan Motor efficiency}\label{field-supply-fan-motor-efficiency-8}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Supply Fan Motor in Air Stream Fraction}\label{field-supply-fan-motor-in-air-stream-fraction-4}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-8}
+
+There are two coil types available:
+
+\begin{itemize}
+\item
+  ChilledWater
+\item
+  ChilledWaterDetailedFlatModel
+\end{itemize}
+
+\emph{ChilledWater} uses the COIL:Cooling:Water object with the DetailedAnalysis option. This is the preferred coil model for most applications. \emph{ChilledWaterDetailedFlatModel} uses the Coil:Cooling:Water:DetailedGeometry object. This option is available for special applications. The default is \emph{ChilledWater}.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-7}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of one indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Coil Setpoint Schedule Name}\label{field-cooling-coil-setpoint-schedule-name}
+
+If a constant setpoint for the cooling coil is to be specified, leave this field blank, and the Cooling Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the cooling coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the cooling coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Cooling Coil Setpoint Reset Type is something other than None (see below).
+
+\paragraph{Field: Cooling Coil Design Setpoint}\label{field-cooling-coil-design-setpoint-1}
+
+Enter the cooling supply air temperature in C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8C. If no Cooling Coil Setpoint Schedule or Cooling Coil Setpoint Reset Type is specified, this value is used as a constant cooling supply air setpoint temperature.
+
+\paragraph{Field: Heating Coil Type}\label{field-heating-coil-type-4}
+
+The heating coil is located in the supply air stream, upstream of the cooling coil and after the outdoor air mixing box. If no central heating coil is used in the VAV system, then the option ``none'' should be specified here. Otherwise this indicates the type of heating coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\item
+  None
+\end{itemize}
+
+The default value is None. Note that the configuration of HVACTemplate:System:VAV assumes that there will be reheat coils or baseboard heating to provide heating control at the zone level. If a heating coil is specified, the heating and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
+
+\paragraph{Field: Heating Coil Availability Schedule Name}\label{field-heating-coil-availability-schedule-name-4}
+
+Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period
+
+\paragraph{Field: Heating Coil Setpoint Schedule Name}\label{field-heating-coil-setpoint-schedule-name}
+
+If a constant setpoint for the heating coil is to be specified, leave this field blank, and the Heating Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the heating coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the heating coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Heating Coil Setpoint Reset Type is something other than None (see below).
+
+\paragraph{Field: Heating Coil Design Setpoint}\label{field-heating-coil-design-setpoint-1}
+
+Enter the heating supply air temperature in C to be used for sizing the heating coil and zone supply air flow rates. If no Heating Coil Setpoint Schedule or Heating Coil Setpoint Reset Type is specified, this value is used as a constant heating supply air setpoint temperature. The default is 10.0C.
+
+\paragraph{Field: Gas Heating Coil Efficiency}\label{field-gas-heating-coil-efficiency-3}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default
+
+\paragraph{Field: Gas Heating Coil Parasitic Electric Load}\label{field-gas-heating-coil-parasitic-electric-load-3}
+
+Enter the parasitic electric load associated with the gas heating operation, such as a combustion fan. The units are in W.
+
+\paragraph{Field: Preheat Coil Type}\label{field-preheat-coil-type}
+
+The preheat coil is located in the outdoor air stream, upstream of the outdoor air mixing box and tempers the outdoor air. If no preheat coil is used in the VAV system, then the option ``none'' should be specified here. Otherwise this indicates the type of preheat coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\item
+  None
+\end{itemize}
+
+The default value is None. If a preheat coil is specified, the preheat and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
+
+\paragraph{Field: Preheat Coil Availability Schedule Name}\label{field-preheat-coil-availability-schedule-name}
+
+Usually set to blank, which allows the preheat coil to be available anytime the system is operating. If a schedule name is specified, it defines when the preheat coil is available. This is most often used when preheat is only available seasonally. The schedule values denote whether the preheat coil can run during a given time period. A schedule value of 1.0 indicates that the preheat coil can be on during a given time period. A value of zero denotes that the preheat coil cannot be used during that time period
+
+\paragraph{Field: Preheat Coil Setpoint Schedule Name}\label{field-preheat-coil-setpoint-schedule-name}
+
+If a constant setpoint for the preheat coil is to be specified, leave this field blank, and the Preheat Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the preheat coil specify the schedule name here. The schedule should control the leaving air temperature from the preheat coil. The values in the schedule are in degrees C.
+
+\paragraph{Field: Preheat Coil Design Setpoint}\label{field-preheat-coil-design-setpoint}
+
+Enter the preheat supply air temperature in C to be used for sizing the preheat coil. If no Preheat Coil Setpoint Schedule is specified, this value is used as a constant preheat supply air setpoint temperature. The default is 7.2C.
+
+\paragraph{Field: Gas Preheat Coil Efficiency}\label{field-gas-preheat-coil-efficiency}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default
+
+\paragraph{Field: Gas Preheat Coil Parasitic Electric Load}\label{field-gas-preheat-coil-parasitic-electric-load}
+
+Enter the parasitic electric load associated with the gas heating operation, such as an combustion fan. The units are in W.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-3}
+
+Enter autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100\% of the full supply flow may be taken from outdoor air. If a value is entered, it is used instead of the autosize value. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Flow Rate}\label{field-minimum-outdoor-air-flow-rate-3}
+
+Enter autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Control Type}\label{field-minimum-outdoor-air-control-type}
+
+Choices for this field are \textbf{FixedMinimum} or \textbf{ProportionalMinimum}. FixedMinimum means that the minimum outdoor air flow rate is fixed no matter what the actual system flow rate is. ProportionalMinimum means the minimum outdoor air flow rate varies in proportion to the total system air flow rate. The default is ProportionalMinimum.
+
+\paragraph{Field: Minimum Outdoor Air Schedule Name Name}\label{field-minimum-outdoor-air-schedule-name-name}
+
+Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 -- 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours.
+
+\paragraph{Field: Economizer Type}\label{field-economizer-type-3}
+
+The options for this field are
+
+\begin{itemize}
+\item
+  `FixedDryBulb'
+\item
+  `DifferentialDryBulb'
+\item
+  `FixedEnthalpy'
+\item
+  `DifferentialEnthalpy'
+\item
+  `ElectronicEnthalpy' (i.e., humidity ratio curve strategy)
+\item
+  `FixedDewPointAndDryBulb'
+\item
+  `DifferentialDryBulbAndEnthalpy'
+\item
+  `NoEconomizer'
+\end{itemize}
+
+Choosing \textbf{NoEconomizer} means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
+
+Choosing \textbf{FixedDryBulb} means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
+
+Choosing \textbf{DifferentialDryBulb} will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
+
+\textbf{FixedEnthalpy} checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
+
+\textbf{DifferentialEnthalpy} does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
+
+Choosing \textbf{ElectronicEnthalpy} enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
+
+Choosing \textbf{FixedDewPointAndDryBulb} compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
+
+Another option \textbf{DifferentialDryBulbAndEnthalpy} enables the control strategy to be based on both the \textbf{DifferentialDryBulb} and \textbf{DifferentialEnthalpy} economizer control strategies.
+
+In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
+
+The default for this field is \textbf{NoEconomizer}.
+
+\paragraph{Field: Economizer Lockout}\label{field-economizer-lockout-3}
+
+The only choice for this field is
+
+\begin{itemize}
+\tightlist
+\item
+  NoLockout
+\end{itemize}
+
+The default value is NoLockout. Future versions may have additional options.
+
+\paragraph{Field: Economizer Upper Temperature Limit}\label{field-economizer-upper-temperature-limit-1}
+
+Enter the outdoor air temperature high limit (\(^{o}\)C) for economizer operation. If the outdoor air temperature is above this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature high limit control.
+
+\paragraph{Field: Economizer Lower Temperature Limit}\label{field-economizer-lower-temperature-limit-1}
+
+Enter the outdoor air temperature low limit (\(^{o}\)C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
+
+\paragraph{Field: Economizer Upper Enthalpy Limit}\label{field-economizer-upper-enthalpy-limit-1}
+
+Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
+
+\paragraph{Field: Economizer Maximum Limit Dewpoint Temperature}\label{field-economizer-maximum-limit-dewpoint-temperature-3}
+
+Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type `FixedDewPointAndDryBulb' has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name-8}
+
+Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any supply plenums have been specified, the outlet from the system supply plenum will flow through the supply plenum to the zone terminal unit.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-9}
+
+Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement-7}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{Draw Through}.
+
+\paragraph{Field: Supply Fan Part-Load Power Coefficients}\label{field-supply-fan-part-load-power-coefficients}
+
+Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
+
+\begin{itemize}
+\item
+  InletVaneDampers
+\item
+  OutletDampers
+\item
+  VariableSpeedMotor
+\item
+  ASHRAE90.1-2004Appendix G
+\item
+  VariableSpeedMotorPressureReset
+\end{itemize}
+
+The default is \emph{InletVaneDampers}. The resulting power curves are shown in Figure~\ref{fig:vav-supply-fan-part-load-power-coefficient}. VAV Supply Fan Part-Load Power Coefficient Options below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The \emph{VariableSpeedMotorPressureReset} option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources': \emph{Design Guidelines: Advanced Variable Air Volume (VAV) Systems} (EDR\_DesignGuidelines\_VAV.pdf).
+
+\begin{figure}[hbtp] % fig 158
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image611.png}
+\caption{VAV Supply Fan Part-Load Power Coefficient Options \protect \label{fig:vav-supply-fan-part-load-power-coefficient}}
+\end{figure}
+
+\paragraph{Field: Night Cycle Control}\label{field-night-cycle-control-2}
+
+Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are \emph{StayOff}, \emph{CycleOnAny}, \emph{CycleOnControl Zone or CycleOnAnyZoneFansOnly}. \emph{StayOff} means the system will remain off, no matter how hot or cold the zones may be. \emph{CycleOnAny} means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. \emph{CycleOnControlZone} means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. \emph{CycleOnAnyZoneFansOnly} is the same as \emph{CycleOnAny} except that only the zone fans are cycled on and the central air handler fan is left off (applicable only if using HVACTemplate:Zone:VAV:FanPowered in one or more zones). The default is \emph{StayOff}.
+
+\paragraph{Field: Night Cycle Control Zone Name}\label{field-night-cycle-control-zone-name-2}
+
+For the Night Cycle Control option \emph{Cycle On Control Zone} enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
+
+\paragraph{Field: Heat Recovery Type}\label{field-heat-recovery-type-4}
+
+Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
+
+\begin{itemize}
+\item
+  None
+\item
+  Sensible
+\item
+  Enthalpy
+\end{itemize}
+
+The default is \textbf{None}\emph{.}
+
+\paragraph{Field: Sensible Heat Recovery Effectiveness}\label{field-sensible-heat-recovery-effectiveness-4}
+
+Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
+
+\paragraph{Field: Latent Heat Recovery Effectiveness}\label{field-latent-heat-recovery-effectiveness-4}
+
+Enter the latent heat recovery effectiveness if Heat Recovery Type is \emph{Enthalpy}. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
+
+\paragraph{Field: Cooling Coil Setpoint Reset Type}\label{field-cooling-coil-setpoint-reset-type}
+
+Select the type of automatic reset control for the cooling supply air temperature. The choices are:
+
+\begin{itemize}
+\item
+  None -- no reset, use the Cooling Coil Setpoint Schedule or Cooling Coil Design Setpoint.
+\item
+  Warmest -- reset the cooling supply air temperature to the highest supply air temperature that will meet the cooling requirements of all the zones at the maximum supply air flow rate. The minimum setpoint allowed is the Cooling Coil Design Setpoint. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:Warmest)
+\item
+  OutdoorAirTemperatureReset -- reset the cooling supply air temperature based on the following default rules. When the outdoor dry-bulb temperature (ODB) is at or below 15.6C the setpoint is the Cooling Coil Design Setpoint plus 5.2C. When the ODB is at or above 26.7C the setpoint is the Cooling Coil Design Setpoint. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset)
+\item
+  WarmestTemperatureFirst -- find the highest setpoint temperature that will satisfy all the zone cooling loads at minimum supply air flow rate. If this setpoint temperature is less than the Cooling Coil Design Setpoint, the setpoint temperature is set to the minimum, and the supply air flow rate is increased to meet the loads. This option is appropriate when modeling a single-zone VAV system. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:WarmestTemperatureFlow)
+\end{itemize}
+
+The default is \emph{None}.
+
+\paragraph{Field: Heating Coil Setpoint Reset Type}\label{field-heating-coil-setpoint-reset-type}
+
+Select the type of automatic reset control for the central heating supply air temperature. The choices are:
+
+\begin{itemize}
+\item
+  None -- no reset, use the Heating Coil Setpoint Schedule or Heating Coil Design Setpoint.
+\item
+  OutdoorAirTemperatureReset -- reset the heating supply air temperature based on the following default rules. When the outdoor dry-bulb temperature (ODB) is at or below --6.7C the setpoint is the Heating Coil Design Setpoint. When the ODB is at or above 10.0C the setpoint is the Heating Coil Design Setpoint minus 5.2C. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset).
+\end{itemize}
+
+The default is \emph{None}.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-3}
+
+There are two dehumidification control type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  CoolReheat
+\end{itemize}
+
+The \emph{CoolReheat} option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so. Reheat is provided as required by the terminal unit reheat coils if available.
+
+The default is \emph{None} which meets the sensible cooling setpoint only.
+
+\paragraph{Field: Dehumidification Control Zone Name}\label{field-dehumidification-control-zone-name-2}
+
+This field specifies the zone name where the humidistat is located for controlling dehumidification.
+
+\paragraph{Field: Dehumidification Setpoint}\label{field-dehumidification-setpoint-2}
+
+This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100). The default is 60\%.
+
+\paragraph{Field: Humidifier Type}\label{field-humidifier-type-3}
+
+There are two humidifier type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  ElectricSteam
+\end{itemize}
+
+The \emph{ElectricSteam} humidifier option uses the Humidifier:Steam:Electric object. The default is \emph{None.}
+
+\paragraph{Field: Humidifier Availability Schedule Name}\label{field-humidifier-availability-schedule-name-3}
+
+If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
+
+\paragraph{Field: Humidifier Rated Capacity}\label{field-humidifier-rated-capacity-3}
+
+Enter the rated moisture output rate in m3/s. The humidifier does not currently autosize, so the default is very large to allow for adequate capacity. The default is 0.000001 m3/s.
+
+\paragraph{Field: Humidifier Rated Electric Power}\label{field-humidifier-rated-electric-power-3}
+
+Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
+
+\paragraph{Field: Humidifier Control Zone Name}\label{field-humidifier-control-zone-name-3}
+
+This field specifies the zone name where the humidistat is located for controlling humidification.
+
+\paragraph{Field: Humidifier Setpoint}\label{field-humidifier-setpoint-2}
+
+This field specifies the zone humidistat setpoint for humidification in percent (0 to 100). The default is 30\%.
+
+\paragraph{Field: Sizing Option}\label{field-sizing-option-1}
+
+This field specifies the sizing method for the system supply air flow rate. \emph{Coincident} sizes on the sum of the coincident zone supply air flow rates. \emph{NonCoincident} sizes on sum of the noncoincident zone design supply air flow rates. The default is \emph{NonCoincident}.
+
+\paragraph{Field: Return Fan}\label{field-return-fan-1}
+
+Enter \emph{Yes} if the system has a return fan. The default is \emph{No}.
+
+\paragraph{Field: Return Fan Total Efficiency}\label{field-return-fan-total-efficiency-1}
+
+Enter the total efficiency of the return fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Return Fan Delta Pressure}\label{field-return-fan-delta-pressure-3}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 500 Pa.
+
+\paragraph{Field: Return Fan Motor efficiency}\label{field-return-fan-motor-efficiency-3}
+
+Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Return Fan Motor in Air Stream Fraction}\label{field-return-fan-motor-in-air-stream-fraction-3}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Return Fan Part-Load Power Coefficients}\label{field-return-fan-part-load-power-coefficients}
+
+Select the set of generic pre-defined coefficients to use for the return fan part-load power consumption. This alpha field has the following choices:
+
+\begin{itemize}
+\item
+  InletVaneDampers
+\item
+  OutletDampers
+\item
+  VariableSpeedMotor
+\item
+  ASHRAE90.1-2004Appendix G
+\item
+  VariableSpeedMotorPressureReset
+\end{itemize}
+
+The default is \emph{InletVaneDampers}. The resulting power curves are shown in Figure~\ref{fig:vav-supply-fan-part-load-power-coefficient}. VAV Supply Fan Part-Load Power Coefficient Options (see Supply Fan Part-Load Power Coefficients above). The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The \emph{VariableSpeedMotorPressureReset} option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources': \emph{Design Guidelines: Advanced Variable Air Volume (VAV) Systems} (EDR\_DesignGuidelines\_VAV.pdf).
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:System:VAV,
+  VAV Sys 1,               !-Name
+  FanAvailSched,           !- System Availability Schedule Name
+  autosize,                !- Supply Fan Maximum Flow Rate {m3/s}
+  autosize,                !- Supply Fan Minimum Flow Rate {m3/s}
+  0.7,                     !- Supply Fan Total Efficiency
+  600,                     !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  1,                       !- Supply Fan Motor in Air Stream Fraction
+  ChilledWater,            !- Cooling Coil Type
+  ,                        !- Cooling Coil Availability Schedule Name
+  ,                        !- Cooling Coil Setpoint Schedule Name
+  12.8,                    !- Cooling Coil Design Setpoint {C}
+  HotWater,                !- Heating Coil Type
+  ,                        !- Heating Coil Availability Schedule Name
+  ,                        !- Heating Coil Setpoint Schedule Name
+  10.0,                    !- Heating Coil Design Setpoint {C}
+  0.8,                     !- Gas Heating Coil Efficiency
+  0.0,                     !- Gas Heating Coil Parasitic Electric Load {W}
+  None,                    !- Preheat Coil Type
+  ,                        !- Preheat Coil Availability Schedule Name
+  ,                        !- Preheat Coil Setpoint Schedule Name
+  ,                        !- Preheat Coil Design Setpoint {C}
+  0.8,                     !- Gas Preheat Coil Efficiency
+  0.0,                     !- Gas Preheat Coil Parasitic Electric Load {W}
+  autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
+  autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}
+  FixedMinimum,            !- Minimum Outdoor Air Control Type
+  Min OA Sched,            !- Minimum Outdoor Air Schedule Name
+  DifferentialDryBulb,     !- Economizer Type
+  NoLockout,               !- Economizer Lockout
+  19,                      !- Economizer Upper Temperature Limit {C}
+  4,                       !- Economizer Lower Temperature Limit {C}
+  ,                        !- Economizer Upper Enthalpy Limit {J/kg}
+  ,                    !- Economizer Maximum Limit Dewpoint Temperature {C}
+  ,                        !- Supply Plenum Name
+  PLENUM-1,                !- Return Plenum Name
+  DrawThrough,             !- Supply Fan Placement
+  InletVaneDampers,        !- Supply Fan Part-Load Power Coefficients
+  CycleOnAnyZoneFansOnly,  !- Night Cycle Control
+  ,                        !- Night Cycle Control Zone Name
+  None,                    !- Heat Recovery Type
+  0.70,                    !- Sensible Heat Recovery Effectiveness
+  0.65,                    !- Latent Heat Recovery Effectiveness
+  None,                    !- Cooling Coil Setpoint Reset Type
+  None,                    !- Heating Coil Setpoint Reset Type
+  None,                    !- Dehumidification Control Type
+  ,                        !- Dehumidification Control Zone Name
+  60.0,                    !- Dehumidification Setpoint {percent}
+  None,                    !- Humidifier Type
+  ,                        !- Humidifier Availability Schedule Name
+  0.000001,                !- Humidifier Rated Capacity {m3/s}
+  2690.0,                  !- Humidifier Rated Electric Power {W}
+  ,                        !- Humidifier Control Zone Name
+  30.0,                    !- Humidifier Setpoint {percent}
+  NonCoincident,           !- Sizing Option
+  No,                      !- Return Fan
+  0.7,                     !- Return Fan Total Efficiency
+  500,                     !- Return Fan Delta Pressure {Pa}
+  0.9,                     !- Return Fan Motor Efficiency
+  1.0,                     !- Return Fan Motor in Air Stream Fraction
+  InletVaneDampers;        !- Return Fan Part-Load Power Coefficients
+\end{lstlisting}
+
+\subsection{HVACTemplate:System:PackagedVAV}\label{hvactemplatesystempackagedvav}
+
+This object simulates the system portion of a packaged direct-expansion based variable air volume HVAC configuration with several different heating options. Multiple HVACTemplate:Zone:VAV objects are usually specified for each HVACTemplate:System:PackagedVAV object.
+
+\subsubsection{Inputs}\label{inputs-19-002}
+
+\paragraph{Field: Name}\label{field-name-6-008}
+
+Enter a name for the HVACTemplate:System:PackagedVAV object. This name is used in the HVACTemplate:Zone:VAV object to reference this system.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-11}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. Please note that for this system type, this is a schedule of when the system is providing air flow.
+
+\paragraph{Field: Supply Fan Maximum Flow Rate}\label{field-supply-fan-maximum-flow-rate-2}
+
+Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m\(^{3}\)/s. The default is Autosize.
+
+\paragraph{Field: Supply Fan Minimum Flow Rate}\label{field-supply-fan-minimum-flow-rate-1}
+
+Enter the minimum supply air volume that may be provided. This field may be set to autosize. The units are in m\(^{3}\)/s.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement-8}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{DrawThrough}.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-9}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure-8}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 1000 Pa.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency-9}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater or equal to the Supply Fan Total Efficiency and less than or equal to 1. The default is 0.9.
+
+\paragraph{Field: Supply Fan Motor in Air Stream Fraction}\label{field-supply-fan-motor-in-air-stream-fraction-5}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-9}
+
+The coil types available:
+
+\begin{itemize}
+\item
+  TwoSpeedDX
+\item
+  TwoSpeedHumidControlDX
+\end{itemize}
+
+\emph{TwoSpeedDX} uses the Coil:Cooling:DX:TwoSpeed object. This is the preferred coil model for most applications. The \emph{TwoSpeedHumidControlDX} option uses the Coil:Cooling:DX:TwoStageWithHumidityControlMode object.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-8}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of one indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Coil Setpoint Schedule Name}\label{field-cooling-coil-setpoint-schedule-name-1}
+
+If a constant setpoint for the cooling coil is to be specified, leave this field blank, and the Cooling Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the cooling coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the cooling coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Cooling Coil Setpoint Reset Type is something other than None (see below). The default is None.
+
+\paragraph{Field: Cooling Coil Design Setpoint}\label{field-cooling-coil-design-setpoint-2}
+
+Enter the cooling supply air temperature in degrees C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8C. If no Cooling Coil Setpoint Schedule or Cooling Coil Setpoint Reset Type is specified, this value is used as a constant cooling supply air setpoint temperature.
+
+\paragraph{Field: Cooling Coil Gross Rated Total Capacity}\label{field-cooling-coil-gross-rated-total-capacity-6}
+
+Enter Autosize to let the automatic sizing algorithm determine the cooling coil gross rated total capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. For Cooling Coil Type = TwoSpeedDX, the low-speed capacity is assumed to be 0.33 times this value. For Cooling Coil Type = TwoSpeedHumidControlDX, the stage 1 capacity is assumed to be 0.5 times this value. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is Autosize.
+
+\paragraph{Field: Cooling Coil Gross Rated Sensible Heat Ratio}\label{field-cooling-coil-gross-rated-sensible-heat-ratio-6}
+
+Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by the gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be ``gross'', i.e., the effect of supply air fan heat is not accounted for. The default is Autosize.
+
+\paragraph{Field: Cooling Coil Gross Rated COP}\label{field-cooling-coil-gross-rated-cop-4}
+
+Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 3.0.
+
+\paragraph{Field: Heating Coil Type}\label{field-heating-coil-type-5}
+
+Enter the type of heating used in the unitary system. The choices for this field are
+
+\begin{itemize}
+\item
+  Electric
+\item
+  Gas
+\item
+  HotWater
+\end{itemize}
+
+\paragraph{Field: Heating Coil Availability Schedule Name}\label{field-heating-coil-availability-schedule-name-5}
+
+Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of 1.0 indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period
+
+\paragraph{Field: Heating Coil Setpoint Schedule Name}\label{field-heating-coil-setpoint-schedule-name-1}
+
+If a constant setpoint for the heating coil is to be specified, leave this field blank, and the Heating Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the heating coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the heating coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Heating Coil Setpoint Reset Type is something other than None (see below).
+
+\paragraph{Field: Heating Coil Design Setpoint}\label{field-heating-coil-design-setpoint-2}
+
+Enter the heating supply air temperature in degrees C to be used for sizing the heating coil and zone supply air flow rates. If no Heating Coil Setpoint Schedule or Heating Coil Setpoint Reset Type is specified, this value is used as a constant heating supply air setpoint temperature. The default is 10.0C.
+
+\paragraph{Field: Heating Coil Capacity}\label{field-heating-coil-capacity-2}
+
+Enter Autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the coil can deliver in Watts.
+
+\paragraph{Field: Gas Heating Coil Efficiency}\label{field-gas-heating-coil-efficiency-4}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default
+
+\paragraph{Field: Gas Heating Coil Parasitic Electric Load}\label{field-gas-heating-coil-parasitic-electric-load-4}
+
+Enter the parasitic electric load associated with the gas heating coil operation, such as a combustion fan. The units are in W. The default is 0.0 W.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-4}
+
+Enter Autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100\% of the full supply flow may be taken from outdoor air. If a value is entered, it is used instead of the autosize value. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template. The default is Autosize.
+
+\paragraph{Field: Minimum Outdoor Air Flow Rate}\label{field-minimum-outdoor-air-flow-rate-4}
+
+Enter Autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Control Type}\label{field-minimum-outdoor-air-control-type-1}
+
+Choices for this field are \textbf{FixedMinimum} or \textbf{ProportionalMinimum}. FixedMinimum means that the minimum outdoor air flow rate is fixed no matter what the actual system flow rate is. ProportionalMinimum means the minimum outdoor air flow rate varies in proportion to the total system air flow rate. The default is ProportionalMinimum.
+
+\paragraph{Field: Minimum Outdoor Air Schedule Name}\label{field-minimum-outdoor-air-schedule-name-3}
+
+Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 -- 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours.
+
+\paragraph{Field: Economizer Type}\label{field-economizer-type-4}
+
+The options for this field are
+
+\begin{itemize}
+\item
+  `FixedDryBulb'
+\item
+  `DifferentialDryBulb'
+\item
+  `FixedEnthalpy'
+\item
+  `DifferentialEnthalpy'
+\item
+  `ElectronicEnthalpy' (i.e., humidity ratio curve strategy)
+\item
+  `FixedDewPointAndDryBulb'
+\item
+  `DifferentialDryBulbAndEnthalpy'
+\item
+  `NoEconomizer'
+\end{itemize}
+
+Choosing \textbf{NoEconomizer} means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
+
+Choosing \textbf{FixedDryBulb} means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
+
+Choosing \textbf{DifferentialDryBulb} will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
+
+\textbf{FixedEnthalpy} checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
+
+\textbf{DifferentialEnthalpy} does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
+
+Choosing \textbf{ElectronicEnthalpy} enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
+
+Choosing \textbf{FixedDewPointAndDryBulb} compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
+
+Another option \textbf{DifferentialDryBulbAndEnthalpy} enables the control strategy to be based on both the \textbf{DifferentialDryBulb} and \textbf{DifferentialEnthalpy} economizer control strategies.
+
+In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
+
+The default for this field is \textbf{NoEconomizer}.
+
+\paragraph{Field: Economizer Lockout}\label{field-economizer-lockout-4}
+
+Enter one of the following choices for this field:
+
+\begin{itemize}
+\item
+  NoLockout
+\item
+  LockoutWithHeating
+\item
+  LockoutWithCompressor
+\end{itemize}
+
+The default value is \textbf{NoLockout}. The \textbf{LockoutWithHeating} means that if the packaged unit is in heating mode, the economizer is locked out -- i.e., the economizer dampers are closed and there is minimum outdoor air flow. \textbf{LockoutWithCompressor} means that in addition to locking out the economizer when the unit is in heating mode the economizer is locked out when the DX unit compressor is on. In other words, when the DX coil is off, the economizer must meet the entire cooling load -- it isn't allowed to operate in conjunction with the DX cooling coil. Similarly, when the DX coil is operating, the economizer is not allowed to operate. The \textbf{LockoutWithCompressor} option is sometimes called a ``nonintegrated'' economizer.
+
+\paragraph{Field: Economizer Maximum Limit Dry-Bulb Temperature}\label{field-economizer-maximum-limit-dry-bulb-temperature-2}
+
+Input for this field is the outdoor air temperature high limit (ºC) for economizer operation. If the outdoor air temperature is above this limit, the outdoor airflow rate will be set to the minimum. This field is required if Economizer Control Type `FixedDryBulb' or `FixedDewPointAndDryBulb' has been specified. No input (blank) in this field means that there is no outdoor air temperature high limit control.
+
+\paragraph{Field: Economizer Maximum Limit Enthalpy}\label{field-economizer-maximum-limit-enthalpy-2}
+
+Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
+
+\paragraph{Field: Economizer Maximum Limit Dewpoint Temperature}\label{field-economizer-maximum-limit-dewpoint-temperature-4}
+
+Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type `FixedDewPointAndDryBulb' has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
+
+\paragraph{Field: Economizer Minimum Limit Dry-Bulb Temperature}\label{field-economizer-minimum-limit-dry-bulb-temperature-2}
+
+Enter the outdoor air temperature low limit (C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name-9}
+
+Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any zone supply plenums have been specified, the outlet from the system supply plenum will flow through the zone supply plenum to the zone terminal unit.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-10}
+
+Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
+
+\paragraph{Field: Supply Fan Part-Load Power Coefficients}\label{field-supply-fan-part-load-power-coefficients-1}
+
+Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
+
+\begin{itemize}
+\item
+  InletVaneDampers
+\item
+  OutletDampers
+\item
+  VariableSpeedMotor
+\item
+  ASHRAE90.1-2004Appendix G
+\item
+  VariableSpeedMotorPressureReset
+\end{itemize}
+
+The default is \emph{InletVaneDampers}. The resulting power curves are shown in Figure~\ref{fig:vav-supply-fan-part-load-power-coefficient-001} below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The \emph{VariableSpeedMotorPressureReset} option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources': \emph{Design Guidelines: Advanced Variable Air Volume (VAV) Systems} (EDR\_DesignGuidelines\_VAV.pdf).
+
+\begin{figure}[hbtp] % fig 159
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image612.png}
+\caption{VAV Supply Fan Part-Load Power Coefficient Options \protect \label{fig:vav-supply-fan-part-load-power-coefficient-001}}
+\end{figure}
+
+\paragraph{Field: Night Cycle Control}\label{field-night-cycle-control-3}
+
+Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are \emph{StayOff}, \emph{CycleOnAny}, \emph{CycleOnControl Zone or CycleOnAnyZoneFansOnly}. \emph{StayOff} means the system will remain off, no matter how hot or cold the zones may be. \emph{CycleOnAny} means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. \emph{CycleOnControlZone} means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. \emph{CycleOnAnyZoneFansOnly} is the same as \emph{CycleOnAny} except that only the zone fans are cycled on and the central air handler fan is left off (applicable only if using HVACTemplate:Zone:VAV:FanPowered in one or more zones). The default is \emph{StayOff}.
+
+\paragraph{Field: Night Cycle Control Zone Name}\label{field-night-cycle-control-zone-name-3}
+
+For the Night Cycle Control option \emph{Cycle On Control Zone} enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
+
+\paragraph{Field: Heat Recovery Type}\label{field-heat-recovery-type-5}
+
+Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
+
+\begin{itemize}
+\item
+  None
+\item
+  Sensible
+\item
+  Enthalpy
+\end{itemize}
+
+The default is \textbf{None}\emph{.}
+
+\paragraph{Field: Sensible Heat Recovery Effectiveness}\label{field-sensible-heat-recovery-effectiveness-5}
+
+Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
+
+\paragraph{Field: Latent Heat Recovery Effectiveness}\label{field-latent-heat-recovery-effectiveness-5}
+
+Enter the latent heat recovery effectiveness if Heat Recovery Type is \emph{Enthalpy}. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
+
+\paragraph{Field: Cooling Coil Setpoint Reset Type}\label{field-cooling-coil-setpoint-reset-type-1}
+
+Select the type of automatic reset control for the cooling supply air temperature. The choices are:
+
+\begin{itemize}
+\item
+  None -- no reset, use the Cooling Coil Setpoint Schedule or Cooling Coil Design Setpoint.
+\item
+  Warmest -- reset the cooling supply air temperature to the highest supply air temperature that will meet the cooling requirements of all the zones at the maximum supply air flow rate. The minimum setpoint allowed is the Cooling Coil Design Setpoint. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:Warmest)
+\item
+  OutdoorAirTemperatureReset -- reset the cooling supply air temperature based on the following default rules. When the outdoor dry-bulb temperature (ODB) is at or below 15.6C the setpoint isthe Cooling Coil Design Setpoint plus 5.2C. When the ODB is at or above 26.7C the setpoint is the Cooling Coil Design Setpoint. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset)
+\item
+  WarmestTemperatureFirst -- find the highest setpoint temperature that will satisfy all the zone cooling loads at minimum supply air flow rate. If this setpoint temperature is less than the Cooling Coil Design Setpoint, the setpoint temperature is set to the minimum, and the supply air flow rate is increased to meet the loads. This option is appropriate when modeling a single-zone VAV system. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:WarmestTemperatureFlow)
+\end{itemize}
+
+The default is \emph{None}.
+
+\paragraph{Field: Heating Coil Setpoint Reset Type}\label{field-heating-coil-setpoint-reset-type-1}
+
+Select the type of automatic reset control for the central heating supply air temperature. The choices are:
+
+\begin{itemize}
+\item
+  None -- no reset, use the Heating Coil Setpoint Schedule or Heating Coil Design Setpoint.
+\item
+  OutdoorAirTemperatureReset -- reset the heating supply air temperature based on the following default rules. When the outdoor dry-bulb temperature (ODB) is at or below --6.7C the setpoint is the Heating Coil Design Setpoint. When the ODB is at or above 10.0C the setpoint isthe Heating Coil Design Setpoint minus 5.2C. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset).
+\end{itemize}
+
+The default is \emph{None}.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-4}
+
+There are two dehumidification control type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  CoolReheat
+\end{itemize}
+
+The \emph{CoolReheat} option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so. Reheat is provided as required by the terminal unit reheat coils if available.
+
+The default is \emph{None} which meets the sensible cooling setpoint only.
+
+\paragraph{Field: Dehumidification Control Zone Name}\label{field-dehumidification-control-zone-name-3}
+
+This field specifies the zone name where the humidistat is located for controlling dehumidification.
+
+\paragraph{Field: Dehumidification Setpoint}\label{field-dehumidification-setpoint-3}
+
+This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100). The default is 60\%.
+
+\paragraph{Field: Humidifier Type}\label{field-humidifier-type-4}
+
+There are two humidifier type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  ElectricSteam
+\end{itemize}
+
+The \emph{ElectricSteam} humidifier option uses the Humidifier:Steam:Electric object. The default is \emph{None.}
+
+\paragraph{Field: Humidifier Availability Schedule Name}\label{field-humidifier-availability-schedule-name-4}
+
+If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
+
+\paragraph{Field: Humidifier Rated Capacity}\label{field-humidifier-rated-capacity-4}
+
+Enter the rated moisture output rate in m3/s. The humidifier does not currently autosize, so the default is very large to allow for adequate capacity. The default is 0.000001 m3/s.
+
+\paragraph{Field: Humidifier Rated Electric Power}\label{field-humidifier-rated-electric-power-4}
+
+Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
+
+\paragraph{Field: Humidifier Control Zone Name}\label{field-humidifier-control-zone-name-4}
+
+This field specifies the zone name where the humidistat is located for controlling humidification.
+
+\paragraph{Field: Humidifier Setpoint}\label{field-humidifier-setpoint-3}
+
+This field specifies the zone humidistat setpoint for humidification in percent (0 to 100). The default is 30\%.
+
+\paragraph{Field: Sizing Option}\label{field-sizing-option-2}
+
+This field specifies the sizing method for the system supply air flow rate. \emph{Coincident} sizes on the sum of the coincident zone supply air flow rates. \emph{NonCoincident} sizes on sum of the noncoincident zone design supply air flow rates. The default is \emph{NonCoincident}.
+
+\paragraph{Field: Return Fan}\label{field-return-fan-2}
+
+Enter \emph{Yes} if the system has a return fan. The default is \emph{No}.
+
+\paragraph{Field: Return Fan Total Efficiency}\label{field-return-fan-total-efficiency-2}
+
+Enter the total efficiency of the return fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Return Fan Delta Pressure}\label{field-return-fan-delta-pressure-4}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 500 Pa.
+
+\paragraph{Field: Return Fan Motor efficiency}\label{field-return-fan-motor-efficiency-4}
+
+Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Return Fan Motor in Air Stream Fraction}\label{field-return-fan-motor-in-air-stream-fraction-4}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Return Fan Part-Load Power Coefficients}\label{field-return-fan-part-load-power-coefficients-1}
+
+Select the set of generic pre-defined coefficients to use for the return fan part-load power consumption. This alpha field has the following choices:
+
+\begin{itemize}
+\item
+  InletVaneDampers
+\item
+  OutletDampers
+\item
+  VariableSpeedMotor
+\item
+  ASHRAE90.1-2004Appendix G
+\item
+  VariableSpeedMotorPressureReset
+\end{itemize}
+
+The default is \emph{InletVaneDampers}. The resulting power curves are shown in Figure~\ref{fig:vav-supply-fan-part-load-power-coefficient}. VAV Supply Fan Part-Load Power Coefficient Options (see Supply Fan Part-Load Power Coefficients above). The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The \emph{VariableSpeedMotorPressureReset} option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources': \emph{Design Guidelines: Advanced Variable Air Volume (VAV) Systems} (EDR\_DesignGuidelines\_VAV.pdf).
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:System:PackagedVAV,
+  DXVAV Sys 1,             !-Name
+  FanAvailSched,           !- System Availability Schedule Name
+  autosize,                !- Supply Fan Maximum Flow Rate {m3/s}
+  autosize,                !- Supply Fan Minimum Flow Rate {m3/s}
+  DrawThrough,             !- Supply Fan Placement
+  0.7,                     !- Supply Fan Total Efficiency
+  1000,                    !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  1,                       !- Supply Fan Motor in Air Stream Fraction
+  TwoSpeedDX,              !- Cooling Coil Type
+  ,                        !- Cooling Coil Availability Schedule Name
+  ,                        !- Cooling Coil Setpoint Schedule Name
+  12.8,                    !- Cooling Coil Design Setpoint {C}
+  autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
+  autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
+  3,                       !- Cooling Coil Gross Rated COP
+  Gas,                     !- Heating Coil Type
+  ,                        !- Heating Coil Availability Schedule Name
+  ,                        !- Heating Coil Setpoint Schedule Name
+  10,                      !- Heating Coil Design Setpoint {C}
+  autosize,                !- Heating Coil Capacity {W}
+  0.8,                     !- Gas Heating Coil Efficiency
+  ,                        !- Gas Heating Coil Parasitic Electric Load {W}
+  autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
+  autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}
+  ProportionalMinimum,     !- Minimum Outdoor Air Control Type
+  Min OA Sched,            !- Minimum Outdoor Air Schedule Name
+  DifferentialDryBulb,     !- Economizer Type
+  NoLockout,               !- Economizer Lockout
+  19,                  !- Economizer Maximum Limit Dry-Bulb Temperature {C}
+  ,                        !- Economizer Maximum Limit Enthalpy {J/kg}
+  ,                    !- Economizer Maximum Limit Dewpoint Temperature {C}
+  4,                   !- Economizer Minimum Limit Dry-Bulb Temperature {C}
+  ,                        !- Supply Plenum Name
+  PLENUM-1,                !- Return Plenum Name
+  InletVaneDampers,        !- Supply Fan Part-Load Power Coefficients
+  CycleOnAny,              !- Night Cycle Control
+  ,                        !- Night Cycle Control Zone Name
+  None,                    !- Heat Recovery Type
+  0.7,                     !- Sensible Heat Recovery Effectiveness
+  0.65,                    !- Latent Heat Recovery Effectiveness
+  None,                    !- Cooling Coil Setpoint Reset Type
+  None,                    !- Heating Coil Setpoint Reset Type
+  None,                    !- Dehumidification Control Type
+  ,                        !- Dehumidification Control Zone Name
+  60,                      !- Dehumidification Setpoint {percent}
+  None,                    !- Humidifier Type
+  ,                        !- Humidifier Availability Schedule Name
+  0.000001,                !- Humidifier Rated Capacity {m3/s}
+  2690,                    !- Humidifier Rated Electric Power {W}
+  ,                        !- Humidifier Control Zone Name
+  30,                      !- Humidifier Setpoint {percent}
+  NonCoincident,           !- Sizing Option
+  No,                      !- Return Fan
+  0.7,                     !- Return Fan Total Efficiency
+  500,                     !- Return Fan Delta Pressure {Pa}
+  0.9,                     !- Return Fan Motor Efficiency
+  1.0,                     !- Return Fan Motor in Air Stream Fraction
+  InletVaneDampers;        !- Return Fan Part-Load Power Coefficients
+\end{lstlisting}
+
+\subsection{HVACTemplate:System:ConstantVolume}\label{hvactemplatesystemconstantvolume}
+
+This object simulates the system portion of a constant air volume HVAC configuration with option chilled water cooling and several different heating options. One or more HVACTemplate:Zone:ConstantVolume objects are specified for each zone served by the HVACTemplate:System:ConstantVolume object.
+
+\subsubsection{Inputs}\label{inputs-20-002}
+
+\paragraph{Field: Name}\label{field-name-7-007}
+
+Enter a name for the HVACTemplate:System:ConstantVolume object. This name is used in the HVACTemplate:Zone:ConstantVolume object to reference this system.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-12}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. Please note that for this system type, this is a schedule of when the system is providing air flow.
+
+\paragraph{Field: Supply Fan Maximum Flow Rate}\label{field-supply-fan-maximum-flow-rate-3}
+
+Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m\(^{3}\)/s.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-10}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure-9}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 600 Pa.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency-10}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Supply Fan Motor in Air Stream Fraction}\label{field-supply-fan-motor-in-air-stream-fraction-6}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement-9}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{Draw Through}.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-10}
+
+There are two coil types available:
+
+\begin{itemize}
+\item
+  ChilledWater
+\item
+  ChilledWaterDetailedFlatModel
+\item
+  HeatExchangerAssistedChilledWater
+\item
+  None
+\end{itemize}
+
+\emph{ChilledWater} uses the COIL:Cooling:Water object with the DetailedAnalysis option. This is the preferred coil model for most applications. \emph{ChilledWaterDetailedFlatModel} uses the Coil:Cooling:Water:DetailedGeometry object. This option is available for special applications. \emph{HeatExchangerAssistedChilledWater} uses the CoilSystem:Cooling:Water:HeatExchangerAssisted, HeatExchanger:AirToAir:SensibleAndLatent, and Coil:Cooling:Water objects. The default is \emph{ChilledWater}.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-9}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1 indicates that the cooling coil can be on during a given time period. A value of 0 denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Coil Setpoint Control Type}\label{field-cooling-coil-setpoint-control-type}
+
+Specifies the cooling coil setpoint control type:
+
+\begin{itemize}
+\item
+  FixedSetpoint - uses the Cooling Coil Design Setpoint as the supply air setpoint.
+\item
+  Scheduled - uses the Cooling Coil Design Setpoint as the supply air setpoint.
+\item
+  OutdoorAirTemperatureReset - varies the supply air setpoint based on the values entered for Cooling Coil Setpoint at Outdoor Dry-Bulb Low, Cooling Coil Reset Outdoor Dry-Bulb Low, Cooling Coil Setpoint at Outdoor Dry-Bulb High, and Cooling Coil Reset Outdoor Dry-Bulb High.
+\item
+  Warmest -- resets the cooling supply air temperature to the highest supply air temperature that will meet the cooling requirements of all the zones. The minimum setpoint allowed is the Cooling Coil Design Setpoint. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:Warmest)
+\item
+  ControlZone -- controls the supply air temperature to meet the current cooling load for the zone specified as the Cooling Coil Control Zone Name (below). The minimum setpoint is the Cooling Coil Design Setpoint. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:SingleZone:Cooling)
+\end{itemize}
+
+The default is \emph{FixedSetpoint}.
+
+NOTE: The user must ensure that the cooling coil and heating coil setpoints do not overlap to avoid unwanted simultaneous heating and cooling. The simulation will not check this automatically. It is recommended that the cooling setpoint always be at least 0.1C higher than the heating coil setpoint.
+
+\paragraph{Field: Cooling Coil Control Zone Name}\label{field-cooling-coil-control-zone-name}
+
+If the Cooling Coil Setpoint Control Type is ControlZone, enter the name of the HVACTemplate:Zone:ConstantVolume object that contains the cooling thermostat.
+
+\paragraph{Field: Cooling Coil Design Setpoint Temperature}\label{field-cooling-coil-design-setpoint-temperature}
+
+Enter the cooling supply air temperature in C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8C. If no Cooling Coil Setpoint Schedule or Cooling Coil Setpoint Reset Type is specified, this value is used as a constant cooling supply air setpoint temperature.
+
+\paragraph{Field: Cooling Coil Setpoint Schedule Name}\label{field-cooling-coil-setpoint-schedule-name-2}
+
+If a constant setpoint for the cooling coil is to be specified, leave this field blank, and the Cooling Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the cooling coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the cooling coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Cooling Coil Setpoint Reset Type is something other than None (see above).
+
+\paragraph{Field: Cooling Coil Setpoint at Outdoor Dry-Bulb Low}\label{field-cooling-coil-setpoint-at-outdoor-dry-bulb-low}
+
+The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Cooling Coil Reset Outdoor Dry-Bulb Low). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
+
+\paragraph{Field: Cooling Coil Reset Outdoor Dry-Bulb Low}\label{field-cooling-coil-reset-outdoor-dry-bulb-low}
+
+The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
+
+\paragraph{Field: Cooling Coil Setpoint at Outdoor Dry-Bulb High}\label{field-cooling-coil-setpoint-at-outdoor-dry-bulb-high}
+
+The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Cooling Coil Reset Outdoor Dry-Bulb High). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.8C.
+
+\paragraph{Field: Cooling Coil Reset Outdoor Dry-Bulb High}\label{field-cooling-coil-reset-outdoor-dry-bulb-high}
+
+The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb High. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 23.3C.
+
+\paragraph{Field: Heating Coil Type}\label{field-heating-coil-type-6}
+
+The heating coil is located in the supply air stream, upstream of the cooling coil and after the outdoor air mixing box. If no central heating coil is used in the Constant Volume system, then the option ``none'' should be specified here. Otherwise this indicates the type of heating coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\item
+  None
+\end{itemize}
+
+The default value is \emph{HotWater}. Note that the configuration of HVACTemplate:System:ConstantVolume assumes that there will be reheat coils or baseboard heating to provide heating control at the zone level. If a heating coil is specified, the heating and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
+
+\paragraph{Field: Heating Coil Availability Schedule Name}\label{field-heating-coil-availability-schedule-name-6}
+
+Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period.
+
+\paragraph{Field: Heating Coil Setpoint Control Type}\label{field-heating-coil-setpoint-control-type}
+
+Specifies the heating coil setpoint control type:
+
+\begin{itemize}
+\item
+  FixedSetpoint - uses the Heating Coil Design Setpoint as the supply air setpoint.
+\item
+  Scheduled - uses the Heating Coil Setpoint Schedule to set the supply air setpoint.
+\item
+  OutdoorAirTemperatureReset - varies the supply air setpoint based on the values entered for Heating Coil Setpoint at Outdoor Dry-Bulb Low, Heating Coil Reset Outdoor Dry-Bulb Low, Heating Coil Setpoint at Outdoor Dry-Bulb High, and Heating Coil Reset Outdoor Dry-Bulb High.
+\item
+  ControlZone - controls the supply air temperature to meet the current heating load for the zone specified as the Heating Coil Control Zone Name (below). The maximum setpoint is the Heating Coil Design Setpoint. The minimum setpoint allowed is defaulted to the lesser of the Heating Coil Design Setpoint minus 5.2C or the Cooling Coil Design Setpoint minus 1.0C. (Reference SetpointManager:SingleZone:Heating)
+\end{itemize}
+
+The default is FixedSetpoint.
+
+NOTE: The user must ensure that the cooling coil and heating coil setpoints do not overlap to avoid unwanted simultaneous heating and cooling. The simulation will not check this automatically. It is recommended that the cooling setpoint always be at least 0.1C higher than the heating coil setpoint.
+
+\paragraph{Field: Heating Coil Control Zone Name}\label{field-heating-coil-control-zone-name}
+
+Enter the name of the HVACTemplate:Zone:ConstantVolume object that contains the heating thermostat. While multiple HVACTemplate:Zone:ConstantVolume objects can be part of a HVACTemplate:System:ConstantVolume system, only one of the zones contains a thermostat that controls heating operation. For a single zone system, this field should contain the name of that zone.
+
+\paragraph{Field: Heating Coil Design Setpoint}\label{field-heating-coil-design-setpoint-3}
+
+Enter the heating supply air temperature in C to be used for sizing the heating coil and zone supply air flow rates. If no Heating Coil Setpoint Schedule or Heating Coil Setpoint Reset Type is specified, this value is used as a constant heating supply air setpoint temperature. The default is 10.0C.
+
+\paragraph{Field: Heating Coil Setpoint Schedule Name}\label{field-heating-coil-setpoint-schedule-name-2}
+
+If a constant setpoint for the heating coil is to be specified, leave this field blank, and the Heating Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the heating coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the heating coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Heating Coil Setpoint Reset Type is something other than None (see above).
+
+\paragraph{Field: Heating Coil Setpoint at Outdoor Dry-Bulb Low}\label{field-heating-coil-setpoint-at-outdoor-dry-bulb-low}
+
+The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Heating Coil Reset Outdoor Dry-Bulb Low). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.0C.
+
+\paragraph{Field: Heating Coil Reset Outdoor Dry-Bulb Low}\label{field-heating-coil-reset-outdoor-dry-bulb-low}
+
+The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 7.8C.
+
+\paragraph{Field: Heating Coil Setpoint at Outdoor Dry-Bulb High}\label{field-heating-coil-setpoint-at-outdoor-dry-bulb-high}
+
+The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Heating Coil Reset Outdoor Dry-Bulb High). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.2C.
+
+\paragraph{Field: Heating Coil Reset Outdoor Dry-Bulb High}\label{field-heating-coil-reset-outdoor-dry-bulb-high}
+
+The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb High. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.2C.
+
+\paragraph{Field: Heating Coil Capacity}\label{field-heating-coil-capacity-3}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the coil can deliver in Watts.
+
+\paragraph{Field: Gas Heating Coil Efficiency}\label{field-gas-heating-coil-efficiency-5}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default
+
+\paragraph{Field: Gas Heating Coil Parasitic Electric Load}\label{field-gas-heating-coil-parasitic-electric-load-5}
+
+Enter the parasitic electric load associated with the gas heating operation, such as a combustion fan. The units are in W.
+
+\paragraph{Field: Preheat Coil Type}\label{field-preheat-coil-type-1}
+
+The preheat coil is located in the outdoor air stream, upstream of the outdoor air mixing box and tempers the outdoor air. If no preheat coil is used in the constant volume system, then the option ``none'' should be specified here. Otherwise this indicates the type of preheat coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\item
+  None
+\end{itemize}
+
+The default value is None. If a preheat coil is specified, the preheat and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
+
+\paragraph{Field: Preheat Coil Availability Schedule Name}\label{field-preheat-coil-availability-schedule-name-1}
+
+Usually set to blank, which allows the preheat coil to be available anytime the system is operating. If a schedule name is specified, it defines when the preheat coil is available. This is most often used when preheat is only available seasonally. The schedule values denote whether the preheat coil can run during a given time period. A schedule value of 1.0 indicates that the preheat coil can be on during a given time period. A value of zero denotes that the preheat coil cannot be used during that time period
+
+\paragraph{Field: Preheat Coil Design Setpoint}\label{field-preheat-coil-design-setpoint-1}
+
+Enter the preheat supply air temperature in C to be used for sizing the preheat coil. If no Preheat Coil Setpoint Schedule is specified, this value is used as a constant preheat supply air setpoint temperature. The default is 7.2C.
+
+\paragraph{Field: Preheat Coil Setpoint Schedule Name}\label{field-preheat-coil-setpoint-schedule-name-1}
+
+If a constant setpoint for the preheat coil is to be specified, leave this field blank, and the Preheat Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the preheat coil specify the schedule name here. The schedule should control the leaving air temperature from the preheat coil. The values in the schedule are in degrees C.
+
+\paragraph{Field: Gas Preheat Coil Efficiency}\label{field-gas-preheat-coil-efficiency-1}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default
+
+\paragraph{Field: Gas Preheat Coil Parasitic Electric Load}\label{field-gas-preheat-coil-parasitic-electric-load-1}
+
+Enter the parasitic electric load associated with the gas heating operation, such as an combustion fan. The units are in W.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-5}
+
+Enter autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100\% of the full supply flow may be taken from outdoor air. If a value is entered, it is used instead of the autosize value. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Flow Rate}\label{field-minimum-outdoor-air-flow-rate-5}
+
+Enter autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Schedule Name}\label{field-minimum-outdoor-air-schedule-name-4}
+
+Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 -- 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours.
+
+\paragraph{Field: Economizer Type}\label{field-economizer-type-5}
+
+The options for this field are
+
+\begin{itemize}
+\item
+  `FixedDryBulb'
+\item
+  `DifferentialDryBulb'
+\item
+  `FixedEnthalpy'
+\item
+  `DifferentialEnthalpy'
+\item
+  `ElectronicEnthalpy' (i.e., humidity ratio curve strategy)
+\item
+  `FixedDewPointAndDryBulb'
+\item
+  `DifferentialDryBulbAndEnthalpy'
+\item
+  `NoEconomizer'
+\end{itemize}
+
+Choosing \textbf{NoEconomizer} means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
+
+Choosing \textbf{FixedDryBulb} means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
+
+Choosing \textbf{DifferentialDryBulb} will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
+
+\textbf{FixedEnthalpy} checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
+
+\textbf{DifferentialEnthalpy} does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
+
+Choosing \textbf{ElectronicEnthalpy} enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
+
+Choosing \textbf{FixedDewPointAndDryBulb} compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
+
+Another option \textbf{DifferentialDryBulbAndEnthalpy} enables the control strategy to be based on both the \textbf{DifferentialDryBulb} and \textbf{DifferentialEnthalpy} economizer control strategies.
+
+In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
+
+The default for this field is \textbf{NoEconomizer}.
+
+\paragraph{Field: Economizer Upper Temperature Limit}\label{field-economizer-upper-temperature-limit-2}
+
+Enter the outdoor air temperature high limit (\(^{o}\)C) for economizer operation. If the outdoor air temperature is above this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature high limit control.
+
+\paragraph{Field: Economizer Lower Temperature Limit}\label{field-economizer-lower-temperature-limit-2}
+
+Enter the outdoor air temperature low limit (\(^{o}\)C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
+
+\paragraph{Field: Economizer Upper Enthalpy Limit}\label{field-economizer-upper-enthalpy-limit-2}
+
+Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
+
+\paragraph{Field: Economizer Maximum Limit Dewpoint Temperature}\label{field-economizer-maximum-limit-dewpoint-temperature-5}
+
+Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type `FixedDewPointAndDryBulb' has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
+
+\paragraph{Field: Supply Plenum Name}\label{field-supply-plenum-name-10}
+
+Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any supply plenums have been specified, the outlet from the system supply plenum will flow through the supply plenum to the zone terminal unit.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-11}
+
+Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
+
+\paragraph{Field: Night Cycle Control}\label{field-night-cycle-control-4}
+
+Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are \emph{StayOff}, \emph{CycleOnAny}, \emph{CycleOnControlZone or CycleOnAnyZoneFansOnly}. \emph{StayOff} means the system will remain off, no matter how hot or cold the zones may be. \emph{CycleOnAny} means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. \emph{CycleOnControlZone} means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. \emph{CycleOnAnyZoneFansOnly} is the same as \emph{CycleOnAny} except that only the zone fans are cycled on and the central air handler fan is left off (applicable only if using HVACTemplate:Zone:VAV:FanPowered in one or more zones). The default is \emph{StayOff}.
+
+\paragraph{Field: Night Cycle Control Zone Name}\label{field-night-cycle-control-zone-name-4}
+
+For the Night Cycle Control option \emph{Cycle On Control Zone} enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
+
+\paragraph{Field: Heat Recovery Type}\label{field-heat-recovery-type-6}
+
+Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
+
+\begin{itemize}
+\item
+  None
+\item
+  Sensible
+\item
+  Enthalpy
+\end{itemize}
+
+The default is \textbf{None}\emph{.}
+
+\paragraph{Field: Sensible Heat Recovery Effectiveness}\label{field-sensible-heat-recovery-effectiveness-6}
+
+Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
+
+\paragraph{Field: Latent Heat Recovery Effectiveness}\label{field-latent-heat-recovery-effectiveness-6}
+
+Enter the latent heat recovery effectiveness if Heat Recovery Type is \emph{Enthalpy}. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
+
+\paragraph{Field: Heat Recovery Heat Exchanger Type}\label{field-heat-recovery-heat-exchanger-type-1}
+
+This alpha field denotes the type of heat exchanger being modeled: Plate (e.g., fixed plate) or Rotary (e.g., rotating cylinder or wheel). The default choice for this field is ``Plate''. The heat exchanger type affects the modeling of frost control options and supply air outlet temperature control. For rotary heat exchangers, rotational speed is varied to control frost formation or the supply air outlet temperature. For plate exchangers, air bypass around the heat exchanger is used to obtain the desired effect.
+
+\paragraph{Field: Heat Recovery Frost Control Type}\label{field-heat-recovery-frost-control-type-1}
+
+This alpha field has four choices: None, ExhaustAirRecirculation, ExhaustOnly and MinimumExhaustTemperature. If this field is left blank, the default frost control type is ``None''. For modeling preheat frost control, specify ``None'' for this input field and insert a separate heating coil object in the supply inlet air stream to keep the air temperature above the desired frost threshold temperature.
+
+\emph{ExhaustAirRecirculation}: dampers are used to direct exhaust air back into the zone through the supply side of the heat exchanger when the supply (outdoor) air inlet temperature falls below a threshold temperature. The fraction of time that exhaust air is circulated through the supply side of the heat exchanger is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When exhaust air is being recirculated, no supply (outdoor ventilation) air is being provided through the heat exchanger unit (which may or may not be acceptable regarding ventilation for occupants).
+
+\emph{ExhaustOnly (supply air bypass)}: this control cycles off the supply air flow through the heat exchanger for a certain period of time while the exhaust air continues to flow through the exhaust side of the heat exchanger. The fraction of time that the supply flow through the heat exchanger is cycled off is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When implemented in real applications, provisions are usually made to avoid building depressurization when this frost control is operating (automatic or pressure-operated dampers, or a bypass air damper around the supply side of the heat exchanger). For this frost control type, it is assumed that the supply air is bypassed around the heat exchanger during frost control operation (i.e., the total supply flow is not reduced during defrost, but merely bypassed around the heat exchanger).
+
+\emph{MinimumExhaustTemperature}: the temperature of the exhaust air leaving the heat exchanger is monitored and the heat exchanger effectiveness is decreased (by slowing heat exchanger rotation or bypassing supply air around the plate exchanger) to keep the exhaust air from falling below the threshold temperature.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-5}
+
+There are two dehumidification control type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  CoolReheat
+\end{itemize}
+
+The \emph{CoolReheat} option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so. Reheat is provided as required by the central heating coil if available or the terminal unit reheat coils if available.
+
+The default is \emph{None} which meets the sensible cooling setpoint only.
+
+\paragraph{Field: Dehumidification Control Zone Name}\label{field-dehumidification-control-zone-name-4}
+
+This field specifies the zone name where the humidistat is located for controlling dehumidification.
+
+\paragraph{Field: Dehumidification Relative Humidity Setpoint}\label{field-dehumidification-relative-humidity-setpoint-1}
+
+This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100). The default is 60\%. This field is ignored if a Dehumidification Relative Humidity Setpoint Schedule Name is specified.
+
+\paragraph{Field: Dehumidification Relative Humidity Setpoint Schedule Name}\label{field-dehumidification-relative-humidity-setpoint-schedule-name-1}
+
+Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint, The values in the schedule are in percent (0 to 100).
+
+\paragraph{Field: Humidifier Type}\label{field-humidifier-type-5}
+
+There are two humidifier type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  ElectricSteam
+\end{itemize}
+
+The \emph{ElectricSteam} humidifier option uses the Humidifier:Steam:Electric object. The default is \emph{None.}
+
+\paragraph{Field: Humidifier Availability Schedule Name}\label{field-humidifier-availability-schedule-name-5}
+
+If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
+
+\paragraph{Field: Humidifier Rated Capacity}\label{field-humidifier-rated-capacity-5}
+
+Enter the rated moisture output rate in m3/s. The humidifier does not currently autosize, so the default is very large to allow for adequate capacity. The default is 0.000001 m3/s.
+
+\paragraph{Field: Humidifier Rated Electric Power}\label{field-humidifier-rated-electric-power-5}
+
+Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
+
+\paragraph{Field: Humidifier Control Zone Name}\label{field-humidifier-control-zone-name-5}
+
+This field specifies the zone name where the humidistat is located for controlling humidification.
+
+\paragraph{Field: Humidifier Relative Humidity Setpoint}\label{field-humidifier-relative-humidity-setpoint-1}
+
+This field specifies the zone humidistat setpoint for humidification in percent (0 to 100). The default is 30\%. This field is ignored if a Humidifier Relative Humidity Setpoint Schedule Name is specified.
+
+\paragraph{Field: Humidifier Relative Humidity Setpoint Schedule Name}\label{field-humidifier-relative-humidity-setpoint-schedule-name-1}
+
+Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint, The values in the schedule are in percent (0 to 100).
+
+\paragraph{Field: Return Fan}\label{field-return-fan-3}
+
+Enter \emph{Yes} if the system has a return fan. The default is \emph{No}.
+
+\paragraph{Field: Return Fan Total Efficiency}\label{field-return-fan-total-efficiency-3}
+
+Enter the total efficiency of the return fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1. Default is 0.7.
+
+\paragraph{Field: Return Fan Delta Pressure}\label{field-return-fan-delta-pressure-5}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 300 Pa.
+
+\paragraph{Field: Return Fan Motor efficiency}\label{field-return-fan-motor-efficiency-5}
+
+Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. Default is 0.9.
+
+\paragraph{Field: Return Fan Motor in Air Stream Fraction}\label{field-return-fan-motor-in-air-stream-fraction-5}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. Default is 1.0.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:System:ConstantVolume,
+  CAV Sys 1,               !-Name
+  FanAvailSched,           !- System Availability Schedule Name
+  autosize,                !- Supply Fan Maximum Flow Rate {m3/s}
+  0.7,                     !- Supply Fan Total Efficiency
+  600,                     !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  1,                       !- Supply Fan Motor in Air Stream Fraction
+  DrawThrough,             !- Supply Fan Placement
+  ChilledWater,            !- Cooling Coil Type
+  ,                        !- Cooling Coil Availability Schedule Name
+  ControlZone,             !- Cooling Coil Setpoint Control Type
+  SPACE 1-1,               !- Cooling Coil Conrol Zone
+  12.8,                        !- Cooling Coil Design Setpoint {C}
+  ,                        !- Cooling Coil Setpoint Schedule Name
+  ,                   !- Cooling Coil Setpoint at Outdoor Dry-Bulb Low {C}
+  ,                        !- Cooling Coil Reset Outdoor Dry-Bulb Low {C}
+  ,                   !- Cooling Coil Setpoint at Outdoor Dry-Bulb High {C}
+  ,                        !- Cooling Coil Reset Outdoor Dry-Bulb High {C}
+  HotWater,                !- Heating Coil Type
+  ,                        !- Heating Coil Availability Schedule Name
+  FixedSetpoint,           !- Heating Coil Setpoint Control Type
+  ,                        !- Heating Coil Control Zone
+  50,                        !- Heating Coil Design Setpoint {C}
+  ,                        !- Heating Coil Setpoint Schedule Name
+  ,                   !- Heating Coil Setpoint at Outdoor Dry-Bulb Low {C}
+  ,                        !- Hedating Coil Reset Outdoor Dry-Bulb Low {C}
+  ,                   !- Heating Coil Setpoint at Outdoor Dry-Bulb High {C}
+  ,                        !- Heating Coil Reset Outdoor Dry-Bulb High {C}
+  Autosize,                !- Heating Coil Capacity {W}
+  0.8,                     !- Gas Heating Coil Efficiency
+  0.0,                     !- Gas Heating Coil Parasitic Electric Load {W}
+  None,                    !- Preheat Coil Type
+  ,                        !- Preheat Coil Availability Schedule Name
+  ,                        !- Preheat Coil Design Setpoint {C}
+  ,                        !- Preheat Coil Setpoint Schedule Name
+  0.8,                     !- Gas Preheat Coil Efficiency
+  0.0,                     !- Gas Preheat Coil Parasitic Electric Load {W}
+  autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
+  autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}
+  Min OA Sched,            !- Minimum Outdoor Air Schedule Name
+  DifferentialDryBulb,     !- Economizer Type
+  19,                      !- Economizer Upper Temperature Limit {C}
+  4,                       !- Economizer Lower Temperature Limit {C}
+  ,                        !- Economizer Upper Enthalpy Limit {J/kg}
+  ,                    !- Economizer Maximum Limit Dewpoint Temperature {C}
+  ,                        !- Supply Plenum Name
+  PLENUM-1,                !- Return Plenum Name
+  CycleOnAnyZoneFansOnly,  !- Night Cycle Control
+  ,                        !- Night Cycle Control Zone Name
+  None,                    !- Heat Recovery Type
+  0.70,                    !- Sensible Heat Recovery Effectiveness
+  0.65,                    !- Latent Heat Recovery Effectiveness
+  ,                        !- Heat Recovery Heat Exchanger Type
+  ,                        !- Heat Recovery Frost Control Type
+  None,                    !- Dehumidification Control Type
+  ,                        !- Dehumidification Control Zone Name
+  60.0,     !- Dehumidification Relative Humidity Setpoint {percent}
+  ,         !- Dehumidification Relative Humidity Setpoint Schedule Name
+  None,                    !- Humidifier Type
+  ,                        !- Humidifier Availability Schedule Name
+  0.000001,                !- Humidifier Rated Capacity {m3/s}
+  2690.0,                  !- Humidifier Rated Electric Power {W}
+  ,                        !- Humidifier Control Zone Name
+  30.0,     !- Humidifier Relative Humidity Setpoint {percent}
+  ,         !- Humidifier Relative Humidity Setpoint Schedule Name
+  No,                      !- Return Fan
+  0.7,                     !- Return Fan Total Efficiency
+  600,                     !- Return Fan Delta Pressure {Pa}
+  0.9,                     !- Return Fan Motor Efficiency
+  1.0;                     !- Return Fan Motor in Air Stream Fraction
+\end{lstlisting}
+
+\subsection{HVACTemplate:System:DualDuct}\label{hvactemplatesystemdualduct}
+
+This object simulates the system portion of a constant air volume or variable air volume dual-duct HVAC configuration with optional chilled water cooling and several different heating options. One or more HVACTemplate:Zone:DualDuct objects may be specified for each zone served by the HVACTemplate:System:DualDuct object. The system will be constant volume if all of the HVACTemplate:Zone:DualDuct objects served by this system have Zone Minimum Air Flow Fraction = 1.0.
+
+\subsubsection{Inputs}\label{inputs-21-002}
+
+\paragraph{Field: Name}\label{field-name-8-007}
+
+Enter a name for the HVACTemplate:System:DualDuct object. This name is used in the HVACTemplate:Zone:DualDuct object to reference this system.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-13}
+
+Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. Please note that for this system type, this is a schedule of when the system is providing air flow.
+
+\paragraph{Field: Supply Fan Configuration Type}\label{field-supply-fan-configuration-type}
+
+This field specifies the supply fan configuration. * SingleConstantVolume* and \emph{SingleVariableVolume} specify one supply fan located in the main supply air duct before the split into a cold supply air duct and a hot supply air duct. This configuration uses the `Main Supply Fan' input fields which follow immediately below. \emph{DualConstantVolume} and \emph{DualVariableVolume} specify two supply fans, one located in the cold supply air duct and one located in the hot supply air duct. \emph{Dual} uses the `Cold Duct Supply Fan' and Hot Duct Supply Fan' inputs which follow below. The default is\emph{SingleConstantVolume}.
+
+\paragraph{Field: Main Supply Fan Maximum Flow Rate}\label{field-main-supply-fan-maximum-flow-rate}
+
+Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m\(^{3}\)/s.
+
+\paragraph{Field: Main Supply Fan Minimum Flow Fraction}\label{field-main-supply-fan-minimum-flow-fraction}
+
+Enter the minimum supply air flow fraction that may be provided. This field is ignored if the system is constant volume.
+
+\paragraph{Field: Main Supply Fan Total Efficiency}\label{field-main-supply-fan-total-efficiency}
+
+Enter the total efficiency of the main supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7..
+
+\paragraph{Field: Main Supply Fan Delta Pressure}\label{field-main-supply-fan-delta-pressure}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 1000 Pa.
+
+\paragraph{Field: Main Supply Fan Motor Efficiency}\label{field-main-supply-fan-motor-efficiency}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Main Supply Fan Motor in Air Stream Fraction}\label{field-main-supply-fan-motor-in-air-stream-fraction}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Main Supply Fan Part-Load Power Coefficients}\label{field-main-supply-fan-part-load-power-coefficients}
+
+Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
+
+\begin{itemize}
+\item
+  InletVaneDampers
+\item
+  OutletDampers
+\item
+  VariableSpeedMotor
+\item
+  ASHRAE90.1-2004Appendix G
+\item
+  VariableSpeedMotorPressureReset
+\end{itemize}
+
+The default is \emph{InletVaneDampers}. The resulting power curves are shown in Figure~\ref{fig:vav-supply-fan-part-load-power-coefficient}. VAV Supply Fan Part-Load Power Coefficient Options below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The \emph{VariableSpeedMotorPressureReset} option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources': \emph{Design Guidelines: Advanced Variable Air Volume (VAV) Systems} (EDR\_DesignGuidelines\_VAV.pdf).
+
+\begin{figure}[hbtp] % fig 160
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image613.png}
+\caption{VAV Supply Fan Part-Load Power Coefficient Options \protect \label{fig:vav-supply-fan-part-load-power-coefficient-002}}
+\end{figure}
+
+\paragraph{Field: Cold Duct Supply Fan Maximum Flow Rate}\label{field-cold-duct-supply-fan-maximum-flow-rate}
+
+Enter Autosize to set the system maximum cold duct air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m\(^{3}\)/s.
+
+\paragraph{Field: Cold Duct Supply Fan Minimum Flow Fraction}\label{field-cold-duct-supply-fan-minimum-flow-fraction}
+
+Enter the minimum cold duct air flow fraction that may be provided. This field is ignored if the system is constant volume.
+
+\paragraph{Field: Cold Duct Supply Fan Total Efficiency}\label{field-cold-duct-supply-fan-total-efficiency}
+
+Enter the total efficiency of the cold duct supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Cold Duct Supply Fan Delta Pressure}\label{field-cold-duct-supply-fan-delta-pressure}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 1000 Pa.
+
+\paragraph{Field: Cold Duct Supply Fan Motor efficiency}\label{field-cold-duct-supply-fan-motor-efficiency}
+
+Enter the shaft power of the cold duct supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Cold Duct Supply Fan Motor in Air Stream Fraction}\label{field-cold-duct-supply-fan-motor-in-air-stream-fraction}
+
+Enter the fraction of the motor heat that is added to the cold duct air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Cold Duct Supply Fan Part-Load Power Coefficients}\label{field-cold-duct-supply-fan-part-load-power-coefficients}
+
+Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
+
+\begin{itemize}
+\item
+  InletVaneDampers
+\item
+  OutletDampers
+\item
+  VariableSpeedMotor
+\item
+  ASHRAE90.1-2004Appendix G
+\item
+  VariableSpeedMotorPressureReset
+\end{itemize}
+
+The default is \emph{InletVaneDampers}. The resulting power curves are shown in Figure~\ref{fig:vav-supply-fan-part-load-power-coefficient}. VAV Supply Fan Part-Load Power Coefficient Options below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The \emph{VariableSpeedMotorPressureReset} option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources': \emph{Design Guidelines: Advanced Variable Air Volume (VAV) Systems} (EDR\_DesignGuidelines\_VAV.pdf).
+
+\paragraph{Field: Cold Duct Supply Fan Placement}\label{field-cold-duct-supply-fan-placement}
+
+Enter the cold duct supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{Draw Through}.
+
+\paragraph{Field: Hot Duct Supply Fan Maximum Flow Rate}\label{field-hot-duct-supply-fan-maximum-flow-rate}
+
+Enter Autosize to set the system maximum hot duct air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will \emph{not} be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m\(^{3}\)/s.
+
+\paragraph{Field: Hot Duct Supply Fan Minimum Flow Fraction}\label{field-hot-duct-supply-fan-minimum-flow-fraction}
+
+Enter the minimum hot duct air flow fraction that may be provided. This field is ignored if the system is constant volume.
+
+\paragraph{Field: Hot Duct Supply Fan Total Efficiency}\label{field-hot-duct-supply-fan-total-efficiency}
+
+Enter the total efficiency of the hot duct supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Hot Duct Supply Fan Delta Pressure}\label{field-hot-duct-supply-fan-delta-pressure}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 1000 Pa.
+
+\paragraph{Field: Hot Duct Supply Fan Motor efficiency}\label{field-hot-duct-supply-fan-motor-efficiency}
+
+Enter the shaft power of the hot duct supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Hot Duct Supply Fan Motor in Air Stream Fraction}\label{field-hot-duct-supply-fan-motor-in-air-stream-fraction}
+
+Enter the fraction of the motor heat that is added to the hot duct air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Hot Duct Supply Fan Part-Load Power Coefficients}\label{field-hot-duct-supply-fan-part-load-power-coefficients}
+
+Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
+
+\begin{itemize}
+\item
+  InletVaneDampers
+\item
+  OutletDampers
+\item
+  VariableSpeedMotor
+\item
+  ASHRAE90.1-2004Appendix G
+\item
+  VariableSpeedMotorPressureReset
+\end{itemize}
+
+The default is \emph{InletVaneDampers}. The resulting power curves are shown in Figure~\ref{fig:vav-supply-fan-part-load-power-coefficient}. VAV Supply Fan Part-Load Power Coefficient Options below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The \emph{VariableSpeedMotorPressureReset} option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources': \emph{Design Guidelines: Advanced Variable Air Volume (VAV) Systems} (EDR\_DesignGuidelines\_VAV.pdf).
+
+\paragraph{Field: Hot Duct Supply Fan Placement}\label{field-hot-duct-supply-fan-placement}
+
+Enter the hot duct supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{Draw Through}.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-11}
+
+There are two coil types available:
+
+\begin{itemize}
+\item
+  ChilledWater
+\item
+  ChilledWaterDetailedFlatModel
+\item
+  None
+\end{itemize}
+
+\emph{ChilledWater} uses the COIL:Cooling:Water object with the DetailedAnalysis option. This is the preferred coil model for most applications. \emph{ChilledWaterDetailedFlatModel} uses the Coil:Cooling:Water:DetailedGeometry object. This option is available for special applications. The default is \emph{ChilledWater}.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-10}
+
+Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1 indicates that the cooling coil can be on during a given time period. A value of 0 denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Coil Setpoint Control Type}\label{field-cooling-coil-setpoint-control-type-1}
+
+Specifies the cooling coil setpoint control type:
+
+\begin{itemize}
+\item
+  FixedSetpoint
+\item
+  Scheduled
+\item
+  OutdoorAirTemperatureReset
+\item
+  Warmest -- reset the cooling supply air temperature to the highest supply air temperature that will meet the cooling requirements of all the zones. The minimum setpoint allowed is the Cooling Coil Design Setpoint. The maximum setpoint allowed is defaulted to 18C or the Cooling Design Setpoint + 5.2C whichever is greater.. (Reference SetpointManager:Warmest)
+\end{itemize}
+
+FixedSetpoint uses the Cooling Coil Design Setpoint as the supply air setpoint. Scheduled uses the Cooling Coil Setpoint Schedule to set the supply air setpoint. OutdoorAirTemperatureReset varies the supply air setpoint based on the values entered for Cooling Coil Setpoint at Outdoor Dry-Bulb Low, Cooling Coil Reset Outdoor Dry-Bulb Low, Cooling Coil Setpoint at Outdoor Dry-Bulb High, and Cooling Coil Reset Outdoor Dry-Bulb High. The default is FixedSetpoint.
+
+\paragraph{Field: Cooling Coil Design Setpoint Temperature}\label{field-cooling-coil-design-setpoint-temperature-1}
+
+Enter the cooling supply air temperature in C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8C. If no Cooling Coil Setpoint Schedule or Cooling Coil Setpoint Reset Type is specified, this value is used as a constant cooling supply air setpoint temperature.
+
+\paragraph{Field: Cooling Coil Setpoint Schedule Name}\label{field-cooling-coil-setpoint-schedule-name-3}
+
+If a constant setpoint for the cooling coil is to be specified, leave this field blank, and the Cooling Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the cooling coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the cooling coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Cooling Coil Setpoint Reset Type is something other than None (see above).
+
+\paragraph{Field: Cooling Coil Setpoint at Outdoor Dry-Bulb Low}\label{field-cooling-coil-setpoint-at-outdoor-dry-bulb-low-1}
+
+The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Cooling Coil Reset Outdoor Dry-Bulb Low). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
+
+\paragraph{Field: Cooling Coil Reset Outdoor Dry-Bulb Low}\label{field-cooling-coil-reset-outdoor-dry-bulb-low-1}
+
+The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
+
+\paragraph{Field: Cooling Coil Setpoint at Outdoor Dry-Bulb High}\label{field-cooling-coil-setpoint-at-outdoor-dry-bulb-high-1}
+
+The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Cooling Coil Reset Outdoor Dry-Bulb High). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.8C.
+
+\paragraph{Field: Cooling Coil Reset Outdoor Dry-Bulb High}\label{field-cooling-coil-reset-outdoor-dry-bulb-high-1}
+
+The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb High. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 23.3C.
+
+\paragraph{Field: Heating Coil Type}\label{field-heating-coil-type-7}
+
+The heating coil is located in the supply air stream, upstream of the cooling coil and after the outdoor air mixing box. If no central heating coil is used in the Constant Volume system, then the option ``none'' should be specified here. Otherwise this indicates the type of heating coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\item
+  None
+\end{itemize}
+
+The default value is HotWater. Note that the configuration of HVACTemplate:System:ConstantVolume assumes that there will be reheat coils or baseboard heating to provide heating control at the zone level. If a heating coil is specified, the heating and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
+
+\paragraph{Field: Heating Coil Availability Schedule Name}\label{field-heating-coil-availability-schedule-name-7}
+
+Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period.
+
+\paragraph{Field: Heating Coil Setpoint Control Type}\label{field-heating-coil-setpoint-control-type-1}
+
+Specifies the heating coil setpoint control type:
+
+\begin{itemize}
+\item
+  FixedSetpoint
+\item
+  Scheduled
+\item
+  OutdoorAirTemperatureReset
+\item
+  Warmest -- reset the heating supply air temperature to the coldest supply air temperature that will meet the heating requirements of all the zones. The maximum setpoint allowed is the Heating Coil Design Setpoint. The minimum setpoint allowed is defaulted to 20C or the Heating Coil Design Setpoint -- 5.2C whichever is lower.. (Reference SetpointManager:Coldest)
+\end{itemize}
+
+FixedSetpoint uses the Heating Coil Design Setpoint as the supply air setpoint. Scheduled uses the Heating Coil Setpoint Schedule to set the supply air setpoint. OutdoorAirTemperatureReset varies the supply air setpoint based on the values entered for Heating Coil Setpoint at Outdoor Dry-Bulb Low, Heating Coil Reset Outdoor Dry-Bulb Low, Heating Coil Setpoint at Outdoor Dry-Bulb High, and Heating Coil Reset Outdoor Dry-Bulb High. The default is FixedSetpoint.
+
+\paragraph{Field: Heating Coil Design Setpoint}\label{field-heating-coil-design-setpoint-4}
+
+Enter the heating supply air temperature in C to be used for sizing the heating coil and zone supply air flow rates. If no Heating Coil Setpoint Schedule or Heating Coil Setpoint Reset Type is specified, this value is used as a constant heating supply air setpoint temperature. The default is 50.0C.
+
+\paragraph{Field: Heating Coil Setpoint Schedule Name}\label{field-heating-coil-setpoint-schedule-name-3}
+
+If a constant setpoint for the heating coil is to be specified, leave this field blank, and the Heating Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the heating coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the heating coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Heating Coil Setpoint Reset Type is something other than None (see above).
+
+\paragraph{Field: Heating Coil Setpoint at Outdoor Dry-Bulb Low}\label{field-heating-coil-setpoint-at-outdoor-dry-bulb-low-1}
+
+The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Heating Coil Reset Outdoor Dry-Bulb Low). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 50.0C.
+
+\paragraph{Field: Heating Coil Reset Outdoor Dry-Bulb Low}\label{field-heating-coil-reset-outdoor-dry-bulb-low-1}
+
+The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 7.8C.
+
+\paragraph{Field: Heating Coil Setpoint at Outdoor Dry-Bulb High}\label{field-heating-coil-setpoint-at-outdoor-dry-bulb-high-1}
+
+The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Heating Coil Reset Outdoor Dry-Bulb High). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 20.0C.
+
+\paragraph{Field: Heating Coil Reset Outdoor Dry-Bulb High}\label{field-heating-coil-reset-outdoor-dry-bulb-high-1}
+
+The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb High. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.2C.
+
+\paragraph{Field: Heating Coil Capacity}\label{field-heating-coil-capacity-4}
+
+Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the coil can deliver in Watts.
+
+\paragraph{Field: Gas Heating Coil Efficiency}\label{field-gas-heating-coil-efficiency-6}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default
+
+\paragraph{Field: Gas Heating Coil Parasitic Electric Load}\label{field-gas-heating-coil-parasitic-electric-load-6}
+
+Enter the parasitic electric load associated with the gas heating operation, such as a combustion fan. The units are in W.
+
+\paragraph{Field: Preheat Coil Type}\label{field-preheat-coil-type-2}
+
+The preheat coil is located in the outdoor air stream, upstream of the outdoor air mixing box and tempers the outdoor air. If no preheat coil is used in the constant volume system, then the option ``none'' should be specified here. Otherwise this indicates the type of preheat coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\item
+  None
+\end{itemize}
+
+The default value is None. If a preheat coil is specified, the preheat and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
+
+\paragraph{Field: Preheat Coil Availability Schedule Name}\label{field-preheat-coil-availability-schedule-name-2}
+
+Usually set to blank, which allows the preheat coil to be available anytime the system is operating. If a schedule name is specified, it defines when the preheat coil is available. This is most often used when preheat is only available seasonally. The schedule values denote whether the preheat coil can run during a given time period. A schedule value of 1.0 indicates that the preheat coil can be on during a given time period. A value of zero denotes that the preheat coil cannot be used during that time period
+
+\paragraph{Field: Preheat Coil Design Setpoint}\label{field-preheat-coil-design-setpoint-2}
+
+Enter the preheat supply air temperature in C to be used for sizing the preheat coil. If no Preheat Coil Setpoint Schedule is specified, this value is used as a constant preheat supply air setpoint temperature. The default is 7.2C.
+
+\paragraph{Field: Preheat Coil Setpoint Schedule Name}\label{field-preheat-coil-setpoint-schedule-name-2}
+
+If a constant setpoint for the preheat coil is to be specified, leave this field blank, and the Preheat Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the preheat coil specify the schedule name here. The schedule should control the leaving air temperature from the preheat coil. The values in the schedule are in degrees C.
+
+\paragraph{Field: Gas Preheat Coil Efficiency}\label{field-gas-preheat-coil-efficiency-2}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default
+
+\paragraph{Field: Gas Preheat Coil Parasitic Electric Load}\label{field-gas-preheat-coil-parasitic-electric-load-2}
+
+Enter the parasitic electric load associated with the gas heating operation, such as an combustion fan. The units are in W.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-6}
+
+Enter autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100\% of the full supply flow may be taken from outdoor air. If a value is entered, it is used instead of the autosize value. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Flow Rate}\label{field-minimum-outdoor-air-flow-rate-6}
+
+Enter autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
+
+\paragraph{Field: Minimum Outdoor Air Control Type}\label{field-minimum-outdoor-air-control-type-2}
+
+Choices for this field are \textbf{FixedMinimum} or \textbf{ProportionalMinimum}. FixedMinimum means that the minimum outdoor air flow rate is fixed no matter what the actual system flow rate is. ProportionalMinimum means the minimum outdoor air flow rate varies in proportion to the total system air flow rate. The default is ProportionalMinimum.
+
+\paragraph{Field: Minimum Outdoor Air Schedule Name Name}\label{field-minimum-outdoor-air-schedule-name-name-1}
+
+Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 -- 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours.
+
+\paragraph{Field: Economizer Type}\label{field-economizer-type-6}
+
+The options for this field are
+
+\begin{itemize}
+\item
+  `FixedDryBulb'
+\item
+  `DifferentialDryBulb'
+\item
+  `FixedEnthalpy'
+\item
+  `DifferentialEnthalpy'
+\item
+  `ElectronicEnthalpy' (i.e., humidity ratio curve strategy)
+\item
+  `FixedDewPointAndDryBulb'
+\item
+  `DifferentialDryBulbAndEnthalpy'
+\item
+  `NoEconomizer'
+\end{itemize}
+
+Choosing \textbf{NoEconomizer} means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
+
+Choosing \textbf{FixedDryBulb} means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
+
+Choosing \textbf{DifferentialDryBulb} will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
+
+\textbf{FixedEnthalpy} checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
+
+\textbf{DifferentialEnthalpy} does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
+
+Choosing \textbf{ElectronicEnthalpy} enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
+
+Choosing \textbf{FixedDewPointAndDryBulb} compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
+
+Another option \textbf{DifferentialDryBulbAndEnthalpy} enables the control strategy to be based on both the \textbf{DifferentialDryBulb} and \textbf{DifferentialEnthalpy} economizer control strategies.
+
+In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
+
+The default for this field is \textbf{NoEconomizer}.
+
+\paragraph{Field: Economizer Lockout}\label{field-economizer-lockout-5}
+
+The only choice for this field is
+
+\begin{itemize}
+\tightlist
+\item
+  NoLockout
+\end{itemize}
+
+The default value is NoLockout. Future versions may have additional options.
+
+\paragraph{Field: Economizer Upper Temperature Limit}\label{field-economizer-upper-temperature-limit-3}
+
+Enter the outdoor air temperature high limit (\(^{o}\)C) for economizer operation. If the outdoor air temperature is above this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature high limit control.
+
+\paragraph{Field: Economizer Lower Temperature Limit}\label{field-economizer-lower-temperature-limit-3}
+
+Enter the outdoor air temperature low limit (\(^{o}\)C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
+
+\paragraph{Field: Economizer Upper Enthalpy Limit}\label{field-economizer-upper-enthalpy-limit-3}
+
+Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
+
+\paragraph{Field: Economizer Maximum Limit Dewpoint Temperature}\label{field-economizer-maximum-limit-dewpoint-temperature-6}
+
+Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type `FixedDewPointAndDryBulb' has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
+
+\paragraph{Field: Cold Supply Plenum Name}\label{field-cold-supply-plenum-name-1}
+
+Set to blank if no cold supply plenum is to be modeled. If a cold supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves the cold inlets of all zones on this system. If any zone supply plenums have been specified, the outlet from the system supply plenum will flow through the zone supply plenum to the zone terminal unit.
+
+\paragraph{Field: Hot Supply Plenum Name}\label{field-hot-supply-plenum-name-1}
+
+Set to blank if no hot supply plenum is to be modeled. If a hot supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves hot inlets of all zones on this system. If any zone supply plenums have been specified, the outlet from the system supply plenum will flow through the zone supply plenum to the zone terminal unit.
+
+\paragraph{Field: Return Plenum Name}\label{field-return-plenum-name-12}
+
+Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
+
+\paragraph{Field: Night Cycle Control}\label{field-night-cycle-control-5}
+
+Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are \emph{StayOff}, \emph{CycleOnAny}, or \emph{CycleOnControlZone}. \emph{StayOff} means the system will remain off, no matter how hot or cold the zones may be. \emph{CycleOnAny} means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. \emph{CycleOnControlZone} means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. The default is \emph{StayOff}.
+
+\paragraph{Field: Night Cycle Control Zone Name}\label{field-night-cycle-control-zone-name-5}
+
+For the Night Cycle Control option \emph{Cycle On Control Zone} enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
+
+\paragraph{Field: Heat Recovery Type}\label{field-heat-recovery-type-7}
+
+Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
+
+\begin{itemize}
+\item
+  None
+\item
+  Sensible
+\item
+  Enthalpy
+\end{itemize}
+
+The default is \textbf{None}\emph{.}
+
+\paragraph{Field: Sensible Heat Recovery Effectiveness}\label{field-sensible-heat-recovery-effectiveness-7}
+
+Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
+
+\paragraph{Field: Latent Heat Recovery Effectiveness}\label{field-latent-heat-recovery-effectiveness-7}
+
+Enter the latent heat recovery effectiveness if Heat Recovery Type is \emph{Enthalpy}. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
+
+\paragraph{Field: Heat Recovery Heat Exchanger Type}\label{field-heat-recovery-heat-exchanger-type-2}
+
+This alpha field denotes the type of heat exchanger being modeled: Plate (e.g., fixed plate) or Rotary (e.g., rotating cylinder or wheel). The default choice for this field is ``Plate''. The heat exchanger type affects the modeling of frost control options and supply air outlet temperature control. For rotary heat exchangers, rotational speed is varied to control frost formation or the supply air outlet temperature. For plate exchangers, air bypass around the heat exchanger is used to obtain the desired effect.
+
+\paragraph{Field: Heat Recovery Frost Control Type}\label{field-heat-recovery-frost-control-type-2}
+
+This alpha field has four choices: None, ExhaustAirRecirculation, ExhaustOnly and MinimumExhaustTemperature. If this field is left blank, the default frost control type is ``None''. For modeling preheat frost control, specify ``None'' for this input field and insert a separate heating coil object in the supply inlet air stream to keep the air temperature above the desired frost threshold temperature.
+
+\emph{ExhaustAirRecirculation}: dampers are used to direct exhaust air back into the zone through the supply side of the heat exchanger when the supply (outdoor) air inlet temperature falls below a threshold temperature. The fraction of time that exhaust air is circulated through the supply side of the heat exchanger is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When exhaust air is being recirculated, no supply (outdoor ventilation) air is being provided through the heat exchanger unit (which may or may not be acceptable regarding ventilation for occupants).
+
+\emph{ExhaustOnly (supply air bypass)}: this control cycles off the supply air flow through the heat exchanger for a certain period of time while the exhaust air continues to flow through the exhaust side of the heat exchanger. The fraction of time that the supply flow through the heat exchanger is cycled off is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When implemented in real applications, provisions are usually made to avoid building depressurization when this frost control is operating (automatic or pressure-operated dampers, or a bypass air damper around the supply side of the heat exchanger). For this frost control type, it is assumed that the supply air is bypassed around the heat exchanger during frost control operation (i.e., the total supply flow is not reduced during defrost, but merely bypassed around the heat exchanger).
+
+\emph{MinimumExhaustTemperature}: the temperature of the exhaust air leaving the heat exchanger is monitored and the heat exchanger effectiveness is decreased (by slowing heat exchanger rotation or bypassing supply air around the plate exchanger) to keep the exhaust air from falling below the threshold temperature.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-6}
+
+There are two dehumidification control type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  CoolReheat
+\end{itemize}
+
+The \emph{CoolReheat} option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so. Reheat is provided as required by the terminal unit reheat coils if available.
+
+The default is \emph{None} which meets the sensible cooling setpoint only.
+
+\paragraph{Field: Dehumidification Control Zone Name}\label{field-dehumidification-control-zone-name-5}
+
+This field specifies the zone name where the humidistat is located for controlling dehumidification.
+
+\paragraph{Field: Dehumidification Relative Humidity Setpoint}\label{field-dehumidification-relative-humidity-setpoint-2}
+
+This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100). The default is 60\%. This field is ignored if a Dehumidification Relative Humidity Setpoint Schedule Name is specified.
+
+\paragraph{Field: Dehumidification Relative Humidity Setpoint Schedule Name}\label{field-dehumidification-relative-humidity-setpoint-schedule-name-2}
+
+Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint, The values in the schedule are in percent (0 to 100).
+
+\paragraph{Field: Humidifier Type}\label{field-humidifier-type-6}
+
+There are two humidifier type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  ElectricSteam
+\end{itemize}
+
+The \emph{ElectricSteam} humidifier option uses the Humidifier:Steam:Electric object. The default is \emph{None.}
+
+\paragraph{Field: Humidifier Availability Schedule Name}\label{field-humidifier-availability-schedule-name-6}
+
+If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
+
+\paragraph{Field: Humidifier Rated Capacity}\label{field-humidifier-rated-capacity-6}
+
+Enter the rated moisture output rate in m3/s. The humidifier does not currently autosize, so the default is very large to allow for adequate capacity. The default is 0.000001 m3/s.
+
+\paragraph{Field: Humidifier Rated Electric Power}\label{field-humidifier-rated-electric-power-6}
+
+Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
+
+\paragraph{Field: Humidifier Control Zone Name}\label{field-humidifier-control-zone-name-6}
+
+This field specifies the zone name where the humidistat is located for controlling humidification.
+
+\paragraph{Field: Humidifier Relative Humidity Setpoint}\label{field-humidifier-relative-humidity-setpoint-2}
+
+This field specifies the zone humidistat setpoint for humidification in percent (0 to 100). The default is 30\%. This field is ignored if a Humidifier Relative Humidity Setpoint Schedule Name is specified.
+
+\paragraph{Field: Humidifier Relative Humidity Setpoint Schedule Name}\label{field-humidifier-relative-humidity-setpoint-schedule-name-2}
+
+Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint, The values in the schedule are in percent (0 to 100).
+
+\paragraph{Field: Sizing Option}\label{field-sizing-option-3}
+
+This field specifies the sizing method for the system supply air flow rate when the system type if variable volume. \emph{Coincident} sizes on the sum of the coincident zone supply air flow rates. \emph{NonCoincident} sizes on sum of the noncoincident zone design supply air flow rates. The default is \emph{NonCoincident}.
+
+\paragraph{Field: Return Fan}\label{field-return-fan-4}
+
+Enter \emph{Yes} if the system has a return fan. The default is \emph{No}.
+
+\paragraph{Field: Return Fan Total Efficiency}\label{field-return-fan-total-efficiency-4}
+
+Enter the total efficiency of the return fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Return Fan Delta Pressure}\label{field-return-fan-delta-pressure-6}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20\(^{o}\) C at sea level, 101325 Pa. The default is 500 Pa.
+
+\paragraph{Field: Return Fan Motor efficiency}\label{field-return-fan-motor-efficiency-6}
+
+Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Return Fan Motor in Air Stream Fraction}\label{field-return-fan-motor-in-air-stream-fraction-6}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Return Fan Part-Load Power Coefficients}\label{field-return-fan-part-load-power-coefficients-2}
+
+Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
+
+\begin{itemize}
+\item
+  InletVaneDampers
+\item
+  OutletDampers
+\item
+  VariableSpeedMotor
+\item
+  ASHRAE90.1-2004Appendix G
+\item
+  VariableSpeedMotorPressureReset
+\end{itemize}
+
+The default is \emph{InletVaneDampers}. The resulting power curves are shown in Figure~\ref{fig:vav-supply-fan-part-load-power-coefficient}. VAV Supply Fan Part-Load Power Coefficient Options below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The \emph{VariableSpeedMotorPressureReset} option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources': \emph{Design Guidelines: Advanced Variable Air Volume (VAV) Systems} (EDR\_DesignGuidelines\_VAV.pdf).
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:System:DualDuct,
+  DD Sys 1,               !-Name
+  FanAvailSched,          !- System Availability Schedule Name
+  Single,                 !- Supply Fan Configuration Type  
+  autosize,               !- Main Supply Fan Maximum Flow Rate {m3/s}
+  0.2,                    !- Main Supply Fan Minimum Flow Fraction
+  0.7,                    !- Main Supply Fan Total Efficiency
+  600,                    !- Main Supply Fan Delta Pressure {Pa}
+  0.9,                    !- Main Supply Fan Motor Efficiency
+  1,                      !- Main Supply Fan Motor in Air Stream Fraction
+  InletVaneDampers,       !- Main Supply Fan Part-Load Power Coefficients
+  autosize,               !- Cold Duct Supply Fan Maximum Flow Rate {m3/s}
+  0.2,                    !- Cold Duct Supply Fan Minimum Flow Fraction
+  0.7,                    !- Cold Duct Supply Fan Total Efficiency
+  600,                    !- Cold Duct Supply Fan Delta Pressure {Pa}
+  0.9,                    !- Cold Duct Supply Fan Motor Efficiency
+  1,                   !- Cold Duct Supply Fan Motor in Air Stream Fraction
+  InletVaneDampers,    !- Cold Duct Supply Fan Part-Load Power Coefficients
+  DrawThrough,            !- Cold Duct Supply Fan Placement
+  autosize,               !- Hot Duct Supply Fan Maximum Flow Rate {m3/s}
+  0.2,                    !- Hot Duct Supply Fan Minimum Flow Fraction
+  0.7,                    !- Hot Duct Supply Fan Total Efficiency
+  600,                    !- Hot Duct Supply Fan Delta Pressure {Pa}
+  0.9,                    !- Hot Duct Supply Fan Motor Efficiency
+  1,                   !- Hot Duct Supply Fan Motor in Air Stream Fraction
+  InletVaneDampers,    !- Hot Duct Supply Fan Part-Load Power Coefficients
+  DrawThrough,            !- Hot Duct Supply Fan Placement
+  ChilledWater,           !- Cooling Coil Type
+  ,                       !- Cooling Coil Availability Schedule Name
+  ControlZone,            !- Cooling Coil Setpoint Control Type
+  12.8,                   !- Cooling Coil Design Setpoint {C}
+  ,                       !- Cooling Coil Setpoint Schedule Name
+  ,                   !- Cooling Coil Setpoint at Outdoor Dry-Bulb Low {C}
+  ,                       !- Cooling Coil Reset Outdoor Dry-Bulb Low {C}
+  ,                   !- Cooling Coil Setpoint at Outdoor Dry-Bulb High {C}
+  ,                       !- Cooling Coil Reset Outdoor Dry-Bulb High {C}
+  HotWater,               !- Heating Coil Type
+  ,                       !- Heating Coil Availability Schedule Name
+  FixedSetpoint,          !- Heating Coil Setpoint Control Type
+  50,                     !- Heating Coil Design Setpoint {C}
+  ,                       !- Heating Coil Setpoint Schedule Name
+  ,                   !- Heating Coil Setpoint at Outdoor Dry-Bulb Low {C}
+  ,                       !- Hedating Coil Reset Outdoor Dry-Bulb Low {C}
+  ,                   !- Heating Coil Setpoint at Outdoor Dry-Bulb High {C}
+  ,                       !- Heating Coil Reset Outdoor Dry-Bulb High {C}
+  Autosize,               !- Heating Coil Capacity {W}
+  0.8,                    !- Gas Heating Coil Efficiency
+  0.0,                    !- Gas Heating Coil Parasitic Electric Load {W}
+  None,                   !- Preheat Coil Type
+  ,                       !- Preheat Coil Availability Schedule Name
+  ,                       !- Preheat Coil Setpoint Schedule Name
+  ,                       !- Preheat Coil Design Setpoint {C}
+  0.8,                    !- Gas Preheat Coil Efficiency
+  0.0,                    !- Gas Preheat Coil Parasitic Electric Load {W}
+  autosize,               !- Maximum Outdoor Air Flow Rate {m3/s}
+  autosize,               !- Minimum Outdoor Air Flow Rate {m3/s}
+  FixedMinimum,           !- Minimum Outdoor Air Control Type
+  Min OA Sched,           !- Minimum Outdoor Air Schedule Name
+  DifferentialDryBulb,    !- Economizer Type
+  NoLockout,              !- Economizer Lockout
+  19,                     !- Economizer Upper Temperature Limit {C}
+  4,                      !- Economizer Lower Temperature Limit {C}
+  ,                       !- Economizer Upper Enthalpy Limit {J/kg}
+  ,                    !- Economizer Maximum Limit Dewpoint Temperature {C}
+  ,                       !- Cold Supply Plenum Name
+  ,                       !- Hot Supply Plenum Name
+  PLENUM-1,               !- Return Plenum Name
+  CycleOnAnyZoneFansOnly, !- Night Cycle Control
+  ,                       !- Night Cycle Control Zone Name
+  None,                   !- Heat Recovery Type
+  0.70,                   !- Sensible Heat Recovery Effectiveness
+  0.65,                   !- Latent Heat Recovery Effectiveness
+  ,                       !- Heat Recovery Heat Exchanger Type
+  ,                       !- Heat Recovery Frost Control Type
+  None,                   !- Dehumidification Control Type
+  ,                       !- Dehumidification Control Zone Name
+  60.0,    !- Dehumidification Relative Humidity Setpoint {percent}
+  ,         !- Dehumidification Relative Humidity Setpoint Schedule Name
+  None,                   !- Humidifier Type
+  ,                       !- Humidifier Availability Schedule Name
+  0.000001,               !- Humidifier Rated Capacity {m3/s}
+  2690.0,                 !- Humidifier Rated Electric Power {W}
+  ,                       !- Humidifier Control Zone Name
+  30.0,    !- Humidifier Relative Humidity Setpoint {percent}
+  ,         !- Humidifier Relative Humidity Setpoint Schedule Name
+  NonCoincident,          !- Sizing Option
+  No,                     !- Return Fan
+  0.7,                    !- Return Fan Total Efficiency
+  600,                    !- Return Fan Delta Pressure {Pa}
+  0.9,                    !- Return Fan Motor Efficiency
+  1.0;                    !- Return Fan Motor in Air Stream Fraction
+  InletVaneDampers;       !- Return Fan Part-Load Power Coefficients
+\end{lstlisting}
+
+\subsection{HVACTemplate:System:DedicatedOutdoorAir}\label{hvactemplatesystemdedicatedoutdoorair}
+
+The HVACTemplate:System:DedicatedOutdoorAir creates a dedicated outdoor air system which must be used in conjunction with one or more of the following objects:
+
+HVACTemplate:Zone:BaseboardHeat
+
+HVACTemplate:Zone:FanCoil
+
+HVACTemplate:Zone:PTAC
+
+HVACTemplate:Zone:PTHP
+
+HVACTemplate:Zone:WaterToAirHeatPump
+
+HVACTemplate:Zone:VRF
+
+It is a constant volume dedicated outdoor air system which can serve multiple zones. It may have any combination of heating coil, cooling coil, and heat recovery. It may have dehumidification and humidification controls as well as several supply temperature control types. It supplies 100\% outdoor air when the system is available, and assumes an equal volume of return air is available for heat recovery. If the system to be modeled does not have actual return ducts, but collects flow from exhaust fans to a central heat recovery point, then this approach should be equivalent. If the system does not have heat recovery and the air is exhausted or leaves by exfiltration, then the return path of this system will simply be a path to dump the flow as relief air with no impact on energy use.
+
+\begin{figure}[hbtp] % fig 161
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image614.png}
+\caption{DOAS serving three zones with PTACs. \protect \label{fig:doas-serving-three-zones-with-ptacs.}}
+\end{figure}
+
+There may be more than one HVACTemplate:System:DedicatedOutdoorAir object in an idf file. If a zone is to be served by one of these systems, this is specified in the HVACTemplate:Zone:* object using the field ``Dedicated Outdoor Air System Name''. For zones which are served by one of these DOAS systems, the outdoor air flow rate in the zone equipment (fan coil, PTAC, etc.) will be set to zero.
+
+\subsubsection{Inputs}\label{inputs-22-001}
+
+\paragraph{Field: Name}\label{field-name-9-007}
+
+This field is a unique name which the user assigns to this system. This name can then be referred to in an HVACTemplate:Zone:* object to specify that this system provides outdoor air to that zone.
+
+\paragraph{Field: System Availability Schedule Name}\label{field-system-availability-schedule-name-14}
+
+Leave this field blank if you want the system to operate at all times. If a schedule name is specified, those times that the system is operating should be specified as 1.0. Those times that the system is not operating should have a zero value in the schedule specified. Please note that for this system type, this is a schedule of when the system is providing air flow.
+
+\paragraph{Field: Air Outlet Type}\label{field-air-outlet-type}
+
+This field indicates if the air is delivered directly into the zone(s) or into the other system(s) that serve the zone(s) (e.g.~fan coil system). For now, only one option is available for this field: DirectIntoZone.
+
+\paragraph{Field: Supply Fan Flow Rate}\label{field-supply-fan-flow-rate}
+
+Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone air flow inputs sum to a greater value. The units are m\(^{3}\)/s.
+
+\paragraph{Field: Supply Fan Total Efficiency}\label{field-supply-fan-total-efficiency-11}
+
+Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Supply Fan Delta Pressure}\label{field-supply-fan-delta-pressure-10}
+
+Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered to be 20\(^{o}\) C at sea level, 101325 Pa.
+
+\paragraph{Field: Supply Fan Motor Efficiency}\label{field-supply-fan-motor-efficiency-11}
+
+Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
+
+\paragraph{Field: Supply Fan Motor in Air Stream Fraction}\label{field-supply-fan-motor-in-air-stream-fraction-7}
+
+Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
+
+\paragraph{Field: Supply Fan Placement}\label{field-supply-fan-placement-10}
+
+Enter the supply fan placement type. This alpha field has two choices, \emph{DrawThrough} or \emph{BlowThrough}. \emph{DrawThrough} models a system where the supply air fan is after the cooling and heating coils. \emph{BlowThrough} models a system where the supply air fan is before the cooling and heating coils. The default is \emph{DrawThrough}.
+
+\paragraph{Field: Cooling Coil Type}\label{field-cooling-coil-type-12}
+
+There are seven coil types available:
+
+\begin{itemize}
+\item
+  ChilledWater
+\item
+  ChilledWaterDetailedFlatModel
+\item
+  TwoSpeedDX
+\item
+  TwoStageDX
+\item
+  TwoStageHumidityControlDX
+\item
+  HeatExchangerAssistedChilledWater
+\item
+  HeatExchangerAssistedDX
+\item
+  None
+\end{itemize}
+
+\emph{ChilledWater} uses the Coil:Cooling:Water object with the DetailedAnalysis option. This is the preferred coil model for most chilled water applications.
+
+\emph{ChilledWaterDetailedFlatModel} uses the Coil:Cooling:Water:DetailedGeometry object. This option is available for special applications.
+
+\emph{TwoSpeedDX} uses the Coil:Cooling:DX:TwoSpeed object.
+
+\emph{TwoStageDX} and \emph{TwoStageHumidityControlDX} use the Coil:Cooling:DX:TwoStageWithHumidityControlMode object.
+
+\emph{HeatExchangerAssistedChilledWater} uses the CoilSystem:Cooling:Water:HeatExchangerAssisted, HeatExchanger:AirToAir:SensibleAndLatent, and Coil:Cooling:Water objects.
+
+\emph{HeatExchangerAssistedDX} uses the CoilSystem:Cooling:DX:HeatExchangerAssisted, HeatExchanger:AirToAir:SensibleAndLatent, and Coil:Cooling:DX:SingleSpeed objects.
+
+The default type is \emph{ChilledWater}.
+
+\paragraph{Field: Cooling Coil Availability Schedule Name}\label{field-cooling-coil-availability-schedule-name-11}
+
+Usually left blank, which allows the cooling coil to be available as needed anytime the system is operating. If a schedule name is specified, it defines when the cooling coil is available. This is most often used when cooling is only available seasonally. A schedule value of one indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
+
+\paragraph{Field: Cooling Coil Setpoint Control Type}\label{field-cooling-coil-setpoint-control-type-2}
+
+Specifies the cooling coil setpoint control type:
+
+\begin{itemize}
+\item
+  FixedSetpoint
+\item
+  Scheduled
+\item
+  OutdoorAirTemperatureReset
+\end{itemize}
+
+FixedSetpoint uses the Cooling Coil Design Setpoint as the supply air setpoint. Scheduled uses the Cooling Coil Setpoint Schedule to set the supply air setpoint. OutdoorAirTemperatureReset varies the supply air setpoint based on the values entered for Cooling Coil Setpoint at Outdoor Dry-Bulb Low, Cooling Coil Reset Outdoor Dry-Bulb Low, Cooling Coil Setpoint at Outdoor Dry-Bulb High, and Cooling Coil Reset Outdoor Dry-Bulb High. The default is FixedSetpoint.
+
+NOTE: The user must ensure that the cooling coil and heating coil setpoints do not overlap to avoid unwanted simultaneous heating and cooling. The simulation will not check this automatically. It is recommended that the cooling setpoint always be at least 0.1C higher than the heating coil setpoint.
+
+\paragraph{Field: Cooling Coil Design Setpoint}\label{field-cooling-coil-design-setpoint-3}
+
+Enter the cooling supply air temperature in C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8C. If Cooling Coil Setpoint Control Type = FixedSetpoint, then this value is also used as the constant cooling supply air setpoint temperature.
+
+\paragraph{Field: Cooling Coil Setpoint Schedule Name}\label{field-cooling-coil-setpoint-schedule-name-4}
+
+This field is used when Cooling Coil Setpoint Control Type = Scheduled. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the cooling coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Cooling Coil Setpoint Reset Type is something other than Scheduled (see above).
+
+\paragraph{Field: Cooling Coil Setpoint at Outdoor Dry-Bulb Low}\label{field-cooling-coil-setpoint-at-outdoor-dry-bulb-low-2}
+
+The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Cooling Coil Reset Outdoor Dry-Bulb Low). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
+
+\paragraph{Field: Cooling Coil Reset Outdoor Dry-Bulb Low}\label{field-cooling-coil-reset-outdoor-dry-bulb-low-2}
+
+The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
+
+\paragraph{Field: Cooling Coil Setpoint at Outdoor Dry-Bulb High}\label{field-cooling-coil-setpoint-at-outdoor-dry-bulb-high-2}
+
+The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Cooling Coil Reset Outdoor Dry-Bulb High). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.8C.
+
+\paragraph{Field: Cooling Coil Reset Outdoor Dry-Bulb High}\label{field-cooling-coil-reset-outdoor-dry-bulb-high-2}
+
+The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb High. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 23.3C.
+
+\paragraph{Field: DX Cooling Coil Gross Rated Total Capacity}\label{field-dx-cooling-coil-gross-rated-total-capacity-1}
+
+Enter Autosize to let the automatic sizing algorithm determine the cooling coil gross total cooling capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb. Capacity should be the ``gross'', i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is Autosize. This field is only used when the cooling coil type is set to one of the DX options. For two-speed DX coils, the low-speed capacity is assumed to be 0.33 times this value. For two-stage DX coils, the stage 1 capacity is assumed to be 0.5 times this value.
+
+\paragraph{Field: DX Cooling Coil Gross Rated Sensible Heat Ratio}\label{field-dx-cooling-coil-gross-rated-sensible-heat-ratio-1}
+
+Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the gross rated cooling total capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be ``gross'', i.e., the effect of supply air fan heat is not accounted for. The default is Autosize. This field is only used when the cooling coil type is set to one of the DX options. For two-speed DX coils, the low-speed SHR is assumed to be equal to this value. For two-stage DX coils, the stage 1 SHR is assumed to be equal to this value. For two-stage DX coil with humidity control, the humidity control mode SHR is assumed to be 0.9 times this value (for both stage 1 and stage 2).
+
+\paragraph{Field: DX Cooling Coil Gross Rated COP}\label{field-dx-cooling-coil-gross-rated-cop-1}
+
+Enter the coefficient of performance defined as the gross cooling coil total capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The default is 3.0. This field is only used when the cooling coil type is set to one of the DX options. For two-speed DX coils, the low-speed COP is assumed to be 1.5 times this value. For two-stage DX coils, the stage 1 COP is assumed to be this this value. For two-stage DX coil with humidity control, the humidity control mode COP is assumed to be 0.9 times this value (for both stage 1 and stage 2). The gross COP should not account for the supply air fan.
+
+\paragraph{Field: Heating Coil Type}\label{field-heating-coil-type-8}
+
+The heating coil is located in the supply air stream, downstream of the cooling coil. If no central heating coil is used in the dedicated outdoor air system, then the option ``none'' should be specified here. Otherwise this indicates the type of heating coil. The choices for this field are
+
+\begin{itemize}
+\item
+  HotWater
+\item
+  Electric
+\item
+  Gas
+\item
+  None
+\end{itemize}
+
+The default value is HotWater. If a heating coil is specified, the heating and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other. When the dehumidification control type is set to \emph{CoolReheatHeatingCoil,} the heating coil is used for reheat.
+
+\paragraph{Field: Heating Coil Availability Schedule Name}\label{field-heating-coil-availability-schedule-name-8}
+
+Usually left blank, which allows the heating coil to be available as needed anytime the system is operating. If a schedule name is specified, it defines when the heating coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period.
+
+\paragraph{Field: Heating Coil Setpoint Control Type}\label{field-heating-coil-setpoint-control-type-2}
+
+Specifies the cooling coil setpoint control type:
+
+\begin{itemize}
+\item
+  FixedSetpoint
+\item
+  Scheduled
+\item
+  OutdoorAirTemperatureReset
+\end{itemize}
+
+FixedSetpoint uses the Heating Coil Design Setpoint as the supply air setpoint. Scheduled uses the Heating Coil Setpoint Schedule to set the supply air setpoint. OutdoorAirTemperatureReset varies the supply air setpoint based on the values entered for Heating Coil Setpoint at Outdoor Dry-Bulb Low, Heating Coil Reset Outdoor Dry-Bulb Low, Heating Coil Setpoint at Outdoor Dry-Bulb High, and Heating Coil Reset Outdoor Dry-Bulb High. The default is FixedSetpoint.
+
+NOTE: The user must ensure that the cooling coil and heating coil setpoints do not overlap to avoid unwanted simultaneous heating and cooling. The simulation will not check this automatically. It is recommended that the cooling setpoint always be at least 0.1C higher than the heating coil setpoint.
+
+\paragraph{Field: Heating Coil Design Setpoint}\label{field-heating-coil-design-setpoint-5}
+
+Enter the heating supply air temperature in C to be used for sizing the heating coil and zone supply air flow rates. If Heating Coil Setpoint Control Type = FixedSetpoint, then this value is also used as the constant heating supply air setpoint temperature. The default is 12.2C.
+
+\paragraph{Field: Heating Coil Setpoint Schedule Name}\label{field-heating-coil-setpoint-schedule-name-4}
+
+This field is used when Heating Coil Setpoint Control Type = Scheduled. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the heating coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C.
+
+\paragraph{Field: Heating Coil Setpoint at Outdoor Dry-Bulb Low}\label{field-heating-coil-setpoint-at-outdoor-dry-bulb-low-2}
+
+The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Heating Coil Reset Outdoor Dry-Bulb Low). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.0C.
+
+\paragraph{Field: Heating Coil Reset Outdoor Dry-Bulb Low}\label{field-heating-coil-reset-outdoor-dry-bulb-low-2}
+
+The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 7.8C.
+
+\paragraph{Field: Heating Coil Setpoint at Outdoor Dry-Bulb High}\label{field-heating-coil-setpoint-at-outdoor-dry-bulb-high-2}
+
+The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Heating Coil Reset Outdoor Dry-Bulb High). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.2C.
+
+\paragraph{Field: Heating Coil Reset Outdoor Dry-Bulb High}\label{field-heating-coil-reset-outdoor-dry-bulb-high-2}
+
+The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb High. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.2C.
+
+\paragraph{Field: Gas Heating Coil Efficiency}\label{field-gas-heating-coil-efficiency-7}
+
+Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80\% efficient would have an entry of 0.8 here, which is the default. This field is only used when the heating coil type is set to gas.
+
+\paragraph{Field: Gas Heating Coil Parasitic Electric Load}\label{field-gas-heating-coil-parasitic-electric-load-7}
+
+Enter the parasitic electric load associated with the gas heating coil operation, such as a combustion fan. The units are in W. This field is only used when the heating coil type is set to gas.
+
+\paragraph{Field: Heat Recovery Type}\label{field-heat-recovery-type-8}
+
+Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
+
+\begin{itemize}
+\item
+  None
+\item
+  Sensible
+\item
+  Enthalpy
+\end{itemize}
+
+The default is None\emph{.}
+
+\paragraph{\texorpdfstring{Field: Heat Recovery Sensible Effectiveness {[]}}{Field: Heat Recovery Sensible Effectiveness }}\label{field-heat-recovery-sensible-effectiveness}
+
+Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
+
+\paragraph{\texorpdfstring{Field: Heat Recovery Latent Effectiveness {[]}}{Field: Heat Recovery Latent Effectiveness }}\label{field-heat-recovery-latent-effectiveness}
+
+Enter the latent heat recovery effectiveness if Heat Recovery Type is \emph{Enthalpy}. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
+
+\paragraph{Field: Heat Recovery Heat Exchanger Type}\label{field-heat-recovery-heat-exchanger-type-3}
+
+This alpha field denotes the type of heat exchanger being modeled: Plate (e.g., fixed plate) or Rotary (e.g., rotating cylinder or wheel). The default choice for this field is ``Plate''. The heat exchanger type affects the modeling of frost control options and supply air outlet temperature control. For rotary heat exchangers, rotational speed is varied to control frost formation or the supply air outlet temperature. For plate exchangers, air bypass around the heat exchanger is used to obtain the desired effect.
+
+\paragraph{Field: Heat Recovery Frost Control Type}\label{field-heat-recovery-frost-control-type-3}
+
+This alpha field has four choices: None, ExhaustAirRecirculation, ExhaustOnly and MinimumExhaustTemperature. If this field is left blank, the default frost control type is ``None''. For modeling preheat frost control, specify ``None'' for this input field and insert a separate heating coil object in the supply inlet air stream to keep the air temperature above the desired frost threshold temperature.
+
+\emph{ExhaustAirRecirculation}: dampers are used to direct exhaust air back into the zone through the supply side of the heat exchanger when the supply (outdoor) air inlet temperature falls below a threshold temperature. The fraction of time that exhaust air is circulated through the supply side of the heat exchanger is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When exhaust air is being recirculated, no supply (outdoor ventilation) air is being provided through the heat exchanger unit (which may or may not be acceptable regarding ventilation for occupants).
+
+\emph{ExhaustOnly (supply air bypass)}: this control cycles off the supply air flow through the heat exchanger for a certain period of time while the exhaust air continues to flow through the exhaust side of the heat exchanger. The fraction of time that the supply flow through the heat exchanger is cycled off is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When implemented in real applications, provisions are usually made to avoid building depressurization when this frost control is operating (automatic or pressure-operated dampers, or a bypass air damper around the supply side of the heat exchanger). For this frost control type, it is assumed that the supply air is bypassed around the heat exchanger during frost control operation (i.e., the total supply flow is not reduced during defrost, but merely bypassed around the heat exchanger).
+
+\emph{MinimumExhaustTemperature}: the temperature of the exhaust air leaving the heat exchanger is monitored and the heat exchanger effectiveness is decreased (by slowing heat exchanger rotation or bypassing supply air around the plate exchanger) to keep the exhaust air from falling below the threshold temperature.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-7}
+
+There are three dehumidification control type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  CoolReheatHeatingCoil
+\item
+  CoolReheatDesuperheater
+\item
+  Multimode
+\end{itemize}
+
+The \emph{CoolReheatHeatingCoil} option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so. Reheat is provided as required by the heating coil, if available.
+
+The \emph{CollReheatDesuperheater} option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so. Reheat is provided by a desuperheater coil (Ref. object Coil:Heating:Desuperheater). The desuperheater coil setpoint is set to the cooling setpoint and the desuperheater Heat Reclaim Recovery Efficiency is set to 0.3. \emph{CollReheatDesuperheater} is only applicable for Cooling Coil Type \emph{TwoSpeedDX, TwoStageDX, TwoStageHumidityControlDX, or HeatExchangerAssistedDX.}
+
+\emph{Multimode} is only applicable for cooling coil type \emph{TwoStageHumidityControlDX}. In this case, the enhanced dehumidification mode is activated as needed, but the system operates to meet the sensible dry-bulb temperature cooling setpoint.
+
+The default is \emph{None} which meets the sensible dry-bulb temperature cooling setpoint only.
+
+\paragraph{Field: Dehumidification Setpoint}\label{field-dehumidification-setpoint-4}
+
+This field specifies the supply air humidity ratio setpoint for dehumidification. The default is 0.00924 kgWater/kgDryAir (12.8C or 55F dewpoint). This value is also used as the Central Cooling Design Supply Air Humidity Ratio in the Sizing:System object. If a Dehumidification Setpoint Schedule Name is specified, the schedule will be used for control.
+
+\paragraph{Field: Humidifier Type}\label{field-humidifier-type-7}
+
+There are two humidifier type options available:
+
+\begin{itemize}
+\item
+  None
+\item
+  ElectricSteam
+\end{itemize}
+
+The \emph{ElectricSteam} humidifier option uses the Humidifier:Steam:Electric object. The default is \emph{None.}
+
+\paragraph{Field: Humidifier Availability Schedule Name}\label{field-humidifier-availability-schedule-name-7}
+
+If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period.
+
+\paragraph{Field: Humidifier Rated Capacity}\label{field-humidifier-rated-capacity-7}
+
+Enter the rated moisture output rate in m3/s. The humidifier does not currently autosize, so the default is very large to allow for adequate capacity. The default is 0.000001 m3/s.
+
+\paragraph{Field: Humidifier Rated Electric Power}\label{field-humidifier-rated-electric-power-7}
+
+Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
+
+\paragraph{Field: Humidifier Setpoint}\label{field-humidifier-setpoint-4}
+
+This field specifies the supply air humidity ratio setpoint for humidification. The default is 0.003 kgWater/kgDryAir. This value is also used as the Central Heating Design Supply Air Humidity Ratio in the Sizing:System object. If a Humidifier Setpoint Schedule Name is specified, the schedule will be used for control.
+
+\paragraph{Field: Dehumidification Setpoint Schedule Name}\label{field-dehumidification-setpoint-schedule-name}
+
+Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Setpoint, The values in the schedule are in units of humidity ratio (kgWater/kgDryAir or lbWater/lbDryAir).
+
+\paragraph{Field: Humidifier Setpoint Schedule Name}\label{field-humidifier-setpoint-schedule-name}
+
+Enter the name of the humidifier setpoint schedule. If this field is left blank, the setpoint will be constant at the Humidifier Setpoint, The values in the schedule are in units of humidity ratio (kgWater/kgDryAir or lbWater/lbDryAir).
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:System:DedicatedOutdoorAir,
+  DOAS,                    !- Name
+  ,                        !- System Availability Schedule Name
+  DirectIntoZone,          !- Air Outlet Type
+  autosize,                !- Supply Fan Flow Rate {m3/s}
+  0.7,                     !- Supply Fan Total Efficiency
+  1000,                    !- Supply Fan Delta Pressure {Pa}
+  0.9,                     !- Supply Fan Motor Efficiency
+  1,                       !- Supply Fan Motor in Air Stream Fraction
+  DrawThrough,             !- Supply Fan Placement
+  ChilledWater,            !- Cooling Coil Type
+  ,                        !- Cooling Coil Availability Schedule Name
+  FixedSetpoint,           !- Cooling Coil Setpoint Control Type
+  ,                        !- Cooling Coil Setpoint Schedule Name
+  12.8,                    !- Cooling Coil Design Setpoint {C}
+  15.6,                !- Cooling Coil Setpoint at Outdoor Dry-Bulb Low {C}
+  15.6,                    !- Cooling Coil Reset Outdoor Dry-Bulb Low {C}
+  12.8,               !- Cooling Coil Setpoint at Outdoor Dry-Bulb High {C}
+  23.3,                    !- Cooling Coil Reset Outdoor Dry-Bulb High {C}
+  autosize,           !- DX Cooling Coil Gross Rated Total Capacity {W}
+  autosize,           !- DX Cooling Coil Gross Rated Sensible Heat Ratio
+  3,                       !- DX Cooling Coil Gross Rated COP
+  HotWater,                !- Heating Coil Type
+  ,                        !- Heating Coil Availability Schedule Name
+  FixedSetpoint,           !- Heating Coil Setpoint Control Type
+  ,                        !- Heating Coil Setpoint Schedule Name
+  12.2,                    !- Heating Coil Design Setpoint {C}
+  15,                  !- Heating Coil Setpoint at Outdoor Dry-Bulb Low {C}
+  7.8,                     !- Heating Coil Reset Outdoor Dry-Bulb Low {C}
+  12.2,               !- Heating Coil Setpoint at Outdoor Dry-Bulb High {C}
+  12.2,                    !- Heating Coil Reset Outdoor Dry-Bulb High {C}
+  0.8,                     !- Gas Heating Coil Efficiency
+  ,                        !- Gas Heating Coil Parasitic Electric Load {W}
+  Enthalpy,                !- Heat Recovery Type
+  0.7,                     !- Sensible Heat Recovery Effectiveness
+  0.65,                    !- Latent Heat Recovery Effectiveness
+  Plate,                   !- Heat Exchanger Type
+  None,                    !- Frost Control Type
+  None,                    !- Dehumidification Control Type
+  0.00924,                 !- Dehumidification Setpoint {kgWater/kgDryAir}
+  None,                    !- Humidifier Type
+  ,                        !- Humidifier Availability Schedule Name
+  0.000001,                !- Humidifier Rated Capacity {m3/s}
+  2690,                    !- Humidifier Rated Electric Power {W}
+  0.003,                   !- Humidifier Setpoint {kgWater/kgDryAir}
+  ,                        !- Dehumidification Setpoint Schedule Name
+  ;                        !- Humidifier Setpoint Schedule Name
+\end{lstlisting}
+
+\subsection{HVACTemplate:Plant:ChilledWaterLoop}\label{hvactemplateplantchilledwaterloop}
+
+The piping systems that connect the chilled water coils in the HVAC template objects with the chillers and the cooling towers (if present) are described with this object. The piping systems are called loops and this object describes the controls and pumps on the loops. Only one of these objects may be defined in an input file and all chilled water coils from HVAC template objects are served with this object.
+
+\subsubsection{Inputs}\label{inputs-23-001}
+
+\paragraph{Field: Name}\label{field-name-10-007}
+
+The name used to designate the HVACTemplate:Plant:ChilledWaterLoop.
+
+\paragraph{Field: Pump Schedule Name}\label{field-pump-schedule-name}
+
+Leave this field blank if the chilled water and condenser water pumps are always available. If a schedule name is specified, those times that the pumps are available should be specified as 1.0. Those times that the pumps are not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the system is providing chilled water to the coils but a schedule of when it can provide chilled water to the coils.
+
+\paragraph{Field: Pump Control Type}\label{field-pump-control-type}
+
+Applies to both chilled water and condenser loop pumps. The choices for this field are:
+
+\begin{itemize}
+\item
+  Intermittent
+\item
+  Continuous
+\end{itemize}
+
+The default value is Intermittent.
+
+If the pump control type is \textbf{Continuous}, the pump will run according to the Pump Schedule (see above) regardless of whether or not there is a load. If the pump control type is \textbf{Intermittent}, the pump will run if a load is sensed and will shut off if there is no load on the loop.
+
+\paragraph{Field: Chiller Plant Operation Scheme Type}\label{field-chiller-plant-operation-scheme-type}
+
+The choices for this field are:
+
+\begin{itemize}
+\item
+  Default
+\item
+  UserDefined
+\end{itemize}
+
+Default operation type makes all equipment available at all times operating in order of Priority specified in HVACTemplate:Plant:Chiller objects. If a different scheme is to be used to sequence the chillers, then this entry should be set to User Defined. If the User Defined option is chosen, then additional EnergyPlus objects must be included and completely defined in the IDF file such as shown below depending on the type of plant operation control scheme chosen:
+
+\begin{itemize}
+\item
+  PlantEquipmentOperationSchemes
+\item
+  PlantEquipmentOperation:CoolingLoad
+\item
+  PlantEquipmentList (refer to HVACTemplate:Plant:Chiller object description for chiller key name required in this object).
+\end{itemize}
+
+The default value is Default.
+
+\paragraph{Field: Chiller Plant Equipment Operation Schemes Name}\label{field-chiller-plant-equipment-operation-schemes-name}
+
+This field should contain the name of a PlantEquipmentOperationSchemes object only when the previous field is set to UserDefined. It is ignored if Chiller Plant Operation Scheme Type is Default.
+
+\paragraph{Field: Chilled Water Setpoint Schedule Name}\label{field-chilled-water-setpoint-schedule-name}
+
+Enter the name of a chilled water setpoint schedule that has values that change at different times of the year. If a constant set point is needed simply leave this field blank and the value in the next field will be used at all times. The values in the schedule are in degrees C. This field is ignored if the Chilled Water Setpoint Reset Type is something other than None.
+
+\paragraph{Field: Chilled Water Design Setpoint}\label{field-chilled-water-design-setpoint}
+
+Enter the chilled water setpoint temperature to be used for sizing the chilled water loop and associated equipment in degrees C. If the Chilled Water Setpoint Schedule is blank and the Chilled Water Setpoint Reset Type is \emph{None}, then this value will be used as the setpoint at all times.
+
+\paragraph{Field: Chilled Water Pump Configuration}\label{field-chilled-water-pump-configuration}
+
+The choices for this field are
+
+\begin{itemize}
+\item
+  VariablePrimaryNoSecondary -- variable flow to chillers and coils
+\item
+  ConstantPrimaryNoSecondary -- constant flow to chillers and coils with bypass
+\item
+  ConstantPrimaryVariableSecondary -- constant flow to chillers with bypass, variable flow to coils
+\item
+  VariablePrimaryConstantSecondary -- variable flow to chillers, constant flow to coils with bypass
+\end{itemize}
+
+The default value is ConstantPrimaryNoSecondary.
+
+The operation of a constant speed pump is fairly straightforward. If the user designates a constant speed pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump is constant speed and operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop.
+
+A variable speed pump is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump is operating intermittently, then the pump can shutdown. For any other condition such as the loop having a load and the pump is operating intermittently or the pump is continuously operating (regardless of the loading condition), the pump will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump is running, it will try to meet the flow request made by demand side components.
+
+\paragraph{Field: Primary Chilled Water Pump Rated Head}\label{field-primary-chilled-water-pump-rated-head}
+
+The rated head of the primary chilled water pump in Pa. The default value is 179352 Pa which is equivalent to 60 feet H2O.
+
+\paragraph{Field: Secondary Chilled Water Pump Rated Head}\label{field-secondary-chilled-water-pump-rated-head}
+
+The rated head of the secondary chilled water pump in Pa. The default value is 179352 Pa which is equivalent to 60 feet H\(_{2}\)O. This field is applicable only if the ``Chilled Water Pump Configuration'' is \emph{Constant Primary Variable Secondary} or \emph{Variable Primary Constant Secondary}.
+
+\paragraph{Field: Condenser Plant Operation Scheme Type}\label{field-condenser-plant-operation-scheme-type}
+
+The choices for this field are:
+
+\begin{itemize}
+\item
+  Default
+\item
+  UserDefined
+\end{itemize}
+
+Default operation type makes all equipment available at all times operating in order of Priority specified in HVACTemplate:Plant:Tower objects. If a different scheme is to be used to sequence the towers, then this entry should be set to User Defined. May be left blank if not serving any water cooled chillers.
+
+If User Defined option is chosen, then additional EnergyPlus objects must be included and completely defined in the IDF file such as shown below depending on the type of condenser operation control scheme chosen:
+
+\begin{itemize}
+\item
+  CondenserEquipmentOperationSchemes
+\item
+  PlantEquipmentOperation:CoolingLoad
+\item
+  PlantEquipmentList (refer to the HVACTemplate:Plant:Tower object description for key name required for this object.
+\end{itemize}
+
+The default value is Default.
+
+\paragraph{Field: Condenser Equipment Operation Schemes Name}\label{field-condenser-equipment-operation-schemes-name}
+
+This field should contain the name of a CondenserEquipmentOperationSchemes object only when the previous field is set to UserDefined. It is ignored if Condenser Plant Operation Scheme Type is Default. May be left blank if not serving any water cooled chillers.
+
+\paragraph{Field: Condenser Water Temperature Control Type}\label{field-condenser-water-temperature-control-type}
+
+If water cooled chillers are present the condenser water temperature control can be one of the following options:
+
+\begin{itemize}
+\item
+  OutdoorWetBulbTemperature
+\item
+  SpecifiedSetpoint
+\end{itemize}
+
+If a specified set point is used then the towers are operated to deliver that condenser water set point. If outdoor wet-bulb is used then the condenser water temperature decreases with decreasing outdoor wet-bulb temperature. May be left blank if not serving any water cooled chillers.
+
+\paragraph{Field: Condenser Water Setpoint Schedule Name}\label{field-condenser-water-setpoint-schedule-name}
+
+Used when Condenser Water Temperature Control Type is set to Specified Setpoint. Ignored if Condenser Water Temperature Control Type is set to Outdoor Wet-bulb. The field may be left blank if constant setpoint temperature is used for the condenser water temperature. If may also be left blank if not serving any water cooled chillers. If specified, the schedule should contain the set point temperatures in degrees C for the condenser water loop.
+
+\paragraph{Field: Condenser Water Design Setpoint}\label{field-condenser-water-design-setpoint}
+
+\begin{itemize}
+\tightlist
+\item
+  Enter the condenser water temperature to be used for sizing the condenser loop and associated equipment. If a constant setpoint control is used for the condenser water, this value will be used as the setpoint at all times. May be left blank if not serving any water cooled chillers. Used when Condenser Water Temperature Control Type is set to Specified Setpoint. Ignored if Condenser Water Temperature Control Type is set to OutdoorWetBulbTemperature. The units are in C.
+\end{itemize}
+
+\paragraph{Field: Condenser Water Pump Rated Head}\label{field-condenser-water-pump-rated-head}
+
+The rated head of the condenser water pumps in Pa. May be left blank if not serving any water cooled chillers. The default value is 179352 Pa which is equivalent to 60 feet H2O.
+
+\paragraph{Field: Chilled Water Setpoint Reset Type}\label{field-chilled-water-setpoint-reset-type}
+
+Select the type of automatic reset control for the chilled water supply temperature. The choices are:
+
+\begin{itemize}
+\item
+  None -- no reset, use the Chilled Water Setpoint Schedule or Chilled Water Design Setpoint.
+\item
+  OutdoorAirTemperatureReset -- reset the chilled water supply temperature based on the following default rules. The temperature limits and setpoints are specified using the fields below. If the default values are used, when the outdoor dry-bulb temperature (ODB) is at or below 15.6C the setpoint is 12.2C. When the ODB is at or above 26.7C the setpoint is 6.7C. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset)
+\end{itemize}
+
+The default is \emph{None}.
+
+\paragraph{Field: Chilled Water Setpoint at Outdoor Dry-Bulb Low}\label{field-chilled-water-setpoint-at-outdoor-dry-bulb-low}
+
+The chilled water setpoint temperature in C when the outdoor dry-bulb is at or below the low limit (Chilled Water Reset Outdoor Dry Bulb Low). The default is 12.2C.
+
+\paragraph{Field: Chilled Water Reset Outdoor Dry-Bulb Low}\label{field-chilled-water-reset-outdoor-dry-bulb-low}
+
+The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Chilled Water Setpoint at Outdoor Dry Bulb Low. The default is 15.6C.
+
+\paragraph{Field: Chilled Water Setpoint at Outdoor Dry-Bulb High}\label{field-chilled-water-setpoint-at-outdoor-dry-bulb-high}
+
+The chilled water setpoint temperature in C when the outdoor dry-bulb is at or above the high limit (Chilled Water Reset Outdoor Dry Bulb Low). The default is 6.7C.
+
+\paragraph{Field: Chilled Water Reset Outdoor Dry-Bulb High}\label{field-chilled-water-reset-outdoor-dry-bulb-high}
+
+The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Chilled Water Setpoint at Outdoor Dry Bulb High. The default is 26.7C.
+
+\paragraph{Field: Chilled Water Primary Pump Type}\label{field-chilled-water-primary-pump-type}
+
+Describes the type of pump configuration used for the primary portion of the chilled water loop. The options include:
+
+\begin{itemize}
+\item
+  SinglePump
+\item
+  PumpPerChiller
+\item
+  TwoHeaderedPumps
+\item
+  ThreeHeaderedPumps
+\item
+  FourHeaderedPumps
+\item
+  FiveHeaderedPumps
+\end{itemize}
+
+\paragraph{Field: Chilled Water Secondary Pump Type}\label{field-chilled-water-secondary-pump-type}
+
+Describes the type of pump configuration used for the secondary portion of the chilled water loop. The options include:
+
+\begin{itemize}
+\item
+  SinglePump
+\item
+  TwoHeaderedPumps
+\item
+  ThreeHeaderedPumps
+\item
+  FourHeaderedPumps
+\item
+  FiveHeaderedPumps
+\end{itemize}
+
+\paragraph{Field: Condenser Water Pump Type}\label{field-condenser-water-pump-type}
+
+Describes the type of pump configuration used for the condenser water loop. The options include:
+
+\begin{itemize}
+\item
+  SinglePump
+\item
+  PumpPerTower
+\item
+  TwoHeaderedPumps
+\item
+  ThreeHeaderedPumps
+\item
+  FourHeaderedPumps
+\item
+  FiveHeaderedPumps
+\end{itemize}
+
+\paragraph{Field: Chilled Water Supply Side Bypass Pipe}\label{field-chilled-water-supply-side-bypass-pipe}
+
+The field determines if a supply side bypass pipe is present in the chilled water loop. The choices for this field are
+
+\begin{itemize}
+\item
+  Yes
+\item
+  No.
+\end{itemize}
+
+\paragraph{Field: Chilled Water Demand Side Bypass Pipe}\label{field-chilled-water-demand-side-bypass-pipe}
+
+The field determines if a demand side bypass pipe is present in the chilled water loop. The choices for this field are
+
+\begin{itemize}
+\item
+  Yes
+\item
+  No.
+\end{itemize}
+
+\paragraph{Field: Condenser Water Supply Side Bypass Pipe}\label{field-condenser-water-supply-side-bypass-pipe}
+
+The field determines if a supply side bypass pipe is present in the condenser water loop. The choices for this field are
+
+\begin{itemize}
+\item
+  Yes
+\item
+  No.
+\end{itemize}
+
+\paragraph{Field: Condenser Water Demand Side Bypass Pipe}\label{field-condenser-water-demand-side-bypass-pipe}
+
+The field determines if a demand side bypass pipe is present in the condenser water loop. The choices for this field are
+
+\begin{itemize}
+\item
+  Yes
+\item
+  No.
+\end{itemize}
+
+\paragraph{Field: Fluid Type}\label{field-fluid-type-000}
+
+This field determines the type of fluid used for the boiler loop. The following options are available:
+
+\begin{itemize}
+\item
+  Water
+\item
+  EthyleneGlycol30
+\item
+  EthyleneGlycol40
+\item
+  EthyleneGlycol50
+\item
+  EthyleneGlycol60
+\item
+  PropyleneGlycol30
+\item
+  PropyleneGlycol40
+\item
+  PropyleneGlycol50
+\item
+  PropyleneGlycol60
+\end{itemize}
+
+\paragraph{Field: Loop Design Delta Temperature}\label{field-loop-design-delta-temperature}
+
+The temperature difference used in sizing the loop flow rate. The default is 6.67C.
+
+\paragraph{Field: Minimum Outdoor Dry Bulb Temperature}\label{field-minimum-outdoor-dry-bulb-temperature}
+
+The minimum outdoor dry bulb temperature that the chilled water loops operate.
+
+\paragraph{Field: Chilled Water Load Distribution Scheme}\label{field-chilled-water-load-distribution-scheme}
+
+The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. \textbf{Optimal} operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{SequentialLoad} loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{UniformLoad} evenly distributes the loop demand among all available components on the equipment list for a given load range. \textbf{SequentialUniformPLR} loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. \textbf{UniformPLR} will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
+
+Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
+
+\paragraph{Field: Condenser Water Load Distribution Scheme}\label{field-condenser-water-load-distribution-scheme}
+
+The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. \textbf{Optimal} operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{SequentialLoad} loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{UniformLoad} evenly distributes the loop demand among all available components on the equipment list for a given load range. \textbf{SequentialUniformPLR} loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. \textbf{UniformPLR} will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
+
+Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Plant:ChilledWaterLoop,
+  Chilled Water Loop,      !- Plant Loop Name
+  CoolingPumpAvailSched,   !- Pump Schedule
+  Intermittent,            !- Pump Control Type
+  Default,                 !- Chiller Plant Operation Scheme Type
+  ,                        !- Chiller Plant Operation Scheme Name
+  CW Loop Temp Schedule,   !- Chilled Water Setpoint Schedule
+  7.22,                    !- Chilled Water Design Setpoint {C}
+  VariableFlowNoSecondary, !- Chilled Water Pump Configuration
+  179352,                  !- Primary Chilled Water Pump Rated Head {Pa}
+  179352,                  !- Secondary Chilled Water Pump Rated Head {Pa}
+  Default,                 !- Condenser Plant Operation Scheme Type
+  ,                        !- Condenser Plant Operation Scheme List Name
+  OutdoorWetBulbTemperature,    !- Condenser Water Temperature Control Type
+  ,                        !- Condenser Water Setpoint Schedule
+  29.4,                    !- Condenser Water Design Setpoint {C}
+  179352,                  !- Condenser Water Pump Rated Head {Pa}
+  None,                    !- Chilled Water Setpoint Reset Type
+  12.2,              !- Chilled Water Setpoint at Outdoor Dry Bulb Low {C}
+  15.6,              !- Chilled Water Reset Outdoor Dry Bulb Low {C}
+  6.7,               !- Chilled Water Setpoint at Outdoor Dry Bulb High {C}
+  26.7,              !- Chilled Water Reset Outdoor Dry Bulb High {C}
+  SinglePump,              !- Chilled Water Primary Pump Type
+  SinglePump,              !- Chilled Water Secondary Pump Type
+  SinglePump,              !- Condenser Water Pump Type
+  Yes,                     !- Chilled Water Supply Side Bypass Pipe
+  Yes,                     !- Chilled Water Demand Side Bypass Pipe
+  Yes,                     !- Condenser Water Supply Side Bypass Pipe
+  Yes,                     !- Condenser Water Demand Side Bypass Pipe
+  Water,                   !- Fluid Type
+  6.67,                    !- Loop Design Delta Temperature {deltaC}
+  ,                        !- Minimum Outdoor Dry Bulb Temperature {C}
+  SequentialLoad,          !- Chilled Water Load Distribution Scheme
+  SequentialLoad;          !- Condenser Water Load Distribution Scheme
+\end{lstlisting}
+
+\subsection{HVACTemplate:Plant:Chiller}\label{hvactemplateplantchiller}
+
+A chiller or purchased cooling source is described with this object. To define multiple chillers, use multiple HVACTemplate:Plant:Chiller objects and use the Sizing Factor field to apportion the total capacity if autosizing.
+
+\subsubsection{Inputs}\label{inputs-24-000}
+
+\paragraph{Field: Name}\label{field-name-11-005}
+
+The name used to reference the HVACTemplate:Plant:Chiller object.
+
+\paragraph{Field: Chiller Type}\label{field-chiller-type}
+
+While EnergyPlus has a variety of chiller options, the only choices currently for this field are:
+
+\begin{itemize}
+\item
+  DistrictChilledWater
+\item
+  ElectricCentrifugalChiller
+\item
+  ElectricScrewChiller
+\item
+  ElectricReciprocatingChiller
+\end{itemize}
+
+The EnergyPlus equipment object types which are used are DistrictCooling or Chiller:Electric:EIR. These equipment type keys must be used if setting up a user-defined chiller plant operation scheme.
+
+\paragraph{Field: Capacity}\label{field-capacity}
+
+This field may be set to autosize, which means that the capacity is based on the peak loads during the design days. This numeric field contains the design cooling capacity of the chiller. This capacity should be at the design temperatures and water flow rates. The units are in W.
+
+\paragraph{Field: Nominal COP}\label{field-nominal-cop}
+
+This numeric field contains the chiller's coefficient of performance. This value should \textbf{not} include energy use due to pumps, evap-cooled or air-cooled condenser fans, or cooling tower fans. This Nominal COP should be at the design temperatures and water flow rates. Not applicable if Chiller Type is DistrictChilledWater.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-1-000}
+
+The choices for this field are
+
+\begin{itemize}
+\item
+  AirCooled
+\item
+  WaterCooled
+\item
+  EvaporativelyCooled
+\end{itemize}
+
+The default value is WaterCooled. If WaterCooled, then at least one HVACTemplate:Plant:Tower object should be defined. Not applicable if Chiller Type is Purchased Chilled Water.
+
+\paragraph{Field: Priority}\label{field-priority}
+
+Enter the priority number of the chiller where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Chiller Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:ChilledWaterLoop. Equipment is operated in order of the priority number. This allows multiple chillers to be sequenced.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-000}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the chiller object inputs that would be altered by the sizing factor are: Reference Capacity, Reference Chilled Water Flow Rate and Reference Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-000}
+
+This numeric field contains the chiller's minimum part-load ratio. The expected range is between 0 and 1. Below this part-load ratio, the compressor cycles on and off to meet the cooling load. The Minimum Part Load Ratio must be less than or equal to the Maximum Part Load Ratio. The default value is 0.0.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-000}
+
+This numeric field contains the chiller's maximum part-load ratio. This value may exceed 1, but the normal range is between 0.0 and 1.0. The Maximum Part Load Ratio must be greater than or equal to the Minimum Part Load Ratio. The default value is 1.0.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-000}
+
+This numeric field contains the chiller's optimum part-load ratio. This is the part-load ratio at which the chiller performs at its maximum COP. The optimum part-load ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 1.0.
+
+\paragraph{Field: Minimum Unloading Ratio}\label{field-minimum-unloading-ratio}
+
+This numeric field contains the chiller's minimum unloading ratio. The expected range is between 0 and 1. The minimum unloading ratio is where the chiller capacity can no longer be reduced by unloading and must be false loaded to meet smaller cooling loads. A typical false loading strategy is hot-gas bypass. The minimum unloading ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 0.25.
+
+\paragraph{Field: Leaving Chilled Water Lower Temperature Limit}\label{field-leaving-chilled-water-lower-temperature-limit}
+
+This numeric field contains the lower limit for the leaving chilled water temperature in Celsius. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn't get too cold. The default value is 5ËšC.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Plant:Chiller,
+  District Cooling,        !- Chiller Name
+  ElectricCentrifugalChiller,  !- Chiller Type
+  autosize,                !- Capacity {W}
+  3.2,                     !- COP
+  WaterCooled,             !- Condenser Type
+  1,                       !- Priority
+  1,                       !- Sizing Factor
+  0.1,                     !- Minimum Part Load Ratio
+  1.1,                     !- Maximum Part Load Ratio
+  0.9,                     !- Optimum Part Load Ratio
+  0.2,                     !- Minimum Unloading Ratio
+  2;                 !- Leaving Chilled Water Lower Temperature Limit {C}
+\end{lstlisting}
+
+\subsection{HVACTemplate:Plant:Chiller:ObjectReference}\label{hvactemplateplantchillerobjectreference}
+
+This object references a detailed chiller object and adds it to an HVACTemplate:Plant:ChilledWaterLoop. The user must create a complete detailed chiller object with all required curve or performance objects. The detailed chiller object is referenced by object type and name and the chiller will be automatically to the chilled water loop branches and equipment list.
+
+\subsubsection{Inputs}\label{inputs-25-000}
+
+\paragraph{Field: Name}\label{field-name-12-004}
+
+The name of this object.
+
+\paragraph{Field: Chiller Object Type}\label{field-chiller-object-type}
+
+The object type of the referenced chiller. Select from one of the following supported chiller object types:
+
+\begin{itemize}
+\item
+  Chiller:Electric:EIR
+\item
+  Chiller:Electric:ReformulatedEIR
+\end{itemize}
+
+\paragraph{Field: Chiller Name}\label{field-chiller-name}
+
+The object name of the referenced chiller.
+
+\paragraph{Field: Priority}\label{field-priority-1}
+
+Enter the priority number of the chiller where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Chiller Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:ChilledWaterLoop. Equipment is operated in order of the priority number. This allows multiple chillers to be sequenced.
+
+An example in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Plant:Chiller:ObjectReference,
+  Main Chiller Connection, !- Name
+  Chiller:Electric:EIR,    !- Chiller Object Type
+  Main Chiller,            !- Chiller Name
+  1;                       !- Priority
+\end{lstlisting}
+
+\subsection{HVACTemplate:Plant:Tower}\label{hvactemplateplanttower}
+
+A cooling tower is described with this object. To define multiple cooling towers, use multiple HVACTemplate:Plant:Tower objects and use the Sizing Factor field to apportion the total capacity if autosizing.
+
+\subsubsection{Inputs}\label{inputs-26-000}
+
+\paragraph{Field: Name}\label{field-name-13-004}
+
+The name used to reference the HVACTemplate:Plant:Tower object.
+
+\paragraph{Field: Tower Type}\label{field-tower-type}
+
+The choices for this field are
+
+\begin{itemize}
+\item
+  SingleSpeed
+\item
+  TwoSpeed
+\end{itemize}
+
+The EnergyPlus equipment object types which are used are CoolingTower:SingleSpeed or CoolingTower:TwoSpeed. These equipment type keys must be used if setting up a user-defined condenser plant operation scheme.
+
+\paragraph{Field: High-Speed Nominal Capacity}\label{field-high-speed-nominal-capacity-000}
+
+Applicable for Tower Type Single Speed and Two Speed. This field may be set to autosize. If this field is set to autosize, then the Low-Speed Nominal Capacity and the Free Convection Capacity must also be autosized. The units are W. This numeric input field contains the ``nominal'' heat rejection capacity of the cooling tower in watts under high-speed fan operation, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of high-speed nominal capacity (3 gpm/ton). 125\% of this nominal tower capacity gives the actual tower heat rejection at these operating conditions (based on historical assumption that the tower must dissipate 0.25W of compressor heat for every watt of heat removed by the evaporator).
+
+\paragraph{Field: High-Speed Fan Power}\label{field-high-speed-fan-power}
+
+The tower fan electric consumption when at high speed. Applicable for Tower Type Single Speed and Two Speed. This field may be set to autosize. The units are W.
+
+\paragraph{Field: Low-Speed Nominal Capacity}\label{field-low-speed-nominal-capacity-000}
+
+Applicable only for Tower Type Two Speed. This field may be set to autosize. If this field is set to autosize, then the High-Speed Nominal Capacity and the Free Convection Capacity must also be autosized. The units are W. This numeric input field contains the ``nominal'' heat rejection capacity of the cooling tower in watts under low-speed fan operation, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of high-speed nominal tower capacity (input field above). 125\% of this nominal tower capacity gives the actual tower heat rejection at these operating conditions (based on historical assumption that the tower must dissipate 0.25W of compressor heat for every watt of heat removed by the evaporator). The value specified for this field must be greater than zero but less than the value specified for the field ``Tower High-Speed Nominal Capacity''.
+
+\paragraph{Field: Low-Speed Fan Power}\label{field-low-speed-fan-power}
+
+The tower fan electric consumption when at low speed. Applicable only for Tower Type Two Speed. This field may be set to autosize. The units are W.
+
+\paragraph{Field: Free Convection Capacity}\label{field-free-convection-capacity-000}
+
+Applicable for Tower Type Single Speed and Two Speed. This field may be set to autosize. If this field is set to autosize, then the High-Speed Nominal Capacity and the Low-Speed Nominal Capacity must also be autosized. The units are W. This numeric input field contains the ``nominal'' heat rejection capacity of the cooling tower in watts when the tower is in the ``free convection'' regime (water flow exists but tower fan is turned off), with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of high-speed nominal tower capacity (input field above). 125\% of this free convection tower capacity gives the actual tower heat rejection at these operating conditions (based on historical assumption that the tower must dissipate 0.25W of compressor heat for every watt of heat removed by the evaporator). If the user does not wish to model ``free convection'', then this field should be set to 0.0.
+
+\paragraph{Field: Priority}\label{field-priority-2}
+
+Enter the priority number of the tower where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Condenser Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:ChilledWaterLoop or HVACTemplate:Plant:MixedWaterLoop. Equipment is operated in order of the priority number. This allows multiple towers to be sequenced.
+
+\textbf{\emph{Field: Sizing Factor}}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.For this component the tower object inputs that would be altered by the sizing factor are:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Design Water Flow Rate;
+\item
+  Air Flow Rate at High Fan Speed;
+\item
+  Fan Power at High Fan Speed;
+\item
+  U-Factor Times Area Value at High Fan Speed;
+\item
+  Air Flow Rate at Low Fan Speed (for two-speed tower);
+\item
+  Fan Power at Low Fan Speed (for two-speed tower);
+\item
+  U-Factor Times Area Value at Low Fan Speed (for two-speed tower);
+\item
+  Air Flow Rate in Free Convection Regime;
+\item
+  U-Factor Times Area Value at Free Convection Air Flow Rate.
+\end{enumerate}
+
+Note that the U-Factor Times Area Value at High Fan Speed is not \emph{multiplied} by the Sizing Factor. Instead the design tower load is multiplied by the sizing factor and the design UA then calculated as usual. The U-Factor Times Area Value at Low Fan Speed is set to 60\% of the full load design UA. The U-Factor Times Area Value at Free Convection Air Flow Rate is set to 10\% of the design Tower UA.
+
+\paragraph{Field: Template Plant Loop Type}\label{field-template-plant-loop-type}
+
+This field specifies whether this tower will serve a \emph{ChilledWaterLoop} (ref. HVACTemplate:Plant:ChilledWaterLoop) or a \emph{MixedWaterLoop} (ref. HVACTemplate:Plant:MixedWaterLoop). If this field is left blank, this tower will serve a ChilledWaterLoop if present or a MixedWaterLoop (if no ChilledWaterLoop is present).
+
+An example in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Plant:Tower,
+  Main Tower,              !- Name
+  SingleSpeed,             !- Tower Type
+  autosize,                !- High Speed Nominal Capacity {W}
+  autosize,                !- High Speed Fan Power {W}
+  autosize,                !- Low Speed Nominal Capacity {W}
+  autosize,                !- Low Speed Fan Power {W}
+  autosize,                !- Free Convection Capacity {W}
+  1,                       !- Priority
+  ;                        !- Sizing Factor
+\end{lstlisting}
+
+\subsection{HVACTemplate:Plant:Tower:ObjectReference}\label{hvactemplateplanttowerobjectreference}
+
+This object references a detailed cooling tower object and adds it to an HVACTemplate:Plant:ChilledWaterLoop or MixedWaterLoop. The user must create a complete detailed cooling tower object with all required curve or performance objects. The detailed cooling tower object is referenced by object type and name and the tower will be automatically to the chilled water loop or mixed water loop branches and equipment list.
+
+\subsubsection{Inputs}\label{inputs-27-000}
+
+\paragraph{Field: Name}\label{field-name-14-003}
+
+The name of this object.
+
+\paragraph{Field: Cooling Tower Object Type}\label{field-cooling-tower-object-type}
+
+The object type of the referenced tower. Select from one of the following supported tower object types:
+
+\begin{itemize}
+\item
+  CoolingTower:SingleSpeed
+\item
+  CoolingTower:TwoSpeed
+\item
+  CoolingTower:VariableSpeed
+\end{itemize}
+
+\paragraph{Field: Cooling Tower Name}\label{field-cooling-tower-name}
+
+The object name of the referenced tower.
+
+\paragraph{Field: Priority}\label{field-priority-3}
+
+Enter the priority number of the tower where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Condenser Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:ChilledWaterLoop or MixedWaterLoop. Equipment is operated in order of the priority number. This allows multiple towers to be sequenced.
+
+\paragraph{Field: Template Plant Loop Type}\label{field-template-plant-loop-type-1}
+
+This field specifies whether this tower will serve a \emph{ChilledWaterLoop} (ref. HVACTemplate:Plant:ChilledWaterLoop) or a \emph{MixedWaterLoop} (ref. HVACTemplate:Plant:MixedWaterLoop). If this field is left blank, this tower will serve a ChilledWaterLoop if present or a MixedWaterLoop (if no ChilledWaterLoop is present).
+
+An example in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Plant:Tower:ObjectReference,
+  Main Tower Connection,   !- Name
+  CoolingTower:TwoSpeed,   !- Cooling Tower Object Type
+  Main Tower,              !- Cooling Tower Name
+  1;                       !- Priority
+\end{lstlisting}
+
+\subsection{HVACTemplate:Plant:HotWaterLoop}\label{hvactemplateplanthotwaterloop}
+
+The piping systems that connect the hot water coils in the HVAC template objects with the boilers are described with this object. The piping systems are called loops and this object describes the controls and pumps on the loops. Only one of these objects should be defined in an input file and all hot water coils from HVAC template objects are served with this object.
+
+\subsubsection{Inputs}\label{inputs-28-000}
+
+\paragraph{Field: Name}\label{field-name-15-003}
+
+The name used to designate the HVACTemplate:Plant:HotWaterLoop.
+
+\paragraph{Field: Pump Schedule Name}\label{field-pump-schedule-name-1}
+
+Leave this field blank if the hot water pump is always available. If a schedule name is specified, those times that the pump is available should be specified as 1.0. Those times that the pump is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the system is providing hot water to the coils but a schedule of when it can provide hot water to the coils.
+
+\paragraph{Field: Pump Control Type}\label{field-pump-control-type-1}
+
+The choices for this field are
+
+\begin{itemize}
+\item
+  Intermittent
+\item
+  Continuous
+\end{itemize}
+
+The default value is Intermittent.
+
+If the pump control type is \textbf{Continuous}, the pump will run according to the Pump Schedule (see above) regardless of whether or not there is a load. If the pump control type is \textbf{Intermittent}, the pump will run if a load is sensed and will shut off if there is no load on the loop.
+
+\paragraph{Field: Hot Water Plant Operation Scheme Type}\label{field-hot-water-plant-operation-scheme-type}
+
+The choices for this field are:
+
+\begin{itemize}
+\item
+  Default
+\item
+  UserDefined
+\end{itemize}
+
+Default operation type makes all equipment available at all times operating in order of Priority specified in HVACTemplate:Plant:Boiler objects. If a different scheme is to be used to sequence the boilers, then this entry should be set to User Defined.
+
+If User Defined option is chosen, then additional EnergyPlus objects must be defined in the IDF file such as shown below depending on the type of plant operation control scheme chosen:
+
+\begin{itemize}
+\item
+  PlantEquipmentOperationSchemes
+\item
+  PlantEquipmentOperation:HeatingLoad
+\item
+  PlantEquipmentList (refer to HVACTemplate:Plant:Boiler object description for key name required in this object)
+\end{itemize}
+
+The default value is Default.
+
+\paragraph{Field: Hot Water Plant Equipment Operation Schemes Name}\label{field-hot-water-plant-equipment-operation-schemes-name}
+
+This field should contain the name of a PlantEquipmentOperationSchemes object only when the previous field is set to User Defined. It is ignored if Hot Water Plant Operation Scheme Type is Default.
+
+\paragraph{Field: Hot Water Setpoint Schedule Name}\label{field-hot-water-setpoint-schedule-name}
+
+Enter the name of a hot water setpoint schedule that has values that change at different times of the year. If a constant set point is needed simply leave this field blank and the value in the next field will be used at all times. The values in the schedule are in degrees C. This field is ignored if the Hot Water Setpoint Reset Type is something other than None.
+
+\paragraph{Field: Hot Water Design Setpoint}\label{field-hot-water-design-setpoint}
+
+Enter the hot water setpoint temperature to be used for sizing the hot water loop and associated equipment in degrees C. If the Hot Water Setpoint Schedule is blank and the Hot Water Setpoint Reset Type is \emph{None}, then this value will be used as the setpoint at all times.
+
+\paragraph{Field: Hot Water Pump Configuration}\label{field-hot-water-pump-configuration}
+
+The choices for this field are
+
+\begin{itemize}
+\item
+  VariableFlow
+\item
+  ConstantFlow
+\end{itemize}
+
+The default value is ConstantFlow. The variable flow option simulates a pump with variable flow to boilers and coils, excess bypassed. The constant flow option simulates constant flow to boilers and coils, excess bypassed.
+
+The operation of a constant speed pump is fairly straightforward. If the user designates a constant speed pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump is constant speed and operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop.
+
+A variable speed pump is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump is operating intermittently, then the pump can shutdown. For any other condition such as the loop having a load and the pump is operating intermittently or the pump is continuously operating (regardless of the loading condition), the pump will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump is running, it will try to meet the flow request made by demand side components.
+
+\paragraph{Field: Hot Water Pump Rated Head}\label{field-hot-water-pump-rated-head}
+
+The rated head of the hot water pump in Pa. The default value is 179352 Pa which is equivalent to 60 feet H2O.
+
+\paragraph{Field: Hot Water Setpoint Reset Type}\label{field-hot-water-setpoint-reset-type}
+
+Select the type of automatic reset control for the Hot Water supply temperature. The choices are:
+
+\begin{itemize}
+\item
+  None -- no reset, use the Hot Water Setpoint Schedule or Hot Water Design Setpoint.
+\item
+  OutdoorAirTemperatureReset -- reset the Hot Water supply temperature based on the following default rules. The temperature limits and setpoints are specified using the fields below. If the default values are used, when the outdoor dry-bulb temperature (ODB) is at or below --6.7C the setpoint is 82.2C. When the ODB is at or above 10.0C the setpoint is 65.6C. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset)
+\end{itemize}
+
+The default is \emph{None}.
+
+\paragraph{Field: Hot Water Setpoint at Outdoor Dry Bulb Low}\label{field-hot-water-setpoint-at-outdoor-dry-bulb-low}
+
+The Hot Water setpoint temperature in C when the outdoor dry-bulb is at or below the low limit (Hot Water Reset Outdoor Dry Bulb Low). The default is --6.7C.
+
+\paragraph{Field: Hot Water Reset Outdoor Dry Bulb Low}\label{field-hot-water-reset-outdoor-dry-bulb-low}
+
+The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Hot Water Setpoint at Outdoor Dry Bulb Low. The default is 82.2C.
+
+\paragraph{Field: Hot Water Setpoint at Outdoor Dry Bulb High}\label{field-hot-water-setpoint-at-outdoor-dry-bulb-high}
+
+The Hot Water setpoint temperature in C when the outdoor dry-bulb is at or above the high limit (Hot Water Reset Outdoor Dry Bulb Low). The default is 10.0C.
+
+\paragraph{Field: Hot Water Reset Outdoor Dry Bulb High}\label{field-hot-water-reset-outdoor-dry-bulb-high}
+
+The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Hot Water Setpoint at Outdoor Dry Bulb High. The default is 65.6C.
+
+\paragraph{Field: Hot Water Pump Type}\label{field-hot-water-pump-type}
+
+Describes the type of pump configuration used for the hot water loop. The options include:
+
+\begin{itemize}
+\item
+  SinglePump
+\item
+  PumpPerBoiler
+\item
+  TwoHeaderedPumps
+\item
+  ThreeHeaderedPumps
+\item
+  FourHeaderedPumps
+\item
+  FiveHeaderedPumps
+\end{itemize}
+
+\paragraph{Field: Supply Side Bypass Pipe}\label{field-supply-side-bypass-pipe}
+
+The field determines if a supply side bypass pipe is present in the hot water loop. The choices for this field are
+
+\begin{itemize}
+\item
+  Yes
+\item
+  No.
+\end{itemize}
+
+\paragraph{Field: Demand Side Bypass Pipe}\label{field-demand-side-bypass-pipe}
+
+The field determines if a demand side bypass pipe is present in the hot water loop. The choices for this field are
+
+\begin{itemize}
+\item
+  Yes
+\item
+  No.
+\end{itemize}
+
+\paragraph{Field: Fluid Type}\label{field-fluid-type-1}
+
+This field determines the type of fluid used for the chilled water loop. The following options are available:
+
+\begin{itemize}
+\item
+  Water
+\item
+  EthyleneGlycol30
+\item
+  EthyleneGlycol40
+\item
+  EthyleneGlycol50
+\item
+  EthyleneGlycol60
+\item
+  PropyleneGlycol30
+\item
+  PropyleneGlycol40
+\item
+  PropyleneGlycol50
+\item
+  PropyleneGlycol60
+\end{itemize}
+
+\paragraph{Field: Loop Design Delta Temperature}\label{field-loop-design-delta-temperature-1}
+
+The temperature difference used in sizing the loop flow rate. The default is 11C.
+
+\paragraph{Field: Maximum Outdoor Dry Bulb Temperature}\label{field-maximum-outdoor-dry-bulb-temperature}
+
+The maximum outdoor dry bulb temperature that the hot water loops operate.
+
+\paragraph{Field: Load Distribution Scheme}\label{field-load-distribution-scheme}
+
+This alpha field contains the Load Distribution Scheme Keyword. The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. \textbf{Optimal} operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{SequentialLoad} loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{UniformLoad} evenly distributes the loop demand among all available components on the equipment list for a given load range. \textbf{SequentialUniformPLR} loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. \textbf{UniformPLR} will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
+
+Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Plant:HotWaterLoop,
+  Hot Water Loop,          !-Plant Loop Name
+  ,                        !- Pump Schedule
+  Intermittent,            !- Pump Control Type
+  Default,                 !- Hot Water Plant Operation Scheme Type
+  ,                        !- Hot Water Plant Operation Scheme List Name
+  HW Loop Temp Schedule,   !- Hot Water Setpoint Schedule
+  82,                    !- Hot Water Design Setpoint {C}
+  VariableFlow,          !- Hot Water Pump Configuration
+  179352,                !- Hot Water Pump Rated Head {Pa}
+  None,                  !- Hot Water Setpoint Reset Type
+  82.2,                  !- Hot Water Setpoint at Outdoor Dry Bulb Low {C}
+  -6.7,                  !- Hot Water Reset Outdoor Dry Bulb Low {C}
+  65.6,                  !- Hot Water Setpoint at Outdoor Dry Bulb High {C}
+  10,                    !- Hot Water Reset Outdoor Dry Bulb High {C}
+  SinglePump,              !- Hot Water Pump Type
+  Yes,                     !- Supply Side Bypass Pipe
+  Yes,                     !- Demand Side Bypass Pipe
+  Water,                   !- Fluid Type
+  11,                      !- Loop Design Delta Temperature {deltaC}
+  ,                        !- Maximum Outdoor Dry Bulb Temperature {C}
+  SequentialLoad;              !- Load Distribution Scheme
+\end{lstlisting}
+
+\subsection{HVACTemplate:Plant:Boiler}\label{hvactemplateplantboiler}
+
+A boiler or purchased heating source is described with this object. To define multiple boilers, use multiple HVACTemplate:Plant:Boiler objects and use the Sizing Factor field to apportion the total capacity if autosizing.
+
+\subsubsection{Inputs}\label{inputs-29-000}
+
+\paragraph{Field: Name}\label{field-name-16-003}
+
+The name used to reference the HVACTemplate:Plant:Boiler object.
+
+\paragraph{Field: Boiler Type}\label{field-boiler-type}
+
+While EnergyPlus has a variety of boiler options, the choices for this field are:
+
+\begin{itemize}
+\item
+  DistrictHotWater -- District heating
+\item
+  HotWaterBoiler -- Hot water boiler (non-condensing)
+\item
+  CondensingHotWaterBoiler -- Hot water boiler (condensing)
+\end{itemize}
+
+The EnergyPlus equipment object types which are used are DistrictHeating or Boiler:HotWater. These equipment type keys must be used if setting up a user-defined boiler plant operation scheme.
+
+\paragraph{Field: Capacity}\label{field-capacity-1}
+
+This field may be set to autosize, which means that the capacity is based on the peak loads during the design days. This numeric field contains the design heating capacity of the boiler. This capacity should be at the design water flow rates. The units are in W.
+
+\paragraph{Field: Efficiency}\label{field-efficiency-000}
+
+This numeric field contains the heating efficiency (as a fraction between 0 and 1) of the boiler's burner. Not applicable if Boiler Type is DistrictHotWater.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-1-001}
+
+The choices for this field are
+
+\begin{itemize}
+\item
+  Electricity
+\item
+  NaturalGas
+\item
+  PropaneGas
+\item
+  FuelOil\#1
+\item
+  FuelOil\#2
+\item
+  Coal
+\item
+  Diesel
+\item
+  Gasoline
+\item
+  OtherFuel1
+\item
+  OtherFuel2
+\end{itemize}
+
+Not applicable if Boiler Type is DistrictHotWater
+
+\paragraph{Field: Priority}\label{field-priority-4}
+
+Enter the priority number of the boiler where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Boiler Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:HotWaterLoop. Equipment is operated in order of the priority number. This allows multiple boilers to be sequenced.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-1-000}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the boiler object inputs that would be altered by the sizing factor are: Nominal Capacity and Design Water Flow Rate. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-1-000}
+
+This numeric field contains the minimum part load ratio. If the ratio of demand to boiler nominal capacity is less than the minimum part load ratio, then the Min PLR will determine the operating PLR. The expected range is between 0 and 1. If this field is left blank, the default value is 0.0.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-1-000}
+
+This numeric field contains the maximum part load ratio. If the ratio of demand to boiler nominal capacity is greater than the maximum part load ratio, then the Max PLR will determine the operating PLR. This value may exceed 1, but the normal range is between 0 and 1.1. If this field is left blank, the default value is 1.1.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-1-000}
+
+This numeric field contains the optimum part load ratio. This is the part load ratio at which the boiler performs at its maximum efficiency. If this field is left blank, the default value is 1.0.
+
+\paragraph{Field: Water Outlet Upper Temperature Limit}\label{field-water-outlet-upper-temperature-limit}
+
+This numeric field contains the outlet temperature upper limit. If this field is left blank, the default value is 100.0ºC.
+
+\paragraph{Field: Template Plant Loop Type}\label{field-template-plant-loop-type-2}
+
+This field specifies whether this boiler will serve a \emph{HotWaterLoop} (ref. HVACTemplate:Plant:HotWaterLoop) or a \emph{MixedWaterLoop} (ref. HVACTemplate:Plant:MixedWaterLoop). If this field is left blank, this tower will serve a HotWaterLoop if present or a MixedWaterLoop (if no HotWaterLoop is present).
+
+An example in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Plant:Boiler,
+  Main Boiler,             !- Name
+  HotWaterBoiler,          !- Boiler Type
+  autosize,                !- Capacity {W}
+  0.8,                     !- Efficiency
+  NaturalGas,              !- Fuel Type
+  1,                       !- Priority
+  1,                       !- Sizing Factor
+  0.1,                     !- Minimum Part Load Ratio
+  1.1,                     !- Maximum Part Load Ratio
+  0.9,                     !- Optimum Part Load Ratio
+  99.9;                    !- Water Outlet Upper Temperature Limit {C}
+\end{lstlisting}
+
+\subsection{HVACTemplate:Plant:Boiler:ObjectReference}\label{hvactemplateplantboilerobjectreference}
+
+This object references a detailed boiler object and adds it to an HVACTemplate:Plant:HotWaterLoop or MixedWaterLoop. The user must create a complete detailed boiler object with all required curve or performance objects. The detailed boiler object is referenced by object type and name and the boiler will be automatically to the hot water or mixed water loop branches and equipment list.
+
+\subsubsection{Inputs}\label{inputs-30-000}
+
+\paragraph{Field: Name}\label{field-name-17-002}
+
+The name of this object.
+
+\paragraph{Field: Boiler Object Type}\label{field-boiler-object-type}
+
+The object type of the referenced boiler. Select from one of the following supported boiler object types:
+
+\begin{itemize}
+\tightlist
+\item
+  Boiler:HotWater
+\end{itemize}
+
+\paragraph{Field: Boiler Name}\label{field-boiler-name}
+
+The object name of the referenced boiler.
+
+\paragraph{Field: Priority}\label{field-priority-5}
+
+Enter the priority number of the boiler where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Hot Water Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:HotWaterLoop or MixedWaterLoop. Equipment is operated in order of the priority number. This allows multiple boilers to be sequenced.
+
+\paragraph{Field: Template Plant Loop Type}\label{field-template-plant-loop-type-3}
+
+This field specifies whether this boiler will serve a \emph{HotWaterLoop} (ref. HVACTemplate:Plant:HotWaterLoop) or a \emph{MixedWaterLoop} (ref. HVACTemplate:Plant:MixedWaterLoop). If this field is left blank, this tower will serve a HotWaterLoop if present or a MixedWaterLoop (if no HotWaterLoop is present).
+
+An example in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Plant:Boiler:ObjectReference,
+  Main Boiler Connection,  !- Name
+  Boiler:HotWater,         !- Boiler Object Type
+  Main Boiler,             !- Boiler Name
+  1;                       !- Priority
+\end{lstlisting}
+
+\subsection{HVACTemplate:Plant:MixedWaterLoop}\label{hvactemplateplantmixedwaterloop}
+
+This object simulates the central plant loop portion of a water source heat pump system. Often many HVACTemplate:Zone:WaterToAirHeatPump objects will be used in a building along with a single HVACTemplate:Plant:MixedWaterLoop that contains one or more cooling towers and boilers. The piping systems are called loops and this object describes the controls and pumps on the loops. Only one of these objects should be defined in an input file.
+
+\subsubsection{Inputs}\label{inputs-31-000}
+
+\paragraph{Field: Name}\label{field-name-18-002}
+
+The name used to designate the HVACTemplate:Plant:MixedWaterLoop.
+
+\paragraph{Field: Pump Schedule Name}\label{field-pump-schedule-name-2}
+
+Leave this field blank if the water pump is always available. If a schedule name is specified, those times that the pump is available should be specified as 1.0. Those times that the pump is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the system is providing water to the water-to-air heat pumps but a schedule of when it can provide water to the water-to-air heat pumps.
+
+\paragraph{Field: Pump Control Type}\label{field-pump-control-type-2}
+
+The choices for this field are
+
+\begin{itemize}
+\item
+  Intermittent
+\item
+  Continuous
+\end{itemize}
+
+The default value is Intermittent.
+
+If the pump control type is \textbf{Continuous}, the pump will run according to the Pump Schedule (see above) regardless of whether or not there is a load. If the pump control type is \textbf{Intermittent}, the pump will run if a load is sensed and will shut off if there is no load on the loop.
+
+\paragraph{Field: Operation Scheme Type}\label{field-operation-scheme-type}
+
+The choices for this field are:
+
+\begin{itemize}
+\item
+  Default
+\item
+  UserDefined
+\end{itemize}
+
+Default operation type makes all equipment available at all times operating in order of Priority specified in HVACTemplate:Plant:Boiler objects. If a different scheme is to be used to sequence the boilers, then this entry should be set to User Defined.
+
+If User Defined option is chosen, then additional EnergyPlus objects must be defined in the IDF file such as shown below depending on the type of plant operation control scheme chosen:
+
+\begin{itemize}
+\item
+  PlantEquipmentOperationSchemes
+\item
+  PlantEquipmentOperation:CoolingLoad
+\item
+  PlantEquipmentOperation:HeatingLoad
+\item
+  PlantEquipmentList (refer to HVACTemplate:Plant:Boiler object description for key name required in this object)
+\end{itemize}
+
+The default value is Default.
+
+\paragraph{Field: Equipment Operation Schemes Name}\label{field-equipment-operation-schemes-name}
+
+This field should contain the name of a PlantEquipmentOperationSchemes object only when the previous field is set to User Defined. It is ignored if Hot Water Plant Operation Scheme Type is Default.
+
+\paragraph{Field: High Temperature Setpoint Schedule Name}\label{field-high-temperature-setpoint-schedule-name}
+
+Enter the name of a high temperature setpoint schedule that has values that change at different times of the year. If a constant set point is needed simply leave this field blank and the value in the next field will be used at all times. The values in the schedule are in degrees C.
+
+\paragraph{Field: High Temperature Design Setpoint}\label{field-high-temperature-design-setpoint}
+
+Enter the high temperature setpoint temperature to be used for sizing the water loop and associated equipment in degrees C. If the High Temperature Setpoint Schedule is blank, then this value will be used as the setpoint at all times. The default is 33C.
+
+\paragraph{Field: Low Temperature Setpoint Schedule Name}\label{field-low-temperature-setpoint-schedule-name}
+
+Enter the name of a low temperature setpoint schedule that has values that change at different times of the year. If a constant set point is needed simply leave this field blank and the value in the next field will be used at all times. The values in the schedule are in degrees C.
+
+\paragraph{Field: Low Temperature Design Setpoint}\label{field-low-temperature-design-setpoint}
+
+Enter the low temperature setpoint temperature to be used for sizing the water loop and associated equipment in degrees C. If the Low Temperature Setpoint Schedule is blank, then this value will be used as the setpoint at all times. The default is 20C.
+
+\paragraph{Field: Water Pump Configuration}\label{field-water-pump-configuration}
+
+The choices for this field are
+
+\begin{itemize}
+\item
+  VariableFlow
+\item
+  ConstantFlow
+\end{itemize}
+
+The default value is ConstantFlow. The variable flow option simulates a pump with variable flow to boilers, cooling towers, and water to air heat pump, excess bypassed. The constant flow option simulates constant flow to boilers, cooling towers, and water to air heat pumps, excess bypassed.
+
+The operation of a constant speed pump is fairly straightforward. If the user designates a constant speed pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump is constant speed and operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop.
+
+A variable speed pump is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump is operating intermittently, then the pump can shutdown. For any other condition such as the loop having a load and the pump is operating intermittently or the pump is continuously operating (regardless of the loading condition), the pump will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump is running, it will try to meet the flow request made by demand side components.
+
+\paragraph{Field: Water Pump Rated Head}\label{field-water-pump-rated-head}
+
+The rated head of the hot water pump in Pa. The default value is 179352 Pa which is equivalent to 60 feet H2O.
+
+\paragraph{Field: Water Pump Type}\label{field-water-pump-type}
+
+Describes the type of pump configuration used for mixed water loop. The options include:
+
+\begin{itemize}
+\item
+  SinglePump
+\item
+  PumpPerTowerOrBoiler
+\item
+  TwoHeaderedPumps
+\item
+  ThreeHeaderedPumps
+\item
+  FourHeaderedPumps
+\item
+  FiveHeaderedPumps
+\end{itemize}
+
+\paragraph{Field: Supply Side Bypass Pipe}\label{field-supply-side-bypass-pipe-1}
+
+The field determines if a supply side bypass pipe is present in the mixed water loop. The choices for this field are
+
+\begin{itemize}
+\item
+  Yes
+\item
+  No
+\end{itemize}
+
+\paragraph{Field: Demand Side Bypass Pipe}\label{field-demand-side-bypass-pipe-1}
+
+The field determines if a demand side bypass pipe is present in the mixed water loop. The choices for this field are
+
+\begin{itemize}
+\item
+  Yes
+\item
+  No
+\end{itemize}
+
+\paragraph{Field: Fluid Type}\label{field-fluid-type-2}
+
+This field determines the type of fluid used for the mixed water loop. The following options are available:
+
+\begin{itemize}
+\item
+  Water
+\item
+  EthyleneGlycol30
+\item
+  EthyleneGlycol40
+\item
+  EthyleneGlycol50
+\item
+  EthyleneGlycol60
+\item
+  PropyleneGlycol30
+\item
+  PropyleneGlycol40
+\item
+  PropyleneGlycol50
+\item
+  PropyleneGlycol60
+\end{itemize}
+
+\paragraph{Field: Loop Design Delta Temperature}\label{field-loop-design-delta-temperature-2}
+
+The temperature difference used in sizing the loop flow rate. The default is 5.6C.
+
+\paragraph{Field: Load Distribution Scheme}\label{field-load-distribution-scheme-1}
+
+This alpha field contains the Load Distribution Scheme Keyword. The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. \textbf{Optimal} operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{SequentialLoad} loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{UniformLoad} evenly distributes the loop demand among all available components on the equipment list for a given load range. \textbf{SequentialUniformPLR} loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. \textbf{UniformPLR} will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
+
+Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
+
+As shown in an IDF:
+
+\begin{lstlisting}
+
+HVACTemplate:Plant:MixedWaterLoop,
+  Only Water Loop,         !- Name
+  ,                        !- Pump Schedule Name
+  Intermittent,            !- Pump Control Type
+  Default,                 !- Operation Scheme Type
+  ,                        !- Equipment Operation Schemes Name
+  ,                        !- High Temperature Setpoint Schedule Name
+  34,                      !- High Temperature Design Setpoint {C}
+  ,                        !- Low Temperature Setpoint Schedule Name
+  20,                      !- Low Temperature Design Setpoint {C}
+  ConstantFlow,            !- Water Pump Configuration
+  179352,                  !- Water Pump Rated Head {Pa}
+  SinglePump,              !- Water Pump Type
+  Yes,                     !- Supply Side Bypass Pipe
+  Yes,                     !- Demand Side Bypass Pipe
+  Water,                   !- Fluid Type
+  6,                       !- Loop Design Delta Temperature {deltaC}
+  SequentialLoad;              !- Load Distribution Scheme
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/hvac-template-objects/hvactemplate-processing.tex b/doc/input-output-reference/src/hvac-template-objects/hvactemplate-processing.tex
new file mode 100644
index 00000000000..69121c05392
--- /dev/null
+++ b/doc/input-output-reference/src/hvac-template-objects/hvactemplate-processing.tex
@@ -0,0 +1,30 @@
+\section{HVACTemplate Processing}\label{hvactemplate-processing}
+
+\textbf{Unlike other EnergyPlus objects, the HVACTemplate objects are not handled by EnergyPlus directly.} Instead, they are preprocessed by a program called ExpandObjects. If you use EP-Launch or RunEPlus.bat, this preprocessor step is performed automatically using the following sequence:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  The preprocessor program, ExpandObjects, reads your IDF file and converts all of the HVACTemplate objects into other EnergyPlus objects.
+\item
+  The ExpandObjects program copies the original idf file with the HVACTemplate objects commented out (i.e., inserts a ``!'' in front of the object name and its input fields) plus all of the new objects created in Step 1 and writes a new file which is saved with the extension ``expidf''. This ``expidf'' file may be used as a standard EnergyPlus IDF file if the extension is changed to idf; however, for safety's sake, both filename and extension should be changed.
+\item
+  The EnergyPlus simulation proceeds using the expidf file as the input stream.
+\item
+  If there are error messages from EnergyPlus, they will refer to the contents of the expidf file. Specific objects referred to in error messages may exist in the original idf, but they may be objects created by ExpandObjects and only exist in the expidf. Remember that the expidf will be overwritten everytime the original idf is run using EP-Launch or RunEPlus.bat.
+\end{enumerate}
+
+If you are trying to go beyond the capabilities of the HVACTemplate objects, one strategy you can use is to start your specification using the HVACTemplate objects, run EnergyPlus using EP-Launch and producing an expidf file, rename that file and start making modifications. This approach may help with getting all of the objects needed and the node names set consistently.
+
+\textbf{Users need to remember that no objects related to HVAC except for HVAC template objects are needed in the IDF file.} The existence of other objects (unless specifically described in the following sections) may cause unexpected errors to occur. Sizing:Zone, Sizing:System, and Sizing:Plant objects will be generated by the corresponding HVACTemplate objects; the user does not need to create these elsewhere in the input file.
+
+There are some exceptions to this rule:
+
+\begin{itemize}
+\item
+  HVACTemplate:Plant:Chiller:ObjectReference which requires that the corresponding chiller object be present in the idf file along with any required curve or performance objects. In this case, the HVACTemplate object does not create the chiller object, but adds all of the connections. HVACTemplate:Plant:Tower:ObjectReference and HVACTemplate:Plant:Boiler;ObjectReferences are similar.
+\item
+  For HVACTemplate:Zone:* objects, if Outdoor Air Method = \emph{DetailedSpecification}, then any referenced DesignSpecification:OutdoorAir and DesignSpecification:ZoneAirDistribution objects must be present in the idf file.
+\item
+  For HVACTemplate:Zone:VAV and HVACTemplate:Zone:DualDuct, if a Design Specification Outdoor Air Object Name for Control is specified, then the referenced DesignSpecification:OutdoorAir object must be present in the idf file.
+\end{itemize}
diff --git a/doc/input-output-reference/src/input-for-output.tex b/doc/input-output-reference/src/input-for-output.tex
new file mode 100644
index 00000000000..30df216514a
--- /dev/null
+++ b/doc/input-output-reference/src/input-for-output.tex
@@ -0,0 +1,2068 @@
+\chapter{Input for Output}\label{input-for-output}
+
+Several items are used to specify what will appear in the output file(s). The output is described in the next section of this document.
+
+\section{Group -- Reports}\label{group-reports}
+
+\subsection{Variable Dictionary Reports}\label{variable-dictionary-reports}
+
+One of the most important outputs for EnergyPlus is the Variable Dictionary reports -- these contain the key variable names for each simulation. This single input object is used to produce two important reports that are used to identify the specific output variables and meters available for a specific EnergyPlus model.~ Two output files are produced (\textbf{eplusout.rdd \& eplusout.mdd}) that list the names of the output variables and meters for that simulation.~ You may need to run your simulation once and produce these files before you ask for specific output variables (\textbf{rdd}) or meters (\textbf{mdd}) (see Output:Variable and Output:Meter objects). Variables available, to some extent, depend on the simulation input. Variables are ``set up'' during the initial ``get input'' processing done within the modules. Therefore, an item that is specific to a certain type of coil would not be available if that coil were not used during the simulation. This command will produce a list of variables available for reporting.
+
+\subsubsection{Field: Key Field}\label{field-key-field}
+
+For this field there are two choices: \textbf{IDF} and \textbf{regular}. The regular option is the default and produces a listing that shows the type of variable: Zone or HVAC, Average or Sum. ``\textbf{Zone}'' variables are calculated and can be reported after each Zone/Heat Balance timestep (ref: Timesteps input object). ``\textbf{HVAC}'' variables are calculated and can be reported with each variable HVAC timestep. ``\textbf{Average}'' variables will be averaged over the time interval being reported whereas ``\textbf{Sum}'' variables are summed over that time interval. (Meter variables are always summed.) Units for the variable are shown in ``{[}\}''.
+
+\subsubsection{Field: Sort Option}\label{field-sort-option}
+
+For this field there are two choices: \textbf{Name} and \textbf{Unsorted}. By default, the listing of available reporting variables are unsorted -- listed in the streaming order that EnergyPlus generates them. Or, you can have them sorted by name.
+
+Examples of the options for this object follow:
+
+\begin{lstlisting}
+Output:VariableDictionary,regular;
+\end{lstlisting}
+
+Results of this are shown in the Output Details document under the \textbf{eplusout.rdd} (output variables) and \textbf{eplusout.mdd} (meter variables) files.
+
+The eplusout.mdd file has a similar format for meters:
+
+\subsubsection{Variable Dictionary Report in IDF Format}\label{variable-dictionary-report-in-idf-format}
+
+The common workflow process of examining Variable Dictionary Reports and then adding reporting requests to an IDF file can be facilitated by using the following alternate form (Report Name = IDF) of the input object that requests the reports.
+
+\begin{lstlisting}
+Output:VariableDictionary, IDF;
+\end{lstlisting}
+
+A sorted request would appear similarly:
+
+\begin{lstlisting}
+Output:VariableDictionary, IDF, Name;
+\end{lstlisting}
+
+\subsection{Surface Reports}\label{surface-reports}
+
+There are two specific objects for surfaces: \textbf{Output:Surfaces:List} and \textbf{Output:Surfaces:Drawing} -- as the names imply, the list reports are simple text reports that are contained in one of the output files whereas the drawing reports will create files that are used in other graphic tools.
+
+These objects and their use is described in the following:
+
+\subsection{Output:Surfaces:List}\label{outputsurfaceslist}
+
+Examples of using the Output:Surfaces:List object follow:
+
+\subsubsection{Inputs}\label{inputs-040}
+
+\paragraph{Lines Data Report}\label{lines-data-report}
+
+An example input object for this report follows.
+
+\begin{lstlisting}
+Output:Surfaces:List, Lines;
+\end{lstlisting}
+
+The above IDF line will produce a simple file of line segments that constitute the surfaces in the IDF file. This file is the~ ``lines'' report (\textbf{eplusout.sln}) and is decribed in more detail in the Output Details and Examples document.
+
+\paragraph{Field: Report Specifications}\label{field-report-specifications}
+
+An extra option of entering ``IDF'' in this field directs the Lines report to produce coordinates transformed into Surface Geometry (Lower Left Corner, CounterClockwise, WorldCoordinates).~ An example of this follows.
+
+\begin{lstlisting}
+Output:Surfaces:List, Lines, IDF;
+\end{lstlisting}
+
+The result is put on the \textbf{eplusout.sln} file and is nearly ready for putting into a IDF. Again, it is described in more detail in the Output Details and Examples document.
+
+\paragraph{Detailed Surface Data Report}\label{detailed-surface-data-report}
+
+An example input object for this report follows.
+
+\begin{lstlisting}
+Output:Surfaces:List, Details;
+\end{lstlisting}
+
+This report (in \textbf{eplusout.eio}) contains details about each surface -- including surface name, associated zone, area, approximate height and width, tilt, outward facing angle. Specific details on this report can be found in the Output Details and Examples document.
+
+\paragraph{Vertices Data Report}\label{vertices-data-report}
+
+An example input object for this report follows.
+
+\begin{lstlisting}
+Output:Surfaces:List, Vertices;
+\end{lstlisting}
+
+This report (in \textbf{eplusout.eio}) contains the vertices of each surface along with surface name and other information. Specific details on this report can be found in the Output Details and Examples document.
+
+\paragraph{Detailed Surface Data With Vertices Report}\label{detailed-surface-data-with-vertices-report}
+
+An example input object for this report follows.
+
+\begin{lstlisting}
+Output:Surfaces:List, DetailsWithVertices;
+\end{lstlisting}
+
+This report (in \textbf{eplusout.eio}) is the combination of the two preceding reports (Details and Vertices). Specific details on this report can be found in the Output Details and Examples document.
+
+\paragraph{View Factor Information Report}\label{view-factor-information-report}
+
+An example input object for this report follows.
+
+\begin{lstlisting}
+Output:Surfaces:List, ViewFactorInfo;
+\end{lstlisting}
+
+This report (in \textbf{eplusout.eio}) provides details about the thermal radiation exchange view factors and interchange factors.~ Specific details on this report can be found in the Output Details and Examples document.
+
+\paragraph{DecayCurvesfromZoneComponentLoads}\label{decaycurvesfromzonecomponentloads}
+
+An example input object for this report follows.
+
+\begin{lstlisting}
+Output:Surfaces:List, DecayCurvesfromZoneComponentLoads;
+\end{lstlisting}
+
+This report (in \textbf{eplusout.eio}) provides an intermediate calculation used, called a decay curve,~ in the Zone Component Loads Summary report for the estimate of the sensible-delayed column values. A decay curve is created for each surface in a zone by introducing a radiant pulse. Each value in each row of the report corresponds to a zone time step from the time the pulse was introduced. See Zone Component Load Summary described in object Output:Table:SummaryReports for more detailed information.
+
+\subsection{Output:Surfaces:Drawing}\label{outputsurfacesdrawing}
+
+Examples of using the Output:Surfaces:Drawing object follow:
+
+\subsubsection{Inputs}\label{inputs-1-037}
+
+\paragraph{DXF Surface Report}\label{dxf-surface-report}
+
+Examples input objects follow.
+
+\begin{lstlisting}
+Output:Surfaces:Drawing, DXF;
+  Output:Surfaces:Drawing, DXF, RegularPolyline;
+  Output:Surfaces:Drawing, DXF, Triangulate3DFace, mycolorscheme;
+\end{lstlisting}
+
+The above IDF specification will produce a DXF file (\textbf{eplusout.dxf}) of the surfaces in the IDF file.~ Only one DXF report can be produced. More specifics on this report can be found in the Output Details and Examples document.
+
+\paragraph{Field: Report Specifications 1}\label{field-report-specifications-1}
+
+As indicated in the example, you can select among three different ways that surfaces with more than four sides will appear in the DXF file. These are:
+
+\begin{itemize}
+\item
+  ThickPolyline -- surface with \textgreater{}4 sides will be represented as a ``thick'' line in the appropriate surface color. It will look like a hole in the drawing with a thicker edge.
+\item
+  RegularPolyline -- surface with \textgreater{}4 sides will be represented as a regular line in the appropriate surface color. It will look like a hole in the drawing.
+\item
+  Triangulate3DFace-- surface with \textgreater{}4 sides will be ``triangulated'' internally within EnergyPlus.~ This is only for drawing purposes and does not affect the calculations in any way.~ In a line version of the DXF, it will appear that the surface is split into triangles. In a solid view, the surface will appear similar to surfaces with \textless{} = 4 sides. The triangulation algorithm is not perfect and warnings do result when the software cannot triangulate the surface.
+\end{itemize}
+
+\paragraph{Field: Report Specifications 2}\label{field-report-specifications-2}
+
+This field can be used to control the color scheme in the DXF file by entering the name of an OutputControl:SurfaceColorScheme object.~ Using OutputControl:SurfaceColorScheme, you can define color schemes for surface representation. This feature will let you align the colors with the software of your choice (colors don't seem to be standard across DXF viewers).
+
+Several software programs can render this file into something viewable and are described in more detail in the Output Details and Examples document under the file name (\textbf{eplusout.dxf}).
+
+\paragraph{DXF Wire Frame Report}\label{dxf-wire-frame-report}
+
+An example input object for this report follows.
+
+\begin{lstlisting}
+Output:Surfaces:Drawing, DXF:WireFrame;
+\end{lstlisting}
+
+The above IDF specification will produce a DXF (Drawing Exchange Format) file (\textbf{eplusout.dxf}) of the surfaces in the IDF file using the DXF ``Lines'' command -- producing only a wire frame capable file. More specifics on this report can be found in the Output Details and Examples document. Only one DXF report can be produced.
+
+\paragraph{VRML Report}\label{vrml-report}
+
+Examples input objects for this report follow.
+
+\begin{lstlisting}
+Output:Surfaces:Drawing, VRML;
+  Output:Surfaces:Drawing, VRML, Triangulate3DFace;
+\end{lstlisting}
+
+The above IDF specification produces a VRML (Virtual Reality Modeling Language) file (\textbf{eplusout.wrl}) of the surfaces in the IDF file.~ Only one VRML report can be produced. VRML files can be viewed in many web browsers after adding a ``plug-in'' and there are some stand-alone viewers as well. More specifics on this report can be found in the Output Details and Examples document.
+
+\paragraph{Field: Report Specifications 1}\label{field-report-specifications-1-1}
+
+As indicated in the example, you can select several figure types (for \textgreater{}4 sided surfaces) in the DXF report. These are:
+
+\begin{itemize}
+\item
+  ThickPolyline -- surface with \textgreater{}4 sides will be represented as a ``thick'' line in the appropriate surface color. It will look like a hole in the drawing with a thicker edge.
+\item
+  RegularPolyline -- surface with \textgreater{}4 sides will be represented as a regular line in the appropriate surface color. It will look like a hole in the drawing.
+\item
+  Triangulate3DFace -- surface with \textgreater{}4 sides will be ``triangulated'' internally within EnergyPlus.~ This is only for drawing purposes and does not affect the calculations in any way.~ In a line version of the VRML, it will appear that the surface is split into triangles. In a solid view, the surface will appear similar to surfaces with \textless{} = 4 sides. The triangulation algorithm is not perfect and warnings do result when the software cannot triangulate the surface.
+\end{itemize}
+
+\paragraph{Field: Report Specifications 2}\label{field-report-specifications-2-1}
+
+Color schemes are not applicable for VRML reports.
+
+\subsection{Output:Schedules}\label{outputschedules}
+
+This is a condensed reporting that illustrates the full range of schedule values -- in the style of input: DaySchedule, WeekSchedule, and Annual Schedule.
+
+\subsubsection{Inputs}\label{inputs-2-034}
+
+\paragraph{Field: Key Field}\label{field-key-field-1}
+
+This field should contain the word \textbf{Hourly} or \textbf{TimeStep} to obtain the respective reports.
+
+\begin{lstlisting}
+Output:Schedules, Hourly;     ! values on hourly increments (day schedule resolution)
+  Output:Schedules, TimeStep; ! will give them at the timestep of the simulation
+\end{lstlisting}
+
+This report is placed on the \textbf{eplusout.eio} file. Details of this reporting are shown in the Output Details and Examples document.~ Schedule values over time can also be obtained in the EnergyPlus Standard Output (in eplusout.eso) using Output:Variable objects.
+
+\subsection{Output:Constructions}\label{outputconstructions}
+
+\subsubsection{Inputs}\label{inputs-3-030}
+
+\paragraph{Constructions Report}\label{constructions-report}
+
+This report content is added to the ``\textbf{eplusout.eio}'' file. It shows the calculated results related to conduction transfer functions for each construction. It also includes similar details about the windows. Specific details on this report can be found in the Output Details and Examples document.~ The following input object is used to obtain the Construction report.
+
+\begin{lstlisting}
+Output:Constructions,Constructions;
+\end{lstlisting}
+
+\paragraph{Field: Details Type 1, Details Type 2}\label{field-details-type-1-details-type-2}
+
+Either field can contain the word ``\textbf{Constructions}'' to get the constructions report.
+
+Or either field can contain the word ``\textbf{Materials}'' to obtain the Materials report.
+
+\paragraph{Materials Report}\label{materials-report}
+
+This report content is added to the ``\textbf{eplusout.eio}'' file. It provides a summary of the thermal properties and thickness of the construction and window materials in the model.~ Specific details on this report can be found in the Output Details and Examples document.~ The following input object is used to obtain the Materials report.
+
+\begin{lstlisting}
+Output:Constructions,Materials;
+\end{lstlisting}
+
+\subsection{Output:DaylightFactors}\label{outputdaylightfactors}
+
+Daylight factors are ratios of interior illuminance at a specific location to exterior horizontal illuminance. In EnergyPlus, they are pre-calculated hourly for every shadow calculation day for every exterior window of a daylight zone. The pre-calculated daylight factors are interpolated between hours and for the actual sky conditions in the time-step calculation of the daylighting performance of daylight zones.
+
+EnergyPlus reports the daylight factors for four sky types (clear, turbid clear, intermediate, and overcast) at noon time (12:00pm) for each exterior windows (base window without shading) in the eio file when the daylight factors are first calculated. This new object can report all hourly pre-calculated daylight factors. Details of the report are shown in the Output Details document.
+
+\subsubsection{Inputs}\label{inputs-4-027}
+
+\paragraph{Field: Reporting Days}\label{field-reporting-days}
+
+This field is used to select days to report the daylight factors. Two choices are ``SizingDays'' and ``AllShadowCalculationDays''. The SizingDays choice will output the daylight factors for only the sizing calculation days, while the AllShadowCalculationDays choice will output daylight factors for all shadow calculation days.
+
+\subsection{Output:EnergyManagementSystem}\label{outputenergymanagementsystem}
+
+This report content is added to the ``eplusout.edd'' file. It shows information useful for the Energy Management System. The user can select the level of detail reported to the file using the fields in this object. However, there must be some other EMS-related input objects in the input file before this report will be generated.
+
+\subsubsection{Inputs}\label{inputs-5-024}
+
+\paragraph{Field: Actuator Availability Dictionary Reporting}\label{field-actuator-availability-dictionary-reporting}
+
+This field is used to control the level of output reporting related to the EMS actuators that are available for a particular model. When EnergyPlus runs with EMS, it sets up a wide array of possible actuators that the EMS could use. (To actually use them requires an EnergyManagementSystem:Actuator object). Actuator availability dictionary reporting is provided to show the user what actuators are available in a particular building model. Regardless of the level of reporting chosen here, the same set of actuators are actually available. There are three levels to choose from. The ``None'' choice means that no reporting of available actuators is done. The ``NotByUniqueNames'' level means that the output includes only the types of actuators and their control options but not the unique, user-defined names that identify a specific actuator in the model. The ``Verbose'' level means that the output includes all combinations of actuator types, control types, and the unique names of specific actuators. The verbose level provides all the information needed for input in an EnergyManagementSystem:Actuator input object.
+
+\paragraph{Field: Internal Variable Availability Dictionary Reporting}\label{field-internal-variable-availability-dictionary-reporting}
+
+This field is used to control the level of output reporting related to the EMS internal variables that are available for a particular model. When EnergyPlus runs with EMS, it sets up a wide array of possible internal data sources that the EMS could use. (To actually use them requires an EnergyManagementSystem:InternalVariable object). Internal variable availability dictionary reporting is provided to show the user what internal data are available. Regardless of the level of reporting chosen here, the same internal data are available. There are three levels to choose from. The ``None'' choice means that no reporting of available internal data is done. The ``NotByUniqueNames'' level means that the output includes only the types of internal data but not the unique names that identify a specific instances in the model. The ``Verbose'' level means that the output includes all combinations of internal variables and the unique names of specific instances. The verbose level provides all the information needed for an EnergyManagementSystem:InternalVariable input object.
+
+\paragraph{Field: EnergyPlus Runtime Language Debug Output Level}\label{field-energyplus-runtime-language-debug-output-level}
+
+This field is used to control the level of output reporting related to the execution of EnergyPlus Runtime Language, or Erl. This reporting is valuable for debugging Erl programs. When Erl programs are run inside EnergyPlus they can report error situations (such as divide by zero) or a full trace of each Erl statement. There are three levels of reporting. The ``None'' choice means that no reporting of Erl debug information is done. The ``ErrorsOnly'' choice means that Erl debugging traces are only output if the statement produces an error situation. The ``Verbose'' choice means that Erl debugging traces are done for each line of each Erl program. The verbose setting needs to be used with care because a large model with a long runperiod can easily create an EDD file that is too large for most computer systems (e.g.~many GBs of text).
+
+An example of this object follows.
+
+\begin{lstlisting}
+Output:EnergyManagementSystem,
+  Verbose,    ! Actuator Availability Dictionary Reporting
+  Verbose,    ! Internal Variable Availability Dictionary Reporting
+  ErrorsOnly; ! EnergyPlus Runtime Language Debug Output Level
+\end{lstlisting}
+
+\subsection{OutputControl:SurfaceColorScheme}\label{outputcontrolsurfacecolorscheme}
+
+This object provides control over the colors that appear in the DXF report, by surface.~ In addition, the Datasets folder contains example objects, including the ``original'' color scheme (prior to the 2.1 release).
+
+\subsubsection{Inputs}\label{inputs-6-021}
+
+\paragraph{Field: Name}\label{field-name-039}
+
+This assigns a unique name to this colorscheme data set.~ This name is used in the DXF output objects.
+
+\paragraph{Field Set: Drawing Element Type and Colorr}\label{field-set-drawing-element-type-and-colorr}
+
+This set of fields can range from none (accepting the default colors) up to 15 sets with individual types of building elements assigned a color number.~ (drawing element types not assigned a color number will use the default color numbers)
+
+\paragraph{Field: Drawing Element \textless{}\#\textgreater{} Type}\label{field-drawing-element-type}
+
+This field uses a choice of the drawing types (Text, Walls, Windows, GlassDoors, Doors, Roofs, Floors, DetachedBuildingShades, DetachedFixedShades, AttachedBuildingShades, Photovoltaics, TubularDaylightDomes, TubularDaylightDiffusers, DaylightReferencePoint1, DaylightReferencePoint2) for the color number assignment in the following field.
+
+\paragraph{Field: Color for Drawing Element \textless{}\#\textgreater{}}\label{field-color-for-drawing-element}
+
+This is a color ``number'' from 0 to 255.~ DXF display software is not standardized -- you may need to play around with these numbers if you don't like the supplied default color scheme.
+
+\subsection{OutputControl:ReportingTolerances}\label{outputcontrolreportingtolerances}
+
+This input object is created to allow more user control over some aspects of output reporting. Specifically, the reporting of ``Time setpoint not met'' hours~ See thermostat reporting (ZoneControl Thermostat Outputs).
+
+\subsubsection{Inputs}\label{inputs-7-021}
+
+\paragraph{Field: Tolerance for Time Heating Setpoint Not Met}\label{field-tolerance-for-time-heating-setpoint-not-met}
+
+This field allows the entry of a value for the tolerance away from the heating setpoint reporting. If the zone temperature is below the heating setpoint by more than this value, the following output variables will increment as appropriate
+
+Zone Heating Setpoint Not Met Time
+
+Zone Heating Setpoint Not Met While Occupied Time
+
+This also impacts table report ``Annual Building Utility Performance Summary'' subtable ``Comfort and Setpoint Not Met Summary''.
+
+\paragraph{Field: Tolerance for Time Cooling Setpoint Not Met}\label{field-tolerance-for-time-cooling-setpoint-not-met}
+
+This field allows the entry of a value for the tolerance away from the cooling setpoint reporting. If the zone temperature is above the cooling setpoint by more than this value, the following output variables will increment as appropriate
+
+Zone Cooling Setpoint Not Met Time
+
+Zone Cooling Setpoint Not Met While Occupied Time
+
+This also impacts table report ``Annual Building Utility Performance Summary'' subtable ``Comfort and Setpoint Not Met Summary''.
+
+As seen in an IDF:
+
+\begin{lstlisting}
+OutputControl:ReportingTolerances,.21,.21;
+\end{lstlisting}
+
+\subsection{Output:Variable}\label{outputvariable}
+
+This input object is used request results reporting.~ As shown above in the Variable Dictionary Report section, there are many different output variables available for reporting results from EnergyPlus.~ The Output:Variable object is primarily used for reporting time series data at various frequencys.
+
+Each Output:Variable object causes a specific number assignment for outputs. For example, you could request separate reporting for the outside temperature:
+
+\begin{lstlisting}
+Output:Variable,*,Site Outdoor Air Drybulb Temperature,timestep;
+Output:Variable,*,Site Outdoor Air Drybulb Temperature,hourly;
+Output:Variable,*,Site Outdoor Air Drybulb Temperature,monthly;
+\end{lstlisting}
+
+\subsubsection{Inputs}\label{inputs-8-019}
+
+\paragraph{Field: Key Value}\label{field-key-value}
+
+This alpha field can be used to make a specific reference for reporting. In addition to the generic variable names listed in the Variable Dictionary Report for the input file, variables will also have a key designator (such as Zone name or Surface name). You can reference the standard output file (\textbf{eplusout.eso}) to see just how these look.
+
+\begin{lstlisting}
+41,2,ZN001:WALL004,Surface Inside Temperature [C]
+42,2,ZN001:WALL004,Surface Outside Temperature [C]
+43,2,ZN001:WALL004,Surface Int Convection Coeff[W/m2-K]
+44,2,ZN001:WALL004,Surface Ext Convection Coeff[W/m2-K]
+46,2,ZONE ONE,Zone Mean Radiant Temperature [C]
+47,2,ZONE ONE,Zone Total Internal Latent Gain Energy [J]
+51,2,ZONE ONE,Zone Lights Electric Energy [J]
+58,2,ZONE ONE,Zone Air Temperature [C]
+\end{lstlisting}
+
+For example, in the previous block, the key for the surface variables is \textbf{ZN001:WALL004} whereas the key for the zone variables is \textbf{ZONE ONE} (note that the space is required and significant for this key).
+
+You can have all keys listed in the standard output file by putting a ``*'' in this field or you can have specific items listed by putting in a key value. If this field is left blank, it will use a * as the default (i.e., you will get all variables of Variable Name).
+
+\paragraph{Field: Variable Name}\label{field-variable-name}
+
+This alpha field is the variable name (you don't have to put on the units) that is shown in the Variable Dictionary Report file (eplusout.rdd). This field is required.
+
+\paragraph{Field: Reporting Frequency}\label{field-reporting-frequency}
+
+This field specifies how often the variable will be listed in the output file. ``\textbf{Detailed}'' will list the value each calculation step (i.e.~Zone or HVAC). ``\textbf{Timestep}'' will be the same as ``Detailed'' for Zone valued variables and will be aggregated to the Zone timestep (i.e.~Timestep in Hour value) for HVAC variables. ``\textbf{Hourly}'' will aggregate the value to the hour. ``\textbf{Daily}'' will aggregate to the day (i.e.~one value per day). ``\textbf{Monthly}'' will aggregate to the month (i.e.~one value per month). ``\textbf{RunPeriod}'' will aggregate to the runperiod specified (each Design Day is a runperiod as is each runperiod object). Default for this field if left blank or omitted is \textbf{Hourly}.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-004}
+
+The final field is a schedule name. This can be used to limit the number of lines that appear in your output file. For example, a schedule such as ``ON PEAK'' or ``OFF PEAK'' could provide a slice of values. Or, a seasonal schedule could be devised. The output variable will be active during any hour in which the schedule value is \textgreater{}0. For daily, monthly, and environment reporting frequencies, the aggregate value will be only for active schedule hours. Summed variables will report the sum for the active hours only. Averaged variables will report the average during the active hours only. If Schedule\_Name is omitted, the output variable will be active for all hours.
+
+Other IDF examples:
+
+\begin{lstlisting}
+Output:Variable, * , Zone Mean Air Temperature, hourly;
+Output:Variable, * , Zone Mean Radiant Temperature, timestep;
+Output:Variable, * , Zone Air System Sensible Heating Energy, hourly;
+Output:Variable, * , Zone Air System Sensible Cooling Energy, hourly;
+Output:Variable, * , Zone Air Temperature, hourly;
+Output:Variable, * , Zone Air Temperature;  ! same as previous line
+\end{lstlisting}
+
+\subsection{Output:\-Meter and Output:\-Meter:\-Meter\-File\-Only}\label{outputmeter-and-outputmetermeterfileonly}
+
+\subsection{Output:\-Meter:\-Cumulative and Output:\-Meter:\-Cumulative:\-Meter\-File\-Only}\label{outputmetercumulative-and-outputmetercumulativemeterfileonly}
+
+Appropriate variables are grouped onto ``meters'' for reporting purposes.~ (The meters available are listed in the eplusout.mdd file, see Variable Dictionary Report section.) If the ``Output:Meter'' input object is used, these results written out to both the \textbf{eplusout.eso} and \textbf{eplusout.mtr} files. This allows easy graphing and comparison with ``normal'' values (such as Zone Temperature or Outdoor Temperature). If the ``Output:Meter:MeterFileOnly'' input object is used, then the values results written out to only the \textbf{eplusout.mtr} file. The \textbf{eplusout.mtr} file has the same structure as the \textbf{eplusout.eso} file. A companion file, the \textbf{eplusout.mtd} file, contains a detailed list and explanation of all meters for a given run and the component values that are accumulated on each meter.
+
+The cumulative meter outputs (Output:Meter:Cumulative and Output:\-Meter:\-Cumulative:\-Meter\-File\-Only) use the same meter names but the output is cumulative for the reporting (for each environment). That is, if the reporting frequency for the cumulative meter output is hourly, then hour 1 value will be that for hour 1, hour 2 value will be hour1 + hour2, etc. In other words, the end value for a cumulative meter reporting should be identical if you reported the value of the meter at the RunPeriod frequency.
+
+\subsubsection{Field: Name}\label{field-name-1-036}
+
+Meter names applicable for the simulation are shown on the Variable Dictionary Report contained in the \textbf{eplusout.mdd} file described in the Output Details and Examples document.
+
+Meter names are of three forms:
+
+\begin{itemize}
+\tightlist
+\item
+  \textless{}ResourceType\textgreater{}:\textless{}name\textgreater{}
+\end{itemize}
+
+Or
+
+\begin{itemize}
+\tightlist
+\item
+  \textless{}EndUseType\textgreater{}:\textless{}ResourceType\textgreater{}:\textless{}name\textgreater{}
+\end{itemize}
+
+Or
+
+\begin{itemize}
+\tightlist
+\item
+  \textless{}EndUseSubcategory\textgreater{}:\textless{}EndUseType\textgreater{}:\textless{}ResourceType\textgreater{}:\textless{}name\textgreater{}.
+\end{itemize}
+
+The user requests reporting by either specifying the full name above (without Units) or a ``wildcard'' representation of that name (to obtain all meters of a type). For example, entering ``Electricity:*'' for the meter name will report on all the Electricity: meters (Electricity:Facility, Electricity:Building, Electricity:Zone:Resistive Zone, Electricity:Zone:East Zone, Electricity:North Zone in the example above). Both the resource types and end-use types are set within the program by the developers. End-use subcategories are user-defined and are an input field for certain objects.
+
+To summarize the previous paragraph, you could use:
+
+\begin{lstlisting}
+Output:Meter,Electricity:*;
+\end{lstlisting}
+
+To get the same outputs as if you had entered:
+
+\begin{lstlisting}
+Output:Meter,Electricity:Facility;
+Output:Meter,Electricity:Building;
+Output:Meter,Electricity:Zone:South Zone;
+Output:Meter,Electricity:Zone:East Zone;
+Output:Meter,Electricity:North Zone;
+\end{lstlisting}
+
+From a three zone file that had no HVAC electricity (i.e., had only electric equipment or lighting equipment in an uncontrolled three zone building).
+
+Current resource types are shown in the table below:
+
+% table 38
+\begin{longtable}[c]{@{}l@{}}
+\caption{Table of Metered Resource  Types \label{table:table-of-metered-resource-types}} \tabularnewline
+\toprule 
+Utility/Fuel Types \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table of Metered Resource  Types} \tabularnewline
+\toprule 
+Utility/Fuel Types \tabularnewline
+\midrule
+\endhead
+
+Electricity \tabularnewline
+Gas \tabularnewline
+Gasoline \tabularnewline
+Diesel \tabularnewline
+Coal \tabularnewline
+FuelOil\#1 \tabularnewline
+FuelOil\#2 \tabularnewline
+Propane \tabularnewline
+OtherFuel1 \tabularnewline
+OtherFuel2 \tabularnewline
+Water \tabularnewline
+Steam \tabularnewline
+DistrictCooling \tabularnewline
+DistrictHeating \tabularnewline
+ElectricityPurchased \tabularnewline
+ElectricitySurplusSold \tabularnewline
+ElectricityNet \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Electricity:Facility & Diesel:Facility \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Electricity:Facility & Diesel:Facility \tabularnewline
+\midrule
+\endhead
+
+DistrictCooling:Facility & DistrictHeating:Facility \tabularnewline
+Gas:Facility & Gasoline:Facility \tabularnewline
+Coal:Facility & FuelOil\#1:Facility \tabularnewline
+FuelOil\#2:Facility & Propane:Facility \tabularnewline
+ElectricityProduced:Facility & Steam:Facility \tabularnewline
+OtherFuel1:Facility & OtherFuel2:Facility \tabularnewline
+\bottomrule
+\end{longtable}
+
+The end use types are shown in the following table (note that certain end use types apply only to the EnergyTransfer resource):
+
+% table 39
+\begin{longtable}[c]{@{}l@{}}
+\caption{End Use Category Types \label{table:end-use-category-types}} \tabularnewline
+\toprule 
+Utility/Fuel End Use Types \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{End Use Category Types} \tabularnewline
+\toprule 
+Utility/Fuel End Use Types \tabularnewline
+\midrule
+\endhead
+
+InteriorLights \tabularnewline
+ExteriorLights \tabularnewline
+InteriorEquipment \tabularnewline
+ExteriorEquipment \tabularnewline
+Fans \tabularnewline
+Pumps \tabularnewline
+Heating \tabularnewline
+Cooling \tabularnewline
+HeatRejection \tabularnewline
+Humidifier \tabularnewline
+HeatRecovery \tabularnewline
+DHW \tabularnewline
+Cogeneration \tabularnewline
+Refrigeration \tabularnewline
+WaterSystems \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Electricity:Facility & Diesel:Facility \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Electricity:Facility & Diesel:Facility \tabularnewline
+\midrule
+\endhead
+
+DistrictCooling:Facility & DistrictHeating:Facility \tabularnewline
+Gas:Facility & Gasoline:Facility \tabularnewline
+Coal:Facility & FuelOil\#1:Facility \tabularnewline
+FuelOil\#2:Facility & Propane:Facility \tabularnewline
+ElectricityProduced:Facility & Steam:Facility \tabularnewline
+OtherFuel1:Facility & OtherFuel2:Facility \tabularnewline
+\bottomrule
+\end{longtable}
+
+Specific meter types are then used for grouping the fuel type meters:
+
+% table 40
+\begin{longtable}[c]{@{}l@{}}
+\caption{Overall Meter Types \label{table:overall-meter-types}} \tabularnewline
+\toprule 
+Meters \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Overall Meter Types} \tabularnewline
+\toprule 
+Meters \tabularnewline
+\midrule
+\endhead
+
+Facility \tabularnewline
+Building \tabularnewline
+Zone \tabularnewline
+HVAC \tabularnewline
+Plant \tabularnewline
+\bottomrule
+\end{longtable}
+
+Facility meters contain all the energy of a fuel type. Building meters contain the sum of each zone's energy. HVAC meters contain the energy from the air and zone HVAC system components. Plant meters contain the energy from the plant equipment.
+
+Thus, the following relationships should be observed:
+
+\begin{equation}
+Facility = \sum {\left( {Building + HVAC + Plant + Exterior} \right)}
+\end{equation}
+
+\begin{equation}
+Building = \sum\limits_1^{NumberOfZones} {Zone}
+\end{equation}
+
+There are also some special purpose meters used to describe electricity resource flows in greater detail.~ Electricity metering is tracked in more detail to accommodate the complexities of onsite electricity generation.~ There are three variations on the electricity resource type including:~ (1) ``ElectrictyPurchased'' which is the quantity of electricity purchased and is always positive, (2) ``ElectricitySold'' which is the quantity of electricity exported by the building, that which is typically ``sold'' back to the power company, and is always positive, and (3) ``ElectricityNet'' which is the net electricity demand considering all sources of onsite generation and demand and can be either positive or negative.
+
+\subsubsection{Field: Reporting Frequency}\label{field-reporting-frequency-1}
+
+Similar to the output variables, meters can be reported at different frequencies. Their resolution is the Zone Timestep interval (Number of Timesteps input). For this frequency, the elemental value of the meter will be reported. For more inclusive frequencies, the summed value along with the maximum and minimum values for the time interval will be reported. Default for this field if left blank or omitted is \textbf{Hourly}.
+
+Examples of specifying the object in the IDF follow.
+
+\begin{lstlisting}
+
+Output:Meter,Electricity:*,RunPeriod;
+  Output:Meter,ExteriorEquipment*,RunPeriod;
+  Output:Meter:Cumulative,Electricity:*,Monthly;
+\end{lstlisting}
+
+\subsubsection{Meter Details File (eplusout.mtd)}\label{meter-details-file-eplusout.mtd}
+
+The meter details file illustrates what is on each meter and vice versa.~ It is described in the Output Details and Examples document under the file name.
+
+\subsection{Output:EnvironmentalImpactFactors}\label{outputenvironmentalimpactfactors}
+
+The Output:EnvironmentalImpactFactors object triggers the necessary Facility meters to be reported and the Pollutants resulting from these on and off-site energy consumptions. These values are put into the eplusout.mtr file. Facility meters contain all the energy of a fuel type. Thus, the following relationships should be observed:
+
+\begin{equation}
+Facility = \sum {\left( {Building + System + Plant + Exterior} \right)}
+\end{equation}
+
+Information regarding how the coefficients are derived and applied can be found in the Engineering Document.
+
+To turn on the reporting and the calculations for the environmental factors the user enters 3 objects:
+
+\textbf{Output:EnvironmentalImpactFactors:} (with associated reporting frequency, more than one frequency can be requested)
+
+\textbf{EnvironmentalImpactFactors:} (contains additional information necessary for the calculations not included in the Fuel Factors)
+
+\textbf{FuelFactors:} (required for every fuel that is simulated and converted in this simulation input file)
+
+Users will enter environmental impact factors for each Fuel Type or FuelFactor. This is the same for each Fuel Type: Natural Gas, Residual Oil, Distillate Oil, Coal, Off-Site Electricity, Gasoline, and Propane. For District Heating, District Cooling, and Steam there are additional fields in the EnvironmentalImpactFactors object that help in the conversion of their energy to Natural Gas and Electricity.
+
+The energy is obtained internally from the following facility meters:
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Electricity:Facility & Diesel:Facility \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Electricity:Facility & Diesel:Facility \tabularnewline
+\midrule
+\endhead
+
+DistrictCooling:Facility & DistrictHeating:Facility \tabularnewline
+Gas:Facility & Gasoline:Facility \tabularnewline
+Coal:Facility & FuelOil\#1:Facility \tabularnewline
+FuelOil\#2:Facility & Propane:Facility \tabularnewline
+ElectricityProduced:Facility & Steam:Facility \tabularnewline
+OtherFuel1:Facility & OtherFuel2:Facility \tabularnewline
+\bottomrule
+\end{longtable}
+
+For the pollutant calculation only the total off-site or purchased electric energy is calculated using Electricity Factors. Off-Site Electricity = Electricity:Facility - ElectricityProduced:Facility, pollutants for the fuel type used by the on-site generator will be calculated, for example Diesel, in these cases.
+
+\subsubsection{Inputs}\label{inputs-9-017}
+
+\paragraph{Field: Reporting Frequency}\label{field-reporting-frequency-2}
+
+Similar to the output variables and meters the environmental impact calculations can be reported at different frequencies. Their resolution is the Zone Timestep interval (Number of Timesteps input). For this frequency, the elemental value of the Environmental Impact Factors Calculation will be reported. For more inclusive frequencies, the summed value along with the maximum and minimum values for the time interval will be reported.
+
+Valid values are Timestep, Hourly, Daily, Monthly or RunPeriod.
+
+An example of specifying in the IDF:
+
+\begin{lstlisting}
+Output:EnvironmentalImpactFactors,
+  Monthly;  !- Reporting_Frequency
+\end{lstlisting}
+
+\subsection{EnvironmentalImpactFactors}\label{environmentalimpactfactors}
+
+The EnvironmentalImpactFactors object contains additional information that is not individually specified in the FuelFactors object and is the second object needed to complete the calculation.~ Source to Site conversion factors for District Heating, District Cooling and Steam are entered in this object.
+
+\subsubsection{Inputs}\label{inputs-10-017}
+
+\paragraph{Field: District Heating Efficiency}\label{field-district-heating-efficiency}
+
+The District Heating Efficiency value is used to convert the district (purchased) heating energy to Natural Gas for the environmental impact calculation. The efficiency is a number between 0 and 1 and divided into the district heating energy and the default is 0.3.
+
+\paragraph{Field: Disctrict Cooling COP}\label{field-disctrict-cooling-cop}
+
+The District Cooling COP value is used to convert the district (purchased) cooling energy to electricity for the environmental impact calculation. The Coefficient of Performance (COP) is a number greater than 0 and divided into the purchased cooling energy with a default of 3.0.
+
+\paragraph{Field: Steam Conversion Efficiency}\label{field-steam-conversion-efficiency}
+
+The Steam Conversion Efficiency is used to convert the Steam usage to Natural Gas for the environmental impact calculation. The efficiency is a number between 0 and 1 and divided into the purchased heating energy and the default is 0.25.
+
+\paragraph{Field: Total Carbon Equivalent Emission Factor From N2O}\label{field-total-carbon-equivalent-emission-factor-from-n2o}
+
+The Intergovernmental Panel on Climate Change has studied the effects on the relative radiative forcing effects of various greenhouse gases. This effect, called Global Warming Potential (GWP), is described in terms of the Carbon Equivalent of a particular greenhouse gase. N\(_{2}\)O (nitrous oxide) can be produced by some Fuel Types and has a default of carbon equivalent emission factor of 80.7272 kg C/kg N\(_{2}\)O.
+
+\paragraph{Field: Total Carbon Equivalent Emission Factor From CH4}\label{field-total-carbon-equivalent-emission-factor-from-ch4}
+
+The Intergovernmental Panel on Climate Change has studied the effects on the relative radiative forcing effects of various greenhouse gases. This effect, called Global Warming Potential (GWP), is described in terms of the Carbon Equivalent of a particular greenhouse gas. CH\(_{4}\) (methane) can be produced by all Fuel Types and has a default carbon equivalent emission factor of 6.2727 kg C/kg CH\(_{4}\).
+
+\paragraph{Field: Total Carbon Equivalent Emission Factor From CO2}\label{field-total-carbon-equivalent-emission-factor-from-co2}
+
+The Intergovernmental Panel on Climate Change has studied the effects on the relative radiative forcing effects of various greenhouse gases. This effect, called Global Warming Potential (GWP), is described in terms of the Carbon Equivalent of a particular greenhouse gas. CO\(_{2}\) (carbon dioxide) can be produced by all Fuel Types and has a default carbon equivalent emission factor of 0.2727 kg C/kg CO\(_{2}\).
+
+An example of specifying in the IDF:
+
+\begin{lstlisting}
+EnvironmentalImpactFactors,
+  0.3,         !- Disctrict Heating Efficiency
+  3.0,         !- District Cooling COP
+  0.25,        !- Steam Conversion Efficiency
+  80.7272,     !- Total Carbon Equivalent Emission Factor From N2O
+  6.2727,      !- Total Carbon Equivalent Emission Factor From CH4
+  0.2727;      !- Total Carbon Equivalent Emission Factor From CO2
+\end{lstlisting}
+
+\subsection{FuelFactors}\label{fuelfactors}
+
+\subsubsection{Inputs}\label{inputs-11-015}
+
+\paragraph{Field: Existing Fuel Resource Name}\label{field-existing-fuel-resource-name}
+
+This is the name of the Fuel that is being described with this object. Source to Site conversion factors for each tool are entered with these objects. Allowable Fuel Types are:~ Electricity, Natural Gas, FuelOil\#1, FuelOil\#2, Coal, Gasoline, Propane, Diesel, OtherFuel1, OtherFuel2.
+
+\paragraph{Field: Units of Measure}\label{field-units-of-measure}
+
+Units in mass with kg or by volume in m3.
+
+\paragraph{Field: Energy per Unit Factor}\label{field-energy-per-unit-factor}
+
+The higher heating value of the fuel type.
+
+\paragraph{Field: Source Energy Factor}\label{field-source-energy-factor}
+
+Multiplied by the fuel consumption to compute the source energy contribution for the fuel. If a schedule is also specified in the next field, the value specified here, the schedule value, and the fuel consumption are multiplied together for each timestep to determine the source energy contribution for the fuel. If the multipliers in the schedule specified in the next field fully represent the source energy conversion factor, the value in this field should be set to one. If the TDV files (described in next field) are used the value should be 0.293 for electricity and 0.01 for natural gas to account for the units used in the files. Units of J/J.
+
+\paragraph{Field: Source Energy Schedule Name}\label{field-source-energy-schedule-name}
+
+This field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the source energy. Specifically, each value in the schedule are multiplied by the Source Energy Factor field value and by the fuel consumption to determine the source energy consumption for the fuel. If the values in the schedule fully represent the source energy conversion factor, the value in the previous field, Source Energy Factor should be set to one.
+
+The use of this field is required for evaluations using source energy factors that change throughout the year such as Time Dependent Valuation (TDV), the method used to show compliance with to California's Title 24 under the ACM (Alternative Compliance Method). Data files containing TDV factors are in the DataSets\textbackslash{}TDV\textbackslash{} directory. An example file for use with TDV file is in the ExampleFiles directory and is named 5zoneTDV.IDF. When using these TDV files with EnergyPlus it is important that a consistent weather file be used. It is also important that the day of the week for January 1 is set to Tuesday since all the TDV and related weather files use 1991 as the year of reference. Also note that the values in the TDV datasets files are in non SI units of measure. The source energy factor field should contain the value of 0.293 for electricity and 0.01 for natural gas to account for the non-standard units used in the files. A summary report that provides a breakdown of the facility energy use in terms of source energy can be obtained by selecting the `\emph{AllSummary}' or `\emph{SourceEnergyEndUseComponentsSummary}' keywords in the `Output:Table:SummaryReports' reporting object. To learn more about TDV see:
+
+http://www.energy.ca.gov/title24/2005standards/archive/rulemaking/documents/tdv/index.html
+
+\textbf{WARNING}
+
+\textbf{THE TDV CALCULATIONS SHOULD ONLY BE PERFORMED ON SIMULATIONS THAT USE THE CALIFORNIA THERMAL ZONE (CTZ REV2) WEATHER FILES. One must match the correct TDV file to its corresponding CTZ weather file. There are 16 TDV files, one for each of the 16 CTZ weather files. The Time Dependent Valuation of TDV files provides a relative cost estimate of the various fuel sources and their relative costs by time of day, month of year and outside temperature. Outside temperature is important as demand for electricity and thus cost of electricity is influenced by temperature. These TDV files are applicable only to the hourly weather data contained in the California Thermal Zone (CTZ rev2) weather files as the time dependent cost information is partially derived from the timing of temperatures in the weather file. Thus using the TDV files with other weather data would provide meaningless results.}
+
+\paragraph{Field: CO2 Emission Factor}\label{field-co2-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the mass of carbon dioxide (CO\(_{2}\)) released into the atmosphere. The units are grams per MegaJoule. Carbon dioxide gas is naturally produced by animals during respiration and through decay of biomass, and used by plants during photosynthesis. Although it only constitutes 0.04 percent of the atmosphere, it is one of the most important greenhouse gases. The combustion of fossil fuels is increasing carbon dioxide concentrations in the atmosphere, which is believed to be contributing to global warming.
+
+\paragraph{Field: CO2 Emission Factor Schedule Name}\label{field-co2-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: CO Emission Factor}\label{field-co-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the mass of carbon monoxide (CO) released into the atmosphere. The units are grams per MegaJoule. Carbon monoxide is a colorless, odorless and poisonous gas produced by incomplete fossil fuel combustion. Carbon monoxide combines with the haemoglobin of human beings, reducing its oxygen carrying capacity, with effects harmful to human beings.
+
+\paragraph{Field: CO Emission Factor Schedule Name}\label{field-co-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: CH4 Emission Factor}\label{field-ch4-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the mass of methane (CH\(_{4}\)) released into the atmosphere. The units are grams per MegaJoule. Methane is a colorless, nonpoisonous, flammable gas created by anaerobic decomposition of organic compounds and is one of the more potent greenhouse gases. A major component of natural gas used in the home.
+
+\paragraph{Field: CH4 Emission Factor Schedule Name}\label{field-ch4-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: NOx Emission Factor}\label{field-nox-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the mass of nitrogen oxides (NO\(_{x}\)) released into the atmosphere. The units are grams per MegaJoule. Nitrogen oxides refers to nitric oxide gas (NO) and nitrogen dioxide gas (NO\(_{2}\)) and many other gaseous oxides containing nitrogen. The main source of these gases in urban areas are motor vehicle exhaust and indoor gas stoves and kerosene heaters. The brown haze sometimes seen over cities is mainly nitrogen oxides. These gases are also partly responsible for the generation of ozone, which is produced when nitrogen oxides react with other chemicals in the presence of sunlight. Exposure to high levels of nitrogen dioxide can interfere with the ability of blood to carry oxygen, leading to dizziness and shortness of breath. Prolonged exposure can lead to respiratory failure.
+
+\paragraph{Field: NOx Emission Factor Schedule Name}\label{field-nox-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: N2O Emission Factor}\label{field-n2o-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the mass of nitrous oxide (N\(_{2}\)O) released into the atmosphere. The units are grams per MegaJoule. Relatively inert oxide of nitrogen produced as a result of microbial action in the soil, use of fertilizers containing nitrogen, burning of timber and coil, chemical industry, and so forth. This nitrogen compound may contribute to greenhouse and ozone-depleting effects.
+
+\paragraph{Field: N2O Emission Factor Schedule Name}\label{field-n2o-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: SO2 Emission Factor}\label{field-so2-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the mass of sulfur dioxide (SO\(_{2}\)) released into the atmosphere. The units are in grams per MegaJoule. Sulfur dioxide gas is formed when fuel containing sulfur, such as coal and oil, is burned, and when gasoline is extracted from oil, or metals are extracted from ore. Sulfur dioxide reacts with other chemicals in the air to form tiny sulfate particles, associated with increased respiratory symptoms and disease, difficulty in breathing, and premature death. Sulfur dioxide and nitrogen oxides react with other substances in the air to form acids, which fall to earth as rain, fog, snow, or dry particles. Acid rain damages forests and crops, changes the makeup of soil, and makes lakes and streams acidic and unsuitable for fish. Sulfur dioxide accelerates the decay of building materials and paints.
+
+\paragraph{Field: SO2 Emission Factor Schedule Name}\label{field-so2-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: PM Emission Factor}\label{field-pm-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the mass of particulate matter (PM) released into the atmosphere. The units are grams per MegaJoule. PM is the sum of all particular matter emitted, including PM10 and PM2.5. Particulate matter, or PM, are particles found in the air, including dust, dirt, soot, smoke, and liquid droplets, which can be suspended in the air for long periods of time. Some particles are large or dark enough to be seen as soot or smoke. Others are so small that individually they can only be detected with an electron microscope. Breathing particulate matter is linked to significant respiratory health problems.
+
+\paragraph{Field: PM Emission Factor Schedule Name}\label{field-pm-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: PM10 Emission Factor}\label{field-pm10-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the mass of particulate matter 10 (PM\(_{10}\)) released into the atmosphere. The units are grams per MegaJoule. PM\(_{10}\), includes particles with an aerodynamic diameter of less than 10 microns. These smaller particles are most likely responsible for the adverse health effects on humans because particles so small can reach the thoracic or lower regions of the respiratory tract.
+
+\paragraph{Field: PM10 Emission Factor Schedule Name}\label{field-pm10-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: PM2.5 Emission Factor}\label{field-pm2.5-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the mass of particulate matter 2.5 (PM\(_{2.5}\)) released into the atmosphere. The units are grams per MegaJoule. EPA's national air quality standards for fine particles, also known as ``PM\(_{2.5}\) standards,'' are levels allowed in the outdoor air for particulate matter 2.5 microns in diameter or smaller. EPA issued the PM\(_{2.5}\) standards in 1997 to protect human health and the environment. Studies have linked increased exposure to PM\(_{2.5}\) to increases in premature death as well as a range of serious respiratory and cardiovascular effects.
+
+\paragraph{Field: PM2.5 Emission Factor Schedule Name}\label{field-pm2.5-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: NH3 Emission Factor}\label{field-nh3-emission-factor}
+
+The Environmental impact coefficient for the Fuel for calculating the mass of ammonia (NH\(_{3}\)) released into the atmosphere. The units are grams per MegaJoule. Ammonia reacts with nitrogen and sulfur compounds in the atmosphere, mainly nitric and sulfuric acids, to form particulate matter.
+
+\paragraph{Field: NH3 Emission Factor Schedule Name}\label{field-nh3-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: NMVOC Emission Factor}\label{field-nmvoc-emission-factor}
+
+The Environmental impact coefficient for the Fuel for calculating the mass of non-methane volatile organic compounds (NMVOC) released into the atmosphere. The units are grams per MegaJoule. Non-methane volatile organic compounds (NMVOC), which include propane, butane, and ethane, are emitted primarily from transportation, industrial processes, and non-industrial consumption of organic solvents. Volatile organic compounds react with nitrogen oxides in the atmosphere to form ozone.
+
+\paragraph{Field: NMVOC Emission Factor Schedule Name}\label{field-nmvoc-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: Hg Emission Factor}\label{field-hg-emission-factor}
+
+The Environmental impact coefficient for the Fuel for calculating the mass lof mercury (Hg) released into the atmosphere. The units are grams per MegaJoule. This heavy metal can accumulate in the environment and is highly toxic if breathed or swallowed. In the U.S., primary sources of mercury air emissions are coal-fired power plants.
+
+\paragraph{Field: Hg Emission Factor Schedule Name}\label{field-hg-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: Pb Emission Factor}\label{field-pb-emission-factor}
+
+The Environmental impact coefficient for the Fuel for calculating the masss of lead (Pb) released into the atmosphere. The units are grams per MegaJoule. A heavy metal that is hazardous to health if breathed or swallowed. Its use in gasoline, paints, and plumbing compounds has been sharply restricted or eliminated by federal laws and regulations.
+
+\paragraph{Field: Pb Emission Factor Schedule Name}\label{field-pb-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: Water Emission Factor}\label{field-water-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the volume of water (H\(_{2}\)O) consumed or evaporated in the generation of electricity. The units are liters per MegaJoule or a volume measurement. This is the water consumed in the production of the energy, ie. electricity off-site evaporated in cooling towers or scrubbers, or in the production or processing of the fuel itself, i.e., refinery for gasoline or diesel.
+
+\paragraph{Field: Water Emission Factor Schedule Name}\label{field-water-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: Nuclear High Level Emission Factor}\label{field-nuclear-high-level-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the mass of high-level nuclear waste, removed as spent nuclear fuel from a nuclear reactor once it no longer is efficient at powering the reactor.. The units are grams per MegaJoule. Once a year, approximately one-third of nuclear fuel is replaced with new fuel. This used fuel is called spent nuclear fuel and is highly radioactive; containing plutonium and other radionuclides. Although there is little information on quantities of high-level nuclear waste, a few utilities are beginning to publish this information.
+
+\paragraph{Field: Nuclear High Level Emission Factor Schedule Name}\label{field-nuclear-high-level-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+\paragraph{Field: Nuclear Low Level Emission factor}\label{field-nuclear-low-level-emission-factor}
+
+The environmental impact coefficient for the Fuel for calculating the volume of low-level nuclear waste, removed from a nuclear reactor after radiation contamination. The units are cubic meters per MegaJoule or a volume measurement. Low-level waste can come from nuclear reactors or other users of radioactive material, like hospitals or research institutes. Low-level waste is less hazardous than high-level waste.
+
+\paragraph{Field: Nuclear Low Level Emission Factor Schedule Name}\label{field-nuclear-low-level-emission-factor-schedule-name}
+
+Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
+
+An example of specifying in the IDF:
+
+\begin{lstlisting}
+FuelFactors,          !  USA national average based on eGRID, EIA 1605
+  Electricity,        !- Existing Fuel Resource Name
+  kg,                 !- Units of Measure (kg or m3)
+  ,                   !- Energy per Unit Factor
+  2.253,              !- Source Energy Factor {J/J}
+  ,                   !- Source Energy Schedule Name
+  168.33317,          !- CO2 Emission Factor {g/MJ}
+  ,                   !- CO2 Emission Factor Schedule Name
+  4.20616E-02,        !- CO Emission Factor {g/MJ}
+  ,                   !- CO Emission Factor Schedule Name
+  1.39858E-03,        !- CH4 Emission Factor {g/MJ}
+  ,                   !- CH4 Emission Factor Schedule Name
+  4.10753E-01,        !- NOx Emission Factor {g/MJ}
+  ,                   !- NOx Emission Factor Schedule Name
+  2.41916E-03,        !- N2O Emission Factor {g/MJ}
+  ,                   !- N2O Emission Factor Schedule Name
+  8.65731E-01,        !- SO2 Emission Factor {g/MJ}
+  ,                   !- SO2 Emission Factor Schedule Name
+  2.95827E-02,        !- PM Emission Factor {g/MJ}
+  ,                   !- PM Emission Factor Schedule Name
+  1.80450E-02,        !- PM10 Emission Factor {g/MJ}
+  ,                   !- PM10 Emission Factor Schedule Name
+  1.15377E-02,        !- PM2.5 Emission Factor {g/MJ}
+  ,                   !- PM2.5 Emission Factor Schedule Name
+  1.10837E-03,        !- NH3 Emission Factor {g/MJ}
+  ,                   !- NH3 Emission Factor Schedule Name
+  3.72332E-03,        !- NMVOC Emission Factor {g/MJ}
+  ,                   !- NMVOC Emission Factor Schedule Name
+  3.36414E-06,        !- Hg Emission Factor {g/MJ}
+  ,                   !- Hg Emission Factor Schedule Name
+  0,                  !- Pb Emission Factor {g/MJ}
+  ,                   !- Pb Emission Factor Schedule Name
+  2.10074,            !- Water Emission Factor {L/MJ}
+  ,                   !- Water Emission Factor Schedule Name
+  0,                  !- Nuclear High Level Emission Factor {g/MJ}
+  ,                   !- Nuclear High Level Emission Factor Schedule Name
+  0;                  !- Nuclear Low Level Emission Factor {m3/MJ}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-029}
+
+Various output variables and meters related to emissions are available when modeling with environmental impact and fuel factor inputs. Output is available as either output variables or output meters. The variables and meters available depending on the number of FuelFactor input objects and the type of fuel used in them. Most of the fuel types have the same set of outputs for emissions that correspond to the types of emission factors in the input objects. The exception is electricity which has two additional outputs to track possible net metering situations that can occur with on-site generation.
+
+The following pollution-emission-related outputs are available for environmental impacts.
+
+\begin{itemize}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas CO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas CO Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas CH4 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas NOx Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas N2O Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas SO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas PM Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas PM10 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas PM2.5 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas NH3 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas NMVOC Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas Hg Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas Pb Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas Water Consumption Volume {[}L{]}
+\item
+  HVAC,Sum,Nuclear High Level Waste From Natural Gas {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Natural Gas Nuclear Low Level Waste Volume {[}m3{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity CO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity CO Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity CH4 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity NOx Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity N2O Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity SO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity PM Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity PM10 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity PM2.5 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity NH3 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity NMVOC Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity Hg Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity Pb Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity Water Consumption Volume {[}L{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity Nuclear High Level Waste Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Electricity Nuclear Low Level Waste Volume {[}m3{]}
+\item
+  HVAC,Sum,Environmental Impact Purchased Electricity Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact Surplus Sold Electricity Source {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact Coal Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact Coal CO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal CO Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal CH4 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal NOx Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal N2O Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal SO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal PM Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal PM10 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal PM2.5 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal NH3 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal NMVOC Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal Hg Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal Pb Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal Water Consumption Volume {[}L{]}
+\item
+  HVAC,Sum,Environmental Impact Coal Nuclear High Level Waste Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Coal Nuclear Low Level Waste Volume {[}m3{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 CO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 CO Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 CH4 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 NOx Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 N2O Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 SO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 PM Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 PM10 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 PM2.5 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 NH3 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 NMVOC Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 Hg Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 Pb Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 Water Consumption Volume {[}L{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 Nuclear High Level Waste Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#2 Nuclear Low Level Waste Volume {[}m3{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 CO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 CO Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 CH4 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 NOx Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 N2O Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 SO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 PM Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 PM10 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 PM2.5 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 NH3 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 NMVOC Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 Hg Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 Pb Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 Water Consumption Volume {[}L{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 Nuclear High Level Waste Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Fuel Oil \#1 Nuclear Low Level Waste Volume {[}m3{]}
+\item
+  HVAC,Sum,Environmental Impact Propane Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact Propane CO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane CO Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane CH4 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane NOx Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane N2O Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane SO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane PM Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane PM10 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane PM2.5 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane NH3 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane NMVOC Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane Hg Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane Pb Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane Water Consumption Volume {[}L{]}
+\item
+  HVAC,Sum,Environmental Impact Propane Nuclear High Level Waste Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Propane Nuclear Low Level Waste Volume {[}m3{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline CO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline CO Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline CH4 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline NOx Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline N2O Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline SO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline PM Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline PM10 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline PM2.5 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline NH3 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline NMVOC Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline Hg Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline Pb Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline Water Consumption Volume {[}L{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline Nuclear High Level Waste Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Gasoline Nuclear Low Level Waste Volume {[}m3{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel CO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel CO Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel CH4 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel NOx Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel N2O Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel SO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel PM Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel PM10 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel PM2.5 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel NH3 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel NMVOC Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel Hg Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel Pb Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel Water Consumption Volume {[}L{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel Nuclear High Level Waste Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Diesel Nuclear Low Level Waste Volume {[}m3{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 CO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 CO Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 CH4 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 NOx Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 N2O Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 SO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 PM Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 PM10 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 PM2.5 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 NH3 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 NMVOC Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 Hg Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 Pb Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 Water Consumption Volume {[}L{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 Nuclear High Level Waste Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel1 Nuclear Low Level Waste Volume {[}m3{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 Source Energy {[}J{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 CO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 CO Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 CH4 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 NOx Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 N2O Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 SO2 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 PM Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 PM10 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 PM2.5 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 NH3 Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 NMVOC Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 Hg Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 Pb Emissions Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 Water Consumption Volume {[}L{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 Nuclear High Level Waste Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact OtherFuel2 Nuclear Low Level Waste Volume {[}m3{]}
+\item
+  HVAC,Sum,Environmental Impact Total N2O Emissions Carbon Equivalent Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Total CH4 Emissions Carbon Equivalent Mass {[}kg{]}
+\item
+  HVAC,Sum,Environmental Impact Total CO2 Emissions Carbon Equivalent Mass {[}kg{]}
+\end{itemize}
+
+\paragraph{Environmental Impact Electricity Source Energy {[}J{]}}\label{environmental-impact-electricity-source-energy-j}
+
+\paragraph{Environmental Impact Purchased Electricity Source Energy {[}J{]}}\label{environmental-impact-purchased-electricity-source-energy-j}
+
+\paragraph{Environmental Impact Surplus Sold Electricity Source {[}J{]}}\label{environmental-impact-surplus-sold-electricity-source-j}
+
+\paragraph{Environmental Impact Natural Gas Source Energy {[}J{]}}\label{environmental-impact-natural-gas-source-energy-j}
+
+\paragraph{Environmental Impact Fuel Oil \#2 Source Energy {[}J{]}}\label{environmental-impact-fuel-oil-2-source-energy-j}
+
+\paragraph{Environmental Impact Fuel Oil \#1 Source Energy {[}J{]}}\label{environmental-impact-fuel-oil-1-source-energy-j}
+
+\paragraph{Environmental Impact Coal Source Energy {[}J{]}}\label{environmental-impact-coal-source-energy-j}
+
+\paragraph{Environmental Impact Gasoline Source Energy {[}J{]}}\label{environmental-impact-gasoline-source-energy-j}
+
+\paragraph{Environmental Impact Propane Source Energy {[}J{]}}\label{environmental-impact-propane-source-energy-j}
+
+\paragraph{Environmental Impact Diesel Source Energy {[}J{]}}\label{environmental-impact-diesel-source-energy-j}
+
+\paragraph{Environmental Impact OtherFuel1 Source Energy {[}J{]}}\label{environmental-impact-otherfuel1-source-energy-j}
+
+\paragraph{Environmental Impact OtherFuel2 Source Energy {[}J{]}}\label{environmental-impact-otherfuel2-source-energy-j}
+
+These outputs provide results for the source energy embodied in each type of fuel that might be used at the site.~ The units are Joules. The EnergyPlus models energy use at the site and conversion factors are used to determine the added energy used to create, process or deliver a fuel to the building.~ There are three types of electricity-related source energy results available.~ The first ``Environmental Impact Electricity Source Energy'' is for the electricity consumed at the site that was not produced at the site.~ The second, ``Environmental Impact Purchased Electricity Source Energy,'' is similar but includes just the electricity purchased form the utility.~ The third, ``Environmental Impact Surplus Sold Electricity Source,'' is the source energy associated with any surplus electricity that is exported to the grid.
+
+\paragraph{Environmental Impact Electricity CO2 Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-co2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas CO2 Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-co2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 CO2 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-co2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 CO2 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-co2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal CO2 Emissions Mass {[}kg{]}}\label{environmental-impact-coal-co2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline CO2 Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-co2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane CO2 Emissions Mass {[}kg{]}}\label{environmental-impact-propane-co2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel CO2 Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-co2-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 CO2 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-co2-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 CO2 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-co2-emissions-mass-kg}
+
+These outputs provide results for the carbon dioxide reelases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity CO Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-co-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas CO Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-co-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 CO Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-co-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 CO Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-co-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal CO Emissions Mass {[}kg{]}}\label{environmental-impact-coal-co-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline CO Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-co-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane CO Emissions Mass {[}kg{]}}\label{environmental-impact-propane-co-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel CO Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-co-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 CO Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-co-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 CO Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-co-emissions-mass-kg}
+
+These outputs provide results for the carbon monoxide releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity CH4 Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-ch4-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas CH4 Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-ch4-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 CH4 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-ch4-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 CH4 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-ch4-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal CH4 Emissions Mass {[}kg{]}}\label{environmental-impact-coal-ch4-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline CH4 Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-ch4-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane CH4 Emissions Mass {[}kg{]}}\label{environmental-impact-propane-ch4-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel CH4 Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-ch4-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 CH4 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-ch4-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 CH4 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-ch4-emissions-mass-kg}
+
+These outputs provide results for the methane releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity NOx Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-nox-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas NOx Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-nox-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 NOx Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-nox-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 NOx Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-nox-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal NOx Emissions Mass {[}kg{]}}\label{environmental-impact-coal-nox-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline NOx Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-nox-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane NOx Emissions Mass {[}kg{]}}\label{environmental-impact-propane-nox-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel NOx Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-nox-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 NOx Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-nox-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 NOx Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-nox-emissions-mass-kg}
+
+These outputs provide results for the various nitrogen oxide releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity N2O Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-n2o-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas N2O Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-n2o-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 N2O Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-n2o-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 N2O Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-n2o-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal N2O Emissions Mass {[}kg{]}}\label{environmental-impact-coal-n2o-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline N2O Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-n2o-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane N2O Emissions Mass {[}kg{]}}\label{environmental-impact-propane-n2o-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel N2O Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-n2o-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 N2O Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-n2o-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 N2O Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-n2o-emissions-mass-kg}
+
+These outputs provide results for the nitrous oxide releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity SO2 Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-so2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas SO2 Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-so2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 SO2 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-so2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 SO2 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-so2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal SO2 Emissions Mass {[}kg{]}}\label{environmental-impact-coal-so2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline SO2 Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-so2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane SO2 Emissions Mass {[}kg{]}}\label{environmental-impact-propane-so2-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel SO2 Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-so2-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 SO2 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-so2-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 SO2 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-so2-emissions-mass-kg}
+
+These outputs provide results for the sulphur dioxide releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity PM Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-pm-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas PM Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-pm-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 PM Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-pm-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 PM Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-pm-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal PM Emissions Mass {[}kg{]}}\label{environmental-impact-coal-pm-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline PM Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-pm-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane PM Emissions Mass {[}kg{]}}\label{environmental-impact-propane-pm-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel PM Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-pm-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 PM Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-pm-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 PM Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-pm-emissions-mass-kg}
+
+These outputs provide results for particulate matter releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity PM10 Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-pm10-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas PM10 Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-pm10-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 PM10 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-pm10-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 PM10 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-pm10-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal PM10 Emissions Mass {[}kg{]}}\label{environmental-impact-coal-pm10-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline PM10 Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-pm10-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane PM10 Emissions Mass {[}kg{]}}\label{environmental-impact-propane-pm10-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel PM10 Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-pm10-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 PM10 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-pm10-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 PM10 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-pm10-emissions-mass-kg}
+
+These outputs provide results for particulate matter of 10 microns or less releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity PM2.5 Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-pm2.5-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas PM2.5 Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-pm2.5-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 PM2.5 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-pm2.5-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 PM2.5 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-pm2.5-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal PM2.5 Emissions Mass {[}kg{]}}\label{environmental-impact-coal-pm2.5-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline PM2.5 Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-pm2.5-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane PM2.5 Emissions Mass {[}kg{]}}\label{environmental-impact-propane-pm2.5-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel PM2.5 Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-pm2.5-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 PM2.5 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-pm2.5-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 PM2.5 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-pm2.5-emissions-mass-kg}
+
+These outputs provide results for particulate matter of 2.5 microns or less releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity NH3 Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-nh3-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas NH3 Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-nh3-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 NH3 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-nh3-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 NH3 Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-nh3-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal NH3 Emissions Mass {[}kg{]}}\label{environmental-impact-coal-nh3-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline NH3 Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-nh3-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane NH3 Emissions Mass {[}kg{]}}\label{environmental-impact-propane-nh3-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel NH3 Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-nh3-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 NH3 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-nh3-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 NH3 Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-nh3-emissions-mass-kg}
+
+These outputs provide results for ammonia releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity NMVOC Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-nmvoc-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas NMVOC Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-nmvoc-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 NMVOC Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-nmvoc-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 NMVOC Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-nmvoc-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal NMVOC Emissions Mass {[}kg{]}}\label{environmental-impact-coal-nmvoc-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline NMVOC Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-nmvoc-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane NMVOC Emissions Mass {[}kg{]}}\label{environmental-impact-propane-nmvoc-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel NMVOC Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-nmvoc-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 NMVOC Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-nmvoc-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 NMVOC Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-nmvoc-emissions-mass-kg}
+
+These outputs provide results for non-methane volatile organic compound releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity Hg Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-hg-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas Hg Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-hg-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 Hg Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-hg-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 Hg Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-hg-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal Hg Emissions Mass {[}kg{]}}\label{environmental-impact-coal-hg-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline Hg Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-hg-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane Hg Emissions Mass {[}kg{]}}\label{environmental-impact-propane-hg-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel Hg Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-hg-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 Hg Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-hg-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 Hg Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-hg-emissions-mass-kg}
+
+These outputs provide results for mercury releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity Pb Emissions Mass {[}kg{]}}\label{environmental-impact-electricity-pb-emissions-mass-kg}
+
+\paragraph{Environmental Impact Natural Gas Pb Emissions Mass {[}kg{]}}\label{environmental-impact-natural-gas-pb-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 Pb Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-pb-emissions-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 Pb Emissions Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-pb-emissions-mass-kg}
+
+\paragraph{Environmental Impact Coal Pb Emissions Mass {[}kg{]}}\label{environmental-impact-coal-pb-emissions-mass-kg}
+
+\paragraph{Environmental Impact Gasoline Pb Emissions Mass {[}kg{]}}\label{environmental-impact-gasoline-pb-emissions-mass-kg}
+
+\paragraph{Environmental Impact Propane Pb Emissions Mass {[}kg{]}}\label{environmental-impact-propane-pb-emissions-mass-kg}
+
+\paragraph{Environmental Impact Diesel Pb Emissions Mass {[}kg{]}}\label{environmental-impact-diesel-pb-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 Pb Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel1-pb-emissions-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 Pb Emissions Mass {[}kg{]}}\label{environmental-impact-otherfuel2-pb-emissions-mass-kg}
+
+These outputs provide results for lead releases associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity Water Consumption Volume {[}L{]}}\label{environmental-impact-electricity-water-consumption-volume-l}
+
+\paragraph{Environmental Impact Natural Gas Water Consumption Volume {[}L{]}}\label{environmental-impact-natural-gas-water-consumption-volume-l}
+
+\paragraph{Environmental Impact Fuel Oil \#2 Water Consumption Volume {[}L{]}}\label{environmental-impact-fuel-oil-2-water-consumption-volume-l}
+
+\paragraph{Environmental Impact Fuel Oil \#1 Water Consumption Volume {[}L{]}}\label{environmental-impact-fuel-oil-1-water-consumption-volume-l}
+
+\paragraph{Environmental Impact Coal Water Consumption Volume {[}L{]}}\label{environmental-impact-coal-water-consumption-volume-l}
+
+\paragraph{Environmental Impact Gasoline Water Consumption Volume {[}L{]}}\label{environmental-impact-gasoline-water-consumption-volume-l}
+
+\paragraph{Environmental Impact Propane Water Consumption Volume {[}L{]}}\label{environmental-impact-propane-water-consumption-volume-l}
+
+\paragraph{Environmental Impact Diesel Water Consumption Volume {[}L{]}}\label{environmental-impact-diesel-water-consumption-volume-l}
+
+\paragraph{Environmental Impact OtherFuel1 Water Consumption Volume {[}L{]}}\label{environmental-impact-otherfuel1-water-consumption-volume-l}
+
+\paragraph{Environmental Impact OtherFuel2 Water Consumption Volume {[}L{]}}\label{environmental-impact-otherfuel2-water-consumption-volume-l}
+
+These outputs provide results for water consumption or evaporation associated with consumption of each type of fuel that might be used at the site.~ The units are liters.
+
+\paragraph{Environmental Impact Electricity Nuclear High Level Waste Mass {[}kg{]}}\label{environmental-impact-electricity-nuclear-high-level-waste-mass-kg}
+
+\paragraph{Nuclear High Level Waste From Natural Gas {[}kg{]}}\label{nuclear-high-level-waste-from-natural-gas-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#2 Nuclear High Level Waste Mass {[}kg{]}}\label{environmental-impact-fuel-oil-2-nuclear-high-level-waste-mass-kg}
+
+\paragraph{Environmental Impact Fuel Oil \#1 Nuclear High Level Waste Mass {[}kg{]}}\label{environmental-impact-fuel-oil-1-nuclear-high-level-waste-mass-kg}
+
+\paragraph{Environmental Impact Coal Nuclear High Level Waste Mass {[}kg{]}}\label{environmental-impact-coal-nuclear-high-level-waste-mass-kg}
+
+\paragraph{Environmental Impact Gasoline Nuclear High Level Waste Mass {[}kg{]}}\label{environmental-impact-gasoline-nuclear-high-level-waste-mass-kg}
+
+\paragraph{Environmental Impact Propane Nuclear High Level Waste Mass {[}kg{]}}\label{environmental-impact-propane-nuclear-high-level-waste-mass-kg}
+
+\paragraph{Environmental Impact Diesel Nuclear High Level Waste Mass {[}kg{]}}\label{environmental-impact-diesel-nuclear-high-level-waste-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel1 Nuclear High Level Waste Mass {[}kg{]}}\label{environmental-impact-otherfuel1-nuclear-high-level-waste-mass-kg}
+
+\paragraph{Environmental Impact OtherFuel2 Nuclear High Level Waste Mass {[}kg{]}}\label{environmental-impact-otherfuel2-nuclear-high-level-waste-mass-kg}
+
+These outputs provide results for high-level nuclear waste associated with consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Electricity Nuclear Low Level Waste Volume {[}m3{]}}\label{environmental-impact-electricity-nuclear-low-level-waste-volume-m3}
+
+\paragraph{Environmental Impact Natural Gas Nuclear Low Level Waste Volume {[}m3{]}}\label{environmental-impact-natural-gas-nuclear-low-level-waste-volume-m3}
+
+\paragraph{Environmental Impact Fuel Oil \#2 Nuclear Low Level Waste Volume {[}m3{]}}\label{environmental-impact-fuel-oil-2-nuclear-low-level-waste-volume-m3}
+
+\paragraph{Environmental Impact Fuel Oil \#1 Nuclear Low Level Waste Volume {[}m3{]}}\label{environmental-impact-fuel-oil-1-nuclear-low-level-waste-volume-m3}
+
+\paragraph{Environmental Impact Coal Nuclear Low Level Waste Volume {[}m3{]}}\label{environmental-impact-coal-nuclear-low-level-waste-volume-m3}
+
+\paragraph{Environmental Impact Gasoline Nuclear Low Level Waste Volume {[}m3{]}}\label{environmental-impact-gasoline-nuclear-low-level-waste-volume-m3}
+
+\paragraph{Environmental Impact Propane Nuclear Low Level Waste Volume {[}m3{]}}\label{environmental-impact-propane-nuclear-low-level-waste-volume-m3}
+
+\paragraph{Environmental Impact Diesel Nuclear Low Level Waste Volume {[}m3{]}}\label{environmental-impact-diesel-nuclear-low-level-waste-volume-m3}
+
+\paragraph{Environmental Impact OtherFuel1 Nuclear Low Level Waste Volume {[}m3{]}}\label{environmental-impact-otherfuel1-nuclear-low-level-waste-volume-m3}
+
+\paragraph{Environmental Impact OtherFuel2 Nuclear Low Level Waste Volume {[}m3{]}}\label{environmental-impact-otherfuel2-nuclear-low-level-waste-volume-m3}
+
+These outputs provide results for low-level nuclear waste associated with consumption of each type of fuel that might be used at the site.~ The units are cubic meters.
+
+\paragraph{Environmental Impact Total N2O Emissions Carbon Equivalent Mass {[}kg{]}}\label{environmental-impact-total-n2o-emissions-carbon-equivalent-mass-kg}
+
+This output provides the result for equivalent carbon mass associated with the nitrous oxide (N\(_{2}\)O ) releases that stem from the consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Total CH4 Emissions Carbon Equivalent Mass {[}kg{]}}\label{environmental-impact-total-ch4-emissions-carbon-equivalent-mass-kg}
+
+This output provides the result for equivalent carbon mass associated with the methane releases that stem from the consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+\paragraph{Environmental Impact Total CO2 Emissions Carbon Equivalent Mass {[}kg{]}}\label{environmental-impact-total-co2-emissions-carbon-equivalent-mass-kg}
+
+This output provides the result for equivalent carbon mass associated with the carbon dioxide releases that stem from the consumption of each type of fuel that might be used at the site.~ The units are kg.
+
+The following different output meters could appear in the standard meter output (.mdd) file:
+
+\begin{itemize}
+\item
+  Zone,Meter,Source:Facility {[}J{]}
+\item
+  Zone,Meter,NaturalGasEmissions:Source {[}J{]}
+\item
+  Zone,Meter,CO2:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:CO2 {[}kg{]}
+\item
+  Zone,Meter,CO:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:CO {[}kg{]}
+\item
+  Zone,Meter,CH4:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:CH4 {[}kg{]}
+\item
+  Zone,Meter,NOx:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:NOx {[}kg{]}
+\item
+  Zone,Meter,N2O:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:N2O {[}kg{]}
+\item
+  Zone,Meter,SO2:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:SO2 {[}kg{]}
+\item
+  Zone,Meter,PM:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:PM {[}kg{]}
+\item
+  Zone,Meter,PM10:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:PM10 {[}kg{]}
+\item
+  Zone,Meter,PM2.5:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:PM2.5 {[}kg{]}
+\item
+  Zone,Meter,NH3:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:NH3 {[}kg{]}
+\item
+  Zone,Meter,NMVOC:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:NMVOC {[}kg{]}
+\item
+  Zone,Meter,Hg:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:Hg {[}kg{]}
+\item
+  Zone,Meter,Pb:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:Pb {[}kg{]}
+\item
+  Zone,Meter,WaterEnvironmentalFactors:Facility {[}L{]}
+\item
+  Zone,Meter,NaturalGasEmissions:WaterEnvironmentalFactors {[}L{]}
+\item
+  Zone,Meter,Nuclear High:Facility {[}kg{]}
+\item
+  Zone,Meter,NaturalGasEmissions:Nuclear High {[}kg{]}
+\item
+  Zone,Meter,Nuclear Low:Facility {[}m3{]}
+\item
+  Zone,Meter,NaturalGasEmissions:Nuclear Low {[}m3{]}
+\item
+  Zone,Meter,ElectricEmissions:Source {[}J{]}
+\item
+  Zone,Meter,ElectricEmissions:CO2 {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:CO {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:CH4 {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:NOx {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:N2O {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:SO2 {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:PM {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:PM10 {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:PM2.5 {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:NH3 {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:NMVOC {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:Hg {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:Pb {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:WaterEnvironmentalFactors {[}L{]}
+\item
+  Zone,Meter,ElectricEmissions:Nuclear High {[}kg{]}
+\item
+  Zone,Meter,ElectricEmissions:Nuclear Low {[}m3{]}
+\item
+  Zone,Meter,PurchasedElectricEmissions:Source {[}J{]}
+\item
+  Zone,Meter,SoldElectricEmissions:Source {[}J{]}
+\item
+  Zone,Meter,CoalEmissions:Source {[}J{]}
+\item
+  Zone,Meter,CoalEmissions:CO2 {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:CO {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:CH4 {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:NOx {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:N2O {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:SO2 {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:PM {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:PM10 {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:PM2.5 {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:NH3 {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:NMVOC {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:Hg {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:Pb {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:WaterEnvironmentalFactors {[}L{]}
+\item
+  Zone,Meter,CoalEmissions:Nuclear High {[}kg{]}
+\item
+  Zone,Meter,CoalEmissions:Nuclear Low {[}m3{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:Source {[}J{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:CO2 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:CO {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:CH4 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:NOx {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:N2O {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:SO2 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:PM {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:PM10 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:PM2.5 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:NH3 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:NMVOC {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:Hg {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:Pb {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:WaterEnvironmentalFactors {[}L{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:Nuclear High {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#2Emissions:Nuclear Low {[}m3{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:Source {[}J{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:CO2 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:CO {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:CH4 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:NOx {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:N2O {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:SO2 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:PM {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:PM10 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:PM2.5 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:NH3 {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:NMVOC {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:Hg {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:Pb {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:WaterEnvironmentalFactors {[}L{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:Nuclear High {[}kg{]}
+\item
+  Zone,Meter,FuelOil\#1Emissions:Nuclear Low {[}m3{]}
+\item
+  Zone,Meter,PropaneEmissions:Source {[}J{]}
+\item
+  Zone,Meter,PropaneEmissions:CO2 {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:CO {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:CH4 {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:NOx {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:N2O {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:SO2 {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:PM {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:PM10 {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:PM2.5 {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:NH3 {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:NMVOC {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:Hg {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:Pb {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:WaterEnvironmentalFactors {[}L{]}
+\item
+  Zone,Meter,PropaneEmissions:Nuclear High {[}kg{]}
+\item
+  Zone,Meter,PropaneEmissions:Nuclear Low {[}m3{]}
+\item
+  Zone,Meter,GasolineEmissions:Source {[}J{]}
+\item
+  Zone,Meter,GasolineEmissions:CO2 {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:CO {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:CH4 {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:NOx {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:N2O {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:SO2 {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:PM {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:PM10 {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:PM2.5 {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:NH3 {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:NMVOC {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:Hg {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:Pb {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:WaterEnvironmentalFactors {[}L{]}
+\item
+  Zone,Meter,GasolineEmissions:Nuclear High {[}kg{]}
+\item
+  Zone,Meter,GasolineEmissions:Nuclear Low {[}m3{]}
+\item
+  Zone,Meter,DieselEmissions:Source {[}J{]}
+\item
+  Zone,Meter,DieselEmissions:CO2 {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:CO {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:CH4 {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:NOx {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:N2O {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:SO2 {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:PM {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:PM10 {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:PM2.5 {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:NH3 {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:NMVOC {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:Hg {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:Pb {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:WaterEnvironmentalFactors {[}L{]}
+\item
+  Zone,Meter,DieselEmissions:Nuclear High {[}kg{]}
+\item
+  Zone,Meter,DieselEmissions:Nuclear Low {[}m3{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:Source {[}J{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:CO2 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:CO {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:CH4 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:NOx {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:N2O {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:SO2 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:PM {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:PM10 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:PM2.5 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:NH3 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:NMVOC {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:Hg {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:Pb {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:WaterEnvironmentalFactors {[}L{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:Nuclear High {[}kg{]}
+\item
+  Zone,Meter,OtherFuel1Emissions:Nuclear Low {[}m3{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:Source {[}J{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:CO2 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:CO {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:CH4 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:NOx {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:N2O {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:SO2 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:PM {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:PM10 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:PM2.5 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:NH3 {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:NMVOC {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:Hg {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:Pb {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:WaterEnvironmentalFactors {[}L{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:Nuclear High {[}kg{]}
+\item
+  Zone,Meter,OtherFuel2Emissions:Nuclear Low {[}m3{]}
+\item
+  Zone,Meter,Carbon Equivalent:Facility {[}kg{]}
+\item
+  Zone,Meter,CarbonEquivalentEmissions:Carbon Equivalent {[}kg{]}
+\end{itemize}
+
+What shows up in the output are the Energy Meters that were utilized in this particular input file, the pollutants, and the Total Carbon Equivalent.
+
+\subsection{Output:SQLite}\label{outputsqlite}
+
+Output from EnergyPlus can be written to SQLite files for manipulation outside some of the standard (such as spreadsheet) tools.
+
+\subsubsection{Inputs}\label{inputs-12-014}
+
+\paragraph{Field: Option}\label{field-option}
+
+Currently, there are limited capabilities for specifying SQLite generation.~ The Simple option will include all of the predefined database tables as well as time series related data.~ Using the SimpleAndTabular choice adds database tables related to the tabular reports that are already output by EnergyPlus in other formats.~ The description for SQLite outputs is described fully in the Output Details document.
+
+And one includes it in the IDF using the following.
+
+\begin{lstlisting}
+Output:SQLite, Simple;
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/output.tex b/doc/input-output-reference/src/output.tex
new file mode 100644
index 00000000000..f894d0199a1
--- /dev/null
+++ b/doc/input-output-reference/src/output.tex
@@ -0,0 +1,79 @@
+\chapter{Output}\label{output}
+
+EnergyPlus produces several output files as shown in the section on ``Running EnergyPlus''.~ This section will discuss the data contained in the ``standard'' output files (\textbf{eplusout.eso, eplusout.mtr}). They, too, have data dictionaries but unlike the input files, the output data dictionary is contained within the output file. Thus, the basic structure of the standard output file is:
+
+\begin{lstlisting}
+Data Dictionary Information
+End of Data Dictionary
+Data
+...
+Data
+End of Data
+\end{lstlisting}
+
+As with the IDF structure, there are rules associated with the interpretation of the standard output data dictionary. These rules are summarized as follows:
+
+\begin{itemize}
+\item
+  The first item on each line is an integer which represents the ``report code''. This ``report code'' will be listed in the data section where it will also be the first item on each line, identifying the data. Only 2 lines in the output file will not have an integer as the first item (``End of Data Dictionary'' and ``End of Data'' lines).
+\item
+  The second item on each line is also an integer. This integer corresponds to the number of items left on the dictionary line. Each string consists of a variable name and units in square brackets. Square brackets are required for all strings. If there are no units associated with a particular variable, then there are no characters between the brackets.
+\end{itemize}
+
+Six standard items appear at the start of every EnergyPlus Standard Output File Data Dictionary:
+
+\begin{lstlisting}
+Program Version,EnergyPlus <version number indicated>
+1,5,Environment Title[],Latitude[degrees],Longitude[degrees],Time Zone[],Elevation[m]
+2,6,Day of Simulation[],Month[],Day of Month[],DST Indicator[1 = yes 0 = no],Hour[],StartMinute[],EndMinute[],DayType
+3,3,Cumulative Day of Simulation[],Month[],Day of Month[],DST Indicator[1 = yes 0 = no],DayType  ! When Daily Output variables Requested
+4,2,Cumulative Days of Simulation[],Month[]  ! When Monthly Output variables Requested
+5,1,Cumulative Days of Simulation[] ! When Run Period Output variables Requested
+\end{lstlisting}
+
+\begin{itemize}
+\item
+  Item 0 is the program version statement.
+\item
+  Item 1 is produced at the beginning of each new ``environment'' (design day, run period).
+\item
+  Item 2 is produced prior to any variable reported at the timestep or hourly intervals. Hourly intervals will be shown with a start minute of 0.0 and an end minute of 60.0. Timestep intervals will show the appropriate start and end minutes.
+\item
+  Item 3 is produced prior to any variable reported at the daily interval.
+\item
+  Item 4 is produced prior to any variable reported at the monthly interval.
+\item
+  Item 5 is produced prior to any variable reported at the end of the ``environment''.
+\end{itemize}
+
+Following these five standard lines will be the variables requested for reporting from the input file (ref. Output:Variable object). For example:
+
+\begin{lstlisting}
+6,1,Environment,Site Outdoor Air Drybulb Temperature [C] !Hourly
+40,1,ZONE ONE,Zone Total Internal Latent Gain Energy [J] !Hourly
+68,1,ZONE ONE,Zone Mean Radiant Temperature [C] !Hourly
+69,1,ZONE ONE,Zone Mean Air Temperature [C] !Hourly
+70,1,ZONE ONE,Zone Air Heat Balance Surface Convection Rate [W] !Hourly
+71,1,ZONE ONE,Zone Air Heat Balance Air Energy Storage Rate [W] !Hourly
+\end{lstlisting}
+
+This example illustrates the non-consecutive nature of the ``report codes''. Internally, EnergyPlus counts each variable that \emph{could} be reported. This is the assigned ``report code''. However, the user may not request each possible variable for reporting. Note that, currently, the requested reporting frequency is shown as a comment (!) line in the standard output file.
+
+The data is produced when the actual simulation is performed (after the warmup days unless the Output:Diagnostics requesting ReportDuringWarmup is used). Data output is simpler in format than the data dictionary lines. From the dictionary above:
+
+\begin{lstlisting}
+1,DENVER STAPLETON INTL ARPT ANN HTG 99% CONDNS DB,  39.74,-105.18,  -7.00,1829.00
+2,1,12,21, 0, 1, 0.00,60.00,WinterDesignDay
+6,-16.
+40,0.0
+68,-19.8183039170649
+69,-19.8220899203323
+70,-3.175272922406513E-002
+71,-3.181520440307718E-002
+\end{lstlisting}
+
+This output file can be easily turned into a form that is read into commonly used spreadsheet programs where it can be further analyzed, graphed, etc.
+
+More details including graphs are shown in the Output Details and Examples Document under the file \textbf{eplusout.eso}.
+
+\input{src/output/using-readvarseso}
diff --git a/doc/input-output-reference/src/output/using-readvarseso.tex b/doc/input-output-reference/src/output/using-readvarseso.tex
new file mode 100644
index 00000000000..7be47dfdd93
--- /dev/null
+++ b/doc/input-output-reference/src/output/using-readvarseso.tex
@@ -0,0 +1,110 @@
+\section{Using ReadVarsESO}\label{using-readvarseso}
+
+\subsection{Creating Charts and Spreadsheet files from Output Variables}\label{creating-charts-and-spreadsheet-files-from-output-variables}
+
+The ReadVarsESO program is distributed with EnergyPlus as a simple approach to converting the standard output files (\textbf{eplusout.eso, eplusout.mtr}) into files that can be put directly into a spreadsheet program and then used to create graphs or do other statistical operations. ReadVarsESO can read the complex output files and sort the data into time-based form, it is a very quick application but does not have a lot of features.~ Note that all the \textbf{Output:Meter} and \textbf{Output:Meter:Cumulative} objects are included on the \textbf{eplusout.eso} file as well as the \textbf{eplusout.mtr} file.~ You can choose the \textbf{Output:Meter:MeterFileOnly} or \textbf{Output:Meter:Cumulative:MeterFileOnly} objects if you do not want a particular meter to show up on the \textbf{eplusout.eso} file. If you wish to see only the metered outputs, the \textbf{eplusout.mtr} file will typically be a lot smaller than the \textbf{eplusout.eso} file.
+
+The ReadVarsESO program has a very simple set of inputs. By default, you will get all the variables listed in the Output:Variable (\textbf{eplusout.eso}) or Output:Meter (\textbf{eplusout.mtr}) objects into the appropriate output files. The outputs from ReadVarsESO are limited to 255 variables (Microsoft Excelâ„¢ limit). You can tailor how many variables to list by specifying variables for the ReadVarsESO runs.
+
+You can override the 255 variable limit by specifying an argument on the command line (\textbf{EP-Launch} has a special option for this). You use ``unlimited'' or ``nolimit'' on the command line to get as many variables into your output file as desired. Again, this will be limited either by the number of variables in the \textbf{eplusout.eso} or \textbf{eplusout.mtr} files or the contents of the ``rvi'' file. If you want to use this option, you must include two arguments to the command line of the ReadVars program -- 1) the ``rvi'' file and 2) the ``unlimited'' argument.
+
+% table 41
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{ReadVarsESO Command Line Options \label{table:readvarseso-command-line-options}} \tabularnewline
+\toprule 
+Option & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{ReadVarsESO Command Line Options} \tabularnewline
+\toprule 
+Option & Description \tabularnewline
+\midrule
+\endhead
+
+< filename > & To use any of these options, you must include a file name (“rvi� file) as the first argument. \tabularnewline
+Unlimited (or Nolimit) & Variables of any number will be produced on the output file. \tabularnewline
+Timestep & Only variables with reported frequency “timestep� (or detailed) will be produced on the output file. \tabularnewline
+Hourly & Only variables with reported frequency “hourly�~ will be produced on the output file. \tabularnewline
+Daily & Only variables with reported frequency “daily�~ will be produced on the output file. \tabularnewline
+Monthly & Only variables with reported frequency “monthly�~ will be produced on the output file. \tabularnewline
+Annual (or RunPeriod) & Only variables with reported frequency “runperiod�~ will be produced on the output file. \tabularnewline
+\bottomrule
+\end{longtable}
+
+In addition, another argument can be used so that the output file is only one time frequency. (By default, all variables -- hourly, monthly, annual, etc. are mixed together in the output file). By using ``Timestep'' as an argument, you would get only the TimeStep reported variables. Using ``Monthly'', only the monthly variables. This is not automated in either \textbf{EP-Launch} or the \textbf{RunEPlus} batch file but can easily be accomplished.
+
+The program is run automatically from the \textbf{EP-Launch} program or the \textbf{RunEPlus} batch file (both these methods for executing EnergyPlus are described in the GettingStarted document). These programs use \textbf{\textless{}filename\textgreater{}.rvi} for input to the ReadVarsESO program executed first after the EnergyPlus execution and \textbf{\textless{}filename\textgreater{}.mvi} for the second execution. Ostensibly, the .rvi file would apply to the eplusout.eso file and the .mvi would apply to the eplusout.mtr file, BUT the contents of the files actually specify the ``\textbf{input}'' reporting file and the ``\textbf{output}'' reorganized file. Typical contents of an .rvi file are:
+
+% table 42
+\begin{longtable}[c]{p{2.1in}p{3.9in}}
+\caption{"RVI" file contents \label{table:rvi-file-contents}} \tabularnewline
+\toprule 
+.rvi line description & Actual .rvi File Contents \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{"RVI" file contents} \tabularnewline
+\toprule 
+.rvi line description & Actual .rvi File Contents \tabularnewline
+\midrule
+\endhead
+
+Input File & eplusout.eso \tabularnewline
+Output File & eplusout.csv \tabularnewline
+Variable Name & Site Outdoor Drybulb Temperature \tabularnewline
+Variable Name & Zone Air Temperature \tabularnewline
+Variable Name & Zone Air Humidity Ratio \tabularnewline
+Variable Name & Zone Air System Sensible Cooling Rate \tabularnewline
+Variable Name & Zone Air System Sensible Heating Rate \tabularnewline
+Variable Name & Zone Total Internal Latent Gain Rate \tabularnewline
+Specific Variable Name & COOLING COIL AIR OUTLET NODE,System Node Temperature \tabularnewline
+Specific Variable Name & AIR LOOP OUTLET NODE,System Node Temperature \tabularnewline
+Specific Variable Name & AIR LOOP OUTLET NODE,System Node Humidity Ratio \tabularnewline
+Specific Variable Name & Mixed Air Node,System Node Mass Flow Rate \tabularnewline
+Specific Variable Name & Outdoor air Inlet Node,System Node Mass Flow Rate \tabularnewline
+Variable Name & Humidifier Water Consumption Rate \tabularnewline
+Variable Name & Humidifier Electric Power \tabularnewline
+Variable Name & Zone Air Relative Humidity \tabularnewline
+Variable Name & Zone Predicted Moisture Load Moisture Transfer Rate \tabularnewline
+Termination Line ~(optional) & 0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Note that the first two lines of the file are ``input file'' (where to read the output variable values from) and ``output file'' (where to put the reorganized data). If you have only those two lines in an ``rvi'' file, the program will use all the available variables on indicated input file to produce the output.
+
+ReadVarsESO takes the input stream but recognizes the date/time information and appropriately places the required data onto the ``output file''. Following these lines are a list of variables to be culled from the ``input file'' and placed onto the output file. ``Variable Name'' will take all variables matching that description whereas ``Specific Variable Name'' will only match the full description of the variable. So, in the above example, ``Zone Air Temperature'' will report air temperatures for all the zones (but available at the HVAC timestep if you choose the ``detailed'' reporting frequency in your input file) but ``AIR LOOP OUTLET NODE'' and ``COOLING COIL AIR OUTLET NODE'' will be the only values reported for the ``System Node Temperature'' variable (the node temperature is available for all nodes used in the simulation). The termination line (0) is included to terminate the input to the ReadVarsESO program and begin the scanning.
+
+The output from ReadVarsESO is in the form commonly called ``comma de-limited'' or ``comma separated variable''. This format can be read easily in spreadsheet programs, such as Excelâ„¢.
+
+Note as described in the ``Input for Output'' above, only variables as listed on the \textbf{eplusout.rdd} file are available for reporting. If you request others, they will become ``Warning'' messages in the \textbf{eplusout.err} file.
+
+\begin{lstlisting}
+** Warning ** The following Output variables were requested but not generated
+**   ~~~   ** because IDF did not contain these elements or misspelled variable name -- check .rdd file
+************* Key = *, VarName = SYSTEM SENSIBLE COOLING RATE
+\end{lstlisting}
+
+The above message was generated from an IDF that requested reporting of the ``SYSTEM SENSIBLE COOLING RATE'' but that variable was not available from the components in the execution.
+
+% table 43
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Example ReadVarsESO command lines and results \label{table:example-readvarseso-command-lines-and-results}} \tabularnewline
+\toprule 
+Command Line & Description/Result \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Example ReadVarsESO command lines and results} \tabularnewline
+\toprule 
+Command Line & Description/Result \tabularnewline
+\midrule
+\endhead
+
+ReadVarsESO & Take eplusout.eso and produce an eplusout.csv file with all variables (up to 255) on it \tabularnewline
+ReadVarsESO my.rvi & Use the contents of “my.rvi� to produce the appropriate output file (limited to 255 variables) \tabularnewline
+ReadVarsESO my.rvi unlimited & Use the contents of “my.rvi� to produce the appropriate output file (no longer limited to 255 variables) \tabularnewline
+ReadVarsESO my.rvi Monthly & Use the contents of “my.rvi� to produce the appropriate output file and only produce those variables reported for “monthly� frequency (up to 255 variables) \tabularnewline
+ReadVarsESO my.rvi Daily unlimited & Use the contents of “my.rvi� to produce the appropriate output file and only produce those variables reported for “daily� frequency (no longer limited to 255 variables) \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/input-output-reference/src/overview.tex b/doc/input-output-reference/src/overview.tex
new file mode 100644
index 00000000000..8603d9a03c5
--- /dev/null
+++ b/doc/input-output-reference/src/overview.tex
@@ -0,0 +1,121 @@
+\chapter{Input-Output Reference}\label{input-output-reference}
+
+This document is intended to be an encyclopedic reference for the EnergyPlus Input Data Dictionary (IDD), Input Data File (IDF) and potential resultant outputs (various output files).
+
+The following descriptions are ``grouped'' by the elements in the IDD (ref: Getting Started Document and the IDD Conventions). In some cases, the descriptions of reporting will be done for an object (e.g., Lighting electrical consumption or thermal comfort value for a group of people) and in some cases for the entire group (e.g., ambient condition reports).
+
+\input{src/overview/what-s-different-about-energyplus-input}
+
+\input{src/overview/idd-conventions}
+
+\input{src/overview/input-output-descriptions}
+
+\input{src/overview/group-simulation-parameters}
+
+\input{src/overview/group-compliance-objects}
+
+\input{src/overview/group-location-climate-weather-file-access}
+
+\input{src/overview/group-schedules}
+
+\input{src/overview/group-surface-construction-elements}
+
+\input{src/overview/group-thermal-zone-description-geometry}
+
+\input{src/overview/group-advanced-surface-concepts}
+
+\input{src/overview/group-detailed-ground-heat-transfer}
+
+\input{src/overview/group-room-air-models}
+
+\input{src/overview/group-internal-gains-people-lights-other}
+
+\input{src/overview/group-daylighting}
+
+\input{src/overview/group-exterior-energy-use-equipment}
+
+\input{src/overview/group-airflow}
+
+\input{src/overview/group-design-objects}
+
+\input{src/overview/hvac-primary-and-secondary-systems}
+
+\input{src/overview/group-node-branch-management}
+
+\input{src/overview/group-plant-condenser-loops}
+
+\input{src/overview/group-plant-condenser-control}
+
+\input{src/overview/group-plant-equipment}
+
+\input{src/overview/group-water-heaters}
+
+\input{src/overview/group-condenser-equipment}
+
+\input{src/overview/group-plant-condenser-flow-control}
+
+\input{src/overview/group-air-distribution}
+
+\input{src/overview/group-airflow-network}
+
+\input{src/overview/group-zone-equipment}
+
+\input{src/overview/group-air-distribution-equipment}
+
+\input{src/overview/group-zone-forced-air-units}
+
+\input{src/overview/group-unitary-equipment}
+
+\input{src/overview/group-variable-refrigerant-flow-equipment}
+
+\input{src/overview/group-radiative-convective-units}
+
+\input{src/overview/group-refrigeration}
+
+\input{src/overview/group-zone-controls-thermostats}
+
+\input{src/overview/group-air-path}
+
+\input{src/overview/group-non-zone-equipment}
+
+\input{src/overview/group-solar-collectors}
+
+\input{src/overview/group-pumps}
+
+\input{src/overview/group-heating-and-cooling-coils}
+
+\input{src/overview/group-fans}
+
+\input{src/overview/group-humidifiers}
+
+\input{src/overview/group-desiccant-dehumidifiers}
+
+\input{src/overview/group-energy-management-system-ems}
+
+\input{src/overview/group-externalinterface}
+
+\input{src/overview/group-user-defined-hvac-and-plant-component}
+
+\input{src/overview/group-system-availability-managers}
+
+\input{src/overview/group-setpoint-managers}
+
+\input{src/overview/group-controllers}
+
+\input{src/overview/group-evaporative-coolers}
+
+\input{src/overview/group-heat-recovery}
+
+\input{src/overview/group-demand-limiting-controls}
+
+\input{src/overview/group-electric-load-center-generator}
+
+\input{src/overview/group-water-systems}
+
+\input{src/overview/group-operational-faults}
+
+\input{src/overview/group-performance-curves}
+
+\input{src/overview/group-performance-tables}
+
+\input{src/overview/group-fluid-properties}
diff --git a/doc/input-output-reference/src/overview/group-advanced-surface-concepts.tex b/doc/input-output-reference/src/overview/group-advanced-surface-concepts.tex
new file mode 100644
index 00000000000..34c335df833
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-advanced-surface-concepts.tex
@@ -0,0 +1,1864 @@
+\section{Group -- Advanced Surface Concepts}\label{group-advanced-surface-concepts}
+
+This group of objects describe concepts applied to heat transfer surfaces that are of an advanced nature. Careful consideration must be given before using these.
+
+\subsection{SurfaceProperty:HeatTransferAlgorithm}\label{surfacepropertyheattransferalgorithm}
+
+This object, and three other related objects, can be used to control which surface heat transfer model is used on specific surfaces. The separate object called HeatBalanceAlgorithm is used to control the heat transfer model in an overall way while this object can be used to revise the algorithm selections for specific surfaces. This object allows selectively overriding the global setting in HeatBalanceAlgorithm to choose one of the following models for a particular surface:
+
+\begin{itemize}
+\item
+  CTF (Conduction Transfer Functions),
+\item
+  EMPD (Effective Moisture Penetration Depth with Conduction Transfer Functions).
+\item
+  CondFD (Conduction Finite Difference)
+\item
+  HAMT (Combined Heat And Moisture Finite Element)
+\end{itemize}
+
+\subsubsection{Inputs}\label{inputs-000}
+
+\paragraph{Field: Surface Name}\label{field-surface-name}
+
+This is the name of the surface that will be assigned to use the heat transfer algorithm selected in the next field. This should be a name of a surface defined elsewhere.
+
+\paragraph{Field: Algorithm}\label{field-algorithm}
+
+This field is used to determine the heat transfer algorithm that is to be applied to the surface named in the previous field. The allowable choices are:
+
+\begin{itemize}
+\item
+  ConductionTransferFunction
+\item
+  MoisturePenetrationDepthConductionTransferFunction
+\item
+  ConductionFiniteDifference
+\item
+  CombinedHeatAndMoistureFiniteElement
+\end{itemize}
+
+\subsection{SurfaceProperty:HeatTransferAlgorithm:MultipleSurface}\label{surfacepropertyheattransferalgorithmmultiplesurface}
+
+This object can be used to control the surface heat transfer model used for specific types of surfaces. The separate object called HeatBalanceAlgorithm is used to control the heat transfer model in an overall way while this object can be used to revise the algorithm selections for specific types of surfaces. This object allows selectively overriding the global setting in HeatBalanceAlgorithm to choose one of the following models for all surfaces of a particular type:
+
+\begin{itemize}
+\item
+  CTF (Conduction Transfer Functions),
+\item
+  EMPD (Effective Moisture Penetration Depth with Conduction Transfer Functions).
+\item
+  CondFD (Conduction Finite Difference)
+\item
+  HAMT (Combined Heat And Moisture Finite Element)
+\end{itemize}
+
+\subsubsection{Inputs}\label{inputs-1-000}
+
+\paragraph{Field: Name}\label{field-name-000}
+
+This is a unique, user-defined name for the object.
+
+\paragraph{Field: Surface Type}\label{field-surface-type}
+
+This field is selects the type of surfaces that are all assigned to use the heat transfer algorithm selected in the next field. This field is used with one of the following allowable keywords:
+
+\begin{itemize}
+\item
+  AllExteriorSurfaces---all surfaces that have ``Outdoors'' outside boundary condition
+\item
+  AllExteriorWalls---all walls that have ``Outdoors'' outside boundary condition
+\item
+  AllExteriorRoofs---all roofs that have ``Outdoors'' outside boundary condition
+\item
+  AllExteriorFloors---all floors that have ``Outdoors'' outside boundary condition
+\item
+  AllGroundContactSurfaces---all surfaces that have ``Ground'' outside boundary condition
+\item
+  AllInteriorSurfaces---all surfaces that are internal partition-type surfaces
+\item
+  AllInteriorWalls---all walls that are internal surfaces
+\item
+  AllInteriorCeilings---all ceilings that are internal surfaces
+\item
+  AllInteriorFloors---all floors that are are internal surfaces
+\end{itemize}
+
+\paragraph{Field: Algorithm}\label{field-algorithm-1}
+
+This field is used to determine the heat transfer algorithm that is to be applied to the surface types in the previous field. The allowable choices are:
+
+\begin{itemize}
+\item
+  ConductionTransferFunction
+\item
+  MoisturePenetrationDepthConductionTransferFunction
+\item
+  ConductionFiniteDifference
+\item
+  CombinedHeatAndMoistureFiniteElement
+\end{itemize}
+
+\begin{lstlisting}
+SurfaceProperty:HeatTransferAlgorithm:MultipleSurface,
+      my exterior wall override,
+      AllExteriorWalls,
+      ConductionFiniteDifference;
+\end{lstlisting}
+
+\subsection{SurfaceProperty:HeatTransferAlgorithm:SurfaceList}\label{surfacepropertyheattransferalgorithmsurfacelist}
+
+This object can be used to control the surface heat transfer model used for a list of surfaces. The separate object called HeatBalanceAlgorithm is used to control the heat transfer model in an overall way while this object can be used to revise the algorithm selections for a list of specific surfaces. This object allows selectively overriding the global setting in HeatBalanceAlgorithm to choose one of the following models for listed:
+
+\begin{itemize}
+\item
+  CTF (Conduction Transfer Functions),
+\item
+  EMPD (Effective Moisture Penetration Depth with Conduction Transfer Functions).
+\item
+  CondFD (Conduction Finite Difference)
+\item
+  HAMT (Combined Heat And Moisture Finite Element)
+\end{itemize}
+
+\subsubsection{Inputs}\label{inputs-2-000}
+
+\paragraph{Field: Name}\label{field-name-1}
+
+This is a unique, user-defined name for the object.
+
+\paragraph{Field: Algorithm}\label{field-algorithm-2}
+
+This field is used to determine the heat transfer algorithm that is to be applied to the surface listed in the remaining fields. The allowable choices are:
+
+\begin{itemize}
+\item
+  ConductionTransferFunction
+\item
+  MoisturePenetrationDepthConductionTransferFunction
+\item
+  ConductionFiniteDifference
+\item
+  CombinedHeatAndMoistureFiniteElement
+\end{itemize}
+
+\paragraph{Field: Surface Name N}\label{field-surface-name-n}
+
+This is the name of the ``Nth'' surface that will be assigned to use the heat transfer algorithm selected in this object. These should be the names of surfaces defined elsewhere. This object is extensible. Additional surfaces can be added to extend the object.
+
+An example IDF object follows.
+
+\begin{lstlisting}
+
+SurfaceProperty:HeatTransferAlgorithm:SurfaceList,
+      my wall construct override,   !- Name
+      ConductionFiniteDifference,   !- Algorithm
+      Zn001:Wall001,                !- Surface Name 1
+      Zn001:Wall002,                !- Surface Name 2
+      Zn001:Wall003,                !- Surface Name 3
+      Zn001:Wall004;                !- Surface Name 4
+\end{lstlisting}
+
+\subsection{SurfaceProperty:HeatTransferAlgorithm:Construction}\label{surfacepropertyheattransferalgorithmconstruction}
+
+This object can be used to control the surface heat transfer model used for surfaces that have a specific type of construction. The separate object called HeatBalanceAlgorithm is used to control the heat transfer model in an overall way while this object can be used to revise the algorithm selections for specific constructions. This object allows selectively overriding the global setting in HeatBalanceAlgorithm to choose one of the following models for all surfaces with particular type of construction:
+
+\begin{itemize}
+\item
+  CTF (Conduction Transfer Functions),
+\item
+  EMPD (Effective Moisture Penetration Depth with Conduction Transfer Functions).
+\item
+  CondFD (Conduction Finite Difference)
+\item
+  HAMT (Combined Heat And Moisture Finite Element)
+\end{itemize}
+
+\subsubsection{Inputs}\label{inputs-3}
+
+\paragraph{Field: Name}\label{field-name-2}
+
+This is a unique, user-defined name for the object.
+
+\paragraph{Field: Algorithm}\label{field-algorithm-3}
+
+This field is used to determine the heat transfer algorithm that is to be applied to the surfaces with the type of of construction listed in the next field. The allowable choices are:
+
+\begin{itemize}
+\item
+  ConductionTransferFunction
+\item
+  MoisturePenetrationDepthConductionTransferFunction
+\item
+  ConductionFiniteDifference
+\item
+  CombinedHeatAndMoistureFiniteElement
+\end{itemize}
+
+\paragraph{Field: Construction Name}\label{field-construction-name}
+
+This field is the name of a Construction object defined elsewhere. All the surfaces in the model that are assigned this type of construction will be assigned to use the heat transfer algorithm slected in the previous field.
+
+An example IDF object follows.
+
+\begin{lstlisting}
+
+SurfaceProperty:HeatTransferAlgorithm:Construction,
+      my wall construct override,  !- Name
+      ConductionFiniteDifference,  !- Algorithm
+      R13WALL;                     !- Construction Name
+\end{lstlisting}
+
+\subsection{SurfaceControl:MoveableInsulation}\label{surfacecontrolmoveableinsulation}
+
+Movable insulation can be used/scheduled on any surface regular surface (such as a wall, floor, roof, etc.) but not on a subsurface (such as a window, use WindowProperty:ShadingControl instead). With movable insulation, no reference is made in the surface that is using the insulation -- rather the movable insulation statement references the surface to which it is applied.
+
+Exterior and interior movable insulation have undergone some testing and appears to producing expected results. The underlying principle has been implemented in EnergyPlus for both interior and exterior movable insulation with the possibility for exterior movable insulation to be transparent (transparent insulation material or TIM).
+
+TIM exterior layers can be used with the ConductionFiniteDifference (CondFD) solution algorithm. With this addition, TIM layers can be used in conjunction with wall layers that have phase change materials (PCM) included, or any other advanced capability of the CondFD algorithm such as variable conductivity. The input requirements are exactly the same as when used with the CTF algorithm. The Solution Algorithm needs to be changed to CondFD, and as with CTF, the ``SurfaceControl:MovableInsulation'' object must be completed to specify the insulated surface and the ``WindowMaterial:Glazing'' object is needed to provide the TIM layer properties.
+
+Basically, the addition of movable insulation allows the user to schedule an extra amount of insulation on either the inside or outside surface of a wall (or both). The insulation must be a simple, homogenous material layer (linked to a material definition within the input data file). Note that EnergyPlus allows the exterior movable insulation layer to be transparent to short wavelength radiation (solar). In this case, incident solar is split between the plane between the movable insulation and the surface and the plane between the movable insulation and the surrounding air. This calculation is fairly basic and based on the solar transmittance of the insulation layer (material properties). Using transparent layers for exterior movable insulation allows solar energy to penetrate deeper into a construction where it can be stored for later use in the building (similar in concept to a Trombe Wall).
+
+\subsubsection{Field: Insulation Type}\label{field-insulation-type}
+
+This field determines whether the movable insulation is applied to the inside or the outside of the surface by entering either ``Inside'' or ``Outside'', respectively.
+
+\subsubsection{Field: Surface Name}\label{field-surface-name-1}
+
+This field refers the movable insulation back to a particular surface (ref: Building Surfaces) via its user assigned name so that EnergyPlus knows where to apply this extra layer of insulation. This will affect either the inside or outside surface heat balance of this surface depending on the value in the insulation type field (see previous field).
+
+\subsubsection{Field: Material Name}\label{field-material-name}
+
+This field refers to a material layer (e.g., Material, Material:NoMass, or WindowMaterial:Glazing; transparent layers are only valid for outside movable insulation) via its user assigned name. This provides the program with a full complement of material properties so that the effect of the insulation (R-value and solar transmittance) can be correctly taken into account by EnergyPlus.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name}
+
+This field is a schedule that theoretically can be any positive real number but was originally intended to be a parameter between 0.0 and 1.0. Its purpose is to act as a fractional modifier on the resistance of the material layer. The actual thermal resistance of the movable insulation is equal to the resistance of the material layer times the current value in the movable insulation schedule. A value of 0.0 simply means that the movable insulation is not present.
+
+An example of this syntax implemented in an input file is:
+
+\begin{lstlisting}
+
+SurfaceControl:MoveableInsulation,
+    Exterior,                      ! Insulation Type
+    Zone001:Wall001,               ! Surface Name
+    TransparentInsulationMaterial, ! Material Name
+    PresentInWinterSchedule;       ! Schedule Name
+\end{lstlisting}
+
+\subsection{SurfaceProperty:OtherSideCoefficients}\label{surfacepropertyothersidecoefficients}
+
+By referencing the Other Side Coefficients statement in the surface statements (i.e.~Outside Boundary Condition), the temperature of the outer plane of a surface (see Figure~\ref{fig:illustration-for-other-side-coefficients}) can be directly controlled. Other side coefficients can also be used to control the exterior convective heat transfer coefficient of a surface and the corresponding exterior air temperature. It should be noted that solar effects are not accounted for when other side coefficients are used. In addition, if other side coefficients are specified for a surface, they also hold for subsurfaces of that surface (though subsurfaces can have their own coefficient set).
+
+other side coefficients have the same effect on all types of heat transfer surfaces. In other words, an interior surface with other side coefficients specified and an exterior wall with identical other side coefficients specified are simulated exactly the same. A surface that uses other side coefficients should be thought of as a new or separate type of surface. All heat transfer surfaces are simulated in the same manner through conduction transfer functions. The only difference between the various types of heat transfer surfaces is the environment on the other side of the surface. For example, the other side environment of an exterior surface is the outdoor environment. For an interior surface, the temperature of the outer plane of the surface is set equal to the temperature of the inner plane of the surface. Similarly, a surface with other side coefficients specified will allow the user to control the other side environment.
+
+Heat transfer through a surface is an extremely important component in the calculation of zone loads. The information to calculate this heat transfer is readily available if the surface is exposed to the outdoor environment or to another zone that is being simulated. Occasionally, a user will want to model the heat transfer through a surface that is adjacent to an area that is not included in the EnergyPlus model. For example, an office area is attached to a warehouse and the user is only interested in simulating the office area. An interior surface with other side coefficients specified could be used to control the environment on the other side of the surface, thereby accounting for the heat transfer through the adjoining surface.
+
+Other Side Coefficients affects the ``other side'' of a surface as described below. Each coefficient has a special meaning. You may enter a 0 or blank if you are not using a particular coefficient. Note that there are two potential ways to use other side coefficients. Either they are used to set the temperature of the exterior side surface directly (if the combined convective/radiative coefficient below is less than or equal to zero) or to set both the film coefficient (positive value for the combined convective/radiative coefficient below) and the outside air temperature.
+
+\subsubsection{Inputs}\label{inputs-4}
+
+\paragraph{Field: Name}\label{field-name-3}
+
+This, of course, is the string referenced in the Surface statement that is using OtherSideCoefficients as the Outside Boundary Condition.
+
+\paragraph{Field: Combined Convective/Radiative Film Coefficient}\label{field-combined-convectiveradiative-film-coefficient}
+
+This is a trigger value. If the value is greater than zero, then it is taken to be the combined convective/radiative film coefficient. In this case (value \textgreater{} 0), the remaining fields are used first to calculate the outside air temperature for the surface and then to calculate the outside surface temperature based on the outside air temperature and the film coefficient. If this field is less than or equal to zero, then the remaining fields are used to calculate the surface temperature (not the outside air temperature). The units for this field are the same as for a convective heat transfer coefficient: W/(m\(^{2}\)*K). This is referred to as ``C1'' in the reference below.
+
+\paragraph{Field: Constant Temperature}\label{field-constant-temperature}
+
+This field defines a temperature term that is a constant part of the calculation either of the surface or outside air temperature. This parameter is shown as ``C2'' in the equation below. The units for this parameter are degrees C. If a schedule name is included as the second parameter, the value of this parameter will be overridden by the value from the schedule. The default for this field is 0.0.
+
+\paragraph{Field: Constant Temperature Coefficient}\label{field-constant-temperature-coefficient}
+
+This field defines a constant coefficient that is applied to the constant temperature (see previous field). This parameter is shown as ``C3'' in the equation below. This parameter is dimensionless. The value of this parameter is usually 1.0 if a schedule is used to set C2. This field is ignored if \emph{Sinusoidal Variation of Constant Temperature Coefficient} = Yes. The default for this field is 1.0.
+
+\paragraph{Field: External Dry-Bulb Temperature Coefficient}\label{field-external-dry-bulb-temperature-coefficient}
+
+This field defines a constant coefficient that is applied to the outside air dry-bulb temperature. This parameter is shown as ``C4'' in the equation below. This parameter is dimensionless. The default for this field is 0.0.
+
+\paragraph{Field: Ground Temperature Coefficient}\label{field-ground-temperature-coefficient}
+
+This field defines a constant coefficient that is applied to the ground temperature (ref. Site:GroundTemperature:BuildingSurface). This parameter is shown as ``C5'' in the equation below. This parameter is dimensionless.
+
+\paragraph{Field: Wind Speed Coefficient}\label{field-wind-speed-coefficient}
+
+This field defines a constant coefficient that is applied to the product of the outside air dry-bulb temperature and the wind speed. This parameter is shown as ``C6'' in the equation below. This parameter has dimensions of inverse velocity or s/m. The default for this field is 0.0.
+
+\paragraph{Field: Zone Air Temperature Coefficient}\label{field-zone-air-temperature-coefficient}
+
+This field defines a constant coefficient that is applied to the temperature of the zone to which this surface belongs. This parameter is shown as ``C7'' in the equation below. This parameter is dimensionless. The default for this field is 0.0.
+
+\paragraph{Field: Constant Temperature Schedule Name}\label{field-constant-temperature-schedule-name}
+
+This field is used to supply a schedule name. That schedule will supply the ``constant'' temperature value C2. Note that the value of the C3 field should normally be 1.0 if a schedule is used for C2. If not blank, this field must be a valid schedule name.
+
+\paragraph{Field: Sinusoidal Variation of Constant Temperature Coefficient}\label{field-sinusoidal-variation-of-constant-temperature-coefficient}
+
+This field is optional and can be used to define an alternate method of prescribing the coefficient that is applied to the constant temperature (see the fields Constant Temperature and Constant Temperature Coefficient). This parameter is shown as ``C2'' in the equation below. If this field is omitted, left blank, or set to ``No,'' then C2 is a constant (defined in the field Constant Temperature Coefficient). However if this is set to ``Yes,'' then the value of C2 varies with a unitary sine wave in the following way:
+
+\begin{equation}
+C2 = Sin\left( {2\pi \frac{{\left( {time\,of\,day} \right)}}{{\left( {period} \right)}}} \right)
+\end{equation}
+
+The value for ``period'' is controlled in the following field. The value for ``time of day'' is based on the zone timestep and is in units of hours. The sine function here uses input as radians. When using this option, the value for C2 will vary between -1.0 and 1.0 and the value put in the field Constant Temperature Coefficient is not used. This option cannot be used at the same time as scheduling a constant temperature with the previous field.
+
+\paragraph{Field: Period of Sinusoidal Variation}\label{field-period-of-sinusoidal-variation}
+
+This field is used to define the period of the sine wave when using the Sinusodial Variation of Constant Temperature Coefficient capability selected in the previous field. This field is the time period of the sine wave in units of hours. The default is 24 hours and provides a diurnal sine wave. The value entered here is ``period'' in the equation in the previous field.
+
+\paragraph{Field: Previous Other Side Temperature Coefficient}\label{field-previous-other-side-temperature-coefficient}
+
+This field defines a constant coefficient that is applied to the other side temperature computed by this object from the previous zone time step. This parameter is shown as ``C8'' in the equation below. This parameter is dimensionless. The default for this field is 0.0.
+
+\paragraph{Field: Minimum Other Side Temperature Limit}\label{field-minimum-other-side-temperature-limit}
+
+This field specifies a lower limit for the other side temperature result in degrees C. If blank, there is no lower limit.
+
+\paragraph{Field: Maximum Other Side Temperature Limit}\label{field-maximum-other-side-temperature-limit}
+
+This field specifies an upper limit for the other side temperature result in degrees C. If blank, there is no upper limit.
+
+The coefficients listed above are used in the following equation:
+
+\begin{equation}
+T = C2*C3 + C4*Toadb + C5*Tgrnd + C6*Wspd*Toadb + C7*Tzone + C8*Tpast
+\end{equation}
+
+where:
+
+T = Outside Air Temperature when C1 (Combined convective/radiative film Coeff) \textgreater{} 0
+
+T = Exterior Surface Temperature when C1 (Combined convective/radiative film Coeff) \textless{} = 0
+
+Tzone = Temperature of the zone being simulated (°C)
+
+Toadb = Dry-bulb temperature of the outdoor air (°C)
+
+Tgrnd = Temperature of the ground (°C) from Site:GroundTemperature:BuildingSurface
+
+Wspd = Outdoor wind speed (m/sec)
+
+Tpast = Other side temperature from previous zone timestep (°C)
+
+\begin{figure}[hbtp] % fig 41
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image069.png}
+\caption{Illustration for Other Side Coefficients \protect \label{fig:illustration-for-other-side-coefficients}}
+\end{figure}
+
+\begin{lstlisting}
+!  Example input using temperature schedule
+SurfaceProperty:OtherSideCoefficients,
+      OSCCoef:Zn005:Wall003,   !- Name
+      0,                       !- Combined Convective/Radiative Film Coefficient {W/m2-K}
+      0.000000,                !- Constant Temperature {C}
+      1.000000,                !- Constant Temperature Coefficient
+      0.000000,                !- External Dry-Bulb Temperature Coefficient
+      0.000000,                !- Ground Temperature Coefficient
+      0.000000,                !- Wind Speed Coefficient
+      0.000000,                !- Zone Air Temperature Coefficient
+      Zn005Wall003OtherSideTempSched;  !- Constant Temperature Schedule Name
+\end{lstlisting}
+
+\begin{lstlisting}
+!  Example input for outside heat transfer coefficient of 1.23, using Tosdb
+SurfaceProperty:OtherSideCoefficients,
+      OSCCoef:Zn005:Wall004,   !- Name
+      1.230000,                !- Combined Convective/Radiative Film Coefficient {W/m2-K}
+      0.000000,                !- Constant Temperature {C}
+      0.000000,                !- Constant Temperature Coefficient
+      1.000000,                !- External Dry-Bulb Temperature Coefficient
+      0.000000,                !- Ground Temperature Coefficient
+      0.000000,                !- Wind Speed Coefficient
+      0.000000,                !- Zone Air Temperature Coefficient
+      ,                        !- Constant Temperature Schedule Name
+      No,                      !- Sinusoidal Variation of Constant Temperature Coefficient
+      24,                      !- Period of Sinusoidal Variation {hr}
+      0.,                      !- Previous Other Side Temperature Coefficient
+      ,                        !- Minimum Other Side Temperature Limit {C}
+      ;                        !- Maximum Other Side Temperature Limit {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs}
+
+\begin{lstlisting}
+Zone,Average,Surface Other Side Coefficients Exterior Air Drybulb Temperature
+\end{lstlisting}
+
+\paragraph{Surface Other Side Coefficients Exterior Air Drybulb Temperature {[}C{]}}\label{surface-other-side-coefficients-exterior-air-drybulb-temperature-c}
+
+This is the air temperature applied to the other side of the surface.
+
+\subsection{SurfaceProperty:OtherSideConditionsModel}\label{surfacepropertyothersideconditionsmodel}
+
+By referencing the Other Side Conditions Model statement in the surface statements (i.e.~Outside Boundary Condition), the boundary conditions for the outer plane of the mass wall can be connected to the appropriate model for various multi-skin components. The types of multi-skin components that use this object include systems that are mounted to the outside surface using standoffs that create a small air gap -- see Figure~\ref{fig:illustration-for-other-side-conditions-model}. This type of modeling allows using the usual heat transfer calculations for the underlying surface with other types of multi-skin component models that are available including: unglazed transpired solar collectors, ventilated photovoltaic panels, and naturally ventilated facades.
+
+The boundary condition values are determined dynamically by the program using internal component models. If you want to define other side surface temperatures or convection conditions, then use SurfaceProperty:OtherSideCoefficients instead of this object.
+
+It should be noted that when other side conditions models are used, solar effects are removed from the surface's outside face heat balance, but are used in modeling the component adjacent to that surface.
+
+In addition, the other side conditions model has been modified to include underground piping system interaction. The PipingSystem:Underground:Domain object represents a mass of ground which may include interaction with, for example, basement surfaces. In this case, the ground model will internally use the other side condition model hook to update boundary conditions for those surfaces which use that other side condition model name reference.
+
+\subsubsection{Inputs}\label{inputs-5}
+
+\paragraph{Field: Name}\label{field-name-4}
+
+This is the string referenced in the Surface statement that is using OtherSideModel as the Exterior Environment.
+
+\paragraph{Field: Type of Modeling}\label{field-type-of-modeling}
+
+This is a string key selection used to identify the type of model that will be used to determine boundary conditions. The only available choices are ''GapConvectionRadiation,'' ``UndergroundPipingSystemSurface,'' and ``GroundCoupledSurface.''
+
+\begin{figure}[hbtp] % fig 42
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image070.png}
+\caption{Illustration for Other Side Conditions Model \protect \label{fig:illustration-for-other-side-conditions-model}}
+\end{figure}
+
+An example specification is:
+
+\begin{lstlisting}
+
+SurfaceProperty:OtherSideConditionsModel,
+      UTSC OSCM ZN11,          ! OtherSideConditionsModel Name
+      GapConvectionRadiation; ! Type of Modeling used to determine Boundary Conditions
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1}
+
+\begin{itemize}
+\item
+  Zone,Average,Surface Other Side Conditions Modeled Convection Air Temperature {[}C{]}
+\item
+  Zone,Average,Surface Other Side Conditions Modeled Convection Heat Transfer Coefficient {[}W/m2-K{]}
+\item
+  Zone,Average,Surface Other Side Conditions Modeled Radiation Temperature {[}C{]}
+\item
+  Zone,Average,Surface Other Side Conditions Modeled Radiation Heat Transfer Coefficient {[}W/m2-K{]}
+\end{itemize}
+
+\paragraph{Surface Other Side Conditions Modeled Convection Air Temperature {[}C{]}}\label{surface-other-side-conditions-modeled-convection-air-temperature-c}
+
+This is the air temperature exposed to the other side of the surface by the model and used in convection heat transfer calculations.
+
+\paragraph{Surface Other Side Conditions Modeled Convection Heat Transfer Coefficient {[}W/m2-K{]}}\label{surface-other-side-conditions-modeled-convection-heat-transfer-coefficient-wm2-k}
+
+This is the surface convection heat transfer coefficient applied to the other side of the surface by the model.
+
+\paragraph{Surface Other Side Conditions Modeled Radiation Temperature {[}C{]}}\label{surface-other-side-conditions-modeled-radiation-temperature-c}
+
+This is the effective temperature exposed to the other side of the surface for thermal radiation heat transfer calculations.
+
+\paragraph{Surface Other Side Conditions Modeled Radiation Heat Transfer Coefficient {[}W/m2-K{]}}\label{surface-other-side-conditions-modeled-radiation-heat-transfer-coefficient-wm2-k}
+
+This is the effective (Iinearized) radiation heat transfer coefficient applied to the other side of the surface by the model.
+
+\subsection{SurfaceConvectionAlgorithm:Inside:AdaptiveModelSelections}\label{surfaceconvectionalgorithminsideadaptivemodelselections}
+
+This object provides options to change the individual convection model equations for dynamic selection when using AdaptiveConvectionAlgorithm. This object is only needed to make changes to the default model selections for any or all of the surface categories. This object is for the inside face, the side of the surface facing a thermal zone.
+
+\subsubsection{Inputs}\label{inputs-6}
+
+\paragraph{Field: Name}\label{field-name-5}
+
+A unique name for the object.
+
+\paragraph{Field: Simple Buoyancy Vertical Wall Equation Source}\label{field-simple-buoyancy-vertical-wall-equation-source}
+
+Applies to zone with no HVAC or when HVAC is off. This is for vertical walls. The key choice options include: FohannoPolidoriVerticalWall, ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq3WallAwayFromHeat, KhalifaEq6NonHeatedWalls FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve
+
+\paragraph{Field: Simple Buoyancy Vertical Wall User Curve Name}\label{field-simple-buoyancy-vertical-wall-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
+
+\paragraph{Field: Simple Buoyancy Stable Horizontal Equation Source}\label{field-simple-buoyancy-stable-horizontal-equation-source}
+
+Applies to zone with no HVAC or when HVAC is off. This is for horizontal surfaces with heat flow directed for stable thermal stratification. The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve
+
+\paragraph{Field: Simple Buoyancy Stable Horizontal Equation User Curve Name}\label{field-simple-buoyancy-stable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
+
+\paragraph{Field: Simple Buoyancy Unstable Horizontal Equation Source}\label{field-simple-buoyancy-unstable-horizontal-equation-source}
+
+Applies to zone with no HVAC or when HVAC is off. This is for passive horizontal surfaces with heat flow for unstable thermal stratification. The key choice options include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
+
+\paragraph{Field: Simple Buoyancy Unstable Horizontal Equation User Curve Name}\label{field-simple-buoyancy-unstable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Simple Buoyancy Stable Tilted Equation Source}\label{field-simple-buoyancy-stable-tilted-equation-source}
+
+Applies to zone with no HVAC or when HVAC is off. This is for tilted surfaces with heat flow for stable thermal stratification. The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve
+
+\paragraph{Field: Simple Buoyancy Stable Tilted Equation User Curve Name}\label{field-simple-buoyancy-stable-tilted-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Simple Buoyancy Unstable Tilted Equation Source}\label{field-simple-buoyancy-unstable-tilted-equation-source}
+
+Applies to zone with no HVAC or when HVAC is off. This is for tilted surfaces with heat flow for unstable thermal stratification. The key choices include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
+
+\paragraph{Field: Simple Buoyancy Unstable Tilted Equation User Curve Name}\label{field-simple-buoyancy-unstable-tilted-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Simple Buoyancy Windows Equation Source}\label{field-simple-buoyancy-windows-equation-source}
+
+Applies to zone with no HVAC or when HVAC is off. This is for all window surfaces. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, KaradagChilledCeiling, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Simple Buoyancy Windows Equation User Curve Name}\label{field-simple-buoyancy-windows-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Vertical Wall Equation Source}\label{field-floor-heat-ceiling-cool-vertical-wall-equation-source}
+
+Applies to zone with in-floor heating and/or in-ceiling cooling. This is for vertical walls. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq3WallAwayFromHeat, FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Vertical Wall Equation User Curve Name}\label{field-floor-heat-ceiling-cool-vertical-wall-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Stable Horizontal Equation Source}\label{field-floor-heat-ceiling-cool-stable-horizontal-equation-source}
+
+Applies to zone with in-floor heating and/or in-ceiling cooling. This is for passive horizontal surfaces with heat flow for stable thermal stratification. The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Stable Horizontal Equation User Curve Name}\label{field-floor-heat-ceiling-cool-stable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Unstable Horizontal Equation Source}\label{field-floor-heat-ceiling-cool-unstable-horizontal-equation-source}
+
+Applies to zone with in-floor heating and/or in-ceiling cooling. This is for passive horizontal surfaces with heat flow for unstable thermal stratification. The key choice options include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, KhalifaEq4CeilingAwayFromHeat, or UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Unstable Horizontal Equation User Curve Name}\label{field-floor-heat-ceiling-cool-unstable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Heated Floor Equation Source}\label{field-floor-heat-ceiling-cool-heated-floor-equation-source}
+
+Applies to zone with in-floor heating and/or in-ceiling cooling. This is for a floor with active heating elements. The key choice options include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, AwbiHattonHeatedFloor, or UserCurve
+
+\paragraph{Field: Floor Heat Ceiling Cool Heated Floor Equation User Curve Name}\label{field-floor-heat-ceiling-cool-heated-floor-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Chilled Ceiling Equation Source}\label{field-floor-heat-ceiling-cool-chilled-ceiling-equation-source}
+
+Applies to zone with in-floor heating and/or in-ceiling cooling. This is for a ceiling with active cooling elements. The key choice options include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, KaradagChilledCeiling, or UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Chilled Ceiling Equation User Curve Name}\label{field-floor-heat-ceiling-cool-chilled-ceiling-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
+
+\paragraph{Field: Floor Heat Ceiling Cool Stable Tilted Equation Source}\label{field-floor-heat-ceiling-cool-stable-tilted-equation-source}
+
+Applies to zone with in-floor heating and/or in-ceiling cooling. This is for tilted surfaces with heat flow for stable thermal stratification. The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Stable Tilted Equation User Curve Name}\label{field-floor-heat-ceiling-cool-stable-tilted-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Unstable Tilted Equation Source}\label{field-floor-heat-ceiling-cool-unstable-tilted-equation-source}
+
+Applies to zone with in-floor heating and/or in-ceiling cooling. This is for tilted surfaces with heat flow for unstable thermal stratification. The key choice options include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Unstable Tilted Equation User Curve Name}\label{field-floor-heat-ceiling-cool-unstable-tilted-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Window Equation Source}\label{field-floor-heat-ceiling-cool-window-equation-source}
+
+Applies to zone with in-floor heating and/or in-ceiling cooling. This is for all window surfaces. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Floor Heat Ceiling Cool Window Equation User Curve Name}\label{field-floor-heat-ceiling-cool-window-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Wall Panel Heating Vertical Wall Equation Source}\label{field-wall-panel-heating-vertical-wall-equation-source}
+
+Applies to zone with in-wall panel heating. This is for vertical walls that are not actively heated. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq6NonHeatedWalls, FohannoPolidoriVerticalWall, AlamdariHammondVerticalWall, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Wall Panel Heating Vertical Wall Equation User Curve Name}\label{field-wall-panel-heating-vertical-wall-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Wall Panel Heating Heated Wall Equation Source}\label{field-wall-panel-heating-heated-wall-equation-source}
+
+Applies to zone with in-wall panel heating. This is for vertical walls that are being actively heated. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq5WallNearHeat, AwbiHattonHeatedWall, FohannoPolidoriVerticalWall, AlamdariHammondVerticalWall, or UserCurve.
+
+\paragraph{Field: Wall Panel Heating Heated Wall Equation User Curve Name}\label{field-wall-panel-heating-heated-wall-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Wall Panel Heating Stable Horizontal Equation Source}\label{field-wall-panel-heating-stable-horizontal-equation-source}
+
+Applies to zone with in-wall panel heating. This is for horizontal surfaces with heat flow directed for stable thermal stratification. The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
+
+\paragraph{Field: Wall Panel Heating Stable Horizontal Equation User Curve Name}\label{field-wall-panel-heating-stable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Wall Panel Heating Unstable Horizontal Equation Source}\label{field-wall-panel-heating-unstable-horizontal-equation-source}
+
+Applies to zone with in-wall panel heating. This is for horizontal surfaces with heat flow directed for unstable thermal stratification. The key choice options include: ASHRAEVerticalWall, WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, KhalifaEq7Ceiling, or UserCurve
+
+\paragraph{Field: Wall Panel Heating Unstable Horizontal Equation User Curve Name}\label{field-wall-panel-heating-unstable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Wall Panel Heating Stable Tilted Equation Source}\label{field-wall-panel-heating-stable-tilted-equation-source}
+
+Applies to zone with in-wall panel heating. This is for tilted surfaces with heat flow for stable thermal stratification. The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Wall Panel Heating Stable Tilted Equation User Curve Name}\label{field-wall-panel-heating-stable-tilted-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
+
+\paragraph{Field: Wall Panel Heating Unstable Tilted Equation Source}\label{field-wall-panel-heating-unstable-tilted-equation-source}
+
+Applies to zone with in-wall panel heating. This is for tilted surfaces with heat flow for unstable thermal stratification. The key choice options include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Wall Panel Heating Unstable Tilted Equation User Curve Name}\label{field-wall-panel-heating-unstable-tilted-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Wall Panel Heating Window Equation Source}\label{field-wall-panel-heating-window-equation-source}
+
+Applies to zone with in-wall panel heating. This is for all window surfaces. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Wall Panel Heating Window Equation User Curve Name}\label{field-wall-panel-heating-window-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Convective Zone Heater Vertical Wall Equation Source}\label{field-convective-zone-heater-vertical-wall-equation-source}
+
+Applies to zone with convective heater. This is for vertical walls not directly affected by heater. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq3WallAwayFromHeat, KhalifaEq6NonHeatedWalls, FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve
+
+\paragraph{Field: Convective Zone Heater Vertical Wall Equation User Curve Name}\label{field-convective-zone-heater-vertical-wall-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Convective Zone Heater Vertical Walls Near Heater Equation Source}\label{field-convective-zone-heater-vertical-walls-near-heater-equation-source}
+
+Applies to zone with convective heater. This is for vertical walls that are directly affected by heater. Walls are considered ``near'' when listed in field set for Fraction of Radiant Energy to Surface. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq5WallNearHeat, AwbiHattonHeatedWall, FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Convective Zone Heater Vertical Walls Near Heater Equation User Curve Name}\label{field-convective-zone-heater-vertical-walls-near-heater-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Convective Zone Heater Stable Horizontal Equation Source}\label{field-convective-zone-heater-stable-horizontal-equation-source}
+
+Applies to zone with convective heater. This is for horizontal surfaces with heat flow directed for stable thermal stratification. The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
+
+\paragraph{Field: Convective Zone Heater Stable Horizontal Equation User Curve Name}\label{field-convective-zone-heater-stable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
+
+\paragraph{Field: Convective Zone Heater Unstable Horizontal Equation Source}\label{field-convective-zone-heater-unstable-horizontal-equation-source}
+
+Applies to zone with convective heater. This is for horizontal surfaces with heat flow directed for unstable thermal stratification. The key choice options include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, KhalifaEq4CeilingAwayFromHeat, KhalifaEq7Ceiling, or UserCurve.
+
+\paragraph{Field: Convective Zone Heater Unstable Horizontal Equation User Curve Name}\label{field-convective-zone-heater-unstable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Convective Zone Heater Stable Tilted Equation Source}\label{field-convective-zone-heater-stable-tilted-equation-source}
+
+Applies to zone with convective heater. This is for tilted surfaces with heat flow for stable thermal stratification. The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
+
+\paragraph{Field: Convective Zone Heater Stable Tilted Equation User Curve Name}\label{field-convective-zone-heater-stable-tilted-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Convective Zone Heater Unstable Tilted Equation Source}\label{field-convective-zone-heater-unstable-tilted-equation-source}
+
+Applies to zone with convective heater. This is for tilted surfaces with heat flow for unstable thermal stratification. The key choice options include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
+
+\paragraph{Field: Convective Zone Heater Unstable Tilted Equation User Curve Name}\label{field-convective-zone-heater-unstable-tilted-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Convective Zone Heater Windows Equation Source}\label{field-convective-zone-heater-windows-equation-source}
+
+Applies to zone with convective heater. This is for all window surfaces. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq3WallAwayFromHeat, FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Convective Zone Heater Windows Equation User Curve Name}\label{field-convective-zone-heater-windows-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Central Air Diffuser Wall Equation Source}\label{field-central-air-diffuser-wall-equation-source}
+
+Applies to zone with mechanical forced central air with diffusers. This is for all wall surfaces. The key choice options include: ASHRAEVerticalWall, FisherPedersenCeilingDiffuserWalls, AlamdariHammondVerticalWall, BeausoleilMorrisonMixedAssistedWall, BeausoleilMorrisonMixedOpposingWall, FohannoPolidoriVerticalWall, ISO15099Windows, GoldsteinNovoselacCeilingDiffuserWalls, or UserCurve
+
+\paragraph{Field: Central Air Diffuser Wall Equation User Curve Name}\label{field-central-air-diffuser-wall-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Central Air Diffuser Ceiling Equation Source}\label{field-central-air-diffuser-ceiling-equation-source}
+
+Applies to zone with mechanical forced central air with diffusers. This is for all ceiling surfaces. The key choice options include: FisherPedersenCeilingDiffuserCeiling, BeausoleilMorrisonMixedStableCeiling, BeausoleilMorrisonMixedUnstableCeiling, or UserCurve.
+
+\paragraph{Field: Central Air Diffuser Ceiling Equation User Curve Name}\label{field-central-air-diffuser-ceiling-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Central Air Diffuser Floor Equation Source}\label{field-central-air-diffuser-floor-equation-source}
+
+Applies to zone with mechanical forced central air with diffusers. This is for all floor surfaces. The key choice options include: FisherPedersenCeilingDiffuserFloor, BeausoleilMorrisonMixedStableFloor, BeausoleilMorrisonMixedUnstableFloor, GoldsteinNovoselacCeilingDiffuserFloor, or UserCurve.
+
+\paragraph{Field: Central Air Diffuser Floor Equation User Curve Name}\label{field-central-air-diffuser-floor-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Central Air Diffuser Window Equation Source}\label{field-central-air-diffuser-window-equation-source}
+
+Applies to zone with mechanical forced central air with diffusers. This is for all window surfaces. The key choice options include: ASHRAEVerticalWall, FisherPedersenCeilingDiffuserWalls, BeausoleilMorrisonMixedAssistedWall, BeausoleilMorrisonMixedOpposingWall, FohannoPolidoriVerticalWall, AlamdariHammondVerticalWall, ISO15099Windows, GoldsteinNovoselacCeilingDiffuserWindow, or UserCurve.
+
+\paragraph{Field: Central Air Diffuser Window Equation User Curve Name}\label{field-central-air-diffuser-window-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
+
+\paragraph{Field: Mechanical Zone Fan Circulation Vertical Wall Equation Source}\label{field-mechanical-zone-fan-circulation-vertical-wall-equation-source}
+
+The key choice options include: KhalifaEq3WallAwayFromHeat, ASHRAEVerticalWall, FisherPedersenCeilingDiffuserWalls, AlamdariHammondVerticalWall, BeausoleilMorrisonMixedAssistedWall, BeausoleilMorrisonMixedOpposingWall, FohannoPolidoriVerticalWall, ISO15099Windows, GoldsteinNovoselacCeilingDiffuserWalls, or UserCurve.
+
+\paragraph{Field: Mechanical Zone Fan Circulation Vertical Wall Equation User Curve Name}\label{field-mechanical-zone-fan-circulation-vertical-wall-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
+
+\paragraph{Field: Mechanical Zone Fan Circulation Stable Horizontal Equation Source}\label{field-mechanical-zone-fan-circulation-stable-horizontal-equation-source}
+
+The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
+
+\paragraph{Field: Mechanical Zone Fan Circulation Stable Horizontal Equation User Curve Name}\label{field-mechanical-zone-fan-circulation-stable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Mechanical Zone Fan Circulation Unstable Horizontal Equation Source}\label{field-mechanical-zone-fan-circulation-unstable-horizontal-equation-source}
+
+The key choice options include: KhalifaEq4CeilingAwayFromHeat, WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
+
+\paragraph{Field: Mechanical Zone Fan Circulation Unstable Horizontal Equation User Curve Name}\label{field-mechanical-zone-fan-circulation-unstable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Mechanical Zone Fan Circulation Stable Tilted Equation Source}\label{field-mechanical-zone-fan-circulation-stable-tilted-equation-source}
+
+The key choice options include: WaltonStableHorizontalOrTilt or UserCurve
+
+\paragraph{Field Mechanical Zone Fan Circulation Stable Tilted Equation User Curve Name}\label{field-mechanical-zone-fan-circulation-stable-tilted-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Mechanical Zone Fan Circulation Unstable Tilted Equation Source}\label{field-mechanical-zone-fan-circulation-unstable-tilted-equation-source}
+
+The key choice options include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
+
+\paragraph{Field: Mechanical Zone Fan Circulation Unstable Tilted Equation User Curve Name}\label{field-mechanical-zone-fan-circulation-unstable-tilted-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Mechanical Zone Fan Circulation Window Equation Source}\label{field-mechanical-zone-fan-circulation-window-equation-source}
+
+The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, ISO15099Windows, GoldsteinNovoselacCeilingDiffuserWindow, or UserCurve.
+
+\paragraph{Field: Mechanical Zone Fan Circulation Unstable Tilted Equation User Curve Name}\label{field-mechanical-zone-fan-circulation-unstable-tilted-equation-user-curve-name-1}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
+
+\paragraph{Field: Mixed Regime Buoyancy Assisting Flow on Walls Equation Source}\label{field-mixed-regime-buoyancy-assisting-flow-on-walls-equation-source}
+
+The key choice options include: BeausoleilMorrisonMixedAssistedWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, ASHRAEVerticalWall, FisherPedersenCeilingDiffuserWalls, GoldsteinNovoselacCeilingDiffuserWalls, or UserCurve.
+
+\paragraph{Field: Mixed Regime Buoyancy Assisting Flow on Walls Equation User Curve Name}\label{field-mixed-regime-buoyancy-assisting-flow-on-walls-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Mixed Regime Buoyancy Oppossing Flow on Walls Equation Source}\label{field-mixed-regime-buoyancy-oppossing-flow-on-walls-equation-source}
+
+The key choice options include: BeausoleilMorrisonMixedOpposingWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, ASHRAEVerticalWall, FisherPedersenCeilingDiffuserWalls, GoldsteinNovoselacCeilingDiffuserWalls, or UserCurve
+
+\paragraph{Field: Mixed Regime Buoyancy Oppossing Flow on Walls Equation User Curve Name}\label{field-mixed-regime-buoyancy-oppossing-flow-on-walls-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
+
+\paragraph{Field: Mixed Regime Stable Floor Equation Source}\label{field-mixed-regime-stable-floor-equation-source}
+
+The key choice options include: BeausoleilMorrisonMixedStableFloor, WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve
+
+\paragraph{Field: Mixed Regime Stable Floor Equation User Curve Name}\label{field-mixed-regime-stable-floor-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Mixed Regime Unstable Floor Equation Source}\label{field-mixed-regime-unstable-floor-equation-source}
+
+The key choice options include: BeausoleilMorrisonMixedUnstableFloor, WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
+
+\paragraph{Field: Mixed Regime Unstable Floor Equation User Curve Name}\label{field-mixed-regime-unstable-floor-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Mixed Regime Stable Ceiling Equation Source}\label{field-mixed-regime-stable-ceiling-equation-source}
+
+The key choice options include: BeausoleilMorrisonMixedStableCeiling, WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
+
+\paragraph{Field: Mixed Regime Stable Ceiling Equation User Curve Name}\label{field-mixed-regime-stable-ceiling-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Mixed Regime Unstable Ceiling Equation Source}\label{field-mixed-regime-unstable-ceiling-equation-source}
+
+The key choice options include: BeausoleilMorrisonMixedUnstableCeiling, WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
+
+\paragraph{Field: Mixed Regime Unstable Ceiling Equation User Curve Name}\label{field-mixed-regime-unstable-ceiling-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Mixed Regime Window Equation Source}\label{field-mixed-regime-window-equation-source}
+
+The key choice options include: GoldsteinNovoselacCeilingDiffuserWindow, ISO15099Windows, or UserCurve.
+
+\paragraph{Field: Mixed Regime Window Equation User Curve Name}\label{field-mixed-regime-window-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\subsection{SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections}\label{surfaceconvectionalgorithmoutsideadaptivemodelselections}
+
+Options to change the individual convection model equations for dynamic selection when using AdaptiveConvectionAlgorithm. This object is only needed to make changes to the default model selections for any or all of the surface categories. This object is for the outside face, the side of the surface facing away from the thermal zone.
+
+\subsubsection{Inputs}\label{inputs-7}
+
+\paragraph{Field: Name}\label{field-name-6}
+
+A unique name for the object
+
+\paragraph{Field: Wind Convection Windward Vertical Wall Equation Source}\label{field-wind-convection-windward-vertical-wall-equation-source}
+
+This is for just the wind-driven component of the total convection coefficient. The key choice options include: SimpleCombined, TARPWindward, MoWiTTWindward, DOE2Windward, NusseltJurges, McAdams, Mitchell, Blocken, Emmel, or UserCurve.
+
+\paragraph{Field: Wind Convection Windward Equation Vertical Wall User Curve Name}\label{field-wind-convection-windward-equation-vertical-wall-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Wind Convection Leeward Vertical Wall Equation Source}\label{field-wind-convection-leeward-vertical-wall-equation-source}
+
+This is for just the wind-driven component of the total convection coefficient. The key choice options include: SimpleCombined, TARPLeeward, MoWiTTLeeward, DOE2Leeward, Emmel, NusseltJurges, McAdams, Mitchell, or UserCurve.
+
+\paragraph{Field: Wind Convection Leeward Vertical Wall Equation User Curve Name}\label{field-wind-convection-leeward-vertical-wall-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Wind Convection Horizontal Roof Equation Source}\label{field-wind-convection-horizontal-roof-equation-source}
+
+This is for just the wind-driven component of the total convection coefficient. The key choice options include: SimpleCombined, TARPWindward, MoWiTTWindward, DOE2Windward, NusseltJurges, McAdams, Mitchell, Blocken, Emmel, ClearRoof, or UserCurve.
+
+\paragraph{Field: Wind Convection Horizontal Roof User Curve Name}\label{field-wind-convection-horizontal-roof-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Natural Convection Vertical Wall Equation Source}\label{field-natural-convection-vertical-wall-equation-source}
+
+This is for just the natural convection portion of the total film coefficient. This is for vertical walls. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, ISO15099Windows, UserCurve, or None.
+
+\paragraph{Field: Natural Convection Vertical Wall Equation User Curve Name}\label{field-natural-convection-vertical-wall-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Natural Convection Stable Horizontal Equation Source}\label{field-natural-convection-stable-horizontal-equation-source}
+
+This is for just the natural convection portion of the total film coefficient. This is for horizontal surfaces with heat flow directed for stable thermal stratification. The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, UserCurve, or None.
+
+\paragraph{Field: Natural Convection Stable Horizontal Equation User Curve Name}\label{field-natural-convection-stable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\paragraph{Field: Natural Convection Unstable Horizontal Equation Source}\label{field-natural-convection-unstable-horizontal-equation-source}
+
+This is for just the natural convection portion of the total film coefficient. This is for horizontal surfaces with heat flow directed for unstable thermal stratification. The key choice optios include: WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, UserCurve, or None
+
+\paragraph{Field: Natural Convection Unstable Horizontal Equation User Curve Name}\label{field-natural-convection-unstable-horizontal-equation-user-curve-name}
+
+The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
+
+\subsection{SurfaceConvectionAlgorithm:Inside:UserCurve}\label{surfaceconvectionalgorithminsideusercurve}
+
+This object is used to describe a custom model equation for surface convection heat transfer coefficients. If more than one curve is referenced, or non-blank, then they are all used and the result is the simple addition of all the curve results.
+
+\subsubsection{Inputs}\label{inputs-8}
+
+\paragraph{Field: Name}\label{field-name-7}
+
+Unique name of input object.
+
+\paragraph{Field: Reference Temperature for Convection Heat Transfer}\label{field-reference-temperature-for-convection-heat-transfer}
+
+This field controls the nature of the reference temperature used with convection coefficient when calculating the heat flow at the surface. Select one of the three choices: MeanAirTemperature, AdjacentAirTemperature, SupplyAirTemperature. MeanAirTemperature is the typical application for the classic convection model used with the complete mixing of room air. AdjacentAirTemperature applies when used with Roomair models that account for temperature variations within the zone air and directs the model to use the temperature near the surface rather than the average for the entire zone. SupplyAirTemperature directs the model to use the supply air conditions for the heat transfer conditions.
+
+\paragraph{Field: Hc Function of Temperature Difference Curve Name}\label{field-hc-function-of-temperature-difference-curve-name}
+
+This field contains the name of separate performance curve or table object that describes \emph{h\(_{c}\)}, the convection coefficient, as a function of temperature difference. The curve's ``x'' is absolute value of delta-T (Surface temperature minus air temperature, (C))
+
+\paragraph{Field: Hc Function of Temperature Difference Divided by Height Curve Name}\label{field-hc-function-of-temperature-difference-divided-by-height-curve-name}
+
+This field contains the name of separate performance curve or table object that describes \emph{h\(_{c}\)}, the convection coefficient, as a function of temperature difference divided by height. The curve's ``x'' is absolute value of delta-T/Height (Surface temp minus Air temp)/(vertical length scale), (C/m). For an inside face, the vertical length scale is the zone's interior height.
+
+\paragraph{Field: Hc Function of Air Change Rate Curve Name}\label{field-hc-function-of-air-change-rate-curve-name}
+
+This field contains the name of separate performance curve or table object that describes \emph{h\(_{c}\)}, the convection coefficient, as a function of air change rate. The curve's ``x'' is mechanical ACH (Air Changes per hour from mechanical air system), (1/hr)
+
+\paragraph{Field: Hc Function of Air System Volume Flow Rate Divided by Zone Perimeter Length Curve Name}\label{field-hc-function-of-air-system-volume-flow-rate-divided-by-zone-perimeter-length-curve-name}
+
+This field contains the name of separate performance curve or table object that describes \emph{h\(_{c}\)}, the convection coefficient, as a function of air change rate divided perimeter scale. Curve's ``x'' is mechanical system air flow rate (m\(^{3}\)/s) divided by zone's length along exterior walls (m).
+
+\subsection{SurfaceConvectionAlgorithm:Outside:UserCurve}\label{surfaceconvectionalgorithmoutsideusercurve}
+
+This object is used to describe a custom model equation for surface convection heat transfer coefficients. If more than one curve is referenced, or non-blank, then they are all used and the result is the simple addition of all the curve results.
+
+\subsubsection{Inputs}\label{inputs-9}
+
+\paragraph{Field: Name}\label{field-name-8}
+
+Unique name of input object.
+
+\paragraph{Field: Wind Speed Type for Curve}\label{field-wind-speed-type-for-curve}
+
+This field specifies what sort of wind velocity data should be used in when evaluating the curve in the following field. There are for key choice options. ``WeatherFile'' directs using the unmodified value from the epw file or design weather data. ``HeightAdjust'' uses the value from the epw file modified for height above ground, as determined by the z cooridinate, using the site terrain and weather station information. ``ParallelComponent'' uses the value from the epw file modified to take just the velocity component that is parallel to the surface. ``ParallelComponentHeightAdjust'' uses the height adjusted wind velocity and then computes the parallel component.
+
+\paragraph{Field: Hf Function of Wind Speed Curve Name}\label{field-hf-function-of-wind-speed-curve-name}
+
+This field contains the name of separate performance curve or table object that describes \emph{h\(_{f}\)}, the forced convection coefficient, as a function of wind speed. The curve's ``x'' is wind speed as defined by the method chosen in the previous field.
+
+\paragraph{Field: Hn Function of Temperature Difference Curve Name}\label{field-hn-function-of-temperature-difference-curve-name}
+
+This field contains the name of separate performance curve or table object that describes \emph{h\(_{n}\)}, the natural convection coefficient, as a function of temperature difference. Curve's ``x'' is absolute value of delta-T (Surface temperature minus air temperature, (C))
+
+\paragraph{Field: Hc Function of Temperature Difference Divided by Height Curve Name}\label{field-hc-function-of-temperature-difference-divided-by-height-curve-name-1}
+
+This field contains the name of separate performance curve or table object that describes \emph{h\(_{n}\)}, the natural convection coefficient, as a function of temperature difference divided by height. Curve's ``x'' is absolute value of delta-T/Height (Surface temp minus Air temp)/(vertical length scale), (C/m). For an outside face the vertical length scale is the exterior facade's overall height.
+
+\subsection{SurfaceProperty:ConvectionCoefficients}\label{surfacepropertyconvectioncoefficients}
+
+The convection coefficients of each surface, both exterior and interior, are automatically calculated during EnergyPlus execution. These calculations are ``governed'' by other objects such as the SurfaceConvectionAlgorithm:Inside (overall default), the Zone object's field called Zone Inside Convection Algorithm (Zone Default), the and the SurfaceConvectionAlgorithm:Outside (overall default), and/or the Zone object's field called Zone Outside Convection Algorithm (Zone Default). Usually, that will be enough flexibility for most users. However, if you need to match pre-existing convection coefficients (from another program) or are trying to match a test suite of results, you may wish to use the ``override'' convection coefficients in the following object. This object allows for a single surface to be given specific convection coefficients.
+
+Note that using these in conjunction, in particular, the ``Simple'' option on either the Outside Convection Algorithm or the Zone Outside Convection Algorithm field will result in a combined coefficient regardless of choice chosen here.
+
+\begin{callout}
+Note that surfaces with ``SurfaceProperty:OtherSideCoefficients'' cannot use this object with the ``outside'' coefficient -- attempting to do so will cause a severe error; SurfaceProperty:OtherSideCoefficients surfaces can apply an ``inside'' coefficient. And, surfaces with ``Ground'' exposure do not use the ``outside'' coefficient that might be supplied here. Note, too, that some lower boundaries are used regardless by certain surface types (i.e.~Window) or certain algorithm types.
+\end{callout}
+
+\subsubsection{Inputs}\label{inputs-10}
+
+\paragraph{Field: Surface Name}\label{field-surface-name-2}
+
+This field is the applicable surface name for the user supplied convection coefficient.
+
+\paragraph{Fields (Convection Location, Type, Coefficient \& Schedule Name)}\label{fields-convection-location-type-coefficient-schedule-name}
+
+For simplicity, the descriptions of these field occur together -- however, the fields are used sequentially when put into the IDF file (reference the IDF examples following the descriptions).
+
+\paragraph{Field: Convection Coefficient 1 Location}\label{field-convection-coefficient-1-location}
+
+\paragraph{Field: Convection Coefficient 2 Location}\label{field-convection-coefficient-2-location}
+
+This field contains the word ``Outside'' or ``Inside'' depending on which location is being described.
+
+\paragraph{Field: Convection Coefficient 1 Type}\label{field-convection-coefficient-1-type}
+
+\paragraph{Field: Convection Coefficient 2 Type}\label{field-convection-coefficient-2-type}
+
+The entries can be of several types: Value (simple numeric value), Schedule (name of schedule with the values), the usual key choices for overall models for Outside or Inside (Simple, SimpleCombined, TARP, AdaptiveConvectionAlgorithm etc.), the key choices for individual convection equations used for customizing the adaptive algorithm, or a custom user defined correlation. The field should contain one of the keys listed in the table below along with face they can be applied. The definitions of the models and key choices are discussed under SurfaceConvectionAlgorithm:Inside, SurfaceConvectionAlgorithm:Outside, SurfaceConvectionAlgorithm:Inside:AdaptiveModelSelections, and SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections.
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endhead
+
+300 & None~ \tabularnewline
+301 & UserValue \tabularnewline
+302 & UserSchedule \tabularnewline
+303 & UserCurve~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+304 & ASHRAESimpleCombined~~~~~~~~~~~~~~~~~~~ \tabularnewline
+305 & NaturalASHRAEVerticalWall~~~~~~~~~~~~~~ \tabularnewline
+306 & NaturalWaltonUnstableHorizontalOrTilt~~ \tabularnewline
+307 & NaturalWaltonStableHorizontalOrTilt~~~~ \tabularnewline
+308 & SparrowWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+309 & SparrowLeeward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+310 & MoWiTTWindward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+311 & MoWiTTLeeward~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+312 & DOE2Windward~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+313 & DOE2Leeward~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+314 & NusseltJurges~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+315 & McAdams~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+316 & Mitchell~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+317 & ClearRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+318 & BlockenWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+319 & EmmelVertical~~~~~~~~~~~~ ~~~~~~~~~~~~~~ \tabularnewline
+320 & EmmelRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+321 & AlamdariHammondVerticalWall~~~~~~~~~~~~ \tabularnewline
+322 & FohannoPolidoriVerticalWall~~~~~~~~~~~~ \tabularnewline
+323 & ISO15099Windows~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+324 & AlamdariHammondStableHorizontal~~~~~~~~ \tabularnewline
+325 & AlamdariHammondUnstableHorizontal~~~~~~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Field: Convection Coefficient 1}\label{field-convection-coefficient-1}
+
+\paragraph{Field: Convection Coefficient 2}\label{field-convection-coefficient-2}
+
+If the Convection type was ``Value'', then this field is filled and contains the simple value to be used. Otherwise, this can be blank.
+
+\paragraph{Field: Convection Coefficient 1 Schedule Name}\label{field-convection-coefficient-1-schedule-name}
+
+\paragraph{Field: Convection Coefficient 2 Schedule Name}\label{field-convection-coefficient-2-schedule-name}
+
+If the Convection type was ``Schedule'', then this field contains the name of a schedule describing the value to be used during the time intervals for the schedule.
+
+The complete IDD definition for the ConvectionCoefficients object follows:
+
+\paragraph{Field: Convection Coefficient 1 User Curve Name}\label{field-convection-coefficient-1-user-curve-name}
+
+\paragraph{Field: Convection Coefficient 2 User Curve Name}\label{field-convection-coefficient-2-user-curve-name}
+
+If the Convection type was ``UserCurve'', then this field contains the name of a SurfaceConvectionAlgorithm:UserCurve input objct describing the model equations to be used during the time intervals for the schedule.
+
+In IDF usage:
+
+\begin{lstlisting}
+
+SurfaceProperty:ConvectionCoefficients,
+  Zn001:Wall001,  ! Surface Name
+  Outside,        ! Convection Coefficient 1 Location
+  Value,          ! Convection Coefficient 1 Type
+  9.8,            ! Convection Coefficient 1
+  ,               ! Convection Coefficient 1 Schedule Name
+  ,               ! Convection Coefficient 1 User Curve Name
+  Inside,         ! Convection Coefficient 2 Location
+  Schedule,       ! Convection Coefficient 2 Type
+  ,               ! Convection Coefficient 2 {blank because using schedule}
+  MyInteriorCC,   ! Convection Coefficient 2 Schedule Name
+  ;               ! Convection Coefficient 2 User Curve Name
+
+  SurfaceProperty:ConvectionCoefficients,
+  Zn001:Wall002,  ! Surface Name
+  Inside,         ! Convection Coefficient 1 Location
+  Value,          ! Convection Coefficient 1 Type
+  .8,             ! Convection Coefficient 1
+  ,               ! Convection Coefficient 1 Schedule Name
+  ,               ! Convection Coefficient 1 User Curve Name
+  Outside,        ! Convection Coefficient 2 Location
+  Value,          ! Convection Coefficient 2 Type
+  5.5,            ! Convection Coefficient 2
+  ;               ! Convection Coefficient 2 User Curve Name
+
+  SurfaceProperty:ConvectionCoefficients,
+  Zn001:Wall003,  ! Surface Name
+  Outside,        ! Convection Coefficient 1 Location
+  Value,          ! Convection Coefficient 1 Type
+  9.8;            ! Convection Coefficient 1
+\end{lstlisting}
+
+\subsection{SurfaceProperty:ConvectionCoefficients:MultipleSurface}\label{surfacepropertyconvectioncoefficientsmultiplesurface}
+
+The convection coefficients of each surface, both outside and inside, are automatically calculated during EnergyPlus execution. These calculations are ``governed'' by other objects such as the Inside Convection Algorithm (overall default) and the Zone Inside Convection Algorithm (Zone Default) and the Outside Convection Algorithm (overall default) and/or the Zone Outside Convection Algorithm (Zone Default). Usually, that will be enough flexibility for most users. However, if you need to match pre-existing convection coefficients (from another program) or are trying to match a test suite of results, you may wish to use the ``override'' convection coefficients in the following object. This object is similar to the preceding ``ConvectionCoefficients'' object but allows multiple surfaces to be assigned a type with one object entry.
+
+Note that using these in conjunction, in particular, the ``Simple'' option on either the Outside Convection Algorithm or the Zone Outside Convection Algorithm field will result in a combined coefficient regardless of choice chosen here.
+
+Note that surfaces with ``SurfaceProperty:OtherSideCoefficients'' cannot use this object with the ``outside'' coefficient -- attempting to do so will ignore OSC surfaces during a multiple surface ``apply''; SurfaceProperty:OtherSideCoefficients surfaces can apply an ``inside'' coefficient. And, surfaces with ``Ground'' exposure do not use the ``outside'' coefficient that might be supplied here. Note, too, that some lower boundaries are used regardless by certain surface types (i.e.~Window) or certain algorithm types.
+
+\subsubsection{Inputs}\label{inputs-11}
+
+\paragraph{Field: Surface Type}\label{field-surface-type-1}
+
+This field is the applicable surface name for the user supplied convection coefficient. The allowable surface types are:
+
+\begin{itemize}
+\item
+  AllExteriorSurfaces~ (all surfaces that are ``external environment'' surfaces)
+\item
+  AllExteriorWindows (all windows that are ``external environment'' surfaces)
+\item
+  AllExteriorWalls
+\item
+  AllExteriorRoofs
+\item
+  AllExteriorFloors
+\item
+  AllInteriorSurface (all surfaces that are ``internal'' surfaces)
+\item
+  AllInteriorWindows
+\item
+  AllInteriorCeilings
+\item
+  AllInteriorFloors
+\end{itemize}
+
+\paragraph{Fields (Convection Location, Type, Coefficient \& Schedule Name)}\label{fields-convection-location-type-coefficient-schedule-name-1}
+
+For simplicity, the descriptions of these field occur together -- however, the fields are used sequentially when put into the IDF file (reference the IDF examples following the descriptions).
+
+\paragraph{Field: Convection Coefficient 1 Location}\label{field-convection-coefficient-1-location-1}
+
+\paragraph{Field: Convection Coefficient 2 Location}\label{field-convection-coefficient-2-location-1}
+
+This field contains the word ``Outside'' or ``Inside'' depending on which location is being described.
+
+\paragraph{Field: Convection Coefficient 1 Type}\label{field-convection-coefficient-1-type-1}
+
+\paragraph{Field: Convection Coefficient 2 Type}\label{field-convection-coefficient-2-type-1}
+
+The entries can be of several types: Value (simple numeric value), Schedule (name of schedule with the values), the usual key choices for overall models for Outside or Inside (Simple, SimpleCombined, TARP, AdaptiveConvectionAlgorithm etc.), the key choices for individual convection equations used for customizing the adaptive algorithm, or a custom user defined correlation. The field should contain one of the keys listed in the table below along with face they can be applied.~ The definitions of the models and key choices are discussed under SurfaceConvectionAlgorithm:Inside , SurfaceConvectionAlgorithm:Outside, SurfaceConvectionAlgorithm:Inside:AdaptiveModelSelections, and SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections.
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endhead
+
+300 & None~ \tabularnewline
+301 & UserValue \tabularnewline
+302 & UserSchedule \tabularnewline
+303 & UserCurve~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+304 & ASHRAESimpleCombined~~~~~~~~~~~~~~~~~~~ \tabularnewline
+305 & NaturalASHRAEVerticalWall~~~~~~~~~~~~~~ \tabularnewline
+306 & NaturalWaltonUnstableHorizontalOrTilt~~ \tabularnewline
+307 & NaturalWaltonStableHorizontalOrTilt~~~~ \tabularnewline
+308 & SparrowWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+309 & SparrowLeeward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+310 & MoWiTTWindward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+311 & MoWiTTLeeward~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+312 & DOE2Windward~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+313 & DOE2Leeward~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+314 & NusseltJurges~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+315 & McAdams~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+316 & Mitchell~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+317 & ClearRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+318 & BlockenWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+319 & EmmelVertical~~~~~~~~~~~~ ~~~~~~~~~~~~~~ \tabularnewline
+320 & EmmelRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+321 & AlamdariHammondVerticalWall~~~~~~~~~~~~ \tabularnewline
+322 & FohannoPolidoriVerticalWall~~~~~~~~~~~~ \tabularnewline
+323 & ISO15099Windows~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+324 & AlamdariHammondStableHorizontal~~~~~~~~ \tabularnewline
+325 & AlamdariHammondUnstableHorizontal~~~~~~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Field: Convection Coefficient 1}\label{field-convection-coefficient-1-1}
+
+\paragraph{Field: Convection Coefficient 2}\label{field-convection-coefficient-2-1}
+
+If the Convection type was ``Value'', then this field is filled and contains the simple value to be used. Otherwise, this can be blank.
+
+\paragraph{Field: Convection Coefficient 1 Schedule Name}\label{field-convection-coefficient-1-schedule-name-1}
+
+\paragraph{Field: Convection Coefficient 2 Schedule Name}\label{field-convection-coefficient-2-schedule-name-1}
+
+If the Convection type was ``Schedule'', then this field contains the name of a schedule describing the value to be used during the time intervals for the schedule.
+
+\paragraph{Field: Convection Coefficient 1 User Curve Name}\label{field-convection-coefficient-1-user-curve-name-1}
+
+\paragraph{Field: Convection Coefficient 2 User Curve Name}\label{field-convection-coefficient-2-user-curve-name-1}
+
+If the Convection type was ``UserCurve'', then this field contains the name of a SurfaceConvectionAlgorithm:UserCurve input objct describing the model equations to be used during the time intervals for the schedule.
+
+In IDF usage:
+
+\begin{lstlisting}
+
+SurfaceProperty:ConvectionCoefficients:MultipleSurface,
+  AllExteriorWindows,  ! Surface Types
+  Outside,             ! Convection Coefficient 1 Location
+  MoWitt;              ! Convection Coefficient 1 Type
+\end{lstlisting}
+
+\subsection{Convection Coefficient Application Hierarchy}\label{convection-coefficient-application-hierarchy}
+
+Ultimate flexibility and possibly ultimate user confusion can result from the convection coefficient possibilties in EnergyPlus. The objects that control how convection models are assigned to individual surfaces~ are:
+
+\begin{itemize}
+\item
+  SurfaceConvectionAlgorithm:Inside
+\item
+  SurfaceConvectionAlgorithm:Outside
+\item
+  Zone, Field: Zone Inside Convection Algorithm
+\item
+  Zone, Field: Zone Outside Convection Algorithm
+\item
+  SurfaceProperty:ConvectionCoefficients
+\item
+  SurfaceProperty:ConvectionCoefficients:MultipleSurface
+\end{itemize}
+
+General to Specific, they are assigned in this order:
+
+% table 9
+\begin{longtable}[c]{p{2.96in}p{3.03in}}
+\caption{Convection Coefficient Assignment Hierarchy \label{table:convection-coefficient-assignment-hierarchy}} \tabularnewline
+\toprule 
+Objects/Description & Action \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Convection Coefficient Assignment Hierarchy} \tabularnewline
+\toprule 
+Objects/Description & Action \tabularnewline
+\midrule
+\endhead
+
+SurfaceConvectionAlgorithm:* & Assigns for all surfaces in the run. \tabularnewline
+Zone, Fields: Zone * Convection Algorithm & Trumps global assignment and assigns for all surfaces in Zone. \tabularnewline
+SurfaceProperty:...:MultipleSurfaces & Trumps above and assigns for specific types of surfaces. \tabularnewline
+Two Multiple Surface Assignments overlapping (such as AllExteriorSurfaces vs AllExteriorWalls) & Order in IDF is now important. Whichever is first gets the cookie and the second gets a warning. \tabularnewline
+Specific Surface Assignment & Trumps all Above. \tabularnewline
+\bottomrule
+\end{longtable}
+
+There are additional objects that provide fine control over the models that get assigned.
+
+\begin{itemize}
+\item
+  SurfaceConvectionAlgorithm:Inside:AdaptiveModelSelections
+\item
+  SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections
+\item
+  SurfaceConvectionAlgorithm:Inside:UserCurve
+\item
+  SurfaceConvectionAlgorithm:Outside:UserCurve
+\end{itemize}
+
+\subsection{Convection Coefficients Outputs}\label{convection-coefficients-outputs}
+
+Outputs for the User Supplied Convection Coefficients appear as values in the Surface Output Variables (\emph{Surface Inside Face Convection Heat Transfer Coefficient} and \emph{Surface Outside Face Convection Heat Transfer Coefficient}). What the program expects to use is shown in the Surface Details report (\emph{Output:Surfaces:List, Details;})
+
+When EnergyPlus is set to Display Advanced Variables (Output:Diagnostics, DisplayAdvancedVariables;), then additional output variables are available that indicate the status of convection modeling by identifying which models are in effect at a given time.~ The adaptive convection algorithms may switch between models over time and the following output variables provide a way to monitor this behavior.~ These outputs are integer codes and the integer values are explained in tables.
+
+\subsubsection{Surface Inside Face Convection Classification Index}\label{surface-inside-face-convection-classification-index}
+
+This variable reports how the surface was classified as part of the adaptive convection algorithm for the inside face.~ The algorithm examines probable flow regimes, heat flow directions, orientations, HVAC equipment connections, and current operating status to assign each surface a category.~ The numbers in this report are integer codes that correspond to surface categories as described in the following table.
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endhead
+
+300 & None~ \tabularnewline
+301 & UserValue \tabularnewline
+302 & UserSchedule \tabularnewline
+303 & UserCurve~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+304 & ASHRAESimpleCombined~~~~~~~~~~~~~~~~~~~ \tabularnewline
+305 & NaturalASHRAEVerticalWall~~~~~~~~~~~~~~ \tabularnewline
+306 & NaturalWaltonUnstableHorizontalOrTilt~~ \tabularnewline
+307 & NaturalWaltonStableHorizontalOrTilt~~~~ \tabularnewline
+308 & SparrowWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+309 & SparrowLeeward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+310 & MoWiTTWindward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+311 & MoWiTTLeeward~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+312 & DOE2Windward~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+313 & DOE2Leeward~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+314 & NusseltJurges~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+315 & McAdams~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+316 & Mitchell~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+317 & ClearRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+318 & BlockenWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+319 & EmmelVertical~~~~~~~~~~~~ ~~~~~~~~~~~~~~ \tabularnewline
+320 & EmmelRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+321 & AlamdariHammondVerticalWall~~~~~~~~~~~~ \tabularnewline
+322 & FohannoPolidoriVerticalWall~~~~~~~~~~~~ \tabularnewline
+323 & ISO15099Windows~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+324 & AlamdariHammondStableHorizontal~~~~~~~~ \tabularnewline
+325 & AlamdariHammondUnstableHorizontal~~~~~~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Surface Inside Face Convection Model Equation Index}\label{surface-inside-face-convection-model-equation-index}
+
+This variable reports the specific model equation used to calculate the inside face convection coefficient.~ This can vary when using the adaptive convection algorithm and so the result of that selection algorithm is reported here.~ The following table lists the models associated with specific interger codes reported here.~ The models correspond to key words used in input objects.
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endhead
+
+300 & None~ \tabularnewline
+301 & UserValue \tabularnewline
+302 & UserSchedule \tabularnewline
+303 & UserCurve~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+304 & ASHRAESimpleCombined~~~~~~~~~~~~~~~~~~~ \tabularnewline
+305 & NaturalASHRAEVerticalWall~~~~~~~~~~~~~~ \tabularnewline
+306 & NaturalWaltonUnstableHorizontalOrTilt~~ \tabularnewline
+307 & NaturalWaltonStableHorizontalOrTilt~~~~ \tabularnewline
+308 & SparrowWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+309 & SparrowLeeward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+310 & MoWiTTWindward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+311 & MoWiTTLeeward~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+312 & DOE2Windward~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+313 & DOE2Leeward~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+314 & NusseltJurges~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+315 & McAdams~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+316 & Mitchell~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+317 & ClearRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+318 & BlockenWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+319 & EmmelVertical~~~~~~~~~~~~ ~~~~~~~~~~~~~~ \tabularnewline
+320 & EmmelRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+321 & AlamdariHammondVerticalWall~~~~~~~~~~~~ \tabularnewline
+322 & FohannoPolidoriVerticalWall~~~~~~~~~~~~ \tabularnewline
+323 & ISO15099Windows~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+324 & AlamdariHammondStableHorizontal~~~~~~~~ \tabularnewline
+325 & AlamdariHammondUnstableHorizontal~~~~~~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Surface Inside Face Convection Reference Air Index}\label{surface-inside-face-convection-reference-air-index}
+
+The inside face convection heat transfer calculations can be based on different reference air temperatures.~ This reference air temperature can vary during the simulation when the adaptive algorithm selects models that use different references.~ The following table lists the meaning of the integer codes.
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endhead
+
+300 & None~ \tabularnewline
+301 & UserValue \tabularnewline
+302 & UserSchedule \tabularnewline
+303 & UserCurve~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+304 & ASHRAESimpleCombined~~~~~~~~~~~~~~~~~~~ \tabularnewline
+305 & NaturalASHRAEVerticalWall~~~~~~~~~~~~~~ \tabularnewline
+306 & NaturalWaltonUnstableHorizontalOrTilt~~ \tabularnewline
+307 & NaturalWaltonStableHorizontalOrTilt~~~~ \tabularnewline
+308 & SparrowWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+309 & SparrowLeeward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+310 & MoWiTTWindward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+311 & MoWiTTLeeward~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+312 & DOE2Windward~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+313 & DOE2Leeward~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+314 & NusseltJurges~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+315 & McAdams~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+316 & Mitchell~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+317 & ClearRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+318 & BlockenWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+319 & EmmelVertical~~~~~~~~~~~~ ~~~~~~~~~~~~~~ \tabularnewline
+320 & EmmelRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+321 & AlamdariHammondVerticalWall~~~~~~~~~~~~ \tabularnewline
+322 & FohannoPolidoriVerticalWall~~~~~~~~~~~~ \tabularnewline
+323 & ISO15099Windows~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+324 & AlamdariHammondStableHorizontal~~~~~~~~ \tabularnewline
+325 & AlamdariHammondUnstableHorizontal~~~~~~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Surface Outside Face Convection Classification Index}\label{surface-outside-face-convection-classification-index}
+
+This variable reports how the surface was classified as part of the adaptive convection algorithm for the outside face.~ The algorithm examines the wind direction, heat flow directions and orientations to assign each surface a category.~ The numbers in this report are integer codes that correspond to surface categories as described in the following table.
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endhead
+
+300 & None~ \tabularnewline
+301 & UserValue \tabularnewline
+302 & UserSchedule \tabularnewline
+303 & UserCurve~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+304 & ASHRAESimpleCombined~~~~~~~~~~~~~~~~~~~ \tabularnewline
+305 & NaturalASHRAEVerticalWall~~~~~~~~~~~~~~ \tabularnewline
+306 & NaturalWaltonUnstableHorizontalOrTilt~~ \tabularnewline
+307 & NaturalWaltonStableHorizontalOrTilt~~~~ \tabularnewline
+308 & SparrowWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+309 & SparrowLeeward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+310 & MoWiTTWindward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+311 & MoWiTTLeeward~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+312 & DOE2Windward~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+313 & DOE2Leeward~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+314 & NusseltJurges~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+315 & McAdams~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+316 & Mitchell~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+317 & ClearRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+318 & BlockenWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+319 & EmmelVertical~~~~~~~~~~~~ ~~~~~~~~~~~~~~ \tabularnewline
+320 & EmmelRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+321 & AlamdariHammondVerticalWall~~~~~~~~~~~~ \tabularnewline
+322 & FohannoPolidoriVerticalWall~~~~~~~~~~~~ \tabularnewline
+323 & ISO15099Windows~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+324 & AlamdariHammondStableHorizontal~~~~~~~~ \tabularnewline
+325 & AlamdariHammondUnstableHorizontal~~~~~~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Surface Outside Face Forced Convection Model Equation Index}\label{surface-outside-face-forced-convection-model-equation-index}
+
+\subsubsection{Surface Outside Face Natural Convection Model Equation Index}\label{surface-outside-face-natural-convection-model-equation-index}
+
+These variables report the specific model equation used to calculate the outside face's convection coefficient.~ They can vary when using the adaptive convection algorithm and so the results of that selection algorithm are reported in these variables.~ The following table lists the models associated with specific integer codes that might be reported here.~ The models correspond to key words used in input objects.
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Report Code & Related key and model \tabularnewline
+\midrule
+\endhead
+
+300 & None~ \tabularnewline
+301 & UserValue \tabularnewline
+302 & UserSchedule \tabularnewline
+303 & UserCurve~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+304 & ASHRAESimpleCombined~~~~~~~~~~~~~~~~~~~ \tabularnewline
+305 & NaturalASHRAEVerticalWall~~~~~~~~~~~~~~ \tabularnewline
+306 & NaturalWaltonUnstableHorizontalOrTilt~~ \tabularnewline
+307 & NaturalWaltonStableHorizontalOrTilt~~~~ \tabularnewline
+308 & SparrowWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+309 & SparrowLeeward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+310 & MoWiTTWindward~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+311 & MoWiTTLeeward~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+312 & DOE2Windward~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+313 & DOE2Leeward~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+314 & NusseltJurges~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+315 & McAdams~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+316 & Mitchell~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+317 & ClearRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+318 & BlockenWindward~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+319 & EmmelVertical~~~~~~~~~~~~ ~~~~~~~~~~~~~~ \tabularnewline
+320 & EmmelRoof~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+321 & AlamdariHammondVerticalWall~~~~~~~~~~~~ \tabularnewline
+322 & FohannoPolidoriVerticalWall~~~~~~~~~~~~ \tabularnewline
+323 & ISO15099Windows~~~~~~~~~~~~~~~~~~~~~~~~ \tabularnewline
+324 & AlamdariHammondStableHorizontal~~~~~~~~ \tabularnewline
+325 & AlamdariHammondUnstableHorizontal~~~~~~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{SurfaceProperties:VaporCoefficients}\label{surfacepropertiesvaporcoefficients}
+
+Advanced/Research Usage: The internal and external vapor transfer coefficients that are used by the CombinedHeatAndMoistureFiniteElement model are automatically calculated during EnergyPlus execution using information on the convection coefficients. However it is sometimes useful to be able to ``override'' the calculation and set fixed values of vapor transfer coefficient for a single surface. These coefficients are only used by the CombinedHeatAndMoistureFiniteElement model and will be ignored by other solution algorithms.
+
+\subsubsection{Inputs}\label{inputs-12}
+
+\paragraph{Field: Surface Name}\label{field-surface-name-3}
+
+This field is the applicable surface name for the user supplied vapor transfer coefficient.
+
+\paragraph{Field: Constant External Vapor Transfer Coefficient}\label{field-constant-external-vapor-transfer-coefficient}
+
+Select `yes' to use the value supplied as the external vapor transfer coefficient
+
+\paragraph{Field: External Vapor Coefficient Value}\label{field-external-vapor-coefficient-value}
+
+HAMT will use this value to calculate the vapour transfer into and out off the external surface of this surface. Units are kg/Pa.s.m2.
+
+\paragraph{Field: Constant Internal vapor Transfer Coefficient}\label{field-constant-internal-vapor-transfer-coefficient}
+
+Select `yes' to use the value supplied as the internal vapor transfer coefficient
+
+\paragraph{Field: Internal Vapor Coefficient Value}\label{field-internal-vapor-coefficient-value}
+
+The CombinedHeatAndMoistureFiniteElement algorithm will use this value to calculate the vapor transfer into and out of the internal surface of this surface. Units are kg/Pa.s.m2.
+
+Below is an example input of vapor transfer coefficients for a surface.
+
+\begin{lstlisting}
+
+SurfaceProperties:VaporCoefficients,
+        South wall,     !- Surface Name
+        Yes,     !- Constant External Vapor Transfer Coefficient
+        0.0000000625,     !- External Vapor Coefficient Value
+        Yes,     !- Constant Internal vapor Transfer Coefficient
+        0.00000002;     !- Internal Vapor Coefficient Value
+\end{lstlisting}
+
+\subsection{SurfaceProperty:ExteriorNaturalVentedCavity}\label{surfacepropertyexteriornaturalventedcavity}
+
+This object is used to model a multi-skin exterior heat transfer surface. This is a special case where the outside face is a slightly detached layer forming a naturally ventilated cavity. The actual outer surface is referred to as the baffle. The modeling here assumes that the heat capacity in the outer baffle can be neglected since it is much lower than the underlying mass surface. This object is used with the BuildingSurface:Detailed object where the Heat Transfer surfaces are referred to as the underlying surfaces. The constructions and materials for the BuildingSurface:Detailed object should reflect the construction of just the underlying surface. The SurfaceProperty:ExteriorNaturalVentedCavity object is used to describe the decoupled layer, or baffle, and the characteristics of the cavity and openings for natural ventilation. This object is also used in conjunction with the OtherSideConditionsModel.
+
+The area and orientation are obtained from \textbf{BuildingSurface:Detailed} objects, which are referenced by name. This object can be used to model certain types of photovoltaic mounting configurations such as interlocking roof pavers. If the baffle covers only part of a surface, then that surface should be split into separate \textbf{BuildingSurface:Detailed} objects where one matches the size of the baffle. A single baffle can be associated with as many \textbf{BuildingSurface:Detailed} objects as desired (although if you need to use more than 10 surfaces, then the IDD will need to be extended). The base heat transfer surfaces need not be contiguous nor have the same orientation, but the program will issue warnings if surfaces have widely ranging tilts and azimuths.
+
+Note that the model involves predicting the rates that ambient air moves in and out of the cavity. Accurate modeling of these air flows would be extremely challenging and so the models provided through this object are simplistic engineering models based on discharge coefficients that are sensitive to wind and bouancy effects. The accuracy depends on the values for, and applicability of, the discharge coefficients and unfortunately little research is available to help characterize these. The models should be considered rudimentary and the user is encouraged to explore different values for the coefficients in attempts to bound the importance of natural ventilation for the cavities. See the Engineering Reference for more details.
+
+\subsubsection{Inputs}\label{inputs-13}
+
+\paragraph{Field: Name}\label{field-name-9}
+
+This field contains a unique name for the ventilated cavity.
+
+\paragraph{Field: Boundary Conditions Model Name}\label{field-boundary-conditions-model-name}
+
+This field contains the name of an SurfaceProperty:OtherSideConditionsModel object declared elsewhere in the input file. This will connect the baffle and ventilated cavity to the exterior boundary conditions for the underlying heat transfer surface.
+
+\paragraph{Field: Area Fraction of Openings}\label{field-area-fraction-of-openings}
+
+This field is used to enter an area fraction for what part of the baffle consists of openings. The area of the openings will set to the product of this field and the sum of the area of the underlying surfaces.
+
+\paragraph{Field: Thermal Emissivity of Exterior Baffle Material}\label{field-thermal-emissivity-of-exterior-baffle-material}
+
+This field is used to enter the thermal emissivity of the baffler. This surface property is for longwave infrared radiation. The property is used for both sides of collector. Most painted materials have an emissivity of 0.9.
+
+\paragraph{Field: Solar Absorptivity of Exterior Baffle}\label{field-solar-absorptivity-of-exterior-baffle}
+
+This field is used to enter the solar absorbtivity of the baffle. This surface property is for shortwave, solar radiation. The property is used for the front side of the baffle that faces the environment. Darker colors have a higher absorptivity. While black is the highest performance, other colors might be used to match the color scheme of the rest of the façade.
+
+\paragraph{Field: Height Scale for Buoyancy-Driven Ventilation}\label{field-height-scale-for-buoyancy-driven-ventilation}
+
+This field is used to enter a nominal height scale (m) for prediction of ventilation induced by bouancy. This value (\(\Delta {H_{NPL}}\) ) is defined as the height from the midpoint of the lower opening to the neutral pressure level. Increasing the value will increase the ventilation rate due to buoyancy.
+
+\paragraph{Field: Effective Thickness of Cavity Behind Exterior Baffle}\label{field-effective-thickness-of-cavity-behind-exterior-baffle}
+
+This field is used to enter a nominal gap thickness (m) for the collector. If the baffle is corrugated, use the average depth. This distance value is only used when the collector is near horizontal to determine a length scale in the vertical direction for buoyancy calculations. For example, if the collector is mounted on a flat roof, its tilt-adjusted height is zero and the program will use this gap thickness as a length scale rather than the height from the previous field.
+
+\paragraph{Field: Ratio of Actual Surface Area to Projected Surface Area}\label{field-ratio-of-actual-surface-area-to-projected-surface-area}
+
+This field is used to enter a factor that accounts for the extra surface area resulting from and uneven baffle surface. Corrugations may be present to help stiffen the baffle or ventilated roofing tiles may have more surface are for convection heat transfer than the underlying surface. The projected surface area is obtained by the program from the (flat) underlying surfaces. If the baffle is flat then this ratio is 1.0. If the baffle is corrugated, then this ratio will be greater than one with a typical value might be 1.165.
+
+\paragraph{Field: Roughness of Exterior Surface}\label{field-roughness-of-exterior-surface}
+
+This field is used to describe the relative roughness of the baffle material. This field is similar to one in the \textbf{Material} object. This parameter only influences the convection coefficients, more specifically the exterior convection coefficient. A special keyword is expected in this field with the options being ``VeryRough'', ``Rough'', ``MediumRough'', ``MediumSmooth'', ``Smooth'', and ``VerySmooth'' in order of roughest to smoothest options.
+
+\paragraph{Field: Effectiveness for Perforations with Respect to Wind}\label{field-effectiveness-for-perforations-with-respect-to-wind}
+
+This field is used to enter a value for the coefficient used to determine natural air exchanges from wind. Wind will cause exterior air to move in and out of the cavity. Cv is an arbitrary coefficient used to model the effectiveness of openings and depends on opening geometry and the orientation with respect to the wind. Cv should probably be in the range 0.05 to 0.65. Increasing Cv will increase the amount of natural ventilation. The following equation shows how Cv is used in the program to predict the volumetric flow rate due to wind:
+
+\begin{equation}
+  \dot{V}_{\rm{wind}} = C_v A_{\rm{in}} U_{\infty}
+\end{equation}
+
+\paragraph{Field: Discharge Coefficient for Openings with Respect to Buoyancy Driven Flow}\label{field-discharge-coefficient-for-openings-with-respect-to-buoyancy-driven-flow}
+
+This field is used to enter a value for the coefficient used to determine natural air exchanges from buoyancy. Stack or buoyancy effects will cause exterior air to move in and out of the cavity. Cd is an arbitrary discharge coefficient that depends on the geometry of the opening. Cd should probably be in the range 0.1 to 1.0. Increasing Cd will increase the amount of natural ventilation. The following equations show how Cd is used in the program to predict the volume flow rate due to buoyancy:
+
+\(\dot{V}_{thermal} = C_D A_{in} \sqrt 2 g \Delta H_{NPL} \left( T_{a,cav} - T_{amb} \right) / T_{a,cav}\) (if \(T_{a,cav} > T_{amb}\) )
+
+\(\dot{V}_{\text{thermal}} = C_D A_{in} \sqrt 2 g \Delta H_{NPL} \left( T_{amb} - T_{a,cav} \right) / T_{amb}\) (if \(T_{amb} > T_{a,cav}\) and baffle is vertical)
+
+where \(\Delta {H_{NPL}}\) is the value input into the field above for the height scale for buoyancy-driven ventilation.
+
+\paragraph{Field(s): Surface \textless{}1 thru x\textgreater{} Name}\label{fields-surface-1-thru-x-name}
+
+The remaining fields are used to name the \textbf{BuildingSurface:Detailed} objects that are associated with the exterior naturally vented cavity. These are the underlying heat transfer surfaces and are defined elsewhere in the input file. These surfaces should all specify OtherSideConditionsModel as their exterior environment. The input object can currently accommodate up to ten surfaces, but it is extensible by modifying the Energy+.idd entry.
+
+An example IDF entry is
+
+\begin{lstlisting}
+SurfaceProperty:ExteriorNaturalVentedCavity,
+  PVRoofPaverExtVentCav1 ,   ! Name
+  PVRoofPaverSystem1,        ! OtherSideConditionsModel Object Name
+  0.02,    ! Area Fraction of Openings
+  0.9,     ! Thermal Emissivity of Exterior Baffle Material
+  0.92,    ! Solar Absorbtivity of Exterior Baffle
+  0.05,    ! Height scale for buoyancy-driven ventilation
+  0.05,    ! Effective Thickness of Cavity Behind Exterior Baffle
+  0.97,    ! Ratio of Actual surface area to projected surface area
+  Smooth , ! Roughness of collector
+  0.1 ,    ! Cv, Effectiveness for perforations with respect to Wind
+  0.5 ,    ! Cd, Discharge Coefficient for Openings with respect to buoyancy-driven flow
+  Zn001:Roof001 ;    ! Surface Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2}
+
+In addition to related output that can be obtained for all surfaces, these outputs are available for exterior naturally vented cavity configurations:
+
+\begin{itemize}
+\item
+  HVAC,Average, Surface Exterior Cavity Air Drybulb Temperature {[}C{]}
+\item
+  HVAC,Average, Surface Exterior Cavity Baffle Surface Temperature {[}C{]}
+\item
+  HVAC,Average, Surface Exterior Cavity Total Natural Ventilation Air Change Rate {[}ACH{]}
+\item
+  HVAC,Average, Surface Exterior Cavity Total Natural Ventilation Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average, Surface Exterior Cavity Natural Ventilation from Wind Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average, Surface Exterior Cavity Natural Ventilation from Buoyancy Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Surface Exterior Cavity Air Drybulb Temperature {[}C{]}}\label{surface-exterior-cavity-air-drybulb-temperature-c}
+
+The temperature of air inside the cavity behind the baffle.
+
+\paragraph{Surface Exterior Cavity Baffle Surface Temperature {[}C{]}}\label{surface-exterior-cavity-baffle-surface-temperature-c}
+
+The surface temperature of the exterior baffle material itself.
+
+\paragraph{Surface Exterior Cavity Total Natural Ventilation Air Change Rate {[}ACH{]}}\label{surface-exterior-cavity-total-natural-ventilation-air-change-rate-ach}
+
+The rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive in Air Changes per Hour.
+
+\paragraph{Surface Exterior Cavity Total Natural Ventilation Mass Flow Rate {[}kg/s{]}}\label{surface-exterior-cavity-total-natural-ventilation-mass-flow-rate-kgs}
+
+The mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive.
+
+\paragraph{Surface Exterior Cavity Natural Ventilation from Wind Mass Flow Rate {[}kg/s{]}}\label{surface-exterior-cavity-natural-ventilation-from-wind-mass-flow-rate-kgs}
+
+The part of mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive due to wind-driven forces.
+
+\paragraph{Surface Exterior Cavity Natural Ventilation from Buoyancy Mass Flow Rate {[}kg/s{]}}\label{surface-exterior-cavity-natural-ventilation-from-buoyancy-mass-flow-rate-kgs}
+
+The part of mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive due to buoyancy-driven forces.
+
+\subsection{SurfaceProperty:SolarIncidentInside}\label{surfacepropertysolarincidentinside}
+
+This object can be used as an alternative to the standard (automatic) EnergyPlus calculation of the solar radiation incident on interior surfaces of the building. Using this method, the normal EnergyPlus calculation is replaced with a schedule of solar incidence values that are calculated outside the program.
+
+\subsubsection{Inputs}\label{inputs-14}
+
+\paragraph{Field: Name}\label{field-name-10}
+
+The name of the SurfaceProperty:SolarIncidentInside object Must be unique between all SurfaceProperty:SolarIncidentInside objects.
+
+\paragraph{Field: Surface Name}\label{field-surface-name-4}
+
+The building surface associated with this object (ref BuildingSurface:Detailed). Solar absorptance values in the schedule file will be applied to the inside of this surface.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-1}
+
+The building construction associated with this object (ref Construction). It is possible that the Energy Management System will change the construction associated with the surface; if the construction is changed, a new set of data may need to be applied to the current surface.
+
+\paragraph{Field: Inside Surface Incident Sun Solar Radiation Schedule Name}\label{field-inside-surface-incident-sun-solar-radiation-schedule-name}
+
+This field specifies the name of a schedule that contains the values for incident solar radiation. Values from the schedule data will be used to replace the absorbed solar radiation that would normally be calculated by EnergyPlus. Units in the external schedule file must be W/m\(^{2}\).
+
+Example for SurfaceProperty:SolarIncidentInside using a compact schedule:
+
+\begin{lstlisting}
+
+  Schedule:Compact,
+      North Wall SSG,          !- Name
+      Positive Number,         !- Schedule Type Limits Name
+      Through: 12/31,          !- Field 1
+      For: AllDays,            !- Field 2
+      Until: 07:00,10,         !- Field 3
+      Until: 17:00,20,         !- Field 5
+      Until: 24:00,15;         !- Field 7
+
+
+    SurfaceProperty:SolarIncidentInside,
+      North Wall Solar Incident,  !- Name
+      Room102 North Wall,         !- Surface Name
+      Room Wall - North,          !- Construction Name
+      North Wall SSG;             !- Schedule Name
+\end{lstlisting}
+
+\subsection{ComplexFenestrationProperty:SolarAbsorbedLayers}\label{complexfenestrationpropertysolarabsorbedlayers}
+
+This object can be used as an alternative to the standard (automatic) EnergyPlus calculation of the solar radiation absorbed by fenestration systems in the building. Using this method, the normal EnergyPlus calculation is replaced with a schedule of solar absorptance values that are calculated outside the program.
+
+\subsubsection{Inputs}\label{inputs-15}
+
+\paragraph{Field: Name}\label{field-name-11}
+
+The name of the ComplexFenestrationProperty:SolarAbsorbedLayers object Must be unique between all ComplexFenestrationProperty:SolarAbsorbedLayers objects.
+
+\paragraph{Field: Fenestration Surface}\label{field-fenestration-surface}
+
+The fenestration surface associated with this object (ref FenestrationSurface:Detailed). Values from the schedule data will be used to replace the absorbed solar radiation in the fenestration layers that would normally be calculated by EnergyPlus. Value units in the schedule must be W/m\(^{2}\).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-2}
+
+The building construction associated with this object (ref Construction). It is possible that the Energy Management System will change the construction associated with the surface; if the construction is changed, a new set of data may need to be applied to the current surface.
+
+\paragraph{Field: Layer 1 Solar Radiation Absorbed Schedule Name}\label{field-layer-1-solar-radiation-absorbed-schedule-name}
+
+Specifies the name of a schedule that contains the absorbed solar radiation values in units of W/m\(^{2}\). Values from the schedule are used for the absorbed solar radiation of the first (outside) layer .
+
+\paragraph{Field: Layer 2 Solar Radiation Absorbed Schedule Name}\label{field-layer-2-solar-radiation-absorbed-schedule-name}
+
+Specifies the name of a schedule that contains absorbed solar radiation values in units of W/m\(^{2}\). Values from the schedule are used for the absorbed solar radiation of the second layer .
+
+\paragraph{Field: Layer 3 Solar Radiation Absorbed Schedule Name}\label{field-layer-3-solar-radiation-absorbed-schedule-name}
+
+Specifies the name of a schedule that contains absorbed solar radiation values in units of W/m\(^{2}\). Values from the schedule are used for the absorbed solar radiation for the third layer .
+
+\paragraph{Field: Layer 4 Solar Radiation Absorbed Schedule Name}\label{field-layer-4-solar-radiation-absorbed-schedule-name}
+
+Specifies the name of a schedule that contains absorbed solar radiation values in units of W/m\(^{2}\). Values from the schedule are used for the absorbed solar radiation of the fourth layer.
+
+\paragraph{Field: Layer 5 Solar Radiation Absorbed Schedule Name}\label{field-layer-5-solar-radiation-absorbed-schedule-name}
+
+Specifies the name of a schedule that contains absorbed solar radiation values in units of W/m\(^{2}\). Values from the schedule are used for the absorbed solar radiation of the fifth layer .
+
+Example for ComplexFenestrationProperty:SolarAbsorbedLayers with compact schedules:
+
+\begin{lstlisting}
+
+  Schedule:Compact,
+      Layer 1,                 !- Name
+      Positive Number,         !- Schedule Type Limits Name
+      Through: 12/31,          !- Field 1
+      For: AllDays,            !- Field 2
+      Until: 07:00,1,         !- Field 3
+      Until: 17:00,2,         !- Field 5
+      Until: 24:00,1.5;         !- Field 7
+
+
+    Schedule:Compact,
+      Layer 2,                 !- Name
+      Positive Number,         !- Schedule Type Limits Name
+      Through: 12/31,          !- Field 1
+      For: AllDays,            !- Field 2
+      Until: 07:00,0.8,        !- Field 3
+      Until: 17:00,1.2,        !- Field 5
+      Until: 24:00,1.0;        !- Field 7
+
+
+    Schedule:Compact,
+      Layer 3,                 !- Name
+      Positive Number,         !- Schedule Type Limits Name
+      Through: 12/31,          !- Field 1
+      For: AllDays,            !- Field 2
+      Until: 07:00,1,          !- Field 3
+      Until: 17:00,2.1,        !- Field 5
+      Until: 24:00,1.7;        !- Field 7
+
+
+    ComplexFenestrationProperty:SolarAbsorbedLayers,
+      South Window Solar Absorbed Layers, !- Name
+      Room 102 South Window,              !- Fenestration surface name
+      CFS_Glz_2,                          !- Construction Surface name
+      Layer 1,                            !- Absorbed solar energy in layer 1
+      Layer 2,                            !- Absorbed solar energy in layer 2
+      Layer 3;                            !- Absorbed solar energy in layer 3
+\end{lstlisting}
+
+\subsection{GeometryTransform}\label{geometrytransform}
+
+This object provides a simple method of altering the footprint geometry of a model. The intent is to provide a single parameter that can be used to reshape the building description contained in the rest of the input file. This object was implemented for use in parametric massing studies and with the optimization program GenOpt. Although building footprint is often constrained in practice, analysts may find this object useful for investigating how building form impacts daylighting and solar gains on the east and west facades with out having to change all of the surface geometry input.
+
+Aspect Ratio is defined as the overall length in the East-West direction divided by the overall length in the North-South direction.
+
+This object should be used with considerable care since it will completely alter the geometry modeled by EnergyPlus and may have unintended side effects. The surface areas of all horizontal surfaces may change radically with corresponding changes in Zone floor areas. The total floor area will not change but individual horizontal surfaces will gain and loose area. Vertical surfaces will have the same height but will gain and lose length. Lighting and electrical equipment design levels for individual zones will likely have a different energy per unit area in the transformed geometry.
+
+The surface geometry must be set to \textbf{Relative}, see \textbf{GlobalGeometryRules}. Of course, the coordinates must be entered in relative coordinates as well.
+
+Since windows in EnergyPlus need to be rectangular, it is possible to define a horizontal window (skylight) that once transformed is no longer rectangular and will cause EnergyPlus to halt. To avoid this problem, horizontal windows should be defined orthogonal to the Cardinal directions and building rotation (see \textbf{Building}) used to orient the final form with respect to North.
+
+The object doesn't create any specific output, but the results of using it can be understood by viewing DXF output files. Figure~\ref{fig:example-of-geometry-transform-aspect-ratio} shows an example of a building that has been morphed using the Aspect Ratio Transform object. Using this object allowed the same geometry input to generate both of the models represented in by their DXF output files.
+
+\begin{figure}[hbtp] % fig 43
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image078.png}
+\caption{Example of Geometry Transform -- Aspect Ratio \protect \label{fig:example-of-geometry-transform-aspect-ratio}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-16}
+
+\paragraph{Field: Plane of Transform}\label{field-plane-of-transform}
+
+This field specifies the plane that the geometry transform should act on. It is currently restricted to altering the horizontal footprint of a building and must be set to ``XY.''
+
+\paragraph{Field: Current Aspect Ratio}\label{field-current-aspect-ratio}
+
+This field specifies the aspect ratio of the building geometry described in the rest of the input file. It is used to scale the new aspect ratio. If this field is set to 1.0, then the altered building will not necessarily have the new aspect ratio defined in the next field.
+
+\paragraph{Field: New Aspect Ratio}\label{field-new-aspect-ratio}
+
+This field specifies the aspect ratio that the building described in the rest of the input file will be changed to.
+
+\subsection{Zone Property View Factors}\label{zone-property-view-factors}
+
+EnergyPlus has two options for specifying the thermal radiation exchange view factors between surfaces in a zone: the approximate option and the user input option. Because the actual geometric arrangement within a zone is very complex, the approximate method of including thermal mass and other forced exchanges is more realistic than trying to come up with ``exact'' view factors. However, in some research situations it might be desirable to have control of the view factors used. For this reason, a user input mode has been included in EnergyPlus. The two modes are described in the next sections.
+
+\subsubsection{Approximate Option}\label{approximate-option}
+
+The first option produces approximate results and uses an area weighted scheme to calculate ``view factors'' between surfaces within a thermal zone. Each surface uses the total area that it can ``see'' among the other surfaces. The approximate view factor from this surface to each other surface is then the area of the receiving surface over the sum of areas that are visible to the sending surface.
+
+In order to account in some limited way for the fact that certain surfaces will not see each other, several assumptions have been built into this view factor approximation. First, a surface cannot see itself. Second, surfaces with approximately the same azimuth (facing direction) and tilt (``same'' being within a built in limit) will not see each other. This means that a window will not see the wall that it is placed on, for example. Third, floors cannot see each other. Fourth, if the surface is a floor, ceiling, roof, or internal mass, the rule for the same azimuth and tilt eliminating radiant exchange between surfaces is waived when the receiving surface is floor, roof, ceiling, or internal mass as long as both surfaces are not floors.
+
+Note that this does not take into account that surfaces may be ``around the corner'' from each other and in reality not see each other at all. Rooms are assumed to be convex rather than concave in this method.
+
+To summarize, using the Surface ``Class'', the approximate view factors have:
+
+\begin{enumerate}
+  \item
+    No surface sees itself.
+  \item
+    No Floor sees another floor.
+  \item
+    All other surface types see Internal Mass.
+  \item
+    All other surface types see floors.
+  \item
+    Floors always see ceilings.
+  \item
+    Floors always see roofs.
+  \item
+    All other surfaces whose tilt or facing angle differences are greater than 10 degrees see each other.
+\end{enumerate}
+
+If geometry is correct, conditions 1, 3, and 7 should take care of all surfaces, but the other conditions supply common sense when the geometry is incorrect. More information about the EnergyPlus view factor calculation is contained in the Engineering Reference document.
+
+\subsubsection{User Input View Factors}\label{user-input-view-factors}
+
+The second option for specifying view factors requires user input values. These should be used with care in research or special situations. The object available for this is ZoneProperty:UserViewFactors:bySurfaceName.
+
+\subsection{ZoneProperty:UserViewFactors:bySurfaceName}\label{zonepropertyuserviewfactorsbysurfacename}
+
+The method of entering user view factors is to entere each surface name and its view factor value to other surfaces in the zone
+
+\subsubsection{Inputs}\label{inputs-17}
+
+\paragraph{Field: Zone Name}\label{field-zone-name}
+
+This field is the zone name for the view factors.
+
+\paragraph{Field: From Surface 1}\label{field-from-surface-1}
+
+This field specifies the name of the ``from surface''.
+
+\paragraph{Field: To Surface 1}\label{field-to-surface-1}
+
+This field specifies the name of the ``to surface''.
+
+\paragraph{Field: Factor 1}\label{field-factor-1}
+
+This value is the view factor for ``from Surface'' to ``to Surface''.
+
+An IDF Example:
+
+\begin{lstlisting}
+ZoneProperty:UserViewFactors:bySurfaceName,Lshaped Zone,
+    Lshaped Zone:South Wall,Lshaped Zone:South Wall,0.000000,
+    Lshaped Zone:South Wall,Lshaped Zone:East Wall,0.101310,
+  <snip>
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-air-distribution-equipment.tex b/doc/input-output-reference/src/overview/group-air-distribution-equipment.tex
new file mode 100644
index 00000000000..c7b7bbc980e
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-air-distribution-equipment.tex
@@ -0,0 +1,2035 @@
+\section{Group -- Air Distribution Equipment}\label{group-air-distribution-equipment}
+
+The systems described in the Air Distribution Units (ADU's) are shown below. A variety of air terminal units are available for connecting air systems to thermal zones. These single description ADU's contain the reference to the components and the actual controls in one block of input. The idea is that the control volume is drawn tightly around the controls and loosely around the components. This allows complex interactions to take place between all of the components that respond to the Zone Thermostatic Control output. The coils that are referenced in the ADU's are explained fully in the ``Coils'' section of this manual.
+
+\subsection{AirTerminal:SingleDuct:Uncontrolled}\label{airterminalsingleductuncontrolled}
+
+Central system air is usually supplied to a zone through a terminal unit such as a single duct VAV reheat box. Sometimes, however, it is desirable to supply central system air directly to a zone without any zone level control or tempering. An example would be a single zone reheat system.
+
+The control zone receives supply air directly from the central system since the supply air temperature has been adjusted to control the temperature in the control zone. The slave zones then have baseboards or reheat coils to allow some temperature adjustment. The AirTerminal:SingleDuct:Uncontrolled object creates the capability of supplying central system air directly to a zone. Its input consists of the object name, an availability (on/off) schedule, and a node name. This node is both a zone inlet node and an outlet node of the AirLoopHVAC:ZoneSplitter.
+
+For the objects to work correctly, it is important in any systems including Direct Air objects for the sum of the maximum zone air flow rates to be equal to the maximum central system flow rate. The zone maximum flow rates are specified in the zone terminal unit or direct air inputs. The central air system flow rate is specified in the AirLoopHVAC input and also in the air loop branch and central fan inputs.
+
+\subsubsection{Inputs}\label{inputs-001}
+
+\paragraph{Field: Name}\label{field-name-001}
+
+A unique user assigned name for each AirTerminal:SingleDuct:Uncontrolled component. Any other component that needs to use this direct air component will refer to it by this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes whether the component can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Zone Supply Air Node Name}\label{field-zone-supply-air-node-name}
+
+The name of the node to which the component is supplying air. This should be one of the supply air nodes for the zone the component is serving. This node should also be an outlet node of a AirLoopHVAC:ZoneSplitter component.
+
+\paragraph{Field: Maximum Air Flow Rate}\label{field-maximum-air-flow-rate}
+
+The design maximum volume flow rate~ (m\(^{3}\)/sec) specified for the AirTerminal:SingleDuct:Uncontrolled object.~ This field is autosizable.
+
+An example input follows.
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:Uncontrolled,
+      Zone1DirectAir,
+      FanAndCoilAvailSched,
+      Zone 1 Inlet Node,
+      0.47;
+  AirTerminal:SingleDuct:Uncontrolled,
+      Zone2DirectAir,
+      FanAndCoilAvailSched,
+      Zone 2 Inlet Node,
+      0.36;
+  AirTerminal:SingleDuct:Uncontrolled,
+      Zone3DirectAir,
+      FanAndCoilAvailSched,
+      Zone 3 Inlet Node,
+      0.47;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-000}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Zone Air Terminal Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Air Terminal Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Air Terminal Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air Terminal Sensible Cooling Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Zone Air Terminal Sensible Heating Energy~ {[}J{]}}\label{zone-air-terminal-sensible-heating-energy-j}
+
+\paragraph{Zone Air Terminal Sensible Heating Rate {[}W{]}}\label{zone-air-terminal-sensible-heating-rate-w}
+
+These outputs are the sensible heating power and energy provided to the zone by the uncontrolled air terminal unit.
+
+\paragraph{Zone Air Terminal Sensible Cooling Energy {[}J{]}}\label{zone-air-terminal-sensible-cooling-energy-j}
+
+\paragraph{Zone Air Terminal Sensible Cooling Rate {[}W{]}}\label{zone-air-terminal-sensible-cooling-rate-w}
+
+These outputs are the sensible cooling power and energy provided to the zone by the uncontrolled air terminal unit.
+
+\subsection{AirTerminal:SingleDuct:ConstantVolume:Reheat}\label{airterminalsingleductconstantvolumereheat}
+
+The AirTerminal:SingleDuct:ConstantVolume:Reheat or terminal reheat system is a constant volume reheat system. The systems cooling capabilities are provided by way of cooling coil that supplies cooling to the entire supply air volume. The cooling coil is controlled by a controller setpoint specified for the cooling coil. Zone control is accomplished by heating (reheating) the airflow into each zone as determined by the zone thermostat. Currently the reheat can be supplied by a electric, gas, or hot water coil that tries to meet the zone demand.
+
+\subsubsection{Inputs}\label{inputs-1-001}
+
+\paragraph{Field: Name}\label{field-name-1-000}
+
+Unique name for the terminal reheat Air Distribution Unit (ADU).
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1}
+
+Schedule that this component will operate or is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name}
+
+The outlet node from the ADU to the zone. This is the same node as the reheat component air outlet node.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name}
+
+The air-inlet node name that connects the air splitter to the individual zone ADU. This is the same node as the reheat component air inlet node.
+
+\paragraph{Field: Maximum Air Flow Rate}\label{field-maximum-air-flow-rate-1}
+
+The design constant volume flow rate (m\(^{3}\)/sec) specified for the terminal reheat ADU.
+
+\paragraph{Field: Reheat Coil Object Type}\label{field-reheat-coil-object-type}
+
+The valid reheat component objects currently available are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Reheat Coil Name}\label{field-reheat-coil-name}
+
+Reheat Coil Object name being simulated with this ADU. Applicable for all coils.
+
+\paragraph{Field: Maximum Hot Water or Steam Flow Rate}\label{field-maximum-hot-water-or-steam-flow-rate}
+
+This field is zero for gas and electric coils. Set to the maximum design hot water or steam volumetric flow rate in m\(^{3}\)/s for the hot water or steam heating coil. The steam volumetric~ flow rate is calculated at 100C and 101325 Pa.
+
+\paragraph{Field: Minimum Hot Water or Steam Flow Rate}\label{field-minimum-hot-water-or-steam-flow-rate}
+
+This field is zero for gas and electric coils. Set to the minimum design hot water or steam volumetric flow rate in m\(^{3}\)/s for the hot water or steam coil, normally set to be a shut off valve that is set to zero. The steam volumetric~ flow rate is calculated at 100C and 101325 Pa.
+
+\paragraph{Field: Convergence Tolerance}\label{field-convergence-tolerance}
+
+The coil is controlled by knowing the zone demand determined by the zone thermostat and setting the outlet conditions to meet this demand. For the electric and gas coils, this is set exactly since the coil model solution can be inverted. With the hot water coil that uses an effectiveness-NTU method, the solution cannot be inverted directly. Therefore, to determine the correct mass flow rate for the hot water the solution is solved for by iteration. The iterative solution uses an interval halving routine and needs a termination criteria that is set with the Convergence Tolerance parameter. This control offset is set to a decimal fraction of the zone demand as the criteria, i.e.~0.001. The default for the field is 0.001.
+
+\paragraph{Field: Maximum Reheat Air Temperature}\label{field-maximum-reheat-air-temperature}
+
+This is the upper limit on the temperature in degrees C of the air leaving the terminal unit -- reheat coil (and being delivered to the zone). If the user leaves this field blank, no maximum reheat air temperature is enforced.
+
+An IDF example:
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:ConstantVolume:Reheat,
+      Reheat Zone 1,  !- Name of System
+      FanAndCoilAvailSched,  !- Availability schedule for VAV System
+      Zone 1 Reheat Air Outlet Node,  !- Unit Air Outlet Node
+      Zone 1 Reheat Air Inlet Node,  !- Unit Air Inlet Node
+      0.59,  !- Maximum air flow rate {m3/s}
+      COIL:Gas:Heating,  !- Reheat Component Object
+      Reheat Coil Zone 1,  !- Name of Reheat Component
+      0.0,  !- Max Reheat Water Flow {m3/s}
+      0.0,  !- Min Reheat Water Flow {m3/s}
+      0.001;  !- Convergence Tolerance
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-000}
+
+There are no outputs for the constant volume reheat air terminal.
+
+\subsection{AirTerminal:SingleDuct:VAV:Reheat}\label{airterminalsingleductvavreheat}
+
+AirTerminal:SingleDuct:VAV:Reheat - Variable air volume (VAV) systems control the dry-bulb temperature inside a zone by varying the supply air volume instead of the air temperature. At full cooling the VAV damper is fully open supplying the specified maximum air flow rate. As the cooling load decreases, the damper closes until it reaches the minimum stop specified by the zone minimum air flow fraction.
+
+VAV systems can be used for interior or perimeter zones with a common fan system, air temperature control, and reheating devices. The VAV concept may vary according to the VAV box locations, air temperature controls and types of heating elements. Heating can usually be provided by use of reheat coils or thermostatic baseboard.
+
+\subsubsection{Inputs}\label{inputs-2-001}
+
+\paragraph{Field: Name}\label{field-name-2-000}
+
+Unique name for the AirTerminal:SingleDuct:VAV:Reheat Air Distribution Unit (ADU).
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-2}
+
+Schedule that this component will operate or is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Damper Air Outlet Node Name}\label{field-damper-air-outlet-node-name}
+
+The VAV damper outlet node. This is the outlet node of the damper and the inlet node of the reheat coil.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-1}
+
+The air inlet node name that connects the air splitter to the individual zone ADU. This is \emph{not} the same as the air inlet node of the reheat component: it is upstream of that node. This is the inlet node to the terminal unit and the damper
+
+\paragraph{Field: Maximum Air Flow Rate}\label{field-maximum-air-flow-rate-2}
+
+The design maximum volume flow rate (m\(^{3}\)/sec) specified for VAV ADU.
+
+\paragraph{Field: Zone Minimum Air Flow Method}\label{field-zone-minimum-air-flow-method}
+
+This field is used to select how the program will determine the minimum flow rate to the zone while the system is operating.~ There are three choices for selecting how the minimum flow rate is specified:~ Constant, FixedFlowRate, and Scheduled.~ If Constant is entered, then the program will use the value for the constant minimum air flow fraction entered in the following field.~ If FixedFlowRate is entered, then the program will use the value entered in the field below called Fixed Minimum Air Flow Rate.If Scheduled is entered, then the program will obtain the value for minimum flow fraction from the schedule named in the field below called Minimum Air Flow Fraction Schedule Name.
+
+\paragraph{Field: Constant Minimum Air Flow Fraction}\label{field-constant-minimum-air-flow-fraction}
+
+The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default).~ This field is used if the previous field is set to Constant.~ If the previous field is set to Scheduled (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then this field is optional and can be used to separately control the air flow rate used for sizing normal-action reheat coils. If this field and the following field have values, the greater of the two is used for sizing.
+
+\paragraph{Field: Fixed Minimum Air Flow Rate}\label{field-fixed-minimum-air-flow-rate}
+
+The minimum flow rate to the zone while the system is operating, specified as a fixed minimum air flow rate in meters cubed per second. The minimum air flow rate is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default).~ This field is used if the Zone Minimum Air Flow Method field is set to FixedFlowRate. If the Zone Minimum Air Flow Method field is set to Scheduled (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then this field is optional and can be used to separately control the air flow rate used for sizing normal-action reheat coils. Only one of these two minimum air flow fields (i.e., this field and the previous field) should be used at any time. If this field and the previous field have values, the greater of the two is used for sizing.
+
+\paragraph{Field: Minimum Air Flow Fraction Schedule Name}\label{field-minimum-air-flow-fraction-schedule-name}
+
+The name of a schedule that determines the value of the minimum air flow fraction.~ The schedule should contain fractions from 0.0 to 1.0.~ These values will define the minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate.~ The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default).~ This field is used if the previous field is set to Scheduled.~ If the previous field is left blank (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then the air flow rate usedfor sizing normal-action reheat coils is the average of the minimum and maximum values in this schedule.~ The air flow rate used for reheat coil sizing is reported with other component sizing information as ``Reheat Coil Sizing Air Volume Flow Rate.''
+
+\paragraph{Field: Reheat Coil Object Type}\label{field-reheat-coil-object-type-1}
+
+The valid reheat component objects currently available are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+If there is no reheat coil,use AirTerminal:SingleDuct:VAV:NoReheat instead of this object.
+
+\paragraph{Field: Reheat Coil Name}\label{field-reheat-coil-name-1}
+
+Reheat Coil Object name being simulated with this ADU. Applicable for all coils. If there is no reheat coil,use object AirTerminal:SingleDuct:VAV:NoReheat instead of this object.
+
+\paragraph{Field: Maximum Hot Water or Steam Flow Rate}\label{field-maximum-hot-water-or-steam-flow-rate-1}
+
+This field is zero for gas and electric coils. Set to the maximum design hot water or steam volumetric flow rate in m\(^{3}\)/s for the hot water or steam heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. This field is autosizable. If there is no reheat coil,~ this is left blank.
+
+\paragraph{Field: Minimum Hot Water or Steam Flow Rate}\label{field-minimum-hot-water-or-steam-flow-rate-1}
+
+This field is zero for gas and electric coils. Set to the minimum design hot water or steam volumetric flow rate in m\(^{3}\)/s for the hot water or steam heating coil, normally set to be a shut off valve that is set to zero. The steam volumetric flow rate is calculated at 100C and 101325 Pa. If there is no reheat coil,~ this is left blank.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-1}
+
+The terminal unit outlet node. This is the outlet node of the reheat coil and the zone inlet node.
+
+\paragraph{Field: Convergence Tolerance}\label{field-convergence-tolerance-1}
+
+The coil is controlled by knowing the zone demand determined by the zone thermostat and setting the outlet conditions to meet this demand. For the electric and gas coils, this is set exactly since the coil model solution can be inverted. With the hot water coil that uses an effectiveness-NTU method, the solution cannot be inverted directly. Therefore, to determine the correct mass flow rate for the hot water the solution is solved for by iteration. The iterative solution uses an interval halving routine and needs a termination criteria that is set with the Convergence Tolerance parameter. This control offset is set to a decimal fraction of the zone demand as the criteria, i.e.~0.001. The default for the field is 0.001.
+
+\paragraph{Field: Damper Heating Action}\label{field-damper-heating-action}
+
+During heating operation, there are two control options for the damper controlling the air flow in the VAV terminal unit as the zone moves above or below the zone setpoint. With both control options, the damper is at the minimum air flow rate whenever the zone temperature is between the cooling and heating setpoints (deadband condition).
+
+With \textbf{Normal} (the default) action, the damper will remain at the minimum air flow rate during heating operation. As the heating load increases, the water flow rate in the reheat coil will be increased to maintain temperature in the zone until the maximum water flow rate is reached or the user-specified maximum reheat air temperature is reached.. ~This is sometimes called the single maximum control logic as illustrated below.
+
+\begin{figure}[hbtp] % fig 102
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image264.png}
+\caption{The Single Maximum Control Logic \protect \label{fig:the-single-maximum-control-logic}}
+\end{figure}
+
+With \textbf{Reverse} action, as the heating load increases, the unit starts at minimum air flow and minimum hot water flow. The hot water flow is increased until it reaches maximum flow or the user-specified maximum reheat air temperature is reached, then the air damper starts to open to meet the load. This option is used if the minimum air flow rate is not adequate to serve the peak heating load. This is sometimes called the dual maximum control logic as illustrated in following figure. For heating coil types other than the hot-water coil, e.g.~electric, steam, and gas, the reverse action works the same as the normal action -- always keeping the air flow at the minimum during heating.
+
+The dual-max control currently applies to the AirTerminal:SingleDuct:VAV:Reheat objects with reverse acting dampers and hot-water coils.
+
+\begin{figure}[hbtp] % fig 103
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image265.png}
+\caption{  The Dual Maximum Control Logic \protect \label{fig:the-dual-maximum-control-logic}}
+\end{figure}
+
+\paragraph{Control Fields for Maximum Flow During Reheat:}\label{control-fields-for-maximum-flow-during-reheat}
+
+The following two fields are used only when Reheat Coil Object Type = Coil:Heating:Water and Damper Heating Action = Reverse. Maximum Flow per Zone Floor Area During Reheat and Maximum Flow Fraction During Reheat are two optional methods to calculate the maximum allowable air flow rate during reheat operation. If both are entered, the greater resulting flow rate is used. If Design Specification Outdoor Air Object Name is also specified, it may increase this limit to meet the outdoor air flow rate requirement. At no time will the maximum flow rate calculated here exceed the value for Maximum Air Flow Rate.
+
+This limit is active only when the zone thermostat requests heating and the VAV box damper is reverse acting.
+
+\paragraph{Field: Maximum Flow per Zone Floor Area During Reheat}\label{field-maximum-flow-per-zone-floor-area-during-reheat}
+
+This factor (m\(^{3}\)/s-m\(^{2}\)) is multiplied by the zone area, to determine the maximum volume flow rate (m\(^{3}\)/s) allowed during reheat operation (see detailed explanation above). This field is autocalculatable. If autocalculate is selected, the value is set to 0.002032 m\(^{3}\)/s-m\(^{2}\) (0.4 cfm/ft\(^{2}\)). If this field and the following field are entered, the greater of the two inputs is used. If this field and the following field are left blank, the maximum flow will not be limited.
+
+\paragraph{Field: Maximum Flow Fraction During Reheat}\label{field-maximum-flow-fraction-during-reheat}
+
+This fraction is multiplied by the Maximum Air Flow Rate to determine the maximum volume flow rate (m\(^{3}\)/s) allowed during reheat operation (see detailed explanation above). This field is autocalculatable. If autocalculate is selected, the value is set to 0.002032 m\(^{3}\)/s-m\(^{2}\) (0.4 cfm/ft\(^{2}\)) multiplied by the zone floor area divided by the Maximum Air Flow Rate. If this field and the previous field are entered, the greater of the two inputs is used. If this field and the previous field are left blank, the maximum flow will not be limited.
+
+\paragraph{Field: Maximum Reheat Air Temperature}\label{field-maximum-reheat-air-temperature-1}
+
+This field specifies a maximum supply air temperature (°C) leaving the reheat coil in a VAV terminal unit during heating operation. If leaving blank, the temperature of the supply air to the space in heating operation may get unrealistic high.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object. When this field is used, the terminal unit will increase flow as needed to meet this outdoor air requirement. If Outdoor Air Flow per Person is non-zero, then the outdoor air requirement will be computed based on the current number of occupants in the zone. At no time will the supply air flow rate exceed the value for Maximum Air Flow Rate. If this field is blank, then the terminal unit will not be controlled for outdoor air flow. See documentation for the zone HVAC outdoor air object for further information (Ref DesignSpecification:OutdoorAir).
+
+An IDF example:
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:VAV:Reheat,
+      SPACE2-1 VAV Reheat,  !- Name of System
+      ReheatCoilAvailSched,  !- Availability schedule for VAV System
+      SPACE2-1 Zone Coil Air In Node,  !- Damper Air Outlet Node
+      SPACE2-1 ATU In Node,  !- Unit Air Inlet Node
+      autosize,  !- Maximum air flow rate {m3/s}
+      Constant,  !- Zone Minimum Air Flow Input Method
+      0.3,  !- Constant Minimum Air Flow Fraction
+      ,  !- Fixed Minimum Air Flow Rate
+      ,  !- Minimum Air Flow Fraction Schedule Name
+      COIL:Gas:Heating,  !- Reheat Component Object
+      SPACE2-1 Zone Coil,  !- Name of Reheat Component
+      0.0,  !- Max Reheat Water Flow {m3/s}
+      0.0,  !- Min Reheat Water Flow {m3/s}
+      SPACE2-1 In Node,  !- Unit Air Outlet Node
+      0.001,  !- Convergence Tolerance
+  Reverse,  !- Damper Heating Action
+  ,         !- Maximum Flow per Zone Floor Area During Reheat
+  ,         !- Maximum Flow Fraction During Reheat
+  35.0,     !- Maximum Reheat Air Temperature {C}
+      ;         !- Design Specification Outdoor Air Object Name
+
+    DesignSpecification:OutdoorAir,
+      ZoneMinOARequirements,    !- Name
+      Sum,                      !- Outdoor Air Method
+      0.00472,                  !- Outdoor Air Flow per Person {m3/s}
+      0.000508,                 !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
+      ,                         !- Outdoor Air Flow per Zone
+      ,                         !- Outdoor Air Flow Air Changes per Hour
+      Min OARequirements Sched; !- Outdoor Air Flow Rate Fraction Schedule Name
+
+
+    Schedule:Compact,
+      Min OARequirements Sched,  !- Name
+      Any Number,                !- Schedule Type Limits Name
+      Through: 12/31,            !- Field 1
+      For: Weekdays SummerDesignDay WinterDesignDay, !- Field 2
+      Until: 24:00,1.0,          !- Field 7
+      For: AllOtherDays,         !- Field 9
+      Until: 24:00,0.25;         !- Field 10
+  COIL:Heating:Gas,
+      SPACE1-1 Zone Coil,  !- Coil Name
+      ReheatCoilAvailSched,  !- Availability Schedule Name
+      0.8,  !- Gas Burner Efficiency of the Coil
+      autosize,  !- Nominal Capacity of the Coil {W}
+      SPACE1-1 Zone Coil Air In Node,  !- Coil_Air_Inlet_Node
+      SPACE1-1 In Node;  !- Coil_Air_Outlet_Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-000}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Air Terminal VAV Damper Position {[]}
+\item
+  HVAC,Average,Zone Air Terminal Minimum Air Flow Fraction {[]}
+\item
+  HVAC,Average,Zone Air Terminal Outdoor Air Volume Flow Rate {[}m3/s{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Zone Air Terminal VAV Damper Position {[]}}{Zone Air Terminal VAV Damper Position }}\label{zone-air-terminal-vav-damper-position}
+
+This output is the variable air volume damper position required to meet the zone load. This is the average value over the frequency being reported. The damper position is defined as the terminal unit air mass flow rate divided by the terminal unit's maximum air mass flow rate.
+
+\paragraph{\texorpdfstring{Zone Air Terminal Minimum Air Flow Fraction {[]}}{Zone Air Terminal Minimum Air Flow Fraction }}\label{zone-air-terminal-minimum-air-flow-fraction}
+
+This output is the value for the minimum air flow fraction setting on a VAV terminal.~~ This is the average value over the frequency being reported.~ The minimum air flow fraction is defined as the lower limit on the terminal unit air mass flow rate divided by the terminal units maximum air mass flow rate.
+
+\paragraph{Zone Air Terminal Outdoor Air Volume Flow Rate {[}m3/s{]}}\label{zone-air-terminal-outdoor-air-volume-flow-rate-m3s}
+
+This output is the amount of outdoor air entering the zone. This is the average value over the frequency being reported.~ The amount of outdoor air is defined as the terminal unit air volume flow rate multiplied by the fraction of outdoor air entering the air loop's outside air system.
+
+\subsection{AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan}\label{airterminalsingleductvavreheatvariablespeedfan}
+
+The VAV terminal unit with variable-speed fan and reheat coil is an air system terminal unit consisting of a variable speed fan in series with a heating coil. These units are usually employed in underfloor air distribution (UFAD) systems where the air is supplied at low static pressure through an underfloor plenum. The fan is used to control the flow of conditioned air that enters the space. When the fan is off the plenum pressure drives the minimum air flow through the terminal unit. At maximum cooling the fan runs at its maximum speed. At full heating the fan runs at its heating maximum -- usually less than the cooling maximum flow rate. Thus this unit has two separate maximum flow rates -- one for heating and one for cooling.
+
+For cooling, control is maintained simply by varying the fan speed. For heating, the unit first tries to meet the heating load by varying the heating coil output while keeping the air flow at minimum (fan off). If this is not adequate the fan turns on and operates in variable flow mode up to the heating maximum flow rate.
+
+This unit is modeled in EnergyPlus as a compound component -- a variable speed fan and a heating coil in series in the air stream. The unit is blow through -- the fan is upstream of the heating coil.
+
+\subsubsection{Inputs}\label{inputs-3-000}
+
+\paragraph{Field: Name}\label{field-name-3-000}
+
+A unique user assigned name for a particular VS fan VAV reheat terminal unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-3}
+
+The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Maximum Cooling Air Flow Rate}\label{field-maximum-cooling-air-flow-rate}
+
+The maximum volumetric air flow rate through the unit in cubic meters per second when the thermostat is calling for cooling. Normally this is the same as the unit's fan maximum volumetric flow rate.
+
+\paragraph{Field: Maximum Heating Air Flow Rate}\label{field-maximum-heating-air-flow-rate}
+
+The maximum volumetric air flow rate through the unit in cubic meters per second when the thermostat is calling for heating.
+
+\paragraph{Field: Zone Minimum Air Flow Fraction}\label{field-zone-minimum-air-flow-fraction}
+
+The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. For this unit this is the flow rate when the fan is off.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-2}
+
+The name of the HVAC system node that is the air inlet node for the terminal unit. This is also the air inlet node for the unit's fan.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-2}
+
+The name of the HVAC system node that is the air outlet node of the unit. This same node will be the unit heating coil's air outlet node. This node is also a zone inlet node.
+
+\paragraph{Field: Fan Object Type}\label{field-fan-object-type}
+
+The type of fan in the terminal unit. At this time the only type of fan allowed is \emph{Fan:VariableVolume}.
+
+\paragraph{Field: Fan Name}\label{field-fan-name}
+
+The name of the particular fan object in this terminal unit.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type}
+
+The type of heating coil in the terminal unit. The valid choices are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name}
+
+The name of the heating coil object contained in this terminal unit.
+
+\paragraph{Field: Maximum Hot Water or Steam Flow Rate}\label{field-maximum-hot-water-or-steam-flow-rate-2}
+
+The maximum hot water or steam volumetric flow rate in m\(^{3}\)/s through the unit's heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. If the heating coil is not a hot water or steam coil this field should be left blank.
+
+\paragraph{Field: Minimum Hot Water or Steam Flow Rate}\label{field-minimum-hot-water-or-steam-flow-rate-2}
+
+The minimum hot water or steam volumetric flow rate in m\(^{3}\)/s through the unit's heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. If the heating coil is not a hot water or steam coil this field should be left blank.
+
+The control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. The model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+  \frac{\left| Q_{\rm{unit, out}} - Q_{\rm{zone load}} \right|}{Q_{\rm{zone load}}} \le \rm{ConvergenceTolerance}
+\end{equation}
+
+% \begin{equation}
+%   \frac{\left| Q_{\rm{PIU, out}} - Q_{\rm{zone load}} \right|}{Q_{\rm{zone load}}} \le \rm{ConvergenceTolerance}
+% \end{equation}
+
+The default is 0.001.
+
+An IDF example:
+
+\begin{lstlisting}
+AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan,
+  SPACE2-1 VAV Reheat,                  !- Name of System
+  ReheatCoilAvailSched,                 !- System Availability schedule
+  autosize,                             !- Maximum cooling air volume flow rate
+  autosize,                             !- Maximum heating air volume flow rate
+  0.05,                                 !- Zone Minimum Air Flow Fraction
+  SPACE2-1 ATU In Node,                 !- Air Inlet Node Name
+  SPACE2-1 In Node,                     !- Air Outlet Node Name
+  FAN:SIMPLE:VariableVol,               !- Fan object
+  SPACE2-1 Zone Fan,                    !- Fan name
+  COIL:Water:SimpleHeating,             Heating coil object
+  SPACE2-1 Zone Coil,                   !- Heating coil name
+  autosize,                             !- Max hot water flow
+  0.0,                                  !- Min hot water flow
+  0.001;                                !- Heating Convergence Tolerance
+
+Coil:Heating:Water,
+  SPACE2-1 Zone Coil,                   !- Coil Name
+  ReheatCoilAvailSched,                 !- Availability Schedule Name
+  autosize,                             !- UA of the Coil {W/K}
+  autosize,                             !- Max Water Flow Rate of Coil {m3/s}
+  SPACE2-1 Zone Coil Water In Node,     !- Coil_Water_Inlet_Node
+  SPACE2-1 Zone Coil Water Out Node,    !- Coil_Water_Outlet_Node
+  SPACE2-1 Zone Coil Air In Node,       !- Coil_Air_Inlet_Node
+  SPACE2-1 In Node;                     !- Coil_Air_Outlet_Node
+
+Fan:VariableVolume,
+  SPACE2-1 Zone Fan,                    !- Fan Name
+  FanAvailSched,                        !- Availability Schedule Name
+  0.7,                                  !- Fan Total Efficiency
+  125.0,                                !- Delta Pressure {Pa}
+  autosize,                             !- Max Flow Rate {m3/s}
+  0.0,                                  !- Min Flow Rate {m3/s}
+  0.9,                                  !- Motor Efficiency
+  1.0,                                  !- Motor In Airstream Fraction
+  0.00153028,                           !- FanCoefficient 1
+  0.00520806,                           !- FanCoefficient 2
+  1.1086242,                            !- FanCoefficient 3
+  -.11635563,                           !- FanCoefficient 4
+  0.000,                                !- FanCoefficient 5
+  SPACE2-1 ATU In Node,                 !- Fan_Inlet_Node
+  SPACE2-1 Zone Coil AirIn Node;        !- Fan_Outlet_Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3}
+
+HVAC,Average,Zone Air Terminal VAV Damper Position {[]}
+
+\paragraph{Zone Air Terminal VAV Damper Position}\label{zone-air-terminal-vav-damper-position-1}
+
+This output is the variable air volume flow fraction required to meet the zone load. This is the average value over the frequency being reported. The flow fraction is defined as the terminal unit air mass flow rate divided by the terminal unit's maximum air mass flow rate.
+
+\subsection{AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat}\label{airterminalsingleductvavheatandcoolreheat}
+
+Variable air volume (VAV) systems typically control the dry-bulb temperature inside a zone by varying the supply air volume instead of the supply air temperature (ref: AirTerminal:SingleDuct:VAV:NoReheat). Reheat coils may be required to avoid overcooling (ref: AirTerminal:SingleDuct:VAV:Reheat).
+
+This terminal unit is slightly different from the AirTerminal:SingleDuct:VAV:Reheat terminal unit. Both operate the same in cooling mode: the damper opens as needed to provide additional sensible cooling to the zone. The difference between the two is in heating mode.~ For the Single Duct VAV Reheat terminal unit, the air flow rate is reduced to the minimum value (max air flow rate x zone minimum air flow fraction) when zone heating is required and the reheat coil output is modulated to meet the zone heating load.~ For the AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat terminal unit, the air flow rate in heating mode is increased to meet higher zone heating loads (similar to what is done in cooling mode). If additional heat is required (beyond what the terminal unit can provide with its damper fully open), then the reheat coil is modulated as needed to meet the additional heating load.
+
+This terminal unit model was originally developed and tested for use with the changeover-bypass VAV unitary system.
+
+\begin{figure}[hbtp] % fig 104
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image267.png}
+\caption{Single Duct VAV Heat and Cool Reheat Schematic \protect \label{fig:single-duct-vav-heat-and-cool-reheat}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-4-000}
+
+\paragraph{Field: Name}\label{field-name-4-000}
+
+Unique user-defined name for this Air Distribution Unit (ADU).
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-4}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether or not this component is available to operate during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Damper Air Outlet Node Name}\label{field-damper-air-outlet-node-name-1}
+
+This alpha field defines the name of the VAV damper air outlet node. This is the outlet node of the damper and the inlet node of the reheat coil.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-3}
+
+This alpha field defines the name of the air inlet node that connects the air splitter to the individual zone ADU. This is \emph{not} the same as the air inlet node of the reheat component: it is upstream of that node. This is the inlet node to the terminal unit and the damper.
+
+\paragraph{Field: Maximum Air Flow Rate}\label{field-maximum-air-flow-rate-3}
+
+This numeric field defines the design maximum volumetric flow rate (m\(^{3}\)/sec) specified for this VAV ADU. This flow rate must be greater than 0 or can be autosized.
+
+\paragraph{Field: Zone Minimum Air Flow Fraction}\label{field-zone-minimum-air-flow-fraction-1}
+
+This numeric field defines the minimum air volumetric flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates as needed to maintain the heating set point specified in the Zone Control:Thermostatic object. This value must be between 0 and 1.
+
+\paragraph{Field: Reheat Coil Object Type}\label{field-reheat-coil-object-type-2}
+
+The valid reheat component objects currently available are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+If no reheat coil is required, use AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat instead of this object.
+
+\paragraph{Field: Reheat Coil Name}\label{field-reheat-coil-name-2}
+
+Unique coil name being simulated with this ADU. Applicable for all coils. If there is no reheat coil, use AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat instead of this object.
+
+\paragraph{Field: Maximum Hot Water or Steam Flow Rate}\label{field-maximum-hot-water-or-steam-flow-rate-3}
+
+This field is ignored for gas or electric reheat coils. If using a hot water or steam reheat coil, set to the maximum design water or steam volumetric flow rate in m\(^{3}\)/s for the hot water or steam heating coil. The steam volume flow rate is calculated at 100C and 101325 Pa. This volumetric flow rate can be autosized.
+
+\paragraph{Field: Minimum Hot Water or Steam Flow Rate}\label{field-minimum-hot-water-or-steam-flow-rate-3}
+
+This field is ignored for gas and electric coils. Set to the minimum design water or steam volumetric flow rate in m\(^{3}\)/s for the hot water or steam heating coil, normally set to be a shut-off valve that is set to zero. The steam volume flow rate is calculated at 100C and 101325 Pa.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-3}
+
+This is the air outlet node for the ADU and is then connected to the zone. This is the same node as the air outlet node of the reheat component.
+
+\paragraph{Field: Convergence Tolerance}\label{field-convergence-tolerance-2}
+
+The coil is controlled by knowing the zone demand determined by the zone thermostat and setting the outlet conditions to meet this demand. For the electric and gas coils, this is set exactly since the coil model solution can be inverted and this field is not used. With the hot water coil that uses an effectiveness-NTU method, the solution cannot be inverted directly. Therefore, to determine the correct mass flow rate for the hot water the solution is solved by iteration. The iterative solution uses an interval-halving routine and needs a termination criteria that is set with this Convergence Tolerance parameter. This control offset is set to a decimal fraction of the zone demand. The default value for this field is 0.001.
+
+\paragraph{Field: Maximum Reheat Air Temperature}\label{field-maximum-reheat-air-temperature-2}
+
+This is the upper limit on the temperature in degrees C of the air leaving the terminal unit -- reheat coil (and being delivered to the zone). If the user leaves this field blank, no maximum reheat air temperature is enforced.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat,
+      Zone 1 VAV System,             !- Name of System
+      FanAndCoilAvailSched,          !- System Availability schedule
+      Zone 1 Reheat Air Inlet Node,  !- DAMPER Air Outlet Node
+      Zone 1 VAV Inlet Node,         !- UNIT Air Inlet Node
+      0.583,                         !- Maximum air flow rate {m3/s}
+      0.25,                          !- Zone Minimum Air Flow Fraction
+      Coil:Heating:Electric,         !- Reheat Component Object
+      Reheat Coil Zone 1,            !- Name of Reheat Component
+      0.0,                           !- Max Reheat Water Flow {m3/s}
+      0.0,                           !- Min Reheat Water Flow {m3/s}
+      Zone 1 Reheat Air Outlet Node, !- UNIT Air Outlet Node
+      0.001;                         !- Convergence Tolerance
+
+  Coil:Heating:Electric,
+      Reheat Coil Zone 1,            !- Coil Name
+      FanAndCoilAvailSched,          !- Availability Schedule Name
+      1.0,                           !- Efficiency of the Coil
+      3000.0,                        !- Nominal Capacity of the Coil {W}
+      Zone 1 Reheat Air Inlet Node,  !- Coil_Air_Inlet_Node
+      Zone 1 Reheat Air Outlet Node; !- Coil_Air_Outlet_Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4}
+
+HVAC,Average,Zone Air Terminal VAV Damper Position {[]}
+
+\paragraph{\texorpdfstring{Zone Air Terminal VAV Damper Position {[]}}{Zone Air Terminal VAV Damper Position }}\label{zone-air-terminal-vav-damper-position-2}
+
+This output is the damper position required to meet the zone load. This is the average value over the simulation timestep being reported. The damper position is defined as the terminal unit air mass flow rate divided by the terminal unit's maximum air mass flow rate.
+
+\subsection{AirTerminal:SingleDuct:VAV:NoReheat}\label{airterminalsingleductvavnoreheat}
+
+Variable air volume (VAV) systems control the dry-bulb temperature inside a zone by varying the supply air volume instead of the air temperature. At full cooling the VAV damper is fully open supplying the specified maximum air flow rate. As the cooling load decreases, the damper closes until it reaches the minimum stop specified by the zone minimum air flow fraction.
+
+VAV systems can be used for interior or perimeter zones with a common fan system and air temperature control. The VAV concept may vary according to the VAV box locations and air temperature controls. Heating can be provided if necessary by use of baseboard.
+
+\subsubsection{Inputs}\label{inputs-5-000}
+
+\paragraph{Field: Name}\label{field-name-5-000}
+
+Unique name for the VAV Air Distribution Unit (ADU).
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-5}
+
+Schedule that this component will operate or is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-4}
+
+The VAV damper and Unit outlet node.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-4}
+
+The air inlet node name that connects the air splitter to the individual zone ADU.
+
+\paragraph{Field: Maximum Air Flow Rate}\label{field-maximum-air-flow-rate-4}
+
+The design maximum volume flow rate (m\(^{3}\)/sec) specified for VAV ADU. This is autosizable.
+
+\paragraph{Field: Zone Minimum Air Flow Method}\label{field-zone-minimum-air-flow-method-1}
+
+This field is used to select how the program will determine the minimum flow rate to the zone while the system is operating.~ The minimum flow rate is modeled as a fraction of the maximum flow rate.~ There are five choices:~ Constant, FixedFlowRate, Scheduled, Sum and Maximum.~ If Constant is entered, then the program will use the value for minimum flow fraction entered in the following field.~ If FixedFlowRate is entered, then the program will use the value for minimum flow rate entered in the field below called Fixed Minimum Air Flow Rate.If Scheduled is entered, then the program will obtain the value for minimum flow fraction from the schedule named in the field below called Minimum Air Flow Fraction Schedule Name. Sum and Maximum are used to either provide the summation of all ``entered'' inputs or the maximum of all ``entered'' inputs.
+
+\paragraph{Field: Constant Minimum Air Flow Fraction}\label{field-constant-minimum-air-flow-fraction-1}
+
+The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. This field is only used if the Zone Minimum Air Flow Method field is set to Constant.
+
+\paragraph{Field: Fixed Minimum Air Flow Rate}\label{field-fixed-minimum-air-flow-rate-1}
+
+The minimum flow rate to the zone while the system is operating, specified as a fixed minimum air flow rate in meters cubed per second. The minimum air flow rate is normally specified to meet the minimum ventilation requirement for the occupants. This field is only used if the Zone Minimum Air Flow Method field is set to FixedFlowRate.
+
+\paragraph{Field: Minimum Air Flow Fraction Schedule Name}\label{field-minimum-air-flow-fraction-schedule-name-1}
+
+The name of a schedule that determines the value of the minimum air flow fraction.~ The schedule should contain fractions from 0.0 to 1.0.~ These values will define the minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. This field is only used if the Zone Minimum Air Flow Method field is set to Scheduled.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-1}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object. When this field is used, the terminal unit will increase flow as needed to meet this outdoor air requirement. If Outdoor Air Flow per Person is non-zero, then the outdoor air requirement will be computed based on the current number of occupants in the zone. At no time will the supply air flow rate exceed the value for Maximum Air Flow Rate. If this field is blank, then the terminal unit will not be controlled for outdoor air flow. See documentation for the zone HVAC outdoor air object for further information (Ref DesignSpecification:OutdoorAir).
+
+An IDF example:
+
+\begin{lstlisting}
+
+  AirTerminal:SingleDuct:VAV:NoReheat,
+      Zone 1 VAV System,       !- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      Zone 1 Reheat Air Outlet Node,  !- Air Outlet Node Name
+      Zone 1 Damper Inlet Node,!- Air Inlet Node Name
+      0.47,                    !- Maximum Air Flow Rate {m3/s}
+      Constant,                !- Zone Minimum Air Flow Input Method
+      0.3,                     !- Constant Minimum Air Flow Fraction
+      ,                        !- Fixed Minimum Air Flow Rate
+      ,                        !- Minimum Air Flow Fraction Schedule Name
+      ZoneOAData;              !- Design Specification Outdoor Air Object Name
+
+    DesignSpecification:OutdoorAir,
+      ZoneOAData,            !- Name
+      Sum,                   !- Outdoor Air Method
+      0.00236,               !- Outdoor Air Flow per Person {m3/s}
+      0.00305,               !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
+      ,                      !- Outdoor Air Flow per Zone {m3/s}
+      ,                      !- Outdoor Air Flow Air Changes per Hour
+      OARequirements Sched;  !- Outdoor Air Flow Rate Fraction Schedule Name
+
+  Schedule:Compact,
+      OARequirements Sched,    !- Name
+      Any Number,              !- Schedule Type Limits Name
+      Through: 12/31,          !- Field 1
+      For: Weekdays SummerDesignDay WinterDesignDay,  !- Field 2
+      Until: 24:00, 1.0,       !- Field 4
+      For: AllOtherDays,       !- Field 5
+      Until: 24:00, 0.5;       !- Field 7
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Air Terminal VAV Damper Position {[]}
+\item
+  HVAC,Average,Zone Air Terminal Outdoor Air Volume Flow Rate {[}m3/s{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Zone Air Terminal VAV Damper Position {[]}}{Zone Air Terminal VAV Damper Position }}\label{zone-air-terminal-vav-damper-position-3}
+
+This output is the damper position required to meet the zone load. This is the average value over the simulation timestep being reported. The damper position is defined as the terminal unit air mass flow rate divided by the terminal unit's maximum air mass flow rate.
+
+\paragraph{Zone Air Terminal Outdoor Air Volume Flow Rate {[}m3/s{]}}\label{zone-air-terminal-outdoor-air-volume-flow-rate-m3s-1}
+
+This output is the amount of outdoor air entering the zone. This is the average value over the frequency being reported.~ The amount of outdoor air is defined as the terminal unit air volume flow rate multiplied by the fraction of outdoor air entering the air loop's outside air system.
+
+\subsection{AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat}\label{airterminalsingleductvavheatandcoolnoreheat}
+
+Variable air volume (VAV) systems typically control the dry-bulb temperature inside a zone by varying the supply air volume instead of the supply air temperature (ref: AirTerminal:SingleDuct:VAV:NoReheat). Reheat coils may be required to avoid overcooling (ref: AirTerminal:SingleDuct:VAV:Reheat).
+
+This terminal unit is slightly different from the AirTerminal:SingleDuct:VAV:NoReheat terminal unit. Both operate the same in cooling mode: the damper opens as needed to provide additional sensible cooling to the zone. The difference between the two is in heating mode. For the Single Duct VAV NoReheat terminal unit, the air flow rate is reduced to the minimum value (max air flow rate x zone minimum air flow fraction) when zone heating is required. For the AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat terminal unit, the air flow rate in heating mode is increased to meet higher zone heating loads (similar to what is done in cooling mode).
+
+This terminal unit model was originally developed and tested for use with the changeover-bypass VAV unitary system..This object may be used when the central heating coil is sufficient to maintain the heating set point temperature. Additional heating may be provided, if necessary, by use of AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat or ZoneHVAC:Baseboard:* objects.
+
+\begin{figure}[hbtp] % fig 105
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image268.png}
+\caption{Single Duct VAV Heat and Cool NoReheat Schematic \protect \label{fig:single-duct-vav-heat-and-cool-noreheat}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-6-000}
+
+\paragraph{Field: Name}\label{field-name-6-000}
+
+Unique user-defined name for this Air Distribution Unit (ADU).
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-6}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether or not this component is available to operate during a given time period. If a schedule value is greater than zero then the system is available to operate; otherwise, the system is unavailable for that time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-5}
+
+This alpha field defines the name of the VAV damper air outlet node.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-5}
+
+This alpha field defines the name of the air inlet node that connects the air splitter to the individual zone ADU.
+
+\paragraph{Field: Maximum Air Flow Rate}\label{field-maximum-air-flow-rate-5}
+
+This numeric field defines the design maximum volume flow rate (m\(^{3}\)/sec) specified for this VAV ADU. This flow rate must be greater than 0 or can be autosized.
+
+\paragraph{Field: Zone Minimum Air Flow Fraction}\label{field-zone-minimum-air-flow-fraction-2}
+
+This numeric field defines the minimum air volume flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. This value must be between 0 and 1.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat,
+      Zone 3 VAV System,       !- Name of System
+      FanAndCoilAvailSched,    !- System Availability schedule
+      Zone 3 Reheat Air Outlet Node,  !- UNIT Air Outlet Node
+      Zone 3 VAV Inlet Node,   !- UNIT Air Inlet Node
+      0.584,                   !- Maximum air flow rate {m3/s}
+      0.25;                    !- Zone Minimum Air Flow Fraction
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6}
+
+HVAC,Average,Zone Air Terminal VAV Damper Position {[]}
+
+\paragraph{\texorpdfstring{Zone Air Terminal VAV Damper Position {[]}}{Zone Air Terminal VAV Damper Position }}\label{zone-air-terminal-vav-damper-position-4}
+
+This output is the damper position required to meet the zone load. This is the average value over the simulation timestep being reported. The damper position is defined as the terminal unit air mass flow rate divided by the terminal unit's maximum air mass flow rate.
+
+\subsection{AirTerminal:SingleDuct:SeriesPIU:Reheat}\label{airterminalsingleductseriespiureheat}
+
+The series powered induction unit is an air system terminal unit that mixes varying amounts of secondary (recirculated) air and primary (conditioned supply) air to produce a fixed flow of air to a zone. The unit contains a small fan that acts to induce the secondary air and a heating coil for heating the mixed secondary and primary air. The fan runs at a constant volume flow rate whenever the unit is on (and the fan's availability schedule is on or it is activated by an availability manager). The fan is downstream of the primary and secondary air inlets. The variable mixing is accomplished by a damper in the unit's primary air supply inlet duct. This damper can move from fully open (100\% primary air. 0\% secondary air) to a minimum stop that is specified in the input description. At full cooling the damper will be fully open. At minimum cooling and for heating the damper will be at the minimum stop and the secondary air flow will be at its maximum.
+
+The EnergyPlus model of the series PIU terminal unit is composed of three components: a zone mixer, a constant volume fan, and a heating coil (hot water, electric, or gas).
+
+\begin{figure}[hbtp] % fig 106
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image269.png}
+\caption{Series PIU Terminal Unit \protect \label{fig:series-piu-terminal-unit}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-7-000}
+
+\paragraph{Field: Name}\label{field-name-7-000}
+
+A unique user assigned name for a particular series powered induction terminal unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-7}
+
+The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Maximum Air Flow Rate}\label{field-maximum-air-flow-rate-6}
+
+The maximum volumetric air flow rate through the unit in cubic meters per second. Since this is a constant air volume unit, this is also the design, rated air flow rate of the unit.
+
+\paragraph{Field: Maximum Primary Air Flow Rate}\label{field-maximum-primary-air-flow-rate}
+
+The maximum volumetric air flow rate of primary air through the unit in cubic meters per second. This is the primary air flow rate at full cooling load when the primary air damper is fully open. Usually this quantity is the same as the total unit flow rate, but it can be less.
+
+\paragraph{Field: Minimum Primary Air Flow Fraction}\label{field-minimum-primary-air-flow-fraction}
+
+The minimum volumetric air flow rate of primary air through the unit expressed as a fraction of the maximum volumetric air flow rate of primary air. This input can be 0.0.
+
+\paragraph{Field: Supply Air Inlet Node Name}\label{field-supply-air-inlet-node-name}
+
+The name of the HVAC system node from which the unit draws its primary or supply air
+
+\paragraph{Field: Secondary Air Inlet Node Name}\label{field-secondary-air-inlet-node-name}
+
+The name of the HVAC system node from which the unit draws its secondary or recirculated air. The unit can draw secondary air from its conditioned zone directly or from a return air plenum. Thus this node should be one of the zones exhaust air nodes (see \emph{Zone Air Exhaust Node} in \textbf{ZoneHVAC:EquipmentConnections}) or an induced air node outlet of a return plenum (see \emph{Induced Air Outlet Node} in \textbf{AirLoopHVAC:ReturnPlenum}).
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name}
+
+The name of the HVAC system node to which the unit sends its outlet air. This should be one of the inlet air nodes of the zone which is being served.
+
+\paragraph{Field: Reheat Coil Air Inlet Node Name}\label{field-reheat-coil-air-inlet-node-name}
+
+The name of the HVAC system node which is the inlet node of the unit's heating coil. This is also the outlet node of the unit's fan.
+
+\paragraph{Field: Zone Mixer Name}\label{field-zone-mixer-name}
+
+The name of an zone mixer component (object: AirLoopHVAC:ZoneMixer) which composes part of the unit. Note that some of the input for the mixer will duplicate input fields of the powered induction unit. One of the zone mixer inlet nodes should be the same as the supply air inlet node of the PIU; the other inlet node of the zone mixer should be the same as the secondary air inlet node of the PIU. The outlet node of the zone mixer should be the same as the inlet node of the PIU fan.
+
+\paragraph{Field: Fan Name}\label{field-fan-name-1}
+
+The name of a fan component which composes part of the unit. Note that the fan's maximum flow rate should be the same as the maximum air flow rate of the PIU and the type of fan object must be Fan:ConstantVolume. The fan's inlet node should be the same as the zone mixer's outlet node. The fan's outlet node should be the same as the heating coil's air inlet node. The secondary fan will run according to the Availability Schedule specified in the Fan:ConstantVolume object, unless it is overridden by an availability manager (ref. AvailabilityManager:NightCycle and others).
+
+\paragraph{Field: Reheat Coil Object Type}\label{field-reheat-coil-object-type-3}
+
+The type of coil in the PIU. The valid choices are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+In other words the PIU may have a hot water, gas, electric or steam reheat coil.
+
+\paragraph{Field: Reheat Coil Name}\label{field-reheat-coil-name-3}
+
+The name of the heating coil component which composes part of the unit. Note that the heating coil's air inlet node is the same as the fan outlet node and the heating coil's air outlet node is the same as the PIU outlet node.
+
+\paragraph{Field: Maximum Hot Water or Steam Flow Rate}\label{field-maximum-hot-water-or-steam-flow-rate-4}
+
+The maximum hot water volumetric flow rate in m\(^{3}\)/sec through the unit's heating coil. If the heating coil is gas or electric this field should be blank.
+
+\paragraph{Field: Minimum Hot Water or Steam Flow Rate}\label{field-minimum-hot-water-or-steam-flow-rate-4}
+
+The minimum hot water volumetric flow rate in m\(^{3}\)/sec through the unit's heating coil. If the heating coil is gas or electric this field should be blank.
+
+\paragraph{Field: Convergence Tolerance}\label{field-convergence-tolerance-3}
+
+The control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {{Q_{PIU,out}} - {Q_{zone\;load}}} \right|}}{{{Q_{zone\;load}}}} \le ConvergenceTolerance
+\end{equation}
+
+For gas or electric heating coils, this input should be left blank. The default is 0.001.
+
+An IDF example:
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:SeriesPIU:Reheat,
+            Zone 1 SPIU ATU,          ! Name of air terminal unit
+            FanAndCoilAvailSched,     ! Availability schedule for series PIU ATU
+            0.47,                     ! Total volume flow rate through ATU
+            0.47,                     ! Maximum primary air flow rate through terminal unit
+            0.3,                      ! Minimum primary air flow rate (fraction of max)
+            Zone 1 PIU Pri Air Inlet Node,   ! Air Terminal unit supply air inlet node
+            Zone 1 PIU Sec Air Inlet Node,   ! Air Terminal unit secondary air inlet node
+            Zone 1 PIU Air Outlet Node,      ! Air Terminal unit outlet node
+            Zone 1 Reheat Air Inlet Node,    ! Reheat coil air inlet node (fan outlet node)
+            Zone 1 PIU Mixer,                ! Air terminal unit mixer name
+            Zone 1 PIU Fan,                  ! Air terminal unit fan name
+            COIL:Heating:Water,              ! type of air terminal unit reheat coil
+            Reheat Coil Zone 1,              ! name of air terminal unit reheat coil
+            0.0013,                          ! Max Reheat Water Flow {Flow: m3/sec}
+            0.0,                             ! Min Reheat Water Flow {Flow: m3/sec}
+           0.001;                           ! Convergence tolerance
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Air Terminal Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Air Terminal Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Air Terminal Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Air Terminal Sensible Cooling Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Zone Air Terminal Heating Rate {[}W{]}}\label{zone-air-terminal-heating-rate-w}
+
+This field reports the dry air heating addition rate of the series PIU terminal unit to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the terminal unit.
+
+\paragraph{Zone Air Terminal Heating Energy {[}J{]}}\label{zone-air-terminal-heating-energy-j}
+
+This field reports the dry air heat addition of the series PIU terminal unit~ to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the terminal unit, and the timestep.
+
+\paragraph{Zone Air Terminal Sensible Cooling Rate {[}W{]}}\label{zone-air-terminal-sensible-cooling-rate-w-1}
+
+This field reports the dry air sensible heat extraction rate of the series PIU terminal unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the terminal unit.
+
+\paragraph{Zone Air Terminal Sensible Cooling Energy {[}J{]}}\label{zone-air-terminal-sensible-cooling-energy-j-1}
+
+This field reports the dry air sensible heat extraction of the series PIU terminal unit from the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the terminal unit, and the timestep.
+
+\subsection{AirTerminal:SingleDuct:ParallelPIU:Reheat}\label{airterminalsingleductparallelpiureheat}
+
+The parallel powered induction unit is an air system terminal unit that mixes varying amounts of secondary (recirculated) air and primary (conditioned supply) air to produce a variable total flow of air to a zone. The unit contains a small fan that acts to induce the secondary air and a heating coil for heating the mixed secondary and primary air. The secondary and primary air streams enter the unit in parallel. The fan sits in the secondary air stream and runs only when the primary air flow is below the Fan On Flow Fraction and the fan's availability schedule is on or it is activated by an availability manager. The primary air inlet contains a damper that can move from fully open (maximum primary air) to a minimum stop (minimum primary air).
+
+At full cooling load the primary air damper is fully open and the fan is off. The primary air flow is at maximum and there is little or no secondary air flow. As the cooling load decreases, the primary air damper gradually closes and the secondary air flow remains close to zero. At some point, usually when the primary air flow has reached the minimum, the fan switches on and secondary air is induced. The heating coil will switch on as needed to meet any heating demand.
+
+The EnergyPlus model of the parallel PIU terminal unit is composed of three components: a constant volume fan, a zone mixer, and a heating coil (hot water, electric, or gas).
+
+\begin{figure}[hbtp] % fig 107
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image271.png}
+\caption{Parallel PIU Terminal Unit \protect \label{fig:parallel-piu-terminal-unit}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-8-000}
+
+\paragraph{Field: Name}\label{field-name-8-000}
+
+A unique user assigned name for a particular~ parallel powered induction terminal unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-8}
+
+The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Maximum Primary Air Flow Rate}\label{field-maximum-primary-air-flow-rate-1}
+
+The maximum volumetric air flow rate of primary air through the unit in cubic meters per second. This is the primary air flow rate at full cooling load when the primary air damper is fully open.
+
+\paragraph{Field: Maximum Secondary Air Flow Rate}\label{field-maximum-secondary-air-flow-rate}
+
+The maximum volumetric air flow rate of secondary air through the unit in cubic meters per second. This flow rate can be any amount but is commonly less than the maximum primary air flow rate.
+
+\paragraph{Field: Minimum Primary Air Flow Fraction}\label{field-minimum-primary-air-flow-fraction-1}
+
+The minimum volumetric air flow rate of primary air through the unit expressed as a fraction of the maximum volumetric air flow rate of primary air. This input can be 0.0.
+
+\paragraph{Field: Fan On Flow Fraction}\label{field-fan-on-flow-fraction}
+
+The fraction of the primary air flow at which fan turns on. In the parallel PIU the fan operation is intermittent. If the primary air flow is above this fraction of the maximum, the fan is off. Otherwise the secondary fan will run according to the Availability Schedule specified in the Fan:ConstantVolume object (see Fan Name below), unless it is overridden by an availability manager (ref. AvailabilityManager:NightCycle and others).
+
+\paragraph{Field: Supply Air Inlet Node Name}\label{field-supply-air-inlet-node-name-1}
+
+The name of the HVAC system node from which the unit draws its primary or supply air
+
+\paragraph{Field: Secondary Air Inlet Node Name}\label{field-secondary-air-inlet-node-name-1}
+
+The name of the HVAC system node from which the unit draws its secondary or recirculated air. The unit can draw secondary air from its conditioned zone directly or from a return air plenum. Thus this node should be one of the zones exhaust air nodes (see \emph{Zone Air Exhaust Node} in \textbf{ZoneHVAC:EquipmentConnections}) or an induced air node outlet of a return plenum (see \emph{Induced Air Outlet Node} in \textbf{AirLoopHVAC:ReturnPlenum}).
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-1}
+
+The name of the HVAC system node to which the unit sends its outlet air. This should be one of the inlet air nodes of the zone which is being served.
+
+\paragraph{Field: Reheat Coil Air Inlet Node Name}\label{field-reheat-coil-air-inlet-node-name-1}
+
+The name of the HVAC system node which is the inlet node of the unit's heating coil. This is also the outlet node of the unit's zone mixer.
+
+\paragraph{Field: Zone Mixer Name}\label{field-zone-mixer-name-1}
+
+The name of an zone mixer component (object: AirLoopHVAC:ZoneMixer) which composes part of the unit. Note that some of the input for the mixer will duplicate input fields of the powered induction unit. One of the zone mixer inlet nodes should be the same as the supply air inlet node of the PIU; the other inlet node of the zone mixer should be the same as the air outlet node of the fan. The outlet node of the zone mixer should be the same as the inlet node of the heating coil.
+
+\paragraph{Field: Fan Name}\label{field-fan-name-2}
+
+The name of a fan component which composes part of the unit. Note that the fan's maximum flow rate should be the same as the maximum secondary air flow rate of the PIU and the type of fan object must be Fan:ConstantVolume. The fan's inlet node should be the same as the PIU secondary air inlet node. The fan's outlet node should be the same as one of the zone mixer's inlet nodes. When the primary air flow is below the Fan On Flow Fraction (above), the secondary fan will run according to the Availability Schedule specified in the Fan:ConstantVolume object, unless it is overridden by an availability manager (ref. AvailabilityManager:NightCycle and others).
+
+\paragraph{Field: Reheat Coil Object Type}\label{field-reheat-coil-object-type-4}
+
+The type of coil in the PIU. The valid choices are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+In other words the PIU may have a hot water, gas, electric or steam reheat coil.
+
+\paragraph{Field: Reheat Coil Name}\label{field-reheat-coil-name-4}
+
+The name of the heating coil component which composes part of the unit. Note that the heating coil's air inlet node is the same as the zone mixer's outlet node and the heating coil's air outlet node is the same as the PIU outlet node.
+
+\paragraph{Field: Maximum Hot Water or Steam Flow Rate}\label{field-maximum-hot-water-or-steam-flow-rate-5}
+
+The maximum hot water or steam volumetric flow rate in m\(^{3}\)/s through the unit's heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. If the heating coil is gas or electric this field should be blank.
+
+\paragraph{Field: Minimum Hot Water or Steam Flow Rate}\label{field-minimum-hot-water-or-steam-flow-rate-5}
+
+The minimum hot water or steam volumetric flow rate in m\(^{3}\)/s through the unit's heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. If the heating coil is gas or electric this field should be blank.
+
+\paragraph{Field: Convergence Tolerance}\label{field-convergence-tolerance-4}
+
+The control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {{Q_{PIU,out}} - {Q_{zone\;load}}} \right|}}{{{Q_{zone\;load}}}} \le ConvergenceTolerance
+\end{equation}
+
+For gas or electric heating coils, this input should be left blank. The default is 0.001.
+
+An IDF example:
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:ParallelPIU:Reheat,
+            Zone 3 PPIU ATU,          ! Name of air terminal unit
+            FanAndCoilAvailSched,     ! Availability schedule for series PIU ATU
+            0.47,                     ! Maximum primary air flow rate through terminal unit
+            0.375,                    ! Maximum secondary air flow rate through the terminal unit
+            0.1,                      ! Minimum primary air flow rate (fraction of max)
+            0.1,                      ! fan on flow fraction
+            Zone 3 PIU Pri Air Inlet Node,   ! Air Terminal unit supply air inlet node
+            Zone 3 PIU Sec Air Inlet Node,   ! Air Terminal unit secondary air inlet node
+            Zone 3 PIU Air Outlet Node,      ! Air Terminal unit outlet node
+            Zone 3 Reheat Air Inlet Node,    ! Reheat coil air inlet node (fan outlet node)
+            Zone 3 PIU Mixer,                ! Air terminal unit mixer name
+            Zone 3 PIU Fan,                  ! Air terminal unit fan name
+            Coil:Heating:Water,              ! type of air terminal unit reheat coil
+            Reheat Coil Zone 3,              ! name of air terminal unit reheat coil
+            0.0013,                          ! Max Reheat Water Flow {Flow: m3/sec}
+            0.0,                             ! Min Reheat Water Flow {Flow: m3/sec}
+            0.001;                           ! Convergence tolerance
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Air Terminal Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Air Terminal Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Air Terminal Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Zone Air Terminal Sensible Cooling Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Zone Air Terminal Heating Rate {[}W{]}}\label{zone-air-terminal-heating-rate-w-1}
+
+This field reports the dry air heating addition rate of the parallel PIU terminal unit to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the terminal unit.
+
+\paragraph{Zone Air Terminal Heating Energy {[}J{]}}\label{zone-air-terminal-heating-energy-j-1}
+
+This field reports the dry air heat addition of the parallel PIU terminal unit~ to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the terminal unit, and the timestep.
+
+\paragraph{Zone Air Terminal Sensible Cooling Rate {[}W{]}}\label{zone-air-terminal-sensible-cooling-rate-w-2}
+
+This field reports the sensible heat extraction rate of the parallel PIU terminal unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the terminal unit.
+
+\paragraph{Zone Air Terminal Sensible Cooling Energy {[}J{]}}\label{zone-air-terminal-sensible-cooling-energy-j-2}
+
+This field reports the dry air sensible heat extraction of the parallel PIU terminal unit from the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the terminal unit, and the timestep.
+
+\subsection{AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction}\label{airterminalsingleductconstantvolumefourpipeinduction}
+
+The four pipe induction terminal unit provides local hot water heating or chilled water cooling of induced zone air which then mixes with centrally conditioned supply air. An air conditioning system consisting of these terminal units is effectively a mixed cental air / local hydronic system. The centrally conditioned air supplied to the induction terminal units is constant volume at quite high pressure. The central air is discharged through a nozzle in the terminal unit, inducing a flow of room air over a hydronic heating/cooling coil. The coil is connected either to a single inlet and outlet pipe (2 pipe unit) or to 2 inlets and 2 outlets (4 pipe unit). The heated or cooled induced air mixes with the centrally conditioned air before being discharged into the zone. The terminal units are usually expected to do only sensible cooling -- any dehumidification is done by the central air conditioning system.
+
+The EnergyPlus model of the four pipe induction terminal unit is a compound component consisting of a hot water heating coil, a chilled water cooling coil, and an air mixer. The unit has two inlet air streams: the centrally conditioned supply air and the induced air from the zone. The induced air passes first through the heating coil, then through the cooling coil and finally through the mixer. The central supply air goes directly into the mixer. The water flow through the hot or cold water coil is varied to meet the zone air conditioning requirement. Note that EnergyPlus models the four pipe induction terminal unit as having separate heating and cooling coils whereas real units have only a single coil used for both heating and cooling. Note also that the four pipe induction unit model can be used to model a two pipe unit by simply adjusting the heating and cooling coil schedules so that the heating coil is off when the cooling coil is on and vice versa.
+
+\subsubsection{Inputs}\label{inputs-9-000}
+
+\paragraph{Field: Name}\label{field-name-9-000}
+
+A unique user assigned name for a particular~ four pipe induction terminal unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-9}
+
+The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Maximum Total Air Flow Rate}\label{field-maximum-total-air-flow-rate}
+
+The maximum volumetric air flow rate discharged from the unit in cubic meters per second. Since this is a constant air volume unit, this is also the design, rated air flow rate of the unit. Note that this is the total discharge flow rate -- including both central supply and induced air.
+
+\paragraph{Field: Induction Ratio}\label{field-induction-ratio}
+
+The ratio of induced air flow rate to primary supply air flow rate. The default is 2.5 the supply air induces zone air flow at 2.5 times the primary supply air flow rate.
+
+\paragraph{Field: Supply Air Inlet Node Name}\label{field-supply-air-inlet-node-name-2}
+
+The name of the HVAC system node from which the unit draws its primary or supply air
+
+\paragraph{Field: Induced Air Inlet Node Name}\label{field-induced-air-inlet-node-name}
+
+The name of the HVAC system node from which the unit draws its secondary or recirculated air. This should be the same node as one of the zone exhaust nodes.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-6}
+
+The name of the HVAC system node to which the unit sends its outlet air. This should be one of the inlet air nodes of the zone which is being served.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-1}
+
+The type of heating coil in the terminal unit. The choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  Coil:Heating:Water
+\end{itemize}
+
+In other words the unit may have a hot water coil only.
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-1}
+
+The name of the heating coil component which composes part of the unit. Note that the heating coil's air inlet node is the same as the terminal unit's induced air inlet node. The heating coil's air outlet node is the same as the cooling coil's air inlet node.
+
+\paragraph{Field: Maximum Hot Water Flow Rate}\label{field-maximum-hot-water-flow-rate}
+
+The maximum hot water volumetric flow rate in m\(^{3}\)/sec through the unit's heating coil.
+
+\paragraph{Field: Minimum Hot Water Flow Rate}\label{field-minimum-hot-water-flow-rate}
+
+The minimum hot water volumetric flow rate in m\(^{3}\)/sec through the unit's heating coil.
+
+\paragraph{Field: Heating Convergence Tolerance}\label{field-heating-convergence-tolerance}
+
+The control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. The model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {{Q_{unit,out}} - {Q_{zone\;load}}} \right|}}{{{Q_{zone\;load}}}} \le ConvergenceTolerance
+\end{equation}
+
+The default is 0.001.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type}
+
+The type of cooling coil in the terminal unit. The choices are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:Water
+\item
+  Coil:Cooling:Water:DetailedGeometry
+\end{itemize}
+
+In other words the unit must use only the water cooling coils.
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name}
+
+The name of the cooling coil component which composes part of the unit. Note that the cooling coil's air inlet node is the same as the heating coil's air outlet node. The cooling coil's air outlet node is the same as one of the zone mixer's inlets.
+
+\paragraph{Field: Maximum Cold Water Flow Rate}\label{field-maximum-cold-water-flow-rate}
+
+The maximum cold water volumetric flow rate in m\(^{3}\)/sec through the unit's cooling coil.
+
+\paragraph{Field: Minimum Cold Water Flow Rate}\label{field-minimum-cold-water-flow-rate}
+
+The minimum cold water volumetric flow rate in m\(^{3}\)/sec through the unit's cooling coil.
+
+\paragraph{Field: Cooling Convergence Tolerance}\label{field-cooling-convergence-tolerance}
+
+The control tolerance for the unit cooling output. The unit is controlled by matching the unit output to the zone demand. The model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {{Q_{unit,out}} - {Q_{zone\;load}}} \right|}}{{{Q_{zone\;load}}}} \le ConvergenceTolerance
+\end{equation}
+
+The default is 0.001.
+
+\paragraph{Field: Zone Mixer Name}\label{field-zone-mixer-name-2}
+
+The name of an zone mixer component (object: AirLoopHVAC:ZoneMixer) which composes part of the terminal unit. Note that some of the zone mixer's inputs will duplicate some of the terminal units's inputs. One of the zone mixer inlet nodes should be the same as the supply air inlet node of the terminal unit; the other inlet node of the zone mixer should be the same as the cooling coil air outlet node. The outlet node of the zone mixer should be the same as the outlet node of the terminal unit.
+
+An IDF example:
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction,
+      SPACE2-1 FPIU,            !- Name of System
+      ReheatCoilAvailSched,     !- System Availability schedule
+      autosize,                 !- Maximum total air volume flow rate
+      1.0,                      !- Induction ratio
+      SPACE2-1 ATU Supply Node, !- Terminal unit supply air inlet node
+      SPACE2-1 ATU Induc Node,  !- Terminal unit induced air inlet node
+      SPACE2-1 In Node,         !- Terminal unit air outlet node
+      COIL:Heating:Water,       !- Heating coil object
+      SPACE2-1 HW Coil,         !- Heating coil name
+      autosize,                 !- Max hot water flow
+      0.0,                      !- Min hot water flow
+      0.001,                    !- Heating Convergence Tolerance
+      COIL:Cooling:Water,       !- Cooling coil object
+      SPACE2-1 CW Coil,         !- Cooling coil name
+      autosize,                 !- Max cold water flow
+      0.0,                      !- Min cold water flow
+      0.001,                    !- Cooling Convergence Tolerance
+      SPACE2-1 ATU Mixer;       !- Zone mixer component name
+
+  COIL:Heating:Water,
+      SPACE2-1 HW Coil,        !- Coil Name
+      ReheatCoilAvailSched,    !- Availability Schedule Name
+      autosize,                !- UA of the Coil {W/K}
+      autosize,                !- Max Water Flow Rate of Coil {m3/s}
+      SPACE2-1 HW Coil Water In Node,  !- Coil_Water_Inlet_Node
+      SPACE2-1 HW Coil Water Out Node, !- Coil_Water_Outlet_Node
+      SPACE2-1 ATU Induc Node, !- Coil_Air_Inlet_Node
+      SPACE2-1 HW Coil Air Out Node;   !- Coil_Air_Outlet_Node
+
+  COIL:Cooling:Water,
+      SPACE2-1 CW Coil,        !- Coil Name
+      CWCoilAvailSched,        !- Availability Schedule
+      autosize,                !- UA of the Coil
+      autosize,                !- Max Water Flow Rate of Coil
+      ,                        !- Leaving Relative Humidity of Coil
+      SPACE2-1 CW Coil Water In Node,  !- Coil_Water_Inlet_Node
+      SPACE2-1 CW Coil Water Out Node, !- Coil_Water_Outlet_Node
+      SPACE2-1 HW Coil Air Out Node,   !- Coil_Air_Inlet_Node
+      SPACE2-1 CW Coil Air Out Node;   !- Coil_Air_Outlet_Node
+
+  AirLoopHVAC:ZoneMixer,
+      SPACE2-1 ATU Mixer,              !- Mixer Name
+      SPACE2-1 In Node,                !- Outlet_Node
+      SPACE2-1 ATU Supply Node,        !- Inlet_Node_1
+      SPACE2-1 CW Coil Air Out Node;   !- Inlet_Node_2
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-9}
+
+There are no specific outputs for the four pipe induction terminal units.
+
+\subsection{AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam}\label{airterminalsingleductconstantvolumefourpipebeam}
+
+The four-pipe beam air terminal system is a mixed air-hydronic system. A central, single-duct forced-air system that supplies conditioned air to the zones. Chilled water circulates through ceiling-mounted fin-tube convector units to provide sensible cooling. Hot water circulates through the same convectors to provide heating. Water flow rate through the beam unit is varied to meet the zone sensible cooling or heating load. Any dehumidification is done by the central forced-air system. Thermodynamically, the cooled beam system resembles the four-pipe induction unit (\textbf{AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction}).
+
+To model a typical four-pipe beam system the user will need to define a conventional central constant volume forced air system in order to deliver primary air to the beam. This central system (usually) provides outside air for ventilation. Primary air is normally delivered at a fixed temperature but could be reset by a schedule or using an outdoor air reset setpoint manager. On the supply side of this air loop there will be the usual central conditioning equipment: outside air mixer, fan, heating and cooling coil. On the zone equipment (demand) side of the loop, the four-pipe beams will be represented as air terminal units. Because the four-pipe beam can provide heating the system can avoid over-cooling zones during times of low load with cool primary air temperatures, similar to the action of a reheat coil in a VAV terminal. Therefore it is not necessary to have additional zone equipment (such as baseboard heaters) to handle heating (or reheating) loads.
+
+Although the four-pipe beam equipment in a zone is treated by the program as a single terminal unit, the actual installation will often have multiple beam units in each zone. In this model, it is only the total length of all the beams and the total air flow of all the units that are described, not the number of individual beam units.
+
+If needed, the program (in its sizing calculation for the system) determines the total length of beams and primary supply air flow that is needed to meet the zone design loads. The four pipe beam air terminal sizing differs from other air terminals in that the primary supply air flow rate is sized using the entire performance model and the flow rate is not the direct result from the Sizing:Zone and Sizing:System calculations. The flow rates will be somewhere between what an air terminal would size out using \emph{VentilationRequirement} or \emph{Sensible} in the Sizing:System object (either setting can be used).
+
+The model includes two different types of inputs for flow rates, ``design'' and ``rated \ldots{} per-meter.'' The design values are the actual sizes of the flow rates as viewed from the zone and central air handler (but before zone multipliers). The design values include all the individual beam units and their lengths. The rated per-meter values are used to characterize product performance at nominal rating conditions in such a way that it can be scaled to match the size of a zone. The performance characteristics at the rating point are not fixed in the program and can be entered by the user when they differ from default values. The rated per meter values are normalized by the linear dimensions of the beam and are generally obtained from product catalog data by dividing by the length of the beam. The rated primary air flow rate is assumed to be for sea level conditions while the design primary air flow rate is modeled for the location elevation above sea level.
+
+\subsubsection{Inputs}\label{inputs-10-000}
+
+\paragraph{Field: Name}\label{field-name-10-000}
+
+A unique user-assigned name for a particular beam unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Primary Air Availability Schedule Name}\label{field-primary-air-availability-schedule-name}
+
+The name of the schedule that denotes whether the terminal unit is operating to provide primary air during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit is on and requesting primary air flow during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Cooling Availability Schedule Name}\label{field-cooling-availability-schedule-name}
+
+The name of the schedule that denotes whether the terminal unit is operating to provide cooling during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit is on and available for beam cooling during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods. The primary air availability schedule named in the previous input field must have a value that is ``on'' during times that cooling is available.
+
+\paragraph{Field: Heating Availability Schedule Name}\label{field-heating-availability-schedule-name}
+
+The name of the schedule that denotes whether the terminal unit can operate to provide heating during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit is on and available for beam heating during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods. The primary air availability schedule named in the input field above must have a value that is ``on'' during times that heating is available.
+
+\paragraph{Field: Primary Air Inlet Node Name}\label{field-primary-air-inlet-node-name}
+
+The name of the HVAC system air node from which the unit draws its primary air.
+
+\paragraph{Field: Primary Air Outlet Node Name}\label{field-primary-air-outlet-node-name}
+
+The name of the HVAC system air node that connects this terminal unit to the zone. The will be the same as one of the zone inlet nodes.
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name}
+
+The name of the chilled water inlet node. If desired, the chilled water node connections can be omitted and the model will assume the intent is to model a two-pipe heating only beam.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name}
+
+The name of the chilled water outlet node.
+
+\paragraph{Field: Design Primary Air Volume Flow Rate}\label{field-design-primary-air-volume-flow-rate}
+
+This is the air flow rate (m3/s) of the primary air entering the air terminal unit from the central air handling unit. This input can be autosized.
+
+\paragraph{Field: Design Chilled Water Volume Flow Rate}\label{field-design-chilled-water-volume-flow-rate}
+
+The maximum chilled water flow rate (m3/s) for the unit(s) serving the entire zone. This input can be autosized based on the zone design load.
+
+\paragraph{Field: Design Hot Water Volume Flow Rate}\label{field-design-hot-water-volume-flow-rate}
+
+The maximum hot water flow rate (m3/s) for the unit(s) serving the entire zone. This input can be autosized based on the zone design load.
+
+\paragraph{Field: Zone Total Beam Length (m)}\label{field-zone-total-beam-length-m}
+
+The total length of all the beams in the zone (m). The real spaces may actually have a number of individual beam units of a specific length and this is the length of individual beams times the total number of beams in the thermal zone. It need not be an even multiple of actual unit's beam length but it can be if desired. This field is autosizable.
+
+\paragraph{Field: Rated Primary Air Flow Rate per Beam Length (m3/s-m)}\label{field-rated-primary-air-flow-rate-per-beam-length-m3s-m}
+
+This is the primary air volume flow rate at rating conditions divided by the length of the beam, in m3/s-m. This ``catalog'' value for volume flow rate input is converted to a mass flow rate using standard air density at sea level. This value will be used for sizing the design primary air volume flow rate if the total beam length is not also autosized. The default is 0.035 m3/s-m.
+
+\paragraph{Field: Beam Rated Cooling Capacity per Beam Length (W/m)}\label{field-beam-rated-cooling-capacity-per-beam-length-wm}
+
+This is the beam cooling capacity at rating conditions divided by the length of the beam, in W/m. This is only the cooling contributed by the chilled water circulating through the convector and is separate from any cooling (or heating) that may also be provided by the primary air. The default is 600 W/m.
+
+\paragraph{Field: Beam Rated Cooling Room Air Chilled Water Temperature Difference (Delta C)}\label{field-beam-rated-cooling-room-air-chilled-water-temperature-difference-delta-c}
+
+This input defines the value of the temperature difference between the room air and entering chilled water at the rating point, in delta Celsius. This ``catalog'' input helps to define the operating conditions that correspond with Rated Beam Cooling Capacity per Meter. It is used to normalize the independent variable in the input field called Beam Cooling Capacity Temperature Difference Modification Factor Curve or Table Name. The default is 10.0 delta C.
+
+\paragraph{Field: Beam Rated Chilled Water Volume Flow Rate per Beam Length (m3/s-m)}\label{field-beam-rated-chilled-water-volume-flow-rate-per-beam-length-m3s-m}
+
+This input defines the value of the chilled water flow rate per meter length of beam at the rating point, in m3/s-m. This input helps to define the operating conditions that correspond with Rated Beam Cooling Capacity per Meter. It is used to normalize the independent variable in the input field called Beam Cooling Capacity Chilled Water Flow Modification Factor Curve or Table Name. The default is 0.00005 m3/s-m.
+
+\paragraph{Field: Beam Cooling Capacity Temperature Difference Modification Factor Curve Name}\label{field-beam-cooling-capacity-temperature-difference-modification-factor-curve-name}
+
+This field is the name of a curve or table object that describes how the beam convector's cooling capacity varies as a function of the temperature difference between the zone air and the entering chilled water. The single independent variable is the ratio of the current simulation results for the difference between the air and entering water and the difference at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the cooling capacity.
+
+\paragraph{Field: Beam Cooling Capacity Air Flow Modification Factor Curve Name}\label{field-beam-cooling-capacity-air-flow-modification-factor-curve-name}
+
+This field is the name of a curve or table object that describes how the beam convector's cooling capacity varies as a function of the primary air flow rate. The single independent variable is the ratio of the current primary air flow rate and the primary air flow rate at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the cooling capacity. The factor is useful to adjust for a range of primary air flow rates that a given product can accommodate. However since this is a constant volume air terminal, the modification does not typically vary during the simulation and the range of independent variable does not need to be all that broad in practice.
+
+\paragraph{Field: Beam Cooling Capacity Chilled Water Flow Modification Factor Curve Name}\label{field-beam-cooling-capacity-chilled-water-flow-modification-factor-curve-name}
+
+This field is the name of a curve or table object that describes how the beam convector's cooling capacity varies as a function of the water flow rate. The single independent variable is the ratio of the current fluid flow rate to the fluid flow rate at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the cooling capacity. The model will adjust the chilled water flow rate to vary cooling power to meet the zone load, so for control purposes, the range of the independent variable must include all the way down to zero flow, with zero capacity at zero flow.
+
+\paragraph{Field: Beam Rated Heating Capacity per Beam Length (W/m)}\label{field-beam-rated-heating-capacity-per-beam-length-wm}
+
+This is the beam heating capacity at rating conditions divided by the length of the beam, in W/m. This is only the heating contributed by the hot water circulating through the convector and is separate from any heating (or cooling) that may also be provided by the primary air. The default is 1.200 W/m.
+
+\paragraph{Field: Beam Rated Heating Room Air Hot Water Temperature Difference (Delta C)}\label{field-beam-rated-heating-room-air-hot-water-temperature-difference-delta-c}
+
+This input defines the value of the temperature difference between the entering hot water and the room air at the rating point, in delta Celsius. This input helps to define the operating conditions that correspond with Rated Beam Heating Capacity per Meter. It is used to normalize the independent variable in the input field called Beam Heating Capacity Temperature Difference Modification Factor Curve or Table Name. The default is 27.8 delta C.
+
+\paragraph{Field: Beam Rated Hot Water Volume Flow Rate per Beam Length (m3/s-m)}\label{field-beam-rated-hot-water-volume-flow-rate-per-beam-length-m3s-m}
+
+This input defines the value of the hot water flow rate per meter length of beam at the rating point, in m3/s/m, or more strictly m3/s-m. This input helps to define the operating conditions that correspond with Rated Beam Heating Capacity per Meter. It is used to normalize the independent variable in the input field called Beam Heating Capacity Hot Water Flow Modification Factor Curve or Table Name. The default is 0.00005 m3/s-m.
+
+\paragraph{Field: Beam Heating Capacity Temperature Difference Modification Factor Curve Name}\label{field-beam-heating-capacity-temperature-difference-modification-factor-curve-name}
+
+This field is the name of a curve or table object that describes how the beam convector's heating capacity varies as a function of the temperature difference between the entering hot water and the zone air. The single independent variable is the ratio of the current simulation results for the difference between the water and air and the difference at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the heating capacity.
+
+\paragraph{Field: Beam Heating Capacity Air Flow Modification Factor Curve Name}\label{field-beam-heating-capacity-air-flow-modification-factor-curve-name}
+
+This field is the name of a curve or table object that describes how the beam convectors heating capacity varies as a function of the primary air flow rate. The single independent variable is the ratio of the current primary air flow rate and the primary air flow rate at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the heating capacity. The factor is useful to adjust for a range of primary air rates that a given product can accommodate. However since this is a constant volume air terminal, the modification does not typically vary during the simulation and the range of independent variable does not need to be all that broad in practice.
+
+\paragraph{Field: Beam Heating Capacity Hot Water Flow Modification Factor Curve Name}\label{field-beam-heating-capacity-hot-water-flow-modification-factor-curve-name}
+
+This field is the name of a curve or table object that describes how the beam convector's heating capacity varies as a function of the water flow rate. The single independent variable is the ratio of the current fluid flow rate to the fluid flow rate at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the heating capacity. The model will adjust the hot water flow rate to vary heating power to meet the zone load, so for control purposes, the range of the independent variable must include all the way down to zero flow, with zero capacity at zero flow.
+
+An example input follows:
+
+\begin{lstlisting}
+  AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam,
+    Zone One 4pipe Beam, !- Name
+    ALWAYS_ON , !- Primary Air Availability Schedule Name
+    ALWAYS_ON , !- Cooling Availability Schedule Name
+    ALWAYS_ON , !- Heating Availability Schedule Name
+    Zone One 4pipe Beam Inlet Node Name , !- Primary Air Inlet Node Name
+    Zone One 4pipe Beam Outlet Node Name , !- Primary Air Outlet Node Name
+    Zone One 4pipe Beam CW Inlet Node , !- Chilled Water Inlet Node Name
+    Zone One 4pipe Beam CW Outlet Node , !- Chilled Water Outlet Node Name
+    AUTOSIZE , !- Design Primary Air Volume Flow Rate
+    AUTOSIZE , !- Design Chilled Water Volume Flow Rate
+    AUTOSIZE , !- Design Hot Water Volume Flow Rate
+    AUTOSIZE , !- Zone Total Beam Length
+    0.036 , !- Rated Primary Air Flow Rate per Beam Length
+    597 , !- Rated Beam Cooling Capacity per Beam Length
+    10.0 , !- Rated Cooling Room Air Chilled Water Temperature Difference
+    5.2E-5 , !- Rated Chilled Water Volume Flow Rate per Beam Length
+    CapModFuncOfTempDiff, !- Beam Cooling Capacity Temperature Difference Modification Factor Curve or Table Name
+    CoolCapModFuncOfSAFlow, !- Beam Cooling Capacity Air Flow Modification Factor Curve or Table Name
+    CapModFuncOfWaterFlow, !- Beam Cooling Capacity Chilled Water Flow Modification Factor Curve or Table Name
+    1548 , !- Rated Beam Heating Capacity per Beam Length
+    27.8, !- Rated Heating Room Air Hot Water Temperature Difference
+    5.2E-5, !- Rated Hot Water Volume Flow Rate per Beam Length
+    CapModFuncOfTempDiff, !- Beam Heating Capacity Temperature Difference Modification Factor Curve or Table Name
+    HeatCapModFuncOfSAFlow, !- Beam Heating Capacity Air Flow Modification Factor Curve or Table Name
+    CapModFuncOfWaterFlow; !- Beam Heating Capacity Hot Water Flow Modification Factor Curve or Table Name
+\end{lstlisting}
+
+\begin{lstlisting}
+  Curve:Linear,  ! y = x
+    CapModFuncOfTempDiff, !-Name
+    0, !_ Coef Const
+    1, !- Coef x
+    0,  !- min x
+    1.5, !- max x
+    0.0 , !- min y
+    1.5; ! max y
+\end{lstlisting}
+
+\begin{lstlisting}
+  Table:OneIndependentVariable,
+    CoolCapModFuncOfSAFlow, !- Name
+    quadratic,!- Curve Type
+    EvaluateCurveToLimits,!- Interpolation Method
+    0.714,!- min x
+    1.2857,!- max x
+    0.8234,!- min y
+    1.1256,!- max y
+    dimensionless, !-
+    dimensionless, !-
+    , !- normalization ref
+    0.714286, 0.823403,
+    1.0,      1.0,
+    1.2857,   1.1256;
+\end{lstlisting}
+
+\begin{lstlisting}
+  Table:OneIndependentVariable,
+    CapModFuncOfWaterFlow, !- Name
+    quadratic,!- Curve Type
+    EvaluateCurveToLimits,!- Interpolation Method
+    0.0,!- min x
+    1.333333,!- max x
+    0.0,!- min y
+    1.04,!- max y
+    dimensionless, !-
+    dimensionless, !-
+     , !- normalization ref
+    0.0,      0.0,
+    0.05,     0.001,
+    0.33333,  0.71,
+    0.5,      0.85,
+    0.666667, 0.92,
+    0.833333, 0.97,
+    1.0,      1.0,
+    1.333333, 1.04;
+\end{lstlisting}
+
+\begin{lstlisting}
+  Table:OneIndependentVariable,
+    HeatCapModFuncOfSAFlow, !- Name
+    quadratic,!- Curve Type
+    EvaluateCurveToLimits,!- Interpolation Method
+    0.714,!- min x
+    1.2857,!- max x
+    0.8554,!- min y
+    1.0778,!- max y
+    dimensionless, !-
+    dimensionless, !-
+    , !- normalization ref
+    0.714286, 0.8554,
+    1.0,      1.0,
+    1.2857,   1.0778;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-10}
+
+\paragraph{Zone Air Terminal Beam Sensible Cooling Rate {[}W{]}}\label{zone-air-terminal-beam-sensible-cooling-rate-w}
+
+\paragraph{Zone Air Terminal Beam Sensible Cooling Energy {[}J{]}}\label{zone-air-terminal-beam-sensible-cooling-energy-j}
+
+These are the sensible cooling power and energy delivered by the beams to the zone, exclusive of any cooling or heating done by the primary air.
+
+\paragraph{Zone Air Terminal Beam Sensible Heating Rate {[}W{]}}\label{zone-air-terminal-beam-sensible-heating-rate-w}
+
+\paragraph{Zone Air Terminal Beam Sensible Heating Energy {[}J{]}}\label{zone-air-terminal-beam-sensible-heating-energy-j}
+
+These are the sensible heating power and energy delivered by the beams to the zone, exclusive of any cooling or heating done by the primary air.
+
+\paragraph{Zone Air Terminal Primary Air Sensible Cooling Rate {[}W{]}}\label{zone-air-terminal-primary-air-sensible-cooling-rate-w}
+
+Sensible cooling by the primary air to the zone, exclusive of any cooling or heating done by the beams.
+
+\paragraph{Zone Air Terminal Primary Air Sensible Cooling Energy {[}J{]}}\label{zone-air-terminal-primary-air-sensible-cooling-energy-j}
+
+Sensible cooling by the primary air to the zone, exclusive of any cooling or heating done by the beams.
+
+\paragraph{Zone Air Terminal Primary Air Sensible Heating Rate {[}W{]}}\label{zone-air-terminal-primary-air-sensible-heating-rate-w}
+
+Heating by the primary air to the zone, exclusive of any cooling or heating done by the beams.
+
+\paragraph{Zone Air Terminal Primary Air Sensible Heating Energy {[}J{]}}\label{zone-air-terminal-primary-air-sensible-heating-energy-j}
+
+Heating by the primary air to the zone, exclusive of any cooling or heating done by the beams.
+
+\paragraph{Zone Air Terminal Primary Air Flow Rate {[}m3/s{]}}\label{zone-air-terminal-primary-air-flow-rate-m3s}
+
+Air flow rate from the central air handler into the zone in m3/s. Note that this does not include any of the secondary air flow that is induced by the convector and nozzle action (the model does not resolve secondary air flow rate and the result are not available).
+
+\subsection{AirTerminal:SingleDuct:ConstantVolume:CooledBeam}\label{airterminalsingleductconstantvolumecooledbeam}
+
+The Cooled Beam system is a mixed air-hydronic system. A central, single-duct forced-air system supplies conditioned ventilation air to the zones. Sensible cooling is done by chilled water circulating through ceiling mounted cooled beam units. Chilled water flow rate through the cooled beam units is varied to meet the zone sensible cooling load. Any dehumidification is done by the central ventilation air system. Heating is usually accomplished with hot water radiators. Thermodynamically, the cooled beam system resembles the four-pipe induction unit.
+
+To model a typical cooled beam system the user will need to define a conventional central constant volume forced air system. This system will normally be 100\% outside air delivered at a fixed supply temperature (which could be reset by schedule or by outside air temperature). On the supply side of this air loop there will be the usual central AC equipment: outside air mixer, fan, heating and cooling coil. On the zone equipment (demand) side of the loop, the chilled beams will be represented as terminal units. Additional zone equipment (such as baseboard heaters) will be needed to handle heating loads.
+
+Although the cooled beam equipment in a zone is treated by the program as a single terminal unit, the actual installation will have multiple beams in each zone. The program (in its sizing calculation for the system) figures out how many beams of what length are needed to meet the zone design load.
+
+\subsubsection{Inputs}\label{inputs-11-000}
+
+\paragraph{Field: Name}\label{field-name-11-000}
+
+A unique user assigned name for a particular chilled beam unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-10}
+
+The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Cooled Beam Type}\label{field-cooled-beam-type}
+
+Two types of units are modeled: \emph{Active} or \emph{Passive}. In the active unit, primary air is supplied through the beam, inducing some secondary zone air into contact with the coil. This unit acts as an active convector. The passive unit is simply a passive, finned convector. Primary air is supplied through a normal diffuser.
+
+\paragraph{Field: Supply Air Inlet Node Name}\label{field-supply-air-inlet-node-name-3}
+
+The name of the HVAC system node from which the unit draws its primary or supply air. Note that this field should be specified for both types of unit, even though supply air does not pass through the passive unit.
+
+\paragraph{Field: Supply Air Outlet Node Name}\label{field-supply-air-outlet-node-name}
+
+The name of the air node that connects this terminal unit to the zone. The will be the same as one of the zone inlet nodes. The name of this node must be entered even if the actual beams are passive and is not actually supplying air to the zone.
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-1}
+
+The name of the chilled water inlet node.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-1}
+
+The name of the chilled water outlet node.
+
+\paragraph{Field: Supply Air Volumetric Flow Rate}\label{field-supply-air-volumetric-flow-rate}
+
+This is the air flow rate in cubic meters per second of the supply air entering the zone. This input would normally be autosized based on the ventilation requirement (see Zone Sizing).
+
+\paragraph{Field: Maximum Total Chilled Water Volumetric Flow Rate}\label{field-maximum-total-chilled-water-volumetric-flow-rate}
+
+The maximum chilled water flow rate (in cubic meters per second) for the unit. This input would normally be autosized based on the zone design load.
+
+\paragraph{Field: Number of Beams}\label{field-number-of-beams}
+
+The number of individual cooled beam units in the zone. Normally this unit would be autocalculated by the program based upon the previous field and the nominal flow rate for a single beam unit (set by the program to 0.07 kg/s).
+
+\paragraph{Field: Beam Length}\label{field-beam-length}
+
+The length of an individual beam in meters. Normally this will be autocalculated by the program based upon the number of beam units and the zone design sensible cooling load. 1 to 4 meters is a typical length range.
+
+\paragraph{Field: Design Inlet Water Temperature}\label{field-design-inlet-water-temperature}
+
+The nominal or design inlet water temperature in degrees Celsius. The default is 15°C.
+
+\paragraph{Field: Design Outlet Water Temperature}\label{field-design-outlet-water-temperature}
+
+The nominal or design outlet water temperature in degrees Celsius. The default is 17°C.
+
+\emph{The following inputs are parameters used to characterize the performance of the chilled beam units. Values for a given unit can be obtained from the manufacturer. The parameters are used in the following equations.~~~~~}
+
+\emph{P\(_{beam}\)} = \emph{A·K·DT~~~~~~~} ~~~~~~~~~~~~~~~~~~~~~~~ beam cooling output per unit length W/m
+
+\emph{K = a·DT\(^{n1}\)·vr\(^{n2}\)·w\(^{n3}\)}~~~~~~~~~~~~~~~~~~~~~~~~~~~ coil heat transfer coefficient W/(m\(^{2}\)K)
+
+\emph{vr = (q\(_{in}\)}/a\emph{\(_{0}\))·r\(_{air}\)}~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ room air mass flow rate across coil kg/(m\(^{2}\)s)
+
+\emph{q\(_{in}\) = K\(_{1}\)·DT\(^{n}\)+K\(_{in}\)·q\(_{pr}\)}~~~~~~~~~~~~~~~~ room air volumetric flow rate across coil per
+
+unit length m\(^{3}\)/(s-m)
+
+DT is the room air --water temperature difference (average water temperature is used) in degrees C.
+
+w is the water velocity in m/s.
+
+q\(_{pr}\) is the supply air flow rate per unit length m\(^{3}\)/(s-m)
+
+\paragraph{Field: Coil Surface Area per Coil Length}\label{field-coil-surface-area-per-coil-length}
+
+Surface area on the air side of the beam per unit beam length. The units are square meters per meter. The default is 5.422. This is \emph{A} in the above equations.
+
+\paragraph{Field: Model Parameter a (a)}\label{field-model-parameter-a-a}
+
+This is ain the above equations. The default is 15.3
+
+\paragraph{Field: Model Parameter n1}\label{field-model-parameter-n1}
+
+This is n1 in the above equations. The default is 0.
+
+\paragraph{Field: Model Parameter n2}\label{field-model-parameter-n2}
+
+This is n2 in the above equations. The default is 0.84.
+
+\paragraph{Field: Model Parameter n3}\label{field-model-parameter-n3}
+
+This is n3 in the above equations. The default is 0.12.
+
+\paragraph{\texorpdfstring{Field: Model Parameter a\(_{0}\) (a)}{Field: Model Parameter a\_\{0\} (a)}}\label{field-model-parameter-aux5f0-a}
+
+This is a\(_{0}\) in the above equations. It is the free area of the coil in plan view (for the air flow) per unit beam length. The units are square meters per meter. The default is 0.171.
+
+\paragraph{\texorpdfstring{Field: Model Parameter K\(_{1}\) (K1)}{Field: Model Parameter K\_\{1\} (K1)}}\label{field-model-parameter-kux5f1-k1}
+
+This is K\(_{1}\) in the above equations. The default is 0.005.
+
+\paragraph{Field: Model Parameter n}\label{field-model-parameter-n}
+
+This is n in the above equations. The default is 0.4.
+
+\paragraph{\texorpdfstring{Field: Coefficient of Induction K\(_{in}\) (Kin)}{Field: Coefficient of Induction K\_\{in\} (Kin)}}\label{field-coefficient-of-induction-kux5fin-kin}
+
+The coefficient of induction K\(_{in}\) in the above equations. The default is 2.0 for active beams and 0.0 for passive beams.
+
+\paragraph{Field: Pipe Inside Diameter}\label{field-pipe-inside-diameter}
+
+The water pipe inside diameter in meters. The default is 0.0145.
+
+An example input is:
+
+\begin{lstlisting}
+
+  AirTerminal:SingleDuct:ConstantVolume:CooledBeam,
+      SPACE2-1 CB,             !- Name
+      CWCoilAvailSched,        !- Availability Schedule Name
+      Active,                  !- Cooled Beam Type
+      SPACE2-1 ATU Supply Node,!- Supply Air Inlet Node Name
+      SPACE2-1 In Node,        !- Supply Air Outlet Node Name
+      SPACE2-1 CW Coil Water In Node,  !- Chilled Water Inlet Node Name
+      SPACE2-1 CW Coil Water Out Node, !- Chilled Water Outlet Node Name
+      ,                        !- Supply Air Volumetric Flow Rate
+      ,                   !- Maximum Total Chilled Water Volumetric Flow Rate
+      ,                        !- Number of Beams
+      ,                        !- Beam Length
+      ,                        !- Design Inlet Water Temperature
+      ,                        !- Design Outlet Water temperature
+      ,                        !- Coil Surface Area per Coil Length
+      ,                        !- Model Parameter a
+      ,                        !- Model Parameter n1
+      ,                        !- Model Parameter n2
+     ,                        !- Model Parameter n3
+      ,                        !- Model Parameter a0
+      ,                        !- Model Parameter K1
+      ,                        !- Model Parameter n
+      ,                        !- Coefficient of Induction Kin
+      ;                        !- Leaving Pipe Inside Diameter
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-11}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Zone Air Terminal Beam Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Air Terminal Beam Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Zone Air Terminal Supply Air Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Air Terminal Supply Air Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Air Terminal Supply Air Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Air Terminal Supply Air Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Air Terminal Beam Chilled Water Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Zone Air Terminal Beam Sensible Cooling Rate {[}W{]}}\label{zone-air-terminal-beam-sensible-cooling-rate-w-1}
+
+Sensible cooling by the beams in the zone, exclusive of any cooling or heating done by the supply air.
+
+\paragraph{Zone Air Terminal Beam Sensible Cooling Energy {[}J{]}}\label{zone-air-terminal-beam-sensible-cooling-energy-j-1}
+
+Sensible cooling by the beams in the zone, exclusive of any cooling or heating done by the supply air.
+
+\paragraph{Zone Air Terminal Supply Air Sensible Cooling Rate {[}W{]}}\label{zone-air-terminal-supply-air-sensible-cooling-rate-w}
+
+Sensible cooling by the supply air to the zone, exclusive of any cooling done by the beams.
+
+\paragraph{Zone Air Terminal Supply Air Sensible Cooling Energy {[}J{]}}\label{zone-air-terminal-supply-air-sensible-cooling-energy-j}
+
+Sensible cooling by the supply air to the zone, exclusive of any cooling done by the beams.
+
+\paragraph{Zone Air Terminal Supply Air Sensible Heating Rate {[}W{]}}\label{zone-air-terminal-supply-air-sensible-heating-rate-w}
+
+Heating by the supply air to the zone, exclusive of any cooling done by the beams.
+
+\paragraph{Zone Air Terminal Supply Air Sensible Heating Energy {[}J{]}}\label{zone-air-terminal-supply-air-sensible-heating-energy-j}
+
+Heating by the supply air to the zone, exclusive of any cooling done by the beams.
+
+\paragraph{Zone Air Terminal Beam Chilled Water Energy {[}J{]}}\label{zone-air-terminal-beam-chilled-water-energy-j}
+
+The heat transfer energy for the chilled water serving the beams, in Joules.
+
+\subsection{AirTerminal:SingleDuct:InletSideMixer}\label{airterminalsingleductinletsidemixer}
+
+The inlet side mixer air terminal unit provides a means of supplying central system air to the air inlet of a zone AC unit such as a four pipe fan coil. Normally the central air would be ventilation air from a dedicated outside air system (DOAS).
+
+The AirTerminal:SingleDuct:InletSideMixer simply mixes two inlet air streams into a single outlet stream. One inlet - designated the primary air stream - is from the DOAS. The other inlet - designated the secondary air stream - is recirculated air from the zone. The outlet air stream of the inlet side mixer is then the inlet to the zone AC unit.
+
+\begin{figure}[hbtp] % fig 108
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image275.png}
+\caption{Inlet Side Mixer Air Terminal Unit with Fan Coil \protect \label{fig:inlet-side-mixer-air-terminal-unit-with-fan}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-12-000}
+
+\paragraph{Field: Name}\label{field-name-12}
+
+A unique user assigned name for a particular inlet side mixer terminal unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: ZoneHVAC Terminal Unit Object Type}\label{field-zonehvac-terminal-unit-object-type}
+
+The type of zone AC unit to which this terminal unit will be connected. This is a choice field. The choices are ZoneHVAC:FourPipeFanCoil or ZoneHVAC:WaterToAirHeatPump.
+
+\paragraph{Field: ZoneHVAC Terminal Unit Name}\label{field-zonehvac-terminal-unit-name}
+
+The name of the zone AC unit to which this terminal will be connected.
+
+\paragraph{Field: Terminal Unit Outlet Node Name}\label{field-terminal-unit-outlet-node-name}
+
+The name of the air outlet node of the inlet side mixer. This will be the inlet air node of the zone AC unit.
+
+\paragraph{Field: Terminal Unit Primary Air Inlet Node Name}\label{field-terminal-unit-primary-air-inlet-node-name}
+
+The name of the primary air inlet node of the inlet side mixer. This will be an outlet node of an AirLoopHVAC:ZoneSplitter, providing the connection to the DOAS system.
+
+\paragraph{Field: Terminal Unit Secondary Air Inlet Node Name}\label{field-terminal-unit-secondary-air-inlet-node-name}
+
+The name of the secondary air inlet node of the inlet side mixer. This will be an exhaust node of the zone that is being conditioned.
+
+An IDF example:
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:InletSideMixer,
+      SPACE2-1 DOAS Air Terminal,  !- Name
+      ZoneHVAC:FourPipeFanCoil,!- ZoneHVAC Terminal Unit Object Type
+      SPACE2-1 Fan Coil,       !- ZoneHVAC Terminal Unit Name
+      SPACE2-1 Fan Coil Inlet, !- Terminal Unit Outlet Node Name
+      SPACE2-1 Air Terminal Mixer Primary Inlet,  !- Terminal Unit Primary Air Inlet Node Name
+      SPACE2-1 Air Terminal Mixer Secondary Inlet;  !- Terminal Unit Secondary Air Inlet Node Name
+\end{lstlisting}
+
+\subsection{AirTerminal:SingleDuct:SupplySideMixer}\label{airterminalsingleductsupplysidemixer}
+
+The supply side mixer air terminal unit provides a means of supplying central system air to the air outlet of a zone AC unit such as a four pipe fan coil. Normally the central air would be ventilation air from a dedicated outside air system (DOAS).
+
+The AirTerminal:SingleDuct:SupplySideMixer simply mixes two inlet air streams into a single outlet stream. One inlet - designated the primary air stream - is from the DOAS. The other inlet - designated the secondary air stream - is outlet air from the zone AC unit. The outlet air stream from the supply side mixer is then the inlet to the conditioned zone.
+
+\begin{figure}[hbtp] % fig 109
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image276.png}
+\caption{Supply Side Mixer Air Terminal Unit with Fan Coil \protect \label{fig:supply-side-mixer-air-terminal-unit-with-fan}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-13-000}
+
+\paragraph{Field: Name}\label{field-name-13}
+
+A unique user assigned name for a particular supply side mixer terminal unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: ZoneHVAC Terminal Unit Object Type}\label{field-zonehvac-terminal-unit-object-type-1}
+
+The type of zone AC unit to which this terminal unit will be connected. This is a choice field. The choices are ZoneHVAC:FourPipeFanCoil or ZoneHVAC:WaterToAirHeatPump.
+
+\paragraph{Field: ZoneHVAC Terminal Unit Name}\label{field-zonehvac-terminal-unit-name-1}
+
+The name of the zone AC unit to which this terminal will be connected.
+
+\paragraph{Field: Terminal Unit Outlet Node Name}\label{field-terminal-unit-outlet-node-name-1}
+
+The name of the air outlet node of the supply side mixer. This will be an inlet air node of the conditioned zone.
+
+\paragraph{Field: Terminal Unit Primary Air Inlet Node Name}\label{field-terminal-unit-primary-air-inlet-node-name-1}
+
+The name of the primary air inlet node of the supply side mixer. This will be an outlet node of an AirLoopHVAC:ZoneSplitter, providing the connection to the DOAS system.
+
+\paragraph{Field: Terminal Unit Secondary Air Inlet Node Name}\label{field-terminal-unit-secondary-air-inlet-node-name-1}
+
+The name of the secondary air inlet node of the supply side mixer. This will be the outlet air node of the zone AC unit.
+
+An IDF example:
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:SupplySideMixer,
+      SPACE1-1 DOAS Air Terminal,  !- Name
+      ZoneHVAC:FourPipeFanCoil,!- ZoneHVAC Terminal Unit Object Type
+      SPACE1-1 Fan Coil,       !- ZoneHVAC Terminal Unit Name
+      SPACE1-1 Supply Inlet,   !- Terminal Unit Outlet Node Name
+      SPACE1-1 Air Terminal Mixer Primary Inlet,  !- Terminal Unit Primary Air Inlet Node Name
+      SPACE1-1 Fan Coil Outlet;!- Terminal Unit Secondary Air Inlet Node Name
+\end{lstlisting}
+
+\subsection{AirTerminal:DualDuct:ConstantVolume}\label{airterminaldualductconstantvolume}
+
+The AirTerminal:DualDuct:ConstantVolume simulation or the typical Multizone is described by this Air Distribution Unit (ADU). Multizone systems condition all the air in a central apparatus and distribute it to the conditioned zones through two parallel ducts. One duct carries cold air and the other warm air, providing air sources for both heating and cooling at all times. In each conditioned zone, a mixing valve responsive to a room thermostat mixes the warm and cold air in proper proportions to satisfy the prevailing heating or cooling load of the space. The Multizone ADU is the specific component that leads to the zone containing the mixer and the mixing damper and then connecting to the zone. The total airflow to each room is kept constant while the proportion of hot air to cold air is adjusted to maintain the temperature in each zone at the desired level.
+
+\subsubsection{Inputs}\label{inputs-14-000}
+
+\paragraph{Field: Name}\label{field-name-14}
+
+Unique name for the Multizone ADU.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-11}
+
+Schedule that this component will operate or is available to operate for a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-7}
+
+The outlet node from the ADU to the zone.
+
+\paragraph{Field: Hot Air Inlet Node Name}\label{field-hot-air-inlet-node-name}
+
+The air-inlet node name that connects the hot air splitter to the individual zone ADU.
+
+\paragraph{Field: Cold Air Inlet Node Name}\label{field-cold-air-inlet-node-name}
+
+The air-inlet node name that connects the cold air splitter to the individual zone ADU.
+
+\paragraph{Field: Maximum Air Flow Rate}\label{field-maximum-air-flow-rate-7}
+
+The design constant volume flow rate~ (m\(^{3}\)/sec) specified for that Multizone ADU.
+
+An IDF example:
+
+\begin{lstlisting}
+
+AirTerminal:DualDuct:ConstantVolume,
+      Zone2MixDamp,  !- Name
+      FanAndCoilAvailSched,  !- Availability Schedule
+      Zone 2 Dual Duct Outlet,  !- Unit Air Outlet Node
+      Zone 2 Dual Duct Hot Inlet,  !- Unit Hot Air Inlet Node
+      Zone 2 Dual Duct Cold Inlet,  !- Unit Cold Air Inlet Node
+      0.36;  !- Max Air Flow Rate {m3/s}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-12}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Air Terminal Cold Supply Duct Damper Position {[]}
+\item
+  HVAC,Average,Zone Air Terminal Hot Supply Duct Damper Position {[]}
+\end{itemize}
+
+\paragraph{Zone Air Terminal Cold Supply Duct Damper Position}\label{zone-air-terminal-cold-supply-duct-damper-position}
+
+This output is the damper position of the cold air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit cold air mass flow rate divided by the terminal unit's maximum cold air mass flow rate. This output is dimensionless and ranges from 0.0 to 1.0.
+
+\paragraph{Zone Air Terminal Hot Supply Duct Damper Position}\label{zone-air-terminal-hot-supply-duct-damper-position}
+
+This output is the damper position of the hot air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit hot air mass flow rate divided by the terminal unit's maximum hot air mass flow rate. This output is dimensionless and ranges from 0.0 to 1.0.
+
+\subsection{AirTerminal:DualDuct:VAV}\label{airterminaldualductvav}
+
+AirTerminal:DualDuct:VAV (i.e., Dual duct variable air volume (DDVAV)) systems are used to obtain zone temperature control by mixing the cold and warm air in various volume combinations. The fan is sized for the anticipated maximum coincident hot or cold volume, not the sum of the instantaneous peaks. This system has an advantage of a true single path VAV system, except for warm port leakage. When cold air is modulated for control before mixing, it operates similar to the VAV induction when mixing occurs without hot deck reheat. It is similar to a reheat system when mixing occurs while the hot deck is using the reheat coil. It uses more energy than a true VAV system, but less than a constant volume dual duct system.
+
+\subsubsection{Inputs}\label{inputs-15-000}
+
+\paragraph{Field: Name}\label{field-name-15}
+
+Unique name for the AirTerminal:DualDuct:VAV Air Distribution Unit (ADU).
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-12}
+
+Schedule that this component will operate or is available to operate for a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-8}
+
+The outlet node from the ADU to the zone.
+
+\paragraph{Field: Hot Air Inlet Node Name}\label{field-hot-air-inlet-node-name-1}
+
+The air-inlet node name that connects the hot air splitter to the individual zone ADU.
+
+\paragraph{Field: Cold Air Inlet Node Name}\label{field-cold-air-inlet-node-name-1}
+
+The air-inlet node name that connects the cold air splitter to the individual zone ADU.
+
+\paragraph{Field: Maximum Damper Air Flow Rate}\label{field-maximum-damper-air-flow-rate}
+
+The design maximum volume flow rate~ (m\(^{3}\)/sec) specified for DDVAV ADU.
+
+\paragraph{Field: Zone Minimum Air Flow Fraction}\label{field-zone-minimum-air-flow-fraction-3}
+
+The minimum flow rate to the zone while the system is operating, specified as a fraction of the Max Damper Air Flow Rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-2}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object. When this field is used, the terminal unit will increase flow as needed to meet this outdoor air requirement. If Outdoor Air Flow per Person is non-zero, then the outdoor air requirement will be computed based on the current number of occupants in the zone. At no time will the supply air flow rate exceed the value for Maximum Air Flow Rate. If this field is blank, then the terminal unit will not be controlled for outdoor air flow. See documentation for the zone HVAC outdoor air object for further information (Ref DesignSpecification:OutdoorAir).
+
+An IDF example:
+
+\begin{lstlisting}
+
+  AirTerminal:DualDuct:VAV,
+      Zone1MixDamp,            !- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      Zone 1 Dual Duct Outlet, !- Air Outlet Node Name
+      Zone 1 Dual Duct Hot Inlet,  !- Hot Air Inlet Node Name
+      Zone 1 Dual Duct Cold Inlet,  !- Cold Air Inlet Node Name
+      autosize,                !- Maximum Air Flow Rate {m3/s}
+      0.1,                     !- Zone Minimum Air Flow Fraction
+      ZoneMinOARequirements;   !- Design Specification Outdoor Air Object Name
+
+  ! Outdoor air specification should be consistent with Sizing:Zone object inputs.
+    DesignSpecification:OutdoorAir,
+      ZoneMinOARequirements,    !- Name
+      Sum,                      !- Outdoor Air Method
+      0.00944,                  !- Outdoor Air Flow per Person {m3/s}
+      0.000508,                 !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
+      ,                         !- Outdoor Air Flow per Zone
+      ,                         !- Outdoor Air Flow Air Changes per Hour
+      Min OARequirements Sched; !- Outdoor Air Flow Rate Fraction Schedule Name
+
+    Schedule:Compact,
+      Min OARequirements Sched,  !- Name
+      Any Number,                !- Schedule Type Limits Name
+      Through: 12/31,            !- Field 1
+      For: Weekdays SummerDesignDay WinterDesignDay, !- Field 2
+      Until: 24:00,1.0,          !- Field 7
+      For: AllOtherDays,         !- Field 9
+      Until: 24:00,0.25;         !- Field 10
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-13}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Air Terminal Cold Supply Duct Damper Position {[]}
+\item
+  HVAC,Average,Zone Air Terminal Hot Supply Duct Damper Position {[]}
+\item
+  HVAC,Average,Zone Air Terminal Outdoor Air Volume Flow Rate {[}m3/s{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Zone Air Terminal Cold Supply Duct Damper Position {[]}}{Zone Air Terminal Cold Supply Duct Damper Position }}\label{zone-air-terminal-cold-supply-duct-damper-position-1}
+
+This output is the damper position of the cold air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit cold air mass flow rate divided by the terminal unit's maximum cold air mass flow rate.
+
+\paragraph{\texorpdfstring{Zone Air Terminal Hot Supply Duct Damper Position {[]}}{Zone Air Terminal Hot Supply Duct Damper Position }}\label{zone-air-terminal-hot-supply-duct-damper-position-1}
+
+This output is the damper position of the hot air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit hot air mass flow rate divided by the terminal unit's maximum hot air mass flow rate.
+
+\paragraph{Zone Air Terminal Outdoor Air Volume Flow Rate {[}m3/s{]}}\label{zone-air-terminal-outdoor-air-volume-flow-rate-m3s-2}
+
+This output is the amount of outdoor air entering the zone. This is the average value over the frequency being reported.~ The amount of outdoor air is defined as the terminal unit air volume flow rate multiplied by the fraction of outdoor air entering the air loop's outdoor air system.
+
+\subsection{AirTerminal:DualDuct:VAV:OutdoorAir}\label{airterminaldualductvavoutdoorair}
+
+AirTerminal:DualDuct:VAV:OutdoorAir provides a model for a type of dual duct air system in which one duct provides outdoor air ventilation and the other provides VAV cooling.~ The Outdoor Air stream and the Recirculated Air stream are conditioned and supplied through separate air streams as part of a centralized dedicated outdoor air~ (DOAS) distribution system. The dual duct arrangement allows the ventilation air to be controlled separately using schedules or occupancy demand while the recirculated air is controlled to meet the dry-bulb zone temperature setpoint. The two airstreams remain decoupled until the terminal box where they are mixed. The terminal unit is meant for systems regulating outdoor air based only on demand control or code minimum settings and not on economizer operation.
+
+This air terminal does not have heating coils and is not configured for conditions zones that need heat. Additional ZoneHVAC equipment, such as baseboards or fan coil units, are needed to provide heating to the zone when using this air terminal.
+
+Although this air terminal is primarily for dual duct system, it is allowed to use just the outdoor air side in a single duct system. This can be useful for modeling single duct DOAS when the required volume of outdoor air varies over time.
+
+\subsubsection{Inputs}\label{inputs-16-000}
+
+\paragraph{Field: Name}\label{field-name-16}
+
+Unique name for the AirTerminal:DualDuct:VAV:OutdoorAir Air Distribution Unit (ADU).
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-13}
+
+Schedule that this component will operate or is available to operate for a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-9}
+
+The outlet node of the terminal unit.~ This is the node leaving the unit and serving as the inlet to the zone. It is for the mixed flow leaving from both of the inlet node.
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name}
+
+The inlet node of the Outdoor Air (OA) stream deck of the Dual Duct system.
+
+\paragraph{Field: Recirculated Air Inlet Node Name}\label{field-recirculated-air-inlet-node-name}
+
+The inlet node of the Recirculated Air (RA) stream deck of the Dual Duct system. ~This input is optional.~ If no node name is entered here, then the recirulation duct is disabled and the model functions as a single duct terminal and no second cooling deck is needed.
+
+\paragraph{Field: Maximum Zone Total Airflow Rate}\label{field-maximum-zone-total-airflow-rate}
+
+Max total airflow rate (in m3/s) at the terminal unit outlet including both the Outdoor Air stream and the Recirculated stream.~ Can be autosized based on the Design Outdoor Airflow Rate and the zone thermal cooling load.~ The autosized flow rate will be the sum of the maximum outdoor air requirement and the flow for cooling. ~When autosizing, this maximum and the individual inlet flow rate sizes are reported to the eio file.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-3}
+
+This field specifies the name of a DesignSpecification:OutdoorAir object.~ This field is required for this object.~ The terminal unit will modulate the Outdoor Air stream to meet this outdoor air requirement.~ If Outdoor Air Flow per Person is applied, then the outdoor air required will be based on either the current number of occupants in the zone, as for demand controlled ventilation, or the design level of occupants depending on the setting in the next field.
+
+\paragraph{Field: Per Person Ventilation Rate Mode}\label{field-per-person-ventilation-rate-mode}
+
+This field specifies how the outdoor air ventilation rates are calculated when based on a rate per person.~ It can be either based on the current number of people as affected by time-varying occupancy schedules, or on the constant value for the maximum number of people.~~ Enter the key CurrentOccupancy for the former and DesignOccupancy for the later.
+
+An example input object follows.
+
+\begin{lstlisting}
+
+  AirTerminal:DualDuct:VAV:OutdoorAir,
+      Media_Center Dual Duct Box Component,          !- Name
+      ALWAYS_ON,                                     !- Availability Schedule Name
+      Media_Center Dual Duct Box Outlet Node Name,   !- Air Outlet Node Name
+      Media_Center Dual Duct Box Inlet Node Name,    !- Outdoor Air Inlet Node Name
+      RC Media_Center Dual Duct Box Inlet Node Name, !- Recirculated Air Inlet Node Name
+      AUTOSIZE,                                      !- Maximum Terminal Air Flow Rate {m3/s}
+      Media_Center Dual Duct Box OA Design Spec,     !- Design Specification Outdoor Air Object Name
+      CurrentOccupancy;                              !- Per Person Ventilation Rate Mode
+
+
+    DesignSpecification:OutdoorAir,
+      Media_Center Dual Duct Box OA Design Spec,  !- Name
+      Sum,                     !- Outdoor Air Method
+      0.004719,                !- Outdoor Air Flow per Person {m3/s-person}
+      0.00061,                 !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
+      0.0,                     !- Outdoor Air Flow per Zone {m3/s}
+      0.0,                     !- Outdoor Air Flow Air Changes per Hour
+      MinOA_Sched;             !- Outdoor Air Flow Rate Fraction Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-14}
+
+\begin{itemize}
+\item
+  Output:Variable,*,Zone Air Terminal Outdoor Air Duct Damper Position,hourly; !- HVAC Average {[]}
+\item
+  Output:Variable,*,Zone Air Terminal Recirculated Air Duct Damper Position,hourly; !- HVAC Average {[]}
+\item
+  Output:Variable,*,Zone Air Terminal Outdoor Air Fraction,hourly; !- HVAC Average {[]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Zone Air Terminal Outdoor Air Duct Damper Position {[]}}{Zone Air Terminal Outdoor Air Duct Damper Position }}\label{zone-air-terminal-outdoor-air-duct-damper-position}
+
+This output is the damper position of the outdoor air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit outdoor air mass flow rate divided by the terminal unit's maximum outdoor air mass flow rate.~ This output is dimensionless and ranges from 0.0 to 1.0.
+
+\paragraph{\texorpdfstring{Zone Air Terminal Recirculated Air Duct Damper Position {[]}}{Zone Air Terminal Recirculated Air Duct Damper Position }}\label{zone-air-terminal-recirculated-air-duct-damper-position}
+
+This output is the damper position of the recirculated cool air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit cool air mass flow rate divided by the terminal unit's maximum cool air mass flow rate.~ This output is dimensionless and ranges from 0.0 to 1.0.
+
+\paragraph{\texorpdfstring{Zone Air Terminal Outdoor Air Fraction {[]}}{Zone Air Terminal Outdoor Air Fraction }}\label{zone-air-terminal-outdoor-air-fraction}
+
+This output is the current fraction of outdoor air contained in the combined flow of aire entering the zone from the terminal unit. This is the average value over the frequency being reported. The outdoor air fraction is defined as the terminal unit outdoor air mass flow rate divided by the total air mass flow rate.~ This output is dimensionless and ranges from 0.0 to 1.0.
diff --git a/doc/input-output-reference/src/overview/group-air-distribution.tex b/doc/input-output-reference/src/overview/group-air-distribution.tex
new file mode 100644
index 00000000000..bfd560a3535
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+++ b/doc/input-output-reference/src/overview/group-air-distribution.tex
@@ -0,0 +1,853 @@
+\section{Group -- Air Distribution}\label{group-air-distribution}
+
+\subsection{AirLoopHVAC}\label{airloophvac}
+
+Air loops along with zone equipment form the entire forced air heating and cooling system (air side). The main statement for defining an air loop is the \emph{AirLoopHVAC} object described here. As with the main plant and condenser statements, several of the items in the AirLoopHVAC object definition are actually names that refer to other objects in the input file. After the AirLoopHVAC object name, four such list pointers are encountered: for controllers, system availability, branches, and connectors. The Controller List defines how the air loop will respond due to various inputs (control signals). The Availability Manager List refers to methods for controlling when a system is operational. This may be as simple as a schedule to define when the system is shutdown. The Branch List lists the branches that comprise the primary air system. Finally, the Connector List lists the connections between the branches. The branches and connections together define the primary air system topology.
+
+The only numeric input is the design primary air flow rate. This item is input just before the BranchList name.
+
+The next series of names refer to nodes for the various inlet and outlet points of the air loop. The air loop starts where the zone equipment ends. This is a single point consisting of the return air duct once all of the zone return air streams have been collected. While in reality, there is really only one point, for clarity within the simulation components and consistency with the other HVAC loop sections, this point in the systems is defined as two points: one that resides with the zone equipment simulation and one that is acted upon by the air loop simulation. Both node names must be entered into the input file, and both nodes must have unique names. Similarly, the end points of the air loop that also correspond to the beginning points of the zone equipment loop must also be defined. These consist of names referencing lists of up to three pairs of node names as shown below. Up to three air loop outlets are allowed to accommodate the simulation of three deck systems.
+
+\subsubsection{Inputs}\label{inputs-002}
+
+\paragraph{Field: Name}\label{field-name-002}
+
+This field is a unique, user assigned name for a single instance of an AirLoopHVAC object. Any other object referencing this AirLoopHVAC will use this name.
+
+\paragraph{Field: Controller List Name}\label{field-controller-list-name}
+
+This field is the name of a ControllerList object. A Controller List is simply a list of controllers giving both controller name and type. This Controller List specifies all the controllers that will act on this primary air loop. The order of the controllers in the list is significant: controllers are simulated sequentially in the order given in the Controller List.
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name}
+
+This field is the name of a AvailabilityManagerList object. A Availability Manager List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this primary air loop. That is, they determine when and if this air loop is on or off, overriding the control provided by the central fan on/off schedule.
+
+\paragraph{Field: Design Supply Air Flow Rate}\label{field-design-supply-air-flow-rate}
+
+This is the system primary air design volumetric flow rate in cubic meters per second.
+
+\paragraph{Field: Branch List Name}\label{field-branch-list-name}
+
+This field is the object name of a BranchList object (see BranchList and Branch). The BranchList named here specifies all the branches composing the primary air system. These branches, together with the Connectors listed in the ConnectorList, define the primary air system topology.
+
+\paragraph{Field: Connector List Name}\label{field-connector-list-name}
+
+This field is the name of ConnectorList object. This ConnectorList object lists all the Connectors (by type and name) that are included in this primary air system. These Connectors, together with the Branches in the BranchList, define the topology of the primary air system.
+
+\paragraph{Field: Supply Side Inlet Node Name}\label{field-supply-side-inlet-node-name}
+
+The name of the air entrance node of this primary air system. This is the inlet node for return air for this air system.
+
+\paragraph{Field: Demand Side Outlet Node Name}\label{field-demand-side-outlet-node-name}
+
+The name of the air outlet node for the zone equipment group (ZoneHVAC:EquipmentConnections objects) attached to the primary air system. This should be the outlet node of a AirLoopHVAC:ZoneMixer in the AirLoopHVAC:ReturnPath for the zone equipment group attached to this primary air system.
+
+\paragraph{Field: Demand Side Inlet Node Names}\label{field-demand-side-inlet-node-names}
+
+This field can be the name of a node which is the air inlet node for the zone equipment group (see ZoneHVAC:EquipmentConnections objects) attached to this primary air system. Or, this field can be the name of a node list containing one or more nodes (up to 3). These nodes should be the inlet nodes to the AirLoopHVAC:ZoneSplitter or AirLoopHVAC:SupplyPlenum in each of the AirLoopHVAC:SupplyPaths for the zone equipment groups attached to this primary air system. For single duct systems, there is only one node name in this list. For two and three duct systems, the order of the nodes in this list must correspond with the order of the nodes in the Supply Side Outlet Node Names list.
+
+\paragraph{Field: Supply Side Outlet Node Names}\label{field-supply-side-outlet-node-names}
+
+This field can be the name of a node which is the air outlet node for each supply duct of this primary air system. Or, this field can be the name of a node list containing one or more nodes (up to 3). The list can contain the names of up to three nodes. For single duct systems, there is only one node name in this list. For two and three duct systems, the order of the nodes in this list must correspond with the order of the nodes in the Demand Side Inlet Node Names list.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+AirLoopHVAC,
+    Main Dual Duct Air Loop,           ! Primary Air Loop Name
+    Dual Duct System 1 Controllers,    ! Controller List
+    Dual Duct System 1 Schedule List , ! System Availability Manager List
+    1.3 ,                              ! Primary air design volumetric flow rate
+    Dual Duct Air Loop Branches ,      ! Air Loop Branch List Name
+    Dual Duct Connectors ,             ! Air Loop Connector List Name
+    Supply Fan Inlet Node ,            ! ReturnAir AirLoop Inlet Node
+    Return Air Mixer Outlet ,          ! ZoneEquipGroup Outlet Node
+    Zone Equipment Inlet Node List ,   ! SupplyAirPath ZoneEquipGroup Inlet Nodes
+    Air Loop Outlet Node List ;        ! AirLoop Outlet Nodes
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-001}
+
+\begin{itemize}
+\item
+  HVAC,Average,Air System Simulation Cycle On Off Status
+\item
+  HVAC,Sum,HVAC System Solver Iteration Count {[]}
+\item
+  HVAC,Sum,Air System Solver Iteration Count {[]}
+\item
+  HVAC,Sum,Air System Simulation Maximum Iteration Count {[]}
+\item
+  HVAC,Sum,Air System Simulation Iteration Count {[]}
+\item
+  HVAC,Sum,Air System Component Model Simulation Calls {[]}
+\end{itemize}
+
+\paragraph{Air System Simulation Cycle On Off Status}\label{air-system-simulation-cycle-on-off-status}
+
+This field is the availability status of an AirLoopHVAC. This status flag is a result of the calculations made by the System Availability Manager(s) listed in a System Availability Manager List. When a single availability manager is used in a System Availability Manager List, this is also the availability status reported by the specific availability manager (Ref. System Availability Manager Outputs). When multiple availability managers are used in a System Availability Manager List, the loop availability status is determine by the rules associated with AirLoopHVACs (see rules described for Group -- System Availability Managers). The control status outputs are represented using integers 0 through 3.. These integers represent \emph{NoAction} (0), \emph{ForceOff} (1), \emph{CycleOn} (2), and \emph{CycleOnZoneFansOnly} (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\paragraph{\texorpdfstring{HVAC System Solver Iteration Count {[]}}{HVAC System Solver Iteration Count }}\label{hvac-system-solver-iteration-count}
+
+\paragraph{\texorpdfstring{Air System Solver Iteration Count {[]}}{Air System Solver Iteration Count }}\label{air-system-solver-iteration-count}
+
+\paragraph{\texorpdfstring{Air System Simulation Maximum Iteration Count {[]}}{Air System Simulation Maximum Iteration Count }}\label{air-system-simulation-maximum-iteration-count}
+
+\paragraph{\texorpdfstring{Air System Simulation Iteration Count {[]}}{Air System Simulation Iteration Count }}\label{air-system-simulation-iteration-count}
+
+\paragraph{\texorpdfstring{Air System Component Model Simulation Calls {[]}}{Air System Component Model Simulation Calls }}\label{air-system-component-model-simulation-calls}
+
+These variables are simply counters of how many iterations were executed. The count for any given HVAC time step will be the iterations executed before convergence was achieved, or the max allowed in which case the simulation throws a warning and proceeds to the next time step.
+
+\subsubsection{Outputs}\label{outputs-1-001}
+
+This section provides more detailed information on the reporting available for outdoor air ventilation.~ Sixteen cooling and heating load variables and eight energy summary variables are available that report the impact of system outdoor air on zone loads, system demand and total energy use. The representative air system shown in the diagram below shows outdoor air (OA), return air (RA), supply air (SA) and mixed air (MA).
+
+\begin{figure}[hbtp] % fig 90
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image209.png}
+\caption{Example System for Ventilation Loads Report \protect \label{fig:example-system-for-ventilation-loads-report}}
+\end{figure}
+
+The overall effect of outdoor air on the system shown above can be summarized by considering the mixing box. In this system, part or all of the return air is replaced by outdoor air. The presence of any heat recovery will already be taken into account and thus will automatically be accounted for by using the outdoor air inlet conditions to the mixing box (point OA in the diagram) rather than actual outdoor air conditions. Thus, the overall energy impact of outdoor air (ventilation) on a particular system can be evaluated by multiplying the outdoor air mass flow rate by the enthalpy difference between the outdoor air entering the mixing box (OA) and the return air entering the mixing box (RA') as shown in the following equation.
+
+\begin{equation}
+{\dot q_{OA}} = {\dot m_{OA}}\left( {{h_{OA}} - {h_{RA'}}} \right) = {\dot m_{sys}}\left( {{h_{MA}} - {h_{RA'}}} \right)
+\end{equation}
+
+\paragraph{Ventilation Flow Outputs}\label{ventilation-flow-outputs}
+
+The fresh air flow into each zones are reported using the ventilation flow output variables. The total outdoor air flow in a primary air system is divided to each zone based on the fraction of flow each zone is supplied. There are six variables which deals with the mechanical ventilation flow reporting. Those six variables are:
+
+\paragraph{Zone Mechanical Ventilation Mass Flow Rate {[}kg/s{]}}\label{zone-mechanical-ventilation-mass-flow-rate-kgs}
+
+Reports the average outdoor air mass flow rate to any zone over the reporting interval.
+
+\paragraph{Zone Mechanical Ventilation Mass {[}kg{]}}\label{zone-mechanical-ventilation-mass-kg}
+
+Reports the total outdoor air mass that has been supplied to any zone over the reporting interval.
+
+\paragraph{Zone Mechanical Ventilation Standard Density Volume Flow Rate {[}m3/s{]}}\label{zone-mechanical-ventilation-standard-density-volume-flow-rate-m3s}
+
+Reports the average outdoor air volume flow rate to any zone over the reporting interval, calculated using a standard density for air.~ Standard density in EnergyPlus corresponds to 20ºC drybulb, dry air, and nominally adjusted for elevation.
+
+\paragraph{Zone Mechanical Ventilation Standard Density Volume {[}m3{]}}\label{zone-mechanical-ventilation-standard-density-volume-m3}
+
+Reports the total outdoor air volume that has been supplied to a zone over the reporting interval, calculated using a standard density for air.~ Standard density in EnergyPlus corresponds to 20ºC drybulb, dry air, and nominally adjusted for elevation.
+
+\paragraph{Zone Mechanical Ventilation Current Density Volume Flow Rate {[}m3/s{]}}\label{zone-mechanical-ventilation-current-density-volume-flow-rate-m3s}
+
+Reports the average outdoor air volume flow rate to any zone over the reporting interval, calculated using the current density for zone air.
+
+\paragraph{Zone Mechanical Ventilation Current Density Volume {[}m3{]}}\label{zone-mechanical-ventilation-current-density-volume-m3}
+
+Reports the total outdoor air volume that has been supplied to a zone over the reporting interval, calculated using the current density for zone air.
+
+\paragraph{Zone Mechanical Ventilation Air Changes per Hour {[}ach{]}}\label{zone-mechanical-ventilation-air-changes-per-hour-ach}
+
+Reports the air changes per hour in the zone due to the outside fresh air supplied by mechanical ventilation system.
+
+The example syntax below shows the basic ventilation flow variables reported on an hourly basis.
+
+\begin{itemize}
+\item
+  Output:Variable,*,Zone Mechanical Ventilation Mass Flow Rate,Hourly;
+\item
+  Output:Variable,*,Zone Mechanical Ventilation Mass,Hourly;
+\item
+  Output:Variable,*,Zone Mechanical Ventilation Standard Density Volume Flow Rate,Hourly;
+\item
+  Output:Variable,*,Zone Mechanical Ventilation Standard Density Volume,Hourly;
+\item
+  Output:Variable,*,Zone Mechanical Ventilation Current Density Volume Flow Rate,Hourly;
+\item
+  Output:Variable,*,Zone Mechanical Ventilation Current Density Volume,Hourly;
+\item
+  Output:Variable,*, Zone Mechanical Ventilation Air Changes per Hour,Hourly;
+\end{itemize}
+
+\paragraph{Ventilation Load Reports}\label{ventilation-load-reports}
+
+The impact of system outdoor air on a particular zone may be calculated by summing the mass flow weighted \({\dot q_{OA}}\) ~over the supply air paths (both cooling and heating) serving the zone as follows:
+
+\begin{equation}
+{\dot q_{OA,Zone\;1}} = \sum\limits_{n = 1}^{AirPathNum} {{{\dot q}_{OA}}\frac{{{{\dot m}_n}}}{{{{\dot m}_{sys}}}}}
+\end{equation}
+
+Four output variables each for cooling and heating report the impact of the ventilation air on the zone load in the absence of ventilation air system interactions. The ventilation load output variables are:
+
+\paragraph{Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy {[}J{]}}\label{zone-mechanical-ventilation-cooling-load-increase-due-to-overheating-energy-j}
+
+\paragraph{Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy {[}J{]}}\label{zone-mechanical-ventilation-heating-load-increase-due-to-overcooling-energy-j}
+
+The cooling/heating load that would occur once ventilation air met the zone cooling/heating load and continued to overcool/overheat the zone. No system effects are accounted for.
+
+\paragraph{Zone Mechanical Ventilation Cooling Load Decrease Energy {[}J{]}}\label{zone-mechanical-ventilation-cooling-load-decrease-energy-j}
+
+\paragraph{Zone Mechanical Ventilation Heating~ Load Decrease{[}J{]}}\label{zone-mechanical-ventilation-heating-load-decreasej}
+
+The decrease in zone cooling/heating load that would occur as a result of ventilation air introduced directly into the zone. No system effects are accounted for.
+
+\paragraph{Zone Mechanical Ventilation No Load Heat Removal Energy {[}J{]}}\label{zone-mechanical-ventilation-no-load-heat-removal-energy-j}
+
+\paragraph{Zone Mechanical Ventilation No Load Heat Addition Energy {[}J{]}}\label{zone-mechanical-ventilation-no-load-heat-addition-energy-j}
+
+The addition or removal of heat to a zone with no load. The heat addition or removal is due to mechanical ventilation while the zone thermostat is in the deadband.
+
+To summarize:
+
+\textbf{Cooling:}
+
+\textbf{\emph{1.~~~~Zone Mechanical Ventilation No Load Heat Removal Energy {[}J{]}}}
+
+Cooling that would be provided directly to zone by ventilation air. Ventilation occurred with no zone load.
+
+\textbf{\emph{2.~~~~Zone Mechanical Ventilation Cooling Load Increase Energy {[}J{]}}}
+
+The increase in zone cooling load that would occur as a result of ventilation air introduced directly into the zone. No system effects are accounted for.
+
+\textbf{\emph{3.~~~~Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy {[}J{]}}}
+
+The cooling load that would occur once ventilation air met the zone heating load and continued to overheat the zone. No system effects are accounted for.
+
+\textbf{\emph{4.~~~~Zone Mechanical Ventilation Cooling Load Decrease Energy {[}J{]}}}
+
+The decrease in zone cooling load that would occur as a result of ventilation air introduced directly into the zone. No system effects are accounted for.
+
+\textbf{Heating:}
+
+\textbf{\emph{1.~~~~Zone Mechanical Ventilation No Load Heat Addition Energy {[}J{]}}}
+
+Heating that would be provided directly to zone by ventilation air. Ventilation occurred with no zone load.
+
+\textbf{\emph{2.~~~~Zone Mechanical Ventilation Heating Load Increase Energy {[}J{]}}}
+
+The increase in zone heating load that would occur as a result of ventilation air introduced directly into the zone. No system effects are accounted for.
+
+\textbf{\emph{3.~~~~Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy {[}J{]}}}
+
+The heating load that would occur once ventilation air met the zone cooling load and continued to overcool the zone. No system effects are accounted for.
+
+\textbf{\emph{4.~~~~Zone Mechanical Ventilation Heating Load Decrease Energy {[}J{]}}}
+
+The decrease in zone heating load that would occur as a result of ventilation air introduced directly into the zone. No system effects are accounted for.
+
+The output variables are calculated by comparing the zone ventilation load with the zone cooling or heating load.~ `Ventilation cooling' decreases the zone cooling load until the cooling load has been eliminated. The remaining `ventilation cooling' is reported as `overcooling'. `Overheating' is calculated in the same manner. The actual system operation, which determines whether or not an `overcooling' or `overheating' load actually results in increased energy consumption, is not considered in the calculation of these output variables.
+
+The ventilation zone load output variables are shown in Table~\ref{table:ventilation-load-output-variables}. The variables report the maximum potential ``cost'' or ``benefit'' of ventilation air introduced directly into the zone.
+
+% table 24
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Ventilation Load Output Variables \label{table:ventilation-load-output-variables}} \tabularnewline
+\toprule 
+ & No Zone Load & Zone Cooling Load & Zone Heating Load \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Ventilation Load Output Variables} \tabularnewline
+\toprule 
+ & No Zone Load & Zone Cooling Load & Zone Heating Load \tabularnewline
+\midrule
+\endhead
+
+Ventilation Cooling & Zone Mechanical Ventilation No Load Heat Removal Energy & Zone Mechanical Ventilation Cooling Load Decrease Energy & Zone Mechanical Ventilation Heating Load Increase Energy \tabularnewline
+Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy \tabularnewline
+Ventilation Heating & Zone Mechanical Ventilation No Load Heat Addition Energy & Zone Mechanical Ventilation Cooling Load Increase Energy & Zone Mechanical Ventilation Heating Load Decrease Energy \tabularnewline
+Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy \tabularnewline
+\bottomrule
+\end{longtable}
+
+The example syntax below shows the basic ventilation load variables reported on a monthly basis.
+
+\begin{itemize}
+\item
+  ~ Output:Variable,*,Zone Mechanical Ventilation Heating Load Increase Energy,monthly;
+\item
+  ~ Output:Variable,*,Zone Mechanical Ventilation Heating Load Decrease Energy,monthly;
+\item
+  ~ Output:Variable,*,Zone Mechanical Ventilation No Load Heat Addition Energy,monthly;
+\item
+  ~ Output:Variable,*,Zone Mechanical Ventilation Cooling Load Increase Energy,monthly;
+\item
+  ~ Output:Variable,*,Zone Mechanical Ventilation Cooling Load Decrease Energy,monthly;
+\item
+  ~ Output:Variable,*,Zone Mechanical Ventilation No Load Heat Removal Energy,monthly;
+\end{itemize}
+
+Reporting on a timestep or hourly level would produce a detailed report with variables intermingled with the other output variables that might be requested in the input file.
+
+Another method will more easily encapsulate the report:
+
+\begin{lstlisting}
+
+OutputControl:Table:Style, HTML;     !- ColumnSeparator
+
+
+  Output:Table:Monthly,
+    Ventilation Loads,       !- Name
+    ,                        !- DigitsAfterDecimal
+  Zone Mechanical Ventilation No Load Heat Removal Energy,
+           SumOrAverage,
+  Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy,
+           SumOrAverage,
+  Zone Mechanical Ventilation Cooling Load Decrease Energy,
+           SumOrAverage,
+  Zone Mechanical Ventilation Cooling Load Increase Energy,
+           SumOrAverage,
+  Zone Mechanical Ventilation No Load Heat Addition Energy,
+           SumOrAverage,
+  Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy,
+           SumOrAverage,
+  Zone Mechanical Ventilation Heating Load Decrease Energy,
+           SumOrAverage,
+  Zone Mechanical Ventilation Heating Load Increase Energy,
+           SumOrAverage;
+\end{lstlisting}
+
+This combination will report the ventilation loads on a monthly basis in a HTML style report that can be easily read in a web browser. Review the Output:Table:Monthly object for other methods of display or further options on this report item.
+
+\subsection{Systems Level Reporting}\label{systems-level-reporting}
+
+Most output variables are a single entity reporting. Meters are a combination of like variables -- specifically for Energy Consumption. This section introduces a slightly different concept -- where output variables described herein are a combination of several similar items -- specifically targeted at HVAC/System level reporting. This reporting is coupled with an Air Loop (ref: AirLoopHVAC)
+
+All items shown in this section are typical ``output variables'' and can be reported with the Output:Variable object.
+
+Or, as is shown by example here, perhaps a more readable form is to generate them in Tabular Form with the ``Output:Table:Monthly'' object.
+
+\begin{figure}[hbtp] % fig 91
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image213.png}
+\caption{View of System Level Reporting \protect \label{fig:view-of-system-level-reporting}}
+\end{figure}
+
+\subsection{System Loads Outputs}\label{system-loads-outputs}
+
+In this category, the total system load is reported. Two aspects are reported here: Heating and Cooling. The following two variables report the heat energy that system components (including packaged equipment, fans, main coils, reheat coils, humidifiers, desiccant dehumidifiers, evaporative coolers and heat exchangers) add or remove from the air loop. Each variable within these grouping wil
+
+\subsubsection{Air System Total Heating Energy}\label{air-system-total-heating-energy}
+
+Heat Addition to the Air Loop (Sum of all components) in Joules
+
+\subsubsection{Air System Total Cooling Energy}\label{air-system-total-cooling-energy}
+
+Heat Removal from the Air Loop (Sum of all components) in Joules
+
+In `Output:Table:Monthly' format shown below.
+
+\begin{lstlisting}
+
+  OutputControl:Table:Style,HTML;
+
+    Output:Table:Monthly,
+      System Loads,       !- Name
+      ,                        !- DigitsAfterDecimal
+      Air System Total Heating Energy,  SumOrAverage,
+      Air System Total Cooling Energy,  SumOrAverage;
+\end{lstlisting}
+
+\subsection{System Energy Use Outputs}\label{system-energy-use-outputs}
+
+System Energy Use consists of six output variables that report the total energy (in Joules) and water consumption (in m\(^{3}\)) for all system components and including packaged equipment, fans, main coils, reheat coils, humidifiers, desiccant dehumidifiers, and evaporative coolers. The output variables shown below show hot and cold water, steam, electric and gas energy. Hot and cold water energy includes all `district cooling' and `district heating' energy.
+
+\subsubsection{Air System Hot Water Energy}\label{air-system-hot-water-energy}
+
+Hot Water Consumption for the system (Joules).
+
+\subsubsection{Air System Steam Energy}\label{air-system-steam-energy}
+
+Steam Consumption for the system (Joules).
+
+\subsubsection{Air System Chilled Water Energy}\label{air-system-chilled-water-energy}
+
+Chilled Water Consumption for the system (Joules).
+
+\subsubsection{Air System Electric Energy}\label{air-system-electric-energy}
+
+Electric Consumption for the system (Joules).
+
+\subsubsection{Air System Gas Energy}\label{air-system-gas-energy}
+
+Gas (Natural Gas and Propane) Consumption for the system (Joules).
+
+\subsubsection{Air System Water Volume}\label{air-system-water-volume}
+
+Water Consumption for the system (humidifiers and evaporative coolers) (m3).
+
+The Standard reports file includes these variables reporting in the Tabular report form as ``Air Loop System Energy and Water Use''.
+
+\begin{lstlisting}
+
+  OutputControl:Table:Style,HTML;
+
+    Output:Table:Monthly,
+      Air Loop System Energy and Water Use,       !- Name
+      ,                        !- DigitsAfterDecimal
+      Air System Hot Water Energy ,  SumOrAverage,
+      Air System Steam Energy ,  SumOrAverage,
+      Air System Chilled Water Energy,  SumOrAverage,
+      Air System Electric Energy,  SumOrAverage,
+      Air System Gas Energy,  SumOrAverage,
+      Air System Water Volume,  SumOrAverage;
+\end{lstlisting}
+
+\subsection{System Component Loads Outputs}\label{system-component-loads-outputs}
+
+Reporting System Component Loads shows the energy transferred to or extracted from the air loop by system component type. Fans, Cooling Coils, Heating Coils, Heat exchangers, humidifiers, evaporative coolers, and desiccant dehumidifiers show heat transfer rates in Joules. The components may be located in outdoor air systems bundled with packaged equipment or specified as stand-alone components. The reporting accounts for both main branch and reheat coils.
+
+The Standard reports file includes these variables reporting in the Tabular report form as ``Air Loop System Component Loads''.
+
+\begin{lstlisting}
+
+  OutputControl:Table:Style,HTML;
+
+
+    Output:Table:Monthly,
+      Air Loop System Component Loads,       !- Name
+      ,                        !- DigitsAfterDecimal
+      Air System Fan Air Heating Energy,  SumOrAverage,
+      Air System Cooling Coil Total Cooling Energy,  SumOrAverage,
+      Air System Heating Coil Total Heating Energy,  SumOrAverage,
+      Air System Heat Exchanger Total Heating Energy,  SumOrAverage,
+      Air System Heat Exchanger Total Cooling Energy,  SumOrAverage,
+      Air System Humidifier Total Heating Energy,  SumOrAverage,
+      Air System Evaporative Cooler Total Cooling Energy,  SumOrAverage,
+      Air System Desiccant Dehumidifier Total Cooling Energy,  SumOrAverage;
+\end{lstlisting}
+
+\subsubsection{Air System Fan Air Heating Energy}\label{air-system-fan-air-heating-energy}
+
+Energy added to the air loop by Fans (Joules)
+
+\subsubsection{Air System Cooling Coil Total Cooling Energy}\label{air-system-cooling-coil-total-cooling-energy}
+
+Energy removed from air loop by Cooling Coils (Joules)
+
+\subsubsection{Air System Heating Coil Total Heating Energy}\label{air-system-heating-coil-total-heating-energy}
+
+Energy added to air loop by Heating Coils (Joules)
+
+\subsubsection{Air System Heat Exchanger Total Heating Energy}\label{air-system-heat-exchanger-total-heating-energy}
+
+Energy added to air loop by air-to-air heat recovery heat exchangers (Joules)
+
+\subsubsection{Air System Heat Exchanger Total Cooling Energy}\label{air-system-heat-exchanger-total-cooling-energy}
+
+Energy removed from air loop by air-to-air heat recovery heat exchangers (Joules)
+
+\subsubsection{Air System Humidifier Total Heating Energy}\label{air-system-humidifier-total-heating-energy}
+
+Energy added to air loop by humidifiers (Joules)
+
+\subsubsection{Air System Evaporative Cooler Total Cooling Energy}\label{air-system-evaporative-cooler-total-cooling-energy}
+
+Energy removed from air loop by evaporative coolers (Joules)
+
+\subsubsection{Air System Desiccant Dehumidifier Total Cooling Energy}\label{air-system-desiccant-dehumidifier-total-cooling-energy}
+
+Energy removed from air loop by desiccant dehumidifiers (Joules)
+
+\subsubsection{Air System Solar Collector Total Heating Energy}\label{air-system-solar-collector-total-heating-energy}
+
+Energy added to air loop by solar collectors (Joules)
+
+\subsubsection{Air System Solar Collector Total Cooling Energy}\label{air-system-solar-collector-total-cooling-energy}
+
+Energy removed from air loop by solar collectors (Joules)
+
+\subsubsection{Air System User Defined Air Terminal Total Heating Energy}\label{air-system-user-defined-air-terminal-total-heating-energy}
+
+Energy added to air loop by user defined air terminal units (Joules)
+
+\subsubsection{Air System User Defined Air Terminal Total Cooling Energy}\label{air-system-user-defined-air-terminal-total-cooling-energy}
+
+Energy removed from air loop by user defined air terminal units (Joules)
+
+\subsection{System Component Energy Use Outputs}\label{system-component-energy-use-outputs}
+
+Reporting System Component Energy Use consists of eleven output variables that report the total energy consumption (in Joules) of system components by energy type and coil type. Electric energy consumption is reported for fans, heating and cooling coils in packaged (DX) systems, electric resistance heating coils, humidifiers, evaporative coolers and desiccant dehumidifiers.
+
+\subsubsection{Air System Fan Electric Energy}\label{air-system-fan-electric-energy}
+
+Electric consumption for fans. (Joules)
+
+\subsubsection{Air System Heating Coil Hot Water Energy}\label{air-system-heating-coil-hot-water-energy}
+
+Consumption for heating coil hot water (both purchased and plant supplied) (Joules)
+
+\subsubsection{Air System Cooling Coil Chilled Water Energy}\label{air-system-cooling-coil-chilled-water-energy}
+
+Consumption for cooling coil chilled water (both purchased and plant supplied) (Joules)
+
+\subsubsection{Air System DX Heating Coil Electric Energy}\label{air-system-dx-heating-coil-electric-energy}
+
+Compressor plus condenser fan electricity use. (Joules)
+
+\subsubsection{Air System DX Cooling Coil Electric Energy}\label{air-system-dx-cooling-coil-electric-energy}
+
+Compressor plus condenser fan electricity use. (Joules)
+
+\subsubsection{Air System Heating Coil Electric Energy}\label{air-system-heating-coil-electric-energy}
+
+Electricity consumption for the heating coil. (Joules)
+
+\subsubsection{Air System Heating Coil Gas Energy}\label{air-system-heating-coil-gas-energy}
+
+Gas (Propane and Natural Gas) consumption for the heating coil. (Joules)
+
+\subsubsection{Air System Heating Coil Steam Energy}\label{air-system-heating-coil-steam-energy}
+
+Steam consumption for the heating coil (steam coils). (Joules)
+
+\subsubsection{Air System Humidifier Electric Energy}\label{air-system-humidifier-electric-energy}
+
+Electricity consumption for the humidifiers. (Joules)
+
+\subsubsection{Air System Evaporative Cooler Electric Energy}\label{air-system-evaporative-cooler-electric-energy}
+
+Electricity consumption for the evaporative coolers. (Joules)
+
+\subsubsection{Air System Desiccant Dehumidifier Electric Energy}\label{air-system-desiccant-dehumidifier-electric-energy}
+
+Electricity consumption for the desiccant dehumidifiers. (Joules)
+
+The Standard reports file includes these variables reporting in the Tabular report form as ``Air Loop System Component Energy Use''.
+
+\begin{lstlisting}
+
+  OutputControl:Table:Style,HTML;
+
+
+    Output:Table:Monthly,
+      Air Loop System Component Energy Use,       !- Name
+      ,                        !- DigitsAfterDecimal
+      Air System Fan Electric Energy,  SumOrAverage,
+      Air System Heating Coil Hot Water Energy,  SumOrAverage,
+      Air System Cooling Coil Chilled Water Energy,  SumOrAverage,
+      Air System DX Heating Coil Electric Energy,  SumOrAverage,
+      Air System DX Cooling Coil Electric Energy,  SumOrAverage,
+      Air System Heating Coil Electric Energy,  SumOrAverage,
+      Air System Heating Coil Gas Energy,  SumOrAverage,
+      Air System Heating Coil Steam Energy,  SumOrAverage,
+      Air System Humidifier Electric Energy,  SumOrAverage,
+      Air System Evaporative Cooler Electric Energy,  SumOrAverage,
+      Air System Desiccant Dehumidifier Electric Energy,  SumOrAverage;
+\end{lstlisting}
+
+\subsection{Overall Air Loop Syntax}\label{overall-air-loop-syntax}
+
+A map for Air Loop input syntax is shown in the following diagram.
+
+\begin{figure}[hbtp] % fig 92
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image214.png}
+\caption{Air Loop Input Syntax Map \protect \label{fig:air-loop-input-syntax-map}}
+\end{figure}
+
+\subsection{AirLoopHVAC:ControllerList}\label{airloophvaccontrollerlist}
+
+The syntax for the AirLoopHVAC:ControllerList definition is shown below. As with other lists in EnergyPlus input, the object title and identifying name are followed by type-name pairs. In this case, the types are controller types. The order in which controllers appear on this list also define the priority as described below. The identifying name refers back to the name recorded in the AirLoopHVAC statement.
+
+\subsubsection{Inputs}\label{inputs-1-002}
+
+\paragraph{Field: Name}\label{field-name-1-001}
+
+The user designated unique name of an instance of a Controller List. Any object referencing this Controller List will do so using this name.
+
+\paragraph{Field Set (Object Type, Controller Name) up to 8}\label{field-set-object-type-controller-name-up-to-8}
+
+After the identifying name, input for the controller list consists of up to 8 pairs of data items: a controller type and a controller name. The first controller listed has the highest priority, the second the second highest priority, and so forth.
+
+\paragraph{Field: Controller \textless{}x\textgreater{} Object Type}\label{field-controller-x-object-type}
+
+The type of~ controller. This should be a key word defining a class of controllers such as Controller:WaterCoil.
+
+\paragraph{Field: Controller \textless{}x\textgreater{} Name}\label{field-controller-x-name}
+
+The name of a controller object (such as a Controller:WaterCoil) defined elsewhere in the input file.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+AirLoopHVAC:ControllerList,
+             Dual Duct System 1 Controllers,
+             Controller:WaterCoil, Main Cooling Coil Controller,
+             Controller:WaterCoil, Main Heating Coil Controller;
+\end{lstlisting}
+
+\subsection{AvailabilityManagerAssignmentList}\label{availabilitymanagerassignmentlist}
+
+The AvailabilityManagerAssignmentList defines the applicable managers used for an AirLoopHVAC or PlantLoop. The priority of availability managers is based on a set of rules and are specific to the type of loop. The output from each Availability Manager is an availability status flag. This flag can have the values \emph{NoAction}, \emph{ForceOff}, \emph{CycleOn}, or \emph{CycleOnZoneFansOnly} (used only for air loops). The availability status flags for the Availability Managers referenced by an air or plant loop are used to set the availability status flag for each loop. For the air loops, \emph{ForceOff} takes precedence: if any of the loop's availability managers are showing status \emph{ForceOff}, the loop status will be \emph{ForceOff}. Next in precedence is \emph{CycleOnZoneFansOnly,} followed by \emph{CycleOn}, and \emph{NoAction}. For the plant loops, there is no precedence among the Availability Manager status flag values. Instead, the first availability manager giving a status flag value other than \emph{NoAction} sets the status for the loop. The Availability Managers are executed in Availability Manager List order.
+
+Special rules also apply for which managers may be listed in a Availability Manager list. The Hybrid Ventilation Control Manager (object: AvailabilityManager:HybridVentilation) is a special type of manager and is never specified in a Availability Manager List (it is used stand-alone for a specific air loop). All other types of availability managers may be listed in the Availability Manager List used for AirLoopHVACs. For Plant Loops, the Night Cycle and Night Ventilation managers (objects: AvailabilityManager:NightCycle ~and AvailabilityManager:NightVentilation) are not allowed in the Availability Manager List.
+
+\subsubsection{Inputs}\label{inputs-2-002}
+
+\paragraph{Field: Name}\label{field-name-2-001}
+
+The name of the AvailabilityManagerAssignmentList ~object. This is referenced by AirLoopHVAC and PlantLoop objects.
+
+\paragraph{Field Set (Availability Manager Object Type, Name)}\label{field-set-availability-manager-object-type-name}
+
+Managers are listed by pairs of data items:~ \emph{Availability Manager Object Type} and \emph{Availability Manager Name}. The managers are simulated down the list and calculate a control status for use by the AirLoopHVAC or PlantLoop. The priority of each manager used for a specific loop is based on the rules described above. Availability managers are not currently used for condenser loops. The availability managers, along with the AirLoopHVAC and PlantLoop object, report the control status calculated each simulation timestep. These output variables can be used to prioritize the managers according to the required control strategy. Six managers are accomodated in the list by default, however, this IDD specification is extensible. Additional pairs may be added by directly editing the IDD.
+
+\paragraph{Field: Availability Manager \textless{}x\textgreater{} Object Type}\label{field-availability-manager-x-object-type}
+
+The key word defining the type of manager, e.g.~AvailabilityManager:NightCycle.
+
+\paragraph{Field: Availability Manager\textless{}x\textgreater{}~ Name}\label{field-availability-managerx-name}
+
+The name of a AvailabilityManager object defined elsewhere in the input file.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+AvailabilityManagerAssignmentList,
+    Collector Loop Availability Manager List,  !- Name
+    AvailabilityManager:HighTemperatureTurnOff,    !- System Availability Manager Type 1
+    High Temperature Turn Off Availability Manager,  !- System Availability Manager Name 1
+    AvailabilityManager:LowTemperatureTurnOn ,     !- System Availability Manager Type 2
+    Low Temperature Turn On Availability Manager,  !- System Availability Manager Name 2
+    AvailabilityManager:DifferentialThermostat,    !- System Availability Manager Type 3
+    Differential Thermostat Availability Manager;  !- System Availability Manager Name 3
+\end{lstlisting}
+
+\subsection{AirLoopHVAC:OutdoorAirSystem}\label{airloophvacoutdoorairsystem}
+
+The Outside Air System (object AirLoopHVAC:OutdoorAirSystem) is a subsystem of an AirLoopHVAC. It handles the mixed air portion of the primary air system: the system relief air, the outside air inlet, and any components and controllers associated with the system relief air and outside air streams. From the perspective of the primary air loop the Outside Air System is treated as a single component. As a subsystem, it can contain one or more components and controllers.
+
+The input for the Outside Air System consists of a system name, a controller list name, an equipment list name, and an availability manager list name. The controller list simply lists, by type and unique name, all the controllers in the subsystem. The controllers will be simulated in list order. The equipment list lists all the components in the subsystem, by type and name. The equipment is simulated in list order. Finally, the availability manager list gives the type and name of the availability managers used by the subsystem.
+
+The equipment inlet/outlet must be sequential with no loops - the simulation can only handle a straight-through air path, both on the primary air side and on the secondary air side, if any. Heat exchanger secondary air inlets need to be independent of the primary air stream -- usually relief air is used.
+
+\subsubsection{Inputs}\label{inputs-3-001}
+
+\paragraph{Field: Name}\label{field-name-3-001}
+
+The unique, user assigned name for a single instance of an Outside Air System. Any other object referencing this Outside Air System will use this name.
+
+\paragraph{Field: Name: Controller List Name}\label{field-name-controller-list-name}
+
+This field is the name of a AirLoopHVAC:ControllerList object. A AirLoopHVAC:ControllerList is simply a list of controllers giving both controller name and type. This Controller List specifies all the controllers that will act on this outside air system. The order of the controllers in the list is significant: controllers are simulated sequentially in the order given in the Controller List. Typically the Controller List would contain a Controller:OutdoorAir. If there are chilled water or hot water coils in the outdoor air system, each such coil will need a Controller:WaterCoil.
+
+\paragraph{Field: Outdoor Air Equipment List Name}\label{field-outdoor-air-equipment-list-name}
+
+This field is the name of an AirLoopHVAC:OutdoorAirSystem:EquipmentList object. An AirLoopHVAC:OutdoorAirSystem:EquipmentList is simply a list of components giving both component name and type. This Outdoor Air Equipment List specifies all the components that will be simulated in this outside air system. The order of the components in the list is significant: components are simulated sequentially in the order given in the Outdoor Air Equipment List. Typically the equipment list would contain at least an OutdoorAir:Mixer. If there is more than one component, the components must be listed in order from the outside air to the OutdoorAir:Mixer (the OutdoorAir:Mixer is last).
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-1}
+
+This field is the name of a AvailabilityManagerAssignmentList object. An Availability Manager List is a list of Availability Managers giving both Availability Manager Object Type and Name. \textbf{Use of this input is optional.} This field may be omitted; it is not currently used by the program.
+
+An IDF example, including the AirLoopHVAC, and the controller and equipment lists.
+
+\begin{lstlisting}
+
+AirLoopHVAC,Typical Terminal Reheat 1,
+             Reheat System 1 Controllers,
+             Reheat System 1 Avail List,
+             1.3,
+             Air Loop Branches,,
+             Air Loop Inlet Node, Return Air Mixer Outlet,
+             Zone Equipment Inlet Node, Air Loop Outlet Node;
+
+  AirLoopHVAC:ControllerList,
+             Reheat System 1 Controllers,
+             Controller:WaterCoil, Main Cooling Coil Controller;
+
+  BranchList, Air Loop Branches,
+             Air Loop Main Branch;
+
+  Branch, Air Loop Main Branch,
+             1.3,
+             ,
+             AirLoopHVAC:OutdoorAirSystem, OA Sys 1,
+             Air Loop Inlet Node, Mixed Air Node,PASSIVE
+             Fan:ConstantVolume, Supply Fan 1,
+             Mixed Air Node, Cooling Coil Air Inlet Node, ACTIVE,
+             Coil:Cooling:Water:DetailedGeometry, Detailed Cooling Coil,
+             Cooling Coil Air Inlet Node, Air Loop Outlet Node, PASSIVE;
+
+  AvailabilityManagerAssignmentList, Reheat System 1 Avail List,
+             AvailabilityManager:Scheduled, Reheat System 1 Avail;
+
+  AvailabilityManager:Scheduled, Reheat System 1 Avail,
+             FanAndCoilAvailSched;
+
+  AirLoopHVAC:OutdoorAirSystem,
+             OA Sys 1,
+             OA Sys 1 Controllers,
+             OA Sys 1 Equipment;
+
+  AirLoopHVAC:ControllerList,
+             OA Sys 1 Controllers,
+             Controller:OutdoorAir, OA Controller 1;
+
+  AirLoopHVAC:OutdoorAirSystem:EquipmentList,
+             OA Sys 1 Equipment,
+             HeatExchanger:AirToAir:FlatPlate,OA Heat Recovery 1,
+             OutdoorAir:Mixer, OA Mixing Box 1;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-001}
+
+The impact of using outside air/mechanical ventilation is described in the section: Outdoor Air Ventilation Outputs.
+
+\subsection{AirLoopHVAC:OutdoorAirSystem:EquipmentList}\label{airloophvacoutdoorairsystemequipmentlist}
+
+Used to specify the components in the outdoor air system. The components will be simulated in the order in which they occur in the list.
+
+The following HVAC equipment types are allowed as outdoor air system equipment. The component matrix shows which coils and fans are allowed with which equipment models.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/OASysComponentMatrix.png}
+\caption{}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-4-001}
+
+\paragraph{Field: Name}\label{field-name-4-001}
+
+The user designated unique name of an instance of an Air Loop Equipment List. Any object referencing this Air Loop Equipment List will do so using this name.
+
+\paragraph{Field Set (Component Object Type,, Component Name) up to 8}\label{field-set-component-object-type-component-name-up-to-8}
+
+After the identifying name, the list consists of up to 8 pairs of data items:
+
+\paragraph{Field: Component \textless{}x\textgreater{} Object Type}\label{field-component-x-object-type}
+
+This field specifies the keyword for the type of component used.
+
+\paragraph{Field: Component \textless{}x\textgreater{} Name}\label{field-component-x-name}
+
+This field is the unique name of the component specified in the previous field. This named object must appear in the IDF.
+
+An example from an IDF:
+
+\begin{lstlisting}
+
+AirLoopHVAC:OutdoorAirSystem:EquipmentList,
+             OA Sys 1 Equipment,
+             HeatExchanger:AirToAir:FlatPlate,OA Heat Recovery 1,
+             OutdoorAir:Mixer, OA Mixing Box 1;
+\end{lstlisting}
+
+\subsection{OutdoorAir:Node}\label{outdoorairnode}
+
+The OutdoorAir:Node object declares an HVAC system node for outdoor air conditions. The program automatically sets the air conditions at these nodes to correspond to the ambient environmental conditions at the beginning of every timestep. The outdoor air node is typically used as the inlet air node to an HVAC component such as the OutdoorAir:Mixer object. Multiple OutdoorAir:Node objects can be used in an input file, however, duplicate node names are not allowed.
+
+The \emph{Height Above Ground} field is used to adjust the weather file air conditions, e.g., outdoor dry-bulb and wet-bulb air temperatures, for atmospheric variation with height. This variation can become a significant factor when modeling tall buildings. See the Engineering Reference section on Atmospheric Variation for a description of the algorithm for variation of atmospheric properties with height. A blank entry or a value less than zero for this field indicates that the height will be ignored and the weather file conditions will be used.
+
+\textbf{OutdoorAir:Node} and \textbf{OutdoorAir:NodeList} both set a node to outdoor air conditions. \textbf{OutdoorAir:Node} modifies the weather file conditions if a height has been specified. \textbf{OutdoorAir:NodeList} does not have a height input and always uses the weather file conditions without modification. The same node name may not be used with both of these objects.
+
+\subsubsection{Inputs}\label{inputs-5-001}
+
+\paragraph{Field: Name}\label{field-name-5-001}
+
+The unique name for this outdoor air node.
+
+\paragraph{Field: Height Above Ground}\label{field-height-above-ground}
+
+The height {[}m{]} of the node above ground level. A value greater than zero allows the weather file conditions, e.g., outdoor dry-bulb and wet-bulb air temperatures, to be adjusted according to atmospheric variation with height.
+
+A blank entry or value less than zero indicates that the height will be ignored and the weather file conditions will be used.
+
+An example IDF:
+
+\begin{lstlisting}
+
+OutdoorAir:Node,
+    OA Node 1;  !- Name
+
+  OutdoorAir:Node,
+    Floor 10 Outdoor air Inlet Node,  !- Name
+    30.0;  !- Height Above Ground {m}
+\end{lstlisting}
+
+\subsection{Outdoor Air Node outputs:}\label{outdoor-air-node-outputs}
+
+The ambient dry-bulb air temperature and flow rate at the outdoor air node can be monitored using the system node output variables:
+
+\begin{itemize}
+\item
+  HVAC,Average,System Node Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+e.g.
+
+\begin{lstlisting}
+
+Output:Variable,
+  Floor 10 Outdoor air Inlet Node,
+  System Node Temperature,
+  Hourly;
+\end{lstlisting}
+
+\subsection{OutdoorAir:NodeList}\label{outdoorairnodelist}
+
+The program needs to know which HVAC system nodes are inlets for outdoor air. Knowing this, the program can set the conditions at these nodes to the outdoor conditions at the start of each major timestep. The OutdoorAir:NodeList provides the means for specifying which nodes are outdoor air nodes.
+
+The input is flexible: there may be one or more OutdoorAir:NodeList in each input file. Each list contains up to 25 names. The names can be the name of a unique HVAC system node, or the name of a Node List which will contain the actual node names. Duplicate node names are ignored.
+
+\textbf{OutdoorAir:Node} and \textbf{OutdoorAir:NodeList} both set a node to outdoor air conditions. \textbf{OutdoorAir:Node} modifies the weather file conditions if a height has been specified. \textbf{OutdoorAir:NodeList} does not have a height input and always uses the weather file conditions without modification. The same node name may not be used with both of these objects.
+
+\subsubsection{Inputs}\label{inputs-6-001}
+
+\paragraph{Field: Node or NodeList name}\label{field-node-or-nodelist-name}
+
+The name of an HVAC system node or of a NodeList object. There can be up to 25 names.
+
+An example IDF:
+
+\begin{lstlisting}
+
+OutdoorAir:NodeList,
+      OutsideAirInletNodes;
+
+  NodeList,OutsideAirInletNodes,
+      Outdoor air Inlet Node;
+\end{lstlisting}
+
+\subsection{OutdoorAir:Mixer}\label{outdoorairmixer}
+
+The OutdoorAir:Mixer is the most common component used in an outdoor air system. The outdoor air mixer has 2 inlet air streams: the system return air and the outdoor air. It has 2 outlet air streams: the system relief air and the mixed air. This is a passive component. It takes the inlet mass flows and conditions plus the relief air mass flow and calculates the mixed air flow rate and conditions (as well as the relief air conditions). The inlet and relief mass flow must be set outside the component -- most commonly by an outdoor air controller. The OutdoorAir:Mixer can also be used in compound components such as a fan coil unit.
+
+Input for this object is very simple: a unique name plus the node names of the 2 inlet nodes and the 2 outlet nodes.
+
+\subsubsection{Inputs}\label{inputs-7-001}
+
+\paragraph{Field: Name}\label{field-name-6-001}
+
+A unique user assigned name for a particular outdoor air mixer component. Any reference to this component by another object will use this name.
+
+\paragraph{Field: Mixed Air Node Name}\label{field-mixed-air-node-name}
+
+The name of the HVAC system node which is the outlet for the mixed air stream.
+
+\paragraph{Field: Outdoor Air Stream Node Name}\label{field-outdoor-air-stream-node-name}
+
+The name of the HVAC system node which is the inlet for the outdoor air stream.
+
+\paragraph{Field: Relief Air Stream Node Name}\label{field-relief-air-stream-node-name}
+
+The name of the HVAC system node which is the outlet for the system relief air.
+
+\paragraph{Field: Return Air Stream Node Name}\label{field-return-air-stream-node-name}
+
+The name of the HVAC system node which is the inlet for the return air stream.
+
+An IDF example:
+
+\begin{lstlisting}
+
+OutdoorAir:Mixer,
+      Zone1WindACOAMixer,           ! name
+      Zone1WindACOAMixerOutletNode, ! mixer outlet node
+      Zone1WindACOAInNode,          ! mixer OA node
+      Zone1WindACExhNode,           ! mixer relief node
+      Zone1WindACAirInletNode;      ! mixer inlet node
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-air-path.tex b/doc/input-output-reference/src/overview/group-air-path.tex
new file mode 100644
index 00000000000..1e628cfa9ce
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-air-path.tex
@@ -0,0 +1,280 @@
+\section{Group -- Air Path}\label{group-air-path}
+
+\subsection{AirLoopHVAC:SupplyPath, AirLoopHVAC:ReturnPath}\label{airloophvacsupplypath-airloophvacreturnpath}
+
+The zone supply and return air paths are used to describe the configuration of the flow path that the supply air takes in moving from the main air handler to the zone terminal units and that the return air takes on leaving the zones and returning to the central return air duct. The air paths consist of a group of components AirLoopHVAC:ZoneSplitters and AirLoopHVAC:SupplyPlenums for the supply path and AirLoopHVAC:ReturnPlenums and AirLoopHVAC:ZoneMixers for the return path. The connectivity of the paths is established by the components node connections. There are no branches defined in the zone air path constructs.
+
+For a typical single duct air system there will be one AirLoopHVAC:SupplyPath and one AirLoopHVAC:ReturnPath. A typical dual duct system would have 2 AirLoopHVAC:SupplyPaths one for the hot air and one for the cold air and 1 AirLoopHVAC:ReturnPath.
+
+The AirLoopHVAC:SupplyPlenum component provides the capability to have supply air distributed to the conditioned zones through one or more plenum zones such as would occur in an underfloor air distribution system (UFAD). The AirLoopHVAC:ReturnPlenum component allows the program to model return air plenums. Of course plenums are always optional. The simplest AirLoopHVAC:SupplyPath would consist of only an AirLoopHVAC:ZoneSplitter; similarly the simplest return air path consists of a single AirLoopHVAC:ZoneMixer. A UFAD system supply air path might consist of a single AirLoopHVAC:ZoneSplitter connecting to multiple AirLoopHVAC:SupplyPlenums which in turn could each supply one or more conditioned zones. A system with return plenums would have an AirLoopHVAC:ReturnPath in which the conditioned zones connect to the return plenum inlets and the return plenum s outlets connect to a single AirLoopHVAC:ZoneMixer.
+
+Both the zone supply and return plenums are solved in the heat balance as thermal zones which couple through heat conduction with adjacent zones. Since they are solved as thermal zones the solution scheme involves the zone predictor-corrector technique which will lag the temperature at the system timestep in every zone. See Summary of Predictor-Corrector Procedure in the EnergyPlus Engineering Reference.
+
+Below are the descriptions of the zone supply and return path statements. Note that each statement type has an identifying name, a single inlet/outlet node name, and a list of component type/name pairs. For a single zone being served by an air loop, the inlet to its air distribution unit and the zone return air outlet can be the zone equipment inlet and outlet nodes directly, thus eliminating the need to specify an AirLoopHVAC:SupplyPath and an AirLoopHVAC:ReturnPath.
+
+\subsection{AirLoopHVAC:SupplyPath}\label{airloophvacsupplypath}
+
+The AirLoopHVAC:SupplyPath lists one or more AirLoopHVAC:ZoneSplitter and AirLoopHVAC:SupplyPlenum components comprising the path. The components are listed in flow order: upstream to downstream and may be in series, parallel, or both. Connectivity is established by means of the individual component inlet and outlet nodes.
+
+\subsubsection{Inputs}\label{inputs-003}
+
+\paragraph{Field: Name}\label{field-name-003}
+
+Unique name to identify the supply air path..
+
+\paragraph{Field: Supply Air Path Inlet Node Name}\label{field-supply-air-path-inlet-node-name}
+
+The name of an inlet node for the zone equipment half of the air loop. This should be one of the nodes named in the AirLoopHVAC field: Demand Side Inlet Node Names.
+
+\paragraph{Field Set Component Type and Name}\label{field-set-component-type-and-name}
+
+The remaining fields are sets of two repeated times: a component type and a name. These pairs of fields define the components on the supply air path.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Object Type}\label{field-component-object-type}
+
+Start of the component list for the AirLoopHVAC:SupplyPath. This field should contain either \emph{AirLoopHVAC:SupplyPlenum} or \emph{AirLoopHVAC:ZoneSplitter}.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Name}\label{field-component-name}
+
+Unique name of the AirLoopHVAC:SupplyPlenum or AirLoopHVAC:ZoneSplitter component.
+
+\subsection{AirLoopHVAC:ReturnPath}\label{airloophvacreturnpath}
+
+The AirLoopHVAC:ReturnPath lists one or more AirLoopHVAC:ZoneMixer and AirLoopHVAC:ReturnPlenum components comprising the path. The components are listed in flow order: upstream to downstream and may be in series, parallel, or both. Connectivity is established by means of the individual component inlet and outlet nodes. At this time there can only be 1 AirLoopHVAC:ZoneMixer in an AirLoopHVAC:ReturnPath.
+
+\subsubsection{Inputs}\label{inputs-1-003}
+
+\paragraph{Field: Name}\label{field-name-1-002}
+
+Unique name to identify the return air path.
+
+\paragraph{Field: Return Air Path Outlet Node Name}\label{field-return-air-path-outlet-node-name}
+
+The name of the node that is the outlet to the air loop from the AirLoopHVAC:ReturnPath. This should be the same node named in the AirLoopHVAC field: Demand Side Outlet Node Name.
+
+\paragraph{Field Set Component Type and Name}\label{field-set-component-type-and-name-1}
+
+The remaining fields are sets of two repeated times: a component type and a name. These pairs of fields define the components on the return air path.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Object Type}\label{field-component-object-type-1}
+
+Start of the component list for the AirLoopHVAC:ReturnPath. This field should contain either \emph{AirLoopHVAC:ReturnPlenum} or \emph{AirLoopHVAC:ZoneMixer}.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Name}\label{field-component-name-1}
+
+Unique name of the AirLoopHVAC:ReturnPlenum or AirLoopHVAC:ZoneMixer.
+
+Example inputs are shown below
+
+\begin{lstlisting}
+
+AirLoopHVAC:SupplyPath,
+  SupplyAirPath 1,              !- Name
+  Zone Equip In Node,           !- Supply Air Path Inlet Node Name
+  AirLoopHVAC:SupplyPlenum,     !- Component 1 Object Type
+  Supply-Plenum-1,              !- Component 1 Name
+  AirLoopHVAC:ZoneSplitter,     !- Component 2 Object Type
+  Zone Supply Air Splitter 1;   !- Component 2 Name
+
+
+  AirLoopHVAC:ReturnPath,
+  ReturnAirPath1,               !- Name
+  PLENUM-1 Out Node,            !- Return Air Path Outlet Node Name
+  Zone Return Plenum,           !- Component 1 Object Type
+  Return-Plenum-1;              !- Component 1 Name
+\end{lstlisting}
+
+\subsection{AirLoopHVAC:ReturnPlenum}\label{airloophvacreturnplenum}
+
+The simple building shown in the figure below consists of a controlled zone and a return plenum zone that is used for the return air. This simple configuration contains a ground floor controlled zone with a window and a return plenum zone which handles the roof load. The return air plenum is a special type of component since there is both a heat balance connection and building description and a system airflow connection that transfers the airflow directly from the controlled zone to the return plenum zone in the system air simulation. The input described in this section is mainly just for the system airflow connections in the HVAC algorithms. In addition the return plenum zone must be fully input as a zone object for the heat balance calculation. The zone description needs to contain the wall descriptions - the interzone ceiling and floor, and for this simple case the roof. All the other attributes of a zone that can be specified in the building description can be used with a return plenum zone if necessary: scheduled loads, windows, etc.
+
+\begin{figure}[hbtp] % fig 130
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image337.png}
+\caption{Illustration of Zone Return Plenum \protect \label{fig:illustration-of-zone-return-plenum}}
+\end{figure}
+
+After all the building zone attributes are specified, the AirLoopHVAC:ReturnPlenum object is specified and included as one of the named components in an AirLoopHVAC:ReturnPath.
+
+\subsubsection{Inputs}\label{inputs-2-003}
+
+\paragraph{Field: Name}\label{field-name-2-002}
+
+A unique identifying name identifying the AirLoopHVAC:ReturnPlenum system component.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-000}
+
+The zone name specified in the heat balance portion of the input. This piece of input connects the zone return plenum system component to the heat balance data structure.
+
+\paragraph{Field: Zone Node Name}\label{field-zone-node-name}
+
+The name of the zone node. The zone node name connects the heat balance data structure to the system airflow data structure through this node. This node name must be unique otherwise a warning is reported. Do not use the Zone Air Node Name specified in any ZoneHVAC:EquipmentConnections object, and since this zone is a plenum a ZoneHVAC:EquipmentConnections object is not required for the zone named in the previous field.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-000}
+
+The name of the return plenum outlet node. For the zone return plenum there is only one outlet node that can be specified.
+
+\paragraph{Field: Induced Air Outlet Node or NodeList Name}\label{field-induced-air-outlet-node-or-nodelist-name}
+
+The name of an induced air outlet node or the name of a NodeList of such nodes. These nodes are to be used as the secondary inlet air nodes of powered induction terminal units (See \textbf{AirTerminal:SingleDuct:SeriesPIU:Reheat} and \textbf{AirTerminal:SingleDuct:ParallelPIU:Reheat}).
+
+\paragraph{Field: Inlet \textless{}\#\textgreater{} Node Name}\label{field-inlet-node-name}
+
+The name of a plenum inlet node. There is no limit to the number of inlet nodes, and there may be no duplicate inlet node names. (Note that some EnergyPlus editing tools may allow only 500 inlet node names, but this may be increased by extending the object in the Energy+.idd file.)
+
+An IDF example of a zone return plenum component specification:
+
+\begin{lstlisting}
+
+AirLoopHVAC:ReturnPlenum,
+  Return-Plenum-1,            !- Name
+  PLENUM-1,                   !- Zone Name
+  PLENUM-1 Node,              !- Zone Node Name
+  PLENUM-1 Out Node,          !- Outlet Node Name
+  PLENUM-1 Induced Air Nodes, !- Induced Air Outlet Node or NodeList Name
+  SPACE1-1 Out Node,          !- Inlet 1 Node Name
+  SPACE2-1 Out Node,          !- Inlet 2 Node Name
+  SPACE3-1 Out Node,          !- Inlet 3 Node Name
+  SPACE4-1 Out Node,          !- Inlet 4 Node Name
+  SPACE5-1 Out Node;          !- Inlet 5 Node Name
+
+
+  NodeList,
+  PLENUM-1 Induced Air Nodes, !- Name
+  SPACE1-1 ATU Sec Node,      !- Node 1 Name
+  SPACE2-1 ATU Sec Node,      !- Node 2 Name
+  SPACE3-1 ATU Sec Node,      !- Node 3 Name
+  SPACE4-1 ATU Sec Node;      !- Node 4 Name
+\end{lstlisting}
+
+Below is an example of the AirLoopHVAC:ReturnPath for the simple case shown above.
+
+\begin{lstlisting}
+
+AirLoopHVAC:ReturnPath,
+  ReturnAirPath1,              !- Name
+  PLENUM-1 Out Node,           !- Return Air Path Outlet Node Name
+  AirLoopHVAC:ReturnPlenum,    !- Component 1 Object Type
+  Return-Plenum-1;             !- Component 1 Name
+\end{lstlisting}
+
+\subsection{AirLoopHVAC:SupplyPlenum}\label{airloophvacsupplyplenum}
+
+The building shown in the figure below consists of three controlled zones served by an AirLoopHVAC:SupplyPlenum beneath the floor.
+
+\begin{figure}[hbtp] % fig 131
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image338.png}
+\caption{Illustration of AirLoopHVAC:SupplyPlenum \protect \label{fig:illustration-of-airloophvac-supplyplenum}}
+\end{figure}
+
+The AirLoopHVAC:SupplyPlenum has a heat balance connection and building description, and a system airflow connection which transfers the airflow from the supply plenum zone to the controlled zones in the system simulation. The input described in this section is mainly just for the system airflow connections in the HVAC algorithms. In addition the supply plenum zone must be fully input in the building zone description. The supply plenum zone description needs to contain the wall descriptions, the interzone ceiling and floor, and the ground connection. All the other attributes of a zone that can be specified in the building description can be utilized with a supply plenum zone if necessary, i.e.~scheduled loads, windows, etc.
+
+After all the building zone attributes are specified, the AirLoopHVAC:SupplyPlenum object is specified and included as one of the named components in an AirLoopHVAC:SupplyPath.
+
+\subsubsection{Inputs}\label{inputs-3-002}
+
+\paragraph{Field: Name}\label{field-name-3-002}
+
+A unique identifying name identifying the AirLoopHVAC:SupplyPlenum system component.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1}
+
+The zone name specified in the heat balance portion of the input. This piece of input connects the AirLoopHVAC:SupplyPlenum system component to the heat balance data structure.
+
+\paragraph{Field: Zone Node Name}\label{field-zone-node-name-1}
+
+The name of the zone node. The zone node name connects the heat balance data structure to the system airflow data structure through this node. This node name is defined by the user in the field Zone Air Node Name in the ZoneHVAC:EquipmentConnections object for the zone named in the previous field.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-1}
+
+The name of the inlet node to the supply plenum. The AirLoopHVAC:SupplyPlenum component can send air to many outlets, but there is only one inlet.
+
+\paragraph{Field: Outlet \textless{}\#\textgreater{} Node Name}\label{field-outlet-node-name-1-000}
+
+The name of a plenum outlet node. There is no limit to the number of outlet nodes, and there may be no duplicate outlet node names. (Note that some EnergyPlus editing tools may allow only 500 outlet node names, but this may be increased by extending the object in the Energy+.idd file.)
+
+An IDF example of an AirLoopHVAC:SupplyPlenum component specification:
+
+\begin{lstlisting}
+
+AirLoopHVAC:SupplyPlenum,
+  Supply Plenum 1,                         ! Name
+  SUPPLY PLENUM ZONE,                   ! Zone Name
+  Supply Plenum 1 Zone Node,     ! Zone Node Name
+  Zone Equipment Inlet Node,     ! Inlet Node Name
+  Supply Plenum 1 Outlet Node; ! Outlet 1 Node Name
+\end{lstlisting}
+
+Below is an example of the AirLoopHVAC:SupplyPath for the building shown above.
+
+\begin{lstlisting}
+
+AirLoopHVAC:SupplyPath,
+  TermReheatSupplyPath,               ! Name
+  Zone Equipment Inlet Node,     ! Supply Air Path Inlet Node Name
+  AirLoopHVAC:SupplyPlenum,       ! Component 1 Object Type
+  Supply Plenum 1,                         ! Component 1 Name
+  AirLoopHVAC:ZoneSplitter,       ! Component 2 Object Type
+  Zone Supply Air Splitter;       ! Component 2 Name
+\end{lstlisting}
+
+\subsection{AirLoopHVAC:ZoneSplitter}\label{airloophvaczonesplitter}
+
+The AirLoopHVAC:ZoneSplitter is a component that splits airflow from a single inlet to multiple outlets. This component must be referenced in an AirLoopHVAC:SupplyPath object. The input contains only node connection information.
+
+\subsubsection{Inputs}\label{inputs-4-002}
+
+\paragraph{Field: Name}\label{field-name-4-002}
+
+Unique name for this zone splitter.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-2}
+
+The name of the single inlet node going into the splitter.
+
+\paragraph{Field: Outlet \textless{}\#\textgreater{} Node Name}\label{field-outlet-node-name-2}
+
+The name of a splitter outlet node. There is no limit to the number of outlet nodes, and there may be no duplicate outlet node names. (Note that some EnergyPlus editing tools may allow only 500 outlet node names, but this may be increased by extending the object in the Energy+.idd file.)
+
+An example is shown below.
+
+\begin{lstlisting}
+
+AirLoopHVAC:ZoneSplitter,
+  Zone Supply Air Splitter,     ! Name
+  Zone Equipment Inlet Node,   ! Inlet Node Name
+  Zone 1 Damper Inlet Node,     ! Outlet 1 Node Name
+  Zone 2 Damper Inlet Node,     ! Outlet 2 Node Name
+  Zone 3 Damper Inlet Node;     ! Outlet 3 Node Name
+\end{lstlisting}
+
+\subsection{AirLoopHVAC:ZoneMixer}\label{airloophvaczonemixer}
+
+The AirLoopHVAC:ZoneMixer takes the air from multiple inlets and mixes the streams together to be sent out of a single outlet node. This is a simple process of summing flows and averaging the air properties. This compoment may be part of an air loop return path or part of an induction terminal unit. When used as a return air mixer, this component must be listed in an AirLoopHVAC:ReturnPath object, and the inlets may be zone return air nodes or AirLoopHVAC:ReturnPlenum outlet nodes. When used in an induction terminal unit (ref. AirTerminal:SingleDuct:SeriesPIU:Reheat, AirTerminal:SingleDuct:ParallelPIU:Reheat, and AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction), one inlet node is the supply (primary) air inlet from the central air handler, and the second inlet node is the induced (secondary) air inlet. These node names should match equivalent node names in the terminal unit.
+
+\subsubsection{Inputs}\label{inputs-5-002}
+
+\paragraph{Field: Name}\label{field-name-5-002}
+
+Unique name for this zone mixer.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-3}
+
+The name of the single outlet node leaving the mixer.
+
+\paragraph{Field: Inlet \textless{}\#\textgreater{} Node Name}\label{field-inlet-node-name-3}
+
+The name of a mixer inlet node. There is no limit to the number of inlet nodes, and there may be no duplicate inlet node names. (Note that some EnergyPlus editing tools may allow only 500 inlet node names, but this may be increased by extending the object in the Energy+.idd file.)
+
+An input example is shown below.
+
+\begin{lstlisting}
+
+AirLoopHVAC:ZoneMixer,
+  Zone Return Air Mixer,               ! Name
+  Return Air Mixer Outlet Node, ! Outlet Node Name
+  Zone 1 Outlet Node,                     ! Inlet 1 Node Name
+  Zone 2 Outlet Node,                     ! Inlet 2 Node Name
+  Zone 3 Outlet Node;                     ! Inlet 3 Node Name
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-airflow-network.tex b/doc/input-output-reference/src/overview/group-airflow-network.tex
new file mode 100644
index 00000000000..0003aad8e87
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-airflow-network.tex
@@ -0,0 +1,2797 @@
+\section{Group -- Airflow Network}\label{group-airflow-network}
+
+\subsection{Overview}\label{overview}
+
+The Airflow Network model provides the ability to simulate multizone airflows driven by wind and also by a forced air distribution system. The model can also simulate the heat and moisture gains or losses from the air distribution system itself (e.g., ductwork). When modeling an air distribution system, the current version of the Airflow Network model is restricted to a single forced air system (i.e., AirLoopHVAC object) with a constant volume supply air fan (Fan:ConstantVolume or Fan:OnOff). The capabilities of the model are to:
+
+\begin{itemize}
+\item
+  Simulate zone pressures due to envelope leakage and forced air distribution during HVAC system fan operation
+\item
+  Simulate node pressures in a forced air distribution system during HVAC system fan operation
+\item
+  Calculate multizone airflows due to forced air, wind, and surface leakage, including adjacent zones and outdoors, during HVAC system fan operation
+\item
+  Simulate distribution system airflows, including supply and return air leaks, during HVAC system fan operation
+\item
+  Simulate air distribution system node temperatures and humidity ratios during HVAC system fan operation
+\item
+  Calculate duct conduction losses during HVAC system fan operation
+\item
+  Calculate vapor diffusion losses of ducts during HVAC system fan operation
+\item
+  Calculate sensible and latent loads on the surrounding zones due to supply and return air leaks in the air distribution system during HVAC system fan operation
+\item
+  Simulate zone pressures due to envelope leakage driven by wind when the HVAC system fan is off or if no air distribution system is specified
+\item
+  Calculate multizone airflows due to wind and surface leakage, including adjacent zones and outdoors when the HVAC system fan is off or if no air distribution system is specified
+\item
+  Allow zone exhaust fans to be included as part of the airflow network
+\item
+  For airflow networks with a forced air distribution system, calculate zone sensible and latent loads for two different supply air fan operation modes as required: cycling fan, cycling compressor (CyclingFanAndCompressor) and continuous fan, cycling compressor (ContinuousFanWithCyclingCompressor)
+\end{itemize}
+
+\subsection{Summary of Objects}\label{summary-of-objects}
+
+Before describing the Airflow Network input objects in detail, we list all of the objects and then give a short description of what the objects do.
+
+The Airflow Network input objects are:
+
+\textbf{AirflowNetwork:SimulationControl}
+
+\textbf{AirflowNetwork:Multizone:Zone}
+
+\textbf{AirflowNetwork:Multizone:Surface}
+
+\textbf{AirflowNetwork:MultiZone:Component:SimpleOpening}
+
+\textbf{AirflowNetwork:MultiZone:Component:DetailedOpening}
+
+\textbf{AirflowNetwork:MultiZone:Component:HorizontalOpening}
+
+\textbf{AirflowNetwork:MultiZone:Surface:Crack}
+
+\textbf{AirflowNetwork:MultiZone:ReferenceCrackConditions}
+
+\textbf{AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea}
+
+\textbf{AirflowNetwork:MultiZone:Component:ZoneExhaustFan}
+
+\textbf{AirflowNetwork:MultiZone:ExternalNode}
+
+\textbf{AirflowNetwork:MultiZone:WindPressureCoefficientArray}
+
+\textbf{AirflowNetwork:MultiZone:WindPressureCoefficientValues}
+
+\textbf{AirflowNetwork:Intrazone:Node}
+
+\textbf{AirflowNetwork:Intrazone:Linkage}
+
+\textbf{AirflowNetwork:Distribution:Node}
+
+\textbf{AirflowNetwork:Distribution:Component:Leak}
+
+\textbf{AirflowNetwork:Distribution:Component:LeakageRatio}
+
+\textbf{AirflowNetwork:Distribution:Component:Duct}
+
+\textbf{AirflowNetwork:Distribution:Component:ConstantPressureDrop}
+
+\textbf{AirflowNetwork:Distribution:Component:ConstantVolumeFan}
+
+\textbf{AirflowNetwork:Distribution:Component:Coil}
+
+\textbf{AirflowNetwork:Distribution:Component:HeatExchanger}
+
+\textbf{AirflowNetwork:Distribution:Component:TerminalUnit}
+
+\textbf{AirflowNetwork:Distribution:Linkage}
+
+\textbf{~}
+
+\begin{itemize}
+\item
+  \textbf{AirflowNetwork:SimulationControl} defines basic run parameters for the air flow calculations and specifies whether wind pressure coefficients are input by the user or, for rectangular buildings, calculated by the program.
+\item
+  The \textbf{AirflowNetwork:Multizone:Zone} object specifies the ventilation control that applies to all of the openable exterior and interior windows and doors in the corresponding thermal zone. Surface-level ventilation control can be used to override the zone-level ventilation control if required (see AirflowNetwork: Multizone:Surface object below).
+\item
+  \textbf{AirflowNetwork:Multizone:Surface} object indicates whether a heat transfer surface (wall, window, etc.) has a crack or opening and references an \textbf{AirflowNetwork:MultiZone:Surface:Crack, AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea, AirflowNetwork:MultiZone:Component:SimpleOpening, AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:MultiZone:Component:HorizontalOpening or AirflowNetwork:MultiZone:Component:ZoneExhaustFan} object that gives the air flow characteristics of that crack, opening, or zone exhaust fan. The AirflowNetwork:Multizone:Surface object can also be used to specify individual ventilation control for openable exterior and interior windows and doors.
+\item
+  \textbf{AirflowNetwork:MultiZone:ReferenceCrackConditions} is used to normalize crack information that is based on measurements of crack air flow.
+\item
+  \textbf{AirflowNetwork:Distribution:Node} represents air distribution system nodes for the AirflowNetwork model. A set of an AirLoopHVAC and ZoneHVAC:EquipmentList nodes is a subset of the AirflowNetwork:Distribution:Nodes.
+\item
+  \textbf{AirflowNetwork:Distribution:Component} objects consist of \textbf{Leak, LeakageRatio, Duct, ConstantPressureDrop, ConstantVolumeFan, Coil,} and \textbf{TerminalUnit.} The components provide a relationship between pressure and airflow. The \textbf{Leak} and \textbf{Leakage} components can be used to simulate supply and/or return leaks in an air distribution system\textbf{.} The \textbf{Duct} and \textbf{ConstantPressureDrop components} can be used to deliver forced air into conditioned spaces. The components \textbf{ConstantVolumeFan, Coil, and TerminalUnit} reference normal EnergyPlus objects. The Airflow Network model gets information from these objects to perform an airflow network simulation.
+\item
+  \textbf{AirflowNetwork:Distribution:Linkage} object represents a connection between two node objects and an AirflowNetwork component. The node objects can be an AirflowNetwork:Distribution:Node, AirflowNetwork:MultiZone:ExternalNode or AirflowNetwork:Multizone:Zone.
+\end{itemize}
+
+If you input wind pressure coefficients, \textbf{AirflowNetwork:Multizone:Surface} also has an associated \textbf{AirflowNetwork:MultiZone:ExternalNode}, that, via the \textbf{AirflowNetwork:Multizone:WindPressureCoefficientArray} and \textbf{AirflowNetwork:MultiZone:WindPressureCoefficientValues} objects, gives the wind pressure distribution vs.~wind direction for that node and, implicitly, for the cracks and openings in the exterior surfaces associated with that node.
+
+Figure~\ref{fig:relationships-among-airflownetwork-objects} shows the relationships among AirflowNetwork:Multizone objects and between AirflowNetwork:Multizone objects and regular EnergyPlus objects. In this figure an arrow from object A to object B means A references B, i.e., one of the inputs in A is the name of object B. For example, one input for AirflowNetwork: Multizone:Surface is the name of a heat transfer surface, and another is the name of a crack or opening object. The arrow between AirflowNetwork:Multizone:Surface and AirflowNetwork:MultiZone:ExternalNode is shown dashed to indicate that this reference is not used when wind pressure coefficients are calculated by the program rather than being input by the user.
+
+Figure~\ref{fig:relationships-among-airflownetwork-objects} also shows the relationships among AirflowNetwork:Distribution objects and between AirflowNetwork:Distribution objects and regular EnergyPlus objects. The AirflowNetwork:Distribution:Linkage objects link two nodes from AirflowNetwork:Distribution:Node and/or AirflowNetwork:Multizone:Zone objects with a component defined in the object AirflowNetwork:Distribution:Component. The solid arrows show a reference from object A to object B. The dashed arrows indicate the components which can be used in a linkage object. The red arrows pointing to the Zone object indicate the components that interact with the zone air. For example, the temperature in a zone where a supply leak terminates is used to calculate duct leakage energy loss. The temperature in a zone where a duct component is located is also used to calculate duct conduction loss.
+
+\begin{figure}[hbtp] % fig 93
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image215.png}
+\caption{Relationships among AirflowNetwork objects (right-hand side) and between AirflowNetwork objects and regular EnergyPlus objects. An arrow from object A to object B means that A references B. \protect \label{fig:relationships-among-airflownetwork-objects}}
+\end{figure}
+
+Much of the information needed for the air flow calculation is automatically extracted from the building description for thermal modeling. This includes things like the volume and neutral height of the zones, and the orientation and location of the building surfaces that contain cracks or openings through which air flows. From all of this information the program creates a ``pressure-flow network'' that is solved each timestep using iterative solution methods to obtain the unknown pressures and air flows.
+
+Figure~\ref{fig:plan-view-of-a-simple-air-flow-network} shows a plan view of a very simple air flow network that you can construct using the above AirflowNetwork objects. There are three thermal zones, Zone-1, Zone-2 and Zone-3. There are openable exterior windows---Window-1, Window-2 and Window-3---and openable interior doors---Door-12 and Door-23. Two External Nodes are indicated. ExternalNode-1 is associated with the façade that contains Window-1 and Window-2. ExternalNode-2 is associated with the façade containing Window-3.
+
+One possible air flow pattern is shown in this figure. The actual air flow pattern in a particular timestep, and the size of the flows, depends on many factors, such as (1) What is the wind pressure distribution seen by the exterior windows? (2) Are the exterior windows open or closed, and if open, how far are they open? (3) Are the interior doors open or closed? (4) What are the air temperature differences between zones and between zones and the outdoor air (which affect buoyancy flows)?
+
+\begin{figure}[hbtp] % fig 94
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image216.png}
+\caption{Plan view of a simple air flow network showing a possible air flow pattern in which all of the windows and doors are open. \protect \label{fig:plan-view-of-a-simple-air-flow-network}}
+\end{figure}
+
+Figure~\ref{fig:plan-view-of-a-simple-air-flow-network} shows a possible air flow pattern in which all of the windows and doors are open. Associated with the external nodes are wind pressure coefficient distributions as a function of wind direction that are input using two AirflowNetwork:Multizone:Wind Pressure Coefficient objects. The nature of the air flows through the windows and doors is specified using AirflowNetwork:MultiZone:Component:DetailedOpening and AirflowNetwork:MultiZone:Component:SimpleOpening objects. The Airflow Network model calculates the flows each system timestep depending on various factors, including wind direction and speed, size and vertical position of openings, outdoor air temperature, and zone air temperatures.
+
+\subsection{Airflow Network Example Files (included in the installation)}\label{airflow-network-example-files-included-in-the-installation}
+
+\begin{itemize}
+\item
+  AirflowNetwork3zVent.idf
+\item
+  AirflowNetwork3zVentAutoWPC.idf
+\item
+  AirflowNetwork\_Simple\_House.idf
+\item
+  AirflowNetwork\_Simple\_SmallOffice.idf
+\item
+  AirflowNetwork\_Multizone\_House.idf
+\item
+  AirflowNetwork\_MultiZone\_House\_OvercoolDehumid.idf
+\item
+  AirflowNetwork\_Multizone\_House\_TwoSpeed.idf
+\item
+  AirflowNetwork\_Multizone\_SmallOffice.idf
+\item
+  AirflowNetwork\_Multizone\_SmallOffice\_CoilHXAssistedDX.idf
+\item
+  AirflowNetwork\_MultiZone\_SmallOffice\_GenericContam.idf
+\item
+  AirflowNetwork\_Multizone\_SmallOffice\_HeatRecoveryHXSL.idf
+\item
+  AirflowNetwork\_Multizone\_SmallOffice\_VAV.idf
+\item
+  AirflowNetwor\_Multizone\_HorizontalOpening.idf
+\item
+  CrossVent\_1Zone\_AirflowNetwork.idf
+\item
+  DisplacementVent\_Nat\_AirflowNetwork.idf
+\item
+  HybridVentilationControl.idf
+\end{itemize}
+
+\subsection{What the Airflow Network Model Can and Cannot Do}\label{what-the-airflow-network-model-can-and-cannot-do}
+
+Here is a list of some of the things that the Airflow Network calculation can and cannot model.
+
+\subsubsection{Can Do}\label{can-do}
+
+1)~~~Air flow through cracks in exterior or interzone surfaces.
+
+2)~~~Air flow through cracks around windows and doors when closed.
+
+3)~~~Natural ventilation (i.e., air flow through open or partially open exterior windows and doors).
+
+4)~~~Zone level control of natural ventilation (all windows/doors in a zone that are defined with a component opening object have identical controls).
+
+5)~~~Individual surface control of natural ventilation for a subsurface (window, door, or glassdoor).
+
+6)~~~Modulation of natural ventilation to prevent large zone air temperature swings.
+
+7)~~~Interzone air flow (i.e., air flow through open interzone windows and doors, and through cracks in interzone surfaces).
+
+8)~~~Dependence of air flow on buoyancy effects and wind pressure.
+
+9)~~~Dependence of wind pressure on wind speed, wind direction and surface orientation.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{9}
+\item
+  Supply and return air leaks in an air distribution system.
+\item
+  Account for the effect of supply-air and/or return-air leakage on zone pressure when a forced air distribution system is present and is operating.
+\item
+  When duct leakage is modeled and the HVAC system is on, interzone airflow or infiltration/exfiltration can occur due to changes in zone pressure.
+\item
+  Bi-directional flow through large openings. See discussion below under AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:Multizone:Component:HorizontalOpening, and AirflowNetwork:Multizone:Component:SimpleOpening.
+\item
+  Calculate air flows and pressures in ducts or other components of a forced air distribution system.
+\item
+  Calculate zone loads when the supply air fan cycles on and off during a system timestep using the CyclingFanAndCompressor fan operation mode (Fan:OnOff).
+\item
+  Determine the impact of zone exhaust fans on air flows, pressures, air temperatures/humidity levels and energy consumption.
+\end{enumerate}
+
+\subsubsection{Cannot Do or Restricted}\label{cannot-do-or-restricted}
+
+1)~~~The model is restricted to using a constant volume fan (Fan:ConstantVolume and Fan:OnOff) and cannot model variable volume fan equipment.
+
+2)~~~Air circulation and/or air temperature stratification within a thermal zone. For example, you should not try to divide a high space, such as an atrium, into subzones separated by artificial horizontal surfaces that have cracks or openings with the expectation that AirflowNetwork will give you a realistic temperature in each subzone and/or a realistic air flow between subzones.
+
+3)~~~The model is restricted to eleven types of coils that can be in the air distribution system (Coil:Cooling:DX:SingleSpeed, Coil:Heating:Gas, Coil:Heating:Electric,~ Coil:Heating:DX:SingleSpeed, Coil:Cooling:Water, Coil:Heating:Water, Coil:Cooling:Water:DetailedGeometry, Coil:Cooling:DX:TwoStageWithHumidityControlMode, Coil:Cooling:DX:MultiSpeed, Coil:Heating:DX:MultiSpeed, and Coil:Heating:Desuperheater).
+
+4)~~~The model is restricted to a single type of air distribution equipment terminal units (AirTerminal:SingleDuct:ConstantVolume:Reheat).
+
+5)~~~Pollutant transport cannot currently be modeled.
+
+6)~~~Supply and return leaks are not allowed in an AirLoopHVAC. They can only be modeled in the Zone Equipment portion of the air loop (i.e., return leaks may be modeled between the zone return node and the zone mixer inlet or the zone mixer outlet and the zone equipment loop outlet; and supply leaks may be modeled between the zone equipment loop inlet and the AirLoopHVAC:ZoneSplitter inlet node or the AirLoopHVAC:ZoneSplitter outlet node and the zone supply node).
+
+7)~~~An air distribution system must be located inside the building (i.e., the ducts must pass through zones within the building).
+
+8)~~~Zone exhaust fans must be defined in ZoneHVAC:EquipmentConnections objects.
+
+The input specifications consist of five main sections: \textbf{AirflowNetwork:SimulationControl object, AirflowNetwork multizone data objects, AirflowNetwork distribution node objects, AirflowNetwork distribution component objects,} and \textbf{AirflowNetwork distribution linkage objects.} Each of these object types is described in detail below.
+
+\subsection{AirflowNetwork:SimulationControl}\label{airflownetworksimulationcontrol}
+
+The basic run parameters for this model are defined in this unique object which has the following input specifications:
+
+\subsubsection{Inputs}\label{inputs-004}
+
+\paragraph{Field: Name}\label{field-name-004}
+
+This is a unique character string associated with this instance of the AirflowNetwork:SimulationControl object. At this time, only one AirflowNetwork:SimulationControl object can be specified in an input data file (idf).
+
+\paragraph{Field: AirflowNetwork Control}\label{field-airflownetwork-control}
+
+The following selections are available to control the Airflow Network simulation:
+
+\textbf{MultizoneWithDistribution:} Multizone air flow calculations are performed during all simulation timesteps, including the impacts of the air distribution system when a HVAC system fan is operating. Any \textbf{ZoneInfiltration:*}, \textbf{ZoneVentilation:*}, \textbf{ZoneMixing} and \textbf{ZoneCrossMixing} objects specified in the input data file are not simulated.
+
+\textbf{MultizoneWithoutDistribution}: Multizone air flow calculations are performed during all simulation timesteps, but the air distribution system portion of the network is not modeled even if it is specified in the input data file. Any \textbf{ZoneInfiltration:*}, \textbf{ZoneVentilation:*}, \textbf{ZoneMixing} and \textbf{ZoneCrossMixing} objects specified in the input data file are not simulated.
+
+\textbf{MultizoneWithDistributionOnlyDuringFanOperation:} Multizone air flow calculations, including the impacts of the air distribution system, are only performed when the HVAC system fan is operating. Any \textbf{ZoneInfiltration:*}, \textbf{ZoneVentilation:*}, \textbf{ZoneMixing} and \textbf{ZoneCrossMixing} objects specified in the input data file are used when the HVAC system fan is OFF (if none are specified, then no air flow calculations are performed when the fan is OFF).
+
+\textbf{NoMultizoneOrDistribution:} No multizone air flow calculations (with or without the air distribution system portion of the network) are performed during the simulation. Any \textbf{ZoneInfiltration:*}, \textbf{ZoneVentilation:*}, \textbf{ZoneMixing} and \textbf{ZoneCrossMixing} objects specified in the input data file are simulated (if none are specified, then no air flow calculations are performed). Note: Having an input data file with no AirflowNetwork:SimulationControl objects gives the same impact -- no multizone air flow calculations. However, this choice is provided as a convenience to the user to easily disable the multizone air flow calculations for an input data file that already contains AirflowNetwork objects.
+
+\textbf{Note:} A \textbf{ZoneInfiltration:*} object indicates any one of \textbf{ZoneInfiltration:DesignFlowRate}, \textbf{ZoneInfiltration:EffectiveLeakageArea},and \textbf{ZoneInfiltration:FlowCoefficient} objects.A object of\textbf{ZoneVentilation:*} indicates any one of \textbf{ZoneVentilation:DesignFlowRate} and \textbf{ZoneVentilation:WindandStackOpenArea} objects\textbf{.}
+
+\paragraph{Field: Wind Pressure Coefficient Type}\label{field-wind-pressure-coefficient-type}
+
+Determines whether the wind pressure coefficients are input by the user or calculated. The choices are \textbf{Input} or \textbf{SurfaceAverageCalculation}, with the default being SurfaceAverageCalculation.
+
+If INPUT, you must enter an AirflowNetwork:MultiZone:WindPressureCoefficientArray object, one or more AirflowNetwork:MultiZone:ExternalNode objects, and one or more AirflowNetwork:MultiZone:WindPressureCoefficientValues objects.
+
+The second choice, SurfaceAverageCalculation, should only be used for \textbf{rectangular} buildings. In this case surface-average wind pressure coefficients vs.~wind direction are calculated by the program for the four vertical facades and the roof based on user entries for ``Building Type,'' ``Azimuth Angle of Long Axis of Building,'' and ``Ratio of Building Width Along Short Axis to Width Along Long Axis'' (see description of these fields below). With this choice you do \textbf{not} have to enter any of the following objects: AirflowNetwork:MultiZone: Wind Pressure Coefficient Array, AirflowNetwork:MultiZone:ExternalNode and AirflowNetwork:MultiZone:WindPressureCoefficientValues.
+
+\paragraph{Field: AirflowNetwork Wind Pressure Coefficient Array Name}\label{field-airflownetwork-wind-pressure-coefficient-array-name}
+
+This is the name of the AirflowNetwork:MultiZone:WindPressureCoefficientArray object that contains wind directions corresponding to the wind pressure coefficients given in the AirflowNetwork:MultiZone:WindPressureCoefficientValues objects.
+
+A value need be entered only if Wind Pressure Coefficient Type = INPUT (see description of previous field).
+
+\paragraph{Field: Height Selection for Local Wind Pressure Calculation}\label{field-height-selection-for-local-wind-pressure-calculation}
+
+Determines whether the local wind pressure is calculated based on either given external node heights or surface opening heights. The choices are \textbf{ExternalNode} or \textbf{OpeningHeight}, with the default being OpeningHeight. The local outdoor wind speed calculation procedure is given in the section of ``Local Wind Speed Calculation'' in the Engineering Reference. The calculation procedure requires the height input.
+
+If \textbf{ExternalNode}, the heights given in the AirflowNetwork:MultiZone:ExternalNode objects are used to calculate local wind pressures based on the given height local wind speed.~ Used only if Wind Pressure Coefficient Type = INPUT (see description of previous field).
+
+If \textbf{OpeningHeight}, the number of the AirflowNetwork:MultiZone:ExternalNode objects has to be equal to the number of external surfaces defined in the AirflowNetwork:MultiZone:Surface objects. The centroids in the z direction of the AirflowNetwork:MultiZone:Surface objects are the heights used in the local wind pressure calculation with the given height wind speed. The input is required if Wind Pressure Coefficient Type = INPUT (see description of previous field).
+
+If Wind Pressure Coefficient Type = \textbf{SurfaceAverageCalculation}, a value in this field is not required and a blank may be entered. The default choice is used internally to generate the AirflowNetwork:MultiZone:ExternalNode objects
+
+\paragraph{Field: Building Type}\label{field-building-type}
+
+Used only if Wind Pressure Coefficient Type = SurfaceAverageCalculation. The choices for Building Type are LowRise and HighRise, with the default being LowRise.
+
+LowRise corresponds to a rectangular building whose height is less than three times the width of the footprint (\emph{w\(_{short}\)} in Figure~\ref{fig:footprint-of-a-rectangular-building-showing}) and is less than three times the length of the footprint (\emph{w\(_{long}\)} in the same figure).
+
+HighRise corresponds to a rectangular building whose height is more than three times the width of the footprint (\emph{w\(_{short}\)} in Figure~\ref{fig:footprint-of-a-rectangular-building-showing}) or is more than three times the length of the footprint (\emph{w\(_{long}\)} in the same figure).
+
+\paragraph{Field: Maximum Number of Iterations}\label{field-maximum-number-of-iterations}
+
+The maximum number of iterations allowed in finding an AirflowNetwork solution. If the number of iterations at each simulation timestep is above the maximum number of iterations defined by this field, the program could not find the solution and a Severe error is issued and the program is aborted. The default value is 500.
+
+\paragraph{Field: Initialization Type}\label{field-initialization-type}
+
+Designates which method is used for AirflowNetwork initialization. The choices for Initialization Type are LinearInitializationMethod and ZeroNodePressures, with the default being ZeroNodePressures.
+
+\paragraph{Field: Relative Airflow Convergence Tolerance}\label{field-relative-airflow-convergence-tolerance}
+
+The solution is assumed to have converged when \({{\left| {\,\sum\limits_{} {{{\mathop m\limits^ \bullet }_{_i}}} } \right|} \mathord{\left/ {\vphantom {{\left| {\,\sum\limits_{} {{{\mathop m\limits^ \bullet }_{_i}}} } \right|} {\sum\limits_{} {\left| {{{\mathop m\limits^ \bullet }_{_i}}} \right|} }}} \right. } {\sum\limits_{} {\left| {{{\mathop m\limits^ \bullet }_{_i}}} \right|} }}\) is less than the value specified for this input field. This convergence criteria is equivalent to the ratio of the absolute value of the sum of all network airflows (\(\left| {\sum {{{\mathop m\limits^ \bullet }_{_i}}} } \right|\) ) to the sum of network airflow magnitudes (\(\sum\limits_{}^{} {\left| {{{\mathop m\limits^ \bullet }_{_i}}} \right|}\) ). The default value is 1.0x10\(^{-4}\).
+
+\paragraph{Field: Absolute Airflow Convergence Tolerance}\label{field-absolute-airflow-convergence-tolerance}
+
+The solution is assumed to have converged when the summation of the absolute value of all network airflows (\(\left| {\sum {{{\mathop m\limits^ \bullet }_{_i}}} } \right|\) ) is less than the value specified for this input field. The default value is 1.0x10\(^{-6}\).
+
+\paragraph{Field: Convergence Acceleration Limit}\label{field-convergence-acceleration-limit}
+
+If the ratio of successive pressure corrections is less than this limit, use Steffensen acceleration algorithm (Ref. AirflowNetwork Model in the EnergyPlus Engineering Reference). The range for this field is -1 to 1, with the default value being -0.5.
+
+\paragraph{Field: Azimuth Angle of Long Axis of Building}\label{field-azimuth-angle-of-long-axis-of-building}
+
+Gives the orientation of a rectangular building for calculating wind pressure coefficients. This is the smaller of the angles, measured clockwise, between North and the long axis of the building (see Figure~\ref{fig:footprint-of-a-rectangular-building-showing}). Used only if Wind Pressure Coefficient Type = SurfaceAverageCalculation. The range for this input is 0 to 180, with the default value being 0.
+
+\paragraph{Field: Ratio of Building Width Along Short Axis to Width Along Long Axis}\label{field-ratio-of-building-width-along-short-axis-to-width-along-long-axis}
+
+This is the aspect ratio of a rectangular footprint. It is given by the width of the footprint along its short axis divided by the width along the long axis (see Figure~\ref{fig:footprint-of-a-rectangular-building-showing}). If the footprint is square, the value of this field is 1.0. Used only if Wind Pressure Coefficient Type = SurfaceAverageCalculation. The range for this input is \textgreater{} 0 to 1, with the default value being 1.
+
+\begin{figure}[hbtp] % fig 95
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image221.png}
+\caption{Footprint of a rectangular building showing variables used by the program to calculate surface-average wind pressure coefficients. The angle a is the “Azimuth Angle of Long Axis of Building.�  *w\$\_\{short\}\$*/*w\$\_\{long\}\$* is the “Ratio of Building Width Along Short Axis to Width Along Long Axis.� \protect \label{fig:footprint-of-a-rectangular-building-showing}}
+\end{figure}
+
+\paragraph{Field: Height Dependence of External Node Temperature}\label{field-height-dependence-of-external-node-temperature}
+
+This is an optional field. Input is Yes or No. The default is No. Yes is that external node temperature is dependent on node height. No means that external node temperature is calculated with zero height.
+
+An IDF example is shown below:
+
+\begin{lstlisting}
+
+AirflowNetwork:SimulationControl,
+      AirflowNetwork_All,      !- Name
+      MultiZoneWithDistribution,  !- AirflowNetwork Control
+      Input,                   !- Wind Pressure Coefficient Type
+      Every 30 Degrees,        !- AirflowNetwork Wind Pressure Coefficient Array Name
+      OpeningHeight,           !- Height Selection for Local Wind Speed Calculation
+      LowRise,                 !- Building Type
+      500,                     !- Maximum Number of Iterations {dimensionless}
+      ZeroNodePressures,       !- Initialization Type
+      1.0E-05,                 !- Relative Airflow Convergence Tolerance {dimensionless}
+      1.0E-06,                 !- Absolute Airflow Convergence Tolerance {kg/s}
+      -0.5,                    !- Convergence Acceleration Limit {dimensionless}
+      0.0,                     !- Azimuth Angle of Long Axis of Building {deg}
+      1.0;                     !- Ratio of Building Width Along Short Axis to Width Along Long Axis
+\end{lstlisting}
+
+AirflowNetwork:Multizone data objects are used to calculate multizone airflows. This section describes the input requirements for the following objects:
+
+\begin{itemize}
+\tightlist
+\item
+  AirflowNetwork:MultiZone:Zone
+\end{itemize}
+
+AirflowNetwork:Multizone data objects are used to calculate multizone airflows. This section describes the input requirements for the following objects:
+
+\begin{itemize}
+\item
+  AirflowNetwork:MultiZone:Zone
+\item
+  AirflowNetwork:MultiZone:Surface
+\item
+  AirflowNetwork:MultiZone:Surface:Crack
+\item
+  AirflowNetwork:MultiZone:ReferenceCrackConditions
+\item
+  AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea
+\item
+  AirflowNetwork:MultiZone:Component:DetailedOpening
+\item
+  AirflowNetwork:MultiZone:Component:SimpleOpening
+\item
+  AirflowNetwork:MultiZone:Component:HorizontalOpening
+\item
+  AirflowNetwork:MultiZone:Component:ZoneExhaustFan
+\item
+  AirflowNetwork:MultiZone:ExternalNode
+\item
+  AirflowNetwork:MultiZone:WindPressureCoefficientArray
+\item
+  AirflowNetwork:MultiZone:WindPressureCoefficientValues
+\end{itemize}
+
+A detailed description for each of these objects is provided below.
+
+\subsection{AirflowNetwork:Multizone:Zone}\label{airflownetworkmultizonezone}
+
+This object allows control of natural ventilation through exterior and interior openings in a zone, where ``opening'' is defined as an openable window or door. (Note that only window, door or glass door subsurfaces in a zone that are specified using AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:MultiZone:Component:HorizontalOpening or AirflowNetwork:Multizone:Component:SimpleOpening and have an associated AirflowNetwork:Multizone:Surface object are considered to be openings). The control will be applied in the same way to all of the openings in the zone.
+
+This object is required to perform Airflow Network calculations. Note that ventilation control for all openings is provided at the zone level as default and individual ventilation control of a surface opening can be used to override the zone-level control (see the AirflowNetwork:Multizone:Surface object description below).
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-001}
+
+The name of the EnergyPlus thermal zone corresponding to the AirflowNetwork zone.
+
+\subsubsection{Field: Ventilation Control Mode}\label{field-ventilation-control-mode}
+
+Specifies the type of zone-level natural ventilation control.
+
+Let T\(_{out}\) equal the outdoor air temperature, T\(_{zone}\) equal the previous timestep's zone air temperature, T\(_{set}\) equal the Vent Temperature Schedule value, H\(_{zone}\) equal the specific enthalpy of zone air from the previous timestep, and H\(_{out}\) equal the specific enthalpy of outdoor air. Then the four allowed choices for Ventilation Control Mode are:
+
+\textbf{NoVent}: All of the zone's openable windows and doors are closed at all times independent of indoor or outdoor conditions. The Venting Availability Schedule is ignored in this case. This is the default value for this field.
+
+\textbf{Temperature}: All of the zone's openable windows and doors are opened if T\(_{zone}\) \textgreater{} T\(_{out}\) \textbf{and} T\(_{zone}\) \textgreater{} T\(_{set}\) \textbf{and} Venting Availability Schedule (see below) allows venting.
+
+\textbf{Enthalpy:} All of the zone's openable windows and doors are opened if H\(_{zone}\) \textgreater{} H\(_{out}\) \textbf{and} T\(_{zone}\) \textgreater{} T\(_{set}\) \textbf{and} Venting Availability Schedule allows venting.
+
+\textbf{Constant}: Whenever this object's Venting Availability Schedule allows venting, all of the zone's openable windows and doors are open, independent of indoor or outdoor conditions. Note that ``Constant'' here means that the size of each opening is fixed while venting; the air flow through each opening can, of course, vary from timestep to timestep.
+
+\textbf{ASHRAE55Adaptive}: All of the zone's operable windows and doors are opened if the operative temperature is greater than the comfort temperature (central line) calculated from the ASHRAE Standard 55-2010 adaptive comfort model and Venting Availability Schedule allows venting.
+
+\textbf{CEN15251Adaptive:} All of the zone's operable windows and doors are opened if the operative temperature is greater than the comfort temperature (central line) calculated from the CEN15251 adaptive comfort model and Venting Availability Schedule allows venting.
+
+\subsubsection{Field: Ventilation Control Zone Temperature Setpoint Schedule Name}\label{field-ventilation-control-zone-temperature-setpoint-schedule-name}
+
+The name of a schedule of zone air temperature set points that controls the opening of windows and doors in the thermal zone to provide natural ventilation. This setpoint is the temperature above which all the openable windows and doors in the zone will be opened if the conditions described in the previous field Ventilation Control Mode are met.
+
+The Ventilation Control Zone Temperature Setpoint Schedule Name applies only to windows and doors in the zone that are specified using AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:MultiZone:Component:HorizontalOpening or AirflowNetwork:MultiZone:Component:SimpleOpening and have an associated AirflowNetwork:MultiZone:Surface object.
+
+(The discussion under the field Window/Door Opening Factor in the AirflowNetwork:MultiZone:Surface object describes how the actual opening area of a window or door in a particular timestep is determined.)
+
+\emph{Modulation of Openings}
+
+The following five fields can be used to modulate the window/door openings when Ventilation Control Mode = Temperature or Enthalpy. These fields determine a factor between 0 and 1 that multiplies the opening factor of each window and door in the zone according to the control action shown in Figure~\ref{fig:modulation-of-venting-area-according-to} for Ventilation Control Mode = Temperature and in Figure~\ref{fig:modulation-of-venting-area-according-to-001} for Ventilation Control Mode = Enthalpy. Modulation of the openings can reduce the large temperature swings that can occur if the windows/doors are open too far when they are venting, especially when there is a large inside-outside temperature difference.
+
+The modulation takes the following form when Ventilation Control Mode = Temperature:
+
+\textbf{if} T\(_{zone}\) - T\(_{out}\) ~\textless{} = ~ {[}Lower Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor{]}~~\textbf{then}~~Multiplication factor = 1.0
+
+\textbf{if} {[}Lower Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor{]} \textless{} T\(_{zone}\) - T\(_{out}\) \textless{} {[}Upper Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor{]}~ \textbf{then} Multiplication factor varies linearly from 1.0 to {[}Limit Value on Multiplier for Modulating Venting Open Factor{]}
+
+\textbf{if} T\(_{zone}\) - T\(_{out}\)~\textgreater{} = ~ {[}Upper Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor{]} \textbf{then} Multiplication factor = {[}Limit Value on Multiplier for Modulating Venting Open Factor{]}
+
+One way of ``tuning'' the following modulation control parameters is to perform a sensitivity analysis for winter and/or summer design days to determine what combination of values causes the biggest reduction in zone air temperature fluctuations due to venting.
+
+Note that the default values for the following fields are such that, if none of the fields are specified, the default values are assigned.
+
+\subsubsection{Field: Minimum Venting Open Factor}\label{field-minimum-venting-open-factor}
+
+See Figure~\ref{fig:modulation-of-venting-area-according-to} or Figure~\ref{fig:modulation-of-venting-area-according-to-001}. This field applies only if Ventilation Control Mode = Temperature or Enthalpy. This value may be from zero to 1.0, with the default being 0.0.
+
+\subsubsection{Field: Indoor and Outdoor Temperature Difference Lower Limit For Maximum Venting Open Factor}\label{field-indoor-and-outdoor-temperature-difference-lower-limit-for-maximum-venting-open-factor}
+
+See Figure~\ref{fig:modulation-of-venting-area-according-to}. This field applies only if Ventilation Control Mode = Temperature. This value may be from zero to less than 100ËšC, with the default being 0ËšC. The value for this field must be less than the value specified for the following field.
+
+\subsubsection{Field: Indoor and Outdoor Temperature Difference Upper Limit for Minimun Venting Open Factor}\label{field-indoor-and-outdoor-temperature-difference-upper-limit-for-minimun-venting-open-factor}
+
+See Figure~\ref{fig:modulation-of-venting-area-according-to}. This field applies only if Ventilation Control Mode = Temperature. This value must be greater than 0ËšC, with the default being 100ËšC. The value for this field must be greater than the value specified for the previous field..
+
+\subsubsection{Field: Indoor and Outdoor Enthalpy Difference Lower Limit For Maximum Venting Open Factor}\label{field-indoor-and-outdoor-enthalpy-difference-lower-limit-for-maximum-venting-open-factor}
+
+See Figure~\ref{fig:modulation-of-venting-area-according-to-001}. This field applies only if Ventilation Control Mode = Enthalpy. This value may be from zero to less than 300,000 J/kg, with the default being 0 J/kg. The value for this field must be less than the value specified for the following field.
+
+\subsubsection{Field: Indoor and Outdoor Enthalpy Difference Upper Limit for Minimun Venting Open Factor}\label{field-indoor-and-outdoor-enthalpy-difference-upper-limit-for-minimun-venting-open-factor}
+
+See Figure~\ref{fig:modulation-of-venting-area-according-to-001}. This field applies only if Ventilation Control Mode = Enthalpy. This value must be greater than zero, with the default being 300,000 J/kg. The value for this field must be greater than the value specified for the previous field.
+
+\subsubsection{Field: Venting Availability Schedule Name}\label{field-venting-availability-schedule-name}
+
+The name of a schedule that specifies when venting is available. A zero or negative schedule value means venting is not allowed. A value greater than zero means venting can occur if other venting control conditions (specified by Ventilation Control Mode and Vent Temperature Schedule Name) are satisfied. This schedule name should not be confused with Vent Temperature Schedule Name.
+
+If a Venting Availability Schedule Name is not specified, it is assumed that venting is always available.
+
+Using Venting Availability Schedule allows you to turn off venting at certain times of the day (at night, for example), of the week (on weekends, for example), or of the year (during the winter, for example).
+
+If used with Ventilation Control Mode = Constant, the ventilation rate is constant only when this schedule allows venting; otherwise the ventilation rate is set to zero.
+
+If Ventilation Control Mode = NoVent, this schedule has no effect.
+
+\subsubsection{Field: Occupant Ventilation Control Name}\label{field-occupant-ventilation-control-name}
+
+The name of an AirlowNetwork:OccupantVentilationControl object. The object is used to perform advanced window opening control based on occupant conditions. When an object name is given, advanced window opening control is performed and, the ventilation control defined in the Ventilation Control Mode field will be overridden.
+
+\textbf{Note:} The Occupant Ventilation Control object can be assigned to a zone (AirflowNetwork:MultiZone:Zone) or a surface (AirflowNetwork:MultiZone:Surface). When the object is assigned to a zone, the Occupant Ventilation Control is assigned to the surfaces belonging to the zone automatically. The surface objects must have an associated AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:MultiZone:Component:HorizontalOpening, or AirflowNetwork:MultiZone:Component:SimpleOpening component specified in the field of Leakage Component Name. All output variables will be shown under surface names only, and not under zone names.
+
+\begin{figure}[hbtp] % fig 96
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image222.png}
+\caption{Modulation of venting area according to inside-outside temperature difference. \protect \label{fig:modulation-of-venting-area-according-to}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 97
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image223.png}
+\caption{Modulation of venting area according to inside-outside enthalpy difference. \protect \label{fig:modulation-of-venting-area-according-to-001}}
+\end{figure}
+
+\textbf{Note:} In order to establish an airflow network, each AirflowNetwork:Multizone:Zone object must have at least two surfaces defined with AirflowNetwork:Multizone:Surface objects, so that air can flow from one zone into other zones (or to outdoors) through the network (air mass flow conserved). In addition, for all AirflowNetwork:Multizone:Surface objects facing the same Zone (ref. BuildingSurface:Detailed), at least two different environments must be defined for the other side of these surfaces (e.g., an external node and an adjacent zone, two adjacent zones, or two external nodes).
+
+An IDF example is shown below:
+
+\begin{lstlisting}
+
+AirflowNetwork:MultiZone:Zone,
+      RESISTIVE ZONE,          !- Name of Associated Thermal Zone
+      Temperature,             !- Ventilation Control Mode
+      WindowVentSched,         !- Vent Temperature Schedule Name
+      0.3,                     !- Limit Value on Multiplier for Modulating Venting Open Factor
+                               !- {dimensionless}
+      5.0,                     !- Lower Value on Inside/Outside Temperature Difference for
+                               !- Modulating the Venting Open Factor {deltaC}
+      10.0,                    !- Upper Value on Inside/Outside Temperature Difference for
+                               !- Modulating the Venting Open Factor {deltaC}
+      0.0,                     !- Lower Value on Inside/Outside Enthalpy Difference for Modulating
+                               !- the Venting Open Factor {J/kg}
+      300000.0,                !- Upper Value on Inside/Outside Enthalpy Difference for Modulating
+                               !- the Venting Open Factor {J/kg}
+      VentingSched;            !- Venting Availability Schedule Name
+\end{lstlisting}
+
+\subsection{AirflowNetwork:Multizone:Surface}\label{airflownetworkmultizonesurface}
+
+The AirflowNetwork:Multizone:Surface object specifies the properties of a surface ``linkage'' through which air flows. This linkage is always associated with a heat transfer surface (wall, roof, floor, or a ceiling) or subsurface (door, glass door, or window) with both faces exposed to air. The linkage specifies two connected nodes: two zone nodes defined in AirflowNetwork:Multizone:Zone objects based on inside and outside face environment for an interior surface, or a zone node defined in an AirflowNetwork:Multizone:Zone object based on inside face environment and an external node defined in an AirflowNetwork:MultiZone:ExternalNode object for an exterior surface. The associated leakage component for this surface can be a crack (or surface effective leakage area) in an exterior or interior heat transfer surface or subsurface, or an exterior or interior window, door or glass door (heat transfer subsurface) that can be opened to allow air flow. The allowed surface air leakage components are:
+
+\begin{itemize}
+\item
+  AirflowNetwork:MultiZone:Surface:Crack
+\item
+  AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea
+\item
+  AirflowNetwork:MultiZone:Component:DetailedOpening
+\item
+  AirflowNetwork:MultiZone:Component:HorizontalOpening
+\item
+  AirflowNetwork:MultiZone:Component:SimpleOpening
+\item
+  AirflowNetwork:MultiZone:Component:ZoneExhaustFan
+\end{itemize}
+
+The two ``opening'' components are used to modulate openness based on required conditions.
+
+The AirflowNetwork:Multizone:Surface object allows a heat transfer surface or subsurface to have one crack (or one surface effective leakage area object), or a subsurface (i.e., window, door or glass door) to have one opening (detailed or simple).
+
+An interior heat transfer surface (BuildingSurface:Detailed) whose surface name is used as the input for the Outside Boundary Condition Object field represents a floor without ground contact and is not allowed as an AirflowNetwork:Multizone:Surface. A heat transfer surface defined in the BuildingSurface:Detailed:ExteriorNaturalVentedCavity is also not allowed.
+
+When a triangular subsurface is used, the model provides a warning and treats this subsurface as rectangular. The effective width and height calculated in the ProcessSurfaceVertices function of the SurfaceGeometry module are used to represent a rectangular subsurface.
+
+Effective width = 0.75 x Length between Vertex 1 and Vertex 2
+
+Effective height = 4 x Area / ( 3 x Length between Vertex 2 and Vertex 3 )
+
+\subsubsection{Field: Surface Name}\label{field-surface-name-000}
+
+This is the name of the corresponding surface (wall, roof, ceiling, floor, window, door or glass door).
+
+Information on this surface is used by the program as follows:
+
+(1)~~For a linkage associated with an exterior heat transfer surface: air flow through this linkage is between the outside environment and the thermal zone to which the surface belongs.
+
+(2)~~For a linkage associated with an interior (i.e., interzone) heat transfer surface: air flow through this linkage is between the thermal zones separated by the surface (i.e., the thermal zone associated with the inside face environment and the thermal zone associated with the outside face environment).
+
+(3)~~This heat transfer surface determines the height of the linkage, which is used in calculating buoyancy-related flow through the linkage.
+
+\textbf{Note:} It is possible to define an interzone surface twice in EnergyPlus, once in each of the zones that the surface separates. Previously this was a requirement of EnergyPlus (prior to version 2.0), but now it is optional and the user also has the option of only defining the surface once (EnergyPlus defines the second surface automatically within the program). For each interzone surface, use only one (of possible two) interzone surface names in the AirflowNetwork:Multizone:Surface object for ``Surface Name.'' \textbf{Do not} enter two AirflowNetwork:Multizone:Surface objects corresponding to the two possible interzone names. This would cause the air flow through the surface to be counted twice.
+
+\subsubsection{Field: Leakage Component Name}\label{field-leakage-component-name}
+
+The name of the AirflowNetwork:MultiZone:Surface:Crack, AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea, AirflowNetwork:MultiZone:Component:SimpleOpening, AirflowNetwork:MultiZone:Component:HorizontalOpening, AirflowNetwork:MultiZone:Component:DetailedOpening or AirflowNetwork:MultiZone:Component:ZoneExhaustFan object associated with this air flow linkage.
+
+If the name of an opening component (i.e.~AirflowNetwork:MultiZone:Component:DetailedOpening. AirflowNetwork:MultiZone:Component:HorizontalOpening,~ or AirflowNetwork:MultiZone:Component:SimpleOpening is given here, then the Surface Name in the previous field must be that of a window, door or glass door heat transfer subsurface. Otherwise an error message will be reported.
+
+If the name of an AirflowNetwork:MultiZone:Surface:Crack object or AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea object is given here, the program will position the crack at the average height of the associated heat transfer surface or subsurface. The user can define multiple heat transfer surfaces (e.g., split a wall into several surfaces) to be more precise in establishing the crack location. Similarly, the user can define multiple heat transfer surfaces if a wall, for example, has multiple cracks or openings that need to be defined individually.
+
+If the name of an AirflowNetwork:MultiZone:Component:ZoneExhaustFan is given here, then the Surface Name in the previous field must be that of an exterior heat transfer surface. The zone name defined in the Zone Name field for this heat transfer surface must be the same zone name defined in the ZoneHVAC:EquipmentConnections object (which references a ZoneHVAC:EquipmentList containing the name of the corresponding zone exhaust fan).Otherwise an error message will be reported. When this zone exhaust fan is operating for a simulation timestep, all surface-level controls described below are ignored for that timestep.
+
+\subsubsection{Field: External Node Name}\label{field-external-node-name}
+
+The name of the associated AirflowNetwork:MultiZone:ExternalNode object, which determines the wind pressure coefficients for the heat transfer surface. Used only if Surface Name is for an exterior surface.
+
+If Wind Pressure Coefficient Type = SurfaceAverageCalculation in the AirflowNetwork:SimulationControl object, this field is not used and a blank may be entered. If the surface is an interior (i.e., interzone) surface, leave this field blank.
+
+\subsubsection{Field: Window/Door Opening Factor, or Crack Factor}\label{field-windowdoor-opening-factor-or-crack-factor}
+
+If this linkage is associated with an AirflowNetwork:MultiZone:Component:DetailedOpening or AirflowNetwork:MultiZone:Component:SimpleOpening object (which means it is an openable window or door), then this field is called ``Window/Door Opening Factor'' and represents the value of the Opening Factor that is in effect when the Vent Temperature Schedule (defined in the AirflowNetwork:Multizone:Zone object) indicates that this window or door is open.
+
+The AirflowNetwork model uses a combination of factors to determine the actual opening area for a window or door when it is venting. For example, consider a window that is 1.5m high and 2.0m wide (excluding frame). Assume that the AirflowNetwork:MultiZone:Component:DetailedOpening for this window has Type of Large Vertical Opening = 1 (non-pivoting window), Height Factor = 0.5 and Width Factor = 0.8. Then when the window is fully open, the opening area = height of opening (0.5x1.5) times width of opening (0.8x2.0) = 0.75x1.6 = 1.2 m\(^{2}\). If the Window/Door Opening Factor is 0.75, then the opening area = 0.75x1.2 = 0.9 m\(^{2}\).
+
+If, in addition, the window is in a thermal zone for which opening modulation has been specified (ref: AirflowNetwork:Multizone:Zone) and the multiplication factor due to modulation is 0.3 in a particular timestep, then the actual opening factor that timestep = 0.3x0.75 = 0.225 and the actual opening area that timestep = 0.3x0.9 = 0.27 m\(^{2}\).
+
+If this linkage is associated with an AirflowNetwork:MultiZone:Surface:Crack object, the following crack air flow equation is used. 
+
+\begin{equation}
+Q = \left( Crack\;Factor \right) * C_T * C_Q \left( \Delta P \right)^{n}
+\end{equation}
+
+Where
+
+\emph{Q}~~~ = air mass flow (kg/s)
+
+\emph{C\(_{Q}\)}~ = air mass flow coefficient (kg/s @ 1 Pa)
+
+\emph{C\(_{T}\)}~ = reference condition temperature correction factor (dimensionless). See AirflowNetwork:MultiZone:Surface:Crack object.
+
+\(\Delta P\) = pressure difference across crack (Pa)
+
+\emph{n}~~~ = air flow exponent (dimensionless)
+
+\emph{The following fields control venting. They are used only when Name of Associated Heat Transfer Surface is that of an openable exterior or interior window, door or glass door. They only apply to openings, and do not apply to surface cracks, effective leakage area or zone exhaust fans. If none of these fields is specified, or if Ventilation Control Mode = ZoneLevel, venting is controlled by the AirflowNetwork:Multizone:Zone object for the thermal zone containing the window or door (ref: AirflowNetwork:Multizone:Zone Data).}
+
+\subsubsection{Field: Ventilation Control Mode}\label{field-ventilation-control-mode-1}
+
+Specifies the type of surface-level natural ventilation control.
+
+Let T\(_{out}\) equal the outdoor air temperature, T\(_{zone}\) equal the previous timestep's zone air temperature, T\(_{set}\) equal the Vent Temperature Schedule value, H\(_{zone}\) equal the specific enthalpy of zone air from the previous timestep, and H\(_{out}\) equal the specific enthalpy of outdoor air. Then the four allowed choices for Ventilation Control Mode are:
+
+\textbf{NoVent}: The openable window or door associated with this surface is closed at all times independent of indoor or outdoor conditions. The Venting Availability Schedule is ignored in this case.
+
+\textbf{Temperature}: The openable window or door associated with this surface is opened if T\(_{zone}\) \textgreater{} T\(_{out}\) \textbf{and} T\(_{zone}\) \textgreater{} T\(_{set}\) \textbf{and} Venting Availability Schedule (see below) allows venting.
+
+\textbf{Enthalpy:} The openable window or door associated with this surface is opened if H\(_{zone}\) \textgreater{} H\(_{out}\) \textbf{and} T\(_{zone}\) \textgreater{} T\(_{set}\) \textbf{and} Venting Availability Schedule allows venting.
+
+\textbf{Constant}: Whenever this object's Venting Availability Schedule allows venting, the openable window or door associated with this surface is open, independent of indoor or outdoor conditions. Note that ``Constant'' here means that the size of this opening is fixed while venting; the air flow through this opening can, of course, vary from timestep to timestep.
+
+\textbf{ASHRAE55Adaptive}: The openable window or door associated with this surface is opened if the operative temperature is greater than the comfort temperature (central line) calculated from the ASHRAE Standard 55-2010 adaptive comfort model \textbf{and} Venting Availability Schedule allows venting.
+
+\textbf{CEN15251Adaptive:} The openable window or door associated with this surface is opened if the operative temperature is greater than the comfort temperature (central line) calculated from the CEN15251 adaptive comfort model \textbf{and} Venting Availability Schedule allows venting.
+
+\textbf{ZoneLevel}: Venting of the window or door is not controlled individually, but is controlled instead at the zone level. This means that the venting is determined by the AirflowNetwork:Multizone:Zone object for the thermal zone containing the window or door (ref: AirflowNetwork:Multizone:Zone object). This is the default value for this field.
+
+\textbf{AdjacentTemperature}: This choice is used for an interior surface only. The openable interior window or door associated with this surface is opened if T\(_{zone}\) \textgreater{} T\(_{adjacent\\ zone}\) \textbf{and} T\(_{zone}\) \textgreater{} T\(_{set}\) \textbf{and} Venting Availability Schedule (see below) allows venting, where T\(_{adjacent\\ zone}\)is the adjacent zone temperature.
+
+\textbf{AdjacentEnthalpy:} This choice is also used for an interior surface only. The interior openable window or door associated with this surface is opened if H\(_{zone}\) \textgreater{} H\(_{adjacent\\ zone}\) \textbf{and} T\(_{zone}\) \textgreater{} T\(_{set}\) \textbf{and} Venting Availability Schedule allows venting, where H\(_{adjacent\\ zone}\)is the adjacent zone specific enthalpy.
+
+\subsubsection{Field: Ventilation Control Zone Temperature Setpoint Schedule Name}\label{field-ventilation-control-zone-temperature-setpoint-schedule-name-1}
+
+The name of a schedule of zone air temperature set points that controls the opening of a window or door associated with this surface to provide natural ventilation. This setpoint is the temperature above which this openable window or door will be opened if the conditions described in the previous field Ventilation Control Mode are met.
+
+The Ventilation Control Zone Temperature Setpoint Schedule applies only to a window or door attached to this surface that is specified using AirflowNetwork:MultiZone:Component:DetailedOpening or AirflowNetwork:MultiZone:Component:SimpleOpening.
+
+(The discussion under the field Window/Door Opening Factor in this object describes how the actual opening area of a window or door in a particular timestep is determined.)
+
+\emph{Modulation of Openings}
+
+The following five fields can be used to modulate this window/door opening when Ventilation Control Mode = Temperature or Enthalpy. These fields determine a factor between 0 and 1 that multiplies the opening factor of this window or door according to the control action shown in Figure~\ref{fig:modulation-of-venting-area-according-to} for Ventilation Control Mode = Temperature and in Figure~\ref{fig:modulation-of-venting-area-according-to-001} for Ventilation Control Mode = Enthalpy. Modulation of this opening can reduce the large temperature swings that can occur if the window/door is open too far when it is venting, especially when there is a large inside-outside temperature difference.
+
+The modulation takes the following form when Ventilation Control Mode = Temperature:
+
+\textbf{if} T\(_{zone}\) - T\(_{out}\)~\textless{} = {[}Lower Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor{]}~~\textbf{then}~~Multiplication factor = 1.0
+
+\textbf{if} {[}Lower Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor{]} \textless{} T\(_{zone}\) - T\(_{out}\) \textless{} {[}Upper Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor{]}~ \textbf{then} Multiplication factor varies linearly from 1.0 to {[}Limit Value on Multiplier for Modulating Venting Open Factor{]}
+
+\textbf{if} T\(_{zone}\) - T\(_{out}\)~\textgreater{} = ~ {[}Upper Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor{]}~ \textbf{then} Multiplication factor = {[}Limit Value on Multiplier for Modulating Venting Open Factor{]}
+
+One way of ``tuning'' the following modulation control parameters is to perform a sensitivity analysis for winter and/or summer design days to determine what combination of values causes the biggest reduction in zone air temperature fluctuations due to venting.
+
+Note that the default values for the following fields are such that, if none of the fields are specified, modulation will not occur.
+
+\subsubsection{Field: Minimum Venting Open Factor}\label{field-minimum-venting-open-factor-1}
+
+See Figure~\ref{fig:modulation-of-venting-area-according-to} or Figure~\ref{fig:modulation-of-venting-area-according-to-001}. This field applies only if Ventilation Control Mode = Temperature or Enthalpy. This value may be from zero to 1.0, with the default being 0.0.
+
+\subsubsection{Field: Indoor and Outdoor Temperature Difference Lower Limit For Maximum Venting Open Factor}\label{field-indoor-and-outdoor-temperature-difference-lower-limit-for-maximum-venting-open-factor-1}
+
+See Figure~\ref{fig:modulation-of-venting-area-according-to}. This field applies only if Ventilation Control Mode = Temperature. This value may be from zero to less than 100°C, with the default being 0°C. The value for this field must be less than the value specified for the following field.
+
+\subsubsection{Field: Indoor and Outdoor Temperature Difference Upper Limit for Minimun Venting Open Factor}\label{field-indoor-and-outdoor-temperature-difference-upper-limit-for-minimun-venting-open-factor-1}
+
+See Figure~\ref{fig:modulation-of-venting-area-according-to}. This field applies only if Ventilation Control Mode = Temperature. This value must be greater than 0°C, with the default being 100°C. The value for this field must be greater than the value specified for the previous field.
+
+\subsubsection{Field: Indoor and Outdoor Enthalpy Difference Lower Limit For Maximum Venting Open Factor}\label{field-indoor-and-outdoor-enthalpy-difference-lower-limit-for-maximum-venting-open-factor-1}
+
+See Figure~\ref{fig:modulation-of-venting-area-according-to-001}. This field applies only if Ventilation Control Mode = Enthalpy. This value may be from zero to less than 300,000 J/kg, with the default being 0 J/kg. The value for this field must be less than the value specified for the following field.
+
+\subsubsection{Field: Indoor and Outdoor Enthalpy Difference Upper Limit for Minimun Venting Open Factor}\label{field-indoor-and-outdoor-enthalpy-difference-upper-limit-for-minimun-venting-open-factor-1}
+
+See Figure~\ref{fig:modulation-of-venting-area-according-to-001}. This field applies only if Ventilation Control Mode = Enthalpy. This value must be greater than zero, with the default being 300,000 J/kg. The value for this field must be greater than the value specified for the previous field.
+
+\subsubsection{Field: Venting Availability Schedule Name}\label{field-venting-availability-schedule-name-1}
+
+The name of a schedule that specifies when venting is available. A zero or negative schedule value means venting is not allowed. A value greater than zero means venting can occur if other venting control conditions (specified by Ventilation Control Mode and Vent Temperature Schedule Name) are satisfied. This schedule name should not be confused with Vent Temperature Schedule Name.
+
+If a Venting Availability Schedule Name is not specified, it is assumed that venting is always available.
+
+Using Venting Availability Schedule allows you to turn off venting at certain times of the day (at night, for example), week (on weekends, for example), or year (during the winter, for example).
+
+If used with Ventilation Control Mode = Constant, the ventilation rate is constant only when this schedule allows venting; otherwise the ventilation rate is set to zero.
+
+If Ventilation Control Mode = NoVent, this schedule has no effect.
+
+\textbf{Note:} In order to establish an airflow network, each AirflowNetwork:Multizone:Zone object must have at least two surfaces defined with AirflowNetwork:Multizone:Surface objects, so that air can flow from one zone into other zones (or to outdoors) through the network (air mass flow conserved). In addition, for all AirflowNetwork:Multizone:Surface objects facing the same Zone Name (ref. BuildingSurface:Detailed), at least two different environments must be defined for the other side of these surfaces (e.g., an external node and an adjacent zone, two adjacent zones, or two external nodes).
+
+\subsubsection{Field: Occupant Ventilation Control Name}\label{field-occupant-ventilation-control-name-1}
+
+The name of an AirlowNetwork:OccupantVentilationControl object. The object is used to perform advanced window opening control based on occupant conditions. When an object name is given, advanced window opening control is performed and, the Ventilation Control defined in the Ventilation Control Mode field will be overridden.
+
+IDF examples are provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:MultiZone:Surface,
+      Zn001:Wall001,           !- Name of Associated Heat Transfer Surface
+      CR-1,                    !- Leakage Component Name
+      SFacade,                 !- External Node Name
+      1.0;                     !- Window/Door Opening Factor, or Crack Factor {dimensionless}
+
+  AirflowNetwork:MultiZone:Surface,
+      Zn001:Wall001:Win001,    !- Name of Associated Heat Transfer Surface
+      WiOpen1,                 !- Leakage Component Name
+      SFacade,                 !- External Node Name
+      0.5;                     !- Window/Door Opening Factor, or Crack Factor {dimensionless}
+
+  AirflowNetwork:MultiZone:Surface,
+      Zn003:Wall003,           !- Name of Associated Heat Transfer Surface
+      Zone3 Exhaust Fan,       !- Leakage Component Name
+      EFacade,                 !- External Node Name
+      1.0;                     !- Window/Door Opening Factor, or Crack Factor {dimensionless}
+
+  AirflowNetwork:MultiZone:Surface,
+      Zn001:Wall001:Win002,    !- Name of Associated Heat Transfer Surface
+      WiOpen2,                 !- Leakage Component Name
+      WFacade,                 !- External Node Name
+      0.5;                     !- Window/Door Opening Factor, or Crack Factor {dimensionless}
+      Temperature,             !- Ventilation Control Mode
+      WindowVentSched,         !- Vent Temperature Schedule Name
+      0.3,                     !- Limit Value on Multiplier for Modulating Venting Open Factor
+                               !- {dimensionless}
+      5.0,                     !- Lower Value on Inside/Outside Temperature Difference for
+                               !- Modulating the Venting Open Factor {deltaC}
+      10.0,                    !- Upper Value on Inside/Outside Temperature Difference for
+                               !- Modulating the Venting Open Factor {deltaC}
+      0.0,                     !- Lower Value on Inside/Outside Enthalpy Difference for Modulating
+                               !- the Venting Open Factor {J/kg}
+      300000.0,                !- Upper Value on Inside/Outside Enthalpy Difference for Modulating
+                               !- the Venting Open Factor {J/kg}
+      VentingSched;            !- Venting Availability Schedule Name
+\end{lstlisting}
+
+\subsection{AirflowNetwork:MultiZone:ReferenceCrackConditions}\label{airflownetworkmultizonereferencecrackconditions}
+
+This object specifies the reference conditions for temperature, humidity, and pressure which correspond to the AirflowNetwork:MultiZone:Surface:Crack object.
+
+\subsubsection{Inputs}\label{inputs-1-004}
+
+\paragraph{Field: Name}\label{field-name-1-003}
+
+The name of this Reference Crack Conditons object. This name is referenced by an AirflowNetwork:MultiZone:Surface:Crack object.
+
+\paragraph{Field: Reference Temperature}\label{field-reference-temperature}
+
+The reference temperature in °C under which the Surface Crack Data were obtained. The default value is 20°C.
+
+\paragraph{Field: Reference Barometric Pressure}\label{field-reference-barometric-pressure}
+
+The reference barometric pressure in Pa under which the Surface Crack Data were obtained. The default value is 101325 Pa.
+
+\paragraph{Field: Reference Humidity Ratio}\label{field-reference-humidity-ratio}
+
+The reference humidity ratio in kgWater/kgDryAir under which the Surface Crack Data were obtained. The default value is 0 kgWater/kgDryAir.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:MultiZone:ReferenceCrackConditions,
+      ReferenceCrackConditions,      !- Name of Reference Crack Conditions
+      20.0,                          !- Reference Temperature for Crack Data {C}
+      101325,                        !- Reference Barometric Pressure for Crack Data {Pa}
+      0.0;                           !- Reference Humidity Ratio for Crack Data {kgWater/kgDryAir}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:MultiZone:Surface:Crack}\label{airflownetworkmultizonesurfacecrack}
+
+This object specifies the properties of air flow through a crack and the associated measurement conditions. The following power law form is used that gives air flow through the crack as a function of the pressure difference across the crack: 
+
+\begin{equation}
+Q = \left( Crack\;Factor \right) * C_T * C_Q \left( \Delta P \right)^{n}
+\end{equation}
+
+Where
+
+\emph{Q}~~~ = air mass flow (kg/s)
+
+\emph{C\(_{Q}\)}~ = air mass flow coefficient (kg/s-Pa\(^{n}\) @ 1 Pa)
+
+\emph{C\(_{T}\)}~ = reference condition temperature correction factor (dimensionless)
+
+\(\Delta P\) = pressure difference across crack (Pa)
+
+\emph{n}~~~ = air flow exponent (dimensionless)
+
+\begin{equation}
+{C_T} = {\left[ {\frac{{{\rho_o}}}{\rho }} \right]^{n - 1}}{\left[ {\frac{{{\nu_o}}}{\nu }} \right]^{2n - 1}}
+\end{equation}
+
+where
+
+\(\rho\) = Air density at the specific air temperature and humidity ratio conditions {[}kg/m\(^{3}\){]}
+
+\(\nu\) = Air kinetic viscosity at the specific air temperature condition {[}m\(^{2}\)/s{]}
+
+\(\rho_o\) = Air density at the reference air conditions provided by the object Air\-flow\-Net\-work:\-Multi\-Zone:\-Refer\-ence\-Crack\-Con\-ditions specified in the field Reference Crack Conditions {[}kg/m\(^{3}\){]}
+
+\(\nu_o\) = Air kinetic viscosity at the reference air temperature provided by the object Air\-flow\-Net\-work:\-Multi\-Zone:\-Refer\-ence\-Crack\-Con\-ditions specified in the field Reference Crack Conditions {[}m\(^{2}\)/s{]}
+
+Note: The correction factor shown above is use for this particular component as specified.
+
+\subsubsection{Inputs}\label{inputs-2-004}
+
+\paragraph{Field: Name}\label{field-name-2-003}
+
+This is a name for this AirflowNetwork:MultiZone:Surface:Crack object. It is referenced by an AirflowNetwork:Multizone:Surface object.
+
+\paragraph{Field: Air Mass Flow Coefficient at Reference Conditions}\label{field-air-mass-flow-coefficient-at-reference-conditions}
+
+The value of the air mass flow coefficient,\({C_Q}\) , in the crack air flow equation. It has units of kg/s at 1Pa. This value must be greater than zero.
+
+\paragraph{Field: Air Mass Flow Exponent}\label{field-air-mass-flow-exponent}
+
+The value of the exponent,* n*, in the crack air flow equation. The valid range is 0.5 to 1.0, with the default value being 0.65.
+
+\paragraph{Field: Reference Crack Conditions}\label{field-reference-crack-conditions}
+
+The name of the AirflowNetwork:MultiZone:ReferenceCrackConditions object which specifies the conditions under which the air mass flow coefficient was measured. If the user omits this field and only one AirflowNetwork:MultiZone:ReferenceCrackConditions object is defined in the input data file, then those reference crack conditions will be used. If the user omits this field and either zero or more than one AirflowNetwork:MultiZone:ReferenceCrackConditions objects are defined in the input data file, then the default conditions for the AirflowNetwork:Multizone: Reference Crack Conditions object will be used.
+
+An IDF example is shown below:
+
+\begin{lstlisting}
+AirflowNetwork:MultiZone:Surface:Crack,
+  CR-1,                   !- Name of Surface Crack Component
+  0.01,                   !- Air Mass Flow Coefficient at Reference Conditions {kg/s}
+  0.667,                  !- Air Mass Flow Exponent {dimensionless}
+  ReferenceCrackConditions; !- Reference Crack Conditions
+\end{lstlisting}
+
+\subsection{AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea}\label{airflownetworkmultizonesurfaceeffectiveleakagearea}
+
+The effective leakage area (ELA) object is used to define surface air leakage. It has
+
+five fields. The relationship between pressure and airflow may be expressed as:
+
+\begin{equation}
+\dot m = ELA*{C_d}\sqrt {2\rho } *{\left( {\Delta {P_r}} \right)^{0.5 - n}}{\left( {\Delta P} \right)^n}
+\end{equation}
+
+where
+
+\(\dot m\) = Air mass flow rate {[}kg/s{]}
+
+\(\rm{ELA}\) = Effective leakage area {[}m\(^{2}\){]}
+
+\(\rho\) = Air density {[}kg/m\(^{3}\){]}
+
+\(\Delta {P_r}\) = Reference pressure difference {[}Pa{]}
+
+\(\Delta P\) = Pressure difference across this component {[}Pa{]}
+
+\(C_{d}\) = Discharge coefficient {[}dimensionless{]}
+
+\(n\) = Air mass flow exponent {[}dimensionless{]}
+
+\subsubsection{Inputs}\label{inputs-3-003}
+
+\paragraph{Field: Name}\label{field-name-3-003}
+
+This is a name for this AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea object. It is referenced by an AirflowNetwork:Multizone:Surface object.
+
+\paragraph{Field: Effective Leakage Area}\label{field-effective-leakage-area}
+
+This numeric field is used to input the effective leakage area~ in square meters. The effective leakage area is used to characterize openings for infiltration calculations (ASHRAE Handbook of Fundamentals, 1997, pp 25.18). This value must be greater than zero.
+
+\paragraph{Field: Discharge Coefficient}\label{field-discharge-coefficient}
+
+This numeric field is used to input the discharge coefficient. This value must be greater than zero, with a default value of 1.0.
+
+\paragraph{Field: Reference Pressure Difference}\label{field-reference-pressure-difference}
+
+This numeric field is used to input the reference pressure difference {[}Pa{]}. This value must be greater than zero, with a default value of 4.0 Pa.
+
+\paragraph{Field: Air Mass Flow Exponent}\label{field-air-mass-flow-exponent-1}
+
+This numeric field is used to input the pressure difference exponent. The valid range of the exponent is from 0.5 to 1.0, with a default value of 0.65.
+
+\begin{callout}
+  Note: There are two common sets of reference conditions: \(C_{d}\) = 1.0 and \(\Delta P\) = 4 Pa, or \(C_d\) = 0.6 and \(\Delta P\) = 10 Pa
+\end{callout}
+
+An IDF example is shown below:
+
+\begin{lstlisting}
+AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea,
+  SurfaceELR,           !- Name of surface effective leakage area component
+  0.07,                 !- Effective leakage area {dimensionless}
+  1.00,                 !- Discharge coefficient {dimensionless}
+  4.0,                  !- Reference pressure difference {Pa}
+  0.65;                 !- Air mass flow exponent {dimensionless}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:MultiZone:Component:DetailedOpening}\label{airflownetworkmultizonecomponentdetailedopening}
+
+This object specifies the properties of air flow through windows and doors (window, door and glass door heat transfer subsurfaces) when they are closed or open. The fields are similar to those for AirflowNetwork:Multizone:SurfaceCrack object when the window or door is closed, but additional fields are required to describe the air flow characteristics when the window or door is open. These additional fields include opening type, opening dimensions, degree of opening, and opening schedule.
+
+The AirflowNetwork model assumes that open windows or doors are vertical or close to vertical; for this reason they are called ``Large Vertical Openings.'' Such openings can have air flow moving simultaneously in two different directions depending on stack effects and wind conditions (for example, flow from inside to outside at the top of a window and from outside to inside at the bottom). AirflowNetwork models such two-directional flow, but only for vertical openings.
+
+It is assumed that the air flow through a window opening is unaffected by the presence of a shading device such as a shade or blind on the window. Also, the calculation of conductive heat transfer and solar gain through a window or door assumes that the window or door is closed.
+
+The AirflowNetwork model does not have a model for bi-directional flow through large horizontal openings. For this reason, \textbf{Air\-flow\-Net\-work:\-Multi\-Zone:\-Component:\-Detailed\-Opening should not be used for horizontal openings}. The best modeling technique in this case is to put an Air\-flow\-Net\-work:\-Multi\-Zone:\-Sur\-face:\-Crack object in a horizontal surface and use a large air mass flow coefficient. Crack flow is assumed to be uni-directional in any given timestep (but can reverse flow direction from timestep to timestep).
+
+A subsurface multiplier may be used to represent multiple subsurfaces and calculates total air flow when the subsurface (window, glassdoor, or door) is either closed or open. The total airflow across the surface is equal to the airflow based on the surface geometry multiplied by the subsurface multiplier.
+
+\subsubsection{Inputs}\label{inputs-4-003}
+
+\paragraph{Field: Name}\label{field-name-4-003}
+
+The name of this Air\-flow\-Net\-work:\-Multi\-Zone:\-Com\-ponent:\-Detailed\-Opening object. It is referenced by an Air\-flow\-Net\-work:\-Multi\-zone:\-Surface object.
+
+\paragraph{Field: Air Mass Flow Coefficient When Opening is Closed}\label{field-air-mass-flow-coefficient-when-opening-is-closed}
+
+Crack flow is assumed when the window or door is closed. The units for this air mass flow coefficient (\({C_{Q,\;unit\;length}}\) ) are different from the units for \({C_Q}\) (kg/s at 1 Pa pressure difference) defined in an Air\-flow\-Net\-work:\-Multi\-Zone:\-Sur\-face:\-Crack object. There is no default but the entered value must be greater than zero. The program will automatically generate four cracks around the perimeter of the window or door--one along the bottom, one along the top, and one on each side. The temperature correction factor used in the Air\-flow\-Net\-work:\-Multi\-Zone:\-Sur\-face:\-Crack object is not used for this component to calculate air mass flow rate.
+
+\paragraph{Field: Air Mass Flow Exponent When Opening Is Closed}\label{field-air-mass-flow-exponent-when-opening-is-closed}
+
+Crack flow is assumed when the window or door is closed. In this case, the value of this field is the exponent, \emph{n}, in the crack air flow equation. The valid range for this exponent is 0.5 to 1.0, with the default value being 0.65. Mass Flow Rate = Air Mass Flow Coefficient (deltaP) Air Mass Flow Exponent.
+
+\paragraph{Field: Type of Rectanguler Large Vertical Opening (LVO)}\label{field-type-of-rectanguler-large-vertical-opening-lvo}
+
+This alpha field specifies the type of rectangular window or door. (Open windows or doors are also called Large Vertical Openings (LVOs). The choices for the opening type are \textbf{NonPivoted} (LVO Type 1) and \textbf{HorizontallyPivoted} (LVO Type 2) with the default being \textbf{NonPivoted}. The NonPivoted type represents a regular window or door. The HorizontallyPivoted type represents a window with a horizontal axis (i.e., a horizontally-pivoting window) and cannot be used for a door.
+
+\paragraph{Field: Extra Crack Length or Height of Pivoting Axis}\label{field-extra-crack-length-or-height-of-pivoting-axis}
+
+Specifies window or door characteristics that depend on the LVO type.
+
+For LVO Type 1 (rectangular non-pivoted windows and doors) this field is the extra crack length in meters due to multiple openable parts, if present. ``Extra'' here means in addition to the length, calculated by the program, of the cracks on the top, bottom and sides of the window/door.
+
+For LVO Type 2 (rectangular horizontally-pivoted windows) this field gives the height of the pivoting axis measured from the bottom of the glazed part of the window (m).
+
+\paragraph{Field: Number of Sets of Opening Factor Data}\label{field-number-of-sets-of-opening-factor-data}
+
+This is the number of the following sets of data for opening factor, discharge coefficient, width factor, height factor, and start height factor. From two to four of these sets must be defined. The first set should be for Opening Factor = 0.0 and the last set should be for Opening Factor = 1.0. For example, if only two sets are defined, the first set should be for Opening Factor = 0.0 and the second set should be for Opening Factor = 1.0, as shown below in the IDF example below.
+
+An ``opening factor'' refers to the amount that a window or door is opened. The program linearly interpolates each timestep between the values of discharge coefficient, width factor, etc., in these sets using the opening factor for the window or door for the timestep. (See discussion under the field Window/Door Opening Factor in the Air\-flow\-Net\-work:\-Multi\-zone:\-Zone object for a description of how the Air\-flow\-Net\-work model determines the time-step value of the opening factor.)
+
+\paragraph{Field Group: Opening Factor, Discharge Coefficient, Width Factor, Height Factor, Start Height Factor}\label{field-group-opening-factor-discharge-coefficient-width-factor-height-factor-start-height-factor}
+
+Each field is described for as many groups as required in the previous field (number of sets of opening factor data). As the final field has specific requirements, this field (n) will be described.
+
+\paragraph{Field: Opening Factor 11}\label{field-opening-factor-11}
+
+The first opening factor of a window or door. This value must be 0.0. The default value is also 0.0.
+
+For LVO Type 1 (rectangular non-pivoted window or door), the Opening Factor corresponds to the fraction of window or door that is opened.
+
+For LVO Type 2 (rectangular horizontally-pivoted windows), the Opening Factor is determined by the window opening angle. For example, an opening angle of 45° corresponds to an Opening Factor of 0.50 since the maximum opening angle is 90°.
+
+\paragraph{Field: Discharge Coefficient for Opening Factor 1}\label{field-discharge-coefficient-for-opening-factor-1}
+
+The discharge coefficient of the window or door for Opening Factor 1. The range is greater than 0.0 to less than or equal to 1.0. The default value is 0.001. The Discharge Coefficient indicates the fractional effectiveness for air flow through a window or door at that Opening Factor.
+
+\textbf{Note:} In the following, ``window width'' and ``window height'' are glazing dimensions; they do not include the frame, if present.
+
+\paragraph{Field: Width Factor for Opening Factor 1}\label{field-width-factor-for-opening-factor-1}
+
+The Width Factor of the rectangular window or door for Opening Factor 1. The Width Factor is the opening width divided by the window or door width (see Figure~\ref{fig:window-or-door-showing-geometrical-factors}). The range is 0.0 to 1.0. The default value is 0.0. Note that the width factor applies to rectangular windows or doors where the width is assumed constant along the entire height of the opening.
+
+\paragraph{Field: Height Factor for Opening Factor 1}\label{field-height-factor-for-opening-factor-1}
+
+The Height Factor of the rectangular window or door for Opening Factor 1. The Height Factor is the opening height divided by the window or door height (see Figure~\ref{fig:window-or-door-showing-geometrical-factors}). The range is 0.0 to 1.0. The default value is 0.0. Note that the height factor applies to rectangular windows or doors where the height is assumed constant along the entire width of the opening.
+
+\paragraph{Field: Start Height Factor for Opening Factor 1}\label{field-start-height-factor-for-opening-factor-1}
+
+The Start Height Factor of the window or door for Opening Factor 1. The Start Height Factor is the Start Height divided by the window or door height (see Figure~\ref{fig:window-or-door-showing-geometrical-factors}). The range is 0.0 to 1.0. The default is 0. Start Height is the distance between the bottom of the window or door and the bottom of the window or door opening. The sum of the Height Factor and the Start Height Factor must be less than 1.0 in order to have the opening within the window or door dimensions.
+
+\begin{figure}[hbtp] % fig 98
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image236.png}
+\caption{Window (or door) showing geometrical factors associated with an opening through which air flows. \protect \label{fig:window-or-door-showing-geometrical-factors}}
+\end{figure}
+
+\paragraph{Field: Opening Factor \textless{}n\textgreater{}}\label{field-opening-factor-n}
+
+When Number of Sets of Opening Factor Data = n, the value of Opening Factor n must be set to 1.0.
+
+\paragraph{Field: Discharge Coefficient for Opening Factor \textless{}n\textgreater{}}\label{field-discharge-coefficient-for-opening-factor-n}
+
+The discharge coefficient of the window or door for Opening Factor n. The range is greater than 0.0 to less than or equal to 1.0. The default value is 1.0.
+
+\paragraph{Field: Width Factor for Opening Factor \textless{}n\textgreater{}}\label{field-width-factor-for-opening-factor-n}
+
+The Width Factor of the rectangular window or door for Opening Factor n. The Width Factor is the opening width divided by the window or door width (see Figure~\ref{fig:window-or-door-showing-geometrical-factors}). The range is 0.0 to 1.0. The default value is 1.0.
+
+\paragraph{Field: Height Factor for Opening Factor \textless{}n\textgreater{}}\label{field-height-factor-for-opening-factor-n}
+
+The Height Factor of the rectangular window or door for Opening Factor n. The Height Factor is the opening height divided by the window or door height (see Figure~\ref{fig:window-or-door-showing-geometrical-factors}). The range is 0.0 to 1.0. The default value is 1.0.
+
+\paragraph{Field: Start Height Factor for Opening Factor \textless{}n\textgreater{}}\label{field-start-height-factor-for-opening-factor-n}
+
+The Start Height Factor of the window or door for Opening Factor n. The Start Height Factor is the Start Height divided by the window or door height (see Figure~\ref{fig:window-or-door-showing-geometrical-factors}). The range is 0.0 to 1.0. The default is 0.
+
+When the opening factor value (as described under the field Window/Door Opening Factor in the AirflowNetwork:Multizone:Surface object) is between two Opening Factor field values, the values of Discharge Coefficient, Width Factor, Height Factor, and Start Height Factor are linearly interpolated.
+
+An IDF example is shown below:
+
+\begin{lstlisting}
+
+AirflowNetwork:MultiZone:Component:DetailedOpening,
+      WiOpen1,                 !- Detailed Opening Name
+      0.001,                   !- Air Mass Flow Coefficient When Opening is Closed {kg/s-m}
+      0.667,                   !- Air Mass Flow Exponent When Opening is Closed {dimensionless}
+      NonPivoted,             !- Type of Large Vertical Opening (LVO)
+      0.0,                     !- Extra crack length for LVO type 1 with multiple openable parts,
+                               !- or Height of pivoting axis for LVO type 2 {m}
+      2,                       !- Number of Sets of Opening Factor Data
+      0.0,                     !- Opening factor 1 {dimensionless}
+      0.5,                     !- Discharge coefficient for opening factor 1 {dimensionless}
+      0.0,                     !- Width factor for opening factor 1 {dimensionless}
+      1.0,                     !- Height factor for opening factor 1 {dimensionless}
+      0.0,                     !- Start height factor for opening factor 1 {dimensionless}
+      1.0,  0.6,  1.0,  1.0,  0.0;  !-  Set of values for opening factor 2
+\end{lstlisting}
+
+\subsection{AirflowNetwork:MultiZone:Component:HorizontalOpening}\label{airflownetworkmultizonecomponenthorizontalopening}
+
+This object specifies the properties of air flow through windows, doors and glass doors (heat transfer subsurfaces defined as a subset of FenestrationSurface:Detailed objects) when they are closed or open. This AirflowNetwork model assumes that these openings are horizontal or close to horizontal and are interzone surfaces. The second and third input fields are similar to those for AirflowNetwork:MultiZone:Surface:Crack, when the window or door is closed, but additional information is required to describe the air flow characteristics when the window or door is open. This additional information is specified in the last two input fields. The airflow across the opening consists of two types of flows: forced and buoyancy. The forced flow is caused by the pressure difference between two zones, while the buoyancy flow only occurs when the air density in the upper zone is greater than the air density in the lower zone. This opening also allows for the possibility of two-way flow when forced and buoyancy flows co-exist. This object's openness can also be modulated based on the same opening factor control as an AirflowNetwork:MultiZone:Component:DetailedOpening object. However, the opening factor is only applied to the subsurface width. The opening width is equal to opening factor multiplied by the subsurface width.
+
+A subsurface multiplier may be used to represent multiple subsurfaces and calculates total air flow when the subsurface (window, glassdoor, or door) is either closed or open. The total airflow across the surface is equal to the airflow based on the surface geometry multiplied by the subsurface multiplier.
+
+\subsubsection{Inputs}\label{inputs-5-003}
+
+\paragraph{Field: Name}\label{field-name-5-003}
+
+This is a name for this AirflowNetwork:MultiZone:Component:HorizontalOpening object. It is referenced by an AirflowNetwork:Multizone:Surface object.
+
+\paragraph{Field: Air Mass Flow Coefficient When Opening is Closed}\label{field-air-mass-flow-coefficient-when-opening-is-closed-1}
+
+The value of the air mass flow coefficient, \({C_{Q,\;unit\;length}}\) , in the horizontal opening air flow equation. It has units of kg/s-m at 1Pa. The temperature correction factor is not applied to the mass flow calculation. This is a required input field and the entered value must be greater than zero.
+
+\paragraph{Field: Air Mass Flow Exponent When Opening is Closed}\label{field-air-mass-flow-exponent-when-opening-is-closed-1}
+
+The value of the exponent,* n*, in the crack air flow equation. The valid range is 0.5 to 1.0, with the default value being 0.65.
+
+\paragraph{Field: Sloping Plane Angle}\label{field-sloping-plane-angle}
+
+This numeric field is used to represent the angle between the horizontal plane and a sloped plane under the horizontal opening. Sloping plane angle = 90 is equivalent to fully open. The valid range is \textgreater{}0 to 90, with the default value being 90.
+
+\paragraph{Field: Discharge Coefficient}\label{field-discharge-coefficient-1}
+
+This numeric field is used to input the discharge coefficient. This is a required field and the entered value must be greater than zero.
+
+An IDF example is shown below:
+
+\begin{lstlisting}
+
+AirflowNetwork:MultiZone:Component:HorizontalOpening,
+      HrOpen,                  !- Name
+      0.001,                   !- Air Mass Flow Coefficient When Opening is Closed {kg/s-m}
+      0.667,                   !- Air Mass Flow Exponent When Opening is Closed {dimensionless}
+      90.0,                    !- Sloping Plane Angle
+      0.2;                     !- Discharge Coefficient
+\end{lstlisting}
+
+\subsection{AirflowNetwork:MultiZone:Component:SimpleOpening}\label{airflownetworkmultizonecomponentsimpleopening}
+
+This object specifies the properties of air flow through windows, doors and glass doors (heat transfer subsurfaces) when they are closed or open. The AirflowNetwork model assumes that open windows or doors are vertical or close to vertical. The second and third fields are similar to those for AirflowNetwork:MultiZone:Surface:Crack, when the window or door is closed, but additional information is required to describe the air flow characteristics when the window or door is open. This additional information is specified in the last two fields. Compared to the object AirflowNetwork:MultiZone:Component:DetailedOpening, which requires more inputs at different opening factors, this object needs comparatively less inputs. For this reason it is called a simple opening. This opening also allows for the possibility of two-way flow due to temperature and resulting density differences. Therefore, it is possible to have a positive pressure difference at the top of the opening, and a negative pressure difference at the bottom (or vice versa) when the neutral height is between the bottom and top heights of the associated surface. This object's openness can also be modulated based on the same opening factor control as an AirflowNetwork:MultiZone:Component:DetailedOpening object. However, the opening factor is only applied to the subsurface width. The opening width is equal to opening factor multiplied by the subsurface width.
+
+A subsurface multiplier may be used to represent multiple subsurfaces and calculates total air flow when the subsurface (window, glassdoor, or door) is either closed or open. The total airflow across the surface is equal to the airflow based on the surface geometry multiplied by the subsurface multiplier.
+
+\subsubsection{Inputs}\label{inputs-6-002}
+
+\paragraph{Field: Name}\label{field-name-6-002}
+
+This is a name for this AirflowNetwork:MultiZone:Component:SimpleOpening object. It is referenced by an AirflowNetwork:Multizone:Surface object.
+
+\paragraph{Field: Air Mass Flow Coefficient When Opening is Closed}\label{field-air-mass-flow-coefficient-when-opening-is-closed-2}
+
+The value of the air mass flow coefficient, \({C_{Q,\;unit\;length}}\) , in the simple opening air flow equation. It has units of kg/s-m at 1Pa. The temperature correction factor is not applied for mass flow calculation.
+
+\paragraph{Field: Air Mass Flow Exponent When Opening is Closed}\label{field-air-mass-flow-exponent-when-opening-is-closed-2}
+
+The value of the exponent,* n\emph{, in the crack air flow equation. The valid range is 0.5 to 1.0, with the default value being 0.65. Mass Flow Rate = Air Mass Flow Coefficient} (deltaP)\^{}Air Mass Flow Exponent.
+
+\paragraph{Field: Minimum Density Difference for Two-Way Flow}\label{field-minimum-density-difference-for-two-way-flow}
+
+This numeric field is used to input the minimum density difference above which two-way or one way flow may occur due to stack effect with the window being open. Two-way flow occurs only when the neutral plane is within the opening. Density differences less than this value result in one-way flow only with the window being closed. The minimum value for this field is greater than zero.
+
+\paragraph{Field: Discharge Coefficient}\label{field-discharge-coefficient-2}
+
+This numeric field is used to input the discharge coefficient. This value must be greater than zero.
+
+An IDF example is shown below:
+
+\begin{lstlisting}
+
+ AirflowNetwork:MultiZone:Component:SimpleOpening,
+      WiOpen2,                 !- Simple Opening Name
+      0.001,                   !- Air Mass Flow Coefficient When Opening Is Closed {kg/s-m}
+      0.650,                   !- Air Mass Flow Exponent When Opening Is Closed {dimensionless}
+      0.0001,                  !- Minimum density difference for two-way flow (kg/m3)
+      1.0;                     !- Discharge coefficient (dimensionless)
+\end{lstlisting}
+
+\subsection{AirflowNetwork:MultiZone:Component:ZoneExhaustFan}\label{airflownetworkmultizonecomponentzoneexhaustfan}
+
+This object specifies the properties of air flow through an exterior heat transfer surface with a zone exhaust fan. The zone exhaust fan turns on or off based on the availability schedule defined in the corresponding Fan:ZoneExhaust object. When the exhaust fan mass flow rate is greater than zero, the airflow network model treats this object as a constant volume fan. When the fan is off based on the availability schedule, the model treats this object as a crack.
+
+When the fan is on, the air mass flow rate modeled for the airflow network is based on the value defined in the MaximumFlow Rate field of the Fan:ZoneExhaust object. The airflow direction is from the corresponding zone to outdoors.
+
+When the fan is off, the following power law form is used that gives air flow through the crack as a function of the pressure difference across the crack: 
+
+\begin{equation}
+Q = \left( Crack\;Factor \right) * C_T * C_Q \left( \Delta P \right)^{n}
+\end{equation}
+
+Where
+
+\emph{Q}~~~ = air mass flow (kg/s)
+
+\emph{C\(_{Q}\)}~ = air mass flow coefficient (kg/s-Pa\(^{n}\) @ 1 Pa)
+
+\emph{C\(_{T}\)}~ = reference condition temperature correction factor (dimensionless)
+
+\(\Delta P\) = pressure difference across crack (Pa)
+
+\emph{n}~~~ = air flow exponent (dimensionless)
+
+\begin{equation}
+{C_T} = {\left[ {\frac{{{\rho_o}}}{\rho }} \right]^{n - 1}}{\left[ {\frac{{{\nu_o}}}{\nu }} \right]^{2n - 1}}
+\end{equation}
+
+where
+
+\(\rho\) = Air density at the specific air temperature and humidity ratio conditions {[}kg/m\(^{3}\){]}
+
+\(\nu\) = Air kinetic viscosity at the specific air temperature condition {[}m\(^{2}\)/s{]}
+
+\(\rho_o\) = Air density at the reference air conditions provided by the object Air\-flow\-Net\-work:\-Multi\-Zone:\-Reference\-Crack\-Con\-ditions specified in the field Reference Crack Conditions {[}kg/m\(^{3}\){]}
+
+\(\nu_o\) = Air kinetic viscosity at the reference air temperature provided by the object Air\-flow\-Net\-work:\-Multi\-Zone:\-Reference\-Crack\-Con\-ditions specified in the field Reference Crack Conditions {[}m\(^{2}\)/s{]}
+
+Note: The correction factor shown above is used when the exhaust fan is off. The airflow direction is based on the pressure difference between the zone and outdoors.
+
+\subsubsection{Inputs}\label{inputs-7-002}
+
+\paragraph{Field: Name}\label{field-name-7-001}
+
+This is the name for this instance of the Air\-flow\-Net\-work:\-Multi\-Zone:\-Com\-ponent:\-Zone\-Exhaust\-Fan object. This name must be the same name defined in the Fan:\-Zone\-Exhaust object. It is referenced by an Air\-flow\-Net\-work:\-Multi\-zone:\-Sur\-face object.
+
+\paragraph{Field: Air Mass Flow Coefficient When the Zone Exhaust Fan is Off at Reference Conditions}\label{field-air-mass-flow-coefficient-when-the-zone-exhaust-fan-is-off-at-reference-conditions}
+
+The value of the air mass flow coefficient,\({C_Q}\) , in the crack air flow equation. It has units of kg/s at 1Pa. This value must be greater than zero. The value is used when the fan is off.
+
+\paragraph{Field: Air Mass Flow Exponent When the Zone Exhaust Fan is Off}\label{field-air-mass-flow-exponent-when-the-zone-exhaust-fan-is-off}
+
+The value of the exponent,* n*, in the crack air flow equation. The valid range is 0.5 to 1.0, with the default value being 0.65. The value is used when the fan is off.
+
+\paragraph{Field: Reference Crack Conditions}\label{field-reference-crack-conditions-1}
+
+The name of the AirflowNetwork:MultiZone:ReferenceCrackConditions object which specifies the conditions under which the air mass flow coefficient was measured. If the user omits this field and only one AirflowNetwork:MultiZone:ReferenceCrackConditions object is defined in the input data file, then those reference crack conditions will be used. If the user omits this field and either zero or more than one AirflowNetwork:MultiZone:ReferenceCrackConditions objects are defined in the input data file, then the default conditions for the AirflowNetwork:Multizone: Reference Crack Conditions object will be used.
+
+An IDF example is shown below:
+
+\begin{lstlisting}
+
+AirflowNetwork:MultiZone:Component:ZoneExhaustFan,
+      Zone3 Exhaust Fan,       !- Name
+      0.01,     !- Air Mass Flow Coefficient When the Zone Exhaust Fan is Off at Reference Conditions {kg/s}
+      0.667;    !- Air Mass Flow Exponent When the Zone Exhaust Fan is Off{dimensionless}
+      ReferenceCrackConditions; !- Reference Crack Conditions
+\end{lstlisting}
+
+\subsection{AirflowNetwork:MultiZone:ExternalNode}\label{airflownetworkmultizoneexternalnode}
+
+External nodes in the AirflowNetwork model define environmental conditions outside of the building. These conditions include wind pressure coefficients that vary from façade to façade and can be highly dependent on the building geometry.
+
+AirflowNetwork:MultiZone:ExternalNode objects do \textbf{not} have to be entered if Wind Pressure Coefficient Type = SurfaceAverageCalculation in the AirflowNetwork:SimulationControl object.
+
+\subsubsection{Inputs}\label{inputs-8-001}
+
+\paragraph{Field: Name}\label{field-name-8-001}
+
+The external node name is associated with a particular building façade. This name is referenced by the External Node Name field of an AirflowNetwork:MultiZone:WindPressureCoefficientValues object (which gives wind pressure coefficients for the façade as a function of angle of wind incident on the façade) and by the External Node Name field of an AirflowNetwork:MultiZone:Surface object.
+
+\paragraph{Field: External Node Height}\label{field-external-node-height}
+
+Designates the reference height, in meters, used to calculate relative pressure. The default value is 0 meters.
+
+\paragraph{Field: Wind Pressure Coefficient Values Object Name}\label{field-wind-pressure-coefficient-values-object-name}
+
+The name of a specific AirflowNetwork:MultiZone:WindPressureCoefficientValues object (which gives wind pressure coefficients for the façade as a function of angle of wind incident on the façade).
+
+IDF examples are provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:MultiZone:ExternalNode,
+      NFacade,                 !- Name
+      1.524,                   !- External Node Height {m}
+      NFacade_WPCValue;        !- Wind Pressure Coefficient Values Object Name
+
+  AirflowNetwork:MultiZone:ExternalNode,
+      EFacade,                 !- Name
+      1.524,                   !- External Node Height {m}
+      EFacade_WPCValue;        !- Wind Pressure Coefficient Values Object Name
+
+  AirflowNetwork:MultiZone:ExternalNode,
+      SFacade,                 !- Name
+      1.524,                   !- External Node Height {m}
+      SFacade_WPCValue;        !- Wind Pressure Coefficient Values Object Name
+
+  AirflowNetwork:MultiZone:ExternalNode,
+      WFacade,                 !- Name
+      1.524,                   !- External Node Height {m}
+      WFacade_WPCValue;        !- Wind Pressure Coefficient Values Object Name
+
+  AirflowNetwork:MultiZone:ExternalNode,
+      Horizontal,              !- Name
+      3.028,                   !- External Node Height {m}
+      Horizontal_WPCValue;     !- Wind Pressure Coefficient Values Object Name
+\end{lstlisting}
+
+\subsection{AirflowNetwork:MultiZone:WindPressureCoefficientArray}\label{airflownetworkmultizonewindpressurecoefficientarray}
+
+The reference height and wind directions are first specified under the AirflowNetwork:MultiZone:WindPressureCoefficientArray object. The user may specify up to 36 different wind directions in ascending order. These are then referenced by AirflowNetwork:MultiZone:WindPressureCoefficientValues objects defined for each AirflowNetwork:MultiZone:ExternalNode.
+
+The AirflowNetwork:MultiZone:WindPressureCoefficientArray object is unique and needs to be entered only if Wind Pressure Coefficient Type = INPUT in the AirflowNetwork:SimulationControl object. If Wind Pressure Coefficient Type = SurfaceAverageCalculation, this object is not required.
+
+\subsubsection{Inputs}\label{inputs-9-001}
+
+\paragraph{Field: Name}\label{field-name-9-001}
+
+The name of this AirflowNetwork:MultiZone:WindPressureCoefficientArray object. This name is referenced by each AirflowNetwork:MultiZone:WindPressureCoefficientValues object which, for each AirflowNetwork:MultiZone:ExternalNode, gives the wind pressure coefficients at each of the wind directions listed in the AirflowNetwork:MultiZone:WindPressureCoefficientArray. This name is also referenced by the AirflowNetwork:SimulationControl object, indicating that this AirflowNetwork:MultiZone:WindPressureCoefficientArray and the pressure coefficients in the associated AirflowNetwork:MultiZone:WindPressureCoefficientValues objects will be used in the air flow simulation.
+
+\paragraph{Field: Wind Direction 1-Wind Direction N}\label{field-wind-direction-1-wind-direction-n}
+
+Each field references the wind direction corresponding to the first through the Nth WPC value in each of the AirflowNetwork:MultiZone:WindPressureCoefficientValues objects. \emph{N} can be as high as 36.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:MultiZone:WindPressureCoefficientArray,
+      Every 30 Degrees,        !- WPC Array Name
+      0,                       !- Wind Direction #1 {deg}
+      30,                      !- Wind Direction #2 {deg}
+      60,                      !- Wind Direction #3 {deg}
+      90,                      !- Wind Direction #4 {deg}
+      120,                     !- Wind Direction #5 {deg}
+      150,                     !- Wind Direction #6 {deg}
+      180,                     !- Wind Direction #7 {deg}
+      210,                     !- Wind Direction #8 {deg}
+      240,                     !- Wind Direction #9 {deg}
+      270,                     !- Wind Direction #10 {deg}
+      300,                     !- Wind Direction #11 {deg}
+      330;                     !- Wind Direction #12 {deg}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:MultiZone:WindPressureCoefficientValues}\label{airflownetworkmultizonewindpressurecoefficientvalues}
+
+This object specifies up to 36 wind pressure coefficients (WPCs) for an AirflowNetwork:MultiZone:ExternalNode. These coefficients are defined for each of the wind directions defined in the unique AirflowNetwork:MultiZone:WindPressureCoefficientArray object. In the air flow calculation, interpolation of the specified WPC values is done for time-step values of wind direction.
+
+AirflowNetwork:MultiZone:WindPressureCoefficientValues objects need to be entered only if the Wind Pressure Coefficient Type = INPUT in the AirflowNetwork:SimulationControl object. If Wind Pressure Coefficient Type = SurfaceAverageCalculation, this object is not required and is not used.
+
+\subsubsection{Inputs}\label{inputs-10-001}
+
+\paragraph{Field: Name}\label{field-name-10-001}
+
+The name of this WindPressureCoefficientValues object. This name can be referenced by multiple AirflowNetwork:MultiZone:ExternalNode objects.
+
+\paragraph{Field: WindPressureCoefficientArray Name}\label{field-windpressurecoefficientarray-name}
+
+Name of the associated AirflowNetwork:MultiZone:WindPressureCoefficientArray, which lists the wind direction corresponding to each wind pressure coefficient value in this AirflowNetwork:MultiZone:WindPressureCoefficientValues object.
+
+\paragraph{Field: Wind Pressure Coefficient Value 1 to Wind Pressure Coefficient Value N}\label{field-wind-pressure-coefficient-value-1-to-wind-pressure-coefficient-value-n}
+
+The WPC (wind pressure coefficient) value for the building façade indicated by the External Node Name field above. This WPC value corresponds to the first wind direction in the AirflowNetwork:MultiZone:WindPressureCoefficientArray. Note that WPC values can be positive, negative or zero.
+
+\paragraph{Obtaining WPC values}\label{obtaining-wpc-values}
+
+WPC values can be obtained from wind tunnel measurements, CFD calculations, or from published values for different building shapes.
+
+For \textbf{rectangular buildings} EnergyPlus will automatically calculate surface-averaged Cp values for the walls and roof of the building if you specify Wind Pressure Coefficient Type = SurfaceAverageCalculation in the AirflowNetwork:SimulationControl object. In this case you do not have to enter any AirflowNetwork:MultiZone:WindPressureCoefficientValues objects.
+
+Wind pressure coefficients are reported in the eplusout.eio either from inputs using ``INPUT'' as the choice for the Wind Pressure Coefficient Type field defined in the AirflowNetwork:SimulationControl object, or from internal calculation using SurfaceAverageCalculation as the choice for the Wind Pressure Coefficient Type field defined in the same object. Below is an output example from the eplusout.eio file:
+
+\begin{lstlisting}
+AirflowNetwork Model:Wind Direction, 0.0,30.0,60.0,90.0,120.0,150.0,180.0,210.0,240.0,270.0,300.0,330.0
+! <AirflowNetwork Model:Wind Pressure Coefficients, WPC Name, Wind Pressure Coefficients #1 to n (dimensionless)>
+AirflowNetwork Model:Wind Pressure Coefficients, NFACADE, 0.60,0.48,4.00E-002,-0.56,-0.56,-0.42,-0.37,-0.42,-0.56,-0.56,4.00E-002,0.48
+AirflowNetwork Model:Wind Pressure Coefficients, EFACADE, -0.56,4.00E-002,0.48,0.60,0.48,4.00E-002,-0.56,-0.56,-0.42,-0.37,-0.42,-0.56
+AirflowNetwork Model:Wind Pressure Coefficients, SFACADE, -0.37,-0.42,-0.56,-0.56,4.00E-002,0.48,0.60,0.48,4.00E-002,-0.56,-0.56,-0.42
+AirflowNetwork Model:Wind Pressure Coefficients, WFACADE, -0.56,-0.56,-0.42,-0.37,-0.42,-0.56,-0.56,4.00E-002,0.48,0.60,0.48,4.00E-002
+\end{lstlisting}
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:MultiZone:WindPressureCoefficientValues,
+      NFacade_WPCValue,        !- Name
+      Every 30 Degrees,        !- AirflowNetwork:MultiZone:WindPressureCoefficientArray Name
+      0.60,                    !- Wind Pressure Coefficient Value 1 {dimensionless}
+      0.48,                    !- Wind Pressure Coefficient Value 2 {dimensionless}
+      0.04,                    !- Wind Pressure Coefficient Value 3 {dimensionless}
+      -0.56,                   !- Wind Pressure Coefficient Value 4 {dimensionless}
+      -0.56,                   !- Wind Pressure Coefficient Value 5 {dimensionless}
+      -0.42,                   !- Wind Pressure Coefficient Value 6 {dimensionless}
+      -0.37,                   !- Wind Pressure Coefficient Value 7 {dimensionless}
+      -0.42,                   !- Wind Pressure Coefficient Value 8 {dimensionless}
+      -0.56,                   !- Wind Pressure Coefficient Value 9 {dimensionless}
+      -0.56,                   !- Wind Pressure Coefficient Value 10 {dimensionless}
+      0.04,                    !- Wind Pressure Coefficient Value 11 {dimensionless}
+      0.48;                    !- Wind Pressure Coefficient Value 12 {dimensionless}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:OccupantVentilationControl}\label{airflownetworkoccupantventilationcontrol}
+
+The AirflowNetwork:OccupantVentilationControl object provides control options with minimum opening and closing time checks and opening and closing probability values. In general, the probability values could be a constant or a specific function. Due to lack of real data, two schedules are selected to represent probability values. If real data are available, this object may be modified to adopt new data.
+
+\subsubsection{Inputs}\label{inputs-11-001}
+
+\paragraph{Field: Name}\label{field-name-11-001}
+
+This is the name of the object.
+
+\paragraph{Field: Minimum Opening Time}\label{field-minimum-opening-time}
+
+The field represents the minimum time that windows will remain open. If a window has been open for a time less than this value, the window will remain open.
+
+\paragraph{Field: Minimum Closing Time}\label{field-minimum-closing-time}
+
+The field represents the minimum time that windows will remain closed. If a window has been closed for a time less than this value, the window will remain closed.
+
+\paragraph{Field: Thermal Comfort Low Temperature Curve Name}\label{field-thermal-comfort-low-temperature-curve-name}
+
+This alpha field defines the name of a curve to be used for thermal comfort temperature calculation at low outdoor dry-bulb temperature. This curve is a linear or quadratic equation using outdoor dry-bulb temperatures as an independent variable. This performance curve can be used to describe the thermal comfort temperature at low outdoor dry-bulb temperature. It allows maximum two curves to describe the thermal comfort temperature in two different outdoor dry-bulb temperature regions. If a single curve is used, blanks are entered in the following two fields.
+
+\paragraph{Field: Thermal Comfort Temperature Boundary Point}\label{field-thermal-comfort-temperature-boundary-point}
+
+When there are two piecewise curves to represent thermal comfort temperature calculation, this field represents a boundary point of outdoor dry-bulb temperature. The low temperature curve and the high temperature curve should have the same values at the boundary point. If a single curve is used, this field may be left blank.
+
+\paragraph{Field: Thermal Comfort High Temperature Curve Name}\label{field-thermal-comfort-high-temperature-curve-name}
+
+This alpha field defines the name of a curve to be used for thermal comfort temperature calculation at high outdoor dry-bulb temperature. This curve is a linear or quadratic equation using outdoor dry-bulb temperatures as an independent variable. This performance curve can be used to describe the thermal comfort temperature at high outdoor dry-bulb temperature. It allows maximum two curves to describe the thermal comfort temperature in two different outdoor dry-bulb temperature regions. If a single curve is used, blanks are entered in this field.
+
+\paragraph{Field: Maximum Threshold for Persons Dissatisfied PPD}\label{field-maximum-threshold-for-persons-dissatisfied-ppd}
+
+This field is used to calculate the comfort band as a function of predicted percentage of dissatisfied (PPD). The default value is 10\%. The equation is based on curve fit and is valid between 0\% and 35\%.
+
+\begin{equation}
+\Theta = -0.0028 (100-PPD)^2 + 0.3419 (100-PPD) - 6.6275
+\end{equation}
+
+where
+
+\begin{itemize}
+\tightlist
+\item
+  \(\Theta\) is the comfort band (degC)
+\item
+  PPD is predicted percentage person of dissatisfied (\%)
+\end{itemize}
+
+\paragraph{Field: Occupancy Check}\label{field-occupancy-check}
+
+Input is Yes or No. The default is No. If Yes, an occupancy check is performed used in the opening probability check. If No, the occupancy check is bypassed.
+
+\paragraph{Field: Opening Probability Schedule Name}\label{field-opening-probability-schedule-name}
+
+The name of a schedule of opening probability that controls the opening of windows and doors in the thermal zone to provide natural ventilation. If the probability value is greater a random number, windows are allowed to open. Otherwise, the output will be false. This control will occur when minimum time checks for both opening and closing are satisfied.
+
+\paragraph{Field: Closing Probability Schedule Name}\label{field-closing-probability-schedule-name}
+
+The name of a schedule of closing probability that controls the closing of windows and doors in the thermal zone to reduce natural ventilation. If the probability value is greater a random number, windows are allowed to be closed. Otherwise, the output will be false. This control will occur when minimum time checks for both opening and closing are satisfied.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirlowNetwork:OccupantVentilationControl,
+  VentilationControl,      !- Name
+  5.0,                     !- Minimum Opening Time
+  5.0,                     !- Minimum Opening Time
+  ComfortLowTempCurve,     !- Thermal Comfort Low Temperature Curve Name
+  10.0,                    !- Thermal Comfort Temperature Boundary Point
+  ComfortHighTempCurve,    !- Thermal Comfort High Temperature Curve Name
+  10.0,                    !- Maximum Threshold for Persons Dissatisfied PPD
+  Yes,                     !- Occupancy Check
+  OpeningProbabilitySch,   !- Opening Probability Schedule Name
+  ClosingProbabilitySch;   !- Closing Probability Schedule Name
+\end{lstlisting}
+
+The next two objects of AirflowNetwork:Intrazone:Node and AirflowNetwork:Intrazone:Linkage are used with RoomAir:Node:AirflowNetwork objects together to simulate multiple internal airflows via multiple intrazone nodes and linkages in a thermal zone. The mixed-air assumption for zone air conditions is not always appropriate. EnergyPlus includes several RoomAir models that can model the implications for different flow patterns on variations in temperature within the zone. However none of them are generalized enough for different types of air flow situations and none are coupled tightly with AirflowNetwork. A general RoomAir model based on pressure network solver will allow modeling a variety of spaces types not currently covered by existing models such as tall spaces.
+
+Recent advancements have been made to AirflowNetwork to model large horizontal openings. This new development makes AirflowNetwork useful for not only modeling air movement between zones (and outdoors), but also within individual thermal zones.
+
+The possible combination will allow the EnergyPlus to simulate a thermal zone using a network approach by assuming internal nodes connected by user-defined patterns of temperatures and airflows. It should be pointed out that the new model works when the MultizoneWithoutDistribution is selected in the field of AirflowNetwork Control of the AirflowNetwork:SimulationCOntrol object. The model cannot work with other choices.
+
+\subsection{AirflowNetwork:Intrazone:Node}\label{airflownetworkintrazonenode}
+
+This object allows users to input multiple nodes in a zone. A single object represent a node. If there is only one node per zone, then use the AirflowNetwork:Multizone:Zone input object. The zone node is not defined in this object.
+
+\subsubsection{Field: Name}\label{field-name-12-000}
+
+The name identifies the node for later reference and in the output listing. Each node should have a unique name. This name can be referenced as AirflowNetworkNodeNames.
+
+\subsubsection{Field: RoomAir:Node:AirflowNetwork Name}\label{field-roomairnodeairflownetwork-name}
+
+The name of a RoomAir:Node:AirflowNetwork object, which is also defined in a RoomAirSettings:AirflowNetwork object (zone based).
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-1-000}
+
+The name of a zone object, which is also defined in a AirflowNetwork:MultiZone:Zone object (zone based).
+
+\subsubsection{Field: Node Height}\label{field-node-height}
+
+This field requires input of node height in meters.
+
+An IDF example is provided below:
+
+VentilationControl, !- Name
+
+\begin{lstlisting}
+
+AirflowNetwork:IntraZone:Node,
+  LeftUpper,               !- Name
+  LeftUpper,               !- RoomAir:Node:AirflowNetwork Name
+  NORTH_ZONE,              !- Zone Name
+  4.572;                   !- Node Height {m}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:Intrazone:Linkage}\label{airflownetworkintrazonelinkage}
+
+The input object specifies a connection between two AirflowNetwork:Intrazone:Node objects and an AiflowNetwork component defined elsewhere. The object also allow users to specify a connection between an AirflowNetwork:Intrazone:Node and an adjacent zone defined in an AirflowNetwork:MultiZone:Zone object. This object provides flexibility to define a linkage either in the same zone or in two different zones.
+
+\subsubsection{Field: Name}\label{field-name-13-000}
+
+The name identifies the linkage for later reference and in the output listing. Each linkage should have a unique name.
+
+\subsubsection{Field: Node 1 Name}\label{field-node-1-name}
+
+The input designates a node name where airflow starts. The node name should be defined in an AirflowNetwork:Intrazone:Node object or an AirflowNetwork:MultiZone:Zone object.
+
+\subsubsection{Field: Node 2 Name}\label{field-node-2-name}
+
+The input designates a node name where airflow ends. The node name should be defined in an AirflowNetwork:Intrazone:Node object or an AirflowNetwork:MultiZone:Zone object.
+
+Note: One of Node 1 and Node 2 should be defined as an AirflowNetwork:Intrazone:Node object. In other words, both nodes cannot be defined as AirflowNetwork:MultiZone:Zone object. This type of connection should be defined as an AirflowNetwork:MultiZone:Surface object.
+
+\subsubsection{Field: Component Name}\label{field-component-name-000}
+
+The input designates an AirflowNetwork component name associated with the two nodes. The component name should be one of the AirflowNetwork:Multizone:Component object names. The component is used for intrazone node connection only. If the next field is specified, the input of this field could be a blank.
+
+It should be pointed out that an AirflowNetwork:Multizone:Surface object allows following five AirflowNetwork:Multizone:Component objects:
+
+\begin{itemize}
+\tightlist
+\item
+  AirflowNetwork:MultiZone:Component:DetailedOpening,
+\item
+  AirflowNetwork:MultiZone:Component:SimpleOpening,
+\item
+  AirflowNetwork:MultiZone:Surface:Crack,
+\item
+  AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea,
+\item
+  AirflowNetwork:MultiZone:Component:HorizontalOpening
+\end{itemize}
+
+However, an AirflowNetwork:Intrazone:Linkage object without a surface connection has connection with two intrazone nodes in the same zone and allows two AirflowNetwork:Multizone:Component objects due to lack of geometry inputs.
+
+\begin{itemize}
+\tightlist
+\item
+  AirflowNetwork:MultiZone:Surface:Crack,
+\item
+  AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea,
+\end{itemize}
+
+\subsubsection{Field: Connection Surface}\label{field-connection-surface}
+
+The input specifies an AirflowNetwork:Multizone:Surface object name, when the nodes defined above are not located in the same zone. The surface linkage will be connected by the above two nodes, instead of zone nodes in normal definition. In other words, the connection defined in an AirflowNetwork:Multizone:Surface is removed. Instead, this new connection replaces the the connection specified before. A warning message is issued to let users be aware of the changes. Since each AirflowNetwork:Multizone:Surface object has its own component defined in the Leakage Component Name field, the input of the Component Name field in this object will be ignored.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:IntraZone:Linkage,
+  IntraZoneMiddleUpperLink, !- Name
+  LeftUpper,               !- Node 1 Name
+  CentralUpper,            !- Node 2 Name
+  CR-1;                    !- Component Name
+
+  AirflowNetwork:IntraZone:Linkage,
+  IntraZoneLeftUpperLink,
+  LeftUpper,               !- Node 1 Name
+  EAST_ZONE_T,             !- Node 2 Name
+  CR-1,                    !- Component Name
+  Surface_11_T;            !- Surface Name
+\end{lstlisting}
+
+The previous sections of this AirflowNetwork model discussion describe input objects used for multizone airflow calculations. The following sections describe input objects used for air distribution system simulations. These objects work when control option ``MultiZone with Distribution'' or ``MultiZone with Distribution Only During Fan Operation'' is defined in the AirflowNetwork Control field in the AirflowNetwork:SimulationControl object.
+
+The first section presents the input object for distribution system nodes. Although thermal zones are required to perform air distribution system simulations, the thermal zones are already defined in the multizone input section (described previously), so that there is no need to repeat the inputs for thermal zones when modeling an air distribution system. The same is also true for surface air leakage. This section has only one object: AirflowNetwork:Distribution:Node.
+
+\subsection{AirflowNetwork:Distribution:Node}\label{airflownetworkdistributionnode}
+
+The AirflowNetwork:Distribution:Node object is used to represent air distribution system nodes for the AirflowNetwork model. The EnergyPlus nodes defined in an AirLoopHVAC are a subset of the nodes used to simulate the distribution system using the AirflowNetwork model. For example, the inlet node of a fan and the outlet node of a coil defined in an AirLoopHVAC must be defined as nodes using the AirflowNetwork:Distribution:Node object. A set of EnergyPlus Zone Equipment nodes is also a subset of the AirflowNetwork:Distribution:Nodes. For example, zone inlet and outlet nodes must be defined as nodes using the AirflowNetwork:Distribution: Node object. In addition, although mixers and splitters are defined as objects with inlet and outlet nodes within EnergyPlus, the AirflowNetwork:Distribution:Node object treats mixers and splitters as single nodes. The node objects are referenced by AirflowNetwork:Distribution:Linkage objects.
+
+In summary, all nodes used to define an AirLoopHVAC (except splitters, mixers, and outdoor air systems which are treated as single nodes) and its connections to a thermal zone must be specified as AirflowNetwork:Distribution:Nodes. If distribution system air leaks are to be modeled, additional AirflowNetwork:Distribution:Nodes may be defined along with AirflowNetwork:Distribution:Components (e.g., leak or leak ratio) to define the air leakage characteristics.
+
+Note: Supply and return leaks are not allowed in an AirLoopHVAC. They can only be modeled in the Zone Equipment Loop (i.e., return leaks may be modeled between the zone return node and the zone mixer inlet or the zone mixer outlet and the zone equipment loop outlet; and supply leaks may be modeled between the zone equipment loop inlet and the AirLoopHVAC:ZoneSplitter inlet node or the AirLoopHVAC:ZoneSplitter outlet node and the zone supply node).
+
+\subsubsection{Inputs}\label{inputs-12-001}
+
+\paragraph{Field: Name}\label{field-name-14-000}
+
+The name of an air distribution system node. This node name is referenced by an AirflowNetwork:Distribution:Linkage and in the output listing. Each node should have a unique name within the AirflowNetwork:Distribution:Node objects (however, the node name may be used elsewhere as regular EnergyPlus node names such as the fan inlet node or coil outlet node).
+
+\paragraph{Field:Component Name or Node Name}\label{fieldcomponent-name-or-node-name}
+
+Designates node names defined in another EnergyPlus object, so that the AirflowNetwork:Distribution:Node object is able to get input parameters and node conditions from the associated EnergyPlus node or object. The actual node name is entered here and represents a node already defined in an AirLoopHVAC or zone equipment loop. This field is left blank if the EnergyPlus Node Type field below is entered as Mixer, Splitter, Outdoor air System, or Other.
+
+\paragraph{Field: Component Object Type or Node Type}\label{field-component-object-type-or-node-type}
+
+This choice field distinguishes the node type for the EnergyPlus node or object name defined above. Five node types are available:
+
+\begin{itemize}
+\item
+  \textbf{AirLoopHVAC:ZoneMixer}: Represents an AirLoopHVAC:ZoneMixer object defined in EnergyPlus
+\item
+  \textbf{AirLoopHVAC:ZoneSplitter}: Represents an AirLoopHVAC:ZoneSplitter object defined in EnergyPlus
+\item
+  \textbf{AirLoopHVAC:OutdoorAirSystem}: Represents an AirLoopHVAC:OutdoorAirSystem object used in EnergyPlus
+\item
+  \textbf{OAMixerOutdoorAirStreamNode}: Represents an external node name specified as an Outdoor Air Stream Node Name in the OutdoorAir:Mixer object when the AirLoopHVAC:OutdoorAirSystem object is used.
+\item
+  \textbf{OutdoorAir:NodeList}: Represents an external node name defined in the OutdoorAir:NodeList object when the AirLoopHVAC:OutdoorAirSystem object and an exhaust energy recovery system (air-to-air heat exchanger) are used.
+\item
+  \textbf{OutdoorAir}: Represents an external node name defined in the OutdoorAir:Node object when the AirLoopHVAC:OutdoorAirSystem and an exhaust energy recovery system (air-to-air heat exchanger) are used.
+\item
+  \textbf{Other}: Represents a type not already defined above.
+\end{itemize}
+
+Note: Both the OutdoorAir:NodeList and OutdoorAir:Node node types represent a node to outdoor air conditions. Either one of these node types can be used to represent an external node when an air-to-air heat exchanger is used to recover energy from the exhaust air stream as part of an AirLoopHVAC:OutdoorAirSystem object. Node type OAMixerOutdoorAirStreamNode does not represent an external node when an OutdoorAir:NodeList or OutdoorAir:Node object is specified. If no exhaust heat recovery system (i.e., air-to-air heat exchanger) is specified in the AirLoopHVAC:OutdoorAirSystem, the node type OAMixerOutdoorAirStreamNode represents an external node.
+
+\paragraph{Field: Node Height}\label{field-node-height-1}
+
+Designates the reference height in meters used to calculate relative pressure. The default value is 0 meters.
+
+IDF examples are provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:Distribution:Node,
+      EquipmentInletNode,      !- Name
+      Zone Equipment Inlet Node,  !- Component Name or Node Name
+      Other,                   !- Component Object Type or Node Type
+      3.0;                     !- Node Height {m}
+
+
+  AirflowNetwork:Distribution:Node,
+      SupplyMainNode,          !- Name
+      ,                        !- Component Name or Node Name
+      Other,                   !- Component Object Type or Node Type
+      3.0;                     !- Node Height {m}
+
+
+  AirflowNetwork:Distribution:Node,
+      MainSplitterNode,        !- Name
+      ,                        !- Component Name or Node Name
+      AirLoopHVAC:ZoneSplitter,  !- Component Object Type or Node Type
+      3.0;                     !- Node Height {m}
+
+
+  AirflowNetwork:Distribution:Node,
+      MainSplitterNode,        !- Name of Node
+      ,                        !- Name of Associated EnergyPlus Node or Object
+      AirLoopHVAC:ZoneSplitter,  !- EnergyPlus Object or Node Type
+      3.0;                     !- Node Height {m}
+\end{lstlisting}
+
+The next section describes AirflowNetwork Distribution Components, with 7 available types listed below. All required fields for each component represent a relationship between pressure difference and airflow. The components are referenced in AirflowNetwork:Distribution:Linkage objects.
+
+\begin{itemize}
+\item
+  AirflowNetwork:Distribution:Component:Leak
+\item
+  AirflowNetwork:Distribution:Component:LeakageRatio
+\item
+  AirflowNetwork:Distribution:Component:Duct
+\item
+  AirflowNetwork:Distribution:Component:ConstantVolumeFan
+\item
+  AirflowNetwork:Distribution:Component:Coil
+\item
+  AirflowNetwork:Distribution:Component:HeatExchanger
+\item
+  AirflowNetwork:Distribution:Component:TerminalUnit
+\item
+  AirflowNetwork:Distribution:Component:ConstantPressureDrop
+\end{itemize}
+
+\subsection{AirflowNetwork:Distribution:Component:Leak}\label{airflownetworkdistributioncomponentleak}
+
+This component may be also called a power law component and is used to represent a supply or return air leak in an air distribution system. Its relationship between pressure difference and airflow may be expressed as:
+
+\begin{equation}
+\dot m = {C_T}C{\left( {\Delta P} \right)^n}
+\end{equation}
+
+where
+
+\(\dot m\) ~ = Air mass flow rate through the component {[}kg/s{]}
+
+C = Air mass flow coefficient (kg/s at 1 Pa pressure difference)
+
+\(\Delta P\) ~ = Total pressure loss across the element {[}Pa{]}
+
+n = Air mass flow exponent
+
+C\(_{T}\) = Temperature correction factor
+
+\begin{equation}
+{C_T} = {\left[ {\frac{{{\rho_o}}}{\rho }} \right]^{n - 1}}{\left[ {\frac{{{\nu_o}}}{\nu }} \right]^{2n - 1}}
+\end{equation}
+
+where
+
+\(\rho\) = Air density at the specific air temperature and humidity ratio conditions {[}kg/m\(^{3}\){]}
+
+\(\nu\) = Air kinetic viscosity at the specific air temperature condition {[}m\(^{2}\)/s{]}
+
+\(\rho_o\) = Air density at air conditions of 20°C, 0 kg/kg and 101325 Pa {[}kg/m\(^{3}\){]}
+
+\(\nu_o\) = Air kinetic viscosity at an air temperature of 20°C {[}m\(^{2}\)/s{]}
+
+Note: The correction factor shown above is use for this particular component as specified.
+
+\subsubsection{Inputs}\label{inputs-13-001}
+
+\paragraph{Field: Name}\label{field-name-15-000}
+
+A unique name identifying a supply or return air leak in an air distribution system. This unique name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component leak.
+
+\paragraph{Field: Air Mass Flow Coefficient}\label{field-air-mass-flow-coefficient}
+
+This numeric field is defined as the air mass flow coefficient at 1 Pa pressure difference across this component. Valid entries must be greater than zero.
+
+\paragraph{Field: Air Mass Flow Exponent}\label{field-air-mass-flow-exponent-2}
+
+This numeric field is defined as the pressure difference exponent across the component. Valid entries are from 0.5 to 1.0, with the default value being 0.65.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+AirflowNetwork:Distribution:Component:Leak,
+  MainSupplyLeak,       !- Name of Supply or Return Leak
+  0.0001,               !- Air Mass Flow Coefficient {kg/s}
+  0.65;                 !- Air Mass Flow Exponent {dimensionless}
+
+AirflowNetwork:Distribution:Component:Leak,
+  ZoneSupplyLeak,       !- Name of Supply or Return Leak
+  0.01,                 !- Air Mass Flow Coefficient {kg/s}
+  0.65;                 !- Air Mass Flow Exponent {dimensionless}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:Distribution:Component:LeakageRatio}\label{airflownetworkdistributioncomponentleakageratio}
+
+The leakage ratio component is generally used to define supply and return leaks with respect to a constant fan flow. This object requires 5 inputs. The relationship between pressure and airflow may be expressed as a power law element:
+
+\begin{equation}
+\dot m = {C_{equ}}{\left( {\Delta P} \right)^n}
+\end{equation}
+
+where
+
+\(\rho\) = Air density {[}kg/m\(^{3}\){]}
+
+\(\Delta P\) = Total pressure loss across the element {[}Pa{]}
+
+\(n\) = Air mass flow exponent
+
+\(C_{equ}\) = Equivalent air mass flow coefficient
+
+\begin{equation}
+{C_{equ}}\,\,\,\,\,\, = r*{Q_r}*\rho *{\left( {\Delta {P_r}} \right)^{ - n}}
+\end{equation}
+
+where
+
+\(\rho\) = Effective leakage ratio {[}dimensionless{]}
+
+\(Q_{r}\) = Maximum airflow rate {[}m\(^{3}\)/s{]}
+
+\(\Delta {P_r}\) = Reference pressure difference {[}Pa{]}
+
+\(n\) = Air mass flow exponent {[}dimensionless{]}
+
+The above calculation is valid only for a HVAC system using a constant volume supply fan: Fan:ConstantVolume or Fan:OnOff.
+
+\subsubsection{Inputs}\label{inputs-14-001}
+
+\paragraph{Field: Name}\label{field-name-16-000}
+
+A unique name identifying a supply or return air leak (ratio with respect to the constant volume fan flow rate) in an air distribution system. This unique name will be referenced in an AirflowNetwork:Distribution:Linkage object to represent a component.
+
+\paragraph{Field: Effective Leakage Ratio}\label{field-effective-leakage-ratio}
+
+This numeric field is used to input the effective leakage ratio. This value must be greater than zero and less than or equal to 1. The effective leakage ratio is used to characterize supply and return leaks with respect to the constant fan flow (supply or return air leak flow rate divided by the maximum air flow rate for the fan). When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, the ratio for a supply leak is defined as the value of supply air leak flow rate divided by the supply fan air flow rate at the current time step. The inputs of the rest of 3 fields are not used.
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate}
+
+This numeric field is used to input the maximum flow rate for a constant volume fan {[}m\(^{3}\)/s{]}. This value must be greater than 0 m\(^{3}\)/s. When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, this input is not used, because the real supply fan flow rate at the current time step is used to calculate the amount of a supply leak.
+
+\paragraph{Field: Reference Pressure Difference}\label{field-reference-pressure-difference-1}
+
+This numeric field is used to input the reference pressure difference {[}Pa{]}. This value must be greater than 0 Pa. When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, this input is not used, because the real supply fan flow rate at the current time step is used to calculate the amount of a supply leak.
+
+\paragraph{Field: Air Mass Flow Exponent}\label{field-air-mass-flow-exponent-3}
+
+This numeric field is used to input the pressure difference exponent. The value of the exponent can be from 0.5 to 1.0, with the default value being 0.65. When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, this input is not used, because the real supply fan flow rate at the current time step is used to calculate the amount of a supply leak.
+
+Note: The reference pressure difference is defined as the difference between pressures of originate and terminate nodes for supply and return leaks. In general, it may require that a simulation be performed with an initial guess for reference pressure difference using design day conditions. After obtaining pressures at the leakage nodes, more realistic reference pressure differences can be entered. It should be pointed out that since pressures at the nodes vary with temperature and other conditions, the effective leakage ratio is only an estimate. In other words, the exact leakage ratio may not be available.
+
+When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, the AirflowNetwork:Distribution:Component:LeakageRatio object has to be used to define a supply leak. The other components cannot be used. In addition, the first node in a AirflowNetwork:Distribution:Linkage to define a supply leak has to be the node in the duct to originate a supply leak, and the second node has to be the node of a zone to terminate a supply leak. In other words, the supply leak has to flow from node 1 to node 2. ~When this object is used to define a return leak, the first node in a AirflowNetwork:Distribution:Linkage has to be a thermal zone to originate a leak, and the second node has to be the node of a duct to terminate a leak.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:Distribution:Component:LeakageRatio,
+      Zone1SupplyLeakELA,      !- Name of Effective Leakage Ratio
+      0.043527,                !- Effective Leakage Ratio {dimensionless}
+      1.0,                     !- Maximum Flow Rate {m3/s}
+      20.0,                    !- Reference Pressure Difference {Pa}
+      0.65;                    !- Air Mass Flow Exponent {dimensionless}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:Distribution:Component:Duct}\label{airflownetworkdistributioncomponentduct}
+
+This object represents a duct component and requires 9 input fields, one alpha field and 8 numeric fields. The relationship between pressure and airflow across the component may be expressed as (2001 ASHRAE Handbook of Fundamentals, Chapter 34):
+
+\begin{equation}
+\dot m = \sqrt {\frac{{2\rho {A^2}\Delta P}}{{fL/D + \sum {C_d}}}}
+\end{equation}
+
+where
+
+\(\dot m\) ~ = Mass flow rate of air through the component {[}kg/s{]}
+
+r = Air density {[}kg/m\(^{3}\){]}
+
+A = Cross sectional area {[}m\(^{2}\){]}
+
+\(\Delta P\) ~ = Total pressure loss across the component {[}Pa{]}
+
+L = Duct length {[}m{]}
+
+D = Hydraulic diameter {[}m{]}
+
+C\(_{d}\) = Dynamic loss coefficient due to fitting {[}dimensionless{]}
+
+f = Friction factor
+
+The friction factor can be calculated using the nonlinear Colebrook equation (ASHRAE Handbook of Fundamentals, 1997. p.~2.9, Eq. 29b)
+
+\begin{equation}
+\frac{1}{{\sqrt f }} = 1.44 + 2*\log \left( {\frac{D}{\varepsilon }} \right) - 2*\log \left( {1 + \frac{{9.3}}{{{\mathop{\rm Re}\nolimits} *\varepsilon /D*\sqrt f }}} \right)
+\end{equation}
+
+where
+
+e = Surface roughness {[}m{]}
+
+Re = Reynolds number = \(\frac{\rho VD}{\mu}\)
+
+\subsubsection{Inputs}\label{inputs-15-001}
+
+\paragraph{Field: Name}\label{field-name-17}
+
+A unique name for an AirflowNetwork duct component in an air distribution system. This unique name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component.
+
+\paragraph{Field: Duct Length}\label{field-duct-length}
+
+This numeric field is used to input duct length {[}m{]}. This value must be greater than zero.
+
+\paragraph{Field: Hydraulic Diameter}\label{field-hydraulic-diameter}
+
+This numeric field is used to input hydraulic diameter, which is defined as:
+
+\begin{equation}
+{D_h} = \frac{{4A}}{P}
+\end{equation}
+
+where
+
+D\(_{h}\) = Hydraulic diameter {[}m{]}
+
+A = Duct cross sectional area {[}m\(^{2}\){]}
+
+P = Perimeter of cross section {[}m{]}
+
+\paragraph{Field: Cross Section Area}\label{field-cross-section-area}
+
+This numeric field is used to input cross section area {[}m\(^{2}\){]}. The model assumes that this element has no area change along its length. Otherwise, effective cross sectional area is required.
+
+\paragraph{Field: Surface Roughness}\label{field-surface-roughness}
+
+This numeric field is used to input surface roughness {[}m{]}. This value must be greater than zero, and the default value is 0.0009 m.
+
+\paragraph{Field: Coefficient for Local Dynamic Loss Due to fitting}\label{field-coefficient-for-local-dynamic-loss-due-to-fitting}
+
+This numeric field is defined as a coefficient for dynamic loss {[}dimensionless{]}. It represents dynamic loss due to fittings (such as an elbow).
+
+\paragraph{Field: Overall Heat Transmittance Coefficient (U-Factor) from Air to Air}\label{field-overall-heat-transmittance-coefficient-u-factor-from-air-to-air}
+
+This numeric field is defined as the overall heat transmittance coefficient (U value, W/m\(^{2}\)-K) from air to air, including film coefficients at both surfaces.
+
+\paragraph{Field: Overall Moisture Transmittance Coefficient from Air to Air}\label{field-overall-moisture-transmittance-coefficient-from-air-to-air}
+
+This numeric field is defined as the overall moisture transmittance coefficient (kg/m\(^{2}\)) from air to air, including film coefficients at both surfaces.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:Distribution:Component:Duct,
+      MainTruck1,              !- Name of Duct Component
+      3.0,                     !- Duct Length {m}
+      0.6,                     !- Hydraulic Diameter {m}
+      0.2827,                  !- Cross Section Area {m2}
+      0.0009,                  !- Surface Roughness {m}
+      0.01,                    !- Coefficient for local dynamic loss due to fitting {dimensionless}
+      0.772,                   !- Overall heat transmittance coefficient (U value) from air to air {W/m2-K}
+      0.0001;                  !- Overall moisture transmittance coefficient from air to air {kg/m2}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:Distribution:Component:Fan}\label{airflownetworkdistributioncomponentfan}
+
+This component represents a constant volume fan in the air distribution system (AirLoopHVAC). The air flow rate and air conditions (temperature and humidity) are obtained from the associated Fan:ConstantVolume, Fan:OnOff, or Fan:VariableVolume object.
+
+\subsubsection{Inputs}\label{inputs-16-001}
+
+\paragraph{Field: Fan Name}\label{field-fan-name-000}
+
+The name identifying an AirflowNetwork constant volume fan in an air distribution system. This name must be the same as the name of the associated Fan:ConstantVolume,~ Fan:OnOff or Fan:VariableVolume object. This name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component.
+
+\paragraph{Field: Supply Fan Object Type}\label{field-supply-fan-object-type}
+
+This choice field defines the type of fan. The only valid choices are Fan:OnOff,~ Fan:ConstantVolume, and Fan:VariableVolume, with the default being Fan:ConstantVolume. Both cycling and continuous fan operating modes are allowed for Fan:OnOff. Only the continuous fan operating mode is allowed for Fan:ConstantVolume. The variable airflow rate is allowed for Fan:VariableVolume.
+
+Note: Make sure that the volumetric air flow rates for the fan, coils, and parent components (e.g., unitary system or furnace) are the same so that fan energy and air distribution system losses/gains are properly calculated.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:Distribution:Component:Fan,
+      Supply Fan 1,            !- Name of Constant Volume Fan
+      Fan:ConstantVolume;  !- Supply fan type
+\end{lstlisting}
+
+\subsection{AirflowNetwork:Distribution:Component:Coil}\label{airflownetworkdistributioncomponentcoil}
+
+This component represents a cooling or heating coil. The main purpose for this object is to get calculated values (air flow and temperature/humidity conditions) from the associated coil models.
+
+\subsubsection{Inputs}\label{inputs-17}
+
+\paragraph{Field: Coil Name}\label{field-coil-name}
+
+The name identifying an AirflowNetwork cooling coil or heating coil defined in an air loop. This name must be the same name as the associated coil object. This unique name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component.
+
+\paragraph{Field: Coil Object Type}\label{field-coil-object-type}
+
+This field requires input of the coil type used in the AirflowNetwork model. The available choices are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:DX:SingleSpeed
+\item
+  Coil:Cooling:Water
+\item
+  Coil:Heating:Water
+\item
+  Coil:Cooling:Water:DetailedGeometry
+\item
+  Coil:Cooling:DX:TwoStageWithHumidityControlMode
+\item
+  Coil:Cooling:DX:MultiSpeed
+\item
+  Coil:Heating:DX:MultiSpeed
+\item
+  Coil:Heating:Desuperheater
+\end{itemize}
+
+\paragraph{Field: Air Path Length}\label{field-air-path-length}
+
+This numeric field is used to input air path length for the coil {[}m{]}. This value must be greater than 0 meters.
+
+\paragraph{Field: Air Path Hydraulic Diameter}\label{field-air-path-hydraulic-diameter}
+
+This numeric field is used to input hydraulic diameter of a coil's air path, which is defined as:
+
+\begin{equation}
+{D_h} = \frac{{4A}}{P}
+\end{equation}
+
+where
+
+D\(_{h}\) = Hydraulic diameter {[}m{]}
+
+A = Duct cross section area {[}m\(^{2}\){]}
+
+P = Perimeter of cross section {[}m{]}
+
+For this component, the relationship between airflow and pressure is similar to the component AirflowNetwork:Distribution:Component:Duct. However, the model assumes very small surface roughness (10\(^{-4}\)) and no local dynamic loss due to fittings for this component. Therefore, this component only requires two numerical fields. Heat and moisture exchange from surroundings is ignored.
+
+Note: Make sure that the volumetric air flow rates for the fan, coils, and parent components (e.g., unitary system or furnace) are the same so that fan energy and air distribution system losses/gains are properly calculated.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:Distribution:Component:Coil,
+      ACDXCoil 1,                            !- Name of Associated EnergyPlus Coil
+      Coil:Cooling:DX:SingleSpeed,           !- EnergyPlus Coil Type
+      0.1,                                   !- Air Path Length {m}
+      1.00;                                  !- Air Path Hydraulic Diameter {m}
+
+
+  AirflowNetwork:Distribution:Component:Coil,
+      HP Heating Coil 1,                     !- Name of Associated EnergyPlus Coil
+      Coil:Heating:DX:SingleSpeed,           !- EnergyPlus Coil Type
+      0.1,                                   !- Air Path Length {m}
+      1.00;                                  !- Air Path Hydraulic Diameter {m}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:Distribution:Component:HeatExchanger}\label{airflownetworkdistributioncomponentheatexchanger}
+
+This component represents an air-to-air heat exchanger typically used in combination with a cooling coil to enhance dehumidification or in an outside air system to recover energy from exhaust air to pretreat incoming outdoor ventilation air. The cooling coils with enhanced dehumidification are defined in the two objects CoilSystem:Cooling:DX:HeatExchangerAssisted and CoilSystem:Cooling:Water:HeatExchangerAssisted using one of three heat exchanger objects specified below. The exhaust air energy recovery system also has the same restriction using the one of three heat exchanger objects. The main purpose for this object is to obtain calculated values (air flow and temperature/humidity conditions) from the associated heat exchanger models for the airflow network calculations.
+
+\subsubsection{Inputs}\label{inputs-18}
+
+\paragraph{Field: Heat Exchanger Name}\label{field-heat-exchanger-name}
+
+The name identifying an AirflowNetwork heat exchanger defined in an air loop. This name must be the same name that is used in the associated heat exchanger object. This unique name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component.
+
+\paragraph{Field: Heat Exchanger Object Type}\label{field-heat-exchanger-object-type}
+
+This field requires input of the heat exchanger type. The available choices are:
+
+\begin{itemize}
+\item
+  ~~~HeatExchanger:AirToAir:FlatPlate
+\item
+  ~~~HeatExchanger:AirToAir:SensibleAndLatent
+\item
+  ~~~HeatExchanger:Desiccant:BalancedFlow
+\end{itemize}
+
+\paragraph{Field: Air Path Length}\label{field-air-path-length-1}
+
+This numeric field is used to input air path length for the heat exchanger coil {[}m{]}. This value must be greater than 0 meters.
+
+\paragraph{Field: Air Path Hydraulic Diameter}\label{field-air-path-hydraulic-diameter-1}
+
+This numeric field is used to input hydraulic diameter of a heat exchanger coil's air path, which is defined as:
+
+\begin{equation}
+{D_h} = \frac{{4A}}{P}
+\end{equation}
+
+where
+
+D\(_{h}\) = Hydraulic diameter {[}m{]}
+
+A = Duct cross section area {[}m\(^{2}\){]}
+
+P = Perimeter of cross section {[}m{]}
+
+For this component, the relationship between airflow and pressure is similar to the component AirflowNetwork:Distribution:Component:Duct. However, the model assumes very small surface roughness (10\(^{-4}\)) and no local dynamic loss due to fittings for this component. Therefore, this component only requires two numerical fields. Heat and moisture exchange from surroundings are ignored.
+
+Note: When a heat exchanger is used as a component of either CoilSystem:Cooling:DX:HeatExchangerAssisted or CoilSystem:Cooling:Water:HeatExchangerAssisted, the heat exchanger acts as two components in an air primary loop. For example, an air-to-air heat exchanger has a component connected to the supply air side (equivalent to a supply coil) and a component connected to exhaust air side (equivalent to an exhaust coil). The desiccant heat exchanger has a component connected to regeneration air side (equivalent to a regeneration air coil) and a component connected to process air side (equivalent to a process air coil). Therefore, each air-to-air heat exchanger used in this configuration requires two linkage objects (instead of only one linkage object as required for other AirflowNetwork components).
+
+When a heat exchanger is used in an exhaust air energy recovery system (i.e., in an AirLoopHVAC:OutdoorAirSystem object to recover waste heat from exhaust air to pretreat incoming outdoor ventilation air), the heat exchanger is treated as a single component. The AirflowNetwork model only connects the two nodes associated with the incoming outdoor ventilation air, while the two exhaust nodes are not defined as part of the AirflowNetwork model. Therefore, each heat exchanger component used in an exhaust air energy recovery system has only one linkage object, similar to AirflowNetwork coil components.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:Distribution:Component:HeatExchanger,
+      OA Heat Recovery 1,      !- HeatExchanger Name
+      HeatExchanger:AirToAir:SensibleAndLatent,  !- HeatExchanger Object Type
+      0.1,                     !- Air Path Length {m}
+      1.00;                    !- Air Path Hydraulic Diameter {m}
+
+
+  AirflowNetwork:Distribution:Component:HeatExchanger,
+      Desiccant Heat Exchanger 1, !- HeatExchanger Name
+      HeatExchanger:Desiccant:BalancedFlow,  !- HeatExchanger Object Type
+      0.1,                     !- Air Path Length {m}
+      1.00;                    !- Air Path Hydraulic Diameter {m}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:Distribution:Component:TerminalUnit}\label{airflownetworkdistributioncomponentterminalunit}
+
+This component represents a terminal unit for reheating the incoming supply air. The main purpose is to get calculated values from the terminal unit models.
+
+\subsubsection{Inputs}\label{inputs-19}
+
+\paragraph{Field: Terminal Unit Name}\label{field-terminal-unit-name}
+
+A name identifying an AirflowNetwork terminal unit defined in a zone equipment list. This name must be the same as the associated terminal unit object. This unique name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component.
+
+\paragraph{Field: Terminal Unit Object Type}\label{field-terminal-unit-object-type}
+
+This field requires input of the terminal unit type used in the AirflowNetwork model. The available types are AirTerminal:SingleDuct:ConstantVolume:Reheat and AirTerminal:SingleDuct:VAV:Reheat. The AirTerminal:SingleDuct:ConstantVolume:Reheat type is used when the Supply Fan Object Type in the AirflowNetwork:Distribution:Component:Fan is either Fan:ConstantVolume or Fan:OnOff. The AirTerminal:SingleDuct:VAV:Reheat type is used when the Supply Fan Object Type in the AirflowNetwork:Distribution:Component:Fan is Fan:VariableVolume only.
+
+\paragraph{Field: Air Path Length}\label{field-air-path-length-2}
+
+This numeric field is used to input the air path length for the terminal unit {[}m{]}. This value must be greater than 0 meters.
+
+\paragraph{Field: Air Path Hydraulic Diameter}\label{field-air-path-hydraulic-diameter-2}
+
+This numeric field is used to input hydraulic diameter for the terminal unit's air path, which is defined as:
+
+\begin{equation}
+{D_h} = \frac{{4A}}{P}
+\end{equation}
+
+where
+
+D\(_{h}\) = Hydraulic diameter {[}m{]}
+
+A = Duct cross section area {[}m\(^{2}\){]}
+
+P = Perimeter of cross section {[}m{]}
+
+It should be noted that the relationship for this component between airflow and pressure is similar to the component AirflowNetwork:Distribution:Component:Duct. However, the model assumes very small surface roughness (10\(^{-4}\)) and no local dynamic loss due to fittings for this component. Therefore, this component only requires two numerical fields. Heat and moisture exchange from surroundings is ignored.
+
+Note: The AirflowNetwork:Distribution:Component:TerminalUnit object is used to represent an AirTerminal:SingleDuct:ConstantVolume:Reheat or an AirTerminal:SingleDuct:VAV:Reheat object in an AirflowNetwork simulation. The AirflowNetwork:Distribution:Component:TerminalUnit should not be used to represent any other air terminal unit types. When the ZoneHVAC:EquipmentList object specifies an Air:Terminal:SingleDuct:Uncontrolled object, the AirflowNetwork:Distribution:Component:Duct object should be used instead.
+
+The AirTerminal:SingleDuct:VAV:Reheat object has two components: a damper and a reheat coil. When the AirTerminal:SingleDuct:VAV:Reheat type is used, two objects of AirflowNetwork:Distribution:Linkage have to be used to make two links, one of which is a link to connect two nodes for a damper, and the other is a link to connect two nodes for a reheat coil.
+
+When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, the type of all terminals has to be AirTerminal:SingleDuct:VAV:Reheat. The object of Air:Terminal:SingleDuct:Uncontrolled is not allowed.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:Distribution:Component:TerminalUnit,
+      Reheat Zone 1,                    !- Name of Associated Energyplus Terminal Unit
+      AirTerminal:SingleDuct:ConstantVolume:Reheat,  !- EnergyPlus Terminal Unit Type
+      0.1,                              !- Air Path Length {m}
+      0.44;                             !- Air Path Hydraulic Diameter {m}
+\end{lstlisting}
+
+\subsection{AirflowNetwork:Distribution:Component:ConstantPressureDrop}\label{airflownetworkdistributioncomponentconstantpressuredrop}
+
+This component represents a constant pressure drop component. It is generally used to simulate a constant pressure drop filter. The mathematical equation may be written as:
+
+\begin{equation}
+\Delta P = const
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-20}
+
+\paragraph{Field: Name}\label{field-name-18}
+
+A unique name identifying an AirflowNetwork constant pressure drop component in an air distribution system. This unique name will be referenced by an AirflowNetwork: Distribution:Linkage object to represent a component.
+
+\paragraph{Field: Pressure Difference across the Component}\label{field-pressure-difference-across-the-component}
+
+This numeric field is used to input the pressure difference across the element {[}Pa{]}.
+
+Note: This object should be used with caution. Each node connected to this object cannot be a node for a mixer or splitter, a node in an AirLoopHVAC, or a node in a zone configuration loop. It is recommended that duct components be specified at both ends of this object.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:Distribution:Component:ConstantPressureDrop,
+   SupplyCPDComp, ! Name of Constant Pressure Drop Component
+   1.0;           ! Pressure Difference Across the Component [Pa]
+\end{lstlisting}
+
+\subsection{AirflowNetwork:Distribution:Linkage}\label{airflownetworkdistributionlinkage}
+
+The AirflowNetwork:Distribution:Linkage represents a connection between two AirflowNetwork:Distribution:Node objects and an AirflowNetwork component defined above. In addition, the relative height from node height to linkage height for each node is required.
+
+\subsubsection{Inputs}\label{inputs-21}
+
+\paragraph{Field: Name}\label{field-name-19}
+
+The name identifies the linkage for later reference and in the output listing. Each linkage should have a unique name.
+
+\paragraph{Field: Node 1 Name}\label{field-node-1-name-1}
+
+Designates a node name where airflow starts. The node name should be defined in an AirflowNetwork:Distribution:Node object.
+
+\paragraph{Field: Node 2 Name}\label{field-node-2-name-1}
+
+Designates a node name where airflow ends. The node name should be defined in an AirflowNetwork:Distribution:Node object.
+
+\paragraph{Field: Component Name}\label{field-component-name-1-000}
+
+Designates an AirflowNetwork component name associated with the two nodes. The component name should be one of the AirflowNetwork:Distribution:Component\ldots{} object names.
+
+\paragraph{Field: Thermal Zone Name}\label{field-thermal-zone-name}
+
+Designates a thermal zone where the linkage is located. The information provides the ambient conditions for duct elements to calculate duct conduction losses (only used if component is AirflowNetwork:Distribution:Component:Duct).
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+AirflowNetwork:Distribution:Linkage,
+      Main Link 1,             !- Name of Linkage
+      EquipmentInletNode,      !- Node 1 Name
+      SupplyMainNode,          !- Node 2 Name
+      MainTruck1,              !- Component Name
+      Attic Zone;              !- Thermal Zone Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-002}
+
+The AirflowNetwork nodes in the following output variables includes zones defined in AirflowNetwork:Multizone:Zone objects, external nodes defined in AirflowNetwork:MultiZone:ExternalNode objects, and nodes defined in AirflowNetwork:Distribution:Node objects.
+
+The AirflowNetwork linkage used in following output variables includes surfaces defined in AirflowNetwork:Multizone:Surface objects, and linkages defined in AirflowNetwork:Distribution:Linkage objects. The surface linkages represent airflows through surface cracks or openings between two zones or between a zone and outdoors. The distribution linkages represent airflows in an air distribution system.
+
+\begin{itemize}
+\item
+  HVAC,Average,AFN Node Temperature {[}C{]}
+\item
+  HVAC,Average,AFN Node Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,AFN Node Total Pressure {[}Pa{]}
+\item
+  HVAC,Average,AFN Node Wind Pressure {[}Pa{]}
+\item
+  HVAC,Average,AFN Node CO2 Concentration {[}ppm{]}
+\item
+  HVAC,Average,AFN Node Generic Air Contaminant Concentration {[}ppm{]}
+\item
+  HVAC,Average,AFN Linkage Node 1 to Node 2 Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,AFN Linkage Node 2 to Node 1 Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,AFN Linkage Node 1 to Node 2 Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,AFN Linkage Node 2 to Node 1 Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,AFN Linkage Node 1 to Node 2 Pressure Difference {[}Pa{]}
+\item
+  HVAC,Average,AFN Surface Venting Window or Door Opening Factor {[]}
+\item
+  HVAC,Average,AFN Surface Venting Window or Door Opening Modulation Multiplier {[]}
+\item
+  HVAC,Average,AFN Surface Venting Inside Setpoint Temperature {[}C{]}
+\item
+  HVAC,Average,AFN Surface Venting Availability Status {[]}
+\item
+  HVAC,Average,AFN Zone Infiltration Sensible Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Infiltration Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Mixing Sensible Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Mixing Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Infiltration Sensible Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Infiltration Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Mixing Sensible Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Mixing Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Infiltration Latent Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Infiltration Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Infiltration Latent Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Infiltration Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Mixing Latent Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Mixing Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Mixing Latent Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Mixing Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Duct Leaked Air Sensible Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Duct Leaked Air Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Duct Leaked Air Sensible Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Duct Leaked Air Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Duct Leaked Air Latent Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Duct Leaked Air Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Duct Leaked Air Latent Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Duct Leaked Air Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Duct Conduction Sensible Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Duct Conduction Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Duct Conduction Sensible Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Duct Conduction Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Duct Diffusion Latent Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Duct Diffusion Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,AFN Zone Duct Diffusion Latent Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Zone Duct Diffusion Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,AFN Distribution Sensible Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Distribution Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,AFN Distribution Sensible Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Distribution Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,AFN Distribution Latent Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Distribution Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,AFN Distribution Latent Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,AFN Distribution Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,AFN Zone Infiltration Volume {[}m3{]}
+\item
+  HVAC,Sum,AFN Zone Infiltration Mass {[}kg{]}
+\item
+  HVAC,Average,AFN Zone Infiltration Air Change Rate {[}ach{]}
+\item
+  HVAC,Sum,AFN Zone Mixing Volume {[}m3{]}
+\item
+  HVAC,Sum,AFN Zone Mixing Mass {[}kg{]}
+\end{itemize}
+
+\textbf{The following output variables are reported only when a Fan:OnOff object is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average,AFN Zone Average Pressure {[}Pa{]}
+\item
+  HVAC,Average,AFN Zone On Cycle Pressure {[}Pa{]}
+\item
+  HVAC,Average,AFN Zone Off Cycle Pressure {[}Pa{]}
+\item
+  HVAC,Average,AFN Linkage Node 1 to 2 Average Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,AFN Linkage Node 2 to 1 Average Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,AFN Linkage Node 1 to 2 Average Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,AFN Linkage Node 2 to 1 Average Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,AFN Surface Average Pressure Difference {[}Pa{]}
+\item
+  HVAC,Average,AFN Surface On Cycle Pressure Difference {[}Pa{]}
+\item
+  HVAC,Average,AFN Surface Off Cycle Pressure Difference {[}Pa{]}
+\end{itemize}
+
+\textbf{The following output variables are reported only when an AirflowNetwork:OccupantVentilationControl object is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average,AFN Surface Venting Window or Door Opening Factor at Previous Time Step {[]}
+\item
+  HVAC,Average,AFN Surface Opening Elapsed Time {[}min{]}
+\item
+  HVAC,Average,AFN Surface Closing Elapsed Time {[}min{]}
+\item
+  HVAC,Average,AFN Surface Opening Status at Previous Time Step {[]}
+\item
+  HVAC,Average,AFN Surface Opening Status {[]}
+\item
+  HVAC,Average,AFN Surface Opening Probability Status {[]}
+\item
+  HVAC,Average,AFN Surface Closing Probability Status {[]}
+\end{itemize}
+
+\textbf{The following are reported only when an integrated model of RoomAir and AirflowNetwork is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average, RoomAirflowNetwork Node Total Pressure {[}Pa{]}
+\item
+  HVAC,Average, RoomAirflowNetwork Node Temperature {[}C{]}
+\item
+  HVAC,Average, RoomAirflowNetwork Node Humidity Ratio {[}kgWater/kgDryAir{]}
+\end{itemize}
+
+\paragraph{AFN Node Temperature {[}C{]}}\label{afn-node-temperature-c}
+
+This is the AirflowNetwork node temperature output in degrees C. When a Fan:OnOff object is used and is scheduled to operate in the cycling fan operation mode, this value for AirflowNetwork:Distribution:Node objects reflects the temperature when the fan is operating (ON).
+
+\paragraph{AFN Node Humidity Ratio {[}kgWater/kgDryAir{]}}\label{afn-node-humidity-ratio-kgwaterkgdryair}
+
+This is the AirflowNetwork node humidity ratio output in kgWater/kgDryAir. When a Fan:OnOff object is used and is scheduled to operate in the cycling fan operation mode, this value for AirflowNetwork:Distribution:Node objects reflects the humidity ratio when the fan is operating (ON).
+
+\paragraph{AFN Node Total Pressure {[}Pa{]}}\label{afn-node-total-pressure-pa}
+
+This is the AirflowNetwork node total pressure in Pa with respect to outdoor barometric pressure. The total pressure is the sum of static pressure, dynamic pressure, and elevation impact at the node's relative height. When a Fan:OnOff object is used and is scheduled to operate in the cycling fan operation mode, the value for AirflowNetwork:Distribution:Node objects reflects the total pressure when the fan is operating (ON). The total pressures for nodes associate with AirflowNetwork:Multizone:Zone objects are reported in different output variables (below).
+
+\paragraph{AFN Node CO2 Concentration {[} ppm{]}}\label{afn-node-co2-concentration-ppm}
+
+This is the AirflowNetwork node carbon dioxide concentration level in parts per million (ppm). When a Fan:OnOff object is used and is scheduled to operate in the cycling fan operation mode, this value for AirflowNetwork:Distribution:Node objects reflects the carbon dioxide when the fan is operating (ON).
+
+\paragraph{AFN Node Generic Air Contaminant Concentration {[}ppm{]}}\label{afn-node-generic-air-contaminant-concentration-ppm}
+
+This is the AirflowNetwork node generic contaminant concentration level in parts per million (ppm). When a Fan:OnOff object is used and is scheduled to operate in the cycling fan operation mode, this value for AirflowNetwork:Distribution:Node objects reflects the carbon dioxide when the fan is operating (ON).
+
+\paragraph{AFN Zone Average Pressure {[}Pa{]}}\label{afn-zone-average-pressure-pa}
+
+This is the AirflowNetwork average zone total pressure in Pa with respect to outdoor barometric pressure. This output is only available when a Fan:OnOff object is used in the air distribution system. The average zone pressure is weighted by the system fan part-load ratio using the calculated zone pressures during the fan on and off periods for the system timestep. The system fan part-load ratio is defined as the ratio of the air distribution system mass flow rate (average for the simulation timestep) to the system design mass flow rate.
+
+Average zone pressure = (Zone pressure during on cycle * Part-load ratio) + Zone pressure during off cycle * (1.0 -- Part-load ratio)
+
+\paragraph{AFN Zone On Cycle Pressure {[}Pa{]}}\label{afn-zone-on-cycle-pressure-pa}
+
+This is the AirflowNetwork zone total pressure in Pa with respect to outdoor barometric pressure when the air distribution system fan is operating (ON). This output is only available when a Fan:OnOff object is used in the air distribution system. When the fan part-load ratio is equal to 0.0, this pressure value will be zero because the air distribution system is not simulated when the fan is off for the entire timestep.
+
+\paragraph{AFN Zone Off Cycle Pressure {[}Pa{]}}\label{afn-zone-off-cycle-pressure-pa}
+
+This is the AirflowNetwork zone total pressure in Pa with respect to outdoor barometric pressure when the air distribution system fan is not operating (OFF). This output is only available when a Fan:OnOff object is used in the air distribution system. Even if the fan part-load ratio is equal to 1.0, the pressure calculated as if the fan were not operating (OFF) is reported.
+
+\paragraph{AFN Node Wind Pressure {[}Pa{]}}\label{afn-node-wind-pressure-pa}
+
+This is the AirflowNetwork wind pressure output in Pa. The wind pressure depends on several factors, including wind speed, wind direction, the wind-pressure coefficient (Cp) values for the AirflowNetwork:MultiZone:ExternalNode associated with the heat transfer surface and the site wind conditions.
+
+When Wind Pressure Coefficient Type = ``Input'' in the AirflowNetwork:SimulationControl object, the output represents external node pressures driven by wind defined in an AirflowNetwork:MultiZone:ExternalNode object. When Wind Pressure Coefficient Type = ``SurfaceAverageCalculation'' in AirflowNetwork:SimulationControl, the program assumes five external nodes:
+
+\begin{itemize}
+\item
+  FACADE1~~~~~~~~ Representing north orientation
+\item
+  FACADE2~~~~~~~~ Representing east orientation
+\item
+  FACADE3~~~~~~~~ Representing south orientation
+\item
+  FACADE4~~~~~~~~ Representing west orientation
+\item
+  ROOF~~~~~~~~~~~~~~ Representing horizontal orientation
+\end{itemize}
+
+In this case, the output represents the wind pressures for the five external nodes defined above.
+
+\paragraph{AFN Linkage Node 1 to Node 2 Mass Flow Rate {[}kg/s{]}}\label{afn-linkage-node-1-to-node-2-mass-flow-rate-kgs}
+
+This is the AirflowNetwork linkage mass flow rate output in kg/s in the direction from Node 1 to Node 2. It reports surface airflows through a crack or opening, and through linkages defined in an AirflowNetwork:Distribution:Linkage object. The surface linkage is divided into two types of surfaces, exterior surface and interior surface. Node 1 for an exterior surface linkage is a thermal zone and Node 2 is an external node. The value of AFN Linkage Node 1 to Node 2 Mass Flow Rate represents the flow rate from a thermal zone to outdoors. The flow direction through an interior surface crack or opening is defined from a thermal zone defined by a surface's Zone Name (Node 1) to an adjacent thermal zone defined by a surface's OutsideFaceEnvironment (Node 2). For an AirflowNetwork:Distribution:Linkage object, the value represents the air mass flow rate flowing from Node 1 to Node 2.
+
+It should be pointed out that in general, each linkage has one directional flow at any given time, either from Node 1 to 2 or from Node 2 to 1. However, there are three components which may have flows in both directions simultaneously: AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:MultiZone:Component:SimpleOpening, and AirflowNetwork:MultiZone:Component:HorizontalOpening.
+
+When a Fan:OnOff object is used, the air mass flow rates reported for the AirflowNetwork:Distribution:Linkage objects are the values when the fan is operating (ON). It is assumed that the air mass flow rates when the fan is off are zero for the distribution system air linkage objects. The air mass flow rates for the AirflowNetwork:Multizone:Surface object are reported in different output variables (below).
+
+\paragraph{AFN Linkage Node 2 to Node 1 Mass Flow Rate {[}kg/s{]}}\label{afn-linkage-node-2-to-node-1-mass-flow-rate-kgs}
+
+This is the AirflowNetwork linkage mass flow rate output in kg/s in the direction from Node 2 to Node 1. It reports airflows from surfaces through a crack or opening, and from linkages defined in an AirflowNetwork:Distribution:Linkage object. Node 1 and Node 2 for a surface or subsurface are defined in the same manner as AFN Linkage Node 1 to Node 2 Mass Flow Rate.
+
+When a Fan:OnOff object is used, the air mass flow rates reported for the AirflowNetwork:Distribution:Linkage objects are the values when the fan is operating (ON). It is assumed that the air mass flow rates when the fan is off are zero for the distribution system air linkage objects. The air mass flow rates for the AirflowNetwork:Multizone:Surface object are reported in different output variables (below).
+
+\paragraph{AFN Linkage Node 1 to 2 Average Mass Flow Rate {[}kg/s{]}}\label{afn-linkage-node-1-to-2-average-mass-flow-rate-kgs}
+
+This is the AirflowNetwork linkage average mass flow rate in kg/s in the direction from Node 1 to Node 2 defined in the AirflowNetwork:Multizone:Surface objects. This output is only available when a Fan:OnOff object is used in the air distribution system. The average mass flow rate is weighted by the system fan part-load ratio using the calculated air mass flow rates during the fan on and off periods for the system timestep. The system fan part-load ratio is defined as the ratio of the air distribution system mass flow rate (average for the simulation timestep) to the system design mass flow rate.
+
+Average surface mass flow rate = (Surface mass flow rate during on cycle * Part-load ratio) + Surface mass flow rate during off cycle * (1.0 -- Part-load ratio)
+
+\paragraph{AFN Linkage Node 2 to 1 Average Mass Flow Rate {[}kg/s{]}}\label{afn-linkage-node-2-to-1-average-mass-flow-rate-kgs}
+
+This is the AirflowNetwork linkage average mass flow rate in kg/s in the direction from Node 2 to Node 1 defined in the AirflowNetwork:Multizone:Surface objects. This output is only available when a Fan:OnOff object is used in the air distribution system. The average mass flow rate is weighted by the system fan part-load ratio using the calculated air mass flow rates during the fan on and off periods for the system timestep. The system fan part-load ratio is defined as the ratio of the air distribution system mass flow rate (average for the simulation timestep) to the system design mass flow rate.
+
+\paragraph{\texorpdfstring{AFN Linkage Node 1 to Node 2 Volume Flow Rate {[}m\(^{3}\)/s{]}}{AFN Linkage Node 1 to Node 2 Volume Flow Rate {[}m\^{}\{3\}/s{]}}}\label{afn-linkage-node-1-to-node-2-volume-flow-rate-m3s}
+
+This is the AirflowNetwork linkage volume flow rate output in m\(^{3}\)/s in the direction from the Node 1 to Node 2. It is defined in the same manner as AFN Linkage Node 1 to Node 2 Mass Flow Rate.
+
+When a Fan:OnOff object is used, the air volume flow rates reported for the AirflowNetwork:Distribution:Linkage objects are the values when the fan is operating (ON). It is assumed that the air volume flow rates when the fan is off are zero for the distribution system air linkage objects. The air volume flow rates for the AirflowNetwork:Multizone:Surface object are reported in different output variables (below).
+
+\paragraph{\texorpdfstring{AFN Linkage Node 2 to Node 1 Volume Flow Rate {[}m\(^{3}\)/s{]}}{AFN Linkage Node 2 to Node 1 Volume Flow Rate {[}m\^{}\{3\}/s{]}}}\label{afn-linkage-node-2-to-node-1-volume-flow-rate-m3s}
+
+This is the AirflowNetwork linkage volume flow rate output in m\(^{3}\)/s in the direction from Node 2 to Node 1. It is defined in the same manner as AFN Linkage Node 2 to Node 1 Mass Flow Rate.
+
+When a Fan:OnOff object is used, the air volume flow rates reported for the AirflowNetwork:Distribution:Linkage objects are the values when the fan is operating (ON). It is assumed that the air volume flow rates when the fan is off are zero for the distribution system air linkage objects. The air volume flow rates for the AirflowNetwork:Multizone:Surface object are reported in different output variables (below).
+
+\paragraph{\texorpdfstring{AFN Linkage Node 1 to 2 Average Volume Flow Rate {[}m\(^{3}\)/s{]}}{AFN Linkage Node 1 to 2 Average Volume Flow Rate {[}m\^{}\{3\}/s{]}}}\label{afn-linkage-node-1-to-2-average-volume-flow-rate-m3s}
+
+This is the AirflowNetwork linkage average volume flow rate in m\(^{3}\)/s in the direction from Node 1 to Node 2 defined in the AirflowNetwork:Multizone:Surface objects. This output is only available when a Fan:OnOff object is used. The average volume flow rate is weighted by the system fan part-load ratio using the calculated air volume flow rates during the fan on and off periods for the system timestep.
+
+Average surface volume flow rate = (Surface volume flow rate during on cycle * Part-load ratio) + Surface volume flow rate during off cycle * (1.0 -- Part-load ratio)
+
+\paragraph{\texorpdfstring{AFN Linkage Node 2 to 1 Average Volume Flow Rate {[}m\(^{3}\)/s{]}}{AFN Linkage Node 2 to 1 Average Volume Flow Rate {[}m\^{}\{3\}/s{]}}}\label{afn-linkage-node-2-to-1-average-volume-flow-rate-m3s}
+
+This is the AirflowNetwork linkage average volume flow rate in m\(^{3}\)/s in the direction from Node 2 to Node 1 defined in the AirflowNetwork:Multizone:Surface objects. This output is only available when a Fan:OnOff object is used. The average volume flow rate is weighted by the system fan part-load ratio using the calculated air volume flow rates during the fan on and off periods for the system timestep.
+
+\paragraph{AFN Linkage Node 1 to Node 2 Pressure Difference {[}Pa{]}}\label{afn-linkage-node-1-to-node-2-pressure-difference-pa}
+
+This is the pressure difference across a linkage in Pa. The linkage includes both objects: AirflowNetwork:Multizone:Surface and AirflowNetwork: Distribution:Linkage.
+
+When a Fan:OnOff object is used, the pressure differences reported for the AirflowNetwork:Distribution:Linkage objects are the values calculated when the fan is operating (ON). It is assumed that the pressure differences when the fan is off are zero for the distribution system air linkage objects. The pressure differences defined in the AirflowNetwork:Multizone:Surface are reported in different output variables (below).
+
+\paragraph{AFN Surface Average Pressure Difference {[}Pa{]}}\label{afn-surface-average-pressure-difference-pa}
+
+This is the average pressure difference across a linkage in Pa for the AirflowNetwork:Multizone:Surface objects only when a Fan:OnOff object is used. The average pressure difference is weighted by the system fan part-load ratio using the calculated pressure differences during the fan on and off periods for the system timestep. The system fan part-load ratio is defined as the ratio of the air distribution system mass flow rate (average for the simulation timestep) to the system design mass flow rate.
+
+Surface Average Pressure Difference = (Surface Average Pressure Difference during on cycle * Part-load ratio) + Surface Average Pressure Difference during off cycle * (1.0 - Part-load ratio)
+
+\paragraph{AFN Surface On Cycle Pressure Difference {[}Pa{]}}\label{afn-surface-on-cycle-pressure-difference-pa}
+
+This is the pressure difference across a linkage in Pa for the AirflowNetwork:Multizone:Surface objects only when the air distribution system fan is operating (ON). This output is only available when a Fan:OnOff object is used. When the fan part-load ratio is equal to 0.0, this pressure difference value will be zero because the air distribution system is not simulated when the fan is off for the entire timestep.
+
+\paragraph{AFN Surface Off Cycle Pressure Difference {[}Pa{]}}\label{afn-surface-off-cycle-pressure-difference-pa}
+
+This is the pressure difference across a linkage in Pa for the AirflowNetwork:Multizone:Surface objects only when the air distribution system fan is not operating (OFF). This output is only available when a Fan:OnOff object is used. Even if the fan part-load ratio is equal to 1.0, the pressure difference calculated as if the fan were not operating (OFF) is reported.
+
+\paragraph{\texorpdfstring{AFN Surface Venting Window or Door Opening Factor {[]}}{AFN Surface Venting Window or Door Opening Factor }}\label{afn-surface-venting-window-or-door-opening-factor}
+
+The current time-step value of the venting opening factor for a particular window or door. When the window or door is venting, this is the input value of the opening factor (see AirflowNetwork:Multizone:Surface, Window/Door Opening Factor) times the multiplier for venting modulation (see description of next output variable, ``Opening Factor Multiplier for AirflowNetwork Venting Modulation''). For example, if~ the input Window/Door opening factor is 0.5 and the modulation multiplier is 0.7, then the value of this output variable will be 0.5x0.7 = 0.35.
+
+\paragraph{\texorpdfstring{AFN Surface Venting Window or Door Opening Modulation Multiplier~ {[]}}{AFN Surface Venting Window or Door Opening Modulation Multiplier~ }}\label{afn-surface-venting-window-or-door-opening-modulation-multiplier}
+
+This is the multiplier on a window or door opening factor when venting modulation is in effect. See ``Modulation of Openings'' under AirflowNetwork:Multizone:Zone for a description of how the multiplier is determined.
+
+When modulation is in effect the value of the multiplier is between 0.0 and 1.0. When modulation does not apply the value of the multiplier may be --1.0. When modulation applies but the surface is not venting, the value is --1.0. This is summarized in the following table. In this table, ``Zone'' means a thermal zone for which AirflowNetwork:Multizone:Zone has been specified. See object AirflowNetwork: Multizone:Zone for definition of ``Ventilation Control Mode.''
+
+% table 25
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Value of opening factor multiplier for different venting conditions. \label{table:value-of-opening-factor-multiplier-for}} \tabularnewline
+\toprule 
+Is surface in a Zone? & Ventilation Control Mode & Is surface venting? & Value of opening factor multiplier \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Value of opening factor multiplier for different venting conditions.} \tabularnewline
+\toprule 
+Is surface in a Zone? & Ventilation Control Mode & Is surface venting? & Value of opening factor multiplier \tabularnewline
+\midrule
+\endhead
+
+Yes & Temperature & Yes & 0.0 to 1.0 \tabularnewline
+No & -1.0 \tabularnewline
+Enthalpy & Yes & 0.0 to 1.0 \tabularnewline
+No & -1.0 \tabularnewline
+Constant & Yes & 1.0 \tabularnewline
+NoVent & No & -1.0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{AFN Surface Venting Inside Setpoint Temperature {[}C{]}}\label{afn-surface-venting-inside-setpoint-temperature-c}
+
+The time-step value of the venting setpoint temperature for the zone to which the surface belongs. This setpoint is determined from the Vent Temperature Schedule input (ref: AirflowNetwork:Multizone:Zone).
+
+\paragraph{\texorpdfstring{AFN Surface Venting Availability Status {[]}}{AFN Surface Venting Availability Status }}\label{afn-surface-venting-availability-status}
+
+A value of 1.0 means venting through the surface can occur if venting control conditions are satisfied. A value of 0.0 means venting through the surface cannot occur under any circumstances. This value is determined by the Venting Availability Schedule input (ref: AirflowNetwork:Multizone:Zone or AirflowNetwork:Multizone:Surface).
+
+\paragraph{AFN Zone Infiltration Sensible Heat Gain Rate {[}W{]}}\label{afn-zone-infiltration-sensible-heat-gain-rate-w}
+
+The average convective sensible heat gain rate, in Watts, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period. This value is calculated for each timestep when the outdoor dry-bulb temperature is higher than the zone temperature; otherwise, the sensible gain rate is set to 0.
+
+When a Fan:OnOff object is used, this reported value is weighted by the system run time fraction using the calculated infiltration sensible gain rate during the system on and off cycles for the reporting period:
+
+Infiltration Sensible Gain Rate = (Infiltration Sensible Gain Rate during on cycle * Run time fraction) + Infiltration Sensible Gain Rate during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Infiltration Sensible Heat Gain Energy {[}J{]}}\label{afn-zone-infiltration-sensible-heat-gain-energy-j}
+
+The average convective sensible heat gain, in Joules, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period. This value is calculated for each timestep when the outdoor dry-bulb temperature is higher than the zone temperature; otherwise, the sensible gain rate is set to 0.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration sensible gain during the system on and off cycles for the reporting period:
+
+Infiltration Sensible Gain = (Infiltration Sensible Gain during on cycle * Run time fraction) + Infiltration Sensible Gain during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Infiltration Sensible Heat Loss Rate {[}W{]}}\label{afn-zone-infiltration-sensible-heat-loss-rate-w}
+
+The average convective sensible heat loss rate, in Watts, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration sensible loss rate during the system on and off cycles for the reporting period:
+
+Infiltration Sensible Loss Rate = (Infiltration Sensible Loss Rate during on cycle * Run time fraction) + Infiltration Sensible Loss Rate during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Infiltration Sensible Heat Loss Energy {[}J{]}}\label{afn-zone-infiltration-sensible-heat-loss-energy-j}
+
+The average convective sensible heat loss, in Joules, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration sensible loss rate during the system on and off cycles for the reporting period:
+
+Infiltration Sensible Loss = (Infiltration Sensible Loss during on cycle * Run time fraction) + Infiltration Sensible Loss during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Infiltration Latent Heat Gain Rate {[}W{]}}\label{afn-zone-infiltration-latent-heat-gain-rate-w}
+
+The average convective latent heat gain rate, in Watts, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period, when the outdoor humidity ratio is higher than the zone air humidity ratio.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration latent gain rate during the system on and off cycles for the reporting period:
+
+Infiltration Latent Gain Rate = (Infiltration Latent Gain Rate during on cycle * Run time fraction) + Infiltration Latent Gain Rate during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Infiltration Latent Heat Gain Energy {[}J{]}}\label{afn-zone-infiltration-latent-heat-gain-energy-j}
+
+The total convective latent heat gain, in Joules, to the zone air corresponding to the Zone Infiltration Volume summed over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration latent gain during the system on and off cycles for the reporting period:
+
+Infiltration Latent Gain = (Infiltration Latent Gain during on cycle * Run time fraction) + Infiltration Latent Gain during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Infiltration Latent Heat Loss Rate {[}W{]}}\label{afn-zone-infiltration-latent-heat-loss-rate-w}
+
+The average convective latent heat loss rate, in Watts, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration latent loss rate during the system on and off cycles for the reporting period:
+
+Infiltration Latent Loss Rate = (Infiltration Latent Gain Loss Rate during on cycle * Run time fraction) + Infiltration Latent Loss Rate during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Infiltration Latent Heat Loss Energy {[}J{]}}\label{afn-zone-infiltration-latent-heat-loss-energy-j}
+
+The total convective latent heat loss, in Joules, to the zone air corresponding to the Zone Infiltration Volume summed over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration latent loss during the system on and off cycles for the reporting period:
+
+Infiltration Latent Loss = (Infiltration Latent Gain Loss during on cycle * Run time fraction) + Infiltration Latent Loss during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Mixing Sensible Heat Gain Rate {[}W{]}}\label{afn-zone-mixing-sensible-heat-gain-rate-w}
+
+The average convective sensible heat gain rate, in Watts, to the zone air corresponding to the Zone Mixing Volume averaged over the reporting period. The mixing-volume is defined as incoming volume flow from other adjacent zones where the air temperature is higher than the temperature in this zone. For example, there are two zones (Zone 2 and Zone 3) adjacent to this zone (Zone 1). Zone 1 receives airflows from both Zone 2 and Zone 3. The air temperature is 21°C in Zone 1. The air temperatures are 20°C in Zone 2 and 22°C in Zone 3. The sensible gain rate only includes heat gain from Zone 3 with respect to Zone 1. The energy received from Zone 2 is considered as a sensible loss, instead of a gain, because the air temperature in Zone 2 is lower than in Zone 1.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing sensible gain rate during the system on and off cycles for the reporting period:
+
+Mixing Sensible Gain Rate = (Mixing Sensible Gain Rate during on cycle * Run time fraction) + Mixing Sensible Gain Rate during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Mixing Sensible Heat Loss Rate {[}W{]}}\label{afn-zone-mixing-sensible-heat-loss-rate-w}
+
+The average convective sensible heat loss rate, in Watts, to the zone air corresponding to the Zone Mixing Volume averaged over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing sensible loss rate during the on and off cycles for the reporting period:
+
+Mixing Sensible Loss Rate = (Mixing Sensible Loss Rate during on cycle * Run time fraction) + Mixing Sensible Loss Rate during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Mixing Sensible Heat Gain Energy {[}J{]}}\label{afn-zone-mixing-sensible-heat-gain-energy-j}
+
+The total convective sensible heat gain, in Joules, to the zone air corresponding to the Zone Mixing Volume summed over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing sensible gain during the on and off cycles for the reporting period:
+
+Mixing Sensible Gain = (Mixing Sensible Gain during on cycle * Run time fraction) + Mixing Sensible Gain during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Mixing Sensible Heat Loss Energy {[}J{]}}\label{afn-zone-mixing-sensible-heat-loss-energy-j}
+
+The total convective sensible heat loss, in Joules, to the zone air corresponding to the Zone Mixing Volume summed over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing sensible loss during the on and off cycles for the reporting period:
+
+Mixing Sensible Loss = (Mixing Sensible Loss during on cycle * Run time fraction) + Mixing Sensible Loss during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Mixing Latent Heat Gain Rate {[}W{]}}\label{afn-zone-mixing-latent-heat-gain-rate-w}
+
+The average convective latent heat gain rate, in Watts, to the zone air corresponding to the Zone Mixing Volume averaged over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing latent gain rate during the on and off cycles for the reporting period:
+
+Mixing Latent Gain Rate = (Mixing Latent Gain Rate during on cycle * Run time fraction) + Mixing Latent Gain Rate during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Mixing Latent Heat Gain Energy {[}J{]}}\label{afn-zone-mixing-latent-heat-gain-energy-j}
+
+The total convective latent heat gain, in Joules, to the zone air corresponding to the Zone Mixing Volume summed over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing latent gain during the on and off cycles for the reporting period:
+
+Mixing Latent Gain = (Mixing Latent Gain during on cycle * Run time fraction) + Mixing Latent Gain during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Mixing Latent Heat Loss Rate {[}W{]}}\label{afn-zone-mixing-latent-heat-loss-rate-w}
+
+The average convective latent heat loss rate, in Watts, to the zone air corresponding to the Zone Mixing Volume averaged over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing latent loss rate during the on and off cycles for the reporting period:
+
+Mixing Latent Loss Rate = (Mixing Latent Loss Rate during on cycle * Run time fraction) + Mixing Latent Loss Rate during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Mixing Latent Heat Loss Energy {[}J{]}}\label{afn-zone-mixing-latent-heat-loss-energy-j}
+
+The total convective latent heat loss, in Joules, to the zone air corresponding to the Zone Mixing Volume summed over the reporting period.
+
+When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing latent loss during the on and off cycles for the reporting period:
+
+Mixing Latent Loss = (Mixing Latent Loss during on cycle * Run time fraction) + Mixing Latent Loss during off cycle * (1.0 -- Run time fraction)
+
+\paragraph{AFN Zone Mixing CO2 Mass Flow Rate {[}kg/s{]}}\label{afn-zone-mixing-co2-mass-flow-rate-kgs}
+
+This is a sum of mass flow rates from adjacent zones multiplied by the corresponding zone carbon dioxide concentration level to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the mixing mass flow rate calculated during the fan on and off periods for the simulation timestep.
+
+\paragraph{AFN Zone Mixing Generic Air Contaminant Mass Flow Rate {[}kg/s{]}}\label{afn-zone-mixing-generic-air-contaminant-mass-flow-rate-kgs}
+
+This is a sum of mass flow rates from adjacent zones multiplied by the corresponding zone generic contaminant concentration level to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the mixing mass flow rate calculated during the fan on and off periods for the simulation timestep.
+
+\paragraph{AFN Zone Duct Leaked Air Sensible Heat Gain Rate {[}W{]}}\label{afn-zone-duct-leaked-air-sensible-heat-gain-rate-w}
+
+This is the average sensible heat gain rate, in Watts, to a specific zone due to supply air leaks from the forced air distribution system. This value is averaged over the reporting period. A sensible heat gain occurs when duct air is warmer than zone air. It should be pointed out that when multiple supply air leaks are present in a single zone, the output value is the summation of all the supply air leak gains in this zone. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Leaked Air Sensible Heat Gain Energy {[}J{]}}\label{afn-zone-duct-leaked-air-sensible-heat-gain-energy-j}
+
+This is the total sensible heat gain, in Joules, to a specific zone due to supply air leaks summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Leaked Air Sensible Heat Loss Rate {[}W{]}}\label{afn-zone-duct-leaked-air-sensible-heat-loss-rate-w}
+
+This is the average sensible heat loss rate, in Watts, to a specific zone due to supply air leaks from the forced air distribution system. This value is averaged over the reporting period. A sensible heat loss occurs when duct air is cooler than zone air. It should be pointed out that when multiple supply air leaks are present in this zone, the output value is the summation of all the supply air leak losses in this zone. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Leaked Air Sensible Heat Loss Energy {[}J{]}}\label{afn-zone-duct-leaked-air-sensible-heat-loss-energy-j}
+
+This is the total sensible heat loss, in Joules, to a specific zone due to supply air leaks summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Leaked Air Latent Heat Gain Rate {[}W{]}}\label{afn-zone-duct-leaked-air-latent-heat-gain-rate-w}
+
+This is the average latent heat gain rate, in Watts, to a specific zone due to supply air leaks from the forced air distribution system for the reported time period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Leaked Air Latent Heat Gain Energy {[}J{]}}\label{afn-zone-duct-leaked-air-latent-heat-gain-energy-j}
+
+This is the total latent heat gain, in Joules, to a specific zone due to supply air leaks summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Leaked Air Latent Heat Loss Rate {[}W{]}}\label{afn-zone-duct-leaked-air-latent-heat-loss-rate-w}
+
+This is the average latent heat loss rate, in Watts, to a specific zone due to supply air leaks from the forced air distribution system for the reported time period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Leaked Air Latent Heat Loss Energy {[}J{]}}\label{afn-zone-duct-leaked-air-latent-heat-loss-energy-j}
+
+This is the total latent heat loss, in Joules, to a specific zone due to supply air leaks summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Conduction Sensible Heat Gain Rate {[}W{]}}\label{afn-zone-duct-conduction-sensible-heat-gain-rate-w}
+
+This is the average sensible heat gain rate, in Watts, of duct conduction to a specific zone where the ducts are located. This value is averaged over the reporting period. A sensible heat gain occurs when duct air is warmer than the zone air. It should be pointed out that when ducts are located in different zones, the total duct conduction loss should be the summation of the duct conduction losses in these zones. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Conduction Sensible Heat Gain Energy {[}J{]}}\label{afn-zone-duct-conduction-sensible-heat-gain-energy-j}
+
+This is the total sensible heat gain, in Joules, to a specific zone due to duct conduction summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Conduction Sensible Heat Loss Rate {[}W{]}}\label{afn-zone-duct-conduction-sensible-heat-loss-rate-w}
+
+This is the average sensible heat loss rate, in Watts, of duct conduction to a specific zone where the ducts are located. This value is averaged over the reporting period. A sensible heat loss occurs when duct air is cooler than the zone air. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Conduction Sensible Heat Loss Energy {[}J{]}}\label{afn-zone-duct-conduction-sensible-heat-loss-energy-j}
+
+This is the total sensible heat loss, in Joules, to a specific zone due to duct conduction summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Diffusion Latent Heat Gain Rate {[}W{]}}\label{afn-zone-duct-diffusion-latent-heat-gain-rate-w}
+
+This is the average latent heat gain rate, in Watts, of vapor diffusion through the walls of the air distribution system to a specific zone where the ducts are located. This value is averaged over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Diffusion Latent Heat Gain Energy {[}J{]}}\label{afn-zone-duct-diffusion-latent-heat-gain-energy-j}
+
+This is the total latent heat gain, in Joules, to a specific zone due to duct vapor diffusion summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Diffusion Latent Heat Loss Rate {[}W{]}}\label{afn-zone-duct-diffusion-latent-heat-loss-rate-w}
+
+This is the average latent heat loss rate, in Watts, of duct vapor diffusion to a specific zone where the ducts are located. This value is averaged over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Duct Diffusion Latent Heat Loss Energy {[}J{]}}\label{afn-zone-duct-diffusion-latent-heat-loss-energy-j}
+
+This is the total latent heat loss, in Joules, to a specific zone due to duct vapor diffusion summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Distribution Sensible Heat Gain Rate {[}W{]}}\label{afn-distribution-sensible-heat-gain-rate-w}
+
+This is the average total sensible heat gain rate, in Watts, in a specific zone caused by the forced air distribution system. The total sensible gain rate is the sum of duct leakage sensible gain rate and duct conduction sensible gain rate. This value is averaged over the reporting period. The multizone airflow sensible gain rate is excluded in this output variable. The output of multizone airflow sensible gain is reported in the previously-described output variables AFN Zone Infiltration Sensible Heat Gain Rate and AFN Zone Mixing Sensible Heat Gain Rate. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Distribution Sensible Heat Gain Energy {[}J{]}}\label{afn-distribution-sensible-heat-gain-energy-j}
+
+This is the total sensible heat gain, in Joules, in a specific zone caused by the forced air distribution system. The total sensible gain is the sum of duct leakage sensible gain and duct conduction sensible gain. This value is summed over the reporting period. The multizone airflow sensible gain is excluded in this output variable. The output of multizone airflow sensible gain is reported in the previously-described output variables AFN Zone Infiltration Sensible Heat Gain Energy and AFN Zone Mixing Sensible Heat Gain Energy. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Distribution Sensible Heat Loss Rate {[}W{]}}\label{afn-distribution-sensible-heat-loss-rate-w}
+
+This is the average total sensible heat loss rate, in Watts, in a specific zone caused by the forced air distribution system. The total sensible loss rate is the sum of duct leakage sensible loss rate and duct conduction sensible loss rate. This value is averaged over the reporting period. The multizone airflow sensible loss rate is excluded in this output variable. The output of multizone airflow sensible loss rate is reported in the previously-described output variables AFN Zone Infiltration Sensible Heat Loss Rate and AFN Zone Mixing Sensible Heat Loss Rate. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Distribution Sensible Heat Loss Energy {[}J{]}}\label{afn-distribution-sensible-heat-loss-energy-j}
+
+This is the total sensible heat loss, in Joules, in a specific zone caused by the forced air distribution system. The total sensible loss is the sum of duct leakage sensible loss and duct conduction sensible loss. This value is summed over the reporting period. The multizone airflow sensible loss is excluded in this output variable. The output of multizone airflow sensible loss is reported in the previously-described output variables AFN Zone Infiltration Sensible Heat Loss Energy and AFN Zone Mixing Sensible Heat Loss Energy. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Distribution Latent Heat Gain Rate {[}W{]}}\label{afn-distribution-latent-heat-gain-rate-w}
+
+This is the average total latent heat gain rate, in Watts, in a specific zone caused by the forced air distribution system. The total latent gain rate is the sum of duct leakage latent gain rate and duct conduction latent gain rate. This value is averaged over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Distribution Latent Heat Gain Energy {[}J{]}}\label{afn-distribution-latent-heat-gain-energy-j}
+
+This is the total latent heat gain, in Joules, in a specific zone caused by the forced air distribution system. The total latent gain is the sum of duct leakage latent gain and duct diffusion latent gain. This value is summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Distribution Latent Heat Loss Rate {[}W{]}}\label{afn-distribution-latent-heat-loss-rate-w}
+
+This is the average total latent heat loss rate, in Watts, in a specific zone caused by the forced air distribution system. The total latent loss rate is a sum of duct leakage latent loss rate and duct diffusion latent loss rate. This value is averaged over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Distribution Latent Heat Loss Energy {[}J{]}}\label{afn-distribution-latent-heat-loss-energy-j}
+
+This is the total latent heat loss, in Joules, in a specific zone caused by the forced air distribution system. The total latent loss is the sum of duct leakage latent loss and duct diffusion latent loss. This value is summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\textbf{NOTE:} The following output variables should not be confused with similar output variables for the infiltration, mixing, and cross mixing objects (Ref. Infiltration Output, Mixing Output, or Cross Mixing Output). The output variables described below refer to infiltration, mixing, and cross-mixing when an Airflow Network Simulation is performed. The following output variables are always used to describe infiltration, mixing, and cross mixing when the AirflowNetwork Control field in the AirflowNetwork:SimulationControl object is set to ``MultizoneWithoutDistribution'' or ``MultizoneWithDistribution''. In this case the output variables for the infiltration, mixing, and cross mixing objects will always be 0.
+
+In contrast, the following output variables are only used to describe infiltration, mixing, and cross mixing when the AirflowNetwork Control field in the AirflowNetwork:SimulationControl object is set to ``MultizoneAirflowWithDistributionOnlyDuringFanOperation'' and the fan is operating. When the fan is not operating, the output variables for the infiltration, mixing, and cross mixing objects are used.
+
+In the case where the AirflowNetwork Control field in the AirflowNetwork:SimulationControl object is set to ``NoMultizoneOrDistribution'', the following output variables are not used and the output variables for the infiltration, mixing, and cross mixing objects are used instead.
+
+\paragraph{AFN Zone Infiltration Sensible Heat Gain Energy {[}J{]}}\label{afn-zone-infiltration-sensible-heat-gain-energy-j-1}
+
+The total convective sensible heat gain, in Joules, to the zone air corresponding to the Zone Infiltration Volume summed over the reporting period. This value is calculated for each timestep when the outdoor dry-bulb temperature is higher than the zone temperature, otherwise the sensible gain is set to 0. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Infiltration Sensible Heat Loss Energy {[}J{]}}\label{afn-zone-infiltration-sensible-heat-loss-energy-j-1}
+
+The total convective sensible heat loss, in Joules to the zone air corresponding to the Zone Infiltration Volume summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
+
+\paragraph{AFN Zone Infiltration Volume {[}m3{]}}\label{afn-zone-infiltration-volume-m3}
+
+The volume of outdoor air flow into the zone from window/door openings and cracks in the exterior surfaces of the zone (i.e., the sum of ventilation and crack flows from the exterior into the zone). The zone air density is used to calculate the zone infiltration volume based on the mass flow rate. Note that AirflowNetwork Zone Infiltration Volume will be zero if all of the flows through the zone's exterior surfaces are out of the zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the infiltration volume calculated during the fan on and off periods for the simulation timestep.
+
+\paragraph{AFN Zone Infiltration Mass {[}kg{]}}\label{afn-zone-infiltration-mass-kg}
+
+The mass of air corresponding to the AirflowNetwork Zone Infiltration Volume. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the infiltration mass calculated during the fan on and off periods for the simulation timestep.
+
+\paragraph{AFN Zone Infiltration Air Change Rate {[}ach{]}}\label{afn-zone-infiltration-air-change-rate-ach}
+
+The number of air changes per hour produced by outdoor air flow into the zone from window/door openings and cracks in the exterior surfaces of the zone (i.e.~the sum of ventilation and crack flows from the exterior into the zone). The target zone air density is used to calculate the zone infiltration air change rate based on the mass flow rate Note that, like Zone Infiltration Volume, Zone Infiltration Air Change Rate will be zero if all flows through the zone's exterior surfaces are out of the zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the infiltration air change rate calculated during the fan on and off periods for the simulation timestep.
+
+\paragraph{AFN Zone Mixing Volume {[}m3{]}}\label{afn-zone-mixing-volume-m3}
+
+This is a measure of interzone air flow for each thermal zone. It is the volume of air flow into the zone from adjacent zones through window/door openings and cracks in the interior heat transfer surfaces of the zone. The target zone air density is used to calculate the zone mixing volume based on the mass flow rate. This variable does not include flows that are from the zone to adjacent zones. Note that Zone Mixing Volume will be zero if all flows through the zone's interior surfaces are out of the zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the mixing volume calculated during the fan on and off periods for the simulation timestep.
+
+\paragraph{AFN Zone Mixing Mass {[}kg{]}}\label{afn-zone-mixing-mass-kg}
+
+The mass of air corresponding to the AFN Zone Mixing Volume. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the mixing mass calculated during the fan on and off periods for the simulation timestep.
+
+\paragraph{AFN Zone Mixing Mass Flow Rate {[}kg/s{]}}\label{afn-zone-mixing-mass-flow-rate-kgs}
+
+This is a sum of mass flow rates from adjacent zones to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the mixing mass flow rate calculated during the fan on and off periods for the simulation timestep.
+
+\paragraph{AFN Zone Outdoor Air CO2 Mass Flow Rate {[}kg/s{]}}\label{afn-zone-outdoor-air-co2-mass-flow-rate-kgs}
+
+This is a sum of mass flow rates from outdoors multiplied by the outdoor carbon dioxide concentration level to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the outdoor mass flow rate calculated during the fan on and off periods for the simulation timestep.
+
+\paragraph{AFN Zone Outdoor Air Generic Air Contaminant Mass Flow Rate {[}kg/s{]}}\label{afn-zone-outdoor-air-generic-air-contaminant-mass-flow-rate-kgs}
+
+This is a sum of mass flow rates from outdoors multiplied by the outdoor generic air contaminant concentration level to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the outdoor mass flow rate calculated during the fan on and off periods for the simulation timestep
+
+\paragraph{AFN Zone Outdoor Air Mass Flow Rate {[}kg/s{]}}\label{afn-zone-outdoor-air-mass-flow-rate-kgs}
+
+This is a sum of mass flow rates from outdoors to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the outdoor mass flow rate calculated during the fan on and off periods for the simulation timestep.
+
+\paragraph{AFN Zone Total CO2 Mass Flow Rate {[}kg/s{]}}\label{afn-zone-total-co2-mass-flow-rate-kgs}
+
+This is a sum of mass flow rates from adjacent zones or outdoors multiplied by the carbon dioxide concentration differences between the corresponding zone and the receiving zone.
+
+\paragraph{AFN Zone Total Generic Air Contaminant Mass Flow Rate {[}kg/s{]}}\label{afn-zone-total-generic-air-contaminant-mass-flow-rate-kgs}
+
+This is a sum of mass flow rates from adjacent zones or outdoors multiplied by the generic contaminant concentration differences between the corresponding zone and the receiving zone.
+
+The following output variables are reported only when an AirflowNetwork:OccupantVentilationControl object is used:
+
+\paragraph{\texorpdfstring{AFN Surface Venting Window or Door Opening Factor at Previous Time Step {[]}}{AFN Surface Venting Window or Door Opening Factor at Previous Time Step }}\label{afn-surface-venting-window-or-door-opening-factor-at-previous-time-step}
+
+The value of the venting opening factor for a particular window or door at the previous time step. When the window or door is venting, this is the input value of the opening factor (see AirflowNetwork:Multizone:Surface, Window/Door Opening Factor) times the multiplier for venting modulation (see description of next output variable, ``Opening Factor Multiplier for AirflowNetwork Venting Modulation''). For example, if the input Window/Door opening factor is 0.5 and the modulation multiplier is 0.7, then the value of this output variable will be 0.5*0.7 = 0.35.
+
+\paragraph{AFN Surface Opening Elapsed Time {[}min{]}}\label{afn-surface-opening-elapsed-time-min}
+
+This output is the opening elapsed time in the units of minutes since the window opened.
+
+\paragraph{AFN Surface Closing Elapsed Time {[}min{]}}\label{afn-surface-closing-elapsed-time-min}
+
+This output is the opening elapsed time in the units of minutes since the windows closed.
+
+\paragraph{\texorpdfstring{AFN Surface Opening Status at Previous Time Step {[]}}{AFN Surface Opening Status at Previous Time Step }}\label{afn-surface-opening-status-at-previous-time-step}
+
+This is the window or door opening factor control status at the previous time step using an AirflowNetwork:OccupantVentilationControl object, which can have three integer values: 0, 1, and 2. A 0 value indicates no occupant ventilation control. The opening factor is determined by the Ventilation Control Mode field. A value of 1 indicates that a window or door is allowed to open. The value of 1 is determined when the opening elapsed time is less than the minimum opening time. A value of 2 denotes that a window or door is forced to close. The value of 2 is determined when the closing elapsed time is less than the minimum closing time.
+
+\paragraph{\texorpdfstring{AFN Surface Opening Status {[]}}{AFN Surface Opening Status }}\label{afn-surface-opening-status}
+
+This is the window or door opening factor control status at the current time step using an AirflowNetwork:OccupantVentilationControl object, which can have three integer values: 0, 1, and 2. A 0 value indicates no occupant ventilation control. The opening factor is determined by the Ventilation Control Mode field. A value of 1 indicates that a window or door is allowed to open. The value of 1 is determined when the opening elapsed time is less than the minimum opening time. A value of 2 denotes that a window or door is forced to close. The value of 2 is determined when the closing elapsed time is less than the minimum closing time.
+
+\paragraph{\texorpdfstring{AFN Surface Opening Probability Status {[]}}{AFN Surface Opening Probability Status }}\label{afn-surface-opening-probability-status}
+
+This is the opening probability status at the current time step using an AirflowNetwork:OccupantVentilationControl object, which can have three integer values: 0, 1, and 2. A 0 value indicates no opening probability control action. A value of 1 indicates that a window or door is forced to open when the opening status is 0. A value of 2 denotes that the status at the previous time step will be kept.
+
+\paragraph{\texorpdfstring{AFN Surface Closing Probability Status {[]}}{AFN Surface Closing Probability Status }}\label{afn-surface-closing-probability-status}
+
+This is the closing probability status at the current time step using an AirflowNetwork:OccupantVentilationControl object, which can have three integer values: 0, 1, and 2. A 0 value indicates no closing probability control action. A value of 1 indicates that a window or door is forced to close when the opening status is 0. A value of 2 denotes that the status at the previous time step will be kept.
+
+\paragraph{RoomAirflowNetwork Node Temperature {[}C{]}}\label{roomairflownetwork-node-temperature-c}
+
+This is the RoomAirflowNetwork node temperature output in degrees C.
+
+\paragraph{RoomAirflowNetwork Node Humidity Ratio {[}kgWater/kgDryAir{]}}\label{roomairflownetwork-node-humidity-ratio-kgwaterkgdryair}
+
+This is the RoomAirflowNetwork node humidity ratio output in kgWater/kgDryAir.
+
+\paragraph{RoomAirflowNetwork Node Total Pressure {[}Pa{]}}\label{roomairflownetwork-node-total-pressure-pa}
+
+This is the RoomAirflowNetwork node total pressure in Pa with respect to outdoor barometric pressure. The total pressure is the sum of static pressure, dynamic pressure, and elevation impact at the node's relative height.
diff --git a/doc/input-output-reference/src/overview/group-airflow.tex b/doc/input-output-reference/src/overview/group-airflow.tex
new file mode 100644
index 00000000000..ad1cfd2c2b2
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-airflow.tex
@@ -0,0 +1,2373 @@
+\section{Group -- Airflow}\label{group-airflow}
+
+An important characteristic of energy consumption in buildings is the airflow between zones and airflow due to natural ventilation (e.g., open windows) or mechanically-induced ventilation (e.g., exhaust air fans). This group of objects describes those elements.
+
+The AirflowNetwork model can also be used to model infiltration and mixing (zone-to-zone air flow) with or without the HVAC air distribution system operating (see Group -- Airflow Network).
+
+\subsection{ZoneInfiltration:DesignFlowRate}\label{zoneinfiltrationdesignflowrate}
+
+Infiltration is the unintended flow of air from the outdoor environment directly into a thermal zone. Infiltration is generally caused by the opening and closing of exterior doors, cracks around windows, and even in very small amounts through building elements. The basic equation used to calculate infiltration with this object is:
+
+\begin{equation}
+  \rm{Infiltration} = \left( {{I_{design}}} \right)\left( {{F_{schedule}}} \right)\left[ {A + B\left| {\left( {{T_{zone}} - {T_{odb}}} \right)} \right| + C\left( {WindSpeed} \right) + D\left( {Windspee{d^2}} \right)} \right]
+\end{equation}
+
+More advanced infiltration calculations are possible using the EnergyPlus AirflowNetwork model for natural infiltration driven by wind and/or by forced air. Infiltration described by the equation shown above is entered into EnergyPlus using the following syntax. Exfiltration (the leakage of zone air to the outside) is generally handled better as zone exhaust air in the zone equipment description. The equation must always yield a non-negative results; negative values are set to 0.0.
+
+The question of typical values for these coefficients is subject to debate. Ideally, one should do a detailed analysis of the infiltration situation and then determine a custom set of coefficients using methods such as those laid out in Chapter 26 of the ASHRAE Handbook of Fundamentals. The EnergyPlus defaults are 1,0,0,0 which give a constant volume flow of infiltration under all conditions.
+
+BLAST (one of the EnergyPlus predecessors) used the following values as defaults: 0.606, 0.03636, 0.1177, 0. These coefficients produce a value of 1.0 at 0C deltaT and 3.35 m/s (7.5 mph) windspeed, which corresponds to a typical summer condition. At a winter condition of 40C deltaT and 6 m/s (13.4 mph) windspeed, these coefficients would increase the infiltration rate by a factor of 2.75.
+
+In DOE-2 (the other EnergyPlus predecessor), the air change method defaults are (adjusted to SI units) 0, 0, 0.224 (windspeed), 0. With these coefficients, the summer conditions above would give a factor of 0.75, and the winter conditions would give 1.34. A windspeed of 4.47 m/s (10 mph) gives a factor of 1.0.
+
+The source of the BLAST defaults is noted in the BLAST documentation as:
+
+``Empirical equation and the coefficient default were determined from ASHRAE journal articles and other data on the effects of outdoor weather conditions.''
+
+The source of the DOE-2 defaults is based on examining the infiltration relationships described in the ASHRAE Handbook of Fundamentals.
+
+The EnergyPlus example files use all of the above, the BLAST defaults in some (e.g., GeometryTest), the DOE-2 defaults in some (e.g., 5ZoneAirCooled), and the EnergyPlus defaults in some (e.g., LgOffVAVDetCoil).
+
+The local outdoor dry-bulb temperature used in the above basic equation (T\(_{odb}\)) is typically a function of the height of the zone centroid above ground. The corresponding zone name is given in the second field. The local outdoor dry-bulb temperature calculation procedure is given in the section of ``Local Outdoor Air Temperature Calculation'' in the Engineering Reference.
+
+The local outdoor wind speed used in the above basic equation (WindSpeed) is also a function of the height of the zone centroid above ground. The corresponding zone name is given in the second filed. The local outdoor wind speed calculation procedure is given in the section of ``Local Wind Speed Calculation'' in the Engineering Reference.
+
+\begin{callout}
+  Note: When the value of the Wind Speed Profile Exponent field in the Site:HeightVariation is equal to 0.0. The local wind speed is always equal to the wind speed given in the weather data and will not be dependent on zone centroid height. Similarly, if the value of the Air Temperature Gradient Coefficient is set equal to 0 the local air dry-bulb temperature is also always equal to the air dry-bulb temperature given in the weather data and will not be dependent on zone centroid height.
+\end{callout}
+
+One or more infiltration objects can be defined for each zone, and the resulting infiltration rate for the zone will simply be the summation of the flow rates specified by the infiltration objects.
+
+\subsubsection{Inputs}\label{inputs-005}
+
+\paragraph{Field: Name}\label{field-name-005}
+
+The name of the ZoneInfiltration:DesignFlowRate object. This needs to be unique across all different ZoneInfiltration objects.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name}
+
+This field is the name of the zone (ref: Zone) or ZoneList (ref: ZoneLIst) and attaches a particular infiltration statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this infiltration definition is applied to each of the zones in the zone list effecting a global definition for the amount of infiltration flow rate in the zone. The Zonelist option can be used effectively with the flow/area, flow/exteriorarea, flow/exteriorwallarea, or airchanges/hour of the Design Flow Rate Calculation Method.
+
+The name of the actual infiltration object becomes \textless{}Zone Name\textgreater{} \textless{}ZoneInfiltration:DesignFlowRate Object Name\textgreater{} and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-000}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design volume flow rate (I\(_{design}\)) (see Design Flow Rate Calculation Method field and related subsequent fields). This fraction between 0.0 and 1.0 is noted as F\(_{schedule}\) in the above equation.
+
+\paragraph{Field: Design Flow Rate Calculation Method}\label{field-design-flow-rate-calculation-method}
+
+This field is a key/choice field that tells which of the next four fields are filled and is descriptive of the method for calculating the design volume flow rate. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Zone
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the design volume flow rate.~ (The Design Flow Rate field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The flow per Zone Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/ExteriorArea
+\end{itemize}
+
+With this choice, the method used will be a factor per exterior surface area of the zone. (The flow per Exterior Surface Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/ExteriorWallArea
+\end{itemize}
+
+With this choice, the method used will be a factor per exterior wall surface area of the zone. (The flow per Exterior Surface Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  AirChanges/Hour
+\end{itemize}
+
+With this choice, the method used will be the number of air changes per hour for the infiltration amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. (The Air Changes per Hour field should be filled).
+
+\paragraph{Field: Design Flow Rate}\label{field-design-flow-rate}
+
+This field denotes the full design volume flow rate (m\(^{3}\)/s). The previous field should choose ``flow/zone'' as the choice. The design volume flow rate (noted as I\(_{design}\) in the above equation) is the maximum amount of infiltration expected at design conditions. The design value is modified by the schedule fraction (see Field:Schedule Name) and user specified coefficients (see ''coefficient'' fields below). The resulting volume flow rate is converted to mass flow using the current outdoor air density at each time step.
+
+\paragraph{Field: Flow per Zone Floor Area}\label{field-flow-per-zone-floor-area}
+
+This factor (m\(^{3}\)/s-m\(^{2}\)) is used, along with the Zone Area to determine the maximum Design Flow Rate as described in the Design Flow Rate field. The choice from the method field should be ``Flow/Area''.
+
+\paragraph{Field: Flow per Exterior Surface Area}\label{field-flow-per-exterior-surface-area}
+
+This factor (m\(^{3}\)/s-m\(^{2}\)) is used, along with the Exterior Surface Area in the Zone to determine the maximum Design Flow Rate as described in the Design Flow Rate field. The choice from the method field should be ``Flow/Exteriorarea'' or ``Flow/ExteriorWallArea''.
+
+\paragraph{Field: Air Changes per Hour}\label{field-air-changes-per-hour}
+
+This factor is used, along with the Zone Volume to determine the maximum Design Flow Rate as described in the Design Flow Rate field. The choice from the method field should be ``AirChanges/Hour''.
+
+\paragraph{Field: Constant Term Coefficient}\label{field-constant-term-coefficient}
+
+This number is the ``A'' parameter in the above infiltration equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter, however, is a constant under all conditions and is not modified by any environmental effect. As a result, it is dimensionless.
+
+\paragraph{Field: Temperature Term Coefficient}\label{field-temperature-term-coefficient}
+
+This number is the ``B'' parameter in the above infiltration equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the temperature difference between the outdoor and indoor air dry-bulb temperatures. The units for this parameter are inverse Celsius.
+
+\paragraph{Field: Velocity Term Coefficient}\label{field-velocity-term-coefficient}
+
+This number is the ``C'' parameter in the above infiltration equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the speed of wind being experienced outside the building. The units for this parameter are s/m.
+
+\paragraph{Field: Velocity Squared Term Coefficient}\label{field-velocity-squared-term-coefficient}
+
+This number is the ``D'' parameter in the above infiltration equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by square of the speed of wind being experienced outside the building. The units for this parameter are s\(^{2}\)/m\(^{2}\).
+
+An IDF example:
+
+\begin{lstlisting}
+
+ZoneInfiltration:DesignFlowRate,
+    Infiltration 1,   !- Name
+    DORM ROOMS AND COMMON AREAS, !- Zone Name
+    Infiltration Sch, !- Schedule Name
+    Flow/Zone,      !- Design Flow Rate Calculation Method
+    2.831685,       !- Design Flow Rate {m3/s}
+    ,               !- Flow per Zone Floor Area {m3/s/m2}
+    ,               !- Flow per Exterior Surface Area {m3/s/m2}
+    ,               !- Air Changes per Hour
+    0.6060000    ,  !- Constant Term Coefficient
+    3.6359996E-02,  !- Temperature Term Coefficient
+    0.1177165    ,  !- Velocity Term Coefficient
+    0.0000000E+00;  !- Velocity Squared Term Coefficient
+\end{lstlisting}
+
+Global Infiltration example:
+
+\begin{lstlisting}
+
+  ZoneList,OfficeZones,Left Fork, Middle Fork, Right Fork;
+
+
+    ZoneInfiltration:DesignFlowRate,
+      OfficeZones Infiltration,       !- Name
+      OfficeZones,             !- Zone or ZoneList Name
+      Infiltration Sch,        !- Schedule Name
+      AirChanges/Hour,         !- Design Flow Rate Calculation Method
+      ,                        !- Design Flow Rate {m3/s}
+      ,                        !- Flow per Zone Floor Area {m3/s-m2}
+      ,                        !- Flow per Exterior Surface Area {m3/s-m2}
+      4.7,                     !- Air Changes per Hour
+      0.6060000,               !- Constant Term Coefficient
+      3.6359996E-02,           !- Temperature Term Coefficient
+      0.1177165,               !- Velocity Term Coefficient
+      0.0000000E+00;           !- Velocity Squared Term Coefficient
+\end{lstlisting}
+
+\subsection{ZoneInfiltration:EffectiveLeakageArea}\label{zoneinfiltrationeffectiveleakagearea}
+
+ZoneInfiltration:EffectiveLeakageArea model is similar to the other infiltration objects but uses a different equation to model the unintended flow of air from the outdoor environment directly into a thermal zone.~ Infiltration is generally caused by the opening and closing of exterior doors, cracks around windows, and even in very small amounts through building elements.~ This model is based on work by Sherman and Grimsrud (1980) and is appropriate for smaller, residential-type buildings.~ The equation used to calculate infiltration in the effective leakage area model is:
+
+\begin{equation}
+Infiltration = \left( {{F_{Schedule}}} \right)\frac{{{A_L}}}{{1000}}\sqrt {{C_s}\Delta T + {C_w}{{\left( {WindSpeed} \right)}^2}}
+\end{equation}
+
+where \(\Delta T\) ~is the average difference between zone air temperature and the outdoor air temperature and the other coefficients are described below.
+
+Note that the coefficients for the ``EffectiveLeakageArea'' model are not interchangeable with the similarly named coefficients in the ``FlowCoefficient'' model (see ZoneInfiltration:FlowCoefficient object).
+
+One or more infiltration objects of different types can be defined for each zone, and the resulting infiltration rate for the zone will simply be the summation of the flow rates specified by the infiltration objects.
+
+\subsubsection{Inputs}\label{inputs-1-005}
+
+\paragraph{Field: Name}\label{field-name-1-004}
+
+The name of the ZoneInfiltration:EffectiveLeakageArea object.~ This needs to be unique across all different ZoneInfiltration objects.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-002}
+
+This field is the name of the zone (ref: Zone) and attaches a particular infiltration statement to a thermal zone in the building.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-1}
+
+This field is the name of a schedule (ref: Schedule) that modifies the volume flow rate calculated by the model. This fraction between 0.0 and 1.0 is noted as F\(_{schedule}\) in the above equation.
+
+\paragraph{Field: Effective Air Leakage Area}\label{field-effective-air-leakage-area}
+
+This field is the effective air leakage area, in cm\(^{2}\), at 4 Pa. This is the value \({A_L}\) in the equation above. Effective leakage area data can be obtained from a whole-building pressure test (eg. blower door test). ASHRAE Handbook of Fundamentals also lists typical values component leakage areas for low-rise residential (e.g.~Table~\ref{table:values-for-terrain} in Chapter 26 of HoF 2001). The value should correspond to a pressure difference of 4 Pa.
+
+\paragraph{Field: Stack Coefficient}\label{field-stack-coefficient}
+
+This field is the value of the stack coefficient, \({C_s}\) in the equation above. The coefficient has units of (L/s)\(^{2}\)/(cm\(^{4}\)·K). Values for the ``Basic Model Stack Coefficient'' listed in the ASHRAE Handbook of Fundamentals (2005 and 2001) are:
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Shelter class & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Shelter class & Description \tabularnewline
+\midrule
+\endhead
+
+1 & No obstructions or local shielding \tabularnewline
+2 & Typical shelter for an isolated rural house \tabularnewline
+3 & Typical shelter caused by other buildings across the street \tabularnewline
+4 & Typical shelter for urban buildings on larger lots \tabularnewline
+5 & Typical shelter produced by buildings that are immediately adjacent. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Field: Wind Coefficient}\label{field-wind-coefficient}
+
+This field is the value of the wind coefficient, \({C_w}\) in the equation above. The coefficient has units of (L/s)\(^{2}\)/(cm\(^{4}\)·(m/s)\(^{2}\)). Values for the ``Basic Model Wind Coefficient'' listed in the ASHRAE Handbook of Fundamentals (2005 chapter 27; 2001, Chapter 26) depend on the type of shelter and are listed in the following tables.
+
+\begin{longtable}[c]{@{}llll@{}}
+\toprule
+Shelter class & One story house & Two story house & Three story house \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Shelter class & One story house & Two story house & Three story house \tabularnewline
+\midrule
+\endhead
+
+1 & 0.000319 & 0.000420 & 0.000494 \tabularnewline
+2 & 0.000246 & 0.000325 & 0.000382 \tabularnewline
+3 & 0.000174 & 0.000231 & 0.000271 \tabularnewline
+4 & 0.000104 & 0.000137 & 0.000161 \tabularnewline
+5 & 0.000032 & 0.000042 & 0.000049 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Shelter class & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Shelter class & Description \tabularnewline
+\midrule
+\endhead
+
+1 & No obstructions or local shielding \tabularnewline
+2 & Typical shelter for an isolated rural house \tabularnewline
+3 & Typical shelter caused by other buildings across the street \tabularnewline
+4 & Typical shelter for urban buildings on larger lots \tabularnewline
+5 & Typical shelter produced by buildings that are immediately adjacent. \tabularnewline
+\bottomrule
+\end{longtable}
+
+An example IDF object is
+
+\begin{lstlisting}
+
+ZoneInfiltration:EffectiveLeakageArea,
+      LIVING ZONE Infil 1,     !- Name
+      LIVING ZONE,             !- Zone Name
+      INF-SCHED,               !- Schedule Name
+      500.0,                   !- Effective Air Leakage Area
+      0.000145,                !- Stack Coefficient
+      0.000174 ;               !- Wind Coefficient
+\end{lstlisting}
+
+\subsection{ZoneInfiltration:FlowCoefficient}\label{zoneinfiltrationflowcoefficient}
+
+ZoneInfiltration:FlowCoefficient model is similar to the other infiltration objects but uses a different equation to model the unintended flow of air from the outdoor environment directly into a thermal zone.~ Infiltration is generally caused by the opening and closing of exterior doors, cracks around windows, and even in very small amounts through building elements.~ This reformulated model is based on the AIM-2 model by Walker and Wilson (1998) and is appropriate for smaller, residential-type buildings.~ The equation used to calculate infiltration in the flow coefficient model is:
+
+\begin{equation}
+Infiltration = \left( {{F_{Schedule}}} \right)\sqrt {{{\left( {c\,{C_s}\Delta {T^n}} \right)}^2} + {{\left( {c\,{C_w}{{\left( {s * WindSpeed} \right)}^{2n}}} \right)}^2}}
+\end{equation}
+
+Where \(\Delta T\) ~is the average difference between zone air temperature and the outdoor air temperature and the other coefficients are described below.
+
+Note that the coefficients for the ``Flow Coefficient'' model are not interchangeable with the similarly named coefficients in the ``Effective Leakage Area'' model (see ZoneInfiltration:EffectiveLeakageArea object).
+
+One or more infiltration objects of different types can be defined for each zone, and the resulting infiltration rate for the zone will simply be the summation of the flow rates specified by the infiltration objects.
+
+\subsubsection{Inputs}\label{inputs-2-005}
+
+\paragraph{Field: Name}\label{field-name-2-004}
+
+The name of the ZoneInfiltration:FlowCoefficient object. This needs to be unique across all different ZoneInfiltration objects.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-001}
+
+This field is the name of the zone (ref: Zone) and attaches a particular infiltration statement to a thermal zone in the building.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-2}
+
+This field is the name of a schedule (ref: Schedule) that modifies the volume flow rate calculated by the model. This fraction between 0.0 and 1.0 is noted as F\(_{schedule}\) in the above equation.
+
+\paragraph{Field: Flow Coefficient}\label{field-flow-coefficient}
+
+This field is the flow coefficient in m\(^{3}\)/(s·Pa\(^{n}\)).~ This is the value \(c\) ~in the equation above.~ The flow coefficient can be determined from the effective leakage area and whole-building pressure tests (eg. blower door test).
+
+\paragraph{Field: Stack Coefficient}\label{field-stack-coefficient-1}
+
+This field is the value of the stack coefficient, \({C_s}\) ~in the equation above.~ The coefficient has units of (Pa/K)\(^{n}\). Values for the ``Enhanced Model Stack Coefficient'' listed in the ASHRAE Handbook of Fundamentals (2005 and 2001) are:
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Shelter class & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Shelter class & Description \tabularnewline
+\midrule
+\endhead
+
+1 & No obstructions or local shielding \tabularnewline
+2 & Typical shelter for an isolated rural house \tabularnewline
+3 & Typical shelter caused by other buildings across the street \tabularnewline
+4 & Typical shelter for urban buildings on larger lots \tabularnewline
+5 & Typical shelter produced by buildings that are immediately adjacent. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Field: Pressure Exponent}\label{field-pressure-exponent}
+
+This field is the value of the pressure exponent, \emph{n} in the equation above.~ The pressure exponent generally lies between 0.6 and 0.7 with a typical value of \emph{n} = 0.67 for the enhanced model.
+
+\paragraph{Field: Wind Coefficient}\label{field-wind-coefficient-1}
+
+This field is the value of the wind coefficient, \({C_w}\) ~in the equation above.~ The coefficient has units of (Pa·s\(^{2}\)/m\(^{2}\))\(^{n}\) .~ Values for the ``Enhanced Model Wind Coefficient'' listed in the ASHRAE Handbook of Fundamentals (2005 and 2001) are:
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Shelter class & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Shelter class & Description \tabularnewline
+\midrule
+\endhead
+
+1 & No obstructions or local shielding \tabularnewline
+2 & Typical shelter for an isolated rural house \tabularnewline
+3 & Typical shelter caused by other buildings across the street \tabularnewline
+4 & Typical shelter for urban buildings on larger lots \tabularnewline
+5 & Typical shelter produced by buildings that are immediately adjacent. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Field: Shelter Factor}\label{field-shelter-factor}
+
+This field is the value of the wind coefficient, \(s\) ~in the equation above.~ The coefficient is dimensionless.~ Values for the ``Enhanced Model Shelter Factor'' listed in the ASHRAE Handbook of Fundamentals (2005 and 2001) are:
+
+\begin{longtable}[c]{@{}lllll@{}}
+\toprule
+Shelter class & No Flue & One story house with flue & Two story house with flue & Three story house with flue \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule
+Shelter class & No Flue & One story house with flue & Two story house with flue & Three story house with flue \tabularnewline
+\midrule
+\endhead
+
+1 & 1.00 & 1.10 & 1.07 & 1.06 \tabularnewline
+2 & 0.90 & 1.02 & 0.98 & 0.97 \tabularnewline
+3 & 0.70 & 0.86 & 0.81 & 0.79 \tabularnewline
+4 & 0.50 & 0.70 & 0.64 & 0.61 \tabularnewline
+5 & 0.30 & 0.54 & 0.47 & 0.43 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Shelter class & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Shelter class & Description \tabularnewline
+\midrule
+\endhead
+
+1 & No obstructions or local shielding \tabularnewline
+2 & Typical shelter for an isolated rural house \tabularnewline
+3 & Typical shelter caused by other buildings across the street \tabularnewline
+4 & Typical shelter for urban buildings on larger lots \tabularnewline
+5 & Typical shelter produced by buildings that are immediately adjacent. \tabularnewline
+\bottomrule
+\end{longtable}
+
+An Example IDF object is:
+
+\begin{lstlisting}
+ZoneInfiltration:FlowCoefficient,
+      LIVING ZONE Infil 1,     !- Name
+      LIVING ZONE,             !- Zone Name
+      INF-SCHED,               !- Schedule Name
+      0.05,                    !- Flow Coefficient
+      0.089,                   !- Stack Coefficient
+       0.67  ,                 !- Pressure Exponent
+      0.156 ,                  !- Wind Coefficient
+      0.64;                    !- Shelter Factor
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-003}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Zone Infiltration Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Infiltration Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Infiltration Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Infiltration Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Infiltration Total Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Infiltration Total Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,Zone Infiltration Current Density Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Zone Infiltration Standard Density Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Infiltration Current Density Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Infiltration Standard Density Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Infiltration Mass {[}kg{]}
+\item
+  HVAC,Sum,Zone Infiltration Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Infiltration Air Change Rate {[}ach{]}
+\end{itemize}
+
+Note: If ZoneInfiltration:* objects and ZoneAirBalance:OutdoorAir (with Air Balance Method = Quadrature) objects reference the same Zone Name, the above infiltration output variables will not be reported for that zone. Instead, output variables for zone outdoor air flow will be reported by the corresponding ZoneAirBalance:OutdoorAir object.
+
+\paragraph{Zone Infiltration Sensible Heat Loss Energy {[}J{]}}\label{zone-infiltration-sensible-heat-loss-energy-j}
+
+The sensible (temperature) heat loss that occurs when the infiltration air temperature (outdoor) \textless{} zone air temperature.
+
+\paragraph{Zone Infiltration Sensible Heat Gain Energy {[}J{]}}\label{zone-infiltration-sensible-heat-gain-energy-j}
+
+The sensible (temperature) heat gain that occurs when the infiltration air temperature (outdoor) \textgreater{} = zone air temperature.
+
+\paragraph{Zone Infiltration Latent Heat Loss Energy {[}J{]}}\label{zone-infiltration-latent-heat-loss-energy-j}
+
+The latent heat loss that occurs when the infiltration air humidity ratio (outdoor) \textless{} zone air humidity ratio.
+
+\paragraph{Zone Infiltration Latent Heat Gain Energy {[}J{]}}\label{zone-infiltration-latent-heat-gain-energy-j}
+
+The latent heat gain that occurs when the infiltration air humidity ratio (outdoor) \textgreater{} = zone air humidity ratio.
+
+\paragraph{Zone Infiltration Total Heat Loss Energy {[}J{]}}\label{zone-infiltration-total-heat-loss-energy-j}
+
+The total heat loss that occurs when the sum of Zone Infiltration Sensible Heat Gain Energy and Zone Infiltration Latent Heat Gain Energy \textless{} the sum of Zone Infiltration Sensible Heat Loss Energy and Zone Infiltration Latent Heat Loss Energy.
+
+\paragraph{Zone Infiltration Total Heat Gain Energy {[}J{]}}\label{zone-infiltration-total-heat-gain-energy-j}
+
+The total heat gain that occurs when the sum of Zone Infiltration Sensible Heat Gain Energy and Zone Infiltration Latent Heat Gain Energy \textgreater{} = the sum of Zone Infiltration Sensible Heat Loss Energy and Zone Infiltration Latent Heat Loss Energy.
+
+\paragraph{Zone Infiltration Current Density Volume~ {[}m3{]}}\label{zone-infiltration-current-density-volume-m3}
+
+\paragraph{Zone Infiltration Current Density Volume Flow Rate {[}m3/s{]}}\label{zone-infiltration-current-density-volume-flow-rate-m3s}
+
+These outputs are the total volume and volume flow rate of infiltration air based on the current density of zone air.
+
+\paragraph{Zone Infiltration Standard Density Volume {[}m3{]}}\label{zone-infiltration-standard-density-volume-m3}
+
+\paragraph{Zone Infiltration Standard Density Volume Flow Rate {[}m3/s{]}}\label{zone-infiltration-standard-density-volume-flow-rate-m3s}
+
+These outputs are the total volume and volume flow rate of infiltration air based on the standard density of air.~ Standard density in EnergyPlus corresponds to 20ºC drybulb, dry air, and nominally adjusted for elevation.
+
+\paragraph{Zone Infiltration Mass {[}kg{]}}\label{zone-infiltration-mass-kg}
+
+The mass flow of the Infiltration air.
+
+\paragraph{Zone Infiltration Mass Flow Rate {[}kg/s{]}}\label{zone-infiltration-mass-flow-rate-kgs}
+
+The mass flow rate of the Infiltration air.
+
+\paragraph{Zone Infiltration Air Change Rate {[}ach{]}}\label{zone-infiltration-air-change-rate-ach}
+
+The rate of infiltration in air changes per hour.
+
+\subsection{ZoneVentilation:DesignFlowRate}\label{zoneventilationdesignflowrate}
+
+Ventilation is the purposeful flow of air from the outdoor environment directly into a thermal zone in order to provide some amount of non-mechanical cooling. Ventilation, as specified by the input syntax for the ZoneVentilation:DesignFlowRate object, is intended to model ``simple'' ventilation as opposed to the more detailed ventilation investigations that can be performed with the AirflowNetwork model or with air systems that have outdoor air mixers. Zone ventilation, as specified via this input object, can be controlled by a schedule and through the specification of minimum, maximum and delta temperatures as described below. The temperatures can be either single constant values for the entire simulation or schedules which can vary over time. As with infiltration, the actual flow rate of ventilation air can be modified by the temperature difference between the inside and outside environment and the wind speed. The basic equation used to calculate ventilation with this model is:
+
+\begin{equation}
+Ventilation = \left( {{V_{design}}} \right)\left( {{F_{schedule}}} \right)\left[ {A + B\left| {{T_{zone}} - {T_{odb}}} \right| + C\left( {WindSpeed} \right) + D\left( {WindSpee{d^2}} \right)} \right]
+\end{equation}
+
+Similar to infiltration, the question of typical values for these coefficients is subject to debate. Ideally, one should do a detailed analysis of the ventilation situation and then determine a custom set of coefficients using methods such as those laid out in Chapter 26 of the ASHRAE Handbook of Fundamentals. The EnergyPlus defaults are 1,0,0,0 which give a constant volume flow of ventilation under all conditions. The following discussion is duplicated from the infiltration design flow rate object. The equation must always yield a non-negative results; negative values are set to 0.0.
+
+BLAST (one of the EnergyPlus predecessors) used the following values as defaults:~ 0.606, 0.03636, 0.1177, 0. These coefficients produce a value of 1.0 at 0C deltaT and 3.35 m/s (7.5 mph) windspeed, which corresponds to a typical summer condition. At a winter condition of 40C deltaT and 6 m/s (13.4 mph) windspeed, these coefficients would increase the infiltration rate by a factor of 2.75.
+
+In DOE-2 (the other EnergyPlus predecessor), the air change method defaults are (adjusted to SI units) 0, 0, 0.224 (windspeed), 0. With these coefficients, the summer conditions above would give a factor of 0.75, and the winter conditions would give 1.34. A windspeed of 4.47 m/s (10 mph) gives a factor of 1.0.
+
+The source of the BLAST defaults is noted in the BLAST documentation as:
+
+``Empirical equation and the coefficient default were determined from ASHRAE journal articles and other data on the effects of outdoor weather conditions.''
+
+The source of the DOE-2 defaults is based on examining the \emph{infiltration} relationships described in the ASHRAE Handbook of Fundamentals.
+
+The local outdoor dry-bulb temperature used in the above basic equation (T\(_{odb}\)) is typically a function of the height of the zone centroid above ground. The corresponding zone name is given in the second field. The local outdoor dry-bulb temperature calculation procedure is described in the ``Local Outdoor Air Temperature Calculation'' section of the Engineering Reference.
+
+The local outdoor wind speed used in the above basic equation (WindSpeed) is also a function of the height of the zone centroid above ground. The corresponding zone name is given in the second field. The local outdoor wind speed calculation procedure is described in the ``Local Wind Speed Calculation'' section of the Engineering Reference.
+
+Note: When the value of the Wind Speed Profile Exponent field in the Site:HeightVariation object is equal to 0.0, the local wind speed is always equal to the wind speed given in the weather data and will not be dependent on zone centroid height.~ Similarly, if the value of the Air Temperature Gradient Coefficient is set equal to 0, the local air dry-bulb temperature is also always equal to the air dry-bulb temperature given in the weather data and will not be dependent on zone centroid height.
+
+One or more ventilation objects (i.e., ZoneVentilation:DesignFlowRate and/or ZoneVentilation:WindandStackOpenArea) can be defined for each zone, and the resulting ventilation rate for the zone will simply be the summation of the flow rates specified by the ventilation objects.
+
+More advanced ventilation calculations are possible using the EnergyPlus AirflowNetwork model.
+
+\subsubsection{Inputs}\label{inputs-2-005}
+
+\paragraph{Field: Name}\label{field-name-2-004}
+
+The name of the ZoneVentilation:DesignFlowRate object.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-1}
+
+This field is the name of the zone (ref: Zone) or ZoneList (ref: ZoneList) and attaches a particular ventilation statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this ventilation definition is applied to each of the zones in the zone list effecting a global definition for the amount of infiltration flow rate in the zone. The Zonelist option can be used effectively with the flow/area, flow/person, or airchanges/hour of the Design Flow Rate Calculation Method.
+
+The name of the actual ventilation object becomes \textless{}Zone Name\textgreater{} \textless{}ZoneVentilation:DesignFlowRate Object Name\textgreater{} and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-2}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design volume flow rate (V\(_{design}\)) (see Design Flow Rate Calculation Method field and related subsequent fields). This fraction between 0.0 and 1.0 is noted as F\(_{schedule}\) in the above equation.
+
+\paragraph{Field: Design Flow Rate Calculation Method}\label{field-design-flow-rate-calculation-method-1}
+
+This field is a key/choice field that tells which of the next four fields are filled and is descriptive of the method for calculating the design volume flow rate. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Zone
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the design volume flow rate.~ (The Design Flow Rate field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The Flow per Zone Floor Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Person
+\end{itemize}
+
+With this choice, the method used will be a factor per nominal number of people in the zone. (The Flow per Person field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  AirChanges/Hour
+\end{itemize}
+
+With this choice, the method used will be the number of air changes per hour for the infiltration amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. (The Air Changes per Hour field should be filled).
+
+\paragraph{Field: Design Flow Rate}\label{field-design-flow-rate-1}
+
+This field denotes the full design volume flow rate (m\(^{3}\)/s). The previous field should choose ``flow/zone'' as the choice. The design volume flow rate (noted as V\(_{design}\) in the above equation) is the maximum amount of ventilation expected at design conditions. The design value is modified by the schedule fraction (see Field: Schedule Name) and user specified coefficients (see four ``coefficient'' fields below).
+
+\paragraph{Field: Flow Rate per Zone Floor Area}\label{field-flow-rate-per-zone-floor-area}
+
+This factor (m\(^{3}\)/s-m\(^{2}\)) is used, along with the Zone Area to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be ``flow/area''.
+
+\paragraph{Field: Flow Rate per Person}\label{field-flow-rate-per-person}
+
+This factor (m\(^{3}\)/s-person) is used, along with the nominal (maximum) number of occupants (people) in the Zone to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be ``flow/person''.
+
+\paragraph{Field: Air Changes per Hour}\label{field-air-changes-per-hour-1}
+
+With this choice, the method used will be the number of air changes per hour for the ventilation amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. The choice from the method field should be ``AirChanges/Hour''.
+
+\paragraph{Field: Ventilation Type}\label{field-ventilation-type}
+
+This alpha character string defines the type of ventilation as one of the following options: Natural, Exhaust, Intake, or Balanced. Natural ventilation is assumed to be air movement/exchange as a result of openings in the building façade and will not consume any fan energy. Values for fan pressure and efficiency for natural ventilation are ignored. For either Exhaust or Intake, values for fan pressure and efficiency define the fan electric consumption. For Natural and Exhaust ventilation, the conditions of the air entering the space are assumed to be equivalent to outside air conditions. For Intake and Balanced ventilation, an appropriate amount of fan heat is added to the entering air stream. For Balanced ventilation, both an intake fan and an exhaust fan are assumed to co-exist, both having the same flow rate and power consumption (using the entered values for fan pressure rise and fan total efficiency). Thus, the fan electric consumption for Balanced ventilation is twice that for the Exhaust or Intake ventilation types which employ only a single fan.
+
+\paragraph{Field: Fan Pressure Rise}\label{field-fan-pressure-rise}
+
+This is the pressure rise experienced across the fan in Pascals (N/m\(^{2}\)). This is a function of the fan and plays a role in determining the amount of energy consumed by the fan.
+
+\paragraph{Field: Fan Total Efficiency}\label{field-fan-total-efficiency}
+
+This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1."
+
+\paragraph{Field: Constant Term Coefficient}\label{field-constant-term-coefficient-1}
+
+This number is the ``A'' parameter in the above ventilation equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter, however, is a constant under all conditions and is not modified by any environmental effect. As a result, it is dimensionless.
+
+\paragraph{Field: Temperature Term Coefficient}\label{field-temperature-term-coefficient-1}
+
+This number is the ``B'' parameter in the above ventilation equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the temperature difference between the outdoor and indoor air dry-bulb temperatures. The units for this parameter are inverse Celsius.
+
+\paragraph{Field: Velocity Term Coefficient}\label{field-velocity-term-coefficient-1}
+
+This number is the ``C'' parameter in the above ventilation equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the speed of wind being experienced outside the building. The units for this parameter are s/m.
+
+\paragraph{Field: Velocity Squared Term Coefficient}\label{field-velocity-squared-term-coefficient-1}
+
+This number is the ``D'' parameter in the above ventilation equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by square of the speed of wind being experienced outside the building. The units for this parameter are s\(^{2}\)/m\(^{2}\).
+
+\paragraph{Field: Minimum Indoor Temperature}\label{field-minimum-indoor-temperature}
+
+This is the indoor temperature (in Celsius) below which ventilation is shutoff. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is -100.0°C if the field is left blank. This lower temperature limit is intended to avoid overcooling a space and thus result in a heating load. For example, if the user specifies a minimum temperature of 20°C, ventilation is assumed to be available if the zone air temperature is above 20°C. If the zone air temperature drops below 20°C, then ventilation is automatically turned off.
+
+\paragraph{Field: Minimum Indoor Temperature Schedule Name}\label{field-minimum-indoor-temperature-schedule-name}
+
+This alpha field defines the name of a schedule (ref. Schedule objects) which contains the minimum indoor temperature (in Celsius) below which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Minimum Indoor Temperature field. If the user enters a valid schedule name, the minimum temperature values specified in this schedule will override the constant value specified in the Minimum Indoor Temperature field.
+
+\paragraph{Field: Maximum Indoor Temperature}\label{field-maximum-indoor-temperature}
+
+This is the indoor temperature (in Celsius) above which ventilation is shutoff. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is 100.0°C if the field is left blank. This upper temperature limit is intended to avoid overheating a space and thus result in a cooling load. For example, if the user specifies a maximum temperature of 28°C, ventilation is assumed to be available if the zone air temperature is below 28°C. If the zone air temperature increases to 28°C, then ventilation is automatically turned off.
+
+\paragraph{Field: Maximum Indoor Temperature Schedule Name}\label{field-maximum-indoor-temperature-schedule-name}
+
+This alpha field defines the name of a schedule (ref. Schedule objects) which contains the maximum indoor temperature (in Celsius) above which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Maximum Indoor Temperature field. If the user enters a valid schedule name, the maximum temperature values specified in this schedule will override the constant value specified in the Maximum Indoor Temperature field.
+
+\paragraph{Field: Delta Temperature}\label{field-delta-temperature}
+
+This is the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which ventilation is shutoff. The minimum value for this field is -100.0°C and thedefault value is also -100.0°C if the field is left blank. This field allows ventilation to be stopped if the temperature outside is too warm and could potentially heat the space. For example, if the user specifies a delta temperature of 2°C, ventilation is assumed to be available if the outside air temperature is at least 2°C cooler than the zone air temperature. If the outside air dry-bulb temperature is less than 2°C cooler than the indoor dry-bulb temperature, then ventilation is automatically turned off.
+
+The values for this field can include negative numbers. This allows ventilation to occur even if the outdoor temperature is above the indoor temperature. The Delta Temperature is used in the code in the following way:
+
+IF ((IndoorTemp - OutdoorTemp) \textless{} DeltaTemperature) Then ventilation is not allowed.
+
+Thus, if a large negative number is input for DeltaTemperature, the ventilation can be kept on even if the outdoor temperature is greater than the indoor temperature. This is useful for uncontrolled natural ventilation (open windows) or as a way to estimate the effect of required ventilation air for load calculations.
+
+\paragraph{Field: Delta Temperature Schedule Name}\label{field-delta-temperature-schedule-name}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which ventilation is shutoff as a function of time. The minimum temperature difference value in the schedule can be -100°C. This field is an optional field and has the same functionality as the Delta Temperature field. If the user enters a valid schedule name, the delta temperature values specified in this schedule will override the constant value specified in the Delta Temperature field.
+
+\paragraph{Field: Minimum Outdoor Temperature}\label{field-minimum-outdoor-temperature}
+
+This is the outdoor temperature (in Celsius) below which ventilation is shut off. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is~~~~~~~~~~ -100.0°C if the field is left blank. This lower temperature limit is intended to avoid overcooling a space, which could result in a heating load.
+
+\paragraph{Field: Minimum Outdoor Temperature Schedule Name}\label{field-minimum-outdoor-temperature-schedule-name}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) below which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Minimum Outdoor Temperature field. If the user enters a valid schedule name, the temperature values in this schedule will override the constant value specified in the Minimum Outdoor Temperature field.
+
+\paragraph{Field: Maximum Outdoor Temperature}\label{field-maximum-outdoor-temperature}
+
+This is the outdoor temperature (in Celsius) above which ventilation is shut off. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is 100.0°C if the field is left blank. This upper temperature limit is intended to avoid overheating a space, which could result in a cooling load.
+
+\paragraph{Field: Maximum Outdoor Temperature Schedule Name}\label{field-maximum-outdoor-temperature-schedule-name}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) above which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Maximum Outdoor Temperature field. If the user enters a valid schedule name, the temperature values in this schedule will override the constant value specified in the Maximum Outdoor Temperature field.
+
+\paragraph{Field: Maximum Wind Speed}\label{field-maximum-wind-speed}
+
+This is the wind speed (m/s) above which ventilation is shut off. This can help simulate conditions where one would normally close windows to avoid chaos in a space (papers blowing around, etc.).
+
+Two IDF examples are provided below:
+
+\begin{lstlisting}
+
+ZoneVentilation:DesignFlowRate,
+    Ventilation 1,  !- Name
+    ZONE 2,         !- Zone Name
+    Simple Vent,    !- Schedule Name
+    Flow/Zone,      !- Design Volume Flow Rate calculation method
+    6.131944,       !- Design Volume Flow Rate {m3/s}
+    ,               !- Volume Flow Rate per area {m3/s/m2}
+    ,               !- Volume Flow Rate per person {m3/s/person}
+    ,               !- Air Changes Per Hour
+    INTAKE,         !- Ventilation Type
+    400.0,          !- Fan Pressure Rise{Pa}
+    0.9,            !- Fan Total Efficiency
+    0.6060000    ,  !- Constant Term Coefficient
+    2.0199999E-02,  !- Temperature Term Coefficient
+    5.9800001E-04,  !- Velocity Term Coefficient
+    0.0000000E+00!- Velocity Squared Term Coefficient
+    18.0,           !- Minimum Indoor Temperature {C}
+    ,               !- Minimum Indoor Temperature Schedule Name
+    ,               !- Maximum Indoor Temperature {C}
+    ,               !- Maximum Indoor Temperature Schedule Name
+    1.0;            !- Delta temperature {C}
+
+  ZoneVentilation:DesignFlowRate,
+      SPACE1-1 Ventl 1,        !-Name
+      SPACE1-1,                !- Zone Name
+      NightVentSched,          !- SCHEDULE Name
+      Flow/Zone,               !- Design Volume Flow Rate calculation method
+      .05295,                  !- Design Volume Flow Rate {m3/s}
+      ,                        !- Volume Flow Rate per area {m3/s/m2}
+      ,                        !- Volume Flow Rate per person {m3/s/person}
+      ,                        !- Air Changes Per Hour
+      Intake,                  !- Ventilation Type
+      67.,                     !- Fan Pressure Rise
+      .7,                      !- Fan Total Efficiency
+      1,                       !- Constant Term Coefficient
+      0,                       !- Temperature Term Coefficient
+      0,                       !- Velocity Term Coefficient
+      0,                       !- Velocity Squared Term Coefficient
+      ,                        !- Minimum Indoor Temperature {C}
+      MinIndoorTemp,           !- Minimum Indoor Temperature Schedule Name
+      ,                        !- Maximum Indoor Temperature {C}
+      MaxIndoorTemp,           !- Maximum Indoor Temperature Schedule Name
+      ,                        !- Delta Temperature {deltaC}
+      DeltaTemp,               !- Delta Temperature Schedule Name
+     ,                        !- Minimum Outdoor Temperature {C}
+      MinOutdoorTemp,          !- Minimum Outdoor Temperature Schedule Name
+      ,                        !- Maximum Outdoor Temperature {C}
+      MaxOutdoorTemp,          !- Maximum Outdoor Temperature Schedule Name
+      40;                      !- Maximum WindSpeed {m/s}
+\end{lstlisting}
+
+Global Ventilation example:
+
+\begin{lstlisting}
+
+  Zonelist, West-East Zones, West Zone, East Zone;
+
+
+    ZoneVentilation:DesignFlowRate,
+      West-East Zones Ventilation,         !- Name
+      West-East Zones,         !- Zone or ZoneList Name
+      VentSched,               !- Schedule Name
+      AirChanges/Hour,         !- Design Flow Rate Calculation Method
+      ,                        !- Design Flow Rate {m3/s}
+      ,                        !- Flow Rate per Zone Floor Area {m3/s-m2}
+      ,                        !- Flow Rate per Person {m3/s-person}
+      1.7,                        !- Air Changes per Hour
+      Intake,                  !- Ventilation Type
+      67.,                     !- Fan Pressure Rise {Pa}
+      0.7,                     !- Fan Total Efficiency
+      1,                       !- Constant Term Coefficient
+      0,                       !- Temperature Term Coefficient
+      0,                       !- Velocity Term Coefficient
+      0,                       !- Velocity Squared Term Coefficient
+      ,                        !- Minimum Indoor Temperature {C}
+      MinIndoorTemp,           !- Minimum Indoor Temperature Schedule Name
+      ,                        !- Maximum Indoor Temperature {C}
+      MaxIndoorTemp,           !- Maximum Indoor Temperature Schedule Name
+      ,                        !- Delta Temperature {deltaC}
+      DeltaTemp,               !- Delta Temperature Schedule Name
+      ,                        !- Minimum Outdoor Temperature {C}
+      MinOutdoorTemp,          !- Minimum Outdoor Temperature Schedule Name
+      ,                        !- Maximum Outdoor Temperature {C}
+      MaxOutdoorTemp,          !- Maximum Outdoor Temperature Schedule Name
+      40;                      !- Maximum Wind Speed {m/s}
+\end{lstlisting}
+
+\subsection{ZoneVentilation:WindandStackOpenArea}\label{zoneventilationwindandstackopenarea}
+
+For this model, the ventilation air flow rate is a function of wind speed and thermal stack effect, along with the area of the opening being modeled. This object can be used alone or in combination with ZoneVentilation:DesignFlowRate objects. This model is intended for simplified ventilation calculations as opposed to the more detailed ventilation investigations that can be performed with the AirflowNetwork model. Using the ``Wind and Stack with Open Area'' model, the natural ventilation flow rate can be controlled by a multiplier fraction schedule applied to the user-defined opening area and through the specification of minimum, maximum and delta temperatures. The temperatures can be either single constant values for the entire simulation or schedules which can vary over time. The equation used to calculate the ventilation rate driven by wind is:
+
+\begin{equation}
+{Q_w} = {C_w}{A_{opening}}{F_{schedule}}V
+\end{equation}
+
+where,
+
+~~~~~ \emph{Q\(_{w}\)}~~~~~~~ = Volumetric air flow rate driven by wind {[}m\(^{3}\)/s{]}
+
+~~~~~ \emph{C\(_{w}\)}~~~~~~~ = Opening effectiveness {[}dimensionless{]}
+
+~~~~~ \emph{A\(_{opening}\)}~ = Opening area {[}m\(^{2}\){]}
+
+~~~~~ \emph{F\(_{schedule}\)} = Open area fraction {[}user-defined schedule value, dimensionless{]}
+
+~~~~~ \emph{V}~~~~~~~~~ = Local wind speed {[}m/s{]}
+
+The equation used to calculate the ventilation rate due to stack effect is:
+
+\begin{equation}
+{Q_s} = {C_D}{A_{opening}}{F_{schedule}}\sqrt {2g\Delta {H_{NPL}}(|{T_{zone}} - {T_{odb}}|/{T_{zone}})}
+\end{equation}
+
+where,
+
+~~~~~ \emph{Q\(_{s}\)}~~~~~~~ = Volumetric air flow rate due to stack effect {[}m\(^{3}\)/s{]}
+
+~~~~~ \emph{C\(_{D}\)}~~~~~~~ = Discharge coefficient for opening {[}dimensionless{]}
+
+~~~~~ \emph{A\(_{opening}\)}~ = Opening area {[}m\(^{2}\){]}
+
+~~~~~ \emph{F\(_{schedule}\)} = Open area fraction {[}user-defined schedule value, dimensionless{]}
+
+~~~~~ \emph{ΔH\(_{NPL}\)}~ = Height from midpoint of lower opening to the neutral pressure level {[}m{]}.
+
+Estimation of this value is difficult; refer to Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals for guidance.
+
+~~~~~ \emph{T\(_{zone}\)}~~~~~ = Zone air dry-bulb temperature {[}K{]}
+
+\emph{T\(_{odb}\)} = Local outdoor air dry-bulb temperature {[}K{]}
+
+The total ventilation rate calculated by this model is the quadrature sum of the wind and stack air flow components:
+
+\begin{equation}
+Ventilatio{n_{WindAndStack}} = \sqrt {{Q_s}^2 + {Q_w}^2}
+\end{equation}
+
+The local outdoor air dry-bulb temperature used in the stack effect equation (T\(_{odb}\)) is typically a function of the height of the zone centroid above ground. The corresponding zone name is given in the second field. The local outdoor air dry-bulb temperature calculation procedure is described in the ``Local Outdoor Air Temperature Calculation'' section of the Engineering Reference.
+
+The local outdoor wind speed used in the above wind-driven equation (V) is also a function of the height of the zone centroid above ground. The corresponding zone name is given in the second field. The local outdoor wind speed calculation procedure is described in the ``Local Wind Speed Calculation'' section of the Engineering Reference.
+
+Note: When the value of the Wind Speed Profile Exponent field in the Site:HeightVariation object is equal to 0.0, the local wind speed is always equal to the wind speed given in the weather data and will not be dependent on zone centroid height.~ Similarly, if the value of the Air Temperature Gradient Coefficient is set equal to 0, the local air dry-bulb temperature is also always equal to the air dry-bulb temperature given in the weather data and will not be dependent on zone centroid height.
+
+One or more ventilation objects (i.e., ZoneVentilation:DesignFlowRate and/or ZoneVentilation:WindandStackOpenArea) can be defined for each zone, and the resulting ventilation rate for the zone will simply be the summation of the flow rates specified by the ventilation objects.
+
+More advanced ventilation calculations are possible using the EnergyPlus AirflowNetwork model.
+
+\subsubsection{Inputs}\label{inputs-3-004}
+
+\paragraph{Field: Name}\label{field-name-3-004}
+
+The name of the ZoneVentilation:WindandStackOpenArea object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-001}
+
+This field is the name of the zone (ref: Zone) and attaches a particular ventilation statement to a thermal zone in the building.
+
+\paragraph{Field: Opening Area}\label{field-opening-area}
+
+This is the opening area exposed to outdoors (m\(^{2}\)) in a zone.
+
+\paragraph{Field: Opening Area Fraction Schedule Name}\label{field-opening-area-fraction-schedule-name}
+
+This field is the name of the schedule (ref: Schedule) which modifies the Opening Area value (see previous field). The schedule values must be any positive number between 0 and 1 as a fraction. The actual opening area in a zone for a particular simulation time step is defined as the product of the Opening Area input field and the value specified by the schedule named in this input field.
+
+\paragraph{Field: Opening Effectiveness}\label{field-opening-effectiveness}
+
+This field is the opening effectiveness (C\(_{w}\)). The value must be between 0.0 and 1.0 or the value can be autocalculated. If a real value is input, that constant value will be used in the calculations. Otherwise, this field can be left blank (default = Autocalculate) or the user can input \textbf{Autocalculate.} Based on recommended values provided in Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals, C\(_{w}\) = 0.55 for perpendicular winds and C\(_{w}\) = 0.3 for diagonal winds. For Autocalculate, any angles between perpendicular and diagonal are linearly interpolated between 0.3 and 0.55 by the model.
+
+\paragraph{Field: Effective Angle}\label{field-effective-angle}
+
+This is the angle in degrees counting from the North clockwise to the opening outward normal. The value must be between 0 and 360, with the default being 0 if this input field is left blank. The Effective Angle is 0 if the opening outward normal faces North, 90 if faces East, 180 if faces South, and 270 if faces West. The value is fixed and independent of coordinate system defined in the GlobalGeometryRules object. This input field value is used to calculate the angle between the wind direction and the opening outward normal to determine the opening effectiveness values when the input field Opening Effectiveness = Autocalculate.
+
+\paragraph{Field: Height Difference}\label{field-height-difference}
+
+This is the height difference between the midpoint of the lower opening and the neutral pressure level in meters. This value is a required user input.
+
+Note: Estimation of the height difference is difficult for natural ventilated buildings. Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals may provide guidance for estimating the height difference.
+
+\paragraph{Field: Discharge Coefficient for Opening}\label{field-discharge-coefficient-for-opening}
+
+This is the discharge coefficient for the opening (C\(_{D}\)). The value must be between 0.0 and 1.0, or the value can be autocalculated. If a real value is input, that constant value will be used in the calculations. Otherwise, this field can be left blank (default = Autocalculate) or the user can input \textbf{Autocalculate.} For Autocalculate, the program will determine the discharge coefficient based on the following equation:
+
+\begin{equation}
+{C_D} = 0.40 + 0.0045\left| {{T_{zone}} - {T_{odb}}} \right|
+\end{equation}
+
+\paragraph{Field: Minimum Indoor Temperature}\label{field-minimum-indoor-temperature-1}
+
+This is the indoor temperature (in Celsius) below which ventilation is shutoff. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is~~~~~~~~~~ -100.0°C if the field is left blank. This lower temperature limit is intended to avoid overcooling a space and thus result in a heating load. For example, if the user specifies a minimum temperature of 20°C, ventilation is assumed to be available if the zone air temperature is above 20°C. If the zone air temperature drops below 20°C, then ventilation is automatically turned off.
+
+\paragraph{Field: Minimum Indoor Temperature Schedule Name}\label{field-minimum-indoor-temperature-schedule-name-1}
+
+This alpha field defines the name of a schedule (ref. Schedule objects) which contains the minimum indoor temperature (in Celsius) below which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Minimum Indoor Temperature field. If the user enters a valid schedule name, the minimum temperature values specified in this schedule will override the constant value specified in the Minimum Indoor Temperature field.
+
+\paragraph{Field: Maximum Indoor Temperature}\label{field-maximum-indoor-temperature-1}
+
+This is the indoor temperature (in Celsius) above which ventilation is shutoff. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is 100.0°C if the field is left blank. This upper temperature limit is intended to avoid overheating a space and thus result in a cooling load. For example, if the user specifies a maximum temperature of 28°C, ventilation is assumed to be available if the zone air temperature is below 28°C. If the zone air temperature increases to 28°C, then ventilation is automatically turned off.
+
+\paragraph{Field: Maximum Indoor Temperature Schedule Name}\label{field-maximum-indoor-temperature-schedule-name-1}
+
+This alpha field defines the name of a schedule (ref. Schedule objects) which contains the maximum indoor temperature (in Celsius) above which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Maximum Indoor Temperature field. If the user enters a valid schedule name, the maximum temperature values specified in this schedule will override the constant value specified in the Maximum Indoor Temperature field.
+
+\paragraph{Field: Delta Temperature}\label{field-delta-temperature-1}
+
+This is the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which ventilation is shutoff. The minimum value for this field is -100.0°C and the default value is also -100.0°C if the field is left blank. This field allows ventilation to be stopped if the temperature outside is too warm and could potentially heat the space. For example, if the user specifies a delta temperature of 2°C, ventilation is assumed to be available if the outside air temperature is at least 2°C cooler than the zone air temperature. If the outside air dry-bulb temperature is less than 2°C cooler than the indoor dry-bulb temperature, then ventilation is automatically turned off.
+
+The values for this field can include negative numbers. This allows ventilation to occur even if the outdoor temperature is above the indoor temperature. The Delta Temperature is used in the code in the following way:
+
+IF ((IndoorTemp - OutdoorTemp) \textless{} DeltaTemperature) Then ventilation is not allowed.
+
+Thus, if a large negative number is input for DeltaTemperature, the ventilation can be kept on even if the outdoor temperature is greater than the indoor temperature. This is useful for uncontrolled natural ventilation (open windows) or as a way to estimate the effect of required ventilation air for load calculations.
+
+\paragraph{Field: Delta Temperature Schedule Name}\label{field-delta-temperature-schedule-name-1}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which ventilation is shutoff as a function of time. The minimum temperature difference value in the schedule can be -100°C. This field is an optional field and has the same functionality as the Delta Temperature field. If the user enters a valid schedule name, the delta temperature values specified in this schedule will override the constant value specified in the Delta Temperature field.
+
+\paragraph{Field: Minimum Outdoor Temperature}\label{field-minimum-outdoor-temperature-1}
+
+This is the outdoor temperature (in Celsius) below which ventilation is shut off. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is~~~~~~~~~~ -100.0°C if the field is left blank. This lower temperature limit is intended to avoid overcooling a space, which could result in a heating load.
+
+\paragraph{Field: Minimum Outdoor Temperature Schedule Name}\label{field-minimum-outdoor-temperature-schedule-name-1}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) below which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Minimum Outdoor Temperature field. If the user enters a valid schedule name, the temperature values in this schedule will override the constant value specified in the Minimum Outdoor Temperature field.
+
+\paragraph{Field: Maximum Outdoor Temperature}\label{field-maximum-outdoor-temperature-1}
+
+This is the outdoor temperature (in Celsius) above which ventilation is shut off. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is 100.0°C if the field is left blank. This upper temperature limit is intended to avoid overheating a space, which could result in a cooling load.
+
+\paragraph{Field: Maximum Outdoor Temperature Schedule Name}\label{field-maximum-outdoor-temperature-schedule-name-1}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) above which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Maximum Outdoor Temperature field. If the user enters a valid schedule name, the temperature values in this schedule will override the constant value specified in the Maximum Outdoor Temperature field.
+
+\paragraph{Field: Maximum Wind Speed}\label{field-maximum-wind-speed-1}
+
+This is the wind speed (m/s) above which ventilation is shut off. This can help simulate conditions where one would normally close windows to avoid chaos in a space (papers blowing around, etc.).
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+  ZoneVentilation:WindandStackOpenArea,
+      ZONE 3 Ventl 1,          !- Name
+      ZONE 3,                  !- Zone Name
+      0.5,                     !- Opening Area {m2}
+      Constant,                !- Opening Area Fraction Schedule Name
+      AutoCalculate,           !- Opening Effectiveness
+      0.0,                     !- Effective Angle {deg}
+      1.0,                     !- Height Difference {m}
+      AutoCalculate,           !- Discharge Coefficient for Opening
+      18.0,                    !- Minimum Indoor Temperature {C}
+      ,                        !- Minimum Indoor Temperature Schedule Name
+      ,                        !- Maximum Indoor Temperature {C}
+      ,                        !- Maximum Indoor Temperature Schedule Name
+      1.0;                     !- Delta Temperature {deltaC}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-002}
+
+Current ventilation output variables:
+
+\begin{itemize}
+\item
+  HVAC,Sum,Zone Ventilation Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ventilation Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ventilation Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ventilation Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ventilation Total Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ventilation Total Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilation Current Density Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Zone Ventilation Standard Density Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Ventilation Current Density Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Ventilation Standard Density Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Ventilation Mass {[}kg{]}
+\item
+  HVAC,Sum,Zone Ventilation Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Ventilation Air Change Rate {[}ach{]}
+\item
+  HVAC,Sum,Zone Ventilation Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilation Air Inlet Temperature {[}C{]}
+\end{itemize}
+
+Note: If ZoneVentilation:* objects and ZoneAirBalance:OutdoorAir (with Air Balance Method = Quadrature) objects reference the same Zone Name, the above ventilation output variables will not be reported for that zone. Instead, output variables for zone outdoor air flow will be reported by the corresponding ZoneAirBalance:OutdoorAir object.
+
+\paragraph{Zone Ventilation Sensible Heat Loss Energy {[}J{]}}\label{zone-ventilation-sensible-heat-loss-energy-j}
+
+The sensible (temperature) heat loss that occurs when the ventilation inlet air temperature \textless{} zone air temperature. If multiple ventilation objects are specified for a particular zone, the ventilation inlet air temperature is from all ZoneVentilation:DesignFlowRate and ZoneVentilation:WindandStackOpenArea objects specified for the zone.
+
+\paragraph{Zone Ventilation Sensible Heat Gain Energy {[}J{]}}\label{zone-ventilation-sensible-heat-gain-energy-j}
+
+The sensible (temperature) heat gain that occurs when the ventilation inlet air temperature \textgreater{} = zone air temperature. If multiple ventilation objects are specified for a particular zone, the ventilation inlet air temperature is from all ZoneVentilation:DesignFlowRate and ZoneVentilation:WindandStackOpenArea objects specified for the zone.
+
+\paragraph{Zone Ventilation Latent Heat Loss Energy {[}J{]}}\label{zone-ventilation-latent-heat-loss-energy-j}
+
+The latent heat loss that occurs when the Ventilation air humidity ratio (outdoor) \textless{} zone air humidity ratio from all ZoneVentilation:DesignFlowRate and ZoneVentilation:WindandStackOpenArea objects specified for the zone.
+
+\paragraph{Zone Ventilation Latent Heat Gain Energy {[}J{]}}\label{zone-ventilation-latent-heat-gain-energy-j}
+
+The latent heat gain that occurs when the Ventilation air humidity ratio (outdoor) \textgreater{} = zone air humidity ratio from all ZoneVentilation:DesignFlowRate and ZoneVentilation:WindandStackOpenArea objects specified for the zone.
+
+\paragraph{Zone Ventilation Total Heat Loss Energy {[}J{]}}\label{zone-ventilation-total-heat-loss-energy-j}
+
+The total heat loss that occurs when the sum of Zone Ventilation Sensible Heat Gain Energy and Zone Ventilation Latent Heat Gain Energy \textless{} the sum of Zone Ventilation Sensible Heat Loss Energy and Zone Ventilation Latent Heat Loss Energy.
+
+\paragraph{Zone Ventilation Total Heat Gain Energy {[}J{]}}\label{zone-ventilation-total-heat-gain-energy-j}
+
+The total heat gain that occurs when the sum of Zone Ventilation Sensible Heat Gain Energy and Zone Ventilation Latent Heat Gain Energy \textgreater{} = the sum of Zone Ventilation Sensible Heat Loss Energy and Zone Ventilation Latent Heat Loss Energy.
+
+\paragraph{Zone Ventilation Current Density Volume {[}m3{]}}\label{zone-ventilation-current-density-volume-m3}
+
+\paragraph{Zone Ventilation Current Density Volume Flow Rate {[}m3/s{]}}\label{zone-ventilation-current-density-volume-flow-rate-m3s}
+
+These outputs are the total volume and volume flow rate of ventilation air based on the current density of zone air.
+
+\paragraph{Zone Ventilation Standard Density Volume {[}m3{]}}\label{zone-ventilation-standard-density-volume-m3}
+
+\paragraph{Zone Ventilation Standard Density Volume Flow Rate {[}m3/s{]}}\label{zone-ventilation-standard-density-volume-flow-rate-m3s}
+
+These outputs are the total volume and volume flow rate of ventilation air based on the standard density of air.~ Standard density in EnergyPlus corresponds to 20ºC drybulb, dry air, and nominally adjusted for elevation.
+
+\paragraph{Zone Ventilation Mass {[}kg{]}}\label{zone-ventilation-mass-kg}
+
+This output is the total mass flow into a particular zone from outdoors.
+
+\paragraph{Zone Ventilation Mass Flow Rate {[}kg/s{]}}\label{zone-ventilation-mass-flow-rate-kgs}
+
+This output is the total mass flow rate into a particular zone from outdoors.
+
+\paragraph{Zone Ventilation Air Change Rate {[}ach{]}}\label{zone-ventilation-air-change-rate-ach}
+
+The volume flow rate of the ventilation air in air changes per hour.
+
+\paragraph{Zone Ventilation Fan Electric Energy {[}J{]}}\label{zone-ventilation-fan-electric-energy-j}
+
+The fan electrical consumption for Intake or Exhaust ventilation types (for ZoneVentilation:DesignFlowRate objects only).
+
+\paragraph{Zone Ventilation Air Inlet Temperature {[}C{]}}\label{zone-ventilation-air-inlet-temperature-c}
+
+This is equal to the outdoor air temperature except when INTAKE fan power is included (for ZoneVentilation:DesignFlowRate objects only). When intake fan power is used, then the additional heat due to the fan is added to the outdoor temperature and this will be reported as the inlet air temperature. If multiple ventilation objects are specified for a particular zone, the reported value is the mass flow weighted temperature for the multiple ventilation objects specified for this zone.
+
+\subsection{ZoneAirBalance:OutdoorAir}\label{zoneairbalanceoutdoorair}
+
+This model calculates a combined zone outdoor airflow by including interactions between mechanical ventilation, infiltration and duct leakage. It is mainly applied to a single zone (e.g., residential) building. The model combines all outdoor airflows from ZoneInfiltration and ZoneVentilation objects in the same zone. This object also includes the induced outdoor airflows due to unbalanced duct leakage, and unbalanced outdoor airflows introduced by unbalanced airflows from ZoneHVAC:EnergyRecoveryVentilator objects when the exhaust airflow is greater than the supply outdoor airflow. This model is intended for simplified outdoor airflow calculations as opposed to the more detailed outdoor airflow investigations that can be performed with the AirflowNetwork model. The equation used to calculate the combined zone outdoor airflow is:
+
+\begin{equation}
+Q = \sqrt {{Q_n}^2 + {Q_{u,v}}^2 + {Q_{u,l}}^2}  + {Q_{b,v}}
+\end{equation}
+
+where,
+
+\emph{Q}~~~ = Combined outdoor airflow with infiltration, balanced and unbalanced outdoor air flows, and unbalanced duct leakage {[}m\(^{3}\)/s{]}
+
+\emph{Q\(_{n}\)}~~ = Natural infiltration airflow from ZoneInfiltration:* objects {[}m\(^{3}\)/s{]}
+
+\emph{Q\(_{b,v}\)} = Balanced ventilation airflow, excluding infiltration {[}m\(^{3}\)/s{]}
+
+\emph{Q\(_{u,v}\)} = Unbalanced ventilation airflow, excluding infiltration {[}m\(^{3}\)/s{]}
+
+\emph{Q\(_{u,l}\)}~ = Unbalanced duct leakage: the difference between supply and return leaks {[}m\(^{3}\)/s{]}
+
+This object cannot be used simultaneously with the EnergyPlus AirflowNetwork model.~ If the AirflowNetwork model is active for a simulation time step, the Air Balance Method is reset to ``None'' for that time step. More advanced outdoor airflow calculations are possible using the EnergyPlus AirflowNetwork model.
+
+This object does not combine any airflows from Fan:ZoneExhaust objects and is independent of HVAC equipment operation.
+
+This object will not work with the AvailabilityManager:HybridVentilation object in the same zone, when the Simple Airflow Control Type Schedule Name is provided in the HybridVentilation object. For this case, the Air Balance Method is reset to ``None''.
+
+\subsubsection{Inputs}\label{inputs-4-004}
+
+\paragraph{Field: Name}\label{field-name-4-004}
+
+The name of the ZoneOutdoorAir:Combined object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-2}
+
+This field is the name of the zone (ref: Zone) and attaches a combined outdoor airflow statement to a thermal zone in the building.
+
+\paragraph{Field: Air Balance Method}\label{field-air-balance-method}
+
+This choice field determines the air balance method. Two choices are Quadrature and None. If Quadrature, the combined zone outdoor air flow is calculated based on the above equation. If None, no combining of outdoor air will be performed (i.e., any ZoneInfiltration:* and ZoneVentilation:* objects specified for this zone are simulated individually).
+
+\paragraph{Field: Induced Outdoor Air Due to Unbalanced Duct Leakage}\label{field-induced-outdoor-air-due-to-unbalanced-duct-leakage}
+
+This is the induced outdoor airflow rate, in m\(^{3}\)/s, due to unbalanced duct leakage. If left blank, the default value is 0.
+
+\paragraph{Field: Induced Outdoor Air Schedule Name}\label{field-induced-outdoor-air-schedule-name}
+
+This field is the name of the schedule (ref: Schedule) which modifies the induced outdoor airflow rate value (see previous field). The schedule values must be any positive number between 0 and 1 as a fraction. The actual induced outdoor airflow rate in a zone for a particular simulation time step is defined as the product of the Induced Outdoor Air Due to Unbalanced Duct Leakage input field and the value specified by the schedule named in this input field.
+
+Note: Since this object is independent of HVAC operation, the inputs for the last two fields should be carefully selected to match HVAC system operation schedules.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+ZoneAirBalance:OutdoorAir,
+      ZONE 2 Balance 1,        !- Name
+      ZONE 2,                  !- Zone Name
+      Quadrature,              !- Air Balance Method
+      0.00,                    !- Induced Outdoor Air Due to Unbalanced Duct Leakage {m3/s}
+      Constant;                !- Induced Outdoor Air Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-002}
+
+ZoneAirBalance:OutdoorAir output variables will be provided when the Air Balance Method is Quadrature. Output variables from the associated ZoneVentilation:* and ZoneInfiltration:* objects for the same zone will not be produced when ZoneAirBalance:OutdoorAir output variables are available. If the Air Balance Method = None, then no ZoneAirBalance:OutputAir outputs will be produced and the associated ZoneVentilation:* and ZoneInfiltration:* objects will specify their output variables for the zone.
+
+\begin{itemize}
+\item
+  HVAC,Sum,Zone Combined Outdoor Air Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Combined Outdoor Air Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Combined Outdoor Air Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Combined Outdoor Air Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Combined Outdoor Air Total Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Combined Outdoor Air Total Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,Zone Combined Outdoor Air Current Density Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Zone Combined Outdoor Air Standard Density Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Combined Outdoor Air Current Density Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Combined Outdoor Air Standard Density Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Combined Outdoor Air Mass {[}kg{]}
+\item
+  HVAC,Sum,Zone Combined Outdoor Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average, Zone Combined Outdoor Air Changes per Hour {[}ach{]}
+\item
+  HVAC,Sum, Zone Combined Outdoor Air Fan Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Zone Combined Outdoor Air Sensible Heat Loss Energy {[}J{]}}\label{zone-combined-outdoor-air-sensible-heat-loss-energy-j}
+
+The sensible (temperature) heat loss that occurs when the outdoor air temperature \textless{} zone air temperature.
+
+\paragraph{Zone Combined Outdoor Air Sensible Heat Gain Energy {[}J{]}}\label{zone-combined-outdoor-air-sensible-heat-gain-energy-j}
+
+The sensible (temperature) heat gain that occurs when the outdoor air temperature \textgreater{} = zone air temperature.
+
+\paragraph{Zone Combined Outdoor Air Latent Heat Loss Energy {[}J{]}}\label{zone-combined-outdoor-air-latent-heat-loss-energy-j}
+
+The latent heat loss that occurs when the outdoor air humidity ratio \textless{} zone air humidity ratio.
+
+\paragraph{Zone Combined Outdoor Air Latent Heat Gain Energy {[}J{]}}\label{zone-combined-outdoor-air-latent-heat-gain-energy-j}
+
+The latent heat gain that occurs when the outdoor air humidity ratio \textgreater{} = zone air humidity ratio.
+
+\paragraph{Zone Combined Outdoor Air Total Heat Loss Energy {[}J{]}}\label{zone-combined-outdoor-air-total-heat-loss-energy-j}
+
+The total heat loss that occurs when the sum of Zone Combined Outdoor Air Sensible Heat Gain Energy and Zone Combined Outdoor Air Latent Heat Gain Energy \textless{} the sum of Zone Combined Outdoor Air Sensible Heat Loss Energy and Zone Combined Outdoor Air Latent Heat Loss Energy.
+
+\paragraph{Zone Combined Outdoor Air Total Heat Gain Energy {[}J{]}}\label{zone-combined-outdoor-air-total-heat-gain-energy-j}
+
+The total heat gain that occurs when the sum of Zone Combined Outdoor Air Sensible Heat Gain Energy and Zone Combined Outdoor Air Latent Heat Gain Energy \textgreater{} = the sum of Zone Combined Outdoor Air Sensible Heat Loss Energy and Zone Combined Outdoor Air Latent Heat Loss Energy.
+
+\paragraph{Zone Combined Outdoor Air Current Density Volume {[}m3{]}}\label{zone-combined-outdoor-air-current-density-volume-m3}
+
+\paragraph{Zone Combined Outdoor Air Current Density Volume Flow Rate {[}m3/s{]}}\label{zone-combined-outdoor-air-current-density-volume-flow-rate-m3s}
+
+These outputs are the total volume and volume flow rate of outdoor air based on the current density of zone air.
+
+\paragraph{Zone Combined Outdoor Air Standard Density Volume {[}m3{]}}\label{zone-combined-outdoor-air-standard-density-volume-m3}
+
+\paragraph{Zone Combined Outdoor Air Standard Density Volume Flow Rate {[}m3/s{]}}\label{zone-combined-outdoor-air-standard-density-volume-flow-rate-m3s}
+
+These outputs are the total volume and volume flow rate of outdoor air based on the standard density of air.~ Standard density in EnergyPlus corresponds to 20ºC drybulb, dry air, and nominally adjusted for elevation.
+
+\paragraph{Zone Combined Outdoor Air Mass {[}kg{]}}\label{zone-combined-outdoor-air-mass-kg}
+
+This output is the total mass flow into a particular zone from outdoors.
+
+\paragraph{Zone Combined Outdoor Air Mass Flow Rate {[}kg/s{]}}\label{zone-combined-outdoor-air-mass-flow-rate-kgs}
+
+This output is the total mass flow rate into a particular zone from outdoors.
+
+\paragraph{Zone Combined Outdoor Air Changes per Hour {[}ach{]}}\label{zone-combined-outdoor-air-changes-per-hour-ach}
+
+The volume flow rate of the ventilation air in air changes per hour.
+
+\paragraph{Zone Combined Outdoor Air Fan Electric Energy {[}J{]}}\label{zone-combined-outdoor-air-fan-electric-energy-j}
+
+The fan electrical consumption for Intake, Exhaust, or Balanced ventilation types (for
+
+ZoneVentilation:DesignFlowRate objects used to calculate a combined zone outdoor airflow).
+
+\subsection{ZoneMixing}\label{zonemixing}
+
+In EnergyPlus, the ZoneMixing syntax is intended to allow simplified treatment of air exchange between zones. Note that this statement only affects the energy balance of the ``receiving'' zone and that this statement will not produce any effect on the ``source'' zone. Mixing statements can be complementary and include multiple zones, but the balancing of flows between zones is left to the user's discretion. The use of the Cross Mixing syntax (ref: Cross Mixing) can allow for automatic balancing of flows and energy flow rates between zones but is hindered by the limitation of only a single cross mixing statement per zone. The use of Refrigeration Door Mixing syntax (ref: Refrigeration Door Mixing) automatically balances the flow and energy between two zones and allows multiple mixing statements per zone. More advanced mixing calculations are possible using the EnergyPlus AirflowNetwork model for multi-zone airflow with or without HVAC system operation. Mixing is entered using the following syntax.
+
+\subsubsection{Inputs}\label{inputs-5-004}
+
+\paragraph{Field: Name}\label{field-name-5-004}
+
+The name of the ZoneMixing object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-3}
+
+This field is the name of the zone (ref: Zone) receiving the amount of air being exchanged and attaches a particular mixing statement to a thermal zone in the building.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-3}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design volume flow rate parameter (see next field). This fraction between 0.0 and 1.0 modifies the design level parameter.
+
+\paragraph{Field: Design Flow Rate Calculation Method}\label{field-design-flow-rate-calculation-method-2}
+
+This field is a key/choice field that tells which of the next four fields are filled and is descriptive of the method for calculating the design volume flow rate. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Zone
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the design volume flow rate.~ (The Design Flow Rate field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The Flow per Zone Floor Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Person
+\end{itemize}
+
+With this choice, the method used will be a factor per nominal number of people in the zone. (The Flow per Person field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  AirChanges/Hour
+\end{itemize}
+
+With this choice, the method used will be the number of air changes per hour for the infiltration amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. (The Air Changes per Hour field should be filled).
+
+\paragraph{Field: Design Flow Rate}\label{field-design-flow-rate-2}
+
+This field denotes the full design volume flow rate (m\(^{3}\)/s). The previous field should choose ``flow/zone'' as the choice. The design volume flow rate is the maximum amount of mixing air expected. The design value is modified by the schedule fraction (see Field: Schedule Name) and user specified coefficients (see four ``coefficient'' fields below).
+
+\paragraph{Field: Flow Rate per Zone Floor Area}\label{field-flow-rate-per-zone-floor-area-1}
+
+This factor (m\(^{3}\)/s-m\(^{2}\)) is used, along with the Zone Area to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be ``Flow/Area''.
+
+\paragraph{Field: Flow Rate per Person}\label{field-flow-rate-per-person-1}
+
+This factor (m\(^{3}\)/s-person) is used, along with the nominal (maximum) number of occupants (people) in the Zone to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be ``Flow/Person''.
+
+\paragraph{Field: Air Changes per Hour}\label{field-air-changes-per-hour-2}
+
+With this choice, the method used will be the number of air changes per hour for the mixing amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. The choice from the method field should be ``AirChanges/Hour''.
+
+\paragraph{Field: Source Zone Name}\label{field-source-zone-name}
+
+This field is the name of the ``source'' zone (ref: Zone) that exhausts the amount of air specified by the design level and schedule fields to the zone named in the zone name field.
+
+\paragraph{Field: Delta Temperature}\label{field-delta-temperature-2}
+
+This number controls when mixing air from the source zone is sent to the receiving zone. This parameter is a temperature and is expressed in units of Celsius. If this field is positive, the temperature of the zone from which the air is being drawn (source zone) must be ``Delta Temperature'' warmer than the receiving zone air or else no mixing occurs. If this field is negative, the temperature of the source zone must be ``Delta Temperature'' cooler than the receiving zone air or else no mixing occurs. If this parameter is zero, mixing occurs regardless of the relative zone temperatures.
+
+\paragraph{Field: Delta Temperature Schedule Name}\label{field-delta-temperature-schedule-name-2}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the temperature difference (in Celsius) between the source zone and receiving zone air dry-bulb temperatures as a function of time. This field is an optional field and has the same functionality as the Delta Temperature field. If the user enters a valid schedule name, the delta temperature values specified in this schedule will supersede the constant value specified in the Delta Temperature field.
+
+\paragraph{Field: Minimum Zone Temperature Schedule Name}\label{field-minimum-zone-temperature-schedule-name}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum receiving zone temperature (in Celsius) below which mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum zone temperature control is not applied.
+
+\paragraph{Field: Maximum Zone Temperature Schedule Name}\label{field-maximum-zone-temperature-schedule-name}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum receiving zone temperature (in Celsius) above which mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum zone temperature control is not applied.
+
+\textbf{Note:} The maximum zone temperature when mixing is shutoff must be greater than or equal to the minimum zone temperature when mixing is shutoff at any given time. Otherwise, warnings will be issued and the maximum zone shutoff temperature will be set to the minimum zone shutoff temperature.
+
+\paragraph{Field: Minimum Source Zone Temperature Schedule Name}\label{field-minimum-source-zone-temperature-schedule-name}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum source zone temperature (in Celsius) below which mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum source zone temperature control is not applied.
+
+\paragraph{Field: Maximum Source Zone Temperature Schedule Name}\label{field-maximum-source-zone-temperature-schedule-name}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum source zone temperature (in Celsius) above which mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum source zone temperature control is not applied.
+
+\textbf{Note:} The maximum source zone temperature when mixing is shutoff must be greater than or equal to the minimum source zone temperature when mixing is shutoff at any given time. Otherwise, warnings will be issued and the maximum source zone shutoff temperature will be set to the minimum source zone shutoff temperature.
+
+\paragraph{Field: Minimum Outdoor Temperature Schedule Name}\label{field-minimum-outdoor-temperature-schedule-name-2}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) below which mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum outdoor temperature control is not applied.
+
+\paragraph{Field: Maximum Outdoor Temperature Schedule Name}\label{field-maximum-outdoor-temperature-schedule-name-2}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum outdoor temperature (in Celsius) above which mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum outdoor temperature control is not applied.
+
+\textbf{Note:} The maximum outdoor temperature when mixing is shutoff must be greater than or equal to the minimum outdoor temperature which mixing is shutoff at any given time. Otherwise, a warning will be issued and the maximum outdoor shutoff temperature will be set to the minimum outdoor shutoff temperature.
+
+An IDF Example:
+
+\begin{lstlisting}
+
+ZoneMixing,
+    Kitchen_ZN_1_FLR_1 Exhaust Fanmixing_0,  !- Name
+    Kitchen_ZN_1_FLR_1,  !- Zone Name
+    Hours_of_operation,  !- Schedule Name
+    Flow/Zone,  !- Design Flow Rate Calculation Method
+    1.4540,  !- Design Level
+    ,  !- Volume Flow Rate per Area {m3/s/m2}
+    ,  !- Volume Flow Rate Per Person {m3/s/person}
+    ,  !- Air Changes per Hour {ACH}
+    CAFETERIA_ZN_1_FLR_1,  !- Source Zone Name
+    0.0;  !- Delta Temperature
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-000}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Zone Mixing Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Mixing Current Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Mixing Standard Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Mixing Mass {[}kg{]}
+\item
+  HVAC,Sum,Zone Mixing Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum,Zone Mixing Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Total Heat Loss {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Total Heat Gain Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Zone Mixing Volume {[}m3{]}}\label{zone-mixing-volume-m3}
+
+The air volume in m\(^{3}\) entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
+
+\paragraph{Zone Mixing Current Density Volumetric Flow Rate {[}m3/s{]}}\label{zone-mixing-current-density-volumetric-flow-rate-m3s}
+
+The air volumetric flow rate in m\(^{3}\)/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at current zone air conditions.
+
+\paragraph{Zone Mixing Standard Density Volumetric Flow Rate {[}m3/s{]}}\label{zone-mixing-standard-density-volumetric-flow-rate-m3s}
+
+The air volumetric flow rate in m\(^{3}\)/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at standard conditions.
+
+\paragraph{Zone Mixing Mass {[}kg{]}}\label{zone-mixing-mass-kg}
+
+The air mass in kg entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep. The air mass is calculated using the air volume flow from each ``source'' zone and the density of air calculated for the average conditions (temperature and humidity) between the ``source'' and ``receiving'' zones.
+
+\paragraph{Zone Mixing Mass Flow Rate {[}kg/s{]}}\label{zone-mixing-mass-flow-rate-kgs}
+
+The air mass flow rate in kg/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
+
+\paragraph{Zone Mixing Sensible Heat Loss Energy {[}J{]}}\label{zone-mixing-sensible-heat-loss-energy-j}
+
+\paragraph{Zone Mixing Sensible Heat Gain Energy {[}J{]}}\label{zone-mixing-sensible-heat-gain-energy-j}
+
+The sensible (temperature) heat transfer due to the sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the specific heat (calculated for the average conditions (temperature and humidity) between the ``source'' and ``receiving'' zones) and the temperature differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing sensible heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing sensible heat gain.
+
+\paragraph{Zone Mixing Latent Heat Loss Energy {[}J{]}}\label{zone-mixing-latent-heat-loss-energy-j}
+
+\paragraph{Zone Mixing Latent Heat Gain Energy {[}J{]}}\label{zone-mixing-latent-heat-gain-energy-j}
+
+The latent heat transfer due to the sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the heat of vaporization (calculated for the average conditions (temperature and humidity) between the ``source'' and ``receiving'' zones) and the humidity ratio differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing latent heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing latent heat gain.
+
+\paragraph{Zone Mixing Total Heat Loss Energy {[}J{]}}\label{zone-mixing-total-heat-loss-energy-j}
+
+The total heat loss due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy \textless{} the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
+
+\paragraph{Zone Mixing Total Heat Gain Energy {[}J{]}}\label{zone-mixing-total-heat-gain-energy-j}
+
+The total heat gain due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy \textgreater{} = the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
+
+\subsection{ZoneCrossMixing}\label{zonecrossmixing}
+
+The ZoneCrossMixing syntax is ideally suited for two zones that exchange an equal amount of air between each other and do not have any air exchange with other zones. As with Mixing (ref: Mixing), this is a simplified view of interzone airflow in EnergyPlus. The main difference between Mixing and Cross Mixing is that Cross Mixing has an energy effect on both the source and the receiving zone, thus maintaining both the air mass and energy balances in the two zones.
+
+Cross Mixing can be entered once, in one of the mixing zones; or twice, once for each zone. The object should be entered once if Delta Temperature \textgreater{} 0.0 and it is desirable to have mixing only when the source zone~ is warmer than the receiving zone. This might be the case when the warmer zone is below the colder zone and the mixing is buoyancy driven. If the zones are next to each other, separated by an open doorway, it would be more suitable to input a cross mixing object for each zone. Then mixing would occur if the zone temperatures differed by Delta Temperature or greater regardless of which is the warmer zone.
+
+If Delta Temperature = 0.0, Cross Mixing can be entered either once or twice: the effect is exactly the same.
+
+Cross Mixing is entered using the following syntax.
+
+\subsubsection{Inputs}\label{inputs-6-003}
+
+\paragraph{Field: Name}\label{field-name-6-003}
+
+The name of the ZoneCrossMixing object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-4}
+
+This field is the name of the zone (ref: Zone) receiving the amount of air being exchanged and attaches a particular cross mixing statement to a thermal zone in the building.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-4}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design volume flow rate parameter (see next field). This fraction between 0.0 and 1.0 modifies the design level parameter.
+
+\paragraph{Field: Design Flow Rate Calculation Method}\label{field-design-flow-rate-calculation-method-3}
+
+This field is a key/choice field that tells which of the next four fields are filled and is descriptive of the method for calculating the design volume flow rate. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Zone
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the design volume flow rate.~ (The Design Flow Rate field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The Flow per Zone Floor Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Flow/Person
+\end{itemize}
+
+With this choice, the method used will be a factor per nominal number of people in the zone. (The flow per person field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  AirChanges/Hour
+\end{itemize}
+
+With this choice, the method used will be the number of air changes per hour for the infiltration amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. (The Air Changes per Hour field should be filled).
+
+\paragraph{Field: Design Flow Rate}\label{field-design-flow-rate-3}
+
+This field denotes the full design volume flow rate (m\(^{3}\)/s). The previous field should choose ``flow/zone'' as the choice. The design volume flow rate is the maximum amount of mixing air expected. The design value is modified by the schedule fraction (see Field: Schedule Name) and user specified coefficients (see four ``coefficient'' fields below).
+
+\paragraph{Field: Flow Rate per Zone Floor Area}\label{field-flow-rate-per-zone-floor-area-2}
+
+This factor (m\(^{3}\)/s-m\(^{2}\)) is used, along with the Zone Area to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be ``Flow/Area''.
+
+\paragraph{Field: Flow Rate per Person}\label{field-flow-rate-per-person-2}
+
+This factor (m\(^{3}\)/s-person) is used, along with the nominal (maximum) number of occupants (people) in the Zone to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be ``Flow/Person''.
+
+\paragraph{Field: Air Changes per Hour}\label{field-air-changes-per-hour-3}
+
+With this choice, the method used will be the number of air changes per hour for the mixing amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. The choice from the method field should be ``AirChanges/Hour''.
+
+\paragraph{Field: Source Zone Name}\label{field-source-zone-name-1}
+
+This field is the name of the ``source'' zone (ref: Zone) that exhausts the amount of air specified by the design level and schedule fields to the zone named in the zone name field. In reality, the ``source'' and ``receiving'' zones are interchangeable since the cross-mixed air affects both zones.
+
+\paragraph{Field: Delta Temperature}\label{field-delta-temperature-3}
+
+This number controls when mixing air from the source zone is sent to the receiving zone. This parameter is a temperature and is expressed in units of Celsius. If this field is positive, the temperature of the zone from which air is being drawn (``source zone'') must be ``Delta Temperature'' warmer than the zone air or no mixing occurs. If this field is zero, mixing occurs regardless of the relative air temperatures. Negative values for ``Delta Temperature'' are not permitted.
+
+\paragraph{Field: Delta Temperature Schedule Name}\label{field-delta-temperature-schedule-name-3}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the temperature difference (in Celsius) between the source zone and receiving zone air dry-bulb temperatures as a function of time. This field is an optional field and has the same functionality as the Delta Temperature field. If the user enters a valid schedule name, the delta temperature values specified in this schedule will supersede the constant value specified in the Delta Temperature field.
+
+\paragraph{Field: Minimum Zone Temperature Schedule Name}\label{field-minimum-zone-temperature-schedule-name-1}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum receiving zone temperature (in Celsius) below which cross mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum zone temperature control is not applied.
+
+\paragraph{Field: Maximum Zone Temperature Schedule Name}\label{field-maximum-zone-temperature-schedule-name-1}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum receiving zone temperature (in Celsius) above which cross mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum zone temperature control is not applied.
+
+\textbf{Note:} The maximum zone temperature when cross mixing is shutoff must be greater than or equal to the minimum zone temperature when cross mixing is shutoff at any given time. Otherwise, warnings will be issued and the maximum zone shutoff temperature will be set to the minimum zone shutoff temperature.
+
+\paragraph{Field: Minimum Source Zone Temperature Schedule Name}\label{field-minimum-source-zone-temperature-schedule-name-1}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum source zone temperature (in Celsius) below which cross mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum source zone temperature control is not applied.
+
+\paragraph{Field: Maximum Source Zone Temperature Schedule Name}\label{field-maximum-source-zone-temperature-schedule-name-1}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum source zone temperature (in Celsius) above which cross mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum source zone temperature control is not applied.
+
+\textbf{Note:} The maximum source zone temperature when cross mixing is shutoff must be greater than or equal to the minimum source zone temperature when cross mixing is shutoff at any given time. Otherwise, warnings will be issued and the maximum source zone shutoff temperature will be set to the minimum source zone shutoff temperature.
+
+\paragraph{Field: Minimum Outdoor Temperature Schedule Name}\label{field-minimum-outdoor-temperature-schedule-name-3}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) below which cross mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum outdoor temperature control is not applied.
+
+\paragraph{Field: Maximum Outdoor Temperature Schedule Name}\label{field-maximum-outdoor-temperature-schedule-name-3}
+
+This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum outdoor temperature (in Celsius) above which cross mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum outdoor temperature control is not applied.
+
+\textbf{Note:} The maximum outdoor temperature when cross mixing is shutoff must be greater than or equal to the minimum outdoor temperature which cross mixing is shutoff at any given time. Otherwise, a warning will be issued and the maximum outdoor shutoff temperature will be set to the minimum outdoor shutoff temperature.
+
+An IDF Example:
+
+\begin{lstlisting}
+
+ZoneCrossMixing,
+      1stFloor-Garage,  !- Name
+      GARAGE,      !- Zone Name
+      Always On,   !- SCHEDULE Name
+      Flow/Zone,               !- Design Flow Rate calculation method
+      0.1,                     !- Design Flow Rate {m3/s}
+      ,                        !- Flow Rate per Area {m3/s/m2}
+      ,                        !- Flow Rate per Person {m3/s/person}
+      ,                        !- Air Changes Per Hour
+      1ST-FLOOR,   !- Source Zone Name
+      1.0;         !- Delta temp
+
+  ZoneCrossMixing,
+      Garage-1stFloor,  !- Name
+      1ST-FLOOR,   ! Zone Name
+      Always On,   !- SCHEDULE Name
+      flow/zone,               !- Design Flow Rate calculation method
+      0.1,                     !- Design Flow Rate {m3/s}
+      ,                        !- Flow Rate per area {m3/s/m2}
+      ,                        !- Flow Rate per person {m3/s/person}
+      ,                        !- Air Changes Per Hour
+      GARAGE,      ! Source Zone Name
+      1.0;         ! Delta temp
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-000}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Zone Mixing Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Mixing Current Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Mixing Standard Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Mixing Mass {[}kg{]}
+\item
+  HVAC,Sum,Zone Mixing Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum,Zone Mixing Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Total Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Total Heat Gain Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Zone Mixing Volume {[}m3{]}}\label{zone-mixing-volume-m3-1}
+
+The air volume in m\(^{3}\) entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
+
+\paragraph{Zone Mixing Current Density Volumetric Flow Rate {[}m3/s{]}}\label{zone-mixing-current-density-volumetric-flow-rate-m3s-1}
+
+The air volumetric flow rate in m\(^{3}\)/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at current zone air conditions.
+
+\paragraph{Zone Mixing Standard Density Volumetric Flow Rate {[}m3/s{]}}\label{zone-mixing-standard-density-volumetric-flow-rate-m3s-1}
+
+The air volumetric flow rate in m\(^{3}\)/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at standard conditions.
+
+\paragraph{Zone Mixing Mass {[}kg{]}}\label{zone-mixing-mass-kg-1}
+
+The air mass in kg entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep. The air mass is calculated using the air volume flow from each ``source'' zone and the density of air calculated for the average conditions (temperature and humidity) between the ``source'' and ``receiving'' zones.
+
+\paragraph{Zone Mixing Mass Flow Rate {[}kg/s{]}}\label{zone-mixing-mass-flow-rate-kgs-1}
+
+The air mass flow rate in kg/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
+
+\paragraph{Zone Mixing Sensible Heat Loss Energy {[}J{]}}\label{zone-mixing-sensible-heat-loss-energy-j-1}
+
+\paragraph{Zone Mixing Sensible Heat Gain Energy {[}J{]}}\label{zone-mixing-sensible-heat-gain-energy-j-1}
+
+The sensible (temperature) heat transfer due to the sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the specific heat (calculated for the average conditions (temperature and humidity) between the ``source'' and ``receiving'' zones) and the temperature differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing sensible heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing sensible heat gain.
+
+\paragraph{Zone Mixing Latent Heat Loss Energy {[}J{]}}\label{zone-mixing-latent-heat-loss-energy-j-1}
+
+\paragraph{Zone Mixing Latent Heat Gain Energy {[}J{]}}\label{zone-mixing-latent-heat-gain-energy-j-1}
+
+The latent heat transfer due tothe sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the heat of vaporization (calculated for the average conditions (temperature and humidity) between the ``source'' and ``receiving'' zones)and the humidity ratio differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing latent heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing latent heat gain.
+
+\paragraph{Zone Mixing Total Heat Loss Energy {[}J{]}}\label{zone-mixing-total-heat-loss-energy-j-1}
+
+The total heat loss due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy \textless{} the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
+
+\paragraph{Zone Mixing Total Heat Gain Energy {[}J{]}}\label{zone-mixing-total-heat-gain-energy-j-1}
+
+The total heat gain due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy \textgreater{} = the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
+
+\subsection{ZoneRefrigerationDoorMixing}\label{zonerefrigerationdoormixing}
+
+The ZoneRefrigerationDoorMixing syntax is ideally suited for two zones, at least one of which is refrigerated, that exchange an equal amount of dry air. They may also have mixed air from other zones, but only one object should be entered for any one pair of zones. As with Mixing (ref: Mixing), this is a simplified view of interzone airflow in EnergyPlus. The ZoneRefrigerationDoorMixing approach shares some features of both Mixing and Cross Mixing. Like Cross Mixing, RefrigerationDoorMixing has an energy effect on both the source and the receiving zone, thus maintaining both the air mass and energy balances in the two zones. Like Mixing, the refrigerated zone can exchange air with multiple zones.~ Unlike either of the other two mixing objects, the RefrigeratedDoorMixing always calculates the air exchange based on the zone temperature and relative humidity. That is, the user does not specify the air flow rate. The user can moderate the flow through a door-opening schedule.
+
+Unlike, Cross Mixing, Refrigeration Door Mixing can only be entered once for any unique pair of zones. It doesn't matter which zone is listed first and the zones will automatically switch back and forth between source and receiving zones depending upon which zone is colder.
+
+Refrigeration Door Mixing is entered using the following syntax.
+
+\subsubsection{Inputs}\label{inputs-7-003}
+
+\paragraph{Field: Name}\label{field-name-7-002}
+
+The name of the ZoneRefrigerationDoorMixing object.
+
+\paragraph{Field: Zone 1~ Name}\label{field-zone-1-name}
+
+This field is the name of one of the two zones (ref: Zone) exchanging air and attaches a particular refrigeration door~ mixing statement to both thermal zones in the building.
+
+\paragraph{Field: Zone 2~ Name}\label{field-zone-2-name}
+
+This field is the name of the other zone (ref: Zone) exchanging air and attaches a particular refrigeration door~ mixing statement to both thermal zones in the building.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-5}
+
+This field is the name of the schedule (ref: Schedule) that modifies the door opening between the two zones and should contain values between~ 0.0 and 1.0.
+
+\paragraph{Field: Door Height}\label{field-door-height}
+
+This field denotes the door opening height (m). The default value is 3 m.
+
+\paragraph{Field: Door~ Area}\label{field-door-area}
+
+This field denotes the door opening area (m\(^{2}\)). The default value is 9 m\(^{2}\).
+
+\paragraph{Field: Door Protection Type}\label{field-door-protection-type}
+
+This field is a key/choice field that tells how the door is protected. The impact of this choice is decribed in the Engineering Reference. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  None
+\end{itemize}
+
+None, or no door protection is the default choice
+
+\begin{itemize}
+\item
+  AirCurtain
+\item
+  StripCurtain
+\end{itemize}
+
+An IDF Example:
+
+\begin{lstlisting}
+
+ZoneRefrigerationDoorMixing,
+      Freezer1_Cooler1,  !- Name
+      Freezer1,          !- Zone 1 Name
+      Cooler1,           !- Zone 2 Name
+      Freezer1DoorSched, !- Schedule Name
+      1.8,               !- Door height {m}
+      2.3,               !- Door area {m2}
+      StripCurtain;      !- Door protection type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-000}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Zone Mixing Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Mixing Current Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Mixing Standard Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Mixing Mass {[}kg{]}
+\item
+  HVAC,Sum,Zone Mixing Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum,Zone Mixing Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Latent Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Total Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Mixing Total Heat Gain Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Zone Mixing Volume {[}m3{]}}\label{zone-mixing-volume-m3-2}
+
+The air volume in m\(^{3}\) entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
+
+\paragraph{Zone Mixing Current Density Volumetric Flow Rate {[}m3/s{]}}\label{zone-mixing-current-density-volumetric-flow-rate-m3s-2}
+
+The air volumetric flow rate in m\(^{3}\)/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at current zone air conditions.
+
+\paragraph{Zone Mixing Standard Density Volumetric Flow Rate {[}m3/s{]}}\label{zone-mixing-standard-density-volumetric-flow-rate-m3s-2}
+
+The air volumetric flow rate in m\(^{3}\)/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at standard conditions.
+
+\paragraph{Zone Mixing Mass {[}kg{]}}\label{zone-mixing-mass-kg-2}
+
+The air mass in kg entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep. The air mass is calculated using the air volume flow from each ``source'' zone and the density of air calculated for the average conditions (temperature and humidity) between the ``source'' and ``receiving'' zones.
+
+\paragraph{Zone Mixing Mass Flow Rate {[}kg/s{]}}\label{zone-mixing-mass-flow-rate-kgs-2}
+
+The air mass flow rate in kg/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
+
+\paragraph{Zone Mixing Sensible Heat Loss Energy {[}J{]}}\label{zone-mixing-sensible-heat-loss-energy-j-2}
+
+\paragraph{Zone Mixing Sensible Heat Gain Energy {[}J{]}}\label{zone-mixing-sensible-heat-gain-energy-j-2}
+
+The sensible (temperature) heat transfer due to the sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the specific heat (calculated for the average conditions (temperature and humidity) between the ``source'' and ``receiving'' zones) and the temperature differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing sensible heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing sensible heat gain.
+
+\paragraph{Zone Mixing Latent Heat Loss Energy {[}J{]}}\label{zone-mixing-latent-heat-loss-energy-j-2}
+
+\paragraph{Zone Mixing Latent Heat Gain Energy {[}J{]}}\label{zone-mixing-latent-heat-gain-energy-j-2}
+
+The latent heat transfer due tothe sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the heat of vaporization (calculated for the average conditions (temperature and humidity) between the ``source'' and ``receiving'' zones)and the humidity ratio differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing latent heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing latent heat gain.
+
+\paragraph{Zone Mixing Total Heat Loss Energy {[}J{]}}\label{zone-mixing-total-heat-loss-energy-j-2}
+
+The total heat loss due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy \textless{} the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
+
+\paragraph{Zone Mixing Total Heat Gain Energy {[}J{]}}\label{zone-mixing-total-heat-gain-energy-j-2}
+
+The total heat gain due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy \textgreater{} = the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
+
+\subsection{ZoneEarthtube (Earth Tube)}\label{zoneearthtube-earth-tube}
+
+An earth tube is a long, underground metal or plastic pipe through which air is drawn. During cooling season, as air travels through the pipe, it gives up some of its heat to the surrounding soil and enters the room as cooler air. Similarly, during heating season, as air travels through the pipe, it receives some of its heat from the soil and enters the room as warmer air. Simple earth tubes in EnergyPlus can be controlled by a schedule and through the specification of minimum, maximum, and delta temperatures as described below. As with infiltration and ventilation, the actual flow rate of air through the earth tube can be modified by the temperature difference between the inside and outside environment and the wind speed. The basic equation used to calculate air flow rate of earth tube in EnergyPlus is:
+
+\begin{equation}
+EarthTubeFlowRate = \left( {{E_{design}}} \right)\left( {{F_{schedule}}} \right)\left[ {A + B\left| {{T_{zone}} - {T_{odb}}} \right| + C\left( {WindSpeed} \right) + D\left( {WindSpee{d^2}} \right)} \right]
+\end{equation}
+
+For the simulation of the earth tube, a weather data file is required and, therefore, the earth tube cannot run without weather data file. The required input fields to simulate the earth tube include the average soil surface temperature, the amplitude of soil surface temperature, and the phase constant of soil surface temperature. These fields should be calculated in advance by using a separate stand-alone program (CalcSoilSurfTemp) and should be input into earth tube.
+
+\subsubsection{CalcSoilSurfTemp -- Auxiliary Programs Document}\label{calcsoilsurftemp-auxiliary-programs-document}
+
+The CalcSoilSurfTemp program is simple and requires only two input fields : soil condition and soil surface condition in addition to a valid weather file. For soil condition, the user should select the number corresponding to the actual condition of the soil surrounding the earth tube from the four following options: 1. HEAVY AND SATURATED, 2. HEAVY AND DAMP, 3. HEAVY AND DRY and 4. LIGHT AND DRY. This determines the thermal diffusivity and thermal conductivity of the surrounding soil. For soil surface conditions, the user should select the number corresponding to the actual condition of the ground surface above the earth tube from the eight following options: 1. BARE AND WET, 2. BARE AND MOIST, 3. BARE AND ARID, 4. BARE AND DRY, 5. COVERED AND WET, 6. COVERED AND MOIST, 7. COVERED AND ARID and 8. COVERED AND DRY. This determines the absorption coefficient and the fraction of evaporation rate of the ground surface.
+
+From this information and an analysis of the weather for the location selected, the CalcSoilSurfTemp program (ref. Auxiliary Programs document) calculates the three parameters listed above. The user must then add these parameters as input into EnergyPlus. The full input description of an earth tube in EnergyPlus is given below.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-5}
+
+This field is the name of the zone (ref: Zone) and attaches a particular earth tube statement to a thermal zone in the building.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name-6}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design volume flow rate parameter (see next field). This fraction between 0.0 and 1.0 is noted as F\(_{schedule}\) in the above equation.
+
+\subsubsection{Field: Design Flow Rate}\label{field-design-flow-rate-4}
+
+This number (noted as E\(_{design}\) in the above equation) is the maximum amount of air mass flow rate of the earth tube expected at design conditions. The flow rate is expressed in units of m\(^{3}\)/s. The design value is modified by the schedule fraction (see previous field) and user specified coefficients (see last four fields).
+
+\subsubsection{Field: Minimum Zone Temperature when Cooling}\label{field-minimum-zone-temperature-when-cooling}
+
+This is the indoor temperature (in Celsius) below which the earth tube is shut off. This lower temperature limit is intended to avoid overcooling a space and thus result in a heating load. For example, if the user specifies a minimum temperature of 20°C, earth tube is assumed to be available if the zone air temperature is above 20°C. If the zone air temperature drops below 20°C, then earth tube is automatically turned off.
+
+\subsubsection{Field: Maximum Zone Temperature when Heating}\label{field-maximum-zone-temperature-when-heating}
+
+This is the indoor temperature (in Celsius) above which the earth tube is shut off. This higher temperature limit is intended to avoid overheating a space and thus result in a cooling load. For example, if the user specifies a maximum temperature of 20°C, earth tube is assumed to be available if the zone air temperature is below 20°C. If the zone air temperature rises above 20°C, then earth tube is automatically turned off.
+
+\subsubsection{Field: Delta Temperature}\label{field-delta-temperature-4}
+
+This is the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which the earth tube is shut off. This is to allow the earth tube to be stopped either if the temperature outside is too warm and could potentially heat the space or if the temperature outside is too cold and could potentially cool the space. For example, if the user specifies a delta temperature of 2°C, earth tube is assumed to be available if the temperature difference between indoor and outdoor temperature is at least 2°C. If the outside air dry-bulb temperature is less than 2°C cooler or warmer than the indoor dry-bulb temperature, then the earth tube is automatically turned off.
+
+\subsubsection{Field: Earthtube Type}\label{field-earthtube-type}
+
+This alpha character string defines the type of earth tube as one of the following options: Natural, Exhaust, or Intake. A natural earth tube is assumed to be air movement/exchange that will not consume any fan energy or is the result of natural air flow through the tube and into the building. Values for fan pressure and efficiency for a natural flow earth tube are ignored. For either EXHAUST or Intake, values for fan pressure and efficiency define the fan electric consumption. For Natural and Exhaustearth tubes, the conditions of the air entering the space are assumed to be equivalent to the air which is cooled or heated by passing along the pipe. For Intake earth tubes, an appropriate amount of fan heat is added to the air stream.
+
+\subsubsection{Field: Fan Pressure Rise}\label{field-fan-pressure-rise-1}
+
+This is the pressure rise experienced across the fan in Pascals (N/m\(^{2}\)). This is a function of the fan and plays a role in determining the amount of energy consumed by the fan.
+
+\subsubsection{Field: Fan Total Efficiency}\label{field-fan-total-efficiency-1}
+
+This is the total fan efficiency (a decimal number between 0.0 and 1.0). This is a function of the fan and plays a role in determining the amount of energy consumed by the fan.
+
+\subsubsection{Field: Pipe Radius}\label{field-pipe-radius}
+
+This is the radius of the earth tube/pipe (in meters). This plays a role in determining the amount of heat transferred from the surrounding soil to the air passing along the pipe. If the pipe has non-circular cross section, user can use the concept of hydraulic diameter as follows.
+
+\begin{equation}
+D = 4 \times Area/Perimeter
+\end{equation}
+
+However, since this field requires the pipe radius, hydraulic diameter should be divided by two.
+
+\subsubsection{Field: Pipe Thickness}\label{field-pipe-thickness}
+
+This is the thickness of the pipe wall (in meters). This plays a role in determining the amount of heat transferred from the surrounding soil to the air passing along the pipe.
+
+\subsubsection{Field: Pipe Length}\label{field-pipe-length}
+
+This is the total length of the pipe (in meters). This plays a role in determining the amount of heat transferred from the surrounding soil to the air passing along the pipe. As the length of the pipe becomes longer, the amount of the heat transfer becomes larger.
+
+\subsubsection{Field: Pipe Thermal Conductivity}\label{field-pipe-thermal-conductivity}
+
+This is the thermal conductivity of the pipe (in W/m°C). This plays a role in determining the amount of heat transferred from the surrounding soil to the air passing along the pipe.
+
+\subsubsection{Field: Pipe Depth Under Ground Surface}\label{field-pipe-depth-under-ground-surface}
+
+This is the depth of the pipe under the ground surface (in meters). This plays a role in determining the temperature of the soil surrounding the pipe.
+
+\subsubsection{Field: Soil Condition}\label{field-soil-condition}
+
+This alpha character string defines the actual condition of the soil surrounding the earth tube and can be one of any of the following options: HeavyAndSaturated, HeavyAndDamp, HeavyAndDry or LightAndDry. This determines the thermal diffusivity and thermal conductivity of the surrounding soil, which play a role in determining the amount of heat transferred from the surrounding soil to the air passing along the pipe.
+
+\subsubsection{Field: Average Soil Surface Temperature}\label{field-average-soil-surface-temperature}
+
+This is the annual average soil surface temperature straight above the earth tube, which plays a role in determining the temperature of the soil surrounding the pipe. This field should be calculated in advance using the separate CalcSoilSurfTemp program.
+
+\subsubsection{Field: Amplitude of Soil Surface Temperature}\label{field-amplitude-of-soil-surface-temperature}
+
+This is the amplitude of soil surface temperature above the earth tube, which plays a role in determining the temperature of the soil surrounding the pipe. This is the difference between the maximum and minimum soil surface temperature for the whole year divided by two. This field should be calculated in advance using the separate CalcSoilSurfTemp program.
+
+\subsubsection{Field: Phase Constant of Soil Surface Temperature}\label{field-phase-constant-of-soil-surface-temperature}
+
+This is the phase constant of the soil surface temperature straight above the earth tube, which play a role in determining the temperature of the soil surrounding the pipe at particular time. This is the time elapsed from the beginning of the year until the soil surface temperature reaches the minimum value of the year. This field should be calculated in advance using the separate CalcSoilSurfTemp program.
+
+\subsubsection{Field: Constant Term Flow Coefficient}\label{field-constant-term-flow-coefficient}
+
+This number is the ``A'' parameter in the above earth tube equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter, however, is a constant under all conditions and is not modified by any environmental effect. As a result, it is dimensionless.
+
+\subsubsection{Field: Temperature Term Flow Coefficient}\label{field-temperature-term-flow-coefficient}
+
+This number is the ``B'' parameter in the above earth tube equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the temperature difference between the outdoor and indoor air dry-bulb temperatures. The units for this parameter are inverse Celsius.
+
+\subsubsection{Field: Velocity Term Flow Coefficient}\label{field-velocity-term-flow-coefficient}
+
+This number is the ``C'' parameter in the above earth tube equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the speed of wind being experienced outside the building. The units for this parameter are s/m.
+
+\subsubsection{Field: Velocity Squared Term Flow Coefficient}\label{field-velocity-squared-term-flow-coefficient}
+
+This number is the ``D'' parameter in the above earth tube equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by square of the speed of wind being experienced outside the building. The units for this parameter are s\(^{2}\)/m\(^{2}\).
+
+An IDF example:
+
+\begin{lstlisting}
+
+EARTHTUBE,
+  Zone 2,           !- Zone Name
+  Simple EarthTube, !- Schedule Name
+  3.425198,         !- Design Volume Flow Rate
+  10.0,             !- Minimum Zone Temperature when Cooling
+  30.0,             !- Maximum Zone Temperature when Heating
+  1.0,              !- Delta Temperature
+  NATURAL,          !- EarthTube Type
+  350.0,            !- Fan Pressure Rise
+  0.9,              !- Fan Total Efficiency
+  0.25,             !- Pipe Radius
+  0.2,              !- Pipe Thickness
+  15.0,             !- Pipe Length
+  200.0,            !- Pipe Thermal Conductivity
+  3.5,              !- Pipe Depth Under Ground Surface
+  HeavyAndDamp,     !- Soil Condition
+  15.0,             !- Average Soil Surface Temperature
+  5.6,              !- Amplitude of Soil Surface Temperature
+  0.0,              !- Phase Constant of Soil Surface Temperature
+  0.6060000    ,    !- Constant Term Flow Coef
+  2.0199999E-02,    !- Temp Term Flow Coef
+  5.9800001E-04,    !- Velocity Term Flow Coef
+  0.0000000E+00;    !- Velocity**2 Term Flow Coef
+\end{lstlisting}
+
+\subsection{ZoneEarthTube Outputs}\label{zoneearthtube-outputs}
+
+Current Earth Tube output variables:
+
+\begin{itemize}
+\item
+  HVAC,Sum,Earth Tube Zone Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Earth Tube Zone Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Earth Tube Zone Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Earth Tube Zone Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Earth Tube Air Flow Volume {[}m3{]}
+\item
+  HVAC,Average,Earth Tube Air Current Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Earth Tube Air Standard Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Earth Tube Air Flow Mass {[}kg{]}
+\item
+  HVAC,Average,Earth Tube Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum,Earth Tube Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Earth Tube Fan Electric Power {[}W{]}
+\item
+  HVAC,Average,Earth Tube Zone Inlet Air Temperature {[}C{]}
+\item
+  HVAC,Average,Earth Tube Ground Interface Temperature {[}C{]}
+\item
+  HVAC,Average,Earth Tube Outdoor Air Heat Transfer Rate {[}W{]}
+\end{itemize}
+
+\subsubsection{Earth Tube Zone Sensible Cooling Energy {[}J{]}}\label{earth-tube-zone-sensible-cooling-energy-j}
+
+\subsubsection{Earth Tube Zone Sensible Cooling Rate {[}W{]}}\label{earth-tube-zone-sensible-cooling-rate-w}
+
+These are the energy and rate associated with the zone cooling provided by the air from the earth tube.~ This occurs when the earth tube outlet air temperature is less than zone air temperature.
+
+\subsubsection{Earth Tube Zone Sensible Heating Energy {[}J{]}}\label{earth-tube-zone-sensible-heating-energy-j}
+
+\subsubsection{Earth Tube Zone Sensible Heating Rate {[}W{]}}\label{earth-tube-zone-sensible-heating-rate-w}
+
+These are the energy and rate associated with the zone heating provided by the air from the earth tube.~ This occurs when the earth tube outlet air temperature is greater than the zone air temperature.
+
+\subsubsection{Earth Tube Air Flow Volume {[}m3{]}}\label{earth-tube-air-flow-volume-m3}
+
+The volume flow of air through the earth tube.
+
+\subsubsection{Earth Tube Air Current Density Volumetric Flow Rate {[}m3/s{]}}\label{earth-tube-air-current-density-volumetric-flow-rate-m3s}
+
+The volume flow rate of air through the earth tube evaluating density at current zone conditions.
+
+\subsubsection{Earth Tube Air Standard Density Volumetric Flow Rate {[}m3/s{]}}\label{earth-tube-air-standard-density-volumetric-flow-rate-m3s}
+
+The volume flow rate of air through the earth tube evaluating density at standard conditions.
+
+\subsubsection{Earth Tube Air Flow Mass {[}kg{]}}\label{earth-tube-air-flow-mass-kg}
+
+The mass flow of air through the earth tube.
+
+\subsubsection{Earth Tube Air Mass Flow Rate {[}kg/s{]}}\label{earth-tube-air-mass-flow-rate-kgs}
+
+The mass flow rate of air through the earth tube.
+
+\subsubsection{Earth Tube Fan Electric Energy {[}J{]}}\label{earth-tube-fan-electric-energy-j}
+
+\subsubsection{Earth Tube Fan Electric Power {[}W{]}}\label{earth-tube-fan-electric-power-w}
+
+These are the fan electricity consumption and power for intake or exhaust earth tube types.
+
+\subsubsection{Earth Tube Zone Inlet Air Temperature {[}C{]}}\label{earth-tube-zone-inlet-air-temperature-c}
+
+This is the temperature of the air entering the zone after passing through the earth tube {[}C{]}.~ This temperature includes the cooling or heating of outdoor air as it passes along the pipe. ~When intake fan assist is used, then the additional heat due to the fan is included in the inlet air temperature.
+
+\subsubsection{Earth Tube Ground Interface Temperature {[}C{]}}\label{earth-tube-ground-interface-temperature-c}
+
+This is the average temperature of the ground along the outer surface of the earth tube {[}C{]}.
+
+\subsubsection{Earth Tube Outdoor Air Heat Transfer Rate {[}W{]}}\label{earth-tube-outdoor-air-heat-transfer-rate-w}
+
+This is the rate of heat transfer from the earth tube to the outdoor air {[}W{]}.~ Positive values indicate the rate at which outdoor air is preheated; negative values indicate the rate of precooling.
+
+\subsection{ZoneCoolTower:Shower}\label{zonecooltowershower}
+
+A cooltower (which is sometimes referred to as a wind tower or a shower cooling tower) is a component that is intended to model a passive downdraught evaporative cooling (PDEC) that is designed to capture the wind at the top of a tower and cool the outside air using water evaporation before delivering it to a space.~ The air flow in these systems is natural as the evaporation process increases the density of the air causing it to fall through the tower and into the space without the aid of a fan. ~A cooltower typically consists of a water spray or an evaporative pad, a shaft, and a water tank or reservoir. ~Wind catchers to improve the wind-driven performance at the top of the tower are optional. ~Water is pumped over an evaporative device by water pump which is the only component consumed power for this system.~ This water cools and humidifies incoming air and then the cool, dense air naturally falls down through shaft and leaves through large openings at the bottom of cooltowers.
+
+The shower cooling tower can be controlled by a schedule and the specification of maximum water flow rate and volume flow rate as well as minimum indoor temperature.~ The actual flow rate of water and air can be controlled as users specify the fractions of water loss and flow schedule.~ The required input fields include effective tower height and exit area to obtain the temperature and flow rate of the air exiting the tower.~ A schedule and rated power for the water pump are also required to determine the power consumed. The component typically has a stand alone water system that is not added to the water consumption from mains. However, users are required to specify the water source through an optional field, the name of water supply storage tank, in case any water comes from a water main. The model is described more fully in the Engineering Reference document.
+
+This model requires weather information obtained from either design day or weather file specifications. ~The control is accomplished by either specifying the water flow rate or obtaining the velocity at the outlet with inputs and weather conditions when the water flow rate is unknown.~ As with infiltration, ventilation, and earth tubes, the component is treated in a similar fashion to ``natural ventilation'' in EnergyPlus.
+
+\subsubsection{Inputs}\label{inputs-8-002}
+
+\paragraph{Field: Name}\label{field-name-8-002}
+
+This field is a unique user assigned name for each cooltower.~ Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-000}
+
+This field is the name of the schedule that denotes whether the cooltower can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the cooltower is available and can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the cooltower is not available and must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-6}
+
+This field is the name of the zone (ref: Zone) and attaches a particular cooltower statement to a thermal zone in the building.
+
+\paragraph{Field: Water Supply Storage Tank Name}\label{field-water-supply-storage-tank-name}
+
+This field is optional. ~It is used to describe where the cooltower obtains water used for evaporative cooling. ~If blank or omitted, then the cooltower will obtain water directly from local water main. ~If the name of a Water Storage Tank object is used here, then the cooltower will obtain its water from that tank. ~If a tank is specified, the cooltower will attempt to obtain all the water it uses from the tank. ~However, if the tank cannot provide all the water the cooltower needs, then the cooltower will still operate and obtain the rest of the water it needs from the mains (referred to as `Starved' water).
+
+\paragraph{Field: Flow Control Type}\label{field-flow-control-type}
+
+This field specifies how the user wishes to control the cooltower.~ The air flow from the cooltower may be controlled by either the water flow rate along with the water pump schedule or naturally driven by wind flow.~ The user must select from the following options: \textbf{WaterFlowSchedule} and \textbf{WindDrivenFlow}.~ If the user either wishes to control the water flow rate or has information about the water flow rate, \textbf{WaterFlowSchedule} must be selected.~ \textbf{WindDrivenFlow} for cooltower flow control must be selected when the water flow rate is unknown and the user wishes to have the flow rate of both air and water controlled by the external weather conditions (wind speed).~ If the user does not select a control type, \textbf{WindDrivenFlow} is assumed as a flow control type.
+
+\paragraph{Field: Pump Flow Rate Schedule Name}\label{field-pump-flow-rate-schedule-name}
+
+This field modifies the maximum flow rate of water through the cooltower in m3/sec.~This input is ``optional.'' If the user does not enter a schedule, the flow rate through the cooltower is assumed to be constant during all hours that it is operating based on the value entered in the previous input field. Note that the values for this schedule must be between zero and one.
+
+\paragraph{Field: Maximum Water Flow Rate}\label{field-maximum-water-flow-rate}
+
+This field is the maximum water flow rate distributed to the tower in m3/s. This limit is intended to avoid over estimation of water flow rate, which leads higher air flow rate and exit temperature of the air.
+
+\paragraph{Field: Effective Tower Height}\label{field-effective-tower-height}
+
+This field is the effective tower height for evaporative cooling, from the water spray to the top of the exit in m.
+
+\paragraph{Field: Airflow Outlet Area}\label{field-airflow-outlet-area}
+
+This field is the area at the exit of the tower in m2. ~This field is used to determine the air flow rate leaving the tower with the velocity of the air flow.
+
+\paragraph{Field: Maximum Air Flow Rate}\label{field-maximum-air-flow-rate-000}
+
+This field is the maximum volumetric flow rate of the air leaving the tower in m3/s. ~This airflow maximum allows the cooltower performance to be limited if the outside wind speed and the tower height are relatively high and thus result in high airflow supplied to the space.
+
+\paragraph{Field: Minimum Indoor Temperature}\label{field-minimum-indoor-temperature-2}
+
+This field is the minimum indoor temperature in Celsius below which cooltower is shutoff. ~This lower temperature limit is intended to avoid overcooling a space and thus result in a heating load. ~For example, if the user specifies a minimum temperature of 20°C, cooltower is assumed to be available if the zone air temperature is above 20°C. ~If the zone air temperature drops below 20°C, then cooltower is automatically turned off.
+
+\paragraph{Field: Fraction of Water Loss}\label{field-fraction-of-water-loss}
+
+This field specifies the fraction of the loss of water during either operation or transient operation. If the user does not enter a fraction, no loss of water is assumed and the cooltower water consumption includes only evaporation.~ Note that the fraction must be between zero and one.
+
+\paragraph{Field: Fraction of Flow Schedule}\label{field-fraction-of-flow-schedule}
+
+This field specifies the fraction of the airflow that actually goes to the outside.~ The user who wishes to control the actual flow to the inside of the building must specify the value of the fraction.~ If the user does not enter a fraction, the calculated flow rate is the ``zone cooltower volume flow rate.''~ Note that the fraction must be between zero and one.
+
+\paragraph{Field: Rated Power Consumption}\label{field-rated-power-consumption}
+
+This field is the pump's rated power consumption in Watts.
+
+Below is an example input for a cooltower.
+
+\begin{lstlisting}
+
+ZoneCoolTower:Shower
+  Cool Tower 1,         !- Name of cooltowers
+  Zone 1,               !- Zone name
+  Simple Vent,          !- Schedule
+  ,                     !- Name of water supply storage tanks
+  WindDrivenFlow,       !- Flow control type
+  0.0005,               !- Water flow rate from the spray in m3/s
+  ,                     !- schedule for flow rate (optional, non-existent means constant)
+  5.0,                  !- Effective tower height in m
+  1.0,                  !- Exit area in m2
+  10.0,                 !- Maximum supply air volume flow rate in m3/s
+  18.0,                 !- Minimum indoor temperature to prevent overcooling in C
+  0.05,                 !- Fraction of Water loss
+  0.05,                 !- Fraction of flow that goes to outside
+  250.0;                !- Rated power consumption in W
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-000}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Zone Cooltower Sensible Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,Zone Cooltower Sensible Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Cooltower Latent Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average,Zone Cooltower Latent Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Cooltower Air Volume {[}m3{]}
+\item
+  HVAC,Average,Zone Cooltower Air Current Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Zone Cooltower Air Standard Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Cooltower Air Mass {[}kg{]}
+\item
+  HVAC,Average,Zone Cooltower Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Cooltower Air Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Cooltower Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,Zone Cooltower Air Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Cooltower Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,Zone Cooltower Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Zone Cooltower Pump Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Cooltower Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Cooltower Mains Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Cooltower Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Cooltower Starved Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Zone Cooltower Sensible Heat Loss Energy {[}J{]}}\label{zone-cooltower-sensible-heat-loss-energy-j}
+
+\paragraph{Zone Cooltower Sensible Heat Loss Rate {[}W{]}}\label{zone-cooltower-sensible-heat-loss-rate-w}
+
+The sensible heat loss that occurs when the temperature at the exit of the cooltower is less than that of the zone.
+
+\paragraph{Zone Cooltower Latent Heat Loss Energy {[}J{]}}\label{zone-cooltower-latent-heat-loss-energy-j}
+
+\paragraph{Zone Cooltower Latent Heat Loss Rate {[}W{]}}\label{zone-cooltower-latent-heat-loss-rate-w}
+
+The latent heat loss that occurs when the humidity ratio at the exit of the cooltower is greater than that of the zone.
+
+\paragraph{Zone Cooltower Air Current Density Volumetric Flow Rate {[}m3/s{]}}\label{zone-cooltower-air-current-density-volumetric-flow-rate-m3s}
+
+The volumetric flow rate of the air leaving the cooltower evaluating density at current zone conditions.
+
+\paragraph{Zone Cooltower Air Standard Density Volumetric Flow Rate {[}m3/s{]}}\label{zone-cooltower-air-standard-density-volumetric-flow-rate-m3s}
+
+The volumetric flow rate of the air leaving the cooltower evaluating density at standard conditions.
+
+\paragraph{Zone Cooltower Air Volume {[}m3{]}}\label{zone-cooltower-air-volume-m3}
+
+The sum of actual volumetric flow of the air leaving cooltower
+
+\paragraph{Zone Cooltower Air Mass Flow Rate {[}kg/s{]}}\label{zone-cooltower-air-mass-flow-rate-kgs}
+
+The mass flow rate of the air leaving the cooltower
+
+\paragraph{Zone Cooltower Air Mass {[}kg{]}}\label{zone-cooltower-air-mass-kg}
+
+The sum of actual mass flow of the air leaving the cooltower
+
+\paragraph{Zone Cooltower Air Inlet Temperature {[}C{]}}\label{zone-cooltower-air-inlet-temperature-c}
+
+The dry-bulb temperature of the outdoor air the inlet of the cooltower
+
+\paragraph{Zone Cooltower Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{zone-cooltower-air-inlet-humidity-ratio-kgwaterkgdryair}
+
+~The humidity ratio of the outdoorair at the inlet of the cooltower
+
+\paragraph{Zone Cooltower Air Outlet Temperature {[}C{]}}\label{zone-cooltower-air-outlet-temperature-c}
+
+The temperature at the exit of the cooltower.
+
+\paragraph{Zone Cooltower Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{zone-cooltower-air-outlet-humidity-ratio-kgwaterkgdryair}
+
+The humidity ratio of the air at the exit of the cooltower.
+
+\paragraph{Zone Cooltower Water Volume ~{[}m3{]}}\label{zone-cooltower-water-volume-m3}
+
+The water consumption includes not only the direct thermodynamics of water evaporation but also other sources of consumption such as drift or concentration blow down specified by users throughout all processes during the operation.
+
+\paragraph{Zone Cooltower Mains Water Volume ~{[}m3{]}}\label{zone-cooltower-mains-water-volume-m3}
+
+This is the water consumed by the cooltower that actually be met by the mains water. This output variable appears only when the water comes from mains.
+
+\paragraph{Zone Cooltower Storage Tank Water Volume ~{[}m3{]}}\label{zone-cooltower-storage-tank-water-volume-m3}
+
+This is the water consumed by the cooltower that actually be met by the water storage tank.~ If any amount of the water is starved from mains, this water consumption is the difference between the Zone Cooltower Water Volume and the following output.~ This output variable appears only when the water comes from storage tank waters.
+
+\paragraph{Zone Cooltower Starved Mains Water Volume {[}m3{]}}\label{zone-cooltower-starved-mains-water-volume-m3}
+
+This is the source (mains) of water consumed by the cooltower that could not actually be met by the storage tank. ~This output variable appears only when the water comes from storage tank waters.
+
+\paragraph{Zone Cooltower Pump Electric Power {[}W{]}}\label{zone-cooltower-pump-electric-power-w}
+
+The power consumed by the recirculating pump in Watts.
+
+\paragraph{Zone Cooltower Pump Electric Energy {[}J{]}}\label{zone-cooltower-pump-electric-energy-j}
+
+The energy consumed by the recirculating pump in Joules.
+
+\subsection{ZoneThermalChimney (Thermal Chimney)}\label{zonethermalchimney-thermal-chimney}
+
+A thermal chimney is a vertical shaft utilizing solar radiation to enhance the natural ventilation in buildings. It consists of a absorber wall, air gap and glass cover with high solar transmissivity. For the high solar absorption, it is usually south facing.
+
+The key output parameter in the thermal chimney model is the enhanced amount of natural ventilation rate caused by the presence of a thermal chimney. In order to determine the enhanced ventilation, the discharge air temperature from a thermal chimney should be calculated, which, in turn, should be computed based on the information on the absorber wall temperature, glass cover temperature and the vertical air temperature distribution within the thermal chimney. Among them, energy balances for the absorber wall and the glass cover are carried out using the existing algorithm currently available in EnergyPlus, which has the similar approach to the Trombe wall. As stated in the Trombe wall object as well, this approach allows the flexibility for users to specify the various wall parameters and to explore unusual configurations. On the other hand, the vertical air temperature distribution and the resultant discharge air temperature of the thermal chimney are computed using the separate thermal chimney algorithm described in the Engineering Reference document.
+
+Similar to the Trombe wall model, a zone is coupled to the desired surface via an interzone partition. To simulate the thermal chimney, the Solar Distribution field in the Building object should be set to FullInteriorAndExterior so that the majority of the solar flux is directed on the absorber wall. For a normal sized thermal chimney zone, the user can set the Zone Inside Convection Algorithm to ``Detailed'', which takes into account natural convection effects intended for a normal zone. For a narrow cavity zone having high aspect ratios, there is no built-in algorithm for calculating the correct convection coefficients on the inside of thermal chimney zone walls. One option is to use the ``Detailed'' convection algorithm similar to the Trombe wall model. However, some error may be incurred when used with a narrow zone. Another option is to use the SurfaceProperty:ConvectionCoefficients object to schedule coefficients that have been determined beforehand by the user. In addition, the wall construction of the adjoining zone must be the mirror image of the wall construction in the thermal chimney zone.
+
+The full input description of a thermal chimney in EnergyPlus is given below.
+
+\subsubsection{Field: Name}\label{field-name-9-002}
+
+This field is a unique user assigned name for an instance of the thermal chimney system.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-7}
+
+This field is the name of the thermal chimney zone (ref: Zone). Since the thermal chimney is not only a system component but also a zone itself, this field is also necessary. It should be differentiated from the \emph{Zone name} field described later.
+
+\subsubsection{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-000}
+
+This field is the name of the schedule (ref: Schedule) that denotes whether the thermal chimney can operate during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the system is available and can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the system is not available and must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\subsubsection{Field: Width of the Absorber Wall}\label{field-width-of-the-absorber-wall}
+
+This number is the width of the absorber wall in the thermal chimney.~ The width is expressed in units of m. Even though this value is specified in Surface objects as well, this value is used to compute the discharge air temperature and the enhanced ventilation rate caused by the thermal chimney.
+
+\subsubsection{Field: Cross Sectional Area of Air Channel Outlet}\label{field-cross-sectional-area-of-air-channel-outlet}
+
+This number is the cross sectional area of air channel outlet. The area is expressed in units of m\(^{2}\). The enhanced air flow rate by the thermal chimney is dependent on cross sectional areas of air channel inlet and outlet. Cross sectional areas of air channel inlet will be described later in conjunction with the distance from the top of thermal chimney to each inlet and relative ratios of air flow rates passing through each inlet.
+
+\subsubsection{Field: Discharge Coefficient}\label{field-discharge-coefficient-000}
+
+This dimensionless number is the discharge coefficient of the thermal chimney. The ventilation rate enhanced by the thermal chimney is also dependent on the discharge coefficient.
+
+\subsubsection{Field: Zone \textless{}\#\textgreater{} Name}\label{field-zone-name-8}
+
+This field is the name of the zone (ref: Zone) to which the thermal chimney is attached. It is used in conjunction with the next three fields. Note that up to 20 sets of zone name, distance from the top of the thermal chimney to each inlet, relative ratios of air flow rates passing through each zone and cross sectional areas of each air channel inlet may be entered for a single thermal chimney if multiple zones share the common thermal chimney.
+
+\subsubsection{Field: Distance from Top of Thermal Chimney to Inlet \textless{}\#\textgreater{}}\label{field-distance-from-top-of-thermal-chimney-to-inlet}
+
+This field is the distance from the top of the thermal chimney to each inlet corresponding to each zone. It is used in conjunction with the zone name, relative ratios of air flow rates passing through each zone and cross sectional areas of each air channel inlet. The distance is expressed in units of m. The air flow rate enhanced by the thermal chimney is dependent on the distance between the thermal chimney outlet and inlet.
+
+\subsubsection{Field: Relative Ratios of Air Flow Rates Passing through Zone \textless{}\#\textgreater{}}\label{field-relative-ratios-of-air-flow-rates-passing-through-zone}
+
+This dimensionless number is the relative ratio of air flow rates enhanced by the thermal chimney passing through each zone. The total air flow rate enhanced by the thermal chimney is distributed to each zone based on this number if multiple zones share the common thermal chimney. It is used in conjunction with the zone name, the distance from the top of the thermal chimney to each inlet and cross sectional areas of each air channel inlet. Note that the sum of all ratios must be equal to 1.0.
+
+\subsubsection{Field: Cross Sectional Areas of Air Channel Inlet \textless{}\#\textgreater{}}\label{field-cross-sectional-areas-of-air-channel-inlet}
+
+This field is the cross sectional areas of each air channel inlet corresponding to each zone. It is used in conjunction with the zone name, the distance from the top of the thermal chimney to each inlet and relative ratios of air flow rates passing through each zone. The area is expressed in units of m\(^{2}\). The air flow rate enhanced by the thermal chimney is dependent on cross sectional areas of air channel inlet and outlet.
+
+An IDF example:
+
+\begin{lstlisting}
+
+ZoneThermalChimney,
+    ThermalChimney1,               !- Name of Thermal Chimney System
+    ThermalChimneyZone,            !- Name of Thermal Chimney Zone
+    ThermalChimneyAvail,           !- Availability Schedule Name
+    3.5,                           !- Width of the Absorber Wall
+    0.04,                          !- Cross Sectional Area of Air Channel Outlet
+    0.8,                           !- Discharge Coefficient
+    Zone1,                         !- Zone Name 1
+    8.0,                           !- Distance from the Top of the Thermal Chimney to Inlet 1
+    0.8,                           !- Relative Ratios of Air Flow Rates Passing through Zone 1
+    0.02,                          !- Cross Sectional Areas of Air Channel Inlet 1
+    Zone2,                         !- Zone Name 2
+    5.0,                           !- Distance from the Top of the Thermal Chimney to Inlet 2
+    0.2,                           !- Relative Ratios of Air Flow Rates Passing through Zone 2
+    0.02;                          !- Cross Sectional Areas of Air Channel Inlet 2
+\end{lstlisting}
+
+\subsection{ZoneThermalChimney Outputs}\label{zonethermalchimney-outputs}
+
+Current ThermalChimney output variables:
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Thermal Chimney Current Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Zone Thermal Chimney Standard Density Volumetric Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Zone Thermal Chimney Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Thermal Chimney Outlet Temperature {[}C{]}
+\item
+  HVAC,Sum,Zone Thermal Chimney Heat Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Thermal Chimney Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Thermal Chimney Volume {[}m3{]}
+\item
+  HVAC,Sum,Zone Thermal Chimney Mass {[}kg{]}
+\end{itemize}
+
+\subsubsection{Zone Thermal Chimney Heat Loss Energy {[}J{]}}\label{zone-thermal-chimney-heat-loss-energy-j}
+
+The sensible (temperature) heat loss of each zone that occurs when the thermal chimney cools the zone air.
+
+\subsubsection{Zone Thermal Chimney Heat Gain Energy {[}J{]}}\label{zone-thermal-chimney-heat-gain-energy-j}
+
+The sensible (temperature) heat gain of each zone that occurs when the thermal chimney heats the zone air.
+
+\subsubsection{Zone Thermal Chimney Volume {[}m3{]}}\label{zone-thermal-chimney-volume-m3}
+
+The air volumetric flow of each zone enhanced by the thermal chimney.
+
+\subsubsection{Zone Thermal Chimney Mass {[}kg{]}}\label{zone-thermal-chimney-mass-kg}
+
+The air mass flow of each zone enhanced by the thermal chimney.
+
+\subsubsection{Zone Thermal Chimney Current Density Volumetric Flow Rate {[}m3/s{]}}\label{zone-thermal-chimney-current-density-volumetric-flow-rate-m3s}
+
+The total air volumetric flow rate caused by the thermal chimney evaluating density at the current zone conditions.
+
+\subsubsection{Zone Thermal Chimney Standard Density Volumetric Flow Rate {[}m3/s{]}}\label{zone-thermal-chimney-standard-density-volumetric-flow-rate-m3s}
+
+The total air volumetric flow rate caused by the thermal chimney evaluating density at standard conditions.
+
+\subsubsection{Zone Thermal Chimney Mass Flow Rate {[}kg/s{]}}\label{zone-thermal-chimney-mass-flow-rate-kgs}
+
+The total air mass flow rate caused by the thermal chimney.
+
+\subsubsection{Zone Thermal Chimney Outlet Temperature {[}C{]}}\label{zone-thermal-chimney-outlet-temperature-c}
+
+The temperature of the air which is discharged from the thermal chimney through the outlet.
+
+\subsection{ZoneAirMassFlowConservation}\label{zoneairmassflowconservation}
+
+This global object allows users to trigger the zone air mass flow conservation calculation when desired. This object has three input fields; the first choice input field allows the user whether to adjust mixing flows to enforce the zone air mass flow conservation; and the other fields allows the user to specify how infiltration object mass flow rate is calculated for zone air mass flow balance calculation.~ If adjustments for either mixing or infiltration is specified then the zone air mass balance attempts to enforce conservation. If both mixing and infiltration adjustments are off, then the zone air mass flow calculation uses the default method which does not include zone mixing objects and assumes self-balanced simple infiltration. The default method may not necessarily enforce zone air mass flow conservation unless the user has specified a balanced flow to begin with. The zone air mass flow conservation primarily accounts for the zonemixing objects air flow in the zone air flow mass balance calculation. In addition to the zonemixing object flow, the procedure accounts for zone supply, exhaust, and return flows and adjusts infiltration air flows (up or down) when required in order to balance the zone air mass flow.~ Mixing and infiltration adjustments will only be made in zones which have zonemixing or infiltration objects defined in the input. For example, if a zone does not have any infiltration objects, then no infiltration adjustment will be made for that zone.
+
+First, the ZoneMixing object mass flow rate is adjusted or modified in order to balance zone air mass flow while assuming any zone infiltration objects are self-balanced. This step will always results in balanced zone air mass for receiving zones of ZoneMixing object but it may not necessarily result in a balanced air mass flow for source zones.~
+
+Second, infiltration flow rates are adjusted accoring to the options set. Infiltration flow will be increased or decreased to balance the net flow from supply, exhaust, mixing, and return air flows. If a negative infiltration rate (exfiltration) is required to balance a zone's airflow, then the infiltration rate will be set to zero. This can happen, for example, if the total supply flow exceeds the total exahust plus return flow.
+
+This object is optional. If it is not present in the input file, the default zone air mass flow calculastion are used which do not account for zonemixing and infiltration flows.
+
+\subsubsection{Inputs}\label{inputs-9-002}
+
+\paragraph{Field: Adjust Zone Mixing For Zone Air Mass Flow Balance}\label{field-adjust-zone-mixing-for-zone-air-mass-flow-balance}
+
+This field has two choices: \emph{Yes} or \emph{No}.~ When set to \emph{Yes}, the zone air mass flow balance attempts to enforce conservation by adjusting zone mixing flow rates. When set to \emph{No}, mixing flow rates are not adjusted; the mixing flows specified in ZoneMixing obects will be used.~ The default is \emph{No}.
+
+\paragraph{Field: Infiltration Balancing Method}\label{field-infiltration-balancing-method}
+
+This field has three choices: \emph{AddInfiltrationFlow}, \emph{AdjustInfiltrationFlow}, or \emph{None}. The default is \emph{AddInfiltrationFlow}. With all three options, the base infiltration flow rate is the flow specified in all Infiltration:* objects for a given zone.
+
+\emph{AddInfiltrationFlow}: The base infiltration flow may be increased in order to balance the zone air mass flow.~ This additional infiltration air mass flow is not self-balanced, i.e., it is always assumed to be incoming flow which leaves by exahust, mixing, or return. If no infiltration air is required in order to balance the zone air mass flow, then the additional infiltration air mass flow rate is set to zero. For this option, the base infiltration flow is always assumed to be self-balanced (i.e., exfiltration = infiltration) and is not included in the zone air mass flow balance.
+
+\emph{AdjustInfiltrationFlow}: The base infiltration flow may be increased or decreased in order to balance the zone air mass flow. If no infiltration is required to balance the zone air flow, then the base infiltration flow rate is retained and assumed to be self-balanced (i.e., exfiltration = infiltration). If the required infiltration flow rate is negative (exfiltration), then the infiltration flow rate is set to zero and surplus flow in the zone is assumed to leave as exfiltration.
+
+\emph{None}: The base infiltration flow is always assumed to be self-balanced (i.e., exfiltration = infiltration) and is not included in the zone air mass flow balance. No changes are made to the base infiltration flow rate.
+
+\paragraph{Field: Infiltration Balancing Zones}\label{field-infiltration-balancing-zones}
+
+This field allows user to choose which zones are included in infiltration balancing. There are two choices: \emph{MixingSourceZoneOnly} or \emph{AllZones}.
+
+\emph{MixingSourceZonesOnly}: Infiltration balancing is active only in zones which are source zones for mixing and which have a base infiltration object defined.
+
+\emph{AllZones}: Infiltration balance is active in any zone which has a base infiltration object defined.
+
+An IDF example is shown below:
+
+\begin{lstlisting}
+
+ZoneAirMassFlowConservation,
+    Yes,                       !- Adjust Zone Mixing For Zone Air Mass Flow Balance
+    AdjustInfiltrationFlow;    !- Infiltration Balancing Method
+  AllZones;                  !- Infiltration Balancing Zones
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-000}
+
+Current ZoneAirMassFlowConservation output variables (only applicable variables will be generated):
+
+\begin{itemize}
+\item
+  HVAC, Average, Zone Air Mass Balance Supply Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Zone Air Mass Balance Exhaust Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Zone Air Mass Balance Return Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Zone Air Mass Balance Mixing Receiving Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Zone Air Mass Balance Mixing Source Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Zone Infiltration Air Mass Flow Balance Status, {[]}
+\item
+  HVAC, Average, Zone Mass Balance Infiltration Air Mass Flow Rate, {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Zone Air Mass Balance Supply Mass Flow Rate {[}kg/s{]}}\label{zone-air-mass-balance-supply-mass-flow-rate-kgs}
+
+This output variable represents the total supply air mass flow rate of a zone. The value is determined by summing the supply air mass flow rates contributions from all supply air inlet nodes of a zone.
+
+\paragraph{Zone Air Mass Balance Exhaust Mass Flow Rate {[}kg/s{]}}\label{zone-air-mass-balance-exhaust-mass-flow-rate-kgs}
+
+This output variable represents the total exhaust air mass flow rate of a zone. The value is determined by summing the exhaust air mass flow rates contributions from all exhaust air nodes of a zone.
+
+\paragraph{Zone Air Mass Balance Return Mass Flow Rate {[}kg/s{]}}\label{zone-air-mass-balance-return-mass-flow-rate-kgs}
+
+This output variable represents the total return air mass flow rate of a zone. The value is determined by summing the return air mass flow rates contributions from return air nodes of a zone.
+
+\paragraph{Zone Air Mass Balance Mixing Receiving Mass Flow Rate {[}kg/s{]}}\label{zone-air-mass-balance-mixing-receiving-mass-flow-rate-kgs}
+
+This output variable represents the total zone mixing air mass flow rate of a receiving zone from one or more mixing objects. The value is determined by summing the air mass flow contributions from all zone mixing objects connected to a single receiving zone.
+
+\paragraph{Zone Air Mass Balance Mixing Source Mass Flow Rate {[}kg/s{]}}\label{zone-air-mass-balance-mixing-source-mass-flow-rate-kgs}
+
+This output variable represents the total zone mixing source air mass flow rate of a source zone feeding one or more mixing objects. The value is determined by summing the air mass flow contributions from all zone mixing objects connected to a single source zone.
+
+\paragraph{\texorpdfstring{Zone Air Mass Balance Infiltration Status {[]}}{Zone Air Mass Balance Infiltration Status }}\label{zone-air-mass-balance-infiltration-status}
+
+This output variable indicates the status of the infiltration object mass flow rate use for balancing the zone mass flow at each time step. It has values of either \textbf{0} or \textbf{1}.~ If the value of this report variable is \textbf{0} then the zone infiltration object mass flow rate is not used in the zone mass conservation calculation, hence the infiltration rate calculated based on the user specified inputs is manintained and the infiltration rate is assumed as self-balanced for the current timestep.~ If the value is 1 then the zone infiltration object mass flow rate is included in the zone air mass flow balance calculation, hence the user specified infiltration rate is modified and it is considered as incoming flow to the zone, i.e., self-balanced assumption is not valid for this zone and current time step.
+
+\paragraph{Zone Air Mass Balance Infiltration Mass Flow Rate {[}kg/s{]}}\label{zone-air-mass-balance-infiltration-mass-flow-rate-kgs}
+
+This output variable represents the zone infiltration air mass flow rate in kg/s.~ This output variable is reported only for source zones and when the zone air mass flow balance is active. Its value depends on the Infiltration Balancing Method specified.~ When the infiltration method is \emph{AddInfiltrationFlow} this output represents the additional infiltration air mass flow rate added on top of the base infiltration air flow in order to balance the zone air mass flow. In this case, the base infiltration air mass flow calculated using the user specified input is assumed self-balanced.~ When the infiltration method is \emph{AdjustInfiltrationFlow} and the value of ``Zone Air Mass Balance Infiltration Status'' is \textbf{1}, this output represents the infiltration air mass flow rate required to balance the zone air mass flow. This value could be negative if the zone supply exceeds all other outflows. If the value of ``Zone Air Mass Balance Infiltration Status'' is \textbf{0}, then this output is the self-balanced base infiltration flow rate for current timestep.
diff --git a/doc/input-output-reference/src/overview/group-compliance-objects.tex b/doc/input-output-reference/src/overview/group-compliance-objects.tex
new file mode 100644
index 00000000000..67166a90638
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-compliance-objects.tex
@@ -0,0 +1,20 @@
+\section{Group -- Compliance Objects}\label{group-compliance-objects}
+
+Not necessarily related directly to simulation, the Compliance Object group provides a repository for a group of objects that can be used directly or indirectly in reporting compliance (such as ASHRAE 90.1) to building standards.
+
+\subsection{Compliance:Building}\label{compliancebuilding}
+
+The Compliance:Building object describes parameters related to compliance to building standards, building codes, and beyond energy code programs.
+
+\subsubsection{Inputs}\label{inputs-006}
+
+\paragraph{Field: Building Rotation for Appendix G}\label{field-building-rotation-for-appendix-g}
+
+Building Rotation for Appendix G allows for the building model to be rotated for use with compliance such as ASHRAE 90.1 Appendix G. Appendix G requires the building to be rotated 0, 90, 180 and 270 degrees and the values averaged to establish baseline energy use. This input works with relative or world coordinate systems.
+
+An example from an IDF:
+
+\begin{lstlisting}
+Compliance:Building,
+  90;       !- Building Rotation for Appendix G
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-condenser-equipment.tex b/doc/input-output-reference/src/overview/group-condenser-equipment.tex
new file mode 100644
index 00000000000..8ddcb37c43a
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-condenser-equipment.tex
@@ -0,0 +1,3827 @@
+\section{Group -- Condenser Equipment}\label{group-condenser-equipment}
+
+\subsection{Equipment Types}\label{equipment-types}
+
+In each CondenserEquipmentList, various equipment types and names must be given. Each type-name pair must then have a corresponding equipment definition. This subsection lists the various equipment types that are available and examples from an IDF. Where appropriate, notes and comments on the input structure are provided.
+
+\subsection{CoolingTower:SingleSpeed}\label{coolingtowersinglespeed}
+
+Cooling towers are components that may be assigned to condenser loops. The cooling tower is modeled as a counterflow heat exchanger with a single-speed fan (induced draft configuration) based on Merkel's theory. The user must define tower performance via one of two methods: design heat transfer coefficient-area product (UA) and design water flow rate, or nominal tower capacity at a specific rating point. Regardless of which method is chosen, the design airflow rate and corresponding fan power must be specified. The model will also account for tower performance in the ``free convection'' regime, when the tower fan is off but the water pump remains on and heat transfer still occurs (albeit at a low level). If the user wants the model to account for ``free convection'', they must specify the corresponding airflow rate and heat transfer coefficient-area product (UA), or the nominal tower capacity during this mode of operation.
+
+The cooling tower seeks to maintain the temperature of the water exiting the cooling tower at (or below) a set point. The set point schedule value is defined by the field ``Condenser Loop Temperature Setpoint Node Name or Reference'' for the CondenserLoop object. The model first checks to determine the impact of ``free convection'', if specified by the user, on the tower exiting water temperature. If the exiting water temperature based on ``free convection'' is at or below the set point, then the tower fan is not turned on. If the exiting water temperature based on ``free convection'' is below the set point, the tower will operate in FluidBypass mode -- portion of the water goes through the tower media and gets cooled while the remaining water flow gets bypassed, two water flows then mix together trying to meet the water setpoint temperature. If the exiting water temperature remains above the set point after ``free convection'' is modeled, then the tower fan is turned on to reduce the exiting water temperature to the set point. If the capacity control is FanCycling, the model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., tower fan on for the entire simulation timestep and tower fan off for the entire simulation timestep). Cyclic losses are not taken into account. If the capacity control is FluidBypass, the model determines the fraction of water flow to be bypassed while the remaining water goes through the tower cooling media and gets cooled, then the two water flows mix to meet the setpoint temperature. In this case, the fan runs at full speed for the entire timestep.
+
+Cooling towers here are ``wet'' and consume water through evaporation, drift, and blowdown. The model can be used to predict water consumed by the towers. The last six input fields are optional and provide methods of controlling details of the water consumption calculations. The user can specifiy connections to the rest of the buildings water system by providing the name of a water storage tanks (i.e.~WaterUse:Storage objects).
+
+For the operation of multi-cell towers, the first step is to determine the number of cells to operate based on the cell control method -- between the minimum number of cells subject to the maximum water flow rate fraction per cell, and maximum number of cells subject to the minimum water flow rate fraction per cell. If the calculated cells do not meet the loads, additional cells will be operating to help meet the loads. Inside each cell, the existing capacity controls still apply.
+
+For multi-cell towers, the following inputs are assumed to be for the entire tower including all cells:
+
+\begin{itemize}
+\item
+  Design Water Flow Rate; Design Air Flow Rate; Fan Power at Design Air Flow Rate;
+\item
+  Air Flow Rate in Free Convection Regime; Nominal Capacity; Free Convection Capacity
+\item
+  BASIN HEATER (we assume that there is a common basin)
+\end{itemize}
+
+\subsubsection{Inputs}\label{inputs-007}
+
+\paragraph{Field: Name}\label{field-name-006}
+
+This alpha field contains the identifying name for the cooling tower.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name}
+
+This alpha field contains the identifying name for the cooling tower's water inlet node.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name}
+
+This alpha field contains the identifying name for the cooling tower's water outlet node.
+
+\paragraph{Field: Design Water Flow Rate}\label{field-design-water-flow-rate}
+
+This numeric field contains the design water flow rate through the tower in m\(^{3}\)/s. This value is the flow rate of the condenser loop water being cooled by the tower (not the flow rate of water being sprayed on the outside of the heat exchange coil). If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a water flow rate greater than zero must be defined or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections). If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically assumes a water flow rate of 5.382E-8 m3/s per watt (3 gpm/ton) of tower capacity specified in the field ``Nominal Capacity''.
+
+\paragraph{Field: Design Air Flow Rate}\label{field-design-air-flow-rate}
+
+This numeric field contains the design air flow rate induced by the tower fan in m\(^{3}\)/s. A value greater than zero must be defined regardless of the tower performance input method. Alternately, this field can be autosized. If autosized, the design air flow rate is calculated as follows:
+
+\begin{equation}
+Design\;Air\;Flow\;Rate = \frac{{0.5{\rho_{air}}(Fan\;power\;at\;Design\;Air\;Flow\;Rate)}}{{190.}}
+\end{equation}
+
+where a fan pressure rise of 190 Pascals and total fan efficiency of 0.5 are assumed.
+
+\textbf{\emph{Field: Design Fan Power}}
+
+This numeric field contains the fan power (in watts) at the design air flow rate specified in the previous field. A value greater than zero must be specified regardless of the tower performance input method, or this field can be autosized. If autosized, the fan power is calculated as follows:
+
+If``Performance Input Method'' is specified as ``\emph{UFactorTimesAreaAndDesignWaterFlowRate}'', then
+
+\begin{equation}
+Fan\;power = 0.0105\cdot {\rho_{water}}\cdot {C_{p,water}}\cdot Design\;Water\;Flow\;Rate\cdot Design\;Loop\Delta T
+\end{equation}
+
+is used.
+
+If``Performance Input Method'' is specified as ``\emph{NominalCapacity}'', then
+
+\begin{equation}
+Fan\;power = 0.0105\cdot Tower\;Nominal\;Capacity
+\end{equation}
+
+is used.
+
+\paragraph{Field: Design U-Factor Times Area Value}\label{field-design-u-factor-times-area-value}
+
+This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the design air and water flow rates specified above. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design tower UA value is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), assuming a tower water inlet temperature of 35C and tower inlet air at 35C drybulb/25.6C wetbulb. If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field ``Nominal Capacity''.
+
+\paragraph{Field:Free Convection Regime Air Flow Rate}\label{fieldfree-convection-regime-air-flow-rate}
+
+This numeric field contains the air flow rate (m\(^{3}\)/s) when the tower is in the ``free convection'' regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field ``Design Air Flow Rate''. This field may be autocalculated, in which case it is set to a fraction of the ``Design Air Flow Rate'' determined in the following input field. If the user does not wish to model ``free convection'' and is using the Performance Input Method ``UFactorTimesAreaAndDesignWaterFlowRate'', then this field should be set to 0.0. If the user specifies the U-Factor Times Area Value at Free Convection Air Flow Rate or Free Convection Capacity as a value greater than zero, then the free convection air flow rate must be specified greater than 0.0.
+
+\paragraph{Field: Free Convection Regime Air Flow Rate Sizing Factor}\label{field-free-convection-regime-air-flow-rate-sizing-factor}
+
+This numeric field contains the sizing factor to use when calculating the free convection regime air flow rate.~ The default is 0.1.
+
+\paragraph{Field:Free Convection Regine U-Factor Times Area Value}\label{fieldfree-convection-regine-u-factor-times-area-value}
+
+This numeric field contains the heat transfer coefficient-area product (W/K) when the tower is in the ``free convection'' regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field ``U-Factor Times Area Value at Design Air Flow Rate''. This field may be autosized, in which case it is set to a fraction of the ``U-Factor Times Area Value at Design Air Flow Rate'' determined in the following input field. If the user does not wish to model ``free convection'' and is using the~ Performance Input Method ``UFactorTimesAreaAndDesignWaterFlowRate'', then this field should be set to 0.0. If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field ``Free Convection Capacity''.\textbackslash{}
+
+\paragraph{Field: Free Convection U-Factor Times Area Value Sizing Factor}\label{field-free-convection-u-factor-times-area-value-sizing-factor}
+
+This numeric field contains the sizing factor to use when calculating the free convection regime U-Factor times area value.~ The default is 0.1.
+
+\paragraph{Field: Performance Input Method}\label{field-performance-input-method}
+
+This alpha field contains the method by which the user will specify tower performance: ``\textbf{UFactorTimesAreaAndDesignWaterFlowRate}'' or ``\textbf{NominalCapacity}''. If this field is left blank in the input data file, the default input method is assumed to be ``\textbf{UFactorTimesAreaAndDesignWaterFlowRate}''. If the method ``\textbf{UFactorTimesAreaAndDesignWaterFlowRate}'' is selected, then the user must enter design UA values, design water flow rates and air flow rates as described for the previous input fields. If the method ``NominalCapacity'' is selected then the fields ``Design Water Flow Rate'', ``U-Factor Times Area Value at Design Air Flow Rate'' and ``U-Factor Times Area Value at Free Convection Air Flow Rate'' must be left blank, but the fields ``Nominal Capacity'' and ``Free Convection Capacity'' must be entered as described below.
+
+\paragraph{Field: Heat Rejection Capacity and Nominal Capacity Sizing Ratio}\label{field-heat-rejection-capacity-and-nominal-capacity-sizing-ratio}
+
+This numeric field contains the value for the ratio of actual tower heat rejection to nominal capacity.~ This ratio is defined at entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. Historically this ratio has been set at 1.25 based on the assumption that the tower must dissipate 0.25 W of compressor power for every what of heat removed at the chiller evaporator.~ The default is 1.25.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity}
+
+This numeric input field contains the ``nominal'' heat rejection capacity of the cooling tower in watts, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of nominal capacity (3 gpm/ton). The value in the previous field times this nominal tower capacity gives the actual tower heat rejection at these operating conditions (based on historical assumption that the tower must dissipate additional heat from the compressor heat for heat removed at the evaporator).
+
+\paragraph{Field: Free Convection Capacity}\label{field-free-convection-capacity}
+
+This numeric input field contains the ``nominal'' heat rejection capacity of the cooling tower in watts when the tower is in the ``free convection'' regime (water flow exists but tower fan is turned off), with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of nominal tower capacity (input field above). The heat rejection capacity and nominal capacity sizing ratio is applied tof this free convection tower capacity to give the actual tower heat rejection at these operating conditions (typical value is 1.25 based on historical assumption that the tower must dissipate 0.25W of compressor heat for every watt of heat removed by the evaporator). The value specified for this field must be less than the value specified for the field ``Tower Nominal Capacity''. If the user does not wish to model ``free convection'', then this field should be set to 0.0. If the user specifies a value greater than zero, then the ``Air Flow Rate in Free Convection Regime'' field must contain a value greater than zero. This field can be automatically calculated using the sizing factor in the following field.
+
+\paragraph{Field: Free Convection Nominal Capacity Sizing Factor}\label{field-free-convection-nominal-capacity-sizing-factor}
+
+This numeric field contains the sizing factor to use when calculating the Free Convection Capacity. The default is 0.1.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity}
+
+This numeric field contains the capacity of the tower's electric basin heater in watts per degree Kelvin. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the tower fan is off and water is not flowing through the tower, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the tower fan is off and water is not flowing through the tower. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name}
+
+This alpha field contains the name of the basin heater operating schedule. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the cooling tower fan is off and water is not flowing through the tower.
+
+\paragraph{Field: Evaporation Loss Mode}\label{field-evaporation-loss-mode}
+
+This field is used to choose which method is used to model the amount of water evaporated by the cooling tower. There are two options: \textbf{LossFactor} or \textbf{SaturatedExit}. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the tower is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the cooling tower model (and does not require additional user input).
+
+\paragraph{Field: Evaporation Loss Factor}\label{field-evaporation-loss-factor}
+
+This field is used to specify the rate of water evaporated from the cooling tower and lost to the outside air {[}percent/K{]}. This field is only used if the Evaporation Calculation Mode is set to \textbf{LossFactor}. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-degree Kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Typical values are from 0.15 to 0.27 {[}percent/K{]}. The default is 0.2.
+
+\paragraph{Field: Drift Loss Percent}\label{field-drift-loss-percent}
+
+This field is used to specify the rate of water lost to the exiting air as entrained droplets {[}\%{]}. The drift loss is a percent of the condenser water flow. Typical values for towers with efficient drift eliminators are between 0.002 and 0.2\% of the condenser water flow rate. The default value is 0.008\%.
+
+\paragraph{Field: Blowdown Calculation Mode}\label{field-blowdown-calculation-mode}
+
+This field specifies which method is used to determine blowdown rates. There two options \textbf{ConcentrationRatio} or \textbf{ScheduledRate}. The choice will determine which of the two models below is used. The default is ConcentrationRatio.
+
+\paragraph{Field: Blowdown Concentration Ratio}\label{field-blowdown-concentration-ratio}
+
+This field is used to dynamically adjust the rate of blowdown in the cooling tower as a function of the rate of evaporation. Blowdown is water intentionally drained from the tower in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values for tower operation are 3 to 5. The default value is 3.
+
+\paragraph{Field: Blowdown Makeup Water Usage Schedule Name}\label{field-blowdown-makeup-water-usage-schedule-name}
+
+This alpha field contains the name of the schedule used to define the amount of water (m\(^{3}\)/s) flushed from the basin on a periodic basis to purge the tower of mineral scale build-up and other contaminants. This schedule is only used if the Blowdown Calculation Mode is set to ScheduledRate. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Typical values range from 0.0002 to 0.0013 m\(^{3}\)/s (17.3 to 112.3 m\(^{3}\)/day). This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the cooling tower is active and water is flowing through the tower (regardless of the water usage defined by this schedule).
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name}
+
+This field is optional. It is used to describe where the tower obtains water used for evaporative cooling. If blank or omitted, then the tower will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the tower will obtain its water from that tank. If a tank is specified, the tower will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the tower needs, then the tower will still operate and obtain the rest of the water it needs from the mains (referred to as `Starved' water).
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-000}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the cooling tower. If this field is left blank, the outdoor air conditions entering the cooling tower are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+\paragraph{Field:Capacity Control}\label{fieldcapacity-control}
+
+This alpha field contains the cooling capacity control for the cooling tower. Two choices are available: \textbf{FanCycling} and \textbf{FluidBypass}. During part-load conditions, there are two ways to maintain the exiting water temperature at the setpoint: either cycling the tower fan, or bypassing portion of the tower water with a three-way valve. For FluidBypass, the tower fan still runs at full speed for the entire timestep, but only portion of the water flow goes through the cooling tower media to get cooled while the remaining portion of the water flow gets bypassed. Two water flows then mix at the common water sump to meet the setpoint temperature.
+
+\paragraph{Field: Number of Cells}\label{field-number-of-cells}
+
+This integer field contains the number of cells in the multi-cell cooling tower. If not entered, the program will assume it is a single-cell cooling tower
+
+\paragraph{Field: Cell Control}\label{field-cell-control}
+
+This alpha field specifies the method used to control the number of cells used to meet the load, the two choices are:
+
+\textbf{MinimalCell} : the program will use minimal number of cells needed, all other cells will be shut down with no water flow. It will attempt to use as few cells as possible to cool the fluid. In no case, however, will the flow per cell be allowed to exceed its maximum value defined by the \emph{Maximum Water Flow Rate Fraction.}
+
+\textbf{MaximalCell}: As many cells as possible will be turned on. In no case, however, will the flow per cell be allowed to drop below its minimum value specified by the \emph{Minimum Water Flow Rate Fraction}.
+
+\paragraph{Field: Cell Minimum Water Flow Rate Fraction}\label{field-cell-minimum-water-flow-rate-fraction}
+
+This numeric field specifies the allowable smallest fraction of the design water flow rate. Flows less than this value will commonly result in fluid distribution problems; the pressure at each nozzle will be too weak for the fluid to be sprayed out in the correct pattern, not all the fill would be wet. If this field is left blank, the default value is 0.33.
+
+\paragraph{Field: Cell Maximum~ Water Flow Rate Fraction}\label{field-cell-maximum-water-flow-rate-fraction}
+
+This numeric field specifies the allowable largest fraction of the design water flow rate. If this field is left blank, the default value is 2.5.
+
+\textbf{\emph{Field: Sizing Factor}}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature. For this component the inputs that would be altered by the sizing factor are:
+
+1.~~~~Design Water Flow Rate;
+
+2.~~~~Design Air Flow Rate;
+
+3.~~~~Fan Power at Design Air Flow Rate;
+
+4.~~~~U-Factor Times Area Value at Design Air Flow Rate;
+
+5.~~~~Air Flow Rate in Free Convection Regime;
+
+6.~~~~U-Factor Times Area Value at Free Convection Air Flow Rate.
+
+Note that the U-Factor Times Area Value at Design Air Flow Rate is not \emph{multiplied} by the Sizing Factor. Instead the design tower load is multiplied by the sizing factor and the design UA then calculated as usual. The U-Factor Times Area Value at Free Convection Air Flow Rate is set to 10\% of the new design Tower UA.
+
+Three examples of an IDF specification for this object are shown below:
+
+\begin{lstlisting}
+
+CoolingTower:SingleSpeed,
+    My Tower,                     !- Name
+    Condenser Tower Inlet Node,   !- Water Inlet Node Name
+    Condenser Tower Outlet Node,  !- Water Outlet Node Name
+    .0011,                        !- Design Water Flow Rate (m3/s)
+    16.0,                         !- Design Air Flow Rate (m3/s)
+    10000.,                       !- Fan Power at Design Air Flow Rate (W)
+    3500.,  !- U-Factor Times Area Value at Design Air Flow Fate (W/C)
+    0.0,    !- Air Flow Rate in Free Convection Regime (m3/s)
+    0.0,    !- U-Factor Times Area Value at Free Convection Air Flow Rate (W/C)
+    UFactorTimesAreaAndDesignWaterFlowRate,!- Performance Input Method
+    ,                             !- Nominal Capacity (W)
+    ,                             !- Free Convection Capacity (W)
+    ,                             !- Basin Heater Capacity {W/K}
+    ,                             !- Basin Heater Setpoint Temperature {C}
+    ,                             !- Basin Heater Operating Schedule Name
+    ,                             !- Evaporation Loss Mode
+    ,                             !- Evaporation Loss Factor (percent/K)
+    ,                             !- Drift Loss Percent (percent)
+    ,                             !- Blowdown Calculation Mode
+    ,                             !- Blowdown Concentration Ratio
+    ,                             !- Blowdown Makeup Water Usage Schedule Name
+    ,                             !- Supply Water Storage Tank Name
+    ,                             !- Outdoor Air Inlet Node Name
+    FluidBypass,                  !- Capacity Control
+    4,                            !- Number of Cells
+    MinimalCell,                  !- Cell Control
+    0.25,                         !- Cell Minimum Water Flow Rate Fraction
+    1.50;                         !- Cell Maximum Water Flow Rate Fraction
+
+
+  CoolingTower:SingleSpeed,
+    My Tower,                   !- Name
+    Condenser Tower Inlet Node, !- Water Inlet Node Name
+    Condenser Tower Outlet Node,!- Water Outlet Node Name
+    ,                           !- Design Water Flow Rate (m3/s)
+    autosize,                   !- Design Air Flow Rate (m3/s)
+    1000.,                      !- Fan Power at Design Air Flow Rate (W)
+    ,                !- U-Factor Times Area Value at Design Air Flow Fate (W/C)
+    autosize,        !- Air Flow Rate in Free Convection Regime (m3/s)
+    ,       !- U-Factor Times Area Value at Free Convection Air Flow Rate (W/C)
+    NominalCapacity,            !- Performance Input Method
+    95250.,                     !- Nominal Capacity (W)
+    9525.;                      !- Free Convection Capacity (W)
+
+
+  CoolingTower:SingleSpeed,
+      TowerWaterSys CoolTower, !- Name
+      TowerWaterSys Pump-TowerWaterSys CoolTowerNode,  !- Water Inlet Node Name
+      TowerWaterSys Supply Equipment Outlet Node,  !- Water Outlet Node Name
+      AUTOSIZE,                !- Design Water Flow Rate {m3/s}
+      AUTOSIZE,                !- Design Air Flow Rate {m3/s}
+      AUTOSIZE,                !- Fan Power at Design Air Flow Rate {W}
+      AUTOSIZE,   !- U-Factor Times Area Value at Design Air Flow Rate {W/K}
+      AUTOSIZE,   !- Air Flow Rate in Free Convection Regime {m3/s}
+      AUTOSIZE,   !- U-Factor Times Area at Free Convection Air Flow Rate {W/K}
+      UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
+      ,                        !- Nominal Capacity {W}
+      ,                        !- Free Convection Capacity {W}
+      ,                        !- Basin Heater Capacity {W/K}
+      ,                        !- Basin Heater Setpoint Temperature {C}
+      ,                        !- Basin Heater Operating Schedule Name
+      SaturatedExit,           !- Evaporation Loss Mode
+      ,                        !- Evaporation Loss Factor {percent/K}
+      0.0080,                  !- Drift Loss Percent {percent}
+      ConcentrationRatio,      !- Blowdown Calculation Mode
+      3.0000,                  !- Blowdown Concentration Ratio
+      ,                        !- Blowdown Makeup Water Usage Schedule Name
+      ,                        !- Supply Water Storage Tank Name
+      TowerWaterSys CoolTowerOA ref Node,  !- Outdoor Air Inlet Node Name
+      FanCycling,              !- Capacity Control
+      4,                       !- Number of Cells
+      MinimalCell,             !- Cell Control
+      0.25,                    !- Cell Minimum Water Flow Rate Fraction
+      1.50,                    !- Cell Maximum Water Flow Rate Fraction
+      1.0000;                  !- Sizing Factor
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-004}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Tower Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Tower Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Cooling Tower Bypass Fraction {[]}
+\item
+  HVAC,Average,Cooling Tower Fan Cycling Ratio {[]}
+\item
+  HVAC,Average,Cooling Tower Operating Cells Count {[]}
+\end{itemize}
+
+A tower uses either mains water or storage tank for make-up water.
+
+\emph{When mains water is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate~ {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\emph{When storage tank water is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate~ {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Mains Water Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Evaporation Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Drift Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Blowdown Volume {[}m3{]}
+\end{itemize}
+
+IF specified:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Cooling Tower Fan Electric Power {[}W{]}}\label{cooling-tower-fan-electric-power-w}
+
+\paragraph{Cooling Tower Fan Electric Energy {[}J{]}}\label{cooling-tower-fan-electric-energy-j}
+
+These outputs are the electric power input to the tower fans. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Cooling Tower Heat Transfer Rate {[}W{]}}\label{cooling-tower-heat-transfer-rate-w}
+
+This is the rate at which heat is removed from the condenser water loop by the tower.
+
+\paragraph{Cooling Tower Inlet Temperature {[}C{]}}\label{cooling-tower-inlet-temperature-c}
+
+\paragraph{Cooling Tower Outlet Temperature {[}C{]}}\label{cooling-tower-outlet-temperature-c}
+
+\paragraph{Cooling Tower Mass Flow Rate {[}kg/s{]}}\label{cooling-tower-mass-flow-rate-kgs}
+
+These outputs are the tower water inlet and outlet temperatures, and mass flow rate of the circulating condenser water loop.
+
+\paragraph{Cooling Tower Basin Heater Electric Power {[}W{]}}\label{cooling-tower-basin-heater-electric-power-w}
+
+\paragraph{Cooling Tower Basin Heater Electric Energy {[}J{]}}\label{cooling-tower-basin-heater-electric-energy-j}
+
+These outputs are the electric power input to the tower basin heater. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility
+
+\paragraph{Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-make-up-water-volume-flow-rate-m3s}
+
+\paragraph{Cooling Tower Make Up Water Volume {[}m3{]}}\label{cooling-tower-make-up-water-volume-m3}
+
+These outputs are the water consumed by the wet cooling tower for external water sprays used to augment heat transfer. This is the total of evaporation, drift, and blowdown.
+
+\paragraph{Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-evaporation-volume-flow-rate-m3s}
+
+\paragraph{Cooling Tower Water Evaporation Volume {[}m3{]}}\label{cooling-tower-water-evaporation-volume-m3}
+
+\paragraph{Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-drift-volume-flow-rate-m3s}
+
+\paragraph{Cooling Tower Water Drift Volume {[}m3{]}}\label{cooling-tower-water-drift-volume-m3}
+
+\paragraph{Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-blowdown-volume-flow-rate-m3s}
+
+\paragraph{Cooling Tower Water Blowdown Volume {[}m3{]}}\label{cooling-tower-water-blowdown-volume-m3}
+
+These outputs provide the breakdown of the different components of water use during cooling tower operation.
+
+\paragraph{Cooling Tower Make Up Mains Water Volume {[}m3{]}}\label{cooling-tower-make-up-mains-water-volume-m3}
+
+This is the volume of water drawn from mains service to feed the cooling tower.
+
+If a water storage tank is used to provide water to the tower, then the following output variables will also be available.
+
+\paragraph{Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-storage-tank-water-volume-flow-rate-m3s}
+
+\paragraph{Cooling Tower Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-storage-tank-water-volume-m3}
+
+These are the rate and volume of water provided by the Water Storage Tank.
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-starved-storage-tank-water-volume-flow-rate-m3s}
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-starved-storage-tank-water-volume-m3}
+
+These are the rate and volume of water the Storage Tank connections was not able to provide. The starved water is assumed to come from the mains. The tower's operation is not affected by a lack of storage tank water.
+
+\paragraph{\texorpdfstring{Cooling Tower Fan Cycling Ratio {[]}}{Cooling Tower Fan Cycling Ratio }}\label{cooling-tower-fan-cycling-ratio}
+
+This represents the fraction of a time-step when tower fan is on.
+
+\paragraph{\texorpdfstring{Cooling Tower Bypass Fraction {[]}}{Cooling Tower Bypass Fraction }}\label{cooling-tower-bypass-fraction}
+
+This represents the fraction of a fluid bypassing the tower when a mixture of the tower fluid and tower return water is able to meet the set point temperature.
+
+\paragraph{\texorpdfstring{Cooling Tower Operating Cells Count {[]}}{Cooling Tower Operating Cells Count }}\label{cooling-tower-operating-cells-count}
+
+This represents the number of cells operating at each time step.
+
+\subsection{CoolingTower:TwoSpeed}\label{coolingtowertwospeed}
+
+The two-speed cooling tower is modeled in a similar fashion to the single-speed tower. The cooling tower is modeled as a counterflow heat exchanger with a two-speed fan (induced draft configuration) based on Merkel's theory. The user must define tower performance via one of two methods: heat transfer coefficient-area product (UA) and design water flow rate, or nominal tower capacity at a specific rating point. Regardless of which method is chosen, the airflow rate and corresponding fan power at both high and low fan speed must be specified. The model will also account for tower performance in the ``free convection'' regime, when the tower fan is off but the water pump remains on and heat transfer still occurs (albeit at a low level). If the user wants the model to account for ``free convection'', they must specify the corresponding air flow rate and heat transfer coefficient-area product (UA), or the nominal tower capacity during this mode of operation.
+
+The cooling tower seeks to maintain the temperature of the water exiting the cooling tower at (or below) a set point. The set point schedule value is defined by the field ``Condenser Loop Temperature Setpoint Node Name or Reference'' for the CondenserLoop object. The model first checks to determine the impact of ``free convection'', if specified by the user, on the tower exiting water temperature. If the exiting water temperature based on ``free convection'' is at or below the set point, then the tower fan is not turned on. If the exiting water temperature remains above the set point after ``free convection'' is modeled, then the tower fan is turned on at low speed to reduce the exiting water temperature. If operating the tower fan at low speed does not reduce the exiting water temperature to the set point, then the tower fan is increased to its high speed.
+
+The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., tower fan at high speed for the entire simulation timestep and tower fan at low speed for the entire simulation timestep, or tower fan at low speed for the entire simulation timestep and tower fan off for the entire simulation timestep). Cyclic losses are not taken into account.
+
+Cooling towers here are ``wet'' and consume water through evaporation, drift, and blowdown. The model can be used to predict water consumed by the towers. The last six input fields are optional and provide methods of controlling details of the water consumption calculations. The user can specifiy connections to the rest of the buildings water system by providing the name of a WaterUse:Storage object.
+
+For the operation of multi-cell towers, the first step is to determine the number of cells to operate based on the cell control method -- between the minimum number of cells subject to the maximum water flow rate fraction per cell, and maximum number of cells subject to the minimum water flow rate fraction per cell. If the calculated cells do not meet the loads, additional cells will be operating to help meet the loads. Inside each cell, the existing capacity controls still apply.
+
+For multi-cell towers, the following inputs are assumed to be for the entire tower including all cells:
+
+\begin{itemize}
+\item
+  Design Water Flow Rate; Design Air Flow Rate; Fan Power at Design Air Flow Rate;
+\item
+  Air Flow Rate in Free Convection Regime; Nominal Capacity; Free Convection Capacity
+\item
+  BASIN HEATER (we assume that there is a common basin)
+\end{itemize}
+
+\textbf{\emph{Field: Name}}
+
+This alpha field contains the identifying name for the cooling tower.
+
+\subsubsection{Inputs}\label{inputs-1-006}
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-1}
+
+This alpha field contains the identifying name for the cooling tower's water inlet node.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-1}
+
+This alpha field contains the identifying name for the cooling tower's water outlet node.
+
+\paragraph{Field: Design Water Flow Rate}\label{field-design-water-flow-rate-1}
+
+This numeric field contains the design water flow rate through the tower in m\(^{3}\)/s. This value is the flow rate of the condenser loop water being cooled by the tower (not the flow rate of water being sprayed on the outside of the heat exchange coil). If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a water flow rate greater than zero must be defined or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections). If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically assumes a design water flow rate of 5.382E-8 m3/s per watt (3 gpm/ton) of tower capacity specified in the field ``Tower High-Speed Nominal Capacity''.
+
+\paragraph{Field: High Fan Speed Air Flow Rate}\label{field-high-fan-speed-air-flow-rate}
+
+This numeric field contains the tower air flow rate at high fan speed in m\(^{3}\)/s. A value greater than zero must be defined regardless of the tower performance input method. Alternately, this field can be autosized. If autosized, the design air flow rate is calculated as follows:
+
+\begin{equation}
+Air\,Flow\,Rate\,at\,High\,Fan\,Speed\, = \,\frac{{0.5{\rho_{air}}(Fan\,Power\,at\,High\,Fan\,Speed\,)}}{{190.}}
+\end{equation}
+
+where a fan pressure rise of 190 Pascals and total fan efficiency of 0.5 are assumed.
+
+\textbf{\emph{Field: High Fan Speed Fan Power}}
+
+This numeric field contains the fan power (in Watts) at the high-speed air flow rate specified in the previous field. A value greater than zero must be specified regardless of the tower performance input method, or this field can be autosized. If autosized, the fan power is calculated as follows:
+
+If``Performance Input Method'' is specified as ``\emph{UFactorTimesAreaAndDesignWaterFlowRate}'', then
+
+\begin{equation}
+Fan\;powe{r_{High\;Fan\;Speed}} = 0.0105\cdot {\rho_{water}}\cdot {C_{p,water}}\cdot Design\;Water\;Flow\;Rate\cdot Design\;Loop\Delta T
+\end{equation}
+
+is used.
+
+If``Performance Input Method'' is specified as ``\emph{NominalCapacity}'', then
+
+\begin{equation}
+Fan\;powe{r_{High\;Fan\;Speed}} = 0.0105\cdot Tower\;High - Speed\;Nominal\;Capacity
+\end{equation}
+
+is used.
+
+\paragraph{Field: High Fan Speed U-Factor Times Area Value}\label{field-high-fan-speed-u-factor-times-area-value}
+
+This numeric field contains the heat transfer coefficient-area product (UA) in watts per degree Celsius corresponding to the high-speed air flow rate and design water flow rate specified above. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the tower UA value at high fan speed is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), assuming a tower water inlet temperature of 35C and tower inlet air at 35C drybulb/25.6C wetbulb. If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically calculates the tower UA based on the capacity specified in the field ``High-Speed Nominal Capacity''.
+
+\paragraph{Field: Low Fan Speed Air Flow Rate}\label{field-low-fan-speed-air-flow-rate}
+
+This numeric field contains the tower air flow rate at low fan speed in m\(^{3}\)/s. This value must be greater than zero, less than the value specified for the field ``Air Flow Rate at High Fan Speed'', and greater than the value specified for the field ``Air Flow Rate in Free Convection Regime''. This field may be autocalculated, in which case it is set to a fraction of the ``Air Flow Rate at High Fan Speed'' determined in the next field.
+
+\paragraph{Field: Low Fan Speed Air Flow Rate Sizing Factor}\label{field-low-fan-speed-air-flow-rate-sizing-factor}
+
+This numeric field contains the sizing factor to use when calculating the low fan speed air flow rate.~ The default is 0.5.
+
+\paragraph{Field: Low Fan Speed Fan Power}\label{field-low-fan-speed-fan-power}
+
+This numeric field contains the fan power (in Watts) at the low-speed air flow rate specified in the previous field. This value must be specified greater than zero or the field may be autocalculated, in which case it is set to a fraction of the ``Fan Power at High Fan Speed'' determined in the next field.
+
+\paragraph{Field: Low Fan Speed Fan Power Sizing Factor}\label{field-low-fan-speed-fan-power-sizing-factor}
+
+This numeric field contains the sizing factor to use when calculating the low speed fan power.~ The default is 0.16.
+
+\paragraph{Field: Low Fan Speed U-Factor Times Area Value}\label{field-low-fan-speed-u-factor-times-area-value}
+
+This numeric field contains the heat transfer coefficient-area product (UA) in watts per degree Celsius corresponding to the design water flow rate and low-speed air flow rate specified above. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', this value must be greater than zero but less than or equal to 300,000, less than the value specified for the field ``U-Factor Times Area Value at High Fan Speed'', and greater than the value specified for the field ``U-Factor Times Area Value at Free Convection Air Flow Rate''. This field may be autocalculated, in which case it is set to a fraction of the ``U-Factor Times Area Value at High Fan Speed'' determined in the following field. If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field ``Low Speed Nominal Capacity''.
+
+\paragraph{Field: Low Fan Speed U-Factor Times Area Sizing Factor}\label{field-low-fan-speed-u-factor-times-area-sizing-factor}
+
+This numeric field contains the sizing factor to use when calculating the low speed heat transfer coefficient-area product (UA).~ The default is 0.6.
+
+\paragraph{Field: Free Convection Regime Air Flow Rate}\label{field-free-convection-regime-air-flow-rate}
+
+This numeric field contains the air flow rate (m\(^{3}\)/s) when the tower is in the ``free convection'' regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field ``Air Flow Rate at Low Fan Speed''. This field may be autocalculated, in which case it is set to a fraction of the ``Air Flow Rate at High Fan Speed'' determined in the following field. If the user does not wish to model ``free convection'' and is using the Performance Input Method ``UFactorTimesAreaAndDesignWaterFlowRate'', then this field should be set to 0.0. If the user specifies the U-Factor Times Area Value at Free Convection Air Flow Rate or Free Convection Capacity as a value greater than zero, then the free convection air flow rate must be specified greater than 0.0.
+
+\paragraph{Field: Free Convection Air Flow Rate Sizing Factor}\label{field-free-convection-air-flow-rate-sizing-factor}
+
+This numeric field contains the sizing factor to use when calculating the free convection regime air flow rate.~ The default is 0.1.
+
+\paragraph{Field: Free ConvectionU-Factor Times Area Value}\label{field-free-convectionu-factor-times-area-value}
+
+This numeric field contains the heat transfer coefficient-area product (W/°C) when the tower is in the ``free convection'' regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field ``U-Factor Times Area Value at Low Fan Speed''. This field may be autocalculated, in which case it is set to a fraction of the ``U-Factor Times Area Value at High Fan Speed'' determined in the following field. If the user does not wish to model ``free convection'' and is using the Performance Input Method ``UFactorTimesAreaAndDesignWaterFlowRate'', then this field should be set to 0.0. If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field ``Free Convection Capacity''.
+
+\paragraph{Field: Free Convection U-Factor Times Area Value Sizing Factor}\label{field-free-convection-u-factor-times-area-value-sizing-factor-1}
+
+This numeric field contains the sizing factor to use when calculating the free convection regime U-Factor times area value.~ The default is 0.1.
+
+\paragraph{Field: Performance Input Method}\label{field-performance-input-method-1}
+
+This alpha field contains the method by which the user will specify tower performance: ``UFactorTimesAreaAndDesignWaterFlowRate'' or ``NominalCapacity''. If this field is left blank in the input data file, the default input method is assumed to be ``UFactorTimesAreaAndDesignWaterFlowRate''. If the method ``UFactorTimesAreaAndDesignWaterFlowRate'' is selected, then the user must enter UA values, design water flow rate and air flow rates as described for the previous input fields. If the method ``NominalCapacity'' is selected then the fields ``Design Water Flow Rate'', ``U-Factor Times Area Value at High Fan Speed'', ``U-Factor Times Area Value at Low Fan Speed'' and ``U-Factor Times Area Value at Free Convection Air Flow Rate'' must be left blank, but the fields ``High Speed Nominal Capacity'', ``Low Speed Nominal Capacity'' and ``Free Convection Capacity'' must be entered as described below.
+
+\paragraph{Field: Heat Rejection Capacity and Nominal Capacity Sizing Ratio}\label{field-heat-rejection-capacity-and-nominal-capacity-sizing-ratio-1}
+
+This numeric field contains the value for the ratio of actual tower heat rejection to nominal capacity.~ This ratio is defined at entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. Historically this ratio has been set at 1.25 based on the assumption that the tower must dissipate 0.25 W of compressor power for every what of heat removed at the chiller evaporator.~ The default is 1.25.
+
+\paragraph{Field: High Speed Nominal Capacity}\label{field-high-speed-nominal-capacity}
+
+This numeric input field contains the ``nominal'' heat rejection capacity of the cooling tower in watts under high-speed fan operation, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of high-speed nominal capacity (3 gpm/ton). The Heat Rejection Capacity and Nominal Capacity Sizing Ratio set in the previous field is applied to this nominal tower capacity to give the actual tower heat rejection at these operating.
+
+\paragraph{Field: Low Speed Nominal Capacity}\label{field-low-speed-nominal-capacity}
+
+This numeric input field contains the ``nominal'' heat rejection capacity of the cooling tower in watts under low-speed fan operation, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of high-speed nominal tower capacity (input field above). The Heat Rejection Capacity and Nominal Capacity Sizing Ratio is applied to this nominal tower capacity to give the actual tower heat rejection at these operating conditions. The value specified for this field must be greater than zero but less than the value specified for the field ``High-Speed Nominal Capacity''.~ This field may be autocalculated, in which case it is set to a fraction of the High Speed Nominal Capacity determined in the following field.
+
+\paragraph{Field: Low Speed Nominal Capacity Sizing Factor}\label{field-low-speed-nominal-capacity-sizing-factor}
+
+This numeric field contains the sizing factor to use when calculating the Low Speed Nominal Capacity. The default is 0.5.
+
+\paragraph{Field: Free Convection Capacity}\label{field-free-convection-capacity-1}
+
+This numeric input field contains the ``nominal'' heat rejection capacity of the cooling tower in watts when the tower is in the ``free convection'' regime (water flow exists but tower fan is turned off), with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of high-speed nominal tower capacity (input field above). The Heat Rejection Capacity and Nominal Capacity Sizing Ratio is applied to this free convection tower capacity to give the actual tower heat rejection at these operating conditions.The value specified for this field must be less than the value specified for the field ``Tower Low-Speed Nominal Capacity''. If the user does not wish to model ``free convection'', then this field should be set to 0.0. If the user specifies a value greater than zero, then the ``Air Flow Rate in Free Convection Regime'' field must contain a value greater than zero. This field may be autocalculated, in which case it is set to a fraction of the High Speed Nominal Capacity determined in the following field.
+
+\paragraph{Field: Free Convection Nominal Capacity Sizing Factor}\label{field-free-convection-nominal-capacity-sizing-factor-1}
+
+This numeric field contains the sizing factor to use when calculating the Free Convection Capacity. The default is 0.1.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-1}
+
+This numeric field contains the capacity of the tower's electric basin heater in watts per degree Kelvin. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the tower fan is off and water is not flowing through the tower, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-1}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the tower fan is off and water is not flowing through the tower. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-1}
+
+This alpha field contains the name of the basin heater operating schedule. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the cooling tower fan is off and water is not flowing through the tower.
+
+\paragraph{Field: Evaporation Loss Mode}\label{field-evaporation-loss-mode-1}
+
+This field is used to choose which method is used to model the amount of water evaporated by the cooling tower. There are two options: `LossFactor' or `SaturatedExit'. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the tower is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the cooling tower model (and does not require additional user input).
+
+\paragraph{Field: Evaporation Loss Factor}\label{field-evaporation-loss-factor-1}
+
+This field is used to specify the rate of water evaporated from the cooling tower and lost to the outside air {[}percent/K{]}. This field is only used if the Evaporation Calculation Mode is set to LossFactor. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-degree Kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Typical values are from 0.15 to 0.27 {[}percent/K{]}. The default is 0.2.
+
+\paragraph{Field: Drift Loss Percent}\label{field-drift-loss-percent-1}
+
+This field is used to specify the rate of water lost to the exiting air as entrained droplets {[}\%{]}. The drift loss is a percent of the condenser water flow. Typical values for towers with efficient drift eliminators are between 0.002 and 0.2\% of the condenser water flow rate. The default value is 0.008\%.
+
+\paragraph{Field: Blowdown Calculation Mode}\label{field-blowdown-calculation-mode-1}
+
+This field specifies which method is used to determine blowdown rates. There two options ConcentrationRatio or ScheduledRate. The choice will determine which of the two models below is used. The default is ConcentrationRatio
+
+\paragraph{Field: Blowdown Concentration Ratio}\label{field-blowdown-concentration-ratio-1}
+
+This field is used to dynamically adjust the rate of blowdown in the cooling tower as a function of the rate of evaporation. Blowdown is water intentionally drained from the tower in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values for tower operation are 3 to 5. The default value is 3.
+
+\paragraph{Field: Blowdown Makeup Water Usage Schedule Name}\label{field-blowdown-makeup-water-usage-schedule-name-1}
+
+This alpha field contains the name of the schedule used to define the amount of water (m\(^{3}\)/s) flushed from the basin on a periodic basis to purge the tower of mineral scale build-up and other contaminants. This schedule is only used if the Blowdown Calculation mode is set to ScheduledRate. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Typical values range from 0.0002 to 0.0013 m\(^{3}\)/s (17.3 to 112.3 m\(^{3}\)/day). This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the cooling tower is active and water is flowing through the tower (regardless of the water usage defined by this schedule).
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-1}
+
+This field is optional. It is used to describe where the tower obtains water used for evaporative cooling. If blank or omitted, then the tower will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the tower will obtain its water from that tank. If a tank is specified, the tower will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the tower needs, then the tower will still operate and obtain the rest of the water it needs from the mains (referred to as `Starved' water).
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-1}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the cooling tower. If this field is left blank, the outdoor air conditions entering the cooling tower are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+\paragraph{Field: Number of Cells}\label{field-number-of-cells-1}
+
+This integer field contains the number of cells in the multi-cell cooling tower. If not entered, the program will assume it is a single-cell cooling tower
+
+\paragraph{Field: Cell Control}\label{field-cell-control-1}
+
+This alpha field specifies the method used to control the number of cells used to meet the load, the two choices are:
+
+\textbf{MinimalCell}: the program will use minimal number of cells needed, all other cells will be shut down with no water flow. It will attempt to use as few cells as possible to cool the fluid. In no case, however, will the flow per cell be allowed to exceed its maximum value defined by the \emph{Maximum Water Flow Rate Fraction.}
+
+\textbf{MaximalCell}: As many cells as possible will be turned on. In no case, however, will the flow per cell be allowed to drop below its minimum value specified by the \emph{Minimum Water Flow Rate Fraction}.
+
+\paragraph{Field: Cell Minimum Water Flow Rate Fraction}\label{field-cell-minimum-water-flow-rate-fraction-1}
+
+This numeric field specifies the allowable smallest fraction of the design water flow rate. Flows less than this value will commonly result in fluid distribution problems; the pressure at each nozzle will be too weak for the fluid to be sprayed out in the correct pattern, not all the fill would be wet. If this field is left blank, the default value is 0.33.
+
+\paragraph{Field: Cell Maximum~ Water Flow Rate Fraction}\label{field-cell-maximum-water-flow-rate-fraction-1}
+
+This numeric field specifies the allowable largest fraction of the design water flow rate. If this field is left blank, the default value is 2.5.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.For this component the inputs that would be altered by the sizing factor are:
+
+1.~~~~Design Water Flow Rate;
+
+2.~~~~Air Flow Rate at High Fan Speed;
+
+3.~~~~Fan Power at High Fan Speed;
+
+4.~~~~U-Factor Times Area Value at High Fan Speed;
+
+5.~~~~Air Flow Rate at Low Fan Speed;
+
+6.~~~~Fan Power at Low Fan Speed;
+
+7.~~~~U-Factor Times Area Value at Low Fan Speed;
+
+8.~~~~Air Flow Rate in Free Convection Regime;
+
+9.~~~~U-Factor Times Area Value at Free Convection Air Flow Rate.
+
+Note that the U-Factor Times Area Value at High Fan Speed is not \emph{multiplied} by the Sizing Factor. Instead the design tower load is multiplied by the sizing factor and the design UA then calculated as usual. The U-Factor Times Area Value at Low Fan Speed is set to a fraction of the full load design UA determined by the field Low Fan Speed U-Factor Times Area Sizing Factor. The U-Factor Times Area Value at Free Convection Air Flow Rate is set to a fraction of the design Tower UA determined by the field Free Convection Air U-Factor Times Area Value Sizing Factor.
+
+Four examples of an IDF specification for this object are shown below:
+
+\begin{lstlisting}
+
+CoolingTower:TwoSpeed,
+     My Tower,                      !- Name
+     Condenser Tower Inlet Node,    !- Water inlet node name
+     Condenser Tower Outlet Node,   !- Water outlet node name
+     .0011,                         !- Design water flow rate, m3/s
+     16.0,                          !- Air flow rate at high fan speed, m3/s
+     10000,                         !- Fan power at high fan speed, W
+     3500.,                         !- Tower UA at high fan speed, W/C
+     8.0,                           !- Air flow rate at low fan speed, m3/s
+     1600,                          !- Fan power at low fan speed, W
+     2100.,                         !- Tower UA at low fan speed, W/C
+     1.6,                           !- Air flow rate for free convection, m3/s
+     350,                          !- Tower UA at free convection air flow, W/C
+     UFactorTimesAreaAndDesignWaterFlowRate; !- Tower performance input method
+
+
+    CoolingTower:TwoSpeed,
+      My Tower,                !- Name
+      Condenser Tower Inlet Node,   !- Water Inlet Node Name
+      Condenser Tower Outlet Node,  !- Water Outlet Node Name
+      ,                        !- Design Water Flow Rate {m3/s}
+      8.0,                     !- Air Flow Rate at High Fan Speed {m3/s}
+      500,                     !- Fan Power at High Fan Speed {W}
+      ,                   !- U-Factor Times Area Value at High Fan Speed {W/K}
+      4.0,                     !- Air Flow Rate at Low Fan Speed {m3/s}
+      125,                     !- Fan Power at Low Fan Speed {W}
+      ,                   !- U-Factor Times Area Value at Low Fan Speed {W/K}
+      0.8,                !- Air Flow Rate in Free Convection Regime {m3/s}
+      ,     !- U-Factor Times Area Value at Free Convection Air Flow Rate {W/K}
+      NominalCapacity,         !- Performance Input Method
+      20000.0,                 !- High Speed Nominal Capacity {W}
+      10000.0,                 !- Low Speed Nominal Capacity {W}
+      2000.0;                  !- Free Convection Capacity {W}
+
+
+  CoolingTower:TwoSpeed,
+    Big Tower1,  !- Tower Name
+    Condenser Tower 1 Inlet Node,  !- Water Inlet Node Name
+    Condenser Tower 1 Outlet Node,  !- Water Outlet Node Name
+    ,  !- Design Water Flow Rate {m3/s}
+    8.0,  !- Design High Speed Air Flow Rate {m3/s}
+    500,  !- Fan Power at Design High Speed Air Flow Rate {W}
+    ,  !- Tower UA Value at Design High Speed Air Flow Rate {W/K}
+    4.0,  !- Design Low Speed Air Flow Rate {m3/s}
+    125,  !- Fan Power at Design Low Speed Air Flow Rate {W}
+    ,  !- Tower UA Value at Design Low Speed Air Flow Rate {W/K}
+    0.8,  !- Air Flow Rate in Free Convection Regime {m3/s}
+    ,  !- Tower UA Value at Free Convection Air Flow Rate {W/K}
+    NominalCapacity,  !- Tower Performance Input Method
+    20000.0,  !- Tower High Speed Nominal Capacity
+    10000.0,  !- Tower Low Speed Nominal Capacity
+    2000.0,  !- Tower Free Convection Nominal Capacity
+    ,        !- Basin Heater Capacity {W/K}
+    ,        !- Basin Heater Setpoint Temperature {C}
+    ,        !- Basin Heater Operating Schedule Name
+    SaturatedExit,  !- Evaporation Loss Mode
+    ,  !- Evaporation Loss Factor [%/C]
+    0.008 ,  !- Drift Loss Percent
+    ConcentrationRatio,  !- Blowdown Calculation Mode
+    3.0,  !- Blowdown Concentration Ratio
+    ,  !- Schedule Name for Makeup Water Usage due to Blowdown
+    Recovery Tank;  !- Name of Water Storage Tank for Supply
+
+
+  CoolingTower:TwoSpeed,
+      TowerWaterSys CoolTower,   !- Name
+      TowerWaterSys Pump-TowerWaterSys CoolTowerNode,  !- Water Inlet Node Name
+      TowerWaterSys Supply Equipment Outlet Node,  !- Water Outlet Node Name
+      AUTOSIZE,                        !- Design Water Flow Rate {m3/s}
+      AUTOSIZE,                     !- Air Flow Rate at High Fan Speed {m3/s}
+      AUTOSIZE,                     !- Fan Power at High Fan Speed {W}
+      AUTOSIZE,           !- U-Factor Times Area Value at High Fan Speed {W/K}
+      AUTOSIZE,           !- Air Flow Rate at Low Fan Speed {m3/s}
+      AUTOSIZE,                     !- Fan Power at Low Fan Speed {W}
+      AUTOSIZE,           !- U-Factor Times Area Value at Low Fan Speed {W/K}
+      AUTOSIZE,           !- Air Flow Rate in Free Convection Regime {m3/s}
+      AUTOSIZE,   !- U-Factor Times Area at Free Convection Air Flow Rate {W/K}
+      UFactorTimesAreaAndDesignWaterFlowRate,     !- Performance Input Method
+      ,                 !- High Speed Nominal Capacity {W}
+      ,                 !- Low Speed Nominal Capacity {W}
+      ,                  !- Free Convection Capacity {W}
+      ,  !- Basin Heater Capacity {W/K}
+      ,  !- Basin Heater Setpoint Temperature {C}
+      ,  !- Basin Heater Operating Schedule Name
+      SaturatedExit,  !- Evaporation Loss Mode { LossFactor | SaturatedExit }
+      ,  !- Evaporation Loss Factor
+      0.0080,  !- Drift Loss Percent
+      ConcentrationRatio,  !- Blowdown Calculation Mode { ConcentrationRatio |
+                           !- ScheduledRate }
+      3.0000,  !- Blowdown Concentration Ratio
+      ,  !- Blowdown Makeup Water Usage Schedule Name
+      ,  !- Supply Water Storage Tank Name
+      TowerWaterSys CoolTower OA ref Node,  !- Outdoor Air Inlet Node Name
+      ,         !- Number of cells available
+      MinimalCell, !- Cell Control
+      ,        !- Cell Minimum Water Flow Rate Fraction
+      ,        !- Cell Maximum Water Flow Rate Fraction
+      1.0000;  !- Sizing Factor
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-003}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Tower Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Tower Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Cooling Tower Fan Cycling Ratio {[]}
+\item
+  HVAC,Average,Cooling Tower Operating Cells Count {[]}
+\item
+  HVAC,Average,Cooling Tower Fan Speed Level {[]}
+\item
+  HVAC,Average,Cooling Tower Bypass Fraction {[]}
+\end{itemize}
+
+A tower uses either mains water or storage tank for make-up water.
+
+\emph{When mains water is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\emph{When storage tank water is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Mains Water Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Evaporation Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Drift Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Blowdown Volume {[}m3{]}
+\end{itemize}
+
+IF specified:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Cooling Tower Fan Electric Power {[}W{]}}\label{cooling-tower-fan-electric-power-w-1}
+
+\paragraph{Cooling Tower Fan Electric Energy {[}J{]}}\label{cooling-tower-fan-electric-energy-j-1}
+
+These outputs are the electric power input to the tower fans. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Cooling Tower Heat Transfer Rate {[}W{]}}\label{cooling-tower-heat-transfer-rate-w-1}
+
+This is the rate at which heat is removed from the condenser water loop by the tower.
+
+\paragraph{Cooling Tower Inlet Temperature {[}C{]}}\label{cooling-tower-inlet-temperature-c-1}
+
+\paragraph{Cooling Tower Outlet Temperature {[}C{]}}\label{cooling-tower-outlet-temperature-c-1}
+
+\paragraph{Cooling Tower Mass Flow Rate {[}kg/s{]}}\label{cooling-tower-mass-flow-rate-kgs-1}
+
+These outputs are the tower water inlet and outlet temperatures, and mass flow rate.
+
+\paragraph{Cooling Tower Basin Heater Electric Power {[}W{]}}\label{cooling-tower-basin-heater-electric-power-w-1}
+
+\paragraph{Cooling Tower Basin Heater Electric Energy {[}J{]}}\label{cooling-tower-basin-heater-electric-energy-j-1}
+
+These outputs are the electric power input to the tower basin heater. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility
+
+\paragraph{Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-make-up-water-volume-flow-rate-m3s-1}
+
+\paragraph{Cooling Tower Make Up Water Volume {[}m3{]}}\label{cooling-tower-make-up-water-volume-m3-1}
+
+These outputs are the water consumed by the wet cooling tower for external water sprays used to augment heat transfer. This is the total of evaporation, drift, and blowdown.
+
+\paragraph{Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-evaporation-volume-flow-rate-m3s-1}
+
+\paragraph{Cooling Tower Water Evaporation Volume {[}m3{]}}\label{cooling-tower-water-evaporation-volume-m3-1}
+
+\paragraph{Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-drift-volume-flow-rate-m3s-1}
+
+\paragraph{Cooling Tower Water Drift Volume {[}m3{]}}\label{cooling-tower-water-drift-volume-m3-1}
+
+\paragraph{Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-blowdown-volume-flow-rate-m3s-1}
+
+\paragraph{Cooling Tower Water Blowdown Volume {[}m3{]}}\label{cooling-tower-water-blowdown-volume-m3-1}
+
+These outputs provide the breakdown of the different components of water use during cooling tower operation.
+
+\paragraph{Cooling Tower Make Up Mains Water Volume {[}m3{]}}\label{cooling-tower-make-up-mains-water-volume-m3-1}
+
+This is the volume of water drawn from mains service to feed the cooling tower. If a water storage tank is used to provide water to the tower, then the following output variables will also be available.
+
+\paragraph{Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-storage-tank-water-volume-flow-rate-m3s-1}
+
+\paragraph{Cooling Tower Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-storage-tank-water-volume-m3-1}
+
+These are the rate and volume of water provided by the Water Storage Tank.
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-starved-storage-tank-water-volume-flow-rate-m3s-1}
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-starved-storage-tank-water-volume-m3-1}
+
+These are the rate and volume of water the Storage Tank connections was not able to provide. The starved water is assumed to come from the mains. The tower's operation is not affected by a lack of storage tank water.
+
+\paragraph{\texorpdfstring{Cooling Tower Fan Cycling Ratio {[]}}{Cooling Tower Fan Cycling Ratio }}\label{cooling-tower-fan-cycling-ratio-1}
+
+This represents the fraction of a time-step when tower fan is on. The fan can cycle at both speeds.
+
+\paragraph{\texorpdfstring{Cooling Tower Operating Cells Count {[]}}{Cooling Tower Operating Cells Count }}\label{cooling-tower-operating-cells-count-1}
+
+This represents the number of cells operating at each time step.
+
+\paragraph{\texorpdfstring{Cooling Tower Fan Speed Level {[]}}{Cooling Tower Fan Speed Level }}\label{cooling-tower-fan-speed-level}
+
+This represents the fan speed operating at each time step: 2 for High Speed, 1 for Low Speed, and 0 when the fan is OFF.
+
+\subsection{CoolingTower:VariableSpeed:Merkel}\label{coolingtowervariablespeedmerkel}
+
+This variable speed tower model is based on Merkel's theory and is similar to the single-speed and two-speed tower models.~ The open wet cooling tower is modeled as a counter flow heat exchanger with a variable-speed fan drawing air through the tower (induced-draft configuration). The model also includes a ``free convection'' regime where cooling tower performance modeled with the fan off.
+
+For this model, Merkel's theory is modified to include adjustments developed by Scheier to alter the heat transfer effectiveness based on current wetbulb, air flow rates, and water flow rates. The input requires performance curves or lookup tables to describe these three adjustment factors.
+
+For a multi-cell tower, the capacity and air/water flow rate inputs are for the entire tower.
+
+\subsubsection{Inputs}\label{inputs-2-006}
+
+\paragraph{Field: Name}\label{field-name-1-005}
+
+This alpha field contains the identifying name for the cooling tower.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-2}
+
+This alpha field contains the identifying name for the cooling tower's water inlet node.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-2}
+
+This alpha field contains the identifying name for the cooling tower's water outlet node.
+
+\paragraph{Field: Performance Input Method}\label{field-performance-input-method-2}
+
+This alpha field contains the method by which the user will specify tower performance: ``\textbf{UFactorTimesAreaAndDesignWaterFlowRate}'' or ``\textbf{NominalCapacity}''. If this field is left blank in the input data file, the default input method is assumed to be ``\textbf{NominalCapacity}''. If the method ``'' is selected, then the user must enter design UA values, design water flow rates and air flow rates as described for the previous input fields. If the method ``NominalCapacity'' is selected then the fields ``Design Water Flow Rate'', ``U-Factor Times Area Value at Design Air Flow Rate'' and ``U-Factor Times Area Value at Free Convection Air Flow Rate'' must be left blank, but the fields ``Nominal Capacity'' and ``Free Convection Capacity'' must be entered as described below.
+
+\paragraph{Field: Heat Rejection Capacity and Nominal Capacity Sizing Ratio}\label{field-heat-rejection-capacity-and-nominal-capacity-sizing-ratio-2}
+
+This numeric field contains the value for the ratio of actual tower heat rejection to nominal capacity.~ This ratio is defined at entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. Historically this ratio has been set at 1.25 based on the assumption that the tower must dissipate 0.25 W of compressor power for every what of heat removed at the chiller evaporator.~ The default is 1.25.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-1}
+
+This numeric input field contains the ``nominal'' heat rejection capacity of the cooling tower in watts under full-speed fan operation, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The Heat Rejection Capacity and Nominal Capacity Sizing Ratio set in the previous field is applied to this nominal tower capacity to give the actual tower heat rejection at these operating conditions.~ This field can be autosized, in which case a Sizing:Plant object is needed for the condenser loop.
+
+\paragraph{Field: Free Convection Nominal Capacity}\label{field-free-convection-nominal-capacity}
+
+This numeric input field contains the ``nominal'' heat rejection capacity of the cooling tower in watts when the tower is in the ``free convection'' regime (water flow exists but tower fan is turned off), with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The Heat Rejection Capacity and Nominal Capacity Sizing Ratio is applied to this free convection tower capacity to give the actual tower heat rejection at these operating conditions.The value specified for this field must be less than the value specified for the field ``Tower Low-Speed Nominal Capacity''. If the user does not wish to model ``free convection'', then this field should be set to 0.0. If the user specifies a value greater than zero, then the ``Air Flow Rate in Free Convection Regime'' field must contain a value greater than zero. This field may be autocalculated, in which case it is set to a fraction of the High Speed Nominal Capacity determined in the following field.
+
+\paragraph{Field: Free Convection Nominal Capacity Sizing Factor}\label{field-free-convection-nominal-capacity-sizing-factor-2}
+
+This numeric field contains the sizing factor to use when calculating the Free Convection Capacity. The default is 0.1.
+
+\paragraph{Field: Design Water Flow Rate}\label{field-design-water-flow-rate-2}
+
+This numeric field contains the design water flow rate through the tower in m\(^{3}\)/s. This value is the flow rate of the condenser loop water being cooled by the tower. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a water flow rate greater than zero must be defined or the field can be autosized. If autosized, a Sizing:Plant object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections). If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field can be autocalculated using the sizing factor in the following field.
+
+\paragraph{Field: Design Water Flow Rate per Unit of Nominal Capacity}\label{field-design-water-flow-rate-per-unit-of-nominal-capacity}
+
+This numeric field contains a scalable sizing factor for design water flow rate that scales with nominal capacity, in units of m\(^{3}\)/s/W. The default value is 5.382*10\(^{-8}\). This field is only used if the previous field is set to autocalculate and performance input method is NominalCapacity.~ (If the performance input method is set to UFactorTimesAreaAndDesignWaterFlowRate then the design water flow rate is obtained from the plant sizing result.)
+
+\paragraph{Field: Design Air Flow Rate}\label{field-design-air-flow-rate-1}
+
+This numeric field contains the tower air flow rate at full fan speed, in m\(^{3}\)/s.~ The value can be autocalculated, in which case the air flow rate is based off of the scalable sizing factor in the following input field.
+
+\paragraph{Field: Design Air Flow Rate Per Unit of Nominal Capacity}\label{field-design-air-flow-rate-per-unit-of-nominal-capacity}
+
+This numeric field contains the sizing factor to use when calculating the design air flow rate from the nominal capacity, in units of m\(^{3}\)/s/W.~ The default is 2.76316*10\(^{-5}\).~ When this field is left blank, then the default value is used but the flow rate is also scaled to account for elevation (with larger volume flow rates at higher altitudes).~ When a hard value is entered, even if it is the same as the default, then the design air flow rate is not also adjusted for elevation and the scaling factor is used directly.
+
+\paragraph{Field: Minimum Air Flow Rate Ratio}\label{field-minimum-air-flow-rate-ratio}
+
+This numeric field contains the minimum air flow rate ratio. The tower fan is allowed to operate between the ratio defined here and a maximum air flow rate ratio of 1.0 (which corresponds to the design {[}maximum{]} tower air flow rate). Below this value the tower is assumed to operate in the ``free convection'' regime with the tower fan off. The minimum air flow rate ratio must be greater than or equal to 0.1 and less than or equal to 0.5, with a default value of 0.2 if the field is left blank.
+
+\paragraph{Field: Design Fan Power}\label{field-design-fan-power}
+
+This numeric field contains the fan power in watts at the design (maximum) air flow rate through the tower. A value greater than zero must be specified or this field can be autocalculated. When the field is autocalculated the following input field is used to size the fan power based on nominal capacity.
+
+\paragraph{Field: Design Fan Power Per Unit of Nominal Capacity}\label{field-design-fan-power-per-unit-of-nominal-capacity}
+
+This numeric field contains the sizing factor to use when calculating the design fan power from the nominal capacity, in units of Watts per Watt. This field is only used if the previous is set to autocalculate. The default values is 0.0105.
+
+\paragraph{Field: Fan Power Modifier Function of Air Flow Rate Ratio Curve Name}\label{field-fan-power-modifier-function-of-air-flow-rate-ratio-curve-name}
+
+This alpha field contains the name of a curve or table object that describes fan power ratio (fan power/design fan power) as a function of air flow rate ratio (air flow rate/design air flow rate). The curve or table object must be for one independent variable, typically a cubic, and should be normalized to 1.0 at an air flow rate ratio of 1.0.~ This field is required.
+
+\paragraph{Field: Free Convection Regime Air Flow Rate}\label{field-free-convection-regime-air-flow-rate-1}
+
+This numeric field contains the air flow rate (m\(^{3}\)/s) when the tower is in the ``free convection'' regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field ``Design Air Flow Rate''. This field may be autocalculated, in which case it is set to a fraction of the ``Design Air Flow Rate'' determined in the following input field. If the user does not wish to model ``free convection'' and is using the Performance Input Method ``UFactorTimesAreaAndDesignWaterFlowRate'', then this field should be set to 0.0. If the user specifies the U-Factor Times Area Value at Free Convection Air Flow Rate or Free Convection Capacity as a value greater than zero, then the free convection air flow rate must be specified greater than 0.0.
+
+\paragraph{Field: Free Convection Regime Air Flow Rate Sizing Factor}\label{field-free-convection-regime-air-flow-rate-sizing-factor-1}
+
+This numeric field contains the sizing factor to use when calculating the free convection regime air flow rate.~ The default is 0.1.
+
+\paragraph{Field: Design Air Flow Rate U-Factor Times Area Value}\label{field-design-air-flow-rate-u-factor-times-area-value}
+
+This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the design air and water flow rates specified above. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design tower UA value is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), assuming a tower water inlet temperature of 35C and tower inlet air at 35C drybulb/25.6C wetbulb. If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field ``Nominal Capacity''.
+
+\paragraph{Field: Free Convection Regime U-Factor Times Area Value}\label{field-free-convection-regime-u-factor-times-area-value}
+
+This numeric field contains the heat transfer coefficient-area product (W/K) when the tower is in the ``free convection'' regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field ``U-Factor Times Area Value at Design Air Flow Rate''. This field may be autosized, in which case it is set to a fraction of the ``U-Factor Times Area Value at Design Air Flow Rate'' determined in the following input field. If the user does not wish to model ``free convection'' and is using the~ Performance Input Method ``UFactorTimesAreaAndDesignWaterFlowRate'', then this field should be set to 0.0. If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field ``Free Convection Capacity''.
+
+\paragraph{Field: Free Convection U-Factor Times Area Value Sizing Factor}\label{field-free-convection-u-factor-times-area-value-sizing-factor-2}
+
+This numeric field contains the sizing factor to use when calculating the free convection regime U-Factor times area value.~ The default is 0.1. This field is only used if the previous field is set to autocalculate and the performance input method is UFactorTimesAreaAndDesignWaterFlowRate.
+
+\paragraph{Field: U-Factor Times Area Modifier Function of Air Flow Ratio Curve Name}\label{field-u-factor-times-area-modifier-function-of-air-flow-ratio-curve-name}
+
+This alpha field contains the name of a curve or table object that describes how the UA value varies as a function of air flow rate ratio (air flow rate/design air flow rate).~ The result of this curve is multiplied by the design UA value to adjust for air flow rate, along with the two other modifiers discussed below.~ The curve or table object must be for one independent variable and should be normalized to 1.0 at an air flow rate ratio of 1.0.~ This field is required.
+
+\paragraph{Field: U-Factor Times Area Modifier Function of Wetbulb Temperature Difference Curve Name}\label{field-u-factor-times-area-modifier-function-of-wetbulb-temperature-difference-curve-name}
+
+This alpha field contains the name of a curve or table object that describes how the UA value varies as a function of the current wetbulb temperature.~ The result of this curve is multiplied by the design UA value to adjust for wetbulb temperatures that differ from design conditions at 25.56°C (78°F), along with the two other modifiers discussed in the previous and following fields.~ The independe variable is the design wetbulb minus the current outdoor air wetbulb, in units of degrees Celsius.~ The curve or table object must be for one independent variable and should be normalized to 1.0 at a wetbulb temperature difference of 0.0.~ This field is required.
+
+\paragraph{Field: U-Factor Times Area Modifier Function of Water Flow Ratio Curve Name}\label{field-u-factor-times-area-modifier-function-of-water-flow-ratio-curve-name}
+
+This alpha field contains the name of a curve or table object that describes how the UA value varies as a function of the current water flow rate ratio (water flow rate/design water flow rate). The result of this curve is multiplied by the design UA value to adjust for water flow rates that differ from design level, along with the other two modifiers discussed above. The curve or table object must be for one independent variable and should be normalized to 1.0 at a water flow ratio of 1.0.~ This field is required
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-2}
+
+This numeric field contains the capacity of the tower's electric basin heater in watts per degree Kelvin. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the tower fan is off and water is not flowing through the tower, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-2}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the tower fan is off and water is not flowing through the tower. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-2}
+
+This alpha field contains the name of the basin heater operating schedule. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the cooling tower fan is off and water is not flowing through the tower.
+
+\paragraph{Field: Evaporation Loss Mode}\label{field-evaporation-loss-mode-2}
+
+This field is used to choose which method is used to model the amount of water evaporated by the cooling tower. There are two options: \textbf{LossFactor} or \textbf{SaturatedExit}. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the tower is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the cooling tower model (and does not require additional user input).
+
+\paragraph{Field: Evaporation Loss Factor}\label{field-evaporation-loss-factor-2}
+
+This field is used to specify the rate of water evaporated from the cooling tower and lost to the outside air {[}percent/K{]}. This field is only used if the Evaporation Calculation Mode is set to \textbf{LossFactor}. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-degree Kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Typical values are from 0.15 to 0.27 {[}percent/K{]}. The default is 0.2.
+
+\paragraph{Field: Drift Loss Percent}\label{field-drift-loss-percent-2}
+
+This field is used to specify the rate of water lost to the exiting air as entrained droplets {[}\%{]}. The drift loss is a percent of the condenser water flow. Typical values for towers with efficient drift eliminators are between 0.002 and 0.2\% of the condenser water flow rate. The default value is 0.008\%.
+
+\paragraph{Field: Blowdown Calculation Mode}\label{field-blowdown-calculation-mode-2}
+
+This field specifies which method is used to determine blowdown rates. There two options \textbf{ConcentrationRatio} or \textbf{ScheduledRate}. The choice will determine which of the two models below is used. The default is ConcentrationRatio.
+
+\paragraph{Field: Blowdown Concentration Ratio}\label{field-blowdown-concentration-ratio-2}
+
+This field is used to dynamically adjust the rate of blowdown in the cooling tower as a function of the rate of evaporation. Blowdown is water intentionally drained from the tower in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values for tower operation are 3 to 5. The default value is 3.
+
+\paragraph{Field: Blowdown Makeup Water Usage Schedule Name}\label{field-blowdown-makeup-water-usage-schedule-name-2}
+
+This alpha field contains the name of the schedule used to define the amount of water (m\(^{3}\)/s) flushed from the basin on a periodic basis to purge the tower of mineral scale build-up and other contaminants. This schedule is only used if the Blowdown Calculation Mode is set to ScheduledRate. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Typical values range from 0.0002 to 0.0013 m\(^{3}\)/s (17.3 to 112.3 m\(^{3}\)/day). This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the cooling tower is active and water is flowing through the tower (regardless of the water usage defined by this schedule).
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-2}
+
+This field is optional. It is used to describe where the tower obtains water used for evaporative cooling. If blank or omitted, then the tower will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the tower will obtain its water from that tank. If a tank is specified, the tower will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the tower needs, then the tower will still operate and obtain the rest of the water it needs from the mains (referred to as `Starved' water).
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-2}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the cooling tower. If this field is left blank, the outdoor air conditions entering the cooling tower are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+\paragraph{Field: Number of Cells}\label{field-number-of-cells-2}
+
+This integer field contains the number of cells in the multi-cell cooling tower. If not entered, the program will assume it is a single-cell cooling tower
+
+\paragraph{Field: Cell Control}\label{field-cell-control-2}
+
+This alpha field specifies the method used to control the number of cells used to meet the load, the two choices are:
+
+\textbf{MinimalCell} : the program will use minimal number of cells needed, all other cells will be shut down with no water flow. It will attempt to use as few cells as possible to cool the fluid. In no case, however, will the flow per cell be allowed to exceed its maximum value defined by the \emph{Maximum Water Flow Rate Fraction.}
+
+\textbf{MaximalCell}: As many cells as possible will be turned on. In no case, however, will the flow per cell be allowed to drop below its minimum value specified by the \emph{Minimum Water Flow Rate Fraction}.
+
+\paragraph{Field: Cell Minimum~ Water Flow Rate Fraction}\label{field-cell-minimum-water-flow-rate-fraction-2}
+
+This numeric field specifies the allowable smallest fraction of the design water flow rate. Flows less than this value will commonly result in fluid distribution problems; the pressure at each nozzle will be too weak for the fluid to be sprayed out in the correct pattern, not all the fill would be wet. If this field is left blank, the default value is 0.33.
+
+\paragraph{Field: Cell Maximum Water Flow Rate Fraction}\label{field-cell-maximum-water-flow-rate-fraction-2}
+
+This numeric field specifies the allowable largest fraction of the design water flow rate. If this field is left blank, the default value is 2.5.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-1}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+An example IDF specification follows.
+
+\begin{lstlisting}
+
+  CoolingTower:VariableSpeed:Merkel,
+      Big Tower1, !- Name
+      Condenser Tower 1 Inlet Node, !- Water Inlet Node Name
+      Condenser Tower 1 Outlet Node, !- Water Outlet Node Name
+      NominalCapacity, !- Performance Input Method
+      1.25, !- Heat Rejection Capacity and Nominal Capacity Sizing Ratio
+      20000.0,  !- Nominal Capacity
+      autocalculate, !- Free Convection Nominal Capacity
+      0.1, !- Free Convection Nominal Capacity Sizing Factor
+      autocalculate, !- Design Water Flow Rate
+      5.382E-8, !- Design Water Flow Rate per Unit of Nominal Capacity
+      autocalculate, !- Design Air Flow Rate
+      2.76316E-5, !- Design Air Flow Rate Per Unit of Nominal Capacity
+      0.2, !- Minimum Air Flow Rate Ratio
+      autocalculate, !- Design Fan Power
+      0.0105, !- Design Fan Power Per Unit of Nominal Capacity
+      VS tower fan power mod func air flow ratio, !- Fan Power Modifier Function of Air Flow Rate Ratio Curve Name
+      autocalculate, !- Free Convection Regime Air Flow Rate
+      0.1, !- Free Convection Regime Air Flow Rate Sizing Factor
+      , !- Design Air Flow Rate U-Factor Times Area Value
+      , !- Free Convection Regime U-Factor Times Area Value
+      , !- Free Convection U-Factor Times Area Value Sizing Factor
+      VS tower UA mod func air flow ratio, !- U-Factor Times Area Modifier Function of Air Flow Ratio Curve Name
+      VS tower UA mod func wetbulb difference, !- U-Factor Times Area Modifier Function of Wetbulb Temperature Difference Curve Name
+      VS tower UA mod func water flow ratio; !- U-Factor Times Area Modifier Function of Water Flow Ratio Curve Name
+
+
+    Curve:Cubic,
+      VS tower fan power mod func air flow ratio, !- Name
+      0.02 , !- Coefficient1 Constant
+      0.0 ,  !- Coefficient2 x
+      0.0 ,  !- Coefficient3 x**2
+      0.98 , !- Coefficient4 x**3
+      0.2,   !- Minimum Value of x
+      1.0 ,  !- Maximum Value of x
+      0.0 ,  !- Minimum Curve Output
+      1.0 ,  !- Maximum Curve Output
+      Dimensionless,  !- Input Unit Type for X
+      Dimensionless;  !- Output Unit Type
+
+
+    Curve:Quadratic,
+      VS tower UA mod func air flow ratio, !- Name
+      0.0 , !- Coefficient1 Constant
+      1.3 , !- Coefficient2 x
+      -0.3 , !- Coefficient3 x**2
+      0.2 , !- Minimum Value of x
+      1.0 , !- Maximum Value of x
+      0.0 , !- Minimum Curve Output
+      1.0 , !- Maximum Curve Output
+      Dimensionless,  !- Input Unit Type for X
+      Dimensionless;  !- Output Unit Type
+
+
+    Curve:Linear,
+      VS tower UA mod func wetbulb difference , !- Name
+      1.0 , !- Coefficient1 Constant
+      0.0081 , !- Coefficient2 x
+      -10 , !- Minimum Value of x
+      25.0 , !- Maximum Value of x
+      0.85 , !- Minimum Curve Output
+      1.3 , !- Maximum Curve Output
+      Dimensionless,  !- Input Unit Type for X
+      Dimensionless; !- Output Unit Type
+
+
+    Curve:Quadratic,
+      VS tower UA mod func water flow ratio, !- Name
+      0.1082 , !- Coefficient1 Constant
+      1.667 , !- Coefficient2 x
+      -0.7713 , !- Coefficient3 x**2
+      0.3 , !- Minimum Value of x
+      1.0 , !- Maximum Value of x
+      0.5 , !- Minimum Curve Output
+      1.1 , !- Maximum Curve Output
+      Dimensionless,  !- Input Unit Type for X
+      Dimensionless;  !- Output Unit Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-003}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Cooling Tower Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Tower Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Tower Operating Cells Count {[]}
+\item
+  HVAC,Average,Cooling Tower Fan Speed Ratio {[]}
+\end{itemize}
+
+A tower uses either mains water or storage tank for make-up water.
+
+\emph{When mains water is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\emph{When storage tank water is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Mains Water Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Evaporation Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Drift Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Blowdown Volume {[}m3{]}
+\end{itemize}
+
+IF specified:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Cooling Tower Fan Electric Power {[}W{]}}\label{cooling-tower-fan-electric-power-w-2}
+
+\paragraph{Cooling Tower Fan Electric Energy {[}J{]}}\label{cooling-tower-fan-electric-energy-j-2}
+
+These outputs are the electric power input to the tower fans. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Cooling Tower Heat Transfer Rate {[}W{]}}\label{cooling-tower-heat-transfer-rate-w-2}
+
+This is the rate at which heat is removed from the condenser water loop by the tower.
+
+\paragraph{Cooling Tower Inlet Temperature {[}C{]}}\label{cooling-tower-inlet-temperature-c-2}
+
+\paragraph{Cooling Tower Outlet Temperature {[}C{]}}\label{cooling-tower-outlet-temperature-c-2}
+
+\paragraph{Cooling Tower Mass Flow Rate {[}kg/s{]}}\label{cooling-tower-mass-flow-rate-kgs-2}
+
+These outputs are the tower water inlet and outlet temperatures, and mass flow rate.
+
+\paragraph{Cooling Tower Fan Speed Ratio}\label{cooling-tower-fan-speed-ratio}
+
+This output is the air flow ratio.~ The current air flow rate divided by the design air flow rate with values from 0.0 to 1.0.
+
+\paragraph{\texorpdfstring{Cooling Tower Operating Cells Count {[]}}{Cooling Tower Operating Cells Count }}\label{cooling-tower-operating-cells-count-2}
+
+This represents the number of cells operating at each time step.
+
+\paragraph{Cooling Tower Basin Heater Electric Power {[}W{]}}\label{cooling-tower-basin-heater-electric-power-w-2}
+
+\paragraph{Cooling Tower Basin Heater Electric Energy {[}J{]}}\label{cooling-tower-basin-heater-electric-energy-j-2}
+
+These outputs are the electric power input to the tower basin heater. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility
+
+\paragraph{Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-make-up-water-volume-flow-rate-m3s-2}
+
+\paragraph{Cooling Tower Make Up Water Volume {[}m3{]}}\label{cooling-tower-make-up-water-volume-m3-2}
+
+These outputs are the water consumed by the wet cooling tower for external water sprays used to augment heat transfer. This is the total of evaporation, drift, and blowdown.
+
+\paragraph{Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-evaporation-volume-flow-rate-m3s-2}
+
+\paragraph{Cooling Tower Water Evaporation Volume {[}m3{]}}\label{cooling-tower-water-evaporation-volume-m3-2}
+
+\paragraph{Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-drift-volume-flow-rate-m3s-2}
+
+\paragraph{Cooling Tower Water Drift Volume {[}m3{]}}\label{cooling-tower-water-drift-volume-m3-2}
+
+\paragraph{Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-blowdown-volume-flow-rate-m3s-2}
+
+\paragraph{Cooling Tower Water Blowdown Volume {[}m3{]}}\label{cooling-tower-water-blowdown-volume-m3-2}
+
+These outputs provide the breakdown of the different components of water use during cooling tower operation.
+
+\paragraph{Cooling Tower Make Up Mains Water Volume {[}m3{]}}\label{cooling-tower-make-up-mains-water-volume-m3-2}
+
+This is the volume of water drawn from mains service to feed the cooling tower. If a water storage tank is used to provide water to the tower, then the following output variables will also be available.
+
+\paragraph{Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-storage-tank-water-volume-flow-rate-m3s-2}
+
+\paragraph{Cooling Tower Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-storage-tank-water-volume-m3-2}
+
+These are the rate and volume of water provided by the Water Storage Tank.
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-starved-storage-tank-water-volume-flow-rate-m3s-2}
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-starved-storage-tank-water-volume-m3-2}
+
+These are the rate and volume of water the Storage Tank connections was not able to provide. The starved water is assumed to come from the mains. The tower's operation is not affected by a lack of storage tank water.
+
+\subsection{CoolingTower:VariableSpeed}\label{coolingtowervariablespeed}
+
+The variable speed tower model is based on empirical curve fits of manufacturer's performance data or field measurements. The user specifies tower performance at design conditions, and empirical curves are used to determine the approach temperature and fan power at off-design conditions. The user defines tower performance by entering the inlet air wet-bulb temperature, tower range, and tower approach temperature at the design conditions. The corresponding water flow rate (within ±25\% of the tower's rated water mass flow rate), air flow rate, and fan power must also be specified. The model will account for tower performance in the ``free convection'' regime, when the tower fan is off but the water pump remains on and heat transfer still occurs (albeit at a low level). Basin heater operation and makeup water usage (due to evaporation, drift, and blowdown) are also modeled.
+
+The cooling tower seeks to maintain the temperature of the water exiting the cooling tower at (or below) a set point. The set point schedule is defined by the field ``Condenser Loop Temperature Setpoint Node Name or Reference'' for the CondenserLoop object. The model first checks to determine the impact of ``free convection'' on the tower exiting water temperature. If the exiting water temperature based on ``free convection'' is at or below the set point, then the variable-speed tower fan is not turned on. If the exiting water temperature is above the set point after ``free convection'' is modeled, then the variable-speed tower fan is turned on to reduce the exiting water temperature. Tower fan power is calculated based on the tower air flow rate required to achieve the exiting water set point temperature.
+
+Cooling towers here are ``wet'' and consume water through evaporation, drift, and blowdown. The model can be used to predict water consumed by the towers. The last six input fields are optional and provide methods of controlling details of the water consumption calculations. The user can specifiy connections to the rest of the buildings water system by providing the name of a WaterUse:Storage object.
+
+For the operation of multi-cell towers, the first step is to determine the number of cells to operate based on the cell control method -- between the minimum number of cells subject to the maximum water flow rate fraction per cell, and maximum number of cells subject to the minimum water flow rate fraction per cell. If the calculated cells do not meet the loads, additional cells will be operating to help meet the loads. Inside each cell, the existing capacity controls still apply.
+
+For multi-cell towers, the following inputs are assumed to be for the entire tower including all cells:
+
+\begin{itemize}
+\item
+  Design Water Flow Rate; Design Air Flow Rate; Fan Power at Design Air Flow Rate;
+\item
+  Air Flow Rate in Free Convection Regime; Nominal Capacity; Free Convection Capacity
+\item
+  BASIN HEATER (we assume that there is a common basin)
+\end{itemize}
+
+\subsubsection{Inputs}\label{inputs-3-005}
+
+\paragraph{Field: Name}\label{field-name-2-005}
+
+This alpha field contains the identifying name for the variable speed cooling tower.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-3}
+
+This alpha field contains the identifying name for the cooling tower's water inlet node.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-3}
+
+This alpha field contains the identifying name for the cooling tower's water outlet node.
+
+\paragraph{Field: Model Type}\label{field-model-type}
+
+This alpha field contains the type of empirical model used to simulate the tower's thermal performance (approach temperature). Valid choices for this field are ``CoolToolsCrossFlow'', ``CoolToolsUserDefined'', ``YorkCalc'', or ``YorkCalcUserDefined''. ``CoolToolsCrossFlow'' and ``YorkCalc'' are empirical models with the equation form and model coefficients already defined within EnergyPlus. If ``CoolToolsUserDefined'' or ``YorkCalcUserDefined'' is selected, the user must specify a valid Model Coefficient Name in the next input field to reference an appropriate CoolingTowerPerformance:CoolTools or CoolingTowerPerformance:YorkCalc object. If a user-defined model type is selected and the specified Model Coefficient Name is not found in the input data file (idf), then a severe message is issued and the simulation will terminate.
+
+\paragraph{Field: Model Coefficient Name}\label{field-model-coefficient-name}
+
+This alpha field contains the identifying name for the object(s) CoolingTowerPerformance:CoolTools or CoolingTowerPerformance:YorkCalc. A single model coefficient object may be used to define coefficients for multiple variable speed cooling tower objects (i.e., the same name may be used in this input field for more than one variable speed tower). This field is only used when the field Tower Model Type described above is set to ``CoolToolsUserDefined'' or ``YorkCalcUserDefined'', and should be left blank otherwise.
+
+\paragraph{Field: Design Inlet Air Wet-Bulb Temperature}\label{field-design-inlet-air-wet-bulb-temperature}
+
+This numeric field specifies the inlet air wet-bulb temperature (ËšC) at design conditions. This design temperature should correspond with the design values for range temperature, approach temperature, water flow rate, and air flow rate specified in the following fields. The minimum value for this field is 20ËšC and the default value is 25.6ËšC if this field is left blank.
+
+\paragraph{Field: Design Approach Temperature}\label{field-design-approach-temperature}
+
+This numeric field specifies the tower approach temperature (ËšC) at design conditions. The approach temperature is the outlet water temperature minus the inlet air wet-bulb temperature. The design approach temperature should correspond with the design values for inlet air wet-bulb temperature, range temperature, water flow rate, and air flow rate specified for this tower. The value for this field must be greater than 0ËšC and the default value is 3.9ËšC if this field is left blank.
+
+\paragraph{Field: Design Range Temperature}\label{field-design-range-temperature}
+
+This numeric field specifies the range temperature (ËšC) at design conditions. The range temperature is defined as the inlet water temperature minus the outlet water temperature. The design range temperature should correspond with the design values for inlet air wet-bulb temperature, approach temperature, water flow rate, and air flow rate specified for this tower. The value for this field must be greater than 0ËšC and the default value is 5.6ËšC if this field is left blank.
+
+\paragraph{Field: Design Water Flow Rate}\label{field-design-water-flow-rate-3}
+
+This numeric field contains the design water flow rate through the tower in m\(^{3}\)/s. The value entered should be within ±25\% of the tower's rated water mass flow rate as specified by the manufacturer if Model Type is ``CoolToolsCrossFlow'' or ``YorkCalc''. This constraint may be different for Model Type ``CoolToolsUserDefined'' or ``YorkCalcUserDefined'' (ref. CoolingTowerPerformance:CoolTools or CoolingTowerPerformance:YorkCalc).
+
+This value is the flow rate of the condenser loop water being cooled by the tower. A value greater than zero must be specified or this field can be autosized. A Plant Sizing object must be defined if the field is autosized and the design water flow rate is then derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections). The design water flow rate should correspond with the design values specified for the inlet air wet-bulb temperature, approach temperature, range temperature, and air flow rate. When this field is not autosized, the condenser loop flow rate specified in other objects should be within ±25\% of the tower's rated water flow rate (different range is permissible if Model Type is ``User Defined'').
+
+\paragraph{Field: Design Air Flow Rate}\label{field-design-air-flow-rate-2}
+
+This numeric field contains the design (maximum) air flow rate through the tower in m\(^{3}\)/s. A value greater than zero must be specified or this field can be autosized. Autosizing of this field does not require a Plant Sizing object since the design air flow rate is assumed to be the design fan power multiplied by a total fan efficiency of 0.5 and divided by a fan pressure rise of 190 Pascals. A correction for altitude is also included as follows:
+
+\begin{equation}
+Design\;Air\;Flow\;Rate = \frac{{0.5(Fan\;power\;at\;Design\;Air\;Flow\;Rate)}}{{190.}}\left( {\frac{{101325.}}{{{P_{atm}}}}} \right)
+\end{equation}
+
+\paragraph{Field: Design Fan Power}\label{field-design-fan-power-1}
+
+This numeric field contains the fan power in watts at the design (maximum) air flow rate through the tower. A value greater than zero must be specified or this field can be autosized. If autosized, a Plant Sizing object must be defined and the fan power is calculated as follows:
+
+\begin{equation}
+Design\,fan\;power = 0.0105\cdot {\rho_{water}}\cdot {C_{p,water}}\cdot Design\;Water\;Flow\;Rate\cdot Design\;Loop\Delta T
+\end{equation}
+
+\paragraph{Field: Fan Power Ratio Function of Air Flow Rate Ratio Curve Name}\label{field-fan-power-ratio-function-of-air-flow-rate-ratio-curve-name}
+
+This alpha field contains the curve object name for fan power ratio (fan power/design fan power) as a function of air flow rate ratio (air flow rate/design air flow rate) {[}ref. Performance Curves{]}. The curve object must be a cubic curve and should be normalized to 1.0 at an air flow rate ratio of 1.0. If this field is left blank, a theoretical fan curve is assumed where fan power ratio is directly proportional to the air flow rate ratio cubed.
+
+\paragraph{Field: Minimum Air Flow Rate Ratio}\label{field-minimum-air-flow-rate-ratio-1}
+
+This numeric field contains the minimum air flow rate ratio. The tower fan is allowed to operate between the ratio defined here and a maximum air flow rate ratio of 1.0 (which corresponds to the design {[}maximum{]} tower air flow rate). Below this value, the tower is assumed to operate either in the ``free convection'' regime with the tower fan off, or the tower fan is cycled on/off to maintain the exiting water set point temperature. The minimum air flow rate ratio must be greater than or equal to 0.2 and less than or equal to 0.5, with a default value of 0.2 if the field is left blank.
+
+\paragraph{Field: Fraction of Tower Capacity in Free Convection Regime}\label{field-fraction-of-tower-capacity-in-free-convection-regime}
+
+This numeric field contains the fraction of tower capacity available in the free convection regime (i.e., when the tower fan is off but water continues to flow through the tower). The tower fan does not operate when the free convection tower capacity is able to meet or exceed the exiting water set point temperature. The air flow rate through the tower in the free convection regime is assumed to be this same fraction of the tower design air flow rate. The fraction of tower capacity in free convection regime must be greater than or equal to 0 and less than or equal to 0.2, with a default value of 0.125 if this field is left blank.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-3}
+
+This numeric field contains the capacity of the tower's electric basin heater in watts per degree Kelvin. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the tower fan is off and water is not flowing through the tower, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-3}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the tower fan is off and water is not flowing through the tower. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-3}
+
+This alpha field contains the name of the basin heater operating schedule. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the cooling tower fan is off and water is not flowing through the tower.
+
+\paragraph{Field: Evaporation Loss Mode}\label{field-evaporation-loss-mode-3}
+
+This field is used to choose which method is used to model the amount of water evaporated by the cooling tower. There are two options: `LossFactor' or `SaturatedExit'. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the tower is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the cooling tower model (and does not require additional user input).
+
+\paragraph{Field: Evaporation Loss Factor}\label{field-evaporation-loss-factor-3}
+
+This field is used to specify the rate of water evaporated from the cooling tower and lost to the outside air {[}percent/K{]}. This field is only used if the Evaporation Calculation Mode is set to LossFactor. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-degree Kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Typical values are from 0.15 to 0.27 {[}percent/K{]}. The default is 0.2.
+
+\paragraph{Field: Drift Loss Percent}\label{field-drift-loss-percent-3}
+
+This numeric field contains the percent (\%) of design water flow rate lost to the atmosphere at the design air flow rate due to drift, which is water droplets that are entrained in the airstream as it passes through the tower. Drift is assumed to vary directly with tower air flow rate ratio, and is in addition to the amount of water lost to the atmosphere due to evaporation and/or blowdown. Typical values for water usage due to drift are from 0.05 to 0.2\% of the total water circulation rate with currently-available drift eliminators from tower manufacturers. The value entered in this field must be greater than or equal to zero, and the default is zero if the field is left blank.
+
+\paragraph{Field: Blowdown Calculation Mode}\label{field-blowdown-calculation-mode-3}
+
+This field specifies which method is used to determine blowdown rates. There two options `ConcentrationRatio' or `ScheduledRate'. The choice will determine which of the two models below is used. The default is ConcentrationRatio.
+
+\paragraph{Field: Blowdown Concentration Ratio}\label{field-blowdown-concentration-ratio-3}
+
+This field is used to dynamically adjust the rate of blowdown in the cooling tower as a function of the rate of evaporation. Blowdown is water intentionally drained from the tower in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values for tower operation are 3 to 5. The default value is 3.
+
+\paragraph{Field: Blowdown Makeup Water Usage Schedule Name}\label{field-blowdown-makeup-water-usage-schedule-name-3}
+
+This alpha field contains the name of the schedule used to define the amount of water (m\(^{3}\)/s) flushed from the basin on a periodic basis to purge the condenser loop of mineral scale build-up and other contaminants. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Typical values range from 0.0002 to 0.0013 m\(^{3}\)/s (17.3 to 112.3 m\(^{3}\)/day). This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the cooling tower is active and water is flowing through the tower (regardless of the water usage defined by this schedule).
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-3}
+
+This field is optional. It is used to describe where the tower obtains water used for evaporative cooling. If blank or omitted, then the tower will obtain water directly from the mains. If the name of a WaterUser:Storage object is used here, then the tower will obtain its water from that tank. If a tank is specified, the tower will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the tower needs, then the tower will still operate and obtain the rest of the water it needs from the mains (referred to as `Starved' water).
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-3}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the cooling tower. If this field is left blank, the outdoor air conditions entering the cooling tower are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+\paragraph{Field: Number of Cells}\label{field-number-of-cells-3}
+
+This integer field contains the number of cells in the multi-cell cooling tower. If not entered, the program will assume it is a single-cell cooling tower
+
+\paragraph{Field: Cell Control}\label{field-cell-control-3}
+
+This alpha field specifies the method used to control the number of cells used to meet the load, the two choices are:
+
+\textbf{MinimalCell}: the program will use minimal number of cells needed, all other cells will be shut down with no water flow. It will attempt to use as few cells as possible to cool the fluid. In no case, however, will the flow per cell be allowed to exceed its maximum value defined by the \emph{Maximum Water Flow Rate Fraction.}
+
+\textbf{MaximalCel} : As many cells as possible will be turned on. In no case, however, will the flow per cell be allowed to drop below its minimum value specified by the \emph{Minimum Water Flow Rate Fraction}.
+
+\paragraph{Field: Cell Minimum Water Flow Rate Fraction}\label{field-cell-minimum-water-flow-rate-fraction-3}
+
+This numeric field specifies the allowable smallest fraction of the design water flow rate. Flows less than this value will commonly result in fluid distribution problems; the pressure at each nozzle will be too weak for the fluid to be sprayed out in the correct pattern, not all the fill would be wet. If this field is left blank, the default value is 0.33.
+
+\paragraph{Field: Cell Maximum~ Water Flow Rate Fraction}\label{field-cell-maximum-water-flow-rate-fraction-3}
+
+This numeric field specifies the allowable largest fraction of the design water flow rate. If this field is left blank, the default value is 2.5.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-2}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.For this component the inputs that would be altered by the sizing factor are:
+
+1.~~~~Design Water Flow Rate;
+
+2.~~~~Design Air Flow Rate;
+
+3.~~~~Design Fan Power.
+
+An example IDF specification for this object is shown below:
+
+\begin{lstlisting}
+
+CoolingTower:VariableSpeed,
+    Big Tower1,  !- Tower Name
+    Condenser 1 Inlet Node,  !- Water Inlet Node Name
+    Condenser 1 Outlet Node,  !- Water Outlet Node Name
+    YorkCalc,  !- Tower Model Type
+    ,  !- Tower Model Coefficient Name
+    25.5556,  !- Design Inlet Air Wet-Bulb Temperature {C}
+    3.8889,  !- Design Approach Temperature {C}
+    5.5556,  !- Design Range Temperature {C}
+    0.0015,  !- Design Water Flow Rate {m3/s}
+    1.6435,  !- Design Air Flow Rate {m3/s}
+    275,  !- Design Fan Power {W}
+    FanRatioCurve,  !- Fan Power Ratio - function of Air Flow Rate Curve Name
+    0.2,  !- Minimum Air Flow Rate Ratio
+    0.125,  !- Fraction of Tower Capacity in Free Convection Regime
+    450.0,  !- Basin Heater Capacity {W/K}
+    4.5,  !- Basin Heater Set Point Temperature {C}
+    BasinSchedule,  !- Basin Heater Operating Schedule Name
+    SaturatedExit,  !- Evaporation Loss Mode
+    ,  !- Evaporation Loss Factor
+    0.05,  !- Makeup Water Usage due to Drift {percent}
+    ScheduledRate,  !- Blowdown Calculation Mode
+    BlowDownSchedule,  !- Schedule Name for Makeup Water Usage due to Blowdown
+    ,  !- Name of Water Storage Tank for Supply
+    ,  !- Outdoor Air Inlet Node Name
+    4, !- Number of Cells
+    MinimalCell, !- Cell Control
+    ,  !- Cell Minimum Water Flow Rate Fraction
+    ,  !- Cell Maximum Water Flow Rate Fraction
+    1.000 ;  !- Sizing Factor
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-001}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Tower Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Tower Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Cooling Tower Fan Part Load Ratio
+\item
+  HVAC,Average,Cooling Tower Air Flow Rate Ratio
+\item
+  HVAC,Average,Cooling Tower Operating Cells Count
+\end{itemize}
+
+A tower uses either mains water or storage tank for make-up water.
+
+\emph{When mains water is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate~ {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\emph{When storage tank water is used:}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate~ {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Mains Water Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Evaporation Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Drift Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Blowdown Volume {[}m3{]}
+\end{itemize}
+
+IF specified:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Cooling Tower Fan Electric Power {[}W{]}}\label{cooling-tower-fan-electric-power-w-3}
+
+\paragraph{Cooling Tower Fan Electric Energy {[}J{]}}\label{cooling-tower-fan-electric-energy-j-3}
+
+These outputs are the electric power input to the tower fan. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{\texorpdfstring{Cooling Tower Fan Part Load Ratio {[]}}{Cooling Tower Fan Part Load Ratio }}\label{cooling-tower-fan-part-load-ratio}
+
+This is the on/off cycling rate of the tower fan when free convection cannot meet the set point temperature and the tower capacity at the minimum air flow rate ratio drives the tower exiting water temperature below the set point temperature. The fan part-load ratio is calculated as the ratio of the exiting water temperature in the free convection regime minus the exiting water temperature set point divided by the exiting water temperature in the free convection regime minus the exiting water temperature at the minimum air flow rate ratio. If tower air flow is at or above the minimum air flow rate ratio, then the tower fan part-load ratio is 1.0.
+
+\paragraph{Cooling Tower Heat Transfer Rate {[}W{]}}\label{cooling-tower-heat-transfer-rate-w-3}
+
+This is the rate at which heat is removed from the condenser water loop by the tower.
+
+\paragraph{Cooling Tower Inlet Temperature {[}C{]}}\label{cooling-tower-inlet-temperature-c-3}
+
+\paragraph{Cooling Tower Outlet Temperature {[}C{]}}\label{cooling-tower-outlet-temperature-c-3}
+
+\paragraph{Cooling Tower Mass Flow Rate {[}kg/s{]}}\label{cooling-tower-mass-flow-rate-kgs-3}
+
+These outputs are the tower water inlet and outlet temperatures, and mass flow rate of the circulating condenser water loop.
+
+\paragraph{\texorpdfstring{Cooling Tower Air Flow Rate Ratio {[]}}{Cooling Tower Air Flow Rate Ratio }}\label{cooling-tower-air-flow-rate-ratio}
+
+This is the ratio of air flow through the tower to the design air flow rate. During times when the tower can maintain the condenser loop set point temperature using free convection (when the fan in not operating), the air flow rate ratio is assumed to be equal to the field Fraction of Tower Capacity in Free Convection Regime. During times when the fan cycles on/off to maintain the outlet water set point temperature, the air flow rate ratio is calculated as the summation of Fan Part-Load Ratio multiplied by the Minimum Air Flow Rate Ratio and (1.0 - Fan Part-Load Ratio) multiplied by the fraction of Tower Capacity in Free Convection Regime.
+
+\paragraph{Cooling Tower Basin Heater Electric Power {[}W{]}}\label{cooling-tower-basin-heater-electric-power-w-3}
+
+\paragraph{Cooling Tower Basin Heater Electric Energy {[}J{]}}\label{cooling-tower-basin-heater-electric-energy-j-3}
+
+These outputs are the electric power input to the tower basin heater. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-make-up-water-volume-flow-rate-m3s-3}
+
+\paragraph{Cooling Tower Make Up Water Volume {[}m3{]}}\label{cooling-tower-make-up-water-volume-m3-3}
+
+These outputs are the water consumed by the wet cooling tower for external water sprays used to augment heat transfer. This is the total of evaporation, drift, and blowdown.
+
+\paragraph{Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-evaporation-volume-flow-rate-m3s-3}
+
+\paragraph{Cooling Tower Water Evaporation Volume {[}m3{]}}\label{cooling-tower-water-evaporation-volume-m3-3}
+
+\paragraph{Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-drift-volume-flow-rate-m3s-3}
+
+\paragraph{Cooling Tower Water Drift Volume {[}m3{]}}\label{cooling-tower-water-drift-volume-m3-3}
+
+\paragraph{Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-blowdown-volume-flow-rate-m3s-3}
+
+\paragraph{Cooling Tower Water Blowdown Volume {[}m3{]}}\label{cooling-tower-water-blowdown-volume-m3-3}
+
+These outputs provide the breakdown of the different components of water use during cooling tower operation.
+
+\paragraph{Cooling Tower Make Up Mains Water Volume {[}m3{]}}\label{cooling-tower-make-up-mains-water-volume-m3-3}
+
+This is the volume of water drawn from mains service to feed the cooling tower.~ If a water storage tank is used to provide water to the tower, then the following output variables will also be available.
+
+\paragraph{Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-storage-tank-water-volume-flow-rate-m3s-3}
+
+\paragraph{Cooling Tower Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-storage-tank-water-volume-m3-3}
+
+These are the rate and volume of water provided by the Water Storage Tank.
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-starved-storage-tank-water-volume-flow-rate-m3s-3}
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-starved-storage-tank-water-volume-m3-3}
+
+These are the rate and volume of water the Storage Tank connections was not able to provide. The starved water is assumed to come from the mains. The tower's operation is not affected by a lack of storage tank water.
+
+\paragraph{\texorpdfstring{Cooling Tower Operating Cells Count {[]}}{Cooling Tower Operating Cells Count }}\label{cooling-tower-operating-cells-count-3}
+
+This represents the number of cells operating at each time step.
+
+\subsection{CoolingTowerPerformance:CoolTools}\label{coolingtowerperformancecooltools}
+
+Variable speed cooling towers can be modeled by EnergyPlus with user-selectable performance based on the CoolTools correlation, YorkCalc correlation, or user-defined coefficients for either the CoolTools or YorkCalc correlations.The empirical CoolTools tower correlation uses a set of 35 coefficients to model the thermal performance (approach temperature) of a cooling tower based on four independent variables. If the user specifies Model Type = CoolToolsCrossFlow in the CoolingTower:VariableSpeed object, then the 35 coefficients derived for the CoolTools simulation model are used and these coefficients are already defined within EnergyPlus. If the user specifies Model Type = CoolToolsUserDefined, then the user must enter a CoolingTowerPerformance:CoolTools object to define the 35 coefficients that will be used by the CoolTools correlation.
+
+The user must specify a name for the model coefficient object, and this name must be used in the CoolingTower:VariableSpeed object (field Model Coefficient Name) to tell the program to use these coefficients. Next, the user enters the minimum and maximum values for inlet air wet-bulb temperature, range temperature, approach temperature, and water mass flow rate ratio to specify the valid range for which the model coefficients were derived. For all of these variables, the program issues warnings if the actual values are beyond the minimum/maximum values specified. For inlet air wet-bulb temperature and water mass flow rate ratio, the values of these variables used in the calculation of approach temperature are limited to be within the valid minimum/maximum range specified. For approach and range, the warnings are issued if the values are beyond the specified minimum/maximum range but the actual values are still used.
+
+The CoolTools correlation has four independent variables: inlet air wet-bulb temperature (Twb), tower range temperature (Tr), water flow rate ratio (FRwater), and air flow rate ratio (FRair). Temperatures are in units of ËšC and flow rate ratios are dimensionless (actual flow rate divided by design flow rate). Using these independent variables, tower approach temperature (ËšC) is calculated as follows:
+
+Approach = ~~ Coeff(1)~ +~ Coeff(2)•FRair~ +~ Coeff(3)•(FRair)\(^{2}\)~ +
+
+Coeff(4)•(FRair)\(^{3}\)~ +~ Coeff(5)•FRwater~ +
+
+Coeff(6)•FRair•FRwater~ +~ Coeff(7)•(FRair)\(^{2}\)•FRwater~ +
+
+Coeff(8)•(FRwater)\(^{2}\)~ +~ Coeff(9)•FRair•(FRwater)\(^{2}\)~ +
+
+Coeff(10)•(FRwater)\(^{3}\)~ +~ Coeff(11)•Twb~ +~ Coeff(12)•FRair•Twb~ +
+
+Coeff(13)•(FRair)\(^{2}\)•Twb~ +~ Coeff(14)•FRwater•Twb~ +
+
+Coeff(15)•FRair•FRwater•Twb~ +~ Coeff(16)•(FRwater)\(^{2}\)•Twb~ +
+
+Coeff(17)•(Twb)\(^{2}\)~ +~ Coeff(18)•FRair•(Twb)\(^{2}\)~ +
+
+Coeff(19)•FRwater•(Twb)\(^{2}\)~ +~ Coeff(20)•(Twb)\(^{3}\)~ +~ Coeff(21)•Tr~ +
+
+Coeff(22)•FRair•Tr~ +~ Coeff(23)•FRair•FRair•Tr~ +
+
+Coeff(24)•FRwater•Tr~ +~ Coeff(25)•FRair•FRwater•Tr~ +
+
+Coeff(26)•(FRwater)\(^{2}\)•Tr~ +~ Coeff(27)•Twb•Tr~ +
+
+Coeff(28)•FRair•Twb•Tr~ +~ Coeff(29)•FRwater•Twb•Tr~ +
+
+Coeff(30)•(Twb)\(^{2}\)•Tr~ +~ Coeff(31)•(Tr)\(^{2}\) + Coeff(32)•FRair•(Tr)\(^{2}\) +
+
+Coeff(33)•FRwater•(Tr)\(^{2}\) +~ Coeff(34)•Twb•(Tr)\(^{2}\) +~ Coeff(35)•(Tr)\(^{3}\)
+
+This object allows the user to specify model coefficients for use with the CoolTools correlation shown above. It is recommended that a broad set of cooling tower performance data be used to generate these model coefficients. The data set used to create the model coefficients should cover the entire range of water and air flow rate ratios and inlet air wet-bulb, range, and approach temperatures expected during the simulation.
+
+\subsubsection{Inputs}\label{inputs-4-005}
+
+\paragraph{Field: Name}\label{field-name-3-005}
+
+This alpha field contains the identifying name for the variable speed cooling tower model coefficients.
+
+\paragraph{Field: Minimum Inlet Air Wet-Bulb Temperature}\label{field-minimum-inlet-air-wet-bulb-temperature}
+
+This numeric field contains the minimum inlet air wet-bulb temperature to be used by the model (approach temperature correlation). Inlet air wet-bulb temperatures less than this value will not be used; instead, the minimum inlet air wet-bulb temperature specified here will be used by the correlation and a warning will be issued.
+
+\paragraph{Field: Maximum Inlet Air Wet-Bulb Temperature}\label{field-maximum-inlet-air-wet-bulb-temperature}
+
+This numeric field contains the maximum inlet air wet-bulb temperature to be used by the model (approach temperature correlation). Inlet air wet-bulb temperatures greater than this value will not be used; instead, the maximum inlet air wet-bulb temperature specified here will be used by the correlation and a warning will be issued.
+
+\paragraph{Field: Minimum Range Temperature}\label{field-minimum-range-temperature}
+
+This numeric field contains the minimum range temperature (inlet water temperature minus outlet water temperature) to be used by the empirical model. If the range temperature is less than this value the actual range temperature is still passed to the empirical model but a warning will be issued.
+
+\paragraph{Field: Maximum Range Temperature}\label{field-maximum-range-temperature}
+
+This numeric field contains the maximum range temperature (inlet water temperature minus outlet water temperature) to be used by the empirical model. If the range temperature is greater than this value the actual range temperature is still passed to the empirical model but a warning will be issued.
+
+\paragraph{Field: Minimum Approach Temperature}\label{field-minimum-approach-temperature}
+
+This numeric field contains the minimum approach temperature (outlet water temperature minus inlet air wet-bulb temperature) to be used by the empirical model. If the calculated approach temperature is less than this value then the calculated value is still used but a warning will be issued.
+
+\paragraph{Field: Maximum Approach Temperature}\label{field-maximum-approach-temperature}
+
+This numeric field contains the maximum approach temperature (outlet water temperature minus inlet air wet-bulb temperature) to be used by the empirical model. If the calculated approach temperature is greater than this value then the calculated value is still used but a warning will be issued.
+
+\paragraph{Field: Minimum Water Flow Rate Ratio}\label{field-minimum-water-flow-rate-ratio}
+
+This numeric field contains the minimum water flow rate ratio (ratio of actual water flow rate to rated water flow rate) to be used by the empirical model. Water flow rate ratios less than this value will not be used; instead, the minimum water flow rate ratio specified here will be used by the model and a warning will be issued.
+
+\paragraph{Field: Maximum Water Flow Rate Ratio}\label{field-maximum-water-flow-rate-ratio}
+
+This numeric field contains the maximum water flow rate ratio (ratio of actual water flow rate to rated water flow rate) to be used by the empirical model. Water flow rate ratios greater than this value will not be used; instead, the maximum water flow rate ratio specified here will be used by the model and a warning will be issued.
+
+\paragraph{Field: Coefficient 1 to 35}\label{field-coefficient-1-to-35}
+
+These numeric fields contain the coefficients to be used by the CoolTools approach temperature correlation shown above.
+
+An example IDF specification for this object is shown below:
+
+\begin{lstlisting}
+
+CoolingTowerPerformance:CoolTools,
+   CoolTools CrossFlow Default Model, !- Tower Model Coefficient Name
+       -1.0,               !- Minimum Inlet Air Wet-Bulb Temperature {C}
+       26.6667,            !- Maximum Inlet Air Wet-Bulb Temperature {C}
+       1.1111,             !- Minimum Range Temperature {C}
+       11.1111,            !- Maximum Range Temperature {C}
+       1.1111,             !- Minimum Approach Temperature {C}
+       11.1111,            !- Maximum Approach Temperature {C}
+       0.75,               !- Minimum Water Flow Rate Ratio
+       1.25,               !- Maximum Water Flow Rate Ratio
+       0.52049709836241,                !- Coefficient 1
+     -10.617046395344,                  !- Coefficient 2
+      10.7292974722538,                 !- Coefficient 3
+      -2.74988377158227,                !- Coefficient 4
+       4.73629943913743,                !- Coefficient 5
+      -8.25759700874711,                !- Coefficient 6
+       1.57640938114136,                !- Coefficient 7
+       6.51119643791324,                !- Coefficient 8
+       1.50433525206692,                !- Coefficient 9
+      -3.2888529287801,                 !- Coefficient 10
+       0.0257786145353773,              !- Coefficient 11
+       0.182464289315254,               !- Coefficient 12
+      -0.0818947291400898,              !- Coefficient 13
+      -0.215010003996285,               !- Coefficient 14
+       0.0186741309635284,              !- Coefficient 15
+       0.0536824177590012,              !- Coefficient 16
+      -0.00270968955115031,             !- Coefficient 17
+       0.00112277498589279,             !- Coefficient 18
+      -0.00127758497497718,             !- Coefficient 19
+       0.0000760420796601607,           !- Coefficient 20
+       1.43600088336017,                !- Coefficient 21
+      -0.5198695909109,                 !- Coefficient 22
+       0.117339576910507,               !- Coefficient 23
+       1.50492810819924,                !- Coefficient 24
+      -0.135898905926974,               !- Coefficient 25
+      -0.152577581866506,               !- Coefficient 26
+      -0.0533843828114562,              !- Coefficient 27
+       0.00493294869565511,             !- Coefficient 28
+      -0.00796260394174197,             !- Coefficient 29
+       0.000222619828621544,            !- Coefficient 30
+      -0.0543952001568055,              !- Coefficient 31
+       0.00474266879161693,             !- Coefficient 32
+      -0.0185854671815598,              !- Coefficient 33
+       0.00115667701293848,             !- Coefficient 34
+       0.000807370664460284;            !- Coefficient 35
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-001}
+
+No additional cooling tower output variables are output when this object is used.
+
+\subsection{CoolingTowerPerformance:YorkCalc}\label{coolingtowerperformanceyorkcalc}
+
+Variable speed cooling towers can be modeled by EnergyPlus with user-selectable performance based on the CoolTools correlation, YorkCalc correlation, or user-defined coefficients for either the CoolTools or YorkCalc correlations.The empirical YorkCalc tower correlation uses a set of 27 coefficients to model the thermal performance (approach temperature) of a variable speed cooling tower based on three independent variables. If the user specifies Tower Model Type = YorkCalc in the CoolingTower:VariableSpeed object, then the 27 coefficients derived for the YorkCalc simulation model are used and these coefficients are already defined within EnergyPlus. If the user specifies Tower Model Type = YorkCalcUserDefined, then the user must enter a CoolingTowerPerformance:YorkCalc object to define the 27 coefficients that will be used by the YorkCalc correlation.
+
+The user must specify a name for the model coefficient object, and this name must be used in the CoolingTower:VariableSpeed object (field Model Coefficient Name) to tell the program to use these coefficients. Next, the user enters the minimum and maximum values for inlet air wet-bulb temperature, range temperature, approach temperature, and water mass flow rate ratio to specify the valid range for which the model coefficients were derived. The user also specifies the maximum valid liquid-to-gas ratio. For all of these variables, the program issues warnings if the actual values are beyond the minimum/maximum values specified. For inlet air wet-bulb temperature and water mass flow rate ratio, the values of these variables used in the calculation of approach temperature are limited to be within the valid minimum/maximum range specified. For approach, range, and liquid-to-gas ratio the warnings are issued if the values are beyond the specified minimum/maximum range but the actual values are still used.
+
+The YorkCalc correlation has three independent variables: inlet air wet-bulb temperature (Twb), tower range temperature (Tr), and the liquid-to-gas ratio (ratio of water flow rate ratio to air flow rate ratio = LGRatio). Temperatures are in units of ËšC and liquid-to-gas ratio is dimensionless. Using these independent variables, an approach temperature (ËšC) is calculated as follows:
+
+~~~ Approach = ~~~~~ Coeff(1)~ +~ Coeff(2)•Twb~ +~ Coeff(3)•Twb\(^{2}\) +~ Coeff(4)•Tr~ +
+
+Coeff(5)•Twb•Tr~ +~ Coeff(6)•Twb\(^{2}\)•Tr~ +~ Coeff(7)•Tr\(^{2}\)~ +
+
+Coeff(8)•Twb•Tr\(^{2}\) +~ Coeff(9)•Twb\(^{2}\)•Tr\(^{2}\) + Coeff(10)•LGRatio~ +
+
+Coeff(11)•Twb•LGRatio~ +~ Coeff(12)•Twb\(^{2}\)•LGRatio~ +
+
+Coeff(13)•Tr•LGRatio~ +~ Coeff(14)•Twb•Tr•LGRatio~ +
+
+Coeff(15)•Twb\(^{2}\)•Tr•LGRatio~ +~ Coeff(16)•Tr\(^{2}\)•LGRatio~ +
+
+Coeff(17)•Twb•Tr\(^{2}\)•LGRatio~ +~ Coeff(18)•Twb\(^{2}\)•Tr\(^{2}\)•LGRatio +
+
+Coeff(19)•LGRatio\(^{2}\) +~ Coeff(20)•Twb•LGRatio\(^{2}\)~ +
+
+Coeff(21)• Twb\(^{2}\)•LGRatio\(^{2}\) +~ Coeff(22)•Tr•LGRatio\(^{2}\) +
+
+Coeff(23)•Twb•Tr•LGRatio\(^{2}\) +~ Coeff(24)•Twb\(^{2}\)•Tr•LGRatio\(^{2}\) +
+
+Coeff(25)•Tr\(^{2}\)•LGRatio\(^{2}\) +~ Coeff(26)•Twb•Tr\(^{2}\)•LGRatio\(^{2}\) +
+
+Coeff(27)•Twb\(^{2}\)•Tr\(^{2}\)•LGRatio\(^{2}\)
+
+This object allows the user to specify model coefficients for use with the YorkCalc correlation shown above. It is recommended that a broad set of cooling tower performance data be used to generate these model coefficients. The data set used to create the model coefficients should cover the entire range of water and air flow rate ratios and inlet air wet-bulb, range, and approach temperatures expected during the simulation.
+
+\subsubsection{Inputs}\label{inputs-5-005}
+
+\paragraph{Field: Name}\label{field-name-4-005}
+
+This alpha field contains the identifying name for the variable speed cooling tower model coefficients.
+
+\paragraph{Field: Minimum Inlet Air Wet-Bulb Temperature}\label{field-minimum-inlet-air-wet-bulb-temperature-1}
+
+This numeric field contains the minimum inlet air wet-bulb temperature to be used by the model (approach temperature correlation). Inlet air wet-bulb temperatures less than this value will not be used; instead, the minimum inlet air wet-bulb temperature specified here will be used by the correlation and a warning will be issued.
+
+\paragraph{Field: Maximum Inlet Air Wet-Bulb Temperature}\label{field-maximum-inlet-air-wet-bulb-temperature-1}
+
+This numeric field contains the maximum inlet air wet-bulb temperature to be used by the model (approach temperature correlation). Inlet air wet-bulb temperatures greater than this value will not be used; instead, the maximum inlet air wet-bulb temperature specified here will be used by the model and a warning will be issued.
+
+\paragraph{Field: Minimum Range Temperature}\label{field-minimum-range-temperature-1}
+
+This numeric field contains the minimum range temperature (inlet water temperature minus outlet water temperature) to be used by the empirical model. If the range temperature is less than this value the actual range temperature is still passed to the empirical model but a warning will be issued.
+
+\paragraph{Field: Maximum Range Temperature}\label{field-maximum-range-temperature-1}
+
+This numeric field contains the maximum range temperature (inlet water temperature minus outlet water temperature) to be used by the empirical model. If the range temperature is greater than this value the actual range temperature is still passed to the empirical model but a warning will be issued.
+
+\paragraph{Field: Minimum Approach Temperature}\label{field-minimum-approach-temperature-1}
+
+This numeric field contains the minimum approach temperature (outlet water temperature minus inlet air wet-bulb temperature) to be used by the empirical model. If the calculated approach temperature is less than this value then the calculated value is still used but a warning will be issued.
+
+\paragraph{Field: Maximum Approach Temperature}\label{field-maximum-approach-temperature-1}
+
+This numeric field contains the maximum approach temperature (outlet water temperature minus inlet air wet-bulb temperature) to be used by the empirical model. If the calculated approach temperature is greater than this value then the calculated value is still used but a warning will be issued.
+
+\paragraph{Field: Minimum Water Flow Rate Ratio}\label{field-minimum-water-flow-rate-ratio-1}
+
+This numeric field contains the minimum water flow rate ratio (ratio of actual water flow rate to rated water flow rate) to be used by the empirical model. Water flow rate ratios less than this value will not be used; instead, the minimum water flow rate ratio specified here will be used by the model and a warning will be issued.
+
+\paragraph{Field: Maximum Water Flow Rate Ratio}\label{field-maximum-water-flow-rate-ratio-1}
+
+This numeric field contains the maximum water flow rate ratio (ratio of actual water flow rate to rated water flow rate) to be used by the empirical model. Water flow rate ratios greater than this value will not be used; instead, the maximum water flow rate ratio specified here will be used by the model and a warning will be issued.
+
+\paragraph{Field: Maximum Liquid to Gas Ratio}\label{field-maximum-liquid-to-gas-ratio}
+
+This numeric field contains the maximum liquid-to-gas ratio (ratio of actual water flow rate ratio {[}capped to be within the minimum/maximum water flow rate ratio defined above as necessary{]} to actual air flow rate ratio) to be used by the empirical model. If the liquid-to-gas ratio is greater than this value the actual liquid to gas ratio is still passed to the empirical model but a warning will be issued.
+
+\paragraph{Field: Coefficient 1 to 27}\label{field-coefficient-1-to-27}
+
+These numeric fields contain the coefficients to be used by the YorkCalc approach temperature correlation shown above.
+
+An example IDF specification for this object is shown below:
+
+\begin{lstlisting}
+
+CoolingTowerPerformance:YorkCalc
+   YorkCalc Default Tower Model, !- Tower Model Coefficient Name
+       -34.4,              !- Minimum Inlet Air Wet-Bulb Temperature {C}
+       26.6667,            !- Maximum Inlet Air Wet-Bulb Temperature {C}
+       1.1111,             !- Minimum Range Temperature {C}
+       22.2222,            !- Maximum Range Temperature {C}
+       1.1111,             !- Minimum Approach Temperature {C}
+       40.0,               !- Maximum Approach Temperature {C}
+       0.75,               !- Minimum Water Flow Rate Ratio
+       1.25,               !- Maximum Water Flow Rate Ratio
+       8.0,                !- Maximum Liquid to Gas Ratio
+      -0.359741205,                     !- Coefficient 1
+      -0.055053608,                     !- Coefficient 2
+       0.0023850432,                    !- Coefficient 3
+       0.173926877,                     !- Coefficient 4
+      -0.0248473764,                    !- Coefficient 5
+       0.00048430224,                   !- Coefficient 6
+      -0.005589849456,                  !- Coefficient 7
+       0.0005770079712,                 !- Coefficient 8
+      -0.00001342427256,                !- Coefficient 9
+       2.84765801111111,                !- Coefficient 10
+      -0.121765149,                     !- Coefficient 11
+       0.0014599242,                    !- Coefficient 12
+       1.680428651,                     !- Coefficient 13
+      -0.0166920786,                    !- Coefficient 14
+      -0.0007190532,                    !- Coefficient 15
+      -0.025485194448,                  !- Coefficient 16
+       0.0000487491696,                 !- Coefficient 17
+       0.00002719234152,                !- Coefficient 18
+      -0.0653766255555556,              !- Coefficient 19
+      -0.002278167,                     !- Coefficient 20
+       0.0002500254,                    !- Coefficient 21
+      -0.0910565458,                    !- Coefficient 22
+       0.00318176316,                   !- Coefficient 23
+       0.000038621772,                  !- Coefficient 24
+      -0.0034285382352,                 !- Coefficient 25
+       0.00000856589904,                !- Coefficient 26
+      -0.000001516821552;               !- Coefficient 27
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-001}
+
+No additional cooling tower output variables are output when this object is used.
+
+\subsection{EvaporativeFluidCooler:SingleSpeed}\label{evaporativefluidcoolersinglespeed}
+
+Evaporative fluid coolers are components that may be assigned to condenser loops. The Evaporative fluid cooler is modeled as a counter flow heat exchanger with single-speed fans (induced draft configuration). The user must define fluid cooler performance via one of three methods: design heat transfer coefficient-area product (UA) and design water flow rate, or standard fluid cooler design capacity at a specific rating point or design capacity at non standard conditions. Regardless of which method is chosen, the design airflow rate and corresponding fan power must be specified.
+
+The evaporative fluid cooler seeks to maintain the temperature of the water exiting the evaporative fluid cooler at (or below) a set point. The set point schedule value is defined by the field ``Condenser Loop Temperature Setpoint Node Name or Reference'' for the CondenserLoop object. The model first checks to see whether inlet water temperature is at or below the set point. If so, then the fluid cooler fan is not turned on and all the flow goes through bypass. If the inlet water temperature is above the set point then the fluid cooler fan is turned on to reduce the exiting water temperature to the set point. If the capacity control is FanCycling, the model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., fluid cooler fan on for the entire simulation timestep and fluid cooler fan off for the entire simulation timestep). Cyclic losses are not taken into account. If the capacity control is FluidBypass, the model determines the fraction of water flow to be bypassed while the remaining water goes through the fluid cooler cooling media and gets cooled, then the two water flows mix to meet the setpoint temperature. In this case, the fan runs at full speed for the entire timestep.
+
+Evaporative fluid coolers consume water through evaporation, drift, and blowdown. The model can be used to predict water consumed by the fluid coolers. For this purpose, the last seven input fields can either be provided in the input or if nothing is specified then the default values for these fields will be used. These fields provide the methods of controlling details of the water consumption calculations. The user can specify connections to the rest of the building's water system by providing the name of a water storage tanks (i.e.~WaterUse:Storage objects). The schematic of the system is shown below:
+
+\begin{figure}[hbtp] % fig 82
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image201.png}
+\caption{Schematic diagram for evaporative fluid cooler \protect \label{fig:schematic-diagram-for-evaporative-fluid}}
+\end{figure}
+
+Where,
+
+\begin{itemize}
+\item
+  h = Enthalpy (j/kg-K)
+\item
+  m = mass flow rate (kg/s)
+\item
+  Subscripts
+\item
+  a = air
+\item
+  w = water
+\item
+  wb = wet-bulb
+\item
+  in = inlet
+\item
+  out = outlet
+\end{itemize}
+
+\subsubsection{Inputs}\label{inputs-6-004}
+
+\paragraph{Field: Name}\label{field-name-5-005}
+
+This alpha field contains the identifying name for the fluid cooler.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-4}
+
+This alpha field contains the identifying name for the fluid cooler's water inlet node.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-4}
+
+This alpha field contains the identifying name for the fluid cooler's water outlet node.
+
+\paragraph{Field: Design Air Flow Rate}\label{field-design-air-flow-rate-3}
+
+This numeric field contains the design air flow rate induced by the fluid cooler fan in m\(^{3}\)/s. The field must contain a value greater than zero regardless of the fluid cooler performance input method. Alternately, this field can be autosized. See Engineering Reference document for autosizing calculations.
+
+\paragraph{Field: Design Air Flow Rate Fan Power}\label{field-design-air-flow-rate-fan-power}
+
+This numeric field contains the fan power (in watts) at the design air flow rate specified in the previous field. The field must contain a value greater than zero regardless of the fluid cooler performance input method. Alternately, this field can be autosized. See Engineering Reference document for autosizing calculations.
+
+\paragraph{Field: Design Spray Water Flow Rate}\label{field-design-spray-water-flow-rate}
+
+This numeric field contains the design spray water flow rate through the fluid cooler in m\(^{3}\)/s. A value greater than zero must be specified regardless of the performance input method,
+
+\paragraph{Field: Performance Input Method}\label{field-performance-input-method-3}
+
+This alpha field contains the method by which the user will specify fluid cooler performance: ``UFactorTimesAreaAndDesignWaterFlowRate'' or ``StandardDesignCapacity'' or ``UserSpecifiedDesignCapacity''.
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-4}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the fluid cooler. If this field is left blank, the outdoor air conditions entering the fluid cooler are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+\paragraph{Field: Heat Rejection Capacity and Nominal Capacity Sizing Ratio}\label{field-heat-rejection-capacity-and-nominal-capacity-sizing-ratio-3}
+
+This numeric field contains the value for the ratio of actual tower heat rejection to nominal capacity.~ This ratio is defined at entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. Historically this ratio has been set at 1.25 based on the assumption that the tower must dissipate 0.25 W of compressor power for every what of heat removed at the chiller evaporator.~ The default is 1.25.
+
+\paragraph{Field: Standard Design Capacity}\label{field-standard-design-capacity}
+
+This numeric input field contains the heat rejection capacity of the fluid cooler in watts, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of nominal capacity (3 gpm/ton). 125\% of this capacity gives the actual fluid cooler heat rejection at these operating conditions (based on historical assumption that the evaporative fluid cooler must dissipate 0.25W of compressor heat for every watt of heat removed by the evaporator). This field is only used for performance input method = ''StandardDesignCapacity''. For other input methods this field is ignored. The standard conditions mentioned above for ``standard design capacity'' are already specified in the EnergyPlus. So the input fields such as design entering water temp., design entering air wet-bulb and dry-bulb temp. and design water flow rate, if provided in the input, will be ignored for the StandardDesignCapacity performance input method. Also, the standard conditions are for water as a fluid type so this performance input method can only be used with water as a fluid type (ref. CondenserLoop object).
+
+\paragraph{Field: Design Air Flow Rate U-factor Times Area Value}\label{field-design-air-flow-rate-u-factor-times-area-value-1}
+
+This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the design air and water flow rates specified above. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design fluid cooler UA value is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), the fluid cooler inlet air dry-bulb and wetbulb temperature are taken from the input. This field is only used for performance input method = '' UFactorTimesAreaAndDesignWaterFlowRate''. For other performance input methods, this field is ignored.
+
+\paragraph{Field: Design Water Flow Rate}\label{field-design-water-flow-rate-4}
+
+This numeric field contains the design water flow rate through the fluid cooler in m\(^{3}\)/s. This value is the flow rate of the condenser loop water being cooled by the fluid cooler. This field is ignored for the ``StandardDesignCapacity'' performance input method. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections).
+
+\paragraph{Field: User Specified Design Capacity}\label{field-user-specified-design-capacity}
+
+This numeric input field contains the heat rejection capacity of the fluid cooler in watts. Design conditions for this capacity i.e.~entering air dry-bulb temperature, entering air wet-bulb temperature and entering water temperature must be provided in the input. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
+
+\paragraph{Field:Design Entering Water Temperature}\label{fielddesign-entering-water-temperature}
+
+This numeric field contains entering water temperature at nominal conditions in degrees Celsius. The design entering water temperature must be greater than the design entering air temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
+
+\paragraph{Field:Design Entering Air Temperature}\label{fielddesign-entering-air-temperature}
+
+This numeric field contains entering air dry-bulb temperature at nominal conditions in degrees Celsius. The design entering air temperature must be greater than the design entering air wet-bulb temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
+
+\paragraph{Field:Design Entering Air Wet-bulb Temperature}\label{fielddesign-entering-air-wet-bulb-temperature}
+
+This numeric field contains entering air wetbulb temperature at nominal conditions in degrees Celsius. The design entering air wet-bulb temperature must be less than the design entering air (dry-bulb) temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
+
+\paragraph{Field: Capacity Control}\label{field-capacity-control}
+
+This alpha field contains the cooling capacity control for the evaporative fluid cooler. Two choices are available: FanCycling and FluidBypass. During part-load conditions, there are two ways to maintain the exiting water temperature at the setpoint: either cycling the evaporative fluid cooler fan, or bypassing portion of the evaporative fluid cooler water with a three-way valve. For FluidBypass, the evaporative fluid cooler fan still runs at full speed for the entire timestep, but only portion of the water flow goes through the evaporative fluid cooler media to get cooled while the remaining portion of the water flow gets bypassed. Two water flows then mix at the common water sump to meet the setpoint temperature.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-3}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature. For this component the inputs that would be altered by the sizing factor are:
+
+1.~~ Design Water Flow Rate;
+
+2.~~ Design Air Flow Rate;
+
+3.~~ Fan Power at Design Air Flow Rate;
+
+4.~~ U-Factor Times Area Value at Design Air Flow Rate;
+
+Note that the U-Factor Times Area Value at Design Air Flow Rate is not multiplied by the Sizing Factor. Instead the design evaporative fluid cooler load is multiplied by the sizing factor and the design UA then calculated as usual.
+
+\paragraph{Field: Evaporation Loss Mode}\label{field-evaporation-loss-mode-4}
+
+This field is used to choose which method is used to model the amount of water evaporated by the evaporative fluid cooler. There are two options: LossFactor or SaturatedExit. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the evaporative fluid cooler is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the evaporative fluid cooler model (and does not require additional user input).
+
+\paragraph{Field: Evaporation Loss Factor}\label{field-evaporation-loss-factor-4}
+
+This field is used to specify the rate of water evaporated from the evaporative fluid cooler and lost to the outside air {[}percent/K{]}. This field is only used if the Evaporation Calculation Mode is set to LossFactor. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Empirical correlation is used to calculate default loss factor if it not explicitly specified in the input file.
+
+\paragraph{Field: Drift Loss Percent}\label{field-drift-loss-percent-4}
+
+This field is used to specify the rate of water lost to the exiting air as entrained droplets {[}\%{]}. The drift loss is a percent of the condenser water flow. Default value is under investigation for now cooling tower's evaporation loss factor is taken as default value.
+
+\paragraph{Field: Blowdown Calculation Mode}\label{field-blowdown-calculation-mode-4}
+
+This field specifies which method is used to determine blowdown rates. There two options ConcentrationRatio or ScheduledRate. The choice will determine which of the two models below is used. The default is ConcentrationRatio.
+
+\paragraph{Field: Blowdown Concentration Ratio}\label{field-blowdown-concentration-ratio-4}
+
+This field is used to dynamically adjust the rate of blowdown in the evaporative fluid cooler as a function of the rate of evaporation. Blowdown is water intentionally drained from the evaporative fluid cooler in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Default value is under investigation for now cooling tower's evaporation loss factor is taken as default value.
+
+\paragraph{Field: Blowdown Makeup Water Usage Schedule Name}\label{field-blowdown-makeup-water-usage-schedule-name-4}
+
+This alpha field contains the name of the schedule used to define the amount of water (m3/s) flushed from the basin on a periodic basis to purge the evaporative fluid cooler of mineral scale build-up and other contaminants. This schedule is only used if the Blowdown Calculation Mode is set to ScheduledRate. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Default value is under investigation for now cooling tower's evaporation loss factor is taken as default value.This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the evaporative fluid cooler is active and water is flowing through the evaporative fluid cooler (regardless of the water usage defined by this schedule).
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-4}
+
+This field is optional. It is used to describe where the evaporative fluid cooler obtains water used for evaporative cooling. If blank or omitted, then the evaporative fluid cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the evaporative fluid cooler will obtain its water from that tank. If a tank is specified, the evaporative fluid cooler will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the evaporative fluid cooler needs, then the evaporative fluid cooler will still operate and obtain the rest of the water it needs from the mains (referred to as `Starved' water).
+
+An IDF specification for this object is shown below:
+
+\begin{lstlisting}
+
+EvaporativeFluidCooler:SingleSpeed,
+      Big EvaporativeFluidCooler,         !- Name
+      Condenser EvaporativeFluidcooler Inlet Node,  !- Water Inlet Node Name
+      Condenser EvaporativeFluidcooler Outlet Node,  !- Water Outlet Node Name
+      3.02,                    !- Design Air Flow Rate {m3/s}
+      2250,                    !- Design Air Flow Rate Fan Power {W}
+      0.002208,                !- Design Spray Water Flow Rate {m3/s}
+      UserSpecifiedDesignCapacity,                        !- Performance Input Method
+      ,                        !- Outdoor Air Inlet Node Name
+      1.25,                    !- Heat Rejection Capacity and Nominal Capacity Sizing Ratio
+      ,                        !- Standard Design Capacity {W}
+      ,                        !- Design Air Flow Rate U-factor Times Area Value {W/K}
+      0.001703,                !- Design Water Flow Rate {m3/s}
+      87921,                   !- User Specified Design Capacity {W}
+      46.11,                   !- Design Entering Water Temperature {C}
+      35,                      !- Design Entering Air Temperature {C}
+      25.6;                    !- Design Entering Air Wet-bulb Temperature {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-001}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Tower Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Tower Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Cooling Tower Bypass Fraction {[]}
+\item
+  HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Water Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Evaporation Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Evaporative Fluid Cooler Water Drift {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Blowdown Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Mains Water Volume {[}m3{]}
+\end{itemize}
+
+If Supply Water Storage Tank Name is specified:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Cooling Tower Fan Electric Power {[}W{]}}\label{cooling-tower-fan-electric-power-w-4}
+
+The average electric power consumption of the fluid cooler fan in Watts for the timestep being reported.
+
+\paragraph{Cooling Tower Fan Electric Energy {[}J{]}}\label{cooling-tower-fan-electric-energy-j-4}
+
+Fan energy use in Joules.~ Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Cooling Tower Heat Transfer Rate {[}W{]}}\label{cooling-tower-heat-transfer-rate-w-4}
+
+This is the average rate, in Watts, at which heat is removed from the condenser water loop by the fluid cooler for the time step being reported.
+
+\paragraph{Cooling Tower Inlet Temperature {[}C{]}}\label{cooling-tower-inlet-temperature-c-4}
+
+The fluid temperature at the fluid cooler inlet in degrees Celsius.
+
+\paragraph{Cooling Tower Outlet Temperature {[}C{]}}\label{cooling-tower-outlet-temperature-c-4}
+
+The fluid temperature at the fluid cooler outlet in degrees Celsius.
+
+\paragraph{Cooling Tower Mass Flow Rate {[}kg/s{]}}\label{cooling-tower-mass-flow-rate-kgs-4}
+
+The average fluid mass flow rate through the fluid cooler in kg/s for the time step being reported.
+
+\paragraph{\texorpdfstring{Cooling Tower Bypass Fraction {[]}}{Cooling Tower Bypass Fraction }}\label{cooling-tower-bypass-fraction-1}
+
+This output is the average fluid bypass fraction for the time step being reported. See Capacity Control input field.
+
+\paragraph{Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-make-up-water-volume-flow-rate-m3s-4}
+
+\paragraph{Cooling Tower Make Up Water Volume {[}m3{]}}\label{cooling-tower-make-up-water-volume-m3-4}
+
+These outputs are the external spray water consumed by the evaporative fluid cooler. This is the total of evaporation, drift, and blowdown.
+
+\paragraph{Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-evaporation-volume-flow-rate-m3s-4}
+
+\paragraph{Cooling Tower Water Evaporation Volume {[}m3{]}}\label{cooling-tower-water-evaporation-volume-m3-4}
+
+\paragraph{Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-drift-volume-flow-rate-m3s-4}
+
+\paragraph{Cooling Tower Water Drift Volume~ {[}m3{]}}\label{cooling-tower-water-drift-volume-m3-4}
+
+\paragraph{Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-blowdown-volume-flow-rate-m3s-4}
+
+\paragraph{Cooling Tower Water Blowdown Volume {[}m3{]}}\label{cooling-tower-water-blowdown-volume-m3-4}
+
+These outputs provide the breakdown of the different components of water use during fluid cooler operation.
+
+\paragraph{Cooling Tower Make Up Mains Water Volume {[}m3{]}}\label{cooling-tower-make-up-mains-water-volume-m3-4}
+
+The volume of make up water provided by the mains in cubic meters. If no Supply Water Storage Tank is specified, then all fluid cooler make up water is provided by the mains (same as Cooling Tower Make Up Water Volume). If a Supply Water Storage Tank is specified, then the make up from the mains only occurs when sufficient water supply is not available from the tank (same as Evaporative Fluid Cooler Water Starved by Storage Tank). This output variable is metered on HeatRejection:MainsWater, MainsWater:Plant and MainsWater:Facility.
+
+\paragraph{Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-storage-tank-water-volume-flow-rate-m3s-4}
+
+\paragraph{Cooling Tower Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-storage-tank-water-volume-m3-4}
+
+These are the rate and volume of water provided by the Supply Water Storage Tank.
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-starved-storage-tank-water-volume-flow-rate-m3s-4}
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-starved-storage-tank-water-volume-m3-4}
+
+These are the rate and volume of water the Supply Water Storage Tank was not able to provide. The starved water is assumed to come from the mains. The fluid cooler's operation is not affected by a lack of storage tank water.
+
+\subsection{EvaporativeFluidCooler:TwoSpeed}\label{evaporativefluidcoolertwospeed}
+
+The two-speed evaporative fluid cooler is modeled in a similar fashion to the single-speed evaporative fluid cooler. The evaporative fluid cooler is modeled as a counter flow heat exchanger with two-speed fan (induced draft configuration. See schematic diagram in EvaporativeFluidCooler:SingleSpeed section). The user must define fluid cooler performance via one of the three methods: design heat transfer coefficient-area product (UA) and design water flow rate, or standard fluid cooler design capacity at a specific rating point or design capacity at non standard conditions. Regardless of which method is chosen, the design airflow rate and corresponding fan power must be specified.
+
+The evaporative fluid cooler seeks to maintain the temperature of the water exiting the evaporative fluid cooler at (or below) a set point. The set point schedule value is defined by the field ``Condenser Loop Temperature Setpoint Node Name or Reference'' for the CondenserLoop object. The model first checks to see whether inlet water temperature is at or below the set point. If so, then the fluid cooler fan is not turned on and all the flow goes through bypass. If the inlet water temperature is above the set point then the fluid cooler fan is turned on at low speed to reduce the exiting water temperature to the set point. If operating the fluid cooler fan at low speed does not reduce the exiting water temperature to the set point, then the fluid cooler fan is increased to its high speed.
+
+The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., fluid cooler fan at high speed for the entire simulation timestep and fluid cooler fan at low speed for the entire simulation timestep, or fluid cooler fan at low speed for the entire simulation timestep and fluid cooler fan off for the entire simulation timestep). Cyclic losses are not taken into account.
+
+Evaporative fluid coolers consume water through evaporation, drift, and blowdown. The model can be used to predict water consumed by the evaporative fluid coolers. For this purpose, the last seven input fields can either be provided in the input or if nothing is specified then the default values for these fields will be used. These fields provide methods of controlling details of the water consumption calculations. The user can specify connections to the rest of the buildings water system by providing the name of a water storage tanks (i.e.~WaterUse:Storage objects).
+
+\subsubsection{Inputs}\label{inputs-7-004}
+
+\paragraph{Field: Name}\label{field-name-6-004}
+
+This alpha field contains the identifying name for the fluid cooler.
+
+\paragraph{Field: WaterInlet Node Name}\label{field-waterinlet-node-name}
+
+This alpha field contains the identifying name for the fluid cooler's water inlet node.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-5}
+
+This alpha field contains the identifying name for the fluid cooler's water outlet node.
+
+\paragraph{Field: High Fan Speed Air Flow Rate}\label{field-high-fan-speed-air-flow-rate-1}
+
+This numeric field contains the fluid cooler air flow rate at high fan speed in m\(^{3}\)/s. A value greater than zero must be defined regardless of fluid cooler performance input method. Alternately, this field can be autosized. See Engineering Reference document for fluid cooler autosizing.
+
+\paragraph{Field: High Fan Speed Fan Power}\label{field-high-fan-speed-fan-power}
+
+This numeric field contains the fan power (in Watts) at the high-speed air flow rate specified in the previous field. A value greater than zero must be specified regardless of fluid cooler performance input method, or this field can be autosized. See Engineering Reference document for fluid cooler autosizing.
+
+\paragraph{Field: Low Fan Speed Air Flow Rate}\label{field-low-fan-speed-air-flow-rate-1}
+
+This numeric field contains the fluid cooler air flow rate at low fan speed in m\(^{3}\)/s. This value must be greater than zero, less than the value specified for the field ``Air Flow Rate at High Fan Speed''. This field may be autocalculated, in which case it is set to a fraction of the ``Air Flow Rate at High Fan Speed'' determined in the following field.
+
+\paragraph{Field: Low Fan Speed Air Flow Rate Sizing Factor}\label{field-low-fan-speed-air-flow-rate-sizing-factor-1}
+
+This numeric field contains the sizing factor for calculating the low fan speed air flow rate as a fraction of the high fan speed air flow rate.~ The default is 0.5.
+
+\paragraph{Field: Low Fan Speed Fan Power}\label{field-low-fan-speed-fan-power-1}
+
+This numeric field contains the fan power (in Watts) at the low-speed air flow rate specified in the previous field. This value must be specified greater than zero or the field may be autocalculated, in which case it is set to a fraction of the ``Fan Power at High Fan Speed'' determined in the following field.
+
+\paragraph{Field: Low Fan Speed Fan Power Sizing Factor}\label{field-low-fan-speed-fan-power-sizing-factor-1}
+
+This numeric field contains the sizing factor for calculating the low fan speed fan power as a fraction of the high fan speed fan power. ~The default is 0.16.
+
+\paragraph{Field: Design Spray Water Flow Rate}\label{field-design-spray-water-flow-rate-1}
+
+This numeric field contains the design spray water flow rate through the fluid cooler in m\(^{3}\)/s. This input field must be specified for all the performance input methods.
+
+\paragraph{Field: Performance Input Method}\label{field-performance-input-method-4}
+
+This alpha field contains the method by which the user will specify fluid cooler performance: ``UFactorTimesAreaAndDesignWaterFlowRate'' or ``StandardDesignCapacity'' or ``UserSpecifiedDesignCapacity''.
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-5}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the fluid cooler. If this field is left blank, the outdoor air conditions entering the fluid cooler are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+\paragraph{Field: Heat Rejection Capacity and Nominal Capacity Sizing Ratio}\label{field-heat-rejection-capacity-and-nominal-capacity-sizing-ratio-4}
+
+This numeric field contains the value for the ratio of actual tower heat rejection to nominal capacity.~ This ratio is defined at entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. Historically this ratio has been set at 1.25 based on the assumption that the tower must dissipate 0.25 W of compressor power for every what of heat removed at the chiller evaporator.~ The default is 1.25.
+
+\paragraph{Field: High Speed Standard Design Capacity}\label{field-high-speed-standard-design-capacity}
+
+This numeric input field contains the heat rejection capacity of the fluid cooler in watts, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of nominal capacity (3 gpm/ton). The Heat Rejection Capacity and Nominal Capacity Sizing Ratio set in the previous field is applied to this capacity to give the actual fluid cooler heat rejection at these operating conditions. This field is only used for performance input method = ''StandardDesignCapacity''. For other input methods this field is ignored. The standard conditions mentioned above for ``standard design capacity'' are already specified in the EnergyPlus. So the input fields such as design entering water temp., design entering air wet-bulb and dry-bulb temp. and design water flow rate, if provided in the input, will be ignored for the StandardDesignCapacity performance input method. Also, the standard conditions are for water as a fluid type so this performance input method can only be used with water as a fluid type (ref. CondenserLoop object).
+
+\paragraph{Field: Low Speed Standard Design Capacity}\label{field-low-speed-standard-design-capacity}
+
+This numeric input field contains the heat rejection capacity of the fluid cooler in watts, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m\(^{3}\)/s per watt of nominal capacity (3 gpm/ton). The Heat Rejection Capacity and Nominal Capacity Sizing Ratio is applied to this capacity to give the actual fluid cooler heat rejection at these operating conditions. This field is only used for performance input method = ''StandardDesignCapacity''. For other input methods this field is ignored. The standard conditions mentioned above for ``standard design capacity'' are already specified in the EnergyPlus. So the input fields such as design entering water temp., design entering air wet-bulb and dry-bulb temp. and design water flow rate, if provided in the input, will be ignored for the StandardDesignCapacity performance input method. Also, the standard conditions are for water as a fluid type so this performance input method can only be used with water as a fluid type (ref. CondenserLoop object). The value specified for this field must be greater than zero but less than the value specified for the field ``High-Speed Standard Design Capacity''. This field may be autocalculated, in which case it is set to a fraction of the High-Speed Standard Design Capacity determined in the following field.
+
+\paragraph{Field: Low Speed Standard Capacity Sizing Factor}\label{field-low-speed-standard-capacity-sizing-factor}
+
+This numeric field contains the sizing factor to use when calculating the Low Speed Standard Design Capacity.~ The default is 0.5.
+
+\paragraph{Field: High Fan Speed U-factor Times Area Value}\label{field-high-fan-speed-u-factor-times-area-value-1}
+
+This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the high speed design air and water flow rates specified above. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a UA value greater than zero but less than or equal to 2,100,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design fluid cooler UA value is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), the fluid cooler inlet air dry-bulb and wetbulb temperature are taken from the input. This field is only used for performance input method = '' UFactorTimesAreaAndDesignWaterFlowRate''. For other input methods this field is ignored.
+
+\paragraph{Field: Low Fan Speed U-factor Times Area Value}\label{field-low-fan-speed-u-factor-times-area-value-1}
+
+This numeric field contains the heat transfer coefficient-area product (UA) in watts per degree Kelvin corresponding to the low speed design air and water flow rates specified above. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a UA value greater than zero but less than or equal to 300,000 and less than the value specified for the field ``U-Factor Times Area Value at High Fan Speed'' must be defined. This field may be autocalculated, in which case it is set to a factor of the ``U-Factor Times Area Value at High Fan Speed'' determined in the following field. This field is only used for performance input method = '' UFactorTimesAreaAndDesignWaterFlowRate''. For other input methods this field is ignored.
+
+\paragraph{Field: Low Fan Speed U-Factor Times Area Sizing Factor}\label{field-low-fan-speed-u-factor-times-area-sizing-factor-1}
+
+This field contains the sizing factor to use when calculating the Low Fan Speed U-Factor Times Area Value.~ The default is 0.6.
+
+\paragraph{Field: Design Water Flow Rate}\label{field-design-water-flow-rate-5}
+
+This numeric field contains the design water flow rate through the fluid cooler in m\(^{3}\)/s. This value is the flow rate of the condenser loop water being cooled by the fluid cooler. This field is ignored for the ``StandardDesignCapacity'' performance input method. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections).
+
+\paragraph{Field: High Speed User Specified Design Capacity}\label{field-high-speed-user-specified-design-capacity}
+
+This numeric input field contains the heat rejection capacity of the fluid cooler in watts. Design conditions for this capacity i.e.~entering air dry-bulb temperature, entering air wet-bulb temperature and entering water temperature must be provided in the input. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
+
+\paragraph{Field: Low Speed User Specified Design Capacity}\label{field-low-speed-user-specified-design-capacity}
+
+This numeric input field contains the heat rejection capacity of the fluid cooler in watts. Design conditions for this capacity i.e.~entering air dry-bulb temperature, entering air wet-bulb temperature and entering water temperature must be provided in the input. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored. This field may be autocalculated, in which case it is set to a fraction of the ``High Speed User Specified Design Capacity'' determined in the following field.
+
+\paragraph{Field: Low Speed User Specified Design Capacity Sizing Factor}\label{field-low-speed-user-specified-design-capacity-sizing-factor}
+
+This field contains the sizing factor to use when calculating the Low-Speed User Specified Design Capacity.~ The default is 0.5.
+
+\paragraph{Field:Design Entering Water Temperature}\label{fielddesign-entering-water-temperature-1}
+
+This numeric field contains entering water temperature at nominal conditions in degrees Celsius. The design entering water temperature must be greater than the design entering air temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
+
+\paragraph{Field:Design Entering Air Temperature}\label{fielddesign-entering-air-temperature-1}
+
+This numeric field contains entering air dry-bulb temperature at nominal conditions in degrees Celsius. The design entering air temperature must be greater than the design entering air wet-bulb temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
+
+\paragraph{Field:Design Entering Air Wet-bulb Temperature}\label{fielddesign-entering-air-wet-bulb-temperature-1}
+
+This numeric field contains entering air wetbulb temperature at nominal conditions in degrees Celsius. The design entering air wet-bulb temperature must be less than the design entering air (dry-bulb) temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
+
+\paragraph{Field: High Speed Sizing Factor}\label{field-high-speed-sizing-factor}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature. For this component the inputs that would be altered by the sizing factor are:
+
+1.~~~~Design Water Flow Rate;
+
+2.~~~~Air Flow Rate at High Fan Speed;
+
+3.~~~~Fan Power at High Fan Speed;
+
+4.~~~~U-Factor Times Area Value at High Fan Speed;
+
+5.~~~~Air Flow Rate at Low Fan Speed;
+
+6.~~~~Fan Power at Low Fan Speed;
+
+7.~~~~U-Factor Times Area Value at Low Fan Speed;
+
+Note that the U-Factor Times Area Value at High Fan Speed is not multiplied by the Sizing Factor. Instead the design evaporative fluid cooler load is multiplied by the sizing factor and the design UA then calculated as usual. The U-Factor Times Area Value at Low Fan Speed is set to Low Fan Speed U-Factor Times Area Sizing Factor times the full load design UA.
+
+\paragraph{Field: Evaporation Loss Mode}\label{field-evaporation-loss-mode-5}
+
+This field is used to choose which method is used to model the amount of water evaporated by the evaporative fluid cooler. There are two options: LossFactor or SaturatedExit. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the evaporative fluid cooler is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the evaporative fluid cooler model (and does not require additional user input).
+
+\paragraph{Field: Evaporation Loss Factor}\label{field-evaporation-loss-factor-5}
+
+This field is used to specify the rate of water evaporated from the evaporative fluid cooler and lost to the outside air {[}percent/K{]}. This field is only used if the Evaporation Calculation Mode is set to LossFactor. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Empirical correlation is used to calculate default loss factor if it not explicitly specified in the input file.
+
+\paragraph{Field: Drift Loss Percent}\label{field-drift-loss-percent-5}
+
+This field is used to specify the rate of water lost to the exiting air as entrained droplets {[}\%{]}. The drift loss is a percent of the condenser water flow. Default value is under investigation for now cooling tower's evaporation loss factor is taken as default value.
+
+\paragraph{Field: Blowdown Calculation Mode}\label{field-blowdown-calculation-mode-5}
+
+This field specifies which method is used to determine blowdown rates. There two options ConcentrationRatio or ScheduledRate. The choice will determine which of the two models below is used. The default is ConcentrationRatio.
+
+\paragraph{Field: Blowdown Concentration Ratio}\label{field-blowdown-concentration-ratio-5}
+
+This field is used to dynamically adjust the rate of blowdown in the evaporative fluid cooler as a function of the rate of evaporation. Blowdown is water intentionally drained from the evaporative fluid cooler in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Default value is under investigation for now cooling tower's evaporation loss factor is taken as default value.
+
+\paragraph{Field: Blowdown Makeup Water Usage Schedule Name}\label{field-blowdown-makeup-water-usage-schedule-name-5}
+
+This alpha field contains the name of the schedule used to define the amount of water (m3/s) flushed from the basin on a periodic basis to purge the evaporative fluid cooler of mineral scale build-up and other contaminants. This schedule is only used if the Blowdown Calculation Mode is set to ScheduledRate. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Default value is under investigation for now cooling tower's evaporation loss factor is taken as default value.This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the evaporative fluid cooler is active and water is flowing through the evaporative fluid cooler (regardless of the water usage defined by this schedule).
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-5}
+
+This field is optional. It is used to describe where the evaporative fluid cooler obtains water used for evaporative cooling. If blank or omitted, then the evaporative fluid cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the evaporative fluid cooler will obtain its water from that tank. If a tank is specified, the evaporative fluid cooler will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the evaporative fluid cooler needs, then the evaporative fluid cooler will still operate and obtain the rest of the water it needs from the mains (referred to as `Starved' water).
+
+Examples of an IDF specification for this object are shown below:
+
+\begin{lstlisting}
+
+EvaporativeFluidCooler:TwoSpeed,
+      Big EvaporativeFluidCooler,         !- Name
+      Condenser EvaporativeFluidcooler Inlet Node,  !- Water Inlet Node Name
+      Condenser EvaporativeFluidcooler Outlet Node,  !- Water Outlet Node Name
+      9.911,                   !- High Fan Speed Air Flow Rate {m3/s}
+      autosize,                !- High Fan Speed Fan Power {W}
+      4.911,                   !- Low Fan Speed Air Flow Rate {m3/s}
+      0.5,                     !- Low Fan Speed Air Flow Rate Sizing Factor
+      autosize,                !- Low Fan Speed Fan Power {W}
+      0.16,                    !- Low Fan Speed Fan Power Sizing Factor
+      0.002208,                !- Design Spray Water Flow Rate {m3/s}
+      UserSpecifiedDesignCapacity,    !- Performance Input Method
+      ,                        !- Outdoor Air Inlet Node Name
+      1.25,                    !- Heat Rejection Capacity and Nominal Capacity Sizing Ratio
+      ,                        !- High Speed Standard Design Capacity {W}
+      ,                        !- Low Speed Standard Design Capacity {W}
+      0.5,                     !- Low Speed Standard Capacity Sizing Factor
+      ,                        !- High Fan Speed U-factor Times Area Value  {W/K}
+      ,                        !- Low Fan Speed U-factor Times Area Value  {W/K}
+      0.6,                     !- Low Fan Speed U-Factor Times Area Sizing Factor
+      0.001703,                !- Design Water Flow Rate {m3/s}
+      87921,                   !- High Speed User Specified Design Capacity {W}
+      47921,                   !- Low Speed User Specified Design Capacity {W}
+      0.5,                     !- Low Speed User Specified Design Capacity Sizing Factor
+      46.11,                   !- Design Entering Water Temperature {C}
+      35,                      !- Design Entering Air Temperature {C}
+      25.6;                    !- Design Entering Air Wet-bulb Temperature {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-001}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Tower Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Tower Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Water Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Evaporation Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Drift Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Water Blowdown Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Tower Make Up Mains Water Volume {[}m3{]}
+\end{itemize}
+
+If Supply Water Storage Tank Name is specified:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Cooling Tower Fan Electric Power {[}W{]}}\label{cooling-tower-fan-electric-power-w-5}
+
+The average electric power consumption of the fluid cooler fan in Watts for the timestep being reported.
+
+\paragraph{Cooling Tower Fan Electric Energy {[}J{]}}\label{cooling-tower-fan-electric-energy-j-5}
+
+Fan energy use in Joules.~ Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Cooling Tower Heat Transfer Rate {[}W{]}}\label{cooling-tower-heat-transfer-rate-w-5}
+
+This is the average rate, in Watts, at which heat is removed from the condenser water loop by the fluid cooler for the time step being reported.
+
+\paragraph{Cooling Tower Inlet Temperature {[}C{]}}\label{cooling-tower-inlet-temperature-c-5}
+
+The fluid temperature at the fluid cooler inlet in degrees Celsius.
+
+\paragraph{Cooling Tower Outlet Temperature {[}C{]}}\label{cooling-tower-outlet-temperature-c-5}
+
+The fluid temperature at the fluid cooler outlet in degrees Celsius.
+
+\paragraph{Cooling Tower Mass Flow Rate {[}kg/s{]}}\label{cooling-tower-mass-flow-rate-kgs-5}
+
+The average fluid mass flow rate through the fluid cooler in kg/s for the time step being reported.
+
+\paragraph{Cooling Tower Make Up Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-make-up-water-volume-flow-rate-m3s-5}
+
+\paragraph{Cooling Tower Make Up Water Volume {[}m3{]}}\label{cooling-tower-make-up-water-volume-m3-5}
+
+These outputs are the external spray water consumed by the evaporative fluid cooler. This is the total of evaporation, drift, and blowdown.
+
+\paragraph{Cooling Tower Water Evaporation Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-evaporation-volume-flow-rate-m3s-5}
+
+\paragraph{Cooling Tower Water Evaporation Volume {[}m3{]}}\label{cooling-tower-water-evaporation-volume-m3-5}
+
+\paragraph{Cooling Tower Water Drift Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-drift-volume-flow-rate-m3s-5}
+
+\paragraph{Cooling Tower Water Drift Volume {[}m3{]}}\label{cooling-tower-water-drift-volume-m3-5}
+
+\paragraph{Cooling Tower Water Blowdown Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-water-blowdown-volume-flow-rate-m3s-5}
+
+\paragraph{Cooling Tower Water Blowdown Volume {[}m3{]}}\label{cooling-tower-water-blowdown-volume-m3-5}
+
+These outputs provide the breakdown of the different components of water use during fluid cooler operation.
+
+\paragraph{Cooling Tower Make Up Mains Water Volume {[}m3{]}}\label{cooling-tower-make-up-mains-water-volume-m3-5}
+
+The volume of make up water provided by the mains in cubic meters. If no Supply Water Storage Tank is specified, then all fluid cooler make up water is provided by the mains (same as Cooling Tower Make Up Water Volume). If a Supply Water Storage Tank is specified, then the make up from the mains only occurs when sufficient water supply is not available from the tank (same as Cooling Tower Starved Storage Tank Water Volume). This output variable is metered on HeatRejection:MainsWater, MainsWater:Plant and MainsWater:Facility.
+
+\paragraph{Cooling Tower Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-storage-tank-water-volume-flow-rate-m3s-5}
+
+\paragraph{Cooling Tower Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-storage-tank-water-volume-m3-5}
+
+These are the rate and volume of water provided by the Supply Water Storage Tank.
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{cooling-tower-starved-storage-tank-water-volume-flow-rate-m3s-5}
+
+\paragraph{Cooling Tower Starved Storage Tank Water Volume {[}m3{]}}\label{cooling-tower-starved-storage-tank-water-volume-m3-5}
+
+These are the rate and volume of water the Supply Water Storage Tank was not able to provide. The starved water is assumed to come from the mains. The fluid cooler's operation is not affected by a lack of storage tank water.
+
+\subsection{FluidCooler:SingleSpeed}\label{fluidcoolersinglespeed}
+
+Fluid coolers are components that may be assigned to condenser loops. The Fluid cooler is modeled as a cross flow heat exchanger (both streams unmixed) with single-speed fans (induced draft configuration). The user must define fluid cooler performance via one of the two methods: design heat transfer coefficient-area product (UA) and design water flow rate, or nominal fluid cooler capacity at a specific rating point. Regardless of which method is chosen, the design airflow rate and corresponding fan power must be specified.
+
+The fluid cooler seeks to maintain the temperature of the water exiting the fluid cooler at (or below) a set point. The set point schedule value is defined by the field ``Condenser Loop Temperature Setpoint Node Name or Reference'' for the CondenserLoop object. The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., fluid cooler fan on for the entire simulation timestep and fluid cooler fan off for the entire simulation timestep). Cyclic losses are not taken into account.
+
+\subsubsection{Inputs}\label{inputs-8-003}
+
+\paragraph{Field: Name}\label{field-name-7-003}
+
+This alpha field contains the identifying name for the Fluid Cooler.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-5}
+
+This alpha field contains the identifying name for the Fluid Cooler's water inlet node.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-6}
+
+This alpha field contains the identifying name for the Fluid Cooler's water outlet node.
+
+\paragraph{Field: Performance Input Method}\label{field-performance-input-method-5}
+
+This alpha field contains the method by which the user will specify fluid cooler performance: ``UFactorTimesAreaAndDesignWaterFlowRate'' or ``NominalCapacity''.
+
+\paragraph{Field: Design Air Flow Rate U-factor Times Area Value}\label{field-design-air-flow-rate-u-factor-times-area-value-2}
+
+This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the design air and water flow rates specified above. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design fluid cooler UA value is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), the fluid cooler inlet air dry-bulb and wetbulb temperature are taken from the input. If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically calculates the fluid cooler UA based on the fluid cooler capacity and nominal conditions specified in input file.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-2}
+
+This numeric input field contains the ``nominal'' heat rejection capacity of the fluid cooler in watts, Nominal conditions i.e.~entering air dry-bulb temperature, entering air wet-bulb temperature and Entering water temperature should be provided in the input.
+
+\paragraph{Field:Design Entering Water Temperature}\label{fielddesign-entering-water-temperature-2}
+
+This numeric field contains entering water temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering water temperature must be greater than the design entering air temperature.
+
+\paragraph{Field:Design Entering Air Temperature}\label{fielddesign-entering-air-temperature-2}
+
+This numeric field contains entering air dry-bulb temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering air temperature must be greater than the design entering air wet-bulb temperature.
+
+\paragraph{Field:Design Entering Air Wet-bulb Temperature}\label{fielddesign-entering-air-wet-bulb-temperature-2}
+
+This numeric field contains entering air wetbulb temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering air wet-bulb temperature must be less than the design entering air (dry-bulb) temperature.
+
+\paragraph{Field: Design Water Flow Rate}\label{field-design-water-flow-rate-6}
+
+This numeric field contains the design water flow rate through the fluid cooler in m\(^{3}\)/s. This value is the flow rate of the condenser loop water being cooled by the fluid cooler. A water flow rate greater than zero must be defined or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections).
+
+\paragraph{Field: Design Air Flow Rate}\label{field-design-air-flow-rate-4}
+
+This numeric field contains the design air flow rate induced by the fluid cooler fan in m\(^{3}\)/s. A value greater than zero must be defined regardless of the fluid cooler performance input method. Alternately, this field can be autosized. See Engineering Reference document for fluid cooler autosizing.
+
+\paragraph{Field: Design Air Flow Rate Fan Power}\label{field-design-air-flow-rate-fan-power-1}
+
+This numeric field contains the fan power (in watts) at the design air flow rate specified in the previous field. A value greater than zero must be specified regardless of the performance input method, or this field can be autosized. See Engineering ref. for fluid cooler autosizing.
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-6}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the fluid cooler. If this field is left blank, the outdoor air conditions entering the fluid cooler are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+An IDF specification for this object is shown below:
+
+\begin{lstlisting}
+
+FluidCooler:SingleSpeed,
+      Big FLUIDCOOLER1,              !- Name
+      Condenser FLUIDCOOLER 1 Inlet Node,  !- Water Inlet Node Name
+      Condenser FLUIDCOOLER 1 Outlet Node, !- Water Outlet Node Name
+      NominalCapacity,        !- Performance Input Method
+      ,                       !- Design Air Flow Rate U-factor Times Area Value {W/K}
+      58601.,                 !- Nominal Capacity {W}
+      51.67,                  !- Design Entering Water Temperature {C}
+      35,                     !- Design Entering Air Temperature {C}
+      25.6,                   !- Design Entering Air Wetbulb Temperature {C}
+      0.001388,               !- Design Water Flow Rate{m3/s}
+      9.911,                  !- Design Air Flow Rate {m3/s}
+      Autosize;               !- Design Air Flow Rate Fan Power {W}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8-000}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Fan Electric Energy {[}J{]}
+\item
+  Zone,Meter,HeatRejection:Electricity {[}J{]}
+\item
+  HVAC,Average,Cooling Tower Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average, Cooling Tower Inlet Temperature {[}C{]}
+\item
+  HVAC,Average, Cooling Tower Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Cooling Tower Fan Electric Power {[}W{]}}\label{cooling-tower-fan-electric-power-w-6}
+
+The electric power consumption of the fluid cooler fans.
+
+\paragraph{Cooling Tower Fan Electric Energy {[}J{]}}\label{cooling-tower-fan-electric-energy-j-6}
+
+Fan energy use.~ Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Cooling Tower Heat Transfer Rate {[}W{]}}\label{cooling-tower-heat-transfer-rate-w-6}
+
+This is the rate at which heat is removed from the condenser water loop by the fluid cooler.
+
+\paragraph{Cooling Tower Inlet Temperature {[}C{]}}\label{cooling-tower-inlet-temperature-c-6}
+
+The loop temperature at the fluid cooler inlet.
+
+\paragraph{Cooling Tower Outlet Temperature {[}C{]}}\label{cooling-tower-outlet-temperature-c-6}
+
+The loop temperature at the fluid cooler outlet.
+
+\paragraph{Cooling Tower Mass Flow Rate {[}kg/s{]}}\label{cooling-tower-mass-flow-rate-kgs-6}
+
+The loop mass flow rate of the circulating condenser water loop.
+
+\subsection{FluidCooler:TwoSpeed}\label{fluidcoolertwospeed}
+
+The two-speed fluid cooler is modeled in a similar fashion to the single-speed fluid cooler. The fluid cooler is modeled as a cross flow heat exchanger (both stream unmixed) with~ two-speed fans (induced draft configuration). The user must define fluid cooler performance via one of two methods: heat transfer coefficient-area product (UA) and design water flow rate, or nominal fluid cooler capacity at a specific rating point. Regardless of which method is chosen, the airflow rate and corresponding fan power at both high and low fan speed must be specified. The Fluid Cooler seeks to maintain the temperature of the water exiting the Fluid Cooler at (or below) a set point. The set point schedule is defined by the field ``Condenser Loop Temperature Setpoint Node Name or Reference'' for the CondenserLoop object. The model first runs at low speed and calculates the fluid cooler exiting water temperature. If the exiting water temperature based on ``low speed'' is at or below the set point, then the fluid cooler fan runs at this speed or below this speed. If the exiting water temperature remains above the set point after ``low speed'' is modeled, then the fluid cooler fan runs at high speed to reduce the exiting water temperature.
+
+The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., fluid cooler fan at high speed for the entire simulation timestep and fluid cooler fan at low speed for the entire simulation timestep,). Cyclic losses are not taken into account.
+
+\subsubsection{Inputs}\label{inputs-9-003}
+
+\paragraph{Field: Name}\label{field-name-8-003}
+
+This alpha field contains the identifying name for the fluid cooler.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-6}
+
+This alpha field contains the identifying name for the fluid cooler's water inlet node.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-7}
+
+This alpha field contains the identifying name for the fluid cooler's water outlet node.
+
+\paragraph{Field: Performance Input Method}\label{field-performance-input-method-6}
+
+This alpha field contains the method by which the user will specify fluid cooler performance: ``UFactorTimesAreaAndDesignWaterFlowRate'' or ``NominalCapacity''.
+
+\paragraph{Field: High Fan Speed U-factor Times Area Value}\label{field-high-fan-speed-u-factor-times-area-value-2}
+
+This numeric field contains the heat transfer coefficient-area product (UA) in watts per degree Celsius corresponding to the high-speed air flow rate and design water flow rate specified above. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the fluid cooler UA value at high fan speed is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), fluid cooler water inlet temperature, fluid cooler inlet air drybulb and wetbulb are provided in the input. If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically calculates the fluid cooler UA based on the capacity specified in the field ``High Speed Nominal Capacity'' and nominal conditions.
+
+\paragraph{Field: Low Fan Speed U-factor Times Area Value}\label{field-low-fan-speed-u-factor-times-area-value-2}
+
+This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the design water flow rate and low-speed air flow rate specified above. If the input field ``Performance Input Method'' is specified as ``UFactorTimesAreaAndDesignWaterFlowRate'', this value must be greater than zero but less than or equal to 300,000, less than the value specified for the field ``U-factor Times Area Value at High Fan Speed''. This field may be autocalculated, in which case it is set to a factor of the ``U-factor Times Area Value at High Fan Speed'' determined in the following field. If ``Performance Input Method'' is specified as ``NominalCapacity'', then this field must be left blank since the model automatically calculates the fluid cooler UA based on the fluid cooler capacity specified in the field ``Low Speed Nominal Capacity''.
+
+\paragraph{Field: Low Fan Speed U-Factor Times Area Sizing Factor}\label{field-low-fan-speed-u-factor-times-area-sizing-factor-2}
+
+This numeric field contains the sizing factor to use when calculating the Low Fan Speed U-factor Times Area Value.~ The default is 0.6.
+
+\paragraph{Field: High Speed Nominal Capacity}\label{field-high-speed-nominal-capacity-1}
+
+This numeric input field contains the ``nominal'' heat rejection capacity of the fluid cooler in watts under high-speed fan operation, with nominal (design) inputs entering water temperature, entering air temperature and entering air wet-bulb temperature. The design water flow rate is also provided in the input.
+
+\paragraph{Field: Low Speed Nominal Capacity}\label{field-low-speed-nominal-capacity-1}
+
+This numeric input field contains the ``nominal'' heat rejection capacity of the Fluid Cooler in watts under low-speed fan operation, with nominal (design) inputs entering water temperature, entering air temperature and entering air wet-bulb temperature. The design water flow rate is also provided in the input. The value specified for this field must be greater than zero but less than the value specified for the field ``High Speed Nominal Capacity''. This field may be autocalculated, in which case it is set to a fraction of the ``High Speed Nominal Capacity'' determined in the following field.
+
+\paragraph{Field: Low Speed Nominal Capacity Sizing Factor}\label{field-low-speed-nominal-capacity-sizing-factor-1}
+
+This numeric field contains the sizing factor to use when calculating the Low Speed Nominal Capacity.~ The default is 0.5.
+
+\paragraph{Field:Design Entering Water Temperature}\label{fielddesign-entering-water-temperature-3}
+
+This numeric field contains entering water temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering water temperature must be greater than the design entering air temperature.
+
+\paragraph{Field:Design Entering Air Temperature}\label{fielddesign-entering-air-temperature-3}
+
+This numeric field contains entering air dry-bulb temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering air temperature must be greater than the design entering air wet-bulb temperature.
+
+\paragraph{Field:Design Entering Air Wet-bulb Temperature}\label{fielddesign-entering-air-wet-bulb-temperature-3}
+
+This numeric field contains entering air wet-bulb temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering air wet-bulb temperature must be less than the design entering air (dry-bulb) temperature.
+
+\paragraph{Field: Design Water Flow Rate}\label{field-design-water-flow-rate-7}
+
+This numeric field contains the design water flow rate through the fluid cooler in m\(^{3}\)/s. This value is the flow rate of the condenser loop water being cooled by the fluid cooler. A water flow rate greater than zero must be defined or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections).
+
+\paragraph{Field: High Fan Speed Air Flow Rate}\label{field-high-fan-speed-air-flow-rate-2}
+
+This numeric field contains the fluid cooler air flow rate at high fan speed in m\(^{3}\)/s. A value greater than zero must be defined regardless of the fluid cooler performance input method. Alternately, this field can be autosized. See Engineering ref. for fluid cooler autosizing.
+
+\paragraph{Field: High Fan Speed Fan Power}\label{field-high-fan-speed-fan-power-1}
+
+This numeric field contains the fan power (in Watts) at the high-speed air flow rate specified in the previous field. A value greater than zero must be specified regardless of the fluid cooler performance input method, or this field can be autosized. See Engineering ref. for fluid cooler autosizing.
+
+\paragraph{Field: Low Fan Speed Air Flow Rate}\label{field-low-fan-speed-air-flow-rate-2}
+
+This numeric field contains the fluid cooler air flow rate at low fan speed in m\(^{3}\)/s. This value must be greater than zero, less than the value specified for the field ``Air Flow Rate at High Fan Speed''. This field may be autocalculated, in which case it is set to a fraction of the ``Air Flow Rate at High Fan Speed'' determined in the following field.
+
+\paragraph{Field: Low Fan Speed Air Flow Rate Sizing Factor}\label{field-low-fan-speed-air-flow-rate-sizing-factor-2}
+
+This numeric field contains the sizing factor to use when calculating the Low Fan Speed Air Flow Rate. The default is 0.5.
+
+\paragraph{Field: Low Fan Speed Fan Power}\label{field-low-fan-speed-fan-power-2}
+
+This numeric field contains the fan power (in Watts) at the low-speed air flow rate specified in the previous field. This value must be specified greater than zero or the field may be autocalculated, in which case it is set to set to a fraction of the ``Fan Power at High Fan Speed'' determined in the following field.
+
+\paragraph{Field: Low Fan Speed Fan Power Sizing Factor}\label{field-low-fan-speed-fan-power-sizing-factor-2}
+
+This numeric field contains the sizing factor to use whe calculating the Low Fan Speed Fan Power.~ The default is 0.16.
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-7}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the Fluid Cooler. If this field is left blank, the outdoor air conditions entering the Fluid Cooler are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+Examples of an IDF specification for this object are shown below:
+
+\begin{lstlisting}
+
+FluidCooler:TwoSpeed,
+      Big FLUIDCOOLER1,              !- Name
+      Condenser FLUIDCOOLER 1 inlet Node,  !- Water Inlet Node Name
+      Condenser FLUIDCOOLER 1 Outlet Node,  !- Water Outlet Node Name
+      NominalCapacity,         !- Performance Input Method
+      ,                        !- High Fan Speed U-factor Times Area Value {W/K}
+      ,                        !- Low Fan Speed U-factor Times Area Value {W/K}
+      ,                        !- Low Fan Speed U-Factor Times Area Sizing Factor
+      58601.,                  !- High Speed Nominal Capacity {W}
+      28601.,                  !- Low Speed Nominal Capacity {W}
+  .   0.6,                     !- Low Speed Nominal Capacity Sizing Factor
+      51.67,                   !- Design Entering Water tempereture {C}
+      35,                      !- Design Entering Air tempereture {C}
+      25.6,                    !- Design Entering Air Wet-bulb tempereture {C}
+      0.001388,                !- Design Water Flow Rate {m3/s}
+      9.911,                   !- High Fan Speed Air Flow Rate {m3/s}
+      autosize,                !- High Fan Speed Fan Power {W}
+      autosize,                !- Low Fan Speed Air Flow Rate {m3/s}
+      0.5,                     !- Low Fan Speed Air Flow Rate Sizing Factor
+      autosize,                !- Low Fan Speed Fan Power {W}
+      0.16;                    !- Low Fan Speed Fan Power Sizing Factor
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-9-000}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Tower Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Tower Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Tower Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average, Cooling Tower Inlet Temperature {[}C{]}
+\item
+  HVAC,Average, Cooling Tower Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Tower Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Cooling Tower Fan Electric Power {[}W{]}}\label{cooling-tower-fan-electric-power-w-7}
+
+Average fan electric power consumed.
+
+\paragraph{Cooling Tower Fan Electric Energy {[}J{]}}\label{cooling-tower-fan-electric-energy-j-7}
+
+Total energy used by the fan. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Cooling Tower Heat Transfer Rate {[}W{]}}\label{cooling-tower-heat-transfer-rate-w-7}
+
+This is the rate at which heat is removed from the condenser water loop by the fluid cooler.
+
+\paragraph{Cooling Tower Inlet Temperature {[}C{]}}\label{cooling-tower-inlet-temperature-c-7}
+
+Loop temperature at the fluid cooler inlet.
+
+\paragraph{Cooling Tower Outlet Temperature {[}C{]}}\label{cooling-tower-outlet-temperature-c-7}
+
+Loop temperature at the fluid cooler outlet.
+
+\paragraph{Cooling Tower Mass Flow Rate {[}kg/s{]}}\label{cooling-tower-mass-flow-rate-kgs-7}
+
+Loop mass flow rate through the fluid cooler.
+
+\subsection{GroundHeatExchanger:Vertical}\label{groundheatexchangervertical}
+
+The EnergyPlus Ground loop heat exchanger is a condenser component. This serves the condenser supply side in addition to the cooling towers and other condensing components. The following figure shows the Ground Heat Exchanger in the simulation environment.
+
+The heat exchanger response is defined by a G-function. This is a non-dimensional function that is used to calculate the response to square heat pulses of different duration. (This function is not the same as `G-factors' referred to in the ASHRAE Applications Handbook). This continuous function is specified by a series of data pairs (LNTTS\emph{i}, GFNC\emph{i}) where,
+
+\begin{itemize}
+\item
+  LNTTS\emph{i} is the non-dimensional time: \emph{ln(T/T\(_{s}\))}
+\item
+  GFNC\emph{i} is the G-function value
+\end{itemize}
+
+The G-function is different for each borehole field configuration (i.e.~a 4x4 field has a different response than a 80x80 field) and the borehole thermal resistance. It is also dependant on the ratio of borehole spacing to depth. G-function values, for accurate simulation, have to be calculated for each specific heat exchanger design. This can be done using some commercial ground loop heat exchanger design tool and the like. A reference data set, containing examples input data for 1x2, 4x4 and 8x8 configurations and for both standard and thermally enhanced grout, have also been provided. These data are provided as examples only. Custom G-function values may be generated using an external program such as GLHEPro. For more information about the datasets and GLHEPro, see the Auxiliary Programs document section ``G-Function Spreadsheet.''
+
+Further details of the implementation of this model can be found in:
+
+Murugappan, A. \emph{Implementing Ground Source Heat Pump and Ground Loop Heat Exchanger Models in the EnergyPlus Simulation Environment}. M.S. Thesis, Oklahoma State University, December 2002.
+
+\begin{figure}[hbtp] % fig 83
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image202.png}
+\caption{Schematic of EnergyPlus Ground Loop Heat Exchanger \protect \label{fig:schematic-of-energyplus-ground-loop-heat}}
+\end{figure}
+
+The data definition for the ground loop heat exchanger from the Energy+.idd is shown below. The syntax to the specification of Borehole, U-tube and ground are illustrated in the example following.
+
+\subsubsection{Inputs}\label{inputs-10-002}
+
+\paragraph{Field: Name}\label{field-name-9-003}
+
+This alpha field contains the identifying name for the ground heat exchanger (GHE).
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-000}
+
+This alpha field contains the ground heat exchanger inlet node name.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-001}
+
+This alpha field contains the ground heat exchanger outlet node name.
+
+\paragraph{Field: Design Flow Rate}\label{field-design-flow-rate-000}
+
+This numeric field contains the GHE design flow rate in cubic meters per second \{m\(^{3}\)/s\}.
+
+\paragraph{Field: Number of Bore Holes}\label{field-number-of-bore-holes}
+
+This numeric field contains the number of bore holes in the GHE installation.
+
+\paragraph{Field: Bore Hole Length}\label{field-bore-hole-length}
+
+This numeric field contains the length of the borehole in meters \{m\}.
+
+\paragraph{Field: Bore Hole Radius}\label{field-bore-hole-radius}
+
+This numeric field contains the radius of the borehole in meters.
+
+\paragraph{Field: Ground Thermal Conductivity}\label{field-ground-thermal-conductivity}
+
+This numeric field contains the thermal conductivity of the ground in W/m-K.
+
+\paragraph{FieldSet: Ground Thermal Heat Capacity}\label{fieldset-ground-thermal-heat-capacity}
+
+This numeric field contains the thermal heat capacity of the ground in J/m\(^{3}\)-K.
+
+\paragraph{Field: Ground Temperature}\label{field-ground-temperature}
+
+This numeric field contains the far field temperature of the ground in °C.
+
+\paragraph{Field: Grout Thermal Conductivity}\label{field-grout-thermal-conductivity}
+
+This numeric field contains the thermal conductivity of the filler material in W/m-K.
+
+\paragraph{Field: Pipe Thermal Conductivity}\label{field-pipe-thermal-conductivity-000}
+
+This numeric field contains the thermal conductivity of the pipe in W/m-K.
+
+\paragraph{Field: Pipe Out Diameter}\label{field-pipe-out-diameter}
+
+This numeric field contains the outer diameter of the U-tube (pipe) in meters \{m\}.
+
+\paragraph{Field: U-Tube Distance}\label{field-u-tube-distance}
+
+This numeric field contains the distance between the two legs of the U-tube in meters \{m\}.
+
+\paragraph{Field: Pipe Thickness}\label{field-pipe-thickness-000}
+
+This numeric field contains the outer diameter of the U-tube (pipe) in meters.
+
+\paragraph{Field: Maximum Length of Simulation}\label{field-maximum-length-of-simulation}
+
+This numeric field contains the maximum number of years of simulation to be carried out.
+
+\paragraph{Field: G-Function Reference Ratio}\label{field-g-function-reference-ratio}
+
+The G-Functions may be formulated slightly differently based on the program which generated them. The ``raw'' G-Functions are based on an borehole radius to active length ratio of 0.0005. If the physical ratio is different from this, a correction must be applied. EnergyPlus will apply the correction, based on the reference ratio entered in this field. Therefore, therefore two possible input configurations.
+
+\begin{itemize}
+\item
+  If the G-Functions have not had a correction applied, then the G-Functions are still based on a reference of 0.0005, so use a value of 0.0005 in this field. EnergyPlus will adjust the G-Functions internally to create the properly referenced G-Function.
+\item
+  If the correction has already been applied, then the input G-Functions are based on a reference to the actual (physical) radius/length ratio, so enter the physical radius/length in this field. Entering the actual value will nullify any internal corrections, which will avoid re-basing the G-Function set.
+\end{itemize}
+
+The software GLHEPro has been making this ``pre-correction'' to the data sets since version 3.1 of that software, so this input field should match the actual (physical) radius/length ratio.
+
+\paragraph{Field: Number of Data Pairs of the G Function}\label{field-number-of-data-pairs-of-the-g-function}
+
+The borehole response is defined by a non-dimensional `G-function'. This is specified as a series of data points giving values of non-dimensional time \emph{vs} G-function value (LNTTS1, GFUNC1), (LNTTS2, GFUNC2), (LNTTS3, GFUNC3) \ldots{}\ldots{}.. (LNTTS\emph{n}, GFUNC\emph{n}), This numeric field contains the number of data pairs to be read in (\emph{n}).
+
+\paragraph{Field: G-Function Ln(T/Ts) Value \textless{}x\textgreater{}}\label{field-g-function-lntts-value-x}
+
+This numeric field contains the natural log of time/steady state time: \emph{ln(T/T\(_{s}\))}
+
+\paragraph{\texorpdfstring{Field: G-Function `G' Value \textless{}x\textgreater{}}{Field: G-Function G Value \textless{}x\textgreater{}}}\label{field-g-function-g-value-x}
+
+This numeric field contains the G-function value of the corresponding LNTTS.
+
+The following is an example input:
+
+\begin{lstlisting}
+
+GroundHeatExchanger:Vertical,
+  Vertical Ground Heat Exchanger, !- Name
+  GHE Inlet Node,                 !- Inlet Node Name
+  GHE Outlet Node,                !- Outlet Node Name
+  0.00330000,                     !- Design Flow Rate {m3/s}
+  120,                            !- Number of Bore Holes
+  76.2,                           !- Bore Hole Length {m}
+  .635080E-01,                    !- Bore Hole Radius {m}
+  .692626E+00,                    !- Ground Thermal Conductivity {W/m-K}
+  .234700E+07,                    !- Ground Thermal Heat Capacity {J/m3-K}
+  13.375,                         !- Ground Temperature {C}
+  .692626E+00,                    !- Grout Thermal Conductivity {W/m-K}
+  .391312E+00,                    !- Pipe Thermal Conductivity {W/m-K}
+  2.66667E-02,                    !- Pipe Out Diameter {m}
+  2.53977E-02,                    !- U-Tube Distance {m}
+  2.41285E-03,                    !- Pipe Thickness {m}
+  2,                              !- Maximum Length of Simulation
+  0.0005,                         !- G-Function Reference Ratio
+  35,                             !- Number of Data Pairs of the G Function
+  ! The G-function is defined by the following data pairs
+  -15.2996, -0.348322,            ! G-Function Ln(T/Ts) Value 1, G-Function G Value 1
+  -14.201,  0.022208,             ! G-Function Ln(T/Ts) Value 2, G-Function G Value 2
+  -13.2202, 0.412345,             ! G-Function Ln(T/Ts) Value 3, G-Function G Value 3
+  -12.2086, 0.867498,             ! G-Function Ln(T/Ts) Value 4, G-Function G Value 4
+  -11.1888, 1.357839,             ! G-Function Ln(T/Ts) Value 5, G-Function G Value 5
+  -10.1816, 1.852024,             ! G-Function Ln(T/Ts) Value 6, G-Function G Value 6
+  -9.1815,  2.345656,             ! G-Function Ln(T/Ts) Value 7, G-Function G Value 7
+  -8.6809,  2.593958,             ! G-Function Ln(T/Ts) Value 8, G-Function G Value 8
+  -8.5,     2.679,                ! etc, etc.
+  -7.8,     3.023,
+  -7.2,     3.32,
+  -6.5,     3.681,
+  -5.9,     4.071,
+  -5.2,     4.828,
+  -4.5,     6.253,
+  -3.963,   7.894,
+  -3.27,    11.82,
+  -2.864,   15.117,
+  -2.577,   18.006,
+  -2.171,   22.887,
+  -1.884,   26.924,
+  -1.191,   38.004,
+  -0.497,   49.919,
+  -0.274,   53.407,
+  -0.051,   56.632,
+  0.196,    59.825,
+  0.419,    62.349,
+  0.642,    64.524,
+  0.873,    66.412,
+  1.112,    67.993,
+  1.335,    69.162,
+  1.679,    70.476,
+  2.028,    71.361,
+  2.275,    71.79,
+  3.003,    72.511;               !- 35 PAIRS
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-10-000}
+
+\begin{itemize}
+\item
+  HVAC,Average,Ground Heat Exchanger Average Borehole Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Average Fluid Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Ground Heat Exchanger Average Borehole Temperature {[}C{]}}\label{ground-heat-exchanger-average-borehole-temperature-c}
+
+This is the model result for the average temperature of the borehole heat exchanger.
+
+\paragraph{Ground Heat Exchanger Heat Transfer Rate {[}W{]}}\label{ground-heat-exchanger-heat-transfer-rate-w}
+
+This is the rate of heat transfer between the working fluid and the ground heat exchanger, in Watts.
+
+\paragraph{Ground Heat Exchanger Inlet Temperature {[}C{]}}\label{ground-heat-exchanger-inlet-temperature-c}
+
+This is the temperature of the working fluid entering the ground heat exchanger.
+
+\paragraph{Ground Heat Exchanger Outlet Temperature {[}C{]}}\label{ground-heat-exchanger-outlet-temperature-c}
+
+This is the temperature of the working fluid leaving the ground heat exchanger.
+
+\paragraph{Ground Heat Exchanger Mass Flow Rate {[}kg/s{]}}\label{ground-heat-exchanger-mass-flow-rate-kgs}
+
+This is the mass flow rate of the working fluid through the heat exchanger.
+
+\paragraph{Ground Heat Exchanger Average Fluid Temperature {[}C{]}}\label{ground-heat-exchanger-average-fluid-temperature-c}
+
+This is the average temperature of the working fluid inside the heat exchanger.
+
+\subsection{GroundHeatExchanger:Slinky}\label{groundheatexchangerslinky}
+
+The GroundHeatExchanger:Slinky use the g-functions to calculate the GHX temperature response, similar to the GroundHeatExchanger:Vertical model, however for this model g-functions are automatically calculated by EnergyPlus without the need of external software or data.
+
+Horizontal slinky-loop ground heat exchangers (GHXs) consist of coiled tubing, with the individual rings spread out along the direction of the trench either horizontally or vertically, as shown in \protect\hyperlink{SlinkyIOFig1}{Figure}. A schematic of a slinky GHX can be seen in \protect\hyperlink{SlinkyIOFig2}{Figure}. Compared to conventional straight tube horizontal GHXs, slinky loops have a higher tube density; hence, with the same cooling/heating loads, slinky-loop GHXs require less land area and excavation work than straight tube HGHXs.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image901.png}
+\caption{slinky heat exchanger}
+\end{figure}
+
+Figure: Slinky Ground Heat Exchanger Configurations.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image902.png}
+\caption{slinky heat exchanger}
+\end{figure}
+
+Figure: Schematic of Slinky HX.
+
+An example GroundHeatExchanger:Slinky object is shown below.
+
+\begin{lstlisting}
+
+GroundHeatExchanger:Slinky,
+  Slinky GHX,       !- Name
+  GHE Inlet Node,   !- Inlet Node
+  GHE Outlet Node,  !- Outlet Node
+  0.0033,           !- Design Flow Rate [m3/s]
+  1.2,              !- Soil Thermal Conductivity [W/m-K]
+  3200,             !- Soil Density [kg/m3]
+  850,              !- Soil Specific Heat [J/kg-K]
+  1.8,              !- Pipe Thermal Conductivity [W/m-K]
+  920,              !- Pipe Density [kg/m3]
+  2200,             !- Pipe Specific Heat [J/kg-K]
+  0.02667,          !- Pipe Outside Diameter [m]
+  0.002413,         !- Pipe Wall Thickness [m]
+  Vertical,         !- Heat Exchanger Configuration (Vertical, Horizontal)
+  1,                !- Coil Diameter [m]
+  0.2,              !- Coil Pitch [m]
+  2.5,              !- Trench Depth [m]
+  40,               !- Trench Length [m]
+  15,               !- Number of Parallel Trenches
+  2,                !- Trench Spacing [m]
+  Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
+  KATemps,          !- Name of Undisturbed Ground Temperature Object
+  10;               !- Maximum length of simulation [years]
+\end{lstlisting}
+
+\subsubsection{Inputs}\label{inputs-11-002}
+
+\paragraph{Field: Name}\label{field-name-10-002}
+
+Alpha field used as identifying field for heat exchanger
+
+\paragraph{Field: Inlet Node}\label{field-inlet-node}
+
+This alpha field is the name of the inlet node of the component on a plant loop.
+
+\paragraph{Field: Outlet Node}\label{field-outlet-node}
+
+This alpha field is the name of the outlet node of the component on a plant loop.
+
+\paragraph{Field: Design Flow Rate}\label{field-design-flow-rate-1-000}
+
+This numeric field is the design flow rate in m3/s for the heat exchanger. The plant loop will attempt to meet this request based on loop and flow conditions.
+
+\paragraph{Field: Soil Thermal Conductivity}\label{field-soil-thermal-conductivity}
+
+This numeric field is the thermal conductivity of the soil, in W/m-K.
+
+\paragraph{Field: Soil Density}\label{field-soil-density}
+
+This numeric field is the density of the soil, in kg/m3.
+
+\paragraph{Field: Soil Specific Heat}\label{field-soil-specific-heat}
+
+This numeric field is the specific heat of the soil, in J/kg-K.
+
+\paragraph{Field: Pipe Thermal Conductivity}\label{field-pipe-thermal-conductivity-1}
+
+This numeric field is the thermal conductivity of the heat exchanger pipe.
+
+\paragraph{Field: Pipe Density}\label{field-pipe-density}
+
+This numeric field is the density of the heat exchanger pipe, in kg/m3.
+
+\paragraph{Field: Pipe Specific Heat}\label{field-pipe-specific-heat}
+
+This numeric field is the specific heat of the heat exchanger pipe, in J/kg-K.
+
+\paragraph{Field: Pipe Outside Diameter}\label{field-pipe-outside-diameter}
+
+This numeric field is the outside pipe diameter, in meters.
+
+\paragraph{Field: Pipe Wall Thickness}\label{field-pipe-wall-thickness}
+
+This numeric field is the pipe wall thickness, in meters.
+
+\paragraph{Field: Heat Exchanger Configuration}\label{field-heat-exchanger-configuration}
+
+This alpha field is heat exchanger configuration, either Vertical or Horizontal.
+
+\paragraph{Field: Coil Diameter}\label{field-coil-diameter}
+
+This numeric is the diameter of the slinky coil, in meters.
+
+\paragraph{Field: Coil Pitch}\label{field-coil-pitch}
+
+This numeric field is the center-to-center distance between heat exchanger coils, in meters.
+
+\paragraph{Field: Trench Depth}\label{field-trench-depth}
+
+This numeric field is the distance from the bottom of the trench to the ground surface, in meters.
+
+\paragraph{Field: Trench Length}\label{field-trench-length}
+
+This numeric field is the length of the heat exchanger trench, in meters. This assumes the heat exchanger runs the full length of the trench.
+
+\paragraph{Field: Number of Parallel Trenches}\label{field-number-of-parallel-trenches}
+
+This numeric field is the number of parallel trenches. Design flow rate will be equally divided among all parallel trenches.
+
+\paragraph{Field: Trench Spacing}\label{field-trench-spacing}
+
+This numeric field is the center-to-center distance in between parallel trenches, in meters.
+
+\paragraph{Field: Type of Undisturbed Ground Temperature Object}\label{field-type-of-undisturbed-ground-temperature-object}
+
+The type of undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
+
+\paragraph{Field: Name of Undisturbed Ground Temperature Object}\label{field-name-of-undisturbed-ground-temperature-object}
+
+The name of the undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
+
+\paragraph{Field: Maximum Length of Simulation}\label{field-maximum-length-of-simulation-1}
+
+This numeric field contains the maximum number of years of simulation to be carried out.
+
+\subsubsection{Outputs}\label{outputs-11-000}
+
+The following output variables are available.
+
+\begin{itemize}
+\item
+  HVAC,Average,Ground Heat Exchanger Average Borehole Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Average Fluid Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Ground Heat Exchanger Average Borehole Temperature {[}C{]}}\label{ground-heat-exchanger-average-borehole-temperature-c-1}
+
+This is the model result for the average temperature of the borehole heat exchanger.
+
+\paragraph{Ground Heat Exchanger Heat Transfer Rate {[}W{]}}\label{ground-heat-exchanger-heat-transfer-rate-w-1}
+
+This is the rate of heat transfer between the working fluid and the ground heat exchanger, in Watts.
+
+\paragraph{Ground Heat Exchanger Inlet Temperature {[}C{]}}\label{ground-heat-exchanger-inlet-temperature-c-1}
+
+This is the temperature of the working fluid entering the ground heat exchanger.
+
+\paragraph{Ground Heat Exchanger Outlet Temperature {[}C{]}}\label{ground-heat-exchanger-outlet-temperature-c-1}
+
+This is the temperature of the working fluid leaving the ground heat exchanger.
+
+\paragraph{Ground Heat Exchanger Mass Flow Rate {[}kg/s{]}}\label{ground-heat-exchanger-mass-flow-rate-kgs-1}
+
+This is the mass flow rate of the working fluid through the heat exchanger.
+
+\paragraph{Ground Heat Exchanger Average Fluid Temperature {[}C{]}}\label{ground-heat-exchanger-average-fluid-temperature-c-1}
+
+This is the average temperature of the working fluid inside the heat exchanger.
+
+\subsection{GroundHeatExchanger:Pond}\label{groundheatexchangerpond}
+
+The pond heat exchanger model represents a shallow pond with submerged hydronic tubes through which the heat transfer fluid is circulated. The model represents a `shallow' pond in that no attempt is made to model any stratification effects that may~ be present in deeper ponds.
+
+This type of heat exchanger is intended to be connected to the supply side of a condenser loop, and can be used with any type of plant loop. The pond may be specified as the only heat exchanger on the condenser loop (as shown in Figure~\ref{fig:example-of-pond-ground-heat-exchanger-as-only}) or it may be connected in parallel with other condenser loop heat exchangers (such as cooling towers, ground surface heat exchangers) as shown in the second figure below.
+
+\begin{figure}[hbtp] % fig 84
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image203.png}
+\caption{Example of Pond Ground Heat Exchanger as only heat exchanger on condenser loop \protect \label{fig:example-of-pond-ground-heat-exchanger-as-only}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 85
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image204.png}
+\caption{Pond Ground Heat Exchanger with other heat exchangers on condenser loop \protect \label{fig:pond-ground-heat-exchanger-with-other-heat}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-12-002}
+
+\paragraph{Field: Name}\label{field-name-11-002}
+
+This alpha field contains the identifying name for the outside pond heat exchanger.
+
+\paragraph{Field: Fluid Inlet Node Name}\label{field-fluid-inlet-node-name}
+
+This alpha field contains the fluid inlet node name.
+
+\paragraph{Field: Fluid Outlet Node Name}\label{field-fluid-outlet-node-name}
+
+This alpha field contains the fluid outlet node name.
+
+\paragraph{Field: Pond Depth}\label{field-pond-depth}
+
+This numeric field contains the pond depth \{m\}.
+
+\paragraph{Field: Pond Area}\label{field-pond-area}
+
+This numeric field contains the pond area m\(^{2}\).
+
+\paragraph{Field: Hydronic Tubing Inside Diameter}\label{field-hydronic-tubing-inside-diameter}
+
+This numeric field contains the hydronic tubing inside diameter \{m\}.
+
+\paragraph{Field: Hydronic Tubing Outside Diameter}\label{field-hydronic-tubing-outside-diameter}
+
+This numeric field contains the hydronic tubing outside diameter \{m\}.
+
+\paragraph{Field: Hydronic Tubing Thermal Conductivity}\label{field-hydronic-tubing-thermal-conductivity}
+
+This numeric field contains the hydronic tubing thermal conductivity in W/mK.
+
+\paragraph{Field: Ground Thermal Conductivity}\label{field-ground-thermal-conductivity-1}
+
+This numeric field contains the ground thermal conductivity in W/m\(^{2}\)K.
+
+\paragraph{Field: Number of Tubing Circuits}\label{field-number-of-tubing-circuits}
+
+This numeric field contains the number of hydronic tubing circuits, total in parallel in this pond..
+
+\paragraph{Field: Length of Each Tubing Circuit}\label{field-length-of-each-tubing-circuit}
+
+This numeric field contains length \{m\} of each hydronic tubing circuit.
+
+An example of the IDF is shown below.
+
+\begin{lstlisting}
+
+  GroundHeatExchanger:Pond,
+      Pond 1,                  !- Name
+      Condenser Tower 1 Inlet Node,  !- Fluid Inlet Node Name
+      Condenser Tower 1 Outlet Node,  !- Fluid Outlet Node Name
+      2.0,                     !- Pond Depth {m}
+      1000.0,                  !- Pond Area {m2}
+      0.02,                    !- Hydronic Tubing Inside Diameter {m}
+      0.025,                   !- Hydronic Tubing Outside Diameter {m}
+      0.4,                     !- Hydronic Tubing Thermal Conductivity {W/m-K}
+      1.0,                     !- Ground Thermal Conductivity {W/m2-K}
+      10,                      !- Number of Tubing Circuits
+      50.0;                    !- Length of Each Tubing Circuit {m}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-12-000}
+
+\begin{itemize}
+\item
+  HVAC,Average,Pond Heat Exchanger Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Pond Heat Exchanger Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Pond Heat Exchanger Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Pond Heat Exchanger Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Pond Heat Exchanger Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Pond Heat Exchanger Bulk Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Pond Heat Exchanger Heat Transfer Rate {[}W{]}}\label{pond-heat-exchanger-heat-transfer-rate-w}
+
+\paragraph{Pond Heat Exchanger Heat Transfer Energy {[}J{]}}\label{pond-heat-exchanger-heat-transfer-energy-j}
+
+These outputs are the pond ground heat exchanger heat transfer rate and total energy exchange for the timestep.
+
+\paragraph{Pond Heat Exchanger Mass Flow Rate {[}kg/s{]}}\label{pond-heat-exchanger-mass-flow-rate-kgs}
+
+\paragraph{Pond Heat Exchanger Inlet Temperature {[}C{]}}\label{pond-heat-exchanger-inlet-temperature-c}
+
+\paragraph{Pond Heat Exchanger Outlet Temperature {[}C{]}}\label{pond-heat-exchanger-outlet-temperature-c}
+
+These outputs are the pond fluid inlet and outlet temperatures and mass flow rate.
+
+\paragraph{Pond Heat Exchanger Bulk Temperature {[}C{]}}\label{pond-heat-exchanger-bulk-temperature-c}
+
+This output is the pond bulk temperature.
+
+\subsection{GroundHeatExchanger:Surface}\label{groundheatexchangersurface}
+
+The surface heat exchanger model is to simulate hydronic surface ground heat exchangers. This includes pavement surfaces with embedded pipes for snow-melting or heat rejection from hybrid ground source heat pump systems.
+
+The heat exchanger may be ground coupled or not. In the latter case the bottom surface is exposed to the wind but not solar gains. This type of heat exchanger is intended to be connected to the supply side of a condenser loop, and can be used with any type of plant loop. The surface heat exchanger may be specified as the only heat exchanger on the condenser loop (as shown in the first figure below) or it may be connected in parallel with other condenser loop heat exchangers (such as cooling towers, ground surface heat exchangers) as shown in the second figure below.
+
+\begin{figure}[hbtp] % fig 86
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image205.png}
+\caption{Example of Surface Ground Heat Exchanger as only heat exchanger on condenser loop \protect \label{fig:example-of-surface-ground-heat-exchanger}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 87
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image206.png}
+\caption{Surface Ground Heat Exchanger with other heat exchangers on condenser loop \protect \label{fig:surface-ground-heat-exchanger-with-other-heat}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-13-002}
+
+\paragraph{Field: Name}\label{field-name-12-001}
+
+This alpha field contains the identifying name for the outside panel heat exchanger.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-000}
+
+This alpha field contains the construction name. It must contain a valid ``Construction'' name that is usual for Surfaces. (Ref: Group -- Surface Construction Elements).
+
+\paragraph{Field: Fluid Inlet Node Name}\label{field-fluid-inlet-node-name-1}
+
+This alpha field contains the fluid inlet node name.
+
+\paragraph{Field: Fluid Outlet Node Name}\label{field-fluid-outlet-node-name-1}
+
+This alpha field contains the fluid outlet node name.
+
+\paragraph{Field: Hydronic Tubing Inside Diameter}\label{field-hydronic-tubing-inside-diameter-1}
+
+This numeric field contains the hydronic tubing inside diameter in m.
+
+\paragraph{Field: Number of Tubing Circuits}\label{field-number-of-tubing-circuits-1}
+
+This numeric field contains the number of hydronic tubing circuits.
+
+\paragraph{Field: Hydronic Tube Spacing}\label{field-hydronic-tube-spacing}
+
+This numeric field contains the hydronic tube spacing in m.
+
+\paragraph{Field: Surface Length}\label{field-surface-length}
+
+This numeric field contains the surface length in m.
+
+\paragraph{Field: Surface Width}\label{field-surface-width}
+
+This numeric field contains the surface width in m.
+
+\paragraph{Field: Lower Surface Environment}\label{field-lower-surface-environment}
+
+This alpha field expresses the lower surface exposure: Exposed or Ground.
+
+An example of this statement in an IDF is shown below:
+
+\begin{lstlisting}
+
+  GroundHeatExchanger:Surface,
+      SURFACE 1,               !- Name
+      Outside Surface Construction,  !- Construction Name
+      Condenser Tower 1 Inlet Node,  !- Fluid Inlet Node Name
+      Condenser Tower 1 Outlet Node,  !- Fluid Outlet Node Name
+      0.02,                    !- Hydronic Tubing Inside Diameter {m}
+      10.0,                    !- Number of Tubing Circuits
+      0.3,                     !- Hydronic Tube Spacing {m}
+      100.0,                   !- Surface Length {m}
+      100.0,                   !- Surface Width {m}
+      GROUND;                  !- Lower Surface Environment
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-13-000}
+
+\begin{itemize}
+\item
+  HVAC,Average,Ground Heat Exchanger Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Surface Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Ground Heat Exchanger Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Top Surface Temperature {[}C{]}
+\item
+  HVAC,Average Ground Heat Exchanger Bottom Surface Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Top Surface Heat Transfer Energy per Area {[}J/m2{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Bottom Surface Heat Transfer Energy per Area{[}J/m2{]}
+\item
+  HVAC,Sum,Ground Heat Exchanger Surface Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Source Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Ground Heat Exchanger Heat Transfer Rate {[}W{]}}\label{ground-heat-exchanger-heat-transfer-rate-w-2}
+
+\paragraph{Ground Heat Exchanger Surface Heat Transfer Rate {[}W{]}}\label{ground-heat-exchanger-surface-heat-transfer-rate-w}
+
+\paragraph{Ground Heat Exchanger Heat Transfer Energy {[}J{]}}\label{ground-heat-exchanger-heat-transfer-energy-j}
+
+These outputs are the source heat transfer rate, surface heat transfer rate and the total source energy input for the timestep.
+
+\paragraph{Ground Heat Exchanger Mass Flow Rate {[}kg/s{]}}\label{ground-heat-exchanger-mass-flow-rate-kgs-2}
+
+\paragraph{Ground Heat Exchanger Inlet Temperature {[}C{]}}\label{ground-heat-exchanger-inlet-temperature-c-2}
+
+\paragraph{Ground Heat Exchanger Outlet Temperature {[}C{]}}\label{ground-heat-exchanger-outlet-temperature-c-2}
+
+These outputs are the surface heat exchanger fluid inlet and outlet temperatures and mass flow rate.
+
+\paragraph{Ground Heat Exchanger Top Surface Temperature {[}C{]}}\label{ground-heat-exchanger-top-surface-temperature-c}
+
+\paragraph{Ground Heat Exchanger Bottom Surface Temperature {[}C{]}}\label{ground-heat-exchanger-bottom-surface-temperature-c}
+
+These outputs are the surface heat exchanger top and bottom surface temperatures.
+
+\paragraph{\texorpdfstring{Ground Heat Exchanger Top Surface Heat Transfer Energy per Area~ {[}J/m\(^{2}\){]}}{Ground Heat Exchanger Top Surface Heat Transfer Energy per Area~ {[}J/m\^{}\{2\}{]}}}\label{ground-heat-exchanger-top-surface-heat-transfer-energy-per-area-jm2}
+
+\paragraph{\texorpdfstring{Ground Heat Exchanger Bottom Surface Heat Transfer Energy per Area {[}J/m\(^{2}\){]}}{Ground Heat Exchanger Bottom Surface Heat Transfer Energy per Area {[}J/m\^{}\{2\}{]}}}\label{ground-heat-exchanger-bottom-surface-heat-transfer-energy-per-area-jm2}
+
+These outputs are the surface heat exchanger top and bottom surface flux.
+
+\paragraph{Ground Heat Exchanger Surface Heat Transfer Energy {[}J{]}}\label{ground-heat-exchanger-surface-heat-transfer-energy-j}
+
+This is the total surface energy exchange for the timestep.
+
+\paragraph{Ground Heat Exchanger Source Temperature {[}C{]}}\label{ground-heat-exchanger-source-temperature-c}
+
+This is the surface heat exchanger source temperature.
+
+\subsection{GroundHeatExchanger:HorizontalTrench}\label{groundheatexchangerhorizontaltrench}
+
+The horizontal trench ground heat exchanger object provides an alternate interface to the detailed PipingSystem:Underground:* objects.~ The same underlying simulation algorithm is utilized, providing a transient numerical simulation of soil with buried pipes and a detailed surface heat balance.~ The input syntax is much smaller and useful for simple applications.~ For full flexibility, use the PipingSystem:Underground:* objects to build a detailed simulation domain and piping circuit.~ For information regarding the simulation algorithms, see the engineering reference document section covering the buried piping system objects.
+
+\textbf{\emph{Field: Name}}
+
+This alpha field is used as an identifying field for the ground heat exchanger.
+
+\textbf{\emph{Field: Inlet Node Name}}
+
+This alpha field is the name of the inlet node of this component on a plant loop, and must match other topology definitions such as branch objects.
+
+\textbf{\emph{Field: Outlet Node Name}}
+
+This alpha field is the name of the outlet node of this component on a plant loop, and must match other topology definitions such as branch objects.
+
+\textbf{\emph{Field: Design Flow Rate {[}m3/s{]}}}
+
+This numeric field is the designed flow rate for this heat exchanger; the plant loop solver will attempt to meet this request based on flow and loop conditions.
+
+\textbf{\emph{Field: Trench Length in Pipe Axial Direction {[}m{]}}}
+
+This numeric field represents the axial length of each pipe trench.~ Each pipe defined for this ground heat exchanger will have the same length.~ If different pipes have different lengths, they must use separate GroundHeatExchanger:HorizontalTrench objects with different lengths.
+
+\textbf{\emph{Field: Number of Trenches}}
+
+This integer field is the number of trenches for this heat exchanger.~ Since each trench has a single pipe, this defines the number of ``pipe segments'' for this overall heat exchanger.~ The total piping length is then calculated as the trench length times the number of trenches.
+
+\textbf{\emph{Field: Horizontal Spacing Between Pipes {[}m{]}}}
+
+This numeric field represents the horizontal spacing (pipe centroid to pipe centroid) between pipes/trenches.
+
+\textbf{\emph{Field: Pipe Inner Diameter {[}m{]}}}
+
+This numeric field is the inner diameter of the pipe.~ The same pipe properties are used for all pipes in this heat exchanger.
+
+\textbf{\emph{Field: Pipe Outer Diameter {[}m{]}}}
+
+This numeric field is the outer diameter of the pipe.~ The same pipe properties are used for all pipes in this heat exchanger.
+
+\textbf{\emph{Field: Burial Depth {[}m{]}}}
+
+This numeric field is the burial depth of each pipe, from ground surface to pipe cross section centroid. The same pipe depth is used for all pipes in this heat exchanger.
+
+\textbf{\emph{Field: Soil Thermal Conductivity {[}W/mK{]}}}
+
+This numeric field is the soil thermal conductivity.
+
+\textbf{\emph{Field: Soil Density {[}kg/m3{]}}}
+
+This numeric field is the soil density.
+
+\textbf{\emph{Field: Soil Specific Heat {[}J/kgK{]}}}
+
+This numeric field is the nominal soil specific heat, but is corrected for moisture content and in freezing conditions.
+
+\textbf{\emph{Field: Pipe Thermal Conductivity {[}W/mK{]}}}
+
+This numeric field is the pipe thermal conductivity.
+
+\textbf{\emph{Field: Pipe Density {[}kg/m3{]}}}
+
+This numeric field is the pipe density.
+
+\textbf{\emph{Field: Pipe Specific Heat {[}J/kgK{]}}}
+
+This numeric field is the pipe specific heat.
+
+\textbf{\emph{Field: Soil Moisture Content Percent {[}\%{]}}}
+
+This numeric field represents the volume fraction, in percent, of water content in the soil.
+
+\textbf{\emph{Field: Soil Moisture Content Percent at Saturation {[}\%{]}}}
+
+This numeric field represents the volume fraction, in percent, of water content in the soil which results in saturation.
+
+\subsubsection{Inputs}\label{inputs-14-002}
+
+\paragraph{Field: Type of Undisturbed Ground Temperature Object}\label{field-type-of-undisturbed-ground-temperature-object-1}
+
+The type of undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
+
+\paragraph{Field: Name of Undisturbed Ground Temperature Object}\label{field-name-of-undisturbed-ground-temperature-object-1}
+
+The name of the undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
+
+\textbf{\emph{Field: Evapotranspiration Ground Cover Parameter {[}-{]}}}
+
+This numeric field specifies the ground cover effects used in the evapotranspiration model at the ground surface heat balance.~ The values range from 0 (solid, non-permeable ground surface) to 1.5 (wild growth).
+
+An example of this statement in an IDF is shown below:
+
+\begin{lstlisting}
+
+GroundHeatExchanger:HorizontalTrench,
+     My Pipe Circuit, !- Name
+     Plant Supply Intermediate Node, !- Inlet Node Name
+     Plant Supply Outlet Node, !- Outlet Node Name
+     0.004,       !- Design Flow Rate
+     75,          !- Trench Length in Pipe Axial Direction
+     2,           !- Number of Trenches
+     2.0,         !- Horizontal Spacing Between Pipes
+     0.016,       !- Pipe Inner Diameter
+     0.02667,     !- Pipe Outer Diameter
+     1.25,        !- Burial Depth
+     1.08,        !- Soil Thermal Conductivity
+     962,         !- Soil Density
+     2576,        !- Soil Specific Heat
+     0.3895,      !- Pipe Thermal Conductivity {W/m-K}
+     641,         !- Pipe Density {kg/m3}
+     2405,        !- Pipe Specific Heat {J/kg-K}
+     30,          !- Soil Moisture Content Volume Fraction {percent}
+     50,          !- Soil Moisture Content Volume Fraction at Saturation {percent}
+     Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
+     KATemps,     !- Name of Undisturbed Ground Temperature Object
+     0.408;       !- Evapotranspiration Ground Cover Parameter
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-14-000}
+
+\begin{itemize}
+\item
+  HVAC,Average,Ground Heat Exchanger Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Ground Heat Exchanger Fluid Heat Transfer Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Ground Heat Exchanger Mass Flow Rate {[}kg/s{]}}\label{ground-heat-exchanger-mass-flow-rate-kgs-3}
+
+The output provides the mass flow rate currently being sent through the heat exchanger.
+
+\paragraph{Ground Heat Exchanger Inlet Temperature {[}C{]}}\label{ground-heat-exchanger-inlet-temperature-c-3}
+
+\paragraph{Ground Heat Exchanger Outlet Temperature {[}C{]}}\label{ground-heat-exchanger-outlet-temperature-c-3}
+
+Temperature of fluid at the inlet and outlet of the heat exchanger.
+
+\paragraph{Ground Heat Exchanger Fluid Heat Transfer Rate {[}W{]}}\label{ground-heat-exchanger-fluid-heat-transfer-rate-w}
+
+Heat transfer rate for the heat exchanger, defined as positive for \textbf{\emph{fluid heat loss}}.
+
+\subsection{HeatExchanger:FluidToFluid}\label{heatexchangerfluidtofluid}
+
+A fluid-to-fluid heat exchanger designed to couple the supply side of one plant or condenser loop to the demand side of another plant or condenser loop. This heat exchanger is fairly general and can be configured for use in any application where any two loops need to be connected together. The only constraints are that that one side must be connected to the supply side of one loop and the other side connected to the demand side of a different loop.~ Because the heat exchanger is intended to be generic, its two sides are distinguished by the nature of loop side being connected.~ One side is called ``Loop Supply Side'' to indicate the heat exchanger is situated on the supply side of a loop. The other side is called ``Loop Demand Side'' to indicate it is on the demand side of a loop.~ The heat exchanger is intended to act as a supply component for the loop connected to it as the ``Loop Supply Side'' and as a demand component for the loop connected to it as the ``Loop Demand Side.''~ From the point of view of the heat exchanger model itself, the Loop Demand Side fluid serves as the source/sink to supply heating/cooling to the fluid in the Loop Supply Side.~ Only hydronic ``plant'' fluids are allowed, no air-side connections are possible with this heat exchanger.
+
+\begin{figure}[hbtp] % fig 88
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image207.png}
+\caption{Plant Fluid-to-Fluid Heat Exchanger \protect \label{fig:plant-fluid-to-fluid-heat-exchanger}}
+\end{figure}
+
+Various options are available for the heat exchanger model. The heat transfer between the two sides can be modeled using one of seven different models for different types of heat exchangers. Heat transfer is calculated and reported using a sign convention from chilled water applications where positive heat transfer indicates energy was extracted from the Loop Supply Side and added to the Loop Demand Side.
+
+There are eleven options for different ways to control the heat exchanger.~ One general type of control is ``OnOff'' where the flow through the heat exchanger is either fully on or fully off.~ Another type of control is ``Modulated'' where the flow through the Loop Demand Side is controlled to try and meet a target setpoint or load on the Loop Supply Side.
+
+This heat exchanger can be used for a wide variety of applications including chilled water, hot water, condenser, ground source, primary-secondary systems, etc.~ As of Version 8.0, this object replaces three separate objects that were available prior to version 8.0 of EnergyPlus.~ The former HeatExchanger:Hydronic object corresponds to a situation where the Loop Demand Side is the demand side of condenser loop, the Loop Supply Side is a the supply side of a chilled water loop, the control type is ``CoolingSetpointOnOffWithComponentOverride,'' and the remote override component is a chiller. The former HeatExchanger:WatersideEconomizer object corresponds to a situation where the Loop Demand Side is the demand side of condenser loop, the Loop Supply Side is a the supply side of a chilled water loop, and the control type is ``CoolingDifferentialOnOff.'' ~The former HeatExchanger:Plate object corresponds to a situation where the Loop Demand Side is the demand side of a condenser loop, the Loop Supply Side is the supply side of a second condenser loop, and the control type is ``UncontrolledOn.''
+
+\subsubsection{Inputs}\label{inputs-15-002}
+
+\paragraph{Field: Name}\label{field-name-13-001}
+
+This alpha field provides the unique identifying name for this heat exchanger.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-001}
+
+This field specifies the name of an availability schedule that can be used for supervisory control of the device.~ If blank, the default is that heat exchanger is always available.~ If a scheduled is named here, then the heat exchanger is available for use whenever the schedule value is greater than zero.~ The heat exchanger is not available whenever the schedule value is zero or less.
+
+\paragraph{Field: Loop Demand Side Inlet Node Name}\label{field-loop-demand-side-inlet-node-name}
+
+This field specifies the name of a plant system node that connects an inlet of the heat exchanger to the demand side of a loop.~ This node must be on a branch located on the demand side of a plant or condenser loop.
+
+\paragraph{Field: Loop Demand Side Outlet Node Name}\label{field-loop-demand-side-outlet-node-name}
+
+This field specifies the name of a plant system node that connects an outlet of the heat exchanger to the demand side of a loop.~ This node must be on a branch located on the demand side of a plant or condenser loop.
+
+\paragraph{Field: Loop Demand Side Design Flow Rate}\label{field-loop-demand-side-design-flow-rate}
+
+This field specifies the design flow rate, in m\(^{3}\)/s, of the hydronic fluid passing through the heat exchanger on the Loop Demand Side. This field is autosizable. When autosized, this design flow rate is set to equal the design flow rate for the Loop Supply Side.
+
+\paragraph{Field: Loop Supply Side Inlet Node Name}\label{field-loop-supply-side-inlet-node-name}
+
+This field specifies the name of a plant system node that connects an inlet of the heat exchanger to the supply side of a loop.~ This node must be on a branch located on the supply side of a plant or condenser loop.
+
+\paragraph{Field: Loop Supply Side Outlet Node Name}\label{field-loop-supply-side-outlet-node-name}
+
+This field specifies the name of a plant system node that connects an outlet of the heat exchanger to the supply side of a loop.~ This node must be on a branch located on the supply side of a plant or condenser loop.
+
+\paragraph{Field: Loop Supply Side Design Flow Rate}\label{field-loop-supply-side-design-flow-rate}
+
+This field specifies the design flow rate, in m\(^{3}\)/s, of the fluid passing through the heat exchanger on the Loop Supply Side. This field is autosizable. When autosized, this design flow rate is set equal to the overall design flow rate of the loop that is connected.~ If a sizing factor is entered in the field below, then it is multiplied to modify the design flow rate.
+
+\paragraph{Field: Heat Exchange Model Type}\label{field-heat-exchange-model-type}
+
+This alpha field identifies the nature of heat exchanger.~ Heat exchanger model type is specified by one of the following four key word choices:
+
+\begin{itemize}
+\item
+  \textbf{CrossFlowBothUnMixed}.~ Specifies a single-pass, cross-flow heat exchanger.~ The effectiveness will be calculated using a cross-flow heat exchanger correlation for both streams unmixed.
+\item
+  \textbf{CrossFlowBothMixed}.~ Specifies a single-pass, cross-flow heat exchanger. The effectiveness will be calculated using a cross-flow heat exchanger correlation for both streams mixed.
+\item
+  \textbf{CrossFlowSupplyMixedDemandUnMixed}.~ Specifes a single-pass, cross-flow heat exchanger.~ The effectiveness will be calculated using a cross-flow heat exchanger correlation for flow mixed on the Loop Supply side and flow unmixed on the Loop Demand Side.
+\item
+  \textbf{CrossFlowSupplyUnMixedDemandMixed}.~~ Specifes a single-pass, cross-flow heat exchanger.~ The effectiveness will be calculated using a cross-flow heat exchanger correlation for flow unmixed on the Loop Supply side and flow mixed on the Loop Demand Side.
+\item
+  \textbf{CounterFlow}. Specifies a counter-flow shell and tube heat exchanger.~ The effectiveness will be calculated using a counter-flow shell and tube heat exchanger correlation.
+\item
+  \textbf{ParallelFlow}. Specifies a parallel-flow shell and tube heat exchanger.~ The effectiveness will be calculated using a parallel-flow shell and tube heat exchanger correlation.
+\item
+  \textbf{Ideal}. Specifies an ideal heat exchanger.~ The effectiveness will be set to `1.0' and the specified UA will be ignored.~ The heat transfer rate will be calculated as the maximum possible heat transfer rate.
+\end{itemize}
+
+\paragraph{Field: Heat Exchanger U-Factor Times Area Value}\label{field-heat-exchanger-u-factor-times-area-value}
+
+This numerical field is used to specify the overall U-Factor Times Area (UA) \{W/K\} for use in the calculation of the heat exchanger effectiveness using the appropriate D-NTU correlation.~ If \textbf{Ideal} is specified as the heat exchanger type, the effectiveness will be set to 1.0. When set to autosize Heat Exchanger U-Factor Times Area Value is calculated based on an effectiveness of 1.0 where capacity is such that the temperatures in the Sizing:Plant objects for the two loops can be maintained.
+
+\paragraph{Field: Control Type}\label{field-control-type}
+
+This field is used to specify how the heat exchanger is to be controlled during operation.~ Different applications for connecting two loops will require different control behavior and different control options are needed depending on the desired behavior.~ There are the following eleven key choice options to choose from:
+
+\begin{itemize}
+\item
+  \textbf{UncontrolledOn}. This control mode is applicable to situations where the heat exchanger is passively running all the time and always transfers as much heat as possible between the fluid streams.~ However there is one aspect of control in that it will only request flow on the Loop Demand Side when there is non-zero flow into the heat exchanger on the Loop Supply Side.~ This control mode corresponds to that available in the HeatExchanger:Plate object prior to version 8.0.
+\item
+  \textbf{OperationSchemeModulated}.~ This control mode is applicable to situations where the heat exchanger is controlled by an operation scheme (see objects called PlantEquipmentOperationScheme or CondenserEquipmentOperationSchemes).~ When using this control mode the heat exchanger must be listed in PlantEquipmentList or a CondenserEquipmentList and it serves as a supply component.~ The operation scheme will dispatch a load request to the heat exchanger which it will try meet by conditioning the fluid stream connected as the Loop Supply Side.~ If the heat exchanger could exceed the load request, then the flow through the fluid stream connected as the Loop Demand Side will be modulated to just meet the load request.
+\item
+  \textbf{OperationSchemeOnOff}. This control mode is applicable to situations where the heat exchanger is controlled by an operation scheme (see objects called PlantEquipmentOperationScheme or CondenserEquipmentOperationSchemes).~ When using this control mode the heat exchanger must be listed in PlantEquipmentList or a CondenserEquipmentList and it serves as a supply component.~ The operation scheme will dispatch a load request to the heat exchanger which it will use as an on/off signal to decide if the heat exchange should run or not.~ If it runs, it will run at full capacity and may exceed the load request.
+\item
+  \textbf{HeatingSetpointModulated}.~ This control mode is applicable to situations where the Loop Demand Side can provide useful heating to the Loop Supply Side.~ A heating setpoint is obtained from a node named in the following field.~ If the setpoint and inlet temperatures are such that heat exchanger could transfer heat from the Loop Demand Side to the Loop Supply Side to meet the heating setpoint, then the heat exchanger will run.~ The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate. ~If the heat exchanger could overshoot the setpoint, then the flow through the fluid stream connected as the Loop Demand Side will be modulated to just meet the setpoint.
+\item
+  \textbf{HeatingSetpointOnOff}. This control mode is applicable to situations where the Loop Demand Side can provide useful heating to the Loop Supply Side.~ A heating setpoint is obtained from a node named in the following field.~ If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Demand Side to the Loop Supply Side to meet the heating setpoint, then the heat exchanger will run. The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate. ~If it runs, it will run at full capacity and may overshoot the setpoint.
+\item
+  \textbf{CoolingSetpointModulated}.~ This control mode is applicable to situations where the Loop Demand Side can provide useful cooling to the Loop Supply Side.~ A cooling setpoint is obtained from a node named in the following field.~ If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Supply Side to the Loop Demand Side to meet the cooling setpoint, then the heat exchanger will run. The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate. If the heat exchanger could undershoot the setpoint, then the flow through the fluid stream connected as the Loop Demand Side will be modulated to just meet the setpoint.
+\item
+  \textbf{CoolingSetpointOnOff}. This control mode is applicable to situations where the Loop Demand Side can provide useful cooling to the Loop Supply Side.~ A cooling setpoint is obtained from a node named in the following field.~ If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Supply Side to the Loop Demand Side to meet the cooling setpoint, then the heat exchanger will run. The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate. If it runs, it will run at full capacity and may undershoot the setpoint.~ This control mode corresponds to that available in the HeatExchanger:WatersideEconomizer object prior to version 8.0.
+\item
+  \textbf{DualDeadbandSetpointModulated}. This control mode is applicable to situations where the Loop Demand Side can provide either useful cooling or heating to the Loop Supply Side.~ A dual deadband setpoint is obtained from a node named in the following field.~ If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Demand Side to the Loop Supply Side to meet the lower setpoint, then the heat exchanger will run. If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Supply Side to the Loop Demand Side to meet the high setpoint, then the heat exchanger will run. The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate.~ If the heat exchanger could overshoot the lower setpoint, or undershoot the higher setpoint, then the flow through the fluid stream connected as the Loop Demand Side will be modulated to just meet the deadband setpoint.
+\item
+  \textbf{DualDeadbandSetpointOnOff}. This control mode is applicable to situations where the Loop Demand Side can provide either useful cooling or heating to the Loop Supply Side.~ A dual deadband setpoint is obtained from a node named in the following field.~ If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Demand Side to the Loop Supply Side to meet the lower setpoint, then the heat exchanger will run. If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Supply Side to the Loop Demand Side to meet the high setpoint, then the heat exchanger will run. The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate. If the heat exchanger runs, it will run at full capacity and may overshoot the lower setpoint or undershoot the higher setpoint.
+\item
+  \textbf{CoolingDifferentialOnOff}.~ This control mode is applicable to situations where the Loop Demand Side can provide useful cooling to the Loop Supply Side.~ This mode is similar to CoolingSetpointOnOff except that it ignores any cooling setpoint and its control is based only on the temperature difference between Loop Demand Side and the Loop Supply Side.~ The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate.~ ~This control mode corresponds to that available in the HeatExchanger:WatersideEconomizer object prior to version 8.0.
+\item
+  \textbf{CoolingSetpointOnOffWithComponentOverride}.~ This control mode is applicable to situations where the heat exchanger operation is integrated with the operation of a specific chiller.~ When conditions are favorable for the heat exchanger to provide cooling to the Loop Supply Side, the heat exchanger is run and the integrated chiller is turned off.~ A cooling setpoint is obtained from a node named in the following field.~~ If it runs it will run at full capacity and may undershoot the setpoint.~ The chiller that is integrated with the heat exchanger is identified by entering the names of the chiller's inlet nodes in the input fields below.~ The control decision can be based on one of three different temperature signals selected in the field below called Component Override Cooling Control Temperature Mode.~ The setpoint and control signal temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate. This control mode corresponds to that available in the HeatExchanger:Hydronic object prior to version 8.0.
+\end{itemize}
+
+\paragraph{Field: Heat Exchanger Setpoint Node Name}\label{field-heat-exchanger-setpoint-node-name}
+
+This field specifies the name of a plant system node located on loop attached to the Loop Supply Side.~ This field is used and required when the previous field is set to one of the ``Setpoint'' control types.~ The node must have a temperature setpoint placed on it by a setpoint manager (or EMS actuator).
+
+If the previous field is set to DualDeadbandSetpointModulated or DeadbandSetpointOnOff then there must be a setpoint manager that places both a high and low setpoint on the node named in this field. (see SetpointManager:Scheduled:DualSetpoint).
+
+\paragraph{Field: Minimum Temperature Difference to Activate Heat Exchanger}\label{field-minimum-temperature-difference-to-activate-heat-exchanger}
+
+This field specifies the value of a temperature tolerance used in control decisions, in deg. Celsius.~ Whenever the control logic needs to compare two temperatures, the value entered in this field is used as a threshold for comparisons.
+
+\paragraph{Field: Heat Transfer Metering End Use Type}\label{field-heat-transfer-metering-end-use-type}
+
+This field specifies how the metering for heat transfer will be accounted with respect to end uses.~ Although the heat exchanger consumes no energy that needs to be metered, there are also meters for heat transfers that apply to the model. The nature of the end use may vary depending on the application that the heat exchanger is being used for.~ The available choices are FreeCooling, HeatRecovery, HeatRejection, HeatRecoveryForCooling, HeatRecoveryForHeating, and LoopToLoop.
+
+\paragraph{Field: Component Override Loop Supply Side Inlet Node Name}\label{field-component-override-loop-supply-side-inlet-node-name}
+
+This field specifies the name of an inlet node for the remote component that will be integrated with this heat exchanger.~ This inlet should be on the supply side of a loop -- typically chilled water inlet or return for a chiller.~ This field and the next two are only used for the control type called CoolingSetpointOnOffWithComponentOverride.
+
+\paragraph{Field: Component Override Loop Demand Side Inlet Node Name}\label{field-component-override-loop-demand-side-inlet-node-name}
+
+This field specifies the name of an inlet node for the remote component that will be integrated with this heat exchanger.~ This inlet should be on the demand side of a loop -- typically condenser water inlet or return for a water-cooled chiller.~ This field is only used for the control type called CoolingSetpointOnOffWithComponentOverride.
+
+\paragraph{Field: Component Override Cooling Control Temperature Mode}\label{field-component-override-cooling-control-temperature-mode}
+
+This field specifies which type of temperature is used to control a heat exchanger that uses the control type called CoolingSetpointOnOffWithComponentOverride.~ There are three options: Loop, WetBulbTemperature, and DryBulbTemperature.~ The option called ``Loop'' directs the program to use the inlet fluid temperature at the Loop Demand Side connection of~ heat exchanger for the temperature used as a signal to be compared with the setpoint. The option call ``WetBulbTemperature'' uses the outdoor air wetbulb temperature as the signal.~ The option called ``DryBulbTemperature'' uses the outdoor air drybulb temperature as the signal.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-4}
+
+This optional field can be used to modify the results of autosize calculations.~ This sizing factor is used for this heat exchanger and modifies sizing results by multiplying them by the factor entered here.~ This factor is applied to the Loop Supply Side Design Flow rate and in turn affects the heat exchanger UA and the loop demand side flow rate which are derived from that flow rate.~ This allows fine control over the size of the heat exchanger when using autosize in those fields.
+
+\paragraph{Field: Operation Minimum Temperature Limit}\label{field-operation-minimum-temperature-limit}
+
+This optional field can be used to provide supervisory control of the heat exchanger. If either of the inlet temperatures are below this limit (°C), the heat exchanger will not operate.
+
+\paragraph{Field: Operation Maximum Temperature Limit}\label{field-operation-maximum-temperature-limit}
+
+This optional field can be used to provide supervisory control of the heat exchanger. If either of the inlet temperatures are above this limit~ (°C), the heat exchanger will not operate.
+
+Some example IDF input objects follow.
+
+\begin{lstlisting}
+
+  HeatExchanger:FluidToFluid,
+      CondenserLoop HX,!- Name
+      ALWAYS_ON,     !- Availability Schedule Name
+      CondenserLoop HX HX Inlet Node, !- Loop Demand Side Inlet Node Name
+      CondenserLoop HX HX Outlet Node, !- Loop Demand Side Outlet Node Name
+      autosize,                     !- Loop Demand Side Design Flow Rate
+      CondenserLoop Pump- HXNode,   !- Loop Supply Side Inlet Node Name
+      CondenserLoop HX- ChillerNode,!- Loop Supply Side Outlet Node Name
+      autosize,                !- Loop Supply Side Design Flow Rate
+      CounterFlow,             !- Heat Exchange Model Type
+      autosize,                !- Heat Exchanger U-Factor Times Area Value
+      CoolingDifferentialOnOff,    !- Control Type
+      ,   !- Heat Exchanger Setpoint Node Name
+      2.0,         !- Minimum Temperature Difference to Activate Heat Exchanger
+      FreeCooling;             !- Heat Transfer Metering End Use Type
+
+
+  HeatExchanger:FluidToFluid,
+      SOURCE to TRANSFER HX , !- Name
+      AlwaysOnSchedule, !- Availability Schedule Name
+      SOURCE Demand HX Inlet Node , !- Loop Demand Side Inlet Node Name
+      SOURCE Demand HX Outlet Node , !- Loop Demand Side Outlet Node Name
+      0.003 , !- Loop Demand Side Design Flow Rate
+      TRANSFER HX Supply Inlet Node, !- Loop Supply Side Inlet Node Name
+      TRANSFER HX Supply Outlet Node, !- Loop Supply Side Outlet Node Name
+      0.003 , !- Loop Supply Side Design Flow Rate
+      CrossFlow, !- Heat Exchange Model Type
+      15000 , !- Heat Exchanger U-Factor Times Area Value
+      DualDeadbandSetpointModulated , !- Control Type
+      TRANSFER Supply Outlet Node, !- Heat Exchanger Setpoint Node Name
+      0.2 , !- Minimum Temperature Difference to Activate Heat Exchanger
+      LoopToLoop; !- Heat Transfer Metering End Use Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-15}
+
+\paragraph{Fluid Heat Exchanger Heat Transfer Rate {[}W{]}}\label{fluid-heat-exchanger-heat-transfer-rate-w}
+
+\paragraph{Fluid Heat Exchanger Heat Transfer Energy {[}J{]}}\label{fluid-heat-exchanger-heat-transfer-energy-j}
+
+These outputs are the rate and energy transferred from the Loop Supply Side to the Loop Demand Side.~ The sign convention is taken from cooling or heat rejection applications such that positive values indicate cooling of the Loop Supply Side.
+
+\paragraph{Fluid Heat Exchanger Loop Supply Side Mass Flow Rate {[}kg/s{]}}\label{fluid-heat-exchanger-loop-supply-side-mass-flow-rate-kgs}
+
+This is the system mass flow of fluid through the heat exchanger side connected as the Loop Supply Side, in kg/s.
+
+\paragraph{Fluid Heat Exchanger Loop Supply Side Inlet Temperature {[}C{]}}\label{fluid-heat-exchanger-loop-supply-side-inlet-temperature-c}
+
+This is the temperature, in degrees Celsius, of the fluid entering the heat exchanger on the side connected as the Loop Supply Side.
+
+\paragraph{Fluid Heat Exchanger Loop Supply Side Outlet Temperature {[}C{]}}\label{fluid-heat-exchanger-loop-supply-side-outlet-temperature-c}
+
+This is the temperature, in degrees Celsius, of the fluid leaving the heat exchanger on the side connected as the Loop Supply Side.
+
+\paragraph{Fluid Heat Exchanger Loop Demand Side Mass Flow Rate {[}kg/s{]}}\label{fluid-heat-exchanger-loop-demand-side-mass-flow-rate-kgs}
+
+This is the system mass flow of fluid through the heat exchanger side connected as the Loop Demand Side, in kg/s.
+
+\paragraph{Fluid Heat Exchanger Loop Demand Side Inlet Temperature {[}C{]}}\label{fluid-heat-exchanger-loop-demand-side-inlet-temperature-c}
+
+This is the temperature, in degrees Celsius, of the fluid entering the heat exchanger on the side connected as the Loop Demand Side.
+
+\paragraph{Fluid Heat Exchanger Loop Demand Side Outlet Temperature {[}C{]}}\label{fluid-heat-exchanger-loop-demand-side-outlet-temperature-c}
+
+This is the temperature, in degrees Celsius, of the fluid leaving the heat exchanger on the side connected as the Loop Demand Side.
+
+\paragraph{Fluid Heat Exchanger Operation Status {[}0 = off, 1 = on{]}}\label{fluid-heat-exchanger-operation-status-0-off-1-on}
+
+This output is a numeric flag that indicates whether or not the heat exchanger was operating or not.~ If the value is 0, then the heat exchanger was not operating.~ If the value is 1, then the heat was operating.
+
+\paragraph{\texorpdfstring{Fluid Heat Exchanger Effectiveness {[]}}{Fluid Heat Exchanger Effectiveness }}\label{fluid-heat-exchanger-effectiveness}
+
+This output is the calculated heat exchanger effectiveness (non-dimensional).~ It is an intermediate value in the NTU model calculations for heat flow rate.~ Values range between 0 and 1.0.~ A value of 1.0 indicates ideal heat transfer.
diff --git a/doc/input-output-reference/src/overview/group-controllers.tex b/doc/input-output-reference/src/overview/group-controllers.tex
new file mode 100644
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+++ b/doc/input-output-reference/src/overview/group-controllers.tex
@@ -0,0 +1,580 @@
+\section{Group Controllers}\label{group-controllers}
+
+\subsection{Controls (Air Loop and Zone Equipment)}\label{controls-air-loop-and-zone-equipment}
+
+A controller mimics the function of an actual physical controller in a somewhat rudimentary way. It can sense one node variable, compare it with its setpoint, and determine the desired value for another node variable. It should be noted that a controller cannot span a loop manager boundary (but a Setpoint Manager can). Thus, in an air loop (AirLoopHVAC), the sensed node and the controlled device must be in the air loop simulation. This means that a single zone system cannot be modeled with a simple controller sensing zone temperature and controlling coil water flow. Instead this must be modeled as a Setpoint Manager sensing a zone temperature and resetting the supply air temperature setpoint each timestep. This is artificial but should simplify the control modeling task. It should also be noted that there are various types of controllers and that each controller might hook into loops in a slightly different way. As a result, each controller type is described separately below.
+
+\subsection{Controller:WaterCoil}\label{controllerwatercoil}
+
+This controller is really a solution inverter. For a water coil the simulation cannot be inverted where the mass flow rate of the water through the coil can be solved directly given an air temperature. Thus, this controller will numerically step through all of the water flow possibilities by an interval-halving technique until the mass flow rate is determined to meet the specified outlet air temperature within a specified user tolerance.
+
+As the reader probably noted when reading the descriptions of the coil syntax shown earlier in this section, there were no controls attached directly to a particular component. This is because the input can be simplified somewhat by entering node names to be controlled. This avoids having to search through multiple lists of component types for the sake of simply controlling components. The Controller:WaterCoil shown below is a way of controlling variables at one node based on conditions at another node. After the identifying name for the controller, the user must define which control variable the controller is managing. These options include Temperature, Humidity Ratio, TemperatureAndHumidityRatio, or Flow.
+
+The next parameter in the input syntax is the Action of the control, which determines how the controlled variable (e.g., mass flow rate through a water coil) is changed based on the control signal. The following input parameter is the actuator variable, which is currently limited to mass flow through a water coil.
+
+The next two parameters in the input syntax are node names corresponding to the node that is being sensed and the actuated node which controls the water mass flow through the coil. For example, in the case of a cooling coil the control variable might be the outlet air temperature of the coil while the actuated variable might be the water flow rate through the coil. These two parameters are followed by the controller convergence tolerance. Finally, the last two input parameters represent the maximum and minimum values allowed for the actuated variable at the actuated node.
+
+\subsubsection{Inputs}\label{inputs-008}
+
+\paragraph{Field: Name}\label{field-name-007}
+
+This is the unique name of the controller.
+
+\paragraph{Field: Control Variable}\label{field-control-variable}
+
+This was setup to be generic but to date has only been used for temperature control, or temperature and humidity ratio control, of a water coil in the air loop simulation. The keyword Temperature is used for air temperature control and is normally specified for the coils outlet air node. The keyword TemperatureAndHumidityRatio is used for controlling both air temperature and high humidity levels, and is normally specified for a cooling coils outlet air node. The keyword HumidityRatio is used for humidity control and would normally be specified for a dehumidifier outlet node. These two keywords require a ZoneControl:Humidistat object and a maximum humidity setpoint manager object (SetPointManager:SingleZone:Humidity:Maximum, SetPointManager:MultiZone:MaximumHumidity:Average or SetPointManager:MultiZone:Humidity:Maximum). If the coil is located in the outdoor air stream, it may also be necessary to use SetpointManager:OutdoorAirPretreat.
+
+\paragraph{Field: Action}\label{field-action}
+
+The next input refers to the action of the control. This can be best described by an example. In a coil where water mass flow rate is to be controlled, a coil will increase the mass flow rate through the coil when more heating or cooling is requested. In a heating coil, this increases the value of heat transfer from the water to the air stream. As a result, this is considered a Normal action controller. In a cooling coil, an increase in water mass flow rate through the coil decreases the value of heat transfer from the water to the air stream (absolute value increases, but since cooling is traditionally described as a negative number, an increase in absolute value results in a decrease in the actual heat transfer value). Thus, the cooling coil controller has Reverse action since an increase in flow rate results in a decrease in heat transfer.
+
+\paragraph{Field: Actuator Variable}\label{field-actuator-variable}
+
+This was again meant to be more generic but currently has only been used to control the water mass flow rate of a heating or cooling coil. This actuator variable must be set to the keyword Flow to control the water mass flow rate.
+
+\paragraph{Field: Sensor Node Name}\label{field-sensor-node-name}
+
+Name of the node where the temperature, humidity ratio or flow is sensed.
+
+\paragraph{Field: Actuator Node Name}\label{field-actuator-node-name}
+
+Name of the actuated node that controls the water mass flow rate through the coil.
+
+\paragraph{Field: Controller Convergence Tolerance}\label{field-controller-convergence-tolerance}
+
+The coil is controlled by knowing the outlet temperature and/or humidity ratio specified by the setpoint managers, and setting the outlet conditions from the coil to meet these setpoints. The hot and chilled water coils use complex models that cannot be inverted directly. Therefore, to determine the correct mass flow rate for the hot or cold water the models are inverted numerically using an iterative procedure. The iterative solution uses an interval-halving routine and needs a termination criteria that is set with the Controller Convergence Tolerance parameter. The convergence tolerance is the maximum difference between the actual temperature at the setpoint node and the setpoint temperature. This control offset is set to a small temperature difference, such as 0.01 to denote 1/100 degree C. The default is 0.1 degree C.
+
+\paragraph{Field: Maximum Actuated Flow}\label{field-maximum-actuated-flow}
+
+This is the maximum water flow (m\(^{3}\)/sec) through the coil. Set to the maximum design water flow for the coil.
+
+\paragraph{Field: Minimum Actuated Flow}\label{field-minimum-actuated-flow}
+
+Set to the minimum design water flow (m\(^{3}\)/sec) for the water coil, normally a shut off valve that is set to zero.
+
+An example of this object in an IDF, along with appropriate setpoint managers, is shown below:
+
+\begin{lstlisting}
+
+Controller:WaterCoil,
+  Central Cooling Coil Contoller 1,     !- Name
+  TemperatureAndHumidityRatio,          !- Control Variable
+  Reverse,                              !- Action
+  Flow,                                 !- Actuator Variable
+  VAV Sys 1 Outlet Node,                !- Sensor Node Name
+  Main Cooling Coil 1 Water Inlet Node, !- Actuator Node Name
+  0.002,                                !- Controller Convergence Tolerance {deltaC}
+  0.025,                                !- Maximum Actuated Flow {m3/s}
+  0.0;                                  !- Minimum Actuated Flow {m3/s}
+
+
+  SetpointManager:SingleZone:Humidity:Maximum,
+  Zone Max Set Point Manager,           !- Name
+  ,                                     !- Control Variable
+  ,                                     !- Schedule name
+  VAV Sys 1 Outlet Node,                !- Setpoint Node or NodeList Name
+  Zone 2 Node;                          !- Control Zone Air Node Name
+
+
+  SetpointManager:Scheduled,
+  Scheduled Set Point Manager 1,        !- Name
+  Temperature,                          !- Control Variable
+  Seasonal Reset Supply Air Temp Sch,   !- Schedule Name
+  VAV Sys 1 Outlet Node;                !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{Controller:OutdoorAir}\label{controlleroutdoorair}
+
+A mixed air box has its own controller type called Controller:OutdoorAir. The purpose of the outdoor air controller is to provide outdoor air for ventilation and also provide free cooling (through additional outdoor air and/or bypassing an air-to-air heat exchanger) whenever possible. The outdoor air controller includes a number of user-selectable limit controls. If any of the selected limits are exceeded, the outdoor airflow rate is set to the minimum.
+
+If all the limits are satisfied, the outdoor air controller does the following for continuous air flow systems: if the outdoor air temperature is greater than or equal to the mixed air temperature setpoint, the outdoor air flow rate is set to the maximum; if the outdoor air temperature is less than the mixed air temperature setpoint, the outdoor air controller will modulate the outdoor air flow so that the mixed air temperature will match the mixed air setpoint temperature.
+
+A time-of-day schedule may also be used to simulate an increase in outdoor air flow rate for push-button type economizer applications. When the schedule permits (i.e., schedule values are greater than 0), the outdoor air flow rate is increased to the user-specified maximum outdoor air flow rate.
+
+The outdoor air controller can also account for changes in the outdoor air flow rate during times when indoor humidity levels are high. A zone humidistat must be used with this control option. During high indoor humidity, the outdoor air flow rate is modified in response to a high indoor humidity condition. If high humidity control is based on the outdoor air humidity ratio and the outdoor humidity ratio is greater than the indoor humidity ratio, high humidity control is terminated. When the economizer is used in conjunction with the high humidity control option, high humidity control has priority and controls the change in air flow rates. The Night Ventilation Availability Manager has priority over high humidity control and will use the controllers maximum outdoor air flow rate when this Availability Manager cycles the fan on (Ref. System Availability Managers AvailabilityManager:NightVentilation)
+
+The mixed air box connections are defined separately in the \textbf{OutdoorAir:Mixer} object.
+
+Although the mixer will commonly be connected directly to the outdoor air, other components may be placed on the outdoor air path upstream of the mixer. When this is the case, any modulation will be determined by the conditions at the inlet node of the mixer rather than the outdoor air. This means that the controller will account for any heat recovery or other preheating/precooling components that may modify the condition of outdoor air before it reaches the mixer.
+
+If all the limits are satisfied, the outdoor air controller does the following for cycling fan systems: the outdoor air flow rate is set to the maximum when the fan cycles on. If the limits are not satisfied, the outdoor air flow rate is at the minimum when the fan cycles on.
+
+\subsubsection{Inputs}\label{inputs-1-007}
+
+\paragraph{Field: Name}\label{field-name-1-006}
+
+The unique user-assigned name for an instance of an outdoor air controller. Any other object referencing this outdoor air controller will use this name.
+
+\paragraph{Field: Relief Air Outlet Node Name}\label{field-relief-air-outlet-node-name}
+
+The name of the relief air node of the outdoor air mixer associated with this outdoor air controller.
+
+\paragraph{Field: Return Air Node Name}\label{field-return-air-node-name}
+
+The name of the return air node of the outdoor air mixer associated with this outdoor air controller.
+
+\paragraph{Field: Mixed Air Node Name}\label{field-mixed-air-node-name-000}
+
+Name of the node where the mixed air setpoint is set. The outdoor air controller senses the temperature at this node and attempts to control that temperature to the node setpoint.
+
+\paragraph{Field: Actuator Node Name}\label{field-actuator-node-name-1}
+
+The name of the node that is associated with the outdoor air damper. This should be the outermost air node on the outdoor air path connected to the outdoor air stream for the mixer associated with this outdoor air controller.
+
+\paragraph{Field: Minimum Outdoor Air Flow Rate}\label{field-minimum-outdoor-air-flow-rate}
+
+Input for this field is the minimum outdoor air flow rate for the system in cubic meters per second.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate}
+
+Input for this field is the maximum outdoor air flow rate for the system in cubic meters per second.
+
+\paragraph{Field: Economizer Control Type}\label{field-economizer-control-type}
+
+The options for this field are
+
+\begin{itemize}
+\item
+  FixedDryBulb
+\item
+  DifferentialDryBulb
+\item
+  FixedEnthalpy
+\item
+  DifferentialEnthalpy
+\item
+  ElectronicEnthalpy
+\item
+  FixedDewPointAndDryBulb
+\item
+  DifferentialDryBulbAndEnthalpy
+\item
+  NoEconomizer
+\end{itemize}
+
+Choosing \textbf{NoEconomizer} means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
+
+Choosing \textbf{FixedDryBulb} means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
+
+Choosing \textbf{DifferentialDryBulb} will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
+
+\textbf{FixedEnthalpy} checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
+
+\textbf{DifferentialEnthalpy} does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
+
+Choosing \textbf{ElectronicEnthalpy} enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
+
+Choosing \textbf{FixedDewPointAndDryBulb} compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
+
+Another option \textbf{DifferentialDryBulbAndEnthalpy} enables the control strategy to be based on both the DifferentialDryBulb and DifferentialEnthalpy economizer control strategies.
+
+In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
+
+The default for this field is \textbf{NoEconomizer}.
+
+\paragraph{Field: Economizer Control Action Type}\label{field-economizer-control-action-type}
+
+There are two choices for this Field: \textbf{MinimumFlowWithBypass} and \textbf{ModulateFlow}, with the default being \textbf{ModulateFlow} if this input field is left blank.
+
+\textbf{ModulateFlow} means the outdoor air flow rate will be increased to meet the mixed air setpoint temperature, subject to the limits imposed via other inputs for this object (e.g., Economizer Maximum Limit Dry-Bulb Temperature, Maximum Outdoor Air Flow Rate, etc.).
+
+\textbf{MinimumFlowWithBypass} is used exclusively in conjunction with air-to-air heat exchanger:objects (Ref. HeatExchanger:*) for providing free cooling operation in the absence of a conventional air-side economizer (i.e., when outdoor air flow rate is not increased during economizer mode). The MinimumFlowWithBypass choice forces the outdoor air flow rate to always remain at the minimum. However, when high humidity control is used, the outdoor air flow rate is set to the product of the maximum outdoor air flow rate multiplied by the high humidity outdoor air flow ratio. The heat exchanger uses the limit checking in the outdoor air controller to decide whether or not to bypass the outdoor air around the heat exchanger or turn off the wheel motor in the case of a rotary heat exchanger. Heat exchange is also suspended when high humidity control is active.
+
+The \textbf{ModulateFlow} option can also be used with the HeatExchanger:AirToAir:FlatPlate or HeatExchanger:AirToAir:SensibleAndLatent objects.
+
+\paragraph{Field: Economizer Maximum Limit Dry-Bulb Temperature}\label{field-economizer-maximum-limit-dry-bulb-temperature}
+
+Input for this field is the outdoor air temperature high limit ( °C) for economizer operation. If the outdoor air temperature is above this limit, the outdoor airflow rate will be set to the minimum. This field is required if Economizer Control Type FixedDryBulb or FixedDewPointAndDryBulb has been specified.
+
+No input (blank) in this field means that there is no outdoor air temperature high limit control. This limit applies to the conditions at the Actuator Node regardless of whether or not there are any other components in the outdoor air path upstream of the mixer. If non-blank, this limit is applied regardless of the specified Economizer Control Type.
+
+\paragraph{Field: Economizer Maximum Limit Enthalpy}\label{field-economizer-maximum-limit-enthalpy}
+
+Input for this field is the outdoor air enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor airflow rate will be set to the minimum. This field is required if Economizer Control Type FixedEnthalpy has been specified.
+
+No input (blank) in this field means that there is no outdoor air enthalpy limit control. This limit applies to the conditions at the Actuator Node regardless of whether or not there are any other components in the outdoor air path upstream of the mixer. If non-blank, this limit is applied regardless of the specified Economizer Control Type.
+
+\paragraph{Field: Economizer Maximum Limit Dewpoint Temperature}\label{field-economizer-maximum-limit-dewpoint-temperature}
+
+Input for this field is the outdoor air dewpoint limit (°C) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type FixedDewPointAndDryBulb has been specified.
+
+No input (blank) in this field means that there is no outdoor air dewpoint limit control. This limit applies to the conditions at the Actuator Node regardless of whether or not there are any other components in the outdoor air path upstream of the mixer. If non-blank, this limit is applied regardless of the specified Economizer Control Type.
+
+\paragraph{Field: Electronic Enthalpy Limit Curve Name}\label{field-electronic-enthalpy-limit-curve-name}
+
+Input for this field is the name of a quadratic or cubic curve which provides the maximum outdoor air humidity ratio (function of outdoor air dry-bulb temperature) for economizer operation. If the outdoor air humidity ratio is greater than the curve's maximum humidity ratio (evaluated at the outdoor air dry-bulb temperature), the outdoor air flow rate will be set to the minimum. This limit applies to the conditions at the Actuator Node regardless of whether or not there are any other components in the outdoor air path upstream of the mixer. No input (blank) in this field means that there is no electronic enthalpy limit control. If non-blank, this limit is applied regardless of the specified Economizer Control Type.
+
+\paragraph{Field: Economizer Minimum Limit Dry-Bulb Temperature}\label{field-economizer-minimum-limit-dry-bulb-temperature}
+
+Input for this field is the outdoor air temperature low limit ( °C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor airflow rate will be set to the minimum.
+
+No input (blank) in this field means that there is no outdoor air temperature low limit control. This limit applies to the conditions at the Actuator Node regardless of whether or not there are any other components in the outdoor air path upstream of the mixer. If non-blank, this limit is applied regardless of the specified Economizer Control Type.
+
+\paragraph{Field: Lockout Type}\label{field-lockout-type}
+
+Choices for this field are NoLockout, LockoutWithHeating, and LockoutWithCompressor. This field is used for packaged systems with DX coils. LockoutWithHeating means that if the packaged unit is in heating mode, the economizer is locked out i.e., the economizer dampers are closed and there is minimum outdoor air flow. LockoutWithCompressor means that in addition to locking out the economizer when the unit is in heating mode the economizer is locked out when the DX unit compressor is operating to provide cooling. In other words, the economizer must meet the entire cooling load; it is not allowed to operate in conjunction with the DX cooling coil. This option (LockoutWithCompressor) is sometimes called a nonintegrated economizer.
+
+When LockoutWithHeating or LockoutWithCompressor is selected, the lockout may also be applied to non-packaged systems for heating. If any air loop heating coil is operating, the lockout control compares the mixed air temperature at minimum outdoor air flow without heat recovery (if any) to the mixed air temperature set point. If the mixed air temperature at minimum outdoor air flow is less than the mixed air temperature set point, then the economizer is locked out and the outdoor air flow rate is set to the minimum. When the economizer is locked out, the heat recovery bypass control will be set to activate heat recovery (no bypass), if present. This action is meant to minimize heating energy (this action may also disable the heating coil on subsequent iterations, see output variable Air System Outdoor Air Heat Recovery Bypass Heating Coil Activity Status).
+
+The default is NoLockout.
+
+\paragraph{Field: Minimum Limit Type}\label{field-minimum-limit-type}
+
+Choices for this field are FixedMinimum or ProportionalMinimum. FixedMinimum means that the minimum outdoor airflow rate is fixed no matter what the actual system flow rate is. ProportionalMinimum means the minimum outdoor airflow rate varies in proportion to the total system air flow rate. The default is ProportionalMinimum.
+
+\paragraph{Field: Minimum Outdoor Air Schedule Name}\label{field-minimum-outdoor-air-schedule-name}
+
+The name of a schedule which uses decimal values (e.g., 0.0 or 1.0). These values are multiplied by the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours. If this field is not entered, the minimum outdoor air flow rate either remains constant during the simulation period (Minimum Outdoor Air Control Type = FixedMinimum) or varies in proportion to the supply air flow rate (Minimum Outdoor Air Control Type = ProportionalMinimum).
+
+\paragraph{Field: Minimum Fraction of Outdoor Air Schedule Name}\label{field-minimum-fraction-of-outdoor-air-schedule-name}
+
+The name of a schedule which uses decimal values (0.0 1.0) These values are multiplied by the total (design) air flow rate. This is an alternate method for specifying the minimum outdoor air amount. (The other method is the \textbf{\emph{Minimum Outdoor Air Schedule}} \emph{described above.) Note: This field overrides \textbf{Minimum Outdoor Air Schedule} and \textbf{Minimum Outdoor Air Flowrate.}}
+
+\paragraph{Field: Maximum Fraction of Outdoor Air Schedule Name}\label{field-maximum-fraction-of-outdoor-air-schedule-name}
+
+This is an optional field with the schedule values in decimal fractions (0.0-1.0). This field enables the user to limit the maximum of amount of outdoor air permissible and thus also limits the permissible maximum outdoor air into the system.
+
+If both the above schedules are given values of 1.0, the system works at 100\% outdoor air, so in a system if 100\% outdoor air is required regardless of any other condition, these fields are helpful.
+
+\paragraph{Field: Mechanical Ventilation Controller Name}\label{field-mechanical-ventilation-controller-name}
+
+This optional field is the name of the mechanical ventilation controller object to be used in conjunction with this outdoor air controller. The Controller:MechanicalVentilation object allows the user to define the minimum outdoor air flow rate based on air flow per unit floor area and air flow per person (occupant) for the zones being served by the air loop that utilizes this controller.
+
+This feature allows the user to perform a first-order evaluation of carbon dioxide(CO\(_{2}\))-based demand controlled ventilation (outdoor ventilation varied according to occupancy levels).
+
+If a valid name for a Controller:MechanicalVentilation object is entered in this field, the minimum outdoor air flow rate delivered will be the greater of:
+
+\begin{itemize}
+\item
+  the minimum outdoor air flow rate calculated by the fields Minimum Outdoor Air Flow Rate, Minimum Limit Type, and Minimum Outdoor Air Schedule Name as defined for this outdoor air controller, or
+\item
+  the outdoor air flow rate calculated using the Controller:MechanicalVentilation object named in this input field.
+\end{itemize}
+
+Leaving this input field blank will bypass the Controller:MechanicalVentilation object calculations and the minimum outdoor air flow rate will be based on the other inputs associated with this outdoor air controller object. Actual outdoor air flow rates may be higher than the minimum if free cooling is available and the object inputs are properly selected. Regardless, the maximum outdoor air flow rate is limited by the field Maximum Outdoor Air Flow Rate.
+
+\paragraph{Field: Time of Day Economizer Control Schedule Name}\label{field-time-of-day-economizer-control-schedule-name}
+
+This alpha field is the name of a schedule which controls the outdoor air flow rate based on a time-of-day economizer. Schedule values equal to 0 disable this feature. Schedule values greater than 0 cause the outdoor air flow rate to increase to the maximum. When an economizer is used in conjunction with the high humidity control option, high humidity control has priority.
+
+\paragraph{Field: High Humidity Control}\label{field-high-humidity-control}
+
+This choice field establishes whether or not the outdoor air flow rate is modified in response to high indoor relative humidity. Valid choices are Yes and No. If Yes is selected, the outdoor air flow rate may be modified when the indoor relative humidity is above the humidstat setpoint. If No is selected, this option is disabled and the following three fields are not used.
+
+\paragraph{Field: Humidistat Control Zone Name}\label{field-humidistat-control-zone-name}
+
+This input defines the zone name where the humidistat is located. This is the same name used in the ZoneControl:Humidistat object. This field is required when the input field High Humidity Control is specified as Yes.
+
+\paragraph{Field: High Humidity Outdoor Air Flow Ratio}\label{field-high-humidity-outdoor-air-flow-ratio}
+
+This input is the ratio of the modified outdoor air flow rate to the maximum outdoor air flow rate. When the high humidity control algorithm determines that the outdoor air flow rate will be changed (i.e., increased or decreased), the operating outdoor air flow rate is equal to the maximum outdoor air flow rate multiplied by this ratio. The minimum value for this field is 0. If this field is blank, the default value is 1. This field is used only when the input field High Humidity Control is specified as Yes. When an economizer is used in conjunction with the high humidity control option, high humidity control has priority.
+
+\paragraph{Field: Control High Indoor Humidity Based on Outdoor Humidity Ratio}\label{field-control-high-indoor-humidity-based-on-outdoor-humidity-ratio}
+
+This choice field determines if high humidity control is activated based on high indoor relative humidity alone or is activated only when the indoor relative humidity is above the humidstat setpoint \emph{and} the indoor humidity ratio is greater than the outdoor humidity ratio. Valid choices are \textbf{Yes} and \textbf{No}. If No is selected, high humidity control is active any time the zone humidistat senses a moisture load. If Yes is selected, the model also verifies that the outdoor humidity ratio is less than the humidistat s zone air humidity ratio. This field is used only when the input field High Humidity Control is specified as Yes. The default value is \textbf{Yes}.
+
+\paragraph{Field: Heat Recovery Bypass Control Type}\label{field-heat-recovery-bypass-control-type}
+
+This choice field determines if specialized control is used to optimize the use of heat recovery. Valid choices are \textbf{BypassWhenWithinEconomizerLimits} and \textbf{BypassWhenOAFlowGreaterThanMinimum}. If BypassWhenWithinEconomizerLimits is selected, heat recovery is disabled any time the controller determines that the economizer is active (i.e., all controls are within limits). If BypassWhenOAFlowGreaterThanMinimum is selected, the model first verifies that the economizer is active and then checks to see if the outdoor air flow rate is greater than the minimum. If it is greater than minimum, then heat recovery (if any) is set to bypass. When this option is used with Time of Day Economizer Control or High Humidity Control, this option has priority. The default value is \textbf{BypassWhenWithinEconomizerLimits}.
+
+An Example IDF specification:
+
+\begin{lstlisting}
+
+Controller:OutdoorAir,
+  OA Controller 1,                 !- Name
+  Relief Air Outlet Node,   !- Relief Air Outlet Node Name
+  Outdoor Air Mixer Inlet Node,   !- Return Air Node Name
+  Mixed Air Node,                   !- Mixed Air Node Name
+  Outdoor Air Inlet Node,   !- Actuator Node Name
+  0.25,                                       !- Minimum Outdoor Air Flow Rate {m3/s}
+  1.6,                                         !- Maximum Outdoor Air Flow Rate {m3/s}
+  ElectronicEnthalpy,           !- Economizer Control Type
+  ModulateFlow,                       !- Economizer Control Action Type
+  23.,                                 !- Economizer Maximum Limit Dry-Bulb Temperature {C}
+  ,                                       !- Economizer Maximum Limit Enthalpy {J/kg}
+  13.5,                               !- Economizer Maximum Limit Dewpoint Temperature {C}
+  ElectronicEnthalpyCurveA,!- Electronic Enthalpy Limit Curve Name
+  14.,                                 !- Economizer Minimum Limit Dry-Bulb Temperature {C}
+  NoLockout,                             !- Lockout Type
+  FixedMinimum,                       !- Minimum Limit Type
+  OAFractionSched,                 !- Minimum Outdoor Air Schedule Name
+  ,                                               !- Minimum Fraction of Outdoor Air Schedule Name
+  ,                                               !- Maximum Fraction of Outdoor Air Schedule Name
+  ,                                               !- Mechanical Ventilation Controller Name
+  TimeOfDayEconomizerSch,   !- Time of Day Economizer Control Schedule Name
+  Yes,                                         !- High Humidity Control
+  EAST ZONE,                             !- Humidistat Control Zone Name
+  0.9,                                         !- High Humidity Outdoor Air Flow Ratio
+  Yes;           !- Control High Indoor Humidity Based on Outdoor Humidity Ratio
+
+
+  Curve:Cubic,
+  ElectronicEnthalpyCurveA,!- Name
+  0.01342704,                           !- Coefficient1 Constant
+  -0.00047892,                         !- Coefficient2 x
+  0.000053352,                         !- Coefficient3 x**2
+  -0.0000018103,                     !- Coefficient4 x**3
+  16.6,                                       !- Minimum Value of x
+  29.13;                                     !- Maximum Value of x
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-005}
+
+Note that the key value for these outputs is the AirLoopHVAC name, not the name of the Controller:OutdoorAir.
+
+\begin{itemize}
+\item
+  HVAC,Average,Air System Outdoor Air Economizer Status {[]}
+\item
+  HVAC,Average,Air System Outdoor Air Heat Recovery Bypass Status {[]}
+\item
+  HVAC,Average,Air System Outdoor Air Heat Recovery Bypass Heating Coil Activity Status {[]}
+\item
+  HVAC,Average,Air System Outdoor Air Heat Recovery Bypass Minimum Outdoor Air Mixed Air Temperature {[}C{]}
+\item
+  HVAC,Average,Air System Outdoor Air High Humidity Control Status {[]}
+\item
+  HVAC,Average,Air System Outdoor Air Flow Fraction {[]}
+\item
+  HVAC,Average,Air System Outdoor Air Minimum Flow Fraction {[]}
+\item
+  HVAC,Average,Air System Outdoor Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Air System Mixed Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Air System Outdoor Air Maximum Flow Fraction {[]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Air System Outdoor Air Economizer Status {[]}}{Air System Outdoor Air Economizer Status }}\label{air-system-outdoor-air-economizer-status}
+
+Reports the average operating status of an air economizer over the reporting interval. The economizer status is set to 1 when the conditions are favorable for the economizer to operate (i.e., none of the control limits have been exceeded). While conditions may be favorable for economizer operation, it does not guarantee that the air-side economizer has increased outdoor air flow above the minimum level since the actual outdoor air flow rate is also governed by other controls (e.g., mixed air set point tempeature, time of day economizer control, maximum humidity setpoint, etc.). This variable is set to 0 if conditions disable economizer operation or NoEconomizer (Economizer Control Type) is specified.
+
+\paragraph{\texorpdfstring{Air System Outdoor Air Heat Recovery Bypass Status {[]}}{Air System Outdoor Air Heat Recovery Bypass Status }}\label{air-system-outdoor-air-heat-recovery-bypass-status}
+
+This indicates if the controls have determined if the bypass mode for heat recovery is in effect or not.
+
+\paragraph{\texorpdfstring{Air System Outdoor Air Heat Recovery Bypass Heating Coil Activity Status {[]}}{Air System Outdoor Air Heat Recovery Bypass Heating Coil Activity Status }}\label{air-system-outdoor-air-heat-recovery-bypass-heating-coil-activity-status}
+
+Reports the operating status of any heating coil in the air loop. If the heating coil is active, the heat exchanger will be activated (no air bypassed) and the heating energy will be reduced or eliminated. While conditions may be favorable for economizer operation, it does not guarantee that the air-side economizer has increased outdoor air flow above the minimum level since the actual outdoor air flow rate is also governed by other controls (e.g., mixed air set point temperature, time of day economizer control, maximum humidity setpoint, etc.). This variable is set to 0 if conditions disable economizer operation. This output variable is only available when using Heat Recovery Bypass Control Type = BypassWhenOAFlowGreaterThanMinimum.
+
+\paragraph{Air System Outdoor Air Heat Recovery Bypass Minimum Outdoor Air Mixed Air Temperature {[}C{]}}\label{air-system-outdoor-air-heat-recovery-bypass-minimum-outdoor-air-mixed-air-temperature-c}
+
+Reports the outdoor air mixer s mixed air node temperature at minimum outdoor air flow rate when the heat exchanger is disabled (off). This temperature is calculated as the return air temperature multiplied by the return air mass flow rate plus the mixer s inlet node temperature multipled by the minimum outdoor air flow rate. This quantity is then divided by the mixed air mass flow rate. If this temperature is less than the outdoor air mixer s mixed air node set point temperature, and the Heat Recovery Bypass Control Type = BypassWhenOAFlowGreaterThanMinimum, the outdoor air flow rate is set to the minimum. This output variable is only available when using Heat Recvoery Bypass Control Type = BypassWhenOAFlowGreaterThanMinimum.
+
+\paragraph{\texorpdfstring{Air System Outdoor Air High Humidity Control Status {[]}}{Air System Outdoor Air High Humidity Control Status }}\label{air-system-outdoor-air-high-humidity-control-status}
+
+Reports the average operating status of the controller s high humidity control over the reporting interval. The high humidity control status is set to 1 when the controller determines that a zone high humidity condition exists \emph{according to the settings specified in the controller}. This variable is set to 0 if conditions disable high humidity control operation or High Humidity Control is specified as No.
+
+\paragraph{\texorpdfstring{Air System Outdoor Air Flow Fraction {[]}}{Air System Outdoor Air Flow Fraction }}\label{air-system-outdoor-air-flow-fraction}
+
+Reports the average actual outdoor air fraction for the outdoor air controller over the reporting interval.
+
+\paragraph{\texorpdfstring{Air System Outdoor Air Minimum Flow Fraction {[]}}{Air System Outdoor Air Minimum Flow Fraction }}\label{air-system-outdoor-air-minimum-flow-fraction}
+
+Reports the average minimum limit of the outdoor air fraction for the outdoor air controller over the reporting interval.
+
+\paragraph{Air System Outdoor Air Mass Flow Rate {[}kg/s{]}}\label{air-system-outdoor-air-mass-flow-rate-kgs}
+
+Reports the average outdoor air mass flow rate introduced by the outdoor air controller over the reporting interval.
+
+\paragraph{Air System Mixed Air Mass Flow Rate {[}kg/s{]}}\label{air-system-mixed-air-mass-flow-rate-kgs}
+
+Reports the average mixed air mass flow rate of the HVAC air loop associated with this outdoor air controller over the reporting interval.
+
+\paragraph{\texorpdfstring{Air System Outdoor Air Maximum Flow Fraction {[]}}{Air System Outdoor Air Maximum Flow Fraction }}\label{air-system-outdoor-air-maximum-flow-fraction}
+
+Reports the average maximum limit of the outdoor air fraction for the outdoor air controller over the reporting interval. The maximum flow fraction is used to prevent DX cooling coils from freezing, specified by ASHRAE Stadard 90.1. This output variable is available when a corresponding SetpointManager:MixedAir object specifies optional inputs of Cooling Coil Inlet Node Name, Cooling coil Outlet Node Name, and Minimum Temperature at Cooling Coil Outlet Node.
+
+\subsection{Controller:MechanicalVentilation}\label{controllermechanicalventilation}
+
+This object is used in conjunction with an outdoor air controller (Ref. Controller:OutdoorAir, Field: Mechanical Ventilation Controller Name) to establish the minimum outdoor air flow rate provided by a mixed air box.
+
+Ventilation standards provide guidance on appropriate levels of outdoor ventilation air required for acceptable indoor air quality. The Ventilation Rate Procedure (VRP) of ASHRAE Standard 62.1-2007/2010 (\href{http://www.ashrae.org}{www.ashrae.org}) requires outdoor ventilation rates to be determined based on the floor area of each occupied zone plus the number of people in each zone and considers the zone air distribution effectiveness and system ventilation efficiency. The outdoor air ventilation rate can be reset dynamically as operating conditions change (e.g., variations in occupancy). The Controller:MechanicalVentilation object implements the VRP for calculating these outdoor air ventilation requirements and resetting them based on varying occupancy levels and zone diversification. This is particularly useful for large air distribution systems that serve a number of different zone types with varying occupancy levels. This object can also be used to model the Indoor Air Quality Procedure (IAQP) as defined in Standard 62.1
+
+The first five inputs for this object are the name, the availability schedule, the zone outdoor air method, the system outdoor air method, and the zone maximum outdoor air fraction. The next three input fields define the zone name (or zone list name), the design specification outdoor air object name, and the design specification zone air distribution object name to be applied to this zone (or zone list). The last three fields are extensible
+
+\subsubsection{Inputs}\label{inputs-2-007}
+
+\paragraph{Field: Name}\label{field-name-2-006}
+
+The unique user assigned name for an instance of mechanical ventilation. Any other object referencing this mechanical ventilation object will use this name.
+
+\paragraph{Field: AvailabilitySchedule Name}\label{field-availabilityschedule-name}
+
+The name of a schedule whose values are greater than 0 when mechanical ventilation, as calculated by this object, is desired. If the schedule s value is 0.0, then mechanical ventilation is not available and flow will not be requested. If the schedule s value is \textgreater{} 0.0 (usually 1 is used), mechanical ventilation is available. If this field is blank, the schedule has values of 1 for all time periods. This schedule is useful for purging the building of contaminants prior to occupancy (i.e., ventilation rate per unit floor area will be provided even if the occupancy is zero).
+
+\paragraph{Field: Demand Controlled Ventilation}\label{field-demand-controlled-ventilation}
+
+This field indicates whether the air loop is capable of doing demand controlled ventilation (DCV) to vary the amount of outdoor air based on actual number of occupants in spaces. Two choices: Yes and No. Default is No.
+
+\paragraph{Field: System Outdoor Air Method}\label{field-system-outdoor-air-method}
+
+The method used to calculate the system minimum outdoor air flow. Several choices are allowed: \textbf{ZoneSum}, \textbf{VentilationRateProcedure,} \textbf{IndoorAirQualityProcedure, ProportionalControlBasedonOccupancySchedule,} \textbf{ProportionalControlBasedonDesignOccupancy,} and \textbf{IndoorAirQualityProcedureGenericContaminant}. ZoneSum sums the outdoor air flows across all zones served by the system. VentilationRateProcedure (VRP) uses the multi-zone equations defined in 62.1-2007 to calculate the system outdoor air flow. VRP considers zone air distribution effectiveness and zone diversification of outdoor air fractions. IndoorAirQualityProcedure (IAQP) is the other procedure defined in ASHRAE Standard 62.1-2007 for calculate the amount of outdoor air necessary to maintain the levels of indoor air carbon dioxide at or below the setpoint defined in the ZoneControl:ContaminantController object. Appendix A of the ASHRAE 62.1-2010 user's manual discusses another method for implementing CO\(_{2}\)-based DCV in a single zone system. This method (Proportional Control) calculates the required outdoor air flow rate which varies in proportion to the percentage of the CO\(_{2}\) signal range and has two choices to calculate occupancy-based outdoor air rate. The ProportionalControlBasedonOccupancySchedule choice uses the real occupancy at the current time step to calculate outdoor air rate, while the ProportionalControlBasedonDesignOccupancy uses the design occupancy level to calculate outdoor air rate. The former choice is a good approach to estimate outdoor air rate. However, for practical applications, the zone controller usually does not have the real time occupancy information, and the design occupancy level is assumed. The latter choice is used in the design stage. The IndoorAirQualityProcedure-GenericContaminant method calculates the amount of outdoor air necessary to maintain the levels of indoor air generic contaminant at or below the setpoint defined in the ZoneControl:ContaminantController object.
+
+Note: When System Outdoor Air Method = IndoorAirQualityProcedure or IndoorAirQualityProcedureGenericContaminant is specified, only the Zone \textless{}x\textgreater{} Name fields are used. The other field inputs described below are not used.
+
+\paragraph{Field: Zone Maximum Outdoor Air Fraction}\label{field-zone-maximum-outdoor-air-fraction}
+
+This positive numeric input is the zone maximum outdoor air fraction. For VAV systems, when a zone requires outdoor air higher than the user specified Zone Maximum Outdoor Air Fraction, the zone supply air flow will be increased (if damper not fully open yet) to cap the outdoor air fraction at the maximum value. This allows the system level outdoor air flow to be reduced while the total supply air flow increases to meet zone outdoor air requirement. Valid values are from 0 to 1.0. Default is 1.0 which indicates zones can have 100\% outdoor air maintaining backward compatibility. This inputs work for single and dual duct VAV systems.
+
+\paragraph{Field Set (Zone Name, Design Specification Outdoor Air Object Name, and Design Specification Zone Air Distribution Object Name)}\label{field-set-zone-name-design-specification-outdoor-air-object-name-and-design-specification-zone-air-distribution-object-name}
+
+The following three fields are needed to define the parameters for the ventilation. This object is extensible by duplicating these three fields.
+
+\paragraph{Field:Zone \textless{}x\textgreater{} Name}\label{fieldzone-x-name}
+
+The zone name or zone list to apply the ventilation rates specified in the DesignSpecification:OutdoorAir object.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name \textless{}x\textgreater{}}\label{field-design-specification-outdoor-air-object-name-x}
+
+The name of the DesignSpecification:OutdoorAir object, defining the amount of outdoor air, that applies to the zone or zone list. If this field is blank, the corresponding DesignSpecification:OutdoorAir object for the zone will come from the DesignSpecification:OutdoorAir object referenced by the Sizing:Zone object for the same zone. If no such zone match is found, default values from the IDD will be used for the DesignSpecification:OutdoorAir object.
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name \textless{}x\textgreater{}}\label{field-design-specification-zone-air-distribution-object-name-x}
+
+The name of the DesignSpecification:ZoneAirDistribution object, defining the air distribution effectiveness and secondary recirculation air fraction, that applies to the zone or zone list. If this field is blank, the corresponding DesignSpecification:ZoneAirDistribution object for the zone will come from the DesignSpecification:ZoneAirDistribution object referenced by the Sizing:Zone object for the same zone. If no such zone match is found, default values from the IDD will be used for the DesignSpecification:ZoneAirDistribution object.
+
+As described previously, the Controller:MechanicalVentilation object works in conjunction with Controller:OutdoorAir. As such, the minimum quantity of outdoor air delivered via the mixed air box will be the greater of:
+
+\begin{itemize}
+\item
+  the minimum outdoor air flow rate calculated by the fields Minimum Outdoor Air Flow Rate, Minimum Limit and Minimum Outdoor Air Schedule Name in the associated Controller:OutdoorAir object, or
+\item
+  the outdoor air flow rate calculated by the VRP (details in the Engineering Reference) with inputs specified in this object and the referenced DesignSpecification:OutdoorAir and DesignSpecification:ZoneAirDistribution objects.
+\end{itemize}
+
+The actual outdoor air flow rate may be higher than the minimum if free cooling is available. Regardless, the outdoor air flow rate will not exceed the Maximum Outdoor Air Flow Rate specified in the associated Controller:OutdoorAir object.
+
+An example input for this object is shown below:
+
+\begin{lstlisting}
+
+Controller:MechanicalVentilation,
+  VentObject,                             !- Name
+  VentSchedule,                         !- Availability Schedule Name
+  VentilationRateProcedure, !- System Outdoor Air Method
+  1.0,                                           !- Zone Maximum Outdoor Air Fraction
+  Resistive Zone,                     !- Zone 1 Name
+  DSOA1,                                       !- Design Specification Outdoor Air Object Name 1
+  DSZADO1,                                   !- Design Specification Zone Air Distribution Object Name 1
+  DCV Zone List,                       !- Zone 2 Name
+  DSO_ZList,                               !- Design Specification Outdoor Air Object Name 2
+  ;                                                !- Design Specification Zone Air Distribution Object Name 2
+
+  ZoneList,
+  DCV Zone List,                       !- Zone List Name
+  East Zone,                               !- Zone Name 1
+  North Zone;                             !- Zone Name 2
+
+  DesignSpecification:OutdoorAir,
+  DSOA1,                                     !- Name
+  SUM,                                         !- Outdoor Air Method
+  0.00236,                                 !- Outdoor Air Flow per Person
+  0.000305,                               !- Outdoor Air Flow per Zone Floor Area
+  0.0,                                         !- Outdoor Air Flow per Zone
+  0.0,                                         !- Outdoor Air Flow Air Changes per Hour
+  ;                                               !- Outdoor Air Flow Rate Fraction Schedule Name
+
+  DesignSpecification:ZoneAirDistribution,
+  DSZADO1,                                 !- Name
+  1.2,                                         !- Zone Air Distribution Effectiveness in Cooling Mode
+  1.0,                                         !- Zone Air Distribution Effectiveness in Heating Mode
+  ,                                               !- Zone Air Distribution Effectiveness Schedule Name
+  0.3;                                         !- Zone Secondary Recirculation Fraction
+\end{lstlisting}
+
+\subsection{ZoneHVAC:EnergyRecoveryVentilator:Controller}\label{zonehvacenergyrecoveryventilatorcontroller}
+
+This controller object is used exclusively by the stand alone energy recovery ventilator (ZoneHVAC:EnergyRecoveryVentilator, see Figure~\ref{fig:schematic-of-the-zonehvac}). The purpose of this controller is to simulate economizer operation for the stand alone ERV and provide free cooling whenever possible or modify the outdoor air flow rate during high indoor humidity conditions. During economizer operation, if all of the limits are satisfied, the controller activates economizer mode (fully bypassing the fixed-plate air-to-air heat exchanger or stopping the rotation of a rotary heat exchanger). If any of the selected limits are exceeded, economizer operation is terminated. A time-of-day schedule may also be used to simulate a push-button type economizer controller.
+
+In addition, the outdoor air flow rate may be modified and heat exchange suspended in response to high indoor relative humidities. When the indoor relative humidity exceeds the zone humidistat s relative humidity set point, high humidity control is activated. When activated, if high humidity control is based on the outdoor air humidity ratio and the outdoor humidity ratio is greater than the indoor humidity ratio, high humidity control is terminated.
+
+\begin{figure}[hbtp] % fig 143
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image414.png}
+\caption{Schematic of the ZoneHVAC:EnergyRecoveryVentilator compound object \protect \label{fig:schematic-of-the-zonehvac}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-3-006}
+
+\paragraph{Field: Name}\label{field-name-3-006}
+
+A unique user-assigned name for the stand alone ERV controller. Any reference to this controller by another object will use this name.
+
+\paragraph{Field: Temperature High Limit}\label{field-temperature-high-limit}
+
+The input for this field is the outdoor air temperature high limit ( °C) for economizer operation. If the outdoor air temperature is above this limit, economizer (free cooling) operation is terminated. No input (blank) in this field means that there is no outdoor air temperature high limit control.
+
+\paragraph{Field: Temperature Low Limit}\label{field-temperature-low-limit}
+
+The input for this field is the outdoor air temperature low limit ( °C) for economizer operation. If the outdoor air temperature is below this limit, economizer (free cooling) operation is terminated. No input (blank) in this field means that there is no outdoor air temperature low limit control.
+
+\paragraph{Field: Enthalpy High Limit}\label{field-enthalpy-high-limit}
+
+The input for this field is the outdoor air enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, economizer (free cooling) operation is terminated. No input (blank) in this field means that there is no outdoor air economizer limit control.
+
+\paragraph{Field: Dewpoint Temperature Limit}\label{field-dewpoint-temperature-limit}
+
+Input for this field is the outdoor air dewpoint limit ( °C) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. No input (blank) in this field means that there is no outdoor air dewpoint limit control. This limit applies to the conditions at the Actuated Node regardless of whether or not there are any other components on the outdoor air path upstream of the mixer.
+
+\paragraph{Field: Electronic Enthalpy Limit Curve Name}\label{field-electronic-enthalpy-limit-curve-name-1}
+
+Input for this field is the name of a quadratic or cubic curve which provides the maximum outdoor air humidity ratio (function of outdoor air dry-bulb temperature) for economizer operation. If the outdoor air humidity ratio is greater than the curve s maximum humidity ratio (evaluated at the outdoor air dry-bulb temperature), the outdoor air flow rate will be set to the minimum. This limit applies to the conditions at the Actuated Node regardless of whether or not there are any other components on the outdoor air path upstream of the mixer. No input (blank) in this field means that there is no electronic enthalpy limit control.
+
+\paragraph{Field: Exhaust Air Temperature Limit}\label{field-exhaust-air-temperature-limit}
+
+This input establishes whether or not there is a limit control on the exhaust air temperature. The choices are \textbf{ExhaustAirTemperatureLimit} or \textbf{NoExhaustAirTemperatureLimit}. If \textbf{ExhaustAirTemperatureLimit} is chosen, the controller deactivates economizer mode whenever the outdoor air temperature is greater than the exhaust air temperature. If \textbf{NoExhaustAirTemperatureLimit} is chosen, no limit check on the exhaust air temperature is performed.
+
+\paragraph{Field: Exhaust Air Enthalpy Limit}\label{field-exhaust-air-enthalpy-limit}
+
+This input establishes whether or not there is a limit control on the exhaust air enthalpy. The choices are \textbf{ExhaustAirEnthalpyLimit} or \textbf{NoExhaustAirEnthalpyLimit}. If \textbf{ExhaustAirEnthalpyLimit} is chosen, the controller deactivates economizer mode whenever the outdoor air enthalpy is greater than the exhaust air enthalpy. If \textbf{NoExhaustAirEnthalpyLimit} is chosen, no limit check on the exhaust air enthalpy is performed.
+
+\paragraph{Field: Time of Day Economizer Flow Control Schedule Name}\label{field-time-of-day-economizer-flow-control-schedule-name}
+
+This alpha field is the name of a schedule which controls the change in air flow rate based on time-of-day. Schedule values equal to 0 disable this feature. Schedule values greater than 0 activate the economizer. Note that heat exchange between the air streams is suspended when the economizer is active. This schedule can be used with or without the high humidity control option. When an economizer is used in conjunction with the high humidity control option, high humidity control has priority.
+
+\paragraph{Field: High Humidity Control Flag}\label{field-high-humidity-control-flag}
+
+This optional choice field establishes whether or not the supply and exhaust air flow rates are modified in response to high indoor relative humidity. Valid choices are Yes and No. If Yes is selected, the supply and exhaust air flow rates may be modified when the indoor relative humidity is above the humidstat set point. If No is selected, this option is disabled and the following three fields are not used. Note that heat exchange between the air streams is suspended during times when high humidity control is active. The default value is No.
+
+\paragraph{Field: Humidistat Control Zone Name}\label{field-humidistat-control-zone-name-1}
+
+This optional input defines the zone name where the humidistat is located. This is the same zone name used in the Zone Control:Humidistat object. This field is required when the High Humidity Control Flag is specified as Yes.
+
+\paragraph{Field: High Humidity Outdoor Air Flow Ratio}\label{field-high-humidity-outdoor-air-flow-ratio-1}
+
+This optional input is the ratio of the modified supply (outdoor) air flow rate to the supply air flow rate specified in the Energy Recovery Ventilator:Stand Alone ERV object. When the high humidity control algorithm determines that the supply air flow rate will be changed (i.e.~increased or decreased), the operating supply air flow rate is equal to the supply air flow rate specified in the Energy Recovery Ventilator:Stand Alone ERV object multiplied by this ratio. The minimum value for this field is 0. This field is used to modify both the supply and exhasut air flow rates when high humidity control is active. The supply and exhasut air fan volumetric flow rates must be able to account for the increase in air flow when this input is greater than 1. The default value is 1.
+
+\paragraph{Field: Control High Indoor Humidity based on Outdoor Humidity Ratio}\label{field-control-high-indoor-humidity-based-on-outdoor-humidity-ratio-1}
+
+This optional choice field determines if high humidity control is activated based on high indoor relative humidity alone or is activated only when the indoor relative humidity is above the humidstat set point \emph{and} the outdoor humidity ratio is less than the indoor humidity ratio. Valid choices are Yes and No. If No is selected, high humidity control is active any time the zone humidistat senses a moisture load. If yes is selected, the model also verifies that the outdoor humidity ratio is less than the humidistat s zone air humidity ratio. This field is used only when the High Humidity Control Flag is specified as Yes. The default value is Yes.
+
+Following is an example input for this stand alone ERV controller object:
+
+\begin{lstlisting}
+
+ZoneHVAC:EnergyRecoveryVentilator:Controller,
+  ERV OA Controller 1,                       !- ERV controller name
+  19.,                                                       !- Temperature high limit {C}
+  14.,                                                       !- Temperature low limit {C}
+  ,                                                             !- Enthalpy high limit {J/kg}
+  15.55,                                                   !- dew point temperature limit (C)
+  ElectronicEnthalpyCurveA,             !- electronic enthalpy limit curve name
+  NoExhaustAirTemperatureLimit,     !- Exhaust air temperature limit
+  NoExhaustAirEnthalpyLimit,           !- Exhaust air enthalpy limit
+  OutsideAirFlowSchedule,                 !- Time of Day Economizer Flow Control Schedule Name
+  Yes,                                                       !- High Humidity Control Flag
+  East Zone,                                           !- Humidistat Control Zone Name
+  1.2,                                                       !- High Humidity Outdoor air Flow Ratio
+  Yes;                           !- Control High Indoor Humidity based on Outdoor Humidity Ratio
+
+
+  Curve:Cubic,
+  ElectronicEnthalpyCurveA, !- Name
+  0.01342704,                             !- Coefficient1 Constant
+  -0.00047892,                             !- Coefficient2 x
+  0.000053352,                           !- Coefficient3 x**2
+  -0.0000018103,                         !- Coefficient4 x**3
+  16.6,                                         !- Minimum Value of x
+  29.13;                                       !- Maximum Value of x
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-daylighting.tex b/doc/input-output-reference/src/overview/group-daylighting.tex
new file mode 100644
index 00000000000..e8d0b2b74a5
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-daylighting.tex
@@ -0,0 +1,1235 @@
+\section{Group -- Daylighting}\label{group-daylighting}
+
+Daylighting can be invoked in EnergyPlus by the use of two objects: \textbf{Daylighting:Controls} and \textbf{Daylighting:DELight:Controls}. These are described in the following object descriptions.
+
+\begin{callout}
+  Note that Daylighting:Controls and Daylighting:DELight:Controls objects may be intermixed in a single IDF but may not be used in the same zone.
+\end{callout}
+
+\subsection{Daylighting:Controls}\label{daylightingcontrols-000}
+
+In this method daylighting illuminance levels are calculated and then used to determine how much the electric lighting can be reduced. The daylight illuminance level in a zone depends on many factors, including sky condition; sun position; calculation point; location, size, and glass transmittance of windows; window shading devices; and reflectance of interior surfaces. Reduction of electric lighting depends on daylight illuminance level, illuminance set point, fraction of zone controlled and type of lighting control.
+
+\subsubsection{Inputs}\label{inputs-009}
+
+\paragraph{Field: Zone name}\label{field-zone-name-003}
+
+The name of the zone to which the following daylighting-related input applies.
+
+\paragraph{Field: Total Daylighting Reference Points}\label{field-total-daylighting-reference-points}
+
+Allowed values are 1 or 2. This the number of reference points in the zone at which horizontal daylighting illuminance will be calculated based on input for the following fields. It is assumed that the photocells that control the overhead electric lighting respond to the light levels at the specified reference points.
+
+\paragraph{Fields: (X,Y,Z) of First Reference Point}\label{fields-xyz-of-first-reference-point}
+
+Required if Total Daylighting Reference Points = 1 or 2. These three fields are the X, Y and Z values of the First Reference point in the coordinate system you specified for daylighting reference points in the GlobalGeometryRules object. Figure~\ref{fig:example-showing-location-of-daylighting} shows an example using the relative coordinate (to zone) system. Z is typically at desk height (0.8 m).
+
+If you want to divide a thermal zone into two independently-controlled lighting zones, then Total Daylighting Reference Points should be set to 2 and (X,Y,Z) of the Second Reference Point (see following input fields) should also be specified.
+
+\paragraph{Fields: (X,Y,Z) of Second Reference Point}\label{fields-xyz-of-second-reference-point}
+
+The X, Y, and Z coordinates, in the same coordinate system, of the second daylighting reference point. Required if Total Daylighting Reference Points = 2. See Figure~\ref{fig:example-showing-location-of-daylighting} for an example.
+
+\begin{figure}[hbtp] % fig 53
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image095.png}
+\caption{Example showing location of daylighting reference points in the zone coordinate system (relative) of a rectangular zone with three windows. (a) Perspective view, (b) plan view, (c) elevation view. All dimensions are in meters. \protect \label{fig:example-showing-location-of-daylighting}}
+\end{figure}
+
+\paragraph{Field: Fraction of Zone Controlled by First Reference Point}\label{field-fraction-of-zone-controlled-by-first-reference-point}
+
+The fraction of the zone's floor-area whose electric lighting is controlled by the daylight illuminance at the First Reference Point. If there is only one reference point then a fraction equal to
+
+\begin{equation}
+  1.0 - (\rm{Fraction of Zone Controlled by First Reference Point})
+\end{equation}
+
+is assumed to have no lighting control.
+
+\paragraph{Field: Fraction of Zone Controlled by Second Reference Point}\label{field-fraction-of-zone-controlled-by-second-reference-point}
+
+The fraction of the zone's floor-area whose electric lighting is controlled by the daylight illuminance at the Second Reference Point. Required if Total Daylighting Reference Points = 2. A fraction equal to
+
+\begin{equation}
+  1.0 - ([\rm{Fraction of Zone Controlled by First Reference Point}] + [\rm{Fraction of Zone Controlled by Second Reference Point}])
+\end{equation}
+
+is assumed to have no lighting control.
+
+\paragraph{Field: Illuminance SetPoint at First Reference Point}\label{field-illuminance-setpoint-at-first-reference-point}
+
+The desired lighting level (in lux) at the First Reference Point. This is the lighting level that would be produced at this reference point at night if the overhead electric lighting were operating at full input power. Recommended values depend on type of activity; they may be found, for example, in the Lighting Handbook of the Illuminating Engineering Society of North America. A typical value for general office work (excluding computer terminals) is 500 lux.
+
+\paragraph{Field: Illuminance SetPoint at Second Reference Point}\label{field-illuminance-setpoint-at-second-reference-point}
+
+The desired lighting level (in lux) at the Second Reference Point. Required if Total Daylighting Reference Points = 2. This is the lighting level that would be produced at this reference point at night if the overhead electric lighting were operating at full input power.
+
+\paragraph{Field: Lighting Control Type}\label{field-lighting-control-type}
+
+The type of overhead electric lighting control. All reference points specified are assumed to have this type of control.
+
+For Lighting Control Type = 1 (continuous), the overhead lights dim continuously and linearly from (maximum electric power, maximum light output) to (minimum electric power, minimum light output) as the daylight illuminance increases. The lights stay on at the minimum point with further increase in the daylight illuminance.
+
+For Lighting Control Type = 2 (stepped), the electric power input and light output vary in discrete, equally spaced steps. The number of steps is given by Number of Steps (Excluding Off) of Stepped Control. For example, if Number of Steps = 3 and Illuminance Setpoint = 600, then the following table shows the fraction of the lights that are on vs.~daylight illuminance.
+
+% table 18
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Example of a Stepped Lighting Control System with Three Steps \label{table:stepped-lighting-control-example}} \tabularnewline
+\toprule 
+Daylight illuminance & Fraction of lights that are on \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Example of a Stepped Lighting Control System with Three Steps} \tabularnewline
+\toprule 
+Daylight illuminance & Fraction of lights that are on \tabularnewline
+\midrule
+\endhead
+
+0-200 & 1.0 \tabularnewline
+200-400 & 2/3 \tabularnewline
+400-600 & 1/3 \tabularnewline
+600 and above & 0.0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Lighting Control Type = 3 (continuous/off) is the same as Lighting Control Type = 1 except that the lights switch off completely when the minimum dimming point is reached.
+
+\paragraph{Field: Glare Calculation Azimuth Angle of View Direction Clockwise from Zone y-Axis}\label{field-glare-calculation-azimuth-angle-of-view-direction-clockwise-from-zone-y-axis}
+
+Daylight glare from a window depends on occupant view direction. It is highest when you look directly at a window and decreases as you look away from a window. This field specifies the view direction for calculating glare. It is the angle, measured clockwise in the horizontal plane, between the zone y-axis and the occupant view direction.
+
+\paragraph{Field: Maximum Allowable Discomfort Glare Index}\label{field-maximum-allowable-discomfort-glare-index}
+
+If a daylit zone has windows with shading devices (except exterior screens), the shades will be deployed if the daylight glare at the First Reference Point exceeds the value of this field. To get this type of glare control you have to specify Trigger = Glare, GlareOrSolarOnWindow, GlareOrHorizontalSolar, GlareOrOutsideAirTemp, GlareOrZoneAirTemp or GlareOrZoneLoad in WindowProperty:ShadingControl for one or more windows in the zone (see WindowProperty:ShadingControl).
+
+If a zone has two or more windows with glare control, the shading devices will be deployed one by one in the order in which the windows are input until the glare level at each reference point falls below Maximum Allowable Discomfort Glare Index or is as close as possible to it.
+
+The following table gives recommended values of Maximum Allowable Discomfort Glare Index.
+
+% table 19
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Recommended Values of Maximum Allowable Discomfort Glare Index (DGI) \label{table:recommended-values-discomfort-glare-index}} \tabularnewline
+\toprule 
+Activity or Zone Type & Maximum Allowable DGI \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Recommended Values of Maximum Allowable Discomfort Glare Index (DGI)} \tabularnewline
+\toprule 
+Activity or Zone Type & Maximum Allowable DGI \tabularnewline
+\midrule
+\endhead
+
+Art Galleries & 16 \tabularnewline
+Factories: Rough work & 28 \tabularnewline
+Factories: Engine assembly & 26 \tabularnewline
+Factories: Fine assembly & 24 \tabularnewline
+Factories: Instrument assembly & 22 \tabularnewline
+Hospital wards & 18 \tabularnewline
+Laboratories & 22 \tabularnewline
+Museums & 20 \tabularnewline
+Offices & 22 \tabularnewline
+School classrooms & 20 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Field: Minimum Input Power Fraction for Continuous Dimming Control}\label{field-minimum-input-power-fraction-for-continuous-dimming-control}
+
+For Lighting Control Type = 1 (continuous), the lowest power the lighting system can dim down to, expressed as a fraction of maximum input power (see figure, below). For Lighting Control Type = 3 (continuous/off) this is the power fraction reached just before the lights switch off completely.
+
+\begin{figure}[hbtp] % fig 54
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image096.png}
+\caption{Illustration of continuous dimming relationship \protect \label{fig:illustration-of-continuous-dimming}}
+\end{figure}
+
+The figure above shows the relationship between electric light output and electrical input.
+
+\paragraph{Field: Minimum Light Output Fraction for Continuous Dimming Control}\label{field-minimum-light-output-fraction-for-continuous-dimming-control}
+
+For Lighting Control Type = 1 (continuous), the lowest lighting output the lighting system can dim down to, expressed as a fraction of maximum light output (see figure, above). This is the fractional light output that the system produces at minimum input power. For Lighting Control Type = 3 (continuous/off) this is the light output fraction reached just before the lights switch off completely.
+
+\paragraph{Field: Number of Stepped Control Steps}\label{field-number-of-stepped-control-steps}
+
+The number of steps, excluding off, in a stepped lighting control system (see figure, below). Required and must be \textgreater{}0 if Lighting Control Type = 2. The steps are assumed to be equally spaced.
+
+\begin{figure}[hbtp] % fig 55
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image097.png}
+\caption{Stepped lighting control with Number of Steps = 3. \protect \label{fig:stepped-lighting-control-with-number-of-steps}}
+\end{figure}
+
+\paragraph{Field: Probability Lighting will be Reset When Needed in Manual Stepped Control}\label{field-probability-lighting-will-be-reset-when-needed-in-manual-stepped-control}
+
+May be specified if a stepped lighting control system (Lighting Control Type = 2) is manually operated, such as in a simple, one-step (on-off) system. Gives the probability the occupants of a daylit zone will set the electric lights to the correct level to obtain the required illuminance. The rest of the time the lights are assumed to be set one step too high. For example, consider an on-off lighting system (Number of Steps = 1) with a set point of 600 lux and 0.7 reset probability. Then, when daylighting exceeds 600 lux, the electric lights will be off 70\% of the time and on 30\% of the time.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-002}
+
+This alpha field is optional and may be used to define the name of a schedule that denotes whether or not the control is available to operate during a given time period. If the schedule value is greater than zero, then the controls will be available to operate for that time period.~ If the schedule value is zero or less, then the controls will not be available. If this field is left blank, the controls will be always available. For example, this can be useful for scheduling the daylighting controls off during design days so that the daylighting controls do not affect lighting power during sizing.
+
+An IDF example:
+
+\begin{lstlisting}
+Daylighting:Controls, ! Zone Name
+  1,                  ! Total Daylighting Reference Points
+  3.048,3.048,0.9,    ! X,Y,Z coordinates of first reference point {m}
+  0.0,0.0,0.0,        ! X,Y,Z coordinates of second reference point, if present {m}
+  0.99,               ! Fraction of zone controlled by first reference point
+  0.0,                ! Fraction of zone controlled by second reference point, if present
+  500.,               ! Illuminance setpoint at first reference point {lux}
+  500.,               ! Illuminance setpoint at second reference point, if present {lux}
+  1,                  ! Lighting control type {1 = continuous,2 = stepped,3 = continuous/off}
+  180.0,              ! Azimuth angle of view direction for glare calculation {deg},
+                      !   measured clockwise from zone y-axis. Value of 180 gives view
+                      !   (from reference point) that is directly at window, maximizing glare.
+  20.0,               ! Maximum discomfort glare index for window shade control
+  0.3,                ! Minimum input power fraction for continuous dimming control
+  0.2,                ! Minimum light output fraction for continuous dimming control
+  0,                  ! Number of steps, excluding off, for stepped control
+  1.0;                ! Probability electric lighting will be reset when needed (used only
+                      !   for stepped control, to simulate manual on/off control)
+\end{lstlisting}
+
+\subsection{Guidelines for Daylighting Modeling (Detailed Method)}\label{guidelines-for-daylighting-modeling-detailed-method}
+
+Following are some guidelines for preparing EnergyPlus input to model the effects of daylighting. Before studying these guidelines, however, you should read the description of each input field under Daylighting:Controls, and review the IDF example, above, and the sample daylighting input, PurchAirWithDaylighting.idf.
+
+\subsubsection{Use of Window Multipliers}\label{use-of-window-multipliers}
+
+If an exterior wall in a daylit zone has a number of identical windows, the windows should be entered separately rather than using a window multiplier (ref: FenestrationSurface:Detailed). Using a multiplier would give an incorrect illuminance calculation since individual windows would not be positioned correctly on the wall.
+
+\subsubsection{Use of Zone Multipliers}\label{use-of-zone-multipliers}
+
+A zone multiplier should not be used on a daylit zone if the windows in the zone are shadowed by exterior obstructions like trees or neighboring buildings, or by obstructions caused by other parts of building. The reason for this is that the shadowing on the windows of the multiplied zone may be different from zone to zone depending on exactly how the shadows fall on the zones. However, a zone multiplier may be used on a daylit zone if the shadowing is by overhangs, fins and/or window setback.
+
+\subsubsection{Thermal Zoning for Daylighting}\label{thermal-zoning-for-daylighting}
+
+To correctly calculate both direct and inter-reflected daylight illuminance you should try to model a thermal zone consisting of several similar rooms separated by interior walls as a representative room with a zone multiplier (ref: Zone). An example of this is shown in Figure~\ref{fig:for-daylighting-purposes-the-thermal-zone}. Room-1 is the representative room, with a zone multiplier = 4.
+
+Interior walls IW-1, IW-2 and IW-3 should be treated as adiabatic, i.e., they should have Outside Boundary Condition = Surface and Outside Boundary Condition Object = IW-1, IW-2, or IW-3, respectively (ref: BuildingSurface:Detailed). Similarly, if the ceiling and floor of Room-1 are interior surfaces, they should be treated as adiabatic.
+
+\begin{figure}[hbtp] % fig 56
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image098.png}
+\caption{For daylighting purposes the thermal zone enclosed by the dashed boundary line should be modeled as a typical zone (Room-1) with a zone multiplier of 4. \protect \label{fig:for-daylighting-purposes-the-thermal-zone}}
+\end{figure}
+
+Sometimes a representative room cannot be found. Figure~\ref{fig:rooms-a-b-c-and-d-have-different-daylighting} shows a section of a building with four rooms having different daylighting characteristics because of different floor area, orientation and/or window size. In this case lumping the rooms into a single thermal zone would give nonsensical daylighting illuminance values because of the presence of the interior walls, which EnergyPlus ignores when calculating illuminance reaching a reference point directly from a window (i.e., without reflection). The solution in this case is to describe each room as a separate thermal zone with its own daylighting reference points, and input the interior walls because these will participate in the calculation of inter-reflected illuminance.
+
+\begin{figure}[hbtp] % fig 57
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image099.png}
+\caption{Rooms A, B, C and D have different daylighting characteristics. If lumped into a single thermal zone the daylighting calculation will be less accurate because the blockage of direct light by the interior walls between these rooms is modeled with some simplifications (see Interior Obstructions below). To get a good daylighting calculation each room should be input as a separate thermal zone. \protect \label{fig:rooms-a-b-c-and-d-have-different-daylighting}}
+\end{figure}
+
+\subsubsection{Multiple Lighting Zones}\label{multiple-lighting-zones}
+
+The detailed daylighting calculation allows a thermal zone to be divided into two independently-controlled lighting zones. (See the fields: Fraction of Zone Controlled by First Reference Point, Fraction of Zone Controlled by Second Reference Point, Illuminance SetPoint at First Reference Point, and Illuminance SetPoint at Second Reference Point.) An example is shown in Figure~\ref{fig:two-independently-controlled-lighting-zones}, where a relatively deep thermal zone has two lighting zones of equal area.
+
+\begin{figure}[hbtp] % fig 58
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image100.png}
+\caption{Two independently-controlled lighting zones, each with 50\% of the area of the thermal zone. \protect \label{fig:two-independently-controlled-lighting-zones}}
+\end{figure}
+
+\subsubsection{Fins, Overhangs and Other Exterior Obstructions}\label{fins-overhangs-and-other-exterior-obstructions}
+
+The daylighting calculation accounts for the presence of exterior obstructions in determining the amount of light that strikes the windows. For daylighting purposes exterior obstructions fall into three categories:
+
+\begin{itemize}
+  \item
+    Fins, overhangs, trees, neighboring buildings, etc., entered with the objects Shading:Zone:Detailed, Shading:Site:Detailed, or Shading:Building:Detailed.
+  \item
+    Building surfaces like walls and roofs (in an L-shaped building, for example).
+  \item
+    Surfaces associated with window setback.
+\end{itemize}
+
+Category (1) obstructions can have an associated solar transmittance schedule (see description of the field Transmittance Schedule Name for these shading surfaces). If this schedule is not specified, the surface is opaque (has zero transmittance).
+
+The daylighting calculation takes the transmittance into account in determining, for example, how much light enters a window through a translucent awning. It is assumed that the solar and visible transmittance is the same and that the surfaces are non-diffusing, i.e., they do not change the direction of transmitted light. Ref:Daylighting:Controls.
+
+Category (2) and (3) surfaces are assumed to be opaque.
+
+Surfaces in all three categories are assumed to be black, i.e., they do not reflect light, unless you set if ``Reflections'' option is chosen~ in the Building object. Then obstructions can reflect light, such as the top of an overhang reflecting light onto the window above. Ref: Building, Field: Solar Distribution (with reflections options).
+
+\subsubsection{Interior Obstructions}\label{interior-obstructions}
+
+The daylighting calculation accounts for the presence of interior obstructions that lie between a window and a reference point. Unlike exterior obstructions, which can be light transmitting, interior obstructions are assumed to be opaque. Interior obstructions can reduce or eliminate the light directly reaching the reference point through a window.
+
+However, interior obstructions that are walls, ceilings or floors are reflecting so they~ contribute to the inter-reflected component of daylight illuminance as do the non-obstructing zone surfaces.
+
+Interior obstructions can belong to the Shading object series. This type of obstruction is assumed to be non-reflecting so does not contribute to the inter-reflected component of daylight illuminance.
+
+An example of an interior obstruction that is a wall in an L-shaped room is shown in Figure~\ref{fig:wall-a-or-wall-b-is-an-interior-obstruction}. Here, wall A (or, equivalently, Wall B) prevents light from directly getting to the Reference Point from the window.
+
+\begin{figure}[hbtp] % fig 59
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image101.png}
+\caption{Wall A (or Wall B) is an interior obstruction that prevents light from directly reaching the daylighting reference point from the window. \protect \label{fig:wall-a-or-wall-b-is-an-interior-obstruction}}
+\end{figure}
+
+\subsubsection{Double Façades: Daylighting through Interior Windows}\label{double-fauxe7ades-daylighting-through-interior-windows}
+
+The Daylighting:Controls method, with no additional user input,~ calculates the contribution of daylight that passes into a target zone through interior windows.\protect\hyperlink{ux5fftn1}{{[}1{]}} The origin of this daylight is exterior windows in adjacent zones that share interior windows with the target zone. This capability is aimed at daylighting through a \textbf{double façade} (also called ``double envelope'' or ``double skin.'')
+
+This is illustrated in Figure~\ref{fig:vertical-section-through-a-double-faade}, which shows a double-façade buffer zone, Z0, with exterior windows EW1 and EW2. Z0 shares interior windows IW1, IW2 and IW3 with daylit occupied zones ZD1, ZD2 and ZD3, respectively (``daylit'' here means the zone has an associated Daylighting:Controls object). The daylight illuminance at reference points RP1, RP2 and RP3 comes from the interior windows and has two main sources:
+
+\begin{itemize}
+  \item
+    Daylight that passes through both an exterior window and an interior window in Z0 and reaches a reference point without reflection. This is called ``direct illuminance.''
+  \item
+    Daylight from Z0 that passes through an interior window and reaches a reference point by inter-reflection in the daylit zone. Because the program calculates this source from the interior solar distribution in Z0 it is recommended that the most accurate calculation of this distribution be made, which occurs if Solar Distribution = FullInteriorAndExterior in the Building object.
+\end{itemize}
+
+A third possible source is neglected because it is generally small in double-façade cases. This is daylight that is reflected from the surfaces of Z0, passes through an interior window and then reaches a reference point without inter-reflection in the daylit zone.
+
+PurchAirWithDoubleFacadeDaylighting.idf is an input example of daylighting through an interior window.
+
+\begin{figure}[hbtp] % fig 60
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image102.png}
+\caption{Vertical section through a double-façade building showing daylighting through interior windows. The dashed lines show that (1) reference point RP1 receives direct light from exterior window EW1 via interior window IW1; (2) RP2 receives direct light from EW1 and EW2 via IW2; and (3) RP3 receives direct light from EW2 via IW3. \protect \label{fig:vertical-section-through-a-double-faade}}
+\end{figure}
+
+\subsubsection{Interior Window Daylighting Configurations that EnergyPlus Can Calculate}\label{interior-window-daylighting-configurations-that-energyplus-can-calculate}
+
+Figure~\ref{fig:general-configuration-of-daylighting-through} shows schematically the general configuration of daylighting through interior windows that can be calculated with EnergyPlus. Here, daylit zone ZD has one or more interior windows that are adjacent to other zones, each of which has one or more exterior windows. ZD itself may or may not have exterior windows. If it does, than the daylight illuminance from its exterior and interior windows will be additive. The zones adjacent to ZD may or may not be daylit and may or may not have other interior windows that are not adjacent to ZD. (The program does not consider the illuminance in ZD from electric lighting in adjacent zones.)
+
+\begin{figure}[hbtp] % fig 61
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image103.png}
+\caption{General configuration of daylighting through interior windows that can be calculated with EnergyPlus. IW = interior window, EW = exterior window. \protect \label{fig:general-configuration-of-daylighting-through}}
+\end{figure}
+
+\subsubsection{Interior Window Daylighting Configurations that EnergyPlus Cannot Calculate}\label{interior-window-daylighting-configurations-that-energyplus-cannot-calculate}
+
+Figure~\ref{fig:configuration-in-which-daylighting-of-zone-z} shows schematically a configuration of daylighting through interior windows that cannot be calculated with EnergyPlus. Here, zone Z has an interior window that is adjacent to zone Z1 which in turn has an interior window adjacent to zone Z2. However, the daylight from the exterior window in Z2 that enters Z after passing through Z1 is not calculated because Z2 is not adjacent to Z.
+
+\begin{figure}[hbtp] % fig 62
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image104.png}
+\caption{Configuration in which daylighting of zone Z through its interior window  cannot be calculated with EnergyPlus. IW = interior window, EW = exterior window. \protect \label{fig:configuration-in-which-daylighting-of-zone-z}}
+\end{figure}
+
+\subsubsection{Restrictions on Shading Devices}\label{restrictions-on-shading-devices}
+
+There are two restrictions on the use of exterior-window shading devices when a daylit zone has interior windows:
+
+1)~~~If two daylit zones share an interior window, neither zone can have an exterior window whose shading device does glare control (i.e., the WindowProperty:ShadingControl for the exterior window has Glare Control Is Active = Yes).
+
+2)~~~If two daylit zones share an interior window, neither zone can have an exterior window with a WindowProperty:ShadingControl that has Shading Control Type = MeetDaylightIlluminanceSetpoint.
+
+\subsection{DElight Daylighting Method}\label{delight-daylighting-method}
+
+The DElight method of analyzing daylighting in buildings is very similar to that used in the Detailed method. For each point in time, DElight calculates the interior daylighting illuminance at specified reference points and then determines how much the electric lighting can be reduced while still achieving a combined daylighting and electric lighting illuminance target. The daylight illuminance level in a zone depends on many factors, including exterior light sources; location, size, and visible light transmittance of simple and complex fenestration systems; reflectance of interior surfaces; and location of calculation reference points. The subsequent reduction of electric lighting depends on daylight illuminance level, illuminance set point, fraction of zone controlled, and type of lighting control.
+
+There are two primary differences between the Detailed and DElight methods of calculating interior illuminance levels. The first is that DElight includes the capability of analyzing complex fenestration systems that include geometrically complicated shading systems (e.g., roof monitors) and/or optically complicated glazings (e.g., prismatic or holographic glass). The second key difference is that DElight uses a radiosity method to calculate the effects of light reflection inside a zone. These methods are discussed in more detail in the engineering documentation.
+
+There are other important differences between the two methods. One is the inability of DElight to perform the type of dynamic shading controls possible using the Detailed method at each point in time during the thermal simulation (e.g., changes in electrochromic glazing transmittances and blind slat angles). Another is the DElight ability to include more than two reference points in its interior illuminance and electric lighting reduction calculations. A third is the current lack of visual quality (e.g., glare) calculations performed by DElight. Fourth, the modeling of interior obstructions is different in the two methods. In the DElight method interior obstructions block interreflections but do not block the intial direct illuminance. In the Detailed method, interior obstructions block the initial direct illuminance but do not block interreflections. See the engineering documentation for more details. Fifth, when using DElight daylighting the presence of exterior shading surfaces such as overhangs is ignored.
+
+Input for invoking the DElight method involves three object types: \textbf{Daylighting:DELight:Controls}, \textbf{Daylighting:DELight:ReferencePoint}, and \textbf{Daylighting:DELight:ComplexFenestration}. Each of these objects is described below.
+
+\subsection{Daylighting:DELight:Controls}\label{daylightingdelightcontrols}
+
+The first input object required for invoking the DElight method is the Daylighting:DELight:Controls object, which defines the parameters of each daylighting zone within a building. This object must be associated with a specific thermal zone within the building for which the reduction in electric lighting due to daylight illuminance will be accounted.
+
+\subsubsection{Inputs}\label{inputs-1-008}
+
+\paragraph{Field: Name}\label{field-name-008}
+
+User name of the DElight daylighting zone to which the following input applies.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-002}
+
+The name of the thermal Zone hosting this DElight daylighting zone. This must be a valid name that has been associated with a thermal Zone contained in the same EnergyPlus input data file.
+
+\paragraph{Field: Lighting Control Type}\label{field-lighting-control-type-1}
+
+The type of overhead electric lighting control. All reference points specified are assumed to have this type of control.
+
+For Lighting Control Type = 1 (continuous), the overhead lights dim continuously and linearly from (maximum electric power, maximum light output) to (minimum electric power, minimum light output) as the daylight illuminance increases. The lights stay on at the minimum point with further increase in the daylight illuminance.
+
+For Lighting Control Type = 2 (stepped), the electric power input and light output vary in discrete, equally spaced steps. The number of steps is given by Number of Steps (Excluding Off) of Stepped Control. For example, if Number of Steps = 3 and Illuminance Setpoint = 600, then the following table shows the fraction of the lights that are on vs.~daylight illuminance.
+
+% table 20
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Example of a Stepped Lighting Control System with Three Steps \label{table:stepped-lighting-control-example-001}} \tabularnewline
+\toprule 
+Daylight illuminance & Fraction of lights that are on \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Example of a Stepped Lighting Control System with Three Steps} \tabularnewline
+\toprule 
+Daylight illuminance & Fraction of lights that are on \tabularnewline
+\midrule
+\endhead
+
+0-200 & 1.0 \tabularnewline
+200-400 & 2/3 \tabularnewline
+400-600 & 1/3 \tabularnewline
+600 and above & 0.0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Lighting Control Type = 3 (continuous/off) is the same as Lighting Control Type = 1 except that the lights switch off completely when the minimum dimming point is reached.
+
+\paragraph{Field: Minimum Input Power Fraction for Continuous Dimming Control}\label{field-minimum-input-power-fraction-for-continuous-dimming-control-1}
+
+For Lighting Control Type = 1 (continuous), the lowest power the lighting system can dim down to, expressed as a fraction of maximum input power (see figure, below). For Lighting Control Type = 3 (continuous/off) this is the power fraction reached just before the lights switch off completely.
+
+\begin{figure}[hbtp] % fig 63
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image105.png}
+\caption{Illustration of continuous dimming relationship \protect \label{fig:illustration-of-continuous-dimming-001}}
+\end{figure}
+
+The figure above shows the relationship between electric light output and electrical input.
+
+\paragraph{Field: Minimum Light Output Fraction for Continuous Dimming Control}\label{field-minimum-light-output-fraction-for-continuous-dimming-control-1}
+
+For Lighting Control Type = 1 (continuous), the lowest lighting output the lighting system can dim down to, expressed as a fraction of maximum light output (see figure, above). This is the fractional light output that the system produces at minimum input power. For Lighting Control Type = 3 (continuous/off) this is the power fraction reached just before the lights switch off completely.
+
+\paragraph{Field: Number of Steps (Excluding Off) for Stepped Control}\label{field-number-of-steps-excluding-off-for-stepped-control}
+
+The number of steps, excluding off, in a stepped lighting control system (see figure, below). Required and must be \textgreater{}0 if Lighting Control Type = 2. The steps are assumed to be equally spaced.
+
+\begin{figure}[hbtp] % fig 64
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image106.png}
+\caption{Stepped lighting control with Number of Steps = 3. \protect \label{fig:stepped-lighting-control-with-number-of-steps-001}}
+\end{figure}
+
+\paragraph{Field: Probability Lighting Will Be Reset When Needed in Manual Stepped Control}\label{field-probability-lighting-will-be-reset-when-needed-in-manual-stepped-control-1}
+
+May be specified if a stepped lighting control system (Lighting Control Type = 2) is manually operated, such as in a simple, one-step (on-off) system. Gives the probability the occupants of a daylit zone will set the electric lights to the correct level to obtain the required illuminance. The rest of the time the lights are assumed to be set one step too high. For example, consider an on-off lighting system (Number of Steps = 1) with a set point of 600 lux and 0.7 reset probability. Then, when daylighting exceeds 600 lux, the electric lights will be off 70\% of the time and on 30\% of the time.
+
+\paragraph{Field: Gridding Resolution}\label{field-gridding-resolution}
+
+The maximum surface area for nodes in gridding (subdividing) all surfaces in the DElight zone. All reflective and transmitting surfaces will be subdivided into approximately square nodes that do not exceed this maximum. Higher resolution subdivisions require greater calculation times, but generally produce more accurate results. This same gridding resolution is also used to subdivide any Complex Fenestration System surfaces. It is advisable to perform at least one simulation of new input using a small gridding resolution such as 0.1m2 to compare these results against simulation runs at lower resolution (i.e., higher maximum area nodal grids) to get a sense of possible levels of error.
+
+An IDF example:
+
+\begin{lstlisting}
+Daylighting:DELight:Controls,
+  DElight NORTH ZONE, !- DElight Zone Name
+  NORTH ZONE,         !- Zone Name
+  1,     !- Lighting control type
+  0.3,   !- Minimum input power fraction for continuous dimming control
+  0.2,   !- Minimum light output fraction for continuous dimming control
+  0,     !- Number of steps (excluding off) for stepped control
+  1.0,   !- Probability lighting will be reset when needed in manual stepped control
+  1.0;   !- Gridding Resolution {m2}
+\end{lstlisting}
+
+\subsection{Daylighting:DELight:ReferencePoint}\label{daylightingdelightreferencepoint}
+
+The second input object required for invoking the DElight method is the Daylighting:DELight:ReferencePoint object, which defines the parameters of each Reference Point within the associated DElight daylighting zone. This object must be associated with a specific Daylighting:DELight:Controls object instance. There may be up to a maximum of 100 Reference Points for each DElight daylighting zone. Each Reference Point that is input does NOT need to be included in the control of the electric lighting system within the zone. This is determined by the fraction of the zone controlled by each Reference Point, which can be input as 0. Note that the sum of all Reference Point control fractions must equal 1 to obtain correct overall results.
+
+\subsubsection{Inputs}\label{inputs-2-008}
+
+\paragraph{Field: Name}\label{field-name-1-007}
+
+User name of the DElight daylighting Reference Point to which the following input applies.
+
+\paragraph{Field: DElight Name}\label{field-delight-name}
+
+The name of the Daylighting:DELight:Controls object instance hosting this Reference Point. This must be a valid name that has been associated with a DElight daylighting Zone contained in the same EnergyPlus input data file.
+
+\paragraph{Fields: (X,Y,Z) of Reference Point}\label{fields-xyz-of-reference-point}
+
+These three fields are the X, Y and Z values of the Reference point in the coordinate system you specified for daylighting reference points in the GlobalGeometryRules object. Figure~\ref{fig:example-showing-location-of-two-daylighting} shows an example using the relative coordinate (to zone) system. Z is typically at work surface height (e.g., 0.8m for a desk).
+
+\begin{figure}[hbtp] % fig 65
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image107.png}
+\caption{Example showing location of two daylighting reference points in the zone coordinate system (relative) of a rectangular zone with three windows. (a) Perspective view, (b) plan view, (c) elevation view. All dimensions are in meters. \protect \label{fig:example-showing-location-of-two-daylighting}}
+\end{figure}
+
+\paragraph{Field: Fraction of Zone Controlled by Reference Point}\label{field-fraction-of-zone-controlled-by-reference-point}
+
+The zone floor-area fraction of the electric lighting that is controlled by the daylight illuminance at this Reference Point. If the sum of the values for this field for all Reference Points input for a given daylighting zone is less than 1.0, then the remaining fraction (i.e., 1.0 -- Sum) is assumed to not have lighting control.
+
+Note that Reference Points may be input with a 0.0 value for this fraction. In this case, daylight factors and interior illuminance values will be calculated for the Reference Point, but it will play no role in controlling the electric lighting within the daylighting zone to which it belongs.
+
+\paragraph{Field: Illuminance Setpoint at Reference Point}\label{field-illuminance-setpoint-at-reference-point}
+
+The desired lighting level (in lux) at this Reference Point. This is assumed to be the lighting level that would be produced at this reference point at night if the overhead electric lighting were operating at full input power. Recommended values depend on the type of activity and may be found, for example, in the Lighting Handbook of the Illuminating Engineering Society of North America. A typical value for general office work (excluding computer terminals) is 500 lux.
+
+An IDF example:
+
+\begin{lstlisting}
+Daylighting:DELight:ReferencePoint,
+  RefPt 2,              !- Reference Point Name
+  DElight NORTH ZONE,   !- DElight Zone Name
+  5.0,                  !- X-coordinate of reference point {m}
+  3.0,                  !- Y-coordinate of reference point {m}
+  0.9,                  !- Z-coordinate of reference point {m}
+  0.5,                  !- Fraction of zone controlled by reference point
+  500.;                 !- Illuminance setpoint at reference point {lux}
+\end{lstlisting}
+
+\subsection{Daylighting:DELight:ComplexFenestration}\label{daylightingdelightcomplexfenestration}
+
+The third input object related to the DElight method is the Daylighting:DElight: Complex Fenestration object. The DElight daylighting analysis method can be applied to daylighting zones that contain only simple fenestration systems such as windows and skylights that are standard EnergyPlus sub-surfaces. In this situation, no Daylighting:DElight: Complex Fenestration object would be input.
+
+In addition to analyzing simple fenestration systems, DElight includes the capability of analyzing complex fenestration systems such as geometrically complicated static shading systems (e.g., roof monitors) and/or optically complicated glazings (e.g., prismatic or holographic glass). This capability is based on characterizing these complex fenestration systems (CFS) using bi-directional transmittance distribution functions (BTDF). In general, BTDF data for a specific CFS must be either measured or simulated (e.g., using ray-tracing techniques) prior to employing DElight to analyze it within EnergyPlus. The current implementation of DElight CFS calculations within EnergyPlus supports two approaches to the input of BTDF, an analytical approach and a file-based approach. The details of inputting these two approaches are described below under the User Complex Fenestration Type field.
+
+Two analytical CFS BTDF types are currently supported, window and light shelf. The file-based approach requires that a user has access to a data file containing raw BTDF data that DElight reads as additional input during its analysis calculations. BTDF data files are described separately since it is anticipated that individual EnergyPlus users will not create these data files themselves.
+
+The methods related to characterizing and analyzing CFS using BTDF are still evolving. DElight is an early implementation of CFS analysis methods. These methods, and the input associated with them here, will likely change in the future.
+
+\subsubsection{Inputs}\label{inputs-3-007}
+
+\paragraph{Field: User Name}\label{field-user-name}
+
+User name of the DElight daylighting Complex Fenestration to which the following input applies.
+
+\paragraph{Field: Complex Fenestration Type}\label{field-complex-fenestration-type}
+
+Type name of the DElight daylighting Complex Fenestration system to be analyzed. This type name must take one of the following two forms.
+
+BTDF\textsuperscript{GEN}Analytical Type\^{}Normal Visible Transmittance\^{}Dispersion Angle
+
+BTDF\textsuperscript{FILE}Filename
+
+The first form above is for supported analytical CFS types which currently include WINDOW and LIGHTSHELF. While these analytical types are relatively simple, they represent flexible ways to explore diffusing CFS systems and the impact of light shelves in redirecting light through an aperture. Each of these types also requires the visible transmittance of the CFS at normal incidence angle, and a dispersion angle (in degrees) that represents the ``spread'' of transmitted light. A small dispersion angle of 10 corresponds to clear glazing while a large angle of 90 corresponds to perfectly diffusing glazing. The ``\^{}'' symbol must be used as a delimiter between sub-fields within this Complex Fenestration type name string as shown in the IDF example for WINDOW below, and in the DElight sample input data files.
+
+The second form above is for CFS types for which there is pre-measured or pre-simulated BTDF data. In this case the Filename sub-field must be a valid data file name that is associated with an existing BTDF dataset that DElight can use in its calculations.
+
+\paragraph{Field: Building Surface Name}\label{field-building-surface-name}
+
+The name of the heat transfer surface object instance hosting this Complex Fenestration, analogous to the Building Surface Name field for subsurfaces such as Windows. This must be a valid name that has been associated with a heat transfer surface contained in the same EnergyPlus input data file.
+
+\paragraph{Field: Window Name}\label{field-window-name}
+
+The name of the Window (ref: FenestrationSurface:Detailed object) instance that will be used to account for the geometry, and the solar/thermal gains/losses, of the Complex Fenestration system surface. This must be a valid name that has been associated with a Window contained in the same EnergyPlus input data file. The geometry for the Complex Fenestration is taken from the geometry input for this standard EnergyPlus subsurface, hence the term ``Doppelganger.''
+
+Note that DElight only deals with the visible spectrum of light transmitted through a Complex Fenestration. To account for the solar/thermal influences of a Complex Fenestration, a geometrically coincident subsurface that will be accounted for by methods already within EnergyPlus must be defined in the input data file. This is an interim solution to the issue of accounting for solar/thermal influences that will likely change as techniques analogous to the daylighting analysis of BTDF are developed.
+
+\paragraph{Field: Fenestration Rotation}\label{field-fenestration-rotation}
+
+The in-plane counter-clockwise rotation angle between the Complex Fenestration optical reference direction and the base edge of the Doppelganger Surface geometry. The Complex Fenestration optical reference direction is the direction of the zero azimuth angle for the BDTF dataset. This Rotation angle will typically be zero when the Doppelganger surface is rectangular and its width edge is aligned with the Complex Fenestration optical reference direction.
+
+An IDF example for an analytical WINDOW type CFS:
+
+\begin{lstlisting}
+
+Daylighting:DELight:ComplexFenestration,
+      Window CFS,       !- DElight Complex Fenestration User Name
+      BTDF^GEN^WINDOW^1.0^20.0,     !- Complex Fenestration Type
+      ZN003:WALL001,  !- Complex Fenestration Host Surface
+      Zn003:Wall001:Doppel001, !- Doppelganger Surface Name
+      0.0;            !- Fenestration Rotation {deg}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-006}
+
+In addition to the daylighting-specific outputs for DElight listed below, two ASCII text files are created during an EnergyPlus run that includes DElight analysis.~ Following completion of an EnergyPlus run, these files are given names that consist of the project name appended with DElight.in and DElight.out.~ The format of these files is described in the Output Details and Examples document.
+
+Zone,Average,Daylighting Reference Point Illuminance {[}lux{]}
+
+Zone,Average,Daylighting Lighting Power Multiplier {[]}
+
+\paragraph{Daylighting Reference Point Illuminance {[}lux{]}}\label{daylighting-reference-point-illuminance-lux}
+
+The total daylight illuminance at a DElight reference point from all of the exterior windows in a daylit zone.
+
+\paragraph{\texorpdfstring{Daylighting Lighting Power Multiplier {[]}}{Daylighting Lighting Power Multiplier }}\label{daylighting-lighting-power-multiplier}
+
+The amount by which the overhead electric lighting power in a zone is multiplied due to usage of DElight calculated daylighting to dim or switch electric lights. For example, if the multiplier is M and the electric power without dimming is P, then the electric power with dimming is M*P. The multiplier varies from 0.0, which corresponds to maximum dimming (zero electric lighting), to 1.0, which corresponds to no dimming.
+
+\subsubsection{Outputs}\label{outputs-1-004}
+
+The following daylighting-specific outputs are available for Daylighting:Controls:
+
+\begin{itemize}
+\item
+  Zone,Average,Site Exterior Beam Normal Illuminance {[}lux{]}
+\item
+  Zone,Average,Site Exterior Horizontal Beam Illuminance {[}lux{]}
+\item
+  Zone,Average,Site Exterior Horizontal Sky Illuminance {[}lux{]}
+\item
+  Zone,Average,Site Beam Solar Radiation Luminous Efficacy {[}lum/W{]}
+\item
+  Zone,Average,Site Sky Diffuse Solar Radiation Luminous Efficacy {[}lum/W{]}
+\item
+  Zone,Average,Site Daylighting Model Sky Clearness {[]}
+\item
+  Zone,Average,Site Daylighting Model Sky Brightness {[]}
+\item
+  Surface,Average,Daylighting Window Reference Point 1 View Luminance {[}cd/m2{]}
+\item
+  Surface,Average,Daylighting Window Reference Point 1 Illuminance {[}lux{]}
+\item
+  Zone,Average,Daylighting Reference Point 1 Illuminance {[}lux{]}
+\item
+  Zone,Average,Daylighting Reference Point 1 Glare Index {[]}
+\item
+  Zone,Sum,Daylighting Reference Point 1 Glare Index Setpoint Exceeded Time {[}hr{]}
+\item
+  Zone,Sum,Daylighting Reference Point 1 Daylight Illuminance Setpoint Exceeded Time {[}hr{]}
+\item
+  Surface,Average,Daylighting Window Reference Point 2 View Luminance {[}cd/m2{]}
+\item
+  Surface,Average,Daylighting Window Reference Point 2 Illuminance {[}lux{]}
+\item
+  Zone,Average,Daylighting Reference Point 2 Illuminance {[}lux{]}, if applicable
+\item
+  Zone,Average,Daylighting Reference Point 2 Glare Index {[]}, if applicable
+\item
+  Zone,Sum,Daylighting Reference Point 2 Glare Index Setpoint Exceeded Time {[}hr{]}
+\item
+  Zone,Sum,Daylighting Reference Point 2 Daylight Illuminance Setpoint Exceeded Time {[}hr{]}
+\item
+  Zone,Average,Daylighting Lighting Power Multiplier {[]}
+\end{itemize}
+
+\paragraph{Site Exterior Beam Normal Illuminance {[}lux{]}}\label{site-exterior-beam-normal-illuminance-lux}
+
+Beam normal illuminance of the sun at the earth's surface, measured in lux (lumens/m\(^{2}\))
+
+\paragraph{Site Exterior Horizontal Beam Illuminance {[}lux{]}}\label{site-exterior-horizontal-beam-illuminance-lux}
+
+Beam illuminance on an unobstructed horizontal plane at the earth's surface. Equals ``Site Exterior Beam Normal Illuminance'' times sine of solar altitude.
+
+\paragraph{Site Exterior Horizontal Sky Illuminance {[}lux{]}}\label{site-exterior-horizontal-sky-illuminance-lux}
+
+Illuminance from sky solar radiation on an unobstructed horizontal plane at the earth's surface. The total exterior horizontal illuminance is the sum of ``Site Exterior Horizontal Beam Illuminance'' and ``Site Exterior Horizontal Sky Illuminance.''
+
+\paragraph{Site Beam Solar Radiation Luminous Efficacy {[}lum/W{]}}\label{site-beam-solar-radiation-luminous-efficacy-lumw}
+
+A measure of the visible light content of beam solar radiation; equal to the number of lumens per watt of beam solar radiation. Depends on atmospheric conditions (moisture, turbidity, cloudiness) and solar altitude.
+
+\paragraph{Site Sky Diffuse Solar Radiation Luminous Efficacy {[}lum/W{]}}\label{site-sky-diffuse-solar-radiation-luminous-efficacy-lumw}
+
+A measure of the visible light content of sky diffuse solar radiation; equal to the number of lumens per watt of sky diffuse solar radiation. Depends on atmospheric conditions (moisture, turbidity, cloudiness) and solar altitude.
+
+\paragraph{\texorpdfstring{Site Daylighting Model Sky Clearness {[]}}{Site Daylighting Model Sky Clearness }}\label{site-daylighting-model-sky-clearness}
+
+Clearness of sky. One of the factors used to determine sky type and luminous efficacy of solar radiation (see \emph{EnergyPlus Engineering Document}). Sky Clearness close to 1.0 corresponds to an overcast sky. Sky Clearness \textgreater{} 6 is a clear sky.
+
+\paragraph{\texorpdfstring{Site Daylighting Model Sky Brightness {[]}}{Site Daylighting Model Sky Brightness }}\label{site-daylighting-model-sky-brightness}
+
+Brightness of sky. One of the factors used to determine sky type and luminous efficacy of solar radiation (see \emph{EnergyPlus Engineering Document}).
+
+\paragraph{Daylighting Window Reference Point 1 View Luminance {[}cd/m2{]}}\label{daylighting-window-reference-point-1-view-luminance-cdm2}
+
+The area-averaged luminance of an exterior window as viewed from the first reference point in the daylit zone containing the window. In general, higher window luminance values are associated with higher daylight glare values. (Printed only for exterior windows in daylit zones without interior windows.)
+
+\paragraph{Daylighting Window Reference Point 1 Illuminance {[}lux{]}}\label{daylighting-window-reference-point-1-illuminance-lux}
+
+The contribution from a particular exterior window to the daylight illuminance at the first reference point in the daylit zone containing the window. (Not printed for exterior windows in daylit zones with interior windows.)
+
+\paragraph{Daylighting Reference Point 1 Illuminance {[}lux{]}}\label{daylighting-reference-point-1-illuminance-lux}
+
+The total daylight illuminance at the first reference point from all of the windows in a daylit zone.
+
+\paragraph{\texorpdfstring{Daylighting Reference Point 1 Glare Index {[]}}{Daylighting Reference Point 1 Glare Index }}\label{daylighting-reference-point-1-glare-index}
+
+The daylight glare index at the first reference point in a daylit zone.
+
+\paragraph{Daylighting Reference Point 1 Glare Index Setpoint Exceeded Time {[}hr{]}}\label{daylighting-reference-point-1-glare-index-setpoint-exceeded-time-hr}
+
+The number of hours when the calculated daylight glare index at the first reference point exceeds the glare index setpoint.
+
+\paragraph{Daylighting Reference Point 1 Daylight Illuminance Setpoint Exceeded Time {[}hr{]}}\label{daylighting-reference-point-1-daylight-illuminance-setpoint-exceeded-time-hr}
+
+The number of hours when the calculated daylight illuminance at the first reference point exceeds the daylight illuminance setpoint.
+
+\paragraph{Daylighting Reference Point 2 Illuminance {[}lux{]}}\label{daylighting-reference-point-2-illuminance-lux}
+
+The total daylight illuminance at the second reference point from all of the windows in a daylit zone.
+
+\paragraph{Daylighting Window Reference Point 2 View Luminance {[}cd/m2{]}}\label{daylighting-window-reference-point-2-view-luminance-cdm2}
+
+The area-averaged luminance of an exterior window as viewed from the second reference point, if present, in the daylit zone containing the window. Note that, for a bare window, this value can be different from the corresponding value at the first reference point since different regions of the sky and ground will be visible from the two reference points, and different ranges of angles of incidence and associated glass transmittance values will be involved. (Not printed for exterior windows in daylit zones with interior windows.)
+
+\paragraph{Daylighting Window Reference Point 2 Illuminance {[}lux{]}}\label{daylighting-window-reference-point-2-illuminance-lux}
+
+The contribution from a particular exterior window to the daylight illuminance at the second reference point, if present, in the daylit zone containing the window. (Not printed for exterior windows in daylit zones with interior windows.)
+
+\paragraph{\texorpdfstring{Daylighting Reference Point 2 Glare Index {[]}}{Daylighting Reference Point 2 Glare Index }}\label{daylighting-reference-point-2-glare-index}
+
+The daylight glare index at the second reference point, if present, in a daylit zone.
+
+\paragraph{Daylighting Reference Point 2 Glare Index Setpoint Exceeded Time {[}hr{]}}\label{daylighting-reference-point-2-glare-index-setpoint-exceeded-time-hr}
+
+The number of hours when the calculated daylight glare index at the second reference point exceeds the glare index setpoint.
+
+\paragraph{Daylighting Reference Point 2 Daylight Illuminance Setpoint Exceeded Time {[}hr{]}}\label{daylighting-reference-point-2-daylight-illuminance-setpoint-exceeded-time-hr}
+
+The number of hours when the calculated daylight illuminance at the second reference point exceeds the daylight illuminance setpoint.
+
+\paragraph{\texorpdfstring{Daylighting Lighting Power Multiplier {[]}}{Daylighting Lighting Power Multiplier }}\label{daylighting-lighting-power-multiplier-1}
+
+The amount by which the overhead electric lighting power in a zone is multiplied due to usage of daylighting to dim or switch electric lights. For example, if the multiplier is M and the electric power without dimming is P, then the electric power with dimming is M*P. The multiplier varies from 0.0, which corresponds to maximum dimming (zero electric lighting), to 1.0, which corresponds to no dimming.
+
+\subsection{Output:IlluminanceMap}\label{outputilluminancemap}
+
+The Output:IlluminanceMap object expands on the reporting capabilities of the daylighting simulation. For any zone simulated with Daylighting:Controls, the illuminance map can generate up to 2,500 points of additional daylighting illuminance values. The resulting map is output as a comma delimited text file that can be imported into a spreadsheet program for rapid visualization of the daylighting illuminance patterns in a zone. The values are produced on an hourly basis. The Z height of the map is constant (parallel to a flat floor). More than one illuminance map can be created for a zone.
+
+\subsubsection{Inputs}\label{inputs-4-006}
+
+\paragraph{Field: Name}\label{field-name-2-007}
+
+The name of the map object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-2-000}
+
+Reference to a zone with Daylighting:Controls.
+
+\paragraph{Field: Z Height}\label{field-z-height}
+
+The height or elevation of the grid of daylighting points.
+
+\paragraph{Field: X Minimum Coordinate}\label{field-x-minimum-coordinate}
+
+The minimum X coordinate boundary for the map.
+
+\paragraph{Field: X Maximum Coordinate}\label{field-x-maximum-coordinate}
+
+The maximum X coordinate boundary for the map.
+
+\paragraph{Field: Number of X Grid Points}\label{field-number-of-x-grid-points}
+
+The number of daylighting reference points in the X direction from the minimum to the maximum boundaries. The maximum number of points that can be generated is 2500 (Number of X Grid Points X Number of Y Grid Points).
+
+\paragraph{Field: Y Minimum Coordinate}\label{field-y-minimum-coordinate}
+
+The minimum Y coordinate boundary for the map.
+
+\paragraph{Field: Y Maximum Coordinate}\label{field-y-maximum-coordinate}
+
+The maximum Y coordinate boundary for the map.
+
+\paragraph{Field: Number of Y Grid Points}\label{field-number-of-y-grid-points}
+
+The number of daylighting reference points in the Y direction from the minimum to the maximum boundaries. The maximum number of points that can be generated is 2500 (Number of X Grid Points X Number of Y Grid Points).
+
+Note:~ Daylighting factors cannot be accurately calculated for reference points that are very close to a wall or window (less than 0.15 m or 6 inches). An error is reported for a reference point that is too close to a window, but no error is reported for a point that is too close to a wall.
+
+\begin{lstlisting}
+
+Output:IlluminanceMap,
+    Daylit Map,      ! Map Name
+    Daylit Zone,     ! Zone Name
+    0,               ! Z Height [m]
+    0.1,             ! X Minimum Coordinate [m]
+    4.9,             ! X Maximum Coordinate [m]
+    10,              ! Number of X Grid Points
+    0.1,             ! Y Minimum Coordinate [m]
+    9.9,             ! Y Maximum Coordinate [m]
+    10;              ! Number of Y grid Points
+\end{lstlisting}
+
+Since not all zones are rectangular, it is possible to have map points that are outside the zone. Any illuminance registered at these points is inaccurate and, additionally, a ``*'' marks these values for easy observance.
+
+\subsection{OutputControl:IlluminanceMap:Style}\label{outputcontrolilluminancemapstyle}
+
+This object specifies the ``style'' for the illuminance map output (described in the Output Details and Examples document). As described early in the document (see: EnergyPlus Output Processing), the user may select the ``style'' for the daylighting illuminance map output file (eplusmap.\textless{}ext\textgreater{}).
+
+\subsubsection{Inputs}\label{inputs-5-006}
+
+\paragraph{Field: Column Separator}\label{field-column-separator}
+
+For this field, the desired separator for columns is entered. ``Comma'' creates comma separated fields/columns in the outputs (eplusmap.csv file is created). ``Tab'' creates tab separated fields/columns in the outputs (eplusmap.tab file is created). ``Fixed'' creates space separated fields/columns in the outputs (eplusmap.txt file is created) but these are not necessarily lined up for easy printing.
+
+Note that both tab and comma separated files easily import into Excelâ„¢ or other spreadsheet programs. The tab delimited files can also be viewed by text editors, word processing programs and easily converted to ``tables'' within those programs.
+
+\subsection{Daylighting Devices}\label{daylighting-devices}
+
+Daylighting devices work in conjunction with the Daylighting:Controls object to simulate components that can improve daylighting in a zone.
+
+Daylighting devices are also tightly integrated into the zone heat balance. The thermal effects of these devices are simulated with or without the use of a Daylighting:Controls object.
+
+There are two types of daylighting device in EnergyPlus:~ tubular daylighting devices and daylighting shelves.
+
+\subsection{DaylightingDevice:Tubular}\label{daylightingdevicetubular}
+
+Tubular daylighting devices (TDDs), also known as tubular skylights or light pipes, are used to bring natural exterior daylight into the hard-to-reach, interior spaces of a building.
+
+TDDs consist of three components: a dome, a pipe, and a diffuser.
+
+\begin{figure}[hbtp] % fig 66
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image108.png}
+\caption{Tubular daylighting device diagram. \protect \label{fig:tubular-daylighting-device-diagram.}}
+\end{figure}
+
+In EnergyPlus each of these components corresponds to an object in the input file.
+
+The dome and diffuser are defined in the same way as windows using the FenestrationSurface:Detailed object. The \emph{Surface Type} field must be specified as TubularDaylightDome or TubularDaylightDiffuser accordingly.
+
+The location and orientation of the dome surface affect the total amount of daylight collected.
+
+The \emph{Base Surface} of the diffuser object determines to which zone the daylighting is delivered. The location and orientation of the diffuser surface affect the amount of daylight received at the Daylighting:Controls reference points.
+
+Although the object definition is the same as for a window, there are several restrictions on TubularDaylightDome and TubularDaylightDiffuser objects:
+
+\begin{itemize}
+\item
+  Shading control devices are not allowed.
+\item
+  Frames and dividers are not allowed.
+\item
+  Multipliers must be 1.0.
+\item
+  Dome, diffuser, and pipe areas (as given by diameter) must be approximately equal.
+\item
+  Outside face environment objects are not allowed.
+\item
+  Dome and diffuser constructions cannot be more than one layer.
+\end{itemize}
+
+Since commercial TDDs are assumed to be cylindrical in shape, it is recommended that the circular areas of the actual dome and diffuser be approximated with a square of equivalent area for the TubularDaylightDome and TubularDaylightDiffuser objects. Although it is possible to use a triangular surface instead, a square is a much better geometric approximation of a circle.
+
+Note that the TubularDaylightDome surface is allowed to have a different position and tilt from the roof base surface. If the actual TDD projects some height above the roof surface, the TubularDaylightDome coordinates should be located accordingly.
+
+\begin{figure}[hbtp] % fig 67
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image109.png}
+\caption{Tubular daylighting device DXF output. \protect \label{fig:tubular-daylighting-device-dxf-output.}}
+\end{figure}
+
+The TubularDaylightDome surface automatically casts a shadow on the roof base surface. However, since the pipe is not represented by a surface, it will not cast a shadow. If this effect must be simulated, one or more SURFACE:SHADING objects can be used.
+
+The dome and diffuser objects are connected by the DAYLIGHTING DEVICE:TUBULAR object:
+
+\subsubsection{Inputs}\label{inputs-6-005}
+
+\paragraph{Field: Name}\label{field-name-3-007}
+
+The name of the TDD object.
+
+\paragraph{Field: Dome Name}\label{field-dome-name}
+
+Reference to a FenestrationSurface:Detailed object with \emph{Surface Type} TubularDaylightDome.
+
+\paragraph{Field: Diffuser Name}\label{field-diffuser-name}
+
+Reference to a FenestrationSurface:Detailed object with \emph{Surface Type} TubularDaylightDiffuser.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-001}
+
+The construction of the TDD pipe. The visible and solar absorptance of the inside material layer determines the reflectivity of the inner mirrored surface of the TDD. This is very important for the overall transmittance of the TDD.
+
+\paragraph{Field: Diameter}\label{field-diameter}
+
+The diameter {[}m{]} of the TDD pipe. The area of the pipe must match the areas of the dome and diffuser.
+
+\paragraph{Field: Total Length}\label{field-total-length}
+
+The total length {[}m{]} of the TDD pipe between the dome and the diffuser, including the exterior part above the roof. The exterior length is determined internally by subtracting the transition zone lengths from the total length.
+
+\paragraph{Field: Effective Thermal Resistance}\label{field-effective-thermal-resistance}
+
+The effective thermal resistance {[}m\(^{2}\)-K/W{]}, i.e.~R-value, of the TDD between the exterior dome surface and the interior diffuser surface.
+
+\paragraph{Field: Transition Zone\textless{}\#\textgreater{}~ Name}\label{field-transition-zone-name}
+
+Name of zone that the TDD pipe passes through before reaching the delivery zone.
+
+\paragraph{Field: Transition Zone \textless{}\#\textgreater{} Length}\label{field-transition-zone-length}
+
+Length of pipe {[}m{]} in the transition zone. This is used for determining heat gains due to solar absorbed by the pipe in each transition zone. The distribution of absorbed solar gains can be customized by adjusting the length of pipe in each transition zone.~~ The transition zone gain is proportional to the length of pipe in the zone. If no transition zones are specified, all solar absorbed by the pipe is lost to the exterior environment.
+
+The \emph{Transition Zone Name} and \emph{Transition Zone Length} fields can be repeated for additional transition zones.
+
+\begin{lstlisting}
+DaylightingDevice:Tubular,
+  Pipe1,                    !- Object Name
+  Dome1,                    !- Dome Name
+  Diffuser1,                !- Diffuser Name
+  Reflective Aluminum,      !- Construction Name
+  0.3556,                   !- Diameter [m] (approximately 14", a standard size)
+  1.4,                      !- Total Length [m] (subtract zone lengths to get outdoor exposed length)
+  0.28,                     !- Effective Thermal Resistance [m2-K/W] between TubularDaylightDome and TubularDaylightDiffuser
+  Attic Zone,               !- Transition Zone 1 Name
+  1.1;                      !- Transition Zone 1 Length [m]
+
+FenestrationSurface:Detailed,
+  Dome1,  !- Subsurface Name
+  TubularDaylightDome,  !- Surface Type
+  Clear Acrylic Dome,  !- Construction Name (only 1 layer allowed in construction)
+  Attic Roof,  !- Base Surface Name
+  ,  !- Outside Face Environment (not allowed for TubularDaylightDome)
+  0.0,  !- VF to Ground
+  ,  !- Window Shading Control (not allowed for TubularDaylightDome)
+  ,  !- Frame/Divider Name (not allowed for TubularDaylightDome)
+  1.0,  !- Multiplier (must be 1.0 for TubularDaylightDome)
+  4,  !- Number of Vertices
+  2.3425,  3.1575,  3.9,
+  2.3425,  2.8425,  3.9,
+  2.6575,  2.8425,  3.9,
+  2.6575,  3.1575,  3.9;
+
+FenestrationSurface:Detailed,
+  Diffuser1,  !- Subsurface Name
+  TubularDaylightDiffuser,  !- Surface Type
+  Frosted Acrylic Diffuser,  !- Construction Name (only 1 layer allowed in construction)
+  Daylit Zone Ceiling,  !- Base Surface Name
+  ,  !- Outside Face Environment (not allowed for TubularDaylightDiffuser)
+  0.0,  !- VF to Ground
+  ,  !- Window Shading Control (not allowed for TubularDaylightDiffuser)
+  ,  !- Frame/Divider Name (not allowed for TubularDaylightDiffuser)
+  1.0,  !- Multiplier (must be 1.0 for TubularDaylightDiffuser)
+  4,  !- Number of Vertices
+  2.3425,  3.1575,  2.5,
+  2.3425,  2.8425,  2.5,
+  2.6575,  2.8425,  2.5,
+  2.6575,  3.1575,  2.5;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-004}
+
+\begin{itemize}
+\item
+  Zone,Average,Tubular Daylighting Device Transmitted Solar Radiation Rate {[}W{]}
+\item
+  Zone,Average,Tubular Daylighting Device Pipe Absorbed Solar Radiation Rate {[}W{]}
+\item
+  Zone,Average,Tubular Daylighting Device Heat Gain Rate {[}W{]}
+\item
+  Zone,Average,Tubular Daylighting Device Heat Loss Rate {[}W{]}
+\item
+  Zone,Average,Tubular Daylighting Device Beam Solar Transmittance {[]}
+\item
+  Zone,Average,Tubular Daylighting Device Beam Visible Transmittance {[]}
+\item
+  Zone,Average,Tubular Daylighting Device Diffuse Solar Transmittance {[]}
+\item
+  Zone,Average,Tubular Daylighting Device Diffuse Visible Transmittance {[]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Tubular Daylighting Device Beam Solar Transmittance {[]}}{Tubular Daylighting Device Beam Solar Transmittance }}\label{tubular-daylighting-device-beam-solar-transmittance}
+
+This is the transmittance of beam solar radiation through the TDD.
+
+\paragraph{\texorpdfstring{Tubular Daylighting Device Beam Visible Transmittance {[]}}{Tubular Daylighting Device Beam Visible Transmittance }}\label{tubular-daylighting-device-beam-visible-transmittance}
+
+This is the transmittance of beam visible radiation, or daylight, through the TDD.
+
+\paragraph{\texorpdfstring{Tubular Daylighting Device Diffuse Solar Transmittance {[]}}{Tubular Daylighting Device Diffuse Solar Transmittance }}\label{tubular-daylighting-device-diffuse-solar-transmittance}
+
+This is the transmittance of diffuse solar radiation through the TDD.
+
+\paragraph{\texorpdfstring{Tubular Daylighting Device Diffuse Visible Transmittance {[]}}{Tubular Daylighting Device Diffuse Visible Transmittance }}\label{tubular-daylighting-device-diffuse-visible-transmittance}
+
+This is the transmittance of diffuse visible radiation, or daylight, through the TDD.
+
+\paragraph{Tubular Daylighting Device Heat Gain Rate {[}W{]}}\label{tubular-daylighting-device-heat-gain-rate-w}
+
+This is the rate of heat gain to the zone by the TDD, in Watts.
+
+\paragraph{Tubular Daylighting Device Heat Loss Rate {[}W{]}}\label{tubular-daylighting-device-heat-loss-rate-w}
+
+This is the rate of heat loss from the zone by the TDD, in Watts.
+
+\paragraph{Tubular Daylighting Device Pipe Absorbed Solar Radiation Rate {[}W{]}}\label{tubular-daylighting-device-pipe-absorbed-solar-radiation-rate-w}
+
+This is the rate at which solar radiation is absorbed by the pipe in the TDD, in Watts.
+
+\paragraph{Tubular Daylighting Device Transmitted Solar Radiation Rate {[}W{]}}\label{tubular-daylighting-device-transmitted-solar-radiation-rate-w}
+
+This is the rate at which solar radiation is transmitted by the TDD, in Watts.
+
+In addition, several surface and window variables are also reported for the TubularDaylightDome and TubularDaylightDiffuser objects. For the TubularDaylightDome:
+
+\begin{itemize}
+\item
+  Zone,Average,Surface Outside Face Sunlit Area {[}m2{]}
+\item
+  Zone,Average,Surface Outside Face Sunlit Fraction {[]}
+\item
+  Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Beam Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Beam Solar Incident Angle Cosine Value{[]}
+\item
+  Zone,Average,Surface Window Transmitted Solar Radiation Rate {[}W{]}
+\item
+  Zone,Average,Surface Window Total Glazing Layers Absorbed Solar Radiation Rate {[}W{]}
+\end{itemize}
+
+For the TubularDaylightDiffuser:
+
+\begin{itemize}
+\item
+  Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area{[}W/m2{]} \emph{(incident inside of pipe)}
+\item
+  Zone,Average,Surface Window Transmitted Solar Radiation Rate {[}W{]} \emph{(same as Tubular Daylighting Device Transmitted Solar Radiation Rate)}
+\item
+  Zone,Average,Surface Window Total Glazing Layers Absorbed Solar Radiation Rate {[}W{]}
+\end{itemize}
+
+\subsection{DaylightingDevice:Shelf}\label{daylightingdeviceshelf}
+
+Daylighting shelves, or simply light shelves, are another device for bringing more daylight into a building. Installed as an accessory to a window, daylighting shelves work by reflecting exterior light onto the ceiling of a room. Daylighting shelves can have an inside shelf, an outside shelf, or both.
+
+\begin{figure}[hbtp] % fig 68
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image110.png}
+\caption{Daylighting shelf diagram. \protect \label{fig:daylighting-shelf-diagram.}}
+\end{figure}
+
+The inside shelf redistributes light that would have entered the zone anyway. Instead of entering as a beam, all light is reflected onto the zone ceiling and is converted to diffuse shortwave radiation.
+
+The outside shelf changes the amount of light entering the zone. If the shelf surface is more reflective than the ground, it can increase the amount of light incident on the upper part of the window. However, the shading effect of the outside shelf on the lower part of the window must also be considered as it can easily negate any gain achieved in the upper part of the window. All light reflected from the outside shelf that enters the upper window is assumed to strike the ceiling.
+
+\begin{figure}[hbtp] % fig 69
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image111.png}
+\caption{Daylighting shelf DXF output. \protect \label{fig:daylighting-shelf-dxf-output.}}
+\end{figure}
+
+In EnergyPlus a daylighting shelf is simulated using a DaylightingDevice:Shelf object in combination with up to three other objects: a window, a heat transfer surface, and an attached shading surface.
+
+The window must be divided into two window surfaces: an upper window and a lower window. The upper window interacts directly with the daylighting shelf object and is not allowed to have any shading control devices or frames or dividers. The lower window does not interact with the daylighting shelf object, but does receive shading from the outside shelf. There are no restrictions on the lower window.
+
+The inside shelf is defined as a regular heat transfer surface in the zone. However, the surface must have the \emph{Outside Boundary Condition} field set to Surface with itself as the other zone surface. Shading and thermal mass effects are taken into account.
+
+The outside shelf is defined as a Shading:Zone:Detailed object. The visible and solar absorptance of the outside material layer determines the reflectivity of the shelf.
+
+\begin{callout}
+  NOTE: Unlike a regular Shading:Zone:Detailed object, the vertices of the outside shelf surface must be ordered so that the outward normal vector points \emph{upward}, i.e.~toward the upper window. This is necessary in order for the outside shelf to properly receive sunlight and shading from other surfaces. A mirror shading surface with the outward normal vector pointing in the opposite direction is automatically created by the program to shade the lower window.
+\end{callout}
+
+The inside shelf and outside shelf are both optional. However, if neither shelf is specified, the daylighting shelf object has no effect on the simulation.
+
+\subsubsection{Inputs}\label{inputs-7-005}
+
+\paragraph{Field: Name}\label{field-name-4-006}
+
+The name of the daylighting shelf object.
+
+\paragraph{Field: Window Name}\label{field-window-name-1}
+
+Reference to a FenestrationSurface:Detailed object with \emph{Surface Type} WINDOW.
+
+\paragraph{Field: Inside Shelf Name}\label{field-inside-shelf-name}
+
+Reference to a BuildingSurface:Detailed object. This field is optional. If used, this surface must have OTHERZONESURFACE specified for the \emph{Outside Face Environment} field and the referenced other zone surface must be itself. The number of vertices of this surface object must be 4.
+
+\paragraph{Field: Outside Shelf Name}\label{field-outside-shelf-name}
+
+Reference to a Shading:Zone:Detailed object. This field is optional. If used, the number of vertices of this surface object must be 4.
+
+\paragraph{Field: Outside Shelf Construction Name}\label{field-outside-shelf-construction-name}
+
+Reference to a CONSTRUCTION object. This field is required if an outside shelf is specified. The visible and solar absorptance of the outside material layer determines the shelf reflectivity.
+
+\paragraph{Field: View Factor To Outside Shelf}\label{field-view-factor-to-outside-shelf}
+
+User defined value for the view factor from the window to the outside shelf. This field is optional. If not specified, an exact view factor is calculated for two perpendicular rectangles of the same width having a shared edge. If the given surfaces do not meet these geometric requirements, it is necessary to specify a value here.
+
+\begin{callout}
+  NOTE: It is up to the user to adjust the view factor to ground of the upper window to account for the part of the view blocked by the outside shelf. The calculated \emph{View Factor To Outside Shelf} is reported in the eio file for this purpose. For the typical case where the shelf is parallel to the ground and the upper window is perpendicular to the ground, the view factor to ground is simply: 0.5 -- \emph{View Factor To Outside Shelf}.
+\end{callout}
+
+\begin{lstlisting}
+DaylightingDevice:Shelf,
+    Shelf,  !- Name
+    Daylit Upper Window,  !- Window Name
+    Inside Shelf,  !- Inside Shelf Name
+    Outside Shelf,  !- Outside Shelf Name
+    Shelf Construction;  !- Outside Shelf Construction Name (required if outside shelf specified)
+    ! 0.29;  !- View Factor To Outside Shelf (optional)
+
+FenestrationSurface:Detailed,
+    Daylit Upper Window,  !- Subsurface Name
+    Window,  !- Surface Type
+    Standard Window,  !- Construction Name
+    Daylit South Wall,  !- Base Surface Name
+    ,  !- Outside Face Environment
+    0.211,  !- VF to Ground (user must adjust to account for view factor to outside shelf)
+    ,  !- Window Shading Control (not allowed)
+    ,  !- Frame/Divider Name (not allowed)
+    1.0,  !- Multiplier (must be 1.0)
+    4,  !- Number of Vertices
+    1.0,  0.0,  2.8,
+    1.0,  0.0,  2.0,
+    4.0,  0.0,  2.0,
+    4.0,  0.0,  2.8;
+
+BuildingSurface:Detailed,
+    Inside Shelf,  !- Surface Name
+    Wall,  !- Surface Type
+    Shelf Construction,  !- Construction Name
+    Daylit Zone,  !- Zone Name
+    OtherZoneSurface,  !- Exterior Conditions (must be OtherZoneSurface)
+    Inside Shelf,  !- Target (must be itself)
+    NoSun,  !- Solar Exposure
+    NoWind,  !- Wind Exposure
+    0.0,  !- VF to Ground
+    4,  !- Number of Vertices
+    1.0,  0.0,  2.0,
+    4.0,  0.0,  2.0,
+    4.0,  1.0,  2.0,
+    1.0,  1.0,  2.0;
+
+Shading:Zone:Detailed,
+    Outside Shelf,  !- Surface Name
+    Daylit South Wall,  !- Base Surface Name
+    ,  !- Shading Transmittance Schedule (default is always opaque)
+    4,  !- Number of Vertices
+    1.0,  0.0,  2.0,  !- Outward normal vector must point up toward the upper window
+    1.0, -1.0,  2.0,
+    4.0, -1.0,  2.0,
+    4.0,  0.0,  2.0;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-002}
+
+The view factor to outside shelf calculation shows up in the .eio file along with the associated window and window view factors to sky and ground:
+
+! \textless{}Shelf Details\textgreater{},Name,View Factor to Outside Shelf,Window Name,Window View Factor to Sky,Window View Factor to Ground
+
+SHELF,0.29,DAYLIT UPPER WINDOW,0.50,0.21
+
+This variable reports the calculated \emph{View Factor To Outside Shelf} so that the user can correctly adjust the view factor to ground of the upper window.
+
+The usual window and surface variables are relevant for the upper window:
+
+\begin{itemize}
+\item
+  Zone,Average,Surface Outside Face Sunlit Area {[}m2{]}
+\item
+  Zone,Average,Surface Outside Face Sunlit Fraction {[]}
+\item
+  Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Beam Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Beam Solar Incident Angle Cosine Value{[]}
+\item
+  Zone,Average,Surface Window Transmitted Solar Radiation Rate {[}W{]}
+\item
+  Zone,Average,Surface Window Total Glazing Layers Absorbed Solar Radiation Rate {[}W{]}
+\item
+  Zone,Average,Surface Window Heat Gain Rate {[}W{]}
+\item
+  Zone,Average,Surface Window Heat Loss Rate {[}W{]}
+\end{itemize}
+
+The following surface variables are reported for the outside shelf surface, if specified:
+
+\begin{itemize}
+\item
+  Zone,Average,Surface Outside Face Sunlit Area {[}m2{]}
+\item
+  Zone,Average,Surface Outside Face Sunlit Fraction {[]}
+\item
+  Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Beam Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area{[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Beam Solar Incident Angle Cosine Value{[]}
+\end{itemize}
+
+\subsection{DaylightingDevice:LightWell}\label{daylightingdevicelightwell}
+
+This object is used to model the impacts on daylighting of a ``light well'' that might be associated with exterior windows such as skylights.~ The light well model attenuates the light transmitted by the skylight. The attenuation is characterized by the \textbf{well efficiency}, which is the ratio of the amount of light leaving the well to the amount of light entering the well. The well efficiency varies from close to 1.0~ to close to zero if there is high attenuation. The well efficiency is used only in the EnergyPlus detailed daylighting calculation, where it multiplies the beam and diffuse light transmitted by the skylight. (The well efficiency is not used in calculating the solar gain through the skylight.)
+
+The input object describes the light well using basic characteristics of the geometry along with the visible reflectance of the well's side walls.~ The following figure diagrams how the geometry is characterized.
+
+\begin{figure}[hbtp] % fig 70
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image112.png}
+\caption{Skylight with light well: (a) perspective view, (b) vertical section. If the bottom of the light well is a rectangle of side lengths c and d, as shown in (a), then the perimeter of the bottom of the well = 2(c+d) and the area = cd (see description of field names for the Light Well object). \protect \label{fig:skylight-with-light-well-a-perspective-view-b}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-8-004}
+
+\paragraph{Field: Exterior Window Name}\label{field-exterior-window-name}
+
+The name of the exterior window that this Light Well is associated with. Generally this is a skylight in a roof. However, light wells can be applied to an exterior window of any slope. Light wells can be assigned to both rectangular and triangular exterior windows, but they should not be assigned to interior windows. Note that the sides of the light well can be sloped and the bottom of the light well can be any shape, not~ just rectangular.
+
+\paragraph{Field: Height of Well}\label{field-height-of-well}
+
+The distance from the bottom of the skylight to the bottom of the well. If the skylight and well bottom are not coplanar, this is the distance from the center of the bottom of the skylight to center of the bottom of the well. See Figure~\ref{fig:skylight-with-light-well-a-perspective-view-b}.
+
+\paragraph{Field: Perimeter of Bottom of Well}\label{field-perimeter-of-bottom-of-well}
+
+The perimeter of the bottom opening of the well. See Figure~\ref{fig:skylight-with-light-well-a-perspective-view-b}.
+
+\paragraph{Field: Area of Bottom of Well}\label{field-area-of-bottom-of-well}
+
+The area of the bottom opening of the well. A warning will be issued if this area is less that the area of the skylight, including frame if present. See Figure~\ref{fig:skylight-with-light-well-a-perspective-view-b}.
+
+\paragraph{Field: Visible Reflectance of Well Walls}\label{field-visible-reflectance-of-well-walls}
+
+The visible reflectance of the side walls of the well. If the walls do not all have the same reflectance, an area-weighted average value can be used.~ This is the well-wall reflectance expressed as a fraction.
+
+An IDF example:
+
+\begin{lstlisting}
+DaylightingDevice:LightWell,  ! The well is 60% reflecting, is 1.2m high and has a 2.5m x 5.5m bottom opening.
+   Skylight-1, !- Name of Exterior Window that this Light Well Applies To
+   1.2,        !- Height of Well(m)
+   16.0,       !- Perimeter of Bottom of Well (m)
+   13.75,      !- Area of Bottom of Well (m2)
+   0.60;       !- Visible Reflectance of Well Walls
+\end{lstlisting}
+
+\subsection{Daylighting Modeling Options}\label{daylighting-modeling-options}
+
+The following table shows what input objects/fields to use to model different daylighting options. It also gives the name of an example input, if available, that demonstrates the option.
+
+% table 21
+{\scriptsize
+\begin{longtable}[c]{>{\raggedright}p{1.5in}>{\raggedright}p{3.0in}>{\raggedright}p{1.5in}}
+\caption{Daylighting Modeling Options \label{table:daylighting-modeling-options}} \tabularnewline
+\toprule 
+Option & Object/Field or Output Variable & Input File \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Daylighting Modeling Options} \tabularnewline
+\toprule 
+Option & Object/Field or Output Variable & Input File \tabularnewline
+\midrule
+\endhead
+
+Allow a thermal zone to be daylit & Daylighting:Controls, Daylighting:DELight:Controls & PurchAirWithDaylighting.idf, DElight-Detailed-Comparison.idf \tabularnewline
+Specify visible transmittance of the glazing & WindowMaterial:Glazing & PurchAirWithDaylighting.idf \tabularnewline
+Specify the visible transmittance of a shading device & WindowMaterial:Shade, WindowMaterial:Screen or WindowMaterial:Blind & PurchAirWindowBlind.idf \tabularnewline
+Use a shading device to control glare & WindowMaterial:Shade or WindowMaterial:Blind; WindowProperty:ShadingControl* & PurchAirWindowBlind.idf \tabularnewline
+Use electrochromic glazing to control glare & WindowProperty:ShadingControl/Shading Type = SwitchableGlazing, Shading Control Type = On If High Glare, Glare Control Is Active = Yes* & PurchAirWithDaylighting.idf \tabularnewline
+Adjust electrochromic glazing to just meet daylighting illuminance setpoint & WindowProperty:ShadingControl/Shading Type = SwitchableGlazing, Shading Control Type = MeetDaylightIlluminanceSetpoint* & ~ \tabularnewline
+Print an illuminance map & Daylighting:Illuminance Map* & ~ \tabularnewline
+Control electric lighting response to daylight illuminance level & Daylighting:Controls/Lighting Control Type = Continuous, Stepped or Continuous/Off, plus other fields; or …. Daylighting:DELight:Controls/Lighting Control Type = Continuous, Stepped or Continuous/Off, plus other fields & PurchAirWithDaylighting.idf; DElight-Detailed-Comparison.idf \tabularnewline
+Add a light shelf (with Daylighting:Controls) & DaylightingDevice:Shelf * & DaylightingDeviceShelf.idf \tabularnewline
+Add a light shelf (with Daylighting:DELight:Controls) & Daylighting:DELight:Controls & DElightCFSLightShelf.idf \tabularnewline
+Add a light pipe & DaylightingDevice:Tubular * & DaylightingDeviceTubular.idf \tabularnewline
+Model a skylight having a light well & DaylightingDevice:LightWell * & ~ \tabularnewline
+Model daylighting through double facade & See “Double Facades: Daylighting through Interior Windows�* & PurchAirWithDoubleFacadeDaylighting.idf \tabularnewline
+Add diffusing (translucent) glass & WindowMaterial:Glazing/Solar Diffusing = Yes* & ~ \tabularnewline
+Model complex fenestration & Daylighting:DELight:Controls & DElightCFSWindow.idf \tabularnewline
+Get a radiosity-based interior light inter-reflection calculation & Daylighting:DELight:Controls & DElight-Detailed-Comparison.idf \tabularnewline
+Find effect on daylighting of solar reflected from overhangs, neighboring buildings, etc. & Building/SolarDistribution uses “withReflections� option & ~ \tabularnewline
+Find visible transmittance effect of dirt on window & WindowMaterial:Glazing/Dirt Correction Factor for Solar and Visible Transmittance* & ~ \tabularnewline
+\bottomrule
+\end{longtable}}
+
+*Used only with Daylighting:Controls
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+\protect\hyperlink{ux5fftnref1}{{[}1{]}} Formerly, only the exterior windows in a zone could provide daylight to that zone.
diff --git a/doc/input-output-reference/src/overview/group-demand-limiting-controls.tex b/doc/input-output-reference/src/overview/group-demand-limiting-controls.tex
new file mode 100644
index 00000000000..c2a0aa625c7
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-demand-limiting-controls.tex
@@ -0,0 +1,521 @@
+\section{Group Demand Limiting Controls}\label{group-demand-limiting-controls}
+
+Demand limiting, or demand management, is a strategy for reducing a building's demand for utilities, e.g., electricity. Utility companies typically charge a monthly fee for ``demand charges'' that is based on the peak demand during a certain time period. Often the peak demand charge is set by one exceptional day that is much higher than the peak demand for an average day during the month. Therefore, to save utility costs, it is in the interest of building owners to find ways to manage the demand on peak days. While demand management is generally concerned with the demand for electricity, the future will likely see demand management of other utilities, such as natural gas or water.
+
+Demand limiting controls shut off or reduce the power to non-essential loads in order to reduce the overall building demand. Some typical controls:
+
+\begin{itemize}
+\item
+  shut off or dim electric lights, equipment, or HVAC systems
+\item
+  reset the thermostatic set points on HVAC systems
+\item
+  reduce the load of a set of similar components by rotating one or more components ``off'' for a short time interval
+\item
+  turn on generators to meet some or all of the building's demand.
+\end{itemize}
+
+The demand limiting controls implemented in EnergyPlus are intended to allow some of the more common demand limiting strategies. Currently, only Exterior:Lights, Lights, ElectricEquipment, ZoneControl:Thermostat, and Controller:OutdoorAir objects can be demand limited. Additional components will be demand limited in future releases.
+
+\subsection{DemandManagerAssignmentList}\label{demandmanagerassignmentlist}
+
+The DemandManagerAssignmentList object is a high level control that makes demand limiting decisions based on a list of possible demand limiting strategies. Each demand limiting strategy is described in a separate DemandManager object. (This is structured like the relationship between the AvailabilityManagerAssignmentList and the AvailabilityManager objects.)
+
+Each DemandManagerAssignmentList monitors and demand limits one meter. Only electricity meters are currently allowed. In many cases, the meter will be \emph{Electricity:Facility}. A schedule and safety factor are used to set the demand limit above which the DemandManagers become activated. The billing month schedule and demand window are also taken into account when calculating the demand limit.
+
+DemandManagers in the list are activated based on the \emph{Demand Manager Priority}. If the \textbf{Sequential} option is used, each manager in the list is activated in sequence from first to last until demand is reduced below the limit or until all managers are activated. If the \textbf{All} option is used, all managers are activated simultaneously to achieve the maximum demand reduction.
+
+A DemandManager is skipped if it cannot reduce the demand. Possible reasons that a manager cannot reduce demand include:
+
+\begin{itemize}
+\item
+  not enough load to limit
+\item
+  not available because of its \emph{Availability Schedule}
+\item
+  already activated; load limited during a previous timestep.
+\end{itemize}
+
+\subsubsection{Inputs}\label{inputs-010}
+
+\paragraph{Field: Name}\label{field-name-009}
+
+The name of the DemandManagerAssignmentList object.
+
+\paragraph{Field: Meter Name}\label{field-meter-name}
+
+This field references the meter that is to be monitored and demand limited. Only electricity meters are currently allowed.
+
+\paragraph{Field: Demand Limit Schedule Name}\label{field-demand-limit-schedule-name}
+
+The reference to the schedule object specifying the target demand limits {[}schedule values should be in Watts{]}.
+
+\paragraph{Field: Demand Limit Safety Fraction}\label{field-demand-limit-safety-fraction}
+
+This field is a multiplier that is applied to the target demand limit (above). When the metered demand exceeds (target demand limit * safety fraction), the DemandManagers begin to limit the demand. This helps to ensure that the target limit is not exceeded.
+
+\paragraph{Field: Billing Period Schedule Name}\label{field-billing-period-schedule-name}
+
+The reference to the schedule object that defines the monthly billing periods. The peak demand during the peak period of the billing period typically determines the demand charge. This should reference the same schedule that is used in the \emph{Month Schedule Name} field of the UtilityCost:Tariff object. If left blank, it defaults to the regular divisions between months.
+
+\paragraph{Field: Peak Period Schedule Name}\label{field-peak-period-schedule-name}
+
+The reference to the schedule object that defines the peak/off-peak time-of-use periods. The peak demand during the peak period of the billing period typically determines the demand charge. This should reference the same schedule that is used in the \emph{Time of Use Period Schedule Name} field of the UtilityCost:Tariff object. A value of 1 indicates the peak period; any other value is off-peak. If left blank, it defaults to always on the peak period. The DemandManagerAssignmentList only attempts to demand limit during peak periods.
+
+\paragraph{Field: Demand Window Length}\label{field-demand-window-length}
+
+This field is similar to the field of the same name in the UtilityCost:Tariff object. However, the user may not want to limit using the same demand window as the utility company. This field allows the user to input the number of minutes over which to calculate the current demand. The minutes are rounded to match the nearest multiple of time steps.
+
+\paragraph{Field: Demand Manager Priority}\label{field-demand-manager-priority}
+
+This field indicates what logic should be used to activate the individual DemandManagers in the list. \textbf{Sequential} treats the list of DemandManagers as a sequential priority list, i.e., the first DemandManager in the list is activated first, then the second, etc., until the demand falls below the limit. \textbf{All} activates all demand managers to achieve the maximum demand reduction.
+
+\paragraph{Field: Demand Manager Type 1}\label{field-demand-manager-type-1}
+
+The key word defining the type of DemandManager.
+
+\paragraph{Field: Demand Manager Name 1}\label{field-demand-manager-name-1}
+
+The name of a DemandManager object defined elsewhere in the input file.
+
+DemandManagers are listed by pairs of data items: \emph{Demand Manager Type} and \emph{Demand Manager Name}. Ten managers are accomodated in the list by default. The IDD specification, however, is extensible and additional pairs may be added by directly editing the IDD.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+DemandManagerAssignmentList,
+  Demand Manager,                   !- Name
+  Electricity:Facility,       !- Meter Name
+  Limit Schedule,                   !- Demand Limit Schedule Name
+  1.0,                                         !- Demand Limit Safety Fraction
+  ,                                               !- Billing Period Schedule Name
+  ,                                               !- Peak Period Schedule Name
+  15,                                           !- Demand Window Length {minutes}
+  Sequential,                           !- Demand Manager Priority
+  DemandManager:ExteriorLights,   !- DemandManager 1 Object Type
+  Ext Lights Manager,           !- DemandManager 1 Name
+  DemandManager:ElectricEquipment,   !- DemandManager 2 Object Type
+  Eq Mgr Stage 1,                   !- DemandManager 2 Name
+  DemandManager:ElectricEquipment,   !- DemandManager 3 Object Type
+  Eq Mgr Stage 2,                   !- DemandManager 3 Name
+  DemandManager:ElectricEquipment,   !- DemandManager 4 Object Type
+  Eq Mgr Stage 3,                   !- DemandManager 4 Name
+  DemandManager:Lights,       !- DemandManager 5 Object Type
+  Lights Manager,                   !- DemandManager 5 Name
+  DemandManager:Thermostats,   !- DemandManager 6 Object Type
+  Thermostats Manager;         !- DemandManager 6 Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-007}
+
+The following output variables are reported for the DemandManagerAssignmentList object:
+
+\begin{itemize}
+\item
+  Zone,Average,Demand Manager Meter Demand Power {[}W{]}
+\item
+  Zone,Average,Demand Manager Average Demand Power {[}W{]}
+\item
+  Zone,Average,Demand Manager Peak Demand Power {[}W{]}
+\item
+  Zone,Average,Demand Manager Scheduled Limit Power {[}W{]}
+\item
+  Zone,Average,Demand Manager Demand Limit Power {[}W{]}
+\item
+  Zone,Average,Demand Manager Avoided Demand {[}W{]}
+\item
+  Zone,Average,Demand Manager Over Limit Power {[}W{]}
+\item
+  Zone,Sum,Demand Manager Over Limit Time {[}hr{]}
+\item
+  Zone,Sum,Demand Manager Exterior Energy Iteration Count {[]}
+\item
+  Zone,Sum,Demand Manager Heat Balance Iteration Count {[]}
+\item
+  Zone,Sum,Demand Manager HVAC Iteration Count {[]}
+\end{itemize}
+
+\paragraph{Demand Manager Meter Demand Power {[}W{]}}\label{demand-manager-meter-demand-power-w}
+
+The current demand for the designated meter.
+
+\paragraph{Demand Manager Average Demand Power {[}W{]}}\label{demand-manager-average-demand-power-w}
+
+The current demand for the designated meter averaged over the \emph{Demand Window Length}.
+
+\paragraph{Demand Manager Peak Demand Power {[}W{]}}\label{demand-manager-peak-demand-power-w}
+
+The peak demand in the billing month so far.
+
+\paragraph{Demand Manager Scheduled Limit Power {[}W{]}}\label{demand-manager-scheduled-limit-power-w}
+
+The scheduled target demand limit from the \emph{Demand Limit Schedule}.
+
+\paragraph{Demand Manager Demand Limit Power {[}W{]}}\label{demand-manager-demand-limit-power-w}
+
+The actual demand limit after multiplication by the \emph{Demand Limit Safety Fraction}.
+
+\paragraph{Demand Manager Avoided Demand {[}W{]}}\label{demand-manager-avoided-demand-w}
+
+The demand that was avoided by the active DemandManagers.
+
+\paragraph{Demand Manager Over Limit Power {[}W{]}}\label{demand-manager-over-limit-power-w}
+
+The difference between the demand limit and the average demand.
+
+\paragraph{Demand Manager Over Limit Time {[}hr{]}}\label{demand-manager-over-limit-time-hr}
+
+The number of hours that the demand limit was exceeded.
+
+\paragraph{\texorpdfstring{Demand Manager Exterior Energy Iteration Count {[]}}{Demand Manager Exterior Energy Iteration Count }}\label{demand-manager-exterior-energy-iteration-count}
+
+The number times that the exterior energy use was resimulated for demand limiting.
+
+\paragraph{\texorpdfstring{Demand Manager Heat Balance Iteration Count {[]}}{Demand Manager Heat Balance Iteration Count }}\label{demand-manager-heat-balance-iteration-count}
+
+The number times that the zone heat balance was resimulated for demand limiting.
+
+\paragraph{\texorpdfstring{Demand Manager HVAC Iteration Count {[]}}{Demand Manager HVAC Iteration Count }}\label{demand-manager-hvac-iteration-count}
+
+The number times that the HVAC system was resimulated for demand limiting.
+
+\subsection{DemandManager:ExteriorLights}\label{demandmanagerexteriorlights}
+
+The DemandManager:ExteriorLights object is used for demand limiting Exterior:Lights objects.
+
+\subsubsection{Inputs}\label{inputs-1-009}
+
+\paragraph{Field: Name}\label{field-name-1-008}
+
+The name of the DemandManager:ExteriorLights object.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-003}
+
+The reference to the schedule object specifying the availability of this DemandManager. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Limit Control}\label{field-limit-control}
+
+This field specifies the type of limiting control. The \textbf{Fixed} option reduces the power to the controlled loads by a fixed amount determined by the \emph{Maximum Limit Fraction} field. The \textbf{Off} option disables the DemandManager in the simulation.
+
+\paragraph{Field: Minimum Limit Duration}\label{field-minimum-limit-duration}
+
+The minimum amount of time {[}minutes{]} that the DemandManager will continue to demand limit after being activated. This prevents loads from turning on and off every time step.
+
+\paragraph{Field: Maximum Limit Fraction}\label{field-maximum-limit-fraction}
+
+This field specifies a fraction of the \emph{Design Level} power for the load that determines the lowest allowable power level. With \emph{Limit Control} set to \textbf{Fixed}, the power is reduced to \emph{Maximum Limit Fraction * Design Level} whenever the manager is activated. For example, if the \emph{Maximum Limit Fraction} is 0.8, then a 100 W design level load is reduced to 80 W when limiting. A \emph{Maximum Limit Fraction} of zero means that the load can be shut off entirely.
+
+\paragraph{Field: Limit Step Change}\label{field-limit-step-change}
+
+NOT YET IMPLEMENTED.
+
+\paragraph{Field: Selection Control}\label{field-selection-control}
+
+This field specifies which loads are selected to be limited. The \textbf{All} option simultaneously limits all of the loads listed in this DemandManager. The \textbf{RotateMany} option limits all loads except for one which rotates sequentially through the loads listed. The \textbf{RotateOne} limits only one load which rotates sequentially through the loads listed. The time interval between rotations is set by the \emph{Rotation Duration} field.
+
+\paragraph{Field: Rotation Duration}\label{field-rotation-duration}
+
+If the \textbf{RotateOne} or \textbf{RotateMany} option is used for \emph{Selection Control}, this field sets the time interval {[}minutes{]} between rotations.
+
+\paragraph{Field: Exterior Lights 1-10 Name}\label{field-exterior-lights-1-10-name}
+
+The names of Exterior:Lights objects defined elsewhere in the input file. These are the loads to be limited by this DemandManager.
+
+Ten objects are accomodated in the list by default. The IDD specification, however, is extensible and additional fields may be added by directly editing the IDD.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+DemandManager:ExteriorLights,
+  Ext Lights Manager,           !- Name
+  ,                                               !- Availability Schedule Name
+  Fixed,                                     !- Limit Control
+  60,                                           !- Minimum Limit Duration {minutes}
+  0.0,                                         !- Maximum Limit Fraction
+  ,                                               !- Limit Step Change
+  All,                                         !- Selection Control
+  ,                                               !- Rotation Duration {minutes}
+  Exterior Lights;                 !- Exterior Lights 1 Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-005}
+
+There are no output variables reported for the DemandManager:ExteriorLights object.
+
+\subsection{DemandManager:Lights}\label{demandmanagerlights}
+
+The DemandManager:Lights object is used for demand limiting Lights objects.
+
+\subsubsection{Inputs}\label{inputs-2-009}
+
+\paragraph{Field: Name}\label{field-name-2-008}
+
+The name of the DemandManager:Lights object.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-001}
+
+The reference to the schedule object specifying the availability of this DemandManager. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Limit Control}\label{field-limit-control-1}
+
+This field specifies the type of limiting control. The \textbf{Fixed} option reduces the power to the controlled loads by a fixed amount determined by the \emph{Maximum Limit Fraction} field. The \textbf{Off} option disables the DemandManager in the simulation.
+
+\paragraph{Field: Minimum Limit Duration}\label{field-minimum-limit-duration-1}
+
+The minimum amount of time {[}minutes{]} that the DemandManager will continue to demand limit after being activated. This prevents loads from turning on and off every time step.
+
+\paragraph{Field: Maximum Limit Fraction}\label{field-maximum-limit-fraction-1}
+
+This field specifies a fraction of the \emph{Design Level} power for the load that determines the lowest allowable power level. With \emph{Limit Control} set to \textbf{Fixed}, the power is reduced to \emph{Maximum Limit Fraction * Design Level} whenever the manager is activated. For example, if the \emph{Maximum Limit Fraction} is 0.8, then a 100 W design level load is reduced to 80 W when limiting. A \emph{Maximum Limit Fraction} of zero means that the load can be shut off entirely.
+
+\paragraph{Field: Limit Step Change}\label{field-limit-step-change-1}
+
+NOT YET IMPLEMENTED.
+
+\paragraph{Field: Selection Control}\label{field-selection-control-1}
+
+This field specifies which loads are selected to be limited. The \textbf{All} option simultaneously limits all of the loads listed in this DemandManager. The \textbf{RotateMany} option limits all loads except for one which rotates sequentially through the loads listed. The \textbf{RotateOne} limits only one load which rotates sequentially through the loads listed. The time interval between rotations is set by the \emph{Rotation Duration} field.
+
+\paragraph{Field: Rotation Duration}\label{field-rotation-duration-1}
+
+If the \textbf{RotateOne} or \textbf{RotateMany} option is used for \emph{Selection Control}, this field sets the time interval {[}minutes{]} between rotations.
+
+\paragraph{Field: Lights 1-10 Name}\label{field-lights-1-10-name}
+
+The names of Lights objects defined elsewhere in the input file. These are the loads to be limited by this DemandManager.
+
+Ten objects are accomodated in the list by default. The IDD specification, however, is extensible and additional fields may be added by directly editing the IDD.
+
+If a global lights statement is used (Ref: Lights), then only that name need be entered and the demand limiting will be applied to all the zones for that lighting. If only one of a set of zones from a global lights statement is desired, then the name to be entered is: \textless{}Zone Name\textgreater{} \textless{}Name of Lights Global Object\textgreater{}.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+DemandManager:Lights,
+  Lights Manager,                   !- Name
+  ,                                               !- Availability Schedule Name
+  Fixed,                                     !- Limit Control
+  60,                                           !- Minimum Limit Duration {minutes}
+  0.5,                                         !- Maximum Limit Fraction
+  ,                                               !- Limit Step Change
+  All,                                         !- Selection Control
+  ,                                               !- Rotation Duration {minutes}
+  Space1-1 Lights 1,             !- Lights 1 Name
+  Space2-1 Lights 1,             !- Lights 2 Name
+  Space3-1 Lights 1,             !- Lights 3 Name
+  Space4-1 Lights 1,             !- Lights 4 Name
+  Space5-1 Lights 1;             !- Lights 5 Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-005}
+
+There are no output variables reported for the DemandManager:Lights object.
+
+\subsection{DemandManager:ElectricEquipment}\label{demandmanagerelectricequipment}
+
+The DemandManager:ElectricEquipment object is used for demand limiting ElectricEquipment objects.
+
+\subsubsection{Inputs}\label{inputs-3-008}
+
+\paragraph{Field: Name}\label{field-name-3-008}
+
+The name of the DemandManager:ElectricEquipment object.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-2-000}
+
+The reference to the schedule object specifying the availability of this DemandManager. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Limit Control}\label{field-limit-control-2}
+
+This field specifies the type of limiting control. The \textbf{Fixed} option reduces the power to the controlled loads by a fixed amount determined by the \emph{Maximum Limit Fraction} field. The \textbf{Off} option disables the DemandManager in the simulation.
+
+\paragraph{Field: Minimum Limit Duration}\label{field-minimum-limit-duration-2}
+
+The minimum amount of time {[}minutes{]} that the DemandManager will continue to demand limit after being activated. This prevents loads from turning on and off every time step.
+
+\paragraph{Field: Maximum Limit Fraction}\label{field-maximum-limit-fraction-2}
+
+This field specifies a fraction of the \emph{Design Level} power for the load that determines the lowest allowable power level. With \emph{Limit Control} set to \textbf{Fixed}, the power is reduced to \emph{Maximum Limit Fraction * Design Level} whenever the manager is activated. For example, if the \emph{Maximum Limit Fraction} is 0.8, then a 100 W design level load is reduced to 80 W when limiting. A \emph{Maximum Limit Fraction} of zero means that the load can be shut off entirely.
+
+\paragraph{Field: Limit Step Change}\label{field-limit-step-change-2}
+
+NOT YET IMPLEMENTED.
+
+\paragraph{Field: Selection Control}\label{field-selection-control-2}
+
+This field specifies which loads are selected to be limited. The \textbf{All} option simultaneously limits all of the loads listed in this DemandManager. The \textbf{RotateMany} option limits all loads except for one which rotates sequentially through the loads listed. The \textbf{RotateOne} limits only one load which rotates sequentially through the loads listed. The time interval between rotations is set by the \emph{Rotation Duration} field.
+
+\paragraph{Field: Rotation Duration}\label{field-rotation-duration-2}
+
+If the \textbf{RotateOne} or \textbf{RotateMany} option is used for \emph{Selection Control}, this field sets the time interval {[}minutes{]} between rotations.
+
+\paragraph{Field: Electric Equipment 1-10 Name}\label{field-electric-equipment-1-10-name}
+
+The names of ElectricEquipment objects defined elsewhere in the input file. These are the loads to be limited by this DemandManager.
+
+Ten objects are accomodated in the list by default. The IDD specification, however, is extensible and additional fields may be added by directly editing the IDD.
+
+If a global Electric Equipment statement is used (Ref: ElectricEquipment), then only that name need be entered and the demand limiting will be applied to all the zones for that equipment. If only one of a set of zones from a global electric equipment statement is desired, then the name to be entered is: \textless{}Zone Name\textgreater{} \textless{}Name of ElectricEquipment Global Object\textgreater{}.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+DemandManager:ElectricEquipment,
+  Eq Mgr Stage 3,                   !- Name
+  ,                                               !- Availability Schedule Name
+  Fixed,                                     !- Limit Control
+  60,                                           !- Minimum Limit Duration {minutes}
+  0.0,                                         !- Maximum Limit Fraction
+  ,                                               !- Limit Step Change
+  All,                                         !- Selection Control
+  ,                                               !- Rotation Duration {minutes}
+  Space5-1 ElecEq 1;             !- Electric Equipment 1 Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-003}
+
+There are no output variables reported for the DemandManager:ElectricEquipment object.
+
+\subsection{DemandManager:Thermostats}\label{demandmanagerthermostats}
+
+The DemandManager:Thermostats object is used for demand limiting ZoneControl:Thermostat objects.
+
+\subsubsection{Inputs}\label{inputs-4-007}
+
+\paragraph{Field: Name}\label{field-name-4-007}
+
+The name of the DemandManager:Thermostats object.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-3-000}
+
+The reference to the schedule object specifying the availability of the DemandManager. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Reset Control}\label{field-reset-control}
+
+This field specifies the type of limiting control. The \textbf{Fixed} option resets the thermostats to a fixed temperature determined by the \emph{Maximum Heating Setpoint Reset} and \emph{Maximum Cooling Setpoint Reset} fields. The \textbf{Off} option disables the DemandManager in the simulation.
+
+\paragraph{Field: Minimum Reset Duration}\label{field-minimum-reset-duration}
+
+The minimum amount of time {[}minutes{]} that the DemandManager will continue to demand limit after being activated. This prevents thermostats from resetting on and off every time step.
+
+\paragraph{Field: Maximum Heating Setpoint Reset}\label{field-maximum-heating-setpoint-reset}
+
+This field specifies the thermostat heating setpoint temperature {[}C{]} that represents the largest allowable temperature reset or setback. With \emph{Reset Control} set to \textbf{Fixed}, the setpoint temperature is reset to the \emph{Maximum Heating Setpoint Reset} whenever the manager is activated. For example, if the heating setpoint is normally 22 C and the \emph{Maximum Heating Setpoint Reset} is 20 C, then the setpoint is reset to 20 C when limiting.
+
+\paragraph{Field: Maximum Cooling Setpoint Reset}\label{field-maximum-cooling-setpoint-reset}
+
+This field specifies the thermostat cooling setpoint temperature {[}C{]} that represents the largest allowable temperature reset or setback. With \emph{Reset Control} set to \textbf{Fixed}, the setpoint temperature is reset to the \emph{Maximum Cooling Setpoint Reset} whenever the manager is activated. For example, if the cooling setpoint is normally 22 C and the \emph{Maximum Cooling Setpoint Reset} is 24 C, then the setpoint is reset to 24 C when limiting.
+
+\paragraph{Field: Reset Step Change}\label{field-reset-step-change}
+
+NOT YET IMPLEMENTED.
+
+\paragraph{Field: Selection Control}\label{field-selection-control-3}
+
+This field specifies which loads are selected to be limited. The \textbf{All} option simultaneously limits all of the loads listed in this DemandManager. The \textbf{RotateMany} option limits all loads except for one which rotates sequentially through the loads listed. The \textbf{RotateOne} limits only one load which rotates sequentially through the loads listed. The time interval between rotations is set by the \emph{Rotation Duration} field.
+
+\paragraph{Field: Rotation Duration}\label{field-rotation-duration-3}
+
+If the \textbf{RotateOne} or \textbf{RotateMany} option is used for \emph{Selection Control}, this field sets the time interval {[}minutes{]} between rotations.
+
+\paragraph{Field: Thermostat 1-10 Name}\label{field-thermostat-1-10-name}
+
+The names of ZoneControl:Thermostat objects defined elsewhere in the input file. These are the loads to be limited by this DemandManager.
+
+Ten objects are accomodated in the list by default. The IDD specification, however, is extensible and additional fields may be added by directly editing the IDD.
+
+If a global thermostat statement is used (Ref: ZoneControl:Thermostat), then only that name need be entered and the demand limiting will be applied to all the zones for that thermostatic control. If only one of a set of zones from a global thermostat statement is desired, then the name to be entered is: \textless{}Zone Name\textgreater{} \textless{}Name of Thermostat Global Object\textgreater{}.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+DemandManager:Thermostats,
+  Thermostats Manager,         !- Name
+  ,                                               !- Availability Schedule Name
+  Fixed,                                     !- Reset Control
+  60,                                           !- Minimum Reset Duration {minutes}
+  19,                                           !- Maximum Heating Setpoint Reset {C}
+  26,                                           !- Maximum Cooling Setpoint Reset {C}
+  ,                                               !- Reset Step Change
+  All,                                         !- Selection Control
+  ,                                               !- Rotation Duration {minutes}
+  SPACE1-1 Control,               !- Thermostat 1 Name
+  SPACE2-1 Control,               !- Thermostat 2 Name
+  SPACE3-1 Control,               !- Thermostat 3 Name
+  SPACE4-1 Control,               !- Thermostat 4 Name
+  SPACE5-1 Control;               !- Thermostat 5 Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-002}
+
+There are no output variables reported for the DemandManager:Thermostats object.
+
+\subsection{DemandManager:Ventilation}\label{demandmanagerventilation}
+
+The DemandManager:Ventilation object is used for limiting the ventilation rate calculated from the Controller:OutdoorAir object.
+
+\subsubsection{Field: Name}\label{field-name-5-006}
+
+The name of the DemandManager:Ventilation object.
+
+\subsubsection{Field: Availability Schedule Name}\label{field-availability-schedule-name-4-000}
+
+The reference to the schedule object specifying the availability of this demand manager. A schedule value of zero indicates that this demand response (DR) is not applicable for that time period. A schedule greater than zero indicates that the demand response applies during the time period. If this field is blank, the schedule has values of one for all time period.
+
+\subsubsection{Field: Limit Control}\label{field-limit-control-3}
+
+This field specifies the type of limiting control. There are three options. The \textbf{FixedRate} option reduces the ventilation to a specified air flow rate. The \textbf{ReductionRatio} specifies the multiplier of the ventilation rate. The \textbf{Off} option disables the demand manager in the simulation.
+
+\subsubsection{Field: Minimum Limit Duration}\label{field-minimum-limit-duration-3}
+
+The minimum amount of time {[}minutes{]} that the demand manager will continue to demand limit after being activated. This prevent loads from turning on and off every time step.
+
+\subsubsection{Field: Fixed Rate}\label{field-fixed-rate}
+
+This field specifies the amount of fixed ventilation rate when the demand manager is active and \emph{FixedRate} limit control is applied. The unit is m3/s.
+
+\subsubsection{Field: Reduction Ratio}\label{field-reduction-ratio}
+
+This field specifies the multiplier of the ventilation rate when the demand manager is active and \emph{ReductionRatio} limit control is applied.
+
+\subsubsection{Field: Limit Step Change}\label{field-limit-step-change-3}
+
+NOT YET IMPLEMENTED.
+
+\subsubsection{Field: Selection Control}\label{field-selection-control-4}
+
+This field specifies which loads (ventilation rates) are selected to be limited. The \textbf{All} option simultaneously limits all of the loads listed in the demand manager. The \textbf{RotateMany} option limits all loads except for one which rotates sequentially through the loads listed. The \textbf{RotateOne} limits only one load which rotates sequentially through the loads listed. The time interval between rotations is set by the \emph{Rotation Duration} field.
+
+\subsubsection{Field: Rotation Duration}\label{field-rotation-duration-4}
+
+If the \textbf{RotateOne} of \textbf{RotateMany} option is used for \emph{Selection Control}, this field sets the time interval {[}minues{]} between rotations.
+
+\subsubsection{Field: Controller Outdoor Air 1-10 Name}\label{field-controller-outdoor-air-1-10-name}
+
+The names of Controller:OutdoorAir objects defined elsewhere in the input file. These are the ventilation rates to be limited by this demand manager. Then objects are accommodated in the list by default. The IDD specification, however, is extensible and additional fields may be added by directly editing the IDD.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+DemandManager:Ventilation,
+  Ventilation Manager,         !- Name
+  ,                            !- Availability Schedule Name
+  ReductionRatio,              !- Reset Control
+  60,                          !- Minimum Limit Duration {minutes}
+  ,                            !- Fixed Rate {m3/s}
+  0.5,                         !- Reduction Ratio
+  ,                            !- Limit Step Change
+  All,                         !- Selection Control
+  ,                            !- Rotation Duration {minutes}
+  OA Controller 1;             !- Controller:OutdoorAir Name
+\end{lstlisting}
+
+\subsection{DemandManager:Ventilation Outputs}\label{demandmanagerventilation-outputs}
+
+There are no output variables reported for the DemandManager:Ventilation object.
diff --git a/doc/input-output-reference/src/overview/group-desiccant-dehumidifiers.tex b/doc/input-output-reference/src/overview/group-desiccant-dehumidifiers.tex
new file mode 100644
index 00000000000..d94ba98d48b
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+\section{Group Desiccant Dehumidifiers}\label{group-desiccant-dehumidifiers}
+
+\subsection{Dehumidifier:Desiccant:NoFans}\label{dehumidifierdesiccantnofans}
+
+This object models a solid desiccant dehumidifier (excluding associated fans). The process air stream is the air which is dehumidified. The regen air stream is the air which is heated to regenerate the desiccant. This object determines the process air outlet conditions, the load on the regeneration heating coil, the electric power consumption for the wheel rotor motor, and the regeneration air fan mass flow rate. All other heat exchangers are modeled as separate objects connected to the inlet and outlet nodes of the dehumidifier. The solid desiccant dehumidifier is typically used in an AirLoopHVAC:OutdoorAirSystem object, but can also be specified in any AirLoopHVAC. The regeneration heating coil can be Gas, Electric, Steam , or Hot Water coil. When hot water coil is selected as regeneration heating coil user-defined curves designed for lower temperature operation must be specified in the input field Performance Model Type along with the Nominal Regeneration Temperature input field. The default performance model type is valid for higher nominal regeneration temperature (e.g.~121C).
+
+\subsubsection{Inputs}\label{inputs-011}
+
+\paragraph{Field: Name}\label{field-name-010}
+
+This alpha field contains the identifying name for the desiccant dehumidifier.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-004}
+
+The name of the schedule (ref: Schedule) that denotes whether the desiccant unit can run during a given time period. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Process Air Inlet Node Name}\label{field-process-air-inlet-node-name}
+
+The name of the node entering the process side of the desiccant wheel.
+
+\paragraph{Field: Process Air Outlet Node Name}\label{field-process-air-outlet-node-name}
+
+The name of the node leaving the process side of the desiccant wheel.
+
+\paragraph{Field: Regeneration Air inlet Node Name}\label{field-regeneration-air-inlet-node-name}
+
+The name of the node entering the regeneration side of the desiccant wheel after the regeneration coil.
+
+\paragraph{Field: Regeneration Fan Inlet Node Name}\label{field-regeneration-fan-inlet-node-name}
+
+Node name for air entering the regeneration fan, mass flow is set by this desiccant dehumidifier model.
+
+\paragraph{Field: Control Type}\label{field-control-type-000}
+
+Type of setpoint control. Options are
+
+\begin{itemize}
+\item
+  LeavingMaximumHumidityRatioSetpoint
+\item
+  SystemNodeMaximumHumidityRatioSetpoint
+\end{itemize}
+
+\textbf{LeavingMaximumHumidityRatioSetpoint} means that the unit is controlled to deliver air at the \emph{Leaving Maximum Humidity Ratio Setpoint}, using bypass dampers to prevent overdrying.
+
+\textbf{SystemNodeMaximumHumidityRatioSetpoint} means that the unit is controlled to deliver air at the maximum humidity ratio setpoint (System Node Humidity Ratio Max) on the \emph{Process Air outlet node}, using bypass dampers to prevent overdrying. This setpoint must be established using a set point manager which sets the MaximumHumidityRatio control variable:
+
+\begin{itemize}
+\item
+  SetpointManager:SingleZone:Humidity:Maximum
+\item
+  SetpointManager:MultiZone:MaximumHumidity:Average
+\item
+  SetpointManager:MultiZone:Humidity:Maximum
+\end{itemize}
+
+This will also require the use of a \textbf{ZoneControl:Humidistat} object. If the dehumidifer is located in the outdoor air stream, it may also be necessary to use \textbf{SetpointManager:OutdoorAirPretreat}.
+
+\paragraph{Field: Leaving Maximum Humidity Ratio Setpoint}\label{field-leaving-maximum-humidity-ratio-setpoint}
+
+Fixed setpoint for maximum process air leaving humidity ratio. Applicable only when Control Type = LeavingMaximumHumidityRatioSetpoint.
+
+\paragraph{Field: Nominal Process Air Flow Rate}\label{field-nominal-process-air-flow-rate}
+
+Process air flow rate in m\(^{3}\)/s at nominal conditions. This field is autosizable.
+
+\paragraph{Field: Nominal Process Air Velocity}\label{field-nominal-process-air-velocity}
+
+Process air velocity in m/s at nominal flow. The default value is 3m/s.
+
+\paragraph{Field: Rotor Power}\label{field-rotor-power}
+
+Power input to wheel rotor motor in W. If this field is unknown, electricity consumption of the unit can be obtained from nominal power per unit air flow rate below.
+
+\paragraph{Field: Regeneration Coil Object Type}\label{field-regeneration-coil-object-type}
+
+Type of heating coil object for regeneration air. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the regeneration air heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Dehumidifier:Desiccant:NoFans) itself provides the ``controller'' function of modulating water flow. The valid choices are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Regeneration Coil Name}\label{field-regeneration-coil-name}
+
+Name of heating coil object for regeneration air.
+
+\paragraph{Field: Regeneration Fan Object Type}\label{field-regeneration-fan-object-type}
+
+Type of fan object for regeneration air. For UserCurves performance (see below) Fan:VariableVolume and Fan:ConstantVolume are valid. For Default performance (see below) only Fan:VariableVolume is valid.
+
+\paragraph{Field: Regeneration Fan Name}\label{field-regeneration-fan-name}
+
+Name of fan object for regeneration air.
+
+\paragraph{Field: Performance Model Type}\label{field-performance-model-type}
+
+Specifies whether the Default performance model or UserCurves curves should be used to model the performance. The default model is a generic solid desiccant wheel using performance curves of the form:
+
+curve = C1 + C2*edb + C3*edb**2 + C4*ew + C5*ew**2 + C6*vel + C7*vel**2 + C8*edb*ew + C9*edb**2*ew**2 + C10*edb*vel + C11*edb**2*vel**2 + C12*ew*vel + C13*ew**2*vel**2 + C14*ALOG(edb) + C15*ALOG(ew) + C16*ALOG(vel)
+
+edb = process entering drybulb temperature {[}C{]}\\
+ew = process entering humidity ratio {[}kgWater/kgDryAir{]}\\
+vel = process air velocity {[}m/s{]}
+
+The Default curves are valid for the following range of process inlet conditions: dry-bulb temperatures of 1.67C (35F) to 48.9C (120F) and humidity ratios of 0.002857 kgWater/kgDryAir (20 gr/lb) to 0.02857 kgWater/kgDryAir (200 gr/lb). If the process inlet conditions are outside this range, the dehumidifier will not operate.
+
+If UserCurves are specified, then performance is calculated as follows:
+
+Leaving Dry-bulb = (Leaving Dry-Bulb Function of Entering Dry-Bulb and Humidity Ratio Curve) * (Leaving Dry-Bulb Function of Air Velocity Curve)
+
+Leaving Humidity Ratio = (Leaving Humidity Ratio Function of Entering Dry-Bulb and Humidity Ratio Curve) * (Leaving Humidity Ratio Function of Air Velocity Curve)
+
+Regeneration Energy = (Regeneration Energy Function of Entering Dry-Bulb and Humidity Ratio Curve) * (Regeneration Energy Function of Air Velocity Curve)
+
+Regeneration Velocity = (Regeneration Velocity Function of Entering Dry-Bulb and Humidity Ratio Curve) * (Regeneration Velocity Function of Air Velocity Curve)
+
+The UserCurves are limited to the following range of process inlet conditions (essentially not limited): dry-bulb temperatures of 73.3C (-100F) to 65.6C (150F) and humidity ratios of 0.0 kgWater/kgDryAir (0 gr/lb) to 0.21273 kgWater/kgDryAir (1490 gr/lb). If the process inlet conditions are outside this range, the dehumidifier will not operate.
+
+When the Default performance model is selected, the remaining fields are ignored.
+
+\paragraph{Field: Leaving Dry-Bulb Function of Entering Dry-Bulb and Humidity Ratio Curve Name}\label{field-leaving-dry-bulb-function-of-entering-dry-bulb-and-humidity-ratio-curve-name}
+
+\emph{This field is applicable only when} UserCurves \emph{performance model type is specified.}
+
+Leaving dry-bulb of process air as a function of entering dry-bulb and entering humidity ratio, biquadratic curve.
+
+curve = C1 + C2*edb + C3*edb**2 + C4*ew + C5*ew**2 + C6*edb*ew
+
+edb = process entering drybulb temperature {[}C{]}
+
+ew = process entering humidity ratio {[}kgWater/kgDryAir{]}
+
+\paragraph{Field: Leaving Dry-Bulb Function of Air Velocity Curve Name}\label{field-leaving-dry-bulb-function-of-air-velocity-curve-name}
+
+\emph{This field is applicable only when} UserCurves \emph{performance model type is specified.}
+
+Leaving dry-bulb of process air as a function of air velocity, quadratic curve.
+
+curve = C1 + C2*v + C3*v**2
+
+v = process air velocity {[}m/s{]}
+
+\paragraph{Field: Leaving Humidity Ratio Function of Entering Dry-Bulb and Humidity Ratio Curve Name}\label{field-leaving-humidity-ratio-function-of-entering-dry-bulb-and-humidity-ratio-curve-name}
+
+\emph{This field is applicable only when} UserCurves \emph{performance model type is specified.}
+
+Leaving humidity ratio of process air as a function of entering dry-bulb and entering humidity ratio, biquadratic curve
+
+curve = C1 + C2*edb + C3*edb**2 + C4*ew + C5*ew**2 + C6*edb*ew
+
+edb = process entering drybulb temperature {[}C{]}
+
+ew = process entering humidity ratio {[}kgWater/kgDryAir{]}
+
+\paragraph{Field: Leaving Humidity Ratio Function of Air Velocity Curve Name}\label{field-leaving-humidity-ratio-function-of-air-velocity-curve-name}
+
+\emph{This field is applicable only when} UserCurves \emph{performance model type is specified.}
+
+Leaving humidity ratio of process air as a function of process air velocity, quadratic curve.
+
+curve = C1 + C2*v + C3*v**2
+
+v = process air velocity {[}m/s{]}
+
+\paragraph{Field: Regeneration Energy Function of Entering Dry-Bulb and Humidity Ratio Curve Name}\label{field-regeneration-energy-function-of-entering-dry-bulb-and-humidity-ratio-curve-name}
+
+\emph{This field is applicable only when} UserCurves \emph{performance model type is specified.}
+
+Regeneration energy {[}J/kg of water removed{]} as a function of entering dry-bulb and entering humidity ratio, biquadratic curve
+
+curve = C1 + C2*edb + C3*edb**2 + C4*ew + C5*ew**2 + C6*edb*ew
+
+edb = process entering drybulb temperature {[}C{]}
+
+ew = process entering humidity ratio {[}kgWater/kgDryAir{]}
+
+\paragraph{Field: Regeneration Energy Function of Air Velocity Curve Name}\label{field-regeneration-energy-function-of-air-velocity-curve-name}
+
+\emph{This field is applicable only when} UserCurves \emph{performance model type is specified.}
+
+Regeneration energy {[}J/kg of water removed{]} as a function of process air velocity, quadratic curve.
+
+curve = C1 + C2*v + C3*v**2
+
+v = process air velocity {[}m/s{]}
+
+\paragraph{Field: Regeneration Velocity Function of Entering Dry-Bulb and Humidity Ratio Curve Name}\label{field-regeneration-velocity-function-of-entering-dry-bulb-and-humidity-ratio-curve-name}
+
+\emph{This field is applicable only when} UserCurves \emph{performance model type is specified.}
+
+Regeneration velocity {[}m/s{]} as a function of entering dry-bulb and entering humidity ratio, biquadratic curve
+
+curve = C1 + C2*edb + C3*edb**2 + C4*ew + C5*ew**2 + C6*edb*ew
+
+edb = process entering drybulb temperature {[}C{]}
+
+ew = process entering humidity ratio {[}kgWater/kgDryAir{]}
+
+\paragraph{Field: Regeneration Velocity Function of Air Velocity Curve Name}\label{field-regeneration-velocity-function-of-air-velocity-curve-name}
+
+\emph{This field is applicable only when} UserCurves \emph{performance model type is specified.}
+
+Regeneration velocity {[}m/s{]} as a function of process air velocity, quadratic curve.
+
+curve = C1 + C2*v + C3*v**2
+
+v = process air velocity {[}m/s{]}
+
+\paragraph{Field: Nominal Regeneration Temperature}\label{field-nominal-regeneration-temperature}
+
+\emph{This field is applicable only when} UserCurves \emph{performance model type is specified.}
+
+Nominal regeneration temperature upon which the regeneration energy modifier curve is based. This input is ignored when Performance Model Type = Default, which assume a regeneration temperature of 121C.
+
+\paragraph{Field: Nominal Power Per Unit Air Flow Rate}\label{field-nominal-power-per-unit-air-flow-rate}
+
+This field is nominal power consumption per unit air flow rate. It is used to calculate electricity consumption of the unit when no rotor power is entered.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Dehumidifier:Desiccant:NoFans,
+  Desiccant 1,                         !- Name
+  FanAndCoilAvailSched,       !- Availability Schedule Name
+  Outside Air Inlet Node,   !- Process Air Inlet Node Name
+  Desiccant Process Outlet Node,   !- Process Air Outlet Node Name
+  Regen Coil Out Node,         !- Regeneration Air Inlet Node Name
+  Outside Air Inlet Node 2,!- Regeneration Fan Inlet Node Name
+  SystemNodeMaximumHumidityRatioSetpoint,   !- Control Type
+  0.007,                                     !- Leaving Maximum Humidity Ratio Setpoint {kgWater/kgDryAir}
+  1,                                             !- Nominal Process Air Flow Rate {m3/s}
+  2.5,                                         !- Nominal Process Air Velocity {m/s}
+  10,                                           !- Rotor Power {W}
+  Coil:Heating:Gas,               !- Regeneration Coil Object Type
+  Desiccant Regen Coil,       !- Regeneration Coil Name
+  Fan:VariableVolume,           !- Regeneration Fan Object Type
+  Desiccant Regen Fan,         !- Regeneration Fan Name
+  UserCurves,                           !- Performance Model Type
+  Desiccant DryBulb fTW Curve, !- Leaving Dry-Bulb Function of Entering Dry-Bulb and Humidity Ratio
+  !                                                 Curve Name
+  Desiccant DryBulb fV Curve,   !- Leaving Dry-Bulb Function of Air Velocity Curve Name
+  Desiccant HumRat fTW Curve,   !- Leaving Humidity Ratio Function of Entering Dry-Bulb and Humidity Ratio Curve Name
+  Desiccant HumRat fV Curve,     !- Leaving Humidity Ratio Function of Air Velocity Curve Name
+  Desiccant RegenEnergy fTW Curve, !- Regeneration Energy Function of Entering Dry-Bulb and Humidity Ratio Curve Name
+  Desiccant RegenEnergy fV Curve,   !- Regeneration Energy Function of Air Velocity Curve Name
+  Desiccant RegenVel fTW Curve,       !- Regeneration Velocity Function of Entering Dry-Bulb and Humidity Ratio Curve Name
+  Desiccant RegenVel fV Curve,         !- Regeneration Velocity Function of Air Velocity Curve Name
+  121,                                         !- Nominal Regeneration Temperature {C}
+  ;                                  !- Nominal Power Per Unit Air Flow Rate {W/m3/s}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-008}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Dehumidifier Removed Water Mass {[}kg{]}
+\item
+  HVAC,Average,Dehumidifier Removed Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Dehumidifier Part Load Ratio {[]}
+\item
+  HVAC,Average,Dehumidifier Electric Power {[}W{]}
+\item
+  HVAC,Sum,Dehumidifier Electric Energy {[}J{]}
+\item
+  HVAC,Average,Dehumidifier Regeneration Specific Energy {[}J/kgWater{]}
+\item
+  HVAC,Average,Dehumidifier Regeneration Rate {[}W{]}
+\item
+  HVAC,Sum,Dehumidifier Regeneration Energy {[}J{]}
+\item
+  HVAC,Average,Dehumidifier Regeneration Air Speed {[}m/s{]}
+\item
+  HVAC,Average,Dehumidifier Regeneration Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Dehumidifier Process Air Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Dehumidifier Removed Water Mass {[}kg{]}}\label{dehumidifier-removed-water-mass-kg}
+
+Mass of water removed from process air stream.
+
+\paragraph{Dehumidifier Removed Water Mass Flow Rate {[}kg/s{]}}\label{dehumidifier-removed-water-mass-flow-rate-kgs}
+
+Rate of water removal from process air stream.
+
+\paragraph{\texorpdfstring{Dehumidifier Part Load Ratio {[]}}{Dehumidifier Part Load Ratio }}\label{dehumidifier-part-load-ratio}
+
+Dehumidifier water removal rate divided by full-load water removal rate.
+
+\paragraph{Dehumidifier Electric Power {[}W{]}}\label{dehumidifier-electric-power-w}
+
+Dehumidifier rotor electric power.
+
+\paragraph{Dehumidifier Electric Energy {[}J{]}}\label{dehumidifier-electric-energy-j}
+
+Dehumidifier rotor electric energy.
+
+\paragraph{Dehumidifier Regeneration Specific Energy {[}J/kgWater{]}}\label{dehumidifier-regeneration-specific-energy-jkgwater}
+
+Regeneration heating coil energy divided by water removed.
+
+\paragraph{Dehumidifier Regeneration Rate {[}W{]}}\label{dehumidifier-regeneration-rate-w}
+
+Regeneration heating coil output rate.
+
+\paragraph{Dehumidifier Regeneration Energy {[}J{]}}\label{dehumidifier-regeneration-energy-j}
+
+Regeneration heating coil output energy.
+
+\paragraph{Dehumidifier Regeneration Air Speed{[}m/s{]}}\label{dehumidifier-regeneration-air-speedms}
+
+Regeneration air velocity.
+
+\paragraph{Dehumidifier Regeneration Air Mass Flow Rate {[}kg/s{]}}\label{dehumidifier-regeneration-air-mass-flow-rate-kgs}
+
+Regeneration air mass flow rate.
+
+\paragraph{Dehumidifier Process Air Mass Flow Rate {[}kg/s{]}}\label{dehumidifier-process-air-mass-flow-rate-kgs}
+
+Process air mass flow rate.
+
+\subsection{Dehumidifier:Desiccant:System}\label{dehumidifierdesiccantsystem}
+
+The Dehumidifier:Desiccant:System object models the dehumidification of an air stream, normally called the process air stream. A second heated air stream, called the regeneration air stream, is used to remove the collected moisture from the desiccant heat exchanger and this moisture-laden air is then usually exhausted from the building. This Dehumidifier:Desiccant:System object is similar to the Dehumidifier:Desiccant:NoFans object but has some additional modeling capabilities.
+
+The Dehumidifier:Desiccant:System object in EnergyPlus is a compound object that can be placed anywhere in an air loop (AirLoopHVAC). Common locations for this object are in an AirLoopHVAC:OutdoorAirSystem or in the main air loop (AirLoopHVAC) downstream of a cooling coil (postcooling desiccant dehumidifier). This compound object coordinates the operation of several children objects: a desiccant heat exchanger, a regeneration air fan, and an optional regeneration air heater. Gas, Electric, Steam, or Hot Water heating coils can be used for regenerator air heaters. If this dehumidifier is placed in the main air loop immediately downstream of a direct expansion (DX) cooling coil, then the dehumidifier s operation can be coordinated with the operation of the companion DX coil and it is also possible to specify that the DX system s condenser waste heat can be used to help regenerate the desiccant heat exchanger. For the case of condenser waste heat regeneration, an optional exhaust fan can also be modeled by this desiccant dehumidifier compound object to help maintain a set point temperature for air entering the regeneration side of the desiccant heat exchanger.
+
+It is important to note that the optional exhaust air fan is modeled internal to the Dehumidifier:Desiccant:System and a separate fan object should \emph{not} be added to the input data file (idf) for this fan. On the other hand, a separate fan object \emph{is} required in the input data file for the regeneration air fan.
+
+\begin{figure}[hbtp] % fig 141
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image409.png}
+\caption{Schematic of Dehumidifier:Desiccant:System with Draw Through Regeneration Fan Placement \protect \label{fig:schematic-of-dehumidifier-desiccant-system}}
+\end{figure}
+
+A schematic of the compound object Dehumidifier:Desiccant:Systemis shown in Figure~\ref{fig:schematic-of-dehumidifier-desiccant-system} with the draw through regeneration air fan placement. Figure~\ref{fig:schematic-of-dehumidifier-desiccant-system-001} shows the Dehumidifier:Desiccant:System object configured with the blow through regeneration air fan placement.
+
+NOTE: As with any air loop compound object, the Dehumidifier:Desiccant:System object itself is specified on the AirLoopHVAC Branch or in the AirLoopHVAC:OutdoorAirSystem:EquipmentList for an AirLoopHVAC:OutdoorAirSystem. The children objects (e.g., desiccant heat exchanger, regeneration air fan, and optional regeneration air heater) must be specified separately in the input data file and their inlet/outlet connections must be as shown in Figure~\ref{fig:schematic-of-dehumidifier-desiccant-system} or Figure~\ref{fig:schematic-of-dehumidifier-desiccant-system-001}.
+
+\begin{figure}[hbtp] % fig 142
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image410.png}
+\caption{Schematic of Dehumidifier:Desiccant:System with Blow Through Regeneration Fan Placement \protect \label{fig:schematic-of-dehumidifier-desiccant-system-001}}
+\end{figure}
+
+Currently the only heat exchanger choice for this object is HeatExchanger:Desiccant: BalancedFlow. So to model a Dehumidifier:Desiccant:System located in an air loop, the input data file should include the following objects:
+
+\begin{itemize}
+\item
+  Dehumidifier:Desiccant:System (in an air loop (AirLoopHVAC) Branch or AirLoopHVAC:OutdoorAirSystem:EquipmentList for an AirLoopHVAC:OutdoorAirSystem)
+\item
+  HeatExchanger:Desiccant:BalancedFlow (desiccant heat exchanger child object)
+\item
+  HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 (desiccant heat exchanger data object)
+\item
+  ZoneControl:Humidistat, and one of:
+\item
+  SetpointManager:SingleZone:Humidity:Maximum
+\item
+  SetpointManager:MultiZone:Humidity:Maximum
+\item
+  SetpointManager:MultiZone:MaximumHumidity:Average
+\item
+  (when in an air loop (AirLoopHVAC) Branch), and SetpointManager:OutdoorAirPretreat (when in an AirLoopHVAC:OutdoorAirSystem) to place a maximum humidity ratio set point on the sensor node, typically the process air outlet node
+\item
+  Fan:OnOff or Fan:ConstantVolume (regeneration air fan)
+\item
+  Coil:Heating:Electric or Coil:Heating:Gas (optional regeneration air heater)
+\item
+  Coil:Cooling:DX:SingleSpeed or Coil:Cooling:DX:TwoStageWithHumidityControlMode (optional companion cooling coil)
+\end{itemize}
+
+If the user wants to model the Dehumidifier:Desiccant:System in an AirLoopHVAC:OutdoorAirSystem, then the process air path of the dehumidifier should be located in the outdoor air stream and the regeneration air path may be placed in the relief air stream or modeled by the desiccant dehumidifier itself where the first node for the regeneration inlet air stream must be an outdoor air node. If the user wants to model the Dehumidifier:Desiccant:System in an air loop (AirLoopHVAC) Branch, then the process air path of the dehumidifier should be located in the air loop Branch object. For this case, the regeneration air stream is modeled by the desiccant dehumidifier object itself (i.e., not part of an air loop Branch statement) and the first node for the regeneration inlet air stream must be an outdoor air node (ref. Figure~\ref{fig:schematic-of-dehumidifier-desiccant-system} or Figure~\ref{fig:schematic-of-dehumidifier-desiccant-system-001}).
+
+A description of each input field for this object is provided below:
+
+\subsubsection{Inputs}\label{inputs-1-010}
+
+\paragraph{Field: Name}\label{field-name-1-009}
+
+A unique, user-assigned name for a particular Dehumidifier:Desiccant:System. Any reference to this dehumidifier by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-002}
+
+The name of the schedule (ref: Schedule) that denotes whether the dehumidifier can operate during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the dehumidifier can operate. A value less than or equal to 0 (usually 0 is used) denotes that the dehumidifier will not operate (i.e., no heat exchange will take place and the regeneration air fan does not operate). If the field is blank, the schedule has a value of 1 for all time periods. For the case where companion cooling coil regeneration air heating has been specified, the desiccant dehumidifier s exhaust fan serves as the condenser air fan for the cooling coil system so this availability schedule will not disable exhaust fan operation.
+
+\paragraph{Field: Desiccant Heat Exchanger Object Type}\label{field-desiccant-heat-exchanger-object-type}
+
+This alpha field contains the type of desiccant heat exchanger used with this dehumidifier. Currently, the only valid choice is HeatExchanger:Desiccant:BalancedFlow.
+
+\paragraph{Field: Desiccant Heat Exchanger Name}\label{field-desiccant-heat-exchanger-name}
+
+This alpha field contains the name of the desiccant heat exchanger used with this dehumidifier.
+
+\paragraph{Field: Sensor Node Name}\label{field-sensor-node-name-000}
+
+This alpha field specifies the name of the air loop node used to control desiccant heat exchanger operation. A set point manager must be used to place a maximum humidity ratio set point on this node (e.g., SetpointManager:SingleZone:Humidity:Maximum or SetpointManager:OutdoorAirPretreat).
+
+\paragraph{Field: Regeneration Air Fan Object Type}\label{field-regeneration-air-fan-object-type}
+
+This alpha field contains the type of regeneration air fan used. Available fan types are Fan:OnOff and Fan:ConstantVolume.
+
+\paragraph{Field: Regeneration Air Fan Name}\label{field-regeneration-air-fan-name}
+
+This alpha field contains the name of the regeneration air fan used with this dehumidifier.
+
+\paragraph{Field: Regeneration Air Fan Placement}\label{field-regeneration-air-fan-placement}
+
+This alpha field specifies the fan configuration used in the desiccant dehumidifier. Valid choices are BlowThrough and DrawThrough , with a default of DrawThrough if this field is left blank.
+
+\paragraph{Field: Regeneration Air Heater Object Type}\label{field-regeneration-air-heater-object-type}
+
+This alpha field contains the type of heating coil used to heat the regeneration air stream. This field may be left blank when no regeneration air heater is required. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the regeneration air heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Dehumidifier:Desiccant:System) itself provides the ``controller'' function of modulating water flow. For autosizing regeneration air heating coil the \emph{Design Coil Inlet Air Condition} used is the outdoor air condition if the desiccant system is on the primary air loop, or else if the desiccant system is on outdoor air system then it is the return air condition. The \emph{Design Coil Outlet Air Temperature} is the \emph{Regeneration Inlet Air Setpoint Temperature} specified in the input field below. Valid heating coil choices are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Regeneration Air Heater Name}\label{field-regeneration-air-heater-name}
+
+This alpha field contains the name of the heating coil used to heat the regeneration air stream. This field may be left blank when no regeneration air heater is required.
+
+\paragraph{Field: Regeneration Inlet Air Setpoint Temperature}\label{field-regeneration-inlet-air-setpoint-temperature}
+
+This optional numeric field specifies the regeneration air inlet temperature setpoint in Celsius. The regeneration air heater and/or the companion coil regeneration air heating will be controlled to this temperature to the extent possible. This field may be left blank when no regeneration air heater is required or when control of the exhaust fan used with the companion coil regeneration air heating option is not required. If regeneration air heating coils is autosized, then the value of this input field is used as the \emph{Regeneration Air Heater Design Outlet Air Temperature} for the coil sizing calculation. The default value is 46.0 degrees.
+
+\paragraph{Field: Companion Cooling Coil Object Type}\label{field-companion-cooling-coil-object-type}
+
+This optional alpha field contains the type of companion cooling coil used with this desiccant dehumidifier. The only valid choices are Coil:Cooling:DX:SingleSpeed and Coil:Cooling:DX:TwoStageWithHumidityControlMode.
+
+\paragraph{Field: Companion Cooling Coil Name}\label{field-companion-cooling-coil-name}
+
+This optional alpha field contains the name of the companion cooling coil used with this desiccant dehumidifier. This field may be left blank when no companion cooling coil is being modeled.
+
+\paragraph{Field: Companion Cooling Coil Upstream of Dehumidifier Process Inlet}\label{field-companion-cooling-coil-upstream-of-dehumidifier-process-inlet}
+
+This choice field specifies if the companion cooling coil is located immediately upstream of the dehumidifiers process inlet. Valid choices are Yes and No. If Yes is selected, then the outlet air node for the companion cooling coil must be the same as the dehumidifier s process air inlet node (i.e., the process air inlet node name for the desiccant heat exchanger specified for this desiccant dehumidifier). For this case, the companion cooling coil and the desiccant dehumidifier are assumed to operate in tandem ; that is, if the simulation determines that the companion cooling coil is unable to meet the humidity set point specified on the sensor node based on its own operation, then the desiccant dehumidifier operates at the same time and for the same duration as the cooling coil to provide improved dehumidification. If No is selected, then the dehumidifier will control to the humidity set point specified on the sensor node to the extent possible. The default value is No if this field is left blank.
+
+\paragraph{Field: Companion Coil Regeneration Air Heating}\label{field-companion-coil-regeneration-air-heating}
+
+This choice field determines if the companion cooling coil s condenser waste heat is used to heat the regeneration inlet air. Valid choices are Yes and No. The default value is No if this field is left blank.
+
+\paragraph{Field: Exhaust Fan Maximum Flow Rate}\label{field-exhaust-fan-maximum-flow-rate}
+
+This optional numeric field contains the maximum fan volumetric flow rate for the exhaust fan in cubic meters per second. As noted previously, this exhaust fan is modeled internally by the Dehumidifier:Desiccant:System object and a separate fan object should NOT be specified in the input data file for this fan. This field is used only when a companion cooling coil is specified and the Companion Coil Regeneration Air Heating field is set to Yes . This field must be used in conjunction with the Exhaust Fan Maximum Power and the Exhaust Fan Power Curve Name input fields. The model assumes that the exhaust fan will operate as needed to maintain the Regeneration Inlet Air Setpoint Temperature , up to the maximum flow rate specified in this input field. If the desiccant dehumidifier is OFF for a simulation timestep but its companion cooling coil is operating and is specified to provide regeneration air heating, then the exhaust fan operates at this maximum air flow rate (i.e., this fan serves as the condenser fan for the companion cooling coil system when regeneration air heating is specified, so the inputs to the companion cooling coil object should not include the condenser fan energy since the condenser fan energy is modeled by the Dehumidifier:Desiccant:System object).
+
+\paragraph{Field: Exhaust Fan Maximum Power}\label{field-exhaust-fan-maximum-power}
+
+This optional numeric field contains the maximum power for the exhaust fan in Watts (i.e., at the Exhaust Fan Maximum Flow Rate). This field is used only when a companion cooling coil is used and the Companion Coil Regeneration Air Heating field is set to Yes . This field must be used in conjunction with the Exhaust Fan Maximum Flow Rate and the Exhaust Fan Power Curve Name input fields.
+
+\paragraph{Field: Exhaust Fan Power Curve Name}\label{field-exhaust-fan-power-curve-name}
+
+This optional alpha field contains the name of the exhaust fan power modifier curve. This field is used only when a companion cooling coil is used and the Companion Coil Regeneration Air Heating field is set to Yes . This field must be used in conjunction with the Exhaust Fan Maximum Flow Rate and the Exhaust Fan Maximum Power input fields. If this field is blank, the exhaust fan operates (when required) at the maximum power specified in the field above. The curve object type for this Exhaust Fan Power Curve Name must be Curve:Cubic or Curve:Quadratic. The curve object (Curve:Cubic or Curve:Quadratic) defines the change in exhaust fan power as a function of the ratio of the actual exhaust air flow rate divided by the maximum flow rate.
+
+Following is an example input for this object:
+
+\begin{lstlisting}
+
+Dehumidifier:Desiccant:System,
+  Desiccant 1,                         !- Name
+  FanAvailSched,                     !- Availability Schedule Name
+  HeatExchanger:Desiccant:BalancedFlow,   !- Desiccant Heat Exchanger Object Type
+  Desiccant Heat Exchanger 1,   !- Desiccant Heat Exchanger Name
+  HX Process Outlet Node,   !- Sensor Node Name
+  Fan:ConstantVolume,           !- Regeneration Air Fan Object Type
+  Desiccant Regen Fan,         !- Regeneration Air Fan Name
+  DrawThrough,                         !- Regeneration Air Fan Placement
+  Coil:Heating:Gas,               !- Regeneration Air Heater Object Type
+  Desiccant Regen Coil,       !- Regeneration Air Heater Name
+  46.111111,                             !- Regeneration Inlet Air Setpoint Temperature {C}
+  Coil:Cooling:DX:SingleSpeed,   !- Companion Cooling Coil Object Type
+  Desiccant DXSystem Cooling Coil,   !- Companion Cooling Coil Name
+  Yes,                           !- Companion Cooling Coil Upstream of Dehumidifier Process Inlet
+  Yes,                                         !- Companion Coil Regeneration Air Heating
+  1.05,                                       !- Exhaust Fan Maximum Flow Rate {m3/s}
+  50,                                           !- Exhaust Fan Maximum Power {W}
+  EXHAUSTFANPLF;                     !- Exhaust Fan Power Curve Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-006}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Dehumidifier Removed Water Mass {[}kg{]}
+\item
+  HVAC,Average,Dehumidifier Removed Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Dehumidifier Part Load Ratio {[]}
+\item
+  HVAC,Average,Dehumidifier Exhaust Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Dehumidifier Exhaust Fan Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Dehumidifier Removed Water Mass {[}kg{]}}\label{dehumidifier-removed-water-mass-kg-1}
+
+This output is the mass of water removed from the process air stream in kilograms for the timestep being reported.
+
+\paragraph{Dehumidifier Removed Water Mass Flow Rate {[}kg/s{]}}\label{dehumidifier-removed-water-mass-flow-rate-kgs-1}
+
+This output is the average rate of water removal from the process air stream in kilograms per second for the timestep being reported.
+
+\paragraph{\texorpdfstring{Dehumidifier Part Load Ratio {[]}}{Dehumidifier Part Load Ratio }}\label{dehumidifier-part-load-ratio-1}
+
+This output is the fraction of time that the desiccant heat exchanger (and associated regeneration air heater and fans, if appropriate) operate for the timestep being reported.
+
+\paragraph{Dehumidifier Exhaust Fan Electric Power {[}W{]}}\label{dehumidifier-exhaust-fan-electric-power-w}
+
+This output is the average electric consumption rate for the exhaust fan in Watts for the timestep being reported.
+
+\paragraph{Dehumidifier Exhaust Fan Electric Energy {[}J{]}}\label{dehumidifier-exhaust-fan-electric-energy-j}
+
+This output is the electric consumption for the exhaust fan in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, EndUseKey = Cooling, GroupKey = System (ref. Output:Meter objects).
diff --git a/doc/input-output-reference/src/overview/group-design-objects.tex b/doc/input-output-reference/src/overview/group-design-objects.tex
new file mode 100644
index 00000000000..035d4731c9b
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-design-objects.tex
@@ -0,0 +1,1748 @@
+\section{Group -- Design Objects}\label{group-design-objects}
+
+\subsection{Input for Design Calculations and Component Autosizing}\label{input-for-design-calculations-and-component-autosizing}
+
+\subsubsection{Overview}\label{overview-000}
+
+In order for EnergyPlus to successfully calculate zone design heating and cooling loads and air flow rates and for the program to use these results to automatically size the HVAC components a number of input objects must be present and certain object input fields must be entered.
+
+\begin{itemize}
+\item
+  The input file should contain a SimulationControl object. The 1\(^{st}\) field \emph{Do Zone Sizing Calculation} should be entered as \emph{Yes}. This will cause a zone sizing simulation to be done using all the sizing periods in the input file as weather. If there are no air or water loops in the HVAC input fields 2 and 3 can be set to \emph{No.} If there are one or more air loops (i.e., there is at least one AirLoopHVAC object in the input file) then the 2\(^{nd}\) field \emph{Do System Sizing Calculation} should be entered as \emph{Yes}. If there are one or more water loops (Plant Loop objects) then the 3\(^{rd}\) field \emph{Do Plant Sizing Calculation} should be set to \emph{Yes}. Finally either the 4\(^{th}\) field (\emph{Run Simulation for Sizing Periods}) or the 5\(^{th}\) field (\emph{Run Simulation for Weather File Run Periods}) should be set to \emph{Yes} in order to autosize the components and do a real simulation using the autosized components. The component autosizing calculations are done on the first pass through the HVAC system in the real simulation.
+\item
+  There must be at least 2 (up to any number) SizingPeriod objects present. Normally one will be for summer conditions and one for winter. The summer day should normally have the field \emph{Day Type} set to \emph{SummerDesignDay}. The winter design day should normally have \emph{Day Type} set to \emph{WinterDesignDay}.
+\item
+  To apply a global sizing factor include the Sizing:Parameters object.
+\item
+  For each controlled zone in the input file there should be a corresponding Sizing:Zone object. Similarly for each AirLoopHVAC there should be a Sizing:System object. And for each Plant or Condenser Loop there should be a Sizing:Plant object. Note however that if a controlled zone has no corresponding Zone Sizing object the data from the first Zone Sizing object will be used. Thus if all the zone sizing information is the same only one Zone Sizing object need be entered.
+\item
+  Only controlled zones are included in the zone and system sizing calculations. Thus for a design air flow rate to be calculated for a zone, it must contain a thermostat \emph{even though it might not need or have a thermostat in the full simulation}. An illustration would be a three zone building with a packaged single zone system and a thermostat in one of the zones. In order for the two slave zones to be included in the design air flow calculations they must be treated as if they have a thermostat: there must be a ZoneControl:Thermostat for each of the slave zones.
+\item
+  Some attention should be paid to schedules. In a weekly schedule object the 9\(^{th}\) and 10\(^{th}\) day schedules are for summer and winter design days respectively. This means that if a SizingPeriod object has field \emph{Day Type} set to \emph{SummerDesignDay} ~the day schedule for summer sizing periods will be in effect. Similarly if a SizingPeriod object has field \emph{Day Type} set to \emph{WinterDesignDay} ~the day schedule for winter sizing periods will be in effect. Some possible applications of this capability are:
+\end{itemize}
+
+1)~~~setting internal loads (lights, equipment, occupancy) to maximum all day for cooling and to zero all day for heating;
+
+2)~~~setting heating and cooling thermostat set points to constant values (no set up or set back);
+
+3)~~~setting heating and cooling equipment to be always on.
+
+None of these applications are necessarily recommended but these and other uses of the special summer/winter design day schedules may prove useful for specific situations.
+
+\begin{itemize}
+\item
+  Other than zone thermostat setpoints, the sizing calculations generally know nothing about the system control inputs such as setpoints and availability schedules. The user must coordinate sizing inputs with the actual simulation control inputs.
+\item
+  The sizing calculations only recognize the presence of central heating and cooling coils, preheat and precool coils and reheat coils. These are assumed to deliver the various supply temperatures specified in the Sizing:System and Sizing:Zone objects. The impact of other components such as heat recovery, dehumidifiers, and pumps are not accounted for in the sizing calculations. Central supply and return fan temperature rise is taken into account in sizing the central cooling coils.
+\end{itemize}
+
+\subsubsection{Component Autosizing}\label{component-autosizing}
+
+For autosizing to occur at the component level the user must enter the special value \emph{autosize} in the numeric fields for which autosizing is available. Those fields can be found by looking at the Energy+.idd data dictionary file or under individual object details in this document. Fields that can be autosized are denoted with the comment \emph{\textbackslash{}autosizable}. The components and fields that are autosizable are listed in the following table. Note that spaces may be inserted in object names to facilitate readability.
+
+% table 22
+\begin{longtable}[c]{p{2.75in}p{3.24in}}
+\caption{Details of Autosizable Objects/Fields \label{table:details-of-autosizable-objectsfields}} \tabularnewline
+\toprule 
+Component / Object Name & Autosizable Fields \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Details of Autosizable Objects/Fields} \tabularnewline
+\toprule 
+Component / Object Name & Autosizable Fields \tabularnewline
+\midrule
+\endhead
+
+AirConditioner:VariableRefrigerantFlow \tabularnewline
+ & Gross Rated Total Cooling Capacity \tabularnewline
+ & Gross Rated Heating Capacity \tabularnewline
+ & Resistive Defrost Heater Capacity \tabularnewline
+ & Water Condenser Volume Flow Rate \tabularnewline
+ & Evaporative Condenser Air Flow Rate \tabularnewline
+ & Evaporative Condenser Pump Rated Power Consumption \tabularnewline
+AirLoopHVAC \tabularnewline
+ & Design Supply Air Flow Rate \tabularnewline
+AirLoopHVAC:Unitary:Furnace:HeatCool \tabularnewline
+ & Maximum Supply Air Temperature \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+AirLoopHVAC:Unitary:Furnace:HeatOnly \tabularnewline
+ & Maximum Supply Air Temperature \tabularnewline
+ & Supply Air Flow Rate \tabularnewline
+AirLoopHVAC:UnitaryHeatCool \tabularnewline
+ & Maximum Supply Air Temperature \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass \tabularnewline
+ & Cooling System Air Flow Rate \tabularnewline
+ & Heating System Air Flow Rate \tabularnewline
+ & No Load System Air Flow Rate \tabularnewline
+ & Cooling Outdoor Air Flow Rate \tabularnewline
+ & Heating Outdoor Air Flow Rate \tabularnewline
+ & No Load Outdoor Air Flow Rate \tabularnewline
+AirLoopHVAC:UnitaryHeatOnly \tabularnewline
+ & Maximum Supply Air Temperature \tabularnewline
+ & Supply Air Flow Rate \tabularnewline
+AirLoopHVAC:UnitaryHeatPump:AirToAir \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & Maximum Supply Air Temperature from Supplemental Heater \tabularnewline
+AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed \tabularnewline
+ & Maximum Supply Air Temperature from Supplemental Heater \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & Heating Speed 1 Supply Air Flow Rate \tabularnewline
+ & Heating Speed 2 Supply Air Flow Rate \tabularnewline
+ & Heating Speed 3 Supply Air Flow Rate \tabularnewline
+ & Heating Speed 4 Supply Air Flow Rate \tabularnewline
+ & Cooling Speed 1 Supply Air Flow Rate \tabularnewline
+ & Cooling Speed 2 Supply Air Flow Rate \tabularnewline
+ & Cooling Speed 3 Supply Air Flow Rate \tabularnewline
+ & Cooling Speed 4 Supply Air Flow Rate \tabularnewline
+AirLoopHVAC:UnitaryHeatPump:WaterToAir \tabularnewline
+ & Supply Air Flow Rate \tabularnewline
+ & Maximum Supply Air Temperature from Supplemental Heater \tabularnewline
+AirLoopHVAC:UnitarySystem \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & Maximum Supply Air Temperature \tabularnewline
+AirTerminal:DualDuct:ConstantVolume \tabularnewline
+ & Maximum Air Flow Rate \tabularnewline
+AirTerminal:DualDuct:VAV \tabularnewline
+ & Maximum Damper Air Flow Rate \tabularnewline
+AirTerminal:DualDuct:VAV:OutdoorAir \tabularnewline
+ & Maximum Terminal Air Flow Rate \tabularnewline
+AirTerminal:SingleDuct:ConstantVolume:CooledBeam \tabularnewline
+ & Supply Air Volumetric Flow Rate \tabularnewline
+ & Maximum Total Chilled Water Volumetric Flow Rate \tabularnewline
+ & Number of Beams \tabularnewline
+ & Beam Length \tabularnewline
+AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction \tabularnewline
+ & Maximum Total Air Flow Rate \tabularnewline
+ & Maximum Hot Water Flow Rate \tabularnewline
+ & Maximum Cold Water Flow Rate \tabularnewline
+AirTerminal:SingleDuct:ConstantVolume:Reheat \tabularnewline
+ & Maximum Air Flow Rate \tabularnewline
+ & Maximum Hot Water or Steam Flow Rate \tabularnewline
+AirTerminal:SingleDuct:ParallelPIU:Reheat \tabularnewline
+ & Maximum Primary Air Flow Rate \tabularnewline
+ & Maximum Secondary Air Flow Rate \tabularnewline
+ & Minimum Primary Air Flow Fraction \tabularnewline
+ & Fan On Flow Fraction \tabularnewline
+ & Maximum Hot Water or Steam Flow Rate \tabularnewline
+AirTerminal:SingleDuct:SeriesPIU:Reheat \tabularnewline
+ & Maximum Air Flow Rate \tabularnewline
+ & Maximum Primary Air Flow Rate \tabularnewline
+ & Minimum Primary Air Flow Fraction \tabularnewline
+ & Maximum Hot Water or Steam Flow Rate \tabularnewline
+AirTerminal:SingleDuct:Uncontrolled \tabularnewline
+ & Maximum Air Flow Rate \tabularnewline
+AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat \tabularnewline
+ & Maximum Air Flow Rate \tabularnewline
+AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat \tabularnewline
+ & Maximum Air Flow Rate \tabularnewline
+ & Maximum Hot Water or Steam Flow Rate \tabularnewline
+AirTerminal:SingleDuct:VAV:NoReheat \tabularnewline
+ & Maximum Air Flow Rate \tabularnewline
+AirTerminal:SingleDuct:VAV:Reheat \tabularnewline
+ & Maximum Air Flow Rate \tabularnewline
+ & Maximum Hot Water or Steam Flow Rate \tabularnewline
+AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan \tabularnewline
+ & Maximum Cooling Air Flow Rate \tabularnewline
+ & Maximum Heating Air Flow Rate \tabularnewline
+ & Maximum Hot Water or Steam Flow Rate \tabularnewline
+Boiler:HotWater \tabularnewline
+ & Nominal Capacity \tabularnewline
+ & Design Water Flow Rate \tabularnewline
+Boiler:Steam \tabularnewline
+ & Nominal Capacity \tabularnewline
+Branch \tabularnewline
+ & Maximum Flow Rate \tabularnewline
+Chiller:Absorption \tabularnewline
+ & Nominal Capacity \tabularnewline
+ & Nominal Pumping Power \tabularnewline
+ & Design Chilled Water Flow Rate \tabularnewline
+ & Design Condenser Water Flow Rate \tabularnewline
+ & Design Generator Fluid Flow Rate \tabularnewline
+Chiller:Absorption:Indirect \tabularnewline
+ & Nominal Capacity \tabularnewline
+ & Nominal Pumping Power \tabularnewline
+ & Design Chilled Water Flow Rate \tabularnewline
+ & Design Condenser Water Flow Rate \tabularnewline
+ & Design Generator Fluid Flow Rate \tabularnewline
+Chiller:CombustionTurbine \tabularnewline
+ & Nominal Capacity \tabularnewline
+ & Design Chilled Water Flow Rate \tabularnewline
+ & Design Condenser Water Flow Rate \tabularnewline
+ & Gas Turbine Engine Capacity \tabularnewline
+Chiller:ConstantCOP \tabularnewline
+ & Nominal Capacity \tabularnewline
+ & Design Chilled Water Flow Rate \tabularnewline
+ & Design Condenser Water Flow Rate \tabularnewline
+Chiller:Electric \tabularnewline
+ & Nominal Capacity \tabularnewline
+ & Design Chilled Water Flow Rate \tabularnewline
+ & Design Condenser Fluid Flow Rate \tabularnewline
+ & Design Heat Recovery Water Flow Rate \tabularnewline
+Chiller:Electric:EIR \tabularnewline
+ & Reference Capacity \tabularnewline
+ & Reference Chilled Water Flow Rate \tabularnewline
+ & Reference Condenser Fluid Flow Rate \tabularnewline
+ & Design Heat Recovery Water Flow Rate \tabularnewline
+Chiller:Electric:ReformulatedEIR \tabularnewline
+ & Reference Capacity \tabularnewline
+ & Reference Chilled Water Flow Rate \tabularnewline
+ & Reference Condenser Water Flow Rate \tabularnewline
+ & Design Heat Recovery Water Flow Rate \tabularnewline
+Chiller:EngineDriven \tabularnewline
+ & Nominal Capacity \tabularnewline
+ & Design Chilled Water Flow Rate \tabularnewline
+ & Design Condenser Water Flow Rate \tabularnewline
+ChillerHeater:Absorption:DirectFired \tabularnewline
+ & Nominal Cooling Capacity \tabularnewline
+ & Design Chilled Water Flow Rate \tabularnewline
+ & Design Condenser Water Flow Rate \tabularnewline
+ & Design Hot Water Flow Rate \tabularnewline
+ChillerHeater:Absorption:DoubleEffect \tabularnewline
+ & Nominal Cooling Capacity \tabularnewline
+ & Design Chilled Water Flow Rate \tabularnewline
+ & Design Condenser Water Flow Rate \tabularnewline
+ & Design Hot Water Flow Rate \tabularnewline
+ChillerHeaterPerformance:Electric:EIR \tabularnewline
+ & Reference Cooling Mode Evaporator Capacity \tabularnewline
+ & Design Chilled Water Flow Rate \tabularnewline
+ & Design Condenser Water Flow Rate \tabularnewline
+Coil:Cooling:DX:MultiSpeed \tabularnewline
+ & Speed 1 Gross Rated Total Cooling Capacity \tabularnewline
+ & Speed 1 Gross Rated Sensible Heat Ratio \tabularnewline
+ & Speed 1 Rated Air Flow Rate \tabularnewline
+ & Speed 1 Evaporative Condenser Air Flow Rate \tabularnewline
+ & Speed 1 Rated Evaporative Condenser Pump Power Consumption \tabularnewline
+ & Speed 2 Gross Rated Total Cooling Capacity \tabularnewline
+ & Speed 2 Gross Rated Sensible Heat Ratio \tabularnewline
+ & Speed 2 Rated Air Flow Rate \tabularnewline
+ & Speed 2 Evaporative Condenser Air Flow Rate \tabularnewline
+ & Speed 2 Rated Evaporative Condenser Pump Power Consumption \tabularnewline
+ & Speed 3 Gross Rated Total Cooling Capacity \tabularnewline
+ & Speed 3 Gross Rated Sensible Heat Ratio \tabularnewline
+ & Speed 3 Rated Air Flow Rate \tabularnewline
+ & Speed 3 Evaporative Condenser Air Flow Rate \tabularnewline
+ & Speed 3 Rated Evaporative Condenser Pump Power Consumption \tabularnewline
+ & Speed 4 Gross Rated Total Cooling Capacity \tabularnewline
+ & Speed 4 Gross Rated Sensible Heat Ratio \tabularnewline
+ & Speed 4 Rated Air Flow Rate \tabularnewline
+ & Speed 4 Evaporative Condenser Air Flow Rate \tabularnewline
+ & Speed 4 Rated Evaporative Condenser Pump Power Consumption \tabularnewline
+Coil:Cooling:DX:SingleSpeed \tabularnewline
+ & Gross Rated Total Cooling Capacity \tabularnewline
+ & Gross Rated Sensible Heat Ratio \tabularnewline
+ & Rated Air Flow Rate \tabularnewline
+ & Evaporative Condenser Air Flow Rate \tabularnewline
+ & Evaporative Condenser Pump Rated Power Consumption \tabularnewline
+Coil:Cooling:DX:SingleSpeed:ThermalStorage \tabularnewline
+ & Rated Evaporator Air Flow Rate \tabularnewline
+ & Cooling Only Mode Rated Total Evaporator Cooling Capacity \tabularnewline
+ & Evaporative Condenser Pump Rated Power Consumption \tabularnewline
+Coil:Cooling:DX:TwoSpeed \tabularnewline
+ & High Speed Gross Rated Total Cooling Capacity \tabularnewline
+ & High Speed Rated Sensible Heat Ratio \tabularnewline
+ & High Speed Rated Air Flow Rate \tabularnewline
+ & Low Speed Gross Rated Total Cooling Capacity \tabularnewline
+ & Low Speed Gross Rated Sensible Heat Ratio \tabularnewline
+ & Low Speed Rated Air Flow Rate \tabularnewline
+ & High Speed Evaporative Condenser Air Flow Rate \tabularnewline
+ & High Speed Evaporative Condenser Pump Rated Power Consumption \tabularnewline
+ & Low Speed Evaporative Condenser Air Flow Rate \tabularnewline
+ & Low Speed Evaporative Condenser Pump Rated Power Consumption \tabularnewline
+Coil:Cooling:DX:VariableRefrigerantFlow \tabularnewline
+ & Gross Rated Total Cooling Capacity \tabularnewline
+ & Gross Rated Sensible Heat Ratio \tabularnewline
+ & Rated Air Flow Rate \tabularnewline
+Coil:Cooling:DX:VariableSpeed \tabularnewline
+ & Gross Rated Total Cooling Capacity At Selected Nominal Speed Level \tabularnewline
+ & Rated Air Flow Rate At Selected Nominal Speed Level \tabularnewline
+ & Evaporative Condenser Pump Rated Power Consumption \tabularnewline
+Coil:Cooling:Water \tabularnewline
+ & Design Water Flow Rate \tabularnewline
+ & Design Air Flow Rate \tabularnewline
+ & Design Inlet Water Temperature \tabularnewline
+ & Design Inlet Air Temperature \tabularnewline
+ & Design Outlet Air Temperature \tabularnewline
+ & Design Inlet Air Humidity Ratio \tabularnewline
+ & Design Outlet Air Humidity Ratio \tabularnewline
+Coil:Cooling:Water:DetailedGeometry \tabularnewline
+ & Maximum Water Flow Rate \tabularnewline
+ & Tube Outside Surface Area \tabularnewline
+ & Total Tube Inside Area \tabularnewline
+ & Fin Surface Area \tabularnewline
+ & Minimum Airflow Area \tabularnewline
+ & Coil Depth \tabularnewline
+ & Fin Diameter \tabularnewline
+ & Number of Tubes per Row \tabularnewline
+Coil:Cooling:WaterToAirHeatPump:EquationFit \tabularnewline
+ & Rated Air Flow Rate \tabularnewline
+ & Rated Water Flow Rate \tabularnewline
+ & Gross Rated Total Cooling Capacity \tabularnewline
+ & Gross Rated Sensible Cooling Capacity \tabularnewline
+Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit \tabularnewline
+ & Gross Rated Total Cooling Capacity At Selected Nominal Speed Level \tabularnewline
+ & Rated Air Flow Rate At Selected Nominal Speed Level \tabularnewline
+ & Rated Water Flow Rate At Selected Nominal Speed Level \tabularnewline
+Coil:Heating:DX:MultiSpeed \tabularnewline
+ & Resistive Defrost Heater Capacity \tabularnewline
+ & Speed 1 Gross Rated Heating Capacity \tabularnewline
+ & Speed 1 Rated Air Flow Rate \tabularnewline
+ & Speed 2 Gross Rated Heating Capacity \tabularnewline
+ & Speed 2 Rated Air Flow Rate \tabularnewline
+ & Speed 3 Gross Rated Heating Capacity \tabularnewline
+ & Speed 3 Rated Air Flow Rate \tabularnewline
+ & Speed 4 Gross Rated Heating Capacity \tabularnewline
+ & Speed 4 Rated Air Flow Rate \tabularnewline
+Coil:Heating:DX:SingleSpeed \tabularnewline
+ & Gross Rated Heating Capacity \tabularnewline
+ & Rated Air Flow Rate \tabularnewline
+ & Resistive Defrost Heater Capacity \tabularnewline
+Coil:Heating:DX:VariableRefrigerantFlow \tabularnewline
+ & Gross Rated Heating Capacity \tabularnewline
+ & Rated Air Flow Rate \tabularnewline
+Coil:Heating:DX:VariableSpeed \tabularnewline
+ & Rated Heating Capacity At Selected Nominal Speed Level \tabularnewline
+ & Rated Air Flow Rate At Selected Nominal Speed Level \tabularnewline
+ & Resistive Defrost Heater Capacity \tabularnewline
+Coil:Heating:Electric \tabularnewline
+ & Nominal Capacity \tabularnewline
+Coil:Heating:Electric:MultiStage \tabularnewline
+ & Stage 1 Nominal Capacity \tabularnewline
+ & Stage 2 Nominal Capacity \tabularnewline
+ & Stage 3 Nominal Capacity \tabularnewline
+ & Stage 4 Nominal Capacity \tabularnewline
+Coil:Heating:Gas \tabularnewline
+ & Nominal Capacity \tabularnewline
+Coil:Heating:Gas:MultiStage \tabularnewline
+ & Stage 1 Nominal Capacity \tabularnewline
+ & Stage 2 Nominal Capacity \tabularnewline
+ & Stage 3 Nominal Capacity \tabularnewline
+ & Stage 4 Nominal Capacity \tabularnewline
+Coil:Heating:Steam \tabularnewline
+ & Maximum Steam Flow Rate \tabularnewline
+Coil:Heating:Water \tabularnewline
+ & U-Factor Times Area Value \tabularnewline
+ & Maximum Water Flow Rate \tabularnewline
+ & Rated Capacity \tabularnewline
+Coil:Heating:WaterToAirHeatPump:EquationFit \tabularnewline
+ & Rated Air Flow Rate \tabularnewline
+ & Rated Water Flow Rate \tabularnewline
+ & Gross Rated Heating Capacity \tabularnewline
+Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit \tabularnewline
+ & Rated Heating Capacity At Selected Nominal Speed Level \tabularnewline
+ & Rated Air Flow Rate At Selected Nominal Speed Level \tabularnewline
+ & Rated Water Flow Rate At Selected Nominal Speed Level \tabularnewline
+CoilPerformance:DX:Cooling \tabularnewline
+ & Gross Rated Total Cooling Capacity \tabularnewline
+ & Gross Rated Sensible Heat Ratio \tabularnewline
+ & Rated Air Flow Rate \tabularnewline
+ & Evaporative Condenser Air Flow Rate \tabularnewline
+ & Evaporative Condenser Pump Rated Power Consumption \tabularnewline
+CondenserLoop \tabularnewline
+ & Maximum Loop Flow Rate \tabularnewline
+Controller:OutdoorAir \tabularnewline
+ & Minimum Outdoor Air Flow Rate \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+Controller:WaterCoil \tabularnewline
+ & Controller Convergence Tolerance \tabularnewline
+ & Maximum Actuated Flow \tabularnewline
+CoolingTower:SingleSpeed \tabularnewline
+ & Design Water Flow Rate \tabularnewline
+ & Design Air Flow Rate \tabularnewline
+ & Design Fan Power \tabularnewline
+ & Design U-Factor Times Area Value \tabularnewline
+CoolingTower:TwoSpeed \tabularnewline
+ & Design Water Flow Rate \tabularnewline
+ & High Fan Speed Air Flow Rate \tabularnewline
+ & High Fan Speed Fan Power \tabularnewline
+ & High Fan Speed U-Factor Times Area Value \tabularnewline
+CoolingTower:VariableSpeed \tabularnewline
+ & Design Water Flow Rate \tabularnewline
+ & Design Air Flow Rate \tabularnewline
+ & Design Fan Power \tabularnewline
+CoolingTower:VariableSpeed:Merkel \tabularnewline
+ & Nominal Capacity \tabularnewline
+ & Design Water Flow Rate \tabularnewline
+ & Design Air Flow Rate U-Factor Times Area Value \tabularnewline
+EvaporativeCooler:Indirect:ResearchSpecial \tabularnewline
+ & Secondary Fan Flow Rate \tabularnewline
+EvaporativeFluidCooler:SingleSpeed \tabularnewline
+ & Design Air Flow Rate \tabularnewline
+ & Design Air Flow Rate Fan Power \tabularnewline
+ & Design Air Flow Rate U-factor Times Area Value \tabularnewline
+ & Design Water Flow Rate \tabularnewline
+EvaporativeFluidCooler:TwoSpeed \tabularnewline
+ & High Fan Speed Air Flow Rate \tabularnewline
+ & High Fan Speed Fan Power \tabularnewline
+ & High Fan Speed U-factor Times Area Value \tabularnewline
+ & Design Water Flow Rate \tabularnewline
+Fan:ComponentModel \tabularnewline
+ & Maximum Flow Rate \tabularnewline
+ & Minimum Flow Rate \tabularnewline
+ & Motor Fan Pulley Ratio \tabularnewline
+ & Belt Maximum Torque \tabularnewline
+ & Maximum Motor Output Power \tabularnewline
+ & Maximum VFD Output Power \tabularnewline
+Fan:ConstantVolume \tabularnewline
+ & Maximum Flow Rate \tabularnewline
+Fan:OnOff \tabularnewline
+ & Maximum Flow Rate \tabularnewline
+FanPerformance:NightVentilation \tabularnewline
+ & Maximum Flow Rate \tabularnewline
+Fan:VariableVolume \tabularnewline
+ & Maximum Flow Rate \tabularnewline
+FluidCooler:SingleSpeed \tabularnewline
+ & Design Air Flow Rate U-factor Times Area Value \tabularnewline
+ & Design Water Flow Rate \tabularnewline
+ & Design Air Flow Rate \tabularnewline
+ & Design Air Flow Rate Fan Power \tabularnewline
+FluidCooler:TwoSpeed \tabularnewline
+ & High Fan Speed U-factor Times Area Value \tabularnewline
+ & Design Water Flow Rate \tabularnewline
+ & High Fan Speed Air Flow Rate \tabularnewline
+ & High Fan Speed Fan Power \tabularnewline
+HeaderedPumps:ConstantSpeed \tabularnewline
+ & Total Rated Flow Rate \tabularnewline
+ & Rated Power Consumption \tabularnewline
+HeaderedPumps:VariableSpeed \tabularnewline
+ & Total Rated Flow Rate \tabularnewline
+ & Rated Power Consumption \tabularnewline
+HeatExchanger:AirToAir:SensibleAndLatent \tabularnewline
+ & Nominal Supply Air Flow Rate \tabularnewline
+HeatExchanger:FluidToFluid \tabularnewline
+ & Loop Demand Side Design Flow Rate \tabularnewline
+ & Loop Supply Side Design Flow Rate \tabularnewline
+ & Heat Exchanger U-Factor Times Area Value \tabularnewline
+Humidifier:Steam:Electric \tabularnewline
+ & Rated Power \tabularnewline
+HVACTemplate:Plant:Boiler \tabularnewline
+ & Capacity \tabularnewline
+HVACTemplate:Plant:Chiller \tabularnewline
+ & Capacity \tabularnewline
+HVACTemplate:Plant:Tower \tabularnewline
+ & High Speed Nominal Capacity \tabularnewline
+ & High Speed Fan Power \tabularnewline
+ & Low Speed Nominal Capacity \tabularnewline
+ & Low Speed Fan Power \tabularnewline
+ & Free Convection Capacity \tabularnewline
+HVACTemplate:System:ConstantVolume \tabularnewline
+ & Supply Fan Maximum Flow Rate \tabularnewline
+ & Heating Coil Capacity \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+ & Minimum Outdoor Air Flow Rate \tabularnewline
+ & Humidifier Rated Electric Power \tabularnewline
+HVACTemplate:System:DedicatedOutdoorAir \tabularnewline
+ & Supply Fan Flow Rate \tabularnewline
+ & DX Cooling Coil Gross Rated Total Capacity \tabularnewline
+ & DX Cooling Coil Gross Rated Sensible Heat Ratio \tabularnewline
+ & Humidifier Rated Electric Power \tabularnewline
+HVACTemplate:System:DualDuct \tabularnewline
+ & Main Supply Fan Maximum Flow Rate \tabularnewline
+ & Cold Duct Supply Fan Maximum Flow Rate \tabularnewline
+ & Hot Duct Supply Fan Maximum Flow Rate \tabularnewline
+ & Heating Coil Capacity \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+ & Minimum Outdoor Air Flow Rate \tabularnewline
+ & Humidifier Rated Electric Power \tabularnewline
+HVACTemplate:System:PackagedVAV \tabularnewline
+ & Supply Fan Maximum Flow Rate \tabularnewline
+ & Supply Fan Minimum Flow Rate \tabularnewline
+ & Cooling Coil Gross Rated Total Capacity \tabularnewline
+ & Cooling Coil Gross Rated Sensible Heat Ratio \tabularnewline
+ & Heating Coil Capacity \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+ & Minimum Outdoor Air Flow Rate \tabularnewline
+ & Humidifier Rated Electric Power \tabularnewline
+HVACTemplate:System:Unitary \tabularnewline
+ & Supply Fan Maximum Flow Rate \tabularnewline
+ & Cooling Coil Gross Rated Total Capacity \tabularnewline
+ & Cooling Coil Gross Rated Sensible Heat Ratio \tabularnewline
+ & Heating Coil Capacity \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+ & Minimum Outdoor Air Flow Rate \tabularnewline
+ & Humidifier Rated Electric Power \tabularnewline
+HVACTemplate:System:UnitaryHeatPump:AirToAir \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & Cooling Coil Gross Rated Total Capacity \tabularnewline
+ & Cooling Coil Gross Rated Sensible Heat Ratio \tabularnewline
+ & Heat Pump Heating Coil Gross Rated Capacity \tabularnewline
+ & Supplemental Heating Coil Capacity \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+ & Minimum Outdoor Air Flow Rate \tabularnewline
+ & Humidifier Rated Electric Power \tabularnewline
+HVACTemplate:System:UnitarySystem \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & DX Cooling Coil Gross Rated Total Capacity \tabularnewline
+ & DX Cooling Coil Gross Rated Sensible Heat Ratio \tabularnewline
+ & Heating Coil Gross Rated Capacity \tabularnewline
+ & Supplemental Heating or Reheat Coil Capacity \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+ & Minimum Outdoor Air Flow Rate \tabularnewline
+ & Humidifier Rated Electric Power \tabularnewline
+HVACTemplate:System:VAV \tabularnewline
+ & Supply Fan Maximum Flow Rate \tabularnewline
+ & Supply Fan Minimum Flow Rate \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+ & Minimum Outdoor Air Flow Rate \tabularnewline
+ & Humidifier Rated Electric Power \tabularnewline
+HVACTemplate:System:VRF \tabularnewline
+ & Gross Rated Total Cooling Capacity \tabularnewline
+ & Gross Rated Heating Capacity \tabularnewline
+ & Resistive Defrost Heater Capacity \tabularnewline
+ & Water Condenser Volume Flow Rate \tabularnewline
+ & Evaporative Condenser Air Flow Rate \tabularnewline
+ & Evaporative Condenser Pump Rated Power Consumption \tabularnewline
+HVACTemplate:Zone:BaseboardHeat \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:ConstantVolume \tabularnewline
+ & Supply Air Maximum Flow Rate \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:DualDuct \tabularnewline
+ & Supply Air Maximum Flow Rate \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:FanCoil \tabularnewline
+ & Supply Air Maximum Flow Rate \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:IdealLoadsAirSystem \tabularnewline
+ & Maximum Heating Air Flow Rate \tabularnewline
+ & Maximum Sensible Heating Capacity \tabularnewline
+ & Maximum Cooling Air Flow Rate \tabularnewline
+ & Maximum Total Cooling Capacity \tabularnewline
+HVACTemplate:Zone:PTAC \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & Cooling Coil Gross Rated Total Capacity \tabularnewline
+ & Cooling Coil Gross Rated Sensible Heat Ratio \tabularnewline
+ & Heating Coil Capacity \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:PTHP \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & Cooling Coil Gross Rated Total Capacity \tabularnewline
+ & Cooling Coil Gross Rated Sensible Heat Ratio \tabularnewline
+ & Heat Pump Heating Coil Gross Rated Capacity \tabularnewline
+ & Supplemental Heating Coil Capacity \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:Unitary \tabularnewline
+ & Supply Air Maximum Flow Rate \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:VAV \tabularnewline
+ & Supply Air Maximum Flow Rate \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:VAV:FanPowered \tabularnewline
+ & Primary Supply Air Maximum Flow Rate \tabularnewline
+ & Primary Supply Air Minimum Flow Fraction \tabularnewline
+ & Secondary Supply Air Maximum Flow Rate \tabularnewline
+ & Parallel Fan On Flow Fraction \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:VAV:HeatAndCool \tabularnewline
+ & Supply Air Maximum Flow Rate \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:VRF \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & No Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Heating Supply Air Flow Rate \tabularnewline
+ & Cooling Outdoor Air Flow Rate \tabularnewline
+ & Heating Outdoor Air Flow Rate \tabularnewline
+ & No Load Outdoor Air Flow Rate \tabularnewline
+ & Cooling Coil Gross Rated Total Capacity \tabularnewline
+ & Cooling Coil Gross Rated Sensible Heat Ratio \tabularnewline
+ & Heat Pump Heating Coil Gross Rated Capacity \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+HVACTemplate:Zone:WaterToAirHeatPump \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & Cooling Coil Gross Rated Total Capacity \tabularnewline
+ & Cooling Coil Gross Rated Sensible Heat Ratio \tabularnewline
+ & Heat Pump Heating Coil Gross Rated Capacity \tabularnewline
+ & Supplemental Heating Coil Capacity \tabularnewline
+ & Baseboard Heating Capacity \tabularnewline
+PlantComponent:TemperatureSource \tabularnewline
+ & Design Volume Flow Rate \tabularnewline
+PlantEquipmentOperation:ComponentSetpoint \tabularnewline
+ & Component 1 Flow Rate \tabularnewline
+ & Component 2 Flow Rate \tabularnewline
+ & Component 3 Flow Rate \tabularnewline
+ & Component 4 Flow Rate \tabularnewline
+ & Component 5 Flow Rate \tabularnewline
+ & Component 6 Flow Rate \tabularnewline
+ & Component 7 Flow Rate \tabularnewline
+ & Component 8 Flow Rate \tabularnewline
+ & Component 9 Flow Rate \tabularnewline
+ & Component 10 Flow Rate \tabularnewline
+PlantLoop \tabularnewline
+ & Maximum Loop Flow Rate \tabularnewline
+Pump:ConstantSpeed \tabularnewline
+ & Rated Flow Rate \tabularnewline
+ & Rated Power Consumption \tabularnewline
+Pump:VariableSpeed \tabularnewline
+ & Rated Flow Rate \tabularnewline
+ & Rated Power Consumption \tabularnewline
+Pump:VariableSpeed:Condensate \tabularnewline
+ & Rated Flow Rate \tabularnewline
+ & Rated Power Consumption \tabularnewline
+Sizing:System \tabularnewline
+ & Design Outdoor Air Flow Rate \tabularnewline
+SolarCollector:FlatPlate:PhotovoltaicThermal \tabularnewline
+ & Design Flow Rate \tabularnewline
+ThermalStorage:ChilledWater:Mixed \tabularnewline
+ & Use Side Design Flow Rate \tabularnewline
+ & Source Side Design Flow Rate \tabularnewline
+ThermalStorage:ChilledWater:Stratified \tabularnewline
+ & Use Side Design Flow Rate \tabularnewline
+ & Source Side Design Flow Rate \tabularnewline
+UnitarySystemPerformance:HeatPump:Multispeed \tabularnewline
+ & Heating Speed 1 Supply Air Flow Ratio \tabularnewline
+ & Cooling Speed 1 Supply Air Flow Ratio \tabularnewline
+ & Heating Speed 2 Supply Air Flow Ratio \tabularnewline
+ & Cooling Speed 2 Supply Air Flow Ratio \tabularnewline
+ & Heating Speed 3 Supply Air Flow Ratio \tabularnewline
+ & Cooling Speed 3 Supply Air Flow Ratio \tabularnewline
+ & Heating Speed 4 Supply Air Flow Ratio \tabularnewline
+ & Cooling Speed 4 Supply Air Flow Ratio \tabularnewline
+WaterHeater:Mixed \tabularnewline
+ & Tank Volume \tabularnewline
+ & Heater Maximum Capacity \tabularnewline
+ & Use Side Design Flow Rate \tabularnewline
+ & Source Side Design Flow Rate \tabularnewline
+WaterHeater:Stratified \tabularnewline
+ & Tank Volume \tabularnewline
+ & Tank Height \tabularnewline
+ & Heater 1 Capacity \tabularnewline
+ & Use Side Design Flow Rate \tabularnewline
+ & Source Side Design Flow Rate \tabularnewline
+ZoneHVAC:Baseboard:Convective:Electric \tabularnewline
+ & Nominal Capacity \tabularnewline
+ZoneHVAC:Baseboard:Convective:Water \tabularnewline
+ & U-Factor Times Area Value \tabularnewline
+ & Maximum Water Flow Rate \tabularnewline
+ZoneHVAC:Baseboard:RadiantConvective:Electric \tabularnewline
+ & Nominal Capacity \tabularnewline
+ZoneHVAC:Baseboard:RadiantConvective:Steam \tabularnewline
+ & Maximum Steam Flow Rate \tabularnewline
+ZoneHVAC:Baseboard:RadiantConvective:Water \tabularnewline
+ & Rated Capacity \tabularnewline
+ & Maximum Water Flow Rate \tabularnewline
+ZoneHVAC:EnergyRecoveryVentilator \tabularnewline
+ & Supply Air Flow Rate \tabularnewline
+ & Exhaust Air Flow Rate \tabularnewline
+ZoneHVAC:EvaporativeCoolerUnit \tabularnewline
+ & Design Supply Air Flow Rate \tabularnewline
+ZoneHVAC:FourPipeFanCoil \tabularnewline
+ & Maximum Supply Air Flow Rate \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+ & Maximum Cold Water Flow Rate \tabularnewline
+ & Maximum Hot Water Flow Rate \tabularnewline
+ZoneHVAC:HighTemperatureRadiant \tabularnewline
+ & Maximum Power Input \tabularnewline
+ZoneHVAC:IdealLoadsAirSystem \tabularnewline
+ & Maximum Heating Air Flow Rate \tabularnewline
+ & Maximum Sensible Heating Capacity \tabularnewline
+ & Maximum Cooling Air Flow Rate \tabularnewline
+ & Maximum Total Cooling Capacity \tabularnewline
+ZoneHVAC:LowTemperatureRadiant:Electric \tabularnewline
+ & Maximum Electrical Power to Panel \tabularnewline
+ZoneHVAC:LowTemperatureRadiant:VariableFlow \tabularnewline
+ & Hydronic Tubing Length \tabularnewline
+ & Maximum Hot Water Flow \tabularnewline
+ & Maximum Cold Water Flow \tabularnewline
+ZoneHVAC:OutdoorAirUnit \tabularnewline
+ & Outdoor Air Flow Rate \tabularnewline
+ & Exhaust Air Flow Rate \tabularnewline
+ZoneHVAC:PackagedTerminalAirConditioner \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & Cooling Outdoor Air Flow Rate \tabularnewline
+ & Heating Outdoor Air Flow Rate \tabularnewline
+ & No Load Outdoor Air Flow Rate \tabularnewline
+ZoneHVAC:PackagedTerminalHeatPump \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & Cooling Outdoor Air Flow Rate \tabularnewline
+ & Heating Outdoor Air Flow Rate \tabularnewline
+ & No Load Outdoor Air Flow Rate \tabularnewline
+ & Maximum Supply Air Temperature from Supplemental Heater \tabularnewline
+ZoneHVAC:TerminalUnit:VariableRefrigerantFlow \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & No Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Heating Supply Air Flow Rate \tabularnewline
+ & Cooling Outdoor Air Flow Rate \tabularnewline
+ & Heating Outdoor Air Flow Rate \tabularnewline
+ & No Load Outdoor Air Flow Rate \tabularnewline
+ZoneHVAC:UnitHeater \tabularnewline
+ & Maximum Supply Air Flow Rate \tabularnewline
+ & Maximum Hot Water or Steam Flow Rate \tabularnewline
+ZoneHVAC:UnitVentilator \tabularnewline
+ & Maximum Supply Air Flow Rate \tabularnewline
+ & Minimum Outdoor Air Flow Rate \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+ZoneHVAC:VentilatedSlab \tabularnewline
+ & Maximum Air Flow Rate \tabularnewline
+ & Minimum Outdoor Air Flow Rate \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+ZoneHVAC:WaterToAirHeatPump \tabularnewline
+ & Cooling Supply Air Flow Rate \tabularnewline
+ & Heating Supply Air Flow Rate \tabularnewline
+ & No Load Supply Air Flow Rate \tabularnewline
+ & Cooling Outdoor Air Flow Rate \tabularnewline
+ & Heating Outdoor Air Flow Rate \tabularnewline
+ & No Load Outdoor Air Flow Rate \tabularnewline
+ & Maximum Supply Air Temperature from Supplemental Heater \tabularnewline
+ZoneHVAC:WindowAirConditioner \tabularnewline
+ & Maximum Supply Air Flow Rate \tabularnewline
+ & Maximum Outdoor Air Flow Rate \tabularnewline
+\bottomrule
+\end{longtable}
+
+There are 3 places in the input where the user can impose sizing factors.
+
+1.~~~~In Sizing Parameters (object: Sizing:Parameters), the user can specify an over-all sizing factor. This factor is applied to all the zone design loads and air flow rates resulting from the zone sizing calculations.
+
+2.~~~~In Zone Sizing (object: Sizing:Zone), the user can specify a sizing factor for a specific zone. The factor is applied to the calculated zone design loads and air flow rates for the zone named in the Sizing:Zone object. This sizing factor overrides the global sizing factor. That is, a zone sizing factor, if specified, replaces the global sizing factor for the named zone.
+
+3.~~~~For some plant components (basically all central chillers, boilers and cooling towers) the user can specify a sizing factor that modifies the autosized component capacity and flow rates. These factors are applied after the application of global or zone sizing factors. They are primarily used to split the design load between multiple components. These sizing factors can change the autosizing of the associated loops and pumps. The following rules are followed the effect of plant component sizing factors on loops and pumps.
+
+a.~~~~For supply side branches, the sizing factors of all components in series on the branch are summed and the result becomes the branch sizing factor. If there is a branch pump its autosized design flow rate is multiplied by the branch sizing factor.
+
+b.~~~For each loop, if the average of the branch sizing factors is less than 1, the loop sizing factor is set equal to the sum of the branch sizing factors. If the average is greater than 1, the loop sizing factor is set equal to the maximum of the branch sizing factors. The loop sizing factor is applied to the loop design flow rate (if autosized) and to the loop pump flow rate (if autosized).
+
+\subsubsection{Mixing User-Specified and Autosized Inputs}\label{mixing-user-specified-and-autosized-inputs}
+
+Mixed user-specified and autosized inputs can be successfully used if the following points and suggestions are followed.
+
+1.~~~~Each component is autosized independently. Thus user input for a flow rate in one component will have no effect on other components' autosized flow rates. For instance, specifying the chilled water loop pump's rated flow rate will have no effect on the autosizing of the chiller's design evaporator flow rate or on the plant loop's autosized maximum loop flow rate.
+
+2.~~~~Within a component it is best to autosize all inputs are enter specified values for all inputs. For example, in a chiller, if only the nominal capaciity is user-specified, the autosized chilled water flow rate may not be consistent with the specified capacity.
+
+3.~~~~Sizing information flows only from the sizing objects to the components. The sizing calculations have no knowledge of user-specified values in a component. The only exception to this rule is that plant loop sizing will collect all component design water flow rates whether autosized or user-specified.
+
+4.~~~~If the user wants to specify a zone or system air flow rate it should be done using the Sizing:Zone and Sizing:System~ objects rather than done in the individual components.
+
+5.~~~~The plant loop flow rates are sized from the total design demand of the components connected to each loop. The components demanding water need not be autosized for the plant loop autosizing to work successfully. So the user could specify all the air side components and autosize all the plant loops and plant components. Or specify the chilled water loop flow rate, chilled water pump inputs and chiller inputs and let the condenser loop and tower autosize.
+
+\subsubsection{Component Sizing Output}\label{component-sizing-output}
+
+The results of the component autosizing calculations are reported on the \emph{eplusout.eio} file. For each component field that has been autosized the object type, object name, field description with unit, and value are printed out as comma separated data on a line beginning with \emph{Component Sizing}. Examples of this are shown in the Output Details and Examples document.
+
+The complete list of objects that have autosized fields is shown in the following table. Note that spaces may be inserted in object names to facilitate readability.
+
+% table 23
+\begin{longtable}[c]{p{3.02in}p{2.97in}}
+\caption{Complete list of Objects with autosized Fields \label{table:complete-list-of-objects-with-autosized}} \tabularnewline
+\toprule 
+Object Name & Object Name \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Complete list of Objects with autosized Fields} \tabularnewline
+\toprule 
+Object Name & Object Name \tabularnewline
+\midrule
+\endhead
+
+AirConditioner:VariableRefrigerantFlow & AirLoopHVAC \tabularnewline
+AirLoopHVAC:Unitary:Furnace:HeatCool & AirLoopHVAC:Unitary:Furnace:HeatOnly \tabularnewline
+AirLoopHVAC:UnitaryHeatCool & AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass \tabularnewline
+AirLoopHVAC:UnitaryHeatOnly & AirLoopHVAC:UnitaryHeatPump:AirToAir \tabularnewline
+AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed & AirLoopHVAC:UnitaryHeatPump:WaterToAir \tabularnewline
+AirLoopHVAC:UnitarySystem & AirTerminal:DualDuct:ConstantVolume \tabularnewline
+AirTerminal:DualDuct:VAV & AirTerminal:DualDuct:VAV:OutdoorAir \tabularnewline
+AirTerminal:SingleDuct:ConstantVolume:CooledBeam & AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction \tabularnewline
+AirTerminal:SingleDuct:ConstantVolume:Reheat & AirTerminal:SingleDuct:ParallelPIU:Reheat \tabularnewline
+AirTerminal:SingleDuct:SeriesPIU:Reheat & AirTerminal:SingleDuct:Uncontrolled \tabularnewline
+AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat & AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat \tabularnewline
+AirTerminal:SingleDuct:VAV:NoReheat & AirTerminal:SingleDuct:VAV:Reheat \tabularnewline
+AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan & Boiler:HotWater \tabularnewline
+Boiler:Steam & Branch \tabularnewline
+Chiller:Absorption & Chiller:Absorption:Indirect \tabularnewline
+Chiller:CombustionTurbine & Chiller:ConstantCOP \tabularnewline
+Chiller:Electric & Chiller:Electric:EIR \tabularnewline
+Chiller:Electric:ReformulatedEIR & Chiller:EngineDriven \tabularnewline
+ChillerHeater:Absorption:DirectFired & ChillerHeater:Absorption:DoubleEffect \tabularnewline
+ChillerHeaterPerformance:Electric:EIR & Coil:Cooling:DX:MultiSpeed \tabularnewline
+Coil:Cooling:DX:SingleSpeed & Coil:Cooling:DX:SingleSpeed:ThermalStorage \tabularnewline
+Coil:Cooling:DX:TwoSpeed & Coil:Cooling:DX:VariableRefrigerantFlow \tabularnewline
+Coil:Cooling:DX:VariableSpeed & Coil:Cooling:Water \tabularnewline
+Coil:Cooling:Water:DetailedGeometry & Coil:Cooling:WaterToAirHeatPump:EquationFit \tabularnewline
+Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit & Coil:Heating:DX:MultiSpeed \tabularnewline
+Coil:Heating:DX:SingleSpeed & Coil:Heating:DX:VariableRefrigerantFlow \tabularnewline
+Coil:Heating:DX:VariableSpeed & Coil:Heating:Electric \tabularnewline
+Coil:Heating:Electric:MultiStage & Coil:Heating:Gas \tabularnewline
+Coil:Heating:Gas:MultiStage & Coil:Heating:Steam \tabularnewline
+Coil:Heating:Water & Coil:Heating:WaterToAirHeatPump:EquationFit \tabularnewline
+Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit & CoilPerformance:DX:Cooling \tabularnewline
+CondenserLoop & Controller:OutdoorAir \tabularnewline
+Controller:WaterCoil & CoolingTower:SingleSpeed \tabularnewline
+CoolingTower:TwoSpeed & CoolingTower:VariableSpeed \tabularnewline
+CoolingTower:VariableSpeed:Merkel & EvaporativeCooler:Indirect:ResearchSpecial \tabularnewline
+EvaporativeFluidCooler:SingleSpeed & EvaporativeFluidCooler:TwoSpeed \tabularnewline
+Fan:ComponentModel & Fan:ConstantVolume \tabularnewline
+Fan:OnOff & FanPerformance:NightVentilation \tabularnewline
+Fan:VariableVolume & FluidCooler:SingleSpeed \tabularnewline
+FluidCooler:TwoSpeed & HeaderedPumps:ConstantSpeed \tabularnewline
+HeaderedPumps:VariableSpeed & HeatExchanger:AirToAir:SensibleAndLatent \tabularnewline
+HeatExchanger:FluidToFluid & Humidifier:Steam:Electric \tabularnewline
+HVACTemplate:Plant:Boiler & HVACTemplate:Plant:Chiller \tabularnewline
+HVACTemplate:Plant:Tower & HVACTemplate:System:ConstantVolume \tabularnewline
+HVACTemplate:System:DedicatedOutdoorAir & HVACTemplate:System:DualDuct \tabularnewline
+HVACTemplate:System:PackagedVAV & HVACTemplate:System:Unitary \tabularnewline
+HVACTemplate:System:UnitaryHeatPump:AirToAir & HVACTemplate:System:UnitarySystem \tabularnewline
+HVACTemplate:System:VAV & HVACTemplate:System:VRF \tabularnewline
+HVACTemplate:Zone:BaseboardHeat & HVACTemplate:Zone:ConstantVolume \tabularnewline
+HVACTemplate:Zone:DualDuct & HVACTemplate:Zone:FanCoil \tabularnewline
+HVACTemplate:Zone:IdealLoadsAirSystem & HVACTemplate:Zone:PTAC \tabularnewline
+HVACTemplate:Zone:PTHP & HVACTemplate:Zone:Unitary \tabularnewline
+HVACTemplate:Zone:VAV & HVACTemplate:Zone:VAV:FanPowered \tabularnewline
+HVACTemplate:Zone:VAV:HeatAndCool & HVACTemplate:Zone:VRF \tabularnewline
+HVACTemplate:Zone:WaterToAirHeatPump & PlantComponent:TemperatureSource \tabularnewline
+PlantEquipmentOperation:ComponentSetpoint & PlantLoop \tabularnewline
+Pump:ConstantSpeed & Pump:VariableSpeed \tabularnewline
+Pump:VariableSpeed:Condensate & Sizing:System \tabularnewline
+SolarCollector:FlatPlate:PhotovoltaicThermal & ThermalStorage:ChilledWater:Mixed \tabularnewline
+ThermalStorage:ChilledWater:Stratified & UnitarySystemPerformance:HeatPump:Multispeed \tabularnewline
+WaterHeater:Mixed & WaterHeater:Stratified \tabularnewline
+ZoneHVAC:Baseboard:Convective:Electric & ZoneHVAC:Baseboard:Convective:Water \tabularnewline
+ZoneHVAC:Baseboard:RadiantConvective:Electric & ZoneHVAC:Baseboard:RadiantConvective:Steam \tabularnewline
+ZoneHVAC:Baseboard:RadiantConvective:Water & ZoneHVAC:EnergyRecoveryVentilator \tabularnewline
+ZoneHVAC:EvaporativeCoolerUnit & ZoneHVAC:FourPipeFanCoil \tabularnewline
+ZoneHVAC:HighTemperatureRadiant & ZoneHVAC:IdealLoadsAirSystem \tabularnewline
+ZoneHVAC:LowTemperatureRadiant:Electric & ZoneHVAC:LowTemperatureRadiant:VariableFlow \tabularnewline
+ZoneHVAC:OutdoorAirUnit & ZoneHVAC:PackagedTerminalAirConditioner \tabularnewline
+ZoneHVAC:PackagedTerminalHeatPump & ZoneHVAC:TerminalUnit:VariableRefrigerantFlow \tabularnewline
+ZoneHVAC:UnitHeater & ZoneHVAC:UnitVentilator \tabularnewline
+ZoneHVAC:VentilatedSlab & ZoneHVAC:WaterToAirHeatPump \tabularnewline
+ZoneHVAC:WindowAirConditioner &  \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{User or External Zone Design Flow Rate Inputs}\label{user-or-external-zone-design-flow-rate-inputs}
+
+In EnergyPlus the autosizing calculations start with a calculation of the zone design air flow rates using zone by zone design day simulations. The resulting zone design air flow rates and daily air flow sequences are used in the subsequent HVAC and central plant air and fluid flow design calculations and in the component autosizing calculations. The user can override or change the calculated zone design air flow rates in several ways.
+
+1)~~~~The user can enter a value for \emph{Sizing Factor} in the \emph{Sizing:Parameters} object (see description below).
+
+2)~~~~The user can specify a zone level \emph{Zone Sizing Factor} in each \emph{Sizing:Zone} object.
+
+3)~~~~For each zone the user can input a \emph{Cooling Design Air Flow Rate} and/or a \emph{Heating Design Air Flow Rate} (and specify \emph{Cooling Design Air Flow Method = Flow/Zone} and \emph{Heating Design Air Flow Method = Flow/Zone}). These user inputs override the calculated values. The program divides the user input cooling or heating design air flow rate by the calculated values and uses the result as a zone sizing factor to multiply all the elements in the design heating and cooling air flow and load sequences. From this point the design calculations proceed as usual.
+
+\subsubsection{User or External System Design Flow Rate Inputs}\label{user-or-external-system-design-flow-rate-inputs}
+
+Using the results of the zone design air flow rate calculation (including any user input or altered flow rates) EnergyPlus proceeds to calculate central air system flow rates and cooling and heating loads. The results of this calculation can be overridden in the following way.
+
+For each system (AirLoopHVAC), in the corresponding Sizing:System object, specify \emph{Cooling Design Air Flow Method} to be \emph{Flow/System} and input a value for \emph{Cooling Design Air Flow Rate}. Similarly for heating specify \emph{Heating Design Air Flow Method} to be \emph{Flow/System} and input a value for \emph{Heating Design Air Flow Rate}.
+
+\subsection{DesignSpecification:OutdoorAir}\label{designspecificationoutdoorair}
+
+This object allows for the outdoor air requirements to be defined in a common location for use by other objects. This object may be referenced by name from other objects (e.g., VAV terminal units) as required to identify an outdoor air quantity for use by that object. Note that a zone name Is not included as an input to this zone outdoor air definition and the number of people in a zone, zone floor area, and zone volume can only be determined after this object has been referenced by another. A single zone outdoor air definition may be referenced by multiple objects to specify that the same outdoor air requirements are used by those objects \emph{or} multiple zone outdoor air objects may be defined and referenced by other objects as needed. If multiple zone outdoor air definitions are used, each outdoor air definition must have a unique name.
+
+\subsubsection{Inputs}\label{inputs-012}
+
+\paragraph{Field: Name}\label{field-name-011}
+
+Unique identifying name. Any reference to this name by other objects will denote that the following outdoor air requirements will be used.
+
+\paragraph{Field: Outdoor Air Method}\label{field-outdoor-air-method}
+
+The input must be either \emph{Flow/Person}, \emph{Flow/Area}, \emph{Flow/Zone, AirChanges/Hour}, \emph{Sum}, or \emph{Maximum}. \emph{Flow/Person} means the program will use the input from the field \emph{Outdoor Air Flow per Person} and the actual zone occupancy to calculate a zone outdoor air flow rate. \emph{Flow/Area} means that the program will use the input from the field \emph{Outdoor Air Flow per Zone Floor Area} and the actual zone floor area as the zone outdoor air flow rate. \emph{Flow/Zone} means that the program will use the input of the field \emph{Outdoor Air Flow per Zone} as the zone outdoor air flow rate. \emph{AirChanges/Hour} means that the program will use the input from the field \emph{Air Changes per Hour} and the actual zone volume (divided by 3600 seconds per hour) as the zone outdoor air flow rate. \emph{Sum} means that the flows calculated from the fields \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area, Outdoor Air Flow per Zone}, and \emph{Air Changes per Hour} (using the associated conversions to m\(^{3}\)/s for each field) will be added to obtain the zone outdoor air flow rate. \emph{Maximum} means that the maximum flow derived from \emph{Outdoor Air Flow per Person,} \emph{Outdoor Air Flow per Area, Outdoor Air Flow per Zone,} and \emph{Air Changes per Hour} (using the associated conversions to m\(^{3}\)/s for each field) will be used as the zone outdoor air flow rate. The default is \emph{Flow/Person}.
+
+\paragraph{Field: Outdoor Air Flow per Person}\label{field-outdoor-air-flow-per-person}
+
+The design outdoor air volume flow rate per person for this zone in cubic meters per second per person. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values \emph{are not} applied during sizing calculations and \emph{are} applied during the remainder of the simulation. This input is used if \emph{Outdoor Air Method} is one of \emph{Outdoor Air Flow per Person}, \emph{Sum}, or \emph{Maximum}.
+
+\paragraph{Field: Outdoor Air Flow per Zone Floor Area}\label{field-outdoor-air-flow-per-zone-floor-area}
+
+The design outdoor air volume flow rate per square meter of floor area (units are m\(^{3}\)/s-m\(^{2}\)). This input is used if \emph{Outdoor Air Method} is \emph{Flow/Area, Sum} or \emph{Maximum}. The default value for this field is 0.
+
+\paragraph{Field: Outdoor Air Flow per Zone}\label{field-outdoor-air-flow-per-zone}
+
+The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{Flow/Zone, Sum} or \emph{Maximum}. The default value for this field is 0.
+
+\paragraph{Field: Outdoor Air Flow Changes per Hour}\label{field-outdoor-air-flow-changes-per-hour}
+
+The design outdoor air volume flow rate in air changes per hour. This factor is used along with the Zone Volume and converted to cubic meters per second. This input field is used if \emph{Outdoor Air Method} is \emph{AirChanges/Hour, Sum} or \emph{Maximum}. The default value for this field is 0.
+
+\paragraph{Field: Outdoor Air Flow Rate Fraction Schedule Name}\label{field-outdoor-air-flow-rate-fraction-schedule-name}
+
+This field is the name of schedule that defines how outdoor air requirements change over time.~ The field is optional.~ If used, then the schedule values are multiplied by the outdoor air flow rate defined by the previous fields.~ The schedule values must be between 0 and 1, inclusive.
+
+An IDF example:
+
+\begin{lstlisting}
+
+DesignSpecification:OutdoorAir
+      ZoneOAData,            !- Name
+      Sum,                   !- Outdoor Air Method
+      0.00944,               !- Outdoor Air Flow per Person {m3/s}
+      0.00305,               !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
+      ,                      !- Outdoor Air Flow per Zone {m3/s}
+      ,                      !- Outdoor Air Flow Air Changes per Hour
+      OARequirements Sched;  !- Outdoor Air Flow Rate Fraction Schedule Name
+
+
+  Schedule:Compact,
+      OARequirements Sched,    !- Name
+      Any Number,              !- Schedule Type Limits Name
+      Through: 12/31,          !- Field 1
+      For: Weekdays SummerDesignDay WinterDesignDay,  !- Field 2
+      Until: 24:00, 1.0,       !- Field 4
+      For: AllOtherDays,       !- Field 5
+      Until: 24:00, 0.5;       !- Field 7
+\end{lstlisting}
+
+\subsection{DesignSpecification:ZoneAirDistribution}\label{designspecificationzoneairdistribution}
+
+This object is used to describe the air distribution effectiveness and fraction of secondary recirculation air (return air not directly mixed with outdoor air) of a zone. It is referenced by the Sizing:Zone and Controller:MechanicalVentilation objects.
+
+\subsubsection{Inputs}\label{inputs-1-011}
+
+\paragraph{Field: Name}\label{field-name-1-010}
+
+The unique user assigned name for an instance of this object. Any other object referencing this object will use this name.
+
+\paragraph{Field: Zone Air Distribution Effectiveness in Cooling Mode}\label{field-zone-air-distribution-effectiveness-in-cooling-mode}
+
+The positive numeric input for this field is the zone air distribution effectiveness when the zone is in cooling mode. Default value of this field is 1.0. ASHRAE Standard 62.1-2010 provides typical values.
+
+\paragraph{Field: Zone Air Distribution Effectiveness in Heating Mode}\label{field-zone-air-distribution-effectiveness-in-heating-mode}
+
+The positive numeric input for this field is the zone air distribution effectiveness when the zone is in heating mode. Default value of this field is 1.0. ASHRAE Standard 62.1-2010 provides typical values as follows:
+
+\begin{figure}[hbtp] % fig 71
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image133.png}
+\caption{Zone Air Distribution Effectiveness (Source: ASHRAE Standard 62.1-2010) \protect \label{fig:zone-air-distribution-effectiveness-source}}
+\end{figure}
+
+\paragraph{Field: Zone Air Distribution Effectiveness Schedule Name}\label{field-zone-air-distribution-effectiveness-schedule-name}
+
+This optional field input points to a schedule with values of zone air distribution effectiveness. It provides a more flexible way of specifying zone air distribution effectiveness if it changes with time and/or system operating status and controls. If the schedule is specified, the zone air distribution effectiveness in cooling mode and heating mode will be ignored.
+
+\paragraph{Field: Zone Secondary Recirculation Fraction}\label{field-zone-secondary-recirculation-fraction}
+
+The non-negative numeric input for this field is the fraction of a zone's recirculation air that does not directly mix with the outdoor air. The zone secondary recirculation fraction Er is determined by the designer based on system configuration. For plenum return systems with secondary recirculation (e.g., fan-powered VAV with plenum return) Er is usually less than 1.0, although values may range from 0.1 to 1.2 depending upon the location of the ventilation zone relative to other zones and the air handler. For ducted return systems with secondary recirculation (e.g., fan-powered VAV with ducted return), Er is typically 0.0, while for those with system-level recirculation (e.g, dual-fan dual-duct systems with ducted return) Er is typically 1.0. For other system types, Er is typically 0.75. Minimum is 0.0, and default is 0.0 for single-path systems (also to maintain backward compatibility). For parallel fan-powered VAV systems, the secondary ventilation path only functions (Er \textgreater{} 0.0) when the fans in the VAV boxes operate, which is during heating. The local ventilation path and the benefits of secondary recirculation disappear during cooling, when the local parallel fans are off (Er = 0.0).
+
+An example of this in an IDF context is shown:
+
+\begin{lstlisting}
+
+DesignSpecification:ZoneAirDistribution,
+      CM DSZAD ZN_1_FLR_1_SEC_1,  !- Name
+      1,                       !- Zone Air Distribution Effectiveness in Cooling Mode {dimensionless}
+      1,                       !- Zone Air Distribution Effectiveness in Heating Mode {dimensionless}
+      ;                        !- Zone Air Distribution Effectiveness Schedule Name
+\end{lstlisting}
+
+\subsection{Sizing:Parameters}\label{sizingparameters}
+
+This object allows the user to specify global heating and cooling sizing ratios. These ratios will be applied at the zone level to all of the zone heating and cooling loads and air flow rates. These new loads and air flow rates are then used to calculate the system level flow rates and capacities and are used in all component sizing calculations.
+
+The user can also specify the width (in load timesteps) of a moving average window which can be used to smooth the calculated zone design flow sequences. The use of this parameter is described below.
+
+\subsubsection{Inputs}\label{inputs-2-010}
+
+\paragraph{Field: Heating Sizing Factor}\label{field-heating-sizing-factor}
+
+The global heating sizing ratio applied to all of the zone design heating loads and air flow rates.
+
+\paragraph{Field: Cooling Sizing Factor}\label{field-cooling-sizing-factor}
+
+The global cooling sizing ratio applied to all of the zone design cooling loads and air flow rates
+
+\paragraph{Field: Timesteps in Averaging Window}\label{field-timesteps-in-averaging-window}
+
+The number of load timesteps in the zone design flow sequence averaging window. The default is 1, in which case the calculated zone design flow rates are averaged over the load timestep.
+
+The zone design air flow rate calculation is performed assuming a potentially infinite supply of heating or cooling air at a fixed temperature. Thus the calculated design air flow rate will always be able to meet any load or change in load no matter how large or abrupt. In reality air flow rates are limited by duct sizes and fan capacities. The idealized zone design flow calculation may result in unrealistically large flow rates, especially if the user is performing the sizing calculations using thermostat schedules with night setup or setback. The calculated zone design flow rates are always averaged over the load timestep. The user may want to perform a broader average to mitigate the effect of thermostat setup and setback and prevent the warm up or cool down flow rates from dominating the design flow rate calculation.. Specifying the width of the averaging window allows the user to do this.
+
+For example, if the load calculation timestep is 15 minutes and the user specifies the \emph{Timesteps in Averaging Window} to be 4, the zone design air flows will be averaged over a time period of 1 hour. Specifying 8 would result in averaging over a 2 hour period.
+
+\subsubsection{Outputs}\label{outputs-009}
+
+The sizing factors and the averaging window size are reported out on the \emph{eplusout.eio} file. An example is:
+
+\begin{lstlisting}
+! <Load Timesteps in Zone Design Calculation Averaging Window>, Value
+ Timesteps in Averaging Window,    1
+! <Heating Sizing Factor Information>, Sizing Factor ID, Value
+ Heating Sizing Factor, Global,   1.3000
+ Heating Sizing Factor, Zone SPACE1-1,   1.3000
+ Heating Sizing Factor, Zone SPACE2-1,   1.3000
+ Heating Sizing Factor, Zone SPACE3-1,   1.3000
+ Heating Sizing Factor, Zone SPACE4-1,   1.3000
+ Heating Sizing Factor, Zone SPACE5-1,   1.3000
+! <Cooling Sizing Factor Information>, Sizing Factor ID, Value
+ Cooling Sizing Factor, Global,   1.3000
+ Cooling Sizing Factor, Zone SPACE1-1,   1.3000
+ Cooling Sizing Factor, Zone SPACE2-1,   1.3000
+ Cooling Sizing Factor, Zone SPACE3-1,   1.3000
+ Cooling Sizing Factor, Zone SPACE4-1,   1.3000
+ Cooling Sizing Factor, Zone SPACE5-1,   1.3000
+\end{lstlisting}
+
+\subsection{OutputControl:Sizing:Style}\label{outputcontrolsizingstyle}
+
+As described early in the document (see: EnergyPlus Output Processing), the user may select the ``style'' for the sizing result files (epluszsz.\textless{}ext\textgreater{}, eplusssz.\textless{}ext\textgreater{}). This object applies to all sizing output files.
+
+\begin{lstlisting}
+OutputControl:Sizing:Style,
+       \memo default style for the Sizing output files is comma -- this works well for
+       \memo importing into spreadsheet programs such as Excel(tm) but not so well for word
+       \memo processing progams -- there tab may be a better choice.  fixed puts spaces between
+       \memo the "columns"
+       \unique-object
+   A1; \field Column Separator
+       \required-field
+       \type choice
+       \key Comma
+       \key Tab
+       \key Fixed
+\end{lstlisting}
+
+\subsubsection{Inputs}\label{inputs-3-009}
+
+\paragraph{Field: Column Separator}\label{field-column-separator-000}
+
+For this field, the desired separator for columns is entered. ``Comma'' creates comma separated fields/columns in the outputs (eplus\textless{}sizing type\textgreater{}.csv files are created). ``Tab'' creates tab separated fields/columns in the outputs (eplus\textless{}sizing type\textgreater{}.tab files are created). ``Fixed'' creates space separated fields/columns in the outputs (eplus\textless{}sizing type\textgreater{}.txt files are created) but these are not necessarily lined up for easy printing.
+
+Note that both tab and comma separated files easily import into Excelâ„¢ or other spreadsheet programs. The tab delimited files can also be viewed by text editors, word processing programs and easily converted to ``tables'' within those programs.
+
+\subsection{Sizing:Zone}\label{sizingzone}
+
+The Sizing:Zone object provides the data needed to perform a zone design air flow calculation for a single zone. This calculation assumes a variable amount of supply air at a fixed temperature and humidity. The information needed consists of the zone inlet supply air conditions: temperature and humidity ratio for heating and cooling. The calculation is done for every design day included in the input. The maximum cooling load and air flow and the maximum heating load and air flow are then saved for the system level design calculations and for the component automatic sizing calculations.
+
+The Sizing:Zone object is also the place where the user can specify the design outdoor air flow rate by referencing the name of a design specification outdoor air object. This can be specified in a number of ways (ref. DesignSpecification:OutdoorAir).This data is saved for use in the system sizing calculation or for sizing zone components that use outdoor air.
+
+The user can also place limits on the heating and design cooling air flow rates. See \emph{~Heating Design Air Flow Method} and \emph{Cooling Design Air Flow Method} below and the explanations of the various heating and cooling flow input fields.
+
+The user can ask the zone design calculation to take into account the effect of a Dedicated Outdoor Air System on the zone design loads and airflow rates. The design calculation will calculate the heat addition rate to the zone of an idealized SOA system and add or subtract the result from the total zone loads and flow rates.
+
+\subsubsection{Inputs}\label{inputs-4-008}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-004}
+
+The name of the Zone corresponding to this Sizing:Zone object. This is the zone for which the design air flow calculation will be made using the input data of this Sizing:Zone Object.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Input Method}\label{field-zone-cooling-design-supply-air-temperature-input-method}
+
+The input must be either \emph{SupplyAirTemperature} or \emph{TemperatureDifference}. \emph{SupplyAirTemperature} means that the user inputs from the fields of Zone Cooling Design Supply Air Temperature will be used to determine the zone cooling design air flow rates. \emph{TemperatureDifference} means that the user inputs from the fields of Zone Cooling Design Supply Air Temperature Difference will be used to determine the zone cooling design air flow rates.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature}\label{field-zone-cooling-design-supply-air-temperature}
+
+The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation. Air is supplied to the zone at this temperature during the cooling design day simulation, The zone load is met by varying the zone air flow rate. The maximum zone flow rate is saved as the~ zone cooling design air flow rate. This field is only used when Zone Cooling Design Supply Air Temperature Input Method = \textbf{SupplyAirTemperature}.
+
+\paragraph{Field: Zone Cooling Design Supply Air Temperature Difference}\label{field-zone-cooling-design-supply-air-temperature-difference}
+
+The temperature difference between cooling design supply air temperature and room air temperature in degrees Celsius for the zone cooling design air flow rate calculation. Air is supplied to the zone at this temperature during the cooling design day simulation. The zone load is met by varying the zone air flow rate. The maximum zone flow rate is saved as the zone cooling design air flow rate. This field is only used when Zone Cooling Design Supply Air Temperature Input Method = \textbf{TemperatureDifference}.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Input Method}\label{field-zone-heating-design-supply-air-temperature-input-method}
+
+The input must be either \emph{SupplyAirTemperature} or \emph{TemperatureDifference}. \emph{SupplyAirTemperature} means that the user inputs from the fields of Zone Heating Design Supply Air Temperature will be used to determine the zone heating design air flow rates. \emph{TemperatureDifference} means that the user inputs from the fields of Zone Heating Design Supply Air Temperature Difference will be used to determine the zone heating design air flow rates.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature}\label{field-zone-heating-design-supply-air-temperature}
+
+The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation. Air is supplied to the zone at this temperature during the heating design day simulation, The zone load is met by varying the zone air flow rate. The maximum zone flow rate is saved as the zone heating design air flow rate. This field is only used when Zone Heating Design Supply Air Temperature Input Method = \textbf{SupplyAirTemperature}.
+
+\paragraph{Field: Zone Heating Design Supply Air Temperature Difference}\label{field-zone-heating-design-supply-air-temperature-difference}
+
+The temperature difference between heating design supply air temperature and room air temperature in degrees Celsius for the zone heating design air flow rate calculation. Air is supplied to the zone at this temperature during the heating design day simulation. The zone load is met by varying the zone air flow rate. The maximum zone flow rate is saved as the zone heating design air flow rate. This field is only used when Zone Heating Design Supply Air Temperature Input Method = \textbf{TemperatureDifference}.
+
+\paragraph{Field: Zone Cooling Design Supply Air Humidity Ratio}\label{field-zone-cooling-design-supply-air-humidity-ratio}
+
+The humidity ratio in kilograms of water per kilogram of dry air of the supply air in the zone cooling design air flow rate calculation.
+
+\paragraph{Field: Zone Heating Design Supply Air Humidity Ratio}\label{field-zone-heating-design-supply-air-humidity-ratio}
+
+The humidity ratio in kilograms of water per kilogram of dry air of the supply air in the zone heating design air flow rate calculation.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-000}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.
+
+\paragraph{Field: Zone Heating Sizing Factor}\label{field-zone-heating-sizing-factor}
+
+This input is a zone level heating sizing ratio. The zone design heating air flow rates and loads will be multiplied by the number input in this field. This input overrides the building level sizing factor input in the Sizing:Parameters object. And, of course, if this field is blank or zero, the global heating sizing factor from the Sizing:Parameters object is used.
+
+\paragraph{Field: Zone Cooling Sizing Factor}\label{field-zone-cooling-sizing-factor}
+
+This input is a zone level cooling sizing ratio. The zone design cooling air flow rates and loads will be multiplied by the number input in this field. This input overrides the building level sizing factor input in the Sizing:Parameters object. And, of course, if this field is blank or zero, the global cooling sizing factor from the Sizing:Parameters object is used.
+
+\paragraph{Field: Cooling Design Air Flow Method}\label{field-cooling-design-air-flow-method}
+
+The input must be either \emph{Flow/Zone, DesignDay, or DesignDayWithLimit}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Cooling Design Air Flow Rate} as the zone design cooling air flow rate. \emph{DesignDay} means the program will calculate the zone design cooling air flow rate using the Sizing:Zone input data and a design day simulation without imposing any limits other than those set by the minimum outside air requirements. \emph{DesignDayWithLimit} means that the maximum from \emph{Cooling Minimum Air Flow per Zone Floor Area} and \emph{Cooling Minimum Air Flow} will set a lower limit on the design maximum cooling air flow rate. The default method is \emph{DesignDay}: i.e., the program uses the calculated design values subject to ventilation requirements.
+
+\paragraph{Field: Cooling Design Air Flow Rate}\label{field-cooling-design-air-flow-rate}
+
+The design zone cooling air flow rate in cubic meters per second. This input is used if \emph{Cooling Design Air Flow Method} is specified as \emph{Flow/Zone}. This value will be multiplied by the global or zone sizing factor and by zone multipliers.
+
+\paragraph{Field: Cooling Minimum Air Flow per Zone Floor Area}\label{field-cooling-minimum-air-flow-per-zone-floor-area}
+
+The minimum zone cooling volumetric flow rate per square meter (units are m\(^{3}\)/s-m\(^{2}\)). This field is used when \emph{Cooling Design Air Flow Method} is specified as \emph{DesignDayWithLimit}. In this case it sets a lower bound on the zone design cooling air flow rate. In all cases the maximum flow derived from \emph{Cooling Minimum Air Flow per Zone Floor Area}, \emph{Cooling Minimum Air Flow}, and \emph{Cooling Minimum Air Flow Fraction}~ is used to set a minimum supply air flow rate for the zone for VAV systems. The default is .000762, corresponding to .15 cfm/ft\(^{2}\).~ The applicable sizing factor is not applied to this value.
+
+\paragraph{Field: Cooling Minimum Air Flow}\label{field-cooling-minimum-air-flow}
+
+The minimum zone cooling volumetric flow rate in m\(^{3}\)/s. This field is used when \emph{Cooling Design Air Flow Method} is specified as \emph{DesignDayWithLimit}. In this case it sets a lower bound on the zone design cooling air flow rate. In all cases the maximum flow derived from \emph{Cooling Minimum Air Flow per Zone Floor Area}, \emph{Cooling Minimum Air Flow}, and \emph{Cooling Minimum Air Flow Fraction}~ is used to set a minimum supply air flow rate for the zone for VAV systems. The default is zero.~ The applicable sizing factor is not applied to this value.
+
+\paragraph{Field: Cooling Minimum Air Flow Fraction}\label{field-cooling-minimum-air-flow-fraction}
+
+The minimum zone design cooling volumetric flow rate expressed as a fraction of the zone design cooling volumetric flow rate. . In all cases the maximum flow derived from \emph{Cooling Minimum Air Flow per Zone Floor Area}, \emph{Cooling Minimum Air Flow}, and \emph{Cooling Minimum Air Flow Fraction}~ is used to set a minimum supply air flow rate for the zone for VAV systems. The default is zero. This input is currently used in sizing the fan minimum flow rate. It does not currently affect other component autosizing.
+
+\paragraph{Field: Heating Design Air Flow Method}\label{field-heating-design-air-flow-method}
+
+The input must be either \emph{Flow/Zone, DesignDay, or DesignDayWithLimit}. \emph{Flow/Zone} means that the program will use the input of the field \emph{Heating Design Air Flow Rate} as the zone design heating air flow rate. \emph{DesignDay} means the program will calculate the zone design heating air flow rate using the Sizing:Zone input data and a design day simulation without imposing any limits other than those set by the minimum outside air requirements. \emph{DesignDayWithLimit} means that the maximum from \emph{Heating Maximum Air Flow per Zone Floor Area} and \emph{Heating Maximum Air Flow} will set a lower limit on the design maximum heating air flow rate. The default method is \emph{DesignDay}: i.e., the program uses the calculated design values subject to ventilation requirements.
+
+\paragraph{Field: Heating Design Air Flow Rate}\label{field-heating-design-air-flow-rate}
+
+The design zone heating air flow rate in cubic meters per second. This input is used if \emph{Heating Design Air Flow Method} is specified as \emph{Flow/Zone}. This value will be multiplied by the global or zone sizing factor and by zone multipliers.
+
+\paragraph{Field: Heating Maximum Air Flow per Zone Floor Area}\label{field-heating-maximum-air-flow-per-zone-floor-area}
+
+The maximum zone heating volumetric flow rate per square meter (units are m\(^{3}\)/s-m\(^{2}\)). This field is used when \emph{Heating Design Air Flow Method} is specified as \emph{DesignDayWithLimit}. In this case it sets an upper bound on the zone design heating air flow rate. For this and the next two input fields, the maximum flow derived from \emph{Heating Maximum Air Flow per Zone Floor Area}, \emph{Heating Maximum Air Flow}, and \emph{Heating Maximum Air Flow Fraction}~ is used to set a maximum heating supply air flow rate for the zone for VAV systems. The default is .002032, corresponding to .40 cfm/ft\(^{2}\). If the maximum heating design flow rate calculated using these input fields is greater than the design heating flow rate calculated during sizing, these input fields have no impact on sizing. It may be more appropriate to select only one of these three fields to calculate the maximum heating design flow rate (i.e., if one ore more of these three fields is 0, it will not be used in calculating the maximum heating design flow rate).
+
+\paragraph{Field: Heating Maximum Air Flow}\label{field-heating-maximum-air-flow}
+
+The maximum zone heating volumetric flow rate in m\(^{3}\)/s. This field is used when \emph{Heating Design Air Flow Method} is specified as \emph{DesignDayWithLimit}. In this case it sets an upper bound on the zone design heating air flow rate. For this field and the two input fields just prior to and after this field,,the maximum flow derived from \emph{Heating Maximum Air Flow per Zone Floor Area}, \emph{Heating Maximum Air Flow}, and \emph{Heating Maximum Air Flow Fraction} is used to set a maximum heating supply air flow rate for the zone for VAV systems. The default is .1415762, corresponding to 300 cfm. If the maximum heating design flow rate calculated using these input fields is greater than the design heating flow rate calculated during sizing, these input fields have no impact on sizing. It may be more appropriate to select only one of these three fields to calculate the maximum heating design flow rate (i.e., if one ore more of these three fields is 0, it will not be used in calculating the maximum heating design flow rate).
+
+\paragraph{Field: Heating Maximum Air Flow Fraction}\label{field-heating-maximum-air-flow-fraction}
+
+The maximum zone design heating volumetric flow rate expressed as a fraction of the zone design cooling volumetric flow rate. For this and the previous two input fields, the maximum flow derived from \emph{Heating Maximum Air Flow per Zone Floor Area}, \emph{Heating Maximum Air Flow}, and \emph{Heating Maximum Air Flow Fraction}~ is used to set a maximum heating supply air flow rate for the zone for VAV systems. The default is 0.3. If the maximum heating design flow rate calculated using these input fields is greater than the design heating flow rate calculated during sizing, these input fields have no impact on sizing. It may be more appropriate to select only one of these three fields to calculate the maximum heating design flow rate (i.e., if one ore more of these three fields is 0, it will not be used in calculating the maximum heating design flow rate).
+
+\paragraph{Field: Design Specification Zone Air Distribution Object Name}\label{field-design-specification-zone-air-distribution-object-name}
+
+The name of the DesignSpecification:ZoneAirDistribution object, defining the air distribution effectiveness and secondary recirculation air fraction, that applies to the zone or zone list. This object may be used for the same zone in the Controller:MechanicalVentilation object if no such DesignSpecification:ZoneAirDistribution object is specified.
+
+\paragraph{Field: Account for Dedicated Outdoor Air System}\label{field-account-for-dedicated-outdoor-air-system}
+
+This is a choice field with choices \emph{Yes} or \emph{No}. The default is \emph{No}. Choosing \emph{Yes} means that the zone sizing calculation will use the subsequent inputs to calculate the heat gain or loss (heat gains are positive, heat loss is negative) imposed on the zone by a Dedicated Outdoor Air System (DOAS). This heat gain is then added to the zone design heat gain for the zone and the zone design air flow rate is adjusted to meet the DOAS heat gain plus the zone design heat gain.
+
+\paragraph{Field: Dedicated Outdoor Air System Control Strategy}\label{field-dedicated-outdoor-air-system-control-strategy}
+
+This is a choice field with a choice of three ideal control strategies for the DOA system. The choices are \emph{NeutralSupplyAir}, \emph{NeutralDehumidifiedSupplyAir}, or \emph{ColdSupplyAir}. The default is \emph{NeutralSupplyAir}.
+
+\emph{NeutralSupplyAir} implies that the ventilation air supplied to the zone will cause little heating or cooling. The air will be heated or cooled to keep it between the low and high temperature setpoints specified in the subsequent two fields. A good choice for these fields might be 21.1 and 23.9 degrees C.
+
+\emph{NeutralDehumidifiedSupplyAir} means that the ventilation air will be cooled and dehumidified and then reheated to a neutral temperature. The ventilation air is cooled to the lower setpoint temperature (if necessary) and reheated to the upper setpoint temperature. A good choice for the setpoints would be 14.4 and 22.2 degrees C.
+
+\emph{ColdSupplyAir} means that the ventilation air will be used to supply cooling to the zone. Cold outside air is heated to the upper setpoint; warm outside air is cooled to the lower setpoint. A good choice for the setpoints would be 12.2 and 14.4 degrees C.
+
+\paragraph{Field: Dedicated Outdoor Air Low Temperatue Setpoint for Design}\label{field-dedicated-outdoor-air-low-temperatue-setpoint-for-design}
+
+The lower setpoint temperature to be used with the DOAS design control strategy. The units are degrees C. The default is autosized to the values given above for the three design control strategies.
+
+\paragraph{Field: Dedicated Outdoor Air High Temperature Setpoint for Design}\label{field-dedicated-outdoor-air-high-temperature-setpoint-for-design}
+
+The higher setpoint temperature to be used with the DOAS design control strategy. The units are degrees C. The default is autosized to the values given above for the three design control strategies.
+
+An IDF example:
+
+\begin{lstlisting}
+
+Sizing:Zone,
+      SPACE5-1,                !- Name of a zone
+      14.,                     !- Zone cooling design supply air temperature {C}
+      50.,                     !- Zone heating design supply air temperature {C}
+      0.009,                   !- Zone cooling design supply air humidity ratio {kg-H2O/kg-air}
+      0.004,                   !- Zone heating design supply air humidity ratio {kg-H2O/kg-air}
+      DSOA1,                   !- Design Specification Outdoor Air Object Name
+      0.0,                     !- zone heating sizing factor
+      0.0,                     !- zone cooling sizing factor
+      designdaywithlimit,      !- Cooling Design Air Flow Method
+      ,                        !- cooling design air flow rate {m3/s}
+      ,                        !- Cooling Minimum Air Flow per zone area {m3/s-m2}
+      ,                        !- Cooling Minimum Air Flow {m3/s}
+      ,                        !- fraction of the cooling design air flow rate
+      designday,               !- Heating Design Air Flow Method
+      ,                        !- heating design air flow rate {m3/s}
+      ,                        !- heating max air flow per zone area {m3/s-m2}
+      ,                        !- heating max air flow {m3/s}
+      ,                        !- fraction of the cooling design air flow rate
+      DSZADO1,                 !- Design Specification Zone Air Distribution Object Name
+      Yes,                     !- Account for Dedicated Outside Air System
+      ColdSupplyAir,           !- Dedicated Outside Air System Control Strategy
+      12.2,                    !- Dedicated Outside Air Low Setpoint for Design
+      14.4;                    !- Dedicated Outside Air High Setpoint for Design
+
+  DesignSpecification:OutdoorAir,
+  DSOA1,                   !- Name
+  SUM,                     !- Outdoor Air Method
+  0.00236,                 !- Outdoor Air Flow per Person
+  0.000305,                !- Outdoor Air Flow per Zone Floor Area
+  0.0,                     !- Outdoor Air Flow per Zone
+  0.0,                     !- Outdoor Air Flow Air Changes per Hour
+  ;                        !- Outdoor Air Flow Rate Fraction Schedule Name
+
+  DesignSpecification:ZoneAirDistribution,
+      DSZADO1,                 !- Name
+      1.0,                     !- Zone Air Distribution Effectiveness in Cooling Mode
+      1.0,                     !- Zone Air Distribution Effectiveness in Heating Mode
+      ,                        !- Zone Air Distribution Effectiveness Schedule Name
+      0.3;                     !- Zone Secondary Recirculation Fraction
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-007}
+
+The zone design air flow rates and loads are output onto the local file ``epluszsz.\textless{}ext\textgreater{}'' where \textless{}ext\textgreater{} is the extension from the sizing style object (default is csv -- a comma separated file \emph{epluszsz.csv)}. The columns are clearly labeled. It will easily import into Excel or other spreadsheet program that accepts delimited files. All of these values are design air flow rates and loads \emph{calculated by the program}. No sizing factors have been applied.
+
+The calculated zone design air flow rates and the user input or altered zone design air flow rates are also reported on the \emph{eplusout.eio} file. The values are printed out for each zone as comma separated records beginning with \emph{Zone Sizing}. Items output on the \emph{eio} file are: zone name, load type (heating or cooling), design load, calculated design air flow rate, user design air flow rate, design day name, time of peak, outside temperature at peak, outside humidity ratio at peak.
+
+\subsection{DesignSpecification:ZoneHVAC:Sizing}\label{designspecificationzonehvacsizing}
+
+This object is used to describe general sizing and scalable sizing methods which are referenced by zone HVAC equipment objects. It is optional input field in zone HVAC objects. If a name of this optional input is not specified or is blank then the sizing method or input specified in the parent object is used.~ If the name of this object is entered, then the values or method specified overrides the sizing method in the parent zone HVAC objects. This object is meant to provide scalable sizing method to users. The name of this object is an optional input field in the zoneHVAC objects. When this name in not specified in the zone HVAC object the sizing method or the value specified in the zone HVAC object will be used.
+
+List of zoneHVAC objects than can reference this object include:
+
+\begin{itemize}
+\item
+  ZoneHVAC:TerminalUnit:VariableRefrigerantFlow
+\item
+  ZoneHVAC:PackagedTerminalAirConditioner
+\item
+  ZoneHVAC:PackagedTerminalHeatPump
+\item
+  ZoneHVAC:WaterToAirHeatPump
+\item
+  ZoneHVAC:WindowAirConditioner
+\item
+  ZoneHVAC:UnitHeater
+\item
+  ZoneHVAC:UnitVentilator
+\item
+  ZoneHVAC:FourPipeFanCoil
+\item
+  ZoneHVAC:VentilatedSlab
+\item
+  ZoneHVAC:EvaporativeCoolerUnit
+\item
+  ZoneHVAC:IdealLoadsAirSystem
+\end{itemize}
+
+The sizing methods input fields available in this objects are for supply air flow and capacity for heating and cooling operating modes. Some zone HVAC equipment has single supply air flow rate input field that serves both cooling and heating operating modes.~ So entering either of the cooling or heating scalable sizing input field is sufficient.~ When there are separate input fields for cooling, heating, no-cooling, and no-heating operating modes, the corresponding input fields are specified.~ The child components supply air flow rate are also sized using scalable sizing methods specified in the parent objects. The methods allow users to enter a fixed or hard sized values, autosizable, or scalable sizing methods.~ Methods allowed for sizing supply air flow rates include: \emph{SupplyAirFlowRate}, \emph{FractionOfAutosizedCoolingAirflow}, \emph{FractionOfAutosizedHeatingAirflow}, \emph{FlowPerFloorArea, FlowPerCoolingCapacity}, and \emph{FlowPerHeatingCapacity}.~ The different sizing options are defined as follows:
+
+\begin{itemize}
+\item
+  \textbf{SupplyAirFlowRate}: entered when it is intended that the user specified either hard value or the simulation engine autosize the supply air flow rates for cooling, heating, and no-cooling or no-heating operating modes.
+\item
+  \textbf{FlowPerFloorArea}: entered when it is intended that the simulation engine determine the supply air flow rates from the user specified \emph{supply air flow rates per unit floor area} and the zone floor area of the zone served by the zone HVAC equipment.
+\item
+  \textbf{FractionOfAutosizedCoolingAirflow}: entered when it is intended that the simulation engine determines the supply air flow rates from the user specified \emph{flow fraction} and \emph{autosized cooling design supply air flow rate}.
+\item
+  \textbf{FractionOfAutosizedHeatingAirflow}: entered when it is intended that the simulation engine determines the supply air flow rates from the user specified \emph{flow fraction} and \emph{autosized heating design supply air flow rate}.
+\item
+  \textbf{FlowPerCoolingCapacity}: entered when it is intended t that he simulation engine determines the supply air flow rates from the user specified \emph{supply air flow per cooling capacity value} and \emph{autosized cooling design capacity}.
+\item
+  \textbf{FlowPerHeatingCapacity}: entered when it is intended that the simulation engine determines the supply air flow rates from the user specified \emph{supply air flow per heating capacity value} and \emph{autosized heating design capacity}.
+\end{itemize}
+
+The~ Design Specification ZoneHVAC Sizing object also has input fields for sizing or scalable sizing of cooling and heating capacity. However, most of the parent zone HVAC objects do not have input fields for sizing capacities. So, the capacity scalable sizing fields in the parent objects are used for sizing child components capacity sizings.~ The scalable capacity sizing may be indirectly impacted by the scalable supply air flow rates sizing values. Moreover, the autosized cold water, hot water and steam flow rates in the parent zone HVAC objects (e.g.~FanCoils, UnitHeaters, UnitVentilators, and VentilatedSlabs) and capacity in child components are determined using the scalable sizing methods.~ Sizing methods allowed for cooling and heating capacity include: \emph{CoolingDesignCapacity, HeatingDesignCapacity}, \emph{CapacityPerFloorArea, FractionOfAutosizedCoolingCapacity}, \emph{FractionOfAutosizedHeatingCapacity}.
+
+\begin{itemize}
+\item
+  \textbf{CoolingDesignCapacity}: entered when it is intended that user specifies either a hard sized cooling capacity value or the simulation engine autosizes cooling capacity value for the cooling design capacity.
+\item
+  \textbf{HeatingDesignCapacity}: entered when it is intended that user specifies either a hard sized heating capacity value or the simulation engine autosized heating capacity value for the heating design capacity.
+\item
+  \textbf{CapacityPerFloorArea}: is entered when it is intended that the simulation engine determines the cooling or heating capacity from user specified capacity per floor area value and the floor area of the zone served by the zone HVAC equipment.
+\item
+  \textbf{FractionOfAutosizedCoolingCapacity}: entered when it is intended that the simulation engine sizes the cooling capacity from the user specified \emph{capacity fraction} and \emph{autosized cooling design capacity} value.
+\item
+  \textbf{FractionOfAutosizedHeatingCapacity}: entered when it is intended that the simulation engine sizes the heating capacity from the user specified \emph{capacity fraction} and \emph{autosized heating design capacity} value.
+\end{itemize}
+
+Description of the input fields of the design specification zone HVAC sizing object ``DesignSpecification:ZoneHVAC:Sizing'':
+
+\subsubsection{Inputs}\label{inputs-5-007}
+
+\paragraph{Field: Name}\label{field-name-2-009}
+
+Unique identifier name of the DesignSpecification:ZoneHVAC:Sizing object. This sizing specification object referenced by a zone HVAC equipment whose design calculation will be made using the input data of this object.
+
+\paragraph{Field: Cooling Design Air Flow Method}\label{field-cooling-design-air-flow-method-1}
+
+The input of this field must be the method used to determine the cooling supply air volume flow rate. Input allowed is either \emph{None}, \emph{SupplyAirFlowRate}, \emph{FlowPerFloorArea}, \emph{FractionOfAutosizedCoolingAirflow}, or \emph{FlowPerCoolingCapacity}.~ None means cooling coil is not included in the zone HVAC equipment or this field may be left blank. \emph{SupplyAirFlowRate} means the user specifies the magnitude of supply air flow rate or the program calculates the design cooling supply air volume flow rate if autosize is specified. \emph{FlowPerFloorArea} means the program calculates the cooling supply air volume flow rate from zone floor area served by the zone HVAC unit and user specified \emph{Flow Per Floor Area} value. \emph{FractionOfAutosizedCoolingAirflow} means the program calculates the cooling supply air volume flow rate from user specified fraction and the autosized design cooling supply air volume flow rate value determined by the simulation. FlowPerCoolingCapacity means the supply air volume is calculated from user specified flow per cooling capacity and design cooling capacity determined by the simulation. The default method is \emph{SupplyAirFlowRate}.
+
+\paragraph{Field: Cooling Design Supply Air Flow Rate \{m3/s\}}\label{field-cooling-design-supply-air-flow-rate-m3s}
+
+Enter the magnitude of the cooling supply air volume flow rate in m3/s. This input is an alternative to using the program auto-calculated value. This input is a required field when the Cooling Design air Flow Method is \emph{SupplyAirFlowRate}. This field may be left blank if a cooling coil is not included in the zone HVAC equipment. This input field is also autosizable.
+
+\paragraph{Field: Cooling Design Supply Air Flow Rate Per Floor Area \{m3/s-m2\}}\label{field-cooling-design-supply-air-flow-rate-per-floor-area-m3s-m2}
+
+Enter the cooling supply air volume flow rate per zone conditioned floor area in m3/s-m2. This field is required field when the Cooling Design air Flow Method is \emph{FlowPerFloorArea}. This field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design Air Flow Method is not \emph{FlowPerFloorArea}. The program calculates the cooling supply air volume flow rate from the zone conditioned floor area served by the zone HVAC equipment and the flow per unit area value specified by the user. Zone sizing object (Sizing:Zone) is not required.
+
+\paragraph{Field: Fraction of Autosized Cooling Design Supply Air Flow Rate}\label{field-fraction-of-autosized-cooling-design-supply-air-flow-rate}
+
+Enter the cooling supply air volume flow rate as a fraction of the autosized cooling supply air flow rate. This input field is required when the Cooling Design air Flow Method is \emph{FractionOfAutosizedCoolingAirflow}. This input field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design air Flow Method is not \emph{FractionOfAutosizedCoolingAirflow}. The program calculates the cooling supply air volume flow rate from the design autosized cooling supply air flow rate and user specified fraction. Zone sizing object (Sizing:Zone) is required.
+
+\paragraph{Field: Cooling Design Supply Air Flow Rate Per Unit Cooling Capacity \{m3/s-W\}}\label{field-cooling-design-supply-air-flow-rate-per-unit-cooling-capacity-m3s-w}
+
+Enter the cooling supply air volume flow rate per unit cooling capacity in m3/s-W. This input field is required when the Cooling Design air Flow Method is \emph{FlowPerCoolingCapacity}. This field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design air Flow Method is not \emph{FlowPerCoolingCapacity}. The program calculates the cooling supply air volume flow rate from the design autosized cooling capacity and user specified flow per cooling capacity value. Zone sizing object (Sizing:Zone) is required.
+
+\paragraph{Field: Supply Air Flow Rate Method When No Cooling or Heating is Required}\label{field-supply-air-flow-rate-method-when-no-cooling-or-heating-is-required}
+
+Enter the method used to determine the supply air volume flow rate when No Cooling or Heating is required. Inputs allowed are \emph{None}, \emph{SupplyAirFlowRate}, \emph{FlowPerFloorArea}, \emph{FractionOfAutosizedCoolingAirflow}, and \emph{FractionOfAutosizedHeatingAirflow.} \emph{None} is used when a cooling or heating coil is not included in the zone HVAC equipment or this field may be left blank. \emph{SupplyAirFlowRate} means user specifies the magnitude of supply air flow rate or the program calculates the design supply air volume flow rate if autosize is specified. \emph{FlowPerFloorArea} means the program calculates the supply air volume flow rate from the zone floor area served by the zone HVAC unit and Flow Per Floor Area value specified by user. \emph{FractionOfAutosizedCoolingAirflow} means the program calculates the supply air volume flow rate from user specified fraction and autosized design cooling supply air volume flow rate value determined by the program. FractionOfAutosizedHeatingAirflow means the program calculates the supply air volume flow rate from user specified fraction and autosized heating supply air flow rate value determined by the program. The default method is \emph{SupplyAirFlowRate}.
+
+\paragraph{Field: Supply Air Flow Rate When No Cooling or Heating is Required \{m3/s\}}\label{field-supply-air-flow-rate-when-no-cooling-or-heating-is-required-m3s}
+
+Enter the magnitude of the supply air volume flow rate when no cooling or heating is required in m3/s. This input is an alternative to using the program auto-calculated value. This input is a required field when the Supply Air Flow Rate Method When No Cooling or Heating is Required is \emph{SupplyAirFlowRate}. This field may be left blank if a cooling coil is not included in the zone HVAC equipment. This input field is also autosizable.
+
+\paragraph{Field: Supply Air Flow Rate Per Floor Area When No Clg or Htg is Required~ \{m3/s-m2\}}\label{field-supply-air-flow-rate-per-floor-area-when-no-clg-or-htg-is-required-m3s-m2}
+
+Enter the magnitude of supply air volume flow rate per zone floor area in m3/s-m2. This input is a required field when Supply Air ~Flow Rate Method When No Cooling or Heating is Required is \emph{FlowPerFloorArea}. The program calculates the supply air flow rate when no cooling or heating is required from user specified flow per floor area and the zone area served by current zoneHVAC equipment.
+
+\paragraph{~Field: Fraction of Design Cooling Supply Air Flow Rate When No Clg or Htg Required}\label{field-fraction-of-design-cooling-supply-air-flow-rate-when-no-clg-or-htg-required}
+
+Enter the fraction of supply air volume flow rate as a fraction of the autosized cooling supply air flow rate. This input field is required field when Supply Air Flow Rate Method When No Cooling or Heating is Required is \emph{FractionOfAutosizedCoolingAirflow}.~ The program calculates the supply air flow rate when no cooling or heating is required from user specified fraction and the design cooling autosized supply air flow rate.
+
+\paragraph{Field: Fraction of Design Heating Supply Air Flow Rate When No Clg or Htg Required}\label{field-fraction-of-design-heating-supply-air-flow-rate-when-no-clg-or-htg-required}
+
+Enter the fraction of supply air volume flow rate as a fraction of the autosized cooling supply air flow rate. This input field is required field when Supply Air Flow Rate Method When No Cooling or Heating is Required is \emph{FractionOfAutosizedHeatingAirflow}.~ The program calculates the supply air flow rate when no cooling or heating is required from user specified fraction and the design heating autosized supply air flow rate.
+
+\paragraph{Field: Heating Design Air Flow Method}\label{field-heating-design-air-flow-method-1}
+
+The input of this field must be the method used to determine the heating supply air volume flow rate. Input allowed is either \emph{None}, \emph{SupplyAirFlowRate}, \emph{FlowPerFloorArea}, \emph{FractionOfAutosizedCoolingAirflow}, or \emph{FlowPerCoolingCapacity}.~ \emph{None} means heating coil is not included in the zone HVAC equipment or this field may be left blank. \emph{SupplyAirFlowRate} means the user specifies the magnitude of supply air flow rate or the program calculates the design heating supply air volume flow rate if autosize is specified. \emph{FlowPerFloorArea} means the program calculates the heating supply air volume flow rate from zone floor area served by the zone HVAC unit and user specified \emph{Flow Per Floor Area} value. \emph{FractionOfAutosizedHeatingAirflow} means the program calculates the heating supply air volume flow rate from user specified fraction and the autosized design heating supply air volume flow rate value determined by the simulation. \emph{FlowPerHeatingCapacity} means the supply air volume is calculated from user specified flow per heating capacity and design heating capacity determined by the simulation. The default method is \emph{SupplyAirFlowRate}.
+
+\paragraph{Field: Heating Design Supply Air Flow Rate \{m3/s\}}\label{field-heating-design-supply-air-flow-rate-m3s}
+
+Enter the magnitude of the heating supply air volume flow rate in m3/s. This input is an alternative to using the program auto-calculated value. This input is a required field when the Heating Design air Flow Method is \emph{SupplyAirFlowRate}. This field may be left blank if a heating coil is not included in the zone HVAC equipment. This input field is also autosizable.
+
+\paragraph{Field: Heating Design Supply Air Flow Rate Per Floor Area \{m3/s-m2\}}\label{field-heating-design-supply-air-flow-rate-per-floor-area-m3s-m2}
+
+Enter the heating supply air volume flow rate per zone conditioned floor area in m3/s-m2. This field is required field when the Heating Design air Flow Method is \emph{FlowPerFloorArea}. This field may be left blank if a heating coil is not included in the zone HVAC equipment or the Heating Design Air Flow Method is not \emph{FlowPerFloorArea}. The program calculates the heating supply air volume flow rate from the zone conditioned floor area served by the zone HVAC equipment and the flow per unit area value specified by the user.
+
+\paragraph{Field: Fraction of Autosized Heating Design Supply Air Flow Rate}\label{field-fraction-of-autosized-heating-design-supply-air-flow-rate}
+
+Enter the heating supply air volume flow rate as a fraction of the autosized heating supply air flow rate. This input field is required when the Heating Design air Flow Method is \emph{FractionOfAutosizedHeatingAirflow}. This input field may be left blank if a heating coil is not included in the zone HVAC equipment or the Heating Design air Flow Method is not \emph{FractionOfAutosizedHeatingAirflow}. The program calculates the heating supply air volume flow rate from the design autosized heating supply air flow rate and user specified fraction.
+
+\paragraph{Field: Heating Design Supply Air Flow Rate Per Unit Heating Capacity \{m3/s-W\}}\label{field-heating-design-supply-air-flow-rate-per-unit-heating-capacity-m3s-w}
+
+Enter the heating supply air volume flow rate per unit heating capacity in m3/s-W. This input field is required when the Heating Design air Flow Method is \emph{FlowPerHeatingCapacity}. This field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Heating Design air Flow Method is not \emph{FlowPerHeatingCapacity}. The program calculates the heating supply air volume flow rate from the design autosized heating capacity and user specified flow per unit heating capacity value.
+
+\paragraph{Field Cooling Design Capacity Method}\label{field-cooling-design-capacity-method}
+
+Enter the method used to determine the cooling design capacity for scalable sizing. Input allowed is either \emph{None}, \emph{CoolingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedCoolingCapacity}. None is used when a cooling coil is not included in the Zone HVAC equipment or this field may be left blank. If this input field is left blank, then the design cooling capacity is set to zero. \emph{CoolingDesignCapacity} means user specifies the magnitude of cooling capacity or the program calculates the design cooling capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design cooling capacity from user specified cooling capacity per floor area and floor area of the zone served by the HVAC unit. \emph{FractionOfAutosizedCoolingCapacity} means the program calculates the design cooling capacity from user specified fraction and the auto-sized design cooling capacity. The default method is \emph{CoolingDesignCapacity}.
+
+\paragraph{Field: Cooling Design Capacity \{W\}}\label{field-cooling-design-capacity-w}
+
+Enter the magnitude of the cooling capacity in Watts. This input is an alternative to using the program auto-calculated cooling capacity value. This input is a required field when the Cooling Design Capacity Method is \emph{CoolingDesignCapacity}. This field may be left blank if a cooling coil is not included in the zone HVAC equipment or alternative method is specified. This input field is autosizable. Design day sizing run must be specified.
+
+\paragraph{Field: Cooling Design Capacity Per Floor Area \{W/m2\}}\label{field-cooling-design-capacity-per-floor-area-wm2}
+
+Enter the cooling capacity per unit floor area in m3/s-m2. This field is required field when the Cooling Design Capacity Method is \emph{CapacityPerFloorArea}. This field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design Capacity Method is not \emph{CapacityPerFloorArea}. The program calculates the cooling capacity from floor area of the zone served by the zone HVAC equipment and the cooling capacity per unit floor area value specified by the user.
+
+\paragraph{Field: Fraction of Autosized Cooling Design Capacity}\label{field-fraction-of-autosized-cooling-design-capacity}
+
+Enter the cooling capacity as a fraction of the autosized cooling capacity. This input field is required when the Cooling Design Capacity Method is \emph{FractionOfAutosizedCoolingCapacity}. This input field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design Capacity Method is not \emph{FractionOfAutosizedCoolingCapacity}. The program calculates the cooling capacity from the design autosized cooling capacity and user specified fraction. Design day sizing run must be specified.
+
+\paragraph{Field: Heating Design Capacity Method}\label{field-heating-design-capacity-method}
+
+Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either \emph{None}, \emph{HeatingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedHeatingCapacity}. None is used when a heating coil is not included in the Zone HVAC equipment or this field may be left blank. If this input field is left blank, then the design heating capacity is set to zero. \emph{HeatingDesignCapacity} means user specifies the magnitude of heating capacity or the program calculates the design heating capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the HVAC unit. \emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is \emph{HeatingDesignCapacity}.
+
+\paragraph{Field: Heating Design Capacity \{W\}}\label{field-heating-design-capacity-w}
+
+Enter the magnitude of the heating capacity in Watts. This input is an alternative to using the program auto-calculated heating capacity value. This input is a required field when the Heating Design Capacity Method is \emph{HeatingDesignCapacity}. This field may be left blank if a heating coil is not included in the zone HVAC equipment or alternative method is specified. This input field is autosizable. Design day sizing run must be specified.
+
+\paragraph{Field: Heating Design Capacity Per Floor Area \{W/m2\}}\label{field-heating-design-capacity-per-floor-area-wm2}
+
+Enter the heating capacity per unit floor area in m3/s-m2. This field is required field when the Heating Design Capacity Method is \emph{CapacityPerFloorArea}. This field may be left blank if a heating coil is not included in the zone HVAC equipment or the Heating Design Capacity Method is not \emph{CapacityPerFloorArea}. The program calculates the heating capacity from floor area of the zone served by the zone HVAC equipment and the heating capacity per unit floor area value specified by the user.
+
+\paragraph{Field: Fraction of Autosized Heating Design Capacity}\label{field-fraction-of-autosized-heating-design-capacity}
+
+Enter the heating capacity as a fraction of the autosized heating capacity. This input field is required when the Heating Design Capacity Method is \emph{FractionOfAutosizedHeatingCapacity}. This input field may be left blank if a heating coil is not included in the zone HVAC equipment or the Heating Design Capacity Method is not \emph{FractionOfAutosizedHeatingCapacity}. The program calculates the heating capacity from the design autosized cooling capacity and user specified fraction. Design day sizing run must be specified.
+
+\begin{lstlisting}
+
+  DesignSpecification:ZoneHVAC:Sizing,
+      VRFDesignSpec1,          !- Name
+      SupplyAirFlowRate,       !- Cooling Design Air Flow Method
+      autosize,                !- Cooling Design Supply Air Flow Rate
+      ,                        !- Cooling Design Supply Air Flow Rate Per Floor Area
+      ,                        !- Fraction of Autosized Cooling Design Supply Air Flow Rate
+      ,                        !- Cooling Design Supply Air Flow Rate Per Unit of Capacity {m3/s-W}
+      SupplyAirFlowRate,       !- Supply Air Flow Rate Method When No Cooling or Heating is Required
+      autosize,                !- Supply Air Flow Rate When No Cooling or Heating is Required
+      ,                        !- Supply Air Flow Rate Per Floor Area When No Clg or Htg is Required
+      ,                     !- Fraction of Autosized Design Cooling Supply Air Flow Rate When No Clg or Htg
+      ,                     !- Fraction of Autosized Design Heating Supply Air Flow Rate When No Clg or Htg
+      SupplyAirFlowRate,       !- Heating Design Air Flow Method
+      autosize,                !- Heating Design Supply Air Flow Rate
+      ,                        !- Heating Design Supply Air Flow Rate Per Floor Area
+      ,                        !- Fraction of Autosized Heating Design Supply Air Flow Rate
+      ,                        !- Heating Design Supply Air Flow Rate Per Unit of Heating Capacity
+      CoolingDesignCapacity,   !- Cooling Design Capacity Method
+      autosize,                !- Cooling Design Capacity {W}
+      ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
+      ,                        !- Fraction of Autosized Cooling Design Capacity {-}
+      HeatingDesignCapacity,   !- Heating Design Capacity Method
+      autosize,                !- Heating Design Capacity {W}
+      ,                        !- Heating Design Capacity Per Floor Area {W/m2}
+      ;                        !- Fraction of Autosized Cooling Design Capacity {-}
+
+    DesignSpecification:ZoneHVAC:Sizing,
+      VRFDesignSpec2,          !- Name
+      FlowPerFloorArea,        !- Cooling Design Air Flow Method
+      ,                        !- Cooling Design Supply Air Flow Rate
+      3.6311418E-03,           !- Cooling Design Supply Air Flow Rate Per Floor Area
+      ,                        !- Fraction of Autosized Cooling Design Supply Air Flow Rate
+      ,                        !- Cooling Design Supply Air Flow Rate Per Unit of Capacity {m3/s-W}
+      FlowPerFloorArea,        !- Supply Air Flow Rate Method When No Cooling or Heating is Required
+      ,                        !- Supply Air Flow Rate When No Cooling or Heating is Required
+      3.6311418E-03,           !- Supply Air Flow Rate Per Floor Area When No Clg or Htg is Required
+      ,                     !- Fraction of Autosized Design Cooling Supply Air Flow Rate When No Clg or Htg
+      ,                     !- Fraction of Autosized Design Heating Supply Air Flow Rate When No Clg or Htg
+      FlowPerFloorArea,        !- Heating Design Air Flow Method
+      ,                        !- Heating Design Supply Air Flow Rate
+      3.6311418E-03,           !- Heating Design Supply Air Flow Rate Per Floor Area
+      ,                        !- Fraction of Autosized Heating Design Supply Air Flow Rate
+      ,                        !- Heating Design Supply Air Flow Rate Per Unit of Heating Capacity
+      CoolingDesignCapacity,   !- Cooling Design Capacity Method
+      autosize,                !- Cooling Design Capacity {W}
+      ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
+      ,                        !- Fraction of Autosized Cooling Design Capacity {-}
+      HeatingDesignCapacity,   !- Heating Design Capacity Method
+      autosize,                !- Heating Design Capacity {W}
+      ,                        !- Heating Design Capacity Per Floor Area {W/m2}
+      ;                        !- Fraction of Autosized Cooling Design Capacity {-}
+
+  DesignSpecification:ZoneHVAC:Sizing,
+      VRFDesignSpec3,          !- Name
+      FractionOfAutosizedCoolingAirflow,  !- Cooling Design Air Flow Method
+      ,                        !- Cooling Design Supply Air Flow Rate
+      ,                        !- Cooling Design Supply Air Flow Rate Per Floor Area
+      0.5,                     !- Fraction of Autosized Cooling Design Supply Air Flow Rate
+      ,                        !- Cooling Design Supply Air Flow Rate Per Unit of Capacity {m3/s-W}
+    FractionOfAutosizedCoolingAirflow, !- Supply Air Flow Rate Method When No Cooling or Heating is Required
+      ,                        !- Supply Air Flow Rate When No Cooling or Heating is Required
+      ,                        !- Supply Air Flow Rate Per Floor Area When No Clg or Htg is Required
+      0.5,                 !- Fraction of Autosized Design Cooling Supply Air Flow Rate When No Clg or Htg
+      ,                    !- Fraction of Autosized Design Heating Supply Air Flow Rate When No Clg or Htg
+      FractionOfAutosizedHeatingAirflow,  !- Heating Design Air Flow Method
+      ,                        !- Heating Design Supply Air Flow Rate
+      ,                        !- Heating Design Supply Air Flow Rate Per Floor Area
+      0.5,                     !- Fraction of Autosized Heating Design Supply Air Flow Rate
+      ,                        !- Heating Design Supply Air Flow Rate Per Unit of Heating Capacity
+      CoolingDesignCapacity,   !- Cooling Design Capacity Method
+      autosize,                !- Cooling Design Capacity {W}
+      ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
+      ,                        !- Fraction of Autosized Cooling Design Capacity {-}
+      HeatingDesignCapacity,   !- Heating Design Capacity Method
+      autosize,                !- Heating Design Capacity {W}
+      ,                        !- Heating Design Capacity Per Floor Area {W/m2}
+      ;                        !- Fraction of Autosized Cooling Design Capacity {-}
+
+  DesignSpecification:ZoneHVAC:Sizing,
+      VRFDesignSpec4,          !- Name
+      FlowPerCoolingCapacity,  !- Cooling Design Air Flow Method
+      ,                        !- Cooling Design Supply Air Flow Rate
+      ,                        !- Cooling Design Supply Air Flow Rate Per Floor Area
+      ,                        !- Fraction of Autosized Cooling Design Supply Air Flow Rate
+      2.9541628E-05,           !- Cooling Design Supply Air Flow Rate Per Unit of Capacity {m3/s-W}
+    FractionOfAutosizedHeatingAirflow, !- Supply Air Flow Rate Method When No Cooling or Heating is Required
+      ,                        !- Supply Air Flow Rate When No Cooling or Heating is Required
+      ,                        !- Supply Air Flow Rate Per Floor Area When No Clg or Htg is Required
+      ,                    !- Fraction of Autosized Design Cooling Supply Air Flow Rate When No Clg or Htg
+      0.413231177,         !- Fraction of Autosized Design Heating Supply Air Flow Rate When No Clg or Htg
+      FlowPerHeatingCapacity,  !- Heating Design Air Flow Method
+      ,                        !- Heating Design Supply Air Flow Rate
+      ,                        !- Heating Design Supply Air Flow Rate Per Floor Area
+      ,                        !- Fraction of Autosized Heating Design Supply Air Flow Rate
+      2.9541628E-05,           !- Heating Design Supply Air Flow Rate Per Unit of Heating Capacity
+      CoolingDesignCapacity,   !- Cooling Design Capacity Method
+      autosize,                !- Cooling Design Capacity {W}
+      ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
+      ,                        !- Fraction of Autosized Cooling Design Capacity {-}
+      HeatingDesignCapacity,   !- Heating Design Capacity Method
+      autosize,                !- Heating Design Capacity {W}
+      ,                        !- Heating Design Capacity Per Floor Area {W/m2}
+      ;                        !- Fraction of Autosized Cooling Design Capacity {-}
+\end{lstlisting}
+
+\subsection{Sizing:System}\label{sizingsystem}
+
+The Sizing:System object contains the input needed to perform a central forced air system design air flow, heating capacity, and cooling capacity calculation for a system serving one or more zones. The information needed consists of the outside environmental conditions and the design supply air temperatures, outdoor air flow rate, and minimum system air flow ratio.
+
+The outside conditions come from the design days in the input. A system sizing calculation is performed for every design day in the input file and the resulting maximum heating and cooling air flow rates and capacities are saved for use in the component sizing calculations.
+
+Supply air conditions are specified by inputting a supply air temperature for cooling, a supply air temperature for heating, and a preheat temperature.
+
+The system sizing calculation sums the zone design air flow rates to obtain a system supply air flow rate. The design conditions and the outdoor air flow rate are used to calculate a design mixed air temperature. The temperature plus the design supply air temperatures allows the calculation of system design heating and cooling capacities.
+
+\subsubsection{Inputs}\label{inputs-6-006}
+
+\paragraph{Field: AirLoop Name}\label{field-airloop-name}
+
+The name of the AirLoopHVAC corresponding to this Sizing:System object. This is the air system for which the design calculation will be made using the input data of this Sizing:System Object.
+
+\paragraph{Field: Type of Load to Size On}\label{field-type-of-load-to-size-on}
+
+The user specified type of load on which to size the central system. The choices are \emph{Sensible}, \emph{Total} and \emph{VentilationRequirement}. \emph{Sensible} and \emph{Total} mean that the central system supply air flow rate will be determined by combining the zone design air flow rates, which have been calculated to meet the zone sensible loads from the design days. \emph{VentilationRequirement} means that the central system supply air flow rate will be determined by the system ventilation requirement. In addition \emph{Sensible} tells the program to size the central cooling coil using entering air flow rate and air conditions at the sensible load peak; \emph{Total} indicates that the program should size the central cooling coil at the air flow rate and conditions at the total load peak. The central heating coil is always sized at the conditions at the peak sensible heating load.
+
+\paragraph{Field: Design Outdoor Air Flow Rate}\label{field-design-outdoor-air-flow-rate}
+
+The design outdoor air flow rate in cubic meters per second. Generally this should be the minimum outdoor air flow. It is used for both heating and cooling design calculations. The assumption for cooling is that any outdoor air economizer will be closed. If \emph{Autosize} is input the outdoor air flow rate will be taken from the sum of the zone outdoor air flow rates or calculated based on the System Outdoor Air Method selection (field below).
+
+\paragraph{Field: Central Heating Maximum System Air Flow Ratio}\label{field-central-heating-maximum-system-air-flow-ratio}
+
+The ratio of the maximum system air flow rate for heating to the maximum system air flow rate. The value must be between 0 and 1. For constant volume systems the ratio should be set to 1. This ratio should be set to reflect what the user expects the system flow rate to be when maximum heating demand occurs. This ratio is used in calculating the central system heating capacity. Thus if the system is VAV with the zone VAV dampers held at minimum flow when there is a zone heating demand, this ratio should be set to the minimum flow ratio. If the zone VAV dampers are reverse action and can open to full flow to meet heating demand, this ratio should be set to 1. The default is set to 0.5, reflecting the fact that VAV dampers are typically not allowed to fully open during heating.
+
+\paragraph{Field: Preheat Design Temperature}\label{field-preheat-design-temperature}
+
+The design air temperature exiting the preheat coil (if any) in degrees Celsius.
+
+\paragraph{Field: Preheat Design Humidity Ratio}\label{field-preheat-design-humidity-ratio}
+
+The design humidity ratio exiting the preheat coil (if any) in kilograms of water per kilogram of dry air. (kgWater/kgDryAir)
+
+\paragraph{Field: Precool Design Temperature}\label{field-precool-design-temperature}
+
+The design air temperature exiting the precooling coil (if any) in degrees Celsius.
+
+\paragraph{Field: Precool Design Humidity Ratio}\label{field-precool-design-humidity-ratio}
+
+The design humidity ratio exiting the precooling coil (if any) in kilograms of water per kilogram of dry air. (kgWater/kgDryAir)
+
+\paragraph{Field: Central Cooling Design Supply Air Temperature}\label{field-central-cooling-design-supply-air-temperature}
+
+The design supply air temperature for cooling in degrees Celsius. This should be the temperature of the air exiting the central cooling coil.
+
+\paragraph{Field: Central Heating Design Supply Air Temperature}\label{field-central-heating-design-supply-air-temperature}
+
+The design supply air temperature for heating in degrees Celsius. This can be either the reset temperature for a single duct system or the actual hot duct supply air temperature for dual duct systems. It should be the temperature at the exit of the main heating coil. This value is also used for the sizing of zone equipment (e.g., reheat coil) for the system embedded with central heating coils, but it is not used if there is no central heating coil in the system.
+
+\paragraph{Field: Type of Zone Sum to Use}\label{field-type-of-zone-sum-to-use}
+
+If the input is \emph{coincident} the central system air flow rate will be sized on the sum of the coincident zone air flow rates. If the input is \emph{noncoincident} the central system air flow rate will be sized on the sum of the noncoincident zone air flow rates. The default is noncoincident.
+
+\paragraph{Field: 100\% Outdoor Air in Cooling}\label{field-100-outdoor-air-in-cooling}
+
+Entering \emph{Yes} means the system will be sized for cooling using 100\% outdoor air. Entering \emph{No} means the system will be sized for cooling using minimum outside air (the default).
+
+\paragraph{Field: 100\% Outdoor Air in Heating}\label{field-100-outdoor-air-in-heating}
+
+Entering \emph{Yes} means the system will be sized for heating using 100\% outdoor air. Entering \emph{No} means the system will be sized for heating using minimum outside air (the default).
+
+\paragraph{Field: Central Cooling Design Supply Air Humidity Ratio}\label{field-central-cooling-design-supply-air-humidity-ratio}
+
+The design humidity ratio in kilograms of water per kilogram of dry air at the exit of the central cooling coil. The default is .008 (kgWater/kgDryAir).
+
+\paragraph{Field: Central Heating Design Supply Air Humidity Ratio}\label{field-central-heating-design-supply-air-humidity-ratio}
+
+The design humidity ratio in kilograms of water per kilogram of dry air at the exit of the central heating coil. This value is also used for the sizing of zone equipment (e.g., reheat coil) for the system embedded with central heating coils, but it is not used if there is no central heating coil in the system. The default is .008 (kgWater/kgDryAir).
+
+\paragraph{Field: Cooling Supply Air Flow Rate Method}\label{field-cooling-supply-air-flow-rate-method}
+
+The input of this field must be the method used to determine the airloop cooling supply air volume flow rate. The input must be either, \emph{DesignDay}, \emph{Flow/System,} \emph{FlowPerFloorArea}, \emph{FractionOfAutosizedCoolingAirflow}, or \emph{FlowPerCoolingCapacity}. \emph{DesignDay} means the program will calculate the system design cooling supply air volume flow rate using the System Sizing input data and a design day simulation. \emph{Flow/System} means that the program will use the input of the field \emph{Cooling Design Air Flow Rate} as the system design cooling supply air volume flow rate. \emph{FlowPerFloorArea} means the program calculates the cooling supply air volume flow rate from zone floor area served by the airloop and user specified \emph{Flow Per Floor Area} value. \emph{FractionOfAutosizedCoolingAirflow} means the program calculates the cooling supply air volume flow rate from user specified fraction and the autosized design cooling supply air volume flow rate value determined by the simulation. \emph{FlowPerCoolingCapacity} means the supply air volume is calculated from user specified flow per cooling capacity and design cooling capacity determined by the simulation. The default method is \emph{DesignDay}: i.e., the program uses the calculated design values.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate}
+
+The design system cooling air flow rate in cubic meters per second. This input is an alternative to using the program autocalculated value. This input is used if Coolingi Supply Air Flow Rate Method is Flow/System. This value will \emph{not} be multiplied by any sizing factor or by zone multipliers. If using zone multipliers, this value must be large enough to serve the multiplied zones.
+
+\paragraph{Field: Cooling Supply Air Flow Rate Per Floor Area \{m3/s-m2\}}\label{field-cooling-supply-air-flow-rate-per-floor-area-m3s-m2}
+
+Enter the cooling supply air volume flow rate per zone conditioned floor area in m3/s-m2. This field is required field when the Cooling Supply Air Flow Rate Method is \emph{FlowPerFloorArea}. This field may be left blank if a cooling coil is not included in the airloop or the Cooling Supply Air Flow Rate Method is not \emph{FlowPerFloorArea}. The program calculates the cooling supply air volume flow rate from the cooled floor area served by the air loop and the \emph{Flow Per Unit Area} value specified by the user.
+
+\paragraph{Field: Cooling Fraction of Autosized Cooling Design Supply Air Flow Rate}\label{field-cooling-fraction-of-autosized-cooling-design-supply-air-flow-rate}
+
+Enter the cooling supply air volume flow rate as a fraction of the airloop autosized cooling supply air flow rate. This input field is required when the Cooling Supply Air Flow Rate Method is \emph{FractionOfAutosizedCoolingAirflow}. This input field may be left blank if a cooling coil is not included in the airloop or the Cooling Supply Air Flow Rate Method is not \emph{FractionOfAutosizedCoolingAirflow}. The program calculates the cooling supply air volume flow rate from the design autosized cooling supply air flow rate and user specified fraction.
+
+\paragraph{Field: Cooling Supply Air Flow Rate Per Unit Cooling Capacity \{m3/s-W\}}\label{field-cooling-supply-air-flow-rate-per-unit-cooling-capacity-m3s-w}
+
+Enter the cooling supply air volume flow rate per unit cooling capacity in m3/s-W. This input field is required when the Cooling Supply Air Flow Rate Method is \emph{FlowPerCoolingCapacity}. This field may be left blank if a cooling coil is not included in the airloop or the Cooling Supply Air Flow Rate Method is not \emph{FlowPerCoolingCapacity}. The program calculates the airloop cooling supply air volume flow rate from the design autosized cooling capacity and user specified \emph{Flow Per Cooling Capacity} value.
+
+\paragraph{Field: Heating Supply Air Flow Rate Method}\label{field-heating-supply-air-flow-rate-method}
+
+The input of this field must be the method used to determine the airloop heating supply air volume flow rate. The input must be either, \emph{DesignDay}, \emph{Flow/System,} \emph{FlowPerFloorArea}, \emph{FractionOfAutosizedHeatingAirflow}, \emph{FractionOfAutosizedCoolingAirflow} or \emph{FlowPerHeatingCapacity}. \emph{DesignDay} means the program will calculate the system design heating supply air volume flow rate using the System Sizing input data and a design day simulation. \emph{Flow/System} means that the program will use the input of the field \emph{Heating Design Air Flow Rate} as the system design heating supply air volume flow rate. \emph{FlowPerFloorArea} means the program calculates the system heating supply air volume flow rate from zone floor area served by the airloop and user specified \emph{Flow Per Floor Area} value. \emph{FractionOfAutosizedHeatingAirflow} means the program calculates the system heating supply air volume flow rate from user specified fraction and the autosized system design heating supply air volume flow rate value determined by the simulation. \emph{FractionOfAutosizedCoolingAirflow} means the program calculates the system heating supply air volume flow rate from user specified fraction and the autosized system design cooling supply air volume flow rate value determined by the simulation. \emph{FlowPerHeatingCapacity} means the system heating supply air volume is calculated from user specified flow per heating capacity and design heating capacity determined by the simulation. The default method is \emph{DesignDay}: i.e., the program uses the calculated design values.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate}
+
+The design system heating air flow rate in cubic meters per second. This input is an alternative to using the program autocalculated value. This input is used if Heating Supply Air Flow Rate Method is Flow/System. This value will \emph{not} be multiplied by any sizing factor or by zone multipliers. If using zone multipliers, this value must be large enough to serve the multiplied zones.
+
+\paragraph{Field: Heating Supply Air Flow Rate Per Floor Area \{m3/s-m2\}}\label{field-heating-supply-air-flow-rate-per-floor-area-m3s-m2}
+
+Enter the heating supply air volume flow rate per zone conditioned floor area in m3/s-m2. This field is required field when the Heating Supply Air Flow Rate Method is \emph{FlowPerFloorArea}. This field may be left blank if a heating coil is not included in the airloop or the Heating Supply Air Flow Rate Method is not \emph{FlowPerFloorArea}. The program calculates the heating supply air volume flow rate from the heated or cooled floor area served by the air loop and the \emph{Flow Per Unit Area} value specified by the user.
+
+\paragraph{Field: Heating Fraction of Autosized Heating Supply Air Flow Rate}\label{field-heating-fraction-of-autosized-heating-supply-air-flow-rate}
+
+Enter the heating supply air volume flow rate as a fraction of the airloop autosized heating supply air flow rate. This input field is required when the Heating Supply Air Flow Rate Method is \emph{FractionOfAutosizedHeatingAirflow}. This input field may be left blank if heating coil is not included in the airloop or the Heating Supply Air Flow Rate Method is not \emph{FractionOfAutosizedHeatingAirflow}. The program calculates the heating supply air volume flow rate from the design autosized heating supply air flow rate and user specified fraction.
+
+\paragraph{Field: Heating Fraction of Autosized Cooling Supply Air Flow Rate}\label{field-heating-fraction-of-autosized-cooling-supply-air-flow-rate}
+
+Enter the heating supply air volume flow rate as a fraction of the airloop autosized cooling supply air flow rate. This input field is required when the Heating Supply Air Flow Rate Method is \emph{FractionOfAutosizedCoolingAirflow}. This input field may be left blank if heating coil is not included in the airloop or the Heating Supply Air Flow Rate Method is not \emph{FractionOfAutosizedCoolingAirflow}. The program calculates the heating supply air volume flow rate from the design autosized cooling supply air flow rate and user specified fraction.
+
+\paragraph{Field: Heating Design Supply Air Flow Rate Per Unit Heating Capacity \{m3/s-W\}}\label{field-heating-design-supply-air-flow-rate-per-unit-heating-capacity-m3s-w-1}
+
+Enter the heating supply air volume flow rate per unit heating capacity in m3/s-W. This input field is required when the Heating Design air Flow Method is \emph{FlowPerCoolingCapacity}. This field may be left blank if a heating coil is not included in the airloop or the Heating Design air Flow Method is not \emph{FlowPerHeatingCapacity}. The program calculates the airloop heating supply air volume flow rate from the design autosized heating capacity and user specified \emph{Flow Per Heating Capacity} value.
+
+\paragraph{Field: System Outdoor Air Method}\label{field-system-outdoor-air-method-000}
+
+The method used to calculate the system minimum outdoor air flow. The two choices are ZoneSum and VentilationRateProcedure (VRP). ZoneSum sums the outdoor air flows across all zones served by the system. VRP uses the multi-zone equations defined in 62.1-2007 to calculate the system outdoor air flow. VRP considers zone air distribution effectiveness and zone diversification of outdoor air fractions.
+
+\paragraph{Field: Zone Maximum Outdoor Air Fraction}\label{field-zone-maximum-outdoor-air-fraction-000}
+
+This positive numeric input is the zone maximum outdoor air fraction. For an air loop, when a zone requires outdoor air higher than the user specified Zone Maximum Outdoor Air Fraction, the zone supply air flow will be increased to cap the outdoor air fraction at the maximum value. This allows the system level outdoor air flow to be reduced while the total supply air flow increases. Valid values are from 0 to 1.0. Default is 1.0 which indicates zones can have 100\% outdoor air maintaining backward compatibility. This inputs work for constant volume air systems, single and dual duct VAV systems.
+
+\paragraph{Field Cooling Design Capacity Method}\label{field-cooling-design-capacity-method-1}
+
+Enter the method used to determine the cooling design capacity for scalable sizing. Input allowed is either \emph{None}, \emph{CoolingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedCoolingCapacity}. None is used when a cooling coil is not included in the airloop. If this input field is left blank, or None is specified, then the autosized design cooling capacity determined by the program is used. \emph{CoolingDesignCapacity} means user specifies the magnitude of cooling capacity or the program calculates the design cooling capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design cooling capacity from user specified cooling capacity per floor area and floor area of the zones served by the airloop. \emph{FractionOfAutosizedCoolingCapacity} means the program calculates the design cooling capacity from user specified fraction and the auto-sized design cooling capacity. If the value this input field is blank or specified as None, then the next three input fields are not required. The default method is \emph{CoolingDesignCapacity}.
+
+\paragraph{Field: Cooling Design Capacity \{W\}}\label{field-cooling-design-capacity-w-1}
+
+Enter the magnitude of the cooling capacity in Watts. This input is an alternative to using the program auto-calculated cooling capacity value. This input is a required field when the Cooling Design Capacity Method is \emph{CoolingDesignCapacity}. This field may be left blank if a cooling coil is not included in the air loop or alternative method is specified. This input field is autosizable.
+
+\paragraph{Field: Cooling Design Capacity Per Floor Area \{W/m2\}}\label{field-cooling-design-capacity-per-floor-area-wm2-1}
+
+Enter the cooling capacity per unit floor area in m3/s-m2. This field is required field when the Cooling Design Capacity Method is \emph{CapacityPerFloorArea}. This field may be left blank if a cooling coil is not included in the airloop or the Cooling Design Capacity Method is not \emph{CapacityPerFloorArea}. The program calculates the cooling capacity from floor area of the zones served by the airloop and the cooling capacity per unit floor area value specified by the user.
+
+\paragraph{Field: Fraction of Autosized Cooling Design Capacity}\label{field-fraction-of-autosized-cooling-design-capacity-1}
+
+Enter the cooling capacity as a fraction of the autosized cooling capacity. This input field is required when the Cooling Design Capacity Method is \emph{FractionOfAutosizedCoolingCapacity}. This input field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design Capacity Method is not \emph{FractionOfAutosizedCoolingCapacity}. The program calculates the cooling capacity from the design autosized cooling capacity and user specified fraction. Design day sizing run must be specified.
+
+\paragraph{Field: Heating Design Capacity Method}\label{field-heating-design-capacity-method-1}
+
+Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either \emph{None}, \emph{HeatingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedHeatingCapacity}. \emph{None} is used when a heating coil is not included in the airloop. If this input field is left blank, then the autosized design heating capacity determined by the program is used. \emph{HeatingDesignCapacity} means user specifies the magnitude of heating capacity or the program calculates the design heating capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zones served by the airllop. \emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. If the value this input field is blank or specified as None, then the next three input fields are not required. The default method is \emph{HeatingDesignCapacity}.
+
+\paragraph{Field: Heating Design Capacity \{W\}}\label{field-heating-design-capacity-w-1}
+
+Enter the magnitude of the heating capacity in Watts. This input is an alternative to using the program auto-calculated heating capacity value. This input is a required field when the Heating Design Capacity Method is \emph{HeatingDesignCapacity}. This field may be left blank if a heating coil is not included in the airloop or alternative method is specified. This input field is autosizable.
+
+\paragraph{Field: Heating Design Capacity Per Floor Area \{W/m2\}}\label{field-heating-design-capacity-per-floor-area-wm2-1}
+
+Enter the heating capacity per unit floor area in m3/s-m2. This field is required field when the Heating Design Capacity Method is \emph{CapacityPerFloorArea}. This field may be left blank if a heating coil is not included in the airloop or the Heating Design Capacity Method is not \emph{CapacityPerFloorArea}. The program calculates the heating capacity from floor area of the zones served by the airloop and the heating capacity per unit floor area value specified by the user.
+
+\paragraph{Field: Fraction of Autosized Heating Design Capacity}\label{field-fraction-of-autosized-heating-design-capacity-1}
+
+Enter the heating capacity as a fraction of the autosized heating capacity. This input field is required when the Heating Design Capacity Method is FractionOfAutosizedHeatingCapacity. This input field may be left blank if heating coil is not included in the airloop or the Heating Design Capacity Method is not FractionOfAutosizedHeatingCapacity. The program calculates the heating capacity from the design autosized cooling capacity and user specified fraction.
+
+\paragraph{Field: Central Cooling Capacity Control Method}\label{field-central-cooling-capacity-control-method}
+
+Specifies how the central cooling coil will be controlled, which affects the coil sizing calculation. There are 4 choices: VAV, Bypass, VT, and OnOff. Choose VAV if the cooling output is controlled by varying the air flow. Bypass should be chosen if the capacity is controlled by bypassing a variable fraction of the mixed air around the coil face. VT indicates that cooling coil output is controlled by varying the coil exit temperature while the flow rate is constant. And OnOff means that the cooling output is controlled by cycling the air flow.
+
+An IDF example:
+
+\begin{lstlisting}
+
+Sizing:System,
+  VAV Sys 1,               !- AirLoop Name
+  sensible,                !- Type of Load to Size On
+  autosize,                !- Design Outdoor Air Flow Rate {m3/s}
+  0.3,                     !- Minimum System Air Flow Ratio
+  4.5,                     !- Preheat Design Temperature {C}
+  .008,                    !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
+  11.0,                    !- Precool Design Temperature {C}
+  .008,                    !- Precool Design Humidity Ratio {kgWater/kgDryAir}
+  12.8,                    !- Central Cooling Design Supply Air Temperature {C}
+  16.7,                    !- Central Heating Design Supply Air Temperature {C}
+  noncoincident,           !- Sizing Option
+  no,                      !- 100% Outdoor Air in Cooling
+  no,                      !- 100% Outdoor Air in Heating
+  0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
+  0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
+  designday,               !- Cooling Supply Air Flow Rate Method
+  0,                       !- Cooling Supply Air Flow Rate {m3/s}
+  ,                        !- Cooling Supply Air Flow Rate Per Floor Area {m3/s-m2}
+  ,                        !- Cooling Fraction of Autosized Cooling Supply Air Flow Rate {-}
+  ,                        !- Cooling Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
+  designday,               !- Heating Supply Air Flow Rate Method
+  0,                       !- Heating Supply Air Flow Rate {m3/s}
+  ,                        !- Heating Supply Air Flow Rate Per Floor Area {m3/s-m2}
+  ,                        !- Heating Fraction of Autosized Heating Supply Air Flow Rate {-}
+  ,                        !- Heating Fraction of Autosized Cooling Supply Air Flow Rate {-}
+  ,                        !- Heating Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
+  ZoneSum,                 !- System Outdoor Air Method
+  0.5,                     !- Zone Maximum Outdoor Air Fraction
+  CoolingDesignCapacity,   !- Cooling Design Capacity Method
+  autosize,                !- Cooling Design Capacity {W}
+  ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
+  ,                        !- Fraction of Autosized Cooling Design Capacity {-}
+  HeatingDesignCapacity,   !- Heating Design Capacity Method
+  autosize,                !- Heating Design Capacity {W}
+  ,                        !- Heating Design Capacity Per Floor Area {W/m2}
+  ;                        !- Fraction of Autosized Cooling Design Capacity {-}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-006}
+
+The system design air flow rates and heating and cooling capacities are output onto the local file ``eplusssz.\textless{}ext\textgreater{}'' where \textless{}ext\textgreater{} is the extension from the sizing style object (default is csv -- a comma separated file \emph{eplusssz.csv)}. The columns are clearly labeled. It will easily import into Excel or other spreadsheet program that accepts delimited files. The results are calculated values and do not include any user input system flow rates.
+
+The calculated system design air flow rates and the user input system design air flow rates are also reported on the \emph{eplusout.eio} file. The values are printed out for each system as comma separated records beginning with \emph{System Sizing}. An example is:
+
+\begin{lstlisting}
+! <System Sizing Information>c++, System Name, Field Description, Value
+ System Sizing, VAV SYS 1, Calculated Cooling Design Air Flow Rate [m3/s],   1.3194
+ System Sizing, VAV SYS 1, User Cooling Design Air Flow Rate [m3/s],   1.5000
+ System Sizing, VAV SYS 1, Calculated Heating Design Air Flow Rate [m3/s],  0.90363
+ System Sizing, VAV SYS 1, User Heating Design Air Flow Rate [m3/s],   1.0000
+\end{lstlisting}
+
+\subsection{Sizing:Plant}\label{sizingplant}
+
+The Sizing:Plant object contains the input needed for the program to calculate plant loop flow rates and equipment capacities when autosizing. This information is initially used by components that use water for heating or cooling such as hot or chilled water coils to calculate their maximum water flow rates. These flow rates are then summed for use in calculating the Plant Loop flow rates.
+
+The program will size any number of chilled water, hot water, condenser water and other plant loops. There should be one Sizing:Plant object for each plant loop that is to be autosized.
+
+\subsubsection{Inputs}\label{inputs-7-006}
+
+\paragraph{Field: Plant or Condenser Loop Name}\label{field-plant-or-condenser-loop-name}
+
+The name of a Plant Loop or Condenser Loop object corresponding to this Sizing:Plant object. This is the plant loop for which this data will be used for calculating the loop flow rate.
+
+\paragraph{Field: Loop Type}\label{field-loop-type}
+
+The possible inputs are \emph{Heating, Steam, Cooling,} or \emph{Condenser}.
+
+\paragraph{Field: Design Loop Exit Temperature}\label{field-design-loop-exit-temperature}
+
+The water temperature in degrees Celsius at the exit of the supply side of the plant loop, Thus this is the temperature of the water supplied to the inlet of chilled or hot water coils and other equipment that places loads on a plant loop.
+
+\paragraph{Field: Loop Design Temperature Difference}\label{field-loop-design-temperature-difference}
+
+The design temperature rise (for cooling or condenser loops) or fall (for heating loops) in degrees Celsius across the demand side of a plant loop.~ This temperature difference is used by component models to determine flow rates required to meet design capacities.~ Larger values lead to smaller design flow rates.
+
+\paragraph{Field: Sizing Option}\label{field-sizing-option}
+
+This field is optional. This field controls how concurrence issues impact the plant loop design flow rate. If it is not used then the program uses noncoincident method, which is the historical behavior prior to version 8.3. There are two choices, noncoincident and coincident. The use of Coincident sizing option requires that the SimulationControl object be set to YES for the input field called Do HVAC Sizing Simulation for Sizing Periods.
+
+\paragraph{Field: Zone Timesteps in Averaging Window}\label{field-zone-timesteps-in-averaging-window}
+
+This field is optional and is only used if the preceding field is set to Coincident. This is the number of zone timesteps used in a moving average to determine the design flow rate from HVAC Sizing Simulation approach. This allows using a broader average over time when using coincident plant sizing. This is similar in concept to the similar field in Sizing:Parameters which specifies the averaging window for zone loads. The default is 1.
+
+\paragraph{Field: Coincident Sizing Factor Mode}\label{field-coincident-sizing-factor-mode}
+
+This field is only used if the sizing option is set to Coincident. This field controls the behavior of coincident sizing with respect to what, if any, sizing factor should be applied to further modify the flow rate measured while running HVAC Sizing Simulations. There are four options. Enter the keword None to use the raw value for flow rate without modification. Enter the keyword GlobalHeatingSizingFactor to modify the flow by the sizing factor entered in the object called Sizing:Parameters for heating. Enter the keyword GlobalCoolingSizingFactor to modify the flow by the sizing factor entered in the object called Sizing:Parameters for cooling. Enter the keyword LoopComponentSizingFactor to modify the flow by a sizing factor determined from the combination of component-level sizing factors in the associated plant loop.
+
+An IDF example:
+
+\begin{lstlisting}
+
+Sizing:Plant,
+     Chilled Water Loop, ! name of loop
+     Cooling,            ! type of loop
+     7.22,               ! chilled water supply temperature
+     6.67,               ! chilled water delta T
+  NonCoincident,      !- Sizing Option
+  1,                  !- Zone Timesteps in Averaging Window
+  GlobalCoolingSizingFactor; !- Coincident Sizing Factor Mode
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-004}
+
+The loop flow rates are reported on the \emph{eplusout.eio} file along with the component sizing results.
+
+When coincident plant sizing method is used, the eio file contains special summary report with various details and interim values from the calculations, under the following record header: ! , Plant Loop Name, Sizing Pass \{\#\}, Measured Mass Flow\{kg/s\}, Measured Demand \{W\}, Demand Calculated Mass Flow\{kg/s\}, Sizes Changed \{Yes/No\}, Previous Volume Flow Rate \{m3/s\}, New Volume Flow Rate \{m3/s\}, Demand Check Applied \{Yes/No\}, Sizing Factor \{\}, Normalized Change \{\}, Specific Heat\{\}.
diff --git a/doc/input-output-reference/src/overview/group-detailed-ground-heat-transfer.tex b/doc/input-output-reference/src/overview/group-detailed-ground-heat-transfer.tex
new file mode 100644
index 00000000000..216e9393d96
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-detailed-ground-heat-transfer.tex
@@ -0,0 +1,87 @@
+\section{Group -- Detailed Ground Heat Transfer}\label{group-detailed-ground-heat-transfer}
+
+\subsection{Detailed Ground Heat Transfer}\label{detailed-ground-heat-transfer}
+
+The following objects may be included in an EnergyPlus input IDF file but are handled by the Slab preprocessor:
+
+\begin{itemize}
+\tightlist
+\item
+  GroundHeatTransfer:Slab:Materials
+\item
+  GroundHeatTransfer:Slab:MatlProps
+\item
+  GroundHeatTransfer:Slab:BoundConds
+\item
+  GroundHeatTransfer:Slab:BldgProps
+\item
+  GroundHeatTransfer:Slab:Insulation
+\item
+  GroundHeatTransfer:Slab:EquivalentSlab
+\item
+  GroundHeatTransfer:Slab:AutoGrid
+\item
+  GroundHeatTransfer:Slab:ManualGrid
+\item
+  GroundHeatTransfer:Slab:XFACE
+\item
+  GroundHeatTransfer:Slab:YFACE
+\item
+  GroundHeatTransfer:Slab:ZFACE
+\end{itemize}
+
+The following objects may be included in an EnergyPlus input IDF file but are handled by the Basement preprocessor:
+
+\begin{itemize}
+\tightlist
+\item
+  GroundHeatTransfer:Basement:SimParameters
+\item
+  GroundHeatTransfer:Basement:MatlProps
+\item
+  GroundHeatTransfer:Basement:Insulation
+\item
+  GroundHeatTransfer:Basement:SurfaceProps
+\item
+  GroundHeatTransfer:Basement:BldgData
+\item
+  GroundHeatTransfer:Basement:Interior
+\item
+  GroundHeatTransfer:Basement:ComBldg
+\item
+  GroundHeatTransfer:Basement:EquivSlab
+\item
+  GroundHeatTransfer:Basement:EquivAutoGrid
+\item
+  GroundHeatTransfer:Basement:AutoGrid
+\item
+  GroundHeatTransfer:Basement:ManualGrid
+\item
+  GroundHeatTransfer:Basement:XFACE
+\item
+  GroundHeatTransfer:Basement:YFACE
+\item
+  GroundHeatTransfer:Basement:ZFACE
+\end{itemize}
+
+The documentation both the Slab and Basement objects appear in the AuxiliaryPrograms document under the ``Ground Heat Transfer in EnergyPlus'' heading.
+
+The only object described in this section is the control object which activates the use of the preprocessor.
+
+\subsection{GroundHeatTransfer:Control}\label{groundheattransfercontrol}
+
+The GroundHeatTransfer:Control object determines if the Slab and Basement preprocessors are going to be executed. When a Slab or Basement run is performed the results are saved in files with extensions .SLAB or .BSMT so that they do not need to be rerun if no input changes are made to the GroundHeatTransfer:Slab or GroundHeatTransfer:Basement objects.
+
+\subsubsection{Inputs}\label{inputs-013}
+
+\paragraph{Field: Name}\label{field-name-012}
+
+This alpha field is the name of the GroundHeatTransfer:Control object. It is used as an identifier.
+
+\paragraph{Field: Run Basement Preprocessor}\label{field-run-basement-preprocessor}
+
+The field can either be Yes or No and defaults to No. It is used to control whether the Basement preprocessor program is executed. If it has been previously executed the results are stored in the .BSMT file and do not necessary need to be run again unless the GroundHeatTransfer:Basement objects have changed.
+
+\paragraph{Field: Run Slab Preprocessor}\label{field-run-slab-preprocessor}
+
+The field can either be Yes or No and defaults to No. It is used to control whether the Slab preprocessor program is executed. If it has been previously executed the results are stored in the .SLAB file and do not necessary need to be run again unless the GroundHeatTransfer:Slab objects have changed.
diff --git a/doc/input-output-reference/src/overview/group-electric-load-center-generator.tex b/doc/input-output-reference/src/overview/group-electric-load-center-generator.tex
new file mode 100644
index 00000000000..2e12e602912
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-electric-load-center-generator.tex
@@ -0,0 +1,4955 @@
+\section{Group -- Electric Load Center-Generator Specifications}\label{group-electric-load-center-generator-specifications}
+
+This group of input objects is related to electric power serving the facility. EnergyPlus has models for various types of electric generators and power conditioning devices that might be part of the electric power system serving the building being modeled. Buildings with simple utility electric power service will not necesarily need any of the models in this group. All EnergyPlus models that have any electric power consumption are assumed to have a straightforward connection to utility grid service and no extra input is needed. The models in this group of inputs are useful for facilities that more complex electric power service such as:
+
+\begin{itemize}
+\tightlist
+\item
+  Utility service is at a voltage higher than used in the building and a transformer conditions power coming into to the building as part of the facility.
+\item
+  On site generators produce electricity within the facility. For example solar photovoltaic panels or natural gas powered electric generators.
+\item
+  On site electric storage devices.
+\end{itemize}
+
+For facilities that own their transformer, and the utility services is metered on the high voltage side, the ElectricLoadCenter:Transformer object can be used, and may be the only input object needed.
+
+All other applications involving on-site generation or storage will require at least one ElectricLoadCenter:Distribution to describe the arrangement and control of a set of electric power devices. Each of these load centers is like a subpanel connected to the main electrical panel for the facility. The main panel is assumed to exist whenever the rest of the model includes something that consumes electricity (and does not require any input object). Each ElectricLoadCenter:Distribution input object describes what devices are on a subpanel connected to the main panel, as well as how they are controlled, dispatched, and arranged to provide some service related to the facility's electric power. The ElectricLoadCenter:Distribution object manages and calls the individual generator models that are connected to it by being listed in an ElectricLoadCenter:Generators object, such as natural gas powered turbines, photovoltaic panels, wind turbines, etc. Unlike elsewhere in EnergyPlus where there are loops, branches, or generic equipment lists that allow describing custom arrangements, the electric power service modeling is restricted to a collection of predefined arrangements, called ``buss types.'' Many on site generation and storage configurations common in buildings can be modeled using just one ElectricLoadCenter:Distribution object. However, by combining multiple load centers with different equipment and operations schemes, it is possible to model more complex configurations. (Note that when using multiple ElectricLoadCenter:Distribution objects, the order of the ElectricLoadCenter:Distribution objects within the input file determines the order in which they are called to interact with the main panel.)
+
+The following diagram shows some of the devices and arrangements that can be modeled using the inputs in this group.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/ElectPowerServiceOverview.png}
+\caption{PowerServiceOverview}
+\end{figure}
+
+\subsection{ElectricLoadCenter:Transformer}\label{electricloadcentertransformer}
+
+This object is used to model the energy losses of transformers when they are used to transfer electricity from the grid to a building (as distribution transformers) or transfer electricity from onsite generators to the grid. Distribution transformers reduce the voltage on utility distribution lines (34.5 kV or less) to a lower secondary voltage (600 V or less) suitable for customer equipment. According to the medium used for cooling and insulation, distribution transformers can be classified into liquid-immersed and dry type transformers. According to the input voltages, distribution transformers can be classified into medium-voltage (between 600 V and 34.5kV) and low-voltage transformer (less than 600 V). The transformers used to output the surplus electricity from onsite generators to the grid usually match the cogeneration voltage to the grid. This object can be used for all types of distribution transformers and the transformers used to output electricity from onsite generators to the grid, but the model defaults applies to the low-voltage dry type transformers because they are the most common type found in commercial and industrial facilities.
+
+Energy losses in transformers consist of the no load (core) loss and the load (winding) loss. The no load loss comes primarily from the switching of the magnetic fields in the core material. It is roughly constant and exists continuously in the core material as long as the transformer is energized. The load loss comes from the electrical resistance in the windings when there is a load on the transformer. The load loss is proportional to the load squared with a small temperature correction. The energy losses at a given load depend on the transformer s performance. This object provides the user two alternative ways to indicate the transformer s performance. First, the user can provide the no load loss and load loss at rated conditions. Second, the user can provide the nameplate efficiency and the corresponding reference conditions. The detailed algorithms to calculate the energy losses are described in the Engineering Reference.
+
+The user needs to specify which loads are connected to the transformer. This is achieved in different manners depending on the transformer usage. For a distribution transformer, the user needs to provide a number of electric meters wired to that transformer. The input object can currently accommodate up to ten meters, but it is extensible by modifying the Energy+.idd entry. For a transformer used to output electricity from onsite generators to the grid, the user needs to indicate the transformer name in the served electric load center.
+
+\subsubsection{Inputs}\label{inputs-014}
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-005}
+
+This alpha field contains the schedule name (ref. Schedule objects) that contains information on the availability of the transformer. A schedule value greater than 0 (usually 1 is used) indicates that the transformer is available to convert AC power from one voltage to another. A value less than or equal to 0 (usually 0 is used) denotes that the transformer is not available. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Transformer Usage}\label{field-transformer-usage}
+
+This field indicates one of the three supported transformer application types: PowerInFromGrid, PowerOutToGrid, and LoadCenterPowerConditioning. A PowerInFromGrid type of transformer is used to step down voltage from the electricity grid to the building. The transformer with this type of use is somewhat free standing and does not need to be referenced in any ElectricLoadCenter:Distribution object. There should be only one PowerInFromGrid transformer in the model. A PowerOutToGrid type of transformer is used to match voltage from the building to the electricity grid. This conditions power exported out of the facility and feed back into the grid. This type of transformer will only be needed if the building ever exports power and the building and grid connection have different voltages. There should be only one PowerOutToGrid transformer in the model and it will serve all the surplus electricity produced by electric load center(s). A LoadCenterPowerConditioning type of transformer is used to match voltage between an electic load center (subpanel) and the facility's main panel. Each electric load center can have its own transformer to condition power fed into the main panel. For electric load centers that also draw power from the main panel, to charge storage, the transformer is assumed to operate in both directions (at the same performance). This type of transformer should be named in an ElectricLoadCenter:Distribution object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-005}
+
+This field contains the name of the thermal zone where the transformer is located. Entering a valid name of zone here will direct EnergyPlus to include the transformer s losses as heat gains to the named thermal zone. If the transformer is not within a thermal zone, this field can be left blank and the thermal energy associated with transformer losses is removed from the building model.
+
+\paragraph{Field: Radiative Fraction}\label{field-radiative-fraction}
+
+This field contains the fraction of transformer s losses that enter the zone as long-wave thermal radiation. This numeric filed should have a value between 0.0 and 1.0. The balance of the losses is convective. This field is not used if the previous field for zone name is left blank.
+
+\paragraph{Field: Rated Capacity}\label{field-rated-capacity}
+
+This field defines the rated capacity of the transformer in VA.
+
+\paragraph{Field: Phase}\label{field-phase}
+
+This field indicates whether the transformer is a single phase or three phase type. The two alternative values are 1 or 3. The default is 3. This field is currently not used in the model.
+
+\paragraph{Field: Conductor Material}\label{field-conductor-material}
+
+This field specifies the winding material used by the transformer. There are two options: Copper and Aluminum. The choice will determine the thermal coefficient of resistance used to calculate the temperature correction factor for the transformer load losses. The default is Aluminum.
+
+\paragraph{Field: Full Load Temperature Rise}\label{field-full-load-temperature-rise}
+
+This numeric field defines the temperature rise of the windings above the ambient temperature, when the transformer is loaded at its nameplate rating. For liquid-immersed distribution transformers, the full load temperature rise usually takes the value of 65 °C. For dry-type transformers, the temperature rise usually takes three optional values: 80, 115 and 150 °C. This field accepts any value between the minimum (50 °C) and the maximum (180 °C). The default is 150 °C.
+
+\paragraph{Field: Fraction of Eddy Current Losses}\label{field-fraction-of-eddy-current-losses}
+
+This field defines the fraction of load losses resulting from the eddy currents. Transformer's load losses comprise two parts: the ohmic loss due to the current flowing in the resistance of the windings and the eddy and stray losses due to the eddy currents. This field indicates the fraction of the load losses due to the eddy currents. This numeric field should have a value between 0.0 and 1.0. The default is 0.1.
+
+\paragraph{Field: Performance Input Method}\label{field-performance-input-method-000}
+
+This alpha field contains the method by which the user will specify the transformer performance: RatedLosses or NominalEfficiency. If this field is left blank in the input data file, the default input method is assumed to be RatedLosses. If the method NominalEfficiency is selected, the user must enter the fields for the nameplate efficiency and the corresponding reference coditions as described below. If the method RatedLosses is selected, then the fields for rated no load loss and load loss must be entered as described below.
+
+\paragraph{Field: Rated No Load Loss}\label{field-rated-no-load-loss}
+
+This field defines the no load loss (W) at rated load and conditions. The no load loss is roughly constant and exists whenever the transformer is energized. The no load loss is also called the core loss. This field is used only if the field of Performance Input Method is specified as RatedLosses.
+
+\paragraph{Field: Rated Load Loss}\label{field-rated-load-loss}
+
+This field defines the load loss (W) at rated load and conditions. The load loss varies with the square of the load being served by the transformer. The load loss is also called the winding loss because the load loss occurs in the primary and secondary windings around the core. This field is used only if the field of Performance Input Method is specified as RatedLosses.
+
+\paragraph{Field: Nameplate Efficiency}\label{field-nameplate-efficiency}
+
+This field contains the value for transformer efficiency at a given per unit load and specified reference temperature. This field is used only if the field of Performance Input Method is specified as NominalEfficiency. The default is 0.98.
+
+\paragraph{Field: Per Unit Load for Nameplate Efficiency}\label{field-per-unit-load-for-nameplate-efficiency}
+
+This field defines the percentage of the rated capacity at which the nameplate efficiency is measured. According to the NEMA (National Electrical Manufactures Association) Standard TP-1, the per unit load takes the value of 0.35 for dry-type distribution transformers and it takes the value of 0.50 for liquid-filled distribution transformers. The default is 0.35.
+
+\paragraph{Field: Reference Temperature for Nameplate Efficiency}\label{field-reference-temperature-for-nameplate-efficiency}
+
+This field defines the conductor temperature at which the nameplate efficiency is measured. This field is used only if the field of Performance Input Method is specified as NominalEfficiency . According to the NEMA Standard TP-1, the reference temperature takes the value of 75 °C for dry-type distribution transformers and it takes the value of 55 °C for liquid-filled distribution transformers. The default is 75 °C.
+
+\paragraph{Field: Per Unit Load for Maximum Efficiency}\label{field-per-unit-load-for-maximum-efficiency}
+
+This field defines the percentage of the rated capacity at which the maximum efficiency is obtained. This field is used only if the field of Performance Input Method is specified as NominalEfficiency . A blank field indicates that it takes the same value as the per unit load for nameplate efficiency.
+
+\paragraph{Field: Consider Transformer Loss for Utility Cost}\label{field-consider-transformer-loss-for-utility-cost}
+
+This field indicates whether the transformer losses are considered to calculate utility cost. This field applies to a PowerInFromGrid type of transformer. In some cases, the transformer losses are required but they are not part of the energy consumption for utility cost calculation. For example, the transformer is owned by the utility company but it locates in the building. In this case, it might be desired to model transformer energy losses for HVAC operation but the energy losses will not be accounted for utility cost.
+
+\paragraph{Field: Electric Meter 1-10 Name}\label{field-electric-meter-1-10-name}
+
+A transformer may serve different loads such as plug loads, some lighting loads, and some HVAC equipment loads. These fields apply to a PowerInFromGrid type of transformer. The user needs to specify which loads are connected to the transformer. For example the HVAC and Plant equipment might use a higher voltage than the building and only the building loads need power conditioning. This is achieved by providing a list of electric meters wired to the transformer. The input object can currently accommodate up to ten meters, but it is extensible by modifying the Energy+.idd entry. Any valid electric meter name can be used here to wire to the transformer loads. Many different meters are automatically generated by the program and will depend on the objects used throughout the input file. The typical process of determining the exact name to enter in this field involves doing an initial run of EnergyPlus and then examining the *.mdd file which will list the meters and their resulting names. A custom meter is also supported. The meter must have electricity as its resource type.
+
+An example input of the ElectricLoadCenter:Transformer input is:
+
+\begin{lstlisting}
+
+ElectricLoadCenter:Transformer,
+  Transformer 1,                       !-Name
+  Always On,                           !- Availability Schedule Name
+  PowerInFromGrid,                     !- Transformer Usage
+  ,                                    !- Zone Name
+  ,                                    !-Radiative Fraction
+  15000,                               !- Nameplate Rating {VA}
+  3,                                   !- Phase
+  Aluminum,                            !- Conductor Material
+  150,                                 !- Full Load Temperature Rise { &deg;C}
+  0.1,                                 !- Fraction of Eddy Current Losses
+  NominalEfficiency,                   !- Performance Input Method
+  ,                                    !- Rated No Load Loss {W}
+  ,                                    !- Rated Load Loss {W}
+  0.985,                               !- Nameplate Efficiency
+  0.35,                                !- Per Unit Load for Nameplate Efficiency
+  75,                                  !- Reference Temperature for Nameplate Efficiency { &deg;C}
+  ,                                    !- Per Unit Load for Maximum Efficiency
+  Yes,                                 !- Consider Transformer Loss for Utility Cost
+  Electricity:Building;                !- Meter 1 Name
+
+
+  Schedule:Compact,
+  Always On,                             !- Name
+  Fraction,                               !- ScheduleType
+  Through: 12/31,                   !- Field #1
+  For: AllDays,                       !- Field #2
+  Until: 24:00,                       !- Field #3
+  1.0;                                         !- Field #4
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-010}
+
+\begin{itemize}
+\item
+  HVAC,Average,Transformer Efficiency{[]}
+\item
+  HVAC,Average,Transformer Output Electric Power{[}W{]}
+\item
+  HVAC,Sum,Transformer Output Elecric Energy {[}J{]}
+\item
+  HVAC,Average,Transformer Input Electric Power{[}W{]}
+\item
+  HVAC,Sum,Transformer Input Electric Energy {[}J{]}
+\item
+  HVAC,Average,Transformer No Load Loss Rate {[}W{]}
+\item
+  HVAC,Sum,Transformer No Load Loss Energy {[}J{]}
+\item
+  HVAC,Average,Transformer Load Loss Rate {[}W{]}
+\item
+  HVAC,Sum,Transformer Load Loss Energy {[}J{]}
+\item
+  HVAC,Average,Transformer Thermal Loss Rate {[}W{]}
+\item
+  HVAC,Sum,Transformer Thermal Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Transformer Distribution Electric Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Transformer Cogeneration Electric Loss Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Transformer Efficiency}\label{transformer-efficiency}
+
+This output field is the efficiency at which the distribution transformer changes alternating current from the higher primary voltage to a lower secondary voltage. The efficiency is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{Transformer Output Electric Power {[}W{]}}\label{transformer-output-electric-power-w}
+
+\paragraph{Transformer Output Elecric Energy {[}J{]}}\label{transformer-output-elecric-energy-j}
+
+These outputs are the total electricity power or energy provided by the transformer. They are equal to the metered loads which are wired to the transformer. These values are calculated for each HVAC system timestep being simulated, and the results are averaged (for power) or summed (for energy) for the timestep being reported.
+
+\paragraph{Transformer Input Electric Power {[}W{]}}\label{transformer-input-electric-power-w}
+
+\paragraph{Transformer Input Electric Energy {[}J{]}}\label{transformer-input-electric-energy-j}
+
+These outputs are the total electricity power or energy fed into the transformer. These values are calculated for each HVAC system timestep being simulated, and the results are averaged (for power) or summed (for energy) for the timestep being reported.
+
+\paragraph{Transformer No Load Loss Rate {[}W{]}}\label{transformer-no-load-loss-rate-w}
+
+\paragraph{Transformer No Load Loss Energy {[}J{]}}\label{transformer-no-load-loss-energy-j}
+
+These outputs are the no load loss occurred in the transformer. These values are calculated for each HVAC system timestep being simulated, and the results are averaged (for rate) or summed (for energy) for the timestep being reported.
+
+\paragraph{Transformer Load Loss Rate {[}W{]}}\label{transformer-load-loss-rate-w}
+
+\paragraph{Transformer Load Loss Energy {[}J{]}}\label{transformer-load-loss-energy-j}
+
+These outputs are the load loss occurred in the transformer. These values are calculated for each HVAC system timestep being simulated, and the results are averaged (for rate) or summed (for energy) for the timestep being reported.
+
+\paragraph{Transformer Thermal Loss Rate {[}W{]}}\label{transformer-thermal-loss-rate-w}
+
+\paragraph{Transformer Thermal Loss Energy {[}J{]}}\label{transformer-thermal-loss-energy-j}
+
+These outputs are the total energy losses occurred in the transformer. They are equal to the sum of the no load loss and the load loss. These values are calculated for each HVAC system timestep being simulated, and the results are averaged (for rate) or summed (for energy) for the timestep being reported.
+
+\paragraph{Transformer Distribution Electric Loss Energy {[}J{]}}\label{transformer-distribution-electric-loss-energy-j}
+
+This output is the total energy losses occurred in the transformer when it is used for input power from grid to building. It is set as zero if the transformer is used to transfer energy from onsite power generators to the electricity grid. This output is also added to a meter with ResourceType = Electricity, GroupKey = System.
+
+\paragraph{Transformer Cogeneration Electric Loss Energy {[}J{]}}\label{transformer-cogeneration-electric-loss-energy-j}
+
+This output is the total energy losses occurred in the transformer when it is used for input onsite cogeneration to the grid. It is set as zero if the transformer is used to transfer the electricity grid to building. This output is also added to a meter with ResourceType = ElectricityProduced, EndUseKey = Cogeneration, GroupKey = System.
+
+\subsection{ElectricLoadCenter:Distribution}\label{electricloadcenterdistribution}
+
+ElectricLoadCenter:Distribution objects are used to include on-site electricity generators and or storage in a simulation. The electric load center dispatches both generators and storage according to operation schemes and tracks and reports the amount of electricity generated and purchased. When using on-site generators, the program provides various reports for the electricity used, generated on site, stored, exported etc. There are two separate operation schemes, one for generators and a second for storage, and they can be different. The generator operation is managed before the storage operation. Facility electrical demand tracking is done by the internal or custom meters used by EnergyPlus for reporting. The thermal demand tracking uses internal load calculations from the plant simulation. The dispatching of different generators is based on expectations based on their nominal/rated electric power output. If the current conditions are such that the generator model determines that generation was higher or lower, then the results of the dispatch may differ from expectations.
+
+Multiple different ElectricLoadCenter:Distribution objects can be included in an input file. A great deal of flexibility is available by mixing different load centers and operating schemes. If multiple load centers are used, the supervisory control will dispatch generators sequentially across the load centers. Therefore, the order of these input objects in the IDF file becomes important with the generators associated with first load center in the file being the first to be managed. A certain amount of caution is needed to avoid conflicting operating schemes.
+
+\subsubsection{Inputs}\label{inputs-1-012}
+
+\paragraph{Field: Name}\label{field-name-013}
+
+This alpha field contains the identifying name for the electric load center.
+
+\paragraph{Field: Generator List Name}\label{field-generator-list-name}
+
+This alpha field contains the identifying name for the list of generators in the set defined in an ElectricLoadCenter:Generators object. All the generators connected to this load center need to be of the same type in terms of all AC or all DC. Currently the only DC generators are photovoltaic panels, the others are all AC. A facility with both AC and DC generators will need to use seperate ElectricLoadCenter:Distribution objects. The generator list named here can only be associated with one load center. This field can be left blank if there are no generators.
+
+\paragraph{Field: Generator Operation Scheme Type}\label{field-generator-operation-scheme-type}
+
+This alpha field specifies the type of operating scheme for the generator set. The available operating schemes are Baseload, DemandLimit, TrackElectrical, TrackSchedule, TrackMeter, FollowThermal, and FollowThermalLimitElectrical. The Baseload scheme operates the generators at their rated (requested) electric power output when the generator is scheduled ON (ref. ElectricLoadCenter:Generators). The Baseload scheme requests all generators scheduled ON (available) to operate, even if the amount of electric power generated exceeds the total facility electric power demand. The DemandLimit scheme limits the amount of purchased electrical from the utility to the amount specified in the input object. The DemandLimit scheme tries to have the generators meet all of the demand above the purchased electric limit set by the user in the next field. The TrackElectrical scheme tries to have the generators meet all of the electrical demand for the building. The TrackSchedule scheme tries to have the generators meet all of the electrical demand determined in a user-defined schedule. The TrackMeter scheme tries to have the generators meet all the electrical demand from a meter, which could also be a user-defined custom meter.
+
+The DemandLimit, TrackElectrical, TrackSchedule, and TrackMeter schemes will sequentially load the available generators. All demand not met by available generator capacity (or storage) will be met by purchased electrical. Therefore, if DemandLimit, TrackElectrical, TrackSchedule, or TrackMeter is utilized and the available generators are not enough to meet demand, then purchased electrical will offset the difference. If a generator is needed in the simulation for a small load and it is less than the minimum part load ratio the generator will operate at the minimum part load ratio and the excess will either reduce demand or the excess energy will be available for returning to the electric grid.
+
+The FollowThermal and FollowThermalLimitElectrical schemes are for heat following cogeneration and run the generators to meet the thermal demand. The FollowThermal schemes allow excess electrical generation to be exported to the grid, while the FollowThermalLimitElectrical scheme restricts generator output to a maximum of the building's current electrical demand (so that no electricity is exported). The thermal demand is determined from the plant modeling and depends on the flow requested by other components on the demand side of the plant loop, the loop temperatures, and the loop temperature set point. The electric load center converts the thermal load to an electrical load using a nominal ratio of the thermal to electrical power production for each generator. For these schemes, the generator needs to be connected to the supply side of a plant loop and components that request hot water need to be on the demand side of the plant loop. This is different than the usual configuration for electrical following schemes where the generator is put on the demand side and request flow for the purposes of cooling the generator. Therefore a switch from one of the electrical-based operating schemes to one of the thermal-based operating schemes requires a substantial change in plant topology.
+
+If the load center includes electrical storage, then the choice of generator operating schemes will also affect how storage is managed. The generator operation scheme and dispatch is modeled before the storage operation scheme so that the current generator production is available for use with the storage operation scheme.
+
+\paragraph{Field: Demand Limit Scheme Purchased Electric Demand Limit}\label{field-demand-limit-scheme-purchased-electric-demand-limit}
+
+This numerical field is the user input for the demand limit above which the generators will try and meet the entire electrical load on the building minus the photovoltaic array if available.
+
+\paragraph{Field: Track Schedule Name Scheme Schedule Name}\label{field-track-schedule-name-scheme-schedule-name}
+
+This alpha field is the user input for the name of a schedule defined elsewhere in the input file that contains values for the demand loads placed on the generator(s). The schedule values should be in Watts.
+
+\paragraph{Field: Track Meter Scheme Meter Name}\label{field-track-meter-scheme-meter-name}
+
+This alpha field is the user input for the name of a meter. Any valid meter name can be used here to control the loads that the generator(s) will try to meet. Many different meters are automatically generated by the program and will depend on the objects used throughout the input file. The typical process of determining the exact name to enter in this field involves doing an initial run of EnergyPlus and then examining the *.rdd file which will list the meters and their resulting names. The *.mtd file will also be useful to understand what exactly is included in a meter. The user can also use the Output:CustomMeter objects to redefine meter names and to control what electrical loads are included on them in a flexible manner.
+
+\paragraph{Field: Electrical Buss Type}\label{field-electrical-buss-type}
+
+This alpha field is used to describe how the electric load center is configured with respect to any power conditioning and/or storage equipment. There are five configurations available for load centers that are selected using one of these keywords: AlternatingCurrent, AlternatingCurrentWithStorage, DirectCurrentWithInverter, DirectCurrentWithInverterDCStorage, or DirectCurrentWithInverterACStorage. This input informs the program which of the five pre-configured arrangements is to be used for this load center. The following diagrams show the kinds of devices and how they are arranged for each of the buss types.
+
+\begin{itemize}
+\tightlist
+\item
+  AlternatingCurrent. This type of load center is for adding one or more on-site generators that produce AC power. If the voltage does not match a transformer can be included but is not needed. AlternatingCurrent is the default.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/ACBussDiagram.png}
+\caption{LoadCenterBussType}
+\end{figure}
+
+\begin{itemize}
+\tightlist
+\item
+  AlternatingCurrentWithStorage. This type of load center is for adding one or more on-site generators that produce AC power and one on-site electric storage device that uses AC power. The connection between the load center and the main building panel is bidirectional so that storage can be charged by drawing from the grid. Transformer is optional.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/ACStorageBussDiagram.png}
+\caption{LoadCenterBussType}
+\end{figure}
+
+\begin{itemize}
+\tightlist
+\item
+  DirectCurrentWithInverter. This type of load center is for adding one or more on-site generators that produce DC power, typically photovoltaic panels. An inverter is needed to convert generated power from DC to AC. Transformer is optional.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/DCInverterBussDiagram.png}
+\caption{LoadCenterBussType}
+\end{figure}
+
+\begin{itemize}
+\tightlist
+\item
+  DirectCurrentWithInverterDCStorage. This type of load center is for adding one or more on-site generatros the produce DC power and one on-site storage device that uses DC power. An inverter is needed to convert power from DC to AC and is located between the storage and where the subpanel feeds into the main panel. The connection between the load center and the main building panel is bidirectional so that storage can be charged by drawing from the grid. An AC to DC converter is needed if the storage operation scheme is such that the control might draw power from the main facility panel into the load center in order to charge storage. Transformer is optional.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/DCInverterWithDCStorageBussDiagram.png}
+\caption{LoadCenterBussType}
+\end{figure}
+
+\begin{itemize}
+\tightlist
+\item
+  DirectCurrentWithInverterACStorage. This type of load center is for adding one or more on-site generatros the produce DC power and one on-site storage device that uses AC power. The connection between the load center and the main building panel is bidirectional so that storage can be charged by drawing from the grid. The inverter is located between the generators and the storage device. Transformer is optional.
+\end{itemize}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/DCInverterWithACStorageBussDiagram.png}
+\caption{LoadCenterBussType}
+\end{figure}
+
+\paragraph{Field: Inverter Object Name}\label{field-inverter-object-name}
+
+This field is used to identify the inverter connected to this load center (if any). This field is only used if the Electrical Buss Type is set to DirectCurrentWithInverter, DirectCurrentWithInverterDCStorage, or DirectCurrentWithInverterACStorage and should contain the user-defined name of an inverter object. There are three types of inverter models available -see ElectricLoadCenter:Inverter:Simple, ElectricLoadCenter:Inverter:LookUpTable, or ElectricLoadCenter:Inverter:FunctionOfPower. Enter the name of one of these types of inverter objects defined elsewhere in the input file.
+
+\paragraph{Field: Electrical Storage Object Name}\label{field-electrical-storage-object-name}
+
+This field is used to identify the electrical storage connected to this load center (if any). This field is only used if the Electrical Buss Type is set to AlternatingCurrentWithStorage, DirectCurrentWithInverterDCStorage or DirectCurrentWithInverterACStorage. Enter the name of an ElectricLoadCenter:Storage:* object defined elsewhere in the input file.
+
+\paragraph{Field: Transformer Object Name}\label{field-transformer-object-name}
+
+This field is used to identify the transformer connected to this load center (if any). This field can be used for any electrical buss types. Enter the name of an ElectricLoadCenter:Transformer object defined elsewhere in the input file. The transformer should have use type set to LoadCenterPowerConditioning.
+
+\paragraph{Field: Storage Operation Scheme}\label{field-storage-operation-scheme}
+
+This field is used to select the operation scheme used to govern how storage charge and discharge is controlled. There are four options: TrackFacilityElectricDemandStoreExcessOnSite, TrackMeterDemandStoreExcessOnSite, TrackChargeDischargeSchedules, or FacilityDemandLeveling.
+
+TrackFacilityElectricDemandStoreExcessOnSite indicates that storage control will follow the facility power demand (meter Facility:Electricity) while accounting for any on-site generation. Only excess on site generation gets stored. This is the legacy control behavior before version 8.5 and is the default.
+
+TrackMeterDemandStoreExcessOnSite indicates that storage discharge control will follow an electric meter named in the field called Storage Control Track Meter Name. This scheme is similar TrackFacilityElectricDemandStoreExcessOnSite except that instead of the main facility electric meter, the control is based off of a user-selected meter.
+
+TrackChargeDischargeSchedules indicates that control will follow the charging and discharging power and schedules defined in the fields called Maximum Storage Charge Grid Supply Power, Storage Charge Grid Supply Power Fraction Schedule Name, Design Storage Discharge Grid Export Power, and Storage Discharge Grid Export Fraction Schedule Name.
+
+FacilityDemandLeveling indicates that storage control will attempt to control the facility's power demand drawn from the utility service to a prescribed level. The target utility demand is entered in the fields called Storage Control Utility Demand Limit and Storage Control Utility Demand Limit Fraction Schedule Name. This scheme first accounts for any on-site generation and during times of high use will discharge storage to reduce facility grid demand to meet the target level and during times of low use will charge storage from the grid to increase facility grid demand to meet the target level. This scheme allows controlling the load factor as long as the storage capacity and rates are not limiting what is possible. Negative schedule values can be used so that a negative demand target is exporting power out to the grid.
+
+\paragraph{Field: Storage Control Track Meter Name}\label{field-storage-control-track-meter-name}
+
+This field is the name of a meter to use when a custom meter is to be used. This is required when Storage Operation Scheme is set to TrackMeterDemandStoreExcessOnSite.
+
+\paragraph{Field: Storage Converter Object Name}\label{field-storage-converter-object-name}
+
+This field is the name of an ElectricLoadCenter:Storage:Converter object defined elsewhere in the input file that describes the performance when converting AC to DC when charging DC storage from grid supply. This field is required when using DC storage (buss type DirectCurrentWithInverterDCStorage) with grid supplied charging power (Storage Operation Scheme is set to TrackChargeDischargeSchedules or FacilityDemandLeveling.) Although some inverter devices are bidirectional a separate converter object is needed to describe AC to DC performance.
+
+\paragraph{Field: Maximum Storage State of Charge Fraction}\label{field-maximum-storage-state-of-charge-fraction}
+
+This numeric field specifies the fraction of storage capacity used as an upper limit for controlling charging. Charging will be constrained so that charging will stop the once this limit is reached. This fraction is the state of charge of the storage device where 1.0 is completely full and 0.0 is completely empty. This allows supervisory control over charging to model behavior intended to protect the battery from damage. The legacy behavior prior to version 8.5 was to charge to full capacity and therefore the default is 1.0.
+
+\paragraph{Field: Minimum Storage State of Charge Fraction}\label{field-minimum-storage-state-of-charge-fraction}
+
+This numeric field specifies the fraction of storage capacity used as lower limit for controlling discharging. Discharging will be constrained so that discharging will stop once this limit is reached. This fraction is the state of charge of the storage device where 1.0 is completely full and 0.0 is completely empty. This allows supervisory control over discharging to model behavior intended to protect the battery from damage. The legacy behavior prior to version 8.5 was to discharge to empty and therefore the default is 0.0.
+
+\paragraph{Field: Design Storage Control Charge Power}\label{field-design-storage-control-charge-power}
+
+This field is the design maximum rate that electric power can be charged into storage, in Watts. This field is used as an upper limit for most storage control operation schemes. However for TrackChargeDischargeSchedules, this is the design value for how much power to use when charging and it is multipled by the power fraction schedule in the next field. Required field when using Storage Operation Schemes set to FacilityDemandLeveling or TrackChargeDischargeSchedules.
+
+\paragraph{Field: Storage Charge Power Fraction Schedule Name}\label{field-storage-charge-power-fraction-schedule-name}
+
+This field contains the name of a schedule that controls the timing and magnitude of charging storage. This is a required field if Storage Operation Scheme is set to TrackChargeDischargeSchedules. Schedule values should be fractions from 0.0 to 1.0, inclusive. This schedule will need to be coordinated with the discharging schedule named below.
+
+\paragraph{Field: Design Storage Control Discharge Power}\label{field-design-storage-control-discharge-power}
+
+This field is the design maximum rate that electric power can be discharged from storage. This field is used as an upper limit for most storage control operation schemes. However for TrackChargeDischargeSchedules, this is the design value for how much power to draw when discharging and it is multiplied by the power fraction schedule in the next field. Required field when using Storage Operation Schemes set to FacilityDemandLeveling or TrackChargeDischargeSchedules.
+
+\paragraph{Field: Storage Discharge Power Fraction Schedule Name}\label{field-storage-discharge-power-fraction-schedule-name}
+
+This field contains the name of a schedule that controls the timing and magnitude of discharging storage. Required field if Storage Operation Scheme is set to TrackChargeDischargeSchedules. Schedule values should be fractions from 0.0 to 1.0, inclusive. This schedule will need to be coordinated with the charging schedule named above.
+
+\paragraph{Field: Storage Control Utility Demand Target}\label{field-storage-control-utility-demand-target}
+
+This field contains the design demand target in Watts. This field is used when the storage operation scheme is set to FacilityDemandLeveling. This becomes the target utility service demand power for discharge control. This design value is multiplied by the fraction schedule named in the next field. This is more than an upper limit, it is also going to call for extra electric power to raise demand up to the target and put the extra power into on-site storage. This field is required for FacilityDemandLimit storage operation scheme.
+
+\paragraph{Field: Storage Control Utility Demand Target Fraction Schedule Name}\label{field-storage-control-utility-demand-target-fraction-schedule-name}
+
+This field is the name of schedule that modifies the utility demand power target over time. Schedule values should be fractions from -1.0 to 1.0, inclusive. Negative values indicate export to grid. This field is required if Storage Operation Scheme is set to FacilityDemandLeveling.
+
+Examples of this object are:
+
+\begin{lstlisting}
+
+ElectricLoadCenter:Distribution,
+  SOFC Electric Load Center,      !- Name
+  Micro-Generators,               !- Generator List Name
+  Baseload,                       !- Generator Operation Scheme Type
+  0.0,                            !- Demand Limit Scheme Purchased Electric Demand Limit {W}
+  ,                               !- Track Schedule Name Scheme Schedule Name
+  ,                               !- Track Meter Scheme Meter Name
+  AlternatingCurrent,             !- Electrical Buss Type
+  ,                               !- Inverter Object Name
+  ;                               !- Electrical Storage Object Name
+
+
+  ElectricLoadCenter:Distribution,
+  Electric Load Center,       !- Name
+  Backup Generators,             !- Generator List Name
+  DemandLimit,                         !- Generator Operation Scheme Type
+  10000.0,                                 !- Demand Limit Scheme Purchased Electric Demand Limit {W}
+  ,                                               !- Track Schedule Name Scheme Schedule Name
+  ,                                               !- Track Meter Scheme Meter Name
+  AlternatingCurrent,           !- Electrical Buss Type
+  ,                                               !- Inverter Object Name
+  ;                                               !- Electrical Storage Object Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-008}
+
+There are three levels of results reporting related to electric load centers and generators. The top level of reporting provides results across the whole building and all the different electric load centers and generators. The second level of reporting provides results for individual load centers. The third level is for each type of generator (see individual generator descriptions). This section discusses the first two levels.
+
+Even if no ElectricLoadCenter:Distribution object is included, the following whole-building summary output variables are also available for all simulations that have any electricity consuming equipment.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Facility Total Purchased Electric Power {[}W{]}
+\item
+  HVAC,Sum,Facility Total Purchased Electric Energy {[}J{]}
+\item
+  HVAC,Average,Facility Total Surplus Electric Power {[}W{]}
+\item
+  HVAC,Sum,Facility Total Surplus Electric Energy {[}J{]}
+\item
+  HVAC,Average,Facility Net Purchased Electric Power {[}W{]}
+\item
+  HVAC,Sum,Facility Net Purchased Electric Energy {[}J{]}
+\item
+  HVAC,Average,Facility Total Building Electric Demand Power {[}W{]}
+\item
+  HVAC,Average,Facility Total HVAC Electric Demand Power {[}W{]}
+\item
+  HVAC,Average,Facility Total Electric Demand Power {[}W{]}
+\item
+  HVAC,Average,Facility Total Produced Electric Power {[}W{]}
+\item
+  HVAC,Sum,Facility Total Produced Electric Energy {[}J{]}
+\end{itemize}
+
+These output variables all use a default keyword Whole Building.
+
+\paragraph{Facility Total Purchased Electric Power {[}W{]}}\label{facility-total-purchased-electric-power-w}
+
+\paragraph{Facility Total Purchased Electric Energy {[}J{]}}\label{facility-total-purchased-electric-energy-j}
+
+These outputs are the total of electricity purchased for the entire facility in both power and energy units. This value is always positive and indicates the amount of energy that is purchased from the utility.
+
+\paragraph{Facility Total Surplus Electric Power {[}W{]}}\label{facility-total-surplus-electric-power-w}
+
+\paragraph{Facility Total Surplus Electric Energy {[}J{]}}\label{facility-total-surplus-electric-energy-j}
+
+These outputs are the total excess electricity exported and sent out to the electrical grid in both power and energy units. This value is always positive and indicates the surplus electric power (from generation and/or storage discharge) exceeds the whole-building demand and electricity is being fed from the facility into the grid.
+
+\paragraph{Facility Net Purchased Electric Power {[}W{]}}\label{facility-net-purchased-electric-power-w}
+
+\paragraph{Facility Net Purchased Electric Energy {[}J{]}}\label{facility-net-purchased-electric-energy-j}
+
+These outputs are the net electricity purchased in both Power and Energy units. This value can be either positive or negative. Positive values are defined as electricity purchased from the utility. Negative values are defined as surplus electricity fed back into the grid.
+
+\paragraph{Facility Total Building Electric Demand Power {[}W{]}}\label{facility-total-building-electric-demand-power-w}
+
+This output variable includes all of the electric demand from the building (non-HVAC) portion of the simulation, which would contain lights, electrical equipment, exterior lights and equipment, etc.
+
+\paragraph{Facility Total HVAC Electric Demand Power {[}W{]}}\label{facility-total-hvac-electric-demand-power-w}
+
+This output variable includes all of the electric demand from the HVAC portion of the simulation, which would contain fans, electric coils, pumps, chillers, cooling towers, etc.
+
+\paragraph{Facility Total Electric Demand Power {[}W{]}}\label{facility-total-electric-demand-power-w}
+
+This is the total of the whole Building and HVAC electric demands.
+
+\paragraph{Facility Total Produced Electric Power {[}W{]}}\label{facility-total-produced-electric-power-w}
+
+\paragraph{Facility Total Produced Electric Energy {[}J{]}}\label{facility-total-produced-electric-energy-j}
+
+These outputs are the total generator and photovoltaic electricity produced on-site for the entire model, and they are in both Power and Energy units. When the electric power production system includes power conversion devices including DC to AC inverters, AC to DC converters, or transformers, the power conversion losses are included as negative values in these reports. When electrical storage is used with on-site production, the electricity put into storage is decremented from production and the electricity removed storage is added to production. This means that losses from a round trip through electrical storage decrease on-site electricity production.
+
+Each ElectricLoadCenter also collects results from the individual generators that are connected to that load center. The keywords for these reports are the unique names of ElectricLoadCenter:Distribution objects. The output variables available at the ElectricLoadCenter level are:
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Electric Load Center Produced Electric Power {[}W{]}
+\item
+  HVAC,Sum,Electric Load Center Produced Electric Energy {[}J{]}
+\item
+  HVAC,Average,Electric Load Center Supplied Electric Power {[}W{]}
+\item
+  HVAC,Average,Electric Load Center Drawn Electric Power {[}W{]}
+\item
+  HVAC,Average,Electric Load Center Produced Thermal Rate {[}W{]}
+\item
+  HVAC,Sum,Electric Load Center Produced Thermal Energy {[}J{]}
+\item
+  HVAC,Average,Electric Load Center Requested Electric Power {[}W{]}
+\end{itemize}
+
+\paragraph{Electric Load Center Produced Electric Power {[}W{]}}\label{electric-load-center-produced-electric-power-w}
+
+\paragraph{Electric Load Center Produced Electric Energy {[}J{]}}\label{electric-load-center-produced-electric-energy-j}
+
+These outputs are the sum of electrical energy and power produced by the generators attached to a particular load center. This could be DC or AC depending on the type of buss. The power actually delivered by the load center may be adjusted by power conversion losses from an inverter or transformer or by interaction with the any electrical storage.
+
+\paragraph{Electric Load Center Supplied Electric Power {[}W{]}}\label{electric-load-center-supplied-electric-power-w}
+
+This output is the power fed from the electric load center into the main distribution panel, in Watts. This power is generated or discharged by on site equipment and has been adjusted to account for any power conversion by an inverter and/or transformer on the load center.
+
+\paragraph{Electric Load Center Drawn Electric Power {[}W{]}}\label{electric-load-center-drawn-electric-power-w}
+
+This output is the power fed from the main distribution panel into the load center, in Watts. This power draw is typically only for charging storage with power from either the grid or another load center.
+
+\paragraph{Electric Load Center Produced Thermal Rate {[}W{]}}\label{electric-load-center-produced-thermal-rate-w}
+
+\paragraph{Electric Load Center Produced Thermal Energy {[}J{]}}\label{electric-load-center-produced-thermal-energy-j}
+
+These outputs are the sum of the thermal energy and power produced by the generators attached to a particular load center. The keywords for these reports are the unique names of ElectricLoadCenter:Distribution objects.
+
+\paragraph{Electric Load Center Requested Electric Power {[}W{]}}\label{electric-load-center-requested-electric-power-w}
+
+This output variable is the average electric power supply (in watts) requested of the load center by the facility's main distribution panel, for the time step being reported. This is used by the load center generator and storage operation control logic when determining how to run the generators and/or storage devices. For the baseload generator operating scheme, this output variable should equal the sum of the power supply requests for the available generators associated with this load center (ref. ElectricLoadCenter:Generators). In other cases, this output could be different from the sum of the power supply requests for the generators associated with this load center. For example, a generator might be requested to provide a certain amount of power but can only provide a fraction of the requested amount. In this case the load center will detect this shortfall and include it when calculating the power request for the next available generator. Therefore, the sum of the power supply requests for the individual generators associated with this load center (ref. ElectricLoadCenter:Generators) could be greater than the Electric Load Center Requested Electric Power output variable.
+
+\subsection{ElectricLoadCenter:Generators}\label{electricloadcentergenerators}
+
+The ElectricLoadCenter:Generators object is used to provide a list of the generators to include in the simulation. The list includes the names and types of all the generators along with separate availability schedules, the rated power output, and thermal-to-electrical power ratio for each. Sets of five input fields are repeated for each generator. If more than 30 generators are needed, EnergyPlus will auto-extend to suit the needs but other interfaces (such as the IDF Editor may not). The user can always modify the Energy+.idd file to accommodate the extra fields necessary, but it is likely the next release of EnergyPlus will overwrite any user modifications.
+
+\subsubsection{Inputs}\label{inputs-2-011}
+
+\paragraph{Field: Name}\label{field-name-1-011}
+
+This alpha field contains the identifying name for the generators in the set.
+
+\paragraph{FieldSet: Name, Object Type, Rated Power Output, Availability, Thermal Ratio up to 30}\label{fieldset-name-object-type-rated-power-output-availability-thermal-ratio-up-to-30}
+
+Each generator is specified by a set of 5 input fields that contain an identifying name, a keyword that indicates the type of generator, the rated output of the generator, the availability schedule of the generator, and the thermal to electrical power production ratio.
+
+\paragraph{Field: Generator \textless{}x\textgreater{} Name}\label{field-generator-x-name}
+
+This alpha field contains the identifying name for the first generator in the list.
+
+\paragraph{Field: Generator \textless{}x\textgreater{} Object Type}\label{field-generator-x-object-type}
+
+This alpha field contains the keyword for the type of generator. The available types include:
+
+\begin{itemize}
+\item
+  Generator:InternalCombustionEngine
+\item
+  Generator:CombustionTurbine
+\item
+  Generator:Photovoltaic
+\item
+  Generator:FuelCell
+\item
+  Generator:MicroCHP
+\item
+  Generator:MicroTurbine
+\item
+  Generator:WindTurbine
+\end{itemize}
+
+These keywords are the names of the input objects for the type of generator.
+
+\paragraph{Field: Generator \textless{}x\textgreater{} Rated Electric Power Output}\label{field-generator-x-rated-electric-power-output}
+
+This numeric field contains the nominal electric power output to be requested from generator 1. It is normally equal to the rated power output of the generator in Watts. This value is used only for supervisory control and generator dispatch; the actual power output for each time step is determined by the generator models. This value affects how much a generator is loaded (i.e., requested electric power output) and can also impact the operation of an electric storage unit (e.g., LoadCenter:Storage:Simple) if one is connected to the associated load distribution center (ref. ElectricLoadCenter:Distribution). Refer to Electrical Storage in the EnergyPlus Engineering Reference for more details regarding this input field and its relationship with electric storage.
+
+\paragraph{Field: Generator \textless{}x\textgreater{} Availability Schedule Name}\label{field-generator-x-availability-schedule-name}
+
+This alpha field is used as an identifying field for the generator availability schedule. If not blank, this field must contain the name of a schedule defined elsewhere in the input file. A schedule value of \textless{} = 0.0 indicates the generator is not available, while a schedule value \textgreater{} 0.0 indicates that the generator is available to operate. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Generator \textless{}x\textgreater{} Rated Thermal to Electrical Power Ratio}\label{field-generator-x-rated-thermal-to-electrical-power-ratio}
+
+This numeric field contains the ratio of the rated thermal output to the rated electric output. It is required and used if the operation scheme is set to \textbf{FollowThermal} or \textbf{FollowThermalLimitElectrical}. This nominal ratio is only used for control and dispatch decisions. This value should be generally consistent with the more detailed performance input for the individual generator component models but it is not used in those component models.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+ElectricLoadCenter:Generators,
+  Backup Generators,             !- Name
+  Cat Diesel,                           !- Generator 1 Name
+  Generator:InternalCombustionEngine,   !- Generator 1 Object Type
+  50000,                                     !- Generator 1 Rated Electric Power Output
+  ON PEAK GENERATOR SCHEDULE,   !- Generator 1 Availability Schedule Name
+  ,                                               !- Generator 1 Rated Thermal to Electrical Power Ratio
+  Solar Turbine,                     !- Generator 2 Name
+  Generator:CombustionTurbine,   !- Generator 2 Object Type
+  30000,                                     !- Generator 2 Rated Electric Power Output
+  OFF PEAK GENERATOR SCHEDULE,   !- Generator 2 Availability Schedule Name
+  ,                                               !- Generator 2 Rated Thermal to Electrical Power Ratio
+  Capstone C65,                       !- Generator 3 Name
+  Generator:Microturbine,   !- Generator 3 Object Type
+  65000,                                     !- Generator 3 Rated Electric Power Output
+  MID PEAK GENERATOR SCHEDULE,   !- Generator 3 Availability Schedule Name
+  ;                                               !- Generator 3 Rated Thermal to Electrical Power Ratio
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-007}
+
+A single output variable is available for each generator specified via this object as described below:
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Generator Requested Electric Power {[}W{]}
+\end{itemize}
+
+\paragraph{Generator Requested Electric Power {[}W{]}}\label{generator-requested-electric-power-w}
+
+This output variable represents the average electric power supply in Watts that is being requested by the generator operation scheme from a specific generator for the time step being reported. In some instances the output value may be the Rated Electric Power Output specified for the generator in the ElectricLoadCenter:Generators object. If the generator is not available for a simulation time step (as indicated by its availability schedule), then the power supply request will be zero. The power supply request may be less than the rated electric power output if the overall electric power reduction target has already been met, partially or completely, by electric power produced by other generators. If an EnergyPlus Energy Management System is used to specify an electric power supply request for this generator, then that EMS request will be reflected in this output variable.
+
+\subsection{ElectricLoadCenter:Inverter:Simple}\label{electricloadcenterinvertersimple}
+
+This input object is used to model conversion from Direct Current (DC) to Alternating Current (AC) in an electric load center that contains photovoltaic modules. Such a load center has an array of photovoltaic modules that feed an inverter DC power and the inverter produces AC power. This input object is for the simplest inverter model and uses a fixed efficiency. There are two other types of inverters with more complex models described below.
+
+\subsubsection{Inputs}\label{inputs-3-010}
+
+\paragraph{Field: Name}\label{field-name-2-010}
+
+This field contains a unique name for the inverter. The name entered must also be unique across all other types of inverters that may also be in the input file.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-003}
+
+This field contains the name of a schedule that describes when the inverter is available. If the inverter is scheduled to not be available, by scheduling a value of 0, then it cannot produce AC power and will not consume ancillary power during standby. Any non-zero schedule value means the inverter is available to produce AC power and consume ancillary power during standby. If the Inverter is scheduled to be unavailable but it is being supplied with DC power anyway, then the energy is dissipated as heat. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-003}
+
+This field contains the name of the thermal zone where the inverter is located. Entering a valid name of zone here will direct EnergyPlus to include the inverter s losses as heat gains to the named thermal zone. If the inverter is not within a thermal zone, then this field can be left blank (and the thermal energy associated with inverter losses is removed from the building model).
+
+\paragraph{Field: Radiative Fraction}\label{field-radiative-fraction-1}
+
+This field contains the fraction of inverter thermal losses that enter the zone as long-wave thermal radiation. This should be a factor between 0.0 and 1.0. The balance of the losses is convective. This field is not used if the previous field for zone name is left blank.
+
+\paragraph{Field: Inverter Efficiency}\label{field-inverter-efficiency}
+
+This field contains the value for inverter efficiency. In the simple model, efficiency is a constant. This is the so-called 1-term model. Input data for different types of inverters is available at http://www.gosolarcalifornia.org/equipment/inverter\_tests/summaries where the CEC Efficiency would be the value to enter here.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+ElectricLoadCenter:Inverter:Simple,
+  Simple Ideal Inverter,     !- Name
+  Always On,                             !- Availability Schedule Name
+  ,                                               !- Zone Name
+  0.0,                                         !- Radiative Fraction
+  1.0;                                         !- Inverter Efficiency
+\end{lstlisting}
+
+\subsection{ElectricLoadCenter:Inverter:FunctionOfPower}\label{electricloadcenterinverterfunctionofpower}
+
+This input object is used to model conversion from Direct Current (DC) to Alternating Current (AC) in an electric load center that contains photovoltaic modules. Such a load center has an array of photovoltaic modules that feed an inverter DC power and the inverter produces AC power. This input object is for an inverter model where efficiency is a function of normalized power.
+
+\subsubsection{Inputs}\label{inputs-4-009}
+
+\paragraph{Field: Name}\label{field-name-3-009}
+
+This field contains a unique name for the inverter. The name entered must also be unique across all other types of inverters that may also be in the input file.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-2-001}
+
+This field contains the name of a schedule that describes when the inverter is available. If the inverter is scheduled to not be available, by scheduling a value of 0, then it cannot produce AC power, nor contribute heat gains to the zone, and will not consume ancillary power during standby. Any non-zero schedule value means the inverter is available to produce AC power, contribute heat gains to the zone and consume ancillary power during standby. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-2-001}
+
+This field contains the name of the thermal zone where the inverter is located. Entering a valid name of zone here will direct EnergyPlus to include the inverter s losses as heat gains to the named thermal zone. If the inverter is not within a thermal zone, then this field can be left blank (and the thermal energy associated with inverter losses is removed from the building model).
+
+\paragraph{Field: Radiative Fraction}\label{field-radiative-fraction-2}
+
+This field contains the fraction of inverter thermal losses that enter the zone as long-wave thermal radiation. This should be a factor between 0.0 and 1.0. The balance of the losses is convective. This field is not used if the previous field for zone name is left blank.
+
+\paragraph{Field: Efficiency Function of Power Curve Name}\label{field-efficiency-function-of-power-curve-name}
+
+This field contains the name of curve representing the relationship between DC power input into the inverter and the efficiency with which that power is converted to AC. The curve can be either a Curve:Linear, Curve:Quadratic, or Curve:Cubic. The curve s x value is DC power input normalized by the following field. The result of the curve should be power conversion efficiency expressed as a fraction between 0.0 and 1.0.
+
+\paragraph{Field: Rated Maximum Continuous Input Power}\label{field-rated-maximum-continuous-input-power}
+
+This field contains the rated power input in watts. This is value used to normalize input power for use with the curve named in the previous field. This is DC power from the PV arrays going into the inverter.
+
+\paragraph{Field: Minimum Efficiency}\label{field-minimum-efficiency}
+
+This field contains a minimum bound on the inverter efficiency. This value will be used as a limit on the curve s result.
+
+\paragraph{Field: Maximum Efficiency}\label{field-maximum-efficiency}
+
+This field contains a maximum bound on the inverter efficiency. This value will be used as a limit on the curve s result.
+
+\paragraph{Field: Minimum Power Output}\label{field-minimum-power-output}
+
+This field contains a lower limit on the AC power produced by the inverter. If the resulting power output would be below this level, then the inverter is assumed to not produce any power and is in stand by mode. All DC power input is lost (unless it is going into storage).
+
+\paragraph{Field: Maximum Power}\label{field-maximum-power}
+
+This field contains an upper limit on the AC power produced by the inverter. If the resulting power output would be above this level, then the power produced is capped at this level with the rest of input power converted to losses (unless it is going into storage).
+
+\paragraph{Field: Ancillary Power Consumed In Standby}\label{field-ancillary-power-consumed-in-standby}
+
+This field contains the ancillary power in watts used by the inverter when not producing AC power. This is AC electricity consumed in standby mode. Standby mode occurs when the inverter is scheduled to be available but the incoming DC power is too low.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+ElectricLoadCenter:Inverter:FunctionOfPower,
+  Curve Inverter,                   !- Name
+  ALWAYS_ON,                             !- Availability Schedule Name
+  ,                                               !- Zone Name
+  0.3,                                         !- Radiative Fraction
+  Inverter Curve,                   !- Efficiency Function of Power Curve Name
+  15000,                                     !- Rated Maximum Continuous Input Power {W}
+  0.0,                                         !- Minimum Efficiency
+  1.0,                                         !- Maximum Efficiency
+  200,                                         !- Minimum Power Output {W}
+  20000,                                     !- Maximum Power Output {W}
+  0.0;                                         !- Ancillary Power Consumed In Standby {W}
+\end{lstlisting}
+
+\subsection{ElectricLoadCenter:Inverter:LookUpTable}\label{electricloadcenterinverterlookuptable}
+
+This input object is used to model conversion from Direct Current (DC) to Alternating Current (AC) in an electric load center that contains photovoltaic modules. Such a load center has an array of photovoltaic modules that feed an inverter DC power and the inverter produces AC power. This input object is for an inverter model where efficiency is interpolated using a look up table.
+
+This object was designed for use with data contained in the Inverter Performance Test Summaries available at http://www.gosolarcalifornia.org/equipment/inverter\_tests/summaries. All of the data needed for this object can be found there by make and model of inverter. The core of the data set is a 3x6 matrix of efficiency at different voltage and power levels. These form the look up table used in the model. Note that EnergyPlus PV models currently model only power and not the voltage and current situation. Therefore, only the nominal voltage data are used. This is the middle row of data in the Go Solar summaries.
+
+\subsubsection{Inputs}\label{inputs-5-008}
+
+\paragraph{Field: Name}\label{field-name-4-008}
+
+This field contains a unique name for the inverter. The name entered must also be unique across all other types of inverters that may also be in the input file.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-3-001}
+
+This field contains the name of a schedule that describes when the inverter is available. If the inverter is scheduled to not be available, by setting a value of 0, then it cannot produce AC power, nor contribute heat gains to the zone, and will not consume ancillary power during standby. Any non-zero schedule value means the inverter is available to produce AC power, contribute heat gains to the zone and consume ancillary power during standby. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-3-000}
+
+This field contains the name of the thermal zone where the inverter is located. Entering a valid name of zone here will direct EnergyPlus to include the inverter s losses as heat gains to the named thermal zone. If the inverter is not within a thermal zone, then this field can be left blank (and the thermal energy associated with inverter losses is removed from the building model).
+
+\paragraph{Field: Radiative Fraction}\label{field-radiative-fraction-3}
+
+This field contains the fraction of inverter thermal losses that enter the zone as long-wave thermal radiation. This should be a factor between 0.0 and 1.0. The balance of the losses is convective. This field is not used if the previous field for zone name is left blank.
+
+\paragraph{Field: Rated Maximum Continuous Output Power}\label{field-rated-maximum-continuous-output-power}
+
+This field contains the rated maximum continuous output power in watts.
+
+\paragraph{Field: Night Tare Loss Power}\label{field-night-tare-loss-power}
+
+This field contains the night tare loss in watts. This is modeled as ancillary power consumed during standby.
+
+\paragraph{Field: Nominal Voltage Input}\label{field-nominal-voltage-input}
+
+This field contains the nominal DC input voltage in volts. This is Vnom in the Go Solar test summaries.
+
+\paragraph{Field: Efficiency at 10\% Power and Nominal Voltage}\label{field-efficiency-at-10-power-and-nominal-voltage}
+
+This field contains the fractional efficiency at nominal voltage and 10\% power.
+
+\paragraph{Field: Efficiency at 20\% Power and Nominal Voltage}\label{field-efficiency-at-20-power-and-nominal-voltage}
+
+This field contains the fractional efficiency at nominal voltage and 20\% power.
+
+\paragraph{Field: Efficiency at 30\% Power and Nominal Voltage}\label{field-efficiency-at-30-power-and-nominal-voltage}
+
+This field contains the fractional efficiency at nominal voltage and 30\% power.
+
+\paragraph{Field: Efficiency at 50\% Power and Nominal Voltage}\label{field-efficiency-at-50-power-and-nominal-voltage}
+
+This field contains the fractional efficiency at nominal voltage and 50\% power.
+
+\paragraph{Field: Efficiency at 75\% Power and Nominal Voltage}\label{field-efficiency-at-75-power-and-nominal-voltage}
+
+This field contains the fractional efficiency at nominal voltage and 75\% power.
+
+\paragraph{Field: Efficiency at 100\% Power and Nominal Voltage}\label{field-efficiency-at-100-power-and-nominal-voltage}
+
+This field contains the fractional efficiency at nominal voltage and 100\% power.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+ElectricLoadCenter:Inverter:LookUpTable,
+  PV Inverter,                         !- Name
+  ALWAYS_ON,                             !- Availability Schedule Name
+  ,                                               !- Zone Name
+  0.25,                                       !- Radiative Fraction
+  14000,                                     !- Rated Maximum Continuous Output Power {W}
+  200.0,                                     !- Night Tare Loss Power {W}
+  368,                                         !- Nominal Voltage Input {V}
+  0.839,                                     !- Efficiency at 10% Power and Nominal Voltage
+  0.897,                                     !- Efficiency at 20% Power and Nominal Voltage
+  0.916,                                     !- Efficiency at 30% Power and Nominal Voltage
+  0.931,                                     !- Efficiency at 50% Power and Nominal Voltage
+  0.934,                                     !- Efficiency at 75% Power and Nominal Voltage
+  0.930;                                     !- Efficiency at 100% Power and Nominal Voltage
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-005}
+
+Each inverter can report the following seven output variables.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Inverter DC to AC Efficiency {[]}
+\item
+  HVAC,Average,Inverter DC Input Electric Power {[}W{]}
+\item
+  HVAC,Sum,Inverter DC Input Electric Energy {[}J{]}
+\item
+  HVAC,Average,Inverter AC Output Electric Power {[}W{]}
+\item
+  HVAC,Sum,Inverter AC Output Electric Energy {[}J{]}
+\item
+  HVAC,Average,Inverter Conversion Loss Power {[}W{]}
+\item
+  HVAC,Sum,Inverter Conversion Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Inverter Conversion Loss Decrement Energy {[}J{]}
+\item
+  HVAC,Average,Inverter Thermal Loss Rate {[}W{]}
+\item
+  HVAC,Sum,Inverter Thermal Loss Energy {[}J{]}
+\item
+  HVAC,Average,Inverter Ancillary AC Electric Power {[}W{]}
+\item
+  HVAC,Sum,Inverter Ancillary AC Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Inverter DC to AC Efficiency {[]}}{Inverter DC to AC Efficiency }}\label{inverter-dc-to-ac-efficiency}
+
+This is the efficiency with which DC power is converted to AC power by the inverter.
+
+\paragraph{Inverter DC Input Elecric Power {[}W{]}}\label{inverter-dc-input-elecric-power-w}
+
+\paragraph{Inverter DC Input Electric Energy {[}J{]}}\label{inverter-dc-input-electric-energy-j}
+
+These outputs are total electricity power or energy fed into the inverter. This is Direct Current from photovoltaics (or DC-based electrical storage) going into the inverter.
+
+\paragraph{Inverter AC Output Electric Power {[}W{]}}\label{inverter-ac-output-electric-power-w}
+
+\paragraph{Inverter AC Output Electric Energy {[}J{]}}\label{inverter-ac-output-electric-energy-j}
+
+These outputs are the total electricity power or energy produced by the inverter. This is Alternating Current going out of the inverter.
+
+\paragraph{Inverter Conversion Loss Power {[}W{]}}\label{inverter-conversion-loss-power-w}
+
+\paragraph{Inverter Conversion Loss Energy {[}J{]}}\label{inverter-conversion-loss-energy-j}
+
+\paragraph{Inverter Conversion Loss Decrement Energy {[}J{]}}\label{inverter-conversion-loss-decrement-energy-j}
+
+These outputs are the thermal power or energy losses in the inverter that stem from converting from DC to AC. The decrement energy is negative and is metered as ``PowerConversion'' on the ``ElectricityProduced'' resource.
+
+\paragraph{Inverter Thermal Loss Rate {[}W{]}}\label{inverter-thermal-loss-rate-w}
+
+\paragraph{Inverter Thermal Loss Energy {[}J{]}}\label{inverter-thermal-loss-energy-j}
+
+These outputs are the thermal power or energy losses in the inverter that stem from converting from DC to AC plus any ancillary electric power.
+
+\paragraph{Inverter Ancillary AC Electric Power {[}W{]}}\label{inverter-ancillary-ac-electric-power-w}
+
+\paragraph{Inverter Ancillary AC Electric Energy {[}J{]}}\label{inverter-ancillary-ac-electric-energy-j}
+
+These outputs are the Alternating Current electricity consumed by the inverter. These are ancillary, or night tare loss, power uses by the inverter and modeled as if powered by the building s grid connection. These ancillary power draws generally occur when the inverter is not generating power but waiting in a standby mode ready to begin generating power.
+
+\subsection{ElectricLoadCenter:Storage:Converter}\label{electricloadcenterstorageconverter}
+
+This model is for converting AC to DC for grid-supplied charging of DC storage. The model is only for power conversion and does not consider voltage. There are two methods available for determining the efficiency with which power is converted. The efficiency is defined as the ratio of DC power output divided by AC power input. If the name of a zone is entered the power conversion losses will be added to the zone as internal heat gains. The converter is part of a single electric load center.
+
+\subsubsection{Field: Name}\label{field-name-5-007}
+
+This field contains a unique name for the AC to DC converter. This name will be referenced in an ElectricLoadCenter:Distribution object.
+
+\subsubsection{Field: Availability Schedule Name}\label{field-availability-schedule-name-4-001}
+
+This field contains the name of a schedule that describes when the power converter is available. If power conversion is not available then electric power from the grid cannot be used to charge storage. Any non-zero value means the converter is available. If this field is blank, the schedule has a value of 1 for all time periods and the converter is always available. Standby power consumption is on when converter is available and off when the converter is not available.
+
+\subsubsection{Field: Power Conversion Efficiency Method}\label{field-power-conversion-efficiency-method}
+
+This choice field is used to select which method is used to define the efficiency with which power is converted from AC to DC. There are two options: SimpleFixed or FunctionOfPower. - SimpleFixed indicates that power conversion efficiency is a constant with the value set in the next field. There is no need to size the converter (with a value in the field called Design Maximum Continuous Input Power) and varying levels of power do not affect the efficiency. SimpleFixed is the default. - FunctionOfPower indicates that the power conversion efficiency is a function of the level of power being converted. This method is intended to model the characteristic that converters tend to operate less efficiently when loaded well below their design size. The converter must be sized with a value in the Design Maximum Continuous Input Power and the functional relationship described in a performance curve or look-up table.
+
+\subsubsection{Field: Simple Fixed Efficiency}\label{field-simple-fixed-efficiency}
+
+This numeric field is used to set a constant efficiency for conversion of AC to DC at all power levels. This field is only used, and is required, when the Power Conversion Efficiency Method is set to SimpleFixed. The value must be greater than 0.0 and less than equal to 1.0. The default is 0.95.
+
+\subsubsection{Field: Design Maximum Continuous Input Power}\label{field-design-maximum-continuous-input-power}
+
+This numeric field describes the size of the power converter in terms of its design input power level, in Watts. This is the AC power going into the converter. This field is only used, and is required, when the the Power Conversion Efficiency Method is set to FunctionOfPower. This input serves as an upper limit for the AC power input and is used to normalize power for use in the performance curve or table. The AC power being converted at any given time is divided by the value in this field.
+
+\subsubsection{Field: Efficiency Function of Power Curve Name}\label{field-efficiency-function-of-power-curve-name-1}
+
+This field is the name of a performance curve or table object that describes how efficiency varies as a function of normalized power. The single independent ``x'' variable input for the curve or table is the ratio of AC input power at a given time divided by design power in the previous field. The result of the curve should be the power conversion efficiency for that normalized power so that DC power output is the product of efficiency multiplied by the AC power input. Any of the single-variable performance curves or lookup table objects can be used to describe performance. This field is only used, and is required, when the the Power Conversion Efficiency Method is set to FunctionOfPower.
+
+\subsubsection{Field: Ancillary Power Consumed In Standby}\label{field-ancillary-power-consumed-in-standby-1}
+
+This numeric field describes the ancillary power consumed by the converter when it is available but not converting power, in Watts. This field is optional and can be used with any of the efficiency methods. If this converter is really on mode of a bidirectional inverter, take care not to double count the ancillary consumption by including them in both this component and the inverter component.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-4-000}
+
+This field is the name of thermal zone where the converter is located. If this field is omitted then the converter is considered outdoors. The power lost during the conversion process is treated as heat gains and added the thermal zone named in this field. The split between radiation and convection can be controlled in the next input field.
+
+\#\#\#\# Field: Radiative Fraction
+
+This numeric field is the fraction of zone heat gains that are handled as infrared thermal radiation. This field is only used if a zone is named in the previous field. The portion of zone gains that are not radiative are added to the zone as convection. If a zone is named and this field left blank or omitted then all the zone heat gains will be convective.
+
+An example IDF showing how this object is used is provided below:
+
+ElectricLoadCenter:Storage:Converter, Grid Charge Converter , !- Name ALWAYS\_ON , !- Availability Schedule Name SimpleFixed , !- Power Conversion Efficiency Method 0.95 , !- Simple Fixed Efficiency , !- Design Maximum Continuous Input Power , !- Efficiency Function of Power Curve Name 20 , !- Ancillary Power Consumed In Standby , !- Zone Name 0.25; !- Radiative Fraction
+
+\subsection{Electric Load Center Converter Outputs}\label{electric-load-center-converter-outputs}
+
+Each converter can report the following output variables
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Converter AC to DC Efficiency {[]}
+\item
+  HVAC,Average,Converter AC Input Electric Power {[}W{]}
+\item
+  HVAC,Sum,Converter AC Input Electric Energy {[}J{]}
+\item
+  HVAC,Average,Converter DC Output Electric Power {[}W{]}
+\item
+  HVAC,Sum,Converter DC Output Electric Energy {[}J{]}
+\item
+  HVAC,Average,Converter Electric Loss Power {[}W{]}
+\item
+  HVAC,Sum,Converter Electric Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Converter Electric Loss Decrement Energy {[}J{]}
+\item
+  HVAC,Average,Converter Thermal Loss Rate {[}W{]}
+\item
+  HVAC,Sum,Converter Thermal Loss Energy {[}J{]}
+\item
+  HVAC,Average,Converter Ancillary AC Electric Power {[}W{]}
+\item
+  HVAC,Sum,Converter Ancillary AC Electric Energy {[}J{]}
+\end{itemize}
+
+\subsubsection{\texorpdfstring{Converter AC to DC Efficiency {[]}}{Converter AC to DC Efficiency }}\label{converter-ac-to-dc-efficiency}
+
+This is the efficiency with which AC power is converted to DC power by the converter
+
+\subsubsection{Converter AC Input Electric Power {[}W{]}}\label{converter-ac-input-electric-power-w}
+
+\subsubsection{Converter AC Input Electric Energy {[}J{]}}\label{converter-ac-input-electric-energy-j}
+
+These outputs are the total electric power or energy fed into the converter. This is Alternating Current, or AC, drawn from the main panel into the load center.
+
+\subsubsection{Converter DC Output Electric Power {[}W{]}}\label{converter-dc-output-electric-power-w}
+
+\subsubsection{Converter DC Output Electric Energy {[}J{]}}\label{converter-dc-output-electric-energy-j}
+
+These outputs are the total electric power or energy leaving the converter. This is Direct Current, or DC, that will go into charging storage.
+
+\subsubsection{Converter Electric Loss Power {[}W{]}}\label{converter-electric-loss-power-w}
+
+\subsubsection{Converter Electric Loss Energy {[}J{]}}\label{converter-electric-loss-energy-j}
+
+\subsubsection{Converter Electric Loss Decrement Energy {[}J{]}}\label{converter-electric-loss-decrement-energy-j}
+
+These outputs are the conversion losses that result from inefficiencies in the conversion from AC to DC. The power and energy are positive while the decrement energy is negative and is metered on the ``PowerConversion'' end use for ``ElectricityProduced''.
+
+\subsubsection{Converter Thermal Loss Rate {[}W{]}}\label{converter-thermal-loss-rate-w}
+
+\subsubsection{Converter Thermal Loss Energy {[}J{]}}\label{converter-thermal-loss-energy-j}
+
+These outputs are the power and energy losses that result from the inefficiencies in the conversion from AC to DC and the ancillary standby power.
+
+\subsubsection{Converter Ancillary AC Electric Power {[}W{]}}\label{converter-ancillary-ac-electric-power-w}
+
+\subsubsection{Converter Ancillary AC Electric Energy {[}J{]}}\label{converter-ancillary-ac-electric-energy-j}
+
+These outputs are the power and energy consumed in standby operation when the converter is not being used but is available and ready to be used. The ancillary power consumption is metered on the ``Cogeneration'' end use for ``Electricity.''
+
+\subsection{ElectricLoadCenter:Storage:Simple}\label{electricloadcenterstoragesimple}
+
+This input object is used to model storage of electricity in an electric load center. This is a simple model that does not attempt to represent any of the characteristics of a real storage device such as a battery. The type of power, AC or DC, depends on the configuration chosen as the Electrical Buss Type in the ElectricLoadCenter:Distribution object.
+
+\subsubsection{Inputs}\label{inputs-6-007}
+
+\paragraph{Field: Name}\label{field-name-6-005}
+
+This field contains a unique name for the electric storage device.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-5-000}
+
+This field contains the name of a schedule that describes when the storage device is available. If storage is not available, by scheduling a value of 0, then no electrical energy can be stored or drawn from the device. Any non-zero schedule value means the devices is available. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-5-000}
+
+This field contains the name of the thermal zone where the storage device is located. Entering a valid name of a zone here will direct EnergyPlus to include the storage losses as heat gains to the name thermal zone. If the storage is not within a therma zone, then this field can be left blank.
+
+\paragraph{Field: Radiative Fraction for Zone Heat Gains}\label{field-radiative-fraction-for-zone-heat-gains}
+
+This field contains the fraction of storage losses that enter the zone as long-wave thermal radiation. This should be a factor between 0.0 and 1.0. The balance of the losses are convective. This field is not used if the previous field for zone name is left blank.
+
+\paragraph{Field: Nominal Energetic Efficiency for Charging}\label{field-nominal-energetic-efficiency-for-charging}
+
+This field contains the charging efficiency. This is the energetic efficiency of storing electrical energy in the storage device. A value of 1.0 means the device does not lose any energy when charging.
+
+\paragraph{Field: Nominal Discharging Energetic Efficiency}\label{field-nominal-discharging-energetic-efficiency}
+
+This field contains the discharging efficiency. This is the energetic efficiency of drawing electrical energy from the storage device. A value of 1.0 means the device does not lose any energy when drawing power.
+
+\paragraph{Field: Maximum Storage Capacity}\label{field-maximum-storage-capacity}
+
+This field describes the maximum amount of energy that can be stored in the device in Joules. Once the storage device is full, no additional energy can be stored in it.
+
+\paragraph{Field: Maximum Power for Discharging}\label{field-maximum-power-for-discharging}
+
+This field describes the maximum rate at which electrical power can be discharged from the storage device in watts.
+
+\paragraph{Field: Maximum Power for Charging}\label{field-maximum-power-for-charging}
+
+This field describes the maximum rate at which electrical power can be stored in the device in watts.
+
+\paragraph{Field: Initial State of Charge}\label{field-initial-state-of-charge}
+
+This field describes the value for the initial state of charge in Joules. This is used to model the storage device as having some amount of stored energy at the beginning of the simulation period.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+ElectricLoadCenter:Storage:Simple,
+  Battery,                                 !- Name
+  ALWAYS_ON,                             !- Availability Schedule Name
+  ,                                               !- Zone Name
+  0.0,                                         !- Radiative Fraction for Zone Heat Gains
+  0.7,                                         !- Nominal Energetic Efficiency for Charging
+  0.7,                                         !- Nominal Discharging Energetic Efficiency
+  1.0E11,                                   !- Maximum Storage Capacity {J}
+  50000,                                     !- Maximum Power for Discharging {W}
+  25000,                                     !- Maximum Power for Charging {W}
+  1.0E10;                                   !- Initial State of Charge {J}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-003}
+
+Each electrical storage device can report the following seven output variables.
+
+\begin{itemize}
+\item
+  HVAC,Average,Electric Storage Simple Charge State {[}J{]}
+\item
+  HVAC,Average,Electric Storage Charge Power {[}W{]}
+\item
+  HVAC,Sum,Electric Storage Charge Energy {[}J{]}
+\item
+  HVAC,Average,Electric Storage Discharge Power {[}W{]}
+\item
+  HVAC,Sum,Electric Storage Discharge Energy {[}J{]}
+\item
+  HVAC,Average,Electric Storage Thermal Loss Rate {[}W{]}
+\item
+  HVAC,Sum,Electric Storage Thermal Loss Energy {[}J{]}
+\item
+  HVAC,Sum,Electric Storage Production Decrement Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Electric Storage Simple Charge State {[}J{]}}\label{electric-storage-simple-charge-state-j}
+
+This output is the state of charge of the storage device. State of charge is the amount of electrical energy stored in the device at a point of time. The amount of energy stored in tracked in Joules.
+
+\paragraph{Electric Storage Charge Power {[}W{]}}\label{electric-storage-charge-power-w}
+
+\paragraph{Electric Storage Charge Energy {[}J{]}}\label{electric-storage-charge-energy-j}
+
+These outputs are total electricity power or energy fed into the storage device. This is the rate or amount of charging.
+
+\paragraph{Electric Storage Production Decrement Energy {[}J{]}}\label{electric-storage-production-decrement-energy-j}
+
+This output is the total electricity energy decremented from electricity production because it has fed into the storage device. This output has the opposite sign of Electric Storage Charge Energy but is otherwise similar. This decrement output variable is also a meter associated with the resource type ElectricityProduced that reduces the metered electricity production to account for power that went into storage after production.
+
+\paragraph{Electric Storage Discharge Power {[}W{]}}\label{electric-storage-discharge-power-w}
+
+\paragraph{Electric Storage Discharge Energy {[}J{]}}\label{electric-storage-discharge-energy-j}
+
+These outputs are total electricity power or energy drawn from the storage device. This is the rate or amount of discharging. The energy from storage output variable is also a meter associated with the resource type ElectricityProduced that increases the metered electricity production to account for power that has come back out of storage.
+
+\paragraph{Electric Storage Thermal Loss Rate {[}W{]}}\label{electric-storage-thermal-loss-rate-w}
+
+\paragraph{Electric Storage Thermal Loss Energy {[}J{]}}\label{electric-storage-thermal-loss-energy-j}
+
+These outputs are the thermal power or energy losses from both charging and drawing electrical power in or out of the storage device. These losses are the result of inefficiencies in charging and drawing.
+
+\subsection{ElectricLoadCenter:Storage: Battery}\label{electricloadcenterstorage-battery}
+
+This object uses the kinetic battery model (KiBaM) to simulate rechargeable battery banks in an electrical load center. The battery bank is a collection of one or more individual battery modules. Given the surplus or deficit power from the electrical system and the state of charge from the previous time step, this object can model the voltage, current, and energy losses with charging and discharging during each time step. The cumulative battery damage can be also modeled and reported at the end of each simulation run.
+
+This object allows the simulation of both lead-acid and Nickel Cadmium batteries. With input parameters derived from specific battery tests, the object is expected to support other battery types such as Lithium-ion batteries.
+
+The kinetic battery model assumes that part of the battery s energy storage capacity is immediately available in discharging or charging while the rest is chemically bound. As a function of constant current, the battery capacity is related to three parameters: the maximum capacity at infinitesimal current, the capacity ratio of available charges, and the conversion ratio between available charges and bound charges. These parameters are usually obtained via curve fitting based on battery data sheets or test data.
+
+Each individual battery module is modeled as a voltage source in series with an electrical resistance. KiBaM assumes that the internal resistance is constant and the open circuit voltage varies with the electric current, the state of charge and the operation mode (charging or discharging). For an individual battery module, the open circuit voltage at any time is correlated to the voltage at fully charged/discharged state and three other regression coefficients. These regression coefficients are usually obtained via curve fitting based on battery test data.
+
+The object offers user the option to perform battery life calculation. If battery life is modeled, the user needs to provide a group of coefficients for the correlation between the number of cycles for battery failure and the corresponding cycle range. More detailed information can be found from the Engineering Reference.
+
+\subsubsection{Field: Name}\label{field-name-7-004}
+
+This alpha field contains the identifying name for the battery bank.
+
+\subsubsection{Field: Availability Schedule Name}\label{field-availability-schedule-name-6-000}
+
+This alpha field contains the schedule name (ref. Schedule objects) that describes when the battery is available. A schedule value greater than 0 (usually 1 is used) indicates that electrical energy can be stored or drawn from the battery. A value less than or equal to 0 (usually 0 is used) denotes that the battery is not available. If this field is blank, the schedule has values of 1 for all time periods.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-6-000}
+
+This field contains the name of the thermal zone where the battery is located. Entering a valid name of zone here will direct EnergyPlus to include the energy storage losses as heat gains to the named thermal zone. If the battery is not within a thermal zone, this field can be left blank and the thermal energy associated with storage losses is removed from the building model.
+
+\subsubsection{Field: Radiative Fraction}\label{field-radiative-fraction-4}
+
+This field contains the fraction of storage losses that enter the zone as long-wave thermal radiation. This numeric filed should have a value between 0.0 and 1.0. The balance of the losses is convective. This field is not used if the previous field for zone name is left blank.
+
+\subsubsection{Field: Number of Battery Modules in Parallel}\label{field-number-of-battery-modules-in-parallel}
+
+This field defines the number of modules connected in parallel in the battery bank.
+
+\subsubsection{Field: Number of Battery Modules in Series}\label{field-number-of-battery-modules-in-series}
+
+This field defines the number of modules connected in series in the battery bank. The total number of modules in a battery bank is equal to the number of modules in parallel times the number of modules in series.
+
+\subsubsection{Field: Maximum Module Capacity}\label{field-maximum-module-capacity}
+
+This field indicates the maximum capacity of one battery module. It is evaluated as the total Amp-hours available when a full battery is discharged at infinitesimal current. This capacity is for an individual battery module, not for the whole battery bank. The maximum capacity can be found from manufacture s data or derived from test data by curve fitting.
+
+\subsubsection{Field: Initial Fractional State of Charge}\label{field-initial-fractional-state-of-charge}
+
+This field describes the initial state of charge in terms of the fraction of maximum capacity as defined in the previous field.
+
+\subsubsection{Field: Fraction of Available Charge Capacity}\label{field-fraction-of-available-charge-capacity}
+
+The kinetic battery model assumes that battery is a two-tank electrical energy storage device: an available tank and a bound tank. The available tank can be immediately charged or discharged, while the bound tank can only be charged or discharged via the available tank. This field specifies the fraction of total charge in the battery that is part of the available tank. The ratio of available charge capacity to total capacity is a parameter usually derived from test data by curve fitting.
+
+\subsubsection{Field: Change Rate from Bound Charge to Available Charge}\label{field-change-rate-from-bound-charge-to-available-charge}
+
+This field specifies the rate at which the charge flows between the available tank and the bound tank. It is a parameter used to calculate the conversion between available charge and chemically bound charge when charging and discharging the battery. This parameter is usually derived from test data by curve fitting.
+
+\subsubsection{Field: Fully Charged Module Open Circuit Voltage}\label{field-fully-charged-module-open-circuit-voltage}
+
+This field indicates the open circuit voltage for a fully charged battery module. It can be found from manufacture s data or battery tests.
+
+\subsubsection{Field: Fully Discharged Module Open Circuit Voltage}\label{field-fully-discharged-module-open-circuit-voltage}
+
+This field indicates the open circuit voltage for a fully discharged battery module. It can be found from manufacture s data or battery tests.
+
+\subsubsection{Field: Voltage Change Curve Name for Charging}\label{field-voltage-change-curve-name-for-charging}
+
+This field specifies the name of a rectangular hyperbola type 2 performance curve (ref: Curve:RectangularHyperbola2 in Performance Curves) that determines the change of open circuit voltage (\(\Delta E\) ) as a function of the battery state of charge in charging. The change of open circuit voltage is relative to a fully discharged battery.
+
+The curve has the following form:
+
+\begin{equation}
+\Delta E = ({C_1}*X)/({C_2} + X) + {C_3}*X
+\end{equation}
+
+where X is the battery charge divided by the maximum capacity at a given current. More details can be found from the Engineering Reference.
+
+\subsubsection{Field: Voltage Change Curve Name for Discharging}\label{field-voltage-change-curve-name-for-discharging}
+
+This field specifies the name of a rectangular hyperbola type 2 performance curve (ref: Curve:RectangularHyperbola2 in Performance Curves) that determines the change of open circuit voltage (\(\Delta E\) ) as a function of the battery state of charge in discharging. The change of open circuit voltage is relative to a fully charged battery.
+
+The curve has the following form:
+
+\begin{equation}
+\Delta E = ({C_1}*X)/({C_2} + X) + {C_3}*X
+\end{equation}
+
+where X is the removed charge divided by the maximum capacity at a given current. More details can be found from the Engineering Reference.
+
+\subsubsection{Field: Module Internal Electrical Resistance}\label{field-module-internal-electrical-resistance}
+
+This field specifies the battery internal resistance in ohms. In theory, the electrical resistance within the battery varies with the state of charge and depends on whether it is in charging or discharging. In the kinetic battery model, the internal resistance is assumed as constant and the terminal voltage varies with current and state of charge. The internal resistance may be obtained from the battery manufacture or battery test data. Note that the field is for an individual module, not for the whole battery bank.
+
+\subsubsection{Field: Maximum Module Discharging Current}\label{field-maximum-module-discharging-current}
+
+This field indicates the maximum current at which the battery can be discharged continuously. The limit on discharge current is usually defined by the battery manufacture to avoid battery damage. The limit is for an individual battery module.
+
+\subsubsection{Field: Module Cut-off Voltage}\label{field-module-cut-off-voltage}
+
+This field specifies the minimum allowable voltage, below which the battery is generally regarded as empty. The cut-off voltage is usually defined by the battery manufacture and it is for an individual battery module.
+
+\subsubsection{Field: Module Charge Rate Limit}\label{field-module-charge-rate-limit}
+
+This field specifies the limit on charging current relative to the remaining charge until the battery is full. This limit reflects the common practice that the charge rate is reduced as the battery gets more charged.
+
+\subsubsection{Field: Battery Life Calculation}\label{field-battery-life-calculation}
+
+This field indicates whether the battery life model is activated in the simulation. If the battery life model is activated, the following five inputs on curve coefficients are required; otherwise, they are not used.
+
+\subsubsection{Field: Number of Cycle Bins}\label{field-number-of-cycle-bins}
+
+This field specifies the number of equally ranged cycle bins in battery life simulation. If 10 bins are used, the cycle ranges will include 10\%, 20\%, \ldots{}, 100\%.
+
+\subsubsection{Field: Battery Cycle Life Curve Name}\label{field-battery-cycle-life-curve-name}
+
+This field specifies the name of a double exponential decay curve (ref: Curve:DoubleExponentialDecay in Performance Curves) that correlates the cycles of battery failure (C\(_{F}\)) and fractional depth of discharge (R). The curve is:
+
+\begin{equation}
+{C_F} = {C_1} + {C_2}{e^{{C_3}R}} + {C_4}{e^{{C_5}R}}
+\end{equation}
+
+An example input of the ElectricLoadCenter:Storage: Battery input is:
+
+\begin{lstlisting}
+
+ElectricLoadCenter:Storage:Battery,
+  Lead Acid Battery A,   !-Name
+  Always On,                       !- Availability Schedule Name
+  ,                                         !- Zone Name
+  ,                                         !-Radiative Fraction
+  1,                                       !- Number of Battery Modules in Parallel
+  1,                                       !- Number of Battery Modules in Series
+  86.1,                                 !- Maximum Module Capacity {Ah}
+  1.0,                                   !- Initial Fractional State of Charge
+  0.3747,                             !- Fraction of Available Charge Capacity
+  0.5874,                             !- Change Rate from Bound Charge to Available Charge {hr$^{-1}$}
+  12.60,                               !- Fully Charged Module Open Circuit Voltage {V}
+  12.37,                               !- Fully Discharged Module Open Circuit Voltage {V}
+  BatteryChargeCurve,     !- Voltage Change Curve Name for Charging
+  BatteryDischargeCurve,!- Voltage Change Curve Name for Discharging
+  0.0538,                             !- Module Internal Electrical Resistance {Ohm}
+  100,                                   !- Maximum Module Discharging Current {A}
+  10.2,                                 !- Module Cut-off Voltage {V}
+  1,                                       !- Module Charge Rate Limit {1/hr}
+  Yes,                                   !- Battery Life Calculation
+  10,                                   !- Number of Cycle Bins
+  BatteryCycleCurve;       !- Battery Cycle Life Curve Name
+
+  Curve:RectangularHyperbola2,
+  BatteryChargeCurve,     !- Name
+  -0.2765,                           !- Coefficient1 C1
+  -93.27,                             !- Coefficient2 C2
+  0.0068,                             !- Coefficient3 C3
+  0,                                       !- Minimum Value of x
+  1.0,                                   !- Maximum Value of x
+  -100,                                 !- Minimum Curve Output
+  100;                                   !- Maximum Curve Output
+
+  Curve:RectangularHyperbola2,
+  BatteryDischargeCurve,     !- Name
+  0.0899,                                   !- Coefficient1 C1
+  -98.24,                                   !- Coefficient2 C2
+  -0.0082,                                 !- Coefficient3 C3
+  0,                                             !- Minimum Value of x
+  1.0,                                         !- Maximum Value of x
+  -100,                                       !- Minimum Curve Output
+  100;                                         !- Maximum Curve Output
+
+  Curve:DoubleExponentialDecay,
+  BatteryCycleCurve,         !- Name
+  1380,                                   !- Coefficient1 C1
+  6834,                                   !- Coefficient2 C2
+  -8.75,                                 !- Coefficient3 C3
+  6747,                                   !- Coefficient4 C4
+  -6.22,                                 !- Coefficient5 C5
+  0,                                         !- Minimum Value of x
+  1.0;                                     !- Maximum Value of x
+\end{lstlisting}
+
+\subsection{ElectricLoadCenter: Storage:Battery Outputs}\label{electricloadcenter-storagebattery-outputs}
+
+\begin{itemize}
+\item
+  HVAC,Average, Electric Storage Operating Mode Index {[]}
+\item
+  HVAC,Average,Electric Storage Charge State{[}Ah{]}
+\item
+  HVAC,Average, Electric Storage Charge Fraction {[]}
+\item
+  HVAC,Average,Electric Storage Charge Power{[}W{]}
+\item
+  HVAC,Sum,Electric Storage Charge Energy {[}J{]}
+\item
+  HVAC,Average,Electric Storage Discharge Power{[}W{]}
+\item
+  HVAC,Sum,Electric Storage Discharge Energy {[}J{]}
+\item
+  HVAC,Average,Electric Storage Total Current{[}A{]}
+\item
+  HVAC,Average, Electric Storage Total Voltage {[}V{]}
+\item
+  HVAC,Average,Electric Storage Thermal Loss Rate {[}W{]}
+\item
+  HVAC,Average, Electric Storage Degradation Fraction {[]}
+\item
+  HVAC,Sum,Electric Storage Production Decrement Energy {[}J{]}
+\item
+  HVAC,Sum,Electric Storage Thermal Loss Energy {[}J{]}
+\end{itemize}
+
+\subsubsection{\texorpdfstring{Electric Storage Operating Mode Index {[]}}{Electric Storage Operating Mode Index }}\label{electric-storage-operating-mode-index}
+
+This output reports the battery mode of operation: 0 for idle; 1 for discharging; 2 for charging. It is expected that more operation modes would be added when a smart and active power dispatch controller is used in future.
+
+\subsubsection{Electric Storage Charge State {[}Ah{]}}\label{electric-storage-charge-state-ah}
+
+The state of charge is expressed as the amount of charge stored in the battery at a point of time. It has the same unit as the maximum capacity. This value is given for an individual battery module
+
+\subsubsection{\texorpdfstring{Electric Storage Charge Fraction {[]}}{Electric Storage Charge Fraction }}\label{electric-storage-charge-fraction}
+
+This output is the ratio between the electrical storage state of charge and the maximum capacity.
+
+\subsubsection{Electric Storage Charge Power {[}W{]}}\label{electric-storage-charge-power-w-1}
+
+\subsubsection{Electric Storage Charge Energy {[}J{]}}\label{electric-storage-charge-energy-j-1}
+
+These outputs are total electricity power or energy fed into the battery. This is the rate of amount of charging.
+
+\subsubsection{Electric Storage Production Decrement Energy {[}J{]}}\label{electric-storage-production-decrement-energy-j-1}
+
+This output is the total electricity energy decremented from electricity production because it has fed into the battery. This output has the opposite sign of Electric Storage Charge Energy but is otherwise similar. This decrement output variable is also a meter associated with the resource type ElectricityProduced that reduces the metered electricity production to account for power that went into storage after production.
+
+\subsubsection{Electric Storage Discharge Power {[}W{]}}\label{electric-storage-discharge-power-w-1}
+
+\subsubsection{Electric Storage Discharge Energy {[}J{]}}\label{electric-storage-discharge-energy-j-1}
+
+These outputs are total electricity power or energy drawn from the battery. This is the rate or amount of discharging. The energy from storage output variable is also a meter associated with the resource type ElectricityProduced that increases the metered electricity production to account for power that has come back out of storage.
+
+\subsubsection{Electric Storage Total Current {[}A{]}}\label{electric-storage-total-current-a}
+
+This output is the current to or from the battery bank depending on whether the battery is in the state of charging or discharging. The value is positive for discharging and negative for charging.
+
+\subsubsection{Electric Storage Total Voltage {[}V{]}}\label{electric-storage-total-voltage-v}
+
+This output is the total terminal voltage of the battery bank.
+
+\subsubsection{Electric Storage Thermal Loss Rate {[}W{]}}\label{electric-storage-thermal-loss-rate-w-1}
+
+\subsubsection{Electric Storage Thermal Loss Energy {[}J{]}}\label{electric-storage-thermal-loss-energy-j-1}
+
+These outputs are the thermal power or energy losses from both charging and drawing electrical power in or out of the storage device. These losses are due to the battery internal resistance in charging and discharging.
+
+\subsubsection{\texorpdfstring{Electric Storage Degradation Fraction {[]}}{Electric Storage Degradation Fraction }}\label{electric-storage-degradation-fraction}
+
+This output reports the fractional battery life used up at a point of time. For example, a value of 0.4 at the end of one year simulation means that the 40\% of the battery life is used up, so the battery needs to be replaced every two and a half years.
+
+\subsection{Generator:InternalCombustionEngine}\label{generatorinternalcombustionengine}
+
+The Internal Combustion (IC) Engine generator uses a modified Otto cycle. This generator model uses the electrical load and rated engine generator size to compute part-load ratios (PLR). Fuel energy input and recoverable jacket and lube oil heat are then computed. Finally, the recoverable exhaust heat is calculated.
+
+Manufacturer's curves or tables must be obtained for IC engine generators to derive the equipment performance parameters that are specified in the quadratic curve fits. Note that simple transformation of the form of the manufacturer's curves may be required. Electric energy output/fuel energy input is related to the part-load ratio (i.e., electric/load generator capacity) with a polynomial. Recoverable jacket heat/fuel energy equipment, recoverable lube oil heat/fuel energy input equipment performance, total exhaust heat/fuel energy input equipment, exhaust gas temperature/fuel energy input equipment performance parameters are all specified with a quadratic curve fit.
+
+When the heat recovery curve fits = 0.0, this means that no heat recovery is done on the IC engine generator exhaust gas; and no heat recovery is specified.
+
+\subsubsection{Inputs}\label{inputs-7-007}
+
+\paragraph{Field: Name}\label{field-name-8-004}
+
+This alpha field contains the identifying name for the IC engine generator.
+
+\paragraph{Field: Rated Power Output}\label{field-rated-power-output}
+
+The design nominal capacity of the generator in Watts {[}W{]}.
+
+\paragraph{Field: Electric Circuit Node Name}\label{field-electric-circuit-node-name}
+
+This named node contains where the electric power is put in the program simulation for use by the electric equipment in the Load Center.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio}
+
+This field contains the minimum allowed operating fraction of full load. The input value must be \textgreater{} = 0.0 and \textless{} = 1.0.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio}
+
+This field contains the maximum allowed operating fraction of full load. The input value must be \textgreater{}0.0 and \textless{} = 1.0.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio}
+
+This alpha field contains the optimal operating fraction of full load. This is the part load ratio that gives the optimal production of electric power with the least amount of fuel usage.
+
+\paragraph{Field: Shaft Power Curve Name}\label{field-shaft-power-curve-name}
+
+This alpha field contains the name of the shaft power curve. The curve itself is specified separately using a curve object (ref: Curve:QuadLinear). The Shaft Power Curve is a quadratic equation that determines the electric output versus the fuel used. Used to calculate the electric energy output divided by the fuel energy consumption as a function of part-load ratio. The defining equation is:
+
+\begin{equation}
+ShaftPowerToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}
+\end{equation}
+
+where RL is the Ratio of Load to Rated Power Output.
+
+\paragraph{Field: Jacket Heat Recovery Curve Name}\label{field-jacket-heat-recovery-curve-name}
+
+This alpha field contains the name of the Recovery Jacket Heat curve. The curve itself is specified separately using a curve object (ref: Curve:QuadLinear). The Jacket Heat Recovery Curve is a quadratic equation that determines the ratio of recovery jacket heat to fuel energy. Used to calculate the recoverable jacket heat as a function of part-load ratio.
+
+The defining equation is:
+
+\begin{equation}
+RecoveryJacketHeatToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}
+\end{equation}
+
+where RL is the Ratio of Load to Rated Power Output.
+
+\paragraph{Field: Lube Heat Recovery Curve Name}\label{field-lube-heat-recovery-curve-name}
+
+This alpha field contains the name of the Recovery Lube Heat curve. The curve itself is specified separately using a curve object (ref Curve:QuadLinear). The Lube Heat Recovery Curve is a quadratic equation that determines the ratio of recovery lube heat to fuel energy. Used to calculate the recoverable lube oil heat as a function of part-load ratio. The defining equation is:
+
+\begin{equation}
+RecoveryLubeHeatToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}
+\end{equation}
+
+where RL is the Ratio of Load to Rated Power Output.
+
+\paragraph{Field: Total Exhaust Energy Curve Name}\label{field-total-exhaust-energy-curve-name}
+
+This alpha field contains the name of the Total Exhaust Energy curve. The curve itself is specified separately using a curve object (ref Curve:QuadLinear object). The Total Exhaust Energy Curve is a quadratic equation that determines the ratio of total exhaust energy to fuel energy. Used to calculate the total exhaust heat as a function of part-load ratio. The defining equation is:
+
+\begin{equation}
+TotalExhaustToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}
+\end{equation}
+
+where RL is the Ratio of Load to Rated Power Output.
+
+\paragraph{Field: Exhaust Temperature Curve Name}\label{field-exhaust-temperature-curve-name}
+
+This alpha field contains the name of the Exhaust Temperature curve. The curve itself is specified separately using a curve object (ref Curve:QuadLinear object). The Exhaust Temperature Curve is a quadratic equation that determines the absolute exhaust temperature. Used to determine the exhaust gas temperature as a function of part-load ratio. The defining equation is:
+
+\begin{equation}
+AbsoluteExhaustTemperature = {C_1} + {C_2}RL + {C_3}R{L^2}
+\end{equation}
+
+where RL is the Ratio of Load to Rated Power Output.
+
+\paragraph{U-Factor Times Area (UA) Curve}\label{u-factor-times-area-ua-curve}
+
+The UA curve applies to the exhaust gas heat exchanger. The curve is an equation that determines the overall heat transfer coefficient for the exhaust gases with the stack. The heat transfer coefficient ultimately helps determine the exhaust stack temperature. The defining equation is:
+
+\begin{equation}
+UAToCapacityRatio = {C_1}GeneratorRatedPowerOutpu{t^{{C_2}}}
+\end{equation}
+
+The following two fields contain the coefficients for the equation.
+
+\paragraph{Field: Coefficient 1 of U-Factor Times Area Curve}\label{field-coefficient-1-of-u-factor-times-area-curve}
+
+This numeric field contains the first coefficient for the overall heat transfer coefficient curve.
+
+\paragraph{Field: Coefficient 2 of U-Factor Times Area Curve}\label{field-coefficient-2-of-u-factor-times-area-curve}
+
+This numeric field contains the second (exponential) coefficient for the overall heat transfer coefficient curve.
+
+\paragraph{Field: Maximum Exhaust Flow per Unit of Power Output}\label{field-maximum-exhaust-flow-per-unit-of-power-output}
+
+Maximum exhaust flow per unit capacity for the generator. The parameter sets an upper limit on exhaust gas flow and exhaust gas heat recovery for the generator. Units: kg/sec per kW capacity
+
+\paragraph{Field: Design Minimum Exhaust Temperature}\label{field-design-minimum-exhaust-temperature}
+
+This is the design engine stack saturated steam temperature in degrees C.
+
+\paragraph{Field: Fuel Higher Heating Value}\label{field-fuel-higher-heating-value}
+
+This numeric field contains the higher heating value of the fuel used in kJ/kg.
+
+\paragraph{Field: Design Heat Recovery Water Flow Rate}\label{field-design-heat-recovery-water-flow-rate}
+
+Design water volumetric flow rate through heat recovery loop in m\(^{3}\)/sec.
+
+\paragraph{Field: Heat Recovery Inlet Node Name}\label{field-heat-recovery-inlet-node-name}
+
+This alpha field contains the identifying name for the generator s heat recovery side inlet node.
+
+\paragraph{Field: Heat Recovery Outlet Node Name}\label{field-heat-recovery-outlet-node-name}
+
+This alpha field contains the identifying name for the generator s heat recovery side outlet node.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type}
+
+This alpha field determines the type of fuel that the generator uses. The default is Diesel. Valid values are: \textbf{NaturalGas}, \textbf{PropaneGas}, \textbf{Diesel}, \textbf{Gasoline}, \textbf{FuelOil\#1}, \textbf{FuelOil\#2, OtherFuel1,} and \textbf{OtherFuel2}.
+
+\paragraph{Field: Heat Recovery Maximum Temperature}\label{field-heat-recovery-maximum-temperature}
+
+This field sets the maximum temperature that this piece of equipment can produce for heat recovery. The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit. This temperature limit puts an upper bound on the recovered heat and limits the max temperatures leaving the component.
+
+As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting. This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply.
+
+The temperature is specified in degrees C.
+
+An IDF example showing how it is used is provided below:
+
+\begin{lstlisting}
+
+Generator:InternalCombustionEngine,
+  Cat Diesel,                           !- Name
+  50000,                                     !- Rated Power Output {W}
+  Generator Diesel Electric Node,   !- Electric Circuit Node Name
+  0.15,                                       !- Minimum Part Load Ratio
+  1.0,                                         !- Maximum Part Load Ratio
+  0.65,                                       !- Optimum Part Load Ratio
+  BG Shaft Power Curve,       !- Shaft Power Curve Name
+  BG Recovery Jacket Heat Curve,   !- Jacket Heat Recovery Curve Name
+  BG Recovery Lube Heat Curve,   !- Lube Heat Recovery Curve Name
+  BG Total Exhaust Energy Curve,   !- Total Exhaust Energy Curve Name
+  BG Exhaust Temperature Curve,   !- Exhaust Temperature Curve Name
+  0.00952329,                           !- Coefficient 1 of U-Factor Times Area Curve
+  0.9,                                         !- Coefficient 2 of U-Factor Times Area Curve
+  0.00000063,                           !- Maximum Exhaust Flow per Unit of Power Output {(kg/s)/W}
+  150,                                         !- Design Minimum Exhaust Temperature {C}
+  45500,                                     !- Fuel Higher Heating Value {kJ/kg}
+  0.0,                                         !- Design Heat Recovery Water Flow Rate {m3/s}
+  ,                                               !- Heat Recovery Inlet Node Name
+  ,                                               !- Heat Recovery Outlet Node Name
+  Diesel;                                   !- Fuel Type
+
+  Curve:Quadratic,
+  BG Shaft Power Curve,       !- Name
+  0.09755,                                 !- Coefficient1 Constant
+  0.6318,                                   !- Coefficient2 x
+  -0.4165,                                 !- Coefficient3 x**2
+  0,                                             !- Minimum Value of x
+  1;                                             !- Maximum Value of x
+
+  Curve:Quadratic,
+  BG Recovery Jacket Heat Curve,   !- Name
+  0.25,                                       !- Coefficient1 Constant
+  0,                                             !- Coefficient2 x
+  0,                                             !- Coefficient3 x**2
+  0,                                             !- Minimum Value of x
+  1;                                             !- Maximum Value of x
+
+  Curve:Quadratic,
+  BG Recovery Lube Heat Curve,   !- Name
+  0.15,                                       !- Coefficient1 Constant
+  0,                                             !- Coefficient2 x
+  0,                                             !- Coefficient3 x**2
+  0,                                             !- Minimum Value of x
+  1;                                             !- Maximum Value of x
+
+  Curve:Quadratic,
+  BG Total Exhaust Energy Curve,   !- Name
+  0.1,                                         !- Coefficient1 Constant
+  0,                                             !- Coefficient2 x
+  0,                                             !- Coefficient3 x**2
+  0,                                             !- Minimum Value of x
+  1;                                             !- Maximum Value of x
+
+  Curve:Quadratic,
+  BG Exhaust Temperature Curve,   !- Name
+  425,                                         !- Coefficient1 Constant
+  0,                                             !- Coefficient2 x
+  0,                                             !- Coefficient3 x**2
+  0,                                             !- Minimum Value of x
+  1;                                             !- Maximum Value of x
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-002}
+
+The output variables that are available for the IC engine generator are:
+
+\begin{itemize}
+\item
+  HVAC,Average,Generator Produced Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Produced Electric Energy {[}J{]}
+\item
+  HVAC,Average,Generator Lube Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Lube Heat Recovery Energy {[}J{]}
+\item
+  HVAC,Average,Generator Jacket Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Jacket Heat Recovery Energy {[}J{]}
+\item
+  HVAC,Average,Generator Exhaust Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Exhaust Heat Recovery Energy {[}J{]}
+\item
+  HVAC,Average,Generator Total Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Total Heat Recovery {[}J{]}
+\item
+  HVAC,Average,Generator Exhaust Air Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Heat Recovery Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Heat Recovery Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Heat Recovery Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Generator Fuel HHV Basis Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Fuel HHV Basis Energy {[}J{]}
+\item
+  HVAC,Average,Generator \textless{}Fuel Type\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,Generator\textless{}Fuel Type\textgreater{} Energy {[}J{]}
+\item
+  HVAC,Average,Generator \textless{}Fuel Type\textgreater{} Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Generator Produced Electric Power {[}W{]}}\label{generator-produced-electric-power-w}
+
+\paragraph{Generator Produced Electric Energy {[}J{]}}\label{generator-produced-electric-energy-j}
+
+These outputs are the electric power output from the electric generator. Energy is metered on Cogeneration:ElectricityProduced, ElectricityProduced:Plant, and ElectricityProduced:Facility.
+
+\paragraph{Generator Lube Heat Recovery Rate {[}W{]}}\label{generator-lube-heat-recovery-rate-w}
+
+\paragraph{Generator Lube Heat Recovery Energy {[}J{]}}\label{generator-lube-heat-recovery-energy-j}
+
+\paragraph{Generator Jacket Heat Recovery Rate {[}W{]}}\label{generator-jacket-heat-recovery-rate-w}
+
+\paragraph{Generator Jacket Heat Recovery Energy {[}J{]}}\label{generator-jacket-heat-recovery-energy-j}
+
+\paragraph{Generator Exhaust Heat Recovery Rate {[}W{]}}\label{generator-exhaust-heat-recovery-rate-w}
+
+\paragraph{Generator Exhaust Heat Recovery Energy {[}J{]}}\label{generator-exhaust-heat-recovery-energy-j}
+
+\paragraph{Generator Produced Thermal Rate {[}W{]}}\label{generator-produced-thermal-rate-w}
+
+\paragraph{Generator Produced Thermal Energy {[}J{]}}\label{generator-produced-thermal-energy-j}
+
+For electric generators with heat recovery these outputs are the components of recoverable energy available. For the IC engine generator, the following heat recovery components are reported: Lube (engine lubricant), Jacket (engine coolant), and Exhaust (engine exhaust). These components are totaled together for Generator Produced Thermal Rate and Generator Produced Thermal Energy reports. Generator Lube Heat Recovery Energy, Generator Jacket Heat Recovery Energy, and Generator Exhaust Heat Recovery Energy are metered on HeatRecovery:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\paragraph{Generator Exhaust Air Temperature {[}C{]}}\label{generator-exhaust-air-temperature-c}
+
+This is the exhaust temperature leaving the engine.
+
+\paragraph{Generator Heat Recovery Inlet Temperature {[}C{]}}\label{generator-heat-recovery-inlet-temperature-c}
+
+\paragraph{Generator Heat Recovery Outlet Temperature {[}C{]}}\label{generator-heat-recovery-outlet-temperature-c}
+
+\paragraph{Generator Heat Recovery Mass Flow Rate {[}kg/s{]}}\label{generator-heat-recovery-mass-flow-rate-kgs}
+
+These outputs are the heat recovery inlet and outlet temperatures and flow rate for generators with heat recovery.
+
+\paragraph{Generator Fuel HHV Basis Rate {[}W{]}}\label{generator-fuel-hhv-basis-rate-w}
+
+\paragraph{Generator Fuel HHV Basis Energy {[}J{]}}\label{generator-fuel-hhv-basis-energy-j}
+
+These outputs are the generator s fuel energy and use rate. The energy content of the fuel is based on the higher heating value (HHV).
+
+\paragraph{Generator \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{generator-fuel-type-rate-w}
+
+\paragraph{Generator \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{generator-fuel-type-energy-j}
+
+\paragraph{Generator \textless{}Fuel Type\textgreater{} Mass Flow Rate {[}kg/s{]}}\label{generator-fuel-type-mass-flow-rate-kgs}
+
+If the fuel type is Diesel, then Diesel is shown as the fuel type. They are the diesel fuel input to the electric generator. Consumption is metered on Cogeneration:Diesel, Diesel:Plant, and Diesel:Facility.
+
+If the fuel type is Natural Gas, then Gas is shown as the fuel type. They are the natural gas fuel input to the electric generator. Consumption is metered on Cogeneration:Gas, Gas:Plant, and Gas:Facility.
+
+If the fuel type is Propane, then Propane is shown as the fuel type. They are the propane fuel input to the electric generator. Consumption is metered on Cogeneration:Propane, Propane:Plant, and Propane:Facility.
+
+If the fuel type is Gasoline, then Gasoline is shown as the fuel type. They are the gasoline fuel input to the electric generator. Consumption is metered on Cogeneration:Gasoline, Gasoline:Plant, and Gasoline:Facility.
+
+If the fuel type is FuelOil\#1, then FuelOil\#1 is shown as the fuel type. They are the fuel oil input to the electric generator. Consumption is metered on Cogeneration:FuelOil\#1, FuelOil\#1:Plant, and FuelOil\#1:Facility.
+
+If the fuel type is FuelOil\#2, then FuelOil\#2 is shown as the fuel type. They are the fuel oil input to the electric generator. Consumption is metered on Cogeneration:FuelOil\#2, FuelOil\#2:Plant, and FuelOil\#2:Facility.
+
+If the fuel type is OtherFuel1, then OtherFuel1 is shown as the fuel type. They are the fuel oil input to the electric generator. Consumption is metered on Cogeneration:OtherFuel1, OtherFuel1:Plant, and OtherFuel1:Facility.
+
+If the fuel type is OtherFuel2, then OtherFuel2 is shown as the fuel type. They are the fuel oil input to the electric generator. Consumption is metered on Cogeneration:OtherFuel2, OtherFuel2:Plant, and OtherFuel2:Facility.
+
+\subsection{Generator:CombustionTurbine}\label{generatorcombustionturbine}
+
+EnergyPlus has two different models for combustion turbine style generators. This one stems for a model that was originally in the BLAST computer program. A newer model with a different formulation is also available -see the Generator:MicroTurbine input object. The basic combustion-turbine cycle is the Brayton Cycle or open cycle, which consists of an adiabatic compression, constant pressure heating, and adiabatic expansion. The Combustion turbine model uses the electrical load and engine generator size to compute part-load ratios (PLR). Fuel energy input and recoverable lube oil heat are then computed. Finally, the recoverable exhaust heat is calculated.
+
+Combustion turbine generators use performance parameters to compute fuel energy consumption as a function of part-load and ambient (entering) air temperature. Recoverable fuel energy equipment, recoverable lube oil heat/fuel energy input equipment performance, total exhaust heat/fuel energy input equipment, exhaust gas temperature/fuel energy input equipment performance parameters are all specified with a quadratic curve fit.
+
+When the heat recovery curve fits = 0.0, this means that no heat recovery is done on the diesel generator exhaust gas; and no heat recovery is specified.
+
+\subsubsection{Inputs}\label{inputs-8-005}
+
+\paragraph{Field: Name}\label{field-name-9-004}
+
+Unique name to identify this combustion turbine generator.
+
+\paragraph{Field: Rated Power Output}\label{field-rated-power-output-1}
+
+The design nominal capacity of the combustion turbine generator in Watts {[}W{]}.
+
+\paragraph{Field: Electric Circuit Node Name}\label{field-electric-circuit-node-name-1}
+
+This Named node contains where the electric power is put in the program simulation for use by the electric equipment in the Load Center.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-1}
+
+This field contains the minimum allowed operating fraction of full load. The input value must be \textgreater{} = 0.0 and \textless{} = 1.0.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-1}
+
+This field contains the maximum allowed operating fraction of full load. The input value must be \textgreater{}0.0 and \textless{} = 1.0.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-1}
+
+This alpha field contains the optimal operating fraction of full load. This is the part load ratio that gives the optimal production of electric power with the least amount of fuel usage.
+
+\paragraph{Field: Part Load Based Fuel Input Curve Name}\label{field-part-load-based-fuel-input-curve-name}
+
+Needs a Curve:Quadratic object to be specified.
+
+Fuel Input = a + b*PLR + c*PLR**2
+
+PLR = Ratio of Generator Load to Rated Power Output. This curve is multiplied to the Temperature Based Fuel Input Curve to determine Fuel Energy In.
+
+\paragraph{Field: Temperature Based Fuel Input Curve Name}\label{field-temperature-based-fuel-input-curve-name}
+
+Needs a Curve:Quadratic object to be specified.
+
+Fuel Input = a + b*AT + c*AT**2 where: AT = Ambient Delta T
+
+\paragraph{Field: Exhaust Flow Curve Name}\label{field-exhaust-flow-curve-name}
+
+The Total Exhaust Energy Curve is a quadratic equation that needs to be specified by a curve object. Used to calculate the total exhaust heat as a function of part-load ratio.
+
+\paragraph{Field: Part Load Based Exhaust Temperature Curve Name}\label{field-part-load-based-exhaust-temperature-curve-name}
+
+The Exhaust Temperature Curve is a quadratic equation that needs to be specified by a curve object. Used to determine the exhaust gas temperature as a function of part-load ratio.
+
+\paragraph{Field: Temperature Based Exhaust Temperature Curve Name}\label{field-temperature-based-exhaust-temperature-curve-name}
+
+The Exhaust Temperature Curve is a quadratic equation that needs to be specified by a curve object. Used to determine the exhaust gas temperature as a function of part-load ratio.
+
+\paragraph{Field: Heat Recovery Lube Energy Curve Name}\label{field-heat-recovery-lube-energy-curve-name}
+
+This alpha field contains the name of the Recovery Lube Heat curve. The curve itself is specified separately using a curve object (see Curve:Quadlinear object). The Recovery Lubricant Heat Curve is a quadratic equation that determines the ratio of recovery lube heat to fuel energy. Used to calculate the recoverable lube oil heat as a function of part-load ratio. The defining equation is:
+
+\begin{equation}
+RecoveryLubeHeatToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}
+\end{equation}
+
+where RL is the Ratio of Load to Rated Power Output.
+
+\paragraph{U-Factor Times Area (UA) Curve}\label{u-factor-times-area-ua-curve-1}
+
+The UA curve applies to the exhaust gas heat exchanger. The curve is an equation that determines the overall heat transfer coefficient for the exhaust gases with the stack. The heat transfer coefficient ultimately helps determine the exhaust stack temperature. The defining equation is:
+
+\begin{equation}
+UAToCapacityRatio = {C_1}GeneratorRatedPowerOutpu{t^{{C_2}}}
+\end{equation}
+
+The following two fields contain the coefficients for the equation.
+
+\paragraph{Field: Coefficient 1 of U-Factor Times Area Curve}\label{field-coefficient-1-of-u-factor-times-area-curve-1}
+
+This numeric field contains the first coefficient for the overall heat transfer coefficient curve.
+
+\paragraph{Field: Coefficient 2 of U-Factor Times Area Curve}\label{field-coefficient-2-of-u-factor-times-area-curve-1}
+
+This numeric field contains the second (exponential) coefficient for the overall heat transfer coefficient curve.
+
+\paragraph{Field: Maximum Exhaust Flow per Unit of Power Output}\label{field-maximum-exhaust-flow-per-unit-of-power-output-1}
+
+Maximum exhaust flow per unit capacity for diesel engines. The parameter sets an upper limit on exhaust gas flow and exhaust gas heat recovery for diesel engines. Units: kg/sec per kW capacity
+
+\paragraph{Field: Design Minimum Exhaust Temperature}\label{field-design-minimum-exhaust-temperature-1}
+
+This is the design engine stack saturated steam temperature in degrees C.
+
+\paragraph{Field: Design Air Inlet Temperature}\label{field-design-air-inlet-temperature}
+
+Design air inlet temperature in degrees C.
+
+\paragraph{Field: Fuel Higher Heating Value}\label{field-fuel-higher-heating-value-1}
+
+This numeric field contains the higher heating value of the fuel used in kJ/kg.
+
+\paragraph{Field: Design Heat Recovery Water Flow Rate}\label{field-design-heat-recovery-water-flow-rate-1}
+
+Design water volumetric flow rate through heat recovery loop in m\(^{3}\)/sec.
+
+\paragraph{Field: Heat Recovery Inlet Node Name}\label{field-heat-recovery-inlet-node-name-1}
+
+This alpha field contains the identifying name for the combustion turbine generator heat recovery side inlet node.
+
+\paragraph{Field: Heat Recovery Outlet Node Name}\label{field-heat-recovery-outlet-node-name-1}
+
+This alpha field contains the identifying name for the combustion turbine generator heat recovery side outlet node.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-1}
+
+This alpha field determines the type of fuel that the generator uses. Valid choices are: \textbf{NaturalGas, PropaneGas, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1} and \textbf{OtherFuel2}. The default is \textbf{NaturalGas}.
+
+\paragraph{Field: Heat Recovery Maximum Temperature}\label{field-heat-recovery-maximum-temperature-1}
+
+This field sets the maximum temperature that this piece of equipment can produce for heat recovery. The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit. This temperature limit puts an upper bound on the recovered heat and limits the max temperatures leaving the component.
+
+As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting. This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply.
+
+The temperature is specified in degrees C.
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-001}
+
+This field is optional. It is used to explicitly define an outdoor air node for the inlet for combustion air stream. Defining an outdoor air node here allows using the height-dependent model for outdoor air conditions.
+
+An IDF example showing how it is used is provided below:
+
+\begin{lstlisting}
+
+Generator:CombustionTurbine,
+  Solar Turbine,                     !- Name
+  30000,                                     !- Rated Power Output {W}
+  GT gen Electric Node,       !- Electric Circuit Node Name
+  0.15,                                       !- Minimum Part Load Ratio
+  1.0,                                         !- Maximum Part Load Ratio
+  0.65,                                       !- Optimum Part Load Ratio
+  BG PL Based Fuel Input Curve,   !- Part Load Based Fuel Input Curve Name
+  BG Temp Based Fuel Input Curve,   !- Temperature Based Fuel Input Curve Name
+  BG Exhaust Flow Curve,     !- Exhaust Flow Curve Name
+  BG PL Based Exhaust Temp Curve,   !- Part Load Based Exhaust Temperature Curve Name
+  BG Temp Based Exhaust Temp Curve,   !- Temperature Based Exhaust Temperature Curve Name
+  BG Tur Recovery Lube Heat Curve,   !- Heat Recovery Lube Energy Curve Name
+  0.01907045,                           !- Coefficient 1 of U-Factor Times Area Curve
+  0.9,                                         !- Coefficient 2 of U-Factor Times Area Curve
+  0.00000504,                           !- Maximum Exhaust Flow per Unit of Power Output {(Kg/s)/W}
+  150,                                         !- Design Minimum Exhaust Temperature {C}
+  25,                                           !- Design Air Inlet Temperature {C}
+  43500,                                     !- Fuel Higher Heating Value {kJ/kg}
+  0.0,                                         !- Design Heat Recovery Water Flow Rate {m3/s}
+  ,                                               !- Heat Recovery Inlet Node Name
+  ,                                               !- Heat Recovery Outlet Node Name
+  NaturalGas,                           !- Fuel Type
+  ,                                               !- Heat Recovery Maximum Temperature {C}
+  CT OA inlet;                         !- Outdoor Air Inlet Node Name
+
+  Curve:Quadratic,
+  BG PL Based Fuel Input Curve,   !- Name
+  9.41,                                       !- Coefficient1 Constant
+  -9.48,                                     !- Coefficient2 x
+  4.32,                                       !- Coefficient3 x**2
+  0,                                             !- Minimum Value of x
+  1;                                             !- Maximum Value of x
+
+  Curve:Quadratic,
+  BG Temp Based Fuel Input Curve,   !- Name
+  1.0044,                                   !- Coefficient1 Constant
+  -0.0008,                                 !- Coefficient2 x
+  0,                                             !- Coefficient3 x**2
+  -30,                                         !- Minimum Value of x
+  +30;                                         !- Maximum Value of x
+
+  Curve:Quadratic,
+  BG Exhaust Flow Curve,     !- Name
+  0.05,                                       !- Coefficient1 Constant
+  0.0,                                         !- Coefficient2 x
+  0.0,                                         !- Coefficient3 x**2
+  0,                                             !- Minimum Value of x
+  1;                                             !- Maximum Value of x
+
+  Curve:Quadratic,
+  BG PL Based Exhaust Temp Curve,   !- Name
+  450,                                         !- Coefficient1 Constant
+  0,                                             !- Coefficient2 x
+  0,                                             !- Coefficient3 x**2
+  0,                                             !- Minimum Value of x
+  1;                                             !- Maximum Value of x
+
+  Curve:Quadratic,
+  BG Temp Based Exhaust Temp Curve,   !- Name
+  1.005,                                     !- Coefficient1 Constant
+  0.0018,                                   !- Coefficient2 x
+  0,                                             !- Coefficient3 x**2
+  -30,                                         !- Minimum Value of x
+  +30;                                         !- Maximum Value of x
+
+  Curve:Quadratic,
+  BG Tur Recovery Lube Heat Curve,   !- Name
+  0.223,                                     !- Coefficient1 Constant
+  -0.4,                                       !- Coefficient2 x
+  0.2286,                                   !- Coefficient3 x**2
+  0,                                             !- Minimum Value of x
+  1;                                             !- Maximum Value of x
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-002}
+
+The output variables that are available for the combustion turbine generator are:
+
+\begin{itemize}
+\item
+  HVAC,Average,Generator Produced Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Produced Electric Energy {[}J{]}
+\item
+  Zone,Meter,ElectricityProduced:Facility {[}J{]}
+\item
+  Zone,Meter,ElectricityProduced:Plant {[}J{]}
+\item
+  Zone,Meter,Cogeneration:ElectricityProduced {[}J{]}
+\item
+  HVAC,Average,Generator Lube Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Lube Heat Recovery Energy {[}J{]}
+\item
+  HVAC,Average,Generator Exhaust Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Exhaust Heat Recovery {[}J{]}
+\item
+  HVAC,Average,Generator Total Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Total Heat Recovery {[}J{]}
+\item
+  HVAC,Average,Generator Exhaust Air Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Heat Recovery Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Heat Recovery Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Heat Recovery Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Generator \textless{}Fuel Type\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,Generator \textless{}Fuel Type\textgreater{} Energy {[}J{]}
+\item
+  HVAC,Average,Generator \textless{}Fuel Type\textgreater{} Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+All of these outputs, except for the Combustion use outputs, are described above under ``Generator:InternalCombustionEngine Outputs.''
+
+\paragraph{Generator \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{generator-fuel-type-rate-w-1}
+
+\paragraph{Generator \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{generator-fuel-type-energy-j-1}
+
+\paragraph{Generator \textless{}Fuel Type\textgreater{} Mass Flow Rate {[}kg/s{]}}\label{generator-fuel-type-mass-flow-rate-kgs-1}
+
+These outputs are the fuel input to the electric generator. Consumption is metered on Cogeneration:\textless{}Fuel Type\textgreater{}, \textless{}Fuel Type\textgreater{}:Plant, and \textless{}Fuel Type\textgreater{}:Facility.
+
+\subsection{Generator:MicroTurbine}\label{generatormicroturbine}
+
+MicroTurbine generators are small combustion turbines that produce electricity on a relatively small scale (e.g., 25kW to 500kW). This model uses nominal performance at reference conditions along with several modifier curves to determine electrical power output and fuel use at non-reference conditions. Standby and ancillary power can also be taken into account. Furthermore, energy recovery from exhaust air can be used to heat water. Similar to electrical power output, thermal power (heat recovery) output is calculated using nominal performance at reference conditions with modifier curves to account for variations at non-reference conditions.
+
+The following inputs define the MicroTurbine electric generator. The ElectricLoadCenter:Generators and ElectricLoadCenter:Distribution objects are used to define the availability and control of all electric generators included in the simulation (ref. ElectricLoadCenter:Generators and ElectricLoadCenter:Distribution).
+
+\subsubsection{Inputs}\label{inputs-9-004}
+
+\paragraph{Field: Name}\label{field-name-10-003}
+
+This alpha field specifies a unique user-defined name to identify this generator. This is a required input.
+
+\paragraph{Field: Reference Electrical Power Output}\label{field-reference-electrical-power-output}
+
+This numeric field specifies the full-load electrical power output of the microturbine generator in Watts at reference conditions. The reference conditions are defined via additional input fields for this object (see below). This is a required input, and the value entered in this field must be greater than zero.
+
+\paragraph{Field: Minimum Full Load Electrical Power Output}\label{field-minimum-full-load-electrical-power-output}
+
+This numeric field specifies the minimum electrical power output in Watts at full-load conditions. The electrical power output of the generator is determined by multiplying the Reference Electrical Power Output by the Electrical Power Function of Temperature and Elevation modifier curve. If the result is less than the numeric value specified in this input field, then the generator s electrical power output is reset to the minimum full-load value specified in this input field. The value entered in this field must be greater than or equal to zero. If this field is left blank, the default value of 0.0 will be used.
+
+\paragraph{Field: Maximum Full Load Electrical Power Output}\label{field-maximum-full-load-electrical-power-output}
+
+This numeric field specifies the maximum electrical power output in Watts at full-load conditions. The electrical power output of the generator is determined by multiplying the Reference Electrical Power Output by the Electrical Power Function of Temperature and Elevation Modifier curve. If the result is greater than the numeric value specified in this input field, then the generator s electrical power output is reset to the maximum full-load value specified in this input field. The value entered in this field must be greater than zero. If this field is left blank, then the value entered for the Reference Electrical Power Output field (above) will be used as the Maximum Full Load Electrical Power Output.
+
+\paragraph{Field: Reference Electrical Efficiency Using Lower Heating Value}\label{field-reference-electrical-efficiency-using-lower-heating-value}
+
+This numeric field contains the electrical efficiency of the generator at reference conditions, based on the lower heating value of the fuel. The electrical efficiency is the electric power output divided by the fuel energy consumption rate (LHV basis). The reference conditions are defined via additional input fields for this object (see below). This is a required input, and the value entered in this field must be greater than zero and less than or equal to 1.0.
+
+\paragraph{Field: Reference Combustion Air Inlet Temperature}\label{field-reference-combustion-air-inlet-temperature}
+
+This numeric field specifies the reference temperature for the combustion inlet air in degrees Celsius. If this field is left blank, the default value of 15 °C will be used.
+
+\paragraph{Field: Reference Combustion Air Inlet Humidity Ratio}\label{field-reference-combustion-air-inlet-humidity-ratio}
+
+This numeric field specifies the reference humidity ratio for the combustion inlet air in kgWater/kgDryAir. The value specified for this field must be greater than zero. If this field is left blank, the default value of 0.00638 (kgWater/kgDryAir) will be used.
+
+\paragraph{Field: Reference Elevation}\label{field-reference-elevation}
+
+This numeric field specifies the reference elevation in meters (relative to sea level). The value specified for this field must be greater than or equal to -300.0 meters. If this field is left blank, the default value of 0.0 meters will be used.
+
+\paragraph{Field: Electrical Power Function of Temperature and Elevation Curve Name}\label{field-electrical-power-function-of-temperature-and-elevation-curve-name}
+
+This alpha field specifies the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of electrical power output as a function of the combustion air inlet temperature and elevation. The output of this curve is multiplied by the Reference Electrical Power Output to give the full-load power output at a specific combustion air inlet temperature and elevation (i.e., at values different from the reference conditions). This curve should be normalized to have a value of 1.0 at the reference conditions, and the curve should be valid for the range of inlet air temperatures anticipated for the simulation period and for the actual elevation of the generator.
+
+\paragraph{Field: Electrical Efficiency Function of Temperature Curve Name}\label{field-electrical-efficiency-function-of-temperature-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of electrical efficiency as a function of the combustion air inlet temperature. The output of this curve is multiplied by the Reference Electrical Efficiency Using Lower Heating Value to give the full-load electrical efficiency at specific combustion air inlet temperatures (i.e., at inlet air temperatures different from the Reference Combustion Air Inlet Temperature). This curve should be normalized to have a value of 1.0 at the Reference Combustion Air Inlet Temperature, and the curve should be valid for the range of inlet air temperatures anticipated for the simulation period.
+
+\paragraph{Field: Electrical Efficiency Function of Part Load Ratio Curve Name}\label{field-electrical-efficiency-function-of-part-load-ratio-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of electrical efficiency as a function of the generator s part-load ratio (part-load ratio is the actual electrical power output divided by the full-load electrical power output at the current operating conditions). The output of this curve is multiplied by the Reference Electrical Efficiency Using Lower Heating Value and the output of the Electrical Efficiency Function of Temperature modifier curve to give the electrical efficiency at specific part-load and combustion air inlet (temperature) conditions. This curve should be normalized to have a value of 1.0 when the generator s part-load ratio is 1.0, and the curve should be valid for the range of part-load ratios anticipated for the simulation period.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-2}
+
+This choice field specifies the type of fuel used by the generator. Valid fueld types are PropaneGas and NaturalGas. If the field is left blank, the fuel type will be assumed to be NaturalGas.
+
+\paragraph{Field: Fuel Higher Heating Value}\label{field-fuel-higher-heating-value-2}
+
+This numeric field specifies the higher heating value of the fuel used in kJ/kg. The value specified for this field must be greater than zero and greater than the specified Fuel Lower Heating Value. If this field is left blank, the default value of 50,000 kJ/kg will be used.
+
+\paragraph{Field: Fuel Lower Heating Value}\label{field-fuel-lower-heating-value}
+
+This numeric field specifies the lower heating value of the fuel used in kJ/kg. The value specified for this field must be greater than zero but less than the specified Fuel Higher Heating Value. If this field is left blank, the default value of 45,450 kJ/kg will be used.
+
+\paragraph{Field: Standby Power}\label{field-standby-power}
+
+This numeric field specifies the standby electric power consumed by the generator in Watts. The standby power is the electrical power consumed by the generator (e.g., air fans and controls) when the generator is available to operate but the generator electrical power output is zero (power output is not being requested by the electric load center). The value specified for this field must be greater than or equal to zero. If this field is left blank, the default value of 0.0 W will be used.
+
+\paragraph{Field: Ancillary Power}\label{field-ancillary-power}
+
+This numeric field specifies the ancillary electric power consumed by the generator in Watts. The ancillary power is the electrical power consumed by other associated equipment (e.g., external fuel pressurization pumps) when the generator is operating. Specify this input as 0.0 if the Reference Electrical Power Output and Reference Electrical Efficiency Using Lower Heating Value input fields and associated modifier curves reflect the net electrical power output from the generator (i.e., ancillary power already deducted from the generator s gross electrical power output). A value greater than zero indicates that this electrical power is consumed whenever the generator is operating and will be deducted from the generator s overall electrical power output (Generator Produced Electric Power). The value specified for this field must be greater than or equal to zero. If this field is left blank, the default value of 0.0 W will be used.
+
+\paragraph{Field: Ancillary Power Function of Fuel Input Curve Name}\label{field-ancillary-power-function-of-fuel-input-curve-name}
+
+This alpha field specifies the name of a quadratic performance curve (ref: Performance Curves) that parameterizes the variation of ancillary power as a function of the generator s input fuel mass flow rate (kg/s). The output of this curve is multiplied by the ancillary power to give the ancillary power at a specific fuel mass flow rate. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation (i.e., the ancillary power is constant whenever the generator operates).
+
+\paragraph{Field: Heat Recovery Water Inlet Node Name}\label{field-heat-recovery-water-inlet-node-name}
+
+This alpha field specifies the identifying name for the generator s heat recovery water inlet node.
+
+\paragraph{Field: Heat Recovery Water Outlet Node Name}\label{field-heat-recovery-water-outlet-node-name}
+
+This alpha field specifies the identifying name for the generator s heat recovery water outlet node.
+
+\paragraph{Field: Reference Thermal Efficiency Using Lower Heat Value}\label{field-reference-thermal-efficiency-using-lower-heat-value}
+
+This numeric field specifies the thermal efficiency (heat recovery to water) at reference conditions, based on the lower heating value of the fuel. The thermal efficiency is the thermal power output (to water) divided by the fuel energy consumption rate (LHV basis). The reference conditions are defined via additional input fields for this object. This value must be from 0.0 to 1.0. If this field is left blank, the default value of 0.0 will be used.
+
+\paragraph{Field: Reference Inlet Water Temperature}\label{field-reference-inlet-water-temperature}
+
+This numeric field specifies the reference temperature for the inlet water to the heat recovery heat exchanger in degrees Celsius.
+
+\paragraph{Field: Heat Recovery Water Flow Operating Mode}\label{field-heat-recovery-water-flow-operating-mode}
+
+This field is used to choose between different modes of controlling the mass flow rate of water being heated by energy recovered from exhaust air. There are two options available for this field: PlantControl or InternalControl. The PlantControl option indicates that the heat recovery water flow rate through the generator is determined externally (by the wider balance of plant). In this case, the generator will request the Reference Heat Recovery Water Flow Rate whenever it operates but the actual flow rate may be limited by other plant components (e.g., pump). The InternalControl option indicates the flow of water is controlled inside the generator based on current operating conditions. For InternalControl, the generator should (probably) include a bypass branch when connecting to the plant loop.
+
+\paragraph{Field: Reference Heat Recovery Water Flow Rate}\label{field-reference-heat-recovery-water-flow-rate}
+
+This numeric field is the reference heat recovery (volumetric) water flow rate in cubic meters per second. Entered values must be greater than zero.
+
+\paragraph{Field: Heat Recovery Water Flow Rate Function of Temperature and Power Curve Name}\label{field-heat-recovery-water-flow-rate-function-of-temperature-and-power-curve-name}
+
+This alpha field specifies the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of heat recovery water flow rate as a function of the inlet water temperature and net electrical power output. This field is only used if the Heat Recovery Water Flow Operating Mode is InternalControl . The output of this curve is multiplied by the Reference Heat Recovery Water Flow Rate to give the water flow rate at the specific inlet water temperature and net power operating conditions. This curve should be normalized to have a value of 1.0 at the reference conditions, and the curve should be valid for the range of inlet water temperatures and net electrical power output anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
+
+\paragraph{Field: Thermal Efficiency Function of Temperature and Elevation Curve Name}\label{field-thermal-efficiency-function-of-temperature-and-elevation-curve-name}
+
+This alpha field specifies the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of thermal efficiency as a function of the combustion air inlet temperature and elevation. The output of this curve is multiplied by the Reference Thermal Efficiency Using Lower Heating Value to give the full-load thermal efficiency at a specific combustion air inlet temperature and elevation (i.e., at values different from the reference conditions). This curve should be normalized to have a value of 1.0 at the reference conditions, and the curve should be valid for the range of inlet air temperatures anticipated for the simulation period and for the actual elevation of the generator. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
+
+\paragraph{Field: Heat Recovery Rate Function of Part Load Ratio Curve Name}\label{field-heat-recovery-rate-function-of-part-load-ratio-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of heat recovery to water (thermal power output) as a function of the generator s part-load ratio (part-load ratio is the actual electrical power output divided by the full-load electrical power output at the current operating conditions). The output of this curve is multiplied by the steady-state heat recovery at the current combustion inlet air temperature and elevation to give the heat recovery rate (thermal power output) at specific part-load operating conditions. This curve should be normalized to have a value of 1.0 when the generator s part-load ratio is 1.0, and the curve should be valid for the range of part-load ratios anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
+
+\paragraph{Field: Heat Recovery Rate Function of Inlet Water Temperature Curve Name}\label{field-heat-recovery-rate-function-of-inlet-water-temperature-curve-name}
+
+This alpha field specifies the name of a quadratic performance curve (ref: Performance Curves) that parameterizes the variation of heat recovery to water (thermal power output) as a function of the inlet water temperature. The output of this curve is multiplied by the steady-state heat recovery at the current combustion inlet air temperature and elevation to give the heat recovery rate (thermal power output) at non-reference inlet water conditions. This curve should be normalized to have a value of 1.0 at the Reference Inlet Water Temperature, and the curve should be valid for the range of inlet water temperatures anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
+
+\paragraph{Field: Heat Recovery Rate Function of Water Flow Rate Curve Name}\label{field-heat-recovery-rate-function-of-water-flow-rate-curve-name}
+
+This alpha field specifies the name of a quadratic performance curve (ref: Performance Curves) that parameterizes the variation of heat recovery to water (thermal power output) as a function of the heat recovery water flow rate. The output of this curve is multiplied by the steady-state heat recovery at the current combustion inlet air temperature and elevation to give the heat recovery rate (thermal power output) at non-reference heat recovery water flow rates. This curve should be normalized to have a value of 1.0 at the Reference Heat Recovery Water Flow Rate, and the curve should be valid for the range of water flow rates anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
+
+\paragraph{Field: Minimum Heat Recovery Water Flow Rate}\label{field-minimum-heat-recovery-water-flow-rate}
+
+This numeric field specifies the minimum (volumetric) water flow rate through the heat recovery heat exchanger in cubic meters per second. The minimum input value is 0.0, and a value of 0.0 is assumed if this field is left blank.
+
+\paragraph{Field: Maximum Heat Recovery Water Flow Rate}\label{field-maximum-heat-recovery-water-flow-rate}
+
+This numeric field specifies the maximum (volumetric) water flow rate through the heat recovery heat exchanger in cubic meters per second. The minimum input value for this field is 0.0, and a value of 0.0 is assumed if this field is left blank. The maximum heat recovery water flow rate must be greater than or equal to the minimum heat recovery water flow rate.
+
+\paragraph{Field: Maximum Heat Recovery Water Temperature}\label{field-maximum-heat-recovery-water-temperature}
+
+This field sets the maximum water temperature, in degrees Celsius, that this generator can produce via heat recovery. This temperature limit puts an upper bound on the recovered heat and limits the max temperatures leaving the component.
+
+As temperatures in the water loop approach this maximum temperature, the temperature difference between the entering water and the surfaces in generator s heat recovery heat exchanger becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The amount of heat recovered will diminish if the inlet water temperature approaches the maximum temperature, and this will show up in the reporting.
+
+\paragraph{Field: Combustion Air Inlet Node Name}\label{field-combustion-air-inlet-node-name}
+
+This alpha field specifies the name of the combustion air inlet node. If a node name is specified, this node must be an outdoor air node and must also be specified elsewhere in the input (ref: OutdoorAir:Node and OutdoorAir:NodeList). If this field is left blank, the combustion air inlet conditions are assumed to be the outdoor weather conditions used for the simulation.
+
+\paragraph{Field: Combustion Air Outlet Node Name}\label{field-combustion-air-outlet-node-name}
+
+This alpha field specifies the name of the combustion air outlet node.
+
+\paragraph{Field: Reference Exhaust Air Mass Flow Rate}\label{field-reference-exhaust-air-mass-flow-rate}
+
+This numeric field is the reference exhaust air mass flow rate in kilograms per second. Entered values must be greater than zero.
+
+\paragraph{Field: Exhaust Air Flow Rate Function of Temperature Curve Name}\label{field-exhaust-air-flow-rate-function-of-temperature-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of exhaust air flow rate as a function of the combustion air inlet temperature. The output of this curve is multiplied by the Reference Exhaust Air Mass Flow Rate to give the exhaust air mass flow rate at non-reference combustion air inlet temperatures. This curve should be normalized to have a value of 1.0 at the Reference Combustion Air Inlet Temperature, and the curve should be valid for the range of inlet air temperatures anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
+
+\paragraph{Field: Exhaust Air Flow Rate Function of Part Load Ratio Curve Name}\label{field-exhaust-air-flow-rate-function-of-part-load-ratio-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of exhaust air flow rate as a function of the generator s part-load ratio (part-load ratio is the actual electrical power output divided by the full-load electrical power output at the current operating conditions). The output of this curve is multiplied by the Reference Exhaust Air Mass Flow Rate to give the exhaust air mass flow rate at specific part-load operating conditions. This curve should be normalized to have a value of 1.0 when the generator s part-load ratio is 1.0, and the curve should be valid for the range of part-load ratios anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
+
+\paragraph{Field: Nominal Exhaust Air Outlet Temperature}\label{field-nominal-exhaust-air-outlet-temperature}
+
+This numeric field is the exhaust air outlet temperature at nominal (reference) conditions in degrees Celsius.
+
+\paragraph{Field: Exhaust Air Temperature Function of Temperature Curve Name}\label{field-exhaust-air-temperature-function-of-temperature-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of exhaust air outlet temperature as a function of the combustion air inlet temperature. The output of this curve is multiplied by the Nominal Exhaust Air Outlet Temperature to give the exhaust air temperature at non-reference combustion air inlet temperatures. This curve should be normalized to have a value of 1.0 at the Reference Combustion Air Inlet Temperature, and the curve should be valid for the range of inlet air temperatures anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
+
+\paragraph{Field: Exhaust Air Temperature Function of Part Load Ratio Curve Name}\label{field-exhaust-air-temperature-function-of-part-load-ratio-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of exhaust air outlet temperature as a function of the generator s part-load ratio (part-load ratio is the actual electrical power output divided by the full-load electrical power output at the current operating conditions). The output of this curve is multiplied by the Nominal Exhaust Air Outlet Temperature to give the exhaust air temperature at specific part-load operating conditions. This curve should be normalized to have a value of 1.0 when the generator s part-load ratio is 1.0, and the curve should be valid for the range of part-load ratios anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+Generator:MicroTurbine,
+  Generator 3,                         !- Name
+  65000,                                     !- Reference Electrical Power Output {W}
+  29900,                                     !- Minimum Full Load Electrical Power Output {W}
+  65000,                                     !- Maximum Full Load Electrical Power Output {W}
+  0.29,                                       !- Reference Electrical Efficiency Using Lower Heating Value
+  15.0,                                       !- Reference Combustion Air Inlet Temperature {C}
+  0.00638,                                 !- Reference Combustion Air Inlet Humidity Ratio (kgWater/kgDryAir)
+  0.0,                                         !- Reference Elevation {m}
+  Power_vs_Temp_Elev,           !- Electrical Power Function of Temperature and Elevation Curve Name
+  Efficiency_vs_Temp,           !- Electrical Efficiency Function of Temperature Curve Name
+  Efficiency_vs_PLR,             !- Electrical Efficiency Function of Part Load Ratio Curve Name
+  NaturalGas,                           !- Fuel Type
+  50000,                                     !- Fuel Higher Heating Value {kJ/kg}
+  45450,                                     !- Fuel Lower Heating Value {kJ/kg}
+  300,                                         !- Standby Power {W}
+  4500;                                       !- Ancillary Power {W}
+
+  ! Electrical Power Modifier Curve (function of temperature and elevation)
+  ! x = Dry-Bulb Temperature of Combustion Inlet Air (C) and y = Elevation (meters)
+  Curve:Biquadratic,
+  Power_vs_Temp_Elev,           !- Name
+  1.2027697,                             !- Coefficient1 Constant
+  -9.671305E-03,                     !- Coefficient2 x
+  -4.860793E-06,                     !- Coefficient3 x**2
+  -1.542394E-04,                     !- Coefficient4 y
+  9.111418E-09,                       !- Coefficient5 y**2
+  8.797885E-07,                       !- Coefficient6 x*y
+  -17.8,                                     !- Minimum Value of x
+  50.0,                                       !- Maximum Value of x
+  0.0,                                         !- Minimum Value of y
+  3050.;                                     !- Maximum Value of y
+
+  ! Electrical Efficiency Modifier Curve (function of temperature)
+  ! x = Dry-Bulb Temperature of Combustion Inlet Air (C)
+  Curve:Cubic,
+  Efficiency_vs_Temp,           !- Name
+  1.0402217,                             !- Coefficient1 Constant
+  -0.0017314,                           !- Coefficient2 x
+  -6.497040E-05,                     !- Coefficient3 x**2
+  5.133175E-07,                       !- Coefficient4 x**3
+  -20.0,                                     !- Minimum Value of x
+  50.0;                                       !- Maximum Value of x
+
+  ! Electrical Efficiency Modifier Curve (function of part-load ratio)
+  ! x = Part-Load Ratio (electrical load/steady-state electrical power output)
+  Curve:Cubic,
+  Efficiency_vs_PLR,             !- Name
+  0.215290,                               !- Coefficient1 Constant
+  2.561463,                               !- Coefficient2 x
+  -3.24613,                               !- Coefficient3 x**2
+  1.497306,                               !- Coefficient4 x**3
+  0.03,                                       !- Minimum Value of x
+  1.0;                                         !- Maximum Value of x!
+
+  ElectricLoadCenter:Distribution,
+  Electric Load Center,       !- Name
+  Backup Generators,             !- Generator List Name
+  DemandLimit,                         !- Generator Operation Scheme Type
+  10000.0,                                 !- Demand Limit Scheme Purchased Electric Demand Limit {W}
+  ,                                               !- Track Schedule Name Scheme Schedule Name
+  ,                                               !- Track Meter Scheme Meter Name
+  AlternatingCurrent,           !- Electrical Buss Type
+  ,                                               !- Inverter Object Name
+  ;                                               !- Electrical Storage Object Name
+
+  ElectricLoadCenter:Generators,
+  Backup Generators,             !- Name
+  Generator 1,                         !- Generator 1 Name
+  Generator:InternalCombustionEngine,   !- Generator 1 Object Type
+  50000,                                     !- Generator 1 Rated Electric Power Output
+  ON PEAK GENERATOR SCHEDULE,   !- Generator 1 Availability Schedule Name
+  ,                                               !- Generator 1 Rated Thermal to Electrical Power Ratio
+  Generator 2,                         !- Generator 2 Name
+  Generator:CombustionTurbine,   !- Generator 2 Object Type
+  30000,                                     !- Generator 2 Rated Electric Power Output
+  OFF PEAK GENERATOR SCHEDULE,   !- Generator 2 Availability Schedule Name
+  ,                                               !- Generator 2 Rated Thermal to Electrical Power Ratio
+  Generator 3,                         !- Generator 3 Name
+  Generator:MicroTurbine,   !- Generator 3 Object Type
+  65000,                                     !- Generator 3 Rated Electric Power Output
+  MID PEAK GENERATOR SCHEDULE,   !- Generator 3 Availability Schedule Name
+  ;                                               !- Generator 3 Rated Thermal to Electrical Power Ratio
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-002}
+
+The output variables that are available for the microturbine generator are:
+
+\begin{itemize}
+\item
+  HVAC,Average,Generator Produced Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Produced Electric Energy {[}J{]}
+\item
+  HVAC,Average,Generator LHV Basis Electric Efficiency {[}-{]}
+\item
+  HVAC,Average,Generator \textless{}Fuel Type\textgreater{} HHV Basis Rate {[}W{]}
+\item
+  HVAC,Average,Generator Fuel HHV Basis Rate {[}W{]}
+\item
+  HVAC,Sum,Generator \textless{}Fuel Type\textgreater{} HHV Basis Energy {[}J{]}
+\item
+  HVAC,Sum,Generator Fuel HHV Basis Energy {[}J{]}
+\item
+  HVAC,Average,Generator \textless{}Fuel Type\textgreater{} Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+If Standby Power input field \textgreater{} 0.0:
+
+\begin{itemize}
+\item
+  HVAC,Average,Generator Standby Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Standby Electric Energy {[}J{]}
+\end{itemize}
+
+If Ancillary Power input field \textgreater{} 0.0:
+
+\begin{itemize}
+\item
+  HVAC,Average,Generator Ancillary Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Ancillary Electric Energy {[}J{]}
+\end{itemize}
+
+If heat recovery water inlet and outlet node names are entered (and valid):
+
+\begin{itemize}
+\item
+  HVAC,Average,Generator Produced Thermal Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Produced Thermal Energy {[}J{]}
+\item
+  HVAC,Average,Generator Thermal Efficiency LHV Basis {[}-{]}
+\item
+  HVAC,Average,Generator Heat Recovery Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Heat Recovery Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Heat Recovery Water Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+If exhaust air calculations are performed:
+
+\begin{itemize}
+\item
+  HVAC,Average,Generator Exhaust Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Generator Exhaust Air Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Generator Produced Electric Power {[}W{]}}\label{generator-produced-electric-power-w-1}
+
+This output variable is the average electric power produced by the generator in Watts for the timestep being reported. This is the net electric power produced, accounting for ancillary electric power consumed during generator operation.
+
+\paragraph{Generator Produced Electric Energy {[}J{]}}\label{generator-produced-electric-energy-j-1}
+
+This output variable is the electric energy produced by the generator in Joules for the timestep being reported. This output is also added to a meter with Resource Type = ElectricityProduced, End Use Key = Cogeneration, Group Key = Plant (Ref. Output:Meter objects). This is the net electric energy produced, accounting for ancillary electric consumption during generator operation.
+
+\paragraph{\texorpdfstring{Generator LHV Basis Electric Efficiency {[]}}{Generator LHV Basis Electric Efficiency }}\label{generator-lhv-basis-electric-efficiency}
+
+This output variable is the average electric efficiency of the generator (lower heating value basis) for the timestep being reported. The electric efficiency is the Generator Produced Electric Power in Watts divided by the generator s fuel energy consumption rate in Watts (lower heating value basis).
+
+\paragraph{Generator \textless{}Fuel Type\textgreater{} HHV Basis Rate {[}W{]}}\label{generator-fuel-type-hhv-basis-rate-w}
+
+This output variable is the average fuel-specific energy consumption rate of the electric generator in Watts (higher heating value basis) for the timestep being reported. \textless{}Fuel Type\textgreater{} is the name of the fuel used by this electric generator. \textless{}Fuel Type\textgreater{} can be one of the following: NaturalGas ( = \textgreater{} Gas ) or PropaneGas ( = \textgreater{} Propane ).
+
+\paragraph{Generator Fuel HHV Basis Rate {[}W{]}}\label{generator-fuel-hhv-basis-rate-w-1}
+
+This output variable is the average fuel energy consumption rate of the electric generator in Watts (higher heating value basis) for the timestep being reported. The output variable name is non-fuel specific.
+
+\paragraph{Generator \textless{}Fuel Type\textgreater{} HHV Basis Energy {[}J{]}}\label{generator-fuel-type-hhv-basis-energy-j}
+
+This output variable is the fuel-specific energy consumption of the electric generator in Joules (higher heating value basis) for the timestep being reported. This output is also added to a meter with Resource Type = \textless{}Fuel Type\textgreater{}, End Use Key = Cogeneration, Group Key = Plant (Ref. Output:Meter objects). \textless{}Fuel Type\textgreater{} is the name of the fuel used by this electric generator. \textless{}Fuel Type\textgreater{} can be one of the following: NaturalGas ( = \textgreater{} Gas ) or PropaneGas ( = \textgreater{} Propane ).
+
+\paragraph{Generator Fuel HHV Basis Energy {[}J{]}}\label{generator-fuel-hhv-basis-energy-j-1}
+
+This output variable is the fuel energy consumption of the electric generator in Joules (higher heating value basis) for the timestep being reported. The output variable name is non-fuel specific.
+
+\paragraph{Generator \textless{}Fuel Type\textgreater{} Mass Flow Rate {[}kg/s{]}}\label{generator-fuel-type-mass-flow-rate-kgs-2}
+
+This output variable is the average mass flow rate of fuel being consumed by the electric generator in kg/s for the timestep being reported. \textless{}Fuel Type\textgreater{} is the name of the fuel used by this electric generator. \textless{}Fuel Type\textgreater{} can be one of the following: Natural Gas ( = \textgreater{} Gas ) or Propane Gas ( = \textgreater{} Propane ).
+
+\paragraph{Generator Standby Electric Power {[}W{]}}\label{generator-standby-electric-power-w}
+
+This output variable is the average standby electric power consumed by the generator in Watts for the timestep being reported. Standby power is electrical power consumed by the generator (e.g., air fans and controls) when the generator is available to operate but the generator electrical power output is zero (power output is not being requested by the electric load center). This output variable is only produced when the user enters a value greater than 0.0 for the input field Standby Power.
+
+\paragraph{Generator Standby Electric Energy {[}J{]}}\label{generator-standby-electric-energy-j}
+
+This output variable is the standby electric energy consumption for the generator in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cogeneration, Group Key = Plant (Ref. Output:Meter objects). This output variable is only produced when the user enters a value greater than 0.0 for the input field Standby Power.
+
+\paragraph{Generator Ancillary Electric Power {[}W{]}}\label{generator-ancillary-electric-power-w}
+
+This output variable is the average ancillary electric power consumed by the generator in Watts for the timestep being reported. Ancillary power is the electrical power consumed by other associated equipment (e.g., external fuel pressurization pumps) when the generator is operating. This output variable is only produced when the user enters a value greater than 0.0 for the input field Ancillary Power.
+
+\paragraph{Generator Ancillary Electric Energy {[}J{]}}\label{generator-ancillary-electric-energy-j}
+
+This output variable is the ancillary electric energy consumption for the generator in Joules for the timestep being reported. This energy consumption is already deducted from the output variable Generator Produced Electric Energy ( net electric energy produced by the generator). This output variable is only produced when the user enters a value greater than 0.0 for the input field Ancillary Power.
+
+\paragraph{Generator Produced Thermal Rate {[}W{]}}\label{generator-produced-thermal-rate-w-1}
+
+This output variable is the average thermal power produced (i.e., exhaust energy recovery to heat water) in Watts for the timestep being reported.
+
+\paragraph{Generator Produced Thermal Energy {[}J{]}}\label{generator-produced-thermal-energy-j-1}
+
+This output variable is the thermal energy produced (i.e., exhaust energy recovery to heat water) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatRecovery, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Generator Thermal Efficiency LHV Basis {[}-{]}}\label{generator-thermal-efficiency-lhv-basis--}
+
+This output variable is the average thermal efficiency of the generator (lower heating value basis) for the timestep being reported. The thermal efficiency is the Generator Produced Thermal Rate in Watts divided by the generator s fuel energy consumption rate in Watts (lower heating value basis).
+
+\paragraph{Generator Heat Recovery Inlet Temperature {[}C{]}}\label{generator-heat-recovery-inlet-temperature-c-1}
+
+This output variable is the average heat recovery inlet water temperature in degrees Celsius for the timestep being reported.
+
+\paragraph{Generator Heat Recovery Outlet Temperature {[}C{]}}\label{generator-heat-recovery-outlet-temperature-c-1}
+
+This output variable is the average heat recovery outlet water temperature in degrees Celsius for the timestep being reported.
+
+\paragraph{Generator Heat Recovery Water Mass Flow Rate {[}kg/s{]}}\label{generator-heat-recovery-water-mass-flow-rate-kgs}
+
+This output variable is the average heat recovery water mass flow rate in kilograms per second for the timestep being reported.
+
+\paragraph{Generator Exhaust Air Mass Flow Rate {[}kg/s{]}}\label{generator-exhaust-air-mass-flow-rate-kgs}
+
+This is the mass flow rate of exhaust leaving the generator. This output is available when the model input is setup for exhaust conditions.
+
+\paragraph{Generator Exhaust Air Temperature {[}C{]}}\label{generator-exhaust-air-temperature-c-1}
+
+This is the temperature of exhaust leaving the generator. This output is available when the model input is setup for exhaust conditions.
+
+\subsection{Generator:MicroCHP}\label{generatormicrochp}
+
+This object is used to model small-scale combined heat and power (micro CHP) electric generators using the model developed by IEA/ECBCS \href{http://www.ecbcs.org/annexes/annex42.htm}{Annex 42}. The model was developed for both internal combustion and Stirling cycle engines, but might be used for other types of residential CHP devices.
+
+Note that unlike other component models in EnergyPlus, this model is not normalized. Therefore, performance coefficients developed for one type and capacity of CHP device cannot be used for a device with a different capacity.
+
+This model is an empirical, curve fit model. This object describes the connections to the rest of the building model and includes a reference to another object called Generator:MicroCHP:NonNormalizedParameters that provides the operating characteristics.
+
+\subsubsection{Inputs}\label{inputs-10-003}
+
+\paragraph{Field: Name}\label{field-name-11-003}
+
+This field contains a unique name for the residential CHP device.
+
+\paragraph{Field: Performance Parameters Name}\label{field-performance-parameters-name}
+
+This field contains the name of a Generator:MicroCHP:NonNormalizedParameters object defined elsewhere in the input.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-7-000}
+
+This field contains the name of the thermal zone where the CHP device is located in the model. If the device is outdoors, or you do not want skin losses to be added to a zone, then leave this field blank.
+
+\paragraph{Field: Cooling Water Inlet Node Name}\label{field-cooling-water-inlet-node-name}
+
+This field provides the name of a node that is the inlet to the CHP device. The node should be on the plant loop that will receive the heat from the residential CHP unit. This inlet serves as the cooling water for the CHP device.
+
+\paragraph{Field: Cooling Water Outlet Node Name}\label{field-cooling-water-outlet-node-name}
+
+This field provides the name of a node that is the outlet to the CHP device. The node should be on the plant loop that will receive the heat from the residential CHP unit. This outlet serves as the exit of the cooling water leaving the CHP unit.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-000}
+
+The name of an air node that supplies the CHP unit with air for use inside the generator.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-000}
+
+The name of an air node that receives the exhaust from the CHP unit.
+
+\paragraph{Field: Generator Fuel Supply Name}\label{field-generator-fuel-supply-name}
+
+This field contains the name of a Generator:FuelSupply object defined elsewhere in the input file.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-7-000}
+
+This field contains the name of a schedule used to control whether or not the unit is available. It is available any time the value is greater than zero. If it is available, it may consume standby power at times when there is no request for power from the Electric Load Center. If it is not available (schedule value = 0.0) then the CHP unit is in a completely off mode and will not consume standby power. If this field is blank, the schedule has values of 1 for all time periods.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+Generator:MicroCHP,
+  MicroCoGen1,                         !- Name
+  SENERTECH5_5KW,                   !- Performance Parameters Name
+  ZN_1_FLR_1_SEC_1,               !- Zone Name
+  MICROCHP SENERTECH Pump-MicroCoGen1Node,   !- Cooling Water Inlet Node Name
+  MICROCHP SENERTECH Supply Equipment Outlet Node,   !- Cooling Water Outlet Node Name
+  MicroCoGen1 air inlet node,   !- Air Inlet Node Name
+  ,                                               !- Air Outlet Node Name
+  NATURALGAS,                           !- Generator Fuel Supply Name
+  ALWAYS_ON;                             !- Availability Schedule Name
+\end{lstlisting}
+
+\subsection{Generator:MicroCHP:NonNormalizedParameters}\label{generatormicrochpnonnormalizedparameters}
+
+This object is referenced by a Generator:MicroCHP object and provides the non-normalized parameters for the MicroCHP generator model.
+
+\subsubsection{Inputs}\label{inputs-11-003}
+
+\paragraph{Field: Name}\label{field-name-12-002}
+
+Unique name to identify this set of parameter data.
+
+\paragraph{Field: Maximum Electric Power}\label{field-maximum-electric-power}
+
+This is the size of the CHP unit in terms of the maximum electrical power it can produce {[}W{]}. If the electric load center requests more power than this maximum, then the unit will restrict its output to this level.
+
+\paragraph{Field: Minimum Electric Power}\label{field-minimum-electric-power}
+
+This is the size of the CHP unit in terms of the minimum electrical power it can produce {[}W{]}. If the electric load center requests less power than this minimum, then the unit will hold its output to this level.
+
+\paragraph{Field: Minimum Cooling Water Flow Rate}\label{field-minimum-cooling-water-flow-rate}
+
+This is the minimum flow rate of cooling water that must be available for the unit to operate {[}kg/s{]}. If the plant loop is not providing this flow of water, the unit will shut down to protect it from overheating.
+
+\paragraph{Field: Maximum Cooling Water Temperature}\label{field-maximum-cooling-water-temperature}
+
+This is the maximum temperature of cooling water inlet or outlet that can occur without the unit shutting down to protect from overheating {[} °C{]}.
+
+\paragraph{Field: Electrical Efficiency Curve Name}\label{field-electrical-efficiency-curve-name}
+
+This is the name of Curve:Triquadratic object that defines the steady-state net electrical efficiency. The electrical efficiency, \(\eta_e\) , is a function of the cooling water mass flow rate \(\dot m_{cw}\) , the temperature of the cooling water at the inlet, \(T_{cw}\) , the steady-state net electrical power produced, \(P_{net,ss}\) .
+
+\begin{equation}
+\eta_e = f\left( {{P_{net,ss}},{{\dot m}_{cw}},{T_{cw}}} \right)
+\end{equation}
+
+The associated Curve:Triquadratic object should be defined with the independent variables \({P_{net,ss}},{\dot m_{cw}},{T_{cw}}\) corresponding to \emph{x}, \emph{y}, and \emph{z}, respectively.
+
+\paragraph{Field: Thermal Efficiency Curve Name}\label{field-thermal-efficiency-curve-name}
+
+This is the name of a Curve:Triquadratic object that defines the steady-state net thermal efficiency. The thermal efficiency, \(\eta_q\) , is a function of the cooling water mass flow rate, \(\dot m_{cw}\) , the temperature of the cooling water at the inlet, \(T_{cw}\) , the steady-state net electrical power produced, \(P_{net,ss}\) .
+
+\begin{equation}
+{\eta_q} = f\left( {{P_{net,ss}},{{\dot m}_{cw}},{T_{cw}}} \right)
+\end{equation}
+
+The associated Curve:Triquadratic object should be defined with the independent variables \({P_{net,ss}},{\dot m_{cw}},{T_{cw}}\) corresponding to \emph{x}, \emph{y}, and \emph{z}, respectively.
+
+\paragraph{Field: Cooling Water Flow Rate Mode}\label{field-cooling-water-flow-rate-mode}
+
+This field is used to choose between different modes of controlling the mass flow rate of cooling water. There are two options available for this field: PlantControl or InternalControl. The PlantControl option indicates that the cooling water flow rate through the CHP device is determined externally (by the wider balance of plant). The InternalControl option indicates the flow of cooling water is controlled inside the CHP device (e.g., like an automobile s thermostat).
+
+For internal control, the following field is used to define a Biquadratic curve that will determine the cooling water flow rate. For internal control, the CHP device should (probably) include a bypass branch when connecting to the plant loop.
+
+\paragraph{Field: Cooling Water Flow Rate Curve Name}\label{field-cooling-water-flow-rate-curve-name}
+
+This field contains the name of a Curve:Biquadratic object that defines the mass flow rate of cooling water, \({\dot m_{cw}}\) . This field is only used if the prior field is set to InternalControl. The mass flow of cooling water is a function of steady-state power, \({P_{net,ss}}\) , and the inlet temperature of the cooling water, \({T_{cw}}\) . The associated Curve:Biquadratic should be defined with the independent variables \({P_{net,ss}}\) and \({T_{cw}}\) corresponding to \emph{x} and \emph{y}, respectively.
+
+\paragraph{Field: Air Flow Rate Curve Name}\label{field-air-flow-rate-curve-name}
+
+This is the name of a Curve:Quadratic object that defines the steady state air flow into the CHP device as a function of the mass flow rate of fuel.
+
+\paragraph{Field: Maximum Net Electrical Power Rate of Change}\label{field-maximum-net-electrical-power-rate-of-change}
+
+This field contains input on the limits for how fast the generator can ramp up or down in terms of the net electrical power.
+
+\paragraph{Field: Maximum Fuel Flow Rate of Change}\label{field-maximum-fuel-flow-rate-of-change}
+
+This field contains input on the limits for how fast the generator can ramp up or down in terms of the fuel flow rates.
+
+\paragraph{Field: Heat Exchanger U-Factor Times Area Value}\label{field-heat-exchanger-u-factor-times-area-value-000}
+
+This field describes the effective UA value for the heat exchanger that transfers heat from the generator to the cooling water.
+
+\paragraph{Field: Skin Loss U-Factor Times Area Value}\label{field-skin-loss-u-factor-times-area-value}
+
+This field describes the effective UA value for the heat transfer from the generator to the surrounding air.
+
+\paragraph{Field: Skin Loss Radiative Fraction}\label{field-skin-loss-radiative-fraction}
+
+This field describes the split between thermal radiation and thermal convection for the heat losses from the skin of the generator.
+
+\paragraph{Field: Aggregated Thermal Mass of Energy Conversion Portion of Generator}\label{field-aggregated-thermal-mass-of-energy-conversion-portion-of-generator}
+
+This field describes the aggregated thermal mass of the energy conversion portion of the generator. This includes the engine block in an internal combustion engine.
+
+\paragraph{Field: Aggregated Thermal Mass of Heat Recovery Portion of Generator}\label{field-aggregated-thermal-mass-of-heat-recovery-portion-of-generator}
+
+This field describes the aggregated thermal mass of the heat recovery portion of the generator. This includes the encapsulated cooling water and heat exchanger shell in immediate thermal contact.
+
+\paragraph{Field: Standby Power}\label{field-standby-power-1}
+
+This field describes the power used by the CHP unit s control systems while in standby operation. Standby operation mode occurs whenever the unit is available but not being called upon to produce power. Power is entered as a positive value but indicates negative generation.
+
+\paragraph{Field: Warm Up Mode}\label{field-warm-up-mode}
+
+This field is used to choose between different modes of controlling the warm up characteristics. Residential CHP units such as Stirling engines have different warm up characteristics than internal combustion engines. There are two warm up modes available: NominalEngineTemperature or TimeDelay. If the former mode is input in this field, then the next three fields are used to model warm up. If the later mode is input, then the fourth field below is used to model warm up.
+
+\paragraph{Field: Warm Up Fuel Flow Rate Coefficient}\label{field-warm-up-fuel-flow-rate-coefficient}
+
+This field describes the value for the coefficient used to determine the rate of fuel flow during warm up. The coefficient, \emph{k\(_{f}\)}, is used in the following relation,
+
+\begin{equation}
+{\dot m_{fuel,warm - up}} = {\dot m_{fuel,ss - \max }} + {k_f}{\dot m_{fuel,ss - \max }}\left( {\frac{{{T_{eng,nom}} - {T_{room}}}}{{{T_{eng}} - {T_{room}}}}} \right)
+\end{equation}
+
+\paragraph{Field: Nominal Engine Operating Temperature}\label{field-nominal-engine-operating-temperature}
+
+This field describes the nominal engine temperature during normal, steady-state operation, \({T_{eng,nom}}\) {[} °C{]}.
+
+\paragraph{Field: Warm Up Power Coefficient}\label{field-warm-up-power-coefficient}
+
+This field describes the value for the coefficient used to determine the rate of power production during warm up. The coefficient k\(_{p}\) is used in the following relation,
+
+\begin{equation}
+{P_{net,warm - up}} = {P_{\max }}{k_p}\left( {\frac{{{T_{eng}} - {T_{room}}}}{{{T_{eng,nom}} - {T_{room}}}}} \right)
+\end{equation}
+
+\paragraph{Field: Warm Up Fuel Flow Rate Limit Ratio}\label{field-warm-up-fuel-flow-rate-limit-ratio}
+
+This field is used to describe a limit to the fuel flow rate during warm up. The limit is a ratio multiplied by the maximum fuel flow rate during normal operation (corresponding to the fuel flow for maximum electrical power). If the warm up operating fuel flow rate is twice the steady state fuel flow at maximum power, then a value of 2.0 would be entered in this field. This field is only used with the nominal engine temperature warm up mode and is intended for Stirling engines.
+
+\paragraph{Field: Warm Up Delay Time}\label{field-warm-up-delay-time}
+
+This field is used to model the warm up operation when the warm up mode is TimeDelay.
+
+Enter the time between activation and power generation in seconds.
+
+\paragraph{Field: Cool Down Power}\label{field-cool-down-power}
+
+This field describes the power used by the CHP unit s ancillary systems while in cool down operation mode. Cool down operation mode occurs whenever the unit has recently been told to stop producing power. Power here is consumed and entered as a positive value that indicates negative generation. For example, a component such as a cooling fan might continue to run during cool down.
+
+\paragraph{Field: Cool Down Delay Time}\label{field-cool-down-delay-time}
+
+This field is used to describe the time it takes for the CHP unit to cool off and complete the cool down operation. Enter the time between deactivation and the end of a cool down period in seconds.
+
+\paragraph{Field: Restart Mode}\label{field-restart-mode}
+
+This field is used to choose between two different control situations for the cool down operation. The two options for this field are MandatoryCoolDown and OptionalCoolDown. The former is used to direct the model to complete the entire cool down period before the generator can subsequently enter warm up mode. The latter directs the model to allow immediately switching to warm up mode, if power is requested before the cool down period is completed.
+
+An example IDF showing how this object is used is provided below:
+
+\begin{lstlisting}
+
+Generator:MicroCHP:NonNormalizedParameters,
+  SENERTECH5_5KW,         !- Name
+  5500.0000,              !- Maximum Electric Power {W}
+  0.0000,                 !- Minimum Electric Power {W}
+  0.0000,                 !- Minimum Cooling Water Flow Rate {kg/s}
+  80.0000,                !- Maximum Cooling Water Temperature {C}
+  SenerTechElEff,         !- Electrical Efficiency Curve Name
+  SenerTechThermEff,      !- Thermal Efficiency Curve Name
+  InternalControl,        !- Cooling Water Flow Rate Mode
+  SenerTechCoolWaterflow, !- Cooling Water Flow Rate Curve Name
+  SenerTechAirFlow,       !- Air Flow Rate Curve Name
+  1000000000.0000,        !- Maximum Net Electrical Power Rate of Change {W/s}
+  1000000000.0000,        !- Maximum Fuel Flow Rate of Change {kg/s2}
+  741.0000,               !- Heat Exchanger U-Factor Times Area Value {W/K}
+  13.7000,                !- Skin Loss U-Factor Times Area Value {W/K}
+  0.5000,                 !- Skin Loss Radiative Fraction
+  63605.6000,             !- Aggregated Thermal Mass of Energy Conversion Portion of Generator {W/K}
+  1000.7000,              !- Aggregated Thermal Mass of Heat Recovery Portion of Generator {W/K}
+  0.0000,                 !- Standby Power {W}
+  TimeDelay,              !- Warm Up Mode
+  ,                       !- Warm Up Fuel Flow Rate Coefficient
+  ,                       !- Nominal Engine Operating Temperature {C}
+  ,                       !- Warm Up Power Coefficient
+  ,                       !- Warm Up Fuel Flow Rate Limit Ratio
+  60.0000,                !- Warm Up Delay Time {s}
+  0.0000,                 !- Cool Down Power {W}
+  60.0000,                !- Cool Down Delay Time {s}
+  OptionalCoolDown;       !- Restart Mode
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8-001}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Generator Off Mode Time {[}s{]}
+\item
+  HVAC,Sum,Generator Standby Mode Time {[}s{]}
+\item
+  HVAC,Sum,Generator Warm Up Mode Time {[}s{]}
+\item
+  HVAC,Sum,Generator Normal Operating Mode Time {[}s{]}
+\item
+  HVAC,Sum,Generator Cool Down Mode Time {[}s{]}
+\item
+  HVAC,Average,Generator Produced Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Produced Electric Energy {[}J{]}
+\item
+  HVAC,Average,Generator Electric Efficiency {[]}
+\item
+  HVAC,Average,Generator Thermal Efficiency {[]}
+\item
+  HVAC,Average,Generator Gross Input Heat Rate {[}W{]}
+\item
+  HVAC,Average,Generator Steady State Engine Heat Generation Rate {[}W{]}
+\item
+  HVAC,Average, Generator Engine Heat Exchange Rate {[}W{]}
+\item
+  HVAC,Average,Generator Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Generator Fuel Molar Flow Rate {[}kmol/s{]}
+\item
+  HVAC,Average,Generator Fuel Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Generator Engine Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Coolant Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Coolant Outlet Temperature {[}C{]}
+\item
+  HVAC,Sum,Generator Fuel HHV Basis Energy {[}J{]}
+\item
+  HVAC,Average,Generator Fuel HHV Basis Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Fuel LHV Basis Energy {[}J{]}
+\item
+  HVAC,Average,Generator Fuel LHV Basis Rate {[}W{]}
+\item
+  HVAC,Average,Generator Fuel Compressor Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Fuel Compressor Electric Energy {[}J{]}
+\item
+  HVAC,Average,Generator Fuel Compressor Skin Heat Loss Rate {[}W{]}
+\item
+  HVAC,Average,Generator Zone Sensible Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Zone Sensible Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Generator Zone Convection Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Generator Zone Radiation Heat Transfer Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Generator Off Mode Time {[}s{]}}\label{generator-off-mode-time-s}
+
+This report is the amount of time the generator spent in Off mode in seconds.
+
+\paragraph{Generator Standby Mode Time {[}s{]}}\label{generator-standby-mode-time-s}
+
+This report is the amount of time the generator spent in Stand By mode in seconds.
+
+\paragraph{Generator Warm Up Mode Time {[}s{]}}\label{generator-warm-up-mode-time-s}
+
+This report is the amount of time the generator spent in Warm Up mode in seconds.
+
+\paragraph{Generator Normal Operating Mode Time {[}s{]}}\label{generator-normal-operating-mode-time-s}
+
+This report is the amount of time the generator spent in Normal Operating mode in seconds.
+
+\paragraph{Generator Cool Down Mode Time {[}s{]}}\label{generator-cool-down-mode-time-s}
+
+This report is the amount of time the generator spent in Cool Down mode in seconds.
+
+\paragraph{Generator Produced Electric Power {[}W{]}}\label{generator-produced-electric-power-w-2}
+
+This report is the net electrical power produced by the generator in watts.
+
+\paragraph{Generator Produced Electric Energy {[}J{]}}\label{generator-produced-electric-energy-j-2}
+
+This report is the net electrical energy produced by the generator in joules. This output variable is also put on the meter for on-site production.
+
+\paragraph{\texorpdfstring{Generator Electric Efficiency {[]}}{Generator Electric Efficiency }}\label{generator-electric-efficiency}
+
+This is the result for electrical efficiency.
+
+\paragraph{\texorpdfstring{Generator Thermal Efficiency {[]}}{Generator Thermal Efficiency }}\label{generator-thermal-efficiency}
+
+This is the result for thermal efficiency.
+
+\paragraph{Generator Gross Input Heat Rate {[}W{]}}\label{generator-gross-input-heat-rate-w}
+
+This is the gross rate of heat input (from fuel consumption) into the engine control volume.
+
+\paragraph{Generator Steady State Engine Heat Generation Rate {[}W{]}}\label{generator-steady-state-engine-heat-generation-rate-w}
+
+This is an interim value in the dynamic thermal calculation that describes the steady-state heat generation in the engine.
+
+\paragraph{Generator Engine Heat Exchange Rate {[}W{]}}\label{generator-engine-heat-exchange-rate-w}
+
+This is the rate of heat transfer within the generator between the engine section and the heat recovery section, in Watts.
+
+\paragraph{Generator Produced Thermal Rate {[}W{]}}\label{generator-produced-thermal-rate-w-2}
+
+\paragraph{Generator Produced Thermal Energy {[}J{]}}\label{generator-produced-thermal-energy-j-2}
+
+These are the rate and energy of thermal heat transferred from the engine to the heat recovery fluid in the coolant control volume.
+
+\paragraph{Generator Air Mass Flow Rate {[}kg/s{]}}\label{generator-air-mass-flow-rate-kgs}
+
+This is the rate of air flow thru the engine on a mass basis.
+
+\paragraph{Generator Fuel Molar Flow Rate {[}kmol/s{]}}\label{generator-fuel-molar-flow-rate-kmols}
+
+This is the rate of fuel flow thru the engine on a molar basis.
+
+\paragraph{Generator Fuel Mass Flow Rate {[}kg/s{]}}\label{generator-fuel-mass-flow-rate-kgs}
+
+This is the rate of fuel flow thru the engine on a mass basis.
+
+\paragraph{Generator Engine Temperature {[}C{]}}\label{generator-engine-temperature-c}
+
+This is the model result for engine temperature in C. This is the lumped temperature for the engine control volume.
+
+\paragraph{Generator Coolant Inlet Temperature {[}C{]}}\label{generator-coolant-inlet-temperature-c}
+
+This is the temperature of the inlet water used for heat recovery. It is determined by the balance of plant connected to the generator.
+
+\paragraph{Generator Coolant Outlet Temperature {[}C{]}}\label{generator-coolant-outlet-temperature-c}
+
+This report is the model prediction for the leaving temperature of water used for heat recovery. If there is no flow this is the modeled prediction for the mass of cooling water in contact with the engine.
+
+\paragraph{Generator Fuel HHV Basis Energy {[}J{]}}\label{generator-fuel-hhv-basis-energy-j-2}
+
+This is the energy used by the cogeneration device in terms of higher heating value in joules. This is the output variable is also put on the meter for natural gas.
+
+\paragraph{Generator Fuel HHV Basis Rate {[}W{]}}\label{generator-fuel-hhv-basis-rate-w-2}
+
+This is the rate of fuel energy use by the cogeneration device in terms of higher heating value in watts.
+
+\paragraph{Generator Fuel LHV Basis Energy {[}J{]}}\label{generator-fuel-lhv-basis-energy-j}
+
+This is the fuel energy used by the cogeneration device in terms of lower heating value in joules.
+
+\paragraph{Generator Fuel LHV Basis Rate {[}W{]}}\label{generator-fuel-lhv-basis-rate-w}
+
+This is the rate of fuel energy use by the cogeneration device in terms of lower heating value in watts
+
+\paragraph{Generator Zone Sensible Heat Transfer Rate {[}W{]}}\label{generator-zone-sensible-heat-transfer-rate-w}
+
+Rate of heat gain to zone from cogeneration unit.
+
+\paragraph{Generator Zone Sensible Heat Transfer Energy {[}J{]}}\label{generator-zone-sensible-heat-transfer-energy-j}
+
+Heat gains to zone from cogeneration unit.
+
+\paragraph{Generator Zone Convection Heat Transfer Rate {[}W{]}}\label{generator-zone-convection-heat-transfer-rate-w}
+
+Portion of rate of heat gain to zone in the form of surface convection heat transfer.
+
+\paragraph{Generator Zone Radiation Heat Transfer Rate {[}W{]}}\label{generator-zone-radiation-heat-transfer-rate-w}
+
+Portion of heat gains to zone in the form of surface radiation heat transfer (to other surfaces in zone).
+
+\subsection{Generator:FuelCell}\label{generatorfuelcell}
+
+This object is used to model small Fuel Cell (FC) generators. IEA/ECBCS Annex 42 see www.cogen-sim.net, developed the FC model implemented in EnergyPlus. The model can be used for two general types of fuel cells, solid oxide fuel cells (SOFC) and proton exchange membrane fuel cells (PEMFC). Warning! This is a complicated model, intended primarily for research. Because fuel cells for cogeneration (producing both heat and electricity) are not yet a mature product for building systems, the input data for this model are extremely difficult to obtain. However, the model is designed to allow investigating the relative implications of a broad array of subsystems and interactions with the building.
+
+There should be one Generator:FuelCell object for each individual FC generator in the model. Multiple fuel cell generators can be included in a given simulation. Because there are a large number of inputs to the FC model and numerous, somewhat separable subsystems within a fuel cell, the EnergyPlus input objects have been organized into a number of separate input objects. This object simply refers to the names of all the other input objects that provide the input details for individual subsystems within the fuel cell cogeneration device. The following figure diagrams these separate subsystems. (not shown is an optional stack cooler with separate connections to heat recovery water loop and surrounding zone air).
+
+\begin{figure}[hbtp] % fig 152
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image467.png}
+\caption{Fuel cell subsystems. \protect \label{fig:fuel-cell-subsystems.}}
+\end{figure}
+
+Note that the FC model is formulated using the Lower Heating Value (LHV) of the fuel, whereas most other parts of EnergyPlus use the Higher Heating Value (HHV). LHV has important advantages over HHV in the context of the quality of heat recovered. While model coefficients for input performance descriptions are to be based on LHV, energy consumption and tariff calculations are also reported on HHV basis when using this model.
+
+\subsubsection{Inputs}\label{inputs-12-003}
+
+\paragraph{Field: Name}\label{field-name-13-002}
+
+This field contains a unique name for the fuel cell.
+
+\paragraph{Field: Power Module Name}\label{field-power-module-name}
+
+This field contains the name of a Generator:FuelCell:PowerModule input object.
+
+\paragraph{Field: Air Supply Name}\label{field-air-supply-name}
+
+This field contains the name of a Generator:FuelCell:AirSupply input object.
+
+\paragraph{Field: Fuel Supply Name}\label{field-fuel-supply-name}
+
+This field contains the name of a Generator:FuelSupply input object.
+
+\paragraph{Field: Water Supply Name}\label{field-water-supply-name}
+
+This field contains the name of a Generator:FuelCell:WaterSupply input object.
+
+\paragraph{Field: Auxiliary Heater Name}\label{field-auxiliary-heater-name}
+
+This field contains the name of a Generator:FuelCell:AuxiliaryHeater input object.
+
+\paragraph{Field: Heat Exchanger Name}\label{field-heat-exchanger-name-000}
+
+This field contains the name of a Generator:FuelCell:ExhaustGasToWaterHeatExchanger input object.
+
+\paragraph{Field: Electrical Storage Name}\label{field-electrical-storage-name}
+
+This field contains the name of a Generator:FuelCell:ElectricalStorage input object.
+
+\paragraph{Field: Inverter Name}\label{field-inverter-name}
+
+This field contains the name of a Generator:FuelCell:Inverter input object.
+
+\paragraph{Field: Stack Cooler Name}\label{field-stack-cooler-name}
+
+This field contains the name of a Generator:FuelCell:StackCooler input object. This is optional. The presence of a stack cooler distinguishes between SOFC and PEMFC with PEMFC operating at lower temperatures and requiring a separate subsystem to maintain stack temperatures.
+
+An example input data file (IDF) entry for this object is provided below:
+
+\begin{lstlisting}
+
+Generator:FuelCell,
+  FCT SOFC,                               !- Name
+  FCT SOFC Power Module,     !- Power Module Name
+  FCT SOFC Air Supply,         !- Air Supply Name
+  FCT SOFC Fuel Supply,       !- Fuel Supply Name
+  FCT SOFC Water Supply,     !- Water Supply Name
+  FCT SOFC Auxiliary Heater,   !- Auxiliary Heater Name
+  FCT SOFC Exhaust HX,         !- Heat Exchanger Name
+  FCT SOFC Battery,               !- Electrical Storage Name
+  FCT SOFC Inverter;             !- Inverter Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-9-001}
+
+The following output variables are available for the fuel cell model.
+
+\begin{itemize}
+\item
+  Output:Variable,*,Generator Produced Electric Power,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,Generator Produced Electric Energy,hourly; !- HVAC Sum {[}J{]}
+\item
+  Output:Variable,*,Generator Produced Thermal Rate,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,Generator Produced Thermal Energy,hourly; !- HVAC Sum {[}J{]}
+\item
+  Output:Variable,*,Generator Fuel HHV Basis Energy,hourly; !- HVAC Sum {[}J{]}
+\item
+  Output:Variable,*,Generator Fuel HHV Basis Rate,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,Generator Fuel LHV Basis Energy,hourly; !- HVAC Sum {[}J{]}
+\item
+  Output:Variable,*,Generator Fuel Consumption Rate LHV Basis,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,FuelCell Heat Loss Rate to Zone,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,FuelCell Heat Loss Energy to Zone,hourly; !- HVAC Sum {[}J{]}
+\item
+  Output:Variable,*,FuelCell Convection Heat Loss Rate to Zone,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,FuelCell Radiation Heat Loss Rate to Zone,hourly; !- HVAC Average {[}W{]}
+\end{itemize}
+
+\paragraph{Generator Produced Electric Power {[}W{]}}\label{generator-produced-electric-power-w-3}
+
+This report is the net electrical power produced by the generator in watts.
+
+\paragraph{Generator Produced Electric Energy {[}J{]}}\label{generator-produced-electric-energy-j-3}
+
+This report is the net electrical energy produced by the generator in joules. This output variable is also put on the meter for on-site production.
+
+\paragraph{Generator Produced Thermal Rate {[}W{]}}\label{generator-produced-thermal-rate-w-3}
+
+\paragraph{Generator Produced Thermal Energy {[}J{]}}\label{generator-produced-thermal-energy-j-3}
+
+These are the rate and energy of thermal heat transferred from the engine to the heat recovery fluid in the coolant control volume.
+
+\paragraph{Generator Fuel HHV Basis Energy {[}J{]}}\label{generator-fuel-hhv-basis-energy-j-3}
+
+This is the energy used by the cogeneration device in terms of higher heating value in joules. This is the output variable is also put on the meter for natural gas.
+
+\paragraph{Generator Fuel HHV Basis Rate {[}W{]}}\label{generator-fuel-hhv-basis-rate-w-3}
+
+This is the rate of fuel energy use by the cogeneration device in terms of higher heating value in watts.
+
+\paragraph{Generator Fuel LHV Basis Energy {[}J{]}}\label{generator-fuel-lhv-basis-energy-j-1}
+
+This is the fuel energy used by the cogeneration device in terms of lower heating value in joules.
+
+\paragraph{Generator Fuel Consumption Rate LHV Basis {[}W{]}}\label{generator-fuel-consumption-rate-lhv-basis-w}
+
+This is the rate of fuel energy use by the cogeneration device in terms of lower heating value in watts.
+
+\paragraph{Generator Zone Sensible Heat Transfer Rate {[}W{]}}\label{generator-zone-sensible-heat-transfer-rate-w-1}
+
+This variable provides the results for the total rate of skin losses from the fuel cell to the surrounding zone.
+
+\paragraph{Generator Zone Sensible Heat Transfer Energy {[}J{]}}\label{generator-zone-sensible-heat-transfer-energy-j-1}
+
+This variable provides the results for the total energy in skin losses from the fuel cell to the surrounding zone.
+
+\paragraph{Generator Zone Convection Heat Transfer Rate {[}W{]}}\label{generator-zone-convection-heat-transfer-rate-w-1}
+
+This variable provides the results for the rate of skin losses in the form of surface convection heat transfer from the fuel cell to the surrounding zone.
+
+\paragraph{Generator Zone Radiation Heat Transfer Rate {[}W{]}}\label{generator-zone-radiation-heat-transfer-rate-w-1}
+
+This variable provides the results for the rate of skin losses in the form of radiation heat transfer from the fuel cell to the surrounding zone.
+
+Using the FC model with DisplayAdvancedReportVariables (see Diagnostics object or use of operating system s environment variables) makes the following output variables available as listed in the RDD file. There are a large number of output variables that provide access to the inner workings of the model and individual subsystems that are not likely to be useful for the average user.
+
+\begin{itemize}
+\item
+  HVAC,Average,Generator Air Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Power Module Entering Air Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Air Molar Flow Rate {[}kmol/s{]}
+\item
+  HVAC,Average,Generator Power Module Entering Air Enthalpy {[}W{]}
+\item
+  HVAC,Average,Generator Blower Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Blower Electric Energy {[}J{]}
+\item
+  HVAC,Average,Generator Blower Skin Heat Loss Rate {[}W{]}
+\item
+  HVAC,Average,Generator Fuel Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Power Module Entering Fuel Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Fuel Molar Flow Rate {[}kmol/s{]}
+\item
+  HVAC,Average,Generator Power Module Entering Fuel Enthalpy {[}W{]}
+\item
+  HVAC,Average,Generator Fuel Compressor Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Fuel Compressor Electric Energy {[}J{]}
+\item
+  HVAC,Average,Generator Fuel Compressor Skin Heat Loss Rate {[}W{]}
+\item
+  HVAC,Average,Generator Fuel Reformer Water Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Power Module Entering Reforming Water Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Fuel Reformer Water Molar Flow Rate {[}kmol/s{]}
+\item
+  HVAC,Average,Generator Fuel Reformer Water Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Fuel Reformer Water Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Generator Power Module Entering Reforming Water Enthalpy {[}W{]}
+\item
+  HVAC,Average,Generator Product Gas Temperature {[}C{]}
+\item
+  HVAC,Average,Generator Product Gas Enthalpy {[}W{]}
+\item
+  HVAC,Average,Generator Product Gas Molar Flow Rate {[}kmol/s{]}
+\item
+  HVAC,Average,Generator Product Gas Ar Molar Flow Rate {[}kmol/s{]}
+\item
+  HVAC,Average,Generator Product Gas CO2 Molar Flow Rate {[}kmol/s{]}
+\item
+  HVAC,Average,Generator Product Gas H2O Vapor Molar Flow Rate {[}kmol/s{]}
+\item
+  HVAC,Average,Generator Product Gas N2 Molar Flow Rate {[}kmol/s{]}
+\item
+  HVAC,Average,Generator Product Gas O2 Molar Flow Rate {[}kmol/s{]}
+\item
+  HVAC,Average,Generator Inverter Loss Power {[}W{]}
+\item
+  HVAC,Average,Generator Produced DC Electric Power {[}W{]}
+\item
+  HVAC,Average,Generator DC Power Efficiency {[]}
+\item
+  HVAC,Average,Generator Electric Storage Charge State {[}J{]}
+\item
+  HVAC,Average,Generator Produced DC Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator DC Storage Charging Energy {[}J{]}
+\item
+  HVAC,Average,Generator DC Storage Discharging Power {[}W{]}
+\item
+  HVAC,Sum,Generator DC Storage Discharging Energy {[}J{]}
+\item
+  HVAC,Average,Generator Ancillary AC Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Ancillary AC Electric Energy {[}J{]}
+\item
+  HVAC,Average,Generator Zone Sensible Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Zone Sensible Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Generator Zone Convection Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Generator Zone Radiation Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum, Generator Fuel Cell Model Iteration Count {[]}
+\item
+  HVAC,Sum,Generator Regula Falsi Iteration Count {[]}
+\end{itemize}
+
+\paragraph{Generator Air Inlet Temperature {[}C{]}}\label{generator-air-inlet-temperature-c}
+
+This variable provides the temperature of air supplied to the FC.
+
+\paragraph{Generator Power Module Entering Air Temperature {[}C{]}}\label{generator-power-module-entering-air-temperature-c}
+
+This variable provides the temperature of the air supplied to the power module after it has gone through the blower and received any heat recovered from other subsystems.
+
+\paragraph{Generator Air Molar Flow Rate {[}kmol/s{]}}\label{generator-air-molar-flow-rate-kmols}
+
+This variable provides the results for \({\dot N_{air}}\) , the flow rate of air into the FC.
+
+\paragraph{Generator Power Module Entering Air Enthalpy {[}W{]}}\label{generator-power-module-entering-air-enthalpy-w}
+
+This variable provides the results for \({\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\hat h}_i} - {\Delta_f}\hat h_i^0} \right]} \right)}_{air}}\) , which is the enthalpy flow in the air stream entering the power module relative to 25 °C.
+
+\paragraph{Generator Blower Electric Power {[}W{]}}\label{generator-blower-electric-power-w}
+
+This variable provides the results for \({P_{blower - el}}\) , which is the electrical power used by the air supply blower.
+
+\paragraph{Generator Blower Electric Energy {[}J{]}}\label{generator-blower-electric-energy-j}
+
+This variable provides the results for the energy used by the air supply blower. It is also added to the appropriate meters.
+
+\paragraph{Generator Blower Skin Heat Loss Rate {[}W{]}}\label{generator-blower-skin-heat-loss-rate-w}
+
+This variable provides the results for \({q_{blower - heat - loss}}\) , which is the rate of energy lost to the surroundings.
+
+\paragraph{Generator Fuel Inlet Temperature {[}C{]}}\label{generator-fuel-inlet-temperature-c}
+
+This variable provides the temperature of the fuel supplied to the FC.
+
+\paragraph{Generator Power Module Entering Fuel Temperature {[}C{]}}\label{generator-power-module-entering-fuel-temperature-c}
+
+This variable provides the temperature of the fuel supplied to the power module after it has gone through the compressor.
+
+\paragraph{Generator Fuel Molar Flow Rate {[}kmol/s{]}}\label{generator-fuel-molar-flow-rate-kmols-1}
+
+This variable provides the results for \({\dot N_{fuel}}\) , which is the flow rate of fuel into the FC.
+
+\paragraph{Generator Power Module Entering Fuel Enthalpy {[}W{]}}\label{generator-power-module-entering-fuel-enthalpy-w}
+
+This variable provides the results for \({\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\hat h}_i} - {\Delta_f}\hat h_i^0} \right]} \right)}_{fuel}}\) , which is the enthalpy flow in the fuel stream entering the power module relative to 25 °C.
+
+\paragraph{Generator Fuel Compressor Electric Power {[}W{]}}\label{generator-fuel-compressor-electric-power-w}
+
+This variable provides the results for \({P_{comp - el}}\) , which is the electrical power used by the fuel supply compressor.
+
+\paragraph{Generator Fuel Compressor Electric Energy {[}J{]}}\label{generator-fuel-compressor-electric-energy-j}
+
+This variable provides the results for the energy used by the fuel supply compressor. It is also added to the appropriate meters.
+
+\paragraph{Generator Fuel Compressor Skin Heat Loss Rate {[}W{]}}\label{generator-fuel-compressor-skin-heat-loss-rate-w}
+
+This variable provides the results for the rate of energy lost to the surroundings.
+
+\paragraph{Generator Fuel Reformer Water Inlet Temperature {[}C{]}}\label{generator-fuel-reformer-water-inlet-temperature-c}
+
+This variable provides the temperature of the water supplied to the FC for reforming.
+
+\paragraph{Generator Power Module Entering Reforming Water Temperature {[}C{]}}\label{generator-power-module-entering-reforming-water-temperature-c}
+
+This variable provides the temperature of the water supplied to the power module after it has gone through the pump.
+
+\paragraph{Generator Fuel Reformer Water Molar Flow Rate {[}kmol/s{]}}\label{generator-fuel-reformer-water-molar-flow-rate-kmols}
+
+This variable provides the results for \({\dot N_{water}}\) , which the flow rate of reforming water into the FC.
+
+\paragraph{Generator Fuel Reformer Water Pump Electric Power {[}W{]}}\label{generator-fuel-reformer-water-pump-electric-power-w}
+
+This variable provides the results for \({P_{pump - el}}\) , which is the electrical power used by the water pump.
+
+\paragraph{Generator Fuel Reformer Water Pump Electric Energy {[}J{]}}\label{generator-fuel-reformer-water-pump-electric-energy-j}
+
+This variable provides the results for energy used by the water pump. It is also added to the appropriate meters.
+
+\paragraph{Generator Power Module Entering Reforming Water Enthalpy {[}W{]}}\label{generator-power-module-entering-reforming-water-enthalpy-w}
+
+This variable provides the results for \({\dot H_{liq - water}}\) which is the enthalpy flow of the water stream entering the power module relative to 25 °C.
+
+\paragraph{Generator Product Gas Temperature {[}C{]}}\label{generator-product-gas-temperature-c}
+
+This variable provides the results for the temperature of the product gas stream leaving the fuel cell power module.
+
+\paragraph{Generator Product Gas Enthalpy {[}W{]}}\label{generator-product-gas-enthalpy-w}
+
+This variable provides the results for \({\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\hat h}_i} - {\Delta_f}\hat h_i^0} \right]} \right)}_{FCPM - cg}}\) , which is the enthalpy flow in the product gas stream leaving the power module relative to 25 °C.
+
+\paragraph{Generator Product Gas Molar Flow Rate {[}kmol/s{]}}\label{generator-product-gas-molar-flow-rate-kmols}
+
+This variable provides the results for the flow rate of all the product gases leaving the fuel cell power module.
+
+\paragraph{Generator Product Gas Ar Molar Flow Rate {[}kmol/s{]}}\label{generator-product-gas-ar-molar-flow-rate-kmols}
+
+This variable provides the results for the flow rate of the argon gas leaving the fuel cell power module.
+
+\paragraph{Generator Product Gas CO2 Molar Flow Rate {[}kmol/s{]}}\label{generator-product-gas-co2-molar-flow-rate-kmols}
+
+This variable provides the results for the flow rate of the carbon dioxide gas leaving the fuel cell power module.
+
+\paragraph{Generator Product Gas H2O Vapor Molar Flow Rate {[}kmol/s{]}}\label{generator-product-gas-h2o-vapor-molar-flow-rate-kmols}
+
+This variable provides the results for the flow rate of the water gas leaving the fuel cell power module.
+
+\paragraph{Generator Product Gas N2 Molar Flow Rate {[}kmol/s{]}}\label{generator-product-gas-n2-molar-flow-rate-kmols}
+
+This variable provides the results for the flow rate of the nitrogen gas leaving the fuel cell power module.
+
+\paragraph{Generator Product Gas O2 Molar Flow Rate {[}kmol/s{]}}\label{generator-product-gas-o2-molar-flow-rate-kmols}
+
+This variable provides the results for the flow rate of the oxygen gas leaving the fuel cell power module.
+
+\paragraph{Generator Inverter Loss Power {[}W{]}}\label{generator-inverter-loss-power-w}
+
+This variable provides the results for the power losses associated with inefficiencies in the inverter.
+
+\paragraph{Generator Produced DC Electric Power {[}W{]}}\label{generator-produced-dc-electric-power-w}
+
+This variable provides the results for \({P_{el}}\) , which is the net DC electrical power produced by the fuel cell power module.
+
+\paragraph{\texorpdfstring{Generator DC Power Efficiency {[]}}{Generator DC Power Efficiency }}\label{generator-dc-power-efficiency}
+
+This variable provides the results for \({\varepsilon_{el}}\) , which is the electrical efficiency of the fuel cell power module.
+
+\paragraph{Generator Electric Storage Charge State {[}J{]}}\label{generator-electric-storage-charge-state-j}
+
+This variable provides the results for state of charge of the electrical storage device inside the fuel cell. Although the units are Joules, this is a state variable and is reported as an average rather than a sum.
+
+\paragraph{Generator Produced DC Electric Power {[}W{]}}\label{generator-produced-dc-electric-power-w-1}
+
+This variable provides the rate at which power was stored into the fuel cell s electrical storage subsystem.
+
+\paragraph{Generator DC Storage Charging Energy {[}J{]}}\label{generator-dc-storage-charging-energy-j}
+
+This variable provides the energy stored into the fuel cell s electrical storage subsystem.
+
+\paragraph{Generator DC Storage Discharging Power {[}W{]}}\label{generator-dc-storage-discharging-power-w}
+
+This variable provides the rate at which power was drawn from the fuel cell s electrical storage subsystem.
+
+\paragraph{Generator DC Storage Discharging Energy {[}J{]}}\label{generator-dc-storage-discharging-energy-j}
+
+This variable provides the energy drawn from the fuel cell s electrical storage subsystem.
+
+\paragraph{Generator Ancillary AC Electric Power {[}W{]}}\label{generator-ancillary-ac-electric-power-w}
+
+This variable provides the results for \({P_{el,ancillaries - AC}}\) , which is the rate at which ancillary devices within the power module use electricity supplied to the fuel cell by an external source.
+
+\paragraph{Generator Ancillary AC Electric Energy {[}J{]}}\label{generator-ancillary-ac-electric-energy-j}
+
+This variable provides the results for the energy used by AC ancillaries. It is also added to the appropriate meters.
+
+\paragraph{\texorpdfstring{Generator Fuel Cell Model Iteration Count {[]}}{Generator Fuel Cell Model Iteration Count }}\label{generator-fuel-cell-model-iteration-count}
+
+This variable provides information on the numerical method used to calculate the FC model. EnergyPlus uses a sequential substitution iterative algorithm to solve the main heat balance equation for the FC model. This output variable indicates the number of iterations needed to converge.
+
+\paragraph{\texorpdfstring{Generator Regula Falsi Iteration Count {[]}}{Generator Regula Falsi Iteration Count }}\label{generator-regula-falsi-iteration-count}
+
+This variable provides information on the numerical method used to calculate product gas temperature as a function of the product gas s enthalpy. A Regula Falsi numerical method is used to invert the Shomate equation for enthalpy as a function of temperature. This output variable indicates the number of iterations needed for the Regula Falsi method to converge.
+
+\paragraph{Generator Heat Recovery Exit Gas Temperature {[}C{]}}\label{generator-heat-recovery-exit-gas-temperature-c}
+
+This is the temperature of the exiting gas for heat recovery in C.
+
+\paragraph{\texorpdfstring{Generator Heat Recovery Exit Gas H2O Vapor Fraction {[]}}{Generator Heat Recovery Exit Gas H2O Vapor Fraction }}\label{generator-heat-recovery-exit-gas-h2o-vapor-fraction}
+
+This is the water vapor fraction in the exit gas.
+
+\paragraph{Generator Heat Recovery Water Condensate Molar Flow Rate {[}kmol/s{]}}\label{generator-heat-recovery-water-condensate-molar-flow-rate-kmols}
+
+This is the flow of condensed water in kmol/s.
+
+\subsection{Generator:FuelCell:PowerModule}\label{generatorfuelcellpowermodule}
+
+This object is used to describe the core power module subsystem of the FC. This includes the fuel cell stack, fuel reformer, and whatever ancillary devices are included inside. If the model has multiple FC generators that are of the exact same type, then only one of these objects is needed and all the Generator:FuelCell can reference it. The model uses a number of curves to describe operating performance. Input data for specific models of FC are not yet available but will be produced by IEA Annex 42 and should be available in the future.
+
+\subsubsection{Inputs}\label{inputs-13-003}
+
+\paragraph{Field: Name}\label{field-name-14-001}
+
+This field contains a unique name for the fuel cell power module subsystem.
+
+\paragraph{Field: Efficiency Curve Mode}\label{field-efficiency-curve-mode}
+
+This field is used to choose between different modes of inputting the electrical efficiency curve. There are two options available for this Field: Annex42 and Normalized . The Annex42 option indicates that the efficiency curves are not normalized and are used for the single size and type of FC product. The Normalized option indicates that the efficiency curves are normalized (as is standard practice in EnergyPlus) relative to a single rating point. In the Annex42 mode, the curves directly represent efficiency as a function of fuel use, but in the Normalized mode, the curves represent an efficiency modification that is applied to the efficiency at the rating point.
+
+\paragraph{Field: Efficiency Curve Name}\label{field-efficiency-curve-name}
+
+This field contains the name of a Curve:Quadratic input object described elsewhere in the input file. The curve is a function of the net DC electric power, \({P_{el}}\) (W), produced by the power module and describes either the electrical efficiency or the how the efficiency is modified depending on the mode selected in the previous field. This quadratic curve is just one part of the entire parametric relation used to describe electrical efficiency \({\varepsilon_{el}}\) . For the Annex42 mode the full relation for efficiency is,
+
+\begin{equation}
+{\varepsilon_{el}} = \left[ {{\varepsilon_0} + {\varepsilon_1} \cdot {P_{el}} + {\varepsilon_2} \cdot P_{el}^2} \right] \cdot \left[ {1 - {N_{stops}} \cdot D} \right] \cdot \left[ {1 - (MAX(\int\limits_{} {dt - {t_{threshold}},0.0))}  \cdot L} \right]
+\end{equation}
+
+where the Curve:Quadratic input object named in this field serves to define the quadratic portion in the first set of brackets. For the Normalized mode the full relation for efficiency is,
+
+\begin{equation}
+{\varepsilon_{el}} = \left[ {{\varepsilon_0} + {\varepsilon_1} \cdot \frac{{{P_{el}}}}{{{P_{nom}}}} + {\varepsilon_2} \cdot {{\left( {\frac{{{P_{el}}}}{{{P_{nom}}}}} \right)}^2}} \right] \cdot {\varepsilon_{nom}} \cdot \left[ {1 - {N_{stops}} \cdot D} \right] \cdot \left[ {1 - (MAX(\int\limits_0 {dt - {t_{threshold}},0.0))}  \cdot L} \right]
+\end{equation}
+
+where \({\varepsilon_{nom}}\) is the nominal electrical efficiency at the rating point \({P_{nom}}\) which are described in the next two fields. The Normalized mode may be more useful for a simulation study that needs to vary the capacity of the FC.
+
+\paragraph{Field: Nominal Efficiency}\label{field-nominal-efficiency}
+
+This field is used for the Normalized efficiency curve mode and provides the nominal efficiency \({\varepsilon_{nom}}\) (dimensionless) at the rating point. This field can be left blank if using the Annex42 mode.
+
+\paragraph{Field: Nominal Electrical Power}\label{field-nominal-electrical-power}
+
+This field is used for the Normalized efficiency curve mode and provides the nominal net DC electrical power produced \({P_{nom}}\) (W) at the rating point. This field can be left blank if using the Annex42 mode.
+
+\paragraph{Field: Number of Stops at Start of Simulation}\label{field-number-of-stops-at-start-of-simulation}
+
+This field is used to describe the number of times the FC has been cycled on and off prior to the start of the simulation. FC products might degrade as a result of starting and stopping the fuel cell stack, so the model includes terms to model the degradation effects of cycling FC units on and off. This is the initial value of the \({N_{stops}}\) \emph{\(_{}\)}term in the efficiency relation above.
+
+\paragraph{Field: Cycling Performance Degradation Coefficient}\label{field-cycling-performance-degradation-coefficient}
+
+This field is used to describe the fixed value representing the fractional performance degradation associated with each start and stop cycle. This is the value of \(D\) in the efficiency relations above. If there is no degradation from cycling, then D should be 0.0.
+
+\paragraph{Field: Number of Run Hours at Beginning of Simulation}\label{field-number-of-run-hours-at-beginning-of-simulation}
+
+This field is used to describe the amount of time the FC has been operating prior to the start of the simulation. FC products might degrade over time so the model includes terms to model the degradation effects of FC run time. This is the initial value of the integrated run time term \(\int\limits_0 {dt}\) .
+
+\paragraph{Field: Accumulated Run Time Degradation Coefficient}\label{field-accumulated-run-time-degradation-coefficient}
+
+This field is used to describe the fixed value representing the fractional performance degradation associated with the total amount of run time. This is the value of \(L\) in the efficiency relations above. If there is no degradation from run time, the L should be 0.0.
+
+\paragraph{Field: Run Time Degradation Initiation Time Threshold}\label{field-run-time-degradation-initiation-time-threshold}
+
+This field is used to describe the time period for which there is no degradation associated with the amount of run time. This provides the ability to model a system that initially operates without degradation for some period time before it starts to degrade. This is the value of \({t_{threshold}}\) in the efficiency relations above.
+
+\paragraph{Field: Power Up Transient Limit}\label{field-power-up-transient-limit}
+
+This field is used to describe the maximum allowable rate at which the fuel cell can increase the level of power it produces (W/s). This is a time derivative of the net DC electrical power used to limit how fast the FC can ramp up.
+
+\paragraph{Field: Power Down Transient Limit}\label{field-power-down-transient-limit}
+
+This field is used to describe the maximum allowable rate at which the fuel cell can decrease the level of power it produces (W/s). This is a time derivative of the net DC electrical power used to limit how fast the FC can ramp down.
+
+\paragraph{Field: Start Up Time}\label{field-start-up-time}
+
+This field is used to describe the length of time (seconds) of the start up period when the FC is turned on.
+
+\paragraph{Field: Start Up Fuel}\label{field-start-up-fuel}
+
+This field is used to describe the amount of fuel (kmol) used during the entire start up period. The fuel is the same type as what is described in the Generator:FuelSupply object elsewhere in the input file.
+
+\paragraph{Field: Start Up Electricity Consumption}\label{field-start-up-electricity-consumption}
+
+This field is used to describe the amount of electricity (Joules) used by ancillary equipment during the entire start up period.
+
+\paragraph{Field: Start Up Electricity Produced}\label{field-start-up-electricity-produced}
+
+This field is used to describe the amount of electricity (Joules) produced by the power module during the entire start up period.
+
+\paragraph{Field: Shut Down Time}\label{field-shut-down-time}
+
+This field is used to describe the length of time (seconds) of the shut down period.
+
+\paragraph{Field: Shut Down Fuel}\label{field-shut-down-fuel}
+
+This field is used to describe the amount of fuel (kmol) used during the entire shut down period. The fuel is the same type as what is described in the Generator:FuelSupply object elsewhere in the input file.
+
+\paragraph{Field: Shut Down Electricity Consumption}\label{field-shut-down-electricity-consumption}
+
+This field is used to describe the amount of electricity (J) used by ancillary equipment during the entire shut down period.
+
+\paragraph{Field: Ancillary Electricity Constant Term}\label{field-ancillary-electricity-constant-term}
+
+This field is used to describe the constant term, \(an{c_0}\) , in a relation that describes the AC electrical power used by ancillary equipment located inside the power module, \({P_{el,ancillaries - AC}}\) . The model uses this relation,
+
+\begin{equation}
+{P_{el,ancillaries - AC}} = an{c_0} + an{c_1} \cdot {\dot N_{fuel}}
+\end{equation}
+
+where \({\dot N_{fuel}}\) is the rate of fuel use in the power module (kmol/s).
+
+\paragraph{Field: Ancillary Electricity Linear Term}\label{field-ancillary-electricity-linear-term}
+
+This field is used to describe the linear term, \(an{c_1}\) , in the relation shown in the previous field.
+
+\paragraph{Field: Skin Loss Calculation Mode}\label{field-skin-loss-calculation-mode}
+
+This field is used to select the mode for how skin losses are modeled. Skin losses are heat energy lost from the power module and transferred to the surrounding thermal zone named in the following field. There are three alpha options to choose from: ConstantRate , UAForProcessGasTemperature , or QuadraticFunctionOfFuelRate. Enter ConstantRate in this field to model skin losses using a constant rate, e.g.~100 watts. Enter UAForProcessGasTemperature to model skin losses using a UA-Delta-T calculation method with the temperature difference determined by the power module s product gas temperature and the surrounding zone. Enter QuadraticFunctionOfFuelRate to model skin losses as a function of the rate of fuel use.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-8-000}
+
+This field is used to describe the thermal zone that will receive skin and other heat losses from the FC. This should be the name of a Zone input object declared elsewhere in the input file.
+
+\paragraph{Field: Skin Loss Radiative Fraction}\label{field-skin-loss-radiative-fraction-1}
+
+This field is used to describe the portion of skin losses that are in the form of thermal radiation. This controls the radiative/convective split for the energy transferred to the zone by the FC.
+
+\paragraph{Field: Constant Skin Loss Rate}\label{field-constant-skin-loss-rate}
+
+This field is used to describe the constant rate of skin losses (W). This field is used with the ConstantRate mode. It can be left blank for other skin loss modes.
+
+\paragraph{Field: Skin Loss U-Factor Times Area Term}\label{field-skin-loss-u-factor-times-area-term}
+
+This field is used to describe the UA term (W/K). This field is used with the UAForProcessGasTemperature mode. It can be left blank for other skin loss modes. UA is the product of the overall heat transfer coefficient U and the area A.
+
+\paragraph{Field: Skin Loss Quadratic Curve Name}\label{field-skin-loss-quadratic-curve-name}
+
+This field is used to refer to the name of a quadratic curve object defined elsewhere in the input file. The quadratic curve should define skin heat loss rate as a function of the fuel use rate (kmol/s) so that,
+
+\begin{equation}
+{q_{skin - loss}} = {s_0} + {s_1} \cdot {\dot N_{fuel}} + {s_2} \cdot \dot N_{fuel}^2
+\end{equation}
+
+\paragraph{Field: Dilution Air Flow Rate}\label{field-dilution-air-flow-rate}
+
+This field is used to describe the rate of dilution air (kmol/sec) drawn into, or through, the power module. This air stream may not be present in all FC products. It is used for limiting skin and stack heat losses and for strategies that mitigate potential safety issue were fuel gases to escape the stack.
+
+\paragraph{Field: Stack Heat loss to Dilution Air}\label{field-stack-heat-loss-to-dilution-air}
+
+This field is used to describe the rate at which the fuel cell stack adds energy to the dilution air stream. It is entered as a constant heat rate (W).
+
+\paragraph{Field: Dilution Inlet Air Node Name}\label{field-dilution-inlet-air-node-name}
+
+This field is used to describe the air node where the dilution air is drawn from. This would typically be the name of the air node associated with the thermal zone where the FC is located.
+
+\paragraph{Field: Dilution Outlet Air Node Name}\label{field-dilution-outlet-air-node-name}
+
+This field is used to describe the air node where the dilution air is exhausted to. This could be the inlets to a heat recovery ventilator or an exhaust node.
+
+\paragraph{Field: Minimum Operating Point}\label{field-minimum-operating-point}
+
+This field is used to describe the minimum operating point for the net DC electric power, \({P_{el}}\) (W).
+
+\paragraph{Field: Maximum Operating Point}\label{field-maximum-operating-point}
+
+This field is used to describe the maximum operating point for the net DC electric power, \({P_{el}}\) (W).
+
+An example input data file (IDF) entry for this object is provided below:
+
+\begin{lstlisting}
+
+Generator:FuelCell:PowerModule,
+  FCT SOFC Power Module,     !- Name
+  Annex42,                                 !- Efficiency Curve Mode
+  FCT Power Curve,                 !- Efficiency Curve Name
+  0.354,                                     !- Nominal Efficiency
+  3400,                                       !- Nominal Electrical Power {W}
+  0,                                             !- Number of Stops at Start of Simulation
+  0.0,                                         !- Cycling Performance Degradation Coefficient
+  0,                                             !- Number of Run Hours at Beginning of Simulation {hr}
+  0.0,                                         !- Accumulated Run Time Degradation Coefficient
+  10000,                                     !- Run Time Degradation Initiation Time Threshold {hr}
+  1.4,                                         !- Power Up Transient Limit {W/s}
+  0.2,                                         !- Power Down Transient Limit {W/s}
+  0.0,                                         !- Start Up Time {s}
+  0.2,                                         !- Start Up Fuel {kmol}
+  ,                                               !- Start Up Electricity Consumption {J}
+  0.0,                                         !- Start Up Electricity Produced {J}
+  0.0,                                         !- Shut Down Time {s}
+  0.2,                                         !- Shut Down Fuel {kmol}
+  ,                                               !- Shut Down Electricity Consumption {J}
+  0.0,                                         !- Ancillary Electricity Constant Term
+  0.0,                                         !- Ancillary Electricity Linear Term
+  ConstantRate,                       !- Skin Loss Calculation Mode
+  ZN_1_FLR_1_SEC_5,               !- Zone Name
+  0.6392,                                   !- Skin Loss Radiative Fraction
+  729,                                         !- Constant Skin Loss Rate {W}
+  0.0,                                         !- Skin Loss U-Factor Times Area Term {W/K}
+  ,                                               !- Skin Loss Quadratic Curve Name
+  6.156E-3,                               !- Dilution Air Flow Rate {kmol/s}
+  2307,                                       !- Stack Heat loss to Dilution Air {W}
+  SOFC Air HR Inlet,             !- Dilution Inlet Air Node Name
+  SOFC Air HR Outlet,           !- Dilution Outlet Air Node Name
+  3010,                                       !- Minimum Operating Point {W}
+  3728;                                       !- Maximum Operating Point {W}
+\end{lstlisting}
+
+\subsection{Generator:FuelCell:StackCooler}\label{generatorfuelcellstackcooler}
+
+This object is optional and is used to define details needed to model the stack cooler on PEMFC.
+
+\subsubsection{Field: Name}\label{field-name-15-001}
+
+This field contains a unique name for the PEM fuel cell stack cooler
+
+\subsubsection{Field: Heat Recovery Water Inlet Node Name}\label{field-heat-recovery-water-inlet-node-name-1}
+
+This field contains the node name for the water inlet to the stack cooler.
+
+\subsubsection{Field: Heat Recovery Water Outlet Node Nane}\label{field-heat-recovery-water-outlet-node-nane}
+
+This field contains the node name for the water outlet from the stack cooler.
+
+\subsubsection{Field: Nominal Stack Temperature}\label{field-nominal-stack-temperature}
+
+This field contains the nominal stack operating temperature for the PEMFC, \(T_{stack}^o\) . This field and the next five provide values for use in the empirical equation for the rate of heat extracted from the fuel cell power module by the stack cooler using the following relation
+
+\begin{equation}
+{q_{s - cool}} = \left[ {{r_0} + {r_1}\left( {{T_{stack}} - T_{stack}^o} \right)} \right] \cdot \left[ {1 + {r_2}{P_{el}} + {r_3}P_{el}^2} \right]
+\end{equation}
+
+\subsubsection{Field: Actual Stack Temperature{]}}\label{field-actual-stack-temperature}
+
+This field contains the actual stack operating temperature for the PEMFC, \({T_{stack}}\) .
+
+\subsubsection{Field: Coefficient r0}\label{field-coefficient-r0}
+
+This field contains the coefficient r\(_{0}\) in the equation above.
+
+\subsubsection{Field: Coefficient r1}\label{field-coefficient-r1}
+
+This field contains the coefficient r\(_{1}\) in the equation above.
+
+\subsubsection{Field: Coefficient r2}\label{field-coefficient-r2}
+
+This field contains the coefficient r\(_{2}\) in the equation above.
+
+\subsubsection{Field: Coefficient r3}\label{field-coefficient-r3}
+
+This field contains the coefficient r\(_{3}\) in the equation above.
+
+\subsubsection{Field: Stack Coolant Flow Rate}\label{field-stack-coolant-flow-rate}
+
+The stack cooler is assumed to have a closed water circulation loop that is used to extract heat from the stack and move it to a cogeneration heat exchanger and/or an air cooler. This field is used to enter the flow rate of coolant in this loop.
+
+\subsubsection{Field: Stack Cooler U-Factor Times Area Value}\label{field-stack-cooler-u-factor-times-area-value}
+
+This is the heat transfer coefficient between the stack and the coolant.
+
+\subsubsection{Field: Fs-cogen Adjustment Factor}\label{field-fs-cogen-adjustment-factor}
+
+This field provides the value for an adjustment factor, \({F_{s - cogen}}\) , used in the following relation for the cogeneration heat transfer coefficient, \({\left( {UA} \right)_{s - cogen}}\) :
+
+\begin{equation}
+{\left( {UA} \right)_{s - cogen}} = {\left[ {\frac{1}{{{{\left( {hA} \right)}_{s - cogen}}}} + {F_{s - cogen}}} \right]^{ - 1}}
+\end{equation}
+
+\subsubsection{Field: Stack Cogeneration Exchanger Area}\label{field-stack-cogeneration-exchanger-area}
+
+This field provides the value for the cogeneration heat exchanger area, \({A_{s - cogen}}\)
+
+\subsubsection{Field: Stack Cogeneration Exchanger Nominal Flow Rate}\label{field-stack-cogeneration-exchanger-nominal-flow-rate}
+
+This field provides the value for \(\dot N_{s - cogen}^0\) in the following relation for the cogeneration heat exchanger convection coefficient, \({h_{s - cogen}}\) :
+
+\begin{equation}
+{h_{s - cogen}} = h_{s - cogen}^0 \cdot {\left( {\frac{{{{\dot N}_{s - cogen}}}}{{\dot N_{s - cogen}^0}}} \right)^{{n_s}}}
+\end{equation}
+
+\subsubsection{Field: Stack Cogeneration Exchanger Nominal Heat Transfer Coefficient}\label{field-stack-cogeneration-exchanger-nominal-heat-transfer-coefficient}
+
+This field provides the value for \(h_{s - cogen}^0\) in the relation above for the cogeneration heat exchanger convection coefficient, \({h_{s - cogen}}\) .
+
+\subsubsection{Field: Stack Cogeneration Exchanger Nominal Heat Transfer Coefficient Exponent}\label{field-stack-cogeneration-exchanger-nominal-heat-transfer-coefficient-exponent}
+
+This field provides the value for \({n_s}\) is the relation above for the cogeneration heat exchanger convection coefficient, \({h_{s - cogen}}\) .
+
+\subsubsection{Field: Stack Cooler Pump Power}\label{field-stack-cooler-pump-power}
+
+This field is the power used by the stack cooler s circulating pump in Watts. It is a constant power draw whenever the stack cooler is active.
+
+\subsubsection{Field: Stack Cooler Pump Heat loss}\label{field-stack-cooler-pump-heat-loss}
+
+This field is the fraction of the pump power consumption that is lost to the surround zone.
+
+\subsubsection{Field: Stack Air Cooler Fan Coefficient f0}\label{field-stack-air-cooler-fan-coefficient-f0}
+
+This field and the next two are used to define coefficients for the following relation for the power used by the air-cooler s fan to dump excess heat into the surrounding zone:
+
+\begin{equation}
+{P_{s - air - el}} = {f_0} + {f_1} \cdot {q_{s - air}} + {f_2} \cdot q_{s - air}^2
+\end{equation}
+
+\subsubsection{Field: Stack Air Cooler Fan Coefficient f1}\label{field-stack-air-cooler-fan-coefficient-f1}
+
+This field provides a value for the coefficient \emph{f\(_{1}\)} in the relation above.
+
+\subsubsection{Field: Stack Air Cooler Fan Coefficient f2}\label{field-stack-air-cooler-fan-coefficient-f2}
+
+This field provides a value for the coefficient \emph{f\(_{2}\)} in the relation above.
+
+\subsection{Generator:FuelCell:AirSupply}\label{generatorfuelcellairsupply}
+
+This object is used to define details of the air supply subsystem.
+
+\subsubsection{Inputs}\label{inputs-14-003}
+
+\paragraph{Field: Name}\label{field-name-16-001}
+
+This field contains a unique name for the fuel cell air supply subsystem.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-1-000}
+
+This field is used to define the air node where the inlet air stream is drawn from. If the FC uses outdoor air then the node named here should be designated an outdoor air node. If the FC draws air from its surroundings, then this would be the name of the air node associated with the thermal zone containing the FC.
+
+\paragraph{Field: Blower Power Curve Name}\label{field-blower-power-curve-name}
+
+This field contains the name of a Curve:Cubic input object described elsewhere in the input file. The curve provides the power used by the air blower (W) as a cubic function of the rate of air supply (kmol/s).
+
+\begin{equation}
+{P_{blower - el}} = {b_0} + {b_1} \cdot {\dot N_{air}} + {b_2} \cdot \dot N_{air}^2 + {b_3} \cdot \dot N_{air}^3
+\end{equation}
+
+\paragraph{Field: Blower Heat Loss Factor}\label{field-blower-heat-loss-factor}
+
+This field describes the portion of blower electrical power that is lost to the surroundings. The rest of the energy is added to the air stream. A heat loss factor of 1.0 indicates that all the heat is lost to the surroundings and no energy is added to the air inlet stream.
+
+\paragraph{Field: Air Supply Rate Calculation Mode}\label{field-air-supply-rate-calculation-mode}
+
+This field describes how the model will calculate the air supply rate. There are three options to choose from: AirRatiobyStoics , QuadraticFunctionofElectricPower , and QuadraticFunctionofFuelRate. The choice will determine how the model calculates the rate of air and will depend on the formulations used to develop model input data. The choices are described in the next four fields.
+
+\paragraph{Field: Stoichiometric Ratio}\label{field-stoichiometric-ratio}
+
+This field describes the excess air ratio beyond stoichiometric air supply. This field is only used if the air supply rate calculation mode is AirRatiobyStoics. The total air supply ratio will be the value entered here plus 1.0. Thus if 1.0 is entered in this field, the total air flow will be 2.0 times what is needed to exactly match stoichiometry with the fuel supply.
+
+\paragraph{Field: Air Rate Function of Electric Power Curve Name}\label{field-air-rate-function-of-electric-power-curve-name}
+
+This field contains the name of a QuadraticCurve input object described elsewhere in the input file. This field is only used if the air supply rate calculation mode is QuadraticFunctionofElectricPower. The quadratic curve named here describes the first part of the relation below used to calculate the rate of inlet air, \({\dot N_{air}}\) (kmol/s). It is a quadratic function of the net DC electrical power, \({P_{el}}\) (W).
+
+\begin{equation}
+{a_3}
+\end{equation}
+
+\paragraph{Field: Air Rate Air Temperature Coefficient}\label{field-air-rate-air-temperature-coefficient}
+
+This field is used to describe the air temperature coefficient, \({\dot N_{air}} = \left[ {{a_0} + {a_1} \cdot {{\dot N}_{fuel}} + {a_2} \cdot \dot N_{fuel}^2} \right].\left[ {1 + {a_3} \cdot {T_{air}}} \right]\) , used to adjust inlet air flow rate in the relations for inlet air rate.
+
+\paragraph{Field: Air Rate Function of Fuel Rate Curve Name}\label{field-air-rate-function-of-fuel-rate-curve-name}
+
+This field contains the name of a Curve:Quadratic input object described elsewhere in the input file. This field is only used if the air supply rate calculation mode is QuadraticFunctionofFuelRate. The quadratic curve named here describes the first part of the relation used to calculate the rate of inlet air, \({\dot N_{air}}\) (kmol/s). It is a quadratic function of the fuel flow rate, \({\dot N_{fuel}}\) .
+
+\({\dot N_{air}} = \left[ {{a_0} + {a_1} \cdot {P_{el}} + {a_2} \cdot P_{el}^2} \right].\left[ {1 + {a_3} \cdot {T_{air}}} \right]\) \({\dot N_{air}} = \left[ {{a_0} + {a_1} \cdot {{\dot N}_{fuel}} + {a_2} \cdot \dot N_{fuel}^2} \right].\left[ {1 + {a_3} \cdot {T_{air}}} \right]\)
+
+\paragraph{Field: Air Intake Heat Recovery Mode}\label{field-air-intake-heat-recovery-mode}
+
+This field is used to control how heat losses from three other subsystems within the FC may or may not be recovered by the air inlet. There are six possible choices for what to use in this Field: NoRecovery RecoverBurnerInverterStorage RecoverAuxiliaryBurner RecoverInverterandStorage RecoverInverter and RecoverElectricalStorage . If heat is recovered then that means that energy losses from those subsystems are added to the inlet air and fed back into the FC power module. The following table clarifies the meaning of the six possible choices.
+
+% table 32
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Air Intake Heat Recovery Mode Choices \label{table:air-intake-heat-recovery-mode-choices}} \tabularnewline
+\toprule 
+Field Choice & Inverter Heat Losses Recovered? & Electrical Storage Heat Losses Recovered? & Auxiliary Heater Losses Recovered? \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Air Intake Heat Recovery Mode Choices} \tabularnewline
+\toprule 
+Field Choice & Inverter Heat Losses Recovered? & Electrical Storage Heat Losses Recovered? & Auxiliary Heater Losses Recovered? \tabularnewline
+\midrule
+\endhead
+
+NoRecovery & No & No & No \tabularnewline
+RecoverBurnerInverterStorage & Yes & Yes & Yes \tabularnewline
+RecoverAuxiliaryBurner & No & No & Yes \tabularnewline
+RecoverInverterandStorage & Yes & Yes & No \tabularnewline
+RecoverInverter & Yes & No & No \tabularnewline
+RecoverElectricalStorage & No & Yes & No \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Field: Air Supply Constituent Mode}\label{field-air-supply-constituent-mode}
+
+This field is used to choose between two different modes for describing the make up of the inlet air stream. There are two possible choices: AmbientAir or UserDefinedConstituents. Choosing the AmbientAir mode will automatically set the composition of air to be usual at: 77.28\% nitrogen, 20.73\% oxygen, 1.04\% water, 0.92\% argon, and 0.03\% carbon dioxide. Choosing UserDefinedConstituents allows the user to customize the make up the inlet air in the remaining fields.
+
+\paragraph{Field: Number of UserDefined Constituents}\label{field-number-of-userdefined-constituents}
+
+This field is used to describe the number of constituents in the inlet air. This field is only used if the air supply constituent mode is set to UserDefinedConstituents. The maximum number is 5.
+
+The remaining fields in this object are repeating pairs of fields with one pair for each constituent and the same number as described in the previous field. The pairs consist of the name of the constituent followed by the molar fraction of that constituent.
+
+\paragraph{Field: Constituent 1-5 Name}\label{field-constituent-1-5-name}
+
+These fields describe the air stream constituents by name. The name field for each pair must be filled with one of these choices: CarbonDioxide , Nitrogen, Oxygen, Water, or Argon.
+
+\paragraph{Field: Molar Fraction 1-5}\label{field-molar-fraction-1-5}
+
+These fields describe the molar fraction of the air stream constituents. It is very important that the sum of the molar fractions add up to 1.0.
+
+An example input data file (IDF) entry for this object is provided below:
+
+\begin{lstlisting}
+
+Generator:FuelCell:AirSupply,
+  FCT SOFC Air Supply,         !- Name
+  SOFC Air Inlet Node,         !- Air Inlet Node Name
+  FCT Blower Power Curve,   !- Blower Power Curve Name
+  1.0,                                         !- Blower Heat Loss Factor
+  QuadraticFunctionofElectricPower,   !- Air Supply Rate Calculation Mode
+  ,                                               !- Stoichiometric Ratio
+  FCT Excess Air Ratio Curve,   !- Air Rate Function of Electric Power Curve Name
+  2.83507E-3,                           !- Air Rate Air Temperature Coefficient
+  ,                                               !- Air Rate Function of Fuel Rate Curve Name
+  NoRecovery,                           !- Air Intake Heat Recovery Mode
+  UserDefinedConstituents,   !- Air Supply Constituent Mode
+  5,                                             !- Number of UserDefined Constituents
+  Nitrogen,                               !- Constituent 1 Name
+  0.7728,                                   !- Molar Fraction 1
+  Oxygen,                                   !- Constituent 2 Name
+  0.2073,                                   !- Molar Fraction 2
+  Water,                                     !- Constituent 3 Name
+  0.0104,                                   !- Molar Fraction 3
+  Argon,                                     !- Constituent 4 Name
+  0.0092,                                   !- Molar Fraction 4
+  CarbonDioxide,                     !- Constituent 5 Name
+  0.0003;                                   !- Molar Fraction 5
+\end{lstlisting}
+
+\subsection{Generator:FuelCell:WaterSupply}\label{generatorfuelcellwatersupply}
+
+This object is used to provide details of the water supply subsystem. This water is used for steam reforming of the fuel and is not the same as the water used for thermal heat recovery.
+
+\begin{lstlisting}
+Generator:FuelCell:WaterSupply,
+   A1, \field Name
+           \required-field
+           \reference FCWaterSupNames
+   A2, \field Reformer Water Flow Rate Function of Fuel Rate Curve Name
+           \type object-list
+           \object-list QuadraticCurves
+   A3, \field Reformer Water Pump Power Function of Fuel Rate Curve Name
+           \type object-list
+           \object-list QubicCurves
+   N1, \field Pump Heat Loss Factor
+   A4, \field Water Temperature Modeling Mode
+           \type choice
+           \key TemperatureFromAirNode
+           \key TemperatureFromWaterNode
+           \key TemperatureFromSchedule
+           \key MainsWaterTemperature
+   A5, \field Water Temperature Reference Node Name
+   A6; \field Water Temperature Schedule Name
+           \type object-list
+           \object-list ScheduleNames
+\end{lstlisting}
+
+\subsubsection{Inputs}\label{inputs-15-003}
+
+\paragraph{Field: Name}\label{field-name-17-000}
+
+This field contains a unique name for the fuel cell water supply subsystem.
+
+\paragraph{Field: Reformer Water Flow Rate Function of Fuel Rate Curve Name}\label{field-reformer-water-flow-rate-function-of-fuel-rate-curve-name}
+
+This field contains the name of a Curve:Quadratic input object described elsewhere in the input file. The curve provides the rate of water flow (kmol/sec) as a function of fuel flow rate (kmol/sec).
+
+\begin{equation}
+{\dot N_{liq - water}} = {w_0} + {w_1} \cdot {\dot N_{fuel}} + {w_2} \cdot \dot N_{fuel}^2
+\end{equation}
+
+If the unit does not use water for reforming then use a null quadratic where all the coefficients are 0.0.
+
+\paragraph{Field: Reformer Water Pump Power Function of Fuel Rate Curve Name}\label{field-reformer-water-pump-power-function-of-fuel-rate-curve-name}
+
+This field contains the name of a Curve:Cubic input object described elsewhere in the input file. The curve provides the power used by the water pump (W) as a cubic function of the rate of water supply (kmol/s).
+
+\begin{equation}
+{P_{pump - el}} = {p_0} + {p_1} \cdot {\dot N_{water}} + {p_2} \cdot \dot N_{water}^2 + {p_3} \cdot \dot N_{water}^3
+\end{equation}
+
+If the unit does not use water for reforming then use a null cubic where all the coefficients are 0.0.
+
+\paragraph{Field: Pump Heat Loss Factor}\label{field-pump-heat-loss-factor}
+
+This field describes the portion of pump electrical power that is lost to the surroundings. The rest of the energy is added to the water stream. A heat loss factor of 1.0 indicates that all the heat is lost to the surroundings and no energy is added to the water inlet stream.
+
+\paragraph{Field: Water Temperature Modeling Mode}\label{field-water-temperature-modeling-mode}
+
+This field describes how the model will determine the inlet temperature of the water stream. There are four options to choose from: TemperatureFromAirNode, TemperatureFromWaterNode, TemperatureFromSchedule, and MainsWaterTemperature. For the first two options, the temperature of the water inlet is determined by the temperature at the node named in the next field. For the third option, the temperature is determined by the schedule in the last field. Using the MainsWaterTemperature option requires also defining a separate Site:WaterMainsTemperature input object elsewhere in the input file.
+
+\paragraph{Field: Water Temperature Reference Node Name}\label{field-water-temperature-reference-node-name}
+
+This field is used to define the node where the temperature of the inlet water stream is obtained. This can be either an air node or a water node.
+
+\paragraph{Field: Water Temperature Schedule Name}\label{field-water-temperature-schedule-name}
+
+This field is used to define the name of a schedule, defined elsewhere in the input file, that will be used to determine the temperature of the water inlet stream when using the TemperatureFromSchedule mode.
+
+An example input data file (IDF) entry for this object is provided below:
+
+\begin{lstlisting}
+
+Generator:FuelCell:WaterSupply,
+  FCT SOFC Water Supply,     !- Name
+  Null Quadratic,                   !- Reformer Water Flow Rate Function of Fuel Rate Curve Name
+  Null Cubic,                           !- Reformer Water Pump Power Function of Fuel Rate Curve Name
+  0.0,                                         !- Pump Heat Loss Factor
+  TemperatureFromAirNode,   !- Water Temperature Modeling Mode
+  SOFC Air Inlet Node,         !- Water Temperature Reference Node Name
+  ;                                               !- Water Temperature Schedule Name
+
+  Curve:Quadratic,
+  Null Quadratic,                   !- Name
+  0.0,                                         !- Coefficient1 Constant
+  0.0,                                         !- Coefficient2 x
+  0.0,                                         !- Coefficient3 x**2
+  -1.0E+10,                               !- Minimum Value of x
+  1.0E+10;                                 !- Maximum Value of x
+
+  Curve:Cubic,
+  Null Cubic,                           !- Name
+  0.0,                                         !- Coefficient1 Constant
+  0.0,                                         !- Coefficient2 x
+  0.0,                                         !- Coefficient3 x**2
+  0.0,                                         !- Coefficient4 x**3
+  -1.0E+10,                               !- Minimum Value of x
+  1.0E+10;                                 !- Maximum Value of x
+\end{lstlisting}
+
+\subsection{Generator:FuelCell:AuxiliaryHeater}\label{generatorfuelcellauxiliaryheater}
+
+This object is intended for modeling an auxiliary heater, however this portion of the model is not yet available in EnergyPlus. An auxiliary heater may be present in fuel cell products so that the unit can meet much higher thermal loads than would be possible using only cogeneration. This portion of the model will be added in the future once suitable cogeneration control capabilities are also available. The input fields are described for future reference but may change. The program still requires one of these objects be included even though the data are not yet used (so that internal data structures can be allocated).
+
+\subsubsection{Inputs}\label{inputs-16-002}
+
+\paragraph{Field: Name}\label{field-name-18-000}
+
+This field contains a unique name for the fuel cell auxiliary heater subsystem.
+
+\paragraph{Field: Excess Air Ratio}\label{field-excess-air-ratio}
+
+This field describes the excess air ratio beyond stoichiometric air supply for the heater. The total air supply ratio will be the value entered here plus 1.0. Thus if 1.0 is entered in this field, the total air flow will be 2.0 times what is needed to exactly match stoichiometry with the fuel supply.
+
+\paragraph{Field: Ancillary Power Constant Term}\label{field-ancillary-power-constant-term}
+
+This field describes the constant term, \({x_0}\) , used to model the auxiliary burner s ancillary devices such as fans and ignition controls. The electrical power for ancillaries is calculated using,
+
+\begin{equation}
+{P_{el,aux - ancillaries}} = {x_0} + {x_1} \cdot {\dot N_{aux - fuel}}
+\end{equation}
+
+\paragraph{Field: Ancillary Power Linear Term}\label{field-ancillary-power-linear-term}
+
+This field describes the linear term, \({x_1}\) , used to model the auxiliary burner s ancillary devices.
+
+\paragraph{Field: Skin Loss U-Factor Times Area Value}\label{field-skin-loss-u-factor-times-area-value-1}
+
+This field describes the UA term (W/K) for calculating skin losses in the auxiliary burner. UA is the product of the overall heat transfer coefficient U and the area A. The skin heat losses are calculated using,
+
+\begin{equation}
+{q_{aux - skin - losses}} = {(UA)_{aux}} \cdot ({T_{aux - mix}} - {T_{room}})
+\end{equation}
+
+where, \({T_{aux - mix}}\) is temperature of product gases leaving the auxiliary burner and includes the mixing of the product gases from the fuel cell power module. Thus, the input for UA should reflect this choice of reference temperature rather than an exterior surface temperature of the auxiliary burner.
+
+\paragraph{Field: Skin Loss Destination}\label{field-skin-loss-destination}
+
+This field describes the user s choice for what happens to the skin losses. There are two options: SurroundingZone and AirInletForFuelCell . Entering SurroundingZone will direct the model to put the lost energy into the surrounding thermal Zone named in the next field. Entering AirInletForFuelCell will direct the model to put the lost energy into the air inlet stream for the fuel cell to preheat that air.
+
+\paragraph{Field: Zone Name to Receive Skin Losses}\label{field-zone-name-to-receive-skin-losses}
+
+This field is used to determine the zone that will receive the skin losses. Enter the name of a Zone declared elsewhere in the input file. This field is only used if the SurroundingZone mode is used in the previous field.
+
+\paragraph{Field: Heating Capacity Units}\label{field-heating-capacity-units}
+
+This field describes the user s choice for how the capacity of the auxiliary heater will be defined. There are two options: Watts or kmol/s. Entering Watts will direct the program to use the next two fields to determine the maximum and minimum heating capacity. Entering kmol/s will direct the program to use the last two fields to determine the maximum and minimum heating capacities.
+
+\paragraph{Field: Maximum Heating Capacity in Watts}\label{field-maximum-heating-capacity-in-watts}
+
+This field is used to describe the maximum heating capacity of the auxiliary burner (W).
+
+\paragraph{Field: Minimum Heating Capacity in Watts}\label{field-minimum-heating-capacity-in-watts}
+
+This field is used to describe the minimum heating capacity of the auxiliary burner (W).
+
+\paragraph{Field: Maximum Heating Capacity in Kmol per Second}\label{field-maximum-heating-capacity-in-kmol-per-second}
+
+This field is used to describe the maximum fuel use rate for the auxiliary burner (kmol/s).
+
+\paragraph{Field: Minimum Heating Capacity in Kmol per Second}\label{field-minimum-heating-capacity-in-kmol-per-second}
+
+This field is used to describe the minimum fuel use rate for the auxiliary burner (kmol/s).
+
+An example input data file (IDF) entry for this object is provided below:
+
+\begin{lstlisting}
+
+Generator:FuelCell:AuxiliaryHeater,
+  FCT SOFC Auxiliary Heater,   !- Name
+  0.0,                                         !- Excess Air Ratio
+  0.0,                                         !- Ancillary Power Constant Term
+  0.0,                                         !- Ancillary Power Linear Term
+  0.5,                                         !- Skin Loss U-Factor Times Area Value
+  SurroundingZone,                 !- Skin Loss Destination
+  ZN_1_FLR_1_SEC_5,               !- Zone Name to Receive Skin Losses
+  Watts,                                     !- Heating Capacity Units
+  0.0,                                         !- Maximum Heating Capacity in Watts
+  0.0,                                         !- Minimum Heating Capacity in Watts
+  ,                                               !- Maximum Heating Capacity in Kmol per Second
+  ;                                               !- Minimum Heating Capacity in Kmol per Second
+\end{lstlisting}
+
+Generator:FuelCell:ExhaustGasToWaterHeatExchanger
+
+This object is used to describe the exhaust gas heat exchanger subsystem of the FC used to recovery thermal energy.
+
+\paragraph{Field: Name}\label{field-name-19-000}
+
+This field contains a unique name for the fuel cell power module subsystem.
+
+\paragraph{Field: Heat Recovery Water Inlet Node Name}\label{field-heat-recovery-water-inlet-node-name-2}
+
+This field contains the name of the node that connects the heat exchanger s inlet to the plant loop. This water is used for heat recovery.
+
+\paragraph{Field: Heat Recovery Water Outlet Node Name}\label{field-heat-recovery-water-outlet-node-name-1}
+
+This field contains the name of the node that connects the heat exchanger s outlet to the plant loop.
+
+\paragraph{Field: Heat Recovery Water Maximum Flow Rate}\label{field-heat-recovery-water-maximum-flow-rate}
+
+This field describes the design maximum flow rate of the heat recovery water (m\(^{3}\)/s). The value should match the design flow rate of the plant loop connected to the FC.
+
+\paragraph{Field: Exhaust Outlet Air Node Name}\label{field-exhaust-outlet-air-node-name}
+
+This field is used to determine which node will receive the exhaust air stream leaving the FC. This node will usually be outside and not be referenced elsewhere. However, if the exhaust stream is used in a heat recovery ventilator (as described in section 11 of the Annex 42 specification) then the node would be reference in the heat recovery ventilator object.
+
+\paragraph{Field: Heat Exchanger Calculation Method}\label{field-heat-exchanger-calculation-method}
+
+This field is used to direct how EnergyPlus will calculate heat exchanger performance. The Annex 42 model provides for four different methods of modeling the heat exchanger. The choices available for this field are: FixedEffectiveness (method 1 in Annex 42 specification), EmpiricalUAeff (method 2), FundementalUAeff (method 3), or Condensing (method 4). The remaining fields provide input data for the different methods. The heat exchanger correlations are described below.
+
+\paragraph{Field: Method 1 Heat Exchanger Effectiveness}\label{field-method-1-heat-exchanger-effectiveness}
+
+This field describes constant heat exchanger effectiveness, \({\varepsilon_{HX}}\) . This field is only used with the FixedEffectiveness mode, which corresponds to method 1 in the Annex 42 specification. For this mode, the heat exchange between the exhaust gases and the heat recovery water are calculated using,
+
+\begin{equation}
+{q_{HX}} = {\varepsilon_{HX}} \cdot {\left( {\dot N{{\hat c}_p}} \right)_{\min }} \cdot \left( {{T_{aux - mix}} - {T_{water,in}}} \right)
+\end{equation}
+
+where, \({\left( {\dot N{{\hat c}_p}} \right)_{\min }}\) is the minimum value of \({\left( {\dot N{{\hat c}_p}} \right)_{aux - mix}}\) and \({\left( {\dot N{{\hat c}_p}} \right)_{water}}\) .
+
+\paragraph{Field: Method 2 Parameter hxs0}\label{field-method-2-parameter-hxs0}
+
+This field describes the value of \(h{x_{s,0}}\) in the relation below for effective UA. This field is used with the EmpiricalUAeff mode, which corresponds to method 2 in the Annex 42 specification and with the Condensing mode, which corresponds to method 4 . This method uses the log mean temperature difference (LMTD) approach to calculate the heat exchange:
+
+\begin{equation}
+{q_{HX}} = {\left( {UA} \right)_{eff}} \cdot \frac{{\left( {{T_{aux - mix}} - {T_{water,out}}} \right) - \left( {{T_{HX - exh}} - {T_{water,in}}} \right)}}{{\ln \left( {\frac{{{T_{aux - mix}} - {T_{water,out}}}}{{{T_{HX - exh}} - {T_{water,in}}}}} \right)}}
+\end{equation}
+
+The user input in this field, and the next four fields, describe coefficients in an empirical relation for \({\left( {UA} \right)_{eff}}\) :
+
+\begin{equation}
+{\left( {UA} \right)_{eff}} = h{x_{s,0}} + h{x_{s,1}} \cdot {\dot N_{water}} + h{x_{s,2}} \cdot \dot N_{water}^2 + h{x_{s,3}} \cdot {\dot N_{aux - mix}} + h{x_{s,4}} \cdot \dot N_{aux - mix}^2
+\end{equation}
+
+\paragraph{Field: Method 2 Parameter hxs1}\label{field-method-2-parameter-hxs1}
+
+This field describes the value of \(h{x_{s,1}}\) in the relation above for effective UA. This field is used with the EmpiricalUAeff mode, which corresponds to method 2 in the Annex 42 specification and with the Condensing mode, which corresponds to method 4 .
+
+\paragraph{Field: Method 2 Parameter hxs2}\label{field-method-2-parameter-hxs2}
+
+This field describes the value of \(h{x_{s,2}}\) in the relation above for effective UA. This field is used with the EmpiricalUAeff mode, which corresponds to method 2 in the Annex 42 specification and with the Condensing mode, which corresponds to method 4 .
+
+\paragraph{Field: Method 2 Parameter hxs3}\label{field-method-2-parameter-hxs3}
+
+This field describes the value of \(h{x_{s,3}}\) in the relation above for effective UA. This field is used with the EmpiricalUAeff mode, which corresponds to method 2 in the Annex 42 specification and with the Condensing mode, which corresponds to method 4 .
+
+\paragraph{Field: Method 2 Parameter hxs4}\label{field-method-2-parameter-hxs4}
+
+This field describes the value of \(h{x_{s,4}}\) in the relation above for effective UA. This field is used with the EmpiricalUAeff mode, which corresponds to method 2 in the Annex 42 specification and with the Condensing mode, which corresponds to method 4 .
+
+\paragraph{Field: Method 3 h0Gas Coefficient}\label{field-method-3-h0gas-coefficient}
+
+This field describes the value of \(h_{gas}^0\) in the relation below. This field is only used with the FundementalUAeff mode, which corresponds to method 3 in the Annex 42 specification. For this mode, the heat exchange is calculated using the LMTD method, but the effective UA is determined using:
+
+\begin{equation}
+{\left( {UA} \right)_{eff}} = {\left[ {\frac{1}{{{{\left( {hA} \right)}_{gas}}}} + \frac{1}{{{{(hA)}_{water}}}} + {F_{HX}}} \right]^{ - 1}}
+\end{equation}
+
+where,
+
+\({F_{HX}}\) is an adjustment factor,
+
+\({h_{gas}} = h_{gas}^0 \cdot {\left( {\frac{{{{\dot N}_{gas}}}}{{\dot N_{gas}^0}}} \right)^n}\) ,
+
+\begin{equation}
+{h_{water}} = h_{water}^0 \cdot {\left( {\frac{{{{\dot N}_{water}}}}{{\dot N_{water}^0}}} \right)^m}
+\end{equation}
+
+\paragraph{Field: Method 3 NdotGasRef Coefficient}\label{field-method-3-ndotgasref-coefficient}
+
+This field describes the value of \(\dot N_{gas}^0\) in the relation above. This field is only used with the FundementalUAeff mode, which corresponds to method 3 in the Annex 42 specification.
+
+\paragraph{Field: Method 3 n Coefficient}\label{field-method-3-n-coefficient}
+
+This field describes the value of \(n\) in the relation above. This field is only used with the FundementalUAeff mode, which corresponds to method 3 in the Annex 42 specification.
+
+\paragraph{Field: Method 3 Gas Area}\label{field-method-3-gas-area}
+
+This field describes the value of \({A_{gas}}\) in the relation above. This field is only used with the FundementalUAeff mode, which corresponds to method 3 in the Annex 42 specification.
+
+\paragraph{Field: Method 3 h0 Water Coefficient}\label{field-method-3-h0-water-coefficient}
+
+This field describes the value of \(h_{water}^0\) in the relation above. This field is only used with the FundementalUAeff mode, which corresponds to method 3 in the Annex 42 specification.
+
+\paragraph{Field: Method 3 N dot Water ref Coefficient}\label{field-method-3-n-dot-water-ref-coefficient}
+
+This field describes the value of \(\dot N_{water}^0\) in the relation above. This field is only used with the FundementalUAeff mode, which corresponds to method 3 in the Annex 42 specification.
+
+\paragraph{Field: Method 3 m Coefficient}\label{field-method-3-m-coefficient}
+
+This field describes the value of \(m\) in the relation above. This field is only used with the FundementalUAeff mode, which corresponds to method 3 in the Annex 42 specification.
+
+\paragraph{Field: Method 3 Area Water Coefficient}\label{field-method-3-area-water-coefficient}
+
+This field describes the value of \({A_{water}}\) in the relation above. This field is only used with the FundementalUAeff mode, which corresponds to method 3 in the Annex 42 specification.
+
+\paragraph{Field: Method 3 F Adjustment Factor}\label{field-method-3-f-adjustment-factor}
+
+This field describes the value of \({F_{HX}}\) in the relation above. This field is only used with the FundementalUAeff mode, which corresponds to method 3 in the Annex 42 specification.
+
+\paragraph{Field: Method 4 hxl1 Coefficient}\label{field-method-4-hxl1-coefficient}
+
+This field describes the value of \(h{x_{l,1}}\) in the relation below for the rate of condensation of water from the gas stream, \({\dot N_{{H_2}O - cond}}\) . This field is only used with the Condensing mode, which corresponds to method 4 in the Annex 42 specification. This method uses a modified version of the LMTD approach to calculate heat exchange:
+
+\begin{equation}
+{q_{HX}} = {\left( {UA} \right)_{eff}} \cdot \frac{{\left( {{T_{aux - mix}} - {T_{water,out}}} \right) - \left( {{T_{HX - exh}} - {T_{water,in}}} \right)}}{{\ln \left( {\frac{{{T_{aux - mix}} - {T_{water,out}}}}{{{T_{HX - exh}} - {T_{water,in}}}}} \right)}} + {\dot N_{{H_2}O - cond}} \cdot {\hat h_{fg}}
+\end{equation}
+
+where,
+
+\begin{equation}
+{\dot N_{{H_2}O - cond}} = \left( {{T_{cond - threshold}} - {T_{water,in}}} \right) \cdot \left[ {h{x_{l,1}} \cdot \left( {\frac{{{{\dot N}_{{H_2}O}}}}{{{{\dot N}_{aux - mix}}}}} \right) + h{x_{l,2}} \cdot {{\left( {\frac{{{{\dot N}_{{H_2}O}}}}{{{{\dot N}_{aux - mix}}}}} \right)}^2}} \right]
+\end{equation}
+
+\paragraph{Field: Method 4 hxl2 Coefficient}\label{field-method-4-hxl2-coefficient}
+
+This field describes the value of \(h{x_{l,2}}\) in the relation above for the rate of condensation of water from the gas stream, \({\dot N_{{H_2}O - cond}}\) . This field is only used with the Condensing mode, which corresponds to method 4 in the Annex 42 specification.
+
+\paragraph{Field: Method 4 Condensation Threshold}\label{field-method-4-condensation-threshold}
+
+This field describes the value of \({T_{cond - threshold}}\) in the relation above for the rate of condensation of water from the gas stream, \({\dot N_{{H_2}O - cond}}\) . This field is only used with the Condensing mode, which corresponds to method 4 in the Annex 42 specification.
+
+An example input data file (IDF) entry for this object is provided below:
+
+\begin{lstlisting}
+
+Generator:FuelCell:ExhaustGasToWaterHeatExchanger,
+  FCT SOFC Exhaust HX,         !- Name
+  Small SOFC Heat Rec Inlet Node,   !- Heat Recovery Water Inlet Node Name
+  Small SOFC Heat Rec Outlet Node,   !- Heat Recovery Water Outlet Node Name
+  0.0004,                                   !- Heat Recovery Water Maximum Flow Rate {m3/s}
+  SOFC Air Outlet Node,       !- Exhaust Outlet Air Node Name
+  CONDENSING,                           !- Heat Exchanger Calculation Method
+  ,                                               !- Method 1 Heat Exchanger Effectiveness
+  83.1,                                       !- Method 2 Parameter hxs0
+  4798,                                       !- Method 2 Parameter hxs1
+  -138E+3,                                 !- Method 2 Parameter hxs2
+  -353.8E+3,                             !- Method 2 Parameter hxs3
+  5.15E+8,                                 !- Method 2 Parameter hxs4
+  ,                                               !- Method 3 h0Gas Coefficient
+  ,                                               !- Method 3 NdotGasRef Coefficient
+  ,                                               !- Method 3 n Coefficient
+  ,                                               !- Method 3 Gas Area
+  ,                                               !- Method 3 h0 Water Coefficient
+  ,                                               !- Method 3 N dot Water ref Coefficient
+  ,                                               !- Method 3 m Coefficient
+  ,                                               !- Method 3 Area Water Coefficient
+  ,                                               !- Method 3 F Adjustment Factor
+  -1.96E-4,                               !- Method 4 hxl1 Coefficient
+  3.1E-3,                                   !- Method 4 hxl2 Coefficient
+  35.0;                                       !- Method 4 Condensation Threshold {C}
+\end{lstlisting}
+
+\subsection{Generator:FuelCell:ElectricalStorage}\label{generatorfuelcellelectricalstorage}
+
+This object is used to describe the electrical storage subsystem for the FC. The electrical storage model is a very simple constrained bucket model. Future developments made add additional models for battery systems. Note that this electrical storage is embedded within the FC device.
+
+\subsubsection{Inputs}\label{inputs-17-000}
+
+\paragraph{Field: Name}\label{field-name-20}
+
+This field contains a unique name for the fuel cell electrical storage subsystem.
+
+\paragraph{Field: Choice of Model}\label{field-choice-of-model}
+
+This field is used to direct how EnergyPlus will model electrical storage. The only choice currently available is SimpleEfficiencyWithConstraints, which should be entered in this field. Future developments may expand the number of models available for electrical storage.
+
+\paragraph{Field: Nominal Charging Energetic Efficiency}\label{field-nominal-charging-energetic-efficiency}
+
+This field describes the value of \({\varepsilon_{charge}}\) in the relation for the State of Charge, \(Q_{battery}^{t + \Delta t}\) :
+
+\begin{equation}
+Q_{battery}^{t + \Delta t} = Q_{battery}^t + {P_{battery - charge}} \cdot {\varepsilon_{charge}} \cdot \Delta t
+\end{equation}
+
+This is the energetic efficiency of charging the storage device. A value of 1.0 means that the storage device does not lose any energy when charging. Note that the model can recover the lost energy into the air supply intake.
+
+\paragraph{Field: Nominal Discharging Energetic Efficiency}\label{field-nominal-discharging-energetic-efficiency-1}
+
+This field describes the value of \({\varepsilon_{discharge}}\) in the relation for the State of Charge, \(Q_{battery}^{t + \Delta t}\) :
+
+\begin{equation}
+Q_{battery}^{t + \Delta t} = Q_{battery}^t + \frac{{{P_{battery - discharge}} \cdot \Delta t}}{{{\varepsilon_{discharge}}}}
+\end{equation}
+
+This is the energetic efficiency of discharging the storage device. A value of 1.0 means that the storage device does not lose any energy when discharging. Note that the model can recover the lost energy into the air supply intake.
+
+\paragraph{Field: Simple Maximum Capacity}\label{field-simple-maximum-capacity}
+
+This field describes the maximum amount of electrical energy that can be stored in the device (J).
+
+\paragraph{Field: Simple Maximum Power Draw}\label{field-simple-maximum-power-draw}
+
+This field describes the maximum rate at which electrical power can be discharged from the storage device (W).
+
+\paragraph{Field: Simple Maximum Power Store}\label{field-simple-maximum-power-store}
+
+This field describes the maximum rate at which electrical power can charge the storage device (W).
+
+\paragraph{Field: Initial Charge State}\label{field-initial-charge-state}
+
+This field describes the value for the initial state of charge (J). This allows the storage device to contain some amount of stored electricity at the beginning of the simulation period.
+
+An example input data file (IDF) entry for this object is provided below:
+
+\begin{lstlisting}
+
+Generator:FuelCell:ElectricalStorage,
+  FCT SOFC Battery,               !- Name
+  SimpleEfficiencyWithConstraints,   !- Choice of Model
+  1.0,                                         !- Nominal Charging Energetic Efficiency
+  1.0,                                         !- Nominal Discharging Energetic Efficiency
+  0,                                             !- Simple Maximum Capacity {J}
+  0,                                             !- Simple Maximum Power Draw {W}
+  0,                                             !- Simple Maximum Power Store {W}
+  0;                                             !- Initial Charge State {J}
+\end{lstlisting}
+
+\subsection{Generator:FuelCell:Inverter}\label{generatorfuelcellinverter}
+
+This object is used to describe the power condition unit subsystem of the FC. This object models an inverter system contained within a fuel cell system that converts from direct current (DC) to alternating current (AC).
+
+\subsubsection{Inputs}\label{inputs-18-000}
+
+\paragraph{Field: Name}\label{field-name-21}
+
+This field contains a unique name for the fuel cell inverter subsystem.
+
+\paragraph{Field: Inverter Efficiency Calculation Mode}\label{field-inverter-efficiency-calculation-mode}
+
+This field is used to direct how EnergyPlus will calculate the inverter efficiency. There are two possible choices: Constant or Quadratic .
+
+\paragraph{Field: Inverter Efficiency}\label{field-inverter-efficiency-1}
+
+This field describes the value for inverter efficiency when using the \textbf{Constant} mode.
+
+\paragraph{Field: Efficiency Function of DC Power Curve Name}\label{field-efficiency-function-of-dc-power-curve-name}
+
+This field names a Curve:Quadratic object defined elsewhere in the input file. The curve determines inverter efficiency as a function of the DC power entering the inverter as follows:
+
+\begin{equation}
+{\eta_{PCU}} = {u_0} + {u_1} \cdot {P_{PCU - in}} + {u_2} \cdot P_{PCU - in}^2
+\end{equation}
+
+An example input data file (IDF) entry for this object is provided below:
+
+\begin{lstlisting}
+
+Generator:FuelCell:Inverter,
+  FCT SOFC Inverter,             !- Name
+  Quadratic,                             !- Inverter Efficiency Calculation Mode
+  ,                                               !- Inverter Efficiency
+  FCT Inverter Quadratic;   !- Efficiency Function of DC Power Curve Name
+
+
+  Curve:Quadratic,
+  FCT Inverter Quadratic,   !- Name
+  0.560717,                               !- Coefficient1 Constant
+  1.24019E-4,                           !- Coefficient2 x
+  -2.01648E-8,                         !- Coefficient3 x**2
+  -1.0E+10,                               !- Minimum Value of x
+  1.0E+10;                                 !- Maximum Value of x
+\end{lstlisting}
+
+\subsection{Generator:FuelSupply}\label{generatorfuelsupply}
+
+This object is used to define details of the fuel supply for certain generators. This object allows the user to describe a wide array of possible fuel mixtures. The program contains data and internal methods to calculate the properties of the various mixtures of gaseous fuels. The program will calculate the Lower Heating Value (LHV), Higher Heating Value (HHV), and molecular weight for the fuel mixture. The fuel properties are then use by both fuel cell and Micro CHP models. Results of the gas phase thermochemistry modeling are also reported in the EIO file.
+
+In addition to gaseous mixtures, the Micro CHP model is able to use generic liquid fuels and this object is used to describe the properties.
+
+Note that the fuel consumption metering is currently handled by the Natural Gas meter. So no matter what fuel mixture is defined in this object, the aggregated reports from EnergyPlus meters for (natural) Gas will include the fuel used for the generator (with the Joule content based on HHV).
+
+\subsubsection{Inputs}\label{inputs-19-000}
+
+\paragraph{Field: Name}\label{field-name-22}
+
+This field contains a unique name for the fuel cell fuel supply subsystem.
+
+\paragraph{Field: Fuel Temperature Modeling Mode}\label{field-fuel-temperature-modeling-mode}
+
+This field describes how the model will determine the temperature of the fuel. There are two options for this field to choose from: TemperatureFromAirNode and Scheduled. If this field contains TemperatureFromAirNode then the fuel is modeled as having the same temperature as the air node that is named in the next field. If this field contains Scheduled then the fuel is modeled as having the temperature described in a schedule defined elsewhere in the input file.
+
+\paragraph{Field: Fuel Temperature Reference Node Name}\label{field-fuel-temperature-reference-node-name}
+
+This field contains the name of the air node used to obtain the inlet temperature of the fuel. This field is only used if the Fuel Temperature Modeling Mode is set to TemperatureFromAirNode.
+
+\paragraph{Field: Fuel Temperature Schedule Name}\label{field-fuel-temperature-schedule-name}
+
+This field contains the name of a temperature schedule defined elsewhere in the input file. This field is only used if the Fuel Temperature Modeling Mode is set to Scheduled. The temperature of the fuel inlet will be obtained from the schedule.
+
+\paragraph{Field: Compressor Power Function of Fuel Rate Curve Name}\label{field-compressor-power-function-of-fuel-rate-curve-name}
+
+This field contains the name of a Curve:Cubic input object described elsewhere in the input file. The curve provides the electrical power used by the fuel compressor (W) as a cubic function of the rate of fuel supply (kmol/s).
+
+\begin{equation}
+{P_{comp - el}} = {c_0} + {c_1} \cdot {\dot N_{fuel}} + {c_2} \cdot \dot N_{fuel}^2 + {c_3} \cdot \dot N_{fuel}^3
+\end{equation}
+
+\paragraph{Field: Compressor Heat Loss Factor}\label{field-compressor-heat-loss-factor}
+
+This field describes the portion of the compressor electrical power that is lost to the surroundings. The rest of the energy is added to the fuel stream. A heat loss factor of 1.0 indicates that all the heat is lost to the surroundings and no energy is added to the fuel inlet stream.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-3}
+
+Choose between GaseousConstituents or LiquidGeneric .
+
+\paragraph{Field: Liquid Generic Fuel Lower Heating Value}\label{field-liquid-generic-fuel-lower-heating-value}
+
+For fuel type LiquidGeneric, this field is used to enter the lower heating value of the fuel in units of kJ/kg.
+
+\paragraph{Field: Liquid Generic Fuel Higher Heating Value}\label{field-liquid-generic-fuel-higher-heating-value}
+
+For fuel type LiquidGeneric, this field is used to enter the higher heating value of the fuel in units of kJ/kg.
+
+\paragraph{Field: Liquid Generic Fuel Molecular Weight}\label{field-liquid-generic-fuel-molecular-weight}
+
+For fuel type LiquidGeneric, this field is used to enter the molecular weight of the fuel in units of g/mol.
+
+\paragraph{Field: Liquid Generic Fuel CO2 Emission Factor}\label{field-liquid-generic-fuel-co2-emission-factor}
+
+This field is not used. This part of the Annex 42 model was not implemented in EnergyPlus; see the FuelFactors object.
+
+\paragraph{Field: Number of Constituents in Gaseous Constituent Fuel Supply}\label{field-number-of-constituents-in-gaseous-constituent-fuel-supply}
+
+This field is used to describe the number of constituents in the inlet fuel supply. The maximum number of different types of constituents is currently set to 12.
+
+The remaining fields in this object are repeating pairs of fields with one pair for each constituent and the same number as described in the previous field. The field set pairs consist of the name of the constituent followed by the molar fraction of that constituent.
+
+\paragraph{Field: Constituent 1-12 Name}\label{field-constituent-1-12-name}
+
+These fields describe the fuel stream constituents by name. The name field for each pair must be filled with one of these 14 choices: CarbonDioxide , Nitrogen , Oxygen , Water , Argon , Hydrogen , Methane , Ethane , Propane , Butane , Pentane , Hexane , Methanol , and Ethanol . No other fuel constituents can currently be modeled. The properties of the constituents are already contained inside the program as provided in the Annex 42 model specification.
+
+\paragraph{Field: Constituent 1-12 Molar Fraction}\label{field-constituent-1-12-molar-fraction}
+
+These fields describe the molar fraction of the fuel stream constituents. It is very important that the sum of the molar fractions add up to 1.0.
+
+\subsubsection{Outputs}\label{outputs-10-001}
+
+In addition to the following output variables, the resulting fuel heating values are also reported to the eio file.
+
+HVAC,Average,Generator Fuel Compressor Electric Power {[}W{]}
+
+HVAC,Sum,Generator Fuel Compressor Electric Energy {[}J{]}
+
+HVAC,Average,Generator Fuel Compressor Skin Heat Loss Rate {[}W{]}
+
+\paragraph{Generator Fuel Compressor Electric Power {[}W{]}}\label{generator-fuel-compressor-electric-power-w-1}
+
+This is the rate of energy use by the gas compressor, if any, that provides fuel at a higher pressure.
+
+\paragraph{Generator Fuel Compressor Electric Energy {[}J{]}}\label{generator-fuel-compressor-electric-energy-j-1}
+
+This is the energy used by the gas compressor, if any, that provides fuel at a higher pressure.
+
+\paragraph{Generator Fuel Compressor Skin Heat Loss Rate {[}W{]}}\label{generator-fuel-compressor-skin-heat-loss-rate-w-1}
+
+Convective heat gains to zone from gas compressor, if any, that provides fuel at a higher pressure.
+
+\subsection{Photovoltaic Generators}\label{photovoltaic-generators}
+
+EnergyPlus offers different options for predicting the electricity produced by solar electric photovoltaic (PV) panels. The three different options are Simple , Equivalent One-Diode and Sandia and the choice will determine the mathematical models used to determine energy production. The first allows the user to input an arbitrary efficiency. The other two models use empirical relationships to predict PV operating performance based on many environmental variables such as cell temperature. The PV models can be used with either normal PV modules or as part of a hybrid photovoltaic/thermal (PVT) flat plat collector.
+
+The generator is connected to an Electric Load Center. The PV models refer to surface input objects defined elsewhere in the input file. This object describes an array that is attached to a surface object in order to describe its orientation and to access results of the solar insolation calculations. These can be either Heat Transfer or Shading objects (see Surfaces). This will define the orientation of the solar panel for the detailed models and also the area for the simple model. The exposure of that surface to incident solar radiation is calculated using the full set of models in EnergyPlus that are used to account for solar thermal loads arising from building windows and walls. Therefore the incident solar radiation is calculated to include the effects of shading and reflections from other surfaces declared in the input file. In addition to the output variables associated with PV models, there are numerous related output variables available for the surfaces including: `Surface Outside Face Sunlit Area', `Surface Outside Face Sunlit Fraction', `Surface Outside Face Incident Solar Radiation Rate per Area', `Surface Outside Face Incident Beam Solar Radiation Rate per Area', `Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area', `Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area', `Surface Outside Face Beam Solar Incident Angle Cosine Value', `Surface Outside Face Incident Sky Diffuse Ground Reflected Solar Radiation Rate per Area', `Surface Outside Face Incident Sky Diffuse Surface Reflected Solar Radiation Rate per Area', `Surface Outside Face Incident Beam To Beam Reflected From Surfaces Solar Radiation Rate per Area', `Surface Outside Face Incident Beam To Diffuse Surface Reflected Solar Radiation Rate per Area', and 'Surface Outside Face Incident Beam To Diffuse Ground Reflected Solar Radiation Rate per Area. Note that it is possible to define a PV array area that doesn t conform to the surface area (i.e.~model a PV array area that is larger or smaller than what is available on the surface) so it is the users responsibility to not over-specify area when determining how many modules will fit onto a surface. However this type of input is allowed.
+
+EnergyPlus does not include models for ancillary equipment for a PV array including charge controllers or power-point trackers. The operation of the entire electrical system that must go along with a PV array is not currently modeled in EnergyPlus and is therefore assumed to operate in ideal ways. The PV production models do not resolve voltage and current, only power (and energy). Electricity production is metered based on the output of the inverter. Output results are available before and after the inverter. One assumption is that the array is assumed to be always operating at the maximum power point. Energy production is based on the assumption that the quasi-steady power prediction is constant and continuous over the simulation timestep.
+
+For a variety of reasons, actual installations of photovoltaics are often observed to exhibit system-level problems that significantly reduce electricity production. Therefore this modeling should be considered a method of bracketing the upper end of electricity production rather than an accurate prediction of what the panels will produce. Also note that the model predictions are closely related to the solar radiation data (typically of of TMY2 origin) in the EnergyPlus weather file, that the solar data in these is usually from a model rather than direct measurements, and that solar resources encountered by a real installation in a given year are likely to differ from the weather data file.
+
+\subsection{Generator:Photovoltaic}\label{generatorphotovoltaic-000}
+
+This object is used to describe an array of PV modules and how they are to be modeled. A series of different PV arrays can be connected to a single electric load center (and inverter) by listing them all in an ElectricLoadCenter:Generator object.
+
+\subsubsection{Inputs}\label{inputs-20-000}
+
+\paragraph{Field: Name}\label{field-name-23}
+
+This field is a unique name for the PV array.
+
+\paragraph{Field: Surface Name}\label{field-surface-name-001}
+
+This field is the name of a surface that defines the location and geometry of the array.
+
+\paragraph{Field: Photovoltaic Performance Object Type}\label{field-photovoltaic-performance-object-type}
+
+This field is the type of PV performance model. The choices are the class names for the three modeling options:
+
+\begin{itemize}
+\item
+  PhotovoltaicPerformance:Simple
+\item
+  PhotovoltaicPerformance:EquivalentOne-Diode
+\item
+  PhotovoltaicPerformance:Sandia.
+\end{itemize}
+
+\paragraph{Field: Module Performance Name}\label{field-module-performance-name}
+
+This is the name of the PV performance object define elsewhere (corresponding to the object type listed in the previous field)
+
+\paragraph{Field: Heat Transfer Integration Mode}\label{field-heat-transfer-integration-mode}
+
+The PV model allows for different ways of integrating with other EnergyPlus heat transfer surfaces and models and calculating cell temperature. For Building Integrated PV (BIPV), the Integrated options allow for the PV modeling to be coupled to the surface heat transfer models elsewhere in EnergyPlus. The user must select one of these options for this field:
+
+\begin{itemize}
+\item
+  \textbf{Decoupled.} The cell temperature of modules in the array is computed based on a energy balance relative to NOCT conditions. The input fields for Module Heat Capacity and Module Heat Loss Coefficient are ignored.
+\item
+  \textbf{DecoupledUllebergDynamic} the cell temperature is calculated based on a dynamic model developed by Ulleberg\protect\hyperlink{ux5fftn1}{{[}1{]}}. The input fields for Module Heat Capacity and Module Heat Loss Coefficient are required.
+\item
+  \textbf{IntegratedSurfaceOutsideFace} The cell temperature is obtained from the outside face of the Surface:Heat Transfer named in the previous field. Energy exported by the module is removed from the heat transfer surface (at the position determined by the associated Construction with Internal Source). The input fields for Module Heat Capacity and Module Heat Loss Coefficient are ignored.
+\item
+  \textbf{IntegratedTranspiredCollector} The cell temperature is obtained from the collector surface temperature in the unglazed transpired collector model. Energy exported by the module is removed from the collector surface. The input fields for Module Heat Capacity and Module Heat Loss Coefficient are ignored.
+\item
+  \textbf{IntegratedExteriorVentedCavity} The cell temperature is obtained from the exterior baffle temperature in the naturally ventilated exterior cavity model. Energy exported by the module is removed from the exterior baffle surface. The input fields for Module Heat Capacity and Module Heat Loss Coefficient are ignored.
+\item
+  \textbf{PhotovoltaicThermalSolarCollector} The cell temperature is obtained from the photovoltaic/thermal solar collector model. If the PV layer is inside the collector, then the incident solar is modified by the photovoltaic/thermal solar collector model.
+\end{itemize}
+
+\paragraph{Field: Number of Series Strings in Parallel}\label{field-number-of-series-strings-in-parallel}
+
+This field is the number of series-wired strings of PV modules that are in parallel to form the PV array. The product of this field and the next field should equal the total number of modules in the array.
+
+\paragraph{Field: Number of Modules in Series}\label{field-number-of-modules-in-series}
+
+This field is the number of modules wired in series (on each string) to form the PV array. The product of this field and the previous field should equal the total number of modules in the array.
+
+\subsubsection{Outputs}\label{outputs-11-001}
+
+Using the Generator:PV:Simple object makes a number of output variables available.\textbackslash{}
+
+\begin{itemize}
+\item
+  HVAC,Average,Generator Produced DC Electric Power {[}W{]}
+\item
+  HVAC,Sum,Generator Produced DC Electric Energy {[}J{]}
+\item
+  HVAC,Average,Generator PV Cell Temperature {[}C{]}
+\item
+  HVAC,Average,Generator PV Short Circuit Current {[}A{]}
+\item
+  HVAC,Average,Generator PV Open Circuit Voltage {[}V{]}
+\item
+  HVAC,Average,Generator PV Array Efficiency {[]}
+\end{itemize}
+
+\paragraph{Generator Produced DC Electric Power {[}W{]}}\label{generator-produced-dc-electric-power-w-2}
+
+This output variable is the power of DC electricity produced by the PV array in Watts..
+
+\paragraph{Generator Produced DC Electric Energy {[}J{]}}\label{generator-produced-dc-electric-energy-j}
+
+This output variable is the energy in DC electricity produced by the PV array, in Joules.
+
+\paragraph{\texorpdfstring{Generator PV Array Efficiency {[]}}{Generator PV Array Efficiency }}\label{generator-pv-array-efficiency}
+
+This output variable is the resulting efficiency of the PV array .
+
+The two more detailed PV models also have the following output variables.
+
+\paragraph{Generator PV Cell Temperature {[} °C{]}}\label{generator-pv-cell-temperature-c}
+
+This output variable represents the temperature of the solar cell used in the calculation of cell performance.
+
+\paragraph{Generator PV Short Circuit Current {[}A{]}}\label{generator-pv-short-circuit-current-a}
+
+This output variable represents the short circuit current of the PV array, in Amps. This is provided to describe the I-V characteristics.
+
+\paragraph{Generator PV Open Circuit Voltage {[}V{]}}\label{generator-pv-open-circuit-voltage-v}
+
+This output variable represents the open circuit voltage of the PV array, in Volts. This is provided to describe the I-V characteristics.
+
+\subsection{PhotovoltaicPerformance:Simple}\label{photovoltaicperformancesimple}
+
+The PhotovoltaicPerformance:Simple object describes a simple model of photovoltaics that may be useful for early phase design analysis. In this model the user has direct access to the efficiency with which surfaces convert incident solar radiation to electricity and need not specify arrays of specific modules. The full geometric model for solar radiation is used, including shading and reflections, to determine the incident solar resource. This model is intended to be useful for design purposes to quickly get an idea of the levels for annual production and peak power. The model can also accept arbitrary conversion efficiencies and does not require actual production units be tested to obtain performance coefficients.
+
+\subsubsection{Inputs}\label{inputs-21-000}
+
+\paragraph{Field: Name}\label{field-name-24}
+
+This field is the name of the PV array. The name is only used as an identifier. Multiple instances need have unique names.
+
+\paragraph{Field: Fraction of Surface Area with Active Solar Cells}\label{field-fraction-of-surface-area-with-active-solar-cells}
+
+This field is the user defined fraction for the area of surface named in the parent PV object that will have active PV cells on it. The area actually covered with solar cells will be the net area of the surface (gross area less any subsurfaces like windows) times the fraction entered here. This fraction includes the difference between PV module area and active cells within it and any losses for how closely packed modules can be arranged on surface. The value should be between 0.0 and 1.0.
+
+\paragraph{Field: Conversion Efficiency Input Mode}\label{field-conversion-efficiency-input-mode}
+
+This field specifies how the PV array efficiency values are input. There are two choices, \textbf{Fixed} and \textbf{Scheduled}. If this field is set to Fixed then the PV array always has the efficiency value specified in the next field. If this field is set to Scheduled then the efficiency is determined by a user defined schedule named in the second field to follow.
+
+\paragraph{Field: Value for Cell Efficiency if Fixed}\label{field-value-for-cell-efficiency-if-fixed}
+
+This field specifies the efficiency with which solar incident energy is converted to electricity. Efficiency = (electrical power generated {[}W{]})/(power of incident solar{[}W{]}). These efficiency values are dimensionless and should be between 0.0 and 1.0.
+
+\paragraph{Field: Efficiency Schedule Name}\label{field-efficiency-schedule-name}
+
+This field should be set to the name of schedule defined elsewhere in the input file. This schedule should specify dimensionless efficiency values between 0.0 and 1.0. This could be used for example to vary the efficiency to match results computed with more detailed models.
+
+An example idf instance of this object follows:
+
+\begin{lstlisting}
+
+PhotovoltaicPerformance:Simple,
+  Simple PV Flat, !- Name
+  0.1044 , !- Fraction of Surface area that has active solar cells
+  FIXED ,   !- Conversion efficiency input mode
+  0.12 ,     !- Value for cell efficiency if fixed
+  ;           !- Name of Schedule that Defines Efficiency
+\end{lstlisting}
+
+\subsection{PhotovoltaicPerformance:EquivalentOne-Diode}\label{photovoltaicperformanceequivalentone-diode}
+
+This object describes the performance characteristics of Photovoltaic (PV) modules to be modeled using an equivalent one-diode circuit. This model is also known at the 4- or 5-parameter TRNSYS model for photovoltaics.
+
+The following table shows several sample PV array types with their input values.
+
+% table 33
+\begin{longtable}[c]{p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}p{0.6in}}
+\caption{Photovoltaics Array Types with Values \label{table:photovoltaics-array-types-with-values}} \tabularnewline
+\toprule 
+ & Short Circuit Current & Open Circuit Voltage & Voltage at Maximum Power & Current at Maximum Power & Temperature Coefficient of Short Circuit Current & Temperature Coefficient of Open Circuit Voltage & Number of Cells in Series per Module & Cell Temperature at NOCT Conditions & Module Area \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Photovoltaics Array Types with Values} \tabularnewline
+\toprule 
+ & Short Circuit Current & Open Circuit Voltage & Voltage at Maximum Power & Current at Maximum Power & Temperature Coefficient of Short Circuit Current & Temperature Coefficient of Open Circuit Voltage & Number of Cells in Series per Module & Cell Temperature at NOCT Conditions & Module Area \tabularnewline
+\midrule
+\endhead
+
+Units: & [A] & [V] & [V] & [A] & \{A/K] & [V/K] & [-] & [K] & [m2] \tabularnewline
+ASE 300-DFG/50 & 6.2 & 60 & 50.5 & 5.6 & 0.001 & -0.0038 & 216 & 318 & 2.43 \tabularnewline
+BPsolar 275 & 4.75 & 21.4 & 17 & 4.45 & 0.00065 & -0.08 & 36 & 320 & 0.63 \tabularnewline
+BPsolar 3160 & 4.8 & 44.2 & 35.1 & 4.55 & 0.00065 & -0.16 & 72 & 320 & 1.26 \tabularnewline
+BPsolar 380 & 4.8 & 22.1 & 17.6 & 4.55 & 0.00065 & -0.08 & 36 & 320 & 0.65 \tabularnewline
+BPsolar 4160 & 4.9 & 44.2 & 35.4 & 4.52 & 0.00065 & -0.16 & 72 & 320 & 1.26 \tabularnewline
+BPsolar 5170 & 5 & 44.2 & 36 & 4.72 & 0.00065 & -0.16 & 72 & 320 & 1.26 \tabularnewline
+BPsolar 585 & 5 & 22.1 & 18 & 4.72 & 0.00065 & -0.08 & 36 & 320 & 0.65 \tabularnewline
+Shell SM110-12 & 6.9 & 21.7 & 17.5 & 6.3 & 0.0028 & -0.076 & 36 & 318 & 0.86856 \tabularnewline
+Shell SM110-24 & 3.45 & 43.5 & 35 & 3.15 & 0.0014 & -0.152 & 72 & 318 & 0.86856 \tabularnewline
+Shell SP70 & 4.7 & 21.4 & 16.5 & 4.25 & 0.002 & -0.076 & 36 & 318 & 0.6324 \tabularnewline
+Shell SP75 & 4.8 & 21.7 & 17 & 4.4 & 0.002 & -0.076 & 36 & 318 & 0.6324 \tabularnewline
+Shell SP140 & 4.7 & 42.8 & 33 & 4.25 & 0.002 & -0.152 & 72 & 318 & 1.320308 \tabularnewline
+Shell SP150 & 4.8 & 43.4 & 34 & 4.4 & 0.002 & -0.152 & 72 & 318 & 1.320308 \tabularnewline
+Shell S70 & 4.5 & 21.2 & 17 & 4 & 0.002 & -0.076 & 36 & 317 & 0.7076 \tabularnewline
+Shell S75 & 4.7 & 21.6 & 17.6 & 4.2 & 0.002 & -0.076 & 36 & 317 & 0.7076 \tabularnewline
+Shell S105 & 4.5 & 31.8 & 25.5 & 3.9 & 0.002 & -0.115 & 54 & 317 & 1.037 \tabularnewline
+Shell S115 & 4.7 & 32.8 & 26.8 & 4.2 & 0.002 & -0.115 & 54 & 317 & 1.037 \tabularnewline
+Shell ST40 & 2.68 & 23.3 & 16.6 & 2.41 & 0.00035 & -0.1 & 16 & 320 & 0.424104 \tabularnewline
+UniSolar PVL-64 & 4.8 & 23.8 & 16.5 & 3.88 & 0.00065 & -0.1 & 40 & 323 & 0.65 \tabularnewline
+UniSolar PVL-128 & 4.8 & 47.6 & 33 & 3.88 & 0.00065 & -0.2 & 80 & 323 & 1.25 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Where:
+
+\begin{itemize}
+\item
+  Shunt Resistance: the value of shunt resistance is finite only if the PV Module being modeled is a thin film variety. For all crystaline silicon modules the value is essentially infinite
+\item
+  Shunt Resistance value: 1,000,000 W (ohms)
+\item
+  Module Heat Loss Coefficient: this value is dependent more on the array configuration than on the module itself.
+\item
+  Module Heat Loss Coefficient value: 30 W/m2-K
+\item
+  Module Heat Capacity: this is a typical value for a silicon based sandwich construction framed PV panel.
+\item
+  Module Heat Capacity Value: 50,000 J/m2-K
+\item
+  Reference Temperature: 298K (25C)
+\item
+  Insolation at Reference Conditions: 1000 W/m2
+\item
+  Ambient Temperature at NOCT conditions: 293K (20C)
+\item
+  Insolation at NOCT Conditions: 800 W/m2
+\item
+  Average tau-alpha Product: .9
+\item
+  Semiconductor Bandgap: 1.12 eV
+\end{itemize}
+
+\subsubsection{Field: Name}\label{field-name-25}
+
+This field contains the uniqe name for the photovoltaic module performance data. The name is only used as an identifier.
+
+\subsubsection{Field: Cell Type}\label{field-cell-type}
+
+This field is used to describe the type of technology used in the PV module. There are two options available, \textbf{CrystallineSilicon} and \textbf{AmorphousSilicon}. The choice affects the modeling.
+
+\subsubsection{Field: Number of Cells in Series}\label{field-number-of-cells-in-series}
+
+This field is an integer representing the number of individual cells wired in series to make up a single module. The typical number for a 12V crystalline silicon PV module is 36.
+
+\subsubsection{Field: Active Area}\label{field-active-area}
+
+This field is the active area of the PV module in m\(^{2}\).
+
+\subsubsection{Field: Transmittance Absorptance Product}\label{field-transmittance-absorptance-product}
+
+This field indicates the transmittance-absorptance product at normal incidence angles for the PV modules. If the ta product is positive, that value will be used for all angles of incidence. If the value specified is negative, then the magnitude of the given value will be used for normal incidence and the IAM modifier correlation will be used for all other angles.
+
+\subsubsection{Field: Semiconductor Bandgap}\label{field-semiconductor-bandgap}
+
+This field is the semiconductor bandgap for the PV material. The bandgap for silicon is 1.12 eV (electron volts).
+
+\subsubsection{Field: Shunt Resistance}\label{field-shunt-resistance}
+
+This field is the shunt (parallel) resistance (in W) in the single diode electrical model of the PV. The shunt resistance is effectively infinite for crystalline silicon based PV modules and is finite for thin film and exotic metal modules.
+
+\subsubsection{Field: Short Circuit Current}\label{field-short-circuit-current}
+
+This field is the short circuit current (in Amps) for an individual module in the PV array at reference conditions.
+
+\subsubsection{Field: Open Circuit Voltage}\label{field-open-circuit-voltage}
+
+This field is the open circuit voltage (in Volts) for an individual module in the PV array at reference conditions.
+
+\subsubsection{Field: Reference Temperature}\label{field-reference-temperature-000}
+
+This field is the ambient temperature (in Kelvin) at reference conditions. The value is usually 298K
+
+\subsubsection{Field: Reference Insolation}\label{field-reference-insolation}
+
+This field is the radiation level (in W/m\(^{2}\)) at reference conditions. The value is usually 1000 W/m\(^{2}\).
+
+\subsubsection{Field: Module Current at Maximum Power}\label{field-module-current-at-maximum-power}
+
+This field is module current (in Amps) at the maximum power point and reference conditions.
+
+\subsubsection{Field: Module Voltage at Maximum Power}\label{field-module-voltage-at-maximum-power}
+
+This field is module voltage (in Volts) at the maximum power point and reference conditions.
+
+\subsubsection{Field: Temperature Coefficient of Short Circuit Current}\label{field-temperature-coefficient-of-short-circuit-current}
+
+This field accounts for the fact that the module short circuit current is temperature dependent. The coefficient is given in Amps/Kelvin.
+
+\subsubsection{Field: Temperature Coefficient of Open Circuit Voltage}\label{field-temperature-coefficient-of-open-circuit-voltage}
+
+This field accounts for the fact that the module open circuit voltage is temperature dependent. The coefficient is given in Volts/Kelvin.
+
+\subsubsection{Field: Nominal Operating Cell Temperature Test Ambient Temperature}\label{field-nominal-operating-cell-temperature-test-ambient-temperature}
+
+This field is the ambient temperature (in Kelvin) from the Nominal Operating Cell Temperature (NOCT) test. The value is usually 293 K
+
+\subsubsection{Field: Nominal Operating Cell Temperature Test Cell Temperature}\label{field-nominal-operating-cell-temperature-test-cell-temperature}
+
+This field is the cell temperature (in Kelvin) from the Nominal Operating Cell Temperature (NOCT) test.
+
+\subsubsection{Field: Nominal Operating Cell Temperature Test Insolation}\label{field-nominal-operating-cell-temperature-test-insolation}
+
+This field is the insolation level (in W/m\(^{2}\)) from the Nominal Operating Cell Temperature (NOCT) test. The value is usually 800 W/m\(^{2}\).
+
+\subsubsection{Field: Module Heat Loss Coefficient}\label{field-module-heat-loss-coefficient}
+
+This field is the heat loss coefficient (in W/m\(^{2}\).K) for the array. The heat loss coefficient is dependent upon measures taken to actively or passively promote airflow over the array surface. The heat loss coefficient value is used only if the Integration and Cell Temperature Mode is set to Decoupled Ulleberg Dynamic.
+
+\subsubsection{Field: Total Heat Capacity}\label{field-total-heat-capacity}
+
+This field is the heat capacity (in J/m\(^{2}\).K) of the modules in the array. It describes the module s ability to store incident solar radiation internally. Such energy storage is manifested as a temperature increase in the modules that is considered to be undesirable. The total heat capacity value is used only if the Integration and Cell Temperature Mode is set to Decoupled Ulleberg Dynamic.
+
+An IDF example:
+
+\begin{lstlisting}
+
+PhotovoltaicPerformance:EquivalentOne-Diode,
+  Siemens, ! Name
+  CrystallineSilicon, !cell Type
+  36,           !cells in series [-]
+  1.0,         !module area [m2]
+  0.9,         !tau alpha product at normal incidence [-]
+  1.12,       !electron bandgap [eV]
+  1000000, !shunt resistance [ohms]
+  6.5,         !short circuit current at reference conditions [A/K]
+  21.6,       !open circuit voltage at reference conditions [V/K]
+  25,           !temperature at reference conditions [C]
+  1000,       !radiation at reference conditions [W/m2]
+  5.9,         !current at max power
+  17,           !voltage at max power
+  0.002,     !temperature coefficient of short circuit current
+  -0.079,   !temperature coefficient of open circuit voltage
+  20,           !ambient temperature at NOCT [C]
+  45,           !cell temperature at NOCT [C]
+  800,         !radiation at NOCT [W/m2]
+  30,           !heat loss coefficient [W/m2.K]
+  50000;     !total heat capacity (only used in TC mode 1)
+\end{lstlisting}
+
+\subsection{PhotovoltaicPerformance:Sandia}\label{photovoltaicperformancesandia}
+
+This PhotovoltaicPerformance:Sandia object describes the performance of a single type of module. The model used with this object for predicting the electricity generated by photovoltaics is referred to as the Sandia model. This model is based on work done at Sandia National Lab, Albuquerque, NM by David King -- with the help of many others.
+
+This object describes performance input data needed for specific makes and models of production PV panels using the empirical coefficients assembled by Sandia National Laboratory. There are a large number of empirical coefficients required to use the Sandia model. These data are obtained after extensive measurements and data reduction. This testing has been performed for some types of production panels and Sandia publishes a database of module and array performance parameters on the web at www.sandia.gov/pv. The entries in the database as of January 15, 2004 were converted to idf segments and are included with the EnergyPlus release in the library file SandiaPVData.imf. There are more than hundred different module types included in the library and identified by the manufacturer s model names listed at the beginning of the file SandiaPVData.imf. This data library file is arranged for use with EpMacro but the user can also copy .idf segments directly from the macro data set.
+
+The Sandia model itself can aggregate multiple PV modules. Therefore, an instance of a PhotovoltaicPerformance:Sandia object could actually represent an array of modules as well as the more usual single module. These can be can be thought of as simple larger modules and used by Generator:PV:Sandia objects in the usual manner.
+
+The many empirical coefficients for the model are listed below and are described in more more detail in the EnergyPlus engineering documentation EngineeringDoc.pdf.
+
+The field descriptions below focus on providing the parameter s variable name as identified in the Sandia database. See the the EngineeringDoc.pdf for details on how the input fields are used in the correlations. The user generally would not need to worry about the details of the fields since he/she is not likely to generate the data on their own.
+
+\subsubsection{Inputs}\label{inputs-22}
+
+\paragraph{Field: Name}\label{field-name-26}
+
+This field provides a unique name for the PV module. This is often the manufacturer s identifier for a particular model of a PV module.
+
+\paragraph{Field: Active Area}\label{field-active-area-1}
+
+Units m\(^{2}\) , real number, area of active solar electric cell for the entire module.
+
+\paragraph{Field: Number of Cells in Series}\label{field-number-of-cells-in-series-1}
+
+Series\_Cells in Sandia Database.
+
+\paragraph{Field: Number of Cells in Parallel}\label{field-number-of-cells-in-parallel}
+
+Parallel\_Cells in Sandia Database
+
+\paragraph{Field: Short-Circuit Current}\label{field-short-circuit-current-1}
+
+Isco in Sandia Database. Short-circuit current is a basic parameter Typically supplied by manufacturers at Standard Report Conditions. (Amps)
+
+\paragraph{Field: Open-Circuit Voltage}\label{field-open-circuit-voltage-1}
+
+Voco in Sandia Database, Open-circuit voltage is a basic parameter typically provided by manufacturers a t Standard Report Conditions. (Volts)
+
+\paragraph{Field: Current at Maximum Power Point}\label{field-current-at-maximum-power-point}
+
+Impo in Sandia Database. Current at maximum powerpoint is a basic parameter provided by manufacturers at Standard Report Conditions. (Amps)
+
+\paragraph{Field: Voltage at Maximum PowerPoint}\label{field-voltage-at-maximum-powerpoint}
+
+Vmpo in Sandia Database. Voltage at maximum powerpoint is a a basic parameter typically provided by manufacturers a t Standard Report Conditions. (Volts)
+
+\paragraph{Field: Sandia Database Parameter aIsc}\label{field-sandia-database-parameter-aisc}
+
+aIsc in Sandia Database (1/degC)
+
+\paragraph{Field: Sandia Database Parameter aImp}\label{field-sandia-database-parameter-aimp}
+
+aImp in Sandia Database (1/degC)
+
+\paragraph{Field: Sandia Database Parameter c0}\label{field-sandia-database-parameter-c0}
+
+C0 in Sandia Database, (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter c1}\label{field-sandia-database-parameter-c1}
+
+C1 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter Bvoc0}\label{field-sandia-database-parameter-bvoc0}
+
+Bvoco in Sandia Database (Volts/degC)
+
+\paragraph{Field: Sandia Database Parameter mBVoc}\label{field-sandia-database-parameter-mbvoc}
+
+mBVoc in Sandia Database (Volts/degC)
+
+\paragraph{Field: Sandia Database Parameter BVmp0}\label{field-sandia-database-parameter-bvmp0}
+
+Bvmpo in Sandia Database (Volts/degC)
+
+\paragraph{Field: Sandia Database Parameter mBVmp}\label{field-sandia-database-parameter-mbvmp}
+
+mBVmp in Sandia Database (Volts/degC)
+
+\paragraph{Field:Diode Factor}\label{fielddiode-factor}
+
+n in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter c2}\label{field-sandia-database-parameter-c2}
+
+C2 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter c3}\label{field-sandia-database-parameter-c3}
+
+C3 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter a0}\label{field-sandia-database-parameter-a0}
+
+A0 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter a1}\label{field-sandia-database-parameter-a1}
+
+A1 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter a2}\label{field-sandia-database-parameter-a2}
+
+A2 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter a3}\label{field-sandia-database-parameter-a3}
+
+A3 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter a4}\label{field-sandia-database-parameter-a4}
+
+A4 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter b0}\label{field-sandia-database-parameter-b0}
+
+B0 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter b1}\label{field-sandia-database-parameter-b1}
+
+B1 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter b2}\label{field-sandia-database-parameter-b2}
+
+B2 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter b3}\label{field-sandia-database-parameter-b3}
+
+B3 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter b4}\label{field-sandia-database-parameter-b4}
+
+B4 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter b5}\label{field-sandia-database-parameter-b5}
+
+B5 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter Delta(TC)}\label{field-sandia-database-parameter-deltatc}
+
+d(Tc) in Sandia Database (deg C)
+
+\paragraph{Field: Sandia Database Parameter fd}\label{field-sandia-database-parameter-fd}
+
+fd in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter a}\label{field-sandia-database-parameter-a}
+
+a in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter b}\label{field-sandia-database-parameter-b}
+
+b in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter c4}\label{field-sandia-database-parameter-c4}
+
+C4 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter c5}\label{field-sandia-database-parameter-c5}
+
+C5 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter Ix0}\label{field-sandia-database-parameter-ix0}
+
+Ix0 in Sandia Database (Amps)
+
+\paragraph{Field: Sandia Database Parameter Ixx0}\label{field-sandia-database-parameter-ixx0}
+
+Ixx0 in Sandia Database (Amps)
+
+\paragraph{Field: Sandia Database Parameter c6}\label{field-sandia-database-parameter-c6}
+
+C6 in Sandia Database (non-dimensional)
+
+\paragraph{Field: Sandia Database Parameter c7}\label{field-sandia-database-parameter-c7}
+
+C7 in Sandia Database (non-dimensional)
+
+An example of the object follows:
+
+\begin{lstlisting}
+
+PhotovoltaicPerformance:Sandia,
+  ASE-50-ATF-17_45, ! Module Name (production Name)
+  0.43, ! field Active Area Acoll {m2}, single module
+  36, ! NcellSer {unitless}
+  1, ! NparSerCells
+  2.90, ! Isc0 {Amps}
+  20.70, ! Voc0 {Volts}
+  2.65, ! Imp0 {Amps}
+  17.00, ! Vmp0 {Volts}
+  7.8e-04, ! aIsc {1/degC}
+  1.0e-04, ! aImp {1/degC}
+  0.99, ! C0 {unitless}
+  3.0e-03, ! C1 {unitless}
+  -0.07, ! BVoc0 {Volts/degC}
+  0.00, ! mBVoc {Volts/degC}
+  -0.07, ! BVmp0 {Volts/degC}
+  0.00, ! mBVmp {Volts/degC}
+  1.29, ! Diode Factor (n) {Unitless}
+
+
+  0.20, ! C2 {Unitless}
+  -8.60, ! C3 {Unitless}
+  0.93, ! A0 {Unitless}
+  0.05, ! A1 {Unitless}
+  -7.9402e-03, ! A2 {Unitless}
+  5.2228e-04, ! A3 {Unitless}
+  -1.3142e-05, ! A4 {Unitless}
+  1.00, ! B0 {Unitless}
+  -2.438e-03, ! B1 {Unitless}
+  3.103e-04, ! B2 {Unitless}
+  -1.246e-05, ! B3 {Unitless}
+  2.112e-07, ! B4 {Unitless}
+  -1.359e-09, ! B5 {Unitless}
+  3.00, ! dT0 {degC}
+  1.00, ! fd {Unitless}
+  -3.47, ! a {Unitless}
+  -0.05, ! b {Unitless}
+  0.98, ! C4 {Unitless}
+  0.01, ! C5 {Unitless}
+  2.86, ! Ix0 {Amps}
+  1.85, ! Ixx0 {Amps}
+  1.13, ! C6 {Unitless}
+  -0.13, ! C7 {Unitless}
+  -1.359e-09, ! B5 {Unitless}
+  3.00, ! dT0 {degC}
+  1.00; ! fd {Unitless}
+\end{lstlisting}
+
+When using EpMacro with an typical installation of EnergyPlus, the above entry can be included in an input file by adding the following two lines to an input macro file (*.imf).
+
+\#\#include C:\textbackslash{}EnergyPlus\textbackslash{}MacroDataSets\textbackslash{}SandiaPVdata.imf ASE-50-ATF-17\_45{[]}
+
+\subsection{Generator:WindTurbine}\label{generatorwindturbine}
+
+A wind turbine is a component that converts the kinetic energy of the surrounding airstream into electricity. This model is intended to calculate the electrical power that a wind turbine system produces. The performance of wind turbine systems is dependent on the local environmental conditions such as wind speed and density of air at the height of the systems. An analysis of these conditions is necessary to accurately estimate power output. The model obtains the weather information from the weather data file in EnergyPlus and then determines the wind speed and air density at the specific height of the system. It also requires the user to input the annual average wind speed measured at the local site and the height of the measurement so that it factors in differences between the weather file wind data and the local wind data.
+
+The model employs the general kinetic energy equation to calculate the performance characteristics of the horizontal axis wind turbine (HAWT) systems. It provides a simple approximation algorithm when the power coefficient, Cp, is available which represents the efficiency of the wind turbine in the wind power extraction from the ambient air stream. It also allows the user to input experimental constants so that the power coefficient can precisely be determined according to the characteristic of the airfoil of the system. As for the vertical axis wind turbine (VAWT) systems, it employs the general mathematical equations for straight-bladed Darrieus-type VAWT systems, which are common to VAWT systems. Various types of VAWT systems such as the Savonius-type and the curved-blade (or Egg-beater) type may be simulated with this same model.
+
+It includes two different types of dynamic power control: FixedSpeedFixedPitch (FSFP) and VariableSpeedFixedPitch (VSFP). Currently, it does not include an algorithm for modeling pitch control such as FixedSpeedVariablePitch (FSVP) and VariableSpeedVariablePitch (VSVP). If the control type of the wind turbine is either FSVP or VSVP, the control type of VSFP will be assumed. In addition, constant power generation is assumed when the ambient wind speed is between the rated wind speed and the cut out wind speed, if the user specifies one of the last three options. The model also has the ability to account for transient losses associate with the power produced during dynamic control by a user-specified fraction.
+
+The model does not include detailed algorithms for generators and inverters due to concerns for computational convergence, time, and usability. Instead, all conversion losses of these subsystems are included by applying a user-supplied total system efficiency to the maximum power extraction of the wind turbine. The field of the total system efficiency must be specified by the user.
+
+\subsubsection{Inputs}\label{inputs-23}
+
+\paragraph{Field: Name}\label{field-name-27}
+
+A unique user assigned name for a particular wind turbine system. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-8-000}
+
+The name of the schedule (ref: Schedule) that denotes whether the wind turbine system can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit is off and will not operate for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Rotor Type}\label{field-rotor-type}
+
+This field is the type of axis of the wind turbine. The user specifies either a horizontal axis wind turbine or a vertical axis wind turbine. Each type of wind turbine employs a different algorithm for the calculation of the electrical power output of the wind turbine. The default value is HorizontalAxisWindTurbine.
+
+\paragraph{Field: Power Control}\label{field-power-control}
+
+This field is the type of rotor control for the wind turbine. This protects the system against the overloading for a system with no speed or pitch control and also to maximize the energy yield for the system. Four different control types are classified in the literature: FixedSpeedFixedPitch (FSFP), FixedSpeedVariablePitch (FSVP), VariableSpeedFixedPitch (VSFP), and VariableSpeedVariablePitch (VSVP). Currently, FSFP and VSFP types can be modeled in EnergyPlus. The other two types will be modeled as VSFP. If the first FSFP control type is chosen, the model assumes the maximum power at a fixed rotor speed when the power output predicted is greater than the maximum until the rotor speed reaches the maximum wind speed (see next field). If one of the last three control options is chosen, the model assumes that the system produces a constant power at the rated wind speed when the wind speed is between the rated wind speed and cut-out wind speed. The default value is VariableSpeedFixedPitch (VSFP).
+
+\paragraph{Field: Rated Rotor Speed}\label{field-rated-rotor-speed}
+
+This field is the maximum rotational speed of the rotor at the rated power of the wind turbine in rev/min (revolution per minute). It is used to determine the tip speed ratio of the rotor and relative flow velocity incident on a single blade of the VAWT systems.
+
+\paragraph{Field: Rotor Diameter}\label{field-rotor-diameter}
+
+This field is the diameter of the rotor in meters. Note that this field is not the height of the blade, but the diameter of the perpendicular circle from the vertical pole in the VAWT systems. It determines the swept area of the rotor of the HAWT systems and the chordal velocity of the VAWT systems.
+
+\paragraph{Field: Overall Height}\label{field-overall-height}
+
+This field is the height of the hub of the HAWT system, or of the pole of the VAWT system in meters. It is necessary to estimate local air density and the wind speed at this particular height where the wind turbine system is installed.
+
+\paragraph{Field: Number of Blades}\label{field-number-of-blades}
+
+This field is the number of blades of the wind turbine. The azimuth angle of the rotor of the VAWT system is determined by dividing 360 degree by this field so that the model determines the chordal velocity component and the normal velocity component of the system. The default value is 3.
+
+\paragraph{Field: Rated Power}\label{field-rated-power}
+
+This field is the nominal power output of the wind turbine system at the rated wind speed in Watts. Note that the user should input the maximum power of the system with no control, i.e., FSFP control type, can physically produce. Manufacturers data also indicates it as peak power or rated capacity . If the local wind speed is greater than the rated wind speed, the model assumes constant power output of this field.
+
+\paragraph{Field: Rated Wind Speed}\label{field-rated-wind-speed}
+
+This field is the wind speed that the wind turbine system indicates the peak in the power curve in m/s. The system produces the maximum power at this speed and the speed of the rotor is managed based on this wind speed.
+
+\paragraph{Field: Cut In Wind Speed}\label{field-cut-in-wind-speed}
+
+This field is the lowest wind speed where the wind turbine system can be operated in m/s. No power generation is achieved as long as the ambient wind speed is lower than this speed.
+
+\paragraph{Field: Cut Out Wind Speed}\label{field-cut-out-wind-speed}
+
+This field is the greatest wind speed in m/s. When the wind speed exceeds this value, the wind turbine system needs to be stopped because of inefficiencies in the system. All systems that have either pitch or speed control must be stopped when the ambient wind speed exceeds this speed. Note that the user should input a wind speed above which physical damage to the system might be caused in the case of a FSFP system. It appears as extreme/survival/design wind speed in the literature. The system will be turned off when the ambient wind speed is over this speed.
+
+\paragraph{Field: Fraction System Efficiency}\label{field-fraction-system-efficiency}
+
+This field is the overall system efficiency of the wind turbine system. It includes all the conversion losses as well as transient losses during the dynamic control when the ambient wind speed is between the rated wind speed and cut-out wind speed (see previous fields). The user also has the ability to specify delivery losses from the system to the local area. If the user does not enter a fraction, the model assumes the default value of 0.835. Note that the fraction must be between zero and one.
+
+\paragraph{Field: Maximum Tip Speed Ratio}\label{field-maximum-tip-speed-ratio}
+
+This field is the maximum tip speed ratio between the rotor velocity and ambient wind velocity. The rotor speed varies with this ratio to maximize the power output when the rotor control types are variable speed ones. This field allows the user to adjust the power output from the particular system or to find the optimal tip speed ratio of the system. Optimal tip speed ratio is dependent on the number of blades. It is typically about 6, 5, and 3 for two-bladed, three-bladed, and four-bladed rotor, respectively. For the vertical axis wind turbine, it is smaller than horizontal axis wind turbine, and varies with the chord area. The default and maximum values are 5.0 and 12.0.
+
+\paragraph{Field: Maximum Power Coefficient}\label{field-maximum-power-coefficient}
+
+This field is the maximum fraction of power extraction from ambient wind. If the user inputs this field, the simple approximation model is assumed. The model simply employs the value of this field into the general kinetic energy equation, so that the power output is obtained. The user can obtain this field with a simple calculation from the power curve published in almost all manufacturers' specifications by using the kinetic energy equation as:
+
+\begin{equation}
+{C_p} = \frac{P}{{0.5\rho A{V^3}}}
+\end{equation}
+
+where
+
+\emph{P} = power production at the rated wind speed {[}W{]}
+
+\emph{�} = density of air {[}kg/m3{]}
+
+\emph{A} = swept area of rotor {[}m2{]}
+
+\emph{V} = rated wind speed {[}m/s{]}
+
+\emph{C\(_{p}\)} = power coefficient
+
+The maximum and default values are 0.59 and 0.35.
+
+\paragraph{Field: Annual Local Average Wind Speed}\label{field-annual-local-average-wind-speed}
+
+This field is the local annual average wind speed that represents a representative wind profile at the location of the system in m/s. It is used to factor the difference in wind speed between the weather file wind data and the locally measured wind data so that the model minimizes uncertainties caused by improper wind data at the particular location. Considerable differences between the weather file wind data and the local wind data typically appear. The user thus needs to enter this field in order to obtain accurate local wind data. The model internally determines a multiplier and it is multiplied by the weather file wind data adjusted at the height of the system. If this field is not entered, then the model will use the wind speed from the design day or weather file information with only adjustment at the height of the rotor.
+
+\paragraph{Field: Height for Local Average Wind Speed}\label{field-height-for-local-average-wind-speed}
+
+This field is the height that the local wind speed is measured in meters. The annual average wind speed (see previous field) input by the user is internally recalculated by existing EnergyPlus functions at the height of the local station. This modified wind speed is then factored and applied to the weather file wind data. If the annual local average wind speed is not entered, this field is then assumed as zero. The minimum and default values are zero and 50 meters.
+
+\paragraph{Field: Blade Chord Area}\label{field-blade-chord-area}
+
+This field is the blade chord area of a single blade of VAWT system in m2. It is necessary to determine the net tangential and normal forces of a single blade.
+
+\paragraph{Field: Blade Drag Coefficient}\label{field-blade-drag-coefficient}
+
+This field is the blade drag coefficient for a specific blade. It is for determining the tangential and normal force coefficients with the blade lift coefficient (see next field) so that the model can calculate the power output from the system. The user should be able to obtain this parameter for a specific blade from the manufacturers data. This field is only valid for VAWT systems.
+
+\paragraph{Field: Blade Lift Coefficient}\label{field-blade-lift-coefficient}
+
+This field is the blade lift coefficient for a specific blade. It is for determining the tangential and normal force coefficients with the blade drag coefficient (see previous field) so that the model can calculate the power output from the system. The user should also be able to obtain it for a specific blade from the manufacturers data. This field is only valid for VAWT systems.
+
+\paragraph{Field: Power Coefficient Parameter \textless{}x\textgreater{}}\label{field-power-coefficient-parameter-x}
+
+These six fields are the parameters for the power coefficient equation shown below. These fields are used to determine the power coefficient of the system. The analytical approximation model of the power coefficient in EnergyPlus is:
+
+\begin{equation}
+{C_p} = {C_1}(\frac{{{C_2}}}{{{\lambda_i}}} - {C_3}\theta  - {C_4}{\theta ^x} - {C_5}){e^{ - \frac{{{C_6}(\lambda ,\theta )}}{{{\lambda_i}}}}}
+\end{equation}
+
+with
+
+\begin{equation}
+\frac{1}{{{\lambda_i}}} = \frac{1}{{\lambda  + 0.08\theta }} - \frac{{0.035}}{{{\theta ^3} + 1}}
+\end{equation}
+
+where
+
+\(C_p\) = power coefficient
+
+\(C_{1-6}\) = empirical power coefficient parameters
+
+\(\lambda\) = tip speed ratio (often known as TSR)
+
+\(\lambda_i\) = tip speed ratio at ith time step
+
+\(\theta\) = azimuth angle of the pitch, 0 {[}degree{]}
+
+If the user does not input any field of these parameters, the simple approximation model for the power coefficient will be used (see previous maximum power coefficient field). That is, the analytical approximation model of the power coefficient will be chosen only if the user inputs all these six parameters. The user also has the ability to modify each parameter when the specific value of the system is available. The default values are given in the table below.
+
+\begin{longtable}[c]{@{}llllll@{}}
+\toprule 
+C & C & C & C & C & C \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+C & C & C & C & C & C \tabularnewline
+\midrule
+\endhead
+
+0.5176 & 116 & 0.4 & 0.0 & 5.0 & 21 \tabularnewline
+\bottomrule
+\end{longtable}
+
+These fields are only valid for HAWT systems.
+
+An example input for the wind turbine is shown in below.
+
+\begin{lstlisting}
+
+Generator:WindTurbine,
+  WT1,                     ! Name
+  WT Schedule,     ! Availability Schedule Name
+  HorizontalAxisWindTurbine,     ! Rotor type
+  FixedSpeedVariablePitch,         ! Power control type
+  41,                       ! Maximum rotational speed of the rotor {rev/min}
+  19.2,                   ! Diameter of the rotor {m}
+  30.5,                   ! Overall height of the system {m}
+  3,                         ! Number of blades
+  55000,                 ! Rated power output at the rated wind speed {W}
+  11,                       ! Rated wind speed {m/s}
+  3.5,                     ! Cut In wind speed {m/s}
+  25,                       ! Cut Out wind speed {m/s}
+  0.835,                 ! Overall wind turbine system efficiency
+  8,                         ! Maximum tip speed ratio
+  0.4,                     ! Maximum power coefficient
+  6.4,                     ! Annual local wind speed {m/s}
+  50,                       ! Height of local meteorological station {m}
+  ,                           ! Blade chord area {m2}
+  ,                           ! Blade drag coefficient
+  ,                           ! Blade lift coefficient
+  0.5176,               ! Power Coefficient C1
+  116,                     ! Power Coefficient C2
+  0.4,                     ! Power Coefficient C3
+  0,                         ! Power Coefficient C4
+  5,                         ! Power Coefficient C5
+  21;                       ! Power Coefficient C6
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-12-001}
+
+\begin{itemize}
+\item
+  HVAC,Average, Generator Produced Electric Power {[}W{]}
+\item
+  HVAC,Sum, Generator Produced Electric Energy {[}J{]}
+\item
+  HVAC,Average, Generator Turbine Local Wind Speed {[}m/s{]}
+\item
+  HVAC,Average, Generator Turbine Local Air Density {[}kg/m3{]}
+\item
+  HVAC,Average, Generator Turbine Power Coefficient {[]}
+\item
+  HVAC,Average, Generator Turbine Tip Speed Ratio {[]}
+\item
+  HVAC,Average, Generator Turbine Chordal Component Velocity {[}m/s{]}
+\item
+  HVAC,Average, Generator Turbine Normal Component Velocity {[}m/s{]}
+\item
+  HVAC,Average, Generator Turbine Relative Flow Velocity {[}m/s{]}
+\item
+  HVAC,Average, Generator Turbine Attack Angle {[}deg{]}
+\end{itemize}
+
+\paragraph{Generator Produced Electric Power {[}W{]}}\label{generator-produced-electric-power-w-4}
+
+This report is the electric power that the wind turbine system produces.
+
+\paragraph{Generator Produced Electric Energy {[}J{]}}\label{generator-produced-electric-energy-j-4}
+
+This report is the electric energy that the wind turbine system produces.
+
+\paragraph{Generator Turbine Local Wind Speed {[}m/s{]}}\label{generator-turbine-local-wind-speed-ms}
+
+This report is the local wind speed at the specific height of the wind turbine.
+
+\paragraph{Generator Turbine Local Air Density {[}kg/m3{]}}\label{generator-turbine-local-air-density-kgm3}
+
+This report is the local density of the air at the specific height of the wind turbine.
+
+\paragraph{\texorpdfstring{Generator Turbine Tip Speed Ratio {[]}}{Generator Turbine Tip Speed Ratio }}\label{generator-turbine-tip-speed-ratio}
+
+This report is the ratio between the rotational speed of the tip of the blades and the ambient wind speed at the height of the hub or pole of the wind turbine.
+
+\paragraph{\texorpdfstring{Generator Turbine Power Coefficient {[]}}{Generator Turbine Power Coefficient }}\label{generator-turbine-power-coefficient}
+
+This report represents the efficiency of the power extraction from the ambient wind of the wind turbine. It is function of the tip speed ratio and pitch angle. It is only valid for HAWT systems.
+
+\paragraph{Generator Turbine Chordal Component Velocity {[}m/s{]}}\label{generator-turbine-chordal-component-velocity-ms}
+
+This report is the axial velocity component along the chord of the wind turbine system. It is only valid for VAWT systems.
+
+\paragraph{Generator Turbine Normal Component Velocity {[}m/s{]}}\label{generator-turbine-normal-component-velocity-ms}
+
+This report is the axial velocity component of the rotor of the wind turbine system. It is only valid for VAWT systems.
+
+\paragraph{Generator Turbine Relative Flow Velocity {[}m/s{]}}\label{generator-turbine-relative-flow-velocity-ms}
+
+This report is the local relative flow velocity that represents actual direction and velocity incident on the blades. It is the square root of the sum of both chordal velocity component and normal velocity component. It is only valid for VAWT systems.
+
+\paragraph{Generator Turbine Attack Angle {[}deg{]}}\label{generator-turbine-attack-angle-deg}
+
+This report is the azimuth angle between the relative flow velocity and the plane of chord. It varies as the wind speed increases, so that the lift and drag forces change.
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+\protect\hyperlink{ux5fftnref1}{{[}1{]}} Ulleberg Ø . (1997) Simulation of autonomous PV-H2 systems: analysis of the PHOEBUS plant design, operation and energy management. In \emph{Proceedings of ISES 1997 Solar World Congress}, August 24-30, Taejon, Korea.
+
+Ulleberg Ø . (1998) \emph{Stand-Alone Power Systems for the Future: Optimal Design, Operation \& Control of Solar-Hydrogen Energy Systems}. PhD thesis, Norwegian University of Science and Technology, Trondheim.
diff --git a/doc/input-output-reference/src/overview/group-energy-management-system-ems.tex b/doc/input-output-reference/src/overview/group-energy-management-system-ems.tex
new file mode 100644
index 00000000000..54c8767d837
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+++ b/doc/input-output-reference/src/overview/group-energy-management-system-ems.tex
@@ -0,0 +1,622 @@
+\section{Group Energy Management System (EMS)}\label{group-energy-management-system-ems}
+
+The Energy Management System (EMS) is one of the high-level control methods available in EnergyPlus. An EMS is able to access a wide variety of sensor data and use this data to direct various types of control actions. The concept is to emulate, inside EnergyPlus, the types of controls possible with the digital energy management systems used in real buildings.
+
+In the hierarchy of EnergyPlus controls, the EMS module is a high-level, generalized, supervisory control for building systems. The EMS replicates the functionality of many of the existing high-level control objects in EnergyPlus. Similar to the AvailabilityManager objects, the EMS can turn on and off pumps and fans. Similar to the DemandManager objects, the EMS can turn on and off lights and electric equipment, change the set points on zone thermostats, and dispatch on-site generation. Similar to the SetpointManager objects, the EMS can change the set points on system nodes. Similar to the PlantEquipmentOperation objects, the EMS can turn on and off supply-side heating, cooling, and heat rejection equipment, i.e., boilers, chillers, cooling towers, etc. Similar to the ElectricLoadCenter:Distribution, the EMS can turn on and off on-site generation equipment.
+
+A separate document called \emph{Application Guide for EMS} contains much more information on how to use the EMS. The EMS uses the EnergyPlus Runtime Language (Erl) for custom programming of control routines.
+
+\subsection{EnergyManagementSystem:Sensor}\label{energymanagementsystemsensor}
+
+The EnergyManagmentSystem:Sensor object is used to declare an Erl variable that is linked to EnergyPlus output variables or meters. EMS sensors are used to get information from elsewhere in the model for use in control calculations. The separate output files called eplusout.rdd and eplusout.mdd provide a listing of the output variables and meters that can be used as sensors.
+
+\subsubsection{Inputs}\label{inputs-015}
+
+\paragraph{Field: Name}\label{field-name-014}
+
+This field contains a unique name for the sensor that becomes the name of a variable for use in Erl programs. No spaces are allowed in the object name. This name will be a global variable in Erl programs and cannot duplicate any other global scope Erl variable.
+
+\paragraph{Field: Output:Variable or Output:Meter Index Key Name}\label{field-outputvariable-or-outputmeter-index-key-name}
+
+The key reference for the specified output variable. For example, if System Node Temperature is the output variable, the unique node name is the key. The \emph{Key Name} field should be omitted for weather variables and meters because they do not have a key.
+
+\paragraph{Field: Output:Variable or Output:Meter Name}\label{field-outputvariable-or-outputmeter-name}
+
+The name of the output variable or meter that is to be mapped to the Erl variable for the sensor. The names that can be used in a specific model are included in the .RDD output file.
+
+Examples of this object follow.
+
+\begin{lstlisting}
+
+EnergyManagementSystem:Sensor,
+  T1, !Name
+  Perimeter_ZN_1 , ! Output:Variable or Output:Meter Index Key Name
+  Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
+
+  EnergyManagementSystem:Sensor,
+  PMV5, !Name
+  Core_ZN , ! Output:Variable Index Key Name
+  Zone Thermal Comfort Fanger Model PMV ; ! Output:Variable Name
+
+  EnergyManagementSystem:Sensor,
+  T_VAV5FanIn, !Name
+  VAV_5_HeatC-VAV_5_FanNode , ! Output:Variable Index Key Name
+  System Node Temperature ; ! Output:Variable Name
+
+  EnergyManagementSystem:Sensor,
+  cooling_setpoint,                                   ! Name
+  CLGSETP_SCH ,                 ! Output:Variable Index Key Name
+  Schedule Value ; ! Output:Variable Name
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:Actuator}\label{energymanagementsystemactuator}
+
+This object maps an Erl variable to a control actuator elsewhere in EnergyPlus. The EMS then initiates control actions by changing the value of this variable inside an Erl program. The Application Guide for EMS contains much more information on EMS actuators. The eplusout.EDD file can contain a listing of the actuators available for a specific model.
+
+\subsubsection{Inputs}\label{inputs-1-013}
+
+\paragraph{Field: Name}\label{field-name-1-012}
+
+The field contains a unique name for the actuator that becomes the name of a variable for use in Erl programs. No spaces are allowed in the object name. This name will be a global variable in Erl programs and cannot duplicate any other global scope Erl variable.
+
+\paragraph{Field: Actuated Component Unique Name}\label{field-actuated-component-unique-name}
+
+This field defines a unique name for the specific entity that is to be controlled. The names for each individual component are listed in the EDD output file when Verbose mode is used see the input object Output:EnergyManagementSystem for more on the EDD file. These will often be user-defined names of input objects or system nodes, but some actuators are automatically setup by the program and will not be completely user-defined.
+
+\paragraph{Field: Actuated Component Type}\label{field-actuated-component-type}
+
+The field defines the type of the entity that is to be controlled by the actuator. The component types available vary with the specifics of individual models. The types of components that can be used as actuators in a specific model are listed in the EDD output file see the input object Output:EnergyManagementSystem for more on the EDD file. Components can be object types defined elsewhere in the IDD but there are other types of entities such as nodes and system-level actuators that do not directly correspond to IDF objects.
+
+\paragraph{Field: Actuated Component Control Type}\label{field-actuated-component-control-type}
+
+This field defines the type of control to be done on the specific entity being controlled. The control types available are listed in the EDD output. Specific components may have more than one type of control available, such as flow rate or temperature, and this field is used to distinguish between them.
+
+Example input objects.
+
+\begin{lstlisting}
+
+EnergyManagementSystem:Actuator,
+  VAV_5_NightCycleStatus,     ! Name
+  VAV_5,                                       ! Actuated Component Unique Name
+  AirLoopHVAC,                           ! Actuated Component Type
+  Availability Status;           ! Actuated Component Control Type
+
+  EnergyManagementSystem:Actuator,
+  VAV_1_SAT_setpoint,                                       ! Name
+  VAV_1 Supply Equipment Outlet Node ,     ! Actuated Component Unique Name
+  System Node Setpoint,                                   ! Actuated Component Type
+  Temperature Setpoint;                                   ! Actuated Component Control Type
+
+  EnergyManagementSystem:Actuator,
+  myCLGSETP_SCH_Override,                             ! Name
+  CLGSETP_SCH,                                                   !- Actuated Component Unique Name
+  Schedule:Constant,                                       ! Actuated Component Type
+  Schedule Value;                                             ! Actuated Component Control Type
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:ProgramCallingManager}\label{energymanagementsystemprogramcallingmanager}
+
+The EnergyManagementSystem:ProgramCallingManager object is used to specify when individual Erl programs are run. This object manages two temporal aspects of running Erl programs. The first is when they are run relative to the rest of EnergyPlus, and the second is when they are run relative to each other. EMS applications can use multiple EnergyManagementSystem:ProgramCallingManager objects. For example, one manager may execute an initialization program once at the beginning of the run period while additional managers call various sets of programs from different EMS Calling Points.
+
+Control schemes can be organized using a multiple Erl programs and this object this specifies the order in which they are executed. \emph{Program Name 1} is run first, \emph{Program Name 2} is run second, etc. The run order can be important if there are interactions or dependencies between two or more programs. Within each program there may be calls to execute subroutine programs but only calling managers are used to execute main-level programs.
+
+\subsubsection{Inputs}\label{inputs-2-012}
+
+\paragraph{Field: Name}\label{field-name-2-011}
+
+This is a unique name for this particular program manager.
+
+\paragraph{Field: EnergyPlus Model Calling Point}\label{field-energyplus-model-calling-point}
+
+This field describes when the Erl programs managed under this object are called during an EnergyPlus simulation. All of the programs listed are called at this same calling point. There are 15 possible calling points summarized below. For more information see the section on EMS Calling Points in the Application Guide for EMS.
+
+\begin{itemize}
+\item
+  BeginNewEnvironment. This calling point occurs near the beginning of each environment period. Environment periods include sizing periods such as design days and run periods. This calling point will not be useful for control actions but is useful for initialization of Erl program variables and other one-time set up actions for EMS.
+\item
+  AfterNewEnvironmentWarmUpIsComplete. This calling point occurs at the beginning of each environment period but after warm up days are complete. Warm up days are used to condition the transient aspects of the model with the first day before proceeding. This calling point will not be useful for control actions but is useful for re-initializing Erl programs with fresh values after warm up is complete. Programs called from this point might be used to reset counters or summed variables that would change during warmup.
+\item
+  BeginTimestepBeforePredictor. This calling point happens near the beginning of each timestep but before predictor executes. Predictor refers to the step in EnergyPlus modeling where the zone s thermal loads are calculated. This calling point is useful for controlling components that affect the thermal loads that the systems will be attempting to meet. Programs called from this point might actuate the building envelope or internal gains based on current weather and the results from the previous timestep.
+\item
+  AfterPredictorBeforeHVACManagers. This calling point happens each timestep just after predictor executes but before the traditional supervisory control models for SetpointManager and AvailabilityManager are called. This calling point is useful for a variety of control actions. However, if there are conflicts, the EMS control actions may be overwritten by the actions of any traditional SetpointManagers or AvailabilityManagers in the model.
+\item
+  AfterPredictorAfterHVACManagers. This calling point happens each timestep after predictor executes and after the SetpointManager and AvailabilityManager models are called. This calling point is useful for a variety of control actions. However, if there are conflicts, SetpointManager or AvailabilityManager actions may be overwritten by EMS control actions.
+\item
+  InsideHVACSystemIterationLoop. This calling point happens each HVAC iteration. The HVAC systems solvers iterate to convergence within each timestep and this calling point is inside this iteration loop. This calling point is useful for a variety of control actions. Being inside the interation loop, this calling point has the advantage that input data need not necessarily be lagged from prior timestep results and can, in some cases, improve the accuracy of controls. The disadvantage is that programs may run an excessive number of times slowing down the execution of the program.
+\item
+  EndOfZoneTimestepBeforeZoneReporting. This calling point happens each zone timestep just before the output reports are updated for zone-timestep variables and meters. This calling point is useful for custom output variables with Zone frequency because they will be in sync with the rest of the zone output variables.
+\item
+  EndOfZoneTimestepAfterZoneReporting. This calling point happens each zone timestep just after the output reports are updated for zone-timestep variables and meters. This calling point is the last one of a timestep and is useful for making control decisions for the next zone timestep using the final meter values for the current zone timestep.
+\item
+  EndOfSystemTimestepBeforeHVACReporting. This calling point happens each system timestep just before the output reports are updated for HVAC-timestep variables and meters. This calling point is useful for custom output variables with HVAC frequency because they will be in sync with the rest of the system output variables.
+\item
+  EndOfSystemTimestepAfterHVACReporting. This calling point happens each system timestep just after the output reports are updated for HVAC-timestep variables and meters. This calling point is useful for making control decisions for the next system timestep using the final meter values for the current system timestep.
+\item
+  EndOfZoneSizing. This calling point happens once during each simulation and only if the run is set to do zone sizing. The calling point occurs just after the native zone sizing calculations are completed but before the sizing results are finalized. This calling point is useful for taking the intermediate results of zone sizing calculations and modifying them based on custom calculations.
+\item
+  EndOfSystemSizing. This calling pont happens once during each simulation and only if the run is set to do system sizing. The calling point occurs just after the native air system sizing calculations are completed but before the sizing results are finalized. This calling point is useful for taking the intermediate results of zone and system sizing calculations and modifying them based on custom calculations.
+\item
+  AfterComponentInputReadIn. This calling point occurs early in the simulation when HVAC component s input data has been processed but before any component-level calculations for automatic sizing. This calling point occurs once for each of the types of HVAC components that have EMS actuators for autosize overrides. This calling point is not directly useful for control actions but is useful for overriding the results of sizing at the component level.
+\item
+  UserDefinedComponentModel. This calling point occurs when user-defined HVAC and plant component models are called to be simulated. This calling point is only used for the programs that model custom components. This calling point differs from the others in that when it is being used the calls to trigger include a reference to a specific EnergyManagementSystem:ProgramCallingManager and only the one manger is executed.
+\item
+  UnitarySystemSizing. This calling point occurs when Unitary systems begin their calculations for determining the size values for autosized input fields. This calling point is used for overriding the autosizing outcomes for unitary systems. Each unitary system in the simulation will call this point one time. This calling point is used to override sizing in the following input objects: AirLoopHVAC:UnitarySystem, AirLoopHVAC:Unitary:Furnace:HeatOnly, AirLoopHVAC:UnitaryHeatOnly, AirLoopHVAC:UnitaryHeatCool,AirLoopHVAC:Unitary:Furnace:HeatCool, AirLoopHVAC:UnitaryHeatPump:AirToAir, and AirLoopHVAC:UnitaryHeatPump:WaterToAir.
+\end{itemize}
+
+\paragraph{Field: Program Name 1}\label{field-program-name-1}
+
+The name of the EnergyManagementSystem:Program object that will be the first to run for the calling point.
+
+\paragraph{Field: Program Name 2 .. N}\label{field-program-name-2-..-n}
+
+The name of the EnergyManagementSystem:Program object that will be the second to run. Additional programs can be listed. The object is automatically extensible to accommodate as many programs as needed.
+
+IDF examples:
+
+\begin{lstlisting}
+
+EnergyManagementSystem:ProgramCallingManager,
+  Initialize EMS for Run , ! Name
+  BeginNewEnvironment ,       ! EnergyPlus Model Calling Point
+  InitializeMyEMS;                 ! Program Name 1
+
+
+  EnergyManagementSystem:ProgramCallingManager,
+  EMS-based Setpoint Managers , ! Name
+  AfterPredictorAfterHVACManagers , ! EnergyPlus Model Calling Point
+  VAV_5_SchedSetpoint , !Program Name 2
+  VAV5MixedAirManagers,
+  VAV_1_SchedSetpoint,
+  VAV1MixedAirManagers,
+  VAV_3_SchedSetpoint,
+  VAV3MixedAirManagers,
+  VAV_2_SchedSetpoint,
+  VAV2MixedAirManagers,
+  CoolSys1_SchedSetpoint,
+  HeatSys1_SchedSetpoint,
+  SHWSys1_SchedSetpoint,
+  VAV_5_NightCycleMGR,
+  VAV_1_NightCycleMGR,
+  VAV_2_NightCycleMGR,
+  VAV_3_NightCycleMGR;
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:Program}\label{energymanagementsystemprogram}
+
+The EnergyManagementSystem:Program object is the central processor of the EMS and the primary container for the \emph{EnergyPlus Runtime Language}, or Erl. The EnergyManagementSystem:Program objects are run in the order and point during an EnergyPlus simulation that is specified in an EnergyManagementSystem:ProgramCallingManager object. Multiple EnergyManagementSystem:Program objects are allowed and may interact (or interfere) with each other. The \emph{Application Guide for EMS} provides a comprehensive overview of Erl programming.
+
+The object definition is very simple. There is a name followed by lines of Erl program code.
+
+\subsubsection{Inputs}\label{inputs-3-011}
+
+\paragraph{Field: Name}\label{field-name-3-010}
+
+This field is the unique name of the Erl program. The name can be used to call the program to run from another program or subroutine. No spaces are allowed in the name.
+
+\paragraph{Field Set: Program lines 1 to N}\label{field-set-program-lines-1-to-n}
+
+Each remaining field contains a single line of code for the \emph{EnergyPlus Runtime Language}, or Erl. Erl is a little programming language with its own syntax. The commas separating fields can be thought of as end of line characters. The \emph{Application Guide for EMS} provides a the details on Erl program code.
+
+Example IDF input objects follow.
+
+\begin{lstlisting}
+
+EnergyManagementSystem:Program,
+  RH_OpeningController ,         ! Name
+  IF ZoneRH < 25,
+  SET MyOpenFactor = 0.0 ,
+  ELSEIF ZoneRH > 60,
+  SET MyOpenFactor = 1.0 ,
+  ELSE,
+  SET MyOpenFactor = (ZoneRH - 25) / (60 - 25),
+  ENDIF;
+
+  EnergyManagementSystem:Program,
+  AverageZoneTemps , ! Name
+  SET Zn1vol = 346.0225, ! zone air volume
+  SET Zn2vol = 205.2650, ! zone air volume
+  SET Zn3vol = 346.0225, ! zone air volume
+  SET Zn4vol = 205.2650, ! zone air volume
+  SET Zn5vol = 456.4551, ! zone air volume
+  SET SumNumerator = T1*Zn1vol + T2*Zn2vol + T3*Zn3vol + T4*Zn4vol + T5*Zn5vol,
+  SET SumDenominator = Zn1vol + Zn2vol + Zn3vol + Zn4vol + Zn5vol,
+  SET AverageBuildingTemp = SumNumerator / SumDenominator;
+
+
+  EnergyManagementSystem:Program,
+  VAV2MixedAirManagers , ! Name
+  SET VAV_2_CoolC_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV2FanOut - T_VAV2FanIn),
+  SET VAV_2_HeatC_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV2FanOut - T_VAV2FanIn),
+  SET VAV_2_OA_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV2FanOut - T_VAV2FanIn);
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:Subroutine}\label{energymanagementsystemsubroutine}
+
+The EnergyManagementSystem:Subroutine object contains a block of code written in the \emph{EnergyPlus Runtime Language} that can be run from another Erl program. If the subroutine is never called, it will never run by itself. Subroutines are useful for encapsulating code that is called in multiple places. It is also helpful for organizing and structuring code. When the subroutine finishes running, control is returned to the object that called it. See the \emph{Application Guide for EMS} for information on writing Erl programs.
+
+\subsubsection{Inputs}\label{inputs-4-010}
+
+\paragraph{Field: Name}\label{field-name-4-009}
+
+The name uniquely identifying the subroutine. The name can be used to call the subroutine to run from a program or another subroutine or even itself. No spaces are allowed in the name.
+
+\paragraph{Field set: Lines 1 to N}\label{field-set-lines-1-to-n}
+
+Each remaining field contains a single line of code for the \emph{EnergyPlus Runtime Language}, or Erl. Erl is a little programming language with its own special syntax. The commas separating fields can be thought of as end of line characters. The \emph{Application Guide for EMS} contains the details on the rules for Erl program code.
+
+IDF examples:
+
+\begin{lstlisting}
+
+EnergyManagementSystem:Subroutine,
+  Add4ToN,                                                           !- Name
+  SET N = N + 4;                                               !- EnergyPlus Runtime Language
+
+  EnergyManagementSystem:Subroutine,
+  manage_ext_lights,                                       !- Name
+  IF inc_solar > 0,                                         !- EnergyPlus Runtime Language
+  SET ext_lights_pwr = Off,
+  ELSE,
+  SET ext_lights_pwr = On,
+  ENDIF;
+
+  EnergyManagementSystem:Subroutine,
+  manage_solar_collector,                             !- Name
+  IF Tout_F < 32,                                             !- EnergyPlus Runtime Language
+  SET pump_pwr = On,
+  EXIT,
+  ENDIF,
+  SET delta_T = Tcollector     Ttank,
+  IF delta_T > 0,
+  SET pump_pwr = On,
+  ELSE,
+  SET pump_pwr = Off,
+  ENDIF;
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:GlobalVariable}\label{energymanagementsystemglobalvariable}
+
+The EnergyManagementSystem:GlobalVariable object declares one or more global variables that can be accessed by all Erl programs in the EMS. Erl variables declared by the user as sensor and actuators objects are already global variables. Global scope variables are needed to move date in and out of subroutines because Erl does not support passing arguments within such calls. Global scope variables are also needed to pass an Erl variable result to an output variable. Each field in this object names a new global Erl variable.
+
+\subsubsection{Inputs}\label{inputs-5-009}
+
+\paragraph{Field: Erl Variable (1..N) Name}\label{field-erl-variable-1..n-name}
+
+The name becomes the global Erl variable name that can be referenced in the \emph{EnergyPlus Runtime Language}. No spaces are allowed in the object name. The name must be unique across all global scope variables including those declared as sensor and actuators and the built-in variables.
+
+IDF examples using this object follow:
+
+\begin{lstlisting}
+
+EnergyManagementSystem:GlobalVariable,
+  global_var;                                                                   !- Name
+
+  EnergyManagementSystem:GlobalVariable, Temp_C;
+
+  EnergyManagementSystem:GlobalVariable, Temp_F;
+
+  EnergyManagementSystem:Subroutine,
+  CalcFahrenheit,                                                           !- Name
+  SET Temp_F = Temp_C * (9/5) + 32;
+
+  EnergyManagementSystem:Program,
+  DummyProgram,                                                               !- Name
+  SET Temp_C = Tout,
+  RUN CalcFahrenheit,
+  SET Tout_F = Temp_F,
+  IF Tout_F > 32,
+  RUN FreezeProtect,
+  ENDIF;
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:OutputVariable}\label{energymanagementsystemoutputvariable}
+
+The \textbf{EnergyManagementSystem:OutputVariable} object creates a custom output variable that is mapped to an EMS variable. These can be declared by an \textbf{EnergyManagementSystem:Sensor} object, an \textbf{EnergyManagementSystem:Actuator} object, or an \textbf{EnergyManagementSystem:GlobalVariable} object, or any local variable in an Erl program. The custom output variable can then be reported to the output file using the standard EnergyPlus output mechanisms such as with the Output:Variable object.
+
+The EnergyManagementSystem:OutputVariable object is a primary way to obtain data from an Erl program and is likely to be essential for developing and debugging programs. This object also provides a powerful mechanism to create custom output variables. See the \emph{Application Guide for EMS} for more information.
+
+\subsubsection{Inputs}\label{inputs-6-008}
+
+\paragraph{Field: Name}\label{field-name-5-008}
+
+This field contains the user-defined name for the new output variable. This is the name that will appear in the RDD output file and can be referenced in other input for output such as an Output:Variable object. By convention, the name is in title case for capitalization. Units are provided in the Units field.
+
+\paragraph{Field: EMS Variable Name}\label{field-ems-variable-name}
+
+This field contains the EMS variable name that is to be mapped to the custom output variable. This must be used elsewhere in Erl programs and cannot have spaces.
+
+\paragraph{Field: Type of Data in Variable}\label{field-type-of-data-in-variable}
+
+This field describes the nature of the variable. There are two choices, Averaged or Summed. Averaged variables are state variables such as temperature, power, or flow rate. Summed variables are quantities such as energy that accumulate across time.
+
+\paragraph{Field: Update Frequency}\label{field-update-frequency}
+
+This field describes which timestep the variable is associated with. There are two choices, ZoneTimestep or SystemTimestep. Variables that are related to the building or zone loads are generally associated with the zone timestep. Variables that are related to HVAC system operation are generally associated with the system timestep.
+
+\paragraph{Field: EMS Program or Subroutine Name}\label{field-ems-program-or-subroutine-name}
+
+If the EMS variables is a local scope variable, i.e., not declared as a global scope variable, then this field identifies which program uses the variable. The field references the object name of the Erl program or subroutine object. For global variables, this field should be omitted.
+
+\paragraph{Field: Units}\label{field-units}
+
+This field should contain the units for the output variable in standard EnergyPlus units. It does not need to be enclosed in square brackets.
+
+Examples of this object follow.
+
+\begin{lstlisting}
+
+EnergyManagementSystem:OutputVariable,
+  Weighted Average Building Zone Air Temperature, ! Name
+  AverageBuildingTemp, ! EMS Variable Name
+  Averaged, ! Type of Data in Variable
+  ZoneTimeStep , ! Update Frequency
+  ,           ! EMS Program or Subroutine Name
+  C;
+
+
+  EnergyManagementSystem:OutputVariable,
+  Main CW Coil Total Cooling Rate,   !- Name
+  CWcoil1_tot_cool_Power,   !- EMS Variable Name
+  Averaged,                               !- Type of Data in Variable
+  SystemTimestep,                   !- Update Frequency
+  MainCWCoil1_ModelOuput,   !- EMS Program or Subroutine Name
+  W;                                             !- Units
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:MeteredOutputVariable,}\label{energymanagementsystemmeteredoutputvariable}
+
+The EnergyManagementSystem:MeteredOutputVariable object creates a custom output variable that is mapped to an EMS variable and is also included in the metering system that EnergyPlus has for aggregating results for different resources across the model. This object is very similar to EnergyManagementSystem:OutputVariable with the main differences being that only summed types of data in the Erl variable and the quantity is to be added to a meter. This allows for custom output variables that also impact the results for the amount of electricity or gas consumed.
+
+\subsubsection{Field: Name}\label{field-name-6-006}
+
+This field contains the user-defined name for the new output variable. This is the name that will appear in the RDD and MTD output files and can be referenced in other input for output such as an Output:Variable object. Units are provided in the Units field.
+
+\subsubsection{Field: EMS Variable Name}\label{field-ems-variable-name-1}
+
+This field contains the EMS variable name that is to be mapped to the custom output variable. This must be used elsewhere in Erl programs and cannot have spaces.
+
+\subsubsection{Field: Update Frequency}\label{field-update-frequency-1}
+
+This field describes which timestep the variable is associated with. There are two choices, ZoneTimestep or SystemTimestep. Variables that are related to the building or zone loads are generally associated with the zone timestep. Variables that are related to HVAC system operation are generally associated with the system timestep.
+
+\subsubsection{Field: EMS Program or Subroutine Name}\label{field-ems-program-or-subroutine-name-1}
+
+If the EMS variables is a local scope variable, i.e., not declared as a global scope variable, then this field identifies which program uses the variable. The field references the object name of the Erl program or subroutine object. For global variables, this field should be omitted.
+
+\subsubsection{Field: Resource Type}\label{field-resource-type}
+
+This field is used to specify the type of resource that the output variable consumes or produces. The choice here will determine which of the meters the output should be added to when EnergyPlus aggregates results for overall consumption. The following keywords can be used to choose the type of resource that should be metered:
+
+\begin{itemize}
+\item
+  \textbf{Electricity}, this selects the main meter for electricity consumption, in units of Joules {[}J{]},
+\item
+  \textbf{NaturalGas}, this selects the meter for natural gas consumption, in units of Joules {[}J{]},
+\item
+  \textbf{Gasoline}, this selects the meter for gasoline consumption, in units of Joules {[}J{]},
+\item
+  \textbf{Diesel}, this selects the meter for diesel consumption, in units of Joules {[}J{]},
+\item
+  \textbf{Coal}, this selects the meter for coal consumption, in units of Joules {[}J{]},
+\item
+  \textbf{FuelOil\#1}, this selects the meter for \#1 Fuel Oil consumption, in units of Joules {[}J{]},
+\item
+  \textbf{FuelOil\#2}, this selects the meter for \#2 Fuel Oil consumption, in units of Joules {[}J{]},
+\item
+  \textbf{Propane}, this selects the meter for propane consumption, in units of Joules {[}J{]},
+\item
+  \textbf{WaterUse}, this selects the meter for overall water consumption, in units of cubic meters {[}m\(^{3}\){]},
+\item
+  \textbf{OnSiteWaterProduced}, this selects the meter for overall on-site water collection, in units of cubic meters {[}m\(^{3}\){]},
+\item
+  \textbf{MainsWaterSupply}, this selects the meter for water supplied by utility mains, in units of cubic meters {[}m\(^{3}\){]},
+\item
+  \textbf{RainWaterCollected}, this selects the meter for water collected from rain, in units of cubic meters {[}m\(^{3}\){]},
+\item
+  \textbf{WellWaterDrawn}, this selects the meter for water drawn from a local well, in units of cubic meters {[}m\(^{3}\){]},
+\item
+  \textbf{CondensateWaterCollected}, this selects the meter for water collected from cooling coils as condensate, in units of cubic meters {[}m\(^{3}\){]},
+\item
+  \textbf{EnergyTransfer}, this selects the general meter for energy transfers, in units of Joules {[}J{]},
+\item
+  \textbf{Steam}, this selects the meter for steam energy consumption, in units of Joules {[}J{]},
+\item
+  \textbf{DistrictCooling}, this selects the meter for district chilled water energy consumption, in units of Joules {[}J{]},
+\item
+  \textbf{DistrictHeating}, this selects the meter for district hot water energy consumption, in units of Joules {[}J{]},
+\item
+  \textbf{ElectricityProducedOnSite}, this selects the meter for electricity produced on the site, in units of Joules {[}J{]},
+\item
+  \textbf{SolarWaterHeating}, this selects the meter for hot water heating energy from solar collectors, in units of Joules {[}J{]}, and,
+\item
+  \textbf{SolarAirHeating}, this selects the meter for air heating energy from solar collectors in units of Joules {[}J{]},.
+\end{itemize}
+
+\subsubsection{Field: Group Type}\label{field-group-type}
+
+This field is used to specify how the output variable fits into the categorization scheme used by the metering system in EnergyPlus to identify what part of the model is involved. Metered output variables are classified as being in one of the following general groups:
+
+\begin{itemize}
+\item
+  \textbf{Building}, this category includes all the meters associated with parts of the building that are not related to HVAC or Plant. This includes internal and exterior services such as lights, electric equipment, exterior lights, etc.
+\item
+  \textbf{HVAC}, this category includes all the meters associated with parts of the HVAC system that are related to air and zone thermal conditioning and ventilation (but not hydronic plant systems). This includes things like fans, air conditioners, furnaces etc.
+\item
+  \textbf{Plant}, this category includes all the meters associated with parts of the hydronic plant system that are related to heating, cooling, service water heating, and heat rejection. This includes things like boilers, chillers, water heaters, towers, etc.
+\end{itemize}
+
+\subsubsection{Field: End-Use Category}\label{field-end-use-category}
+
+This field is used to specify the end use category that should be assigned to the resource associated with the output variable. EnergyPlus reporting includes the breakdown of how resources are used across different end uses. Metered output variables must be classified as being in one of the following end use categories:
+
+\begin{itemize}
+\item
+  Heating
+\item
+  Cooling
+\item
+  InteriorLights
+\item
+  ExteriorLights
+\item
+  InteriorEquipment
+\item
+  ExteriorEquipment
+\item
+  Fans
+\item
+  Pumps
+\item
+  HeatRejection
+\item
+  Humidifier
+\item
+  HeatRecovery
+\item
+  WaterSystems
+\item
+  Refrigeration
+\item
+  OnSiteGeneration
+\end{itemize}
+
+\subsubsection{Field: End-Use Subcategory}\label{field-end-use-subcategory}
+
+This field is used to specify the end use subcategory that will be assigned to the output variable. EnergyPlus reporting includes the breakdown of how resources are used across different end uses with added breakdown for the different subcategories within a particular end use. This user can define his or her own subcategories and enter them in this field. If left blank, then no subcategory classification is made and the output is included in the general subcategory for the end use category determined in the previous field.
+
+\subsubsection{Field: Units}\label{field-units-1}
+
+This field should contain the units for the output variable in standard EnergyPlus units. It does not need to be enclosed in square brackets.
+
+Examples of this object follow.
+
+\begin{lstlisting}
+
+EnergyManagementSystem:MeteredOutputVariable,
+  Zone 1 WinAC Electricity Consumption,   !- Name
+  Zone1WinAC_ElectEnergy,   !- EMS Variable Name
+  SystemTimestep,                   !- Update Frequency
+  Zone1_WinAC_ModelOuput,   !- EMS Program or Subroutine Name
+  Electricity,                         !- Resource Type
+  HVAC,                                       !- Group Type
+  Cooling,                                 !- End-Use Category
+  Window Air Conditioners, !- End-Use Subcategory
+  J;                                             !- Units
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:TrendVariable}\label{energymanagementsystemtrendvariable}
+
+The EnergyManagementSystem:TrendVariable object declares a global trend EMS variable that can be accessed by all Erl programs in the EMS. Trend variables store the recent history of the Erl variable they are associated with. The trend data are useful for examining the progression of time series data. The user declares a new trend variable using this object and associates it with another global Erl variable that will be logged. Trend data are pushed into a stack so that the most recent data are always at the beginning of the stack. Once the stack is full, the oldest data are lost from the trend log. Each value in the trend log is for a zone timestep into the past. The first value in the trend is the one from the previous zone time step.
+
+\subsubsection{Inputs}\label{inputs-7-008}
+
+\paragraph{Field: Name}\label{field-name-7-005}
+
+The object name becomes the global EMS trend variable name that can be referenced in the \emph{EnergyPlus Runtime Language}. No spaces are allowed in the name. Then name must be unique across all global scope variables including those declared as sensor and actuators and the built-in variables.
+
+\paragraph{Field: EMS Variable Name}\label{field-ems-variable-name-2}
+
+This field contains the EMS variable name that is to be mapped to the trend variable. This must be a global EMS variable defined elsewhere and cannot have spaces.
+
+\paragraph{Field: Number of Timesteps to be Logged}\label{field-number-of-timesteps-to-be-logged}
+
+This field describes how much data are to be held in the trend variable. The trended data are held in an array with one value for each data point going back in time. This field determines how many elements are in that array. If there are six timesteps per hour and this field is set to 144, then the trend will contain data for the most recent 24 hours period.
+
+Examples of this object follow.
+
+\begin{lstlisting}
+
+EnergyManagementSystem:TrendVariable,
+  AvgTemptrendLog1,                   !- Name
+  AverageBuildingTemp,             !- EMS Variable Name
+  300;                                             !- Number of Timesteps to be Logged
+
+
+  EnergyManagementSystem:TrendVariable,
+  PMVtrendLog1, ,                       !- Name
+  PMV5,                                           !- EMS Variable Name
+  144;                                             !- Number of Timesteps to be Logged
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:InternalVariable}\label{energymanagementsysteminternalvariable}
+
+The EMS also provides a method to obtain static data from elsewhere in the model. Whereas EMS sensors are used for time-varying data, there are also data that describe certain design parameters for the building which may be useful for EMS calculations. A method for accessing internal data is provided as a time saver and means of better generalizing Erl programs for wider applicability. Information needed for this input object is output by EnergyPlus to the eplusout.edd file see the Output:EnergyManagementSystem input object. The EDD file can list the internal data index keys and types that are available for use with this object. The Application Guide for EMS discusse internal variables in more depth.
+
+\subsubsection{Inputs}\label{inputs-8-006}
+
+\paragraph{Field: Name}\label{field-name-8-005}
+
+This field contains a unique name for the internal variable that becomes the name of a variable for use in Erl programs. No spaces are allowed in the name. This name will be a global variable in Erl programs and cannot duplicate any other global scope EMS variable.
+
+\paragraph{Field: Internal Data Index Key Name}\label{field-internal-data-index-key-name}
+
+This field contains the unique identifier for the internal variable. This is usually a name defined by the user elsewhere in an IDF input object. For example, for an internal variable for the floor area of a zone, this would be the name of the zone.
+
+\paragraph{Field: Internal Data Type}\label{field-internal-data-type}
+
+This field defines the type of internal data source that is to be mapped to the EMS variable. The types of internal source data that can be used as internal variables are listed in the EIO output file whan an input file has any EMS-related objects.
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+EnergyManagementSystem:InternalVariable,
+  Zn1vol,                   !- Name
+  Perimeter_ZN_1,   !- Internal Data Index Key Name
+  Zone Air Volume; !- Internal Data Type
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:CurveOrTableIndexVariable}\label{energymanagementsystemcurveortableindexvariable}
+
+The EMS provides a method for reusing curve and table input objects from elsewhere in the model. Input objects, such as Curve:Cubic, Curve:Biquadratic, or Table:TwoIndependetVariables, are used by various component models to describe performance relationships in a generic way. By using an EnergyManagementSystem:CurveOrTableIndexVariable input object, these curves and tables can be used in your own Erl programs. This object sets up an Erl variable that contains an index that points to specific curve or table. This index variable is then used as the first argument in a call to the built-in function called @CurveValue so that the correct curve or table is evaluated.
+
+\subsubsection{Inputs}\label{inputs-9-005}
+
+\paragraph{Field: Name}\label{field-name-9-005}
+
+This field contains a unique name for the index variable that becomes the name of a variable for use in Erl programs. No spaces are allowed in the name. This name will be a global variable in Erl programs and cannot duplicate any other global scope EMS variable. The variable will be filled by the EMS system to have a value that points to the curve or table object named in the following field.
+
+\paragraph{Field: Curve or Table Object Name}\label{field-curve-or-table-object-name}
+
+This field contains the unique name of a Curve:* or Table:* object defined elsewhere in the input file. The Erl variable in the previous field will be filled with the index for the curve or table named here. The value of this index tracks the order that Curve: and Table: input objects are listed in the input file.
+
+An example IDF object is:
+
+\begin{lstlisting}
+
+EnergyManagementSystem:CurveOrTableIndexVariable,
+  Curve_Quadratic_Ptr,             !- Name
+  HPACCOOLPLFFPLR_curve;         !- Curve or Table Object Name
+\end{lstlisting}
+
+\subsection{EnergyManagementSystem:ConstructionIndexVariable}\label{energymanagementsystemconstructionindexvariable}
+
+The EMS provides actuators for overriding the type of construction used by a surface. The EnergyManagementSystem:ConstructionIndexVariable input object is used to setup an Erl variable that contains an index that points to specific Construction. This index variable is then used with a special actuator called Surface with the control type Construction State. See the Application Guide for EMS for more information on how to use this index variable and the associated actuator.
+
+\subsubsection{Inputs}\label{inputs-10-004}
+
+\paragraph{Field: Name}\label{field-name-10-004}
+
+This field contains a unique name for the index variable that becomes the name of a variable for use in Erl programs. No spaces are allowed in the name. This name will be a global variable in Erl programs and cannot duplicate any other global scope EMS variable. The variable will be filled by the EMS system to have a value that points to the Construction object named in the following field.
+
+\paragraph{Field: Construction Object Name}\label{field-construction-object-name}
+
+This field contains the unique name of a Construction object defined elsewhere in the input file. The Erl variable in the previous field will be filled with the index for the Construction named here. The value of this index tracks the order that Construction input objects are listed in the input file.
+
+An example IDF object is:
+
+\begin{lstlisting}
+
+Construction,
+  TCwindow_25,                               !- Name
+  Clear3PPG,                             !- Outside Layer
+  AIR 3MM,                                 !- Layer 2
+  WO18RT25,                           !- Layer 3
+  AIR 8MM,                                 !- Layer 4
+  SB60Clear3PPG;                     !- Layer 5
+
+
+  EnergyManagementSystem:ConstructionIndexVariable,
+  TCwindow_25,
+  TCwindow_25;
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-evaporative-coolers.tex b/doc/input-output-reference/src/overview/group-evaporative-coolers.tex
new file mode 100644
index 00000000000..27f692d1d76
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-evaporative-coolers.tex
@@ -0,0 +1,816 @@
+\section{Group Evaporative Coolers}\label{group-evaporative-coolers}
+
+This group of objects describes the properties and configuration for the evaporative coolers models for the HVAC section.
+
+\subsection{EvaporativeCooler:Direct:CelDekPad}\label{evaporativecoolerdirectceldekpad}
+
+The direct stage, shown in the figure below, consists of a rigid media evaporative pad, with water recirculated from a reservoir. The water is pumped from the reservoir to a water distribution header, for water feed by gravity from above the media. The evaporative pad provides the area for the adiabatic saturation of the air. While the process provides a lower dry-bulb temperature, the moisture content of the leaving air is higher than the entering condition. The direct stage is used for comfort cooling in a building where adding humidity to the air can be tolerated.
+
+\begin{figure}[hbtp] % fig 144
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image415.png}
+\caption{Direct Stage Evaporative Cooler \protect \label{fig:direct-stage-evaporative-cooler}}
+\end{figure}
+
+The thermodynamic process is a simultaneous heat and mass transfer, or adiabatic cooling, and follows a constant enthalpy line on the psychrometric chart, it is shown in the figure below as a process from A to B. Since the deviation of the constant wet-bulb line and the constant enthalpy line is small, it is assumed that the wet-bulb temperature is constant across the direct evaporative stage.
+
+\begin{figure}[hbtp] % fig 145
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image416.png}
+\caption{Psychrometric Chart -- Constant Enthalpy \protect \label{fig:psychrometric-chart-constant-enthalpy}}
+\end{figure}
+
+If the direct evaporative process were 100\% efficient, the leaving dry-bulb temperature would equal the entering wet-bulb temperature. The efficiency of the direct evaporative process is less than 100\% and by defining saturation efficiency (\(\varepsilon\) se) for the direct stage or evaporative pad, the leaving dry-bulb temperature can be expressed by the following equation.
+
+\begin{equation}
+{T_{db\,supout}} = {T_{db\,sup\,in}} - {\varepsilon_{se}}\cdot \left( {{T_{db\,sup\,in}} - {T_{wb\,sup\,in}}} \right)
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-016}
+
+\paragraph{Field: Name}\label{field-name-015}
+
+A unique identifying name for each evaporative cooler.
+
+\paragraph{Field:Availability Schedule Name}\label{fieldavailability-schedule-name}
+
+The name of a schedule which defines when the evaporative cooler is available. A schedule value of 0 indicates that the evaporative cooler is off for that time period. A schedule value greater than 0 indicates that the evaporative cooler can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Direct Pad Area}\label{field-direct-pad-area}
+
+The face area of the evaporative pad in m\(^{2}\). With the area and mass flow rate, the air velocity is calculated and is used to determine the saturation efficiency. This field is autosizable.
+
+\paragraph{Field: Direct Pad Depth}\label{field-direct-pad-depth}
+
+The depth of the evaporative pad in meters. The pad depth is used to determine the saturation efficiency. This field is autosizable.
+
+\paragraph{Field: Recirculating Water Pump Power Consumption}\label{field-recirculating-water-pump-power-consumption}
+
+This field is used to specify the power consumed by the evaporative cooler recirculating pump in Watts.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-001}
+
+The name of the evaporative cooler air inlet node from the Air Loop Simulation.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-001}
+
+The name of the evaporative cooler air outlet node from the Air Loop Simulation.
+
+\paragraph{Field: Control Type}\label{field-control-type-001}
+
+This input field is currently unused and can be left blank.
+
+\paragraph{Field: Water Supply Storage Tank Name}\label{field-water-supply-storage-tank-name-000}
+
+This field is optional. It is used to describe where the cooler obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the cooler will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains.
+
+An IDF example showing how this object is:
+
+\begin{lstlisting}
+
+EvaporativeCooler:Direct:CelDekPad,
+  Evaporative Cooler,           !- Name
+  System Availability Schedule,   !- Availability Schedule Name
+  0.6,                                         !- Direct Pad Area {m2}
+  0.2,                                         !- Direct Pad Depth {m}
+  225,                                         !- Recirculating Water Pump Power Consumption {W}
+  Evap Cooler Inlet Node,   !- Air Inlet Node Name
+  Supply Outlet Node;           !- Air Outlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-011}
+
+The output variables that are available for this direct evaporative cooler are shown below:
+
+\begin{itemize}
+\item
+  HVAC,Average, Evaporative Cooler Wet Bulb Effectiveness
+\item
+  HVAC,Average, Evaporative Cooler Electric Power{[}W{]}
+\item
+  HVAC,Sum, Evaporative Cooler Electric Energy {[}J{]}
+\item
+  HVAC,Sum, Evaporative Cooler Water Volume{[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Mains Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Starved Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Starved Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Evaporative Cooler Wet Bulb Effectiveness}\label{evaporative-cooler-wet-bulb-effectiveness}
+
+The effectivenss, or saturation efficiency, is the temperature change of the supply air divided by the difference between the inlet air dry-bulb and wet-bulb temperatures. In other words, it is a measure of the approach to the inlet air wet-bulb temperature.
+
+\paragraph{Evaporative Cooler Electric Power{[}W{]}}\label{evaporative-cooler-electric-powerw}
+
+\paragraph{Evaporative Cooler Electric Energy {[}J{]}}\label{evaporative-cooler-electric-energy-j}
+
+These output variables report the electric power and electric energy required to operate the water pump.
+
+\paragraph{Evaporative Cooler Water Volume {[}m3{]}}\label{evaporative-cooler-water-volume-m3}
+
+The water consumption is the water evaporated from the pad. This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down. This output variable appears when mains water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Mains Water Volume {[}m3{]}}\label{evaporative-cooler-mains-water-volume-m3}
+
+This is the source of the water consumed. This output variable appears when mains water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Storage Tank Water Volume {[}m3{]}}\label{evaporative-cooler-storage-tank-water-volume-m3}
+
+The water consumption is the water evaporated from the pad. This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down. This output variable appears when storage tank water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Starved Water Volume {[}m3{]}}\label{evaporative-cooler-starved-water-volume-m3}
+
+This is the water consumed by the evaporative cooler that could not accually be met by the storage tank. This output variable appears when storage tank water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Starved Mains Water Volume {[}m3{]}}\label{evaporative-cooler-starved-mains-water-volume-m3}
+
+This is the source (mains) of water consumed by the evaporative cooler that could not accually be met by the storage tank. This output variable appears when storage tank water is supplied to the cooler.
+
+\subsection{EvaporativeCooler:Direct:ResearchSpecial}\label{evaporativecoolerdirectresearchspecial}
+
+This cooler is similar in principal to the EvaporativeCooler:Direct:CelDekPad. The model differs in that it gives the user a simple way of specify the cooler effectiveness. Using the ResearchSpecial input object also allows the cooler to control the amount of cooling based on node setpoints (controlled by SetpointManagers). This avoid problems from over cooling when conditions are such that loads are low and cooling power is high.
+
+The model allows to vary the effectiveness depending on the primary air flow rates. The design effectiveness is modified by multiplying with Effectiveness Flow Fraction Modifier Curve value. The flow fraction is the ratio of the current primary airflow rate to the design flow rate. The recirculating and spray water pump power is assumed to vary with the primary air flow. The design pump power is modified using user specified pump modifier curve value. The normalized pump power modifier curve is a function of primary air flow fraction as a independent variable.
+
+Also the direct evaporative cooler operating range can be controlled depending on the entering air dry bulb and wet bulb temperatures. The operating range controlled based on minimum and maximum inlet node air temperature limits. The evaporative cooler can be turned on or off depending user specified minimum and maximum temperature limits. If the inlet node entering air temperature is lower or higher than the minimum and maximum limits, respectively, then the direct research special evaporative cooler is turned off. If these two input fields are left blank then, no user specified operating temperature control is applied. Operating range control feature is primarily intended for application in data centers.
+
+\subsubsection{Inputs}\label{inputs-1-014}
+
+\paragraph{Field: Name}\label{field-name-1-013}
+
+A unique identifying name for each cooler.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-006}
+
+The name of a schedule that defines when the evaporative cooler is available. A schedule value of 0 indicates that the evaporative cooler is off for that time period. A schedule value greater than 0 indicates that the evaporative cooler can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Cooler Design Effectiveness}\label{field-cooler-design-effectiveness}
+
+This field specifies the effectiveness at design flow rate that is applied to the wetbulb depression to determine the conditions leaving the cooler. This model assumes that the effectiveness can vary with supply air flow rate. For effectiveness variation with supply air flow fraction enter the Effectiveness Flow Ratio Modifier Curve Name input field below. The flow fraction is the ratio of the sum of current primary air and secondary air sides flow rates and the sum of the design flow rates.
+
+\paragraph{Field: Effectiveness Flow Ratio Modifier Curve Name}\label{field-effectiveness-flow-ratio-modifier-curve-name}
+
+This curve modifies the effectiveness design value specified the previous field by multiplying the value by the result of this curve. The modifying curve is a function of flow fraction, which is the ratio of the current primary air flow rates divided by the design primary air flow rates. If this input field is left blank, the effectiveness is assumed to be constant. Any curve or table with one independent variable can be used. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
+
+\paragraph{Field:Primary Design Air Flow Rate}\label{fieldprimary-design-air-flow-rate}
+
+This numeric input field is the primary air design air flow rate in m3/s. This input field is autosizable. If the evaporative cooler is on main air loop branch, the design flow rate is the same as branch design flow rate, or else if it is on outdoor air system it will be the maximum of the the outdoor air design flow rate and the half of the primary air flow rate on the main air loop branch.
+
+\paragraph{Field: Recirculationg Water Pump Design Power}\label{field-recirculationg-water-pump-design-power}
+
+This numeric input field is the recirculating and spray pump electric power at Secondary Design Air Flow Rate in W. This is the nominal water recirculating and spray pump power of evaporative cooler at primary air design flow rates and cooler design effectiveness. This input field is autosizable. Average Pump Power sizing factor was estimated from pump power and primary air design flow rates inputs from energyplus example files is about 90.0 {[}W/(m3/s){]} ( = 90.0 \textasciitilde{} Pump Power / Primary Air Design Flow Rate). The factor ranges from 55.0 to 150.0 {[}W/(m3/s){]}.
+
+\paragraph{Field: Water Pump Power Sizing Factor}\label{field-water-pump-power-sizing-factor}
+
+This numeric input field value is recirculating water pump sizing factor in W/(m3/s). This field is used when the previous field is set to autosize. The pump design electric power is scaled with Secondary Design Air Flow Rate. This input field is autosizable. Average Pump Power sizing factor was estimated from pump power and primary air design flow rates inputs from energyplus example files is about 90.0 {[}W/(m3/s){]} ( = 90.0 \textasciitilde{} Pump Power / Primary Air Design Flow Rate). The factor ranges from 55.0 to 150.0 {[}W/(m3/s){]}.
+
+\paragraph{Field: Water Pump Power Modifier Curve Name}\label{field-water-pump-power-modifier-curve-name}
+
+This alpha input field is the name of a dimensionless normalized pump power modifying curve. This curve modifies the pump electric power in the previous field by multiplying the design power by the result of this curve. The normalized curve is a function of the primary air flow fraction as independent variable. The curve shall yield a value of 1.0 at a flow fraction of 1.0. The flow fraction is the ratio of the primary air during current operation divided by primary air Design Air Flow Rate. If this input field is left blank, the pump power is assumed to lineary vary with the load. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-1-001}
+
+The name of the air inlet node for the primary air flow path through the cooler.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-1-000}
+
+The name of the air outlet node for the primary air flow path through the cooler.
+
+\paragraph{Field: Sensor Node Name}\label{field-sensor-node-name-001}
+
+This field specifies the name of a node that will provide system air temperature setpoint information. A separate SetpointManager object should be setup to update this node.
+
+\paragraph{Field: Water Supply Storage Tank Name}\label{field-water-supply-storage-tank-name-1}
+
+This field is optional. It is used to describe where the cooler obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the cooler will attempt to obtain all the water it uses from the tank. However, if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains.
+
+\paragraph{Field: Drift Loss Fraction}\label{field-drift-loss-fraction}
+
+This field is optional and can be used to model additional water consumed by the cooler from drift. Drift is water that leaves the cooling media as droplets and does not evaporate into the process air stream. For example, water may get blown off the evaporative media by winds and escape the air system. The value entered here is a simple fraction of the water consumed by the cooler for normal process evaporation. The amount of drift is this fraction times the water evaporated for the normal cooling process. This field can be left blank and then there will be no added water consumption from drift.
+
+\paragraph{Field: Blowdown Concentration Ratio}\label{field-blowdown-concentration-ratio-000}
+
+This field is optional and can be used to model additional water consumed by the cooler from blowdown. Blowdown is water that is intentionally drained from the cooler s sump to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values are 3 to 5. The default is 3.0.
+
+\paragraph{Field: Evaporative Cooler Operation Minimum Drybulb Temperature}\label{field-evaporative-cooler-operation-minimum-drybulb-temperature}
+
+This numeric field defines the evaporative cooler inlet node drybulb temperature minimum limit in degrees Celsius. The evaporative cooler will be turned off when evaporator cooler air inlet node dry-bulb temperature falls below this value. The typical minimum value is 16 °C. Users are allowed to specify their own limits. If this field is left blank, then there is no drybulb temperature lower limit for evaporative cooler operation.
+
+\paragraph{Field: Evaporative Operation Maximum Limit Wetbulb Temperature}\label{field-evaporative-operation-maximum-limit-wetbulb-temperature}
+
+This numeric field defines the evaporative cooler air inlet node air wetbulb temperature maximum limits in degree Celsius. When the evaporative cooler air inlet node air wetbulb temperature exceeds this limit, then the evaporative cooler is turns off. The typical maximum value is 24 °C. If this input field is left blank, then there is no wetbulb temperature upper limit for evaporative cooler operation.
+
+\paragraph{Field: Evaporative Operation Maximum Limit Drybulb Temperature}\label{field-evaporative-operation-maximum-limit-drybulb-temperature}
+
+This numeric field defines the evaporative cooler air inlet node drybulb temperature maximum limits in degree Celsius. The evaporative cooler will be turned off when the evaporative cooler air inlet node drybulb temperature exceeds this value. The typical maximum value is 28 °C. If this input field is left blank, then there is no upper drybulb temperature limit for evaporative cooler operation.
+
+An example IDF entry is
+
+\begin{lstlisting}
+
+EvaporativeCooler:Direct:ResearchSpecial,
+  Direct Evap Cooler, !- Name
+  ALWAYS_ON, !- Availability Schedule Name
+  0.7 , !- Cooler Design Effectiveness
+  ,     !- Effectiveness Flow Ratio Modifier Curve Name
+  30.0 , !- Recirculating Water Pump Design Power
+  ,     !- Water Pump Power Sizing Factor
+  ,     !- Water Pump Power Modifier Curve Name
+  OAIndRDD Evap Cooler- OADirect Evap CoolerNode , !- Air Inlet Node Name
+  OADirect Evap Cooler- OAMixing BoxNode, !- Air Outlet Node Name
+  OADirect Evap Cooler- OAMixing BoxNode, !- Sensor Node Name
+  , !- Water Supply Storage Tank Name
+  0.0, !- Drift Loss Fraction
+  3; !- Blowdown Concentration Ratio
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-009}
+
+The output variables that are available for this direct evaporative cooler are shown below:
+
+\begin{itemize}
+\item
+  HVAC,Average, Evaporative Cooler Electric Power{[}W{]}
+\item
+  HVAC,Average, Evaporative Cooler Stage Effectiveness {[]}
+\item
+  HVAC,Sum, Evaporative Cooler Electric Energy {[}J{]}
+\item
+  HVAC,Sum, Evaporative Cooler Water Volume{[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Mains Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Starved Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Starved Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Evaporative Cooler Electric Power{[}W{]}}\label{evaporative-cooler-electric-powerw-1}
+
+\paragraph{Evaporative Cooler Electric Energy {[}J{]}}\label{evaporative-cooler-electric-energy-j-1}
+
+These output variables report the electric power and electric energy required to operate the water pump.
+
+\paragraph{\texorpdfstring{Evaporative Cooler Stage Effectiveness {[]}}{Evaporative Cooler Stage Effectiveness }}\label{evaporative-cooler-stage-effectiveness}
+
+The cooler stage efficiency is defined as the temperature change of the supply air divided by the difference between the outdoor dry-bulb and wet-bulb temperatures, including the effect of the reduction in the primary air flow rate in other words, it is a measure of the approach to the entering air wet-bulb temperature.
+
+\paragraph{Evaporative Cooler Water Volume {[}m3{]}}\label{evaporative-cooler-water-volume-m3-1}
+
+The water consumption is the water evaporated from the pad. This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down. This output variable appears when mains water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Mains Water Volume {[}m3{]}}\label{evaporative-cooler-mains-water-volume-m3-1}
+
+This is the source of the water consumed. This output variable appears when mains water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Storage Tank Water Volume {[}m3{]}}\label{evaporative-cooler-storage-tank-water-volume-m3-1}
+
+The water consumption is the water evaporated from the pad. This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down. This output variable appears when storage tank water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Starved Water Volume {[}m3{]}}\label{evaporative-cooler-starved-water-volume-m3-1}
+
+This is the water consumed by the evaporative cooler that could not accually be met by the storage tank. This output variable appears when storage tank water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Starved Mains Water Volume {[}m3{]}}\label{evaporative-cooler-starved-mains-water-volume-m3-1}
+
+This is the source (mains) of water consumed by the evaporative cooler that could not accually be met by the storage tank. This output variable appears when storage tank water is supplied to the cooler.
+
+\subsection{EvaporativeCooler:Indirect:CelDekPad}\label{evaporativecoolerindirectceldekpad}
+
+The dry coil indirect evaporative cooler, shown in the figure below, has a rigid media pad, similar to the direct evaporative stage, where the adiabatic cooling takes place. The secondary air leaves the rigid media pad and enters an air to air heat exchanger where it cools the supply air flowing through the heat exchanger tubes. The moist secondary air is then exhausted to the environment. The secondary air stream has its own fan and consists of a rigid media evaporative pad, with water recirculated from a reservoir. The water is pumped from the reservoir to a water distribution header, for water feed by gravity from above the media. The evaporative pad provides the area for the adiabatic saturation of the air.
+
+\begin{figure}[hbtp] % fig 146
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image419.png}
+\caption{Evaporative Cooler -- Indirect Dry Coil \protect \label{fig:evaporative-cooler-indirect-dry-coil}}
+\end{figure}
+
+The process that the secondary air goes through, A to C to D, is shown by the dashed lines in the following figure. Process A to C is adiabatic cooling in the rigid media pad. Then the air enters the shell side of the heat exchanger and is sensibly heated from C to D by the warm supply air passing through the tube side. The secondary air inlet is modeled as a separate stream of outdoor air and the user has the option of defining the name of an outdoor air node.
+
+\begin{figure}[hbtp] % fig 147
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image420.png}
+\caption{Secondary Air Process -- Indirect Dry Coil Evap Cooler \protect \label{fig:secondary-air-process-indirect-dry-coil-evap}}
+\end{figure}
+
+The advantage of the dry coil heat exchanger is that the heat exchanger does not have the evaporation taking place on the outside of the tubes, thus no mineral deposits are left on the heat exchange surface to reduce the efficiency of the heat exchanger. The rigid media pads are designed to flush the mineral deposits to the sump, so the saturation efficiency of the pad stays relatively constant.
+
+\subsubsection{Inputs}\label{inputs-2-013}
+
+\paragraph{Field: Name}\label{field-name-2-012}
+
+A unique identifying name for each evaporative cooler.
+
+\paragraph{Field:Availability Schedule Name}\label{fieldavailability-schedule-name-1}
+
+The name of a schedule which defines when the evaporative cooler is available. A schedule value of 0 indicates that the evaporative cooler is off for that time period. A schedule value greater than 0 indicates that the evaporative cooler can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Direct Pad Area}\label{field-direct-pad-area-1}
+
+The face area of the evaporative pad in m\(^{2}\). With the area and mass flow rate, the air velocity is calculated and is used to determine the saturation efficiency on the secondary side of the evaporative cooler. This field is autosizable.
+
+\paragraph{Field: Direct Pad Depth}\label{field-direct-pad-depth-1}
+
+The depth of the evaporative pad in meters. The pad depth is used to determine the saturation efficiency on the secondary side of the evaporative cooler. This field is autosizable.
+
+\paragraph{Field: Recirculating Water Pump Power Consumption}\label{field-recirculating-water-pump-power-consumption-1}
+
+This field is used to specify the power consumed by the evaporative cooler recirculating pump in Watts.
+
+\paragraph{Field: Secondary Air Fan Flow Rate}\label{field-secondary-air-fan-flow-rate}
+
+This field is used to specify the secondary air fan flow rate and is specified in m\(^{3}\)/sec.
+
+\paragraph{Field: Secondary Fan Total Efficiency}\label{field-secondary-fan-total-efficiency}
+
+This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1.
+
+\paragraph{Field: Secondary Fan Delta Pressure}\label{field-secondary-fan-delta-pressure}
+
+This field is used to specify the delta pressure across the secondary stage of the evaporative cooler in Pascals.
+
+\paragraph{Field: Indirect Heat Exchanger Effectiveness}\label{field-indirect-heat-exchanger-effectiveness}
+
+This field is used to specify the effectiveness of the indirect heat exchanger between the primary and secondary air flow.
+
+\paragraph{Field: Primary Air Inlet Node Name}\label{field-primary-air-inlet-node-name-000}
+
+The name of the evaporative cooler s primary air inlet node from the Air Loop Simulation. This is the air flow being cooled indirectly.
+
+\paragraph{Field: Primary Air Outlet Node Name}\label{field-primary-air-outlet-node-name-000}
+
+The name of the evaporative cooler s primary air outlet node from the Air Loop Simulation.
+
+\paragraph{Field: Control Type}\label{field-control-type-1}
+
+This input field is currently unused and can be left blank.
+
+\paragraph{Field: Water Supply Storage Tank Name}\label{field-water-supply-storage-tank-name-2}
+
+This field is optional. It is used to describe where the cooler obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the cooler will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains.
+
+\paragraph{Field: Secondary Air Inlet Node Name}\label{field-secondary-air-inlet-node-name-000}
+
+This field is optional. It is used to explicitly define an outdoor air node for the inlet for secondary air stream. Defining an outdoor air node here allows using the height-dependent model for outdoor air conditions.
+
+And an IDF example showing how this object is specified:
+
+\begin{lstlisting}
+
+EvaporativeCooler:Indirect:CelDekPad,
+  IndirectEvapCooler1,         !- Name
+  FanAndCoilAvailSched,       !- Availability Schedule Name
+  0.6,                                         !- Direct Pad Area {m2}
+  0.2,                                         !- Direct Pad Depth {m}
+  225.,                                       !- Recirculating Water Pump Power Consumption {W}
+  1.0,                                         !- Secondary Air Fan Flow Rate {m3/s}
+  0.7,                                         !- Secondary Fan Total Efficiency
+  200.0,                                     !- Secondary Fan Delta Pressure {Pa}
+  0.67,                                       !- Indirect Heat Exchanger Effectiveness
+  EvapCoolerIndirectInletAirNode,   !- Primary Air Inlet Node Name
+  EvapCoolerDirectInletAirNode,   !- Primary Air Outlet Node Name
+  ,                                           !- Control Type
+  ,                                               !- Water Supply Storage Tank Name
+  Secondary side OA inlet node;   !- Secondary Air Inlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-008}
+
+The output variables that are available for the indirect dry evaporative cooler are shown below:
+
+\begin{itemize}
+\item
+  HVAC,Average, Evaporative Cooler Wetbulb Effectiveness
+\item
+  HVAC,Average, Evaporative Cooler Total Stage Effectiveness
+\item
+  HVAC,Average, Evaporative Cooler Electric Power{[}W{]}
+\item
+  HVAC,Sum, Evaporative Cooler Electric Energy {[}J{]}
+\item
+  HVAC,Sum, Evaporative Cooler Water Volume{[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Mains Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Starved Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Starved Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Evaporative Cooler Wetbulb Effectiveness}\label{evaporative-cooler-wetbulb-effectiveness}
+
+The dry evaporation saturation efficiency is the saturation efficiency of the secondary or wet side air stream defined as the temperature change of the supply air divided by the difference between the outdoor dry-bulb and wet-bulb temperatures. In other words, it is a measure of the approach to the outdoor wet-bulb temperature.
+
+\paragraph{Evaporative Cooler Total Stage Effectiveness}\label{evaporative-cooler-total-stage-effectiveness}
+
+The total stage efficiency includes the sensible heat exchanger effectiveness of the heat exchanger in the supply air stream. It is the saturation efficiency multiplied by the heat exchanger effectiveness.
+
+\paragraph{Evaporative Cooler Electric Power{[}W{]}}\label{evaporative-cooler-electric-powerw-2}
+
+\paragraph{Evaporative Cooler Electric Energy {[}J{]}}\label{evaporative-cooler-electric-energy-j-2}
+
+These output variables report the electric power and energy consumed by the secondary air fan and the sump pump.
+
+\paragraph{Evaporative Cooler Water Volume{[}m3{]}}\label{evaporative-cooler-water-volumem3}
+
+The water consumption is the water evaporated from the pad. This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down. This output variable appears when mains water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Mains Water Volume {[}m3{]}}\label{evaporative-cooler-mains-water-volume-m3-2}
+
+This is the source of the water consumed. This output variable appears when mains water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Storage Tank Water Volume {[}m3{]}}\label{evaporative-cooler-storage-tank-water-volume-m3-2}
+
+The water consumption is the water evaporated from the pad. This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down. This output variable appears when storage tank water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Starved Water Volume {[}m3{]}}\label{evaporative-cooler-starved-water-volume-m3-2}
+
+This is the water consumed by the evaporative cooler that could not accually be met by the storage tank. This output variable appears when storage tank water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Starved Mains Water Volume {[}m3{]}}\label{evaporative-cooler-starved-mains-water-volume-m3-2}
+
+This is the source (mains) of water consumed by the evaporative cooler that could not accually be met by the storage tank. This output variable appears when storage tank water is supplied to the cooler.
+
+\subsection{EvaporativeCooler:Indirect:WetCoil}\label{evaporativecoolerindirectwetcoil}
+
+The wetted coil evaporative cooler shown in the figure below, has water sprayed directly on the tubes of the heat exchanger where latent cooling takes place. The vaporization of the water on the outside of the heat exchanger tubes allows the simultaneous heat and mass transfer which removes heat from the supply air on the tube side. Then the moist secondary air is exhausted. The secondary air stream has its own fan.
+
+\begin{figure}[hbtp] % fig 148
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image421.png}
+\caption{Evaporative Cooler Indirect Wet Coil \protect \label{fig:evaporative-cooler-indirect-wet-coil}}
+\end{figure}
+
+The process that the secondary air goes through, A to C on the following figure, is a path of simultaneous heat and mass transfer, but it does not follow a line of constant enthalpy as in the direct stage. The process is not adiabatic due to the heat gain from the supply air flowing through the tubes of the heat exchanger.
+
+\begin{figure}[hbtp] % fig 149
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image422.png}
+\caption{Secondary Air Process Indirect Wet Coil Evap Cooler \protect \label{fig:secondary-air-process-indirect-wet-coil-evap}}
+\end{figure}
+
+The wet coil heat exchanger can have a higher stage efficiency than the dry coil due to a higher heat transfer rate on the outside of the heat exchanger tubes. Over the operating lifetime of the heat exchanger, the vaporization taking place on the heat exchange surface can leave mineral deposits which will decrease the effectiveness of the heat exchanger.
+
+\subsubsection{Inputs}\label{inputs-3-012}
+
+\paragraph{Field: Name}\label{field-name-3-011}
+
+A unique identifying name for each evaporative cooler.
+
+\paragraph{Field:Availability Schedule Name}\label{fieldavailability-schedule-name-2}
+
+The name of a schedule which defines when the evaporative cooler is available. A schedule value of 0 indicates that the evaporative cooler is off for that time period. A schedule value greater than 0 indicates that the evaporative cooler can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Coil Maximum Efficiency}\label{field-coil-maximum-efficiency}
+
+The maximum efficiency of the stage is a combination of the efficiency due to the simultaneous heat and mass transfer on the outside of the tube and the efficiency of the heat exchanger. This value can be higher than the dry coil overall efficiency since the convective coefficients on the outside of the tube are larger.
+
+\paragraph{Field: Coil Flow Ratio}\label{field-coil-flow-ratio}
+
+The Coil Flow Ratio is determined from performance data. The Coil Flow Ratio tells how quickly the efficiency of the stage would decrease with a mismatch of the supply and secondary flows.
+
+\paragraph{Field: Recirculating Water Pump Power Consumption}\label{field-recirculating-water-pump-power-consumption-2}
+
+This field is used to specify the power consumed by the evaporative cooler recirculating pump in Watts.
+
+\paragraph{Field: Secondary Air Fan Flow Rate}\label{field-secondary-air-fan-flow-rate-1}
+
+This field is used to specify the secondary air fan flow rate and is specified in m\(^{3}\)/sec.
+
+\paragraph{Field: Secondary Air Fan Total Efficiency}\label{field-secondary-air-fan-total-efficiency}
+
+This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1..
+
+\paragraph{Field: Secondary Air Fan Delta Pressure}\label{field-secondary-air-fan-delta-pressure}
+
+This field is used to specify the delta pressure across the secondary stage of the evaporative cooler in Pascals.
+
+\paragraph{Field: Primary Air Inlet Node Name}\label{field-primary-air-inlet-node-name-1}
+
+The name of the evaporative cooler air inlet from the Air Loop Simulation.
+
+\paragraph{Field: Primary Air Outlet Node Name}\label{field-primary-air-outlet-node-name-1}
+
+The name of the evaporative cooler air outlet from the Air Loop Simulation.
+
+\paragraph{Field: Control Type}\label{field-control-type-2}
+
+This input field is currently unused and can be left blank.
+
+\paragraph{Field: Water Supply Storage Tank Name}\label{field-water-supply-storage-tank-name-3}
+
+This field is optional. It is used to describe where the cooler obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the cooler will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains.
+
+\paragraph{Field: Secondary Air Inlet Node Name}\label{field-secondary-air-inlet-node-name-1-000}
+
+This field is optional. It is used to explicitly define an outdoor air node for the inlet for secondary air stream. Defining an outdoor air node here allows using the height-dependent model for outdoor air conditions.
+
+\paragraph{Field: Drift Loss Fraction}\label{field-drift-loss-fraction-1}
+
+This field is optional and can be used to model additional water consumed by the cooler from drift. Drift is water that leaves the cooling media as droplets and does not evaporate into the process air stream. For example, water may get blown off the evaporative media by winds and escape the air system. The value entered here is a simple fraction of the water consumed by the cooler for normal process evaporation. The amount of drift is this fraction times the water evaporated for the normal cooling process. This field can be left blank and then there will be no added water consumption from drift.
+
+\paragraph{Field: Blowdown Concentration Ratio}\label{field-blowdown-concentration-ratio-1-000}
+
+This field is optional and can be used to model additional water consumed by the cooler from blowdown. Blowdown is water that is intentionally drained from the cooler s sump to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values are 3 to 5. The default is 3.0.
+
+And an IDF example showing how this object is specified:
+
+\begin{lstlisting}
+
+EvaporativeCooler:Indirect:WetCoil,
+  IndirectEvapCooler1,         !- Name
+  FanAndCoilAvailSched,       !- Availability Schedule Name
+  0.8,                                         !- Coil Maximum Efficiency
+  0.16,                                       !- Coil Flow Ratio
+  225.,                                       !- Recirculating Water Pump Power Consumption {W}
+  1.0,                                         !- Secondary Air Fan Flow Rate {m3/s}
+  0.7,                                         !- Secondary Air Fan Total Efficiency
+  200.0,                                     !- Secondary Air Fan Delta Pressure {Pa}
+  EvapCoolerIndirectInletAirNode,   !- Primary Air Inlet Node Name
+  EvapCoolerDirectInletAirNode,   !- Primary Air Outlet Node Name
+  ,                                               !- Control Type
+  ,                                               !- Water Supply Storage Tank Name
+  Secondary side OA inlet node;   !- Secondary Air Inlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-006}
+
+The output variables that are available for the wet indirect evaporative cooler are shown below:
+
+\begin{itemize}
+\item
+  HVAC,Average, Evaporative Cooler Total Stage Effectiveness
+\item
+  HVAC,Average, Evaporative Cooler Electric Power{[}W{]}
+\item
+  HVAC,Sum, Evaporative Cooler Electric Energy {[}J{]}
+\item
+  HVAC,Sum, Evaporative Cooler Water Volume{[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Mains Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Starved Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Starved Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Evaporative Cooler Total Stage Effectiveness {[]}}{Evaporative Cooler Total Stage Effectiveness }}\label{evaporative-cooler-total-stage-effectiveness-1}
+
+The Total Stage Efficiency is defined as the temperature change of the supply air divided by the difference between the outdoor dry-bulb and wet-bulb temperatures, including the effect of the reduction in flow because of the secondary air stream. In other words, it is a measure of the approach to the outdoor wet-bulb temperature.
+
+\paragraph{Evaporative Cooler Electric Power {[}W{]}}\label{evaporative-cooler-electric-power-w}
+
+\paragraph{Evaporative Cooler Electric Energy {[}J{]}}\label{evaporative-cooler-electric-energy-j-3}
+
+These output variables report the electric power and energy that are consumed by the secondary air fan and the sump pump.
+
+\paragraph{Evaporative Cooler Water Volume {[}m3{]}}\label{evaporative-cooler-water-volume-m3-2}
+
+The water consumption is the water evaporated from the pad. This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down. This output variable appears when mains water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Mains Water Volume {[}m3{]}}\label{evaporative-cooler-mains-water-volume-m3-3}
+
+This is the source of the water consumed. This output variable appears when mains water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Storage Tank Water Volume {[}m3{]}}\label{evaporative-cooler-storage-tank-water-volume-m3-3}
+
+The water consumption is the water evaporated from the pad. This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down. This output variable appears when storage tank water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Starved Water Volume {[}m3{]}}\label{evaporative-cooler-starved-water-volume-m3-3}
+
+This is the water consumed by the evaporative cooler that could not accually be met by the storage tank. This output variable appears when storage tank water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Starved Mains Water Volume {[}m3{]}}\label{evaporative-cooler-starved-mains-water-volume-m3-3}
+
+This is the source (mains) of water consumed by the evaporative cooler that could not accually be met by the storage tank. This output variable appears when storage tank water is supplied to the cooler.
+
+\subsection{EvaporativeCooler:Indirect:ResearchSpecial}\label{evaporativecoolerindirectresearchspecial}
+
+This cooler is similar in principal to the EvaporativeCooler:Indirect:CelDekPad and EvaporativeCooler:Indirect:WetCoil (see Figure~\ref{fig:secondary-air-process-indirect-dry-coil-evap}, Figure~\ref{fig:evaporative-cooler-indirect-wet-coil}, and Figure~\ref{fig:secondary-air-process-indirect-wet-coil-evap}). The model differs in that it gives the user more flexibility to specify the source of secondary air. The cooler effectiveness with respect to wetbulb depression is allowed to go beyond 1.0. Using the ResearchSpecial input object also allows the cooler to control the amount of cooling based on node setpoints (controlled by SetpointManagers). This avoid problems from over cooling when conditions are such that loads are low and cooling power is high. Fan power is assumed to vary linearly when the cooler is operating at less than full capacity.
+
+The indirect evaporative cooler research special calculation procedure allows accounting for dry and wet effectiveness value variation with flow fraction. Two effectiveness modifier curves are included as optional user inputs for this purpose. Effectiveness modifier curves operate on the design dry and wet effectiveness values. The flow fraction is calculated as a ratio of the sum of current primary and secondary air flow rates to the sum of the design flow rates. Model also accounts for fan and recirculation water pump power variation with secondary air flow rates using pump power modifying curve. The fan power is calculated by multiplying the design fan power using fan power modify curve value evaluated at current secondary air flow fraction. Similarly, recirculating pump power is is calculated by multiplying the design pump power by pump power modifier curve value evaluated at current secondary air flow fraction. If the secondary air fan and recirculating pump power modifier curves are not specified, then fan and pump power are assumed to vary linearly with part load fraction.
+
+\subsubsection{Inputs}\label{inputs-4-011}
+
+\paragraph{Field: Name}\label{field-name-4-010}
+
+A unique identifying name for each cooler.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-004}
+
+The name of a schedule that defines when the evaporative cooler is available. A schedule value of 0 indicates that the evaporative cooler is off for that time period. A schedule value greater than 0 indicates that the evaporative cooler can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Cooler Wetbulb Design Effectiveness}\label{field-cooler-wetbulb-design-effectiveness}
+
+This field specifies the design effectiveness that is applied to the wetbulb depression to determine the conditions leaving the cooler. This effectiveness is a complicated function of the efficiency with which heat and mass are transferred on the secondary side and the efficiency of heat exchange between the secondary and primary flows. The model assumes that the effectiveness a function of flow fraction. The flow fraction is the ratio of the sum of primary air and secondary air current flow rates and the sum of the primary air and secondary air design flow rates.
+
+\paragraph{Field: Wet Bulb Effectiveness Flow Ratio Modifier Curve Name}\label{field-wet-bulb-effectiveness-flow-ratio-modifier-curve-name}
+
+This curve modifies the wet bulb effectiveness design value specified the previous field by multiplying the value by the result of this curve. The modifying curve is a function of flow fraction, which is the ratio of the sum of the primary and secondary flow rates divided by the sum of the design flow rates. If this input field is left blank, the effectiveness is assumed to be constant. Any curve or table with one independent variable can be used. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
+
+\paragraph{Field: Cooler Drybulb Design Effectiveness}\label{field-cooler-drybulb-design-effectiveness}
+
+This input value is dry bulb design effectiveness of the evaporative cooler. This is the nominal design dry blub effectiveness with respect to dry bulb temperature difference, i.e., dry operation and at design air flow rates, and no water evaporation or spraying on the secondary side.
+
+\paragraph{Field Drybulb Effectiveness Flow Ratio Modifier Curve Name}\label{field-drybulb-effectiveness-flow-ratio-modifier-curve-name}
+
+This this curve modifies the drybulb effectiveness in the previous field (eff\_db\_design) by multiplying the design effectiveness value by the result of this curve. The curve is evaluated flow fraction as independent variable. The flow fraction is the ratio of sum of the primary and secondary flow rates divided by the sum of the design flow rates. If this input field is left blank, the effectiveness is assumed to be constant. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
+
+\paragraph{Field: Recirculating Water Pump Design Power}\label{field-recirculating-water-pump-design-power}
+
+This numeric input field is the recirculating pump electric power at Secondary Design Air Flow Rate in W. This is the nominal design pump power water recirculation and spray for evaporation at design secondary air flow rates and cooler design effectiveness. This input field is autosizable.
+
+\paragraph{Field: Water Pump Power Sizing Factor}\label{field-water-pump-power-sizing-factor-1}
+
+This numeric input field value is recirculating water pump sizing factor in W/(m3/s). This field is used when the previous field is set to autosize. The pump design electric power is scaled with Secondary Design Air Flow Rate. Average Pump Power sizing factor was estimated from pump power and secondary air design flow rates inputs from energyplus example files is about 90.0 {[}W/(m3/s){]} ( = 90.0 \textasciitilde{} Pump Power / Secondary Air Design Flow Rate). The factor ranges from 55.0 to 150.0 {[}W/(m3/s){]}.
+
+\paragraph{Field: Water Pump Power Modifier Curve Name}\label{field-water-pump-power-modifier-curve-name-1}
+
+This alpha input field is the name of a dimensionless normalized pump power modifying curve. This curve modifies the pump electric power in the previous field by multiplying the design power by the result of this curve. The normalized curve is a function of the secondary side flow fraction as independent variable. The curve shall yield a value of 1.0 at a flow fraction of 1.0. The flow fraction is the secondary air flow rate during operation divided by Secondary Design Air Flow Rate. If this input field is left blank, the pump power is assumed to be constant. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
+
+\paragraph{Field: Secondary Air Design Flow Rate}\label{field-secondary-air-design-flow-rate}
+
+This field is used to specify the secondary air fan flow rate and is specified in m\(^{3}\)/s. This flow rate would typically be similar in magnitude to the flow through the primary side. This field can be autosized. When it is autosized, the program detects if the component is in the main air loop or on an outdoor air path. If it is on the main air loop, then the flow rate is set to the AirLoopHVAC system s design supply air flow rate (which is the maximum required for heating and cooling). If it is on the outdoor air path, then the flow rate is set to the larger of either the design minimum outdoor air flow rate or one-half of the main air loop design flow rate. The flow rate is used to determine parasitic fan energy and cooler effectiveness. The flow rate (and fan power) is effectively reduced by cycling when the amount of cooling needs to be restricted for control purpose. This field can be autosized. When this input is autosized, the program calculates by scaling the Primary Air Design Flow Rate using secondary air scaling factor specified in the input field below.
+
+\paragraph{Field: Secondary Air Flow Scaling Factor}\label{field-secondary-air-flow-scaling-factor}
+
+This numeric input field is used to scale the secondary air design flow rate and it is dimensionless. This field is used when the previous field is set to autosize. The Primary Design Air Flow Rate is scaled using this factor to calculate the secondary design air flow rate.
+
+\paragraph{Field: Secondary Air Fan Design Power}\label{field-secondary-air-fan-design-power}
+
+This numeric input field is the fan electric power at Secondary Design Air Flow Rate. This is the nominal design electric power at full speed of the secondary air fan. This input field is autosizable.
+
+\paragraph{Field: Secondary Air Fan Sizing Specific Power}\label{field-secondary-air-fan-sizing-specific-power}
+
+This input field value is secondary air fan sizing specific power in W/(m3/s). This field is used when the previous field is set to autosize. The fan power is scaled with Secondary Design Air Flow Rate.
+
+\paragraph{Field: Secondary Air Fan Power Modifier Curve Name}\label{field-secondary-air-fan-power-modifier-curve-name}
+
+This input field is the name of a dimensionless normalized curve. The normalized curve modifies the design secondary air fan power in the previous field by multiplying the value by the result of this curve. The normalized curve is a function of the secondary side flow fraction as independent variable. The curve shall yield a value of 1.0 at a flow fraction of 1.0. The flow fraction is the secondary air flow rate during operation divided by Secondary Design Air Flow Rate. If this input field is left blank, the fan power is assumed to be constant. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
+
+\paragraph{Field: Primary Air Inlet Node Name}\label{field-primary-air-inlet-node-name-2}
+
+The name of the air inlet node for the primary air flow path through the cooler.
+
+\paragraph{Field: Primary Air Outlet Node Name}\label{field-primary-air-outlet-node-name-2}
+
+The name of the air outlet node for the primary air flow path through the cooler.
+
+\paragraph{Field:Primary Design Air Flow Rate}\label{fieldprimary-design-air-flow-rate-1}
+
+This numeric input field is the primary air design air flow rate in m3/s. This input field is autosizable. If the evaporative cooler is on main air loop branch, the design flow rate is the same as branch design flow rate, or else if it is on outdoor air system it will be the maximum of the the outdoor air design flow rate and the half of the primary air flow rate on the main air loop branch.
+
+\paragraph{Field: Dewpoint Effectiveness Factor}\label{field-dewpoint-effectiveness-factor}
+
+This field specifies an effectiveness that is applied to the dewpoint depression to determine a bound for the conditions leaving the cooler. The model uses the warmer of the two temperatures determined from wetbulb depression and dewpoint depression.
+
+\paragraph{Field: Secondary Air Inlet Node Name}\label{field-secondary-air-inlet-node-name-2}
+
+This field specifies the name of the node providing air to the secondary/wet side of the cooler. Typically this node could appear in an outdoor air node list or be part of an air system loop.
+
+\paragraph{Field: Secondary Air Outlet Node Name}\label{field-secondary-air-outlet-node-name}
+
+This alpha input field is the name of the secondary air side outlet node.
+
+\paragraph{Field: Sensor Node Name}\label{field-sensor-node-name-1}
+
+This field specifies the name of a node that will provide system air temperature setpoint information. A separate SetpointManager object should be setup to update this node.
+
+\paragraph{Field: Relief Air Inlet Node Name}\label{field-relief-air-inlet-node-name}
+
+This field is optional, but can be used to feed two sources of secondary air into the wet side of the cooler. Typical use is to run the air system relief air into the system. The model first uses all of the air flow available from this node and then adds the air flow from the secondary air inlet node to make up the total defined by Secondary air Fan Flow Rate.
+
+\paragraph{Field: Water Supply Storage Tank Name}\label{field-water-supply-storage-tank-name-4}
+
+This field is optional. It is used to describe where the cooler obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the cooler will attempt to obtain all the water it uses from the tank. However, if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains.
+
+\paragraph{Field: Drift Loss Fraction}\label{field-drift-loss-fraction-2}
+
+This field is optional and can be used to model additional water consumed by the cooler from drift. Drift is water that leaves the cooling media as droplets and does not evaporate into the process air stream. For example, water may get blown off the evaporative media by winds and escape the air system. The value entered here is a simple fraction of the water consumed by the cooler for normal process evaporation. The amount of drift is this fraction times the water evaporated for the normal cooling process. This field can be left blank and then there will be no added water consumption from drift.
+
+\paragraph{Field: Blowdown Concentration Ratio}\label{field-blowdown-concentration-ratio-2-000}
+
+This field is optional and can be used to model additional water consumed by the cooler from blowdown. Blowdown is water that is intentionally drained from the cooler s sump to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values are 3 to 5. The default is 3.0.
+
+\paragraph{Field: Evaporative Operation Minimum Limit Drybulb Temperature}\label{field-evaporative-operation-minimum-limit-drybulb-temperature}
+
+This input field value defines the secondary air inlet node drybulb temperature limits in degree Celsius. When the secondary side entering air dry bulb temperature drops below this limit, then the evaporative cooler operation mode changes to dry heat exchanger. Users specify their own limits. If this field is left blank, then there is no drybulb temperature lower limit for evaporative cooler operation. If operating range control is desired then this input field and the next two input fields should be specified or all the three should be left blank or left out. If no minimum drybulb temperature limit is required while there are maximum drybulb and wetbulb temperature limits then specify very low temperature limit value (e.g., -99.0 C).
+
+\paragraph{Field: Evaporative Operation Maximum Limit Wetbulb Temperature}\label{field-evaporative-operation-maximum-limit-wetbulb-temperature-1}
+
+This input field value defines the secondary air inlet node wetbulb temperature limits in degree Celsius. When the secondary side entering air wet bulb temperature exceeds this limit, then the evaporative cooler is turns off and does not attempt to do any cooling. If this field is left blank, then there is no wetbulb temperature maximum limit for evaporative cooler wet operation mode. If no upper wetbulb temperature limits is desired while there are minimum drybulb and maximum drybulb upper temperature limits then then specify very high maximum wetbulb temperature limit value (e.g.~99.0 C).
+
+\paragraph{Field: Evaporative Operation Maximum Limit Drybulb Temperature}\label{field-evaporative-operation-maximum-limit-drybulb-temperature-1}
+
+This input field value defines the secondary air inlet node drybulb temperature limits in degree Celsius. When the secondary side entering air drybulb temperature exceeds this limit, the evaporative cooler will not run in dry operation mode or may be turned off depending on its wetbulb temperature. If this field is left blank, then there is no drybulb temperature maximum limit for evaporative cooler dry operation mode.
+
+If no drybulb temperature limit is desired while there are minimum drybulb and maximum wetbulb temperature limits then specify very high maximum drybulb temperature limit value (e.g.~99.0 C).
+
+An IDF example is shown below:
+
+\begin{lstlisting}
+
+EvaporativeCooler:Indirect:ResearchSpecial,
+  DataC_IndirectEvapCooler,     !- Name
+  ALWAYS_ON,                    !- Availability Schedule Name
+  0.75,                         !- Cooler Wetbulb Design Effectiveness
+  ,              !- Wetbulb Effectiveness Flow Ratio Modifier Curve Name
+  ,                          !- Cooler Drybulb Design Effectiveness
+  ,              !- Drybulb Effectiveness Flow Ratio Modifier Curve Name
+  autosize,                     !- Recirculating Water Pump Power
+  autosize,                     !- Secondary Air Design Flow Rate  
+  1.0,                          !- Secondary Air Flow Scaling Factor
+
+  autosize,                     !- Secondary Air Fan Design Power
+  800.0,                        !- Secondary Air Fan Sizing Specific Power W
+  ,               !- Secondary Air Fan Power Modifier Curve Name
+  Return Air Node,              !- Primary Air Inlet Node Name
+  IndEC Outlet Node,            !- Primary Air Outlet Node Name
+  autosize,                     !- Primary Design Air Flow Rate  
+  0.9 ,                         !- Dewpoint Effectiveness Factor
+  IndEC OA Air Inlet Node,      !- Secondary Air Inlet Node Name
+  IndEC OA Air Outlet Node,     !- Secondary Air Outlet Node Name
+  IndEC Outlet Node,            !- Sensor Node Name
+  ,                             !- Relief Air Inlet Node Name
+  ,                             !- Water Supply Storage Tank Name
+  0.0,                          !- Drift Loss Fraction
+  ;                             !- Blowdown Concentration Ratio
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-004}
+
+The output variables that are available for the EvaporativeCooler:Indirect:ResearchSpecial object are shown below:
+
+\begin{itemize}
+\item
+  HVAC,Average,Evaporative Cooler Total Stage Effectiveness
+\item
+  HVAC,Average,Evaporative Cooler Part Load Ratio
+\item
+  HVAC,Average,Evaporative Cooler Dewpoint Bound Status
+\item
+  HVAC,Average,Evaporative Cooler Operating Mode Satus {[]}
+\item
+  HVAC,Sum,Evaporative Cooler Electric Energy {[}J{]}
+\item
+  HVAC,Average,Evaporative Cooler Electric Power {[}W{]}
+\item
+  HVAC,Sum,Evaporative Cooler Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Starved Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Evaporative Cooler Starved Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Evaporative Cooler Total Stage Effectiveness {[]}}{Evaporative Cooler Total Stage Effectiveness }}\label{evaporative-cooler-total-stage-effectiveness-2}
+
+The Total Stage Efficiency is defined as the temperature change of the supply air divided by the difference between the primary air entering dry-bulb temperature and the secondary air enterig wet-bulb temperature for wet operating mode or the the difference between the primary air entering dry-bulb temperature and the secondary air enterig dry-bulb temperature for dry operating mode, including the effect of the reduction in flow because of the secondary air stream. In other words, it is a measure of the approach to the secondary air wet-bulb temperature for wet operating mode, or it is a measure of the approach to the secondary air entering dry-bulb temperature for dry operating mode.
+
+\paragraph{\texorpdfstring{Evaporative Cooler Operating Mode Status {[]}}{Evaporative Cooler Operating Mode Status }}\label{evaporative-cooler-operating-mode-status}
+
+This output variable provides the operating modes or status of the indirect evaporative cooler. This output variable can have status indicator integer value of 0, 1, or 2 representing Off, Dry and Wet operating modes, respectively.
+
+\paragraph{\texorpdfstring{Evaporative Cooler Part Load Ratio {[]}}{Evaporative Cooler Part Load Ratio }}\label{evaporative-cooler-part-load-ratio}
+
+This output variable provides the part load fraction of the indirect cooler. The ResearchSpecial cooler model is able to modulate to meet a temperature set point to avoid over cooling. This output variable is the fraction formed by the ratio of the capacity needed over the maximum cooling capacity available. A value of 1.0 corresponds to full capacity cooling.
+
+\paragraph{\texorpdfstring{Evaporative Cooler Dewpoint Bound Status {[]}}{Evaporative Cooler Dewpoint Bound Status }}\label{evaporative-cooler-dewpoint-bound-status}
+
+This output variable is a flag that indicates if the modeling was based on dewpoint effectivenss rather than wetbulb effectiveness The ResearchSpecial model is usually based on wet-bulb approach, but since values in excess of 1.0 are allowed, there is a secondary constraint imposed by dewpoint. If the dewpoint effectiveness was applied, then this flag variable will have the value 1.0, otherwise it is 0.0.
+
+\paragraph{Evaporative Cooler Electric Power {[}W{]}}\label{evaporative-cooler-electric-power-w-1}
+
+\paragraph{Evaporative Cooler Electric Energy {[}J{]}}\label{evaporative-cooler-electric-energy-j-4}
+
+These output variables report the electric power and energy that are consumed by the secondary air fan and the sump pump.
+
+\paragraph{Evaporative Cooler Water Volume {[}m3{]}}\label{evaporative-cooler-water-volume-m3-3}
+
+The water consumption is the water evaporated from the pad. This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down. This output variable appears when mains water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Mains Water Volume {[}m3{]}}\label{evaporative-cooler-mains-water-volume-m3-4}
+
+This is the source of the water consumed. This output variable appears when mains water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Storage Tank Water Volume {[}m3{]}}\label{evaporative-cooler-storage-tank-water-volume-m3-4}
+
+The water consumption is the water evaporated from the pad. This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down. This output variable appears when storage tank water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Starved Water Volume {[}m3{]}}\label{evaporative-cooler-starved-water-volume-m3-4}
+
+This is the water consumed by the evaporative cooler that could not accually be met by the storage tank. This output variable appears when storage tank water is supplied to the cooler.
+
+\paragraph{Evaporative Cooler Starved Mains Water Volume {[}m3{]}}\label{evaporative-cooler-starved-mains-water-volume-m3-4}
+
+This is the source (mains) of water consumed by the evaporative cooler that could not accually be met by the storage tank. This output variable appears when storage tank water is supplied to the cooler.
diff --git a/doc/input-output-reference/src/overview/group-exterior-energy-use-equipment.tex b/doc/input-output-reference/src/overview/group-exterior-energy-use-equipment.tex
new file mode 100644
index 00000000000..9f48476f0bb
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-exterior-energy-use-equipment.tex
@@ -0,0 +1,176 @@
+\section{Group -- Exterior Energy Use Equipment}\label{group-exterior-energy-use-equipment}
+
+To facilitate the reporting of exterior consumption (to the building's heat balance/loads considerations), several objects have been included. The consumption related to these items will appear on meters specific to the items.
+
+\subsection{Exterior:Lights}\label{exteriorlights}
+
+\subsubsection{Inputs}\label{inputs-017}
+
+\paragraph{Field: Name}\label{field-name-016}
+
+This descriptive name allows the values of exterior lights consumption to appear in the ``normal'' output variable list as well as the meters. It cannot be blank nor can it be duplicated by other Exterior:Lights statements.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-001}
+
+A schedule will allow the exterior lights consumption to be operationally different, hour to hour as well as seasonally. Fractional values in the basic schedule will be applied to the design level field below.
+
+\paragraph{Field: Design Level}\label{field-design-level}
+
+This field (in Watts) is typically used to represent the maximum electrical input to exterior lighting fixtures that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the lighting design level could be a ``diversity factor'' applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour and seasonally, the design level field is constant for all simulation environments.
+
+\paragraph{Field: Control Option}\label{field-control-option}
+
+This field is used to determine how the exterior lights are controlled. There are currently two options, `ScheduleNameOnly' and `AstronomicalClock.'~ If this field is omitted or left blank then the program will default to Schedule Name Only mode. The `ScheduleNameOnly' mode dictates that the exterior lights always follow the schedule named in the field above. The `AstronomicalClock' mode dictates that despite what the schedule indicates, the exterior lights will not run when the sun is up. Using the Astronomical Clock mode makes it simple to model exterior lights that are controlled by a photocell or other controller that ensures that outdoor lights will not run during the daytime. However, the Astronomical Clock control works off of the position of the sun and therefore does not operate exactly like a photocell. During the night, the schedule values are still applied in the usual way.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-000}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Grounds Lights'', ``Facade Lights'', etc. A new meter for reporting is created for each unique subcategory~ (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the lights will be assigned to the ``General'' end-use subcategory.
+
+An IDF Example:
+
+\begin{lstlisting}
+
+Exterior:Lights,
+    OutsideLights,       !- Name
+    ON,                  !- SCHEDULE Name
+    1000,                !- Design Level
+    AstronomicalClock,  !- Control Option
+    Grounds Lights;      !- End-Use Subcategory
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-012}
+
+Output for exterior lights appears in three possible places. It will appear on two meters (Electricity:Facility and ExteriorLights:Electricity) as well as in its own designated value in the standard output file.
+
+Output for exterior lights appears in three possible places. It will appear on two meters (Electricity:Facility and ExteriorLights:Electricity) as well as in its own designated value in the standard output file.
+
+\begin{itemize}
+\item
+  Zone,Average,Exterior Lights Electric Power {[}W{]}
+\item
+  Zone,Sum,Exterior Lights Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Exterior Lights Electric Power {[}W{]}}\label{exterior-lights-electric-power-w}
+
+\paragraph{Exterior Lights Electric Energy {[}J{]}}\label{exterior-lights-electric-energy-j}
+
+These are the electric power and energy consumed by the exterior lights.
+
+\subsection{Exterior:FuelEquipment}\label{exteriorfuelequipment}
+
+\subsubsection{Inputs}\label{inputs-1-015}
+
+\paragraph{Field: Name}\label{field-name-1-014}
+
+This descriptive name allows the values of exterior equipment consumption to appear in the ``normal'' output variable list as well as the meters. It cannot be blank nor can it be duplicated by other Exterior:FuelEquipment or Exterior:WaterEquipment statements.
+
+\paragraph{Field: Fuel Use Type}\label{field-fuel-use-type}
+
+This field designates the appropriate meter for the exterior fuel equipment. Valid fuel types are: Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Diesel, Gasoline, Coal, Steam, DistrictHeating, DistrictCooling, OtherFuel1 and OtherFuel2. The fuel type triggers the application of consumption amounts to the appropriate energy meters.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-1-000}
+
+A schedule will allow the exterior lights consumption to be operationally different, hour to hour as well as seasonally. Fractional values in the basic schedule will be applied to the design level field below.
+
+\paragraph{Field: Design Level}\label{field-design-level-1}
+
+This field (Watts) is typically used to represent the maximum input to exterior fixtures that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the design level could be a ``diversity factor'' applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour and seasonally, the design level field is constant for all simulation environments.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-1}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Fountains'', etc. A new meter for reporting is created for each unique subcategory~ (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+IDF Examples:
+
+\begin{lstlisting}
+
+Exterior:FuelEquipment,OutsideGasEq,Gas,ON,1000;
+  Exterior:FuelEquipment,OutsideCoalEq,Coal,ON,1000;
+  Exterior:FuelEquipment,OutsideFuelOil1Eq,FuelOil#1,ON,1000;
+  Exterior:FuelEquipment,OutsideFuelOil2Eq,FuelOil#2,ON,1000;
+  Exterior:FuelEquipment,OutsideLPGEq,PropaneGas,ON,1000;
+\end{lstlisting}
+
+\subsection{Exterior:WaterEquipment}\label{exteriorwaterequipment}
+
+\subsubsection{Inputs}\label{inputs-2-014}
+
+\paragraph{Field: Name}\label{field-name-2-013}
+
+This descriptive name allows the values of exterior equipment consumption to appear in the ``normal'' output variable list as well as the meters. It cannot be blank nor can it be duplicated by other Exterior:FuelEquipment or Exterior:WaterEquipment statements.
+
+\paragraph{Field: FuelUseType}\label{field-fuelusetype}
+
+For Exterior:WaterEquipment, only ``Water'' is current allowed for this field.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-2-000}
+
+A schedule will allow the exterior water consumption to be operationally different, hour to hour as well as seasonally. Fractional values in the basic schedule will be applied to the design level field below.
+
+\paragraph{Field: Design Level}\label{field-design-level-2}
+
+This field (in m3/s) is typically used to represent the maximum volumetric flow for water fixtures that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the exterior water equipment design level could be a ``diversity factor'' applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour and seasonally, the design level field is constant for all simulation environments.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-2}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Landscaping'', etc. A new meter for reporting is created for each unique subcategory~ (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+IDF Example:
+
+Exterior:WaterEquipment,OutsideWaterEq,Water,ON,10000;
+
+\subsubsection{Outputs}\label{outputs-1-010}
+
+Output for exterior equipment consumption appears in three possible places. It will appear on two meters (\textless{}Fuel Type\textgreater{}:Facility and ExteriorEquipment:\textless{}Fuel Type\textgreater{}) as well as in its own designated value in the standard output file, Exterior Equipment \textless{}Fuel Type\textgreater{} Energy. Consumption also appears on any user-defined end-use subcategory meters, i.e., \textless{}End-Use Subcategory\textgreater{}:ExteriorEquipment:\textless{}Fuel Type\textgreater{}. All outputs are in {[}J{]} except water consumption which is in {[}m3{]}. There are also rate versions
+
+\begin{itemize}
+\item
+  Zone, Average, Exterior Equipment Fuel Rate {[}W{]}
+\item
+  Zone,Sum, Exterior Equipment Electric Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment Gas Energy {[}J{]}
+\item
+  Zone,Average, Exterior Equipment Water Volume Flow Rate {[}m3/s{]}
+\item
+  Zone,Sum, Exterior Equipment Water Volume {[}m3{]}
+\item
+  Zone,Sum, Exterior Equipment Mains Water Volume {[}m3{]}
+\item
+  Zone,Sum, Exterior Equipment Coal Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment FuelOil\#1 Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment FuelOil\#2 Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment Propane Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment Gasoline Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment Diesel Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment Steam Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment OtherFuel1 Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment OtherFuel2 Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment District Heating Energy {[}J{]}
+\item
+  Zone,Sum, Exterior Equipment District Cooling Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Exterior Equipment Fuel Rate {[}W{]}}\label{exterior-equipment-fuel-rate-w}
+
+\paragraph{Exterior Equipment \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{exterior-equipment-fuel-type-energy-j}
+
+These are the fuel consumption rate and energy for the exterior equipment.
+
+\paragraph{Exterior Equipment Water Volume Flow Rate {[}m3/s{]}}\label{exterior-equipment-water-volume-flow-rate-m3s}
+
+\paragraph{Exterior Equipment Water Volume {[}m3{]}}\label{exterior-equipment-water-volume-m3}
+
+These are the water consumption rate and volume for the exterior equipment.
+
+Exterior Equipment Mains Water Volume {[}m3{]}This is the water volume drawn for the mains water service to serve the exterior equipment.
diff --git a/doc/input-output-reference/src/overview/group-externalinterface.tex b/doc/input-output-reference/src/overview/group-externalinterface.tex
new file mode 100644
index 00000000000..2a9c693949a
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-externalinterface.tex
@@ -0,0 +1,494 @@
+\section{Group ExternalInterface}\label{group-externalinterface}
+
+The ExternalInterface allows coupling EnergyPlus to the Building Controls Virtual Test Bed (BCVTB). It supports the import of Functional Mock-up Units (FMUs) for co-simulation as well as the export of EnergyPlus as a FMU for co-simulation. BCVTB is a software environment that allows expert users to couple different simulation programs for distributed simulation or for a real-time simulation that is connected to a building control system. For example, the BCVTB allows simulation of the building envelope and HVAC system in EnergyPlus and the control logic in MATLAB/Simulink, while exchanging data between the two programs as they simulate. The BCVTB can be downloaded from http://simulationresearch.lbl.gov/bcvtb. A FMU is a component which implements the Functional Mock-up Interface (FMI) standard (http://www.modelisar.com).
+
+\subsection{ExternalInterface}\label{externalinterface}
+
+This object activates the external interface of EnergyPlus. If the object ExternalInterface is present, then the external interface objects listed below will receive their values from the BCVTB interface or from FMUs at each zone time step. If this object is not present, then the values of these objects will be fixed at the value declared in the initial value field of the corresponding object, and a warning will be written to the EnergyPlus error file.
+
+\subsubsection{Inputs}\label{inputs-018}
+
+\paragraph{Field: Name}\label{field-name-017}
+
+The name of the external interface. The only valid entries are \textbf{PtolemyServer}, \textbf{FunctionalMockupUnitImport}, and \textbf{FunctionalMockupUnitExport}.
+
+An example IDF object is:
+
+\begin{lstlisting}
+
+ExternalInterface,                     !- Object to activate the external interface
+  PtolemyServer;                           !- Name of external interface
+\end{lstlisting}
+
+\subsection{Building Controls Virtual Test Bed (BCVTB)}\label{building-controls-virtual-test-bed-bcvtb}
+
+The following objects are designed to couple EnergyPlus with the BCVTB.
+
+\subsection{ExternalInterface:Schedule}\label{externalinterfaceschedule}
+
+This input object is similar to Schedule:Compact. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field initial value.
+
+\subsubsection{Inputs}\label{inputs-1-016}
+
+\paragraph{Field: Name}\label{field-name-1-015}
+
+This field should contain a unique (within all DaySchedules) designation for this schedule. It is referenced by WeekSchedules to define the appropriate schedule values.
+
+\paragraph{Field: Schedule Type Limits Name}\label{field-schedule-type-limits-name}
+
+This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see above), then the restrictions from the referenced object will be used to validate the current field values.
+
+\paragraph{Field: Initial Value}\label{field-initial-value}
+
+This field contains the schedule value that is used during the warm-up period and during the system sizing.
+
+! Cooling schedule. This schedule is set directly by the external interface.
+
+! During warm-up and system-sizing, it is fixed at 24 degC.
+
+\begin{lstlisting}
+
+ExternalInterface:Schedule,
+  TSetCoo,                                 !- Name
+  Temperature,                         !- ScheduleType
+  24;                                           !- Initial value, used during warm-up
+\end{lstlisting}
+
+! Heating schedule. This schedule is set directly by the external interface.
+
+! During warm-up and system-sizing, it is fixed at 20 degC.
+
+\begin{lstlisting}
+
+ExternalInterface:Schedule,
+  TSetHea,                                 !- Name
+  Temperature,                         !- ScheduleType
+  20;                                           !- Initial value, used during warm-up
+\end{lstlisting}
+
+\subsection{ExternalInterface:Actuator}\label{externalinterfaceactuator}
+
+This object maps a value received from the external interface to an actuator of the Energy Management System. The object is similar to EnergyManagementSystem:Actuator. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field initial value.
+
+\subsubsection{Inputs}\label{inputs-2-015}
+
+\paragraph{Field: Name}\label{field-name-2-014}
+
+This field contains a unique name for the actuator. No spaces are allowed in the object name. This name will be a global read-only variable in Erl programs and cannot duplicate any other global scope Erl variable.
+
+\paragraph{Field: Actuated Component Unique Name}\label{field-actuated-component-unique-name-000}
+
+This field defines a unique name for the specific entity that is to be controlled. The names for each individual component are listed in the EDD output file when Verbose mode is used see the input object \textbf{Output:EnergyManagementSystem} for more on the EDD file. These will often be user-defined names of input objects or system nodes, but some actuators are automatically setup by the program and will not be completely user-defined.
+
+\paragraph{Field: Actuated Component Type}\label{field-actuated-component-type-000}
+
+The field defines the type of the entity that is to be controlled by the actuator. The component types available vary with the specifics of individual models. The types of components that can be used as actuators in a specific model are listed in the EDD output file see the input object \textbf{Output:EnergyManagementSystem} for more on the EDD file. Components can be object types defined elsewhere in the IDD but there are other types of entities such as nodes and system-level actuators that do not directly correspond to IDF objects.
+
+\paragraph{Field: Actuated Component Control Type}\label{field-actuated-component-control-type-000}
+
+This field defines the type of control to be done on the specific entity being controlled. The control types available are listed in the EDD output. Specific components may have more than one type of control available, such as flow rate or temperature, and this field is used to distinguish between them.
+
+\paragraph{Field: Initial Value}\label{field-initial-value-1}
+
+This field contains the initial value. If a value is specified, then this value is used during the warm-up period and the system sizing. If no value is specified, then the actuated component will only be updated once the time stepping starts, i.e., after the warm-up and the system-sizing. This allows, for example, to schedule a setpoint with a Schedule:Compact during warm-up and system-sizing, and then overwrite the value of this schedule during each zone time step based on a feedback control loop that is implemented in the BCVTB.
+
+\begin{lstlisting}
+
+ExternalInterface:Actuator,
+  Zn001_Wall001_Win001_Shading_Deploy_Status,   !- Name
+  Zn001:Wall001:Win001,       !- Actuated Component Unique Name
+  Window Shading Control,   !- Actuated Component Type
+  Control Status,                   !- Actuated Component Control Type
+  ;                                             ! initial value
+\end{lstlisting}
+
+\subsection{ExternalInterface:Variable}\label{externalinterfacevariable}
+
+This input object is similar to EnergyManagementSystem:GlobalVariable. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field initial value. This object can be used to move data into Erl subroutines.
+
+\subsubsection{Inputs}\label{inputs-3-013}
+
+\paragraph{Field: Name}\label{field-name-3-012}
+
+This field becomes the global Erl variable name that can be referenced in the EnergyPlus Runtime Language. No spaces are allowed in the object name. The name must be unique across all global scope variables including those declared as sensor and actuators and the built-in variables.
+
+\paragraph{Field: Initial Value}\label{field-initial-value-2}
+
+This field contains the initial value that is used during the warm-up period and during the system sizing.
+
+\begin{lstlisting}
+
+ExternalInterface:Variable,
+  yShade,                                   !- Name of Erl variable
+  1;                                             !- Initial value
+\end{lstlisting}
+
+\subsection{Functional Mock-up Unit (FMU) Import}\label{functional-mock-up-unit-fmu-import}
+
+The following objects are designed to couple EnergyPlus with FMUs for co-simulation.
+
+\subsection{ExternalInterface:FunctionalMockupUnitImport}\label{externalinterfacefunctionalmockupunitimport}
+
+This object defines the FMU that will be linked to EnergyPlus.
+
+\subsubsection{Inputs}\label{inputs-4-012}
+
+\paragraph{Field: FMU File Name}\label{field-fmu-file-name}
+
+This field contains the name of the FMU file including the extension. The field should include a full path with file name, for best results. The field must be \textless{} = 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
+
+\paragraph{Field: FMU Timeout}\label{field-fmu-timeout}
+
+This field contains the communication timeout value in milli-seconds to allow interprocess communication to take place.
+
+\paragraph{Field: FMU LoggingOn}\label{field-fmu-loggingon}
+
+This field contains the loggingOn value to enable or disable debug in FMU. If loggingOn = 1, debug logging is enabled. If loggingOn = 0, debug logging is disabled.
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport,
+  MoistAir.fmu,                       !- FMU File Name
+  15,                                           !- FMU Timeout
+  0;                                             !- FMU LoggingOn
+\end{lstlisting}
+
+\subsection{ExternalInterface:FunctionalMockupUnitImport:From:Variable}\label{externalinterfacefunctionalmockupunitimportfromvariable}
+
+This input object maps the names of the output variables of EnergyPlus to the input variables of the FMU.
+
+\subsubsection{Inputs}\label{inputs-5-010}
+
+\paragraph{Field: EnergyPlus Key Value}\label{field-energyplus-key-value}
+
+This input object maps the names of the EnergyPlus output variables (\textbf{Output:Variable} or \textbf{EnergyManagementSystem:OutputVariable}) to the input variables of the FMU.
+
+\paragraph{Field: EnergyPlus Variable Name}\label{field-energyplus-variable-name}
+
+This field contains the output variable name as defined in the InputOutput Reference. For an \textbf{EnergyManagementSystem:OutputVariable}, the EnergyPlus Variable Name is the name of the \textbf{EnergyManagementSystem:OutputVariable} s object.
+
+\paragraph{Field: FMU File Name}\label{field-fmu-file-name-1}
+
+This field contains the name of the FMU file including the extension. The field should include a full path with file name, for best results. The field must be \textless{} = 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
+
+\paragraph{Field: FMU Instance Name}\label{field-fmu-instance-name}
+
+This field contains the EnergyPlus instance name of the FMU. See External Interface Application guide for more details.
+
+\paragraph{Field: FMU Variable Name}\label{field-fmu-variable-name}
+
+This field contains the name of the variable in the FMU that will be mapped to the corresponding variable in EnergyPlus.
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+  Environment,                         !- EnergyPlus Key Value
+  Site Outdoor Air Drybulb Temperature,       !- EnergyPlus Variable Name
+  MoistAir.fmu,                       !- FMU File Name
+  Model1,                                   !- FMU Instance Name
+  TDryBul;                                 !- FMU Variable Name
+
+
+  ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+  ZONE ONE,                               !- EnergyPlus Key Value
+  Zone Mean Air Temperature, !- EnergyPlus Variable Name
+  MoistAir.fmu,                       !- FMU File Name
+  Model1,                                   !- FMU Instance Name
+  TRooMea;                                 !- FMU Variable Name
+
+
+  ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+  Environment,                         !- EnergyPlus Key Value
+  Site Outdoor Air Relative Humidity,   !- EnergyPlus Variable Name
+  MoistAir.fmu,                       !- FMU File Name
+  Model1,                                   !- FMU Instance Name
+  outRelHum;                             !- FMU Variable Name
+
+
+  ExternalInterface:FunctionalMockupUnitImport:From:Variable,
+  ZONE ONE,                               !- EnergyPlus Key Value
+  Zone Air Relative Humidity,   !- EnergyPlus Variable Name
+  MoistAir.fmu,                       !-FMU File Name
+  Model1,                                   !- FMU Instance Name
+  rooRelHum;                             !- FMU Variable Name
+\end{lstlisting}
+
+\subsection{ExternalInterface:FunctionalMockupUnitImport:To:Schedule}\label{externalinterfacefunctionalmockupunitimporttoschedule}
+
+This input object is similar to Schedule:Compact. However, during the time stepping, its value is set to the value received from the external interface. During the system sizing, its value is set to the value specified by the field initial value.
+
+\subsubsection{Inputs}\label{inputs-6-009}
+
+\paragraph{Field: EnergyPlus Variable Name}\label{field-energyplus-variable-name-1}
+
+This field contains a unique (within all Schedules) designation for this schedule in EnergyPlus.
+
+\paragraph{Field: Schedule Type Limits Name}\label{field-schedule-type-limits-name-1}
+
+This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see above), then the restrictions from the referenced object will be used to validate the current field values.
+
+\paragraph{Field: FMU File Name}\label{field-fmu-file-name-2}
+
+This field contains the name of the FMU file including the extension. The field should include a full path with file name, for best results. The field must be \textless{} = 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
+
+\paragraph{Field: FMU Instance Name}\label{field-fmu-instance-name-1}
+
+This field contains the EnergyPlus instance name of the FMU. See External Interface Application guide for more details.
+
+\paragraph{Field: FMU Variable Name}\label{field-fmu-variable-name-1}
+
+This field contains the name of the variable in the FMU that will be mapped to the schedule in EnergyPlus.
+
+\paragraph{Field: Initial Value}\label{field-initial-value-3}
+
+This field contains the schedule value that is used during the system sizing.
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport:To:Schedule,
+  FMU_OthEquSen_ZoneOne,     !- EnergyPlus Variable Name
+  Any Number,                           !- Schedule Type Limits Names
+  MoistAir.fmu,                       !- FMU File Name
+  Model1,                                   !- FMU Instance Name
+  QSensible,                             !- FMU Variable Name
+  0;                                             !- Initial Value
+
+
+  ExternalInterface:FunctionalMockupUnitImport:To:Schedule,
+  FMU_OthEquLat_ZoneOne,     !- EnergyPlus Variable Name
+  Any Number,                           !- Schedule Type Limits Names
+  MoistAir.fmu,                       !- FMU File Name
+  Model1,                                   !- FMU Instance Name
+  QLatent,                                 !- FMU Variable Name
+  0;                                             !- Initial Value
+\end{lstlisting}
+
+\subsection{ExternalInterface:FunctionalMockupUnitImport:To:Actuator}\label{externalinterfacefunctionalmockupunitimporttoactuator}
+
+This object maps a value received from the external interface to an actuator of the Energy Management System. The object is similar to EnergyManagementSystem:Actuator. However, during the warm-up and time stepping, its value is set to the value received from the external interface. During the system sizing, its value is set to the value specified by the field initial value.
+
+\subsubsection{Inputs}\label{inputs-7-009}
+
+\paragraph{Field: EnergyPlus Variable Name}\label{field-energyplus-variable-name-2}
+
+This field contains a unique name for the actuator. No spaces are allowed in the object name. This name will be a global read-only variable in Erl programs and cannot duplicate any other global scope Erl variable.
+
+\paragraph{Field: Actuated Component Unique Name}\label{field-actuated-component-unique-name-1}
+
+This field defines a unique name for the specific entity that is to be controlled. The names for each individual component are listed in the EDD output file when Verbose mode is used see the input object \textbf{Output:EnergyManagementSystem} for more on the EDD file. These will often be user-defined names of input objects or system nodes, but some actuators are automatically setup by the program and will not be completely user-defined.
+
+\paragraph{Field: Actuated Component Type}\label{field-actuated-component-type-1}
+
+The field defines the type of the entity that is to be controlled by the actuator. The component types available vary with the specifics of individual models. The types of components that can be used as actuators in a specific model are listed in the EDD output file see the input object \textbf{Output:EnergyManagementSystem} for more on the EDD file. Components can be object types defined elsewhere in the IDD but there are other types of entities such as nodes and system-level actuators that do not directly correspond to IDF objects.
+
+\paragraph{Field: Actuated Component Control Type}\label{field-actuated-component-control-type-1}
+
+This field defines the type of control to be done on the specific entity being controlled. The control types available are listed in the EDD output. Specific components may have more than one type of control available, such as flow rate or temperature, and this field is used to distinguish between them.
+
+\paragraph{Field: FMU File Name}\label{field-fmu-file-name-3}
+
+This field contains the name of the FMU file including the extension. The field should include a full path with file name, for best results. The field must be \textless{} = 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
+
+\paragraph{Field: FMU Instance Name}\label{field-fmu-instance-name-2}
+
+This field contains the EnergyPlus instance name of the FMU. See External Interface Application guide for more details.
+
+\paragraph{Field: FMU Variable Name}\label{field-fmu-variable-name-2}
+
+This field contains the name of the variable in the FMU that will be mapped to the actuator in EnergyPlus.
+
+\paragraph{Field: Initial Value}\label{field-initial-value-4}
+
+This field contains the value that is used during the system sizing.
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport:To:Actuator,
+  Zn001_Wall001_Win001_Shading_Deploy_Status,   !- EnergyPlus Variable Name
+  Zn001:Wall001:Win001,                                 !- Actuated Component Unique Name
+  Window Shading Control,                                   !- Actuated Component Type
+  Control Status,                                             !- Actuated Component Control Type
+  ShadingController.fmu,                                     !- FMU File Name
+  Model1,                                                                   !- FMU Instance Name
+  yShade,                                                                   !- FMU Variable Name
+  6;                                                                             !- Initial Value
+\end{lstlisting}
+
+\subsection{ExternalInterface:FunctionalMockupUnitImport:To:Variable}\label{externalinterfacefunctionalmockupunitimporttovariable}
+
+This input object is similar to EnergyManagementSystem:GlobalVariable. However, during the warm-up and time stepping, its value is set to the value received from the external interface. During the system sizing its value is set to the value specified by the field initial value. This object can be used to move data into Erl subroutines.
+
+\subsubsection{Inputs}\label{inputs-8-007}
+
+\paragraph{Field: EnergyPlus Variable Name}\label{field-energyplus-variable-name-3}
+
+This field becomes the global Erl variable name that can be referenced in the EnergyPlus Runtime Language. No spaces are allowed in the object name. The name must be unique across all global scope variables including those declared as sensor and actuators and the built-in variables.
+
+\paragraph{Field: FMU File Name}\label{field-fmu-file-name-4}
+
+This field contains the name of the FMU file including the extension. The field should include a full path with file name, for best results. The field must be \textless{} = 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
+
+\paragraph{Field: FMU Instance Name}\label{field-fmu-instance-name-3}
+
+This field contains the EnergyPlus instance name of the FMU. See External Interface Application guide for more details.
+
+\paragraph{Field: FMU Variable Name}\label{field-fmu-variable-name-3}
+
+This field contains the name of the variable in the FMU that will be mapped to the corresponding variable in EnergyPlus.
+
+\paragraph{Field: Initial Value}\label{field-initial-value-5}
+
+This field contains the initial value that is used during the system sizing.
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitImport:To:Variable,
+  Shade_Signal,                       !- EnergyPlus Variable Name
+  ShadingController.fmu,     !- FMU File Name
+  Model1,                                   !- FMU Instance Name
+  yShade,                                   !- FMU Variable Name
+  1;                                             !- Initial Value
+\end{lstlisting}
+
+\subsection{Functional Mock-up Unit (FMU) Export}\label{functional-mock-up-unit-fmu-export}
+
+The following objects are designed to support the export of EnergyPlus as a FMU for co-simulation.
+
+\subsection{ExternalInterface:FunctionalMockupUnitExport:From:Variable}\label{externalinterfacefunctionalmockupunitexportfromvariable}
+
+This object exposes the EnergyPlus output variables (\textbf{Output:Variable} or \textbf{EnergyManagementSystem:OutputVariable}) to the outside simulation program.
+
+\subsubsection{Inputs}\label{inputs-9-006}
+
+\paragraph{Field: EnergyPlus Key Value}\label{field-energyplus-key-value-1}
+
+This field contains a Key Value for an EnergyPlus output variable (ref Output:Variable/.rdd file). For an \textbf{EnergyManagementSystem:OutputVariable}, the EnergyPlus Key Value needs to be set to \textbf{EMS} .
+
+\paragraph{Field: EnergyPlus Variable Name}\label{field-energyplus-variable-name-4}
+
+This field contains the Variable Name as defined in the InputOutput Reference. For an \textbf{EnergyManagementSystem:OutputVariable}, the EnergyPlus Variable Name is the name of the \textbf{EnergyManagementSystem:OutputVariable} s object.
+
+\paragraph{Field: FMU Variable Name}\label{field-fmu-variable-name-4}
+
+This field contains the name of the variable in the model description file of the FMU that will be mapped to the corresponding variable in EnergyPlus.
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitExport:From:Variable,
+  Environment,                         !- EnergyPlus Key Value
+  Site Outdoor Air Drybulb Temperature,   !- EnergyPlus Variable Name
+  TDryBul;                                 !- FMU Variable Name
+
+  ExternalInterface: FunctionalMockupUnitExport:From:Variable,
+  ZONE ONE,                                   !- EnergyPlus Key Value
+  Zone Mean Air Temperature, !- EnergyPlus Variable Name
+  TRooMea;                                     !- FMU Variable Name
+
+  ExternalInterface: FunctionalMockupUnitExport:From:Variable,
+  Environment,                               !- EnergyPlus Key Value
+  Site Outdoor Air Relative Humidity,   !- EnergyPlus Variable Name
+  outRelHum;                                   !- FMU Variable Name
+
+  ExternalInterface:FunctionalMockupUnitExport:From:Variable,
+  ZONE ONE,                                       !- EnergyPlus Key Value
+  Zone Air Relative Humidity,   !- EnergyPlus Variable Name
+  rooRelHum;                                     !- FMU Variable Name
+\end{lstlisting}
+
+\subsection{ExternalInterface:FunctionalMockupUnitExport:To:Schedule}\label{externalinterfacefunctionalmockupunitexporttoschedule}
+
+This object is similar to Schedule:Compact. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field initial value.
+
+\subsubsection{Inputs}\label{inputs-10-005}
+
+\paragraph{Field: EnergyPlus Variable Name}\label{field-energyplus-variable-name-5}
+
+This field contains a unique (within all Schedules) designation for this schedule in EnergyPlus.
+
+\paragraph{Field: Schedule Type Limits Name}\label{field-schedule-type-limits-name-2}
+
+This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see above), then the restrictions from the referenced object will be used to validate the current field values.
+
+\paragraph{Field: FMU Variable Name}\label{field-fmu-variable-name-5}
+
+This field contains the name of the variable in the model description file of the FMU that will be mapped to the schedule in EnergyPlus.
+
+\paragraph{Field: Initial Value}\label{field-initial-value-6}
+
+This field contains the schedule value that is used during the warm-up period and during the system sizing.
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitExport:To:Schedule,
+  FMU_OthEquSen_ZoneOne,     !- EnergyPlus Variable Name
+  Any Number,                           !- Schedule Type Limits Names
+  QSensible,                             !- FMU Variable Name
+  0;                                             !- Initial Value
+\end{lstlisting}
+
+\subsection{ExternalInterface:FunctionalMockupUnitExport:To:Actuator}\label{externalinterfacefunctionalmockupunitexporttoactuator}
+
+This object maps a value received from the external interface to an actuator of the Energy Management System. The object is similar to EnergyManagementSystem:Actuator. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field initial value.
+
+\subsubsection{Inputs}\label{inputs-11-004}
+
+\paragraph{Field: EnergyPlus Variable Name}\label{field-energyplus-variable-name-6}
+
+This field contains a unique name for the actuator. No spaces are allowed in the object name. This name will be a global read-only variable in Erl programs and cannot duplicate any other global scope Erl variable.
+
+\paragraph{Field: Actuated Component Unique Name}\label{field-actuated-component-unique-name-2}
+
+This field defines a unique name for the specific entity that is to be controlled. The names for each individual component are listed in the EDD output file when Verbose mode is used see the input object \textbf{Output:EnergyManagementSystem} for more on the EDD file. These will often be user-defined names of input objects or system nodes, but some actuators are automatically setup by the program and will not be completely user-defined.
+
+\paragraph{Field: Actuated Component Type}\label{field-actuated-component-type-2}
+
+The field defines the type of the entity that is to be controlled by the actuator. The component types available vary with the specifics of individual models. The types of components that can be used as actuators in a specific model are listed in the EDD output file see the input object \textbf{Output:EnergyManagementSystem} for more on the EDD file. Components can be object types defined elsewhere in the IDD but there are other types of entities such as nodes and system-level actuators that do not directly correspond to IDF objects.
+
+\paragraph{Field: Actuated Component Control Type}\label{field-actuated-component-control-type-2}
+
+This field defines the type of control to be done on the specific entity being controlled. The control types available are listed in the EDD output. Specific components may have more than one type of control available, such as flow rate or temperature, and this field is used to distinguish between them.
+
+\paragraph{Field: FMU Variable Name}\label{field-fmu-variable-name-6}
+
+This field contains the name of the variable in the model description file of the FMU that will be mapped to the actuator in EnergyPlus.
+
+\paragraph{Field: Initial Value}\label{field-initial-value-7}
+
+This field contains the initial value. If a value is specified, then this value is used during the warm-up period and the system sizing. If no value is specified, then the actuated component will only be updated once the time stepping starts, i.e., after the warm-up and the system-sizing.
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitExport:To:Actuator,
+  Zn001_Wall001_Win001_Shading_Deploy_Status,   !- EnergyPlus Variable Name
+  Zn001:Wall001:Win001,                                   !- Actuated Component Unique Name
+  Window Shading Control,                               !- Actuated Component Type
+  Control Status,                                               !- Actuated Component Control Type
+  yShade,                                                               !- FMU Variable Name
+  6;                                                                         !- Initial Value
+\end{lstlisting}
+
+\subsection{ExternalInterface:FunctionalMockupUnitExport:To:Variable}\label{externalinterfacefunctionalmockupunitexporttovariable}
+
+This input object is similar to EnergyManagementSystem:GlobalVariable. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field initial value. This object can be used to move data into Erl subroutines.
+
+\subsubsection{Inputs}\label{inputs-12-004}
+
+\paragraph{Field: EnergyPlus Variable Name}\label{field-energyplus-variable-name-7}
+
+This field becomes the global Erl variable name that can be referenced in the EnergyPlus Runtime Language. No spaces are allowed in the object name. The name must be unique across all global scope variables including those declared as sensor and actuators and the built-in variables.
+
+\paragraph{Field: FMU Variable Name}\label{field-fmu-variable-name-7}
+
+This field contains the name of the variable in the model description file of the FMU that will be mapped to the corresponding variable in EnergyPlus.
+
+\paragraph{Field: Initial Value}\label{field-initial-value-8}
+
+This field contains the initial value that is used during the warm-up period and during the system sizing.
+
+\begin{lstlisting}
+
+ExternalInterface:FunctionalMockupUnitExport:To:Variable,
+  Shade_Signal,                       !- EnergyPlus Variable Name
+  yShade,                                   !- FMU Variable Name
+  1;                                             !- Initial Value
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-fans.tex b/doc/input-output-reference/src/overview/group-fans.tex
new file mode 100644
index 00000000000..d88240c2ce2
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-fans.tex
@@ -0,0 +1,894 @@
+\section{Group Fans}\label{group-fans}
+
+The following fans may be defined either in the air loop or as a zone equipment component: Fan:ConstantVolume, Fan:OnOff, Fan:VariableVolume, Fan:ZoneExhaust, and FanPerformance:NightVentilation. The data that are common to these fan types include an identifying name, an availability schedule name, a total efficiency rating, a rated pressure rise, and inlet and outlet air node names. In the case of a variable volume fan, additional input includes parameters for modeling fan performance over a range of fan speeds. See the engineering documentation for the variable speed fan for a further description of what these coefficients represent. Commonly-used values for different variable volume systems are shown in the following table.
+
+% table 29
+\begin{longtable}[c]{p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}p{1.0in}}
+\caption{Fan Coefficient Values \label{table:fan-coefficient-values}} \tabularnewline
+\toprule 
+Type of Fan & Fan Coeff. 1 & Fan Coeff. 2 & Fan Coeff. 3 & Fan Coeff. 4 & Fan Coeff. 5 \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Fan Coefficient Values} \tabularnewline
+\toprule 
+Type of Fan & Fan Coeff. 1 & Fan Coeff. 2 & Fan Coeff. 3 & Fan Coeff. 4 & Fan Coeff. 5 \tabularnewline
+\midrule
+\endhead
+
+Inlet Vane Dampers & 0.35071223 & 0.30850535 & -0.54137364 & 0.87198823 & 0.000 \tabularnewline
+Discharge Dampers & 0.37073425 & 0.97250253 & -0.34240761 & 0.000 & 0.000 \tabularnewline
+Var. Speed Motor & 0.0015302446 & 0.0052080574 & 1.1086242 & -0.11635563 & 0.000 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Fan:ConstantVolume}\label{fanconstantvolume}
+
+This object models a constant air volume fan that is intended to operate continuously based on a time schedule. This fan will not cycle on and off based on cooling/heating load or other control signals (Ref: Fan:OnOff).
+
+\subsubsection{Inputs}\label{inputs-019}
+
+\paragraph{Field: Name}\label{field-name-018}
+
+A unique user-assigned name for an instance of a Fan:ConstantVolume. Any reference to this fan by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-007}
+
+The name of the schedule (ref: Schedule) that denotes whether the fan can run during a given time period. A schedule value of 0 indicates that the fan is off for that time period. A schedule value greater than 0 indicates that the fan can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this schedule by forcing the fan to be on or off.
+
+\paragraph{Field: Fan Total Efficiency}\label{field-fan-total-efficiency-000}
+
+This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1.The default is 0.7.
+
+\paragraph{Field: Pressure Rise}\label{field-pressure-rise}
+
+The pressure rise in Pascals at full flow and standard (sea level) conditions (20 °C and 101325 Pa).
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate-000}
+
+The full load air volumetric flow rate (m\(^{3}\)/sec) at standard temperature and pressure (dry air at 20 °C drybulb). The program does use local barometric pressure to account for altitude using equation for ``standard atmospheric'' pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
+
+p = 101325*(1-2.25577E-05*Z)**5.2559
+
+where p = pressure in Pa and Z = altitude in m
+
+\paragraph{Field: Motor Efficiency}\label{field-motor-efficiency}
+
+The shaft power divided by the electrical power consumed. Must be between 0 and 1. The default is 0.9.
+
+\paragraph{Field: Motor In Airstream Fraction}\label{field-motor-in-airstream-fraction}
+
+The fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat loss will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-002}
+
+The name of the HVAC system node which supplies the inlet air conditions to the fan.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-002}
+
+The name of the HVAC system node to which the fan sends its outlet air.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-001}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Central System'', etc. A new meter for reporting is created for each unique subcategory (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the fan will be assigned to the ``General'' end-use subcategory.
+
+\subsubsection{Outputs}\label{outputs-013}
+
+\begin{itemize}
+\item
+  HVAC,Average,Fan Electric Power{[}W{]}
+\item
+  HVAC,Average,Fan Rise in Air Temperature {[}deltaC{]}
+\item
+  HVAC,Sum,Fan Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Fan Electric Power {[}W{]}}\label{fan-electric-power-w}
+
+This output field contains the average electricity consumption rate for the fan in Watts for the timestep being reported.
+
+\paragraph{Fan Rise in Air Temperature {[}deltaC{]}}\label{fan-rise-in-air-temperature-deltac}
+
+This output field contains the average rise in air temperature across the fan (outlet air temperature minus inlet air temperature) in degrees Celsius for the timestep being reported.
+
+\paragraph{Fan Electric Energy {[}J{]}}\label{fan-electric-energy-j}
+
+This output field contains the electricity consumption of the fan in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Fans, Group Key = System (ref. Output:Meter objects).
+
+\subsection{Fan:OnOff}\label{fanonoff}
+
+This object models a constant air volume fan that is intended to cycle on and off in tandem with a cooling or heating system (i.e., AUTO fan control mode). The fan can also operate continuously like Fan:ConstantVolume. If modeling continuous operation and this object is used as part of a system that utilizes Coil:Heating:Gas, Coil:Cooling:DX:SingleSpeed or Coil:Heating:DX:SingleSpeed, the user should confirm proper air flow rates (coil and fan max flows are equal) and that the coil part-load fraction correlation(s) are appropriate (e.g., part-load fraction is less than or equal to 1 for all values of coil part-load ratio). If modeling multi-speed fan operation, this object must be used as part of a compound object that allows multiple fan speeds (e.g., AirLoopHVAC:Unitary:Furnace:HeatCool, ZoneHVAC:PackagedTerminalAirConditioner, etc.). In this case, the ratio of the compound object air flow rate to the fan s maximum air flow rate is used to determine the power at alternate fan speeds. The optional input for Fan Power Ratio Function of Speed Ratio Curve Name must be entered to model multi-speed fan operation. An optional fan total efficiency ratio curve is also available to model efficiency differences at alternate fan speeds.
+
+\subsubsection{Inputs}\label{inputs-1-017}
+
+\paragraph{Field: Name}\label{field-name-1-016}
+
+A unique user-assigned name for an instance of a Fan:OnOff. Any reference to this fan by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-005}
+
+The name of the schedule (ref: Schedule) that denotes whether the fan can run during a given time period. A schedule value of 0 indicates that the fan is off for that time period. A schedule value greater than 0 indicates that the fan can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this schedule by forcing the fan to be on or off.
+
+\paragraph{Field: Fan Total Efficiency}\label{field-fan-total-efficiency-1-000}
+
+This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1.The default is 0.6.
+
+\paragraph{Field: Pressure Rise}\label{field-pressure-rise-1}
+
+The pressure rise in Pascals at full flow and standard (sea level) conditions (20 °C and 101325 Pa).
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate-1}
+
+The full load air volumetric flow rate (m\(^{3}\)/sec) at standard temperature and pressure (dry air at 20 °C drybulb). The program does use local barometric pressure to account for altitude using equation for ``standard atmospheric'' pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
+
+p = 101325*(1-2.25577E-05*Z)**5.2559
+
+where p = pressure in Pa and Z = altitude in m
+
+\paragraph{Field: Motor Efficiency}\label{field-motor-efficiency-1}
+
+The shaft power divided by the electrical power consumed. Must be between 0 and 1. The default is 0.8.
+
+\paragraph{Field: Motor In Airstream Fraction}\label{field-motor-in-airstream-fraction-1}
+
+The fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat loss will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-1-002}
+
+The name of the HVAC system node which supplies the inlet air conditions to the fan.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-1-001}
+
+The name of the HVAC system node to which the fan sends its outlet air.
+
+\paragraph{Field: Fan Power Ratio Function of Speed Ratio Curve Name}\label{field-fan-power-ratio-function-of-speed-ratio-curve-name}
+
+Enter the name of an exponent performance curve. This optional alpha field must be used to simulate multi-speed fan motors. This curve represents the ratio of actual fan power to rated fan power when a change in fan speed occurs. Leave this field blank when simulating constant-speed fan motors.
+
+\paragraph{Field: Fan Efficiency Ratio Function of Speed Ratio Curve Name}\label{field-fan-efficiency-ratio-function-of-speed-ratio-curve-name}
+
+Enter the name of a quadratic or cubic performance curve. This optional alpha field is used to simulate multi-speed fan motors. This curve represents the ratio of actual fan total efficiency to rated fan total efficiency when a change in fan speed occurs. Leave this field blank when simulating constant-speed fan motors.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-1-000}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Main Fans'', etc. A new meter for reporting is created for each unique subcategory (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the fan will be assigned to the ``General'' end-use subcategory.
+
+Following is an example input for an OnOff Fan.
+
+\begin{lstlisting}
+
+Fan:OnOff,
+  Supply Fan 1,                   ! Fan Name
+  FanAndCoilAvailSched,   ! Fan Schedule
+  0.7,                                     ! Fan Total Efficiency
+  600.0,                                 ! Delta Pressure [N/M^2]
+  1.3,                                     ! Max Flow Rate   [m^3/Sec]
+  0.9,                                     ! Motor Efficiency
+  1.0,                                     ! Motor in Airstream Fraction (1.0 means motor in air stream)
+  Air Loop Inlet Node, Cooling Coil Air Inlet Node;   !Inlet Node, Outlet Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-011}
+
+HVAC,Average,Fan Electric Power{[}W{]}
+
+HVAC,Average,Fan Rise in Air Temperature {[}deltaC{]}
+
+HVAC,Sum,Fan Electric Energy {[}J{]}
+
+HVAC,Average,Fan Runtime Fraction {[]}
+
+\paragraph{Fan Electric Power {[}W{]}}\label{fan-electric-power-w-1}
+
+This output field contains the average electricity consumption rate for the fan in Watts for the timestep being reported.
+
+\paragraph{Fan Rise in Air Temperature {[}deltaC{]}}\label{fan-rise-in-air-temperature-deltac-1}
+
+This output field contains the average rise in air temperature across the fan (outlet air temperature minus inlet air temperature) in degrees Celsius for the timestep being reported.
+
+\paragraph{Fan Electric Energy {[}J{]}}\label{fan-electric-energy-j-1}
+
+This output field contains the electricity consumption of the fan in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Fans, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Fan Runtime Fraction {[]}}{Fan Runtime Fraction }}\label{fan-runtime-fraction}
+
+This output field contains the fraction of time that this fan operated for the timestep being reported.
+
+\subsection{Fan:VariableVolume}\label{fanvariablevolume}
+
+\subsubsection{Inputs}\label{inputs-2-016}
+
+\paragraph{Field: Name}\label{field-name-2-015}
+
+A unique user-assigned name for an instance of a Fan:VariableVolume. Any reference to this fan by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-2-002}
+
+The name of the schedule (ref: Schedule) that denotes whether the fan can run during a given time period. A schedule value of 0 indicates that the fan is off for that time period. A schedule value greater than 0 indicates that the fan can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this schedule by forcing the fan to be on or off.
+
+\paragraph{Field: Fan Total Efficiency}\label{field-fan-total-efficiency-2}
+
+This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
+
+\paragraph{Field: Pressure Rise}\label{field-pressure-rise-2}
+
+The pressure rise in Pascals at full flow and standard (sea level) conditions (20 °C and 101325 Pa).
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate-2}
+
+The full load air volumetric flow rate (m\(^{3}\)/sec) at standard temperature and pressure (dry air at 20 °C drybulb). The program does use local barometric pressure to account for altitude using equation for ``standard atmospheric'' pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
+
+p = 101325*(1-2.25577E-05*Z)**5.2559
+
+where p = pressure in Pa and Z = altitude in m
+
+\paragraph{Field: Fan Power Minimum Flow Rate Input Method}\label{field-fan-power-minimum-flow-rate-input-method}
+
+This field is a key/choice field that tells which of the next two fields is filled and is descriptive of how the minimum flow rate is specified for calculating the fan power. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  Fraction
+\end{itemize}
+
+With this choice, the fan power will be calculated using the value specified in the Fan Power Minimum Flow Fraction field. (The Fan Power Minimum Flow Fraction field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  FixedFlowRate
+\end{itemize}
+
+With this choice, the fan power will be calculated using the value specified in the Fan Power Minimum Air Flow Rate field. (The Fan Power Minimum Air Flow Rate field should be filled.)
+
+The default is Fraction.
+
+\paragraph{Field: Fan Power Minimum Flow Fraction}\label{field-fan-power-minimum-flow-fraction}
+
+The minimum air volumetric flow rate for fan power, specified as a fraction of maximum system air flow rate. Must be between 0 and 1. Note that this field is only used to calculate the fan power. This field does not enforce the system air flow rate during simulation. The default is 0.25.
+
+\paragraph{Field: Fan Power Minimum Air Flow Rate}\label{field-fan-power-minimum-air-flow-rate}
+
+The minimum air volumetric flow rate for fan power, specified as a constant minimum air flow rate (m3/sec). Note that this field is only used to calculate the fan power. This field does not enforce the system air flow rate during simulation.
+
+\paragraph{Field: Motor Efficiency}\label{field-motor-efficiency-2}
+
+The shaft power divided by the electrical power consumed. Must be between 0 and 1. The default is 0.9.
+
+\paragraph{Field: Motor In Airstream Fraction}\label{field-motor-in-airstream-fraction-2}
+
+The fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat loss will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
+
+\paragraph{Field: Fan Power Coefficient 1}\label{field-fan-power-coefficient-1}
+
+The constant coefficient (C\(_{1}\)) in a fourth order polynomial curve giving the fraction of full load power (PLF) as a function of flow fraction (FF). Flow fraction is the air mass flow rate divided by the maximum air mass flow rate. The curve is:
+
+PLF = C\(_{1}\) + C\(_{2}\)\(^{.}\) FF + C\(_{3}\)\(^{.}\) FF\(^{2\\ +}\) C\(_{4}\)\(^{.}\) FF\(^{3}\) + C\(_{5}\)\(^{.}\) FF\(^{4}\)
+
+\paragraph{Field: Fan Power Coefficient 2}\label{field-fan-power-coefficient-2}
+
+The linear coefficient (C\(_{2}\)) in a fourth order polynomial curve giving the fraction of full load power (PLF) as a function of flow fraction (FF). Flow fraction is the air mass flow rate divided by the maximum air mass flow rate. The curve is:
+
+PLF = C\(_{1}\) + C\(_{2}\)\(^{.}\) FF + C\(_{3}\)\(^{.}\) FF\(^{2\\ +}\) C\(_{4}\)\(^{.}\) FF\(^{3}\) + C\(_{5}\)\(^{.}\) FF\(^{4}\)
+
+\paragraph{Field: Fan Power Coefficient 3}\label{field-fan-power-coefficient-3}
+
+The quadratic coefficient (C\(_{3}\)) in a fourth order polynomial curve giving the fraction of full load power (PLF) as a function of flow fraction (FF). Flow fraction is the air mass flow rate divided by the maximum air mass flow rate. The curve is:
+
+PLF = C\(_{1}\) + C\(_{2}\)\(^{.}\) FF + C\(_{3}\)\(^{.}\) FF\(^{2\\ +}\) C\(_{4}\)\(^{.}\) FF\(^{3}\) + C\(_{5}\)\(^{.}\) FF\(^{4}\)
+
+\paragraph{Field: Fan Power Coefficient 4}\label{field-fan-power-coefficient-4}
+
+The cubic coefficient (C\(_{1}\)) in a fourth order polynomial curve giving the fraction of full load power (PLF) as a function of flow fraction (FF). Flow fraction is the air mass flow rate divided by the maximum air mass flow rate. The curve is:
+
+\begin{lstlisting}
+       PLF = C$_{1}$ + C$_{2}$$^{.}$ FF + C$_{3}$$^{.}$ FF$^{2\\ +}$ C$_{4}$$^{.}$ FF$^{3}$ + C$_{5}$$^{.}$ FF$^{4}$
+\end{lstlisting}
+
+\paragraph{Field: Fan Power Coefficient 5}\label{field-fan-power-coefficient-5}
+
+The coefficient C\(_{5}\) in a fourth order polynomial curve giving the fraction of full load power (PLF) as a function of flow fraction (FF). Flow fraction is the air mass flow rate divided by the maximum air mass flow rate. The curve is:
+
+\begin{lstlisting}
+       PLF = C$_{1}$ + C$_{2}$$^{.}$ FF + C$_{3}$$^{.}$ FF$^{2\\ +}$ C$_{4}$$^{.}$ FF$^{3}$ + C$_{5}$$^{.}$ FF$^{4}$
+\end{lstlisting}
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-2-000}
+
+The name of the HVAC system node which supplies the inlet air conditions to the fan.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-2-000}
+
+The name of the HVAC system node to which the fan sends its outlet air.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-2-000}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Central System'', etc. A new meter for reporting is created for each unique subcategory (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the fan will be assigned to the ``General'' end-use subcategory.
+
+\subsubsection{Outputs}\label{outputs-2-009}
+
+\begin{itemize}
+\item
+  HVAC,Average,Fan Electric Power{[}W{]}
+\item
+  HVAC,Average,Fan Rise in Air Temperature {[}deltaC{]}
+\item
+  HVAC,Sum,Fan Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Fan Electric Power {[}W{]}}\label{fan-electric-power-w-2}
+
+This output field contains the average electricity consumption rate for the fan in Watts for the timestep being reported.
+
+\paragraph{Fan Rise in Air Temperature {[}deltaC{]}}\label{fan-rise-in-air-temperature-deltac-2}
+
+This output field contains the average rise in air temperature across the fan (outlet air temperature minus inlet air temperature) in degrees Celsius for the timestep being reported.
+
+\paragraph{Fan Electric Energy {[}J{]}}\label{fan-electric-energy-j-2}
+
+This output field contains the electricity consumption of the fan in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Fans, Group Key = System (ref. Output:Meter objects).
+
+\subsection{Fan:ZoneExhaust}\label{fanzoneexhaust}
+
+This fan object differs from the other fans in that it stands on its own in a zone rather than serving as one part of an HVAC air system. This object appears directly in a ZoneHVAC:EquipmentList object and all the controls are contained within the fan object. The zone exhaust fan model provides a way to include the electrical power used by the fan. It can also impact air flows in central air handlers by decreasing the flow of return air and sometimes increasing the outdoor air flow rate.
+
+There are several control options available for the exhaust fan including: an on/off availability schedule, interaction with system availability managers, minimum zone air temperature control limits and a variable flow fraction schedule.
+
+The way in which the exhaust fan impacts central air system can be controlled by declaring what portion of the flow has been balanced by simple airflow from infiltration, ventilation, or mixing. However it is important to note that presence of an exhaust fan does not by itself drive any simple airflow such as infiltration, ventilation, or zone mixing. There is no comprehensive automatic mass balancing between air system flows, exhaust flows, and the separate simple airflows. For balancing, the simple airflows need to have their own input objects that need to be coordinated with the exhaust fan.
+
+\subsubsection{Inputs}\label{inputs-3-014}
+
+\paragraph{Field: Name}\label{field-name-3-013}
+
+A unique user-assigned name for an instance of a Fan:ZoneExhaust. Any reference to this fan by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-3-002}
+
+The name of the schedule (ref: Schedule) that denotes whether the fan can run during a given time period. A schedule value of 0 indicates that the fan is off for that time period. A schedule value greater than 0 indicates that the fan can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this schedule by forcing the fan to be on or off.
+
+\paragraph{Field: Fan Total Efficiency}\label{field-fan-total-efficiency-3}
+
+This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.6.
+
+\paragraph{Field: Pressure Rise}\label{field-pressure-rise-3}
+
+The pressure rise in Pascals at full flow and standard (sea level) conditions (20 °C and 101325 Pa).
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate-3}
+
+The full load air volumetric flow rate (m\(^{3}\)/sec) at standard temperature and pressure (dry air at 20 °C drybulb). The program does use local barometric pressure to account for altitude using equation for ``standard atmospheric'' pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
+
+p = 101325*(1-2.25577E-05*Z)**5.2559
+
+where p = pressure in Pa and Z = altitude in m
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-3-000}
+
+The name of the HVAC system node which supplies the inlet air conditions to the fan. This node should be listed as a zone exhaust node in an associated ZoneHVAC:EquipmentConnections object.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-3-000}
+
+The name of the HVAC system node to which the fan sends its outlet air.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-3}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Kitchen Exhaust'', ``Fume Hoods'', etc. A new meter for reporting is created for each unique subcategory (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the fan will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Flow Fraction Schedule Name}\label{field-flow-fraction-schedule-name}
+
+This field is optional. If it is not used then the fan operates at the maximum flow rate. If a schedule is input here, then it should contain fractional values between 0.0 and 1.0, inclusive. The flow rate that the fan operates will be this fraction times the maximum flow rate. This allows a variable speed exhaust fan to be modeled according to a schedule.
+
+\paragraph{Field: System Availability Manager Coupling Mode}\label{field-system-availability-manager-coupling-mode}
+
+This field is optional. If if is not used then the exhaust fan is assumed to be integrated with the central air handler s system availability manager. This field can be used to control if the exhaust fan should operate independently or not. For example, when a night cycle availability manager turns on the central air system for freeze protection, this field can be used to control if the zone exhaust fans should also run at the same time or not. The key choice Coupled indicates that the exhaust fan should be integrated with the system availability manager so that the fan runs when the air system is forced to run. The key choice Decoupled indicates that the exhaust fan should operate on its own and ignore the system availability manager s requests so that the exhaust fan can remain off when the air system runs. The default is Coupled.
+
+\paragraph{Field: Minimum Zone Temperature Limit Schedule Name}\label{field-minimum-zone-temperature-limit-schedule-name}
+
+This field is optional. If it is not used then there will be no temperature-related control over the operation of the exhaust fan. If the field is used, then enter the name of a schedule with values for zone temperature values ( °C). The fan s control will be based on a comparison between the current zone air temperature and the schedule values. If the zone is warmer than the scheduled limit, then the fan will operate. When balancing with simple ventilation, this feature can be used to coordinate exhaust fan operation with ZoneVentilation:* controls for minimum indoor temperature.
+
+\paragraph{Field: Balanced Exhaust Fraction Schedule Name}\label{field-balanced-exhaust-fraction-schedule-name}
+
+This field is optional. If it is not used, then all the exhaust air flow is assumed to be unbalanced by any simple airflows, such as infiltration, ventilation, or zone mixing. Unbalanced exhaust is then modeled as being provided by the outdoor air system in the central air system. The modeling of unbalanced will reduce the flow rates at the zone s return air node by the flow rate that is being exhausted and will insure that the outdoor air flow rate is sufficient to serve the exhaust. If this field is used, then enter the name of a schedule with fractional values between 0.0 and 1.0, inclusive. This fraction is applied to the exhaust fan flow rate and the model tracks the portion of the exhaust that is balanced. Balanced exhaust is then modeled as being provided by simple airflows and does not impact the central air system return air or outdoor air flow rates. For example, if a kitchen zone with an exhaust fan is designed to draw half of its make up air from a neighboring dining room and the other half from the outdoor air system, then a schedule value of 0.5 could be used here.
+
+\subsubsection{Outputs}\label{outputs-3-007}
+
+\begin{itemize}
+\item
+  HVAC,Average,Fan Electric Power {[}W{]}
+\item
+  HVAC,Average,Fan Rise in Air Temperature{[}deltaC{]}
+\item
+  HVAC,Sum,Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Fan Unbalanced Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Fan Balanced Air Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Fan Electric Power {[}W{]}}\label{fan-electric-power-w-3}
+
+This output field contains the average electricity consumption rate for the fan in Watts for the timestep being reported.
+
+\paragraph{Fan Rise in Air Temperature {[}deltaC{]}}\label{fan-rise-in-air-temperature-deltac-3}
+
+This output field contains the average rise in air temperature across the fan (outlet air temperature minus inlet air temperature) in degrees Celsius for the timestep being reported.
+
+\paragraph{Fan Electric Energy {[}J{]}}\label{fan-electric-energy-j-3}
+
+This output field contains the electricity consumption of the fan in Joules for the timestep being reported. This output is also added to an output meter with Resource Type = Electricity, End Use Key = Fans, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Fan Unbalanced Air Mass Flow Rate {[}kg/s{]}}\label{fan-unbalanced-air-mass-flow-rate-kgs}
+
+\paragraph{Fan Balanced Air Mass Flow Rate {[}kg/s{]}}\label{fan-balanced-air-mass-flow-rate-kgs}
+
+These two output variables are available when the exhaust fan uses the input field called Balanced Exhaust Fraction Schedule Name. The balanced air flow is the result of the current flow rate times the balance fraction. The unbalanced air flow is the difference between the current flow rate and the balanced flow rate. These outputs are the resulting flow rates in kg/s.
+
+Examples of Fan:ConstantVolume, Fan:VariableVolume, Fan:ZoneExhaust, and , Fan:OnOff, fans in an IDF are:
+
+\begin{lstlisting}
+
+Fan:ConstantVolume,
+  Supply Fan 1,   !- Name
+  FanAndCoilAvailSched,               !- Availability Schedule Name
+  0.7,                     !- Fan Total Efficiency
+  600.0,                 !- Pressure Rise {Pa}
+  1.3,                     !- Maximum Flow Rate {m3/sec}
+  0.9,                     !- Motor Efficiency
+  1.0,                     !- Motor in Airstream Fraction
+  Air Loop Inlet Node, Cooling Coil Air Inlet Node;   !- Air Inlet Node Name, Air Outlet Node Name
+
+
+  Fan:VariableVolume,
+  Var Vol Supply Fan 1,   !- Name
+  FanAndCoilAvailSched,   !-Availability Schedule Name
+  0.7,                    !- Fan Total Efficiency
+  600.0,                !- Pressure Rise {Pa}
+  1.3,                    !- Maximum Flow Rate {m3/s}
+  0.20,                   !- Minimum Flow Rate {m3/s}
+  0.9,                    !- Motor Efficiency
+  1.0,                     !- Motor in Airstream Fraction
+  0.35071223,       !- Fan Coefficient 1
+  0.30850535,       !- Fan Coefficient 2
+  -0.54137364,       !- Fan Coefficient 3
+  0.87198823,       !- Fan Coefficient 4
+  0.000,                 !- Fan Coefficient 5
+  Air Loop Inlet Node, Cooling Coil Air Inlet Node;  !- Air Inlet Node Name,Air Outlet Node Name
+
+
+  Fan:ZoneExhaust,
+  Zone 2 Exhaust Fan,                           !-Name
+  FanAndCoilAvailSched,                       !-Availability Schedule Name
+  0.6,                                                         !-Fan Total Efficiency
+  125,                                                         !-Pressure Rise {Pa}
+  0.1,                                                         !-Maximum Flow Rate {m3/s}
+  Zone 2 Exhaust Node,                         !-Air Inlet Node Name
+  Zone 2 Exhaust Fan Outlet Node,   !-Air Outlet Node Name
+  Kitchen Exhaust;                                 !- End-Use Subcategory
+
+
+  Fan:OnOff,
+  AHU 1 Supply Fan,               !- Name
+  FanAvailSched,                     !- Availability Schedule Name
+  0.7,                                         !- Fan Total Efficiency
+  600.0,                                     !- Pressure Rise {Pa}
+  2.0,                                         !- Maximum Flow Rate {m3/s}
+  0.9,                                         !- Motor Efficiency
+  1.0,                                         !- Motor in Airstream Fraction
+  AHU 1 Air Loop Inlet,       !- Air Inlet Node Name
+  AHU 1 Supply Fan Outlet; !- Air Outlet Node Name
+\end{lstlisting}
+
+\subsection{FanPerformance:NightVentilation}\label{fanperformancenightventilation}
+
+This object is used for specifying an alternate set of performance parameters for a fan. These alternate parameters are used when a system manager (such as \emph{AvailabilityManager:NightVentilation}) sets a specified flow rate for a central forced air system. At this time, it can be used with Fan:ConstantVolume, Fan:VariableVolume, Fan:ZoneExhaust, and , Fan:OnOff fans, but not with Fan:ComponentModel fans. The fan model checks whether a fixed flow rate has been set; if it has the fan model will use these alternate performance parameters. Note that it is assumed that the fan will run at a fixed speed in the alternate mode. The inputs needed by this object are the fan name, fan total efficiency, pressure rise, flow rate, motor efficiency, and motor in airstream fraction.
+
+\subsubsection{Inputs}\label{inputs-4-013}
+
+\paragraph{Field: Fan Name}\label{field-fan-name-001}
+
+This is the name of a fan defined elsewhere in the input file. The night vent performance parameters will be applied to the named fan when a system manager has set the air system flow rate.
+
+\paragraph{Field: Fan Total Efficiency}\label{field-fan-total-efficiency-4}
+
+This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. This is a required field with no default.
+
+\paragraph{Field: Pressure Rise}\label{field-pressure-rise-4}
+
+The pressure rise in Pascals at full flow and standard (sea level) conditions (20 °C and 101325 Pa).
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate-4}
+
+The design volumetric flow rate of the fan (m\(^{3}\)/sec) at standard conditions. This input is not currently used by the night ventilation manager. The flow rate during night ventilation is specified using the SystemAvailabilityManager:NightVentilation ``Night Venting Flow Fraction'' field. This fraction is multiplied times the fan object's design flow rate.
+
+\paragraph{Field: Motor Efficiency}\label{field-motor-efficiency-3}
+
+The shaft power divided by the electrical power consumed. Must be between 0 and 1. This is a required field with no default.
+
+\paragraph{Field: Motor in Airstream Fraction}\label{field-motor-in-airstream-fraction-3}
+
+The fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat loss will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
+
+An example of use in an IDF:
+
+\begin{lstlisting}
+
+Fan:VariableVolume,
+  Supply Fan 1,                       !- Name
+  FanAvailSched,                     !- Availability Schedule Name
+  0.7,                                         !- Fan Efficiency
+  600.0,                                     !- Pressure Rise {Pa}
+  autosize,                               !- Maximum Flow Rate {m3/s}
+  autosize,                               !- Minimum Flow Rate {m3/s}
+  0.9,                                         !- Motor Efficiency
+  1.0,                                         !- Motor In Airstream Fraction
+  0.35071223,                           !- Fan Coefficient 1
+  0.30850535,                           !- Fan Coefficient 2
+  -0.54137364,                         !- Fan Coefficient 3
+  0.87198823,                           !- Fan Coefficient 4
+  0.000,                                     !- Fan Coefficient 5
+  Main Heating Coil 1 Outlet Node,   !- Air Inlet Node Name
+  VAV Sys 1 Outlet Node;     !- Air Outlet Node Name
+
+
+  FanPerformance:NightVentilation,
+  Supply Fan 1,                       !- Fan Name
+  0.7,                                         !- Fan Total Efficiency
+  67.0,                                       !- Pressure Rise {Pa}
+  autosize,                               !- Maximum Flow Rate {m3/s}
+  0.9,                                         !- Motor Efficiency
+  1.0;                                         !- Motor in Airstream Fraction
+\end{lstlisting}
+
+\subsection{Fan:ComponentModel}\label{fancomponentmodel}
+
+The Fan:ComponentModel fan is a more detailed fan type that can be defined in the air loop for central constant-air-volume (CAV) and variable-air-volume (VAV) systems. It includes inputs that describe the air-distribution system as well as the fan, its drive belt (if used), its motor, and its variable-frequency-drive (if used). See the engineering documentation for further descriptions about the inputs for this fan type.
+
+\subsubsection{Inputs}\label{inputs-5-011}
+
+\paragraph{Field: Name}\label{field-name-4-011}
+
+The required unique user-assigned alpha name for an instance of a Fan:ComponentModel. Any reference to this fan by another object will use this name.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-4-000}
+
+The required alpha name of the HVAC system node which supplies the inlet air conditions to the fan.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-4-000}
+
+The required alpha name of the HVAC system node to which the fan sends its outlet air.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-4-002}
+
+The required alpha name of the schedule (ref: Schedule) that denotes whether the fan can run during a given time period. A schedule value of 0 indicates that the fan is off for that time period. A schedule value greater than 0 indicates that the fan can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this schedule by forcing the fan to be on or off.
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate-5}
+
+The full-load volumetric airflow (m\(^{3}\)/sec) through the fan at standard temperature and pressure (dry air at 20 °C dry-bulb). To initialize the air systems being simulated, the program uses local barometric pressure adjusted for altitude, based on the equation for ``standard atmospheric'' pressure on p.6.1 of the 1997 ASHRAE Handbook of Fundamentals (SI edition):
+
+p = 101325 * (1 - 2.25577E-05 * Z)**5.2559
+
+where p = pressure in Pa and Z = altitude in m. Can be autosized.
+
+Specified or autosized maximum airflow rate (including effects of scaling by Field: Fan Sizing Factor) along with corresponding fan static pressure rise and fan shaft power are reported in the .eio file as, respectively, Design Fan Airflow {[}m3/s{]}, Design Fan Static Pressure Rise {[}Pa{]}, and Design Fan Shaft Power {[}W{]}.
+
+\paragraph{Field: Minimum Flow Rate}\label{field-minimum-flow-rate}
+
+The minimum volumetric airflow (m\(^{3}\)/sec) through the fan at standard temperature and pressure (see Maximum Flow Rate field above for condition details). Can be autosized.
+
+\paragraph{Field: Fan Sizing Factor}\label{field-fan-sizing-factor}
+
+The numeric dimensionless factor (\emph{F\(_{fan}\)}) used to multiply the specified or autosized full-load volumetric airflow (see Maximum Flow Rate field above for details) for fan sizing. If specified, minimum value is 1.0. Default is 1.0 if field is blank.
+
+\paragraph{Field: Fan Wheel Diameter}\label{field-fan-wheel-diameter}
+
+The required numeric outer diameter of the fan wheel (\emph{D\(_{fan}\)}, m). This value is determined from manufacturer s data. In general, larger diameter fans have higher maximum efficiency than smaller diameter fans of the same type (Ref: AMCA Standard 205-10: Energy Efficiency Classification for Fans). Must be greater than zero.
+
+\paragraph{Field: Fan Outlet Area}\label{field-fan-outlet-area}
+
+The required numeric outlet area of the fan (\emph{A\(_{fan,out}\)}, m\(^{2}\)). This value is determined from manufacturer s data. It is used to convert fan total pressure rise to fan static pressure rise. Fan static pressure rise is the fan total pressure rise minus the fan outlet velocity pressure; it is not the difference between fan outlet and inlet static pressures (Ref: ANSI/AMCA Standard 210-07, ANSI/ASHRAE Standard 51-07: Laboratory Methods of Testing Fans for Certified Aerodynamic Performance Rating). Must be greater than zero.
+
+\paragraph{Field: Maximum Fan Static Efficiency}\label{field-maximum-fan-static-efficiency}
+
+The required numeric maximum ratio (\(\eta_{fan,max}\) ) between the power delivered to the air (\emph{H\(_{air}\)}, W) and the fan shaft input power (\emph{H\(_{fan}\)}, W). For this parameter, \emph{H\(_{air}\)} is the volumetric airflow through the fan multiplied by the fan static pressure rise. Maximum fan static efficiency is determined from analyses of manufacturers data using:
+
+\begin{equation}
+{\eta_{fan,\max }} = \max \left[ {\frac{{\left( {\Delta {P_{fan}} * {Q_{fan}}} \right)}}{{{H_{fan}}}}} \right]
+\end{equation}
+
+where \emph{P\(_{fan}\)} is fan static pressure rise (Pa) and \emph{Q\(_{fan}\)} is airflow through the fan (m\(^{3}\)/sec). Typically, do not select curves on fan performance maps of pressure rise versus flow correspond to or are near maximum efficiency. Must be greater than zero and less than or equal to 1.0.
+
+Calculated fan static efficiency at design flow condition (including part-load effects of oversized fan) is reported in the .eio file as Design Fan Efficiency {[}-{]}.
+
+\paragraph{Field: Euler Number at Maximum Fan Static Efficiency}\label{field-euler-number-at-maximum-fan-static-efficiency}
+
+The required numeric Euler number (\emph{Eu\(_{max}\)}), which is also called the throttling or pressure coefficient, and is the ratio of pressure forces to inertial forces. The Euler number is determined from analyses of manufacturer s data using:
+
+\begin{equation}
+Eu = \frac{{\left( {\Delta {P_{fan}} * D_{fan}^4} \right)}}{{\left( {\rho  * Q_{fan}^2} \right)}}
+\end{equation}
+
+where \emph{P\(_{fan}\)} is fan static pressure rise (Pa; see \emph{Fan Pressure Rise Curve Name} field), \emph{D\(_{fan}\)} is wheel diameter (m), \emph{�} is the manufacturer s reference air density (kg/m\(^{3}\)), and \emph{Q\(_{fan}\)} is airflow through the fan (m\(^{3}\)/sec). \emph{Eu\(_{max}\)} is calculated using any pair of pressure rise and airflow values that correspond with maximum fan static efficiency for the specified fan. Must be greater than zero.
+
+\paragraph{Field: Maximum Dimensionless Fan Airflow}\label{field-maximum-dimensionless-fan-airflow}
+
+The required numeric maximum dimensionless airflow (\(\psi_{max}\)) through the fan, which corresponds to the maximum ratio between the airflow through the fan (\(Q_{fan}\), m\(^{3}\)/sec) and the fan shaft rotational speed (\(\omega_{fan}\)\emph{, rpm}) for the specified fan wheel diameter (D\(_{fan}\)\emph{, m}). \(\varphi_{max}\) is determined from manufacturers data using:
+
+\begin{equation}
+\varphi_{\max} = \frac{30}{\pi D_{fan}^3} \cdot \max \left( \frac{Q_{fan}}{\omega_{fan}} \right)
+\end{equation}
+
+\(\varphi_{max}\) occurs at minimum \emph{Eu}, which corresponds to maximum speed (high flow) with zero pressure rise. The factor (\(30/\pi\)) converts revolutions per minute (rpm) to rad/s. Must be greater than zero.
+
+\paragraph{Field: Motor Fan Pulley Ratio}\label{field-motor-fan-pulley-ratio}
+
+The numeric dimensionless ratio of the motor pulley diameter to the fan pulley diameter (\emph{D\(_{motor,pulley}\) / D\(_{fan,pulley}\)}). If specified, must be greater than zero. This ratio can be adjusted to account for belt slip if the fractional slip is known (multiply the drive ratio with no slip by 1+s, where s is the belt fractional slip). Default is 1.0 if field is blank (leave blank if no belt; i.e., direct drive). Can be autosized (assumes no slip).
+
+Specified or autosized motor/fan pulley diameter ratio is reported in the .eio file as Drive Ratio {[}-{]}. Autosized ratio is based on fan speed in revolutions per minute (rpm), calculated at design flow condition, divided by Field: Motor Maximum Speed.
+
+\paragraph{Field: Belt Maximum Torque}\label{field-belt-maximum-torque}
+
+The required numeric maximum output torque capacity of the fan drive belt (\(\tau_{belt,max}\) {[}N-m{]}). If specified, must be greater than zero. Can be autosized. Use autosize if no belt (i.e., direct drive).
+
+Specified or autosized belt maximum output torque (including effects of scaling by Field: Belt Sizing Factor) is reported in the .eio file as Design Belt Output Torque {[}N -m{]}. Also, calculated maximum belt efficiency corresponding to Design Fan Shaft Power, along with belt efficiency at design flow condition (including part-load effects of oversized belt), are reported in the .eio file as, respectively, Maximum Belt Efficiency {[}-{]} and Design Belt Efficiency {[}-{]}.
+
+\paragraph{Field: Belt Sizing Factor}\label{field-belt-sizing-factor}
+
+The numeric dimensionless factor (\emph{F\(_{belt}\)}) used to multiply the specified or autosized fan shaft maximum output torque (\(_{belt,max}\)*). If specified, minimum value is 1.0. Default is 1.0 if field is blank.
+
+\paragraph{Field: Belt Fractional Torque Transition}\label{field-belt-fractional-torque-transition}
+
+The numeric transition point (\emph{x\(_{belt,trans}\)}) between performance curves for Regions 1 and 2 for the drive belt normalized part-load efficiency. Must be between 0.0 and 1.0. Default is 0.167 (corresponds to generic V-belt) if field is blank.
+
+\paragraph{Field: Motor Maximum Speed}\label{field-motor-maximum-speed}
+
+The required numeric maximum rotational speed of the fan motor shaft (\(\omega_{motor,max}\)) in revolutions per minute (rpm). Typical values for motors supplied by 60 Hz power are near 900, 1200, 1800, and 3600 rpm. Must be greater than zero.
+
+\paragraph{Field: Maximum Motor Output Power}\label{field-maximum-motor-output-power}
+
+The required numeric maximum output power (input power to the fan drive belt) by the motor (\emph{H\(_{belt,max}\)}, W). If specified, must be greater than zero. Can be autosized. In the case of direct drive, \emph{H\(_{belt,max}\)} corresponds to the maximum fan shaft power (\emph{H\(_{fan,max}\)}).
+
+Specified or autosized maximum motor output power (including effects of scaling by Field: Motor Sizing Factor) is reported in the .eio file as Design Motor Output Power {[}W{]}. Also, calculated maximum motor efficiency corresponding to Design Motor Output Power, along with motor efficiency at design flow condition (including part-load effects of oversized motor), are reported in the .eio file as, respectively, Maximum Motor Efficiency {[}-{]} and Design Motor Efficiency {[}-{]}. Note that maximum motor efficiency often occurs at less than full load.
+
+\paragraph{Field: Motor Sizing Factor}\label{field-motor-sizing-factor}
+
+The numeric dimensionless sizing factor (\emph{F\(_{motor}\)}) used to multiply the specified or autosized fan motor output power (\emph{H\(_{belt,max}\)}). If specified, minimum value is 1.0. Default is 1.0.
+
+\paragraph{Field: Motor In Airstream Fraction}\label{field-motor-in-airstream-fraction-4}
+
+The numeric fraction of the combined motor and belt heat that is added to the air stream. A value of 0.0 means that the motor and belt are completely outside the air stream. A value of 1.0 means that all of the motor and belt heat loss will go into the air stream and act to cause an air enthalpy rise. Must be between 0.0 and 1.0. Default is 1.0.
+
+\paragraph{Field: VFD Efficiency Type}\label{field-vfd-efficiency-type}
+
+The alpha basis for calculating fan variable-frequency-drive (VFD) efficiency: Power , which corresponds to a function of the fraction of full-load motor input power (\emph{H\(_{motor}\)} / \emph{H\(_{motor,max}\)}), or Speed , which corresponds to a function of the fraction of full-load speed (\(\omega_{motor} / \omega_{max}\)). If this field is blank, then it is assumed that the VFD efficiency is 0.97. If no VFD is used, then specify Power and also specify a VFD efficiency curve with a constant value of 1.0 (see VFD Efficiency Curve Name field for details).
+
+\paragraph{Field: Maximum VFD Output Power}\label{field-maximum-vfd-output-power}
+
+The required numeric maximum output power (input power to the fan motor) by the variable frequency drive (\emph{H\(_{motor,max}\)}, W). If specified, must be greater than zero. Can be autosized.
+
+Specified or autosized maximum VFD output power (including effects of scaling by Field: VFD Sizing Factor) and corresponding VFD input power are reported in the .eio file as, respectively, Design VFD Output Power {[}W{]} and Rated Power {[}W{]}. Also, calculated VFD efficiency corresponding to Design VFD Output Power (including part-load effects of oversized VFD) along with corresponding combined system efficiency (fan, belt, motor, and VFD efficiencies multiplied together) at design flow condition are reported in the .eio file as, respectively, Design VFD Efficiency {[}-{]} and Design Combined Efficiency {[}-{]}.
+
+\paragraph{Field: VFD Sizing Factor}\label{field-vfd-sizing-factor}
+
+The numeric dimensionless factor (\emph{F\(_{VFD}\)}) used to multiply the specified or autosized motor maximum input power (\emph{H\(_{motor,max}\)}). If specified, minimum value is 1.0. Default is 1.0 if field is blank.
+
+\paragraph{Field: Fan Pressure Rise Curve Name}\label{field-fan-pressure-rise-curve-name}
+
+The required alpha name of the fan total pressure rise performance curve (ref: Curve:FanPressureRise in Performance Curves) that parameterizes the variation of fan total pressure rise (\emph{P\(_{fan,tot}\)}, Pa) as a function of volumetric flow through the fan (\emph{Q\(_{fan}\)}, m\(^{3}\)/s) and duct static pressure set point (\emph{P\(_{sm}\)}, Pa). The fan outlet velocity pressure is subtracted from the output of this curve to determine fan static pressure rise, which is then used to calculate a dimensionless Euler number at each time step. The Euler number is in turn used to determine fan efficiency, speed, and torque (the Euler number is defined in the \emph{Euler Number at Maximum Fan Static Efficiency} field). This curve should be valid for the range of volumetric flows, distribution system leakage, duct static pressures, and static pressures surrounding the ducts anticipated for the simulation period.
+
+\paragraph{Field: Duct Static Pressure Reset Curve Name}\label{field-duct-static-pressure-reset-curve-name}
+
+The required alpha name of the performance curve that parameterizes the variation of the duct static pressure set point (\(P_{sm}\), Pa) as a function of volumetric flow through the fan (\(Q_{fan}\), m\(^{3}\)/s), which is used so that the resistance associated with VAV box damper operation is reduced.
+
+The output of this curve is used to calculate the duct static pressure set point at each time step. This curve should be valid for the range of duct static pressure set points and volumetric flows, anticipated for the simulation period.
+
+For an ad hoc linear duct static pressure reset scheme, the relation (ref: Curve:Linear in Performance Curves) between duct static pressure (\(P_{sm}\), Pa) and flow through the fan (\(Q_{fan}\), m\(^{3}\)/s) for \(Q_{fan,min} \le Q_{fan} \le Q_{fan,max}\) is:
+
+\begin{equation}
+P_{sm} = P_{sm,\min } + \left( P_{sm,\max } - P_{sm,\min } \right) * \frac{{\left( {{Q_{fan}} - {Q_{fan,\min }}} \right)}}{{\left( {{Q_{fan,\max }} - {Q_{fan,\min }}} \right)}} = {C_1} + {C_2}*{Q_{fan}}
+\end{equation}
+
+where \({C_1} = {P_{sm,\min }} - {C_2}*{Q_{fan,\min }}\) and \({C_2} = \frac{{\left( {{P_{sm,\max }} - {P_{sm,\min }}} \right)}}{{\left( {{Q_{fan,\max }} - {Q_{fan,\min }}} \right)}}\)
+
+For \emph{Q\(_{fan}\)} \textless{} \emph{Q\(_{fan,min}\)}, \emph{P\(_{sm}\)} = \emph{P\(_{sm,min}\)};for \emph{Q\(_{fan}\)} \textgreater{} \emph{Q\(_{fan,max}\)}, \emph{P\(_{sm}\)} = \emph{P\(_{sm,max}\)}
+
+The minimum and maximum fan airflows (\emph{Q\(_{fan,min}\)} and \emph{Q\(_{fan,max}\)}) correspond respectively to the minimum and maximum duct static pressure set points (\emph{P\(_{sm,min}\)} and \emph{P\(_{sm,max}\)}).
+
+If no duct static pressure reset scheme is used and the duct static pressure set point is constant, then parameter \emph{C\(_{2}\)} is set to zero and \emph{C\(_{1}\)} represents the constant duct static pressure set point.
+
+\paragraph{Field: Normalized Fan Static Efficiency Curve Name Non-Stall Region}\label{field-normalized-fan-static-efficiency-curve-name-non-stall-region}
+
+The required alpha name of the exponential-modified skew normal performance curve (ref: Curve:ExponentialSkewNormal in Performance Curves) that parameterizes the normalized fan static efficiency (\(\eta_{\rm{fan}}(x_{\rm{fan}}) / \eta_{\rm{fan, max}}\)) at each time step for the normal operating (non-stall) region of the fan performance map as a function of \(x_{\rm{fan}}\), which is defined as log-base-10 of Eu at the fan flow and pressure rise operating point divided by Eu at maximum fan static efficiency \([log_{10}(Eu / Eu_{\rm{max}})]\). In this region, \(x_{\rm{fan}} \le 0\).
+
+The output of this curve is used to calculate the fan efficiency \(\eta_{\rm{fan}} (x_{\rm{fan}})\) at each time step by modifying \(\eta_{\rm{fan, max}}\) (see \emph{Maximum Fan Static Efficiency} field). This curve should have a maximum of 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
+
+\paragraph{Field: Normalized Fan Static Efficiency Curve Name Stall Region}\label{field-normalized-fan-static-efficiency-curve-name-stall-region}
+
+The required alpha name of the exponential-modified skew normal performance curve (ref: Curve:ExponentialSkewNormal in Performance Curves) that parameterizes the normalized fan static efficiency (\(\eta_{\rm{fan}} (x_{\rm{fan}}) / \eta_{\rm{fan, max}}\)) at each time step for the stall region of the fan performance map as a function of \(x_{\rm{fan}}\) (see \emph{Normalized Fan Static Efficiency Curve Name Non-Stall Region} field). In this region, \(x_{\rm{fan}} > 0\).
+
+The output of this curve is used to calculate the fan efficiency \(\eta_{\rm{fan}} ( x_{\rm{fan}} )\) at each time step by modifying \(\eta_{\rm{fan, max}}\) (see \emph{Maximum Fan Static Efficiency} field). This curve should have a maximum of 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
+
+\paragraph{Field: Normalized Dimensionless Airflow Curve Name Non-Stall Region}\label{field-normalized-dimensionless-airflow-curve-name-non-stall-region}
+
+The required alpha name of the sigmoid performance curve (ref: Curve:Sigmoid in Performance Curves) that parameterizes the normalized dimensionless airflow through the fan (\(\varphi (x_{\rm{fan}}) / \varphi_{\rm{max}}\)) at each time step for the normal operating (non-stall) region of the fan performance map as a function of \(x_{\rm{fan}}\), which is defined as log-base-10 of Eu at the fan flow and pressure rise operating point divided by Eu at maximum fan static efficiency \([log_{10}(Eu / Eu_{\rm{max}})]\). In this region, \(x_{\rm{fan}} \le 0\).
+
+The output of this curve is used to calculate the dimensionless airflow \(\varphi (x_{\rm{fan}})\) at each time step by modifying \(\varphi_{\rm{max}}\) (see \emph{Maximum Dimensionless Fan Airflow} field). This curve should have a maximum of 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
+
+\paragraph{Field: Normalized Dimensionless Airflow Curve Name Stall Region}\label{field-normalized-dimensionless-airflow-curve-name-stall-region}
+
+The required alpha name of the sigmoid performance curve (ref: Curve:Sigmoid in Performance Curves) that parameterizes the normalized dimensionless airflow through the fan (\(\varphi (x_{\rm{fan}}) / \varphi_{\rm{max}}\)) at each time step for the stall region of the fan performance map as a function of \(x_{\rm{fan}}\) (see \emph{Normalized Dimensionless Airflow Curve Name Non-Stall Region} field). In this region, \(x_{\rm{fan}} > 0\).
+
+The output of this curve is used to calculate the dimensionless airflow \(\varphi (x_{\rm{fan}})\) at each time step by modifying \(\varphi_{\rm{max}}\) (see \emph{Maximum Dimensionless Fan Airflow} field). This curve should have a maximum of 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
+
+\paragraph{Field: Maximum Belt Efficiency Curve Name}\label{field-maximum-belt-efficiency-curve-name}
+
+The alpha name of the quartic polynomial performance curve (ref: Curve:Quartic in Performance Curves) that determines the maximum fan drive belt efficiency in logarithmic space (\(\eta_{\rm{belt, max, ln}}\)) as a function of \(x_{\rm{belt, max}}\). The curve is:
+
+\begin{equation}
+\eta_{\rm{belt, max, ln}} = C_1 + C_2 \cdot x_{\rm{belt, max}} + C_3 \cdot x_{\rm{belt, max}}^2 + C_4 \cdot x_{\rm{belt, max}}^3 + C_5 \cdot x_{\rm{belt, max}}^4
+\end{equation}
+
+where \(x_{\rm{belt, max}} = ln(F_{\rm{belt}} \cdot H_{\rm{fan, max}})\) with \(H_{\rm{fan, max}}\) expressed in terms of hp.
+
+Note that \(\eta_{\rm{belt, max}} = exp(\eta_{\rm{belt, max, ln}})\).
+
+The output of this curve must be greater than zero and less than or equal to 1.0. If \(\eta_{\rm{belt, max}}\) is known, it is represented by coefficient \(C_1\) (\(= ln(\eta_{\rm{belt, max}})\)). In this case, coefficients \(C_2\) through \(C_5\) are set to zero. If this field is left blank (e.g., there is no belt), the model assumes that the output of the modifier curve is 1.0 for the entire simulation (maximum belt efficiency = 1.0).
+
+\paragraph{Field: Normalized Belt Efficiency Curve Name Region 1}\label{field-normalized-belt-efficiency-curve-name-region-1}
+
+The alpha name of the single rectangular hyperbola type 2 performance curve (ref: Curve:RectangularHyperbola2 in Performance Curves) that determines the normalized (par-load) fan drive belt efficiency (\(\eta_{\rm{belt}}(x_{\rm{belt}}) / \eta_{\rm{belt, max}}\)) as a function of \(x_{\rm{belt}}\). Normalized belt efficiency is represented by a segmented curve with three different regions. The curve for Region 1 (\(0 \le x_{\rm{belt}} < x_{\rm{belt, trans}}\)) is:
+
+\begin{equation}
+  \frac{\eta_{\rm{belt}} ( x_{\rm{belt}} )}{\eta_{\rm{belt, max}}} = \frac{(C_1 \cdot x_{\rm{belt}})}{(C_2 + x_{\rm{belt}})} + C_3 \cdot x_{\rm{belt}}
+\end{equation}
+
+where \(x_{\rm{belt}}\) = \(\tau_{\rm{belt}} / \tau_{\rm{belt, max}}\); \(\tau_{\rm{belt}}\) is the belt output torque that corresponds to the calculated power input to the fan shaft (\(H_{\rm{fan}}\), W) by the drive belt and the calculated fan shaft speed (\(\omega_{\rm{fan}}\), rpm).
+
+The output of this curve is used to calculate the belt efficiency \(\eta_{\rm{belt}} (x_{\rm{belt}})\) in Region 1 at each time step by modifying \(\eta_{\rm{belt, max}}\) (see \emph{Maximum Belt Efficiency Curve Name} field). The output of this curve must be greater than zero and less than or equal to 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
+
+If this field is left blank, the model assumes that the output of the modifier curve is 1.0 for the entire simulation (i.e., constant belt efficiency at \(\eta_{\rm{belt, max}}\) in Region 1).
+
+\paragraph{Field: Normalized Belt Efficiency Curve Name Region 2}\label{field-normalized-belt-efficiency-curve-name-region-2}
+
+The alpha name of the exponential decay performance curve (ref: Curve:ExponentialDecay in Performance Curves) that determines the normalized (part-load) fan drive belt efficiency (\(\eta_{\rm{belt}} (x_{\rm{belt}}) / \eta_{\rm{belt, max}}\)) as a function of \(x_{\rm{belt}}\). Normalized belt efficiency is represented by a segmented curve with three different regions. The curve for Region 2 (\(x_{\rm{belt, trans}} \le x_{\rm{belt}} \le 1\)) is:
+
+\begin{equation}
+  \eta_{\rm{belt}} (x_{\rm{belt}}) / \eta_{\rm{belt, max}} = C_1 + C_2 \cdot exp(C_3 \cdot x_{\rm{belt}})
+\end{equation}
+
+where \(x_{\rm{belt}} = \tau_{\rm{belt}} / \tau_{\rm{belt, max}}\); \(\tau_{\rm{belt}}\) is the belt output torque that corresponds to the calculated power input to the fan shaft (\(H_{\rm{fan}}\), W) by the drive belt and the calculated fan shaft speed (\(\omega_{\rm{fan}}\), rpm).
+
+The output of this curve is used to calculate the belt efficiency \(\eta_{\rm{belt}} (x_{\rm{belt}}\) in Region 2 at each time step by modifying \(\eta_{\rm{belt, max}}\) (see \emph{Maximum Belt Efficiency Curve Name} field). The output of this curve must be greater than zero and less than or equal to 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
+
+If this field is left blank, the model assumes that the output of the modifier curve is 1.0 for the entire simulation (i.e., constant belt efficiency at \(\eta_{\rm{belt, max}}\) in Region 2).
+
+\paragraph{Field: Normalized Belt Efficiency Curve Name Region 3}\label{field-normalized-belt-efficiency-curve-name-region-3}
+
+The alpha name of the single rectangular hyperbola type 2 performance curve (ref: Curve:RectangularHyperbola2 in Performance Curves) that determines the normalized (part-load) fan drive belt efficiency (\(\eta_{\rm{belt}} (x_{\rm{belt}}) / \eta_{\rm{belt, max}}\)) as a function of \(x_{\rm{belt}}\). Normalized belt efficiency is represented by a segmented curve with three different regions. The curve for Region 3 (\(x_{\rm{belt}} > 1\)) is:
+
+\begin{equation}
+  \eta_{\rm{belt}} ( x_{\rm{belt}} ) / \eta_{\rm{belt, max}} = ( C_1 \cdot x_{\rm{belt}} ) / ( C_2 + x_{\rm{belt}} ) + C_3 \cdot x_{\rm{belt}}
+\end{equation}
+
+where \(x_{\rm{belt}} = \tau_{\rm{belt}} / \tau_{\rm{belt, max}}\); \(\tau_{\rm{belt}}\) is the belt output torque that corresponds to the calculated power input to the fan shaft (\(H_{\rm{fan}}\), W) by the drive belt and the calculated fan shaft speed (\(\omega_{\rm{fan}}\), rpm).
+
+The output of this curve is used to calculate the belt efficiency \(\eta_{\rm{belt}} (x_{\rm{belt}})\) in Region 3 at each time step by modifying \(\eta_{\rm{belt, max}}\) (see \emph{Maximum Belt Efficiency Curve Name} field). The output of this curve must be greater than zero and less than or equal to 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
+
+If this field is left blank, the model assumes that the output of the modifier curve is 1.0 for the entire simulation (i.e., constant belt efficiency at \(\eta_{\rm{belt, max}}\) in Region 3).
+
+\paragraph{Field: Maximum Motor Efficiency Curve Name}\label{field-maximum-motor-efficiency-curve-name}
+
+The alpha name of the single rectangular hyperbola type 1 performance curve (ref: Curve: RectangularHyperbola1 in Performance Curves) that determines the maximum fan motor efficiency (\(\eta_{\rm{motor, max}}\)) as a function of \(x_{\rm{motor, max}}\). The curve is:
+
+\begin{equation}
+  \eta_{\rm{motor, max}} = (C_1 \cdot x_{\rm{motor, max}}) / (C_2 + x_{\rm{motor, max}}) + C_3
+\end{equation}
+
+where \(x_{\rm{motor, max}} = ln(F_{\rm{motor}} \cdot H_{\rm{belt, max}})\) with \(H_{\rm{belt, max}}\) expressed in terms of hp. \(H_{\rm{belt, max}}\) is the maximum output power from the motor to the belt, which corresponds to the calculated maximum power input to the fan shaft (\(H_{\rm{fan, max}}\), W).
+
+The output of this curve must be greater than zero and less than or equal to 1.0. If \(\eta_{\rm{motor, max}}\) is known, it is represented by coefficient \(C_3\). In this case, coefficients \(C_1\) and \(C_2\) are set to zero.
+
+If this field is left blank, the model assumes that the output of the modifier curve is 1.0 for the entire simulation (maximum motor efficiency = 1.0).
+
+\paragraph{Field: Normalized Motor Efficiency Curve Name}\label{field-normalized-motor-efficiency-curve-name}
+
+The name of the HVAC system node to which the fan sends its outlet air.
+
+The alpha name of the single rectangular hyperbola type 2 performance curve (ref: Curve:RectangularHyperbola2 in Performance Curves) that determines the normalized (part-load) fan motor efficiency (\(\eta_{\rm{motor}} (x_{\rm{motor}}) /  \eta_{\rm{motor, max}}\)) as a function of the motor load fraction \(x_{\rm{motor}}\). The curve is:
+
+\begin{equation}
+  \eta_{\rm{motor}} (x_{\rm{motor}}) / \eta_{\rm{motor, max}} = (C_1 \cdot x_{\rm{motor}}) / (C_2 + x_{\rm{motor}}) + (C_3 \cdot x_{\rm{motor}}
+\end{equation}
+
+where \(x_{\rm{motor}} = H_{\rm{belt}} / H_{\rm{belt, max}}\). \(H_{\rm{belt}}\) is the calculated output power from the motor to the belt (W), which corresponds to the calculated power input to the fan shaft (\(H_{\rm{fan}}\), W).
+
+  The output of this curve is used to calculate the motor efficiency (\(\eta_{\rm{motor}} (x_{\rm{motor}})\)) at each time step by modifying \(\eta_{\rm{motor, max}}\) (see \emph{Maximum Motor Efficiency Curve Name} field). The output of this curve must be greater than zero and less than or equal to 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
+
+If this field is left blank, the model assumes that the output of the modifier curve is 1.0 for the entire simulation (i.e., constant motor efficiency at \(\eta_{\rm{motor, max}}\)).
+
+\paragraph{Field: VFD Efficiency Curve Name}\label{field-vfd-efficiency-curve-name}
+
+The alpha name of the single rectangular hyperbola type 2 performance curve (e.g., Curve:RectangularHyperbola2 in Performance Curves) that determines the VFD efficiency (\(\eta_{VFD}(x_{VFD})\)) as a function of the fractional input power of the motor or fractional motor speed (\(x_{VFD}\)). An example of the curve is:
+
+\begin{equation}
+  \eta_{VFD}(x_{VFD}) = (C_1 \cdot x_{VFD}) / (C_2 + x_{VFD}) + C_3 \cdot x_{VFD}
+\end{equation}
+
+where \(x_{VFD} = H_{\rm{motor}} / H_{\rm{motor, max}}\) or \(\omega_{\rm{motor}} / \omega_{\rm{motor, max}}\).
+
+The output of this curve is used to calculate the VFD efficiency \(\eta_{VFD}(x_{VFD})\) at each time step. The output of this curve must be greater than zero and less than or equal to 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
+
+If this field is left blank, the model assumes that the output of the modifier curve is 0.97 for the entire simulation (i.e., constant VFD efficiency of 0.97).
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-4}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Central System''. A new meter for reporting is created for each unique subcategory (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the fan will be assigned to the ``General'' end-use subcategory.
+
+An example of use in an IDF:
+
+\begin{lstlisting}
+Fan:ComponentModel,
+  Supply Fan 1,                     ! Fan Name
+  Main Heating Coil 1 Outlet Node,  ! Inlet Node Name
+  VAV Sys 1 Outlet Node,            ! Outlet Node Name
+  FanAvailSched,                    ! Fan Schedule
+  autosize,                         ! Maximum Flow Rate [m3/s]
+  autosize,                         ! Minimum Flow Rate [m3/s]
+  1.0,                              ! Fan Sizing Factor [-]
+  0.3048,                           ! Fan Wheel Diameter [m]
+  0.0873288576,                     ! Fan Outlet Area [m2]
+  0.514,                            ! Maximum Fan Static Efficiency [-]
+  9.76,                             ! Euler Number at Maximum Fan Static Efficiency [-]
+  0.160331811647483,                ! Maximum Dimensionless Fan Airflow [-]
+  autosize,                         ! Motor/Fan Pulley Ratio [-]
+  autosize,                         ! Belt Maximum Torque [N m]
+  1.0,                              ! Belt Sizing Factor [-]
+  0.167,                            ! Belt Fractional Torque Transition [-]
+  1800,                             ! Motor Maximum Speed [rpm]
+  autosize,                         ! Maximum Motor Output Power [W]
+  1.0,                              ! Motor Sizing Factor [-]
+  1.0,                              ! Motor In Airstream Fraction [-]
+  Power,                            ! VFD Efficiency Type
+  autosize,                         ! Maximum VFD Output Power [W]
+  1.0,                              ! VFD Sizing Factor [-]
+  VSD Example,                      ! Fan Pressure Rise Curve Name
+  DiagnosticSPR,                    ! Duct Static Pressure Reset Curve Name
+  FanEff120CPLANormal,              ! Fan Efficiency Curve Name     Non-Stall
+  FanEff120CPLAStall,               ! Fan Efficiency Curve Name - Stall
+  FanDimFlowNormal,                 ! Dimensionless Airflow Curve Name-Non-Stall
+  FanDimFlowStall,                  ! Dimensionless Airflow Curve Name-Stall
+  BeltMaxEffMedium,                 ! Maximum Belt Efficiency Curve Name
+  BeltPartLoadRegion1,              ! Normalized Belt Efficiency Curve Name
+  BeltPartLoadRegion2,              ! Normalized Belt Efficiency Curve Name
+  BeltPartLoadRegion3,              ! Normalized Belt Efficiency Curve Name
+  MotorMaxEffAvg,                   ! Maximum Motor Efficiency Curve Name
+  MotorPartLoad,                    ! Normalized Motor Efficiency Curve Name
+  VFDPartLoad;                      ! VFD Efficiency Curve Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-005}
+
+\begin{itemize}
+\item
+  HVAC,Average,Fan Electric Power{[}W{]}
+\item
+  HVAC,Average,Fan Rise in Air Temperature {[}deltaC{]}
+\item
+  HVAC,Sum,Fan Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Fan Electric Power {[}W{]}}\label{fan-electric-power-w-4}
+
+This output field contains the average electricity consumption rate for the fan in Watts for the timestep being reported.
+
+\paragraph{Fan Rise in Air Temperature {[}deltaC{]}}\label{fan-rise-in-air-temperature-deltac-4}
+
+This output field contains the average rise in air temperature across the fan (outlet air temperature minus inlet air temperature) in degrees Celsius for the timestep being reported.
+
+\paragraph{Fan Electric Energy {[}J{]}}\label{fan-electric-energy-j-4}
+
+This output field contains the electricity consumption of the fan in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Fans, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Other Outputs}\label{other-outputs}
+
+Several parameters input by the user or calculated during component sizing for the design condition (maximum system airflow) are reported separately in the \textless{}filename\textgreater{}.eio file. These parameters include fan airflow and pressure rise; fan shaft input, motor output, VFD output, and VFD input (rated) power; pulley drive ratio; belt output torque; and fan, belt, motor, VFD, and combined system efficiencies. They can be identified by lines in the .eio file beginning with Component Sizing Information, Fan:ComponentModel . The same values are also reported under the ComponentSizingSummary heading in the \textless{}filename\textgreater{}Table.html file.
diff --git a/doc/input-output-reference/src/overview/group-fluid-properties.tex b/doc/input-output-reference/src/overview/group-fluid-properties.tex
new file mode 100644
index 00000000000..9a8412ee8b1
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-fluid-properties.tex
@@ -0,0 +1,233 @@
+\section{Group Fluid Properties}\label{group-fluid-properties}
+
+The Fluid Property routines in EnergyPlus have been designed for ease of use and to allow users to add refrigerant and glycol data to the input file without having to make any changes to the program code. Fluid properties are calculated by interpolating the tabulated data in the input file. The main input requirement is that in order to add a new fluid, a user must enter a full set of data. The user may determine the interval between data points according to the desired accuracy and range required. Data for a number of common fluids are available in the required format in a reference dataset so that the user may append this data to their input file. In addition, data for Water, Ethylene Glycol (in various concentrations from 0 to 90\%), and Propylene Glycol (in various concentrations from 0 to 90\%) are available as default values within EnergyPlus.
+
+Each fluid is categorized as either a Refrigerant or Glycol . Refrigerant data is further categorized as either saturated or superheated. Saturated refrigerant data is indexed, in the input data, according to pressure and temperature i.e.~the specific heat, density, enthalpy in the input data are given for a given combination of pressure and temperature. Saturated refrigerant data is indexed according to pressure and quality. In the case of saturated pressure data only a temperature index is used. Glycol data is indexed in the input data according to temperature and concentration. The input data structure for each property is essentially two-dimensional (a matrix). However, since all fluid loops are assumed to be of constant concentration, EnergyPlus internally will interpolate from input data to data for the actual concentration being used in a particular loop. This reduces internally to a one-dimensional array of data for various properties where temperature is the only variable. This saves time since it reduces all interpolations for glycols to a single dimension.
+
+In most cases there will be combinations of index variable (e.g.~some combination of pressure and temperature) at which either no data is available, or the property data is invalid/irrelevant. For example, in the superheated refrigerant data, some combinations of temperature and pressure may correspond to a state in the saturated rather than superheated region. Similarly, in the case of glycols there may be some combinations of temperature and concentration that would correspond to the frozen state. In these cases, and where data is just not available, a zero should be present in the data at these points to indicate an invalid condition. EnergyPlus uses the presence of zeros to detect invalid conditions and give warning messages.
+
+\subsection{FluidProperties:Name}\label{fluidpropertiesname}
+
+The names of each fluid for which property data is given in the user input have to be specified in FluidProperties:Name data objects. If data is to be included for a given fluid, either a refrigerant or a glycol, then its name must be included in the FluidProperties:Name objects.
+
+\subsubsection{Inputs}\label{inputs-020}
+
+\paragraph{Field: Fluid Name}\label{field-fluid-name}
+
+Each fluid name is a unique identifier that will be used in conjunction with the data statements described later in this section. The fluid name is either referred to by a component (in the case of a Refrigerant) or by another input line (in the case of a Glycol). This list is simply a list of user defined fluids present in the input data file.
+
+\paragraph{Field: Fluid Type}\label{field-fluid-type}
+
+Each fluid name must be identified by type - either \textbf{Refrigerant} or \textbf{Glycol}. This designation determines what type of data EnergyPlus expects for the fluid name. If the fluid name is defined as a Refrigerant, the user must supply valid data for pressure, enthalpy, specific heat, and density in the saturated region and enthalpy and density in the superheated region. If the fluid name is defined as a Glycol, the user must supply valid data for specific heat, conductivity, viscosity, and density at various concentrations (percentage of non-water liquid) and temperatures.
+
+An example of these statements in an input data file is:
+
+\begin{lstlisting}
+
+FluidProperties:Name,
+  R11,Refrigerant;
+
+
+  FluidProperties:Name,
+  R12,Refrigerant;
+
+
+  FluidProperties:Name,
+  R22,Refrigerant;
+
+
+  FluidProperties:Name,
+  NH3,Refrigerant;
+
+
+  FluidProperties:Name,
+  Steam,Refrigerant;
+
+
+  FluidProperties:Name,
+  SaltBrine, Glycol;
+
+
+  FluidProperties:Name,
+  NewGlycol, Glycol;
+\end{lstlisting}
+
+\subsection{FluidProperties:GlycolConcentration}\label{fluidpropertiesglycolconcentration}
+
+This input syntax is used to specify fluids that will be used with HVAC loops such as plant and condenser loops. It allows the user to define a mixture of water and some other substance and the particular concentration being used. The fluid name will be referred to by the loops or components and thus used to identify which value is valid for a particular fluid at a particular temperature. A series of three inputs is requires for each fluid concentration definition.
+
+\subsubsection{Inputs}\label{inputs-1-018}
+
+\paragraph{Field: Name}\label{field-name-019}
+
+Each glycol concentration name is a unique identifier that will be used to define a particular combination of water and some other substance (usually another fluid). Other input (such as loop definitions) will refer to this name, linking the other input to the proper fluid definition.
+
+\paragraph{Field: Glycol Type}\label{field-glycol-type}
+
+This field refers to the substance that is being mixed with water to create the glycol. The user may either select from the two default fluids (\textbf{EthyleneGlycol} or \textbf{PropyleneGlycol}) or specify \textbf{UserDefinedGlycolType} and use a name in the subsequent field for fluids that have been entered elsewhere in the input file. It should be noted that users must enter a complete definition of new glycols -including values for conductivity, specific heat, density, and viscosity at various concentrations and temperatures -in order for them to be used in conjunction with a user defined glycol type.
+
+\paragraph{Field: User Defined Glycol Name}\label{field-user-defined-glycol-name}
+
+This field is the name used elsewhere in a FluidProperties:Name object for defining your own glycol properties. This field is left blank unless you enter \textbf{UserDefinedGlycolType} in the previous field.
+
+\paragraph{Field: Glycol Concentration}\label{field-glycol-concentration}
+
+This field allows the user to specify the actual concentration of glycol being used for this particular fluid. A concentration of 0.0 refers to pure water. A concentration of 1.0 would denote 100\% of the fluid referenced in the Glycol Name input discussed above. Users should enter this value as a decimal fraction since EnergyPlus will limit the range of valid input values to between 0.0 and 1.0.
+
+An example of this statement in an input data file is:
+
+\begin{lstlisting}
+
+FluidProperties:GlycolConcentration,
+  EthGly25Percent, EthyleneGlycol, ,0.25;
+  FluidProperties:GlycolConcentration,
+  ProGly40Percent, PropyleneGlycol, ,0.40;
+  FluidProperties:GlycolConcentration,
+  HalfAndHalf, UserDefinedGlycolType, NewBrine, 0.5;
+\end{lstlisting}
+
+\subsection{FluidProperties:Temperatures}\label{fluidpropertiestemperatures}
+
+It is assumed that all fluid properties vary with temperature. A common set of temperatures is required for each set of fluid property data. Fluid property data supplied by the user must correspondingly be given at these temperatures. Since in most cases, refrigerant data can be specified at a common set of temperatures, a single set of FluidProperties:Temperatures can be referenced by a number of sets of property data. This provides a more compact input structure and avoids listing the temperatures multiple times. In the case of glycol data the same set of temperatures have to be used for each set of data at a given concentration. Units for the temperatures are degrees Celsius.
+
+\subsubsection{Inputs}\label{inputs-2-017}
+
+\paragraph{Field: Name}\label{field-name-1-017}
+
+This field is simply an unique identifier name that is used to cross reference the list of temperatures with a specific list of fluid property data. A single temperature list can be used for more than one thermal property or fluid. For example, the same temperature list can be used for the superheated enthalpy of a refrigerant and the specific heat of a glycol if appropriate.
+
+\paragraph{Field(s) 1-250: Temperature}\label{fields-1-250-temperature}
+
+These fields (up to 250) are the temperatures at which the data for the thermal properties are to be expected. Temperatures are assumed to be in ascending order in units of Celsius.
+
+An example of this statement in an input data file is:
+
+\begin{lstlisting}
+
+FluidProperties:Temperatures,
+  R11Temperatures,
+  -70,-65,-60,-55,-50,-45,-40,-35,-30,-25,-20,-15,-10,-5,0,2,4,6,8,10,12,
+  14,16,18,20,22,24,26,28,30,32,34,36,38,40,42,44,46,48,50,55,60,65,70,
+  75,80,85,90,95,100,105,110,115,120,125,130,135,140,145,150,155,160,
+  165,170,175,180,185,190,198;
+\end{lstlisting}
+
+\subsection{FluidProperties:Saturated}\label{fluidpropertiessaturated}
+
+Refrigerant property data for the saturated region is entered with the following syntax. For each set of property data a unique name, the type of property, phase and the corresponding list of temperatures have to be specified along with the property values.
+
+\subsubsection{Inputs}\label{inputs-3-015}
+
+\paragraph{Field: Name}\label{field-name-2-016}
+
+This name identifies the fluid for which data follows in the remaining syntax. This fluid name must also be given in the fluid names list (ref: FluidProperties:Names object) as a \textbf{Refrigerant}.
+
+\paragraph{Field: Fluid Property Type}\label{field-fluid-property-type}
+
+This field identifies the fluid property for which data is being entered with this statement. The options for the saturated region are \textbf{Enthalpy, Density, SpecificHeat}, and \textbf{Pressure}. The units for these properties are J/kg, kg/m\(^{3}\), J/kg-K and Pa, respectively.
+
+\paragraph{Field: Fluid Phase}\label{field-fluid-phase}
+
+In the saturated region, each property has two values: one for the saturated liquid state and one for the saturated gaseous state. Accordingly, the phase for which the saturated property data applies is specified as either \textbf{Fluid} or \textbf{FluidGas}. Data for each phase are required and are interpolated according to quality. However, in the case of saturated pressure data values for only one phase are required (i.e.~can be specified with phase specified as either Fluid or FluidGas, as this is irrelevant).
+
+\paragraph{Field: Temperatures Values Name}\label{field-temperatures-values-name}
+
+This name refers to the corresponding list of temperatures (ref: FluidProperties:Temperatures object). Each temperature in the temperature list corresponds to a data item found in the remaining fields of this syntax. The first temperature in the temperature list corresponds to the first fluid property value, the second temperature in the temperature list corresponds to the second fluid property value, etc.
+
+\paragraph{Field(s) 1-250: Property Value}\label{fields-1-250-property-value}
+
+These fields (up to 250) are the values of the thermal property specified in the fluid property type field for the phase specified in the fluid phase field. The temperature list specified in the temperature list name field links the data with the corresponding temperatures.
+
+An example of this statement in an input data file is:
+
+\begin{lstlisting}
+
+FluidProperties:Saturated,
+  R11,Enthalpy,Fluid,R11Temperatures, ! Enthalpy in J/kg
+  153580,154600,156310,158580,161300,164380,167740,171330,175100,179020,183060,
+  187190,191400,195680,200000,201740,203490,205240,207000,208770,210530,212310,
+  214080,215870,217650,219860,221230,223030,224830,226630,228860,230250,232060,
+  233860,235700,237520,239350,241180,243010,246350,249450,254080,258730,263480,
+  268110,272860,277000,282410,287240,292120,297030,302000,307090,312080,317210,
+  322400,327670,333020,338460,344010,349680,355500,361480,367690,374100,381060,
+  388850,397280,426300;
+\end{lstlisting}
+
+\subsection{FluidProperties:Superheated}\label{fluidpropertiessuperheated}
+
+The format of the data for the superheated region is similar to that of the saturated region but with the addition of the pressure for which each set of property values applies. A single temperature specification is required for each set of property data at a number of pressures.
+
+\subsubsection{Inputs}\label{inputs-4-014}
+
+\paragraph{Field: Fluid Name}\label{field-fluid-name-1}
+
+This name identifies the fluid for which data follows in the remaining syntax. This fluid name must show up in the fluid names list (ref: FluidProperties:Names object) as a \textbf{Refrigerant}.
+
+\paragraph{Field: Fluid Property Type}\label{field-fluid-property-type-1}
+
+This field identifies the fluid property for which data is being entered with this statement. The options for the superheated region are \textbf{Enthalpy} and \textbf{Density}. The units for these properties are J/kg and kg/m\(^{3}\), respectively.
+
+\paragraph{Field: Temperatures Values Name}\label{field-temperatures-values-name-1}
+
+This name refers to the corresponding list of temperatures (ref: FluidProperties:Temperatures object). Each temperature in the temperature list corresponds to a given property data item at each pressure. The first temperature in the temperature list corresponds to the first fluid property value, the second temperature in the temperature list corresponds to the second fluid property value, etc.
+
+\paragraph{Field: Pressure}\label{field-pressure}
+
+In the superheated region, each fluid property is indexed according to temperature and pressure. Thus, a pressure must be listed for each set of property values. The units for pressure are Pascals (Pa). Lists of properties are various pressures and temperatures form a two-dimensional table from which EnergyPlus interpolates to find the property value at a specified temperature and pressure.
+
+\paragraph{Field(s) 1-250: Property Value}\label{fields-1-250-property-value-1}
+
+These fields (up to 250) are the values of the thermal property specified in the fluid property type field for the phase specified in the fluid phase field. The temperature list specified in the temperature list name field links the data with the corresponding temperatures.
+
+An example of this statement in an input data file is:
+
+\begin{lstlisting}
+
+FluidProperties:Superheated,
+  R11,Density,SuperR11Temperatures, ! Density in kg/m^3
+  62000., !Pressure = 62000Pa
+  0,0,0,0,0,0,0,0.0139,0.0134,0.0129,0.0124,0.012,0.0116,0.0112,0.0109,0.0105,
+  0.0102,0.0099,0.0097,0.0094,0.0092,0.0089,0,0,0,0,0,0,0,0,0,0;
+\end{lstlisting}
+
+\subsection{Glycol Fluid Types}\label{glycol-fluid-types}
+
+A full data set for a glycol fluid type in EnergyPlus includes: a temperature list and lists of values for specific heat at a given concentration. Data have to be given for at least two different concentrations. The syntax lines for the property value lists are described below.
+
+\subsection{FluidProperties:Concentration}\label{fluidpropertiesconcentration}
+
+The format of the data for the glycols is similar to that of superheated refrigerants except that data at a number of concentrations is given, rather than pressures. The concentration is listed before the rest of the data and is normalized (i.e.~in the range 0.0 to 1.0, rather than a percentage). Note that glycol solutions are assumed to exist in liquid form only in EnergyPlus.
+
+\subsubsection{Inputs}\label{inputs-5-012}
+
+\paragraph{Field: Fluid Name}\label{field-fluid-name-2}
+
+This name identifies the fluid for which data follows in the remaining syntax. This fluid name must show up in the fluid names list (ref: FluidProperties:Names object) as a \textbf{Glycol}.. Note that users should not use Water, EthyleneGlycol, or PropyleneGlycol as names since these are default fluids.
+
+\paragraph{Field: Fluid Property Type}\label{field-fluid-property-type-2}
+
+This field identifies the fluid property for which data is being entered with this statement. The required data for glycols includes \textbf{SpecificHeat} with units of J/kg-K, \textbf{Density} with units of kg/m\(^{3}\), \textbf{Conductivity} with units of W/m-K, and \textbf{Viscosity} with units of N-s/m\(^{2}\).
+
+\paragraph{Field: Temperatures Values Name}\label{field-temperatures-values-name-2}
+
+This name refers to the corresponding list of temperatures (ref: FluidProperties:Temperatures object). Each temperature in the temperature list corresponds to a data item found in the remaining fields of this syntax. The first temperature in the temperature list corresponds to the first fluid property value, the second temperature in the temperature list corresponds to the second fluid property value, etc.
+
+\paragraph{Field: Concentration}\label{field-concentration}
+
+A concentration must be listed for the values of specific heat that follow. Lists of properties are various concentrations and temperatures form a two-dimensional table from which EnergyPlus interpolates to find the property value at a specified temperature and concentration. Concentrations are specified in a normalized form (i.e.~in the range 0.0 to 1.0, rather than a percentage)
+
+\paragraph{Field(s) 1-250: Property Value}\label{fields-1-250-property-value-2}
+
+These fields (up to 250) are the values of the thermal property specified in the fluid property type field for the phase specified in the fluid phase field. The temperature list specified in the temperature list name field links the data with the corresponding temperatures.
+
+An example of this statement in an input data file is:
+
+\begin{lstlisting}
+
+FluidProperties:Concentration,
+  NewGlycol,SpecificHeat ,GlycolTemperatures, ! Spec. heat in J/kg-K
+  0.8, ! Concentration
+  2572,2600,2627,2655,2683,2710,2738,2766,2793,2821,2849,2876,2904,2931,2959,
+  2987,3014,3042,3070,3097,3125,3153,3180,3208,3236,3263,3291,3319,3346,3374,
+  3402,3429,3457;
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-heat-recovery.tex b/doc/input-output-reference/src/overview/group-heat-recovery.tex
new file mode 100644
index 00000000000..29ef2b20b7d
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-heat-recovery.tex
@@ -0,0 +1,1030 @@
+\section{Group Heat Recovery}\label{group-heat-recovery}
+
+\subsection{HeatExchanger:AirToAir:FlatPlate}\label{heatexchangerairtoairflatplate}
+
+The air-to-air flat plate heat exchanger is an HVAC component typically used for exhaust or relief air heat recovery. The user can choose the flow arrangement type: counter flow, parallel flow, or cross flow with both streams unmixed. The input requires no geometric data. Performance is defined by specifying primary outlet air temperature at nominal (user specified) inlet conditions. In addition, the ratio (h\(^{.}\)A)\(_{p}\) / (h\(^{.}\)A)\(_{s}\) at nominal flow needs to be input, where h is the convective heat transfer coefficient, A is the surface area, p stands for primary side, s for secondary side.
+
+If the heat exchanger is operated in conjunction with an outdoor air economizer (economizer lockout set to \emph{Yes}), the nominal supply air flow rate should be set equal to the minimum outdoor air flow rate specified in the Controller:OutdoorAir. The heat exchanger detects that the economizer is operating by the fact that its inlet air flow rate is greater than its nominal supply air flow rate.
+
+\subsubsection{Inputs}\label{inputs-021}
+
+\paragraph{Field: Name}\label{field-name-020}
+
+A unique user-assigned name for a particular air-to-air flat plate heat exchanger unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-008}
+
+The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Flow Arrangement Type}\label{field-flow-arrangement-type}
+
+The user specified flow arrangement of the heat exchanger. The possible inputs are \emph{CounterFlow}, \emph{ParallelFlow}, or \emph{CrossFlowBothUnmixed}.
+
+\paragraph{Field: Economizer Lockout}\label{field-economizer-lockout}
+
+This input denotes whether the heat exchanger unit is locked out (bypassed) when the air-side economizer is operating. Both the economizer and high humidity control (Ref. Controller:OutdoorAir) activate the heat exchanger lockout as specified by this input. The input choices are \emph{Yes} (meaning locked out) or \emph{No}. The default input for this field is Yes.
+
+\paragraph{Field: Ratio of Supply to Secondary hA Values}\label{field-ratio-of-supply-to-secondary-ha-values}
+
+The ratio (h\(^{.}\)A)\(_{p}\) / (h\(^{.}\)A)\(_{s}\) at nominal flow. h is the surface convective heat transfer coefficient, A is the heat transfer area, and p and s stand for primary side and secondary side respectively. A typical value for this ratio is 1.0.
+
+\paragraph{Field: Nominal Supply Air Flow Rate}\label{field-nominal-supply-air-flow-rate}
+
+The nominal primary side air flow rate in cubic meters per second. If the unit is operated in conjunction with an outdoor air economizer this should be equal to the minimum outdoor air flow rate. This field is autosizable.
+
+\paragraph{Field: Nominal Supply Air Inlet Temperature}\label{field-nominal-supply-air-inlet-temperature}
+
+The nominal primary side air inlet temperature in Celsius.
+
+\paragraph{Field: Nominal Supply Air Outlet Temperature}\label{field-nominal-supply-air-outlet-temperature}
+
+The nominal primary side air outlet temperature in Celsius.
+
+\paragraph{Field: Nominal Secondary Air Flow Rate}\label{field-nominal-secondary-air-flow-rate}
+
+The nominal secondary side air flow rate in cubic meters per second. This field is autosizable. It is equal to the primary side air flow rate defined above, if autosized.
+
+\paragraph{Field: Nominal Secondary Air Inlet Temperature}\label{field-nominal-secondary-air-inlet-temperature}
+
+The nominal secondary side air inlet temperature in Celsius.
+
+\paragraph{Field: Nominal Electric Power}\label{field-nominal-electric-power}
+
+The electric consumption rate of the unit in watts. Electric power is considered constant whenever the unit operates. This input can be used to model electric power consumption by controls (transformers, relays, etc.) and/or a motor for a rotary heat exchanger. None of this electric power contributes thermal load to the supply or exhaust air streams. The default value for this field is 0.
+
+\paragraph{Field: Supply Air Inlet Node Name}\label{field-supply-air-inlet-node-name-000}
+
+The name of the HVAC system node from which the unit draws its primary inlet air.
+
+\paragraph{Field: Supply Air Outlet Node Name}\label{field-supply-air-outlet-node-name-000}
+
+The name of the HVAC system node to which the unit sends its primary outlet air.
+
+\paragraph{Field: Secondary Air Inlet Node Name}\label{field-secondary-air-inlet-node-name-001}
+
+The name of the HVAC system node from which the unit draws its secondary inlet air.
+
+\paragraph{Field: Secondary Air Outlet Node Name}\label{field-secondary-air-outlet-node-name-000}
+
+The name of the HVAC system node to which the unit sends its secondary outlet air.
+
+An IDF example:
+
+\begin{lstlisting}
+
+HeatExchanger:AirToAir:FlatPlate,
+  OA Heat Recovery 1,         !- Name
+  FanAndCoilAvailSched,       !- Availability Schedule Name
+  CounterFlow,                !- Flow Arrangement Type
+  Yes,                        !- Economizer Lockout
+  1.0,                        !- Ratio of Supply to Secondary hA Values
+  0.4333,                     !- Nominal Supply Air Flow Rate {m3/s}
+  5.0,                        !- Nominal Supply Air Inlet Temperature {C}
+  15.0,                       !- Nominal Supply Air Outlet Temperature {C}
+  0.4333,                     !- Nominal Secondary Air Flow Rate {m3/s}
+  20.0,                       !- Nominal Secondary Air Inlet Temperature {C}
+  0.0,                        !- Nominal Electric Power {W}
+  Desiccant Process Outlet Node,   !- Supply Air Inlet Node Name
+  Heat Recovery Outlet Node,   !- Supply Air Outlet Node Name
+  Relief Air Outlet Node,   !- Secondary Air Inlet Node Name
+  Heat Recovery Secondary Outlet Node;   !- Secondary Air Outlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-014}
+
+\begin{itemize}
+\item
+  HVAC,Average,Heat Exchanger Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Latent Gain Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Latent Gain Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Electric Power{[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Heat Exchanger Sensible Heating Rate {[}W{]}}\label{heat-exchanger-sensible-heating-rate-w}
+
+This output is the sensible heating rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, the supply air inlet and outlet conditions, and the specific heat of the inlet supply air. A positive value is reported if the supply air is heated by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Sensible Heating Energy {[}J{]}}\label{heat-exchanger-sensible-heating-energy-j}
+
+This output is the sensible heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Latent Gain Rate {[}W{]}}\label{heat-exchanger-latent-gain-rate-w}
+
+This output is the latent heating rate (humidification) of the supply air by the heat exchanger in Watts. This rate is determined by taking the difference between the Heat Exchanger Total Heating Rate and the Heat Exchanger Sensible Heating Rate. A positive value is reported if the supply air is humidified by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Latent Heating Energy {[}J{]}}\label{heat-exchanger-latent-heating-energy-j}
+
+This output is the latent heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Total Heating Rate {[}W{]}}\label{heat-exchanger-total-heating-rate-w}
+
+This output is the total heating rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, and the enthalpy of the supply air entering and leaving the unit. A positive value is reported if the enthalpy of the supply air is increased by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Total Heating Energy {[}J{]}}\label{heat-exchanger-total-heating-energy-j}
+
+This output is the total heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforHeating, GroupKey = System (ref. Output:Meter objects).
+
+\paragraph{Heat Exchanger Sensible Cooling Rate {[}W{]}}\label{heat-exchanger-sensible-cooling-rate-w}
+
+This output is the sensible cooling rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, the supply air inlet and outlet conditions, and the specific heat of the inlet supply air. A positive value is reported if the supply air is cooled by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Sensible Cooling Energy {[}J{]}}\label{heat-exchanger-sensible-cooling-energy-j}
+
+This output is the sensible cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Latent Cooling Rate {[}W{]}}\label{heat-exchanger-latent-cooling-rate-w}
+
+This output is the latent cooling rate (dehumidification) of the supply air by the heat exchanger in Watts. This rate is determined by taking the difference between the Heat Exchanger Total Cooling Rate and the Heat Exchanger Sensible Cooling Rate. A positive value is reported if the supply air is dehumidified by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Latent Cooling Energy {[}J{]}}\label{heat-exchanger-latent-cooling-energy-j}
+
+This output is the latent cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Total Cooling Rate {[}W{]}}\label{heat-exchanger-total-cooling-rate-w}
+
+This output is the total cooling rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, and the enthalpy of the supply air entering and leaving the unit. A positive value is reported if the enthalpy of the supply air is decreased by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Total Cooling Energy {[}J{]}}\label{heat-exchanger-total-cooling-energy-j}
+
+This output is the total cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported. This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforCooling, GroupKey = System (ref. Output:Meter objects).
+
+\paragraph{Heat Exchanger Electric Power {[}W{]}}\label{heat-exchanger-electric-power-w}
+
+This output is the electric consumption rate of the unit in Watts. This rate is applicable whenever the unit operates (i.e., whenever the unit is scheduled to be available and supply and exhaust air flows exist).
+
+\paragraph{Heat Exchanger Electric Energy {[}J{]}}\label{heat-exchanger-electric-energy-j}
+
+This output is the electric consumption of the unit in Joules for the timestep being reported. This ouput is also added to a meter with ResourceType = Electricity, EndUseKey = HeatRecovery, GroupKey = System (ref. Output:Meter objects).
+
+\subsection{HeatExchanger:AirToAir:SensibleAndLatent}\label{heatexchangerairtoairsensibleandlatent}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image423.png}
+\caption{}
+\end{figure}
+
+The sensible and latent air-to-air heat exchanger is an HVAC component typically used for exhaust or relief air heat recovery (Figure 150). Heat exchanger performance can be specified to transfer sensible energy, latent energy or both between the supply and exhaust air streams. The input requires no geometric data. Performance is defined by specifying sensible and/or latent effectiveness at 75\% and 100\% of the nominal (rated) supply air flow rate at two operating conditions as shown in Table~\ref{table:operating-conditions-for-defining-heat}.
+
+Figure 150. Schematic of the Sensible and Latent Air-to-Air Heat Exchanger
+
+% table 30
+\begin{longtable}[c]{@{}lll@{}}
+\caption{Operating Conditions for Defining Heat Exchanger Performance \label{table:operating-conditions-for-defining-heat}} \tabularnewline
+\toprule 
+Parameter & Conditions \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Operating Conditions for Defining Heat Exchanger Performance} \tabularnewline
+\toprule 
+Parameter & Conditions \tabularnewline
+\midrule
+\endhead
+
+Heating & Cooling \tabularnewline
+Entering supply air temperature: &  &  \tabularnewline
+Dry-bulb: & 1.7°C (35°F) & 35°C (95°F) \tabularnewline
+Wet-bulb: & 0.6°C (33°F) & 26°C (78°F) \tabularnewline
+Entering supply air temperature: &  &  \tabularnewline
+Dry-bulb: & 21°C (70°F) & 24°C (75°F) \tabularnewline
+Wet-bulb: & 14°C (58°F) & 17C (63F) \tabularnewline
+\bottomrule
+\end{longtable}
+
+Note: Conditions consistent with the Air-Conditioning and Refrigeration Institute s (ARI) Standard 1060-2001.
+
+This object models the basic operation of an air-to-air heat exchanger. Heat exchange between the supply and exhaust air streams occurs whenever the unit is scheduled to be available (Availability schedule) and supply/exhaust air flow is present. This heat exchanger object can be used in conjunction with a conventional air-side economizer (i.e., specify ModulateFlow in the Controller:OutdoorAir object), whereby heat exchange is suspended whenever the air-side economizer (or high humidity control) is active (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped). This object is also able to suspend heat exchange for the purpose of providing free cooling operation in the absence of a conventional air-side economizer (i.e., specify MinimumFlowWithBypass in the Controller:OutdoorAir object).
+
+During winter weather, humid exhaust air entering the heat exchanger can form frost on the cold heat exchanger surfaces, which can reduce air flow and the amount of energy recovery. Several methods are used to control or eliminate frost formation, and the following types can be modeled for this heat exchanger object: supply air preheat, minimum exhaust air temperature, exhaust air recirculation and exhaust only. For preheat frost control, a separate heating coil object must be placed in the supply inlet air stream to keep the air temperature above the frost threshold temperature. The other frost control types are modeled within this object itself (i.e., do not require a separate object to be defined) based on alpha and numeric inputs to this heat exchanger object.
+
+Air-to-air heat exchangers are sometimes controlled to maintain a fixed supply air outlet temperature to avoid overheating when the heat exchanger is heating the supply (primary) air. To model this control in EnergyPlus, a set point manager object is used to establish a temperature set point at the supply air outlet node of the heat exchanger. Wheel speed modulation or plate supply air bypass is used to control the supply air exiting conditions to this set point. The set point for supply air temperature control should be set at the minimum economizer temperature set point if an air-side economizer is also being used by the air system. If frost control and supply air outlet temperature control are used, frost control takes precedence over supply air temperature control (e.g., frost control defrost time fraction is determined as if wheel speed modulation or plate supply air bypass is not used).
+
+To model a sensible and latent air-to-air heat exchanger located in an air loop, the input data file should include the following objects:
+
+\begin{itemize}
+\item
+  AirLoopHVAC:OutdoorAirSystem
+\item
+  Controller:OutdoorAir
+\item
+  OutdoorAir:Mixer
+\item
+  HeatExchanger:AirToAir:SensibleAndLatent
+\item
+  Coil:Heating:Water, Coil:Heating:Electric or Coil:Heating:Gas (if preheat frost control is to be modeled)
+\item
+  SetpointManager:Scheduled (if supply air outlet temperature control is used)
+\end{itemize}
+
+The sensible and latent air-to-air heat exchanger can also be used in a number of other applications, including conditioning outdoor ventilation air and supplying it directly to a zone without an air loop. See object ZoneHVAC:EnergyRecoveryVentilator for further details on this specific application.
+
+A description of each input field for this object is provided below.
+
+\subsubsection{Inputs}\label{inputs-1-019}
+
+\paragraph{Field: Name}\label{field-name-1-018}
+
+A unique user-assigned name for a particular sensible/latent air-to-air heat exchanger. Any reference to this heat exchanger by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-006}
+
+The name of the schedule (ref: Schedule) that denotes whether the unit can operate during a given time period. A schedule value of less than or equal to 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Nominal Supply Air Flow Rate}\label{field-nominal-supply-air-flow-rate-1}
+
+The nominal primary side (supply) air flow rate in cubic meters per second. The actual supply and exhaust air flow rates must be between 50\% and 130\% of this value or a warning will be issued.
+
+\paragraph{Field: Sensible Effectiveness at 100\% Heating Air Flow}\label{field-sensible-effectiveness-at-100-heating-air-flow}
+
+The sensible heat exchange effectiveness at the \emph{heating} condition defined in Table~\ref{table:operating-conditions-for-defining-heat} above with both the supply and exhaust air volume flow rates equal to 100\% of the nominal supply air flow rate specified in the previous input field. The default value for this field is 0.
+
+\paragraph{Field: Latent Effectiveness at 100\% Heating Air Flow}\label{field-latent-effectiveness-at-100-heating-air-flow}
+
+The latent heat exchange effectiveness at the \emph{heating} condition defined in Table~\ref{table:operating-conditions-for-defining-heat} with both the supply and exhaust air volume flow rates equal to 100\% of the nominal supply air flow rate. Specify this value as 0.0 if the heat exchanger does not transfer latent energy. The default value for this field is 0.
+
+\paragraph{Field: Sensible Effectiveness at 75\% Heating Air Flow}\label{field-sensible-effectiveness-at-75-heating-air-flow}
+
+The sensible heat exchange effectiveness at the \emph{heating} condition defined in Table~\ref{table:operating-conditions-for-defining-heat} with both the supply and exhaust air volume flow rates equal to 75\% of the nominal supply air flow rate. The default value for this field is 0.
+
+\paragraph{Field: Latent Effectiveness at 75\% Heating Air Flow}\label{field-latent-effectiveness-at-75-heating-air-flow}
+
+The latent heat exchange effectiveness at the \emph{heating} condition defined in Table~\ref{table:operating-conditions-for-defining-heat} with both the supply and exhaust air volume flow rates equal to 75\% of the nominal supply air flow rate. Specify this value as 0.0 if the heat exchanger does not transfer latent energy. The default value for this field is 0.
+
+\paragraph{Field: Sensible Effectiveness at 100\% Cooling Air Flow}\label{field-sensible-effectiveness-at-100-cooling-air-flow}
+
+The sensible heat exchange effectiveness at the \emph{cooling} condition defined in Table~\ref{table:operating-conditions-for-defining-heat} with both the supply and exhaust air volume flow rates equal to 100\% of the nominal supply air flow rate. The default value for this field is 0.
+
+\paragraph{Field: Latent Effectiveness at 100\% Cooling Air Flow}\label{field-latent-effectiveness-at-100-cooling-air-flow}
+
+The latent heat exchange effectiveness at the \emph{cooling} condition defined in Table~\ref{table:operating-conditions-for-defining-heat} with both the supply and exhaust air volume flow rates equal to 100\% of the nominal supply air flow rate. Specify this value as 0.0 if the heat exchanger does not transfer latent energy. The default value for this field is 0.
+
+\paragraph{Field: Sensible Effectiveness at 75\% Cooling Air Flow}\label{field-sensible-effectiveness-at-75-cooling-air-flow}
+
+The sensible heat exchange effectiveness at the \emph{cooling} condition defined in Table~\ref{table:operating-conditions-for-defining-heat} with both the supply and exhaust air volume flow rates equal to 75\% of the nominal supply air flow rate. The default value for this field is 0.
+
+\paragraph{Field: Latent Effectiveness at 75\% Cooling Air Flow}\label{field-latent-effectiveness-at-75-cooling-air-flow}
+
+The latent heat exchange effectiveness at the \emph{cooling} condition defined in Table~\ref{table:operating-conditions-for-defining-heat} with both the supply and exhaust air volume flow rates equal to 75\% of the nominal supply air flow rate. Specify this value as 0.0 if the heat exchanger does not transfer latent energy. The default value for this field is 0.
+
+\paragraph{Field: Supply Air Inlet Node Name}\label{field-supply-air-inlet-node-name-1-000}
+
+The name of the HVAC system node from which the unit draws its supply (primary) inlet air.
+
+\paragraph{Field: Supply Air Outlet Node Name}\label{field-supply-air-outlet-node-name-1}
+
+The name of the HVAC system node to which the unit sends its supply (primary) outlet air.
+
+\paragraph{Field: Exhaust Air Inlet Node Name}\label{field-exhaust-air-inlet-node-name}
+
+The name of the HVAC system node from which the unit draws its exhaust (secondary) inlet air.
+
+\paragraph{Field: Exhaust Air Outlet Node Name}\label{field-exhaust-air-outlet-node-name}
+
+The name of the HVAC system node to which the unit sends its exhaust (secondary) outlet air.
+
+\paragraph{Field: Nominal Electric Power}\label{field-nominal-electric-power-1}
+
+The electric consumption rate of the unit in watts. Electric power is considered constant whenever the unit operates. This numeric input can be used to model electric power consumption by controls (transformers, relays, etc.) and/or a motor for a rotary heat exchanger. None of this electric power contributes thermal load to the supply or exhaust air streams. The default value for this field is 0.
+
+\paragraph{Field: Supply Air Outlet Temperature Control}\label{field-supply-air-outlet-temperature-control}
+
+This alpha field determines if the heat exchanger's supply air outlet is controlled to a temperature set point when the heat exchanger is actively conditioning the supply (primary) air. The choices for this input field are Yes or No, with the default being No. When supply air outlet temperature control is used, the wheel rotational speed modulates or supply air is bypassed around the plate heat exchanger to maintain the desired setpoint temperature. A setpoint manager object is required to establish the desired set point at the supply air outlet node (reference: SetpointManager:Scheduled). When an air-side economizer is also being modeled for this air system, the heat exchanger is deactivated during economizer operation. Additionally, the set point for the supply air outlet temperature control should be equal to the economizer outdoor air temperature lower limit (reference: Controller:OutdoorAir, field Economizer Minimum Limit Dry-Bulb Temperature), however, any temperature set point may be used.
+
+\paragraph{Field: Heat Exchanger Type}\label{field-heat-exchanger-type}
+
+This alpha field denotes the type of heat exchanger being modeled: Plate (e.g., fixed plate) or Rotary (e.g., rotating cylinder or wheel). The default choice for this field is Plate . The heat exchanger type affects the modeling of frost control options and supply air outlet temperature control. For rotary heat exchangers, rotational speed is varied to control frost formation or the supply air outlet temperature. For plate exchangers, air bypass around the heat exchanger is used to obtain the desired effect.
+
+\paragraph{Field: Frost Control Type}\label{field-frost-control-type}
+
+This alpha field has four choices: None, ExhaustAirRecirculation, ExhaustOnly and MinimumExhaustTemperature. If this field is left blank, the default frost control type is None . For modeling preheat frost control, specify None for this input field and insert a separate heating coil object in the supply inlet air stream to keep the air temperature above the desired frost threshold temperature.
+
+\emph{ExhaustAirRecirculation}: dampers are used to direct exhaust air back into the zone through the supply side of the heat exchanger when the supply (outdoor) air inlet temperature falls below a threshold temperature (defined in the next input field). The fraction of time that exhaust air is circulated through the supply side of the heat exchanger is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time fraction (see \emph{Field: Rate of Defrost Time Fraction Increase}). When exhaust air is being recirculated, no supply (outdoor ventilation) air is being provided through the heat exchanger unit (which may or may not be acceptable regarding ventilation for occupants).
+
+\emph{ExhaustOnly (supply air bypass)}: this control cycles off the supply air flow through the heat exchanger for a certain period of time while the exhaust air continues to flow through the exhaust side of the heat exchanger. The fraction of time that the supply flow through the heat exchanger is cycled off is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time fraction (see \emph{Field: Rate of Defrost Time Fraction Increase}). When implemented in real applications, provisions are usually made to avoid building depressurization when this frost control is operating (automatic or pressure-operated dampers, or a bypass air damper around the supply side of the heat exchanger). For this frost control type, it is assumed that the supply air is bypassed around the heat exchanger during frost control operation (i.e., the total supply flow is not reduced during defrost, but merely bypassed around the heat exchanger).
+
+\emph{MinimumExhaustTemperature}: the temperature of the exhaust air leaving the heat exchanger is monitored and the heat exchanger effectiveness is decreased (by slowing heat exchanger rotation or bypassing supply air around the plate exchanger) to keep the exhaust air from falling below the threshold temperature.
+
+\paragraph{Field: Threshold Temperature}\label{field-threshold-temperature}
+
+This numeric field defines the dry-bulb temperature of air which is used to initiate frost control. The default value is 1.7 °C. For ExhaustAirRecirculation and ExhaustOnly frost control, the threshold temperature defines the supply (outdoor) air inlet temperature below which frost control is active. For MinimumExhaustTemperature frost control, heat exchanger effectiveness is controlled to keep the exhaust air outlet temperature from falling below this threshold temperature value.
+
+The appropriate threshold temperature varies with exhaust (inlet) air temperature and humidity, frost control type, heat exchanger type, and whether the heat exchanger transfers sensible energy alone or both sensible and latent energy (enthalpy). Typical threshold temperatures are provided in Table~\ref{table:typical-threshold-temperatures} below. However, it is recommended that the user consult manufacturer s information for the specific air-to-air heat exchanger being modeled.
+
+% table 31
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Typical threshold temperatures \label{table:typical-threshold-temperatures}} \tabularnewline
+\toprule 
+Frost Control Type & Heat Exchanger Type & Energy Exchange & Threshold Temperature \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Typical threshold temperatures} \tabularnewline
+\toprule 
+Frost Control Type & Heat Exchanger Type & Energy Exchange & Threshold Temperature \tabularnewline
+\midrule
+\endhead
+
+Exhaust Air Recirculation & Plate & Sensible-only & -1.1°C (30°F) \tabularnewline
+Sensible + latent & -12.2°C (10°F) \tabularnewline
+Rotary & Sensible-only & -12.2°C (10°F) \tabularnewline
+Sensible + latent & -12.2°C (10°F) \tabularnewline
+Exhaust Only & Plate & Sensible-only & -23.3°C (-10°F) \tabularnewline
+Sensible + latent & -1.1°C (30°F) \tabularnewline
+Rotary & Sensible-only & -12.2°C (10°F) \tabularnewline
+Sensible + latent & -12.2°C (10°F) \tabularnewline
+Minimum Exhaust Temperature & Plate & Sensible-only & -23.3°C (-10°F) \tabularnewline
+Sensible + latent & 1.7°C (35°F) \tabularnewline
+Rotary & Sensible-only & 1.7°C (35°F) \tabularnewline
+Sensible + latent & 1.7°C (35°F) \tabularnewline
+Preheat ** & Plate & Sensible-only & 1.7°C (35°F) \tabularnewline
+Sensible + latent & -1.1°C (30°F) \tabularnewline
+Rotary & Sensible-only & -12.2°C (10°F) \tabularnewline
+Sensible + latent & -23.3°C (-10°F) \tabularnewline
+\bottomrule
+\end{longtable}
+
+Source: Indoor Humidity Assessment Tool, U.S. Environmental Protection Agency,\url{http://www.epa.gov/iaq/schooldesign/saves.html}
+
+** To model preheat frost control, specify frost control type as None and place a heating coil in the supply inlet air stream controlled to the keep the air temperature above the frost threshold temperature.
+
+\paragraph{Field: Initial Defrost Time Fraction}\label{field-initial-defrost-time-fraction}
+
+This numeric field defines the fraction of the simulation timestep when frost control will be invoked when the threshold temperature is reached. This field is only used for the ExhaustAirRecirculation and ExhaustOnly frost control types. The value for this field must be ≥ 0 and ≤ 1. The default time fraction is 0.083 (e.g., 5 min / 60 min) which is typical for ExhaustAirRecirculation frost control. Higher initial defrost time fractions (e.g., 0.167 = 10 min / 60 min) are typically required for ExhaustOnly frost control. For best results, the user should obtain this information from the manufacturer.
+
+\paragraph{Field: Rate of Defrost Time Fraction Increase}\label{field-rate-of-defrost-time-fraction-increase}
+
+This numeric field defines the rate of increase in the defrost time fraction as the supply (outdoor) air inlet temperature falls below the threshold temperature. This field is only used for the ExhaustAirRecirculation and ExhaustOnly frost control types. The value for this field must be ≥ 0. The default value is 0.012 (e.g., 0.72 min / 60 min per degree C temperature difference) which is typical for ExhaustAirRecirculation frost control. Higher values (e.g., 0.024 = 1.44 min / 60 min per degree C temperature difference) are typically required for ExhaustOnly frost control. For best results, the user should obtain this information from the manufacturer.
+
+This value is used to determine the total defrost time fraction as follows:
+
+Total defrost time fraction = Initial Defrost Time Fraction +
+
+\begin{lstlisting}
+       Rate of Defrost Time Fraction Increase \* (T$_{threshold}$     T$_{supply\\ air\\ inlet}$)
+\end{lstlisting}
+
+The model does not allow the total defrost time fraction to exceed 1.0 or be less than 0.
+
+\paragraph{Field: Economizer Lockout}\label{field-economizer-lockout-1}
+
+This input denotes whether the heat exchanger unit is locked out (bypassed for plate type heat exchangers or the rotation is suspended for rotary type heat exchangers) when the air-side economizer is operating. Both the economizer and high humidity control (Ref. Controller:OutdoorAir) activate the heat exchanger lockout as specified by this input. The input choices are \emph{Yes} (meaning locked out) or \emph{No}. The default input for this field is Yes.
+
+Following is an example input for this heat exchanger object:
+
+\begin{lstlisting}
+
+HeatExchanger:AirToAir:SensibleAndLatent,
+  OA Heat Recovery 1,         !- Name
+  FanAndCoilAvailSched,       !- Availability Schedule Name
+  0.4333,                     !- Nominal Supply Air Flow Rate {m3/s}
+  .76,                        !- Sensible Effectiveness at 100% Heating Air Flow {dimensionless}
+  .68,                        !- Latent Effectiveness at 100% Heating Air Flow {dimensionless}
+  .81,                        !- Sensible Effectiveness at 75% Heating Air Flow {dimensionless}
+  .73,                        !- Latent Effectiveness at 75% Heating Air Flow {dimensionless}
+  .76,                        !- Sensible Effectiveness at 100% Cooling Air Flow {dimensionless}
+  .68,                        !- Latent Effectiveness at 100% Cooling Air Flow {dimensionless}
+  .81,                        !- Sensible Effectiveness at 75% Cooling Air Flow {dimensionless}
+  .73,                        !- Latent Effectiveness at 75% Cooling Air Flow {dimensionless}
+  Outside Air Inlet Node Preheated,   !- Supply Air Inlet Node Name
+  Heat Recovery Outlet Node,  !- Supply Air Outlet Node Name
+  Relief Air Outlet Node,     !- Exhaust Air Inlet Node Name
+  Heat Recovery Secondary Outlet Node,   !- Exhaust Air Outlet Node Name
+  200.0,                      !- Nominal Electric Power {W}
+  No,                         !- Supply Air Outlet Temperature Control
+  Plate,                      !- Heat Exchanger Type
+  None;                       !- Frost Control Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-012}
+
+\begin{itemize}
+\item
+  HVAC,Average,Heat Exchanger Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Latent Gain Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Latent Gain Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Electric Power{[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Sensible Effectiveness{[]}
+\item
+  HVAC,Average,Heat Exchanger Latent Effectiveness{[]}
+\item
+  HVAC,Average,Heat Exchanger Supply Air Bypass Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Heat Exchanger Exhaust Air Bypass Mass Flow Rate {[}kg/s{]} HVAC,Average,Heat Exchanger Defrost Time Fraction{[]}
+\end{itemize}
+
+\paragraph{Heat Exchanger Sensible Heating Rate {[}W{]}}\label{heat-exchanger-sensible-heating-rate-w-1}
+
+This output is the sensible heating rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, the supply air inlet and outlet conditions, and the specific heat of the inlet supply air. A positive value is reported if the supply air is heated by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Sensible Heating Energy {[}J{]}}\label{heat-exchanger-sensible-heating-energy-j-1}
+
+This output is the sensible heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Latent Gain Rate {[}W{]}}\label{heat-exchanger-latent-gain-rate-w-1}
+
+This output is the latent heating rate (humidification) of the supply air by the heat exchanger in Watts. This rate is determined by taking the difference between the Heat Exchanger Total Heating Rate and the Heat Exchanger Sensible Heating Rate. A positive value is reported if the supply air is humidified by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Latent Gain Energy {[}J{]}}\label{heat-exchanger-latent-gain-energy-j}
+
+This output is the latent heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Total Heating Rate {[}W{]}}\label{heat-exchanger-total-heating-rate-w-1}
+
+This output is the total heating rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, and the enthalpy of the supply air entering and leaving the unit. A positive value is reported if the enthalpy of the supply air is increased by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Total Heating Energy {[}J{]}}\label{heat-exchanger-total-heating-energy-j-1}
+
+This output is the total heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforHeating, GroupKey = System (ref. Output:Meter objects).
+
+\paragraph{Heat Exchanger Sensible Cooling Rate {[}W{]}}\label{heat-exchanger-sensible-cooling-rate-w-1}
+
+This output is the sensible cooling rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, the supply air inlet and outlet conditions, and the specific heat of the inlet supply air. A positive value is reported if the supply air is cooled by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Sensible Cooling Energy {[}J{]}}\label{heat-exchanger-sensible-cooling-energy-j-1}
+
+This output is the sensible cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Latent Cooling Rate {[}W{]}}\label{heat-exchanger-latent-cooling-rate-w-1}
+
+This output is the latent cooling rate (dehumidification) of the supply air by the heat exchanger in Watts. This rate is determined by taking the difference between the Heat Exchanger Total Cooling Rate and the Heat Exchanger Sensible Cooling Rate. A positive value is reported if the supply air is dehumidified by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Latent Cooling Energy {[}J{]}}\label{heat-exchanger-latent-cooling-energy-j-1}
+
+This output is the latent cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Total Cooling Rate {[}W{]}}\label{heat-exchanger-total-cooling-rate-w-1}
+
+This output is the total cooling rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, and the enthalpy of the supply air entering and leaving the unit. A positive value is reported if the enthalpy of the supply air is decreased by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Total Cooling Energy {[}J{]}}\label{heat-exchanger-total-cooling-energy-j-1}
+
+This output is the total cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported. This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforCooling, GroupKey = System (ref. Output:Meter objects).
+
+\paragraph{Heat Exchanger Electric Power {[}W{]}}\label{heat-exchanger-electric-power-w-1}
+
+This output is the electric consumption rate of the unit in Watts. This rate is applicable whenever the unit operates (i.e., whenever the unit is scheduled to be available and supply and exhaust air flows exist).
+
+\paragraph{Heat Exchanger Electric Energy {[}J{]}}\label{heat-exchanger-electric-energy-j-1}
+
+This output is the electric consumption of the unit in Joules for the timestep being reported. This ouput is also added to a meter with ResourceType = Electricity, EndUseKey = HeatRecovery, GroupKey = System (ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Heat Exchanger Sensible Effectiveness {[]}}{Heat Exchanger Sensible Effectiveness }}\label{heat-exchanger-sensible-effectiveness}
+
+This output is the average sensible effectiveness of the heat exchanger (excluding bypass air, if any) over the timestep being reported.
+
+\paragraph{\texorpdfstring{Heat Exchanger Latent Effectiveness {[]}}{Heat Exchanger Latent Effectiveness }}\label{heat-exchanger-latent-effectiveness}
+
+This output is the average latent effectiveness of the heat exchanger (excluding bypass air, if any) over the timestep being reported.
+
+\paragraph{Heat Exchanger Supply Air Bypass Mass Flow Rate {[}kg/s{]}}\label{heat-exchanger-supply-air-bypass-mass-flow-rate-kgs}
+
+This output is the average mass flow rate in kg/second of the supply (primary) air stream that is bypassing the heat exchanger over the timestep being reported. This flow rate is equal to the total supply mass flow rate through the heat exchanger \textbf{unit} minus the amount passing through the supply side of the heat exchanger \textbf{core}.
+
+\paragraph{Heat Exchanger Exhaust Air Bypass Mass Flow Rate {[}kg/s{]}}\label{heat-exchanger-exhaust-air-bypass-mass-flow-rate-kgs}
+
+This output is the average mass flow rate in kg/second of the exhaust (secondary) air stream that is bypassing the heat exchanger over the timestep being reported. This flow rate is equal to the total exhaust mass flow rate through the heat exchanger \textbf{unit} minus the amount passing through the exhaust side of the heat exchanger \textbf{core}.
+
+\paragraph{\texorpdfstring{Heat Exchanger Defrost Time Fraction {[]}}{Heat Exchanger Defrost Time Fraction }}\label{heat-exchanger-defrost-time-fraction}
+
+This output is the average fraction of the reporting timestep when frost control is being implemented.
+
+\subsection{HeatExchanger:Desiccant:BalancedFlow}\label{heatexchangerdesiccantbalancedflow}
+
+This desiccant heat exchanger object is an HVAC component used to model both temperature (sensible) and moisture (latent) heat exchange between two air streams (Figure~\ref{fig:schematic-of-the-balanced-flow-desiccant-heat}). The model assumes balanced air flow through the regeneration and process sides of the heat exchanger (i.e., regeneration and process air volume flow rates and face velocities are the same). Heat exchanger performance is specified through a performance data type object (e.g., HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1).
+
+\begin{figure}[hbtp] % fig 151
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image424.png}
+\caption{Schematic of the Balanced Flow Desiccant Heat Exchanger \protect \label{fig:schematic-of-the-balanced-flow-desiccant-heat}}
+\end{figure}
+
+Currently, this desiccant heat exchanger model can be referenced by two compound objects: CoilSystem:Cooling:DX:HeatExchangerAssisted and Dehumidifier:Desiccant:System, both of which are used to provide enhanced dehumidification over conventional systems. If this heat exchanger is referenced by a compound object, the compound object will control heat exchanger operation (i.e., tell the heat exchanger if heat exchange is needed or not for each simulation timestep).
+
+This desiccant heat exchanger object may also be specified directly in an AirLoopHVAC (air loop BranchList) or in an AirLoopHVAC:OutdoorAirSystem (AirLoopHVAC:OutdoorAirSystem:EquipmentList) without being referenced by a compound object. If specified directly in an AirLoopHVAC or AirLoopHVAC:OutdoorAirSystem, then the heat exchanger can be controlled to provide heat exchange based on a maximum and/or minimum humidity set point placed on the process air outlet node (ref. Setpoint Managers). If no humidity set points are provided on this node, then heat exchange will be provided whenever the heat exchanger is available to operate (via its availability schedule) and there is a temperature and/or humidity ratio difference between the two air streams.
+
+Inputs to this model include an availability schedule name, inlet and outlet air node names, and the type and name of the heat exchanger performance data object. A description of each input field for this object is provided below.
+
+\subsubsection{Inputs}\label{inputs-2-018}
+
+\paragraph{Field: Name}\label{field-name-2-017}
+
+A unique, user-assigned name for a particular balanced flow desiccant heat exchanger. Any reference to this heat exchanger by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-2-003}
+
+The name of the schedule (ref: Schedule) that denotes whether the heat exchanger can operate during a given time period. A schedule value of less than or equal to 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Regeneration Air Inlet Node Name}\label{field-regeneration-air-inlet-node-name-000}
+
+The name of the HVAC system node from which the unit draws its regeneration inlet air.
+
+\paragraph{Field: Regeneration Air Outlet Node Name}\label{field-regeneration-air-outlet-node-name}
+
+The name of the HVAC system node to which the unit sends its regeneration outlet air.
+
+\paragraph{Field: Process Air Inlet Node Name}\label{field-process-air-inlet-node-name-000}
+
+The name of the HVAC system node from which the unit draws its process inlet air.
+
+\paragraph{Field: Process Air Outlet Node Name}\label{field-process-air-outlet-node-name-000}
+
+The name of the HVAC system node to which the unit sends its process outlet air.
+
+\paragraph{Field: Heat Exchanger Performance Object Type}\label{field-heat-exchanger-performance-object-type}
+
+This alpha field contains the type of model used to simulate the desiccant heat exchanger s thermal performance and electrical energy use. Currently, the only valid choice is HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1.
+
+\paragraph{Field: Heat Exchanger Performance Name}\label{field-heat-exchanger-performance-name}
+
+This alpha field contains the identifying name of the specific heat exchanger performance type object (e.g., HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1) that defines the performance for this heat exchanger. A single heat exchanger performance type object may be used to define performance for many HeatExchanger:Desiccant:BalancedFlow objects (i.e., the same name may be used in this input field for more than one balanced flow desiccant heat exchanger).
+
+\paragraph{Field: Economizer Lockout}\label{field-economizer-lockout-2}
+
+This input denotes whether the heat exchanger unit is locked out (heat exchanger rotation is suspended) when the air-side economizer is operating. Both the economizer and high humidity control (Ref. Controller:OutdoorAir) activate the heat exchanger lockout as specified by this input. The input choices are \emph{Yes} (meaning locked out) or \emph{No}. Economizer lockout is typically \emph{not} used for this type of heat exchanger. For this reason, the default input for this field is No.
+
+Following is an example input for this heat exchanger object:
+
+\begin{lstlisting}
+
+HeatExchanger:Desiccant:BalancedFlow,
+  Desiccant Heat Exchanger 1,                 !- Name
+  OfficeHeatCoolAvail,                               !- Availability Schedule Name
+  DXSystem 1 Mixed Air Node,                   !- Regeneration Air Inlet Node Name
+  DX Cooling Coil Air Inlet Node,         !- Regeneration Air Outlet Node Name
+  DX Cooling Coil Air Outlet Node,       !- Process Air Inlet Node Name
+  DXSystem 1 Fan Air Inlet Node,           !- Process Air Outlet Node Name
+  HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1, !- Heat Exchanger Performance Object Type
+  HXDesPerf1;                                                 !- Heat Exchanger Performance Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-010}
+
+\begin{itemize}
+\item
+  HVAC,Average,Heat Exchanger Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Latent Gain Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Latent Gain Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Heat Exchanger Electric Power{[}W{]}
+\item
+  HVAC,Sum,Heat Exchanger Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Heat Exchanger Sensible Heating Rate {[}W{]}}\label{heat-exchanger-sensible-heating-rate-w-2}
+
+This output is the sensible heating rate of the process air by the heat exchanger in Watts. This rate is determined using the process air mass flow rate through the heat exchanger unit, the process air inlet and outlet temperatures, and the specific heat of the inlet process air. A positive value is reported if the process air is heated by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Sensible Heating Energy {[}J{]}}\label{heat-exchanger-sensible-heating-energy-j-2}
+
+This output is the sensible heating energy added to the process air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Latent Gain Rate {[}W{]}}\label{heat-exchanger-latent-gain-rate-w-2}
+
+This output is the latent heating rate (humidification) of the process air by the heat exchanger in Watts. This rate is determined by taking the difference between the heat exchanger s total heat recovery rate and the sensible heat recovery rate. A positive value is reported if the process air is humidified by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Latent Gain Energy {[}J{]}}\label{heat-exchanger-latent-gain-energy-j-1}
+
+This output is the latent heating energy added to the process air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Total Heating Rate {[}W{]}}\label{heat-exchanger-total-heating-rate-w-2}
+
+This output is the total heating rate of the process air by the heat exchanger in Watts. This rate is determined using the process air mass flow rate through the heat exchanger unit and the enthalpy of the air entering and leaving the process side of the unit. A positive value is reported if the enthalpy of the process air is increased by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Total Heating Energy {[}J{]}}\label{heat-exchanger-total-heating-energy-j-2}
+
+This output is the total heating energy added to the process air by the heat exchanger in Joules over the timestep being reported.This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforHeating, GroupKey = System (ref. Output:Meter objects).
+
+\paragraph{Heat Exchanger Sensible Cooling Rate {[}W{]}}\label{heat-exchanger-sensible-cooling-rate-w-2}
+
+This output is the sensible cooling rate of the process air by the heat exchanger in Watts. This rate is determined using the process air mass flow rate through the heat exchanger unit, the process air inlet and outlet temperatures, and the specific heat of the inlet process air. A positive value is reported if the process air is cooled by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Sensible Cooling Energy {[}J{]}}\label{heat-exchanger-sensible-cooling-energy-j-2}
+
+This output is the sensible cooling energy added to the process air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Latent Cooling Rate {[}W{]}}\label{heat-exchanger-latent-cooling-rate-w-2}
+
+This output is the latent cooling rate (dehumidification) of the process air by the heat exchanger in Watts. This rate is determined by taking the difference between the heat exchanger s total heat recovery rate and the sensible heat recovery rate. A positive value is reported if the process air is dehumidified by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Latent Cooling Energy {[}J{]}}\label{heat-exchanger-latent-cooling-energy-j-2}
+
+This output is the latent cooling energy added to the process air by the heat exchanger in Joules over the timestep being reported.
+
+\paragraph{Heat Exchanger Total Cooling Rate {[}W{]}}\label{heat-exchanger-total-cooling-rate-w-2}
+
+This output is the total cooling rate of the process air by the heat exchanger in Watts. This rate is determined using the process air mass flow rate through the heat exchanger unit and the enthalpy of the air entering and leaving the process side of the unit. A positive value is reported if the enthalpy of the process air is decreased by the heat exchanger, else the rate is set to zero.
+
+\paragraph{Heat Exchanger Total Cooling Energy {[}J{]}}\label{heat-exchanger-total-cooling-energy-j-2}
+
+This output is the total cooling energy added to the process air by the heat exchanger in Joules over the timestep being reported. This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforCooling, GroupKey = System (ref. Output:Meter objects).
+
+\paragraph{Heat Exchanger Electric Power {[}W{]}}\label{heat-exchanger-electric-power-w-2}
+
+This output is the average electric consumption rate of the unit in Watts. This average rate includes portions of the simulation timestep when the heat exchanger may be cycled off (i.e., average of on and off periods, as appropriate).
+
+\paragraph{Heat Exchanger Electric Energy {[}J{]}}\label{heat-exchanger-electric-energy-j-2}
+
+This output is the electric consumption of the unit in Joules for the timestep being reported. This ouput is also added to a meter with ResourceType = Electricity, EndUseKey = HeatRecovery, GroupKey = System (ref. Output:Meter objects).
+
+\subsection{HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1}\label{heatexchangerdesiccantbalancedflowperformancedatatype1}
+
+This object specifies a performance model and model coefficients for a balanced flow desiccant heat exchanger. A HeatExchanger:Desiccant:BalancedFlow object will reference a HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 object. This performance data object is used to specify the thermal performance and electric consumption of the heat exchanger. Some representative inputs for this object are provided in the EnergyPlus Reference DataSets (PerfCurves.idf and AllDataSets.idf).
+
+This model predicts the regeneration air stream outlet temperature and humidity ratio values based on the entering regeneration and process air stream temperature, humidity ratio and face velocity. The process air stream outlet humidity ratio and temperatures are calculated based on a simple heat and moisture balance. The model requires that the user enter the nominal volumetric flow rate and a nominal face velocity, electric power consumption, empirical model coefficients for the regeneration outlet air temperature and humidity ratio equations, and the applicable minimum and maximum values for both the independent and dependent variables for the empirical model coefficients provided. This model is based on the following equations:
+
+\begin{itemize}
+\tightlist
+\item
+  The dry-bulb temperature of the regeneration outlet air is defined using the following equation:
+\end{itemize}
+
+\begin{equation}
+RTO = B1 + B2*RWI + B3*RTI + B4*\left( {\frac{{RWI}}{{RTI}}} \right) + B5*PWI + B6*PTI + B7*\left( {\frac{{PWI}}{{PTI}}} \right) + B8*RFV
+\end{equation}
+
+where,
+
+\(RTO\) = Regeneration outlet air dry-bulb temperature (C)
+
+\(RWI\) = Regeneration inlet air humidity ratio (kgWater/kgDryAir)
+
+\(RTI\) = Regeneration inlet air dry-bulb temperature (C)
+
+\(PWI\) = Process inlet air humidity ratio (kgWater/kgDryAir)
+
+\(PTI\) = Process inlet air dry-bulb temperature (C)
+
+\(RFV\) = Regeneration (and process) face velocity (m/s)
+
+\begin{itemize}
+\tightlist
+\item
+  The humidity ratio of the regeneration outlet air is defined using the same empirical equation form; however, different coefficients are used as follows:
+\end{itemize}
+
+\begin{equation}
+RWO = C1 + C2*RWI + C3*RTI + C4*\left( {\frac{{RWI}}{{RTI}}} \right) + C5*PWI + C6*PTI + C7*\left( {\frac{{PWI}}{{PTI}}} \right) + C8*RFV
+\end{equation}
+
+where,
+
+\(RWO\) = Regeneration outlet air humidity ratio (kgWater/kgDryAir)
+
+\begin{itemize}
+\tightlist
+\item
+  The process outlet air conditions are then calculated based on the regeneration outlet air conditions (temperature or humidity ratio) calculated above, the actual regeneration inlet air conditions entering the heat exchanger, and assuming the same amount of sensible and total energy transfer across both the process and regeneration sides of the heat exchanger. The difference between the actual inlet air conditions and RTI/RWI/PTI/PWI is made here because user-defined limits for RTI/RWI/PTI/PWI may result in a difference between the actual conditions and those used in the equations shown above (see the EnergyPlus Engineering Reference for further discussion).
+\end{itemize}
+
+A description of each input field for this object is provided below.
+
+\subsubsection{Inputs}\label{inputs-3-016}
+
+\paragraph{Field: Name}\label{field-name-3-014}
+
+This alpha field contains the identifying name for this set of desiccant heat exchanger performance data. Any reference to this performance data set by another object (e.g., HeatExchanger:Desiccant:BalancedFlow) will use this name.
+
+\paragraph{Field: Nominal Air Flow Rate}\label{field-nominal-air-flow-rate}
+
+The nominal air volume flow rate in cubic meters per second. This model assumes balanced air flow (i.e., the same air volume flow rate across the process and regeneration sides of the heat exchanger). The minimum value should be greater than 0. This field is autosizable.
+
+\paragraph{Field: Nominal Air Face Velocity}\label{field-nominal-air-face-velocity}
+
+This numeric field contains the nominal air velocity across the heat exchanger face area in meters per second. It is assumed that this air velocity is the same for both sides of the heat exchanger. This value, along with the Nominal Air Flow Rate sets the heat exchanger face area. With this fixed face area, the air face velocity is calculated every simulation timestep based on the actual air volume flow rate for the timestep. The minimum value should be greater than 0 and less than or equal to 6. The default value is 3.0.
+
+\paragraph{Field: Nominal Electric Power}\label{field-nominal-electric-power-2}
+
+This numeric field contains the nominal electric consumption rate of the heat exchanger in watts. This electric power is considered constant and is consumed only when the heat exchanger operates (e.g., for all or a portion of the simulation timestep, as appropriate). This numeric input can be used to model electric power consumption by controls (transformers, relays, etc.) and/or a motor for a rotary heat exchanger. None of this electric power contributes thermal load to the process or regeneration air streams. The minimum value should be greater than or equal to 0. The default value for this field is also 0.
+
+The coefficients for the regeneration air outlet temperature equation described above are defined in the following eight fields:
+
+\paragraph{Field: Temperature Equation Coefficient 1}\label{field-temperature-equation-coefficient-1}
+
+The constant coefficient (B\(_{1}\)) in the temperature equation shown above (RTO).
+
+\paragraph{Field: Temperature Equation Coefficient 2}\label{field-temperature-equation-coefficient-2}
+
+The coefficient (B\(_{2}\)) in the temperature equation shown above (RTO).
+
+\paragraph{Field: Temperature Equation Coefficient 3}\label{field-temperature-equation-coefficient-3}
+
+The coefficient (B\(_{3}\)) in the temperature equation shown above (RTO).
+
+\paragraph{Field: Temperature Equation Coefficient 4}\label{field-temperature-equation-coefficient-4}
+
+The coefficient (B\(_{4}\)) in the temperature equation shown above (RTO).
+
+\paragraph{Field: Temperature Equation Coefficient 5}\label{field-temperature-equation-coefficient-5}
+
+The coefficient (B\(_{5}\)) in the temperature equation shown above (RTO).
+
+\paragraph{Field: Temperature Equation Coefficient 6}\label{field-temperature-equation-coefficient-6}
+
+The coefficient (B\(_{6}\)) in the temperature equation shown above (RTO).
+
+\paragraph{Field: Temperature Equation Coefficient 7}\label{field-temperature-equation-coefficient-7}
+
+The coefficient (B\(_{7}\)) in the temperature equation shown above (RTO).
+
+\paragraph{Field: Temperature Equation Coefficient 8}\label{field-temperature-equation-coefficient-8}
+
+The coefficient (B\(_{8}\)) in the temperature equation shown above (RTO).
+
+The following 16 fields are used to establish the valid range for the dependent and independent variables associated with the coefficients defined above (B\(_{1}\) through B\(_{8}\)) for the regeneration outlet air temperature equation.
+
+\paragraph{Field: Minimum Regeneration Inlet Air Humidity Ratio for Temperature Equation}\label{field-minimum-regeneration-inlet-air-humidity-ratio-for-temperature-equation}
+
+The minimum allowable value of RWI in the temperature equation shown above (kgWater/kgDryAir). Values of RWI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air temperature and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
+
+\paragraph{Field: Maximum Regeneration Inlet Air Humidity Ratio for Temperature Equation}\label{field-maximum-regeneration-inlet-air-humidity-ratio-for-temperature-equation}
+
+The maximum allowable value of RWI in the temperature equation shown above (kgWater/kgDryAir). Values of RWI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air temperature and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
+
+\paragraph{Field: Minimum Regeneration Inlet Air Temperature for Temperature Equation}\label{field-minimum-regeneration-inlet-air-temperature-for-temperature-equation}
+
+The minimum allowable value of RTI in the temperature equation shown above (C). Values of RTI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air temperature and a warning message will be issued.
+
+\paragraph{Field: Maximum Regeneration Inlet Air Temperature for Temperature Equation}\label{field-maximum-regeneration-inlet-air-temperature-for-temperature-equation}
+
+The maximum allowable value of RTI in the temperature equation shown above (C). Values of RTI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air temperature and a warning message will be issued.
+
+\paragraph{Field: Minimum Process Inlet Air Humidity Ratio for Temperature Equation}\label{field-minimum-process-inlet-air-humidity-ratio-for-temperature-equation}
+
+The minimum allowable value of PWI in the temperature equation shown above (kg/kg). Values of PWI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air temperature and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
+
+\paragraph{Field: Maximum Process Inlet Air Humidity Ratio for Temperature Equation}\label{field-maximum-process-inlet-air-humidity-ratio-for-temperature-equation}
+
+The maximum allowable value of PWI in the temperature equation shown above (kg/kg). Values of PWI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air temperature and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
+
+\paragraph{Field: Minimum Process Inlet Air Temperature for Temperature Equation}\label{field-minimum-process-inlet-air-temperature-for-temperature-equation}
+
+The minimum allowable value of PTI in the temperature equation shown above (C). Values of PTI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air temperature and a warning message will be issued.
+
+\paragraph{Field: Maximum Process Inlet Air Temperature for Temperature Equation}\label{field-maximum-process-inlet-air-temperature-for-temperature-equation}
+
+The maximum allowable value of PTI in the temperature equation shown above (C). Values of PTI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air temperature and a warning message will be issued.
+
+\paragraph{Field: Minimum Regeneration Air Velocity for Temperature Equation}\label{field-minimum-regeneration-air-velocity-for-temperature-equation}
+
+The minimum allowable value of RFV in the temperature equation shown above (m/s). Values of RFV less than the minimum will be replaced by this minimum when calculating the regeneration outlet air temperature and a warning message will be issued. The minimum value for this input field should be greater than 0.
+
+\paragraph{Field: Maximum Regeneration Air Velocity for Temperature Equation}\label{field-maximum-regeneration-air-velocity-for-temperature-equation}
+
+The maximum allowable value of RFV in the temperature equation shown above (m/s). Values of RFV greater than the maximum will be replaced by this maximum value when calculating the regeneration outlet air temperature and a warning message will be issued. The minimum value for this input field should be greater than 0.
+
+\paragraph{Field: Minimum Regeneration Outlet Air Temperature for Temperature Equation}\label{field-minimum-regeneration-outlet-air-temperature-for-temperature-equation}
+
+The minimum value of RTO resulting from the temperature equation shown above (C). If RTO is less than this value, RTO will be replaced by this minimum value and a warning message will be issued.
+
+\paragraph{Field: Maximum Regeneration Outlet Air Temperature for Temperature Equation}\label{field-maximum-regeneration-outlet-air-temperature-for-temperature-equation}
+
+The maximum value of RTO resulting from the temperature equation shown above (C). If RTO is greater than this value, RTO will be replaced by this maximum value and a warning message will be issued.
+
+\paragraph{Field: Minimum Regeneration Inlet Air Relative Humidity for Temperature Equation}\label{field-minimum-regeneration-inlet-air-relative-humidity-for-temperature-equation}
+
+The minimum relative humidity of the regeneration inlet air for the temperature equation shown above (percent). If the relative humidity of the regeneration inlet air is below this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
+
+\paragraph{Field: Maximum Regeneration Inlet Air Relative Humidity for Temperature Equation}\label{field-maximum-regeneration-inlet-air-relative-humidity-for-temperature-equation}
+
+The maximum relative humidity of the regeneration inlet air for the temperature equation shown above (percent). If the relative humidity of the regeneration inlet air is above this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
+
+\paragraph{Field: Minimum Process Inlet Air Relative Humidity for Temperature Equation}\label{field-minimum-process-inlet-air-relative-humidity-for-temperature-equation}
+
+The minimum relative humidity of the process inlet air for the temperature equation shown above (percent). If the relative humidity of the process inlet air is below this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
+
+\paragraph{Field: Maximum Process Inlet Air Relative Humidity for Temperature Equation}\label{field-maximum-process-inlet-air-relative-humidity-for-temperature-equation}
+
+The maximum relative humidity of the process inlet air for the temperature equation shown above (percent). If the relative humidity of the process inlet air is above this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
+
+The coefficients for the regeneration outlet air humidity ratio equation are defined in the following eight fields:
+
+\paragraph{Field: Humidity Ratio Equation Coefficient 1}\label{field-humidity-ratio-equation-coefficient-1}
+
+The constant coefficient (C\(_{1}\)) in the humidity ratio equation shown above (RWO).
+
+\paragraph{Field: Humidity Ratio Equation Coefficient 2}\label{field-humidity-ratio-equation-coefficient-2}
+
+The coefficient (C\(_{2}\)) in the humidity ratio equation shown above (RWO).
+
+\paragraph{Field: Humidity Ratio Equation Coefficient 3}\label{field-humidity-ratio-equation-coefficient-3}
+
+The coefficient (C\(_{3}\)) in the humidity ratio equation shown above (RWO).
+
+\paragraph{Field: Humidity Ratio Equation Coefficient 4}\label{field-humidity-ratio-equation-coefficient-4}
+
+The coefficient (C\(_{4}\)) in the humidity ratio equation shown above (RWO).
+
+\paragraph{Field: Humidity Ratio Equation Coefficient 5}\label{field-humidity-ratio-equation-coefficient-5}
+
+The coefficient (C\(_{5}\)) in the humidity ratio equation shown above (RWO).
+
+\paragraph{Field: Humidity Ratio Equation Coefficient 6}\label{field-humidity-ratio-equation-coefficient-6}
+
+The coefficient (C\(_{6}\)) in the humidity ratio equation shown above (RWO).
+
+\paragraph{Field: Humidity Ratio Equation Coefficient 7}\label{field-humidity-ratio-equation-coefficient-7}
+
+The coefficient (C\(_{7}\)) in the humidity ratio equation shown above (RWO).
+
+\paragraph{Field: Humidity Ratio Equation Coefficient 8}\label{field-humidity-ratio-equation-coefficient-8}
+
+The coefficient (C\(_{8}\)) in the humidity ratio equation shown above (RWO).
+
+The following 16 fields are used to establish the valid range for the dependent and independent variables associated with the coefficients defined above (C\(_{1}\) through C\(_{8}\)) for the regeneration outlet air humidity ratio equation.
+
+\paragraph{Field: Minimum Regeneration Inlet Air Humidity Ratio for Humidity Ratio Equation}\label{field-minimum-regeneration-inlet-air-humidity-ratio-for-humidity-ratio-equation}
+
+The minimum allowable value of RWI in the humidity ratio equation shown above (kgWater/kgDryAir). Values of RWI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
+
+\paragraph{Field: Maximum Regeneration Inlet Air Humidity Ratio for Humidity Ratio Equation}\label{field-maximum-regeneration-inlet-air-humidity-ratio-for-humidity-ratio-equation}
+
+The maximum allowable value of RWI in the humidity ratio equation shown above (kgWater/kgDryAir). Values of RWI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
+
+\paragraph{Field: Minimum Regeneration Inlet Air Temperature for Humidity Ratio Equation}\label{field-minimum-regeneration-inlet-air-temperature-for-humidity-ratio-equation}
+
+The minimum allowable value of RTI in the humidity ratio equation shown above (C). Values of RTI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air humidity ratio and a warning message will be issued.
+
+\paragraph{Field: Maximum Regeneration Inlet Air Temperature for Humidity Ratio Equation}\label{field-maximum-regeneration-inlet-air-temperature-for-humidity-ratio-equation}
+
+The maximum allowable value of RTI in the humidity ratio equation shown above (C). Values of RTI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air humidity ratio and a warning message will be issued.
+
+\paragraph{Field: Minimum Process Inlet Air Humidity Ratio for Humidity Ratio Equation}\label{field-minimum-process-inlet-air-humidity-ratio-for-humidity-ratio-equation}
+
+The minimum allowable value of PWI in the humidity ratio equation shown above (kgWater/kgDryAir). Values of PWI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
+
+\paragraph{Field: Maximum Process Inlet Air Humidity Ratio for Humidity Ratio Equation}\label{field-maximum-process-inlet-air-humidity-ratio-for-humidity-ratio-equation}
+
+The maximum allowable value of PWI in the humidity ratio equation shown above (kgWater/kgDryAir). Values of PWI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
+
+\paragraph{Field: Minimum Process Inlet Air Temperature for Humidity Ratio Equation}\label{field-minimum-process-inlet-air-temperature-for-humidity-ratio-equation}
+
+The minimum allowable value of PTI in the humidity ratio equation shown above (C). Values of PTI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air humidity ratio and a warning message will be issued.
+
+\paragraph{Field: Maximum Process Inlet Air Temperature for Humidity Ratio Equation}\label{field-maximum-process-inlet-air-temperature-for-humidity-ratio-equation}
+
+The maximum allowable value of PTI in the humidity ratio equation shown above (C). Values of PTI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air humidity ratio and a warning message will be issued.
+
+\paragraph{Field: Minimum Regeneration Air Velocity for Humidity Ratio Equation}\label{field-minimum-regeneration-air-velocity-for-humidity-ratio-equation}
+
+The minimum allowable value of RFV in the humidity ratio equation shown above (m/s). Values of RFV less than the minimum will be replaced by this minimum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The minimum value for this input field should be greater than 0.
+
+\paragraph{Field: Maximum Regeneration Air Velocity for Humidity Ratio Equation}\label{field-maximum-regeneration-air-velocity-for-humidity-ratio-equation}
+
+The maximum allowable value of RFV in the humidity ratio equation shown above (m/s). Values of RFV greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The minimum value for this input field should be greater than 0.
+
+\paragraph{Field: Minimum Regeneration Outlet Air Humidity Ratio for Humidity Ratio Equation}\label{field-minimum-regeneration-outlet-air-humidity-ratio-for-humidity-ratio-equation}
+
+The minimum value of RWO resulting from the humidity ratio equation shown above (kgWater/kgDryAir). If RWO is less than this value, RWO will be replaced by this minimum value and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
+
+\paragraph{Field: Maximum Regeneration Outlet Air Humidity Ratio for Humidity Ratio Equation}\label{field-maximum-regeneration-outlet-air-humidity-ratio-for-humidity-ratio-equation}
+
+The maximum value of RWO resulting from the humidity ratio equation shown above (kgWater/kgDryAir). If RWO is greater than this value, RWO will be replaced by this maximum value and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
+
+\paragraph{Field: Minimum Regeneration Inlet Air Relative Humidity for Humidity Ratio Equation}\label{field-minimum-regeneration-inlet-air-relative-humidity-for-humidity-ratio-equation}
+
+The minimum relative humidity of the regeneration inlet air for the humidity ratio equation shown above (percent). If the relative humidity of the regeneration inlet air is below this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
+
+\paragraph{Field: Maximum Regeneration Inlet Air Relative Humidity for Humidity Ratio Equation}\label{field-maximum-regeneration-inlet-air-relative-humidity-for-humidity-ratio-equation}
+
+The maximum relative humidity of the regeneration inlet air for the humidity ratio equation shown above (percent). If the relative humidity of the regeneration inlet air is above this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
+
+\paragraph{Field: Minimum Process Inlet Air Relative Humidity for Humidity Ratio Equation}\label{field-minimum-process-inlet-air-relative-humidity-for-humidity-ratio-equation}
+
+The minimum relative humidity of the process inlet air for the humidity ratio equation shown above (percent). If the relative humidity of the process inlet air is below this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
+
+\paragraph{Field: Maximum Process Inlet Air Relative Humidity for Humidity Ratio Equation}\label{field-maximum-process-inlet-air-relative-humidity-for-humidity-ratio-equation}
+
+The maximum relative humidity of the process inlet air for the humidity ratio equation shown above (percent). If the relative humidity of the process inlet air is above this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
+
+Following is an example input for this heat exchanger performance data type object:
+
+\begin{lstlisting}
+
+HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1,
+  HXDesPerf1,         !- Name
+  1.05,                     !- Nominal Air Flow Rate {m3/s}
+  3.25,                     !- Nominal Air Face Velocity {m/s}
+  50.0,                     !- Nominal Electric Power {W}
+  -2.53636E+00,     !- Temperature Equation Coefficient 1
+  2.13247E+01,       !- Temperature Equation Coefficient 2
+  9.23308E-01,       !- Temperature Equation Coefficient 3
+  9.43276E+02,       !- Temperature Equation Coefficient 4
+  -5.92367E+01,     !- Temperature Equation Coefficient 5
+  -4.27465E-02,     !- Temperature Equation Coefficient 6
+  1.12204E+02,       !- Temperature Equation Coefficient 7
+  7.78252E-01,       !- Temperature Equation Coefficient 8
+
+
+  0.007143,             !- Minimum Regeneration Inlet Air Humidity Ratio for Temperature Equation
+  0.024286,             !- Maximum Regeneration Inlet Air Humidity Ratio for Temperature Equation
+  46.111110,           !- Minimum Regeneration Inlet Air Temperature for Temperature Equation {C}
+  46.111112,           !- Maximum Regeneration Inlet Air Temperature for Temperature Equation {C}
+  0.005000,             !- Minimum Process Inlet Air Humidity Ratio for Temperature Equation
+  0.015714,             !- Maximum Process Inlet Air Humidity Ratio for Temperature Equation
+  4.583333,             !- Minimum Process Inlet Air Temperature for Temperature Equation {C}
+  21.83333,             !- Maximum Process Inlet Air Temperature for Temperature Equation {C}
+  2.286,                   !- Minimum Regeneration Air Velocity for Temperature Equation {m/s}
+  4.826,                   !- Maximum Regeneration Air Velocity for Temperature Equation {m/s}
+  35.0,                     !- Minimum Regeneration Outlet Air Temperature for Temperature Equation {C}
+  50.0,                     !- Maximum Regeneration Outlet Air Temperature for Temperature Equation {C}
+  5.0,                       !- Minimum Regeneration Inlet Air Relative Humidity for Temperature Equation {percent}
+  45.0,                     !- Maximum Regeneration Inlet Air Relative Humidity for Temperature Equation {percent}
+  80.0,                     !- Minimum Process Inlet Air Relative Humidity for Temperature Equation {percent}
+  100.0,                   !- Maximum Process Inlet Air Relative Humidity for Temperature Equation {percent}
+  -2.25547E+01,     !- Humidity Ratio Equation Coefficient 1
+  9.76839E-01,       !- Humidity Ratio Equation Coefficient 2
+  4.89176E-01,       !- Humidity Ratio Equation Coefficient 3
+  -6.30019E-02,     !- Humidity Ratio Equation Coefficient 4
+  1.20773E-02,       !- Humidity Ratio Equation Coefficient 5
+  5.17134E-05,       !- Humidity Ratio Equation Coefficient 6
+  4.94917E-02,       !- Humidity Ratio Equation Coefficient 7
+  -2.59417E-04,     !- Humidity Ratio Equation Coefficient 8
+  0.007143,             !- Minimum Regeneration Inlet Air Humidity Ratio for Humidity Ratio Equation
+  0.024286,             !- Maximum Regeneration Inlet Air Humidity Ratio for Humidity Ratio Equation
+  46.111110,           !- Minimum Regeneration Inlet Air Temperature for Humidity Ratio Equation {C}
+  46.111112,           !- Maximum Regeneration Inlet Air Temperature for Humidity Ratio Equation {C}
+  0.005000,             !- Minimum Process Inlet Air Humidity Ratio for Humidity Ratio Equation
+  0.015714,             !- Maximum Process Inlet Air Humidity Ratio for Humidity Ratio Equation
+  4.583333,             !- Minimum Process Inlet Air Temperature for Humidity Ratio Equation {C}
+  21.83333,             !- Maximum Process Inlet Air Temperature for Humidity Ratio Equation {C}
+  2.286,                   !- Minimum Regeneration Air Velocity for Humidity Ratio Equation {m/s}
+  4.826,                   !- Maximum Regeneration Air Velocity for Humidity Ratio Equation {m/s}
+  0.007914,             !- Minimum Regeneration Outlet Air Humidity Ratio for Humidity Ratio Equation
+  0.026279,             !- Maximum Regeneration Outlet Air Humidity Ratio for Humidity Ratio Equation
+  5.0,                 !- Minimum Regeneration Inlet Air Relative Humidity for Humidity Ratio Equation {%}
+  45.0,               !- Maximum Regeneration Inlet Air Relative Humidity for Humidity Ratio Equation {percent}
+  80.0,                   !- Minimum Process Inlet Air Relative Humidity for Humidity Ratio Equation {percent}
+  100.0;                 !- Maximum Process Inlet Air Relative Humidity for Humidity Ratio Equation {percent}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-008}
+
+No variables are reported for this object. However, outputs are provided by the HeatExchanger:Desiccant:BalancedFlow object that references this PerformanceDataType1 object.
diff --git a/doc/input-output-reference/src/overview/group-heating-and-cooling-coils.tex b/doc/input-output-reference/src/overview/group-heating-and-cooling-coils.tex
new file mode 100644
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@@ -0,0 +1,8531 @@
+\section{Group Heating and Cooling Coils}\label{group-heating-and-cooling-coils}
+
+Several different coils may be added to zone equipment and air loops. This includes simple heating (gas, electric, and hot water) and a simple water-cooling coil as well as a more detailed flat fin water-cooling coil model. In general, the heating coil description can be used for a heating coil, a reheat coil, or a preheat coil in the air loop simulation or for zone equipment. Figure~\ref{fig:example-air-loop-heating-cooling-coil} is an example of a heating and cooling coil in the air loop simulation in a dual duct system. This does show the basic node structure that will be referenced in the input description. The figure does show water coils since they are the most complex to input in the simulation compared to the Electric and Gas coils which only have air connections.
+
+\begin{figure}[hbtp] % fig 135
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image349.png}
+\caption{Example Air Loop Heating \& Cooling Coil \protect \label{fig:example-air-loop-heating-cooling-coil}}
+\end{figure}
+
+\subsection{Coil:Cooling:Water}\label{coilcoolingwater}
+
+The water cooling coil (Coil:Cooling:Water) has the ability to give detailed output with simplified inputs, inputting complicated coil geometry is not required by the user for this model instead the coil is sized in terms of auto-sizeable thermodynamic inputs. The coil requires thermodynamic inputs such as temperatures, mass flow rates and humidity ratios.
+
+The coil is sized using auto-sized/user design input conditions and the UA values are calculated from the design conditions. A rough estimate of the coil area is provided along with percentage of surface wet and/or dry. This model uses the NTU-effectiveness approach to model heat transfer and has two types of flow arrangements cross-flow or counter-flow.
+
+The basic underlying idea is - use auto sizable thermodynamic design inputs, calculate the coil UA s, use these UA values and operating conditions from the nodes connections, calculate the outlet stream conditions, and calculate the heat transfer rates.
+
+See section Cooling Coil Model in the EnergyPlus Engineering Document for further details regarding this model.
+
+\subsubsection{Inputs}\label{inputs-022}
+
+\paragraph{Field: Name}\label{field-name-021}
+
+A unique user-assigned name for an instance of a cooling coil. Any reference to this cooling coil by another object will use this name.
+
+\paragraph{Field:Availability Schedule Name}\label{fieldavailability-schedule-name-000}
+
+Schedule that defines when the coil is available. The name of the schedule (ref: Schedule) that denotes whether the cooling coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during a given time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit is off. If this field is blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Design Water Flow Rate}\label{field-design-water-flow-rate-000}
+
+The maximum possible water volume flow rate (m\(^{3}\)/sec) through the coil. This is an auto sizable design input.
+
+\paragraph{Field: Design Air Flow Rate}\label{field-design-air-flow-rate-000}
+
+The maximum possible air volume flow rate (m\(^{3}\)/sec) through the coil. This is an auto sizable design input.
+
+\paragraph{Field: Design Inlet Water Temperature}\label{field-design-inlet-water-temperature-000}
+
+The inlet water temperature for the design flow (C). This is an auto sizable design input.
+
+\paragraph{Field: Design Inlet Air Temperature}\label{field-design-inlet-air-temperature}
+
+The inlet air temperature for the design flow (C). This is an auto sizable design input.
+
+\paragraph{Field: Design Outlet Air Temperature}\label{field-design-outlet-air-temperature}
+
+The outlet air condition desired for design flow (C). This is an auto sizable design input.
+
+\paragraph{Field: Design Inlet Air Humidity Ratio}\label{field-design-inlet-air-humidity-ratio}
+
+The highest value of humidity ratio possible for the Design inlet air stream (kgWater/kgDryAir). This is an auto sizable input.
+
+\paragraph{Field: Design Outlet Air Humidity Ratio}\label{field-design-outlet-air-humidity-ratio}
+
+The value of humidity ratio for the Design outlet air stream (kgWater/kgDryAir), it is an auto sizable input.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-000}
+
+The name of the water coil inlet from the chilled water loop, i.e.~Cooling Coil Water Inlet Node. It is from this node the operating inputs for water are transferred to the coil.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-000}
+
+The name of the water coil outlet from the chilled water loop, i.e.~Cooling Coil Water Outlet Node. It is from this node the operating output for water are reported to the coil.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-003}
+
+The name of the air inlet to the water coil, i.e.~Cooling Coil Air Inlet Node. It is from this node the operating inputs for air are transferred to the coil.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-003}
+
+The name of the air outlet from the water coil, i.e.~Cooling Coil Air Outlet Node. It is from this node the operating output for airside is reported to the coil.
+
+\paragraph{Field: Type of Analysis}\label{field-type-of-analysis}
+
+The coil has two modes of operation, termed as \textbf{SimpleAnalysis} and \textbf{DetailedAnalysis}. The difference between the two modes being, the simple mode reports the value of surface area fraction wet of the coil as dry or wet. The detailed mode give the exact value, however the execution time in detailed mode is noticeably higher.
+
+\paragraph{Field: Heat Exchanger Configuration}\label{field-heat-exchanger-configuration-000}
+
+The coil is operable in two modes, Cross Flow for general A/C applications and Counter flow mode. Air-conditioning systems generally use cross flow heat exchangers, hence the default is set to cross flow.
+
+\paragraph{Field: Condensate Collection Water Storage Tank Name}\label{field-condensate-collection-water-storage-tank-name}
+
+This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
+
+Examples when auto sized in an IDF are as below:
+
+\begin{lstlisting}
+
+Coil:Cooling:Water,
+  Main Cooling Coil 1,       !- Coil Name
+  CoolingCoilAvailSched,   !-Availability Schedule Name
+  autosize,         !- Design Water Volume Flow Rate of Coil {m3/s}
+  autosize,         !- Design Air Flow Rate of Coil {m3/s}
+  autosize,         !- Design Inlet Water Temperature {C}
+  autosize,         !- Design Inlet Air Temperature {C}
+  autosize,         !- Design Outlet Air Temperature {C}
+  autosize,         !- Design Inlet Air Humidity Ratio(kgWater/kgDryAir)
+  autosize,         !- Design Outlet Air Humidity Ratio(kgWater/kgDryAir)
+  Main Cooling Coil 1 Water Inlet Node,     !- Coil_Water_Inlet_Node
+  Main Cooling Coil 1 Water Outlet Node,   !- Coil_Water_Outlet_Node
+  Mixed Air Node 1,                                             !- Coil_Air_Inlet_Node
+  Main Cooling Coil 1 Outlet Node;               !- Coil_Air_Outlet_Node
+\end{lstlisting}
+
+Examples when values (hard-sized) are input in an IDF are as below:
+
+\begin{lstlisting}
+
+Coil:Cooling:Water,
+  Main Cooling Coil 1,       !- Coil Name
+  CoolingCoilAvailSched,   !-Availability Schedule Name
+  0.0022,       !- Design Water Volume Flow Rate of Coil {m3/s}
+  1.45,           !- Design Air Flow Rate of Coil {m3/s}
+  6.1,             !- Design Inlet Water Temperature {C}
+  25,               !- Design Inlet Air Temperature {C}
+  10,               !- Design Outlet Air Temperature {C}
+  0.012,         !- Design Inlet Air Humidity Ratio
+  0.008,         !- Design Outlet Air Humidity Ratio
+  Main Cooling Coil 1 Water Inlet Node,     !- Coil_Water_Inlet_Node
+  Main Cooling Coil 1 Water Outlet Node,   !- Coil_Water_Outlet_Node
+  Mixed Air Node 1,                                             !- Coil_Air_Inlet_Node
+  Main Cooling Coil 1 Outlet Node;               !- Coil_Air_Outlet_Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-015}
+
+Following are the list of possible output output variables from this coil model:
+
+\begin{itemize}
+\item
+  HVAC,Sum,Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Coil Wetted Area Fraction {[]}
+\item
+  HVAC,Average,Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Coil Source Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Sum,Cooling Coil Condensate Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Cooling Coil Total Cooling Energy (J)}\label{cooling-coil-total-cooling-energy-j}
+
+Cooling Coil Total Cooling Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
+
+\paragraph{Cooling Coil Sensible Cooling Energy (J)}\label{cooling-coil-sensible-cooling-energy-j}
+
+Cooling Coil Sensible Cooling Energy is the total amount of Sensible heat transfer taking place in the coil at the operating conditions. It only takes into account temperature difference in the inlet and outlet air streams at operating conditions.
+
+\paragraph{Cooling Coil Total Cooling Rate (W)}\label{cooling-coil-total-cooling-rate-w}
+
+Cooling Coil Total Cooling Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
+
+\paragraph{Cooling Coil Sensible Cooling Rate (W)}\label{cooling-coil-sensible-cooling-rate-w}
+
+Cooling Coil Sensible Cooling Rate is the Rate of Sensible heat transfer taking place in the coil at the operating conditions.
+
+\paragraph{\texorpdfstring{Cooling Coil Wetted Area Fraction {[]}}{Cooling Coil Wetted Area Fraction }}\label{cooling-coil-wetted-area-fraction}
+
+It defines the fraction of total surface area of coil which is wet due to moisture condensation on the surface of the coil. Value varies between 0.0 and 1.0.
+
+In addition, if a Water Storage Tank is used to collect coil condensate, then the following outputs will be available.
+
+\paragraph{Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}}\label{cooling-coil-condensate-volume-flow-rate-m3s}
+
+\paragraph{Cooling Coil Condensate Volume {[}m3{]}}\label{cooling-coil-condensate-volume-m3}
+
+These reports provide the rate and amount of condensate from the coil. Condensate is water condensed out of the air as a result of cooling. The condensate volume is also reported on the meter for OnSiteWater.
+
+\paragraph{Cooling Coil Source Side Heat Transfer Energy {[}J{]}}\label{cooling-coil-source-side-heat-transfer-energy-j}
+
+This is the energy extracted from the chilled water serving the coil, in Joules.
+
+\subsection{Coil:Heating:Water}\label{coilheatingwater}
+
+This simple heating coil model only does sensible heating of the air. The simple heating coil uses the Effectiveness-NTU algorithm and assumes a cross-flow heat exchanger.
+
+\subsubsection{Inputs}\label{inputs-1-020}
+
+\paragraph{Field: Name}\label{field-name-1-019}
+
+A unique identifying name for each coil.
+
+\paragraph{Field:Availability Schedule Name}\label{fieldavailability-schedule-name-1-000}
+
+Schedule that defines when the coil is available. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during a given time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit is off. If this field is blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: U-Factor Times Area Value}\label{field-u-factor-times-area-value}
+
+The UA value for the coil needed for the Effectiveness-NTU heat exchanger model. An estimate of the UA can be obtained from:
+
+\begin{equation}
+q = UA \times ({T_{water,avg}} - {T_{air,avg}})
+\end{equation}
+
+where q is the heat transferred from water to the air in watts; T\(_{water,\\ avg}\) is the average water temperature in degrees C; and T\(_{air,\\ avg}\) is the average air temperature in degrees C. Or the LMTD temperature difference can be used. This field is used when \emph{Performance Input Method} = \emph{UFactorTimesAreaAndDesignWaterFlowRate}.This field is autosizable.
+
+\paragraph{Field: Maximum Water Flow Rate}\label{field-maximum-water-flow-rate-000}
+
+The maximum possible water flow rate (m\(^{3}\)/sec) through the coil. This field is used when \emph{Coil Performance Input Method} = \emph{UFactorTimesAreaAndDesignWaterFlowRate}. This field is autosizable.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-1-000}
+
+The name of the coil s water inlet node from the hot water loop.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-1-000}
+
+The name of the coil s water outlet node from the hot water loop.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-1-003}
+
+The name of the air inlet node to the water coil.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-1-002}
+
+The name of the air outlet node from the water coil.
+
+\paragraph{Field: Performance Input Method}\label{field-performance-input-method-001}
+
+The user can choose either \emph{UFactorTimesAreaAndDesignWaterFlowRate} or \emph{NominalCapacity}. If \emph{UFactorTimesAreaAndDesignWaterFlowRate} is selected, the user must input values for UA of the Coil and Max Water FlowRate of the Coil (and Rated Capacity is ignored). If \emph{NominalCapacity} is chosen, the user must input a Rated Capacity for the coil; UA of the Coil and Max Water FlowRate of the Coil will be ignored. Rated capacity is defined as the heating capacity in watts of the coil at the rating points (i.e., the rated inlet and outlet water/air temperatures defined in the input fields below). The rated capacity is used to calculate a water mass flow rate and a UA for the coil. The default is \emph{NominalCapacity}.
+
+To autosize the capacity, choose \emph{UfactorTimesAreaAndDesignWaterFlowRate} and put autosize as the inputs for \emph{U-Factor Times Area Value, Maximum Water Flow Rate,} and \emph{Rated Capacity}. The program will use the Sizing inputs to size the coil. The rated temperatures (see below) are ignored in autosizing. These are used only when the user is specifying coil performance using the \emph{NominalCapacity} input method.
+
+\paragraph{Field: Gross Rated Heating Capacity}\label{field-gross-rated-heating-capacity}
+
+The heating capacity of the coil in watts at the rated inlet and outlet air and water temperatures. The gross rated heating capacity does not account for the effect of supply air fan heat. This field is used when the \emph{Performance Input Method} = \emph{Nominal Capacity}. This field is autosizable. The rating points are given in the four subsequent input fields.
+
+\paragraph{Field: Rated Inlet Water Temperature}\label{field-rated-inlet-water-temperature}
+
+The inlet water temperature (degrees C) corresponding to the rated heating capacity. The default is 82.2 degrees C (180 degrees F).
+
+\paragraph{Field: Rated Inlet Air Temperature}\label{field-rated-inlet-air-temperature}
+
+The inlet air temperature (degrees C) corresponding to the rated heating capacity. The default is 16.6 degrees C (60 degrees F).
+
+\paragraph{Field: Rated Outlet Water Temperature}\label{field-rated-outlet-water-temperature}
+
+The outlet water temperature (degrees C) corresponding to the rated heating capacity. The default is 71.1 degrees C (160 degrees F).
+
+\paragraph{Field: Rated Outlet Air Temperature}\label{field-rated-outlet-air-temperature}
+
+The outlet air temperature (degrees C) corresponding to the nominal heating capacity. The default is 32.2 degrees C (90 degrees F).
+
+\paragraph{Field: Rated Ratio for Air and Water Convection}\label{field-rated-ratio-for-air-and-water-convection}
+
+This is the ratio of convective heat transfers between air side and water side of the heating coil at the rated operating conditions. The default is .5. This ratio describes the geometry and the design of the coil and is defined by:
+
+\begin{equation}
+ratio = \frac{{{\eta_f}{{\left( {hA} \right)}_{air}}}}{{{{\left( {hA} \right)}_{water}}}}
+\end{equation}
+
+where,
+
+\({\eta_f}\) is the fin efficiency, (dimensionless)
+
+\emph{h} is the surface convection heat transfer coefficient
+
+\emph{A} is the surface area
+
+An example input of the object is:
+
+\begin{lstlisting}
+
+Coil:Heating:Water,
+  SPACE3-1 Zone Coil,           !- Coil Name
+  ReheatCoilAvailSched,       !- Availability Schedule Name
+  ,                                               !- UA of the Coil {W/K}
+  ,                                               !- Max Water Flow Rate of Coil {m3/s}
+  SPACE3-1 Zone Coil Water In Node,   !- Coil_Water_Inlet_Node
+  SPACE3-1 Zone Coil Water Out Node,   !- Coil_Water_Outlet_Node
+  SPACE3-1 Zone Coil Air In Node,   !- Coil_Air_Inlet_Node
+  SPACE3-1 In Node,               !- Coil_Air_Outlet_Node
+  NominalCapacity,                 !- Coil Performance Input Method
+  10000.,                                   !- Gross Rated Heating Capacity
+  0.55;                                       !- Rated Ratio for Air and Water Convection
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-013}
+
+\begin{itemize}
+\item
+  HVAC,Sum, Heating Coil Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Heating Coil Source Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Heating Rate {[}W{]}
+\item
+  HVAC,Average, Heating Coil U Factor Times Area Value {[}W/K{]}
+\end{itemize}
+
+\paragraph{Heating Coil Heating Energy {[}J{]}}\label{heating-coil-heating-energy-j}
+
+Heating Coil Heating Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
+
+\paragraph{Heating Coil Heating Rate {[}W{]}}\label{heating-coil-heating-rate-w}
+
+Heating Coil Heating Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
+
+\paragraph{Heating Coil U Factor Times Area Value {[}W/K{]}}\label{heating-coil-u-factor-times-area-value-wk}
+
+This characterizes the overall heat transfer UA value, or U-factor times Area. The simple heating coil model adjusts UA value based on inlet temperatures and flow rates and this output contains the results from that adjustment.
+
+\paragraph{Heating Coil Source Side Heat Transfer Energy {[}J{]}}\label{heating-coil-source-side-heat-transfer-energy-j}
+
+This is the same has the Heating Coil Heating Energy but it is also metered as a plant loop heating demand. This represents the heat in Joules extracted from the hot water serving the coil.
+
+\subsection{Coil:Heating:Steam}\label{coilheatingsteam}
+
+The simple steam to air heating coil model only does sensible heating of the air. The steam to air coils condenses the steam and sub cools steam at loop pressure and discharges the condensate through steam traps at low pressure condensate line.
+
+\subsubsection{Inputs}\label{inputs-2-019}
+
+\paragraph{Field: Name}\label{field-name-2-018}
+
+A unique identifying name for each steam coil.
+
+\paragraph{Field:Availability Schedule Name}\label{fieldavailability-schedule-name-2-000}
+
+Schedule that defines when the coil is available. If the schedule s value is less than or equal to 0.0, then the coil is not available and flow will not be requested. If the schedule s value is \textgreater{} 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Maximum Steam Flow Rate}\label{field-maximum-steam-flow-rate}
+
+The maximum possible steam volumetric flow rate in m\(^{3}\)/s through the steam heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. This field is autosizable.
+
+\paragraph{Field: Degree of SubCooling}\label{field-degree-of-subcooling}
+
+Ideally the steam trap located at the outlet of steam coil should remove all the condensate immediately, however there is a delay in this process in actual systems which causes the condensate to SubCool by certain degree in the coil before leaving the coil, this SubCool occurs in the steam coil and this SubCool-heat is added to the zone. The minimum value is 2 ° Celsius and default is 5 ° Celsius.
+
+\paragraph{Field: Degree of Loop SubCooling}\label{field-degree-of-loop-subcooling}
+
+This essentially represents the heat loss to the atmosphere due to uninsulated condensate return piping to the boiler. Condensate return piping operates at atmospheric pressure and is not insulated. The condensate sub cools to certain degree before it is pumped back to the boiler. The minimum value is 10 ° Celsius and default is 20 ° Celsius.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-2-000}
+
+The name of the steam coil inlet from the steam loop, i.e.~Steam Coil steam inlet node.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-2-000}
+
+The name of the steam coil outlet to the condensate loop, i.e.~Steam Coil condensate outlet node.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-2-001}
+
+The name of the air inlet to the steam coil, i.e.~Steam Coil Air Inlet Node.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-2-001}
+
+The name of the air outlet from the steam coil, i.e.~Steam Coil Air Outlet Node.
+
+\paragraph{Field:Coil Control Type}\label{fieldcoil-control-type}
+
+Choice of either \textbf{ZoneLoadControl} steam coil or \textbf{TemperatureSetpointControl} steam coil. A zone coil is load controlled and an air loop steam coil is temperature controlled.
+
+\paragraph{Field: Temperature Setpoint Node Name}\label{field-temperature-setpoint-node-name}
+
+If the coil is used in the air loop simulation and is temperature controlled using a Set Point Manager (i.e., the previous file is TemperatureSetpointConrtol), then the node that is the control node needs to be specified here. If the coil is used in an air terminal unit, the coil is load controlled and a control node set point is not required (i.e., the previous field is ZoneLoadControl).
+
+An example of a Steam Coil input statement (one each for Temperature Controlled and Load Controlled) from an IDF is given below:
+
+\begin{lstlisting}
+
+Coil:Heating:Steam,
+  VAV SYS 1 Heating Coil,                   !- Coil Name
+  ReheatCoilAvailSched,                       !- Availability Schedule Name
+  0.06,                                                       !- Max Steam volume Flow rate
+  5.0,                                                         !- Deg of Subcooling Desired
+  15.0,                                                        !- Loop Subcooling Desired
+  VAV SYS 1 Heating Coil Steam Inlet,   !- Coil Steam Inlet Node
+  VAV SYS 1 Heating Coil Steam Outlet, !- Coil Water Outlet Node
+  VAV SYS 1 Cooling Coil Outlet,       !- Coil Air Inlet Node
+  VAV SYS 1 Heating Coil Outlet,       !- Coil Air Outlet Node
+  TemperatureSetPointControl,             !- field Coil Control Type
+  VAV SYS 1 Heating Coil Outlet;       !- field Coil Temp Setpoint Node
+
+
+  Coil:Heating:Steam,
+  SPACE1-1 Reheat Coil,                             !- Coil Name
+  ReheatCoilAvailSched,                             !- Availability Schedule Name
+  autosize,                                                      !- Max Steam volume Flow rate
+  5.0,                                                                !- Deg of Subcooling Desired
+  15.0,                                                              !- Loop Subcooling Desired
+  SPACE1-1 Reheat Coil Steam Inlet,     !- Coil Steam Inlet Node
+  SPACE1-1 Reheat Coil Steam Outlet,   !- Coil Water Outlet Node
+  SPACE1-1 Damper Outlet,                         !- Coil Air Inlet Node
+  SPACE1-1 Supply Inlet,   !- Coil Air Outlet Node
+  ZoneLoadControl;         !- field Coil Control Type
+\end{lstlisting}
+
+\subsection{Heating Coil (Steam) Outputs:}\label{heating-coil-steam-outputs}
+
+\begin{itemize}
+\item
+  HVAC,Sum, Heating Coil Heating Energy {[}J{]}
+\item
+  HVAC,Average,Total Steam Coil Heating Rate {[}W{]}
+\item
+  HVAC,Average,Heating Coil Steam Trap Loss Rate {[}W{]}
+\item
+  HVAC, Average, Heating Coil Steam Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Heating Coil Steam Outlet Temperature {[}C{]}
+\item
+  HVAC, Average, Heating Coil Steam Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\subsubsection{Heating Coil Heating Energy {[}J{]}}\label{heating-coil-heating-energy-j-1}
+
+Heating Coil Heating Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
+
+\subsubsection{Heating Coil Heating Rate {[}W{]}}\label{heating-coil-heating-rate-w-1}
+
+Heating Coil Heating Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
+
+\subsubsection{Heating Coil Steam Trap Loss Rate {[}W{]}}\label{heating-coil-steam-trap-loss-rate-w}
+
+Loop losses represent the unavoidable loss due to degree of sub cooling in the condensate return piping back to the boiler and the loss occurring due to flashing of steam across the steam trap due to pressure differential between the steam and the condensate side.
+
+\subsubsection{Heating Coil Steam Inlet Temperature {[}C{]}}\label{heating-coil-steam-inlet-temperature-c}
+
+\subsubsection{Heating Coil Steam Outlet Temperature {[}C{]}}\label{heating-coil-steam-outlet-temperature-c}
+
+\subsubsection{Heating Coil Steam Mass Flow Rate {[}kg/s{]}}\label{heating-coil-steam-mass-flow-rate-kgs}
+
+These outputs are the Steam inlet and condensate outlet temperatures and steam flow rate for the boiler.
+
+\subsection{Coil:Heating:Electric}\label{coilheatingelectric}
+
+The electric heating coil is a simple capacity model with a user-inputted efficiency. In many cases, this efficiency for the electric coil will be 100\%. This coil will be simpler than shown in Figure~\ref{fig:example-air-loop-heating-cooling-coil} since it will only have air nodes to connect it in the system. The coil can be used in the air loop simulation or in the zone equipment as a reheat coil. Depending on where it is used determines if this coil is temperature or capacity controlled. If used in the air loop simulation it will be controlled to a specified temperature scheduled from the SetPoint Manager. If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand.
+
+\subsubsection{Inputs}\label{inputs-3-017}
+
+\paragraph{Field: Name}\label{field-name-3-015}
+
+A unique identifying name for each coil.
+
+\paragraph{Field:Availability Schedule Name}\label{fieldavailability-schedule-name-3}
+
+Schedule that defines when the coil is available. If the schedule s value is 0.0, then the coil is not available and flow will not be requested. If the schedule s value is \textgreater{} 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods. Schedule values must be \textgreater{} = 0 and \textless{} = 1.
+
+\paragraph{Field: Efficiency}\label{field-efficiency}
+
+This is user-inputted efficiency (decimal units, not percent) and can account for any loss. In most cases for the electric coil, this will be 100\%.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-000}
+
+This is the maximum capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-3-001}
+
+The name of the air inlet to the electric coil, i.e.~Heating Coil Air Inlet Node.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-3-001}
+
+The name of the air outlet from the electric coil, i.e.~Heating Coil Air Outlet Node.
+
+\paragraph{Field: Temperature Setpoint Node Name}\label{field-temperature-setpoint-node-name-1}
+
+If the coil is used in the air loop simulation and is temperature controlled using a Set Point Manager, then the node that is the control node needs to be specified here. If the coil is used in an air terminal unit, the coil is load controlled and a control node set point is not required.
+
+An example of IDF usage:
+
+\begin{lstlisting}
+
+Coil:Heating:Electric,
+  AHU Reheater,                     !- Name
+  2,                                           !- Availability Schedule Name
+  0.99,                                     !- Efficiency
+  600000,                                 !- Nominal Capacity {W}
+  DOAS Supply Fan Outlet, !- Air Inlet Node Name
+  AHU Reheater Outlet,       !- Air Outlet Node Name
+  AHU Reheater Outlet;       !- Temperature Setpoint Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-011}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Heating Coil Air Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Air Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Electric Power {[}W{]}
+\end{itemize}
+
+\paragraph{Heating Coil Air Heating Energy (J)}\label{heating-coil-air-heating-energy-j}
+
+Heating Coil Air Heating Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
+
+\paragraph{Heating Coil Air Heating Rate {[}W{]}}\label{heating-coil-air-heating-rate-w}
+
+Heating Coil Air Heating Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
+
+\paragraph{Heating Coil Electric Energy {[}J{]}}\label{heating-coil-electric-energy-j}
+
+Heating Coil electric consumption after the efficiency of the coil has been taken into account in Joules for the timestep reported.
+
+\paragraph{Heating Coil Electric Power {[}W{]}}\label{heating-coil-electric-power-w}
+
+This field is the average Heating Coil electric power after the efficiency of the coil has been taken into account in Watts for the timestep reported.
+
+\subsection{Coil:Heating:Electric:MultiStage}\label{coilheatingelectricmultistage}
+
+The multi stage electric heating coil is a simple capacity model with a user-inputted efficiencies at different stages. In many cases, the efficiencies for the electric coil will be 100\%. This coil will only have air nodes to connect it in the system. The coil can be used in the air loop simulation or in the zone equipment as a reheat coil. Depending on where it is used determines if this coil is temperature or capacity controlled. If used in the air loop simulation it will be controlled to a specified temperature scheduled from the SetPoint Manager. If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand. For the time being, this coil model can only be called by the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
+
+\subsubsection{Inputs}\label{inputs-4-015}
+
+\paragraph{Field: Name}\label{field-name-4-012}
+
+A unique identifying name for each coil.
+
+\paragraph{Field:Availability Schedule Name}\label{fieldavailability-schedule-name-4}
+
+Schedule that defines when the coil is available. If the schedule s value is 0.0, then the coil is not available and flow will not be requested. If the schedule s value is \textgreater{} 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods. Schedule values must be \textgreater{} = 0 and \textless{} = 1.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-4-001}
+
+The name of the air inlet to the electric coil, i.e.~Heating Coil Air Inlet Node.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-4-001}
+
+The name of the air outlet from the electric coil, i.e.~Heating Coil Air Outlet Node.
+
+\paragraph{Field: Temperature Setpoint Node Name}\label{field-temperature-setpoint-node-name-2}
+
+If the coil is used in the air loop simulation and is temperature controlled using a Set Point Manager, then the node that is the control node needs to be specified here. If the coil is used in an air terminal unit, the coil is load controlled and a control node set point is not required. At present, the multistage electric heating coil does not model temperature setoint control.
+
+\paragraph{Field: Stage 1 Efficiency}\label{field-stage-1-efficiency}
+
+This is stage 1 user-inputted efficiency (decimal units, not percent) and can account for any loss. In most cases for the electric coil, this will be 100\%.
+
+\paragraph{Field: Stage 1 Nominal Capacity}\label{field-stage-1-nominal-capacity}
+
+This is stage 1 capacity of the coil (W). This field is autosizable.
+
+\paragraph{Field: Stage 2 Efficiency}\label{field-stage-2-efficiency}
+
+This is stage 2 user-inputted efficiency (decimal units, not percent) and can account for any loss. In most cases for the electric coil, this will be 100\%.
+
+\paragraph{Field: Stage 2 Nominal Capacity}\label{field-stage-2-nominal-capacity}
+
+This is stage 2 capacity of the coil (W). This field is autosizable.
+
+\paragraph{Field: Stage 3 Efficiency}\label{field-stage-3-efficiency}
+
+This is stage 3 user-inputted efficiency (decimal units, not percent) and can account for any loss. In most cases for the electric coil, this will be 100\%.
+
+\paragraph{Field: Stage 3 Nominal Capacity}\label{field-stage-3-nominal-capacity}
+
+This is stage 3 capacity of the coil (W). This field is autosizable.
+
+\paragraph{Field: Stage 4 Efficiency}\label{field-stage-4-efficiency}
+
+This is stage 4 user-inputted efficiency (decimal units, not percent) and can account for any loss. In most cases for the electric coil, this will be 100\%.
+
+\paragraph{Field: Stage 4 Nominal Capacity}\label{field-stage-4-nominal-capacity}
+
+This is stage 4 capacity of the coil (W). This field is autosizable.
+
+An example in IDF form:
+
+\begin{lstlisting}
+
+Coil:Heating:Electric:MultiStage,
+  Heat Pump Heating Coil 1,                 !- Name
+  FanAndCoilAvailSched,                         !- Availability Schedule Name
+  Heating Coil Air Inlet Node,           !- Air Inlet Node Name
+  SuppHeating Coil Air Inlet Node,   !- Air Outlet Node Name
+  ,                                               !- Temp Setpoint node name
+  3,                                             !- Number of Stages
+  1,                                             !- Stage 1 Efficiency
+  Autosize,                               !- Stage 1 Nominal Capacity {W}
+  1,                                             !- Stage 2 Efficiency
+  Autosize,                               !- Stage 2 Nominal Capacity {W}
+  1,                                             !- Stage 3 Efficiency
+  Autosize;                               !- Stage 3 Nominal Capacity {W}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-009}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Heating Coil Energy{[}J{]}
+\item
+  HVAC,Average,Heating Coil Rate{[}W{]}
+\item
+  HVAC,Sum,Heating Coil Electric Consumption {[}J{]}
+\item
+  HVAC,Average,Heating Coil Electric Power {[}W{]}
+\end{itemize}
+
+\paragraph{Heating Coil Energy (J)}\label{heating-coil-energy-j}
+
+Heating Coil Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
+
+\paragraph{Heating Coil Rate{[}W{]}}\label{heating-coil-ratew}
+
+Heating Coil Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
+
+\paragraph{Heating Coil Electric Consumption {[}J{]}}\label{heating-coil-electric-consumption-j}
+
+Heating Coil electric consumption after the efficiency of the coil has been taken into account in Joules for the timestep reported.
+
+\paragraph{Heating Coil Electric Power {[}W{]}}\label{heating-coil-electric-power-w-1}
+
+This field is the average Heating Coil electric power after the efficiency of the coil has been taken into account in Watts for the timestep reported.
+
+\subsection{Coil:Heating:Desuperheater}\label{coilheatingdesuperheater}
+
+A simplified approach is used to determine the performance of this air heating coil. The model assumes that the heating energy provided by this coil is reclaimed from the superheated refrigerant gas leaving a compressor (i.e., a desuperheating refrigerant-to-air heating coil) and does not impact the performance of the compressor. This coil can be used in air loop simulations but can t be used by certain compound objects (e.g., AirLoopHVAC:UnitaryHeatPump:AirToAir, AirLoopHVAC:UnitaryHeatPump:WaterToAir, or Dehumidifier:Desiccant:NoFans) or any air distribution equipment (e.g., AirTerminal:SingleDuct:ConstantVolume:Reheat, AirTerminal:SingleDuct:VAV:Reheat, or AirTerminal:SingleDuct:SeriesPIU:Reheat).
+
+The desuperheater heating coil input requires a coil name, an availability schedule, and a heat reclaim recovery efficiency. The reclaim recovery efficiency determines the amount of heat available for use by this heating coil. Approximately 25-30\% of the energy rejected by typical refrigeration system condensers is to reduce the superheated refrigerant vapor temperature to the condensing temperature. Recovery efficiencies higher than 30\% may cause the refrigerant gas to condense which in turn impacts the performance of the refrigeration system. For this reason, the maximum heat reclaim recovery efficiency for this coil is 30\% for most sources of waste heat, including refrigeration compressor racks. The one exception to this 30\% limit is a condenser that is part of a detailed refrigeration system. In a detailed refrigeration system, the portion of the rejected heat that lies within the superheated region is explicitly calculated. Therefore, the desuperheater coils supplied by a condenser attached to a detailed refrigeration system are subject to a maximum reclaim recovery efficiency of 90\% of the heat within the superheated region.
+
+The next two input items for the desuperheater heating coil are the node names for the inlet and outlet air streams. The following two input fields define the source of heating energy for the coil. This desuperheater heating coil may only be used with direct expansion (DX) cooling or refrigeration equipment. The first of these two inputs is the heating source object type while the second defines the name of the heating source. For proper modeling, the desuperheater heating coil must be placed downstream of a DX cooling coil when reclaiming heat from that cooling coil. Desuperheating heating coil placement is unrestricted when reclaiming heat from a Refrigeration:CompressorRack or Refrigeration:Condenser.
+
+The next input field is optional and defines the set point node name if the desuperheater heating coil is to be controlled based on temperature. When a load-based control scheme is used, this field is left blank. A final optional input is used to model parasitic electric energy use of auxiliary equipment associated with the desuperheater heating coil (e.g., solenoid valve).
+
+\subsubsection{Inputs}\label{inputs-5-013}
+
+\paragraph{Field: Name}\label{field-name-5-009}
+
+This alpha field defines a unique user-assigned name for an instance of a desuperheater heating coil. Any reference to this desuperheater heating coil by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-009}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the desuperheater heating coil can run during a given time period. Schedule values must range from 0 to 1. A schedule value greater than 0 indicates that the coil can operate during the time period. A value equal to 0 denotes that the coil must be off for that time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Heat Reclaim Recovery Efficiency}\label{field-heat-reclaim-recovery-efficiency}
+
+This numeric field defines the ratio of recovered waste heat from the superheated refrigerant gas to the total rejected waste heat from the heating source (as if no heat reclaim occurred). Values can range from 0.0 up to a maximum of 0.9 if the source is a refrigeration condenser and 0.3 for all other waste heat sources. If this input field is left blank, the default value is 0.8 for a refrigeration condenser source type and 0.25 for all other sources.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-5-000}
+
+This alpha field defines the name of the HVAC system node from which the desuperheater heating coil draws its inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-5-000}
+
+This alpha field defines the name of the HVAC system node to which the desuperheater heating coil sends its outlet air.
+
+\paragraph{Field: Heating Source Object Type}\label{field-heating-source-object-type}
+
+This alpha field defines the source of superheated refrigerant gas from which the desuperheater heating coil recovers energy. Valid choices are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  Coil:Cooling:DX:TwoSpeed
+\item
+  Coil:Cooling:DX:TwoStageWithHumidityControlMode
+\item
+  Refrigeration:CompressorRack
+\item
+  Refrigeration:Condenser:AirCooled
+\item
+  Refrigeration:Condenser:EvaporativeCooled
+\item
+  Refrigeration:Condenser:WaterCooled
+\end{itemize}
+
+When the heating coil source is a DX Coil, the air loop s supply air fan control mode may be auto fan (cycling fan cycling coil), constant fan, or variable volume. When the heating source is a compressor rack for refrigerated cases or a refrigeration condenser, the supply air fan control mode should be either variable volume or constant fan.
+
+NOTE: Use of the desuperheater heating coil in variable air volume systems should be done with caution since the model assumption of a fixed heat reclaim recovery efficiency may not be valid if the air flow rate over the coil varies significantly.
+
+\paragraph{Field: Heating Source Name}\label{field-heating-source-name}
+
+This alpha field defines the name of the desuperheater heating coil source (e.g., the name of a specific valid coil (as mentioned in the previous field) which provides waste heat to this desuperheater heating coil).
+
+NOTE: When the heating source is a Refrigeration Compressor rack, the heat rejection location in the Refrigeration:CompressorRack object must be Outdoors . If the compressor rack heat rejection location is Zone , the total amount of heat rejection available for reclaim (e.g., by this desuperheater heating coil) is set to zero by the compressor rack object and the simulation proceeds.
+
+\paragraph{Field: Temperature Setpoint Node Name}\label{field-temperature-setpoint-node-name-3}
+
+This optional alpha field defines the name of the HVAC system node used for temperature-based control (e.g., controlling the heating coil s outlet air dry-bulb temperature to a setpoint). If the desuperheater heating coil is temperature controlled through the use of a Set Point Manager, then the control node specified in the Set Point Manager will be entered here. If the desuperheater heating coil is controlled based on a certain heating load to be met (e.g., using this heating coil as part of AirLoopHVAC:Unitary:Furnace:HeatCool for high humidity control), this field should be left blank.
+
+\paragraph{Field: Parasitic Electric Load}\label{field-parasitic-electric-load}
+
+This optional numeric field defines the parasitic electric load (in Watts) due to control valves or other devices specific to the desuperheater heating coil. The load is applied whenever the coil is heating the air. The model assumes that this electric load is small and does not contribute to heating the air.
+
+Following is an example input for a desuperheater heating coil.
+
+\begin{lstlisting}
+
+Coil:Heating:Desuperheater,
+  DesuperheaterCoil,                                   !- Coil Name
+  FanAndCoilAvailSched,                             !- Availability Schedule
+  0.3,                                                               !- Heat Reclaim Recovery Efficiency
+  Cooling Coil Air Outlet Node,             !- Coil Air Inlet Node Name
+  Air Loop Outlet Node,                             !- Coil Air Outlet Node Name
+  Coil:Cooling:DX:SingleSpeed, !- Heating Source Type
+  Furnace ACDXCoil 1,                                 !- Heating Source Name
+  ,                                                                     !- Coil Temperature Setpoint Node Name
+  0.1;                                                               !- Parasitic Electric Load {W}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-006}
+
+\begin{itemize}
+\item
+  HVAC,Average,Heating Coil Rate {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Electric Power {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Electric Consumption {[}J{]}
+\item
+  HVAC,Average,Heating Coil Runtime Fraction {[]}
+\item
+  HVAC,Average,Heating Coil Air Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Air Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Electric Power {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Runtime Fraction
+\end{itemize}
+
+\paragraph{Heating Coil Air Heating Rate {[}W{]}}\label{heating-coil-air-heating-rate-w-1}
+
+This output is the average heating rate of the desuperheater heating coil in Watts over the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Heating Coil Air Heating Energy {[}J{]}}\label{heating-coil-air-heating-energy-j-1}
+
+This output is the total heating output of the desuperheater heating coil in Joules over the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Electric Power {[}W{]}}\label{heating-coil-electric-power-w-2}
+
+This output is the average electric consumption rate for the parasitic load associated with the desuperheater heating coil in Watts.
+
+\paragraph{Heating Coil Electric Energy {[}J{]}}\label{heating-coil-electric-energy-j-1}
+
+This output is the electric consumption of the desuperheater heating coil parasitic load in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Heating Coil Runtime Fraction {[]}}{Heating Coil Runtime Fraction }}\label{heating-coil-runtime-fraction}
+
+This is the runtime fraction of the desuperheater heating coil for the timestep being reported. Since the desuperheater heating coil can only provide heat when the heat source object is active, the runtime fraction of the desuperheater heating coil will always be less than or equal to the runtime fraction of the heat source object.
+
+\subsection{Coil:Cooling:DX:VariableRefrigerantFlow}\label{coilcoolingdxvariablerefrigerantflow}
+
+The variable refrigerant flow (VRF) DX cooling coil model is nearly identical to the single-speed DX cooling coil model (Ref. Coil:Cooling:DX:SingleSpeed). For this reason, an adaptation of the single-speed DX cooling coil model is used to model the variable-speed compression system used in VRF AC systems. The model inputs are quite similar to the input requirements for the single-speed DX cooling coil model, however, the location of a majority of the inputs have been moved to the variable refrigerant flow air conditioner object since multiple DX cooling coils will use the same DX compression system (Ref. AirConditioner:VariableRefrigerantFlow).
+
+\subsubsection{Inputs}\label{inputs-6-010}
+
+\paragraph{Field: Coil Name}\label{field-coil-name-000}
+
+This alpha field defines a unique user-assigned name for an instance of a VRF DX cooling coil. Any reference to this DX cooling coil by another object will use this name. This cooling coil name must be entered in the AirConditioner:VariableRefrigerantFlow object. No other sytem type uses this specific coil.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-007}
+
+This alpha field defines the name of the DX cooling coil availabiltiy schedule. Schedule values of 0 denote the DX cooling coil is off. A schedule value greater than 0 indicates that the coil can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Gross Rated Total Cooling Capacity}\label{field-gross-rated-total-cooling-capacity}
+
+This numeric field defines the gross rated total cooling capacity of the DX cooling coil in watts. The total cooling capacity should be a gross , i.e., the effect of supply air fan heat NOT accounted for.
+
+\paragraph{Field: Gross Ratio Sensible Heat Ratio}\label{field-gross-ratio-sensible-heat-ratio}
+
+This numeric field defines the gross sensible heat ratio (sensible capacity divided by total cooling capacity) of the DX cooling coil at rated conditions. Both the sensible and total cooling capacities used to define the Rated SHR should be gross (i.e., the effect of supply air fan heat is NOT accounted for)
+
+\paragraph{Field: Rated Air Flow Rate}\label{field-rated-air-flow-rate}
+
+The air volume flow rate, in m\(^{3}\) per second, across the DX cooling coil at rated conditions. The rated air volume flow rate should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of rated total cooling capacity (300 to 450 cfm/ton). The gross rated total cooling capacity and gross rated SHR should be performance information for the unit with at this rated air volume flow rate.
+
+\paragraph{Field: Cooling Capacity Ratio Modifier Function of Temperature Curve Name}\label{field-cooling-capacity-ratio-modifier-function-of-temperature-curve-name}
+
+This alpha field defines the cooling capacity ratio modifier as a function of indoor wet-bulb temperature or indoor wet-bulb and outdoor dry-bulb temperatures. This curve is a linear, quadratic, or cubic curve if the cooling capacity is solely a function of indoor wet-bulb temperature (i.e., the indoor terminal units weighted average inlet air wet-bulb temperatures). Without specific manufacturers data indicating otherwise, the use of a single independent variable is recommended for this coil type. If, however, the user has reason to believe the cooling capacity is both a function of indoor wet-bulb temperature and outdoor dry-bulb temperature (and has manufacturers data to create the performance curve), a bi-quadratic equation using weighted average indoor wet-bulb temperature and condenser entering air dry-bulb temperature as the independent variables may be used. See the Engineering Reference for more discussion on using this input field.
+
+\paragraph{Field: Cooling Capacity Modifier Curve Function of Flow Fraction Name}\label{field-cooling-capacity-modifier-curve-function-of-flow-fraction-name}
+
+This alpha field defines the name of a linear, quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
+
+\paragraph{Field: Coil Air Inlet Node Name}\label{field-coil-air-inlet-node-name}
+
+This alpha field defines the name of the air inlet node entering the DX cooling coil.
+
+\paragraph{Field: Coil Air Outlet Node Name}\label{field-coil-air-outlet-node-name}
+
+This alpha field defines the name of the air outlet node exiting the DX cooling coil.
+
+\paragraph{Field: Name of Water Storage Tank for Condensate Collection}\label{field-name-of-water-storage-tank-for-condensate-collection}
+
+This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
+
+Following is an example input for a Coil:Cooling:DX:VariableRefrigerantFlow object.
+
+\begin{lstlisting}
+
+COIL:Cooling:DX:VariableRefrigerantFlow,
+  TU1 VRF DX Cooling Coil, !- Coil Name
+  VRFAvailSched,                     !- Availability Schedule Name
+  autosize,                               !- Gross Rated Total Cooling Capacity {W}
+  autosize,                               !- Gross Rated Sensible Heat Ratio
+  autosize,                               !- Rated Air Flow Rate {m3/s}
+  VRFTUCoolCapFT,                   !- Cooling Capacity Ratio Modifier Function of Temperature Curve Name
+  VRFACCoolCapFFF,                 !- Cooling Capacity Modifier Curve Function of Flow Fraction Name
+  TU1 VRF DX CCoil Inlet Node,   !- Coil Air Inlet Node
+  TU1 VRF DX CCoil Outlet Node;   !- Coil Air Outlet Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-003}
+
+\begin{itemize}
+\item
+  HVAC,Average, Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Cooling Coil Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Cooling Coil Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Cooling Coil Runtime Fraction {[]}
+\end{itemize}
+
+Evaporative-cooled condenser:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}
+\item
+  Zone,Meter,Condensate:OnSiteWater {[}m3{]}
+\item
+  HVAC,Sum,Cooling Coil Condensate Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Cooling Coil Total Cooling Rate {[}W{]}}\label{cooling-coil-total-cooling-rate-w-1}
+
+This field is the total (sensible and latent) cooling rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Total Cooling Energy {[}J{]}}\label{cooling-coil-total-cooling-energy-j-1}
+
+This is the total (sensible plus latent) cooling output of the DX coil in Joules over the time step being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = CoolingCoils, Group Key = System (Ref. Output:Meter objects).
+
+\paragraph{Cooling Coil Sensible Cooling Rate {[}W{]}}\label{cooling-coil-sensible-cooling-rate-w-1}
+
+This output is the moist air sensible cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Sensible Cooling Energy {[}J{]}}\label{cooling-coil-sensible-cooling-energy-j-1}
+
+This is the moist air sensible cooling output of the DX coil in Joules for the time step being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Latent Cooling Rate {[}W{]}}\label{cooling-coil-latent-cooling-rate-w}
+
+This is the latent cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Latent Cooling Energy {[}J{]}}\label{cooling-coil-latent-cooling-energy-j}
+
+This is the latent cooling output of the DX coil in Joules for the time step being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{\texorpdfstring{Cooling Coil Runtime Fraction {[]}}{Cooling Coil Runtime Fraction }}\label{cooling-coil-runtime-fraction}
+
+This is the runtime fraction of the DX coil compressor and condenser fan(s) for the time step being reported.
+
+\paragraph{Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}}\label{cooling-coil-condensate-volume-flow-rate-m3s-1}
+
+\paragraph{Cooling Coil Condensate Volume {[}m3{]}}\label{cooling-coil-condensate-volume-m3-1}
+
+These outputs are the rate and volume of water collected as condensate from the coil. These reports only appear if a water storage tank is named in the input object.
+
+\subsection{Coil:Heating:DX:VariableRefrigerantFlow}\label{coilheatingdxvariablerefrigerantflow}
+
+The variable refrigerant flow (VRF) DX heating coil model uses performance information at rated conditions along with performance curves for variations in total capacity, energy input ratio and part load fraction to determine performance at part-load conditions. The impacts of defrost operation is modeled based a combination of user inputs and empirical models taken from the air-to-air heat pump algorithms in DOE-2.1E.
+
+The VRF DX heating coil input requires an availability schedule, the gross rated heating capacity and the rated air volume flow rate. The rated air volume flow rate should be between 0.00008056 m\(^{3}\)/s and 0.00002684 m\(^{3}\)/s per watt of gross rated heating capacity.
+
+Two performance curves are required. The first performance curve defines the heating capacity as a function of indoor air dry-bulb and outdoor condenser entering air wet-bulb temperature. This curve object is specified in the variable refrigerant flow air-to-air heat pump object. The second performance curve is specific the each VRF DX heating coil and defines the change in heating capacity as a function of air flow fraction. Each of these performance curves are further discussed here.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\tightlist
+\item
+  Heating capacity modifier curve (function of temperature, specified in Heat Pump)
+\end{enumerate}
+
+The heating capacity modifier curve (function of temperature) can be a function of both the outdoor wet-bulb temperature and indoor air dry-bulb temperature. Users have the choice of a bi-quadratic curve with two independent variables or a tri-quadratic curve with three independent variable. The tri-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the combined total capacity of all indoor units connected to the heat pump condenser and a more realistic output. The output of this curve is multiplied by the gross rated heating capacity to give the gross heating capacity at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature) and the combination ratio of the installed system.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Heating capacity modifier curve (function of flow fraction, specified in DX coil)
+\end{enumerate}
+
+The heating capacity modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating.
+
+\subsubsection{Inputs}\label{inputs-7-010}
+
+\paragraph{Field: Name}\label{field-name-6-007}
+
+This alpha field defines a unique user-assigned name for an instance of a VRF DX heating coil. Any reference to this DX heating coil by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-2-004}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the DX heating coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Gross Rated Heating Capacity}\label{field-gross-rated-heating-capacity-1}
+
+This numeric field defines the total, full load gross heating capacity in watts of the DX coil unit at rated conditions (outside air dry-bulb temperature of 8.33 C, outside air wet-bulb temperature of 6.11 C, heating coil entering air dry-bulb temperature of 21.11 C, heating coil entering air wet-bulb temperature of 15.55 C, and a heating coil air flow rate defined by field rated air flow volume below). The value entered here must be greater than 0. The gross total heating capacity should not account for the effect of supply air fan heat.
+
+\paragraph{Field: Rated Air Flow Rate}\label{field-rated-air-flow-rate-1}
+
+This numeric field defines the volume air flow rate, in m\(^{3}\) per second, across the DX heating coil at rated conditions. The value entered here must be greater than 0. The rated air volume flow rate should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of gross rated heating capacity. The gross rated heating capacity and the gross rated COP should be performance information for the unit with outside air dry-bulb temperature of 8.33 C, outside air wet-bulb temperature of 6.11 C, heating coil entering air dry-bulb temperature of 21.11 C, heating coil entering air wet-bulb temperature of 15.55 C, and the rated air volume flow rate defined here.
+
+\paragraph{Field: Coil Air Inlet Node}\label{field-coil-air-inlet-node}
+
+This alpha field defines the name of the HVAC system node from which the DX heating coil draws its inlet air.
+
+\paragraph{Field: Coil Air Outlet Node}\label{field-coil-air-outlet-node}
+
+This alpha field defines the name of the HVAC system node to which the DX heating coil sends its outlet air.
+
+\paragraph{Field: Heating Capacity Ratio Modifier Function of Temperature Curve Name}\label{field-heating-capacity-ratio-modifier-function-of-temperature-curve-name}
+
+This alpha field defines the heating capacity ratio modifier as a function of indoor dry-bulb temperature or indoor dry-bulb and outdoor wet-bulb temperatures. This curve is a linear, quadratic, or cubic curve if the heating capacity is solely a function of indoor dry-bulb temperature (i.e., the indoor terminal units weighted average inlet air dry-bulb temperatures). Without specific manufacturers data indicating otherwise, the use of a single independent variable is recommended for this coil type. If, however, the user has reason to believe the heating capacity is both a function of indoor dry-bulb temperature and outdoor wet-bulb temperature (and has manufacturers data to create the performance curve), a bi-quadratic equation using weighted average indoor dry-bulb temperature and condenser entering air wet-bulb temperature as the independent variables may be used. See the Engineering Reference for more discussion on using this input field.
+
+Note: The choice of using either outdoor dry-bulb temperature or outdoor wet-bulb temperature as the independent variable in this performance curve is set in the parent object AirConditioner: VariableRefrigerantFlow.
+
+\paragraph{Field: Heating Capacity Ratio Modifier Function of Flow Fraction Curve Name}\label{field-heating-capacity-ratio-modifier-function-of-flow-fraction-curve-name}
+
+This alpha field defines the name of a linear, quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of heating capacity as a function of the ratio of actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
+
+Following is an example input for the object.
+
+\begin{lstlisting}
+
+COIL:Heating:DX:VariableRefrigerantFlow,
+  TU1 VRF DX Heating Coil, !- Coil Name
+  VRFAvailSched,                     !- Availability Schedule
+  autosize,                               !- Gross Rated Heating Capacity {W}
+  autosize,                               !- Rated Air Flow Rate {m3/s}
+  TU1 VRF DX CCoil Outlet Node,   !- Coil Air Inlet Node
+  TU1 VRF DX HCoil Outlet Node,   !- Coil Air Outlet Node
+  VRFTUHeatCapFT,                   !- Heating Capacity Ratio Modifier Function of Temperature Curve Name
+  VRFACCoolCapFFF;                 !- Total heating capacity modifier curve Function of Flow Fraction
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-003}
+
+\begin{itemize}
+\item
+  HVAC,Average, Heating Coil Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum, Heating Coil Total Heating Energy {[}J{]}
+\item
+  HVAC,Average, Heating Coil Runtime Fraction {[]}
+\end{itemize}
+
+\paragraph{Heating Coil Total Heating Rate {[}W{]}}\label{heating-coil-total-heating-rate-w}
+
+This field is the total heating rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Heating Coil Total Heating Energy {[}J{]}}\label{heating-coil-total-heating-energy-j}
+
+This is the total heating output of the DX coil in Joules over the time step being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Heating Coil Runtime Fraction {[]}}{Heating Coil Runtime Fraction }}\label{heating-coil-runtime-fraction-1}
+
+This is the runtime fraction of the DX coil compressor and condenser fan(s) for the time step being reported.
+
+\subsection{Coil:Cooling:DX:VariableRefrigerantFlow:FluidTemperatureControl}\label{coilcoolingdxvariablerefrigerantflowfluidtemperaturecontrol}
+
+This coil object is specifically designed for the physics based VRF model applicable for Fluid Temperature Control (VRF-FluidTCtrl). It describes the performance of the indoor unit coil of the VRF system operating at cooling mode. The name of this object is entered as an input to the object \emph{ZoneHVAC:TerminalUnit:VariableRefrigerantFlow}. The outdoor unit part of the VRF system is modeled separately (refer to \emph{AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl} object).
+
+\subsubsection{Inputs}\label{inputs-8-008}
+
+\paragraph{Field: Name}\label{field-name-7-006}
+
+This alpha field defines a unique user-assigned name for an instance of a VRF DX cooling coil. Any reference to this DX cooling coil by another object will use this name. This cooling coil name must be entered in the AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl object. No other system type uses this specific coil.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-3-003}
+
+This alpha field defines the name of the coil availability schedule. A name should be entered to define the availability of the coil. Schedule values of 0 denote the DX cooling coil is off. A schedule value greater than 0 indicates that the coil can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Coil Air Inlet Node}\label{field-coil-air-inlet-node-1}
+
+This alpha field defines the name of the air inlet node entering the DX cooling coil.
+
+\paragraph{Field: Coil Air Outlet Node}\label{field-coil-air-outlet-node-1}
+
+This alpha field defines the name of the air outlet node exiting the DX cooling coil.
+
+\paragraph{Field: Rated Total Cooling Capacity}\label{field-rated-total-cooling-capacity}
+
+This numeric field defines the gross rated total cooling capacity of the DX cooling coil in watts. The total cooling capacity should be a gross , i.e., the effect of supply air fan heat NOT accounted for.
+
+\paragraph{Field: Rated Sensible Heat Ratio}\label{field-rated-sensible-heat-ratio}
+
+This numeric field defines the gross sensible heat ratio (sensible capacity divided by total cooling capacity) of the DX cooling coil at rated conditions. Both the sensible and total cooling capacities used to define the Rated SHR should be gross (i.e., the effect of supply air fan heat is NOT accounted for)
+
+\paragraph{Field: Indoor Unit Reference Superheating}\label{field-indoor-unit-reference-superheating}
+
+This numeric field defines the reference superheating degrees of the indoor unit. If this field is blank, the default value of 5.0 C is used.
+
+\paragraph{Field: Indoor Unit Evaporating Temperature Function of Superheating Curve Name}\label{field-indoor-unit-evaporating-temperature-function-of-superheating-curve-name}
+
+This alpha field defines the name of a quadratic performance curve that parameterizes the variation of indoor unit evaporating temperature as a function of superheating degrees. The output of this curve is the temperature difference between the coil surface air temperature and the evaporating temperature.
+
+\paragraph{Field: Name of Water Storage Tank for Condensate Collection}\label{field-name-of-water-storage-tank-for-condensate-collection-1}
+
+This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
+
+Following is an example input for a Coil:Cooling:DX:VariableRefrigerantFlow:FluidTemperatureControl object.
+
+\begin{lstlisting}
+
+Coil:Cooling:DX:VariableRefrigerantFlow:FluidTemperatureControl,
+  TU1 VRF DX Cooling Coil, !- Name
+  VRFAvailSched,           !- Availability Schedule Name
+  TU1 VRF DX CCoil Inlet Node,  !- Coil Air Inlet Node
+  TU1 VRF DX CCoil Outlet Node,  !- Coil Air Outlet Node
+  autosize,                !- Rated Total Cooling Capacity {W}
+  autosize,                !- Rated Sensible Heat Ratio
+  3,                       !- Indoor Unit Reference Superheating Degrees {C}    
+  IUEvapTempCurve,         !- Indoor Unit Evaporating Temperature Function of Superheating Curve Name    
+  ;                        !- Name of Water Storage Tank for Condensate Collection
+
+  Curve:Quadratic,
+  IUEvapTempCurve,         !- Name
+  0,                       !- Coefficient1 Constant
+  0.843,                   !- Coefficient2 x
+  0,                       !- Coefficient3 x**2
+  0,                       !- Minimum Value of x    
+  15,                      !- Maximum Value of x    
+  ,                        !- Minimum Curve Output
+  ,                        !- Maximum Curve Output
+  Temperature,             !- Input Unit Type for X
+  Temperature;             !- Output Unit Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-003}
+
+\begin{itemize}
+\item
+  HVAC,Average, Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Cooling Coil Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Cooling Coil Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Cooling Coil Runtime Fraction {[]}
+\item
+  HVAC,Average, Cooling Coil VRF Evaporating Temperature {[}C{]}
+\item
+  HVAC,Average, Cooling Coil VRF Super Heating Degrees {[}C{]}
+\end{itemize}
+
+Evaporative-cooled condenser:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}
+\item
+  Zone,Meter,Condensate:OnSiteWater {[}m3{]}
+\item
+  HVAC,Sum,Cooling Coil Condensate Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Cooling Coil Total Cooling Rate {[}W{]}}\label{cooling-coil-total-cooling-rate-w-2}
+
+This field is the total (sensible and latent) cooling rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Total Cooling Energy {[}J{]}}\label{cooling-coil-total-cooling-energy-j-2}
+
+This is the total (sensible plus latent) cooling output of the DX coil in Joules over the time step being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = CoolingCoils, Group Key = System (Ref. Output:Meter objects).
+
+\paragraph{Cooling Coil Sensible Cooling Rate {[}W{]}}\label{cooling-coil-sensible-cooling-rate-w-2}
+
+This output is the moist air sensible cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Sensible Cooling Energy {[}J{]}}\label{cooling-coil-sensible-cooling-energy-j-2}
+
+This is the moist air sensible cooling output of the DX coil in Joules for the time step being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Latent Cooling Rate {[}W{]}}\label{cooling-coil-latent-cooling-rate-w-1}
+
+This is the latent cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Latent Cooling Energy {[}J{]}}\label{cooling-coil-latent-cooling-energy-j-1}
+
+This is the latent cooling output of the DX coil in Joules for the time step being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{\texorpdfstring{Cooling Coil Runtime Fraction {[]}}{Cooling Coil Runtime Fraction }}\label{cooling-coil-runtime-fraction-1}
+
+This is the runtime fraction of the DX coil compressor and condenser fan(s) for the time step being reported.
+
+\paragraph{Cooling Coil VRF Evaporating Temperature {[}C{]}}\label{cooling-coil-vrf-evaporating-temperature-c}
+
+This is the evaporating temperature of the VRF system operating at cooling mode. This value is manipulated by the VRF system considering the load conditions of all the zones it serves. It affects the cooling coil surface temperature and thus the cooling capacity of the coil.
+
+\paragraph{Cooling Coil VRF Super Heating Degrees {[}C{]}}\label{cooling-coil-vrf-super-heating-degrees-c}
+
+This is the super heating degrees of the VRF system operating at cooling mode. This value is manipulated by each VRF terminal unit to adjust the cooling capacity of the coil considering the load conditions of the zone. It affects the cooling coil surface temperature and thus the cooling capacity of the coil.
+
+\paragraph{Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}}\label{cooling-coil-condensate-volume-flow-rate-m3s-2}
+
+This is the volumetric rate of water collected as condensate from the coil. This report only appears if a water storage tank is named in the input object.
+
+\paragraph{Cooling Coil Condensate Volume {[}m3{]}}\label{cooling-coil-condensate-volume-m3-2}
+
+This is the volume of water collected as condensate from the coil. This report only appears if a water storage tank is named in the input object.
+
+\subsection{Coil:Heating:DX:VariableRefrigerantFlow:FluidTemperatureControl}\label{coilheatingdxvariablerefrigerantflowfluidtemperaturecontrol}
+
+This coil object is specifically designed for the physics based VRF model applicable for Fluid Temperature Control (VRF-FluidTCtrl). It describes the performance of the indoor unit coil of the VRF system operating at heating mode. The name of this object is entered as an input to the object \emph{ZoneHVAC:TerminalUnit:VariableRefrigerantFlow}. The outdoor unit part of the VRF system is modeled separately (refer to \emph{AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl} object).
+
+\subsubsection{Inputs}\label{inputs-9-007}
+
+\paragraph{Field: Name}\label{field-name-8-006}
+
+This alpha field defines a unique user-assigned name for an instance of a VRF DX heating coil. Any reference to this DX heating coil by another object will use this name. This heating coil name must be entered in the AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl object. No other system type uses this specific coil.
+
+\paragraph{Field: Availability Schedule}\label{field-availability-schedule}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the DX heating coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank the unit is always available.
+
+\paragraph{Field: Coil Air Inlet Node}\label{field-coil-air-inlet-node-2}
+
+This alpha field defines the name of the HVAC system node from which the DX heating coil draws its inlet air.
+
+\paragraph{Field: Coil Air Outlet Node}\label{field-coil-air-outlet-node-2}
+
+This alpha field defines the name of the HVAC system node to which the DX heating coil sends its outlet air.
+
+\paragraph{Field: Rated Total Heating Capacity}\label{field-rated-total-heating-capacity}
+
+This numeric field defines the total, full load gross heating capacity in watts of the DX coil unit at rated conditions. The value entered here must be greater than 0. The gross total heating capacity should not account for the effect of supply air fan heat.
+
+\paragraph{Field: Indoor Unit Reference Subcooling}\label{field-indoor-unit-reference-subcooling}
+
+This numeric field defines the reference subcooling degrees of the indoor unit. If this field is blank, the default value of 5.0 C is used.
+
+\paragraph{Field: Indoor Unit Condensing Temperature Function of Subcooling Curve Name}\label{field-indoor-unit-condensing-temperature-function-of-subcooling-curve-name}
+
+This alpha field defines the name of a quadratic performance curve that parameterizes the variation of indoor unit condensing temperature as a function of subcooling degrees. The output of this curve is the temperature difference between the condensing temperature and the coil surface air temperature.
+
+Following is an example input for a Coil:Heating:DX:VariableRefrigerantFlow:FluidTemperatureControl object.
+
+\begin{lstlisting}
+
+Coil:Heating:DX:VariableRefrigerantFlow:FluidTemperatureControl,
+  TU1 VRF DX Heating Coil, !- Name
+  VRFAvailSched,           !- Availability Schedule
+  TU1 VRF DX CCoil Outlet Node,  !- Coil Air Inlet Node
+  TU1 VRF DX HCoil Outlet Node,  !- Coil Air Outlet Node
+  autosize,                !- Rated Total Heating Capacity {W}
+  5,                       !- Indoor Unit Reference Subcooling Degrees {C}    
+  IUCondTempCurve;         !- Indoor Unit Condensing Temperature Function of Subcooling Curve Name
+
+  Curve:Quadratic,
+  IUCondTempCurve,         !- Name
+  -1.85,                   !- Coefficient1 Constant
+  0.411,                   !- Coefficient2 x
+  0.0196,                  !- Coefficient3 x**2
+  0,                       !- Minimum Value of x    
+  20,                      !- Maximum Value of x    
+  ,                        !- Minimum Curve Output
+  ,                        !- Maximum Curve Output
+  Temperature,             !- Input Unit Type for X
+  Temperature;             !- Output Unit Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8-002}
+
+\begin{itemize}
+\item
+  HVAC,Average, Heating Coil Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum, Heating Coil Total Heating Energy {[}J{]}
+\item
+  HVAC,Average, Heating Coil Runtime Fraction {[]}
+\item
+  Heating Coil VRF Condensing Temperature {[}C{]}
+\item
+  Heating Coil VRF Subcooling Degrees {[}C{]}
+\end{itemize}
+
+\paragraph{Heating Coil Total Heating Rate {[}W{]}}\label{heating-coil-total-heating-rate-w-1}
+
+This field is the total heating rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Heating Coil Total Heating Energy {[}J{]}}\label{heating-coil-total-heating-energy-j-1}
+
+This is the total heating output of the DX coil in Joules over the time step being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Heating Coil Runtime Fraction {[]}}{Heating Coil Runtime Fraction }}\label{heating-coil-runtime-fraction-2}
+
+This is the runtime fraction of the DX coil compressor and condenser fan(s) for the time step being reported.
+
+\paragraph{Cooling Coil VRF Condensing Temperature {[}C{]}}\label{cooling-coil-vrf-condensing-temperature-c}
+
+This is the condensing temperature of the VRF system operating at heating mode. This value is manipulated by the VRF system considering the load conditions of all the zones it serves. It affects the heating coil surface temperature and thus the heating capacity of the coil.
+
+\paragraph{Cooling Coil VRF Subcooling Degrees {[}C{]}}\label{cooling-coil-vrf-subcooling-degrees-c}
+
+This is the subcooling degrees of the VRF system operating at heating mode. This value is manipulated by each VRF terminal unit to adjust the heating capacity of the coil considering the load conditions of the zone. It affects the heating coil surface temperature and thus the heating capacity of the coil.
+
+\subsection{Coil:Heating:Gas}\label{coilheatinggas-000}
+
+The gas heating coil is a simple capacity model with a user inputted gas burner efficiency. The default for the gas burner efficiency is 80\%. This coil will be simpler than shown in Figure~\ref{fig:example-air-loop-heating-cooling-coil} since it will only have air nodes to connect it in the system. The coil can be used in the air loop simulation or in the zone equipment as a reheat coil. Depending on where it is used determines if this coil is temperature or capacity controlled. If used in the air loop simulation it will be controlled to a specified temperature scheduled from the Setpoint Manager. If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand.
+
+\subsubsection{Inputs}\label{inputs-10-006}
+
+\paragraph{Field: Name}\label{field-name-9-006}
+
+A unique identifying name for each coil.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-4-003}
+
+Schedule that defines when the coil is available. If the schedule s value is 0.0, then the coil is not available and flow will not be requested. If the schedule s value is \textgreater{} 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods. Schedule values must be \textgreater{} = 0 and \textless{} = 1.
+
+\paragraph{Field: Gas Burner Efficiency}\label{field-gas-burner-efficiency}
+
+This is user inputted gas burner efficiency (decimal, not percent) and is defaulted to 80\%.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-1-000}
+
+This is the maximum capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-6}
+
+The name of the air inlet to the gas coil, i.e.~Heating Coil Air Inlet Node.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-6-000}
+
+The name of the air outlet from the gas coil, i.e.~Heating Coil Air Outlet Node.
+
+\paragraph{Field: Temperature Setpoint Node Name}\label{field-temperature-setpoint-node-name-4}
+
+If the coil is used in the air loop simulation and is temperature controlled using a Set Point Manager, then the node that is the control node needs to be specified here. If the coil is used in an air terminal unit, the coil is load controlled and a control node set point is not required.
+
+\paragraph{Field: Parasitic Electric Load}\label{field-parasitic-electric-load-1}
+
+This is the parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.. This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation timestep.
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of gas consumption rate by the heating coil as a function of the part load ratio (PLR, sensible heating load/nominal capacity of the heating coil). For any simulation timestep, the nominal gas consumption rate (heating load/burner efficiency) is divided by the part-load fraction (PLF) if a part-load curve has been defined. The part-load curve accounts for efficiency losses due to transient coil operation.
+
+The part-load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the heating coil runs continuously for the simulation timestep). For PLR values between 0 and 1 ( 0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the heating coil is defined a PLR/PLF. If PLF \textless{} PLR, then a warning message is issues and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional gas heating coil (e.g., residential furnace) would be:
+
+\begin{lstlisting}
+       PLF = 0.8 + 0.2(PLR)
+\end{lstlisting}
+
+\paragraph{Field: Parasitic Gas Load}\label{field-parasitic-gas-load}
+
+This numeric field is the parasitic gas load associated with the gas coil s operation (Watts), such as a standing pilot light. The model assumes that this parasitic load is consumed only for the portion of the simulation timestep where the gas heating coil is not operating.
+
+\subsubsection{Outputs}\label{outputs-9-002}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Heating Coil Air Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Air Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Gas Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Gas Rate {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Electric Power {[}W{]}
+\item
+  HVAC,Average,Heating Coil Runtime Fraction {[]}
+\item
+  HVAC,Sum,Heating Coil Ancillary Gas Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Ancillary Gas Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Heating Coil Air Heating Energy {[}J{]}}\label{heating-coil-air-heating-energy-j-2}
+
+This field is the total heating output of the coil in Joules over the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Air Heating Rate {[}W{]}}\label{heating-coil-air-heating-rate-w-2}
+
+This field is the average heating rate output of the coil in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Gas Energy {[}J{]}}\label{heating-coil-gas-energy-j}
+
+This field is the gas consumption of the heating coil in Joules over the timestep being reported, including the impacts of part-load performance if a part load fraction correlation is specified. This output is also added to a meter with Resource Type = Gas, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Gas Rate {[}W{]}}\label{heating-coil-gas-rate-w}
+
+This field is the average gas consumption rate of the coil in Watts over the timestep being reported, including the impacts of part-load performance if a part load fraction correlation is specified.
+
+\paragraph{Heating Coil Electric Energy {[}J{]}}\label{heating-coil-electric-energy-j-2}
+
+This field is the electric consumption of the heating coil auxiliaries in Joules over the timestep being reported (e.g., inducer fan). This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Electric Power {[}W{]}}\label{heating-coil-electric-power-w-3}
+
+This field is the average electric consumption rate of the heating coil auxiliaries (e.g., inducer fan) in Watts over the timestep being reported.
+
+\paragraph{\texorpdfstring{Heating Coil Runtime Fraction {[]}}{Heating Coil Runtime Fraction }}\label{heating-coil-runtime-fraction-3}
+
+This field is the runtime fraction of the coil over the timestep being reported.
+
+\paragraph{Heating Coil Ancillary Gas Energy {[}J{]}}\label{heating-coil-ancillary-gas-energy-j}
+
+This field is the parasitic gas consumption of the heating coil in Joules over the timestep being reported (e.g., standing pilot light). The model assumes that the parasitic load is accumulated only for the portion of the simulation timestep where the gas heating coil is not operating. This output is also added to a meter with Resource Type = Gas, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Ancillary Gas Rate {[}W{]}}\label{heating-coil-ancillary-gas-rate-w}
+
+This field is the average parasitic gas consumption rate of the heating coil (e.g., standing pilot light) in Watts over the timestep being reported. The model assumes that the parasitic load is present only for the portion of the simulation timestep where the gas heating coil is not operating.
+
+\subsection{Coil:Heating:Gas:MultiStage}\label{coilheatinggasmultistage}
+
+The multi stage gas heating coil is a simple capacity model with a user inputted gas burner efficiencies at different stages. This coil will only have air nodes to connect it in the system. The coil can be used in the air loop simulation or in the zone equipment as a reheat coil. Depending on where it is used determines if this coil is temperature or capacity controlled. If used in the air loop simulation it will be controlled to a specified temperature scheduled from the Setpoint Manager. If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand. For the time being, this coil model can only be called by the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
+
+\subsubsection{Inputs}\label{inputs-11-005}
+
+\paragraph{Field: Name}\label{field-name-10-005}
+
+A unique identifying name for each coil.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-5-001}
+
+Schedule that defines when the coil is available. If the schedule s value is 0.0, then the coil is not available and flow will not be requested. If the schedule s value is \textgreater{} 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods. Schedule values must be \textgreater{} = 0 and \textless{} = 1.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-7}
+
+The name of the air inlet to the gas coil, i.e.~Heating Coil Air Inlet Node.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-7-000}
+
+The name of the air outlet from the gas coil, i.e.~Heating Coil Air Outlet Node.
+
+\paragraph{Field: Temperature Setpoint Node Name}\label{field-temperature-setpoint-node-name-5}
+
+If the coil is used in the air loop simulation and is temperature controlled using a Set Point Manager, then the node that is the control node needs to be specified here. If the coil is used in an air terminal unit, the coil is load controlled and a control node set point is not required. At present, the multistage gas heating coil does not model temperature setoint control.
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-1}
+
+This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of gas consumption rate by the heating coil as a function of the part load ratio (PLR, sensible heating load/nominal capacity of the heating coil). For any simulation timestep, the nominal gas consumption rate (heating load/burner efficiency) is divided by the part-load fraction (PLF) if a part-load curve has been defined. The part-load curve accounts for efficiency losses due to transient coil operation.
+
+The part-load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the heating coil runs continuously for the simulation timestep). For PLR values between 0 and 1 ( 0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the heating coil is defined a PLR/PLF. If PLF \textless{} PLR, then a warning message is issues and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional gas heating coil (e.g., residential furnace) would be:
+
+\begin{lstlisting}
+       PLF = 0.8 + 0.2(PLR)
+\end{lstlisting}
+
+\paragraph{Field: Parasitic Gas Load}\label{field-parasitic-gas-load-1}
+
+This numeric field is the parasitic gas load associated with the gas coil s operation (Watts), such as a standing pilot light. The model assumes that this parasitic load is consumed only for the portion of the simulation timestep where the gas heating coil is not operating.
+
+\paragraph{Field: Stage 1 Gas Burner Efficiency}\label{field-stage-1-gas-burner-efficiency}
+
+This is user inputted stage 1 gas burner efficiency (decimal, not percent) and is defaulted to 80\%.
+
+\paragraph{Field: Stage 1 Nominal Capacity}\label{field-stage-1-nominal-capacity-1}
+
+This is the stage 1 capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
+
+\paragraph{Field: Stage 1 Parasitic Electric Load}\label{field-stage-1-parasitic-electric-load}
+
+This is the stage 1 parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.. This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation timestep.
+
+\paragraph{Field: Stage 2 Gas Burner Efficiency}\label{field-stage-2-gas-burner-efficiency}
+
+This is user inputted stage 2 gas burner efficiency (decimal, not percent) and is defaulted to 80\%.
+
+\paragraph{Field: Stage 2 Nominal Capacity}\label{field-stage-2-nominal-capacity-1}
+
+This is the stage 2 capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
+
+\paragraph{Field: Stage 2 Parasitic Electric Load}\label{field-stage-2-parasitic-electric-load}
+
+This is the stage 2 parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.. This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation timestep.
+
+\paragraph{Field: Stage 3 Gas Burner Efficiency}\label{field-stage-3-gas-burner-efficiency}
+
+This is user inputted stage 3 gas burner efficiency (decimal, not percent) and is defaulted to 80\%.
+
+\paragraph{Field: Stage 3 Nominal Capacity}\label{field-stage-3-nominal-capacity-1}
+
+This is the stage 3 capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
+
+\paragraph{Field: Stage 3 Parasitic Electric Load}\label{field-stage-3-parasitic-electric-load}
+
+This is the stage 3 parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.. This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation timestep.
+
+\paragraph{Field: Stage 4 Gas Burner Efficiency}\label{field-stage-4-gas-burner-efficiency}
+
+This is user inputted stage 4 gas burner efficiency (decimal, not percent) and is defaulted to 80\%.
+
+\paragraph{Field: Stage 4 Nominal Capacity}\label{field-stage-4-nominal-capacity-1}
+
+This is the stage 4 capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
+
+\paragraph{Field: Stage 4 Parasitic Electric Load}\label{field-stage-4-parasitic-electric-load}
+
+This is the stage 4 parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.. This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation timestep.
+
+An example in IDF form:
+
+\begin{lstlisting}
+
+Coil:Heating:Gas:MultiStage,
+  Heat Pump Heating Coil 1,                 !- Name
+  FanAndCoilAvailSched,                         !- Availability Schedule Name
+  Heating Coil Air Inlet Node,           !- Air Inlet Node Name
+  SuppHeating Coil Air Inlet Node,   !- Air Outlet Node Name
+  ,                                               !- Temp Setpoint node name
+  ,                                               !- Part Load Fraction Correlation Curve Name
+  ,                                               !- Parasitic Gas Load
+  3,                                             !- Number of Speeds
+  0.92,                                       !- Speed 1 Gas burner Efficiency
+  Autosize,                               !- Speed 1 Nominal Capacity {W}
+  ,                                               !- Stage 1 Parasitic Electric Load {W}
+  0.88,                                       !- Speed 2 Gas burner Efficiency
+  Autosize,                               !- Speed 2 Nominal Capacity {W}
+  ,                                               !- Stage 2 Parasitic Electric Load {W}
+  0.84,                                       !- Speed 3 Gas burner Efficiency
+  Autosize,                               !- Speed 3 Nominal Capacity {W}
+  ;                                               !- Stage 3 Parasitic Electric Load {W}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-10-002}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Heating Coil Energy{[}J{]}
+\item
+  HVAC,Average,Heating Coil Rate{[}W{]}
+\item
+  HVAC,Sum,Heating Coil Gas Consumption {[}J{]}
+\item
+  HVAC,Average,Heating Coil Gas Consumption Rate {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Electric Consumption {[}J{]}
+\item
+  HVAC,Average,Heating Coil Electric Power {[}W{]}
+\item
+  HVAC,Average,Heating Coil Runtime Fraction
+\item
+  HVAC,Sum,Heating Coil Parasitic Gas Consumption {[}J{]}
+\item
+  HVAC,Average,Heating Coil Parasitic Gas Consumption Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Heating Coil Energy {[}J{]}}\label{heating-coil-energy-j-1}
+
+This field is the total heating output of the coil in Joules over the timestep being reported. This output is also added to an output meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Rate {[}W{]}}\label{heating-coil-rate-w}
+
+This field is the average heating rate output of the coil in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Gas Consumption {[}J{]}}\label{heating-coil-gas-consumption-j}
+
+This field is the gas consumption of the heating coil in Joules over the timestep being reported, including the impacts of part-load performance if a part load fraction correlation is specified. This output is also added to an output meter with Resource Type = Gas, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Gas Consumption Rate {[}W{]}}\label{heating-coil-gas-consumption-rate-w}
+
+This field is the average gas consumption rate of the coil in Watts over the timestep being reported, including the impacts of part-load performance if a part load fraction correlation is specified.
+
+\paragraph{Heating Coil Electric Consumption {[}J{]}}\label{heating-coil-electric-consumption-j-1}
+
+This field is the electric consumption of the heating coil auxiliaries in Joules over the timestep being reported (e.g., inducer fan). This output is also added to an output meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Electric Power {[}W{]}}\label{heating-coil-electric-power-w-4}
+
+This field is the average electric consumption rate of the heating coil auxiliaries (e.g., inducer fan) in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Parasitic Gas Consumption {[}J{]}}\label{heating-coil-parasitic-gas-consumption-j}
+
+This field is the parasitic gas consumption of the heating coil in Joules over the timestep being reported (e.g., standing pilot light). The model assumes that the parasitic load is accumulated only for the portion of the simulation timestep where the gas heating coil is not operating. This output is also added to an output meter with Resource Type = Gas, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Parasitic Gas Consumption Rate {[}W{]}}\label{heating-coil-parasitic-gas-consumption-rate-w}
+
+This field is the average parasitic gas consumption rate of the heating coil (e.g., standing pilot light) in Watts over the timestep being reported. The model assumes that the parasitic load is present only for the portion of the simulation timestep where the gas heating coil is not operating.
+
+\subsection{Coil:Cooling:Water:DetailedGeometry}\label{coilcoolingwaterdetailedgeometry}
+
+This detailed flat fin coil model is for continuous plate fins. First, found in Type 12 from MODSIM, but now programmed directly from Elmahdy, A.H. and Mitalas, G.P. Then there was a discontinuity in their original model that was fixed in the EnergyPlus implementation. Now this model can be used in an interval halving solution technique for controlling this coil without the problems of non-convergence.
+
+``A Model for Cooling and Dehumidifying Coils for Use in Energy Requirements for Buildings'' ASHRAE Transactions, Vol. 83, Part 2, pp.~103-117 (1977). For fin efficiency see K.A. Gardner, ``Efficiency of Extended ,'' Transactions ASME, Vol. 67, pp.~621-631, 1945.
+
+The following figures illustrate the geometry and circuits in a cooling coil.
+
+\begin{figure}[hbtp] % fig 136
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image353.png}
+\caption{Geometry of a Cooling Coil (CC) \protect \label{fig:geometry-of-a-cooling-coil-cc}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 137
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image354.png}
+\caption{Number of Coolant Circuits (CCNCC) \protect \label{fig:number-of-coolant-circuits-ccncc}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-12-005}
+
+\paragraph{Field: Name}\label{field-name-11-004}
+
+A unique identifying name for each coil.
+
+\paragraph{Field:Availability Schedule Name}\label{fieldavailability-schedule-name-5}
+
+Schedule that defines when the coil is available. If the schedule s value is 0.0, then the coil is not available and flow will not be requested. If the schedule s value is \textgreater{} 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Maximum Water Flow Rate}\label{field-maximum-water-flow-rate-1}
+
+The maximum possible water flow rate (m\(^{3}\)/sec) through the coil.
+
+\paragraph{Field: Tube Outside Surface Area}\label{field-tube-outside-surface-area}
+
+The outside surface area (m\(^{2}\)) of the tubes that is exposed to air (i.e.~the outside area of the unfinned tubes minus the area of tubes covered by the fins).
+
+\paragraph{Field: Total Tube Inside Area}\label{field-total-tube-inside-area}
+
+The total surface area (m\(^{2}\)) inside the tubes (water side).
+
+\paragraph{Field: Fin Surface Area}\label{field-fin-surface-area}
+
+The total surface area (m\(^{2}\)) of the fins attached to the coil.
+
+\paragraph{Field: Minimum Air Flow Area}\label{field-minimum-air-flow-area}
+
+The minimum cross sectional area (m\(^{2}\)) available for air passage. Frequently calculated as
+
+\begin{lstlisting}
+       Amin  = (Amin/Afr)\*Afr
+\end{lstlisting}
+
+where Afr is the frontal area of the heat exchanger, and (Amin/Afr) is the ratio of the minimum airflow area to frontal area.
+
+\paragraph{Field: Coil Depth}\label{field-coil-depth}
+
+The distance (m) from the front of the coil to the back of the coil in the airflow direction. Also called the fin depth. Illustrated in the figure (Figure~\ref{fig:geometry-of-a-cooling-coil-cc}. Geometry of a Cooling Coil (CC)).
+
+\paragraph{Field: Fin Diameter}\label{field-fin-diameter}
+
+The outside diameter (m) of the fins. Used instead of COIL HEIGHT
+
+\paragraph{Field: Fin Thickness}\label{field-fin-thickness}
+
+Thickness (m) of the air side fins.
+
+\paragraph{Field: Tube Inside Diameter}\label{field-tube-inside-diameter}
+
+The inside diameter (m) of the tubes.
+
+\paragraph{Field: Tube Outside Diameter}\label{field-tube-outside-diameter}
+
+The outside diameter (m) of the tubes.
+
+\paragraph{Field: Tube Thermal Conductivity}\label{field-tube-thermal-conductivity}
+
+The thermal conductivity (W/m-K) of the tube material.
+
+\paragraph{Field: Fin Thermal Conductivity}\label{field-fin-thermal-conductivity}
+
+The thermal conductivity (W/m-K) of the fin material.
+
+\paragraph{Field: Fin Spacing}\label{field-fin-spacing}
+
+The spacing (m) of the fins, centerline to centerline.
+
+\paragraph{Field: Tube Depth Spacing}\label{field-tube-depth-spacing}
+
+The spacing (m) of the tube rows, centerline to centerline. Also called tube longitudinal spacing.
+
+\paragraph{Field: Number of Tube Rows}\label{field-number-of-tube-rows}
+
+The number of tube rows in the direction of the airflow.
+
+\paragraph{Field: Number of Tubes per Row}\label{field-number-of-tubes-per-row}
+
+The number of tubes per row. (NTPR in the above diagram)
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-3-000}
+
+The name of the water coil inlet from the chilled water loop, i.e.~Cooling Coil Water Inlet Node.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-3-000}
+
+The name of the water coil outlet from the chilled water loop, i.e.~Cooling Coil Water Outlet Node.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-8}
+
+The name of the air inlet to the water coil, i.e.~Cooling Coil Air Inlet Node.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-8-000}
+
+The name of the air outlet from the water coil, i.e.~Cooling Coil Air Outlet Node.
+
+\paragraph{Field: Condensate Collection Water Storage Tank Name}\label{field-condensate-collection-water-storage-tank-name-1}
+
+This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
+
+Examples of these statements in an IDF are:
+
+\begin{lstlisting}
+
+Coil:Cooling:Water:DetailedGeometry,
+  Detailed Cooling Coil,   !Name of cooling coil
+  CoolingCoilAvailSched,   !Cooling Coil Schedule
+  0.0011,                   !Max Water Flow Rate of Coil m3/sec
+  6.23816,                 !Tube Outside Surf Area
+  6.20007018,           !Tube Inside Surf Area
+  101.7158224,         !Fin Surf Area
+  0.300606367,         !Min Air Flow Area
+  0.165097968,         !Coil Depth
+  0.43507152,           !Coil Height
+  0.001499982,         !Fin Thickness
+  0.014449958,         !Tube Inside Diameter
+  0.015879775,         !Tube Outside Diameter
+  386.0,                     !Tube Thermal Conductivity
+  204.0,                     !Fin Thermal Conductivity
+  0.001814292,         !Fin Spacing
+  0.02589977,           !Tube Depth
+  6,                             !Number of Tube Rows
+  16,                           !Number of Tubes per Row
+  NODE_32,NODE_33, !Coil Water Side Inlet & Outlet Node
+  NODE_5, NODE_6;   !Coil Air Side Inlet & Outlet Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-11-002}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Coil Source Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Sum,Cooling Coil Condensate Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Cooling Coil Total Cooling Energy (J)}\label{cooling-coil-total-cooling-energy-j-3}
+
+Cooling Coil Total Cooling Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
+
+\paragraph{Cooling Coil Sensible Cooling Energy (J)}\label{cooling-coil-sensible-cooling-energy-j-3}
+
+Cooling Coil Sensible Cooling Energy is the total amount of Sensible heat transfer taking place in the coil at the operating conditions. It only takes into account temperature difference in the inlet and outlet air streams at operating conditions.
+
+\paragraph{Cooling Coil Total Cooling Rate (W)}\label{cooling-coil-total-cooling-rate-w-3}
+
+Cooling Coil Total Cooling Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
+
+\paragraph{Cooling Coil Sensible Cooling Rate (W)}\label{cooling-coil-sensible-cooling-rate-w-3}
+
+Cooling Coil Sensible Cooling Rate is the Rate of Sensible heat transfer taking place in the coil at the operating conditions.
+
+In addition, if a Water Storage Tank is used to collect coil condensate, then the following outputs will be available.
+
+\paragraph{Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}}\label{cooling-coil-condensate-volume-flow-rate-m3s-3}
+
+\paragraph{Cooling Coil Condensate Volume {[}m3{]}}\label{cooling-coil-condensate-volume-m3-3}
+
+These reports provide the rate and amount of condensate from the coil. Condensate is water condensed out of the air as a result of cooling. The condensate volume is also reported on the meter for OnSiteWater.
+
+\paragraph{Cooling Coil Source Side Heat Transfer Energy {[}J{]}}\label{cooling-coil-source-side-heat-transfer-energy-j-1}
+
+This is the energy extracted from the chilled water serving the cooling coil, in Joules.
+
+\subsection{Coil:Cooling:DX:SingleSpeed}\label{coilcoolingdxsinglespeed}
+
+This DX cooling coil input requires an availability schedule, the gross rated total cooling capacity, the gross rated SHR, the gross rated COP, and the rated air volume flow rate. The latter 4 inputs determine the coil performance at the rating point (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb and air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb). The rated air volume flow rate should be between .00004027 m\(^{3}\)/s and .00006041 m\(^{3}\)/s per watt of gross rated total cooling capacity (300 to 450 cfm/ton).
+
+The rated volumetric air flow to total cooling capacity ratio for 100\% dedicated outdoor air (DOAS) application DX cooling coils should be between 0.00001677 (m3/s)/W (125 cfm/ton) and 0.00003355 (m3/s)/W (250 cfm/ton).
+
+Pumped refrigerant economizer integrated with the single speed DX cooling coil model will use exactly the same model except that performance curves use lookup table to cover the pumped refrigerant economizer and the compressor operating ranges. One or two independent variables may used to represent the performance data.
+
+This model requires 5 curves as follows:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  The total cooling capacity modifier curve (function of temperature) is a curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). This curve is typically a biquadratic but any curve or table with two independent variables can be used.
+\item
+  The total cooling capacity modifier curve (function of flow fraction) is a curve or lookup table with the independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating. This curve is typically a quadratic or cubic but any curve or table with one independent variables can be used.
+\item
+  The energy input ratio (EIR) modifier curve (function of temperature) is a curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). This curve is typically a biquadratic but any curve or table with two independent variables can be used.
+\item
+  The energy input ratio (EIR) modifier curve (function of flow fraction) is a curve or lookup table with the independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating. This curve is typically a quadratic or cubic but any curve or table with one independent variables can be used.
+\item
+  The part load fraction correlation (function of part load ratio) is a curve or a lookup table with the independent variable being part load ratio (sensible cooling load / steady-state sensible cooling capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The curve should be normalized to a value of 1.0 when the part-load ratio equals 1.0 (i.e., the compressor(s) run continuously for the simulation timestep). This curve is typically a quadratic or cubic but any curve or table with one independent variables can be used.
+\end{enumerate}
+
+The curves are simply specified by name. Curve inputs are described in the curve manager section of this document (see Performance Curves in this document).
+
+The next four input fields are optional and relate to the degradation of latent cooling capacity when the supply air fan operates continuously while the cooling coil/compressor cycle on and off to meet the cooling load. The fan operating mode is determined in the partent object and is considered to either be constant (e.g.~CoilSystem:Cooling:DX) or can be scheduled (e.g.~AirLoopHVAC:UnitaryHeatCool). When scheduled, the schedule value must be greater than 0 to calculate degradation of latent cooling capacity. At times when the parent object s supply air fan operating mode schedule is 0, latent degradation will be ignored. When modeling latent capacity degradation, these next four input fields must all have positive values.
+
+The next input specifies the outdoor air node used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor temperature entering the condenser is taken directly from the weather data. If this field is not blank, the node name specified must be listed in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor temperature from the weather data. Alternately, the node name must be specified in an OutdoorAir:NodeList object where the outdoor temperature entering the condenser is taken directly from the weather data.
+
+The next input describes the type of outdoor condenser coil used with the DX cooling coil (Air Cooled or Evap Cooled). The following three inputs are required when modeling an evaporative-cooled condenser: evaporative condenser effectiveness, evaporative condenser air volume flow rate, and the power consumed by the evaporative condenser pump. Crankcase heater capacity and cutout temperature are entered in the next two input fields. These two fields for this object define the name of the water storage tank for supply and condensate collection. See section DX Cooling Coil Model in the EnergyPlus Engineering Document for further details regarding this model.
+
+The last two input fields following the Basin Heater Operating Schedule Name are the Sensible Heat Ratio (SHR) modifier cruve names for temperature and flow fraction. These two input fields are optional and used only when a user intends to override SHR calculated using the apparatus dew point (ADP) and bypass factor (BF) method. See section SHR Calculation Using User Specified SHR Modifier Curves in the EnergyPlus Engineering Document for further details.
+
+\subsubsection{Inputs}\label{inputs-13-004}
+
+\paragraph{Field: Name}\label{field-name-12-003}
+
+A unique user-assigned name for an instance of a DX cooling coil. Any reference to this DX coil by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-6-001}
+
+The name of the schedule (ref: Schedule) that denotes whether the DX cooling coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during a given time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Gross Rated Total Cooling Capacity}\label{field-gross-rated-total-cooling-capacity-1}
+
+The total, full load gross cooling capacity (sensible plus latent) in watts of the DX coil unit at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb\protect\hyperlink{ux5fftn1}{{[}1{]}}, and a cooling coil air flow rate defined by field rated air flow rate below). Capacity should be gross (i.e., the effect of supply air fan heat is NOT accounted for). When used in a heat pump, the gross rated total cooling capacity should be within 20\% of the gross rated heating capacity, otherwise a warning message is issued.
+
+\paragraph{Field: Gross Rated Sensible Heat Ratio}\label{field-gross-rated-sensible-heat-ratio}
+
+The sensible heat ratio (SHR = gross sensible cooling capacity divided by gross total cooling capacity) of the DX cooling coil at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb), and a cooling coil air flow rate defined by field rated air flow rate below). Both the sensible and total cooling capacities used to define the Rated SHR should be gross (i.e., the effect of supply air fan heat is NOT accounted for).
+
+\paragraph{Field: Gross Rated Cooling COP}\label{field-gross-rated-cooling-cop}
+
+The coefficient of performance is the ratio of the gross total cooling capacity in watts to electrical power input in watts of the DX cooling coil unit at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/ 23.9 °C wetbulb, and a cooling coil air flow rate defined by field rated air flow rate below). The input power includes electric power for the compressor(s) and condenser fan(s) but does not include the power consumption of the supply air fan. The gross COP should NOT account for the supply air fan. If this input field is left blank, the default value is 3.0.
+
+\paragraph{Field: Rated Air Flow Rate}\label{field-rated-air-flow-rate-2}
+
+The air volume flow rate, in m\(^{3}\) per second, across the DX cooling coil at rated conditions. The rated air volume flow rate should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of gross rated total cooling capacity (300 to 450 cfm/ton). For DOAS applications the rated air volume flow rate should be between 0.00001677 m\(^{3}\)/s and 0.00003355 m\(^{3}\)/s per watt of gross rated total cooling capacity (125 to 250 cfm/ton). The gross rated total cooling capacity, gross rated SHR and gross rated COP should be performance information for the unit with air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and the rated air volume flow rate defined here.
+
+\paragraph{Field: Rated Evaporator Fan Power Per Volume Flow Rate}\label{field-rated-evaporator-fan-power-per-volume-flow-rate}
+
+This field is the electric power for the evaporator (cooling coil) fan per air volume flow rate through the coil at the rated conditions in W/(m\(^{3}\)/s). The default value is 773.3 W/(m\(^{3}\)/s) (365 W/1000 cfm) if this field is left blank. If a value is entered, it must be \textgreater{} = 0.0 and \textless{} = 1250 W/(m\(^{3}\)/s). This value is only used to calculate Seasonal Energy Efficiency Ratio (SEER), Energy Efficiency Ratio (EER), Integrated Energy Efficiency Ratio (IEER) and the Standard Rating (Net) Cooling Capacity which will be outputs in the EnergyPlus eio file (ref. EnergyPlus Engineering Reference, Single Speed DX Cooling Coil, Standard Ratings). This value is not used for modeling the evaporator (cooling coil) fan during simulations; instead, it is used for calculating SEER, EER, IEER and Standard Rating Cooling Capacity to assist the user in verifying their inputs for modeling this type of equipment.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-9}
+
+The name of the HVAC system node from which the DX cooling coil draws its inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-9-000}
+
+The name of the HVAC system node to which the DX cooling coil sends its outlet air.
+
+\paragraph{Field: Total Cooling Capacity Function of Temperature Curve Name}\label{field-total-cooling-capacity-function-of-temperature-curve-name}
+
+The name of a performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to have the value of 1.0 at the rating point. This curve is typically a biquadratic but any curve or table with two independent variables can be used.
+
+\paragraph{Field: Total Cooling Capacity Function of Flow Fraction Curve Name}\label{field-total-cooling-capacity-function-of-flow-fraction-curve-name}
+
+The name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
+
+\paragraph{Field: Energy Input Ratio Function of Temperature Curve Name}\label{field-energy-input-ratio-function-of-temperature-curve-name}
+
+The name of a performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to a value of 1.0 at the rating point. This curve is typically a biquadratic but any curve or table with two independent variables can be used.
+
+\paragraph{Field: Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-energy-input-ratio-function-of-flow-fraction-curve-name}
+
+The name of a performance curve (Ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This curve is typically a quadratic or cubic but any curve or table with one independent variables can be used.
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-2}
+
+This alpha field defines the name of a performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. This curve is typically a quadratic or cubic but any curve or table with one independent variables can be used.
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
+
+\begin{lstlisting}
+       PLF = 0.85 + 0.15(PLR)
+\end{lstlisting}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{lstlisting}
+       PLF = 1.0 + 0.0(PLR)
+\end{lstlisting}
+
+\paragraph{Field: Nominal Time for Condensate Removal to Begin}\label{field-nominal-time-for-condensate-removal-to-begin}
+
+The nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}), and this field as well as the next three input fields for this object must have positive values in order to model latent capacity degradation.
+
+\paragraph{Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity}\label{field-ratio-of-initial-moisture-evaporation-rate-and-steady-state-latent-capacity}
+
+Ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}); and this field, the previous field and the next two fields must have positive values in order to model latent capacity degradation.
+
+\paragraph{Field: Maximum Cycling Rate}\label{field-maximum-cycling-rate}
+
+The maximum on-off cycling rate for the compressor (cycles per hour), which occurs at 50\% run time fraction. Suggested value is 3; zero value means latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}); and this field, the previous two fields and the next field must have positive values in order to model latent capacity degradation.
+
+\paragraph{Field: Latent Capacity Time Constant}\label{field-latent-capacity-time-constant}
+
+Time constant (in seconds) for the cooling coil's latent capacity to reach steady state after startup. Suggested value is 45: supply air fan operating mode must be continuous. That is, the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects (e.g., AirloopHVAC:UnitaryHeatCool), and this field as well as the previous three input fields for this object must have positive values in order to model latent capacity degradation.
+
+\paragraph{Field: Condenser Air Inlet Node Name}\label{field-condenser-air-inlet-node-name}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type}
+
+The type of condenser used by the DX cooling coil. Valid choices for this input field are \textbf{AirCooled} or \textbf{EvaporativelyCooled}. The default for this field is \textbf{AirCooled}.
+
+\paragraph{Field: Evaporative Condenser Effectiveness}\label{field-evaporative-condenser-effectiveness}
+
+The effectiveness of the evaporative condenser, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
+
+\begin{equation}
+Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectiveness} \right)\left( {Tdb,o\,\, - Twb,o} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{cond\\ inlet}\)} = the temperature of the air entering the condenser coil (C)
+
+\emph{T\(_{wb,o}\)} = the wet-bulb temperature of the outdoor air (C)
+
+\emph{T\(_{db,o}\)} = the dry-bulb temperature of the outdoor air (C)
+
+The resulting condenser inlet air temperature is used by the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled.
+
+If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
+
+If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
+
+If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
+
+\paragraph{Field: Evaporative Condenser Air Flow Rate}\label{field-evaporative-condenser-air-flow-rate}
+
+The air volume flow rate, in m\(^{3}\) per second, entering the evaporative condenser. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000144 m\(^{3}\)/s per watt of rated total cooling capacity {[}850 cfm/ton{]}). This field is not used when Condenser Type = Air Cooled.
+
+\paragraph{Field: Evaporative Condenser Pump Rated Power Consumption}\label{field-evaporative-condenser-pump-rated-power-consumption}
+
+The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt {[}15 W/ton{]} of rated total cooling capacity). This field is not used when Condenser Type = Air Cooled.
+
+\paragraph{Field: Crankcase Heater Capacity}\label{field-crankcase-heater-capacity}
+
+This numeric field defines the crankcase heater capacity in Watts. When the outdoor air dry-bulb temperature is below the value specified in the input field Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation (described below), the crankcase heater is enabled during the time that the compressor is not running. If this cooling coil is used as part of an air-to-air heat pump (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir or PackageTerminal: HeatPump:AirToAir), the crankcase heater defined for this DX cooling coil is ignored and the crankcase heater power defined for the DX heating coil (Ref. Coil:Heating:DX:SingleSpeed) is enabled during the time that the compressor is not running for either heating or cooling. The value for this input field must be greater than or equal to 0, and the default value is 0. To simulate a DX cooling coil without a crankcase heater, enter a value of 0.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-crankcase-heater-operation}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the compressor s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 °C, and the default value is 10 °C.
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-000}
+
+This field is optional. It is used to describe where the coil obtains water used for evaporative cooling of its condenser. If blank or omitted, then the unit will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, then the unit will obtain its water from that tank. If a tank is specified, the unit will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the condenser needs, then the unit will still operate and obtain the rest of the water it needs from the mains (referred to as StarvedWater).
+
+\paragraph{Field: Condensate Collection Water Storage Tank Name}\label{field-condensate-collection-water-storage-tank-name-2}
+
+This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-000}
+
+This numeric field contains the capacity of the DX coil s electric evaporative cooler basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the DX coil is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-000}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the DX coil is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-000}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the DX coil is off.
+
+\paragraph{Field: Sensible Heat Ratio Function of Temperature Curve Name}\label{field-sensible-heat-ratio-function-of-temperature-curve-name}
+
+The name of a biquadratic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of DX cooling coil entering air wet-bulb and dry-bulb temperatures. The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of flow fraction) to give the SHR at the specific coil entering air temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 at the rated condition. This input field is optional.
+
+\paragraph{Field: Sensible Heat Ratio Function of Flow Fraction Curve Name}\label{field-sensible-heat-ratio-function-of-flow-fraction-curve-name}
+
+The name of a quadratic or cubic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of temperature) to give the SHR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This input field is optional.
+
+\paragraph{Field: Zone Name for Condenser Placement}\label{field-zone-name-for-condenser-placement}
+
+This input field is name of a conditioned or unconditioned zone where the secondary coil (condenser) of DX system or a heat pump is to be placed. This is an optional input field specified only when user desires to reject the condenser heat into a zone. The heat rejected is modeled as sensible internal gain of a secondary zone.
+
+Following is an example input for a Coil:Cooling:DX:SingleSpeed coil.
+
+\begin{lstlisting}
+
+Coil:Cooling:DX:SingleSpeed,
+  Zone1WindACDXCoil,               ! Coil Name
+  FanAndCoilAvailSched,         ! Availability Schedule
+  10548,           ! Gross Rated Total Cooling Capacity
+  0.75,             ! Gross Rated Sensible Heat Ratio
+  3.0,               ! Gross Rated Cooling COP
+  0.637,           ! Rated Air Flow Rate (m3/s)
+  773.3,           ! Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
+  Zone1WindACFanOutletNode, ! Coil Air Inlet Node
+  Zone1WindACAirOutletNode, ! Coil Air Outlet Node
+  WindACCoolCapFT,                   ! Total Cooling Capacity Modifier Curve (function of temperature)
+  WindACCoolCapFFF,                 ! Total Cooling Capacity Modifier Curve (function of flow fraction)
+  WindACEIRFT,                           ! Energy Input Ratio Modifier Curve (function of temperature)
+  WindACEIRFFF,                         ! Energy Input Ratio Modifier Curve (function of flow fraction)
+  WindACPLFFPLR,                       ! Part Load Fraction Correlation (function of part load ratio)
+  1000.,                         ! Nominal Time for Condensate Removal to Begin {s}
+  1.5,                             ! Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity
+  3.0,                             ! Maximum ON/OFF Cycling Rate {cycles/hr}
+  45.0,                           ! Latent Capacity Time Constant {s}
+  ,                                   ! Condenser Air Inlet Node Name
+  AirCooled,               ! Condenser Type
+  ,                                   ! Evaporative Condenser Effectiveness
+  ,                                   ! Evaporative Condenser Air Volume Flow Rate {m3/s}
+  ,                                   ! Evaporative Condenser Pump Rated Power Consumption {W}
+  30.,                             ! Crankcase Heater Capacity {W}
+  10.;                             ! Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
+\end{lstlisting}
+
+\subsection{Coil:Cooling:DX:TwoSpeed}\label{coilcoolingdxtwospeed}
+
+This component models a two-speed (or variable speed) DX compressor and fan. The method is based on the model used for the cycling, single speed DX unit. The single speed unit is described by single full load capacity, SHR, COP, and air flow rate at rated conditions. Off rated full load performance is obtained by the use of 4 modifier curves. At partial load the unit cycles on/off and the cycling losses are described by a part load fraction curve.
+
+The multispeed unit is described by specifying the performance at two states: high speed compressor, high speed fan; and low speed compressor, low speed fan. When the unit load is above the high speed capacity, the unit runs with high speed compressor and fan. When the load on the unit is below the high speed capacity but above the low speed capacity, the unit will run with performance intermediate between high speed and low speed. When the load is less than the low speed capacity, the unit will cycle on/off just like the single speed unit.
+
+The multispeed unit model requires 2 full sets of performance data. There must be a high and low speed capacity, SHR, COP, and evaporator air flow rate; as well as high and low speed performance curves total cooling capacity modifier curve (function of temperature) and energy input ratio modifier curve (function of temperature).
+
+The multispeed DX component should be used for all cases in which a DX VAV system is being simulated. Obviously this model in which performance is obtained by interpolating between 2 specified states - is an oversimplification of how real multi-speed and variable speed DX cooling units are controlled. But detailed descriptions of how actual units perform and are controlled are not available. This model should give a good average prediction of multispeed and variable speed DX cooling unit performance. The last four input fields following the Basin Heater Operating Schedule Name are the Sensible Heat Ratio (SHR) modifier cruve names for temperature and flow fraction for high and low speed DX cooling coils. These four input fields are optional and used only when a user intends to override SHR calculated using the apparatus dew point (ADP) and bypass factor (BF) method. See section SHR Calculation Using User Specified SHR Modifier Curves in the EnergyPlus Engineering Document for further details..
+
+\subsubsection{Inputs}\label{inputs-14-004}
+
+\paragraph{Field: Name}\label{field-name-13-003}
+
+A unique user-assigned name for an instance of a multispeed DX cooling coil. Any reference to this DX coil by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-7-001}
+
+The name of the schedule (ref: Schedule) that denotes whether the DX cooling coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: High Speed Gross Rated Total Cooling Capacity}\label{field-high-speed-gross-rated-total-cooling-capacity}
+
+The total, full load gross cooling capacity (sensible plus latent) in watts of the DX coil unit for high speed compressor and high speed fan at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and a cooling coil air flow rate defined by field rated air flow rate below). Capacity should be gross (i.e., the effect of supply air fan heat is NOT accounted for).
+
+\paragraph{Field: High Speed Gross Rated Sensible Heat Ratio}\label{field-high-speed-gross-rated-sensible-heat-ratio}
+
+The sensible heat ratio (gross sensible capacity divided by gross total cooling capacity) of the DX cooling coil for high speed compressor and high speed fan at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb\protect\hyperlink{ux5fftn2}{{[}2{]}}, and a cooling coil air flow rate defined by field rated air flow rate below). Both the sensible and total cooling capacities used to define the Rated SHR should be gross (i.e., the effect of supply air fan heat is NOT accounted for).
+
+\paragraph{Field: High Speed Gross Rated Cooling COP}\label{field-high-speed-gross-rated-cooling-cop}
+
+The coefficient of performance is the ratio of the gross total cooling capacity in watts to electrical power input in watts) of the DX cooling coil unit for high speed compressor and high speed fan at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and a cooling coil air flow rate defined by field rated air flow rate below). The input power includes electric power for the compressor(s) and condenser fan(s) but does not include the power consumption of the supply air fan. The gross COP should NOT account for the supply air fan. If this input field is left blank, the default value is 3.0.
+
+\paragraph{Field: High Speed Rated Air Flow Rate}\label{field-high-speed-rated-air-flow-rate}
+
+The high speed air volume flow rate, in m\(^{3}\) per second, across the DX cooling coil at rated conditions. The rated air volume flow rate should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of gross rated total cooling capacity. For DOAS applications the rated air volume flow rate should be between 0.00001677 m\(^{3}\)/s and 0.00003355 m\(^{3}\)/s per watt of gross rated total cooling capacity (125 to 250 cfm/ton). The gross rated total cooling capacity, gross rated SHR and gross rated COP should be performance information for the unit with air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and the rated air volume flow rate defined here.
+
+\paragraph{Field: Unit Internal Static Air Pressure}\label{field-unit-internal-static-air-pressure}
+
+If this coil is used with a Fan:VariableVolume to model a packaged variable-air-volume unit, then ratings for standard rated net capacity, EER, and IEER will be calculated per ANSI/AHRI Standard 340/360-2007 with Addenda 1 and 2. This field is to specify the internal static air pressure, in units of Pascals, associated with the unit s supply air flow for rating purposes. This field does not affect the performance during operation. This field is optional. If this field is used, then the internal static air pressure is used with the associated fan characteristics when calculating standard rated net capacity, EER, and IEER. If this field is not used, then the standard ratings are still performed but use a default for specific fan power of 773.3 (W/(m\(^{3}\)/s)). The air pressure drop/rise input here should be internal in the sense that it is for the entire package of unitary equipment as it would be tested in a laboratory (including other non-cooling sections inside the package for filters, dampers, and.or heating coils) but none of the external pressure drop for distributing supply air throughout the building. This is different from the input field called Pressure Rise in the fan object which includes both the external static pressure and the internal static pressure. The results of standard rating calculations are reported to the EIO file and to predefined output tables called DX Cooling Coils and VAV DX Cooling Standard Rating Details.
+
+\paragraph{Field: Air Inlet Node}\label{field-air-inlet-node}
+
+The name of the HVAC system node from which the DX cooling coil draws its inlet air.
+
+\paragraph{Field: Air Outlet Node}\label{field-air-outlet-node}
+
+The name of the HVAC system node to which the DX cooling coil sends its outlet air.
+
+\paragraph{Field: Total Cooling Capacity Function of Temperature Curve Name}\label{field-total-cooling-capacity-function-of-temperature-curve-name-1}
+
+The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to have the value of 1.0 at the rating point. This curve is used for performance at the high speed compressor, high speed fan operating point.
+
+\paragraph{Field: Total Cooling Capacity Function of Flow Fraction Curve Name}\label{field-total-cooling-capacity-function-of-flow-fraction-curve-name-1}
+
+The name of a quadratic performance curve (ref: Performance Curves) that parameterizes the variation of gross total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate. This curve is applied only at the high speed compressor, high speed fan operating point. There is no corresponding curve for the low speed operating point.
+
+\paragraph{Field: Energy Input Ratio Function of Temperature Curve Name}\label{field-energy-input-ratio-function-of-temperature-curve-name-1}
+
+The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the wet-bulb temperature of the air entering the cooling coil and the dry-bulb temperature of the air entering the air-cooled condenser (wet-bulb temperature if modeling an evaporative-cooled condenser). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to a value of 1.0 at the rating point. This curve is used for performance at the high speed compressor, high speed fan operating point.
+
+\paragraph{Field: Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-energy-input-ratio-function-of-flow-fraction-curve-name-1}
+
+The name of a quadratic performance curve (Ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This curve is applied only at the high speed compressor, high speed fan operating point. There is no corresponding curve for the low speed operating point.
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-3}
+
+This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
+
+\begin{lstlisting}
+       PLF = 0.85 + 0.15(PLR)
+\end{lstlisting}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{lstlisting}
+       PLF = 1.0 + 0.0(PLR)
+\end{lstlisting}
+
+\paragraph{Field: Low Speed Gross Rated Total Cooling Capacity}\label{field-low-speed-gross-rated-total-cooling-capacity}
+
+The total, full load gross total cooling capacity (sensible plus latent) in watts of the DX coil unit for low speed compressor and low speed fan at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and a cooling coil air flow rate defined by field rated air flow rate, low speed below). Capacity should be gross (i.e., the effect of supply air fan heat is NOT accounted for).
+
+\paragraph{Field: Low Speed Gross Rated Sensible Heat Ratio}\label{field-low-speed-gross-rated-sensible-heat-ratio}
+
+The sensible heat ratio (SHR = gross sensible capacity divided by gross total cooling capacity) of the DX cooling coil for low speed compressor and low speed fan at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and a cooling coil air flow rate defined by field rated air flow rate, low speed below). Both the sensible and total cooling capacities used to define the Rated SHR should be gross (i.e., the effect of supply air fan heat is NOT accounted for).
+
+\paragraph{Field: Low Speed Gross Rated Cooling COP}\label{field-low-speed-gross-rated-cooling-cop}
+
+The coefficient of performance is the ratio of gross total cooling capacity in watts to electrical power input in watts) of the DX cooling coil unit for low speed compressor and low speed fan at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and a cooling coil air flow rate defined by field rated air volume flow rate, low speed below). The input power includes power for the compressor(s) and condenser fan(s) but does not include the power consumption of the supply air fan. The gross COP should NOT account for the supply air fan. If this input field is left blank, the default value is 3.0.
+
+\paragraph{Field: Low Speed Rated Air Flow Rate}\label{field-low-speed-rated-air-flow-rate}
+
+The low speed volume air flow rate, in m\(^{3}\) per second, across the DX cooling coil at rated conditions. The rated air volume flow rate should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of the gross rated total cooling capacity. For DOAS applications the rated air volume flow rate should be between 0.00001677 m\(^{3}\)/s and 0.00003355 m\(^{3}\)/s per watt of gross rated total cooling capacity (125 to 250 cfm/ton). The gross rated total cooling capacity, gross rated SHR and gross rated COP should be performance information for the unit with air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and the rated air volume flow rate defined here.
+
+\paragraph{Field: Low Speed Total Cooling Capacity Function of Temperature Curve Name}\label{field-low-speed-total-cooling-capacity-function-of-temperature-curve-name}
+
+The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to have the value of 1.0 at the rating point. This curve is used for performance at the low speed compressor, low speed fan operating point.
+
+\paragraph{Field: Low Speed Energy Input Ratio Function of Temperature Curve Name}\label{field-low-speed-energy-input-ratio-function-of-temperature-curve-name}
+
+The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the wetbulb temperature of the air entering the cooling coil and the drybulb temperature of the air entering the air-cooled condenser (wetbulb temperature if modeling an evaporative-cooled condenser). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to a value of 1.0 at the rating point. This curve is used for performance at the low speed compressor, low speed fan operating point.
+
+\paragraph{Field: Condenser Air Inlet Node Name}\label{field-condenser-air-inlet-node-name-1}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-1}
+
+The type of condenser used by the multi-speed DX cooling coil. Valid choices for this input field are \textbf{AirCooled} or \textbf{EvaporativelyCooled}. The default for this field is \textbf{AirCooled}.
+
+\paragraph{Field: High Speed Evaporative Condenser Effectiveness}\label{field-high-speed-evaporative-condenser-effectiveness}
+
+The effectiveness of the evaporative condenser at high compressor/fan speed, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
+
+\begin{equation}
+Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectivenes{s_{HighSpeed}}} \right)\left( {Tdb,o\,\, - Twb,o} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{cond\\ inlet}\)} = the temperature of the air entering the condenser coil (C)
+
+\emph{T\(_{wb,o}\)} = the wet-bulb temperature of the outdoor air (C)
+
+\emph{T\(_{db,o}\)} = the dry-bulb temperature of the outdoor air (C)
+
+The resulting condenser inlet air temperature is used by the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled.
+
+If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
+
+If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
+
+If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
+
+\paragraph{Field: High Speed Evaporative Condenser Air Flow Rate}\label{field-high-speed-evaporative-condenser-air-flow-rate}
+
+The air volume flow rate, in m\(^{3}\) per second, entering the evaporative condenser at high compressor/fan speed. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000144 m\(^{3}\)/s per watt of rated high-speed total cooling capacity {[}850 cfm/ton{]}). This field is not used when Condenser Type = Air Cooled.
+
+\paragraph{Field: High Speed Evaporative Condenser Pump Rated Power Consumption}\label{field-high-speed-evaporative-condenser-pump-rated-power-consumption}
+
+The rated power of the evaporative condenser water pump in Watts at high compressor/fan speed. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt {[}15 W/ton{]} of rated high-speed total cooling capacity). This field is not used when Condenser Type = Air Cooled.
+
+\paragraph{Field: Low Speed Evaporative Condenser Effectiveness}\label{field-low-speed-evaporative-condenser-effectiveness}
+
+The effectiveness of the evaporative condenser at low compressor/fan speed, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
+
+\begin{equation}
+Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectivenes{s_{LowSpeed}}} \right)\left( {Tdb,o\,\, - Twb,o} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{cond\\ inlet}\)} = the temperature of the air entering the condenser coil (C)
+
+\emph{T\(_{wb,o}\)} = the wet-bulb temperature of the outdoor air (C)
+
+\emph{T\(_{db,o}\)} = the dry-bulb temperature of the outdoor air (C)
+
+The resulting condenser inlet air temperature is used by the Total Cooling Capacity Modifier Curve, low speed (function of temperature) and the Energy Input Ratio Modifier Curve, low speed (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled. See field Evaporative Condenser Effectiveness, High Speed above for further information.
+
+\paragraph{Field: Low Speed Evaporative Condenser Air Flow Rate}\label{field-low-speed-evaporative-condenser-air-flow-rate}
+
+The air volume flow rate, in m\(^{3}\) per second, entering the evaporative condenser at low compressor/fan speed. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000048 m\(^{3}\)/s per watt of rated high-speed total cooling capacity {[}280 cfm/ton{]}). This field is not used when Condenser Type = Air Cooled.
+
+\paragraph{Field: Low Speed Evaporative Condenser Pump Rated Power Consumption}\label{field-low-speed-evaporative-condenser-pump-rated-power-consumption}
+
+The rated power of the evaporative condenser water pump in Watts at low compressor/fan speed. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.001422 W per watt {[}5 W/ton{]} of rated high-speed total capacity). This field is not used when Condenser Type = Air Cooled.
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-1-000}
+
+This field is optional. It is used to describe where the coil obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the coil will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains (referred to as StarvedWater).
+
+\paragraph{Field: Condensate Collection Water Storage Tank Name}\label{field-condensate-collection-water-storage-tank-name-3}
+
+This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-1-000}
+
+This numeric field contains the capacity of the DX coil s electric evaporative cooler basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the DX coil is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-1-000}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the DX coil is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-1-000}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the DX coil is off.
+
+\paragraph{Field: Sensible Heat Ratio Function of Temperature Curve Name}\label{field-sensible-heat-ratio-function-of-temperature-curve-name-1}
+
+The name of a biquadratic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of DX cooling coil entering air wet-bulb and dry-bulb temperatures. The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of flow fraction) to give the SHR at the specific coil entering air temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 at the rated condition. This input field is optional.
+
+\paragraph{Field: Sensible Heat Ratio Function of Flow Fraction Curve Name}\label{field-sensible-heat-ratio-function-of-flow-fraction-curve-name-1}
+
+The name of a quadratic or cubic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of temperature) to give the SHR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This input field is optional.
+
+\paragraph{Field: Low Sensible Heat Ratio Function of Temperature Curve Name}\label{field-low-sensible-heat-ratio-function-of-temperature-curve-name}
+
+The name of a biquadratic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of DX cooling coil entering air wet-bulb and dry-bulb temperatures. The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of flow fraction) to give the SHR at the specific coil entering air temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 at the rated condition. This input field is optional.
+
+\paragraph{Field: Low Sensible Heat Ratio Function of Flow Fraction Curve Name}\label{field-low-sensible-heat-ratio-function-of-flow-fraction-curve-name}
+
+The name of a quadratic or cubic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of temperature) to give the SHR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This input field is optional.
+
+\paragraph{Field: Zone Name for Condenser Placement}\label{field-zone-name-for-condenser-placement-1}
+
+This input field is name of a conditioned or unconditioned zone where the secondary coil (condenser) of DX system or a heat pump is to be placed. This is an optional input field specified only when user desires to reject the condenser heat into a zone. The heat rejected is modeled as sensible internal gain of a secondary zone.
+
+Following are example inputs for the object.
+
+\begin{lstlisting}
+
+Coil:Cooling:DX:TwoSpeed,
+  Main Cooling Coil 1,         !- Name
+  CoolingCoilAvailSched,     !- Availability Schedule Name
+  autosize,                               !- Gross Rated High Speed Total Cooling Capacity {W}
+  0.68,                                       !- Gross Rated High Speed Sensible Heat Ratio
+  3.0,                                         !- Gross Rated High Speed Cooling COP
+  autosize,                               !- Rated High Speed Air Flow Rate {m3/s}
+  ,                                               !- Unit Internal Static Air Pressure Drop {Pa}
+  Mixed Air Node 1,               !- Air Inlet Node Name
+  Main Cooling Coil 1 Outlet Node,   !- Air Outlet Node Name
+  VarSpeedCoolCapFT,             !- Total Cooling Capacity Function of Temperature Curve Name
+  PackagedRatedCoolCapFFlow,   !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  VarSpeedCoolEIRFT,             !- Energy Input Ratio Function of Temperature Curve Name
+  PackagedRatedCoolEIRFFlow,   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  VarSpeedCyclingPLFFPLR,   !- Part Load Fraction Correlation Curve Name
+  autosize,                               !- Rated Low Speed Total Cooling Capacity {W}
+  0.69,                                       !- Rated Low Speed Sensible Heat Ratio
+  4.2,                                         !- Rated Low Speed COP
+  autosize,                               !- Rated Low Speed Air Flow Rate {m3/s}
+  VarSpeedCoolCapLSFT,         !- Low Speed Total Cooling Capacity Function of Temperature Curve Name
+  VarSpeedCoolEIRLSFT,         !- Low Speed Energy Input Ratio Function of Temperature Curve Name
+  Main Cooling Coil 1 Condenser Node;   !- Condenser Air Inlet Node Name
+
+
+  Coil:Cooling:DX:TwoSpeed,
+  Main Cooling Coil 1,         !- Name
+  CoolingCoilAvailSched,     !- Availability Schedule Name
+  autosize,                               !- High Speed Rated Total Cooling Capacity {W}
+  0.68,                                       !- High Speed Rated Sensible Heat Ratio
+  3.0,                                         !- High Speed Rated Cooling COP
+  autosize,                               !- High Speed Rated Air Flow Rate {m3/s}
+  ,                                               !- Unit Internal Static Air Pressure Drop {Pa}
+  Mixed Air Node 1,               !- Air Inlet Node Name
+  Main Cooling Coil 1 Outlet Node,   !- Air Outlet Node Name
+  VarSpeedCoolCapFT,             !- Total Cooling Capacity Function of Temperature Curve Name
+  PackagedRatedCoolCapFFlow,   !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  VarSpeedCoolEIRFT,             !- Energy Input Ratio Function of Temperature Curve Name
+  PackagedRatedCoolEIRFFlow,   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  VarSpeedCyclingPLFFPLR,   !- Part Load Fraction Correlation Curve Name
+  autosize,                               !- Low Speed Rated Total Cooling Capacity {W}
+  0.69,                                       !- Low Speed Rated Sensible Heat Ratio
+  4.2,                                         !- Low Speed Rated Cooling COP
+  autosize,                               !- Low Speed Rated Air Flow Rate {m3/s}
+  VarSpeedCoolCapLSFT,         !- Low Speed Total Cooling Capacity Function of Temperature Curve Name
+  VarSpeedCoolEIRLSFT,         !- Low Speed Energy Input Ratio Function of Temperature Curve Name
+  Main Cooling Coil 1 Condenser Node;   !- Condenser Air Inlet Node Name
+  ,                                               !- Condenser Type
+  ,                                               !- High Speed Evaporative Condenser Effectiveness {dimensionless}
+  ,                                               !- High Speed Evaporative Condenser Air Flow Rate {m3/s}
+  ,                                               !- High Speed Evaporative Condenser Pump Rated Power Consumption {W}
+  ,                                               !- Low Speed Evaporative Condenser Effectiveness {dimensionless}
+  ,                                               !- Low Speed Evaporative Condenser Air Flow Rate {m3/s}
+  ,                                               !- Low Speed Evaporative Condenser Pump Rated Power Consumption {W}
+  ,                                               !- Supply Water Storage Tank Name
+  ,                                               !- Condensate Collection Water Storage Tank Name
+  ,                                               !- Basin Heater Capacity {W/K}
+  ,                                               !- Basin Heater Setpoint Temperature {C}
+  ,                                               !- Basin Heater Operating Schedule Name
+  DOAS DX Coil SHR-FT,         !- High Speed Sensible Heat Ratio Function of Temperature Curve Name
+  DOAS DX Coil SHR-FF,         !- High Speed Sensible Heat Ratio Function of Flow Fraction Curve Name
+  DOAS DX Coil SHR-FT,         !- Low Speed Sensible Heat Ratio Function of Temperature Curve Name
+  DOAS DX Coil SHR-FF;         !- Low Speed Sensible Heat Ratio Function of Flow Fraction Curve Name
+
+
+  Curve:Quadratic,
+  DOAS DX Coil SHR-FF,                                                                         !- Name
+  0.9317,                                                                                                   !- Coefficient1 Constant
+  -0.0077,                                                                                                   !- Coefficient2 x
+  0.0760,                                                                                                   !- Coefficient3 x**2
+  0.69,                                                                                                       !- Minimum Value of x
+  1.30;                                                                                                       !- Maximum Value of x
+
+
+  Curve:Biquadratic,
+  DOAS DX Coil SHR-FT,                                                                         !- Name
+  1.3294540786,                                                                                       !- Coefficient1 Constant
+  -0.0990649255,                                                                                     !- Coefficient2 x
+  0.0008310043,                                                                                       !- Coefficient3 x**2
+  0.0652277735,                                                                                       !- Coefficient4 y
+  -0.0000793358,                                                                                     !- Coefficient5 y**2
+  -0.0005874422,                                                                                     !- Coefficient6 x*y
+  24.44,                                                                                                     !- Minimum Value of x
+  26.67,                                                                                                     !- Maximum Value of x
+  29.44,                                                                                                     !- Minimum Value of y
+  46.1,                                                                                                       !- Maximum Value of y
+  0.6661,                                                                                                   !- Minimum Curve Output
+  1.6009,                                                                                                   !- Maximum Curve Output
+  Temperature,                                                                                         !- Input Unit Type for X
+  Temperature,                                                                                         !- Input Unit Type for Y
+  Dimensionless;                                                                                     !- Output Unit Type
+\end{lstlisting}
+
+\subsection{Coil:Cooling:DX:TwoStageWithHumidityControlMode}\label{coilcoolingdxtwostagewithhumiditycontrolmode}
+
+The multimode DX coil is functionally equivalent to Coil:Cooling:DX:SingleSpeed but with multiple performance modes. It is capable of modeling two-stage DX units and units with an enhanced dehumidification mode such as coil bypass or subcool reheat. This object contains one-time specifications for the DX unit such as node names and crankcase heater specifications. It references one or more CoilPerformance:DX:Cooling objects which define the performance for each mode of operation. It can have up to 4 performance modes to accommodate a 2-stage 2-mode unit.
+
+The multimode DX coil can be used only as a component of CoilSystem:Cooling:DX or AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass (parent object). These parent objects pass a load and dehumidification mode to this coil. If the coil has 2 capacity stages, the multimode coil model determines the stage sequencing.
+
+\subsubsection{Inputs}\label{inputs-15-004}
+
+\paragraph{Field: Name}\label{field-name-14-002}
+
+A unique user-assigned name for an instance of a DX cooling coil. Any reference to this DX coil by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-8-001}
+
+The name of the schedule (ref: Schedule) that denotes whether the DX cooling coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during a given time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-10}
+
+The name of the HVAC system node from which the DX cooling coil draws its inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-10}
+
+The name of the HVAC system node to which the DX cooling coil sends its outlet air.
+
+\paragraph{Field: Crankcase Heater Capacity}\label{field-crankcase-heater-capacity-1}
+
+This numeric field defines the crankcase heater capacity in Watts. When the outdoor air dry-bulb temperature is below the value specified in the input field Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation (described below), the crankcase heater is enabled during the time that the compressor is not running. If this cooling coil is used as part of an air-to-air heat pump (Ref. AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass), the crankcase heater defined for this DX cooling coil is ignored and the crankcase heater power defined for the DX heating coil (Ref. Coil:Heating:DX:SingleSpeed) is enabled during the time that the compressor is not running for either heating or cooling. The value for this input field must be greater than or equal to 0, and the default value is 0. To simulate a DX cooling coil without a crankcase heater, enter a value of 0.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-crankcase-heater-operation-1}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the compressor s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 °C, and the default value is 10 °C.
+
+\paragraph{Field: Number of Capacity Stages}\label{field-number-of-capacity-stages}
+
+This integer field defines the number of capacity stages. The value for this input field must be either 1 or 2, and the default value is 1. Larger DX units often have two capacity stages, which are often two completely independent compressor/coil circuits with the evaporator coils arranged in parallel in the supply air stream. 2-stage operation affects cycling losses and latent degradation due to re-evaporation of moisture with continuous fan operation.
+
+\paragraph{Field: Number of Enhanced Dehumidification Modes}\label{field-number-of-enhanced-dehumidification-modes}
+
+This integer field defines the number of enhanced dehumidification modes available. The value for this input field must be 0 or 1, and the default value is 0. If the DX unit can switch operating modes to increase dehumidification based on a humidistat signal, then set this to 1. This field just specified the availability of enhanced dehumidification. Actual control of the operating mode is handled by the coil's parent component.
+
+\paragraph{Field: Normal Mode Stage 1 Coil Performance Object Type}\label{field-normal-mode-stage-1-coil-performance-object-type}
+
+\paragraph{Field: Normal Mode Stage 1 Coil Performance Object Name}\label{field-normal-mode-stage-1-coil-performance-object-name}
+
+This pair of fields specifies the object type and name for the coil performance object which specifies the DX coil performance for stage 1 operation without enhanced dehumidification (normal mode). The only valid performance object type is CoilPerformance:DX:Cooling.
+
+\paragraph{Field: Normal Mode Stage 1+2 Coil Performance Object Type}\label{field-normal-mode-stage-12-coil-performance-object-type}
+
+\paragraph{Field: Normal Mode Stage 1+2 Coil Performance Object Name}\label{field-normal-mode-stage-12-coil-performance-object-name}
+
+This pair of fields specifies the object type and name for the coil performance object which specifies the DX coil performance for stage 1+2 operation (both stages active) without enhanced dehumidification (normal mode). The only valid performance object type is CoilPerformance:DX:Cooling.
+
+\paragraph{Field: Dehumidification Mode 1 Stage 1 Coil Performance Object Type}\label{field-dehumidification-mode-1-stage-1-coil-performance-object-type}
+
+\paragraph{Field: Dehumidification Mode 1 Stage 1 Coil Performance Object Name}\label{field-dehumidification-mode-1-stage-1-coil-performance-object-name}
+
+This pair of fields specifies the object type and name for the coil performance object which specifies the DX coil performance for stage 1 operation with enhanced dehumidification active. The only valid performance object type is CoilPerformance:DX:Cooling.
+
+\paragraph{Field: Dehumidification Mode 1 Stage 1+2 Coil Performance Object Type}\label{field-dehumidification-mode-1-stage-12-coil-performance-object-type}
+
+\paragraph{Field: Dehumidification Mode 1 Stage 1+2 Coil Performance Object Name}\label{field-dehumidification-mode-1-stage-12-coil-performance-object-name}
+
+This pair of fields specifies the object type and name for the coil performance object which specifies the DX coil performance for stage 1+2 operation (both stages active) with enhanced dehumidification active. The only valid performance object type is CoilPerformance:DX:Cooling.
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-2-000}
+
+This field is optional. It is used to describe where the coil obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the coil will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains (referred to as StarvedWater).
+
+\paragraph{Field: Condensate Collection Water Storage Tank Name}\label{field-condensate-collection-water-storage-tank-name-4}
+
+This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-2-000}
+
+This numeric field contains the capacity of the DX coil s electric evaporative cooler basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the DX coil is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-2-000}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the DX coil is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-2-000}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the DX coil is off.
+
+Following is an example IDF use of the object:
+
+\begin{lstlisting}
+
+Coil:Cooling:DX:TwoStageWithHumidityControlMode,
+  DOAS Cooling Coil,                          !- Name
+  HVACTemplate-Always 1,                      !- Availability Schedule Name
+  DOAS Supply Fan Outlet,                     !- Air Inlet Node Name
+  DOAS Cooling Coil Outlet,                   !- Air Outlet Node Name
+  ,                                           !- Crankcase Heater Capacity
+  ,                                           !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater
+  2,                                          !- Number of Capacity Stages
+  1,                                          !- Number of Enhanced Dehumidification Modes
+  CoilPerformance:DX:Cooling,                 !- Normal Mode Stage 1 Coil Performance Object Type
+  DOAS Standard Perf 1,                       !- Normal Mode Stage 1 Coil Performance Name
+  CoilPerformance:DX:Cooling,                 !- Normal Mode Stage 1+2 Coil Performance Object Type
+  DOAS Standard Perf 1+2,                     !- Normal Mode Stage 1+2 Coil Performance Name
+  CoilPerformance:DX:Cooling,                 !- Dehumidification Mode 1 Stage 1 Coil Performance Object Type
+  DOAS Dehumid Perf 1,                        !- Dehumidification Mode 1 Stage 1 Coil Performance Name
+  CoilPerformance:DX:Cooling,                 !- Dehumidification Mode 1 Stage 1+2 Coil Performance Object Type
+  DOAS Dehumid Perf 1+2;                      !- Dehumidification Mode 1 Stage 1+2 Coil Performance Name
+\end{lstlisting}
+
+\subsection{Coil:Cooling:DX:MultiSpeed}\label{coilcoolingdxmultispeed}
+
+This component models a DX cooling unit with multiple discrete levels of cooling capacity. Depending on input choices, the user can model a single compressor with multiple operating speeds, or a unit with a single cooling coil fed by multiple compressors (e.g., row split or intertwined coil circuiting). Currently, this cooling coil can only be referenced by a AirLoopHVAC:UnitaryHeatPump:AirToAir:Multispeed object. Refer to Coil:Cooling:DX:TwoStageWithHumidityControlMode if the user wishes to model a cooling coil with discrete levels of cooling and the possibility of air bypass during low speed operation (e.g.~face-split coil circuiting), or if cooling coil operation based on dehumidification requirements is desired.
+
+The multispeed DX cooling coil can have from two to four operating speeds. When the coil operates at Speed 1 (the lowest speed), its performance is very similar to the single speed DX coil where the impacts of part-load ratio and latent capacity degradation can be included. When the coil operates at higher speeds (above Speed 1), the linear approximation methodology is applied. The coil outputs at two consecutive speeds are linearly interpolated to meet the required cooling capacity during an HVAC system timestep. When the coil performs above the lowest speed, the user can chose if they want to include part-load ratio and latent capacity degradation impacts at the higher speeds.
+
+The multispeed unit is described by specifying the performance at different operating speeds. Each speed has its own set of input specifications: full load capacity, SHR, COP and air flow rate at rated conditions, along with modifier curves to determine performance when actual operating conditions are different from the rated conditions.
+
+The coil operates to meet the sensible capacity being requested. When this requested capacity is above the sensible capacity of the highest operating speed, the coil runs continuously at the highest speed. When the requested capacity is between the sensible capacities of two consecutive speeds, the unit will operate a portion of the time at each speed to meet the request. When the requested capacity is less than the low speed (Speed 1) capacity, the unit will cycle on/off as needed.
+
+\subsubsection{Inputs}\label{inputs-16-003}
+
+\paragraph{Field: Name}\label{field-name-15-002}
+
+A unique user-assigned name for an instance of a multispeed DX cooling coil. Any reference to this DX coil by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-9-000}
+
+The name of the schedule (ref: Schedule) that denotes whether the DX cooling coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-11}
+
+The name of the HVAC system node from which the DX cooling coil draws its inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-11}
+
+The name of the HVAC system node to which the DX cooling coil sends its outlet air.
+
+\paragraph{Field: Condenser Air Inlet Node Name}\label{field-condenser-air-inlet-node-name-2}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-2}
+
+The type of condenser used by the multispeed DX cooling coil. Valid choices for this input field are AirCooled or EvaporativelyCooled. The default for this field is AirCooled.
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-3-000}
+
+This field is optional. It is used to describe where the coil obtains water used for evaporative cooling. If blank or omitted, then the evaporative cooler will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the coil will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains (referred to as StarvedWater).
+
+\paragraph{Field: Condensate Collection Water Storage Tank Name}\label{field-condensate-collection-water-storage-tank-name-5}
+
+This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
+
+\paragraph{Field: Apply Part Load Fraction to Speeds Greater than 1}\label{field-apply-part-load-fraction-to-speeds-greater-than-1}
+
+This field determines whether part-load impacts on coil energy use are applied when the coil is operating at speeds greater than speed 1. The allowed choices are Yes or No, with the default being No if this field is left blank. Other input fields in this object allow the user to specify a part-load fraction correlation for each speed to account for compressor start up losses (cycle on/off). For the case of a single multi-speed compressor, the part load losses may only be significant when the compressor cycles between speed 1 and off, but the losses may be extremely small when the compressor operates between speed 1 and speed 2 (or between speeds 2 and 3, etc.). In this case, the user may chose to specify NO for this input field to neglect part-load impacts on energy use at higher operating speeds. If part-load impacts on coil energy use are thought to be significant (e.g., interwined cooling coil with multiple compressors feeding individual refrigerant circuits), then the user may chose to specify YES and the part-load fraction correlations specified for speeds 2 through 4 will be applied as appropriate. The selection for this input field does not affect part-load impacts when the compressor cycles between speed 1 and off (i.e., the part-load fraction correlation for speed 1 is always applied).
+
+\paragraph{Field: Apply Latent Degradation to Speeds Greater than 1}\label{field-apply-latent-degradation-to-speeds-greater-than-1}
+
+This field determines whether latent capacity degradation is applied when the coil is operating at speeds greater than speed 1. The allowed choices are Yes or No, with the default being No if this field is left blank. Other input fields in this object allow the user to specify latent capacity degradation at each speed.
+
+The latent capacity degradation model only applies when the ContinuousFanWithCyclingCompressor supply air fan operating mode is specified, to account for moisture evaporation from the wet cooling coil when the compressor cycles off but the supply air fan continues to operate. For the case of a single multi-speed compressor, latent capacity degradation may only be significant when the compressor cycles between speed 1 and off, but the losses may be extremely small when the compressor operates between speed 1 and speed 2 (or between speeds 2 and 3, etc.). In this case, the user may chose to specify NO for this input field to neglect latent capacity degradation impacts at higher operating speeds. If latent capacity degradation is thought to be significant (e.g., interwined or row-split cooling coil with multiple compressors feeding individual refrigerant circuits), then the user may chose to specify YES and the latent capacity degradation model will be applied for speeds 2 through 4 as appropriate. The selection for this input field does not affect latent capacity degradation between speed 1 and off.
+
+\paragraph{Field: Crankcase Heater Capacity}\label{field-crankcase-heater-capacity-2}
+
+This numeric field defines the crankcase heater capacity in Watts. When the outdoor air dry-bulb temperature is below the value specified in the input field Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation (described below), the crankcase heater is enabled during the time that the compressor is not running. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0. To simulate a unit without a crankcase heater, enter a value of 0.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-crankcase-heater-operation-2}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the compressor s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 °C. If this input field is left blank, the default value is 10 °C.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-3-000}
+
+This numeric field contains the capacity of the DX coil s electric evaporative cooler basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the DX coil is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-3-000}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the DX coil is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-3-000}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the DX coil is off.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-000}
+
+This alpha field determines the type of fuel that this cooling coil uses. This field has seven choices: Electricity, NaturalGas, PropaneGas, Coal, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1 and OtherFuel2. The default is NaturalGas.
+
+\paragraph{Field: Number of Speeds}\label{field-number-of-speeds}
+
+This field specifies the number of sets of data being entered for rated specifications, performance curves, evaporative condenser data, latent degradation data, and waste heat specifications for each cooling speed. The rated specifications consist of gross rated capacity, gross rated SHR, gross rated COP, and rated air flow rate. The performance curves consist of a total capacity modifier curve as a function of temperature, total capacity modifier curve as a function of flow fraction, energy input ratio modifier curve as a function of temperature, energy input ratio modifier curve as a function of flow fraction, and part load fraction correlation as a function of part load ratio. The evaporative condenser data consists of effectiveness, condenser air volume flow rate, and rated pump power consumption. The latent degradation data consists of nominal time for condensate removal to begin, ratio of initial moisture evaporation rate and steady-state latent capacity, maximum On/Off cycling rate, and latent capacity time constant. The latent degradation data are only applied if the supply air fan operation mode is specified as ContinuousFanWithCyclingCompressor. The waste heat specifications include the fraction of energy input to the cooling coil at the fully loaded and rated conditions, and a temperature modifier. The minimum number of speeds for cooling is 2 and the maximum number is 4. The number of speeds should be the same as the number of speeds for cooling defined in its parent object (AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed). The first set of performance inputs is for Speed 1 and should be for low speed, and the last set of performance inputs should be for high speed. For example, if only three cooling speeds are defined, the first set should be for low speed (Speed 1), the second set should be for medium speed (Speed 2), and the third set should be for high speed (Speed 3). In this example, any performance inputs for Speed 4 would be neglected (since this input field specifies that the coil only has three cooling speeds).
+
+\paragraph{Field Group: Rated Specification, Performance Curves, Latent Capacity Degradation Inputs, and Evaporative Cooled Condenser Data}\label{field-group-rated-specification-performance-curves-latent-capacity-degradation-inputs-and-evaporative-cooled-condenser-data}
+
+The performance for each cooling speed must be specified as shown below. All inputs for Speed 1 are required first, followed by the inputs for Speed 2, Speed 3 and Speed 4.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Gross Rated Total Cooling Capacity}\label{field-speed-x-gross-rated-total-cooling-capacity}
+
+The total, full load gross cooling capacity (sensible plus latent) in watts of the DX coil unit for Speed \textless{}x\textgreater{} operation at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb\protect\hyperlink{ux5fftn3}{{[}3{]}}, and a cooling coil air flow rate defined by field Rated Air Flow Rate, Speed \textless{}x\textgreater{} below). Capacity should be gross (i.e., the effect of supply air fan heat is NOT accounted for).
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Gross Rated Sensible Heat Ratio}\label{field-speed-x-gross-rated-sensible-heat-ratio}
+
+The sensible heat ratio (SHR = gross sensible capacity divided by gross total cooling capacity) of the DX cooling coil for Speed \textless{}x\textgreater{} operation at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and a cooling coil air flow rate defined by field Rated Air Flow Rate, Speed \textless{}x\textgreater{} below). Both the sensible and total cooling capacities used to define the Rated SHR should be gross (i.e., the effect of supply air fan heat is NOT accounted for).
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Gross Rated Cooling COP}\label{field-speed-x-gross-rated-cooling-cop}
+
+The coefficient of performance is the ratio of the gross total cooling capacity in watts to electrical power input in watts) of the DX cooling coil unit for Speed \textless{}x\textgreater{} operation at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and a cooling coil air flow rate defined by field Rated Air Flow Rate, Speed \textless{}x\textgreater{} below). The input power includes power for the compressor(s) and condenser fan(s) but does not include the power consumption of the supply air fan. The gross COP should NOT account for the supply air fan. If this input field is left blank, the default value is 3.0.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Rated Air Flow Rate}\label{field-speed-x-rated-air-flow-rate}
+
+The volumetric air flow rate for Speed \textless{}x\textgreater{}, in m\(^{3}\) per second, across the DX cooling coil at rated conditions. The rated air volume flow rate for Speed \textless{}x\textgreater{} should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of the gross rated total cooling capacity for Speed \textless{}x\textgreater{}. The gross rated total cooling capacity, gross rated SHR and gross rated COP for Speed \textless{}x\textgreater{} should be performance information for the unit with air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and the rated air volume flow rate defined here.
+
+\paragraph{Field: Speed \textless{}X\textgreater{} Rated Evaporator Fan Power Per Volume Flow Rate}\label{field-speed-x-rated-evaporator-fan-power-per-volume-flow-rate}
+
+This field is the electric power for the evaporator (cooling coil) fan per air volume flow rate through the coil at the rated conditions for Speed \textless{}x\textgreater{} in W/(m3/s). The default value is 773.3 W/(m3/s) (365 W/1000 cfm) if this field is left blank. If a value is entered, it must be \textgreater{} = 0.0 and \textless{} = 1250 W/(m3/s). This value is only used to calculate Seasonal Energy Efficiency Ratio (SEER), and the Standard Rating (Net) Cooling Capacity which will be outputs in the EnergyPlus eio file (ref. EnergyPlus Engineering Reference, Multi-Speed DX Cooling Coil, Standard Ratings). This value is not used for modeling the evaporator (cooling coil) fan during simulations; instead, it is used for calculating SEER and Standard Rating Cooling Capacity to assist the user in verifying their inputs for modeling this type of equipment.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Total Cooling Capacity Function of Temperature Curve Name}\label{field-speed-x-total-cooling-capacity-function-of-temperature-curve-name}
+
+The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity for Speed \textless{}x\textgreater{} as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity for Speed \textless{}x\textgreater{} to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Total Cooling Capacity Function of Flow Fraction Curve Name}\label{field-speed-x-total-cooling-capacity-function-of-flow-fraction-curve-name}
+
+The name of a quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity for Speed \textless{}x\textgreater{} as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate for Speed \textless{}x\textgreater{} (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity for Speed \textless{}x\textgreater{} at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate for Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Temperature Curve Name}\label{field-speed-x-energy-input-ratio-function-of-temperature-curve-name}
+
+The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) for Speed \textless{}x\textgreater{} as a function of the wetbulb temperature of the air entering the cooling coil and the drybulb temperature of the air entering the air-cooled condenser (wetbulb temperature if modeling an evaporative-cooled condenser). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR for Speed \textless{}x\textgreater{} (inverse of rated COP for Speed \textless{}x\textgreater{}) to give the EIR for Speed \textless{}x\textgreater{} at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to a value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-speed-x-energy-input-ratio-function-of-flow-fraction-curve-name}
+
+The name of a quadratic performance curve (Ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) for Speed \textless{}x\textgreater{} as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate for Speed \textless{}x\textgreater{} (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR for Speed \textless{}x\textgreater{} at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate for Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Part Load Fraction Correlation Curve Name}\label{field-speed-x-part-load-fraction-correlation-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity for Speed \textless{}x\textgreater{}). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep for Speed \textless{}x\textgreater{}. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+\begin{lstlisting}
+       PLF > = 0.7     and     PLF > = PLR
+\end{lstlisting}
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional DX cooling coil (Speed \textless{}x\textgreater{}) would be:
+
+\begin{lstlisting}
+       PLF = 0.85 + 0.15(PLR)
+\end{lstlisting}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{lstlisting}
+       PLF = 1.0 + 0.0(PLR)
+\end{lstlisting}
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Nominal Time for Condensate Removal to Begin}\label{field-speed-x-nominal-time-for-condensate-removal-to-begin}
+
+For Speed \textless{}x\textgreater{}, the nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}), and this field as well as the next three input fields for this object must have positive values in order to model latent capacity degradation for Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity}\label{field-speed-x-ratio-of-initial-moisture-evaporation-rate-and-steady-state-latent-capacity}
+
+For Speed \textless{}x\textgreater{}, the ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) for Speed \textless{}x\textgreater{} at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}); and this field, the previous field and the next two fields must have positive values in order to model latent capacity degradation for Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Maximum Cycling Rate}\label{field-speed-x-maximum-cycling-rate}
+
+For Speed \textless{}x\textgreater{}, the maximum on-off cycling rate for the compressor (cycles per hour), which occurs at 50\% run time fraction. Suggested value is 3; zero value means latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}); and this field, the previous two fields and the next field must have positive values in order to model latent capacity degradation for Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Latent Capacity Time Constant}\label{field-speed-x-latent-capacity-time-constant}
+
+For Speed \textless{}x\textgreater{}, the time constant (in seconds) for the cooling coil's latent capacity to reach steady state after startup. Suggested value is 45; zero value means latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}), and this field as well as the previous three input fields for this object must have positive values in order to model latent capacity degradation for Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Rated Waste Heat Fraction of Power Input}\label{field-speed-x-rated-waste-heat-fraction-of-power-input}
+
+The fraction of energy input to the cooling coil that is available as recoverable waste heat at full load and rated conditions for Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Waste Heat Function of Temperature Curve Name}\label{field-speed-x-waste-heat-function-of-temperature-curve-name}
+
+The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the waste heat recovery as a function of outdoor dry-bulb temperature and the entering coil dry-bulb temperature at Speed \textless{}x\textgreater{}. The output of this curve is multiplied by the rated waste heat fraction at specific temperature operating conditions (i.e., at temperatures different from the rating point). The curve is normalized to a value of 1.0 at the rating point. When the fuel type is electricity, this field can remain blank since it is ignored by the program in this instance. When the fuel type is not electricity and the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed does not require waste heat calculations, this field is ignored. If the field is blank, a warning will be issued and simulation continues. When the fuel type is not electricity and the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed requires waste heat calculations, if this field is left blank, the program assumes a constant value of 1 to make simulation continue and a warning will be issued.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Evaporative Condenser Effectiveness}\label{field-speed-x-evaporative-condenser-effectiveness}
+
+The effectiveness of the evaporative condenser at Speed \textless{}x\textgreater{}, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
+
+\begin{equation}
+Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectivenes{s_{Speed1}}} \right)\left( {Tdb,o\,\, - Twb,o} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{cond\\ inlet}\)} = the temperature of the air entering the condenser coil (C)
+
+\emph{T\(_{wb,o}\)} = the wet-bulb temperature of the outdoor air (C)
+
+\emph{T\(_{db,o}\)} = the dry-bulb temperature of the outdoor air (C)
+
+The resulting condenser inlet air temperature is used by the Total Cooling Capacity Modifier Curve, Speed \textless{}x\textgreater{} (function of temperature) and the Energy Input Ratio Modifier Curve, Speed \textless{}x\textgreater{} (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled.
+
+If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve, Speed \textless{}x\textgreater{} (function of temperature) and the Energy Input Ratio Modifier Curve, Speed \textless{}x\textgreater{} (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
+
+If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve, Speed \textless{}x\textgreater{} (function of temperature) and the Energy Input Ratio Modifier Curve, Speed \textless{}x\textgreater{} (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
+
+If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve, Speed \textless{}x\textgreater{} (function of temperature) and the Energy Input Ratio Modifier Curve, Speed \textless{}x\textgreater{} (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves for Speed \textless{}x\textgreater{} must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Evaporative Condenser Air Flow Rate}\label{field-speed-x-evaporative-condenser-air-flow-rate}
+
+The air volume flow rate, in m\(^{3}\) per second, entering the evaporative condenser at Speed \textless{}x\textgreater{}. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000114 m\(^{3}\)/s per watt of rated total cooling capacity for Speed \textless{}x\textgreater{} {[}850 cfm/ton{]}). This field is not used when Condenser Type = Air Cooled.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Rated Evaporative Condenser Pump Power Consumption}\label{field-speed-x-rated-evaporative-condenser-pump-power-consumption}
+
+The rated power of the evaporative condenser water pump in Watts at Speed \textless{}x\textgreater{}. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt {[}15 W/ton{]} of rated total capacity for Speed \textless{}x\textgreater{}). This field is not used when Condenser Type = Air Cooled.
+
+\paragraph{Field: Zone Name for Condenser Placement}\label{field-zone-name-for-condenser-placement-2}
+
+This input field is name of a conditioned or unconditioned zone where the secondary coil (condenser) of DX system or a heat pump is to be placed. This is an optional input field specified only when user desires to reject the condenser heat into a zone. The heat rejected is modeled as sensible internal gain of a secondary zone.
+
+Following is an example input for this multispeed DX cooling coil.
+
+\begin{lstlisting}
+
+Coil:Cooling:DX:MultiSpeed,
+  Heat Pump ACDXCoil 1,       !- Coil Name
+  FanAndCoilAvailSched,       !- Availability Schedule
+  DX Cooling Coil Air Inlet Node,   !- Coil Air Inlet Node
+  Heating Coil Air Inlet Node,         !- Coil Air Outlet Node
+  Outdoor Condenser Air Node,           !- Condenser Air Inlet Node Name
+  AirCooled,                           !- Condenser Type
+  ,                                               !- Name of Water Storage Tank for Supply
+  ,                                               !- Name of Water Storage Tank for Condensate Collection
+  No,                                           !- Apply Part Load Fraction to Speeds greater than 1
+  No,                                           !- Apply latent degradation to Speeds greater than 1
+  200.0,                                     !- Crankcase Heater Capacity {W}
+  10.0,                                       !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation
+  ,                                               !- Basin Heater Capacity {W/K}
+  ,                                               !- Basin Heater Setpoint Temperature {C}
+  ,                                               !- Basin Heater Operating Schedule Name
+  NaturalGas,                           !- Fuel Type
+  4,                                             !- Number of speeds
+  7500,                                       !- Gross Rated Total Cooling Capacity, Speed 1 {W}
+  0.75,                                       !- Gross Rated Sensible Heat Ratio, Speed 1 {dimensionless}
+  3.0,                                         !- Gross Rated Cooling COP, Speed 1 {dimensionless}
+  0.40,                                       !- Rated Air Flow Rate, Speed 1 {m3/s}
+  ,                                               !- Rated Evaporator Fan Power Per Volume Flow Rate, Speed 1 {W/(m3/s)}
+  HPACCoolCapFT Speed 1,     !- Total Cooling Capacity Modifier Curve, Speed 1 (temperature)
+  HPACCoolCapFF Speed 1,     !- Total Cooling Capacity Modifier Curve, Speed 1 (flow fraction)
+  HPACCOOLEIRFT Speed 1,     !- Energy Input Ratio Modifier Curve, Speed 1 (temperature)
+  HPACCOOLEIRFF Speed 1,     !- Energy Input Ratio Modifier Curve, Speed 1 (flow fraction)
+  HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 1 (part load ratio)
+  1000.0,                                   !- Nominal Time for Condensate Removal to Begin, Speed 1 {s}
+  1.5,                                         !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent
+  3.0,                                         !- Maximum ON/OFF Cycling Rate, Speed 1 {cycles/hr}
+  45.0,                                       !- Latent Capacity Time Constant, Speed 1 {s}
+  0.2,                                         !- Rated waste heat fraction of power input, Speed 1 {dimensionless}
+  HAPCCoolWHFT Speed 1,       !- Waste heat modifier curve, Speed 1 (temperature)
+  0.9,                                         !- Evaporative Condenser Effectiveness, Speed 1 {dimensionless}
+  0.05,                                       !- Evaporative Condenser Air Volume Flow Rate, Speed 1 {m3/s}
+  50,                                           !- Evaporative Condenser Pump Rated Power Consumption, Speed 1 {W}
+  17500,                                     !- Gross Rated Total Cooling Capacity, Speed 2 {W}
+  0.75,                                       !- Gross Rated Sensible Heat Ratio, Speed 2 {dimensionless}
+  3.0,                                         !- Gross Rated Cooling COP, Speed 2 {dimensionless}
+  0.85,                                       !- Rated Air Flow Rate, Speed 2 {m3/s}
+  ,                                               !- Rated Evaporator Fan Power Per Volume Flow Rate, Speed 2 {W/(m3/s)}
+  HPACCoolCapFT Speed 2,     !- Total Cooling Capacity Modifier Curve, Speed 2 (temperature)
+  HPACCoolCapFF Speed 2,     !- Total Cooling Capacity Modifier Curve, Speed 2 (flow fraction)
+  HPACCOOLEIRFT Speed 2,     !- Energy Input Ratio Modifier Curve, Speed 2 (temperature)
+  HPACCOOLEIRFF Speed 2,     !- Energy Input Ratio Modifier Curve, Speed 2 (flow fraction)
+  HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 2 (part load ratio)
+  1000.0,                                   !- Nominal Time for Condensate Removal to Begin, Speed 2
+  1.5,                                         !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent
+  3.0,                                         !- Maximum ON/OFF Cycling Rate, Speed 2
+  45.0,                                       !- Latent Capacity Time Constant, Speed 2
+  0.2,                                         !- Rated waste heat fraction of power input, Speed 2 {dimensionless}
+  HAPCCoolWHFT Speed 2,       !- Waste heat modifier curve, Speed 2 (temperature)
+  0.9,                                         !- Evaporative Condenser Effectiveness, Speed 2 {dimensionless}
+  0.1,                                         !- Evaporative Condenser Air Volume Flow Rate, Speed 2 {m3/s}
+  60,                                           !- Evaporative Condenser Pump Rated Power Consumption, Speed 2 {W}
+  25500,                                     !- Gross Rated Total Cooling Capacity, Speed 3 {W}
+  0.75,                                       !- Gross Rated Sensible Heat Ratio, Speed 3 {dimensionless}
+  3.0,                                         !- Gross Rated Cooling COP, Speed 3 {dimensionless}
+  1.25,                                       !- Rated Air Flow Rate, Speed 3 {m3/s}
+  ,                                               !- Rated Evaporator Fan Power Per Volume Flow Rate, Speed 3 {W/(m3/s)}
+  HPACCoolCapFT Speed 3,     !- Total Cooling Capacity Modifier Curve, Speed 3 (temperature)
+  HPACCoolCapFF Speed 3,     !- Total Cooling Capacity Modifier Curve, Speed 3 (flow fraction)
+  HPACCOOLEIRFT Speed 3,     !- Energy Input Ratio Modifier Curve, Speed 3 (temperature)
+  HPACCOOLEIRFF Speed 3,     !- Energy Input Ratio Modifier Curve, Speed 3 (flow fraction)
+  HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 3 (part load ratio)
+  1000.0,                                   !- Nominal Time for Condensate Removal to Begin, Speed 3 {s}
+  1.5,                                         !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent
+  3.0,                                         !- Maximum ON/OFF Cycling Rate, Speed 3 {cycles/hr}
+  45.0,                                       !- Latent Capacity Time Constant, Speed 3 {s}
+  0.2,                                         !- Rated waste heat fraction of power input, Speed 3 {dimensionless}
+  HAPCCoolWHFT Speed 3,       !- Waste heat modifier curve, Speed 3 (temperature)
+  0.9,                                         !- Evaporative Condenser Effectiveness, Speed 3 {dimensionless}
+  0.2,                                         !- Evaporative Condenser Air Volume Flow Rate, Speed 3 {m3/s}
+  80,                                           !- Evaporative Condenser Pump Rated Power Consumption, Speed 3 {W}
+  35500,                                     !- Gross Rated Total Cooling Capacity, Speed 4 {W}
+  0.75,                                       !- Gross Rated Sensible Heat Ratio, Speed 4 {dimensionless}
+  3.0,                                         !- Gross Rated Cooling COP, Speed 4 {dimensionless}
+  1.75,                                       !- Rated Air Flow Rate, Speed 4 {m3/s}
+  ,                                               !- Rated Evaporator Fan Power Per Volume Flow Rate, Speed 4 {W/(m3/s)}
+  HPACCoolCapFT Speed 4,     !- Total Cooling Capacity Modifier Curve, Speed 4 (temperature)
+  HPACCoolCapFF Speed 4,     !- Total Cooling Capacity Modifier Curve, Speed 4 (flow fraction)
+  HPACCOOLEIRFT Speed 4,     !- Energy Input Ratio Modifier Curve, Speed 4 (temperature)
+  HPACCOOLEIRFF Speed 4,     !- Energy Input Ratio Modifier Curve, Speed 4 (flow fraction)
+  HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 4 (part load ratio)
+  1000.0,                                   !- Nominal Time for Condensate Removal to Begin, Speed 4 {s}
+  1.5,                                         !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent                                                     !- Capacity, Speed 4 {dimensionless}
+  3.0,                                         !- Maximum ON/OFF Cycling Rate, Speed 4 {cycles/hr}
+  45.0,                                       !- Latent Capacity Time Constant, Speed 4 {s}
+  0.2,                                         !- Rated waste heat fraction of power input, Speed 4 {dimensionless}
+  HAPCCoolWHFT Speed 4,       !- Waste heat modifier curve, Speed 4 (temperature)
+  0.9,                                         !- Evaporative Condenser Effectiveness, Speed 4 {dimensionless}
+  0.3,                                         !- Evaporative Condenser Air Volume Flow Rate, Speed 4 {m3/s}
+  100;                                         !- Evaporative Condenser Pump Rated Power Consumption, Speed 4 {W}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-12-002}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Electric Power{[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Runtime Fraction {[]}
+\end{itemize}
+
+If not part of AirLoopHVAC:UnitaryHeatPump:AirToAir (if part of a heat pump, crankcase heater is reported only for the heating coil):
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Crankcase Heater Electric Power{[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Crankcase Heater Electric Energy {[}J{]}
+\end{itemize}
+
+Evaporative-cooled condenser:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Sum,Cooling Coil Evaporative Condenser Water Volume{[}m3{]}
+\item
+  HVAC,Average,Cooling Coil Evaporative Condenser Pump Electric Power{[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Evaporative Condenser Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Basin Heater Electric Power{[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Basin Heater Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Cooling Coil Evaporative Condenser Mains Supply Water Volume {[}m3{]}
+\end{itemize}
+
+Additional variables for Coil:Cooling:DX:TwoStageWithHumidityControlMode only:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Stage 2 Runtime Fraction {[]}
+\item
+  HVAC,Average,Cooling Coil Dehumidification Mode {[]}
+\end{itemize}
+
+Additional variables when condensate is collected using a storage tank:
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}
+\item
+  Zone,Meter,Condensate:OnSiteWater {[}m3{]}
+\item
+  HVAC,Sum,Cooling Coil Condensate Volume {[}m3{]}
+\end{itemize}
+
+Additional variables for Coil:Cooling:DX:Multispeed:
+
+If Fuel Type is not Electricity:
+
+\begin{itemize}
+\item
+  HVAC,Average,DX Cooling Coil \textless{}Fuel Type\textgreater{} Power{[}W{]}
+\item
+  HVAC,Sum,DX Cooling Coil \textless{}Fuel Type\textgreater{} Consumption{[}J{]}
+\end{itemize}
+
+\paragraph{}\label{section}
+
+\paragraph{Cooling Coil Total Cooling Rate {[}W{]}}\label{cooling-coil-total-cooling-rate-w-4}
+
+This field is the total (sensible and latent) cooling rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Total Cooling Energy {[}J{]}}\label{cooling-coil-total-cooling-energy-j-4}
+
+This is the total (sensible plus latent) cooling output of the DX coil in Joules over the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = CoolingCoils, Group Key = System (Ref. Output:Meter objects).
+
+\paragraph{Cooling Coil Sensible Cooling Rate {[}W{]}}\label{cooling-coil-sensible-cooling-rate-w-4}
+
+This output is the moist air sensible cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Sensible Cooling Energy {[}J{]}}\label{cooling-coil-sensible-cooling-energy-j-4}
+
+This is the moist air sensible cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Latent Cooling Rate {[}W{]}}\label{cooling-coil-latent-cooling-rate-w-2}
+
+This is the latent cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Latent Cooling Energy {[}J{]}}\label{cooling-coil-latent-cooling-energy-j-2}
+
+This is the latent cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Electric Power {[}W{]}}\label{cooling-coil-electric-power-w}
+
+This output is the electricity consumption rate of the DX coil compressor and condenser fan(s) in Watts. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
+
+\paragraph{Cooling Coil Electric Energy {[}J{]}}\label{cooling-coil-electric-energy-j}
+
+This is the electricity consumption of the DX coil compressor and condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (Ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Cooling Coil Runtime Fraction {[]}}{Cooling Coil Runtime Fraction }}\label{cooling-coil-runtime-fraction-2}
+
+This is the runtime fraction of the DX coil compressor and condenser fan(s) for the timestep being reported.
+
+\paragraph{Cooling Coil Crankcase Heater Electric Power{[}W{]}}\label{cooling-coil-crankcase-heater-electric-powerw}
+
+This is the average electricity consumption rate of the DX coil compressor s crankcase heater in Watts for the timestep being reported. If the DX Cooling Coil is used in a heat pump, the crankcase heater is reported only for the heating coil.
+
+\paragraph{Cooling Coil Crankcase Heater Electric Energy {[}J{]}}\label{cooling-coil-crankcase-heater-electric-energy-j}
+
+This is the electricity consumption of the DX coil compressor s crankcase heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects). This output variable appears only when the DX Cooling Coil is not used as part of a heat pump, otherwise the crankcase heater is reported only for the heating coil.
+
+\paragraph{Cooling Coil Condenser Inlet Temperature {[}C{]}}\label{cooling-coil-condenser-inlet-temperature-c}
+
+This is the inlet air temperature to the condenser coil in degrees C. This value can represent the outdoor air dry-bulb temperature, wet-bulb temperature, or somewhere in between from the weather data being used, depending on the value used in the input field Evaporative Condenser Effectiveness . The temperature reported here is used in the various modifier curves related to temperature (e.g., Total Cooling Capacity Modifier Curve {[}function of temperature{]}). This output variable appears only when the DX Cooling Coil is not used as part of a heat pump, otherwise the crankcase heater is reported only for the heating coil.
+
+\paragraph{Cooling Coil Evaporative Condenser Water Volume {[}m3{]}}\label{cooling-coil-evaporative-condenser-water-volume-m3}
+
+This output is the amount of water used to evaporatively cool the condenser coil inlet air, in cubic meters. This output is also added to a meter with Resource Type = Water, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects). This output variable appears only when the DX Cooling Coil is evaporatively cooled.
+
+\paragraph{Cooling Coil Evaporative Condenser Mains Supply Water Volume {[}m3{]}}\label{cooling-coil-evaporative-condenser-mains-supply-water-volume-m3}
+
+This is the volume of water drawn from mains water service for the evaporatively cooled condenser.
+
+\paragraph{Cooling Coil Evaporative Condenser Pump Electric Power {[}W{]}}\label{cooling-coil-evaporative-condenser-pump-electric-power-w}
+
+This is the average electricity consumption rate of the evaporative condenser water pump in Watts for the timestep being reported. This output variable appears only when the DX Cooling Coil is evaporatively cooled.
+
+\paragraph{Cooling Coil Evaporative Condenser Pump Electric Energy {[}J{]}}\label{cooling-coil-evaporative-condenser-pump-electric-energy-j}
+
+This is the electricity consumption rate of the evaporative condenser water pump in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects). This output variable appears only when the DX Cooling Coil is evaporatively cooled.
+
+\paragraph{\texorpdfstring{Cooling Coil Stage 2 Runtime Fraction {[]}}{Cooling Coil Stage 2 Runtime Fraction }}\label{cooling-coil-stage-2-runtime-fraction}
+
+This is the runtime fraction of the stage 2 DX coil compressor and condenser fan(s) for the timestep being reported. Applicable only for COIL Coil:Cooling:DX:TwoStageWithHumidityControlMode when 2 capacity stages are specified. For 2-stage systems, Cooling Coil Runtime Fraction is the stage 1 runtime fraction. These runtime fractions overlap, because stage 2 will not run unless stage 1 is already running. For example, a system where stage 1 is 60\% of total capacity is passed a load of 70\%. The Cooling Coil Runtime Fraction (stage 1) will be 1.0, and the Cooling Coil Stage 2 Runtime Fraction will be 0.25 {[}(70\%-60\%)/(100\%-60\%){]}.
+
+\paragraph{\texorpdfstring{Cooling Coil Dehumidification Mode {[]}}{Cooling Coil Dehumidification Mode }}\label{cooling-coil-dehumidification-mode}
+
+This is the dehumidification mode for the timestep being reported. Applicable only for Coil:Cooling:DX:TwoStageWithHumidityControlMode when enhanced dehumidification mode is available. A value of 0 indicates normal mode (extra dehumidification not active). A value of 1 indicates dehumidification mode 1 is active. Note that this is an averaged variable, so fractional values are likely to be reported for reporting frequencies longer than ``detailed''.
+
+\paragraph{Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}}\label{cooling-coil-condensate-volume-flow-rate-m3s-4}
+
+\paragraph{Cooling Coil Condensate Volume {[}m3{]}}\label{cooling-coil-condensate-volume-m3-4}
+
+These outputs are the rate and volume of water collected as condensate from the coil. These reports only appear if a water storage tank is named in the input object.
+
+\paragraph{Cooling Coil Evaporative Condenser Mains Supply Water Volume {[}m3{]}}\label{cooling-coil-evaporative-condenser-mains-supply-water-volume-m3-1}
+
+This is the water consumed by the DX Cooling Coil evaporatively cooled condenser that is met by the mains water. This output variable appears only when the DX Cooling Coil is evaporatively cooled.
+
+\paragraph{Cooling Coil Basin Heater Electric Power {[}W{]}}\label{cooling-coil-basin-heater-electric-power-w}
+
+This is the average electricity consumption rate of the basin heater in Watts for the timestep being reported. This output variable appears only when the DX Cooling Coil is evaporatively cooled and the Basin Heater Capacity is greater than 0.
+
+\paragraph{Cooling Coil Basin Heater Electric Energy {[}J{]}}\label{cooling-coil-basin-heater-electric-energy-j}
+
+This is the electricity consumption rate of the basin heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects). This output variable appears only when the DX Cooling Coil is evaporatively cooled and the Basin Heater Capacity is greater than 0.
+
+\paragraph{Cooling Coil \textless{}Fuel Type\textgreater{} Power {[}W{]}}\label{cooling-coil-fuel-type-power-w}
+
+This output variable appears only when using the Coil:Cooling:DX:Multispeed object and a fuel type other than electricity is used. This variable describes the input fuel type power for the cooling coil in Watts, averaged during the timestep being reported.
+
+\paragraph{Cooling Coil \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{cooling-coil-fuel-type-energy-j}
+
+This output variable appears only when using the Coil:Cooling:DX:Multispeed object and a fuel type other than electricity is used. This variable describes the input fuel type consumption for the multispeed cooling coil in the unit of Joules, summed for the timestep being reported. The electric consumption is excluded..This output is added to a meter with Resource Type = \textless{}Fuel Type\textgreater{}, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
+
+Note: \textless{}Fuel Type\textgreater{} in the above two output variables depends on the user specified input for the Fuel Type field. In addition to Electricity, valid fuel types are NaturalGas, Propane, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1 and OtherFuel2.
+
+\subsection{Coil:Cooling:DX:VariableSpeed}\label{coilcoolingdxvariablespeed}
+
+The Variable-Speed DX Cooling Coil is a collection of performance curves that represent the cooling coil at various speed levels. The performance curves should be generated from a Reference Unit data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. On the other hand, the model uses the bypass factor approach to calculate sensible heat transfer rate, similar to the one used in the single-speed DX coil. The number of speed levels can range from 1 to 10. The cooling coil has two indoor air side connections, and one optional condenser air node connection. The user needs to specify a nominal speed level, at which the gross rated total cooling capacity, and rated volumetric air rate are sized. The rated capacity and rated volumetric flow rate represent the real situation in the air loop, and are used to determine and flow rates at various speed levels in the parent objects, e.g.~of AirLoopHVAC:UnitaryHeatCool, ZoneHVAC:PackagedTerminalAirConditioner, AirLoopHVAC:UnitaryHeatPump:AirToAir and ZoneHVAC:PackagedTerminalHeatPump. It shall be mentioned that the performance correction curves, i.e.~the temperature and flow fraction correction curves, should be normalized to the capacity and flow rate at each individual speed and at the rated conditions, similar to the performance curves used in the single-speed DX coil. However, the performance values, e.g.~capacities, COPs, SHRs and flow rates at individual speed levels, should be given regarding a specific unit from the Reference Unit catalog data. In the following content, the statement started with Reference Unit means the actual Reference Unit catalog data. The rated conditions for obtaining the capacities, COPs and SHRs are at indoor dry-bulb temperature of 26.67 ËšC (80 ËšF), wet bulb temperature of 19.44 ËšC (67 ËšF), and the condenser entering air temperature of 35 ËšC (95 ËšF). Some equations are provided below to help explain the function of the various performance curves and data fields.
+
+\subsubsection{Inputs}\label{inputs-17-001}
+
+\paragraph{Field: Name}\label{field-name-16-002}
+
+This alpha field contains the identifying name for the variable-speed cooling coil.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-12}
+
+This alpha field contains the cooling coil load side inlet node name.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-12}
+
+This alpha field contains the cooling coil load side outlet node name.
+
+\paragraph{Field: Number of Speeds}\label{field-number-of-speeds-1}
+
+This numeric field contains the maximum number of speed levels that the module uses. The number of speeds, for which the user input the performance data and curves, should be equal or higher than the maximum number. The performance inputs at higher speed levels are ignored.
+
+\paragraph{Field: Nominal Speed Level}\label{field-nominal-speed-level}
+
+This numeric field defines the nominal speed level, at which the rated capacity and rated air rate are correlated.
+
+\paragraph{Field: Gross Rated Total Cooling Capacity at Selected Nominal Speed Level}\label{field-gross-rated-total-cooling-capacity-at-selected-nominal-speed-level}
+
+This numeric field contains the gross rated total cooling capacity at the nominal speed level. This field is autosizable. The gross rated total cooling capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
+
+\begin{equation}
+{\rm{CapacityScaleFactor}} = \frac{{{\rm{Gross RatedTotalCoolingCapacity}}}}{{{\rm{ReferenceUnitCapacity}}@{\rm{NominalSpeedLevel}}}}
+\end{equation}
+
+And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below,
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{Gross RatedCapacity} @ \rm{SpeedLevel} \left( {\rm{x}} \right) = \\
+    \quad \quad \quad \rm{CapacityScaleFactor} \times \\
+    \quad \quad \quad \rm{ReferenceUnitCapacity} @ {\rm{SpeedLevel}}(\rm{x})
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Rated Air Flow Rate at Selected Nominal Speed Level}\label{field-rated-air-flow-rate-at-selected-nominal-speed-level}
+
+This numeric field contains the rated volumetric air flow rate on the load side of the DX unit, corresponding to the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects. It is recommended that the ratio of the rated volumetric air flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
+
+\begin{equation}
+\rm{AirFlowScaleFactor} = \frac{\rm{RatedVolumetricAirFlowRate}}{\rm{ReferenceUnitVolAirFlowRate} @ \rm{NominalSpeedLevel} \times \rm{CapacityScaleFactor}}
+\end{equation}
+
+And the volumetric air flow rates in the parent objects are calculated as below,
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{LoopVolumetricAirFlowRate} @ \rm{SpeedLevel} \left( \rm{x} \right) = \\
+    \quad \quad \quad \rm{AirFlowScaleFactor} \times \\
+    \quad \quad \quad \rm{ReferenceUnitVolAirFlowRate} @ \rm{SpeedLevel}(\rm{x}) \times \\
+    \quad \quad \quad \rm{CapacityScaleFactor}
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Nominal Time for Condensate Removal to Begin}\label{field-nominal-time-for-condensate-removal-to-begin-1}
+
+This numeric field defines the nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero.
+
+\paragraph{Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity}\label{field-ratio-of-initial-moisture-evaporation-rate-and-steady-state-latent-capacity-1}
+
+This numeric field defines ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero.
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-4}
+
+This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, sensible or latent load/steady-state sensible or latent cooling capacity for Speed 1), in the case that the unit operates under the lowest speed, i.e.~on/off. The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep for Speed 1. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep).
+
+\paragraph{Field: Condenser Air Inlet Node Name}\label{field-condenser-air-inlet-node-name-3}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-3}
+
+The type of condenser used by the DX cooling coil. Valid choices for this input field are AirCooled or EvaporativelyCooled. The default for this field is AirCooled.
+
+\paragraph{Field: Evaporative Condenser Pump Rated Power Consumption}\label{field-evaporative-condenser-pump-rated-power-consumption-1}
+
+The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt {[}15 W/ton{]} of rated total cooling capacity). This field is not used when Condenser Type = Air Cooled.
+
+\paragraph{Field: Crankcase Heater Capacity}\label{field-crankcase-heater-capacity-3}
+
+This numeric field defines the crankcase heater capacity in Watts. When the outdoor air drybulb temperature is below the value specified in the input field Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation (described below), the crankcase heater is enabled during the time that the compressor is not running. If this cooling coil is used as part of an air-to-air heat pump, the crankcase heater defined for this DX cooling coil is ignored and the crankcase heater power defined for the DX heating coil (Ref. Coil:Heating:DX:SingleSpeed) is enabled during the time that the compressor is not running for either heating or cooling. The value for this input field must be greater than or equal to 0, and the default value is 0. To simulate a DX cooling coil without a crankcase heater, enter a value of 0.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-crankcase-heater-operation-3}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the compressor s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 °C, and the default value is 10 °C.
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-4-000}
+
+This field is optional. It is used to describe where the coil obtains water used for evaporative cooling of its condenser. If blank or omitted, then the unit will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, the unit will obtain its water from that tank. If a tank is specified, the unit will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the condenser needs, then the unit will still operate and obtain the rest of the water it needs from the mains (referred to as StarvedWater).
+
+\paragraph{Field: Condensate Collection Water Storage Tank Name}\label{field-condensate-collection-water-storage-tank-name-6}
+
+This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-4}
+
+This numeric field contains the capacity of the DX coil s electric evaporative cooler basin
+
+heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the DX coil is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-4}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the DX coil is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-4}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the DX coil is off.
+
+\paragraph{Field Group: Rated specification, performance curves}\label{field-group-rated-specification-performance-curves}
+
+The performance for each cooling speed must be specified as shown below. They should be directly given from the Reference Unit catalog data. All inputs for Speed 1 are required, followed by the optional inputs for other speeds.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Gross Rated Total Cooling Capacity}\label{field-speed-x-reference-unit-gross-rated-total-cooling-capacity}
+
+This numeric field defines the total, full load gross cooling capacity in watts of the air-to-air cooling coil unit at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0. Capacity should not account for supply air fan heat.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Gross Rated Sensible Heat Ratio}\label{field-speed-x-reference-unit-gross-rated-sensible-heat-ratio}
+
+This numeric field defines sensible heat transfer ratio (SHR = gross sensible cooling capacity divided by gross total cooling capacity) of the cooling coil unit at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0.0 and less than 1.0. This value should be obtained from the Reference Unit data.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Gross Rated Cooling COP}\label{field-speed-x-reference-unit-gross-rated-cooling-cop}
+
+This numeric field defines the coefficient of performance (COP = the gross total cooling capacity in watts divided by electrical power input in watts) of the cooling coil unit at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0. The input power includes power for the compressor(s), condenser fan and accessories, but does not include the supply air fan. The gross COP should Not account for the supply air fan.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Rated Air Flow Rate}\label{field-speed-x-reference-unit-rated-air-flow-rate}
+
+This numeric field defines the volumetric air flow rate, in m\(^{3}\) per second, across the cooling coil at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here should be directly from the Reference Unit data, corresponding to the given cooling capacity and COP at the speed, as above.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Rated Condenser Air Flow Rate}\label{field-speed-x-reference-unit-rated-condenser-air-flow-rate}
+
+This numeric field defines the condenser volumetric air flow rate, in m\(^{3}\) per second, across the condenser coil at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here should be directly from the Reference Unit data. This field is used to calculate water evaporation rate for an evaporatively-cooled condenser. For an air-cooled condenser, this input is not used.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Rated Pad Effectiveness of Evap Precooling}\label{field-speed-x-reference-unit-rated-pad-effectiveness-of-evap-precooling}
+
+This numeric field defines the effectiveness of condenser evaporative precooling pad at rated condition. The values of effectiveness are given at individual speed levels, since varied condenser air flow rates impact the effectiveness.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Total Cooling Capacity Function of Temperature Curve Name}\label{field-speed-x-total-cooling-capacity-function-of-temperature-curve-name-1}
+
+This alpha field defines the name of a bi-quadratic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the both the indoor wet-bulb and source side entering air temperature, from the Reference Unit. The output of this curve is multiplied by the gross rated total cooling capacity at the speed to give the gross total cooling capacity at specific temperature operating conditions (i.e., at an indoor air wet-bulb temperature or outdoor entering air temperature different from the rating point temperature). It should be noted that the curve is normalized to the cooling capacity at Speed\textless{}x\textgreater{} from the Reference Unit data, and have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Total Cooling Capacity Function of Air Flow Fraction Curve Name}\label{field-speed-x-total-cooling-capacity-function-of-air-flow-fraction-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of full load flow at Speed \textless{}x\textgreater{}, from the Reference Unit data). The curve is normalized to have the value of 1.0 when the actual air flow rate equals the design air flow rate, at Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Temperature Curve Name}\label{field-speed-x-energy-input-ratio-function-of-temperature-curve-name-1}
+
+This alpha field defines the name of a bi-quadratic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor air wet-bulb and condenser entering air temperatures The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP at Speed \textless{}x\textgreater{} from the Reference Unit data) to give the EIR at specific temperature operating conditions (i.e., at an indoor air wet-bulb temperature or condenser entering air temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Air Flow Fraction Curve Name}\label{field-speed-x-energy-input-ratio-function-of-air-flow-fraction-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of full load flow, at Speed \textless{}x\textgreater{} from the Reference Unit data). The EIR is the inverse of the COP. This curve is normalized to a value of 1.0 when the actual air flow rate equals the design air flow rate.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Coil:Cooling:DX:VariableSpeed,
+  Heat Pump ACDXCoil 1,                       !- Name
+  DX Cooling Coil Air Inlet Node,   !- Air Inlet Node Name
+  Heating Coil Air Inlet Node,         !- Air Outlet Node Name
+  10.0,                                     !- Number of Speeds {dimensionless}
+  10.0,                                     !- Nominal Speed Level {dimensionless}
+  32000,                                   !- Gross Rated Total Cooling Capacity {W}
+  1.7,                                       !- Rated Air Flow Rate {m3/s}
+  0.0,                                       !- Nominal Time for Condensate to Begin Leaving the Coil {s}
+  0.0,   !- Initial Moisture Evaporation Rate Divided by Steady-State AC Latent Capacity {dimensionless}
+  HPACCOOLPLFFPLR,                     !- Part Load Fraction Correlation Curve Name
+  ,                                      ! - Condenser Air Inlet Node Name
+  AirCooled,                                ! - Condenser Type
+  ,                                      ! - Evaporative Condenser Pump Rated Power Consumption
+  200.0,                                      ! - Crankcase Heater Capacity, {w}
+  10.0,                                     !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
+  ,                               ! - Supply Water Storage Tank Name
+  ,                                ! - Condensate Collection Water Storage Tank Name
+  ,                                             ! - Basin Heater Capacity
+  ,                               ! - Basin Heater Setpoint Temperature
+  ,                                             ! - Basin Heater Operating Schedule Name
+  1524.1,                                 !- Speed 1 Gross Rated Total Cooling Capacity {w}
+  0.75,                                     !- Speed 1 Gross Rated Sensible Heat Ratio {dimensionless}
+  4.0,                                       !- Speed 1 Gross Rated Cooling COP {dimensionless}
+  0.1359072,                           !- Speed 1 Rated Air Flow Rate {m3/s}
+  0.26,                                     ! - Speed 1 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
+  ,                                             ! - Evaporative precooling effectiveness
+  HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
+  1877.9,                                 !- Speed 2 Gross Rated Total Cooling Capacity {w}
+  0.75,                                     !- Speed 2 Gross Rated Sensible Heat Ratio {dimensionless}
+  4.0,                                       !- Speed 2 Gross Rated Cooling COP {dimensionless}
+  0.151008,                             !- Speed 2 Rated Air Flow Rate {m3/s}
+  0.30,                                     ! - Speed 2 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
+  ,                                             ! - Evaporative precooling effectiveness
+  HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
+  2226.6,                                 !- Speed 3 Gross Rated Total Cooling Capacity {w}
+  0.75,                                     !- Speed 3 Gross Rated Sensible Heat Ratio {dimensionless}
+  4.0,                                       !- Speed 3 Gross Rated Cooling COP {dimensionless}
+  0.1661088,                           !- Speed 3 Rated Air Flow Rate {m3/s}
+  0.33,                                     !- Speed 3 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
+  ,                                             !- Evaporative precooling effectiveness
+  HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
+  2911.3,                                 !- Speed 4 Gross Rated Total Cooling Capacity {w}
+  0.75,                                     !- Speed 4 Gross Rated Sensible Heat Ratio {dimensionless}
+  4.0,                                       !- Speed 4 Gross Rated Cooling COP {dimensionless}
+  0.1963104,                           !- Speed 4 Rated Air Flow Rate {m3/s}
+  0.38,                                     !- Speed 4 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
+  ,                                             !- Evaporative precooling effectiveness
+  HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
+  3581.7,                                 !- Speed 5 Gross Rated Total Cooling Capacity {w}
+  0.75,                                     !- Speed 5 Gross Rated Sensible Heat Ratio {dimensionless}
+  4.0,                                       !- Speed 5 Gross Rated Cooling COP {dimensionless}
+  0.226512,                             !- Speed 5 Rated Air Flow Rate {m3/s}
+  0.44,                                     !- Speed 5 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
+  ,                                             !- Evaporative precooling effectiveness
+  HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
+  4239.5,                                 !- Speed 6 Gross Rated Total Cooling Capacity {w}
+  0.75,                                     !- Speed 6 Gross Rated Sensible Heat Ratio {dimensionless}
+  4.0,                                       !- Speed 6 Gross Rated Cooling COP {dimensionless}
+  0.2567136,                           !- Speed 6 Rated Air Flow Rate {m3/s}
+  0.50,                                     ! - Speed 6 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
+  ,                                             ! - Evaporative precooling effectiveness
+  HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
+  4885.7,                                 !- Speed 7 Gross Rated Total Cooling Capacity {w}
+  0.75,                                     !- Speed 7 Gross Rated Sensible Heat Ratio {dimensionless}
+  4.0,                                       !- Speed 7 Gross Rated Cooling COP {dimensionless}
+  0.2869152,                           !- Speed 7 Rated Air Flow Rate {m3/s}
+  0.57,                                     ! - Speed 7 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
+  ,                                             ! - Evaporative precooling effectiveness
+  HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
+  5520.7,                                 !- Speed 8 Gross Rated Total Cooling Capacity {w}
+  0.75,                                     !- Speed 8 Gross Rated Sensible Heat Ratio {dimensionless}
+  4.0,                                       !- Speed 8 Gross Rated Cooling COP {dimensionless}
+  0.3171168,                           !- Speed 8 Rated Air Flow Rate {m3/s}
+  0.63,                                     ! - Speed 8 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
+  ,                                             ! - Evaporative precooling effectiveness
+  HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
+  6144.8,                                 !- Speed 9 Gross Rated Total Cooling Capacity {w}
+  0.75,                                     !- Speed 9 Gross Rated Sensible Heat Ratio {dimensionless}
+  4.0,                                       !- Speed 9 Rated Cooling COP {dimensionless}
+  0.3473184,                           !- Speed 9 Rated Air Flow Rate {m3/s}
+  0.69,                                     ! - Speed 9 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
+  ,                                             ! - Evaporative precooling effectiveness
+  HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
+  6758.0,                                 !- Speed 10 Gross Rated Total Cooling Capacity {w}
+  0.75,                                     !- Speed 10 Gross Rated Sensible Heat Ratio {dimensionless}
+  4.0,                                       !- Speed 10 Gross Rated Cooling COP {dimensionless}
+  0.37752,                               !- Speed 10 Rated Air Flow Rate {m3/s}
+  0.74,                                     ! - Speed 10 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
+  ,                                             ! - Evaporative precooling effectiveness
+  HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF;                 !- Energy Input Ratio Function of Flow Fraction Curve Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-13-001}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Electric Power {[}W{]}
+\item
+  HVAC,Average,Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Coil Source Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Cooling Coil Part Load Ratio {[]}
+\item
+  HVAC,Average, Cooling Coil Runtime Fraction {[]}
+\item
+  HVAC,Average, Cooling Coil Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Cooling Coil Air Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,Cooling Coil Air Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cooling Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,Cooling Coil Upper Speed Level {[]}
+\item
+  HVAC,Average,Cooling Coil Neighboring Speed Levels Ratio {[]}
+\item
+  HVAC,Average,VSAirtoAirHP Recoverable Waste Heat {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Cooling Coil Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Cooling Coil Source Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Crankcase Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Crankcase Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Cooling Coil Condensate Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Coil Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Sum,Cooling Coil Evaporative Condenser Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Coil Evaporative Condenser Mains Water Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Coil Evaporative Condenser Pump Electric Power{[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Evaporative Condenser Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Cooling Coil Electric Power {[}W{]}}\label{cooling-coil-electric-power-w-1}
+
+This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Total Cooling Rate {[}W{]}}\label{cooling-coil-total-cooling-rate-w-5}
+
+The output variable is the average total cooling load provide by the heat pump which includes the sensible and latent load in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Sensible Cooling Rate {[}W{]}}\label{cooling-coil-sensible-cooling-rate-w-5}
+
+The output variable is the average sensible cooling load provide by the heat pump in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Heat Transfer Rate {[}W{]}}\label{cooling-coil-source-side-heat-transfer-rate-w}
+
+The output variable is the average heat rejected to the water at the heat pump condenser in Watts over the timestep being reported.
+
+\paragraph{\texorpdfstring{Cooling Coil Part Load Ratio {[]}}{Cooling Coil Part Load Ratio }}\label{cooling-coil-part-load-ratio}
+
+This output variable is the ratio of the part-load capacity to the steady state capacity of the VSAirtoAirHP coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the VSAirtoAirHP coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
+
+\paragraph{\texorpdfstring{Cooling Coil Runtime Fraction {[]}}{Cooling Coil Runtime Fraction }}\label{cooling-coil-runtime-fraction-3}
+
+This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The runtime fraction, or duty factor, accounts for efficiency losses due to compressor cycling.
+
+\paragraph{Cooling Coil Air Mass Flow Rate {[}kg/s{]}}\label{cooling-coil-air-mass-flow-rate-kgs}
+
+The output variable is the average air mass flow rate on the load side going through the heat pump over the timestep being reported.
+
+\paragraph{Cooling Coil Air Inlet Temperature {[}C{]}}\label{cooling-coil-air-inlet-temperature-c}
+
+The output variable is the average entering air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Cooling Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{cooling-coil-air-inlet-humidity-ratio-kgwaterkgdryair}
+
+The output variable is the average entering air dry humidity ratio over the timestep being reported.
+
+\paragraph{Cooling Coil Air Outlet Temperature {[}C{]}}\label{cooling-coil-air-outlet-temperature-c}
+
+The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Cooling Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{cooling-coil-air-outlet-humidity-ratio-kgwaterkgdryair}
+
+The output variable is the average leaving air dry humidity ratio over the timestep being reported.
+
+\paragraph{\texorpdfstring{Cooling Coil Upper Speed Level {[]}}{Cooling Coil Upper Speed Level }}\label{cooling-coil-upper-speed-level}
+
+The output variable is the average upper speed level, for interpolating performances between two neighboring speed levels.
+
+\paragraph{\texorpdfstring{Cooling Coil Neighboring Speed Levels Ratio {[]}}{Cooling Coil Neighboring Speed Levels Ratio }}\label{cooling-coil-neighboring-speed-levels-ratio}
+
+The output variable is the average speed ratio, for interpolating performances between two neighboring speed levels.
+
+\paragraph{Cooling Coil Electric Energy {[}J{]}}\label{cooling-coil-electric-energy-j-1}
+
+The output variable is the electric consumption of the heat pump in Joules over the timestep being reported.
+
+\paragraph{Cooling Coil Total Cooling Energy {[}J{]}}\label{cooling-coil-total-cooling-energy-j-5}
+
+The output variable is the total cooling output of the coil in Joules over the timestep being reported.
+
+\paragraph{Cooling Coil Sensible Cooling Energy {[}J{]}}\label{cooling-coil-sensible-cooling-energy-j-5}
+
+The output variable is the total sensible cooling output of the coil in Joules over the timestep being reported
+
+\paragraph{Cooling Coil Latent Cooling Energy {[}J{]}}\label{cooling-coil-latent-cooling-energy-j-3}
+
+\paragraph{Cooling Coil Latent Cooling Rate {[}W{]}}\label{cooling-coil-latent-cooling-rate-w-3}
+
+These output variables are the total latent cooling output of the coil in Joules or Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Heat Transfer Energy {[}J{]}}\label{cooling-coil-source-side-heat-transfer-energy-j-2}
+
+The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported.
+
+\paragraph{Cooling Coil Crankcase Heater Electric Power {[}W{]}}\label{cooling-coil-crankcase-heater-electric-power-w}
+
+The output variable is the average power used for crankcase heater, in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Crankcase Heater Electric Energy {[}J{]}}\label{cooling-coil-crankcase-heater-electric-energy-j-1}
+
+The output variable is the total electric energy usage of the coil for crankcase heater, in Joules over the timestep being reported.
+
+\paragraph{Cooling Coil Condensate Volume Flow Rate {[}m3/s{]}}\label{cooling-coil-condensate-volume-flow-rate-m3s-5}
+
+The output variable is the average water condensate volumetric flow rate from the cooling coil, in m\(^{3}\)/s over the timestep being reported, if choosing to use CondensatetoTank.
+
+\paragraph{Cooling Coil Condensate Volume {[}m3{]}}\label{cooling-coil-condensate-volume-m3-5}
+
+The output variable is the total water condensate volume from the cooling coil, in m\(^{3}\) over the timestep being reported.
+
+\paragraph{Cooling Coil Condenser Inlet Temperature {[}C{]}}\label{cooling-coil-condenser-inlet-temperature-c-1}
+
+The output variable is the average air temperature entering the condenser coil, in °C over the timestep being reported.
+
+\paragraph{Cooling Coil Evaporative Condenser Water Volume {[}m3{]}}\label{cooling-coil-evaporative-condenser-water-volume-m3-1}
+
+The output variable is the total water volume consumed for condenser evaporative pre-cooling, in m\(^{3}\) over the timestep being reported.
+
+\paragraph{Cooling Coil Evaporative Condenser Mains Water Volume {[}m3{]}}\label{cooling-coil-evaporative-condenser-mains-water-volume-m3}
+
+The output variable is the total water volume for condenser evaporative pre-cooling, obtained from the Mains Water supply, in m\(^{3}\) over the timestep being reported.
+
+\paragraph{Cooling Coil Evaporative Condenser Pump Electric Power{[}W{]}}\label{cooling-coil-evaporative-condenser-pump-electric-powerw}
+
+The output variable is the average power consumption rate of the evaporative condenser pump, in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Evaporative Condenser Pump Electric Energy {[}J{]}}\label{cooling-coil-evaporative-condenser-pump-electric-energy-j-1}
+
+The output variable is the total power consumption of the evaporative condenser pump, in Joules over the timestep being reported.
+
+\paragraph{Cooling Coil Basin Heater Electric Power {[}W{]}}\label{cooling-coil-basin-heater-electric-power-w-1}
+
+The output variable is the average power consumption rate by the basin heater, in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Basin Heater Electric Energy {[}J{]}}\label{cooling-coil-basin-heater-electric-energy-j-1}
+
+The output variable is the total power consumption by the basin heater, in Joules over the timestep being reported.
+
+\subsection{CoilPerformance:DX:Cooling}\label{coilperformancedxcooling}
+
+This coil performance object is used to specify DX coil performance for one mode of operation for a Coil:Cooling:DX:TwoStageWithHumidityControlMode. A single Coil:Cooling:DX:TwoStageWithHumidityControlMode object will reference one to four CoilPerformance:DX:Cooling objects depending on the number of available stages and dehumidification modes as specified in the two stage DX object. For example, a standard 2-stage DX system will use two of these performance objects, one to defined the capacity and performance for stage 1 operation, and a second one for stage 1+2 (both stages active) operation. In nearly all cases, the Rated Air Volume Flow Rate will be the same for all performance objects associated with a given multimode DX coil. If bypass is specified, the Rated Air Volume Flow Rate includes both the bypassed flow and the flow through the active coil.
+
+This DX coil model is identical to Coil:Cooling:DX:SingleSpeed with addition of bypass and multi-stage capabilities. This DX cooling coil model and input are quite different from that for the heating and cooling water coils. The simple water coils use an NTU-effectiveness heat exchanger model. The single speed DX coil model uses performance information at rated conditions along with curve fits for variations in total capacity, energy input ratio and part-load fraction to determine performance at part-load conditions. Sensible/latent capacity splits are determined by the rated sensible heat ratio (SHR) and the apparatus dewpoint/bypass factor (ADP/BF) approach. This approach is analogous to the NTU-effectiveness calculations used for sensible-only heat exchanger calculations, extended to a cooling and dehumidifying coil.
+
+An alternative to ADP/BF method for sensible/latent capacity split is to use SHR modifier curves for temperature and flow fraction. These two optional input fields are used only when a user specified SHR calculation method desired over the (ADP/BF) method. Sensible heat ratio calculated using these two SHR modifier curves override the value calculated by ADP/BF method. See section SHR Calculation Using User Specified SHR Modifier Curves in the EnergyPlus Engineering Document for further details.
+
+The DX cooling coil input requires the gross rated total cooling capacity, the gross rated SHR, the gross rated COP, the rated air volume flow rate, and the fraction of air flow which is bypassed around the coil. The first 4 inputs determine the coil performance at the rating point (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb and air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb). The rated air volume flow rate (less any bypassed fraction) should be between .00004027 m\(^{3}\)/s and .00006041 m\(^{3}\)/s per watt of gross rated total cooling capacity (300 to 450 cfm/ton). The rated volumetric air flow to gross total cooling capacity ratio for 100\% dedicated outdoor air (DOAS) application DX cooling coils should be between 0.00001677 (m3/s)/W (125 cfm/ton) and 0.00003355 (m3/s)/W (250 cfm/ton).
+
+This model requires 5 curves as follows:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  The total cooling capacity modifier curve (function of temperature) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures).
+\item
+  The total cooling capacity modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating.
+\item
+  The energy input ratio (EIR) modifier curve (function of temperature) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures).
+\item
+  The energy input ratio (EIR) modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating.
+\item
+  The part load fraction correlation (function of part load ratio) is a quadratic or cubic curve with the independent variable being part load ratio (sensible cooling load / steady-state sensible cooling capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The curve should be normalized to a value of 1.0 when the part-load ratio equals 1.0 (i.e., the compressor(s) run continuously for the simulation timestep).
+\end{enumerate}
+
+The curves are simply specified by name. Curve inputs are described in the curve manager section of this document (see Performance Curves in this document).
+
+The next four input fields are optional and relate to the degradation of latent cooling capacity when the supply air fan operates continuously while the cooling coil/compressor cycle on and off to meet the cooling load. The fan operating mode is either considered to be constant (e.g.~CoilSystem:Cooling:DX) or can be scheduled in the parent object (e.g.~AirLoopHVAC:UnitaryHeatCool). When scheduled, the schedule value must be greater than 0 to calculate degradation of latent cooling capacity. At times when the parent object s supply air fan operating mode schedule is 0, latent degradation will be ignored. When used, these next four input fields must all have positive values in order to model latent capacity degradation.
+
+The next input specifies the outdoor air node used to define the conditions of the air entering the outdoor condenser. If this field is not blank, the node name specified must be listed in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor temperature from the weather data. Alternately, the node name must be specified in an OutdoorAir:NodeList object where the outdoor temperature entering the condenser is taken directly from the weather data. This field may also be left blank, if this is the case then the outdoor temperature entering the condenser is taken directly from the weather data.
+
+The next input describes the type of outdoor condenser coil used with the DX cooling coil (Air Cooled or Evap Cooled). The following three inputs are required when modeling an evaporative-cooled condenser: evaporative condenser effectiveness, evaporative condenser air volume flow rate, and the power consumed by the evaporative condenser pump. See section DX Cooling Coil Model in the EnergyPlus Engineering Document for further details regarding this model.
+
+\subsubsection{Inputs}\label{inputs-18-001}
+
+\paragraph{Field: Name}\label{field-name-17-001}
+
+This alpha field is a unique user-assigned name for an instance of DX cooling coil performance. Any reference to this DX coil performance object by another object will use this name.
+
+\paragraph{Field: Gross Rated Total Cooling Capacity}\label{field-gross-rated-total-cooling-capacity-2}
+
+The total, full load gross cooling capacity (sensible plus latent) in watts of the DX coil unit at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb\protect\hyperlink{ux5fftn4}{{[}4{]}}, and a cooling coil air flow rate defined by field rated air flow rate below). Capacity should be gross (i.e., the effect of supply air fan heat is NOT accounted for).
+
+\paragraph{Field: Gross Rated Sensible Heat Ratio}\label{field-gross-rated-sensible-heat-ratio-1}
+
+The sensible heat ratio (SHR = gross sensible capacity divided by gross total cooling capacity) of the DX cooling coil at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and a cooling coil air flow rate defined by field rated air flow rate below). Both the sensible and total cooling capacities used to define the Rated SHR should be gross (i.e., the effect of supply air fan heat is NOT accounted for).
+
+\paragraph{Field: Gross Rated Cooling COP}\label{field-gross-rated-cooling-cop-1}
+
+The coefficient of performance is the ratio of the gross total cooling capacity in watts to electrical power input in watts) of the DX cooling coil unit at rated conditions (air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/ 23.9 °C wetbulb, and a cooling coil air flow rate defined by field rated air flow rate below). The input power includes electric power for the compressor(s) and condenser fan(s) but does not include the power consumption of the supply air fan. If this input field is left blank, the default value is 3.0.
+
+\paragraph{Field: Rated Air Flow Rate}\label{field-rated-air-flow-rate-3}
+
+The air volume flow rate, in m\(^{3}\) per second, across the DX cooling coil at rated conditions. The gross rated total cooling capacity, gross rated SHR and gross rated COP should be performance information for the unit with air entering the cooling coil at 26.7 °C drybulb/19.4 °C wetbulb, air entering the outdoor condenser coil at 35 °C drybulb/23.9 °C wetbulb, and the rated air volume flow rate defined here.
+
+\paragraph{Field: Fraction of Air Flow Bypassed Around Coil}\label{field-fraction-of-air-flow-bypassed-around-coil}
+
+This numeric field specifies the fraction of the Rated Air Volume Flow Rate which bypasses the active cooling coil for this performance mode. The remaining portion of the flow should be between 0.00004027 m3/s and .00006041 m3/s per watt of gross rated total cooling capacity (300 to 450 cfm/ton) for this performance mode. For DOAS applications the remaining portion of rated air volume flow rate should be between 0.00001677 m\(^{3}\)/s and 0.00003355 m\(^{3}\)/s per watt of gross rated total cooling capacity (125 to 250 cfm/ton). This is used to model face-split coils on multi-stage units or bypass dampers. If total flow rate varies during simulation, the same fraction is bypassed. This input may range from 0.0 to \textless{}1.0. The default is 0.0. For a multi-stage face-split coil in which stage 1 is 60\% of total capacity, this field would be set to 0.4 for the Stage 1 performance and set to 0.0 for the Stage 1+2 performance. For a DX system which activates a bypass damper for improved dehumidification, this field would be set to 0.0 for normal mode performance and set to something greater than zero for enhanced dehumidification mode performance.
+
+\paragraph{Field: Total Cooling Capacity Function of Temperature Curve Name}\label{field-total-cooling-capacity-function-of-temperature-curve-name-2}
+
+The name of a \textbf{biquadratic} performance curve (ref: Performance Curves) that parameterizes the variation of the total gross cooling capacity as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to have the value of 1.0 at the rating point.
+
+\paragraph{Field: Total Cooling Capacity Function of Flow Fraction Curve Name}\label{field-total-cooling-capacity-function-of-flow-fraction-curve-name-2}
+
+The name of a \textbf{quadratic} or \textbf{cubic} performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
+
+\paragraph{Field: Energy Input Ratio Function of Temperature Curve Name}\label{field-energy-input-ratio-function-of-temperature-curve-name-2}
+
+The name of a \textbf{biquadratic} performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to a value of 1.0 at the rating point.
+
+\paragraph{Field: Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-energy-input-ratio-function-of-flow-fraction-curve-name-2}
+
+The name of a \textbf{quadratic} or \textbf{cubic} performance curve (Ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate.
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-5}
+
+This alpha field defines the name of a \textbf{quadratic} or \textbf{cubic} performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
+
+\begin{lstlisting}
+       PLF = 0.85 + 0.15(PLR)
+\end{lstlisting}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{lstlisting}
+       PLF = 1.0 + 0.0(PLR)
+\end{lstlisting}
+
+\paragraph{Field: Nominal Time for Condensate Removal to Begin}\label{field-nominal-time-for-condensate-removal-to-begin-2}
+
+The nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}), and this field as well as the next three input fields for this object must have positive values in order to model latent capacity degradation.
+
+\paragraph{Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity}\label{field-ratio-of-initial-moisture-evaporation-rate-and-steady-state-latent-capacity-2}
+
+Ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}); and this field, the previous field and the next two fields must have positive values in order to model latent capacity degradation.
+
+\paragraph{Field: Maximum Cycling Rate}\label{field-maximum-cycling-rate-1}
+
+The maximum on-off cycling rate for the compressor (cycles per hour), which occurs at 50\% run time fraction. Suggested value is 3; zero value means latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}); and this field, the previous two fields and the next field must have positive values in order to model latent capacity degradation.
+
+\paragraph{Field: Latent Capacity Time Constant}\label{field-latent-capacity-time-constant-1}
+
+Time constant (in seconds) for the cooling coil's latent capacity to reach steady state after startup. Suggested value is 45; zero value means latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other parent objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects {[}e.g., AirloopHVAC:UnitaryHeatCool{]}), and this field as well as the previous three input fields for this object must have positive values in order to model latent capacity degradation.
+
+\paragraph{Field: Condenser Air Inlet Node Name}\label{field-condenser-air-inlet-node-name-4}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-4}
+
+The type of condenser used by the DX cooling coil. Valid choices for this input field are \textbf{AirCooled} or \textbf{EvaporativelyCooled}. The default for this field is \textbf{AirCooled}.
+
+\paragraph{Field: Evaporative Condenser Effectiveness}\label{field-evaporative-condenser-effectiveness-1}
+
+The effectiveness of the evaporative condenser, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
+
+\begin{equation}
+Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectiveness} \right)\left( {Tdb,o\,\, - Twb,o} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{cond\\ inlet}\)} = the temperature of the air entering the condenser coil (C)
+
+\emph{T\(_{wb,o}\)} = the wet-bulb temperature of the outdoor air (C)
+
+\emph{T\(_{db,o}\)} = the dry-bulb temperature of the outdoor air (C)
+
+The resulting condenser inlet air temperature is used by the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled.
+
+If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
+
+If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
+
+If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
+
+\paragraph{Field: Evaporative Condenser Air Flow Rate}\label{field-evaporative-condenser-air-flow-rate-1}
+
+The air volume flow rate, in m\(^{3}\) per second, entering the evaporative condenser. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000144 m\(^{3}\)/s per watt of rated total cooling capacity {[}850 cfm/ton{]}). This field is not used when Condenser Type = Air Cooled.
+
+\paragraph{Field: Evaporative Condenser Pump Rated Power Consumption}\label{field-evaporative-condenser-pump-rated-power-consumption-2}
+
+The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt {[}15 W/ton{]} of rated total cooling capacity). This field is not used when Condenser Type = AirCooled.
+
+\paragraph{Field: Sensible Heat Ratio Function of Temperature Curve Name}\label{field-sensible-heat-ratio-function-of-temperature-curve-name-2}
+
+The name of a biquadratic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of DX cooling coil entering air wet-bulb and dry-bulb temperatures. The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of flow fraction) to give the SHR at the specific coil entering air temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 at the rated condition. This input field is optional.
+
+\paragraph{Field: Sensible Heat Ratio Function of Flow Fraction Curve Name}\label{field-sensible-heat-ratio-function-of-flow-fraction-curve-name-2}
+
+The name of a quadratic or cubic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of temperature) to give the SHR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This input field is optional.
+
+Following is an example input for a Coil:Cooling:DX:TwoStageWithHumidityControlMode with 2 capacity stages and one enhanced dehumidification mode so it requires four CoilPerformance:DX:Cooling objects.
+
+\begin{lstlisting}
+
+Coil:Cooling:DX:TwoStageWithHumidityControlMode,
+  DXSystem 1 Cooling Coil, !- Coil Name
+  OfficeHeatCoolAvail,         !- Availability Schedule
+  DXSystem 1 Mixed Air Node,   !- Coil Air Inlet Node
+  DXSystem 1 Fan Air Inlet Node,   !- Coil Air Outlet Node
+  ,                                               !- Crankcase Heater Capacity {W}
+  ,                                               !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
+  2,                                             !- Number of Capacity Stages
+  1,                                             !- Number of Enhanced Dehumidification Modes
+  CoilPerformance:DX:Cooling,   !- Normal Mode Stage 1 Coil Performance Object Type
+  DXSystem 1 DX Coil Standard Mode-Stage 1,   !- Normal Mode Stage 1 Coil Performance Object Name
+  CoilPerformance:DX:Cooling,   !- Normal Mode Stage 1+2 Coil Perf Object Type
+  DXSystem 1 DX Coil Standard Mode-Stage 1&2,   !- Normal Mode Stage 1+2 Coil Perf Object Name
+  CoilPerformance:DX:Cooling,   !- Dehumid Mode 1 Stage 1 Coil Perf Object Type
+  DXSystem 1 DX Coil SubCoolReheat Mode-Stage 1,   !- Dehumid Mode 1 Stage 1 Coil Perf Object Name
+  CoilPerformance:DX:Cooling,   !- Dehumid Mode 1 Stage 1+2 Coil Perf Object Type
+  DXSystem 1 DX Coil SubCoolReheat Mode-Stage 1&2;   !- Dehumid Mode 1 Stage 1+2 Coil Perf Object Name
+
+
+  CoilPerformance:DX:Cooling,
+  DXSystem 1 DX Coil Standard Mode-Stage 1,   !- Coil Performance Specification Name
+  21327.57812,                         !- Gross Rated Total Cooling Capacity {W}
+  0.68,                                       !- Gross Rated Sensible Heat Ratio
+  3.56,                                       !- Gross Rated Cooling COP
+  1.695372105,                         !- Rated Air Flow Rate {m3/s}
+  0.4,                                         !- Fraction of Air Flow Bypassed Around Coil
+  HPACCoolCapFT,                     !- Total Cooling Capacity Modifier Curve (function of temperature)
+  HPACCoolCapFFF,                   !- Total Cooling Capacity Modifier Curve (function of flow fraction)
+  HPACCOOLEIRFT,                     !- Energy Input Ratio Modifier Curve (function of temperature)
+  HPACCOOLEIRFFF,                   !- Energy Input Ratio Modifier Curve (function of flow fraction)
+  HPACCOOLPLFFPLR,                 !- Part Load Fraction Correlation (function of part load ratio)
+  1000,                                       !- Nominal Time for Condensate Removal to Begin {s}
+  1.5, !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity {dimensionless}
+  3,                                             !- Maximum ON/OFF Cycling Rate {cycles/hr}
+  45,                                           !- Latent Capacity Time Constant {s}
+  ,                                               !- Condenser Air Inlet Node Name
+  ,                                               !- Condenser Type
+  ,                                               !- Evaporative Condenser Effectiveness
+  ,                                               !- Evaporative Condenser Air Flow Rate
+  ,                                               !- Evaporative Condenser Pump Rated Power Consumption
+  DOAS DX Coil SHR-FT,         !- Sensible Heat Ratio Function of Temperature Curve Name
+  DOAS DX Coil SHR-FF;         !- Sensible Heat Ratio Function of Flow Fraction Curve Name
+
+
+  CoilPerformance:DX:Cooling,
+  DXSystem 1 DX Coil Standard Mode-Stage 1&2,   !- Coil Performance Specification Name
+  35545.96484,                         !- Gross Rated Total Cooling Capacity {W}
+  0.68,                                       !- Gross Rated Sensible Heat Ratio
+  3.56,                                       !- Gross Rated Cooling COP
+  1.695372105,                         !- Rated Air Flow Rate {m3/s}
+  0.0,                                         !- Fraction of Air Flow Bypassed Around Coil
+  HPACCoolCapFT,                     !- Total Cooling Capacity Modifier Curve (function of temperature)
+  HPACCoolCapFFF,                   !- Total Cooling Capacity Modifier Curve (function of flow fraction)
+  HPACCOOLEIRFT,                     !- Energy Input Ratio Modifier Curve (function of temperature)
+  HPACCOOLEIRFFF,                   !- Energy Input Ratio Modifier Curve (function of flow fraction)
+  HPACCOOLPLFFPLR,                 !- Part Load Fraction Correlation (function of part load ratio)
+  1000,                                       !- Nominal Time for Condensate Removal to Begin {s}
+  1.5, !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity {dimensionless}
+  3,                                             !- Maximum ON/OFF Cycling Rate {cycles/hr}
+  45,                                           !- Latent Capacity Time Constant {s}
+  ,                                               !- Condenser Air Inlet Node Name
+  ,                                               !- Condenser Type
+  ,                                               !- Evaporative Condenser Effectiveness
+  ,                                               !- Evaporative Condenser Air Flow Rate
+  ,                                               !- Evaporative Condenser Pump Rated Power Consumption
+  DOAS DX Coil SHR-FT,         !- Sensible Heat Ratio Function of Temperature Curve Name
+  DOAS DX Coil SHR-FF;         !- Sensible Heat Ratio Function of Flow Fraction Curve Name
+
+
+  CoilPerformance:DX:Cooling,
+  DXSystem 1 DX Coil SubCoolReheat Mode-Stage 1,   !- Coil Performance Specification Name
+  19962.61328,                         !- Gross Rated Total Cooling Capacity (gross) {W}
+  0.60,                                       !- Gross Rated SHR
+  3.31,                                       !- Gross Rated Cooling COP
+  1.695372105,                         !- Rated Air Flow Rate {m3/s}
+  0.4,                                         !- Fraction of Air Flow Bypassed Around Coil
+  SubCoolReheatCoolCapFT,   !- Total Cooling Capacity Modifier Curve (function of temperature)
+  SubCoolReheatCoolCapFFF, !- Total Cooling Capacity Modifier Curve (function of flow fraction)
+  SubCoolReheatCOOLEIRFT,   !- Energy Input Ratio Modifier Curve (function of temperature)
+  SubCoolReheatCoolEIRFFF, !- Energy Input Ratio Modifier Curve (function of flow fraction)
+  SubCoolReheatCoolPLFFPLR, !- Part Load Fraction Correlation (function of part load ratio)
+  1000,                                       !- Nominal Time for Condensate Removal to Begin {s}
+  1.5, !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity {dimensionless}
+  3,                                             !- Maximum ON/OFF Cycling Rate {cycles/hr}
+  45,                                           !- Latent Capacity Time Constant {s}
+  ,                                               !- Condenser Air Inlet Node Name
+  ,                                               !- Condenser Type
+  ,                                               !- Evaporative Condenser Effectiveness
+  ,                                               !- Evaporative Condenser Air Flow Rate
+  ,                                               !- Evaporative Condenser Pump Rated Power Consumption
+  DOAS DX Coil SHR-FT,         !- Sensible Heat Ratio Function of Temperature Curve Name
+  DOAS DX Coil SHR-FF;         !- Sensible Heat Ratio Function of Flow Fraction Curve Name
+
+
+  CoilPerformance:DX:Cooling,
+  DXSystem 1 DX Coil SubCoolReheat Mode-Stage 1&2,   !- Coil Performance Specification Name
+  33271.01953,                         !- Gross Rated Total Cooling Capacity (gross) {W}
+  0.60,                                       !- Gross Rated SHR
+  3.31,                                       !- Gross Rated Cooling COP
+  1.695372105,                         !- Rated Air Flow Rate {m3/s}
+  0.0,                                         !- Fraction of Air Flow Bypassed Around Coil
+  SubCoolReheatCoolCapFT,   !- Total Cooling Capacity Modifier Curve (function of temperature)
+  SubCoolReheatCoolCapFFF, !- Total Cooling Capacity Modifier Curve (function of flow fraction)
+  SubCoolReheatCOOLEIRFT,   !- Energy Input Ratio Modifier Curve (function of temperature)
+  SubCoolReheatCoolEIRFFF, !- Energy Input Ratio Modifier Curve (function of flow fraction)
+  SubCoolReheatCoolPLFFPLR, !- Part Load Fraction Correlation (function of part load ratio)
+  1000,                                       !- Nominal Time for Condensate Removal to Begin {s}
+  1.5, !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity {dimensionless}
+  3,                                             !- Maximum ON/OFF Cycling Rate {cycles/hr}
+  45,                                           !- Latent Capacity Time Constant {s}
+  ,                                               !- Condenser Air Inlet Node Name
+  ,                                               !- Condenser Type
+  ,                                               !- Evaporative Condenser Effectiveness
+  ,                                               !- Evaporative Condenser Air Flow Rate
+  ,                                               !- Evaporative Condenser Pump Rated Power Consumption
+  DOAS DX Coil SHR-FT,         !- Sensible Heat Ratio Function of Temperature Curve Name
+  DOAS DX Coil SHR-FF;         !- Sensible Heat Ratio Function of Flow Fraction Curve Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-14-001}
+
+The CoilPerformance:DX:Cooling object does not have specific output variables. To request reports, use the parent object Coil:Cooling:DX:TwoStageWithHumidityControlMode output variable options (ref. DX Cooling Coil Outputs). When requesting specific output variables by name, use the name of the parent object as the Key Value for Output:Variable reporting objects (ref. Output:Variable object). The name of the CoilPerformance:DX:Cooling object cannot be used as a Key Value in the Output:Variable object.
+
+\subsection{Coil:Heating:DX:SingleSpeed}\label{coilheatingdxsinglespeed}
+
+The single speed heating DX coil model uses performance information at rated conditions along with curve fits for variations in total capacity, energy input ratio and part load fraction to determine performance at part-load conditions. The impacts of various defrost strategies (reverse cycle, resistive, timed or on-demand) are modeled based on a combination of user inputs and empirical models taken from the air-to-air heat pump algorithms in DOE-2.1E.
+
+The single speed heating DX coil input requires an availability schedule, the gross rated heating capacity, the gross rated COP and the rated air volume flow rate. The latter 3 inputs determine the coil performance at the rating point (outdoor air dry-bulb temperature of 8.33 C, outdoor air wet-bulb temperature of 6.11 C, coil entering air dry-bulb temperature of 21.11 C, coil entering air wet-bulb temperature of 15.55 C). The rated air volume flow rate should be between .00004027 m\(^{3}\)/s and .00006041 m\(^{3}\)/s per watt of gross rated heating capacity.
+
+Up to 6 curves are required depending on the defrost strategy selected.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  The heating capacity modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the gross rated heating capacity to give the gross heating capacity at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
+\item
+  The heating capacity modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating.
+\item
+  The energy input ratio (EIR) modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
+\item
+  The energy input ratio (EIR) modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating.
+\item
+  The part load fraction correlation (function of part load ratio) is a quadratic or cubic curve with the independent variable being part load ratio (sensible heating load / steady-state heating capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the effective EIR for a given simulation timestep. The part load fraction correlation accounts for efficiency losses due to compressor cycling.
+\item
+  The defrost energy input ratio (EIR) modifier curve (function of temperature) is a bi-quadratic curve with two independent variables: outdoor air dry-bulb temperature and the heating coil entering air wet-bulb temperature. The output of this curve is multiplied by the heating coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the coil is operating. This curve is only required when a reverse-cycle defrost strategy is specified.
+\end{enumerate}
+
+The curves are simply specified by name. Curve inputs are described in the curve manager section of this document (ref. Performance Curves).
+
+The next input item for the coil is the supply air fan operation mode. Either the supply air fan runs continuously while the DX coil cycles on/off, or the fan and coil cycle on/off together. The next two inputs define the minimum outdoor dry-bulb temperature that the heat pump compressor will operate and the maximum outdoor dry-bulb temperature for defrost operation. Crankcase heater capacity and cutout temperature are entered in the following two inputs. The final four inputs cover the type of defrost strategy (reverse-cycle or resistive), defrost control (timed or on-demand), the fractional defrost time period (timed defrost control only), and the resistive defrost heater capacity if a resistive defrost strategy is selected.
+
+\subsubsection{Inputs}\label{inputs-19-001}
+
+\paragraph{Field: Name}\label{field-name-18-001}
+
+This alpha field defines a unique user-assigned name for an instance of a DX heating coil. Any reference to this DX heating coil by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-10-000}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the DX heating coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Gross Rated Heating Capacity}\label{field-gross-rated-heating-capacity-2}
+
+This numeric field defines the total, full load gross heating capacity in watts of the DX coil unit at rated conditions (outdoor air dry-bulb temperature of 8.33 C, outdoor air wet-bulb temperature of 6.11 C, heating coil entering air dry-bulb temperature of 21.11 C, heating coil entering air wet-bulb temperature of 15.55 C, and a heating coil air flow rate defined by field rated air flow volume below). The value entered here must be greater than 0. Capacity should not account for supply air fan heat. The gross rated heating capacity should be within 20\% of the gross rated total cooling capacity, otherwise a warning message is issued. The gross heating capacity should NOT include the effect of supply air fan heat.
+
+\paragraph{Field: Gross Rated Heating COP}\label{field-gross-rated-heating-cop}
+
+This numeric field defines the coefficient of performance (COP = the gross heating capacity in watts divided by electrical power input in watts) of the DX heating coil unit at rated conditions (outdoor air dry-bulb temperature of 8.33 C, outdoor air wet-bulb temperature of 6.11 C, coil entering air dry-bulb temperature of 21.11 C, coil entering air wet-bulb temperature of 15.55 C, and a heating coil air flow rate defined by field rated air flow volume rate below). The value entered here must be greater than 0. The input power includes power for the compressor(s) and outdoor fan(s) but does not include the power consumption of the indoor supply air fan. The gross COP should NOT account for the supply air fan.
+
+\paragraph{Field: Rated Air Flow Rate}\label{field-rated-air-flow-rate-4}
+
+This numeric field defines the volume air flow rate, in m\(^{3}\) per second, across the DX heating coil at rated conditions. The value entered here must be greater than 0. The rated air volume flow rate should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of the gross rated heating capacity. The gross rated heating capacity and gross rated COP should be performance information for the unit with outdoor air dry-bulb temperature of 8.33 C, outdoor air wet-bulb temperature of 6.11 C, heating coil entering air dry-bulb temperature of 21.11 C, heating coil entering air wet-bulb temperature of 15.55 C, and the rated air volume flow rate defined here.
+
+\paragraph{Field: Rated Evaporator Fan Power Per Volume Flow Rate}\label{field-rated-evaporator-fan-power-per-volume-flow-rate-1}
+
+This field is the electric power for the evaporator (heating coil) fan per air volume flow rate through the coil at the rated conditions in W/(m\(^{3}\)/s). The default value is 773.3 W/(m\(^{3}\)/s) (365 W/1000 cfm) if this field is left blank. If a value is entered, it must be \textgreater{} = 0.0 and \textless{} = 1250 W/(m\(^{3}\)/s). This value is only used to calculate High Temperature Heating Standard (Net) Rating Capacity, Low Temperature Heating Standard (Net) Rating Capacity and Heating Seasonal Performance Factor (HSPF) which will be outputs in the EnergyPlus eio file (ref. EnergyPlus Engineering Reference, Single Speed DX Heating Coil, Standard Ratings). This value is not used for modeling the evaporator (heating coil) fan during simulations; instead, it is used for calculating the above standard ratings to assist the user in verifying their inputs for modeling this type of equipment.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-13}
+
+This alpha field defines the name of the HVAC system node from which the DX heating coil draws its inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-13}
+
+This alpha field defines the name of the HVAC system node to which the DX heating coil sends its outlet air.
+
+\paragraph{Field: Heating Capacity Function of Temperature Curve Name}\label{field-heating-capacity-function-of-temperature-curve-name}
+
+This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of the total heating capacity as a function of the both the indoor and outdoor air dry-bulb temperature or just the outdoor air dry-bulb temperature depending on the type of curve selected. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the gross rated heating capacity to give the gross total heating capacity at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or outdoor air dry-bulb temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
+
+\paragraph{Field: Heating Capacity Function of Flow Fraction Curve Name}\label{field-heating-capacity-function-of-flow-fraction-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of total heating capacity as a function of the ratio of actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
+
+\paragraph{Field: Energy Input Ratio Function of Temperature Curve Name}\label{field-energy-input-ratio-function-of-temperature-curve-name-3}
+
+This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor and outdoor air dry-bulb temperature or just the outdoor air dry-bulb temperature depending on the type of curve selected. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or outdoor air dry-bulb temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
+
+\paragraph{Field: Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-energy-input-ratio-function-of-flow-fraction-curve-name-3}
+
+This alpha field defines the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate.
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-6}
+
+This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
+
+\begin{lstlisting}
+       PLF = 0.85 + 0.15(PLR)
+\end{lstlisting}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{lstlisting}
+       PLF = 1.0 + 0.0(PLR)
+\end{lstlisting}
+
+\paragraph{Field: Defrost Energy Input Ratio Function of Temperature Curve Name}\label{field-defrost-energy-input-ratio-function-of-temperature-curve-name}
+
+This alpha field defines the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) during reverse-cycle defrost periods as a function of the outdoor air dry-bulb temperature and the wet-bulb temperature of the air entering the indoor coil. The EIR is the inverse of the COP. The output of this curve is multiplied by the coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the indoor and outdoor coils are operating. This curve is only required when a reverse-cycle defrost strategy is selected. The curve is normalized to a value of 1.0 at the rating point conditions.
+
+\paragraph{Field: Minimum Outdoor Dry-Bulb Temperature for Compressor Operation}\label{field-minimum-outdoor-dry-bulb-temperature-for-compressor-operation}
+
+This numeric field defines the minimum outdoor air dry-bulb temperature where the heating coil compressor turns off. The temperature for this input field must be greater than or equal to 20 C. If this input field is left blank, the default value is -8 C.
+
+\paragraph{Field: Outdoor Dry-Bulb Temperature to Turn On Compressor}\label{field-outdoor-dry-bulb-temperature-to-turn-on-compressor}
+
+This numeric field defines the outdoor air dry-bulb temperature when the compressor is automatically turned back on following an automatic shut off because of low outdoor temperature. This field is only used for the calculation heating seasonal performance factor (HSPF) of heating coil. If this field is not provided, outdoor bin temperature is always considered to be greater than this temperature and Minimum Outdoor dry-bulb Temperature for Compressor Operation field described above.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Defrost Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-defrost-operation}
+
+This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 C and less than or equal to 7.22 C. If this input field is left blank, the default value is 5 C.
+
+\paragraph{Field: Crankcase Heater Capacity}\label{field-crankcase-heater-capacity-4}
+
+This numeric field defines the crankcase heater capacity in Watts. When the outdoor air dry-bulb temperature is below the value specified in the input field Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation (described below), the crankcase heater is enabled during the time that the compressor is not running. If this heating coil is used as part of an air-to-air heat pump (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir or ZoneHVAC:PackagedTerminalHeatPump), the crankcase heater defined for this DX heating coil is enabled during the time that the compressor is not running for either heating or cooling (and the crankcase heater power defined in the DX cooling coil object is disregarded in this case). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0. To simulate a unit without a crankcase heater, enter a value of 0.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-crankcase-heater-operation-4}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the compressor s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 C. If this input field is left blank, the default value is 10 C.
+
+\paragraph{Field: Defrost Strategy}\label{field-defrost-strategy}
+
+This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse-cycle.
+
+\paragraph{Field: Defrost Control}\label{field-defrost-control}
+
+This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field Defrost Time Period Fraction described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field Maximum Outdoor Dry-bulb Temperature for Defrost Operation described above. If this input field is left blank, the default defrost control is timed.
+
+\paragraph{Field: Defrost Time Period Fraction}\label{field-defrost-time-period-fraction}
+
+This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to timed defrost (see Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
+
+\paragraph{Field: Resistive Defrost Heater Capacity}\label{field-resistive-defrost-heater-capacity}
+
+This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is resistive (see input field Defrost Strategy above). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.
+
+\paragraph{Field: Region Number}\label{field-region-number}
+
+This optional numeric field defines the region number which is used to calculate HSPF of heating coil. The value for this input field must be between 1 and 6. If this input field is left blank, the default value is 4.
+
+\paragraph{Field: Evaporator Air Inlet Node Name}\label{field-evaporator-air-inlet-node-name}
+
+This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor evaporator. If this field is left blank, the outdoor air temperature entering the evaporator is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
+
+\paragraph{Field: Zone Name for Evaporator Placement}\label{field-zone-name-for-evaporator-placement}
+
+This input field is name of a conditioned or unconditioned zone where the secondary coil (evaporator) of a heat pump is installed. This is an optional input field specified only when user desires to extract heat from the zone via secondary coil. Heat extracted is modeled as internal gain. If the primary DX system is a heat pump, then the zone name should be the same as the zone name specified for placing the secondary cooling DX coil.
+
+\paragraph{Field: Secondary Coil Air Flow Rate}\label{field-secondary-coil-air-flow-rate}
+
+This input value is the secondary coil (evaporator) air flow rate when the heat pump is working in heating mode or the secondary coil (condenser) air flow rate when the heat pump is working in cooling mode. This input field is auto-sizable.
+
+\paragraph{Field: Secondary Coil Fan Flow Scaling Factor}\label{field-secondary-coil-fan-flow-scaling-factor}
+
+This input field is scaling factor for autosizing the secondary DX coil fan flow rate. The secondary air flow rate is determined by multiplying the primary DX coil rated air flow rate by the fan flow scaling factor. Default value is 1.25. If the secondary coil fan flow rate is not autosized, then the secondary coil fan flow scaling factor is set to 1.0.
+
+\paragraph{Field: Nominal Sensible Heat Ratio of Secondary Coil}\label{field-nominal-sensible-heat-ratio-of-secondary-coil}
+
+This input value is the nominal sensible heat ratio used to split the heat extracted by a secondary DX coil (evaporator) of a heat pump into sensible and latent components. This is an optional input field. If this input field is left blank, then pure sensible internal heat gain is assumed, i.e., sensible heat ratio of 1.0.
+
+\paragraph{Field: Sensible Heat Ratio Modifier Function of Temperature Curve Name}\label{field-sensible-heat-ratio-modifier-function-of-temperature-curve-name}
+
+This input field is name of sensible heat ratio modifier biquadratic curve. The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary zone air node wet-bulb temperature and the heating DX coil entering air dry-bulb temperature. This is an optional input field. If this input field is left blank, then the nominal sensible heat ratio modifier curve value for temperature is set to 1.0.
+
+\paragraph{Field: Sensible Heat Ratio Modifier Function of Flow Fraction Curve Name}\label{field-sensible-heat-ratio-modifier-function-of-flow-fraction-curve-name}
+
+This input field is name of sensible heat ratio modifier curve as function of secondary air flow fraction. The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary coil air flow fraction. This is an optional input field. If this input field is left blank, then the sensible heat ratio modifier curve value for flow fraction is set to 1.0.
+
+Following is an example input for the object.
+
+\begin{lstlisting}
+
+Coil:Heating:DX:SingleSpeed,
+  Heat Pump DX Heating Coil 1,     ! Name of heating coil
+  FanAndCoilAvailSched,                   ! Heating coil schedule
+  35000,                                                 ! Gross Rated Heating Capacity
+  2.75,                                                   ! Gross Rated Heating COP
+  1.7,                                                     !rated air flow rate (m3/s)
+  ,                                                       !rated evaporator fan power per volume flow rate (m3/s)
+  Heating Coil Air Inlet Node,     !heating coil air side inlet node
+  SuppHeating Coil Air Inlet Node, !Heating coil air side outlet node
+  HPACHeatCapFT,     ! heating cap modifier curve (temperature, C)
+  HPACHeatCapFFF,   ! heating cap modifier curve (flow fraction)
+  HPACHeatEIRFT,     ! energy input ratio modifier curve (temperature, C)
+  HPACHeatEIRFFF,   ! energy input ratio modifier curve (flow fraction)
+  HPACCOOLPLFFPLR, ! part load fraction modifier curve (function of part load ratio)
+  ,                 ! defrost EIR modifier curve (temp, C) not required for resistive defrost
+  -5.0,                       ! minimum OAT for compressor operation   (C)
+  ,                               ! outdoor dry-bulb temperature to turn on compressor   (C)
+  5.0,                         ! maximum outdoor dry-bulb temp for defrost operation (C)
+  200.0,                     ! Crankcase heater capacity (W)
+  10.0,                       ! Maximum outdoor temp for crankcase heater operation (C)
+  Resistive,             ! Defrost strategy (resistive or reverse-cycle)
+  Timed,                     ! Defrost control (timed or on-demand)
+  0.166667,             ! Defrost time period fraction (used for timed defrost control only)
+  20000;! Resistive defrost heater capacity (used for resistive defrost strategy only)
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-15-000}
+
+\begin{itemize}
+\item
+  HVAC,Average,Heating Coil Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Electric Power{[}W{]}
+\item
+  HVAC,Sum,Heating Coil Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Defrost Electric Power{[}W{]}
+\item
+  HVAC,Sum,Heating Coil Defrost Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Crankcase Heater Electric Power{[}W{]}
+\item
+  HVAC,Sum,Heating Coil Crankcase Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Runtime Fraction {[]}
+\end{itemize}
+
+\paragraph{Heating Coil Total Heating Rate {[}W{]}}\label{heating-coil-total-heating-rate-w-2}
+
+This field is the total heating rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Heating Coil Total Heating Energy {[}J{]}}\label{heating-coil-total-heating-energy-j-2}
+
+This is the total heating output of the DX coil in Joules over the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = CoolingCoils, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Electric Power {[}W{]}}\label{heating-coil-electric-power-w-5}
+
+This output is the electricity consumption rate of the DX coil compressor and outdoor fan(s) in Watts. This rate is applicable when the unit is providing heating to the conditioned zone(s), and excludes periods when the unit is in reverse-cycle defrost mode.
+
+\paragraph{Heating Coil Electric Energy {[}J{]}}\label{heating-coil-electric-energy-j-3}
+
+This is the electricity consumption of the DX coil compressor and condenser fan(s) in Joules for the timestep being reported. This consumption is applicable when the unit is providing heating to the conditioned zone(s), and excludes periods when the unit is in reverse-cycle defrost mode. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Defrost Electric Power {[}W{]}}\label{heating-coil-defrost-electric-power-w}
+
+This is the electricity consumption rate of the DX coil unit in Watts when the unit is in defrost mode (reverse-cycle or resistive).
+
+\paragraph{Heating Coil Defrost Electric Energy {[}J{]}}\label{heating-coil-defrost-electric-energy-j}
+
+This is the electricity consumption of the DX coil unit in Joules for the timestep being reported. This consumption is applicable when the unit is in defrost mode (reverse-cycle or resistive).
+
+\paragraph{Heating Coil Crankcase Heater Electric Power {[}W{]}}\label{heating-coil-crankcase-heater-electric-power-w}
+
+This is the average electricity consumption rate of the DX coil compressor s crankcase heater in Watts for the timestep being reported.
+
+\paragraph{Heating Coil Crankcase Heater Electric Energy {[}J{]}}\label{heating-coil-crankcase-heater-electric-energy-j}
+
+This is the electricity consumption of the DX coil compressor s crankcase heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Miscellaneous, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Heating Coil Runtime Fraction {[]}}{Heating Coil Runtime Fraction }}\label{heating-coil-runtime-fraction-4}
+
+This is the runtime fraction of the DX heating coil compressor and outdoor fan(s) for the timestep being reported.
+
+\subsection{Coil:Heating:DX:MultiSpeed}\label{coilheatingdxmultispeed}
+
+This component models a DX heating unit with multiple discrete levels of heating capacity. Currently, this heating coil can only be referenced by a AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed compound object. The multispeed DX heating coil can have from two to four operating speeds. When the coil operates at Speed 1 (the lowest speed), its performance is very similar to the Coil:Heating:DX:SingleSpeed object where the impacts of part-load ratio can be included. When the coil operates at higher speeds (above Speed 1), the linear approximation methodology is applied. The coil outputs at two consecutive speeds are linearly interpolated to meet the required heating capacity during an HVAC system timestep. When the coil performs above the lowest speed, the user can choose if they want to include part-load ratio impacts at the higher speeds.
+
+The multispeed unit is described by specifying the performance at different operating speeds. Each speed has its own set of input specifications: full load capacity, COP and air flow rate at rated conditions, along with modifier curves to determine performance when actual operating conditions are different from the rated conditions.
+
+The coil operates to meet the sensible capacity being requested. When this requested capacity is above the sensible capacity of the highest operating speed, the coil runs continuously at the highest speed. When the requested capacity is between the sensible capacities of two consecutive speeds, the unit will operate a portion of the time at each speed to meet the request. When the requested capacity is less than the low speed (Speed 1) capacity, the unit will cycle on/off as needed.
+
+The next input defines the minimum outdoor dry-bulb temperature where the compressor will operate. The followed two inputs are related to crankcase heater operation: capacity and maximum outdoor dry-bulb temperature for crankcase heater operation. The next six inputs cover defrost operation: defrost EIR modifier curve, the maximum outdoor dry-bulb temperature for defrost operation, the type of defrost strategy (reverse-cycle or resistive), defrost control (timed or on-demand), the fractional defrost time period (timed defrost control only), and the resistive defrost heater capacity if a resistive defrost strategy is selected. The activation of defrost is dependent on outdoor conditions. The capacity reduction and energy use modification are independent of speed. The defrost EIR modifier is described below:
+
+The defrost energy input ratio (EIR) modifier curve (function of temperature) is a bi-quadratic curve with two independent variables: outdoor air dry-bulb temperature and the heating coil entering air wet-bulb temperature. The output of this curve is multiplied by the heating coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the coil is operating. This curve is only required when a reverse-cycle defrost strategy is specified.
+
+The next input allows the user to choose whether to apply the part load fraction correlation to speeds greater than 1 or not. The following input is the type of fuel.
+
+Then the number of speed for heating is entered. The rest of inputs are speed dependent. Each set of data consists of gross rated heating capacity, gross rated COP, and the rated air volume flow rate. These three inputs determine the coil performance at the rating point (outdoor air dry-bulb temperature of 8.33 °C, outdoor air wet-bulb temperature of 6.11 °C, coil entering air dry-bulb temperature of 21.11 °C, coil entering air wet-bulb temperature of 15.55 °C). The rated air volume flow rate should be between .00004027 m\(^{3}\)/s and .00006041 m\(^{3}\)/s per watt of gross rated heating capacity. The rated waste heat fraction is needed to calculate how much waste heat is available at the rated conditions. In addition, up to 6 modifier curves are required per speed.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  The heating capacity modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the gross rated heating capacity to give the gross total heating capacity at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
+\item
+  The heating capacity modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating.
+\item
+  The energy input ratio (EIR) modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
+\item
+  The energy input ratio (EIR) modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating.
+\item
+  The part load fraction correlation (function of part load ratio) is a quadratic or cubic curve with the independent variable being part load ratio (sensible heating load / steady-state heating capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the effective EIR for a given simulation timestep. The part load fraction correlation accounts for efficiency losses due to compressor cycling.
+\item
+  The waste heat modifier curve (function of temperature) is a bi-quadratic curve with two independent variables: outdoor air dry-bulb temperature and the heating coil entering air dry-bulb temperature. The output of this curve is multiplied by the heating input energy, the waste heat fraction of heat input to give the recoverable waste heat.
+\end{enumerate}
+
+The curves are simply specified by name. Curve inputs are described in the curve manager section of this document (ref. Performance Curves).
+
+\subsubsection{Inputs}\label{inputs-20-001}
+
+\paragraph{Field: Name}\label{field-name-19-001}
+
+This alpha field defines a unique user-assigned name for an instance of a multispeed DX heating coil. Any reference to this DX heating coil by another object will use this name. The only allowed parent is AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-11-000}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the multispeed DX heating coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node name}\label{field-air-inlet-node-name-14}
+
+This alpha field defines the name of the HVAC system node from which the DX heating coil draws its inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-14}
+
+This alpha field defines the name of the HVAC system node to which the DX heating coil sends its outlet air.
+
+\paragraph{Field: Minimum Outdoor Dry-Bulb Temperature for Compressor Operation}\label{field-minimum-outdoor-dry-bulb-temperature-for-compressor-operation-1}
+
+This numeric field defines the minimum outdoor air dry-bulb temperature where the heating coil compressor turns off. The temperature for this input field must be greater than or equal to 20 °C. If this input field is left blank, the default value is -8 °C.
+
+\paragraph{Field: Crankcase Heater Capacity}\label{field-crankcase-heater-capacity-5}
+
+This numeric field defines the crankcase heater capacity in Watts. When the outdoor air dry-bulb temperature is below the value specified in the input field Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation (described below), the crankcase heater is enabled during the time that the compressor is not running. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0. To simulate a unit without a crankcase heater, enter a value of 0.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-crankcase-heater-operation-5}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the compressor s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 °C. If this input field is left blank, the default value is 10 °C.
+
+\paragraph{Field: Defrost Energy Input Ratio Function of Temperature Curve Name}\label{field-defrost-energy-input-ratio-function-of-temperature-curve-name-1}
+
+This alpha field defines the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) during reverse-cycle defrost periods as a function of the outdoor air dry-bulb temperature and the wet-bulb temperature of the air entering the indoor coil. The EIR is the inverse of the COP. The output of this curve is multiplied by the coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the indoor and outdoor coils are operating. This curve is only required when a reverse-cycle defrost strategy is selected. The curve is normalized to a value of 1.0 at the rating point conditions.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Defrost Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-defrost-operation-1}
+
+This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 °C and less than or equal to 7.22 °C. If this input field is left blank, the default value is 5 °C.
+
+\paragraph{Field: Defrost Strategy}\label{field-defrost-strategy-1}
+
+This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse-cycle.
+
+\paragraph{Field: Defrost Control}\label{field-defrost-control-1}
+
+This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field Defrost Time Period Fraction described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field Maximum Outdoor Dry-bulb Temperature for Defrost Operation described above. If this input field is left blank, the default defrost control is timed.
+
+\paragraph{Field: Defrost Time Period Fraction}\label{field-defrost-time-period-fraction-1}
+
+This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to timed defrost (see Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
+
+\paragraph{Field: Resistive Defrost Heater Capacity}\label{field-resistive-defrost-heater-capacity-1}
+
+This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is resistive (see input field Defrost Strategy above). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.
+
+\paragraph{Field: Apply Part Load Fraction to Speeds Greater than 1}\label{field-apply-part-load-fraction-to-speeds-greater-than-1-1}
+
+This field determines whether part-load impacts on coil energy use are applied when the coil is operating at speeds greater than speed 1. The allowed choices are Yes or No, with the default being No if this field is left blank. Other input fields in this object allow the user to specify a part-load fraction correlation for each speed to account for compressor start up losses (cycle on/off). For the case of a single multi-speed compressor, the part load losses may only be significant when the compressor cycles between speed 1 and off, but the losses may be extremely small when the compressor operates between speed 1 and speed 2 (or between speeds 2 and 3, etc.). In this case, the user may chose to specify \textbf{No} for this input field to neglect part-load impacts on energy use at higher operating speeds. If part-load impacts on coil energy use are thought to be significant (e.g., interwined cooling coil with multiple compressors feeding individual refrigerant circuits), then the user may chose to specify \textbf{Yes} and the part-load fraction correlations specified for speeds 2 through 4 will be applied as appropriate. The selection for this input field does not affect part-load impacts when the compressor cycles between speed 1 and off (i.e., the part-load fraction correlation for speed 1 is always applied).
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-1-000}
+
+This alpha field determines the type of fuel that the chiller uses. This field has seven choices: Electricity, NaturalGas, PropaneGas, Coal, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1 and OtherFuel2. The default is NaturalGas.
+
+\paragraph{Field: Number of Speeds}\label{field-number-of-speeds-2}
+
+This field specifies the number of sets of data being entered for rated specifications, performance curves, and waste heat specifications for each cooling speed. The rated specifications consist of gross rated capacity, gross rated COP, and rated air flow rate. The performance curves consist of a total capacity modifier curve as a function of temperature, total capacity modifier curve as a function of flow fraction, energy input ratio modifier curve as a function of temperature, energy input ratio modifier curve as a function of flow fraction, and part load fraction correlation as a function of part load ratio. The waste heat specifications include the fraction of energy input to the heating coil at the fully loaded and rated conditions, and a temperature modifier. The minimum number of speeds for heating is 2 and the maximum number is 4. The number of speeds should be the same as the number of speeds for heating defined in its parent object (AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed). The first set of performance inputs is for Speed 1 and should be for low speed, and the last set of performance inputs should be for high speed. For example, if only three heating speeds are defined, the first set should be for low speed (Speed 1), the second set should be for medium speed (Speed 2), and the third set should be for high speed (Speed 3). In this example, any performance inputs for Speed 4 would be neglected (since this input field specifies that the coil only has three heating speeds).
+
+\paragraph{Field Group: Rated Specification, Performance Curves, and Waste Heat Data}\label{field-group-rated-specification-performance-curves-and-waste-heat-data}
+
+The performance for each heating speed must be specified as shown below. All inputs for Speed 1 are required first, followed by the inputs for Speed 2, Speed 3 and Speed 4.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Gross Rated Heating Capacity}\label{field-speed-x-gross-rated-heating-capacity}
+
+This numeric field defines the total, full load gross heating capacity in watts of the DX coil unit at rated conditions for Speed \textless{}x\textgreater{} operation (outdoor air dry-bulb temperature of 8.33 °C, outdoor air wet-bulb temperature of 6.11 °C, heating coil entering air dry-bulb temperature of 21.11 °C, heating coil entering air wet-bulb temperature of 15.55 °C, and a heating coil air flow rate defined by field Rated Air Flow Rate, Speed \textless{}x\textgreater{} below). The value entered here must be greater than 0. The gross heating capacity should not account for the effect of supply air fan heat.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Gross Rated Heating COP}\label{field-speed-x-gross-rated-heating-cop}
+
+This numeric field defines the coefficient of performance (COP = gross heating capacity in watts divided by electrical power input in watts) of the DX heating coil unit at rated conditions for Speed \textless{}x\textgreater{} operation (outdoor air dry-bulb temperature of 8.33 °C, outdoor air wet-bulb temperature of 6.11 °C, coil entering air dry-bulb temperature of 21.11 °C, coil entering air wet-bulb temperature of 15.55 °C, and a heating coil air flow rate defined by field Speed \textless{}x\textgreater{} Rated Air Flow Rate below). The value entered here must be greater than 0. The input power includes power for the compressor(s) and outdoor fan(s) but does not include the power consumption of the indoor supply air fan. The gross heating capacity is the value entered above in the field Gross Rated Heating Capacity . The gross COP should NOT account for the supply air fan.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Rated Air Flow Rate}\label{field-speed-x-rated-air-flow-rate-1}
+
+This numeric field defines the volume air flow rate, in m\(^{3}\) per second, across the DX heating coil at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0. The rated air volume flow rate should be between 0.00004027 m\(^{3}\)/s and 0.00006041 m\(^{3}\)/s per watt of gross rated heating capacity. The gross rated heating capacity and gross rated COP should be performance information for the unit with outdoor air dry-bulb temperature of 8.33 °C, outdoor air wet-bulb temperature of 6.11 °C, heating coil entering air dry-bulb temperature of 21.11 °C, heating coil entering air wet-bulb temperature of 15.55 °C, and the rated air volume flow rate defined here.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Heating Capacity Function of Temperature Curve Name}\label{field-speed-x-heating-capacity-function-of-temperature-curve-name}
+
+This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the total heating capacity as a function of the both the indoor and outdoor air dry-bulb temperature or just the outdoor air dry-bulb temperature depending on the type of curve selected. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the gross rated heating capacity to give the gross total heating capacity at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or outdoor air dry-bulb temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Heating Capacity Function of Flow Fraction Curve Name}\label{field-speed-x-heating-capacity-function-of-flow-fraction-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of heating capacity as a function of the ratio of actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the gross heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Temperature Curve Name}\label{field-speed-x-energy-input-ratio-function-of-temperature-curve-name-2}
+
+This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor and outdoor air dry-bulb temperature or just the outdoor air dry-bulb temperature depending on the type of curve selected. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or outdoor air dry-bulb temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-speed-x-energy-input-ratio-function-of-flow-fraction-curve-name-1}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate.
+
+\paragraph{Field: Speed \textless{}x\textgreater{}Part Load Fraction Correlation Curve Name}\label{field-speed-xpart-load-fraction-correlation-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+\begin{lstlisting}
+       PLF > = 0.7     and     PLF > = PLR
+\end{lstlisting}
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional DX heating coil (Speed \textless{}x\textgreater{}) would be:
+
+\begin{lstlisting}
+       PLF = 0.85 + 0.15(PLR)
+\end{lstlisting}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{lstlisting}
+       PLF = 1.0 + 0.0(PLR)
+\end{lstlisting}
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Rated Waste Heat Fraction of Power Input}\label{field-speed-x-rated-waste-heat-fraction-of-power-input-1}
+
+The fraction of heat input to heating that is available as recoverable waste heat at full load and rated conditions for Speed \textless{}x\textgreater{} operation.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Waste Heat Function of Temperature Curve Name}\label{field-speed-x-waste-heat-function-of-temperature-curve-name-1}
+
+The name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the waste heat recovery as a function of outdoor dry-bulb temperature and the entering coil dry-bulb temperature for Speed \textless{}x\textgreater{}. The output of this curve is multiplied by the rated recoverable waste heat at specific temperature operating conditions (i.e., at temperatures different from the rating point). The curve is normalized to a value of 1.0 at the rating point. When the fuel type is electricity, the field is either left blank or ignored by the program. When the fuel type is not electricity and the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed does not require waste heat calculations, this field is ignored. If the field is blank, a warning will be issued and simulation continues. When the fuel type is not electricity and the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed requires waste heat calculations, if this field is left blank, the program assumes a constant value of 1 to make simulation continue and a warning will be issued.
+
+\paragraph{Field: Zone Name for Evaporator Placement}\label{field-zone-name-for-evaporator-placement-1}
+
+This input field is name of a conditioned or unconditioned zone where the secondary coil (evaporator) of a heat pump is installed. This is an optional input field specified only when user desires to extract heat from the zone via secondary coil. Heat extracted is modeled as internal gain. If the primary DX system is a heat pump, then the zone name should be the same as the zone name specified for placing the secondary cooling DX coil.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Secondary Coil Air Flow Rate}\label{field-speed-x-secondary-coil-air-flow-rate}
+
+This input value is the secondary coil (evaporator) air flow rate when the heat pump is working in heating mode or the secondary coil (condenser) air flow rate when the heat pump is working in cooling mode. This input field is auto-sizable.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Secondary Coil Fan Flow Scaling Factor}\label{field-speed-x-secondary-coil-fan-flow-scaling-factor}
+
+This input field is scaling factor for autosizing the secondary DX coil fan flow rate. The secondary air flow rate is determined by multiplying the primary DX coil rated air flow rate by the fan flow scaling factor. Default value is 1.25. If the secondary coil fan flow rate is not autosized, then the secondary coil fan flow scaling factor is set to 1.0.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Nominal Sensible Heat Ratio of Secondary Coil}\label{field-speed-x-nominal-sensible-heat-ratio-of-secondary-coil}
+
+This input value is the nominal sensible heat ratio used to split the heat extracted by a secondary DX coil (evaporator) of a heat pump into sensible and latent components. This is an optional input field. If this input field is left blank, then pure sensible internal heat gain is assumed, i.e., sensible heat ratio of 1.0.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Sensible Heat Ratio Modifier Function of Temperature Curve Name}\label{field-speed-x-sensible-heat-ratio-modifier-function-of-temperature-curve-name}
+
+This input field is name of sensible heat ratio modifier biquadratic curve. The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary zone air node wet-bulb temperature and the heating DX coil entering air dry-bulb temperature. This is an optional input field. If this input field is left blank, then the nominal sensible heat ratio modifier curve value for temperature is set to 1.0.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Sensible Heat Ratio Modifier Function of Flow Fraction Curve Name}\label{field-speed-x-sensible-heat-ratio-modifier-function-of-flow-fraction-curve-name}
+
+This input field is name of sensible heat ratio modifier curve as function of secondary air flow fraction. The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary coil air flow fraction. This is an optional input field. If this input field is left blank, then the sensible heat ratio modifier curve value for flow fraction is set to 1.0.
+
+Following is an example input for a multi-speed heating DX coil.
+
+\begin{lstlisting}
+
+COIL:Heating:DX:MultiSpeed,
+  Heat Pump DX Heating Coil 1,   !- Name of heat pump heating coil
+  FanAndCoilAvailSched,       !- Availability Schedule
+  Heating Coil Air Inlet Node,   !- Coil Air Inlet Node
+  SuppHeating Coil Air Inlet Node,   !- Coil Air Outlet Node
+  -8.0,                                       !- Minimum Outdoor Dry-bulb Temperature for Compressor Operation {C}
+  200.0,                                     !- Crankcase Heater Capacity {W}
+  10.0,                                       !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
+  HPACDefrostCAPFT,               !- Defrost energy input ratio modifier curve (temperature)
+  7.22,                                       !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation
+  reverse-cycle,                     !- Defrost Strategy
+  timed,                                     !- Defrost Control
+  0.058333,                               !- Defrost Time Period Fraction
+  2000.0,                                   !- Resistive Defrost Heater Capacity {W}
+  No,                                           !- Apply Part Load Fraction to Speeds greater than 1
+  NaturalGas,                           !- Fuel type
+  4,                                             !- Number of speeds
+  7500,                                       !- Gross Rated Heating Capacity, Speed 1 {W}
+  2.75,                                       !- Gross Rated Heating COP, Speed 1
+  0.45,                                       !- Rated Air Flow Rate, Speed 1 {m3/s}
+  HPACHeatCapFT Speed 1,     !- Heating Capacity Modifier Curve, Speed 1 (temperature)
+  HPACHeatCapFF Speed 1,     !- Heating capacity modifier curve, Speed 1 (flow fraction)
+  HPACHeatEIRFT Speed 1,     !- Energy input ratio modifier curve, Speed 1 (temperature)
+  HPACHeatEIRFF Speed 1,     !- Energy input ratio modifier curve, Speed 1 (flow fraction)
+  HPACHeatPLFFPLR Speed 1, !- Part load fraction correlation, Speed 1 (part load ratio)
+  0.2,                                         !- Rated waste heat fraction of power input, Speed 1
+  HAPCHeatWHFT Speed 1,       !- Waste heat modifier curve, Speed 1 (temperature)
+  17500,                                     !- Gross Rated Heating Capacity, Speed 2 {W}
+  2.75,                                       !- Gross Rated Heating COP, Speed 2
+  0.85,                                       !- Rated Air Flow Rate, Speed 2 {m3/s}
+  HPACHeatCapFT Speed 2,     !- Heating Capacity Modifier Curve, Speed 2 (temperature)
+  HPACHeatCapFF Speed 2,     !- Heating capacity modifier curve, Speed 2 (flow fraction)
+  HPACHeatEIRFT Speed 2,     !- Energy input ratio modifier curve, Speed 2 (temperature)
+  HPACHeatEIRFF Speed 2,     !- Energy input ratio modifier curve, Speed 2 (flow fraction)
+  HPACHeatPLFFPLR Speed 2, !- Part load fraction correlation, Speed 2 (part load ratio)
+  0.2,                                         !- Rated waste heat fraction of power input, Speed 2
+  HAPCHeatWHFT Speed 2,       !- Waste heat modifier curve, Speed 2 (temperature)
+  25500,                                     !- Gross Rated Heating Capacity, Speed 3 {W}
+  2.75,                                       !- Gross Rated Heating COP, Speed 3
+  1.25,                                       !- Rated Air Flow Rate, Speed 3 {m3/s}
+  HPACHeatCapFT Speed 3,     !- Heating Capacity Modifier Curve, Speed 3 (temperature)
+  HPACHeatCapFF Speed 3,     !- Heating capacity modifier curve, Speed 3 (flow fraction)
+  HPACHeatEIRFT Speed 3,     !- Energy input ratio modifier curve, Speed 3 (temperature)
+  HPACHeatEIRFF Speed 3,     !- Energy input ratio modifier curve, Speed 3 (flow fraction)
+  HPACHeatPLFFPLR Speed 3, !- Part load fraction correlation, Speed 3 (part load ratio)
+  0.2,                                         !- Rated waste heat fraction of power input, Speed 3
+  HAPCHeatWHFT Speed 3,       !- Waste heat modifier curve, Speed 3 (temperature)
+  35500,                                     !- Gross Rated Heating Capacity, Speed 4 {W}
+  2.75,                                       !- Gross Rated Heating COP, Speed 4
+  1.75,                                       !- Rated Air Flow Rate, Speed 4 {m3/s}
+  HPACHeatCapFT Speed 4,     !- Heating Capacity Modifier Curve, Speed 4 (temperature)
+  HPACHeatCapFF Speed 4,     !- Heating capacity modifier curve, Speed 4 (flow fraction)
+  HPACHeatEIRFT Speed 4,     !- Energy input ratio modifier curve, Speed 4 (temperature)
+  HPACHeatEIRFF Speed 4,     !- Energy input ratio modifier curve, Speed 4 (flow fraction)
+  HPACHeatPLFFPLR Speed 4, !- Part load fraction correlation, Speed 4 (part load ratio)
+  0.2,                                         !- Rated waste heat fraction of power input, Speed 4
+  HAPCHeatWHFT Speed 4;       !- Waste heat modifier curve, Speed 4 (temperature)
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-16}
+
+\begin{itemize}
+\item
+  HVAC,Average,Heating Coil Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Electric Power{[}W{]}
+\item
+  HVAC,Sum,Heating Coil Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Defrost Electric Power{[}W{]}
+\item
+  HVAC,Sum,Heating Coil Defrost Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Defrost Gas Rate {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Defrost Gas Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Crankcase Heater Electric Power{[}W{]}
+\item
+  HVAC,Sum,Heating Coil Crankcase Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Runtime Fraction {[]}
+\end{itemize}
+
+If Fuel Type is not Electricity:
+
+\begin{itemize}
+\item
+  HVAC,Average, Heating Coil \textless{}Fuel Type\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum, Heating Coil \textless{}Fuel Type\textgreater{} Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Heating Coil Total Heating Rate {[}W{]}}\label{heating-coil-total-heating-rate-w-3}
+
+This field is the total heating rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Heating Coil Total Heating Energy {[}J{]}}\label{heating-coil-total-heating-energy-j-3}
+
+This is the total heating output of the DX coil in Joules over the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoil, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Electric Power {[}W{]}}\label{heating-coil-electric-power-w-6}
+
+This output variable is the input fuel type power for the heating coil in the unit of Watts, averaged during the report period. If Fuel Type is not Electricity, the value is zero.
+
+\paragraph{Cooling Coil Electric Energy {[}J{]}}\label{cooling-coil-electric-energy-j-2}
+
+This output variable is the input fuel type consumption for the multispeed heating coil in the unit of Joules, summed during the report period. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects). If Fuel Type is not Electricity, the value is zero.
+
+\paragraph{Heating Coil Defrost Electric Power {[}W{]}}\label{heating-coil-defrost-electric-power-w-1}
+
+This is the electricity consumption rate of the DX coil unit in Watts when the unit is in defrost mode (reverse-cycle or resistive). The variable is available when the defrost mode is resistive or the fuel type is electricity.
+
+\paragraph{Heating Coil Defrost Electric Energy {[}J{]}}\label{heating-coil-defrost-electric-energy-j-1}
+
+This is the electricity consumption of the DX coil unit in Joules for the timestep being reported. This consumption is applicable when the unit is in defrost mode (reverse-cycle or resistive). The variable is available when the defrost mode is resistive or the fuel type is electricity.
+
+\paragraph{Heating Coil Defrost \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{heating-coil-defrost-fuel-type-rate-w}
+
+This is the fuel consumption rate of the DX coil unit in Watts when the unit is in defrost mode (reverse-cycle). The variable is available when the defrost mode is reverse-cycle and the fuel type is non-electricity.
+
+\paragraph{Heating Coil Defrost \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{heating-coil-defrost-fuel-type-energy-j}
+
+This is the fuel consumption of the DX coil unit in Joules for the timestep being reported. This consumption is applicable when the unit is in defrost mode (reverse-cycle). The variable is available when the defrost mode is reverse-cycle and the fuel type is non-electricity.
+
+\paragraph{Heating Coil Crankcase Heater Electric Power {[}W{]}}\label{heating-coil-crankcase-heater-electric-power-w-1}
+
+This is the average electricity consumption rate of the DX coil compressor s crankcase heater in Watts for the timestep being reported. When a companion cooling coil exits, the crankcase heater power of the companion cool coil is alos reported in this variable.
+
+\paragraph{Heating Coil Crankcase Heater Electric Energy {[}J{]}}\label{heating-coil-crankcase-heater-electric-energy-j-1}
+
+This is the electricity consumption of the DX coil compressor s crankcase heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects). When a companion cooling coil exits, the crankcase heater power of the companion cool coil is alos reported in this variable.
+
+\paragraph{\texorpdfstring{Heating Coil Runtime Fraction {[]}}{Heating Coil Runtime Fraction }}\label{heating-coil-runtime-fraction-5}
+
+This is the runtime fraction of the DX heating coil compressor and outdoor fan(s) for the timestep being reported. When the heating speed is above 1, this output is the run time fraction for the higher speed.
+
+\paragraph{Heating Coil \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{heating-coil-fuel-type-rate-w}
+
+This output variable is the input fuel type power for the heating coil in the unit of Watts, averaged during the report period. The electric power is excluded. If Fuel Type is Electricity, this output variable is not reported.
+
+\paragraph{Cooling Coil \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{cooling-coil-fuel-type-energy-j-1}
+
+This output variable is the input fuel type consumption for the multispeed heating coil in the unit of Joules, summed during the report period. The electric consumption is excluded. This output is also added to a meter with Resource Type = \textless{}Fuel Type\textgreater{}, End Use Key = Heating, Group Key = System (ref. Output:Meter objects). If Fuel Type is Electricity, this output variable is not reported.
+
+Note: The Fuel Type defined in the above two output variables depends on the input in the fuel type filed. In addition to Electricity, Valid fuel types are NaturalGas, Propane, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1 and OtherFuel2.
+
+\subsection{Coil:Heating:DX:VariableSpeed}\label{coilheatingdxvariablespeed}
+
+The Variable-Speed Air-to-Air Heating DX Coil is a collection of performance curves that represent the heating coil at various speed levels. The performance curves should be generated from the heat pump Reference Unit catalog data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. The number of speed levels can range from 1 to 10. The heating coil has two air side node connections. The user needs to specify a nominal speed level, at which the gross rated capacity and rated volumetric air flow rate are sized. The gross rated capacity and rated volumetric flow rate represent the real situation in the air loop, and are used to determine the flow rates at various speed levels in the parent objects, e.g.~AirLoopHVAC:UnitaryHeatPump:AirToAir, ZoneHVAC:PackagedTerminalHeatPump, etc. It shall be mentioned that the performance correction curves, i.e.~the temperature and flow fraction correction curves, should be normalized to the capacity and flow rate at each individual speed and at the rated operating conditions, similar to the performance curves used in the single-speed DX coil. On the other hand, the performance values at individual speed levels, e.g.~capacities, COPs and flow rates, should be given regarding a specific unit from the Reference Unit catalog data. In the following content, the statement started with Reference Unit means the actual Reference Unit catalog data. The rated conditions for obtaining the capacities and COPs are at indoor dry-bulb temperature of 21.1 ËšC (70 ËšF) and the source side entering air temperature of 8.3 ËšC (47 ËšF). Some equations are provided below to help explain the function of the various performance curves and data fields.
+
+\subsubsection{Inputs}\label{inputs-21-001}
+
+\paragraph{Field: Name}\label{field-name-20-000}
+
+This alpha field contains the identifying name for the variable speed heating coil.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-15}
+
+This alpha field contains the heating coil load side inlet node name.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-15}
+
+This alpha field contains the heating coil load side outlet node name.
+
+\paragraph{Field: Number of Speeds}\label{field-number-of-speeds-3}
+
+This numeric field contains the maximum number of speed levels that the module uses. The number of speeds, for which the user input the performance data and curves, has to be equal to or higher than the maximum number. The performance inputs at higher speeds are ignored.
+
+\paragraph{Field: Nominal Speed Level}\label{field-nominal-speed-level-1}
+
+This numeric field defines the nominal speed level, at which the rated capacity, rated air and volumetric flow rate are correlated.
+
+\paragraph{Field: Gross Rated Heating Capacity at Selected Nominal Speed Level}\label{field-gross-rated-heating-capacity-at-selected-nominal-speed-level}
+
+This numeric field contains the rated capacity at the nominal speed level. This field is autosizable. The gross rated heating capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
+
+\begin{equation}
+\rm{CapacityScaleFactor} = \frac{{{\rm{Gross RatedTotalHeatingCapacity}}}}{{{\rm{ReferenceUnitCapacity}}@{\rm{NominalSpeedLevel}}}}
+\end{equation}
+
+And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below,
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{Gross RatedCapacity} @ \rm{SpeedLevel} \left( \rm{x} \right) = \\
+    \quad \quad \quad \rm{CapacityScaleFactor} \times \\
+    \quad \quad \quad \rm{ReferenceUnitCapacity} @ \rm{SpeedLevel}(\rm{x})
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Rated Volumetric Air Flow Rate}\label{field-rated-volumetric-air-flow-rate}
+
+This numeric field contains the rated volumetric air flow rate on the load side of the heat pump corresponding to the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects. It is recommended that the ratio of the rated volumetric air flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
+
+\begin{equation}
+{\rm{AirFlowScaleFactor}} = \frac{{{\rm{RatedVolumetricAirFlowRate}}}}{{{\rm{ReferenceUnitVolAirFlowRate}}@{\rm{NominalSpeedLevel}} \times {\rm{CapacityScaleFactor}}}}
+\end{equation}
+
+And the volumetric air flow rates in the parent objects are calculated as below,
+
+\begin{equation}
+  \begin{array}{l}
+    {\rm{LoopVolumetricAirFlowRate}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = \\
+    \quad \quad \quad {\rm{AirFlowScaleFactor}} \times \\
+    \quad \quad \quad {\rm{ReferenceUnitVolAirFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) \times \\
+    \quad {\kern 1pt} {\kern 1pt} \quad \quad {\rm{CapacityScaleFactor}}
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-7}
+
+This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, heating load/steady-state heating capacity for Speed 1), in the case that the unit operates under the lowest speed, i.e.~on/off. The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep for Speed 1. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep).
+
+\paragraph{Field: Defrost Energy Input Ratio Function of Temperature Curve Name}\label{field-defrost-energy-input-ratio-function-of-temperature-curve-name-2}
+
+This alpha field defines the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) during reverse-cycle defrost periods as a function of the outdoor air dry-bulb temperature and the wet-bulb temperature of the air entering the indoor coil. The EIR is the inverse of the COP. The output of this curve is multiplied by the coil capacity at the maximum speed level, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the indoor and outdoor coils are operating. This curve is only required when a reverse cycle defrost strategy is selected. The curve is normalized to a value of 1.0 at the rating point conditions.
+
+\paragraph{Field: Minimum Outdoor Dry-Bulb Temperature for Compressor Operation}\label{field-minimum-outdoor-dry-bulb-temperature-for-compressor-operation-2}
+
+This numeric field defines the minimum outdoor air dry-bulb temperature where the heating coil compressor turns off. If this input field is left blank, the default value is -8 °C.
+
+\paragraph{Field: Outdoor Dry-Bulb Temperature to Turn On Compressor}\label{field-outdoor-dry-bulb-temperature-to-turn-on-compressor-1}
+
+This numeric field defines the outdoor temperature when the compressor is automatically turned back on following an automatic shut off because of low outdoor dry-bulb temperature. This field is only used for the calculation of HSPF. If this field is not provided, then outdoor bin temperature used in the HSPF calculation is always considered to be greater than this temperature and `Minimum Outdoor Dry-Bulb Temperature for Compressor Operation' field described above. This assumption is based on AHRI standard 210/240 (2008) and can introduce significant error in the final value of HSPF.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Defrost Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-defrost-operation-2}
+
+This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 °C and less than or equal to 7.22 °C. If this input field is left blank, the default value is 5 °C.
+
+\paragraph{Field: Crankcase Heater Capacity}\label{field-crankcase-heater-capacity-6}
+
+This numeric field defines the crankcase heater capacity in Watts. When the outdoor air drybulb temperature is below the value specified in the input field Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation (described below), the crankcase heater is enabled during the time that the compressor is not running. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0. To simulate a unit without a crankcase heater, enter a value of 0.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-crankcase-heater-operation-6}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the compressor s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 °C. If this input field is left blank, the default value is 10 °C.
+
+\paragraph{Field: Defrost Strategy}\label{field-defrost-strategy-2}
+
+This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse cycle.
+
+\paragraph{Field: Defrost Control}\label{field-defrost-control-2}
+
+This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field Defrost Time Period Fraction described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field Maximum Outdoor Dry-bulb Temperature for Defrost Operation described above. If this input field is left blank, the default defrost control is timed.
+
+\paragraph{Field: Defrost Time Period Fraction}\label{field-defrost-time-period-fraction-2}
+
+This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to timed defrost (see Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
+
+\paragraph{Field: Resistive Defrost Heater Capacity}\label{field-resistive-defrost-heater-capacity-2}
+
+This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is resistive (see input field Defrost Strategy above). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.
+
+\paragraph{Field Group: Rated specification and performance curves}\label{field-group-rated-specification-and-performance-curves}
+
+The performance for each heating speed must be specified as shown below. They should be directly given from the Reference Unit data. All inputs for Speed 1 are required, followed by the optional inputs for other speeds.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Gross Rated Heating Capacity}\label{field-speed-x-reference-unit-gross-rated-heating-capacity}
+
+This numeric field defines the total, full load gross heating capacity in watts of the air-to-air heating coil unit at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0. The gross heating capacity should not account for the effects of supply air fan heat.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Gross Rated Heating COP}\label{field-speed-x-reference-unit-gross-rated-heating-cop}
+
+This numeric field defines the coefficient of performance (COP = gross heating capacityin watts divided by electrical power input in watts) of the heating coil unit at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0. The input power includes power for the compressor(s), the outdoor coil fan and accessories, but does not include the power consumption of the indoor supply air fan. The gross COP should NOT account for the supply air fan.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Rated Air Flow Rate}\label{field-speed-x-reference-unit-rated-air-flow-rate-1}
+
+This numeric field defines the volume air flow rate, in m\(^{3}\) per second, across the heating coil at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here should be directly from the Reference Unit data, corresponding to the given gross rated heating capacity and gross rated heating COP at the speed, as above.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Heating Capacity Function of Temperature Curve Name}\label{field-speed-x-heating-capacity-function-of-temperature-curve-name-1}
+
+This alpha field defines the name of a bi-quadratic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the total heating capacity as a function of the indoor dry-bulb and source side entering air temperature, from the Reference Unit. The output of this curve is multiplied by the gross rated heating capacity at the speed to give the gross heating capacity at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or entering air temperature different from the rating point temperature). It should be noted that the curve is normalized to the heating capacity at Speed\textless{}x\textgreater{} from the Reference Unit data, and have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Heating Capacity Function of Air Flow Fraction Curve Name}\label{field-speed-x-heating-capacity-function-of-air-flow-fraction-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the gross heating capacity as a function of the ratio of actual air flow rate across the heating coil to the design air flow rate (i.e., fraction of full load flow), at Speed \textless{}x\textgreater{} from the Reference Unit data. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the design air flow rate at Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Temperature Curve Name}\label{field-speed-x-energy-input-ratio-function-of-temperature-curve-name-3}
+
+This alpha field defines the name of a bi-quadratic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor air dry-bulb and entering air temperatures. The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP at Speed \textless{}x\textgreater{} from the Reference Unit data) to give the EIR at specific temperature operating conditions (i.e., at an indoor air dry bulb temperature or entering air temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Air Flow Fraction Curve Name}\label{field-speed-x-energy-input-ratio-function-of-air-flow-fraction-curve-name-1}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the heating coil to the design air flow rate (i.e., fraction of full load flow, at Speed \textless{}x\textgreater{} from the Reference Unit data). The EIR is the inverse of the COP. This curve is normalized to a value of 1.0 when the actual air flow rate equals the design air flow rate.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Coil:Heating:DX:VariableSpeed,
+  Heat Pump DX Heating Coil 1,         !- Name
+  Heating Coil Air Inlet Node,         !- Air Inlet Node Name
+  SuppHeating Coil Air Inlet Node,   !- Air Outlet Node Name
+  10.0,                                     !- Number of Speeds {dimensionless}
+  10.0,                                     !- Nominal Speed Level {dimensionless}
+  35000,                                   !- Gross Rated Heating Capacity {W}
+  1.7,                                         !- Rated Air Flow Rate {m3/s}
+  HPACCOOLPLFFPLR,                 !- Part Load Fraction Correlation Curve Name
+  ,                                               !- Defrost Energy Input Ratio Function of Temperature Curve Name
+  -5.0,                                       !- Minimum Outdoor Dry-Bulb Temperature for Compressor Operation {C}
+  ,                                               !- Outdoor Dry-Bulb Temperature to Turn Back On Compressor{C}
+  5.0,                                         !- Maximum Outdoor Dry-Bulb Temperature for Defrost Operation {C}
+  200.0,                                     !- Crankcase Heater Capacity {W}
+  10.0,                                       !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
+  Resistive,                             !- Defrost Strategy
+  TIMED,                                     !- Defrost Control
+  0.166667,                               !- Defrost Time Period Fraction
+  20000,                                     !- Resistive Defrost Heater Capacity {W}
+  1838.7,                                   !- Speed 1 Gross Rated Heating Capacity {w}
+  5.0,                                         !- Speed 1 Gross Rated Heating COP {dimensionless}
+  0.1661088,                             !- Speed 1 Rated Air Flow Rate {m3/s}
+  HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  2295.5,                                   !- Speed 2 Gross Rated Heating Capacity {w}
+  5.0,                                         !- Speed 2 Gross Rated Heating COP {dimensionless}
+  0.179322,                               !- Speed 2 Rated Air Flow Rate {m3/s}
+  HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  2751.3,                                   !- Speed 3 Gross Rated Heating Capacity {w}
+  5.0,                                         !- Speed 3 Gross Rated Heating COP {dimensionless}
+  0.1925352,                             !- Speed 3 Rated Air Flow Rate {m3/s}
+  HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  3659.6,                                   !- Speed 4 Gross Rated Heating Capacity {w}
+  5.0,                                         !- Speed 4 Gross Rated Heating COP {dimensionless}
+  0.2189616,                             !- Speed 4 Rated Air Flow Rate {m3/s}
+  HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  4563.7,                                   !- Speed 5 Gross Rated Heating Capacity {w}
+  5.0,                                         !- Speed 5 Gross Rated Heating COP {dimensionless}
+  0.245388,                               !- Speed 5 Rated Air Flow Rate {m3/s}
+  HPACHeatCapFT,                     !- Total Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Total Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  5463.3,                                   !- Speed 6 Gross Rated Heating Capacity {w}
+  5.0,                                         !- Speed 6 Gross Rated Heating COP {dimensionless}
+  0.2718144,                             !- Speed 6 Rated Air Flow Rate {m3/s}
+  HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  6358.4,                                   !- Speed 7 Gross Rated Heating Capacity {w}
+  5.0,                                         !- Speed 7 Gross Rated Heating COP {dimensionless}
+  0.2982408,                             !- Speed 7 Rated Air Flow Rate {m3/s}
+  HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  7248.5,                                   !- Speed 8 Gross Rated Heating Capacity {w}
+  5.0,                                         !- Speed 8 Gross Rated Heating COP {dimensionless}
+  0.3246672,                             !- Speed 8 Rated Air Flow Rate {m3/s}
+  HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  8133.6,                                   !- Speed 9 Gross Rated Heating Capacity {w}
+  5.0,                                         !- Speed 9 Gross Rated Heating COP {dimensionless}
+  0.3510936,                             !- Speed 9 Rated Air Flow Rate {m3/s}
+  HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  9013.2,                                   !- Speed 10 Gross Rated Heating Capacity {w}
+  5.0,                                         !- Speed 10 Gross Rated Heating COP {dimensionless}
+  0.37752,                                 !- Speed 10 Rated Air Flow Rate {m3/s}
+  HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF;                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-17}
+
+\begin{itemize}
+\item
+  HVAC,Average,Heating Coil Electric Power {[}W{]}
+\item
+  HVAC,Average,Heating Coil Heating Rate {[}W{]}
+\item
+  HVAC,Average,Heating Coil Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Heating Coil Source Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Heating Coil Part Load Ratio {[]}
+\item
+  HVAC,Average, Heating Coil Runtime Fraction {[]}
+\item
+  HVAC,Average, Heating Coil Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Heating Coil Air Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Heating Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,Heating Coil Air Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Heating Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,Heating Coil Upper Speed Level {[]}
+\item
+  HVAC,Average,Heating Coil Neighboring Speed Levels Ratio {[]}
+\item
+  HVAC,Average,VSAirtoAirHP Recoverable Waste Heat {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Heating Coil Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Heating Coil Source Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Defrost Electric Power {[}W{]}
+\item
+  HVAC,Sum,Heating Coil Defrost Electric Energy {[}J{]}
+\item
+  HVAC,Average,Heating Coil Crankcase Heater Electric Power{[}W{]}
+\item
+  HVAC,Sum,Heating Coil Crankcase Heater Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Heating Coil Electric Power {[}W{]}}\label{heating-coil-electric-power-w-7}
+
+This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Heating Rate {[}W{]}}\label{heating-coil-heating-rate-w-2}
+
+The output variable is the average total heating capacity provide by the heat pump in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Sensible Heating Rate {[}W{]}}\label{heating-coil-sensible-heating-rate-w}
+
+The output variable is the average sensible heating capacity provide by the heat pump in Watts over the timestep being reported. For heating mode, the sensible capacity is equal to the total capacity.
+
+\paragraph{Heating Coil Source Side Heat Transfer Rate {[}W{]}}\label{heating-coil-source-side-heat-transfer-rate-w}
+
+The output variable is the average heat absorbed at the heat pump evaporator in Watts over the timestep being reported.
+
+\paragraph{\texorpdfstring{Heating Coil Part Load Ratio {[]}}{Heating Coil Part Load Ratio }}\label{heating-coil-part-load-ratio}
+
+This output variable is the ratio of the part-load capacity to the steady state capacity of the heating coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the heating coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
+
+\paragraph{\texorpdfstring{Heating Coil Runtime Fraction {[]}}{Heating Coil Runtime Fraction }}\label{heating-coil-runtime-fraction-6}
+
+This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The duty factor or part load fraction accounts for efficiency losses due to compressor cycling.
+
+\paragraph{Heating Coil Air Mass Flow Rate {[}kg/s{]}}\label{heating-coil-air-mass-flow-rate-kgs}
+
+The output variable is the average air mass flow rate on the load side going through the heat pump over the timestep being reported.
+
+\paragraph{Heating Coil Air Inlet Temperature {[}C{]}}\label{heating-coil-air-inlet-temperature-c}
+
+The output variable is the average entering air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Heating Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{heating-coil-air-inlet-humidity-ratio-kgwaterkgdryair}
+
+The output variable is the average entering air dry humidity ratio over the timestep being reported.
+
+\paragraph{Heating Coil Air Outlet Temperature {[}C{]}}\label{heating-coil-air-outlet-temperature-c}
+
+The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Heating Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{heating-coil-air-outlet-humidity-ratio-kgwaterkgdryair}
+
+The output variable is the average leaving air dry humidity ratio over the timestep being reported.
+
+\paragraph{\texorpdfstring{Heating Coil Upper Speed Level {[]}}{Heating Coil Upper Speed Level }}\label{heating-coil-upper-speed-level}
+
+The output variable is the average upper speed level, for interpolating performances between two neighboring speed levels.
+
+\paragraph{\texorpdfstring{Heating Coil Neighboring Speed Levels Ratio {[]}}{Heating Coil Neighboring Speed Levels Ratio }}\label{heating-coil-neighboring-speed-levels-ratio}
+
+The output variable is the average speed ratio, for interpolating performances between two neighboring speed levels.
+
+\paragraph{Heating Coil Electric Energy {[}J{]}}\label{heating-coil-electric-energy-j-4}
+
+The output variable is the total electric consumption of the heat pump in Joules over the timestep being reported.
+
+\paragraph{Heating Coil Heating Energy {[}J{]}}\label{heating-coil-heating-energy-j-2}
+
+The output variable is the total cooling output of the coil in Joules over the timestep being reported.
+
+\paragraph{Heating Coil Source Side Heat Transfer Energy {[}J{]}}\label{heating-coil-source-side-heat-transfer-energy-j-1}
+
+The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported.
+
+\paragraph{Heating Coil Defrost Electric Power{[}W{]}}\label{heating-coil-defrost-electric-powerw}
+
+The output variable is the average electric power used for defrosting, in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Defrost Electric Energy {[}J{]}}\label{heating-coil-defrost-electric-energy-j-2}
+
+The output variable is the total electric defrosting energy usage of the coil in Joules over the timestep being reported.
+
+\paragraph{Heating Coil Crankcase Heater Electric Power {[}W{]}}\label{heating-coil-crankcase-heater-electric-power-w-2}
+
+The output variable is the average power used for crankcase heater, in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Crankcase Heater Electric Energy {[}J{]}}\label{heating-coil-crankcase-heater-electric-energy-j-2}
+
+The output variable is the total electric energy usage of the coil for crankcase heater, in Joules over the timestep being reported.
+
+\subsection{Coil:WaterHeating:Desuperheater}\label{coilwaterheatingdesuperheater}
+
+A simplified approach is used to determine the performance of this water heating coil. The model assumes that the heating energy provided by this coil is reclaimed from the superheated refrigerant gas leaving a compressor (i.e., a desuperheating refrigerant-to-water heating coil) and does not impact the performance of the compressor. This coil must be used with a water heater tank (e.g., WaterHeater:Mixed) which can supply heated potable water and/or hot water for use in a plant loop (e.g., hydronic air reheat coils).
+
+Except for detailed refrigeration system models, the amount of available superheat is simply a percentage of the total heat being rejected by the DX system s condenser. Approximately 25-30\% of the energy rejected by typical refrigeration system condensers is to reduce the superheated refrigerant vapor temperature to the condensing temperature. Recovery efficiencies higher than 30\% may cause the refrigerant gas to condense which in turn impacts the performance of the refrigeration system. For this reason, the maximum heat reclaim recovery efficiency for this coil is 30\% for most sources of waste heat, including refrigeration compressor racks. The one exception to this 30\% limit is a condenser that is part of a detailed refrigeration system. In a detailed refrigeration system, the portion of the rejected heat that lies within the superheated region is explicitly calculated. Therefore, the desuperheater coils supplied by a condenser attached to a detailed refrigeration system are subject to a maximum reclaim recovery efficiency of 90\% of the heat within the superheated region.
+
+The model includes the ability to modify the heat reclaim recovery efficiency based on variations in inlet water temperature and outdoor air dry-bulb temperature.
+
+This coil model performs the following major functions:
+
+\begin{itemize}
+\item
+  calculates the amount of heat delivered to the water tank
+\item
+  calculates the electricity consumption of the integral water pump and on/off-cycle parasitic loads
+\end{itemize}
+
+The input fields for this object are described below in detail:
+
+\subsubsection{Inputs}\label{inputs-22-000}
+
+\paragraph{Field: Name}\label{field-name-21-000}
+
+This alpha field contains a unique user-assigned name for an instance of a desuperheater water heating coil. Any reference to this desuperheater coil by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-12-000}
+
+This alpha field contains the name of the schedule (ref: Schedule) that denotes whether the desuperheater coil is available to operate during a given time period. A schedule value equal to 0 denotes that the desuperheater coil is off for that time period. A value other than 0 denotes that the desuperheater coil is available to operate during that time period. During times when the desuperheater coil is scheduled off, the heater (element or burner) in the water tank object operates based on its tank set point temperature schedule and the desuperheater coil s parasitic electric power is also off for that time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Setpoint Temperature Schedule Name}\label{field-setpoint-temperature-schedule-name}
+
+This alpha field contains the name of the schedule (ref: Schedule) that specifies the set point (or cut-out ) temperature for the desuperheater coil. Temperature values used in this schedule should be in degrees Celsius. The desuperheater coil turns off when the tank water reaches this set point temperature. Once the desuperheater coil is off, the tank water temperature floats downward until it falls below the set point temperature minus the dead band temperature difference defined below (i.e., the cut-in temperature). At this point, the desuperheater coil turns on and remains on until the desuperheater coil set point temperature is reached.
+
+\paragraph{Field: Dead Band Temperature Difference}\label{field-dead-band-temperature-difference}
+
+This numeric field contains the dead band temperature difference in degrees Celsius. The desuperheater coil cut-in temperature is defined as the desuperheater coil set point temperature defined above minus this dead band temperature difference. The desuperheater coil turns on when the water temperature in the tank falls below the cut-in temperature. The desuperheater coil remains on until the water temperature in the tank rises above the desuperheater coil set point ( cut-out ) temperature defined above. The dead band temperature difference must be greater than 0 °C and less than or equal to 20 °C. If this field is left blank, the default value is 5 °C.
+
+Desuperheater water heating coils are typically used to offset energy consumption by the water tank s heater (element or burner). Therefore, the cut-in temperature for the desuperheater coil (set point minus dead band temperature difference) is usually higher than the set point temperature for the heater (element or burner) in the associated water heater tank object. At times when the water heater tank set point temperature is greater than the cut-in temperature of the desuperheater coil, the model disables the desuperheater coil and the tank s heater is used to heat the water.
+
+\paragraph{Field: Rated Heat Reclaim Recovery Efficiency}\label{field-rated-heat-reclaim-recovery-efficiency}
+
+This numeric field defines the ratio of recovered waste heat from the superheated refrigerant gas to the total rejected waste heat from the heating source (as if no heat reclaim occurred). Input values must be greater than 0 up to a maximum value is 0.3 (with a defaults of 0.25) for most sources of waste heat, including refrigeration compressor racks. The one exception to this 0.3 limit is a source that is a condenser that is part of a detailed refrigeration system. In a detailed refrigeration system, the portion of the rejected heat that lies within the superheated region is explicitly calculated. Therefore, the desuperheater coils supplied by a condenser attached to a detailed refrigeration system are subject to a maximum reclaim recovery efficiency of 0.9. with a default value is 0.8.
+
+\paragraph{Field: Rated Inlet Water Temperature}\label{field-rated-inlet-water-temperature-1}
+
+This numeric field defines the coil inlet water temperature, in degrees Celsius, that corresponds to the rated heat reclaim recovery efficiency. Also see field Heat Reclaim Efficiency Modifier Curve Name (function of temperature) below.
+
+\paragraph{Field: Rated Outdoor Air Temperature}\label{field-rated-outdoor-air-temperature}
+
+This numeric field defines the outdoor air dry-bulb temperature, in degrees Celsius, that corresponds to the rated heat reclaim recovery efficiency. The outdoor air dry-bulb temperature impacts the desuperheater coil refrigerant temperature and the amount of heat available for reclaim. Also see field Heat Reclaim Efficiency Modifier Curve Name(function of temperature) below.
+
+\paragraph{Field: Maximum Inlet Water Temperature for Heat Reclaim}\label{field-maximum-inlet-water-temperature-for-heat-reclaim}
+
+This numeric field defines the maximum coil inlet water temperature in degrees Celsius. Any time the inlet water temperature to the desuperheater coil is above this maximum allowed temperature, heat reclaim is restricted so that the tank water does not exceed this temperature.
+
+\paragraph{Field: Heat Reclaim Efficiency Function of Temperature Curve Name}\label{field-heat-reclaim-efficiency-function-of-temperature-curve-name}
+
+This alpha field specifies the name of a bi-quadratic curve object (ref: Performance Curves) that defines the variation in heat reclaim efficiency as a function of inlet fluid (air and water) temperatures. The bi-quadratic curve uses the coil inlet water temperature and outdoor air dry-bulb temperature (entering the DX coil condenser) as the independent variables. The output of this curve is multiplied by the rated heat reclaim recovery efficiency to give the heat reclaim efficiency at specific operating conditions (i.e., at temperatures different from the rating point temperatures). The curve should be normalized to have the value of 1.0 at the rating point temperatures. If this field is left blank, the heat reclaim efficiency remains constant (curve value assumed to be 1.0 for all conditions). The model restricts the product of the output of this curve and the rated heat reclaim recovery efficiency to a maximum of 0.9 for refrigeration condenser sources and 0.3 for all other sources..
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-4-000}
+
+This alpha field defines the name of the water node from which the desuperheater heating coil draws its inlet water. This node name must also match the source side outlet node name for the water heater tank used with this coil (ref. Water Heaters).
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-4-000}
+
+This alpha field defines the name of the water node to which the desuperheater heating coil sends its outlet water. This node name must also match the source side inlet node name for the water heater tank used with this coil (ref. Water Heaters).
+
+\paragraph{Field: Tank Object Type}\label{field-tank-object-type}
+
+This alpha (choice) field contains the type of water heater tank used by this desuperheater heating coil. Currently, the only valid choice is WaterHeater:Mixed.
+
+\paragraph{Field: Tank Name}\label{field-tank-name}
+
+This alpha field contains the name of the specific water heater tank (WaterHeater:Mixed object) used by this desuperheater heating coil.
+
+\paragraph{Field: Heating Source Object Type}\label{field-heating-source-object-type-1}
+
+This alpha (choice) field defines the source of superheated refrigerant gas from which the desuperheater water heating coil recovers energy through heat reclaim. Valid choices are:
+
+This alpha (choice) field defines the source of superheated refrigerant gas from which the desuperheater water heating coil recovers energy through heat reclaim. Valid choices are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  Coil:Cooling:DX:TwoSpeed
+\item
+  Coil:Cooling:DX:TwoStageWithHumidityControlMode
+\item
+  Refrigeration:CompressorRack
+\item
+  Refrigeration:Condenser:AirCooled
+\item
+  Refrigeration:Condenser:EvaporativeCooled
+\item
+  Refrigeration:Condenser:WaterCooled
+\end{itemize}
+
+\paragraph{Field: Heating Source Name}\label{field-heating-source-name-1}
+
+This alpha field defines the name of the desuperheater coil s heat source (e.g., the name of a specific coil of the type mentioned in the previous field which provides waste heat to this desuperheater water heating coil).
+
+\paragraph{Field: Water Flow Rate}\label{field-water-flow-rate}
+
+This numeric field defines the desuperheater coil s water flow rate in cubic meters per second. The model assumes that this flow rate is constant (throughout the simulation period) when the desuperheater coil operates, and that it corresponds to the heat reclaim recovery efficiency performance specified by the user. This water flow rate must be greater than zero.
+
+\paragraph{Field: Water Pump Power}\label{field-water-pump-power}
+
+This numeric field defines the coil s water circulation pump power in Watts. This is the operating pump power as installed. Values must be greater than or equal to 0. If this field is left blank, the default value is 0. A warning message will be issued if the ratio of water pump power to desuperheater water volumetric flow rate exceeds 7.9264E6 W/m\(^{3}\)/s, but the simulation will continue using the user-defined values. The model assumes that this integral pump (i.e., no need to define a separate pump object) cycles on and off with the desuperheater heating coil.
+
+\paragraph{Field: Fraction of Pump Heat to Water}\label{field-fraction-of-pump-heat-to-water}
+
+This numeric field defines the fraction of water circulation pump heat that is transferred to the water. The pump is assumed to be downstream of the desuperheater water heating coil, and this field is used to determine the desuperheater water outlet temperature. Values must be greater than or equal to 0 and less than or equal to 1. If this field is left blank, the default value is 0.2.
+
+\paragraph{Field: On-Cycle Parasitic Electric Load}\label{field-on-cycle-parasitic-electric-load}
+
+This optional numeric field contains the on-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the desuperheater water heating coil. This parasitic electric load is consumed whenever the desuperheater coil is operating, and the model assumes that this parasitic power does not contribute to heating the water nor does it affect the zone air heat balance. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
+
+\paragraph{Field: Off-Cycle Parasitic Electric Load}\label{field-off-cycle-parasitic-electric-load}
+
+This optional numeric field contains the off-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the desuperheater water heating coil. This parasitic electric load is consumed whenever the desuperheater coil is available but is not operating, and the model assumes that this parasitic power does not contribute to heating the water nor does it affect the zone air heat balance. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
+
+Following is an example input for a desuperheater water heating coil.
+
+\begin{lstlisting}
+
+Coil:WaterHeating:Desuperheater,
+  WaterHeatingCoil,               !- Coil Name
+  DesuperheaterSched,           !- Availability Schedule Name
+  DesuperheaterTempSch,       !- Desuperheater Coil Set Point Temperature Schedule Name
+  5.0,                                         !- Dead Band Temperature Difference {deltaC}
+  0.25,                                       !- Rated Heat Reclaim Recovery Efficiency
+  50.0,                                       !- Rated Inlet Water Temperature {C}
+  35.0,                                       !- Rated Outdoor Air Temperature {C}
+  60.0,                                       !- Maximum Inlet Water Temperature for Heat Reclaim {C}
+  HEffFTemp,                             !- Heat Reclaim Efficiency Modifier Curve Name (function of temperature)
+  WaterHeatingCoilInletNode,     !- Desuperheater Water Inlet Node Name
+  WaterHeatingCoilOutletNode,   !- Desuperheater Water Outlet Node Name
+  WaterHeater:Mixed,           !- Water Heater Tank Type
+  WaterHeatingCoilTank,       !- Water Heater Tank Name
+  Coil:Cooling:DX:SingleSpeed,   !- Heating Source Type
+  Furnace ACDXCoil 1,           !- Heating Source Name
+  0.0001,                                   !- Desuperheater Water Volumetric Flow Rate {m3/s}
+  100.0,                                     !- Water Pump Power {W}
+  0.2,                                         !- Fraction of Pump Heat to Water
+  10.0,                                       !- On-Cycle Parasitic Electric Load {W}
+  10.0;                                       !- Off-Cycle Parasitic Electric Load {W}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-18}
+
+\begin{itemize}
+\item
+  HVAC,Average,Water Heater Part Load Ratio
+\item
+  HVAC,Average,Water Heater Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Heating Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Water Heater Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Heat Reclaim Efficiency Modifier Multiplier {[]}
+\item
+  HVAC,Average,Water Heater On Cycle Parasitic Electric Power {[}W{]}
+\item
+  HVAC,Sum,Water Heater On Cycle Parasitic Electric Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Off Cycle Parasitic Electric Power {[}W{]}
+\item
+  HVAC,Sum,Water Heater Off Cycle Parasitic Electric Energy {[}J{]}
+\end{itemize}
+
+Water Heater Part Load Ratio {[]}This output field contains the part load ratio of the desuperheater heating coil for the timestep being reported. This ratio represents the fraction of the timestep that the desuperheater heating coil is operating.
+
+\paragraph{Water Heater Heating Rate {[}W{]}}\label{water-heater-heating-rate-w}
+
+This output field contains the average heating rate output of the desuperheater heating coil in Watts for the timestep being reported. This value includes the portion of circulation pump heat attributed to heating the water.
+
+\paragraph{Water Heater Heating Energy {[}J{]}}\label{water-heater-heating-energy-j}
+
+This output field contains the total heating output of the desuperheater heating coil in Joules for the timestep being reported. This value includes the portion of circulation pump heat attributed to heating the water.
+
+\paragraph{Water Heater Pump Electric Power {[}W{]}}\label{water-heater-pump-electric-power-w}
+
+This output field contains the average electricity consumption rate for the water circulation pump in Watts for the timestep being reported.
+
+\paragraph{Water Heater Pump Electric Energy {[}J{]}}\label{water-heater-pump-electric-energy-j}
+
+This output field contains the electricity consumption of the water circulation pump in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Water Heater Heat Reclaim Efficiency Modifier Multiplier {[]}}{Water Heater Heat Reclaim Efficiency Modifier Multiplier }}\label{water-heater-heat-reclaim-efficiency-modifier-multiplier}
+
+This output field contains the average output of the Heat Reclaim Efficiency Modifier Curve (function of temperature) for the timestep being reported.
+
+\paragraph{Water Heater On Cycle Parasitic Electric Power {[}W{]}}\label{water-heater-on-cycle-parasitic-electric-power-w}
+
+\paragraph{Water Heater On Cycle Parasitic Electric Energy {[}J{]}}\label{water-heater-on-cycle-parasitic-electric-energy-j}
+
+\paragraph{Water Heater Off Cycle Parasitic Electric Power {[}W{]}}\label{water-heater-off-cycle-parasitic-electric-power-w}
+
+\paragraph{Water Heater Off Cycle Parasitic Electric Energy {[}J{]}}\label{water-heater-off-cycle-parasitic-electric-energy-j}
+
+These outputs are the parasitic electric power and consumption associated with the desuperheater water heating coil. Specific outputs represent parasitic electrical usage during the coil on and off cycles. These outputs represent electronic controls or other electric component. The model assumes that the parasitic power does not contribute to heating the water nor does it impact the zone air heat balance. The parasitic electric consumption outputs are also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
+
+\subsection{CoilSystem:Cooling:DX}\label{coilsystemcoolingdx}
+
+The CoilSystem:Cooling:DX object is a virtual container component that consists of a DX cooling coil component and its associated controls, as shown in the Figure below. This control object supports several different types of DX cooling coils (see field Cooling Coil Object Type).
+
+This component may be used as a cooling coil in constant volume or variable volume systems, as blow through or draw through, with or without humidity controls. Unlike AirLoopHVAC:Unitary system types, this component controls only the DX coil, not the supply fan. CoilSystem:Cooling:DX is added to a system by placing it in an air loop branch (see Branch object) or in an AirLoopHVAC:OutdoorAirSystem:EquipmentList or in a ZoneHVAC:OutdoorAirUnit:EquipmentList . It requires one or more setpoint manager (see SetpointManager:*) objects to specify temperature and/or humidity setpoints (unless it is used in a ZoneHVAC:OutdoorAirUnit which has its own temperature setpoints). This object is the one that is listed in the Branch or equipment list object rather than the coil itself. A constant volume or variable volume fan is modeled separately from this cooling system. These are the only fan types allowed for this system type (ref. Fan:ConstantVolume and Fan:VariableVolume). Cycling fan operation is not available with this model. The CoilSystem:Cooling:DX object can also be placed on dedicated outdoor air system (DOAS) airloop branches or in arloop branches where the air flow to capacity ratio range is between 100 300 cfm/ton. 100\% DOAS DX cooling coils operate in lower flow to capacity ratio range compared to regular DX cooling coils. The CoilSystem:Cooling:DX is selected to operate in DOAS application or in low flow to capacity ratio range by specifying YES to the input field Use Outdoor Air DX Cooling Coil . If this optional input field is left blank or specified as NO , then the coil is modeled as regular DX cooling coil. If the CoilSystem:Cooling:DX object is in an AirLoopHVAC:OutdoorAirSystem:EquipmentList or in a ZoneHVAC:OutdoorAirUnit:EquipmentList then it is treated as 100\% DOAS DX cooling coil only if the choice input field Use Outdoor Air DX Cooling Coil is set too YES . All the control options of the regular DX cooling coils are available to DOAS DX coils as well. Heating DX coils in DOAS airloop operate at the same flow to capacity ratio limits as the DOAS DX cooling coils.
+
+\begin{figure}[hbtp] % fig 138
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image368.png}
+\caption{Schematic of CoilSystem:Cooling:DX Object in an Air Loop for a Blow Through Application \protect \label{fig:schematic-of-coilsystem-cooling-dx-object-in}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-23-000}
+
+\paragraph{Field: Name}\label{field-name-22-000}
+
+This alpha field contains the identifying name for this component.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-13-000}
+
+This alpha field contains the schedule name that contains information on the availability of the DX coil to operate. A schedule value of 0 indicates that the coil is off for that time period. A schedule value greater than 0 indicates that the coil can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: DX Cooling Coil System Inlet Node Name}\label{field-dx-cooling-coil-system-inlet-node-name}
+
+This alpha field contains the identifying name given to the DX cooling coil inlet node, as specified in the DX cooling coil object.
+
+\paragraph{Field: DX Cooling Coil System Outlet Node Name}\label{field-dx-cooling-coil-system-outlet-node-name}
+
+This alpha field contains the identifying name given to the DX cooling coil outlet node, as specified in the cooling coil object.
+
+\paragraph{Field: DX Cooling Coil System Sensor Node Name}\label{field-dx-cooling-coil-system-sensor-node-name}
+
+This alpha field contains the identifying name given to the DX cooling coil control node, this is the node at which the temperature set point is specified by the set point manager.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-000}
+
+This alpha field specifies the type of DX cooling coil. The valid choices for this field are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted
+\item
+  Coil:Cooling:DX:TwoSpeed
+\item
+  Coil:Cooling:DX:TwoStageWithHumidityControlMode
+\item
+  Coil:Cooling:DX:VariableSpeed
+\end{itemize}
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-000}
+
+This alpha field contains the identifying name of the DX cooling coil.
+
+As shown in the example below, correct specification of this system requires specification of the DX Cooling Coil object in addition to the CoilSystem:Cooling:DX object.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type}
+
+This alpha field contains the type of dehumidification control. The following options are valid for this field:
+
+\textbf{None} - meet sensible load only, no active dehumidification control
+
+\textbf{MultiMode} - activate enhanced dehumidification mode as needed and operate to meet the sensible load. If a sensible load exists, the system will operate to meet that sensible load and may not meet the latent load. If no sensible load exists, and Run on Latent Load = Yes, the system will operate to meet the entire latent load. This option is used to model DX equipment with a switchable option such as subcool reheat. It is valid only with Cooling coil type = Coil:Cooling:DX:TwoStageWithHumidityControlMode or CoilSystem:Cooling:DX:HeatExchangerAssisted. If the Run on Latent Load option below is set to Yes, this option may require the use of a heating coil and heating coil outlet air temperature set point manager downstream of this cooling coil to maintain the temperature set point.
+
+\textbf{CoolReheat} - cool beyond the dry-bulb setpoint as required to meet the humidity setpoint. It is valid only with Cooling coil type = Coil:Cooling:DX:TwoStageWithHumidityControlMode. This option requires the use of a heating coil and heating coil outlet air temperature set point manager downstream of this cooling coil to maintain the temperature set point.
+
+The default is \textbf{None}. For all dehumidification controls, the max humidity setpoint on the control node is used. This must be set using a \textbf{ZoneControl:Humidistat} \textbf{ZoneControl:Humidistat} and one of:
+
+\begin{itemize}
+\item
+  \textbf{SetpointManager:SingleZone:Humidity:Maximum}
+\item
+  \textbf{SetpointManager:MultiZone:Humidity:Maximum}
+\item
+  \textbf{SetpointManager:MultiZone:MaximumHumidity:Average}
+\end{itemize}
+
+objects and \textbf{SetpointManager:OutdoorAirPretreat} (optional) objects. When extra dehumidification is required, the equipment may not be able to meet the humidity setpoint if its full capacity is not adequate.
+
+\paragraph{Field: Run on Sensible Load}\label{field-run-on-sensible-load}
+
+This alpha field specifies if the unit will operate to meet a sensible load as determined by the inlet node dry-bulb temperature and the dry-bulb temperature setpoint on the control node. There are two valid choices, \textbf{Yes} or \textbf{No}. If \textbf{Yes}, unit will run if there is a sensible load. If \textbf{No}, unit will not run if there is only a sensible load. The default is \textbf{Yes}.
+
+\paragraph{Field: Run on Latent Load}\label{field-run-on-latent-load}
+
+This alpha field specifies if the unit will operate to meet a latent load as determined by the inlet node humidity ratio and the max humidity setpoint on the control node. There are two valid choices, \textbf{Yes} or \textbf{No}. If \textbf{Yes}, unit will run if there is a latent load. If both a sensible and latent load exist, the system will operate to maintain the temperature set point. When only a latent load exists, the system will operate to meet the humidity ratio set point and requires the use of a heating coil and heating coil outlet air temperature set point manager downstream of this cooling coil to maintain the temperature set point. If \textbf{No}, unit will not run if there is only a latent load. The default is \textbf{No}.
+
+\paragraph{Field: Use Outdoor Air DX Cooling Coil}\label{field-use-outdoor-air-dx-cooling-coil}
+
+This input field enables the Coil System DX Coil to be used for low air flow to capacity ratio range ( 100 300 cfm/ton). This flow to capacity ratio range is common in 100\% dedicated outdoor air system (DOAS) applications. Other airloop or zone HVAC systems may use this input filed if they operate at such a low flow to capacity ratio range. There are two valid choices, \textbf{Yes} or \textbf{No}. If \textbf{Yes}, the DX cooling coil is forced to operate in this flow to capacity ratio range or runs as 100\% DOAS DX coil. If \textbf{No}, DX coil is used as regular DX coil. This input field is optional.
+
+\paragraph{Field: Outdoor Air DX Cooling Coil Leaving Minimum Air Temperature}\label{field-outdoor-air-dx-cooling-coil-leaving-minimum-air-temperature}
+
+This input field is the DX cooling coil leaving supply air minimum temperature specified for frost control. The DX cooling coil leaving air temperature is not allowed to exceed this minimum coil leaving air temperature. The DX cooling coil frost controller adjusts or limits the desired coil outlet air setpoint temperature when the coil outlet temperature exceeds this minimum temperature limit specified. This input field is optional and only used along with in the input field above. The minimum and maximum values of this input field are 0.0 °C and 7.2 °C, and the default value is 2.0 °C.
+
+An example IDF specification:
+
+\begin{lstlisting}
+
+CoilSystem:Cooling:DX,
+  DX Cooling Coil System 1,!- Name
+  CoolingCoilAvailSched,     !- Availability Schedule Name
+  Cooling Coil Air Inlet Node,   !- DX Cooling Coil System Inlet Node Name
+  Air Loop Outlet Node,       !- DX Cooling Coil System Outlet Node Name
+  Air Loop Outlet Node,       !- DX Cooling Coil System Sensor Node Name
+  Coil:Cooling:DX:SingleSpeed,   !- Cooling Coil Object Type
+  ACDXCoil 1,                           !- Cooling Coil Name
+  None,                                       !- Dehumidification Control Type
+  Yes,                                         !- Run on Sensible Load
+  No,                                           !- Run on Latent Load
+  Yes,                                         !- Use DOAS DX Cooling Coil
+  2.0;                                         !- DOAS DX Cooling Coil Leaving Minimum Air Temperature
+
+
+  Coil:Cooling:DX:SingleSpeed,
+  ACDXCoil 1,                           !- Name
+  CoolingCoilAvailSched,     !- Availability Schedule Name
+  25000,                                     !- Gross Rated Total Cooling Capacity {W}
+  0.75,                                       !- Gross Rated Sensible Heat Ratio
+  3.0,                                         !- Gross Rated Cooling COP
+  1.3,                                         !- Rated Air Flow Rate {m3/s}
+  Cooling Coil Air Inlet Node,   !- Air Inlet Node Name
+  Air Loop Outlet Node,       !- Air Outlet Node Name
+  WindACCoolCapFT,                 !- Total Cooling Capacity Function of Temperature Curve Name
+  WindACCoolCapFFF,               !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  WindACEIRFT,                         !- Energy Input Ratio Function of Temperature Curve Name
+  WindACEIRFFF,                       !- Energy Input Ratio Function of Flow Fraction Curve Name
+  WindACPLFFPLR;                     !- Part Load Fraction Correlation Curve Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-19}
+
+\textbf{\emph{All DX Coils:}}
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Coil System Frost Control Status
+\end{itemize}
+
+\textbf{\emph{Coil Type = Coil:Cooling:DX:TwoStageWithHumidityControlMode}}
+
+\begin{itemize}
+\item
+  HVAC,Average,Coil System Cycling Ratio
+\item
+  HVAC,Average,Coil System Compressor Speed Ratio
+\end{itemize}
+
+\textbf{\emph{Coil types = Coil:Cooling:DX:SingleSpeed \& CoilSystem:Cooling:DX:HeatExchangerAssisted}}
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Coil System Part Load Ratio
+\end{itemize}
+
+\paragraph{Coil System Cycling Ratio}\label{coil-system-cycling-ratio}
+
+The system may operate for the entire system timestep, but to meet the load the compressor can cycle on and off. This reports the fraction of the system timestep that the compressor is operating. (1.0 is continuous, 0.0 is off).
+
+\paragraph{Coil System Compressor Speed Ratio}\label{coil-system-compressor-speed-ratio}
+
+This is the ratio of time in a system timestep that the compressor is at rated speed. The compressor speed ratio reports (1.0 is max, 0.0 is min) and any value in between as it is averaged over the timestep.
+
+\paragraph{Coil System Part Load Ratio}\label{coil-system-part-load-ratio}
+
+The DX system can operate with a cycling compressor or a varying speed compressor, This variable reports the fraction of the Full Load that is met during the system timestep. This can differ from the cycling part load ratio or the compressor speed ratio. (1.0 is Full Load and 0.0 is no load)
+
+\paragraph{Coil System Frost Control Status}\label{coil-system-frost-control-status}
+
+This is a flag indicating whether frost control is active at current time step or not. Frost control is activated or enforced when the sensible load control requires DX cooling coil outlet air temperature below the user specified minimum temperature or when the dehumidification load control requires DX cooling coil outlet air humidity ratio below the saturation humidity ratio corresponding to the user specified minimum temperature for frost control. Frost control status of zero means no active frost control, a value of 1 or 2 indicates that frost control is active. If frost control status is 1, then the frost control was enforced when the cooling coil is run to meet sensible load. If the frost control status value is 2, then the control was enforced when the cooling coil is run to meet latent load. When frost control is active the DX cooling coil setpoint value is modified based on user specified limit.
+
+\subsection{CoilSystem:Heating:DX}\label{coilsystemheatingdx}
+
+The CoilSystem:Heating:DX object is a virtual container component for a DX heating coil that provides the controls needed to operate the coil. Only single speed DX air-to-air heating coils are supported.
+
+This component may be used as a heating coil in constant volume or variable volume air handlers. It can also be used in an outside air system (by including it in an AirLoopHVAC:OutdoorAirSystem:EquipmentList object)or in a zone outdoor air unit (by including it in an ZoneHVAC:OutdoorAirUnit:EquipmentList object). This object is the one that is listed in the Branch or equipment list object rather than the coil itself.
+
+The inlet and outlet nodes for the DX heat pump system are defined in the heating coil object. The control node is always the outlet node of the coil. This DX heat pump heating system requires that a (drybulb) temperature setpoint be placed on the outlet node using either a setpoint manager or the energy management system. The coil is controlled to attempt to meet that setpoint using a part load ratio modeling approach.
+
+This model only supports continuous fan and cycling compressor operation -- cycling fan modeling is not available with this model.
+
+\subsubsection{Inputs}\label{inputs-24}
+
+\paragraph{Field: Name}\label{field-name-23-000}
+
+This alpha field contains the identifying name for this component.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-14}
+
+This alpha field contains the schedule name that contains information on the availability of the DX coil to operate. A schedule value of 0 indicates that the coil is off for that time period. A schedule value greater than 0 indicates that the coil can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-000}
+
+This alpha field specifies the type of DX heating coil. This model currently supports only single speed DX heat pump heating coils and the only options for this field are Coil:Heating:DX:SingleSpeed and Coil:Heating:DX:VariableSpeed.
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-000}
+
+This alpha field specifies the unique name of the DX heating coil. This field references the name of a Coil:Heating:DX:SingleSpeed that needs to be defined elsewhere in the input file.
+
+An example of a DX heating coil system follows.
+
+\begin{lstlisting}
+
+CoilSystem:Heating:DX,
+  HeatPump DX Coil 1, !- Name
+  FanAndCoilAvailSched , !- Availability Schedule Name
+  Coil:Heating:DX:SingleSpeed,   !- Heating Coil Object Type
+  Heat Pump DX Heating Coil 1;   !- Heating Coil Name
+
+
+  Coil:Heating:DX:SingleSpeed,
+  Heat Pump DX Heating Coil 1,   !- Name
+  FanAndCoilAvailSched,       !- Availability Schedule Name
+  autosize,                               !- Gross Rated Heating Capacity {W}
+  2.75,                                       !- Gross Rated Heating COP {W/W}
+  autosize,                               !- Rated Air Flow Rate {m3/s}
+  Heating Coil Air Inlet Node,   !- Air Inlet Node Name
+  SuppHeating Coil Air Inlet Node,   !- Air Outlet Node Name
+  HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACCOOLPLFFPLR,                 !- Part Load Fraction Correlation Curve Name
+  ,                                               !- Defrost Energy Input Ratio Function of Temperature Curve Name
+  -8.0,                                       !- Minimum Outdoor Dry-Bulb Temperature for Compressor Operation {C}
+  5.0,                                         !- Maximum Outdoor Dry-Bulb Temperature for Defrost Operation {C}
+  200.0,                                     !- Crankcase Heater Capacity {W}
+  10.0,                                       !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
+  Resistive,                             !- Defrost Strategy
+  TIMED,                                     !- Defrost Control
+  0.166667,                               !- Defrost Time Period Fraction
+  autosize,                               !- Resistive Defrost Heater Capacity {W}
+  Heat Pump 1 Evaporator Node;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-20}
+
+\paragraph{Coil System Part Load Ratio}\label{coil-system-part-load-ratio-1}
+
+The DX system can operate with a cycling compressor or a varying speed compressor, This variable reports the fraction of the Full Load that is met during the system timestep. This can differ from the cycling part load ratio or the compressor speed ratio. (1.0 is Full Load and 0.0 is no load)
+
+\subsection{CoilSystem:Cooling:DX:HeatExchangerAssisted}\label{coilsystemcoolingdxheatexchangerassisted}
+
+The heat exchanger-assisted DX cooling coil is a virtual component consisting of a direct expansion (DX) cooling coil and an air-to-air heat exchanger as shown in Figure~\ref{fig:schematic-of-the-coilsystem-cooling-dx} below. The air-to-air heat exchanger pre-conditions the air entering the cooling coil, and reuses this energy to post-condition the supply air leaving the cooling coil. This heat exchange process improves the latent removal performance of the cooling coil by allowing it to dedicate more of its cooling capacity toward dehumidification (lower sensible heat ratio).
+
+This compound object models the basic operation of an air-to-air heat exchanger in conjunction with a cooling coil. The heat exchanger-assisted DX cooling coil does not have an operating schedule of its own; its operating schedule is governed by the availability schedules for the DX cooling coil and the air-to-air heat exchanger. This compound object is used in place of where a DX cooling coil object would normally be used by itself.
+
+To model a heat exchanger-assisted DX cooling coil, the input data file should include the following objects:
+
+\begin{itemize}
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted object
+\item
+  Air-to-air heat exchanger object (HeatExchanger:AirToAir:FlatPlate, HeatExchanger:AirToAir:SensibleAndLatent, or HeatExchanger:Desiccant:BalancedFlow)
+\item
+  DX cooling coil object (Coil:Cooling:DX:SingleSpeed)
+\end{itemize}
+
+In terms of controlling the operation of the heat exchanger, the heat exchanger is assumed to always provide its heat transfer when the associated DX cooling coil is operating and no high humidity control mechanism is specified. However, the heat exchanger s energy transfer may be controlled (i.e., turned on and off) based on a zone air humidity level using either a humidistat (ref. AirLoopHVAC:Unitary:Furnace:HeatCool or AirLoopHVAC:UnitaryHeatCool) or a humidistat and a maximum humidity set point manager to place a humidity ratio set point on the appropriate control node (ref. CoilSystem:Cooling:DX). This model may also be used with the unitary changeover bypass system and the unitary air-to-air heat pump system (ref. AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass and AirLoopHVAC:UnitaryHeatPump:AirToAir); however, the heat exchanger is assumed to always provide its heat transfer when the cooling coil operates and cannot be turned on and off based on a zone air humidity set point. Two zone air conditioners may also use this model for improved dehumidification. The first type is the packaged terminal heat pump (ref. ZoneHVAC:PackagedTerminalHeatPump) where the heat exchanger s heat transfer is always active whenever the cooling coil operates. The second type is the window air conditioner (ref. ZoneHVAC:WindowAirConditioner) where the heat exchanger s heat transfer is always active when the cooling coil operates and no high humidity control mechanism is specified, OR the heat exchanger s heat transfer may be controlled based on zone air humidity level if a humidistat and high humidity set point manager are specified (maximum humidity ratio set point placed on the heat exchanger s exhaust air outlet node, ref. Figure~\ref{fig:schematic-of-the-coilsystem-cooling-dx}).
+
+Links to the cooling coil and air-to-air heat exchanger specifications are provided in the input data syntax for this compound object. A description of each input field for this compound object is provided below.
+
+\begin{figure}[hbtp] % fig 139
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image369.png}
+\caption{Schematic of the CoilSystem:Cooling:DX:HeatExchangerAssisted compound object \protect \label{fig:schematic-of-the-coilsystem-cooling-dx}}
+\end{figure}
+
+NOTE: Node naming shown in Figure~\ref{fig:schematic-of-the-coilsystem-cooling-dx} is representative for HeatExchanger:AirToAir:SensibleAndLatent. For HeatExchanger:AirToAir:FlatPlate, the exhaust air nodes are referred to as secondary air nodes. For HeatExchanger:Desiccant:BalancedFlow, the supply air nodes are referred to as regeneration air nodes and the exhaust air nodes as process air nodes.
+
+\subsubsection{Inputs}\label{inputs-25}
+
+\paragraph{Field: Name}\label{field-name-24-000}
+
+A unique user-assigned name for the heat exchanger-assisted DX cooling coil. Any reference to this compound component by another object will use this name.
+
+\paragraph{Field: Heat Exchanger Object Type}\label{field-heat-exchanger-object-type-000}
+
+This alpha field denotes the type of heat exchanger being modeled. Valid choices are:
+
+\begin{itemize}
+\item
+  HeatExchanger:AirToAir:FlatPlate
+\item
+  HeatExchanger:AirToAir:SensibleAndLatent
+\item
+  HeatExchanger:Desiccant:BalancedFlow
+\end{itemize}
+
+\paragraph{Field: Heat Exchanger Name}\label{field-heat-exchanger-name-001}
+
+This alpha field denotes the name of the air-to-air heat exchanger being modeled.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-1}
+
+This alpha field denotes the type of DX cooling coil being modeled. The only valid choice is Coil:Cooling:DX:SingleSpeed.
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-1}
+
+This alpha field denotes the name of the DX cooling coil being modeled.
+
+Following is an example input for this compound object:
+
+\begin{lstlisting}
+
+CoilSystem:Cooling:DX:HeatExchangerAssisted,
+  HeatExchangerAssistedCoolingCoil,               ! Name of the heat exchanger assisted cooling coil
+  HeatExchanger:AirToAir:SensibleAndLatent,       ! Heat exchanger type
+  Air to Air Heat Exchanger 1,                    ! Heat exchanger name
+  Coil:Cooling:DX:SingleSpeed,                    ! Cooling coil type
+  DX Cooling Coil 1;                              ! Cooling coil name
+
+
+  HeatExchanger:AirToAir:SensibleAndLatent,
+  Air to Air Heat Exchanger 1,        !- Heat exchanger name
+  FanAndCoilAvailSched,               !- Availability schedule name
+  1.3,                                !- Nominal supply air flow rate {m3/s}
+  .2,                                 !- Sensible effectiveness at 100% airflow heating condition
+  .0,                                 !- Latent effectiveness at 100% airflow heating condition
+  .23,                                !- Sensible effectiveness at 75% airflow heating condition
+  .0,                                 !- Latent effectiveness at 75% airflow heating condition
+  .2,                                 !- Sensible effectiveness at 100% airflow cooling condition
+  .0,                                 !- Latent effectiveness at 100% airflow cooling condition
+  .23,                                !- Sensible effectiveness at 75% airflow cooling condition
+  .0,                                 !- Latent effectiveness at 75% airflow cooling condition
+  HeatExchangerSupplyAirInletNode,    !- Supply air inlet node name
+  DX Cooling Coil Air Inlet Node,     !- Supply air outlet node name
+  HeatExchangerExhaustAirInletNode,   !- Exhaust air inlet node name
+  HeatExchangerExhaustAirOutletNode,  !- Exhaust air outlet node name
+  50.0,                               !- Nominal electric power {W}
+  No,                                 !- Supply air outlet temperature control
+  Rotary,                             !- Heat exchanger type
+  None;                               !- Frost control type
+
+
+  Coil:Cooling:DX:SingleSpeed,
+  DX Cooling Coil 1,                  !- Coil Name
+  FanAndCoilAvailSched,               !- Availability Schedule
+  25000,                              !- Gross Rated Total Cooling Capacity {W}
+  0.75,                               !- Gross Rated Sensible Heat Ratio
+  3.0,                                !- Gross Rated Cooling COP
+  1.3,                                !- Rated Air Flow Rate {m3/s}
+  DX Cooling Coil Air Inlet Node,     !- Coil Air Inlet Node
+  HeatExchangerExhaustAirInletNode,   !- Coil Air Outlet Node
+  ACCoolCapFT,                  !- Total Cooling Capacity Modifier Curve (function of temperature)
+  ACCoolCapFFF,                 !- Total Cooling Capacity Modifier Curve (function of flow fraction)
+  ACEIRFT,                      !- Energy Input Ratio Modifier Curve (function of temperature)
+  ACEIRFFF,                     !- Energy Input Ratio Modifier Curve (function of flow fraction)
+  ACPLFFPLR;                    !- Part Load Fraction Correlation (function of part load ratio)
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-21}
+
+No variables are reported for this compound object. However, outputs are provided by the cooling coil and heat exchanger that are specified.
+
+\subsection{CoilSystem:Cooling:Water:HeatExchangerAssisted}\label{coilsystemcoolingwaterheatexchangerassisted}
+
+The heat exchanger-assisted water cooling coil is a virtual component consisting of a chilled-water cooling coil and an air-to-air heat exchanger as shown in Figure~\ref{fig:schematic-of-the-coilsystem-cooling-water} below. The air-to-air heat exchanger precools the air entering the cooling coil, and reuses this energy to reheat the supply air leaving the cooling coil. This heat exchange process improves the latent removal performance of the cooling coil by allowing it to dedicate more of its cooling capacity toward dehumidification (lower sensible heat ratio).
+
+\begin{figure}[hbtp] % fig 140
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image370.png}
+\caption{Schematic of the CoilSystem:Cooling:Water:HeatExchangerAssisted compound object \protect \label{fig:schematic-of-the-coilsystem-cooling-water}}
+\end{figure}
+
+Note: Node naming shown in Figure~\ref{fig:schematic-of-the-coilsystem-cooling-water} is representative for HeatExchanger:AirToAir:SensibleAndLatent. For HeatExchanger:AirToAir:FlatPlate, the exhaust air nodes are referred to as secondary air nodes.
+
+This compound object models the basic operation of an air-to-air heat exchanger in conjunction with a chilled-water cooling coil. The heat exchanger-assisted water cooling coil does not have an operating schedule of its own; its operating schedule is governed by the availability schedules for the chilled-water cooling coil and the air-to-air heat exchanger. Heat exchange will occur whenever the heat exchanger is available to operate (via its availability schedule) and a temperature difference exists between the two air streams -- there is currently no method to enable or disable heat exchange based on zone air humidity level. This compound object is used in place of where a chilled-water cooling coil object would normally be used by itself.
+
+To model a heat exchanger-assisted water cooling coil, the input data file should include the following objects:
+
+\begin{itemize}
+\item
+  CoilSystem:Cooling:Water:HeatExchangerAssisted compound object
+\item
+  Air-to-air heat exchanger object (HeatExchanger:AirToAir:FlatPlate or HeatExchanger:AirToAir:SensibleAndLatent)
+\item
+  Chilled-water cooling coil object (Coil:Cooling:Water or Coil:Cooling:Water:DetailedGeometry)
+\end{itemize}
+
+Links to the cooling coil and air-to-air heat exchanger specifications are provided in the input data syntax for this compound object. A description of each input field for this compound object is provided below.
+
+\subsubsection{Inputs}\label{inputs-26}
+
+\paragraph{Field: Name}\label{field-name-25-000}
+
+A unique user-assigned name for the heat exchanger-assisted water cooling coil. Any reference to this compound component by another object (e.g., ZoneHVAC:UnitVentilator, ZoneHVAC:FourPipeFanCoil, component in an air loop Branch object) will use this name.
+
+\paragraph{Field: Heat Exchanger Object Type}\label{field-heat-exchanger-object-type-1}
+
+This alpha field denotes the type of heat exchanger being modeled. Valid choices are:
+
+HeatExchanger:AirToAir:FlatPlate
+
+HeatExchanger:AirToAir:SensibleAndLatent
+
+\paragraph{Field: Heat Exchanger Name}\label{field-heat-exchanger-name-1}
+
+This alpha field denotes the name of the air-to-air heat exchanger being modeled.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-2}
+
+This alpha field denotes the type of chilled-water cooling coil being modeled. Valid choices are:
+
+Coil:Cooling:Water
+
+Coil:Cooling:Water:DetailedGeometry
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-2}
+
+This alpha field denotes the name of the chilled-water cooling coil being modeled.
+
+Following is an example input for this compound object:
+
+\begin{lstlisting}
+
+CoilSystem:Cooling:Water:HeatExchangerAssisted,
+  Heat Exchanger Assisted Cooling Coil 1, !- Name of the heat exchanger assisted cooling coil
+  HeatExchanger:AirToAir:FlatPlate,     !- Heat exchanger type
+  Heat Exchanger Assisting Cooling Coil,   !- Heat exchanger name
+  Coil:Cooling:Water:DetailedGeometry,                 !- Cooling coil type
+  Main Cooling Coil 1;                                       !- Cooling coil name
+
+
+  HeatExchanger:AirToAir:FlatPlate,
+  Heat Exchanger Assisting Cooling Coil,   !- Name
+  CoolingCoilAvailSched,     !- Availability Schedule Name
+  Counter Flow,                       !- flow arrangement
+  Yes,                                         !- Economizer lockout
+  1.0,                                         !- hA ratio
+  1.32,                                       !- Nominal supply air flow rate {m3/s}
+  24.0,                                       !- Nominal supply air inlet temperature {C}
+  21.0,                                       !- Nominal supply air outlet temperature {C}
+  1.32,                                       !- Nominal secondary air flow rate {m3/s}
+  12.0,                                       !- Nominal secondary air inlet temperature {C}
+  100.0,                                     !- Nominal electric power {W}
+  Mixed Air Node 1,               !- Supply air inlet node
+  Main Cooling Coil 1 Inlet Node,   !- Supply air outlet node
+  Main Cooling Coil 1 Outlet Node, !- Secondary air inlet node
+  Main Heating Coil 1 Inlet Node;   !- Secondary air outlet node
+
+
+
+
+  Coil:Cooling:Water:DetailedGeometry,
+  Main Cooling Coil 1,         !- Coil Name
+  CoolingCoilAvailSched,     !- Availability Schedule Name
+  autosize,                               !- Max Water Flow Rate of Coil {m3/s}
+  autosize,                               !- Tube Outside Surf Area {m2}
+  autosize,                               !- Total Tube Inside Area {m2}
+  autosize,                               !- Fin Surface Area {m2}
+  autosize,                               !- Minimum Air Flow Area {m2}
+  autosize,                               !- Coil Depth {m}
+  autosize,                               !- Fin Diameter {m}
+  ,                                               !- Fin Thickness {m}
+  ,                                               !- Tube Inside Diameter {m}
+  ,                                               !- Tube Outside Diameter {m}
+  ,                                               !- Tube Thermal Conductivity {W/m-K}
+  ,                                               !- Fin Thermal Conductivity {W/m-K}
+  ,                                               !- Fin Spacing {m}
+  ,                                               !- Tube Depth Spacing {m}
+  ,                                               !- Number of Tube Rows
+  autosize,                               !- Number of Tubes per Row
+  Main Cooling Coil 1 Water Inlet Node,   !- Coil_Water_Inlet_Node
+  Main Cooling Coil 1 Water Outlet Node, !- Coil_Water_Outlet_Node
+  Main Cooling Coil 1 Inlet Node,     !- Coil_Air_Inlet_Node
+  Main Cooling Coil 1 Outlet Node;   !- Coil_Air_Outlet_Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-22}
+
+No variables are reported for this compound object. However, outputs are provided by the cooling coil and heat exchanger that are specified.
+
+\subsection{Coil:WaterHeating:AirToWaterHeatPump:Pumped}\label{coilwaterheatingairtowaterheatpumppumped}
+
+EnergyPlus can model a heat pump water heater (HPWH) consisting of a water heater tank (e.g., \lstinline!WaterHeater:Mixed!), a direct expansion (DX) coil (i.e., an air-to-water DX compression system which includes a water heating coil, air coil, compressor, and water pump), and a fan to provide air flow across the air coil associated with the DX compression system. These objects work together to model a system which heats water using zone air, outdoor air, or a combination of zone and outdoor air as the primary heat source.
+
+The \lstinline!WaterHeater:HeatPump:PumpedCondenser! compound object, water heater tank object (e.g., \lstinline!WaterHeater:Mixed!), and fan object (e.g., \lstinline!Fan:OnOff!) are defined elsewhere in this reference document. \lstinline!Coil:WaterHeating:AirToWaterHeatPump:Pumped! object described here models an air-to-water DX compression system to determine its air-side and water-side performance. This DX coil object calculates the air-side sensible and latent cooling capacity at the specific operating conditions for each simulation timestep, as well as the condenser's water-side temperature difference at a given condenser water flow rate.
+
+The heat pump water heater DX coil model performs the following major functions:
+
+\begin{itemize}
+\item
+  calculates the electric consumption of the DX compressor and water pump
+\item
+  calculates the amount of heat delivered to the water tank
+\item
+  calculates the electric consumption of the compressor's crankcase heater
+\item
+  calculates the air-side performance of the DX coil
+\end{itemize}
+
+The input fields for this object are described below in detail:
+
+\subsubsection{Inputs}\label{inputs-27}
+
+\paragraph{Field: Name}\label{field-name-26-000}
+
+This alpha field defines a unique user-assigned name for an instance of a heat pump water heater DX coil. Any reference to this coil by another object (e.g., \lstinline!WaterHeater:HeatPump:PumpedCondenser!) will use this name.
+
+\paragraph{Field: Rated Heating Capacity}\label{field-rated-heating-capacity}
+
+This numeric field defines the DX coil heating capacity in Watts at the rated evaporator inlet air temperatures, rated condenser inlet water temperature, rated evaporator air flow rate, and rated condenser water flow rate specified below. Values must be greater than 0. This value represents water heating capacity, and it may or may not include the impact of condenser pump heat (see field Condenser Pump Heat Included in Rated Heating Capacity below).
+
+\paragraph{Field: Rated COP}\label{field-rated-cop}
+
+This numeric field defines the DX coil's water heating coefficient of performance (COP = water heating capacity in watts divided by electrical power input in watts) at rated conditions (rated inlet temperatures and flow rates specified below). This input not only determines the electric energy use of the heat pump DX coil, but also the amount of total air cooling provided by the evaporator. The rated COP includes compressor power, and may or may not include condenser pump power or evaporator fan power (see field Evaporator Fan Power Included in Rated COP and field Condenser Pump Power Included in Rated COP). Values must be greater than 0. If this field is left blank, the default value is 3.2.
+
+\paragraph{Field: Rated Sensible Heat Ratio}\label{field-rated-sensible-heat-ratio-1}
+
+This numeric field defines the air-side sensible heat ratio (SHR = sensible cooling capacity divided by total cooling capacity) of the DX coil at rated conditions (rated inlet temperatures and flow rates specified below). This value should not include the effect of evaporator fan heat. Values must be greater than or equal to 0.5, and less than or equal to 1.0. The default value is 0.85.
+
+\paragraph{Field: Rated Evaporator Inlet Air Dry-Bulb Temperature}\label{field-rated-evaporator-inlet-air-dry-bulb-temperature}
+
+This numeric field defines the evaporator inlet air dry-bulb temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 5 °C. If this field is left blank, the default value is 19.7 °C.
+
+\paragraph{Field: Rated Evaporator Inlet Air Wet-Bulb Temperature}\label{field-rated-evaporator-inlet-air-wet-bulb-temperature}
+
+This numeric field defines the evaporator inlet air wet-bulb temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 5 °C. If this field is left blank, the default value is 13.5 °C.
+
+\paragraph{Field: Rated Condenser Inlet Water Temperature}\label{field-rated-condenser-inlet-water-temperature}
+
+This numeric field defines the condenser inlet water temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 25 °C. If this field is left blank, the default value is 57.5 °C.
+
+\paragraph{Field: Rated Evaporator Air Flow Rate}\label{field-rated-evaporator-air-flow-rate}
+
+This numeric field defines the evaporator air volume flow rate in cubic meters per second at rated conditions. Values must be greater than 0. If this field is left blank or autocalculated (field value = \textbf{autocalculate}), the default value is 5.035E-5 m\(^{3}\)/s/W (31.25 cfm/MBH) multiplied by the Rated Heating Capacity specified above. When autocalculating the rated evaporator air volumetric flow rate, a zone sizing object is not required.
+
+\paragraph{Field: Rated Condenser Water Flow Rate}\label{field-rated-condenser-water-flow-rate}
+
+This numeric field defines the condenser water volumetric flow rate in cubic meters per second at rated conditions. Values must be greater than 0. If this field is left blank or autocalculated (field value = \textbf{autocalculate}), the default value is 4.487E-8 m\(^{3}\)/s/W (0.208 gpm/MBH) multiplied by the Rated Heating Capacity specified above. When autocalculating the rated condenser water volumetric flow rate, a zone sizing object is not required. A warning message will be issued if the ratio of Rated Condenser Water Volumetric Flow Rate to Rated Heating Capacity is less than 1.79405E-8 m\(^{3}\)/s/W (0.083 gpm/MBH) or greater than 8.97024E-8 m\(^{3}\)/s/W (0.417 gpm/MBH), but the simulation will continue.
+
+\paragraph{Field: Evaporator Fan Power Included in Rated COP}\label{field-evaporator-fan-power-included-in-rated-cop}
+
+This choice field specifies if evaporator fan power is included in the rated COP defined above. This input impacts the calculation of compressor electric power and total air cooling provided by the evaporator for each simulation timestep. If Yes is selected, the evaporator fan power is subtracted from the total electric heating power when calculating total evaporator cooling capacity. If No is selected, it is assumed that the total heating power does not include evaporator fan power. If this field is left blank, the default is Yes. See the Engineering Reference section for \lstinline!Coil:WaterHeating:AirToWaterHeatPump:\*! for further details.
+
+\paragraph{Field: Condenser Pump Power Included in Rated COP}\label{field-condenser-pump-power-included-in-rated-cop}
+
+This choice field specifies if condenser pump power is included in the rated COP defined above. This input impacts the calculation of compressor electric power which then impacts the total air cooling provided by the evaporator for each simulation timestep. If Yes is selected, the condenser pump power is subtracted from the total electric heating power when calculating total evaporator cooling capacity. If No is selected, it is assumed that the total heating power does not include the condenser pump. If this field is left blank, the default is No. See Engineering Reference section for \lstinline!Coil:WaterHeating:AirToWaterHeatPump:\*! for further details.
+
+\paragraph{Field: Condenser Pump Heat Included in Rated Heating Capacity and Rated COP}\label{field-condenser-pump-heat-included-in-rated-heating-capacity-and-rated-cop}
+
+This choice field specifies if condenser pump heat is included in the rated heating capacity and rated COP defined above. This input impacts the calculation of compressor electric power and total air cooling provided by the evaporator for each simulation timestep. If Yes is selected, the condenser pump heat is already included in the rated heating capacity and rated COP. If No is selected, it is assumed that the rated heating capacity and rated COP do not include the condenser pump heat, and pump heat is added to the total water heating capacity based on the Condenser Water Pump Power and Fraction of Condenser Pump Heat to Water fields below. If this field is left blank, the default is No. See Engineering Reference section for \lstinline!Coil:WaterHeating:AirToWaterHeatPump:\*! for further details.
+
+\paragraph{Field: Condenser Water Pump Power}\label{field-condenser-water-pump-power}
+
+This numeric field defines the DX coil's condenser pump power in Watts. This is the operating pump power as installed. Values must be greater than or equal to 0. If this field is left blank, the default value is 0. A warning message will be issued if the ratio of Condenser Water Pump Power to Rated Heating Capacity exceeds 0.1422 W/W (41.67 Watts/MBH), but the simulation will continue.
+
+\paragraph{Field: Fraction of Condenser Pump Heat to Water}\label{field-fraction-of-condenser-pump-heat-to-water}
+
+This numeric field defines the fraction of condenser pump heat that is transferred to the condenser water. The pump is assumed to be downstream of the condenser water coil, and this field is used to determine the water temperature at the condenser outlet node when the field Condenser Pump Power Included in Rated Heating Capacity is set to No. Values must be greater than or equal to 0 and less than or equal to 1. If this field is left blank, the default value is 0.2.
+
+\paragraph{Field: Evaporator Air Inlet Node Name}\label{field-evaporator-air-inlet-node-name-1}
+
+This alpha field defines the name of the air node from which the evaporator coil draws its inlet air.
+
+\paragraph{Field: Evaporator Air Outlet Node Name}\label{field-evaporator-air-outlet-node-name}
+
+This alpha field defines the name of the air node to which the evaporator coil sends its outlet air.
+
+\paragraph{Field: Condenser Water Inlet Node Name}\label{field-condenser-water-inlet-node-name}
+
+This alpha field defines the name of the node from which the DX coil condenser draws its inlet water. This node name must also match the source side outlet node name for the water heater tank connected to this DX coil (ref: Water Heaters).
+
+\paragraph{Field: Condenser Water Outlet Node Name}\label{field-condenser-water-outlet-node-name}
+
+This alpha field defines the name of the node to which the heat pump condenser sends it outlet water. This node name must also match the source side inlet node name for the water heater tank connected to this DX coil (ref: Water Heaters).
+
+\paragraph{Field: Crankcase Heater Capacity}\label{field-crankcase-heater-capacity-7}
+
+This numeric field defines the compressor's crankcase heater capacity in Watts. The crankcase heater only operates when the compressor is off and the air surrounding the compressor is below the Maximum Ambient Temperature for Crankcase Heater Operation specified below.
+
+\paragraph{Field: Maximum Ambient Temperature for Crankcase Heater Operation}\label{field-maximum-ambient-temperature-for-crankcase-heater-operation}
+
+This numeric field defines the maximum ambient temperature for crankcase heater operation in degree Celsius. The crankcase heater only operates when the air surrounding the compressor is below this maximum temperature value and the compressor is off. The ambient temperature surrounding the compressor is set by the Heat Pump:Water Heater parent object (field Compressor Location).
+
+\paragraph{Field: Evaporator Air Temperature Type for Curve Objects}\label{field-evaporator-air-temperature-type-for-curve-objects}
+
+This choice field specifies the air temperature type used for the heating capacity and COP modifier curve objects below. The valid selections are Dry-bulb Temperature and Wet-bulb Temperature. If dry-bulb temperature is selected, the inlet air dry-bulb temperature entering the heat pump DX coil and fan section is used to evaluate the curve objects. If wet-bulb temperature is selected, the inlet air wet-bulb temperature entering the heat pump DX coil and fan section is used to evaluate the curve objects. If this field is left blank and the following curve names are defined, the default value is wet-bulb temperature. If the following curve names are not defined, this field is not used.
+
+\paragraph{Field: Heating Capacity Function of Temperature Curve Name}\label{field-heating-capacity-function-of-temperature-curve-name-1}
+
+This alpha field specifies the name of a \textbf{biquadratic} or \textbf{cubic} performance curve object (ref: Performance Curves) that defines the variation in DX coil heating capacity as a function of inlet fluid (air and water) temperatures. The biquadratic curve uses evaporator inlet air temperature (dry-bulb or wet-bulb temperature based on the field Evaporator Air Temperature Type for Curve Objects defined above) and condenser inlet water temperature as the independent variables. The cubic curve uses evaporator inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The output of this curve is multiplied by the rated heating capacity to give the heating capacity at specific operating conditions (i.e., at temperatures different from the rating point temperatures). The curve should be normalized to have the value of 1.0 at the rating point temperatures. If this field is left blank, the heating capacity remains constant (curve value assumed to be 1.0 for all conditions).
+
+\paragraph{Field: Heating Capacity Function of Air Flow Fraction Curve Name}\label{field-heating-capacity-function-of-air-flow-fraction-curve-name}
+
+This alpha field specifies the name of a \textbf{quadratic} or \textbf{cubic} performance curve object (ref: Performance Curves) that defines the variation in DX coil heating capacity as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate. The output of this curve is multiplied by the rated heating capacity and the heating capacity modifier curve (function of temperature) to give the DX coil heating capacity at the specific inlet fluid temperatures and air flow rate at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated evaporator air flow rate (air flow fraction of 1.0). If this field is left blank, the heating capacity remains constant (curve value assumed to be 1.0 for all air flow rates).
+
+\paragraph{Field: Heating Capacity Function of Water Flow Fraction Curve Name}\label{field-heating-capacity-function-of-water-flow-fraction-curve-name}
+
+This alpha field specifies the name of a \textbf{quadratic} or \textbf{cubic} performance curve object (ref: Performance Curves) that defines the variation in DX coil heating capacity as a function of the ratio of actual water flow rate through the condenser to the rated condenser water flow rate. The output of this curve is multiplied by the rated heating capacity and the output from the two other heating capacity modifier curves (function of temperature and function of air flow fraction) to give the DX coil heating capacity at the specific inlet fluid temperatures and flow rates at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated condenser water flow rate (water flow fraction of 1.0). If this field is left blank, the heating capacity remains constant (curve value assumed to be 1.0 for all water flow rates).
+
+\paragraph{Field: Heating COP Function of Temperature Curve Name}\label{field-heating-cop-function-of-temperature-curve-name}
+
+This alpha field specifies the name of a \textbf{biquadratic} or \textbf{cubic} performance curve object (ref: Performance Curves) that defines the variation in DX coil heating COP as a function of inlet fluid (air and water) temperatures. The biquadratic curve uses evaporator inlet air temperature (dry-bulb or wet-bulb temperature based on the field Evaporator Air Temperature Type for Curve Objects defined above) and condenser inlet water temperature as the independent variables. The cubic curve uses evaporator inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The output of this curve is multiplied by the rated COP to give the heating COP at specific operating conditions (i.e., at temperatures different from the rating point temperatures). The curve should be normalized to have the value of 1.0 at the rating point temperatures. If this field is left blank, the COP remains constant (curve value assumed to be 1.0 for all conditions).
+
+\paragraph{Field: Heating COP Function of Air Flow Fraction Curve Name}\label{field-heating-cop-function-of-air-flow-fraction-curve-name}
+
+This alpha field specifies the name of a \textbf{quadratic} or \textbf{cubic} performance curve object (ref: Performance Curves) that defines the variation in DX coil heating COP as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate. The output of this curve is multiplied by the rated COP and the heating COP modifier curve (function of temperature) to give the heating COP at the specific inlet fluid temperatures and air flow rate at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated evaporator air flow rate (air flow fraction of 1.0). If this field is left blank, the heating COP remains constant (curve value assumed to be 1.0 for all air flow rates).
+
+\paragraph{Field: Heating COP Function of Water Flow Fraction Curve Name}\label{field-heating-cop-function-of-water-flow-fraction-curve-name}
+
+This alpha field specifies the name of a \textbf{quadratic} or \textbf{cubic} performance curve object (ref: Performance Curves) that defines the variation in DX coil heating COP as a function of the ratio of actual water flow rate through the condenser to the rated condenser water flow rate.. The output of this curve is multiplied by the rated COP and the output from the two other heating COP modifier curves (function of temperature and function of air flow fraction) to give the DX coil heating COP at the specific inlet fluid temperatures and flow rates at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated condenser water flow rate (water flow fraction of 1.0). If this field is left blank, the heating COP remains constant (curve value assumed to be 1.0 for all water flow rates).
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-8}
+
+This alpha field defines the name of a \textbf{quadratic} or \textbf{cubic} performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
+
+\begin{lstlisting}
+       PLF = 0.85 + 0.15(PLR)
+\end{lstlisting}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{lstlisting}
+       PLF = 1.0 + 0.0(PLR)
+\end{lstlisting}
+
+Following is an example input for the \lstinline!Coil:WaterHeating:AirToWaterHeatPump:Pumped! object:
+
+\begin{lstlisting}
+
+Coil:WaterHeating:AirToWaterHeatPump:Pumped,
+  Zone4HPWHDXCoil,           !- Coil Name
+  4000.0,                    !- Heating Capacity {W}
+  3.2,                       !- Rated COP {W/W}
+  0.6956,                    !- Rated SHR (gross)
+  19.7,                      !- Rated Evaporator Inlet Air Dry-Bulb Temperature {C}
+  13.5,                      !- Rated Evaporator Inlet Air Wet-Bulb Temperature {C}
+  57.5,                      !- Rated Condenser Inlet Water Temperature {C}
+  autocalculate,             !- Rated Evaporator Air Volumetric Flow Rate {m3/s}
+  autocalculate,             !- Rated Condenser Water Volumetric Flow Rate {m3/s}
+  No,                        !- Evaporator Fan Power Included in Rated COP
+  No,                        !- Condenser Pump Power Included in Rated COP
+  No,                        !- Condenser Pump Heat Included in Rated Heating Capacity and Rated COP
+  150.0,                     !- Condenser Water Pump Power {W}
+  0.1,                       !- Fraction of Condenser Pump Heat to Water
+  Zone4AirOutletNode,        !- Evaporator Air Inlet Node Name
+  Zone4DXCoilAirOutletNode,  !- Evaporator Air Outlet Node Name
+  Zone4WaterInletNode,       !- Condenser Water Inlet Node Name
+  Zone4WaterOutletNode,      !- Condenser Water Outlet Node Name
+  100.0,                     !- Crankcase Heater Capacity {W}
+  5.0,                       !- Maximum Ambient Temperature for Crankcase Heater Operation {C}
+  wet-bulb temperature,      !- Evaporator Air Temperature Type for Curve Objects
+  HPWHHeatingCapFTemp,       !- Heating Capacity Modifier Curve Name (function of temperature)
+  ,                          !- Heating Capacity Modifier Curve Name (function of air flow fraction)
+  ,                          !- Heating Capacity Modifier Curve Name (function of water flow fraction)
+  HPWHHeatingCOPFTemp,       !- Heating COP Modifier Curve Name (function of temperature)
+  ,                          !- Heating COP Modifier Curve Name (function of air flow fraction)
+  ,                          !- Heating COP Modifier Curve Name (function of water flow fraction)
+  HPWHPLFFPLR;               !- Part Load Fraction Correlation Name (function of part load ratio)
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-23}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Cooling Coil Runtime Fraction {[]}
+\item
+  HVAC,Average,DX Cooling Coil Crankcase Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum, Cooling Coil Crankcase Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Total Water Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Total Water Heating Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Water Heating Electric Power{[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Water Heating Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Cooling Coil Total Cooling Rate {[}W{]}}\label{cooling-coil-total-cooling-rate-w-6}
+
+This output field is the average total (sensible and latent) cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Total Cooling Energy {[}J{]}}\label{cooling-coil-total-cooling-energy-j-6}
+
+This output field is the total (sensible plus latent) cooling output of the DX coil in Joules for the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Sensible Cooling Rate {[}W{]}}\label{cooling-coil-sensible-cooling-rate-w-6}
+
+This output field is the average moist air sensible cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Sensible Cooling Energy {[}J{]}}\label{cooling-coil-sensible-cooling-energy-j-6}
+
+This output field is the moist air sensible cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{DX Coil Latent Cooling Rate {[}W{]}}\label{dx-coil-latent-cooling-rate-w}
+
+This output field is the average latent cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Latent Cooling Energy {[}J{]}}\label{cooling-coil-latent-cooling-energy-j-4}
+
+This output field is the latent cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{\texorpdfstring{Cooling Coil Runtime Fraction {[]}}{Cooling Coil Runtime Fraction }}\label{cooling-coil-runtime-fraction-4}
+
+This output field is the average runtime fraction of the DX coil compressor for the timestep being reported. This also represents the runtime fraction of the condenser water pump.
+
+\paragraph{Cooling Coil Crankcase Heater Electric Power{[}W{]}}\label{cooling-coil-crankcase-heater-electric-powerw-1}
+
+This output field is the average electricity consumption rate of the DX coil compressor's crankcase heater in Watts for the timestep being reported. The crankcase heater operates only when the compressor is off and the air surrounding the compressor is below the Maximum Ambient Temperature for Crankcase Heater Operation, otherwise this output variable is set equal to 0.
+
+\paragraph{Cooling Coil Crankcase Heater Electric Energy {[}J{]}}\label{cooling-coil-crankcase-heater-electric-energy-j-2}
+
+This output field is the total electricity consumption of the DX coil compressor's crankcase heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
+
+\paragraph{Cooling Coil Total Water Heating Rate {[}W{]}}\label{cooling-coil-total-water-heating-rate-w}
+
+This output field is the average water heating rate output of the DX coil (condenser coil plus condenser water pump) in Watts for the timestep being reported. This is determined using the inlet and outlet water temperatures and the water mass flow rate through the condenser coil.
+
+\paragraph{Cooling Coil Total Water Heating Energy {[}J{]}}\label{cooling-coil-total-water-heating-energy-j}
+
+This output field is the total water heating output of the DX coil (condenser coil plus condenser water pump) in Joules for the timestep being reported. This is determined using the inlet and outlet water temperatures and the water mass flow rate through the condenser coil.
+
+\paragraph{Cooling Coil Water Heating Electric Power{[}W{]}}\label{cooling-coil-water-heating-electric-powerw}
+
+This output field is the average electricity consumption rate of the DX coil compressor and condenser pump in Watts for the timestep being reported.
+
+\paragraph{Cooling Coil Water Heating Electric Energy {[}J{]}}\label{cooling-coil-water-heating-electric-energy-j}
+
+This output field is the electricity consumption of the DX coil compressor and condenser pump in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
+
+\subsection{Coil:WaterHeating:AirToWaterHeatPump:Wrapped}\label{coilwaterheatingairtowaterheatpumpwrapped}
+
+EnergyPlus can model a heat pump water heater (HPWH) consisting of a water heater tank (e.g., \lstinline!WaterHeater:Stratified!), a direct expansion (DX) coil (i.e., an air-to-water DX compression system which includes a water heating coil, air coil, compressor, and water pump), and a fan to provide air flow across the air coil associated with the DX compression system. These objects work together to model a system which heats water using zone air, outdoor air, or a combination of zone and outdoor air as the primary heat source.
+
+The \lstinline!WaterHeater:HeatPump:WrappedCondenser! compound object, water heater tank object (e.g., \lstinline!WaterHeater:Mixed!), and fan object (e.g., \lstinline!Fan:OnOff!) are defined elsewhere in this reference document. \lstinline!Coil:WaterHeating:AirToWaterHeatPump:Wrapped! object described here models an air-to-water DX compression system to determine its air-side and water-side performance. This DX coil object calculates the air-side sensible and latent cooling capacity at the specific operating conditions for each simulation timestep, as well as the condenser's water-side temperature difference at a given condenser water flow rate.
+
+The heat pump water heater DX coil model performs the following major functions:
+
+\begin{itemize}
+\item
+  calculates the electric consumption of the DX compressor
+\item
+  calculates the amount of heat delivered to the water tank
+\item
+  calculates the electric consumption of the compressor's crankcase heater
+\item
+  calculates the air-side performance of the DX coil
+\end{itemize}
+
+\subsubsection{Inputs}\label{inputs-28}
+
+\paragraph{Field: Name}\label{field-name-27-000}
+
+This alpha field defines a unique user-assigned name for an instance of a heat pump water heater DX coil. Any reference to this coil by another object (e.g., \lstinline!WaterHeater:HeatPump:WrappedCondenser!) will use this name.
+
+\paragraph{Field: Rated Heating Capacity}\label{field-rated-heating-capacity-1}
+
+This numeric field defines the DX coil heating capacity in Watts at the rated evaporator inlet air temperatures, rated condenser inlet water temperature, rated evaporator air flow rate, and rated condenser water flow rate specified below. Values must be greater than 0. This value represents water heating capacity, and it may or may not include the impact of condenser pump heat (see field Condenser Pump Heat Included in Rated Heating Capacity below).
+
+\paragraph{Field: Rated COP}\label{field-rated-cop-1}
+
+This numeric field defines the DX coil's water heating coefficient of performance (COP = water heating capacity in watts divided by electrical power input in watts) at rated conditions (rated inlet temperatures and flow rates specified below). This input not only determines the electric energy use of the heat pump DX coil, but also the amount of total air cooling provided by the evaporator. The rated COP includes compressor power, and may or may not include condenser pump power or evaporator fan power (see field Evaporator Fan Power Included in Rated COP and field Condenser Pump Power Included in Rated COP). Values must be greater than 0. If this field is left blank, the default value is 3.2.
+
+\paragraph{Field: Rated Sensible Heat Ratio}\label{field-rated-sensible-heat-ratio-2}
+
+This numeric field defines the air-side sensible heat ratio (SHR = sensible cooling capacity divided by total cooling capacity) of the DX coil at rated conditions (rated inlet temperatures and flow rates specified below). This value should not include the effect of evaporator fan heat. Values must be greater than or equal to 0.5, and less than or equal to 1.0. The default value is 0.85.
+
+\paragraph{Field: Rated Evaporator Inlet Air Dry-Bulb Temperature}\label{field-rated-evaporator-inlet-air-dry-bulb-temperature-1}
+
+This numeric field defines the evaporator inlet air dry-bulb temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 5 °C. If this field is left blank, the default value is 19.7 °C.
+
+\paragraph{Field: Rated Evaporator Inlet Air Wet-Bulb Temperature}\label{field-rated-evaporator-inlet-air-wet-bulb-temperature-1}
+
+This numeric field defines the evaporator inlet air wet-bulb temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 5 °C. If this field is left blank, the default value is 13.5 °C.
+
+\paragraph{Field: Rated Condenser Water Temperature}\label{field-rated-condenser-water-temperature}
+
+This numeric field defines the condenser inlet water temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 25 °C. If this field is left blank, the default value is 57.5 °C.
+
+\paragraph{Field: Rated Evaporator Air Flow Rate}\label{field-rated-evaporator-air-flow-rate-1}
+
+This numeric field defines the evaporator air volume flow rate in cubic meters per second at rated conditions. Values must be greater than 0. If this field is left blank or autocalculated (field value = \textbf{autocalculate}), the default value is 5.035E-5 m\(^{3}\)/s/W (31.25 cfm/MBH) multiplied by the Rated Heating Capacity specified above. When autocalculating the rated evaporator air volumetric flow rate, a zone sizing object is not required.
+
+\paragraph{Field: Evaporator Fan Power Included in Rated COP}\label{field-evaporator-fan-power-included-in-rated-cop-1}
+
+This choice field specifies if evaporator fan power is included in the rated COP defined above. This input impacts the calculation of compressor electric power and total air cooling provided by the evaporator for each simulation timestep. If Yes is selected, the evaporator fan power is subtracted from the total electric heating power when calculating total evaporator cooling capacity. If No is selected, it is assumed that the total heating power does not include evaporator fan power. If this field is left blank, the default is Yes. See the Engineering Reference section for \lstinline!Coil:WaterHeating:AirToWaterHeatPump:\*! for further details.
+
+\paragraph{Field: Evaporator Air Inlet Node Name}\label{field-evaporator-air-inlet-node-name-2}
+
+This alpha field defines the name of the air node from which the evaporator coil draws its inlet air.
+
+\paragraph{Field: Evaporator Air Outlet Node Name}\label{field-evaporator-air-outlet-node-name-1}
+
+This alpha field defines the name of the air node to which the evaporator coil sends its outlet air.
+
+\paragraph{Field: Crankcase Heater Capacity}\label{field-crankcase-heater-capacity-8}
+
+This numeric field defines the compressor's crankcase heater capacity in Watts. The crankcase heater only operates when the compressor is off and the air surrounding the compressor is below the Maximum Ambient Temperature for Crankcase Heater Operation specified below.
+
+\paragraph{Field: Maximum Ambient Temperature for Crankcase Heater Operation}\label{field-maximum-ambient-temperature-for-crankcase-heater-operation-1}
+
+This numeric field defines the maximum ambient temperature for crankcase heater operation in degree Celsius. The crankcase heater only operates when the air surrounding the compressor is below this maximum temperature value and the compressor is off. The ambient temperature surrounding the compressor is set by the Heat Pump:Water Heater parent object (field Compressor Location).
+
+\paragraph{Field: Evaporator Air Temperature Type for Curve Objects}\label{field-evaporator-air-temperature-type-for-curve-objects-1}
+
+This choice field specifies the air temperature type used for the heating capacity and COP modifier curve objects below. The valid selections are Dry-bulb Temperature and Wet-bulb Temperature. If dry-bulb temperature is selected, the inlet air dry-bulb temperature entering the heat pump DX coil and fan section is used to evaluate the curve objects. If wet-bulb temperature is selected, the inlet air wet-bulb temperature entering the heat pump DX coil and fan section is used to evaluate the curve objects. If this field is left blank and the following curve names are defined, the default value is wet-bulb temperature. If the following curve names are not defined, this field is not used.
+
+\paragraph{Field: Heating Capacity Function of Temperature Curve Name}\label{field-heating-capacity-function-of-temperature-curve-name-2}
+
+This alpha field specifies the name of a \textbf{biquadratic} or \textbf{cubic} performance curve object (ref: Performance Curves) that defines the variation in DX coil heating capacity as a function of inlet fluid (air and water) temperatures. The biquadratic curve uses evaporator inlet air temperature (dry-bulb or wet-bulb temperature based on the field Evaporator Air Temperature Type for Curve Objects defined above) and condenser inlet water temperature as the independent variables. The cubic curve uses evaporator inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The output of this curve is multiplied by the rated heating capacity to give the heating capacity at specific operating conditions (i.e., at temperatures different from the rating point temperatures). The curve should be normalized to have the value of 1.0 at the rating point temperatures. If this field is left blank, the heating capacity remains constant (curve value assumed to be 1.0 for all conditions).
+
+\paragraph{Field: Heating Capacity Function of Air Flow Fraction Curve Name}\label{field-heating-capacity-function-of-air-flow-fraction-curve-name-1}
+
+This alpha field specifies the name of a \textbf{quadratic} or \textbf{cubic} performance curve object (ref: Performance Curves) that defines the variation in DX coil heating capacity as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate. The output of this curve is multiplied by the rated heating capacity and the heating capacity modifier curve (function of temperature) to give the DX coil heating capacity at the specific inlet fluid temperatures and air flow rate at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated evaporator air flow rate (air flow fraction of 1.0). If this field is left blank, the heating capacity remains constant (curve value assumed to be 1.0 for all air flow rates).
+
+\paragraph{Field: Heating COP Function of Temperature Curve Name}\label{field-heating-cop-function-of-temperature-curve-name-1}
+
+This alpha field specifies the name of a \textbf{biquadratic} or \textbf{cubic} performance curve object (ref: Performance Curves) that defines the variation in DX coil heating COP as a function of inlet fluid (air and water) temperatures. The biquadratic curve uses evaporator inlet air temperature (dry-bulb or wet-bulb temperature based on the field Evaporator Air Temperature Type for Curve Objects defined above) and condenser inlet water temperature as the independent variables. The cubic curve uses evaporator inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The output of this curve is multiplied by the rated COP to give the heating COP at specific operating conditions (i.e., at temperatures different from the rating point temperatures). The curve should be normalized to have the value of 1.0 at the rating point temperatures. If this field is left blank, the COP remains constant (curve value assumed to be 1.0 for all conditions).
+
+\paragraph{Field: Heating COP Function of Air Flow Fraction Curve Name}\label{field-heating-cop-function-of-air-flow-fraction-curve-name-1}
+
+This alpha field specifies the name of a \textbf{quadratic} or \textbf{cubic} performance curve object (ref: Performance Curves) that defines the variation in DX coil heating COP as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate. The output of this curve is multiplied by the rated COP and the heating COP modifier curve (function of temperature) to give the heating COP at the specific inlet fluid temperatures and air flow rate at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated evaporator air flow rate (air flow fraction of 1.0). If this field is left blank, the heating COP remains constant (curve value assumed to be 1.0 for all air flow rates).
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-9}
+
+This alpha field defines the name of a \textbf{quadratic} or \textbf{cubic} performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
+
+A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
+
+\begin{lstlisting}
+       PLF = 0.85 + 0.15(PLR)
+\end{lstlisting}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{lstlisting}
+       PLF = 1.0 + 0.0(PLR)
+\end{lstlisting}
+
+Following is an example input for the \lstinline!Coil:WaterHeating:AirToWaterHeatPump:Wrapped! object:
+
+\begin{lstlisting}
+
+Coil:WaterHeating:AirToWaterHeatPump:Wrapped,
+  HPWH Coil,               !- Name
+  2349.6,                  !- Rated Heating Capacity {W}
+  2.4,                     !- Rated COP {W/W}
+  0.981,                   !- Rated Sensible Heat Ratio
+  19.72,                   !- Rated Evaporator Inlet Air Dry-Bulb Temperature {C}
+  13.5,                    !- Rated Evaporator Inlet Air Wet-Bulb Temperature {C}
+  48.89,                   !- Rated Condenser Water Temperature {C}
+  0.189,                   !- Rated Evaporator Air Flow Rate {m3/s}
+  Yes,                     !- Evaporator Fan Power Included in Rated COP
+  HPWH Air Inlet,          !- Evaporator Air Inlet Node Name
+  HPWH Coil Outlet Fan Inlet,  !- Evaporator Air Outlet Node Name
+  0,                       !- Crankcase Heater Capacity {W}
+  10,                      !- Maximum Ambient Temperature for Crankcase Heater Operation {C}
+  WetBulbTemperature,      !- Evaporator Air Temperature Type for Curve Objects
+  HPWH-Htg-Cap-fT,         !- Heating Capacity Function of Temperature Curve Name
+  ,                        !- Heating Capacity Function of Air Flow Fraction Curve Name
+  HPWH-Htg-COP-fT,         !- Heating COP Function of Temperature Curve Name
+  ,                        !- Heating COP Function of Air Flow Fraction Curve Name
+  HPWH-COP-fPLR;           !- Part Load Fraction Correlation Curve Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-24}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Cooling Coil Runtime Fraction {[]}
+\item
+  HVAC,Average,DX Cooling Coil Crankcase Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum, Cooling Coil Crankcase Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Total Water Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Total Water Heating Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Water Heating Electric Power{[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Water Heating Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Cooling Coil Total Cooling Rate {[}W{]}}\label{cooling-coil-total-cooling-rate-w-7}
+
+This output field is the average total (sensible and latent) cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Total Cooling Energy {[}J{]}}\label{cooling-coil-total-cooling-energy-j-7}
+
+This output field is the total (sensible plus latent) cooling output of the DX coil in Joules for the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Sensible Cooling Rate {[}W{]}}\label{cooling-coil-sensible-cooling-rate-w-7}
+
+This output field is the average moist air sensible cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Sensible Cooling Energy {[}J{]}}\label{cooling-coil-sensible-cooling-energy-j-7}
+
+This output field is the moist air sensible cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{DX Coil Latent Cooling Rate {[}W{]}}\label{dx-coil-latent-cooling-rate-w-1}
+
+This output field is the average latent cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{Cooling Coil Latent Cooling Energy {[}J{]}}\label{cooling-coil-latent-cooling-energy-j-5}
+
+This output field is the latent cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
+
+\paragraph{\texorpdfstring{Cooling Coil Runtime Fraction {[]}}{Cooling Coil Runtime Fraction }}\label{cooling-coil-runtime-fraction-5}
+
+This output field is the average runtime fraction of the DX coil compressor for the timestep being reported. This also represents the runtime fraction of the condenser water pump.
+
+\paragraph{Cooling Coil Crankcase Heater Electric Power{[}W{]}}\label{cooling-coil-crankcase-heater-electric-powerw-2}
+
+This output field is the average electricity consumption rate of the DX coil compressor's crankcase heater in Watts for the timestep being reported. The crankcase heater operates only when the compressor is off and the air surrounding the compressor is below the Maximum Ambient Temperature for Crankcase Heater Operation, otherwise this output variable is set equal to 0.
+
+\paragraph{Cooling Coil Crankcase Heater Electric Energy {[}J{]}}\label{cooling-coil-crankcase-heater-electric-energy-j-3}
+
+This output field is the total electricity consumption of the DX coil compressor's crankcase heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
+
+\paragraph{Cooling Coil Total Water Heating Rate {[}W{]}}\label{cooling-coil-total-water-heating-rate-w-1}
+
+This output field is the average water heating rate output of the DX coil (condenser coil plus condenser water pump) in Watts for the timestep being reported.
+
+\paragraph{Cooling Coil Total Water Heating Energy {[}J{]}}\label{cooling-coil-total-water-heating-energy-j-1}
+
+This output field is the total water heating output of the DX coil (condenser coil plus condenser water pump) in Joules for the timestep being reported.
+
+\paragraph{Cooling Coil Water Heating Electric Power{[}W{]}}\label{cooling-coil-water-heating-electric-powerw-1}
+
+This output field is the average electricity consumption rate of the DX coil compressor in Watts for the timestep being reported.
+
+\paragraph{Cooling Coil Water Heating Electric Energy {[}J{]}}\label{cooling-coil-water-heating-electric-energy-j-1}
+
+This output field is the electricity consumption of the DX coil compressor in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
+
+\subsection{Coil:Cooling:WaterToAirHeatPump:ParameterEstimation}\label{coilcoolingwatertoairheatpumpparameterestimation}
+
+The \textbf{Coil:Cooling:WaterToAirHeatPump:ParameterEstimation} coil is a deterministic model that requires parameters to describe the operating conditions of the heat pump's components. The parameters are generated from the manufacturer catalog data using multi-variable optimization method. In addition, the cooling coil model can be used for 3 type of compressors: \textbf{reciprocating}, \textbf{rotary} and \textbf{scroll}. Descriptions and strength of each respective model is available in the following references:
+
+Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from \href{http://www.hvac.okstate.edu}{http://www.hvac.okstate.edu/})
+
+Tang,C. C. 2005. Modeling Packaged Heat Pumps in Quasi-Steady State Energy Simulation Program. M.S. Thesis. Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from \href{http://www.hvac.okstate.edu}{http://www.hvac.okstate.edu/})
+
+\subsubsection{Inputs}\label{inputs-29}
+
+\paragraph{Field: Name}\label{field-name-28}
+
+This alpha field contains the identifying name for the coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
+
+\paragraph{Field: Compressor Type}\label{field-compressor-type}
+
+Type of compressor mode used for the heat pump. Choices available are reciprocating, rotary and scroll compressor. Note that the parameters vary for different compressor.
+
+\paragraph{Field: Refrigerant Type}\label{field-refrigerant-type}
+
+This alpha field contains the type of refrigerant used by the heat pump.
+
+\paragraph{Field: Design Source Side Flow Rate}\label{field-design-source-side-flow-rate}
+
+This numeric field defines the water flow rate though the coil in m3/sec
+
+\paragraph{Field: Nominal Cooling Coil Capacity}\label{field-nominal-cooling-coil-capacity}
+
+This numeric field defines the nominal cooling capacity for the WatertoAirHP cooling coil in Watts.
+
+\paragraph{Field: Nominal Time for Condensate Removal to Begin}\label{field-nominal-time-for-condensate-removal-to-begin-3}
+
+This numeric field defines the nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero.
+
+\paragraph{Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity}\label{field-ratio-of-initial-moisture-evaporation-rate-and-steady-state-latent-capacity-3}
+
+This numeric field defines ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero.
+
+\paragraph{Field: High Pressure Cutoff}\label{field-high-pressure-cutoff}
+
+This numeric field defines the compressor s maximum allowable pressure in Pascal (N/m2)
+
+\paragraph{Field: Low Pressure Cutoff}\label{field-low-pressure-cutoff}
+
+This numeric field defines the compressor s minimum allowable pressure in Pascal (N/m2)
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-5-000}
+
+This alpha field contains the cooling coil source side inlet node name.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-5-000}
+
+This alpha field contains the cooling coil source side outlet node name.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-16}
+
+This alpha field contains the cooling coil air inlet node name.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-16}
+
+This alpha field contains the cooling coil air outlet node name.
+
+\paragraph{Cooling Coil Parameters}\label{cooling-coil-parameters}
+
+Depending on the type of compressor and the source side fluid specified, the type of parameters and values also differs. An Excel Spreadsheet is developed to estimate the parameters based on the manufacturer data. The general parameters are listed first followed by specific parameters required by the respective compressor model. Lastly, parameters are listed based on the type of source side fluid used.
+
+\paragraph{Field: Load Side Total Heat Transfer Coefficient}\label{field-load-side-total-heat-transfer-coefficient}
+
+This numeric field defines the estimated parameter \textbf{load side total heat transfer coefficient} in W/K. This field was previously known as Parameter 1.
+
+\paragraph{Field: Load Side Outside Surface Heat Transfer Coefficient}\label{field-load-side-outside-surface-heat-transfer-coefficient}
+
+This numeric field defines the estimated parameter \textbf{load side outside surface heat transfer coefficient} in W/K. This field was previously known as Parameter 2.
+
+\paragraph{Field: Superheat Temperature at the Evaporator Outlet}\label{field-superheat-temperature-at-the-evaporator-outlet}
+
+This numeric field defines the estimated parameter \textbf{superheat temperature} at the evaporator outlet in ËšC. This field was previously known as Parameter 3.
+
+\paragraph{Field: Compressor Power Losses}\label{field-compressor-power-losses}
+
+This numeric field defines the estimated parameter \textbf{compressor power losses}, which accounts for the loss of work due to mechanical and electrical losses in the compressor in Watts. This field was previously known as Parameter 4.
+
+\paragraph{Field: Compressor Efficiency}\label{field-compressor-efficiency}
+
+This numeric field defines the estimated parameter of the \textbf{compressor s efficiency}. The compressor efficiency is formulated as the equation below:
+
+\begin{equation}
+\eta  = \frac{{{{\dot W}_{Theoritical}}}}{{{{\dot W}_{CompInput}} - {{\dot W}_{Loss}}}}
+\end{equation}
+
+This field was previously know as Parameter 5.
+
+\paragraph{Field: Compressor Piston Displacement}\label{field-compressor-piston-displacement}
+
+This numeric field defines the estimated parameter \textbf{piston displacement of the compressor} in m3/s. This field was part of what was previously known as Parameter 6. It should be used when the Compressor type is either Reciprocating and Rotary. The field should be left blank when Compressor type is Scroll.
+
+\paragraph{Field: Compressor Suction/Discharge Pressure Drop}\label{field-compressor-suctiondischarge-pressure-drop}
+
+This numeric field defines the estimated parameter \textbf{pressure drop} at the compressor suction and discharge in Pascals (N/m2). This field was part of what was previously known as Parameter 7. It should be used when the Compressor type is either Reciprocating and Rotary. The field should be left blank when Compressor type is Scroll.
+
+\paragraph{Field: Compressor Clearance Factor}\label{field-compressor-clearance-factor}
+
+This numeric field defines the estimated parameter \textbf{clearance factor of the compressor}. This parameter is dimensionless. This field was part of what was previously known as Parameter 8. It should only be used when the Compressor type is Reciprocating. The field should be left blank when Compressor type is Scroll or Rotary.
+
+\paragraph{Field: Refrigerant Volume Flow Rate}\label{field-refrigerant-volume-flow-rate}
+
+This numeric field defines the \textbf{refrigerant volume flow rate} at the beginning of the compression {[}m3/s{]}. This field was part of what was previously known as Parameter 6. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
+
+\paragraph{Field: Volume Ratio}\label{field-volume-ratio}
+
+This numeric field defines the built-in-\textbf{volume ratio}. This field was part of what was previously known as Parameter 7. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
+
+\paragraph{Field: Leak Rate Coefficient}\label{field-leak-rate-coefficient}
+
+This numeric field defines the \textbf{leak rate coefficient} for the relationship between pressure ratio and leakage rate. This field was part of what was previously known as Parameter 8. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
+
+\paragraph{Field: Source Side Heat Transfer Coefficient}\label{field-source-side-heat-transfer-coefficient}
+
+This numeric field defines the estimated parameter \textbf{source side heat transfer coefficient} in W/K. This field was part of what was previously known as Parameter 9. It should only be used when the Source Side Fluid Name is Water.
+
+\paragraph{Field: Source Side Heat Transfer Resistance1}\label{field-source-side-heat-transfer-resistance1}
+
+This numeric field defines the estimated parameter \textbf{source side heat transfer resistance} 1. Unit is dimensionless. This field was part of what was previously known as Parameter 9. It should only be used when the Source Side Fluid Name is an antifreeze.
+
+\paragraph{Field: Source Side Heat Transfer Resistance2}\label{field-source-side-heat-transfer-resistance2}
+
+This numeric field defines the estimated parameter \textbf{source side heat transfer resistance} 2. Unit is W/K. This field was previously known as Parameter 10. It should only be used when the Source Side Fluid Name is an antifreeze.
+
+Following is an example for COIL:WaterToAirHP:ParameterEstimation:Cooling coil input
+
+\begin{lstlisting}
+
+Coil:Cooling:WaterToAirHeatPump:ParameterEstimation,
+  Heat Pump Cooling Mode AHU1,   !- Name
+  Scroll,                                   !- Compressor Type
+  R22,                                         !- Refrigerant Type
+  0.0015,                                   !- Design Source Side Flow Rate {m3/s}
+  38000,                                     !- Nominal Cooling Coil Capacity {W}
+  0,                                             !- Nominal Time for Condensate Removal to Begin {s}
+  0,         !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
+  3000000,                                 !- High Pressure Cutoff {Pa}
+  0,                                             !- Low Pressure Cutoff {Pa}
+  AHU1 Water to Air Heat Pump Source Side1 Inlet Node,   !- Water Inlet Node Name
+  AHU1 Water to Air Heat Pump Source Side1 Outlet Node,   !- Water Outlet Node Name
+  AHU 1 Supply Fan Outlet, !- Air Inlet Node Name
+  Cooling Coil Air Outlet Node AHU1,   !- Air Outlet Node Name
+  3.78019E+03,                         !- Load Side Total Heat Transfer Coefficient {W/K}
+  3.41103E+03,                         !- Load Side Outside Surface Heat Transfer Coefficient {W/K}
+  1.57066E+00,                         !- Superheat Temperature at the Evaporator Outlet {C}
+  2.23529E+03,                         !- Compressor Power Losses {W}
+  1.34624E+00,                         !- Compressor Efficiency
+  ,                                               !- Compressor Piston Displacement {m3/s}
+  ,                                               !- Compressor Suction/Discharge Pressure Drop {Pa}
+  ,                                               !- Compressor Clearance Factor {dimensionless}
+  9.74424E-03,                         !- Refrigerant Volume Flow Rate {m3/s}
+  2.30803E+00,                         !- Volume Ratio {dimensionless}
+  2.06530E-02,                         !-Leak Rate Coefficient
+  1.92757E+03,                         !- Source Side Heat Transfer Coefficient {W/K}
+  ,                                               !- Source Side Heat Transfer Resistance1 {dimensionless}
+  ;                                               !- Source Side Heat Transfer Resistance2 {W/K}
+\end{lstlisting}
+
+\subsection{Coil:Cooling:WaterToAirHeatPump:EquationFit}\label{coilcoolingwatertoairheatpumpequationfit}
+
+The Coil:Cooling:WaterToAirHeatPump:EquationFit is a simple curve-fit model that requires coefficients generated from the heat pump catalog data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. The performance of the heat pump is modeled using curves fitted from the catalog data. Description of the equation-fit model is available in the following reference:
+
+Tang,C. C. 2005. Modeling Packaged Heat Pumps in Quasi-Steady State Energy Simulation Program. M.S. Thesis. Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from \href{http://www.hvac.okstate.edu}{http://www.hvac.okstate.edu/})
+
+\subsubsection{Inputs}\label{inputs-30}
+
+\paragraph{Field: Name}\label{field-name-29}
+
+This alpha field contains the identifying name for the coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-6-000}
+
+This alpha field contains the cooling coil source side inlet node name.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-6-000}
+
+This alpha field contains the cooling coil source side outlet node name.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-17}
+
+This alpha field contains the cooling coil air inlet node name.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-17}
+
+This alpha field contains the cooling coil air outlet node name.
+
+\paragraph{Field: Rated Air Flow Rate}\label{field-rated-air-flow-rate-5}
+
+This numeric field contains the rated volumetric air flow rate on the load side of the heat pump in m3/s. This field is autosizable.
+
+\paragraph{Field: Rated Water Flow Rate}\label{field-rated-water-flow-rate}
+
+This numeric field contains the rated volumetric water flow rate on the source side of the heat pump in m3/s. This field is autosizable.
+
+\paragraph{Field: Gross Rated Total Cooling Capacity}\label{field-gross-rated-total-cooling-capacity-3}
+
+This numeric field contains the gross rated total cooling capacity of the heat pump in W. This field is autosizable.The gross rated total cooling capacity should be within 20\% of the gross rated heating capacity, otherwise a warning message is issued. The gross rated total cooling capacity shouldnot account for the effect of supply air fan heat.
+
+\paragraph{Field: Gross Rated Sensible Cooling Capacity}\label{field-gross-rated-sensible-cooling-capacity}
+
+This numeric field contains the gross rated sensible capacity of the heat pump in W. This field is autosizable. The gross rated sensible cooling capacity shouldnot account for the effect of supply air fan heat.
+
+\paragraph{Field: Rated Cooling Coefficient of Performance}\label{field-rated-cooling-coefficient-of-performance}
+
+This numeric field contains the rated cooling coefficient of performance of the heat pump.
+
+\paragraph{Field: Total Cooling Capacity Coefficient 1 to 5}\label{field-total-cooling-capacity-coefficient-1-to-5}
+
+These numeric fields contain the first to fifth coefficient for the heat pump total cooling capacity.
+
+\paragraph{Field: Sensible Cooling Capacity Coefficient 1 to 6}\label{field-sensible-cooling-capacity-coefficient-1-to-6}
+
+These numeric fields contain the first to sixth coefficient for the heat pump sensible cooling capacity.
+
+\paragraph{Field: Cooling Power Consumption Coefficient 1 to 5}\label{field-cooling-power-consumption-coefficient-1-to-5}
+
+These numeric fields contain the first to fifth coefficient for the heat pump power consumption.
+
+\paragraph{Field: Nominal Time for Condensate Removal to Begin}\label{field-nominal-time-for-condensate-removal-to-begin-4}
+
+This numeric field defines the nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero.
+
+\paragraph{Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity}\label{field-ratio-of-initial-moisture-evaporation-rate-and-steady-state-latent-capacity-4}
+
+This numeric field defines ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero.
+
+Following is an example of the input for Coil:WaterToAirHP:EquationFit:Cooling coil
+
+\begin{lstlisting}
+
+Coil:Cooling:WaterToAirHeatPump:EquationFit,
+  Heat Pump Cooling Mode,!- Name of Coil
+  Water to Air Heat Pump Source Side1 Inlet Node,!- Coil Water Inlet Node Name
+  Water to Air Heat Pump Source Side1 Outlet Node,!- Coil Water Outlet Node Name
+  Cooling Coil Air Inlet Node,!- Coil Air Inlet Node Name
+  Heating Coil Air Inlet Node,!- Coil Air Outlet Node Name
+  4.6015E-01,!- Rated Air Volumetric Flow Rate
+  2.8391E-04,!- Rated Water Volumetric Flow Rate
+  23125.59,!- Gross Rated Total Cooling Capacity
+  16267.05,!- Gross Rated Sensible Cooling Capacity
+  4.7,!- Rated Cooling Coefficient of Performance
+  -0.68126221,!- Total Cooling Capacity Coefficient 1
+  1.99529297,!- Total Cooling Capacity Coefficient 2
+  -0.93611888,!- Total Cooling Capacity Coefficient 3
+  0.02081177,!- Total Cooling Capacity Coefficient 4
+  0.008438868,!- Total Cooling Capacity Coefficient 5
+  2.24209455,!- Sensible Cooling Capacity Coefficient 1
+  7.28913391,!- Sensible Cooling Capacity Coefficient 2
+  -9.06079896,!- Sensible Cooling Capacity Coefficient 3
+  -0.36729404,!- Sensible Cooling Capacity Coefficient 4
+  0.218826161,!- Sensible Cooling Capacity Coefficient 5
+  0.00901534,!- Sensible Cooling Capacity Coefficient 6
+  -3.20456384,!- Cooling Power Consumption Coefficient 1
+  0.47656454,!- Cooling Power Consumption Coefficient 2
+  3.16734236,!- Cooling Power Consumption Coefficient 3
+  0.10244637,!- Cooling Power Consumption Coefficient 4
+  -0.038132556,!- Cooling Power Consumption Coefficient 5
+  0,!- Nominal Time for Condensate Removal to Begin
+  0;!- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-25}
+
+Coil:Cooling:WaterToAirHeatPump:ParameterEstimation and Coil:Cooling:WaterToAirHeatPump:EquationFit have the same output variables listed as follows;
+
+\begin{itemize}
+\item
+  HVAC, Average, Cooling Coil Electric Power {[}W{]}
+\item
+  HVAC, Average, Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC, Average, Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC, Average, Cooling Coil Source Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Average, Cooling Coil Part Load Ratio {[]}
+\item
+  HVAC, Average, Cooling Coil Runtime Fraction {[]}
+\item
+  HVAC, Average, Cooling Coil Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Cooling Coil Air Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Cooling Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC, Average, Cooling Coil Air Outlet Temperature {[}C{]}
+\item
+  HVAC, Average, Cooling Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC, Average, Cooling Coil Source Side Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Cooling Coil Source Side Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Cooling Coil Source Side Outlet Temperature {[}C{]}
+\item
+  HVAC, Sum, Cooling Coil Electric Energy {[}J{]}
+\item
+  HVAC, Sum, Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC, Sum, Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC, Sum, Cooling Coil Latent Cooling Energy {[}J{]}
+\item
+  HVAC, Average, Cooling Coil Latent Cooling Rate {[}W{]}
+\item
+  HVAC, Sum, Cooling Coil Source Side Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Cooling Coil Electric Power {[}W{]}}\label{cooling-coil-electric-power-w-2}
+
+This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Total Cooling Rate {[}W{]}}\label{cooling-coil-total-cooling-rate-w-8}
+
+The output variable is the average total cooling load provide by the heat pump which includes the sensible and latent load in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Sensible Cooling Rate {[}W{]}}\label{cooling-coil-sensible-cooling-rate-w-8}
+
+The output variable is the average sensible cooling load provide by the heat pump in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Heat Transfer Rate {[}W{]}}\label{cooling-coil-source-side-heat-transfer-rate-w-1}
+
+The output variable is the average heat rejected to the water at the heat pump condenser in Watts over the timestep being reported.
+
+\paragraph{\texorpdfstring{Cooling Coil Part Load Ratio {[]}}{Cooling Coil Part Load Ratio }}\label{cooling-coil-part-load-ratio-1}
+
+This output variable is the ratio of the part-load capacity to the steady state capacity of the WatertoAirHP coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the WatertoAirHP coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
+
+\paragraph{\texorpdfstring{Cooling Coil Runtime Fraction {[]}}{Cooling Coil Runtime Fraction }}\label{cooling-coil-runtime-fraction-6}
+
+This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The duty factor or part load fraction accounts for efficiency losses due to compressor cycling.
+
+\paragraph{Cooling Coil Air Mass Flow Rate {[}kg/s{]}}\label{cooling-coil-air-mass-flow-rate-kgs-1}
+
+The output variable is the average air mass flow rate going through the heat pump over the timestep being reported.
+
+\paragraph{Cooling Coil Air Inlet Temperature {[}C{]}}\label{cooling-coil-air-inlet-temperature-c-1}
+
+The output variable is the average entering air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Cooling Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{cooling-coil-air-inlet-humidity-ratio-kgwaterkgdryair-1}
+
+The output variable is the average entering air dry humidity ratio over the timestep being reported.
+
+\paragraph{Cooling Coil Air Outlet Temperature {[}C{]}}\label{cooling-coil-air-outlet-temperature-c-1}
+
+The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Cooling Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{cooling-coil-air-outlet-humidity-ratio-kgwaterkgdryair-1}
+
+The output variable is the average leaving air dry humidity ratio over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Mass Flow Rate {[}kg/s{]}}\label{cooling-coil-source-side-mass-flow-rate-kgs}
+
+The output variable is the average water mass flow rate going through the heat pump over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Inlet Temperature {[}C{]}}\label{cooling-coil-source-side-inlet-temperature-c}
+
+The output variable is the average entering water temperature over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Outlet Temperature {[}C{]}}\label{cooling-coil-source-side-outlet-temperature-c}
+
+The output variable is the average leaving water temperature over the timestep being reported.
+
+\paragraph{Cooling Coil Electric Energy {[}J{]}}\label{cooling-coil-electric-energy-j-3}
+
+The output variable is the electric consumption of the heat pump in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Cooling Coil Total Cooling Energy {[}J{]}}\label{cooling-coil-total-cooling-energy-j-8}
+
+The output variable is the total cooling output of the coil in Joules over the timestep being reported. Resource Type = EnergyTransfer, End Use Key = CoolingCoils, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Cooling Coil Sensible Cooling Energy {[}J{]}}\label{cooling-coil-sensible-cooling-energy-j-8}
+
+The output variable is the total sensible cooling output of the coil in Joules over the timestep being reported
+
+\paragraph{Cooling Coil Latent Cooling Energy {[}J{]}}\label{cooling-coil-latent-cooling-energy-j-6}
+
+\paragraph{Cooling Coil Latent Cooling Rate {[}W{]}}\label{cooling-coil-latent-cooling-rate-w-4}
+
+These output variables are the total latent cooling output of the coil in Joules or Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Heat Transfer Energy {[}J{]}}\label{cooling-coil-source-side-heat-transfer-energy-j-3}
+
+The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+\protect\hyperlink{ux5fftnref1}{{[}1{]}} The 23.9 °C wet-bulb temperature condition is not applicable for air-cooled condensers which do not evaporate condensate.
+
+\protect\hyperlink{ux5fftnref2}{{[}2{]}} The 23.9 °C wet-bulb temperature condition is not applicable for air-cooled condensers which do not evaporate condensate.
+
+\protect\hyperlink{ux5fftnref3}{{[}3{]}} The 23.9 °C wet-bulb temperature condition is not applicable for air-cooled condensers which do not evaporate condensate.
+
+\protect\hyperlink{ux5fftnref4}{{[}4{]}} The 23.9 °C wet-bulb temperature condition is not applicable for air-cooled condensers which do not evaporate condensate.
+
+\subsection{Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit}\label{coilcoolingwatertoairheatpumpvariablespeedequationfit}
+
+The Variable-Speed Water-to-Air Cooling Equation Fit Coil is a collection of performance curves that represent the cooling coil at various speed levels. The performance curves should be generated from the heat pump Reference Unit data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. On the other hand, the model uses the bypass factor approach to calculate sensible heat transfer rate, similar to the one used in the single-speed DX coil. The number of speed levels can range from 2 to 10. The cooling coil has four node connections, i.e.~two air sides and two water sides. The user needs to specify a nominal speed level, at which the gross rated total cooling capacity, rated volumetric air and water flow rates are sized. The rated capacity, rated volumetric flow rates represent the real situation in the air and water loops, and are used to determine and flow rates at various speed levels in the parent objects, e.g.~AirLoopHVAC:UnitaryHeatPump:WaterToAir and ZoneHVAC:WaterToAirHeatPump. It shall be mentioned that the performance correction curves, i.e.~the temperature and flow fraction correction curves, should be normalized to the capacity and flow rates at each individual speed and at the rated conditions, similar to the performance curves used in the DX coils. However, the performance values, e.g.~gross capacities, gross COPs, gross SHRs and flow rates at individual speed levels, should be given regarding a specific unit from the Reference Unit catalog data. In the following content, the statement started with Reference Unit means the actual Reference Unit catalog data. The rated conditions for obtaining the capacities, COPs and SHRs are at indoor dry-bulb temperature of 26.67 ËšC (80 ËšF), wet bulb temperature of 19.44 ËšC (67 ËšF), and the source side entering water temperature of 29.4 ËšC (85 ËšF). Some equations are provided below to help explain the function of the various performance curves and data fields. For a detailed description of the algorithm and how the curves are used in the calculations, please see the Engineering Reference.
+
+\subsubsection{Inputs}\label{inputs-31}
+
+\paragraph{Field: Name}\label{field-name-30}
+
+This alpha field contains the identifying name for the variable speed cooling coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-7}
+
+This alpha field contains the cooling coil source side inlet node name.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-7-000}
+
+This alpha field contains the cooling coil source side outlet node name.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-18}
+
+This alpha field contains the cooling coil load side inlet node name.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-18}
+
+This alpha field contains the cooling coil load side outlet node name.
+
+\paragraph{Field: Number of Speeds}\label{field-number-of-speeds-4}
+
+This numeric field contains the maximum number of speed levels that the module uses. The number of speeds, for which the user input the performance data and curves, should be equal or higher than the maximum number. The performance inputs at higher speed levels are ignored.
+
+\paragraph{Field: Nominal Speed Level}\label{field-nominal-speed-level-2}
+
+This numeric field defines the nominal speed level, at which the rated capacity, rated air and water volumetric flow rates are correlated.
+
+\paragraph{Field: Gross Rated Total Cooling Capacity at Selected Nominal Speed Level}\label{field-gross-rated-total-cooling-capacity-at-selected-nominal-speed-level-1}
+
+This numeric field contains the gross rated total cooling capacity at the nominal speed level. This field is autosizable. The gross rated total cooling capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
+
+\begin{equation}
+CapacityScaleFactor = \frac{{GrossRatedTotalCoolingCapacity}}{{ReferenceUnitCapacity@NominalSpeedLevel}}
+\end{equation}
+
+And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below,
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{GrossRatedCapacity} @ \rm{SpeedLevel} \left( x \right) = \rm{CapacityScaleFactor} \\
+    \quad \quad \quad \quad \times \rm{ReferenceUnitCapacity} @ \rm{SpeedLevel}( x )
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Rated Volumetric Air Flow Rate}\label{field-rated-volumetric-air-flow-rate-1}
+
+This numeric field contains the rated volumetric air flow rate on the load side of the heat pump corresponding to the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects. It is recommended that the ratio of the rated volumetric air flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
+
+\begin{equation}
+  \begin{array}{l}
+    AirFlowScaleFactor = \\\quad \quad \quad \quad \quad \frac{{RatedVolumetricAirFlowRate}}{{ReferenceUnitVolAirFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}
+  \end{array}
+\end{equation}
+
+And the volumetric air flow rates in the parent objects are calculated as below,
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{LoopVolumetricAirFlowRate} @ \rm{SpeedLevel} \left( x \right) = \rm{AirFlowScaleFactor} \\
+    \quad \quad \quad \times \rm{ReferenceUnitVolAirFlowRate} @ \rm{SpeedLevel}(x) \\
+    \quad \quad \quad \times \rm{CapacityScaleFactor}
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Rated Volumetric Water Flow Rate}\label{field-rated-volumetric-water-flow-rate}
+
+This numeric field contains the rated volumetric water flow rate on the source side of the heat pump at the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the water flow rates in the water loop. It is recommended that the ratio of the rated volumetric water flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
+
+\begin{equation}
+  \begin{array}{l}
+    WaterFlowScaleFactor = \\
+    \quad \quad \quad \frac{{RatedVolumetricWaterFlowRate}}{{ReferenceUnitVolWaterFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}
+  \end{array}
+\end{equation}
+
+And the required volumetric water flow rates at the speed levels in the parent objects, other than the nominal speed, are calculated as below,
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{LoopVolumetricWaterFlowRate} @ \rm{SpeedLevel} \left( x \right) = \rm{WaterFlowScaleFactor} \\
+    \quad \quad \quad \times \rm{ReferenceUnitVolWaterFlowRate} @ \rm{SpeedLevel}(x) \\
+    \quad \quad \quad  \times \rm{CapacityScaleFactor}
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Nominal Time for Condensate Removal to Begin}\label{field-nominal-time-for-condensate-removal-to-begin-5}
+
+This numeric field defines the nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero.
+
+\paragraph{Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity}\label{field-ratio-of-initial-moisture-evaporation-rate-and-steady-state-latent-capacity-5}
+
+This numeric field defines ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero.
+
+\paragraph{Field: Flag for Using Hot Gas Reheat, 0 or 1}\label{field-flag-for-using-hot-gas-reheat-0-or-1}
+
+This numeric field dictates whether to use the recoverable waste heat for reheating the supply air, downstream of the coil. The value 1 means using the hot gas reheating, and 0 means not using. If the hot gas reheating is turned on, the recoverable waste heat is subtracted from both the total cooling capacity and the sensible cooling capacity. The default value for this field is zero.
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-10}
+
+This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, sensible or latent load/steady-state sensible or latent cooling capacity for Speed 1), in the case that the unit operates under the lowest speed, i.e.~on/off. The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep for Speed 1. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, the runtime fraction of the coil is limited to 1.0. A typical part load fraction correlation would be:
+
+\begin{equation}
+PLF = 0.85 + 0.15 \times PLR
+\end{equation}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{equation}
+PLF = 0.85 + 0.0 \times PLR
+\end{equation}
+
+\paragraph{Field Group: rated specification, performance curves, and waste heat data}\label{field-group-rated-specification-performance-curves-and-waste-heat-data-1}
+
+The performance for each cooling speed must be specified as shown below. They should be directly given from the Reference Unit catalog data. All inputs for Speed 1 are required, followed by the optional inputs for other speeds.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Gross Rated Total Cooling Capacity}\label{field-speed-x-reference-unit-gross-rated-total-cooling-capacity-1}
+
+This numeric field defines the total, full load cooling capacity in watts of the water-to-air cooling coil unit at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0. The gross rated total capacity should not account for the effect of supply air fan heat.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Gross Rated Sensible Heat Ratio}\label{field-speed-x-reference-unit-gross-rated-sensible-heat-ratio-1}
+
+This numeric field defines sensible heat transfer ratio (SHR = gross sensible cooling capacity divided by gross total cooling capacity) of the cooling coil unit at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0.0 and less than 1.0. This value should be obtained from the Reference Unit data. The gross rated SHR should not account for the effect of supply air fan heat.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Gross Rated Cooling COP}\label{field-speed-x-reference-unit-gross-rated-cooling-cop-1}
+
+This numeric field defines the coefficient of performance (COP = gross total cooling capacity in watts divided by electrical power input in watts) of the cooling coil unit at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0. The input power includes power for the compressor(s) and accessories, but does not include the power consumptions of the indoor supply air fan and water pump. The gross COP should not account for the supply air fan.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Rated Air Flow Rate}\label{field-speed-x-reference-unit-rated-air-flow-rate-2}
+
+This numeric field defines the volumetric air flow rate, in m\(^{3}\)per second, across the cooling coil at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here should be directly from the Reference Unit data, corresponding to the given gross rated total cooling capacity and gross rated cooling COP at the speed, as above.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Rated Water Flow Rate}\label{field-speed-x-reference-unit-rated-water-flow-rate}
+
+This numeric field defines the volumetric water flow rate, in m\(^{3}\)per second, flowing at the source side of the cooling coil at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here should be directly from the Reference Unit data, corresponding to the given gross rated total cooling capacity and gross rated cooling COP at the speed, as above.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Total Cooling Capacity Function of Temperature Curve Name}\label{field-speed-x-total-cooling-capacity-function-of-temperature-curve-name-2}
+
+This alpha field defines the name of a bi-quadratic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the both the indoor wet-bulb and source side entering water temperature, from the Reference Unit. The output of this curve is multiplied by the gross rated total cooling capacity at the speed to give the gross total cooling capacity at specific temperature operating conditions (i.e., at an indoor air wet-bulb temperature or entering water temperature different from the rating point temperature). It should be noted that the curve is normalized to the cooling capacity at Speed\textless{}x\textgreater{} from the Reference Unit data, and have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Total Cooling Capacity Function of Air Flow Fraction Curve Name}\label{field-speed-x-total-cooling-capacity-function-of-air-flow-fraction-curve-name-1}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of full load flow at Speed \textless{}x\textgreater{}, from the Reference Unit data). The curve is normalized to have the value of 1.0 when the actual air flow rate equals the design air flow rate, at Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Total Cooling Capacity Function of Water Flow Fraction Curve Name}\label{field-speed-x-total-cooling-capacity-function-of-water-flow-fraction-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the ratio of actual water flow rate across the cooling coil to the design water flow rate (i.e., fraction of full load flow), at Speed \textless{}x\textgreater{}, from the Reference Unit data. The curve is normalized to have the value of 1.0 when the actual water flow rate equals the design air flow rate, at Speed \textless{}x\textgreater{}.
+
+The actual total cooling capacity at Speed \textless{}x\textgreater{}, considering variations in temperatures, air and water flow rates is calculated as below:
+
+\begin{equation}
+  \begin{array}{l}
+    \rm{ActualCapacity} @ \rm{SpeedLevel} \left( x \right) = \rm{CapacityScaleFactor} \\
+    \quad \quad \quad \times \rm{ReferenceUnitCapacity} @ \rm{SpeedLevel}(x) \\
+    \quad \quad \quad \times \rm{TotCapTempModFac} @ \rm{SpeedLevel}(x) \\
+    \quad \quad \quad \times \rm{TotCapAirFlowModFac} @ \rm{SpeedLevel}(x) \\
+    \quad \quad \quad \times \rm{TotCapWaterFlowModFac} @ \rm{SpeedLevel}(x)
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Temperature Curve Name}\label{field-speed-x-energy-input-ratio-function-of-temperature-curve-name-4}
+
+This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor air wet-bulb and entering water temperatures The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP at Speed \textless{}x\textgreater{} from the Reference Unit data) to give the EIR at specific temperature operating conditions (i.e., at an indoor air wet-bulb temperature or entering water temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Air Flow Fraction Curve Name}\label{field-speed-x-energy-input-ratio-function-of-air-flow-fraction-curve-name-2}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of full load flow, at Speed \textless{}x\textgreater{} from the Reference Unit data). The EIR is the inverse of the COP. This curve is normalized to a value of 1.0 when the actual air flow rate equals the design air flow rate.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Water Flow Fraction Curve Name}\label{field-speed-x-energy-input-ratio-function-of-water-flow-fraction-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual water flow rate across the cooling coil to the design water flow rate (i.e., fraction of full load flow, at Speed \textless{}x\textgreater{} from the Reference Unit data). This curve is normalized to a value of 1.0 when the actual air flow rate equals the design air flow rate.
+
+The actual EIR at Speed \textless{}x\textgreater{}, considering variations in temperatures, air and water flow rates is calculated as below:
+
+\begin{equation}
+  \begin{array}{l}
+    ActualEIR@SpeedLevel\left( x \right) = \frac{{1.0}}{{ReferenceUnitCOP@SpeedLevel(x)}} \\
+    \quad \quad \quad \times EIRTempModFac@SpeedLevel(x) \\
+    \quad \quad \quad \times EIRAirFlowModFac@SpeedLevel(x) \\
+    \quad \quad \quad \times EIRWaterFlowModFac@SpeedLevel(x)
+  \end{array}
+\end{equation}
+
+And, the actual power consumption is calculated:
+
+\begin{equation}
+  \begin{array}{l}
+    ActualPower@SpeedLevel\left( x \right) = ActualCapacity@SpeedLevel\left( x \right) \\
+    \quad \quad \quad \quad  \times ActualEIR@SpeedLevel\left( x \right)
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Waste Heat Fraction of Power Input}\label{field-speed-x-reference-unit-waste-heat-fraction-of-power-input}
+
+The fraction of heat input to cooling that is available as recoverable waste heat at full load and rated conditions for Speed \textless{}x\textgreater{} operation. The part of heat is not discharged to the water loop. And it can be used for hot gas reheating during dehumidification operation, by setting 1 to Flag for Using Hot Gas Reheat.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Waste Heat Function of Temperature Curve Name}\label{field-speed-x-waste-heat-function-of-temperature-curve-name-2}
+
+The name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the waste heat recovery as a function of indoor wet-bulb temperature and the entering water temperature for Speed \textless{}x\textgreater{} from the Reference Unit data. The output of this curve is multiplied by the design recoverable waste heat at specific temperature operating conditions (i.e., at temperatures different from the rating point). The curve is normalized to a value of 1.0 at the rating point.
+
+The actual recoverable waste heat at Speed \textless{}x\textgreater{} is calculated as below:
+
+\begin{equation}
+  \begin{array}{l}
+    ActualWasteHeat@SpeedLevel\left( x \right) = ActualPower@SpeedLevel\left( x \right) \\
+    \quad \quad \quad \quad \times WasteHeatFrac@SpeedLevel(x) \\
+    \quad \quad \quad \quad \times WasteHeatTempModFac@SpeedLevel(x)
+  \end{array}
+\end{equation}
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit,
+  Sys 1 Heat Pump Cooling Mode,                           !- Name
+  Sys 1 Water to Air Heat Pump Source Side1 Inlet Node,   !- Water Inlet Node Name
+  Sys 1 Water to Air Heat Pump Source Side1 Outlet Node,  !- Water Outlet Node Name
+  Sys 1 Cooling Coil Air Inlet Node,!- Air Inlet Node Name
+  Sys 1 Heating Coil Air Inlet Node,!- Air Outlet Node Name
+  10.0,                             !- Number of Speeds
+  10.0,                             !- Nominal Speed Level
+  Autosize,                         !- Gross Rated Total Cooling Capacity {W}
+  Autosize,                         !- Rated Air Flow Rate {m3/s}
+  Autosize,                         !- Rated Water Flow Rate {m3/s}
+  0.0,                              !- Nominal time for Condensate to Begin Leaving the Coil
+  0.0,                              !- Initial Moisture Evaporation Rate Divided by Steady-State AC Latent Capacity
+  1,                                !- Flag for Using Hot Gas Reheat or Not, 0 = false; 1 = true
+  VS Energy Part Load Fraction 1,   !- Energy Part Load Fraction Curve
+  1524.1,                           !- Speed 1 Reference Unit Gross Rated Total Cooling Capacity
+  0.75,                             !- Speed 1 Reference Unit Gross Sensible Heat Ratio
+  4.0,                              !- Speed 1 Reference Unit Gross Cooling COP
+  0.1359072,                        !- Speed 1 Reference Unit Rated air flow rate
+  0.000381695,                      !- Speed 1 Reference Unit Rated water flow rate
+  TC VS Temp1 Test,                 !- Speed 1 Total Cooling Capacity Function of Temperature Curve Name
+  TC VS AirFrac Test,               !- Speed 1 Total Cooling Capacity Function of Air Flow Fraction Curve Name
+  TC VS WaterFrac Test,             !- Speed 1 Total Cooling Capacity Function of Water Flow Fraction Curve Name
+  EIR VS Temp1 Test,                !- Speed 1 Energy Input Ratio Function of Temperature Curve Name
+  EIR VS AirFrac Test,              !- Speed 1 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIR VS WaterFrac Test,            !- Speed 1 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                              !- Speed 1 Waste Heat fraction to power input
+  wasteHeat VS Temp1 Test,          !- Speed 1 Waste Heat Function of Temperature Curve Name
+  1877.9,                           !- Speed 2 Reference Unit Gross Rated Total Cooling Capacity
+  0.75,                             !- Speed 2 Reference Unit Gross Sensible Heat Ratio
+  4.0,                              !- Speed 2 Reference Unit Gross Cooling COP
+  0.151008,                         !- Speed 2 Reference Unit Rated air flow rate
+  0.000381695,                      !- Speed 2 Reference Unit Rated water flow rate
+  TC VS Temp1 Test,                 !- Speed 2 Total Cooling Capacity Function of Temperature Curve Name
+  TC VS AirFrac Test,               !- Speed 2   Total Cooling Capacity Function of Air Flow Fraction Curve Name
+  TC VS WaterFrac Test,             !- Speed 2   Total Cooling Capacity Function of Water Flow Fraction Curve Name
+  EIR VS Temp1 Test,                !- Speed 2   Energy Input Ratio Function of Temperature Curve Name
+  EIR VS AirFrac Test,              !- Speed 2   Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIR VS WaterFrac Test,            !- Speed 2   Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                              !- Speed 2   Waste Heat fraction to power input
+  wasteHeat VS Temp1 Test,          !- Speed 2   Waste Heat Function of Temperature Curve Name
+  2226.6,                           !- Speed 3 Reference Unit Gross Rated Total Cooling Capacity
+  0.75,                             !- Speed 3 Reference Unit Gross Sensible Heat Ratio
+  4.0,                              !- Speed 3 Reference Unit Gross Cooling COP
+  0.1661088,                        !- Speed 3 Reference Unit Rated air flow rate
+  0.000381695,                      !- Speed 3 Reference Unit Rated water flow rate
+  TC VS Temp1 Test,                 !- Speed 3 Total Cooling Capacity Function of Temperature Curve Name
+  TC VS AirFrac Test,               !- Speed 3 Total Cooling Capacity Function of Air Flow Fraction Curve Name
+  TC VS WaterFrac Test,             !- Speed 3 Total Cooling Capacity Function of Water Flow Fraction Curve Name
+  EIR VS Temp1 Test,                !- Speed 3 Energy Input Ratio Function of Temperature Curve Name
+  EIR VS AirFrac Test,              !- Speed 3 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIR VS WaterFrac Test,            !- Speed 3 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                              !- Speed 3 Waste Heat fraction to power input
+  wasteHeat VS Temp1 Test,          !- Speed 3 Waste Heat Function of Temperature Curve Name
+  2911.3,                           !- Speed 4 Reference Unit Gross Rated Total Cooling Capacity
+  0.75,                             !- Speed 4 Reference Unit Gross Sensible Heat Ratio
+  4.0,                              !- Speed 4 Reference Unit Gross Cooling COP
+  0.1963104,                        !- Speed 4 Reference Unit Rated air flow rate
+  0.000381695,                      !- Speed 4 Reference Unit Rated water flow rate
+  TC VS Temp1 Test,                 !- Speed 4 Total Cooling Capacity Function of Temperature Curve Name
+  TC VS AirFrac Test,               !- Speed 4 Total Cooling Capacity Function of Air Flow Fraction Curve Name
+  TC VS WaterFrac Test,             !- Speed 4 Total Cooling Capacity Function of Water Flow Fraction Curve Name
+  EIR VS Temp1 Test,                !- Speed 4 Energy Input Ratio Function of Temperature Curve Name
+  EIR VS AirFrac Test,              !- Speed 4 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIR VS WaterFrac Test,            !- Speed 4 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                              !- Speed 4 Waste Heat fraction to power input
+  wasteHeat VS Temp1 Test,          !- Speed 4 Waste Heat Function of Temperature Curve Name
+  3581.7,                           !- Speed 5 Reference Unit Gross Rated Total Cooling Capacity
+  0.75,                             !- Speed 5 Reference Unit Gross Sensible Heat Ratio
+  4.0,                              !- Speed 5 Reference Unit Gross Cooling COP
+  0.226512,                         !- Speed 5 Reference Unit Rated air flow rate
+  0.000381695,                      !- Speed 5 Reference Unit Rated water flow rate
+  TC VS Temp1 Test,                 !- Speed 5 Total Cooling Capacity Function of Temperature Curve Name
+  TC VS AirFrac Test,               !- Speed 5 Total Cooling Capacity Function of Air Flow Fraction Curve Name
+  TC VS WaterFrac Test,             !- Speed 5 Total Cooling Capacity Function of Water Flow Fraction Curve Name
+  EIR VS Temp1 Test,                !- Speed 5 Energy Input Ratio Function of Temperature Curve Name
+  EIR VS AirFrac Test,              !- Speed 5 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIR VS WaterFrac Test,            !- Speed 5 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                              !- Speed 5 Waste Heat fraction to power input
+  wasteHeat VS Temp1 Test,          !- Speed 5 Waste Heat Function of Temperature Curve Name
+  4239.5,                           !- Speed 6 Reference Unit Gross Total Cooling Capacity
+  0.75,                             !- Speed 6 Reference Unit Gross Sensible Heat Ratio
+  4.0,                              !- Speed 6 Reference Unit Gross Cooling COP
+  0.2567136,                        !- Speed 6 Reference Unit Rated air flow rate
+  0.000381695,                      !- Speed 6 Reference Unit Rated water flow rate
+  TC VS Temp1 Test,                 !- Speed 6 Total Cooling Capacity Function of Temperature Curve Name
+  TC VS AirFrac Test,               !- Speed 6 Total Cooling Capacity Function of Air Flow Fraction Curve Name
+  TC VS WaterFrac Test,             !- Speed 6 Total Cooling Capacity Function of Water Flow Fraction Curve Name
+  EIR VS Temp1 Test,                !- Speed 6 Energy Input Ratio Function of Temperature Curve Name
+  EIR VS AirFrac Test,              !- Speed 6 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIR VS WaterFrac Test,            !- Speed 6 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                              !- Speed 6 Waste Heat fraction to power input
+  wasteHeat VS Temp1 Test,          !- Speed 6 Waste Heat Function of Temperature Curve Name
+  4885.7,                           !- Speed 7 Reference Unit Gross Rated Total Cooling Capacity
+  0.75,                             !- Speed 7 Reference Unit Gross Sensible Heat Ratio
+  4.0,                              !- Speed 7 Reference Unit Gross Cooling COP
+  0.2869152,                        !- Speed 7 Reference Unit Rated air flow rate
+  0.000381695,                      !- Speed 7 Reference Unit Rated water flow rate
+  TC VS Temp1 Test,                 !- Speed 7 Total Cooling Capacity Function of Temperature Curve Name
+  TC VS AirFrac Test,               !- Speed 7 Total Cooling Capacity Function of Air Flow Fraction Curve Name
+  TC VS WaterFrac Test,             !- Speed 7 Total Cooling Capacity Function of Water Flow Fraction Curve Name
+  EIR VS Temp1 Test,                !- Speed 7 Energy Input Ratio Function of Temperature Curve Name
+  EIR VS AirFrac Test,              !- Speed 7 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIR VS WaterFrac Test,            !- Speed 7 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                              !- Speed 7 Waste Heat fraction to power input
+  wasteHeat VS Temp1 Test,          !- Speed 7 Waste Heat Function of Temperature Curve Name
+  5520.7,                           !- Speed 8 Reference Unit Gross Rated Total Cooling Capacity
+  0.75,                             !- Speed 8 Reference Unit Gross Sensible Heat Ratio
+  4.0,                              !- Speed 8 Reference Unit Gross Cooling COP
+  0.3171168,                        !- Speed 8 Reference Unit Rated air flow rate
+  0.000381695,                      !- Speed 8 Reference Unit Rated water flow rate
+  TC VS Temp1 Test,                 !- Speed 8 Total Cooling Capacity Function of Temperature Curve Name
+  TC VS AirFrac Test,               !- Speed 8 Total Cooling Capacity Function of Air Flow Fraction Curve Name
+  TC VS WaterFrac Test,             !- Speed 8 Total Cooling Capacity Function of Water Flow Fraction Curve Name
+  EIR VS Temp1 Test,                !- Speed 8 Energy Input Ratio Function of Temperature Curve Name
+  EIR VS AirFrac Test,              !- Speed 8 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIR VS WaterFrac Test,            !- Speed 8 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                              !- Speed 8 Waste Heat fraction to power input
+  wasteHeat VS Temp1 Test,          !- Speed 8 Waste Heat Function of Temperature Curve Name
+  6144.8,                           !- Speed 9 Reference Unit Gross Rated Total Cooling Capacity
+  0.75,                             !- Speed 9 Reference Unit Gross Sensible Heat Ratio
+  4.0,                              !- Speed 9 Reference Unit Gross Cooling COP
+  0.3473184,                        !- Speed 9 Reference Unit Rated air flow rate
+  0.000381695,                      !- Speed 9 Reference Unit Rated water flow rate
+  TC VS Temp1 Test,                 !- Speed 9 Total Cooling Capacity Function of Temperature Curve Name
+  TC VS AirFrac Test,               !- Speed 9 Total Cooling Capacity Function of Air Flow Fraction Curve Name
+  TC VS WaterFrac Test,             !- Speed 9 Total Cooling Capacity Function of Water Flow Fraction Curve Name
+  EIR VS Temp1 Test,                !- Speed 9 Energy Input Ratio Function of Temperature Curve Name
+  EIR VS AirFrac Test,              !- Speed 9 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIR VS WaterFrac Test,            !- Speed 9 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                              !- Speed 9 Waste Heat fraction to power input
+  wasteHeat VS Temp1 Test,          !- Speed 9 Waste Heat Function of Temperature Curve Name
+  6758.0,                           !- Speed 10 Reference Unit Gross Rated Total Cooling Capacity
+  0.75,                             !- Speed 10 Reference Unit Gross Sensible Heat Ratio
+  4.0,                              !- Speed 10 Reference Unit Gross Cooling COP
+  0.37752,                          !- Speed 10 Reference Unit Rated air flow rate
+  0.000381695,                      !- Speed 10 Reference Unit Rated water flow rate
+  TC VS Temp1 Test,                 !- Speed 10 Total Cooling Capacity Function of Temperature Curve Name
+  TC VS AirFrac Test,               !- Speed 10 Total Cooling Capacity Function of Air Flow Fraction Curve Name
+  TC VS WaterFrac Test,             !- Speed 10 Total Cooling Capacity Function of Water Flow Fraction Curve Name
+  EIR VS Temp1 Test,                !- Speed 10 Energy Input Ratio Function of Temperature Curve Name
+  EIR VS AirFrac Test,              !- Speed 10 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIR VS WaterFrac Test,            !- Speed 10 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                              !- Speed 10 Waste Heat fraction to power input
+  wasteHeat VS Temp1 Test;          !- Speed 10 Waste Heat Function of Temperature Curve Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-26}
+
+\begin{itemize}
+\item
+  HVAC, Average, Cooling Coil Electric Power {[}W{]}
+\item
+  HVAC, Average, Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC, Average, Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC, Average, Cooling Coil Source Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Average, Cooling Coil Part Load Ratio {[]}
+\item
+  HVAC, Average, Cooling Coil Runtime Fraction {[]}
+\item
+  HVAC, Average, Cooling Coil Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Cooling Coil Air Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Cooling Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC, Average, Cooling Coil Air Outlet Temperature {[}C{]}
+\item
+  HVAC, Average, Cooling Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC, Average, Cooling Coil Source Side Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Cooling Coil Source Side Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Cooling Coil Source Side Outlet Temperature {[}C{]}
+\item
+  HVAC, Average, Cooling Coil Upper Speed Level {[]}
+\item
+  HVAC, Average, Cooling Coil Neighboring Speed Levels Ratio {[]}
+\item
+  HVAC, Average, Cooling Coil Recoverable Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Cooling Coil Electric Energy {[}J{]}
+\item
+  HVAC, Sum, Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC, Sum, Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC, Sum, Cooling Coil Latent Cooling Energy {[}J{]}
+\item
+  HVAC, Average, Cooling Coil Latent Cooling Rate {[}W{]}
+\item
+  HVAC, Sum, Cooling Coil Source Side Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Cooling Coil Electric Power {[}W{]}}\label{cooling-coil-electric-power-w-3}
+
+This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Total Cooling Rate {[}W{]}}\label{cooling-coil-total-cooling-rate-w-9}
+
+The output variable is the average total cooling load provide by the heat pump which includes the sensible and latent load in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Sensible Cooling Rate {[}W{]}}\label{cooling-coil-sensible-cooling-rate-w-9}
+
+The output variable is the average sensible cooling load provide by the heat pump in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Heat Transfer Rate {[}W{]}}\label{cooling-coil-source-side-heat-transfer-rate-w-2}
+
+The output variable is the average heat rejected to the water at the heat pump condenser in Watts over the timestep being reported.
+
+\paragraph{\texorpdfstring{Cooling Coil Part Load Ratio {[]}}{Cooling Coil Part Load Ratio }}\label{cooling-coil-part-load-ratio-2}
+
+This output variable is the ratio of the part-load capacity to the steady state capacity of the VSWatertoAirHP coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the VSWatertoAirHP coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
+
+\paragraph{\texorpdfstring{Cooling Coil Runtime Fraction {[]}}{Cooling Coil Runtime Fraction }}\label{cooling-coil-runtime-fraction-7}
+
+This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The duty factor or runtime fraction accounts for efficiency losses due to compressor cycling.
+
+\paragraph{Cooling Coil Air Mass Flow Rate {[}kg/s{]}}\label{cooling-coil-air-mass-flow-rate-kgs-2}
+
+The output variable is the average air mass flow rate going through the heat pump over the timestep being reported.
+
+\paragraph{Cooling Coil Air Inlet Temperature {[}C{]}}\label{cooling-coil-air-inlet-temperature-c-2}
+
+The output variable is the average entering air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Cooling Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{cooling-coil-air-inlet-humidity-ratio-kgwaterkgdryair-2}
+
+The output variable is the average entering air dry humidity ratio over the timestep being reported.
+
+\paragraph{Cooling Coil Air Outlet Temperature {[}C{]}}\label{cooling-coil-air-outlet-temperature-c-2}
+
+The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Cooling Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{cooling-coil-air-outlet-humidity-ratio-kgwaterkgdryair-2}
+
+The output variable is the average leaving air dry humidity ratio over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Mass Flow Rate {[}kg/s{]}}\label{cooling-coil-source-side-mass-flow-rate-kgs-1}
+
+The output variable is the average water mass flow rate going through the heat pump over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Inlet Temperature {[}C{]}}\label{cooling-coil-source-side-inlet-temperature-c-1}
+
+The output variable is the average entering water temperature over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Outlet Temperature {[}C{]}}\label{cooling-coil-source-side-outlet-temperature-c-1}
+
+The output variable is the average leaving water temperature over the timestep being reported.
+
+\paragraph{\texorpdfstring{Cooling Coil Upper Speed Level {[]}}{Cooling Coil Upper Speed Level }}\label{cooling-coil-upper-speed-level-1}
+
+The output variable is the average upper speed level, for interpolating performances between two neighboring speed levels.
+
+\paragraph{\texorpdfstring{Cooling Coil Neighboring Speed Levels Ratio {[]}}{Cooling Coil Neighboring Speed Levels Ratio }}\label{cooling-coil-neighboring-speed-levels-ratio-1}
+
+The output variable is the average speed ratio, for interpolating performances between two neighboring speed levels.
+
+\paragraph{Cooling Coil Recoverable Heat Transfer Rate {[}W{]}}\label{cooling-coil-recoverable-heat-transfer-rate-w}
+
+This output variable is the average recoverable waste heat rate of the heat pump in Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Electric Energy {[}J{]}}\label{cooling-coil-electric-energy-j-4}
+
+The output variable is the electric consumption of the heat pump in Joules over the timestep being reported.
+
+\paragraph{Cooling Coil Total Cooling Energy {[}J{]}}\label{cooling-coil-total-cooling-energy-j-9}
+
+The output variable is the total cooling output of the coil in Joules over the timestep being reported.
+
+\paragraph{Cooling Coil Sensible Cooling Energy {[}J{]}}\label{cooling-coil-sensible-cooling-energy-j-9}
+
+The output variable is the total sensible cooling output of the coil in Joules over the timestep being reported
+
+\paragraph{Cooling Coil Latent Cooling Energy {[}J{]}}\label{cooling-coil-latent-cooling-energy-j-7}
+
+\paragraph{Cooling Coil Latent Cooling Rate {[}W{]}}\label{cooling-coil-latent-cooling-rate-w-5}
+
+These output variables are the total latent cooling output of the coil in Joules or Watts over the timestep being reported.
+
+\paragraph{Cooling Coil Source Side Heat Transfer Energy {[}J{]}}\label{cooling-coil-source-side-heat-transfer-energy-j-4}
+
+The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported.
+
+\subsection{Coil:Heating:WaterToAirHeatPump:ParameterEstimation}\label{coilheatingwatertoairheatpumpparameterestimation}
+
+The Water to Air heat pump heating coil is a deterministic model that requires parameters to describe the operating conditions of the heat pump s components. The parameters are generated from the manufacturer catalog data using multi-variable optimization method. However, the parameters required for WatertoAirHP heating coil is similar to WatertoAirHP cooling except (source side outside heat transfer coefficient) parameter is not required for heating. In addition, the heating coil model can be used for 3 type of compressors which are \textbf{reciprocating}, \textbf{rotary} and \textbf{scroll}.
+
+\subsubsection{Inputs}\label{inputs-32}
+
+\paragraph{Field: Name}\label{field-name-31}
+
+This alpha field contains the identifying name for the coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
+
+\paragraph{Field: Compressor Type}\label{field-compressor-type-1}
+
+Type of compressor mode used for the heat pump. Choices available are reciprocating, rotary and scroll compressor. Note that the parameters vary for different compressor.
+
+\paragraph{Field: Refrigerant Type}\label{field-refrigerant-type-1}
+
+This alpha field contains the type of refrigerant used by the heat pump.
+
+\paragraph{Field: Design Source Side Flow Rate}\label{field-design-source-side-flow-rate-1}
+
+This numeric field defines the water flow rate though the coil in m3/sec
+
+\paragraph{Field: Gross Rated Heating Capacity}\label{field-gross-rated-heating-capacity-3}
+
+This numeric field defines the gross heating capacity for the WatertoAirHP heating coil at the rated condition in Watts. The gross heating capacity should Not inlcude the ffect of supply air fan heat.
+
+\paragraph{Field: High Pressure Cutoff}\label{field-high-pressure-cutoff-1}
+
+This numeric field defines the compressor s maximum allowable pressure in Pascal (N/m2)
+
+\paragraph{Field: Low Pressure Cutoff}\label{field-low-pressure-cutoff-1}
+
+This numeric field defines the compressor s minimum allowable pressure in Pascal (N/m2)
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-8}
+
+This alpha field contains the heating coil source side inlet node name.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-8}
+
+This alpha field contains the heating coil source side outlet node name.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-19}
+
+This alpha field contains the heating coil air inlet node name.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-19}
+
+This alpha field contains the heating coil air outlet node name.
+
+\paragraph{Heating Coil Parameters}\label{heating-coil-parameters}
+
+Depending on the type of compressor specified, the type of parameters and values also differs. An Excel Spreadsheet is in the final stage of development that is capable of estimating the parameters based on the manufacturer data. The general parameters are listed first followed by specific parameters required by the respective compressor model. Lastly, parameters are listed based on the type of source side fluid used.
+
+\paragraph{Field: Load Side Total Heat Transfer Coefficient}\label{field-load-side-total-heat-transfer-coefficient-1}
+
+This numeric field defines the estimated parameter \textbf{load side total heat transfer coefficient} in W/K. This field was previously known as Parameter 1.
+
+\paragraph{Field: Superheat Temperature at the Evaporator Outlet}\label{field-superheat-temperature-at-the-evaporator-outlet-1}
+
+This numeric field defines the estimated parameter \textbf{superheat temperature} at the evaporator outlet in ËšC. This field was previously known as Parameter 2.
+
+\paragraph{Field: Compressor Power Losses}\label{field-compressor-power-losses-1}
+
+This numeric field defines the estimated parameter \textbf{compressor power losses}, which accounts for the loss of work due to mechanical and electrical losses in the compressor in Watts. This field was previously known as Parameter 3.
+
+\paragraph{Field: Compressor Efficiency}\label{field-compressor-efficiency-1}
+
+This numeric field defines the estimated parameter of the \textbf{compressor s efficiency}. The compressor efficiency is formulated as the equation below:
+
+\begin{equation}
+\eta  = \frac{{{{\dot W}_{Theoritical}}}}{{{{\dot W}_{CompInput}} - {{\dot W}_{Loss}}}}
+\end{equation}
+
+This field was previously know as Parameter 4.
+
+\paragraph{Field: Compressor Piston Displacement}\label{field-compressor-piston-displacement-1}
+
+This numeric field defines the estimated parameter \textbf{piston displacement of the compressor} in m3/s. This field was part of what was previously known as Parameter 5. It should be used when the Compressor type is either Reciprocating and Rotary. The field should be left blank when Compressor type is Scroll.
+
+\paragraph{Field: Compressor Suction/Discharge Pressure Drop}\label{field-compressor-suctiondischarge-pressure-drop-1}
+
+This numeric field defines the estimated parameter \textbf{pressure drop at the compressor suction} and discharge in Pascals (N/m2). This field was part of what was previously known as Parameter 6. It should be used when the Compressor type is either Reciprocating and Rotary. The field should be left blank when Compressor type is Scroll.
+
+\paragraph{Field: Compressor Clearance Factor}\label{field-compressor-clearance-factor-1}
+
+This numeric field defines the estimated parameter \textbf{clearance factor of the compressor}. This parameter is dimensionless. This field was part of what was previously known as Parameter 7. It should only be used when the Compressor type is Reciprocating. The field should be left blank when Compressor type is Scroll or Rotary.
+
+\paragraph{Field: Refrigerant Volume Flow Rate}\label{field-refrigerant-volume-flow-rate-1}
+
+This numeric field defines the \textbf{refrigerant volume flow rate} at the beginning of the compression {[}m3/s{]}. This field was part of what was previously known as Parameter 6. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
+
+\paragraph{Field: Volume Ratio}\label{field-volume-ratio-1}
+
+This numeric field defines the \textbf{built-in-volume ratio}. This field was part of what was previously known as Parameter 6. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
+
+\paragraph{Field: Leak Rate Coefficient}\label{field-leak-rate-coefficient-1}
+
+This numeric field defines the coefficient for the relationship between \textbf{pressure ratio and leakage rate}. This field was part of what was previously known as Parameter 7. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
+
+\paragraph{Field: Source Side Heat Transfer Coefficient}\label{field-source-side-heat-transfer-coefficient-1}
+
+This numeric field defines the estimated parameter \textbf{source side heat transfer coefficient} in W/K. This field was part of what was previously known as Parameter 8. It should only be used when the Source Side Fluid Name is Water.
+
+\paragraph{Field: Source Side Heat Transfer Resistance1}\label{field-source-side-heat-transfer-resistance1-1}
+
+This numeric field defines the estimated parameter \textbf{source side heat transfer resistance 1}. Unit is dimensionless. This field was part of what was previously known as Parameter 8. It should only be used when the Source Side Fluid Name is an antifreeze.
+
+\paragraph{Field: Source Side Heat Transfer Resistance2}\label{field-source-side-heat-transfer-resistance2-1}
+
+This numeric field defines the estimated \textbf{parameter source side heat transfer resistance 2}. Unit is W/K. This field was previously known as Parameter 9. It should only be used when the Source Side Fluid Name is an antifreeze.
+
+Following is an example input for Coil:WatertoAirHP:ParameterEstimation:Heating
+
+\begin{lstlisting}
+
+Coil:Heating:WaterToAirHeatPump:ParameterEstimation,
+  Heat Pump HEATING Mode AHU1,   !- Name
+  Scroll,                                   !- Compressor Type
+  R22,                                         !- Refrigerant Type
+  0.0015,                                   !- Design Source Side Flow Rate {m3/s}
+  38000,                                     !- Gross Rated Heating Capacity {W}
+  3000000,                                 !- High Pressure Cutoff
+  0,                                             !- Low Pressure Cutoff {Pa}
+  AHU1 Water to Air Heat Pump Source Side2 Inlet Node,   !- Water Inlet Node Name
+  AHU1 Water to Air Heat Pump Source Side2 Outlet Node,   !- Water Outlet Node Name
+  Cooling Coil Air Outlet Node AHU1,   !- Air Inlet Node Name
+  Heating Coil Air Outlet Node AHU1,   !- Air Outlet Node Name
+  5.79505E+03,                         !- Load Side Total Heat Transfer Coefficient {W/K}
+  1.56696E+00,                         !- Superheat Temperature at the Evaporator Outlet {C}
+  3.91338E+03,                         !- Compressor Power Losses {W}
+  1.26356E+00,                         !- Compressor Efficiency
+  ,                                               !- Compressor Piston Displacement {m3/s}
+  ,                                               !- Compressor Suction/Discharge Pressure Drop {Pa}
+  ,                                               !- Compressor Clearance Factor {dimensionless}
+  6.99573E-03,                         !- Refrigerant Volume Flow Rate {m3/s}
+  4.96167E+00,                         !- Volume Ratio {dimensionless}
+  2.07750E-06,                         !-Leak Rate Coefficient {dimensionless}
+  4.00322E+03,                         !- Source Side Heat Transfer Coefficient {W/K}
+  ,                                               !- Source Side Heat Transfer Resistance1 {dimensionless}
+  ;                                               !- Source Side Heat Transfer Resistance2 {W/K}
+\end{lstlisting}
+
+\subsection{Coil:Heating:WaterToAirHeatPump:EquationFit}\label{coilheatingwatertoairheatpumpequationfit}
+
+The Water to Air Heating Equation Fit Coil is a simple curve-fit model that requires coefficients generated from the heat pump catalog data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. The performance of the heat pump is modeled using curves fitted from the catalog data.
+
+\subsubsection{Inputs}\label{inputs-33}
+
+\paragraph{Field: Name}\label{field-name-32}
+
+This alpha field contains the identifying name for the coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-9}
+
+This alpha field contains the heating coil source side inlet node name.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-9}
+
+This alpha field contains the heating coil source side outlet node name.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-20}
+
+This alpha field contains the heating coil air inlet node name.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-20}
+
+This alpha field contains the heating coil air outlet node name.
+
+\paragraph{Field: Rated Air Flow Rate}\label{field-rated-air-flow-rate-6}
+
+This numeric field contains the rated volumetric air flow rate on the load side of the heat pump in m3/s. This field is autosizable.
+
+\paragraph{Field: Rated Water Flow Rate}\label{field-rated-water-flow-rate-1}
+
+This numeric field contains the rated volumetric water flow rate on the source side of the heat pump in m3/s. This field is autosizable.
+
+\paragraph{Field: Gross Rated Heating Capacity}\label{field-gross-rated-heating-capacity-4}
+
+This numeric field contains the gross heating capacity of the heat pump at the rated condition in W. The gross heating capacity should not account for the effect of supply air fan heat. This field is autosizable.
+
+\paragraph{Field: Gross Rated Heating COP}\label{field-gross-rated-heating-cop-1}
+
+This numeric field contains the gross rated heating coefficient of performance of the heat pump. The gross rated COP of the heat pump should not account for the effect of supply air fan heat.
+
+\paragraph{Field: Heating Capacity Coefficient 1-5}\label{field-heating-capacity-coefficient-1-5}
+
+These numeric fields contain the first to fifth coefficient for the heat pump capacity.
+
+\paragraph{Field: Heating Power Consumption Coefficient 1-5}\label{field-heating-power-consumption-coefficient-1-5}
+
+These numeric fields contain the first to fifth coefficient for the heat pump power consumption.
+
+\subsubsection{Outputs}\label{outputs-27}
+
+Coil:Heating:WaterToAirHeatPump:ParameterEstimation and Coil:Heating:WaterToAirHeatPump:EquationFit have the same output variables listed as follows;
+
+\begin{itemize}
+\item
+  HVAC, Average, Heating Coil Electric Power {[}W{]}
+\item
+  HVAC, Average, Heating Coil Heating Rate {[}W{]}
+\item
+  HVAC, Average, Heating Coil Sensible Heating Rate {[}W{]}
+\item
+  HVAC, Average, Heating Coil Source Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Average, Heating Coil Part Load Ratio
+\item
+  HVAC, Average, Heating Coil Runtime Fraction {[]}
+\item
+  HVAC, Average, Heating Coil Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Heating Coil Air Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Heating Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC, Average, Heating Coil Air Outlet Temperature {[}C{]}
+\item
+  HVAC, Average, Heating Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC, Average, Heating Coil Source Side Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Heating Coil Source Side Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Heating Coil Source Side Outlet Temperature {[}C{]}
+\item
+  HVAC, Sum, Heating Coil Electric Energy {[}J{]}
+\item
+  HVAC, Sum, Heating Coil Heating Energy {[}J{]}
+\item
+  HVAC, Sum, Heating Coil Source Side Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Heating Coil Electric Power {[}W{]}}\label{heating-coil-electric-power-w-8}
+
+This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Heating Rate {[}W{]}}\label{heating-coil-heating-rate-w-3}
+
+The output variable is the average total heating capacity provide by the heat pump which includes the sensible and latent capacity in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Sensible Heating Rate {[}W{]}}\label{heating-coil-sensible-heating-rate-w-1}
+
+The output variable is the average sensible heating capacity provide by the heat pump in Watts over the timestep being reported. For heating mode, the sensible capacity is equal to the total capacity.
+
+\paragraph{Heating Coil Source Side Heat Transfer Rate {[}W{]}}\label{heating-coil-source-side-heat-transfer-rate-w-1}
+
+The output variable is the average heat absorbed at the heat pump evaporator in Watts over the timestep being reported.
+
+\paragraph{\texorpdfstring{Heating Coil Part Load Ratio {[]}}{Heating Coil Part Load Ratio }}\label{heating-coil-part-load-ratio-1}
+
+This output variable is the ratio of the part-load capacity to the steady state capacity of the WatertoAirHP coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the WatertoAirHP coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
+
+\paragraph{\texorpdfstring{Heating Coil Runtime Fraction {[]}}{Heating Coil Runtime Fraction }}\label{heating-coil-runtime-fraction-7}
+
+This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The duty factor or part load fraction accounts for efficiency losses due to compressor cycling.
+
+\paragraph{Heating Coil Air Mass Flow Rate {[}kg/s{]}}\label{heating-coil-air-mass-flow-rate-kgs-1}
+
+The output variable is the average air mass flow rate going through the heat pump over the timestep being reported.
+
+\paragraph{Heating Coil Air Inlet Temperature {[}C{]}}\label{heating-coil-air-inlet-temperature-c-1}
+
+The output variable is the average entering air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Heating Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{heating-coil-air-inlet-humidity-ratio-kgwaterkgdryair-1}
+
+The output variable is the average entering air dry humidity ratio over the timestep being reported.
+
+\paragraph{Heating Coil Air Outlet Temperature {[}C{]}}\label{heating-coil-air-outlet-temperature-c-1}
+
+The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Heating Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{heating-coil-air-outlet-humidity-ratio-kgwaterkgdryair-1}
+
+The output variable is the average leaving air dry humidity ratio over the timestep being reported.
+
+\paragraph{Heating Coil Source Side Mass Flow Rate {[}kg/s{]}}\label{heating-coil-source-side-mass-flow-rate-kgs}
+
+The output variable is the average water mass flow rate going through the heat pump over the timestep being reported.
+
+\paragraph{Heating Coil Source Side Inlet Temperature {[}C{]}}\label{heating-coil-source-side-inlet-temperature-c}
+
+The output variable is the average entering water temperature over the timestep being reported.
+
+\paragraph{Heating Coil Source Side Outlet Temperature {[}C{]}}\label{heating-coil-source-side-outlet-temperature-c}
+
+The output variable is the average leaving water temperature over the timestep being reported.
+
+\paragraph{Heating Coil Electric Energy {[}J{]}}\label{heating-coil-electric-energy-j-5}
+
+The output variable is the total electric consumption of the heat pump in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Heating Energy {[}J{]}}\label{heating-coil-heating-energy-j-3}
+
+The output variable is the total cooling output of the coil in Joules over the timestep being reported. Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Heating Coil Source Side Heat Transfer Energy {[}J{]}}\label{heating-coil-source-side-heat-transfer-energy-j-2}
+
+The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported.
+
+\subsection{Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit}\label{coilheatingwatertoairheatpumpvariablespeedequationfit}
+
+The Variable-Speed Water-to-Air Heating Equation Fit Coil is a collection of performance curves that represent the heating coil at various speed levels. The performance curves should be generated from the heat pump Reference Unit catalog data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. The number of speed levels can range from 2 to 10. The heating coil has four node connections, i.e.~two air sides and two water sides. The user needs to specify a nominal speed level, at which the rated capacity, rated volumetric air and water flow rates are sized. The rated capacity, rated volumetric flow rates represent the real situation in the air and water loops, and are used to determine the flow rates at various speed levels in the parent objects, e.g.~AirLoopHVAC:UnitaryHeatPump:WaterToAir and ZoneHVAC:WaterToAirHeatPump. It shall be mentioned that the performance correction curves, i.e.~the temperature and flow fraction correction curves, should be normalized to the capacity and flow rates at each individual speed and at the rated operating conditions, similar to the performance curves used in the DX coils. On the other hand, the performance values at individual speed levels, e.g.~capacities, COPs and flow rates, should be given regarding a specific unit from the Reference Unit catalog data. In the following content, the statement started with Reference Unit means the actual Reference Unit catalog data. The rated conditions for obtaining the capacities and COPs are at indoor dry-bulb temperature of 21.1 ËšC (70 ËšF) and the source side entering water temperature of 21.1 ËšC (70 ËšF). Some equations are provided below to help explain the function of the various performance curves and data fields. For a detailed description of the algorithm and how the curves are used in the calculations, please see the Engineering Reference.
+
+\subsubsection{Inputs}\label{inputs-34}
+
+\paragraph{Field: Name}\label{field-name-33}
+
+This alpha field contains the identifying name for the variable speed heating coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-10}
+
+This alpha field contains the heating coil source side inlet node name.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-10}
+
+This alpha field contains the heating coil source side outlet node name.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-21}
+
+This alpha field contains the heating coil load side inlet node name.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-21}
+
+This alpha field contains the heating coil load side outlet node name.
+
+\paragraph{Field: Number of Speeds}\label{field-number-of-speeds-5}
+
+This numeric field contains the maximum number of speed levels that the module uses. The number of speeds, for which the user input the performance data and curves, has to be equal to or higher than the maximum number. The performance inputs at higher speeds are ignored.
+
+\paragraph{Field: Nominal Speed Level}\label{field-nominal-speed-level-3}
+
+This numeric field defines the nominal speed level, at which the rated capacity, rated air and water volumetric flow rates are correlated.
+
+\paragraph{Field: Gross Rated Heating Capacity at Selected Nominal Speed Level}\label{field-gross-rated-heating-capacity-at-selected-nominal-speed-level-1}
+
+This numeric field contains the gross rated capacity at the nominal speed level. This field is autosizable. The gross rated heating capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
+
+\begin{equation}
+CapacityScaleFactor = \frac{{GrossRatedHeatingCapacity}}{{ReferenceUnitCapacity@NominalSpeedLevel}}
+\end{equation}
+
+And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below,
+
+\begin{equation}
+  \begin{array}{l}
+    GrossRatedCapacity@SpeedLevel \left( x \right) = \\
+    \quad \quad \quad \quad CapacityScaleFactor \times ReferenceUnitCapacity@SpeedLevel(x)
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Rated Volumetric Air Flow Rate}\label{field-rated-volumetric-air-flow-rate-2}
+
+This numeric field contains the rated volumetric air flow rate on the load side of the heat pump corresponding to the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects. It is recommended that the ratio of the rated volumetric air flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
+
+\begin{equation}
+  \begin{array}{l}
+    AirFlowScaleFactor = \\
+    \quad \quad \quad \quad \frac{{RatedVolumetricAirFlowRate}}{{ReferenceUnitVolAirFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}
+  \end{array}
+\end{equation}
+
+And the volumetric air flow rates in the parent objects are calculated as below,
+
+\begin{equation}
+  \begin{array}{l}
+    LoopVolumetricAirFlowRate@SpeedLevel\left( x \right) = \\
+    \quad \quad \quad \quad AirFlowScaleFactor \\
+    \quad \quad \quad \quad  \times ReferenceUnitVolAirFlowRate@SpeedLevel(x) \\
+    \quad \quad \quad \quad  \times CapacityScaleFactor
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Rated Volumetric Water Flow Rate}\label{field-rated-volumetric-water-flow-rate-1}
+
+This numeric field contains the rated volumetric water flow rate on the source side of the heat pump at the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the water flow rates at other speed levels. It is recommended that the ratio of the rated volumetric water flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
+
+\begin{equation}
+WaterFlowScaleFactor = \frac{{RatedVolumetricWaterFlowRate}}{{ReferenceUnitVolWaterFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}
+\end{equation}
+
+And the required volumetric water flow rates in the water loop are calculated as below,
+
+\begin{equation}
+LoopVolumetricWaterFlowRate@SpeedLevel\left( x \right) = WaterFlowScaleFactor \times ReferenceUnitVolWaterFlowRate@SpeedLevel(x) \times CapacityScaleFactor
+\end{equation}
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-11}
+
+This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, heating load/steady-state heating capacity for Speed 1), in the case that the unit operates under the lowest speed, i.e.~on/off. The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep for Speed 1. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+PLF \textgreater{} = 0.7 and PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF \textless{} PLR, the runtime fraction of the coil is limited to 1.0. A typical part load fraction correlation would be:
+
+\begin{equation}
+PLF = 0.85 + 0.15 \times PLR
+\end{equation}
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+\begin{equation}
+PLF = 0.85 + 0.0 \times PLR
+\end{equation}
+
+\paragraph{Field Group: Rated Specification, Performance Curves, and Waste Heat Data}\label{field-group-rated-specification-performance-curves-and-waste-heat-data-2}
+
+The performance for each heating speed must be specified as shown below. They should be directly given from the Reference Unit data. All inputs for Speed 1 are required, followed by the optional inputs for other speeds.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Gross Rated Heating Capacity}\label{field-speed-x-reference-unit-gross-rated-heating-capacity-1}
+
+This numeric field defines the total, full load gross heating capacity in watts of the water-to-air heating coil unit at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0. Capacity should not account for the effect of supply air fan heat.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Gross Rated Heating COP}\label{field-speed-x-reference-unit-gross-rated-heating-cop-1}
+
+This numeric field defines the coefficient of performance (COP = gross heating capacity in watts divided by electrical power input in watts) of the heating coil unit at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here must be greater than 0. The input power includes power for the compressor(s) and accessories, but does not include the power consumption of the indoor supply air fan and water pump. The gross COP should not account for the supply air fan.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Rated Air Flow Rate}\label{field-speed-x-reference-unit-rated-air-flow-rate-3}
+
+This numeric field defines the volume air flow rate, in m\(^{3}\)per second, across the heating coil at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here should be directly from the Reference Unit data, corresponding to the given gross rated heating capacity and gross rated heating COP at the speed, as above.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Reference Unit Rated Water Flow Rate}\label{field-speed-x-reference-unit-rated-water-flow-rate-1}
+
+This numeric field defines the volume water flow rate, in m\(^{3}\)per second, flowing at the source side of the heating coil at rated conditions for Speed \textless{}x\textgreater{} operation. The value entered here should be directly from the Reference Unit data, corresponding to the given gross rated heating capacity and gross rated heating COP at the speed, as above.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Heating Capacity Function of Temperature Curve Name}\label{field-speed-x-heating-capacity-function-of-temperature-curve-name-2}
+
+This alpha field defines the name of a bi-quadratic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the total heating capacity as a function of the indoor dry-bulb and source side entering water temperature, from the Reference Unit. The output of this curve is multiplied by the gross rated heating capacity at the speed to give the gross total heating capacity at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or entering water temperature different from the rating point temperature). It should be noted that the curve is normalized to the heating capacity at Speed\textless{}x\textgreater{} from the Reference Unit data, and have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Heating Capacity Function of Air Flow Fraction Curve Name}\label{field-speed-x-heating-capacity-function-of-air-flow-fraction-curve-name-1}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the gross total heating capacity as a function of the ratio of actual air flow rate across the heating coil to the design air flow rate (i.e., fraction of full load flow), at Speed \textless{}x\textgreater{} from the Reference Unit data. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the design air flow rate at Speed \textless{}x\textgreater{}.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Heating Capacity Function of Water Flow Fraction Curve Name}\label{field-speed-x-heating-capacity-function-of-water-flow-fraction-curve-name}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of total heating capacity as a function of the ratio of actual water flow rate across the heating coil to the design water flow rate (i.e., fraction of full load flow), at Speed \textless{}x\textgreater{} from the Reference Unit data. The curve is normalized to have the value of 1.0 when the actual water flow rate equals the design air flow rate at Speed \textless{}x\textgreater{}.
+
+The actual total heating capacity at Speed \textless{}x\textgreater{}, considering variations in temperatures, air and water flow rates is calculated as below:
+
+\begin{equation}
+  \begin{array}{l}
+    ActualCapacity@SpeedLevel\left( x \right) = CapacityScaleFactor \\
+    \quad \quad \quad \quad \quad \times ReferenceUnitCapacity@SpeedLevel(x) \\
+    \quad \quad \quad \quad \quad \times TotCapTempModFac@SpeedLevel(x) \\
+    \quad \quad \quad \quad \quad \times TotCapAirFlowModFac@SpeedLevel(x) \\
+    \quad \quad \quad \quad \quad \times TotCapWaterFlowModFac@SpeedLevel(x)
+  \end{array}
+\end{equation}
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Temperature Curve Name}\label{field-speed-x-energy-input-ratio-function-of-temperature-curve-name-5}
+
+This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor air dry-bulb and entering water temperatures The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP at Speed \textless{}x\textgreater{} from the Reference Unit data) to give the EIR at specific temperature operating conditions (i.e., at an indoor air dry bulb temperature or entering water temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Air Flow Fraction Curve Name}\label{field-speed-x-energy-input-ratio-function-of-air-flow-fraction-curve-name-3}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the heating coil to the design air flow rate (i.e., fraction of full load flow, at Speed \textless{}x\textgreater{} from the Reference Unit data). The EIR is the inverse of the COP. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Energy Input Ratio Function of Water Flow Fraction Curve Name}\label{field-speed-x-energy-input-ratio-function-of-water-flow-fraction-curve-name-1}
+
+This alpha field defines the name of a quadratic or cubic performance curve for Speed \textless{}x\textgreater{} (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual water flow rate across the heating coil to the rated water flow rate (i.e., fraction of full load flow, at Speed \textless{}x\textgreater{} from the Reference Unit data). This curve is normalized to a value of 1.0 when the actual air flow rate equals the design air flow rate.
+
+The actual EIR at Speed \textless{}x\textgreater{}, considering variations in temperatures, air and water flow rates is calculated as below:
+
+\begin{equation}
+\begin{array}{l}
+ActualEIR@SpeedLevel \left( x \right) = \frac{{1.0}}{{ReferenceUnitCOP@SpeedLevel(x)}} \\
+\quad \quad \quad \quad \quad \quad \quad \quad \quad \times EIRTempModFac@SpeedLevel(x) \\
+\quad \quad \quad \quad \quad \quad \quad \quad \quad \times EIRAirFlowModFac@SpeedLevel(x) \\
+\quad \quad \quad \quad \quad \quad \quad \quad \quad \times EIRWaterFlowModFac@SpeedLevel(x)
+\end{array}
+\end{equation}
+
+And, the actual power consumption is calculated:
+
+\begin{equation}
+\begin{array}{l}
+ActualPower@SpeedLevel\left( x \right) = ActualCapacity@SpeedLevel\left( x \right) \\
+\quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \times ActualEIR@SpeedLevel\left( x \right)
+\end{array}
+\end{equation}
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Rated Waste Heat Fraction of Power Input}\label{field-speed-x-rated-waste-heat-fraction-of-power-input-2}
+
+The fraction of heat input to heating that is available as recoverable waste heat at full load and rated conditions for Speed \textless{}x\textgreater{} operation. The part of heat is not delivered to the indoor side.
+
+\paragraph{Field: Speed \textless{}x\textgreater{} Waste Heat Function of Temperature Curve Name}\label{field-speed-x-waste-heat-function-of-temperature-curve-name-3}
+
+The name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the waste heat recovery as a function of indoor dry-bulb temperature and the entering water temperature for Speed \textless{}x\textgreater{} from the Reference Unit data. The output of this curve is multiplied by the rated recoverable waste heat at specific temperature operating conditions (i.e., at temperatures different from the rating point). The curve is normalized to a value of 1.0 at the rating point.
+
+The actual recoverable waste heat at Speed \textless{}x\textgreater{} is calculated as below:
+
+\begin{equation}
+\begin{array}{l}
+ActualWasteHeat@SpeedLevel\left( x \right) = ActualPower@SpeedLevel\left( x \right) \\
+\quad \quad \quad \quad \quad \quad \times WasteHeatFrac@SpeedLevel(x) \\
+\quad \quad \quad \quad \quad \quad \times WasteHeatTempModFac@SpeedLevel(x)
+\end{array}
+\end{equation}
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit,
+  Sys 1 Heat Pump Heating Mode,                           !- Name
+  Sys 1 Water to Air Heat Pump Source Side2 Inlet Node,   !- Water Inlet Node Name
+  Sys 1 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
+  Sys 1 Heating Coil Air Inlet Node,                      !- Air Inlet Node Name
+  Sys 1 SuppHeating Coil Air Inlet Node,                  !- Air Outlet Node Name
+  10.0,                           !- Number of Speeds
+  10.0,                           !- Nominal Speed Level
+  Autosize,                       !- Rated Heating Capacity {W}
+  Autosize,                       !- Rated Air Flow Rate {m3/s}
+  Autosize,                       !- Rated Water Flow Rate {m3/s}
+  VS Energy Part Load Fraction 1, !- Energy part load fraction curve
+  1838.7,                         !- Speed 1 Reference Unit Gross Rated Heating Capacity
+  5.0,                            !- Speed 1 Reference Unit Gross Rated Heating COP
+  0.1661088,                      !- Speed 1 Reference Unit Rated Air Flow Rate
+  0.000381695,                    !- Speed 1 Reference Unit Rated Water Flow Rate
+  Heating VS Temp1 Test,          !- Speed 1 Heating Capacity Function of Temperature Curve Name
+  Heating VS AirFrac Test,        !- Speed 1 Heating Capacity Function of Air Flow Fraction Curve Name
+  Heating VS WaterFrac Test,      !- Speed 1 Heating Capacity Function of Water Flow Fraction Curve Name
+  EIRH VS Temp1 Test,             !- Speed 1 Energy Input Ratio Function of Temperature Curve Name
+  EIRH VS AirFrac Test,           !- Speed 1 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIRH VS WaterFrac Test,         !- Speed 1 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                            !- Speed 1 Waste Heat Fraction to Power Input
+  Heating wasteHeat VS Temp1 Test,!- Speed 1 Waste Heat Function of Temperature Curve Name
+  2295.5,                         !- Speed 2 Reference Unit Gross Rated Heating Capacity
+  5.0,                            !- Speed 2 Reference Unit Gross Rated Heating COP
+  0.179322,                       !- Speed 2 Reference Unit Rated air flow rate
+  0.000381695,                    !- Speed 2 Reference Unit Rated water flow rate
+  Heating VS Temp1 Test,          !- Speed 2 Heating Capacity Function of Temperature Curve Name
+  Heating VS AirFrac Test,        !- Speed 2 Heating Capacity Function of Air Flow Fraction Curve Name
+  Heating VS WaterFrac Test,      !- Speed 2 Heating Capacity Function of Water Flow Fraction Curve Name
+  EIRH VS Temp1 Test,             !- Speed 2 Energy Input Ratio Function of Temperature Curve Name
+  EIRH VS AirFrac Test,           !- Speed 2 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIRH VS WaterFrac Test,         !- Speed 2 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                            !- Speed 2 Waste Heat Fraction to Power Input
+  Heating wasteHeat VS Temp1 Test,!- Speed 2 Waste Heat Function of Temperature Curve Name
+  2751.3,                         !- Speed 3 Reference Unit Gross Rated Heating Capacity
+  5.0*,*                          !- Speed 3 Reference Unit Gross COP
+  0.1925352,                      !- Speed 3 Reference Unit Rated Air Flow Rate
+  0.000381695,                    !- Speed 3 Reference Unit Rated Water Flow Rate
+  Heating VS Temp1 Test,          !- Speed 3 Heating Capacity Function of Temperature Curve Name
+  Heating VS AirFrac Test,        !- Speed 3 Heating Capacity Function of Air Flow Fraction Curve Name
+  Heating VS WaterFrac Test,      !- Speed 3 Heating Capacity Function of Water Flow Fraction Curve Name
+  EIRH VS Temp1 Test,             !- Speed 3 Energy Input Ratio Function of Temperature Curve Name
+  EIRH VS AirFrac Test,           !- Speed 3 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIRH VS WaterFrac Test,         !- Speed 3 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                            !- Speed 3 Waste Heat fraction to power input
+  Heating wasteHeat VS Temp1 Test,!- Speed 3 Waste Heat Function of Temperature Curve Name
+  3659.6,                         !- Speed 4 Reference Unit Gross Rated Heating Capacity
+  5.0,                            !- Speed 4 Reference Unit Gross Rated Heating COP
+  0.2189616,                      !- Speed 4 Reference Unit Rated air flow rate
+  0.000381695,                    !- Speed 4 Reference Unit Rated water flow rate
+  Heating VS Temp1 Test,          !- Speed 4 Heating Capacity Function of Temperature Curve Name
+  Heating VS AirFrac Test,        !- Speed 4 Heating Capacity Function of Air Flow Fraction Curve Name
+  Heating VS WaterFrac Test,      !- Speed 4 Heating Capacity Function of Water Flow Fraction Curve Name
+  EIRH VS Temp1 Test,             !- Speed 4 Energy Input Ratio Function of Temperature Curve Name
+  EIRH VS AirFrac Test,           !- Speed 4 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIRH VS WaterFrac Test,         !- Speed 4 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                            !- Speed 4 Waste Heat fraction to power input
+  Heating wasteHeat VS Temp1 Test,!- Speed 4 Waste Heat Function of Temperature Curve Name
+  4563.7,                         !- Speed 5 Reference Unit Gross Rated Heating Capacity
+  5.0,                            !- Speed 5 Reference Unit Gross Rated Heating COP
+  0.245388,                       !- Speed 5 Reference Unit Rated air flow rate
+  0.000381695,                    !- Speed 5 Reference Unit Rated water flow rate
+  Heating VS Temp1 Test,          !- Speed 5 Heating Capacity Function of Temperature Curve Name
+  Heating VS AirFrac Test,        !- Speed 5 Heating Capacity Function of Air Flow Fraction Curve Name
+  Heating VS WaterFrac Test,      !- Speed 5 Heating Capacity Function of Water Flow Fraction Curve Name
+  EIRH VS Temp1 Test,             !- Speed 5 Energy Input Ratio Function of Temperature Curve Name
+  EIRH VS AirFrac Test,           !- Speed 5 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIRH VS WaterFrac Test,         !- Speed 5 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                            !- Speed 5 Waste Heat fraction to power input
+  Heating wasteHeat VS Temp1 Test,!- Speed 5 Waste Heat Function of Temperature Curve Name
+  5463.3,                         !- Speed 6 Reference Unit Gross Rated Heating Capacity
+  5.0,                            !- Speed 6 Reference Unit Gross Rated Heating COP
+  0.2718144,                      !- Speed 6 Reference Unit Rated air flow rate
+  0.000381695,                    !- Speed 6 Reference Unit Rated water flow rate
+  Heating VS Temp1 Test,          !- Speed 6 Heating Capacity Function of Temperature Curve Name
+  Heating VS AirFrac Test,        !- Speed 6 Heating Capacity Function of Air Flow Fraction Curve Name
+  Heating VS WaterFrac Test,      !- Speed 6 Heating Capacity Function of Water Flow Fraction Curve Name
+  EIRH VS Temp1 Test,             !- Speed 6 Energy Input Ratio Function of Temperature Curve Name
+  EIRH VS AirFrac Test,           !- Speed 6 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIRH VS WaterFrac Test,         !- Speed 6 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                            !- Speed 6 Waste Heat fraction to power input
+  Heating wasteHeat VS Temp1 Test,!- Speed 6 Waste Heat Function of Temperature Curve Name
+  6358.4,                         !- Speed 7 Reference Unit Gross Rated Heating Capacity
+  5.0,                            !- Speed 7 Reference Unit Gross Rated Heating COP
+  0.2982408,                      !- Speed 7 Reference Unit Rated air flow rate
+  0.000381695,                    !- Speed 7 Reference Unit Rated water flow rate
+  Heating VS Temp1 Test,          !- Speed 7 Heating Capacity Function of Temperature Curve Name
+  Heating VS AirFrac Test,        !- Speed 7 Heating Capacity Function of Air Flow Fraction Curve Name
+  Heating VS WaterFrac Test,      !- Speed 7 Heating Capacity Function of Water Flow Fraction Curve Name
+  EIRH VS Temp1 Test,             !- Speed 7 Energy Input Ratio Function of Temperature Curve Name
+  EIRH VS AirFrac Test,           !- Speed 7 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIRH VS WaterFrac Test,         !- Speed 7 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                            !- Speed 7 Waste Heat fraction to power input
+  Heating wasteHeat VS Temp1 Test,!- Speed 7 Waste Heat Function of Temperature Curve Name
+  7248.5,                         !- Speed 8 Reference Unit Gross Rated Heating Capacity
+  5.0,                            !- Speed 8 Reference Unit Gross Rated Heating COP
+  0.3246672,                      !- Speed 8 Reference Unit Rated air flow rate
+  0.000381695,                    !- Speed 8 Reference Unit Rated water flow rate
+  Heating VS Temp1 Test,          !- Speed 8 Heating Capacity Function of Temperature Curve Name
+  Heating VS AirFrac Test,        !- Speed 8 Heating Capacity Function of Air Flow Fraction Curve Name
+  Heating VS WaterFrac Test,      !- Speed 8 Heating Capacity Function of Water Flow Fraction Curve Name
+  EIRH VS Temp1 Test,             !- Speed 8 Energy Input Ratio Function of Temperature Curve Name
+  EIRH VS AirFrac Test,           !- Speed 8 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIRH VS WaterFrac Test,         !- Speed 8 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                            !- Speed 8 Waste Heat fraction to power input
+  Heating wasteHeat VS Temp1 Test,!- Speed 8 Waste Heat Function of Temperature Curve Name
+  8133.6,                         !- Speed 9 Reference Unit Gross Heating Capacity
+  5.0,                            !- Speed 9 Reference Unit Gross Rated Heating COP
+  0.3510936,                      !- Speed 9 Reference Unit Rated air flow rate
+  0.000381695,                    !- Speed 9 Reference Unit Rated water flow rate
+  Heating VS Temp1 Test,          !- Speed 9 Heating Capacity Function of Temperature Curve Name
+  Heating VS AirFrac Test,        !- Speed 9 Heating Capacity Function of Air Flow Fraction Curve Name
+  Heating VS WaterFrac Test,      !- Speed 9 Heating Capacity Function of Water Flow Fraction Curve Name
+  EIRH VS Temp1 Test,             !- Speed 9 Energy Input Ratio Function of Temperature Curve Name
+  EIRH VS AirFrac Test,           !- Speed 9 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIRH VS WaterFrac Test,         !- Speed 9 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                            !- Speed 9 Waste Heat fraction to power input
+  Heating wasteHeat VS Temp1 Test,!- Speed 9 Waste Heat Function of Temperature Curve Name
+  9013.2,                         !- Speed 10 Reference Unit Gross Rated Heating Capacity
+  5.0,                            !- Speed 10 Reference Unit Gross Rated Heating COP
+  0.37752,                        !- Speed 10 Reference Unit Rated air flow rate
+  0.000381695,                    !- Speed 10 Reference Unit Rated water flow rate
+  Heating VS Temp1 Test,          !- Speed 10 Heating Capacity Function of Temperature Curve Name
+  Heating VS AirFrac Test,        !- Speed 10 Heating Capacity Function of Air Flow Fraction Curve Name
+  Heating VS WaterFrac Test,      !- Speed 10 Heating Capacity Function of Water Flow Fraction Curve
+  EIRH VS Temp1 Test,             !- Speed 10 Energy Input Ratio Function of Temperature Curve Name
+  EIRH VS AirFrac Test,           !- Speed 10 Energy Input Ratio Function of Air Flow Fraction Curve Name
+  EIRH VS WaterFrac Test,         !- Speed 10 Energy Input Ratio Function of Water Flow Fraction Curve Name
+  0.1,                            !- Speed 10 Waste Heat fraction to power input
+  Heating wasteHeat VS Temp1 Test;!- Speed 10 Waste Heat Function of Temperature Curve Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-28}
+
+\begin{itemize}
+\item
+  HVAC, Average, Heating Coil Electric Power {[}W{]}
+\item
+  HVAC, Average, Heating Coil Heating Rate {[}W{]}
+\item
+  HVAC, Average, Heating Coil Sensible Heating Rate {[}W{]}
+\item
+  HVAC, Average, Heating Coil Source Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Average, Heating Coil Part Load Ratio
+\item
+  HVAC, Average, Heating Coil Runtime Fraction {[]}
+\item
+  HVAC, Average, Heating Coil Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Heating Coil Air Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Heating Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC, Average, Heating Coil Air Outlet Temperature {[}C{]}
+\item
+  HVAC, Average, Heating Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC, Average, Heating Coil Source Side Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Heating Coil Source Side Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Heating Coil Source Side Outlet Temperature {[}C{]}
+\item
+  HVAC, Average, Heating Coil Upper Speed Level {[]}
+\item
+  HVAC, Average, Heating Coil Neighboring Speed Levels Ratio {[]}
+\item
+  HVAC, Average, Heating Coil Recoverable Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Heating Coil Electric Energy {[}J{]}
+\item
+  HVAC, Sum, Heating Coil Heating Energy {[}J{]}
+\item
+  HVAC, Sum, Heating Coil Source Side Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Heating Coil Electric Power {[}W{]}}\label{heating-coil-electric-power-w-9}
+
+This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Heating Rate {[}W{]}}\label{heating-coil-heating-rate-w-4}
+
+The output variable is the average total heating capacity provide by the heat pump in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Sensible Heating Rate {[}W{]}}\label{heating-coil-sensible-heating-rate-w-2}
+
+The output variable is the average sensible heating capacity provide by the heat pump in Watts over the timestep being reported. For heating mode, the sensible capacity is equal to the total capacity.
+
+\paragraph{Heating Coil Source Side Heat Transfer Rate {[}W{]}}\label{heating-coil-source-side-heat-transfer-rate-w-2}
+
+The output variable is the average heat absorbed at the heat pump evaporator in Watts over the timestep being reported.
+
+\paragraph{\texorpdfstring{Heating Coil Part Load Ratio {[]}}{Heating Coil Part Load Ratio }}\label{heating-coil-part-load-ratio-2}
+
+This output variable is the ratio of the part-load capacity to the steady state capacity of the VSWatertoAirHP coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the VSWatertoAirHP coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
+
+\paragraph{\texorpdfstring{Heating Coil Runtime Fraction {[]}}{Heating Coil Runtime Fraction }}\label{heating-coil-runtime-fraction-8}
+
+This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The duty factor or part load fraction accounts for efficiency losses due to compressor cycling.
+
+\paragraph{Heating Coil Air Mass Flow Rate {[}kg/s{]}}\label{heating-coil-air-mass-flow-rate-kgs-2}
+
+The output variable is the average air mass flow rate going through the heat pump over the timestep being reported.
+
+\paragraph{Heating Coil Air Inlet Temperature {[}C{]}}\label{heating-coil-air-inlet-temperature-c-2}
+
+The output variable is the average entering air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Heating Coil Air Inlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{heating-coil-air-inlet-humidity-ratio-kgwaterkgdryair-2}
+
+The output variable is the average entering air dry humidity ratio over the timestep being reported.
+
+\paragraph{Heating Coil Air Outlet Temperature {[}C{]}}\label{heating-coil-air-outlet-temperature-c-2}
+
+The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
+
+\paragraph{Heating Coil Air Outlet Humidity Ratio {[}kgWater/kgDryAir{]}}\label{heating-coil-air-outlet-humidity-ratio-kgwaterkgdryair-2}
+
+The output variable is the average leaving air dry humidity ratio over the timestep being reported.
+
+\paragraph{Heating Coil Source Side Mass Flow Rate {[}kg/s{]}}\label{heating-coil-source-side-mass-flow-rate-kgs-1}
+
+The output variable is the average water mass flow rate going through the heat pump over the timestep being reported.
+
+\paragraph{Heating Coil Source Side Inlet Temperature {[}C{]}}\label{heating-coil-source-side-inlet-temperature-c-1}
+
+The output variable is the average entering water temperature over the timestep being reported.
+
+\paragraph{Heating Coil Source Side Outlet Temperature {[}C{]}}\label{heating-coil-source-side-outlet-temperature-c-1}
+
+The output variable is the average leaving water temperature over the timestep being reported.
+
+\paragraph{\texorpdfstring{Heating Coil Upper Speed Level {[]}}{Heating Coil Upper Speed Level }}\label{heating-coil-upper-speed-level-1}
+
+The output variable is the average upper speed level, for interpolating performances between two neighboring speed levels.
+
+\paragraph{\texorpdfstring{Heating Coil Neighboring Speed Levels Ratio {[]}}{Heating Coil Neighboring Speed Levels Ratio }}\label{heating-coil-neighboring-speed-levels-ratio-1}
+
+The output variable is the average speed ratio, for interpolating performances between two neighboring speed levels.
+
+\paragraph{Heating Coil Recoverable Heat Transfer Rate {[}W{]}}\label{heating-coil-recoverable-heat-transfer-rate-w}
+
+This output variable is the average recoverable waste heat rate of the heat pump in Watts over the timestep being reported.
+
+\paragraph{Heating Coil Electric Energy {[}J{]}}\label{heating-coil-electric-energy-j-6}
+
+The output variable is the total electric consumption of the heat pump in Joules over the timestep being reported.
+
+\paragraph{Heating Coil Heating Energy {[}J{]}}\label{heating-coil-heating-energy-j-4}
+
+The output variable is the total cooling output of the coil in Joules over the timestep being reported.
+
+\paragraph{Heating Coil Source Side Heat Transfer Energy {[}J{]}}\label{heating-coil-source-side-heat-transfer-energy-j-3}
+
+The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported.
+
+\subsection{Coil:Cooling:DX:SingleSpeed:ThermalStorage}\label{coilcoolingdxsinglespeedthermalstorage}
+
+This object models a special direct expansion (DX) cooling coil that includes methods of storing thermal energy within the cooling coil package. This packaged thermal storage cooling coil model includes all of the equipment needed to charge and discharge and the Thermal Energy Storage (TES) tank itself. This coil object is used with CoilSystem:Cooling:DX object and a constant volume supply fan, but all other subcomponents are contained within the package.
+
+Some types of devices may have a process air cooling section that actually has two coils, one an evaporator and the second some other kind of coil that cools by discharging the TES tank. There may also be two separate heat engines inside the package with two compressors. The model wraps these complexities inside of the model which considers just one process air cooling section that combines both types of coils and one heat rejection condenser section that rejects heat from both engines. The operating modes that are likely to have two heat engines offer dual sets of rating points and performance curves to model the energy and capacity implications separately.
+
+The model offers various modes of operation that can be controlled over time using either a schedule or EMS actuators. The user can choose which of the five operating modes are present in the device. Each of the modes has its own separate set of performance characteristics and curves and the model can change abruptly from one mode to the next. For example when using the schedule control, the TES coil can be put into Charge Only Mode for some number of hours at night, operated in Cooling Only Mode during the mild morning hours, and run in Discharge Only Mode during the hottest part of the day. Custom control routines can be programmed using EMS to obtain a dynamic, supervisory control algorithm.
+
+\begin{itemize}
+\item
+  Off Mode. This mode is always present. Although the coil will not do any cooling, the state of the TES tank is still modeled since it can continue to exchange heat with the surrounding ambient air.
+\item
+  Cooling Only Mode. This mode is where the coil cools air at the evaporator using a model that is very similar to the regular, single speed DX cooling coil. The same five performance curves are used to describe cooling capacity and electric power use. The sensible heat ratio is described using two performance curves in the same as is available for 100\% outdoor air coils. The TES tank is neither charged or discharged but it continues to exchange heat with the surrounding ambient air.
+\item
+  Cooling And Charge Mode. This mode is where the coil both cools air at the evaporator and cools the TES tank at the same time. The model supports separate performance characteristics when there two separate heat engines, one for evaporator cooling and one for charging the TES tank.
+\item
+  Cooling and Discharge Mode. This mode is where the coil cools process air and heat is rejected to both the condenser section and the TES tank at the same time. The model supports separate performance characteristics when there two separate heat engines, one for evaporator cooling and one for TES cooling.
+\item
+  Charge Only Mode. This mode is where the coil charges the TES tank but does not provide any cooling at the process air cooling section.
+\item
+  Discharge Only Mode. This mode is where the coil cools process air by discharging the TES tank.
+\end{itemize}
+
+This cooling coil can be autosized. The cooling capacity for the cooling only mode is sized to meet the air system s final design cooling capacity. The cooling capacity for the other modes, and the storage capacity, can all be scaled relative to that one capacity using sizing factors that can be input by the user.
+
+\subsubsection{Inputs}\label{inputs-35}
+
+\paragraph{Field: Name}\label{field-name-34}
+
+A unique name for this TES coil object, assigned by user.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-15}
+
+The name of a schedule that determines whether the TES coil is available for cooling during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during a given time period. A value less than or equal to 0 (usually 0 is used) denotes that unit must be in off mode. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Operating Mode Control Method}\label{field-operating-mode-control-method}
+
+This field determines how the TES coil is to be controlled in terms of which operating mode is in effect for a given time period. There are two choices, ScheduledModes or EMSControlled. Choosing ScheduledModes indicates that the operating mode is determined by the values in a schedule that is named in the following input field. Choosing EMSControlled indicates that the operating mode is determined by the state of an EMS actuator called Coil:Cooling:DX:SingleSpeed:ThermalStorage with the control type Operating Mode.
+
+\paragraph{Field: Operation Mode Control Schedule Name}\label{field-operation-mode-control-schedule-name}
+
+This field is used (and required) if the operating model control method is set to ScheduledModes in the previous input field. The control schedule consists of a series of integer values that indicate what mode the TES coil should operate in for a given time period. The values for various operating modes have been programmed to be as follows:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{-1}
+\item
+  Off Mode
+\item
+  Cooling Only Mode
+\item
+  Cooling And Charge Mode
+\item
+  Cooling And Discharge Mode
+\item
+  Charge Only Mode
+\item
+  Discharge Only Mode
+\end{enumerate}
+
+\paragraph{Field: Storage Type}\label{field-storage-type}
+
+This field is used to determine what type of material is used for thermal storage. There are two basic types of thermal storage material, fluid or ice. For fluid tanks, the material can be water or a user-defined fluid such as a glycol and the storage of thermal energy accompanies changes in the temperature of the fluid in the tank. For ice tanks, the material is water ice and the storage of thermal energy accompanies changes in the fraction of ice. This input field has three possible choices: \textbf{Water}, \textbf{UserDefinedFluidType}, Or \textbf{Ice}. Choose \textbf{Water} for a fluid tank TES based on water. Choose \textbf{UserDefinedFluidType} for a fluid tank TES based on custom or glycol type fluid. Choose \textbf{Ice} for ice-based TES tank.
+
+\paragraph{Field: User Defined Fluid Type}\label{field-user-defined-fluid-type}
+
+This field is used to declare what type of user defined fluid is contained in the TES tank. This input field is only used (and required) if the previous field is set to UserDefinedFluidType. Water, EthyleneGlycol, and PropoleneGlycol have fluid properties built-in to EnergyPlus. Using a FluidProperties:GlycolConcentration object allows specifying a mixture of water and a glycol and the name of one can be entered here. For other types of fluids, a complete set of fluid property data is needed, see FluidProperties:Name, FluidProperties:Temperature, etc.
+
+\paragraph{\texorpdfstring{Field: Fluid Storage Volume {[}m\(^{3}\){]}}{Field: Fluid Storage Volume {[}m\^{}\{3\}{]}}}\label{field-fluid-storage-volume-m3}
+
+This field is used to describe the size of fluid-based TES tank, in m\(^{3}\). The storage volume can be automatically calculated based on the cooling capacity and sizing factor.
+
+\paragraph{Field: Ice Storage Capacity {[}GJ{]}}\label{field-ice-storage-capacity-gj}
+
+This field is used to describe the size of ice-based TES tank, in GJ. The storage capacity can be automatically calculated based on the cooling capacity and a sizing factor.
+
+\paragraph{Field: Storage Capacity Sizing Factor {[}hr{]}}\label{field-storage-capacity-sizing-factor-hr}
+
+This field is used if one of the previous two fields is set to autocalculate. The value entered here is a time duration, in hours. This time period is used for calculating a storage capacity. The basic idea is that storage be sized such that the TES can provide cooling at rated capacity for this amount of time. The rated capacity used in the sizing calculation is the Discharge Only Mode Rated Storage Discharging Capacity unless the Discharge Only mode is not available in which case it is the Cooling Only Mode Rated Total Evaporator Cooling Capacity. This sizing factor approach allows scaling the storage size relative to the TES coil s capacity. The sizing factor is applied for an ice-based TES by simply multiplying the rated capacity by the time duration (converted to seconds). For fluid-based TES, a change in fluid temperature of 10 °C is assumed to calculate the tank volume.
+
+\paragraph{Field: Storage Tank Ambient Temperature Node Name}\label{field-storage-tank-ambient-temperature-node-name}
+
+This field is used to assign the environmental conditions surrounding the TES coil. The thermal storage tank exchanges heat with its surroundings and the boundary conditions for those surrounding are taken from this node named in this field. Typically this is the name of a node declared to be an outdoor air node. This field is required.
+
+\paragraph{Field: Storage Tank to Ambient U-value Times Area Heat Transfer Coefficient {[}W/K{]}}\label{field-storage-tank-to-ambient-u-value-times-area-heat-transfer-coefficient-wk}
+
+This field is used to characterize the rate at which heat is exchanged between the TES tank and the surrounding ambient conditions, in W/K. This is an overall UA value for the tank where the U-factor and surface area are combined into one coefficient. Heat loss or gain to the TES tank is modeled using \(\dot Q = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)\) . This field is required.
+
+\paragraph{Field: Fluid Storage Tank Rating Temperature {[}C{]}}\label{field-fluid-storage-tank-rating-temperature-c}
+
+This field is used to define what temperature is used for rating conditions when using a fluid storage tank. This field is only used for Storage Type of Water or UserDefinedFluidType. The temperature here is used for declaring the state of the TES fluid tank that corresponds to Rated conditions. The temperature entered here is used to define fluid properties and to characterize the performance curves that depend on the state of the TES.
+
+\paragraph{\texorpdfstring{Field: Rated Evaporator Air Flow Rate {[}m\(^{3}\)/s{]}}{Field: Rated Evaporator Air Flow Rate {[}m\^{}\{3\}/s{]}}}\label{field-rated-evaporator-air-flow-rate-m3s}
+
+This field is the air volume flow rate through the coil, in m\(^{3}\)/s, at rating conditions. This is the rated air flow rate through the evaporator (and any other air cooling devices that are in series with the main evaporator). The coil can be operated with a different flow rate than this rated flow rate and the performance of the unit scales accordingly using the curves that are of the type Function of Flow Fraction Curve. All of the other rated values for capacity, COP, and SHR values, for all the various modes, should be determined at the same air flow rate used here. This field can be autosized.
+
+\paragraph{Field: Evaporator Air Inlet Node Name}\label{field-evaporator-air-inlet-node-name-3}
+
+This field is the name of an HVAC system node that the coil draws in as its inlet air. This for the evaporator s connection to air system but it may include other air cooling devices that are in series with the evaporator and contained within the packaged TES coil. This node must be unique across the model. This field is required.
+
+\paragraph{Field: Evaporator Air Outlet Node Name}\label{field-evaporator-air-outlet-node-name-2}
+
+This field is the name of an HVAC system node that the coils sends its outlet air. This for the evaporator s connection to air system but it may include other air cooling devices that are in series with the evaporator and contained within the packaged TES coil. This node must be unique across the model. This field is required.
+
+\paragraph{Field: Cooling Only Mode Available}\label{field-cooling-only-mode-available}
+
+This field is used to indicate if the packaged TES coil includes a mode with only cooling and no equipment is interacting with TES tank to charge or discharge it. The choices are Yes or No. This field is required.
+
+\paragraph{Field: Cooling Only Mode Rated Total Evaporator Cooling Capacity {[}W{]}}\label{field-cooling-only-mode-rated-total-evaporator-cooling-capacity-w}
+
+This field is used to specify the total, full load cooling capacity (sensible plus latent), in Watts, of the TES coil at rated conditions, while operating in Cooling Only Mode. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb and air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, and the air flow rate specified in Rated Evaporator Air Flow Rate. Capacity should be gross (i.e.~supply air fan heat is NOT included). This total cooling capacity is a central value for TES coil in the sense that it is the basis for various autocalculated sizes for the rest of the model which can be scaled off of this one value. This field is required if Cooling Only Mode is available or if another operating mode s capacity, or storage capacity, will be autocalculated from this value. This field is autosizable.
+
+\paragraph{Field: Cooling Only Mode Rated Sensible Heat Ratio}\label{field-cooling-only-mode-rated-sensible-heat-ratio}
+
+This field is used to specify the sensible heat ratio (SHR) at rating conditions while operating in Cooling Only Mode. SHR is the sensible cooling capacity divided by the total (sensible plus latent) cooling capacity and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, and cooling coil air flow rate specified in Rated Evaporator Air Flow Rate. Both the sensible and total cooling capacities used to define the rated SHR should be gross and not include supply fan heat. The packaged TES coil model uses SHR curves to modify the rated SHR as conditions move away from the rating conditions. This field is only used if Cooling Only Mode is available. If this input is left blank, the default is 0.7.
+
+\paragraph{Field: Cooling Only Mode Rated COP}\label{field-cooling-only-mode-rated-cop}
+
+This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Cooling Only Mode. COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, and cooling coil air flow rate specified in Rated Evaporator Air Flow Rate. The electric input power includes power for the compressor(s), condenser fan(s), and internal controls but does not include the electric power for the supply fan (which is modeled separately in EnergyPlus). The total cooling power output is the same as the value for the Cooling Only Mode Rated Total Evaporator Cooling Capacity and is gross cooling without the fan heat. This field is only used if Cooling Only Mode is available. If this input is left blank, the default is 3.0.
+
+\paragraph{Field: Cooling Only Mode Total Evaporator Cooling Capacity Function of Temperature Curve Name}\label{field-cooling-only-mode-total-evaporator-cooling-capacity-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the condenser section. The performance curve can be any curve or table based on two independent variables, x and y, including: Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 °C and y = 35.0 °C. The result of the curve is multiplied by Cooling Only Mode Rated Total Evaporator Cooling Capacity to model capacity at temperatures away from the rating point. This field is required if Cooling Only Mode is available.
+
+\paragraph{Field: Cooling Only Mode Total Evaporator Cooling Capacity Function of Flow Fraction Curve Name}\label{field-cooling-only-mode-total-evaporator-cooling-capacity-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to model capacity at air flow rates away from the rating point. This field is required if Cooling Only Mode is available.
+
+\paragraph{Field: Cooling Only Mode Energy Input Ratio Function of Temperature Curve Name}\label{field-cooling-only-mode-energy-input-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the condenser section. The performance curve can be any curve or table based on two independent variables, x and y, including: Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 °C and y = 35.0 °C. The result of this curve is multiplied by the inverse of the Cooling Only Mode Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Cooling Only Mode is available.
+
+\paragraph{Field: Cooling Only Mode Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-cooling-only-mode-energy-input-ratio-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Cooling Only Mode Rated COP to model electric energy consumption at air flow rates away from the rating point. This field is required if Cooling Only Mode is available.
+
+\paragraph{Field: Cooling Only Mode Part Load Fraction Correlation Curve Name}\label{field-cooling-only-mode-part-load-fraction-correlation-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) as a function of the part load ratio (PLR). PLR is the ratio of current cooling load to the current cooling capacity. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is the part load fraction (PLF) and the runtime fraction of the coil is defined as PLR divided by PLF. The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling. This field is required if Cooling Only Mode is available.
+
+\paragraph{Field: Cooling Only Mode Sensible Heat Ratio Function of Temperature Curve Name}\label{field-cooling-only-mode-sensible-heat-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the evaporator section. The performance curve can be any curve or table based on two independent variables, x and y, including: Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the evaporator section. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 °C and y = 26.7 °C. The result of the curve is multiplied by the Cooling Only Mode Rated Sensible Heat Ratio to model the SHR at coil entering temperatures that differ from the rating point. This field is required if Cooling Only Mode is available.
+
+\paragraph{Field: Cooling Only Mode Sensible Heat Ratio Function of Flow Fraction Curve Name}\label{field-cooling-only-mode-sensible-heat-ratio-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling Only Mode Rated Sensible Heat Ratio to model the SHR at coil air flow rates that differ from the rating point. This field is required if Cooling Only Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Available}\label{field-cooling-and-charge-mode-available}
+
+This field is used to indicate if the packaged TES coil includes a mode with both cooling at the coil and charging of the TES tank at the same time. The choices are Yes or No. This field is required.
+
+\paragraph{Field: Cooling And Charge Mode Rated Total Evaporator Cooling Capacity {[}W{]}}\label{field-cooling-and-charge-mode-rated-total-evaporator-cooling-capacity-w}
+
+This field is used to specify the total, full load cooling capacity (sensible plus latent), in Watts, of the TES coil at rated conditions, while operating in Cooling And Charge Mode. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb and air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, the air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). Capacity should be gross (i.e.~supply air fan heat is NOT included). The Cooling and Charge Mode has two capacities, this first one is for cooling and would typically be for a heat engine operating between the condenser and the evaporator. This field is required if Cooling And Charge Mode is available.
+
+This field is autocalculatable. When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
+
+\paragraph{Field: Cooling And Charge Mode Capacity Sizing Factor}\label{field-cooling-and-charge-mode-capacity-sizing-factor}
+
+This field is used if the previous input field is set to autocalculate. This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Cooling and Charge Mode Rated Total Evaporator Cooling Capacity, in Watts. If this field is left blank the default values is 0.5.
+
+\paragraph{Field: Cooling And Charge Mode Rated Storage Charging Capacity {[}W{]}}\label{field-cooling-and-charge-mode-rated-storage-charging-capacity-w}
+
+This field is used to specify the total, full load charging capacity, in Watts, of the TES coil at rated conditions, while operating in Cooling And Charge Mode. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb and air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, the air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). Capacity should be net (i.e.~any ancillary equipment inside the package needed for charging is included). The Cooling and Charge Mode has two capacities, this second one is for charging and would typically be for a heat engine operating between the condenser and the TES tank. This field is required if Cooling And Charge Mode is available.
+
+This field is autocalculatable. When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
+
+\paragraph{Field: Cooling And Charge Mode Storage Capacity Sizing Factor}\label{field-cooling-and-charge-mode-storage-capacity-sizing-factor}
+
+This field is used if the previous input field is set to autocalculate. This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Cooling and Charge Mode Rated Storage Charging Capacity, in Watts. If this field is left blank the default values is 0.5.
+
+\paragraph{Field: Cooling And Charge Mode Rated Sensible Heat Ratio}\label{field-cooling-and-charge-mode-rated-sensible-heat-ratio}
+
+This field is used to specify the sensible heat ratio (SHR) at rating conditions while operating in Cooling And Charge Mode. SHR is the sensible cooling capacity divided by the total (sensible plus latent) cooling capacity and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, and cooling coil air flow rate specified in Rated Evaporator Air Flow Rate. Both the sensible and total cooling capacities used to define the rated SHR should be gross and not include supply fan heat. The packaged TES coil model uses SHR curves to modify the rated SHR as conditions move away from the rating conditions. This field is only used if Cooling And Charge Mode is available. If this input is left blank, the default is 0.7.
+
+\paragraph{Field: Cooling And Charge Mode Cooling Rated COP}\label{field-cooling-and-charge-mode-cooling-rated-cop}
+
+This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Cooling And Charge Mode to cool air at the evaporator. COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). The electric input power includes power for the compressor(s), condenser fan(s), and internal controls but does not include the electric power for the supply fan (which is modeled separately in EnergyPlus). The total cooling power output is the same as the value for the Cooling And Charge Mode Rated Total Evaporator Cooling Capacity and is gross cooling without the fan heat. The Cooling And Charge Mode has two COP values and this first COP is for cooling and would typically be for a heat engine operating between the condenser and the evaporator. This field is only used if Cooling And Charge Mode is available. If this input is left blank, the default is 3.0.
+
+\paragraph{Field: Cooling And Charge Mode Charging Rated COP}\label{field-cooling-and-charge-mode-charging-rated-cop}
+
+This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Cooling And Charge Mode to charge the TES. COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). The electric input power includes power for the compressor(s), condenser fan(s), and internal controls. The charging power output is the same as the value for the Cooling And Charge Mode Rated Storage Charging Capacity and is net charging including any internal equipment. The Cooling And Charge Mode has two COP values and this second COP is for charging and would typically be for a heat engine operating between the condenser and the TES tank. This field is only used if Cooling And Charge Mode is available. If this input is left blank, the default is 3.0.
+
+\paragraph{Field: Cooling And Charge Mode Total Evaporator Cooling Capacity Function of Temperature Curve Name}\label{field-cooling-and-charge-mode-total-evaporator-cooling-capacity-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 35.0 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by Cooling And Charge Mode Rated Total Evaporator Cooling Capacity to model capacity at temperatures away from the rating point. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Total Evaporator Cooling Capacity Function of Flow Fraction Curve Name}\label{field-cooling-and-charge-mode-total-evaporator-cooling-capacity-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling And Charge Mode Rated Total Evaporator Cooling Capacity to model capacity at air flow rates away from the rating point. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Evaporator Energy Input Ratio Function of Temperature Curve Name}\label{field-cooling-and-charge-mode-evaporator-energy-input-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for evaporator cooling as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 35.0 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The performance curve is normalized to have the value of 1.0 at the rating point. The result of this curve is multiplied by the inverse of the Cooling And Charge Mode Cooling Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Evaporator Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-cooling-and-charge-mode-evaporator-energy-input-ratio-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for evaporator cooling as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Cooling And Charge Mode Cooling Rated COP to model electric energy consumption at air flow rates away from the rating point. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Evaporator Part Load Fraction Correlation Curve Name}\label{field-cooling-and-charge-mode-evaporator-part-load-fraction-correlation-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) (for evaporator cooling) as a function of the part load ratio (PLR). PLR is the ratio of current cooling load to the current cooling capacity. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is the part load fraction (PLF) and the runtime fraction of the coil is defined as PLR divided by PLF. The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Storage Charge Capacity Function of Temperature Curve Name}\label{field-cooling-and-charge-mode-storage-charge-capacity-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the storage charging capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 35.0 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by Cooling And Charge Mode Rated Storage Charging Capacity to model capacity at temperatures away from the rating point. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Storage Charge Capacity Function of Total Evaporator PLR Curve Name}\label{field-cooling-and-charge-mode-storage-charge-capacity-function-of-total-evaporator-plr-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the storage charging capacity as a function of part load ratio (PLR) at the evaporator. PLR is the ratio of current evaporator cooling load to the current evaporator cooling capacity. This curve allows increasing the storage charging capacity when loads at the evaporator are low. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by Cooling And Charge Mode Rated Storage Charging Capacity to model capacity at evaporator PLR less than 1.0. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Storage Energy Input Ratio Function of Temperature Curve Name}\label{field-cooling-and-charge-mode-storage-energy-input-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for charging as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 35.0 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of this curve is multiplied by the inverse of the Cooling And Charge Mode Charging Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Storage Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-cooling-and-charge-mode-storage-energy-input-ratio-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for charging as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Cooling And Charge Mode Charging Rated COP to model electric energy consumption at air flow rates away from the rating point. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Storage Energy Part Load Fraction Correlation Curve Name}\label{field-cooling-and-charge-mode-storage-energy-part-load-fraction-correlation-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) (for storage charging) as a function of the part load ratio (PLR). PLR is the ratio of current cooling load to the current cooling capacity (at the evaporator). The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is the part load fraction (PLF) and the runtime fraction is defined as PLR divided by PLF. The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Sensible Heat Ratio Function of Temperature Curve Name}\label{field-cooling-and-charge-mode-sensible-heat-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of temperature and optionally state of TES tank. The user can enter the name of a curve or table object that has either two or three independent variables.
+
+For a curve or table with two independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the evaporator section. The performance curve can be any curve or table based on two independent variables, x and y, including: Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the evaporator section.
+
+For a curve or table with three independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the evaporator section and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x and y values for the curve are the same as for two independent variables while the z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types.
+
+The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 26.7 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by the Cooling And Charge Mode Rated Sensible Heat Ratio to model the SHR at coil entering temperatures that differ from the rating point. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Charge Mode Sensible Heat Ratio Function of Flow Fraction Curve Name}\label{field-cooling-and-charge-mode-sensible-heat-ratio-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling And Charge Mode Rated Sensible Heat Ratio to model the SHR at coil air flow rates that differ from the rating point. This field is required if Cooling And Charge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Available}\label{field-cooling-and-discharge-mode-available}
+
+This field is used to indicate if the packaged TES coil includes a mode with both cooling at the coil and discharging of the TES tank at the same time. The choices are Yes or No. This field is required.
+
+\paragraph{Field: Cooling And Discharge Mode Rated Total Evaporator Cooling Capacity {[}W{]}}\label{field-cooling-and-discharge-mode-rated-total-evaporator-cooling-capacity-w}
+
+This field is used to specify the total, full load cooling capacity (sensible plus latent), in Watts, of the TES evaporator coil at rated conditions, while operating in Cooling And Discharge Mode. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb and air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, the air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). Capacity should be gross (i.e.~supply air fan heat is NOT included). The Cooling and Discharge Mode has two capacities (and may have two separate cooling coils contained within), this first one is for Evaporator cooling and would typically be for a heat engine operating between the condenser and the evaporator. This field is required if Cooling And Discharge Mode is available.
+
+This field is autocalculatable. When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
+
+\paragraph{Field: Cooling And Discharge Mode Evaporator Capacity Sizing Factor}\label{field-cooling-and-discharge-mode-evaporator-capacity-sizing-factor}
+
+This field is used if the previous input field is set to autocalculate. This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Cooling and Discharge Mode Rated Total Evaporator Cooling Capacity, in Watts. If this field is left blank the default values is 1.0.
+
+\paragraph{Field: Cooling And Discharge Mode Rated Storage Discharging Capacity}\label{field-cooling-and-discharge-mode-rated-storage-discharging-capacity}
+
+This field is used to specify the total, full load discharging capacity, in Watts, of the TES coil at rated conditions, while operating in Cooling And Discharge Mode. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb and air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, the air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). Capacity should be net (i.e.~any ancillary equipment inside the package needed for discharging is included). The Cooling and Discharge Mode has two capacities, this second one is for discharging and would typically be for a heat transfer loop operating between the TES tank and a coil in series with the evaporator. This field is required if Cooling And Discharge Mode is available.
+
+This field is autocalculatable. When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
+
+\paragraph{Field: Cooling And Discharge Mode Storage Discharge Capacity Sizing Factor}\label{field-cooling-and-discharge-mode-storage-discharge-capacity-sizing-factor}
+
+This field is used if the previous input field is set to autocalculate. This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Cooling and Discharge Mode Rated Storage Discharging Capacity, in Watts. If this field is left blank the default value is 1.0.
+
+\paragraph{Field: Cooling And Discharge Mode Rated Sensible Heat Ratio}\label{field-cooling-and-discharge-mode-rated-sensible-heat-ratio}
+
+This field is used to specify the sensible heat ratio (SHR) at rating conditions while operating in Cooling And Discharge Mode. SHR is the sensible cooling capacity divided by the total (sensible plus latent) cooling capacity and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). Both the sensible and total cooling capacities used to define the rated SHR should be gross and not include supply fan heat. The packaged TES coil model uses SHR curves to modify the rated SHR as conditions move away from the rating conditions. Cooling and discharge mode may have two separate coils in series all contained within the package and this SHR should be for the combined performance of the entire package. This field is only used if Cooling And Discharge Mode is available. If this input is left blank, the default is 0.7.
+
+\paragraph{Field: Cooling And Discharge Mode Cooling Rated COP}\label{field-cooling-and-discharge-mode-cooling-rated-cop}
+
+This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Cooling And Discharge Mode to cool air at the evaporator. COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). The electric input power includes power for the compressor(s), condenser fan(s), and internal controls but does not include the electric power for the supply fan (which is modeled separately in EnergyPlus). The total cooling power output is the same as the value for the Cooling And Discharge Mode Rated Total Evaporator Cooling Capacity and is gross cooling without the fan heat. The Cooling And Discharge Mode has two COP values and this first COP is for evaporator cooling and would typically be for a heat engine operating between the condenser and the evaporator. This field is only used if Cooling And Discharge Mode is available. If this input is left blank, the default is 3.0.
+
+\paragraph{Field: Cooling And Discharge Mode Discharging Rated COP}\label{field-cooling-and-discharge-mode-discharging-rated-cop}
+
+This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Cooling And Discharge Mode to discharge the TES. COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). The electric input power includes power for the compressor or circulation pumps and internal controls. The discharging power output is the same as the value for the Cooling And Discharge Mode Rated Storage Discharging Capacity and is net discharging including any internal equipment. The Cooling And Discharge Mode has two COP values and this second COP is for discharging and would typically be for a heat transfer loop operating between the TES tank and a coil in series with the evaporator. This field is only used if Cooling And Discharge Mode is available. If this input is left blank, the default is 3.0.
+
+\paragraph{Field: Cooling And Discharge Mode Total Evaporator Cooling Capacity Function of Temperature Curve Name}\label{field-cooling-and-discharge-mode-total-evaporator-cooling-capacity-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 35.0 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by Cooling And Discharge Mode Rated Total Evaporator Cooling Capacity to model capacity at temperatures away from the rating point. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Total Evaporator Cooling Capacity Function of Flow Fraction Curve Name}\label{field-cooling-and-discharge-mode-total-evaporator-cooling-capacity-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling And Discharge Mode Rated Total Evaporator Cooling Capacity to model capacity at air flow rates away from the rating point. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Evaporator Energy Input Ratio Function of Temperature Curve Name}\label{field-cooling-and-discharge-mode-evaporator-energy-input-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for evaporator cooling as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 35.0 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of this curve is multiplied by the inverse of the Cooling And Discharge Mode Cooling Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Evaporator Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-cooling-and-discharge-mode-evaporator-energy-input-ratio-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for evaporator cooling as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Cooling And Discharge Mode Cooling Rated COP to model electric energy consumption at air flow rates away from the rating point. This field is required if Cooling And discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Evaporator Part Load Fraction Correlation Curve Name}\label{field-cooling-and-discharge-mode-evaporator-part-load-fraction-correlation-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) (for evaporator cooling) as a function of the part load ratio (PLR). PLR is the ratio of current cooling load to the current cooling capacity. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is the part load fraction (PLF) and the runtime fraction of the coil is defined as PLR divided by PLF. The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Storage Discharge Capacity Function of Temperature Curve Name}\label{field-cooling-and-discharge-mode-storage-discharge-capacity-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the storage discharging capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 35.0 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by Cooling And Discharge Mode Rated Storage Discharging Capacity to model capacity at temperatures away from the rating point. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Storage Discharge Capacity Function of Flow Fraction Curve Name}\label{field-cooling-and-discharge-mode-storage-discharge-capacity-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the storage discharge capacity as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling And Discharge Mode Rated Storage Discharging Capacity to model capacity at air flow rates away from the rating point. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Storage Discharge Capacity Function of Total Evaporator PLR Curve Name}\label{field-cooling-and-discharge-mode-storage-discharge-capacity-function-of-total-evaporator-plr-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the storage discharging capacity as a function of part load ratio (PLR) at the evaporator. PLR is the ratio of current evaporator cooling load to the current evaporator cooling capacity. This curve allows varying the storage discharging capacity based on loads at the evaporator. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by Cooling And Discharge Mode Rated Storage Discharging Capacity to model capacity at different evaporator PLR values. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Storage Energy Input Ratio Function of Temperature Curve Name}\label{field-cooling-and-discharge-mode-storage-energy-input-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for discharging as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 35.0 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of this curve is multiplied by the inverse of the Cooling And Discharge Mode Discharging Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Storage Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-cooling-and-discharge-mode-storage-energy-input-ratio-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for discharging as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Cooling And Discharge Mode Discharging Rated COP to model electric energy consumption at air flow rates away from the rating point. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Storage Energy Part Load Fraction Correlation Curve Name}\label{field-cooling-and-discharge-mode-storage-energy-part-load-fraction-correlation-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) (for storage discharging) as a function of the part load ratio (PLR). PLR is the ratio of current cooling load to the current cooling capacity (at the evaporator). The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is the part load fraction (PLF) and the runtime fraction is defined as PLR divided by PLF. The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Sensible Heat Ratio Function of Temperature Curve Name}\label{field-cooling-and-discharge-mode-sensible-heat-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of temperature and optionally state of TES tank. The user can enter the name of a curve or table object that has either two or three independent variables.
+
+For a curve or table with two independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the evaporator section. The performance curve can be any curve or table based on two independent variables, x and y, including: Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the evaporator section.
+
+For a curve or table with three independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the evaporator section and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x and y values for the curve are the same as for two independent variables while the z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types.
+
+The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 26.7 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by the Cooling And Discharge Mode Rated Sensible Heat Ratio to model the SHR at coil entering temperatures that differ from the rating point. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Cooling And Discharge Mode Sensible Heat Ratio Function of Flow Fraction Curve Name}\label{field-cooling-and-discharge-mode-sensible-heat-ratio-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling And Discharge Mode Rated Sensible Heat Ratio to model the SHR at coil air flow rates that differ from the rating point. This field is required if Cooling And Discharge Mode is available.
+
+\paragraph{Field: Charge Only Mode Available}\label{field-charge-only-mode-available}
+
+This field is used to indicate if the packaged TES coil includes a mode with only charging of the TES tank. The choices are Yes or No. This field is required.
+
+\paragraph{Field: Charge Only Mode Rated Storage Charging Capacity {[}W{]}}\label{field-charge-only-mode-rated-storage-charging-capacity-w}
+
+This field is used to specify the total, full load charging capacity, in Watts, of the TES coil at rated conditions, while operating in Charge Only Mode. The rating conditions are air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). Capacity should be net (i.e.~any ancillary equipment inside the package needed for charging is included). The Charge Only Mode capacity would typically be for a heat engine operating between the condenser and the TES tank. This field is required if Charge Only Mode is available.
+
+This field is autocalculatable. When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
+
+\paragraph{Field: Charge Only Mode Capacity Sizing Factor}\label{field-charge-only-mode-capacity-sizing-factor}
+
+This field is used if the previous input field is set to autocalculate. This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Charge Only Mode Rated Storage Charging Capacity, in Watts. If this field is left blank the default values is 1.0.
+
+\paragraph{Field: Charge Only Mode Charging Rated COP}\label{field-charge-only-mode-charging-rated-cop}
+
+This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Charge Only Mode to charge the TES. COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the outdoor condenser section at 35 °C drybulb and 23.9 °C wetbulb and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). The electric input power includes power for the compressor(s), condenser fan(s), and internal controls. The charging power output is the same as the value for the Charge Only Mode Rated Storage Charging Capacity and is net charging including any internal equipment. This field is only used if Charge Only Mode is available. If this input is left blank, the default is 3.0.
+
+\paragraph{Field: Charge Only Mode Storage Charge Capacity Function of Temperature Curve Name}\label{field-charge-only-mode-storage-charge-capacity-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the storage charging capacity as a function of (1) the drybulb temperature of the air entering the condenser section, and (2) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on two independent variables, x and y, including: Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear. The x values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The y values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 35.0 °C, and y = 0.5 for Ice storage type or y = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by Charge Only Mode Rated Storage Charging Capacity to model capacity at temperatures away from the rating point. This field is required if Charge Only Mode is available.
+
+\paragraph{Field: Charge Only Mode Storage Energy Input Ratio Function of Temperature Curve Name}\label{field-charge-only-mode-storage-energy-input-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for charging as a function of (1) the drybulb temperature of the air entering the condenser section, and (2) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on two independent variables, x and y, including: Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear. The x values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The y values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 35.0 °C, and y = 0.5 for Ice storage type or y = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of this curve is multiplied by the inverse of the Charge Only Mode Charging Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Charge Only Mode is available.
+
+\paragraph{Field: Discharge Only Mode Available}\label{field-discharge-only-mode-available}
+
+This field is used to indicate if the packaged TES coil includes a mode with only discharging of the TES tank. The choices are Yes or No. This field is required.
+
+\paragraph{Field: Discharge Only Mode Rated Storage Discharging Capacity {[}W{]}}\label{field-discharge-only-mode-rated-storage-discharging-capacity-w}
+
+This field is used to specify the total, full load discharging capacity, in Watts, of the TES coil at rated conditions, while operating in Discharge Only Mode. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, the air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). Capacity should be net (i.e.~any ancillary equipment inside the package needed for discharging is included) with regard to TES discharge, and gross with regard to supply fan heat. Discharge Only Mode would typically be for a heat transfer loop operating between the TES tank and a coil in series with the evaporator. This field is required if Discharge Only Mode is available.
+
+This field is autocalculatable. When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
+
+\paragraph{Field: Discharge Only Mode Capacity Sizing Factor}\label{field-discharge-only-mode-capacity-sizing-factor}
+
+This field is used if the previous input field is set to autocalculate. This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Discharge Only Mode Rated Storage Discharging Capacity, in Watts. If this field is left blank the default value is 1.0.
+
+\paragraph{Field: Discharge Only Mode Rated Sensible Heat Ratio}\label{field-discharge-only-mode-rated-sensible-heat-ratio}
+
+This field is used to specify the sensible heat ratio (SHR) at rating conditions while operating in Discharge Only Mode. SHR is the sensible cooling capacity divided by the total (sensible plus latent) cooling capacity and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). Both the sensible and total cooling capacities used to define the rated SHR should be gross and not include supply fan heat. The packaged TES coil model uses SHR curves to modify the rated SHR as conditions move away from the rating conditions. This field is only used if Discharge Only Mode is available. If this input is left blank, the default is 0.7.
+
+\paragraph{Field: Discharge Only Mode Rated COP}\label{field-discharge-only-mode-rated-cop}
+
+This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Discharge Only Mode to discharge the TES. COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 °C drybulb, 19.4 °C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type). The electric input power includes power for the compressor or circulation pumps and internal controls. The discharging power output is the same as the value for the Discharge Only Mode Rated Storage Discharging Capacity and is net discharging including any internal equipment. This field is only used if Discharge Only Mode is available. If this input is left blank, the default is 3.0.
+
+\paragraph{Field: Discharge Only Mode Storage Discharge Capacity Function of Temperature Curve Name}\label{field-discharge-only-mode-storage-discharge-capacity-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the storage discharging capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, and (2) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on two independent variables, x and y, including: Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 °C and y = 0.5 for Ice storage type or y = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by Discharge Only Mode Rated Storage Discharging Capacity to model capacity at temperatures away from the rating point. This field is required if Discharge Only Mode is available.
+
+\paragraph{Field: Discharge Only Mode Storage Discharge Capacity Function of Flow Fraction Curve Name}\label{field-discharge-only-mode-storage-discharge-capacity-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the storage discharge capacity as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling Discharge Only Mode Rated Storage Discharging Capacity to model capacity at air flow rates away from the rating point. This field is required if Discharge Only Mode is available.
+
+\paragraph{Field: Discharge Only Mode Energy Input Ratio Function of Temperature Curve Name}\label{field-discharge-only-mode-energy-input-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for discharging as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, and (2) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on two independent variables, x and y, including: Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 °C and y = 0.5 for Ice storage type or y = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of this curve is multiplied by the inverse of the Discharge Only Mode Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Discharge Only Mode is available.
+
+\paragraph{Field: Discharge Only Mode Energy Input Ratio Function of Flow Fraction Curve Name}\label{field-discharge-only-mode-energy-input-ratio-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for discharging as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Discharge Only Mode Rated COP to model electric energy consumption at air flow rates away from the rating point. This field is required if Discharge Only Mode is available.
+
+\paragraph{Field: Discharge Only Mode Part Load Fraction Correlation Curve Name}\label{field-discharge-only-mode-part-load-fraction-correlation-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) (for storage discharging) as a function of the part load ratio (PLR). PLR is the ratio of current cooling load to the current cooling capacity. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is the part load fraction (PLF) and the runtime fraction is defined as PLR divided by PLF. The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling. This field is required if Discharge Only Mode is available.
+
+\paragraph{Field: Discharge Only Mode Sensible Heat Ratio Function of Temperature Curve Name}\label{field-discharge-only-mode-sensible-heat-ratio-function-of-temperature-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of temperature and optionally state of TES tank. The user can enter the name of a curve or table object that has either two or three independent variables.
+
+For a curve or table with two independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the evaporator section. The performance curve can be any curve or table based on two independent variables, x and y, including: Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear. The x values for the performance curve are the wetbulb temperature of air entering the evaporator section. The y values for the performance curve are the drybulb temperature of air entering the evaporator section.
+
+For a curve or table with three independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the evaporator section and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including: Curve:Triquadratic and Table:MultiVariableLookup. The x and y values for the curve are the same as for two independent variables while the z values are the state of the TES tank which are the tank s temperature for water or fluid storage type or the storage fraction for ice storage types.
+
+The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 °C, y = 26.7 °C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by the Discharge Only Mode Rated Sensible Heat Ratio to model the SHR at coil entering temperatures that differ from the rating point. This field is required if Discharge Only Mode is available.
+
+\paragraph{Field: Discharge Only Mode Sensible Heat Ratio Function of Flow Fraction Curve Name}\label{field-discharge-only-mode-sensible-heat-ratio-function-of-flow-fraction-curve-name}
+
+This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Discharge Only Mode Rated Sensible Heat Ratio to model the SHR at coil air flow rates that differ from the rating point. This field is required if Discharge Only Mode is available.
+
+\paragraph{Field: Ancillary Electric Power {[}W{]}}\label{field-ancillary-electric-power-w}
+
+This field is the electric power level for miscellaneous ancillary controls and standby draws, in Watts. This power is not linked to any particular operating mode and will always be on, except when the device is scheduled to not be available by the Availability Schedule. This field is optional.
+
+\paragraph{Field: Cold Weather Operation Minimum Outdoor Air Temperature {[}C{]}}\label{field-cold-weather-operation-minimum-outdoor-air-temperature-c}
+
+This field is the outdoor temperature at which the device operates additional electric components to protect from cold weather, in Degrees Celsius. When the outdoor temperature is below this value, the power draw specified in the next field will be turned on. The outdoor temperature is obtained from the node specified in the input field called Storage Tank Ambient Temperature Node Name.
+
+\paragraph{Field: Cold Weather Operation Ancillary Power {[}W{]}}\label{field-cold-weather-operation-ancillary-power-w}
+
+This field is the electric power level for cold weather protection. Cold weather protection is in effect whenever the outdoor temperature is lower than the limit set in the previous field, except when the device is scheduled to not be available by the Availability Schedule.
+
+\paragraph{Field: Condenser Air Inlet Node Name}\label{field-condenser-air-inlet-node-name-5}
+
+This field is the name of system node that serves as the inlet to the condenser section of the packaged TES coil. This node is typically specified to be an outdoor air node. The conditions exposed to the condenser are obtained from this system node. This field is required.
+
+\paragraph{Field: Condenser Air Outlet Node Name}\label{field-condenser-air-outlet-node-name}
+
+This field is the name of system node that serves as the outlet to the condenser section of the packaged TES coil. This node is typically not connected to anything else. The conditions leaving the condenser are applied to this system node. This field is required.
+
+\paragraph{\texorpdfstring{Field: Condenser Design Air Flow Rate {[}m\(^{3}\)/s{]}}{Field: Condenser Design Air Flow Rate {[}m\^{}\{3\}/s{]}}}\label{field-condenser-design-air-flow-rate-m3s}
+
+This field is the rate of air flow through the condenser section, in m\(^{3}\)/s. The model assumes constant, single-speed condenser fans. The flow rate is not used to determine coil operation but is used to determine the conditions leaving the condenser section. This field is required, for both air-cooled and evaporatively-cooled condenser types.
+
+This field is autocalulatable. When autocalculated, the design flow rate is determined using the sizing factor in the following input field.
+
+\paragraph{Field: Condenser Air Flow Sizing Factor}\label{field-condenser-air-flow-sizing-factor}
+
+This field is used if the previous input field is set to autocalculate. This sizing factor is multiplied by the Rated Evaporator Air Flow Rate to obtain a scaled value for Condenser Design Air Flow Rate, in m\(^{3}\)/s. If this field is left blank the default value is 1.0.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-5}
+
+This field is the type of condenser used by the TES coil. There are two options, \textbf{AirCooled} or \textbf{EvaporativelyCooled}. The default is AirCooled. The next six put fields are used when the condenser section is evaporatively cooled.
+
+\paragraph{Field: Evaporative Condenser Effectiveness}\label{field-evaporative-condenser-effectiveness-2}
+
+This field is the wetbulb effectiveness for the evaporatively-cooled condenser. The effectiveness is used to model the temperature of air exposed to the condenser section as follows:
+
+\begin{equation}
+{T_{Cond\,\;inlet}} = \left( {{T_{wb,o}}} \right) + \left( {1 - EvapCondEffectiveness} \right)\left( {{T_{db,o}} - {T_{wb,o}}} \right)
+\end{equation}
+
+where
+
+\begin{lstlisting}
+       ${T_{cond\;inlet}}$ = the temperature of air entering the condenser section, in  &deg;C. This value will be used when evaluating performance curves that depend on the drybulb entering the condenser section.
+\end{lstlisting}
+
+\begin{lstlisting}
+       ${T_{wb,o}}$ = the wetbulb temperature of outdoor air, in  &deg;C
+\end{lstlisting}
+
+\begin{lstlisting}
+       ${T_{db,o}}$ = the drybulb temperature of outdoor air, in  &deg;C.
+\end{lstlisting}
+
+This field is required if the condenser type is set to EvaporativelyCooled. If the field is left blank then a default of 0.7 is used.
+
+\paragraph{Field: Evaporative Condenser Pump Rated Power Consumption {[}W{]}}\label{field-evaporative-condenser-pump-rated-power-consumption-w}
+
+This field is the rated power of the evaporative condenser water pump, in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default is zero, but this field is autosizable using a sizing factor of 0.004266 W of electricity per W of cooling. This field is only used when the condenser type is set to EvaporativelyCooled.
+
+\paragraph{Field: Basin Heater Capacity {[}W/K{]}}\label{field-basin-heater-capacity-wk}
+
+This input field is the capacity of the evaporative cooler water basin heater for freeze protection in Watts per Kelvin. This field is only used when the condenser type is set to EvaporativelyCooled. This field is used with the following field to determine the electricity consumption rate for freeze protection of the water in a basin needed for evaporative cooling. The basin heater electric power is equal to this field multiplied by the difference between the Basin Heater Setpoint Temperature and the outdoor drybulb temperature. The default is zero.
+
+\paragraph{Field: Basin Heater Setpoint Temperature {[}C{]}}\label{field-basin-heater-setpoint-temperature-c}
+
+This input field contains the setpoint temperature for basin heater operation, in °C. This field is only used when the condenser type is set to EvaporativelyCooled. The basin heater is active when the outdoor drybulb temperatures falls below this setpoint temperature. The default is 2.0 °C.
+
+\paragraph{Field: Basin Heater Availability Schedule Name}\label{field-basin-heater-availability-schedule-name}
+
+This alpha field contains the name of the basin heater operating schedule. This field is only used when the condenser type is set to EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates whenever the schedule is on and the outdoor air drybulb is lower than the setpoint temperature in the previous field. If the field is left blank, the basin heater is available to operate throughout the simulation.
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-5-000}
+
+This optional field is used to describe where the TES coil obtains water used for evaporative cooling of its condenser. If blank or omitted, then the unit will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, then the unit will attempt to obtain all its water from that tank. However, if the tank cannot provide all the water the condenser needs, then the unit will still operate and obtains the rest of the water it needs form the mains (referred to as Starved Water).
+
+\paragraph{Field: Condensate Collection Water Storage Tank Name}\label{field-condensate-collection-water-storage-tank-name-7}
+
+This optional field is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of a Water Storage Tank defined elsewhere and the condensate will be collected in that tank.
+
+\paragraph{Field: Storage Tank Plant Connection Inlet Node Name}\label{field-storage-tank-plant-connection-inlet-node-name}
+
+This is the name of a system node that is the inlet to the TES tank. This field is optional and is only used if the TES tank is directly connected to a plant loop.
+
+\paragraph{Field: Storage Tank Plant Connection Outlet Node Name}\label{field-storage-tank-plant-connection-outlet-node-name}
+
+This is the name of a system node that is the inlet to the TES tank. This field is optional and is only used if the TES tank is directly connected to a plant loop.
+
+\paragraph{Field: Storage Tank Plant Connection Design Flow Rate}\label{field-storage-tank-plant-connection-design-flow-rate}
+
+This field is the design flow rate for the plant connection to the TES tank, in m\(^{3}\)/s. The TES tank will make a passive request for this amount of flow. This field is required if the storage tank is connected to plant.
+
+\paragraph{Field: Storage Tank Plant Connection Heat Transfer Effectiveness}\label{field-storage-tank-plant-connection-heat-transfer-effectiveness}
+
+This field specifies the heat transfer effectiveness between the plant connection and the TES tank. If the effectiveness is set to 1 then ideal heat transfer occurs, as if the fluids were completely mixed and the fluid leaving the tank is the same temperature as the tank. If the effectiveness is less than 1.0, then the leaving fluid temperature approaches that of the tank as would be the case with a heat exchanger. If left blank, the default is 0.7.
+
+\paragraph{Field: Storage Tank Minimum Operating Limit Fluid Temperature {[}C{]}}\label{field-storage-tank-minimum-operating-limit-fluid-temperature-c}
+
+This field is used for fluid-based TES tank (Storage Type of Water or UserDefinedFluidType) to set the a lower limit on the operating temperatures, in Degrees Celsius. This value represents the temperature of the fluid-based TES tank when fully charged. This field is optional. When left blank, the model uses the lowest temperature for which fluid properties are defined.
+
+\paragraph{Field:: Storage Tank Maximum Operating Limit Fluid Temperature {[}C{]}}\label{field-storage-tank-maximum-operating-limit-fluid-temperature-c}
+
+This field is used for fluid-based TES tank (Storage Type of Water or UserDefinedFluidType) to set the an upper limit on the operating temperatures, in Degrees Celsius. This value represents the temperature of the fluid-based TES tank when fully discharged. This field is optional. When left blank, the model uses the highest temperature for which fluid properties are defined.
+
+\subsubsection{Outputs}\label{outputs-29}
+
+\begin{itemize}
+\item
+  HVAC,Average,Cooling Coil Operating Mode Index {[]}
+\item
+  HVAC,Average,Cooling Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Runtime Fraction {[]}
+\item
+  HVAC,Sum,Cooling Coil Cold Weather Protection Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Cold Weather Protection Electric Power {[}W{]}
+\item
+  HVAC,Average,Cooling Coil Thermal Storage Mechanical Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Thermal Storage Mechanical Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Thermal Storage Ambient Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Thermal Storage Ambient Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Ice Thermal Storage End Fraction {[]}
+\item
+  HVAC,Average,Cooling Coil Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Sum,Cooling Coil Evaporative Condenser Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Cooling Coil Evaporative Condenser Mains Supply Water Volume {[}m3{]}
+\item
+  HVAC,Average,Cooling Coil Evaporative Condenser Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Evaporative Condenser Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Basin Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Thermal Storage Plant Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Cooling Coil Thermal Storage Plant Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Cooling Coil Fluid Thermal Storage End Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Cooling Coil Operating Mode Index {[]}}{Cooling Coil Operating Mode Index }}\label{cooling-coil-operating-mode-index}
+
+This output variable reports the operating mode for the cooling coil. The numbers in this output are integer codes that correspond to the operating modes as described in the following table. These codes match the values used for input in schedules and EMS actuators to control operation.
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Code & Operating Mode \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Code & Operating Mode \tabularnewline
+\midrule
+\endhead
+
+0 & Off \tabularnewline
+1 & Cooling Only \tabularnewline
+2 & Cooling and Charge \tabularnewline
+3 & Cooling and Discharge \tabularnewline
+4 & Charge Only \tabularnewline
+5 & Discharge Only \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Cooling Coil Total Cooling Rate {[}W{]}}\label{cooling-coil-total-cooling-rate-w-10}
+
+This output is the total (sensible and latent) cooling rate of the coil in Watts.
+
+\paragraph{Cooling Coil Total Cooling Energy {[}J{]}}\label{cooling-coil-total-cooling-energy-j-10}
+
+This output is the total (sensible and latent) cooling energy transfer by the coil in Joules. This output is metered as EnergyTransfer for CoolingCoils.
+
+\paragraph{Cooling Coil Sensible Cooling Rate {[}W{]}}\label{cooling-coil-sensible-cooling-rate-w-10}
+
+This output is the moist air sensible cooling rate of the coil in Watts.
+
+\paragraph{Cooling Coil Sensible Cooling Energy {[}J{]}}\label{cooling-coil-sensible-cooling-energy-j-10}
+
+This output is the moist air sensible cooling energy transfer by the coil in Joules.
+
+\paragraph{Cooling Coil Latent Cooling Rate {[}W{]}}\label{cooling-coil-latent-cooling-rate-w-6}
+
+This output is the latent cooling rate of the coil in Watts.
+
+\paragraph{Cooling Coil Latent Cooling Energy {[}J{]}}\label{cooling-coil-latent-cooling-energy-j-8}
+
+This output is the latent cooling energy transfer by the coil in Joules.
+
+\paragraph{Cooling Coil Electric Power {[}W{]}}\label{cooling-coil-electric-power-w-4}
+
+This output is the electricity consumption rate, in Watts, of the compressor(s), pump(s), condenser fan(s) that are inside the package to drive heat transfer for the cooling coil. This does not include ancillary electrical consumption for such things as cold weather protection, off cycle ancillary power, or supply fans.
+
+\paragraph{Cooling Coil Electric Energy {[}J{]}}\label{cooling-coil-electric-energy-j-5}
+
+This output is the electricity consumption, in Joules, of the compressor(s), pump(s), condenser fan(s) that are inside the package to drive heat transfer for the cooling coil. This does not include ancillary electrical consumption for such things as cold weather protection, off cycle ancillary power, or supply fans.
+
+\paragraph{\texorpdfstring{Cooling Coil Runtime Fraction {[]}}{Cooling Coil Runtime Fraction }}\label{cooling-coil-runtime-fraction-8}
+
+This output is the runtime fraction of cooling coil.
+
+\paragraph{Cooling Coil Cold Weather Protection Electric Power {[}W{]}}\label{cooling-coil-cold-weather-protection-electric-power-w}
+
+\paragraph{Cooling Coil Cold Weather Protection Electric Energy {[}J{]}}\label{cooling-coil-cold-weather-protection-electric-energy-j}
+
+These are the power and energy outputs associated with Cold Weather Operation Ancillary Power, in Watts and Joules respectively.
+
+\paragraph{Cooling Coil Thermal Storage Mechanical Heat Transfer Rate {[}W{]}}\label{cooling-coil-thermal-storage-mechanical-heat-transfer-rate-w}
+
+\paragraph{Cooling Coil Thermal Storage Mechanical Heat Transfer Energy {[}J{]}}\label{cooling-coil-thermal-storage-mechanical-heat-transfer-energy-j}
+
+These are the power and energy outputs for the coil s heat exchange with the TES tank, in Watts and Joules respectively. The sign convection is that negative values are cooling the TES tank, or charging it, and positive values are heating the TES tank, or discharging. This heat transfer is driven by the mechanical systems used inside the package to charge or discharge the TES tank.
+
+\paragraph{Cooling Coil Thermal Storage Ambient Heat Transfer Rate {[}W{]}}\label{cooling-coil-thermal-storage-ambient-heat-transfer-rate-w}
+
+\paragraph{Cooling Coil Thermal Storage Ambient Heat Transfer Energy {[}J{]}}\label{cooling-coil-thermal-storage-ambient-heat-transfer-energy-j}
+
+These are the power and energy outputs for the TES tank s heat exchange with the surrounding ambient conditions, in Watts and Joules respectively. The sign convection is that negative values are cooling the TES tank, or charging it, and positive values are heating the TES tank, or discharging. This heat transfer is driven by the temperature difference between the media in the tank and the surrounding ambient and is governed by the UA factor.
+
+\paragraph{\texorpdfstring{Cooling Coil Ice Thermal Storage End Fraction {[]}}{Cooling Coil Ice Thermal Storage End Fraction }}\label{cooling-coil-ice-thermal-storage-end-fraction}
+
+This output is the state of the TES tank as fraction of the storage capacity. Because the tank storage model is dynamic, this value corresponds to the point in time right at the end of the timestep. This output variable is only available for a storage type of Ice.
+
+\paragraph{Cooling Coil Fluid Thermal Storage End Temperature {[}C{]}}\label{cooling-coil-fluid-thermal-storage-end-temperature-c}
+
+This output is the state of the TES tank as the temperature of the fluid in the tank, in °C. Because the tank storage model is dynamic, this value corresponds to the point in time right at the end of the timestep. This output variable is only available for a storage type of Water or UserDefinedFluidType.
+
+\paragraph{Cooling Coil Condenser Inlet Temperature {[}C{]}}\label{cooling-coil-condenser-inlet-temperature-c-2}
+
+This output is the inlet temperature entering the condenser section of an evaporatively cooled condenser, in °C. This temperature is for the air stream after the evaporative assist and before entering the condenser. This is the temperature used for condenser entering drybulb conditions when evaluating performance curves for evaporatively cooled condensers. This output is only available for evaporatively cooled condensers.
+
+\paragraph{\texorpdfstring{Cooling Coil Evaporative Condenser Water Volume {[}m\(^{3}\){]}}{Cooling Coil Evaporative Condenser Water Volume {[}m\^{}\{3\}{]}}}\label{cooling-coil-evaporative-condenser-water-volume-m3-2}
+
+This output is the amount of water used to evaporatively cool the condenser inlet air, in cubic meters. This output is only available for evaporatively cooled condensers.
+
+\paragraph{\texorpdfstring{Cooling Coil Evaporative Condenser Mains Supply Water Volume {[}m\(^{3}\){]}}{Cooling Coil Evaporative Condenser Mains Supply Water Volume {[}m\^{}\{3\}{]}}}\label{cooling-coil-evaporative-condenser-mains-supply-water-volume-m3-2}
+
+This output is the volume of water drawn from mains water service for the evaporatively cooled condenser. This output is only available for evaporatively cooled condensers.
+
+\paragraph{Cooling Coil Evaporative Condenser Pump Electric Power {[}W{]}}\label{cooling-coil-evaporative-condenser-pump-electric-power-w-1}
+
+This output is the average electricity consumption rate of the evaporative condenser water pump, in Watts. This output is only available for evaporatively cooled condensers.
+
+\paragraph{Cooling Coil Evaporative Condenser Pump Electric Energy {[}J{]}}\label{cooling-coil-evaporative-condenser-pump-electric-energy-j-2}
+
+This output is the electricity consumption of the evaporative condenser water pump, in Joules. This output is only available for evaporatively cooled condensers.
+
+\paragraph{Cooling Coil Basin Heater Electric Power {[}W{]}}\label{cooling-coil-basin-heater-electric-power-w-2}
+
+This output is the average electricity consumption rate of the basin heater, in Watts. This output is only available for evaporatively cooled condensers.
+
+\paragraph{Cooling Coil Basin Heater Electric Energy {[}J{]}}\label{cooling-coil-basin-heater-electric-energy-j-2}
+
+This output is the electricity consumption of the basin heater, in Joules. This output is only available for evaporatively cooled condensers.
+
+\paragraph{Cooling Coil Thermal Storage Plant Heat Transfer Rate {[}W{]}}\label{cooling-coil-thermal-storage-plant-heat-transfer-rate-w}
+
+\paragraph{Cooling Coil Thermal Storage Plant Heat Transfer Energy {[}J{]}}\label{cooling-coil-thermal-storage-plant-heat-transfer-energy-j}
+
+These are the power and energy outputs for the TES tank s heat exchange with the plant loop, in Watts and Joules respectively. This output is only available if the plant connection to the tank is used. The sign convection is that negative values are cooling the TES tank, or charging it, and positive values are heating the TES tank, or discharging. This heat transfer is driven by the temperature difference between the media in the tank and the plant loop fluid and is governed by the effectiveness and plant fluid mass flow rate.
+
+\subsection{Secondary Coils of DX System and Heat Pump}\label{secondary-coils-of-dx-system-and-heat-pump}
+
+Secondary Coils reject to or remove heat from a secondary zone as part of a DX system or an air-to-air heat pump. Secondary coil refers to a condenser of a DX system or a heat pump in cooling operating mode or an evaporator of a heat pump in heating mode. The secondary coil (e.g.~condenser) of DX system or heat pumps is commonly installed outdoor but when installed inside a zone either heat is dumped to or extracted from a secondary zone. A secondary zone is a conditioned or unconditioned zone where the secondary coil is installed. Secondary coils are not standalone DX coils but they are add-on features on existing DX coil objects. A secondary DX coil is modeled by specifying additional inputs in one of the following DX coil objects: Coil:Cooling:DX:SingleSpeed, Coil:Heating:DX:SingleSpeed, Coil:Cooling:DX:TwoSpeed, Coil:Cooling:DX:MultiSpeed, and Coil:Heating:DX:MultiSpeed. These additional inputs allow us to model the heat rejected or extracted by the secondary coil while the primary (active) coil is serving another controlled zone as shown in \protect\hyperlink{SecondaryCoilsFigure1}{Figure}. A secondary coil is not controlled directly but responds to the requirements of the primary DX coil. Heat is rejected or extracted depending on the primary DX coil operating modes. For instance, heat rejected to a secondary zone by a condenser of a DX system or a heat pump is considered as sensible only whereas the energy extracted from a secondary zone may contain sensible and latent components.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image903.png}
+\caption{}
+\end{figure}
+
+Figure: Schematic of DX System and heat pump in cooling operating mode
+
+Applications of this technology include: inter-zone heat pump in NTED (Dixon, 2010), and PTAC or PTHP serving Offices attached to a Warehouse, where the office partially or fully enclosed by the warehouse and the condenser is inside the Warehouse. Heat rejected or extracted by the secondary DX coil installed in a secondary zone is estimated from the DX coil models and it is considered as internal gains of the secondary zone. The capacity and electric power input of the DX system and heat pumps are determined from the operating modes of the primary cooling or heating DX coils. Calculation of a secondary coil tracks the operating modes of the primary DX coil serving the primary conditioned zone(s). Currently allowed DX coil models are single speed, two speed and multi speed DX Systems and Heat Pumps. To model secondary DX coils the condenser type should be AirCooled. There is no need to specify the condenser air inlet node. The model uses zone air node as the secondary coil air inlet node. And the fuel type in multispeed DX coils should Electricity.
+
+\textbf{Cooling Operating Mode}: the primary DX cooling coil of a DX system serving a primary zone is active and heat is rejected by the secondary coil (condenser) into a secondary zone. The secondary zone name is specified in DX cooling coil objects. This operating mode applies to a DX cooling system and cooling operating mode of air-to-air single and multi-speed heat pumps. Heat rejected by a secondary coil (condenser) calculated at each time step becomes internal gain of the secondary zone as shown in \protect\hyperlink{SecondaryCoilsFigure2}{Figure}. Whenever a secondary zone name is specified in DX cooling coil objects, the secondary DX coil model calculation is invoked. The only input field required to invoke the secondary DX coil in cooling operating model is to add a zone name in the input field \emph{Zone Name for Condenser Placement} in the DX cooling coil object.
+
+\subsubsection{Field: Zone Name for Condenser Placement}\label{field-zone-name-for-condenser-placement-3}
+
+This input field is name of a conditioned or unconditioned zone where the secondary coil (condenser) of DX system or a heat pump is to be placed. This is an optional input field specified only when user desires to reject the condenser heat into this zone. The heat rejected is modeled as sensible internal gain of a secondary zone.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image904.png}
+\caption{}
+\end{figure}
+
+Figure: Schematic of DX system and secondary coil in cooling mode
+
+Following is an example input for a single-speed cooling DX coil with secondary DX coil run option.
+
+\begin{lstlisting}
+
+Coil:Cooling:DX:SingleSpeed,
+  Heat Pump ACDXCoil 1,    !- Name
+  FanAndCoilAvailSched,    !- Availability Schedule Name
+  autosize,                !- Gross Rated Total Cooling Capacity {W}
+  autosize,                !- Gross Rated Sensible Heat Ratio
+  3.0,                     !- Gross Rated Cooling COP {W/W}
+  autosize,                !- Rated Air Flow Rate {m3/s}
+  ,                        !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
+  DX Cooling Coil Air Inlet Node,  !- Air Inlet Node Name
+  Heating Coil Air Inlet Node,  !- Air Outlet Node Name
+  HPACCoolCapFT,           !- Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFFF,          !- Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT,           !- Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFFF,          !- Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACCOOLPLFFPLR,         !- Part Load Fraction Correlation Curve Name
+  ,                        !- Nominal Time for Condensate Removal to Begin {s}
+  ,   !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
+  ,                        !- Maximum Cycling Rate {cycles/hr}
+  ,                        !- Latent Capacity Time Constant {s}
+  ,                        !- Condenser Air Inlet Node Name
+  AirCooled,               !- Condenser Type
+  ,                        !- Evaporative Condenser Effectiveness {dimensionless}
+  ,                        !- Evaporative Condenser Air Flow Rate {m3/s}
+  ,                        !- Evaporative Condenser Pump Rated Power Consumption {W}
+  ,                        !- Crankcase Heater Capacity {W}
+  ,                 !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
+  ,                        !- Supply Water Storage Tank Name
+  ,                        !- Condensate Collection Water Storage Tank Name
+  200,                     !- Basin Heater Capacity {W/K}
+  ,                        !- Basin Heater Setpoint Temperature
+  ,                        !- Basin Heater Operating Schedule Name
+  ,                        !- Sensible Heat Ratio Function of Temperature Curve Name
+  ,                        !- Sensible Heat Ratio Function of Flow Fraction Curve Name
+  NORTH ZONE;              !- Zone Name for Condenser Placement
+\end{lstlisting}
+
+Following is an example input for a two-speed cooling DX coil with secondary DX coil run option.
+
+\begin{lstlisting}
+
+Coil:Cooling:DX:TwoSpeed,
+  PSZ-AC_1:1_CoolC DXCoil, !- Name
+  FanAndCoilAvailSched,    !- Availability Schedule Name
+  AUTOSIZE,                !- High Speed Gross Rated Total Cooling Capacity {W}
+  AUTOSIZE,                !- High Speed Rated Sensible Heat Ratio
+  3.5,                     !- High Speed Gross Rated Cooling COP {W/W}
+  AUTOSIZE,                !- High Speed Rated Air Flow Rate {m3/s}
+  ,                        !- Unit Internal Static Air Pressure {Pa}
+  DX Cooling Coil Air Inlet Node,     !- Air Inlet Node Name
+  Heating Coil Air Inlet Node,        !- Air Outlet Node Name
+  Measured_CoolCStandard10Ton_CapFT,!- Total Cooling Capacity Function of Temperature Curve Name
+  Measured_CoolCStandard10Ton_CapFF,!- Total Cooling Capacity Function of Flow Fraction Curve Name
+  Measured_CoolCStandard10Ton_EIRFT,  !- Energy Input Ratio Function of Temperature Curve Name
+  Measured_CoolCStandard10Ton_EIRFFF, !- Energy Input Ratio Function of Flow Fraction Curve Name
+  No_PLR_Degredation,      !- Part Load Fraction Correlation Curve Name
+  AUTOSIZE,                !- Low Speed Gross Rated Total Cooling Capacity {W}
+  AUTOSIZE,                !- Low Speed Gross Rated Sensible Heat Ratio
+  3.3,                     !- Low Speed Gross Rated Cooling COP {W/W}
+  AUTOSIZE,                !- Low Speed Rated Air Flow Rate {m3/s}
+  MeasuredLowSpeedCoolCapLSFT,!- Low Speed Total Cooling Capacity Function of Temperature Curve Name
+  MeasuredLowSpeedCoolEIRLSFT,!- Low Speed Energy Input Ratio Function of Temperature Curve Name
+  ,                              !- Condenser Air Inlet Node Name
+  AirCooled,               !- Condenser Type
+  ,                        !- High Speed Evaporative Condenser Effectiveness {dimensionless}
+  ,                        !- High Speed Evaporative Condenser Air Flow Rate {m3/s}
+  ,                        !- High Speed Evaporative Condenser Pump Rated Power Consumption {W}
+  ,                        !- Low Speed Evaporative Condenser Effectiveness {dimensionless}
+  ,                        !- Low Speed Evaporative Condenser Air Flow Rate {m3/s}
+  ,                        !- Low Speed Evaporative Condenser Pump Rated Power Consumption {W}
+  ,                        !- Supply Water Storage Tank Name
+  ,                        !- Condensate Collection Water Storage Tank Name
+  ,                        !- Basin Heater Capacity {W/K}
+  ,                        !- Basin Heater Setpoint Temperature {C}
+  ,                        !- Basin Heater Operating Schedule Name
+  ,     !- Sensible Heat Ratio Function of Temperature Curve Name
+  ,     !- Sensible Heat Ratio Function of Flow Fraction Curve Name
+  ,     !- Low Speed Sensible Heat Ratio Function of Temperature Curve Name
+  ,     !- Low Speed Sensible Heat Ratio Function of Flow Fraction Curve Name
+  NORTH ZONE;              !- Zone Name for Condenser Placement
+\end{lstlisting}
+
+Following is an example input for a multi-speed cooling DX coil with secondary DX coil run option.
+
+\begin{lstlisting}
+
+Coil:Cooling:DX:MultiSpeed,
+  Heat Pump ACDXCoil 1,    !- Name
+  FanAndCoilAvailSched,    !- Availability Schedule Name
+  DX Cooling Coil Air Inlet Node,  !- Air Inlet Node Name
+  Heating Coil Air Inlet Node,  !- Air Outlet Node Name
+  Outdoor Condenser Air Node,  !- Condenser Air Inlet Node Name
+  AirCooled,               !- Condenser Type
+  ,                        !- Supply Water Storage Tank Name
+  ,                        !- Condensate Collection Water Storage Tank Name
+  No,                      !- Apply Part Load Fraction to Speeds Greater than 1
+  No,                      !- Apply Latent Degradation to Speeds Greater than 1
+  200.0,                   !- Crankcase Heater Capacity {W}
+  10.0,           !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
+  ,                        !- Basin Heater Capacity {W/K}
+  ,                        !- Basin Heater Setpoint Temperature {C}
+  ,                        !- Basin Heater Operating Schedule Name
+  Electricity,             !- Fuel Type
+  4,                       !- Number of Speeds
+  autosize,                !- Speed 1 Gross Rated Total Cooling Capacity {W}
+  autosize,                !- Speed 1 Gross Rated Sensible Heat Ratio
+  3.0,                     !- Speed 1 Gross Rated Cooling COP {W/W}
+  autosize,                !- Speed 1 Rated Air Flow Rate {m3/s}
+  453.3,                   !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
+  HPACCoolCapFT Speed 1,   !- Speed 1 Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFF Speed 1, !- Speed 1 Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT Speed 1,   !- Speed 1 Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFF Speed 1,   !- Speed 1 Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACCOOLPLFFPLR Speed 1, !- Speed 1 Part Load Fraction Correlation Curve Name
+  1000.0,                  !- Speed 1 Nominal Time for Condensate Removal to Begin {s}
+  1.5,  !- Speed 1 Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
+  3.0,                     !- Speed 1 Maximum Cycling Rate {cycles/hr}
+  45.0,                    !- Speed 1 Latent Capacity Time Constant {s}
+  0.2,                     !- Speed 1 Rated Waste Heat Fraction of Power Input {dimensionless}
+  HAPCCoolWHFT Speed 1,    !- Speed 1 Waste Heat Function of Temperature Curve Name
+  0.9,                     !- Speed 1 Evaporative Condenser Effectiveness {dimensionless}
+  autosize,                !- Speed 1 Evaporative Condenser Air Flow Rate {m3/s}
+  50,                      !- Speed 1 Rated Evaporative Condenser Pump Power Consumption {W}
+  autosize,                !- Speed 2 Gross Rated Total Cooling Capacity {W}
+  autosize,                !- Speed 2 Gross Rated Sensible Heat Ratio
+  3.0,                     !- Speed 2 Gross Rated Cooling COP {W/W}
+  autosize,                !- Speed 2 Rated Air Flow Rate {m3/s}
+  523.3,                   !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
+  HPACCoolCapFT Speed 2,   !- Speed 2 Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFF Speed 2, !- Speed 2 Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT Speed 2,   !- Speed 2 Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFF Speed 2,   !- Speed 2 Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACCOOLPLFFPLR Speed 1, !- Speed 2 Part Load Fraction Correlation Curve Name
+  1000.0,                  !- Speed 2 Nominal Time for Condensate Removal to Begin {s}
+  1.5,  !- Speed 2 Ratio of Initial Moisture Evaporation Rate and steady state Latent Capacity {dimensionless}
+  3.0,                     !- Speed 2 Maximum Cycling Rate {cycles/hr}
+  45.0,                    !- Speed 2 Latent Capacity Time Constant {s}
+  0.2,                     !- Speed 2 Rated Waste Heat Fraction of Power Input {dimensionless}
+  HAPCCoolWHFT Speed 2,    !- Speed 2 Waste Heat Function of Temperature Curve Name
+  0.9,                     !- Speed 2 Evaporative Condenser Effectiveness {dimensionless}
+  autosize,                !- Speed 2 Evaporative Condenser Air Flow Rate {m3/s}
+  60,                      !- Speed 2 Rated Evaporative Condenser Pump Power Consumption {W}
+  autosize,                !- Speed 3 Gross Rated Total Cooling Capacity {W}
+  autosize,                !- Speed 3 Gross Rated Sensible Heat Ratio
+  3.0,                     !- Speed 3 Gross Rated Cooling COP {W/W}
+  autosize,                !- Speed 3 Rated Air Flow Rate {m3/s}
+  573.3,                   !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
+  HPACCoolCapFT Speed 3,   !- Speed 3 Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFF Speed 3, !- Speed 3 Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT Speed 3,   !- Speed 3 Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFF Speed 3,   !- Speed 3 Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACCOOLPLFFPLR Speed 1, !- Speed 3 Part Load Fraction Correlation Curve Name
+  1000.0,                  !- Speed 3 Nominal Time for Condensate Removal to Begin {s}
+  1.5, !- Speed 3 Ratio of Initial Moisture Evaporation Rate and steady state Latent Capacity {dimensionless}
+  3.0,                     !- Speed 3 Maximum Cycling Rate {cycles/hr}
+  45.0,                    !- Speed 3 Latent Capacity Time Constant {s}
+  0.2,                     !- Speed 3 Rated Waste Heat Fraction of Power Input {dimensionless}
+  HAPCCoolWHFT Speed 3,    !- Speed 3 Waste Heat Function of Temperature Curve Name
+  0.9,                     !- Speed 3 Evaporative Condenser Effectiveness {dimensionless}
+  autosize,                !- Speed 3 Evaporative Condenser Air Flow Rate {m3/s}
+  80,                      !- Speed 3 Rated Evaporative Condenser Pump Power Consumption {W}
+  autosize,                !- Speed 4 Gross Rated Total Cooling Capacity {W}
+  autosize,                !- Speed 4 Gross Rated Sensible Heat Ratio
+  3.0,                     !- Speed 4 Gross Rated Cooling COP {W/W}
+  autosize,                !- Speed 4 Rated Air Flow Rate {m3/s}
+  673.3,                   !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
+  HPACCoolCapFT Speed 4,   !- Speed 4 Total Cooling Capacity Function of Temperature Curve Name
+  HPACCoolCapFF Speed 4, !- Speed 4 Total Cooling Capacity Function of Flow Fraction Curve Name
+  HPACCOOLEIRFT Speed 4,   !- Speed 4 Energy Input Ratio Function of Temperature Curve Name
+  HPACCOOLEIRFF Speed 4,   !- Speed 4 Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACCOOLPLFFPLR Speed 1, !- Speed 4 Part Load Fraction Correlation Curve Name
+  1000.0,                  !- Speed 4 Nominal Time for Condensate Removal to Begin {s}
+  1.5, !- Speed 4 Ratio of Initial Moisture Evaporation Rate and steady state Latent Capacity {dimensionless}
+  3.0,                     !- Speed 4 Maximum Cycling Rate {cycles/hr}
+  45.0,                    !- Speed 4 Latent Capacity Time Constant {s}
+  0.2,                     !- Speed 4 Rated Waste Heat Fraction of Power Input {dimensionless}
+  HAPCCoolWHFT Speed 4,    !- Speed 4 Waste Heat Function of Temperature Curve Name
+  0.9,                     !- Speed 4 Evaporative Condenser Effectiveness {dimensionless}
+  autosize,                !- Speed 4 Evaporative Condenser Air Flow Rate {m3/s}
+  100,                     !- Speed 4 Rated Evaporative Condenser Pump Power Consumption {W}
+  NORTH ZONE;              !- Zone Name for Condenser Placement
+\end{lstlisting}
+
+\textbf{Heating Operating Mode}: When a heat pump operates in heating mode then energy is extracted from the secondary zone. Total energy extracted from a secondary zone may contain sensible and latent components. The secondary coil (evaporator) model checks for the coil inlet and outlet air condition to determine if dehumidification has occurred. The sensible and latent split of the energy extracted is done using a user specified rated sensible heat ratio (SHR) and SHR modifier curves for temperature and secondary air flow fraction. If the coil operation is dry, then the SHR is set to 1.0. In addition, the model assumes that condensed water is drained to the outside. If defrosting operation is on, then the defrosting melts the frost and the liquid water from the collecting pan is drained to the outside. Thus, defrosting energy is not included in the zone energy balance. The six optioal input fields required in the DX heating coils are the following. The last five input fields are extensible depending on the speed of the heating DX coil:
+
+\subsubsection{Field: Zone Name for Evaporator Placement}\label{field-zone-name-for-evaporator-placement-2}
+
+This input field is name of a conditioned or unconditioned zone where the secondary coil (evaporator) of a heat pump is installed. This is an optional input field specified only when user desires to extract heat from the zone via secondary coil. Heat extracted is modeled as internal gain. If the primary DX system is a heat pump, then the zone name should be the same as the zone name specified for placing the secondary cooling DX coil.
+
+\subsubsection{\texorpdfstring{Field: Speed Secondary Coil Air Flow Rate}{Field: Speed  Secondary Coil Air Flow Rate}}\label{field-speed-secondary-coil-air-flow-rate}
+
+This input value is the secondary coil (evaporator) air flow rate when the heat pump is working in heating mode or the secondary coil (condenser) air flow rate when the heat pump is working in cooling mode. This input field is auto-sizable.
+
+\subsubsection{\texorpdfstring{Field: Speed Secondary Coil Fan Flow Scaling Factor}{Field: Speed  Secondary Coil Fan Flow Scaling Factor}}\label{field-speed-secondary-coil-fan-flow-scaling-factor}
+
+This input field is scaling factor for autosizing the secondary DX coil fan flow rate. The secondary air flow rate is determined by multiplying the primary DX coil rated air flow rate by the fan flow scaling factor. Default value is 1.25. If the secondary coil fan flow rate is not autosized, then the secondary coil fan flow scaling factor is set to 1.0.
+
+\subsubsection{\texorpdfstring{Field: Speed Nominal Sensible Heat Ratio of Secondary Coil}{Field: Speed  Nominal Sensible Heat Ratio of Secondary Coil}}\label{field-speed-nominal-sensible-heat-ratio-of-secondary-coil}
+
+This input value is the nominal sensible heat ratio used to split the heat extracted by a secondary DX coil (evaporator) of a heat pump into sensible and latent components. This is an optional input field. If this input field is left blank, then pure sensible internal heat gain is assumed, i.e., sensible heat ratio of 1.0.
+
+\subsubsection{\texorpdfstring{Field: Speed Sensible Heat Ratio Modifier Function of Temperature Curve Name}{Field: Speed  Sensible Heat Ratio Modifier Function of Temperature Curve Name}}\label{field-speed-sensible-heat-ratio-modifier-function-of-temperature-curve-name}
+
+This input field is name of sensible heat ratio modifier biquadratic curve. The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary zone air node wet-bulb temperature and the heating DX coil entering air dry-bulb temperature. This is an optional input field. If this input field is left blank, then the nominal sensible heat ratio modifier curve value for temperature is set to 1.0.
+
+\subsubsection{\texorpdfstring{Field: Speed Sensible Heat Ratio Modifier Function of Flow Fraction Curve Name}{Field: Speed  Sensible Heat Ratio Modifier Function of Flow Fraction Curve Name}}\label{field-speed-sensible-heat-ratio-modifier-function-of-flow-fraction-curve-name}
+
+This input field is name of sensible heat ratio modifier curve as function of secondary air flow fraction. The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary coil air flow fraction. This is an optional input field. If this input field is left blank, then the sensible heat ratio modifier curve value for flow fraction is set to 1.0.
+
+Following is an example input for a single-speed heating DX coil with secondary DX coil run option.
+
+\begin{lstlisting}
+
+Coil:Heating:DX:SingleSpeed,
+  Heat Pump DX Heating Coil 1,  !- Name
+  FanAndCoilAvailSched,    !- Availability Schedule Name
+  autosize,                !- Gross Rated Heating Capacity {W}
+  2.75,                    !- Gross Rated Heating COP {W/W}
+  autosize,                !- Rated Air Flow Rate {m3/s}
+  ,                        !- Rated Supply Fan Power Per Volume Flow Rate {W/(m3/s)}
+  Heating Coil Air Inlet Node,  !- Air Inlet Node Name
+  SuppHeating Coil Air Inlet Node,  !- Air Outlet Node Name
+  HPACHeatCapFT,           !- Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFFF,          !- Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT,           !- Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFFF,          !- Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACCOOLPLFFPLR,         !- Part Load Fraction Correlation Curve Name
+  ,                        !- Defrost Energy Input Ratio Function of Temperature Curve Name
+  -5.0,                     !- Minimum Outdoor Dry-Bulb Temperature for Compressor Operation {C}
+  ,                        !- Outdoor Dry-Bulb Temperature to Turn On Compressor {C}
+  5.0,                     !- Maximum Outdoor Dry-Bulb Temperature for Defrost Operation {C}
+  200.0,                   !- Crankcase Heater Capacity {W}
+  10.0,             !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
+  Resistive,               !- Defrost Strategy
+  TIMED,                   !- Defrost Control
+  0.166667,                !- Defrost Time Period Fraction
+  autosize,                !- Resistive Defrost Heater Capacity {W}
+  4,                       !- Region number for calculating HSPF
+  ,                        !- Evaporator Air Inlet Node Name
+  NORTH ZONE,              !- Zone Name for Evaporator Placement
+  autosize,                !- Secondary Coil Air Flow Rate
+  1.5,                     !- Secondary Coil Fan Flow Scaling Factor
+  0.9,                     !- Nominal Sensible Heat Ratio of Secondary Coil
+  DXSecondaryCoilSHRFT,    !- Sensible Heat Ratio Modifier Function of Temperature Curve Name
+  DXSecondaryCoilSHRFFF;   !- Sensible Heat Ratio Function of Flow Fraction Curve Name
+\end{lstlisting}
+
+Following is an example input for a multi-speed heating DX coil with secondary DX coil run option.
+
+\begin{lstlisting}
+
+Coil:Heating:DX:MultiSpeed,
+  Heat Pump DX Heating Coil 1,  !- Name
+  FanAndCoilAvailSched,    !- Availability Schedule Name
+  Heating Coil Air Inlet Node,  !- Air Inlet Node Name
+  SuppHeating Coil Air Inlet Node,  !- Air Outlet Node Name
+  -8.0,                    !- Minimum Outdoor Dry-Bulb Temperature for Compressor Operation {C}
+  -5.0,                    !- Outdoor Dry-Bulb Temperature to Turn On Compressor {C}
+  200.0,                   !- Crankcase Heater Capacity {W}
+  10.0,              !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
+  HPACDefrostCAPFT,        !- Defrost Energy Input Ratio Function of Temperature Curve Name
+  7.22,                    !- Maximum Outdoor Dry-Bulb Temperature for Defrost Operation {C}
+  ReverseCycle,            !- Defrost Strategy
+  timed,                   !- Defrost Control
+  0.058333,                !- Defrost Time Period Fraction
+  autosize,                !- Resistive Defrost Heater Capacity {W}
+  No,                      !- Apply Part Load Fraction to Speeds Greater than 1
+  Electricity,             !- Fuel Type
+  4,                       !- Region number for Calculating HSPF
+  4,                       !- Number of Speeds
+  autosize,                !- Speed 1 Gross Rated Heating Capacity {W}
+  2.75,                    !- Speed 1 Gross Rated Heating COP {W/W}
+  autosize,                !- Speed 1 Rated Air Flow Rate {m3/s}
+  345.0,                   !- Speed 1 Rated Supply Air Fan Power Per Volume Flow Rate {W/(m3/s)}
+  HPACHeatCapFT Speed 1,   !- Speed 1 Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFF Speed 1,   !- Speed 1 Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT Speed 1,   !- Speed 1 Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFF Speed 1,   !- Speed 1 Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACHeatPLFFPLR Speed 1, !- Speed 1 Part Load Fraction Correlation Curve Name
+  0.2,                     !- Speed 1 Rated Waste Heat Fraction of Power Input {dimensionless}
+  HAPCHeatWHFT Speed 1,    !- Speed 1 Waste Heat Function of Temperature Curve Name
+  autosize,                !- Speed 2 Gross Rated Heating Capacity {W}
+  2.75,                    !- Speed 2 Gross Rated Heating COP {W/W}
+  autosize,                !- Speed 2 Rated Air Flow Rate {m3/s}
+  425.0,                   !- Speed 2 Rated Supply Air Fan Power Per Volume Flow Rate {W/(m3/s)}
+  HPACHeatCapFT Speed 2,   !- Speed 2 Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFF Speed 2,   !- Speed 2 Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT Speed 2,   !- Speed 2 Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFF Speed 2,   !- Speed 2 Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACHeatPLFFPLR Speed 2, !- Speed 2 Part Load Fraction Correlation Curve Name
+  0.2,                     !- Speed 2 Rated Waste Heat Fraction of Power Input {dimensionless}
+  HAPCHeatWHFT Speed 2,    !- Speed 2 Waste Heat Function of Temperature Curve Name
+  autosize,                !- Speed 3 Gross Rated Heating Capacity {W}
+  2.75,                    !- Speed 3 Gross Rated Heating COP {W/W}
+  autosize,                !- Speed 3 Rated Air Flow Rate {m3/s}
+  525.0,                   !- Speed 3 Rated Supply Air Fan Power Per Volume Flow Rate {W/(m3/s)}
+  HPACHeatCapFT Speed 3,   !- Speed 3 Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFF Speed 3,   !- Speed 3 Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT Speed 3,   !- Speed 3 Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFF Speed 3,   !- Speed 3 Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACHeatPLFFPLR Speed 3, !- Speed 3 Part Load Fraction Correlation Curve Name
+  0.2,                     !- Speed 3 Rated Waste Heat Fraction of Power Input {dimensionless}
+  HAPCHeatWHFT Speed 3,    !- Speed 3 Waste Heat Function of Temperature Curve Name
+  autosize,                !- Speed 4 Gross Rated Heating Capacity {W}
+  2.75,                    !- Speed 4 Gross Rated Heating COP {W/W}
+  autosize,                !- Speed 4 Rated Air Flow Rate {m3/s}
+  673.0,                   !- Speed 4 Rated Supply Air Fan Power Per Volume Flow Rate {W/(m3/s)}
+  HPACHeatCapFT Speed 4,   !- Speed 4 Heating Capacity Function of Temperature Curve Name
+  HPACHeatCapFF Speed 4,   !- Speed 4 Heating Capacity Function of Flow Fraction Curve Name
+  HPACHeatEIRFT Speed 4,   !- Speed 4 Energy Input Ratio Function of Temperature Curve Name
+  HPACHeatEIRFF Speed 4,   !- Speed 4 Energy Input Ratio Function of Flow Fraction Curve Name
+  HPACHeatPLFFPLR Speed 4, !- Speed 4 Part Load Fraction Correlation Curve Name
+  0.2,                     !- Speed 4 Rated Waste Heat Fraction of Power Input {dimensionless}
+  HAPCHeatWHFT Speed 4,    !- Speed 4 Waste Heat Function of Temperature Curve Name
+  NORTH ZONE,              !- Zone Name for Evaporator Placement
+  autosize,                !- Speed 1 Secondary Coil Air Flow Rate
+  1.5,                     !- Speed 1 Secondary Coil Fan Flow Scaling Factor
+  0.9,                     !- Speed 1 Nominal Sensible Heat Ratio of Secondary Coil
+  DXSecondaryCoilSHRFT,!- Speed 1 Sensible Heat Ratio Modifier Function of Temperature Curve Name
+  DXSecondaryCoilSHRFFF,   !- Speed 1 Sensible Heat Ratio Function of Flow Fraction Curve Name
+  autosize,                !- Speed 2 Secondary Coil Air Flow Rate
+  1.5,                     !- Speed 2 Secondary Coil Fan Flow Scaling Factor
+  0.9,                     !- Speed 2 Nominal Sensible Heat Ratio of Secondary Coil
+  DXSecondaryCoilSHRFT,!- Speed 2 Sensible Heat Ratio Modifier Function of Temperature Curve Name
+  DXSecondaryCoilSHRFFF,   !- Speed 2 Sensible Heat Ratio Function of Flow Fraction Curve Name
+  autosize,                !- Speed 3 Secondary Coil Air Flow Rate
+  1.5,                     !- Speed 3 Secondary Coil Fan Flow Scaling Factor
+  0.9,                     !- Speed 3 Nominal Sensible Heat Ratio of Secondary Coil
+  DXSecondaryCoilSHRFT,!- Speed 3 Sensible Heat Ratio Modifier Function of Temperature Curve Name
+  DXSecondaryCoilSHRFFF,   !- Speed 3 Sensible Heat Ratio Function of Flow Fraction Curve Name
+  autosize,                !- Speed 4 Secondary Coil Air Flow Rate
+  1.5,                     !- Speed 4 Secondary Coil Fan Flow Scaling Factor
+  0.9,                     !- Speed 4 Nominal Sensible Heat Ratio of Secondary Coil
+  DXSecondaryCoilSHRFT,!- Speed 4 Sensible Heat Ratio Modifier Function of Temperature Curve Name
+  DXSecondaryCoilSHRFFF;   !- Speed 4 Sensible Heat Ratio Function of Flow Fraction Curve Name
+\end{lstlisting}
+
+\subsection{Secondary DX Coil Output}\label{secondary-dx-coil-output}
+
+\begin{itemize}
+\item
+  HVAC, Average, Secondary Coil Heat Rejection Rate {[}W{]}
+\item
+  HVAC, Average, Secondary Coil Total Heat Removal Rate {[}W{]}
+\item
+  HVAC, Average, Secondary Coil Sensible Heat Removal Rate {[}W{]}
+\item
+  HVAC, Average, Secondary Coil Latent Heat Removal Rate {[}W{]}
+\item
+  HVAC, Average, Secondary Coil Sensible Heat Ratio {[]}
+\item
+  HVAC, Average, Secondary Coil Compressor Part Load Ratio {[]}
+\end{itemize}
+
+\subsubsection{Secondary Coil Heat Rejection Rate {[}W{]}}\label{secondary-coil-heat-rejection-rate-w}
+
+This is the sensible heat rejected to a zone by a secondary DX coil (condenser) in Watts. This is sum of the total cooling rate of a DX cooling coil and cooling electric power of the primary DX coil. This heat is applied as an internal gain to the secondary zone where the condenser is installed.
+
+\subsubsection{Secondary Coil Total Heat Removal Rate {[}W{]}}\label{secondary-coil-total-heat-removal-rate-w}
+
+This is the total energy removed from a a zone by a secondary DX coil (evaporator) in Watts. This is the total heating rate of the primary DX cooling coil minus the heating electric power of the primary DX coil. This heat is extracted from the secondary zone when the heat pump is operating in heating mode. The negative sign indicate that heat is removed from the zone.
+
+\subsubsection{Secondary Coil Sensible Heat Removal Rate {[}W{]}}\label{secondary-coil-sensible-heat-removal-rate-w}
+
+This is the sensible heat removed from a a zone by a secondary DX coil (evaporator) in Watts. This is determined by multiplying the total heat removed with sensible heat ratio of the secondary coil. This heat is extracted from the secondary zone when the heat pump is operating in heating mode. The negative sign indicate that sensible heat is removed from the zone.
+
+\subsubsection{Secondary Coil Latent Heat Removal Rate {[}W{]}}\label{secondary-coil-latent-heat-removal-rate-w}
+
+This is the latent heat removed from a a zone by a secondary DX coil (evaporator) in Watts. This is the difference between the total heat removal rate and the sensible heat remobal rate of the secondary coil. This heat is extracted from the secondary zone when the heat pump is operating in heating mode. The negative sign indicate that moisture is removed from the zone.
+
+\subsubsection{\texorpdfstring{Secondary Coil Sensible Heat Ratio {[]}}{Secondary Coil Sensible Heat Ratio }}\label{secondary-coil-sensible-heat-ratio}
+
+This is the operating sensible heat ratio the secondary DX coil (condenser) when the heat pump is operating in heating mode.
+
+\subsubsection{\texorpdfstring{Secondary Coil Compressor Part Load Ratio {[]}}{Secondary Coil Compressor Part Load Ratio }}\label{secondary-coil-compressor-part-load-ratio}
+
+This is the compressor part load ratio when the heat pump is operating in heating mode and the secondary coil is extracting heat from a zone where the coil is installed. The secondary coil DX coil compressor part load ratio can be different from the primary DX coil compressor part load ratio in that the later may include the defrosting load.
+
+Reference: Dixon, Erin Elizabeth, ``Energy Model Development and Heating Energy Investigation of the Nested Thermal Envelope Design (NTED (tm))'' (2010). Theses and dissertations. Paper 974.
diff --git a/doc/input-output-reference/src/overview/group-humidifiers.tex b/doc/input-output-reference/src/overview/group-humidifiers.tex
new file mode 100644
index 00000000000..8ac8277b1fb
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-humidifiers.tex
@@ -0,0 +1,285 @@
+\section{Group -- Humidifiers}\label{group-humidifiers}
+
+\subsection{Humidifier:Steam:Electric}\label{humidifiersteamelectric}
+
+The electric steam humidifier is a component that represents an electrically heated, self contained steam humidifier. The component uses electrical energy to convert ordinary tap water to steam which it then injects into the supply air stream by means of a blower fan. The actual unit might be an electrode-type humidifier or a resistance-type humidifier.
+
+The humidifier model includes local control of the humidifier unit to meet a humidity ratio setpoint on its air outlet node. A set point manager is needed to put a setpoint on the exit node but no other local controllers are needed. The humidifier will add moisture to meet the humidity ratio setpoint.
+
+\subsubsection{Inputs}\label{inputs-023}
+
+\paragraph{Field: Name}\label{field-name-022}
+
+A unique user assigned name for a particular humidifier unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-010}
+
+The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Rated Capacity}\label{field-rated-capacity-000}
+
+The nominal full output water addition rate of the unit in m\(^{3}\)/sec of water at 5.05 C. This field is autosizable.
+
+\paragraph{Field: Rated Power}\label{field-rated-power-000}
+
+The nominal full output power consumption of the unit in watts, exclusive of the blower fan power consumption and any standby power. This field can be autosized. When it is autosized, its calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from the a reference temperature of liquid water at 20 °C to a saturated steam at 100 °C.
+
+\paragraph{Field: Rated Fan Power}\label{field-rated-fan-power}
+
+The nominal full output power consumption of the blower fan in watts.
+
+\paragraph{Field: Standby Power}\label{field-standby-power-000}
+
+The standby power consumption in watts. This amount of power will be consumed whenever the unit is available (as defined by the availability schedule).
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-004}
+
+The name of the HVAC system node from which the unit draws inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-004}
+
+The name of the HVAC system node to which the unit sends its outlet air.
+
+\paragraph{Field: Water Storage Tank Name}\label{field-water-storage-tank-name}
+
+This field is optional. If left blank or omitted, then the humidifier obtains its water directly from the mains water. If the name of a Water Storage Tank is specified, then the humidifier will try to obtain its water from that tank. If the tank can t provide all the water then the rest will be drawn from the mains and the humidifier will still operate.
+
+An IDF example:
+
+\begin{lstlisting}
+
+Humidifier:Steam:Electric,
+  Humidifier 1,                   !- Name
+  FanAndCoilAvailSched,   !- Availability Schedule Name
+  0.00000379,                       !- Rated Capacity {m3/s}
+  10200.,                               !- Rated Power {W}
+  27.,                                     !- Rated Fan Power {W}
+  2.,                                       !- Standby Power {W}
+  Cooling Coil Air Outlet Node, !- Air Inlet Node Name
+  Air Loop Outlet Node;   !- Air Outlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-016}
+
+\begin{itemize}
+\item
+  HVAC,Average,Humidifier Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Humidifier Water Volume{[}m3{]}
+\item
+  HVAC,Average,Humidifier Electric Power{[}W{]}
+\item
+  HVAC,Sum,Humidifier Electric Energy {[}J{]}
+\item
+  Zone,Meter,Humidifier:Water {[}m3{]}
+\item
+  Zone,Meter,Humidifier:Electricity {[}J{]}
+\item
+  HVAC,Average,Humidifier Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Humidifier Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Average,Humidifier Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Humidifier Starved Storage Tank Water Volume {[}m3{]}
+\item
+  Zone,Meter,Humidifier:MainsWater {[}m3{]}
+\item
+  HVAC,Sum,Humidifier Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Humidifier Water Volume Flow Rate {[}m3/s{]}}\label{humidifier-water-volume-flow-rate-m3s}
+
+This field reports the water consumption rate of the steam humidifier in cubic meters of water per second.
+
+\paragraph{Humidifier Water Volume{[}m3{]}}\label{humidifier-water-volumem3}
+
+This ouput is the cubic meters of water consumed by the steam humidifier over the timestep being reported.
+
+\paragraph{Humidifier Electric Power{[}W{]}}\label{humidifier-electric-powerw}
+
+This output is the electricity consumption rate in Watts of the steam humidifier.
+
+\paragraph{Humidifier Electric Energy {[}J{]}}\label{humidifier-electric-energy-j}
+
+This is the electricity consumption in Joules of the steam humidifier over the timestep being reported.
+
+\paragraph{Humidifier:Water {[}m3{]}}\label{humidifierwater-m3}
+
+This meter output contains the sum of the water consumed (in cubic neters of water during the report timestep) by all the steam humidifiers at the HVAC level in the simulation.
+
+\paragraph{Humidifier:Electricity {[}J{]}}\label{humidifierelectricity-j}
+
+This meter output contains the sum of the electricity consumed (in Joules during the report timestep) by all the steam humidifiers at the HVAC level in the simulation.
+
+\paragraph{Humidifier Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{humidifier-storage-tank-water-volume-flow-rate-m3s}
+
+\paragraph{Humidifier Storage Tank Water Volume {[}m3{]}}\label{humidifier-storage-tank-water-volume-m3}
+
+These outputs contain the rate and volume of water obtained from water storage tank. These are only present if the humidifier is connected to a Water Storage Tank for its water supply.
+
+\paragraph{Humidifier Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{humidifier-starved-storage-tank-water-volume-flow-rate-m3s}
+
+\paragraph{Humidifier Starved Storage Tank Water Volume {[}m3{]}}\label{humidifier-starved-storage-tank-water-volume-m3}
+
+These outputs contain the rate and volume of water that could not be obtained from the water storage tank. The component will still operate as if it did get all the water with the balance obtained directly from the mains
+
+\paragraph{Humidifier Mains Water Volume {[}m3{]}}\label{humidifier-mains-water-volume-m3}
+
+This output contains the volume of water obtained from the mains.
+
+\subsection{Humidifier:Steam:Gas}\label{humidifiersteamgas}
+
+The gas fired steam humidifier is a component that represents a gas fired self-contained steam humidifier. The component uses gas fired energy to convert ordinary tap water to steam which it then blows or injects into the supply air stream. Blower fan may not be required depending on how the dry steam is delivered into the supply air stream. The humidifier model includes local control of the humidifier unit to meet a humidity ratio setpoint on its air outlet node of the unit. A humidity set point manager is needed to put a setpoint on the outlet node but no other local controllers are needed. The humidifier either blows or injects dry steam to meet the humidity ratio setpoint requirement. If the Rated Gas Use Rate input field is not autosized, the thermal efficiency input specified will be ignored and ovverriden by a thermal efficiency value determined from user specified Rated Gas Use Rate, rated capacity (m3/s) and design conditions for sizing calculation.
+
+\subsubsection{Inputs}\label{inputs-1-021}
+
+\paragraph{Field: Name}\label{field-name-1-020}
+
+A unique user assigned name for a particular humidifier unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-008}
+
+The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Rated Capacity}\label{field-rated-capacity-1}
+
+The nominal full capacity water addition rate in m3/s of water at 5.05 C.
+
+\paragraph{Field: Rated Gas Use Rate \{W\}}\label{field-rated-gas-use-rate-w}
+
+The nominal gas use rate in Watts. This input field can be autosized. When this input field is autosized, it is calculated from the rated capacity in kg/s, the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20 °C to a saturated steam at 100 °C and user specified thermal efficiency. If this input field is hardsized and the Inlet Water Temperature Option input field is selected as FixedInletWaterTemperature, then the thermal efficiency input field will not be used in the calculation or else if the Inlet Water Temperature Option input selected is VariableInletWaterTemperature, then the user specified thermal efficiency value will be overridden using internally calculated efficiency from the capacity, rated gas use rate and design condition.
+
+\paragraph{Field: Thermal Efficiency}\label{field-thermal-efficiency}
+
+The thermal efficiency of the gas fired humidifier. The thermal efficiency is based on the higher heating value of the fuel. The default value is 0.8. If Rated Gas Use Rate in the field above is not autosized and the Inlet Water Temperature Option input field selected is FixedInletWaterTemperature, then the thermal efficiency specified will be ignored in the calculation, or else if the Inlet Water Temperature Option input field is specified as VariableInletWaterTemperature, then the user specified thermal efficiency value will be overridden using internally calculated matching the capacity, rated gas use rate specified and design condition defined for sizing calculation.
+
+\paragraph{Field: Thermal Efficiency Modifier Curve Name}\label{field-thermal-efficiency-modifier-curve-name}
+
+This is thermal efficiency modifier curve name of unit. This curve is normalized, i.e., the curve output value at rated condition is 1.0. If this input field is blank, then constant efficiency value specified in the input field above will be used. Allowed thermal efficiency modifier curve types are linear, quadratic, or cubic. These curves are solely a function of part load ratio.
+
+\paragraph{Field: Rated Fan Power}\label{field-rated-fan-power-1}
+
+The nominal full capacity electric power input to the blower fan in Watts. If no blower fan is required to inject the dry steam to the supply air stream, then this input field is set to zero.
+
+\paragraph{Field: Auxiliary Electric Power}\label{field-auxiliary-electric-power}
+
+The auxiliary electric power input in watts. This amount of power will be consumed whenever the unit is available (as defined by the availability schedule). This electric power is used for control purpose only.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-1-004}
+
+The name of the HVAC system node from which the unit draws inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-1-003}
+
+The name of the HVAC system node to which the unit sends its outlet air.
+
+\paragraph{Field: Water Storage Tank Name}\label{field-water-storage-tank-name-1}
+
+This field is optional. If left blank or omitted, then the humidifier obtains its water directly from the mains water. If the name of a Water Storage Tank is specified, then the humidifier will try to obtain its water from that tank. If the tank can t provide all the water then the rest will be drawn from the mains and the humidifier will still operate.
+
+\paragraph{Field: Inlet Water Temperature Option}\label{field-inlet-water-temperature-option}
+
+This field is a key/choice field that tells which humidifier water inlet temperature to use: fixed inlet temperature or variable water inlet temperature that depends on the source. Currently allowed water sources are main water or water storage tank in water use objects. The key/choice are: FixedInletWaterTemperature, with this choice, the gas fired humidifier will use a fixed 20C water inlet temperature. VariableInletWaterTemperature, with this choice, the gas fired humidifier will use water inlet temperature that depends on the source temperature. If a water use storage tank name is specified, then the gas humidifier water inlet temperature will be the storage water temperature, or else it uses water main temperature. The default main water temperature is 10 °C. If left blank or omitted, then the humidifier assumes fixed inlet water temperature of 20 °C.
+
+An IDF example:
+
+\begin{lstlisting}
+
+Humidifier:Steam:Gas,
+  Main Gas Humidifier,!- Name
+  ALWAYS_ON,          !- Availability Schedule Name
+  4.00E-5,            !- Rated Capacity {m3/s}
+  104000,             !- Rated Gas Use Rate {W}
+  1.0,                !- Thermal Efficiency {-} 
+  ,                   !- Thermal Efficiency Modifier Curve Name
+  0,                  !- Rated Fan Power {W}
+  0,                  !- Auxiliary Electric Power {W}
+  Mixed Air Node 1,   !- Air Inlet Node Name
+  Main Humidifier Outlet Node,  !- Air Outlet Node Name
+  ;                   !- Water Storage Tank Name
+\end{lstlisting}
+
+Steam Gas Humidifier Outputs
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Humidifier Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Humidifier Water Volume{[}m3{]}
+\item
+  HVAC,Average,Humidifier Gas Use Rate{[}W{]}
+\item
+  HVAC,Sum,Humidifier Gas Use Energy {[}J{]}
+\item
+  HVAC,Average,Humidifier Auxiliary Electric Power{[}W{]}
+\item
+  HVAC,Sum,Humidifier Auxiliary Electric Energy {[}J{]}
+\item
+  HVAC,Meter,Humidifier:Water {[}m3{]}
+\item
+  HVAC,Meter,Humidifier:Gas {[}J{]}
+\item
+  HVAC,Meter,Humidifier:Electricity {[}J{]}
+\item
+  HVAC,Average,Humidifier Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Humidifier Storage Tank Water Volume {[}m3{]}
+\item
+  HVAC,Average,Humidifier Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Humidifier Starved Storage Tank Water Volume {[}m3{]}
+\item
+  Zone,Meter,Humidifier:MainsWater {[}m3{]}
+\item
+  HVAC,Sum,Humidifier Mains Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Humidifier Water Volume Flow Rate {[}m3/s{]}}\label{humidifier-water-volume-flow-rate-m3s-1}
+
+This field reports the water consumption rate of the steam humidifier in cubic meters of water per second.
+
+\paragraph{Humidifier Water Volume {[}m3{]}}\label{humidifier-water-volume-m3}
+
+This output is the cubic meters of water consumed by the steam humidifier over the timestep being reported.
+
+\paragraph{Humidifier Gas Use Rate {[}W{]}}\label{humidifier-gas-use-rate-w}
+
+This output is the gas use rate of the gas fired steam humidifier in Watts.
+
+\paragraph{Humidifier Gas Use Energy {[}J{]}}\label{humidifier-gas-use-energy-j}
+
+This output is the gas consumption of the gas fired steam humidifier in Joules.
+
+\paragraph{Humidifier Auxiliary Electric Power {[}W{]}}\label{humidifier-auxiliary-electric-power-w}
+
+This output is the auxiliary electricity consumption rate in Watts of the gas fired steam humidifier. This is the auxiliary electric power input to the blower fan and control unit.
+
+\paragraph{Humidifier Auxiliary Electric Energy {[}J{]}}\label{humidifier-auxiliary-electric-energy-j}
+
+This is the auxiliary electricity consumption in Joules of the gas fired steam humidifier over the timestep being reported. This is the auxiliary electric energy consumed by the blower fan and control unit. This auxiliary electric energy is reported meter output Humidifier:Electricity.
+
+\paragraph{Humidifier:Water {[}m3{]}}\label{humidifierwater-m3-1}
+
+This meter output contains the sum of the water consumed (in cubic meters of water during the report timestep) by all the steam humidifiers at the HVAC level in the simulation.
+
+\paragraph{Humidifier:Gas {[}J{]}}\label{humidifiergas-j}
+
+This meter output contains the sum of the gas consumed (in Joules during the report timestep) by all the steam humidifiers at the HVAC level in the simulation.
+
+\paragraph{Humidifier Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{humidifier-storage-tank-water-volume-flow-rate-m3s-1}
+
+\paragraph{Humidifier Storage Tank Water Volume {[}m3{]}}\label{humidifier-storage-tank-water-volume-m3-1}
+
+These outputs contain the rate and volume of water obtained from water storage tank. These are only present if the humidifier is connected to a Water Storage Tank for its water supply.
+
+\paragraph{Humidifier Starved Storage Tank Water Volume Flow Rate {[}m3/s{]}}\label{humidifier-starved-storage-tank-water-volume-flow-rate-m3s-1}
+
+\paragraph{Humidifier Starved Storage Tank Water Volume {[}m3{]}}\label{humidifier-starved-storage-tank-water-volume-m3-1}
+
+These outputs contain the rate and volume of water that could not be obtained from the water storage tank. The component will still operate as if it did get all the water with the balance obtained directly from the mains
+
+\paragraph{Humidifier Mains Water Volume {[}m3{]}}\label{humidifier-mains-water-volume-m3-1}
+
+This output contains the volume of water obtained from the mains.
diff --git a/doc/input-output-reference/src/overview/group-internal-gains-people-lights-other.tex b/doc/input-output-reference/src/overview/group-internal-gains-people-lights-other.tex
new file mode 100644
index 00000000000..db08de5561a
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-internal-gains-people-lights-other.tex
@@ -0,0 +1,3349 @@
+\section[Group -- Internal Gains]{Group -- Internal Gains (People, Lights, Other internal zone equipment)\sectionmark{Group -- Internal Gains}}\label{group-internal-gains-people-lights-other-internal-zone-equipment}
+\sectionmark{Group -- Internal Gains}
+
+Not all the influence for energy consumption in the building is due to envelope and ambient conditions. This group of objects describes other internal gains that may come into play (People, Lights, Various Equipment Types).
+
+\subsection{People}\label{people}
+
+The people statement is used to model the occupant's effect on the space conditions. The following definition addresses the basic affects as well as providing information that can be used to report the thermal comfort of a group of occupants. The Fanger, Pierce Two-Node, and Kansas State University Two-Node thermal comfort models are available in EnergyPlus. A user may select any of these models for each People statement by simply adding the appropriate choice keyword after the air velocity schedule name. Thermal comfort calculations will only be made for people statements that include specific requests for these thermal comfort models. . This object also requires input of carbon dioxide generation rate based on people activity level for zone carbon dioxide simulations.
+
+\subsubsection{Inputs}\label{inputs-025}
+
+\paragraph{Field: Name}\label{field-name-024}
+
+The name of the People object. Must be unique across all People objects.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-000}
+
+This field is the name of the zone (ref: Zone) or ZoneList (ref: ZoneList) and links a particular people statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this people definition is applied to each of the zones in the zone list effecting a global definition for the number of people in the zone. The Zonelist option can be used effectively with the people/area and area/person options of the Number of People Calculation Method.
+
+The name of the actual people object becomes \textless{}Zone Name\textgreater{} \textless{}People Object Name\textgreater{} and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
+
+\paragraph{Field: Number of People Schedule Name}\label{field-number-of-people-schedule-name}
+
+This field is the name of the schedule (ref: Schedules) that modifies the number of people parameter (see Number of People Calculation Method and related fields). The schedule values can be any positive number. The actual number of people in a zone as defined by this statement is the product of the number of people field and the value of the schedule specified by name in this field.
+
+\paragraph{Field: Number of People Calculation Method}\label{field-number-of-people-calculation-method}
+
+This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal number of occupants (people) in the Zone. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  People
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the number of occupants (people).~ (The Number of People field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  People/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The People per Zone Floor Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Area/Person
+\end{itemize}
+
+With this choice, the method used will be a factor of floor area per person. (The Zone Floor Area per Person field should be filled).
+
+\paragraph{Field: Number of People}\label{field-number-of-people}
+
+This field is used to represent the maximum number of people in a zone that is then multiplied by a schedule fraction (see schedule field). In EnergyPlus, this is slightly more flexible in that the number of people could be a ``diversity factor'' applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour, the number of people field is constant for all simulation environments.
+
+\paragraph{Field: People per Zone Floor Area}\label{field-people-per-zone-floor-area}
+
+This factor (person/m\(^{2}\)) is used, along with the Zone Floor Area to determine the maximum number of people as described in the Number of People field. The choice from the method field should be ``people/area''.
+
+\paragraph{Field: Zone Floor Area per Person}\label{field-zone-floor-area-per-person}
+
+This factor (m\(^{2}\)/person) is used, along with the Zone Floor Area to determine the maximum number of people as described in the Number of People field. The choice from the method field should be ``area/person''.
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the type of heat being given off by people in a zone. The number specified in this field will be multiplied by the total sensible energy emitted by people to give the amount of long wavelength radiation gain from human beings in a zone. The remainder of the sensible load is assumed to be convective heat gain. Note that latent gains from people are not included in either the radiant or convective heat gains. See the Engineering Reference document for more details.
+
+\paragraph{Field: Sensible Heat Fraction}\label{field-sensible-heat-fraction}
+
+The user can use this field to specify a fixed sensible fraction for the heat gain due to this PEOPLE object. Normally the program calculates the sensible/latent split; this field gives the user control over this split. This field is autocalculated: if the field is blank or \textbf{autocalculate}, the program will calculate the sensible/latent split; if a value is entered, it will be used as the sensible fraction of the current total heat gain.
+
+\paragraph{Field: Activity Level Schedule Name}\label{field-activity-level-schedule-name}
+
+This field is the name of the schedule that determines the amount of heat gain per person in the zone under design conditions. This value is modified somewhat based on a correlation to account for variations in space temperature. The schedule values may be any positive number and the units for this parameter is Watts per person. This schedule represents the total heat gain per person including convective, radiant, and latent. An internal algorithm is used to determine what fraction of the total is sensible and what fraction is latent. Then, the sensible portion is divided into radiant and convective portions using the value specified for Fraction Radiant (above). See the Engineering Reference document for more details.
+
+Values for activity level can range anywhere from approximately 100-150 Watts per person for most office activities up to over 900 Watts per person for strenuous physical activities such as competitive wrestling. The following table (Table~\ref{table:metabolic-rates-for-various-activities}) is based on Table~\ref{table:wind-speed-profile-coefficients-ashrae} from the 2005 ASHRAE Handbook of Fundamentals, page 8.6. In addition to the information from the ASHRAE HOF, there is an added column of values in W/Person such as necessary for the activity level schedule values. This column uses the standard adult body surface area of 1.8 m\(^{2}\) to multiply the activity levels in W/m\(^{2}\) that are used in the table. Warnings are produced when the activity level schedule values fall outside normal ranges. Having too low or too high values can also skew thermal comfort reporting values.
+
+\paragraph{Field: Carbon Dioxide Generation Rate}\label{field-carbon-dioxide-generation-rate}
+
+This numeric input field specifies carbon dioxide generation rate per person with units of m3/s-W. The total carbon dioxide generation rate from this object is:
+
+Number of People * People Schedule * People Activity * Carbon Dioxide Generation Rate. The default value is 3.82E-8 m3/s-W (obtained from ASHRAE Standard 62.1-2007 value at 0.0084 cfm/met/person over the general adult population). The maximum value can be 10 times the default value.
+
+\paragraph{Field: Enable ASHRAE 55 comfort warnings}\label{field-enable-ashrae-55-comfort-warnings}
+
+This field accepts either ``Yes'' or ``No'' as values. When ``Yes'' is specified, warnings are generated when the space conditions are outside of the ASHRAE 55 comfort range as discussed in the sections that follow titled ``Simplified ASHRAE 55-2004 Graph Related Outputs'' and ``Simplified ASHRAE 55 Warnings.'' The default is not to provide these warnings so if you want to know if your space is outside this comfort range you must set this field to Yes.
+
+% table 11
+\begin{longtable}[c]{p{2.0in}p{1.34in}p{1.33in}p{1.33in}}
+\caption{Metabolic Rates for Various Activities \label{table:metabolic-rates-for-various-activities}} \tabularnewline
+\toprule 
+Activity & Activity Level w/ Person EnergyPlus Schedule Value & Activity Level W/m\(^2\) & met* \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Metabolic Rates for Various Activities} \tabularnewline
+\toprule 
+Activity & Activity Level w/Person EnergyPlus Schedule Value & Activity Level W/m2 & met* \tabularnewline
+\midrule
+\endhead
+
+\emph{Resting} \tabularnewline \midrule 
+Sleeping & 72 & 40 & 0.7 \tabularnewline
+Reclining & 81 & 45 & 0.8 \tabularnewline
+Seated, quiet & 108 & 60 & 1 \tabularnewline
+Standing, relaxed & 126 & 70 & 1.2 \tabularnewline
+\emph{Walking (on level surface)} \tabularnewline \midrule
+3.2 km/h (0.9 m/s) & 207 & 115 & 2 \tabularnewline
+4.3 km/h (1.2 m/s) & 270 & 150 & 2.6 \tabularnewline
+6.4 km/h (1.8 m/s) & 396 & 220 & 3.8 \tabularnewline
+\emph{Office Activities} \tabularnewline \midrule
+Reading, seated & 99 & 55 & 1 \tabularnewline
+Writing & 108 & 60 & 1 \tabularnewline
+Typing & 117 & 65 & 1.1 \tabularnewline
+Filing, seated & 126 & 70 & 1.2 \tabularnewline
+Filing, standing & 144 & 80 & 1.4 \tabularnewline
+Walking about & 180 & 100 & 1.7 \tabularnewline
+Lifting/packing & 216 & 120 & 2.1 \tabularnewline
+\emph{Miscellaneous Occupational Activities} \tabularnewline \midrule
+Cooking & 171 to 207 & 95 to 115 & 1.6 to 2.0 \tabularnewline
+Housecleaning & 207 to 360 & 115 to 200 & 2.0 to 3.4 \tabularnewline
+Seated, heavy limb movement & 234 & 130 & 2.2 \tabularnewline
+Machine work & 189 & 105 & 1.8 \tabularnewline
+sawing (table saw) & 207 to 252 & 115 to 140 & 2.0 to 2.4 \tabularnewline
+light (electrical industry) & 423 & 235 & 4 \tabularnewline
+Handling 50 kg bags & 423 & 235 & 4 \tabularnewline
+Pick and shovel work & 423 to 504 & 235 to 280 & 4.0 to 4.8 \tabularnewline
+\emph{Miscellaneous Leisure Activities} \tabularnewline \midrule
+Dancing, social & 252 to 459 & 140 to 255 & 2.4 to 4.4 \tabularnewline
+Calisthenics/exercise & 315 to 423 & 175 to 235 & 3.0 to 4.0 \tabularnewline
+Tennis, singles & 378 to 486 & 210 to 270 & 3.6 to 4.0 \tabularnewline
+Basketball, competitive & 522 to 792 & 290 to 440 & 5.0 to 7.6 \tabularnewline
+Wrestling, competitive & 738 to 909 & 410 to 505 & 7.0 to 8.7 \tabularnewline
+\bottomrule
+\scriptsize
+\textbf{*Note that one met = 58.1 W/m\(^{2}\)}
+\end{longtable}
+
+\paragraph{Field: Mean Radiant Temperature Calculation Type}\label{field-mean-radiant-temperature-calculation-type}
+
+This field specifies the type of Mean Radiant Temperature (MRT) calculation the user wishes to use for the thermal comfort model. At the present time, there are two options for MRT calculation type: zone averaged and surface weighted. The default calculation is ``ZoneAveraged''. In the zone averaged MRT calculation, the MRT used for the thermal comfort calculations is for an ``average'' point in the zone. MRT is calculated based on an area-emissivity weighted average of all of the surfaces in the zone. In cases where the emissivity of all of the surfaces are sufficiently small (near zero), the mean radiant temperature will be set to the mean air temperature of the space to avoid divide by zero errors. The other MRT calculation type is ``SurfaceWeighted''. The goal of this calculation type is to estimate a person in the space close to a particular surface without having to define exact view factors for all of the surfaces and the location of the person in the space. The MRT used in the thermal comfort calculations when the ``surface weighted'' calculation type is selected is actually the average of the temperature of the surface to which the person is closest (defined by the next field ``Surface Name'') and the zone averaged MRT (defined above). The surface temperature alone is not used because in theory the maximum view factor from a person to any flat surface is roughly 0.5. In the ``surfaceweighted'' calculation, the surface in question actually gets slightly more weighting than 50\% since the surface selected is still a part of the zone average MRT calculation. Again, this simplification was made to avoid the specification of view factors and the exact location of the person.
+
+A third option is to use ``anglefactor''. This option allows for more explicit positioning of the person within the space by defining the angle factors from the person to the various surfaces in the zone. This option requires the user to list the surfaces that the person can see from a radiation standpoint and also define the angle (or view) factor for each surface. The AngleFactorList object (see next object description) is intended to give the user this opportunity.
+
+\paragraph{Field: Surface Name/Angle Factor List Name}\label{field-surface-nameangle-factor-list-name}
+
+This field is only valid when the user selects ``surfaceweighted'' for the MRT calculation type (see the previous input field description). In this case, the field is the name of a surface within the zone the people are residing. This surface will be used in the MRT calculation as defined above to come up with a more representative MRT for a person near a particular surface. The MRT used for thermal comfort calculations using the ``surface weighted'' MRT calculation method is the average of the temperature of the surface specified in this field and the ``zone averaged'' MRT (see the Mean Radiant Temperature calculation type field above).
+
+\paragraph{Field: Work Efficiency Schedule Name}\label{field-work-efficiency-schedule-name}
+
+This field is the name of the schedule that determines the efficiency of energy usage within the human body that will be used for thermal comfort calculations. Note that all energy produced by the body is assumed to be converted to heat for the zone heat balance calculation. A value of zero correspondsto all of the energy produced in the body being converted to heat. A value of unity corresponds to all of the energy produced in the body being converted to mechanical energy. The values for this parameter defined in the schedule must be between 0.0 and 1.0. Any value greater than zero will result in a reduction of heat that impacts thethermal comfort energy balance of a person within the space, resulting in PMV results appearing lower than expected.~ Ensure that if this value is non-zero, the base activity level is chosen to ensure that the net activity converted to heat and zone conditions are sufficient to maintain thermal comfort..
+
+\paragraph{Field: Clothing Insulation Calculation Method}\label{field-clothing-insulation-calculation-method}
+
+This field is a key/choice field that tells which of the next two fields are filled and is descriptive of the method for calculating the clothing insulation value of occupants (people) in the Zone. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  ClothingInsulationSchedule
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the scheduled clothing insulation values of occupants (people).~ (The Clothing Insulation Schedule Name field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  DynamicClothingModelASHRAE55
+\end{itemize}
+
+With this choice, the method used will be the dynamic predictive clothing insulation model developed by Schiavon and Lee (2013) based on 6,333 selected observations taken from ASHRAE RP-884 and RP-921 databases. It varies the clothing insulation as a function of outdoor air temperature measured at 6am as illustrated below.
+
+\begin{itemize}
+\tightlist
+\item
+  CalculationMethodSchedule
+\end{itemize}
+
+With this choice, the method used can be either the ClothingInsulationSchedule or the DynamicClothingModelASHRAE55, depending on a schedule (to be entered as the next field) that determines which method to use in different time of a day. When this option is chosen, the next field ``Clothing Insulation Calculation Method Schedule Name'' is a required input.
+
+\begin{figure}[hbtp] % fig 48
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image083.png}
+\caption{Graphical representation fo the dynamic predictive clothing insulation model \protect \label{fig:graphical-representation-fo-the-dynamic}}
+\end{figure}
+
+\paragraph{Field: Clothing Insulation Calculation Method Schedule Name}\label{field-clothing-insulation-calculation-method-schedule-name}
+
+This field specifies which clothing insulation method (ClothingInsulationSchedule or DynamicClothingModelASHRAE55) to use at a particular time of the day. A schedule value of 1 means the ClothingInsulationSchedule method, and 2 means the DynamicClothingModelASHRAE55 method. This field is only required when the ``Clothing Insulation Calculation Method'' field is set to \textbf{CalculationMethodSchedule}. If this field is left blank, the specified clothing insulation calculation method will be used and not changed during the simulation.
+
+\paragraph{Field: Clothing Insulation Schedule Name}\label{field-clothing-insulation-schedule-name}
+
+This field is the name of the schedule that defines the amount of clothing being worn by a typical zone occupant during various times in the simulation period. The choice from the Clothing Insulation Calculation Method field should be ``\textbf{ClothingInsulationSchedule}''. This parameter must be a positive real number and has units of Clo. Typical values for Clo can be seen in the ASHRAE 2009 HOF Table 7, page 9.8 (for clothing ensembles) and Table~\ref{table:window-modeling-options}, page 9.9 (for garment values) ) or www.cbe.berkeley.edu/comforttool/.
+
+\paragraph{Field: Air Velocity Schedule Name}\label{field-air-velocity-schedule-name}
+
+This field is the name of the schedule that approximates the amount of air movement in the space as a function of time throughout the simulation period. The user has control over this parameter through the schedule that requires the individual numbers in the schedule to be positive real numbers having units of meters per second.
+
+\paragraph{Field: Thermal Comfort Model Type (up to 5 allowed)}\label{field-thermal-comfort-model-type-up-to-5-allowed}
+
+The final one to five fields are optional and are intended to trigger various thermal comfort models within EnergyPlus. By entering the keywords Fanger, Pierce, KSU, AdaptiveASH55,, and AdaptiveCEN15251, the user can request the Fanger, Pierce Two-Node, Kansas State UniversityTwo-Node, and the adaptive comfort models of the ASHRAE Standard 55 and CEN Standard 15251 results for this particular people statement. AdaptiveASH55 is only applicable when the running average outdoor air temperature for the past 7 days is between 10.0 and 33.5C. AdaptiveCEN15251 is only applicable when the running average outdoor air temperature for the past 30 days is between 10.0 and 30.0C. Note that since up to five models may be specified, the user may opt to have EnergyPlus calculate the thermal comfort for people identified with this people statement using all five models if desired. Note that the KSU model is computationally intensive and may noticeably increase the execution time of the simulation. For descriptions of the thermal comfort calculations, see the Engineering Reference document.
+
+The following IDF example allows for a maximum of 31 people with scheduled occupancy of ``Office Occupancy'', 60\% radiant using an Activity Schedule of ``Activity Sch''. The example allows for thermal comfort reporting.
+
+\begin{lstlisting}
+
+People,
+  Kitchen_ZN_1_FLR_1,   !- Name
+  Kitchen_ZN_1_FLR_1,   !- Zone or ZoneList Name
+  BLDG_OCC_SCH,         !- Number of People Schedule Name
+  People,               !- Number of People Calculation Method
+  25.2000,,,            !- Number of People, People per Zone Floor Area, Zone Floor Area per Person
+  0.3000,               !- Fraction Radiant
+  AUTOCALCULATE,        !- Sensible Heat Fraction
+  ACTIVITY_SCH,         !- Activity Level Schedule Name
+  3.82E-8,              !- Carbon Dioxide Generation Rate {m3/s-W}
+  No,                   !- Enable ASHRAE 55 Comfort Warnings
+  ZoneAveraged,         !- Mean Radiant Temperature Calculation Type
+  ,                     !- Surface Name/Angle Factor List Name
+  WORK_EFF_SCH,         !- Work Efficiency Schedule Name
+  CLOTHING_SCH,         !- Clothing Insulation Schedule Name
+  AIR_VELO_SCH,         !- Air Velocity Schedule Name
+  Fanger;               !- Thermal Comfort Model 1 Type
+\end{lstlisting}
+
+A simpler example, without using the thermal comfort reporting option:
+
+\begin{lstlisting}
+People,
+  RIGHT FORK,     !- Name
+  RIGHT FORK,     !- Zone or ZoneListName
+  Dorm Occupancy, !- Number of People Schedule Name
+  people,         !- Number of People Calculation Method
+  8.00000,        !- Number of People,
+  ,               !- People per Zone Floor Area
+  ,               !- Zone Floor Area per Person
+  0.6000000,      !- Fraction Radiant
+  Autocalculate,  !- Sensible Heat Fraction
+  Activity Sch,   !- Activity level Schedule Name
+\end{lstlisting}
+
+And with the sensible fraction specified:
+
+\begin{lstlisting}
+People,
+  SPACE1-1 People 1,    !- Name
+  SPACE1-1,             !- Zone or ZoneListName
+  OCCUPY-1,             !- Number of People Schedule Name
+  people,               !- Number of People Calculation Method
+  11,                   !- Number of People
+  ,                     !- People per Zone Floor Area
+  ,                     !- Zone Floor Area per Person
+  0.3,                  !- Fraction Radiant
+  0.55,                 !- Sensible Heat Fraction
+  ActSchd;              !- Activity level Schedule Name
+\end{lstlisting}
+
+Global People Object:
+
+\begin{lstlisting}
+ZoneList,AllOccupiedZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
+
+People,
+  AllZones with People, !- Name
+  AllOccupiedZones,     !- Zone or ZoneList Name
+  OCCUPY-1,             !- Number of People Schedule Name
+  People/Area,          !- Number of People Calculation Method
+  ,                     !- Number of People
+  .11,                  !- People per Zone Floor Area {person/m2}
+  ,                     !- Zone Floor Area per Person {m2/person}
+  0.3,                  !- Fraction Radiant
+  ,                     !- Sensible Heat Fraction
+  ActSchd;              !- Activity Level Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-017}
+
+People objects have output variables for individual objects and for zone totals.
+
+People specific outputs include:
+
+\begin{itemize}
+\item
+  Zone,Average,People Occupant Count {[]}
+\item
+  Zone,Sum,People Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,People Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,People Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,People Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,People Sensible Heating Energy {[}J{]}
+\item
+  Zone,Average,People Sensible Heating Rate {[}W{]}
+\item
+  Zone,Sum,People Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,People Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,People Total Heating Energy {[}J{]}
+\item
+  Zone,Average,People Total Heating Rate {[}W{]}
+\item
+  Zone,Average,Zone People Occupant Count {[]}
+\item
+  Zone,Sum,Zone People Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone People Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone People Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone People Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone People Sensible Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone People Sensible Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone People Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Zone People Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Zone People Total Heating Energy {[}J{]}
+\item
+  Zone,Average,People Air Temperature {[}C{]}
+\item
+  Zone,Average,People Air Relative Humidity {[}\%{]}
+\item
+  Zone,Average,Zone People Total Heating Rate {[}W{]}
+\item
+  Zone,Average,Zone Thermal Comfort Mean Radiant Temperature {[}C{]}
+\item
+  Zone,Average,Zone Thermal Comfort Operative Temperature {[}C{]}
+\item
+  Zone,Average,Zone Thermal Comfort Fanger Model PMV {[]}
+\item
+  Zone,Average,Zone Thermal Comfort Fanger Model PPD {[}\%{]}
+\item
+  Zone,Average,Zone Thermal Comfort Clothing Surface Temperature {[}C{]}
+\item
+  Zone,Average,Zone Thermal Comfort Pierce Model Effective Temperature PMV {[]}
+\item
+  Zone,Average,Zone Thermal Comfort Pierce Model Standard Effective Temperature PMV {[]}
+\item
+  Zone,Average,Zone Thermal Comfort Pierce Model Discomfort Index {[]}
+\item
+  Zone,Average,Zone Thermal Comfort Pierce Model Thermal Sensation Index {[]}
+\item
+  Zone,Average,Zone Thermal Comfort KSU Model Thermal Sensation Index {[]}
+\item
+  Zone,Average,Zone Thermal Comfort ASHRAE 55 Adaptive Model 80\% Acceptability Status {[]}
+\item
+  Zone,Average,Zone Thermal Comfort ASHRAE 55 Adaptive Model 90\% Acceptability Status {[]}
+\item
+  Zone,Average,Zone Thermal Comfort ASHRAE 55 Adaptive Model Running Average Outdoor Air Temperature {[}C{]}
+\item
+  Zone,Average,Zone Thermal Comfort ASHRAE 55 Adaptive Model Temperature {[}C{]}
+\item
+  Zone,Average,Zone Thermal Comfort CEN 15251 Adaptive Model Category I Status {[]}
+\item
+  Zone,Average,Zone Thermal Comfort CEN 15251 Adaptive Model Category II Status {[]}
+\item
+  Zone,Average,Zone Thermal Comfort CEN 15251 Adaptive Model Category III Status
+\item
+  Zone,Average,Zone Thermal Comfort CEN 15251 Adaptive Model Running Average Outdoor Air Temperature {[}C{]}
+\item
+  Zone,Average,Zone Thermal Comfort CEN 15251 Adaptive Model Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{People Occupant Count {[]}}{People Occupant Count }}\label{people-occupant-count}
+
+This field is the number of people for this PEOPLE object during the timestep in question.
+
+\paragraph{People Radiant Heating Rate {[}W{]}}\label{people-radiant-heating-rate-w}
+
+\paragraph{People Radiant Heating Energy {[}J{]}}\label{people-radiant-heating-energy-j}
+
+These output variables are the amount of radiant heat gain for this People object in Watts (for rate) or Joules. This is determined by the current sensible heat gain from people to the zone and the ``Fraction Radiant'' specified in the input. The radiant gains from people are distributed to the surfaces using an area weighting scheme.
+
+\paragraph{People Convective Heating Rate {[}W{]}}\label{people-convective-heating-rate-w}
+
+\paragraph{People Convective Heating Energy {[}J{]}}\label{people-convective-heating-energy-j}
+
+These output variables are the amount of convective heat gain for this People object in Watts (for rate) or Joules. This is determined by the current sensible heat gain from people to the zone and the ``Fraction Radiant'' specified in input. Note that the radiant and convective gains should add up to the sensible heat gain from people. The convective heat gain from people is added to the zone air heat balance directly.
+
+\paragraph{People Latent Gain Rate {[}W{]}}\label{people-latent-gain-rate-w}
+
+\paragraph{People Latent Gain Energy {[}J{]}}\label{people-latent-gain-energy-j}
+
+These output variables are the amount of latent heat gain for this People object in Watts (for rate) or Joules. This amount is based on the number of people in the space as well as the total amount of energy produced by a typical person defined by the activity schedule in the input. An internal algorithm is used to determine what fraction of the total is sensible and what fraction is latent. Details about this split are included in the Engineering Reference document.
+
+\paragraph{People Sensible Heating Rate {[}W{]}}\label{people-sensible-heating-rate-w}
+
+\paragraph{People Sensible Heating Energy {[}J{]}}\label{people-sensible-heating-energy-j}
+
+These output variables are the amount of sensible heat gain for this People object in Watts (for rate) or Joules. This amount is based on the number of people in the space as well as the total amount of energy produced by a typical person defined by the activity schedule in the input. An internal algorithm (described in the Engineering Reference document) is used to determine what fraction of the total is sensible and what fraction is latent. The sensible plus the latent heat gain from people equals the total gain specified in the input.
+
+\paragraph{People Total Heating Rate {[}W{]}}\label{people-total-heating-rate-w}
+
+\paragraph{People Total Heating Energy {[}J{]}}\label{people-total-heating-energy-j}
+
+These output variables are the total amount of heat gain for this People object in Watts (for rate) or Joules. This is derived from the activity level times the number of occupants.
+
+\paragraph{People Air Temperature {[}C{]}}\label{people-air-temperature-c}
+
+This output variable represents the zone air temperature based on the Fanger thermal comfort model.~ If there is a ZoneControl:Thermostat:ThermalComfort object specified and the thermal zone is occupied, then the value of ``People Air Temperature'' is determined based on the thermal comfort hat satisfies the thermal comfort setpoint PMV value specified; othwesie, it is set to average zone air temperature.
+
+\paragraph{People Air Relative Humidity {[}\%{]}}\label{people-air-relative-humidity}
+
+This output variable represents the zone air relative humidity based on the Fanger thermal comfort model.~ If there is a ZoneControl:Thermostat:ThermalComfort object specified and the thermal zone is occupied, then the value of ``People Air Relative Humidity'' is determined from the mean zone air temperature and zone air humidity ratio that satisfies the thermal comfort setpoint PMV value specified; othwesie, it is calculated from the zone air temperature and humidity ratio averaged over the time step.
+
+\paragraph{\texorpdfstring{Zone People Occupant Count {[]}}{Zone People Occupant Count }}\label{zone-people-occupant-count}
+
+This field is the total number of people within the zone during the timestep in question.
+
+\paragraph{Zone People Radiant Heating Rate {[}W{]}}\label{zone-people-radiant-heating-rate-w}
+
+\paragraph{Zone People Radiant Heating Energy {[}J{]}}\label{zone-people-radiant-heating-energy-j}
+
+These output variables are the amount of radiant heat gain from people within the zone in Watts (for rate) or Joules. This is determined by the current sensible heat gain from people to the zone and the ``Fraction Radiant'' specified in the input. The radiant gains from people are distributed to the surfaces using an area weighting scheme.
+
+\paragraph{Zone People Convective Heating Rate {[}W{]}}\label{zone-people-convective-heating-rate-w}
+
+\paragraph{Zone People Convective Heating Energy {[}J{]}}\label{zone-people-convective-heating-energy-j}
+
+These output variables are the amount of convective heat gain from people within the zone in Watts (for rate) or Joules. This is determined by the current sensible heat gain from people to the zone and the ``Fraction Radiant'' specified in input. Note that the radiant and convective gains should add up to the sensible heat gain from people. The convective heat gain from people is added to the zone air heat balance directly.
+
+\paragraph{Zone People Latent Gain Rate {[}W{]}}\label{zone-people-latent-gain-rate-w}
+
+\paragraph{Zone People Latent Gain Energy {[}J{]}}\label{zone-people-latent-gain-energy-j}
+
+These output variables are the amount of latent heat gain from people within the zone in Watts (for rate) or Joules. This amount is based on the number of people in the space as well as the total amount of energy produced by a typical person defined by the activity schedule in the input. An internal algorithm is used to determine what fraction of the total is sensible and what fraction is latent. Details about this split are included in the Engineering Reference document.
+
+\paragraph{Zone People Sensible Heating Rate {[}W{]}}\label{zone-people-sensible-heating-rate-w}
+
+\paragraph{Zone People Sensible Heating Energy {[}J{]}}\label{zone-people-sensible-heating-energy-j}
+
+These output variables are the amount of sensible heat gain from people within the zone in Watts (for rate) or Joules. This amount is based on the number of people in the space as well as the total amount of energy produced by a typical person defined by the activity schedule in the input. An internal algorithm (described in the Engineering Reference document) is used to determine what fraction of the total is sensible and what fraction is latent. The sensible plus the latent heat gain from people equals the total gain specified in the input.
+
+\paragraph{Zone People Total Heating Rate {[}W{]}}\label{zone-people-total-heating-rate-w}
+
+\paragraph{Zone People Total Heating Energy {[}J{]}}\label{zone-people-total-heating-energy-j}
+
+These output variables are the total amount of heat gain from people within the zone in Watts (for rate) or Joules. Derived from the activity level times the number of occupants, this is summed for each people object within a zone.
+
+\paragraph{Zone Thermal Comfort Mean Radiant Temperature {[}C{]}}\label{zone-thermal-comfort-mean-radiant-temperature-c}
+
+This output variable is the mean radiant temperature used in the thermal comfort calculations.~ This value is computed according to the ``MRT Calculation Type'' specified in the PEOPLE object.~ If a high temperature radiant system is present in the zone, this value will be adjusted according to the current heater operation and the ``Fraction of radiant energy incident on people'' specified in the HIGH TEMP RADIANT SYSTEM object.
+
+\paragraph{Zone Thermal Comfort Operative Temperature {[}C{]}}\label{zone-thermal-comfort-operative-temperature-c}
+
+This output variable is the operative temperature as defined by the thermal comfort operations. Specifically, it is the average of the thermal comfort mean radiant temperature and the zone air temperature.
+
+Note for all Thermal Comfort reporting:~ Though the published values for thermal comfort ``vote'' have a discrete scale (e.g. --3 to +3 or --4 to +4), the calculations in EnergyPlus are carried out on a continuous scale and, thus, reporting may be ``off the scale'' with specific conditions encountered in the space. This is not necessarily an error in EnergyPlus -- rather a different approach that does not take the ``limits'' of the discrete scale values into account.
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort Fanger Model PMV {[]}}{Zone Thermal Comfort Fanger Model PMV }}\label{zone-thermal-comfort-fanger-model-pmv}
+
+This field is the ``predicted mean vote'' (PMV) calculated using the Fanger thermal comfort model.
+
+\paragraph{Zone Thermal Comfort Fanger Model PPD {[}\%{]}}\label{zone-thermal-comfort-fanger-model-ppd}
+
+This field is the ``predicted percentage of dissatisfied'' (PPD) calculated using the Fanger thermal comfort model.
+
+\paragraph{Zone Thermal Comfort Clothing Surface Temperature {[}C{]}}\label{zone-thermal-comfort-clothing-surface-temperature-c}
+
+This output variable is the calculation of the clothing surface temperature using the Fanger thermal comfort model.
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort Pierce Model Effective Temperature PMV {[]}}{Zone Thermal Comfort Pierce Model Effective Temperature PMV }}\label{zone-thermal-comfort-pierce-model-effective-temperature-pmv}
+
+This field is the ``predicted mean vote'' (PMV) calculated using the effective temperature and the Pierce two-node thermal comfort model.
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort Pierce Model Standard Effective Temperature PMV {[]}}{Zone Thermal Comfort Pierce Model Standard Effective Temperature PMV }}\label{zone-thermal-comfort-pierce-model-standard-effective-temperature-pmv}
+
+This field is the ``predicted mean vote'' (PMV) calculated using the ``standard'' effective temperature and the Pierce two-node thermal comfort model.
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort Pierce Model Discomfort Index {[]}}{Zone Thermal Comfort Pierce Model Discomfort Index }}\label{zone-thermal-comfort-pierce-model-discomfort-index}
+
+This field is the ``discomfort index'' calculated using the the Pierce two-node thermal comfort model.
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort Pierce Model Thermal Sensation Index {[]}}{Zone Thermal Comfort Pierce Model Thermal Sensation Index }}\label{zone-thermal-comfort-pierce-model-thermal-sensation-index}
+
+This field is the ``thermal sensation index'' (PMV) calculated using the Pierce two-node thermal comfort model.
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort KSU Model Thermal Sensation Vote {[]}}{Zone Thermal Comfort KSU Model Thermal Sensation Vote }}\label{zone-thermal-comfort-ksu-model-thermal-sensation-vote}
+
+This field is the ``thermal sensation vote'' (TSV) calculated using the KSU two-node thermal comfort model.
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort ASHRAE 55 Adaptive Model 90\% Acceptability Status {[]}}{Zone Thermal Comfort ASHRAE 55 Adaptive Model 90\% Acceptability Status }}\label{zone-thermal-comfort-ashrae-55-adaptive-model-90-acceptability-status}
+
+This field is to report whether the operative temperature falls into the 90\% acceptability limits of the adaptive comfort in ASHRAE 55-2010. A value of 1 means within (inclusive) the limits, a value of 0 means outside the limits, and a value of -1 means not applicable (when unoccupied or running average outdoor temp is outside the range of 10.0 to 33.5C).
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort ASHRAE 55 Adaptive Model 80\% Acceptability Status {[]}}{Zone Thermal Comfort ASHRAE 55 Adaptive Model 80\% Acceptability Status }}\label{zone-thermal-comfort-ashrae-55-adaptive-model-80-acceptability-status}
+
+This field is to report whether the operative temperature falls into the 80\% acceptability limits of the adaptive comfort in ASHRAE 55-2010. A value of 1 means within (inclusive) the limits, a value of 0 means outside the limits, and a value of -1 means not applicable (when unoccupied or running average outdoor temp is outside the range of 10.0 to 33.5C).
+
+\paragraph{Zone Thermal Comfort ASHRAE 55 Adaptive Model Running Average Outdoor Air Temperature {[}C{]}}\label{zone-thermal-comfort-ashrae-55-adaptive-model-running-average-outdoor-air-temperature-c}
+
+This field reports the mean monthly outdoor air temperature, an input parameter for the ASHRAE-55 adaptive comfort model. This can be computed in two ways. If the .stat file is provided for the simulation, this field will reflect the monthly daily average temperature.
+
+If the .epw file is used, the field reports the simple running average of the daily average outdoor dry-bulb temperatures of the previous 30 days.
+
+\paragraph{Zone Thermal Comfort ASHRAE 55 Adaptive Model Temperature {[}C{]}}\label{zone-thermal-comfort-ashrae-55-adaptive-model-temperature-c}
+
+This field reports the ideal indoor operative temperature, or comfort temperature, as determined by the ASHRAE-55 adaptive comfort model. The 80\% acceptability limits for indoor operative temperature are defined as no greater than 3.5 degrees C from the adaptive comfort temperature. The 90\% acceptability limits are defined as no greater than 2.5 degrees C from the adaptive comfort temperature. A value of -1 means not applicable (when running average outdoor temp is outside the range of 10.0 to 33.5C).
+
+\paragraph{Zone Thermal Comfort CEN 15251 Adaptive Model Category I Status}\label{zone-thermal-comfort-cen-15251-adaptive-model-category-i-status}
+
+This field is to report whether the operative temperature falls into the Category I (90\% acceptability) limits of the adaptive comfort in the European Standard EN15251-2007. A value of 1 means within (inclusive) the limits, a value of 0 means outside the limits, and a value of -1 means not applicable (when unoccupied or running average outdoor temp is outside the range of 10.0 to 30.0C).
+
+\paragraph{Zone Thermal Comfort CEN 15251 Adaptive Model Category II Status}\label{zone-thermal-comfort-cen-15251-adaptive-model-category-ii-status}
+
+This field is to report whether the operative temperature falls into the Category II (80\% acceptability) limits of the adaptive comfort in the European Standard EN15251-2007. A value of 1 means within (inclusive) the limits, a value of 0 means outside the limits, and a value of -1 means not applicable (when unoccupied or running average outdoor temp is outside the range of 10.0 to 30.0C).
+
+\paragraph{Zone Thermal Comfort CEN 15251 Adaptive Model Category III Status}\label{zone-thermal-comfort-cen-15251-adaptive-model-category-iii-status}
+
+This field is to report whether the operative temperature falls into the Category III (65\% acceptability) limits of the adaptive comfort in the European Standard EN15251-2007. A value of 1 means within (inclusive) the limits, a value of 0 means outside the limits, and a value of -1 means not applicable (when unoccupied or running average outdoor temp is outside the range of 10.0 to 30.0C).
+
+\paragraph{Zone Thermal Comfort CEN 15251 Adaptive Model Running Average Outdoor Air Temperature}\label{zone-thermal-comfort-cen-15251-adaptive-model-running-average-outdoor-air-temperature}
+
+This field reports the weighted average of the outdoor air temperature of the previous seven days, an input parameter for the CEN-15251 adaptive comfort model.
+
+\paragraph{Zone Thermal Comfort CEN 15251 Adaptive Model Temperature}\label{zone-thermal-comfort-cen-15251-adaptive-model-temperature}
+
+This field reports the ideal indoor operative temperature, or comfort temperature, as determined by the CEN-15251 adaptive comfort model. Category I, II, and II limits for indoor operative temperature are defined as no greater than 2, 3, and 4 degrees C from this value respectively. A value of -1 means not applicable (when running average outdoor temp is outside the range of 10.0 to 30.0C).
+
+\subsubsection{Outputs}\label{outputs-1-014}
+
+The following output variables are all based on whether the humidity ratio and the operative temperature is within the region shown in ASHRAE Standard 55-2004 in Figure 5.2.1.1. For these outputs the operative temperature is simplified to be the average of the air temperature and the mean radiant temperature. For summer, the 0.5 Clo level is used and, for winter, the 1.0 Clo level is used. The graphs below are based on the following tables which extend the ASHRAE values to zero humidity ratio.
+
+% table 12
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Winter Clothes (1.0 Clo) \label{table:winter-clothes-1.0-clo}} \tabularnewline
+\toprule 
+Operative Temperature (C) & Humidity Ratio (kgWater/kgDryAir) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Winter Clothes (1.0 Clo)} \tabularnewline
+\toprule 
+Operative Temperature (C) & Humidity Ratio (kgWater/kgDryAir) \tabularnewline
+\midrule
+\endhead
+
+19.6 & 0.012 \tabularnewline
+23.9 & 0.012 \tabularnewline
+26.3 & 0.000 \tabularnewline
+21.7 & 0.000 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{figure}[hbtp] % fig 49
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image084.png}
+\caption{Winter Comfort Range \protect \label{fig:winter-comfort-range}}
+\end{figure}
+
+% table 13
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Summer Clothes (0.5 Clo) \label{table:summer-clothes-0.5-clo}} \tabularnewline
+\toprule 
+Operative Temperature (C) & Humidity Ratio (kgWater/kgDryAir) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Summer Clothes (0.5 Clo)} \tabularnewline
+\toprule 
+Operative Temperature (C) & Humidity Ratio (kgWater/kgDryAir) \tabularnewline
+\midrule
+\endhead
+
+23.6 & 0.012 \tabularnewline
+26.8 & 0.012 \tabularnewline
+28.3 & 0.000 \tabularnewline
+25.1 & 0.000 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{figure}[hbtp] % fig 50
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image085.png}
+\caption{Summer Comfort Range \protect \label{fig:summer-comfort-range}}
+\end{figure}
+
+\paragraph{Zone Thermal Comfort ASHRAE 55 Simple Model Summer Clothes Not Comfortable Time{[}hr{]}}\label{zone-thermal-comfort-ashrae-55-simple-model-summer-clothes-not-comfortable-timehr}
+
+The time when the zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 summer clothes region (see above)
+
+\paragraph{Zone Thermal Comfort ASHRAE 55 Simple Model Winter Clothes Not Comfortable Time{[}hr{]}}\label{zone-thermal-comfort-ashrae-55-simple-model-winter-clothes-not-comfortable-timehr}
+
+The time when the zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 winter clothes region (see above)
+
+\paragraph{Zone Thermal Comfort ASHRAE 55 Simple Model Summer or Winter Clothes Not Comfortable Time{[}hr{]}}\label{zone-thermal-comfort-ashrae-55-simple-model-summer-or-winter-clothes-not-comfortable-timehr}
+
+The time when the zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 summer or winter clothes region (see above)
+
+\paragraph{Facility Thermal Comfort ASHRAE 55 Simple Model Summer Clothes Not Comfortable Time{[}hr{]}}\label{facility-thermal-comfort-ashrae-55-simple-model-summer-clothes-not-comfortable-timehr}
+
+The time when any zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 summer clothes region (see above)
+
+\paragraph{Facility Thermal Comfort ASHRAE 55 Simple Model Winter Clothes Not Comfortable Time {[}hr{]}}\label{facility-thermal-comfort-ashrae-55-simple-model-winter-clothes-not-comfortable-time-hr}
+
+The time when any zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 winter clothes region (see above)
+
+\paragraph{Facility Thermal Comfort ASHRAE 55 Simple Model Summer or Winter Clothes Not Comfortable Time {[}hr{]}}\label{facility-thermal-comfort-ashrae-55-simple-model-summer-or-winter-clothes-not-comfortable-time-hr}
+
+The time when any zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 summer or winter clothes region (see above)
+
+\subsection{Simplified ASHRAE 55 Warnings}\label{simplified-ashrae-55-warnings}
+
+The simplified ASHRAE 55 calculations may be computed for occupied zones and, possibly, warnings are shown on the .err file at the end of each simulated environment. To enable this option set the ``Enable ASHRAE 55 comfort warnings'' field of the People object to Yes. These warnings will not be generated by default.
+
+If you enable the warnings, the simplified ASHRAE 55 calculations are done for occupied zones and, possibly, warnings are shown on the .err file at the end of each simulated environment.
+
+\begin{lstlisting}
+** Warning ** More than 4% of time (350.4 hours) uncomfortable in zone ZSF1
+** ~~~ ** 553.0 hours were uncomfortable based on ASHRAE 55-2004 graph (Section 5.2.1.1)
+** ~~~ ** During Environment [10/01 - 09/30]: CHICAGO IL USA TMY2-94846 WMO\# = 725300
+** Warning ** More than 4% of time (350.4 hours) uncomfortable in zone ZNF1
+** ~~~ ** 827.8 hours were uncomfortable based on ASHRAE 55-2004 graph (Section 5.2.1.1)
+** ~~~ ** During Environment [10/01 - 09/30]: CHICAGO IL USA TMY2-94846 WMO\# = 725300
+** Warning ** More than 4% of time (350.4 hours) uncomfortable in zone ZSF2
+** ~~~ ** 593.5 hours were uncomfortable based on ASHRAE 55-2004 graph (Section 5.2.1.1)
+** ~~~ ** During Environment [10/01 - 09/30]: CHICAGO IL USA TMY2-94846 WMO\# = 725300
+** Warning ** More than 4% of time (350.4 hours) uncomfortable in zone ZNF2
+** ~~~ ** 875.8 hours were uncomfortable based on ASHRAE 55-2004 graph (Section 5.2.1.1)
+** ~~~ ** During Environment [10/01 - 09/30]: CHICAGO IL USA TMY2-94846 WMO\# = 725300
+\end{lstlisting}
+
+You may decide if you need to change parameters to reduce these ``uncomfortable'' hours. The individual output variables shown previously may help you get more details on when these are occurring.
+
+Following are some suggestions that might be applicable:
+
+\begin{itemize}
+\item
+  Eliminate occupancy when conditioning equipment is off.
+\item
+  Note that the ASHRAE graph lower limit is (19.6C to 21.7C) -- heating setpoints may need to be nearer 22.2C (72F) than 21.1C (70F).
+\item
+  Unoccupied heating setpoint should be nearer 16.7C (62F) rather than 12.8C (55F) to reduce the start up recovery.
+\item
+  Start the occupied setpoint schedule, fan availability schedule, cooling pump availability schedule, reheat coil availability, one hour before occupancy. Seasonal turn on and off of equipment may cause more warnings (but potentially more energy consumption).
+\item
+  Unoccupied cooling setpoint should be nearer 29.4C (85F) rather than 40.0 (104F) to reduce the start up recovery.
+\end{itemize}
+
+\subsection{ComfortViewFactorAngles}\label{comfortviewfactorangles}
+
+When requesting EnergyPlus to do a thermal comfort calculation, the program user has three options for defining how the mean radiant temperature will be calculated. The user may select ``zoneaveraged'' which results in a mean radiant temperature that is characteristic of an ``average'' location near the center of the zone. The user may also elect to place the person near a particular surface by selecting ``surfaceweighted'' in the People statement. This takes the average of the zone mean radiant temperature and the temperature of the surface that the person is near and uses this value as the mean radiant temperature when calculating thermal comfort.
+
+The third option is for the user to more explicitly position the person within the space by defining the angle factors from the person to the various surfaces in the zone. This option requires the user to list the surfaces that the person can see from a radiation standpoint and also define the angle (or view) factor for each surface. The AngleFactorList input line is intended to give the user this opportunity.
+
+\subsubsection{Inputs}\label{inputs-1-023}
+
+\paragraph{Field: Name}\label{field-name-1-022}
+
+This field is an unique user assigned name for the list of surfaces that can be seen radiantly by the person for whom thermal comfort is to be evaluated. Any reference to this list by a People statement will use this name.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-007}
+
+Zone Name for this surface list. Each of the surfaces listed must be in this zone.
+
+\paragraph{Field: Surface \textless{}\#\textgreater{} Name}\label{field-surface-name-002}
+
+This field is the name of a surface in the zone seen by the person.
+
+\paragraph{Field: Angle Factor \textless{}\#\textgreater{}}\label{field-angle-factor}
+
+This field is the fraction that this surface contributes to the total mean radiant temperature. This can be thought of as a weighting factor for this surface and the actual mean radiant temperature used in the thermal comfort model is simply the sum of all angle factors multiplied by the corresponding inside surface temperature. Note that the Surface Name/Angle Factor pair can be repeated up to 20 times. The sum of all angle factors within any angle factor list must equal unity, otherwise the program will not accept the input as valid.
+
+An example IDF with an electric low temperature radiant system is shown below.
+
+\begin{lstlisting}
+ComfortViewFactorAngles,
+  South Zone Angle Factors,                                                                                                    !- name of angle factor list
+  Sourth Zone,          !- Zone Name
+  Zn001:Flr001,         !- Surface name 1
+  0.75,                 !- Angle factor for surface 1
+  Zn001:Wall001,        !- Surface name 2
+  0.15,                 !- Angle factor for surface 2
+  Zn001:Roof001,        !- Surface name 3
+  0.10;                 !- Angle factor for surface 3
+\end{lstlisting}
+
+\subsection{Lights}\label{lights-000}
+
+The Lights statement allows you to specify information about a zone's electric lighting system, including design power level and operation schedule, and how the heat from lights is distributed thermally.
+
+A zone may have multiple Lights statements. For example, one statement may describe the general lighting in the zone and another the task lighting. Or you can use multiple Lights statements for a zone that has two or more general lighting systems that differ in design level, schedule, etc.
+
+\subsubsection{Inputs}\label{inputs-2-021}
+
+\paragraph{Field: Name}\label{field-name-2-020}
+
+The name of the Lights object.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-1-000}
+
+The field is the name of the thermal zone (ref: Zone) or ZoneList (ref: ZoneLIst) and links this Lights statement to a thermal zone or set of thermal zones in the buidling. When the ZoneList option is used then this lights definition is applied to each of the zones in the zone list effecting a global definition for the amount of light wattage in the zone. The Zonelist option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
+
+The name of the actual lights object becomes \textless{}Zone Name\textgreater{} \textless{}Lights Object Name\textgreater{} and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-002}
+
+The name of the schedule that modifies the lighting power design level (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The electrical input for lighting in a particular timestep is the product of the design level and the value of this schedule in that timestep. If the design level is the maximum lighting power input the schedule should contain values between 0.0 and 1.0.
+
+\paragraph{Field: Design Level Calculation Method}\label{field-design-level-calculation-method}
+
+This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal lighting level in the Zone. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  LightingLevel
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the lighting level (Watts) for the Zone.~ (The Lighting Level field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The Watts per Zone Floor Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Person
+\end{itemize}
+
+With this choice, the method used will be a factor of lighting level (watts) per person. (The Watts per person field should be filled).
+
+\paragraph{Field: Lighting Level}\label{field-lighting-level}
+
+This is typically the maximum electrical power input (in Watts) to lighting in a zone, including ballasts, if present. This value is multiplied by a schedule fraction (see previous field) to get the lighting power in a particular timestep. In EnergyPlus, this is slightly more flexible in that the lighting design level could be a ``diversity factor'' applied to a schedule of real numbers.
+
+\paragraph{Field: Watts per Zone Floor Area}\label{field-watts-per-zone-floor-area}
+
+This factor (watts/m\(^{2}\)) is used, along with the Zone Floor Area to determine the maximum lighting level as described in the Lighting Level field. The choice from the method field should be ``watts/area''.
+
+\paragraph{Field: Watts per Person}\label{field-watts-per-person}
+
+This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum lighting level as described in the Lighting Level field. The choice from the method field should be ``watts/person''.
+
+\paragraph{Heat Gains from Lights:}\label{heat-gains-from-lights}
+
+The electrical input to lighting ultimately appears as heat that contributes to zone loads or to return air heat gains. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Return Air Fraction, Fraction Radiant and Fraction Visible. A fourth, defined as the fraction of the heat from lights convected to the zone air, is calculated by the program as:
+
+f\(_{convected}\) = 1.0 -- (Return Air Fraction + Fraction Radiant + Fraction Visible)
+
+You will get an error message if Return Air Fraction + Fraction Radiant + Fraction Visible exceeds 1.0.
+
+These fractions depend on the type of lamp and luminaire, whether the luminaire is vented to the return air, etc.
+
+\paragraph{Field: Return Air Fraction}\label{field-return-air-fraction}
+
+The fraction of the heat from lights that goes into the zone return air (i.e., into the zone outlet node). If the return air flow is zero or the zone has no return air system, the program will put this fraction into the zone air. Return Air Fraction should be non-zero only for luminaires that are return-air ducted~ (see Table~\ref{table:approximate-values-of-return-air-fraction} and Figure 51). (However, see the field ``Return Air Fraction Is Calculated from Plenum Temperature,'' below, for an approach to modeling the case where Return Air Fraction is caused by \emph{conduction} between a luminaire that is in contact with a return-air plenum.)
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant-1}
+
+The fraction of heat from lights that goes into the zone as long-wave (thermal) radiation. The program calculates how much of this radiation is absorbed by the inside surfaces of the zone according the area times thermal absorptance product of these surfaces.
+
+\paragraph{Field: Fraction Visible}\label{field-fraction-visible}
+
+The fraction of heat from lights that goes into the zone as visible (short-wave) radiation. The program calculates how much of this radiation is absorbed by the inside surfaces of the zone according the area times solar absorptance product of these surfaces.
+
+Approximate values of Return Air Fraction, Fraction Radiant and Fraction Visible are given in Table~\ref{table:approximate-values-of-return-air-fraction} for overhead fluorescent lighting for a variety of luminaire configurations. The data is based on ASHRAE 1282-RP ``Lighting Heat Gain Distribution in Buildings'' by Daniel E. Fisher and Chanvit Chantrasrisalai.
+
+% table 14
+\begin{longtable}[c]{p{0.8in}>{\raggedright}p{1.6in}>{\raggedright}p{0.9in}>{\raggedright}p{0.9in}>{\raggedright}p{0.9in}>{\raggedright}p{0.9in}}
+\caption{Approximate values of Return Air Fraction, Fraction Radiant and Fraction Visible for overhead fluorescent lighting for different luminaire configurations. \label{table:approximate-values-of-return-air-fraction}} \tabularnewline
+\toprule 
+Fixture No. & Luminaire Feature & Return Air Fraction & Fraction Radiant & Fraction Visible & fconvected \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Approximate values of Return Air Fraction, Fraction Radiant and Fraction Visible for overhead fluorescent lighting for different luminaire configurations.} \tabularnewline
+\toprule 
+Fixture No. & Luminaire Feature & Return Air Fraction & Fraction Radiant & Fraction Visible & \(f_{\rm{convected}}\) \tabularnewline
+\midrule
+\endhead
+
+1 & Recessed, Parabolic Louver, Non-Vented, T8 & 0.31 & 0.22 & 0.20 & 0.27 \tabularnewline
+2 & Recessed, Acrylic Lens, Non-Vented, T8 & 0.56 & 0.12 & 0.20 & 0.12 \tabularnewline
+3 & Recessed, Parabolic Louver, Vented, T8 & 0.28 & 0.19 & 0.20 & 0.33 \tabularnewline
+4 & Recessed, Acrylic Lens, Vented, T8 & 0.54 & 0.10 & 0.18 & 0.18 \tabularnewline
+5 & Recessed, Direct/Indirect, T8 & 0.34 & 0.17 & 0.16 & 0.33 \tabularnewline
+6 & Recessed, Volumetric, T5 & 0.54 & 0.13 & 0.20 & 0.13 \tabularnewline
+7 & Downlights, Compact Fluorescent, DTT & 0.86 & 0.04 & 0.10 & 0.00 \tabularnewline
+8 & Downlights, Compact Fluorescent, TRT & 0.78 & 0.09 & 0.13 & 0.00 \tabularnewline
+9a & Downlights, Incandescent, A21 & 0.29 & 0.10 & 0.6 & 0.01 \tabularnewline
+9b & Downlights, Incandescent, BR40 & 0.21 & 0.08 & 0.71 & 0.00 \tabularnewline
+10 & Surface Mounted, T5HO & 0.00 & 0.27 & 0.23 & 0.50 \tabularnewline
+11 & Pendant, Direct/Indirect, T8 & 0.00 & 0.32 & 0.23 & 0.45 \tabularnewline
+12 & Pendant, Indirect, T5HO & 0.00 & 0.32 & 0.25 & 0.43 \tabularnewline
+ &  &  &  &  &  \tabularnewline \midrule
+1 & Recessed, Parabolic Louver, Non-Vented, T8 - Ducted & 0.27 & 0.27 & 0.21 & 0.25 \tabularnewline
+5 & Recessed, Direct/Indirect, T8 - Ducted & 0.27 & 0.22 & 0.17 & 0.34 \tabularnewline
+ &  &  &  &  &  \tabularnewline \midrule
+1 & Recessed, Parabolic Louver, Non-Vented, T8 - Half Typical Supply Airflow Rate & 0.45 & 0.30 & 0.22 & 0.03 \tabularnewline
+3 & Recessed, Parabolic Louver, Vented, T8 - Half Typical Supply Airflow Rate & 0.43 & 0.25 & 0.21 & 0.11 \tabularnewline
+5 & Recessed, Direct/Indirect, T8 - Half Typical Supply Airflow Rate & 0.43 & 0.27 & 0.18 & 0.12 \tabularnewline
+ &  &  &  &  &  \tabularnewline \midrule
+1 & Recessed, Parabolic Louver, Non-Vented, T8 - Half Typical Supply Airflow Rate & 0.10 & 0.16 & 0.20 & 0.54 \tabularnewline
+3 & Recessed, Parabolic Louver, Vented, T8 - Half Typical Supply Airflow Rate & 0.11 & 0.15 & 0.19 & 0.55 \tabularnewline
+5 & Recessed, Direct/Indirect, T8 - Half Typical Supply Airflow Rate & 0.04 & 0.13 & 0.16 & 0.67 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Field: Fraction Replaceable}\label{field-fraction-replaceable}
+
+This field defines the daylighting control for the LIGHTS object.
+
+If \textbf{Daylighting:Controls} or \textbf{Daylighting:DELight:Controls} is specified for the zone, this field is used as an on/off flag for dimming controls. If set to 0.0, the lights are not dimmed by the daylighting controls. If set to 1.0, the lights are allowed to be dimmed by the daylighting controls.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-002}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Task Lights'', ``Hall Lights'', etc. A new meter for reporting is created for each unique subcategory~ (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the lights will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Return Air Fraction Calculated from Plenum Temperature}\label{field-return-air-fraction-calculated-from-plenum-temperature}
+
+Accepts values Yes or No (the default). Yes is for advanced used only. In this case the program will calculate the return air fraction by assuming that it is due to conduction of some of the light heat into the zone's return air plenum and that the amount of the conduction depends on the plenum air temperature. A Yes value should only be used for luminaires that are recessed and non-vented, as shown in Figure~\ref{fig:vertical-section-through-a-zone-and-its}.
+
+The value you enter for the Return Air Fraction field will be ignored and you can enter, for fluorescent lighting, Fraction Radiant = 0.37 and Fraction Visible = 0.18, as indicated in Table~\ref{table:approximate-values-of-return-air-fraction}.
+
+This feature requires that the coefficients described below be determined from measurements or detailed calculations since they are very sensitive to the luminaire type, lamp type, thermal resistance between fixture and plenum, etc.
+
+If ``Return Air Fraction Is Calculated from Plenum Temperature'' = Yes, the return air fraction is calculated \emph{each timestep} from the following empirical correlation:
+
+\begin{equation}
+  (\rm{Return Air Fraction})_{\rm{calculated}} = C_{1} - C_{2} \times T_{\rm{plenum}}
+\end{equation}
+
+where T\(_{\rm{plenum}}\) is the previous-time-step value of the return plenum air temperature (C),
+
+and C\(_{1}\) and C\(_{2}\) are the values of the coefficients entered in the next two fields.
+
+To compensate for the change in the return air fraction relative to its input value, the program modifies Fraction Radiant and \(f_{\rm{convected}}\) by a scale factor such that
+
+\begin{equation}
+  (\rm{Return Air Fraction})_{\rm{calculated}} + (\rm{Fraction Radiant})_{\rm{modified}} + (f_{\rm{convected}})_{\rm{modified}} + (\rm{Fraction Visible})_{\rm{input}} = 1.0
+\end{equation}
+
+It is assumed that Fraction Visible is a constant equal to its input value.
+
+\paragraph{Field: Return Air Fraction Function of Plenum Temperature Coefficient 1}\label{field-return-air-fraction-function-of-plenum-temperature-coefficient-1}
+
+The coefficient C\(_{1}\) in the equation for (Return Air Fraction)\(_{calculated}\).
+
+\paragraph{Field: Return Air Fraction Function of Plenum Temperature Coefficient 2}\label{field-return-air-fraction-function-of-plenum-temperature-coefficient-2}
+
+The coefficient C\(_{2}\) in the equation for (Return Air Fraction)\(_{calculated}\). Its units are 1/\(^{O}\)C.
+
+\begin{figure}[hbtp] % fig 52
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image087.png}
+\caption{Vertical section through a zone and its return air plenum showing recessed lighting (not to scale). The heat from lights is divided into four fractions, three of which --- ReturnAirFraction, FractionRadiant and FractionConvected --- depend on plenum air temperature. \protect \label{fig:vertical-section-through-a-zone-and-its}}
+\end{figure}
+
+An IDF example:
+
+\begin{lstlisting}
+Lights,
+  RIGHT FORK Lights 1,  !- Name
+  RIGHT FORK,           !- Zone Name
+  Office Lighting,      !- SCHEDULE Name
+  LightingLevel,        !- Design Level calculation method
+  1039.706,             !- Lighting Level {W}
+  0.0000000E+00,        !- Return Air Fraction
+  0.4000000,            !- Fraction Radiant
+  0.2000000,            !- Fraction Visible
+  1.0,                  !- Fraction Replaceable
+  GeneralLights;        !- End-Use Subcategory
+\end{lstlisting}
+
+Global Lights Object:
+
+\begin{lstlisting}
+ZoneList,AllOccupiedZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
+
+Lights,
+  AllZones with Lights, !- Name
+  AllOccupiedZones,     !- Zone or ZoneList Name
+  LIGHTS-1,             !- Schedule Name
+  Watts/Area,           !- Design Level Calculation Method
+  ,                     !- Lighting Level {W}
+  16,                   !- Watts per Zone Floor Area {W/m2}
+  ,                     !- Watts per Person {W/person}
+  0.2,                  !- Return Air Fraction
+  0.59,                 !- Fraction Radiant
+  0.2,                  !- Fraction Visible
+  0,                    !- Fraction Replaceable
+  GeneralLights;        !- End-Use Subcategory
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-012}
+
+If daylighting controls are operating in the zone, all of the Lights objects with a Fraction Replaceble~ greater than zero will be reduced by a multiplicative factor that accounts for how much the electric lighting is lowered due to daylighting.
+
+Lights objects have output variables for individual objects and for zone totals.
+
+\begin{itemize}
+\item
+  Zone,Average,Lights Electric Power {[}W{]}
+\item
+  Zone,Sum,Lights Radiant Heat Gain {[}J{]}
+\item
+  Zone,Average,Lights Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Lights Visible Radiation Heating Energy {[}J{]}
+\item
+  Zone,Average,Lights Visible Radiation Heating Rate {[}W{]}
+\item
+  Zone,Sum,Lights Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Lights Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Lights Return Air Heating Energy {[}J{]}
+\item
+  Zone,Average,Lights Return Air Heating Rate {[}W{]}
+\item
+  Zone,Sum,Lights Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Lights Total Heating Rate {[}W{]}
+\item
+  Zone,Sum,Lights Electric Energy {[}J{]}
+\item
+  Zone,Average,Zone Lights Electric Power {[}W{]}
+\item
+  Zone,Sum,Zone Lights Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Lights Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Lights Visible Radiation Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Lights Visible Radiation Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Lights Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Lights Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Lights Return Air Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Lights Return Air Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Lights Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Lights Total Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Lights Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Lights Electric Power {[}W{]}}\label{lights-electric-power-w}
+
+The electric power input for the lights.
+
+\paragraph{Lights Radiant Heating Rate {[}W{]}}\label{lights-radiant-heating-rate-w}
+
+\paragraph{Lights Radiant Heating Energy {[}J{]}}\label{lights-radiant-heating-energy-j}
+
+The amount of heat gain from lights that is in the form of long-wave (thermal) radiation entering the zone. This heat is absorbed by the inside surfaces of the zone according to an area times long-wave absorptance weighting scheme.
+
+\paragraph{Lights Visible Radiation Heating Rate {[}W{]}}\label{lights-visible-radiation-heating-rate-w}
+
+\paragraph{Lights Visible Radiation Heating Energy {[}J{]}}\label{lights-visible-radiation-heating-energy-j}
+
+The amount of heat gain from lights that is in the form of visible (short-wave) radiation entering the zone. This heat is absorbed by the inside surfaces of the zone according~ to an area times short-wave absorptance weighting scheme.
+
+\paragraph{Lights Convective Heating Rate {[}W{]}}\label{lights-convective-heating-rate-w}
+
+\paragraph{Lights Convective Heating Energy {[}J{]}}\label{lights-convective-heating-energy-j}
+
+The amount of heat gain from lights that is convected to the zone air.
+
+\paragraph{Lights Return Air Heating Rate {[}W{]}}\label{lights-return-air-heating-rate-w}
+
+\paragraph{Lights Return Air Heating Energy {[}J{]}}\label{lights-return-air-heating-energy-j}
+
+The amount of heat gain from lights that goes into the zone's return air (and, therefore, does not directly contribute to the zone load). If the zone has no return air system or the zone's air system is off, this heat will be added to the zone air.
+
+\paragraph{Lights Total Heating Rate {[}W{]}}\label{lights-total-heating-rate-w}
+
+\paragraph{Lights Total Heating Energy {[}J{]}}\label{lights-total-heating-energy-j}
+
+The total heat gain from lights. It is the sum of the following four outputs, i.e., Total Heat Gain = Return Air Heat Gain + Radiant Heat Gain + Visible Heat Gain + Convective Heat Gain. It is also equal to the electrical input to the lights.
+
+\paragraph{Lights Electric Energy {[}J{]}}\label{lights-electric-energy-j}
+
+The lighting electrical consumption including ballasts, if present. These will have the same value as Lights Total Heating Energy (above).
+
+\paragraph{Zone Lights Electric Power {[}W{]}}\label{zone-lights-electric-power-w}
+
+The electric power input for all lights in the zone.
+
+\paragraph{Zone Lights Radiant Heating Rate {[}W{]}}\label{zone-lights-radiant-heating-rate-w}
+
+\paragraph{Zone Lights Radiant Heating Energy {[}J{]}}\label{zone-lights-radiant-heating-energy-j}
+
+The amount of heat gain from all lights in the zone that is in the form of long-wave (thermal) radiation entering the zone. This heat is absorbed by the inside surfaces of the zone according to an area times long-wave absorptance weighting scheme.
+
+\paragraph{Zone Lights Visible Radiation Heating Rate {[}W{]}}\label{zone-lights-visible-radiation-heating-rate-w}
+
+\paragraph{Zone Lights Visible Radiation Heating Energy {[}J{]}}\label{zone-lights-visible-radiation-heating-energy-j}
+
+The amount of heat gain from all lights in the zone that is in the form of visible (short-wave) radiation entering the zone. This heat is absorbed by the inside surfaces of the zone according~ to an area times short-wave absorptance weighting scheme.
+
+\paragraph{Zone Lights Convective Heating Rate {[}W{]}}\label{zone-lights-convective-heating-rate-w}
+
+\paragraph{Zone Lights Convective Heating Energy {[}J{]}}\label{zone-lights-convective-heating-energy-j}
+
+The amount of heat gain from all lights in the zone that is convected to the zone air.
+
+\paragraph{Zone Lights Return Air Heating Rate {[}W{]}}\label{zone-lights-return-air-heating-rate-w}
+
+\paragraph{Zone Lights Return Air Heating Energy {[}J{]}}\label{zone-lights-return-air-heating-energy-j}
+
+The amount of heat gain from all lights in the zone that goes into the zone's return air (and, therefore, does not directly contribute to the zone load). If the zone has no return air system or the zone's air system is off, this heat will be added to the zone air.
+
+\paragraph{Zone Lights Total Heating Rate {[}W{]}}\label{zone-lights-total-heating-rate-w}
+
+\paragraph{Zone Lights Total Heating Energy {[}J{]}}\label{zone-lights-total-heating-energy-j}
+
+The total heat gain from all lights in the zone. It is the sum of the following four outputs, i.e., Total Heat Gain = Return Air Heat Gain + Radiant Heat Gain + Visible Heat Gain + Convective Heat Gain. It is also equal to the electrical input to the lights.
+
+\paragraph{Zone Lights Electric Energy {[}J{]}}\label{zone-lights-electric-energy-j}
+
+The lighting electrical consumption for all lights in the zone including ballasts, if present. This will have the same value as Zone Lights Total Heating Energy (above). However, this amount is also shown in the Electricity meters that are associated with the zone:
+
+Electricity:Facility,
+
+Electricity:Building,
+
+Electricity:Zone:\textless{}Zone Name\textgreater{}.
+
+In addition, depending on use, it will be shown in:
+
+InteriorLights: Electricity and
+
+InteriorLights:Electricity:Zone :\textless{}Zone Name\textgreater{}.
+
+\subsubsection{Outputs}\label{outputs-3-010}
+
+As described in the Lights Outputs, values for lights will show up on the following meters:
+
+% table 15
+\begin{longtable}[c]{>{\raggedright}p{3.0in}p{1.5in}p{1.5in}}
+\caption{Distribution of Lights to Meters \label{table:distribution-of-lights-to-meters}} \tabularnewline
+\toprule 
+Meter Name & Scope & Lights Specfics \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Distribution of Lights to Meters} \tabularnewline
+\toprule 
+Meter Name & Scope & Lights Specfics \tabularnewline
+\midrule
+\endhead
+
+Electricity:Facility & Entire Facility & All \tabularnewline
+Electricity:Building & All Zones & All \tabularnewline
+Electricity:Zone: <Zone Name> & Specific Zone & All \tabularnewline
+InteriorLights:Electricity & All Zones & Lights Use \tabularnewline
+InteriorLights:Electricity:Zone: <Zone Name> & Specific Zone & Lights Use \tabularnewline
+<End-Use Subcategory> :InteriorLights:Electricity & Specific Subcategory & Lights Use \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{ElectricEquipment}\label{electricequipment}
+
+The object models equipment in the zone which consumes electricity, such as computers, televisions, and cooking equipment, also known as ``plug loads.'' All of the energy consumed by the equipment becomes a heat gain in the zone or is lost (exhausted) as specified below.
+
+\subsubsection{Inputs}\label{inputs-3-019}
+
+\paragraph{Field: Name}\label{field-name-3-017}
+
+The name of the ElectricEquipment object.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-2}
+
+This field is the name of the zone (ref: Zone) or ZoneList (ref: ZoneList) and attaches a particular electric equipment statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this electric equipment definition is applied to each of the zones in the zone list effecting a global definition for the amount of electric wattage in the zone. The Zonelist option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
+
+The name of the actual electric equipment object becomes \textless{}Zone Name\textgreater{} \textless{}ElectricEquipment Object Name\textgreater{} and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-1-001}
+
+This field is the name of the schedule that modifies the design level parameter for electric equipment (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The actual electrical input for equipment in a zone as defined by this statement is the product of the design level field and the value of the schedule specified by name in this field.
+
+\paragraph{Field: Design Level Calculation Method}\label{field-design-level-calculation-method-1}
+
+This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal electric equipment level in the Zone. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  EquipmentLevel
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the electric equipment level (Watts) for the Zone.~ (The Design Level field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The Watts per Zone Floor Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Person
+\end{itemize}
+
+With this choice, the method used will be a factor of equipment level (watts) per person. (The Watts per Person field should be filled).
+
+\paragraph{Field: Design Level}\label{field-design-level-000}
+
+This field (in Watts) is typically used to represent the maximum electrical input to equipment in a zone that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the electric equipment design level could be a ``diversity factor'' applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour, the design level field is constant for all simulation environments.
+
+\paragraph{Field: Watts per Zone Floor Area}\label{field-watts-per-zone-floor-area-1}
+
+This factor (watts/m\(^{2}\)) is used, along with the Zone Area to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be ``Watts/Area''.
+
+\paragraph{Field: Watts per Person}\label{field-watts-per-person-1}
+
+This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be ``Watts/Person''.
+
+\paragraph{Heat Gains from Electric Equipment:}\label{heat-gains-from-electric-equipment}
+
+The electrical input to the equipment ultimately appears as heat that contributes to zone loads. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Fraction Latent, Fraction Radiant and Fraction Lost. A fourth, defined as the fraction of the heat from electric equipment convected to the zone air, is calculated by the program as:
+
+\begin{equation}
+  f_{\rm{convected}} = 1.0 - (\rm{Fraction Latent} + \rm{Fraction Radiant} + \rm{Fraction Lost})
+\end{equation}
+
+You will get an error message if Fraction Latent + Fraction Radiant + Fraction Lost exceeds 1.0.
+
+\paragraph{Field: Fraction Latent}\label{field-fraction-latent}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of latent heat given off by electric equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by electric equipment to give the amount of latent energy produced by the electric equipment. This energy affects the moisture balance within the zone.
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant-2}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of long-wave radiant heat being given off by electric equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by electric equipment to give the amount of long wavelength radiation gain from electric equipment in a zone.
+
+\paragraph{Field: Fraction Lost}\label{field-fraction-lost}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of ``lost'' heat being given off by electric equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by electric equipment to give the amount of heat which is ``lost'' and does not impact the zone energy balances. This might correspond to electrical energy converted to mechanical work or heat that is vented to the atmosphere.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-1-001}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Computers'', ``Copy Machines'', etc. A new meter for reporting is created for each unique subcategory~ (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+An IDF example:
+
+\begin{lstlisting}
+ElectricEquipment,
+  DORM ROOMS AND COMMON AREAS ElecEq 1, !- Name
+  DORM ROOMS AND COMMON AREAS,          !- Zone Name
+  Residence Equipment,                  !- SCHEDULE Name
+  EquipmentLevel,                       !- Design Level calculation method
+  9210.921,                             !- Design Level {W}
+  ,                                     !- Watts per Zone Floor Area {watts/m2}
+  ,                                     !- Watts per Person {watts/person}
+  0.0000000E+00,                        !- Fraction Latent
+  0.3000000,                            !- Fraction Radiant
+  0.0000000E+00,                        !- Fraction Lost
+  Computers;                            !- End-use Subcategory
+\end{lstlisting}
+
+Global ElectricEquipment example:
+
+\begin{lstlisting}
+ZoneList,AllOccupiedZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
+
+ElectricEquipment,
+  AllZones with Electric Equipment,     !- Name
+  AllOccupiedZones,                     !- Zone or ZoneList Name
+  EQUIP-1,                              !- Schedule Name
+  Watts/Person,                         !- Design Level Calculation Method
+  ,                                     !- Design Level {W}
+  ,                                     !- Watts per Zone Floor Area {W/m2}
+  96,                                   !- Watts per Person {W/person}
+  0,                                    !- Fraction Latent
+  0.3,                                  !- Fraction Radiant
+  0;                                    !- Fraction Lost
+\end{lstlisting}
+
+\subsection{GasEquipment}\label{gasequipment}
+
+The object models equipment in the zone which consumes natural gas, such as cooking equipment or a gas fireplace. All of the energy consumed by the equipment becomes a heat gain in the zone or is lost (exhausted) as specified below.
+
+\subsubsection{Inputs}\label{inputs-4-017}
+
+\paragraph{Field: Name}\label{field-name-4-014}
+
+The name of the GasEquipment object.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-3}
+
+This field is the name of the thermal zone (ref: Zone) or ZoneList (ref: ZoneList) and attaches a particular gas equipment statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this gas equipment definition is applied to each of the zones in the zone list effecting a global definition for the amount of gas in the zone. The Zonelist option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
+
+The name of the actual gas equipment object becomes \textless{}Zone Name\textgreater{} \textless{}GasEquipment Object Name\textgreater{} and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-2-001}
+
+This field is the name of the schedule that modifies the design level parameter for gas equipment (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The actual energy input for gas equipment in a zone as defined by this statement is the product of the design level field and the value of the schedule specified by name in this field.
+
+\paragraph{Field: Design Level Calculation Method}\label{field-design-level-calculation-method-2}
+
+This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal gas equipment level in the Zone. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  EquipmentLevel
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the gas equipment level (Watts) for the Zone.~ (The Design Level field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Area or Power/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The Power per Zone Floor Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Person or Power/Person
+\end{itemize}
+
+With this choice, the method used will be a factor of equipment level (watts) per person. (The Power per Person field should be filled).
+
+\paragraph{Field: Design Level}\label{field-design-level-1-000}
+
+This field (in Watts) is typically used to represent the maximum energy input to gas equipment in a zone that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the gas equipment design level could be a ``diversity factor'' applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour, the design level field is constant for all simulation environments.
+
+\paragraph{Field: Power per Zone Floor Area}\label{field-power-per-zone-floor-area}
+
+This factor (watts/m\(^{2}\)) is used, along with the Zone Area to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be ``\textbf{Watts/Area}'' or ``\textbf{Power/Area}''.
+
+\paragraph{Field: Power per Person}\label{field-power-per-person}
+
+This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be ``\textbf{Watts/Person}'' or ``\textbf{Power/Person}''.
+
+\paragraph{Heat Gains from Gas Equipment:}\label{heat-gains-from-gas-equipment}
+
+The fuel input to the equipment ultimately appears as heat that contributes to zone loads. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Fraction Latent, Fraction Radiant and Fraction Lost. A fourth, defined as the fraction of the heat from gas equipment convected to the zone air, is calculated by the program as:
+
+\begin{equation}
+  f_{convected} = 1.0 - (\rm{Fraction Latent} + \rm{Fraction Radiant} + \rm{Fraction Lost})
+\end{equation}
+
+You will get an error message if Fraction Latent + Fraction Radiant + Fraction Lost exceeds 1.0.
+
+\paragraph{Field: Fraction Latent}\label{field-fraction-latent-1}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of latent heat given off by gas equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by gas equipment to give the amount of latent energy produced by the gas equipment. This energy affects the moisture balance within the zone.
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant-3}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of long-wave radiant heat being given off by gas equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by gas equipment to give the amount of long wavelength radiation gain from gas equipment in a zone.
+
+\paragraph{Field: Fraction Lost}\label{field-fraction-lost-1}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of ``lost'' heat being given off by gas equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by gas equipment to give the amount of heat which is ``lost'' and does not impact the zone energy balances. This might correspond to input energy converted to mechanical work or heat that is vented to the atmosphere.
+
+\paragraph{Field: Carbon Dioxide Generation Rate}\label{field-carbon-dioxide-generation-rate-1}
+
+This numeric input field specifies carbon dioxide generation rate with units of m3/s-W. The default value of 0.0 assumes the equipment is fully vented to outdoors. In the absence of better information, the user might consider using a value of 3.45E-8 m3/s-W which assumes the equipment is not vented to outdoors. This value is converted from natural gas CO\(_{2}\) emission rate at 11.7 lbs CO\(_{2}\) per therm. The CO\(_{2}\) emission rate is provided by U.S. Energy Information Administration, ``Frequently Asked Questions - Environment, Questions About Environmental Emissions'',~ http://tonto.eia.doe.gov/ask/environment\_faqs.asp\#CO2\_quantity, January 2010. The maximum value for this input field is 3.45E-7 m3/s-W.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-2-001}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Cooking'', ``Clothes Drying'', etc. A new meter for reporting is created for each unique subcategory~ (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+An IDF example:
+
+\begin{lstlisting}
+GasEquipment,
+  DORM ROOMS AND COMMON AREAS GasEq 1,  !- Name
+  DORM ROOMS AND COMMON AREAS,          !- Zone Name
+  Gas Eq Sch,                           !-Schedule Name
+  EquipmentLevel,                       !- Design Level Calculation Method
+  29287.51,                             !- Design Level {W}
+  ,                                     !- Power per Zone Floor Area {W/m2}
+  ,                                     !- Power per Person {W/Person}
+  0,                                    !- Fraction Latent
+  0.3,                                  !- Fraction Radiant
+  0,                                    !- Fraction Lost
+  0,                                    !- Carbon Dioxide Generation Rate {m3/s-W}
+  Cooking;                              !- End-Use Subcategory
+\end{lstlisting}
+
+Global Gas Equipment example:
+
+\begin{lstlisting}
+ZoneList,OfficeZones,Left Fork, Middle Fork, Right Fork;
+
+GasEquipment,
+  Office Zones with Gas,                !- Name
+  OfficeZones,                          !- Zone Name
+  Gas Eq Sch,                           !- Schedule Name
+  Watts/Area,                           !- Design Level Calculation Method
+  ,                                     !- Design Level {W}
+  197,                                  !- Power per Zone Floor Area {W/m2}
+  ,                                     !- Power per Person {W/Person}
+  0.0000000E+00,                        !- Fraction Latent
+  0.3000000,                            !- Fraction Radiant
+  0.0000000E+00;                        !- Fraction Lost
+\end{lstlisting}
+
+\subsection{HotWaterEquipment}\label{hotwaterequipment}
+
+The object models hot water equipment in the zone which consumes district heating, such as cooking equipment or process loads. All of the energy consumed by the equipment becomes a heat gain in the zone or is lost (exhausted) as specified below. This object consumes district heating energy directly and does not cause a load on a hot water plant loop or water heater. For domestic hot water uses, such as sinks and showers, see WaterUse:Equipment.
+
+\subsubsection{Inputs}\label{inputs-5-015}
+
+\paragraph{Field: Name}\label{field-name-5-011}
+
+The name of the HotWaterEquipment object.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-4}
+
+This field is the name of the thermal zone (ref: Zone) or ZoneList (ref: ZoneList) and attaches a particular hot water equipment statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this hot water equipment definition is applied to each of the zones in the zone list effecting a global definition for the amount of hot water in the zone. The Zonelist option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
+
+The name of the actual hot water equipment object becomes \textless{}Zone Name\textgreater{} \textless{}HotWaterEquipment Object Name\textgreater{} and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-3-000}
+
+This field is the name of the schedule that modifies the design level parameter for hot water equipment (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The actual energy input for hot water equipment in a zone as defined by this statement is the product of the design level field and the value of the schedule specified by name in this field.
+
+\paragraph{Field: Design Level Calculation Method}\label{field-design-level-calculation-method-3}
+
+This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal hot water equipment level in the Zone. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  EquipmentLevel
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the hot water equipment level (Watts) for the Zone.~ (The Design Level field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Area or Power/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The Power per Zone Floor Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Person or Power/Person
+\end{itemize}
+
+With this choice, the method used will be a factor of equipment level (watts) per person. (The Power per Person field should be filled).
+
+\paragraph{Field: Design Level}\label{field-design-level-2-000}
+
+This field (in Watts) is typically used to represent the maximum energy input to hot water equipment in a zone that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the hot water equipment design level could be a ``diversity factor'' applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour, the design level field is constant for all simulation environments.
+
+\paragraph{Field: Power per Zone Floor Area}\label{field-power-per-zone-floor-area-1}
+
+This factor (watts/m\(^{2}\)) is used, along with the Zone Area to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be ``\textbf{Watts/Area}'' or ``\textbf{Power/Area}''.
+
+\paragraph{Field: Power per Person}\label{field-power-per-person-1}
+
+This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be ``\textbf{Watts/Person}'' or ``\textbf{Power/Person}''.
+
+\paragraph{Heat Gains from Hot Water Equipment:}\label{heat-gains-from-hot-water-equipment}
+
+The fuel input to the equipment ultimately appears as heat that contributes to zone loads. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Fraction Latent, Fraction Radiant and Fraction Lost. A fourth, defined as the fraction of the heat from hot water equipment convected to the zone air, is calculated by the program as:
+
+\begin{equation}
+  f_{\rm{convected}} = 1.0 - (\rm{Fraction Latent} + \rm{Fraction Radiant} + \rm{Fraction Lost})
+\end{equation}
+
+You will get an error message if Fraction Latent + Fraction Radiant + Fraction Lost exceeds 1.0.
+
+\paragraph{Field: Fraction Latent}\label{field-fraction-latent-2}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of latent heat given off by hot water equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by hot water equipment to give the amount of latent energy produced by the hot water equipment. This energy affects the moisture balance within the zone.
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant-4}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of long-wave radiant heat being given off by hot water equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by hot water equipment to give the amount of long wavelength radiation gain from hot water equipment in a zone.
+
+\paragraph{Field: Fraction Lost}\label{field-fraction-lost-2}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of ``lost'' heat being given off by hot water equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by hot water equipment to give the amount of heat which is ``lost'' and does not impact the zone energy balances. This might correspond to input energy converted to mechanical work or heat that is vented to the atmosphere.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-3-000}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Cooking'', ``Clothes Drying'', etc. A new meter for reporting is created for each unique subcategory~ (ref: Output:Meter obejct). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+IDF Examples:
+
+\begin{lstlisting}
+HotWaterEquipment,
+  SPACE2-1 HWEq 1,    !- Name
+  SPACE2-1,           !- Zone Name
+  EQUIP-1,            !- SCHEDULE Name
+  EquipmentLevel,     !- Design Level calculation method
+  300,                !- Design Level {W}
+  ,                   !- Power per Zone Floor Area {watts/m2}
+  ,                   !- Power per Person {watts/person}
+  0.2,                !- Fraction Latent
+  0.1,                !- Fraction Radiant
+  0.5,                !- Fraction Lost
+  Dishwashing;        !- End-Use Subcategory
+\end{lstlisting}
+
+Global Hot Water Equipment example:
+
+\begin{lstlisting}
+ZoneList,OfficeZones,Left Fork, Middle Fork, Right Fork;
+
+HotWaterEquipment,
+  Office Zones with HoWater Equipment,!- Name
+  OfficeZones,                        !- Zone Name
+  HotWater Eq Sch,                    !- Schedule Name
+  Watts/Area,                         !- Design Level Calculation Method
+  ,                                   !- Design Level {W}
+  50,                                 !- Power per Zone Floor Area {W/m2}
+  ,                                   !- Power per Person {W/Person}
+  0.0000000E+00,                      !- Fraction Latent
+  0.3000000,                          !- Fraction Radiant
+  0.0000000E+00;                      !- Fraction Lost
+\end{lstlisting}
+
+\subsection{SteamEquipment}\label{steamequipment}
+
+The object models steam equipment in the zone which consumes district heating, such as cooking equipment or process loads. All of the energy consumed by the equipment becomes a heat gain in the zone or is lost (exhausted) as specified below. This object consumes district heating energy directly and does not cause a load on a steam plant loop.
+
+\subsubsection{Inputs}\label{inputs-6-012}
+
+\paragraph{Field: Name}\label{field-name-6-009}
+
+The name of the SteamEquipment object.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-5}
+
+This field is the name of the thermal zone (ref: Zone) and attaches a particular steam equipment statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this steam equipment definition is applied to each of the zones in the zone list effecting a global definition for the amount of steam in the zone. This option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-4-000}
+
+This field is the name of the schedule that modifies the design level parameter for steam equipment (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The actual energy input for steam equipment in a zone as defined by this statement is the product of the design level field and the value of the schedule specified by name in this field.
+
+\paragraph{Field: Design Level Calculation Method}\label{field-design-level-calculation-method-4}
+
+This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal steam equipment level in the Zone. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  EquipmentLevel
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the steam equipment level (Watts) for the Zone.~ (The Design Level field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Area or Power/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The Power per Zone Floor Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Person or Power/Person
+\end{itemize}
+
+With this choice, the method used will be a factor of equipment level (watts) per person. (The Power per Person field should be filled).
+
+\paragraph{Field: Design Level}\label{field-design-level-3}
+
+This field (in Watts) is typically used to represent the maximum energy input to steam equipment in a zone that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the steam equipment design level could be a ``diversity factor'' applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour, the design level field is constant for all simulation environments.
+
+\paragraph{Field: Power per Zone Floor Area}\label{field-power-per-zone-floor-area-2}
+
+This factor (watts/m\(^{2}\)) is used, along with the Zone Area to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be ``\textbf{Watts/Area}'' or ``\textbf{Power/Area}''.
+
+\paragraph{Field: Power per Person}\label{field-power-per-person-2}
+
+This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be ``\textbf{Watts/Person}'' or ``\textbf{Power/Person}''.
+
+\paragraph{Heat Gains from Steam Equipment:}\label{heat-gains-from-steam-equipment}
+
+The fuel input to the equipment ultimately appears as heat that contributes to zone loads. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Fraction Latent, Fraction Radiant and Fraction Lost. A fourth, defined as the fraction of the heat from steam equipment convected to the zone air, is calculated by the program as:
+
+\begin{equation}
+  f_{\rm{convected}} = 1.0 - (\rm{Fraction Latent} + \rm{Fraction Radiant} + \rm{Fraction Lost})
+\end{equation}
+
+You will get an error message if Fraction Latent + Fraction Radiant + Fraction Lost exceeds 1.0.
+
+\paragraph{Field: Fraction Latent}\label{field-fraction-latent-3}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of latent heat given off by steam equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by steam equipment to give the amount of latent energy produced by the steam equipment. This energy affects the moisture balance within the zone.
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant-5}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of long-wave radiant heat being given off by steam equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by steam equipment to give the amount of long wavelength radiation gain from steam equipment in a zone.
+
+\paragraph{Field: Fraction Lost}\label{field-fraction-lost-3}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of ``lost'' heat being given off by steam equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by steam equipment to give the amount of heat which is ``lost'' and does not impact the zone energy balances. This might correspond to input energy converted to mechanical work or heat that is vented to the atmosphere.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-4-000}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Cooking'', ``Clothes Drying'', etc. A new meter for reporting is created for each unique subcategory~ (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+IDF Examples:
+
+\begin{lstlisting}
+
+SteamEquipment,
+  SPACE4-1 ElecEq 1, !- Name
+  SPACE4-1,          !- Zone Name
+  EQUIP-1,           !- SCHEDULE Name
+  EquipmentLevel,    !- Design Level calculation method
+  1050,              !- Design Level {W}
+  ,                  !- Power per Zone Floor Area {watts/m2}
+  ,                  !- Power per Person {watts/person}
+  0.5,               !- Fraction Latent
+  0.3,               !- Fraction Radiant
+  0,                 !- Fraction Lost
+  Laundry;           !- End-Use Subcategory
+\end{lstlisting}
+
+\subsection{SwimmingPool:Indoor}\label{swimmingpoolindoor}
+
+The Indoor Swimming Pool object is used to describe the indoor swimming pools that are exposed to the internal environment. There are several rules that should be noted regarding the specification of an indoor pool in EnergyPlus. First, the pool is linked to a surface that must be a floor. The pool is assumed to cover the entire floor to which it is linked. If the pool only covers part of the floor in the actual building, then the user must break the floor up into multiple sections.
+
+As pools attempt to achieve a particular water temperature and have a variety of heat losses, heating equipment is necessary to maintain the proper setpoint temperature. In EnergyPlus, the pool itself becomes part of the demand side of a plant loop with heating equipment on the supply side providing whatever heating is needed to maintain the desired temperature. This heating equipment as well as the loop connections must be entered separately and the input shown in this section only details what is needed to specify the pool itself.
+
+The following information is useful for defining and modeling an indoor pool in EnergyPlus. For more information on the algorithm used for this model or details on some of the input parameters, please reference the indoor pool section of the EnergyPlus Engineering Reference document.
+
+\subsubsection{Inputs}\label{inputs-7-012}
+
+\paragraph{Field: Name}\label{field-name-7-008}
+
+This is a unique name associated with the indoor swimming pool.
+
+\paragraph{Field: Surface Name}\label{field-surface-name-1-000}
+
+This is the name of the surface (floor) where the pool is located. Pools are not allowed on any surfaces other than a floor.
+
+\paragraph{Field: Average Depth}\label{field-average-depth}
+
+This field is the average depth of the pool in meters. If the pool has variable depth, the average depth should be specified to achieve the proper volume of water in the pool.
+
+\paragraph{Field: Activity Factor Schedule Name}\label{field-activity-factor-schedule-name}
+
+This field references a schedule that contains values for pool activity. This parameter can be varied using the schedule named here, and it has an impact on the amount of evaporation that will take place from the pool to the surrounding zone air. For example values of the activity factor and what impact it will have on the evaporation of water from the pool, please refer to indoor swimming pool section of the EnergyPlus Engineering Reference document. If left blank, the activity factor will be assumed to be unity.
+
+\paragraph{Field: Make-up Water Supply Schedule Name}\label{field-make-up-water-supply-schedule-name}
+
+The scheduled named by this field establishes a cold water temperature {[}C{]} for the water that replaces the water which is lost from the pool due to evaporation. If blank, water temperatures are calculated by the Site:WaterMainsTemperature object. This field (even if blank) overrides the Cold Water Supply Temperature Schedule in all of the listed WaterUse:Equipment objects.
+
+\paragraph{Field: Cover Schedule Name}\label{field-cover-schedule-name}
+
+This schedule defines when the pool water cover is available and affects the evaporation, convection, and radiation rate calculations. A schedule value of 0.0 means that the pool is not covered. A schedule value of 1.0 means the pool is 100\% covered. The pool may be fully covered, fully open (uncovered), or partially covered (a value between 0.0 and 1.0). The user also has the option to control the evaporation, convection, short-wavelength radiation, and long-wavelength radiation factors when the pool is covered. These terms are discussed in the next four fields.
+
+\paragraph{Field: Cover Evaporation Factor}\label{field-cover-evaporation-factor}
+
+This input field can optionally be used to modify the pool evaporation rate and is used in conjunction with the pool cover factor defined by the Pool Cover Schedule field (see above). The value for this parameter can normally range from 0.0 to 1.0, where 1 means that the pool cover completely eliminates evaporation from the pool surface, 0 means the pool cover has no effect on evaporation, and fractions in between 0 and 1 result in a fractional reduction in evaporation by the pool cover. So, if this parameter is 0.5 and the pool is 50\% covered, the overall reduction in evaporation from a fully uncovered pool is 25\% or 0.25.
+
+\paragraph{Field: Cover Convection Factor}\label{field-cover-convection-factor}
+
+This input field can optionally be used to modify the pool convection rate and is used in conjunction with the pool cover factor defined by the Pool Cover Schedule field (see above). The value for this parameter can normally range from 0.0 to 1.0, where 1 means that the pool cover completely eliminates convection from the pool surface, 0 means the pool cover has no effect on convection, and fractions in between 0 and 1 result in a fractional reduction in convection by the pool cover. So, if this parameter is 0.5 and the pool is 50\% covered, the overall reduction in convection from a fully uncovered pool is 25\% or 0.25.
+
+\paragraph{Field: Cover Short-Wavelength Radiation Factor}\label{field-cover-short-wavelength-radiation-factor}
+
+This input field can optionally be used to modify the pool short-wavelength radiation rate and is used in conjunction with the pool cover factor defined by the Pool Cover Schedule field (see above). The value for this parameter can normally range from 0.0 to 1.0, where 1 means that the pool cover completely eliminates short-wavelength radiation from the pool surface, 0 means the pool cover has no effect on short-wavelength radiation, and fractions in between 0 and 1 result in a fractional reduction in short-wavelength radiation by the pool cover. So, if this parameter is 0.5 and the pool is 50\% covered, the overall reduction in short-wavelength radiation from a fully uncovered pool is 25\% or 0.25. Note that with radiation terms that whatever portion of the short-wavelength radiation is blocked by the cover is transferred via convection to the surrounding zone air.
+
+\paragraph{Field: Cover Long-Wavelength Radiation Factor}\label{field-cover-long-wavelength-radiation-factor}
+
+This input field can optionally be used to modify the pool long-wavelength radiation rate and is used in conjunction with the pool cover factor defined by the Pool Cover Schedule field (see above). The value for this parameter can normally range from 0.0 to 1.0, where 1 means that the pool cover completely eliminates long-wavelength radiation from the pool surface, 0 means the pool cover has no effect on long-wavelength radiation, and fractions in between 0 and 1 result in a fractional reduction in long-wavelength radiation by the pool cover. So, if this parameter is 0.5 and the pool is 50\% covered, the overall reduction in long-wavelength radiation from a fully uncovered pool is 25\% or 0.25. Note that with radiation terms that whatever portion of the long-wavelength radiation is blocked by the cover is transferred via convection to the surrounding zone air.
+
+\paragraph{Field: Pool Water Inlet Node}\label{field-pool-water-inlet-node}
+
+This input is the name of the node on the demand side of a plant loop that leads into the pool. From the standpoint of an EnergyPlus input file, the pool sits on a plant demand loop, and the pump and heater reside on the plant supply loop. The pool heater and pump must be defined by other existing EnergyPlus input.
+
+\paragraph{Field: Pool Water Outlet Node}\label{field-pool-water-outlet-node}
+
+This input is the name of the node on the demand side of a plant loop that leads out of the pool. From the standpoint of an EnergyPlus input file, the pool sits on a plant demand loop, and the pump and heater reside on the plant supply loop. The pool heater and pump must be defined by other existing EnergyPlus input.
+
+\paragraph{Field: Pool Water Maximum Flow Rate}\label{field-pool-water-maximum-flow-rate}
+
+This input is the maximum water volumetric flow rate in m3/s going between the pool and the water heating equipment. This along with the pool setpoint temperature and the heating plant equipment outlet temperature will establish the maximum heat addition to the pool. This flow rate to the pool will be varied in an attempt to reach the desired pool water setpoint temperature (see Setpoint Temperature Schedule below).
+
+\paragraph{Field: Pool Miscellaneous Equipment Power}\label{field-pool-miscellaneous-equipment-power}
+
+This input defines the power consumption rate of miscellaneous equipment such as the filtering and chlorination technology associated with the pool. The units for this input are in power consumption per flow rate of water through the pool from the heater or W/(kg/s). This field will be multiplied by the flow rate of water through the pool to determine the power consumption of this equipment. Any heat generated by this equipment is assumed to have no effect on the pool water itself.
+
+\paragraph{Field: Setpoint Temperature Schedule}\label{field-setpoint-temperature-schedule}
+
+Pools attempt to maintain a particular water temperature. In EnergyPlus, this field defines the setpoint temperature for the desired pool water temperature. It is input as a schedule to allow the user to vary the pool setpoint temperature as desired. The equipment defined to provide heating for the pool will deliver the necessary hot water to the pool, up to the capacity of that equipment defined by other input by the user.
+
+\paragraph{Field: Maximum Number of People}\label{field-maximum-number-of-people}
+
+This field defines the maximum occupancy of people actually in the pool and thus will be used with the next two inputs to determine how much heat people contribute to the pool heat balance. People who are not in the pool should be modeled separately using the standard People description for zones.
+
+\paragraph{Field: People Schedule}\label{field-people-schedule}
+
+This field defines a schedule that establishes how many people are in the pool at any given time. The current value of this schedule is multiplied by the maximum number of people in the previous field determines how many people are currently in the pool.
+
+\paragraph{Field: People Heat Gain Schedule}\label{field-people-heat-gain-schedule}
+
+This field defines the amount of heat given off by an average person in the pool in Watts. This field is a schedule so that this heat gain can be allowed to vary as the type of activity in a pool can vary greatly and thus the amount of heat gain per person also varies. This parameter times the number of people in the pool determines how much heat is added to the pool. All heat given off by people is added to the heat balance of the pool water.
+
+An example of an indoor swimming pool definition is:
+
+\begin{lstlisting}
+
+SwimmingPool:Indoor,
+  Test Pool,             !- Name
+  F1-1,                  !- Surface Name
+  1.5,                   !- Average Depth {m}
+  PoolActivitySched,     !- Pool Activity Schedule
+  MakeUpWaterSched,      !- MakeUp Water Temperature Schedule
+  PoolCoverSched,        !- Pool Cover Schedule
+  0.0,                   !- Cover Evaporation Factor
+  0.2,                   !- Cover Convection Factor
+  0.9,                   !- Cover Short-Wavelength Radiation Factor
+  0.5,                   !- Cover Long-Wavelength Radiation Factor
+  Pool Water Inlet Node,    !- Water Inlet Node (Plant/Heater)
+  Pool Water Outlet Node,   !- Water Outlet Node (Plant/Heater)
+  0.1,                   !- Maximum flow rate from water heating system {m3/s}
+  0.6,                   !- Miscellaneous Equipment Power Factor
+  PoolSetpointTempSched, !- Pool Water Setpoint Temperature Schedule
+  15,                    !- Maximum Number of People in Pool
+  PoolOccupancySched,    !- Pool People Schedule
+  PoolOccHeatGainSched;  !- Pool People Heat Gain Schedule
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-007}
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC, Average, Indoor Pool Makeup Water Rate {[}m3/s{]}
+\item
+  HVAC, Sum, Indoor Pool Makeup Water Volume {[}m3{]}
+\item
+  HVAC, Average, Indoor Pool Makeup Water Temperature {[}C{]}
+\item
+  HVAC, Average, Indoor Pool Water Temperature {[}C{]}
+\item
+  HVAC, Average, Indoor Pool Inlet Water Temperature {[}C{]}
+\item
+  HVAC, Average, Indoor Pool Inlet Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Indoor Pool Miscellaneous Equipment Power {[}W{]}
+\item
+  HVAC, Sum, Indoor Pool Miscellaneous Equipment Energy {[}J{]}
+\item
+  HVAC, Average, Indoor Pool Heating Rate {[}W{]}
+\item
+  HVAC, Sum, Indoor Pool Heating Energy {[}J{]}
+\item
+  HVAC, Average, Indoor Pool Radiant to Convection by Cover {[}W{]}
+\item
+  HVAC, Average, Indoor Pool People Heat Gain {[}W{]}
+\item
+  HVAC, Average, Indoor Pool Current Activity Factor {[]}
+\item
+  HVAC, Average, Indoor Pool Current Cover Factor {[]}
+\item
+  HVAC, Average, Indoor Pool Evaporative Heat Loss Rate {[}W{]}
+\item
+  HVAC, Sum, Indoor Pool Evaporative Heat Loss Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Indoor Pool Makeup Water Rate {[}m3/s{]}}\label{indoor-pool-makeup-water-rate-m3s}
+
+The water consumption rate for the makeup water of indoor swimming pool.
+
+\paragraph{Indoor Pool Makeup Water Volume {[}m3{]}}\label{indoor-pool-makeup-water-volume-m3}
+
+The water consumption for the makeup water of indoor swimming pool.
+
+\paragraph{Indoor Pool Makeup Water Temperature {[}C{]}}\label{indoor-pool-makeup-water-temperature-c}
+
+The temperature of the makeup water of indoor swimming pool.
+
+\paragraph{Indoor Pool Water Temperature {[}C{]}}\label{indoor-pool-water-temperature-c}
+
+The average calculated pool water temperature during the simulation at the time frequency requested.
+
+\paragraph{Indoor Pool Inlet Water Temperature {[}C{]}}\label{indoor-pool-inlet-water-temperature-c}
+
+The temperature of the water being sent to the pool from the plant heating equipment.
+
+\paragraph{Indoor Pool Inlet Water Mass Flow Rate {[}kg/s{]}}\label{indoor-pool-inlet-water-mass-flow-rate-kgs}
+
+The mass flow rate of water being sent to the pool from the plant heating equipment. Typically this water is being passed through a heater and miscellaneous equipment.
+
+\paragraph{Indoor Pool Miscellaneous Equipment Power {[}W{]}}\label{indoor-pool-miscellaneous-equipment-power-w}
+
+The miscellaneous equipment power includes the power consumption of pool filter and chlorinator in Watts.
+
+\paragraph{Indoor Pool Miscellaneous Equipment Energy {[}J{]}}\label{indoor-pool-miscellaneous-equipment-energy-j}
+
+The miscellaneous equipment power consumption includes the energy consumption of pool filter and chlorinator in Joules.
+
+\paragraph{Indoor Pool Heating Rate {[}W{]}}\label{indoor-pool-heating-rate-w}
+
+This is the rate of heating provided by the plant loop to the pool in Watts.
+
+\paragraph{Indoor Pool Heating Energy {[}J{]}}\label{indoor-pool-heating-energy-j}
+
+This is the amount of heating provided by the plant loop to the pool in Joules over the time step requested.
+
+\paragraph{Indoor Pool Radiant to Convection by Cover {[}W{]}}\label{indoor-pool-radiant-to-convection-by-cover-w}
+
+The pool cover may block some or all of short- and long-wavelength radiation incident on the pool. To account for this and to not have the cover result in energy that is not accounted for by the model, the radiation that is blocked by the cover is converted to a convective gain (or loss) to/from the zone air. This output field reports this value.
+
+\paragraph{\texorpdfstring{Indoor Pool Current Activity Factor {[]}}{Indoor Pool Current Activity Factor }}\label{indoor-pool-current-activity-factor}
+
+This is the current activity factor as defined by the user input schedule.
+
+\paragraph{\texorpdfstring{Indoor Pool Current Cover Factor {[]}}{Indoor Pool Current Cover Factor }}\label{indoor-pool-current-cover-factor}
+
+This is the current cover factor as defined by the user input schedule.
+
+\paragraph{Indoor Pool Evaporative Heat Loss Rate {[}W{]}}\label{indoor-pool-evaporative-heat-loss-rate-w}
+
+This is the rate of evaporative heat loss (latent) to the zone from the pool in Watts.
+
+\paragraph{Indoor Pool Evaporative Heat Loss Energy {[}J{]}}\label{indoor-pool-evaporative-heat-loss-energy-j}
+
+This is the amount of evaporative heat loss (latent) to the zone from the pool in in Joules over the time step requested.
+
+\subsection{OtherEquipment}\label{otherequipment}
+
+Other Equipment object is provided as an additional source for heat gains or losses directly to the zone.~ That is to say, a loss can be entered by putting a negative value into the Design Level field(s). Note, too, that this object does not have an end-use component -- gains or losses do not show up in the bottom energy lines (except as influencing overall zone gains or losses).
+
+\subsubsection{Inputs}\label{inputs-8-010}
+
+\paragraph{Field: Name}\label{field-name-8-008}
+
+The name of the OtherEquipment object.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-6}
+
+This field is the name of the thermal zone (ref: Zone) and attaches a particular other equipment statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this other equipment definition is applied to each of the zones in the zone list effecting a global definition for the amount of other in the zone. This option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-5-000}
+
+This field is the name of the schedule that modifies the design level parameter for other equipment (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The actual energy input for other equipment in a zone as defined by this statement is the product of the design level field and the value of the schedule specified by name in this field.
+
+\paragraph{Field: Design Level Calculation Method}\label{field-design-level-calculation-method-5}
+
+This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal other equipment level in the Zone. The key/choices are:
+
+\begin{itemize}
+\tightlist
+\item
+  EquipmentLevel
+\end{itemize}
+
+With this choice, the method used will be a straight insertion of the other equipment level (Watts) for the Zone.~ (The Design Level field should be filled.)
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Area or Power/Area
+\end{itemize}
+
+With this choice, the method used will be a factor per floor area of the zone. (The Power per Zone Floor Area field should be filled).
+
+\begin{itemize}
+\tightlist
+\item
+  Watts/Person or Power/Person
+\end{itemize}
+
+With this choice, the method used will be a factor of equipment level (watts) per person. (The Power per Person field should be filled).
+
+\paragraph{Field: Design Level}\label{field-design-level-4}
+
+This field (in Watts) is typically used to represent the maximum energy input to other equipment in a zone that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the other equipment design level could be a ``diversity factor'' applied to a schedule of real numbers. This value can be negative to denote a loss. Note that while the schedule value can vary from hour to hour, the design level field is constant for all simulation environments.
+
+\paragraph{Field: Power per Zone Floor Area}\label{field-power-per-zone-floor-area-3}
+
+This factor (watts/m\(^{2}\)) is used, along with the Zone Area to determine the maximum equipment level as described in the Design Level field. This value can be negative to denote a loss. The choice from the method field should be ``\textbf{Watts/Area}'' or ``\textbf{Power/Area}''.
+
+\paragraph{Field: Power per Person}\label{field-power-per-person-3}
+
+This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum equipment level as described in the Design Level field. This value can be negative to denote a loss. The choice from the method field should be ``\textbf{Watts/Person}'' or ``\textbf{Power/Person}''.
+
+\paragraph{Heat Gains/Losses from Other Equipment:}\label{heat-gainslosses-from-other-equipment}
+
+The fuel input to the equipment ultimately appears as heat that contributes to zone loads. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Fraction Latent, Fraction Radiant and Fraction Lost. A fourth, defined as the fraction of the heat from other equipment convected to the zone air, is calculated by the program as:
+
+\begin{equation}
+  f_{\rm{convected}} = 1.0 - (\rm{Fraction Latent} + \rm{Fraction Radiant} + \rm{Fraction Lost})
+\end{equation}
+
+You will get an error message if \(\rm{Fraction Latent} + \rm{Fraction Radiant} + \rm{Fraction Lost}\) exceeds 1.0.
+
+\paragraph{Field: Fraction Latent}\label{field-fraction-latent-4}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of latent heat given off by other equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by other equipment to give the amount of latent energy produced by the other equipment. This energy affects the moisture balance within the zone.
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant-6}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of long-wave radiant heat being given off by other equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by other equipment to give the amount of long wavelength radiation gain from other equipment in a zone.
+
+\paragraph{Field: Fraction Lost}\label{field-fraction-lost-4}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of ``lost'' heat being given off by other equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by other equipment to give the amount of heat which is ``lost'' and does not impact the zone energy balances. This might correspond to input energy converted to mechanical work or heat that is vented to the atmosphere.
+
+IDF Examples
+
+\begin{lstlisting}
+OtherEquipment,
+  BASE-1 OthEq 1, !- Name
+  BASE-1,         !- Zone Name
+  ALWAYSON,       !- SCHEDULE Name
+  EquipmentLevel, !- Design Level calculation method
+  6766.,          !- Design Level {W}
+  ,               !- Power per Zone Floor Area {watts/m2}
+  ,               !- Power per Person {watts/person}
+  0,              !- Fraction Latent
+  0.3,            !- Fraction Radiant
+  0;              !- Fraction Lost
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-004}
+
+Each type of equipment object has output variables for individual objects and for zone totals.
+
+Electric Equipment
+
+\begin{itemize}
+\item
+  Zone,Average,Electric Equipment Electric Power {[}W{]}
+\item
+  Zone,Sum,Electric Equipment Electric Energy {[}J{]}
+\item
+  Zone,Sum,Electric Equipment Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Electric Equipment Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Electric Equipment Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Electric Equipment Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Electric Equipment Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Electric Equipment Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Electric Equipment Lost Heat Energy {[}J{]}
+\item
+  Zone,Average,Electric Equipment Lost Heat Rate {[}W{]}
+\item
+  Zone,Sum,Electric Equipment Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Electric Equipment Total Heating Rate {[}W{]}
+\item
+  Zone,Average,Zone Electric Equipment Electric Power {[}W{]}
+\item
+  Zone,Sum,Zone Electric Equipment Electric Energy {[}J{]}
+\item
+  Zone,Sum,Zone Electric Equipment Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Electric Equipment Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Electric Equipment Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Electric Equipment Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Electric Equipment Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Zone Electric Equipment Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Zone Electric Equipment Lost Heat Energy {[}J{]}
+\item
+  Zone,Average,Zone Electric Equipment Lost Heat Rate {[}W{]}
+\item
+  Zone,Sum,Zone Electric Equipment Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Electric Equipment Total Heating Rate {[}W{]}
+\end{itemize}
+
+\textbf{Gas Equipment}
+
+\begin{itemize}
+\item
+  Zone,Average,Gas Equipment Gas Rate {[}W{]}
+\item
+  Zone,Sum,Gas Equipment Gas Energy {[}J{]}
+\item
+  Zone,Sum,Gas Equipment Radiant Heating Energy {[}J{]}
+\item
+  Zone,Sum,Gas Equipment Convective Heating Energy {[}J{]}
+\item
+  Zone,Sum,Gas Equipment Latent Gain Energy {[}J{]}
+\item
+  Zone,Sum,Gas Equipment Lost Heat Energy {[}J{]}
+\item
+  Zone,Sum,Gas Equipment Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Gas Equipment Radiant Heating Rate {[}W{]}
+\item
+  Zone,Average,Gas Equipment Convective Heating Rate {[}W{]}
+\item
+  Zone,Average,Gas Equipment Latent Gain Rate {[}W{]}
+\item
+  Zone,Average,Gas Equipment Lost Heat Rate {[}W{]}
+\item
+  Zone,Average,Gas Equipment Total Heating Rate {[}W{]}
+\item
+  Zone,Average,Zone Gas Equipment Gas Rate {[}W{]}
+\item
+  Zone,Sum,Zone Gas Equipment Gas Energy {[}J{]}
+\item
+  Zone,Sum,Zone Gas Equipment Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Gas Equipment Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Gas Equipment Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Gas Equipment Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Gas Equipment Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Zone Gas Equipment Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Zone Gas Equipment Lost Heat Energy {[}J{]}
+\item
+  Zone,Average,Zone Gas Equipment Lost Heat Rate {[}W{]}
+\item
+  Zone,Sum,Zone Gas Equipment Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Gas Equipment Total Heating Rate {[}W{]}
+\end{itemize}
+
+\textbf{HotWater Equipment}
+
+\begin{itemize}
+\item
+  Zone,Average,Hot Water Equipment District Heating Rate {[}W{]}
+\item
+  Zone,Sum,Hot Water Equipment District Heating Energy {[}J{]}
+\item
+  Zone,Sum,Hot Water Equipment Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Hot Water Equipment Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Hot Water Equipment Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Hot Water Equipment Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Hot Water Equipment Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Hot Water Equipment Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Hot Water Equipment Lost Heat Energy {[}J{]}
+\item
+  Zone,Average,Hot Water Equipment Lost Heat Rate {[}W{]}
+\item
+  Zone,Sum,Hot Water Equipment Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Hot Water Equipment Total Heating Rate {[}W{]}
+\item
+  Zone,Average,Zone Hot Water Equipment District Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Hot Water Equipment District Heating Energy {[}J{]}
+\item
+  Zone,Sum,Zone Hot Water Equipment Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Hot Water Equipment Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Hot Water Equipment Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Hot Water Equipment Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Hot Water Equipment Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Zone Hot Water Equipment Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Zone Hot Water Equipment Lost Heat Energy {[}J{]}
+\item
+  Zone,Average,Zone Hot Water Equipment Lost Heat Rate {[}W{]}
+\item
+  Zone,Sum,Zone Hot Water Equipment Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Hot Water Equipment Total Heating Rate {[}W{]}
+\end{itemize}
+
+\textbf{Steam Equipment}
+
+\begin{itemize}
+\item
+  Zone,Average,Steam Equipment District Heating Rate {[}W{]}
+\item
+  Zone,Sum,Steam Equipment District Heating Energy {[}J{]}
+\item
+  Zone,Sum,Steam Equipment Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Steam Equipment Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Steam Equipment Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Steam Equipment Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Steam Equipment Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Steam Equipment Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Steam Equipment Lost Heat Energy {[}J{]}
+\item
+  Zone,Average,Steam Equipment Lost Heat Rate {[}W{]}
+\item
+  Zone,Sum,Steam Equipment Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Steam Equipment Total Heating Rate {[}W{]}
+\item
+  Zone,Average,Zone Steam Equipment District Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Steam Equipment District Heating Energy {[}J{]}
+\item
+  Zone,Sum,Zone Steam Equipment Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Steam Equipment Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Steam Equipment Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Steam Equipment Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Steam Equipment Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Zone Steam Equipment Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Zone Steam Equipment Lost Heat Energy {[}J{]}
+\item
+  Zone,Average,Zone Steam Equipment Lost Heat Rate {[}W{]}
+\item
+  Zone,Sum,Zone Steam Equipment Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Steam Equipment Total Heating Rate {[}W{]}
+\end{itemize}
+
+\textbf{Other Equipment}
+
+\begin{itemize}
+\item
+  Zone,Sum,Other Equipment Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Other Equipment Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Other Equipment Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Other Equipment Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Other Equipment Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Other Equipment Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Other Equipment Lost Heat Energy {[}J{]}
+\item
+  Zone,Average,Other Equipment Lost Heat Rate {[}W{]}
+\item
+  Zone,Sum,Other Equipment Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Other Equipment Total Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Other Equipment Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Other Equipment Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Other Equipment Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Other Equipment Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Other Equipment Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Zone Other Equipment Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Zone Other Equipment Lost Heat Energy {[}J{]}
+\item
+  Zone,Average,Zone Other Equipment Lost Heat Rate {[}W{]}
+\item
+  Zone,Sum,Zone Other Equipment Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Other Equipment Total Heating Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Electric Equipment Electric Power {[}W{]}}\label{electric-equipment-electric-power-w}
+
+\paragraph{Electric Equipment Electric Energy {[}J{]}}\label{electric-equipment-electric-energy-j}
+
+The electric equipment electric power consumption in Watts (for power) or Joules (for energy). It is the sum of the radiant, convective, latent and lost components. This energy use is added to the electricity meters that are associated with the zone -- Electricity:Facility, Electricity:Buidling, Electricity:Zone:\textless{}Zone Name\textgreater{}, InteriorEquipment:Electricity: :Zone:\textless{}Zone Name\textgreater{}, and \textless{}End-Use Subcategory\textgreater{}:InteriorEquipment:Electricity.
+
+\paragraph{Gas Equipment Gas Rate {[}W{]}}\label{gas-equipment-gas-rate-w}
+
+\paragraph{Gas Equipment Gas Energy {[}J{]}}\label{gas-equipment-gas-energy-j}
+
+The gas equipment natural gas consumption in Watts (for power) or Joules (for energy). It is the sum of the radiant, convective, latent and lost components. This energy use is added to the electricity meters that are associated with the zone -- Gas:Facility, Gas:Buidling, Gas:Zone:\textless{}Zone Name\textgreater{}, InteriorEquipment:Gas: :Zone:\textless{}Zone Name\textgreater{}, and \textless{}End-Use Subcategory\textgreater{}:InteriorEquipment:Gas.
+
+\paragraph{Hot Water Equipment District Heating Rate {[}W{]}}\label{hot-water-equipment-district-heating-rate-w}
+
+\paragraph{Hot Water Equipment District Heating Energy {[}J{]}}\label{hot-water-equipment-district-heating-energy-j}
+
+The hot water equipment district heating consumption in Watts (for power) or Joules (for energy). It is the sum of the radiant, convective, latent and lost components. This energy use is added to the district heating meters that are associated with the zone -- DistrictHeating:Facility, DistrictHeating:Buidling, DistrictHeating:Zone:\textless{}Zone Name\textgreater{}, InteriorEquipment: DistrictHeating: :Zone:\textless{}Zone Name\textgreater{}, and \textless{}End-Use Subcategory\textgreater{}:InteriorEquipment: DistrictHeating.
+
+\paragraph{Steam Equipment District Heating Rate {[}W{]}}\label{steam-equipment-district-heating-rate-w}
+
+\paragraph{Steam Equipment District Heating Energy {[}J{]}}\label{steam-equipment-district-heating-energy-j}
+
+The steam equipment district heating consumption in Watts (for power) or Joules (for energy). It is the sum of the radiant, convective, latent and lost components. This energy use is added to the district heating meters that are associated with the zone -- DistrictHeating:Facility, DistrictHeating:Buidling, DistrictHeating:Zone:\textless{}Zone Name\textgreater{}, InteriorEquipment: DistrictHeating: :Zone:\textless{}Zone Name\textgreater{}, and \textless{}End-Use Subcategory\textgreater{}:InteriorEquipment: DistrictHeating.
+
+Note that zone energy consumption is not reported for OTHER EQUIPMENT and does not go on any meter.
+
+\subsection{ElectricEquipment:ITE:AirCooled}\label{electricequipmentiteaircooled}
+
+This object describes air-cooled electric information technology equipment (ITE) which has variable power consumption as a function of loading and temperature.
+
+\subsubsection{Inputs}\label{inputs-9-009}
+
+\paragraph{Field: Name}\label{field-name-9-008}
+
+The name of this object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-005}
+
+This field is the name of the thermal zone (ref: Zone) which contains this ElectricEquipment:ITE:AirCooled object.
+
+\paragraph{Field: Design Power Input Calculation Method}\label{field-design-power-input-calculation-method}
+
+This field is a key/choice field that tells which of the next two fields are filled and is descriptive of the method for calculating the nominal electric power input to the ITE. The key/choices are:
+
+Watts/Unit
+
+With this choice, the design power input will be the product of Design Level per Unit and Number of Units. (Both of these fields should be filled.) This is the default.
+
+Watts/Area
+
+With this choice, the design power input will be a factor per floor area of the zone. (The Watts per Zone Floor Area field should be filled).
+
+\paragraph{Field: Watts per Unit}\label{field-watts-per-unit}
+
+This field (in Watts) is typically used to represent the design electrical power input to the ITE when fully loaded and the entering air temperatures is at the specified design value. This field is used if the choice from the method field is ``EquipmentLevel''.
+
+\paragraph{Field: Number of Units}\label{field-number-of-units}
+
+This field is multiplied times the Design Level per Unit to determine the design electrical power input to this ITE object when fully loaded and the entering air temperature is at the specified design value. This field is used if the choice from the method field is ``EquipmentLevel''. The default is 1.
+
+\paragraph{Field: Watts per Zone Floor Area}\label{field-watts-per-zone-floor-area-2}
+
+This factor (Watts/m2) is used, along with the Zone Area to determine the design electrical power input as described in the Design Level field above. This field is used if the choice from the method field is ``Watts/Area''.
+
+\paragraph{Field: Design Power Input Schedule Name}\label{field-design-power-input-schedule-name}
+
+This field is the name of the operating schedule that modifies the design level power input for this equipment This schedule specifies the fraction (typically 0.0 to 1.0) of this equipment which is available (powered up), regardless of CPU utilization. If this field is blank, the schedule is assumed to always be 1.0.
+
+\paragraph{Field: CPU Loading Schedule Name}\label{field-cpu-loading-schedule-name}
+
+This field is the name of the schedule that specifies the CPU loading for this equipment as a fraction from 0.0 (idle) to 1.0 (full load). If this field is blank, the schedule is assumed to always be 1.0.
+
+\paragraph{Field: CPU Power Input Function of Loading and Air Temperature Curve Name}\label{field-cpu-power-input-function-of-loading-and-air-temperature-curve-name}
+
+The name of a two-variable curve or table lookup object which modifies the CPU power input as a function of CPU loading (x) and air inlet node temperature (y). This curve (table) should equal 1.0 at design conditions (CPU loading = 1.0 and Design Entering Air Temperature).
+
+\paragraph{Field: Design Fan Power Input Fraction}\label{field-design-fan-power-input-fraction}
+
+This field is a decimal number between 0.0 and 1.0 and is used to specify the fraction of the total power input at design conditions which is for the cooling fan(s). If fan power data is not available, set this fraction to 0.0. The default is 0.0.
+
+\paragraph{Field: Design Fan Air Flow Rate per Power Input}\label{field-design-fan-air-flow-rate-per-power-input}
+
+Specifies the cooling fan air flow rate in m3/s per Watt of total electric power input at design conditions (CPU loading = 1.0 and Design Entering Air Temperature).
+
+This is normalized by power input to allow the design power input to be changed without needing to change this value.
+
+\paragraph{Field: Air Flow Function of Loading and Air Temperature Curve Name}\label{field-air-flow-function-of-loading-and-air-temperature-curve-name}
+
+The name of a two-variable curve or table lookup object which modifies the cooling air flow rate as a function of CPU loading (x) and air inlet node temperature (y). This curve (table) should equal 1.0 at design conditions (CPU loading = 1.0 and Design Entering Air Temperature).
+
+\paragraph{Field: Fan Power Input Function of Flow Curve Name}\label{field-fan-power-input-function-of-flow-curve-name}
+
+The name of a single-variable curve or table lookup object which modifies the fan power input as a function of airflow fraction (x). This curve (table) should equal 1.0 at the design air flow rate (flow fraction = 1.0).
+
+\paragraph{Field: Design Entering Air Temperature}\label{field-design-entering-air-temperature}
+
+Specifies the entering air temperature in deg. C at design conditions. The default is 15C.
+
+\paragraph{Field: Environmental Class}\label{field-environmental-class}
+
+Specifies the allowable operating conditions for the air inlet conditions. The available inputs are A1, A2, A3, A4, B, C, or None. This is used to report the ``ITE Air Inlet Operating Range Exceeded Time'' If None is specified (the default), then no reporting of time outside allowable conditions will be done.
+
+\paragraph{Field: Air Inlet Connection Type}\label{field-air-inlet-connection-type}
+
+Specifies the type of connection between the zone and the ITE air inlet node. The choices are:
+
+AdjustedSupply = This option is used to apply a recirculation adjustment to the ITE inlet conditions. If this option is specified, then the Supply Air Node Name is required and the air inlet temperature to the ITE will be the current supply air node temperature adjusted by the current recirculation fraction. All heat output is added to the zone air heat balance as a convective gain. AdjustedSupply is the default.
+
+ZoneAirNode = This option is used if there is no containment and the ITE air inlet node is at the average zone condition. All heat output is added to the zone air heat balance as a convective gain.
+
+RoomAirModel = This option connects the ITE air inlet and outlet nodes to a room air model (Ref. RoomAirModelType and RoomAir:Node).
+
+\paragraph{Field: Air Inlet Room Air Model Node Name}\label{field-air-inlet-room-air-model-node-name}
+
+Specifies the name of a room air model node (ref. RoomAir:Node) which is the air inlet to this equipment. This field is required if the Air Node Connection Type = RoomAirModel.
+
+\paragraph{Field: Air Outlet Room Air Model Node Name}\label{field-air-outlet-room-air-model-node-name}
+
+Specifies the node name of a room air model node (ref. RoomAir:Node) which is the air outlet from this equipment. This field is required if the Air Node Connection Type = RoomAirModel.
+
+\paragraph{Field: Supply Air Node Name}\label{field-supply-air-node-name}
+
+Specifies the node name of the supply air inlet node service this ITE. If the Air Node Connection Type = AdjustedSupply ,then this field is required, and the conditions at this node will be used to determine the ITE air inlet conditions. This field is also required if reporting of the Supply Heat Index is desired.
+
+\paragraph{Field: Design Recirculation Fraction}\label{field-design-recirculation-fraction}
+
+Specifies the recirculation fraction for this equipment at design conditions. This field is used only if the Air Node Connection Type = AdjustedSupply. The recirculation fraction is defined as the ratio of recirculated air flow to total air flow entering the ITE. Recirculation is dependent upon many factors including rack and containment configuration. The default is 0.0 (no recirculation).
+
+\paragraph{Field: Recirculation Function of Loading and Supply Temperature Curve Name}\label{field-recirculation-function-of-loading-and-supply-temperature-curve-name}
+
+The name of a two-variable curve or table lookup object which modifies the Design Recirculation Fraction as a function of CPU loading (x) and supply air node temperature (y). This curve (table) should equal 1.0 at design conditions (CPU loading = 1.0 and Design Entering Air Temperature). This field is used only if the Air Node Connection Type = AdjustedSupply. If this curve is left blank, then the curve is assumed to always equal 1.0.
+
+\paragraph{Field: Design Electric Power Supply Efficiency}\label{field-design-electric-power-supply-efficiency}
+
+This field is a decimal number used to specify the efficiency of the power supply system serving this ITE. The default is 1.0.
+
+\paragraph{Field: Electric Power Supply Efficiency Function of Part Load Ratio Curve Name}\label{field-electric-power-supply-efficiency-function-of-part-load-ratio-curve-name}
+
+The name of a single-variable curve or table lookup object which modifies the electric power supply efficiency as a function of part load ratio (x). This curve (table) should equal 1.0 at the design power consumption (part load ratio = 1.0). If this curve is left blank, then the curve is assumed to always equal 1.0.
+
+\paragraph{Field: Fraction of Electric Power Supply Losses to Zone}\label{field-fraction-of-electric-power-supply-losses-to-zone}
+
+This field is a decimal number between 0.0 and 1.0 and is used to specify the fraction of the electric power supply losses which are a heat gain to the zone containing the ITE. If this value is less than 1.0, the remainder of the losses are assumed to be lost to the outdoors. The default is 1.0.
+
+\paragraph{Field: CPU End-Use Subcategory}\label{field-cpu-end-use-subcategory}
+
+This equipment is metered on the Interior Equipment end-use category for Electricity. This field allows you to specify a user-defined end-use subcategory for the CPU power consumption. A new meter for reporting is created for each unique subcategory (ref: Output:Meter object). Subcategories are also reported in the ABUPS table. The default is ITE-CPU.
+
+\paragraph{Field: Fan End-Use Subcategory}\label{field-fan-end-use-subcategory}
+
+This equipment is metered on the Interior Equipment end-use category for Electricity. This field allows you to specify a user-defined end-use subcategory for the fan power consumption. A new meter for reporting is created for each unique subcategory (ref: Output:Meter object). Subcategories are also reported in the ABUPS table. The default is ITE-Fans
+
+\paragraph{Field: Electric Power Supply End-Use Subcategory}\label{field-electric-power-supply-end-use-subcategory}
+
+This equipment is metered on the Interior Equipment end-use category for Electricity. This field allows you to specify a user-defined end-use subcategory for the electric power supply power consumption. A new meter for reporting is created for each unique subcategory (ref: Output:Meter object). Subcategories are also reported in the ABUPS table. The default is ITE-UPS
+
+An IDF example:
+
+\begin{lstlisting}
+
+ElectricEquipment:ITE:AirCooled,
+  Data Center Servers,     !- Name
+  Main Zone,               !- Zone Name
+  Watts/Unit,              !- Design Power Input Calculation Method
+  500,                     !- Watts per Unit {W}
+  200,                     !- Number of Units
+  ,                        !- Watts per Zone Floor Area {W/m2}
+  Data Center Operation Schedule,  !- Design Power Input Schedule Name
+  Data Center CPU Loading Schedule,  !- CPU Loading  Schedule Name
+  Model 5250 Power fLoadTemp,  !- CPU Power Input Function of Loading and Air Temperature Curve Name
+  0.4,                     !- Design Fan Power Input Fraction
+  0.0001,                  !- Design Fan Air Flow Rate per Power Input {m3/s-W}
+  Model 5250 AifFlow fLoadTemp,  !- Air Flow Function of Loading and Air Temperature Curve Name
+  ECM FanPower fFlow,      !- Fan Power Input Function of Flow Curve Name
+  15,                      !- Design Entering Air Temperature {C}
+  A3,                      !- Environmental Class
+  AdjustedSupply,          !- Air Inlet Connection Type
+  ,                        !- Air Inlet Room Air Model Node Name
+  ,                        !- Air Outlet Room Air Model Node Name
+  Main Zone Inlet Node,    !- Supply Air Node Name
+  0.1,                     !- Design Recirculation Fraction
+  Data Center Recirculation fLoadTemp,  !- Recirculation Function of Loading and Supply Temperature Curve Name
+  0.9,                     !- Design Electric Power Supply Efficiency
+  UPS Efficiency fPLR,     !- Electric Power Supply Efficiency Function of Part Load Ratio Curve Name
+  1,                       !- Fraction of Electric Power Supply Losses to Zone
+  ITE-CPU,                 !- CPU End-Use Subcategory
+  ITE-Fans,                !- Fan End-Use Subcategory
+  ITE-UPS;                 !- Electric Power Supply End-Use Subcategory
+\end{lstlisting}
+
+ElectricEquipment:ITE:AirCooled Outputs
+
+\begin{itemize}
+\tightlist
+\item
+  Zone,Average,ITE CPU Electric Power {[}W{]}
+\item
+  Zone,Average,ITE Fan Electric Power {[}W{]}
+\item
+  Zone,Average,ITE UPS Electric Power {[}W{]}
+\item
+  Zone,Average,ITE CPU Electric Power at Design Inlet Conditions {[}W{]}
+\item
+  Zone,Average,ITE Fan Electric Power at Design Inlet Conditions {[}W{]}
+\item
+  Zone,Average,ITE UPS Heat Gain to Zone Rate {[}W{]}
+\item
+  Zone,Average,ITE Total Heat Gain to Zone Rate {[}W{]}
+\item
+  Zone,Sum,ITE CPU Electric Energy {[}J{]}
+\item
+  Zone,Sum,ITE Fan Electric Energy {[}J{]}
+\item
+  Zone,Sum,ITE UPS Electric Energy {[}J{]}
+\item
+  Zone,Sum,ITE CPU Electric Energy at Design Inlet Conditions {[}J{]}
+\item
+  Zone,Sum,ITE Fan Electric Energy at Design Inlet Conditions {[}J{]}
+\item
+  Zone,Sum,ITE UPS Heat Gain to Zone Energy {[}J{]}
+\item
+  Zone,Sum,ITE Total Heat Gain to Zone Energy {[}J{]}
+\item
+  Zone,Average,ITE Standard Density Air Volume Flow Rate {[}m3/s{]}
+\item
+  Zone,Average,ITE Current Density Air Volume Flow Rate {[}m3/s{]}
+\item
+  Zone,Average,ITE Air Mass Flow Rate {[}kg/s{]}
+\item
+  Zone,Average,ITE Air Inlet Dry-Bulb Temperature {[}C{]}
+\item
+  Zone,Average,ITE Air Inlet Dewpoint Temperature {[}C{]}
+\item
+  Zone,Average,ITE Air Inlet Relative Humidity {[}\%{]}
+\item
+  Zone,Average,ITE Air Outlet Dry-Bulb Temperature {[}C{]}
+\item
+  Zone,Average,ITE Supply Heat Index {[]}
+\item
+  Zone,Sum,ITE Air Inlet Operating Range Exceeded Time {[}hr{]}
+\item
+  Zone,Sum,ITE Air Inlet Dry-Bulb Temperature Above Operating Range Time {[}hr{]}
+\item
+  Zone,Sum,ITE Air Inlet Dry-Bulb Temperature Below Operating Range Time {[}hr{]}
+\item
+  Zone,Sum,ITE Air Inlet Dewpoint Temperature Above Operating Range Time {[}hr{]}
+\item
+  Zone,Sum,ITE Air Inlet Dewpoint Temperature Below Operating Range Time {[}hr{]}
+\item
+  Zone,Sum,ITE Air Inlet Relative Humidity Above Operating Range Time {[}hr{]}
+\item
+  Zone,Sum,ITE Air Inlet Relative Humidity Below Operating Range Time {[}hr{]}
+\item
+  Zone,Average,ITE Air Inlet Dry-Bulb Temperature Difference Above Operating Range {[}deltaC{]}
+\item
+  Zone,Average,ITE Air Inlet Dry-Bulb Temperature Difference Below Operating Range {[}deltaC{]}
+\item
+  Zone,Average,ITE Air Inlet Dewpoint Temperature Difference Above Operating Range {[}deltaC{]}
+\item
+  Zone,Average,ITE Air Inlet Dewpoint Temperature Difference Below Operating Range {[}deltaC{]}
+\item
+  Zone,Average,ITE Air Inlet Relative Humidity Difference Above Operating Range {[}\%{]}
+\item
+  Zone,Average,ITE Air Inlet Relative Humidity Difference Below Operating Range {[}\%{]}
+\item
+  Zone,Average,Zone ITE CPU Electric Power {[}W{]}
+\item
+  Zone,Average,Zone ITE Fan Electric Power {[}W{]}
+\item
+  Zone,Average,Zone ITE UPS Electric Power {[}W{]}
+\item
+  Zone,Average,Zone ITE CPU Electric Power at Design Inlet Conditions {[}W{]}
+\item
+  Zone,Average,Zone ITE Fan Electric Power at Design Inlet Conditions {[}W{]}
+\item
+  Zone,Average,Zone ITE UPS Heat Gain to Zone Rate {[}W{]}
+\item
+  Zone,Average,Zone ITE Total Heat Gain to Zone Rate {[}W{]}
+\item
+  Zone,Sum,Zone ITE CPU Electric Energy {[}J{]}
+\item
+  Zone,Sum,Zone ITE Fan Electric Energy {[}J{]}
+\item
+  Zone,Sum,Zone ITE UPS Electric Energy {[}J{]}
+\item
+  Zone,Sum,Zone ITE CPU Electric Energy at Design Inlet Conditions {[}J{]}
+\item
+  Zone,Sum,Zone ITE Fan Electric Energy at Design Inlet Conditions {[}J{]}
+\item
+  Zone,Sum,Zone ITE UPS Heat Gain to Zone Energy {[}J{]}
+\item
+  Zone,Sum,Zone ITE Total Heat Gain to Zone Energy {[}J{]}
+\item
+  Zone,Average,Zone ITE Standard Density Air Volume Flow Rate {[}m3/s{]}
+\item
+  Zone,Average,Zone ITE Air Mass Flow Rate {[}kg/s{]}
+\item
+  Zone,Average,Zone ITE Average Supply Heat Index {[]}
+\item
+  Zone,Sum,Zone ITE Any Air Inlet Operating Range Exceeded Time {[}hr{]}
+\item
+  Zone,Sum,Zone ITE Any Air Inlet Dry-Bulb Temperature Above Operating Range Time {[}hr{]}
+\item
+  Zone,Sum,Zone ITE Any Air Inlet Dry-Bulb Temperature Below Operating Range Time {[}hr{]}
+\item
+  Zone,Sum,Zone ITE Any Air Inlet Dewpoint Temperature Above Operating Range Time {[}hr{]}
+\item
+  Zone,Sum,Zone ITE Any Air Inlet Dewpoint Temperature Below Operating Range Time {[}hr{]}
+\item
+  Zone,Sum,Zone ITE Any Air Inlet Relative Humidity Above Operating Range Time {[}hr{]}
+\item
+  Zone,Sum,Zone ITE Any Air Inlet Relative Humidity Below Operating Range Time {[}hr{]}
+\end{itemize}
+
+\paragraph{Zone ITE CPU Electric Power {[}W{]}}\label{zone-ite-cpu-electric-power-w}
+
+ITE CPU Electric Power {[}W{]}
+
+\paragraph{Zone ITE CPU Electric Energy {[}J{]}}\label{zone-ite-cpu-electric-energy-j}
+
+\paragraph{ITE CPU Electric Energy {[}J{]}}\label{ite-cpu-electric-energy-j}
+
+The electric power (or energy) input to the ITE equipment CPU (total power input less cooling fan power). The ITE CPU Electric Energy output is also added to a meter object with Resource Type = Electricity, End Use Key = InteriorEquipment, Group Key = Building (Ref. Output:Meter object).
+
+\paragraph{Zone ITE CPU Electric Power at Design Inlet Conditions {[}W{]}}\label{zone-ite-cpu-electric-power-at-design-inlet-conditions-w}
+
+\paragraph{ITE CPU Electric Power at Design Inlet Conditions {[}W{]}}\label{ite-cpu-electric-power-at-design-inlet-conditions-w}
+
+\paragraph{Zone ITE CPU Electric Energy at Design Inlet Conditions {[}J{]}}\label{zone-ite-cpu-electric-energy-at-design-inlet-conditions-j}
+
+\paragraph{ITE CPU Electric Energy at Design Inlet Conditions {[}J{]}}\label{ite-cpu-electric-energy-at-design-inlet-conditions-j}
+
+The electric power (or energy) input to the ITE equipment CPU (total power input less cooling fan power) if the air inlet temperature were held at the design condition. May be used to calculate ``IT efficiency'', the ratio of (IT energy consumed in the facility) / (IT energy that would have been consumed in the facility if the ITE were held at the reference temperature).
+
+\paragraph{Zone ITE Fan Electric Power {[}W{]}}\label{zone-ite-fan-electric-power-w}
+
+\paragraph{ITE Fan Electric Power {[}W{]}}\label{ite-fan-electric-power-w}
+
+\paragraph{Zone ITE Fan Electric Energy {[}J{]}}\label{zone-ite-fan-electric-energy-j}
+
+\paragraph{ITE Fan Electric Energy {[}J{]}}\label{ite-fan-electric-energy-j}
+
+The electric power (or energy) input to the ITE cooling fan. The ITE Fan Electric Energy output is also added to a meter object with Resource Type = Electricity, End Use Key = InteriorEquipment, Group Key = Building (Ref. Output:Meter object).
+
+\paragraph{Zone ITE Fan Electric Power at Design Inlet Conditions {[}W{]}}\label{zone-ite-fan-electric-power-at-design-inlet-conditions-w}
+
+\paragraph{ITE Fan Electric Power at Design Inlet Conditions {[}W{]}}\label{ite-fan-electric-power-at-design-inlet-conditions-w}
+
+\paragraph{Zone ITE Fan Electric Energy at Design Inlet Conditions {[}J{]}}\label{zone-ite-fan-electric-energy-at-design-inlet-conditions-j}
+
+\paragraph{ITE Fan Electric Energy at Design Inlet Conditions {[}J{]}}\label{ite-fan-electric-energy-at-design-inlet-conditions-j}
+
+The electric power (or energy) input to the ITE cooling fan if the air inlet temperature were held at the design condition. May be used to calculate ``IT efficiency'', the ratio of (IT energy consumed in the facility) / (IT energy that would have been consumed in the facility if the ITE were held at the reference temperature).
+
+\paragraph{Zone ITE UPS Electric Power {[}W{]}}\label{zone-ite-ups-electric-power-w}
+
+\paragraph{ITE UPS Electric Power {[}W{]}}\label{ite-ups-electric-power-w}
+
+\paragraph{Zone ITE UPS Electric Energy {[}J{]}}\label{zone-ite-ups-electric-energy-j}
+
+\paragraph{ITE UPS Electric Energy {[}J{]}}\label{ite-ups-electric-energy-j}
+
+The net electric power (or energy) input to the ITE equipment UPS (total power input less power delivered to ITE). The ITE UPS Electric Energy output is also added to a meter object with Resource Type = Electricity, End Use Key = InteriorEquipment, Group Key = Building (Ref. Output:Meter object).
+
+\paragraph{Zone ITE UPS Heat Gain to Zone Rate {[}W{]}}\label{zone-ite-ups-heat-gain-to-zone-rate-w}
+
+\paragraph{ITE UPS Heat Gain to Zone Rate {[}W{]}}\label{ite-ups-heat-gain-to-zone-rate-w}
+
+\paragraph{Zone ITE UPS Heat Gain to Zone Energy {[}J{]}}\label{zone-ite-ups-heat-gain-to-zone-energy-j}
+
+\paragraph{ITE UPS Heat Gain to Zone Energy {[}J{]}}\label{ite-ups-heat-gain-to-zone-energy-j}
+
+The heat gain rate (or energy) to the zone from the UPS.
+
+\paragraph{Zone ITE Total Heat Gain to Zone Rate {[}W{]}}\label{zone-ite-total-heat-gain-to-zone-rate-w}
+
+\paragraph{ITE Total Heat Gain to Zone Rate {[}W{]}}\label{ite-total-heat-gain-to-zone-rate-w}
+
+\paragraph{Zone ITE Total Heat Gain to Zone Energy {[}J{]}}\label{zone-ite-total-heat-gain-to-zone-energy-j}
+
+\paragraph{ITE Total Heat Gain to Zone Energy {[}J{]}}\label{ite-total-heat-gain-to-zone-energy-j}
+
+The heat gain rate (or energy) to the zone from the UPS and from the CPU and fans if the ITE. Air Inlet Connection Type is AdjustedSupply or ZoneAirNode. If RoomAirModel is selected, then only the heat gain from the UPS is added directly to the zone air heat balance, the heat gain from the CPU and fans will be added to the ITE air Outlet Room Air Model Node
+
+\paragraph{Zone ITE Standard Density Air Volume Flow Rate {[}m3/s{]}}\label{zone-ite-standard-density-air-volume-flow-rate-m3s}
+
+\paragraph{ITE Standard Density Air Volume Flow Rate {[}m3/s{]}}\label{ite-standard-density-air-volume-flow-rate-m3s}
+
+Reports the average air volume flow rate through the ITE over the reporting interval. Standard density in EnergyPlus corresponds to 20ºC dry bulb, dry air, and nominally adjusted for elevation.
+
+\paragraph{Zone ITE Current Density Air Volume Flow Rate {[}m3/s{]}}\label{zone-ite-current-density-air-volume-flow-rate-m3s}
+
+\paragraph{ITE Current Density Air Volume Flow Rate {[}m3/s{]}}\label{ite-current-density-air-volume-flow-rate-m3s}
+
+Reports the average air volume flow rate through the ITE over the reporting interval, calculated using the current density at the air inlet node.
+
+\paragraph{Zone ITE Air Mass Flow Rate {[}kg/s{]}}\label{zone-ite-air-mass-flow-rate-kgs}
+
+\paragraph{ITE Air Mass Flow Rate {[}kg/s{]}}\label{ite-air-mass-flow-rate-kgs}
+
+Reports the average air mass flow rate through the ITE over the reporting interval, calculated using the current density at the air inlet node.
+
+\paragraph{ITE Air Inlet Dry-Bulb Temperature {[}C{]}}\label{ite-air-inlet-dry-bulb-temperature-c}
+
+The dry-bulb temperature of the air entering the ITE.
+
+\paragraph{ITE Air Inlet Dewpoint Temperature {[}C{]}}\label{ite-air-inlet-dewpoint-temperature-c}
+
+The dewpoint temperature of the air entering the ITE.
+
+\paragraph{ITE Air Inlet Relative Humidity {[}\%{]}}\label{ite-air-inlet-relative-humidity}
+
+The dewpoint temperature of the air entering the ITE.
+
+\paragraph{ITE Air Outlet Dry-Bulb Temperature {[}C{]}}\label{ite-air-outlet-dry-bulb-temperature-c}
+
+The dry-bulb temperature of the air leaving the ITE.
+
+\paragraph{\texorpdfstring{Zone ITE Average Supply Heat Index {[]}}{Zone ITE Average Supply Heat Index }}\label{zone-ite-average-supply-heat-index}
+
+\paragraph{\texorpdfstring{ITE Supply Heat Index {[]}}{ITE Supply Heat Index }}\label{ite-supply-heat-index}
+
+The supply heat index (SHI) for this equipment. SHI is a dimensionless measure of recirculation of hot air into the cold air intake of the ITE. SHI = (Tin -- Tsupply)/(Tout-Tsupply) where Tin is the dry-bulb temperature of the air entering the ITE, Tout is the dry-bulb temperature of the air leaving the ITE, and Tsupply is the dry-bulb temperature at the Supply Air Node. If a Supply Air Node Name is not specified for this object, then this output will not be reported.
+
+\paragraph{Zone ITE Any Air Inlet Operating Range Exceeded Time {[}hr{]}}\label{zone-ite-any-air-inlet-operating-range-exceeded-time-hr}
+
+\paragraph{ITE Air Inlet Operating Range Exceeded Time {[}hr{]}}\label{ite-air-inlet-operating-range-exceeded-time-hr}
+
+Hours when the dry-bulb and/or dewpoint temperature of the air entering the ITE is outside the range specified by the ITE Environmental Class.
+
+\paragraph{Zone ITE Any Air Inlet Dry-Bulb Temperature Above Operating Range Time {[}hr{]}}\label{zone-ite-any-air-inlet-dry-bulb-temperature-above-operating-range-time-hr}
+
+\paragraph{ITE Air Inlet Dry-Bulb Temperature Above Operating Range Time {[}hr{]}}\label{ite-air-inlet-dry-bulb-temperature-above-operating-range-time-hr}
+
+Hours when the dry-bulb temperature of the air entering the ITE is above the range specified by the ITE Environmental Class.
+
+\paragraph{ITE Air Inlet Dry-Bulb Temperature Difference Above Operating Range {[}deltaC{]}}\label{ite-air-inlet-dry-bulb-temperature-difference-above-operating-range-deltac}
+
+The temperature difference (in degrees DeltaC) between the air inlet dry-bulb temperature and the maximum allowable dry-bulb temperature specified by the ITE Environmental Class. Only positive values are reported. When the dry-bulb temperature of the air entering the ITE is below the maximum specified by the ITE Environmental Class, this output will be zero.
+
+\paragraph{Zone ITE Any Air Inlet Dry-Bulb Temperature Below Operating Range Time {[}hr{]}}\label{zone-ite-any-air-inlet-dry-bulb-temperature-below-operating-range-time-hr}
+
+\paragraph{ITE Air Inlet Dry-Bulb Temperature Below Operating Range Time {[}hr{]}}\label{ite-air-inlet-dry-bulb-temperature-below-operating-range-time-hr}
+
+Hours when the dry-bulb temperature of the air entering the ITE is above the range specified by the ITE Environmental Class.
+
+\paragraph{ITE Air Inlet Dry-Bulb Temperature Difference Below Operating Range {[}deltaC{]}}\label{ite-air-inlet-dry-bulb-temperature-difference-below-operating-range-deltac}
+
+The temperature difference (in degrees DeltaC) between the air inlet dry-bulb temperature and the minimum allowable dry-bulb temperature specified by the ITE Environmental Class. Only negative values are reported. When the dry-bulb temperature of the air entering the ITE is above the minimum specified by the ITE Environmental Class, this output will be zero.
+
+\paragraph{Zone ITE Any Air Inlet Dewpoint Temperature Above Operating Range Time {[}hr{]}}\label{zone-ite-any-air-inlet-dewpoint-temperature-above-operating-range-time-hr}
+
+\paragraph{ITE Air Inlet Dewpoint Temperature Above Operating Range Time {[}hr{]}}\label{ite-air-inlet-dewpoint-temperature-above-operating-range-time-hr}
+
+Hours when the dewpoint temperature of the air entering the ITE is above the range specified by the ITE Environmental Class.
+
+\paragraph{ITE Air Inlet Dewpoint Temperature Difference Above Operating Range {[}deltaC{]}}\label{ite-air-inlet-dewpoint-temperature-difference-above-operating-range-deltac}
+
+The temperature difference (in degrees DeltaC) between the air inlet dewpoint temperature and the maximum allowable dewpoint temperature specified by the ITE Envionmental Class. Only positive values are reported. When the dewpoint temperature of the air entering the ITE is below the maximum specified by the ITE Environmental Class, this output will be zero.
+
+\paragraph{Zone ITE Any Air Inlet Dewpoint Temperature Below Operating Range Time {[}hr{]}}\label{zone-ite-any-air-inlet-dewpoint-temperature-below-operating-range-time-hr}
+
+\paragraph{ITE Air Inlet Dewpoint Temperature Below Operating Range Time {[}hr{]}}\label{ite-air-inlet-dewpoint-temperature-below-operating-range-time-hr}
+
+Hours when the dewpoint temperature of the air entering the ITE is above the range specified by the ITE Environmental Class.
+
+\paragraph{ITE Air Inlet Dewpoint Temperature Difference Below Operating Range {[}deltaC{]}}\label{ite-air-inlet-dewpoint-temperature-difference-below-operating-range-deltac}
+
+The temperature difference (in degrees DeltaC) between the air inlet dewpoint temperature and the minimum allowable dewpoint temperature specified by the ITE Envionmental Class. Only negative values are reported. When the dewpoint temperature of the air entering the ITE is above the minimum specified by the ITE Environmental Class, this output will be zero.
+
+\paragraph{Zone ITE Any Air Inlet Relative Humidity Above Operating Range Time {[}hr{]}}\label{zone-ite-any-air-inlet-relative-humidity-above-operating-range-time-hr}
+
+\paragraph{ITE Air Inlet Relative Humidity Above Operating Range Time {[}hr{]}}\label{ite-air-inlet-relative-humidity-above-operating-range-time-hr}
+
+Hours when the relative humidity of the air entering the ITE is above the range specified by the ITE Environmental Class.
+
+\paragraph{ITE Air Inlet Relative Humidity Difference Above Operating Range {[}\%{]}}\label{ite-air-inlet-relative-humidity-difference-above-operating-range}
+
+The temperature difference (in degrees DeltaC) between the air inlet relative humidity and the maximum allowable relative humidity specified by the ITE Envionmental Class. Only positive values are reported. When the relative humidity of the air entering the ITE is below the maximum specified by the ITE Environmental Class, this output will be zero.
+
+\paragraph{Zone ITE Any Air Inlet Relative Humidity Below Operating Range Time {[}hr{]}}\label{zone-ite-any-air-inlet-relative-humidity-below-operating-range-time-hr}
+
+\paragraph{ITE Air Inlet Relative Humidity Below Operating Range Time {[}hr{]}}\label{ite-air-inlet-relative-humidity-below-operating-range-time-hr}
+
+Hours when the relative humidity of the air entering the ITE is above the range specified by the ITE Environmental Class.
+
+\paragraph{ITE Air Inlet Relative Humidity Difference Below Operating Range {[}\%{]}}\label{ite-air-inlet-relative-humidity-difference-below-operating-range}
+
+The temperature difference (in degrees DeltaC) between the air inlet relative humidity and the minimum allowable relative humidity specified by the ITE Envionmental Class. Only negative values are reported. When the relative humidity of the air entering the ITE is above the minimum specified by the ITE Environmental Class, this output will be zero.
+
+\subsection{ZoneContaminantSourceAndSink:CarbonDioxide}\label{zonecontaminantsourceandsinkcarbondioxide}
+
+The ZoneContaminantSourceAndSink:CarbonDioxide object allows users to input carbon dioxide sources or sinks in a zone. Note that carbon dioxide generation within a zone can also be specified using People and GasEquipment objects. Multiple ZoneContaminantSourceAndSink:CarbonDioxide~ objects can be specified for the same zone.
+
+\subsubsection{Inputs}\label{inputs-10-008}
+
+\paragraph{Field: Name}\label{field-name-10-007}
+
+The name of the ZoneContaminantSourceAndSink:CarbonDioxide object. The name for each ZoneContaminantSourceAndSink:CarbonDioxide object must be unique.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-2-003}
+
+This field is the name of the zone (ref: \textbf{Zone}) and links a particular ZoneContaminantSourceAndSink:CarbonDioxide object to a thermal zone in the building.
+
+\paragraph{Field: Design Generation Rate}\label{field-design-generation-rate}
+
+This field denotes the design carbon dioxide generation rate (m\(^{3}\)/s). The design value is modified by the schedule fraction (see Field: Schedule Name). The resulting volumetric generation rate is converted to mass generation rate using the current zone indoor air density at each time step. The rate can be either positive or negative. A positive value represents a source rate (CO\(_{2}\) addition to the zone air) and a negative value represents a sink rate (CO\(_{2}\) removal from the zone air).
+
+When the mass design generation rate is available, a conversion is required to meet input requirement with volumetric flow rate. This can be accomplished by the mass flow rate divided by the density of carbon dioxide.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-6-000}
+
+This field is the name of the schedule (ref: Schedules) that modifies the design carbon dioxide generation rate (see previous field). The schedule values can be any positive number between 0.0 and 1.0. For each simulation time step, the actual CO\(_{2}\) generation rate in a zone is the product of the Design Generation Rate field (above) and the value specified by this schedule.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+ZoneContaminantSourceAndSink:CarbonDioxide,
+  NORTH_ZONE CO2,       !- Name
+  NORTH_ZONE,           !- Zone Name
+  1.e-6,                !- Design Generation Rate {m3/s}
+  CO2 Source Schedule;  !- Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-004}
+
+HVAC,Average, Contaminant Source or Sink CO2 Gain Volume Flow Rate {[}m3/s{]}
+
+HVAC,Average, Zone Contaminant Source or Sink CO2 Gain Volume Flow Rate {[}m3/s{]}
+
+\paragraph{Contaminant Source or Sink CO2 Gain Volume Flow Rate {[}m3/s{]}}\label{contaminant-source-or-sink-co2-gain-volume-flow-rate-m3s}
+
+This output is the net carbond dioxide internal gain/loss in m3/s for an individual ZoneContaminantSourceAndSink:CarbonDioxide object.
+
+\paragraph{Zone Contaminant Source or Sink CO2 Gain Volume Flow Rate {[}m3/s{]}}\label{zone-contaminant-source-or-sink-co2-gain-volume-flow-rate-m3s}
+
+This output variable reports the total (net) carbon dioxide internal gains/losses in cubic meters per second for a zone, including impacts from three objects: ZoneContaminantSourceAndSink:CarbonDioxide, People, and GasEquipment. Positive values denote carbon dioxide generation (gain or source), while negative values denote carbon dioxide removal (loss or sink).
+
+\subsection{ZoneContaminantSourceAndSink:Generic:Constant}\label{zonecontaminantsourceandsinkgenericconstant}
+
+The ZoneContaminantSourceAndSink:Generic:Constant object specifies the generic contaminant generation rate and removal rate coefficient in a zone. The associated fraction schedules are required for allowing users to change the magnitude of sources and sinks. The object is equivalent to the combination of the constant coefficient model and the burst source model defined in the sources and sinks element types of CONTAM 3.0. The basic equation used to calculate generic contaminant source and sink for the constant model is given below:
+
+\begin{equation}
+{S_f}(t) = {G_f}(t)*{F_G} - {R_f}(t){C_f}(t)*1.0E - 6*{F_R}
+\end{equation}
+
+where
+
+\emph{S\(_{f}\)} = Contaminant generic contaminant source strength {[}m\(^{3}\)/s{]}
+
+\emph{G\(_{f}\)} = Generic contaminant generation rate {[}m\(^{3}\)/s{]}
+
+\emph{F\(_{G}\)} = Fraction value from the source fraction schedule at a given time {[}dimensionless{]}
+
+\emph{R\(_{f}\)} = Generic contaminant effective removal rate {[}m\(^{3}\)/s{]}
+
+\emph{F\(_{R}\)} = Fraction value from the sink fraction schedule at a given time {[}dimensionless{]}
+
+\emph{C\(_{f}\)} = Generic contaminant concentration value at a given previous time step {[}ppm{]}
+
+\subsubsection{Inputs}\label{inputs-11-007}
+
+\paragraph{Field: Name}\label{field-name-11-006}
+
+This field represents a unique identifying name.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-3-002}
+
+This field signifies the Name of the zone with constant generic contaminant source and sink.
+
+\paragraph{Field: Design Generation Rate}\label{field-design-generation-rate-1}
+
+This field denotes the full generic contaminant design generation rate (m\(^{3}\)/s). The design generation rate is the maximum amount of generic contaminant expected at design conditions. The design value is modified by the schedule fraction (see Field:Generation Schedule Name).
+
+When the mass generation rate is available, the rate must be converted to a volume flow rate. Use the mass flow rate divided by the vapor density of the generic contaminant.
+
+\paragraph{Field: Generation Schedule Name}\label{field-generation-schedule-name}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design generation rate (G\(_{f}\)). This fraction between 0.0 and 1.0 is noted as F\(_{G}\) in the above equation.
+
+\paragraph{Field: Design Removal Coefficient}\label{field-design-removal-coefficient}
+
+This field denotes the full generic contaminant design removal coefficient (m\(^{3}\)/s). The design removal rate is the maximum amount of generic contaminant expected at design conditions times the generic contaminant concentration in the same zone. The design value is modified by the schedule fraction (see Field:Removal Schedule Name).
+
+\paragraph{Field: Removal Schedule Name}\label{field-removal-schedule-name}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design generation rate (R\(_{f}\)). This fraction between 0.0 and 1.0 is noted as F\(_{R}\) in the above equation.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+ZoneContaminantSourceAndSink:Generic:Constant,
+  NORTH ZONE GC,        !- Name
+  NORTH ZONE,           !- Zone Name
+  1.0E-6,               !- Design Generation Rate {m3/s}
+  GC Source Schedule,   !- Generation Schedule Name
+  1.0E-7,               !- Design Removal Coefficient {m3/s}
+  GC Removal Schedule;  !- Removal Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-004}
+
+When a ZoneContaminantSourceAndSink:Generic:Constant object is specified, the following output variables are available:
+
+ZONE,Average, Generic Air Contaminant Constant Source Generation Volume Flow Rate {[}m3/s{]}
+
+\paragraph{Generic Air Contaminant Constant Source Generation Volume Flow Rate {[}m3/s{]}}\label{generic-air-contaminant-constant-source-generation-volume-flow-rate-m3s}
+
+This output is the average generic contaminant generation rate from each ZoneContaminantSourceAndSink:Generic:Constant object. The generation rate is a sum of generation and removal rates. The zone air generic contaminant level at the previous zone time step is used in the removal rate calculation.
+
+\subsection{Surface\-Contaminant\-Source\-And\-Sink:\-Generic:\-Pressure\-Driven}\label{surfacecontaminantsourceandsinkgenericpressuredriven}
+
+The Surface\-Contaminant\-Source\-And\-Sink:\-Generic:\-Pressure\-Driven object specifies the generic contaminant generation rate coefficient, which is used to calculate the generation rate due to the pressure difference across the surface. The object is equivalent to the pressure driven model defined in the sources and sinks element types of CONTAM 3.0. This object assumes to work with the AirflowNetwork model. The surface has to be defined in the AirflowNetwork:Multizone:Surface. Although the model is designed to be applied to radon and soil gas entry, it is expanded to be applied to all contaminant transport, including generic contaminant. However, it should be used in caution. The basic equation used to calculate generic contaminant source for the pressure driven constant model is provided below:
+
+\begin{equation}
+{S_f}(t) = {H_f}(t)*{F_G}*{\left( {{P_j} - {P_i}} \right)^n}
+\end{equation}
+
+where
+
+\emph{S\(_{f}\)} = Generic contaminant source strength {[}m\(^{3}\)/s{]}
+
+\emph{H\(_{f}\)} = Generic contaminant generation rate coefficient {[}m\(^{3}\)/s{]}
+
+\emph{F\(_{G}\)} = Fraction value from the source fraction schedule at a given time {[}dimensionless{]}
+
+\emph{n} = Flow power exponent
+
+P\emph{\(_{i}\)} = Zone pressure {[}Pa{]}
+
+P\emph{\(_{j}\)} = Pressure in an adjacent zone for a interior surface or outdoor for an exterior surface {[}Pa{]}
+
+\subsubsection{Inputs}\label{inputs-12-007}
+
+\paragraph{Field: Name}\label{field-name-12-005}
+
+The field signifies the unique identifying name.
+
+\paragraph{Field: Surface Name}\label{field-surface-name-2-000}
+
+This field represents the name of the surface as a generic contaminant source using the pressure driven model.
+
+\paragraph{Field: Design Generation Rate Coefficient}\label{field-design-generation-rate-coefficient}
+
+This field denotes the generic contaminant design generation coefficient (m\(^{3}\)/s). The design generation rate is the maximum amount of generic contaminant expected at design conditions times the pressure difference with a power exponent across a surface. The design value is modified by the schedule fraction (see Field:Generation Schedule Name).
+
+\paragraph{Field: Generation Exponent}\label{field-generation-exponent}
+
+This field denotes the flow power exponent,* n*, in the contaminant source equation. The valid range is 0.0 to 1.0,
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+SurfaceContaminantSourceAndSink:Generic:PressureDriven,
+  WEST ZONE GC BLD,     !- Name
+  Zn001:Wall001,        !- Surface Name
+  1.0E-6,               !- Design Generation Rate Coefficient {m3/s}
+  GC Source Schedule,   !- Generation Schedule Name
+  0.5;                  !- Generation Exponent
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8-003}
+
+When a Surface\-Contaminant\-Source\-And\-Sink:\-Generic:\-Pressure\-Driven object is specified, the following output variables are available:
+
+\begin{itemize}
+  \tightlist
+  \item
+    ZONE,Average,Generic Air Contaminant Pressure Driven Generation Volume Flow Rate {[}m3/s{]}
+\end{itemize}
+
+\paragraph{Generic Air Contaminant Pressure Driven Generation Volume Flow Rate {[}m3/s{]}}\label{generic-air-contaminant-pressure-driven-generation-volume-flow-rate-m3s}
+
+This output is the average generic contaminant generation rate from each Surface\-Contaminant\-Source\-And\-Sink:\-Generic:\-Pressure\-Driven object.
+
+\subsection{ZoneContaminantSourceAndSink:Generic:CutoffModel}\label{zonecontaminantsourceandsinkgenericcutoffmodel}
+
+The Zone\-Contaminant\-Source\-And\-Sink:\-Generic contaminant:CutoffModel object specifies the generic contaminant generation rate based on the cutoff concentration model. The basic equation used to calculate generic contaminant source for the pressure driven constant model is given below:
+
+\begin{equation}
+{S_f}(t) = \left\{ \begin{array}{l}{G_f}(t)*{F_G}*\left( {1 - \frac{{{C_f}(t)}}{{{C_{cutoff}}}}} \right)\;\;\;\;\;{C_f} < {C_{cutoff}}\\0\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;{C_f} \ge {C_{cutoff}}\end{array} \right\}
+\end{equation}
+
+where
+
+\(S_{f}\) = Generic contaminant source strength {[}m\(^{3}\)/s{]}
+
+\(G_{f}\) = Generic contaminant generation rate {[}m\(^{3}\)/s{]}
+
+\(F_{G}\) = Fraction value from the source fraction schedule at a given time {[}dimensionless{]}
+
+\(C_{\rm{cutoff}}\) = Cutoff concentration at which emission ceases {[}ppm{]}
+
+\(C_{f}\) = Generic contaminant concentration value at a given previous time step {[}ppm{]}
+
+\subsubsection{Inputs}\label{inputs-13-006}
+
+\paragraph{Field: Name}\label{field-name-13-005}
+
+The field signifies the unique identifying name.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-4-002}
+
+This field represents the name of the zone with generic contaminant source and sink using the cutoff model.
+
+\paragraph{Field: Design Generation Rate Coefficient}\label{field-design-generation-rate-coefficient-1}
+
+This field denotes the full generic contaminant design generation rate (m\(^{3}\)/s). The design generation rate is the maximum amount of generic contaminant expected at design conditions. The design value is modified by the schedule fraction (see Field:Generation Schedule Name).
+
+When the mass generation rate is available, the rate must be converted to a volume flow rate. Use the mass flow rate divided by the vapor density of the generic contaminant.
+
+\paragraph{Field: Generation Schedule Name}\label{field-generation-schedule-name-1}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design generation rate (G\(_{f}\)). This fraction between 0.0 and 1.0 is noted as F\(_{G}\) in the above equation.
+
+\paragraph{Field: Cutoff Generic Contaminant at which Emission Ceases}\label{field-cutoff-generic-contaminant-at-which-emission-ceases}
+
+This field is the generic contaminant cutoff concentration level where the source ceases its emission.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+ZoneContaminantSourceAndSink:Generic:CutoffModel,
+  NORTH ZONE GC CutoffModel,            !- Name
+  NORTH ZONE,                           !- Zone Name
+  1.0E-5,                               !- Design Generation Rate Coefficient {m3/s}
+  GC Source Schedule,                   !- Schedule Name
+  100000;                               !- Cutoff Generic Contaminant at which Emission Ceases {ppm}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-9-003}
+
+When a ZoneContaminantSourceAndSink:Generic:CutoffModel object is specified, the following output variables are available:
+
+ZONE,Average, Generic Air Contaminant Cutoff Model Generation Volume Flow Rate {[}m3/s{]}
+
+\paragraph{Generic Air Contaminant Cutoff Model Generation Volume Flow Rate {[}m3/s{]}}\label{generic-air-contaminant-cutoff-model-generation-volume-flow-rate-m3s}
+
+This output is the average generic contaminant generation rate from each Surface\-Contaminant\-Source\-And\-Sink:\-Generic:\-Cutoff\-Model object.
+
+\subsection{ZoneContaminantSourceAndSink:Generic:DecaySource}\label{zonecontaminantsourceandsinkgenericdecaysource}
+
+The ZoneContaminantSourceAndSink:Generic:DecaySource object specifies the generic contaminant generation rate based on the decay source model. The basic equation used to calculate generic contaminant source for the decay source model is given below:
+
+\begin{equation}
+{S_f}(t) = {G_f}(t){F_G}\exp ( - t/{t_c})
+\end{equation}
+
+where
+
+\emph{S\(_{f}\)} = Generic contaminant source strength {[}m\(^{3}\)/s{]}
+
+\emph{G\(_{f}\)} = Initial generic contaminant generation rate {[}m\(^{3}\)/s{]}
+
+\emph{F\(_{G}\)} = Fraction value from the source fraction schedule at a given time {[}dimensionless{]}
+
+\(t\) = Time since the start of emission {[}second{]}
+
+\emph{t\(_{c}\)} = Decay time constant {[}second{]}
+
+\subsubsection{Inputs}\label{inputs-14-006}
+
+\paragraph{Field: Name}\label{field-name-14-004}
+
+This field is the unique identifying name.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-5-002}
+
+This field represents the name of the zone with a generic contaminant decaying source.
+
+\paragraph{Field: Initial Emission Rate}\label{field-initial-emission-rate}
+
+This field denotes the initial generic contaminant design emission rate (m\(^{3}\)/s). The generation is controlled by a schedule, as defined in the next field. Generic contaminant emission begins when the schedule changes from a zero to a non-zero value (between zero and one). The initial emission rate is equal to the schedule value times the initial generation rate. A single schedule may be used to initiate several emissions at different times.(see Field:Generation Schedule Name).
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-7}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design emission rate (G\(_{f}\)). This fraction between 0.0 and 1.0 is noted as F\(_{G}\) in the above equation. When the value is equal to 1, the generation rate is used and time is reset to zero. When the value is equal to zero, the schedule value is ignored in the equation.
+
+\paragraph{Field: Decay Time Constant}\label{field-decay-time-constant}
+
+This field is the time at which the generation rate reaches 0.37 of the original rate.
+
+\begin{callout}
+  Note: The variable \(t\), time since the start of emission, will be reset to zero, when a new run period starts, or the generation schedule value is equal to zero.
+\end{callout}
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+ZoneContaminantSourceAndSink:Generic:DecaySource,
+  WEST ZONE GC DecaySource, !- Name
+  WEST ZONE,              !- Zone Name
+  1.0E-5,                 !- Initial Emission Rate {m3/s}
+  GC Source Schedule,     !- Schedule Name
+  100000;                 !- Delay Time Constant {s}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-10-003}
+
+When a ZoneContaminantSourceAndSink:Generic:DecaySource object is specified, the following output variables are available:
+
+\begin{itemize}
+    \tightlist
+  \item
+    Zone,Average,Generic Air Contaminant Decay Model Generation Volume Flow Rate {[}m3/s{]}
+  \item
+    Zone,Average,Generic Air Contaminant Decay Model Generation Emission Start Elapsed Time {[}s{]}
+\end{itemize}
+
+\paragraph{Generic Air Contaminant Decay Model Generation Volume Flow Rate {[}m3/s{]}}\label{generic-air-contaminant-decay-model-generation-volume-flow-rate-m3s}
+
+This output is the average generic contaminant decay rate from each Surface\-Contaminant\-Source\-And\-Sink:\-Generic:\-Decay\-Source object.
+
+\paragraph{Generic Air Contaminant Decay Model Generation Emission Start Elapsed Time {[}s{]}}\label{generic-air-contaminant-decay-model-generation-emission-start-elapsed-time-s}
+
+This output is the decay time since the start of emission. The start time is either at the beginning of each run period, including design day simulations, or the time when the egenration schedule value is zero.
+
+\subsection{Surface\-Contaminant\-Source\-And\-Sink:\-Generic:\-Boundary\-Layer\-Diffusion}\label{surfacecontaminantsourceandsinkgenericboundarylayerdiffusion}
+
+The Surface\-Contaminant\-Source\-And\-Sink:\-Generic:\-Boundary\-Layer\-Diffusion object specifies the generic contaminant generation rate from surface diffusion. The object is equivalent to the boundary layer diffusion model driven model defined in the sources and sinks element types of CONTAM 3.0.
+
+The boundary layer diffusion controlled reversible sink/source model with a linear sorption isotherm follows the descriptions presented in {[}Axley 1991{]}. The boundary layer refers to the region above the surface of a material through which a concentration gradient exists between the near-surface concentration and the air-phase concentration. The rate at which a contaminant is transferred onto a surface (sink) is defined as:
+
+\begin{equation}
+{S_f} = h*\rho *A\left( {{C_f} - \frac{{{C_s}}}{k}} \right)*1.0E - 6
+\end{equation}
+
+where
+
+\emph{h} = Average film mass transfer coefficient over the sink {[}m/s{]}
+
+\(\rho\) = Film density of air {[}kg/m\(^{3}\){]}
+
+\emph{A} = Surface area of the adsorbent {[}m\(^{2}\){]}
+
+\emph{C\(_{f}\)} = Concentration in the air at the previous time step {[}ppm{]}
+
+\emph{C\(_{s}\)} = Concentration in the adsorbent {[}ppm{]}
+
+\emph{k} = Henry adsorption constant or partition coefficient {[}dimensionless{]}
+
+\subsubsection{Inputs}\label{inputs-15-006}
+
+\paragraph{Field: Name}\label{field-name-15-004}
+
+This field signifies a unique identifying name.
+
+\paragraph{Field: Surface Name}\label{field-surface-name-3-000}
+
+This field denotes the name of the surface as a generic contaminant reversible source or sink using the boundary layer diffusion model.
+
+\paragraph{Field: Mass Transfer Coefficient}\label{field-mass-transfer-coefficient}
+
+This field specifies the average mass transfer coefficient of the contaminant generic contaminant within the boundary layer (or film) above the surface of the adsorbent.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-8}
+
+This field is the name of the schedule (ref: Schedule) that modifies the mass transfer coefficient with the value between 0.0 and 1.0.
+
+\paragraph{Field: Henry Adsorption Constant or Partition Coefficient}\label{field-henry-adsorption-constant-or-partition-coefficient}
+
+This field denotes the generic contaminant Henry partition coefficient in the units of dimensionless. The coefficient relates the concentration of the contaminant generic contaminant in the bulk-air to that at the surface of the adsorption material.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+SurfaceContaminantSourceAndSink:Generic:BoundaryLayerDiffusion,
+  WEST ZONE GC BLD,     !- Name
+  Zn001:Wall001,        !- Surface Name
+  1.0E-2,               !- Mass Transfer Coefficient {m/s}
+  GC Source Schedule,   !- Schedule Name
+  2.0;                  !- Henry adsorption constant or partition coefficient
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-11-003}
+
+When a Sur\-face\-Con\-taminant\-Source\-And\-Sink:\-Generic:\-Boundary\-Layer\-Diffusion object is specified, the following output variables are available:
+
+\begin{itemize}
+  \tightlist
+  \item
+    ZONE,Average, Generic Air Contaminant Boundary Layer Diffusion Generation Volume Flow Rate {[}m3/s{]}
+  \item
+    ZONE,Average, Generic Air Contaminant Boundary Layer Diffusion Inside Face Concentration {[}ppm{]}
+\end{itemize}
+
+\paragraph{Generic Air Contaminant Boundary Layer Diffusion Generation Volume Flow Rate {[}m3/s{]}}\label{generic-air-contaminant-boundary-layer-diffusion-generation-volume-flow-rate-m3s}
+
+This output is the average generic contaminant generation rate from each Sur\-face\-Contaminant\-Source\-And\-Sink:\-Generic:\-Boundary\-Layer\-Diffusion object.
+
+\paragraph{Generic Air Contaminant Boundary Layer Diffusion Inside Face Concentration {[}ppm{]}}\label{generic-air-contaminant-boundary-layer-diffusion-inside-face-concentration-ppm}
+
+This output is the average generic contaminant level at the interior surface.
+
+\subsection{Sur\-face\-Contaminant\-Source\-And\-Sink:\-Generic:\-Deposition\-Velocity\-Sink}\label{surfacecontaminantsourceandsinkgenericdepositionvelocitysink}
+
+The Sur\-face\-Contaminant\-Source\-And\-Sink:\-Generic:\-Deposition\-Velocity\-Sink object specifies the generic contaminant removal rate from a surface. The object is equivalent to the deposition velocity sink model defined in CONTAM 3.0 sources and sinks element types.
+
+The deposition velocity model provides for the input of a sink's characteristic in the familiar term of deposition velocity. The removal stops when the sink concentration level is higher than the zone air concentration level. The deposition velocity model equation is:
+
+\begin{equation}
+{S_f}(t) = {\nu_d}{A_s}m*{C_f}(t)*1.0E - 6*F{}_R
+\end{equation}
+
+where
+
+\(S_f (t)\) = Removal rate at time t {[}m\(^{3}\)/s{]}
+
+\(\nu_d\) = Deposition velocity {[}m/s{]}
+
+\(A_s\) = Deposition surface area {[}m\(^{2}\){]}
+
+\(m\) = Element multiplier {[}dimensionless{]}
+
+\(C_f (t)\) = Concentration of contaminant generic contaminant at the previous time step {[}ppm{]}
+
+\(\rm{F}_{R}\) = Schedule or control signal value at time \(t\) {[}-{]}
+
+\subsubsection{Inputs}\label{inputs-16-005}
+
+\paragraph{Field: Name}\label{field-name-16-004}
+
+This field denotes a unique identifying name.
+
+\paragraph{Field: Surface Name}\label{field-surface-name-4-000}
+
+This field represents the name of the surface as a generic contaminant sink using the deposition velocity sink model.
+
+\paragraph{Field: Deposition Velocity}\label{field-deposition-velocity}
+
+This field specifies the deposition velocity to the surface of the adsorbent in the units of m/s.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-9}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design removal rate (S\(_{f}\)). This fraction between 0.0 and 1.0 is noted as F\(_{R}\) in the above equation.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+SurfaceContaminantSourceAndSink:Generic:DepositionVelocitySink,
+  EAST ZONE GC DVS,     !- Name
+  Zn002:Wall001,        !- Surface Name
+  1.0E-3,               !- Deposition Velocity {m/s}
+  GC Source Schedule;   !- Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-12-003}
+
+The following output variables are available when the Surface\-Contaminant\-Source\-And\-Sink:\-Generic:\-Deposition\-Velocity\-Sink object is specified.
+
+\begin{itemize}
+    \tightlist
+  \item
+    ZONE,Average, Generic Air Contaminant Deposition Velocity Removal Volume Flow Rate {[}m3/s{]}
+\end{itemize}
+
+\paragraph{Generic Air Contaminant Deposition Velocity Removal Volume Flow Rate {[}m3/s{]}}\label{generic-air-contaminant-deposition-velocity-removal-volume-flow-rate-m3s}
+
+This output is the average generic contaminant generation rate from each Surface\-Contaminant\-Source\-And\-Sink:\-Generic:\-Deposition\-Velocity\-Sink object.
+
+\subsection{Zone\-Con\-taminant\-Source\-And\-Sink:\-Generic:\-Deposition\-Rate\-Sink}\label{zonecontaminantsourceandsinkgenericdepositionratesink}
+
+The Zone\-Contaminant\-Source\-And\-Sink:\-Generic:\-Deposition\-Rate\-Sink object specifies the generic contaminant removal rate from a zone. The object is equivalent to the deposition rate sink model defined in CONTAM 3.0 sources and sinks element types.
+
+The deposition rate model provides for the input of a sink's characteristic in the familiar term of deposition rate in a zone. The removal stops when the sink concentration level is higher than the zone air concentration level. The deposition rate model equation is:
+
+\begin{equation}
+{S_f}(t) = {k_d}{V_z}*{C_f}(t)*1.0E - 6*{F_R}m
+\end{equation}
+
+Where
+
+S\(_{f}\)(\emph{t}) = Removal rate at time t {[}m\(^{3}\)/s{]}
+
+\emph{k\(_{d}\)} = Deposition rate {[}1/T{]}
+
+\emph{V\(_{z}\)} = Zone volume {[}m\(^{3}\){]}
+
+\emph{m} = Element multiplier {[}dimensionless{]}
+
+\emph{C}\(_{f}\)(\emph{t}) = Concentration of generic contaminant at the previous time \emph{step} {[}ppm{]}
+
+F\(_{R}\) = Schedule or control signal value at time \emph{t} {[}dimensionless{]}
+
+\subsubsection{Inputs}\label{inputs-17-003}
+
+\paragraph{Field: Name}\label{field-name-17-003}
+
+This field denotes a unique identifying name.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-6-002}
+
+This field represents the name of the zone as a generic contaminant sink using the deposition rate sink model.
+
+\paragraph{Field: Deposition Rate}\label{field-deposition-rate}
+
+This field specifies the deposition rate to the zone in the units of 1/s.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-10}
+
+This field is the name of the schedule (ref: Schedule) that modifies the maximum design removal rate (S\(_{f}\)). This fraction between 0.0 and 1.0 is noted as F\(_{R}\) in the above equation.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+ZoneContaminantSourceAndSink:Generic:DepositionRateSink,
+  NORTH ZONE GC DRS,  !- Name
+  NORTH ZONE,         !- Zone Name
+  1.0E-5,             !- Deposition Rate {m3/s}
+  GC Source Schedule; !- Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-13-002}
+
+When the ZoneContaminantSourceAndSink:Generic:DepositionRateSink object is specified, the following output variables are available:
+
+\begin{itemize}
+    \tightlist
+  \item
+    ZONE,Average, Generic Air Contaminant Deposition Rate Removal Volume Flow Rate {[}m3/s{]}
+\end{itemize}
+
+\paragraph{Generic Air Contaminant Deposition Rate Removal Volume Flow Rate {[}m3/s{]}}\label{generic-air-contaminant-deposition-rate-removal-volume-flow-rate-m3s}
+
+This output is the average generic contaminant generation rate from each Zone\-Contaminant\-Source\-And\-Sink:\-Generic:\-Deposition\-Rate\-Sink object.
+
+\subsection{ZoneBaseboard:OutdoorTemperatureControlled}\label{zonebaseboardoutdoortemperaturecontrolled}
+
+This object specifies outside temperature-controlled (OTC) baseboard heating. The capacities (high and low) are specified in W at the temperatures specified. The schedule allows both capacities to change hourly on a proportional basis. This baseboard heater does not operate if the outdoor dry-bulb is above the high temperature limit. Between the high temperature and the low temperature, the capacity is interpolated (linear) between the high and the low capacity values. Below the low temperature, the capacity is set at the low capacity value. This allows the user to add baseboard heat to a perimeter zone starting at a prescribed temperature and then slowly increases this capacity to a max value.
+
+\textbf{Example:}
+
+\begin{center}
+  \begin{tabular}{@{}ll@{}}
+    Temperature High = 10 C & Capacity High = 100,000 W \\
+    Temperature Low = 0 C & Capacity Low = 500,000 W
+  \end{tabular}
+\end{center}
+
+% table 16
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Outdoor Temperature Controlled Baseboard Heat Temperature vs. Capacity \label{table:outdoor-temperature-controlled-baseboard-heat}} \tabularnewline
+\toprule 
+Outdoor Dry-bulb(C) & Baseboard Output \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Outdoor Temperature Controlled Baseboard Heat Temperature vs. Capacity} \tabularnewline
+\toprule 
+Outdoor Dry-bulb(C) & Baseboard Output \tabularnewline
+\midrule
+\endhead
+
+> 10 & 0 \tabularnewline
+10 & 100,000 \tabularnewline
+8 & 180,000 \tabularnewline
+6 & 260,000 \tabularnewline
+4 & 340,000 \tabularnewline
+2 & 420,000 \tabularnewline
+0 & 500,000 \tabularnewline
+< 0 & 500,000 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Inputs}\label{inputs-18-003}
+
+\paragraph{Field: Name}\label{field-name-18-003}
+
+The name of the ZoneBaseboard:OutdoorTemperatureControlled object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-7-002}
+
+This field is the name of the zone and attaches the baseboard heat equipment statement to a thermal zone in the building.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-11}
+
+This field is the name of the schedule that modifies the capacities (high and low) for baseboard heat equipment (see next four fields). The schedule values can be any positive number. The actual energy input for the baseboard equipment in a zone as defined by this statement depends on the actual outdoor temperature and where that temperature is in the range of Low Temperature to High Temperature..
+
+\paragraph{Field: Capacity at Low Temperature}\label{field-capacity-at-low-temperature}
+
+This is the baseboard equipment capacity (Watts) at the low temperature limit. This is the maximum capacity of the baseboard equipment in full load operation. This field is autosizable.
+
+\paragraph{Field: Low Temperature}\label{field-low-temperature}
+
+If the outdoor dry-bulb temperature (degrees Celsius) is at or below the low temperature the baseboard heater operates at the low temperature capacity. This field is autosizable. The lowest design outdoor dry bulb temperature is chosen, if autosized.
+
+\paragraph{Field: Capacity at High Temperature}\label{field-capacity-at-high-temperature}
+
+This is the baseboard equipment capacity (Watts) at the high temperature limit. This field is autosizable. The capacity at low temperature is prorated against the reference low and high temperature fields, if autosized.
+
+\paragraph{Field: High Temperature}\label{field-high-temperature}
+
+If the outdoor dry-bulb temperature (degrees Celsius) is greater than the high temperature the baseboard heater will not operate. This field is autosizable. If autosized, this is equal to the design zone heating setpoint temperature described below, so that the capacity at high temperature is zero.
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant-7}
+
+This field is a decimal number between 0.0 and 1.0 and is used to characterize the type of heat being given off by baseboard heat equipment in a zone.~ The number specified in this field will be multiplied by the total energy consumed by the baseboard heat equipment to give the amount of long wavelength radiation gain to the zone.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-5}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Perimeter Baseboards'', etc. A new meter for reporting is created for each unique subcategory~ (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the baseboard equipment will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Design Zone Heating Setpoint}\label{field-design-zone-heating-setpoint}
+
+This is heating setpoint temperature in the zone where the unit serves. This is used to autosize high temperature and capacity at high temperature fields. The default value is 20°C.
+
+An IDF example:
+
+\begin{lstlisting}
+ZoneBaseboard:OutdoorTemperatureControlled,
+  SPACE4-1 BBHeat 1,  !- Name
+  SPACE4-1,           !- Zone Name
+  EQUIP-1,            !- SCHEDULE Name
+  1500,               !- Capacity at low temperature {W}
+  0,                  !- Low Temperature {C}
+  500,                !- Capacity at high temperature {W}
+  10,                 !- High Temperature {C}
+  0.5,                !- Fraction Radiant
+  Baseboard Heat,     !- End-Use Subcategory
+  20;                 !- Design Zone Heating Setpoint {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-14-002}
+
+ZoneBaseboard:OutdoorTemperatureControlled objects have output variables for individual objects and for zone totals. The following outputs are available:
+
+\begin{itemize}
+\tightlist
+\item
+  Zone,Average,Baseboard Electric Power {[}W{]}
+\item
+  Zone,Sum,Baseboard Electric Energy {[}J{]}
+\item
+  Zone,Sum,Baseboard Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Baseboard Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Baseboard Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Baseboard Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Baseboard Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Baseboard Total Heating Rate {[}W{]}
+\item
+  Zone,Average,Zone Baseboard Electric Power {[}W{]}
+\item
+  Zone,Sum,Zone Baseboard Electric Energy {[}J{]}
+\item
+  Zone,Sum,Zone Baseboard Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Baseboard Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Baseboard Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Baseboard Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Baseboard Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Baseboard Total Heating Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Baseboard Electric Power {[}W{]}}\label{baseboard-electric-power-w}
+
+This field is the electric power for the ZoneBaseboard:OutdoorTemperatureControlled object in Watts.
+
+\paragraph{Baseboard Electric Energy {[}J{]}}\label{baseboard-electric-energy-j}
+
+The outdoor temperature controlled baseboard heat option is assumed to be fueled by electricity. This field is the same as the Baseboard Total Heating Energy (above) in joules.
+
+\paragraph{Baseboard Radiant Heating Rate {[}W{]}}\label{baseboard-radiant-heating-rate-w}
+
+\paragraph{Baseboard Radiant Heating Energy {[}J{]}}\label{baseboard-radiant-heating-energy-j}
+
+These output variables are the amount of radiant heat gain for the Zone\-Baseboard:\-Outdoor\-Temperature\-Controlled object in Watts (for rate) or Joules. This is determined by the current heat gain from the heater to the zone and the ``Fraction Radiant'' specified in the input. The radiant gains (long wavelength) are distributed to the surfaces using an area weighting scheme.
+
+\paragraph{Baseboard Convective Heating Rate {[}W{]}}\label{baseboard-convective-heating-rate-w}
+
+\paragraph{Baseboard Convective Heating Energy {[}J{]}}\label{baseboard-convective-heating-energy-j}
+
+These output variables are the amount of convective heat gain for the Zone\-Baseboard:\-Outdoor\-Temperature\-Controlled object in Watts (for rate) or Joules. This is determined by the current heat gain from the heater to the zone and the ``Fraction Radiant'' specified in input (1-FractionRadiant = FractionConvected). The convective heat gain is added to the zone air heat balance directly.
+
+\paragraph{Baseboard Total Heating Rate {[}W{]}}\label{baseboard-total-heating-rate-w}
+
+\paragraph{Baseboard Total Heating Energy {[}J{]}}\label{baseboard-total-heating-energy-j}
+
+These output variables are the amount of heat gain for the Zone\-Baseboard:\-Outdoor\-Temperature\-Controlled object in Watts (for rate) or Joules. This is determined by the sum of the radiant and convective heat gains from the baseboard heat.
+
+\paragraph{Zone Baseboard Electric Power {[}W{]}}\label{zone-baseboard-electric-power-w}
+
+This field is the electric power for all Zone\-Baseboard:\-Outdoor\-Temperature\-Controlled objects within the zone in Watts.
+
+\paragraph{Zone Baseboard Electric Energy {[}J{]}}\label{zone-baseboard-electric-energy-j}
+
+The outdoor temperature controlled baseboard heat option is assumed to be fueled by electricity. This field is the same as the Baseboard Total Heating Energy (above) in joules. However, this amount is also shown in the Electricity meters that are associated with the zone -- Electricity:\-Facility, Electricity:\-Buidling, Electricity:\-Zone:\-\textless{}Zone Name\textgreater{}, and Interior\-Equipment:\-Electricity.
+
+\paragraph{Zone Baseboard Radiant Heating Rate {[}W{]}}\label{zone-baseboard-radiant-heating-rate-w}
+
+\paragraph{Zone Baseboard Radiant Heating Energy {[}J{]}}\label{zone-baseboard-radiant-heating-energy-j}
+
+These output variables are the amount of radiant heat gain for all Zone\-Baseboard:\-Outdoor\-Temperature\-Controlled objects within the zone in Watts (for rate) or Joules. This is determined by the current heat gain from the heater to the zone and the ``Fraction Radiant'' specified in the input. The radiant gains (long wavelength) are distributed to the surfaces using an area weighting scheme.
+
+\paragraph{Zone Baseboard Convective Heating Rate {[}W{]}}\label{zone-baseboard-convective-heating-rate-w}
+
+\paragraph{Zone Baseboard Convective Heating Energy {[}J{]}}\label{zone-baseboard-convective-heating-energy-j}
+
+These output variables are the amount of convective heat gain for all Zone\-Baseboard:\-Outdoor\-Temperature\-Controlled objects within the zone in Watts (for rate) or Joules. This is determined by the current heat gain from the heater to the zone and the ``Fraction Radiant'' specified in input (1-FractionRadiant = FractionConvected). The convective heat gain is added to the zone air heat balance directly.
+
+\paragraph{Zone Baseboard Total Heating Rate {[}W{]}}\label{zone-baseboard-total-heating-rate-w}
+
+\paragraph{Zone Baseboard Total Heating Energy {[}J{]}}\label{zone-baseboard-total-heating-energy-j}
+
+These output variables are the amount of heat gain for all Zone\-Baseboard:\-Outdoor\-Temperature\-Controlled objects within the zone in Watts (for rate) or Joules. This is determined by the sum of the radiant and convective heat gains from the baseboard heat.
+
+\subsubsection{Outputs}\label{outputs-15-001}
+
+As described in each of the equipment sections, values for specific equipments will show up on the following meters:
+
+% table 17
+\begin{longtable}[c]{>{\raggedright}p{2.8in}>{\raggedright}p{1.2in}>{\raggedright}p{2.0in}}
+\caption{Distribution of Equipment to Meters \label{table:distribution-of-equipment-to-meters}} \tabularnewline
+\toprule 
+Meter Name & Scope & Equipment Specfics \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Distribution of Equipment to Meters} \tabularnewline
+\toprule 
+Meter Name & Scope & Equipment Specfics \tabularnewline
+\midrule
+\endhead
+
+Electricity:\-Facility & Entire Facility & Electric Equipment, OTC Baseboard Heat \tabularnewline
+Electricity:\-Building & All Zones & Electric Equipment, OTC Baseboard Heat \tabularnewline
+Electricity:\-Zone: <Zone Name> & Specific Zone & Electric Equipment, OTC Baseboard Heat \tabularnewline
+Interior\-Equipment:\-Electricity & AllZones & Electric Equipment, OTC Baseboard Heat \tabularnewline
+<End-Use Subcategory> :\-Interior\-Equipment:\-Electricity & Specific Subcategory & Electric Equipment, OTC Baseboard Heat \tabularnewline
+Gas:\-Facility & Entire Facility & Gas Equipment \tabularnewline
+Gas:\-Building & All Zones & Gas Equipment \tabularnewline
+Gas:\-Zone: <Zone Name> & Specific Zone & Gas Equipment \tabularnewline
+Interior\-Equipment:\-Gas & AllZones & Gas Equipment \tabularnewline
+<End-Use Subcategory> :Interior\-Equipment:\-Gas & Specific Subcategory & Gas Equipment \tabularnewline
+\bottomrule
+\end{longtable}
+
diff --git a/doc/input-output-reference/src/overview/group-location-climate-weather-file-access.tex b/doc/input-output-reference/src/overview/group-location-climate-weather-file-access.tex
new file mode 100644
index 00000000000..75d608a0b2b
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-location-climate-weather-file-access.tex
@@ -0,0 +1,2114 @@
+\section{Group -- Location -- Climate -- Weather File Access}\label{group-location-climate-weather-file-access}
+
+This group of objects describes the ambient conditions for the simulation.
+
+\subsection{Site:Location}\label{sitelocation}
+
+The location class describes the parameters for the building's location. Only one location is allowed. Weather data file location, if it exists, will override any location data in the IDF. Thus, for an annual simulation, a Location does not need to be entered.
+
+\subsubsection{Inputs}\label{inputs-026}
+
+\paragraph{Field: Name}\label{field-name-025}
+
+This alpha field is used as an identifying field in output reports.
+
+\paragraph{Field: Latitude}\label{field-latitude}
+
+This field represents the latitude (in degrees) of the facility. By convention, North Latitude is represented as positive; South Latitude as negative. Minutes should be represented in decimal fractions of 60. (15' is 15/60 or .25)
+
+\paragraph{Field: Longitude}\label{field-longitude}
+
+This field represents the longitude (in degrees) of the facility. By convention, East Longitude is represented as positive; West Longitude as negative. Minutes should be represented in decimal fractions of 60. (15' is 15/60 or .25)
+
+\paragraph{Field: Time Zone}\label{field-time-zone}
+
+This field represents the time zone of the facility (relative to Greenwich Mean Time or the 0\(^{th}\) meridian). Time zones west of GMT (e.g. North America) are represented as negative; east of GMT as positive. Non-whole hours can be represented in decimal (e.g. 6:30 is 6.5).
+
+\paragraph{Field: Elevation}\label{field-elevation}
+
+This field represents the elevation of the facility in meters (relative to sea level).
+
+Units with their abbreviations are shown in Appendix A. And, as shown in an IDF:
+
+\begin{lstlisting}
+Site:Location, DENVER COLORADO, ! Name
+   39.75000,                    ! Latitude {N+ S-}
+  -104.8700,                    ! Longitude {W- E+}
+  -7.000000,                    ! TimeZoneNumber {GMT+/-}
+  1610.26;                      ! Elevation {m}
+\end{lstlisting}
+
+Most examples in this document include the comment lines that illustrate each data field's value. However, this is not necessary (though it makes the IDF more readable). The previous example could also be:
+
+\begin{lstlisting}
+Site:Location, DENVER COLORADO,39.75,-104.87,-7,1610.26;
+\end{lstlisting}
+
+\subsection{SizingPeriod:DesignDay}\label{sizingperioddesignday}
+
+The design day input describes the parameters to effect a ``design day'' simulation, often used for load calculations or sizing equipment. Using the values in these fields, EnergyPlus ``creates'' a complete days' worth of weather data (air temperatures, solar radiation, etc.) Normal operation uses the default range multipliers as shown in Figure~\ref{fig:default-daily-range-multiplier-for-design} though users may choose to input their own multiplier schedule. Likewise, normal operation specifies one ``humidity indicating condition'' which is used to calculate the humidity ratio at maximum temperature -- this is used as the constant humidity ratio for the entire day. Again, this can be overridden by specifying a relative humidity schedule or requesting generation of an hourly wet-bulb temperature profile. Multiple design days may be specified.
+
+We refer you to the ASHRAE Handbook of Fundamentals for philosophy of what parameters are important for use as ``design conditions'' in sizing equipment.
+
+\begin{callout}
+  In the install, the ``design day files'' are included for the weather file locations that are included (weatherdata folder). All the design day definitions from the ASHRAE design conditions (latest publication date) are included, grouped by WMO region, on the main web site with the weather data. http://www.energyplus.gov/cfm/weather\_data.cfm These files are in ``macro'' form but it is easy to cut and paste the appropriate definition segments. These files include the location information as well as some locations have \textbf{RunPeriodControl:DaylightSavingTime} objects.
+\end{callout}
+
+\subsubsection{Inputs}\label{inputs-1-024}
+
+\paragraph{Field: Name}\label{field-name-1-023}
+
+This field, like the location name, is used simply for reporting and identification. This name must be unique among the SizingPeriod names entered.
+
+\paragraph{Field: Month}\label{field-month}
+
+This numeric field specifies the month. That, in conjunction with the day of the month and location information, determines the current solar position and solar radiation values for each hour of the day.
+
+\paragraph{Field: Day of Month}\label{field-day-of-month}
+
+This numeric field specifies the day of the month. That, in conjunction with the month and location information, determines the current solar position and solar radiation values for each hour of the day.
+
+\paragraph{Field: Day Type}\label{field-day-type}
+
+This alpha field specifies the day type for the design day. This value indicates which day profile to use in schedules. For further information, see the Schedule discussion later in this document. (ref: Schedule) Note that two of the possible day types are SummerDesignDay (for cooling) and WinterDesignDay (for heating) -- allowing the user to customize schedules for the design conditions. That is, for design days tagged with a SummerDesignDay type, you can set schedules to be worst or typical schedules for a cooling season.
+
+\paragraph{Field: Maximum Dry-Bulb Temperature}\label{field-maximum-dry-bulb-temperature}
+
+This numeric field should contain the day's maximum dry-bulb temperature in degrees Celsius. (Reference Appendix A of this document for EnergyPlus standard units and abbreviations). The MacroDataSets design day files show extreme temperature for locations as indicated in the ASHRAE HOF design condition tables.
+
+\paragraph{Field: Daily Dry-bulb Temperature Range}\label{field-daily-dry-bulb-temperature-range}
+
+A design day can have a ``high'' temperature and a ``low'' temperature (or can be a constant temperature for each hour of the day). If there is a difference between high and low temperatures, this field should contain the difference from the high to the low. EnergyPlus, by default, distributes this range over the 24 hours in the day as shown in the figure below:
+
+\begin{figure}[hbtp] % fig 6
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image010.png}
+\caption{Default Daily range Multiplier for Design Days \protect \label{fig:default-daily-range-multiplier-for-design}}
+\end{figure}
+
+The multipliers are taken from the ASHRAE 2009 HOF. More explicitly, EnergyPlus creates an air temperature for each timestep by using the entered maximum dry-bulb temperature in conjunction with the entered daily range and the above multiplier values. The actual equation used is shown below:
+
+\begin{equation}
+{T_{current}} = {T_{Max}} - {T_{range}}\cdot {T_{Multiplier}}
+\end{equation}
+
+where
+
+T\(_{current}\) = Air temperature of current Hour of Day
+
+T\(_{Max}\) = User supplied Max Dry-bulb Temperature
+
+T\(_{range}\) = User supplied Daily Temperature Range
+
+T\(_{Multiplier}\) = Range multiplier as shown on the above graph
+
+The range multiplier values represent typical conditions of diurnal temperatures (i.e. the low temperature for the day occurring about 5:00 AM and the maximum temperature for the day occurring about 3:00 PM. Note that EnergyPlus does not shift the profile based on the time of solar noon as is optionally allowed in ASHRAE procedures.
+
+ASHRAE research indicates that dry-bulb and wet-bulb temperatures typically follow the same profile, so EnergyPlus can use the default profile to generate humidity conditions (see Humidity Indicating Type = WetBulbProfileDefaultMultipliers below).
+
+\paragraph{Field: Dry-Bulb Temperature Range Modifier Type}\label{field-dry-bulb-temperature-range-modifier-type}
+
+If you are happy with lows at 5am and highs at 3pm, you can ignore this field. If you want to specify your own temperature range multipliers (see earlier discussion at the Temperature Range field description), you can specify a type here and create a day schedule which you reference in the next field.
+
+If you specify \textbf{MultiplierSchedule} in this field, then you need to create a day schedule that specifies a multiplier applied to the temperature range field (above) to create the proper dry-bulb temperature range profile for your design day.
+
+If you specify \textbf{DifferenceSchedule} in this field, then you need to create a day schedule that specifies a number to be \textbf{subtracted} from dry-bulb maximum temperature for each timestep in the day. Note that numbers in the delta schedules cannot be negative as that would result in a higher maximum than the maximum previously specified.
+
+If you specify \textbf{TemperatureProfileSchedule} in this field, then you need to create a day schedule that specifies the actual dry-bulb temperatures throughout the day. You will not need to include a Maximum Dry-Bulb Temperature in that field.
+
+If you leave this field blank or enter \textbf{DefaultMultipliers}, then the default multipliers will be used as shown in the ``temperature range'' field above.
+
+\paragraph{Field: Dry-Bulb Temperature Range Modifier Day Schedule Name}\label{field-dry-bulb-temperature-range-modifier-day-schedule-name}
+
+This field is the name of a \textbf{day schedule} (ref. Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List objects) with the values as specified in the Dry-Bulb Temperature Range Modifier Type field above.
+
+\paragraph{Field: Humidity Condition Type}\label{field-humidity-condition-type}
+
+The values/schedules indicated here and in subsequent fields create the humidity values in the 24 hour design day conditions profile. Valid choices here are: \textbf{WetBulb}, \textbf{Dewpoint}, \textbf{WetBulbProfileDefaultMultipliers, WetBulbProfileDifferenceSchedule,} \textbf{WetBulbProfileMultiplierSchedule}, \textbf{HumidityRatio}, \textbf{Enthalpy}, and \textbf{Schedule.}
+
+The Humidity Condition Type fields have interacting uses and units, summarized as follows:
+
+% table 2
+\begin{longtable}[c]{p{2.25in}p{1.75in}p{2.0in}}
+\caption{Humidity Indicating Field Interactions - Design Day \label{table:humidity-indicating-field-interactions-design}} \tabularnewline
+\toprule 
+Humidity Condition Type & Primary Humidity Indicating Field & Humidity Indicating Day Schedule \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Humidity Indicating Field Interactions - Design Day} \tabularnewline
+\toprule 
+Humidity Condition Type & Primary Humidity Indicating Field & Humidity Indicating Day Schedule \tabularnewline
+\midrule
+\endhead
+
+WetBulb & Wetbulb or DewPoint at Maximum Dry-Bulb & N/A (unused) \tabularnewline
+DewPoint & Wetbulb or DewPoint at Maximum Dry-Bulb & N/A (unused) \tabularnewline
+HumidityRatio & Humidity Ratio at Maximum Dry-Bulb & N/A (unused) \tabularnewline
+Enthalpy & Enthalpy at Maximum Dry-Bulb & N/A (unused) \tabularnewline
+WetBulbProfile\-DefaultMultipliers & Wetbulb or DewPoint at Maximum Dry-Bulb & N/A (unused) \tabularnewline
+WetBulbProfile\-MultiplierSchedule & Wetbulb or DewPoint at Maximum Dry-Bulb & Fractions of wet-bulb daily range (0 – 1) \tabularnewline
+WetBulbProfile\-DifferenceSchedule & Wetbulb or DewPoint at Maximum Dry-Bulb & Difference between maximum and hour/timestep wet-bulb temperature, C \tabularnewline
+RelativeHumidity\-Schedule & N/A & Relative humidity (\%, 0 – 100) \tabularnewline
+\bottomrule
+\end{longtable}
+
+Humidity conditions over the day are derived as follows:
+
+\textbf{WetBulb, DewPoint, HumidityRatio, or Enthalpy}:
+
+These four methods assume constant absolute humidity over the day. Calculate W = humidity ratio at Maximum Dry-Bulb Temperature and Humidity Indicating Conditions. Derive hourly/timestep humidity conditions from W and hour/timestep dry-bulb temperature.
+
+\textbf{WetBulbProfileDefaultMultipliers}
+
+Generate the wet-bulb temperature profile using Default Daily Range Multiplier for Design Days (shown in Figure~\ref{fig:default-daily-range-multiplier-for-design} above) and Daily Wet-Bulb Temperature Range (below). This method is analogous to DefaultMultiplier generation of the dry-bulb temperature profile and is the procedure recommended in Chapter 14 of ASHRAE 2009 HOF.
+
+\textbf{WetBulbProfileMultiplierSchedule}
+
+Generate the wet-bulb profile using multipliers from the Humidity Indicating Day Schedule and Daily Wet-Bulb Temperature Range (below). Analogous to dry-bulb MultiplierSchedule.
+
+\textbf{WetBulbProfileDifferenceSchedule}
+
+Generate the wet-bulb profile by subtracting Humidity Indicating Day Schedule values from the daily maximum wet-bulb temperature (specified in Humidity Indicating Conditions at Maximum Dry-Bulb). Analogous to dry-bulb DifferenceSchedule.
+
+\textbf{RelativeHumiditySchedule}
+
+Hourly relative humidity is specified in Humidity Indicating Day Schedule.
+
+In all cases, the humidity ratio is limited to saturation at the hour/timestep dry-bulb (that is, the dry-bulb temperature is used as specified, but the humidity ratio is modified as needed to be physically possible). Once a valid air state is determined, a complete set of consistent hour/timestep psychrometric values (dewpoint, wet-bulb, and enthalpy) is derived.
+
+\paragraph{Field: Wetbulb or DewPoint at Maximum Dry-Bulb}\label{field-wetbulb-or-dewpoint-at-maximum-dry-bulb}
+
+If you choose \textbf{Wetbulb} or \textbf{Dewpoint} in the Humidity Condition Type field, then this numeric field should contain that value. Note that this field is unnecessary when you put in a humidity indicating day schedule (described later in this section).
+
+\paragraph{Field: Humidity Condition Day Schedule Name}\label{field-humidity-condition-day-schedule-name}
+
+Allows specification a day schedule (ref. Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List objects) of values for relative humidity or wet-bulb profile per Humidity Indicating Type field.
+
+\paragraph{Field: Humidity Ratio at Maximum Dry-Bulb}\label{field-humidity-ratio-at-maximum-dry-bulb}
+
+If \textbf{HumidityRatio} is chosen for the Humidity Condition Type field, then this numeric field should contain the desired humidity ratio at maximum dry-bulb temperature (units kg Water / kg Dry Air).
+
+\paragraph{Field: Enthalpy at Maximum Dry-Bulb}\label{field-enthalpy-at-maximum-dry-bulb}
+
+If \textbf{Enthalpy} is chosen for the Humidity Condition Type field, then this numeric field should contain the desired enthalpy at maximum dry-bulb temperature (units Joules /kg).
+
+\paragraph{Field: Daily Wet-Bulb Temperature Range}\label{field-daily-wet-bulb-temperature-range}
+
+The difference between the maximum and minimum wet-bulb temperatures on the design day (Celsius). Used for generating daily profiles of humidity conditions when Humidity Condition Type field (above) is \textbf{WetBulbProfileDefaultMultipliers} or \textbf{WetBulbProfileMultiplierSchedule}. Values for wet-bulb temperature range are tabulated by month for 5564 locations worldwide on the CD that accompanies the ASHRAE 2009 HOF.
+
+\paragraph{Field: Barometric Pressure}\label{field-barometric-pressure}
+
+This numeric field is the constant barometric pressure (Pascals) for the entire day.
+
+\paragraph{Field: Wind Speed}\label{field-wind-speed}
+
+This numeric field is the wind speed in meters/second (constant throughout the day) for the day. The MacroDataSets design day files includes wind speed values (99.6\% - heating, 1\% cooling) as indicated in ASHRAE HOF design condition tables. But, you should be aware that traditional values for these are 6.7056 m/s (15 mph) for heating and 3.3528 m/s (7 mph) for cooling. A reminder is shown in the comments for the wind speed values. The comments also note the extreme wind speeds from the ASHRAE tables.
+
+\paragraph{Field: Wind Direction}\label{field-wind-direction}
+
+This numeric field is the source wind direction in degrees. By convention, winds from the North would have a value of 0., from the East a value of 90.
+
+\paragraph{Field: Rain Indicator}\label{field-rain-indicator}
+
+This field indicates whether or not the building surfaces are wet. If the value is Yes, then it is assumed that the building surfaces are wet. Wet surfaces may change the conduction of heat through the surface.
+
+\paragraph{Field: Snow Indicator}\label{field-snow-indicator}
+
+This field indicates whether or not there is snow on the ground. If the value is Yes, then it is assumed there is snow on the ground. Snow on the ground changes the ground reflectance properties.
+
+\paragraph{Field: Daylight Saving Time Indicator}\label{field-daylight-saving-time-indicator}
+
+This field specifies whether to consider this day to be a Daylight Saving Day. Yes in the field indicates that daylight saving time is operational for this day. Yes essentially adds 1 hour to the scheduling times used in items with schedules.
+
+\paragraph{Field: Solar Model Indicator}\label{field-solar-model-indicator}
+
+This field allows the user to select \textbf{ASHRAE\-Clear\-Sky, ASHRAE\-Tau, Zhang\-Huang, or Sche\-dule} for solar modeling in the calculation of the solar radiation in the design day. ASHRAE\-Clear\-Sky and Zhang\-Huang use the Clearness value as part of their calculations. ASHRAE\-Tau invokes the revised model specified in Chapter 14 of the ASHRAE 2009 HOF and uses Taub and Taud values (below). Technical details of the models are described in the Engineering Reference. The \textbf{Schedule} choice allows you to enter schedule values for the day's profile (use the next two fields for the names).
+
+\paragraph{Field: Beam Solar Day Schedule Name}\label{field-beam-solar-day-schedule-name}
+
+This field allows the option for you to put in your own day profile of beam solar values (wh/m2). These values will replace the calculated values during design day processing. Only day schedules (ref. Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List objects) are used here.
+
+\paragraph{Field: Diffuse Solar Day Schedule Name}\label{field-diffuse-solar-day-schedule-name}
+
+This field allows the option for you to put in your own day profile of diffuse solar values (wh/m2). These values will replace the calculated values during design day processing. Only day schedules (ref. Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List objects) are used here.
+
+\paragraph{Field: ASHRAE Clear Sky Optical Depth for Beam Irradiance (taub)}\label{field-ashrae-clear-sky-optical-depth-for-beam-irradiance-taub}
+
+Optical depth for beam radiation, used only when Solar Model Indicator is ASHRAETau. See next field.
+
+\paragraph{Field: ASHRAE Clear Sky Optical Depth for Diffuse Irradiance (taud)}\label{field-ashrae-clear-sky-optical-depth-for-diffuse-irradiance-taud}
+
+Optical depth for diffuse radiation, used only when Solar Model Indicator is ASHRAETau. Taub and Taud values are tabulated by month for 5564 locations worldwide on the CD that accompanies the ASHRAE 2009 HOF.
+
+\paragraph{Field: Sky Clearness}\label{field-sky-clearness}
+
+If the choice in the Solar Model Indicator field is ASHRAEClearSky or ZhangHuang, then this numeric field should be entered. This value represents the ``clearness'' value for the day. This value, along with the solar position as defined by the Location information and the date entered for the design day, help define the solar radiation values for each hour of the day. Clearness may range from 0.0 to 1.2, where 1.0 represents a clear sky at sea level. Values greated than 1.0 may be used for high altitude locations. Traditionally, one uses 0.0 clearness for Winter Design Days. Note that this ``sky clearness'' does not have the same meaning as output variable ``Site Daylighting Model Sky Clearness''.
+
+IDF Examples:
+
+\begin{lstlisting}
+! Phoenix Sky Harbor Intl Ap_AZ_USA Annual Cooling (WB = >MDB)
+!   .4%, MDB = 35.8°C WB = 24.5°C
+SizingPeriod:DesignDay,
+  Phoenix Sky Harbor Intl Ap Ann Clg .4% Condns WB = >MDB, !- Name
+          7,      !- Month
+         21,      !- Day of Month
+  SummerDesignDay,!- Day Type
+       35.8,      !- Maximum Dry-Bulb Temperature {C}
+         12,      !- Daily Dry-Bulb Temperature Range {C}
+  DefaultMultipliers, !- Dry-Bulb Temperature Range Modifier Type
+           ,      !- Dry-Bulb Temperature Range Modifier Schedule Name
+    Wetbulb,      !- Humidity Condition Type
+       24.5,      !- Wetbulb at Maximum Dry-Bulb {C}
+           ,      !- Humidity Indicating Day Schedule Name
+           ,      !- Humidity Ratio at Maximum Dry-Bulb {kgWater/kgDryAir}
+           ,      !- Enthalpy at Maximum Dry-Bulb {J/kg}
+           ,      !- Daily Wet-Bulb Temperature Range {deltaC}
+     97342.,      !- Barometric Pressure {Pa}
+        4.1,      ! Wind Speed {m/s}
+        260,      !- Wind Direction {Degrees; N = 0, S = 180}
+         No,      !- Rain {Yes/No}
+         No,      !- Snow on ground {Yes/No}
+         No,      !- Daylight Savings Time Indicator
+       ASHRAETau, !- Solar Model Indicator
+           ,      !- Beam Solar Day Schedule Name
+           ,      !- Diffuse Solar Day Schedule Name
+      0.588,     !- ASHRAE Clear Sky Optical Depth for Beam Irradiance (taub)
+      1.653;  !- ASHRAE Clear Sky Optical Depth for Diffuse Irradiance (taud)
+
+SizingPeriod:DesignDay,
+  Denver Centennial Golden Ann Htg 99% Condns DB - sched solar,  !- Name
+  1,                       !- Month
+  13,                      !- Day of Month
+  WinterDesignDay,         !- Day Type
+  -16,                     !- Maximum Dry-Bulb Temperature {C}
+  0.0,                     !- Daily Dry-Bulb Temperature Range {deltaC}
+  ,                        !- Dry-Bulb Temperature Range Modifier Type
+  ,                    !- Dry-Bulb Temperature Range Modifier Schedule Name
+  Wetbulb,                 !- Humidity Condition Type
+  -16,                     !- Wetbulb or DewPoint at Maximum Dry-Bulb {C}
+  ,                        !- Humidity Indicating Day Schedule Name
+  ,               !- Humidity Ratio at Maximum Dry-Bulb {kgWater/kgDryAir}
+  ,                        !- Enthalpy at Maximum Dry-Bulb {J/kg}
+  ,                        !- Daily Wet-Bulb Temperature Range {deltaC}
+  83411.,                  !- Barometric Pressure {Pa}
+  2.3,                     !- Wind Speed {m/s}
+  180,                     !- Wind Direction {deg}
+  No,                      !- Rain Indicator
+  No,                      !- Snow Indicator
+  No,                      !- Daylight Saving Time Indicator
+  Schedule,                !- Solar Model Indicator
+  Winter (1/13) Beam Solar,!- Beam Solar Day Schedule Name
+  Winter (1/13) Diffuse Solar;  !- Diffuse Solar Day Schedule Name
+
+Schedule:Day:Hourly,
+  Winter (1/13) Beam Solar,
+  Any Number,
+  0,0,0,0,0,0,0,190,698,852,892,919,957,953,856,700,213,0,0,0,0,0,0,0;
+
+Schedule:Day:Hourly,
+  Winter (1/13) Diffuse Solar,
+  Any Number,
+  0,0,0,0,0,0,0,35,118,116,92,65,40,14,0,0,5,0,0,0,0,0,0,0;
+\end{lstlisting}
+
+Look at the example files 1Zone\-Un\-controll\-ed\_\-DD\-Changes.idf and 1Zone\-Un\-controlled\_\-DD\-2009 for several examples of specifying Design Day inputs.
+
+\subsubsection{Outputs}\label{outputs-018}
+
+For the schedule fields in the object, several output variables can be used:
+
+\begin{itemize}
+\item
+  Zone,Average,Sizing Period Site Beam Solar Schedule Value {[}W/m2{]}
+\item
+  Zone,Average,Sizing Period Site Diffuse Solar Schedule Value {[}W/m2{]}
+\item
+  Zone,Average,Sizing Period Site Humidity Condition Schedule Value {[}\%{]}
+\item
+  Zone,Average,Sizing Period Site Humidity Condition Schedule Value {[]}
+\item
+  Zone,Average,Sizing Period Site Drybulb Temperature Range Modifier Schedule Value {[]}
+\item
+  Zone,Average,Sizing Period Site Drybulb Temperature Range Modifier Schedule Value {[}deltaC{]}
+\item
+  Zone,Average,Sizing Period Site Drybulb Temperature Range Modifier Schedule Value {[}C{]}
+\item
+  Zone,Average,Sizing Period Site Sky Temperature Schedule Value {[}deltaC{]}
+\item
+  Zone,Average,Sizing Period Site Sky Temperature Schedule Value {[}C{]}
+\end{itemize}
+
+\paragraph{Sizing Period Site Beam Solar Schedule Value {[}W/m2{]}}\label{sizing-period-site-beam-solar-schedule-value-wm2}
+
+\paragraph{Sizing Period Site Diffuse Solar Schedule Value {[}W/m2{]}}\label{sizing-period-site-diffuse-solar-schedule-value-wm2}
+
+This schedule value is active when any Design Day objects have / use the solar schedule option. For those objects that don't have this option, the value will be displayed as -999.
+
+\paragraph{Sizing Period Site Humidity Condition Schedule Value {[}\%{]}}\label{sizing-period-site-humidity-condition-schedule-value}
+
+\paragraph{\texorpdfstring{Sizing Period Site Humidity Condition Schedule Value {[]}}{Sizing Period Site Humidity Condition Schedule Value }}\label{sizing-period-site-humidity-condition-schedule-value-1}
+
+This schedule value is active when any Design Day objects have / use the humidity schedule option. For those objects that don't have this option, the value will be displayed as -999.
+
+\paragraph{\texorpdfstring{Sizing Period Site Drybulb Temperature Range Modifier Schedule Value {[]}}{Sizing Period Site Drybulb Temperature Range Modifier Schedule Value }}\label{sizing-period-site-drybulb-temperature-range-modifier-schedule-value}
+
+\paragraph{Sizing Period Site Drybulb Temperature Range Modifier Schedule Value {[}deltaC{]}}\label{sizing-period-site-drybulb-temperature-range-modifier-schedule-value-deltac}
+
+\paragraph{Sizing Period Site Drybulb Temperature Range Modifier Schedule Value {[}C{]}}\label{sizing-period-site-drybulb-temperature-range-modifier-schedule-value-c}
+
+This schedule value is active when any Design Day objects have / use the drybulb temperature range modifier chedule option. For those objects that don't have this option, the value will be displayed as -999.
+
+\paragraph{Sizing Period Site Sky Temperature Schedule Value {[}deltaC{]}}\label{sizing-period-site-sky-temperature-schedule-value-deltac}
+
+\paragraph{Sizing Period Site Sky Temperature Schedule Value {[}C{]}}\label{sizing-period-site-sky-temperature-schedule-value-c}
+
+This schedule value is active when any Design Day objects have / use the WeatherProperties:SkyTemperature schedule option. For those objects that don't have this option, the value will be displayed as -999.
+
+\subsection{Longer Design Periods}\label{longer-design-periods}
+
+Some features may benefit by using a longer design weather period for sizing or loads calculations. Longer design periods may be created by using the \textbf{Si\-zing\-Period:\-Weather\-File\-Days} or \textbf{Si\-zing\-Period:\-Weather\-File\-Con\-dition\-Type} objects. These two objects allow for selections from an attached weather file to be used in the sizing calculations.
+
+\subsection{Sizing\-Period:\-Weather\-File\-Days}\label{sizingperiodweatherfiledays}
+
+The Sizing\-Period:\-Weather\-File\-Days object describes using a selected period from the ``attached'' weather file to be used in load calculations or sizing equipment. The period selected can be as small as a single day or larger. Multiple periods may be input. While this object may be used for sizing calculations, you should also consider using design days that represent more long term extremes or conditions.
+
+\subsubsection{Inputs}\label{inputs-2-022}
+
+\paragraph{Field: Name}\label{field-name-2-021}
+
+This field allows for an assigned name for this run period so it can be tracked easily in sizing and other outputs.
+
+\paragraph{Field: Begin Month}\label{field-begin-month}
+
+This numeric field should contain the starting month number (1 = January, 2 = February, etc.) for the annual run period desired.
+
+\paragraph{Field: Begin Day of Month}\label{field-begin-day-of-month}
+
+This numeric field should contain the starting day of the starting month (must be valid for month) for the annual run period desired.
+
+\paragraph{Field: End Month}\label{field-end-month}
+
+This numeric field should contain the ending month number (1 = January, 2 = February, etc.) for the annual run period desired.
+
+\paragraph{Field: End Day of Month}\label{field-end-day-of-month}
+
+This numeric field should contain the ending day of the ending month (must be valid for month) for the annual run period desired.
+
+\paragraph{Field: Day of Week for Start Day}\label{field-day-of-week-for-start-day}
+
+For flexibility, the day of week indicated on the weather file can be overridden by this field's value. Valid days of the week (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday) or special days (SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2) must be entered in this field. To clarify, this value will be used as the Start Day (type) for this sizing period. When weekdays are used, each subsequent day in the period will be incremented. When SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2 -- are used, the day type will be applied for the entire period.
+
+\paragraph{Field: Use Weather File Daylight Saving Period}\label{field-use-weather-file-daylight-saving-period}
+
+Weather files can contain indicators of Daylight Saving Period days. For flexibility, you may want to ignore these designations on the weather file. This field should contain the word \textbf{Yes} if you will accept daylight saving period days as contained on the weather file (note: not all weather files may actually have this period) or \textbf{No} if you wish to ignore Daylight Saving Period days that may be on the weather file.
+
+Note that a blank or null field in this field will indicate \textbf{Yes}.
+
+\paragraph{Field: Use Weather File Rain and Snow Indicators}\label{field-use-weather-file-rain-and-snow-indicators}
+
+Weather files can contain ``rain'' and ``snow'' indicators. (EPW field ``Present Weather Codes'' -- described in the AuxiliaryPrograms document). In turn, rain indicates wet surfaces which changes the film convection coefficient for the surface. Other models may use rain as well (Ground Heat Exchangers). Snow indicators can change the ground reflectance if there is snow on the ground. Entering ``\textbf{Yes}'' in this field allows the weather file conditions to represent ``Rain'' and ``Snow''; entering ``\textbf{No}'' in the field ``turns off'' the rain/snow indicators for this period. You might use this to be able to compare two ``same location'' weather files of different years, origins, etc.
+
+IDF Example:
+
+\begin{lstlisting}
+SizingPeriod:WeatherFileDays,
+  Summer including Extreme Summer days, !- Name
+  7,18,7,25,                            !- Begin/end Day/Month
+  SummerDesignDay,                      !- Day type
+  No,                                   !- Use Weather File Daylight Saving Period
+  No;                                   !- Use Weather File Rain and Snow Indicators
+
+SizingPeriod:WeatherFileDays,
+  Winter including Extreme Winter days, !- Name
+  1,25,2,1,                             !- Begin/end Day/Month
+  WinterDesignDay,                      !- Day type
+  No,                                   !- Use Weather File Daylight Saving Period
+  No;                                   !- Use Weather File Rain and Snow Indicators
+\end{lstlisting}
+
+\subsection{Sizing\-Period:\-Weather\-File\-Con\-dition\-Type}\label{sizingperiodweatherfileconditiontype}
+
+When the EPW files are created, a heuristic procedure identifies extreme and typical periods in the actual weather file. This object will allow one of those periods to be selected for sizing or load calculations (typically). Multiple objects may be input. While this object may be used for sizing calculations, you should also consider using design days that represent more long term extremes or conditions.
+
+\subsubsection{Inputs}\label{inputs-3-020}
+
+\paragraph{Field: Name}\label{field-name-3-018}
+
+This field allows for an assigned name for this run period so it can be tracked easily in sizing and other outputs.
+
+\paragraph{Field: Period Selection}\label{field-period-selection}
+
+This field allows the generic period calculated from the weather file to be selected for this run period. It is not completely generic as there may be extreme cold periods in some weather files but extreme wet periods (tropical) in others. Not all weather files have all of the valid choices. The choices for this field are:
+
+\begin{itemize}
+\item
+  SummerExtreme
+\item
+  SummerTypical
+\item
+  WinterExtreme
+\item
+  WinterTypical
+\item
+  AutumnTypical
+\item
+  SpringTypical
+\item
+  WetSeason
+\item
+  DrySeason
+\item
+  NoDrySeason
+\item
+  NoWetSeason
+\item
+  TropicalHot
+\item
+  TropicalCold
+\end{itemize}
+
+\paragraph{Field: Day of Week for Start Day}\label{field-day-of-week-for-start-day-1}
+
+For flexibility, the day of week indicated on the weather file can be overridden by this field's value. Valid days of the week (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday) or special days (SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2) must be entered in this field. To clarify, this value will be used as the Start Day (type) for this sizing period. When weekdays are used, each subsequent day in the period will be incremented. When SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2 -- are used, the day type will be applied for the entire period.
+
+\paragraph{Field: Use Weather File Daylight Saving Period}\label{field-use-weather-file-daylight-saving-period-1}
+
+Weather files can contain indicators of Daylight Saving Period days. For flexibility, you may want to ignore these designations on the weather file. This field should contain the word \textbf{Yes} if you will accept daylight saving period days as contained on the weather file (note: not all weather files may actually have this period) or \textbf{No} if you wish to ignore Daylight Saving Period days that may be on the weather file.
+
+Note that a blank or null field in this field will indicate \textbf{Yes}.
+
+\paragraph{Field: Use Weather File Rain and Snow Indicators}\label{field-use-weather-file-rain-and-snow-indicators-1}
+
+Weather files can contain ``rain'' and ``snow'' indicators. (EPW field ``Present Weather Codes'' -- described in the AuxiliaryPrograms document). In turn, rain indicates wet surfaces which changes the film convection coefficient for the surface. Other models may use rain as well (Ground Heat Exchangers). Snow indicators can change the ground reflectance if there is snow on the ground. Entering ``\textbf{Yes}'' in this field allows the weather file conditions to represent ``Rain'' and ``Snow''; entering ``\textbf{No}'' in the field ``turns off'' the rain/snow indicators for this period. You might use this to be able to compare two ``same location'' weather files of different years, origins, etc.
+
+IDF Example:
+
+\begin{lstlisting}
+SizingPeriod:WeatherFileConditionType,
+  Extreme Summer Weather Period for Design, !- Name
+  SummerExtreme,                            !- Period Selection
+  SummerDesignDay,                          !- Day Type
+  No,                                       !- Use Weather File Daylight Saving Period
+  No;                                       !- Use Weather File Rain and Snow Indicators
+
+SizingPeriod:WeatherFileConditionType,
+  Extreme Winter Weather Period for Design, !- Name
+  WinterExtreme,                            !- Period Selection
+  WinterDesignDay,                          !- Day Type
+  No,                                       !- Use Weather File Daylight Saving Period
+  No;                                       !- Use Weather File Rain and Snow Indicators
+\end{lstlisting}
+
+\subsection{RunPeriod}\label{runperiod}
+
+The RunPeriod object describes the elements necessary to create a weather file simulation. Multiple run periods may be input. EnergyPlus accepts weather files in the special EnergyPlus weather format (described briefly below this document and in more detail in the Auxiliary Programs document). These files can describe Daylight Saving Time periods as well as holidays within their definitions. The RunPeriod object allows the user to override the use of both the Daylight Saving Period (i.e. use or ignore) and holidays that are embedded within the weather file. Note that the weather file also may contain design condition information, typical and extreme period information, ground temperatures based on air temperature calculations.
+
+\subsubsection{Inputs}\label{inputs-4-018}
+
+\paragraph{Field: Name}\label{field-name-4-015}
+
+This optional field allows the RunPeriod to be named for output reporting. When left blank, the weather file location name is used. Note that the weather file location name will be appened to this name in tabular/summary reports.
+
+\paragraph{Field: Begin Month}\label{field-begin-month-1}
+
+This numeric field should contain the starting month number (1 = January, 2 = February, etc.) for the annual run period desired.
+
+\paragraph{Field: Begin Day of Month}\label{field-begin-day-of-month-1}
+
+This numeric field should contain the starting day of the starting month (must be valid for month) for the annual run period desired.
+
+\paragraph{Field: End Month}\label{field-end-month-1}
+
+This numeric field should contain the ending month number (1 = January, 2 = February, etc.) for the annual run period desired.
+
+\paragraph{Field: End Day of Month}\label{field-end-day-of-month-1}
+
+This numeric field should contain the ending day of the ending month (must be valid for month) for the annual run period desired.
+
+\paragraph{Field: Day of Week for Start Day}\label{field-day-of-week-for-start-day-2}
+
+For flexibility, the day of week indicated on the weather file can be overridden by this field's value. Valid days of the week (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday) must be entered in this field. To clarify, this value will be used as the Start Day (type) for this run period and subsequent days will be implemented. If a blank or UseWeatherFile is entered here, then the starting day type will be calculated from the weather file (ref: Auxiliary Programs document about Data Periods).
+
+\paragraph{Field: Use Weather File Holidays and Special Days}\label{field-use-weather-file-holidays-and-special-days}
+
+Weather files can contain holiday designations or other kinds of special days. These day types cause a corresponding day's schedule (see SCHEDULE definitions below) to be used during that day. This field should contain the word \textbf{Yes} if holidays or other special days indicated directly on the weather file should retain their ``day type'' or \textbf{No} if holidays or other special days on the weather file should be ignored. Reference the RunPeriodControl:SpecialDays object below to enter your own special days and holidays.
+
+Note that a blank or null field in this field will indicate \textbf{Yes}.
+
+\paragraph{Field: Use Weather File Daylight Saving Period}\label{field-use-weather-file-daylight-saving-period-2}
+
+Weather files can contain indicators of Daylight Saving period days. For flexibility, you may want to ignore these designations on the weather file. This field should contain the word \textbf{Yes} if you will accept daylight saving period days as contained on the weather file (note: not all weather files may actually have this period) or \textbf{No} if you wish to ignore Daylight Saving period days that may be on the weather file.
+
+Note that a blank or null field in this field will indicate \textbf{Yes}.
+
+\paragraph{Field: Apply Weekend Holiday Rule}\label{field-apply-weekend-holiday-rule}
+
+In some countries (notably the US), when holidays fall on weekends, they are often observed on a weekday close to the holiday day. (Usually if the specific day falls on a Saturday, the observed day is Friday; if on a Sunday, the observed day is Monday). EnergyPlus will represent this custom using the value in this field. If the field is \textbf{Yes}, then specific date holidays that have a duration of one day, will be ``observed'' on the Monday after the day. (Specific day holidays are such as January 1 -- a day-month combination). If the field is blank or \textbf{No}, then the holiday will be shown on the day-month as entered. As this option is listed at the RunPeriod, all applicable special days for the run will use the rule -- there is no override for individual special days.
+
+Note that a blank or null field in this field will indicate \textbf{No}.
+
+\begin{callout}
+Note: EnergyPlus processed weather files available on the EnergyPlus web site: \url{http://www.energyplus.gov/cfm/weather\_data.cfm} have neither special days specified nor daylight saving period. However, DDY (Design Day) files produced from the ASHRAE Design Conditions that accompany the EPW files may include a DaylightSavingPeriod object for certain locations.
+\end{callout}
+
+\paragraph{Field: Use Weather File Rain Indicators}\label{field-use-weather-file-rain-indicators}
+
+Weather files can contain ``rain'' indicators. (EPW field ``Present Weather Codes'' -- described in the AuxiliaryPrograms document). In turn, rain indicates wet surfaces which changes the film convection coefficient for the surface. Other models may use rain as well (Ground Heat Exchangers). Entering ``\textbf{Yes}'' in this field allows the weather file conditions to represent ``Rain''; entering ``\textbf{No}'' in the field ``turns off'' the rain indicator for this period. You might use this to be able to compare two ``same location'' weather files of different years, origins, etc.
+
+\paragraph{Field: Use Weather File Snow Indicators}\label{field-use-weather-file-snow-indicators}
+
+Weather files can contain ``snow'' indicators. (EPW field ``Snow Depth'' \textgreater{} 0 indicates ``Snow on the ground''). In turn, snow changes the reflectivity of the ground and cascades changes of this reflectivity. Entering ``\textbf{Yes}'' in this field allows the weather file conditions to represent ``Snow''; entering ``\textbf{No}'' in the field ``turns off'' the snow indicator for this period. You might use this to be able to compare two ``same location'' weather files of different years, origins, etc.
+
+\paragraph{Field: Number of Times Runperiod to be Repeated}\label{field-number-of-times-runperiod-to-be-repeated}
+
+This numeric field represents the number of times (usually years) the simulation has to be carried out in a multi runperiod simulation. The default value is set to 1. The number of years of simulation, in case of a Ground Loop Heat Exchanger (GLHE) simulation, should be equal to the length of simulation field in GLHE object. Note that you can specify a number of simulation years with a shorter run period (e.g. 1 week) and EnergyPlus will repeat the simulation of the shorter run period for that many times. Note that repeating will work with any weather file that contains the start date and end date in a ``Data Period'' (refer to Auxiliary Programs document for more documentation on weather file contents).
+
+\paragraph{Field: Increment Day of Week on Repeat}\label{field-increment-day-of-week-on-repeat}
+
+When repeating RunPeriods (see previous field), you can choose to increment the day of week at the end of the period to have a more continuous day type. Enter \textbf{Yes} to increment the day of the week (default). An entry of \textbf{No} will keep the same day of week values as in the first time through.
+
+\paragraph{Field: Start Year}\label{field-start-year}
+
+When repeating a period, you might (for whatever reason), choose to have a specific year as a starting year. Enter an appropriate 4 digit year in this field. Refer to Auxiliary Programs document for more documentation on weather file contents, particularly in using leap year data (or not) within weather files.
+
+And, as shown in an IDF:
+
+\begin{lstlisting}
+RunPeriod,  ! Winter Simulation
+  Winter Simulation,  !- Name
+  12,  !- Begin Month
+  1,  !- Begin Day of Month
+  3,  !- End Month
+  31,  !- End Day of Month
+  UseWeatherFile,  !- Day of Week for Start Day
+  Yes,  !- Use Weather File Holidays and Special Days
+  Yes,  !- Use Weather File Daylight Saving Period
+  No,  !- Apply Weekend Holiday Rule
+  Yes,  !- Use Weather File Rain Indicators
+  Yes;  !- Use Weather File Snow Indicators
+
+! Multiple year simulation example
+RunPeriod,
+  Multiple Years,  !- Name
+  1,    !- Begin Month
+  1,    !- Begin Day of Month
+  12,   !- End Month
+  31,   !- End Day of Month
+  UseWeatherFile,  !- Day of Week for Start Day
+  Yes,  !- Use Weather File Holidays and Special Days
+  Yes,  !- Use Weather File Daylight Saving Period
+  No,   !- Apply Weekend Holiday Rule
+  Yes,  !- Use Weather File Rain Indicators
+  Yes,  !- Use Weather File Snow Indicators
+  3;    !- Number of Times Runperiod to be Repeated
+\end{lstlisting}
+
+\subsection{RunPeriod:CustomRange}\label{runperiodcustomrange}
+
+The RunPeriod:CustomRange object describes the elements necessary to use a specially crafted (likely multiple year) weather file in a simulation. These kinds of weather files and simulations might be useful for matching utility periods or simulating several years of differing weather data. Multiple run periods may be input. EnergyPlus accepts weather files in the special EnergyPlus weather format (described briefly below this document and in more detail in the Auxiliary Programs document). In order to effectively use this object, however, you will need to use a text editor (EnergyPlus weather files area simple text files) or possibly a spreadsheet program and then save to a csv (comma separated variable) file. Weather files can describe Daylight Saving Time periods as well as holidays within their definitions. The RunPeriod:CustomRange object allows the user to override the use of both the Daylight Saving Period (i.e. use or ignore) and holidays that are embedded within the weather file. Note that the weather file also may contain design condition information, typical and extreme period information, ground temperatures based on air temperature calculations.
+
+\subsubsection{Inputs}\label{inputs-5-016}
+
+\paragraph{Field: Name}\label{field-name-5-012}
+
+This optional field allows the RunPeriod to be named for output reporting. When left blank, the weather file location name is used. Note that the weather file location name will be appened to this name in tabular/summary reports.
+
+\paragraph{Field: Begin Month}\label{field-begin-month-2}
+
+This numeric field should contain the starting month number (1 = January, 2 = February, etc.) for the annual run period desired.
+
+\paragraph{Field: Begin Day of Month}\label{field-begin-day-of-month-2}
+
+This numeric field should contain the starting day of the starting month (must be valid for month) for the annual run period desired.
+
+\paragraph{Field: Begin Year}\label{field-begin-year}
+
+This numeric field should contain the beginning year for the custom range. Though all EnergyPlus (EPW) weather files contain a year/year field, the RunPeriod object does not use this field (previous object). The \textbf{RunPeriod:CustomRange} object causes the program to look specifically for the begin date specified by these three fields (i.e. Begin Month, Begin Day of Month, Begin Year).
+
+\paragraph{Field: End Month}\label{field-end-month-2}
+
+This numeric field should contain the ending month number (1 = January, 2 = February, etc.) for the annual run period desired.
+
+\paragraph{Field: End Day of Month}\label{field-end-day-of-month-2}
+
+This numeric field should contain the ending day of the ending month (must be valid for month) for the annual run period desired.
+
+\paragraph{Field: End Year}\label{field-end-year}
+
+This numeric field should contain the end year for the custom range. Though all EnergyPlus (EPW) weather files contain a year/year field, the RunPeriod object does not use this field (previous object). The \textbf{RunPeriod:CustomRange} object causes the program to look specifically for the end date specified by these three fields (i.e. End Month, End Day of Month, End Year).
+
+\paragraph{Field: Day of Week for Start Day}\label{field-day-of-week-for-start-day-3}
+
+For flexibility, the day of week indicated on the weather file can be overridden by this field's value. Valid days of the week (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday) must be entered in this field. To clarify, this value will be used as the Start Day (type) for this run period and subsequent days will be implemented. If a blank or UseWeatherFile is entered here, then the starting day type will be calculated from the weather file (ref: Auxiliary Programs document about Data Periods).
+
+\paragraph{Field: Use Weather File Holidays and Special Days}\label{field-use-weather-file-holidays-and-special-days-1}
+
+Weather files can contain holiday designations or other kinds of special days. These day types cause a corresponding day's schedule (see SCHEDULE definitions below) to be used during that day. This field should contain the word \textbf{Yes} if holidays or other special days indicated directly on the weather file should retain their ``day type'' or \textbf{No} if holidays or other special days on the weather file should be ignored. Reference the RunPeriodControl:SpecialDays object below to enter your own special days and holidays.
+
+Note that a blank or null field in this field will indicate \textbf{Yes}.
+
+\paragraph{Field: Use Weather File Daylight Saving Period}\label{field-use-weather-file-daylight-saving-period-3}
+
+Weather files can contain indicators of Daylight Saving period days. For flexibility, you may want to ignore these designations on the weather file. This field should contain the word \textbf{Yes} if you will accept daylight saving period days as contained on the weather file (note: not all weather files may actually have this period) or \textbf{No} if you wish to ignore Daylight Saving period days that may be on the weather file.
+
+Note that a blank or null field in this field will indicate \textbf{Yes}.
+
+\paragraph{Field: Apply Weekend Holiday Rule}\label{field-apply-weekend-holiday-rule-1}
+
+In some countries (notably the US), when holidays fall on weekends, they are often observed on a weekday close to the holiday day. (Usually if the specific day falls on a Saturday, the observed day is Friday; if on a Sunday, the observed day is Monday). EnergyPlus will represent this custom using the value in this field. If the field is \textbf{Yes}, then specific date holidays that have a duration of one day, will be ``observed'' on the Monday after the day. (Specific day holidays are such as January 1 -- a day-month combination). If the field is blank or \textbf{No}, then the holiday will be shown on the day-month as entered. As this option is listed at the RunPeriod, all applicable special days for the run will use the rule -- there is no override for individual special days.
+
+Note that a blank or null field in this field will indicate \textbf{No}.
+
+\begin{callout}
+Note: EnergyPlus processed weather files available on the EnergyPlus web site: \url{http://www.energyplus.gov/cfm/weather\_data.cfm} have neither special days specified nor daylight saving period. However, DDY (Design Day) files produced from the ASHRAE Design Conditions that accompany the EPW files may include a DaylightSavingPeriod object for certain locations.
+\end{callout}
+
+\paragraph{Field: Use Weather File Rain Indicators}\label{field-use-weather-file-rain-indicators-1}
+
+Weather files can contain ``rain'' indicators. (EPW field ``Present Weather Codes'' -- described in the AuxiliaryPrograms document). In turn, rain indicates wet surfaces which changes the film convection coefficient for the surface. Other models may use rain as well (Ground Heat Exchangers). Entering ``\textbf{Yes}'' in this field allows the weather file conditions to represent ``Rain''; entering ``\textbf{No}'' in the field ``turns off'' the rain indicator for this period. You might use this to be able to compare two ``same location'' weather files of different years, origins, etc.
+
+\paragraph{Field: Use Weather File Snow Indicators}\label{field-use-weather-file-snow-indicators-1}
+
+Weather files can contain ``snow'' indicators. (EPW field ``Snow Depth'' \textgreater{} 0 indicates ``Snow on the ground''). In turn, snow changes the reflectivity of the ground and cascades changes of this reflectivity. Entering ``\textbf{Yes}'' in this field allows the weather file conditions to represent ``Snow''; entering ``\textbf{No}'' in the field ``turns off'' the snow indicator for this period. You might use this to be able to compare two ``same location'' weather files of different years, origins, etc.
+
+\subsection{RunPeriodControl:SpecialDays}\label{runperiodcontrolspecialdays}
+
+For weather file run periods, special day run periods can be described. These will always be in effect for the selected days in the run period. Depending on the Use Special Days value in the RunPeriod:* object(s), these can augment any special days included on the weather file.
+
+\begin{callout}
+Note: EnergyPlus processed weather files available on the EnergyPlus web site: \url{http://www.energyplus.gov/cfm/weather\_data.cfm} have neither special days specified nor daylight saving period. However, DDY (Design Day) files produced from the ASHRAE Design Conditions that accompany the EPW files may include a DaylightSavingPeriod object for certain locations.
+\end{callout}
+
+\subsubsection{Inputs}\label{inputs-6-013}
+
+\paragraph{Field: Name}\label{field-name-6-010}
+
+This alpha field is the title for the special day period. It must be unique among all the special day period objects entered.
+
+\paragraph{Field: Start Date}\label{field-start-date}
+
+This field is the starting date for the special day period. Dates in this field can be entered in several ways as shown in the accompanying table:
+
+% table 3
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Date Field Interpretation \label{table:date-field-interpretation}} \tabularnewline
+\toprule 
+Field Contents & Interpretation \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Date Field Interpretation} \tabularnewline
+\toprule 
+Field Contents & Interpretation \tabularnewline
+\midrule
+\endhead
+
+< number >  /  < number > & Month / Day \tabularnewline
+< number >  Month & Day and Month \tabularnewline
+Month  < number > & Day and Month \tabularnewline
+< number >  Weekday in Month & Numbered weekday of month \tabularnewline
+Last Weekday In Month & Last weekday of month \tabularnewline
+\bottomrule
+\end{longtable}
+
+In the table, Month can be one of (January, February, March, April, May, June, July, August, September, October, November, December). Abbreviations of the first three characters are also valid.
+
+In the table, Weekday can be one of (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday). Abbreviations of the first three characters are also valid.
+
+\paragraph{Field: Duration}\label{field-duration}
+
+This numeric field specifies how long (number of days) the special day period lasts.
+
+\paragraph{Field: Special Day Type}\label{field-special-day-type}
+
+This alpha field designates the ``day type'' for schedule use during the special period. It must be one of (Holiday, SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2).
+
+An example in the IDF would be:
+
+\begin{lstlisting}
+RunPeriodControl:SpecialDays, President’s Day, 3rd Monday in February,1,Holiday;
+RunPeriodControl:SpecialDays, Thanksgiving, 4th Thursday in November, 1,Holiday;
+RunPeriodControl:SpecialDays, Halloween, 10/31, 1, Holiday;
+RunPeriodControl:SpecialDays, Vacation, 5/1, 14, CustomDay1;
+\end{lstlisting}
+
+\subsection{RunPeriodControl:DaylightSavingTime}\label{runperiodcontroldaylightsavingtime}
+
+Similar to a special day period, a daylight saving period may be entered to be applied to weather file run periods. These will always be in effect, regardless of the value entered on the RunPeriod object. Note that this period will always override any daylight saving period specified in a weather file.
+
+\begin{callout}
+Note: EnergyPlus processed weather files available on the EnergyPlus web site: \url{http://www.energyplus.gov/cfm/weather\_data.cfm} have neither special days specified nor daylight saving period.
+
+\warning{Note: For EnergyPlus Output:Variable and Output:Meter reporting, the time stamps are always in standard time. When daylight saving time is active, scheduled loads and controls will shift one hour relative to standard time.}
+\end{callout}
+
+\subsubsection{Inputs}\label{inputs-7-013}
+
+\paragraph{Field: Start Date}\label{field-start-date-1}
+
+This is the starting date of the daylight saving period. Note that it can be entered in several formats as shown in Table~\ref{table:date-field-interpretation}. Date Field Interpretation.
+
+\paragraph{Field: End Date}\label{field-end-date}
+
+This is the ending date of the daylight saving period. Note that it can be entered in several formats as shown in Table~\ref{table:date-field-interpretation}. Date Field Interpretation.
+
+And in the IDF:
+
+\begin{lstlisting}
+! U.S. Standard for Daylight Saving
+RunPeriodControl:DaylightSavingTime,2nd Sunday in March, 1st Sunday in November; !2007
+! Brazil standard
+RunPeriodControl:DaylightSavingTime,1st Sunday in October, Last Sunday in February;
+! European Standard
+RunPeriodControl:DaylightSavingTime, Last Sunday in March, Last Sunday in October;
+! Syria Standard
+RunPeriodControl:DaylightSavingTime, 4/1, 10/1;
+\end{lstlisting}
+
+Of course, these could not all appear in the same IDF as only one DaylightSavingPeriod object per input file is allowed. More information on Daylight Saving Periods can be seen on the web at: \url{http://www.webexhibits.org/daylightsaving/}. The ASHRAE Handbook of Fundamentals {[}ASHRAE 2005{]} also contains information about daylight saving periods and their climatic information now includes start and end dates for many locations.
+
+\subsection{WeatherProperty:SkyTemperature}\label{weatherpropertyskytemperature}
+
+Sky Temperature, or radiative sky temperature, is internally calculated by EnergyPlus using an algorithm using horizontal infrared radiation from sky, cloudiness factors and current temperaure. The algorithm is fully described in the Engineering Reference document. For flexibility, the following object can be entered to override the internal calculations. Much of the literature describes the sky temperature as relative to either drybulb or dewpoint temperature.
+
+\subsubsection{Inputs}\label{inputs-8-011}
+
+\paragraph{Field: Name}\label{field-name-7-009}
+
+This name references an existing design period (i.e., SizingPeriod:DesignDay, SizingPeriod:WeatherFileDays, or SizingPeriod:WeatherFileConditionType) or run period (by name or blank for all run periods).
+
+\paragraph{Field: Calculation Type}\label{field-calculation-type}
+
+Allowable entries here are: \textbf{ScheduleValue}, \textbf{DifferenceScheduleDryBulbValue}, or \textbf{DifferenceScheduleDewPointValue}. In each case the following field must specify a valid schedule name. \textbf{ScheduleValue} -- the values in the schedule are used as the sky temperature. \textbf{DifferenceScheduleDryBulbValue} -- the values in the schedule are used as a difference to the drybulb temperature value (+values would then be greater than the drybulb temperature, -values would then be less than the drybulb temperature) for the resulting sky temperature value. \textbf{DifferenceScheduleDewPointValue} -- the values in the schedule are used as a difference to the dewpoint temperature value (+values would then be greater than the dewpoint temperature, -values would then be less than the dewpoint temperature) for the resulting sky temperature value.
+
+\paragraph{Field: ScheduleName}\label{field-schedulename}
+
+This field specifies a schedule name to accomplish the sky temperature calculation from the previous field. A Schedule:Day:* (i.e., Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List) should be specified if the name in the name field matches a SizingPeriod:DesignDay object. If the name is one of the weather file period specifications (i.e. matches a SizingPeriod:WeatherFileDays, SizingPeriod:WeatherFileConditionType or RunPeriod), then the schedule name must match a full year schedule (i.e. Schedule:Year, Schedule:Compact, Schedule:File, or Schedule:Constant).
+
+An example of IDF usage (with DesignDay):
+
+\begin{lstlisting}
+SizingPeriod:DesignDay,
+  DENVER_STAPLETON Ann Clg 1% Sky Temperature modfier,  !- Name
+  32.6,              !- Maximum Dry-Bulb Temperature {C}
+  15.2,              !- Daily Temperature Range {deltaC}
+  15.5,              !- Humidity Indicating Conditions at Maximum Dry-Bulb
+  83411.,            !- Barometric Pressure {Pa}
+  4,                 !- Wind Speed {m/s}
+  120,               !- Wind Direction {deg}
+  1.00,              !- Sky Clearness
+  0,                 !- Rain Indicator
+  0,                 !- Snow Indicator
+  25,                !- Day of Month
+  7,                 !- Month
+  SummerDesignDay,   !- Day Type
+  0,                 !- Daylight Saving Time Indicator
+  WetBulb,           !- Humidity Indicating Type
+  ,                  !- Relative Humidity Day Schedule Name
+  deltaschedule,     !- Dry-Bulb Temperature Range Modifier Type
+  temp range deltas; !- Dry-Bulb Temperature Range Modifier Schedule Name
+
+WeatherProperty:SkyTemperature,
+  DENVER_STAPLETON Ann Clg 1% Sky Temperature modfier, !- Name
+  ScheduleValue,     !- Calculation Type
+  DaySchedule5;      !- Schedule Name
+
+Schedule:Day:Interval,
+  DaySchedule5,      !- Name
+  Temperature,       !- Schedule Type Limits Name
+  Yes,               !- Interpolate to Timestep
+  until: 24:00,      !- Time 1
+  5;                 !- Value Until Time 1
+\end{lstlisting}
+
+\subsection{Site:WeatherStation}\label{siteweatherstation}
+
+The Site:WeatherStation object is used to specify the measurement conditions for the climatic data listed in the weather file. These conditions indicate the height above ground of the air temperature sensor, the height above ground of the wind speed sensor, as well as coefficients that describe the wind speed profile due to the terrain surrounding the weather station. There are necessary correlations between the entries for this object and some entries in the Building object, specifically the \textbf{Terrain} field.
+
+Weather stations throughout the world (ref: WMO -- World Meteorological Organization) take their measurements at standard conditions:
+
+\begin{itemize}
+\item
+  Air temperature is measured at approximately 1.5 m above ground
+\item
+  Wind speed is measured at 10 m above ground
+\item
+  Weather station is in a flat, open field with little protection from the wind.
+\end{itemize}
+
+When using weather data from standard sources (e.g., TMY2, IWEC, TMY, or ASHRAE design day data), it is not necessary to use the \textbf{Site:WeatherStation} object. However, if you are using custom weather data or real-time weather data, you may need to read and understand the concepts in the \textbf{Site:WeatherStation} object.
+
+The measurement conditions at the weather station (i.e., the weather file) are used by EnergyPlus in conjunction with the \emph{Terrain} field of the \textbf{Building} object, or optionally with the \textbf{Site:HeightVariation} object (see below), to calculate the local variation in atmospheric properties as a function of height above ground. Outdoor air temperature decreases with height, while wind speed increases with height. The algorithms for this calculation are in the Engineering Reference.
+
+The \textbf{Site:WeatherStation} object is useful when working with a custom weather file that includes data that were not measured at the WMO standard conditions. For example, the weather data could be measured on site, or on the roof top of a nearby building. The wind speed profile coefficients can be estimated from the table below or calculated beforehand using more sophisticated techniques such as CFD modeling of the weather station terrain.
+
+% table 4
+\begin{longtable}[c]{@{}lll@{}}
+\caption{Wind Speed Profile Coefficients (ASHRAE Fundamentals 2005). \label{table:wind-speed-profile-coefficients-ashrae}} \tabularnewline
+\toprule 
+Terrain Description & Exponent & Bounhary Layer Thickness (m) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Wind Speed Profile Coefficients (ASHRAE Fundamentals 2005).} \tabularnewline
+\toprule 
+Terrain Description & Exponent & Bounhary Layer Thickness (m) \tabularnewline
+\midrule
+\endhead
+
+Flat, open country & 0.14 & 270 \tabularnewline
+Rough, wooded country & 0.22 & 370 \tabularnewline
+Towns and cities & 0.33 & 460 \tabularnewline
+Ocean & 0.10 & 210 \tabularnewline
+Urban, industrial, forest & 0.22 & 370 \tabularnewline
+\bottomrule
+\end{longtable}
+
+If the \textbf{Site:WeatherStation} object is omitted from the input file, the WMO standard measurement conditions are assumed.
+
+\subsubsection{Inputs}\label{inputs-9-010}
+
+\paragraph{Field: Wind Sensor Height Above Ground}\label{field-wind-sensor-height-above-ground}
+
+The height {[}m{]} above ground for the wind speed sensor.
+
+\paragraph{Field: Wind Speed Profile Exponent}\label{field-wind-speed-profile-exponent}
+
+The wind speed profile exponent for the terrain surrounding the weather station. The exponent can be estimated from the table above or calculated beforehand using more sophisticated techniques, such as CFD modeling of the weather station terrain.
+
+\paragraph{Field: Wind Speed Profile Boundary Layer Thickness}\label{field-wind-speed-profile-boundary-layer-thickness}
+
+The wind speed profile boundary layer thickness {[}m{]} for the terrain surrounding the weather station. The boundary layer can be estimated from the table above or calculated beforehand using more sophisticated techniques, such as CFD modeling of the weather station terrain.
+
+\paragraph{Field: Air Temperature Sensor Height Above Ground}\label{field-air-temperature-sensor-height-above-ground}
+
+The height {[}m{]} above ground for the air temperature sensor.
+
+For example, if you are using weather data measured on the top of your building, you should set the \emph{Wind Sensor Height Above Ground} and the \emph{Air Temperature Sensor Height Above Ground} to equal the height of your building (say 30 m). The \emph{Wind Speed Profile Exponent} and \emph{Wind Speed Profile Boundary Layer Thickness} should be set to match the values associated with the \emph{Terrain} field of the \textbf{Building} object, or the equivalent fields of the \textbf{Site:HeightVariation} object.
+
+Or, in IDF terms, with a building in a town or city:
+
+\begin{lstlisting}
+Site:WeatherStation,
+  30,    !- Wind Sensor Height Above Ground {m}
+  0.33,  !- Wind Speed Profile Exponent {}
+  460,   !- Wind Speed Profile Boundary Layer Thickness {m}
+  30;    !- Air Temperature Sensor Height Above Ground {m}
+\end{lstlisting}
+
+This would change if you had a different wind speed profile exponent or wind speed profile boundary layer thickness at your site.
+
+\subsection{Site:HeightVariation}\label{siteheightvariation}
+
+The Site:HeightVariation object is used to specify the local variation in atmospheric properties at the site and should be used only if you require advanced control over the height-dependent variations for wind speed and temperature. The coefficients set by this object are used by EnergyPlus, in conjunction with the Site:WeatherStation object (see above), to calculate the local variation in atmospheric properties as a function of height above ground. Outdoor air temperature decreases with height, while wind speed increases with height. The local outdoor air temperature and wind speed are calculated separately for all zones and surfaces, and optionally for outdoor air nodes for which a height has been specified (see OutdoorAir:Node object). With the default inputs, wind speed falls significantly at heights lower than the weather station measurement height, and temperature increases slightly. The algorithms for this calculation are in the Engineering Reference. There are necessary correlations between the entries for this object and some entries in the Building object, specifically the \textbf{Terrain} field.
+
+% table 5
+\begin{longtable}[c]{@{}lllll@{}}
+\caption{Atmospheric Variables at Two Different Heights Above Ground Level. \label{table:atmospheric-variables-at-two-different}} \tabularnewline
+\toprule 
+Variable & 1.5 m & 284 m & Absolute Diff & Percent Diff \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Atmospheric Variables at Two Different Heights Above Ground Level.} \tabularnewline
+\toprule 
+Variable & 1.5 m & 284 m & Absolute Diff & Percent Diff \tabularnewline
+\midrule
+\endhead
+
+Air Temperature & 15°C & 13.15°C & 1.85°C & 12.3\% \tabularnewline
+Barometric Pressure & 101,325 Pa & 97,960 Pa & 3,365 Pa & 3.3\% \tabularnewline
+Wind Speed & 2.46 m/s & 7.75 m/s & 5.29 m/s & 215\% \tabularnewline
+\bottomrule
+\end{longtable}
+
+Note that using this object overrides the wind speed profile coefficients implied by the \emph{Terrain} field of the \textbf{Building} object even if the wind speed profile fields are left blank. The wind speed profile coefficients can be estimated from the table above (see \textbf{Site:WeatherStation}) or calculated beforehand using more sophisticated techniques such as CFD modeling of the site terrain.
+
+\subsubsection{Inputs}\label{inputs-10-009}
+
+\paragraph{Field: Wind Speed Profile Exponent}\label{field-wind-speed-profile-exponent-1}
+
+The wind speed profile exponent for the terrain surrounding the site. The exponent can be estimated from the table above (see \textbf{Site:WeatherStation}) or calculated beforehand using more sophisticated techniques, such as CFD modeling of the site terrain. Note that using this object overrides the wind speed profile coefficients implied by the \emph{Terrain} field of the \textbf{Building} object even if this field is left blank. This field can be set to zero to turn off all wind dependence on height.
+
+\paragraph{Field: Wind Speed Profile Boundary Layer Thickness}\label{field-wind-speed-profile-boundary-layer-thickness-1}
+
+The wind speed profile boundary layer thickness {[}m{]} for the terrain surrounding the site. The boundary layer can be estimated from the table above (see \textbf{Site:WeatherStation}) or calculated beforehand using more sophisticated techniques, such as CFD modeling of the site terrain. Note that using this object overrides the wind speed profile coefficients implied by the \emph{Terrain} field of the \textbf{Building} object even if this field is left blank.
+
+\paragraph{Field: Air Temperature Gradient Coefficient}\label{field-air-temperature-gradient-coefficient}
+
+The air temperature gradient coefficient {[}K/m{]} is a research option that allows the user to control the variation in outdoor air temperature as a function of height above ground. The real physical value is 0.0065 K/m. This field can be set to zero to turn off all temperature dependence on height. Note that the \emph{Air Temperature Sensor Height} in the \textbf{Site:WeatherStation} object should also be set to zero in order to force the local outdoor air temperatures to match the weather file outdoor air temperature. This change is required because the \textbf{Site:WeatherStation} object assumes an air temperature gradient of 0.0065 K/m. This field can be set to zero to turn off all temperature dependence on height.
+
+\begin{lstlisting}
+Site:HeightVariation,
+  0.22,    !- Wind Speed Profile Exponent
+  370,     !- Wind Speed Profile Boundary Layer Thickness {m}
+  0.0065;  !- Air Temperature Gradient Coefficient {deltaC/m}
+\end{lstlisting}
+
+\subsection{Site:GroundTemperature:BuildingSurface}\label{sitegroundtemperaturebuildingsurface}
+
+Ground temperatures are used for the ground heat transfer model. There can be only one ground temperature object included, and it is used as the outside surface temperature for all surfaces with Outside Boundary Condition = Ground. The object is options if you have no surfaces with ground contact. The outside surface temperature for individual surfaces can be specified using the OtherSideCoefficients (ref: SurfaceProperty:OtherSideCoefficients) object that allows Toutside to be set with a schedule. This permits using any number of different outside face temperatures in addition to the ground temperature.
+
+\begin{callout}
+Caution: The ``undisturbed'' ground temperatures calculated by the weather converter should not be used in building losses but are appropriate to be used in the Site:GroundTemperature:Shallow and Site:GroundTemperature:Deep objects. The reasoning (for building losses) is that these values are too extreme for the soil under a conditioned building. For best results, use the Slab or Basement program described in this document to calculate custom monthly average ground temperatures (see the Ground Heat Transfer section). This is especially important for residential applications and very small buildings. If one of these ground temperature preprocessors is not used, for typical commercial buildings in the USA, a reasonable default value is 2C less than the average indoor space temperature.
+\end{callout}
+
+More information about determining appropriate ground temperatures is given in the Auxiliary Programs document.
+
+\subsubsection{Inputs}\label{inputs-11-008}
+
+\paragraph{Field: Month Temperature(s) -- 12 fields in all}\label{field-month-temperatures-12-fields-in-all}
+
+Each numeric field is the monthly ground temperature (degrees Celsius) used for the indicated month (January = 1\(^{st}\) field, February = 2\(^{nd}\) field, etc.)
+
+An IDF example:
+
+\begin{lstlisting}
+Site:GroundTemperature:BuildingSurface,19,20,20,20,20,20,20,20,20,20,20,20;
+\end{lstlisting}
+
+\subsection{Site:GroundTemperature:Shallow}\label{sitegroundtemperatureshallow}
+
+Site:GroundTemperature:Shallow are used by the Surface Ground Heat Exchanger (i.e. object: GroundHeatExchanger:Surface). Only one shallow ground temperature object can be included.
+
+\begin{callout}
+Note that the ground temperatures included in full year weather files may be suitable of being used for the values in these fields -- namely, the .5 m depth temperatures that are calculated for ``undisturbed'' soil of ``typical'' conditions. However, you may wish to use some other change effect -- based on the weather conditions of the building location.
+\end{callout}
+
+This object may be used for objects requiring ``undisturbed'' ground temperatures. In these instances, the ``name'' input field is not required.
+
+\subsubsection{Inputs}\label{inputs-12-008}
+
+\paragraph{Field: Month Temperature(s) -- 12 fields in all}\label{field-month-temperatures-12-fields-in-all-1}
+
+Each numeric field is the monthly surface ground temperature (degrees Celsius) used for the indicated month (January = 1\(^{st}\) field, February = 2\(^{nd}\) field, etc.)
+
+An IDF example:
+
+\begin{lstlisting}
+Site:GroundTemperature:Shallow,4,4,6,6,10,10,15,15,14,14,8,8;
+\end{lstlisting}
+
+\subsection{Site:GroundTemperature:Deep}\label{sitegroundtemperaturedeep}
+
+Site:GroundTemperature:Deep are used by the Pond Ground Heat Exchanger object (i.e. object: GroundHeatExchanger:Pond). Only one deep ground temperature object can be included.
+
+\begin{callout}
+Note that the ground temperatures included in full year weather files may be suitable of being used for the values in these fields -- namely, the 4 m depth temperatures that are calculated for ``undisturbed'' soil of ``typical'' conditions. However, you may wish to use some other change effect -- based on the weather conditions or special knowledge of the building location.
+\end{callout}
+
+This object may be used for objects requiring ``undisturbed'' ground temperatures. In these instances, the ``name'' input field is not required.
+
+\subsubsection{Inputs}\label{inputs-13-007}
+
+\paragraph{Field: Month Temperature(s) -- 12 fields in all}\label{field-month-temperatures-12-fields-in-all-2}
+
+Each numeric field is the monthly deep ground temperature (degrees Celsius) used for the indicated month (January = 1\(^{st}\) field, February = 2\(^{nd}\) field, etc.)
+
+An IDF example:
+
+\begin{lstlisting}
+Site:GroundTemperature:Deep,  16,16,16,16,16,16,16,16,16,16,16,16;
+\end{lstlisting}
+
+\subsection{Site:GroundTemperature:Undisturbed:FiniteDifference}\label{sitegroundtemperatureundisturbedfinitedifference}
+
+Site:GroundTemperature:Undisturbed:FiniteDifference may be used by all objects requiring ``undisturbed'' ground temperatures. The object uses a 1D finite difference heat transfer model which uses the weather file to obtain surface boundary conditions. An annual simulation is run on the model during it's initialization until the annual ground temperature profile has reached steady periodic behavior. Once steady periodic behavior is reached, the ground tempeatures are cached for retrieval during the rest of the simulation.
+
+\subsubsection{Inputs}\label{inputs-14-007}
+
+\paragraph{Field: Soil Thermal Conductivity}\label{field-soil-thermal-conductivity-000}
+
+The thermal conductivity of the soil, in W/m-K.
+
+\paragraph{Field: Soil Density}\label{field-soil-density-000}
+
+The bulk density of the soil, in kg/m3.
+
+\paragraph{Field: Soil Specific Heat}\label{field-soil-specific-heat-000}
+
+The specific heat of dry soil, in J/kg-K.
+
+\paragraph{Field: Soil Moisture Content Volume Fraction}\label{field-soil-moisture-content-volume-fraction}
+
+A nominal value of soil moisture content to be used when evaluating soil thermal properties.
+
+\paragraph{Field: Soil Moisture Content Volume Fraction at Saturation}\label{field-soil-moisture-content-volume-fraction-at-saturation}
+
+A nominal value of soil moisture content when the soil is saturated, this is used in evaluating thermal properties of freezing soil.
+
+\paragraph{Field: Evapotranspiration Ground Cover Parameter}\label{field-evapotranspiration-ground-cover-parameter}
+
+Numeric field specifies the ground cover effects used in the evapotranspiration model at the ground surface heat balance. The values range from 0 (solid, non-permeable ground surface) to 1.5 (wild growth).
+
+An IDF example:
+
+\begin{lstlisting}
+Site:GroundTemperature:Undisturbed:FiniteDifference,
+  FDTemps,  !- Name of object
+  1.08,     !- Soil Thermal Conductivity {W/m-K}
+  962,      !- Soil Density {kg/m3}
+  2576,     !- Soil Specific Heat {J/kg-K}
+  30,       !- Soil Moisture Content Volume Fraction {percent}
+  50,       !- Soil Moisture Content Volume Fraction at Saturation {percent} 
+  0.408;    !- Evapotranspiration Ground Cover Parameter
+\end{lstlisting}
+
+\subsection{Site:GroundTemperature:Undisturbed:KusduaAchenbach}\label{sitegroundtemperatureundisturbedkusduaachenbach}
+
+Site:GroundTemperature:Undisturbed:KusudaAchenbach may be used by all objects requiring ``undisturbed'' ground temperatures. It provides an undisturbed ground temperature based on the correlation developed by Kusuda T. and P. Achenbach. 1965. The correlation uses three parameters for ground temperature at the surface to define a correlation for undisturbed ground temperatures as a function of depth and time. If one thinks of the ground temperature for a given depth as a sinusoid, the average ground temperature, amplitude (average difference between maximum ground temperature and minimum ground temperature), and the phase shift (day of minimum surface temperature) are all required to define the correlation.
+
+If the parameters are left blank they can be autocalculated by including soil surface temperatures in the input using the Site:GroundTemperature:Shallow object. They can also be calculated by using the CalcSoilSurfTemp preprocessor.
+
+Kusuda, T. and P.R. Achenbach. 1965. `Earth Temperatures and Thermal Diffusivity at Selected Stations in the United States.' \emph{ASHRAE Transactions}. 71(1): 61-74.
+
+\subsubsection{Field: Soil Thermal Conductivity}\label{field-soil-thermal-conductivity-1}
+
+The thermal conductivity of the soil, in W/m-K.
+
+\subsubsection{Field: Soil Density}\label{field-soil-density-1}
+
+The bulk density of the soil, in kg/m3.
+
+\subsubsection{Field: Soil Specific Heat}\label{field-soil-specific-heat-1}
+
+The specific heat of dry soil, in J/kg-K.
+
+\subsubsection{Field: Average Annual Ground Surface Temperature}\label{field-average-annual-ground-surface-temperature}
+
+This is the average ground surface temperature throughout the entire year, in °C.
+
+\subsubsection{Field: Average Amplitude of Annual Ground Surface Temperature}\label{field-average-amplitude-of-annual-ground-surface-temperature}
+
+This is the average amplitude of the ground surface temperature, in °C.
+
+\subsubsection{Field: Phase Shift of Minimum Surface Temperature}\label{field-phase-shift-of-minimum-surface-temperature}
+
+This is day of the year which has the lowest ground surface temperature.
+
+An IDF example:
+
+\begin{lstlisting}
+Site:GroundTemperature:Undisturbed:KusudaAchenbach,
+  KATemps,    !- Name of object
+  1.08,       !- Soil Thermal Conductivity {W/m-K}
+  962,        !- Soil Density {kg/m3}
+  2576,       !- Soil Specific Heat {J/kg-K}
+  15.5,       !- Average Soil Surface Temperature {C}
+  12.0,       !- Average Amplitude of Surface Temperature {deltaC}
+  21;         !- Phase Shift of Minimum Surface Temperature {days}
+\end{lstlisting}
+
+\subsection{Site:GroundTemperature:Undisturbed:Xing}\label{sitegroundtemperatureundisturbedxing}
+
+Site:GroundTemperature:Undisturbed:Xing may be used by all objects requiring ``undisturbed'' ground temperatures. It provides an undisturbed ground temperature based on the correlation developed by Xing, 2014. The correlation is a 5 parameter, 2 harmonic model based on the work of Lord Kelvin (Thomson, 1862). The average soil surface temperature and two sets of surface temperature amplitude and phase shift must be provided. Parameters for 4000+ international locations can be found in Xing, 2014.
+
+Thomson, W. 1862. `On the Reduction of Observations of Underground Temperature, with applications to Professor Forbes' Edinburgh Observations and the continued Calton Hill Series.' Proceedings of the Royal Society of Edinburgh. IV: 342-346.
+
+Xing, L. 2014. Estimations of Undisturbed Ground Temperatures using Numerical and Analytical Modeling. Ph.D.~Diss. Oklahoma State University, Stillwater, OK.
+
+\subsubsection{Inputs}\label{inputs-15-007}
+
+\paragraph{Field: Soil Thermal Conductivity}\label{field-soil-thermal-conductivity-2}
+
+The thermal conductivity of the soil, in W/m-K.
+
+\paragraph{Field: Soil Density}\label{field-soil-density-2}
+
+The bulk density of the soil, in kg/m3.
+
+\paragraph{Field: Soil Specific Heat}\label{field-soil-specific-heat-2}
+
+The specific heat of dry soil, in J/kg-K.
+
+\paragraph{Field: Average Soil Surface Temperature}\label{field-average-soil-surface-temperature-000}
+
+The average annual surface temperature of the soil, in deg C.
+
+\paragraph{Field: Soil Surface Temperature Amplitude 1}\label{field-soil-surface-temperature-amplitude-1}
+
+First soil surface temperature amplitude parameter, in deg C.
+
+\paragraph{Field: Soil Surface Temperature Amplitude 2}\label{field-soil-surface-temperature-amplitude-2}
+
+Second soil surface temperature amplitude parameter, in deg C.
+
+\paragraph{Field: Phase Shift of Surface Temperature Amplitude 1}\label{field-phase-shift-of-surface-temperature-amplitude-1}
+
+Phase shift of surface temperature amplitude 1, in days.
+
+\paragraph{Field: Phase Shift of Surface Temperature Amplitude 2}\label{field-phase-shift-of-surface-temperature-amplitude-2}
+
+Phase shift of surface temperature amplitude 2, in days.
+
+An IDF example:
+
+\begin{lstlisting}
+Site:GroundTemperature:Undisturbed:Xing,
+  Chicago-Ohare,!- Name of object
+  1.08,         !- Soil Thermal Conductivity {W/m-K}
+  962,          !- Soil Density {kg/m3}
+  2576,         !- Soil Specific Heat {J/kg-K}
+  11.1,         !- Average Soil Surface Tempeature {C}
+  13.4,         !- Soil Surface Temperature Amplitude 1 {deltaC}
+  0.7,          !- Soil Surface Temperature Amplitude 2 {deltaC}
+  25,           !- Phase Shift of Temperature Amplitude 1 {days}
+  30;           !- Phase Shift of Temperature Amplitude 2 {days}
+\end{lstlisting}
+
+\subsection{Site:GroundDomain:Slab}\label{sitegrounddomainslab}
+
+This section documents the input object used to simulate ground coupled heat transfer with horizontal building surfaces within EnergyPlus. Horizontal ground surfaces within EnergyPlus interact with the Site:GroundDomain object by utilizing the SurfaceProperty:OtherSideConditionsModel object. By utilizing this object, multiple horizontal surfaces can be coupled to the same Site:GroundDomain object. Each horizontal surface may also have its unique ground domain, however, runtime will be adversely affected.
+
+Generally, there are two scenarios which Site:GroundDomain is equipped to model: in-grade slabs, and on-grade slabs.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image012.png}
+\caption{In-grade configuration. \protect \label{fig:in-grade-configuration}}
+\end{figure}
+
+The in-grade slab option can be used to simulate situations when the upper slab surface is near the ground surface level. For this situation, slab's upper surface must interact with the zone via an OSCM boundary. Due to this, the FloorConstruction object for the zone floor must include a thin layer of the upper floor material. Horizontal and vertical insulation are modeled by the GroundDomain in this scenario. Horizontal insulation can be modeled as covering the full horizontal surface, or it can be limited to the perimeter regions only. In the latter case, the perimeter insulation width must be specified.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image013.png}
+\caption{On-grade configuration \protect \label{fig:on-grade-configuration}}
+\end{figure}
+
+The on-grade slab option can be used to simulate situations when the lower slab surface is near the ground surface level. In this situation, the entire floor must be included within the floor construction object. Vertical insulation is modeled by the GroundDomain in this scenario. Horizontal insulation can only be modeled as covering the full horizontal surface.
+
+\subsubsection{Inputs}\label{inputs-16-006}
+
+\paragraph{Field: Name}\label{field-name-8-009}
+
+Alpha field used as a unique identifier for each ground domain.
+
+\paragraph{Field: Ground Domain Depth}\label{field-ground-domain-depth}
+
+Numeric field used to determine the depth of the simulation domain, in meters.
+
+\paragraph{Field: Aspect Ratio}\label{field-aspect-ratio}
+
+Numeric field used to define the height to width ratio of the slab.
+
+\paragraph{Field: Perimeter Offset}\label{field-perimeter-offset}
+
+Numeric field used to determine the distance from the slab perimeter to the domain perimeter, in meters.
+
+\paragraph{Field: Soil Thermal Conductivity}\label{field-soil-thermal-conductivity-3}
+
+The thermal conductivity of the soil, in W/m-K.
+
+\paragraph{Field: Soil Density}\label{field-soil-density-3}
+
+The bulk density of the soil, in kg/m3.
+
+\paragraph{Field: Soil Specific Heat}\label{field-soil-specific-heat-3}
+
+The specific heat of dry soil, in J/kg-K. If moisture is defined in this object, moisture and freezing effects are accounted for by varying the specific heat value.
+
+\paragraph{Field: Soil Moisture Content Volume Fraction}\label{field-soil-moisture-content-volume-fraction-1}
+
+A nominal value of soil moisture content to be used when evaluating soil thermal properties.
+
+\paragraph{Field: Soil Moisture Content Volume Fraction at Saturation}\label{field-soil-moisture-content-volume-fraction-at-saturation-1}
+
+A nominal value of soil moisture content when the soil is saturated, this is used in evaluating thermal properties of freezing soil.
+
+\paragraph{Field: Type of Undisturbed Ground Temperature Object}\label{field-type-of-undisturbed-ground-temperature-object-000}
+
+This is the type of undisturbed ground temperature object that is used to determine the ground temperature.
+
+\paragraph{Field: Name of Undisturbed Ground Temperature Object}\label{field-name-of-undisturbed-ground-temperature-object-000}
+
+This is the name of the undisturbed ground temperature object that is used to determine the ground temperature.
+
+\paragraph{Field: Evapotranspiration Ground Cover Parameter}\label{field-evapotranspiration-ground-cover-parameter-1}
+
+Numeric field specifies the ground cover effects used in the evapotranspiration model at the ground surface heat balance. The values range from 0 (solid, non-permeable ground surface) to 1.5 (wild growth).
+
+\paragraph{Field: Slab Boundary Condition Model Name}\label{field-slab-boundary-condition-model-name}
+
+This is the name of the other side boundary condition model used.
+
+\paragraph{Field: Slab Location}\label{field-slab-location}
+
+Alpha field indicates whether the slab is in-grade (top surface level with ground surface) or on-grade (bottoms surface level with ground surface). Options include ``ONGRADE'' and ``INGRADE''.
+
+\paragraph{Field: Slab Material Name}\label{field-slab-material-name}
+
+Name of the material object representing the slab material. Only applicable to in-grade situations.
+
+\paragraph{Field: Horizontal Insulation}\label{field-horizontal-insulation}
+
+Alpha field indicates whether horizontal insulation is present. Options include ``YES'' and ``NO''. Only applicable to in-grade situations.
+
+\paragraph{Field: Horizontal Insulation Material Name}\label{field-horizontal-insulation-material-name}
+
+Name of material object representing the horizontal slab insulation. Optional argument only required if horizontal insulation is present.
+
+\paragraph{Field: Horizontal Insulation Extents}\label{field-horizontal-insulation-extents}
+
+Alpha field indicates whether the horizontal slab insulation extends to cover the full horizontal area of the slab, or only covers the slab perimeter. Optional argument only required if horizontal insulation is present. Options include ``FULL'' and ``PERIMETER''.
+
+\paragraph{Field: Perimeter Insulation Width}\label{field-perimeter-insulation-width}
+
+Numeric field indicating the width of the perimeter insulation measured from the slab edge. Valid range from \textgreater{} 0 to \textless{} half of smallest slab width.
+
+\paragraph{Field: Vertical Insulation}\label{field-vertical-insulation}
+
+Alpha field indicates whether vertical insulation is present. Options include ``YES'' and ``NO''.
+
+\paragraph{Field: Vertical Insulation Name}\label{field-vertical-insulation-name}
+
+Name of material object representing the vertical slab insulation. Optional argument only required if vertical insulation is present.
+
+\paragraph{Field: Vertical Insulation Depth}\label{field-vertical-insulation-depth}
+
+Numeric field indicates the depth measured in meters from the ground surface to which the vertical perimeter insulation extends. Valid range from \textgreater{} Slab Thickness to \textless{} Domain Depth.
+
+\paragraph{Field: Simulation Timestep}\label{field-simulation-timestep}
+
+Alpha field indicating whether the domain will update temperatures at each zone timestep, or at hourly intervals. Options include ``timestep'' and ``hourly''.
+
+An IDF example of an in-grade slab.
+
+\begin{lstlisting}
+Site:GroundDomain:Slab,
+  IngradeCoupledSlab, !- Name
+  5,                  !- Ground Domain Depth
+  1,                  !- Aspect Ratio
+  5,                  !- Domain Perimeter Offset
+  1.8,                !- Soil Thermal Conductivity
+  3200,               !- Soil Density
+  836,                !- Soil Specific Heat
+  30,                 !- Soil Moisture Content Volume Fraction
+  50,                 !- Soil Moisture Content Volume Fraction at Saturation
+  Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
+  KATemps,            !- Name of Undisturbed Ground Temperature Object
+  1,                  !- Evapotranspiration Ground Cover Parameter
+  GroundCoupledOSCM,  !- Name of Floor Boundary Condition Model
+  InGrade,            !- Slab Location (InGrade/OnGrade)
+  Slab Material-In-grade, !- Slab Material Name
+  Yes,                !- Horizontal Insulation
+  Slab Insulation,    !- Horizontal Insulation Material Name
+  Perimeter,          !- Full Horizontal or Perimeter Only
+  1,                  !- Perimeter insulation width
+  Yes,                !- Vertical Insulation
+  Slab Insulation,    !- Vertical Insulation Name
+  2,                  !- Vertical perimeter insulation depth from surface
+  Hourly;             !- Simulation timestep
+\end{lstlisting}
+
+And IDF example of an on-grade slab
+
+\begin{lstlisting}
+Site:GroundDomain:Slab,
+  OngradeCoupledSlab, !- Name
+  5,                  !- Ground Domain Depth {m}
+  1,                  !- Aspect Ratio
+  5,                  !- Domain Perimeter Offset {m}
+  1.8,                !- Soil Thermal Conductivity {W/m-K}
+  3200,               !- Soil Density {kg/m3}
+  836,                !- Soil Specific Heat {J/kg-K}
+  30,                 !- Soil Moisture Content Volume Fraction
+  50,                 !- Soil Moisture Content Volume Fraction at Saturation
+  Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
+  KATemps;            !- Name of Undisturbed Ground Temperature Object
+  1,                  !- Evapotranspiration Ground Cover Parameter
+  GroundCoupledOSCM,  !- Name of Floor Boundary Condition Model
+  OnGrade,            !- Slab Location (InGrade/OnGrade)
+  ,                   !- Slab Material Name
+  ,                   !- Horizontal Insulation (Yes/No)
+  ,                   !- Horizontal Insulation Material Name
+  ,                   !- Full Horizontal or Perimeter Only
+  ,                   !- Perimeter insulation width (m)
+  Yes,                !- Vertical Insulation (Yes/No)
+  Slab Insulation,    !- Vertical Insulation Name
+  2,                  !- Vertical perimeter insulation depth from surface
+  Hourly;             !- Simulation timestep. (Timestep/Hourly)</td>
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-015}
+
+The following output variables are available.
+
+\begin{itemize}
+\tightlist
+\item
+  Zone, Average, Zone Coupled Surface Heat Flux {[}W/m2{]}
+\item
+  Zone, Average, Zone Coupled Surface Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Zone Coupled Surface Heat Flux {[}W/m2{]}}\label{zone-coupled-surface-heat-flux-wm2}
+
+This is the value of the heat flux provided to the GroundDomain as a boundary condition. This is calculated by taking the average heat flux of all surfaces coupled to the domain's SurfaceProperty:OtherSideConditionsModel model.
+
+\paragraph{Zone Coupled Surface Temperature {[}C{]}}\label{zone-coupled-surface-temperature-c}
+
+This is the value of the SurfaceProperty:OtherSideConditionsModel surface temperature. This is the temperature provided to the ground coupled surfaces as an outside boundary condition.
+
+\subsection{Site:GroundDomain:Basement}\label{sitegrounddomainbasement}
+
+This section documents the input object used to simulate ground coupled heat transfer with underground zones within EnergyPlus. Zone surfaces within EnergyPlus interact with the Site:GroundDomain:Basement object by utilizing the SurfaceProperty:OtherSideConditionsModel object. Two separate OSCM are required for the basement vertical and horizontal surfaces. Vertical wall surfaces will interact with the first OSCM while the horizontal floor surface will interact with the second OSCM. Basement floor and wall surfaces are constructed normally by using the BuildingSurface:Detailed object, with the outside boundary condition being the OtherSideConditionsModel for the basement floor or wall. The outside surface of the wall being the interface between the ground domain and the EnergyPlus zone. Horizontal and vertical ground insulation are simulated by the ground domain, and therefore should not be included in the wall and floor construction objects.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image900.png}
+\caption{Basement Configuration \protect \label{fig:basement-configuration}}
+\end{figure}
+
+\begin{lstlisting}
+Site:GroundDomain:Basement,
+  CoupledBasement,     !- Name
+  10,                  !- Ground Domain Depth {m}
+  1,                   !- Aspect ratio
+  5,                   !- Perimeter offset {m}
+  1.8,                 !- Soil Thermal Conductivity {W/m-K}
+  3200,                !- Soil Density {kg/m3}
+  836,                 !- Soil Specific Heat {J/kg-K}
+  30,                  !- Soil Moisture Content Volume Fraction {percent}
+  50,                  !- Soil Moisture Content Volume Fraction at Saturation {percent}
+  Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
+  KATemps,             !- Name of Undisturbed Ground Temperature Object
+  1,                   !- Evapotranspiration Ground Cover Parameter
+  BasementFloorOSCM,   !- Name of Basement Floor Boundary Condition Model
+  Yes,                 !- Basement Horizontal Underfloor Insulation Present (Yes/No)
+  Basement Insulation, !- Basement Horizontal Insulation Underfloor Material Name
+  Full,                !- Full Horizontal or Perimeter Only (Full/Perimeter)
+  ,                    !- Perimeter width (m)
+  2.5,                 !- Depth of Basement Wall In Ground Domain {m}
+  BasementWallOSCM,    !- Name of Basement Wall Boundary Condition Model
+  Yes,                 !- Basement Wall Vertical Insulation Present(Yes/No)
+  Basement Insulation, !- Basement Wall Vertical Insulation Material Name
+  2.5,                 !- Vertical insulation depth from surface (m)
+  Hourly;              !- Domain Update interval. (Timestep, Hourly)
+  4;                   ! Mesh Density Parameter
+\end{lstlisting}
+
+\subsubsection{Inputs}\label{inputs-17-004}
+
+\paragraph{Field: Name}\label{field-name-9-009}
+
+Alpha field used as a unique identifier for each basement domain. Multiple basements domains can be simulated simultaneously, however, each domain must have a unique name. Additionally, despite the ability to simulate multiple domains simultaneously, these domains do not interact with each other and are treated as independent domains with boundary conditions given by the model parameters below.
+
+\paragraph{Field: Ground Domain Depth}\label{field-ground-domain-depth-1}
+
+Numeric field used to determine the depth of the simulation domain, in meters. A value of 10 meters is the default.
+
+\paragraph{Field: Aspect Ratio}\label{field-aspect-ratio-1}
+
+Numeric field, which is the ratio of basement length to width, used to determine the aspect ratio of the basement. This field along with the total basement floor area, which is taken as the combination of all surfaces connected to the floor OtherSideConditionsModel, are used to determine the size and shape of the basement domain. Aspect ratios and the inverse of aspect ratios should produce identical results. i.e. AR = 2 equals AR = 0.5. This field has units of meters/meters.
+
+\paragraph{Field: Domain Perimeter Offset}\label{field-domain-perimeter-offset}
+
+Numeric field used to determine the distance from the basement perimeter to the domain perimeter, in meters. A value of 5 is default.
+
+\paragraph{Field: Soil Thermal Conductivity}\label{field-soil-thermal-conductivity-4}
+
+The thermal conductivity of the soil, in W/m-K.
+
+\paragraph{Field: Soil Density}\label{field-soil-density-4}
+
+The bulk density of the soil, in kg/m3.
+
+\paragraph{Field: Soil Specific Heat}\label{field-soil-specific-heat-4}
+
+The specific heat of dry soil, in J/kg-K. If moisture is defined in this object, moisture and freezing effects are accounted for by varying the specific heat value.
+
+\paragraph{Field: Soil Moisture Content Volume Fraction}\label{field-soil-moisture-content-volume-fraction-2}
+
+A nominal value of soil moisture content to be used when evaluating soil thermal properties.
+
+\paragraph{Field: Soil Moisture Content Volume Fraction at Saturation}\label{field-soil-moisture-content-volume-fraction-at-saturation-2}
+
+A nominal value of soil moisture content when the soil is saturated, this is used in evaluating thermal properties of freezing soil.
+
+\paragraph{Field: Type of Undisturbed Ground Temperature Object}\label{field-type-of-undisturbed-ground-temperature-object-1-000}
+
+This is the type of undisturbed ground temperature object that is used to determine the ground temperature.
+
+\paragraph{Field: Name of Undisturbed Ground Temperature Object}\label{field-name-of-undisturbed-ground-temperature-object-1-000}
+
+This is the name of the undisturbed ground temperature object that is used to determine the ground temperature.
+
+\paragraph{Field: Evapotranspiration Ground Cover Parameter}\label{field-evapotranspiration-ground-cover-parameter-2}
+
+Numeric field specifies the ground cover effects used in the evapotranspiration model at the ground surface heat balance. The values range from 0 (solid, non-permeable ground surface) to 1.5 (wild growth). Model can be sensitive to variations in this parameter, especially in dry climates.
+
+\paragraph{Field: Basement Floor Boundary Condition Model Name}\label{field-basement-floor-boundary-condition-model-name}
+
+This is the name of the other side boundary condition model used for the basement floor surface.
+
+\paragraph{Field: Horizontal Insulation}\label{field-horizontal-insulation-1}
+
+Alpha field indicates whether horizontal insulation is present. Options include ``YES'' and ``NO''.
+
+\paragraph{Field: Horizontal Insulation Name}\label{field-horizontal-insulation-name}
+
+Name of material object representing the horizontal underfloor basement insulation. Optional argument only required if horizontal insulation is present.
+
+\paragraph{Field: Horizontal Insulation Extents}\label{field-horizontal-insulation-extents-1}
+
+Alpha field indicates whether the horizontal underfloor insulation extends to cover the full horizontal area of the basement floor, or only covers the basement floor perimeter. Optional argument only required if horizontal insulation is present. Options include ``FULL'' and ``PERIMETER''.
+
+\paragraph{Field: Perimeter Insulation Width}\label{field-perimeter-insulation-width-1}
+
+Numeric field indicating the width of the perimeter insulation measured from the basement floor edge. Valid range from \textgreater{} 0 to \textless{} half of smallest basement floor width.
+
+\paragraph{Field: Basement Depth}\label{field-basement-depth}
+
+Depth of basement floor surface referenced from the ground surface, in meters. This domain should be the distance from the ground surface down to the basement floor surface. In cases where the ground surface is below the main above-ground building level, a separate wall surface should be employed between the basement walls and the main level walls.
+
+\paragraph{Field: Basement Wall Boundary Condition Model Name}\label{field-basement-wall-boundary-condition-model-name}
+
+Name of the other side condition boundary model used for the basement walls.
+
+\paragraph{Field: Vertical Insulation}\label{field-vertical-insulation-1}
+
+Alpha field indicates whether vertical insulation is present. Options include ``YES'' and ``NO''.
+
+\paragraph{Field: Vertical Insulation Name}\label{field-vertical-insulation-name-1}
+
+Name of material object representing the vertical slab insulation. Optional argument only required if vertical insulation is present.
+
+\paragraph{Field: Vertical Insulation Depth}\label{field-vertical-insulation-depth-1}
+
+Numeric field indicates the depth measured in meters from the ground surface to which the vertical perimeter insulation extends. Valid range from \textgreater{} 0 to \textless{} Basement Depth.
+
+\paragraph{Field: Simulation Timestep}\label{field-simulation-timestep-1}
+
+Alpha field indicating whether the domain will update temperatures at each zone timestep, or at hourly intervals. Options include ``timestep'' and ``hourly''.
+
+\paragraph{Mesh Density Parameter}\label{mesh-density-parameter}
+
+Integer field indicating the density of the finite difference ground domain cells between the basement and the far field boundaries. Default value is 4. Total number of ground domain cells, insulation cells, and ground surface cells are indicated as outputs to the eio file.
+
+\subsubsection{Outputs}\label{outputs-2-013}
+
+The following output variables are available.
+
+\begin{itemize}
+\item
+  Wall Interface Heat Flux
+\item
+  Wall Interface Temperature
+\item
+  Floor Interface Heat Flux
+\item
+  Floor Interface Temperature
+\end{itemize}
+
+\paragraph{Wall Interface Heat Flux {[}W/m2{]}}\label{wall-interface-heat-flux-wm2}
+
+This is the value of the heat flux provided to ground domain as a boundary condition for the basement walls. Should be equal to the basement wall outside heat flux.
+
+\paragraph{Wall Interface Temperature {[}C{]}}\label{wall-interface-temperature-c}
+
+This is the value of the SurfaceProperty:OtherSideConditionsModel surface temperature. This is the temperature provided to the basement wall surfaces as an outside boundary condition.
+
+\paragraph{Floor Interface Heat Flux {[}W/m2{]}}\label{floor-interface-heat-flux-wm2}
+
+This is the value of the heat flux provided to ground domain as a boundary condition for the basement floor. Should be equal to the basement floor outside heat flux.
+
+\paragraph{Floor Interface Temperature {[}C{]}}\label{floor-interface-temperature-c}
+
+This is the value of the SurfaceProperty:OtherSideConditionsModel surface temperature. This is the temperature provided to the ground coupled floor surfaces as an outside boundary condition.
+
+\subsection{Site:GroundTemperature:FCfactorMethod}\label{sitegroundtemperaturefcfactormethod}
+
+Site:GroundTemperature:FCfactorMethod is used only by the underground walls or slabs-on-grade or underground floors defined with C-factor (Construction:CfactorUndergroundWall) and F-factor (Construction:FfactorGroundFloor) method for code compliance calculations where detailed construction layers are unknown. Only one such ground temperature object can be included. The monthly ground temperatures for this object are close to the monthly outside air temperatures delayed by three months. If user does not input this object in the IDF file, it will be defaulted to the 0.5m set of monthly ground temperatures from the weather file if they are available. Entering these will also overwrite any ground temperatures from the weather file in the F and C factor usage. If neither is available, an error will result.
+
+\subsubsection{Inputs}\label{inputs-18-004}
+
+\paragraph{Field: Month Temperature(s) -- 12 fields in all}\label{field-month-temperatures-12-fields-in-all-3}
+
+Each numeric field is the monthly ground temperature (degrees Celsius) used for the indicated month (January = 1\(^{st}\) field, February = 2\(^{nd}\) field, etc.)
+
+And, the IDF example:
+
+\begin{lstlisting}
+Site:GroundTemperature:FCfactorMethod,  9.5, 3.5, -0.7, -1.7, -0.6, 3.6, 9.3, 14, 18.2, 22.7, 21.2, 16.8;
+\end{lstlisting}
+
+\subsection{Site:GroundReflectance}\label{sitegroundreflectance}
+
+Ground reflectance values are used to calculate the ground reflected solar amount. This fractional amount (entered monthly) is used in this equation:
+
+\begin{equation}
+\rm{GroundReflectedSolar} = \left( \rm{BeamSolar} \cdot cos \left( \rm{SunZenithAngle} \right) + \rm{DiffuseSolar} \right) \cdot \rm{GroundReflectance}
+\end{equation}
+
+Of course, the Ground Reflected Solar is never allowed to be negative. The ground reflectance can be further modified when snow is on the ground by the Snow Ground Reflectance Modifier. To use no ground reflected solar in your simulation, enter 0.0 for each month.
+
+\subsubsection{Inputs}\label{inputs-19-003}
+
+\paragraph{Field: Month Average Ground Reflectance(s) -- 12 fields in all}\label{field-month-average-ground-reflectances-12-fields-in-all}
+
+Each numeric field is the monthly average reflectivity of the ground used for the indicated month (January = 1\(^{st}\) field, February = 2\(^{nd}\) field, etc.)
+
+And use in an IDF:
+
+\begin{lstlisting}
+Site:GroundReflectance,
+  0.600,     !January Ground Reflectance
+  0.600,     !February Ground Reflectance
+  0.400,     !March Ground Reflectance
+  0.300,     !April Ground Reflectance
+  0.200,     !May Ground Reflectance
+  0.200,     !June Ground Reflectance
+  0.200,     !July Ground Reflectance
+  0.200,     !August Ground Reflectance
+  0.200,     !September Ground Reflectance
+  0.200,     !October Ground Reflectance
+  0.300,     !November Ground Reflectance
+  0.400;     !December Ground Reflectance
+\end{lstlisting}
+
+\subsection{Site:GroundReflectance:SnowModifier}\label{sitegroundreflectancesnowmodifier}
+
+It is generally accepted that snow resident on the ground increases the basic ground reflectance. EnergyPlus allows the user control over the snow ground reflectance for both ``normal ground reflected solar'' calculations (see above) and snow ground reflected solar modified for daylighting. These are entered under this object and both default to 1 (same as normal ground reflectance -- no special case for snow which is a conservative approach).
+
+\subsubsection{Inputs}\label{inputs-20-003}
+
+\paragraph{Field: Ground Reflected Solar Modifier}\label{field-ground-reflected-solar-modifier}
+
+This field is a decimal number which is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values).
+
+\begin{equation}
+\rm{GroundReflectance}_{\rm{used}} = \rm{GroundReflectance} \cdot \rm{Modifier}_{\rm{Snow}}
+\end{equation}
+
+The actual Ground Reflectance is limited to {[}0.0,1.0{]}.
+
+\paragraph{Field: Daylighting Ground Reflected Solar Modifier}\label{field-daylighting-ground-reflected-solar-modifier}
+
+This field is a decimal number which is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values).
+
+\begin{equation}
+\rm{DaylightingGroundReflectance}_{\rm{used}} = \rm{GroundReflectance} \cdot \rm{Modifier}_{\rm{Snow}}
+\end{equation}
+
+The actual Ground Reflectance is limited to {[}0.0,1.0{]}.
+
+An IDF example:
+
+\begin{lstlisting}
+Site:GroundReflectance:SnowModifier,
+  1.0;       !- Ground Reflected Solar Modifier
+\end{lstlisting}
+
+Outputs will show both the inputs from the above object as well as monthly values for both Snow Ground Reflectance and Snow Ground Reflectance for Daylighting.
+
+\subsection{Site:WaterMainsTemperature}\label{sitewatermainstemperature}
+
+The Site:WaterMainsTemperature object is used to calculate water temperatures delivered by underground water main pipes. The mains temperatures are used as default, make-up water temperature inputs for several plant objects, including: \textbf{WaterUse:Equipment, WaterUse:Connections, WaterHeater:Mixed} and \textbf{WaterHeater:Stratified}. The mains temperatures are also used in the water systems objects to model the temperature of cold water supplies.
+
+Water mains temperatures are a function of outdoor climate conditions and vary with time of year. A correlation has been formulated to predict water mains temperatures based on two weather inputs:
+
+\begin{itemize}
+\item
+  average annual outdoor air temperature (dry-bulb)
+\item
+  maximum difference in monthly average outdoor air temperatures
+\end{itemize}
+
+These values can be easily calculated from annual weather data using a spreadsheet or from the ``.stat'' file available with the EnergyPlus weather files at \href{http://www.energyplus.gov}{www.energyplus.gov}. Monthly statistics for dry-bulb temperatures are shown with daily averages. The daily averages are averaged to obtain the annual average. The maximum and minimum daily average are subtracted to obtain the maximum difference. For more information on the water mains temperatures correlation, see the \emph{EnergyPlus Engineering Document}.
+
+Alternatively, the Site:WaterMainsTemperature object can read values from a schedule. This is useful for measured data or when water comes from a source other than buried pipes, e.g., a river or lake.
+
+If there is no Site:WaterMainsTemperature object in the input file, a default constant value of 10 C is assumed.
+
+\subsubsection{Inputs}\label{inputs-21-003}
+
+\paragraph{Field: Calculation Method}\label{field-calculation-method}
+
+This field selects the calculation method and must have the keyword Schedule or Correlation.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-003}
+
+If the calculation method is Schedule, the water mains temperatures are read from the schedule referenced by this field. If the calculation method is Correlation, this field is ignored.
+
+\paragraph{Field: Annual Average Outdoor Air Temperature}\label{field-annual-average-outdoor-air-temperature}
+
+If the calculation method is Correlation, this field is used in the calculation as the annual average outdoor air temperature (dry-bulb) {[}C{]}. If the calculation method is Schedule, this field is ignored.
+
+\paragraph{Field: Maximum Difference In Monthly Average Outdoor Air Temperatures}\label{field-maximum-difference-in-monthly-average-outdoor-air-temperatures}
+
+If the calculation method is Correlation, this field is used in the calculation as the maximum difference in monthly average outdoor air temperatures {[}\(\Delta\)C{]}. If the calculation method is Schedule, this field is ignored.
+
+\begin{lstlisting}
+Site:WaterMainsTemperature,
+  Correlation,  !- Calculation Method {SCHEDULE | CORRELATION}
+  ,             !- Schedule Name
+  9.69,         !- Annual Average Outdoor Air Temperature {C}
+  28.1;         !- Maximum Difference In Monthly Average Outdoor Air Temperatures {deltaC}
+\end{lstlisting}
+
+\subsection{Site:Precipitation}\label{siteprecipitation}
+
+The Site:Precipitation object is used to describe the amount of water precipitation at the building site over the course of the simulation run period. Precipitation includes both rain and the equivalent water content of snow. Precipitation is not yet described well enough in the many building weather data files. So this object can be used to provide the data using Schedule objects that define rates of precipitation in meters per hour.
+
+A set of schedules for site precipitation have been developed for USA weather locations and are provided with EnergyPlus in the data set called PrecipitationSchedulesUSA.idf. The user can develop schedules however they want. The schedules in the data set were developed using EnergyPlus' weather file (EPW) observations and the average monthly precipitation for the closest weather site provided by NOAA. EPW files for the USA that were based on TMY or TMY2 include weather observations for Light/Moderate/Heavy rainfall, however most international locations do not include these observations. The values were modeled by taking the middle of the ranges quoted in the EPW data dictionary. The assumed piecewise function is shown below.
+
+\begin{equation}
+\rm{Amount} \, (m/hour) = \, \left\{
+  \begin{array}{*{20}{c}}
+    \rm{Light} = 0.0125 \\
+    \rm{Moderate} = 0.052 \\
+    \rm{Heavy} = 0.1
+  \end{array}
+\right.
+\end{equation}
+
+The values were inserted on hour by hour basis for the month based on the observations. Then each month was rescaled to meet the average precipitation for the month based on the 30-year average (1971-2000) provided by the NOAA/NCDC. Therefore, the flags in the EPW file match the precipitation schedules for the USA. Note that summing the average monthly precipitation values will not give you the average yearly precipitiation. The resulting value may be lower or higher than the average yearly value.
+
+Once the typical rainfall pattern and rates are scheduled, the Site:Precipitation object provides a method of shifting the total rainfall up or down for design purposes. Wetter or drier conditions can be modeled by changing the Design Annual Precipitation although the timing of precipitation throughout the year will not be changed.
+
+\subsubsection{Inputs}\label{inputs-22-002}
+
+\paragraph{Field: Precipitation Model Type}\label{field-precipitation-model-type}
+
+Choose rainfall modeling options. Only available option is ScheduleAndDesignLevel.
+
+\paragraph{Field: Design Level for Total Annual Precipitation}\label{field-design-level-for-total-annual-precipitation}
+
+Magnitude of total precipitation for an annual period to be used in the model. Value selected by the user to correspond with the amount of precipitation expected or being assumed for design purposes. The units are in meters. This field works with the following two fields to allow easily shifting the amounts without having to generate new schedules.
+
+\paragraph{Field: Precipitation Rate Schedule Name}\label{field-precipitation-rate-schedule-name}
+
+Name of a schedule defined elsewhere that describes the rate of precipitation. The precipitation rate schedule is analogous to weather file data. However, weather files for building simulation do not currently contain adequate data for such calculations. Therefore, EnergyPlus schedules are used to enter the pattern of precipitation events. The values in this schedule are the average rate of precipitation in meters per hour. The integration of these values over an annual schedule should equal the nominal annual precipitation.
+
+\paragraph{Field: Average Total Annual Precipitation}\label{field-average-total-annual-precipitation}
+
+Magnitude of annual precipitation associated with the rate schedule. This value is used to normalize the precipitation.
+
+IDF example:
+
+\begin{lstlisting}
+Site:Precipitation,
+  ScheduledAndDesignLevel, !- Precipitation Model Type
+  0.75,                    !- Design Level Total Annual Precipitation {m/yr}
+  PrecipitationSchd,       !- Schedule Name for Precipitation Rates
+  0.80771;                 !- Average Total Annual Precipitation {m/yr}
+\end{lstlisting}
+
+\subsection{RoofIrrigation}\label{roofirrigation}
+
+The RoofIrrigation object is used to describe the amount of irrigation on the ecoroof surface over the course of the simulation runperiod. This object is used to provide irrigation data using Schedule objects that define rates of irrigation in meters per hour. These schedules can be one of two types: Schedule, or SmartSchedule.
+
+\subsubsection{Inputs}\label{inputs-23-002}
+
+\paragraph{Field: Irrigation Model Type}\label{field-irrigation-model-type}
+
+Choose irrigation modeling options. Available options are \textbf{Schedule} and \textbf{SmartSchedule}. The \textbf{Schedule} type is used to force an irrigation schedule regardless of the current moisture state of the soil. The \textbf{SmartSchedule} type allows the precipitation schedule to be overridden if the current moisture state of the soil is greater than 40\% saturated.
+
+\paragraph{Field: Irrigation Rate Schedule Name}\label{field-irrigation-rate-schedule-name}
+
+Name of a schedule defined elsewhere that describes the rate of irrigation. The values in this schedule are the average rate of irrigation in meters per hour.
+
+\paragraph{Field: Irrigation Maximum Saturation Threshold}\label{field-irrigation-maximum-saturation-threshold}
+
+Used with the SmartSchedule option in the Irrigation Model Type field to override the default 40\% saturation limit for turning off the irrigation: values of 0 to 100 (percent) can be entered with 40\% being the default.
+
+IDF example:
+
+\begin{lstlisting}
+RoofIrrigation,
+  Schedule,       !- Irrigation Model Type
+  IrrigationSchd; !- Schedule Name for Irrigation Rates
+\end{lstlisting}
+
+\subsection{Solar and Visible Spectrum Objects}\label{solar-and-visible-spectrum-objects}
+
+The next two objects enable users to enter solar and visible spectrum which is used to calculate the thermal and visual performance of windows if their glazings are defined with full spectral data. EnergyPlus versions 8.0 and older hard-wired the solar and visible spectrum. The solar spectrum assumes air mass 1.5 terrestrial solar global spectral irradiance values (W/m2-micron) on a 37o tilted surface, based on ISO 9845-1 and ASTM E 892; derived from Optics5 data file ISO-9845GlobalNorm.std, 10-14-99. The visible/photopic spectrum is based on CIE 1931 observer; ISO/CIE 10527, CIE Standard Calorimetric Observers; derived from Optics5 data file ``CIE 1931 Color Match from E308.txt'', which is the same as WINDOW4 file Cie31t.dat.
+
+\subsection{Site:SolarAndVisibleSpectrum}\label{sitesolarandvisiblespectrum}
+
+The SolarAndVisibleSpectrum object is used to specify the solar and visible spectrum data which is used as spectral weighting function to calculate the window performance (transmittance and absorptance) in EnergyPlus. This is a unique object, if it is missing from an IDF file, the default (same as EnergyPlus version 8.0) solar and visible spectrum data will be used.
+
+\subsubsection{Inputs}\label{inputs-24-001}
+
+\paragraph{Field: Name}\label{field-name-10-008}
+
+This field specifies the name of the SolarAndVisibleSpectrum object.
+
+\paragraph{Field: Spectrum Data Method}\label{field-spectrum-data-method}
+
+This field specifies the method used to enter the spectrum data. Two choices are available: Default and UserDefined. The choice Default will continue to use the hard-wired spectrum data in EnergyPlus (for backward compatibility). The choice UserDefined allows users to specify custom solar and visible spectrum data. The default choice is Default.
+
+\paragraph{Field: Solar Spectrum Data Name}\label{field-solar-spectrum-data-name}
+
+This field is required if the Spectrum Data Method is set to UserDefined. This field references a spectrum dataset for solar.
+
+\paragraph{Field: Visible Spectrum Data Name}\label{field-visible-spectrum-data-name}
+
+This field is required if the Spectrum Data Method is set to UserDefined. This field references a spectrum dataset for visible.
+
+IDF example:
+
+\begin{lstlisting}
+Site:SolarAndVisibleSpectrum,
+  LocalSpectrum,            !- Name
+  UserDefined,              !- Spectrum Data Method: Default, UserDefined
+  SolarSpectrum,            !- Solar Spectrum Data Object Name
+  VisibleSpectrum;          !- Visible Spectrum Data Object
+\end{lstlisting}
+
+\subsection{Site:SpectrumData}\label{sitespectrumdata}
+
+The Site:SpectrumData object holds the user defined solar or visible spectrum data. For solar spectrum, up to 107 pairs of (wavelength, spectrum) can be entered. For visible spectrum, up to 81 pairs can be entered.
+
+\subsubsection{Inputs}\label{inputs-25-001}
+
+\paragraph{Field: Name}\label{field-name-11-007}
+
+This field specifies the name of the SpectrumData object. The name must be unique across all SpectrumData objects.
+
+\paragraph{Field: Spectrum Data Type}\label{field-spectrum-data-type}
+
+This field specifies the type of spectrum data. Choices are Solar and Visible.
+
+\paragraph{Field: Wavelength \textless{}n\textgreater{}}\label{field-wavelength-n}
+
+This field specifies the nth wavelength in micron.
+
+\paragraph{Field: Spectrum \textless{}n\textgreater{}}\label{field-spectrum-n}
+
+This field specifies the nth spectrum corresponding to the nth wavelength.
+
+IDF example:
+
+\begin{lstlisting}
+Site:SpectrumData,
+  SolarSpectrum, !- Name
+  Solar,         !- Spectrum Data Type
+  0.3,0,         !- up to 107 pair of (wavelength, spectrum)
+  0.305,3.4,
+  0.31,15.6,
+  0.315,41.1,
+  0.32,71.2,
+  0.325,100.2,
+  0.33,152.4,
+  0.335,155.6,
+  0.34,179.4,
+  0.345,186.7,
+  0.35,212,
+  0.36,240.5,
+  0.37,324,
+  0.38,362.4,
+  ...;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-011}
+
+Climate related variables appear in two places for EnergyPlus outputs. Certain objects that are invariant throughout a simulation period have lines appear in the eplusout.eio file. For descriptions of this reporting, please see the Output Details and Examples document.
+
+\subsubsection{Outputs}\label{outputs-4-008}
+
+Variables related to ambient environment data are available at timestep and higher resolutions. Below is a variable dictionary of these variables and subsequent definitions:
+
+\begin{itemize}
+\item
+  Zone,Average,Site Outdoor Air Drybulb Temperature {[}C{]}
+\item
+  Zone,Average,Site Outdoor Air Dewpoint Temperature {[}C{]}
+\item
+  Zone,Average,Site Outdoor Air Wetbulb Temperature {[}C{]}
+\item
+  Zone,Average,Site Outdoor Air Humidity Ratio {[}kgWater/kgAir{]}
+\item
+  Zone,Average,Site Outdoor Air Relative Humidity {[}\%{]}
+\item
+  Zone,Average,Site Outdoor Air Barometric Pressure {[}Pa{]}
+\item
+  Zone,Average,Site Wind Speed {[}m/s{]}
+\item
+  Zone,Average,Site Wind Direction {[}deg{]}
+\item
+  Zone,Average,Site Sky Temperature {[}C{]}
+\item
+  Zone,Average,Site Horizontal Infrared Radiation Rate per Area {[}W/m2{]}
+\item
+  Zone,Average,Site Diffuse Solar Radiation Rate per Area {[}W/m2{]}
+\item
+  Zone,Average,Site Direct Solar Radiation Rate per Area {[}W/m2{]}
+\item
+  Zone,Sum,Site Precipitation Depth {[}m{]}
+\item
+  Zone,Average,Site Ground Reflected Solar Radiation Rate per Area {[}W/m2{]}
+\item
+  Zone,Average,Site Ground Temperature {[}C{]}
+\item
+  Zone,Average,Site Surface Ground Temperature {[}C{]}
+\item
+  Zone,Average,Site Deep Ground Temperature {[}C{]}
+\item
+  Zone,Average,Site Simple Factor Model Ground Temperature {[}C{]}
+\item
+  Zone,Average,Site Outdoor Air Enthalpy {[}J/kg{]}
+\item
+  Zone,Average,Site Outdoor Air Density {[}kg/m3{]}
+\item
+  Zone,Average,Site Solar Azimuth Angle {[}deg{]}
+\item
+  Zone,Average,Site Solar Altitude Angle {[}deg{]}
+\item
+  Zone,Average,Site Solar Hour Angle {[}deg{]}
+\item
+  Zone,Average,Site Rain Status {[]}
+\item
+  Zone,Average,Site Snow on Ground Status {[]}
+\item
+  Zone,Average,Site Exterior Horizontal Sky Illuminance {[}lux{]}
+\item
+  Zone,Average,Site Exterior Horizontal Beam Illuminance {[}lux{]}
+\item
+  Zone,Average,Site Exterior Beam Normal Illuminance {[}lux{]}
+\item
+  Zone,Average,Site Sky Diffuse Solar Radiation Luminous Efficacy {[}lum/W{]}
+\item
+  Zone,Average,Site Beam Solar Radiation Luminous Efficacy {[}lum/W{]}
+\item
+  Zone,Average,Site Daylighting Model Sky Clearness {[]}
+\item
+  Zone,Average,Sky Brightness for Daylighting Calculation {[]}
+\item
+  Zone,Average,Site Daylight Saving Time Status {[]}
+\item
+  Zone,Average,Site Day Type Index {[]}
+\item
+  Zone,Average,Site Mains Water Temperature {[}C{]}
+\item
+  HVAC,Average,Site Precipitation Rate {[}m/s{]}
+\item
+  HVAC,Sum,Site Precipitation Depth {[}m{]}
+\item
+  HVAC,Sum,Water System Roof Irrigation Scheduled Depth{[}m{]}
+\item
+  HVAC,Sum,Water System Roof Irrigation Actual Depth{[}m{]}
+\end{itemize}
+
+Note that these data values may be interpolated from ``hour'' points (ref: Weather Data Hourly Interpolation). Most of the data values represent the ``average'' over the reporting resolution period.
+
+\paragraph{Site Outdoor Air Drybulb Temperature {[}C{]}}\label{site-outdoor-air-drybulb-temperature-c}
+
+This is the outdoor dry-bulb temperature in degrees C.
+
+\paragraph{Site Outdoor Air Dewpoint Temperature {[}C{]}}\label{site-outdoor-air-dewpoint-temperature-c}
+
+This is the outdoor dewpoint temperature in degrees C.
+
+\paragraph{Site Outdoor Air Wetbulb Temperature {[}C{]}}\label{site-outdoor-air-wetbulb-temperature-c}
+
+The outdoor wet-bulb temperature is derived (at the timestep) from the values for dry-bulb temperature, humidity ratio and barometric pressure.
+
+\paragraph{Site Outdoor Air Humidity Ratio {[}kgWater/kgAir{]}}\label{site-outdoor-air-humidity-ratio-kgwaterkgair}
+
+The outdoor humidity ratio is derived (at the timestep) from the dry-bulb temperature, relative humidity and barometric pressure.
+
+\paragraph{Site Outdoor Air Relative Humidity {[}\%{]}}\label{site-outdoor-air-relative-humidity}
+
+This is the outdoor relative humidity expressed in percent.
+
+\paragraph{Site Outdoor Air Barometric Pressure {[}Pa{]}}\label{site-outdoor-air-barometric-pressure-pa}
+
+This is the atmospheric/barometric pressure in Pa.
+
+\paragraph{Site Wind Speed {[}m/s{]}}\label{site-wind-speed-ms}
+
+This is the outdoor wind speed in m/s.
+
+\paragraph{Site Wind Direction {[}deg{]}}\label{site-wind-direction-deg}
+
+This is the wind direction (N = 0, E = 90, S = 180, W = 270).
+
+\paragraph{Site Sky Temperature {[}C{]}}\label{site-sky-temperature-c}
+
+The sky temperature is derived from horizontal infrared radiation intensity. It is expressed in degrees C. The default calculation is shown below but this value may be modified by the WeatherProperty:SkyTemperature object. Note that Sigma is the Stefan-Boltzmann constant in the following equation:
+
+\begin{equation}
+Sky\;Temperature = {\left( {\frac{{Horizontal\;IR}}{{Sigma}}} \right)^{\frac{1}{4}}} - {273.15_{Conversion\;from\;Kelvin\;to\;Centigrade}}
+\end{equation}
+
+\paragraph{Site Horizontal Infrared Radiation Rate per Area {[}W/m2{]}}\label{site-horizontal-infrared-radiation-rate-per-area-wm2}
+
+The horizontal infrared radiation intensity is expressed in W/m\(^{2}\) based, if missing from the weather file, on opaque sky cover, sky emissivity, temperature and other factors. The general calculation of Site Horizontal Infrared Radiation Rate per Area is discussed in both the Engineering Reference and the Auxiliary Programs document.
+
+\paragraph{Site Diffuse Solar Radiation Rate per Area {[}W/m2{]}}\label{site-diffuse-solar-radiation-rate-per-area-wm2}
+
+Diffuse solar is the amount of solar radiation in W/m\(^{2}\) received from the sky (excluding the
+
+solar disk) on a horizontal surface.
+
+\paragraph{Site Direct Solar Radiation Rate per Area {[}W/m2{]}}\label{site-direct-solar-radiation-rate-per-area-wm2}
+
+Site Direct Solar Radiation Rate per Area is amount of solar radiation in W/m\(^{2}\) received within a 5.7° field of view centered on the sun. This is also known as Beam Solar.
+
+\paragraph{Site Precipitation Depth {[}m{]}}\label{site-precipitation-depth-m}
+
+This is the amount of liquid precipitation (m). The source of this field may be the weather file or the Site:Precipitation object. The weather file values are in millimeters, but the report here is in meters. Two separate entities are displayed -- from the weather file the key value is ``Environment''; from the Site:Precipitation object the key value is Site:Precipitation.
+
+If the weather file does not have a liquid precipitation field but does have the present weather fields, then a heuristic calculation is attempted for both flagging when it is raining and the amount of precipitation. If the weather file does have liquid precipitation fields, then the output (e.g. monthly) can be compared with the weather file stat file.
+
+\paragraph{Site Ground Reflected Solar Radiation Rate per Area {[}W/m2{]}}\label{site-ground-reflected-solar-radiation-rate-per-area-wm2}
+
+The ground reflected solar amount (W/m\(^{2}\)) is derived from the Beam Solar, Diffuse Solar, User specified Ground Reflectance (for month) and Solar Altitude Angle:
+
+\begin{multline}
+  \rm{Groundreflectedsolar}
+  \\
+  = \left( \rm{Beamsolar} \cdot cos \left( \rm{SolarAltitudeAngle} \right) + \rm{Diffusesolar} \right) \cdot \rm{Groundreflectance}_{\rm{month}}
+\end{multline}
+
+where if the calculation returns a value \textless{} 0.0, then 0.0 will be reported.
+
+\paragraph{Site Ground Temperature {[}C{]}}\label{site-ground-temperature-c}
+
+The ground temperature is reported in degrees C -- this is a user-specified input by month.
+
+\paragraph{Site Surface Ground Temperature {[}C{]}}\label{site-surface-ground-temperature-c}
+
+The ground temperature is reported in degrees C -- this is a user-specified input (object: Site:GroundTemperature:Shallow) by month.
+
+\paragraph{Site Deep Ground Temperature {[}C{]}}\label{site-deep-ground-temperature-c}
+
+The ground temperature is reported in degrees C -- this is a user-specified input (object: Site:GroundTemperature:Deep) by month.
+
+\paragraph{Site Simple Factor Model Ground Temperature {[}C{]}}\label{site-simple-factor-model-ground-temperature-c}
+
+The Site Simple Factor Model Ground Temperature is reported in degrees C -- this is a user-specified input (object: Site:GroundTemperature:FCfactorMethod) by month or gleaned from the weather file as noted in the description of the object.
+
+\paragraph{Site Outdoor Air Enthalpy {[}J/kg{]}}\label{site-outdoor-air-enthalpy-jkg}
+
+Outdoor enthalpy is derived at each timestep from the Site Outdoor Air Drybulb Temperatureand the Site Outdoor Air Humidity Ratio. It is reported in J/kg.
+
+\paragraph{Site Outdoor Air Density {[}kg/m3{]}}\label{site-outdoor-air-density-kgm3}
+
+Outdoor air density is derived at each timestep from the Site Outdoor Air Barometric Pressure, the Outdoor Dry-bulb temperature and the Outdoor Humidity Ratio. It is reported in units kg/m\(^{3}\).
+
+\paragraph{Site Solar Azimuth Angle {[}deg{]}}\label{site-solar-azimuth-angle-deg}
+
+The Solar Azimuth Angle (f) is measured from the North (clockwise) and is expressed in degrees. This is shown more clearly in the following figure.
+
+\begin{figure}[hbtp] % fig 9
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image020.png}
+\caption{Solar Position Illustration \protect \label{fig:solar-position-illustration}}
+\end{figure}
+
+\paragraph{Site Solar Altitude Angle {[}deg{]}}\label{site-solar-altitude-angle-deg}
+
+The Solar Altitude Angle (b) is the angle of the sun above the horizontal (degrees).
+
+\paragraph{Site Solar Hour Angle {[}deg{]}}\label{site-solar-hour-angle-deg}
+
+The Solar Hour Angle (\emph{H}) gives the apparent solar time for the current time period (degrees). It is common astronomical practice to express the hour angle in hours, minutes and seconds of time rather than in degrees. You can convert the hour angle displayed from EnergyPlus to time by dividing by 15. (Note that 1 hour is equivalent to 15 degrees; 360° of the Earth's rotation takes place every 24 hours.) The relationship of angles in degrees to time is shown in the following table:
+
+% table 6
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Relationship of Angles (degrees) to Time \label{table:relationship-of-angles-degrees-to-time}} \tabularnewline
+\toprule 
+Unit of Angle & Equivalent time \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Relationship of Angles (degrees) to Time} \tabularnewline
+\toprule 
+Unit of Angle & Equivalent time \tabularnewline
+\midrule
+\endhead
+
+1 radian & 3.819719 hours \tabularnewline
+1 degree & 4 minutes \tabularnewline
+1 arcmin & 4 seconds \tabularnewline
+1 arcsec & 0.066667 seconds \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{\texorpdfstring{Site Rain Status {[]}}{Site Rain Status }}\label{site-rain-status}
+
+This field shows whether or not (1 = yes, 0 = no) the weather shows ``raining''. For a Design Day, one can denote rain for the entire day but not timestep by timestep. Weather files may indicate rain for a single time interval. This is an ``averaged'' field -- thus a 1 shown for a time period (e.g. daily reporting) means that it was raining during each timestep of that period.
+
+\paragraph{\texorpdfstring{Site Snow on Ground Status {[]}}{Site Snow on Ground Status }}\label{site-snow-on-ground-status}
+
+This field shows whether or not (1 = yes, 0 = no) the weather shows ``snow on the ground''. For a Design Day, one can denote snow for the entire day but not timestep by timestep. Weather files may indicate snow (snow depth) for a single time interval. This is an ``averaged'' field -- thus a 1 shown for a time period (e.g. daily reporting) means that there was snow on the ground during each timestep of that period.
+
+\paragraph{\texorpdfstring{Site Daylight Saving Time Status {[]}}{Site Daylight Saving Time Status }}\label{site-daylight-saving-time-status}
+
+This field shows when daylight saving time (1 = yes, 0 = no) is in effect. Though shown as an average variable, this value is only set on a daily basis.
+
+\paragraph{\texorpdfstring{Site Day Type Index {[]}}{Site Day Type Index }}\label{site-day-type-index}
+
+This field shows what ``day type'' the current day is. Daytypes are (1 = Sunday, 2 = Monday, etc.) with Holiday = 8, SummerDesignDay = 9, WinterDesignDay = 10, CustomDay1 = 11, CustomDay2 = 12. Though shown as an average variable, this value is only set on a daily basis.
+
+\paragraph{Site Mains Water Temperature {[}C{]}}\label{site-mains-water-temperature-c}
+
+The value of the Water Mains Temperature is reported in C following the calculation shown in the Water Mains Temperature object.
+
+\paragraph{Site Precipitation Rate {[}m/s{]}}\label{site-precipitation-rate-ms}
+
+\paragraph{Site Precipitation Depth {[}m{]}}\label{site-precipitation-depth-m-1}
+
+The rate and quantity of precipitation at the site. These outputs are only available if a Site Precipication object is used. Precipitation is measured in meters.
+
+\paragraph{Water System Roof Irrigation Scheduled Depth{[}m{]}}\label{water-system-roof-irrigation-scheduled-depthm}
+
+This is the scheduled amount of irrigation for the green roof (ecoroof) based on the user input. Amount is measured in meters.
+
+\paragraph{Water System Roof Irrigation Actual Depth{[}m{]}}\label{water-system-roof-irrigation-actual-depthm}
+
+This is the actual amount of irrigation for the green roof (ecoroof) based on the scheduled user input and moisture state/saturation of the soil. Amount is measured in meters.
+
+\subsection{Outputs for local temperature/wind speed calculations}\label{outputs-for-local-temperaturewind-speed-calculations}
+
+Local atmospheric properties for outdoor air temperature and wind speed are separately calculated and reported for all zones, surfaces, and outdoor air nodes. The output variables are associated with their respective objects:
+
+\begin{itemize}
+\item
+  Zone,Average,Zone Outdoor Air Drybulb Temperature {[}C{]}
+\item
+  Zone,Average,Zone Outdoor Air Wetbulb Temperature {[}C{]}
+\item
+  Zone,Average,Zone Outdoor Air Wind Speed {[}m/s{]}
+\item
+  Zone,Average,Surface Ext Outdoor Dry Bulb {[}C{]}
+\item
+  Zone,Average,Surface Ext Outdoor Wet Bulb {[}C{]}
+\item
+  Zone,Average,Surface Ext Wind Speed {[}m/s{]}
+\item
+  HVAC,Average,System Node Temperature {[}C{]}~~~~~~~ (for OUTDOOR AIR NODE object)
+\end{itemize}
+
+\subsubsection{Zone Outdoor Air Drybulb Temperature {[}C{]}}\label{zone-outdoor-air-drybulb-temperature-c}
+
+The outdoor air dry-bulb temperature calculated at the height above ground of the zone centroid.
+
+\subsubsection{Zone Outdoor Air Wetbulb Temperature {[}C{]}}\label{zone-outdoor-air-wetbulb-temperature-c}
+
+The outdoor air wet-bulb temperature calculated at the height above ground of the zone centroid.
+
+\subsubsection{Zone Outdoor Air Wind Speed {[}m/s{]}}\label{zone-outdoor-air-wind-speed-ms}
+
+The outdoor wind speed calculated at the height above ground of the zone centroid.
+
+\subsubsection{Surface Ext Outdoor Dry Bulb {[}C{]}}\label{surface-ext-outdoor-dry-bulb-c}
+
+The outdoor air dry-bulb temperature calculated at the height above ground of the surface centroid.
+
+\subsubsection{Surface Ext Outdoor Wet Bulb {[}C{]}}\label{surface-ext-outdoor-wet-bulb-c}
+
+The outdoor air wet-bulb temperature calculated at the height above ground of the surface centroid.
+
+\subsubsection{Surface Ext Wind Speed {[}m/s{]}}\label{surface-ext-wind-speed-ms}
+
+The outdoor wind speed calculated at the height above ground of the surface centroid.
+
+\subsubsection{System Node Temperature {[}C{]}}\label{system-node-temperature-c}
+
+When reporting for the \textbf{OutdoorAir:Node} object, this is the outdoor air dry-bulb temperature calculated at the height above ground of the node, if height is specified in the input.
diff --git a/doc/input-output-reference/src/overview/group-node-branch-management.tex b/doc/input-output-reference/src/overview/group-node-branch-management.tex
new file mode 100644
index 00000000000..638eaf03e27
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+++ b/doc/input-output-reference/src/overview/group-node-branch-management.tex
@@ -0,0 +1,1240 @@
+\section{Group -- Node-Branch Management}\label{group-node-branch-management}
+
+\textbf{Nodes}, \textbf{Branch} \textbf{Lists} and \textbf{Branches} define the topography of the HVAC connections.
+
+\subsection{NodeList}\label{nodelist}
+
+For convenience, the NodeList object can be used to identify all the nodes for a particular use. A node list is not always required. The advantage of listing all the nodes in this manner is that input fields in other objects that ask for a node name can refer to either a single node or a list of nodes using this object. .
+
+There are other lines of input syntax that require the use of a NodeList as part of the input. These syntax items include: OutdoorAir:NodeList and the SetpointManager objects. In these two cases, the use of a NodeList statement is mandatory if there is more than one node in this particular ``list''. For example, if the outside air only has a single inlet node, then the name of that node can replace the node list name in the input syntax. As a result of this mandatory specification of node lists for certain types of input, nodes can, obviously, and may be members of more than one list.
+
+\subsubsection{Inputs}\label{inputs-027}
+
+\paragraph{Field: Name}\label{field-name-026}
+
+This alpha designation must be unique among all the Node List Names. It is used as reference in various objects (e.g.~OutdoorAir:NodeList).
+
+\paragraph{Field: Node \textless{}\#\textgreater{} Name ~(up to 25 allowed)}\label{field-node-name-up-to-25-allowed}
+
+Each unique Node identifier creates a Node structure with various attributes depending on the type of node. Typical values include Temperature, Mass Flow Rate, and Temperature Set Point. The alpha designators are associated with a particular node.
+
+Though each NodeList is limited to 25 nodes, several node lists may be entered if you choose to identify all the nodes up front. For example:
+
+\begin{lstlisting}
+NodeList, Nodes1-25,
+NODE_1,NODE_2,NODE_3,NODE_4,NODE_5,NODE_6,NODE_7,NODE_8,NODE_9,NODE_10,
+NODE_11,NODE_12,NODE_13,NODE_14,NODE_15,NODE_16,NODE_17,NODE_18,NODE_19,NODE_20,
+NODE_21,NODE_22,NODE_23,NODE_24,NODE_25;
+NodeList, Nodes26-49,NODE_26,NODE_27,NODE_28,NODE_29,NODE_30,
+NODE_31,NODE_32,NODE_33,NODE_34,NODE_35,NODE_36,NODE_37,NODE_38,NODE_39,NODE_40,
+NODE_41,NODE_42,NODE_43,NODE_44,NODE_45,NODE_46,NODE_47,NODE_48,NODE_49;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-019}
+
+A simple detail of Nodes and numbers assigned appears in the \textbf{eplusout.bnd} file:
+
+\begin{lstlisting}
+! <Node>,<NodeNumber>,<Node Name>,<Node Fluid Type>,<\# Times Node Referenced After Definition>
+ Node,1,OUTSIDE AIR INLET NODE 1,Air,2
+ Node,2,VAV SYS 1 INLET NODE,Air,3
+ Node,3,MIXED AIR NODE 1,Air,5
+ Node,4,MAIN COOLING COIL 1 OUTLET NODE,Air,3
+ Node,5,MAIN HEATING COIL 1 OUTLET NODE,Air,4
+ Node,6,VAV SYS 1 OUTLET NODE,Air,7
+\end{lstlisting}
+
+In addition, properties of each node is available during the simulation:
+
+\begin{itemize}
+\item
+  HVAC,Average,System Node Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Last Timestep Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,System Node Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,System Node Setpoint Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Setpoint High Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Setpoint Low Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Setpoint Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,System Node Setpoint Minimum Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,System Node Setpoint Maximum Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,System Node Relative Humidity {[}\%{]}
+\item
+  HVAC,Average,System Node Pressure {[}Pa{]}
+\item
+  HVAC,Average,System Node Standard Density Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,System Node Enthalpy {[}J/kg{]}
+\item
+  HVAC,Average,System Node Last Timestep Enthalpy {[}J/kg{]}
+\item
+  HVAC,Average,System Node Wetbulb Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Dewpoint Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Quality {[]}
+\item
+  HVAC,Average,System Node Height {[}m{]}
+\item
+  HVAC,Average,System Node Specific Heat {[}J/kg-K{]}
+\end{itemize}
+
+\textbf{The following node variable is also available for system nodes that are for ``air'':}
+
+\begin{itemize}
+\item
+  HVAC, Average, System Node Current Density Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC, Average, System Node Current Density {[}kg/m3{]}
+\end{itemize}
+
+\textbf{The following node variables are ``advanced'' and normally used for debugging unusual cases:}
+
+\begin{itemize}
+\item
+  HVAC,Average,System Node Minimum Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Maximum Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Minimum Limit Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,System Node Maximum Limit Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,System Node Minimum Available Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,System Node Maximum Available Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Averge,System Node Requested Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,System Node Setpoint Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\textbf{The following node variable reports node carbon dioxide concentration when carbon dioxide is simulated (ref. ZoneAirContaminantBalance):}
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,System Node CO2 Concentration {[}ppm{]}
+\end{itemize}
+
+\textbf{The following node variable reports node generic contaminant concentration when generic contaminant is simulated (ref. ZoneAirContaminantBalance):}
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,System Node Generic Air Contaminant Concentration {[}ppm{]}
+\end{itemize}
+
+\paragraph{System Node Temperature {[}C{]}}\label{system-node-temperature-c-000}
+
+The current temperature at a system node in degrees C. For air nodes, this is the dry-bulb temperature.
+
+\paragraph{System Node Last Timestep Temperature {[}C{]}}\label{system-node-last-timestep-temperature-c}
+
+The temperature at a system node for the previous timestep.
+
+\paragraph{System Node Mass Flow Rate {[}kg/s{]}}\label{system-node-mass-flow-rate-kgs}
+
+The current mass flow rate at a system node in kg/s.
+
+\paragraph{System Node Humidity Ratio {[}kgWater/kgDryAir{]}}\label{system-node-humidity-ratio-kgwaterkgdryair}
+
+The current humidity ratio at a system node in kg-water/kg-dry-air. Not applicable for liquid nodes.
+
+\paragraph{System Node Setpoint Temperature {[}C{]}}\label{system-node-setpoint-temperature-c}
+
+The current setpoint temperature at a system node in degrees C. Some controllers and equipment types sense this single setpoint.
+
+\paragraph{System Node Setpoint High Temperature {[}C{]}}\label{system-node-setpoint-high-temperature-c}
+
+The current upper setpoint temperature at a system node in degrees C. Some controllers and equipment types use dual setpoints at a single node.
+
+\paragraph{System Node Setpoint Low Temperature {[}C{]}}\label{system-node-setpoint-low-temperature-c}
+
+The current upper setpoint temperature at a system node in degrees C. Some controllers and equipment types use dual setpoints at a single node.
+
+\paragraph{System Node Setpoint Humidity Ratio {[}kgWater/kgDryAir{]}}\label{system-node-setpoint-humidity-ratio-kgwaterkgdryair}
+
+The current humidity ratio setpoint at a system node in kg-water/kg-dry-air. Some controllers and equipment types sense this single setpoint. Not applicable for liquid nodes.
+
+\paragraph{System Node Setpoint Minimum Humidity Ratio {[}kgWater/kgDryAir{]}}\label{system-node-setpoint-minimum-humidity-ratio-kgwaterkgdryair}
+
+The current minimum desired humidity ratio at a system node in kg-water/kg-dry-air. Some controllers and equipment types use the min/max values as dual setpoints at a single node. Not applicable for liquid nodes.
+
+\paragraph{System Node Setpoint Maximum Humidity Ratio {[}kgWater/kgDryAir{]}}\label{system-node-setpoint-maximum-humidity-ratio-kgwaterkgdryair}
+
+The current maximum desired humidity ratio at a system node in kg-water/kg-dry-air. Some controllers and equipment types use the min/max values as dual setpoints at a single node. Not applicable for liquid nodes.
+
+\paragraph{System Node Relative Humidity {[}\%{]}}\label{system-node-relative-humidity}
+
+The current relative humidity (calculated from the node temperature, node humidity ratio and standard barometric pressure for the location). Not applicable for liquid nodes.
+
+\paragraph{System Node Pressure {[}Pa{]}}\label{system-node-pressure-pa}
+
+The current pressure at a system node in Pa.
+
+\paragraph{\texorpdfstring{System Node Standard Density Volume Flow Rate {[}m\(^{3}\)/s{]}}{System Node Standard Density Volume Flow Rate {[}m\^{}\{3\}/s{]}}}\label{system-node-standard-density-volume-flow-rate-m3s}
+
+The current volume flow rate at a system node in m\(^{3}\)/s.~ This is report is calculated from the mass flow using standardized values for density that do not vary over time (except for steam which varies with quality).~ For water nodes this density is determined at a temperature of 5.05ºC.~ For air nodes this density is determined for dry air at the standard barometric pressure for the location's elevation, and a temperature of 20.0ºC.~ For air nodes, also see the report ``System Node Current Density Volume Flow Rate.''
+
+\paragraph{System Node Enthalpy {[}J/kg{]}}\label{system-node-enthalpy-jkg}
+
+The current enthalpy at a system node in J/kg.
+
+\paragraph{System Node Last Timestep Enthalpy {[}J/kg{]}}\label{system-node-last-timestep-enthalpy-jkg}
+
+The enthalpy at the system node for the previous timestep in Joules per kilogram.
+
+\paragraph{System Node Wetbulb Temperature {[}C{]}}\label{system-node-wetbulb-temperature-c}
+
+The current wet-bulb temperature at a system node in degrees C. Not applicable for liquid nodes.
+
+\paragraph{System Node Dewpoint Temperature {[}C{]}}\label{system-node-dewpoint-temperature-c}
+
+The current dewpoint temperature at a system node in degrees C. It is calculated from the System Node Temperature, the System Node Humidity Ratio and the Site Outdoor Air Barometric Pressure. Not applicable for liquid nodes.
+
+\paragraph{\texorpdfstring{System Node Quality {[]}}{System Node Quality }}\label{system-node-quality}
+
+The current system node vapor fraction/percent \{0.0-1.0\}.
+
+\paragraph{System Node Height {[}m{]}}\label{system-node-height-m}
+
+The current system node height \{m\}. Only applicable to outdoor air nodes.
+
+\paragraph{System Node Specific Heat {[}J/kg-K{]}}\label{system-node-specific-heat-jkg-k}
+
+The current specific heat capacity of the fluid at the node in units of J/kg-K. Not available for steam nodes.
+
+\textbf{Additional Node Reporting for Air Nodes}
+
+The following system node variable is available for nodes with a fluid type of air.
+
+\paragraph{\texorpdfstring{System Node Current Density Volume Flow Rate {[}m\(^{3}\)/s{]}}{System Node Current Density Volume Flow Rate {[}m\^{}\{3\}/s{]}}}\label{system-node-current-density-volume-flow-rate-m3s}
+
+The current volume flow rate at a system node in m\(^{3}\)/s based on the current density.~ This report differs from the one called ``System Node Standard Density Volume Flow Rate'' in that it uses an air density calculated for the current moist air conditions rather than a standard density.
+
+\paragraph{System Node Current Density {[}kg/m3{]}}\label{system-node-current-density-kgm3}
+
+The current air density at a system node in kg/m3.~ This is the density used to calculate the volume flow rate above.~ The density is calculated using current outdoor air barometric pressure and the drybulb temperature and humidity ratio at the air node.
+
+\textbf{Advanced Node Reporting}
+
+The following system node variables are available when you request ``Diagnostics, DisplayAdvancedReportVariable;''. They are normally used for debugging unusual system cases and may not be available for all systems. Also, their definitions may change based on the usage in the system.
+
+\paragraph{System Node Minimum Temperature {[}C{]}}\label{system-node-minimum-temperature-c}
+
+\paragraph{System Node Maximum Temperature {[}C{]}}\label{system-node-maximum-temperature-c}
+
+These node variables represent the min/max of loops or branches.
+
+\paragraph{System Node Minimum Limit Mass Flow Rate {[}kg/s{]}}\label{system-node-minimum-limit-mass-flow-rate-kgs}
+
+\paragraph{System Node Maximum Limit Mass Flow Rate {[}kg/s{]}}\label{system-node-maximum-limit-mass-flow-rate-kgs}
+
+These node variables hold the maximum possible and the minimum allowable flow rates for a particular component. As such, they represent the ``hardware limit'' on the flow rate for the component. By convention, these variables are stored at the component inlet node. Since components share their nodes (the outlet node of one component is the inlet node of the next component), the protocol must be strictly followed. These variables are set by each component based on the design flow limits of the equipment.
+
+\paragraph{System Node Minimum Available Mass Flow Rate {[}kg/s{]}}\label{system-node-minimum-available-mass-flow-rate-kgs}
+
+\paragraph{System Node Maximum Available Mass Flow Rate {[}kg/s{]}}\label{system-node-maximum-available-mass-flow-rate-kgs}
+
+These node variables represent the \emph{loop} or \emph{branch} maximum and minimum flow rate for the current configuration of the loop on which the component resides. The central plant routines manage these variables dynamically to resolve flow rates through branches located inside splitters and mixers.
+
+\paragraph{System Node Setpoint Mass Flow Rate {[}kg/s{]}}\label{system-node-setpoint-mass-flow-rate-kgs}
+
+The current mass flow rate setpoint at a system node in kg/s. Some controllers and equipment types sense this single setpoint.
+
+\paragraph{System Node Requested Mass Flow Rate {[}kg/s{]}}\label{system-node-requested-mass-flow-rate-kgs}
+
+This output is the current mass flow rate request at a system node in kg/s.~ Only used for plant simulations and nodes.~ This is the mass flow rate ``requested'' by a component.~ This is a record of what the component wanted which can be useful for diagnostics when the actual simulated flow is different than expected.~ This value is also used to determine overall loop flow rates.
+
+\paragraph{System Node CO2 Concentration {[}ppm{]}}\label{system-node-co2-concentration-ppm}
+
+The average carbon dioxide concentration, in parts per million (ppm), at a system node for the timestep being reported.
+
+\paragraph{System Node Generic Air Contaminant Concentration {[}ppm{]}}\label{system-node-generic-air-contaminant-concentration-ppm}
+
+The average generic contaminant concentration, in parts per million (ppm), at a system node for the timestep being reported.
+
+\subsection{BranchList}\label{branchlist}
+
+A branch list is intended to define the branches or portions of a particular loop that are present on an individual plant or condenser loop. Thus, the BranchList syntax simply provides a list of branch names (see Branch syntax) that then refer to more detailed syntax in another part of the input file. The syntax for describing a list of branches is given below.
+
+Branches in BranchList objects should be listed in flow order: inlet branch, then parallel branches, then outlet branch. Branches (within a splitter/mixer) are simulated in the order listed.
+
+\subsubsection{Inputs}\label{inputs-1-025}
+
+\paragraph{Field: Name}\label{field-name-1-024}
+
+A unique name to identify the branch list.
+
+\paragraph{Field: Branch \textless{}\#\textgreater{} Name}\label{field-branch-name}
+
+Branch name in the list.~ As noted above, Branches in BranchList objects MUST be listed in flow order: inlet branch, then parallel branches, then outlet branch. Branches are simulated in the order listed.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+BranchList, Cooling Supply Side Branches,
+       CW Pump Branch,
+       Little Chiller Branch,
+       Big Chiller Branch,
+       Purchased Cooling Branch,
+       Supply Bypass Branch,
+       Cooling Supply Outlet;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-016}
+
+No output directly related to Branch Lists current is presented.
+
+\subsection{Branch}\label{branch}
+
+Branches can be considered the mid-level grouping of items in the EnergyPlus HVAC loop scheme. Components are the lowest level of information. A collection of components in series forms a branch. Every branch must have at least one component, but it may have several components in series. The air loop also has ``unitary'' objects that are compound objects that wrap components and when they are used it is the unitary objects that appear on the Branch and not the child components.~ The \textbf{Branch} defines the order that components appear on the branch. Moreover, a collection of branches and their connecting information form a loop. Therefore, a branch is a collection of components while a loop is a collection of branches. Thus, components are specified for particular HVAC loops by assigning them to branches and then connecting those branches together to form a loop.
+
+For hydronic plant systems, the Branch object is used on both the demand side and the supply side of the plant loop.~ For HVAC air systems, the Branch object is only used to describe the components on the supply side of an air loop. The demand side of the air loop does not use the Branch object.~ The outside air system appears on a Branch object but it does not use a Branch object itself to describe the components that included in the outside air system.~ So-called ``ZoneHVAC:*'' equipment, HVAC equipment directly associated with a zone, do not use the Branch object.
+
+It should be noted that each component also has at least two nodes associated with it---an inlet node and an outlet node. These nodes, by default, are also part of the branch to which their components are assigned.~ Although it may appear redundant to list the node names in both the Branch and in the component object being referenced, this is needed because many components are connected to more than one loop at a time and the node names are needed here to distinguish which portion of the component is being attached to this particular branch and its loop.~ It should be noted that each branch must have at least one component on it. A ``null'' branch such as one where the first component on the loop is in reality a splitter or mixer should be defined as a single Pipe component for plant, or a single Duct component for air systems.
+
+\subsubsection{Inputs}\label{inputs-2-023}
+
+\paragraph{Field: Name}\label{field-name-2-022}
+
+This alpha field is the unique, user-defined name that allows the branch to be referenced by other elements such as the PlantLoop and CondenserLoop statements.
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate-001}
+
+This field is the maximum flow rate (m\(^{3}\)/sec) allowed on a particular branch. This number will set an absolute maximum flow rate for all components on the loop. Even if components are defined with a higher flow rate, EnergyPlus will limit the flow on this particular branch to the value entered here by the user. Currently this is used in the Air Loop and is not a required field in the Plant and Condenser Loop. The example files for the Plant and Condenser Loops leave this field blank to simplify flow input.
+
+\paragraph{Field: Pressure Drop Curve Name}\label{field-pressure-drop-curve-name}
+
+This is an optional field used to specify pressure drop information for this particular branch. Currently this is only available in plant/condenser fluid loops: PlantLoop and CondenserLoop. Air loops require a full airflow network, so this field is ignored if found on an air loop. The value entered for this field must match a pressure curve object also found in the input. This curve can be of the type: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Exponent, or Curve:Functional:PressureDrop. In order to then perform a pressure simulation for the loop that this branch is located on, a flag must be set in the loop object. Reference the PlantLoop and CondenserLoop field ``Pressure Simulation Type'' for allowable settings. See the Engineering Reference document for further information on pressure simulation in plant loops.
+
+\paragraph{Field Set (Branch Specifications)}\label{field-set-branch-specifications}
+
+Following the two introductory items, there are groups of 5 repeated items: a type, a name, inlet and outlet node names, and a branch control type. All of these items refer to one particular component on the branch. The first component defined by these items will be the first component on this branch, etc. through the end of the list.~ This object is extensible and can use as many field sets as needed.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Object Type}\label{field-component-object-type-000}
+
+This field is the component object type (object class name). The component type refers to other elements within the input file and specifies what kind of component this is. The objects in the~ Group -- Plant Equipment section are valid here when the Branch is used in Plant specifications. Fans, coils, unitary systems, and Outside Air Systems are also valid component types for the Branch object. Pipes or Ducts are also valid for this field.~ No splitter or mixer type objects are allowed.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Name}\label{field-component-name-001}
+
+The component name is the unique, user-defined reference name to distinguish between potentially multiple occurrences of a particular component type in an input file. The set of component type and component name must be unique. (You can only have 1 Boiler object with name MYBOILER).
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Inlet Node Name}\label{field-component-inlet-node-name}
+
+This field references an inlet node name that will be found in the actual component specification.~ The inlet node, and the outlet node specified in the next field, should correspond to component model's connections that are intended for the loop that this Branch is assigned to.~ For example a water-cooled chiller will have two inlet nodes, one for chilled water return and one for condenser water return and so the chiller will appear on two Branch objects accordingly.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Outlet Node Name}\label{field-component-outlet-node-name}
+
+This field references an outlet node name that will be found in the actual component specification.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Branch Control Type}\label{field-component-branch-control-type}
+
+This field is being deprecated and is no longer used or required. Prior to version 7 it was used by plant to resolve branch flow rates but now this is handled automatically by the program.~ The field will be removed in a future version.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Branch,
+      Air Loop Main Branch,    !- Branch Name
+      1.75,                    !- Maximum Branch Flow Rate {m3/s}
+      ,                        !- Pressure Drop Curve Name
+      AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass,  !- Comp1 Type
+      GasHeat CBVAV System,    !- Comp1 Name
+      Air Loop Inlet Node,     !- Comp1 Inlet Node Name
+      Air Loop Outlet Node,    !- Comp1 Outlet Node Name
+      ;                  !- Comp1 Branch Control Type
+\end{lstlisting}
+
+And a more complex one:
+
+\begin{lstlisting}
+
+  BRANCH,
+      Air Loop Main Branch,    !- Branch Name
+      1.3,                     !- Maximum Branch Flow Rate {m3/s}
+      ,                        !- Pressure Drop Curve Name
+      FAN:SIMPLE:ConstVolume,  !- Comp1 Type
+      Supply Fan 1,            !- Comp1 Name
+      Air Loop Inlet Node,     !- Comp1 Inlet Node Name
+      Cooling Coil Air Inlet Node,  !- Comp1 Outlet Node Name
+      ,                  !- Comp1 Branch Control Type
+      COIL:Water:DetailedFlatCooling,  !- Comp2 Type
+      Detailed Cooling Coil,   !- Comp2 Name
+      Cooling Coil Air Inlet Node,  !- Comp2 Inlet Node Name
+      Air Loop Outlet Node,    !- Comp2 Outlet Node Name
+      ;                 !- Comp2 Branch Control Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-014}
+
+The components on a branch are in series and that list is in simulation and connection order. Each branch must obey the rules: the outlet for component 1 has to have the same node name as the inlet for component 2, and so forth.
+
+Eplusout.err contains the test for ``individual branch integrity'':
+
+\begin{lstlisting}
+   ************* Testing Individual Branch Integrity
+   ************* Testing Branch = AIR LOOP MAIN BRANCH
+   ************* ....passed
+   ************* Testing Branch = COOLING DEMAND INLET
+   ************* ....passed
+   ************* Testing Branch = COOLING COIL BRANCH
+   ************* ....passed
+   ************* Testing Branch = DEMAND BYPASS BRANCH
+   ************* ....passed
+   ************* Testing Branch = COOLING DEMAND OUTLET
+   ************* ....passed
+   ************* Testing Branch = COOLING SUPPLY OUTLET
+   ************* ....passed
+\end{lstlisting}
+
+The addition of pressure simulation for branches in fluid loops brings a new output at the branch level:
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Plant Branch Pressure Difference {[}Pa{]}
+\end{itemize}
+
+\paragraph{Plant Branch Pressure Difference {[}Pa{]}}\label{plant-branch-pressure-difference-pa}
+
+This field allows the user to output the pressure drop of a particular branch on a plant loop or condenser loop. This output is only recognized if a valid pressure simulation is being performed. To do this, the user must specify a pressure simulation type as an input in the PlantLoop or CondenserLoop object.
+
+\subsection{ConnectorList}\label{connectorlist}
+
+A connector list is a collection of either one or two connection devices (Connector:Mixer or Connector:Splitter). Due to the definition of a loop in EnergyPlus, there is a maximum of one mixer and one splitter allowed for each loop segment. This limitation still allows a tremendous amount of flexibility to the user and can also still be solved within a reasonable amount of time and without a complex solver routine. The connection list simply allows the specification of the types and names of these devices. This allows the main loop statements to have the flexibility to have multiple lists that can have one or more item.
+
+\subsubsection{Inputs}\label{inputs-3-021}
+
+\paragraph{Field: Name}\label{field-name-3-019}
+
+This field is an identifying name that will be referenced to main loop statements using this connector list. The name must be unique among connector list names.
+
+\paragraph{Field-Set: Connection Object Type and Identifying Name (up to 2 allowed)}\label{field-set-connection-object-type-and-identifying-name-up-to-2-allowed}
+
+Depending on the loop, either one or two of the connectors will be specified. If this particular loop only has a single connector (either Connector:Mixer or Connector:Splitter), then only the first two items (type of connection and identifying name of connector) are included. If both a mixer and splitter are present, the additional type of connection and identifying name must be included. Note that the order that the items appear is inconsequential---either the Connector:Mixer or the Connector:Splitter may appear first. This will not affect the simulation.
+
+\paragraph{Field: Connector 1 Object Type}\label{field-connector-1-object-type}
+
+This field contains the connector type \textbf{Connector:Mixer} or \textbf{Connector:Splitter}.
+
+\paragraph{Field: Connector 1 Name}\label{field-connector-1-name}
+
+This field is an identifying name for the connector. It will be used by other objects in the input file.
+
+\paragraph{Field: Connector 2 Object Type (optional)}\label{field-connector-2-object-type-optional}
+
+This field contains the connector type \textbf{Connector:Mixer} or \textbf{Connector:Splitter}.
+
+\paragraph{Field: Connector 2 Name (optional)}\label{field-connector-2-name-optional}
+
+This field is an identifying name for the connector. It will be used by other objects in the input file.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+ConnectorList LIST, Cooling Supply Side Connectors,
+      Connector:Splitter, CW Loop Splitter,
+      Connector:Mixer, CW Loop Mixer;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-012}
+
+No output directly related to Connector Lists is currently presented.
+
+\subsection{Pipe:Adiabatic}\label{pipeadiabatic}
+
+In reality, every component is connected to its closest neighbors via a pipe or a duct. At the current time, such detail is not needed in EnergyPlus. Thus, the Pipe:Adiabatic component is currently used more as a connection device (for branches that really do not have any components associated with them) or as a bypass than anything else. As such, its input is very simple and its algorithm is equally simple. The current algorithm for a pipe is simply to pass the inlet conditions to the outlet of the pipe component.
+
+\subsubsection{Inputs}\label{inputs-4-019}
+
+\paragraph{Field: Name}\label{field-name-4-016}
+
+This alpha field is used as an identifying field for the pipe.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-001}
+
+This alpha field is used as an identifying field for the pipe inlet node.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-002}
+
+This alpha field is used as an identifying field for the pipe outlet node.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Pipe:Adiabatic,
+      Demand Side Inlet Pipe,
+      CW Demand Inlet Node,
+      CW Demand Entrance Pipe Outlet Node;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-009}
+
+There are no outputs directly related to Pipes.
+
+\subsection{Pipe:Adiabatic:Steam}\label{pipeadiabaticsteam}
+
+To connect the various components in a steam system regardless of it being the condensate or the steam side of the loop steam pipe needs to be used. In reality, every component is connected to its closest neighbors via a pipe or a duct. At the current time, such detail is not needed in EnergyPlus. Thus, the Pipe:Adiabatic:Steam component is currently used more as a connection device (for branches that really do not have any components associated with them). As such, its input is very simple and its algorithm is equally simple. The current algorithm for a pipe is simply to pass the inlet conditions to the outlet of the pipe component.
+
+\subsubsection{Inputs}\label{inputs-5-017}
+
+\paragraph{Field: Name}\label{field-name-5-013}
+
+This alpha field is used as an identifying field for the steam pipe.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-1-000}
+
+This alpha field is used as an identifying field for the steam pipe inlet node.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-1-001}
+
+This alpha field is used as an identifying field for the steampipe outlet node.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Pipe:Adiabatic:Steam,
+      Steam Demand 1 Steam Inlet Pipe,            !- PipeName
+      Steam Demand 1 Steam Demand Inlet Node,     !- Inlet Node Name
+      Steam Demand 1 Steam Demand Entrance Pipe Outlet Node;  !- Outlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-005}
+
+There are no outputs directly related to Steam Pipes.
+
+\subsection{Pipe:Indoor}\label{pipeindoor}
+
+This object specifies inputs which are used to simulate the heat transfer from a plant loop pipe placed in a zone or when a user schedule is used to specify an environment.
+
+The data definition for object is shown below.
+
+\subsubsection{Inputs}\label{inputs-6-014}
+
+\paragraph{Field: Name}\label{field-name-6-011}
+
+This alpha field is used as an identifying field for the pipe.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-002}
+
+This alpha field references a `wall' construction object that gives a layer-by-layer description of the pipe wall and its insulation.~ The construction object follows standard conventions, describing material properties for each layer beginning with the outermost insulation layer and ending with the pipe wall layer.
+
+\paragraph{Field: Fluid Inlet Node Name}\label{field-fluid-inlet-node-name-000}
+
+This alpha field contains the name of the pipe fluid inlet node.
+
+\paragraph{Field: Fluid Outlet Node Name}\label{field-fluid-outlet-node-name-000}
+
+This alpha field contains the name of the pipe fluid outlet node.
+
+\paragraph{Field: Environment Type}\label{field-environment-type}
+
+Environment type is the environment in which the pipe is placed. It can be either \textbf{Zone} or \textbf{Schedule}. If specified as Zone, a zone name must be specified in the next field. If specified as Schedule, the Ambient Temperature Zone can be left blank, while a schedule must be specified for the temperature and air velocity.
+
+\paragraph{Field: Ambient Temperature Zone Name}\label{field-ambient-temperature-zone-name}
+
+If \textbf{Zone} is specified as the environment type, this field is used to specify the name of the zone in which the pipe is located.~ The zone temperature is used to calculate the heat transfer rate from the pipe.
+
+\paragraph{Field: Ambient Temperature Schedule Name}\label{field-ambient-temperature-schedule-name}
+
+If \textbf{Schedule} is specified as the environment type, this field is used to specify the name of the temperature schedule that gives the ambient air temperature surrounding the pipe.~ This temperature is used as the outside boundary condition to calculate heat transfer from the pipe.
+
+\paragraph{Field: Ambient Air Velocity Schedule Name}\label{field-ambient-air-velocity-schedule-name}
+
+If \textbf{Schedule} is specified as the environment type, this field is used to specify the name of the velocity schedule that gives the air velocity near the pipe.~ This velocity is used to calculate the convection heat transfer coefficient used in the pipe heat transfer calculation.
+
+\paragraph{Field: Pipe Inside Diameter}\label{field-pipe-inside-diameter-000}
+
+This field is used to enter the inside diameter of the pipe in units of m. Pipe inside diameter must be a positive number.
+
+\paragraph{Field: Pipe Length}\label{field-pipe-length-000}
+
+This field is used to enter the length of the pipe in units of m. Pipe length must be a positive number.
+
+An example of this object in an IDF is:
+
+\begin{lstlisting}
+
+Pipe:Indoor,
+      Pipe Heat Transfer Towers,    !- name of outside panel heat exchanger
+      Insulated Pipe,                      !- Construction name
+      Condenser Tower Outlet Node,  !- Comp1 Inlet Node Name
+      HTPipe Outlet Node,           !- Comp1 Outlet Node Name
+      Water,                               !- Fluid name
+      Zone,                         !- field Ambient Temperature Outside Air Node name
+      0.05,                                !- Pipe Inside Diameter (thickness in construction data)
+      100.0;                               !- pipe length
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-005}
+
+\begin{itemize}
+\item
+  HVAC,Average, Pipe Fluid Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average, Pipe Ambient Heat Transfer Rate {[}W{]}
+\item
+  HVAC,SUM, Pipe Fluid Heat Transfer Energy {[}J{]}
+\item
+  HVAC,SUM, Pipe Ambient Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Pipe Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average, Pipe Inlet Temperature {[}C{]}
+\item
+  HVAC,Average, Pipe Outlet Temperature {[}C{]}
+\item
+  HVAC,Average, Pipe Volume Flow Rate {[}m3/s{]}
+\end{itemize}
+
+\paragraph{Pipe Fluid Heat Transfer Rate {[}W{]}}\label{pipe-fluid-heat-transfer-rate-w}
+
+The output provides the total amount of heat loss/gain in the fluid from pipe inlet to outlet.
+
+\paragraph{Pipe Ambient Heat Transfer Rate {[}W{]}}\label{pipe-ambient-heat-transfer-rate-w}
+
+The output provides the amount of heat loss/gain from pipe wall to the environment.
+
+\paragraph{Pipe Fluid Heat Transfer Energy {[}J{]}}\label{pipe-fluid-heat-transfer-energy-j}
+
+Total energy fluid has lost/gained between pipe inlet and outlet. It is metered on EnergyTransfer with an end use of Pipes.
+
+\paragraph{Pipe Ambient Heat Transfer Energy {[}J{]}}\label{pipe-ambient-heat-transfer-energy-j}
+
+Total energy lost from the external pipe surface.
+
+\paragraph{Pipe Mass Flow Rate {[}kg/s{]}}\label{pipe-mass-flow-rate-kgs}
+
+Mass flow rate of the fluid in the pipe.
+
+\paragraph{Pipe Inlet Temperature {[}C{]}}\label{pipe-inlet-temperature-c}
+
+\paragraph{Pipe Outlet Temperature {[}C{]}}\label{pipe-outlet-temperature-c}
+
+Temperature of fluid at entering and exiting of pipe.
+
+\paragraph{Pipe Volume Flow Rate {[}m3/s{]}}\label{pipe-volume-flow-rate-m3s}
+
+Fluid volumetric flow rate, (mass flow rate / density)
+
+\subsection{Pipe:Outdoor}\label{pipeoutdoor}
+
+This object specifies inputs which are used to simulate the heat transfer from a plant loop pipe placed in an outdoor environment.
+
+\subsubsection{Inputs}\label{inputs-7-014}
+
+\paragraph{Field: Name}\label{field-name-7-010}
+
+This alpha field is used as an identifying field for the pipe.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-1-000}
+
+This alpha field references a `wall' construction object that gives a layer-by-layer description of the pipe wall and its insulation.~ The construction object follows standard conventions, describing material properties for each layer beginning with the outermost insulation layer and ending with the pipe wall layer.
+
+\paragraph{Field: Fluid Inlet Node Name}\label{field-fluid-inlet-node-name-1-000}
+
+This alpha field contains the name of the pipe fluid inlet node.
+
+\paragraph{Field: Fluid Outlet Node Name}\label{field-fluid-outlet-node-name-1-000}
+
+This alpha field contains the name of the pipe fluid outlet node.
+
+\paragraph{Field: Ambient Temperature Outside Air Node Name}\label{field-ambient-temperature-outside-air-node-name}
+
+Ambient temperature outdoor air node is a node representing outdoor air with which pipe transfers heat. The node should be included in an outdoor air node list.
+
+\paragraph{Field: Pipe Inside Diameter}\label{field-pipe-inside-diameter-1}
+
+This field is used to enter the inside diameter of the pipe in units of m. Pipe inside diameter must be a positive quantity.
+
+\paragraph{Field: Pipe Length}\label{field-pipe-length-1}
+
+This field is used to enter the length of the pipe in units of m. Pipe length must be a positive~~ quantity.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Pipe:Outdoor,
+      Pipe Heat Transfer Towers,    !- name of outside panel heat exchanger
+      Insulated Pipe,                      !- Construction name
+      Condenser Tower Outlet Node, !- Comp1 Inlet Node Name
+      HTPipe Outlet Node,           !- Comp1 Outlet Node Name
+      Water,                               !- Fluid name
+      PipeHeatTransfer Inlet Node,     !- field Ambient Temperature Outside Air Node name
+      0.05,                         !- Pipe Inside Diameter (thickness given in construction data)
+      100.0;                               !- pipe length
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-005}
+
+\begin{itemize}
+\item
+  HVAC,Average, Pipe Fluid Heat Transfer Rate {[}W{]}
+\item
+  HVAC,SUM, Pipe Fluid Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Pipe Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average, Pipe Inlet Temperature {[}T{]}
+\item
+  HVAC,Average, Pipe Outlet Temperature {[}T{]}
+\item
+  HVAC,Average, Pipe Volume Flow Rate {[}m3/s{]}
+\end{itemize}
+
+\paragraph{Pipe Fluid Heat Transfer Rate {[}W{]}}\label{pipe-fluid-heat-transfer-rate-w-1}
+
+The output provides the total amount of heat loss/gain in the fluid from pipe inlet to outlet.
+
+\paragraph{Pipe Fluid Heat Transfer Energy {[}J{]}}\label{pipe-fluid-heat-transfer-energy-j-1}
+
+Total energy fluid has lost/gained between pipe inlet and outlet. It is metered on EnergyTransfer with an end use of Pipes.
+
+\paragraph{Pipe Mass Flow Rate {[}kg/s{]}}\label{pipe-mass-flow-rate-kgs-1}
+
+Mass flow rate of the fluid in the pipe.
+
+\paragraph{Pipe Inlet Temperature {[}C{]}}\label{pipe-inlet-temperature-c-1}
+
+\paragraph{Pipe Outlet Temperature {[}C{]}}\label{pipe-outlet-temperature-c-1}
+
+Temperature of fluid at entering and exiting of pipe.
+
+\paragraph{Pipe Volume Flow Rate {[}m3/s{]}}\label{pipe-volume-flow-rate-m3s-1}
+
+Fluid volumetric flow rate, (mass flow rate / density)
+
+\subsection{Pipe:Underground}\label{pipeunderground}
+
+This object specifies inputs which are used to simulate the heat transfer from a plant loop pipe placed underground.
+
+\subsubsection{Inputs}\label{inputs-8-012}
+
+\paragraph{Field: Name}\label{field-name-8-010}
+
+This alpha field is used as an identifying field for the pipe.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-2-000}
+
+~This alpha field references a basic construction object that gives a layer-by-layer description of the pipe wall and insulation. The construction object follows standard conventions, describing material properties for each layer beginning with the outermost layer, the insulation, if it exists, and ending with the pipe wall layer.~ The construction object may have either one or two layers.~ If only one, then the material must be the pipe wall.~ If two, then insulation is utilized.
+
+\paragraph{Field: Fluid Inlet Node Name}\label{field-fluid-inlet-node-name-2}
+
+~This alpha field contains the name of the pipe fluid inlet node.
+
+\paragraph{Field: Fluid Outlet Node Name}\label{field-fluid-outlet-node-name-2}
+
+~This alpha field contains the name of the pipe fluid outlet node.
+
+\paragraph{Field: Sun Exposure}\label{field-sun-exposure}
+
+~This alpha field allows the user to specify one of two options: NoSun or SunExposed.~ For SunExposed, the simulation includes diffuse and beam solar effects on the ground surface.~ For NoSun, no solar effects are included.
+
+\paragraph{Field: Pipe Inside Diameter}\label{field-pipe-inside-diameter-2}
+
+~This field is used to enter the inside diameter of the pipe in units of m. Pipe inside diameter must be a positive quantity.
+
+\paragraph{Field: Pipe Length}\label{field-pipe-length-2}
+
+~This field is used to enter the length of the pipe in units of \{m\}. Pipe length must be a positive quantity.
+
+\paragraph{Field: Soil Material Name}\label{field-soil-material-name}
+
+This references a Material object that contains the soil properties and thickness.~ Note that when defining the soil layer, the thickness should be the thickness of soil between the pipe wall and the ground surface.
+
+\paragraph{Field: Type of Undisturbed Ground Temperature Object}\label{field-type-of-undisturbed-ground-temperature-object-001}
+
+This is the type of undisturbed ground temperature object that is used to determine the ground temperature.
+
+\paragraph{Field: Name of Undisturbed Ground Temperature Object}\label{field-name-of-undisturbed-ground-temperature-object-001}
+
+This is the name of the undisturbed ground temperature object that is used to determine the ground temperature.
+
+An example of this object in an IDF is:
+
+\begin{lstlisting}
+
+Pipe:Underground,
+      Pipe Heat Transfer Towers,          !- Name of Pipe
+      Insulated Buried Pipe,              !- Construction Name
+      Condenser Tower Outlet Node,        !- Inlet Node Name
+      HTPipe Outlet Node,                 !- Outlet Node Name
+      Water,                              !- Fluid Name
+      SunExposed,                         !- Sun Exposure
+      0.05,                               !- Pipe Inside Diameter    
+      20.0,                               !- Pipe Length
+      Buried Pipe Soil,                   !- Soil Material
+      Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
+      KATemps;                            !- Name of Undisturbed Ground Temperature Object
+
+    Construction,
+      Insulated Buried Pipe,              !- Name
+      Buried Pipe Insulation,             !- Layer #1
+      Buried Pipe Steel;                  !- Layer #2
+
+    Material,
+      Buried Pipe Soil,                   !- Name
+      Smooth,                             !- Roughness
+      1.5,                                !- Thickness {m}
+      0.36,                               !- Conductivity {W/m-K}
+      2000.0,                             !- Density {kg/m3}
+      1200.0,                             !- Specific Heat {J/kg-K}
+      0.9,                                !- Thermal Absorptance
+      0.5,                                !- Solar Absorptance
+      0.5;                                !- Visible Absorptance
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8-004}
+
+\begin{itemize}
+\item
+  HVAC, Average, Pipe Fluid Heat Transfer Rate {[}W{]}
+\item
+  HVAC, SUM, Pipe Fluid Heat Transfer Energy {[}J{]}
+\item
+  HVAC, Average, Pipe Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Pipe Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC, Average, Pipe Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Pipe Outlet Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Pipe Fluid Heat Transfer Rate {[}W{]}}\label{pipe-fluid-heat-transfer-rate-w-2}
+
+The output provides the total amount of heat loss/gain in the fluid from pipe inlet to outlet.
+
+\paragraph{Pipe Fluid Heat Transfer Energy {[}J{]}}\label{pipe-fluid-heat-transfer-energy-j-2}
+
+Total energy fluid has lost/gained between pipe inlet and outlet. It is metered on
+
+EnergyTransfer with an end use of Pipes.
+
+\paragraph{Pipe Mass Flow Rate {[}kg/s{]}}\label{pipe-mass-flow-rate-kgs-2}
+
+~Mass flow rate of the fluid in the pipe.
+
+\paragraph{Pipe Volume Flow Rate {[}m3/s{]}}\label{pipe-volume-flow-rate-m3s-2}
+
+Fluid volumetric flow rate, (mass flow rate / density)
+
+\paragraph{Pipe Inlet Temperature {[}C{]}}\label{pipe-inlet-temperature-c-2}
+
+\paragraph{Pipe Outlet Temperature {[}C{]}}\label{pipe-outlet-temperature-c-2}
+
+Temperature of fluid at entrance and exit of pipe.
+
+\subsection{PipingSystem:Underground Class Objects}\label{pipingsystemunderground-class-objects}
+
+Objects in this class are used to simulate the heat transfer processes of a piping system placed underground, which may or may not be in contact with a number of zone surfaces.~ There are three related objects, all of which are prefixed with PipingSystem:Underground :
+
+\begin{itemize}
+\item
+  PipingSystem:Underground:Domain
+\item
+  PipingSystem:Underground:PipeCircuit
+\item
+  PipingSystem:Underground:PipeSegment
+\end{itemize}
+
+\subsection{PipingSystem:Underground:Domain}\label{pipingsystemundergrounddomain}
+
+This section documents the domain object, which is used to specify information for the overall ground domain, including thermal properties, mesh parameters, and surface interaction.
+
+\subsubsection{Inputs}\label{inputs-9-011}
+
+\paragraph{Field: Name}\label{field-name-9-010}
+
+This alpha field is used as an identifying field for the ground domain.
+
+\paragraph{Field: XMax, YMax, ZMax}\label{field-xmax-ymax-zmax}
+
+These numeric fields are used to specify the overall domain size, in each of the three Cartesian dimensions.~ The domain will be meshed from \{x, y, z\} = \{0, 0, 0\} to \{Xmax, Ymax, Zmax\}.
+
+Note that for this object, the x-z plane lies parallel to the ground surface, such that the y-dimension can be thought of as representing the burial depth.~ This is in contrast to the way building surface coordinates are defined with the x-y plane lying parallel to the ground.~ Also note that any pipe segments that end up being used in a ground domain will be placed axially in the z-dimension.~ Thus, pipe flow will always be in either the positive z or negative z direction.
+
+\paragraph{Field: X-Direction Mesh Density Parameter}\label{field-x-direction-mesh-density-parameter}
+
+This numeric integer field represents the number of cells to be placed between any two ``domain partitions'' during mesh development.~ A domain partition may be thought of as a basement wall/floor, or a pipe.~ Once these components are laid out in the domain, this field number of cells are placed between the partitions.~ Further information on this is found in the engineering reference manual.
+
+\paragraph{Field: X-Direction Mesh Type}\label{field-x-direction-mesh-type}
+
+This alpha field represents the type of mesh to create when placing cells between ``domain partitions.''~ Two options are available: ``uniform'' and ``symmetricgeometric.''~ For uniform, the cells are placed in the region with all cells having equal size.~ For symmetric-geometric, the cells are compressed toward the partitions so that there are more cells on either side of the mesh region.~ This can help focus computational intensity on the boundary areas where it is likely more desired.~ For symmetric-geometric mesh distribution, the mesh density parameter should be an even number to provide the symmetric condition.
+
+\paragraph{Field: X-Direction Geometric Coefficient}\label{field-x-direction-geometric-coefficient}
+
+This numeric field represents the compression of cell distribution if the x-direction mesh type is set to ``symmetricgeometric.''~ If the mesh type is uniform, this field is not interpreted.~ For symmetric geometric, a value in this field equal to 1 would result in a uniform distribution, while a value of 2 would provide a highly skewed distribution.
+
+\paragraph{Field: Y-Direction Mesh Density Parameter}\label{field-y-direction-mesh-density-parameter}
+
+See Field: X-Direction Mesh Density Parameter.
+
+\paragraph{Field: Y-Direction Mesh Type}\label{field-y-direction-mesh-type}
+
+See Field: X-Direction Mesh Type.
+
+\paragraph{Field: Y-Direction Geometric Coefficient}\label{field-y-direction-geometric-coefficient}
+
+See Field: X-Direction Geometric Coefficient.
+
+\paragraph{Field: Z-Direction Mesh Density Parameter}\label{field-z-direction-mesh-density-parameter}
+
+See Field: X-Direction Mesh Density Parameter.
+
+\paragraph{Field: Z-Direction Mesh Type}\label{field-z-direction-mesh-type}
+
+See Field: X-Direction Mesh Type.
+
+\paragraph{Field: Z-Direction Geometric Coefficient}\label{field-z-direction-geometric-coefficient}
+
+See Field: X-Direction Geometric Coefficient.
+
+\paragraph{Field: Soil Thermal Conductivity}\label{field-soil-thermal-conductivity-001}
+
+The thermal conductivity of the soil, in W/m-K.
+
+\paragraph{Field: Soil Density}\label{field-soil-density-001}
+
+The bulk density of the soil, in kg/m3.
+
+\paragraph{Field: Soil Specific Heat}\label{field-soil-specific-heat-001}
+
+The specific heat of dry soil, in J/kg-K.~ If moisture is defined in this object, moisture and freezing effects are accounted for by varying the specific heat value.
+
+\paragraph{Field: Soil Moisture Content Volume Fraction}\label{field-soil-moisture-content-volume-fraction-000}
+
+A nominal value of soil moisture content to be used when evaluating soil thermal properties.
+
+\paragraph{Field: Soil Moisture Content Volume Fraction at Saturation}\label{field-soil-moisture-content-volume-fraction-at-saturation-000}
+
+A nominal value of soil moisture content when the soil is saturated, this is used in evaluating thermal properties of freezing soil
+
+\paragraph{Field: Type of Undisturbed Ground Temperature Object}\label{field-type-of-undisturbed-ground-temperature-object-1-001}
+
+The type of undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
+
+\paragraph{Field: Name of Undisturbed Ground Temperature Object}\label{field-name-of-undisturbed-ground-temperature-object-1-001}
+
+The name of the undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
+
+\paragraph{Field: This Domain Includes Basement Surface Interaction}\label{field-this-domain-includes-basement-surface-interaction}
+
+A yes/no field stating whether zone surfaces should be coupled to this domain.
+
+\paragraph{Field: Width of Basement Floor in Ground Domain}\label{field-width-of-basement-floor-in-ground-domain}
+
+If this domain does include basement interaction, this represents the width of the domain cutaway to include the basement.~ In essence, this is the width of basement floor to include in the ground simulation.~ This width should \emph{include} the basement wall thickness.
+
+\paragraph{Field: Width of Basement Floor in Ground Domain}\label{field-width-of-basement-floor-in-ground-domain-1}
+
+If this domain does include basement interaction, this represents the depth of the domain cutaway to include the basement.~ In essence, this is the burial depth of the basement to include in the ground simulation.~ This depth should include the basement floor thickness.
+
+\paragraph{Field: Shift Pipe X Coordinates By Basement Width}\label{field-shift-pipe-x-coordinates-by-basement-width}
+
+If this domain does include basement interaction, this flag specifies whether the pipe segment X-values should then be shifted by the basement width.~ In essence, this specifies the reference point for pipe segment x-values: if NO then the reference is domain x = 0, if YES then the reference is the basement width point.
+
+\paragraph{Field: Name of Basement Wall Boundary Condition Model}\label{field-name-of-basement-wall-boundary-condition-model}
+
+The name of an OtherSideConditions model defined in the input file and referenced by the surfaces which should be included as ``wall surfaces'' for the basement interaction part of the ground heat transfer model.
+
+\paragraph{Field: Name of Basement Wall Boundary Condition Model}\label{field-name-of-basement-wall-boundary-condition-model-1}
+
+The name of an OtherSideConditions model defined in the input file and referenced by the surfaces which should be included as ``floor surfaces'' for the basement interaction part of the ground heat transfer model.
+
+\paragraph{Field: Convergence Criterion for the Outer Cartesian Domain Iteration Loop}\label{field-convergence-criterion-for-the-outer-cartesian-domain-iteration-loop}
+
+The maximum temperature deviation within any cell between one iteration and another to decide that the Cartesian domain has converged to within tolerance.~ A smaller value will improve accuracy and computation time.~ A smaller value should be accompanied by a higher number of iterations if maximum accuracy is desired.
+
+\paragraph{Field: Maximum Iterations in the Outer Cartesian Domain Iteration Loop}\label{field-maximum-iterations-in-the-outer-cartesian-domain-iteration-loop}
+
+The maximum number of iterations to make when performing temperature updates of the Cartesian coordinate system.~ The actual number of iterations made will of course depend on transient conditions and convergence tolerance.
+
+\paragraph{Field: Evapotranspiration Ground Cover Parameter}\label{field-evapotranspiration-ground-cover-parameter-000}
+
+Numeric field specifies the ground cover effects used in the evapotranspiration model at the ground surface heat balance. The values range from 0 (solid, nonpermeable ground surface) to 1.5 (wild growth).
+
+\paragraph{Field: Number of Pipe Circuits Entered for this Domain}\label{field-number-of-pipe-circuits-entered-for-this-domain}
+
+The number of pipe circuit objects which will be defined in the following fields.
+
+\paragraph{Field: Pipe Circuit 1 \{\ldots{} to N; extensible\}}\label{field-pipe-circuit-1-to-n-extensible}
+
+A PipingSystem:Underground:PipeCircuit to be included in this domain.~ This indicates that the pipe circuit and all of the underlying pipe segments will be included during mesh development and heat transfer calculations within this domain.~ Any number of pipe circuits can be added, assuming all underlying pipe segments do not cause any conflicts for the mesh development engine (overlapping pipes, etc.).
+
+\subsection{PipingSystem:Underground:PipeCircuit}\label{pipingsystemundergroundpipecircuit}
+
+This section documents the pipe circuit object, which is used to specify information for the plant loop topology, such as inlet and outlet connections.~ This object also groups together pipe segments to define flow paths within a given pipe circuit.
+
+\subsubsection{Inputs}\label{inputs-10-010}
+
+\paragraph{Field: Name}\label{field-name-10-009}
+
+This alpha field is used as an identifying field for the pipe circuit.
+
+\paragraph{Field: Pipe Thermal Conductivity}\label{field-pipe-thermal-conductivity-001}
+
+~The thermal conductivity of the pipe, in W/m-K.
+
+\paragraph{Field: Pipe Density}\label{field-pipe-density-000}
+
+~The bulk density of the pipe, in kg/m3.
+
+\paragraph{Field: Pipe Specific Heat}\label{field-pipe-specific-heat-000}
+
+~The specific heat of the pipe, in J/kg-K.
+
+\paragraph{Field: Pipe Inner Diameter}\label{field-pipe-inner-diameter}
+
+~The inner diameter of the pipe, in m.
+
+\paragraph{Field: Pipe Outer Diameter}\label{field-pipe-outer-diameter}
+
+~The outer diameter of the pipe, in m.
+
+\paragraph{Field: Design Flow Rate}\label{field-design-flow-rate-001}
+
+~The ``design'' flow in this pipe circuit, in m3/s.~ This is the flow which this component will request during the simulation.~ Of course, other components and overall plant management will decide the flow actually given to this component.
+
+\paragraph{Field: Circuit Inlet Node Name}\label{field-circuit-inlet-node-name}
+
+~The inlet node name for this circuit, which is used when placing this circuit on a branch on a plant or condenser loop.
+
+\paragraph{Field: Circuit Outlet Node Name}\label{field-circuit-outlet-node-name}
+
+~The outlet node name for this circuit, which is used when placing this circuit on a branch on a plant or condenser loop.
+
+\paragraph{Field: Convergence Criterion for the Inner Radial Iteration Loop}\label{field-convergence-criterion-for-the-inner-radial-iteration-loop}
+
+~The maximum temperature deviation within any cell between one iteration and another to decide that the radial domain has converged to within tolerance.~ A smaller value will improve accuracy and computation time.~ A smaller value should be accompanied by a higher number of iterations if maximum accuracy is desired.
+
+\paragraph{Field: Maximum Iterations in the Inner Radial Iteration Loop}\label{field-maximum-iterations-in-the-inner-radial-iteration-loop}
+
+~The maximum number of iterations to make when performing temperature updates of the radial coordinate system.~ The actual number of iterations made will of course depend on transient conditions and convergence tolerance.
+
+\paragraph{Field: Number of Soil Nodes in the Inner Radial Near Pipe Mesh Region}\label{field-number-of-soil-nodes-in-the-inner-radial-near-pipe-mesh-region}
+
+~The number of soil nodes to discretize pipe cells.~ More information on mesh development is provided in the engineering reference manual.
+
+\paragraph{Field: Radial Thickness of Inner Radial Near Pipe Mesh Region}\label{field-radial-thickness-of-inner-radial-near-pipe-mesh-region}
+
+~The radial distance used to discretize pipe cells.~ More information on mesh development is provided in the engineering reference manual.
+
+\paragraph{Field: Number of Pipe Segments Entered for this Pipe Circuit}\label{field-number-of-pipe-segments-entered-for-this-pipe-circuit}
+
+~The number of pipe segment objects which will be defined in the following fields.
+
+\paragraph{Field: Pipe Segment 1 \{\ldots{} to N; extensible\}}\label{field-pipe-segment-1-to-n-extensible}
+
+~A PipingSystem:Underground:PipeSegment to be included in this pipe circuit.~ The circuit is set up so that flow passes through the \emph{N} segments in the order they are entered here.
+
+\subsection{PipingSystem:Underground:PipeSegment}\label{pipingsystemundergroundpipesegment}
+
+This section documents the pipe segment object, which is used to specify information for a single pipe segment placed at some x, y coordinate in the ground.~ The flow direction is also defined in this object to allow for careful description of varying flow paths.~ This can be useful for accounting for short circuiting effects if two pipes are placed in counterflow vs.~parallel flow.
+
+\subsubsection{Inputs}\label{inputs-11-009}
+
+\paragraph{Field: Name}\label{field-name-11-008}
+
+This alpha field is used as an identifying field for the pipe segment.
+
+\paragraph{Field: X Position}\label{field-x-position}
+
+This numeric field represents the x-direction placement of the pipe.~ If no basement is included in the simulation, this is measured from x = 0.~ If a basement is included, and the domain object specifies that pipes should be shifted, this is measured from the basement wall.
+
+\paragraph{Field: Y Position}\label{field-y-position}
+
+This numeric field represents the burial depth of the pipe, measured from the ground surface.~ This will always be a positive number.
+
+\paragraph{Field: Flow Direction}\label{field-flow-direction}
+
+This alpha field is used to define the flow direction within this pipe segment.~ The choices are ``increasing'' or ``decreasing.''~ These can be chosen carefully to encapsulate specific short-circuiting effects due to varying flow configurations (circuiting).
+
+An example of this object in an IDF is offered here for a foundation heat exchanger
+
+\begin{lstlisting}
+
+  PipingSystem:Underground:Domain,
+      My Piping System,        !- Name
+      12,                      !- Xmax
+      4.5,                     !- Ymax
+      36.84,                   !- Zmax
+      2,                       !- XMeshCount
+      Uniform,                 !- XMeshType
+      ,                        !- XGeometricCoeff
+      2,                       !- YMeshCount
+      Uniform,                 !- YMeshType
+      ,                        !- YGeometricCoeff
+      6,                       !- ZMeshCount
+      Uniform,                 !- ZMeshType
+      ,                        !- ZGeometricCoeff
+      1.08,                    !- GroundThermalConductivity
+      962,                     !- GroundDensity
+      2576,                    !- GroundSpecificHeat
+      30,                      !- MoistureContent
+      50,                      !- MoistureContentAtSaturation
+      Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
+      KATemps,                 !- Name of Undisturbed Ground Temperature Object
+      Yes,                     !- DomainHasBasement
+      6,                       !- BasementWidthInDomain
+      2.5,                     !- BasementDepthInDomain
+      Yes,                     !- ShiftPipeXValuesByBasementWidth
+      BasementWallOSCM,        !- BasementWallBoundaryConditionModel
+      BasementFloorOSCM,       !- BasementFloorBoundaryConditionModel
+      0.005,                   !- CartesianIterationConvergenceCriterion
+      100,                     !- CartesianMaxIterations
+      0.408,                   !- EvapotranspirationGroundCoverParameter
+      1,                       !- NumPipeCircuits
+      My Pipe Circuit;         !- PipeCircuit
+
+    PipingSystem:Underground:PipeCircuit,
+      My Pipe Circuit,         !- Name
+      0.3895,                  !- PipeThermalConductivity
+      641,                     !- PipeDensity
+      2405,                    !- PipeSpecificHeat
+      0.016,                   !- PipeInnerDiameter
+      0.02667,                 !- PipeOuterDiameter
+      0.004,                   !- DesignFlowRate
+      Piping System Inlet Node, !- InletNode
+      Piping System Outlet Node, !- OutletNode
+      0.001,                   !- RadialIterationConvergenceCriterion
+      100,                     !- RadialMaxIterations
+      2,                       !- RadialMeshCount
+      0.03,                    !- RadialMeshThickness
+      6,                       !- NumSegments
+      Segment 1,               !- Segment1
+      Segment 2,               !- Segment2
+      Segment 3,               !- Segment3
+      Segment 4,               !- Segment4
+      Segment 5,               !- Segment5
+      Segment 6;               !- Segment6
+
+    PipingSystem:Underground:PipeSegment,
+      Segment 1,               !- Name
+      0.67,                    !- X
+      2.20,                    !- Burial Depth
+      IncreasingZ;             !- Flow Direction
+
+    PipingSystem:Underground:PipeSegment,
+      Segment 2,               !- Name
+      0.95,                    !- X
+      2.20,                    !- Burial Depth
+      IncreasingZ;             !- Flow Direction
+
+    PipingSystem:Underground:PipeSegment,
+      Segment 3,               !- Name
+      1.23,                    !- X
+      2.20,                    !- Burial Depth
+      IncreasingZ;             !- Flow Direction
+
+    PipingSystem:Underground:PipeSegment,
+      Segment 4,               !- Name
+      1.40,                    !- X
+      1.94,                    !- Burial Depth
+      DecreasingZ;             !- Flow Direction
+
+    PipingSystem:Underground:PipeSegment,
+      Segment 5,               !- Name
+      1.40,                    !- X
+      1.66,                    !- Burial Depth
+      DecreasingZ;             !- Flow Direction
+
+    PipingSystem:Underground:PipeSegment,
+      Segment 6,               !- Name
+      1.40,                    !- X
+      1.39,                    !- Burial Depth
+      DecreasingZ;             !- Flow Direction
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-9-004}
+
+\begin{itemize}
+\item
+  HVAC, Average, Pipe Circuit Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC, Average, Pipe Circuit Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Pipe Circuit Outlet Temperature {[}C{]}
+\item
+  HVAC, Average, Pipe Segment Inlet Temperature {[}C{]}
+\item
+  HVAC, Average, Pipe Segment Outlet Temperature {[}C{]}
+\item
+  HVAC, Average, Pipe Circuit Fluid Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Average, Pipe Segment Fluid Heat Transfer Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Pipe Circuit Mass Flow Rate {[}kg/s{]}}\label{pipe-circuit-mass-flow-rate-kgs}
+
+The output provides the mass flow rate currently being sent through the pipe circuit.
+
+\paragraph{Pipe Circuit Inlet Temperature {[}C{]}}\label{pipe-circuit-inlet-temperature-c}
+
+\paragraph{Pipe Circuit Outlet Temperature {[}C{]}}\label{pipe-circuit-outlet-temperature-c}
+
+Temperature of fluid at the inlet and outlet of a given pipe circuit.
+
+\paragraph{Pipe Segment Inlet Temperature {[}C{]}}\label{pipe-segment-inlet-temperature-c}
+
+\paragraph{Pipe Segment Outlet Temperature {[}C{]}}\label{pipe-segment-outlet-temperature-c}
+
+Temperature of fluid at the inlet and outlet of a given pipe segment.
+
+\paragraph{Pipe Circuit Fluid Heat Transfer Rate {[}W{]}}\label{pipe-circuit-fluid-heat-transfer-rate-w}
+
+This is the fluid heat gain or loss in the pipe circuit, in Watts.
+
+\paragraph{Pipe Segment Fluid Heat Transfer Rate {[}W{]}}\label{pipe-segment-fluid-heat-transfer-rate-w}
+
+This is the fluid heat gain or loss in the pipe segment, in Watts.
+
+\subsection{Duct}\label{duct}
+
+The Duct object is a component for air systems that is a direct analogue for Pipe:Adiabatic in the fluid loops. It is used when it is necessary (due to the HVAC system configuration) to have a branch that has no functional components. This case most often arises for a bypass branch. Since every branch must have at least one component, the Duct component is used for this situation. The duct is an adiabatic, pass-through component; all of its inlet conditions are passed through unchanged to its outlet.
+
+\subsubsection{Inputs}\label{inputs-12-009}
+
+\paragraph{Field: Name}\label{field-name-12-006}
+
+This is the unique name for this component. Any reference to this component (in a BranchList, for instance) will refer to it by this name.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-2-000}
+
+The name of the component's air inlet node.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-2-000}
+
+The name of the component's air outlet node.
+
+Below is an example input for Duct.
+
+\begin{lstlisting}
+
+DUCT,
+      VAV Sys 1 Bypass Duct,            !- Name
+      VAV Sys 1 Bypass Duct Inlet Node, !- Inlet Node Name
+      VAV Sys 1 Bypass Duct Outlet Node;!- Outlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-10-004}
+
+There are no outputs for Duct.
diff --git a/doc/input-output-reference/src/overview/group-non-zone-equipment.tex b/doc/input-output-reference/src/overview/group-non-zone-equipment.tex
new file mode 100644
index 00000000000..91e01423780
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-non-zone-equipment.tex
@@ -0,0 +1,92 @@
+\section{Group -- Non-Zone Equipment}\label{group-non-zone-equipment}
+
+The non-zone equipment group consists of plant objects that connect to the demand side of the plant loop but are not associated with a a specific Zone (and do not have their own group). There is currently one non-zone equipment object called LoadProfile:Plant. This object places a scheduled demand load on the plant.
+
+Non-zone equipment allows the option of performing a plant-only EnergyPlus simulation, i.e.~without any zones. This can be useful for comparing the performance of various plant configurations or components without the added complexity of a full building description.
+
+\subsection{LoadProfile:Plant}\label{loadprofileplant}
+
+The LoadProfile:Plant object is used to simulate a scheduled demand profile. This can be useful when the building loads are already known. Demanded load and flow rate are schedules specified in the object definition. The load profile can specify heating and cooling loads. Cooling loads are entered as negative numbers. The actual load met is dependent on the performance of the supply loop components.
+
+The LoadProfile:Plant object must be connected on the demand side of the plant loop. It should be located on a Branch with its control type set to Active. If desired, multiple LoadProfile:Plant objects can be combined in series and/or parallel.
+
+\subsubsection{Inputs}\label{inputs-028}
+
+\paragraph{Field: Name}\label{field-name-027}
+
+The unique name of the LoadProfile:Plant object.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-002}
+
+The name of the inlet node connection to the plant loop.
+
+This node should be on the demand side.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-003}
+
+The name of the outlet node connection to the plant loop.
+
+\paragraph{Field: Load Schedule Name}\label{field-load-schedule-name}
+
+Reference to the schedule object specifying the load profile {[}W{]}.
+
+\paragraph{Field: Peak Flow Rate}\label{field-peak-flow-rate}
+
+The peak demanded water flow rate {[}m\(^{3}\)/s{]}. This value is multiplied by the flow rate fraction schedule values (below) to determine the actual volumetric flow rate.
+
+\paragraph{Field: Flow Rate Fraction Schedule Name}\label{field-flow-rate-fraction-schedule-name}
+
+Reference to the schedule object specifying the flow rate fraction relative to the value in the field Peak Flow Rate (above).
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+LoadProfile:Plant,
+  Load Profile 1,                                         !- Name
+  Demand Load Profile 1 Inlet Node,     !- Inlet Node Name
+  Demand Load Profile 1 Outlet Node,   !- Outlet Node Name
+  Load Profile 1 Load Schedule,             !- Load Schedule Name {W}
+  0.003,                                                           !- Peak Flow Rate {m3/s}
+  Load Profile 1 Flow Frac Schedule;   !- Flow Rate Fraction Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-020}
+
+The following output variables and meters are reported for the LoadProfile:Plant object:
+
+\begin{itemize}
+\item
+  HVAC,Average,Plant Load Profile Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Plant Load Profile Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Plant Load Profile Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Sum,Plant Load Profile Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Plant Load Profile Cooling Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Plant Load Profile Mass Flow Rate {[}kg/s{]}}\label{plant-load-profile-mass-flow-rate-kgs}
+
+This is the mass flow of the fluid passing through the load profile object, in kg/s.
+
+\paragraph{Plant Load Profile Heat Transfer Rate {[}W{]}}\label{plant-load-profile-heat-transfer-rate-w}
+
+\paragraph{Plant Load Profile Heat Transfer Energy {[}J{]}}\label{plant-load-profile-heat-transfer-energy-j}
+
+These report the overall heat transfer rate and energy for the load profile object, in Watts or Joules.
+
+\paragraph{Plant Load Profile Cooling Energy {[}J{]}Plant Load Profile Heating Energy {[}J{]}}\label{plant-load-profile-cooling-energy-jplant-load-profile-heating-energy-j}
+
+These report the overall cooling or heating energy that the load profile object places on the plant loop, in Joules.
+
+The inlet and outlet node temperatures and mass flow rates can be monitored using the system node output variables:
+
+\begin{itemize}
+\item
+  HVAC,Average,System Node Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Mass Flow Rate {[}kg/s{]}
+\end{itemize}
diff --git a/doc/input-output-reference/src/overview/group-operational-faults.tex b/doc/input-output-reference/src/overview/group-operational-faults.tex
new file mode 100644
index 00000000000..cf204a2ca82
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-operational-faults.tex
@@ -0,0 +1,463 @@
+\section{Group - Operational Faults}\label{group---operational-faults}
+
+\subsection{Introduction to Operational Faults Modeling}\label{introduction-to-operational-faults-modeling}
+
+Most of the buildings, either new or old, have operational faults in the sensors, controllers, meters, equipment and systems. Being able to model and simulate these faults and their impact on energy performance of buildings is crucial to improve accuracy of building simulations and to support the retrofit of buildings.
+
+To date, the main practitioner use of EnergyPlus has been for new construction design. With the new high priority attached by USDOE to retrofit and improved operation of existing buildings, there is a need to extend the capabilities of EnergyPlus to model existing buildings, including faulty operation:
+
+\begin{itemize}
+\item
+  Retrofit analysis: starts with calibrated simulation; the ability to estimate the severity of common faults is expected to improve the accuracy and transparency of the calibrated model and hence the increase accuracy of the analysis of different retrofit measures.
+\item
+  Commissioning providers can use the fault models to demonstrate the saving to be expected from fixing faults found in retro-commissioning
+\item
+  Support for building operation by using the calibrated model, including unfixed faults, as a real-time reference model to detect, and verify the diagnosis of, newly occurring faults.
+\end{itemize}
+
+The users in these cases are practitioners, not power users, so it is needed to implement the fault models using conventional EnergyPlus objects rather than the EMS, which, in any case, could only be used to model limited types of faults.
+
+\subsection{Operational Fault Objects}\label{operational-fault-objects}
+
+EnergyPlus contains a number of objects to model operational faults of sensors, meters, equipment and systems. The current implementation allows the modeling of the following fault types: (1) sensor faults with air economizers, (2) thermostat/humidistat offset faults, and (3) heating and cooling coil fouling faults.
+
+The objects used by EnergyPlus to model the faults are as follows:
+
+\begin{itemize}
+\item
+  FaultModel:TemperatureSensorOffset:OutdoorAir
+\item
+  FaultModel:HumiditySensorOffset:OutdoorAir
+\item
+  FaultModel:EnthalpySensorOffset:OutdoorAir
+\item
+  FaultModel:TemperatureSensorOffset:ReturnAir
+\item
+  FaultModel:EnthalpySensorOffset:ReturnAir
+\item
+  FaultModel:Fouling:Coil
+\item
+  FaultModel:ThermostatOffset
+\item
+  FaultModel:HumidistatOffset
+\end{itemize}
+
+\subsection{FaultModel:TemperatureSensorOffset:OutdoorAir}\label{faultmodeltemperaturesensoroffsetoutdoorair}
+
+This object defines the offset of an outdoor air dry-bulb temperature sensor that is used to determine applicability of an air economizer.
+
+\subsubsection{Inputs}\label{inputs-029}
+
+\paragraph{Field: Name}\label{field-name-028}
+
+This is the user-defined name of the fault.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-011}
+
+This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to 1.0 when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Severity Schedule Name}\label{field-severity-schedule-name}
+
+This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined temperature offset. This schedule should be set to a non-zero value when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Controller Object Type}\label{field-controller-object-type}
+
+This field defines the controller object type that this fault is associated with. Choices are from a list of applicable controller types. Current implementation supports air economizer the choice is Controller:OutdoorAir.
+
+\paragraph{Field: Controller Object Name}\label{field-controller-object-name}
+
+This field defines the name of the controller object associated with the fault. It should be one of the objects with the defined types.
+
+\paragraph{Field: Temperature Sensor Offset}\label{field-temperature-sensor-offset}
+
+This field defines the offset of the temperature sensor. A positive value means the sensor reads a temperature that is higher than the real value. A negative value means the sensor reads a temperature that is lower than the real value. A 0.0 value means no offset. Default is 0.0. The units are in degrees Celsius.
+
+\subsection{FaultModel:HumiditySensorOffset:OutdoorAir}\label{faultmodelhumiditysensoroffsetoutdoorair}
+
+This object defines the offset of an outdoor air humidity sensor that is used to determine applicability of an air economizer.
+
+\subsubsection{Inputs}\label{inputs-1-026}
+
+\paragraph{Field: Name}\label{field-name-1-025}
+
+This is the user-defined name of the fault.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-009}
+
+This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to 1.0 when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Severity Schedule Name}\label{field-severity-schedule-name-1}
+
+This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined temperature offset. This schedule should be set to a non-zero value when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Controller Object Type}\label{field-controller-object-type-1}
+
+This field defines the controller object type that this fault is associated with. Choices are from a list of applicable controller types. Current implementation supports air economizer the choice is Controller:OutdoorAir.
+
+\paragraph{Field: Controller Object Name}\label{field-controller-object-name-1}
+
+This field defines the name of the controller object associated with the fault. It should be one of the objects with the defined types.
+
+\paragraph{Field: Humidity Sensor Offset}\label{field-humidity-sensor-offset}
+
+This field defines the offset of the humidity ratio sensor. A positive value means the sensor reads a humidity ratio that is higher than the real value. A negative value means the sensor reads a humidity ratio that is lower than the real value. A 0.0 value means no offset. Default is 0.0. The units are in kgWater/kgDryAir.
+
+\subsection{FaultModel:EnthalpySensorOffset:OutdoorAir}\label{faultmodelenthalpysensoroffsetoutdoorair}
+
+This object defines the offset of an outdoor enthalpy sensor that is used to determine applicability of an air economizer.
+
+\subsubsection{Inputs}\label{inputs-2-024}
+
+\paragraph{Field: Name}\label{field-name-2-023}
+
+This is the user-defined name of the fault.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-2-005}
+
+This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to 1.0 when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Severity Schedule Name}\label{field-severity-schedule-name-2}
+
+This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined temperature offset. This schedule should be set to a non-zero value when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Controller Object Type}\label{field-controller-object-type-2}
+
+This field defines the controller object type that this fault is associated with. Choices are from a list of applicable controller types. Current implementation supports air economizer the choice is Controller:OutdoorAir.
+
+\paragraph{Field: Controller Object Name}\label{field-controller-object-name-2}
+
+This field defines the name of the controller object associated with the fault. It should be one of the objects with the defined types.
+
+\paragraph{Field: Enthalpy Sensor Offset}\label{field-enthalpy-sensor-offset}
+
+This field defines the offset of the enthalpy sensor. A positive value means the sensor reads an enthalpy that is higher than the real value. A negative value means the sensor reads an enthalpy that is lower than the real value. A 0.0 value means no offset. Default is 0.0. The units are in J/kg.
+
+\subsection{FaultModel:TemperatureSensorOffset:ReturnAir}\label{faultmodeltemperaturesensoroffsetreturnair}
+
+This object defines the offset of a return air dry-bulb temperature sensor that is used to determine applicability of an air economizer.
+
+\subsubsection{Inputs}\label{inputs-3-022}
+
+\paragraph{Field: Name}\label{field-name-3-020}
+
+This is the user-defined name of the fault.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-3-004}
+
+This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to 1.0 when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Severity Schedule Name}\label{field-severity-schedule-name-3}
+
+This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined temperature offset. This schedule should be set to a non-zero value when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Controller Object Type}\label{field-controller-object-type-3}
+
+This field defines the controller object type that this fault is associated with. Choices are from a list of applicable controller types. Current implementation supports air economizer the choice is Controller:OutdoorAir.
+
+\paragraph{Field: Controller Object Name}\label{field-controller-object-name-3}
+
+This field defines the name of the controller object associated with the fault. It should be one of the objects with the defined types.
+
+\paragraph{Field: Temperature Sensor Offset}\label{field-temperature-sensor-offset-1}
+
+This field defines the offset of the temperature sensor. A positive value means the sensor reads a temperature that is higher than the real value. A negative value means the sensor reads a temperature that is lower than the real value. A 0.0 value means no offset. Default is 0.0. The units are in degrees Celsius.
+
+\subsection{FaultModel:EnthalpySensorOffset:ReturnAir}\label{faultmodelenthalpysensoroffsetreturnair}
+
+This object defines the offset of a return air enthalpy sensor that is used to determine applicability of an air economizer.
+
+\subsubsection{Inputs}\label{inputs-4-020}
+
+\paragraph{Field: Name}\label{field-name-4-017}
+
+This is the user-defined name of the fault.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-4-004}
+
+This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to 1.0 when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Severity Schedule Name}\label{field-severity-schedule-name-4}
+
+This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined temperature offset. This schedule should be set to a non-zero value when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Controller Object Type}\label{field-controller-object-type-4}
+
+This field defines the controller object type that this fault is associated with. Choices are from a list of applicable controller types. Current implementation supports air economizer the choice is Controller:OutdoorAir.
+
+\paragraph{Field: Controller Object Name}\label{field-controller-object-name-4}
+
+This field defines the name of the controller object associated with the fault. It should be one of the objects with the defined types.
+
+\paragraph{Field: Enthalpy Sensor Offset}\label{field-enthalpy-sensor-offset-1}
+
+This field defines the offset of the enthalpy sensor. A positive value means the sensor reads an enthalpy that is higher than the real value. A negative value means the sensor reads an enthalpy that is lower than the real value. A 0.0 value means no offset. Default is 0.0. The units are in J/kg.
+
+\subsection{FaultModel:Fouling:Coil}\label{faultmodelfoulingcoil}
+
+This object defines the fouling for a simple water cooling coil or simple water heating coil.
+
+\subsubsection{Inputs}\label{inputs-5-018}
+
+\paragraph{Field: Name}\label{field-name-5-014}
+
+This is the user-defined name of the fault.
+
+\paragraph{Field: Coil Name}\label{field-coil-name-001}
+
+This field defines the name of the simple cooling coil or simple heating coil that has the fouling fault.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-5-002}
+
+This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then user-defined fouling and a severity schedule will be applied. This schedule should be set to 1.0 when a fault is applicable and 0.0 when it is not. If this field is blank, the schedule has values of 1 for all time periods
+
+\paragraph{Field: Severity Schedule Name}\label{field-severity-schedule-name-5}
+
+This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined fouling. If this field is blank, the schedule has values of 1 (no changes to fouling) for all time periods.
+
+\paragraph{Field: Fouling Input Method}\label{field-fouling-input-method}
+
+There are two methods to input the fouling, i.e.~FouledUARated and FoulingFactor. User chooses the appropriate method to determine the coil fouling.
+
+\paragraph{Field: UAFouled}\label{field-uafouled}
+
+This is the overall coil UA value including the coil fouling when the ``FouledUARated'' method is used. The unit is W/K.
+
+\paragraph{Field: Water Side Fouling Factor}\label{field-water-side-fouling-factor}
+
+The following four fields specify the required inputs when the ``FoulingFactor'' method is used. This field defines the fouling factor for the water side. The units are in m\(^{2}\)-K/W.
+
+\paragraph{Field: Air Side Fouling Factor}\label{field-air-side-fouling-factor}
+
+This field defines the fouling factor for the air side. The units are in m\(^{2}\)-K/W.
+
+\paragraph{Field: Outside Coil Surface Area}\label{field-outside-coil-surface-area}
+
+This field defines outside surface area of the cooling or heating coil. The units are in m\(^{2}\).
+
+\paragraph{Field: Inside to Outside Coil Surface Area Ratio}\label{field-inside-to-outside-coil-surface-area-ratio}
+
+This field specifies the inside to outside surface area ratio of the cooling or heating coil.
+
+IDF examples:
+
+\begin{lstlisting}
+
+! example faults for an air economizer
+
+  Schedule:Compact,
+  OATSeveritySch,                   !- Name
+  On/Off,                                   !- Schedule Type Limits Name
+  Through: 6/30,                     !- Field 1
+  For: AllDays,                       !- Field 2
+  Until: 24:00,0,                   !- Field 3
+  Through: 12/31,                   !- Field 4
+  For: AllDays,                       !- Field 5
+  Until: 24:00,1;                   !- Field 6
+
+  FaultModel:TemperatureSensorOffset:OutdoorAir,
+  OATFault,                                 !- Name
+  ALWAYS_ON,                               !- Availability Schedule Name
+  OATSeveritySch,                     !- Severity Schedule Name
+  Controller:OutdoorAir,       !- Controller Object Type
+  VAV_1_OA_Controller,           !- Controller Object Name
+  -2.0;                                           !- Temperature Sensor Offset, deg C
+
+  FaultModel:TemperatureSensorOffset:ReturnAir,
+  RATFault,                                 !- Name
+  ,                                                 !- Availability Schedule Name
+  ,                                                 !- Severity Schedule Name
+  Controller:OutdoorAir,       !- Controller Object Type
+  VAV_2_OA_Controller,           !- Controller Object Name
+  -2.0;                                         !- Temperature Sensor Offset, deg C
+
+  FaultModel:EnthalpySensorOffset:ReturnAir,
+  RAHFault,                                 !- Name
+  ,                                                 !- Availability Schedule Name
+  ,                                                 !- Severity Schedule Name
+  Controller:OutdoorAir,       !- Controller Object Type
+  VAV_2_OA_Controller,           !- Controller Object Name
+  -2000;                                       !- Enthalpy Sensor Offset, J/Kg
+
+  ! example faults for a fouling coil
+
+  FaultModel:Fouling:Coil,
+  CoolingCoilFault,               !- Name
+  VAV_2_CoolC,                         !- Heating or Cooling Coil Name
+  ALWAYS_ON,                             !- Availability Schedule Name
+  ,                                               !- Severity Schedule Name
+  FouledUARated,                     !- Fouling Input Method
+  3000,                                       !- UAFouled, W/K
+  ,                                               !- Water Side Fouling Factor, m2-K/W
+  ,                                               !- Air Side Fouling Factor, m2-K/W
+  ,                                               !- Outside Coil Surface Area, m2
+  ;                                               !- Inside to Outside Coil Surface Area Ratio
+\end{lstlisting}
+
+\subsection{FaultModel:ThermostatOffset}\label{faultmodelthermostatoffset}
+
+This object defines the offset fault of a thermostat that leads to inappropriate operations of the HVAC system.
+
+\subsubsection{Inputs}\label{inputs-6-015}
+
+\paragraph{Field: Name}\label{field-name-6-012}
+
+This is the user-defined name of the fault.
+
+\paragraph{Field: Thermostat Name}\label{field-thermostat-name}
+
+This field defines the name of the thermostat object associated with the fault. It should be the name of a ZoneControl:Thermostat object.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-6-002}
+
+This field provides the name of a schedule that will determine whether this fault is applicable or not. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to ``1.0'' when a fault is applicable and ``0.0'' when it is not. If this field is blank, the schedule has values of 1.0 for all time periods.
+
+\paragraph{Field: Severity Schedule Name}\label{field-severity-schedule-name-6}
+
+This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the reference thermostat offset value. This schedule should be set to a non-zero value when a fault is applicable and ``0.0'' when it is not. If this field is blank, the schedule has values of 1.0 for all time periods.
+
+\paragraph{Field: Reference Thermostat Offset}\label{field-reference-thermostat-offset}
+
+This field defines the reference offset value of the thermostat. A positive value means the zone air temperature reading is higher than the actual value. A negative value means the reading is lower than the actual value. A ``0.0'' value means no offset. Default is 2.0. The units are in degrees Celsius.
+
+\subsection{FaultModel:HumidistatOffset}\label{faultmodelhumidistatoffset}
+
+This object defines the offset fault of a humidistat that leads to inappropriate operations of the HVAC system.
+
+\subsubsection{Inputs}\label{inputs-7-015}
+
+\paragraph{Field: Name}\label{field-name-7-011}
+
+This is the user-defined name of the fault.
+
+\paragraph{Field: Humidistat Name}\label{field-humidistat-name}
+
+This field defines the name of the humidistat object associated with the fault. It should be the name of a ZoneControl:Humidistat object.
+
+\paragraph{Field: Humidistat Offset Type}\label{field-humidistat-offset-type}
+
+This choice field determines the humidistat offset fault type. Two fault types are available: (1) Type ThermostatOffsetIndependent: humidistat offset is not related with thermostat offset. For this type, user needs to specify the Reference Humidistat Offset, Availability Schedule, and Severity Schedule (2) Type ThermostatOffsetDependent: humidistat offset is caused by thermostat offset fault. For this type, user only needs to specify the Related Thermostat Offset Fault Name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-7-002}
+
+This field provides the name of a schedule that will determine if this fault is applicable. This field is applicable for the Type ThermostatOffsetIndependent. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to ``1.0'' when a fault is applicable and ``0.0'' when it is not. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Severity Schedule Name}\label{field-severity-schedule-name-7}
+
+This field provides the name of a schedule that represents severity of a fault. This field is applicable for the Type ThermostatOffsetIndependent. This is used as a multiplier to the reference humidistat offset value. This schedule should be set to a non-zero value when a fault is applicable and ``0.0'' when it is not. If this field is blank, the schedule has values of 1.0 for all time periods.
+
+\paragraph{Field: Reference Humidistat Offset}\label{field-reference-humidistat-offset}
+
+This field defines the reference offset value of the humidistat. This field is required for the Type ThermostatOffsetIndependent. A positive value means the zone air temperature reading is higher than the actual value. A negative value means the reading is lower than the actual value. A ``0.0'' value means no offset. Default is 5.0. The units are in percentage.
+
+\paragraph{Field: Related Thermostat Offset Fault Name}\label{field-related-thermostat-offset-fault-name}
+
+This field provides the name of a Thermostat Offset Fault object that causes the humidistat offset fault. It should be the name of a FaultModel:ThermostatOffset object. This field is required for the Type ThermostatOffsetDependent. This is used as a multiplier to the reference humidistat offset value. This schedule should be set to a non-zero value when a fault is applicable and ``0.0'' when it is not. If this field is blank, the schedule has values of 1.0 for all time periods.
+
+\subsection{An example of IDF codes for the thermostat/humidistat offset fault models:}\label{an-example-of-idf-codes-for-the-thermostathumidistat-offset-fault-models}
+
+\begin{lstlisting}
+
+FaultModel:ThermostatOffset,
+  Ther_Offset_Zone1,   !- Name
+  Zone 1 Thermostat,   !- Thermostat Name
+  AlwaysOn,            !- Availability Schedule Name
+  AlwaysOne,           !- Severity Schedule Name
+  2.0;                 !- Reference Thermostat Offset
+
+  FaultModel:HumidistatOffset, 
+  Humi_Offset_Zone1,   !- Name
+  Zone 1 Humidistat,   !- Humidistat Name
+  ThermostatOffsetDependent, !- Humidistat Offset Type
+  ,                    !- Availability Schedule Name
+  ,                    !- Severity Schedule Name
+  ,                    !- Reference Humidistat Offset
+  Ther_Offset_Zone1;   !- Related Thermostat Offset Fault Name
+
+  FaultModel:HumidistatOffset, 
+  Humi_Offset_Zone2,   !- Name
+  Zone 2 Humidistat,   !- Humidistat Name
+  ThermostatOffsetIndependent, !- Humidistat Offset Type
+  AlwaysOn,            !- Availability Schedule Name
+  AlwaysOne,           !- Severity Schedule Name
+  10,                  !- Reference Humidistat Offset
+  ;                    !- Related Thermostat Offset Fault Name
+\end{lstlisting}
+
+\subsection{FaultModel:Fouling:AirFilter}\label{faultmodelfoulingairfilter}
+
+This object defines the fault of fouling air filter that leads to inappropriate operations of the corresponding fan.
+
+\subsubsection{Inputs}\label{inputs-8-013}
+
+\paragraph{Field: Name}\label{field-name-8-011}
+
+This is the user-defined name of the fault.
+
+\paragraph{Field: Fan Name}\label{field-fan-name-002}
+
+This field defines the name of a fan object associated with the fault. It should be the name of a fan object (Fan:ConstantVolume, Fan:OnOff, or Fan:VariableVolume).
+
+\paragraph{Field: Fan Object Type}\label{field-fan-object-type-000}
+
+This choice field defines the type of fan. The valid choices are Fan:OnOff, Fan:ConstantVolume, and Fan:VariableVolume. Both cycling and continuous fan operating modes are allowed for Fan:OnOff. Only the continuous fan operating mode is allowed for Fan:ConstantVolume. The variable airflow rate is allowed for Fan:VariableVolume.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-8-002}
+
+This field provides the name of a schedule that will determine if this fault is applicable. This field is applicable for the Type ThermostatOffsetIndependent. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined Pressure Fraction Schedule will be applied. This schedule should be set to ``1.0'' when a fault is applicable and ``0.0'' when it is not. If this field is blank, the schedule has values of 1.0 for all time periods.
+
+\paragraph{Field: Pressure Fraction Schedule Name}\label{field-pressure-fraction-schedule-name}
+
+This field provides the name of a schedule that describes the pressure rise variations of the fan associated with the fouling air filter. This is used as a multiplier to the fan design pressure rise. Because the fan pressure rise in the faulty case is higher than that in the design case, this schedule should be set to a value that is greater than 1.0 when a fault is applicable. If this field is blank, the schedule has values of 1.0 for all time periods.
+
+\paragraph{Field: Fan Curve Name}\label{field-fan-curve-name}
+
+This field provides the name of a fan curve for the fan associated with the fault. The curve describes the relationship between the fan pressure rise and air flow rate. This is used to estimate the variations of the fan air flow rate in the faulty cases, given the Pressure Rise Variation Schedule. For variable speed fans, the curve should be the one corresponding to the maximum fan speed. The fan curve should cover the design operational point specified in the corresponding fan object. It is also required that the faulty fan operatinal state point falls within the fan selection range that is monotonically decreasing.
+
+\subsection{An example of IDF codes for the fouling air filter fault models:}\label{an-example-of-idf-codes-for-the-fouling-air-filter-fault-models}
+
+\begin{lstlisting}
+
+FaultModel:Fouling:AirFilter,
+  DF_VAV_1_Fan,             !- Name
+  VAV_1_Fan,                !- Fan Name
+  Fan:VariableVolume,       !- Fan Object Type
+  ALWAYS_ON,                !- Availability Schedule Name
+  Pressure_Inc_Sch,         !- Pressure Fraction Schedule Name
+  VAV_1_Fan_Curve;          !- Fan Curve Name
+
+  Schedule:Compact,
+  Pressure_Inc_Sch,        !- Name
+  Any Number,              !- Schedule Type Limits Name
+  Through: 12/31,          !- Field 1
+  For: AllDays,            !- Field 2
+  Until: 24:00,1.1;        !- Field 3
+
+  Curve:Cubic,        
+  VAV_1_Fan_Curve,         ! name     
+  1263.1,                  ! Coefficient1 Constant        
+  33.773,                  ! Coefficient2 x       
+  -5.6906,                  ! Coefficient3 x**2        
+  -0.2023,                  ! Coefficient4 x**3        
+  4.0,                     ! Minimum Value of x       
+  15.0;                    ! Maximum Value of x       
+
+  Fan:VariableVolume,
+  VAV_1_Fan,               !- Name
+  HVACOperationSchd,       !- Availability Schedule Name
+  0.5915,                  !- Fan Total Efficiency
+  1109.648,                !- Pressure Rise {Pa}
+  7.5202,                  !- Maximum Flow Rate {m3/s}
+  FixedFlowRate,           !- Fan Power Minimum Flow Rate Input Method
+  ,                        !- Fan Power Minimum Flow Fraction
+  0.0000,                  !- Fan Power Minimum Air Flow Rate {m3/s}
+  0.91,                    !- Motor Efficiency
+  1.0,                     !- Motor In Airstream Fraction
+  0.0407598940,            !- Fan Power Coefficient 1
+  0.08804497,              !- Fan Power Coefficient 2
+  -0.072926120,            !- Fan Power Coefficient 3
+  0.9437398230,            !- Fan Power Coefficient 4
+  0,                       !- Fan Power Coefficient 5
+  VAV_1_HeatC-VAV_1_FanNode,  !- Air Inlet Node Name
+  VAV_1 Supply Equipment Outlet Node,  !- Air Outlet Node Name
+  Fan Energy;              !- End-Use Subcategory
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-performance-curves.tex b/doc/input-output-reference/src/overview/group-performance-curves.tex
new file mode 100644
index 00000000000..c9af1f1424e
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-performance-curves.tex
@@ -0,0 +1,2195 @@
+\section{Group - Performance Curves}\label{group---performance-curves}
+
+This group of objects primarily consists of polynomial curves that are used to characterize the performance of HVAC equipment. Several other non-polynomial curves are also included to characterize the performance of pumps and fans. All of the curves are input, stored, and evaluated entirely within the CurveManager module. The curves are usually derived from fits or regressions to data covering a limited range. Results for independent variable values outside this range are likely to be invalid, so curve input always contains a range of validity (maximum and minimum permitted values) for each independent variable and can optionally have limits on the curve ouput. No error or warning message is issued if an independent variable is outside the range. Instead, the curve manager uses the minimum value if an independent variable is less than the minimum, and the maximum if a variable exceeds the maximum. Similarly, no error or warning message is issued if the curve output is outside the range of the optional minimum and maximum curve output limits. Instead, the curve manager uses the minimum and maximum curve limits to cap the output of the performance curve.
+
+Curve names must be unique across all curve types.
+
+\subsection{Curve:Linear}\label{curvelinear}
+
+Input for the linear curve consists of a curve name, the two coefficients, and the maximum and minimum valid independent variable values. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the linear curve is:
+
+\begin{equation}
+y = {C_1} + {C_2}*x
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-031}
+
+\paragraph{Field: Name}\label{field-name-030}
+
+A user assigned unique name for an instance of a linear curve. When a curve is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant}
+
+The constant coefficient (C\(_{1}\)) in the equation.
+
+\paragraph{Field: Coefficient2 x}\label{field-coefficient2-x}
+
+The linear coefficient (C\(_{2}\)) in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x}
+
+The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+Following is an example input:
+
+\begin{lstlisting}
+
+Curve:Linear,
+  Curve-Linear, ! name
+  -1, ! Coefficient1 Constant
+  2, ! Coefficient2 x
+  0.0, ! min curve output
+  1.0; ! max curve output
+\end{lstlisting}
+
+The following is another example, as might be applied in the Fan:ComponentModel to characterize duct static pressure reset (using a constant duct static pressure set point of 248.84 Pa in this case):
+
+\begin{lstlisting}
+
+Curve:Linear,
+  DiagnosticSPR, ! Curve Name f = C1 + C2\*x
+  248.84, ! Coefficient1 Constant [Pa]
+  0., ! Coefficent 2 Press/Flow [Pa-s/m3]
+  0., ! Minimum Value of x (Qfan) [m3/s]
+  100., ! Maximum Value of x (Qfan) [m3/s]
+  62.5, ! Minimum Curve Output [Pa]
+  248.84; ! Maximum Curve Output [Pa]
+\end{lstlisting}
+
+\subsection{Curve:QuadLinear}\label{curvequadlinear}
+
+Input consists of the curve name, the five coefficients, and maximum and minimum values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is represented by this curve:
+
+\subsubsection{Inputs}\label{inputs-1-028}
+
+\paragraph{y = C1 + C2 * w + C3 * x + C4 * y + C5 * z}\label{y-c1-c2-w-c3-x-c4-y-c5-z}
+
+\paragraph{Field: Name}\label{field-name-1-027}
+
+A user assigned unique name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant-1}
+
+The constant coefficient (C1) in the equation.
+
+\paragraph{Field: Coefficient2 w}\label{field-coefficient2-w}
+
+The coefficient (C2) in the equation.
+
+\paragraph{Field: Coefficient3 x}\label{field-coefficient3-x}
+
+The coefficient (C3) in the equation.
+
+\paragraph{Field: Coefficient4 y}\label{field-coefficient4-y}
+
+The coefficient (C4) in the equation.
+
+\paragraph{Field: Coefficient5 z}\label{field-coefficient5-z}
+
+The coefficient (C5) in the equation.
+
+\paragraph{Field: Minimum Value of w}\label{field-minimum-value-of-w}
+
+The minimum allowable value of w. Values of w less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of w}\label{field-maximum-value-of-w}
+
+The maximum allowable value of w. Values of z greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-1}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-1}
+
+The maximum allowable value of x. Values of z greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Value of y}\label{field-minimum-value-of-y}
+
+The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of y}\label{field-maximum-value-of-y}
+
+The maximum allowable value of y. Values of z greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Value of z}\label{field-minimum-value-of-z}
+
+The minimum allowable value of z. Values of z less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of z}\label{field-maximum-value-of-z}
+
+The maximum allowable value of z. Values of z greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for w}\label{field-input-unit-type-for-w}
+
+This field is used to indicate the kind of units that may be associated with the w values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of w and Maximum Value of w. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select Dimensionless which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\item
+  VolumetricFlowPerPower
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for x}\label{field-input-unit-type-for-x-1}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of x and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select Dimensionless which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\item
+  VolumetricFlowPerPower
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for y}\label{field-input-unit-type-for-y}
+
+This field is used to indicate the kind of units that may be associated with the y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of y and Maximum Value of y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select Dimensionless which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\item
+  VolumetricFlowPerPower
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for z}\label{field-input-unit-type-for-z}
+
+This field is used to indicate the kind of units that may be associated with the z values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of z and Maximum Value of z. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select Dimensionless which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\item
+  VolumetricFlowPerPower
+\end{itemize}
+
+Below are an example inputs for QuadLinear Curves.
+
+\begin{lstlisting}
+
+CURVE:QUADLINEAR,
+  MinDsnWBCurveName, ! Curve Name
+  -3.3333,           ! CoefficientC1
+  0.0,               ! CoefficientC2
+  38.9,              ! CoefficientC3
+  0.,                ! CoefficientC4
+  0.,                ! CoefficientC5
+  -30.,              ! Minimum Value of w
+  40.,               ! Maximum Value of w
+  0.,                ! Minimum Value of x
+  1.,                ! Maximum Value of x
+  10.,               ! Minimum Value of y
+  8.,                ! Maximum Value of y
+  1. E-8,            ! Minimum Value of z
+  8. E-8,            ! Maximum Value of z
+  0.,                ! Minimum Curve Output
+  38.;               ! Maximum Curve Output
+
+  Curve:QuadLinear,
+  MinActWBCurveName, ! Curve Name
+  -8.3333,           ! CoefficientC1
+  2.0,               ! CoefficientC2
+  5.5556.,           ! CoefficientC3
+  -1.0,              ! CoefficientC4
+  0.,                ! CoefficientC5
+  0.,                ! Minimum Value of w
+  38.,               ! Maximum Value of w
+  0.,                ! Minimum Value of x
+  1.,                ! Maximum Value of x
+  10.,               ! Minimum Value of y
+  38.,               ! Maximum Value of y
+  1. E-8,            ! Minimum Value of z
+  8. E-8,            ! Maximum Value of z
+  0.,                ! Minimum Curve Output
+  43.;               ! Maximum Curve Output
+
+  Curve:QuadLinear,
+  OptCondEntCurveName, ! Curve Name
+  12.2711,             ! CoefficientC1
+  0.80,                ! CoefficientC2
+  6.6667,              ! CoefficientC3
+  -0.266,              ! CoefficientC4
+  -6193484.,           ! CoefficientC5
+  0.,                  ! Minimum Value of w
+  38.,                 ! Maximum Value of w
+  0.,                  ! Minimum Value of x
+  1.,                  ! Maximum Value of x
+  10.,                 ! Minimum Value of y
+  38.,                 ! Maximum Value of y
+  1. E-8,              ! Minimum Value of z
+  8. E-8,              ! Maximum Value of z
+  0.,                  ! Minimum Curve Output
+  32.;                 ! Maximum Curve Output
+\end{lstlisting}
+
+\subsection{Curve:Quadratic}\label{curvequadratic}
+
+Input for a quadratic curve consists of the curve name, the three coefficients, and the maximum and minimum valid independent variable values. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the quadratic curve is:
+
+\begin{equation}
+y = {C_1} + {C_2}*x + {C_3}*{x^2}
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-2-026}
+
+\paragraph{Field: Name}\label{field-name-2-025}
+
+A user assigned unique name for an instance of a quadratic curve. When a curve is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant-2}
+
+The constant coefficient (C\(_{1}\)) in the equation.
+
+\paragraph{Field: Coefficient2 x}\label{field-coefficient2-x-1}
+
+The linear coefficient (C\(_{2}\)) in the equation.
+
+\paragraph{Field: Coefficient3 x**2}\label{field-coefficient3-x2}
+
+The quadratic coefficient (C\(_{3}\)) in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-2}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-2}
+
+The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-1}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-1}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x-2}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-1}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+Following is an example input.
+
+\begin{lstlisting}
+
+Curve:Quadratic,
+  WindACCBFFFF, ! name
+  -2.277,       ! Coefficient1 Constant
+  5.2114,       ! Coefficient2 x
+  -1.9344,      ! Coefficient3 x\*\*2
+  0.0,          ! Minimum Value of x
+  1.0;          ! Maximum Value of x
+\end{lstlisting}
+
+\subsection{Curve:Cubic}\label{curvecubic}
+
+Input for a cubic curve consists of the curve name, the 4 coefficients, and the maximum and minimum valid independent variable values. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the cubic curve is:
+
+\begin{equation}
+y = {C_1} + {C_2}*x + {C_3}*{x^2} + {C_4}*{x^3}
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-3-024}
+
+\paragraph{Field: Name}\label{field-name-3-021}
+
+A user assigned unique name for an instance of a cubic curve. When a curve is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant-3}
+
+The constant coefficient (C\(_{1}\)) in the equation.
+
+\paragraph{Field: Coefficient2 x}\label{field-coefficient2-x-2}
+
+The linear coefficient (C\(_{2}\)) in the equation.
+
+\paragraph{Field: Coefficient3 x**2}\label{field-coefficient3-x2-1}
+
+The quadratic coefficient (C\(_{3}\)) in the equation.
+
+\paragraph{Field: Coefficient4 x**3}\label{field-coefficient4-x3}
+
+The cubic coefficient (C\(_{4}\)) in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-3}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-3}
+
+The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-2}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-2}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x-3}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-2}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+Following is an input example.
+
+\begin{lstlisting}
+
+Curve:Cubic,
+  WindACEIRFPLF, ! name
+  .00000273404,  ! Coefficient1 Constant
+  1.05259,       ! Coefficient2 x
+  -.0552087,     ! Coefficient3 x**2
+  .00262236,     ! Coefficient4
+  0.0,           ! min
+  1.1;           ! max
+\end{lstlisting}
+
+\subsection{Curve:Quartic}\label{curvequartic}
+
+Input for a Quartic (fourth order polynomial) curve consists of the curve name, the five coefficients, and the maximum and minimum valid independent variable values. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the quartic curve is:
+
+\begin{equation}
+y = {C_1} + {C_2}x + {C_3}{x^2} + {C_4}{x^3} + {C_5}{x^4}
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-4-021}
+
+\paragraph{Field: Name}\label{field-name-4-018}
+
+A user assigned unique name for an instance of a Quartic curve. When a curve is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant-4}
+
+The constant coefficient (C\(_{1}\)) in the equation.
+
+\paragraph{Field: Coefficient2 x}\label{field-coefficient2-x-3}
+
+The linear coefficient (C\(_{2}\)) in the equation.
+
+\paragraph{Field: Coefficient3 x**2}\label{field-coefficient3-x2-2}
+
+The quadratic coefficient (C\(_{3}\)) in the equation.
+
+\paragraph{Field: Coefficient4 x**3}\label{field-coefficient4-x3-1}
+
+The cubic coefficient (C\(_{4}\)) in the equation.
+
+\paragraph{Field: Coefficient5 x**4}\label{field-coefficient5-x4}
+
+The fourth-order coefficient (C\(_{5}\)) in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-4}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-4}
+
+The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-3}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-5}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x-4}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-3}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+Following is an input example.
+
+\begin{lstlisting}
+
+Curve:Quartic,
+  BGSeries60,                                 !- y = -611.41x4 + 192.68x3 - 88.843x2 + 4.7634x + 5.5656
+  5.5656,                                         !- Constant
+  4.7634,                                         !- 1st coefficient
+  -88.843,                                       !- 2nd coefficient
+  192.68,                                         !- 3rd coefficient
+  -611.41,                                       !- 4th coefficient
+  0.0,                                               !- Min Phi Value
+  0.2412;                                         !- Max Phi Value
+\end{lstlisting}
+
+The following is another example, as might be applied in the Fan:ComponentModel to characterize belt maximum efficiency (using a medium efficiency belt in this case):
+
+\begin{lstlisting}
+
+Curve:Quartic,
+  BeltMaxEffMedium,                               ! Curve Name
+  -0.09504,                                               ! CoefficientC1
+  0.03415,                                                 ! CoefficientC2
+  -0.008897,                                             ! CoefficientC3
+  0.001159,                                               ! CoefficientC4
+  -0.00006132,                                         ! CoefficientC5
+  -1.2,                                                       ! Minimum Value of x
+  6.2,                                                         ! Maximum Value of x
+  -4.6,                                                       ! Minimum Curve Output
+  0.;                                                           ! Maximum Curve Output
+\end{lstlisting}
+
+\subsection{Curve:Exponent}\label{curveexponent}
+
+Input for a exponent curve consists of the curve name, the 3 coefficients, and the maximum and minimum valid independent variable values. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the exponent curve is:
+
+\begin{equation}
+y = C1 + C2*{x^{C3}}
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-5-019}
+
+\paragraph{Field: Name}\label{field-name-5-015}
+
+A user assigned unique name for an instance of an exponent curve. When a curve is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant-5}
+
+The constant coefficient (C\(_{1}\)) in the equation.
+
+\paragraph{Field: Coefficient2 Constant}\label{field-coefficient2-constant}
+
+The linear coefficient (C\(_{2}\)) in the equation.
+
+\paragraph{Field: Coefficient3 Constant}\label{field-coefficient3-constant}
+
+The exponent coefficient (C\(_{3}\)) in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-5}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-6}
+
+The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-4}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-3}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x-5}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-4}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+Following is an input example.
+
+\begin{lstlisting}
+
+Curve:Exponent,
+  !     Curve = C1 + C2\*x\*\*C3, x = fan speed ratio
+  FanPowerExponentCurve, !- Name
+  0.0,                                     !- Coefficient1 Constant
+  1.0,                                     !- Coefficient2 Constant
+  3.0,                                     !- Coefficient3 Constant
+  0.0,                                     !- Minimum Value of x
+  1.5,                                     !- Maximum Value of x
+  0.1,                                     !- Minimum Curve Output
+  1.5;                                     !- Maximum Curve Output
+\end{lstlisting}
+
+\subsection{Curve:Bicubic}\label{curvebicubic}
+
+This curve type is a function of two independent variables. Input consists of the curve name, the ten coefficients, and the minimum and maximum values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the bicubic curve is:
+
+\begin{equation}
+z = {C_1} + {C_2}*x + {C_3}*{x^2} + {C_4}*y + {C_5}*{y^2} + {C_6}*xy + {C_7}*{x^3} + {C_8}*{y^3} + {C_9}*{x^2}y + {C_{10}}*x{y^2}
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-6-016}
+
+\paragraph{Field: Name}\label{field-name-6-013}
+
+A user assigned unique name for an instance of a bicubic curve. When a curve is used by another object, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant-6}
+
+The constant coefficient (C\(_{1}\)) in the equation.
+
+\paragraph{Field: Coefficient2 x}\label{field-coefficient2-x-4}
+
+The coefficient C\(_{2}\) in the equation.
+
+\paragraph{Field: Coefficient3 x**2}\label{field-coefficient3-x2-3}
+
+The coefficient C\(_{3}\) in the equation.
+
+\paragraph{Field: Coefficient4 y}\label{field-coefficient4-y-1}
+
+The coefficient C\(_{4}\) in the equation.
+
+\paragraph{Field: Coefficient5 y**2}\label{field-coefficient5-y2}
+
+The coefficient C\(_{5}\) in the equation.
+
+\paragraph{Field: Coefficient6 x*y}\label{field-coefficient6-xy}
+
+The coefficient C\(_{6}\) in the equation.
+
+\paragraph{Field: Coefficient7 x**3}\label{field-coefficient7-x3}
+
+The coefficient C\(_{7}\) in the equation.
+
+\paragraph{Field: Coefficient8 y**3}\label{field-coefficient8-y3}
+
+The coefficient C\(_{8}\) in the equation.
+
+\paragraph{Field: Coefficient9 x**2*y}\label{field-coefficient9-x2y}
+
+The coefficient C\(_{9}\) in the equation.
+
+\paragraph{Field: Coefficient10 x*y**2}\label{field-coefficient10-xy2}
+
+The coefficient C\(_{10}\) in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-6}
+
+The minimum allowable value of x. Values of x less than this minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-7}
+
+The maximum allowable value of x. Values of x greater than this maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Value of y}\label{field-minimum-value-of-y-1}
+
+The minimum allowable value of y. Values of y less than this minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of y}\label{field-maximum-value-of-y-1}
+
+The maximum allowable value of y. Values of y greater than this maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-5}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-4}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x-6}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for Y}\label{field-input-unit-type-for-y-1}
+
+This field is used to indicate the kind of units that may be associated with the y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Y and Maximum Value of Y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-5}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+Below is an example input.
+
+\begin{lstlisting}
+
+Curve:Bicubic,
+  Main Chiller EIRFPLR,             !- Name
+  7.086284E-02,                             !- Coefficient1 Constant
+  2.787561E-03,                             !- Coefficient2 x
+  -8.917038E-06,                             !- Coefficient3 x\*\*2
+  2.309734E-01,                             !- Coefficient4 y
+  1.250442E+00,                             !- Coefficient5 y\*\*2
+  -2.161029E-03,                             !- Coefficient6 x\*y
+  0.000000E+00,                             !- Coefficient7 x\*\*3
+  -5.630094E-01,                             !- Coefficient8 y\*\*3
+  0.000000E+00,                             !- Coefficient9 x\*\*2\*y
+  0.000000E+00,                             !- Coefficient10 x\*y\*\*2
+  20.33,                                           !- Minimum Value of x
+  35.00,                                           !- Maximum Value of x
+  0.25,                                             !- Minimum Value of y
+  1.01;                                             !- Maximum Value of y
+\end{lstlisting}
+
+\subsection{Curve:Biquadratic}\label{curvebiquadratic}
+
+This curve is a function of two independent variables. Input consists of the curve name, the six coefficients, and min and max values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the bicubic curve is:
+
+\begin{equation}
+z = {C_1} + {C_2}*x + {C_3}*{x^2} + {C_4}*y + {C_5}*{y^2} + {C_6}*xy
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-7-016}
+
+\paragraph{Field: Name}\label{field-name-7-012}
+
+A user assigned unique name for an instance of a biquadratic curve. When a curve is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant-7}
+
+The constant coefficient (C\(_{1}\)) in the equation.
+
+\paragraph{Field: Coefficient2 x}\label{field-coefficient2-x-5}
+
+The coefficient C\(_{2}\) in the equation.
+
+\paragraph{Field: Coefficient3 x**2}\label{field-coefficient3-x2-4}
+
+The coefficient C\(_{3}\) in the equation.
+
+\paragraph{Field: Coefficient4 y}\label{field-coefficient4-y-2}
+
+The coefficient C\(_{4}\) in the equation.
+
+\paragraph{Field: Coefficient5 y**2}\label{field-coefficient5-y2-1}
+
+The coefficient C\(_{5}\) in the equation.
+
+\paragraph{Field: Coefficient6 x*y}\label{field-coefficient6-xy-1}
+
+The coefficient C\(_{6}\) in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-7}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-8}
+
+The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Value of y}\label{field-minimum-value-of-y-2}
+
+The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of y}\label{field-maximum-value-of-y-2}
+
+The maximum allowable value of y. Values of y greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-6}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-5}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x-7}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for Y}\label{field-input-unit-type-for-y-2}
+
+This field is used to indicate the kind of units that may be associated with the y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Y and Maximum Value of Y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-6}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+Below is an example input.
+
+\begin{lstlisting}
+
+Curve:Biquadratic,
+  WindACCoolCapFT, ! name
+  0.942587793,     ! Coefficient1 Constant
+  0.009543347,     ! Coefficient2 x
+  0.000683770,     ! Coefficient3 x\*\*2
+  -0.011042676,    ! Coefficient4 y
+  0.000005249,     ! Coefficient5 y\*\*2
+  -0.000009720,    ! Coefficient6 x\*y
+  15., 22.,        ! min and max of first independent variable
+  29., 47.;        ! min and max of second independent variable
+\end{lstlisting}
+
+\subsection{Curve:CubicLinear}\label{curvecubiclinear}
+
+This curve is a function of two independent variables. Input consists of the curve name, the six coefficients, and min and max values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the cubic linear curve:
+
+\begin{equation}
+y = \left( {{C_1} + {C_2}*x + {C_3}*{x^2} + {C_4}*{x^3}} \right) + \left( {{C_5} + {C_6}*x} \right)*y
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-8-014}
+
+\paragraph{Field: Name}\label{field-name-8-012}
+
+A user assigned unique name for an instance of a quadratic-linear curve. When a curve is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant-8}
+
+The constant coefficient (\(C_1\) ) in the equation.
+
+\paragraph{Field: Coefficient2 x}\label{field-coefficient2-x-6}
+
+The coefficient \(C_2\) in the equation.
+
+\paragraph{\texorpdfstring{Field: Coefficient3 x**2 The coefficient \(C_3\) in the equation.}{Field: Coefficient3 x**2 The coefficient C\_3 in the equation.}}\label{field-coefficient3-x2-the-coefficient-cux5f3-in-the-equation.}
+
+\paragraph{\texorpdfstring{Field: Coefficient4 x**3 The coefficient \(C_4\) in the equation.}{Field: Coefficient4 x**3 The coefficient C\_4 in the equation.}}\label{field-coefficient4-x3-the-coefficient-cux5f4-in-the-equation.}
+
+\paragraph{Field: Coefficient5 y}\label{field-coefficient5-y}
+
+The coefficient \(C_5\) in the equation.
+
+\paragraph{\texorpdfstring{Field: Coefficient6 x*y The coefficient \(C_6\) in the equation.}{Field: Coefficient6 x*y The coefficient C\_6 in the equation.}}\label{field-coefficient6-xy-the-coefficient-cux5f6-in-the-equation.}
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-8}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-9}
+
+The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Value of y}\label{field-minimum-value-of-y-3}
+
+The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of y}\label{field-maximum-value-of-y-3}
+
+The maximum allowable value of y. Values of y greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-7}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-6}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x-8}
+
+This field is used to indicate the kind of units that may be associated with the x values. The only option at this time is \textbf{Dimensionless}.
+
+\paragraph{Field: Input Unit Type for Y}\label{field-input-unit-type-for-y-3}
+
+This field is used to indicate the kind of units that may be associated with the x values. The only option at this time is \textbf{Dimensionless}.
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-7}
+
+This field is used to indicate the kind of units that may be associated with the output values. The only option at this time is \textbf{Dimensionless}.
+
+An example input for the CubicLinear equation form is shown below.
+
+\begin{lstlisting}
+
+Curve:CubicLinear, 
+  InsideMeltIceDischarging, !- Name
+  0.108734675,              !- Coefficient1 Constant
+  -0.989874286,             !- Coefficient2 x
+  0.696303562,              !- Coefficient3 x**2
+  -0.134945307,             !- Coefficient4 x**3
+  1.724007415,              !- Coefficient5 y
+  -1.094020457,             !- Coefficient6 y*x
+  0.25,                     !- Minimum Value of x
+  1,                        !- Maximum Value of x
+  0.69,                     !- Minimum Value of y
+  1.26,                     !- Maximum Value of y
+  0.0926,                   !- Minimum Curve Output
+  0.4938,                   !- Maximum Curve Output
+  Dimensionless,            !- Input Unit Type for X
+  Dimensionless,            !- Input Unit Type for Y
+  Dimensionless,            !- Output Unit Type
+\end{lstlisting}
+
+\subsection{Curve:ChillerPartLoadCustom}\label{curvechillerpartloadcustom}
+
+A custom chiller part-load performance curve is a function of three independent variables, i.e., x, y, and z. Input consists of the curve name, the twelve coefficients, and min and max values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve.
+
+The equation represented by the custom curve is:
+
+\begin{equation}
+C_1 + C_2 \cdot x + C_3 \cdot x^2 + C_4 \cdot y + C_5 \cdot y^2 + C_6 \cdot x \cdot y + C_7 \cdot x^3 + C_8 \cdot y^3 + C_9 \cdot x^2 \cdot y + C_{10} \cdot x \cdot y^2 + C_{11} \cdot x^2 \cdot y^2 + C_{12} \cdot z \cdot y^3
+\end{equation}
+
+where,
+
+\begin{itemize}
+\tightlist
+\item
+  x represents the normalized fractional lift (the delta of temperature across the leaving condenser water temperature and leaving evaporator water temperature of a chiller).
+\item
+  y represents the normalized deviation of leaving chilled water temperature from the reference condition.
+\item
+  z represents the part load ratio.
+\end{itemize}
+
+\subsubsection{Field: Name}\label{field-name-9-011}
+
+A user assigned unique name for an instance of a biquadratic curve. When a curve is used, it is referenced by this name.
+
+\subsubsection{Field: Coefficient1}\label{field-coefficient1}
+
+The constant coefficient (C1) in the equation.
+
+\subsubsection{Field: Coefficient2}\label{field-coefficient2}
+
+The coefficient C2 in the equation.
+
+\subsubsection{Field: Coefficient3}\label{field-coefficient3}
+
+The coefficient C3 in the equation.
+
+\subsubsection{Field: Coefficient4}\label{field-coefficient4}
+
+The coefficient C4 in the equation.
+
+\subsubsection{Field: Coefficient5}\label{field-coefficient5}
+
+The coefficient C5 in the equation.
+
+\subsubsection{Field: Coefficient6}\label{field-coefficient6}
+
+The coefficient C6 in the equation.
+
+\subsubsection{Field: Coefficient7}\label{field-coefficient7}
+
+The constant coefficient (C7) in the equation.
+
+\subsubsection{Field: Coefficient8}\label{field-coefficient8}
+
+The coefficient C8 in the equation.
+
+\subsubsection{Field: Coefficient9}\label{field-coefficient9}
+
+The coefficient C9 in the equation.
+
+\subsubsection{Field: Coefficient10}\label{field-coefficient10}
+
+The coefficient C10 in the equation.
+
+\subsubsection{Field: Coefficient11}\label{field-coefficient11}
+
+The coefficient C11 in the equation.
+
+\subsubsection{Field: Coefficient12}\label{field-coefficient12}
+
+The coefficient C12 in the equation.
+
+\subsubsection{Field: Minimum Value of x}\label{field-minimum-value-of-x-9}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\subsubsection{Field: Maximum Value of x}\label{field-maximum-value-of-x-10}
+
+The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
+
+\subsubsection{Field: Minimum Value of y}\label{field-minimum-value-of-y-4}
+
+The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
+
+\subsubsection{Field: Maximum Value of y}\label{field-maximum-value-of-y-4}
+
+The maximum allowable value of y. Values of y greater than the maximum will be replaced by the maximum.
+
+\subsubsection{Field: Minimum Value of z}\label{field-minimum-value-of-z-1}
+
+The minimum allowable value of z. Values of y less than the minimum will be replaced by the minimum.
+
+\subsubsection{Field: Maximum Value of z}\label{field-maximum-value-of-z-1}
+
+The maximum allowable value of z. Values of y greater than the maximum will be replaced by the maximum.
+
+\subsubsection{Field: Minimum Curve Output}\label{field-minimum-curve-output-8}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\subsubsection{Field: Maximum Curve Output}\label{field-maximum-curve-output-7}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\subsubsection{Field: Input Unit Type for x}\label{field-input-unit-type-for-x-9}
+
+This field is used to indicate the kind of units that may be associated with the x values. Select Dimensionless.
+
+\subsubsection{Field: Input Unit Type for y}\label{field-input-unit-type-for-y-4}
+
+This field is used to indicate the kind of units that may be associated with the y values. Select Dimensionless.
+
+\subsubsection{Field: Input Unit Type for z}\label{field-input-unit-type-for-z-1}
+
+This field is used to indicate the kind of units that may be associated with the y values. Select Dimensionless.
+
+\subsubsection{Field: Output Unit Type}\label{field-output-unit-type-8}
+
+This field is used to indicate the kind of units that may be associated with the output values. Select Dimensionless.
+
+Below is an example input:
+
+\begin{lstlisting}
+
+Curve:ChillerPartLoadCustom,
+  EIRFPLR,        !- Name  
+  0.093291598,        !- Coefficient1 Constant
+  -0.234322952,       !- Coefficient2 x
+  0.426950368,        !- Coefficient3 x**2
+  0.188624721,        !- Coefficient4 y
+  -0.608010978,       !- Coefficient5 y**2
+  0.992031248,        !- Coefficient6 x*y
+  0.000000E+00,       !- Coefficient7 x**3
+  0.502338322,        !- Coefficient8 y**3
+  0.000000E+00,       !- Coefficient9 x**2*y
+  0.000000E+00,       !- Coefficient 10 x*y**2
+  -0.360902326,       !- Coefficient 11 x**2*y**2
+  -0.097978985,       !- Coefficient 12 z*y**3 
+  0.2562,             !- Minimum Value of x
+  1.0365,             !- Maximum Value of x
+  0.1,                !- Minimum Value of y
+  1,                  !- Maximum Value of y
+  -0.035,             !- Minimum Value of z
+  0.3144,             !- Maximum Value of z
+  ,                   !- Minimum Curve Output
+  ,                   !- Maximum Curve Output
+  Dimensionless,      !- Input Unit Type for x
+  Dimensionless,      !- Input Unit Type for y
+  Dimensionless,      !- Input Unit Type for z
+  Dimensionless;      !- Output Unit Type
+\end{lstlisting}
+
+\subsection{Curve:QuadraticLinear}\label{curvequadraticlinear}
+
+This curve is a function of two independent variables. Input consists of the curve name, the six coefficients, and min and max values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the quadratic linear curve:
+
+\begin{equation}
+z = \left( {{C_1} + {C_2}*x + {C_3}*{x^2}} \right) + \left( {{C_4} + {C_5}*x + {C_6}*{x^2}} \right)*y
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-9-012}
+
+\paragraph{Field: Name}\label{field-name-10-010}
+
+A user assigned unique name for an instance of a quadratic-linear curve. When a curve is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant-9}
+
+The constant coefficient (C\(_{1}\)) in the equation.
+
+\paragraph{Field: Coefficient2 x}\label{field-coefficient2-x-7}
+
+The coefficient C\(_{2}\) in the equation.
+
+\paragraph{Field: Coefficient3 x**2}\label{field-coefficient3-x2-5}
+
+The coefficient C\(_{3}\) in the equation.
+
+\paragraph{Field: Coefficient4 y}\label{field-coefficient4-y-3}
+
+The coefficient C\(_{4}\) in the equation.
+
+\paragraph{Field: Coefficient5 x*y}\label{field-coefficient5-xy}
+
+The coefficient C\(_{5}\) in the equation.
+
+\paragraph{Field: Coefficient6 x**2*y}\label{field-coefficient6-x2y}
+
+The coefficient C\(_{6}\) in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-10}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-11}
+
+The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Value of y}\label{field-minimum-value-of-y-5}
+
+The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of y}\label{field-maximum-value-of-y-5}
+
+The maximum allowable value of y. Values of y greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-9}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-8}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x-10}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for Y}\label{field-input-unit-type-for-y-5}
+
+This field is used to indicate the kind of units that may be associated with the y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Y and Maximum Value of Y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-9}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+Below is an example input.
+
+\begin{lstlisting}
+
+Curve:QuadraticLinear,
+  DischargeCurve, !- Curve Name
+  0.0,            !- Coefficient1 Constant
+  0.09,           !- Coefficient2 x
+  -0.15,          !- Coefficient3 x\*\*2
+  0.612,          !- Coefficient4 y
+  -0.324,         !- Coefficient5 x\*y
+  -0.216,         !-Coefficient6 x\*\*2\*y
+  0.0,            !- Minimum Value of x
+  1.0,            !- Maximum Value of x
+  0.0,            !- Minimum Value of y
+  9.9;            !- Maximum Value of y
+\end{lstlisting}
+
+\subsection{Curve:Triquadratic}\label{curvetriquadratic}
+
+This curve is a 2\(^{nd}\) order polynomial function of three variable polynomial independent variables. Input consists of the curve name, the twenty seven coefficients, and min and max values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the triquadratic curve:
+
+\begin{equation}
+  \begin{array}{l}
+    CurveValue = {A_0} + {A_1}*{x^2} + {A_2}*x + {A_3}*{y^2} + {A_4}*y + {A_5}*{z^2} + {A_6}*z + {A_7}*{x^2}{y^2} + {A_8}*xy + \\
+    \quad \quad \quad \quad \quad {A_9}*x{y^2} + {A_{10}}*{x^2}y + {A_{11}}*{x^2}{z^2} + {A_{12}}*xz + {A_{13}}*x{z^2} + {A_{14}}*{x^2}z + {A_{15}}*{y^2}{z^2} + \\
+    \quad \quad \quad \quad \quad {A_{16}}*yz + {A_{17}}*y{z^2} + {A_{18}}*{y^2}z + {A_{19}}*{x^2}{y^2}{z^2} + {A_{20}}*{x^2}{y^2}z + {A_{21}}{x^2}y{z^2} + {A_{22}}x{y^2}{z^2} + \\
+    \quad \quad \quad \quad \quad {A_{23}}{x^2}yz + {A_{24}}x{y^2}z + {A_{25}}xy{z^2} + {A_{26}}xyz
+  \end{array}
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-10-011}
+
+\paragraph{Field: Coefficient1 Constant}\label{field-coefficient1-constant-10}
+
+The constant coefficient (A\(_{0}\)) in the equation.
+
+\paragraph{Field: Coefficient2 x**2}\label{field-coefficient2-x2}
+
+The coefficient (A\(_{1}\)) in the equation.
+
+\paragraph{Field: Coefficient3 x}\label{field-coefficient3-x-1}
+
+The coefficient (A\(_{2}\)) in the equation.
+
+\paragraph{Field: Coefficient4 y**2}\label{field-coefficient4-y2}
+
+The coefficient (A\(_{3}\)) in the equation.
+
+\paragraph{Field: Coefficient5 y}\label{field-coefficient5-y-1}
+
+The coefficient (A\(_{4}\)) in the equation.
+
+\paragraph{Field: Coefficient6 z**2}\label{field-coefficient6-z2}
+
+The coefficient (A\(_{5}\)) in the equation.
+
+\paragraph{Field: Coefficient7 z}\label{field-coefficient7-z}
+
+The coefficient (A\(_{6}\)) in the equation.
+
+\paragraph{Field: Coefficient8 x**2*y**2}\label{field-coefficient8-x2y2}
+
+The coefficient (A\(_{7}\)) in the equation.
+
+\paragraph{Field: Coefficient9 x*y}\label{field-coefficient9-xy}
+
+The coefficient (A\(_{8}\)) in the equation.
+
+\paragraph{Field: Coefficient10 x*y**2}\label{field-coefficient10-xy2-1}
+
+The coefficient (A\(_{9}\)) in the equation.
+
+\paragraph{Field: Coefficient11 x**2*y}\label{field-coefficient11-x2y}
+
+The coefficient (A\(_{10}\)) in the equation.
+
+\paragraph{Field: Coefficient12 x**2*z**2}\label{field-coefficient12-x2z2}
+
+The coefficient (A\(_{11}\)) in the equation.
+
+\paragraph{Field: Coefficient13 x*z}\label{field-coefficient13-xz}
+
+The coefficient (A\(_{12}\)) in the equation.
+
+\paragraph{Field: Coefficient14 x*z**2}\label{field-coefficient14-xz2}
+
+The coefficient (A\(_{13}\)) in the equation.
+
+\paragraph{Field: Coefficient15 x**2*z}\label{field-coefficient15-x2z}
+
+The coefficient (A\(_{14}\)) in the equation.
+
+\paragraph{Field: Coefficient16 y**2*z**2}\label{field-coefficient16-y2z2}
+
+The coefficient (A\(_{15}\)) in the equation.
+
+\paragraph{Field: Coefficient17 y*z}\label{field-coefficient17-yz}
+
+The coefficient (A\(_{16}\)) in the equation.
+
+\paragraph{Field: Coefficient18 y*z**2}\label{field-coefficient18-yz2}
+
+The coefficient (A\(_{17}\)) in the equation.
+
+\paragraph{Field: Coefficient19 y**2*z}\label{field-coefficient19-y2z}
+
+The coefficient (A\(_{18}\)) in the equation.
+
+\paragraph{Field: Coefficient20 x**2*y**2*z**2}\label{field-coefficient20-x2y2z2}
+
+The coefficient (A\(_{19}\)) in the equation.
+
+\paragraph{Field: Coefficient21 x**2*y**2*z}\label{field-coefficient21-x2y2z}
+
+The coefficient (A\(_{20}\)) in the equation.
+
+\paragraph{Field: Coefficient22 x**2*y*z**2}\label{field-coefficient22-x2yz2}
+
+The coefficient (A\(_{21}\)) in the equation.
+
+\paragraph{Field: Coefficient23 x*y**2*z**2}\label{field-coefficient23-xy2z2}
+
+The coefficient (A\(_{22}\)) in the equation.
+
+\paragraph{Field: Coefficient24 x**2*y*z}\label{field-coefficient24-x2yz}
+
+The coefficient (A\(_{23}\)) in the equation.
+
+\paragraph{Field: Coefficient25 x*y**2*z}\label{field-coefficient25-xy2z}
+
+The coefficient (A\(_{24}\)) in the equation.
+
+\paragraph{Field: Coefficient26 x*y*z**2}\label{field-coefficient26-xyz2}
+
+The coefficient (A\(_{25}\)) in the equation.
+
+\paragraph{Field: Coefficient27 x*y*z}\label{field-coefficient27-xyz}
+
+The coefficient (A\(_{26}\)) in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-11}
+
+The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-12}
+
+The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Value of y}\label{field-minimum-value-of-y-6}
+
+The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of y}\label{field-maximum-value-of-y-6}
+
+The maximum allowable value of y. Values of y greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Value of z}\label{field-minimum-value-of-z-2}
+
+The minimum allowable value of z. Values of z less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of z}\label{field-maximum-value-of-z-2}
+
+The maximum allowable value of z. Values of z greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-10}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-9}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x-11}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for Y}\label{field-input-unit-type-for-y-6}
+
+This field is used to indicate the kind of units that may be associated with the y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Y and Maximum Value of Y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for Z}\label{field-input-unit-type-for-z-2}
+
+This field is used to indicate the kind of units that may be associated with the z values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Z and Maximum Value of Z. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Power
+\item
+  Distance
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-10}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+\subsection{Curve:Functional:PressureDrop}\label{curvefunctionalpressuredrop}
+
+Input for a pressure drop curve consists of the curve name, a varying number of parameters, and the maximum and minimum valid independent variable values. The equation represented by the pressure drop curve is:
+
+\begin{equation}
+\Delta P = \left( {K + f\frac{L}{D}} \right)\frac{{\rho {V^2}}}{2}
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-11-010}
+
+\paragraph{Field: Name}\label{field-name-11-009}
+
+A user assigned unique name for an instance of a pressure drop curve. When a curve is used, it is referenced by this name.
+
+\paragraph{Field: Diameter}\label{field-diameter-000}
+
+This diameter represents an equivalent diameter for the given branch. This is parameter (D) in the equation, and has units of \{m\}. Since varying components may be found on the same branch, this value must be selected along with the other inputs in order to provide a proper value of pressure drop. This is used to calculate the velocity in addition to being used directly in the frictional pressure drop calculation.
+
+\paragraph{Field: Minor Loss Coefficient}\label{field-minor-loss-coefficient}
+
+This is the pressure drop coefficient typically applied to components such as fittings and occasionally heat pumps. This is parameter (K) in the equation and is dimensionless. This coefficient is used to describe the amount of dynamic pressure lost during the process. This value may be left blank if the user only wants to account for frictional losses in this branch.
+
+\paragraph{Field: Length}\label{field-length}
+
+This is the length of a pressure drop process in which friction is applied. This is parameter (L) in the equation and has units of \{m\}. In a pipe, this would be the length of the pipe, however in many cases, pressure drop in other components are applied as an equivalent length. This is only required if the user is wanting to perform frictional pressure drop calculations.
+
+\paragraph{Field: Roughness}\label{field-roughness}
+
+This field represents the first method to simulate frictional losses. This parameter does not appear directly in the equation above, as it is only used to develop the friction factor (f), but the roughness will have units of \{m\} if entered. If the user enters this roughness value, the pressure system will use it along with an approximation to the Moody chart to estimate the friction factor given the current flow conditions. This allows the friction calculate to be dynamic throughout the simulation.
+
+\paragraph{Field: Fixed Friction Factor}\label{field-fixed-friction-factor}
+
+This field represents the second method to simulate frictional losses. This is parameter (f) in the equation and is dimensionless. This parameter is a fixed value of friction factor which would override any calculations performed based on roughness, etc. If the user has a known friction factor for a given component, this is where it should be entered.
+
+In the curve outputs for this object:
+
+\begin{itemize}
+\item
+  Curve Input 1: MassFlow
+\item
+  Curve Input 2: Density
+\item
+  Curve Input 3: Velocity
+\item
+  Curve Output: the resultant value
+\end{itemize}
+
+Following is an input example.
+
+\begin{lstlisting}
+
+Curve:Functional:PressureDrop,
+  PressureMinorAndFriction,!- Name
+  0.05,                                       !- Diameter
+  53.8,                                       !- Minor Loss Coefficient
+  200,                                         !- Length
+  ,                                               !- Roughness
+  0.008;                                     !- Fixed Friction Factor
+\end{lstlisting}
+
+\subsection{Curve:FanPressureRise}\label{curvefanpressurerise}
+
+Input for the fan total pressure rise curve consists of the curve name, the four coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
+
+\begin{equation}
+\Delta {P_{fan,tot}} = {C_1}*Q_{fan}^2 + {C_2}*Q_{fan}^{} + {C_3}*Q_{fan}^{}*\sqrt {{P_{sm}} - {P_o}}  + {C_4}*\left( {{P_{sm}} - {P_o}} \right)
+\end{equation}
+
+where \(\Delta P_{fan,tot}\) is the fan total pressure rise (Pa) as a function of volumetric flow through the fan (\(Q_{fan}, m^3/s\) ), duct static pressure set point (\(P_{sm}\) , Pa), and static pressure surrounding the ducts (\(P_o\) , Pa). \(P_o\) is assumed to be zero.
+
+The first term of the curve looks like the common system curve in which the fan pressure rise is proportional to the square of the fan flow, but here it also depends implicitly on supply and return pressure losses, and in part on the fraction of the fan flow that is outdoor air (essentially ``leaks'' into and out of the return side of the system). Very often it is the only term considered, but that would only be correct with fixed-position dampers, no distribution system leakage, no linear resistance components, and no duct static pressure control.
+
+The second term accounts for significant flow resistances in the system where the pressure difference is linearly proportional to the flow. Some filters and coils in the return may need this term to be adequately described. This term could be ignored if there are no linear components or if their pressure drops are very small compared to the other terms.
+
+The third term, which depends on the fan flow and square root of the supply duct pressure \emph{P\(_{sm}\)}, accounts in part for leakage from the supply system when damper positions are fixed or are changed independently of static pressure or fan flow. In this case, reducing or eliminating supply leakage results in a different system curve. This, however, might be only a minor correction to the simple system curves generally used. The third term is zero when the VAV box dampers are modulated to control flow. Consequently, with variable-position supply dampers, reducing or eliminating supply leakage does not change the system curve.
+
+The last term also accounts in part for leakage from the supply system when damper positions are fixed or are changed independently of static pressure or fan flow. This term indicates that the same fan pressure rise can be achieved by raising the duct pressure and closing dampers. The only change in the system in such a case is that the leakage flow may increase. The coefficient for this term is one when the VAV box dampers are modulated to control flow. In both cases, this term may be the most important correction to the simple system curves generally used, especially at low flows.
+
+\subsubsection{Inputs}\label{inputs-12-010}
+
+\paragraph{Field: Name}\label{field-name-12-007}
+
+The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
+
+\paragraph{Field: Fan Pressure Rise Coefficient1 C1}\label{field-fan-pressure-rise-coefficient1-c1}
+
+The required numeric constant coefficient C\emph{\(_{1}\)} (Pa s\(^{2}\)/m\(^{6}\)) in the curve. Must be greater than zero.
+
+\paragraph{Field: Fan Pressure Rise Coefficient2 C2}\label{field-fan-pressure-rise-coefficient2-c2}
+
+The required numeric constant coefficient C\emph{\(_{2}\)} (Pa s/m\(^{3}\)) in the curve\emph{.}
+
+\paragraph{Field: Fan Pressure Rise Coefficient3 C3}\label{field-fan-pressure-rise-coefficient3-c3}
+
+The required numeric constant coefficient \emph{C\(_{3}\)} (Pa\(^{0.5}\) s/m\(^{3}\)) in the curve\emph{.}
+
+\paragraph{Field: Fan Pressure Rise Coefficient4 C4}\label{field-fan-pressure-rise-coefficient4-c4}
+
+The required numeric constant coefficient C\emph{\(_{4}\)} (dimensionless) in the curve\emph{.}
+
+\paragraph{Field: Minimum Value of Qfan}\label{field-minimum-value-of-qfan}
+
+The required numeric minimum allowable value of \emph{Q\(_{fan}\)} (m\(^{3}\)/s). Values of \emph{Q\(_{fan}\)} less than the minimum will be replaced within this curve by the minimum.
+
+\paragraph{Field: Maximum Value of Qfan}\label{field-maximum-value-of-qfan}
+
+The required numeric maximum allowable value of \emph{Q\(_{fan}\)} (m\(^{3}\)/s). Values of \emph{Q\(_{fan}\)} greater than the maximum will be replaced within this curve by the maximum.
+
+\paragraph{Field: Minimum Value of Psm}\label{field-minimum-value-of-psm}
+
+The required numeric minimum allowable value of \emph{P\(_{sm}\)} (Pa). Values of \emph{P\(_{sm}\)} less than the minimum will be replaced within this curve by the minimum.
+
+\paragraph{Field: Maximum Value of Psm}\label{field-maximum-value-of-psm}
+
+The required numeric maximum allowable value of \emph{P\(_{sm}\)} (Pa). Values of \emph{P\(_{sm}\)} greater than the maximum will be replaced within this curve by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-11}
+
+The optional numeric minimum allowable value of the evaluated curve (Pa). Values less than the minimum will be replaced within this curve by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-10}
+
+The optional numeric maximum allowable value of the evaluated curve (Pa). Values greater than the maximum will be replaced within this curve by the maximum.
+
+The following is an input example describing the fan total pressure rise for a VAV system with a constant non-zero duct static pressure set point (the set point is described separately; see the Curve:Linear object for a related example):
+
+\begin{lstlisting}
+
+Curve:FanPressureRise,
+  VSD Example,                   ! Curve Name f = C1*Qfan**2+C2*Qfan+C3*Qfan*(Psm-Po)**0.5+C4*(Psm-Po) with Po = 0
+  1446.75833497653,         ! CoefficientC1 Alpha [Pa s2/m6]
+  0.,                                     ! CoefficientC2 Beta [Pa s/m3]
+  0.,                                     ! CoefficientC3 Gamma [Pa0.5 s/m3]
+  1.,                                     ! CoefficientC4 Delta [-]
+  0.,                                     ! Minimum Value of Qfan [m3/s]
+  100.,                                 ! Maximum Value of Qfan [m3/s]
+  62.5,                                 ! Minimum Value of Psm [Pa]
+  300.,                                 ! Maximum Value of Psm [Pa]
+  0.;                                     ! Minimum Curve Output [Pa]
+  5000.;                               ! Maximum Curve Output [Pa]
+\end{lstlisting}
+
+\subsection{Curve:ExponentialSkewNormal}\label{curveexponentialskewnormal}
+
+Input for the exponential-modified skew normal curve consists of the curve name, the four coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
+
+\begin{equation}
+y = \frac{{{e^{( - 0.5*Z_1^2)}}[1 + \frac{{{Z_2}}}{{\left| {{Z_2}} \right|}}*erf\left( {\frac{{\left| {{Z_2}} \right|}}{{\sqrt 2 }}} \right)}}{{{e^{( - 0.5*Z_3^2)}}[1 + \frac{{{Z_3}}}{{\left| {{Z_3}} \right|}}*erf\left( {\frac{{\left| {{Z_3}} \right|}}{{\sqrt 2 }}} \right)}}
+\end{equation}
+
+where \emph{Z\(_{1}\) =} (\emph{x C\(_{1}\)}) \emph{/ C\(_{2}\)}; \emph{Z\(_{2}\) =} {[}(\emph{exp}\(^{(*C*}\)\emph{3\(^{\*x}\)}\(^{)}\) * \emph{C\(_{4}\)*x}) \emph{- C\(_{1}\)}{]} \emph{/ C\(_{2}\)}; \emph{Z\(_{3}\) = -C\(_{1}\) / C\(_{2}\)}
+
+\subsubsection{Inputs}\label{inputs-13-008}
+
+\paragraph{Field: Name}\label{field-name-13-006}
+
+The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 C1}\label{field-coefficient1-c1}
+
+The required numeric constant coefficient \emph{C\(_{1}\)} in the curve.
+
+\paragraph{Field: Coefficient2 C2}\label{field-coefficient2-c2}
+
+The required numeric constant coefficient \emph{C\(_{2}\)} in the curve. Must be non-zero.
+
+\paragraph{Field: Coefficient3 C3}\label{field-coefficient3-c3}
+
+The required numeric constant coefficient \emph{C\(_{3}\)} in the curve.
+
+\paragraph{Field: Coefficient4 C4}\label{field-coefficient4-c4}
+
+The required numeric constant coefficient \emph{C\(_{4}\)} in the curve.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-12}
+
+The required numeric minimum allowable value of \emph{x}. Values of \emph{x} less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-13}
+
+The required numeric maximum allowable value of \emph{x}. Values of \emph{x} greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-12}
+
+The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-11}
+
+The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for x}\label{field-input-unit-type-for-x-12}
+
+This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Value of \emph{x} and Maximum Value of \emph{x} (currently dimensionless). At this time, only the \textbf{Dimensionless} option is provided so that no unit conversion is used for this curve.
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-11}
+
+This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Curve Output and Maximum Curve Output (currently dimensionless). At this time, only the \textbf{Dimensionless} option is provided so that no unit conversion is used for this curve.
+
+The following are input examples describing the normalized fan efficiency for the normal (non-stall) and stall operating regions of a backward-curved airfoil centrifugal fan:
+
+\begin{lstlisting}
+
+Curve:ExponentialSkewNormal,
+  FanEff120CPLANormal,                         ! Curve Name
+  0.072613,                                               ! CoefficientC1 Afan
+  0.833213,                                               ! CoefficientC2 Bfan
+  0.,                                                           ! CoefficientC3 Cfan
+  0.013911,                                               ! CoefficientC4 Dfan
+  -4.,                                                         ! Minimum Value of x
+  5.,                                                           ! Maximum Value of x
+  0.1,                                                         ! Minimum Curve Output
+  1.;                                                           ! Maximum Curve Output
+
+
+  Curve:ExponentialSkewNormal,
+  FanEff120CPLAStall,                           ! Curve Name
+  -1.674931,                                             ! CoefficientC1 Afan
+  1.980182,                                               ! CoefficientC2 Bfan
+  0.,                                                           ! CoefficientC3 Cfan
+  1.844950,                                               ! CoefficientC4 Dfan
+  -4.,                                                         ! Minimum Value of x
+  5.,                                                           ! Maximum Value of x
+  0.1,                                                         ! Minimum Curve Output
+  1.;                                                           ! Maximum Curve Output
+\end{lstlisting}
+
+\subsection{Curve:Sigmoid}\label{curvesigmoid}
+
+Input for the sigmoid curve consists of the curve name, the five coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
+
+\begin{equation}
+y = {C_1} + \frac{{{C_2}}}{{\left( {{{(1 + {e^{\left[ {\frac{{({C_3} - x)}}{{{C_4}}}} \right]}})}^{{C_5}}}} \right)}}
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-14-008}
+
+\paragraph{Field: Name}\label{field-name-14-005}
+
+The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 C1}\label{field-coefficient1-c1-1}
+
+The required numeric constant coefficient \emph{C\(_{1}\)} in the equation.
+
+\paragraph{Field: Coefficient2 C2}\label{field-coefficient2-c2-1}
+
+The required numeric constant coefficient \emph{C\(_{2}\)} in the equation.
+
+\paragraph{Field: Coefficient3 C3}\label{field-coefficient3-c3-1}
+
+The required numeric constant coefficient \emph{C\(_{3}\)} in the equation.
+
+\paragraph{Field: Coefficient4 C4}\label{field-coefficient4-c4-1}
+
+The required numeric constant coefficient \emph{C\(_{4}\)} in the equation.
+
+\paragraph{Field: Coefficient5 C5}\label{field-coefficient5-c5}
+
+The required numeric constant coefficient \emph{C\(_{5}\)} in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-13}
+
+The required numeric minimum allowable value of \emph{x}. Values of \emph{x} less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-14}
+
+The required numeric maximum allowable value of \emph{x}. Values of \emph{x} greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-13}
+
+The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-12}
+
+The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for x}\label{field-input-unit-type-for-x-13}
+
+This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Value of \emph{x} and Maximum Value of \emph{x} (currently dimensionless). At this time, only the \textbf{Dimensionless} option is provided so that no unit conversion is used for this curve.
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-12}
+
+This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Curve Output and Maximum Curve Output (currently dimensionless). At this time, only the \textbf{Dimensionless} option is provided so that no unit conversion is used for this curve.
+
+The following are input examples describing the normalized dimensionless flow for normal (non-stall) and stall operating regions of a backward-curved airfoil centrifugal fan:
+
+\begin{lstlisting}
+
+Curve:Sigmoid,
+  FanDimFlowNormal,                               ! Curve Name
+  0.,                                                           ! CoefficientC1 Aspd
+  1.001423,                                               ! CoefficientC2 Bspd
+  0.123935,                                               ! CoefficientC3 Cspd
+  -0.476026,                                             ! CoefficientC4 Dspd
+  1.,                                                           ! CoefficientC5 Espd
+  -4.,                                                         ! Minimum Value of x
+  5.,                                                           ! Maximum Value of x
+  0.05,                                                       ! Minimum Curve Output
+  1.;                                                           ! Maximum Curve Output
+
+  Curve:Sigmoid,
+  FanDimFlowStall,                                 ! Curve Name
+  0.,                                                           ! CoefficientC1 Aspd
+  5.924993,                                               ! CoefficientC2 Bspd
+  -1.91636,                                               ! CoefficientC3 Cspd
+  -0.851779,                                             ! CoefficientC4 Dspd
+  1.,                                                           ! CoefficientC5 Espd
+  -4.,                                                         ! Minimum Value of x
+  5.,                                                           ! Maximum Value of x
+  0.05,                                                       ! Minimum Curve Output
+  1.;                                                           ! Maximum Curve Output
+\end{lstlisting}
+
+\subsection{Curve:RectangularHyperbola1}\label{curverectangularhyperbola1}
+
+Input for the single rectangular hyperbola type 1 curve consists of the curve name, the three coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
+
+\emph{y =}(\emph{C\(_{1}\) -* x}) \emph{/} (\emph{C\(_{2}\)+x}) \emph{+ C\(_{3}\)}
+
+\subsubsection{Inputs}\label{inputs-15-008}
+
+\paragraph{Field: Name}\label{field-name-15-005}
+
+The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 C1}\label{field-coefficient1-c1-2}
+
+The required numeric constant coefficient \emph{C\(_{1}\)} in the equation.
+
+\paragraph{Field: Coefficient2 C2}\label{field-coefficient2-c2-2}
+
+The required numeric constant coefficient \emph{C\(_{2}\)} in the equation.
+
+\paragraph{Field: Coefficient3 C3}\label{field-coefficient3-c3-2}
+
+The required numeric constant coefficient \emph{C\(_{3}\)} in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-14}
+
+The required numeric minimum allowable value of \emph{x}. Values of \emph{x} less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-15}
+
+The required numeric maximum allowable value of \emph{x}. Values of \emph{x} greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-14}
+
+The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-13}
+
+The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for x}\label{field-input-unit-type-for-x-14}
+
+This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Value of \emph{x} and Maximum Value of \emph{x} (currently dimensionless). At this time, only the \textbf{Dimensionless} option is provided so that no unit conversion is used for this curve.
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-13}
+
+This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Curve Output and Maximum Curve Output (currently dimensionless). At this time, only the \textbf{Dimensionless} option is provided so that no unit conversion is used for this curve.
+
+The following is an input example describing the maximum efficiency variation for a mid- or average-efficiency type of motor:
+
+\begin{lstlisting}
+
+Curve:RectangularHyperbola1,
+  MotorMaxEffAvg,                                   ! Curve Name
+  0.29228,                                                 ! CoefficientC1
+  3.368739,                                               ! CoefficientC2
+  0.762471,                                               ! CoefficientC3
+  0.,                                                           ! Minimum Value of x
+  7.6,                                                         ! Maximum Value of x
+  0.01,                                                       ! Minimum Curve Output
+  1.;                                                           ! Maximum Curve Output
+\end{lstlisting}
+
+\subsection{Curve:RectangularHyperbola2}\label{curverectangularhyperbola2}
+
+Input for the single rectangular hyperbola type 2 curve consists of the curve name, the three coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
+
+\emph{y =}(\emph{C\(_{1}\) -* x}) \emph{/} (\emph{C\(_{2}\)+x}) \emph{+ C\(_{3}\) -* x}
+
+\subsubsection{Inputs}\label{inputs-16-007}
+
+\paragraph{Field: Name}\label{field-name-16-005}
+
+The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 C1}\label{field-coefficient1-c1-3}
+
+The required numeric constant coefficient \emph{C\(_{1}\)} in the equation.
+
+\paragraph{Field: Coefficient2 C2}\label{field-coefficient2-c2-3}
+
+The required numeric constant coefficient \emph{C\(_{2}\)} in the equation.
+
+\paragraph{Field: Coefficient3 C3}\label{field-coefficient3-c3-3}
+
+The required numeric constant coefficient \emph{C\(_{3}\)} in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-15}
+
+The required numeric minimum allowable value of \emph{x}. Values of \emph{x} less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-16}
+
+The required numeric maximum allowable value of \emph{x}. Values of \emph{x} greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-15}
+
+The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-14}
+
+The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for x}\label{field-input-unit-type-for-x-15}
+
+This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Value of \emph{x} and Maximum Value of \emph{x} (currently dimensionless). At this time, only the \textbf{Dimensionless} option is provided so that no unit conversion is used for this curve.
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-14}
+
+This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Curve Output and Maximum Curve Output (currently dimensionless). At this time, only the \textbf{Dimensionless} option is provided so that no unit conversion is used for this curve.
+
+The following are input examples describing part-load efficiency variations for a medium efficiency type of V-belt (Regions 1 and 3), for a mid- or average-efficiency nominal 25 hp 4-pole motor, and a nominal 30 hp VFD:
+
+\begin{lstlisting}
+
+Curve:RectangularHyperbola2,
+  BeltPartLoadRegion1,                         ! Curve Name
+  0.920797,                                               ! CoefficientC1
+  0.0262686,                                             ! CoefficientC2
+  0.151594,                                               ! CoefficientC3
+  0.,                                                           ! Minimum Value of x
+  1.,                                                           ! Maximum Value of x
+  0.01,                                                       ! Minimum Curve Output
+  1.;                                                           ! Maximum Curve Output
+
+  Curve:RectangularHyperbola2,
+  BeltPartLoadRegion3,                         ! Curve Name
+  1.037778,                                               ! CoefficientC1
+  0.0103068,                                             ! CoefficientC2
+  -0.0268146,                                           ! CoefficientC3
+  0.,                                                           ! Minimum Value of x
+  1.,                                                           ! Maximum Value of x
+  0.01,                                                       ! Minimum Curve Output
+  1.;                                                           ! Maximum Curve Output
+
+  Curve:RectangularHyperbola2,
+  MotorPartLoad,                                     ! Curve Name
+  1.137209,                                               ! CoefficientC1
+  0.0502359,                                             ! CoefficientC2
+  -0.0891503,                                           ! CoefficientC3
+  0.,                                                           ! Minimum Value of x
+  1.,                                                           ! Maximum Value of x
+  0.01,                                                       ! Minimum Curve Output
+  1.;                                                           ! Maximum Curve Output
+
+  Curve:RectangularHyperbola2,
+  VFDPartLoad,                                         ! Curve Name
+  0.987405,                                               ! CoefficientC1
+  0.0155361,                                             ! CoefficientC2
+  -0.0059365,                                           ! CoefficientC3
+  0.,                                                           ! Minimum Value of x
+  1.,                                                           ! Maximum Value of x
+  0.01,                                                       ! Minimum Curve Output
+  1.;                                                           ! Maximum Curve Output
+\end{lstlisting}
+
+\subsection{Curve:ExponentialDecay}\label{curveexponentialdecay}
+
+Input for the exponential decay curve consists of the curve name, the three coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
+
+\emph{y = C\(_{1}\) + C\(_{2}\) * exp}\(^{*C*}\)\emph{3\(^{*x}\)}\(^{)}\)
+
+\subsubsection{Inputs}\label{inputs-17-005}
+
+\paragraph{Field: Name}\label{field-name-17-004}
+
+The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 C1}\label{field-coefficient1-c1-4}
+
+The required numeric constant coefficient \emph{C\(_{1}\)} in the equation.
+
+\paragraph{Field: Coefficient2 C2}\label{field-coefficient2-c2-4}
+
+The required numeric constant coefficient \emph{C\(_{2}\)} in the equation.
+
+\paragraph{Field: Coefficient3 C3}\label{field-coefficient3-c3-4}
+
+The required numeric constant coefficient \emph{C\(_{3}\)} in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-16}
+
+The required numeric minimum allowable value of \emph{x}. Values of \emph{x} less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-17}
+
+The required numeric maximum allowable value of \emph{x}. Values of \emph{x} greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-16}
+
+The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-15}
+
+The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
+
+\paragraph{Field: Input Unit Type for x}\label{field-input-unit-type-for-x-16}
+
+This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Value of \emph{x} and Maximum Value of \emph{x} (currently dimensionless). At this time, only the \textbf{Dimensionless} option is provided so that no unit conversion is used for this curve.
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-15}
+
+This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Curve Output and Maximum Curve Output (currently dimensionless). At this time, only the \textbf{Dimensionless} option is provided so that no unit conversion is used for this curve.
+
+The following is an input example describing the part-load efficiency variation for a medium efficiency type of V-belt (Region 2):
+
+\begin{lstlisting}
+
+Curve:ExponentialDecay,
+  BeltPartLoadRegion2,                         ! Curve Name
+  1.011965,                                               ! CoefficientC1
+  -0.339038,                                             ! CoefficientC2
+  -3.43626,                                               ! CoefficientC3
+  0.,                                                           ! Minimum Value of x
+  1.,                                                           ! Maximum Value of x
+  0.01,                                                       ! Minimum Curve Output
+  1.;                                                           ! Maximum Curve Output
+\end{lstlisting}
+
+\subsection{Curve:DoubleExponentialDecay}\label{curvedoubleexponentialdecay}
+
+Input for the double exponential decay curve consists of the curve name, the five coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve include the minimum and maximum output of the performance curve. The equation is:
+
+\begin{equation}
+y = {C_1} + {C_2}{\exp ^{({C_3}x)}} + {C_4}{\exp ^{({C_5}x)}}
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-18-005}
+
+\paragraph{Field: Name}\label{field-name-18-004}
+
+This field indicates the required user-assigned name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
+
+\paragraph{Field: Coefficient1 C1}\label{field-coefficient1-c1-5}
+
+The required numeric constant coefficient C\(_{1}\) in the equation.
+
+\paragraph{Field: Coefficient2 C2}\label{field-coefficient2-c2-5}
+
+The required numeric constant coefficient C\(_{2}\) in the equation.
+
+\paragraph{Field: Coefficient3 C3}\label{field-coefficient3-c3-5}
+
+The required numeric constant coefficient C\(_{3}\) in the equation.
+
+\paragraph{Field: Coefficient4 C4}\label{field-coefficient4-c4-2}
+
+The required numeric constant coefficient C\(_{4}\) in the equation.
+
+\paragraph{Field: Coefficient5 C5}\label{field-coefficient5-c5-1}
+
+The required numeric constant coefficient C\(_{5}\) in the equation.
+
+\paragraph{Field: Minimum Value of x}\label{field-minimum-value-of-x-17}
+
+The required numeric minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum
+
+\paragraph{Field: Maximum Value of x}\label{field-maximum-value-of-x-18}
+
+The required numeric maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-17}
+
+The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-16}
+
+The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum
+
+\paragraph{Field: Input Unit Type for x}\label{field-input-unit-type-for-x-17}
+
+The optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum and Maximum Value of x. Currently, only Dimensionless option is provided so that no unit conversion is used for this curve
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-16}
+
+The optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum and Maximum Curve Ouput. Currently, only Dimensionless option is provided so that no unit conversion is used for this curve.
+
+An example input of the Curve:DoubleExponentialDecay input is:
+
+\begin{lstlisting}
+
+Curve:DoubleExponentialDecay,
+  BatteryCycleCurve,         !- Name
+  1380,                                   !- Coefficient1 C1
+  6834,                                   !- Coefficient2 C2
+  -8.75,                                 !- Coefficient3 C3
+  6747,                                   !- Coefficient4 C4
+  -6.22,                                 !- Coefficient5 C5
+  0,                                         !- Minimum Value of x
+  1.0;                                     !- Maximum Value of x
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-021}
+
+\paragraph{Performance Curve Output Value}\label{performance-curve-output-value}
+
+The current value of the performance curve. This value is averaged over the time step being reported. Inactive or unused performance curves will show a value of -999 (e.g., equipment is off, a specific performance curve is not required for this aspect of the equipment model at this time step, etc.). This value means that the performance curve was not called during the simulation and, therefore, not evaluated. This inactive state value is only set at the beginning of each environment. When averaging over long periods of time, this inactive state value may skew results. In this case, use a detaled reporting frequency (ref. Output:Variable object) to view results at each HVAC time step.
+
+\paragraph{\texorpdfstring{Performance Curve Input Variable 1(-N) Value {[]}}{Performance Curve Input Variable 1(-N) Value }}\label{performance-curve-input-variable-1-n-value}
+
+The current value of the nth independent variable passed to the performance curve. The order of the independent variables is in the same order as the model equation represented by this performance curve object. This value is averaged over the time step being reported.
+
+HVAC,Average,Performance Curve Output Value {[]}
+
+HVAC,Average,Performance Curve Input Variable 1 Value {[]}
+
+HVAC,Average,Performance Curve Input Variable 2 Value {[]}
+
+HVAC,Average,Performance Curve Input Variable 3 Value {[]}
diff --git a/doc/input-output-reference/src/overview/group-performance-tables.tex b/doc/input-output-reference/src/overview/group-performance-tables.tex
new file mode 100644
index 00000000000..f45a00a3c72
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+++ b/doc/input-output-reference/src/overview/group-performance-tables.tex
@@ -0,0 +1,802 @@
+\section{Group Performance Tables}\label{group-performance-tables}
+
+This group of objects consists of tabular data which are used to characterize the performance of HVAC equipment. The use of performance tables eliminate the need to perform a regression analysis to calculate the performance curve equation coefficients. Two performance tables are available to represent any performance curve having one or two independent variables. The tabular data is entered as data pairs and represent each independent variable followed by the table output at that condition. When using these two performance table objects, a regression analysis may be performed during the simulation to create the associated performance curve. The regression analysis is performed when the user requests to evaluate the curve to the limits specified (see Interpolation Method input field). The performance curve that is created is used throughout the simulation and is also written to the eio file when the user sets the diagnostics output flag DisplayAdvancedVariables (ref. Output:Diagnostics, DisplayAdvancedVariables) This performance curve object may be directly used in future input files. The following descriptions define the input requirements for the performance table objects.
+
+\subsection{Table:OneIndependentVariable}\label{tableoneindependentvariable}
+
+Input for the data table consists of a table name, the curve type, the interpolation method, and the data pairs representing the polynomial equation. Optional inputs for minimum and maximum values for the independent variable and curve minimum and maximum may be used to limit the output of the table when evaluating the regression curve (e.g., limit extrapolation). The existing performance curves represented by this table object are:
+
+\begin{equation}
+Linear\,\,Curve:\,\,\,Output = {C_1} + {C_2}x
+\end{equation}
+
+\begin{equation}
+Quadratic\,\,Curve:\,\,\,Output = {C_1} + {C_2}x + {C_3}{x^2}
+\end{equation}
+
+\begin{equation}
+Cubic\,\,Curve:\,\,\,Output = {C_1} + {C_2}x + {C_3}{x^2} + {C_4}{x^3}
+\end{equation}
+
+\begin{equation}
+Quartic\,\,Curve:\,\,\,Output = {C_1} + {C_2}x + {C_3}{x^2} + {C_4}{x^3} + {C_5}{x^4}
+\end{equation}
+
+\begin{equation}
+Exponent\,\,Curve:\,\,\,Output = {C_1} + {C_2}{x^{{C_3}}}
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-032}
+
+\paragraph{Field: Name}\label{field-name-031}
+
+A unique user assigned name for an instance of a performance table. When a table is used, it is referenced by this name. The name of this table object may be used anywhere a valid performance curve object is allowed.
+
+\paragraph{Field: Curve Type}\label{field-curve-type}
+
+The form of the polynomial equation used to represent the tabular data. Choices are \emph{Linear}, \emph{Quadratic}, \emph{Cubic}, \emph{Quartic} and \emph{Exponent}. This field is used to determine if this table object is representative of the type of performance table (curve) allowed for a particular application (i.e., if this type of polynomial is allowed to be used as the curve type for other objects). This input infers the polynomial order (or degree). This input also specifies the number of interpolation points if the next field, Interpolation Method is set to LagrangeInterpolationLinearExtrapolation. The number of interpolation points for Linear, Quadratic, Cubic, Quartic, and Exponent are set at 2, 3, 4, 5, and 4, respectively.
+
+\paragraph{Field: Interpolation Method}\label{field-interpolation-method}
+
+The method used to evaluate the tabular data. Choices are \emph{LinearInterpolationOfTable, LagrangeInterpolationLinearExtrapolation} and \emph{EvaluateCurveToLimits}. When \emph{LinearInterpolationOfTable} is selected, the tabular data is interpolated within the limits of the data set and the following fields are used only within the boundary of the table limits (i.e., are only used to limit interpolation). Extrapolation of the data set is not allowed. When \emph{LagrangeInterpolationLinearExtrapolation} is selected, a polynomial interpolation routine is used within the table boundaries along with linear extrapolation. Given the valid one independent variable equations above, the polynomial order is up to 5\(^{th}\) order. When \emph{EvaluateCurveToLimits} is selected, the coefficients (i.e., C in the equations above) of the polynomial equation are calculated and used to determine the table output within the limits specified in the following fields. If these fields are not entered, the limits of the tabular data are used. The minimum number of data pairs required for this choice are 2, 3, 4, 5, and 4 data pairs for linear, quadratic, cubic, quartic, and exponent curves, respectively. If insufficient data is provided, the regression analysis is not performed and the simulation reverts to interpolating the tabular data. The performance curve is written to the eio file when the output diagnotics flag DisplayAdvancedVariables is used (ref. Output:Diagnostics, DisplayAdvancedVariables).
+
+\paragraph{Field: Minimum Value of X}\label{field-minimum-value-of-x-000}
+
+The minimum allowable value of X. Values of X less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method}. If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Maximum Value of X}\label{field-maximum-value-of-x-000}
+
+The maximum allowable value of X. Values of X greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method}. If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Minimum Table Output}\label{field-minimum-table-output}
+
+The minimum allowable value of the table output. Values less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method}. If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Maximum Table Output}\label{field-maximum-table-output}
+
+The maximum allowable value of the table output. Values greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method}. If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Input Unit Type for X1}\label{field-input-unit-type-for-x1}
+
+This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of X. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-000}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Normalization Reference}\label{field-normalization-reference}
+
+The normalization point for the data set. This field provides a method for automatically normalizing a set of data. Equipment performance data is typically normalized based on a specific operating condition. Both the output values and minimum/maximum curve limits are normalized. This normalization can be performed simply by entering the data at the reference point. If this field is left blank or a 1 is entered, the data set is assumed to be in the correct format.
+
+\paragraph{Data Pairs}\label{data-pairs}
+
+The following inputs describe the data set. Data pairs are entered as X and Output pairs where X is the independent variable (i.e., x in the equation above) and Output is the dependent variable (i.e., Output in the equation above). Any number of data pairs may be entered, however, a minimum number of data pairs must be entered and depends on the polynomial equation. Linear (1\(^{st}\) order), Quadratic (2\(^{nd}\) order), Cubic (3\(^{rd}\) order), Quartic (4\(^{th}\) order), and Exponent (nth order) polynomials require a minimum of 2, 3, 4, 5, and 4 data pairs, respectively. This minimum requirement is for performing a regression analysis, not interpolating the tabular data. If a regression analysis is not performed (i.e., only table interpolation is used), these minimum requirements are not enforced. If a regression analysis is performed and these minimum requirements are not met, the simulation will revert to table interpolation. These fields may be repeated as many times as necessary to define the tabular data.
+
+\paragraph{Field: X Value \#n}\label{field-x-value-n}
+
+The value of the independent variable n (i.e., independent variable values for data 1 to number of data pairs).
+
+\paragraph{Field: Output Value \#n}\label{field-output-value-n}
+
+The value of the dependent variable n (i.e., dependent variable values for data 1 to number of data pairs).
+
+Following is an example input for a Table:OneIndependentVariable object:
+
+\begin{lstlisting}
+
+Table:OneIndependentVariable,
+  WindACCoolCapFFF,             !- Name
+  Linear,                                 !- Curve Type
+  EvaluateCurveToLimits,   !- Interpolation Type
+  0,                                           !- Minimum Value of X1,
+  1.5,                                       !- Maximum Value of X1,
+  0.8,                                       !- Minimum Table Output
+  1.1,                                       !- Maximum Table Output
+  Dimensionless,                   !- Input Unit Type for X1
+  Dimensionless,                   !- Output Unit Type
+  ,                                             !- Normalization Point
+  0,0.8,                                   !- X Value #1, Output Value #1
+  1.5,1.1;                               !- X Value #2, Output Value #2
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-022}
+
+\paragraph{\texorpdfstring{Performance Curve Output Value {[]}}{Performance Curve Output Value }}\label{performance-curve-output-value-000}
+
+The current value of the performance table. Performance curves and tables use the same output variable. This value is averaged over the time step being reported. Inactive or unused performance curves will show a value of -999 (e.g., equipment is off, a specific performance curve is not required for this aspect of the equipment model at this time step, etc.). This value means that the performance curve was not called during the simulation and, therefore, not evaluated. This inactive state value is only set at the beginning of each environment. When averaging over long periods of time, this inactive state value may skew results. In this case, use a detaled reporting frequency (ref. Output:Variable object) to view results at each HVAC time step.
+
+\paragraph{\texorpdfstring{Performance Curve Input Variable 1 Value {[]}}{Performance Curve Input Variable 1 Value }}\label{performance-curve-input-variable-1-value}
+
+The current value of the independent variable passed to the performance curve. This value is averaged over the time step being reported.
+
+HVAC,Average,Performance Curve Output Value {[]}
+
+HVAC,Average,Performance Curve Input Variable 1 Value {[]}
+
+\subsection{Table:TwoIndependentVariables}\label{tabletwoindependentvariables}
+
+Input for the data table consists of a table name, the curve type, the interpolation method, and the data pairs representing the polynomial equation. Optional inputs for minimum and maximum values for the independent variable, and curve minimum and maximum may be used to limit the output of the table (e.g., limit extrapolation) when evaluating the regression curve instead of the tabular data. The polynomial equations currently represented by this table object are:
+
+\begin{equation}
+BiQuadratic\,\,Curve:\,\,\,\,Output = {C_1} + {C_2}x + {C_3}{x^2} + {C_4}y + {C_5}{y^2} + {C_6}xy
+\end{equation}
+
+\begin{equation}
+QuadraticLinear\,\,Curve:\,\,\,\,Output = {C_1} + {C_2}x + {C_3}{x^2} + {C_4}y + {C_5}xy + {C_6}{x^2}y
+\end{equation}
+
+\subsubsection{Inputs}\label{inputs-1-029}
+
+\paragraph{Field: Name}\label{field-name-1-028}
+
+A unique user assigned name for an instance of a performance table. When a table is used, it is referenced by this name. The name of this table object may be used anywhere a valid performance curve object is allowed.
+
+\paragraph{Field: Curve Type}\label{field-curve-type-1}
+
+The form of the polynomial equation represented by the entered data. The only valid choices are \emph{BiQuadratic} and \emph{QuadraticLinear}. This field is used to determine if this table object is representative of the type of performance table (curve) allowed for a particular equipment model (i.e., if this type of polynomial is allowed to be used as the curve type for specific input fields). A minimum of 6 data pairs are required when selecting \emph{EvaluateCurveToLimits} in the following field. This input also specifies the number of interpolation points if the next field, Interpolation Method is set to LagrangeInterpolationLinearExtrapolation. The number of interpolation points for BiQuadratic and QuadraticLinear are set at 6.
+
+\paragraph{Field: Interpolation Method}\label{field-interpolation-method-1}
+
+The method used to evaluate the tabular data. Choices are \emph{LinearInterpolationOfTable, LagrangeInterpolationLinearExtrapolation,} and \emph{EvaluateCurveToLimits}. When \emph{LinearInterpolationOfTable} is selected, the data entered is evaluated within the limits of the data set and the following fields are used only within the boundary of the table limits (i.e., are only used to limit interpolation). A complete data set is required. For each X variable, entries must include all Y variables and associated curve output (i.e., a complete table, no gaps or missing data). Extrapolation of the data set is not allowed. When Lagrange\emph{InterpolationLinearExtrapolation} is selected, a polynomial interpolation routine is used within the table boundaries along with linear extrapolation. Given the valid equations above, the polynomial order is fixed at 2 which infers that 3 data points will be used for interpolation. When \emph{EvaluateCurveToLimits} is selected, the coefficients (i.e., C in the equations above) of the polynomial equation are calculated and used to determine the table output within the limits specified in the following fields (or the tabular data, whichever provide the larger range). If the following fields are not entered, the limits of the data set are used. A complete table is not required when using this method, however, a minimum number of data is required to perform the regression analysis. The minimum number of data pairs required for this choice is 6 data pairs for both bi-quadratic and quadratic-linear curve types. If insufficient data is provided, the simulation reverts to interpolating the tabular data. The performance curve is written to the eio file when the output diagnotics flag DisplayAdvancedVariables is used (ref. Output:Diagnostics, DisplayAdvancedVariables).
+
+\paragraph{Field: Minimum Value of X}\label{field-minimum-value-of-x-1-000}
+
+The minimum allowable value of X. Values of X less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method}. If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Maximum Value of X}\label{field-maximum-value-of-x-1-000}
+
+The maximum allowable value of X. Values of X greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method}. If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Minimum Value of Y}\label{field-minimum-value-of-y-000}
+
+The minimum allowable value of Y. Values of Y less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method}. If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Maximum Value of Y}\label{field-maximum-value-of-y-000}
+
+The maximum allowable value of Y. Values of Y greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method}. If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Minimum Table Output}\label{field-minimum-table-output-1}
+
+The minimum allowable value of the table output. Values less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method}. If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Maximum Table Output}\label{field-maximum-table-output-1}
+
+The maximum allowable value of the table output. Values greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method}. If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Input Unit Type for X}\label{field-input-unit-type-for-x-000}
+
+This field is used to indicate the kind of units that may be associated with the X values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of X. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for Y}\label{field-input-unit-type-for-y-000}
+
+This field is used to indicate the kind of units that may be associated with the Y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Y and Maximum Value of Y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-1-000}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Normalization Reference}\label{field-normalization-reference-1}
+
+The normalization point for the data set. This field provides a method for automatically normalizing a set of data. Equipment performance data is typically normalized based on a specific operating condition. Both the output values and minimum/maximum curve limits are normalized as applicable. This normalization can be performed simply by entering the data at the reference point. If this field is left blank or a 1 is entered, the data set is assumed to be in the correct format.
+
+\paragraph{Data Pairs}\label{data-pairs-1}
+
+The following inputs describe the data set. Data pairs are entered as X, Y and Output pairs where X and Y are the independent variables (i.e., x and y in the equations above) and Output is the dependent variable (i.e., Output in the equation above). Any number of data pairs may be entered, however, a minimum number of data pairs must be entered and depends on the polynomial equation. BiQuadratic and QuadraticLinear (2\(^{nd}\) order with 2 independent variables) require a minimum of 6 data pairs. This minimum requirement is for performing a regression analysis, not interpolating the tabular data. If a regression analysis is not performed (i.e., only table interpolation is used), these minimum requirements are not enforced. If a regression analysis is performed and these minimum requirements are not met, the simulation will revert to table interpolation. These fields may be repeated as many times as necessary to define the tabular data.
+
+\paragraph{Field: X Value \#n}\label{field-x-value-n-1}
+
+The value of the first independent variable n (i.e., first independent variable values for data pair 1 to number of data pairs).
+
+\paragraph{Field: Y Value \#n}\label{field-y-value-n}
+
+The value of the second independent variable n (i.e., second independent variable values for data pair 1 to number of data pairs).
+
+\paragraph{Field: Output Value \#n}\label{field-output-value-n-1}
+
+The value of the dependent variable n (i.e., dependent variable values for data pair 1 to number of data pairs).
+
+Following is an example input for a Table:TwoIndependentVariable object:
+
+\begin{lstlisting}
+
+Table:TwoIndependentVariables,
+  CCOOLEIRFT,                         !- Name
+  BiQuadratic,                       !- Curve Type
+  EvaluateCurveToLimits,   !- Interpolation Type
+  5.0,                                       !- Minimum Value of x,
+  60.0,                                     !- Maximum Value of x,
+  5.0,                                       !- Minimum Value of y,
+  70.0,                                     !- Maximum Value of y,
+  0.01,                                     !- Minimum Table Output
+  0.5,                                       !- Maximum Table Output
+  Temperature,                       !- Input Unit Type for x
+  Temperature,                       !- Input Unit Type for y
+  Dimensionless,                   !- Output Unit Type
+  0.258266502,                       !- Normalization Point
+  17.2222222,18.3333333,0.18275919, !-X Value #1,Y Value #1,Output #1
+  17.2222222,23.8888889,0.207383768,!-X Value #2,Y Value #2,Output #2
+  17.2222222,29.4444444,0.237525541,!-X Value #3,Y Value #3,Output #3
+  17.2222222,35,0.274217751,               !-X Value #4,Y Value #4,Output #4
+  17.2222222,40.5555556,0.318548624,!-X Value #5,Y Value #5,Output #5
+  17.2222222,46.1111111,0.374560389,!-X Value #6,Y Value #6,Output #6
+  19.4444444,18.3333333,0.172982816,!-X Value #7,Y Value #7,Output #7
+  19.4444444,23.8888889,0.19637691, !-X Value #8,Y Value #8,Output #8
+  19.4444444,29.4444444,0.224789822,!-X Value #9,Y Value #9,Output #9
+  19.4444444,35,0.258266502,               !-X Value #10,Y Value #10,Output #10
+  19.4444444,40.5555556,0.299896794,!-X Value #11,Y Value #11,Output #11
+  19.4444444,46.1111111,0.351242021,!-X Value #12,Y Value #12,Output #12
+  21.6666667,18.3333333,0.164081122,!-X Value #13,Y Value #13,Output #13
+  21.6666667,23.8888889,0.185603303,!-X Value #14,Y Value #14,Output #14
+  21.6666667,29.4444444,0.211709812,!-X Value #15,Y Value #15,Output #15
+  21.6666667,35,0.243492052,               !-X Value #16,Y Value #16,Output #16
+  21.6666667,40.5555556,0.281757875,!-X Value #17,Y Value #17,Output #17
+  21.6666667,46.1111111,0.331185659;!-X Value #18,Y Value #18,Output #18
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-017}
+
+\paragraph{\texorpdfstring{Performance Curve Output Value {[]}}{Performance Curve Output Value }}\label{performance-curve-output-value-1}
+
+The current value of the performance table. Performance curves and tables use the same output variable. This value is averaged over the time step being reported. Inactive or unused performance curves will show a value of -999 (e.g., equipment is off, a specific performance curve is not required for this aspect of the equipment model at this time step, etc.). This value means that the performance curve was not called during the simulation and, therefore, not evaluated. This inactive state value is only set at the beginning of each environment. When averaging over long periods of time, this inactive state value may skew results. In this case, use a detaled reporting frequency (ref. Output:Variable object) to view results at each HVAC time step.
+
+\paragraph{\texorpdfstring{Performance Curve Input Variable 1 Value {[]}}{Performance Curve Input Variable 1 Value }}\label{performance-curve-input-variable-1-value-1}
+
+\paragraph{\texorpdfstring{Performance Curve Input Variable 2 Value {[]}}{Performance Curve Input Variable 2 Value }}\label{performance-curve-input-variable-2-value}
+
+The current value of the first and second independent variable passed to the performance curve. The order of the independent variables is in the same order as the model equation represented by this performance curve object. This value is averaged over the time step being reported.
+
+\begin{itemize}
+\item
+  HVAC,Average,Performance Curve Output Value {[]}
+\item
+  HVAC,Average,Performance Curve Input Variable 1 Value {[]}
+\item
+  HVAC,Average,Performance Curve Input Variable 2 Value {[]}
+\end{itemize}
+
+\subsection{Lookup Tables}\label{lookup-tables}
+
+Lookup tables are useful for determining the results of a nth order polynomial without the need to calculate the polynomial coefficients. The Lagrange method for interpolation is currently the only method available for polynomial interpolation. LinearInterpolationOfTable and EvaluateCurveToLimits may also be used. The multi-variable lookup table can represent from 1 to 5 independent variables and can interpolate these independent variables up to a 4\(^{th}\) order polynomial. The polynomial order is assumed to be the number of interpolation points (n) minus 1. Polynomial interpolation of tabular data takes place when the values of the independent variables are within the upper table boundary and at least n data points are available when approaching the lower table boundary for any independent variable. When any independent variable value is outside the table limits, linear extrapolation is used to predict the table result and is based on the two nearest data points in the table for that particular independent variable.
+
+\subsection{Table:MultiVariableLookup}\label{tablemultivariablelookup}
+
+Input for the multi-variable data table consists of a table name, the interpolation method, the number of points to be used for interpolation, an optional external file name, and, if an external file name is not entered, the tabular data. Optional inputs for minimum and maximum values for the independent variable, and curve minimum and maximum may be used to limit the output of the table (e.g., limit extrapolation).
+
+\subsubsection{Inputs}\label{inputs-2-027}
+
+\paragraph{Field: Name}\label{field-name-2-026}
+
+A unique user assigned name for an instance of a lookup table. When a table is used, it is referenced by this name. The name of this table object may be used anywhere a valid performance curve object is allowed.
+
+\paragraph{Field: Curve Type}\label{field-curve-type-2}
+
+The order of the polynomial used to represent the tabular data. Choices are \emph{Linear}, \emph{Quadratic}, \emph{Cubic}, \emph{Quartic, BiQuadratic, QaudraticLinear, BuCibic}. This field is used to determine if this table object is representative of the type of performance table (curve) allowed for a particular application (i.e., if this type of polynomial is allowed to be used as the curve type for other objects). This input also infers the polynomial order (or degree).
+
+\paragraph{Field: Interpolation Method}\label{field-interpolation-method-2}
+
+The method used to evaluate the lookup table. The choices are \emph{LinearInterpolationOfTable, LagrangeInterpolationLinearExtrapolation, and EvaluateCurveToLimits}. . When \emph{LinearInterpolationOfTable} is selected, the data entered is evaluated within the limits of the data set and the minimum/maximum value of x and output inputs are used only within the boundary of the table limits (i.e., are only used to limit interpolation). A complete data set is required. For each X variable, entries must include all Y variables and associated curve output (i.e., a complete table, no gaps or missing data). Extrapolation of the data set is not allowed. When \emph{LagrangeInterpolationLinearExtrapolation} is selected, the lookup table is evaluated using Lagrange s form of the interpolating polynomial. The order of the polynomial is inferred to be one less than the input in the Number of Interpolation Points field below. When \emph{EvaluateCurveToLimits} is selected, the coefficients (i.e., C in the equation above) of the polynomial equation are calculated and used to determine the table output within the limits specified in the following fields (or the tabular data, whichever provide the larger range). If the minimum/maximum fields below are not entered, the limits of the data set are used. A complete table is not required when using this method, however, a minimum number of data is required to perform the regression analysis. The minimum number of data pairs required for this choice is 6 data pairs for both bi-quadratic and quadratic-linear curve types. If insufficient data is provided, the simulation reverts to interpolating the tabular data. The performance curve is written to the eio file when the output diagnotics flag DisplayAdvancedVariables is used (ref. Output:Diagnostics, DisplayAdvancedVariables). A regression analysis may only be performed on lookup tables with one or two independent variables.
+
+\paragraph{Field: Table Data Format}\label{field-table-data-format}
+
+The format specifier which determines the method used to read the lookup table. The only valid choice at this time is \emph{SingleLineIndependentVariableWithMatrix}. When \emph{SingleLineIndependentVariableWithMatrix} is selected, a free format is used as shown below. The format shown below assumes the output values are in ascending order for both independent variables 1 and 2. Tabular data are entered in 3 groups of data, the header, the independent variable values, and the tabular data matrix. A summary of the external file format is shown below.
+
+Key:
+
+\begin{itemize}
+\item
+  IV = independent variable (i.e., the X1, or X2, etc)
+\item
+  NIV = number of independent variables (i.e., number of values for X1, or X2, etc.)
+\item
+  IVV = independent variable value (i.e., the value for X1, or X2, etc.)
+\item
+  NIV1 = number of values for independent variable \#1 (i.e., X1)
+\item
+  NIV2 = number of values for independent variable \#2 (i.e., X2)
+\item
+  NIV3 = number of values for independent variable \#3 (i.e., X3)
+\item
+  NIV4 = number of values for independent variable \#4 (i.e., X4)
+\item
+  NIV5 = number of values for independent variable \#5 (i.e., X5)
+\item
+  OV = output value 
+\end{itemize}
+
+\begin{lstlisting}
+Header: Row 1: <NIV>, <NIV1>, <NIV2> (only used if NIV>1), <NIV3> (only used if NIV>2), <NIV4> (only used if NIV>3), <NIV5> (only used if NIV>4)
+\end{lstlisting}
+
+\begin{lstlisting}
+Independent Variable Values: Row 2: <IVV1 to IVVn for IV1> where n = NIV1 (max = 10) Row 2a (row included only when NIV > 1): IVV1 to IVVn for IV2 where n = NIV2 (max = 10) Row 2b (row included only when NIV > 2): IVV1 to IVVn for IV3 where n = NIV3 (max = 10) Row 2c (row included only when NIV > 3): IVV1 to IVVn for IV4 where n = NIV4 (max = 10) Row 2d (row included only when NIV > 4): IVV1 to IVVn for IV5 where n = NIV5 (max = 10)
+\end{lstlisting}
+
+\begin{lstlisting}
+Tabular Data Matrix Format (repeat rows 3 and 4(1) 4(m) for each occurrence of a unique data pair for independent variable \#3, \#4, and \#5):
+\end{lstlisting}
+
+\begin{lstlisting}
+Row 3 (row included only when NIV > 2): IVVn for IV3, IVVn for IV4 (included only when NIV > 3), IVVn for IV5 (included only when NIV > 4), (where n = a unique value for the independent variable)
+\end{lstlisting}
+
+\begin{lstlisting}
+Row 4(1): OV1/1 to OVn/1 for each value of IV1 where n = NIV1 representing IV2(1) Row 4(2): OV1/2 to OVn/2 for each value of IV1 where n = NIV1 representing IV2(2) Row 4(3): OV1/3 to OVn/3 for each value of IV1 where n = NIV1 representing IV2(3) ... Row 4(m): OV1/m to OVn/m for each value of IV1 where n = NIV1 representing IV2(m) where m = NIV2
+\end{lstlisting}
+
+\paragraph{Field: Number of Interpolation Points}\label{field-number-of-interpolation-points}
+
+This field specifies the number of data points to be used in the lookup table interpolation. The value specified in this field should be 1 greater than the order (or degree) of the polynomial used for interpolation. For example, if 2 is entered here, the polynomial is assumed to be first order where only 2 data points are required to calculate the table solution. If 3 is entered here, the polynomial is assumed to be second order and 3 data points would be required to calculate the table solution. Linear extrapolation is always used when the independent variable values are near the lower edge or outside the range of the table. The interpolation points selected are always the nearest data point greater than the independent variable with 1 or more values less than the independent variable. For example, if 3 interpolation points are used, the data point greater than the independent variable and 2 data points less than the indpenedent variable are used to determine the table solution. If the independent variable exactly equals a table reference point, that value is used as the table solution.
+
+\paragraph{Field: External File Name}\label{field-external-file-name}
+
+The name of an external file that represents the tabular data. This file would include all data after the Output Unit Type field below starting with the number of independent variables and continuing until all input and output values have been entered. The tabular data may use either comma, space or tab delimited format. The field should include a full path with file name, for best results. The field must be \textless{} = 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
+
+\paragraph{Field: X1 Sort Order}\label{field-x1-sort-order}
+
+The choice field specifies the order of the lookup table data for the 1\(^{st}\) independent variable. Valid choices are \emph{Increasing} or \emph{Decreasing}. If increasing is selected, then the order of the data is from lowest value of the 1\(^{st}\) independent variable to highest. If decreasing is selected, then the order of the data is from highest value of the 1\(^{st}\) independent variable to lowest.
+
+\paragraph{Field: X2 Sort Order}\label{field-x2-sort-order}
+
+The choice field specifies the order of the lookup table data for the 2\(^{nd}\) independent variable. Valid choices are \emph{Increasing} or \emph{Decreasing}. If increasing is selected, then the order of the data is from lowest value of the 2\(^{nd}\) independent variable to highest. If decreasing is selected, then the order of the data is from highest value of the 2\(^{nd}\) independent variable to lowest.
+
+\paragraph{Field: Minimum Value of X1}\label{field-minimum-value-of-x1}
+
+The minimum allowable value of X1. Values of X1 less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Maximum Value of X1}\label{field-maximum-value-of-x1}
+
+The maximum allowable value of X1. Values of X1 greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Minimum Value of X2}\label{field-minimum-value-of-x2}
+
+The minimum allowable value of X2. Values of X2 less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 1.
+
+\paragraph{Field: Maximum Value of X2}\label{field-maximum-value-of-x2}
+
+The maximum allowable value of X2. Values of X2 greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 1.
+
+\paragraph{Field: Minimum Value of X3}\label{field-minimum-value-of-x3}
+
+The minimum allowable value of X3. Values of X3 less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 2.
+
+\paragraph{Field: Maximum Value of X3}\label{field-maximum-value-of-x3}
+
+The maximum allowable value of X3. Values of X3 greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 2.
+
+\paragraph{Field: Minimum Value of X4}\label{field-minimum-value-of-x4}
+
+The minimum allowable value of X4. Values of X4 less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 3.
+
+\paragraph{Field: Maximum Value of X4}\label{field-maximum-value-of-x4}
+
+The maximum allowable value of X4. Values of X4 greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 3.
+
+\paragraph{Field: Minimum Value of X5}\label{field-minimum-value-of-x5}
+
+The minimum allowable value of X5. Values of X5 less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 4.
+
+\paragraph{Field: Maximum Value of X5}\label{field-maximum-value-of-x5}
+
+The maximum allowable value of X5. Values of X5 greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 4.
+
+\paragraph{Field: Minimum Curve Output}\label{field-minimum-curve-output-000}
+
+The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Maximum Curve Output}\label{field-maximum-curve-output-000}
+
+The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the \emph{Interpolation Method} is selected as \emph{EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation}. This filed can be used to limit interpolation using any \emph{Interpolation Method.} If this field is left blank, the data set determines the limit.
+
+\paragraph{Field: Input Unit Type for X1}\label{field-input-unit-type-for-x1-1}
+
+This field is used to indicate the kind of units that may be associated with the X1 values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X1 and Maximum Value of X1. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for X2}\label{field-input-unit-type-for-x2}
+
+This field is used to indicate the kind of units that may be associated with the X2 values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X2 and Maximum Value of X2. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for X3}\label{field-input-unit-type-for-x3}
+
+This field is used to indicate the kind of units that may be associated with the X3 values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X3 and Maximum Value of X3. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for X4}\label{field-input-unit-type-for-x4}
+
+This field is used to indicate the kind of units that may be associated with the X4 values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X4 and Maximum Value of X4. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Input Unit Type for X5}\label{field-input-unit-type-for-x5}
+
+This field is used to indicate the kind of units that may be associated with the X5 values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X5 and Maximum Value of X5. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  VolumetricFlow
+\item
+  MassFlow
+\item
+  Distance
+\item
+  Power
+\end{itemize}
+
+\paragraph{Field: Output Unit Type}\label{field-output-unit-type-2-000}
+
+This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless} which will have no unit conversion.
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Capacity
+\item
+  Power
+\end{itemize}
+
+\subsection{Data Input Format}\label{data-input-format}
+
+The following inputs describe the data set. These values may also be placed in an external file starting with Field \#1. If an external file name is entered above, the following fields are not used. Data are entered in a specific order according to the number and quantity of independent variables. The data input format is described here in 3 groups as Header, Independent Variable Values, and the Tabular Data. The header is always the first line in the data set and represents the number of independent varibles followed by the number of values for each independent variable. The independent variable values are listed next and represent the values of each independent variable on a separate line. These values are only listed once at the top of the data set and are listed in ascending order. The number of independent variables, the first number in the header, specifies how many lines, or rows, make up this section of tabular data. The remaining lines are repeated as many times as necessary to completely describe the tabular data. The values of independent variables 3 n are listed on a single line followed by a matrix of data that represent the table output corresponding to independent variables 1 and 2.
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Header:}
+\end{itemize}
+
+Line 1: The first number specified is the number of independent variables followed by the number of variables for each independent variable.
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Independent Variable Values:}
+\end{itemize}
+
+Line 1: the n values for the first independent variable as specified in the header.
+
+Line 2: the n values for the second independent variable as specified in the header if the number of independent variables is greater than 1. This line is not required if the number of independent variables is less than 2.
+
+Line 3: the n values for the third independent variable as specified in the header if the number of independent variables is greater than 2. This line is not required if the number of independent variables is less than 3.
+
+Line 4: the n values for the fourth independent variable as specified in the header if the number of independent variables is greater than 3. This line is not required if the number of independent variables is less than 4.
+
+Line 5: the n values for the fifth independent variable as specified in the header if the number of independent variables is greater than 4. This line is not required if the number of independent variables is less than 5.
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Tabular Data:}
+\end{itemize}
+
+Line 1: the values of the 3\(^{rd}\) through nth independent variables
+
+Line 2 m (where m-1 equals the number of variables for the second independent variable): the tabular data corresponding to the 1\(^{st}\) independent variable (the number of inputs on this line equals the number of values for 1\(^{st}\) independent variable), the mth values for the 2\(^{nd}\) independent variable and corresponding to the values for the 3\(^{rd}\) nth independent variables (see Line 1 above for Tabular Data).
+
+Three examples are provided here as this can be difficult to describe in text. This example assumes that the table data are listed in ascending order from lowest to highest.
+
+\begin{itemize}
+\item
+  \textbf{One Independent Variable:}
+\item
+  \textbf{Header:}
+\end{itemize}
+
+1, 5, (1 independent variable with 5 values for the single independent variable)
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Independent Variable Values:}
+\end{itemize}
+
+70, 72, 74, 76, 78, (the five values for the single independent variable, these values are always listed in ascending order)
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Tabular Data:}
+\end{itemize}
+
+0.1, 0.3, 0.5, 0.7, 0.9; (the table values associated with the independent variable values listed previously Note: these values may be read in ascending or descending order based on the input in the X1 Sort Order field above). Example: If X1 Sort Order is ascending, 0.1 corresponds to the value of 70 for the first independent variable. If X1 Sort Order is descending, then 0.1 corresponds to the value of 78 for the first independent variable. The use of ascending order provides a direct correlation to inputs for the Independent Variable Values group above.
+
+\begin{itemize}
+\item
+  \textbf{Two Independent Variables:}
+\item
+  \textbf{Header:}
+\end{itemize}
+
+2, 5, 6, (2 independent variables with 5 and 6 values for the 1\(^{st}\) and 2\(^{nd}\) independent variables, respectively)
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Independent Variable Values:}
+\end{itemize}
+
+70, 72, 74, 76, 78, (the five values for the 1st independent variable, these values are always listed in ascending order)
+
+32, 45, 68, 81, 94, 107, (the six values for the 2nd independent variable, these values are always listed in ascending order)
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Tabular Data:}
+\end{itemize}
+
+0.1, 0.3, 0.5, 0.7, 0.9, (the first five table values associated with each value of the 1\(^{st}\) independent variable and the first value (32) of the second independent variable listed previously Note: these values may be listed in ascending or descending order based on the input in the X1 Sort Order field above. Each of these rows may also be listed in ascending or descending order based on the input in the X2 Sort Order field above).
+
+0.2, 0.4, 0.6, 0.8, 1.0, (the second five table values associated with each value of the 1\(^{st}\) independent variable and the second value (45) of the second independent variable listed previously).
+
+0.3, 0.5, 0.7, 0.9, 1.1, (the third five table values associated with each value of the 1\(^{st}\) independent variable and the third value (68) of the second independent variable listed previously).
+
+0.4, 0.6, 0.8, 1.0, 1.2, (the fourth five table values associated with each value of the 1\(^{st}\) independent variable and the fourth value (81) of the second independent variable listed previously).
+
+0.5, 0.7, 0.9, 1.1, 1.3, (the fifth five table values associated with each value of the 1\(^{st}\) independent variable and the fifth value (94) of the second independent variable listed previously).
+
+0.6, 0.8, 1.0, 1.2, 1.4; (the sixth five table values associated with each value of the 1\(^{st}\) independent variable and the sixth value (107) of the second independent variable listed previously).
+
+\begin{itemize}
+\item
+  \textbf{Three Independent Variables:}
+\item
+  \textbf{Header:}
+\end{itemize}
+
+3, 5, 6, 2, (3 independent variables with 5, 6 and 2 values for the 1\(^{st}\) , 2\(^{nd}\), and 3\(^{rd}\) independent variables)
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Independent Variable Values:}
+\end{itemize}
+
+70, 72, 74, 76, 78, (the five values for the 1st independent variable, these values are always listed in ascending order)
+
+32, 45, 68, 81, 94, 107, (the six values for the 2nd independent variable, these values are always listed in ascending order)
+
+15.5, 45.5, (the two values for the 3\(^{rd}\) independent variable, these values are always listed in ascending order)
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Tabular Data:}
+\end{itemize}
+
+15.5, (the first value for the 3\(^{rd}\) independent variable values for the 4\(^{th}\) and 5\(^{th}\) independent variable are also listed on this line if they are used)
+
+0.1, 0.3, 0.5, 0.7, 0.9, (the table values associated with each value of the 1\(^{st}\) independent variable, the first value (32) of the second independent variable, and the first value (15.5) of the 3\(^{rd}\) independent variable). Note: these values may be listed in ascending or descending order based on the input in the X1 Sort Order field above).
+
+0.2, 0.4, 0.6, 0.8, 1.0, (the table values associated with each value of the 1\(^{st}\) independent variable, the second value (45) of the second independent variable, and the first value (15.5) of the 3\(^{rd}\) independent variable).
+
+0.3, 0.5, 0.7, 0.9, 1.1, (the table values associated with each value of the 1\(^{st}\) independent variable, the third value (68) of the second independent variable, and the first value (15.5) of the 3\(^{rd}\) independent variable).
+
+0.4, 0.6, 0.8, 1.0, 1.2, (the table values associated with each value of the 1\(^{st}\) independent variable, the fourth value (81) of the second independent variable, and the first value (15.5) of the 3\(^{rd}\) independent variable).
+
+0.5, 0.7, 0.9, 1.1, 1.3, (the table values associated with each value of the 1\(^{st}\) independent variable, the fifth value (94) of the second independent variable, and the first value (15.5) of the 3\(^{rd}\) independent variable).
+
+0.6, 0.8, 1.0, 1.2, 1.4. (the table values associated with each value of the 1\(^{st}\) independent variable, the sixth value (107) of the second independent variable, and the first value (15.5) of the 3\(^{rd}\) independent variable).
+
+45.5, (the second value for the 3\(^{rd}\) independent variable values for the 4\(^{th}\) and 5\(^{th}\) independent variable are also listed on this line if they are used)
+
+1.1, 1.3, 1.5, 1.7, 1.9, (the table values associated with each value of the 1\(^{st}\) independent variable, the first value (32) of the second independent variable, and the second value (45.5) of the 3\(^{rd}\) independent variable).
+
+1.2, 1.4, 1.6, 1.8, 2.0, (the table values associated with each value of the 1\(^{st}\) independent variable, the second value (45) of the second independent variable, and the second value (45.5) of the 3\(^{rd}\) independent variable).
+
+1.3, 1.5, 1.7, 1.9, 2.1, (the table values associated with each value of the 1\(^{st}\) independent variable, the third value (68) of the second independent variable, and the second value (45.5) of the 3\(^{rd}\) independent variable).
+
+1.4, 1.6, 1.8, 2.0, 2.2, (the table values associated with each value of the 1\(^{st}\) independent variable, the fourth value (81) of the second independent variable, and the second value (45.5) of the 3\(^{rd}\) independent variable).
+
+1.5, 1.7, 1.9, 2.1, 2.3, (the table values associated with each value of the 1\(^{st}\) independent variable, the fifth value (94) of the second independent variable, and the second value (45.5) of the 3\(^{rd}\) independent variable).
+
+1.6, 1.8, 2.0, 2.2, 2.4. (the table values associated with each value of the 1\(^{st}\) independent variable, the sixth value (107) of the second independent variable, and the second value (45.5) of the 3\(^{rd}\) independent variable).
+
+Note: The following fields define the tabular data as described in the previous examples. These field values depend on the number and quantity of independent variables used in the table. The tabular data can be entered in the following fields or entered using an external file. These fields are echoed to the eio file as a check when the output diganostics flag DisplayAdvancedVariables is used (ref. Output:Diagnostics, DisplayAdvancedVariables). The normalization value is not included in the echoed values.
+
+\subsubsection{Field: Field \#1 (NumberOfIndependentVariables)}\label{field-field-1-numberofindependentvariables}
+
+The number of independent variables used in the lookup table. This number (n) can range from 1 to 5. The number entered here will define the following n fields as the number of values for these n independent variables. This is the first number in the external file as shown in the previous examples.
+
+\subsubsection{Field: Field \#2 (NumberOfValuesForIndependentVariable1)}\label{field-field-2-numberofvaluesforindependentvariable1}
+
+The number of values for the first independent variable. This is the second number in the tabular data and resides on the same line as Field \#1.
+
+\subsubsection{Field: Field \#3 (DeterminedByPreviousFields)}\label{field-field-3-determinedbypreviousfields}
+
+The value specified in this field is dependent on the number entered in Field \#1. If a 1 is entered in Field \#1, this field represents the first value of the single independent variable. The number of values entered in Field \#3-\#n will be equal to the number entered in Field \#2. Values entered in fields \#3-\#n are always entered in increasing value (ascending order). If a number greater than 1 is entered in Field \#1, this field represents the number of values for the second independent variable.
+
+\subsubsection{Field: Field \#4}\label{field-field-4}
+
+The value specified in this field is dependent on the number entered in Field \#1. If a 1 is entered in Field \#1, this field represents the second value of the single independent variable. The number of values entered in Field \#3-\#n will be equal to the number entered in Field \#2. Values entered in fields \#3-\#n are always entered in increasing value (ascending order). If a 2 is entered in Field \#1, this field represents the first value of the first independent variable. If a number greater than 2 is entered in Field \#1, this field represents the number of values for the third independent variable.
+
+\textless{}reduced for brevity\textgreater{}
+
+Following is an example input for a Table:MultiVariableLookup object:
+
+\begin{lstlisting}
+
+Table:MultiVariableLookup,
+  HPACCoolCapFT,                       !- Name
+  LagrangeinterpolationLinearExtrapolation,   !- Interpolation Method
+  3,                                               !- Number of Interpolation Points
+  BiQuadratic,                           !- Interpolation Type
+  SingleLineIndependentVariableWithMatrix, !- Table Data Format
+  ,                                                 !- External File Name
+  ASCENDING,                               !- X1 Sort Order
+  ASCENDING,                               !- X2 Sort Order
+  24999.9597049817,                 !- Normalization reference
+  12.77778,                                 !- Minimum Value of X1,
+  23.88889,                                 !- Maximum Value of X1,
+  18.0,                                         !- Minimum Value of X2,
+  46.11111,                                 !- Maximum Value of X2,
+  ,                                                 !- Minimum Value of X3
+  ,                                                 !- Maximum Value of X3
+  ,                                                 !- Minimum Value of X4
+  ,                                                 !- Maximum Value of X4
+  ,                                                 !- Minimum Value of X5
+  ,                                                 !- Maximum Value of X5
+  ,                                                 !- Minimum Table Output
+  ,                                                 !- Maximum Table Output
+  Temperature,                           !- Input Unit Type for X1
+  Temperature,                           !- Input Unit Type for X2
+  ,                                                 !- Input Unit Type for X3
+  ,                                                 !- Input Unit Type for X4
+  ,                                                 !- Input Unit Type for X5
+  Dimensionless,                       !- Output Unit Type
+  2, 6, 7,
+  12.77778, 15, 18, 19.44448943, 21, 23.88889,
+  18, 24, 30, 35, 36, 41, 46.11111,
+  24421.69383, 25997.3589, 28392.31868, 29655.22876, 31094.97495, 33988.3473,
+  22779.73113, 24352.1562, 26742.74198, 28003.546, 29441.02425, 32330.1846,
+  21147.21662, 22716.4017, 25102.61348, 26361.31143, 27796.52175, 30681.4701,
+  19794.00525, 21360.49033, 23743.0571, 25000, 26433.32038, 29314.75872,
+  19524.15032, 21090.0954, 23471.93318, 24728.52506, 26161.46745, 29042.2038,
+  18178.81244, 19742.05753, 22120.2503, 23375.08713, 24806.13958, 27683.36592,
+  16810.36004, 18370.84513, 20745.3119, 21998.35468, 23427.47518, 26301.11353;
+\end{lstlisting}
+
+\subsection{Lookup Table Outputs}\label{lookup-table-outputs}
+
+\subsubsection{\texorpdfstring{Performance Curve Output Value {[]}}{Performance Curve Output Value }}\label{performance-curve-output-value-2}
+
+The current value of the lookup table. Performance curves and tables use the same output variable. This value is averaged over the time step being reported. Inactive or unused performance curves will show a value of -999 (e.g., equipment is off, a specific performance curve is not required for this aspect of the equipment model at this time step, etc.). This value means that the performance curve was not called during the simulation and, therefore, not evaluated. This inactive state value is only set at the beginning of each environment. When averaging over long periods of time, this inactive state value may skew results. In this case, use a detaled reporting frequency (ref. Output:Variable object) to view results at each HVAC time step.
+
+\subsubsection{\texorpdfstring{Performance Curve Input Variable 1(-N) Value {[]}}{Performance Curve Input Variable 1(-N) Value }}\label{performance-curve-input-variable-1-n-value-000}
+
+The current value of the nth independent variable passed to the performance curve. The order of the independent variables is in the same order as the model equation represented by this performance curve object. This value is averaged over the time step being reported.
+
+HVAC,Average,Performance Curve Output Value {[]}
+
+HVAC,Average,Performance Curve Input Variable 1 Value {[]}
+
+HVAC,Average,Performance Curve Input Variable 2 Value {[]}
+
+HVAC,Average,Performance Curve Input Variable 3 Value {[]}
+
+HVAC,Average,Performance Curve Input Variable 4 Value {[]}
+
+HVAC,Average,Performance Curve Input Variable 5 Value {[]}
diff --git a/doc/input-output-reference/src/overview/group-plant-condenser-control.tex b/doc/input-output-reference/src/overview/group-plant-condenser-control.tex
new file mode 100644
index 00000000000..24381ee8bfc
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-plant-condenser-control.tex
@@ -0,0 +1,485 @@
+\section{Group -- Plant-Condenser Control}\label{group-plant-condenser-control}
+
+\subsection{Operation Schemes (Plant and Condenser)}\label{operation-schemes-plant-and-condenser}
+
+Plants and condenser loops must have some mechanism for controlling the operation of the loop and which equipment is available under what conditions. Since there may be multiple control schemes that are assigned various priorities associated with each loop, an overall operation scheme must be defined. The overall scheme consists of the object name, an identifying name that is referenced in the main plant or condenser loop statement, and a list of operation schemes. Each operation scheme must have the type of operation scheme, its identifying name, and the schedule that defines its availability. Note that the order in which the individual operation schemes appear in this list defines its priority versus the others with the same scheduled availability. The first scheme appearing in the list is given the highest priority, the second scheme has second highest priority, etc. In other words, if according to its schedule, the first operation scheme is available, then it is used by the simulation to define how the plant or condenser loop operates. If it is not available, the second operation scheme in the list is checked to see if it is available until the highest priority scheme that is also available is found.~ To allow for simultaneous heating and cooling, there is one configuration where multiple operation schemes are available at a given timestep.~ This is allowed if a user inputs both a heating range based operation and a cooling range based operation with overlapping schedules.~ The simulation will look at the current loop demand to determine if the cooling scheme should be used or the heating scheme.~ In other cases, if two schemes overlap (are available at the same time), a fatal error will be encountered.
+
+\subsection{PlantEquipmentOperationSchemes}\label{plantequipmentoperationschemes}
+
+\subsubsection{Inputs}\label{inputs-033}
+
+\paragraph{Field: Name}\label{field-name-032}
+
+This alpha field contains the identifying name given to the Plant Operation Scheme. This name is placed in the Plant Loop object to select this scheme.
+
+\paragraph{Field Set: (Component Object Type, Name, Schedule) up to 8}\label{field-set-component-object-type-name-schedule-up-to-8}
+
+Operation schemes are listed in ``priority'' order.~ Note that each scheme must address the entire load and/or condition ranges for the simulation. The actual one selected for use will be the first that is ``Scheduled'' on.~ That is, if control scheme 1 is not ``on'' and control scheme 2 is -- then control scheme 2 is selected. Only plant equipment should be listed on a Control Scheme for this item.
+
+\paragraph{Field: Control Scheme \textless{}\#\textgreater{} Object Type}\label{field-control-scheme-object-type}
+
+This alpha field contains the keyword for the type of control scheme used. The options for plant control schemes are:
+
+\begin{itemize}
+\item
+  PlantEquipmentOperation:Uncontrolled
+\item
+  PlantEquipmentOperation:CoolingLoad
+\item
+  PlantEquipmentOperation:HeatingLoad
+\item
+  PlantEquipmentOperation:ComponentSetpoint
+\item
+  PlantEquipmentOperation:ThermalEnergyStorage
+\item
+  PlantEquipmentOperation:UserDefined
+\end{itemize}
+
+\paragraph{Field: Control Scheme \textless{}\#\textgreater{} Name}\label{field-control-scheme-name}
+
+This alpha field contains the identifying name given to the control scheme. These must be the named versions of the referenced Control Scheme (e.g.. a Uncontrolled Loop Operation with this name or a Cooling or Heating Load Range Based Operation with this name).
+
+\paragraph{Field: Control Scheme \textless{}\#\textgreater{} Schedule}\label{field-control-scheme-schedule}
+
+This alpha field contains the schedule name for the control scheme. This schedule consists of weeks and days, with the days containing ``0 or 1'' for each hour of the day. This binary schedule (0 for off, 1 for on) determines if the control scheme is operating for that hour of day or not.
+
+Examples of this statement in two different IDFs:
+
+\begin{lstlisting}
+
+PlantEquipmentOperationSchemes,
+      CW Loop Operation,       !- Name
+      PlantEquipmentOperation:CoolingLoad,  ! Control Scheme 1 Object Type
+      Peak Operation,          !- Control Scheme 1 Name
+      On Peak,                 !- Control Scheme 1 Schedule
+      PlantEquipmentOperation:CoolingLoad,  ! Control Scheme 2 Object Type
+      Off Peak Operation,      !- Control Scheme 2 Name
+      Off Peak;                !- Control Scheme 2 Schedule
+
+  PlantEquipmentOperationSchemes,
+      CW Loop Operation,       !- Name
+      PlantEquipmentOperation:CoolingLoad,  ! Control Scheme 1 Object Type
+      Central Chiller Only,    !- Control Scheme 1 Name
+      PlantOnSched;            !- Control Scheme 1 Schedule
+\end{lstlisting}
+
+In the first IDF example, ``PlantEquipmentOperation:CoolingLoad'' is the type of control scheme. ``Peak Operation'' and ``Off Peak Operation'' are the names of two different load range based controls defined separately (see below -- ). ``On Peak'' and ``Off Peak'' are schedules defined elsewhere in the input file.
+
+The load range based operation scheme has two statements associated with it: a main statement that defines the ranges that individual priority settings are valid and the lists of equipment that may be used for each range.
+
+\subsection{CondenserEquipmentOperationSchemes}\label{condenserequipmentoperationschemes}
+
+\subsubsection{Inputs}\label{inputs-1-030}
+
+\paragraph{Field: Name}\label{field-name-1-029}
+
+This alpha field contains the identifying name given to the Condenser Operation Scheme.
+
+\paragraph{Field Set: (Component Object Type, Name, Schedule) up to 8}\label{field-set-component-object-type-name-schedule-up-to-8-1}
+
+Operation schemes are listed in ``priority'' order.~ Note that each scheme must address the entire load and/or condition ranges for the simulation. The actual one selected for use will be the first that is ``Scheduled'' on.~ That is, if control scheme 1 is not ``on'' and control scheme 2 is -- then control scheme 2 is selected. Only condenser equipment should be listed on a Control Scheme for this item.
+
+\paragraph{Field: Control Scheme \textless{}\#\textgreater{} Object Type}\label{field-control-scheme-object-type-1}
+
+This alpha field contains the keyword for the type of control scheme used. The options for plant control schemes are:
+
+This alpha field contains the keyword for the type of control scheme used. Currently, the available options are:
+
+\begin{itemize}
+\item
+  PlantEquipmentOperation:Uncontrolled
+\item
+  PlantEquipmentOperation:CoolingLoad
+\item
+  PlantEquipmentOperation:HeatingLoad
+\item
+  PlantEquipmentOperation:OutdoorDryBulb
+\item
+  PlantEquipmentOperation:OutdoorWetBulb
+\item
+  PlantEquipmentOperation:OutdoorDewpoint
+\item
+  PlantEquipmentOperation:OutdoorRelativeHumidity
+\item
+  PlantEquipmentOperation:OutdoorDryBulbDifference
+\item
+  PlantEquipmentOperation:OutdoorWetBulbDifference
+\item
+  PlantEquipmentOperation:OutdoorDewpointDifference
+\item
+  PlantEquipmentOperation:UserDefined
+\end{itemize}
+
+The condenser operation schemes apply to the equipment on the `supply side' of the condenser loop---pumps, cooling towers, ground coupled heat exchangers, etc. The keywords select the algorithm that will be used to determine which equipment is available for each timestep. The Load Schemes schemes select a user specified set of equipment for each user specified range of a particular simulation variable. Load schemes compare the demand on the condenser supply side with specified load ranges and associated equipment lists. Outdoor schemes compare the current value of an environmental parameter with user specified ranges of that parameter.
+
+\paragraph{Field: Control Scheme \textless{}\#\textgreater{} Name}\label{field-control-scheme-name-1}
+
+This alpha field contains the identifying name given to the control scheme.
+
+\paragraph{Field: Control Scheme \textless{}\#\textgreater{} Schedule}\label{field-control-scheme-schedule-1}
+
+This alpha field contains the schedule name for the control scheme. This schedule consists of weeks and days, with the days containing ``0 or 1'' for each hour of the day. This binary schedule (0 for off, 1 for on) determines which control scheme is operating for a particular hour. The schedule facilitates daily or seasonal changes in control schemes to meet demand side management or energy conservation goals.
+
+Scheduling conflicts are handled by selecting the first available scheme in order of appearance in the list.
+
+Examples of this statement in two IDFs:
+
+\begin{lstlisting}
+
+CondenserEquipmentOperationSchemes,
+      Tower Loop Operation,    !- CondenserOperationSchemeName
+      PlantEquipmentOperation:CoolingLoad,  Control Scheme 1 Object Type
+      Year Round Tower Operation,  !- Control Scheme 1 Name
+      PlantOnSched;            !- Control Scheme 1 Schedule
+
+  CondenserEquipmentOperationSchemes,Tower Loop Operation,
+      PlantEquipmentOperation:CoolingLoad, Peak Load Operation, AFTERNOONSCHEDULE,
+      PlantEquipmentOperation:CoolingLoad, OffPeak Load Operation, MORNINGSCHEDULE,
+      PlantEquipmentOperation:OutdoorWetBulb, NightOperation, NIGHTSCHEDULE;
+\end{lstlisting}
+
+Each schedule (AFTERNOONSCHEDULE, MORNINGSCHEDULE, NIGHTSCHEDULE) invokes its associated operation scheme (Peak Load Operation, OffPeak Load Operation, NightOperation). The type of operation scheme and its name references the input syntax associated with the range specification and the associated equipment.
+
+\subsection{PlantEquipmentOperation:Uncontrolled}\label{plantequipmentoperationuncontrolled}
+
+Uncontrolled loop operation simply specifies a group of equipment that runs `uncontrolled'. If the loop runs, this equipment will run also, unless turned off by the loop flow resolver to maintain continuity in the fluid loop.
+
+\subsubsection{Inputs}\label{inputs-2-028}
+
+\paragraph{Field: Name}\label{field-name-2-027}
+
+This alpha field contains the identifying name for the control scheme.
+
+\paragraph{Field: Equipment List Name}\label{field-equipment-list-name}
+
+This alpha field contains the identifying name for the Equipment List. This field ties to the Load Range Equipment List input structure, which must also be defined.
+
+\paragraph{Field: Equipment List Name}\label{field-equipment-list-name-1}
+
+This alpha field contains the identifying name for the Equipment List. This field ties to the PlantEquipmentList or CondenserEquipmentList input structure, which must also be defined.
+
+\subsection{PlantEquipmentOperation:CoolingLoad}\label{plantequipmentoperationcoolingload}
+
+\subsubsection{Inputs}\label{inputs-3-025}
+
+\subsection{PlantEquipmentOperation:HeatingLoad}\label{plantequipmentoperationheatingload}
+
+The PlantEquipmentOperation:CoolingLoad ~and PlantEquipmentOperation:HeatingLoad objects define the different ranges and which equipment list is valid for each range. After the keyword and the identifying name, a series of data trios is expected. In each trio, there is a lower limit for the load range, an upper limit for the load range, and a name that links to an equipment availability list (the PlantEquipmentList or CondenserEquipmentList objects).
+
+\subsubsection{Inputs}\label{inputs-4-022}
+
+\paragraph{Field: Name}\label{field-name-3-022}
+
+This alpha field contains the identifying name for the control scheme.
+
+\paragraph{Field Set: (Lower limit, Upper Limit, Equip List name) up to 10}\label{field-set-lower-limit-upper-limit-equip-list-name-up-to-10}
+
+\paragraph{Field: Load Range \textless{}\#\textgreater{} Lower Limit}\label{field-load-range-lower-limit}
+
+This numeric field contains the lower demand range (W) for the equipment list. If demand is below this value, then this equipment list will not turn on to meet the demand.
+
+\paragraph{Field: Load Range \textless{}\#\textgreater{} Upper Limit}\label{field-load-range-upper-limit}
+
+This numeric field contains the upper demand range (W) for the equipment list. If demand is above this value, then this equipment list will not turn on to meet the demand.
+
+\paragraph{Field: Range \textless{}\#\textgreater{} Equipment List Name}\label{field-range-equipment-list-name}
+
+This alpha field contains the identifying name for the Equipment List (i.e., the name of a PlantEquipmentList or CondenserEquipmentList object).
+
+An example of these statements in an IDF is:
+
+\begin{lstlisting}
+
+PlantEquipmentOperation:CoolingLoad, Peak Operation,
+          0,7000,   Chiller Plant,
+          7000,24500,   Chiller Plant and Purchased,
+          24500,500000, Purchased Only;
+\end{lstlisting}
+
+This particular load based operation scheme (above) has three different ranges. ``Chiller Plant'', ``Chiller Plant and Purchased'', and ``Purchased Only'' are names which link to various PlantEquipmentList or CondenserEquipmentList objects as described below. Gaps may be left in the load ranges specified, but to operate equipment over the entire range the upper limit of a given range must equal the lower limit of the next range as shown in the example. If gaps are left in the load ranges specified, a warning message will be issued when the load to be met falls within a load range ``gap''. If the user wishes to leave a load range ``gap'' for a specific reason (no equipment to operate on this plant {[}or condenser{]} loop within this load range) and does not want the warning messages to be generated, then specify a lower limit, upper limit and equipment list name for the gap and do not specify any equipment in the associated equipment list, as shown below.
+
+\begin{lstlisting}
+
+PlantEquipmentOperation:CoolingLoad, Peak Operation,
+      0,7000,   Chiller Plant,
+      7000,7100, NoEquipmentOperationOnThisPlantLoop,
+      7100,24500,   Chiller Plant and Purchased,
+      24500,500000, Purchased Only;
+
+  PlantEquipmentList,
+      Chiller Plant,           !- Name
+      Chiller:Electric,        !- Equipment 1 Object Type
+      Big Chiller;             !- Equipment 1 Name
+
+  PlantEquipmentList,
+      NoEquipmentOperationOnThisPlantLoop;    !- Name
+
+  PlantEquipmentList,
+      Chiller Plant and Purchased,  !- Name
+      Chiller:Electric,        !- Equipment 1 Object Type
+      Big Chiller,             !- Equipment 1 Name
+      DistrictCooling,         !- Equipment 2 Object Type
+      Purchased Cooling;       !- Equipment 2 Name
+
+  PlantEquipmentList,
+      Purchased Only,          !- Name
+      DistrictCooling,         !- Equipment 1 Object Type
+      Purchased Cooling;       !- Equipment 1 Name
+\end{lstlisting}
+
+\subsection{PlantEquipmentOperation:OutdoorDryBulb}\label{plantequipmentoperationoutdoordrybulb}
+
+\subsubsection{Inputs}\label{inputs-5-020}
+
+\subsection{PlantEquipmentOperation:OutdoorWetBulb}\label{plantequipmentoperationoutdoorwetbulb}
+
+\subsubsection{Inputs}\label{inputs-6-017}
+
+\subsection{PlantEquipmentOperation:OutdoorRelativeHumidity}\label{plantequipmentoperationoutdoorrelativehumidity}
+
+\subsubsection{Inputs}\label{inputs-7-017}
+
+\subsection{PlantEquipmentOperation:OutdoorDewpoint}\label{plantequipmentoperationoutdoordewpoint}
+
+The outdoor operation objects define the different ranges of the various environmental parameters and which equipment list is valid for each range. After the keyword and the identifying name, a series of data trios is expected. In each trio, there is a lower limit for the load range, an upper limit for the load range, and a name that links to an equipment availability list (the CondenserEquipmentList).
+
+The fields for each of these are:
+
+\subsubsection{Inputs}\label{inputs-8-015}
+
+\paragraph{Field: Name}\label{field-name-4-019}
+
+This alpha field contains the identifying name for the control scheme.
+
+\paragraph{Field Set: (Lower limit, Upper Limit, Equip List name) up to 10}\label{field-set-lower-limit-upper-limit-equip-list-name-up-to-10-1}
+
+\paragraph{Field: \textless{}specfic type\textgreater{} Range \textless{}\#\textgreater{} Lower Limit}\label{field-specfic-type-range-lower-limit}
+
+This numeric field contains the lower limit (C for temperature operations, Percent for relative humidity operations) for the equipment list. If specific value is below this value, then this equipment list will not turn on to meet the demand.
+
+\paragraph{Field: \textless{}specific type\textgreater{} Range \textless{}\#\textgreater{} Upper Limit}\label{field-specific-type-range-upper-limit}
+
+This numeric field contains the lower limit (C for temperature operations, Percent for relative humidity operations) for the equipment list. If specific value is above this value, then this equipment list will not turn on to meet the demand.
+
+\paragraph{Field: Range \textless{}\#\textgreater{} Equipment List Name}\label{field-range-equipment-list-name-1}
+
+This alpha field contains the identifying name for the Equipment List (i.e., the name of a CondenserEquipmentList object).
+
+\subsection{PlantEquipmentOperation:OutdoorDryBulbDifference}\label{plantequipmentoperationoutdoordrybulbdifference}
+
+\subsubsection{Inputs}\label{inputs-9-013}
+
+\subsection{PlantEquipmentOperation:OutdoorWetBulbDifference}\label{plantequipmentoperationoutdoorwetbulbdifference}
+
+\subsubsection{Inputs}\label{inputs-10-012}
+
+\subsection{PlantEquipmentOperation:OutdoorDewpointDifference}\label{plantequipmentoperationoutdoordewpointdifference}
+
+The Delta Temperature based control strategies help to control any condenser equipment based on the difference between a reference node temperature and any environmental temperature. For example a cooling tower can be controlled by a strategy, which looks at the difference between the tower inlet temperature and wet-bulb temperature. A difference range is specified for each equipment list. IDD excerpts are shown below:
+
+\subsubsection{Inputs}\label{inputs-11-011}
+
+\paragraph{Field: Name}\label{field-name-5-016}
+
+This alpha value contains the identifying name of the control strategy. This name appears as `control scheme name' in Condenser Operation Scheme object.
+
+\paragraph{Field: Reference Temperature Node Name}\label{field-reference-temperature-node-name}
+
+This alpha value specifies the reference node for the operation scheme identified in the first field.
+
+\paragraph{Field Set: (Lower limit, Upper limit, Equipment List)}\label{field-set-lower-limit-upper-limit-equipment-list}
+
+\paragraph{Field: \textless{}specfic type\textgreater{} Range \textless{}\#\textgreater{} Lower Limit}\label{field-specfic-type-range-lower-limit-1}
+
+This numeric field specifies the minimum temperature difference required for the equipment specified in the equipment list to operate.
+
+\paragraph{Field: \textless{}specfic type\textgreater{} Range \textless{}\#\textgreater{} Upper Limit}\label{field-specfic-type-range-upper-limit}
+
+This numeric field specifies the maximum temperature difference below which the equipment specified in the equipment list is available.
+
+\paragraph{Field: Range \textless{}\#\textgreater{} Equipment List Name}\label{field-range-equipment-list-name-2}
+
+This alpha field contains the identifying name for the Equipment List (i.e., the name of a CondenserEquipmentList object).
+
+\subsection{PlantEquipmentOperation:ComponentSetpoint}\label{plantequipmentoperationcomponentsetpoint}
+
+In addition to load range based control on the plant loop, sequencing the plant components based on the outlet temperature of individual equipment is allowed. This scheme is common to many present-day Energy Management Systems sequencing. In this scheme, the sequencing is done based on the order specified in the control object described below.
+
+\subsubsection{Inputs}\label{inputs-12-011}
+
+\paragraph{Field: Name}\label{field-name-6-014}
+
+This field specifies the name of the operation scheme.
+
+\paragraph{Field Set: Equipment Object Type, Name, Demand Calculation Node, Setpoint Node, Flow Rate, Operation Type)}\label{field-set-equipment-object-type-name-demand-calculation-node-setpoint-node-flow-rate-operation-type}
+
+\paragraph{Field: Equipment \textless{}\#\textgreater{} Object Type}\label{field-equipment-object-type}
+
+This field specifies the type of equipment controlled by scheme.
+
+\paragraph{Field: Equipment \textless{}\#\textgreater{} Name}\label{field-equipment-name}
+
+This field specifies the name of the controlled equipment.
+
+\paragraph{Field: Demand Calculation \textless{}\#\textgreater{} Node Name}\label{field-demand-calculation-node-name}
+
+The component demand will be calculated using the difference between the temperature at the demand node and the component set point temperature.
+
+\paragraph{Field: Setpoint \textless{}\#\textgreater{} Node Name}\label{field-setpoint-node-name}
+
+Each component controlled under temperature based control will have its own set point different from the loop set point. This field specifies component set point node (Generally its outlet temperatures). This node is acted upon by a SetpointManager in order to obtain the setpoint at any simulation timestep.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Flow Rate}\label{field-component-flow-rate}
+
+This numeric field specifies the design flow rate for the component specified in earlier fields. This flow rate is used to calculate the component demand. The field can be set to autosize, if the user wants the program to calculate the design flow. This would generally be set to autosize when the user does not know the component flow rate and does a sizing calculation for the corresponding component.
+
+\paragraph{Field: Operation\textless{}\#\textgreater{} Type}\label{field-operation-type}
+
+This alpha field specifies the operation mode for the equipment. The equipment can be in any of the three modes viz. Cooling, Heating and Dual. Dual is used when the components both as heating and cooling equipment (for example heat pumps).
+
+And, as an example in an IDF:
+
+\begin{lstlisting}
+
+PlantEquipmentOperationSchemes,
+      CW Loop Operation,       !- PlantOperationSchemeName
+      PlantEquipmentOperation:ComponentSetpoint, ! Control Scheme 1 Object Type
+      Test Scheme,                         !- Control Scheme 1 Name
+      On;                                  !- Control Scheme 1 Schedule
+
+  PlantEquipmentOperation:ComponentSetpoint,
+      Test Scheme,
+      CHILLER:ELECTRIC,        !- Equipment 1 Object Type
+      Little Chiller,          !- Equipment 1 Name
+      Little Chiller Inlet Node, !- Demand Calculation 1 Node Name
+      Little Chiller Outlet Node, !- Setpoint 1 Node Name
+      0.0011,                     !- Component 1 Flow Rate
+      COOLING,                    !- Operation 1 Type
+      CHILLER:ELECTRIC,        !- Equipment 2 Object Type
+      Big Chiller,             !- Equipment 2 Name
+      Big Chiller Inlet Node,  !- Demand Calculation 2 Node Name
+      Big Chiller Outlet Node, !- Setpoint 2 Node Name
+      0.0011,                  !- Component 2 Flow Rate
+      COOLING;                 !- Operation 2 Type
+\end{lstlisting}
+
+\subsection{PlantEquipmentOperation:ThermalEnergyStorage}\label{plantequipmentoperationthermalenergystorage}
+
+Users of thermal energy storage, particularly ice storage systems, are often faced with a challenge of specifying input for these systems. Essentially, they have to define various setpoint managers, temperature schedules, etc. in order to make the system functional. This plant/condenser control type simplifies the input somewhat by eliminating both a setpoint manager and a schedule for each piece of equipment that makes up the ice storage system. In fact, this operation scheme internally creates the setpoint managers required by the equipment listed as operated by the scheme defined by this syntax. While the more complex definition is possible and provides more flexibility like hourly variation of setpoint temperatures at the outlet of each piece of equipment, this input provides the most convenient method for making the system to work and assumes a single charging setpoint temperature and a single discharging setpoint temperature. For most systems, this is all that is needed.
+
+\subsubsection{Inputs}\label{inputs-13-009}
+
+\paragraph{Field: Name}\label{field-name-7-013}
+
+This field defines the name of the thermal energy (ice) storage plant equipment operation scheme that will be referenced by the PlantEquipmentOperationSchemes list in the plant input.
+
+\paragraph{Field: On-Peak Schedule}\label{field-on-peak-schedule}
+
+This field defines the name of an integer schedule that determines when on-peak electric pricing is in effect. This value is used to determine whether or not the ice storage system should be charging the ice storage unit. In the schedule, a value of 1 (or greater) corresponds to being in the on-peak period while any value of 0 or less corresponds to being in the off-peak period.
+
+\paragraph{Field: Charging Availability Schedule}\label{field-charging-availability-schedule}
+
+This field defines the name of an integer schedule that determines whether or not the system may enter charging mode off-peak. If the current value of the on-peak schedule is ``off'', then charging can take place if the charging availability schedule is ``on''. If the on-peak schedule is ``off'' and charging availability is ``off'', then charging is not allowed and the chiller and ice storage units controlled by this statement are operating to meet the non-charging chilled water temperature defined by the next input parameter. In this schedule, a value of 1 (or greater) corresponds to ``on'' when charging is available during an off-peak period while any value of 0 or less corresponds to chillers not being allowed to charge even during off-peak.
+
+\paragraph{Field: Non-Charging Chilled Water Temperature}\label{field-non-charging-chilled-water-temperature}
+
+This field defines the chilled water temperature when the ice storage system is NOT in charging mode. During these times, the storage system could be discharging or dormant depending on HVAC load conditions and ice storage controls. This value is used as the setpoint temperature for chillers associated with this plant equipment operation scheme during non-cooling season and during cooling season during the on-peak period. The cooling season and on-peak periods are defined by schedules reference to input above.
+
+\paragraph{Field: Charging Chilled Water Temperature}\label{field-charging-chilled-water-temperature}
+
+This field defines the chilled water temperature when the ice storage system is in charging mode. During these times, the chiller is producing a temperature low enough to generate ice in the ice storage unit. This value is used as the setpoint temperature for chillers associated with this plant equipment operation scheme during the cooling season during the off-peak period. The cooling season and on-peak periods are defined by schedules reference to input above.
+
+\paragraph{Field Set: (Component Object Type, Name, Demand Calculation Node, Setpoint Node, Flow Rate, Operation Type)}\label{field-set-component-object-type-name-demand-calculation-node-setpoint-node-flow-rate-operation-type}
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Object Type}\label{field-component-object-type-001}
+
+This field specifies the type of equipment controlled by scheme. This must be a thermal energy storage device (simple or detailed ice storage) or a chiller.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Name}\label{field-component-name-002}
+
+This field specifies the name of the controlled equipment. This name must be defined in the input as a valid ice storage device or chiller.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Demand Calculation Node Name}\label{field-component-demand-calculation-node-name}
+
+The component demand will be calculated using the difference between the temperature at the demand node and the component set point temperature.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Setpoint Node Name}\label{field-component-setpoint-node-name}
+
+Each component controlled under temperature based control will have its own set point different from the loop set point. This field specifies component set point node (Generally its outlet temperatures). This node is acted upon by a SetpointManager in order to obtain the setpoint at any simulation timestep.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Flow Rate}\label{field-component-flow-rate-1}
+
+This numeric field specifies the design flow rate for the component specified in earlier fields. This flow rate is used to calculate the component demand. The field can be set to autosize, if the user wants the program to calculate the design flow. This would generally be set to autosize when the user does not know the component flow rate and does a sizing calculation for the corresponding component.
+
+\paragraph{Field: Component \textless{}\#\textgreater{} Operation Type}\label{field-component-operation-type}
+
+This alpha field specifies the operation mode for the equipment. The equipment can be in any of the three modes viz. Cooling, Heating and Dual. Dual is used when the components both as heating and cooling equipment (for example heat pumps). Ice storage units can potentially either heat or cool the circulating fluid and thus should be defined as Dual mode.
+
+An example IDF is shown below:
+
+\begin{lstlisting}
+
+PlantEquipmentOperationSchemes,
+  CW Loop Operation,       !- Name
+  PlantEquipmentOperation:ThermalEnergyStorage,  !- Control Scheme 1 Object Type
+  Chiller and Partial Ice Storage,  !- Control Scheme 1 Name
+  PlantOnSched;            !- Control Scheme 1 Schedule Name
+
+  PlantEquipmentOperation:ThermalEnergyStorage,
+  Chiller and Partial Ice Storage,  !- Name
+  OnPeakEnergy,            !- On-Peak Schedule Name
+  ChargingAvail,           !- Charging Availability Schedule Name
+  7.22,                    !- Non-charging Chilled Water Temperature
+  -5.0,                    !- Charging Chilled Water Temperature
+  Chiller:Electric,        !- Component 1 Object Type
+  Central Chiller,         !- Component 1 Name
+  Central Chiller Inlet Node,  !- Component 1 Demand Calculation Node Name
+  Central Chiller Outlet Node,  !- Component 1 Setpoint Node Name
+  autosize,                !- Component 1 Flow Rate {m3/s}
+  COOLING,                 !- Component 1 Operation Type
+  ThermalStorage:Ice:Detailed,  !- Component 2 Object Type
+  Ice Tank,                !- Component 2 Name
+  Ice Tank Inlet Node,     !- Component 2 Demand Calculation Node Name
+  Ice Tank Outlet Node,    !- Component 2 Setpoint Node Name
+  0.13506E-02,             !- Component 2 Flow Rate {m3/s}
+  DUAL;                    !- Component 2 Operation Type
+\end{lstlisting}
+
+\subsection{PlantEquipmentList}\label{plantequipmentlist}
+
+\subsubsection{Inputs}\label{inputs-14-009}
+
+\subsection{CondenserEquipmentList}\label{condenserequipmentlist}
+
+The PlantEquipmentList ~and CondenserEquipmentList ~specify available plant and condenser loop equipment respectively for any loop operation scheme. Each statement contains the object name, an identifying name (which links the definition back to one of the operation scheme statements) and a variable length of data pairs. These pairs refer to a plant equipment type and an identifying name. The type in this list of pairs must correspond to a valid plant object as described in the next subsection.
+
+Note: If a PlantEquipmentList or CondenserEquipmentList object is specified with no equipment object types or equipment names, then the corresponding PlantEquipmentOperation:* object will assume all available equipment on this plant (or condenser) loop should be OFF (not operate) within the specified lower/upper limit.
+
+\subsubsection{Inputs}\label{inputs-15-009}
+
+\paragraph{Field: Name}\label{field-name-8-013}
+
+This alpha field contains the identifying name for the Equipment List.
+
+\paragraph{Field Set: (Object Type, Name) up to 10}\label{field-set-object-type-name-up-to-10}
+
+Remember the order of equipment on this list determines operation priority. Equipment on the list first will try to meet demand first. These fields tie to the Equipment Definition input structure, which must also be defined.
+
+\paragraph{Field: Equipment \textless{}\#\textgreater{} Object Type}\label{field-equipment-object-type-1}
+
+This alpha field contains the keyword for the type of equipment in operation. Example: (Chiller:Electric, DistrictCooling). The full list of allowable plant equipment is valid plant objects as described in the next subsection.
+
+\paragraph{Field: Equipment \textless{}\#\textgreater{} Name}\label{field-equipment-name-1}
+
+This alpha field contains the identifying name for the equipment in operation. This distinguishes between two different pieces of equipment of the same type.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+PlantEquipmentList, Chiller Plant and Purchased,
+          Chiller:Electric, Big Chiller,
+          DistrictCooling, Purchased Cooling;
+\end{lstlisting}
+
+Note that this list is the middle range defined in the PlantEquipmentOperation:CoolingLoad statement named ``Peak Operation'' above. This defines the equipment available when the load encountered by the plant (chiller water demand, for example) is between 7000 W and 24500 W. EnergyPlus will run the ``Big Chiller'' first up to its capacity and then attempt to meet the remaining load (while in that range) with the next piece of equipment (in this case, ``Purchased:Cooling'') in the list.
diff --git a/doc/input-output-reference/src/overview/group-plant-condenser-flow-control.tex b/doc/input-output-reference/src/overview/group-plant-condenser-flow-control.tex
new file mode 100644
index 00000000000..917e0c3b8f1
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-plant-condenser-flow-control.tex
@@ -0,0 +1,116 @@
+\section{Group -- Plant-Condenser Flow Control}\label{group-plant-condenser-flow-control}
+
+The connector list described earlier determines how the branches of a particular loop will be hooked together. These connections can be classified either as a separation of a single stream into several outlet streams (splitter) or the merging of several streams into a single outlet stream (mixer). Due to the limitation per branch of a single splitter and a single mixer, the connector list can only have two pieces of equipment as a maximum. The names defined for either/both the splitter or/and the mixer refer then to ``component'' definitions as described below.
+
+\subsection{Connector:Splitter, Connector:Mixer}\label{connectorsplitter-connectormixer}
+
+The format of both the \textbf{Connector:Splitter} and \textbf{Connector:Mixer} statements is similar. Both begin with an identifying name followed by the branch name of the ``single side'' of the component. In the case of the splitter, this is the inlet since the inlet stream is broken into several outlet streams. In the case of the mixer, this is the outlet since several streams are mixed together to form a single outlet. The remaining list of up to 50 names is simply the branch names of the outlet legs in the case of the splitter and inlet legs in the case of the mixer. No control logic is assume in these components---a determination of how much air to split in which direction using the splitter must be defined by other components.
+
+\subsection{Connector:Splitter}\label{connectorsplitter}
+
+\subsubsection{Inputs}\label{inputs-034}
+
+\paragraph{Field: Name}\label{field-name-033}
+
+This alpha field contains the identifying name for the Splitter.
+
+\paragraph{Field: Inlet Branch Name}\label{field-inlet-branch-name}
+
+This alpha field contains the identifying name for the Splitter Inlet Branch.
+
+\paragraph{Field: Outlet Branch \textless{}x\textgreater{} Name}\label{field-outlet-branch-x-name}
+
+This alpha field contains the identifying names for the Splitter Outlet Branches and you enter as many outlet branches as needed.
+
+\subsection{Connector:Mixer}\label{connectormixer}
+
+\subsubsection{Inputs}\label{inputs-1-031}
+
+\paragraph{Field: Name}\label{field-name-1-030}
+
+This alpha field contains the identifying name for the Mixer.
+
+\paragraph{Field: Outlet Branch Name}\label{field-outlet-branch-name}
+
+This alpha field contains the identifying name for the Mixer Outlet Branch.
+
+\paragraph{Field: Inlet Branch \textless{}x\textgreater{} Name}\label{field-inlet-branch-x-name}
+
+This alpha field contains the identifying names for the Mixer Inlet Branches and you enter as many inlet branch names as needed..
+
+An example of these statements in an IDF is:
+
+\begin{lstlisting}
+
+Connector:Splitter,
+               CW Loop Splitter,
+               CW Pump Branch,
+               Little Chiller Branch,
+               Big Chiller Branch,
+               Purchased Cooling Branch,
+               Supply Bypass Branch;
+  Connector:Mixer,
+               CW Loop Mixer,
+               Cooling Supply Outlet,
+               Little Chiller Branch,
+               Big Chiller Branch,
+               Purchased Cooling Branch,
+               Supply Bypass Branch;
+\end{lstlisting}
+
+\subsection{TemperingValve}\label{temperingvalve}
+
+This object is used for special cases where plant flow control is needed to make efficient use of thermal storage. In certain solar hot water and heat recovery situations, a thermal storage tank may become warmer than is necessary or allowable for safe use of the hot water. Although real installations of a tempering, or anti-scald valve, would more commonly mix a new stream of mains water with the hot water to achieve a desired outlet temperature, this is difficult to model directly within EnergyPlus because plant loops need to be closed circuits. For many installations where the water entering the splitter is directly from the mains, such as make up water entering a water heater tank, the modeling provided with this object should be thermodynamically equivalent.
+
+The TemperingValve object models a temperature-controlled diversion valve. It models a valve on a bypass pipe that can open to divert flow around one or more plant components. It can only be used on one of two branches between a Splitter and a Mixer. The figure below shows the use of the tempering valve with a Water Heater:Mixed component on ``Stream 2.''~ The tempering valve acts to divert flow through the branch it is on in order to adjust the temperature at the outlet of the mixer. If the temperature at Stream 2 Source Node is warmer than the setpoint and the inlet flow is cooler than the setpoint, then a controller determines how much flow should bypass the storagew tank to achieve the desired setpoint.
+
+\begin{figure}[hbtp] % fig 89
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image208.png}
+\caption{Tempering Valve Schematic \protect \label{fig:tempering-valve-schematic}}
+\end{figure}
+
+The TemperingValve is an \textbf{Active} component and the other path should have only \textbf{Passive} components. Only two paths in the splitter/mixer can be used; bypasses are not allowed. No other Connector:Splitter and Connector:Mixer pair can be used on the supply side of the plant loop.
+
+\subsubsection{Inputs}\label{inputs-2-029}
+
+\paragraph{Field: Name}\label{field-name-2-028}
+
+This field should contain an unique name for each TemperingValve object
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-003}
+
+This field should contain the name of node which is the inlet for the valve.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-004}
+
+This field should contain the name of node which is the outlet for the valve
+
+\paragraph{Field: Stream 2 Source Node Name}\label{field-stream-2-source-node-name}
+
+This field should contain the name of node that is the inlet to the Mixer object for the second stream containing the component whose flow is being diverted.
+
+\paragraph{Field: Temperature Setpoint Node Name}\label{field-temperature-setpoint-node-name-000}
+
+This field should contain the name of a node that has a temperature setpoint assigned to it. A separate set point manager object is needed to provide a set point on the node listed here.
+
+\paragraph{Field: Pump Outlet Node Name}\label{field-pump-outlet-node-name}
+
+This field should contain the name of the node that is the outlet for the pump that is one the same plant loop. This is node is used to sense the total flow rate.
+
+This object is demonstrated in the example file called SolarCollectorFlatPlateWater.idf. An example of this object is:
+
+\begin{lstlisting}
+
+TemperingValve,
+          DHW Anti-Scald Diverter,
+          DHW Anti-Scald Inlet Node, ! Inlet Node Name
+          DHW Anti-Scald Outlet Node, ! Outlet Node Name
+          SHW Storage Tank Use Outlet Node, ! Stream 2 Source Node Name
+          DHW Instantaneous Boost Outlet Node, ! Temperature Setpoint Node Name
+          DHW Use Side Pump Outlet;  ! pump outlet node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-023}
+
+Use output variables for System Nodes for flow and temperature results.
diff --git a/doc/input-output-reference/src/overview/group-plant-condenser-loops.tex b/doc/input-output-reference/src/overview/group-plant-condenser-loops.tex
new file mode 100644
index 00000000000..533e9c59be9
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-plant-condenser-loops.tex
@@ -0,0 +1,520 @@
+\section{Group -- Plant-Condenser Loops}\label{group-plant-condenser-loops}
+
+\subsection{PlantLoop}\label{plantloop}
+
+The main elements of the PlantLoop syntax are described in further detail below. A map of how the input for this portion of the HVAC input fits together is provided in the following diagram.
+
+!{[}PlantLoopSyntax (media/image135.png)
+
+Figure 73. Plant Loop Input Syntax Map
+
+\subsubsection{Inputs}\label{inputs-035}
+
+\paragraph{Field: Name}\label{field-name-034}
+
+This alpha field is used as an identifying field for the plant loop.
+
+\paragraph{Field: Fluid Type}\label{field-fluid-type-001}
+
+This alpha field must be a keyword selected from the list of available fluids for an EnergyPlus plant loop. Either \textbf{Water}, \textbf{Steam} or \textbf{UserDefinedFluidType} may be used. If the UserDefinedFluidType keyword is used, the following input field i.e.~User Defined Fluid Type must have a value (namely the name of a FluidProperties:GlycolConcentration object).
+
+\paragraph{Field: User Defined Fluid Type}\label{field-user-defined-fluid-type-000}
+
+This alpha field must be specified when the previous field is set to \textbf{UserDefinedFluidType} otherwise it could be left blank. \textbf{Water}, \textbf{EthyleneGlycol}, \textbf{PropoleneGlycol} and \textbf{Steam} are all ``built-in'' fluids for EnergyPlus (that is, all of the appropriate properties are contained within the program). If the fluid specified here is a mixture of water and ethylene or propylene glycol, then only FluidProperties:GlycolConcentration objects need to be specified and the name of the appropriate one is used here. For another water/glycol mixture, a complete set of fluid property data (FluidProperties:Name and FluidProperties:Temperature objects plus multiple FluidProperties:Concentration objects for specific heat, density, etc.) must be specified (Ref dataset: GlycolPropertiesRefData.idf).
+
+\paragraph{Field: Plant Equipment Operation Scheme Name}\label{field-plant-equipment-operation-scheme-name}
+
+This alpha field is used as an identifying field for the plant operation scheme. This field ties to the PlantEquipmentOperationSchemes input structure, which must also be defined.
+
+\paragraph{Field: Loop Temperature Setpoint Node Name}\label{field-loop-temperature-setpoint-node-name}
+
+This alpha field is used to identify the node which the Loop Manager will access the temperature setpoint that it will try to maintain. This is typically the Plant Loop Supply Side Outlet Node so that it will not interfere with component temperature setpoints. An associated temperature setpoint manager will need to be defined.
+
+\paragraph{Field: Maximum Loop Temperature}\label{field-maximum-loop-temperature}
+
+This numeric field contains the maximum allowable temperature in Celsius for this loop.
+
+\paragraph{Field: Minimum Loop Temperature}\label{field-minimum-loop-temperature}
+
+This numeric field contains the minimum allowable temperature in Celsius for this loop.
+
+\paragraph{Field: Maximum Loop Flow Rate}\label{field-maximum-loop-flow-rate}
+
+This numeric field contains the maximum loop flow rate in cubic meters per second. This parameter is also used when the user chooses to autocalculate the loop volume. See Volume of the Plant Loop below and the Engineering Manual for more details. This field is autosizable.
+
+\paragraph{Field: Minimum Loop Flow Rate}\label{field-minimum-loop-flow-rate}
+
+This numeric field contains the minimum loop flow rate in cubic meters per second.
+
+\paragraph{Field: Plant Loop Volume}\label{field-plant-loop-volume}
+
+Volume of the plant loop in m\(^{3}\). This numeric field contains the loop volume for the entire loop, i.e.~both the demand side and the supply side. This is used for the loop capacitance calculation.. Loop volume (m\(^{3}\)) could be calculated from pipe size data but this is not usually known. If zero volume is specified the loop has no fluid heat capacity. If a very large capacitance is specified unrealistic time delay may result and there may be poor response to changes in loop setpoint temperature. The loop capacitance \textbf{autocalculate} option gives reasonable values for most system sizes. This calculation is described in the Engineering Reference manual.
+
+\paragraph{Field: Plant Side Inlet Node Name}\label{field-plant-side-inlet-node-name}
+
+This required alpha field contains the identifying name given to the Plant Side Inlet Node.~ This node is the inlet to the supply side of the loop.
+
+\paragraph{Field: Plant Side Outlet Node Name}\label{field-plant-side-outlet-node-name}
+
+This required alpha field contains the identifying name given to the Plant Side Outlet Node. This node is the outlet of the supply side of the loop.
+
+\paragraph{Field: Plant Side Branch List Name}\label{field-plant-side-branch-list-name}
+
+This required alpha field contains the identifying name given to the Plant Side Branch List. The list referenced here should list all the branches on the supply side of the loop.
+
+\paragraph{Field: Plant Side Connector List Name}\label{field-plant-side-connector-list-name}
+
+This alpha field contains the identifying name given to the Plant Side Connector List. The list referenced here should list the splitter and mixer on the supply side of the loop.
+
+\paragraph{Field: Demand Side Inlet Node Name}\label{field-demand-side-inlet-node-name}
+
+This required alpha field contains the identifying name given to the Demand Side Inlet Node. This node is the inlet to the demand side of the loop.
+
+\paragraph{Field: Demand Side Outlet Node Name}\label{field-demand-side-outlet-node-name-000}
+
+This required alpha field contains the identifying name given to the Demand Side Outlet Node. This node is the outlet of the demand side of the loop.
+
+\paragraph{Field: Demand Side Branch List Name}\label{field-demand-side-branch-list-name}
+
+This required alpha field contains the identifying name given to the Demand Side Branch List. The list referenced here should list all the branches on the demand side of the loop.
+
+\paragraph{Field: Demand Side Connector List Name}\label{field-demand-side-connector-list-name}
+
+This alpha field contains the identifying name given to the Demand Side Connector List. The list referenced here should list the splitter and mixer on the demand side of the loop.
+
+\paragraph{Field: Load Distribution Scheme}\label{field-load-distribution-scheme-000}
+
+This alpha field contains the Load Distribution Scheme Keyword. The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. \textbf{Optimal} operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{SequentialLoad} loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{UniformLoad} evenly distributes the loop demand among all available components on the equipment list for a given load range. \textbf{SequentialUniformPLR} loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. \textbf{UniformPLR} will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
+
+Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-000}
+
+This alpha field contains the identifying name given to the System Availability Manager List.
+
+\paragraph{Field: Plant Loop Demand Calculation Scheme}\label{field-plant-loop-demand-calculation-scheme}
+
+There are two plant loop demand calculations schemes in EnergyPlus. There is a SingleSetpoint and a DualSetpointDeadband; the SingleSetpoint is the default if this field is left blank. In the SingleSetpoint scheme the Plant Loop requires that a Setpoint Manager set a single setpoint value (on Node\%TempSetpoint). Examples of this setpoint manager would be: SetpointManager:Scheduled, SetpointManager:OutsideAir, etc. For the DualSetPointDeadband scheme the Plant Loop requires that a Setpoint Manager set the high and low setpoint values (for Node\%TempSetPointHi and Node\%TempSetPointLo). Examples of this Setpoint manager would be: SetpointManager:Scheduled:DualSetpoint.
+
+The plant loop demand calculation scheme determines the amount of heating or cooling necessary to bring the temperature of the Plant Loop to its setpoint(s). When this value is determined then the load distribution scheme explained in the previous section takes this value and distributes the load to the appropriate equipment. The demand calculation scheme determines how the load is calculated. See more information in the Engineering Document.
+
+\paragraph{Field: Common Pipe Simulation}\label{field-common-pipe-simulation}
+
+This field specifies a primary-secondary plant loop simulation. When a common pipe option is specified, the plant side of the loop is the primary loop and the demand side of the loop is the secondary loop, and a pump object must be placed on the demand side inlet branch. The three options are ``\textbf{None}'', ``\textbf{CommonPipe}'' and ``\textbf{TwoWayCommonPipe}''. ``\textbf{None}'' means that there is no secondary loop and the plant loop is modeled as a single primary loop. ``\textbf{CommonPipe}'' means that the common pipe interface does not attempt any temperature control, it only satisfies secondary (demand side) flow requests. ``\textbf{TwoWayCommonPipe}'' allows control of the secondary (demand side) inlet temperature or the primary (plant side) inlet temperature by placing a setpoint on the corresponding node. If this field is left blank, it will default to ''None''. If the field is set to ``None'' and the program finds a pump on the demand side it will result in a fatal error.~ If the field is set to ``CommonPipe'' or ``TwoWayCommonPipe'' and the program does not find a pump on the demand side it will result in a fatal error. The common pipe simulation is currently limited to simulating loop pumps, i.e.~each pump should be placed on the inlet branch of the plant side or demand side of the loop.
+
+\paragraph{Field: Pressure Simulation Type}\label{field-pressure-simulation-type}
+
+This field lets user to choose if this plant loop will be involved in a pressure drop calculation.~ This requires that at least one branch on the loop have pressure drop data.~ If not, an error will be thrown due to the input mismatch.~ Currently there are two pressure drop simulation types: ``PumpPowerCorrection'' and ``LoopFlowCorrection''.~ In both of these methods, branch pressure drop data is used to calculate a dynamic loop pressure drop and is used to update pumping power accordingly.~ The flow correction method allows the user to enter information regarding the pressure curve of a constant speed pump so that the simulation can dynamically resolve the pressure vs.~flow relationship in the plant loop.~ This is limited to constant speed pumps, as the variable speed pumps are expected to resolve as if it were controlled by a variable drive, so that they can inherently meet any pressure and flow demand required by the loop.~ This is also limited to ``loop pumps'', where there is a single pump on the plant loop. Common pipe simulations and ``branch pump'' simulations are not compatible with this level of pressure simulation.~ See the documentation for the Pump:ConstantSpeed in order to determine required inputs for this pressure simulation method to be performed.~ In the pressure drop system, parallel flow rates are not resolved (to match the pressure drop for the parallel system).~ Enhancements to this calculation are planned which will allow parallel branch flow resolution.~ See the Engineering Reference document for more information on how this works.
+
+An example of this statement used in an IDF is:
+
+\begin{lstlisting}
+
+  PlantLoop,
+      Hot Water Loop,         !- Plant Loop Name
+      Water,                  !- Fluid Type
+      ,                       !- User Defined Fluid Type
+      Hot Loop Operation,     !- Plant Operation Scheme List Name
+      HW Loop Outlet Node,    !- Loop Temperature Setpoint Schedule Name
+      100,                    !- Maximum Loop Temperature {C}
+      10,                     !- Minimum Loop Temperature {C}
+      autosize,               !- Maximum Loop Volumetric Flow Rate {m3/s}
+      0.0,                    !- Minimum Loop Volumetric Flow Rate {m3/s}
+      autosize,               !- volume of the plant loop {m3}
+      HW Supply Inlet Node,   !- Plant Side Inlet Node Name
+      HW Supply Outlet Node,  !- Plant Side Outlet Node Name
+      Heating Supply Side Branches,    !- Plant Side Branch List Name
+      Heating Supply Side Connectors,  !- Plant Side Connector List Name
+      HW Demand Inlet Node,   !- Demand Side Inlet Node Name
+      HW Demand Outlet Node,  !- Demand Side Outlet Nodes Name
+      Heating Demand Side Branches,    !- Demand Side Branch List Name
+      Heating Demand Side Connectors,  !- Demand Side Connector List Name
+      Optimal;                !- Load Distribution Scheme
+\end{lstlisting}
+
+In the above example input there is no system availability manager specified and the Demand Calculation Scheme will default to SingleSetpoint using a single setpoint manager. Common pipe simulation field in the above example will default to ``NONE'' since it is not specified.
+
+\subsubsection{Outputs}\label{outputs-024}
+
+In the following output variables, ``Debug'' denotes variables that are used primarily by the developers and whose names and application may be cryptic to users. .
+
+\begin{itemize}
+\item
+  HVAC,Average,Plant Supply Side Cooling Demand Rate {[}W{]}
+\item
+  HVAC,Average,Plant Supply Side Heating Demand Rate {[}W{]}
+\item
+  HVAC,Average,Plant Supply Side Inlet Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Plant Supply Side Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Plant Supply Side Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Plant Supply Side Not Distributed Demand Rate {[}W{]}
+\item
+  HVAC,Average,Plant Supply Side Unmet Demand Rate {[}W{]}
+\item
+  HVAC,Sum,Plant Solver Sub Iteration Count {[]}
+\item
+  HVAC,Sum,Plant Solver Half Loop Calls Count {[]}
+\item
+  HVAC,Average,Debug Plant Loop Bypass Fraction
+\item
+  HVAC,Average,Debug Plant Last Simulated Loop Side {[}-{]}
+\item
+  HVAC,Average,Plant Common Pipe Mass Flow Rate {[}Kg/s{]}
+\item
+  HVAC,Average,Plant Common Pipe Temperature {[}C{]}
+\item
+  HVAC,Average,Plant Common Pipe Flow Direction Status {[]}
+\item
+  HVAC,Average,Plant Common Pipe Primary Mass Flow Rate {[}Kg/s{]}
+\item
+  HVAC,Average,Plant Common Pipe Secondary Mass Flow Rate {[}Kg/s{]}
+\item
+  HVAC,Average,Primary Side Common Pipe Flow Direction {[]}
+\item
+  HVAC,Average,Secondary Side Common Pipe Flow Direction {[]}
+\item
+  HVAC,Average,Plant Common Pipe Primary to Secondary Mass Flow Rate {[}Kg/s{]}
+\item
+  HVAC,Average,Plant Common Pipe Secondary to Primary Mass Flow Rate {[}Kg/s{]}
+\item
+  HVAC,Average,Plant System Cycle On Off Status {[]}
+\item
+  HVAC,Average,Plant Demand Side Loop Pressure Difference {[}Pa{]}
+\item
+  HVAC,Average,Plant Supply Side Loop Pressure Difference {[}Pa{]}
+\item
+  HVAC,Average,Plant Loop Pressure Difference {[}Pa{]}
+\end{itemize}
+
+\paragraph{Plant Supply Side Cooling Demand Rate {[}W{]}}\label{plant-supply-side-cooling-demand-rate-w}
+
+This is the value of the net demand required to meet the cooling setpoint of the loop.~ If the loop setpoint is met for the current HVAC timestep, Plant Supply Side Cooling Demand Rate will equal sum of the total cooling demand from the demand side coils on the loop.~ It will also equal the cooling output of all chillers (or other cooling equipment) on the loop less any pump heat added to the fluid.~ For example, for a chilled water loop with one chiller and one pump serving one chilled water coil:~ Plant Supply Side Cooling Demand Rate will equal the chiller evaporator heat transfer less the pump heat to fluid, and it will also equal the chilled water coil total cooling output.
+
+If the plant loop setpoint is not met, Plant Supply Side Cooling Demand Rate will equal the sum of the total cooling demand from the demand side coils on the loop plus the additional cooling required to bring the loop flow to setpoint.~ If the loop remains off setpoint for successive timesteps, the demand required to return to setpoint will repeat in each timestep until the loop reaches setpoint.~ For this reason, Plant Supply Side Cooling Demand Rate should not be summed over time, because it will overstate the demand whenever the loop is off setpoint.
+
+\paragraph{Plant Supply Side Heating Demand Rate {[}W{]}}\label{plant-supply-side-heating-demand-rate-w}
+
+This is the value of the net demand required to meet the heating setpoint of the loop.~ If the loop setpoint is met for the current HVAC timestep, Plant Supply Side Heating Demand Rate will equal sum of the total heating demand from the demand side coils on the loop.~ It will also equal the heating output of all boilers (or other cooling equipment) on the loop plus any pump heat added to the fluid.~ For example, for a hot water loop with one boiler and one pump serving one hot water coil: Plant Supply Side Heating Demand Rate will equal the boiler heat transfer plus the pump heat to fluid, and it will also equal the hot water coil total heating output.
+
+If the plant loop setpoint is not met, Plant Supply Side Heating Demand Rate will equal the sum of the total heating demand from the demand side coils on the loop plus the additional heating required to bring the loop flow to setpoint.~ If the loop remains off setpoint for successive timesteps, the demand required to return to setpoint will repeat in each timestep until the loop reaches setpoint.~ For this reason, Plant Supply Side Heating Demand Rate should not be summed over time, because it will overstate the demand whenever the loop is off setpoint.
+
+\paragraph{Plant Supply Side Inlet Mass Flow Rate {[}kg/s{]}}\label{plant-supply-side-inlet-mass-flow-rate-kgs}
+
+This is the value of the mass flow rate at the Inlet to Plant Loop on the supply side. There is not an associated Plant Loop outlet node flow rate since continuity must be maintained in the loop and the outlet must be the same.
+
+\paragraph{Plant Supply Side Inlet Temperature {[}C{]}}\label{plant-supply-side-inlet-temperature-c}
+
+This is the value of the temperature at the Inlet to the plant loop on the supply side.
+
+\paragraph{Plant Supply Side Outlet Temperature {[}C{]}}\label{plant-supply-side-outlet-temperature-c}
+
+This is the value of the temperature at the outlet to the plant loop on the supply side.
+
+\paragraph{Plant Supply Side Not Distributed Demand Rate {[}W{]}}\label{plant-supply-side-not-distributed-demand-rate-w}
+
+This is the value of the demand that could not be distributed to the plant equipment because of some constraint in the plant operation scheme.~ This is a record of the loop operation scheme supervisory controls after attempting to distribute the load.~ For example it would be~ non-zero in situations where the load is larger than the upper limit of capacities set for the plant equipment controls.~ This output is for \emph{before} the equipment has actually been simulated whereas the separate output Plant Supply Side Unmet Demand Rate is for \emph{after} the equipment has simulated.
+
+\paragraph{Plant Supply Side Unmet Demand Rate {[}W{]}}\label{plant-supply-side-unmet-demand-rate-w}
+
+This is the value of the demand NOT provided by the plant equipment to meet the heating or cooling setpoint of the loop. The value is positive when the plant equipment cannot meet the setpoint, and the value is negative when the plant equipment provides more than enough heating or cooling to meet the setpoint. A negative value can happen when the amount of demand is smaller than the minimum capacity of the equipment using the minimum part load ratio.
+
+\paragraph{\texorpdfstring{Plant Solver Sub Iteration Count {[]}}{Plant Solver Sub Iteration Count }}\label{plant-solver-sub-iteration-count}
+
+This is the count of iterations that the overall plant simulation used over the period of time being reported.~ This high-level output is from the plant solver used for all the plant loops and condenser loops in the model.
+
+\paragraph{Plant Solver Half Loop Calls Count}\label{plant-solver-half-loop-calls-count}
+
+This is the count of calls to model individual half-loops that occurred during the overall plant simulation over the period of time being reported.~ This includes all the half-loops for both plant loops and condenser loops.
+
+\paragraph{Plant Common Pipe Mass Flow Rate {[}Kg/s{]}}\label{plant-common-pipe-mass-flow-rate-kgs}
+
+This output gives the magnitude of the flow through common pipe. The value is averaged over the reporting interval.
+
+\paragraph{Plant Common Pipe Temperature {[}C{]}}\label{plant-common-pipe-temperature-c}
+
+This output gives the value of the temperature of the fluid flowing through common pipe. This value is averaged over the reporting interval.
+
+\paragraph{\texorpdfstring{Plant Common Pipe Flow Direction Status {[]}}{Plant Common Pipe Flow Direction Status }}\label{plant-common-pipe-flow-direction-status}
+
+This output gives the direction of flow in common pipe. The value is an integer and can be 0, 1 or 2. Since the output value is averaged over reporting interval, a non-integer value may be shown as an output when the reporting interval is not detailed. An output value of 0 means that there was no flow in common pipe. An output value of 1 means that the secondary flow is greater than primary flow, whereas a value of 2 means that primary flow is greater than secondary flow.
+
+\paragraph{Plant Common Pipe Primary Mass Flow Rate {[}Kg/s{]}}\label{plant-common-pipe-primary-mass-flow-rate-kgs}
+
+This output variable gives the mass flow in the primary side common pipe leg in a Two-Way common pipe simulation. Value is averaged over the reporting interval.
+
+\paragraph{Plant Common Pipe Secondary Mass Flow Rate {[}Kg/s{]}}\label{plant-common-pipe-secondary-mass-flow-rate-kgs}
+
+This output variable gives the mass flow in the secondary side common pipe leg in a Two-Way common pipe simulation. Value is averaged over the reporting interval.
+
+\paragraph{\texorpdfstring{Primary Side Common Pipe Flow Direction {[]}}{Primary Side Common Pipe Flow Direction }}\label{primary-side-common-pipe-flow-direction}
+
+This output variable gives the direction of flow in a primary side common pipe leg in a Two-Way Common Pipe Simulation. A value of zero means there was no flow in the pipe. A value of 1 means the flow was from top to bottom in EnergyPlus loop schematic. So for primary side, a value of 1 means the flow is from Primary side inlet to Primary side outlet and a value of 2 means flow is from Primary side outlet to Primary side inlet.
+
+\paragraph{\texorpdfstring{Secondary Side Common Pipe Flow Direction {[]}}{Secondary Side Common Pipe Flow Direction }}\label{secondary-side-common-pipe-flow-direction}
+
+This output variable gives the direction of flow in a Secondary side common pipe leg in a Two-Way Common Pipe Simulation. A value of zero means there was no flow in the pipe. A value of 1 means the flow was from top to bottom in EnergyPlus loop schematic. So for Secondary side, a value of 1 means the flow is from Secondary side outlet to Secondary side inlet and a value of 2 means flow is from Secondary side inlet to Secondary side outlet. Note that this is opposite to the primary side common pipe.
+
+\paragraph{Plant Common Pipe Primary to Secondary Mass Flow Rate {[}Kg/s{]}}\label{plant-common-pipe-primary-to-secondary-mass-flow-rate-kgs}
+
+This output variable gives the mass flow from primary to secondary side in a Two-Way common pipe simulation. Value is averaged over the reporting interval.
+
+\paragraph{Plant Common Pipe Secondary to Primary Mass Flow Rate {[}Kg/s{]}}\label{plant-common-pipe-secondary-to-primary-mass-flow-rate-kgs}
+
+This output variable gives the mass flow from secondary to primary side in a Two-Way common pipe simulation. Value is averaged over the reporting interval.
+
+\paragraph{Plant System Cycle On Off Status}\label{plant-system-cycle-on-off-status}
+
+This field is the availability status of a Plant Loop. This status flag is a result of the calculations made by the System Availability Manager(s) listed in a System Availability Manager List. When a single availability manager is used in a System Availability Manager List, this is also the availability status reported by the specific availability manager (Ref. System Availability Manager Outputs). When multiple availability managers are used in a System Availability Manager List, the loop availability status is determine by the rules associated with Plant Loops (see rules described for Group -- System Availability Managers). The control status outputs are represented using integers 0 through 2.. These integers represent \emph{NoAction} (0), \emph{ForceOff} (1), and \emph{CycleOn} (2). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\paragraph{Plant Demand Side Loop Pressure Difference {[}Pa{]}}\label{plant-demand-side-loop-pressure-difference-pa}
+
+This field allows the user to output the demand side pressure drop of a plant loop.~ This output is only recognized if a valid pressure simulation is being performed.~ To do this, the user must specify a pressure simulation type as an input in the PlantLoop object, and input at least one pressure drop curve on a branch of the plant loop.~ This particular output is only relevant if the user puts that curve on the demand side of the loop.
+
+\paragraph{Plant Supply Side Loop Pressure Difference {[}Pa{]}}\label{plant-supply-side-loop-pressure-difference-pa}
+
+This field allows the user to output the supply side pressure drop of a plant loop.~ This output is only recognized if a valid pressure simulation is being performed.~ To do this, the user must specify a pressure simulation type as an input in the PlantLoop object, and input at least one pressure drop curve on a branch of the plant loop.~ This particular output is only relevant if the user puts that curve on the supply side of the loop.
+
+\paragraph{Plant Loop Pressure Difference {[}Pa{]}}\label{plant-loop-pressure-difference-pa}
+
+This output is the total pressure drop of a plant loop.~ This output is only recognized if a valid pressure simulation is being performed.~ To do this, the user must specify a pressure simulation type as an input in the PlantLoop object, and input at least one pressure drop curve on a branch of the plant loop.~ This particular output is relevant regardless of the location of pressure drop curves: demand side, supply side, or both.
+
+The following advanced output variables are also available for plant loops (and condenser loops) when advanced output variables are requested (e.g. ``Output:Diagnostics, DisplayAdvancedReportVariable;'').
+
+\begin{itemize}
+\item
+  HVAC,Average,Plant Demand Side Lumped Capacitance Temperature {[}C{]}
+\item
+  HVAC,Average,Plant Supply Side Lumped Capacitance Temperature {[}C{]}
+\item
+  HVAC,Average,Plant Component Distributed Demand Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Plant Demand Side Lumped Capacitance Temperature {[}C{]}}\label{plant-demand-side-lumped-capacitance-temperature-c}
+
+\paragraph{Plant Supply Side Lumped Capacitance Temperature {[}C{]}}\label{plant-supply-side-lumped-capacitance-temperature-c}
+
+These two outputs are the temperature of the plant (or condenser) loop's working fluid where the two half-loops interface together.~ The program models heat capacitance in the volume of fluid inside the plant loop itself using two simple models for ``well-stirred'' tanks located at each of the half-loop inlet and outlet pairs.~ These tank models also receive the heat transferred to the fluid by the work done by pumping and resulting friction heating.~ One output is for the point where the fluid leaves the supply side and enters the demand side.~ The other output is for the point where the fluid leaves the demand side and enters the supply side.
+
+\paragraph{Plant Component Distributed Demand Rate {[}W{]}}\label{plant-component-distributed-demand-rate-w}
+
+This output is available for every component on every branch in a plant (or condenser) loop and shows the outcome of the load dispatch performed by the operation schemes.~ This the load in watts passed from the supervisor routines to the equipment component models.~ This provides a record of what a particular component was asked to do by the supervisory routines. This can be useful for diagnosing issues in operation schemes when a component or loop is failing to meet the load.
+
+\subsection{CondenserLoop}\label{condenserloop}
+
+The condenser loop input is very similar to that for the plant loop. As of version 7, the two loops are modeled the same way and inside the program all condenser loops are just plant loops. (In future versions of the program, this CondenserLoop object might be deprecated and these loops will be described using the PlantLoop object.)~ The main differences are the applicable components and operation schemes. This is depicted in the following diagram.
+
+!{[}CondenserLoopSyntax (media/image136.png)
+
+Figure 74. Condenser Loop Input Syntax Map
+
+\subsubsection{Inputs}\label{inputs-1-032}
+
+\paragraph{Field: Name}\label{field-name-1-031}
+
+This alpha field is used as an identifying field for the condenser loop.
+
+\paragraph{Field: Fluid Type}\label{field-fluid-type-1-000}
+
+This alpha field must be a keyword selected from the list of available fluids for an EnergyPlus plant loop. Either \textbf{Water} or \textbf{UserDefinedFluidType} may be used. If the UserDefinedFluidType keyword is used, the following input field i.e.~User Defined Fluid Type must have a value (namely the name of a FluidProperties:GlycolConcentration object).
+
+\paragraph{Field: User Defined Fluid Type}\label{field-user-defined-fluid-type-1}
+
+This alpha field must be specified when the previous field is set to \textbf{UserDefinedFluidType} otherwise it could be left blank. \textbf{Water}, \textbf{EthyleneGlycol}, and \textbf{PropoleneGlycol} are all ``built-in'' fluids for EnergyPlus (that is, all of the appropriate properties are contained within the program). If the fluid specified here is a mixture of water and ethylene or propylene glycol, then only FluidProperties:GlycolConcentration objects need to be specified and the name of the appropriate one is used here. For another water/glycol mixture, a complete set of fluid property data (FluidProperties:Name and FluidProperties:Temperature objects plus multiple FluidProperties:Concentration objects for specific heat, density, etc.) must be specified (Ref dataset: GlycolPropertiesRefData.idf).
+
+\paragraph{Field: Condenser Equipment Operation Scheme Name}\label{field-condenser-equipment-operation-scheme-name}
+
+This alpha field is used as an identifying field for the condenser operation scheme. This field ties to the Condenser Operation Schemes input structure, which must also be defined.
+
+\paragraph{Field: Condenser Loop Temperature Setpoint Node Name}\label{field-condenser-loop-temperature-setpoint-node-name}
+
+This alpha field is used to identify the node which the Loop Manager will access the temperature setpoint that it will try to maintain. This is typically the Condenser Loop Supply Side Outlet Node so that it will not interfere with component temperature setpoints. An associated temperature setpoint manager will need to be defined.
+
+\paragraph{Field: Maximum Loop Temperature}\label{field-maximum-loop-temperature-1}
+
+This numeric field contains the maximum allowable temperature in Celsius for this loop.
+
+\paragraph{Field: Minimum Loop Temperature}\label{field-minimum-loop-temperature-1}
+
+This numeric field contains the minimum allowable temperature in Celsius for this loop. This minimum loop temperature is used by the cooling towers to make sure that the minimum is not violated to keep the equipment safe. The minimum is also used to trigger the minimum temperature warning and will notify the user if it gets too low.
+
+\paragraph{Field: Maximum Loop Flow Rate}\label{field-maximum-loop-flow-rate-1}
+
+This numeric field contains the maximum loop flow rate in cubic meters per second. This field is autosizable.
+
+\paragraph{Field: Minimum Loop Flow Rate}\label{field-minimum-loop-flow-rate-1}
+
+This numeric field contains the minimum loop flow rate in cubic meters per second.
+
+\paragraph{Field: Condenser Loop Volume}\label{field-condenser-loop-volume}
+
+Volume of the condenser loop in m\(^{3}\). This numeric field contains the loop volume for the entire loop, i.e., both the demand side and the supply side. This is used for the loop capacitance calculation. Loop volume (m\(^{3}\)) could be calculated from pipe size data but this is not usually known. If zero volume is specified the loop has no fluid heat capacity. If a very large capacitance is specified unrealistic time delay may result and there may be poor response to changes in loop setpoint temperature. The loop capacitance \textbf{autocalculate} option gives reasonable values for most system sizes. This calculation is described in the Engineering Reference manual.
+
+\paragraph{Field: Condenser Side Inlet Node Name}\label{field-condenser-side-inlet-node-name}
+
+This required alpha field contains the identifying name given to the Condenser Side Inlet Node. This node is the inlet to the supply side of the loop.
+
+\paragraph{Field: Condenser Side Outlet Node Name}\label{field-condenser-side-outlet-node-name}
+
+This required alpha field contains the identifying name given to the Condenser Side Outlet Node. This node is the outlet of the supply side of the loop.
+
+\paragraph{Field: Condenser Side Branch List Name}\label{field-condenser-side-branch-list-name}
+
+This required alpha field contains the identifying name given to the Condenser Side Branch List. The list referenced here should list all the branches on the supply side of the loop.
+
+\paragraph{Field: Condenser Side Connector List Name}\label{field-condenser-side-connector-list-name}
+
+This required alpha field contains the identifying name given to the Condenser Side Connector List.~ The list referenced here should list the splitter and mixer on the supply side of the loop.
+
+\paragraph{Field: Demand Side Inlet Node Name}\label{field-demand-side-inlet-node-name-1}
+
+This required alpha field contains the identifying name given to the Demand Side Inlet Node.~ This node is the inlet to the demand side of the loop.
+
+\paragraph{Field: Demand Side Outlet Nodes Name}\label{field-demand-side-outlet-nodes-name}
+
+This required alpha field contains the identifying name given to the Demand Side Outlet Node. This node is the outlet of the demand side of the loop.
+
+\paragraph{Field: Condenser Demand Side Branch List Name}\label{field-condenser-demand-side-branch-list-name}
+
+This required alpha field contains the identifying name given to the Demand Side Branch List.~ The list referenced here should list all the branches on the demand side of the loop.
+
+\paragraph{Field: Condenser Demand Side Connector List Name}\label{field-condenser-demand-side-connector-list-name}
+
+This required alpha field contains the identifying name given to the Demand Side Connector List. The list referenced here should list the splitter and mixer on the demand side of the loop.
+
+\paragraph{Field: Load Distribution Scheme}\label{field-load-distribution-scheme-1-000}
+
+This alpha field contains the Load Distribution Scheme Keyword. The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. \textbf{Optimal} operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{SequentialLoad} loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. \textbf{UniformLoad} evenly distributes the loop demand among all available components on the equipment list for a given load range. \textbf{SequentialUniformPLR} loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. \textbf{UniformPLR} will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
+
+Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
+
+\paragraph{Field: Pressure Simulation Type}\label{field-pressure-simulation-type-1}
+
+This field lets user to choose if this plant loop will be involved in a pressure drop calculation.~ This requires that at least one branch on the loop have pressure drop data.~ If not, an error will be thrown due to the input mismatch.~ Currently there are two pressure drop simulation types: ``PumpPowerCorrection'' and ``LoopFlowCorrection''.~ In both of these methods, branch pressure drop data is used to calculate a dynamic loop pressure drop and is used to update pumping power accordingly.~ The flow correction method allows the user to enter information regarding the pressure curve of a constant speed pump so that the simulation can dynamically resolve the pressure vs.~flow relationship in the plant loop.~ This is limited to constant speed pumps, as the variable speed pumps are expected to resolve as if it were controlled by a variable drive, so that they can inherently meet any pressure and flow demand required by the loop.~ This is also limited to ``loop pumps'', where there is a single pump on the plant loop.~ Common pipe simulations and ``branch pump'' simulations are not compatible with this level of pressure simulation.~ See the documentation for the Pump:ConstantSpeed in order to determine required inputs for this pressure simulation method to be performed.~ In the pressure drop system, parallel flow rates are not resolved (to match the pressure drop for the parallel system).~ Enhancements to this calculation are planned which will allow parallel branch flow resolution.~ See the Engineering Reference document for more information on how this works.
+
+An example of this statement used in an IDF is:
+
+\begin{lstlisting}
+
+  CondenserLoop,
+      Condenser Water Loop,    !- Name
+      Water,                   !- Fluid Type
+      ,                        !- User Defined Fluid Type
+      Tower Loop Operation,    !- Condenser Equipment Operation Scheme Name
+      Condenser Supply Outlet Node,  !- Condenser Loop Temperature Setpoint Node Name
+      80,                      !- Maximum Loop Temperature {C}
+      10,                      !- Minimum Loop Temperature {C}
+      autosize,                !- Maximum Loop Flow Rate {m3/s}
+      0.0,                     !- Minimum Loop Flow Rate {m3/s}
+      autocalculate,           !- Condenser Loop Volume {m3}
+      Condenser Supply Inlet Node,  !- Condenser Side Inlet Node Name
+      Condenser Supply Outlet Node,  !- Condenser Side Outlet Node Name
+      Condenser Supply Side Branches,  !- Condenser Side Branch List Name
+      Condenser Supply Side Connectors,  !- Condenser Side Connector List Name
+      Condenser Demand Inlet Node,  !- Demand Side Inlet Node Name
+      Condenser Demand Outlet Node,  !- Demand Side Outlet Node Name
+      Condenser Demand Side Branches,  !- Condenser Demand Side Branch List Name
+      Condenser Demand Side Connectors,  !- Condenser Demand Side Connector List Name
+      SequentialLoad;              !- Load Distribution Scheme
+
+    SetpointManager:FollowOutdoorAirTemperature,
+      MyCondenserControl,      !- Name
+      Temperature,             !- Control Variable
+      OutdoorAirWetBulb,       !- Reference Temperature Type
+      0,                       !- Offset Temperature Difference {deltaC}
+      80,                      !- Maximum Setpoint Temperature {C}
+      10,                      !- Minimum Setpoint Temperature {C}
+      Condenser Supply Outlet Node;  !- Setpoint Node or NodeList Name
+
+    CondenserLoop,
+      Chilled Water Condenser Loop,  !- Name
+      UserDefinedFluidType,    !- Fluid Type
+      PropyleneGlycol15Percent,!- User Defined Fluid Type
+      Tower Loop Operation,    !- Condenser Equipment Operation Scheme Name
+      Condenser Supply Outlet Node,  !- Condenser Loop Temperature Setpoint Node Name
+      80,                      !- Maximum Loop Temperature {C}
+      10,                      !- Minimum Loop Temperature {C}
+      0.00330000,              !- Maximum Loop Flow Rate {m3/s}
+      0,                       !- Minimum Loop Flow Rate {m3/s}
+      autocalculate,           !- Condenser Loop Volume {m3}
+      Condenser Supply Inlet Node,  !- Condenser Side Inlet Node Name
+      Condenser Supply Outlet Node,  !- Condenser Side Outlet Node Name
+      Condenser Supply Side Branches,  !- Condenser Side Branch List Name
+      Condenser Supply Side Connectors,  !- Condenser Side Connector List Name
+      Condenser Demand Inlet Node,  !- Demand Side Inlet Node Name
+      Condenser Demand Outlet Node,  !- Demand Side Outlet Node Name
+      Condenser Demand Side Branches,  !- Condenser Demand Side Branch List Name
+      Condenser Demand Side Connectors,  !- Condenser Demand Side Connector List Name
+      SequentialLoad;              !- Load Distribution Scheme
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-018}
+
+\begin{itemize}
+\item
+  HVAC,Average,Plant Supply Side Cooling Demand Rate {[}W{]}
+\item
+  HVAC,Average,Plant Supply Side Heating Demand Rate {[}W{]}
+\item
+  HVAC,Average,Plant Supply Side Inlet Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Plant Supply Side Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Plant Supply Side Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Cond Loop Demand Not Distributed {[}W{]}
+\item
+  HVAC,Average,Plant Supply Side Unmet Demand Rate {[}W{]}
+\item
+  HVAC,Average,Plant Demand Side Loop Pressure Difference {[}Pa{]}
+\item
+  HVAC,Average,Plant Supply Side Loop Pressure Difference {[}Pa{]}
+\item
+  HVAC,Average,Plant Loop Pressure Difference {[}Pa{]}
+\end{itemize}
+
+\paragraph{Plant Supply Side Cooling Demand Rate {[}W{]}}\label{plant-supply-side-cooling-demand-rate-w-1}
+
+This is the value of the net demand required to meet the cooling setpoint of the loop.~ If the loop setpoint is met for the current HVAC timestep, Plant Supply Side Cooling Demand Rate will equal sum of the total cooling demand from the demand side components on the loop (typically condenser coils of chillers, etc.).~ It will also equal the cooling output of all condensing equipment such as cooling towers on the loop less any pump heat added to the fluid.~ For example, for a condenser loop with one tower and one pump serving one chiller, Plant Supply Side Cooling Demand Rate will equal the tower water-side heat transfer less the pump heat to fluid, and it will also equal the chiller condenser heat transfer rate.
+
+If the condenser loop setpoint is not met, Plant Supply Side Cooling Demand Rate will equal the sum of the total cooling demand from the demand side components on the loop plus the additional cooling required to bring the loop flow to setpoint.~ If the loop remains off setpoint for successive timesteps, the demand required to return to setpoint will repeat in each timestep until the loop reaches setpoint.~ For this reason, Plant Supply Side Cooling Demand Rate should not be summed over time, because it will overstate the demand whenever the loop is off setpoint.
+
+\paragraph{Plant Supply Side Heating Demand Rate {[}W{]}}\label{plant-supply-side-heating-demand-rate-w-1}
+
+This is the value of the net demand required to meet the heating setpoint of the loop.~ If the loop setpoint is met for the current HVAC timestep, Plant Supply Side Heating Demand Rate will equal sum of the total heating demand from the demand side components on the loop.~ It will also equal the heating output of all heating equipment on the supply side of the loop plus any pump heat added to the fluid.~ For example, for a condenser loop with one ground loop heat exchanger and one pump serving one water-to-water heat pump, Plant Supply Side Heating Demand Rate will equal the ground loop heat transfer plus the pump heat to fluid, and it will also equal the heat pump condenser side heat transfer rate.
+
+If the condenser loop setpoint is not met, Plant Supply Side Heating Demand Rate will equal the sum of the total heating demand from the demand side components on the loop plus the additional heating required to bring the loop flow to setpoint.~ If the loop remains off setpoint for successive timesteps, the demand required to return to setpoint will repeat in each timestep until the loop reaches setpoint.~ For this reason, Plant Supply Side Heating Demand Rate should not be summed over time, because it will overstate the demand whenever the loop is off setpoint.
+
+\paragraph{Plant Supply Side Inlet Mass Flow Rate {[}kg/s{]}}\label{plant-supply-side-inlet-mass-flow-rate-kgs-1}
+
+This is the value of the mass flow rate at the Inlet to Condenser Loop on the supply side. There is not an associated Condenser Loop outlet node flow rate since continuity must be maintained in the loop and the outlet must be the same.
+
+\paragraph{Plant Supply Side Inlet Temperature {[}C{]}}\label{plant-supply-side-inlet-temperature-c-1}
+
+This is the value of the temperature at the Inlet to the condenser loop on the supply side.
+
+\paragraph{Cond Loop OutletNode Temperature {[}C{]}}\label{cond-loop-outletnode-temperature-c}
+
+This is the value of the temperature at the outlet to the condenser loop on the supply side.
+
+\paragraph{Cond Loop Demand Not Distributed {[}W{]}}\label{cond-loop-demand-not-distributed-w}
+
+This is the value of the demand that could not be distributed to the condenser equipment because of some constraint in the operation scheme.~ This is a record of the loop operation scheme supervisory controls after attempting to distribute the load.~ For example it would be~ non-zero in situations where the load is larger than the upper limit of capacities set for the condenser equipment controls.~ This output is for \emph{before} the equipment has actually been simulated whereas the separate output Plant Supply Side Unmet Demand Rate is for \emph{after} the equipment has simulated.
+
+\paragraph{Plant Supply Side Unmet Demand Rate {[}W{]}}\label{plant-supply-side-unmet-demand-rate-w-1}
+
+This is the value of the demand NOT provided by the condenser equipment to meet the heating or cooling setpoint of the loop. The value is positive when the condenser equipment cannot meet the setpoint, and the value is negative when the condenser equipment provides more than enough heating or cooling to meet the setpoint. A negative value can happen when the amount of demand is smaller than the minimum capacity of the equipment using the minimum part load ratio.
+
+\paragraph{Plant Demand Side Loop Pressure Difference {[}Pa{]}}\label{plant-demand-side-loop-pressure-difference-pa-1}
+
+This field is the demand side pressure drop of a condenser loop.~ This output is only recognized if a valid pressure simulation is being performed.~ To do this, the user must specify a pressure simulation type as an input in the CondenserLoop object, and input at least one pressure drop curve on a branch of the plant/condenser loop.~ This particular output is only relevant if the user puts that curve on the demand side of the loop.
+
+\paragraph{Plant Supply Side Loop Pressure Difference {[}Pa{]}}\label{plant-supply-side-loop-pressure-difference-pa-1}
+
+This field is the supply side pressure drop of a condenser loop.~ This output is only recognized if a valid pressure simulation is being performed.~ To do this, the user must specify a pressure simulation type as an input in the CondenserLoop object, and input at least one pressure drop curve on a branch of the plant/condenser loop.~ This particular output is only relevant if the user puts that curve on the supply side of the loop.
+
+\paragraph{~Plant Loop Pressure Difference {[}Pa{]}}\label{plant-loop-pressure-difference-pa-1}
+
+This field is the total pressure drop of a condenser loop.~ This output is only recognized if a valid pressure simulation is being performed.~ To do this, the user must specify a pressure simulation type as an input in the CondenserLoop object, and input at least one pressure drop curve on a branch of the plant/condenser loop.~ This particular output is relevant regardless of the location of pressure drop curves: demand side, supply side, or both.
diff --git a/doc/input-output-reference/src/overview/group-plant-equipment.tex b/doc/input-output-reference/src/overview/group-plant-equipment.tex
new file mode 100644
index 00000000000..3a6c95e9a1a
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-plant-equipment.tex
@@ -0,0 +1,6729 @@
+\section{Group -- Plant Equipment}\label{group-plant-equipment}
+
+\subsection{Equipment Types}\label{equipment-types-000}
+
+In each \textbf{PlantEquipmentList} described using the above syntax, various equipment types and names must be given. Each type-name pair must then have a corresponding equipment definition. This subsection lists the various equipment types that are available and examples from an IDF. Where appropriate, notes and comments on the input structure are provided.
+
+\subsection{Generic Chiller Outputs}\label{generic-chiller-outputs}
+
+Many output variable names are common across all chiller types. These generic chiller output names all begin with the word ``Chiller''. Certain chiller types have additional output variables which are specific to that type of chiller. Chiller energy use is added to the appropriate plant-level meters as a cooling end-use.
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Electric Energy {[}J{]}
+\item
+  Zone,Meter,Electricity:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:Electricity {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Evaporator Cooling Energy {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Plant {[}J{]}
+\item
+  Zone,Meter,Chillers:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Meter,HeatRejection:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller COP {[}W/W{]}
+\end{itemize}
+
+The following output is applicable only for air-cooled or evap-cooled chillers
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\end{itemize}
+
+The following outputs are applicable only for evap-cooled chillers
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+The following three outputs are only available for water-cooled chillers
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Drive Shaft Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Drive Shaft Energy {[}J{]}
+\item
+  Zone,Meter,HeatRecovery:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Lube Recovered Heat Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Lube Recovered Heat Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Jacket Recovered Heat Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Jacket Recovered Heat Energy {[}J{]}
+\item
+  HVAC,Average, Chiller Exhaust Recovered Heat Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Exhaust Recovered Heat Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Total Recovered Heat Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Total Recovered Heat Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Exhaust Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Effective Heat Rejection Temperature {[}C{]}
+\end{itemize}
+
+The following blocks of outputs are for steam and fuel-driven chillers
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Gas Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Gas Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Gas Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum,Chiller Gas Mass {[}kg{]}
+\end{itemize}
+
+For steam absorption chillers:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Source Steam Rate {[}W{]}
+\item
+  HVAC,Sum, Chiller Source Steam Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Steam Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+For hot water absorption chillers:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Source Hot Water Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Source Hot Water Energy {[}J{]}
+\item
+  Zone,Meter,Steam:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Hot Water Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+The following output is applicable only for indirect absorption chillersHVAC,Average,Chiller Part Load Ratio
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Cycling Ratio {[]}
+\item
+  HVAC,Average,Chiller Propane Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Propane Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Propane Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Diesel Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Diesel Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Diesel Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Gasoline Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Gasoline Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Gasoline Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller FuelOil\#1 Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller FuelOil\#1 Energy {[}J{]}
+\item
+  HVAC,Average,Chiller FuelOil\#1 Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller FuelOil\#2 Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller FuelOil\#2 Energy {[}J{]}
+\item
+  HVAC,Average,Chiller FuelOil\#2 Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller OtherFuel1 Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller OtherFuel1 Energy {[}J{]}
+\item
+  HVAC,Average,Chiller OtherFuel1 Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller OtherFuel2 Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller OtherFuel2 Energy {[}J{]}
+\item
+  HVAC,Average,Chiller OtherFuel2 Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\subsubsection{Chiller Electric Power {[}W{]}}\label{chiller-electric-power-w}
+
+\subsubsection{Chiller Electric Energy {[}J{]}}\label{chiller-electric-energy-j}
+
+These outputs are the electric power input to the chiller. In the case of steam or fuel-powered chillers, this repesents the internal chiller pumps and other electric power consumption. Consumption is metered on Cooling:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\subsubsection{Chiller Evaporator Cooling Rate {[}W{]}}\label{chiller-evaporator-cooling-rate-w}
+
+\subsubsection{Chiller Evaporator Cooling Energy {[}J{]}}\label{chiller-evaporator-cooling-energy-j}
+
+These outputs are the evaporator heat transfer which is the cooling delivered by the chiller. Chiller Evaporator Cooling Energy is metered on Chillers:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\subsubsection{Chiller Evaporator Inlet Temperature {[}C{]}}\label{chiller-evaporator-inlet-temperature-c}
+
+\subsubsection{Chiller Evaporator Outlet Temperature {[}C{]}}\label{chiller-evaporator-outlet-temperature-c}
+
+\subsubsection{Chiller Evaporator Mass Flow Rate {[}kg/s{]}}\label{chiller-evaporator-mass-flow-rate-kgs}
+
+These outputs are the evaporator (chilled water) inlet and outlet temperatures and flow rate.
+
+\subsubsection{Chiller COP {[}W/W{]}}\label{chiller-cop-ww}
+
+This output is the coefficient of performance for the chiller during cooling operation. It is calculated as the evaporator heat transfer rate (Chiller Evaporator Cooling Rate) divided by the ``fuel'' consumption rate by the chiller. For the constant COP and electric chillers, the ``fuel'' is electricity so the divisor is Chiller Electric Power {[}W{]}. For the absorption chiller, the ``fuel'' is steam so the divisor is Steam Consumption Rate {[}W{]}.
+
+\emph{Note that this variable is reported as zero when the chiller is not operating. When reported for frequencies longer than ``detailed'' (such as timestep, hourly, daily, monthly or environment), this output will only be meaningful when the chiller is operating for the entire reporting period. To determine an average COP for a longer time period, compute the COP based on total evaporator heat transfer divided by total electric or fuel input over the desired period.}
+
+\subsubsection{Chiller Part Load Ratio}\label{chiller-part-load-ratio}
+
+This output is the operating part-load ratio of the indirect absorption chiller. This output may fall below the minimum part-load ratio specified in the input. For this case, the Chiller Cycling Ratio is used to further define the performance of the indirect absorption chiller.
+
+\subsubsection{Chiller Cycling Ratio}\label{chiller-cycling-ratio}
+
+This output is the fraction of the timestep the indirect absorption chiller operates. When the chiller operates above the minimum part-load ratio, a Chiller Cycling Ratio of 1 is reported. When the chiller operates below the minimum part-load ratio, the Chiller Cycling Ratio reports the fraction of the timestep the indirect absorption chiller operates.
+
+\subsubsection{Chiller Condenser Heat Transfer Rate {[}W{]}}\label{chiller-condenser-heat-transfer-rate-w}
+
+\subsubsection{Chiller Condenser Heat Transfer Energy {[}J{]}}\label{chiller-condenser-heat-transfer-energy-j}
+
+These outputs are the condenser heat transfer which is the heat rejected from the chiller to either a condenser water loop or through an air-cooled condenser. Chiller Condenser Heat Transfer Energy is metered on HeatRejection:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\subsubsection{Chiller Condenser Inlet Temperature {[}C{]}}\label{chiller-condenser-inlet-temperature-c}
+
+This output is the condenser (heat rejection) inlet temperature for air-cooled or evap-cooled chillers. For an air-cooled chiller, this output would be the dry-bulb temperature of the air entering the condenser coil. For an evap-cooled chiller, this output would be the wet-bulb temperature of the air entering the evaporatively-cooled condenser coil.
+
+\subsubsection{Chiller Basin Heater Electric Power {[}W{]}}\label{chiller-basin-heater-electric-power-w}
+
+\subsubsection{Chiller Basin Heater Electric Energy {[}J{]}}\label{chiller-basin-heater-electric-energy-j}
+
+These outputs are the electric power input to the chiller's basin heater (for evaporatively-cooled condenser type). Consumption is metered on Chillers:Electricity, Electricity:Plant, and Electricity:Facility
+
+\subsubsection{Chiller Condenser Inlet Temperature {[}C{]}}\label{chiller-condenser-inlet-temperature-c-1}
+
+\subsubsection{Chiller Condenser Outlet Temperature {[}C{]}}\label{chiller-condenser-outlet-temperature-c}
+
+\subsubsection{Chiller Condenser Mass Flow Rate {[}kg/s{]}}\label{chiller-condenser-mass-flow-rate-kgs}
+
+These outputs are the condenser (heat rejection) inlet and outlet temperatures and flow rate for water-cooled chillers.
+
+\subsubsection{Chiller Drive Shaft Power {[}W{]}}\label{chiller-drive-shaft-power-w}
+
+\subsubsection{Chiller Drive Shaft Energy {[}J{]}}\label{chiller-drive-shaft-energy-j}
+
+For engine-driven and turbine-driven chillers, these outputs are the shaft power produced by the prime mover and transferred to the chiller compressor.
+
+\subsubsection{Chiller Lube Recovered Heat Rate {[}W{]}}\label{chiller-lube-recovered-heat-rate-w}
+
+\subsubsection{Chiller Lube Recovered Heat Energy {[}J{]}}\label{chiller-lube-recovered-heat-energy-j}
+
+\subsubsection{Chiller Jacket Recovered Heat Rate {[}W{]}}\label{chiller-jacket-recovered-heat-rate-w}
+
+\subsubsection{Chiller Jacket Recovered Heat Energy {[}J{]}}\label{chiller-jacket-recovered-heat-energy-j}
+
+\subsubsection{Chiller Exhaust Recovered Heat Rate {[}W{]}}\label{chiller-exhaust-recovered-heat-rate-w}
+
+\subsubsection{Chiller Exhaust Recovered Heat Energy {[}J{]}}\label{chiller-exhaust-recovered-heat-energy-j}
+
+\subsubsection{Chiller Total Recovered Heat Rate {[}W{]}}\label{chiller-total-recovered-heat-rate-w}
+
+\subsubsection{Chiller Total Recovered Heat Energy {[}J{]}}\label{chiller-total-recovered-heat-energy-j}
+
+For chillers with heat recovery, such as engine-driven chillers, these outputs are the components of recoverable energy available. For a given chiller type, one or more of the following components may be applicable:~ Lube (engine lubricant), Jacket (engine coolant), Exhaust (engine exhaust), and Total. Chiller Lube Recovered Heat Energy, Chiller Jacket Recovered Heat Energy, and Chiller Exhaust Heat Recovery Energy are metered on HeatRecovery:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\subsubsection{Chiller Exhaust Temperature {[}C{]}}\label{chiller-exhaust-temperature-c}
+
+This is the exhaust temperature leaving an engine chiller.
+
+\subsubsection{Chiller Heat Recovery Inlet Temperature {[}C{]}}\label{chiller-heat-recovery-inlet-temperature-c}
+
+\subsubsection{Chiller Heat Recovery Outlet Temperature {[}C{]}}\label{chiller-heat-recovery-outlet-temperature-c}
+
+\subsubsection{Chiller Heat Recovery Mass Flow Rate {[}kg/s{]}}\label{chiller-heat-recovery-mass-flow-rate-kgs}
+
+These outputs are the heat recovery inlet and outlet temperatures and flow rate for chillers with heat recovery such as engine-driven and gas turbine chillers.
+
+\subsubsection{Chiller Effective Heat Rejection Temperature {[}C{]}}\label{chiller-effective-heat-rejection-temperature-c}
+
+This output variable is available for heat recovery chillers that model split bundle condenser.~ The condenser fluid temperatures used to characterize chiller performance are modified to account for the temperature of the heat recovery fluid.~ This output is the resulting temperature used for characterizing chiller performance and is a blend of the temperatures in the condenser and heat recovery fluid streams.~ For the Chiller:Electric and Chiller:Electric:EIR models, this is an effective inlet temperature while for the Chiller:Electric:ReformulatedEIR model, this is an effective outlet temperature.
+
+\subsubsection{Chiller \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{chiller-fuel-type-rate-w}
+
+\subsubsection{Chiller \textless{}Fuel Type\textgreater{} Energy~ {[}J{]}}\label{chiller-fuel-type-energy-j}
+
+\subsubsection{Chiller~ \textless{}Fuel Type\textgreater{} Mass Flow Rate {[}kg/s{]}}\label{chiller-fuel-type-mass-flow-rate-kgs}
+
+\subsubsection{Chiller Gas~ Mass {[}kg{]} (Gas Turbine Chiller only)}\label{chiller-gas-mass-kg-gas-turbine-chiller-only}
+
+These outputs are the steam or fuel input for steam or fuel-fired chillers. Valid fuel types depend on the type of chiller. \textless{}Fuel Type\textgreater{} may be one of:~ Gas (natural gas), Steam, Propane, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1 and OtherFuel2. Consumption is metered on Cooling:\textless{}Fuel Type\textgreater{}, \textless{}Fuel Type\textgreater{}:Plant, and \textless{}Fuel Type\textgreater{}:Facility.
+
+\subsubsection{Chiller Source Hot Water Rate {[}W{]}}\label{chiller-source-hot-water-rate-w}
+
+\subsubsection{Chiller Source Hot Water Energy {[}J{]}}\label{chiller-source-hot-water-energy-j}
+
+\subsubsection{Chiller Source Steam Rate {[}W{]}}\label{chiller-source-steam-rate-w}
+
+\subsection{Chiller:Absorption}\label{chillerabsorption}
+
+\subsubsection{Inputs}\label{inputs-036}
+
+\paragraph{Field: Name}\label{field-name-035}
+
+This alpha field contains the identifying name for the absorption chiller.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-001}
+
+This numeric field contains the nominal cooling capability of the chiller in Watts.
+
+\paragraph{Field: Nominal Pumping Power}\label{field-nominal-pumping-power}
+
+This numeric field contains the nominal pumping power of the absorber in Watts.
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-000}
+
+This required alpha field contains the identifying name for the absorption chiller plant side inlet node.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-000}
+
+This required alpha field contains the identifying name for the absorption chiller plant side outlet node.
+
+\paragraph{Field: Condenser Inlet Node Name}\label{field-condenser-inlet-node-name}
+
+This required alpha field contains the identifying name for the absorption chiller condenser side inlet node.
+
+\paragraph{Field: Condenser Outlet Node Name}\label{field-condenser-outlet-node-name}
+
+This required alpha field contains the identifying name given to the Heat Recovery Loop Component Outlet Node.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-001}
+
+This numeric field contains the absorption chiller's minimum part load ratio. The expected range is between 0 and 1. The minimum part load is not the load where the machine shuts off, but where the amount of power remains constant to produce smaller loads than this fraction.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-001}
+
+This numeric field contains the absorption chiller's maximum part load ratio. This value may exceed 1, but the normal range is between 0 and 1.1.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-001}
+
+This numeric field contains the absorption chiller's optimum part load ratio. This is the part load ratio at which the chiller performs at its maximum COP.
+
+\paragraph{Field: Design Condenser Inlet Temperature}\label{field-design-condenser-inlet-temperature}
+
+This numeric field contains the absorption chiller's condenser inlet design temperature in Celsius.
+
+\paragraph{Field: Design Chilled Water Flow Rate}\label{field-design-chilled-water-flow-rate}
+
+For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate. The units are in cubic meters per second.
+
+\paragraph{Field: Design Condenser Water Flow Rate}\label{field-design-condenser-water-flow-rate}
+
+This numeric field contains the absorption chiller's design condenser water flow rate in cubic meters per second.
+
+\paragraph{Generator Heat Input Part Load Ratio Curve}\label{generator-heat-input-part-load-ratio-curve}
+
+The Generator Heat Input Part Load Ratio Curve is a quadratic equation that determines the Ratio of the generator load on the absorber to the demand on the chiller. The defining equation is:
+
+\begin{equation}
+SteamInputRatio = \frac{{C1}}{{PLR}} + C2 + C3 * PLR
+\end{equation}
+
+The following three fields contain the coefficients for the equation.
+
+\paragraph{Field: Coefficient 1 of the Steam Use Part Load Ratio Curve}\label{field-coefficient-1-of-the-steam-use-part-load-ratio-curve}
+
+C1 in the Generator Heat Input Part Load Ratio Curve. This value is obtained by fitting manufacturers' performance data to the curve.
+
+\paragraph{Field: Coefficient 2 of the Steam Use Part Load Ratio Curve}\label{field-coefficient-2-of-the-steam-use-part-load-ratio-curve}
+
+C2 in the Generator Heat Input Part Load Ratio Curve. This value is obtained by fitting manufacturers' performance data to the curve.
+
+\paragraph{Field: Coefficient 3 of the Steam Use Part Load Ratio Curve}\label{field-coefficient-3-of-the-steam-use-part-load-ratio-curve}
+
+C3 in the Generator Heat Input Part Load Ratio Curve. This value is obtained by fitting manufacturers' performance data to the curve.
+
+\paragraph{Pump Electric Use Part Load Ratio Curve}\label{pump-electric-use-part-load-ratio-curve}
+
+The Pump Electric Use Part Load Ratio Curve is a quadratic equation that determines the Ratio of~ the actual absorber pumping power to the nominal pumping power. The defining equation is:
+
+\begin{equation}
+ElectricInputRatio = C1 + C2 * PLR + C3 * PL{R^2}
+\end{equation}
+
+The following three fields contain the coefficients for the equation.
+
+\paragraph{Field: Coefficient 1 of the Pump Electric Use Part Load Ratio Curve}\label{field-coefficient-1-of-the-pump-electric-use-part-load-ratio-curve}
+
+C1 in the Pump Electric Use Part Load Ratio Curve. This value is obtained by fitting manufacturers' performance data to the curve.
+
+\paragraph{Field: Coefficient 2 of the Pump Electric Use Part Load Ratio Curve}\label{field-coefficient-2-of-the-pump-electric-use-part-load-ratio-curve}
+
+C2 in the Pump Electric Use Part Load Ratio Curve. This value is obtained by fitting manufacturers' performance data to the curve.
+
+\paragraph{Field: Coefficient 3 of the Pump Electric Use Part Load Ratio Curve}\label{field-coefficient-3-of-the-pump-electric-use-part-load-ratio-curve}
+
+C3 in the Pump Electric Use Part Load Ratio Curve. This value is obtained by fitting manufacturers' performance data to the curve.
+
+\paragraph{Field: Chilled Water Outlet Temperature Lower Limit}\label{field-chilled-water-outlet-temperature-lower-limit}
+
+This numeric field contains the lower limit for the evaporator outlet temperature. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn't get too cold.
+
+\paragraph{Field: Generator Inlet Node Name}\label{field-generator-inlet-node-name}
+
+This alpha field contains the identifying name given to the Generator Inlet Node. A steam or hot water loop is not required to simulate an absorption chiller. If a steam/hot water loop is used, enter the name of the generator inlet node.
+
+\paragraph{Field: Generator Outlet Node Name}\label{field-generator-outlet-node-name}
+
+This alpha field contains the identifying name given to the Generator Outlet Node. A steam or hot water loop is not required to simulate an absorption chiller. If a steam/hot water loop is used, enter the name of the generator outlet node.
+
+\paragraph{Field: Chiller Flow Mode}\label{field-chiller-flow-mode}
+
+This choice field determines how the chiller operates with respect to the intended fluid flow through the device's evaporator. ~There are three different choices for specifying operating modes for the intended flow behavior:~ ``NotModulated,'' ``ConstantFlow,'' and ``LeavingSetpointModulated.''~ NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.~ ConstantFlow is useful for constant speed pumping arrangements where the chiller's request for flow is stricter and can increase the overall loop flow.~ LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint at the evaporator outlet.~ For this absorption chiller, this mode also affects the flow rate on the generator connection.~ In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.~ The default, if not specified, is NotModulated.~ This flow mode does not impact the condenser loop connection.
+
+\paragraph{Field: Generator Fluid Type}\label{field-generator-fluid-type}
+
+This choice field specifies the type of fluid used to heat the generator solution. The valid choices are \textbf{HotWater} or \textbf{Steam}. This field should be specified as Steam or left blank if the generator inlet/outlet nodes are not specified.
+
+\paragraph{Field: Design Generator Fluid Flow Rate}\label{field-design-generator-fluid-flow-rate}
+
+This numeric field contains the absorption chiller's design condenser fluid flow rate in cubic meters per second.
+
+\paragraph{Field: Degree of Subcooling in Steam Generator}\label{field-degree-of-subcooling-in-steam-generator}
+
+Ideally, the steam trap located at the outlet of the generator should remove all the condensate immediately, however, there is a delay in this process in actual systems which causes the condensate to SubCool by a certain amount before leaving the generator. This amount of subcooling is included in the heat transferred to the solution in the generator. The minimum value is 0º Celsius and default is 5º Celsius. This field is not used when the generator inlet/outlet node are not specified or the generator is connected to a hot water loop.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-001}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Nominal Pumping Power, Design Chilled Water Flow Rate, Design Condenser Water Flow Rate and Design Generator Fluid Flow Rate. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+Following is an example input for an Absorption Chiller.
+
+\begin{lstlisting}
+
+Chiller:Absorption,
+      Big Chiller,             !- Chiller Name
+      50000,                   !- Nominal Capacity {W}
+      250,                     !- Nominal Pumping Power {W}
+      Big Chiller Inlet Node,  !- Plant_Side_Inlet_Node
+      Big Chiller Outlet Node, !- Plant_Side_Outlet_Node
+      Big Chiller Condenser Inlet Node,  !- Condenser_Side_Inlet_Node
+      Big Chiller Condenser Outlet Node,  !- Condenser_Side_Outlet_Node
+      0.15,                    !- Minimum Part Load Ratio
+      1.0,                     !- Maximum Part Load Ratio
+      0.65,                    !- Opt Part Load Ratio
+      35.0,                    !- Temp Design Condenser Inlet {C}
+      0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
+      0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
+      0.03303,                 !- Coefficient1 of the steam use part load ratio curve
+      0.6852,                  !- Coefficient2 of the steam use part load ratio curve
+      0.2818,                  !- Coefficient3 of the steam use part load ratio curve
+      1.0,                     !- Coefficient1 of the pump electric use part load ratio curve
+      0,                       !- Coefficient2 of the pump electric part load ratio curve
+      0,                       !- Coefficient3 of the pump electric use part load ratio curve
+      5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
+      AbsorberSteamInletNode,  !- Generator Inlet Node Name
+      AbsorberSteamOutletNode, !- Generator Outlet Node Name
+      VariableFlow,            !- Chiller Flow Mode
+      Steam,                   !- Generator Fluid Type
+      autosize,                !- Design Generator Volumetric Fluid Flow Rate {m3/s}
+      2.0;                     !- Degree of Subcooling in Steam Generator {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-025}
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Electric Energy {[}J{]}
+\item
+  Zone,Meter,Electricity:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:Electricity {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Evaporator Cooling Energy {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Plant {[}J{]}
+\item
+  Zone,Meter,Chillers:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Meter,HeatRejection:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller COP {[}W/W{]}
+\end{itemize}
+
+For Chillers with Steam Generators:
+
+\begin{itemize}
+\item
+  HVAC,Average, Chiller Source Steam Rate {[}W{]}
+\item
+  HVAC,Sum, Chiller Source Steam Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Steam Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+For Chillers with Hot Water Generators:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Source Hot Water Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Source Hot Water Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Hot Water Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+These chiller output variables are defined above under ``Generic Chiller Outputs.''
+
+\subsection{Chiller:Absorption:Indirect}\label{chillerabsorptionindirect}
+
+The Chiller:Absorption:Indirect object is an enhanced version of the absorption chiller model found in the Building Loads and System Thermodynamics (BLAST) program. This enhanced model is nearly identical to the existing absorption chiller model (Ref. Chiller:Absorption) with the exceptions that: 1) the enhanced indirect absorption chiller model provides more flexible performance curves and 2) chiller performance now includes the impact of varying evaporator, condenser, and generator temperatures. Since these absorption chiller models are nearly identical (i.e., the performance curves of the enhanced model can be manipulated to produce similar results to the previous model), it is quite probable that the Chiller:Absorption model will be deprecated in a future release of EnergyPlus.
+
+\subsubsection{Inputs}\label{inputs-1-033}
+
+\paragraph{Field: Name}\label{field-name-1-032}
+
+This required alpha field contains the identifying name for the indirect absorption chiller.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-1-001}
+
+This required numeric field contains the nominal cooling capability of the chiller in Watts. This field must be greater than 0 and is autosizable.
+
+\paragraph{Field: Nominal Pumping Power}\label{field-nominal-pumping-power-1}
+
+This required numeric field contains the nominal pumping power of the chiller in Watts. The minimum value for this field is 0 and is autosizable.
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-1-000}
+
+This required alpha field contains the identifying name for the chiller chilled water inlet node.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-1-000}
+
+This required alpha field contains the identifying name for the chiller chilled water outlet node.
+
+\paragraph{Field: Condenser Inlet Node Name}\label{field-condenser-inlet-node-name-1}
+
+This required alpha field contains the identifying name for the chiller condenser inlet node.
+
+\paragraph{Field: Condenser Outlet Node Name}\label{field-condenser-outlet-node-name-1}
+
+This required alpha field contains the identifying name given to the chiller outlet node.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-1-001}
+
+This numeric field contains the chiller's minimum part-load ratio. The expected range is between 0 and 1. The minimum part load is not the load where the machine shuts off, but where the amount of power remains constant to produce smaller loads than this fraction.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-1-001}
+
+This numeric field contains the chiller's maximum part-load ratio. This value may exceed 1, but the normal range is between 0 and 1.1.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-1-001}
+
+This numeric field contains the chiller's optimum part-load ratio. This is the part-load ratio at which the chiller performs at its maximum COP.
+
+\paragraph{Field: Design Condenser Inlet Temperature}\label{field-design-condenser-inlet-temperature-1}
+
+This numeric field contains the chiller's condenser inlet design temperature in Celsius. The default value for this field is 30º C and is only used when the Design Chilled Water Flow Rate is autosized.
+
+\paragraph{Field: Condenser Inlet Temperature Lower Limit}\label{field-condenser-inlet-temperature-lower-limit}
+
+This numeric field contains the chiller's lower limit for the condenser entering water temperature in Celsius. The default value for this field is 15º C. If this limit is exceeded, a warning message will report the incident. No correction to chiller capacity is made for low condenser entering water temperatures.
+
+\paragraph{Field: Chilled Water Outlet Temperature Lower Limit}\label{field-chilled-water-outlet-temperature-lower-limit-1}
+
+This numeric field contains the chiller's lower limit for the evaporator leaving water temperature in Celsius. The default value for this field is 5º C. If this limit is exceeded, a warning message will report the incident. No correction to chiller capacity is made for low evaporator leaving water temperatures.
+
+\paragraph{Field: Design Chilled Water Flow Rate}\label{field-design-chilled-water-flow-rate-1}
+
+This numeric input specifies the design evaporator volumetric flow rate in cubic meters per second. The value specified must be greater than 0 or this field is autosizable. For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate.
+
+\paragraph{Field: Design Condenser Water Flow Rate}\label{field-design-condenser-water-flow-rate-1}
+
+This numeric field specifies the chiller's design condenser water flow rate in cubic meters per second. The value specified must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: Chiller Flow Mode}\label{field-chiller-flow-mode-1}
+
+This choice field determines how the chiller operates with respect to the intended fluid flow through the device's evaporator.~ There are three different choices for specifying operating modes for the intended flow behavior:~ ``NotModulated,'' ``ConstantFlow,'' and ``LeavingSetpointModulated.''~ NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.~ ConstantFlow is useful for constant speed pumping arrangements where the chiller's request for flow is stricter and can increase the overall loop flow.~ LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint at the evaporator outlet.~ For this absorption chiller, this mode also affects the flow rate on the generator connection.~ In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.~ The default, if not specified, is NotModulated.~ This flow mode does not impact the condenser loop connection.
+
+\paragraph{Field: Generator Heat Input Function of Part Load Ratio Curve Name}\label{field-generator-heat-input-function-of-part-load-ratio-curve-name}
+
+This required alpha field specifies the name of the curve used to determine the heat input to the chiller. The curve is a quadratic or cubic curve which characterizes the heat input as a function of chiller part-load ratio. The curve output is multiplied by the chiller's nominal capacity and operating part-load ratio or minimum part-load ratio, whichever is greater, to determine the amount of heat input required for the given operating conditons.
+
+\paragraph{Field: Pump Electric Input Function of Part Load Ratio Curve Name}\label{field-pump-electric-input-function-of-part-load-ratio-curve-name}
+
+This alpha field specifies the name of the curve used to determine the pump electrical input to the chiller. The curve is a quadratic or cubic curve which characterizes the pump electrical power as a function of chiller part-load ratio. The curve output is multiplied by the chiller's nominal pumping power and operating part-load ratio or minimum part-load ratio, whichever is greater, to determine the amount of pumping power required for the given operating conditons.
+
+\paragraph{Field: Generator Inlet Node Name}\label{field-generator-inlet-node-name-1}
+
+This alpha field contains the identifying name given to the Generator Inlet Node. A steam or hot water loop is not required to simulate an indirect absorption chiller. If a steam/hot water loop is used, enter the name of the generator inlet node.
+
+\paragraph{Field: Generator Outlet Node Name}\label{field-generator-outlet-node-name-1}
+
+This alpha field contains the identifying name given to the Generator Outlet Node. A steam or hot water loop is not required to simulate an indirect absorption chiller. If a steam/hot water loop is used, enter the name of the generator outlet node.
+
+\paragraph{Field: Capacity Correction Function of Condenser Temperature Curve Name}\label{field-capacity-correction-function-of-condenser-temperature-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic curve which correlates the chiller's evaporator capacity as a function of condenser entering water temperature. This curve is used to correct nominal capacity at off-design condensing temperatures.
+
+\paragraph{Field: Capacity Correction Function of Chilled Water Temperature Curve Name}\label{field-capacity-correction-function-of-chilled-water-temperature-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic curve which correlates the chiller's evaporator capacity as a function of evaporator leaving water temperature. This curve is used to correct nominal capacity at off-design evaporator temperatures.
+
+\paragraph{Field: Capacity Correction Function of Generator Temperature Curve Name}\label{field-capacity-correction-function-of-generator-temperature-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic curve which correlates the chiller's evaporator capacity as a function of generator entering water temperature. This curve is used to correct nominal capacity at off-design evaporator temperatures and is only used when the Generator Fluid Type is specified as Hot Water.
+
+\paragraph{Field: Generator Heat Input Correction Function of Condenser Temperature Curve Name}\label{field-generator-heat-input-correction-function-of-condenser-temperature-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic curve which correlates the chiller's heat input as a function of condenser entering water temperature. This curve is used to correct generator heat input at off-design condensing temperatures.
+
+\paragraph{Field: Generator Heat Input Correction Function of Chilled Water Temperature Curve Name}\label{field-generator-heat-input-correction-function-of-chilled-water-temperature-curve-name}
+
+This alpha field specifies the name of a quadratic or cubic curve which correlates the chiller's heat input as a function of evaporator leaving water temperature. This curve is used to correct generator heat input at off-design evaporator temperatures.
+
+\paragraph{Field: Generator Heat Source Type}\label{field-generator-heat-source-type}
+
+This choice field specifies the type of fluid used to heat the generator solution. The valid choices are \textbf{HotWater} or \textbf{Steam}. This input is used to identify the method used to calculate the generator mass flow rate. This field is not used if the generator inlet/outlet nodes are not specified. The default value is Steam.
+
+\paragraph{Field: Design Generator Fluid Flow Rate}\label{field-design-generator-fluid-flow-rate-1}
+
+This numeric field specifies the chiller's design generator \emph{fluid} flow rate in cubic meters per second. The value specified must be greater than 0 or this field is autosizable. For variable flow chillers this is the maximum generator flow rate, for constant flow chillers this is the flow rate.
+
+\paragraph{Field: Temperature Lower Limit Generator Inlet}\label{field-temperature-lower-limit-generator-inlet}
+
+This numeric field specifies the lower limit of the generator's entering water temperature. This field is not used iif the Generator Fluid Type is specified as steam.
+
+\paragraph{Field: Degree of Subcooling in Steam Generator}\label{field-degree-of-subcooling-in-steam-generator-1}
+
+Ideally the steam trap located at the outlet of generator should remove all the condensate immediately, however there is a delay in this process in actual systems which causes the condensate to SubCool by a certain degree before leaving the generator. This amount of subcooling is included in the heat transferred to the solution in the generator. The minimum value is 0º Celsius, the maximum value is 20º Celsius, and the default is 1º Celsius.
+
+\paragraph{Field: Degree of Subcooling in Steam Condensate Loop}\label{field-degree-of-subcooling-in-steam-condensate-loop}
+
+This essentially represents the heat loss to the atmosphere due to uninsulated condensate return piping to the boiler. Condensate return piping operates at atmospheric pressure and is not insulated. The condensate sub cools to certain degree before it is pumped back to the boiler. The minimum value is 0º Celsius and the default is 0º Celsius.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-1-001}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Nominal Pumping Power, Design Chilled Water Flow Rate, Design Condenser Water Flow Rate and Design Generator Fluid Flow Rate. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+Following is an example input for an Absorption Chiller.
+
+\begin{lstlisting}
+
+Chiller:Absorption:Indirect,
+      Big Chiller,             !- Chiller Name
+      100000,                  !- Nominal Capacity {W}
+      250,                     !- Nominal Pumping Power {W}
+      Big Chiller Inlet Node,  !- Evaporator Inlet Node Name
+      Big Chiller Outlet Node, !- Evaporator Outlet Node Name
+      Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
+      Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
+      0.15,                    !- Minimum Part Load Ratio
+      1.0,                     !- Maximum Part Load Ratio
+      0.65,                    !- Opt Part Load Ratio
+      35.0,                    !- Temp Design Condenser Inlet {C}
+      10.0,                    !- Temp Lower Limit Condenser Inlet {C}
+      5.0,                     !- Chilled Water Outlet Temperature Lower Limit {C}
+      0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
+      0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
+      VariableFlow,            !- Chiller Flow Mode
+      SteamUseFPLR,            !- Generator Heat Input function of part-load ratio curve name
+      PumpUseFPLR,             !- Pump Electric Input function of part-load ratio curve name
+      AbsorberSteamInletNode,  !- Generator Inlet Node Name
+      AbsorberSteamOutletNode, !- Generator Outlet Node Name
+      CAPfCOND,                !- Capacity Correction function of condenser temperature curve name
+      CAPfEVAP,                !- Capacity Correction function of evaporator temperature curve name
+      ,                        !- Capacity Correction function of generator temperature curve name
+      SteamFCondTemp,       !- Generator Heat Input Correction function of condenser temperature curve name
+      SteamFEvapTemp,       !- Generator Heat Input Correction function of evaporator temperature curve name
+      Steam,                   !- Generator Heat Source Type
+      autosize,                !- Design Generator Volumetric Fluid Flow Rate {m3/s}
+      30.0,                    !- Temp Lower Limit Generator Inlet {C}
+      2.0,                     !- Degree of Subcooling in Steam Generator {C}
+      12.0;                    !- Degree of Subcooling in Steam Condensate Loop {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-019}
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Electric Energy {[}J{]}
+\item
+  Zone,Meter,Electricity:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:Electricity {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Evaporator Cooling Energy {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Plant {[}J{]}
+\item
+  Zone,Meter,Chillers:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Meter,HeatRejection:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller COP {[}W/W{]}
+\item
+  HVAC,Average,Chiller Part-Load Ratio
+\item
+  HVAC,Average,Chiller Cycling Ratio
+\end{itemize}
+
+For Chillers with Steam Generators:
+
+\begin{itemize}
+\item
+  HVAC,Average, Chiller Source Steam Rate {[}W{]}
+\item
+  HVAC,Sum, Chiller Source Steam Energy {[}J{]}
+\item
+  Zone,Meter,Steam:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:Steam {[}J{]}
+\item
+  HVAC,Average, Chiller Steam Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average, Chiller Steam Heat Loss Rate {[}W{]}
+\end{itemize}
+
+For Chillers with Hot Water Generators:
+
+\begin{itemize}
+\item
+  HVAC,Average, Chiller Source Hot Water Rate {[}W{]}
+\item
+  HVAC,Sum, Chiller Source Hot Water Energy {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average, Chiller Hot Water Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+These chiller output variables are defined above under ``Generic Chiller Outputs.''
+
+\subsection{Chiller:ConstantCOP}\label{chillerconstantcop}
+
+This chiller model is based on a simple, constant COP simulation of the chiller. In this case, performance does not vary with chilled water temperature or condenser conditions.
+
+Such a model is useful when the user does not have access to detailed performance data.
+
+\subsubsection{Inputs}\label{inputs-2-030}
+
+\paragraph{Field: Name}\label{field-name-2-029}
+
+This alpha field contains the identifying name for the constant COP chiller.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-2-000}
+
+This numeric field contains the nominal cooling capability of the chiller in Watts.
+
+\paragraph{Field: Nominal COP}\label{field-nominal-cop-000}
+
+This numeric field contains the Chiller's coefficient of performance.
+
+\paragraph{Field: Design Chilled Water Flow Rate}\label{field-design-chilled-water-flow-rate-2}
+
+For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate. The units are in cubic meters per second.
+
+\paragraph{Field: Design Condenser Water Flow Rate}\label{field-design-condenser-water-flow-rate-2}
+
+This numeric field contains the electric chiller's design condenser water flow rate in cubic meters per second. This field is autosizable. This field is not used for Condenser Type = AirCooled or EvaporativelyCooled.
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-2}
+
+This required alpha field contains the identifying name for the constant COP chiller plant side inlet node.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-2}
+
+This required alpha field contains the identifying name for the constant COP chiller plant side outlet node.
+
+\paragraph{Field: Condenser Inlet Node Name}\label{field-condenser-inlet-node-name-2}
+
+This alpha field contains the identifying name for the constant COP chiller condenser side inlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and a condenser inlet node name is specified here, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates an outdoor air node and the air temperature information on this node is taken directly from the weather file (no node height adjustment).
+
+\paragraph{Field: Condenser Outlet Node Name}\label{field-condenser-outlet-node-name-2}
+
+This alpha field contains the identifying name for the constant COP chiller condenser side outlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates a condenser side outlet air node.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-001}
+
+This alpha field determines what type of condenser will be modeled with this chiller. The 3 type of condensers are AirCooled, WaterCooled, and EvaporativelyCooled with the default being AirCooled if not specified. AirCooled and EvaporativelyCooled do not require a CondenserLoop to be specified, whereas the WaterCooled option requires the full specification of the CondenserLoop and its associated equipment.
+
+\paragraph{Field: Chiller Flow Mode}\label{field-chiller-flow-mode-2}
+
+This choice field determines how the chiller operates with respect to the intended fluid flow through the device's evaporator.~ There are three different choices for specifying operating modes for the intended flow behavior:~ ``NotModulated,'' ``ConstantFlow,'' and ``LeavingSetpointModulated.''~ NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.~ ConstantFlow is useful for constant speed pumping arrangements where the chiller's request for flow is stricter and can increase the overall loop flow.~ LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.~ In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.~ The default, if not specified, is NotModulated.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-2-000}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Design Chilled Water Flow Rate and Design Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-002}
+
+This numeric field contains the capacity of the chiller's electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the chiller is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-002}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the chiller is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-002}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the chiller is off.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Chiller:ConstantCOP, Little Chiller,
+          25000,             ! Nominal Capacity [W]
+          2.5,               ! COP
+          0.0011,            ! Design Chilled Water Flow Rate [m3/s]
+          0.0011,            ! Design Condenser Water Flow Rate [m3/s]
+          Little Chiller Inlet Node, Little Chiller Outlet Node,
+          Little Chiller Condenser Inlet Node, Little Chiller Condenser Outlet Node,
+          WaterCooled,
+          VariableFlow;
+
+
+  Chiller:ConstantCOP,
+      Little Chiller,          !- Name
+      25000,                   !- Nominal Capacity {W}
+      2.5,                     !- Nominal COP {W/W}
+      0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
+      0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
+      Little Chiller Inlet Node,   !- Chilled Water Inlet Node Name
+      Little Chiller Outlet Node,  !- Chilled Water Outlet Node Name
+      Little Chiller Condenser Inlet Node,   !- Condenser Inlet Node Name
+      Little Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
+      EvaporativelyCooled,                   !- Condenser Type
+      VariableFlow,            !- Chiller Flow Mode
+      ,                        !- Sizing Factor
+      450;                     !- Basin Heater Capacity {W/K}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-015}
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Electric Energy {[}J{]}
+\item
+  Zone,Meter,Electricity:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:Electricity {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Evaporator Cooling Energy {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Plant {[}J{]}
+\item
+  Zone,Meter,Chillers:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Meter,HeatRejection:EnergyTransfer {[}J{]}
+\end{itemize}
+
+Air-cooled or Evap-cooled:
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\end{itemize}
+
+Evap-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+Water-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+These chiller output variables are defined above under ``Generic Chiller Outputs.''
+
+\subsection{Chiller:Electric}\label{chillerelectric}
+
+This chiller model is the empirical model from the Building Loads and System Thermodynamics (BLAST) program. Capacity, power, and full load are each defined by a set of performance curves (quadratics). Chiller performance curves are generated by fitting catalog data to third order polynomial equations. The nominal inputs and curves described below are combined as follows to calculate the chiller power:
+
+\begin{equation}
+{\rm{Power  =  FracFullLoadPower }}\cdot {\rm{ FullLoadPowerRat }}\cdot {\rm{ AvailToNominalCapacityRatio }}\cdot \frac{{{\rm{NominalCapacity}}}}{{{\rm{COP}}}}
+\end{equation}
+
+where:
+
+NominalCapacity = Nominal Capacity field
+
+COP = COP field
+
+AvailToNominalCapacityRatio = the result of the Capacity Ratio Curve
+
+FullLoadPowerRat~ = the result of the Power Ratio Curve
+
+FracFullLoadPower = the result of the Full Load Ratio Curve
+
+\subsubsection{Inputs}\label{inputs-3-026}
+
+\paragraph{Field: Name}\label{field-name-3-023}
+
+This alpha field contains the identifying name for the electric chiller.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-1-001}
+
+This alpha field determines what type of condenser will be modeled with this chiller. The 3 type of condensers are AirCooled, WaterCooled, and EvaporativelyCooled with the default being AirCooled if not specified. AirCooled and EvaporativelyCooled do not require a Condenser Loop to be specified, where the WaterCooled option requires the full specification of the Condenser Loop and its associated equipment.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-3}
+
+This numeric field contains the nominal cooling capability of the chiller in Watts.
+
+\paragraph{Field: Nominal COP}\label{field-nominal-cop-1}
+
+This numeric field contains the chiller's coefficient of performance. For a water-cooled chiller, this number does not include energy use due to condenser pumps and/or fans. For an air-cooled or evap-cooled chiller, this number includes condenser fan power.
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-3}
+
+This required alpha field contains the identifying name for the electric chiller plant side inlet node.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-3}
+
+This required alpha field contains the identifying name for the electric chiller plant side outlet node.
+
+\paragraph{Field: Condenser Inlet Node Name}\label{field-condenser-inlet-node-name-3}
+
+This alpha field contains the identifying name for the electric chiller condenser side inlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and a condenser inlet node name is specified here, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates an outdoor air node and the air temperature information on this node is taken directly from the weather file (no node height adjustment).
+
+\paragraph{Field: Condenser Outlet Node Name}\label{field-condenser-outlet-node-name-3}
+
+This alpha field contains the identifying name for the electric chiller condenser side outlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates a condenser side outlet air node.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-2}
+
+This numeric field contains the electric chiller's minimum part load ratio. The expected range is between 0 and 1. The minimum part load is not the load where the machine shuts off, but where the amount of power remains constant to produce smaller loads than this fraction.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-2}
+
+This numeric field contains the electric chiller's maximum part load ratio. This value may exceed 1, but the normal range is between 0 and 1.1.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-2}
+
+This numeric field contains the electric chiller's optimum part load ratio. This is the part load ratio at which the chiller performs at its maximum COP.
+
+\paragraph{Field: Design Condenser Inlet Temperature}\label{field-design-condenser-inlet-temperature-2}
+
+This numeric field contains the electric chiller's condenser inlet design temperature in Celsius.
+
+\paragraph{Field: Temperature Rise Coefficient}\label{field-temperature-rise-coefficient}
+
+This numeric field contains the electric chiller's temperature rise coefficient which is defined as the ratio of the required change in condenser water temperature to a given change in chilled water temperature, which maintains the capacity at the nominal value. This is calculated as the following ratio:
+
+\begin{equation}
+\frac{{TCEn{t_{required}} - TCEn{t_{rated}}}}{{TEL{v_{required}} - TEL{v_{rated}}}}
+\end{equation}
+
+where:
+
+TCEnt\(_{required}\) = Required entering condenser air or water temperature to maintain rated capacity.
+
+TCEnt\(_{rated}\) = Rated entering condenser air or water temperature at rated capacity.
+
+TELv\(_{required}\) = Required leaving evaporator water outlet temperature to maintain rated capacity.
+
+TELv\(_{rated}\) = Rated leaving evaporator water outlet temperature at rated capacity.
+
+\paragraph{Field: Design Chilled Water Outlet Temperature}\label{field-design-chilled-water-outlet-temperature}
+
+This numeric field contains the electric chiller's evaporator outlet design temperature in Celsius.
+
+\paragraph{Field: Design Chilled Water Flow Rate}\label{field-design-chilled-water-flow-rate-3}
+
+For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate. The units are in cubic meters per second.
+
+\paragraph{Field: Design Condenser Fluid Flow Rate}\label{field-design-condenser-fluid-flow-rate}
+
+This numeric field contains the electric chiller's design condenser water flow rate in cubic meters per second. This field is autosizable. This field is also used to enter the air flow rate if the Condenser Type = AirCooled or EvaporativelyCooled and Heat Recovery is specified.
+
+\paragraph{Capacity Ratio Curve}\label{capacity-ratio-curve}
+
+The Capacity Ratio Curve is a quadratic equation that determines the Ratio of Available Capacity to Nominal Capacity. The defining equation is:
+
+\begin{equation}
+AvailToNominalCapacityRatio = {C_1} + {C_2}{\Delta_{temp}} + {C_3}\Delta_{temp}^2
+\end{equation}
+
+Where the Delta Temperature is defined as:
+
+\begin{equation}
+{\Delta_{{\rm{Temp}}}} = \frac{{{\rm{TempCondIn  -  TempCondInDesign }}}}{{{\rm{TempRiseCoefficient}}}} - ({\rm{TempEvapOut  -  TempEvapOutDesign)}}
+\end{equation}
+
+TempCondIn = Temperature entering the condenser (water or air temperature depending on condenser type).
+
+TempCondInDesign = Design Condenser Inlet Temperature from User input above.
+
+TempEvapOut = Temperature leaving the evaporator.
+
+TempEvapOutDesign = Design Chilled Water Outlet Temperature from User input above.
+
+TempRiseCoefficient = User Input from above.
+
+The following three fields contain the coefficients for the quadratic equation.
+
+\paragraph{Field: Coefficient 1 of Capacity Ratio Curve}\label{field-coefficient-1-of-capacity-ratio-curve}
+
+This numeric field contains the first coefficient for the capacity ratio curve.
+
+\paragraph{Field: Coefficient 2 of Capacity Ratio Curve}\label{field-coefficient-2-of-capacity-ratio-curve}
+
+This numeric field contains the second coefficient for the capacity ratio curve.
+
+\paragraph{Field: Coefficient 3 of Capacity Ratio Curve}\label{field-coefficient-3-of-capacity-ratio-curve}
+
+This numeric field contains the third coefficient for the capacity ratio curve.
+
+\paragraph{Power Ratio Curve}\label{power-ratio-curve}
+
+The Power Ratio Curve is a quadratic equation that determines the Ratio of Full Load Power at Available Capacity to Full Load Power at Nominal Capacity. The defining equation is:
+
+\(FullLoadPowerRatio = {C_1} + {C_2}AvailToNominalCapRatio + {C_3}AvailToNominalCapRati{o^2}\) The following three fields contain the coefficients for the quadratic equation.
+
+\paragraph{Field: Coefficient1 of the power ratio curve}\label{field-coefficient1-of-the-power-ratio-curve}
+
+This numeric field contains the first coefficient for the power ratio curve.
+
+\paragraph{Field: Coefficient 2 of Power Ratio Curve}\label{field-coefficient-2-of-power-ratio-curve}
+
+This numeric field contains the second coefficient for the power ratio curve.
+
+\paragraph{Field: Coefficient 3 of Power Ratio Curve}\label{field-coefficient-3-of-power-ratio-curve}
+
+This numeric field contains the third coefficient for the power ratio curve.
+
+\paragraph{Full Load Ratio Curve}\label{full-load-ratio-curve}
+
+The Full Load Ratio Curve is a quadratic equation that determines the fraction of full load power. The defining equation is:
+
+\begin{equation}
+FracFullLoadPower = {C_1} + {C_2}PartLoadRatio + {C_3}PartLoadRati{o^2}
+\end{equation}
+
+The following three fields contain the coefficients for the quadratic equation.
+
+\paragraph{Field: Coefficient 1 of Full Load Ratio Curve}\label{field-coefficient-1-of-full-load-ratio-curve}
+
+This numeric field contains the first coefficient for the full load ratio curve.
+
+\paragraph{Field: Coefficient 2 of Full Load Ratio Curve}\label{field-coefficient-2-of-full-load-ratio-curve}
+
+This numeric field contains the second coefficient for the full load ratio curve.
+
+\paragraph{Field: Coefficient 3 of Full Load Ratio Curve}\label{field-coefficient-3-of-full-load-ratio-curve}
+
+This numeric field contains the third coefficient for the full load ratio curve.
+
+\paragraph{Field: Chilled Water Outlet Temperature Lower Limit}\label{field-chilled-water-outlet-temperature-lower-limit-2}
+
+This numeric field contains the lower limit for the evaporator outlet temperature. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn't get too cold.
+
+\paragraph{Field: Chiller Flow Mode}\label{field-chiller-flow-mode-3}
+
+This choice field determines how the chiller operates with respect to the intended fluid flow through the device's evaporator.~ There are three different choices for specifying operating modes for the intended flow behavior:~ ``NotModulated,'' ``ConstantFlow,'' and ``LeavingSetpointModulated.''~ NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.~ ConstantFlow is useful for constant speed pumping arrangements where the chiller's request for flow is stricter and can increase the overall loop flow.~ LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.~ In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.~ The default, if not specified, is NotModulated.
+
+\paragraph{Field: Design Heat Recovery Water Flow Rate}\label{field-design-heat-recovery-water-flow-rate-000}
+
+This is the design flow rate used if the heat recovery option is being simulated. If this value is greater than 0.0 then a heat recovery loop must be specified and attached to the chiller using the next 2 node fields. To determine how the heat recovery algorithm works look at the Engineering Manual at the Chiller:Electric with Heat Recovery section. The units are in cubic meters per second. This field is autosizable.~ When autosizing, the flow rate is simply the product of the design condenser flow rate and the condenser heat recovery relative capacity fraction set in the field below. Note that heat recovery is only available with Condenser Type = WaterCooled.
+
+\paragraph{Field: Heat Recovery Inlet Node Name}\label{field-heat-recovery-inlet-node-name-000}
+
+This alpha field contains the identifying name for the electric chiller heat recovery side inlet node. A heat recovery loop must be specified.
+
+\paragraph{Field: Heat Recovery Outlet Node Name}\label{field-heat-recovery-outlet-node-name-000}
+
+This alpha field contains the identifying name for the electric chiller heat recovery side outlet node. A heat recovery loop must be specified.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-3-000}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Design Chilled Water Flow Rate and Design Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-1-001}
+
+This numeric field contains the capacity of the chiller's electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the chiller is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-1-001}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the chiller is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-1-001}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the chiller is off.
+
+\paragraph{Field: Condenser Heat Recovery Relative Capacity Fraction}\label{field-condenser-heat-recovery-relative-capacity-fraction}
+
+This field is optional.~ It can be used to describe the physical size of the heat recovery portion of a split bundle condenser section.~ This fraction describes the relative capacity of the heat recovery bundle of a split condenser compared to the nominal, full load heat rejection rate of the chiller.~ This fraction will be applied to the full heat rejection when operating at nominal capacity and nominal COP to model a capacity limit for the heat rejection.~ If this field is not entered then the capacity fraction is set to 1.0.
+
+\paragraph{Field: Heat Recovery Inlet High Temperature Limit Schedule Name}\label{field-heat-recovery-inlet-high-temperature-limit-schedule-name}
+
+This field is optional.~ It can be used to control heat recovery operation of the chiller.~ The schedule named here should contain temperature values, in C, that describe an upper limit for the return fluid temperatures entering the chiller at the heat recovery inlet node.~ If the fluid temperature is too high, then the heat recovery will not operate.~ This is useful to restrict the chiller lift from becoming too high and to avoid overheating the hot water loop.~ This limit can be used with or without the alternate control using leaving setpoint that is set in the next field.
+
+\paragraph{Field: Heat Recovery Leaving Temperature Setpoint Node Name}\label{field-heat-recovery-leaving-temperature-setpoint-node-name}
+
+This field is optional.~ It can be used to refine the model and controls for heat recovery operation of the chiller.~ The node named here should have a setpoint placed on it by a setpoint manager.~ If the plant loop's demand calculation scheme is set to SingleSetpoint, then a single setpoint manager should be used.~ If the plant loop's demand calculation is set to DualSetpointDeadband then a dual setpoint manager should be used and the upper setpoint is used for control.~ When this field is used, a different model is used for determining the distribution of rejected heat between the two bundles that is more appropriate for series bundle arrangements and for chiller's that are able to produce relatively higher temperature heated fluids.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Chiller:Electric,
+      Big Chiller,             !- Chiller Name
+      WaterCooled,             !- Condenser Type
+      100000,                  !- Nominal Capacity {W}
+      2.75,                    !- COP
+      Big Chiller Inlet Node,  !- Chilled Water Inlet Node Name
+      Big Chiller Outlet Node, !- Chilled Water Outlet Node Name
+      Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
+      Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
+      .15,                     !- Minimum Part Load Ratio
+      1.0,                     !- Maximum Part Load Ratio
+      .65,                     !- Optimum Part Load Ratio
+      29.44,                   !- Design Condenser Inlet Temperature {C}
+      2.682759,                !- Temperature Rise Coefficient
+      6.667,                   !- Design Chilled Water Outlet Temperature {C}
+      0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
+      0.0005,                  !- Design Condenser Water Flow Rate {m3/s}
+      0.94483600,              !- Coefficient 1 of Capacity Ratio Curve
+      -.05700880,              !- Coefficient 2 of Capacity Ratio Curve
+      -.00185486,              !- Coefficient 3 of Capacity Ratio Curve
+      1.907846,                !- Coefficient 1 of Power Ratio Curve
+      -1.20498700,             !- Coefficient 2 of Power Ratio Curve
+      0.26346230,              !- Coefficient 3 of Power Ratio Curve
+      0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
+      0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
+      0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
+      5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
+      VariableFlow;            !- Chiller Flow Mode
+\end{lstlisting}
+
+An example of an Air-Cooled Chiller:
+
+\begin{lstlisting}
+
+Chiller:Electric,
+      Big Chiller,             !- Chiller Name
+      AirCooled,              !- Condenser Type
+      100000,                  !- Nominal Capacity {W}
+      2.58,                    !- COP
+      Big Chiller Inlet Node,  !- Chilled Water Inlet Node Name
+      Big Chiller Outlet Node, !- Chilled Water Outlet Node Name
+      Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
+      Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
+      .05,                     !- Minimum Part Load Ratio
+      1.0,                     !- Maximum Part Load Ratio
+      .65,                     !- Optimum Part Load Ratio
+      35.0,                    !- Design Condenser Inlet Temperature {C}
+      2.778,                   !- Temperature Rise Coefficient
+      6.67,                    !- Design Chilled Water Outlet Temperature {C}
+      0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
+      0.002,                   !- Design Condenser Water Flow Rate {m3/s}
+      0.9949,                  !- Coefficient 1 of Capacity Ratio Curve
+      -0.045954,               !- Coefficient 2 of Capacity Ratio Curve
+      -0.0013543,              !- Coefficient 3 of Capacity Ratio Curve
+      2.333,                   !- Coefficient 1 of Power Ratio Curve
+      -1.975,                  !- Coefficient 2 of Power Ratio Curve
+      0.6121,                  !- Coefficient 3 of Power Ratio Curve
+      0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
+      0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
+      0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
+      5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
+      VariableFlow;            !- Chiller Flow Mode
+
+  OutdoorAir:Node,
+      Big Chiller Condenser Inlet Node,  !- Node Name
+      -1.0;                    !- Height Above Ground {m}
+\end{lstlisting}
+
+An example of an Evaporatively-Cooled Chiller:
+
+\begin{lstlisting}
+
+Chiller:Electric,
+      Big Chiller,             !- Name
+      EvaporativelyCooled,               !- Condenser Type
+      100000,                  !- Nominal Capacity {W}
+      2.58,                    !- Nominal COP
+      Big Chiller Inlet Node,  !- Chilled Water Inlet Node Name
+      Big Chiller Outlet Node, !- Chilled Water Outlet Node Name
+      Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
+      Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
+      0.05,                    !- Minimum Part Load Ratio
+      1.0,                     !- Maximum Part Load Ratio
+      0.65,                    !- Optimum Part Load Ratio
+      35.0,                    !- Design Condenser Inlet Temperature {C}
+      2.778,                   !- Temperature Rise Coefficient
+      6.67,                    !- Design Chilled Water Outlet Temperature {C}
+      0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
+      0.002,                   !- Design Condenser Water Flow Rate {m3/s}
+      0.9949,                  !- Coefficient 1 of Capacity Ratio Curve
+      -0.045954,               !- Coefficient 2 of Capacity Ratio Curve
+      -0.0013543,              !- Coefficient 3 of Capacity Ratio Curve
+      2.333,                   !- Coefficient 1 of Power Ratio Curve
+      -1.975,                  !- Coefficient 2 of Power Ratio Curve
+      0.6121,                  !- Coefficient 3 of Power Ratio Curve
+      0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
+      0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
+      0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
+      5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
+      VariableFlow,            !- Chiller Flow Mode
+      ,                        !- Design Heat Recovery Water Flow Rate {m3/s}
+      ,                        !- Heat Recovery Inlet Node Name
+      ,                        !- Heat Recovery Outlet Node Name
+      ,                        !- Sizing Factor
+      450,                     !- Basin Heater Capacity {W/K}
+      3,                       !- Basin Heater Setpoint Temperature {C}
+      Basin heater sch;        !- Basin Heater Operating Schedule Name
+
+    OutdoorAir:Node,
+      Big Chiller Condenser Inlet Node,  !- Name
+      -1.0;                    !- Height Above Ground {m}
+\end{lstlisting}
+
+An example of a Heat Recovery Chiller:
+
+\begin{lstlisting}
+
+Chiller:Electric,
+      Big Chiller,             !- Chiller Name
+      WaterCooled,            !- Condenser Type
+      25000,                   !- Nominal Capacity {W}
+      2.75,                    !- COP
+      Big Chiller Inlet Node,  !- Chilled Water Inlet Node Name
+      Big Chiller Outlet Node, !- Chilled Water Outlet Node Name
+      Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
+      Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
+      .15,                     !- Minimum Part Load Ratio
+      1.0,                     !- Maximum Part Load Ratio
+      .65,                     !- Optimum Part Load Ratio
+      29.44,                   !- Design Condenser Inlet Temperature {C}
+      2.682759,                !- Temperature Rise Coefficient
+      6.667,                   !- Design Chilled Water Outlet Temperature {C}
+      0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
+      0.0005,                  !- Design Condenser Water Flow Rate {m3/s}
+      0.94483600,              !- Coefficient 1 of Capacity Ratio Curve
+      -.05700880,              !- Coefficient 2 of Capacity Ratio Curve
+      -.00185486,              !- Coefficient 3 of Capacity Ratio Curve
+      1.907846,                !- Coefficient 1 of Power Ratio Curve
+      -1.20498700,             !- Coefficient 2 of Power Ratio Curve
+      0.26346230,              !- Coefficient 3 of Power Ratio Curve
+      0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
+      0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
+      0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
+      5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
+      VariableFlow,            !- Chiller Flow Mode
+      0.00055,                 !- Design heat recovery water flow rate {m3/s}
+      Big Chiller Heat Rec Inlet Node,  !- Heat Recovery Inlet Node Name
+      Big Chiller Heat Rec Outlet Node;  !- Heat Recovery Outlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-013}
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Electric Energy {[}J{]}
+\item
+  Zone,Meter,Electricity:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:Electricity {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Evaporator Cooling Energy {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Plant {[}J{]}
+\item
+  Zone,Meter,Chillers:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller COP {[}W/W{]}
+\item
+  HVAC,Average,Chiller Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Meter,HeatRejection:EnergyTransfer {[}J{]}
+\end{itemize}
+
+Air-cooled or Evap-cooled:
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\end{itemize}
+
+Evap-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+Water-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+HeatRecovery:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Total Recovered Heat Rate {[}W{]}
+\item
+  HVAC,Sum, Chiller Total Recovered Heat Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Effective Heat Rejection Temperature {[}C{]}
+\end{itemize}
+
+These chiller output variables are defined above under ``Generic Chiller Outputs.''
+
+\subsection{Chiller:Electric:EIR}\label{chillerelectriceir}
+
+This chiller model is the empirical model used in the DOE-2.1 building energy simulation program. The model uses performance information at reference conditions along with three curve fits for cooling capacity and efficiency to determine chiller operation at off-reference conditions. Chiller performance curves can be generated by fitting manufacturer's catalog data or measured data. Performance curves for more than 160 chillers, including the default DOE-2.1E reciprocating and centrifugal chillers, are provided in the EnergyPlus Reference DataSets (Chillers.idf and AllDataSets.idf).
+
+Note: Chiller:Electric:EIR objects and their associated performance curve objects are developed using performance information for a specific chiller and should normally be used together for an EnergyPlus simulation. Changing the object input values, or swapping performance curves between chillers, should be done with caution.
+
+\subsubsection{Inputs}\label{inputs-4-023}
+
+\paragraph{Field: Name}\label{field-name-4-020}
+
+This alpha field contains the identifying name for the electric EIR chiller.
+
+\paragraph{Field: Reference Capacity}\label{field-reference-capacity}
+
+This numeric field contains the reference cooling capacity of the chiller in Watts. This should be the capacity of the chiller at the reference temperatures and water flow rates defined below. Alternately, this field can be autosized.
+
+\paragraph{Field: Reference COP}\label{field-reference-cop}
+
+This numeric field contains the chiller's coefficient of performance. This value should \textbf{not} include energy use due to pumps or cooling tower fans. This COP should be at the reference temperatures and water flow rates defined below. This value \textbf{should} include evap-cooled or air-cooled condenser fans except when the Condenser Fan Power Ratio input field defined below is used and that input value is greater than 0. For the case when condenser fan power is modeled separately, the calculated condenser fan energy is reported on the same electric meter as compressor power. Be careful to not duplicate this energy use.
+
+\paragraph{Field: Reference Leaving Chilled Water Temperature}\label{field-reference-leaving-chilled-water-temperature}
+
+This numeric field contains the chiller's reference leaving chilled water temperature in Celsius. The default value is 6.67°C.
+
+\paragraph{Field: Reference Entering Condenser Fluid Temperature}\label{field-reference-entering-condenser-fluid-temperature}
+
+This numeric field contains the chiller's reference entering condenser fluid temperature in Celsius. The default value is 29.4°C. For water-cooled chillers this is the water temperature entering the condenser (e.g., leaving the cooling tower). For air- or evap-cooled condensers this is the entering outdoor air dry-bulb or wet-bulb temperature, respectively.
+
+\paragraph{Field: Reference Chilled Water Flow Rate}\label{field-reference-chilled-water-flow-rate}
+
+For a variable flow chiller this is the maximum water flow rate and for a constant flow chiller this is the operating water flow rate through the chiller's evaporator. The units are in cubic meters per second. The minimum value for this numeric input field must be greater than zero, or this field can be autosized.
+
+\paragraph{Field: Reference Condenser Fluid Flow Rate}\label{field-reference-condenser-fluid-flow-rate}
+
+This numeric field contains the chiller's operating condenser water flow rate in cubic meters per second. This field can be autosized. This field is also used to enter the air flow rate if Condenser Type = AirCooled or EvaporativelyCooled and Heat Recovery is specified..
+
+\paragraph{Field: Cooling Capacity Function of Temperature Curve Name}\label{field-cooling-capacity-function-of-temperature-curve-name}
+
+The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the cooling capacity as a function of the leaving chilled water temperature and the entering condenser fluid temperature. The output of this curve is multiplied by the reference capacity to give the cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\paragraph{Field: Electric Input to Cooling Output Ratio Function of Temperature Curve Name}\label{field-electric-input-to-cooling-output-ratio-function-of-temperature-curve-name}
+
+The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and the entering condenser fluid temperature. The EIR is the inverse of the COP. The output of this curve is multiplied by the reference EIR (inverse of the reference COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\paragraph{Field: Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name}\label{field-electric-input-to-cooling-output-ratio-function-of-part-load-ratio-curve-name}
+
+The name of a quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the part-load ratio (EIRfTPLR). The EIR is the inverse of the COP, and the part-load ratio is the actual cooling load divided by the chiller's available cooling capacity. This curve is generated by dividing the operating electric input power by the available full-load capacity (do not divide by load) at the specific operating temperatures. The curve output should decrease from 1 towards 0 as part-load ratio decreases from 1 to 0. The output of this curve is multiplied by the reference full-load EIR (inverse of the reference COP) and the Energy Input to Cooling Output Ratio Function of Temperature Curve to give the EIR at the specific temperatures and part-load ratio at which the chiller is operating. This curve should have a value of 1.0 when the part-load ratio equals 1.0. An ideal chiller with the same efficiency at all part-load ratio's would use a performance curve that has a value of 0 when the part-load ratio equals 0 (i.;e., a line connecting 0,0 and 1,1 when plotted as EIRfTPLR versus PLR), however, actual systems can have part-load EIR's slightly above or below this line (i.e., part-load efficiency often differs from rated efficiency). The quadratic curve should be valid for the range of part-load ratios anticipated for the simulation.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-3}
+
+This numeric field contains the chiller's minimum part-load ratio. The expected range is between 0 and 1. Below this part-load ratio, the compressor cycles on and off to meet the cooling load. The Minimum Part Load Ratio must be less than or equal to the Maximum Part Load Ratio. The default value is 0.1.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-3}
+
+This numeric field contains the chiller's maximum part-load ratio. This value may exceed 1, but the normal range is between 0 and 1.0. The Maximum Part Load Ratio must be greater than or equal to the Minimum Part Load Ratio. The default value is 1.0.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-3}
+
+This numeric field contains the chiller's optimum part-load ratio. This is the part-load ratio at which the chiller performs at its maximum COP. The optimum part-load ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 1.0.
+
+\paragraph{Field: Minimum Unloading Ratio}\label{field-minimum-unloading-ratio-000}
+
+This numeric field contains the chiller's minimum unloading ratio. The expected range is between 0 and 1. The minimum unloading ratio is where the chiller capacity can no longer be reduced by unloading and must be false loaded to meet smaller cooling loads. A typical false loading strategy is hot-gas bypass. The minimum unloading ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 0.2.
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-4}
+
+This required alpha field contains the identifying name for the chiller plant side (chilled water) inlet node.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-4}
+
+This required alpha field contains the identifying name for the chiller plant side (chilled water) outlet node.
+
+\paragraph{Field: Condenser Inlet Node Name}\label{field-condenser-inlet-node-name-4}
+
+This alpha field contains the identifying name for the chiller condenser side inlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and a condenser inlet node name is specified here, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates an outdoor air node and the air temperature information on this node is taken directly from the weather file (no node height adjustment).
+
+\paragraph{Field: Condenser Outlet Node Name}\label{field-condenser-outlet-node-name-4}
+
+This alpha field contains the identifying name for the chiller condenser side outlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates a condenser side outlet air node.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-2-000}
+
+This alpha field determines what type of condenser will be modeled with this chiller. Valid condenser types are AirCooled, WaterCooled, and EvaporativelyCooled with the default being WaterCooled if not specified. AirCooled and EvaporativelyCooled do not require a Condenser Loop to be specified, whereas the WaterCooled option requires the full specification of the Condenser Loop and its associated equipment.
+
+\paragraph{Field: Condenser Fan Power Ratio}\label{field-condenser-fan-power-ratio}
+
+This field is used to model condenser fan power associated with air-cooled or evaporatively-cooled condensers (for cooling towers, refer to Group - Condenser Equipment). Enter the ratio of the condenser fan power to the reference chiller cooling capacity in W/W. If this input is greater than 0, the condenser fan power is modeled seperatly from compressor power. In addition, if condenser fan power is modeled using this input, the reference COP and ``Electric Input to Cooling Output Ratio Function of'' performance curves should not include condenser fan power.
+
+\paragraph{Field: Fraction of Compressor Electric Power Rejected by Condenser}\label{field-fraction-of-compressor-electric-power-rejected-by-condenser}
+
+This numeric input represents the fraction of compressor electrical energy consumption that must be rejected by the condenser. Enter a value of 1.0 when modeling hermetic chillers. For open chillers, enter the compressor motor efficiency. This value must be greater than 0.0 and less than or equal to 1.0, with a default value of 1.0.
+
+\paragraph{Field: Leaving Chilled Water Lower Temperature Limit}\label{field-leaving-chilled-water-lower-temperature-limit-000}
+
+This numeric field contains the lower limit for the leaving chilled water temperature in Celsius. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn't get too cold. This input field is currently unused. The default value is 2°C.
+
+\paragraph{Field: Chiller Flow Mode}\label{field-chiller-flow-mode-4}
+
+This choice field determines how the chiller operates with respect to the intended fluid flow through the device's evaporator.~ There are three different choices for specifying operating modes for the intended flow behavior:~ ``NotModulated,'' ``ConstantFlow,'' and ``LeavingSetpointModulated.''~ NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.~ ConstantFlow is useful for constant speed pumping arrangements where the chiller's request for flow is stricter and can increase the overall loop flow.~ LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.~ In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.~ The default, if not specified, is NotModulated.
+
+\paragraph{Field: Design Heat Recovery Water Flow Rate}\label{field-design-heat-recovery-water-flow-rate-1-000}
+
+This is the design heat recovery water flow rate if the heat recovery option is being simulated. If this value is greater than 0.0 (or Autosize), a heat recovery loop must be specified and attached to the chiller using the next two node fields. The units are in cubic meters per second.~ This field is autosizable.~ When autosizing, the flow rate is simply the product of the design condenser flow rate and the condenser heat recovery relative capacity fraction set in the field below. Note that heat recovery is only available with Condenser Type = WaterCooled.
+
+\paragraph{Field: Heat Recovery Inlet Node Name}\label{field-heat-recovery-inlet-node-name-1-000}
+
+This alpha field contains the identifying name for the chiller heat recovery side inlet node. If the user wants to model chiller heat recovery, a heat recovery loop must be specified.
+
+\paragraph{Field: Heat Recovery Outlet Node Name}\label{field-heat-recovery-outlet-node-name-1-000}
+
+This alpha field contains the identifying name for the chiller heat recovery side outlet node. If the user wants to model chiller heat recovery, a heat recovery loop must be specified.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-4-000}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Reference Capacity, Reference Chilled Water Flow Rate and Reference Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-2-001}
+
+This numeric field contains the capacity of the chiller's electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the chiller is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-2-001}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the chiller is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-2-001}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the chiller is off.
+
+\paragraph{Field: Condenser Heat Recovery Relative Capacity Fraction}\label{field-condenser-heat-recovery-relative-capacity-fraction-1}
+
+This field is optional.~ It can be used to describe the physical size of the heat recovery portion of a split bundle condenser section.~ This fraction describes the relative capacity of the heat recovery bundle of a split condenser compared to the nominal, full load heat rejection rate of the chiller.~ This fraction will be applied to the full heat rejection when operating at nominal capacity and nominal COP to model a capacity limit for the heat rejection.~ If this field is not entered then the capacity fraction is set to 1.0.
+
+\paragraph{Field: Heat Recovery Inlet High Temperature Limit Schedule Name}\label{field-heat-recovery-inlet-high-temperature-limit-schedule-name-1}
+
+This field is optional.~ It can be used to control heat recovery operation of the chiller.~ The schedule named here should contain temperature values, in C, that describe an upper limit for the return fluid temperatures entering the chiller at the heat recovery inlet node.~ If the fluid temperature is too high, then the heat recovery will not operate.~ This is useful to restrict the chiller lift from becoming too high and to avoid overheating the hot water loop.~ This limit can be used with or without the alternate control using leaving setpoint that is set in the next field.
+
+\paragraph{Field: Heat Recovery Leaving Temperature Setpoint Node Name}\label{field-heat-recovery-leaving-temperature-setpoint-node-name-1}
+
+This field is optional.~ It can be used to refine the model and controls for heat recovery operation of the chiller.~ The node named here should have a setpoint placed on it by a setpoint manager.~ If the plant loop's demand calculation scheme is set to SingleSetpoint, then a single setpoint manager should be used.~ If the plant loop's demand calculation is set to DualSetpointDeadband then a dual setpoint manager should be used and the upper setpoint is used for control.~ When this field is used, a different model is used for determining the distribution of rejected heat between the two bundles that is more appropriate for series bundle arrangements and for chiller's that are able to produce relatively higher temperature heated fluilds.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+! ElectricEIRChiller DOE-2 Centrifugal/5.50COP
+  ! A generic centrifugal chiller from DOE-2.1E
+  !
+  Chiller:Electric:EIR,
+   DOE-2 Centrifugal/5.50COP,  !- Chiller Name
+   Autosize,                   !- Reference Capacity {W}
+   5.5,                        !- Reference COP {W/W}
+   6.67,                       !- Reference Leaving Chilled Water Temperature {C}
+   29.4,                       !- Reference Entering Condenser Fluid Temperature {C}
+   Autosize,                   !- Reference Chilled Water Flow Rate {m3/s}
+   Autosize,                   !- Reference Condenser Water Flow Rate {m3/s}
+   DOE-2 Centrifugal/5.50COP CAPFT,  !- Cooling Capacity Function of Temperature Curve
+   DOE-2 Centrifugal/5.50COP EIRFT,  !- Electric Input to Cooling Output Ratio Function of
+                                        Temperature Curve
+   DOE-2 Centrifugal/5.50COP EIRFPLR,!- Electric Input to Cooling Output Ratio Function of Part Load
+                                        Ratio Curve
+   0.1,                        !- Minimum Part Load Ratio
+   1.0,                        !- Maximum Part Load Ratio
+   1.0,                        !- Optimum Part Load Ratio
+   0.2,                        !- Minimum Unloading Ratio
+   Chilled Water Side Inlet Node,        !- Chilled Water Side Inlet Node
+   Chilled Water Side Outlet Node,       !- Chilled Water Side Outlet Node
+   Condenser Side Inlet Node,  !- Condenser Side Inlet Node
+   Condenser Side Outlet Node, !- Condenser Side Outlet Node
+   WaterCooled,               !- Condenser Type
+   ,                           !- Condenser Fan Power Ratio {W/W}
+   1.0,                        !- Fraction of Compressor Electric Power Rejected by Condenser
+   2.0,                        !- Leaving Chilled Water Lower Temperature Limit {C}
+   ConstantFlow;               !- Chiller Evaporator Flow Mode
+
+
+  !
+  ! Curve set (3 Curves):
+  !
+  ! Cooling Capacity Function of Temperature Curve for open or hermetic water-cooled centrifugal
+    chillers
+  ! x = Leaving Chilled Water Temperature and y = Entering Condenser Water Temperature
+  ! Same as DOE-2.1E HERM-CENT-CAP-FT (CCAPT3) and OPEN-CENT-CAP-FT (CCAPT1)
+   Curve:Biquadratic,
+   DOE-2 Centrifugal/5.50COP CAPFT,  !- Name
+   0.257896E+00,               !- Coefficient1 Constant
+   0.389016E-01,               !- Coefficient2 x
+   -0.217080E-03,              !- Coefficient3 x**2
+   0.468684E-01,               !- Coefficient4 y
+   -0.942840E-03,              !- Coefficient5 y**2
+   -0.343440E-03,              !- Coefficient6 x*y
+   5.0,                        !- Minimum Value of x
+   10.0,                       !- Maximum Value of x
+   24.0,                       !- Minimum Value of y
+   35.0;                       !- Maximum Value of y
+  !
+  ! Energy Input to Cooling Output Ratio Function of Temperature Curve for open or hermetic water-
+    cooled centrifugal chillers
+  ! x = Leaving Chilled Water Temperature and y = Entering Condenser Water Temperature
+  ! Same as DOE-2.1E HERM-CENT-EIR-FT (EIRT3) and OPEN-CENT-EIR-FT (EIRT1)
+   Curve:Biquadratic,
+   DOE-2 Centrifugal/5.50COP EIRFT,  !- Name
+   0.933884E+00,               !- Coefficient1 Constant
+   -0.582120E-01,              !- Coefficient2 x
+   0.450036E-02,               !- Coefficient3 x**2
+   0.243000E-02,               !- Coefficient4 y
+   0.486000E-03,               !- Coefficient5 y**2
+   -0.121500E-02,              !- Coefficient6x*y
+   5.0,                        !- Minimum Value of x
+   10.0,                       !- Maximum Value of x
+   24.0,                       !- Minimum Value of y
+   35.0;                       !- Maximum Value of y
+  !
+  ! Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve for open or hermetic
+    water-cooled centrifugal chillers
+  ! x = Part Load Ratio (load/capacity)
+  ! Same as DOE-2.1E HERM-CENT-EIR-FPLR (EIRPLR3) and OPEN-CENT-EIR-FPLR (EIRPLR1)
+   Curve:Quadratic,
+   DOE-2 Centrifugal/5.50COP EIRFPLR, !- Name
+   0.222903,                   !- Coefficient1 Constant
+   0.313387,                   !- Coefficient2 x
+   0.463710,                   !- Coefficient3 x**2
+   0.0,                        !- Minimum Value of x
+   1.0;                        !- Maximum Value of x
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-010}
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Electric Energy {[}J{]}
+\item
+  Zone,Meter,Electricity:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:Electricity {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Evaporator Cooling Energy {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Plant {[}J{]}
+\item
+  Zone,Meter,Chillers:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller COP {[}W/W{]}
+\item
+  HVAC,Average,Chiller Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Meter,HeatRejection:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Part Load Ratio {[]}
+\item
+  HVAC,Average,Chiller Cycling Ratio {[]}
+\item
+  HVAC,Average,Chiller False Load Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller False Load Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+Curve object outputs:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Capacity Temperature Modifier Multiplier {[]}
+\item
+  HVAC,Average,Chiller EIR Temperature Modifier Multiplier {[]}
+\item
+  HVAC,Average,Chiller EIR Part Load Modifier Multiplier {[]}
+\end{itemize}
+
+Air-cooled or Evap-cooled:
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\end{itemize}
+
+Air-cooled or Evap-cooled reported only when the condenser fan power ratio input field is greater than 0:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Condenser Fan Electric Power {[}W{]}
+\item
+  HVAC,Average,Chiller Condenser Fan Electric Consumption {[}J{]}
+\end{itemize}
+
+Evap-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+Water-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+HeatRecovery:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Total Recovered Heat Rate {[}W{]}
+\item
+  Zone,Meter,HeatRecovery:EnergyTransfer {[}J{]}
+\item
+  HVAC,Sum,Chiller Heat Recovery {[}J{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Effective Heat Rejection Temperature {[}C{]}
+\end{itemize}
+
+Most of these chiller output variables are defined above under ``Generic Chiller Outputs.''~ Output variables not described above are discussed here.
+
+\paragraph{Chiller Condenser Fan Electric Power ~{[}W{]}}\label{chiller-condenser-fan-electric-power-w}
+
+\paragraph{Chiller Condenser Fan Electric Energy ~{[}J{]}}\label{chiller-condenser-fan-electric-energy-j}
+
+These outputs are for the electric power consumption of the chiller condenser fan and are applicable to air- or evaporatively-cooled chillers. These reports are available only for the Chiller:Electric:EIR and only when the Condenser Fan Power Ratio input field is greater than 0. This output is also added to a meter object with Resource Type = Electricity, End Use Key = Chillers, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Chiller Capacity Temperature Modifier Multiplier {[]}}{Chiller Capacity Temperature Modifier Multiplier }}\label{chiller-capacity-temperature-modifier-multiplier}
+
+This is the output of the curve object Cooling Capacity Function of Temperature Curve.
+
+\paragraph{\texorpdfstring{Chiller EIR Temperature Modifier Multiplier {[]}}{Chiller EIR Temperature Modifier Multiplier }}\label{chiller-eir-temperature-modifier-multiplier}
+
+This is the output of the curve object Electric Input to Cooling Output Ratio Function of Temperature Curve.
+
+\paragraph{\texorpdfstring{Chiller EIR Part Load Modifier Multiplier {[]}}{Chiller EIR Part Load Modifier Multiplier }}\label{chiller-eir-part-load-modifier-multiplier}
+
+This is the output of the curve object Electric Input to Cooling Output Ratio Function of Part Load Curve.
+
+\paragraph{\texorpdfstring{Chiller Part Load Ratio {[]}}{Chiller Part Load Ratio }}\label{chiller-part-load-ratio-1}
+
+This output is the ratio of the evaporator heat transfer rate plus the false load heat transfer rate (if applicable) to the available chiller capacity. This value is used to determine Chiller EIR Part Load Modifier Multiplier.
+
+\paragraph{\texorpdfstring{Chiller Cycling Ratio {[]}}{Chiller Cycling Ratio }}\label{chiller-cycling-ratio-1}
+
+The cycling ratio is the amount of time the chiller operates during each simulation timestep. If the chiller part-load ratio falls below the minimum part-load ratio, the chiller cycles on and off to meet the cooling load.
+
+\paragraph{Chiller False Load Heat Transfer Rate {[}W{]}}\label{chiller-false-load-heat-transfer-rate-w}
+
+\paragraph{Chiller False Load Heat Transfer Energy {[}J{]}}\label{chiller-false-load-heat-transfer-energy-j}
+
+These outputs are the heat transfer rate and total heat transfer due to false loading of the chiller. When the chiller part-load ratio is below the minimum unloading ratio, the chiller false loads (e.g.~hot-gas bypass) to further reduce capacity. The false load heat transfer output variable is not metered.
+
+\subsection{Chiller:Electric:ReformulatedEIR}\label{chillerelectricreformulatedeir}
+
+This chiller model, developed through the CoolToolsâ„¢ project sponsored by Pacific Gas and Electric Company (PG\&E), is an empirical model similar to EnergyPlus' Chiller:Electric:EIR model. The model uses performance information at reference conditions along with three curve fits for cooling capacity and efficiency to determine chiller operation at off-reference conditions. The model has the same capabilities as the Chiller:Electric:EIR model, but can potentially provide significant accuracy improvement over the Chiller:Electric:EIR model for variable-speed compressor drive and variable condenser water flow applications. Chiller performance curves can be generated by fitting manufacturer's catalog data or measured data. Performance curves developed from manufacturer's performance data are provided in the EnergyPlus Reference DataSets (Chillers.idf and AllDataSets.idf). This chiller model can be used to predict the performance of various chiller types (e.g., reciprocating, screw, scroll, and centrifugal) with water-cooled condensers.
+
+The main difference between this model and the Chiller:Electric:EIR model is the condenser fluid temperature used in the associated performance curves: the Chiller:Electric:ReformulatedEIR model uses the LEAVING condenser water temperature while the Chiller:Electric:EIR model uses the ENTERING condenser water temperature.
+
+Note: Chiller:Electric:Reformulated EIR objects and their associated performance curve objects are developed using performance information for a specific chiller and should almost always be used together for an EnergyPlus simulation. Changing the object input values, or swapping performance curves between chillers, should be done with extreme caution. For example, if the user wishes to model a chiller size that is different from the reference capacity, it is highly recommended that the reference flow rates be scaled proportionately to the change in reference capacity. Although this model can provide more accurate prediction than the Chiller:Electric:EIR model, it requires more performance data to develop the associated performance curves (at least 12 points from full-load performance and 7 points from part-load performance).
+
+\subsubsection{Inputs}\label{inputs-5-021}
+
+\paragraph{Field: Chiller Name}\label{field-chiller-name-000}
+
+This alpha field contains the identifying name for this chiller.
+
+\paragraph{Field: Reference Capacity}\label{field-reference-capacity-1}
+
+This numeric field contains the reference cooling capacity of the chiller in Watts. This should be the capacity of the chiller at the reference temperatures and water flow rates defined below. Alternately, this field can be autosized.
+
+\paragraph{Field: Reference COP}\label{field-reference-cop-1}
+
+This numeric field contains the chiller's coefficient of performance. This value should \textbf{not} include energy use due to pumps or cooling tower fans. This COP should be at the reference temperatures and water flow rates defined below.
+
+\paragraph{Field: Reference Leaving Chilled Water Temperature}\label{field-reference-leaving-chilled-water-temperature-1}
+
+This numeric field contains the chiller's reference leaving chilled water temperature in Celsius. The default value is 6.67°C.
+
+\paragraph{Field: Reference Leaving Condenser Water Temperature}\label{field-reference-leaving-condenser-water-temperature}
+
+This numeric field contains the chiller's reference leaving condenser water temperature in Celsius. The default value is 35°C.
+
+\paragraph{Field: Reference Chilled Water Flow Rate}\label{field-reference-chilled-water-flow-rate-1}
+
+For a variable flow chiller this is the maximum water flow rate and for a constant flow chiller this is the operating water flow rate through the chiller's evaporator. The units are in cubic meters per second. The minimum value for this numeric input field must be greater than zero, or this field can be autosized.
+
+\paragraph{Field: Reference Condenser Water Flow Rate}\label{field-reference-condenser-water-flow-rate}
+
+This numeric field contains the chiller's operating condenser water flow rate in cubic meters per second. The units are in cubic meters per second. The minimum value for this numeric input field must be greater than zero, or this field can be autosized.
+
+\paragraph{Field: Cooling Capacity Function of Temperature Curve Name}\label{field-cooling-capacity-function-of-temperature-curve-name-1}
+
+The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the cooling capacity as a function of the leaving chilled water temperature and the leaving condenser water temperature. The output of this curve is multiplied by the reference capacity to give the cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation (otherwise the program issues warning messages).
+
+\paragraph{Field: Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Type}\label{field-electric-input-to-cooling-output-ratio-function-of-part-load-ratio-curve-type}
+
+This choice field determines which type of the Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve is used in the chiller modeling. Two curve types are available: (1) Type LeavingCondenserWaterTemperature is based on the leaving condenser water temperature. (2) Type Lift is based on the normalized lift, which is the temperature difference between the leaving condenser water temperature and the leaving evaporator water temperature.
+
+\paragraph{Field: Electric Input to Cooling Output Ratio Function of Temperature Curve Name}\label{field-electric-input-to-cooling-output-ratio-function-of-temperature-curve-name-1}
+
+The name of the Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve. The form of this curve is based on the input for Electric Input to Cooling Output RatioFunction of Part Load Ratio Curve Type. For the type of LeavingCondenserWaterTemperature, the curve object type should be Curve:Bicubic or Table:TwoIndependentVariables that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and the leaving condenser water temperature. For the type of Lift, the curve object type should be Curve:ChillerPartLoadWithLiftCurves or Table:MultiVariableLookup that parameterizes the variation of EIR as a function of the normalized fractional Lift, normalized Tdev and the PLR. Tdev is the difference between Leaving Chilled Water Temperature and Reference Chilled Water Temperature. Lift is the Leaving Condenser Water Temperature and Leaving Chilled Water Temperature. The EIR is the inverse of the COP. The output of this curve is multiplied by the reference EIR (inverse of the reference COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation (otherwise the program issues warning messages).
+
+\paragraph{Field: Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name}\label{field-electric-input-to-cooling-output-ratio-function-of-part-load-ratio-curve-name-1}
+
+The name of a bicubic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the leaving condenser water temperature and the part-load ratio (EIRfTPLR). The EIR is the inverse of the COP, and the part-load ratio is the actual cooling load divided by the chiller's available cooling capacity. This curve is generated by dividing the operating electric input power by the available full-load capacity (do not divide by load) at the specific operating temperatures. The curve output should decrease from 1 towards 0 as part-load ratio decreases from 1 to 0. The output of this curve is multiplied by the reference full-load EIR (inverse of the reference COP) and the Energy Input to Cooling Output Ratio Function of Temperature Curve to give the EIR at the specific temperatures and part-load ratio at which the chiller is operating. This curve should have a value of 1.0 at the reference leaving condenser water temperature with the part-load ratio equal to 1.0. An ideal chiller with the same efficiency at all part-load ratio's would use a performance curve that has a value of 0 when the part-load ratio equals 0 (i.;e., a line connecting 0,0 and 1,1 when plotted as EIRfTPLR versus PLR), however, actual systems can have part-load EIR's slightly above or below this line (i.e., part-load efficiency often differs from rated efficiency). The bicubic curve should be valid for the range of condenser water temperatures and part-load ratios anticipated for the simulation (otherwise the program issues warning messages).
+
+Note: Although a bicubic curve requires 10 coefficients (ref. Curve:Bicubic), coefficients 7, 9 and 10 are typically not used in the performance curve described here and should be entered as 0 unless sufficient performance data and regression accuracy exist to justify the use of these coefficients. Additionally, coefficients 2, 3, and 6 should not be used unless sufficient temperature data is available to accurately define the performance curve (i.e., negative values may result from insufficient data).
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-4}
+
+This numeric field contains the chiller's minimum part-load ratio. The expected range is between 0 and 1. Below this part-load ratio, the compressor cycles on and off to meet the cooling load. The Minimum Part Load Ratio must be less than or equal to the Maximum Part Load Ratio. The default value is 0.1.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-4}
+
+This numeric field contains the chiller's maximum part-load ratio. This value may exceed 1, but the normal range is between 0 and 1.0. The Maximum Part Load Ratio must be greater than or equal to the Minimum Part Load Ratio. The default value is 1.0.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-4}
+
+This numeric field contains the chiller's optimum part-load ratio. This is the part-load ratio at which the chiller performs at its maximum COP. The optimum part-load ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 1.0.
+
+\paragraph{Field: Minimum Unloading Ratio}\label{field-minimum-unloading-ratio-1}
+
+This numeric field contains the chiller's minimum unloading ratio. The expected range is between 0 and 1. The minimum unloading ratio is where the chiller capacity can no longer be reduced by unloading and must be false loaded to meet smaller cooling loads. A typical false loading strategy is hot-gas bypass. The minimum unloading ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 0.2.
+
+\paragraph{Field: Chilled Water Side Inlet Node}\label{field-chilled-water-side-inlet-node}
+
+This required alpha field contains the identifying name for the chiller plant side (chilled water) inlet node.
+
+\paragraph{Field: Chilled Water Side Outlet Node}\label{field-chilled-water-side-outlet-node}
+
+This required alpha field contains the identifying name for the chiller plant side (chilled water) outlet node.
+
+\paragraph{Field: Condenser Side Inlet Node}\label{field-condenser-side-inlet-node}
+
+This required alpha field contains the identifying name for the chiller condenser side inlet node.
+
+\paragraph{Field: Condenser Side Outlet Node}\label{field-condenser-side-outlet-node}
+
+This required alpha field contains the identifying name for the chiller condenser side outlet node.
+
+\paragraph{Field: Fraction of Compressor Electric Power Rejected by Condenser}\label{field-fraction-of-compressor-electric-power-rejected-by-condenser-1}
+
+This numeric input represents the fraction of compressor electrical energy consumption that must be rejected by the condenser. Enter a value of 1.0 when modeling hermetic chillers. For open chillers, enter the compressor motor efficiency. This value must be greater than 0.0 and less than or equal to 1.0, with a default value of 1.0.
+
+\paragraph{Field: Leaving Chilled Water Lower Temperature Limit}\label{field-leaving-chilled-water-lower-temperature-limit-1}
+
+This numeric field contains the lower limit for the leaving chilled water temperature in Celsius. This temperature acts as a cut off for heat transfer in the evaporator, so that the water doesn't get too cold. This input field is currently unused. The default value is 2°C.
+
+\paragraph{Field: Chiller Flow Mode Type}\label{field-chiller-flow-mode-type}
+
+This choice field determines how the chiller operates with respect to the intended fluid flow through the device's evaporator.~ There are three different choices for specifying operating modes for the intended flow behavior:~ ``NotModulated,'' ``ConstantFlow,'' and ``LeavingSetpointModulated.''~ NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.~ ConstantFlow is useful for constant speed pumping arrangements where the chiller's request for flow is stricter and can increase the overall loop flow.~ LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.~ In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.~ The default, if not specified, is NotModulated.
+
+\paragraph{Field: Design Heat Recovery Water Flow Rate}\label{field-design-heat-recovery-water-flow-rate-2}
+
+This is the design heat recovery water flow rate if the heat recovery option is being simulated. If this value is greater than 0.0 (or autosize), a heat recovery loop must be specified and attached to the chiller using the next two node fields. The units are in cubic meters per second.~ This field is autosizable.~ When autosizing, the flow rate is simply the product of the design condenser flow rate and the condenser heat recovery relative capacity fraction set in the field below.
+
+\paragraph{Field: Heat Recovery Inlet Node Name}\label{field-heat-recovery-inlet-node-name-2}
+
+This alpha field contains the identifying name for the chiller heat recovery side inlet node. If the user wants to model chiller heat recovery, a heat recovery loop must be specified and it can only be used with a water-cooled condenser.
+
+\paragraph{Field: Heat Recovery Outlet Node Name}\label{field-heat-recovery-outlet-node-name-2}
+
+This alpha field contains the identifying name for the chiller heat recovery side outlet node. If the user wants to model chiller heat recovery, a heat recovery loop must be specified and it can only be used with a water-cooled condenser.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-5}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Reference Capacity, Reference Chilled Water Flow Rate and Reference Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+\paragraph{Field: Condenser Heat Recovery Relative Capacity Fraction}\label{field-condenser-heat-recovery-relative-capacity-fraction-2}
+
+This field is optional.~ It can be used to describe the physical size of the heat recovery portion of a split bundle condenser section.~ This fraction describes the relative capacity of the heat recovery bundle of a split condenser compared to the nominal, full load heat rejection rate of the chiller.~ This fraction will be applied to the full heat rejection when operating at nominal capacity and nominal COP to model a capacity limit for the heat rejection.~ If this field is not entered then the capacity fraction is set to 1.0.
+
+\paragraph{Field: Heat Recovery Inlet High Temperature Limit Schedule Name}\label{field-heat-recovery-inlet-high-temperature-limit-schedule-name-2}
+
+This field is optional.~ It can be used to control heat recovery operation of the chiller.~ The schedule named here should contain temperature values, in C, that describe an upper limit for the return fluid temperatures entering the chiller at the heat recovery inlet node.~ If the fluid temperature is too high, then the heat recovery will not operate.~ This is useful to restrict the chiller lift from becoming too high and to avoid overheating the hot water loop.~ This limit can be used with or without the alternate control using leaving setpoint that is set in the next field.
+
+\paragraph{Field: Heat Recovery Leaving Temperature Setpoint Node Name}\label{field-heat-recovery-leaving-temperature-setpoint-node-name-2}
+
+This field is optional.~ It can be used to refine the model and controls for heat recovery operation of the chiller.~ The node named here should have a setpoint placed on it by a setpoint manager.~ If the plant loop's demand calculation scheme is set to SingleSetpoint, then a single setpoint manager should be used.~ If the plant loop's demand calculation is set to DualSetpointDeadband then a dual setpoint manager should be used and the upper setpoint is used for control.~ When this field is used, a different model is used for determining the distribution of rejected heat between the two bundles that is more appropriate for series bundle arrangements and for chiller's that are able to produce relatively higher temperature heated fluilds.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Chiller:Electric:ReformulatedEIR,
+    Main Chiller,                        !- Chiller Name
+    50000,                               !- Reference Capacity {W}
+    3.99,                                !- Reference COP
+    6.67,                                !- Reference Leaving Chilled Water Temperature {C}
+    35.0,                                !- Reference Leaving Condenser Water Temperature {C}
+    0.00898,                             !- Reference Chilled Water Flow Rate {m3/s}
+    0.01122,                             !- Reference Condenser Water Flow Rate {m3/s}
+    Main Chiller RecipCapFT,             !- Cooling Capacity Function of Temperature Curve
+    Main Chiller RecipEIRFT,             !- Electric Input to Cooling Output Ratio Function of Temperature Curve
+  LeavingCondenserWaterTemperature     !- Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Type
+    Main Chiller RecipEIRFPLR,           !- Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
+    0.01,                                !- Minimum Part Load Ratio
+    1,                                   !- Maximum Part Load Ratio
+    1,                                   !- Optimum Part Load Ratio
+    0.07,                                !- Minimum Unloading Ratio
+    Main Chiller ChW Inlet,              !- Chilled Water Side Inlet Node
+    Main Chiller ChW Outlet,             !- Chilled Water Side Outlet Node
+    Main Chiller Cnd Inlet,              !- Condenser Side Inlet Node
+    Main Chiller Cnd Outlet,             !- Condenser Side Outlet Node
+    1,                                   !- Fraction of Compressor Electric Power Rejected by Condenser
+    2,                                   !- Leaving Chilled Water Lower Temperature Limit {C}
+    ConstantFlow;                        !- Chiller Flow Mode
+
+  ! Cooling capacity to rated capacity function of Temperature Curve
+  ! x = Leaving Chilled Water Temperature and y = Leaving Condenser Water Temperature
+
+    Curve:Biquadratic,
+      Main Chiller RecipCapFT,  !- Name
+      0.958546443,       !- Coefficient1 Constant
+      0.035168695,       !- Coefficient2 x
+      0.000124662,       !- Coefficient3 x\*\*2
+      -0.00274551,       !-Coefficient4y
+      -0.00005000,       !-Coefficient5y\*\*2
+      -0.00017234,       !-Coefficient6x\*y
+      5.00,              !- Minimum Value of x
+      10.0,              !- Maximum Value of x
+      20.00,             !- Minimum Value of y
+      40.94;             !- Maximum Value of y
+
+  ! Energy Input to Cooling Output Ratio Function of Temperature Curve
+  ! x = Leaving Chilled Water Temperature and y = Leaving Condenser Water Temperature
+
+    Curve:Biquadratic,
+      Main Chiller RecipEIRFT,  !- Name
+      0.732700123,       !- Coefficient1 Constant
+      -0.00834360,       !- Coefficient2 x
+      0.000638530,       !- Coefficient3 x\*\*2
+      -0.00303753,       !-Coefficient4y
+      0.000484952,       !-Coefficient5y\*\*2
+      -0.00083584,       !-Coefficient6x\*y
+      5.00,              !- Minimum Value of x
+      10.0,              !- Maximum Value of x
+      20.00,             !- Minimum Value of y
+      40.94;             !- Maximum Value of y
+
+  ! Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve
+  ! x = Leaving Condenser water Temperature and y = Part Load Ratio
+
+    Curve:Bicubic,
+      Main Chiller RecipEIRFPLR, !- Name
+      0.070862846,        !- Coefficient1 Constant
+      0.002787560,        !- Coefficient2 x
+      -0.00000891,        !- Coefficient3 x\*\*2
+      0.230973399,        !-Coefficient4y
+      1.250442176,        !-Coefficient5y\*\*2
+      -0.00216102,        !-Coefficient6x\*y
+      0.000000,           !-Coefficient7x\*\*3
+      -0.56300936,        !-Coefficient8y\*\*3
+      0.000000,           !-Coefficient9x\*\*2\*y
+      0.000000,           !-Coefficient10x\*y\*\*2
+      20.00,              !- Minimum Value of x
+      40.94,              !- Maximum Value of x
+      0.01,               !- Minimum Value of y
+      1.0;               !- Maximum Value of y
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-006}
+
+The output variables for Chiller:Electric:ReformulatedEIR are the same as the output variables for Chiller:Electric:EIR (ref. Electric EIR Chiller Outputs). except for the Chiller Condenser Fan Electric Power and Energy reports
+
+\subsection{Chiller:EngineDriven}\label{chillerenginedriven}
+
+\subsubsection{Inputs}\label{inputs-6-018}
+
+\paragraph{Field: Name}\label{field-name-5-017}
+
+This alpha field contains the identifying name for the engine driven chiller.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-3-000}
+
+This alpha field determines what type of condenser will be modeled with this chiller. The 3 type of condensers are AirCooled, WaterCooled, and EvaporativelyCooled with the default being AirCooled if not specified. AirCooled and EvaporativelyCooled do not require a Condenser Loop to be specified, where the WaterCooled option requires the full specification of the Condenser Loop and its associated equipment.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-4}
+
+This numeric field contains the nominal cooling capability of the chiller in Watts.
+
+\paragraph{Field: Nominal COP}\label{field-nominal-cop-2}
+
+This numeric field contains the chiller's coefficient of performance (COP).
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-5}
+
+This required alpha field contains the identifying name for the chiller plant side inlet node.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-5}
+
+This required alpha field contains the identifying name for the chiller plant side outlet node.
+
+\paragraph{Field: Condenser Inlet Node Name}\label{field-condenser-inlet-node-name-5}
+
+This alpha field contains the identifying name for the chiller condenser side inlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and a condenser inlet node name is specified here, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates an outdoor air node and the air temperature information on this node is taken directly from the weather file (no node height adjustment).
+
+\paragraph{Field: Condenser Outlet Node Name}\label{field-condenser-outlet-node-name-5}
+
+This alpha field contains the identifying name for the chiller condenser side outlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates a condenser side outlet air node.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-5}
+
+This numeric field contains the chiller's minimum part load ratio. The expected range is between 0 and 1. The minimum part load is not the load where the machine shuts off, but where the amount of power remains constant to produce smaller loads than this fraction.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-5}
+
+This numeric field contains the chiller's maximum part load ratio. This value may exceed 1, but the normal range is between 0 and 1.1.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-5}
+
+This numeric field contains the chiller's optimum part load ratio. This is the part load ratio at which the chiller performs at its maximum COP.
+
+\paragraph{Field: Design Condenser Inlet Temperature}\label{field-design-condenser-inlet-temperature-3}
+
+This numeric field contains the chiller's condenser inlet design temperature in Celsius.
+
+\paragraph{Field: Temperature Rise Coefficient}\label{field-temperature-rise-coefficient-1}
+
+This numeric field contains the electric chiller's temperature rise coefficient which is defined as the ratio of the required change in condenser water temperature to a given change in chilled water temperature, which maintains the capacity at the nominal value. This is calculated as the following ratio:
+
+\begin{equation}
+\frac{{TCEn{t_{required}} - TCEn{t_{rated}}}}{{TEL{v_{required}} - TEL{v_{rated}}}}
+\end{equation}
+
+where:
+
+TCEnt\(_{required}\) = Required entering condenser air or water temperature to maintain rated capacity.
+
+TCEnt\(_{rated}\) = Rated entering condenser air or water temperature at rated capacity.
+
+TELv\(_{required}\) = Required leaving evaporator water outlet temperature to maintain rated capacity.
+
+TELv\(_{rated}\) = Rated leaving evaporator water outlet temperature at rated capacity.
+
+\paragraph{Field: Design Chilled Water Outlet Temperature}\label{field-design-chilled-water-outlet-temperature-1}
+
+This numeric field contains the chiller's evaporator outlet design temperature in Celsius.
+
+\paragraph{Field: Design Chilled Water Flow Rate}\label{field-design-chilled-water-flow-rate-4}
+
+For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate. The units are in cubic meters per second.
+
+\paragraph{Field: Design Condenser Water Flow Rate}\label{field-design-condenser-water-flow-rate-3}
+
+This numeric field contains the chiller's design condenser water flow rate in cubic meters per second. This field can be autosized. This field is not user for Condenser Type = AirCooled or EvaporativelyCooled.
+
+\paragraph{Capacity Ratio Curve}\label{capacity-ratio-curve-1}
+
+The Capacity Ratio Curve is a quadratic equation that determines the Ratio of Available Capacity to Nominal Capacity. The defining equation is:
+
+\begin{equation}
+AvailToNominalCapacityRatio = {C_1} + {C_2}{\Delta_{temp}} + {C_3}\Delta_{temp}^2
+\end{equation}
+
+Where the Delta Temperature is defined as:
+
+\begin{equation}
+FullLoadtoPowerRatio = {C_1} + {C_2}AvailToNominalCapRatio + {C_3}AvailToNominalCapRati{o^2}
+\end{equation}
+
+TempCondIn = Temperature entering the condenser (water or air temperature depending on condenser type).
+
+TempCondInDesign = Design Condenser Inlet Temperature from User input above.
+
+TempEvapOut = Temperature leaving the evaporator.
+
+TempEvapOutDesign = Design Chilled Water Outlet Temperature from User input above.
+
+TempRiseCoefficient = User Input from above.
+
+The following three fields contain the coefficients for the quadratic equation.
+
+\paragraph{Field: Coefficient 1 of Capacity Ratio Curve}\label{field-coefficient-1-of-capacity-ratio-curve-1}
+
+This numeric field contains the first coefficient for the capacity ratio curve.
+
+\paragraph{Field: Coefficient 2 of Capacity Ratio Curve}\label{field-coefficient-2-of-capacity-ratio-curve-1}
+
+This numeric field contains the second coefficient for the capacity ratio curve.
+
+\paragraph{Field: Coefficient 3 of Capacity Ratio Curve}\label{field-coefficient-3-of-capacity-ratio-curve-1}
+
+This numeric field contains the third coefficient for the capacity ratio curve.
+
+\paragraph{Power Ratio Curve}\label{power-ratio-curve-1}
+
+The Power Ratio Curve is a quadratic equation that determines the Ratio of Full Load to Power. The defining equation is:
+
+\(FracFullLoadPower = {C_1} + {C_2}PartLoadRatio + {C_3}PartLoadRati{o^2}\) The following three fields contain the coefficients for the quadratic equation.
+
+\paragraph{Field: Coefficient 1 of Power Ratio Curve}\label{field-coefficient-1-of-power-ratio-curve}
+
+This numeric field contains the first coefficient for the power ratio curve.
+
+\paragraph{Field: Coefficient 2 of Power Ratio Curve}\label{field-coefficient-2-of-power-ratio-curve-1}
+
+This numeric field contains the second coefficient for the power ratio curve.
+
+\paragraph{Field: Coefficient 3 of Power Ratio Curve}\label{field-coefficient-3-of-power-ratio-curve-1}
+
+This numeric field contains the third coefficient for the power ratio curve.
+
+\paragraph{Full Load Ratio Curve}\label{full-load-ratio-curve-1}
+
+The Full Load Ratio Curve is a quadratic equation that determines the fraction of full load power. The defining equation is:
+
+\begin{equation}
+{\rm{CoolingLoadtoFuelCurve}} = {C_1} + {C_2} * PLR + {C_3} * PL{R^2}
+\end{equation}
+
+The following three fields contain the coefficients for the quadratic equation.
+
+\paragraph{Field: Coefficient 1 of Full Load Ratio Curve}\label{field-coefficient-1-of-full-load-ratio-curve-1}
+
+This numeric field contains the first coefficient for the full load ratio curve.
+
+\paragraph{Field: Coefficient 2 of Full Load Ratio Curve}\label{field-coefficient-2-of-full-load-ratio-curve-1}
+
+This numeric field contains the second coefficient for the full load ratio curve.
+
+\paragraph{Field: Coefficient 3 of Full Load Ratio Curve}\label{field-coefficient-3-of-full-load-ratio-curve-1}
+
+This numeric field contains the third coefficient for the full load ratio curve.
+
+\paragraph{Field Chilled Water Outlet Temperature Lower Limit}\label{field-chilled-water-outlet-temperature-lower-limit-3}
+
+This numeric field contains the lower limit for the evaporator outlet temperature. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn't get too cold.
+
+\paragraph{Field: Fuel Use Curve Name}\label{field-fuel-use-curve-name}
+
+This alpha field contains the name of the Cooling Load to Fuel Use curve. The curve itself is specified separately using the EnergyPlus Curve Manager. The Fuel Use Curve is a quadratic equation that determines the ratio of Cooling Load to Fuel Energy. The defining equation is:
+
+\begin{equation}
+RecoveryJacketHeatToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}
+\end{equation}
+
+where PLR is the Part Load Ratio from the Chiller. The Part Load Based Fuel Input Curve determines the ratio of fuel energy per unit time (J/s) / cooling load (W). This is illustrated by the logic block in the Engine Driven Chiller algorithm.
+
+\begin{lstlisting}
+IF (PartLoadRat = = 0)THEN
+   EngineDrivenFuelEnergy = 0
+ELSE
+   ClngLoadFuelRat = CurveValue(EngineDrivenChiller(ChillerNum)%ClngLoadtoFuelCurve, PartLoadRat )
+   EngineDrivenFuelEnergy = QEvaporator / ClngLoadFuelRat
+END IF
+\end{lstlisting}
+
+\paragraph{Field: Jacket Heat Recovery Curve Name}\label{field-jacket-heat-recovery-curve-name-000}
+
+This alpha field contains the name of the Recovery Jacket Heat curve. The curve itself is specified separately using the EnergyPlus Curve Manager. The Recovery Jacket Heat Curve is a quadratic equation that determines the ratio of recovery jacket heat to fuel energy. The defining equation is:
+
+\begin{equation}
+RecoveryLubeHeatToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}
+\end{equation}
+
+where RL is the Ratio of Load to Diesel Engine Capacity
+
+\paragraph{Field: Lube Heat Recovery Curve Name}\label{field-lube-heat-recovery-curve-name-000}
+
+This alpha field contains the name of the Recovery Lube Heat curve. The curve itself is specified separately using the EnergyPlus Curve Manager. The Recovery Lubricant Heat Curve is a quadratic equation that determines the ratio of recovery lube heat to fuel energy. The defining equation is:
+
+\begin{equation}
+TotalExhaustToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}
+\end{equation}
+
+where RL is the Ratio of Load to Diesel Engine Capacity
+
+\paragraph{Field: Total Exhaust Energy Curve Name}\label{field-total-exhaust-energy-curve-name-000}
+
+This alpha field contains the name of the Total Exhaust Energy curve. The curve itself is specified separately using the EnergyPlus Curve Manager. The Total Exhaust Energy Curve is a quadratic equation that determines the ratio of total exhaust energy to fuel energy. The defining equation is:
+
+\begin{equation}
+AbsoluteExhaustTemperature = {C_1} + {C_2}RL + {C_3}R{L^2}
+\end{equation}
+
+where RL is the Ratio of Load to Diesel Engine Capacity
+
+\paragraph{Field: Exhaust Temperature Curve Name}\label{field-exhaust-temperature-curve-name-000}
+
+This alpha field contains the name of the Exhaust Temperature curve. The curve itself is specified separately using the EnergyPlus Curve Manager. The Exhaust Temperature Curve is a quadratic equation that determines the absolute exhaust temperature. The defining equation is:
+
+\begin{equation}
+UAToCapacityRatio = {C_1}EngineCapacit{y^{{C_2}}}
+\end{equation}
+
+where RL is the Ratio of Load to Diesel Engine Capacity
+
+\paragraph{U-Factor Times Area Curve}\label{u-factor-times-area-curve}
+
+The U-Factor Times Area (UA) is an equation that determines the overall heat transfer coefficient for the exhaust gasses with the stack. The heat transfer coefficient ultimately helps determine the exhaust stack temperature. The defining equation is:
+
+\begin{equation}
+\frac{{TCEn{t_{required}} - TCEn{t_{rated}}}}{{TEL{v_{required}} - TEL{v_{rated}}}}
+\end{equation}
+
+The following two fields contain the coefficients for the equation.
+
+\paragraph{Field: Coefficient 1 of U-Factor Times Area Curve}\label{field-coefficient-1-of-u-factor-times-area-curve-000}
+
+This numeric field contains the first coefficient for the overall heat transfer coefficient curve.
+
+\paragraph{Field: Coefficient 2 of U-Factor Times Area Curve}\label{field-coefficient-2-of-u-factor-times-area-curve-000}
+
+This numeric field contains the second (exponential) coefficient for the overall heat transfer coefficient curve.
+
+\paragraph{Field: Maximum Exhaust Flow per Unit of Power Output}\label{field-maximum-exhaust-flow-per-unit-of-power-output-000}
+
+This numeric field contains the maximum exhaust gas mass flow rate per watt of cooling provided by the engine driven chiller
+
+\paragraph{Field: Design Minimum Exhaust Temperature}\label{field-design-minimum-exhaust-temperature-000}
+
+This numeric field contains the steam saturation temperature in Celsius that would be used to determine the energy recovered from a water jacket heat exchanger on the engine.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-002}
+
+This alpha value specifies the type of fuel used in the engine. The fuel type can be NaturalGas, PropaneGas, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1 or OtherFuel2. This field is required.
+
+\paragraph{Field: Fuel Higher Heating Value}\label{field-fuel-higher-heating-value-000}
+
+This numeric field contains the higher heating value of the fuel used in kJ/kg.
+
+\paragraph{Field: Design Heat Recovery Water Flow Rate}\label{field-design-heat-recovery-water-flow-rate-3}
+
+This numeric field specifies the heat recovery volumetric flow rate through the engine in m\(^{3}\)/sec.~The heat recovery loop manager and hot water tan must also be specified if heat energy is to be recovered from the engine driven chiller.
+
+\paragraph{Field: Heat Recovery Inlet Node Name}\label{field-heat-recovery-inlet-node-name-3}
+
+This alpha field contains the identifying name for the heat recovery side inlet. If a loop is connected, then the jacket and lubricant heat will be recovered. There is no need for an effectiveness term, since the jacket and lubricant recovered heat energies are the actual recovered energies.
+
+\paragraph{Field: Heat Recovery Outlet Node Name}\label{field-heat-recovery-outlet-node-name-3}
+
+This alpha field contains the identifying name for the heat recovery side outlet.
+
+\paragraph{Field: Chiller Flow Mode}\label{field-chiller-flow-mode-5}
+
+This choice field determines how the chiller operates with respect to the intended fluid flow through the device's evaporator.~ There are three different choices for specifying operating modes for the intended flow behavior:~ ``NotModulated,'' ``ConstantFlow,'' and ``LeavingSetpointModulated.''~ NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.~ ConstantFlow is useful for constant speed pumping arrangements where the chiller's request for flow is stricter and can increase the overall loop flow.~ LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.~ In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.~ The default, if not specified, is NotModulated.
+
+\paragraph{Field: Maximum Temperature for Heat Recovery at Heat Recovery Outlet Node}\label{field-maximum-temperature-for-heat-recovery-at-heat-recovery-outlet-node}
+
+This field sets the maximum temperature that this piece of equipment can produce for heat recovery. The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit. This temperature limit puts an upper bound on the recovered heat and limits the max temperatures leaving the component.
+
+As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting. This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply. The temperature is specified in degrees C.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-6}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Design Chilled Water Flow Rate and Design Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-3-001}
+
+This numeric field contains the capacity of the chiller's electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the chiller is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-3-001}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the chiller is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-3-001}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the chiller is off.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Chiller:EngineDriven,
+      Central Chiller,         !- Chiller Name
+      WaterCooled,            !- Condenser Type
+      autosize,                !- Nominal Capacity {W}
+      2.75,                    !- COP
+      Central Chiller Inlet Node,  !- Chilled Water Inlet Node Name
+      Central Chiller Outlet Node,  !- Chilled Water Outlet Node Name
+      Central Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
+      Central Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
+      0.0,                     !- Minimum Part Load Ratio
+      1.0,                     !- Maximum Part Load Ratio
+      .65,                     !- Optimum Part Load Ratio
+      35.0,                    !- Design Condenser Inlet Temperature {C}
+      2.778,                   !- Temperature Rise Coefficient
+      6.67,                    !- Design Chilled Water Outlet Temperature {C}
+      autosize,                !- Design Chilled Water Flow Rate {m3/s}
+      autosize,                !- Design Condenser Water Flow Rate {m3/s}
+      0.9949,                  !- Coefficient 1 of Capacity Ratio Curve
+      -0.045954,               !- Coefficient 2 of Capacity Ratio Curve
+      -0.0013543,              !- Coefficient 3 of Capacity Ratio Curve
+      2.333,                   !- Coefficient 1 of Power Ratio Curve
+      -1.975,                  !- Coefficient 2 of Power Ratio Curve
+      0.6121,                  !- Coefficient 3 of Power Ratio Curve
+      0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
+      0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
+      0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
+      5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
+      Fuel Use Curve,          !- the Fuel Use Curve
+      Jacket Heat Recovery Curve,  !- the Recovery Jacket Heat curve
+      Lube Heat Recovery Curve,!- the Recovery Lube Heat curve
+      Total Exhaust Energy Curve,  !- the Total Exhaust Energy curve
+      Exhaust Temperature Curve,  !- the Exhaust Temperature curve
+      0.01516,                 !- Coefficient1 of UA curve
+      0.9,                     !- Coefficient2 of UA curve
+      0.00063,                 !- Maximum Exhaust Flow per W of Power Output {(kg/s)/W}
+      150,                     !- Design Minimum Exhaust temp. (Steam Saturation Temperature) {C}
+      DIESEL,                  !- Fuel Type
+      45500,                   !- Fuel Heating Value {kJ/kg}
+      0.0,                     !- Design heat recovery water flow rate {m3/s}
+      ,                        !- Heat Recovery Inlet Node Name
+      ,                        !- Heat Recovery Outlet Node Name
+      VariableFlow,            !- Chiller Flow Mode
+      60.0;                    !- Maximum Temp for Heat Recovery. This sets max availability {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-006}
+
+\begin{lstlisting}
+
+HVAC,Average,Chiller Electric Power [W]
+  HVAC,Sum,Chiller Electric Energy [J]
+  Zone,Meter,Electricity:Plant [J]
+  Zone,Meter,Cooling:Electricity [J]
+  HVAC,Average,Chiller Evaporator Cooling Rate [W]
+  HVAC,Sum,Chiller Evaporator Cooling Energy [J]
+  Zone,Meter,EnergyTransfer:Plant [J]
+  Zone,Meter,Chillers:EnergyTransfer [J]
+  HVAC,Average,Chiller Evaporator Inlet Temperature [C]
+  HVAC,Average,Chiller Evaporator Outlet Temperature [C]
+  HVAC,Average,Chiller Evaporator Mass Flow Rate [kg/s]
+  HVAC,Average,Chiller COP [W/W]
+  HVAC,Average,Chiller Condenser Heat Transfer Energy Rate [W]
+  HVAC,Sum,Chiller Condenser Heat Transfer Energy [J]
+  Zone,Meter,HeatRejection:EnergyTransfer [J]
+\end{lstlisting}
+
+Air-cooled or Evap-cooled:
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\end{itemize}
+
+Evap-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+Water-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Drive Shaft Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Drive Shaft Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Jacket Recovered Heat Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Jacket Recovered Heat Energy {[}J{]}
+\item
+  Zone,Meter,HeatRecovery:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Lube Recovered Heat Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Lube Recovered Heat Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Exhaust Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Exhaust Heat Recovery Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Total Recovered Heat Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Total Recovered Heat Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Exhaust Temperature {[}C{]}
+\end{itemize}
+
+One of the following blocks will be applicable based on fuel type:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Gas Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Gas Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Gas Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Propane Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Propane Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Propane Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Diesel Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Diesel Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Diesel Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Gasoline Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Gasoline Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Gasoline Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller FuelOil\#1 Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller FuelOil\#1 Energy {[}J{]}
+\item
+  HVAC,Average,Chiller FuelOil\#1 Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller FuelOil\#2 Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller FuelOil\#2 Energy {[}J{]}
+\item
+  HVAC,Average,Chiller FuelOil\#2 Mass Flow Rate {[}kg/s
+\item
+  HVAC,Average,Chiller OtherFuel1 Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller OtherFuel1 Energy {[}J{]}
+\item
+  HVAC,Average,Chiller OtherFuel1 Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller OtherFuel2 Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller OtherFuel2 Energy {[}J{]}
+\item
+  HVAC,Average,Chiller OtherFuel2 Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+These chiller output variables are defined above under ``Generic Chiller Outputs.''
+
+\subsection{Chiller:CombustionTurbine}\label{chillercombustionturbine}
+
+This chiller model is the empirical model from the Building Loads and System Thermodynamics (BLAST) program. Chiller performance curves are generated by fitting catalog data to third order polynomial equations. Three sets of coefficients are required.
+
+\subsubsection{Inputs}\label{inputs-7-018}
+
+\paragraph{Field: Name}\label{field-name-6-015}
+
+This alpha field contains the identifying name for the combustion turbine chiller.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-4-000}
+
+This alpha field determines what type of condenser will be modeled with this chiller. The 3 type of condensers are AirCooled, WaterCooled, and EvaporativelyCooled with the default being AirCooled if not specified. AirCooled and EvaporativelyCooled do not require a Condenser Loop to be specified, where the WaterCooled option requires the full specification of the Condenser Loop and its associated equipment.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-5}
+
+This numeric field contains the nominal cooling capability of the chiller in Watts.
+
+\paragraph{Field: Nominal COP}\label{field-nominal-cop-3}
+
+This numeric field contains the chiller's coefficient of performance (COP).
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-6}
+
+This alpha field contains the identifying name for the combustion turbine chiller plant side inlet node.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-6}
+
+This required alpha field contains the identifying name for the combustion turbine chiller plant side inlet node.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-7}
+
+This required alpha field contains the identifying name for the combustion turbine chiller plant side outlet node.
+
+\paragraph{Field: Condenser Inlet Node Name}\label{field-condenser-inlet-node-name-6}
+
+This alpha field contains the identifying name for the combustion turbine chiller condenser side inlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and a condenser inlet node name is specified here, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates an outdoor air node and the air temperature information on this node is taken directly from the weather file (no node height adjustment).
+
+\paragraph{Field: Condenser Outlet Node Name}\label{field-condenser-outlet-node-name-6}
+
+This alpha field contains the identifying name for the combustion turbine chiller condenser side outlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates a condenser side outlet air node.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-6}
+
+This numeric field contains the combustion turbine chiller's minimum part load ratio. The expected range is between 0 and 1. The minimum part load is not the load where the machine shuts off, but where the amount of power remains constant to produce smaller loads than this fraction.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-6}
+
+This numeric field contains the combustion turbine chiller's maximum part load ratio. This value may exceed 1, but the normal range is between 0 and 1.1.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-6}
+
+This numeric field contains the combustion turbine chiller's optimum part load ratio. This is the part load ratio at which the chiller performs at its maximum COP.
+
+\paragraph{Field: Design Condenser Inlet Temperature}\label{field-design-condenser-inlet-temperature-4}
+
+This numeric field contains the combustion turbine chiller's condenser inlet design temperature in Celsius.
+
+\paragraph{Field: Temperature Rise Coefficient}\label{field-temperature-rise-coefficient-2}
+
+This numeric field contains the electric chiller's temperature rise coefficient which is defined as the ratio of the required change in condenser water temperature to a given change in chilled water temperature, which maintains the capacity at the nominal value. This is calculated as the following ratio:
+
+\begin{equation}
+\frac{{TCEn{t_{required}} - TCEn{t_{rated}}}}{{TEL{v_{required}} - TEL{v_{rated}}}}
+\end{equation}
+
+where:
+
+TCEnt\(_{required}\) = Required entering condenser air or water temperature to maintain rated capacity.
+
+TCEnt\(_{rated}\) = Rated entering condenser air or water temperature at rated capacity.
+
+TELv\(_{required}\) = Required leaving evaporator water outlet temperature to maintain rated capacity.
+
+TELv\(_{rated}\) = Rated leaving evaporator water outlet temperature at rated capacity.
+
+\paragraph{Field: Design Chilled Water Outlet Temperature}\label{field-design-chilled-water-outlet-temperature-2}
+
+This numeric field contains the combustion turbine chiller's evaporator outlet design temperature in Celsius.
+
+\paragraph{Field: Design Chilled Water Flow Rate}\label{field-design-chilled-water-flow-rate-5}
+
+For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate. The units are in cubic meters per second.
+
+\paragraph{Field: Design Condenser Water Flow Rate}\label{field-design-condenser-water-flow-rate-4}
+
+This numeric field contains the combustion turbine chiller's design condenser water flow rate in cubic meters per second. This field can be autosized. This field is not used for Condenser Type = AirCooled or EvaporativelyCooled.
+
+\paragraph{Capacity Ratio Curve}\label{capacity-ratio-curve-2}
+
+The Capacity Ratio Curve is a quadratic equation that determines the Ratio of Available Capacity to Nominal Capacity. The defining equation is:
+
+\begin{equation}
+AvailToNominalCapacityRatio = {C_1} + {C_2}{\Delta_{temp}} + {C_3}\Delta_{temp}^2
+\end{equation}
+
+Where the Delta Temperature is defined as:
+
+\begin{equation}
+FullLoadtoPowerRatio = {C_1} + {C_2}AvailToNominalCapRatio + {C_3}AvailToNominalCapRati{o^2}
+\end{equation}
+
+TempCondIn = Temperature entering the condenser (water or air temperature depending on condenser type).
+
+TempCondInDesign = Design Condenser Inlet Temperature from User input above.
+
+TempEvapOut = Temperature leaving the evaporator.
+
+TempEvapOutDesign = Design Chilled Water Outlet Temperature from User input above.
+
+TempRiseCoefficient = User Input from above.
+
+The following three fields contain the coefficients for the quadratic equation.
+
+\paragraph{Field: Coefficient 1 of Capacity Ratio Curve}\label{field-coefficient-1-of-capacity-ratio-curve-2}
+
+This numeric field contains the first coefficient for the capacity ratio curve.
+
+\paragraph{Field: Coefficient 2 of Capacity Ratio Curve}\label{field-coefficient-2-of-capacity-ratio-curve-2}
+
+This numeric field contains the second coefficient for the capacity ratio curve.
+
+\paragraph{Field: Coefficient 3 of Capacity Ratio Curve}\label{field-coefficient-3-of-capacity-ratio-curve-2}
+
+This numeric field contains the third coefficient for the capacity ratio curve.
+
+\paragraph{Power Ratio Curve}\label{power-ratio-curve-2}
+
+The Power Ratio Curve is a quadratic equation that determines the Ratio of Full Load to Power. The defining equation is:
+
+\(FracFullLoadPower = {C_1} + {C_2}PartLoadRatio + {C_3}PartLoadRati{o^2}\) The following three fields contain the coefficients for the quadratic equation.
+
+\paragraph{Field: Coefficient 1 of Power Ratio Curve}\label{field-coefficient-1-of-power-ratio-curve-1}
+
+This numeric field contains the first coefficient for the power ratio curve.
+
+\paragraph{Field: Coefficient 2 of Power Ratio Curve}\label{field-coefficient-2-of-power-ratio-curve-2}
+
+This numeric field contains the second coefficient for the power ratio curve.
+
+\paragraph{Field: Coefficient 3 of Power Ratio Curve}\label{field-coefficient-3-of-power-ratio-curve-2}
+
+This numeric field contains the third coefficient for the power ratio curve.
+
+\paragraph{Full Load Ratio Curve}\label{full-load-ratio-curve-2}
+
+The Full Load Ratio Curve is a quadratic equation that determines the fraction of full load power. The defining equation is:
+
+\begin{equation}
+FuelEnergyInput = PLoad * (FI{C_1} + FI{C_2}RLoad + FI{C_3}RLoa{d^2}) * (TBFI{C_1} + TBFI{C_2}A{T_{air}} + TBFI{C_3}AT_{air}^2)
+\end{equation}
+
+The following three fields contain the coefficients for the quadratic equation.
+
+\paragraph{Field: Coefficient 1 of Full Load Ratio Curve}\label{field-coefficient-1-of-full-load-ratio-curve-2}
+
+This numeric field contains the first coefficient for the full load ratio curve.
+
+\paragraph{Field: Coefficient 2 of Full Load Ratio Curve}\label{field-coefficient-2-of-full-load-ratio-curve-2}
+
+This numeric field contains the second coefficient for the full load ratio curve.
+
+\paragraph{Field: Coefficient 3 of Full Load Ratio Curve}\label{field-coefficient-3-of-full-load-ratio-curve-2}
+
+This numeric field contains the third coefficient for the full load ratio curve.
+
+\paragraph{Field: Chilled Water Outlet Temperature Lower Limit}\label{field-chilled-water-outlet-temperature-lower-limit-4}
+
+This numeric field contains the lower limit for the evaporator outlet temperature. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn't get too cold.
+
+\paragraph{Fuel Input Curve}\label{fuel-input-curve}
+
+The Fuel Input Curve is a polynomial equation that determines the Ratio of Fuel Input to Energy Output. The equation combines both the Fuel Input Curve Coefficients and the Temperature Based Fuel Input Curve Coefficients. The defining equation is:
+
+\begin{equation}
+ExhaustFlowRate = GTCapacity * ({C_1} + {C_2}A{T_{air}} + {C_3}AT_{air}^2)
+\end{equation}
+
+where FIC represents the Fuel Input Curve Coefficients, TBFIC represents the Temperature Based Fuel Input Curve Coefficients, Rload is the Ratio of Load to Combustion Turbine Engine Capacity, and AT\(_{air}\) is the difference between the current ambient and design ambient temperatures.
+
+The following three fields contain the coefficients for the fuel input curve.
+
+\paragraph{Field: Coefficient 1 of Fuel Input Curve}\label{field-coefficient-1-of-fuel-input-curve}
+
+This numeric field contains the first coefficient for the Fuel Input Curve.
+
+\paragraph{Field: Coefficient 2 of Fuel Input Curve}\label{field-coefficient-2-of-fuel-input-curve}
+
+This numeric field contains the second coefficient for the Fuel Input Curve.
+
+\paragraph{Field: Coefficient 3 of Fuel Input Curve}\label{field-coefficient-3-of-fuel-input-curve}
+
+This numeric field contains the third coefficient for the Fuel Input Curve.
+
+The following three fields contain the coefficients for the temperature based fuel input curve.
+
+\paragraph{Field: Coefficient 1 of Temperature Based Fuel Input Curve}\label{field-coefficient-1-of-temperature-based-fuel-input-curve}
+
+This numeric field contains the first coefficient for the Temperature Based Fuel Input Curve.
+
+\paragraph{Field: Coefficient 2 of Temperature Based Fuel Input Curve}\label{field-coefficient-2-of-temperature-based-fuel-input-curve}
+
+This numeric field contains the second coefficient for the Temperature Based Fuel Input Curve.
+
+\paragraph{Field: Coefficient 3 of Temperature Based Fuel Input Curve}\label{field-coefficient-3-of-temperature-based-fuel-input-curve}
+
+This numeric field contains the third coefficient for the Temperature Based Fuel Input Curve.
+
+\paragraph{Exhaust Flow Curve}\label{exhaust-flow-curve}
+
+The Exhaust Flow Curve is a quadratic equation that determines the Ratio of Exhaust Gas Flow Rate to Engine Capacity. The defining equation is:
+
+\emph{\(ExhaustTemperature = ({C_1} + {C_2}RLoad + {C_3}RLoa{d^2}) * (TB{C_1} + TB{C_2}A{T_{air}} + TB{C_3}AT_{air}^2) - 273.15\) ~}
+
+where GTCapacity is the Combustion Turbine Engine Capacity, and AT\(_{air}\) is the difference between the current ambient and design ambient temperatures.
+
+\paragraph{Field: Coefficient 1 of Exhaust Flow Curve}\label{field-coefficient-1-of-exhaust-flow-curve}
+
+This numeric field contains the first coefficient for the Exhaust Flow Curve.
+
+\paragraph{Field: Coefficient 2 of Exhaust Flow Curve}\label{field-coefficient-2-of-exhaust-flow-curve}
+
+This numeric field contains the second coefficient for the Exhaust Flow Curve.
+
+\paragraph{Field: Coefficient 3 of Exhaust Flow Curve}\label{field-coefficient-3-of-exhaust-flow-curve}
+
+This numeric field contains the third coefficient for the Exhaust Flow Curve.
+
+\paragraph{Exhaust Gas Temperature Curve}\label{exhaust-gas-temperature-curve}
+
+The Exhaust Gas Temperature Curve is a polynomial equation that determines the Exhaust Gas Temperature. The equation combines both the Exhaust Gas Temperature Curve Coefficients (Based on the Part Load Ratio) and the (Ambient) Temperature Based Exhaust Gas Temperature Curve Coefficients. The defining equation is:
+
+~\(RecoveryLubeEnergy = PLoad * ({C_1} + {C_2}RL + {C_3}R{L^2})\)
+
+where C represents the Exhaust Gas Temperature Curve Coefficients, TBC are the Temperature Based Exhaust Gas Temperature Curve Coefficients, RLoad is the Ratio of Load to Combustion Turbine Engine Capacity, and AT\(_{air}\) is the difference between the actual ambient and design ambient temperatures.
+
+\paragraph{Field: Coefficient 1 of Exhaust Gas Temperature Curve}\label{field-coefficient-1-of-exhaust-gas-temperature-curve}
+
+This numeric field contains the first coefficient for the Exhaust Gas Temperature Curve.
+
+\paragraph{Field: Coefficient 2 of Exhaust Gas Temperature Curve}\label{field-coefficient-2-of-exhaust-gas-temperature-curve}
+
+This numeric field contains the second coefficient for the Exhaust Gas Temperature Curve.
+
+\paragraph{Field: Coefficient 3 of Exhaust Gas Temperature Curve}\label{field-coefficient-3-of-exhaust-gas-temperature-curve}
+
+This numeric field contains the third coefficient for the Exhaust Gas Temperature Curve.
+
+\paragraph{Field: Coefficient 1 of Temperature Based Exhaust Gas Temperature Curve}\label{field-coefficient-1-of-temperature-based-exhaust-gas-temperature-curve}
+
+This numeric field contains the first coefficient for the Temperature Based Exhaust Gas Temperature Curve.
+
+\paragraph{Field: Coefficient 2 of Temperature Based Exhaust Gas Temperature Curve}\label{field-coefficient-2-of-temperature-based-exhaust-gas-temperature-curve}
+
+This numeric field contains the second coefficient for the Temperature Based Exhaust Gas Temperature Curve.
+
+\paragraph{Field: Coefficient 3 of Temperature Based Exhaust Gas Temperature Curve}\label{field-coefficient-3-of-temperature-based-exhaust-gas-temperature-curve}
+
+This numeric field contains the third coefficient for the Temperature Based Exhaust Gas Temperature Curve.
+
+\paragraph{Recovery Lubricant Heat Curve}\label{recovery-lubricant-heat-curve}
+
+The Recovery Lubricant Heat Curve is a quadratic equation that determines the recovery lube energy. The defining equation is:
+
+\begin{equation}
+UAToCapacityRatio = {C_1}GasTurbineEngineCapacit{y^{{C_2}}}
+\end{equation}
+
+where Pload is the engine load and RL is the Ratio of Load to Combustion Turbine Engine Capacity
+
+The following three fields contain the coefficients for the quadratic equation.
+
+\paragraph{Field: Coefficient 1 of Recovery Lube Heat Curve}\label{field-coefficient-1-of-recovery-lube-heat-curve}
+
+This numeric field contains the first coefficient for the Recovery Lube Heat curve.
+
+\paragraph{Field: Coefficient 2 of Recovery Lube Heat Curve}\label{field-coefficient-2-of-recovery-lube-heat-curve}
+
+This numeric field contains the second coefficient for the Recovery Lube Heat curve.
+
+\paragraph{Field: Coefficient 3 of Recovery Lube Heat Curve}\label{field-coefficient-3-of-recovery-lube-heat-curve}
+
+This numeric field contains the third coefficient for the Recovery Lube Heat curve.
+
+\paragraph{U-Factor Times Area Curve Curve}\label{u-factor-times-area-curve-curve}
+
+The U-Factor Times Area Curve (UA) is an equation that determines the overall heat transfer coefficient for the exhaust gasses with the stack. The heat transfer coefficient ultimately helps determine the exhaust stack temperature. The defining equation is:
+
+\begin{equation}
+AvailableCoolingCapacity = NominalCoolingCapacity*CoolCapfT\left( {{T_{cw,l}},{T_{cond}}} \right)
+\end{equation}
+
+The following two fields contain the coefficients for the equation.
+
+\paragraph{Field: Coefficient 1 of U-Factor Times Area Curve}\label{field-coefficient-1-of-u-factor-times-area-curve-1-000}
+
+This numeric field contains the first coefficient for the overall heat transfer coefficient curve.
+
+\paragraph{Field: Coefficient 2 of U-Factor Times Area Curve}\label{field-coefficient-2-of-u-factor-times-area-curve-1-000}
+
+This numeric field contains the second (exponential) coefficient for the overall heat transfer coefficient curve.
+
+\paragraph{Field: Gas Turbine Engine Capacity}\label{field-gas-turbine-engine-capacity}
+
+This numeric field contains the capacity of the gas turbine engine in watts.
+
+\paragraph{Field: Maximum Exhaust Flow per Unit of Power Output}\label{field-maximum-exhaust-flow-per-unit-of-power-output-1-000}
+
+This numeric field contains the maximum exhaust gas mass flow rate per kilowatt of power out.
+
+\paragraph{Field: Design Steam Saturation Temperature}\label{field-design-steam-saturation-temperature}
+
+This numeric field contains the design steam saturation temperature in Celsius.
+
+\paragraph{Field: Fuel Higher Heating Value}\label{field-fuel-higher-heating-value-1-000}
+
+This numeric field contains the higher heating value of the fuel used in kJ/kg.
+
+\paragraph{Field: Design Heat Recovery Water Flow Rate}\label{field-design-heat-recovery-water-flow-rate-4}
+
+This is the design heat recovery water flow rate if the heat recovery option is being simulated. If this value is greater than 0.0, a heat recovery loop must be specified and attached to the chiller using the next two node fields. The units are in cubic meters per second.
+
+\paragraph{Field: Heat Recovery Inlet Node Name}\label{field-heat-recovery-inlet-node-name-4}
+
+This alpha field contains the identifying name for the heat recovery side inlet.~ If a loop is connected, then the jacket and lubricant heat will be recovered.~ There is no need for an effectiveness term, since the jacket and lubricant recovered heat energies are the actual recovered energies.
+
+\paragraph{Field: Heat Recovery Outlet Node Name}\label{field-heat-recovery-outlet-node-name-4}
+
+This alpha field contains the identifying name for the heat recovery side outlet.
+
+\paragraph{Field: Chiller Flow Mode}\label{field-chiller-flow-mode-6}
+
+This choice field determines how the chiller operates with respect to the intended fluid flow through the device's evaporator.~ There are three different choices for specifying operating modes for the intended flow behavior:~ ``NotModulated,'' ``ConstantFlow,'' and ``LeavingSetpointModulated.''~ NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.~ ConstantFlow is useful for constant speed pumping arrangements where the chiller's request for flow is stricter and can increase the overall loop flow.~ LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.~ In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.~ The default, if not specified, is NotModulated.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-1-002}
+
+This alpha field determines the type of fuel that the chiller uses. Valid choices are: \textbf{NaturalGas, PropaneGas, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1} or \textbf{OtherFuel2}. The default is \textbf{NaturalGas}.
+
+\paragraph{Field: Heat Recovery Maximum Temperature}\label{field-heat-recovery-maximum-temperature-000}
+
+This field sets the maximum temperature that this piece of equipment can produce for heat recovery.~ The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit.~ This temperature limit puts an upper bound on the recovered heat and limits the max temperatures leaving the component.
+
+As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller.~ For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field.~ The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting.~ This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply.
+
+The temperature is specified in degrees C.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-7}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Design Chilled Water Flow Rate and Design Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-4-000}
+
+This numeric field contains the capacity of the chiller's electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the chiller is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-4-000}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the chiller is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-4-000}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the chiller is off.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+Chiller:CombustionTurbine,
+      Big Chiller,             !- Chiller Name
+      WaterCooled,            !- Condenser Type
+      30000,                   !- Nominal Capacity {W}
+      2.75,                    !- COP
+      Big Chiller Inlet Node,  !- Chilled Water Inlet Node Name
+      Big Chiller Outlet Node, !- Chilled Water Outlet Node Name
+      Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
+      Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
+      .15,                     !- Minimum Part Load Ratio
+      1.0,                     !- Maximum Part Load Ratio
+      .65,                     !- Optimum Part Load Ratio
+      35.0,                    !- Design Condenser Inlet Temperature {C}
+      2.778,                   !- Temperature Rise Coefficient
+      6.67,                    !- Design Chilled Water Outlet Temperature {C}
+      0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
+      0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
+      0.9949,                  !- Coefficient 1 of Capacity Ratio Curve
+      -0.045954,               !- Coefficient 2 of Capacity Ratio Curve
+      -0.0013543,              !- Coefficient 3 of Capacity Ratio Curve
+      2.333,                   !- Coefficient 1 of Power Ratio Curve
+      -1.975,                  !- Coefficient 2 of Power Ratio Curve
+      0.6121,                  !- Coefficient 3 of Power Ratio Curve
+      0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
+      0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
+      0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
+      5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
+      9.41,                    !- Coefficient 1 of Fuel Input curve
+      -9.48,                   !- Coefficient 2 of Fuel Input curve
+      4.32,                    !- Coefficient 3 of Fuel Input curve
+      1.0044,                  !- Coefficient 1 of Temperature Based Fuel Input curve
+      -0.0008,                 !- Coefficient 2 of Temperature Based Fuel Input curve
+      0,                       !- Coefficient 3 of Temperature Based Fuel Input curve
+      15.63518363,             !- Coefficient 1 of Exhaust Flow curve
+      -0.03059999,             !- Coefficient 2 of Exhaust Flow curve
+      -0.0002,                 !- Coefficient 3 of Exhaust Flow curve
+      916.992,                 !- Coefficient 1 of Exhaust Gas Temperature curve
+      307.998,                 !- Coefficient 2 of Exhaust Gas Temperature curve
+      79.992,                  !- Coefficient 3 of Exhaust Gas Temperature curve
+      1.005,                   !- Coefficient 1 of Temperature Based Exhaust Gas Temperature c
+      0.0018,                  !- Coefficient 2 of Temperature Based Exhaust Gas Temperature c
+      0,                       !- Coefficient 3 of Temperature Based Exhaust Gas Temperature c
+      0.223,                   !- Coefficient 1 of Recovery Lube Heat curve
+      -0.4,                    !- Coefficient 2 of Recovery Lube Heat curve
+      0.2286,                  !- Coefficient 3 of Recovery Lube Heat curve
+      0.01907045,              !- Coefficient 1 of UA curve
+      0.9,                     !- Coefficient 2 of UA curve
+      50000,                   !- Gas Turbine Engine Capacity {W}
+      0.00000504,              !- Maximum Exhaust Flow per Unit of Power Output {(kg/s)/W}
+      150,                     !- Design Steam Saturation Temperature {C}
+      43500,                   !- Fuel Higher Heating Value {kJ/kg}
+      0.0,                     !- Design Heat Recovery Water Flow Rate {m3/s}
+      ,                        !- Heat Recovery Inlet Node Name
+      ,                        !- Heat Recovery Outlet Node Name
+      VariableFlow,            !- Chiller Flow Mode
+      NaturalGas,              !- Fuel Type
+      80.0;                    !- Heat Recovery Maximum Temperature {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-006}
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Electric Energy {[}J{]}
+\item
+  Zone,Meter,Electricity:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:Electricity {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Evaporator Cooling Energy {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Plant {[}J{]}
+\item
+  Zone,Meter,Chillers:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Evaporator Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Condenser Heat Transfer Energy Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Meter,HeatRejection:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller COP {[}W/W{]}
+\end{itemize}
+
+Air-cooled or Evap-cooled:
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\end{itemize}
+
+Evap-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Average,Chiller Basin Heater Electric Energy {[}J{]}
+\end{itemize}
+
+Water-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Condenser Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Drive Shaft Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Drive Shaft Energy {[}J{]}
+\item
+  HVAC,Sum,Chiller Lube Recovered Heat Energy {[}J{]}
+\item
+  Zone,Meter,HeatRecovery:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Exhaust Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heat Recovery Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller \textless{}Fuel Type\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller \textless{}Fuel Type\textgreater{} Energy {[}J{]}
+\item
+  HVAC,Average,Chiller \textless{}Fuel Type\textgreater{} Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum,Chiller \textless{}Fuel Type\textgreater{} Mass {[}kg{]}
+\item
+  HVAC,Average,Chiller COP {[}W/W{]}
+\end{itemize}
+
+These chiller output variables are defined above under ``Generic Chiller Outputs.''~ The Fuel Type input will determine which fuel type is displayed in the output. In this example with the user choice of \textbf{NaturalGas}, you will have \textbf{Gas} Consumption.
+
+\subsection{ChillerHeater:Absorption:DirectFired}\label{chillerheaterabsorptiondirectfired}
+
+This chiller is a direct fired absorption chiller-heater which is modeled using performance curves similar to the equivalent chiller in DOE-2.1E. This type of chiller is unusual for EnergyPlus, because it may be used in the same plant on both a chilled water supply branch and a hot water supply branch. The chiller has six node connections for chilled water, condenser water, and hot water, and can provide simultaneous heating and cooling. During simultaneous operation, the heating capacity is reduced as the cooling load increases (for more details see below). Some equations are provided below to help explain the function of the various performance curves. For a detailed description of the algorithm and how the curves are used in the calculations, please see the Engineering Reference.
+
+\subsubsection{Inputs}\label{inputs-8-016}
+
+\paragraph{Field: Name}\label{field-name-7-014}
+
+This alpha field contains the identifying name for the chiller.
+
+\paragraph{Field: Nominal Cooling Capacity}\label{field-nominal-cooling-capacity}
+
+This numeric field contains the nominal cooling capability of the chiller in Watts.
+
+\paragraph{Field: Heating to Cooling Capacity Ratio}\label{field-heating-to-cooling-capacity-ratio}
+
+A positive fraction that represents the ratio of the heating capacity divided by the cooling capacity at rated conditions. The default is 0.8.
+
+\paragraph{Field: Fuel Input to Cooling Output Ratio}\label{field-fuel-input-to-cooling-output-ratio}
+
+A positive fraction that represents the ratio of the instantaneous cooling fuel used divided by the cooling capacity at rated conditions. The default is 0.97.
+
+\paragraph{Field: Fuel Input to Heating Output Ratio}\label{field-fuel-input-to-heating-output-ratio}
+
+A positive fraction that represents the ratio of the instantaneous heating fuel used divided by the nominal heating capacity. The default is 1.25.
+
+\paragraph{Field: Electric Input to Cooling Output Ratio}\label{field-electric-input-to-cooling-output-ratio}
+
+A positive fraction that represents the ratio of the instantaneous electricity used divided by the cooling capacity at rated conditions. If the chiller is both heating and cooling only the greater of the computed cooling and heating electricity is used. The default is 0.01.
+
+\paragraph{Field: Electric Input to Heating Output Ratio}\label{field-electric-input-to-heating-output-ratio}
+
+A positive fraction that represents the ratio of the instantaneous electricity used divided by the nominal heating capacity. If the chiller is both heating and cooling, the greater of the cooling electricity and heating eletricity is used. The default is 0.0.
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-7}
+
+This required alpha field contains the identifying name for the chiller chilled water side inlet node. This node name must be the same as the inlet node name for the chilled water supply branch on which this chiller is placed.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-8}
+
+This required alpha field contains the identifying name for the chiller chilled water side outlet node.
+
+\paragraph{Field: Condenser Inlet Node Name}\label{field-condenser-inlet-node-name-7}
+
+This required alpha field contains the identifying name for the chiller condenser side inlet node. If the Chiller is AirCooled, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air dry-bulb temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air dry-bulb temperature is taken directly from the weather data.
+
+\paragraph{Field: Condenser Outlet Node Name}\label{field-condenser-outlet-node-name-7}
+
+This required alpha field contains the identifying name for the chiller condenser side outlet node.
+
+\paragraph{Field: Hot Water Inlet Node Name}\label{field-hot-water-inlet-node-name}
+
+This required alpha field contains the identifying name for the chiller-heater hot water side inlet node. This node name must be the same as the inlet node name for the hot water supply branch on which this chiller-heater is placed.
+
+\paragraph{Field: Hot Water Outlet Node Name}\label{field-hot-water-outlet-node-name}
+
+This required alpha field contains the identifying name for the chiller-heater hot water side outlet node.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-7}
+
+A positive fraction that represents the minimum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. If the load on the chiller is below this fraction, the chiller will cycle. If the chiller is simultaneously heating and cooling, the greater part load ratio will be used. The default is 0.1.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-7}
+
+A positive fraction that represents the maximum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. If greater than 1.0, the chiller is typically thought of as capable of being overloaded. The default is 1.0.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-7}
+
+A positive fraction that represents the optimum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. It represents the most desirable operating point for the chiller. The default is 1.0.
+
+\paragraph{Field: Design Entering Condenser Water Temperature}\label{field-design-entering-condenser-water-temperature}
+
+The temperature in degrees C of the water entering the condenser of the chiller when operating at design conditions. This is usually based on the temperature delivered by the cooling tower in a water cooled application. The default is 29C.
+
+\paragraph{Field: Design Leaving Chilled Water Temperature}\label{field-design-leaving-chilled-water-temperature}
+
+The temperature in degrees C of the water leaving the evaporator of the chiller when operating at design conditions; also called the chilled water supply temperature or leaving chilled water temperature. The default is 7C.
+
+\paragraph{Field: Design Chilled Water Flow Rate}\label{field-design-chilled-water-flow-rate-6}
+
+For variable volume this is the max flow and for constant flow this is the chilled water flow rate in m\(^{3}\)/s.
+
+\paragraph{Field: Design Condenser Water Flow Rate}\label{field-design-condenser-water-flow-rate-5}
+
+The water flow rate at design conditions through the condenser in m\(^{3}\)/s. This field can be autosized. This field can be autosized. This field is not used for Condenser Type = AirCooled.
+
+\paragraph{Field: Design Hot Water Flow Rate}\label{field-design-hot-water-flow-rate}
+
+The water flow rate at design conditions through the heater side in m\(^{3}\)/s.
+
+\paragraph{Field: Cooling Capacity Function of Temperature Curve Name}\label{field-cooling-capacity-function-of-temperature-curve-name-2}
+
+The CoolCapfT curve represents the fraction of the cooling capacity of the chiller as it varies by temperature. The curve is normalized so that at design conditions the value of the curve should be 1.0. The curve is usually a biquadratic or bilinear curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature (see \emph{Temperature Curve Input Variable} below). The available cooling capacity is computed as follows:
+
+\begin{equation}
+\begin{array}{l}
+\rm{CoolFuelInput} = \\
+\rm{AvailCoolCap} \cdot \rm{RunFrac} \cdot \rm{CFIR} \cdot \rm{CFIRfT}( T_{cw,l}, {T_{\rm{cond}}}) \cdot \rm{CFIRfPLR}( \rm{CPLR} )
+\end{array}
+\end{equation}
+
+\paragraph{Field: Fuel Input to Cooling Output Ratio Function of Temperature Curve Name}\label{field-fuel-input-to-cooling-output-ratio-function-of-temperature-curve-name}
+
+The CFIRfT curve represents the fraction of the fuel input to the chiller at full load as it varies by temperature. The curve is normalized so that at design conditions the value of the curve should be 1.0. The curve is usually a biquadratic or bilinear curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature (see \emph{Temperature Curve Input Variable} below).
+
+\paragraph{Field: Fuel Input to Cooling Output Ratio Function of Part Load Ratio Curve Name}\label{field-fuel-input-to-cooling-output-ratio-function-of-part-load-ratio-curve-name}
+
+The CFIRfPLR curve represents the fraction of the fuel input to the chiller as the load the chiller varies but the operating temperatures remain at the design values. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic. The cooling fuel input to the chiller is computed as follows:
+
+\begin{equation}
+\begin{array}{l}
+\rm{CoolElectricPower} = \\
+\rm{NomCoolCap} \cdot \rm{RunFrac} \cdot \rm{CEIR} \cdot \rm{CEIRfT}(T_{cw,l}, T_{cond}) \cdot \rm{CEIRfPLR}(\rm{CPLR})
+\end{array}
+\end{equation}
+
+\paragraph{Field: Electric Input to Cooling Output Ratio Function of Temperature Curve Name}\label{field-electric-input-to-cooling-output-ratio-function-of-temperature-curve-name-2}
+
+The ElecCoolFT curve represents the fraction of the electricity to the chiller at full load as it varies by temperature. The curve is normalized so that at design conditions the of the curve should be 1.0. The curve is usually a biquadratic or bilinear~ curve with the input variables being the leaving chilled water temperature and either~ the entering or leaving condenser water temperature (see \emph{Temperature Curve Input Variable} below).
+
+\paragraph{Field: Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name}\label{field-electric-input-to-cooling-output-ratio-function-of-part-load-ratio-curve-name-2}
+
+The ElecCoolFPLR curve represents the fraction of the electricity to the chiller as the load on the chiller varies but This operating temperatures remain at the design values.~ The curve is normalized so that at full load the value of the curve should be 1.0.~ The curve is usually linear or quadratic. The cooling electric input to the chiller is computed as follows:
+
+\begin{equation}
+AvailHeatCap = NomCoolCap \cdot HeatCoolCapRatio \cdot HeatCapfCPLR(CPLRh)
+\end{equation}
+
+\paragraph{Field: Heating Capacity Function of Cooling Capacity Curve Name}\label{field-heating-capacity-function-of-cooling-capacity-curve-name}
+
+The HeatCapFCool curve represents how the heating capacity of the chiller varies with cooling capacity when the chiller is simultaeous heating and cooling. The curve is normalized so an input of 1.0 represents the nominal cooling capacity and an output of 1.0 represents the full heating capacity (see the Heating to Cooling Capacity Ratio input)~ The curve is usually linear or quadratic. The available heating capacity is computed as follows:
+
+\begin{equation}
+HeatFuelInput = AvailHeatCap \cdot HFIR \cdot HFIRfHPLR(HPLR)
+\end{equation}
+
+\paragraph{Field: Fuel Input to Heat Output Ratio During Heating Only Operation Curve Name}\label{field-fuel-input-to-heat-output-ratio-during-heating-only-operation-curve-name}
+
+When the chiller is operating as only a heater, the~ curve is used to represent the fraction of fuel used as the heating load varies. It is normalized so that a value of 1.0 is the full available heating capacity. The curve is usually linear or quadratic and will probably be similar to a boiler curve for most chillers.
+
+\begin{equation}
+AvailCoolCap = NomCoolCap \cdot CoolCapfT({T_{cw,l}},{T_{cond}})
+\end{equation}
+
+\paragraph{Field: Temperature Curve Input Variable}\label{field-temperature-curve-input-variable}
+
+This field sets the second independent variable in the three temperature dependent performance curves~ to either the leaving or entering condenser water temperature. Manufacturers express the performance of their chillers using either the leaving condenser water temperature (to~ the tower) or the entering condenser water temperature (from the tower). Valid choices for this field are: LeavingCondenser or EnteringCondenser. It is important that the performance curves and this field are consistent with each other. The default is EnteringCondenser.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-5-000}
+
+The condenser can either be air cooled or connected to a cooling tower. This alpha field contains the keyword for the type of condenser, either AirCooled, or WaterCooled. The default is WaterCooled.
+
+\paragraph{Field: Chilled Water Temperature Lower Limit}\label{field-chilled-water-temperature-lower-limit}
+
+The chilled water supply temperature in degrees C below which the chiller will shut off. The default is 2C.
+
+\paragraph{Field: Fuel Higher Heating Value}\label{field-fuel-higher-heating-value-2-000}
+
+The fuel higher heating value in kJ/kg. \emph{This field is not currently used}.
+
+\paragraph{Field: Chiller Flow Mode}\label{field-chiller-flow-mode-7}
+
+This field is deprecated and is not used.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-2-000}
+
+This alpha field determines the type of fuel that the chiller uses. The default is \textbf{NaturalGas}. Valid values are \textbf{NaturalGas}, \textbf{PropaneGas}, \textbf{Diesel}, \textbf{Gasoline}, \textbf{FuelOil\#1}, \textbf{FuelOil\#2, OtherFuel1, OtherFuel2}.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-8}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Cooling Capacity, Design Chilled Water Flow Rate, Design Condenser Water Flow Rate and Design Hot Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+ChillerHeater:Absorption:DirectFired,
+      Big Chiller,             !- Chiller Name
+      100000,                  !- Nominal Cooling Capacity {W}
+      0.8,                     !- Heating to Cooling capacity ratio
+      0.97,                    !- Fuel Input to Cooling Output Ratio
+      1.25,                    !- Fuel Input to Heating Output Ratio
+      0.01,                    !- Electric Input to Cooling Output Ratio
+      0.005,                   !- Electric Input to Heating Output Ratio
+      Big Chiller Inlet Node,  !- Chilled Water Side Inlet Node Name
+      Big Chiller Outlet Node, !- Chilled Water Side Outlet Node Name
+      Big Chiller Condenser Inlet Node,  !- Condenser Side Inlet Node Name
+      Big Chiller Condenser Outlet Node,  !- Condenser Side Outlet Node Name
+      Purchased Heat Inlet Node,  !- Hot Water Side Inlet Node Name
+      Purchased Heat Outlet Node,  !- Hot Water Side Outlet Node Name
+      0.000001,                !- Minimum Part Load Ratio
+      1.0,                     !- Maximum Part Load Ratio
+      0.6,                     !- Optimum Part Load Ratio
+      29,                      !- Design Entering Condenser Water Temperature {C}
+      7,                       !- Design Leaving Chilled Water Temperature {C}
+      0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
+      0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
+      0.0043,                  !- Design Hot Water Flow Rate {m3/s}
+      GasAbsFlatBiQuad,        !- Cooling Capacity Function of Temperature Curve Name
+      GasAbsFlatBiQuad,        !- Fuel Input to Cooling Output Ratio Function of Temperature Curve Name
+      GasAbsLinearQuad,        !- Fuel Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
+      GasAbsFlatBiQuad,        !- Electric Input to Cooling Output Ratio Function of Temperature Curve Name
+      GasAbsFlatQuad,      !- Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
+      GasAbsInvLinearQuad,     !- Heating Capacity Function of Cooling Capacity Curve Name
+      GasAbsLinearQuad,        !- Fuel Input to Heat Output Ratio During Heating Only Operation Curve Name
+      EnteringCondenser,       !- Temperature Curve Input Variable
+      WaterCooled,             !- Condenser Type
+      2,                       !- Chilled Water Temperature Lower Limit {C}
+      0,                       !- Fuel Higher Heating Value {kJ/kg}
+      VariableFlow,            !- Chiller Flow Mode
+      NaturalGas,              !- Fuel Type
+      1.0;                     !- Sizing Factor
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8-005}
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Electric Energy {[}J{]}
+\item
+  Zone,Meter,Electricity:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:Electricity {[}J{]}
+\item
+  HVAC,Average,Chiller \textless{}Fuel Type\textgreater{} Consumption Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller \textless{}Fuel Type\textgreater{} Consumption {[}J{]}
+\item
+  Zone,Meter,\textless{}Fuel Type\textgreater{}:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling:\textless{}Fuel Type\textgreater{} {[}J{]}
+\item
+  HVAC,Average,Chiller Evaporator Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Evaporator Cooling Energy {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Plant {[}J{]}
+\item
+  Zone,Meter,Chillers:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Evaporator Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Evaporator Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Evaporator Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Heater Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Meter,HeatRejection:EnergyTransfer {[}J{]}
+\end{itemize}
+
+The following output is applicable only for air-cooled chillers
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Chiller Heater Condenser Inlet Temperature {[}C{]}
+\end{itemize}
+
+The following three outputs are only available for water-cooled chillers
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Heater Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Condenser Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+Outputs specific to Direct Fired Absorption Chiller
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Chiller Heater Runtime Fraction {[]}
+\end{itemize}
+
+Outputs specific to Direct Fired Absorption Chiller during cooling operation
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Heater Cooling \textless{}Fuel Type\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Cooling \textless{}Fuel Type\textgreater{} Consumption {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Cooling Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Cooling Electric Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Cooling Part Load Ratio
+\item
+  HVAC,Average,Chiller Heater Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Chiller Heater Cooling COP {[}W/W{]}
+\end{itemize}
+
+Outputs specific to Direct Fired Absorption Chiller during heating operation
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Heater Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Heating Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Heating \textless{}Fuel Type\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Heating \textless{}Fuel Type\textgreater{} Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Heating Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Heating Electric Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Heating Part Load Ratio {[]}
+\item
+  HVAC,Average,Chiller Heater Heating Rate {[}W{]}
+\item
+  HVAC,Average,Chiller Heater Heating Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Heating Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Heating Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+The ``Chiller'' output variables are defined above under ``Generic Chiller Outputs.''~ The specific ``Direct Fired Absorption Chiller'' output variables and exceptions to the generic outputs are defined below.
+
+\paragraph{Chiller Heater Electric Power {[}W{]}}\label{chiller-heater-electric-power-w}
+
+\paragraph{Chiller Heater Electric Energy {[}J{]}}\label{chiller-heater-electric-energy-j}
+
+These outputs are the electric power input to the chiller when operating in cooling mode, heating mode, or both. This value is not metered, but the separate cooling and heating electric consumption are metered (see below).
+
+\paragraph{Chiller Heater \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{chiller-heater-fuel-type-rate-w}
+
+\paragraph{Chiller Heater \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{chiller-heater-fuel-type-energy-j}
+
+These outputs are the fuel input to the chiller when operating in cooling mode, heating mode, or both depending on the fuel type entered. This value is not metered, but the separate cooling and heating fuel consumption are metered (see below).
+
+\paragraph{\texorpdfstring{Chiller Heater Runtime Fraction {[]}}{Chiller Heater Runtime Fraction }}\label{chiller-heater-runtime-fraction}
+
+This is the average fraction of the time period during which the direct fired absorption chiller-heater was operating in either cooling mode, heating mode, or both.
+
+\paragraph{Chiller Heater Cooling \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{chiller-heater-cooling-fuel-type-rate-w}
+
+\paragraph{Chiller Heater Cooling \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{chiller-heater-cooling-fuel-type-energy-j}
+
+These outputs are the fuel input to the direct fired absorption chiller to serve cooling operation. Consumption is metered on Cooling:\textless{}Fuel Type\textgreater{}, \textless{}Fuel Type\textgreater{}:Plant, and \textless{}Fuel Type\textgreater{}:Facility.
+
+\paragraph{Chiller Heater Cooling Electric Power {[}W{]}}\label{chiller-heater-cooling-electric-power-w}
+
+\paragraph{Chiller Heater Cooling Electric Energy {[}J{]}}\label{chiller-heater-cooling-electric-energy-j}
+
+These outputs are the electricity input to the direct fired absorption chiller to serve cooling operation. Consumption is metered on Cooling:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Chiller Heater Cooling Rate {[}W{]}}\label{chiller-heater-cooling-rate-w}
+
+This is the average available cooling capacity for the reported time period.
+
+\paragraph{Chiller Heater Cooling Part Load Ratio}\label{chiller-heater-cooling-part-load-ratio}
+
+This is the average cooling load (Chiller Evaporator Cooling Rate {[}W{]}) divided by the average available cooling capacity (Chiller Heater Cooling Rate {[}W{]}) for the reported time period.
+
+\paragraph{Chiller Heater Cooling COP}\label{chiller-heater-cooling-cop}
+
+This is the average coefficient of performance for the chiller in cooling operation, calculated as the average cooling load (Chiller Evaporator Cooling Rate {[}W{]}) divided by the average fuel consumption during cooling (Direct Fired Absorption Chiller Cooling \textless{}Fuel Type\textgreater{} Consumption Rate {[}W{]}) for the reported time period. If the chiller cooling fuel consumption rate (denominator) is zero, then this output variable is set to zero.
+
+\paragraph{Chiller Heater Heating Rate {[}W{]}}\label{chiller-heater-heating-rate-w}
+
+\paragraph{Chiller Heater Heating Energy {[}J{]}}\label{chiller-heater-heating-energy-j}
+
+These outputs are the heating delivered by the direct fired absorption chiller-heater to serve heating operation. Energy is metered on Boilers:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\paragraph{Chiller Heater Heating \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{chiller-heater-heating-fuel-type-rate-w}
+
+\paragraph{Chiller Heater Heating \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{chiller-heater-heating-fuel-type-energy-j}
+
+These outputs are the fuel input to the direct fired absorption chiller-heater to serve heating operation. Consumption is metered on Heating:\textless{}Fuel Type\textgreater{}, \textless{}Fuel Type\textgreater{}:Plant, and \textless{}Fuel Type\textgreater{}:Facility.
+
+\paragraph{Chiller Heater Heating Electric Power {[}W{]}}\label{chiller-heater-heating-electric-power-w}
+
+\paragraph{Chiller Heating Heating Electric Energy {[}J{]}}\label{chiller-heating-heating-electric-energy-j}
+
+These outputs are the electric power input to the direct fired absorption chiller to serve heating operation. Consumption is metered on Heating:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Chiller Heater Heating Rate {[}W{]}}\label{chiller-heater-heating-rate-w-1}
+
+This is the average available heating capacity for the reported time period.
+
+\paragraph{Chiller Heater Heating Part Load Ratio}\label{chiller-heater-heating-part-load-ratio}
+
+This is the average heating load (Chiller Heater Heating Rate {[}W{]}) divided by the average available heating capacity (Chiller Heater Heating Rate {[}W{]}) for the reported time period.
+
+\paragraph{Chiller Heater Heating Inlet Temperature {[}C{]}}\label{chiller-heater-heating-inlet-temperature-c}
+
+\paragraph{Chiller Heater Heating Outlet Temperature {[}C{]}}\label{chiller-heater-heating-outlet-temperature-c}
+
+\paragraph{Chiller Heater Heating Mass Flow Rate {[}kg/s{]}}\label{chiller-heater-heating-mass-flow-rate-kgs}
+
+These outputs are the hot water inlet and outlet temperatures and flow rate for the direct fired absorption chiller-heater during heating mode operation.
+
+\subsection{ChillerHeater:Absorption:DoubleEffect}\label{chillerheaterabsorptiondoubleeffect}
+
+This chiller is an exhaust fired absorption chiller-heater which is modeled using performance curves similar to the direct fired absorption chiller in DOE-2.1E. The model uses the exhaust gas output from MicroTurbine. This type of chiller is unusual for EnergyPlus, because it may be used in the same plant on both a chilled water supply branch and a hot water supply branch. The chiller has six node connections for chilled water, condenser water, and hot water, and can provide simultaneous heating and cooling. During simultaneous operation, the heating capacity is reduced as the cooling load increases (for more details see below). Some equations are provided below to help explain the function of the various performance curves. For a detailed description of the algorithm and how the curves are used in the calculations, please see the Engineering Reference.
+
+\subsubsection{Inputs}\label{inputs-9-014}
+
+\paragraph{Field: Name}\label{field-name-8-014}
+
+This alpha field contains the identifying name for the chiller.
+
+\paragraph{Field: Nominal Cooling Capacity}\label{field-nominal-cooling-capacity-1}
+
+This numeric field contains the nominal cooling capability of the chiller in Watts. Autosize can be used for this field.
+
+\paragraph{Field: Heating to Cooling Capacity Ratio}\label{field-heating-to-cooling-capacity-ratio-1}
+
+A positive fraction that represents the ratio of the heating capacity divided by the cooling capacity at rated conditions. The default is 0.8.
+
+\paragraph{Field: Thermal Energy Input to Cooling Output Ratio}\label{field-thermal-energy-input-to-cooling-output-ratio}
+
+A positive fraction that represents the ratio of the instantaneous cooling Thermal Energy used divided by the cooling capacity at rated conditions. The default is 0.97.
+
+\paragraph{Field: Thermal Energy Input to Heating Output Ratio}\label{field-thermal-energy-input-to-heating-output-ratio}
+
+A positive fraction that represents the ratio of the instantaneous heating Thermal Energy used divided by the nominal heating capacity. The default is 1.25.
+
+\paragraph{Field: Electric Input to Cooling Output Ratio}\label{field-electric-input-to-cooling-output-ratio-1}
+
+A positive fraction that represents the ratio of the instantaneous electricity used divided by the cooling capacity at rated conditions. If the chiller is both heating and cooling only the greater of the computed cooling and heating electricity is used. The default is 0.01.
+
+\paragraph{Field: Electric Input to Heating Output Ratio}\label{field-electric-input-to-heating-output-ratio-1}
+
+A positive fraction that represents the ratio of the instantaneous electricity used divided by the nominal heating capacity. If the chiller is both heating and cooling, the greater of the cooling electricity and heating eletricity is used. The default is 0.0.
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-8}
+
+This required alpha field contains the identifying name for the chiller chilled water side inlet node. This node name must be the same as the inlet node name for the chilled water supply branch on which this chiller is placed.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-9}
+
+This required alpha field contains the identifying name for the chiller chilled water side outlet node.
+
+\paragraph{Field: Condenser Inlet Node Name}\label{field-condenser-inlet-node-name-8}
+
+This required alpha field contains the identifying name for the chiller condenser side inlet node. If the Chiller is AirCooled, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air dry-bulb temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air dry-bulb temperature is taken directly from the weather data.
+
+\paragraph{Field: Condenser Outlet Node Name}\label{field-condenser-outlet-node-name-8}
+
+This required alpha field contains the identifying name for the chiller condenser side outlet node.
+
+\paragraph{Field: Hot Water Inlet Node Name}\label{field-hot-water-inlet-node-name-1}
+
+This required alpha field contains the identifying name for the chiller-heater hot water side inlet node. This node name must be the same as the inlet node name for the hot water supply branch on which this chiller-heater is placed.
+
+\paragraph{Field: Hot Water Outlet Node Name}\label{field-hot-water-outlet-node-name-1}
+
+This required alpha field contains the identifying name for the chiller-heater hot water side outlet node.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-8}
+
+A positive fraction that represents the minimum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. If the load on the chiller is below this fraction, the chiller will cycle. If the chiller is simultaneously heating and cooling, the greater part load ratio will be used. The default is 0.1.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-8}
+
+A positive fraction that represents the maximum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. If greater than 1.0, the chiller is typically thought of as capable of being overloaded. The default is 1.0.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-8}
+
+A positive fraction that represents the optimum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. It represents the most desirable operating point for the chiller. The default is 1.0.
+
+\paragraph{Field: Design Entering Condenser Water Temperature}\label{field-design-entering-condenser-water-temperature-1}
+
+The temperature in degrees C of the water entering the condenser of the chiller when operating at design conditions. This is usually based on the temperature delivered by the cooling tower in a water cooled application. The default is 29°C.
+
+\paragraph{Field: Design Leaving Chilled Water Temperature}\label{field-design-leaving-chilled-water-temperature-1}
+
+The temperature in degrees C of the water leaving the evaporator of the chiller when operating at design conditions; also called the chilled water supply temperature or leaving chilled water temperature. The default is 7°C.
+
+\paragraph{Field: Design Chilled Water Flow Rate}\label{field-design-chilled-water-flow-rate-7}
+
+For variable volume this is the max flow and for constant flow this is the chilled water flow rate in m\(^{3}\)/s. This field can be autosized.
+
+\paragraph{Field: Design Condenser Water Flow Rate}\label{field-design-condenser-water-flow-rate-6}
+
+The water flow rate at design conditions through the condenser in m\(^{3}\)/s. This field can be autosized. This field is not used for Condenser Type = AirCooled.
+
+\paragraph{Field: Design Hot Water Flow Rate}\label{field-design-hot-water-flow-rate-1}
+
+The water flow rate at design conditions through the heater side in m\(^{3}\)/s. This field can be autosized.
+
+\paragraph{Field: Cooling Capacity Function of Temperature Curve Name}\label{field-cooling-capacity-function-of-temperature-curve-name-3}
+
+The CoolCapfT curve represents the fraction of the cooling capacity of the chiller as it varies with temperature. The curve is normalized so that at design conditions the value of the curve should be 1.0. The curve is usually a biquadratic or bilinear curve with the input variables being the leaving chilled water temperature and the entering condenser water temperature (see \emph{Temperature Curve Input Variable} below). The available cooling capacity is computed as follows:
+
+\begin{equation}
+\begin{array}{l}
+\rm{CoolThermalEnergyInput} = \rm{AvailCoolCap} \cdot \rm{RunFrac} \cdot \rm{TeFIR} \cdot \\
+\quad \quad \quad \quad \quad \quad \rm{TeFIRfT} \left( T_{cw,l}, T_{cond} \right) \cdot \rm{TeFIRfPLR}( \rm{CPLR} )
+\end{array}
+\end{equation}
+
+\paragraph{Field: Thermal Energy Input to Cooling Output Ratio Function of Temperature Curve Name}\label{field-thermal-energy-input-to-cooling-output-ratio-function-of-temperature-curve-name}
+
+The TeFIRfT curve represents the fraction of the Thermal Energy Input to the chiller at full load as it varies with temperature. The curve is normalized so that at design conditions the value of the curve should be 1.0. The curve is usually a biquadratic or bilinear curve with the input variables being the leaving chilled water temperature and the entering condenser water temperature (see \emph{Temperature Curve Input Variable} below).
+
+\paragraph{Field: Thermal Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve Name}\label{field-thermal-energy-input-to-cooling-output-ratio-function-of-part-load-ratio-curve-name}
+
+The TeFIRfPLR curve represents the fraction of the Thermal Energy Input to the chiller as the load on the chiller varies but the operating temperatures remain at the design values. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic.
+
+The cooling Thermal Energy Input to the chiller is computed as follows:
+
+\begin{equation}
+CoolElectricPower = NomCoolCap \cdot RunFrac \cdot CEIR \cdot CEIRfT\left( {{T_{cw,l}},{T_{cond}}} \right) \cdot CEIRfPLR(CPLR)
+\end{equation}
+
+\paragraph{Field: Electric Input to Cooling Output Ratio Function of Temperature Curve Name}\label{field-electric-input-to-cooling-output-ratio-function-of-temperature-curve-name-3}
+
+The CEIRfT curve represents the fraction of the electricity to the chiller at full load as it varies with temperature. The curve is normalized so that at design conditions the of the curve should be 1.0. The curve is usually a biquadratic or bilinear~ curve with the input variables being the leaving chilled water temperature and either~ the entering or leaving condenser water temperature (see \emph{Temperature Curve Input Variable} below).
+
+\paragraph{Field: Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name}\label{field-electric-input-to-cooling-output-ratio-function-of-part-load-ratio-curve-name-3}
+
+The CEIRfPLR curve represents the fraction of the electricity to the chiller as the load on the chiller varies but This operating temperatures remain at the design values.~ The curve is normalized so that at full load the value of the curve should be 1.0.~ The curve is usually linear or quadratic.
+
+The cooling electric input to the chiller is computed as follows:
+
+\begin{equation}
+AvailHeatCap = NomCoolCap \cdot HeatCoolCapRatio \cdot HeatCapfCPLR(CPLRh)
+\end{equation}
+
+\paragraph{Field: Heating Capacity Function of Cooling Capacity Curve Name}\label{field-heating-capacity-function-of-cooling-capacity-curve-name-1}
+
+The HeatCapFCPLR curve represents how the heating capacity of the chiller varies with cooling capacity when the chiller is simultaneously heating and cooling. The curve is normalized so an input of 1.0 represents the nominal cooling capacity and an output of 1.0 represents the full heating capacity (see the Heating to Cooling Capacity Ratio input)~ The curve is usually linear or quadratic.
+
+The available heating capacity is computed as follows:
+
+\begin{equation}
+HeatThermalEnergyInput = AvailHeatCap \cdot HFIR \cdot HFIRfHPLR(HPLR)
+\end{equation}
+
+\paragraph{Field: Thermal Energy Input to Heat Output Ratio During Heating Only Operation Curve Name}\label{field-thermal-energy-input-to-heat-output-ratio-during-heating-only-operation-curve-name}
+
+When the chiller is operating as only a heater, the~ curve is used to represent the fraction of Thermal Energy used as the heating load varies. It is normalized so that a value of 1.0 is the full available heating capacity. The curve is usually linear or quadratic and will probably be similar to a boiler curve for most chillers.
+
+The heating Thermal Energy Input to the chiller is computed as follows:
+
+\begin{equation}
+TheoreticalFuelUse = \frac{{BoilerLoad}}{{NominalThermalEfficiency}}
+\end{equation}
+
+\paragraph{Field: Temperature Curve Input Variable}\label{field-temperature-curve-input-variable-1}
+
+This field sets the second independent variable in the three temperature dependent performance curves~ to the entering condenser water temperature. Manufacturers express the performance of their chillers typically using the entering condenser water temperature (from the tower). ). This alpha field contains the keyword for the type of temperature input variable, , either \textbf{EnteringCondenserTemperature}, or \textbf{LeavingCondenserTemperature}. The default is EnteringCondenserTemperature.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-6}
+
+The condenser can either be air cooled or water cooled (connected to a cooling tower). This alpha field contains the keyword for the type of condenser, either AirCooled, or WaterCooled. The default is WaterCooled.
+
+\paragraph{Field: Chilled Water Temperature Lower Limit}\label{field-chilled-water-temperature-lower-limit-1}
+
+The chilled water supply temperature in degrees C below which the chiller will shut off. The default is 2°C.
+
+\paragraph{Field: Exhaust Source}\label{field-exhaust-source}
+
+This alpha field determines the type of exhaust source the chiller uses. The default is MicroTurbine. Key Generator:MicroTurbine
+
+\paragraph{Field: Exhaust Source Object}\label{field-exhaust-source-object}
+
+This alpha field shows the name of the Exhaust source object -- a Generator:MicroTurbine in this case
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-9}
+
+This optional numeric field allows the user to specify a sizing factor for this component. Min value should not be less than 0 and here is no max. The default is 1.~ The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Cooling Capacity, Design Chilled Water Flow Rate, Design Condenser Water Flow Rate and Design Hot Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+ChillerHeater:Absorption:DoubleEffect,
+      Exh Chiller,             !- Chiller Name
+      100000,                  !- Nominal Cooling Capacity {W}
+      0.8,                     !- Heating to Cooling capacity ratio
+      0.97,                    !- Thermal Energy Input to Cooling Output Ratio
+      1.25,                    !- Thermal Energy Input to Heating Output Ratio
+      0.01,                    !- Electric Input to Cooling Output Ratio
+      0.005,                   !- Electric Input to Heating Output Ratio
+      Exh Chiller Inlet Node,  !- Chilled Water Side Inlet Node Name
+      Exh Chiller Outlet Node, !- Chilled Water Side Outlet Node Name
+      Exh Chiller Condenser Inlet Node,  !- Condenser Side Inlet Node Name
+      Exh Chiller Condenser Outlet Node,  !- Condenser Side Outlet Node Name
+      Exh Chiller Heating Inlet Node,  !- Hot Water Side Inlet Node Name
+      Exh Chiller Heating Outlet Node,  !- Hot Water Side Outlet Node Name
+      0.000001,                !- Minimum Part Load Ratio
+      1.0,                     !- Maximum Part Load Ratio
+      0.6,                     !- Optimum Part Load Ratio
+      29,                      !- Design Entering Condenser Water Temperature {C}
+      7,                       !- Design Leaving Chilled Water Temperature {C}
+      0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
+      0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
+      0.0043,                  !- Design Hot Water Flow Rate {m3/s}
+       ExhAbsorb_CapFt,        !- Cooling Capacity Function of Temperature Curve Name
+      ExhAbsorb_EIRFt,         !- Thermal Energy Input to Cooling Output Ratio Function of Temperature Curve Name
+       ExhAbsorb_PLR,        !- Thermal Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
+      ExhAbsFlatBiQuad,        !- Electric Input to Cooling Output Ratio Function of Temperature Curve Name
+      ExhAbsFlatQuad,      !- Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
+      ExhAbsInvLinearQuad,     !- Heating Capacity Function of Cooling Capacity Curve Name
+      ExhAbsLinearQuad,        !- Thermal Energy Input to Heat Output Ratio During Heating Only Operation Curve Name
+      EnteringCondenser,       !- Temperature Curve Input Variable
+      WaterCooled,             !- Condenser Type
+      2,                       !- Chilled Water Temperature Lower Limit {C}
+      Generator:MicroTurbine ; ! Field Exhaust Source Object Type
+  Capston500 ;                ! Field Exhaust Source name
+  1.0;                       !- Sizing Factor
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-9-005}
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Evaporator Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Evaporator Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Evaporator Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Evaporator Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Evaporator Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Heater Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Condenser Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+The following output is applicable only for air-cooled chillers
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Chiller Heater Condenser Inlet Temperature {[}C{]}
+\end{itemize}
+
+The following three outputs are only available for water-cooled chillers
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Heater Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Condenser Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+Outputs specific to Exhaust Fired Absorption Chiller
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Chiller Heater Runtime Fraction {[]}
+\end{itemize}
+
+Outputs specific to Exhaust Fired Absorption Chiller during cooling operation
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Heater Cooling Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Cooling Electric Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Cooling Part Load Ratio
+\item
+  HVAC,Average,Chiller Heater Maximum Cooling Rate {[}W{]}HVAC,Average,Chiller Heater Cooling Source Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average, Chiller Heater Cooling Source Heat COP {[}W/W{]}
+\item
+  HVAC,Average, Chiller Heater Source Exhaust Inlet Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average, Chiller Heater Source Exhaust Inlet Temperature {[}C{]}
+\end{itemize}
+
+Outputs specific to Exhaust Fired Absorption Chiller during heating operation
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Heater Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Heating Energy {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Heating Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Heating Electric Energy {[}J{]}
+\item
+  Zone,Meter,Heating:Electricity {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Heating Part Load Ratio
+\item
+  HVAC,Average,Chiller Heater Maximum Heating Rate {[}W{]}
+\item
+  HVAC,Average,Chiller Heater Heating Source Heat Transfer Rate
+\item
+  HVAC,Average,Chiller Heater Heating Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Heating Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Heating Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+The ``Chiller'' output variables are defined above under ``Generic Chiller Outputs.''~ The specific ``Exhaust Fired Absorption Chiller'' output variables and exceptions to the generic outputs are defined below.
+
+\paragraph{Chiller Heater Electric Power {[}W{]}}\label{chiller-heater-electric-power-w-1}
+
+\paragraph{Chiller Heater Electric Energy {[}J{]}}\label{chiller-heater-electric-energy-j-1}
+
+These outputs are the electric power input to the chiller when operating in cooling mode, heating mode, or both. This value is not metered, but the separate cooling and heating electric consumption are metered (see below).
+
+\paragraph{\texorpdfstring{Chiller Heater Runtime Fraction {[]}}{Chiller Heater Runtime Fraction }}\label{chiller-heater-runtime-fraction-1}
+
+This is the average fraction of the time period during which the Exhaust Fired absorption chiller-heater was operating in either cooling mode, heating mode, or both.
+
+These outputs are the electricity input to the Exhaust Fired absorption chiller heater to serve cooling operation. Consumption is metered on Cooling:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Chiller Heater Maximum Cooling Rate {[}W{]}}\label{chiller-heater-maximum-cooling-rate-w}
+
+This is the average available cooling capacity for the reported time period.
+
+\paragraph{\texorpdfstring{Chiller Heater Cooling Part Load Ratio {[]}}{Chiller Heater Cooling Part Load Ratio }}\label{chiller-heater-cooling-part-load-ratio-1}
+
+This is the average cooling load (Chiller Heater Evaporator Cooling Rate {[}W{]}) divided by the average available cooling capacity (Chiller Heater Maximum Cooling Rate {[}W{]}) for the reported time period.
+
+\paragraph{Chiller Heater Cooling Source Heat COP {[}W/W{]}}\label{chiller-heater-cooling-source-heat-cop-ww}
+
+This is the average coefficient of performance for the chiller in cooling operation, calculated as the average cooling load (Chiller Heater Evaporator Cooling Rate {[}W{]}) divided by the average thermal energy use during cooling (Chiller Heater Cooling Source Heat Transfer Rate {[}W{]}) for the reported time period. If the chiller cooling thermal energy use rate (denominator) is zero, then this output variable is set to zero.
+
+\paragraph{Chiller Heater Heating Rate {[}W{]}}\label{chiller-heater-heating-rate-w-2}
+
+\paragraph{Chiller Heater Heating Energy {[}J{]}}\label{chiller-heater-heating-energy-j-1}
+
+\paragraph{Chiller Heater Heating Electric Power {[}W{]}}\label{chiller-heater-heating-electric-power-w-1}
+
+\paragraph{Chiller Heater Heating Electric Energy {[}J{]}}\label{chiller-heater-heating-electric-energy-j}
+
+These outputs are the electric power input to the Exhaust Fired absorption chiller to serve heating operation. Consumption is metered on Heating:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Chiller Heater Maximum Heating Rate {[}W{]}}\label{chiller-heater-maximum-heating-rate-w}
+
+This is the average available heating capacity for the reported time period.
+
+\paragraph{\texorpdfstring{Chiller Heater Heating Part Load Ratio {[]}}{Chiller Heater Heating Part Load Ratio }}\label{chiller-heater-heating-part-load-ratio-1}
+
+This is the average heating load (Chiller Heater Heating Rate {[}W{]}) divided by the average available heating capacity (Chiller Heater Maximum Heating Rate {[}W{]}) for the reported time period.
+
+\paragraph{Chiller Heater Heating Inlet Temperature {[}C{]}}\label{chiller-heater-heating-inlet-temperature-c-1}
+
+\paragraph{Chiller Heater Heating Outlet Temperature {[}C{]}}\label{chiller-heater-heating-outlet-temperature-c-1}
+
+\paragraph{Chiller Heater Heating Mass Flow Rate {[}kg/s{]}}\label{chiller-heater-heating-mass-flow-rate-kgs-1}
+
+These outputs are the hot water inlet and outlet temperatures and flow rate for the Exhaust Fired absorption chiller-heater during heating mode operation.
+
+\paragraph{Chiller Heater Heating Heat Recovery Potential Rate (W)}\label{chiller-heater-heating-heat-recovery-potential-rate-w}
+
+The heat recovery potential calculated based on Microturbine exhaust temperature and flow rate during heating mode
+
+\paragraph{Chiller Heater Heating Source Heat Transfer Rate (W)}\label{chiller-heater-heating-source-heat-transfer-rate-w}
+
+The thermal energy consumption rate required~ for heating.
+
+\paragraph{Chiller Heater Cooling Heat Recovery Potential Rate (W)}\label{chiller-heater-cooling-heat-recovery-potential-rate-w}
+
+The heat recovery potential calculated based on Microturbine exhaust temperature and flow rate during cooling mode.
+
+\paragraph{Chiller Heater Cooling Source Heat Transfer Rate (W)}\label{chiller-heater-cooling-source-heat-transfer-rate-w}
+
+The thermal energy consumption rate required for cooling.
+
+\paragraph{Chiller Heater Condenser Inlet Temperature {[}C{]}}\label{chiller-heater-condenser-inlet-temperature-c}
+
+The condenser (heat rejection) inlet temperature for air-cooled or water chiller heater. For an air-cooled chiller heater, this output would be the dry-bulb temperature of the air entering the condenser coil. For a water cooled chiller heater, this output would be the wet-bulb temperature of the air entering the condenser coil.
+
+\paragraph{Chiller Heater Condenser Heat Transfer Energy {[}J{]}}\label{chiller-heater-condenser-heat-transfer-energy-j}
+
+The condenser heat transfer energy is the heat rejected from the chiller heater to either a condenser water loop or through an air-cooled condenser. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period. Chiller Heater Condenser Heat Transfer Energy is metered on HeatRejection:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\paragraph{Chiller Heater Condenser Heat Transfer Rate {[}W{]}}\label{chiller-heater-condenser-heat-transfer-rate-w}
+
+The condenser heat transfer is the rate of heat rejected from the chiller heater to either a condenser water loop or through an air-cooled condenser. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Chiller Heater Condenser Mass Flow Rate {[}kg/s{]}}\label{chiller-heater-condenser-mass-flow-rate-kgs}
+
+This is the condenser coil outlet water mass flow rate in kilograms per second. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Chiller Heater Condenser Outlet Temperature {[}C{]}}\label{chiller-heater-condenser-outlet-temperature-c}
+
+This is the condenser coil outlet water temperature in degrees C. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported
+
+\paragraph{Chiller Heater Evaporator Cooling Energy {[}J{]}}\label{chiller-heater-evaporator-cooling-energy-j}
+
+The evaporator heat transfer is the cooling delivered by the chiller heater. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period. Chiller Heater Evaporator Cooling Energy is metered on Chillers:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\paragraph{Chiller Heater Evaporator Cooling Rate {[}W{]}}\label{chiller-heater-evaporator-cooling-rate-w}
+
+The evaporator heat transfer rate of cooling delivered by the chiller heater. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Chiller Heater Evaporator Inlet Temperature {[}C{]}}\label{chiller-heater-evaporator-inlet-temperature-c}
+
+The evaporator (chilled water) inlet temperature over the time step being reported.
+
+\paragraph{Chiller Heater Evaporator Mass Flow Rate {[}kg/s{]}}\label{chiller-heater-evaporator-mass-flow-rate-kgs}
+
+The evaporator (chilled water) average mass flow rate over the time step being reported
+
+\paragraph{Chiller Heater Evaporator Outlet Temperature {[}C{]}}\label{chiller-heater-evaporator-outlet-temperature-c}
+
+The evaporator (chilled water) outlet temperature over the time step being reported
+
+\paragraph{Chiller Heater Cooling Electric Energy {[}J{]}}\label{chiller-heater-cooling-electric-energy-j-1}
+
+The electric power input to the exhaust fired absorption chiller to serve cooling operation. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period. Consumption is metered on Heating:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Chiller Heater Cooling Electric Power {[}W{]}}\label{chiller-heater-cooling-electric-power-w-1}
+
+The electric power input to the Exhaust Fired absorption chiller to serve cooling operation. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Chiller Heater Source Exhaust Inlet Mass Flow Rate {[}kg/s{]}}\label{chiller-heater-source-exhaust-inlet-mass-flow-rate-kgs}
+
+The exhaust flow rate from the Micro Turbine
+
+\paragraph{Chiller Heater Source Exhaust Inlet Temperature {[}C{]}}\label{chiller-heater-source-exhaust-inlet-temperature-c}
+
+The exhaust temperature from~ the Micro Turbine
+
+\subsection{Boiler:HotWater}\label{boilerhotwater}
+
+The boiler model calculates the performance of fuel oil, gas and electric boilers. Boiler performance is based on nominal thermal efficiency. A normailized efficiency performance curve may be used to more accurately represent the performance of non-electric boilers but is not considered a required input. When using the normalized efficiency performance curve, if all coefficients are not required simply set the unused coefficients to 0. For example, an electric boiler could be modeled by setting the nominal thermal efficiency to a value in the range of 0.96 to 1.0. Coefficient A0 in the normalized efficiency performance curve would equal 1 and all other coefficients would be set to 0. Coefficients for other types of non-electric boilers would set a combination of the available coefficents to non-zero values.
+
+\subsubsection{Inputs}\label{inputs-10-013}
+
+\paragraph{Field: Name}\label{field-name-9-012}
+
+This required alpha field contains the identifying name for the boiler.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-3-000}
+
+This required choice field specifies the type of fuel used by the boiler. The fuel type can be \textbf{Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1} or \textbf{OtherFuel2}.
+
+\paragraph{Field: Nominal capacity}\label{field-nominal-capacity-6}
+
+This numeric field contains the nominal operating capacity (W) of the boiler. The boiler may be autosized and would require a heating plant sizing object.
+
+\paragraph{Fuel Use Equation}\label{fuel-use-equation}
+
+The model is based the following two equations:
+
+\begin{equation}
+FuelUsed = \frac{{TheoreticalFuelUse}}{{NormalizedBoilerEfficiencyCurveOutput}}
+\end{equation}
+
+\begin{equation}
+Linear \to Eff = {A_0} + {A_1}\cdot PLR
+\end{equation}
+
+\paragraph{Field: Nominal Thermal Efficiency}\label{field-nominal-thermal-efficiency}
+
+This required numeric field contains the heating efficiency (as a fraction between 0 and 1) of the boiler's burner.~ This is the efficiency relative to the higher heating value (HHV) of fuel at a part load ratio of 1.0 and the temperature entered for the Design Boiler Water Outlet Temp. Manufacturers typically specify the efficiency of a boiler using the higher heating value of the fuel. For the rare occurences when a manufacturers (or particular data set) thermal efficiency is based on the lower heating value (LHV) of the fuel, multiply the thermal efficiency by the lower-to-higher heating value ratio. For example, assume a fuel's lower and higher heating values are approximately 45,450 and 50,000 kJ/kg, respectively. For a manuracturers thermal effiency rating of 0.90 (based on the LHV), the nominal thermal efficiency entered here is 0.82 (i.e.~0.9 multiplied by 45,450/50,000).
+
+\paragraph{Field: Efficiency Curve Temperature Evaluation Variable}\label{field-efficiency-curve-temperature-evaluation-variable}
+
+This field is used to control which value for hot water temperature is used when evaluating the efficiency curve specified in the next field (if applicable).~ There are two options,~ EnteringBoiler or LeavingBoiler.~ EnteringBoiler indicates that the efficiency curves will be evaluated using the temperature at boiler inlet node.~ LeavingBoiler indicates that the efficiency curves will be evaluated using the temperature at the boiler outlet.~ This field is only used if type of curve is one that uses temperature as a independent variable.
+
+\paragraph{Field: Normalized Boiler Efficiency Curve Name}\label{field-normalized-boiler-efficiency-curve-name}
+
+This alpha field contains the curve name which describes the normalized heating efficiency (as a fraction of nominal thermal efficiency) of the boiler's burner. If this field is left blank, the nominal thermal efficiency is assumed to be constant (i.e., Fuel Used is equal to the Theoretical Fuel Use in the equation above). When a boiler efficiency curve is used, the curve may be any valid curve object with 1 (PLR) or 2 (PLR and boiler outlet water temperature) independent variables. A tri-quadratic curve object is not allowed since it uses 3 independent variables. The linear, quadratic, and cubic curve types may be used when the boiler efficiency is solely a function of boiler part-load ratio (PLR). When this type of curve is used, the boiler should operate at (or very near) the design boiler water outlet temperature. Other curve types may be used when the boiler efficiency is a function of both PLR and boiler water temperature. Examples of valid single and dual independent variable equations are shown below. For all curve types PLR is always the x independent variable. When using 2 independent variables, the boiler outlet water temperature (Toutlet) is always the y independent variable.
+
+\begin{equation}
+Quadratic \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2}
+\end{equation}
+
+\begin{equation}
+Cubic \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2} + {A_3}\cdot PL{R^3}
+\end{equation}
+
+\begin{equation}
+Cubic \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2} + {A_3}\cdot PL{R^3}
+\end{equation}
+
+\begin{equation}
+BiQuadratic \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2} + {A_3}\cdot {T_w} + {A_4}\cdot {T_w}^2 + {A_5}\cdot PLR\cdot {T_w}
+\end{equation}
+
+\begin{equation}
+QuadraticLinear \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2} + {A_3}\cdot {T_w} + {A_4}\cdot PLR\cdot {T_w} + {A_5}\cdot PL{R^2}\cdot {T_w}
+\end{equation}
+
+\begin{equation}
+\begin{array}{l}
+  \rm{Bicubic} \to \rm{Eff} = A_0 + A_1 \cdot \rm{PLR} + A_2 \cdot \rm{PLR}^2 + A_3 \cdot T_w + A_4 T_w^2 + A_5 \rm{PLR} \cdot T_w + A_6 \rm{PLR}^3 \\
+  \quad \quad \quad \quad \quad \quad \quad  + A_7 \cdot T_w^3 + A_8 \cdot \rm{PLR}^2 \cdot T_w + A_9 \cdot \rm{PLR} \cdot T_w^2
+\end{array}
+\end{equation}
+
+where
+
+Eff = normalized boiler efficiency
+
+PLR = boiler part-load ratio
+
+T\(_{w}\) = boiler water temperature {[}ºC{]} {]}, this can be either entering or leaving temperature depending on the setting in the previous field
+
+\paragraph{Field: Design Water Outlet Temperature}\label{field-design-water-outlet-temperature}
+
+This numeric field contains the desired boiler water outlet temperature in Celsius.
+
+\paragraph{Field: Design Water Flow Rate}\label{field-design-water-flow-rate-001}
+
+This numeric field contains the maximum design water volumetric flow rate in m\(^{3}\)/sec.~This should be the largest flow rate than can be heated to the design outlet temperature. This field is autosizable.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-9}
+
+This numeric field contains the minimum part load ratio. If the ratio of demand to boiler nominal capacity is less than the minimum part load ratio, then the Min PLR will determine the operating PLR. The expected range is between 0 and 1. If this field is left blank, the default value is 0.0.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-9}
+
+This numeric field contains the maximum part load ratio. If the ratio of demand to boiler nominal capacity is greater than the maximum part load ratio, then the Max PLR will determine the operating PLR. This value may exceed 1, but the normal range is between 0 and 1.1. If this field is left blank, the default value is 1.0.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-9}
+
+This numeric field contains the optimum part load ratio. This is the part load ratio at which the boiler performs at its maximum efficiency. If this field is left blank, the default value is 1.0.
+
+\paragraph{Field: Boiler Water Inlet Node Name}\label{field-boiler-water-inlet-node-name}
+
+This required alpha field contains the water inlet node name.
+
+\paragraph{Field: Boiler Water Outlet Node Name}\label{field-boiler-water-outlet-node-name}
+
+This required alpha field contains the water outlet node name.
+
+\paragraph{Field: Water Outlet Upper Temperature Limit}\label{field-water-outlet-upper-temperature-limit-000}
+
+This numeric field contains the outlet temperature upper limit. If this field is left blank, the default value is 99.9ºC.
+
+\paragraph{Field: Boiler Flow Mode}\label{field-boiler-flow-mode}
+
+This choice field determines how the boiler operates with respect to the intended fluid flow through the device.~ There are three different choices for specifying operating modes for the intended flow behavior:~ ``NotModulated,'' ``ConstantFlow,'' and ``LeavingSetpointModulated.''~ NotModulated is useful for either variable or constant speed pumping arrangements where the boiler is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.~ ConstantFlow is useful for constant speed pumping arrangements where the boiler's request for flow is more strict and can increase the overall loop flow.~ LeavingSetpointModulated changes the boiler model to internally vary the flow rate so that the temperature leaving the boiler matches a setpoint.~ In all cases the operation of the external plant system can also impact the flow through the boiler -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.~~ The default, if not specified, is NotModulated.
+
+\paragraph{Field: Parasitic Electric Load}\label{field-parasitic-electric-load-000}
+
+This optional numeric field contains the parasitic electric power (W) consumed by a forced draft fan or other electrical device associated with the boiler. This parasitic electric load is consumed whenever the boiler is operating, and the model assumes that this parasitic power does not contribute to heating the water. The minimum value for this field is 0.0, and the default value is also 0.0 if the field is left blank.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-10}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity and Design Water Flow Rate. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+  Boiler:HotWater,
+      Condensing Boiler,   !- Boiler Name
+      NaturalGas,          !- Fuel Type
+      25000,               !- Nominal Capacity {W}
+      EnteringBoiler       !- Efficiency Curve Temperature Evaluation Variable
+      0.89,                !- Nominal Thermal Efficiency
+      CondensingBoilerEff, !- Boiler Efficiency Curve Name
+      75,                  !- Design Boiler Water Outlet Temp {C}
+      0.0021,              !- Max Design Boiler Water Flow Rate {m3/s}
+      0.10,                !- Minimum Part Load Ratio
+      1.00,                !- Maximum Part Load Ratio
+      1.00,                !- Optimum Part Load Ratio
+      Boiler Inlet Node,   !- Boiler Water Inlet Node
+      Boiler Outlet Node,  !- Boiler Water Outlet Node
+      80,                  !- Temp Upper Limit Water Outlet {C}
+      ConstantFlow,        !- Boiler Flow Mode
+      25.0;                !- Parasitic Electric Load {W}
+
+
+    Curve:Biquadratic,
+      CondensingBoilerEff,     !- Name
+      1.124970374,             !- Coefficient1 Constant
+      0.014963852,             !- Coefficient2 x
+     -0.02599835,              !- Coefficient3 x**2
+      0.0,                     !-Coefficient4y
+     -1.40464E-6,              !-Coefficient5y**2
+     -0.00153624,              !- Coefficient6x*y
+      0.1,                     !- Minimum Value of x
+      1.0,                     !- Maximum Value of x
+      30.0,                    !- Minimum Value of y
+      85.0;                    !- Maximum Value of y
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-10-005}
+
+Outputs available from the boiler:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Heating Energy {[}J{]}
+\item
+  Zone,Meter,Boilers:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Boiler Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Boiler Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Boiler Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Boiler Parasitic Electric Power {[}W{]}
+\item
+  HVAC,Sum,Boiler Ancillary Electric Energy {[}J{]}
+\item
+  HVAC,Average,Boiler Part Load Ratio
+\end{itemize}
+
+~ One of the following blocks will be applicable based on fuel type:
+
+Electric:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Electric Power {[}W{]}
+\item
+  HVAC,Sum,Boiler Electric Energy {[}J{]}
+\end{itemize}
+
+Gas:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Gas Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Gas Energy {[}J{]}
+\end{itemize}
+
+Propane:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Propane Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Propane Energy {[}J{]}
+\end{itemize}
+
+FuelOil\#1:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler FuelOil\#1 Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler FuelOil\#1 Energy {[}J{]}
+\end{itemize}
+
+FuelOil\#2:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler FuelOil\#2 Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler FuelOil\#2 Energy {[}J{]}
+\end{itemize}
+
+Coal:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Coal Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Coal Energy {[}J{]}
+\end{itemize}
+
+Diesel:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Diesel Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Diesel Energy {[}J{]}
+\end{itemize}
+
+Gasoline:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Gasoline Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Gasoline Energy {[}J{]}
+\end{itemize}
+
+OtherFuel1:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler OtherFuel1 Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler OtherFuel1 Energy {[}J{]}
+\end{itemize}
+
+OtherFuel2:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler OtherFuel2 Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler OtherFuel2 Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Boiler Heating Rate {[}W{]}}\label{boiler-heating-rate-w}
+
+\paragraph{Boiler Heating Energy {[}J{]}}\label{boiler-heating-energy-j}
+
+These outputs are the heating output (load) of the boiler. Energy is metered on Boilers:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\paragraph{Boiler Inlet Temperature {[}C{]}}\label{boiler-inlet-temperature-c}
+
+\paragraph{Boiler Outlet Temperature {[}C{]}}\label{boiler-outlet-temperature-c}
+
+\paragraph{Boiler Mass Flow Rate {[}kg/s{]}}\label{boiler-mass-flow-rate-kgs}
+
+These outputs are the hot water inlet and outlet temperatures and flow rate for the boiler.
+
+\paragraph{\texorpdfstring{Boiler Part Load Ratio {[]}}{Boiler Part Load Ratio }}\label{boiler-part-load-ratio}
+
+This output is the operating part-load ratio of the boiler. The part-load ratio is calculated as the boiler load divided by the boiler nominal capacity. The part-load ratio is limited by the minimum and maximum part-load ratio inputs specified by the user.
+
+\paragraph{Boiler \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{boiler-fuel-type-rate-w}
+
+\paragraph{Boiler \textless{}Fuel Type\textgreater{} Energy {[}J{]} \textbackslash{}}\label{boiler-fuel-type-energy-j}
+
+\paragraph{Boiler Electric Power {[}W{]}}\label{boiler-electric-power-w}
+
+These outputs are the energy input to the boiler. Valid fuel types are:~ Electric, Gas (natural gas), Propane, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1, OtherFuel2. Consumption is metered on Heating:\textless{}Fuel Type\textgreater{}, \textless{}Fuel Type\textgreater{}:Plant, and \textless{}Fuel Type\textgreater{}:Facility.
+
+\paragraph{Boiler Ancillary Electric Power {[}W{]}}\label{boiler-ancillary-electric-power-w}
+
+\paragraph{Boiler Ancillary Electric Energy {[}J{]}}\label{boiler-ancillary-electric-energy-j}
+
+These outputs are the parasitic electric power and parasitic electric consumption associated with the boiler. Used when simulating a forced draft fan or other electric component. Consumption is metered on Heating:Electricity and Electricity:Plant.
+
+\subsection{Boiler:Steam}\label{boilersteam}
+
+The steam boiler model provides a first order approximation of performance for fuel oil, gas and electric boilers. Boiler performance is based on a ``theoretical'' boiler efficiency (overall efficiency at design operating conditions) and a single quadratic fuel use/ part load ratio curve. This single curve accounts for all combustion inefficiencies and stack losses.
+
+\subsubsection{Inputs}\label{inputs-11-012}
+
+\paragraph{Field: Name}\label{field-name-10-011}
+
+This alpha field contains the identifying name for the Steam Boiler.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-4}
+
+This alpha value specifies the type of fuel used by the boiler. The fuel type can be \textbf{Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1} or \textbf{OtherFuel2.}
+
+\paragraph{Field: Maximum Operating Pressure}\label{field-maximum-operating-pressure}
+
+This numeric field contains the maximum value of pressure up to which the boiler would operate, or the maximum design pressure. (Pascal)
+
+\paragraph{Field: Theoretical Efficiency}\label{field-theoretical-efficiency}
+
+This numeric field contains the heating efficiency (as a fraction between 0 and 1) of the boiler's burner
+
+\paragraph{Field: Design Outlet Steam Temperature}\label{field-design-outlet-steam-temperature}
+
+The maximum value of steam temperature the boiler can provide. (Celcius)
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-7}
+
+This numeric field contains the nominal operating capacity (W) of the boiler.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-10}
+
+This numeric field contains the minimum part load ratio. If the ratio of demand to boiler nominal capacity is less than the minimum part load ratio, then the Min PLR will determine the operating PLR. The expected range is between 0 and 1.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-10}
+
+This numeric field contains the maximum part load ratio. If the ratio of demand to boiler nominal capacity is greater than the maximum part load ratio, then the Max PLR will determine the operating PLR. This value may exceed 1, but the normal range is between 0 and 1.1.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-10}
+
+This numeric field contains the optimum part load ratio. This is the part load ratio at which the boiler performs at its maximum efficiency.
+
+\paragraph{Field: Coefficient 1 of Fuel Use Function of Part Load Ratio Curve}\label{field-coefficient-1-of-fuel-use-function-of-part-load-ratio-curve}
+
+This numeric field contains the fuel use / PLR coefficient1.
+
+\paragraph{Field: Coefficient 2 of Fuel Use Function of Part Load Ratio Curve}\label{field-coefficient-2-of-fuel-use-function-of-part-load-ratio-curve}
+
+This numeric field contains the fuel use / PLR coefficient2.
+
+\paragraph{Field: Coefficient 3 of Fuel Use Function of Part Load Ratio Curve}\label{field-coefficient-3-of-fuel-use-function-of-part-load-ratio-curve}
+
+This numeric field contains the fuel use / PLR coefficient3.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-001}
+
+This alpha field contains the water inlet node name.
+
+\paragraph{Field: Steam Outlet Node Name}\label{field-steam-outlet-node-name}
+
+This alpha field contains the steam outlet node name.
+
+\paragraph{Field: Sizing Factor}\label{field-sizing-factor-11}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
+
+More information on the technical aspects of steam boiler can be found in the Engineering Reference Document.
+
+An example of a Steam Boiler input statement from an IDF is:
+
+\begin{lstlisting}
+
+Boiler:Steam,
+      Steam Boiler Plant Boiler,  !- Boiler Name
+      NaturalGas,                 !- Fuel Type
+      160000,                     !-Maximum Boiler Pressure Pascal
+      0.8,                        !- Theoretical Boiler Efficiency
+      115,                        !- Max Design Outlet Steam Temp
+      300000,                     !- Nominal Capacity W
+      0.00001,                    !- Minimum Part Load Ratio
+      1.0,                        !- Maximum Part Load Ratio
+      0.2,                        !- Optimum Part Load Ratio
+      0.8,!- Coefficient 1 of the fuel use/part load ratio curve
+      0.1,!- Coefficient 2 of the fuel use/part load ratio curve
+      0.1,!- Coefficient 3 of the fuel use/part load ratio curve
+      Steam Boiler Plant Boiler Inlet Node,  !- Boiler Steam Inlet Node
+      Steam Boiler Plant Boiler Outlet Node; !- Plant Loop Outlet Node
+
+
+  Boiler:Steam,
+      Steam Boiler Plant Boiler,  !- Boiler Name
+      NaturalGas,                 !- Fuel Type
+      160000,                     !-Maximum Boiler Pressure Pascal
+      0.8,                        !- Theoretical Boiler Efficiency
+      115,                        !- Max Design Outlet Steam Temp
+      autosize,                  !- Nominal Capacity W
+      0.00001,                    !- Minimum Part Load Ratio
+      1.0,                        !- Maximum Part Load Ratio
+      0.2,                        !- Optimum Part Load Ratio
+      0.8,!- Coefficient 1 of the fuel use/part load ratio curve
+      0.1,!- Coefficient 2 of the fuel use/part load ratio curve
+      0.1,!- Coefficient 3 of the fuel use/part load ratio curve
+      Steam Boiler Plant Boiler Inlet Node,  !- Boiler Steam Inlet Node
+      Steam Boiler Plant Boiler Outlet Node; !- Plant Loop Outlet Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-11-004}
+
+Outputs available from the steam boiler:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Heating Energy {[}J{]}
+\item
+  Zone,Meter,Boilers:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Boiler Steam Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Boiler Steam Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Boiler Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+~ One of the following blocks will be applicable based on fuel type:
+
+Electric:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Electric Power {[}W{]}
+\item
+  HVAC,Sum,Boiler Electric Energy {[}J{]}
+\end{itemize}
+
+Gas:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Gas Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Gas Energy {[}J{]}
+\end{itemize}
+
+Propane:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Propane Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Propane Energy {[}J{]}
+\end{itemize}
+
+FuelOil\#1:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler FuelOil\#1 Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler FuelOil\#1 Energy {[}J{]}
+\end{itemize}
+
+FuelOil\#2:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler FuelOil\#2 Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler FuelOil\#2 Energy {[}J{]}
+\end{itemize}
+
+Coal:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Coal Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Coal Energy {[}J{]}
+\end{itemize}
+
+Diesel:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Diesel Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Diesel Energy {[}J{]}
+\end{itemize}
+
+Gasoline:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler Gasoline Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Gasoline Energy {[}J{]}
+\end{itemize}
+
+OtherFuel1:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler OtherFuel1 Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler OtherFuel1 Energy {[}J{]}
+\end{itemize}
+
+OtherFuel2:
+
+\begin{itemize}
+\item
+  HVAC,Average,Boiler OtherFuel2 Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler OtherFuel2 Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Boiler Heating Rate {[}W{]}}\label{boiler-heating-rate-w-1}
+
+\paragraph{Boiler Heating Energy {[}J{]}}\label{boiler-heating-energy-j-1}
+
+These outputs are the heating output (load) of the boiler. Energy is metered on Boilers:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\paragraph{Boiler Steam Inlet Temperature {[}C{]}}\label{boiler-steam-inlet-temperature-c}
+
+\paragraph{Boiler Steam Outlet Temperature {[}C{]}}\label{boiler-steam-outlet-temperature-c}
+
+\paragraph{Boiler Steam Mass Flow Rate {[}kg/s{]}}\label{boiler-steam-mass-flow-rate-kgs}
+
+These outputs are the steam inlet and outlet temperatures and steam flow rate for the boiler.
+
+\paragraph{Boiler \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{boiler-fuel-type-rate-w-1}
+
+\paragraph{Boiler \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{boiler-fuel-type-energy-j-1}
+
+\paragraph{Boiler Electric Power {[}W{]}}\label{boiler-electric-power-w-1}
+
+\paragraph{Boiler Electric Energy {[}J{]}}\label{boiler-electric-energy-j}
+
+These outputs are the energy input to the boiler. Valid fuel types are:~ Electric, Gas (natural gas), Propane, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1, and OtherFuel2. Consumption is metered on Heating:\textless{}Fuel Type\textgreater{}, \textless{}Fuel Type\textgreater{}:Plant, and \textless{}Fuel Type\textgreater{}:Facility.
+
+\subsection{Water to Water Heat Pumps}\label{water-to-water-heat-pumps}
+
+The EnergyPlus has two water-to-water heat pump models, parameter estimation and equation fit, to choose from:
+
+\textbf{HeatPump:WaterToWater:EquationFit:Cooling}
+
+\textbf{HeatPump:WaterToWater:EquationFit:Heating}
+
+This model is an equation-fit model from the catalog data which resembles a black box with no usage of heat transfer equations. The performance of the heat pump is modeled using curves fitted from the catalog data.
+
+\textbf{HeatPump:WaterToWater:ParameterEstimation:Cooling}
+
+\textbf{HeatPump:WaterToWater:ParameterEstimation:Heating}
+
+This model is a parameter estimation based model that uses physical parameters generated from the catalog data. The physical parameters are then used to predict the performance of the heat pump using thermodynamic laws and heat transfer equations. The heat pump has a reciprocating compressor that serves both the hot water and the chilled water loop. Note that this model is currently ``hardwired'' to fluid property R22. FluidProperties:* objects for R-22 must be included in the idf file. These may be copied from DataSets\\FluidPropertiesRefData.idf.
+
+Descriptions and strength of each respective model is available in the following references:
+
+Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from \href{http://www.hvac.okstate.edu}{http://www.hvac.okstate.edu/})
+
+Tang,C. C. 2005. Modeling Packaged Heat Pumps in Quasi-Steady State Energy Simulation Program. M.S. Thesis. Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from \href{http://www.hvac.okstate.edu}{http://www.hvac.okstate.edu/})
+
+The Supply side of the heat pump is usually connected to a Ground Heat Exchanger. The figure below shows the layout and piping diagram of the water-to-water heat pump.
+
+\begin{figure}[hbtp] % fig 75
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image184.png}
+\caption{Schematic of EnergyPlus Ground Loop Heat Exchanger \protect \label{fig:schematic-of-energyplus-ground-loop-heat-001}}
+\end{figure}
+
+First, the equation fit model objects are described. This model has two sets of coefficients, one for the heating mode and other for the cooling mode.
+
+\subsection{HeatPump:WaterToWater:EquationFit:Cooling}\label{heatpumpwatertowaterequationfitcooling}
+
+\subsubsection{Inputs}\label{inputs-12-012}
+
+\paragraph{Field: Name}\label{field-name-11-010}
+
+This alpha field contains the identifying name for the ground source heat pump.
+
+\paragraph{Field: Source Side Inlet Node Name}\label{field-source-side-inlet-node-name}
+
+This alpha field contains the heat pump's source side inlet node name.
+
+\paragraph{Field: Source Side Outlet Node Name}\label{field-source-side-outlet-node-name}
+
+This alpha field contains the heat pump's source side outlet node name.
+
+\paragraph{Field: Load Side Inlet Node Name}\label{field-load-side-inlet-node-name}
+
+This alpha field contains the heat pump's load side inlet node name.
+
+\paragraph{Field: Load Side Outlet Node Name}\label{field-load-side-outlet-node-name}
+
+This alpha field contains the heat pump's load side outlet node name.
+
+\paragraph{Field: Rated Load Side Flow Rate}\label{field-rated-load-side-flow-rate}
+
+This numeric field contains the rated volumetric flow rate on the load side of the heat pump in m3/s. This corresponds to the highest load side heat transfer rate listed in the catalog data.
+
+\paragraph{Field: Rated Source Side Flow Rate}\label{field-rated-source-side-flow-rate}
+
+This numeric field contains the rated volumetric flow rate on the source side of the heat pump in m3/s. This corresponds to the highest load side heat transfer rate listed in the catalog data.
+
+\paragraph{Field: Rated Cooling Capacity}\label{field-rated-cooling-capacity}
+
+This numeric field contains the rated cooling capacity of the heat pump in W. This corresponds to the highest load side heat transfer rate listed in the catalog data.
+
+\paragraph{Field: Rated Cooling Power Consumption}\label{field-rated-cooling-power-consumption}
+
+Rated cooling power consumption, in W.
+
+\paragraph{Fields: Cooling Capacity Coefficients 1-5}\label{fields-cooling-capacity-coefficients-1-5}
+
+Five fields are used to describe the coefficients for the Cooling Capacity curve. More details on how these coefficients are used are described in the Engineering Reference.
+
+\paragraph{Field: Cooling Compressor Power Coefficients 1-5}\label{field-cooling-compressor-power-coefficients-1-5}
+
+Five fields are used to decribe the coefficients for the Cooling Compressor Power curve.
+
+An idf example:
+
+\begin{lstlisting}
+
+HeatPump:WaterToWater:EquationFit:Cooling,
+  GshpCLG,                 !- Name
+  GshpCLG SourceSide Inlet Node,      !- Source Side Inlet Node Name
+  GshpCLG SourceSide Outlet Node,     !- Source Side Outlet Node Name
+  GshpCLG LoadSide Inlet Node,        !- Load Side Inlet Node Name
+  GshpCLG LoadSide Outlet Node,       !- Load Side Outlet Node Name
+  1.89E-03,                !- Rated Load Side Flow Rate {m3/s}
+  1.89E-03,                !- Rated Source Side Flow Rate {m3/s}
+  39890.91,                !- Rated Cooling Capacity {W}
+  4790.00,                 !- Rated Cooling Power Consumption {W}
+  -1.52030596,             !- Cooling Capacity Coefficient 1
+  3.46625667,              !- Cooling Capacity Coefficient 2
+  -1.32267797,             !- Cooling Capacity Coefficient 3
+  0.09395678,              !- Cooling Capacity Coefficient 4
+  0.038975504,             !- Cooling Capacity Coefficient 5
+  -8.59564386,             !- Cooling Compressor Power Coefficient 1
+  0.96265085,              !- Cooling Compressor Power Coefficient 2
+  8.69489229,              !- Cooling Compressor Power Coefficient 3
+  0.02501669,              !- Cooling Compressor Power Coefficient 4
+  -0.20132665;             !- Cooling Compressor Power Coefficient 5
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-12-004}
+
+This section describes the outputs available for the water to water heat pump, equation fit model; both cooling and heating.
+
+\begin{itemize}
+\item
+  HVAC,Sum,Water to Water Heat Pump Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Water to Water Heat Pump Load Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Sum,Water to Water Heat Pump Source Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Electric Power {[}W{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Outlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Inlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Outlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Inlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Water to Water Heat Pump Electric Energy {[}J{]}}\label{water-to-water-heat-pump-electric-energy-j}
+
+This output variable represents the cumulative energy used by the compressor. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
+
+\paragraph{Water to Water Heat Pump Load Side Heat Transfer Energy {[}J{]}}\label{water-to-water-heat-pump-load-side-heat-transfer-energy-j}
+
+This output variable represents the cumulative heat transfer across the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
+
+\paragraph{Water to Water Heat Pump Source Side Heat Transfer Energy {[}J{]}}\label{water-to-water-heat-pump-source-side-heat-transfer-energy-j}
+
+This output variable represents the cumulative heat transfer across the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
+
+\paragraph{Water to Water Heat Pump Electric Power {[}W{]}}\label{water-to-water-heat-pump-electric-power-w}
+
+This output variable represents the compressor power required to run the heat pump. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Load Side Heat Transfer Rate {[}W{]}}\label{water-to-water-heat-pump-load-side-heat-transfer-rate-w}
+
+This output variable represents the heat transfer across the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Source Side Heat Transfer Rate {[}W{]}}\label{water-to-water-heat-pump-source-side-heat-transfer-rate-w}
+
+This output variable represents the heat transfer across the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Load Side Outlet Temperature {[}C{]}}\label{water-to-water-heat-pump-load-side-outlet-temperature-c}
+
+This output variable represents the average fluid temperature leaving the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Load Side Inlet Temperature {[}C{]}}\label{water-to-water-heat-pump-load-side-inlet-temperature-c}
+
+This output variable represents the average fluid temperature entering the load side coil.~ The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Source Side Outlet Temperature {[}C{]}}\label{water-to-water-heat-pump-source-side-outlet-temperature-c}
+
+This output variable represents the average fluid temperature leaving the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Source Side Inlet Temperature {[}C{]}}\label{water-to-water-heat-pump-source-side-inlet-temperature-c}
+
+This output variable represents the average fluid temperature entering the source side coil.~ The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Load Side Mass Flow Rate {[}kg/s{]}}\label{water-to-water-heat-pump-load-side-mass-flow-rate-kgs}
+
+This output variable represents the average fluid flow rate through the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Source Side Mass Flow Rate {[}kg/s{]}}\label{water-to-water-heat-pump-source-side-mass-flow-rate-kgs}
+
+This output variable represents the average fluid flow rate through the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\subsection{HeatPump:WaterToWater:EquationFit:Heating}\label{heatpumpwatertowaterequationfitheating}
+
+\subsubsection{Inputs}\label{inputs-13-010}
+
+\paragraph{Field: Name}\label{field-name-12-008}
+
+This alpha field contains the identifying name for the ground source heat pump.
+
+\paragraph{Field: Source Side Inlet Node Name}\label{field-source-side-inlet-node-name-1}
+
+This alpha field contains the heat pump's source side inlet node name.
+
+\paragraph{Field: Source Side Outlet Node Name}\label{field-source-side-outlet-node-name-1}
+
+This alpha field contains the heat pump's source side outlet node name.
+
+\paragraph{Field: Load Side Inlet Node Name}\label{field-load-side-inlet-node-name-1}
+
+This alpha field contains the heat pump's load side inlet node name.
+
+\paragraph{Field: Load Side Outlet Node Name}\label{field-load-side-outlet-node-name-1}
+
+This alpha field contains the heat pump's load side outlet node name.
+
+\paragraph{Field: Rated Load Side Flow Rate}\label{field-rated-load-side-flow-rate-1}
+
+This numeric field contains the rated volumetric flow rate on the load side of the heat pump in m3/s. This corresponds to the highest load side heat transfer rate listed in the catalog data.
+
+\paragraph{Field: Rated Source Side Flow Rate}\label{field-rated-source-side-flow-rate-1}
+
+This numeric field contains the rated volumetric flow rate on the source side of the heat pump in m3/s. This corresponds to the highest load side heat transfer rate listed in the catalog data.
+
+\paragraph{Field: Rated Heating Capacity}\label{field-rated-heating-capacity-000}
+
+This numeric field contains the rated heating capacity of the heat pump in W. This corresponds to the highest load side heat transfer rate listed in the catalog data.
+
+\paragraph{Field: Rated Heating Power Consumption}\label{field-rated-heating-power-consumption}
+
+Rated heating power consumption, in W.
+
+\paragraph{Fields: Heating Capacity Coefficients 1-5}\label{fields-heating-capacity-coefficients-1-5}
+
+Five fields are used to describe the coefficients for the Heating Capacity curve. More details on how these coefficients are used are described in the Engineering Reference.
+
+\paragraph{Field: Heating Compressor Power Coefficients 1-5}\label{field-heating-compressor-power-coefficients-1-5}
+
+Five fields are used to describe the coefficients for the Heating Compressor Power curve.
+
+An idf example:
+
+\begin{lstlisting}
+
+HeatPump:WaterToWater:EquationFit:Heating,
+  GshpHeating,             !- Name
+  GshpHeating SourceSide Inlet Node,      !- Source Side Inlet Node Name
+  GshpHeating SourceSide Outlet Node,     !- Source Side Outlet Node Name
+  GshpHeating LoadSide Inlet Node,        !- Load Side Inlet Node Name
+  GshpHeating LoadSide Outlet Node,       !- Load Side Outlet Node Name
+  1.89E-03,                !- Rated Load Side Flow Rate {m3/s}
+  1.89E-03,                !- Rated Source Side Flow Rate {m3/s}
+  39040.92,                !- Rated Heating Capacity {W}
+  5130.00,                 !- Rated Heating Power Consumption {W}
+  -3.33491153,             !- Heating Capacity Coefficient 1
+  -0.51451946,             !- Heating Capacity Coefficient 2
+  4.51592706,              !- Heating Capacity Coefficient 3
+  0.01797107,              !- Heating Capacity Coefficient 4
+  0.155797661,             !- Heating Capacity Coefficient 5
+  -8.93121751,             !- Heating Compressor Power Coefficient 1
+  8.57035762,              !- Heating Compressor Power Coefficient 2
+  1.29660976,              !- Heating Compressor Power Coefficient 3
+  -0.21629222,             !- Heating Compressor Power Coefficient 4
+  0.033862378;             !- Heating Compressor Power Coefficient 5
+\end{lstlisting}
+
+Next, the parameter estimation model objects are described. This model has two sets of parameters, one for the heating mode and other for the cooling mode.
+
+\subsection{HeatPump:WaterToWater:ParameterEstimation:Cooling}\label{heatpumpwatertowaterparameterestimationcooling}
+
+\subsubsection{Inputs}\label{inputs-14-010}
+
+\paragraph{Field: Name}\label{field-name-13-007}
+
+This alpha field contains the identifying name for the ground source heat pump.
+
+\paragraph{Field: Source Side Inlet Node Name}\label{field-source-side-inlet-node-name-2}
+
+This alpha field contains the heat pump's source side inlet node name.
+
+\paragraph{Field: Source Side Outlet Node Name}\label{field-source-side-outlet-node-name-2}
+
+This alpha field contains the heat pump's source side outlet node name.
+
+\paragraph{Field: Load Side Inlet Node Name}\label{field-load-side-inlet-node-name-2}
+
+This alpha field contains the heat pump's load side inlet node name.
+
+\paragraph{Field: Load Side Outlet Node Name}\label{field-load-side-outlet-node-name-2}
+
+This alpha field contains the heat pump's load side outlet node name.
+
+\paragraph{Field: Nominal COP}\label{field-nominal-cop-4}
+
+This numeric field contains the nominal coefficient of performance of the heat pump.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-8}
+
+This numeric field contains the nominal capacity of the heat pump in Watts.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-11}
+
+This numeric field contains the minimum part load ratio of the heat pump usually set to 0.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-11}
+
+This numeric field contains the maximum part load ratio of the heat pump usually set to 1.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-11}
+
+This numeric field contains the optimal part load ratio of the heat pump usually set to 1.
+
+\paragraph{Field: Load Side Flow Rate}\label{field-load-side-flow-rate}
+
+This numeric field contains the volumetric flow rate on the load side of the heat pump in m3/s
+
+\paragraph{Field: Source Side Flow Rate}\label{field-source-side-flow-rate}
+
+This numeric field contains the volumetric flow rate on the source side of the heat pump in m3/s
+
+\paragraph{Field: Load Side Heat Transfer Coefficient}\label{field-load-side-heat-transfer-coefficient}
+
+This numeric field contains Estimated parameter load side heat transfer coefficient W/K.
+
+\paragraph{Field: Source Side Heat Transfer Coefficient}\label{field-source-side-heat-transfer-coefficient-000}
+
+This numeric field contains Estimated parameter source side heat transfer coefficient W/K.
+
+\paragraph{Field: Piston Displacement}\label{field-piston-displacement}
+
+This numeric field contains the Estimated parameter displacement of the reciprocating compressor in m3/s.
+
+\paragraph{Field: Compressor Clearance Factor}\label{field-compressor-clearance-factor-000}
+
+This numeric field contains the Estimated parameter clearance factor of the reciprocating compressor.
+
+\paragraph{Field: Compressor Suction and Discharge Pressure Drop}\label{field-compressor-suction-and-discharge-pressure-drop}
+
+This numeric field contains the estimated parameter the pressure drop at compressor suction and discharge in Pascals (N/m2).
+
+\paragraph{Field: Superheating}\label{field-superheating}
+
+This numeric field contains the estimated parameter superheat at the evaporator outlet in °C.
+
+\paragraph{Field: Constant Part of Electromechanical Power Losses}\label{field-constant-part-of-electromechanical-power-losses}
+
+This numeric field contains the estimated parameter power loss, which accounts for the loss of work due mechanical and electrical losses in the compressor in Watts.
+
+\paragraph{Field: Loss Factor}\label{field-loss-factor}
+
+This numeric field contains the factor of electromechanical loss that is proportional to the theoretical power percentage.
+
+\paragraph{Field: High Pressure Cut Off}\label{field-high-pressure-cut-off}
+
+This numeric field contains the design pressure limit of the compressor in Pascals (N/m2).
+
+\paragraph{Field: Low Pressure Cut Off}\label{field-low-pressure-cut-off}
+
+This numeric field contains the design low-pressure limit of the compressor in Pascals (N/m2).
+
+An idf example:
+
+\begin{lstlisting}
+
+HeatPump:WaterToWater:ParameterEstimation:Cooling,
+      GshpCLG,                 !- Water to Water Heat Pump Name
+      GshpCLG SourceSide Inlet Node,  !- Source Side Inlet Node
+      GshpCLG SourceSide Outlet Node,  !- Source Side Outlet Node
+      GshpCLG LoadSide Inlet Node,  !- Load Side Inlet Node
+      GshpCLG LoadSide Outlet Node,  !- Load Side Outlet Node
+      3.5,                     !- Nominal COP
+      45000,                   !- Nominal Capacity {W}
+      0.0,                     !- Min PLR
+      1,                       !- Max PLR
+      1,                       !- optimum PLR
+      .003,                    !- Load side Flow Rate {m3/s}
+      .003,                    !- Source Side Flow Rate {m3/s}
+      7761,                    !- Load side Heat Transfer Coefficient {W/K}
+      3998,                    !- Source Side Heat Transfer Coefficient {W/K}
+      .012544,                 !- Piston Displacement {m3/s}
+      .05469,                  !- Compressor Clearance Factor %
+      92156.2,                 !- Compressor Suction And Discharge Pressure Drop {Pa}
+      4.8907,                  !- Superheating {C}
+      2803.9,                  !- Constant Part of Electro Mechanical Power Losses {W}
+      .699,                    !- Loss Factor
+      0.0,                     !- High Pressure Cut off {Pa}
+      0.0;                     !- LowPressure Cut off {Pa}
+\end{lstlisting}
+
+\subsection{HeatPump:WaterToWater:ParameterEstimation:Heating}\label{heatpumpwatertowaterparameterestimationheating}
+
+\subsubsection{Inputs}\label{inputs-15-010}
+
+\paragraph{Field: Name}\label{field-name-14-006}
+
+This alpha field contains the identifying name for the ground source heat pump.
+
+\paragraph{Field: Source Side Inlet Node Name}\label{field-source-side-inlet-node-name-3}
+
+This alpha field contains the heat pump's source side inlet node name.
+
+\paragraph{Field: Source Side Outlet Node Name}\label{field-source-side-outlet-node-name-3}
+
+This alpha field contains the heat pump's source side outlet node name.
+
+\paragraph{Field: Load Side Inlet Node Name}\label{field-load-side-inlet-node-name-3}
+
+This alpha field contains the heat pump's load side inlet node name.
+
+\paragraph{Field: Load Side Outlet Node Name}\label{field-load-side-outlet-node-name-3}
+
+This alpha field contains the heat pump's load side outlet node name.
+
+\paragraph{Field: Nominal COP}\label{field-nominal-cop-5}
+
+This numeric field contains the nominal coefficient of performance of the heat pump.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-9}
+
+This numeric field contains the nominal capacity of the heat pump in Watts.
+
+\paragraph{Field: Minimum Part Load Ratio}\label{field-minimum-part-load-ratio-12}
+
+This numeric field contains the minimum part load ratio of the heat pump usually set to 0.
+
+\paragraph{Field: Maximum Part Load Ratio}\label{field-maximum-part-load-ratio-12}
+
+This numeric field contains the maximum part load ratio of the heat pump usually set to 1.
+
+\paragraph{Field: Optimum Part Load Ratio}\label{field-optimum-part-load-ratio-12}
+
+This numeric field contains the optimal part load ratio of the heat pump usually set to 1.
+
+\paragraph{Field: Load Side Flow Rate}\label{field-load-side-flow-rate-1}
+
+This numeric field contains the volumetric flow rate on the load side of the heat pump in m3/s
+
+\paragraph{Field: Source Side Flow Rate}\label{field-source-side-flow-rate-1}
+
+This numeric field contains the volumetric flow rate on the source side of the heat pump in m3/s
+
+\paragraph{Field: Load Side Heat Transfer Coefficient}\label{field-load-side-heat-transfer-coefficient-1}
+
+This numeric field contains Estimated parameter load side heat transfer coefficient W/K.
+
+\paragraph{Field: Source Side Heat Transfer Coefficient}\label{field-source-side-heat-transfer-coefficient-1-000}
+
+This numeric field contains Estimated parameter source side heat transfer coefficient W/K.
+
+\paragraph{Field: Piston Displacement}\label{field-piston-displacement-1}
+
+This numeric field contains the Estimated parameter displacement of the reciprocating compressor in m3/s.
+
+\paragraph{Field: Compressor Clearance Factor}\label{field-compressor-clearance-factor-1-000}
+
+This numeric field contains the Estimated parameter clearance factor of the reciprocating compressor.
+
+\paragraph{Field: Compressor Suction and Discharge Pressure Drop}\label{field-compressor-suction-and-discharge-pressure-drop-1}
+
+This numeric field contains the estimated parameter the pressure drop at compressor suction and discharge in Pascals (N/m2).
+
+\paragraph{Field: Superheating}\label{field-superheating-1}
+
+This numeric field contains the estimated parameter superheat at the evaporator outlet in °C.
+
+\paragraph{Field: Constant Part of Electromechanical Power Losses}\label{field-constant-part-of-electromechanical-power-losses-1}
+
+This numeric field contains the estimated parameter power loss, which accounts for the loss of work due mechanical and electrical losses in the compressor in Watts.
+
+\paragraph{Field: Loss Factor}\label{field-loss-factor-1}
+
+This numeric field contains the factor of electromechanical loss that is proportional to the theoretical power percentage.
+
+\paragraph{Field: High Pressure Cut Off}\label{field-high-pressure-cut-off-1}
+
+This numeric field contains the design pressure limit of the compressor in Pascals (N/m2).
+
+\paragraph{Field: Low Pressure Cut Off}\label{field-low-pressure-cut-off-1}
+
+This numeric field contains the design low-pressure limit of the compressor in Pascals (N/m2).
+
+An idf example:
+
+\begin{lstlisting}
+
+HeatPump:WaterToWater:ParameterEstimation:Heating,
+      GshpHeating,             !- Water to Water Heat Pump Name
+      GshpHeating SourceSide Inlet Node,  !- Source Side Inlet Node
+      GshpHeating SourceSide Outlet Node,  !- Source Side Outlet Node
+      GshpHeating LoadSide Inlet Node,  !- Load Side Inlet Node
+      GshpHeating LoadSide Outlet Node,  !- Load Side Outlet Node
+      3.5,                     !- Nominal COP
+      50000,                   !- Nominal Capacity {W}
+      0.0,                     !- Min PLR
+      1,                       !- Max PLR
+      1,                       !- optimum PLR
+      .003,                    !- Load side Flow Rate {m3/s}
+      .003,                    !- Source Side Flow Rate {m3/s}
+      7761,                    !- Load side Heat Transfer Coefficient {W/K}
+      3998,                    !- Source Side Heat Transfer Coefficient {W/K}
+      .012544,                 !- Piston Displacement {m3/s}
+      .05469,                  !- Compressor Clearance Factor %
+      92156.2,                 !- Compressor Suction And Dischrage Pressure Drop {Pa}
+      4.8907,                  !- Superheating {C}
+      2803.9,                  !- Constant Part Of Electro Mechanical Power Losses {W}
+      .699,                    !- Loss Factor
+      0.0,                     !- High Pressure Cut off {Pa}
+      0.0;                     !- LowPressure Cut off {Pa}
+\end{lstlisting}
+
+Since the heat pump is defined with two separate objects (one for heating, one for cooling), the connections to the condenser has to be done carefully. The example below shows the configuration for parameter estimation objects. The same specifications and configuration also applies to the equation fit model.
+
+\paragraph{Steps to specify the Ground Source Heat Pump}\label{steps-to-specify-the-ground-source-heat-pump}
+
+For the heating mode:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  Specify a branch for the Heat pump in hot water loop .
+\item
+  Include the branch name in the splitter and mixer branches.
+\item
+  Add a branch in condenser loop and include its name in the respective splitter and mixer.
+\end{enumerate}
+
+\textbf{! in hot water loop}
+
+\begin{lstlisting}
+
+BRANCH, Heating GshpHeating Branch,
+    ,
+    ,
+    HeatPump:WatertoWater:ParameterEstimatinon:Heating,
+    GshpHeating,
+    GshpHeating LoadSide Inlet Node,
+    GshpHeating LoadSide Outlet Node,
+    ACTIVE;
+\end{lstlisting}
+
+\textbf{!in condenser loop}
+
+\begin{lstlisting}
+
+BRANCH, GshpHeating SourceSide Branch,
+    ,
+    ,
+    HeatPump:WatertoWater:ParameterEstimatinon:Heating,
+    GshpHeating,
+    GshpHeating SourceSide Inlet Node,
+    GshpHeating SourceSide Outlet Node,
+    ACTIVE;
+\end{lstlisting}
+
+Example of Heat Pump Links
+
+For the cooling mode:
+
+1.~Specify a branch for the Heat pump in chilled water loop .
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  Include the branch name in the splitter and mixer branches.
+\end{enumerate}
+
+3.~Add a branch in condenser loop and include its name in the respective splitter and mixer.
+
+\textbf{! in chilled water loop}
+
+\begin{lstlisting}
+
+BRANCH,GshpCLG1 Chiller Branch,
+    ,
+    ,
+    HeatPump:WatertoWater:ParameterEstimatinon:Cooling, GshpCLG1,
+    GshpCLG LoadSide Inlet Node1,
+    GshpCLG LoadSide Outlet Node1,
+    Active;
+\end{lstlisting}
+
+\textbf{!in condenser loop}
+
+\begin{lstlisting}
+
+BRANCH, GshpCLG1 Condenser Branch,
+    ,
+    ,
+    HeatPump:WatertoWater:ParameterEstimatinon:Cooling, GshpCLG1,
+    GshpCLG SourceSide Inlet Node1,
+    GshpCLG SourceSide Outlet Node1,
+    ACTIVE;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-13-003}
+
+This section describes the outputs available for the water to water heat pump, parameter estimation model; both cooling and heating.
+
+\begin{itemize}
+\item
+  HVAC,Average,Water to Water Heat Pump Electric Power {[}W{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Water to Water Heat Pump Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Water to Water Heat Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Water to Water Heat Pump Load Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Sum,Water to Water Heat Pump Load Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Water to Water Heat Pump Source Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Sum,Water to Water Heat Pump Source Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Outlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Outlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Inlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Inlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Outlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Outlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Inlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Inlet Temperature {[}°C{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Load Side Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water to Water Heat Pump Source Side Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Water to Water Heat Pump Electric Power {[}W{]}}\label{water-to-water-heat-pump-electric-power-w-1}
+
+\paragraph{Water to Water Heat Pump Electric Power {[}W{]}}\label{water-to-water-heat-pump-electric-power-w-2}
+
+This output variable represents the compressor power required to run the heat pump. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Electric Energy {[}J{]}}\label{water-to-water-heat-pump-electric-energy-j-1}
+
+\paragraph{Water to Water Heat Pump Electric Energy {[}J{]}}\label{water-to-water-heat-pump-electric-energy-j-2}
+
+This output variable represents the cumulative energy used by the compressor. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
+
+\paragraph{Water to Water Heat Pump Load Side Heat Transfer Rate {[}W{]}}\label{water-to-water-heat-pump-load-side-heat-transfer-rate-w-1}
+
+\paragraph{Water to Water Heat Pump Load Side Heat Transfer Rate {[}W{]}}\label{water-to-water-heat-pump-load-side-heat-transfer-rate-w-2}
+
+This output variable represents the heat transfer across the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Load Side Heat Transfer Energy {[}J{]}}\label{water-to-water-heat-pump-load-side-heat-transfer-energy-j-1}
+
+\paragraph{Water to Water Heat Pump Load Side Heat Transfer Energy {[}J{]}}\label{water-to-water-heat-pump-load-side-heat-transfer-energy-j-2}
+
+This output variable represents the cumulative heat transfer across the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
+
+\paragraph{Water to Water Heat Pump Source Side Heat Transfer Rate {[}W{]}}\label{water-to-water-heat-pump-source-side-heat-transfer-rate-w-1}
+
+\paragraph{Water to Water Heat Pump Source Side Heat Transfer Rate {[}W{]}}\label{water-to-water-heat-pump-source-side-heat-transfer-rate-w-2}
+
+This output variable represents the heat transfer across the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Source Side Heat Transfer Energy {[}J{]}}\label{water-to-water-heat-pump-source-side-heat-transfer-energy-j-1}
+
+\paragraph{Water to Water Heat Pump Source Side Heat Transfer Energy {[}J{]}}\label{water-to-water-heat-pump-source-side-heat-transfer-energy-j-2}
+
+This output variable represents the cumulative heat transfer across the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
+
+\paragraph{Water to Water Heat Pump Load Side Outlet Temperature {[}C{]}}\label{water-to-water-heat-pump-load-side-outlet-temperature-c-1}
+
+\paragraph{Water to Water Heat Pump Load Side Outlet Temperature {[}C{]}}\label{water-to-water-heat-pump-load-side-outlet-temperature-c-2}
+
+This output variable represents the average fluid temperature leaving the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Load Side Inlet Temperature {[}C{]}}\label{water-to-water-heat-pump-load-side-inlet-temperature-c-1}
+
+\paragraph{Water to Water Heat Pump Load Side Inlet Temperature {[}C{]}}\label{water-to-water-heat-pump-load-side-inlet-temperature-c-2}
+
+This output variable represents the average fluid temperature entering the load side coil.~ The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Source Side Outlet Temperature {[}C{]}}\label{water-to-water-heat-pump-source-side-outlet-temperature-c-1}
+
+\paragraph{Water to Water Heat Pump Source Side Outlet Temperature °C{]}}\label{water-to-water-heat-pump-source-side-outlet-temperature-c-2}
+
+This output variable represents the average fluid temperature leaving the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Source Side Inlet Temperature {[}C{]}}\label{water-to-water-heat-pump-source-side-inlet-temperature-c-1}
+
+\paragraph{Water to Water Heat Pump Source Side Inlet Temperature {[}C{]}}\label{water-to-water-heat-pump-source-side-inlet-temperature-c-2}
+
+This output variable represents the average fluid temperature entering the source side coil.~ The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Load Side Mass Flow Rate {[}kg/s{]}}\label{water-to-water-heat-pump-load-side-mass-flow-rate-kgs-1}
+
+\paragraph{Water to Water Heat Pump Load Side Mass Flow Rate {[}kg/s{]}}\label{water-to-water-heat-pump-load-side-mass-flow-rate-kgs-2}
+
+This output variable represents the average fluid flow rate through the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Water to Water Heat Pump Source Side Mass Flow Rate {[}kg/s{]}}\label{water-to-water-heat-pump-source-side-mass-flow-rate-kgs-1}
+
+\paragraph{Water to Water Heat Pump Source Side Mass Flow Rate {[}kg/s{]}}\label{water-to-water-heat-pump-source-side-mass-flow-rate-kgs-2}
+
+This output variable represents the average fluid flow rate through the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\subsection{DistrictCooling}\label{districtcooling}
+
+When the user is not interested in a plant simulation or there is some centralized source of chilled water, the following object can be used in the input.
+
+\subsubsection{Inputs}\label{inputs-16-008}
+
+\paragraph{Field: Name}\label{field-name-15-006}
+
+This alpha field contains the identifying name for the district cooling (i.e., purchased chilled water).
+
+\paragraph{Field: Chilled Water Inlet Node Name}\label{field-chilled-water-inlet-node-name-9}
+
+This alpha field contains the identifying name for the district cooling inlet node.
+
+\paragraph{Field: Chilled Water Outlet Node Name}\label{field-chilled-water-outlet-node-name-10}
+
+This alpha field contains the identifying name for the district cooling outlet node.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-10}
+
+This numeric field contains the nominal demand (W) that the district cooling will meet. This field is autosizable.
+
+\paragraph{Field: Capacity Fraction Schedule Name}\label{field-capacity-fraction-schedule-name}
+
+This alpha field contains the name of a schedule that describes how the nominal capacity varies over time.~ Values must non-negative. The capacity at a given point in time is determined by the product of the previous field and the value in this schedule. If the field is omitted or left blank, then the program assumes a schedule value of 1.0 all the time.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+DistrictCooling, Purchased Cooling,
+          NODE_35,NODE_49,
+          68000;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-14-003}
+
+\begin{itemize}
+\item
+  HVAC,Average, District Cooling Chilled Water Rate {[}W{]}
+\item
+  HVAC,Sum, District Cooling Chilled Water Energy {[}J{]}
+\item
+  Zone,Meter, DistrictCooling:Plant {[}J{]}
+\item
+  Zone,Meter,Cooling: DistrictCooling {[}J{]}
+\item
+  HVAC,Average,District Cooling Rate {[}W{]}
+\item
+  HVAC,Average,District Cooling Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,District Cooling Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,District Cooling Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{District Cooling Chilled Water Rate {[}W{]}}\label{district-cooling-chilled-water-rate-w}
+
+\paragraph{District Cooling Chilled Water Energy {[}J{]}}\label{district-cooling-chilled-water-energy-j}
+
+These outputs are the energy taken from purchased chilled water. Consumption is metered on Cooling:DistrictCooling, DistrictCooling:Plant, and DistrictCooling:Facility.
+
+\paragraph{District Cooling Rate {[}W{]}}\label{district-cooling-rate-w}
+
+This is the useful rate of cooling energy from purchased chilled water. For the current algorithm, this is the same as District Cooling Chilled Water Rate.
+
+\paragraph{District Cooling Inlet Temperature {[}C{]}}\label{district-cooling-inlet-temperature-c}
+
+\paragraph{District Cooling Outlet Temperature {[}C{]}}\label{district-cooling-outlet-temperature-c}
+
+\paragraph{District Cooling Mass Flow Rate {[}kg/s{]}}\label{district-cooling-mass-flow-rate-kgs}
+
+These outputs are the supply-side plant loop chilled water inlet and outlet temperatures and mass flow rate.
+
+\subsection{DistrictHeating}\label{districtheating}
+
+When the user is not interested in a plant simulation or there is some centralized source of hot water (district heating), the following object can be used in the input.
+
+\subsubsection{Inputs}\label{inputs-17-006}
+
+\paragraph{Field: Name}\label{field-name-16-006}
+
+This alpha field contains the identifying name for the district heating (i.e., purchased hot water).
+
+\paragraph{Field: Hot Water Inlet Node Name}\label{field-hot-water-inlet-node-name-2}
+
+This alpha field contains the identifying name for the district heating inlet node.
+
+\paragraph{Field: Hot Water Outlet Node Name}\label{field-hot-water-outlet-node-name-2}
+
+This alpha field contains the identifying name for the district heating outlet node.
+
+\paragraph{Field: Nominal Capacity}\label{field-nominal-capacity-11}
+
+This numeric field contains the nominal demand (W) that the district heating will meet. This field is autosizable.
+
+\paragraph{Field: Capacity Fraction Schedule Name}\label{field-capacity-fraction-schedule-name-1}
+
+This alpha field contains the name of a schedule that describes how the nominal capacity varies over time.~ Values must non-negative. The capacity at a given point in time is determined by the product of the previous field and the value in this schedule. If the field is omitted or left blank, then the program assumes a schedule value of 1.0 all the time.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+DistrictHeating,Purchased Heating,
+          NODE_30,NODE_29,
+          1000000;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-15-002}
+
+\begin{itemize}
+\item
+  HVAC,Average,District Heating Hot Water Rate {[}W{]}
+\item
+  HVAC,Sum,District Heating Hot Water Energy {[}J{]}
+\item
+  Zone,Meter,DistrictHeating:Plant {[}J{]}
+\item
+  Zone,Meter,Heating:DistrictHeating {[}J{]}
+\item
+  HVAC,Average,District Heating Rate {[}W{]}
+\item
+  HVAC,Average,District Heating Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,District Heating Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,District Heating Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{District Heating Hot Water Rate {[}W{]}}\label{district-heating-hot-water-rate-w}
+
+\paragraph{District Heating Hot Water Energy {[}J{]}}\label{district-heating-hot-water-energy-j}
+
+These outputs are the energy taken from purchased hot water. Consumption is metered on Heating:DistrictHeating, DistrictHeating:Plant, and DistrictHeating:Facility.
+
+\paragraph{District Heating Rate {[}W{]}}\label{district-heating-rate-w}
+
+This is the useful rate of heating energy from purchased hot water. For the current algorithm, this is the same as District Heating Hot Water Rate.
+
+\paragraph{District Heating Inlet Temperature {[}C{]}}\label{district-heating-inlet-temperature-c}
+
+\paragraph{District Heating Outlet Temperature {[}C{]}}\label{district-heating-outlet-temperature-c}
+
+\paragraph{District Heating Mass Flow Rate {[}kg/s{]}}\label{district-heating-mass-flow-rate-kgs}
+
+These outputs are the supply-side plant loop hot water inlet and outlet temperatures and mass flow rate.
+
+\subsection{PlantComponent:TemperatureSource}\label{plantcomponenttemperaturesource}
+
+This object allows the simulation of a water (or other fluid) source at a user-specified temperature.~ This could include a river, well, or seawater source, or any other configuration where the fluid temperature being supplied by the component to the plant is known.~ The temperature may be a constant or scheduled.~ Of course, the scheduled value may also be overwritten via EMS in cases where the specified temperature should be calculated at run-time.
+
+\subsubsection{Inputs}\label{inputs-18-006}
+
+\paragraph{Field: Name}\label{field-name-17-005}
+
+This field is the string identifier for this component.
+
+\paragraph{Field: Inlet Node}\label{field-inlet-node-000}
+
+This is the name of this component's inlet node for the plant connection.
+
+\paragraph{Field: Outlet Node}\label{field-outlet-node-000}
+
+This is the name of this component's outlet node for the plant connection. The source temperature is applied to this node when the component is active.
+
+\paragraph{Field: Design Volume Flow Rate}\label{field-design-volume-flow-rate}
+
+This numeric field contains the design value for component volume flow rate in m\(^{3}\)/s.~ This field may be autosized.
+
+\paragraph{Field: Temperature Specification Type}\label{field-temperature-specification-type}
+
+This string field specifies the behavior of the source temperature.~ Two inputs are allowed: Constant or Scheduled.~ For a constant condition, a single input value (the next field) is used as the returning temperature (component outlet temperature) throughout the entire simulation.~ For a scheduled condition, the name of a schedule (the following field) is used to allow the temperature to vary throughout the simulation.~ This schedule value may be actuated via EMS to allow further flexibility on temperature specification at run-time.
+
+\paragraph{Field: Source Temperature}\label{field-source-temperature}
+
+If the Temperature Specification Type field is Constant, then the value in this field is used as the source temperature (in C) throughout the entire simulation.
+
+\paragraph{Field: Source Temperature Schedule Name}\label{field-source-temperature-schedule-name}
+
+If the Temperature Specification Type field is Scheduled, then this is the name of a schedule entered in the IDF which specifies the dynamic temperature of this source object. The units of this schedule should be C.
+
+And, as shown in an IDF:
+
+\begin{lstlisting}
+
+PlantComponent:TemperatureSource,
+      FluidSource,             !- Name
+      FluidSource Inlet Node,  !- Inlet Node
+      FluidSource Outlet Node, !- Outlet Node
+      Autosize,                !- Design Volume Flow Rate {m3/s}
+      Constant,                !- Temperature Specification Type
+      62,                      !- Source Temperature {C}
+      ;                        !- Source Temperature Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-16-000}
+
+The following output variables are available for the temperature source plant components:
+
+\begin{itemize}
+\item
+  HVAC,Average,Plant Temperature Source Component Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Plant Temperature Source Component Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Plant Temperature Source Component Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Plant Temperature Source Component Source Temperature {[}C{]}
+\item
+  HVAC,Average,Plant Temperature Source Component Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Plant Temperature Source Component Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Plant Temperature Source Component Mass Flow Rate {[}kg/s{]}}\label{plant-temperature-source-component-mass-flow-rate-kgs}
+
+The current mass flow rate of this component.
+
+\paragraph{Plant Temperature Source Component Inlet Temperature {[}C{]}}\label{plant-temperature-source-component-inlet-temperature-c}
+
+The current entering fluid temperature of this component.
+
+\paragraph{Plant Temperature Source Component Outlet Temperature {[}C{]}}\label{plant-temperature-source-component-outlet-temperature-c}
+
+The current outlet temperature of this component.
+
+\paragraph{Plant Temperature Source Component Source Temperature {[}C{]}}\label{plant-temperature-source-component-source-temperature-c}
+
+The current source temperature of this component.
+
+\paragraph{Plant Temperature Source Component Heat Transfer Rate {[}W{]}}\label{plant-temperature-source-component-heat-transfer-rate-w}
+
+The current heat transfer rate of this component, positive for outlet temperature \textgreater{} inlet temperature, or adding heat to the loop, or absorbing heat from the source.
+
+\paragraph{Plant Temperature Source Component Heat Transfer Energy {[}J{]}}\label{plant-temperature-source-component-heat-transfer-energy-j}
+
+The current heat transfer energy over the given reporting period of this component.
+
+\subsection{CentralHeatPumpSystem}\label{centralheatpumpsystem}
+
+This is a central geothermal application that contains one or more chiller-heaters centrally located in the building; the available chilled and/or hot water is then piped to the individual zones. Chiller-heaters used for this particular system can be of two types: 1) standard vapor-compression, non-reversible cycle chillers designed for heat recovery or 2) reversible-cycle, water-to-water heat pump chillers. Unlike a distributed ground source heat pump configuration where individual heat pumps are located in each zone, a centralized geothermal configuration has one or more chiller-heaters. Its function is to encapsulate the extra controls needed to turn individual chiller-heater modules on/off and whether they are to operate in cooling-only, heating-only or simultaneous cooling-heating mode and whether to connect the source water to the evaporator or condenser side. A variety of control schemes can be designed by setting schedules for both zone control types and individual chiller-heaters schedules.
+
+The fluid used in this central system is usually water, and there is no sharing of condenser or evaporator water between multiple machines. However, the control logic is such that the source water can be delivered to individual chiller-heaters depending on their operating mode, e.g., modules in simultaneous cooling-heating mode receive no source water, modules in heating-only mode can have source water directed to their evaporator, or modules in cooling-only mode can have source water directed to their condenser; the decision on which module(s) receives the source water dictated by the `smart' controls. The following figures illustrate node interconnections between this central geothermal application and plant and condenser loops in various situations.
+
+The order of the multiple chiller-heaters' operation is assumed to be sequential. In other words, the very first chiller-heater will be called at first to see if it meets all loads that the central heat pump system should meet. If the chiller-heater meets all loads, the rest chiller-heaters are assumed to be turned off. If not, the following chiller-heater will be called to meet the remaining loads until all loads are met in the order as defined in the set of individual chiller-heater objects below. The order of individual chiller-heater modules needs to be carefully arranged in case users are intended to see the performance of various combinations of different sizes of chiller-heaters in a central heat pump system.
+
+\begin{figure}[hbtp] % fig 76
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image185.png}
+\caption{Diagram of a central heat pump system with three chiller-heaters in cooling-only mode (Condensers reject heat to the ground source loop) \protect \label{fig:diagram-of-a-central-heat-pump-system-with}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 77
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image186.png}
+\caption{Diagram of a central heat pump system with three chiller-heaters in heat recovery mode         (No heat is exchanged with the ground source loop) \protect \label{fig:diagram-of-a-central-heat-pump-system-with-001}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 78
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image187.png}
+\caption{Diagram of a central heat pump system with one chiller-heater in heat recovery mode and two chiller-heaters in cooling-only mode \protect \label{fig:diagram-of-a-central-heat-pump-system-with-002}}
+\end{figure}
+
+In the above example, the cooling load needs 3 chiller-heaters and the heating load needs 1 chiller heater. Chiller 1 is in heat recovery mode and isolated from the ground source loop while chillers 2 and 3 are in cooling-only mode, their condensers rejecting heat to the ground source loop.
+
+\begin{figure}[hbtp] % fig 79
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image188.png}
+\caption{Diagram of a central heat pump system with two chiller-heaters in heat recovery mode and one chiller-heater in heating-only mode \protect \label{fig:diagram-of-a-central-heat-pump-system-with-003}}
+\end{figure}
+
+In the above example, the heating load needs 3 chiller-heaters and the cooling load needs two chiller-heaters. Chillers 1 and 2 are in heat recovery mode and isolated from the ground source loop while chiller 3 is in heating-only mode, its evaporator extracting heat from the ground source loop.
+
+Users are required to define three different nodes such as chilled water, hot water, and source water nodes. Only this central heat pump system will be metered, and individual chiller-heaters' energy will be available for reporting only, but not metered.
+
+\subsubsection{Inputs}\label{inputs-19-004}
+
+\paragraph{Field: Name}\label{field-name-18-005}
+
+This alpha field contains the identifying name of the central heat pump system.
+
+\paragraph{Field: Control Method}\label{field-control-method}
+
+\paragraph{This field must contain a keyword defines how the central heat pump system controls the interaction between the chiller-heater modules and the water loops to meet the cooling and heating demands. Currently, the only available option isSmartMixing.}\label{this-field-must-contain-a-keyword-defines-how-the-central-heat-pump-system-controls-the-interaction-between-the-chiller-heater-modules-and-the-water-loops-to-meet-the-cooling-and-heating-demands.-currently-the-only-available-option-issmartmixing.}
+
+\paragraph{Field: Cooling Loop Inlet Node Name}\label{field-cooling-loop-inlet-node-name}
+
+This alpha field contains the identifying name of the chilled water inlet node.
+
+\paragraph{Field: Cooling Loop Outlet Node Name}\label{field-cooling-loop-outlet-node-name}
+
+This alpha field contains the identifying name of the chilled water outlet node.
+
+\paragraph{Field: Source Loop Inlet Node Name}\label{field-source-loop-inlet-node-name}
+
+This alpha field contains the identifying name of the source water inlet node.
+
+\paragraph{Field: Source Loop Outlet Node Name}\label{field-source-loop-outlet-node-name}
+
+This alpha field contains the identifying name of the source water outlet node.
+
+\paragraph{Field: Heating Loop Inlet Node Name}\label{field-heating-loop-inlet-node-name}
+
+This alpha field contains the identifying name of the hot water inlet node.
+
+\paragraph{Field: Heating Loop Outlet Node Name}\label{field-heating-loop-outlet-node-name}
+
+This alpha field contains the identifying name of the hot water outlet node.
+
+\paragraph{Field: Ancillary Power}\label{field-ancillary-power-000}
+
+This numeric field contains the ancillary power of the central heat pump system in watts.
+
+\paragraph{Field: Ancillary Operation Schedule Name}\label{field-ancillary-operation-schedule-name}
+
+This alpha field contains the identifying name of the ancillary power schedule.
+
+\paragraph{Field Set: Individual Chiller-Heater Module Objects}\label{field-set-individual-chiller-heater-module-objects}
+
+The following four items are repeated up to a maximum of 20 individual chiller-heater modulesets. At least one module set must appear in an input file. In other words, a central heat pump system must include at least one chiller-heater module component. A set of the following four fields helps to define the specific type of a chiller-heater module, its operation control, and the number of identical chiller-heater module objects.
+
+\paragraph{Field: Chiller Heater Module Performance Component Object Type \textless{}x\textgreater{}}\label{field-chiller-heater-module-performance-component-object-type-x}
+
+This alpha field describes the type of the chiller-heater comprising this module set. Only the chiller-heater type ChillerHeaterPerformance:EIectric:EIR is currently available. Note that up to 20 sets of chiller-heater module name, schedule, and number of identical chiller-heater may be entered for a single central heat pump system.
+
+\paragraph{Field: Chiller Heater Module Performance Component Name \textless{}x\textgreater{}}\label{field-chiller-heater-module-performance-component-name-x}
+
+This alpha field is paired with the preceding chiller-heater module type to define the name of the module.
+
+\paragraph{Field: Chiller Heater Module Control Schedule Name \textless{}x\textgreater{}}\label{field-chiller-heater-module-control-schedule-name-x}
+
+This alpha field is paired with the preceding chiller-heater module type and name to define its on/off control. This schedule will be used for all identical module components as defined in the next field. Currently, this schedule only controls the module set's availability, i.e., schedule values equal to 1 indicate that the chiller-heater set is available while schedule values equal to 0 indicate that the chiller-heater set is off.
+
+\paragraph{Field: Number of Chiller Heater Modules \textless{}x\textgreater{}}\label{field-number-of-chiller-heater-modules-x}
+
+This numeric field is paired with the preceding three fields to define how many identical chiller-heaters define this module set.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+CentralHeatPumpSystem,
+    ChillerBank,             !- Name
+    SmartMixing,             !- Control Method
+    Chiller Inlet Node,      !- Cooling Loop Inlet Node Name
+    Chiller Outlet Node,     !- Cooling Loop Outlet Node Name
+    Condenser Inlet Node,    !- Source Loop Inlet Node Name
+    Condenser Outlet Node,   !- Source Loop Outlet Node Name
+    HWInlet,                 !- Heating Loop Inlet Node Name
+    HWOutlet,                !- Heating Loop Outlet Node Name
+    460,                     !- Ancillary Power {W}
+    ,                        !- Ancillary Operation Schedule Name
+    ChillerHeaterPerformance:Electric:EIR,  !- Chiller Heater Modules Object Type 1
+    ChillerHeaterModule 1,   !- Chiller Heater Modules Performance Component Name 1
+    ON,                      !- Chiller Heater Modules Control Schedule Name 1
+    2,                       !- Number of Chiller Heater Modules 1
+    ChillerHeaterPerformance:Electric:EIR,  !- Chiller Heater Modules Object Type 2
+    ChillerHeaterModule 2,   !- Chiller Heater Modules Performance Component Name 2
+    ON,                      !- Chiller Heater Modules Control Schedule Name 2
+    2;                       !- Number of Chiller Heater Modules 2
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-17-000}
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Heater System Cooling Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater System Cooling Electric Energy{[}J{]}
+\item
+  HVAC,Average,Chiller Heater System Heating Electric Power {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater System Heating Electric Energy{[}J{]}
+\item
+  HVAC,Average,Chiller Heater System Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater System Cooling Energy{[}J{]}
+\item
+  HVAC,Average,Chiller Heater System Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater System Heating Energy{[}J{]}
+\item
+  HVAC,Average,Chiller Heater System Source Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater System Source Heat Transfer Energy{[}J{]}
+\item
+  HVAC,Average,Chiller Heater System Cooling Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater System Cooling Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater System Cooling Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Heater System Heating Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater System Heating Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater System Heating Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Heater System Source Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater System Source Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Chiller Heater System Source Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Chiller Heater System Cooling Electric Power {[}W{]}}\label{chiller-heater-system-cooling-electric-power-w}
+
+\paragraph{Chiller Heater System Cooling Electric Energy {[}J{]}}\label{chiller-heater-system-cooling-electric-energy-j}
+
+These outputs are the sums of the cooling electric power consumption of the central heat pump system containing one or more child objects. Cooling Energy is metered on Cooling:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Chiller Heater System Heating Electric Power {[}W{]}}\label{chiller-heater-system-heating-electric-power-w}
+
+\paragraph{Chiller Heater System Heating Electric Energy {[}J{]}}\label{chiller-heater-system-heating-electric-energy-j}
+
+These outputs are the sums of the heating electric power consumption of the central heat pump system. Heating Energy is metered on Heating:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Chiller Heater System Cooling Rate {[}W{]}}\label{chiller-heater-system-cooling-rate-w}
+
+\paragraph{Chiller Heater System Cooling Energy {[}J{]}}\label{chiller-heater-system-cooling-energy-j}
+
+These outputs are the evaporator heat transfer which is the cooling delivered by the central heat pump system. These are the sums of the evaporator heat transfer of individual chiller-heater modules included in the central heat pump system. Cooling Energy is metered on Chiller:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\paragraph{Chiller Heater System Heating Rate {[}W{]}}\label{chiller-heater-system-heating-rate-w}
+
+\paragraph{Chiller Heater System Heating Energy {[}J{]}}\label{chiller-heater-system-heating-energy-j}
+
+These outputs are the condenser heat transfer which is the heating delivered by the central heat pump system. These are the sums of the condenser heat transfer of individual chiller-heater modules included in the central heat pump system. Heating Energy is metered on Boiler:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\paragraph{Chiller Heater System Source Heat Transfer Rate {[}W{]}}\label{chiller-heater-system-source-heat-transfer-rate-w}
+
+\paragraph{Chiller Heater System Source Heat Transfer Energy {[}J{]}}\label{chiller-heater-system-source-heat-transfer-energy-j}
+
+These outputs are heat transfer which is the heat rejected to a ground source loop or extracted from the source loop, depending on the operating modes of the chiller-heater modules. This is the sums of evaporator heat transfer of the chiller-heater modules in heating-only mode or heating dominant simultaneous cooling-heating mode while the sums of condenser heat transfer of the chiller-heater modules in cooling-only mode or cooling dominant simultaneous cooling-heating mode. Source Heat Transfer Energy is metered on HeatRejection:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
+
+\paragraph{Chiller Heater System Cooling Inlet Temperature {[}C{]}}\label{chiller-heater-system-cooling-inlet-temperature-c}
+
+\paragraph{Chiller Heater System Cooling Outlet Temperature {[}C{]}}\label{chiller-heater-system-cooling-outlet-temperature-c}
+
+\paragraph{Chiller Heater System Cooling Mass Flow Rate {[}kg/s{]}}\label{chiller-heater-system-cooling-mass-flow-rate-kgs}
+
+These outputs are the chilled water inlet and outlet temperatures and flow rate.
+
+\paragraph{Chiller Heater System Heating Inlet Temperature {[}C{]}}\label{chiller-heater-system-heating-inlet-temperature-c}
+
+\paragraph{Chiller Heater System Heating Outlet Temperature {[}C{]}}\label{chiller-heater-system-heating-outlet-temperature-c}
+
+\paragraph{Chiller Heater System Heating Mass Flow Rate {[}kg/s{]}}\label{chiller-heater-system-heating-mass-flow-rate-kgs}
+
+These outputs are the hot water inlet and outlet temperatures and flow rate.
+
+\paragraph{Chiller Heater System Source Inlet Temperature {[}C{]}}\label{chiller-heater-system-source-inlet-temperature-c}
+
+\paragraph{Chiller Heater System Source Outlet Temperature {[}C{]}}\label{chiller-heater-system-source-outlet-temperature-c}
+
+\paragraph{Chiller Heater System Source Mass Flow Rate {[}kg/s{]}}\label{chiller-heater-system-source-mass-flow-rate-kgs}
+
+These outputs are the source water inlet and outlet temperatures and flow rate.
+
+\subsection{ChillerHeaterPerformance:EIectric:EIR}\label{chillerheaterperformanceeiectriceir}
+
+The performance of the chiller-heater will be defined by two sets of curves meant to describe unloading for: 1) cooling-only mode, and 2) heating-only mode or simultaneous cooling-heating mode. Reference conditions must be defined for both because each has its own set of three unloading curves based on their associated reference conditions. The cooling-mode curves are typically (but not always) based on condenser entering water temperature while the heating-only mode curves are typically based on condenser leaving water temperature. This chiller-heater object allows the user to specify whether to use condenser leaving or condenser entering as a dependent variable to differentiate, if necessary, the condenser temperature basis used to generate the cooling- and heating-only mode curves.
+
+\subsubsection{Field: Name}\label{field-name-19-002}
+
+This alpha field contains the identifying name of the chiller-heater to be included in a central heat pump system.
+
+\subsubsection{Field: Reference Cooling Mode Evaporator Capacity}\label{field-reference-cooling-mode-evaporator-capacity}
+
+This numeric field contains the reference cooling capacity of the evaporator in cooling mode in Watts. This value should be based on the reference temperatures and design water flow rates defined below. This field can be autosized.
+
+\subsubsection{Field: Reference Cooling Mode COP}\label{field-reference-cooling-mode-cop}
+
+This numeric field contains the reference coefficient of performance of the evaporator for cooling. It must be based on the values of Reference Cooling Mode Leaving Chilled Water Temperature and Reference Cooling Mode Entering Condenser Water Temperature defined in the next two fields.
+
+\subsubsection{Field: Reference Cooling Mode Leaving Chilled Water Temperature}\label{field-reference-cooling-mode-leaving-chilled-water-temperature}
+
+This numeric field contains the reference leaving chilled water temperature of the evaporator for cooling in Celsius. The default value is 6.67°C.
+
+\subsubsection{Field: Reference Cooling Mode Entering Condenser Water Temperature}\label{field-reference-cooling-mode-entering-condenser-water-temperature}
+
+This numeric field contains the reference entering condenser water temperature of the condenser in the cooling mode in Celsius. The default value is 29.4°C.
+
+\subsubsection{Field: Reference Cooling Mode Leaving Condenser Water Temperature}\label{field-reference-cooling-mode-leaving-condenser-water-temperature}
+
+This numeric field contains the reference leaving condenser water temperature of the condenser in the cooling mode in Celsius. The default value is 35.0°C.
+
+\subsubsection{Field: Reference Heating Mode Cooling Capacity Ratio}\label{field-reference-heating-mode-cooling-capacity-ratio}
+
+This numeric field contains the evaporator's capacity during the reference heating-only or simultaneous cooling-heating mode as a ratio of reference cooling capacity. For example, the ratio may be expressed as follows:
+
+\begin{equation}
+Ratio = \frac{{EvapCapHt{g_{@Tchw,l = 6.67C,Tcond,l = 51.67C}}}}{{EvapCapC{{\lg }_{@Tchw,l = 6.67C,Tcond,l = 35.0C}}}}
+\end{equation}
+
+where Tchw,l is the leaving chilled water temperature and Tcond,l is the leaving condenser water temperature representing the heating-mode and cooling-mode reference temperatures defined elsewhere in this object.
+
+The default is 0.75. This field is used to determine evaporator capacity in heating-only mode or simultaneous cooling-heating mode, multiplying it by the value entered in the field of the Reference Cooling Mode Evaporator Capacity. Note that even when there is no cooling load, i.e., the machine is in heating-only mode, the evaporator must still run and extract heat from the source water. In heating-only mode, the leaving chilled water temperature (Tchw,l) may ~float depending on the evaporator water flow rate and the source water temperature. In simultaneous cooling and heating mode, the leaving chilled water temperature (Tchw,l) does not float but is determined by the chilled water setpoint controls. For both heating-only and simultaneous cooling and heating mode, the leaving condenser temperature (Tcond,l) is determined by the hot water supply setpoint controls. This value of Tchw,l, combined with Tcond,l is plugged into the CAPFT and EIRFT curves to determine the off-rated heating-mode evaporator capacity and associated compressor power.
+
+\subsubsection{Field: Reference Heating Mode Cooling Power Ratio}\label{field-reference-heating-mode-cooling-power-ratio}
+
+This numeric field contains the compressor power during simultaneous cooling-heating mode as a ratio of reference cooling compressor power. For example, the ratio may be expressed as follows:
+
+\begin{equation}
+Ratio = \frac{{Powe{r_{@Tchw,l = 6.67C,Tcond,l = 51.67C}}}}{{Powe{r_{@Tchw,l = 6.67C,Tcond,l = 35.0C}}}}
+\end{equation}
+
+The default value is 1.5. This field is used to determine full load compressor power at the simultaneous cooling-heating mode's reference chilled water leaving and condenser water leaving temperatures. Note: In heating-only mode, the chilled water leaving temperature floats so the EIRFT curve is used to modify the simultaneouos cooling-heating full load compressor power value.
+
+\subsubsection{Field: Reference Heating Mode Leaving Chilled Water Temperature}\label{field-reference-heating-mode-leaving-chilled-water-temperature}
+
+This numeric field contains the reference leaving chilled water temperature of the evaporator in simultaneous cooling-heating mode in Celsius. This is typically the same as the reference cooling mode value and is used to create the heating-only mode and simultaneous cooling-heating mode unloading curves. The leaving chilled water temperature for the chiller-heater is not allowed to fall below this value during the heating-only mode and simultaneous cooling-heating mode. The default value is 6.67°C.
+
+\subsubsection{Field: Reference Heating Mode Leaving Condenser Water Temperature}\label{field-reference-heating-mode-leaving-condenser-water-temperature}
+
+This numeric field contains the reference leaving condenser water temperature of the condenser in heating mode in Celsius. This field is typically controlled to the design hot water supply temperature, and used to create the heating-only mode and simultaneous cooling-heating mode unloading curves. The default value is 60.0°C.
+
+\subsubsection{Field: Reference Heating Mode Entering Condenser Water Temperature}\label{field-reference-heating-mode-entering-condenser-water-temperature}
+
+This numeric field contains the reference entering condenser water temperature of the condenser in heating mode in Celsius. This field typically represents the upper limit of the source water temperature. The default value is 29.44°C.
+
+\subsubsection{Field: Heating Mode Entering Chilled Water Temperature Low Limit}\label{field-heating-mode-entering-chilled-water-temperature-low-limit}
+
+This numeric field contains the low limit of the entering chilled water temperature in heating-only mode or simultaneous cooling-heating mode in Celsius. This field typically represents the lower limit of the source water temperature. If necessary, auxiliary heat will be activated to prevent source water temperature falling below the chilled water entering minimum. The default value is 12.2°C.
+
+\subsubsection{Field: Chilled Water Flow Mode Type}\label{field-chilled-water-flow-mode-type}
+
+This alpha field contains the chilled water flow control mode. Valid water flow mode includes constant flow and variable flow, and the default water flow mode is constant flow.
+
+\subsubsection{Field: Design Chilled Water Flow Rate}\label{field-design-chilled-water-flow-rate-8}
+
+This numeric field contains the design chilled water flow rate in m\(^{3}\)/s. The minimum value for this field must be greater than zero, and this field is autosizable.
+
+\subsubsection{Field: Design Condenser Water Flow Rate}\label{field-design-condenser-water-flow-rate-7}
+
+This numeric field contains the design condenser water flow rate in m\(^{3}\)/s. The minimum value for this field must be greater than zero, and this field is autosizable.
+
+\subsubsection{Field: Design Hot Water Flow Rate}\label{field-design-hot-water-flow-rate-2}
+
+This numeric field contains the design hot water flow rate in m\(^{3}\)/s. The minimum value and default value for this field are zero, and this field is autosizable.
+
+\subsubsection{Field: Compressor Motor Efficiency}\label{field-compressor-motor-efficiency}
+
+This numeric field contains the fraction of efficiency of the compressor electrical energy consumption that must be rejected by the condenser. This value must be between 0.0 and 1.0, and the default value is 1.0.
+
+\subsubsection{Field: Condenser Type}\label{field-condenser-type-7}
+
+This alpha field contains the type of condenser. WaterCooled is the only valid type, and it requires the full specification of the condenser loop and its associated equipment.
+
+\subsubsection{Field: Cooling Mode Temperature Curve Condenser Water Independent Variable}\label{field-cooling-mode-temperature-curve-condenser-water-independent-variable}
+
+This alpha field determines whether the entering or leaving condenser water temperature is used in the cooling mode unloading performance curves that follow. Valid variables include EnteringCondenser and LeavingCondenser, and the default variable is EnteringCondenser. The condenser temperature used for the cooling mode unloading performance curves will be dependent on this field input. For example, leaving condenser water temperature will be used when the LeavingCondenser is chosen, otherwise entering condenser water temperature.
+
+\subsubsection{Field: Cooling Mode Cooling Capacity Function of Temperature Curve Name}\label{field-cooling-mode-cooling-capacity-function-of-temperature-curve-name}
+
+This alpha field contains the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the evaporator capacity as a function of the leaving chilled water temperature and either the entering condenser water temperature or the leaving condenser water temperature as defined in the previous field. It is then multiplied by the reference evaporator capacity to give the cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\subsubsection{Field: Cooling Mode Electric Input to Cooling Output Ratio Function of Temperature Curve Name}\label{field-cooling-mode-electric-input-to-cooling-output-ratio-function-of-temperature-curve-name}
+
+This alpha field contains the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and either the entering condenser water temperature or the leaving condenser water temperature as defined by the user. The EIR is the inverse of the COP. It is then multiplied by the reference EIR (inverse of the reference COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\subsubsection{Field: Cooling Mode Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name}\label{field-cooling-mode-electric-input-to-cooling-output-ratio-function-of-part-load-ratio-curve-name}
+
+This alpha field contains the name of a performance curve (ref: Performance Curves) that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the part-load ratio (EIRFPLR). The EIR is the inverse of the COP, and the part-load ratio is the actual cooling load divided by the available cooling capacity of the chiller-heater. This curve is generated by dividing the operating electric input power by the available full-load capacity at the specific operating temperatures. The curve output should decrease from 1 towards 0 as part-load ratio decreases from 1 to 0. Note that the bi-cubic formulation is generally only valid when LeavingCondenser variable is chosen for the field of Cooling Mode Condenser Water Temperature Curve Input Variable whereas the quadratic curve can be used both choices, i.e., LeavingCondenser and EnteringCondenser. The output of this curve is then multiplied by the reference full-load EIR and the EIRFT to give the EIR at the specific temperatures and part-load ratio at which the chiller-heater is operating. This curve should have a value of 1.0 when the part-load ratio equals 1.0. The curve should be valid for the range of part-load ratios anticipated for the simulation.
+
+\subsubsection{Field: Cooling Mode Cooling Capacity Optimum Part Load Ratio}\label{field-cooling-mode-cooling-capacity-optimum-part-load-ratio}
+
+This numeric field contains the chiller-heater's optimum part-load ratio. This is the part-load ratio at which the chiller-heater performs at its maximum COP. The optimum part-load ratio must be greater than or equal to the minimum part-load ratio, and less than or equal to the maximum part-load ratio. (Note: Both the minimum part-load ratio and maximum part-load ratio are taken from the Cooling Mode EIRFPLR curve definition.) The default value is 1.0.
+
+\subsubsection{Field: Heating Mode Temperature Curve Condenser Water Independent Variable}\label{field-heating-mode-temperature-curve-condenser-water-independent-variable}
+
+This alpha field determines whether the entering or leaving condenser water temperature is used in the heating mode unloading performance curves that follow. Valid variables include EnteringCondenser and LeavingCondenser, and the default variable is EnteringCondenser. The condenser temperature used for the cooling mode unloading performance curves will be dependent on this field input. For example, leaving condenser water temperature will be used when the LeavingCondenser is chosen, otherwise entering condenser water temperature.
+
+\subsubsection{Field: Heating Mode Cooling Capacity Function of Temperature Curve Name}\label{field-heating-mode-cooling-capacity-function-of-temperature-curve-name}
+
+This alpha field contains the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the evaporator capacity in heating mode as a function of the leaving chilled water temperature and either the entering condenser water temperature or the leaving condenser water temperature as defined in the previous field. This curve is used to evaluate the adjusted evaporator capacity during heating-only mode or simultaneous cooling-heating mode. This adjusted capacity is used as part of the cooling part-load calculation for the EIRFPLR curve. It is then multiplied by the reference evaporator capacity to give the cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\subsubsection{Field: Heating Mode Electric Input to Cooling Output Ratio Function of Temperature Curve Name}\label{field-heating-mode-electric-input-to-cooling-output-ratio-function-of-temperature-curve-name}
+
+This alpha field contains the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and either the entering condenser water temperature or the leaving condenser water temperature as defined by the user. The EIR is the inverse of the COP. It is then multiplied by the reference EIR (inverse of the reference COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
+
+\subsubsection{Field: Heating Mode Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name}\label{field-heating-mode-electric-input-to-cooling-output-ratio-function-of-part-load-ratio-curve-name}
+
+This alpha field contains the name of a performance curve (ref: Performance Curves) that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the part-load ratio (EIRFPLR). The EIR is the inverse of the COP, and the part-load ratio is the actual evaporator load divided by the available evaporator capacity of the chiller-heater at the reference heating and simultaneous cooling-heating mode temperatures. This curve is generated by dividing the operating electric input power by the available full-load capacity (do not divide by load) at the specific operating temperatures. The curve output should decrease from 1 towards 0 as part-load ratio decreases from 1 to 0. Note that the bicubic formulation below can only be used when the chiller-heater uses a variable speed compressor motor drive. It is also generally valid only when LeavingCondenser variable is chosen for the field of Cooling Mode Condenser Water Temperature Curve Input Variable whereas the quadratic curve can be used both choices, i.e., LeavingCondenser and EnteringCondenser. The output of this curve is then multiplied by the reference full-load EIR (inverse of the reference COP) and the EIRFT to give the EIR at the specific temperatures and part-load ratio at which the chiller-heater is operating. This curve should have a value of 1.0 when the part-load ratio equals 1.0. The curve should be valid for the range of part-load ratios anticipated for the simulation.
+
+\subsubsection{Field: Heating Mode Cooling Capacity Optimum Part Load Ratio}\label{field-heating-mode-cooling-capacity-optimum-part-load-ratio}
+
+This numeric field contains the chiller-heater's optimum part-load ratio during heating-only mode or simultaneous cooling-heating mode. This is the part-load ratio at which the chiller-heater performs at its maximum COP. The optimum part-load ratio must be greater than or equal to the minimum part-load ratio, and less than or equal to the maximum part-load ratio. (Note: Both the minimum part-load ratio and maximum part-load ratio are taken from the Heating Mode EIRFPLR curve definition.) The default value is 1.0.
+
+\subsubsection{Field: Sizing Factor}\label{field-sizing-factor-12}
+
+This optional numeric field allows the user to specify a sizing factor for this component. The Sizing Factor is a multiplier on the design plant chilled water loop flow rate associated with the chiller-heaters parent CentralHeatPumpSystem object. The chiller-heater's modified chilled water flow can then be used to autocalculate the Design Condenser Water Flow Rate and Reference Cooling Mode Evaporator Capacity values. In general, it is best to autosize all three fields or set fixed values for all three fields.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+ChillerHeaterPerformance:Electric:EIR,
+    ChillerHeaterModule 1,   !- Name
+    12500,                   !- Reference Cooling Mode Evaporator Capacity {W}
+    1.5,                     !- Reference Cooling Mode COP {W/W}
+    6.67,                    !- Reference Cooling Mode Leaving Chilled Water Temperature {C}
+    29.4,                    !- Reference Cooling Mode Entering Condenser Fluid Temperature {C}
+    35.0,                    !- Reference Cooling Mode Leaving Condenser Water Temperature {C}
+    0.74,                    !- Reference Heating Mode Cooling Capacity Ratio
+    1.38,                    !- Reference Heating Mode Cooling Power Input Ratio
+    6.67,                    !- Reference Heating Mode Leaving Chilled Water Temperature {C}
+    60,                      !- Reference Heating Mode Leaving Condenser Water Temperature {C}
+    29.44,                   !- Reference Heating Mode Entering Condenser Fluid Temperature {C}
+    5,                       !- Heating Mode Entering Chilled Water Temperature Low Limit {C}
+    VariableFlow,            !- Chilled Water Flow Mode Type
+    0.0003525,               !- Design Chilled Water Flow Rate {m$^{3}$/s}
+    0.0005525,               !- Design Condenser Water Flow Rate {m$^{3}$/s}
+    0.0003525,               !- Design Hot Water Flow Rate {m$^{3}$/s}
+    1,                       !- Compressor Motor Efficiency
+    WaterCooled,             !- Condenser Type
+    EnteringCondenser,       !- Cooling Mode Temperature Curve Condenser Water Independent Variable
+    ChillerHeaterClgCapFT,   !- Cooling Mode Cooling Capacity Function of Temperature Curve Name
+    ChillerHeaterClgEIRFT,   !- Cooling Mode Electric Input to Cooling Output Ratio Function of
+                                !-   Temperature Curve Name
+    ChillerHeaterClgEIRFPLR, !- Cooling Mode Electric Input to Cooling Output Ratio Function of Part Load
+                         !-   Ratio Curve Name
+    1,                       !- Cooling Mode Cooling Capacity Optimum Part Load Ratio
+    LeavingCondenser,        !- Heating Mode Temperature Curve Condenser Water Independent Variable
+    ChillerHeaterHtgCapFT,   !- Heating Mode Cooling Capacity Function of Temperature Curve Name
+    ChillerHeaterHtgEIRFT,   !- Heating Mode Electric Input to Cooling Output Ratio Function of
+                               !-   Temperature Curve Name
+    ChillerHeaterHtgEIRFPLR, !- Heating Mode Electric Input to Cooling Output Ratio Function of Part Load
+                               !-   Ratio Curve Name
+    1,                       !- Heating Mode Cooling Capacity Optimum Part Load Ratio
+    1;                       !- Sizing Factor
+\end{lstlisting}
+
+\subsection{ChillerHeaterPerformance:Electric:EIR Outputs}\label{chillerheaterperformanceelectriceir-outputs}
+
+\begin{itemize}
+\item
+  HVAC,Average,Chiller Heater Operation Mode Unit \textless{}x\textgreater{} {[]}
+\item
+  HVAC,Average,Chiller Heater Part Load Ratio Unit \textless{}x\textgreater{} {[]}
+\item
+  HVAC,Average,Chiller Heater Cycling Ratio Unit \textless{}x\textgreater{} {[]}
+\item
+  HVAC,Average,Chiller Heater Cooling Electric Power Unit \textless{}x\textgreater{} {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Cooling Electric Energy Unit \textless{}x\textgreater{} {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Heating Electric Power Unit \textless{}x\textgreater{} {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Heating Electric Energy Unit \textless{}x\textgreater{} {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Cooling Rate Unit \textless{}x\textgreater{} {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Cooling Energy Unit \textless{}x\textgreater{} {[}J{]}
+\item
+  HVAC,Average,Chiller Heater False Load Heat Transfer Rate Unit \textless{}x\textgreater{} {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater False Load Heat Transfer Energy Unit \textless{}x\textgreater{} {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Condenser Heat Transfer Rate Unit \textless{}x\textgreater{} {[}W{]}
+\item
+  HVAC,Sum,Chiller Heater Condenser Heat Transfer Energy Unit \textless{}x\textgreater{} {[}J{]}
+\item
+  HVAC,Average,Chiller Heater Evaporator Inlet Temperature Unit \textless{}x\textgreater{} {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Evaporator Outlet Temperature Unit \textless{}x\textgreater{} {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Evaporator Mass Flow Rate Unit \textless{}x\textgreater{} {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Heater Condenser Inlet Temperature Unit \textless{}x\textgreater{} {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Condenser Outlet Temperature Unit \textless{}x\textgreater{} {[}C{]}
+\item
+  HVAC,Average,Chiller Heater Condenser Mass Flow Rate Unit \textless{}x\textgreater{} {[}kg/s{]}
+\item
+  HVAC,Average,Chiller Heater COP Unit \textless{}x\textgreater{} {[]}
+\item
+  HVAC,Average,Chiller Heater Capacity Temperature Modifier Multiplier Unit \textless{}x\textgreater{} {[]}
+\item
+  HVAC,Average,Chiller Heater EIR Temperature Modifier Multiplier Unit \textless{}x\textgreater{} {[]}
+\item
+  HVAC,Average,Chiller Heater EIR Part Load Modifier Multiplier Unit \textless{}x\textgreater{} {[]}
+\end{itemize}
+
+Note that much of these output variables are adapted from the definitions above under ``Generic Chiller Outputs'' and ``Electric EIR Chiller Outputs.'' The following outputs are repeated up to the maximum of individual chiller-heater module objects. The maximum number may be different from the number of object defined in this object when users define two or more identical chiller-heater modules for a single chiller heater object in the central heat pump system.
+
+\subsubsection{\texorpdfstring{Chiller Heater Operation Mode Unit \textless{}x\textgreater{} \protect\hyperlink{section-1}{~}}{Chiller Heater Operation Mode Unit \textless{}x\textgreater{} ~}}\label{chiller-heater-operation-mode-unit-x}
+
+This output represents the operating mode of the chiller-heater module. Two single mode outputs and three simultaneous cooling-heating mode outputs are possible:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{-1}
+\item
+  off
+\item
+  cooling-only mode
+\item
+  heating-only mode
+\item
+  heat recovery mode
+\item
+  cooling dominant simultaneous cooling-heating mode
+\item
+  heating dominant simultaneous cooling-heating mode.
+\end{enumerate}
+
+The first mode 0 is reported when the chiller-heater is turned off. The next two modes 2 and 3 are reported when the chiller-heater provides only either cooling or heating, respectively. The last three modes 3 to 5 indicate when the chiller-heater is in a simultaneous cooling-heating mode. Mode 3 indicates the chiller-heaters provides simultaneous cooling and heating \textbf{\emph{without}} heat exchange with the ground source. Mode 4 denotes that at least one of the chiller-heater modules in the central heat pump system provides both cooling and heating, and the chiller-heater is meeting remaining cooling demand (see Figure~\ref{fig:diagram-of-a-central-heat-pump-system-with-002}. Diagram of a central heat pump system with one chiller-heater in heat recovery mode and two chiller-heaters in cooling-only mode) Similarly, mode 5 indicates that at least one of the chiller-heater modules in the central heat pump system is in the heat recovery mode, and the chiller-heater is meeting remaining heating demand (see Figure~\ref{fig:diagram-of-a-central-heat-pump-system-with-003}).
+
+Note that the decision to operate individual chiller-heater modules is solely dependent on the chiller-heater schedule and loads. A fraction may appear in case the chiller-heater mode varies within a zone time step. In this particular case, users may define a detailed reporting frequency for this output variable.
+
+\subsubsection{\texorpdfstring{Chiller Heater Part Load Ratio Unit \textless{}x\textgreater{} \protect\hyperlink{section-1}{~}}{Chiller Heater Part Load Ratio Unit \textless{}x\textgreater{} ~}}\label{chiller-heater-part-load-ratio-unit-x}
+
+This output is the ratio of the evaporator heat transfer rate plus the false load heat transfer rate (if applicable) to the available chiller-heater capacity. This value is used to determine ChillerEIRFPLR.
+
+\subsubsection{\texorpdfstring{Chiller Heater Cycling Ratio Unit \textless{}x\textgreater{} \protect\hyperlink{section-1}{~}}{Chiller Heater Cycling Ratio Unit \textless{}x\textgreater{} ~}}\label{chiller-heater-cycling-ratio-unit-x}
+
+The cycling ratio is the amount of time the chiller-heater operates during each simulation time step. If the chiller-heater part-load ratio falls below the minimum part-load ratio, the chiller-heater cycles on and off to meet the loads.
+
+\subsubsection{Chiller Heater Cooling Electric Power Unit \textless{}x\textgreater{} {[}W{]}}\label{chiller-heater-cooling-electric-power-unit-x-w}
+
+\subsubsection{Chiller Heater Cooling Electric Energy Unit \textless{}x\textgreater{} {[}J{]}}\label{chiller-heater-cooling-electric-energy-unit-x-j}
+
+These outputs are the cooling electric power consumption of the chiller-heater.
+
+\subsubsection{Chiller Heater Heating Electric Power Unit \textless{}x\textgreater{} {[}W{]}}\label{chiller-heater-heating-electric-power-unit-x-w}
+
+\subsubsection{Chiller Heater Heating Electric Energy Unit \textless{}x\textgreater{} {[}J{]}}\label{chiller-heater-heating-electric-energy-unit-x-j}
+
+These outputs are the heating electric power consumption of the chiller-heater.
+
+\subsubsection{Chiller Heater Cooling Rate Unit \textless{}x\textgreater{} {[}W{]}}\label{chiller-heater-cooling-rate-unit-x-w}
+
+\subsubsection{Chiller Heater Cooling Energy Unit \textless{}x\textgreater{} {[}J{]}}\label{chiller-heater-cooling-energy-unit-x-j}
+
+These outputs are the evaporator heat transfer which is the cooling delivered by the chiller-heater module.
+
+\subsubsection{Chiller Heater False Load Heat Transfer Rate Unit \textless{}x\textgreater{} {[}W{]}}\label{chiller-heater-false-load-heat-transfer-rate-unit-x-w}
+
+\subsubsection{Chiller Heater False Load Heat Transfer Energy Unit \textless{}x\textgreater{} {[}J{]}}\label{chiller-heater-false-load-heat-transfer-energy-unit-x-j}
+
+These outputs are the heat transfer rate and total heat transfer due to false loading of the chiller-heater. When the chiller-heater part-load ratio is below the minimum unloading ratio, the chiller-heater false loads (e.g.~hot-gas bypass) to further reduce capacity.
+
+\subsubsection{Chiller Heater Condenser Heat Transfer Rate Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-condenser-heat-transfer-rate-unit-x-c}
+
+\subsubsection{Chiller Heater Condenser Heat Transfer Energy Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-condenser-heat-transfer-energy-unit-x-c}
+
+These outputs are the heat transfer which is the heating delivered by the chiller-heater module in heating mode.
+
+\subsubsection{Chiller Heater Evaporator Inlet Temperature Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-evaporator-inlet-temperature-unit-x-c}
+
+\subsubsection{Chiller Heater Evaporator Outlet Temperature Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-evaporator-outlet-temperature-unit-x-c}
+
+\subsubsection{Chiller Heater Evaporator Mass Flow Rate Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-evaporator-mass-flow-rate-unit-x-c}
+
+These outputs are the evaporator water inlet and outlet temperatures and flow rate. Note that these represent the chilled water temperatures and flow rate in cooling mode or the source water temperature and flow rate in heating mode.
+
+\subsubsection{Chiller Heater Condenser Inlet Temperature Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-condenser-inlet-temperature-unit-x-c}
+
+\subsubsection{Chiller Heater Condenser Outlet Temperature Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-condenser-outlet-temperature-unit-x-c}
+
+\subsubsection{Chiller Heater Condenser Mass Flow Rate Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-condenser-mass-flow-rate-unit-x-c}
+
+These outputs are the condenser water inlet and outlet temperatures and flow rate. Note that these represent the hot water temperatures and flow rate in heating mode or the source water temperature and flow rate in cooling mode.
+
+\subsubsection{Chiller Heater COP Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-cop-unit-x-c}
+
+This output is the coefficient of performance for the chiller-heater. It is calculated as the evaporator heat transfer rate divided by the chiller-heater electric power.
+
+\subsubsection{Chiller Heater Capacity Temperature Modifier Multiplier Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-capacity-temperature-modifier-multiplier-unit-x-c}
+
+This is the output of the curve object Cooling Capacity Function of Temperature Curve.
+
+\subsubsection{Chiller Heater EIR Temperature Modifier Multiplier Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-eir-temperature-modifier-multiplier-unit-x-c}
+
+This is the output of the curve object Electric Input to Cooling Output Ratio Function of Temperature Curve.
+
+\subsubsection{Chiller Heater EIR Part Load Modifier Multiplier Unit \textless{}x\textgreater{} {[}C{]}}\label{chiller-heater-eir-part-load-modifier-multiplier-unit-x-c}
+
+This is the output of the curve object Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve.
+
+\subsection{Thermal Storage Objects}\label{thermal-storage-objects}
+
+There are four types of cold thermal storage objects:
+
+\begin{itemize}
+\item
+  ThermalStorage:Ice:Simple
+\item
+  ThermalStorage:Ice:Detailed
+\item
+  ThermalStorage:ChilledWater:Mixed
+\item
+  ThermalStorage:ChilledWater:Stratified
+\end{itemize}
+
+These objects are typically placed on the supply side of a primary chilled water loop in series or in parallel with one or more chillers.~ Using the the component set point (PlantEquipmentOperation:ComponentSetpoint) plant operation scheme type, the chiller and storage tank setpoints are used to control operation. Using a SetpointManager:Scheduled object (or other appropriate type of set point manager), the setpoints on the chiller outlet node and the ice storage outlet node can be used to control how the cooling load is shared and when charging of storage occurs.~ Example setpoints to use for various modes of operation are shown in the table below:
+
+\begin{longtable}[c]{p{3.0in}p{1.5in}p{1.5in}}
+\toprule 
+Mode & Chiller Setpoint & Storage Setpoint \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Mode & Chiller Setpoint & Storage Setpoint \tabularnewline
+\midrule
+\endhead
+
+Charging ice storage tank & -5C & 7C \tabularnewline
+Cooling with chiller only & 7C & 99C \tabularnewline
+Cooling with chiller and storage (fully load chiller before using storage)) & 7C & 7C \tabularnewline
+Cooling with chiller and storage (chiller carries portion of load, valid if chiller is upstream of storage) & 10C & 7C \tabularnewline
+\bottomrule
+\end{longtable}
+
+Example files have been developed for three common storage configurations:
+
+1.~Series -- Chiller Upstream:~ In this configuration, a chiller is placed first on the same branch as the storage unit and both use the \textbf{SeriesActive} branch control type.
+
+2.~Series -- Chiller Downstream:~ In this configuration, a chiller is placed second on the same branch as the storage unit and both use the \textbf{SeriesActive} branch control type.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{2}
+\tightlist
+\item
+  Parallel:~ In this configuration, the chiller is on a branch parallel to the storage unit branch when it is not charging.~ During charging mode, valves will be changed so that the chiller is in series upstream of the storage.~ To accomplish this in EnergyPlus, the chiller must be modeled using two different chiller objects to represent the same chiller.~ One chiller object on a parallel branch operates only when storage is not being charged.~ The other chiller object, in series upstream of the storage unit operates only during charging mode.
+\end{enumerate}
+
+Other considerations for applying cold thermal storage objects include:
+
+\begin{itemize}
+\item
+  In the PlantLoop object, the ``Minimum Loop Temperature'' must be set equal to or less than the lowest setpoint to be used anywhere in the loop.
+\item
+  To end the storage charging cycle, use a AvailabilityManager:LowTemperatureTurnOff to shut off the primary chilled water loop when the temperature leaving the storage tank nears the charging mode chiller setpoint indicating that the tank is fully charged.~ For example, if the chiller is set to provide --5C chilled water during charging, then charging can be shut down when the water temperature leaving the storage unit reaches --4C.~ When using a primary-secondary loop arrangement, it may be necessary to schedule this availability manager to be active only when the HVAC systems are off to avoid fighting between the demand controls and the availability manager.
+\end{itemize}
+
+\subsection{ThermalStorage:Ice:Simple}\label{thermalstorageicesimple}
+
+This thermal storage model is based on a simple simulation of an ice storage tank with a fixed capacity.~ The tank is charged, or frozen, in an ice-on-coil configuration where ice builds up on the outside of the tubes carrying the brine or glycol solution from the chiller.~ There are two discharge (melt) options, internal or external.~ Internal melt uses the same fluid tubes for charging and discharging.~ External melt uses a separate fluid path for discharge such that the outer layers of ice melt first.~ The ice storage model includes an implied 3-way valve to control the amount if charge/discharge based on the incoming water temperature and the outlet node setpoint temperature.~ The storage tank is assumed to be fully charged (full of ice) at the beginning of each environment.~ The tank is then allowed to charge and discharge during the warmup days of the environment.~ The tank is best controlled using the PlantEquipmentOperation:ComponentSetpoint plant operation scheme, and requires that a setpoint be placed by a set point manager on the ice storage Plant Outlet Node.
+
+The input fields for the object are described in detail below:
+
+\subsubsection{Inputs}\label{inputs-20-004}
+
+\paragraph{Field: Name}\label{field-name-20-001}
+
+This alpha field contains the identifying name for the ice storage tank.
+
+\paragraph{Field: Ice Storage Type}\label{field-ice-storage-type}
+
+This alpha field specifies the type of ice storage tank to be modeled. There are two options:~ ``\textbf{IceOnCoilInternal}'' models ice-on-coil, internal melt.``IceOnCoilExternal'' models ice-on-coil, external melt.
+
+\paragraph{Field: Capacity}\label{field-capacity-000}
+
+This numeric field contains the nominal capacity of the ice storage in GJ (Giga is 10\(^{9}\)).
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-004}
+
+This alpha field specifies the name of the chilled water inlet node.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-005}
+
+This alpha field specifies the name of the chilled water outlet node.
+
+Following is an example input for the THERMAL STORAGE:ICE:SIMPLE object.
+
+\begin{lstlisting}
+
+ThermalStorage:Ice:Simple,
+      ITS,                     !- Ice Storage Name
+      IceOnCoilInternal,       !- Ice Storage Type
+      1.5,                     !- Ice Storage Capacity {GJ}
+      ITS Inlet Node,          !- Plant Loop Inlet Node
+      ITS Outlet Node;         !- Plant Loop Outlet Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-18-000}
+
+The following outputs are available for simple Ice Storage model:
+
+\begin{itemize}
+\item
+  HVAC,Average,Ice Thermal Storage Requested Load {[}W{]}
+\item
+  Zone,Average,Ice Thermal Storage End Fraction{[]}
+\item
+  HVAC,Average,Ice Thermal Storage Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Ice Thermal Storage Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Ice Thermal Storage Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Ice Thermal Storage Cooling Discharge Rate {[}W{]}
+\item
+  HVAC,Sum,Ice Thermal Storage Cooling Discharge Energy {[}J{]}
+\item
+  HVAC,Average,Ice Thermal Storage Cooling Charge Rate {[}W{]}
+\item
+  HVAC,Sum,Ice Thermal Storage Cooling Charge Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Ice Thermal Storage Requested Load {[}W{]}}\label{ice-thermal-storage-requested-load-w}
+
+The load requested by the plant control scheme. A positive value indicates a cooling load or a request to discharge (melt) the tank. A negative value indicates a request to charge (freeze) the tank.
+
+\paragraph{\texorpdfstring{Ice Thermal Storage End Fraction {[]}}{Ice Thermal Storage End Fraction }}\label{ice-thermal-storage-end-fraction}
+
+The fraction of full ice storage which is present at the end of the current HVAC timestep. When reported at a frequency less than detailed, this value is averaged over the reporting period.
+
+\paragraph{Ice Thermal Storage Mass Flow Rate {[}kg/s{]}}\label{ice-thermal-storage-mass-flow-rate-kgs}
+
+The total water mass flow rate through the ice storage component. Because the component includes an implied 3-way valve, this flow may be all through the tank, all bypassed through the valve, or a mixture of both.
+
+\paragraph{Ice Thermal Storage Inlet Temperature {[}C{]}}\label{ice-thermal-storage-inlet-temperature-c}
+
+The water temperature entering the ice storage component.
+
+\paragraph{Ice Thermal Storage Outlet Temperature {[}C{]}}\label{ice-thermal-storage-outlet-temperature-c}
+
+The water temperature leaving the ice storage component.
+
+\paragraph{Ice Thermal Storage Cooling Discharge Rate {[}W{]}}\label{ice-thermal-storage-cooling-discharge-rate-w}
+
+The rate of cooling delivered by the ice storage component. A positive value indicates the ice tank is discharging (melting). A zero value indicates the tank is charging or dormant.
+
+\paragraph{Ice Thermal Storage Cooling Discharge Energy {[}J{]}}\label{ice-thermal-storage-cooling-discharge-energy-j}
+
+The cooling energy delivered by the ice storage component. A positive value indicates the ice tank is discharging (melting). A zero value indicates the tank is charging or dormant.
+
+\paragraph{Ice Thermal Storage Cooling Charge Rate {[}W{]}}\label{ice-thermal-storage-cooling-charge-rate-w}
+
+The rate of charging delivered to the ice storage component. A positive value indicates the ice tank is charging (freezing). A zero value indicates the tank is discharging or dormant.
+
+\paragraph{Ice Thermal Storage Cooling Charge Energy {[}J{]}}\label{ice-thermal-storage-cooling-charge-energy-j}
+
+The charging energy delivered to the ice storage component. A positive value indicates the ice tank is charging (freezing). A zero value indicates the tank is discharging or dormant.
+
+\subsection{ThermalStorage:Ice:Detailed}\label{thermalstorageicedetailed}
+
+The detailed ice storage model allows the users of EnergyPlus to model more closely specific manufacturers' ice storage units. This is possible due to the use of curve fits to simulate the performance of the ice storage unit during charging and discharging. In this implementation, both charging and discharging are a function of the fraction charged/discharged as well as the log mean temperature difference across the storage unit. More information on the model is provided in the Engineering Reference for EnergyPlus. The remainder of this section describes the input required for the detailed ice storage model and the output that it can produce.
+
+\subsubsection{Inputs}\label{inputs-21-004}
+
+\paragraph{Field: Name}\label{field-name-21-001}
+
+This field is the name of the detailed ice storage system given to it by the user.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-012}
+
+This field is the name of the schedule (ref: Schedule) that determines whether or not the ice storage system is available during a particular time period. This allows the system to be turned off during a particular season. A value of less than or equal to zero indicates that the ice storage system is not available. Any value greater than zero indicates that the system is available. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Capacity}\label{field-capacity-1-000}
+
+This number is the maximum amount of latent thermal storage available in the ice storage system. This model does not allow the removal or addition of sensible energy from the tank. Thus, it is always assumed to be at the freezing temperature of the storage material. The capacity is expressed in units of GJ.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-1-001}
+
+This is the name of the node that connects the ice storage system to the plant loop. It is the inlet node to the ice storage component. The next field defines the outlet node. Due to presence of an internal bypass in this model, there are other ``nodes'' that are handled internally within the program. Users do not need to define any nodes other than the inlet and outlet nodes.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-1-002}
+
+This is the name of the other node that connects the ice storage system to the plant loop. It is the outlet node to the ice storage component.
+
+\paragraph{Field: Discharging Curve Object Type}\label{field-discharging-curve-object-type}
+
+The detailed ice storage model in EnergyPlus takes advantage of the Curve feature of the program. Currently, the only two allowed curve fit types for the detailed ice storage model are the QuadraticLinear and the CubicLinear curves. More information on this curve can be found in the section on Curves.
+
+\paragraph{Field: Discharging Curve Name}\label{field-discharging-curve-name}
+
+This field specifies the name of the actual curve fit to be used to model the discharging process of the detailed ice storage system.
+
+\paragraph{Field: Charging Curve Object Type}\label{field-charging-curve-object-type}
+
+The detailed ice storage model in EnergyPlus takes advantage of the Curve feature of the program. Currently, the only two allowed curve fit types for the detailed ice storage model are the QuadraticLinear and the CubicLinear curves. More information on this curve can be found in the section on Curves.
+
+\paragraph{Field: Charging Curve Name}\label{field-charging-curve-name}
+
+This field specifies the name of the actual curve fit to be used to model the charging process of the detailed ice storage system.
+
+\paragraph{Field: Timestep of the Curve Data}\label{field-timestep-of-the-curve-data}
+
+This field defines what timestep was used to produce the curve fits named in the previous inputs. This parameter is important because the curve fit is non-dimensional. Thus, the data used to develop the curve fits were based on a specific length of time. In many cases, this is probably one hour or 1.0. The units for this parameter are hours.
+
+\paragraph{Field: Parasitic Electric Load During Discharging}\label{field-parasitic-electric-load-during-discharging}
+
+This field defines the amount of parasitic electric consumption (for controls or other miscellaneous electric consumption associate with the ice storage unit itself) during the discharge phase. This parameter is dimensionless and gets multiplied by the current load on the tank.
+
+\paragraph{Field: Parasitic Electric Load During Charging}\label{field-parasitic-electric-load-during-charging}
+
+This field defines the amount of parasitic electric consumption (for controls or other miscellaneous electric consumption associate with the ice storage unit itself) during the charge phase. This parameter is dimensionless and gets multiplied by the current load on the tank.
+
+\paragraph{Field: Tank Loss Coefficient}\label{field-tank-loss-coefficient}
+
+This field defines the loss of ice stored during a particular hour. This field is dimensionless (per hour). It is not multiplied by any temperature difference between the tank and the environment in which it might be located.
+
+\paragraph{Field: Freezing Temperature of Storage Medium}\label{field-freezing-temperature-of-storage-medium}
+
+This parameter defines the freezing/melting temperature of the ice storage medium in degrees Celsius. For most tanks, this is simply 0.0°C (the default value). However, some tanks may use other materials or salts which would change the freezing temperature. This can be changed using this parameter.
+
+\paragraph{Field: Thaw Process Indicator}\label{field-thaw-process-indicator}
+
+This input field assists in more accurate modeling of the charging process by defining how the thawing of ice takes place. There are two options for this input: \textbf{InsideMelt} and \textbf{OutsideMelt}. Some ice storage systems, by their nature, start the charging process with a bare coil or no ice left on the charging surface even though there is still ice stored in the tank.~ An example of such a system is sometimes referred to as an ice-on-coil inside melt system, and these systems would define this parameter using the ``InsideMelt'' option for this field.~ Other systems melt the ice from the outside, leaving ice still on the charging surface when charging begins. These systems are modeled using the ``OutsideMelt'' option.~ For systems that have a charging process that does not vary significantly with fraction charged can ignore this input by accepting the default value.~ The default value for this field is ``OutsideMelt''.
+
+An IDF example:
+
+\begin{lstlisting}
+
+ThermalStorage:Ice:Detailed,
+      Ice Tank,                !- Ice Storage Name
+      ON,                      !- Ice Storage availability schedule
+      0.5,                     !- Ice Storage Capacity {GJ}
+      Ice Tank Inlet Node,     !- Plant Loop Inlet Node
+      Ice Tank Outlet Node,    !- Plant Loop Outlet Node
+      QuadraticLinear,         !- Discharging Curve Fit Type
+      DischargeCurve,          !- Discharging Curve Name
+      QuadraticLinear,         !- Charging Curve Fit Type
+      ChargeCurve,             !- Charging Curve Name
+      1.0,                     !- Timestep of Curve Fit Data
+      0.0001,                  !- Parasitic electric load during discharging
+      0.0002,                  !- Parasitic electric load during charging
+      0.0003,                  !- Tank loss coefficient
+      0.0;                     !- Freezing temperature [C]
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-19-000}
+
+Current detailed ice storage output variables are:
+
+\begin{itemize}
+\item
+  System, Average, Ice Thermal Storage Cooling Rate {[}W{]}
+\item
+  System, Average, Ice Thermal Storage Change Fraction {[]}
+\item
+  System, Average, Ice Thermal Storage End Fraction {[]}
+\item
+  System, Average, Ice Thermal Storage Mass Flow Rate {[}kg/s{]}
+\item
+  System, Average, Ice Thermal Storage Bypass Mass Flow Rate {[}kg/s{]}
+\item
+  System, Average, Ice Thermal Storage Tank Mass Flow Rate {[}kg/s{]}
+\item
+  System, Average, Ice Thermal Storage Fluid Inlet Temperature {[}C{]}
+\item
+  System, Average, Ice Thermal Storage Blended Outlet Temperature {[}C{]}
+\item
+  System, Average, Ice Thermal Storage Tank Outlet Temperature {[}C{]}
+\item
+  System, Average, Ice Thermal Storage Cooling Discharge Rate {[}W{]}
+\item
+  System, Sum, Ice Thermal Storage Cooling Discharge Energy {[}J{]}
+\item
+  System, Average, Ice Thermal Storage Cooling Charge Rate {[}W{]}
+\item
+  System, Sum, Ice Thermal Storage Cooling Charge Energy {[}J{]}
+\item
+  System, Average, Ice Thermal Storage Ancillary Electric Power {[}W{]}
+\item
+  System, Sum, Ice Thermal Storage Ancillary Electric Energy {[}J{]}
+\item
+  System, Average, Ice Thermal Storage On Coil Fraction {[]}
+\end{itemize}
+
+\paragraph{~Ice Thermal Storage Cooling Rate {[}W{]}}\label{ice-thermal-storage-cooling-rate-w}
+
+The actual load (absolute value) provided by the ice storage system during the current timestep
+
+\paragraph{\texorpdfstring{Ice Thermal Storage Change Fraction {[]}}{Ice Thermal Storage Change Fraction }}\label{ice-thermal-storage-change-fraction}
+
+The change in the ice tank's charge fraction charged during the current timestep (positive for charging, negative for discharging).
+
+\paragraph{\texorpdfstring{Ice Thermal Storage End Fraction {[]}}{Ice Thermal Storage End Fraction }}\label{ice-thermal-storage-end-fraction-1}
+
+The fraction charge of the ice storage system at the end of the timestep
+
+\paragraph{\texorpdfstring{Ice Thermal Storage On Coil Fraction {[]}}{Ice Thermal Storage On Coil Fraction }}\label{ice-thermal-storage-on-coil-fraction}
+
+The fraction of ice that is actually on the freezing surface at the end of the timestep.~ This can be different for an ``inside melt'' system than the end fraction (see previous output parameter).
+
+\paragraph{Ice Thermal Storage Mass Flow Rate {[}kg/s{]}}\label{ice-thermal-storage-mass-flow-rate-kgs-1}
+
+The mass flow through the ice storage component
+
+\paragraph{Ice Thermal Storage Bypass Mass Flow Rate {[}kg/s{]}}\label{ice-thermal-storage-bypass-mass-flow-rate-kgs}
+
+The mass flow through the ice storage component bypass (bypasses the actual unit)
+
+\paragraph{Ice Thermal Storage Tank Mass Flow Rate {[}kg/s{]}}\label{ice-thermal-storage-tank-mass-flow-rate-kgs}
+
+The mass flow through the ice storage unit itself
+
+\paragraph{Ice Thermal Storage Fluid Inlet Temperature {[}C{]}}\label{ice-thermal-storage-fluid-inlet-temperature-c}
+
+The inlet temperature to the ice storage component
+
+\paragraph{Ice Thermal Storage Blended Outlet Temperature {[}C{]}}\label{ice-thermal-storage-blended-outlet-temperature-c}
+
+The outlet temperature of the component after mixing any bypass flow with flow through the ice storage unit
+
+\paragraph{Ice Thermal Storage Tank Outlet Temperature {[}C{]}}\label{ice-thermal-storage-tank-outlet-temperature-c}
+
+The outlet temperature of the ice storage unit itself below mixing with any bypass flow
+
+\paragraph{Ice Thermal Storage Cooling Discharge Rate {[}W{]}}\label{ice-thermal-storage-cooling-discharge-rate-w-1}
+
+The cooling done (as a rate) by the ice storage unit or its discharge rate
+
+\paragraph{Ice Thermal Storage Cooling Discharge Energy {[}J{]}}\label{ice-thermal-storage-cooling-discharge-energy-j-1}
+
+The total cooling done by the ice storage unit or its discharge rate
+
+\paragraph{Ice Thermal Storage Cooling Charge Rate {[}W{]}}\label{ice-thermal-storage-cooling-charge-rate-w-1}
+
+The charging done (as a rate) to the ice storage unit
+
+\paragraph{Ice Thermal Storage Cooling Charge Energy {[}J{]}}\label{ice-thermal-storage-cooling-charge-energy-j-1}
+
+The total charging done to the ice storage unit
+
+\paragraph{Ice Thermal Storage Ancillary Electric Power {[}W{]}}\label{ice-thermal-storage-ancillary-electric-power-w}
+
+The electric power as a result of parasitic loads on the ice storage unit for things like controls or other miscellaneous parts of the ice storage unit itself
+
+\paragraph{Ice Thermal Storage Ancillary Electric Energy {[}J{]}}\label{ice-thermal-storage-ancillary-electric-energy-j}
+
+The electric consumption as a result of parasitic loads on the ice storage unit for things like controls or other miscellaneous parts of the ice storage unit itself
+
+\subsection{ThermalStorage:ChilledWater:Mixed}\label{thermalstoragechilledwatermixed}
+
+The ThermalStorage:ChilledWater:Mixed object analytically solves the differential equation governing the energy balance of the water tank.~ The chilled water is ``used'' by drawing from the ``Use Side'' of the water tank.~ The tank is indirectly charged by circulating cold water through the ``Source Side'' of the water tank.
+
+Control is based on cycling flow through the source side.~ When the tank temperature rises above a ``cut-in'' temperature, source side flow is requested.~ Source side flow will continue until the tank is cooled to below the tank set point or ``cut-out'' temperature.
+
+For heat gains from the ambient environment, the ambient air temperature can be taken from a schedule, a zone, or the exterior. When used with a zone, the skin gains are removed from the zone heat balance as negative internal heat gains.
+
+\subsubsection{Inputs}\label{inputs-22-003}
+
+\paragraph{Field: Name}\label{field-name-22-001}
+
+The unique name of the ThermalStorage:ChilledWater:Mixed object.
+
+\paragraph{Field: Tank Volume}\label{field-tank-volume}
+
+The volume of the thermal storage tank {[}m\(^{3}\){]}.
+
+\paragraph{Field: Setpoint Temperature Schedule Name}\label{field-setpoint-temperature-schedule-name-000}
+
+The reference to the schedule object specifying the chilled water temperature setpoint {[}°C{]}. Also known as the ``cut-out'' temperature.
+
+\paragraph{Field: Deadband Temperature Difference}\label{field-deadband-temperature-difference}
+
+The delta temperature difference {[}Δ°C{]} between the setpoint and the ``cut-in'' temperature at which the storage tank will request cooling. In other words, the ``cut-in'' temperature is Setpoint + Deadband.
+
+\paragraph{Field: Minimum Temperature Limit}\label{field-minimum-temperature-limit}
+
+The temperature {[}°C{]} at which the tank water becomes too cold.~ No source side flow is allowed when the tank temperature is below this limit.~ The minimum temperature must be lower than the setpoint temperature at all times.
+
+\paragraph{Field: Nominal Cooling Capacity}\label{field-nominal-cooling-capacity-2}
+
+This field describes the typical cooling capacity that the chilled water tank will provide.~ Since this is a passive device, the actual cooling capacity depends on water temperatures and flow rates.~ However, this field is used to describe the chilled water tank's nominal cooling capacity for supervisory control where plant operation schemes require a cooling capacity to model how equipment is dispatched.
+
+\paragraph{Field: Ambient Temperature Indicator}\label{field-ambient-temperature-indicator}
+
+The Ambient Temperature Indicator specifies how the ambient air temperature will be indicated. The field can be ``Schedule'', ``Zone'', or ``Exterior.'' If \emph{Schedule} is used, the Ambient Temperature Schedule Name field provides the values for ambient temperature. If \emph{Zone} is used, the zone air temperature of the zone specified in the Ambient Temperature Zone field provides the ambient temperature. If \emph{Exterior} is used, the outdoor dry-bulb air temperature provides the ambient temperature.
+
+\paragraph{Field: Ambient Temperature Schedule Name}\label{field-ambient-temperature-schedule-name-000}
+
+The field contains the name of a schedule object specifying the ambient air temperature around the tank for skin gains. This field is only used if Ambient Temperature Indicator is \emph{Schedule}.
+
+\paragraph{Field: Ambient Temperature Zone Name}\label{field-ambient-temperature-zone-name-000}
+
+The reference to the zone object specifying the ambient air temperature around the tank for skin gains. This field is only used if Ambient Temperature Indicator is \emph{Zone}.
+
+\paragraph{Field: Ambient Temperature Outdoor Air Node Name}\label{field-ambient-temperature-outdoor-air-node-name}
+
+This optional alpha field specifies the outdoor air node (OutdoorAir:Node) name used to define the ambient conditions surrounding the chilled water tank. This field is applicable only when the Ambient Temperature Indicator is specified as \emph{Exterior}, otherwise this field should be left blank. The node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+\paragraph{Field: Heat Gain Coefficient from Ambient Temperature}\label{field-heat-gain-coefficient-from-ambient-temperature}
+
+The gain coefficient {[}W/K{]} from the ambient air temperature. This coefficient is often referred to as the ``UA'' for the overall tank thermal performance with respect to heat gains from the tank's skin..
+
+\paragraph{Field: Use Side Inlet Node Name}\label{field-use-side-inlet-node-name}
+
+The inlet node connection to the plant loop for the use side of the chilled water storage tank. Typically the use side draws chilled water from the tank and returns warmer water.
+
+\paragraph{Field: Use Side Outlet Node Name}\label{field-use-side-outlet-node-name}
+
+The outlet node connection to the plant loop for the use side of the chilled water storage tank. Typically the use side chilled water from the tank and returns warmer water.
+
+\paragraph{Field: Use Side Heat Transfer Effectiveness}\label{field-use-side-heat-transfer-effectiveness}
+
+This field specifies the heat transfer effectiveness between the use side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the use side water and the tank water. If the effectiveness is lower, then the use side outlet water temperature will not be as cold as the tank water, simulating a heat exchanger.
+
+\paragraph{Field: Use Side Availability Schedule Name}\label{field-use-side-availability-schedule-name}
+
+This field contains the name of an availability schedule for the use side of the water tank. If the schedule's value is 0.0, then the use side is not available and flow will not be requested.~ If the schedule's value is note equal to 0.0 (usually 1 is used), the use side is available. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Use Side Design Flow Rate}\label{field-use-side-design-flow-rate}
+
+This field is used to specify the design flow rate through the Use Side of the chilled water tank.~ The volumetric design flow rate is specified in m\(^{3}\)/s.~ The field can be autosized.~ If autosized, then the input file should include a Plant Sizing object for the plant loop connected to the Use side.~ Sizing results are reported in the EIO file.
+
+\paragraph{Field: Source Side Inlet Node Name}\label{field-source-side-inlet-node-name-4}
+
+The inlet node connection to the plant loop for the source side of the chilled water storage tank. Typically the source side draws somewhat warm water from the tank and returns colder water.~ The source side volume flow rate is obtained from the plant loop.~ The magnitude of the flow rates through the source side can be controlled by setting the Maximum Branch Flow Rate field in the BRANCH object that connects the source inlet node.
+
+\paragraph{Field: Source Side Outlet Node Name}\label{field-source-side-outlet-node-name-4}
+
+The outlet node connection to the plant loop for the source side of the chilled water storage tank. Typically the source side draws somewhat warm water from the tank and returns colder water.
+
+\paragraph{Field: Source Side Heat Transfer Effectiveness}\label{field-source-side-heat-transfer-effectiveness}
+
+This field specifies the heat transfer effectiveness between the source side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the source side water and the tank water. If the effectiveness is lower, then the source side outlet water temperature will not be as cold as the tank water, simulating a heat exchanger.
+
+\paragraph{Field: Source Side Availability Schedule Name}\label{field-source-side-availability-schedule-name}
+
+This field contains the name of an availability schedule for the source side of the water tank.~ If the schedule's value is 0.0, then the source side is not available and flow will not be requested.~ If the schedule's value is not equal to 0.0 (usually 1 is used), the source side is available. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Source Side Design Flow Rate}\label{field-source-side-design-flow-rate}
+
+This field is used to specify the design flow rate through the Source Side of the chilled water tank.~ The volumetric design flow rate is specified in m\(^{3}\)/s.~ The field can be autosized.~ If autosized, then the input file should include a Plant Sizing object for the plant loop.~ Sizing results are reported in the EIO file.
+
+\paragraph{Field: Tank Recovery Time}\label{field-tank-recovery-time}
+
+This field is used to autosize the Source Side Design Flow Rate.~ The field is used if the previous field is set to autosize and the water tank's source side is on the demand side of a plant loop.~ This the the time, in hours, that the chilled water tank is to be indirectly cooled from 14.4ºC to 9.0ºC using the exit temperature of in the associated Plant Sizing object.
+
+An example input object follows.
+
+\begin{lstlisting}
+
+  ThermalStorage:ChilledWater:Mixed,
+      Chilled Water Storage Tank 1 ,  !- Name
+      4.0 ,                           !- Tank Volume
+      CW-Tank-Temp-Schedule,          !- Setpoint Temperature Schedule Name
+      3.5,                            !- Deadband Temperature Difference
+      1.0 ,                           !- Minimum Temperature Limit
+      25000 ,                         !- Nominal Cooling Capacity
+      Zone ,                          !- Ambient Temperature Indicator
+      ,                               !- Ambient Temperature Schedule Name
+      ZN_1_FLR_1_SEC_5 ,              !- Ambient Temperature Zone Name
+      ,                               !- Ambient Temperature Outdoor Air Node Name
+      5.0 ,                           !- Heat Gain Coefficient from Ambient Temperature
+      CW Tank Discharge Inlet node,   !- Use Side Inlet Node Name
+      CW Tank Discharge Outlet node , !- Use Side Outlet Node Name
+      1.0 ,                           !- Use Side Effectiveness
+      TES Use Schedule,               !- Use Side Availability Schedule Name
+      Autosize ,                      !- Use Side Design Flow Rate
+      CW Tank Charge Inlet Node,      !- Source Side Inlet Node Name
+      CW Tank Charge Outlet Node,     !- Source Side Outlet Node Name
+      1.0,                            !- Source Side Effectiveness
+      TES Charge Schedule,            !- Source Side Availability Schedule Name
+      Autosize ,                      !- Source Side Design Flow Rate
+      4.0;                            !- Tank Recovery Time
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-20-000}
+
+The following output variables are reported for chilled water thermal storage tanks.
+
+\begin{itemize}
+\item
+  Chilled Water Thermal Storage Tank Temperature~~~~~~~~~~~~~~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Final Tank Temperature~~~~~~~~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Tank Heat Gain Rate~~~~~~~~~~~~~~~~ !- HVAC Average {[}W{]}
+\item
+  Chilled Water Thermal Storage Tank Heat Gain Energy~~~~~~~~~~~~~~ !- HVAC Sum {[}J{]}
+\item
+  Chilled Water Thermal Storage Use Side Mass Flow Rate~~~~~~~~~~~~ !- HVAC Average {[}kg/s{]}
+\item
+  Chilled Water Thermal Storage Use Side Inlet Temperature~~~~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Use Side Outlet Temperature~~~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Use Side Heat Transfer Rate~~~~~~~~~~~~~~~~~ !- HVAC Average {[}W{]}
+\item
+  Chilled Water Thermal Storage Use Side Heat Transfer Energy~~~~~~~~~~~~~~~ !- HVAC Sum {[}J{]}
+\item
+  Chilled Water Thermal Storage Source Side Mass Flow Rate~~~~~~~~~ !- HVAC Average {[}kg/s{]}
+\item
+  Chilled Water Thermal Storage Source Side Inlet Temperature~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Source Side Outlet Temperature !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Source Side Heat Transfer Rate~~~~~~~~~~~~~~ !- HVAC Average {[}W{]}
+\item
+  Chilled Water Thermal Storage Source Side Heat Transfer Energy~~~~~~~~~~~~ !- HVAC Sum {[}J{]}
+\end{itemize}
+
+\paragraph{Chilled Water Thermal Storage Tank Temperature {[}C{]}}\label{chilled-water-thermal-storage-tank-temperature-c}
+
+The average water tank temperature.
+
+\paragraph{Chilled Water Thermal Storage Final Tank Temperature {[}C{]}}\label{chilled-water-thermal-storage-final-tank-temperature-c}
+
+The final water tank temperature at the end of the system timestep. If reported at the ``Detailed'' interval, this output variable can be used to verify an exact energy balance on the water storage tank.
+
+\paragraph{Chilled Water Thermal Storage Tank Heat Gain Rate {[}W{]}}\label{chilled-water-thermal-storage-tank-heat-gain-rate-w}
+
+The average heat exchange rate to the storage tank from the surrounding ambient.~ This is usually positive with surrounding ambient heating the storage tank.
+
+\paragraph{Chilled Water Thermal Storage Tank Heat Gain Energy {[}J{]}}\label{chilled-water-thermal-storage-tank-heat-gain-energy-j}
+
+The energy exchange to the storage tank from the surrounding ambient.~ This is usually positive with surrounding ambient heating the storage tank.
+
+\paragraph{Chilled Water Thermal Storage Use Side Mass Flow Rate {[}kg/s{]}}\label{chilled-water-thermal-storage-use-side-mass-flow-rate-kgs}
+
+The use side mass flow rate.
+
+\paragraph{Chilled Water Thermal Storage Use Side Inlet Temperature {[}C{]}}\label{chilled-water-thermal-storage-use-side-inlet-temperature-c}
+
+The inlet temperature on the use side.
+
+\paragraph{Chilled Water Thermal Storage Use Side Outlet Temperature {[}C{]}}\label{chilled-water-thermal-storage-use-side-outlet-temperature-c}
+
+The outlet temperature on the use side.
+
+\paragraph{Chilled Water Thermal Storage Use Side Heat Transfer Rate {[}W{]}}\label{chilled-water-thermal-storage-use-side-heat-transfer-rate-w}
+
+The average heat transfer rate between the use side water and the tank water.
+
+\paragraph{Chilled Water Thermal Storage Use Side Heat Transfer Energy {[}J{]}}\label{chilled-water-thermal-storage-use-side-heat-transfer-energy-j}
+
+The heat transfer energy between the use side water and the tank water.
+
+\paragraph{Chilled Water Thermal Storage Source Side Mass Flow Rate {[}kg/s{]}}\label{chilled-water-thermal-storage-source-side-mass-flow-rate-kgs}
+
+The source side mass flow rate.
+
+\paragraph{Chilled Water Thermal Storage Source Side Inlet Temperature {[}C{]}}\label{chilled-water-thermal-storage-source-side-inlet-temperature-c}
+
+The inlet temperature on the source side.
+
+\paragraph{Chilled Water Thermal Storage Source Side Outlet Temperature {[}C{]}}\label{chilled-water-thermal-storage-source-side-outlet-temperature-c}
+
+The outlet temperature on the source side.
+
+\paragraph{Chilled Water Thermal Storage Source Side Heat Transfer Rate {[}W{]}}\label{chilled-water-thermal-storage-source-side-heat-transfer-rate-w}
+
+The average heat transfer rate between the source side water and the tank water.
+
+\paragraph{Chilled Water Thermal Storage Source Side Heat Transfer Energy {[}J{]}}\label{chilled-water-thermal-storage-source-side-heat-transfer-energy-j}
+
+The heat transfer energy between the source side water and the tank water.
+
+\subsection{ThermalStorage:ChilledWater:Stratified}\label{thermalstoragechilledwaterstratified}
+
+The ThermalStorage:ChilledWater:Stratified object divides the water tank into multiple nodes of equal volume. The nodes are coupled by vertical conduction effects, internode fluid flow, and temperature inversion mixing. The object simultaneously solves the differential equations governing the energy balances on the nodes using a numerical method. The system timestep is divided into many small substeps that allow the simulation to capture events that occur on a very short time scale.~ The chilled water is ``used'' by drawing from the ``Use Side'' of the water tank.~ The tank is indirectly charged by circulating cold water through the ``Source Side'' of the water tank.
+
+Control is based on cycling flow through the source side.~ When the tank temperature rises above a ``cut-in'' temperature, source side flow is requested.~ Source side flow will continue until the tank is cooled to below the tank set point or ``cut-out'' temperature.
+
+For heat gains from the ambient environment, the ambient air temperature can be taken from a schedule, a zone, or the exterior. When used with a zone, the skin gains are removed from the zone heat balance as negative internal heat gains.
+
+\subsubsection{Inputs}\label{inputs-23-003}
+
+\paragraph{Field: Name}\label{field-name-23-001}
+
+The unique name of the ThermalStorage:ChilledWater:Stratified object.
+
+\paragraph{Field: Tank Volume}\label{field-tank-volume-1}
+
+The volume of the thermal storage tank {[}m\(^{3}\){]}.
+
+\paragraph{Field: Tank Height}\label{field-tank-height}
+
+The height {[}m{]} of the tank. For the HorizontalCylinder shape (see below) the height of the tank is the measure in the axial direction, i.e., the height if you were to stand the cylinder up on its end.
+
+\paragraph{Field: Tank Shape}\label{field-tank-shape}
+
+The tank shape determines the size and skin losses of the stratified nodes. There are three options:~ ``VerticalCylinder,'' ``HorizontalCylinder,'' and ``Other.''
+
+\emph{VerticalCylinder} describes most upright cylindrical water tanks.
+
+\emph{HorizontalCylinder} describes a few specialty water tanks and some large commercial storage tanks. \emph{HorizontalCylinder} implies that the tank is divided into nodes of equal mass, but not equal height.
+
+\emph{Other} describes water storage tanks that have a uniform horizontal cross-section, but are not cylinders, e.g., a cuboid or other shape. The length of the perimeter is then specified by the Tank Perimeter field.
+
+If blank, the default shape is \emph{VerticalCylinder}.
+
+\paragraph{Field: Tank Perimeter}\label{field-tank-perimeter}
+
+The length of the tank perimeter {[}m{]}. This field is only used if Tank Shape is \emph{Other}.
+
+\paragraph{Field: Setpoint Temperature Schedule Name}\label{field-setpoint-temperature-schedule-name-1}
+
+The reference to the schedule object specifying the chilled water temperature setpoint {[}°C{]}. Also known as the ``cut-out'' temperature.
+
+\paragraph{Field: Deadband Temperature Difference}\label{field-deadband-temperature-difference-1}
+
+The delta temperature difference {[}Δ°C{]} between the setpoint and the ``cut-in'' temperature at which the storage tank will request cooling. In other words, the ``cut-in'' temperature is Setpoint + Deadband.
+
+\paragraph{Field: Temperature Sensor Height}\label{field-temperature-sensor-height}
+
+This field is used to describe the location in the tank where the temperature is sensed for control descisions.~ The program will associate one of the nodes with this height and use that node's temperature for control decisions.~ The location is described in meters from the bottom of the tank.
+
+\paragraph{Field: Minimum Temperature Limit}\label{field-minimum-temperature-limit-1}
+
+The temperature {[}°C{]} at which the tank water becomes too cold.~ No source side flow is allowed when the tank temperature is below this limit.~ The minimum temperature must be lower than the setpoint temperature at all times.
+
+\paragraph{Field: Nominal Cooling Capacity}\label{field-nominal-cooling-capacity-3}
+
+This field describes the typical cooling capacity that the chilled water tank will provide.~ Since this is a passive device, the actual cooling capacity depends on water temperatures and flow rates.~ However, this field is used to describe the chilled water tank's nominal cooling capacity for supervisory control where plant operation schemes require a cooling capacity to model how equipment is dispatched.
+
+\paragraph{Field: Ambient Temperature Indicator}\label{field-ambient-temperature-indicator-1}
+
+The Ambient Temperature Indicator specifies how the ambient air temperature will be indicated. The field can be ``Schedule'', ``Zone'', or ``Exterior.'' If \emph{Schedule} is used, the Ambient Temperature Schedule Name field provides the values for ambient temperature. If \emph{Zone} is used, the zone air temperature of the zone specified in the Ambient Temperature Zone field provides the ambient temperature. If \emph{Exterior} is used, the outdoor dry-bulb air temperature provides the ambient temperature.
+
+\paragraph{Field: Ambient Temperature Schedule Name}\label{field-ambient-temperature-schedule-name-1}
+
+The field contains the name of a schedule object specifying the ambient air temperature around the tank for skin gains. This field is only used if Ambient Temperature Indicator is \emph{Schedule}.
+
+\paragraph{Field: Ambient Temperature Zone Name}\label{field-ambient-temperature-zone-name-1}
+
+The reference to the zone object specifying the ambient air temperature around the tank for skin gains. This field is only used if Ambient Temperature Indicator is \emph{Zone}.
+
+\paragraph{Field: Ambient Temperature Outside Air Node Name}\label{field-ambient-temperature-outside-air-node-name-000}
+
+This optional alpha field specifies the outdoor air node name used to define the ambient conditions surrounding the chilled water tank. This field is applicable only when the Ambient Temperature Indicator is specified as \emph{Exterior}, otherwise this field should be left blank. The node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+\paragraph{Field: Uniform Skin Loss Coefficient per Unit Area to Ambient Temperature}\label{field-uniform-skin-loss-coefficient-per-unit-area-to-ambient-temperature}
+
+The uniform skin loss coefficient {[}W/m\(^{2}\)-K{]} or U-Value of the tank to the ambient air temperature. The uniform skin loss accounts for the tank insulation. The overall losses at any particular tank node can be further modified using the Additional Loss Coefficient fields to account for thermal shorting due to pipe penetrations, tank feet, and any other loss effects.
+
+\paragraph{Field: Use Side Inlet Node Name}\label{field-use-side-inlet-node-name-1}
+
+The inlet node connection to the plant loop for the use side of the chilled water storage tank. Typically the use side draws chilled water from the tank and returns warmer water.
+
+\paragraph{Field: Use Side Outlet Node Name}\label{field-use-side-outlet-node-name-1}
+
+The outlet node connection to the plant loop for the use side of the chilled water storage tank. Typically the use side chilled water from the tank and returns warmer water.
+
+\paragraph{Field: Use Side Heat Transfer Effectiveness}\label{field-use-side-heat-transfer-effectiveness-1}
+
+This field specifies the heat transfer effectiveness between the use side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the use side water and the tank water. If the effectiveness is lower, then the use side outlet water temperature will not be as cold as the tank water, simulating a heat exchanger.
+
+\paragraph{Field: Use Side Availability Schedule Name}\label{field-use-side-availability-schedule-name-1}
+
+This field contains the name of an availability schedule for the use side of the water tank.~ If the schedule's value is 0.0, then the use side is not available and flow will not be requested.~ If the schedule's value is not equal to 0.0 (usually 1 is used), then the use side is available. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Use Side Inlet Height}\label{field-use-side-inlet-height}
+
+The height of the use side inlet to the tank. If blank, the inlet defaults to the top of the tank. The inlet height cannot be higher than the tank height.
+
+\paragraph{Field: Use Side Outlet Height}\label{field-use-side-outlet-height}
+
+The height of the use side outlet from the tank. If blank or \textbf{autocalculate}, the inlet defaults to the bottom of the tank. The outlet height cannot be higher than the tank height.
+
+\paragraph{Field: Use Side Design Flow Rate}\label{field-use-side-design-flow-rate-1}
+
+This field is used to specify the design flow rate through the Use Side of the water tank.~ The volumetric design flow rate is specified in m\(^{3}\)/s.~ The field is needed when the Use Side is connected to a plant loop.~ The field can be autosized.~ If autosized, then the input file should include a Plant Sizing object for the plant loop.~ Sizing results are reported in the EIO file.
+
+\paragraph{Field: Source Side Inlet Node Name}\label{field-source-side-inlet-node-name-5}
+
+The inlet node connection to the plant loop for the source side of the chilled water storage tank. Typically the source side draws somewhat warm water from the tank and returns colder water.~ The source side volume flow rate is obtained from the plant loop.~ The magnitude of the flow rates through the source side can be controlled by setting the Maximum Branch Flow Rate field in the BRANCH object that connects the source inlet node.
+
+\paragraph{Field: Source Side Outlet Node Name}\label{field-source-side-outlet-node-name-5}
+
+The outlet node connection to the plant loop for the source side of the chilled water storage tank. Typically the source side draws somewhat warm water from the tank and returns colder water.
+
+\paragraph{Field: Source Side Heat Transfer Effectiveness}\label{field-source-side-heat-transfer-effectiveness-1}
+
+This field specifies the heat transfer effectiveness between the source side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the source side water and the tank water. If the effectiveness is less than 1.0, then the source side outlet water temperature will be less than the tank water at the outlet node, simulating a heat exchanger.
+
+\paragraph{Field: Source Side Availability Schedule Name}\label{field-source-side-availability-schedule-name-1}
+
+This field contains the name of an availability schedule for the source side of the water tank.~ If the schedule's value is 0.0, then the source side is not available and flow will not be requested. If the schedule's value is not equal to 0.0 (usually 1 is used), then the source side is available. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Source Side Inlet Height}\label{field-source-side-inlet-height}
+
+The height of the source side inlet to the tank. If blank or \textbf{autocalculate}, the inlet defaults to the bottom of the tank. The inlet height cannot be higher than the tank height.
+
+\paragraph{Field: Source Side Outlet Height}\label{field-source-side-outlet-height}
+
+The height of the source side outlet from the tank. If blank, the inlet defaults to the top of the tank. The outlet height cannot be higher than the tank height.
+
+\paragraph{Field: Source Side Design Flow Rate}\label{field-source-side-design-flow-rate-1}
+
+This field is optional and is used to specify the design flow rate through the Source Side of the water heater.~ The volumetric design flow rate is specified in m\(^{3}\)/s.~ The field is needed when the Source Side is connected to a plant loop.~ The field can be autosized.~ If autosized, then the input file should include a Plant Sizing object for the plant loop.~ Sizing results are reported in the EIO file.
+
+\paragraph{Field: Tank Recovery Time}\label{field-tank-recovery-time-1}
+
+This field is used to autosize the Source Side Design Flow Rate.~ The field is used if the previous field is set to autosize and the water tank's source side is on the demand side of a plant loop.~ This the the time, in hours, that the chilled water tank is to be indirectly cooled from 14.4C to 9.0C using the exit temperature of in the associated Plant Sizing object.
+
+\paragraph{Field: Inlet Mode}\label{field-inlet-mode}
+
+The inlet mode of entering fluid from the use and source sides. There are two options:~ ``Fixed'' or ``Seeking.'' In \emph{Fixed} mode, the fluid enters at the fixed heights specified above. In \emph{Seeking} mode, the fluid ``seeks out'' the stratified node that is closest to the inlet temperature and adds all flow to that node. The \emph{Seeking} mode provides maximum stratification.
+
+\paragraph{Field: Number of Nodes}\label{field-number-of-nodes}
+
+The number of stratified nodes in the tank. There must be at least one node. The maximum number of nodes is 10, although this limit can be increased by editing the IDD.
+
+\paragraph{Field: Additional Destratification Conductivity}\label{field-additional-destratification-conductivity}
+
+An additional destratification conductivity {[}W/m-K{]} is added to the fluid conductivity of water (0.6 W/m-K) to account for vertical conduction effects along the inside of the tank wall, and perhaps other vertical components such as a dip tube pipe or anode rod.
+
+\paragraph{Field: Node 1-10 Additional Loss Coefficient}\label{field-node-1-10-additional-loss-coefficient}
+
+An additional heat gain coefficient {[}W/K{]} added to the skin gains for a given node to account for thermal shorting due to pipe penetrations, tank feet, and any other loss effects.
+
+An example input object follows.
+
+\begin{lstlisting}
+
+  ThermalStorage:ChilledWater:Stratified,
+      Chilled Water Storage Tank 1 ,  !- Name
+      4.0  ,                          !- Tank Volume
+      2.0 ,                           !- Tank Height
+      VerticalCylinder,               !- Tank Shape
+       ,                              !- Tank Perimeter
+      CW-Tank-Temp-Schedule ,         !- Setpoint Temperature Schedule Name
+      3.5 ,                           !- Deadband Temperature Difference
+      1.4 ,                           !- Temperature Sensor Height
+      1.0 ,                           !- Minimum Temperature Limit
+      2500,                           !- Nominal Cooling Capacity
+      Zone,                           !- Ambient Temperature Indicator
+       ,                              !- Ambient Temperature Schedule Name
+      ZN_1_FLR_1_SEC_5 ,              !- Ambient Temperature Zone Name
+       ,                              !- Ambient Temperature OutdoorAir:Node Name
+      4.2,                            !- Uniform Skin Loss Coefficient Per Unit Area To Ambient Temperature
+      CW Tank Discharge Inlet node,   !- Use Side Inlet Node Name
+      CW Tank Discharge Outlet node,  !- Use Side Outlet Node Name
+      1.0,                            !- Use Side Effectiveness
+      ALWAYS_ON,                      !- Use Side Availability Schedule Name
+      1.85 ,                          !- Use Side Inlet Height
+      0.15 ,                          !- Use Side Outlet Height
+      autosize,                       !- Use Side Design Flow Rate
+      CW Tank Charge Inlet Node,      !- Source Side Inlet Node Name
+      CW Tank Charge Outlet Node,     !- Source Side Outlet Node Name
+      1.0,                            !- Source Side Effectiveness
+      TES Charge Schedule,            !- Source Side Availability Schedule Name
+      0.15,                           !- Source Side Inlet Height
+      1.85,                           !- Source Side Outlet Height
+      autosize,                       !- Source Side Design Flow Rate
+      2.0,                            !- Tank Recovery Time
+      Seeking,                        !- Inlet Mode
+      6,                              !- Number Of Nodes
+      0.0;                            !- Additional Destratification Conductivity
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-21-000}
+
+The following output variables are reported for stratified chilled water thermal storage tanks.
+
+\begin{itemize}
+\item
+  Chilled Water Thermal Storage Tank Temperature~~~~~~~~~~~~~~~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Final Tank Temperature~~~~~~~~~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Tank Heat Gain Rate~~~~~~~~~~~~~~~~~ !- HVAC Average {[}W{]}
+\item
+  Chilled Water Thermal Storage Tank Heat Gain Energy~~~~~~~~~~~~~~~ !- HVAC Sum {[}J{]}
+\item
+  Chilled Water Thermal Storage Use Side Mass Flow Rate~~~~~~~~~~~~~ !- HVAC Average {[}kg/s{]}
+\item
+  Chilled Water Thermal Storage Use Side Inlet Temperature~~~~~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Use Side Outlet Temperature~~~~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Use Side Heat Transfer Rate~~~~~~~~~~~~~~~~~~ !- HVAC Average {[}W{]}
+\item
+  Chilled Water Thermal Storage Use Side Heat Transfer Energy~~~~ ~~~~~~~~~~~~!- HVAC Sum {[}J{]}
+\item
+  Chilled Water Thermal Storage Source Side Mass Flow Rate~~~~~~~~~~ !- HVAC Average {[}kg/s{]}
+\item
+  Chilled Water Thermal Storage Source Side Inlet Temperature~~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Source Side Outlet Temperature~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Source Side Heat Transfer Rate~~~~~~~~~~~~~~~ !- HVAC Average {[}W{]}
+\item
+  Chilled Water Thermal Storage Source Side Heat Transfer Energy~~~~~~~~~~~~~ !- HVAC Sum {[}J{]}
+\item
+  Chilled Water Thermal Storage Temperature Node \textless{}1 - 10\textgreater{}~~~~~~~ !- HVAC Average {[}C{]}
+\item
+  Chilled Water Thermal Storage Final Temperature Node \textless{}1 -- 10\textgreater{} !- HVAC Average {[}C{]}
+\end{itemize}
+
+\paragraph{Chilled Water Thermal Storage Tank Temperature {[}C{]}}\label{chilled-water-thermal-storage-tank-temperature-c-1}
+
+The average water tank temperature, i.e., the average of all of the node average temperatures.
+
+\paragraph{Chilled Water Thermal Storage Tank Final Temperature {[}C{]}}\label{chilled-water-thermal-storage-tank-final-temperature-c}
+
+The final water tank temperature at the end of the system timestep, i.e., the average of all of the final node temperatures at the end of the system timestep.~ If reported at the ``Detailed'' interval, this output variable can be used to verify an exact energy balance on the water storage tank.
+
+\paragraph{Chilled Water Thermal Storage Tank Heat Gain Rate {[}W{]}}\label{chilled-water-thermal-storage-tank-heat-gain-rate-w-1}
+
+The average heat exchange rate to the storage tank from the surrounding ambient.~ This is usually positive with surrounding ambient heating the storage tank.
+
+\paragraph{Chilled Water Thermal Storage Tank Heat Gain Energy {[}J{]}}\label{chilled-water-thermal-storage-tank-heat-gain-energy-j-1}
+
+The energy exchange to the storage tank from the surrounding ambient.~ This is usually positive with surrounding ambient heating the storage tank.
+
+\paragraph{Chilled Water Thermal Storage Use Side Mass Flow Rate {[}kg/s{]}}\label{chilled-water-thermal-storage-use-side-mass-flow-rate-kgs-1}
+
+The use side mass flow rate.
+
+\paragraph{Chilled Water Thermal Storage Use Side Inlet Temperature {[}C{]}}\label{chilled-water-thermal-storage-use-side-inlet-temperature-c-1}
+
+The inlet temperature on the use side.
+
+\paragraph{Chilled Water Thermal Storage Use Side Outlet Temperature {[}C{]}}\label{chilled-water-thermal-storage-use-side-outlet-temperature-c-1}
+
+The outlet temperature on the use side.
+
+\paragraph{Chilled Water Thermal Storage Use Side Heat Transfer Rate {[}W{]}}\label{chilled-water-thermal-storage-use-side-heat-transfer-rate-w-1}
+
+The average heat transfer rate between the use side water and the tank water.
+
+\paragraph{Chilled Water Thermal Storage Use Side Heat Transfer Energy {[}J{]}}\label{chilled-water-thermal-storage-use-side-heat-transfer-energy-j-1}
+
+The heat transfer energy between the use side water and the tank water.
+
+\paragraph{Chilled Water Thermal Storage Source Side Mass Flow Rate {[}kg/s{]}}\label{chilled-water-thermal-storage-source-side-mass-flow-rate-kgs-1}
+
+The source side mass flow rate.
+
+\paragraph{Chilled Water Thermal Storage Source Side Inlet Temperature {[}C{]}}\label{chilled-water-thermal-storage-source-side-inlet-temperature-c-1}
+
+The inlet temperature on the source side.
+
+\paragraph{Chilled Water Thermal Storage Source Side Outlet Temperature {[}C{]}}\label{chilled-water-thermal-storage-source-side-outlet-temperature-c-1}
+
+The outlet temperature on the source side.
+
+\paragraph{Chilled Water Thermal Storage Source Side Heat Transfer Rate {[}W{]}}\label{chilled-water-thermal-storage-source-side-heat-transfer-rate-w-1}
+
+The average heat transfer rate between the source side water and the tank water.
+
+\paragraph{Chilled Water Thermal Storage Source Side Heat Transfer Energy {[}J{]}}\label{chilled-water-thermal-storage-source-side-heat-transfer-energy-j-1}
+
+The heat transfer energy between the source side water and the tank water.
+
+\paragraph{Chilled Water Thermal Storage Temperature Node~ 1-10 {[}C{]}}\label{chilled-water-thermal-storage-temperature-node-1-10-c}
+
+The average node temperature.
+
+\paragraph{Chilled Water Thermal Storage Final Temperature Node 1-10~ {[}C{]}}\label{chilled-water-thermal-storage-final-temperature-node-1-10-c}
+
+The final node temperature at the end of the system timestep.
diff --git a/doc/input-output-reference/src/overview/group-pumps.tex b/doc/input-output-reference/src/overview/group-pumps.tex
new file mode 100644
index 00000000000..55c0c19fc07
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-pumps.tex
@@ -0,0 +1,955 @@
+\section{Group Pumps}\label{group-pumps}
+
+EnergyPlus plant and condenser loops need pump components to drive liquid flow around the loop. There are various types of pump models available.
+
+\subsection{Pump:VariableSpeed}\label{pumpvariablespeed}
+
+Pumps are needed in both plant and condenser loops. The syntax for a variable speed pump is given below.
+
+\subsubsection{Inputs}\label{inputs-037}
+
+\paragraph{Field: Name}\label{field-name-036}
+
+This alpha field contains the identifying a unique name for the pump.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-005}
+
+This alpha field contains the identifying name for the pump inlet node.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-006}
+
+This alpha field contains the identifying name for the pump outlet node.
+
+\paragraph{Field: Design Maximum Flow Rate}\label{field-design-maximum-flow-rate}
+
+This numeric field contains the pump's design maximum volume flow rate in cubic meters per second. This field can be autosized.
+
+\paragraph{Field: Design Pump Head}\label{field-design-pump-head}
+
+This numeric field contains the pump's rated head pressure in Pascals. The default is 179352 Pa, or 60 ftH20, and is for a fairly large building.
+
+\paragraph{Field: Design Power Consumption}\label{field-design-power-consumption}
+
+This numeric field contains the pump's design power consumption in Watts. If the user is performing a pressure simulation on the loop in which this pump is found, this value would only be used to estimate pump efficiency. During reported calculations, the pump would use the loop pressure drop and current flow conditions along with efficiency to calculate pump power dynamically. This field can be autosized. When set to autosize the type of scaling factor is chosen in the input field Design Power Sizing Method.
+
+\paragraph{Field: Motor Efficiency}\label{field-motor-efficiency-000}
+
+This numeric field contains the pump's efficiency in decimal form (0 = 0\%, 1 = 100\%).
+
+\paragraph{Field: Fraction of Motor Inefficiencies to Fluid Stream}\label{field-fraction-of-motor-inefficiencies-to-fluid-stream}
+
+This numeric field contains the pump's fraction of power loss to the fluid.
+
+\paragraph{Field: Coefficient 1 of the Part Load Performance Curve}\label{field-coefficient-1-of-the-part-load-performance-curve}
+
+This numeric field contains the first coefficient in the part load ratio curve. The fraction of full load power is determined by the cubic equation:
+
+\begin{equation}
+FractionFullLoadPower = {C_1} + {C_2}PLR + {C_3}PL{R^2} + {C_4}PL{R^3}
+\end{equation}
+
+where C\(_{1}\),C\(_{2}\),C\(_{3}\),and C\(_{4}\) are Coefficients 1 4 (below) and PLR is the Part Load Ratio.
+
+\paragraph{Field: Coefficient 2 of the Part Load Performance Curve}\label{field-coefficient-2-of-the-part-load-performance-curve}
+
+This numeric field contains the second coefficient in the part load ratio curve.
+
+\paragraph{Field: Coefficient 3 of the Part Load Performance Curve}\label{field-coefficient-3-of-the-part-load-performance-curve}
+
+This numeric field contains the third coefficient in the part load ratio curve.
+
+\paragraph{Field: Coefficient 4 of the Part Load Performance Curve}\label{field-coefficient-4-of-the-part-load-performance-curve}
+
+This numeric field contains the fourth coefficient in the part load ratio curve.
+
+\paragraph{Field: Design Minimum Flow Rate}\label{field-design-minimum-flow-rate}
+
+This field contains the minimum volume flow rate while operating in variable flow capacity rate in cubic meters per second. This field is autosizable. When set to autosize the value in the input field Design Minimum Flow Rate Sizing Factor is used to scale the minimum flow rate as a fraction of the Design Maximum Flow Rate.
+
+\paragraph{Field: Pump Control Type}\label{field-pump-control-type-000}
+
+This is a choice field of Continuous or Intermittent. A variable speed pump is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump is operating intermittently, then the pump can shutdown. For any other condition such as the loop having a load and the pump is operating intermittently or the pump is continuously operating (regardless of the loading condition), the pump will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump is running, it will try to meet the flow request made by demand side components. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this control by forcing the pump to be on or off.
+
+\paragraph{Field: Pump Flow Rate Schedule Name}\label{field-pump-flow-rate-schedule-name-000}
+
+The schedule values modify the value for Rated Flow Rate of the pump on a time basis. This essentially sets the maximum value available for the pump at a given time, \textbf{not the actual flow rate at that time}. The default is that the pump is ON and runs according to its other operational requirements specified above. This schedule is for special, not typical pump operations. For additional control over pump flow, EMS actuators can be employed.
+
+\paragraph{Field: Pump Curve Name}\label{field-pump-curve-name}
+
+This references a pump curve to be used during pump flow-loop head resolution. This is only applicable for loop simulations which include pressure components on at least a single branch. More information regarding pressure system simulation is available in the engineering reference.
+
+\paragraph{Field: Impeller Diameter}\label{field-impeller-diameter}
+
+For pressure simulation cases, this is the impeller diameter used during calculations which is used in non-dimensionalizing the pump curve described in the previous field. The units of this value are meters.
+
+\paragraph{Field: VFD Control Type}\label{field-vfd-control-type}
+
+This string defines which type of VFD control type to perform. PressureSetPointControl is a realistic approach which requires inputs of pressure range schedules to control the pump rpm to maintain a certain pressure drop (head). ManualControl is an idealized control strategy in which the pump RPM is maintained at a scheduled value throughout the simulation, abiding by other flow restrictions in the loop.
+
+\paragraph{Field: Pump RPM Schedule Name}\label{field-pump-rpm-schedule-name}
+
+For VFD Control Type = ManualControl, this defines the pump RPM schedule to use during the simulation. For VFD Control Type = PressureSetPointControl, this field is not interpreted. The value of the schedule is RPM.
+
+\paragraph{Field: Minimum Pressure Schedule}\label{field-minimum-pressure-schedule}
+
+For VFD Control Type = PressureSetPointControl, this field defines the minimum pressure range setpoint value, or the lower bound of pressure drop (head) to use when determining the required pump speed. For VFD Control Type = ManualControl, this field is not interpreted. The value of the schedule is Pascals.
+
+\paragraph{Field: Maximum Pressure Schedule}\label{field-maximum-pressure-schedule}
+
+For VFD Control Type = PressureSetPointControl, this field defines the maximum pressure range setpoint value, or the upper bound of pressure drop (head) to use when determining the required pump speed. For VFD Control Type = ManualControl, this field is not interpreted. The value of the schedule is Pascals.
+
+\paragraph{Field: Minimum RPM Schedule}\label{field-minimum-rpm-schedule}
+
+For VFD Control Type = PressureSetPointControl, this field defines the minimum allowable RPM, or the lower bound of pump speed to use when determining the required pump speed. For VFD Control Type = ManualControl, this field is not interpreted. The value of the schedule is RPM.
+
+\paragraph{Field: Maximum RPM Schedule}\label{field-maximum-rpm-schedule}
+
+For VFD Control Type = PressureSetPointControl, this field defines the maximum allowable RPM, or the upper bound of pump speed to use when determining the required pump speed. For VFD Control Type = ManualControl, this field is not interpreted. The value of the schedule is RPM.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-008}
+
+This field is optional. It can be used to input the name of the Zone in which the pump is located in the model. If the pump is outdoors, or skin losses are not to be modeled, then leave this field blank. If a valid Zone name is entered, then the portion of electrical power consumed by the pump that is not added to the working fluid is added to the surrounding Zone.
+
+\paragraph{Field: Skin Loss Radiative Fraction}\label{field-skin-loss-radiative-fraction-000}
+
+This field is optional. If a Zone is named in the previous field and pump losses are to be added to a surrounding thermal zone, then this input determines the split between thermal radiation and thermal convection for the heat losses from the pump. If it is left blank then all the losses will be convective.
+
+\paragraph{Field: Design Power Sizing Method}\label{field-design-power-sizing-method}
+
+This field is optional. There are two choices PowerPerFlow and PowerPerFlowPerPressure. If PowerPerFlow is used the pump's Design Power Consumption will be calculated using the sizing factor from the input field Design Electric Power per Unit Flow Rate -- with Design Power Consumption = Design Maximum Flow Rate * scaling factor. If PowerPerFlowPerPressure is used the pump's Design Power Consumption will use the sizing factor from the input field Design Shaft Power per Unit Flow Rate Per Unit Head -- with Design Power Consumption = Design Maximum Flow Rate * Design Pump Head * scaling factor / Motor Efficiency. If omitted the default method of PowerPerFlowPerPressure will be used.
+
+\paragraph{Field: Design Electric Power per Unit Flow Rate}\label{field-design-electric-power-per-unit-flow-rate}
+
+This field is optional. This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlow. It allows setting the efficiency the pumping system's power consumption using only the design flow rate. If omitted the default value of 348701.1 W/(m\(^{3}\)/s) ( 22 W/gpm) will be used.
+
+\paragraph{Field: Design Shaft Power per Unit Flow Rate Per Unit Head}\label{field-design-shaft-power-per-unit-flow-rate-per-unit-head}
+
+This field is optional. This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlowPerPressure. It allows setting the efficiency of the impeller and drive assembly when calculating the pump power consumption for the design flow rate, motor efficiency, and pump head. If omitted the default value of 1.282051 W/((m\(^{3}\)/s)-Pa) will be used.
+
+\paragraph{Field: Design Minimum Flow Rate Sizing Factor}\label{field-design-minimum-flow-rate-sizing-factor}
+
+This field is optional. If omitted the default value of 0.0 will be used. This input is used when the input field Design Minimum Flow Rate is set to autosize. The minimum flow rate will be set to the product of this sizing factor and the Design Maximum Flow Rate.
+
+Examples of this object in the IDF follow.
+
+\begin{lstlisting}
+
+Pump:VariableSpeed,
+  HW Circ Pump,                          !- Name
+  HW Supply Inlet Node,                  !- Inlet Node Name
+  HW Pump Outlet Node,                   !- Outlet Node Name
+  autosize,                              !- Design Maximum Flow Rate {m3/s}
+  179352,                                !- Design Pump Head {Pa}
+  autosize,                              !- Design Power Consumption {W}
+  0.9,                                   !- Motor Efficiency
+  0.0,                                   !- Fraction of Motor Inefficiencies to Fluid Stream
+  0,                                     !- Coefficient 1 of the Part Load Performance Curve
+  1,                                     !- Coefficient 2 of the Part Load Performance Curve
+  0,                                     !- Coefficient 3 of the Part Load Performance Curve
+  0,                                     !- Coefficient 4 of the Part Load Performance Curve
+  0,                                     !- Minimum Flow Rate {m3/s}
+  Intermittent;                          !- Pump Control Type
+
+
+  Pump:VariableSpeed,
+  Circ Pump,                             !- Name
+  CW Supply Inlet Node,                  !- Inlet Node Name
+  CW Pump Outlet Node,                   !- Outlet Node Name
+  .0011,                                 !- Design Maximum Flow Rate {m3/s}
+  300000,                                !- Design Pump Head {Pa}
+  500,                                   !- Design Power Consumption {W}
+  .87,                                   !- Motor Efficiency
+  0.0,                                   !- Fraction of Motor Inefficiencies to Fluid Stream
+  0,                                     !- Coefficient 1 of the Part Load Performance Curve
+  1,                                     !- Coefficient 2 of the Part Load Performance Curve
+  0,                                     !- Coefficient 3 of the Part Load Performance Curve
+  0,                                     !- Coefficient 4 of the Part Load Performance Curve
+  0,                                     !- Minimum Flow Rate {m3/s}
+  Intermittent;                          !- Pump Control Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-026}
+
+\begin{itemize}
+\item
+  HVAC,Average,Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Pump Shaft Power {[}W{]}
+\item
+  HVAC,Average,Pump Fluid Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,Pump Fluid Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,Pump Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Pump Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Pump Zone Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Pump Zone Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Pump Zone Convective Heating Rate {[}W{]}
+\item
+  HVAC,Average,Pump Zone Radiative Heating Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Pump Electric Power {[}W{]}}\label{pump-electric-power-w}
+
+\paragraph{Pump Electric Energy {[}J{]}}\label{pump-electric-energy-j}
+
+These outputs are the electric power input to the pump motor. Consumption is metered on Pumps:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Pump Shaft Power {[}W{]}}\label{pump-shaft-power-w}
+
+This is the shaft power delivered from the motor to the pump.
+
+\paragraph{Pump Fluid Heat Gain Rate {[}W{]}}\label{pump-fluid-heat-gain-rate-w}
+
+\paragraph{Pump Fluid Heat Gain Energy {[}J{]}}\label{pump-fluid-heat-gain-energy-j}
+
+These outputs are the energy added to the fluid as heat. For the current algorithm, this is equal to Pump Shaft Power, because the loops are closed and all energy added to the fluid will ultimately become heat due to friction.
+
+\paragraph{Pump Outlet Temperature {[}C{]}}\label{pump-outlet-temperature-c}
+
+\paragraph{Pump Mass Flow Rate {[}kg/s{]}}\label{pump-mass-flow-rate-kgs}
+
+These outputs are the water outlet temperature and mass flow rate.
+
+\paragraph{Pump Zone Total Heating Rate {[}W{]}}\label{pump-zone-total-heating-rate-w}
+
+\paragraph{Pump Zone Total Heating Energy {[}J{]}}\label{pump-zone-total-heating-energy-j}
+
+These outputs are the thermal losses from the pump to the surrounding Zone. They are only available if a Zone was named in the pump s input. These indicate the amount of heat added to the zone from the pump s inefficiencies. They are the total heat loss including both convection and radiation.
+
+\paragraph{Pump Zone Convective Heating Rate {[}W{]}}\label{pump-zone-convective-heating-rate-w}
+
+This output is the thermal loss from the pump to the surrounding Zone in the form of convective gains directly to the zone air. It is only available if a Zone was named in the pump input.
+
+\paragraph{Pump Zone Radiative Heating Rate {[}W{]}}\label{pump-zone-radiative-heating-rate-w}
+
+This output is the thermal loss from the pump to the surrounding Zone in the form of thermal radiation gains directly to the inside face of the zone s surfaces. It is only available if a Zone was named in the pump input.
+
+\subsection{Pump:ConstantSpeed}\label{pumpconstantspeed}
+
+Pumps may be found in both plant and condenser loops. The syntax for a constant speed pump is given below.
+
+\subsubsection{Inputs}\label{inputs-1-034}
+
+\paragraph{Field: Name}\label{field-name-1-033}
+
+This alpha field contains the identifying name for the pump.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-1-002}
+
+This alpha field contains the identifying name for the pump inlet node.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-1-003}
+
+This alpha field contains the identifying name for the pump outlet node.
+
+\paragraph{Field: Design Flow Rate}\label{field-design-flow-rate-002}
+
+This numeric field contains the pump's design volume flow rate in cubic meters per second. This field is autosizable.
+
+\paragraph{Field: Design Pump Head}\label{field-design-pump-head-1}
+
+This numeric field contains the pump's design head pressure in Pascals. The default is 179352 Pa, or 60 ftH20, and is for a fairly large building.
+
+\paragraph{Field: Design Power Consumption}\label{field-design-power-consumption-1}
+
+This numeric field contains the pump's rated power consumption in Watts. If the user is performing a pressure simulation on the loop in which this pump is found, this value would only be used to estimate pump efficiency. During reported calculations, the pump would use the loop pressure drop and current flow conditions along with efficiency to calculate pump power dynamically. This field can be autosized. When set to autosize the type of scaling factor is chosen in the input field Design Power Sizing Method.
+
+\paragraph{Field: Motor Efficiency}\label{field-motor-efficiency-1-000}
+
+This numeric field contains the pump's efficiency in decimal form (0 = 0\%, 1 = 100\%).
+
+\paragraph{Field: Fraction of Motor Inefficiencies to Fluid Stream}\label{field-fraction-of-motor-inefficiencies-to-fluid-stream-1}
+
+This numeric field contains the pump's fraction of power loss to the fluid.
+
+\paragraph{Field: Pump Control Type}\label{field-pump-control-type-1-000}
+
+This is a choice field of Continuous or Intermittent. The operation of a constant speed pump is fairly straightforward. If the user designates a constant speed pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump is constant speed and operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this control by forcing the pump to be on or off.
+
+\paragraph{Field: Pump Flow Rate Schedule Name}\label{field-pump-flow-rate-schedule-name-1}
+
+The schedule values modify the value for Rated Flow Rate of the pump on a time basis. This essentially sets the maximum value available for the pump at a given time, \textbf{not the actual flow rate at that time}. The default is that the pump is ON and runs according to its other operational requirements specified above. This schedule is for special, not typical pump operations. For additional control over pump flow, EMS actuators can be employed.
+
+\paragraph{Field:Pump Curve Name}\label{fieldpump-curve-name}
+
+This field is only used if the user is performing a pressure-based simulation in the plant loop of the LoopFlowCorrection type (see PlantLoop section for how to enable this).
+
+This field references a separate pressure head curve that the user has input separately in the input file. The pressure curve represents a non-dimensional regression of pressure-flow rate data. The equation should be of the following form:
+
+\begin{equation}
+\psi  = {C_4} \times {\varphi ^4} + {C_3} \times {\varphi ^3} + {C_2} \times {\varphi ^2} + {C_1} \times \varphi  + {C_0}.
+\end{equation}
+
+In this equation, the two dimensionless parameters, X and X are defined in terms of physical pump and flow parameters as:
+
+\begin{equation}
+\psi  = \frac{{\Delta P}}{{\rho {N^2}{D^2}}}
+\end{equation}
+
+\begin{equation}
+\varphi  = \frac{{\dot m}}{{\rho N{D^3}}}
+\end{equation}
+
+Where Delta P is the pressure drop, mdot is the fluid mass flow rate, rho is a representative fluid density, N is the rotational speed of the pump, and D is the pump impeller diameter.
+
+Since the user may not need a full fourth order expansion of this, the user may use linear (first order), quadratic (second order), cubic (third order), or full quartic (fourth order). These are available in the objects Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic.
+
+Once this curve is input properly (along with the following two fields), the pump will respond to the plant loop pressure drop when resolving the flow rate. Note that this simulation method will likely result in a plant loop that does not exactly hit the setpoint as the current simulation method does. This is due to the loop flow rate now being pressure-based and not decision-based .
+
+\paragraph{Field:Impeller Diameter}\label{fieldimpeller-diameter}
+
+This field is only used if the user is performing a pressure-based simulation in the plant loop of the LoopFlowCorrection type (see PlantLoop section for how to enable this).
+
+To re-dimensionalize the dimensionless pump curve, the impeller diameter must be known. This value is entered in meters.
+
+\paragraph{Field:Rotational Speed}\label{fieldrotational-speed}
+
+This field is only used if the user is performing a pressure-based simulation in the plant loop of the LoopFlowCorrection type (see PlantLoop section for how to enable this).
+
+To re-dimensionalize the dimensionless pump curve, the rotational speed must be known. This value is entered in RPM (revolutions per minute).
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-006}
+
+This field is optional. It can be used to input the name of the Zone in which the pump is located in the model. If the pump is outdoors, or skin losses are not to be modeled, then leave this field blank. If a valid Zone name is entered, then the portion of electrical power consumed by the pump that is not added to the working fluid is added to the surrounding Zone.
+
+\paragraph{Field: Skin Loss Radiative Fraction}\label{field-skin-loss-radiative-fraction-1-000}
+
+This field is optional. If a Zone is named in the previous field and pump losses are to be added to a surrounding thermal zone, then this input determines the split between thermal radiation and thermal convection for the heat losses from the pump. If it is left blank then all the losses will be convective.
+
+\paragraph{Field: Design Power Sizing Method}\label{field-design-power-sizing-method-1}
+
+This field is optional. There are two choices PowerPerFlow and PowerPerFlowPerPressure. If omitted the default method of PowerPerFlowPerPressure will be used.
+
+If PowerPerFlow is used the pump's Design Power Consumption will be calculated using the sizing factor from the input field Design Electrical Power per Unit Flow Rate -- with Design Power Consumption = Design Maximum Flow Rate * scaling factor.
+
+If PowerPerFlowPerPressure is used the pump's Design Power Consumption will use the sizing factor from the input field Design Shaft Power per Unit Flow Rate Per Unit Head -- with Design Power Consumption = Design Maximum Flow Rate * Design Pump Head * scaling factor / Motor Efficiency.
+
+\paragraph{Field: Design Electrical Power per Unit Flow Rate}\label{field-design-electrical-power-per-unit-flow-rate}
+
+This field is optional. This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlow. It allows setting the efficiency the pumping system's power consumption using only the design flow rate. If omitted the default value of 348701.1 W/(m\(^{3}\)/s) (22 W/gpm) will be used.
+
+\paragraph{Field: Design Shaft Power per Unit Flow Rate Per Unit Head}\label{field-design-shaft-power-per-unit-flow-rate-per-unit-head-1}
+
+This field is optional. This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlowPerPressure. It allows controlling the efficiency of the impeller and drive assembly when calculating the pump power consumption for the design flow rate, motor efficiency, and pump head. If omitted the default value of 1.282051 W/((m\(^{3}\)/s)-Pa) will be used.
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+Pump:ConstantSpeed,
+  Circ Pump,                         !- Name
+  CW Supply Inlet Node,              !- Inlet Node Name
+  PumpChiller Node,                  !- Outlet Node Name
+  0.0011,                            !- Design Flow Rate
+  300000,                            !- Design Pump Head
+  700,                               !- Design Power Consumption
+  0.87,                              !- Motor Efficiency
+  0.0,                               !- Fraction of Motor Inefficiencies to Fluid Stream
+  Intermittent;                      !- Pump Control Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-020}
+
+\begin{itemize}
+\item
+  HVAC,Average,Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Pump Shaft Power {[}W{]}
+\item
+  HVAC,Average,Pump Fluid Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,Pump Fluid Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,Pump Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Pump Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Pump Zone Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Pump Zone Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Pump Zone Convective Heating Rate {[}W{]}
+\item
+  HVAC,Average,Pump Zone Radiative Heating Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Pump Electric Power {[}W{]}}\label{pump-electric-power-w-1}
+
+\paragraph{Pump Electric Energy {[}J{]}}\label{pump-electric-energy-j-1}
+
+These outputs are the electric power input to the pump motor. Consumption is metered on Pumps:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Pump Shaft Power {[}W{]}}\label{pump-shaft-power-w-1}
+
+This is the shaft power delivered from the motor to the pump.
+
+\paragraph{Pump Fluid Heat Gain Rate {[}W{]}}\label{pump-fluid-heat-gain-rate-w-1}
+
+\paragraph{Pump Fluid Heat Gain Energy {[}J{]}}\label{pump-fluid-heat-gain-energy-j-1}
+
+These outputs are the energy added to the fluid as heat. For the current algorithm, this is equal to Pump Shaft Power, because the loops are closed and all energy added to the fluid will ultimately become heat due to friction.
+
+\paragraph{Pump Outlet Temperature {[}C{]}}\label{pump-outlet-temperature-c-1}
+
+\paragraph{Pump Mass Flow Rate {[}kg/s{]}}\label{pump-mass-flow-rate-kgs-1}
+
+These outputs are the water outlet temperature and mass flow rate.
+
+\paragraph{Pump Zone Convective Heating Rate {[}W{]}}\label{pump-zone-convective-heating-rate-w-1}
+
+This output is the thermal loss from the pump to the surrounding Zone in the form of convective gains directly to the zone air. It is only available if a Zone was named in the pump input.
+
+\paragraph{Pump Zone Radiative Heating Rate {[}W{]}}\label{pump-zone-radiative-heating-rate-w-1}
+
+This output is the thermal loss from the pump to the surrounding Zone in the form of thermal radiation gains directly to the inside face of the zone s surfaces. It is only available if a Zone was named in the pump input.
+
+\paragraph{Pump Zone Total Heating Energy {[}J{]}}\label{pump-zone-total-heating-energy-j-1}
+
+\paragraph{Pump Zone Total Heating Rate {[}W{]}}\label{pump-zone-total-heating-rate-w-1}
+
+These outputs are the thermal losses from the pump to the surrounding Zone. They are only available if a Zone was named in the pump s input. These indicate the amount of heat added to the zone from the pump s inefficiencies. They are the total heat loss including both convection and radiation.
+
+\subsection{Pump:VariableSpeed:Condensate}\label{pumpvariablespeedcondensate}
+
+The Pump:VariableSpeed:Condensate object can only be used in steam system simulation for the condensate side of the loop. This is a variable speed pump, which pumps the condensate back to the steam boiler. The syntax for condensate pump is given below.
+
+\subsubsection{Inputs}\label{inputs-2-031}
+
+\paragraph{Field: Name}\label{field-name-2-030}
+
+This alpha field contains the identifying unique name for the pump.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-2-001}
+
+This alpha field contains the identifying name for the pump inlet node.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-2-001}
+
+This alpha field contains the identifying name for the pump outlet node.
+
+\paragraph{Field: Design Steam Volume Flow Rate}\label{field-design-steam-volume-flow-rate}
+
+This numeric field contains the pump's design volume flow rate in cubic meters per second. This field is autosizable. This is the volume flow rate of steam in expanded stated. The volume of condensate is calculated by the software from the steam density and is much lower.
+
+\paragraph{Field: Design Pump Head}\label{field-design-pump-head-2}
+
+This numeric field contains the pump's design head in Pascals. The default is 179352 Pa, or 60 ftH20, and is for a fairly large building.
+
+\paragraph{Field: Design Power Consumption}\label{field-design-power-consumption-2}
+
+This numeric field contains the pump's rated power consumption in Watts. If the user is performing a pressure simulation on the loop in which this pump is found, this value would only be used to estimate pump efficiency. During reported calculations, the pump would use the loop pressure drop and current flow conditions along with efficiency to calculate pump power dynamically. This field can be autosized. When set to autosize the type of scaling factor is chosen in the input field Design Power Sizing Method.
+
+\paragraph{Field: Motor Efficiency}\label{field-motor-efficiency-2-000}
+
+This numeric field contains the pump's efficiency in decimal form (0 = 0\%, 1 = 100\%).
+
+\paragraph{Field: Fraction of Motor Inefficiencies to Fluid Stream}\label{field-fraction-of-motor-inefficiencies-to-fluid-stream-2}
+
+This numeric field contains the pump's fraction of power loss to the fluid.
+
+\paragraph{Field: Coefficient 1 of the Part Load Performance Curve}\label{field-coefficient-1-of-the-part-load-performance-curve-1}
+
+This numeric field contains the first coefficient in the part load ratio curve. The fraction of full load power is determined by the cubic equation:
+
+\begin{equation}
+FractionFullLoadPower = {C_1} + {C_2}PLR + {C_3}PL{R^2} + {C_4}PL{R^3}
+\end{equation}
+
+where C\(_{1}\),C\(_{2}\),C\(_{3}\),and C\(_{4}\) are Coefficients 1 4 (below) and PLR is the Part Load Ratio.
+
+\paragraph{Field: Coefficient 2 of the Part Load Performance Curve}\label{field-coefficient-2-of-the-part-load-performance-curve-1}
+
+This numeric field contains the second coefficient in the part load ratio curve.
+
+\paragraph{Field: Coefficient 3 of the Part Load Performance Curve}\label{field-coefficient-3-of-the-part-load-performance-curve-1}
+
+This numeric field contains the third coefficient in the part load ratio curve.
+
+\paragraph{Field: Coefficient 4 of the Part Load Performance Curve}\label{field-coefficient-4-of-the-part-load-performance-curve-1}
+
+This numeric field contains the fourth coefficient in the part load ratio curve.
+
+\paragraph{Field: Pump Flow Rate Schedule Name}\label{field-pump-flow-rate-schedule-name-2}
+
+The schedule values modify the value for Rated Flow Rate of the pump on a time basis. This essentially sets the maximum value available for the pump at a given time, \textbf{not the actual flow rate at that time}. The default is that the pump is ON and runs according to its other operational requirements specified above. This schedule is for special, not typical pump operations. For additional control over pump flow, EMS actuators can be employed.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-2-004}
+
+This field is optional. It can be used to input the name of the Zone in which the pump is located in the model. If the pump is outdoors, or skin losses are not to be modeled, then leave this field blank. If a valid Zone name is entered, then the portion of electrical power consumed by the pump that is not added to the working fluid is added to the surrounding Zone.
+
+\paragraph{Field: Skin Loss Radiative Fraction}\label{field-skin-loss-radiative-fraction-2}
+
+This field is optional. If a Zone is named in the previous field and pump losses are to be added to a surrounding thermal zone, then this input determines the split between thermal radiation and thermal convection for the heat losses from the pump. If it is left blank then all the losses will be convective.
+
+\paragraph{Field: Design Power Sizing Method}\label{field-design-power-sizing-method-2}
+
+This field is optional. There are two choices PowerPerFlow and PowerPerFlowPerPressure. If PowerPerFlow is used the pump's Design Power Consumption will be calculated using the sizing factor from the input field Design Electric Power per Unit Flow Rate -- with Design Power Consumption = Design Maximum Flow Rate * scaling factor. If PowerPerFlowPerPressure is used the pump's Design Power Consumption will use the sizing factor from the input field Design Shaft Power per Unit Flow Rate Per Unit Head -- with Design Power Consumption = Design Maximum Flow Rate * Design Pump Head * scaling factor / Motor Efficiency. If omitted the default method of PowerPerFlowPerPressure will be used.
+
+\paragraph{Field: Design Electric Power per Unit Flow Rate}\label{field-design-electric-power-per-unit-flow-rate-1}
+
+This field is optional. This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlow. It allows setting the efficiency the pumping system's power consumption using only the design flow rate. If omitted the default value of 348701.1 W/(m\(^{3}\)/s) ( 22 W/gpm) will be used.
+
+\paragraph{Field: Design Shaft Power per Unit Flow Rate Per Unit Head}\label{field-design-shaft-power-per-unit-flow-rate-per-unit-head-2}
+
+This field is optional. This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlowPerPressure. It allows setting the efficiency of the impeller and drive assembly when calculating the pump power consumption for the design flow rate, motor efficiency, and pump head. If omitted the default value of 1.282051 W/((m\(^{3}\)/s)-Pa) will be used.
+
+Examples of this object in the IDF follow.
+
+\begin{lstlisting}
+
+Pump:VariableSpeed:Condensate,
+  Steam Boiler Plant Steam Circ Pump,         !- Name
+  Steam Boiler Plant Steam Supply Inlet Node, !- Inlet Node Name
+  Steam Boiler Plant Steam Pump Outlet Node,  !- Outlet Node Name
+  0.36,                                  !- Design Steam Volume Flow Rate {m3/s}
+  179352,                                !- Design Pump Head {Pa}
+  400,                                   !- Design Power Consumption {W}
+  0.9,                                   !- Motor Efficiency
+  0.0,                                   !- Fraction of Motor Inefficiencies to Fluid Stream
+  0,                                     !- Coefficient 1 of the Part Load Performance Curve
+  1,                                     !- Coefficient 2 of the Part Load Performance Curve
+  0,                                     !- Coefficient 3 of the Part Load Performance Curve
+  0;                                     !- Coefficient 4 of the Part Load Performance Curve
+
+
+  Pump:VariableSpeed:Condensate,
+  Steam Boiler Plant Steam Circ Pump,         !- Name
+  Steam Boiler Plant Steam Supply Inlet Node, !- Inlet Node Name
+  Steam Boiler Plant Steam Pump Outlet Node,  !- Outlet Node Name
+  0.36,                                  !- Design Steam Volume Flow Rate {m3/s}
+  179352,                                !- Design Pump Head {Pa}
+  autosize,                              !- Design Power Consumption {W}
+  0.9,                                   !- Motor Efficiency
+  0.0,                                   !- Fraction of Motor Inefficiencies to Fluid Stream
+  0,                                     !- Coefficient 1 of the Part Load Performance Curve
+  1,                                     !- Coefficient 2 of the Part Load Performance Curve
+  0,                                     !- Coefficient 3 of the Part Load Performance Curve
+  0;                                     !- Coefficient 4 of the Part Load Performance Curve
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-016}
+
+\begin{itemize}
+\item
+  HVAC,Average,Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Pump Shaft Power {[}W{]}
+\item
+  HVAC,Average,Pump Fluid Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,Pump Fluid Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,Pump Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Pump Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average, Pump Zone Total Heating Rate {[}W{]}
+\item
+  HVAC, Sum, Pump Zone Total Heating Energy {[}J{]}
+\item
+  HVAC, Average, Pump Zone Convective Heating Rate {[}W{]}
+\item
+  HVAC, Average, Pump Zone Radiative Heating Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Pump Electric Power {[}W{]}}\label{pump-electric-power-w-2}
+
+\paragraph{Pump Electric Energy {[}J{]}}\label{pump-electric-energy-j-2}
+
+These outputs are the electric power input to the pump motor. Consumption is metered on Pumps:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Pump Shaft Power {[}W{]}}\label{pump-shaft-power-w-2}
+
+This is the shaft power delivered from the motor to the pump.
+
+\paragraph{Pump Fluid Heat Gain Rate {[}W{]}}\label{pump-fluid-heat-gain-rate-w-2}
+
+\paragraph{Pump Fluid Heat Gain Energy {[}J{]}}\label{pump-fluid-heat-gain-energy-j-2}
+
+These outputs are the energy added to the fluid as heat. For the current algorithm, this is equal to Pump Shaft Power, because the loops are closed and all energy added to the fluid will ultimately become heat due to friction.
+
+\paragraph{Pump Outlet Temperature {[}C{]}}\label{pump-outlet-temperature-c-2}
+
+\paragraph{Pump Mass Flow Rate {[}kg/s{]}}\label{pump-mass-flow-rate-kgs-2}
+
+These outputs are the water outlet temperature and mass flow rate.
+
+\paragraph{Pump Zone Total Heating Rate {[}W{]}}\label{pump-zone-total-heating-rate-w-2}
+
+\paragraph{Pump Zone Total Heating Energy {[}J{]}}\label{pump-zone-total-heating-energy-j-2}
+
+These outputs are the thermal losses from the pump to the surrounding Zone. They are only available if a Zone was named in the pump s input. These indicate the amount of heat added to the zone from the pump s inefficiencies. They are the total heat loss including both convection and radiation.
+
+\paragraph{Pump Zone Convective Heating Rate {[}W{]}}\label{pump-zone-convective-heating-rate-w-2}
+
+This output is the thermal loss from the pump to the surrounding Zone in the form of convective gains directly to the zone air. It is only available if a Zone was named in the pump input.
+
+\paragraph{Pump Zone Radiative Heating Rate {[}W{]}}\label{pump-zone-radiative-heating-rate-w-2}
+
+This output is the thermal loss from the pump to the surrounding Zone in the form of thermal radiation gains directly to the inside face of the zone s surfaces. It is only available if a Zone was named in the pump input.
+
+\subsection{HeaderedPumps:ConstantSpeed}\label{headeredpumpsconstantspeed}
+
+Headered pumps are components with more than one identical pumps connected in parallel. The syntax for HeaderedPumps:ConstantSpeed is as follows.
+
+\subsubsection{Inputs}\label{inputs-3-027}
+
+\paragraph{Field: Name}\label{field-name-3-024}
+
+This alpha field contains the identifying name for the pump bank.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-3-000}
+
+This alpha field contains the identifying name for the pump bank inlet node.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-3-000}
+
+This alpha field contains the identifying name for the pump bank outlet node.
+
+\paragraph{Field: Total Design Flow Rate}\label{field-total-design-flow-rate}
+
+This numeric field contains the pump bank s rated volumetric flow rate in cubic meters per second. This is equal to the product of number of pumps and the flow rate of each individual pump. The field can be autosized.
+
+\paragraph{Field: Number of Pumps in Bank}\label{field-number-of-pumps-in-bank}
+
+The numeric field specifies the number of pumps present in the pump bank. All these pumps are connected in parallel internally.
+
+\paragraph{Field: Flow Sequencing Control Scheme}\label{field-flow-sequencing-control-scheme}
+
+The alpha field specifies the scheme for sequencing flow. Currently the only choice is Sequential, where a pump in the pump bank will be turned ON only after fully loading the previous pump.
+
+\paragraph{Field: Design Pump Head}\label{field-design-pump-head-3}
+
+This numeric field contains the pump s rated head pressure in Pascals.
+
+\paragraph{Field: Design Power Consumption}\label{field-design-power-consumption-3}
+
+This numeric field contains the pump bank s total power consumption in Watts. This field is equal to the product of number of pumps and the rated power consumption of each individual pump. If the user is performing a pressure simulation on the loop in which this pump bank is found, this value would only be used to estimate pump efficiency. During reported calculations, the pump would use the loop pressure drop and current flow conditions along with efficiency to calculate pump power dynamically. This field can be autosized. When set to autosize the type of scaling factor is chosen in the input field Design Power Sizing Method.
+
+\paragraph{Field: Motor Efficiency}\label{field-motor-efficiency-3-000}
+
+This numeric field contains the pump s efficiency in decimal form (0 = 0\%, 1 = 100\%).
+
+\paragraph{Field: Fraction of Motor Inefficiencies to Fluid Stream}\label{field-fraction-of-motor-inefficiencies-to-fluid-stream-3}
+
+This numeric field contains the pump s fraction of power loss to the fluid.
+
+\paragraph{Field: Pump Control Type}\label{field-pump-control-type-2-000}
+
+This is a choice field of Continuous or Intermittent. The operation of a constant speed pump bank is fairly straightforward. If the user designates a constant speed pump bank that is operating continuously, the pump bank will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump bank is constant speed and operates intermittently, the pump bank will run at its capacity if a load is sensed and will shut off if there is no load on the loop. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this control by forcing the pump to be on or off.
+
+\paragraph{Field: Pump Flow Rate Schedule Name}\label{field-pump-flow-rate-schedule-name-3}
+
+The schedule values modify the value for Rated Flow Rate of the pump on a time basis. This essentially sets the maximum value available for the pump at a given time, \textbf{not the actual flow rate at that time}. The default is that the pump is ON and runs according to its other operational requirements specified above. This schedule is for special, not typical pump operations. For additional control over pump flow, EMS actuators can be employed.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-3-003}
+
+This field is optional. It can be used to input the name of the Zone in which the pump is located in the model. If the pump is outdoors, or skin losses are not to be modeled, then leave this field blank. If a valid Zone name is entered, then the portion of electrical power consumed by the pump that is not added to the working fluid is added to the surrounding Zone.
+
+\paragraph{Field: Skin Loss Radiative Fraction}\label{field-skin-loss-radiative-fraction-3}
+
+This field is optional. If a Zone is named in the previous field and pump losses are to be added to a surrounding thermal zone, then this input determines the split between thermal radiation and thermal convection for the heat losses from the pump. If it is left blank then all the losses will be convective.
+
+\paragraph{Field: Design Power Sizing Method}\label{field-design-power-sizing-method-3}
+
+This field is optional. There are two choices PowerPerFlow and PowerPerFlowPerPressure. If PowerPerFlow is used the pump's Design Power Consumption will be calculated using the sizing factor from the input field Design Electric Power per Unit Flow Rate -- with Design Power Consumption = Design Maximum Flow Rate * scaling factor. If PowerPerFlowPerPressure is used the pump's Design Power Consumption will use the sizing factor from the input field Design Shaft Power per Unit Flow Rate Per Unit Head -- with Design Power Consumption = Design Maximum Flow Rate * Design Pump Head * scaling factor / Motor Efficiency. If omitted the default method of PowerPerFlowPerPressure will be used.
+
+\paragraph{Field: Design Electric Power per Unit Flow Rate}\label{field-design-electric-power-per-unit-flow-rate-2}
+
+This field is optional. This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlow. It allows setting the efficiency the pumping system's power consumption using only the design flow rate. If omitted the default value of 348701.1 W/(m\(^{3}\)/s) ( 22 W/gpm) will be used.
+
+\paragraph{Field: Design Shaft Power per Unit Flow Rate Per Unit Head}\label{field-design-shaft-power-per-unit-flow-rate-per-unit-head-3}
+
+This field is optional. This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlowPerPressure. It allows setting the efficiency of the impeller and drive assembly when calculating the pump power consumption for the design flow rate, motor efficiency, and pump head. If omitted the default value of 1.282051 W/((m\(^{3}\)/s)-Pa) will be used.
+
+An example for constant speed pump bank follows.
+
+\begin{lstlisting}
+
+HeaderedPumps:ConstantSpeed,
+  Chilled Water Headered Pumps,           !- Name
+  CW Supply Inlet Node,                   !- Inlet Node Name
+  CW Pumps Outlet Node,                   !- Outlet Node Name
+  autosize,                               !- Total Design Flow Rate
+  2,                                      !- Number of Pumps in Bank
+  SEQUENTIAL,                             !- Flow Sequencing Control Scheme
+  179352,                                 !- Design Pump Head
+  autosize,                               !- Design Power Consumption
+  0.9,                                    !- Motor Efficiency
+  0.0,                                    !- Fraction of Motor Inefficiencies to Fluid Stream
+  INTERMITTENT,                           !- Pump Control Type
+  CoolingPumpAvailSched;                  !- Pump Flow Rate Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-014}
+
+\begin{itemize}
+\item
+  HVAC,Average,Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum, Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Pump Shaft Power {[}W{]}
+\item
+  HVAC,Average, Pump Fluid Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum, Pump Fluid Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average, Pump Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Pump Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Number of Pumps Operating {[]}
+\item
+  HVAC, Average, Pump Zone Total Heating Rate {[}W{]}
+\item
+  HVAC, Sum, Pump Zone Total Heating Energy {[}J{]}
+\item
+  HVAC, Average, Pump Zone Convective Heating Rate {[}W{]}
+\item
+  HVAC, Average, Pump Zone Radiative Heating Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Pump Electric Power {[}W{]}}\label{pump-electric-power-w-3}
+
+\paragraph{Pump Electric Energy {[}J{]}}\label{pump-electric-energy-j-3}
+
+These outputs are the electric power input to the pump motor. Consumption is metered on Pumps:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Pump Shaft Power {[}W{]}}\label{pump-shaft-power-w-3}
+
+This is the shaft power delivered from the motor to the pump.
+
+\paragraph{Pump Fluid Heat Gain Rate {[}W{]}}\label{pump-fluid-heat-gain-rate-w-3}
+
+\paragraph{Pump Fluid Heat Gain Energy {[}J{]}}\label{pump-fluid-heat-gain-energy-j-3}
+
+These outputs are the energy added to the fluid as heat. For the current algorithm, this is equal to Pump Shaft Power, because the loops are closed and all energy added to the fluid will ultimately become heat due to friction.
+
+\paragraph{Pump Outlet Temperature {[}C{]}}\label{pump-outlet-temperature-c-3}
+
+\paragraph{Pump Mass Flow Rate {[}kg/s{]}}\label{pump-mass-flow-rate-kgs-3}
+
+These outputs are the water outlet temperature and mass flow rate.
+
+\paragraph{\texorpdfstring{Pump Operating Pumps Count {[]}}{Pump Operating Pumps Count }}\label{pump-operating-pumps-count}
+
+This output tells the number of pumps in the pump bank operating at any reporting frequency.
+
+\paragraph{Pump Zone Total Heating Rate {[}W{]}}\label{pump-zone-total-heating-rate-w-3}
+
+\paragraph{Pump Zone Total Heating Energy {[}J{]}}\label{pump-zone-total-heating-energy-j-3}
+
+These outputs are the thermal losses from the pump to the surrounding Zone. They are only available if a Zone was named in the pump s input. These indicate the amount of heat added to the zone from the pump s inefficiencies. They are the total heat loss including both convection and radiation.
+
+\paragraph{Pump Zone Convective Heating Rate {[}W{]}}\label{pump-zone-convective-heating-rate-w-3}
+
+This output is the thermal loss from the pump to the surrounding Zone in the form of convective gains directly to the zone air. It is only available if a Zone was named in the pump input.
+
+\paragraph{Pump Zone Radiative Heating Rate {[}W{]}}\label{pump-zone-radiative-heating-rate-w-3}
+
+This output is the thermal loss from the pump to the surrounding Zone in the form of thermal radiation gains directly to the inside face of the zone s surfaces. It is only available if a Zone was named in the pump input.
+
+\subsection{HeaderedPumps:VariableSpeed}\label{headeredpumpsvariablespeed}
+
+Headered pumps are components with more than one identical pumps connected in parallel. Currently this object may be found only in plant loops. The syntax for a HeaderedPumps:VariableSpeed pump is given below.
+
+\subsubsection{Inputs}\label{inputs-4-024}
+
+\paragraph{Field: Name}\label{field-name-4-021}
+
+This alpha field contains the identifying unique name for the pump bank.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-4}
+
+This alpha field contains the identifying name for the pump bank inlet node.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-4}
+
+This alpha field contains the identifying name for the pump bank outlet node.
+
+\paragraph{Field: Total Design Flow Rate}\label{field-total-design-flow-rate-1}
+
+This numeric field contains the pump bank's rated volume flow rate in cubic meters per second. This is equal to the product of number of pumps and the flow rate of each individual pump. The field can be autosized.
+
+\paragraph{Field: Number of Pumps in Bank}\label{field-number-of-pumps-in-bank-1}
+
+The numeric field specifies the number of pumps present in the pump bank. All these pumps are connected in parallel internally.
+
+\paragraph{Field: Flow Sequencing Control Scheme}\label{field-flow-sequencing-control-scheme-1}
+
+The alpha field specifies the scheme for sequencing flow. Currently the only choice is Sequential, where a pump in the pump bank will be turned ON only after fully loading the previous pump.
+
+\paragraph{Field: Design Pump Head}\label{field-design-pump-head-4}
+
+This numeric field contains the pump s rated head in Pascals.
+
+\paragraph{Field: Design Power Consumption}\label{field-design-power-consumption-4}
+
+This numeric field contains the pump bank's total power consumption in Watts. This field is equal to the product of number of pumps and the design power consumption of each individual pump. If the user is performing a pressure simulation on the loop in which this pump bank is found, this value would only be used to estimate pump efficiency. During reported calculations, the pump would use the loop pressure drop and current flow conditions along with efficiency to calculate pump power dynamically. This field can be autosized. When set to autosize the type of scaling factor is chosen in the input field Design Power Sizing Method.
+
+\paragraph{Field: Motor Efficiency}\label{field-motor-efficiency-4}
+
+This numeric field contains the efficiency of the individual pump (which will be equivalent to pump bank efficiency) in decimal form (0 = 0\%, 1 = 100\%).
+
+\paragraph{Field: Fraction of Motor Inefficiencies to Fluid Stream}\label{field-fraction-of-motor-inefficiencies-to-fluid-stream-4}
+
+This numeric field contains the individual pump s fraction of power loss to the fluid.
+
+\paragraph{Field: Coefficient 1 of the Part Load Performance Curve}\label{field-coefficient-1-of-the-part-load-performance-curve-2}
+
+This numeric field contains the first coefficient (\emph{C\(_{1}\)}) in the part load ratio curve. The fraction of full load power is determined by the cubic equation:
+
+\begin{equation}
+FractionFullLoadPower = {C_1} + {C_2}PLR + {C_3}PL{R^2} + {C_4}PL{R^3}
+\end{equation}
+
+where C\(_{1}\),C\(_{2}\),C\(_{3}\),and C\(_{4}\) are Coefficients 1 4 (below) and PLR is the Part Load Ratio.
+
+\paragraph{Field: Coefficient 2 of the Part Load Performance Curve}\label{field-coefficient-2-of-the-part-load-performance-curve-2}
+
+This numeric field contains the second coefficient (\emph{C\(_{2}\)}) in the part load ratio curve.
+
+\paragraph{Field: Coefficient 3 of the Part Load Performance Curve}\label{field-coefficient-3-of-the-part-load-performance-curve-2}
+
+This numeric field contains the third coefficient (\emph{C\(_{3}\)}) in the part load ratio curve.
+
+\paragraph{Field: Coefficient 4 of the Part Load Performance Curve}\label{field-coefficient-4-of-the-part-load-performance-curve-2}
+
+This numeric field contains the fourth coefficient (\emph{C\(_{4}\)}) in the part load ratio curve.
+
+\paragraph{Field: Minimum Flow Rate Fraction}\label{field-minimum-flow-rate-fraction}
+
+The numeric field specifies the minimum flow allowed for the pump bank as a fraction of the nominal flow. If the requested flow is less than minimum flow pump bank runs at minimum flow.
+
+\paragraph{Field: Pump Control Type}\label{field-pump-control-type-3}
+
+This is a choice field of Continuous or Intermittent. A variable speed pump bank is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump bank is operating intermittently, then the bank can shutdown. For any other condition such as the loop having a load and the pump bank is operating intermittently or the pump bank is continuously operating (regardless of the loading condition), the bank will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump bank is running, it will try to meet the flow request made by demand side components. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this control by forcing the pump to be on or off.
+
+\paragraph{Field: Pump Flow Rate Schedule Name}\label{field-pump-flow-rate-schedule-name-4}
+
+The schedule values modify the value for Rated Flow Rate of the pump on a time basis. This essentially sets the maximum value available for the pump at a given time, \textbf{not the actual flow rate at that time}. The default is that the pump is ON and runs according to its other operational requirements specified above. This schedule is for special, not typical pump operations. For additional control over pump flow, EMS actuators can be employed.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-4-003}
+
+This field is optional. It can be used to input the name of the Zone in which the pump is located in the model. If the pump is outdoors, or skin losses are not to be modeled, then leave this field blank. If a valid Zone name is entered, then the portion of electrical power consumed by the pump that is not added to the working fluid is added to the surrounding Zone.
+
+\paragraph{Field: Skin Loss Radiative Fraction}\label{field-skin-loss-radiative-fraction-4}
+
+This field is optional. If a Zone is named in the previous field and pump losses are to be added to a surrounding thermal zone, then this input determines the split between thermal radiation and thermal convection for the heat losses from the pump. If it is left blank then all the losses will be convective.
+
+\paragraph{Field: Design Power Sizing Method}\label{field-design-power-sizing-method-4}
+
+This field is optional. There are two choices PowerPerFlow and PowerPerFlowPerPressure. If PowerPerFlow is used the pump's Design Power Consumption will be calculated using the sizing factor from the input field Design Electric Power per Unit Flow Rate -- with Design Power Consumption = Design Maximum Flow Rate * scaling factor. If PowerPerFlowPerPressure is used the pump's Design Power Consumption will use the sizing factor from the input field Design Shaft Power per Unit Flow Rate Per Unit Head -- with Design Power Consumption = Design Maximum Flow Rate * Design Pump Head * scaling factor / Motor Efficiency. If omitted the default method of PowerPerFlowPerPressure will be used.
+
+\paragraph{Field: Design Electric Power per Unit Flow Rate}\label{field-design-electric-power-per-unit-flow-rate-3}
+
+This field is optional. This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlow. It allows setting the efficiency the pumping system's power consumption using only the design flow rate. If omitted the default value of 348701.1 W/(m\(^{3}\)/s) ( 22 W/gpm) will be used.
+
+\paragraph{Field: Design Shaft Power per Unit Flow Rate Per Unit Head}\label{field-design-shaft-power-per-unit-flow-rate-per-unit-head-4}
+
+This field is optional. This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlowPerPressure. It allows setting the efficiency of the impeller and drive assembly when calculating the pump power consumption for the design flow rate, motor efficiency, and pump head. If omitted the default value of 1.282051 W/((m\(^{3}\)/s)-Pa) will be used.
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+HeaderedPumps:VariableSpeed,
+  Chilled Water Headered Pumps, !- Name
+  CW Supply Inlet Node,       !- Inlet Node Name
+  CW Pumps Outlet Node,       !- Outlet Node Name
+  autosize,                   !- Total Design Flow Rate {m3/s}
+  2,                          !- Number of Pumps in Bank
+  SEQUENTIAL,                 !- Flow Sequencing Control Scheme
+  179352,                     !- Design Pump Head {Pa}
+  autosize,                   !- Design Power Consumption {W}
+  0.9,                        !- Motor Efficiency
+  0.0,                        !- Fraction of Motor Inefficiencies to Fluid Stream
+  0,                          !- Coefficient 1 of the Part Load Performance Curve
+  1,                          !- Coefficient 2 of the Part Load Performance Curve
+  0,                          !- Coefficient 3 of the Part Load Performance Curve
+  0,                          !- Coefficient 4 of the Part Load Performance Curve
+  0.1,                        !- Minimum Flow Rate {m3/s}
+  INTERMITTENT,               !- Pump Control Type
+  CoolingPumpAvailSched;      !- Pump Flow Rate Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-011}
+
+\begin{itemize}
+\item
+  HVAC,Average,Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum, Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Pump Shaft Power {[}W{]}
+\item
+  HVAC,Average, Pump Fluid Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum, Pump Fluid Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average, Pump Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Pump Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Number of pumps operating {[]}
+\item
+  HVAC, Average, Pump Zone Total Heating Rate {[}W{]}
+\item
+  HVAC, Sum, Pump Zone Total Heating Energy {[}J{]}
+\item
+  HVAC, Average, Pump Zone Convective Heating Rate {[}W{]}
+\item
+  HVAC, Average, Pump Zone Radiative Heating Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Pump Electric Power {[}W{]}}\label{pump-electric-power-w-4}
+
+\paragraph{Pump Electric Energy {[}J{]}}\label{pump-electric-energy-j-4}
+
+These outputs are the electric power input to the pump motor. Consumption is metered on Pumps:Electricity, Electricity:Plant, and Electricity:Facility.
+
+\paragraph{Pump Shaft Power {[}W{]}}\label{pump-shaft-power-w-4}
+
+This is the shaft power delivered from the motor to the pump.
+
+\paragraph{Pump Fluid Heat Gain Rate {[}W{]}}\label{pump-fluid-heat-gain-rate-w-4}
+
+\paragraph{Pump Fluid Heat Gain Energy {[}J{]}}\label{pump-fluid-heat-gain-energy-j-4}
+
+These outputs are the energy added to the fluid as heat. For the current algorithm, this is equal to Pump Shaft Power, because the loops are closed and all energy added to the fluid will ultimately become heat due to friction.
+
+\paragraph{Pump Outlet Temperature {[}C{]}}\label{pump-outlet-temperature-c-4}
+
+\paragraph{Pump Mass Flow Rate {[}kg/s{]}}\label{pump-mass-flow-rate-kgs-4}
+
+These outputs are the water outlet temperature and mass flow rate.
+
+\paragraph{\texorpdfstring{Pump Operating Pumps Count {[]}}{Pump Operating Pumps Count }}\label{pump-operating-pumps-count-1}
+
+This output tells the number of pumps in the pump bank operating at any reporting frequency.
+
+\paragraph{Pump Zone Total Heating Rate {[}W{]}}\label{pump-zone-total-heating-rate-w-4}
+
+\paragraph{Pump Zone Total Heating Energy {[}J{]}}\label{pump-zone-total-heating-energy-j-4}
+
+These outputs are the thermal losses from the pump to the surrounding Zone. They are only available if a Zone was named in the pump s input. These indicate the amount of heat added to the zone from the pump s inefficiencies. They are the total heat loss including both convection and radiation.
+
+\paragraph{Pump Zone Convective Heating Rate {[}W{]}}\label{pump-zone-convective-heating-rate-w-4}
+
+This output is the thermal loss from the pump to the surrounding Zone in the form of convective gains directly to the zone air. It is only available if a Zone was named in the pump input.
+
+\paragraph{Pump Zone Radiative Heating Rate {[}W{]}}\label{pump-zone-radiative-heating-rate-w-4}
+
+This output is the thermal loss from the pump to the surrounding Zone in the form of thermal radiation gains directly to the inside face of the zone s surfaces. It is only available if a Zone was named in the pump input.
diff --git a/doc/input-output-reference/src/overview/group-radiative-convective-units.tex b/doc/input-output-reference/src/overview/group-radiative-convective-units.tex
new file mode 100644
index 00000000000..c1b03572d38
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-radiative-convective-units.tex
@@ -0,0 +1,2065 @@
+\section{\texorpdfstring{Group -- Radiative \textbf{/} Convective Units}{Group -- Radiative / Convective Units}}\label{group-radiative-convective-units}
+
+This section describes the radiative/convective zone equipment units.~ The following units are included in this section:
+
+\begin{itemize}
+\item
+  ZoneHVAC:Baseboard:Convective:Electric
+\item
+  ZoneHVAC:Baseboard:RadiantConvective:Water
+\item
+  ZoneHVAC:Baseboard:RadiantConvective:Steam
+\item
+  ZoneHVAC:Baseboard:RadiantConvective:Electric
+\item
+  ZoneHVAC:Baseboard:Convective:Water
+\item
+  ZoneHVAC:HighTemperatureRadiant
+\item
+  ZoneHVAC:LowTemperatureRadiant:ConstantFlow
+\item
+  ZoneHVAC:LowTemperatureRadiant:Electric
+\item
+  ZoneHVAC:LowTemperatureRadiant:VariableFlow
+\end{itemize}
+
+\subsection{ZoneHVAC:Baseboard:RadiantConvective:Water}\label{zonehvacbaseboardradiantconvectivewater}
+
+The objective of this model is to calculate the convective and radiant heat transfer from water baseboard heaters to the people and the surfaces within a zone so that surface heat balances can take into account the radiant heat transfer to the surfaces and thus enhance the accuracy of thermal comfort predictions within the space. The radiant heat gains are distributed to the surfaces by fractions defined by user input.
+
+\subsubsection{Inputs}\label{inputs-038}
+
+\paragraph{Field: Name}\label{field-name-037}
+
+A unique user assigned name for an instance of a hot water baseboard heater unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-013}
+
+The name of the schedule (ref: Schedule) that denotes whether the hot water baseboard heater unit can run during a given time period. A schedule value equal to 0 denotes that the unit must be off for that time period. A value greater than 0 denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-006}
+
+This field is the name of the hot water inlet node for the baseboard heater.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-007}
+
+This field is the name of the hot water outlet node for the baseboard heater.
+
+\paragraph{Field: Rated AverageWaterTemperature}\label{field-rated-averagewatertemperature}
+
+This field is the rated average water temperature for the baseboard heater which is published in the manufacturer's literature in degree Celsius. It typically ranges from 65.56°C to 115.36°C in the I = B = R rating document while the lowest allowable temperature is 32.22°C. The default value is 87.78°C. If the user does not enter this field, the default value is assumed.
+
+\paragraph{Field: Rated Water Mass Flow Rate}\label{field-rated-water-mass-flow-rate}
+
+This field is the rated standard water flow rate in kg/s which is published as part of the manufacturer's literature. It is used by the manufacturers when determining the rated capacity (see next field). The default value is 0.063kg/s. If it is blank or zero, the default values is assumed.
+
+\paragraph{Field: Heating Design Capacity Method}\label{field-heating-design-capacity-method-000}
+
+Enter the method used to determine the heating design capacity or the method for scalable sizing. Input allowed is either \emph{HeatingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedHeatingCapacity}. If this input field is left blank or zero, then autosizing is assumed. \emph{HeatingDesignCapacity} means user specifies the magnitude of heating capacity or the program calculates the design heating capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the radiant baseboard unit. \emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is \emph{HeatingDesignCapacity}.
+
+\paragraph{Field: Heating Design Capacity \{W\}}\label{field-heating-design-capacity-w-000}
+
+This field is the radiant-convective water baseboard rated capacity in watts at a rated water mass flow rate (see input field Rated Mass Flow Rate). Almost all publications from manufacturers indicate it as W/m (Btuh per linear foot). The user thus must multiply it by the active length of the unit. The active length is available in the literature. Manufacturers are required to publish the difference between active and total length of the unit (I = B = R rating for boilers baseboard radiation, 2009).If it is blank or zero, autosizing is assumed. Design day sizing run must be specified for autosizing.
+
+\paragraph{Field: Heating Design Capacity Per Floor Area \{W/m2\}}\label{field-heating-design-capacity-per-floor-area-wm2-000}
+
+Enter the rated heating capacity per unit floor area of radiant-convective water baseboard unit in m3/s-m2. This field is required field when the Heating Design Capacity Method is \emph{CapacityPerFloorArea}. The program calculates the heating capacity from floor area of the zone served by the radiant baseboard unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
+
+\paragraph{Field: Fraction of Autosized Heating Design Capacity}\label{field-fraction-of-autosized-heating-design-capacity-000}
+
+Enter the heating capacity as a fraction of the autosized heating capacity of radiant-convective water baseboard. This input field is required when the Heating Design Capacity Method is \emph{FractionOfAutosizedHeatingCapacity}. The program calculates the heating capacity from the design autosized heating capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
+
+\paragraph{Field: Maximum Water Flow Rate}\label{field-maximum-water-flow-rate-001}
+
+This field is the maximum water volumetric flow rate in m\(^{3}\)/sec.~ It can be autosized by EnergyPlus.
+
+\paragraph{Field: Convergence Tolerance}\label{field-convergence-tolerance-000}
+
+This field is the control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. For hot water baseboards, the model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {({Q_{bb,out}} - {Q_{ZoneLoad}})} \right|}}{{{Q_{ZoneLoad}}}} \le Convergence{\kern 1pt} Tolerance
+\end{equation}
+
+The default is 0.001.
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant-000}
+
+This field specifies what fraction of the power input to the baseboard heater is actually transferred to the space as radiant heat. The fraction should be between 0 and 1. This is the portion of the total power that is modeled as radiation. The portion that is radiant heat transfer from the baseboard heater is distributed to people and specific surfaces using the remaining fields. Note that the sum of the fractions in the remaining fields (people and surfaces) must equal 1.0 so that all the radiant power is distributed properly. For more information on the specification of this parameter, please see the Engineering Reference for EnergyPlus.
+
+\paragraph{Field: Fraction of Radiant Energy Incident on People}\label{field-fraction-of-radiant-energy-incident-on-people}
+
+This field specifies the fraction of radiant portion of heat transfer to the zone from the baseboard heater that is incident directly on people within the space. This has an impact on the predicted thermal comfort of the zone occupants. Note that although this energy is ``radiant'' it is actually modeled in the zone heat balance as convective energy (like an internal gain). The basic assumption here is that most radiant energy falling on people will most likely be rereleased to the zone air by convection. This is a simplification of reality, but it maintains the overall energy balance.
+
+\paragraph{Field Set: Surface Name, Fraction of Radiant Energy to Surface}\label{field-set-surface-name-fraction-of-radiant-energy-to-surface}
+
+The following two items are repeated up to a maximum of 20 surface/fraction pairs. At least one surface/fraction pair must appear in an input file. In other words, at least one surface must be identified as a recipient of radiant energy from the baseboard heater.
+
+\paragraph{Field: Surface \textless{}x\textgreater{} Name}\label{field-surface-x-name}
+
+This field is the name of the first surface to which radiant heat transfer from the baseboard heater is distributed. Used in conjunction with the next field, it helps to define the distribution of the radiant energy on the surfaces within the zone. Note that up to 20 pairs of surface names and corresponding fractions may be entered for a single radiant heater system.
+
+\paragraph{Field: Fraction of Radiant Energy to Surface \textless{}x\textgreater{}}\label{field-fraction-of-radiant-energy-to-surface-x}
+
+This field is paired with the preceding surface name (previous field) to define the fraction of radiant heat transfer leaving the baseboard heater that is incident on a particular surface. Users should take into account the directionality of baseboard heaters and their location when defining the value for this input field.
+
+\textbf{\emph{Note on Fraction of Radiant Energy Incident on People and to Surfaces}}
+
+The radiant energy from the baseboard heater is defined by the total energy input to the baseboard heater from the water loop times the fraction radiant field shown above. This radiant energy is distributed to surfaces and people using the surface and fraction pairs and the fraction to people input by the user. These fractions to people and surfaces must add up to 1.0. In other words, in an input file, the following relation should be maintained by the user input:
+
+\begin{equation}
+FractionIndicentOnPeople + \sum {FractionToSurfaces = 1}
+\end{equation}
+
+An example IDF for the water baseboard is shown below.
+
+\begin{lstlisting}
+
+ZoneHVAC:Baseboard:RadiantConvective:Water,
+      SPACE2-1 Baseboard,      !- Baseboard Name
+      ReheatCoilAvailSched,    !- Availability Schedule Name
+      SPACE2-1 Zone Coil Water In Node,  !- Inlet\_Node
+      SPACE2-1 Zone Coil Water Out Node,  !- Outlet\_Node
+      76.67,                   !- Average Water Temperature {C}
+      0.063,                   !- Standard Water Mass Flow Rate {Kg/s}
+      HeatingDesignCapacity,   !- Heating Design Capacity Method
+      3000.0,                  !- Heating Design Capacity{ W }
+      ,                        !- Heating Design Capacity Per Floor Area{ W / m2 }
+      ,                        !- Fraction of Autosized Heating Design Capacity{ -}
+      0.0013,                  !- Max Water Volumetric Flow Rate {m3/s}
+      0.001,                   !- Convergence Tolerance
+      0.3,                     !- Fraction radiant
+      0.3,                     !- Fraction of radiant energy incident on people
+      C2-1,                    !- Surface 1 Name
+      0.1,                     !- Fraction of radiant energy from heater distributed to surface 1
+      F2-1,                    !- Surface 2 Name
+      0.2,                     !- Fraction of radiant energy from heater distributed to surface 2
+      SB21,                    !- surface 3 Name
+      0.1,                     !- fraction of radiant energy from heater distributed to surface 3
+      SB23,                    !- surface 4 Name
+      0.1,                     !- fraction of radiant energy from heater distributed to surface 4
+      SB25,                    !- surface 5 Name
+      0.1,                     !- fraction of radiant energy from heater distributed to surface 5
+      WR-1,                    !- surface 6 Name
+      0.1;                     !- fraction of radiant energy from heater distributed to surface 6
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-027}
+
+\begin{itemize}
+\item
+  HVAC,Average,Baseboard Total Heating Rate {[}W{]}
+\item
+  HVAC,Average,Baseboard Convective Heating Rate {[}W{]}
+\item
+  HVAC,Average,Baseboard Radiant Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Baseboard Total Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Baseboard Total Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Baseboard Convective Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Baseboard Radiant Heating Energy {[}J{]}
+\item
+  HVAC,Meter,Baseboard:EnergyTransfer {[}J{]}
+\end{itemize}
+
+\paragraph{Baseboard Total Heating Rate {[}W{]}}\label{baseboard-total-heating-rate-w-000}
+
+This is the actual convective heat addition rate of the baseboard to the zone in Watts.~ This value includes the heat convected to the zone air from the baseboard unit, the heat radiated to people in the zone from the baseboard unit, and the additional convection from surfaces within the zone that have been heated by radiation from the baseboard unit.~ This value will be different from (and almost always less than) the next field.
+
+\paragraph{Baseboard Convective Heating Rate {[}W{]}}\label{baseboard-convective-heating-rate-w-000}
+
+This field reports the rate at which convective heat addition is transferred from the baseboard to the zone in Watts.
+
+\paragraph{Baseboard Radiant Heating Rate {[}W{]}}\label{baseboard-radiant-heating-rate-w-000}
+
+This field reports the rate at which radiant heat addition is transferred from the baseboard to the people and the surfaces within the zone in Watts.
+
+\paragraph{Baseboard Total Heating Energy ~{[}J{]}}\label{baseboard-total-heating-energy-j-000}
+
+This is the actual, total convective energy transferred directly and indirectly from the baseboard to the zone it is serving in Joules.~ Direct convective heat transfer includes the convective portion of the baseboard unit.~ Indirect convective heat transfer includes heat radiated to people that is then convected to the zone air and heat that is radiated to the surfaces and then convected to the zone air.
+
+\paragraph{Baseboard Convective Heating Energy {[}J{]}}\label{baseboard-convective-heating-energy-j-000}
+
+This field reports the amount of convective energy transferred from the baseboard directly to the zone air in Joules.
+
+\paragraph{Baseboard Radiant Heating Energy {[}J{]}}\label{baseboard-radiant-heating-energy-j-000}
+
+This field reports the amount of radiant energy transferred from the baseboard to the zone in Joules.
+
+\paragraph{Baseboard Hot Water Mass Flow Rate {[}kg/s{]}}\label{baseboard-hot-water-mass-flow-rate-kgs}
+
+This field reports the water mass flow rate at the inlet node of a baseboard unit.
+
+\paragraph{Baseboard Air Mass Flow Rate {[}kg/s{]}}\label{baseboard-air-mass-flow-rate-kgs}
+
+This field reports the air mass flow rate at the inlet node of a baseboard unit.
+
+\paragraph{Baseboard Water Inlet Temperature {[}C{]}}\label{baseboard-water-inlet-temperature-c}
+
+This field reports the water temperatures at the inlet node of a baseboard unit.
+
+\paragraph{Baseboard Water Outlet Temperature {[}C{]}}\label{baseboard-water-outlet-temperature-c}
+
+This field reports the water temperatures at the outlet node of a baseboard unit.
+
+\paragraph{Baseboard Air Inlet Temperature {[}C{]}}\label{baseboard-air-inlet-temperature-c}
+
+This field reports the air temperatures at the inlet node of a baseboard unit.
+
+\paragraph{Baseboard Air Outlet Temperature {[}C{]}}\label{baseboard-air-outlet-temperature-c}
+
+This field reports the air temperatures at the outlet node of a baseboard unit.
+
+\subsection{ZoneHVAC:Baseboard:RadiantConvective:Steam}\label{zonehvacbaseboardradiantconvectivesteam}
+
+The objective of this model is to calculate the convective and radiant heat transfer from steam baseboard heaters to the people and the surfaces within a zone so that surface heat balances can take into account the radiant heat transfer to the surfaces and thus enhance the accuracy of thermal comfort predictions within the space. The radiant heat gains are distributed to the surfaces by fractions defined by the user. Users are requested to provide degree of sub cooling to estimate the outlet conditions of the condensate.
+
+\subsubsection{Inputs}\label{inputs-1-035}
+
+\paragraph{Field: Name}\label{field-name-1-034}
+
+A unique user assigned name for an instance of a steam baseboard heater unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-010}
+
+The name of the schedule (ref: Schedule) that denotes whether the steam baseboard heater unit can run during a given time period. A schedule value equal to 0 denotes that the unit must be off for that time period. A value greater than 0 denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-1-003}
+
+This field is the name of the steam inlet node for the baseboard heater.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-1-004}
+
+This field is the name of the steam outlet node for the baseboard heater.
+
+\paragraph{Field: Heating Design Capacity Method}\label{field-heating-design-capacity-method-1-000}
+
+Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either \emph{HeatingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedHeatingCapacity}. If this input field is left blank or zero, then autosizing is assumed. \emph{HeatingDesignCapacity} means user specifies the magnitude of maximum heating capacity or the program calculates the maximum design heating capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the radiant baseboard unit. \emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is \emph{HeatingDesignCapacity}.
+
+\paragraph{Field: Heating Design Capacity \{W\}}\label{field-heating-design-capacity-w-1-000}
+
+This field is for the a radiant/convective steam baseboard unit heating capacity in watts. This field can be autosized by EnergyPlus. When the Heating Design Capacity Method is \emph{HeatingDesignCapacity}~ and this input is is blank, autosizing is assumed. Design day sizing run must be specified.
+
+\paragraph{Field: Heating Design Capacity Per Floor Area \{W/m2\}}\label{field-heating-design-capacity-per-floor-area-wm2-1-000}
+
+Enter the heating capacity per unit floor area in m3/s-m2 of radiant/convective steam baseboard. This field is required field when the Heating Design Capacity Method is \emph{CapacityPerFloorArea}. The program calculates the heating capacity from floor area of the zone served by the steam baseboard unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
+
+\paragraph{Field: Fraction of Autosized Heating Design Capacity}\label{field-fraction-of-autosized-heating-design-capacity-1-000}
+
+Enter the heating capacity as a fraction of the autosized heating capacity of a radiant/convective steam baseboard unit. This input field is required when the Heating Design Capacity Method is \emph{FractionOfAutosizedHeatingCapacity}. The program calculates the heating capacity from the design autosized heat capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
+
+\paragraph{Field: Degree of SubCooling}\label{field-degree-of-subcooling-000}
+
+This field is the temperature drop of the condensate in the coil of the baseboard heater. The steam condensates in the coil and changes the phase to the water, giving up the latent heat of steam to the air in the steam to air heat exchanger. The condensate due to the phase change then cools by certain degree in the coil, so that this amount of heat is added to the zone. The minimum value is 1.0° Celsius and default is 5.0° Celsius.
+
+\paragraph{Field: Maximum Steam Flow Rate}\label{field-maximum-steam-flow-rate-000}
+
+This field is the maximum steam volumetric flow rate in m\(^{3}\)/s through the steam baseboard heater.~ The steam volumetric flow rate is calculated at 100C and 101325 Pa. It can be autosized by EnergyPlus.
+
+\paragraph{Field: Convergence Tolerance}\label{field-convergence-tolerance-1-000}
+
+This field is the control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. For steam baseboards, the model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {({Q_{bb,out}} - {Q_{ZoneLoad}})} \right|}}{{{Q_{ZoneLoad}}}} \le Convergence{\kern 1pt} Tolerance
+\end{equation}
+
+The default is 0.001.
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant-1-000}
+
+This field specifies what fraction of the power input to the baseboard heater is actually transferred to the space as radiant heat. The fraction should be between 0 and 1. This is the portion of the total power that is modeled as radiation. The portion that is radiant heat transfer from the baseboard heater is distributed to people and specific surfaces using the remaining fields. Note that the sum of the fractions in the remaining fields (people and surfaces) must equal 1.0 so that all the radiant power is distributed properly.
+
+\paragraph{Field: Fraction of Radiant Energy Incident on People}\label{field-fraction-of-radiant-energy-incident-on-people-1}
+
+This field specifies the fraction of radiant portion of heat transfer to the zone from the baseboard heater that is incident directly on people within the space. This has an impact on the predicted thermal comfort of the zone occupants. Note that although this energy is ``radiant'' it is actually modeled in the zone heat balance as convective energy (like an internal gain). The basic assumption here is that most radiant energy falling on people will most likely be rereleased to the zone air by convection. This is a simplification of reality, but it maintains the overall energy balance.
+
+\paragraph{Field Set: Surface Name, Fraction of Radiant Energy to Surface}\label{field-set-surface-name-fraction-of-radiant-energy-to-surface-1}
+
+The following two items are repeated up to a maximum of 20 surface/fraction pairs. At least one surface/fraction pair must appear in an input file. In other words, at least one surface must be identified as a recipient of radiant energy from the baseboard heater.
+
+\paragraph{Field: Surface \textless{}x\textgreater{} Name}\label{field-surface-x-name-1}
+
+This field is the name of the first surface to which radiant heat transfer from the baseboard heater is distributed. Used in conjunction with the next field, it helps to define the distribution of the radiant energy on the surfaces within the zone. Note that up to 20 pairs of surface names and corresponding fractions may be entered for a single radiant heater system.
+
+\paragraph{Field: Fraction of Radiant Energy to Surface \textless{}x\textgreater{}}\label{field-fraction-of-radiant-energy-to-surface-x-1}
+
+This field is paired with the preceding surface name (previous field) to define the fraction of radiant heat transfer leaving the baseboard heater that is incident on a particular surface. Users should take into account the directionality of baseboard heaters and their location when defining the value for this input field.
+
+\paragraph{Note on Fraction of Radiant Energy Incident on People and to Surfaces}\label{note-on-fraction-of-radiant-energy-incident-on-people-and-to-surfaces}
+
+The radiant energy from the baseboard heater is defined by the total energy input to the baseboard heater from the steam loop times the fraction radiant field shown above. This radiant energy is distributed to surfaces and people using the surface and fraction pairs and the fraction to people input by the user. These fractions to people and surfaces must add up to 1.0. In other words, in an input file, the following relation should be maintained by the user input:
+
+\begin{equation}
+FractionIndicentOnPeople + \sum {FractionToSurfaces = 1}
+\end{equation}
+
+An example IDF for the steam baseboard is shown below.
+
+\begin{lstlisting}
+
+ZoneHVAC:Baseboard:RadiantConvective:Steam,
+  Zone1Baseboard,       !- Baseboard name
+  FanAndCoilAvailSched, !- On/off schedule
+  Steam Inlet Node,     !- Steam inlet node
+  Steam Outlet Node,    !- Steam outlet node
+  HeatingDesignCapacity,!- Heating Design Capacity Method
+  autosize,             !- Heating Design Capacity{ W }
+  ,                     !- Heating Design Capacity Per Floor Area{ W / m2 }
+  ,                     !- Fraction of Autosized Heating Design Capacity{ -}
+  5.0,                  !- Degree of sub cooling in the coil {C}
+  autosize,             !- Maximum steam volumetric flow rate {m3/s}
+  0.001,                !- Tolerance
+  0.3,                  !- Fraction radiant
+  0.3,                  !- Fraction of radiant energy that is incident directly on people
+  OuterWall,            !- Surface 1 Name
+  0.4,                  !- Fraction of radiant energy from heater distributed to surface 1
+  Ceiling,              !- Surface 2 Name
+  0.1,                  !- Fraction of radiant energy from heater distributed to surface 2
+  InnerWall,            !- Surface 3 Name
+  0.1,                  !- Fraction of radiant energy from heater distributed to surface 3
+  Floor,                !- Surface 4 Name
+  0.1;                  !- Fraction of radiant energy from heater distributed to surface 4
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-021}
+
+\begin{itemize}
+\item
+  HVAC,Average,Baseboard Total Heating Rate {[}W{]}
+\item
+  HVAC,Average,Baseboard Convective Heating Rate {[}W{]}
+\item
+  HVAC,Average,Baseboard Radiant Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Baseboard Total Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Baseboard Convective Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Baseboard Radiant Heating Energy {[}J{]}
+\item
+  HVAC,Meter,Baseboard:EnergyTransfer {[}J{]}
+\item
+  HVAC,Average,Baseboard Steam Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Baseboard Steam Inlet temperature {[}C{]}
+\item
+  HVAC,Average,Baseboard Steam Outlet temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Baseboard Total Heating Rate {[}W{]}}\label{baseboard-total-heating-rate-w-1}
+
+This is the actual convective heat addition rate of the baseboard to the zone in Watts.~ This value includes the heat convected to the zone air from the baseboard unit, the heat radiated to people in the zone from the baseboard unit, and the additional convection from surfaces within the zone that have been heated by radiation from the baseboard unit. This value will be different from (and almost always less than) the next field.
+
+\paragraph{Baseboard Convective Heating Rate {[}W{]}}\label{baseboard-convective-heating-rate-w-1}
+
+This field reports the rate at which convective heat addition is transferred from the baseboard to the zone in Watts.
+
+\paragraph{Baseboard Radiant Heating Rate {[}W{]}}\label{baseboard-radiant-heating-rate-w-1}
+
+This field reports the rate at which radiant heat addition is transferred from the baseboard to the people and the surfaces within the zone in Watts.
+
+\paragraph{Baseboard Total Heating Energy {[}J{]}}\label{baseboard-total-heating-energy-j-1}
+
+This is the actual, total convective energy transferred directly and indirectly from the baseboard to the zone it is serving in Joules. Direct convective heat transfer includes the convective portion of the baseboard unit. Indirect convective heat transfer includes heat radiated to people that is then convected to the zone air and heat that is radiated to the surfaces and then convected to the zone air.
+
+\paragraph{Baseboard Convective Heating Energy {[}J{]}}\label{baseboard-convective-heating-energy-j-1}
+
+This field reports the amount of convective energy transferred from the baseboard directly to the zone air in Joules.
+
+\paragraph{Baseboard Radiant Heating Energy {[}J{]}}\label{baseboard-radiant-heating-energy-j-1}
+
+This field reports the amount of radiant energy transferred from the baseboard to the zone in Joules.
+
+\paragraph{Baseboard Steam Energy {[}J{]}}\label{baseboard-steam-energy-j}
+
+\paragraph{Baseboard Steam Rate {[}W{]}}\label{baseboard-steam-rate-w}
+
+These are the total heat addition energy and rate of steam used by the baseboard to heat the zone it is serving in Joules and Watts.
+
+\paragraph{Baseboard Steam Mass Flow Rate {[}kg/s{]}}\label{baseboard-steam-mass-flow-rate-kgs}
+
+This field reports the steam mass flow rate at the inlet node of a baseboard unit.
+
+\paragraph{Baseboard Steam Inlet Temperature {[}C{]}}\label{baseboard-steam-inlet-temperature-c}
+
+This field reports the steam temperatures at the inlet node of a baseboard unit.
+
+\paragraph{Baseboard Steam Outlet Temperature {[}C{]}}\label{baseboard-steam-outlet-temperature-c}
+
+This field reports the steam temperatures at the outlet node of a baseboard unit.
+
+\subsection{ZoneHVAC:Baseboard:RadiantConvective:Electric}\label{zonehvacbaseboardradiantconvectiveelectric}
+
+The electric baseboard heater is a component in the zone equipment simulation. Heat from this device is radiated to people and surfaces and also convected to the surrounding air. The electric baseboard model includes the impact of the radiant heat addition to people and surfaces so that the thermal comfort and surface heat balances are impacted. The component is controlled to meet any remaining zone load not met by other equipment baseboard operates to meet the remaining zone load and the total electric consumption is calculated by dividing by the efficiency of the baseboard.
+
+\subsubsection{Inputs}\label{inputs-2-032}
+
+\paragraph{Field: Name}\label{field-name-2-031}
+
+A unique user assigned name for an instance of an electric baseboard heater unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-2-006}
+
+The name of the schedule (ref: Schedule) that denotes whether the electric baseboard heater unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit will be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Heating Design Capacity Method}\label{field-heating-design-capacity-method-2}
+
+Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either \emph{HeatingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedHeatingCapacity}. If this input field is left blank or zero, then autosizing is assumed. \emph{HeatingDesignCapacity} means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the maximum or nominal design heating capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the radiant baseboard unit. \emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is \emph{HeatingDesignCapacity}.
+
+\paragraph{Field: Heating Design Capacity \{W\}}\label{field-heating-design-capacity-w-2}
+
+This field is for the radiant-convective electric baseboard unit nominal heating capacity in watts. This field can be autosized by EnergyPlus. This input field is autosizable. When the Heating Design Capacity Method is \emph{HeatingDesignCapacity}~ and this input is is blank, autosizing is assumed. Design day sizing run must be specified.
+
+\paragraph{Field: Heating Design Capacity Per Floor Area \{W/m2\}}\label{field-heating-design-capacity-per-floor-area-wm2-2}
+
+Enter the heating capacity per unit floor area in m3/s-m2 of radiant/convective electric baseboard. This field is required field when the Heating Design Capacity Method is \emph{CapacityPerFloorArea}. The program calculates the heating capacity from floor area of the zone served by the radiant baseboard unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
+
+\paragraph{Field: Fraction of Autosized Heating Design Capacity}\label{field-fraction-of-autosized-heating-design-capacity-2}
+
+Enter the heating capacity as a fraction of the autosized heating capacity for radiant/convective electric baseboard. This input field is required when the Heating Design Capacity Method is \emph{FractionOfAutosizedHeatingCapacity}. The program calculates the heating capacity from the design autosized heat capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
+
+\paragraph{Field: Efficiency}\label{field-efficiency-001}
+
+This is the overall electrical efficiency of the electric baseboard unit. The zone load met by this unit is divided by the electrical efficiency to obtain the total electric energy used.
+
+\paragraph{Field: Fraction Radiant}\label{field-fraction-radiant-2-000}
+
+This field specifies what fraction of the power input to the baseboard heater is actually transferred to the space as radiant heat. The fraction should be between 0 and 1. This is the portion of the total power that is modeled as radiation. The portion that is radiant heat transfer from the baseboard heater is distributed to people and specific surfaces using the remaining fields. Note that the sum of the fractions in the remaining fields (people and surfaces) must equal 1.0 so that all the radiant power is distributed properly.
+
+\paragraph{Field: Fraction of Radiant Energy Incident on People}\label{field-fraction-of-radiant-energy-incident-on-people-2}
+
+This field specifies the fraction of the radiant portion of heat transfer to the zone from the baseboard heater that is incident directly on people within the space. This has an impact on the predicted thermal comfort of the zone occupants. Note that although this energy is ``radiant'' it is actually modeled in the zone heat balance as a convective energy (like an internal gain). The basic assumption here is that radiant energy falling on people will most likely be rereleased to the zone air by convection. This is a simplification of reality, but it maintains the overall energy balance.
+
+\paragraph{Field Set: Surface Name, Fraction of Radiant Energy to Surface}\label{field-set-surface-name-fraction-of-radiant-energy-to-surface-2}
+
+The following two items are repeated up to a maximum of 20 surface/fraction pairs. At least one surface/fraction pair must appear in an input file. In other words, at least one surface must be identified as a recipient of radiant energy from the baseboard heater.
+
+\paragraph{Field Set: Surface \textless{}x\textgreater{} Name}\label{field-set-surface-x-name}
+
+This field is the name of the first surface to which radiant heat transfer from the baseboard heater is distributed. Used in conjunction with the next field, it helps to define the distribution of the radiant energy on the surfaces within the zone. Note that up to 20 pairs of surface names and corresponding fractions may be entered for a single radiant heater system.
+
+\paragraph{Field Set: Fraction of Radiant Energy to Surface \textless{}x\textgreater{}}\label{field-set-fraction-of-radiant-energy-to-surface-x}
+
+This field is paired with the preceding surface name (previous field) to define the fraction of radiant heat transfer leaving the baseboard heater that is incident on a particular surface. Users should take into account the directionality of baseboard heaters and their location when defining the value for this input field.
+
+\paragraph{Note on Fraction of Radiant Energy Incident on People and to Surfaces}\label{note-on-fraction-of-radiant-energy-incident-on-people-and-to-surfaces-1}
+
+The radiant energy from the baseboard heater is defined by the total energy input to the baseboard heater times the fraction radiant field shown above. This radiant energy is distributed to surfaces and people using the surface and fraction pairs and the fraction to people input by the user. These fractions to people and surfaces must add up to 1.0. In other words, in an input file, the following relation should be maintained by the user input:
+
+\begin{equation}
+FractionIndicentOnPeople + \sum {FractionToSurfaces = 1}
+\end{equation}
+
+Below is an example input for an Electric Baseboard Heater.
+
+\begin{lstlisting}
+
+ZoneHVAC:Baseboard:RadiantConvective:Electric,
+  Baseboard 1,   !- Name
+  BB Schedule,   !- Availability Schedule Name
+  HeatingDesignCapacity,   !- Heating Design Capacity Method
+  5000,          !- Heating Design Capacity{ W }
+  ,              !- Heating Design Capacity Per Floor Area{ W / m2 }
+  ,              !- Fraction of Autosized Heating Design Capacity{ -}
+  0.97,          !- Efficiency of the baseboard
+  0.3,           !- Fraction radiant
+  0.3,           !- Fraction of radiant energy that is incident directly on people
+  EastWall,      !- Surface 1 name
+  0.3,           !- Fraction of radiant energy from heater distributed to surface 1
+  WestWall,      !- Surface 2 name
+  0.1,           !- Fraction of radiant energy from heater distributed to surface 2
+  NorthWall,     !- Surface 3 name
+  0.1,           !- Fraction of radiant energy from heater distributed to surface 3
+  SouthWall,     !- Surface 4 name
+  0.1,           !- Fraction of radiant energy from heater distributed to surface 4
+  Ceiling,       !- Surface 5 name
+  0.1;           !- Fraction of radiant energy from heater distributed to surface 5
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-017}
+
+\begin{itemize}
+\item
+  HVAC,Average,Baseboard Total Heating Rate {[}W{]}
+\item
+  HVAC,Average,Baseboard Radiant Heating Rate {[}W{]}
+\item
+  HVAC,Average,Baseboard Convective Heating Rate {[}W{]}
+\item
+  HVAC,Average,Baseboard Electric Power{[}W{]}
+\item
+  HVAC,Sum,Baseboard Total Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Baseboard Radiant Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Baseboard Convective Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Baseboard Electric Energy {[}J{]}
+\item
+  HVAC,Meter,Baseboard:EnergyTransfer {[}J{]}
+\item
+  HVAC,Meter,Heating:Electricity{[}J{]}
+\end{itemize}
+
+\paragraph{Baseboard Total Heating Rate {[}W{]}}\label{baseboard-total-heating-rate-w-2}
+
+This is the actual convective heat addition rate of the baseboard to the zone in Watts. This value includes the heat convected to the zone air from the baseboard unit, the heat radiated to people in the zone from the baseboard unit, and the additional convection from surfaces within the zone that have been heated by radiation from the baseboard unit. This value will be different from (and almost always less than) the next field.
+
+\paragraph{Baseboard Radiant Heating Rate {[}W{]}}\label{baseboard-radiant-heating-rate-w-2}
+
+This field reports the rate at which radiant heat addition is transferred from the baseboard to the people and the surfaces within the zone in Watts.
+
+\paragraph{Baseboard Convective Heating Rate {[}W{]}}\label{baseboard-convective-heating-rate-w-2}
+
+This field reports the rate at which convective heat addition is transferred from the baseboard to the zone in Watts.
+
+\paragraph{Baseboard Electric Energy {[}J{]}}\label{baseboard-electric-energy-j-000}
+
+This is the electric energy used by the baseboard in Joules.
+
+\paragraph{Baseboard Electric Power {[}J{]}}\label{baseboard-electric-power-j}
+
+This is the electric power required by the baseboard to heat the zone it is serving in Watts
+
+\paragraph{Baseboard Total Heating Energy {[}J{]}}\label{baseboard-total-heating-energy-j-2}
+
+This is the actual convective energy transferred directly and indirectly from the baseboard heater to the zone it is serving in Joules. Direct convective heat transfer includes the convective portion of the baseboard unit. Indirect convective heat transfer includes heat radiated to people that is then convected to the zone air and heat that is radiated to the surfaces and then convected to the zone air.
+
+\paragraph{Baseboard Radiant Heating Energy {[}J{]}}\label{baseboard-radiant-heating-energy-j-2}
+
+This field reports the amount of radiant energy transferred from the baseboard to the zone in Joules.
+
+\paragraph{Baseboard Convective Heating Energy {[}J{]}}\label{baseboard-convective-heating-energy-j-2}
+
+This field reports the amount of convective energy transferred from the baseboard directly to the zone air in Joules.
+
+\subsection{ZoneHVAC:Baseboard:Convective:Water}\label{zonehvacbaseboardconvectivewater}
+
+The hot water baseboard heater is a component of zone equipment. The component is controlled to meet any remaining zone load not met by other equipment in the zone that have higher heating priority. The control is accomplished by throttling the hot water flow. Input resembles that for the simple heating coil: there is an availability schedule, an overall UA, and a maximum hot water mass flow rate. The unit is connected to a hot water loop (demand side) with an inlet and outlet node. Finally, there is the convergence tolerance, which is the tolerance on how closely the baseboard outlet will meet the zone load. Of course, this tolerance is relative to the zone load.
+
+\subsubsection{Inputs}\label{inputs-3-028}
+
+\paragraph{Field: Name}\label{field-name-3-025}
+
+A unique user assigned name for an instance of a hot water baseboard heater unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-3-005}
+
+The name of the schedule (ref: Schedule) that denotes whether the hot water baseboard heater unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-2-002}
+
+The name of the hot water inlet node for the baseboard heater.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-2-002}
+
+The name of the hot water outlet node for the baseboard heater.
+
+\paragraph{Field: Heating Design Capacity Method}\label{field-heating-design-capacity-method-3}
+
+Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either \emph{HeatingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedHeatingCapacity}. If this input field is left blank or zero, then autosizing is assumed. \emph{HeatingDesignCapacity} means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the maximum or nominal design heating capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the hot water baseboard heater. \emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is \emph{HeatingDesignCapacity}.
+
+\paragraph{Field: Heating Design Capacity \{W\}}\label{field-heating-design-capacity-w-3}
+
+This field is for the hot water baseboard heater design heating capacity in watts. This field can be autosized by EnergyPlus. This input field is autosizable. When the Heating Design Capacity Method is \emph{HeatingDesignCapacity}~ and this input is is blank, autosizing is assumed. Design day sizing run must be specified id autosize is specified.
+
+\paragraph{Field: Heating Design Capacity Per Floor Area \{W/m2\}}\label{field-heating-design-capacity-per-floor-area-wm2-3}
+
+Enter the heating capacity per unit floor area in m3/s-m2 of hot water baseboard heater. This field is required field when the Heating Design Capacity Method is \emph{CapacityPerFloorArea}. The program calculates the heating capacity from floor area of the zone served by hot water baseboard heater and the heating capacity per unit floor area value specified by the user. This field may be left blank.
+
+\paragraph{Field: Fraction of Autosized Heating Design Capacity}\label{field-fraction-of-autosized-heating-design-capacity-3}
+
+Enter the heating capacity as a fraction of the autosized heating capacity for the hot water baseboard heater. This input field is required when the Heating Design Capacity Method is \emph{FractionOfAutosizedHeatingCapacity}. The program calculates the heating capacity from the design autosized heat capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
+
+\paragraph{Field: U-Factor Times Area Value}\label{field-u-factor-times-area-value-000}
+
+The overall heat transfer coefficient for the baseboard heater in watts per degree Celsius at design conditions. The U-Factor Times Area Value (UA) is used in an NTU - effectiveness calculation. An estimate of the UA can be obtained from:
+
+\begin{equation}
+q = UA \times ({T_{water,avg}} - {T_{air,avg}})
+\end{equation}
+
+where q is the heat transferred from water to the air in watts; T\(_{water,\\ avg}\) is the average water temperature in degrees C; and T\(_{air,\\ avg}\) is the average air temperature in degrees C. Or the LMTD temperature difference can be used.
+
+\paragraph{Field: Maximum Water Flow Rate}\label{field-maximum-water-flow-rate-1-000}
+
+The maximum hot water volumetric flow rate in m\(^{3}\)/sec.
+
+\paragraph{Field Convergence Tolerance}\label{field-convergence-tolerance-2-000}
+
+The control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. For hot water baseboards, the model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {({Q_{bb,out}} - {Q_{ZoneLoad}})} \right|}}{{{Q_{ZoneLoad}}}} \le Convergence{\kern 1pt} Tolerance
+\end{equation}
+
+The default is 0.001.
+
+An example IDF for the hot water convective baseboard is shown below.
+
+\begin{lstlisting}
+
+ZoneHVAC:Baseboard:Convective:Water,
+          Zone3Baseboard, ! name
+          FanAndCoilAvailSched, ! on/off schedule
+          Zone 3 Reheat Water Inlet Node, ! water inlet node
+          Zone 3 Reheat Water Outlet Node, ! water outlet node
+          HeatingDesignCapacity, !- Heating Design Capacity Method
+          autosize,!- Heating Design Capacity{ W }
+          ,        !- Heating Design Capacity Per Floor Area{ W / m2 }
+          ,        !- Fraction of Autosized Heating Design Capacity{ -}
+          500.,    ! UA
+          0.0013,  ! maximum water flow rate m3/s
+          0.001;   ! tolerance
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-015}
+
+\begin{itemize}
+\item
+  HVAC,Average,Baseboard Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Baseboard Total Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Baseboard Hot Water Energy {[}J{]}
+\item
+  HVAC,Average,Baseboard Hot Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Baseboard Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Baseboard Air Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Baseboard Air Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Baseboard Water Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Baseboard Water Outlet Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Baseboard Total Heating Rate {[}W{]}}\label{baseboard-total-heating-rate-w-3}
+
+This is the heat addition rate of the convective baseboard to the zone it is serving in Watts.
+
+\paragraph{Baseboard Total Heating Energy {[}J{]}}\label{baseboard-total-heating-energy-j-3}
+
+This is the heat addition of the convective baseboard to the zone it is serving in Joules over the timestep being reported.
+
+\paragraph{Baseboard Hot Water Energy {[}J{]}}\label{baseboard-hot-water-energy-j}
+
+This is the energy in the hot water used by the baseboard to heat the zone, in Joules.
+
+\paragraph{Baseboard Hot Water Mass Flow Rate {[}kg/s{]}}\label{baseboard-hot-water-mass-flow-rate-kgs-1}
+
+This field reports the water mass flow rate at the inlet node of a baseboard unit.
+
+\paragraph{Baseboard Air Mass Flow Rate {[}kg/s{]}}\label{baseboard-air-mass-flow-rate-kgs-1}
+
+This field reports the air mass flow rate at the inlet node of a baseboard unit.
+
+\paragraph{Baseboard Water Inlet Temperature {[}C{]}}\label{baseboard-water-inlet-temperature-c-1}
+
+This field reports the water temperatures at the inlet node of a baseboard unit.
+
+\paragraph{Baseboard Water Outlet Temperature {[}C{]}}\label{baseboard-water-outlet-temperature-c-1}
+
+This field reports the water temperatures at the outlet node of a baseboard unit.
+
+\paragraph{Baseboard Air Inlet Temperature {[}C{]}}\label{baseboard-air-inlet-temperature-c-1}
+
+This field reports the air temperatures at the inlet node of a baseboard unit.
+
+\paragraph{Baseboard Air Outlet Temperature {[}C{]}}\label{baseboard-air-outlet-temperature-c-1}
+
+This field reports the air temperatures at the outlet node of a baseboard unit.
+
+\subsection{ZoneHVAC:Baseboard:Convective:Electric}\label{zonehvacbaseboardconvectiveelectric}
+
+The electric baseboard heater is a component in the zone equipment simulation. The component is controlled to meet any remaining zone load not met by other equipment in the zone that have higher heating priority. The control is accomplished by taking the remaining zone load and dividing by the efficiency of the baseboard.
+
+\subsubsection{Inputs}\label{inputs-4-025}
+
+\paragraph{Field: Name}\label{field-name-4-022}
+
+A unique user assigned name for an instance of a electric baseboard heater unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-4-005}
+
+The name of the schedule (ref: Schedule) that denotes whether the electric baseboard heater unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Heating Design Capacity Method}\label{field-heating-design-capacity-method-4}
+
+Enter the method used to determine the heating design capacity or enter the method for scalable sizing of heating capacity of electric baseboard unit. Input allowed is either \emph{HeatingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedHeatingCapacity}. If this input field is left blank or zero, then autosizing is assumed. \emph{HeatingDesignCapacity} means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the maximum or nominal design heating capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the electric convective baseboard unit. \emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is \emph{HeatingDesignCapacity}.
+
+\paragraph{Field: Heating Design Capacity \{W\}}\label{field-heating-design-capacity-w-4}
+
+This field is for the convective electric baseboard nominal heating capacity in watts. This field can be autosized by EnergyPlus. This input field is autosizable. Design day sizing run must be specified. This input field may be left blank.
+
+\paragraph{Field: Heating Design Capacity Per Floor Area \{W/m2\}}\label{field-heating-design-capacity-per-floor-area-wm2-4}
+
+Enter the heating capacity per unit floor area in m3/s-m2 of electric convective baseboard unit. This field is required field when the Heating Design Capacity Method is \emph{CapacityPerFloorArea}. The program calculates the heating capacity from floor area of the zone served by the electric convective baseboard unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
+
+\paragraph{Field: Fraction of Autosized Heating Design Capacity}\label{field-fraction-of-autosized-heating-design-capacity-4}
+
+Enter the heating capacity as a fraction of the autosized heating capacity for convective electric baseboard unit. This input field is required when the Heating Design Capacity Method is \emph{FractionOfAutosizedHeatingCapacity}. The program calculates the heating capacity from the design autosized heating capacity and user specified fraction. Design day sizing must be specified. This field may be left blank.~ Default value is 1.0.
+
+\paragraph{Field: Efficiency}\label{field-efficiency-1}
+
+This is the overall electrical efficiency of the electric baseboard. The zone load met by this unit is divided by the electrical efficiency to obtain the total electric energy used.
+
+An example IDF for the electric convective baseboard is shown below.
+
+\begin{lstlisting}
+
+ZoneHVAC:Baseboard:Convective:Electric,
+      Zone1Baseboard,  !- Baseboard Name
+      FanAndCoilAvailSched,  !- Availability Schedule Name
+      HeatingDesignCapacity,   !- Heating Design Capacity Method
+      5000,                    !- Heating Design Capacity{ W }
+      ,                        !- Heating Design Capacity Per Floor Area{ W / m2 }
+      ,                        !- Fraction of Autosized Heating Design Capacity{ -}
+      0.97;  !- Efficiency of the BaseBoard
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-012}
+
+\begin{itemize}
+\item
+  HVAC,Average,Baseboard Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Baseboard Total Heating Energy {[}J{]}
+\item
+  HVAC,Meter,Baseboard:EnergyTransfer {[}J{]}
+\item
+  HVAC,Sum,Baseboard Electric Energy {[}J{]}
+\item
+  HVAC,Average,Baseboard Electric Power{[}W{]}
+\item
+  HVAC,Meter,Heating:Electricity{[}J{]}
+\end{itemize}
+
+\paragraph{Baseboard Total Heating Rate {[}W{]}}\label{baseboard-total-heating-rate-w-4}
+
+This is the heat addition rate of the electric convective baseboard to the zone it is serving in Watts.
+
+\paragraph{Baseboard Total Heating Energy {[}J{]}}\label{baseboard-total-heating-energy-j-4}
+
+This is the heat addition of the convective baseboard to the zone it is serving in Joules over the timestep being reported.
+
+\paragraph{Baseboard Electric Energy {[}J{]}}\label{baseboard-electric-energy-j-1}
+
+This is the total electric consumption of the baseboard for the zone it is serving in Joules over the timestep being reported.
+
+\paragraph{Baseboard Electric Power {[}W{]}}\label{baseboard-electric-power-w-000}
+
+This is the electric power required by the baseboard to the zone it is serving in Watts.
+
+\subsection{ZoneHVAC:LowTemperatureRadiant:VariableFlow}\label{zonehvaclowtemperatureradiantvariableflow}
+
+This low temperature radiant system (hydronic) is a component of zone equipment that is intended to model any ``radiant system'' where water is used to supply/remove energy to/from a building surface (wall, ceiling, or floor). The component is controlled to meet any remaining zone load not met by other equipment in the zone that have higher priority. The control is accomplished by throttling the hot or chilled water flow to the unit. Note that this system will only control based on the radiant system controls defined by this input syntax and not via a zone thermostat such as is used for forced air systems. Note also that because this unit does not require a thermostat that in cases where no other systems are serving the zone in which this system resides that it will use the heating equipment priority to determine which system will run first.~ If the radiant system is serving a zone with forced air equipment, the radiant system will follow the priority order established by the zone thermostat but will still base its response on the controls defined by the user for the radiant system.
+
+This model covers a wide range of low temperature radiant systems: heating and/or cooling, panel or embedded pipes, etc. It is not intended to simulate high temperature electric or gas radiant heaters. Those devices will be handled by a separate model and different input syntax. Low temperature radiant systems that use electric resistance heating should also be defined using separate input syntax (ref: ZoneHVAC:LowTemperatureRadiant:Electric).
+
+\subsubsection{Inputs}\label{inputs-5-022}
+
+\paragraph{Field: Name}\label{field-name-5-018}
+
+This field is an unique user assigned name for an instance of a hydronic low temperature radiant system. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-5-003}
+
+This field is the name of the schedule (ref: Schedule) that denotes whether the hydronic low temperature radiant system can run during a given time period. A schedule value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for that time period. A value greater than 0 (usually 1 is used) denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-009}
+
+This field is the name of the zone (Ref: Zone) in which the hydronic low temperature radiant system is principally located and intended to affect. A system that is between two zones will still act upon each zone; however, the zone name referenced here should be the zone that controls the radiant system response.
+
+\paragraph{Field: Surface Name or Radiant Surface Group Name}\label{field-surface-name-or-radiant-surface-group-name}
+
+This field is the name of the surface (Ref: BuildingSurface) or surface list (Ref: ZoneHVAC:LowTemperatureRadiant:SurfaceGroup) in which the hydronic tubing is embedded/contained. This specification attaches the source or sink from the radiant system to a particular surface and the contribution of the system to the heat balances of that surface. If this field is a surface list, then the source or sink is attached to all of the surfaces in the list with the radiant system surface group defining the breakdown of how flow rate is split between the various surfaces. Base surfaces (e.g., BuildingSurface:Detailed), door surfaces and internal mass are valid. Window surfaces are not valid surface types for embedded radiant systems.
+
+\paragraph{Field: Hydronic Tubing Inside Diameter}\label{field-hydronic-tubing-inside-diameter-000}
+
+This field is the inside diameter of the tubes through which water is circulated for the system being defined by this statement. The inside diameter should be recorded in meters and is used to determine the convective heat transfer from the water to the inside surface of the hydronic tubing.
+
+\paragraph{Field: Hydronic Tubing Length}\label{field-hydronic-tubing-length}
+
+This field is the total length of pipe embedded in the surface named above in the surface name field. The length of the tube should be entered in meters and is used to determine the effectiveness of heat transfer from the fluid being circulated through the tubes and the tube/surface. Longer tubing lengths result in more heat will be transferred to/from the radiant surface to the circulating fluid. Note that if the user elects to autosize this field that a standard zone thermostat such as would be used for a forced air system must be defined as autosizing calculations are based on the zone thermostat value and not on the radiant system control values.
+
+\paragraph{Field: Temperature Control Type}\label{field-temperature-control-type}
+
+This field specifies along with the throttling range and setpoint schedules how the user wishes to control the hydronic radiant system. The temperature denoted in the setpoint schedule can refer to one of five different temperatures: the zone mean air temperature, the zone mean radiant temperature, the zone operative temperature, the outdoor dry-bulb temperature, or the outdoor wet-bulb temperature. The choice of temperature is controlled by the current field---temperature control type. The user must select from the following options:
+
+\begin{itemize}
+\item
+  MeanAirTemperature
+\item
+  MeanRadiantTemperature
+\item
+  OperativeTemperature
+\item
+  OutdoorDryBulbTemperature
+\item
+  OutdoorWetBulbTemperature
+\end{itemize}
+
+Operative temperature for radiant system controls is the average of Mean Air Temperature and Mean Radiant Temperature. If the user does not select a control type, \textbf{MeanAirTemperature} control is assumed by EnergyPlus. See the throttling range and control temperature schedule fields below for more information.
+
+\paragraph{Field: Heating Design Capacity Method}\label{field-heating-design-capacity-method-5}
+
+Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either \emph{HeatingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedHeatingCapacity}. If this input field is left blank or zero, then autosizing is assumed. \emph{HeatingDesignCapacity} means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the design heating capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the low temperature radiant variable flow unit. \emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is \emph{HeatingDesignCapacity}.
+
+\paragraph{Field: Heating Design Capacity \{W\}}\label{field-heating-design-capacity-w-5}
+
+This field is for the low temperature radiant variable flow unit design heating capacity in watts. This field can be autosized by EnergyPlus. This input field is autosizable. When the Heating Design Capacity Method is \emph{HeatingDesignCapacity}~ and this input is is blank, autosizing is assumed. Design day sizing run must be specified if autosized.
+
+\paragraph{Field: Heating Design Capacity Per Floor Area \{W/m2\}}\label{field-heating-design-capacity-per-floor-area-wm2-5}
+
+Enter the heating capacity per unit floor area in m3/s-m2 of low temperature radiant variable flow unit. This field is required field when the Heating Design Capacity Method is \emph{CapacityPerFloorArea}. The program calculates the heating capacity from floor area of the zone served by the low temperature radiant variable flow unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
+
+\paragraph{Field: Fraction of Autosized Heating Design Capacity}\label{field-fraction-of-autosized-heating-design-capacity-5}
+
+Enter the heating capacity as a fraction of the autosized heating capacity for low temperature radiant variable flow unit. This input field is required when the Heating Design Capacity Method is \emph{FractionOfAutosizedHeatingCapacity}. The program calculates the heating capacity from the design autosized heat capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
+
+\paragraph{Field: Maximum Hot Water Flow}\label{field-maximum-hot-water-flow}
+
+This field is the maximum flow rate of hot water through the radiant system in m\(^{3}\)/sec.~The controls for the radiant system will vary the flow rate of hot water through the surface using zero flow and the maximum flow rate specified in this field as the lower and upper bounds, respectively. Note that if the user elects to autosize this field that a standard zone thermostat such as would be used for a forced air system must be defined as autosizing calculations are based on the zone thermostat value and not on the radiant system control values.
+
+\paragraph{Field: Heating Water Inlet Node Name}\label{field-heating-water-inlet-node-name}
+
+This field contains the name of the hot water inlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a heating coil.
+
+\paragraph{Field: Heating Water Outlet Node Name}\label{field-heating-water-outlet-node-name}
+
+This field contains the name of the hot water oulet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a heating coil.
+
+\paragraph{Field: Heating Control Throttling Range}\label{field-heating-control-throttling-range}
+
+This field specifies the range of temperature in degrees Celsuis over which the radiant system throttles from zero flow rate up to the maximum defined by the maximum hot water flow rate field described above. The throttling range parameter is used in conjunction with the control temperature to define the response of the system to various zone conditions. The heating control temperature schedule specifies the ``setpoint'' temperature where the flow rate to the system is at half of the maximum flow rate. For example, if the heating control temperature setpoint is currently 15°C and the heating throttling range is 2°C, the water flow rate to the radiant system will be zero when the controlling temperature (MAT, MRT, Operative Temperature, ODB, or OWB; see control type field above) is at or above 16°C and the maximum flow rate when the controlling temperature is at or below 14°C. This represents a throttling range of 2°C around the setpoint of 15°C. In between 14°C and 16°C, the flow rate to the radiant system is varied linearly.
+
+\paragraph{Field: Heating Control Temperature Schedule Name}\label{field-heating-control-temperature-schedule-name}
+
+This field specifies the heating setpoint or control temperature for the radiant system in degrees Celsius. Used in conjunction with the previous field (heating control throttling range), it will define whether or not the system is running and the current flow rate. Water flow rate to the system is varied linearly around the setpoint temperature based on the throttling range and the maximum heating flow rate parameters (see above). It should be noted that this control schedule will allow different setpoint temperatures throughout the year for heating. The control of the radiant system is based solely on the heating control temperature schedule, the cooling control temperature schedule (see below), and the control temperature type listed above. The radiant system will not use any zone thermostat that might be used by other systems serving the zone in which the radiant system resides.
+
+\paragraph{Field: Cooling Design Capacity Method}\label{field-cooling-design-capacity-method-000}
+
+Enter the method used to determine the cooling design capacity for scalable sizing. Input allowed is either \emph{CoolingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedCoolingCapacity}. If this input field is left blank or zero, then autosizing is assumed. \emph{CoolingDesignCapacity} means user specifies the design cooling capacity or the program calculates the design cooling capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design cooling capacity from user specified heating capacity per floor area and floor area of the zone served by the low temperature radiant variable flow unit. \emph{FractionOfAutosizedCoolingCapacity} means the program calculates the design cooling capacity from user specified fraction and the auto-sized design cooling capacity. The default method is \emph{CoolingDesignCapacity}.
+
+\paragraph{Field: Cooling Design Capacity \{W\}}\label{field-cooling-design-capacity-w-000}
+
+This field is for the low temperature radiant variable flow unit design cooling capacity in watts. This field can be autosized by EnergyPlus. This input field is autosizable. When the Cooling Design Capacity Method is \emph{CoolingDesignCapacity} and this input is is blank, autosizing is assumed. Design day sizing run must be specified if autosized.
+
+\paragraph{Field: Cooling Design Capacity Per Floor Area \{W/m2\}}\label{field-cooling-design-capacity-per-floor-area-wm2-000}
+
+Enter the cooling capacity per unit floor area in m3/s-m2 of low temperature radiant variable flow unit. This field is required field when the Cooling Design Capacity Method is \emph{CapacityPerFloorArea}. The program calculates the cooling capacity from floor area of the zone served by the low temperature radiant variable flow unit and the cooling capacity per unit floor area value specified by the user. This field may be left blank.
+
+\paragraph{Field: Fraction of Autosized Cooling Design Capacity}\label{field-fraction-of-autosized-cooling-design-capacity-000}
+
+Enter the cooling capacity as a fraction of the autosized cooling capacity for low temperature radiant variable flow unit. This input field is required when the Cooling Design Capacity Method is \emph{FractionOfAutosizedCoolingCapacity}. The program calculates the cooling capacity from the design autosized cooling capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
+
+\paragraph{Field: Maximum Cold Water Flow}\label{field-maximum-cold-water-flow}
+
+This field is the maximum flow rate of cold water through the radiant system in m\(^{3}\)/sec.~The controls for the radiant system will vary the flow rate of cold water through the surface using zero flow and the maximum flow rate specified in this field as the lower and upper bounds, respectively. Note that this field is optional and not required for a heating only system. Note also that if the user elects to autosize this field that a standard zone thermostat such as would be used for a forced air system must be defined as autosizing calculations are based on the zone thermostat value and not on the radiant system control values.
+
+\paragraph{Field: Cooling Water Inlet Node Name}\label{field-cooling-water-inlet-node-name-000}
+
+This field contains the name of the cold water inlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a cooling coil. As with the maximum cold water flow rate, this field is optional and not required for a heating only system.
+
+\paragraph{Field: Cooling Water Outlet Node Name}\label{field-cooling-water-outlet-node-name-000}
+
+This field contains the name of the cold water oulet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a cooling coil. As with the maximum cold water flow rate, this field is optional and not required for a heating only system.
+
+\paragraph{Field: Cooling Control Throttling Range}\label{field-cooling-control-throttling-range}
+
+This field specifies the range of temperature in degrees Celsuis over which the radiant system throttles from zero flow rate up to the maximum defined by the maximum cold water flow rate field described above. The throttling range parameter is used in conjunction with the control temperature to define the response of the system to various zone conditions. The cooling control temperature schedule specifies the ``setpoint'' temperature where the flow rate to the system is at half of the maximum flow rate. For example, if the cooling control temperature setpoint is currently 25°C and the cooling throttling range is 2°C, the water flow rate to the radiant system will be zero when the controlling temperature (MAT, MRT, Operative Temperature, ODB, or OWB; see control type field above) is at or below 24°C and the maximum flow rate when the controlling temperature is at or above 26°C. This represents a throttling range of 2°C around the setpoint of 25°C. In between 24°C and 26°C, the flow rate to the radiant system is varied linearly.
+
+\paragraph{Field: Cooling Control Temperature Schedule Name}\label{field-cooling-control-temperature-schedule-name}
+
+This field specifies the cooling setpoint or control temperature for the radiant system in degrees Celsius. Used in conjunction with the previous field (cooling control throttling range), it will define whether or not the system is running and the current flow rate. Water flow rate to the system is varied linearly around the setpoint temperature based on the throttling range and the maximum cooling flow rate parameters (see above). It should be noted that this control schedule will allow different setpoint temperatures throughout the year for cooling. The control of the radiant system is based solely on the heating control temperature schedule listed above, the cooling control temperature schedule, and the control temperature type listed above. The radiant system will not use any zone thermostat that might be used by other systems serving the zone in which the radiant system resides.
+
+\paragraph{Field: Condensation Control Type}\label{field-condensation-control-type}
+
+When radiant systems do cooling, there is the possibility that condensation will occur on the surface that is being cooled.~ This is due to the fact that the surface temperature may drop below the dew-point temperature of the space.~ When this occurs, condensation on the surface will occur.~ In EnergyPlus, users have several options for handling this situation including: Off and SimpleOff.~ When the user chooses the Off option, EnergyPlus will not do anything other than produce a warning message when condensation is predicted to occur.~ The program will simply continue on; no moisture will be removed from the zone air and there will be no adjustment of the surface temperature as a result of the condensation.~ When the user chooses the SimpleOff option, the program will predict cases where condensation will occur and shut-off the radiant system to avoid this situation.~ With this option, the users also have the opportunity to adjust when the system will shut down.~ This is specified with the next parameter (field: condensation differential parameter). This parameter is optional and EnergyPlus will use the SimpleOff strategy when this parameter is not specified.
+
+\paragraph{Field: Condensation Control Dewpoint Offset}\label{field-condensation-control-dewpoint-offset}
+
+This optional parameter is only valid with the SimpleOff condensation handling algorithm (see previous input parameter).~ It establishes the difference between the calculated dew-point temperature of the space and the allowed surface temperature to which the surface can drop before the radiant system shuts down in degrees Celsius.~ This parameter can be any positive, negative, or zero value.~ When this parameter is zero, the radiant system will shut down when the surface temperature drops to the dew-point temperature or below.~ When this parameter is positive, the radiant system will shut down when the surface is the number of degrees Celsius above the dew-point temperature.~ This allows some extra safety to avoid condensation.~ When this parameter is negative, the radiant system will shut down when the surface temperature is the number of degrees Celsius below the dew-point temperature.~ While not recommended, this strategy allows the user to simulate a situation where small amounts of condensation are tolerable.
+
+\paragraph{Field: Number of Circuits}\label{field-number-of-circuits}
+
+This optional input allows the user to choose between modeling each surface in the radiant system as a single hydronic circuit or to allow the program to divide the surface into multiple parallel hydronic circuits based on the next input field \emph{Circuit Length}. To model as a single circuit choose \emph{OnePerSurface}. To model as multiple circuits choose \emph{CalculateFromCircuitLength}. It is recommended that \emph{CalculateFromCircuitLength} be chosen. The default is \emph{OnePerSurface} for backward compatibility with older versions of EnergyPlus.
+
+\paragraph{Field: Circuit Length}\label{field-circuit-length}
+
+The length in meters of each parallel hydronic circuit in a surface. Used when the previous input field is set to \emph{CalculateFromCircuitLength}. The default is 106.7 meters (350 feet), which is the maximum circuit length allowed in Title 24.
+
+An example IDF with a hydronic low temperature radiant system is shown below.
+
+\begin{lstlisting}
+
+  ZoneHVAC:LowTemperatureRadiant:VariableFlow,
+      SPACE1-1 Zone Radiant Floor,  !- Name
+      RADIANTSYSAVAILSCHED,    !- Availability Schedule Name
+      SPACE1-1,                !- Zone Name
+      C1-1,                    !- Surface Name or Radiant Surface Group Name
+      0.013,                   !- Hydronic Tubing Inside Diameter {m}
+      autosize,                !- Hydronic Tubing Length {m}
+      OperativeTemperature,    !- Temperature Control Type
+      HeatingDesignCapacity,   !- Heating Design Capacity Method
+      autosize,                !- Heating Design Capacity{ W }
+      ,                        !- Heating Design Capacity Per Floor Area{ W / m2 }
+      ,                        !- Fraction of Autosized Heating Design Capacity{ -}
+      0.0004,                  !- Maximum Hot Water Flow {m3/s}
+      SPACE1-1 Zone Radiant Water Inlet Node,  !- Heating Water Inlet Node Name
+      SPACE1-1 Zone Radiant Water Outlet Node,  !- Heating Water Outlet Node Name
+      2.0,                     !- Heating Control Throttling Range {deltaC}
+      RADIANT HEATING SETPOINTS,  !- Heating Control Temperature Schedule Name
+      CoolingDesignCapacity,   !- Cooling Design Capacity Method
+      autosize,                !- Cooling Design Capacity{ W }
+      ,                        !- Cooling Design Capacity Per Floor Area{ W / m2 }
+      ,                        !- Fraction of Autosized Cooling Design Capacity{ -}
+      autosize,                !- Maximum Cold Water Flow {m3/s}
+      SPACE1-1 Cooling Water Inlet Node,  !- Cooling Water Inlet Node Name
+      SPACE1-1 Cooling Water Outlet Node,  !- Cooling Water Outlet Node Name
+      2.0,                     !- Cooling Control Throttling Range {deltaC}
+      RADIANT COOLING SETPOINTS,  !- Cooling Control Temperature Schedule Name
+      Off,                     !- Condensation Control Type
+      1.0,                     !- Condensation Control Dewpoint Offset
+      CalculateFromCircuitLength,   !- Number of Circuits
+      106.7;                   !- Circuit Length
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-007}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Radiant HVAC Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Outlet Temperature {[}C{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Moisture Condensation Time{[}s{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Heating Fluid Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Cooling Fluid Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Zone Radiant HVAC Heating Rate {[}W{]}}\label{zone-radiant-hvac-heating-rate-w}
+
+This field reports the heating input rate to the low temperature radiant system in Watts. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions and the control scheme defined in the user input.
+
+\paragraph{Zone Radiant HVAC Heating Energy {[}J{]}}\label{zone-radiant-hvac-heating-energy-j}
+
+This field reports the heating input to the low temperature radiant system in Joules. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
+
+\paragraph{Zone Radiant HVAC Cooling Rate {[}W{]}}\label{zone-radiant-hvac-cooling-rate-w}
+
+This field reports the cooling input rate to the low temperature radiant system in Watts. This is the heat sink to the surface that is defined as the radiant system. The cooling rate is determined by the zone conditions and the control scheme defined in the user input.
+
+\paragraph{Zone Radiant HVAC Cooling Energy {[}J{]}}\label{zone-radiant-hvac-cooling-energy-j}
+
+This field reports the cooling input to the low temperature radiant system in Joules. This is the heat sink to the surface that is defined as the radiant system. The cooling rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
+
+\paragraph{Zone Radiant HVAC Mass Flow Rate Rate {[}kg/s{]}}\label{zone-radiant-hvac-mass-flow-rate-rate-kgs}
+
+This field reports the mass flow rate of water through the low temperature radiant system in kilograms per second.
+
+\paragraph{Zone Radiant HVAC Inlet Temperature {[}C{]}}\label{zone-radiant-hvac-inlet-temperature-c}
+
+This field reports the temperature of water entering the low temperature radiant system in Celsius.
+
+\paragraph{Zone Radiant HVAC Outlet Temperature {[}C{]}}\label{zone-radiant-hvac-outlet-temperature-c}
+
+This field reports the temperature of water leaving the low temperature radiant system in Celsius.
+
+\paragraph{Zone Radiant HVAC Moisture Condensation Time{[}s{]}}\label{zone-radiant-hvac-moisture-condensation-times}
+
+This field reports the amount of time when condensation is occurring.~ When using the Off condensation control, this simply reports the amount of time when condensation occurs.~ When using the SimpleOff condensation control, this indicates the amount of time when the system has been shut off because of the potential danger of condensation.
+
+\paragraph{Zone Radiant HVAC Heating Fluid Energy {[}J{]}}\label{zone-radiant-hvac-heating-fluid-energy-j}
+
+This is the demand placed on the hot fluid plant loop connection serving the low temperature radiant system, in Joules.
+
+\paragraph{Zone Radiant HVAC Cooling Fluid Energy {[}J{]}}\label{zone-radiant-hvac-cooling-fluid-energy-j}
+
+This is the demand placed on the cooling fluid plant loop connection serving the low temperature radiant system, in Joules.
+
+\subsection{ZoneHVAC:LowTemperatureRadiant:ConstantFlow}\label{zonehvaclowtemperatureradiantconstantflow}
+
+This low temperature radiant system (hydronic) is a component of zone equipment that is intended to model any ``radiant system'' where water is used to supply/remove energy to/from a building surface (wall, ceiling, or floor). The component is controlled via control schedules as described in the syntax below and does not require a zone thermostat. Note that because this unit does not require a thermostat that in cases where no other systems are serving the zone in which this system resides that it will use the heating equipment priority to determine which system will run first.~ If the radiant system is serving a zone with forced air equipment, the radiant system will follow the priority order established by the zone thermostat but will still base its response on the controls defined by the user for the radiant system.
+
+The constant flow system differs from the hydronic system describe above in what it controls. The hydronic system varies the flow rate through the radiant system based on some control temperature. The constant flow system keeps flow rate constant via a local circulation pump and varies the water temperature that is sent to the radiant system. This is accomplished with a mixing valve that is controlled by a sensor. This model covers a wide range of low temperature radiant systems: heating and/or cooling, panel or embedded pipes, etc. It is not intended to simulate high temperature electric or gas radiant heaters. Those devices will be handled by a separate model and different input syntax. Low temperature radiant systems that use electric resistance heating should also be defined using separate input syntax (ref: ZoneHVAC:LowTemperatureRadiant:Electric). Low temperature radiant systems that vary the flow rate through the radiant system should also be defined using separate input syntax (ref: ZoneHVAC:LowTemperatureRadiant:VariableFlow)
+
+One of the other differences between this model and the variable flow hydronic radiant system is that the constant flow radiant system has a built-in local secondary loop. It will recirculate flow coming out of the system and mix this with flow from the loop to arrive at the desired inlet temperature to the radiant system (note that this model has the temperature sensor AFTER the pump to insure proper inlet temperature to the radiant system). The local loop also contains a pump which is assumed to be upstream of the radiant system and after the mixing valve. So, the local loop can have some recirculation. The flow from the main loop may also bypass the radiant system if more than enough flow is available and the main loop is also a constant flow system.
+
+\subsubsection{Inputs}\label{inputs-6-019}
+
+\paragraph{Field: Name}\label{field-name-6-016}
+
+This field is an unique user assigned name for an instance of a constant flow low temperature radiant system. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-6-003}
+
+This field is the name of the schedule (ref: Schedule) that denotes whether the constant flow low temperature radiant system can run during a given time period. A schedule value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for that time period. A value greater than 0 (usually 1 is used) denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-007}
+
+This field is the name of the zone (Ref: Zone) in which the constant flow low temperature radiant system is principally located and intended to affect. A system that is between two zones will still act upon each zone; however, the zone name referenced here should be the zone that controls the radiant system response.
+
+\paragraph{Field: Surface Name or Radiant Surface Group Name}\label{field-surface-name-or-radiant-surface-group-name-1}
+
+This field is the name of the surface (Ref: BuildingSurface:Detailed) or surface list (Ref: ZoneHVAC:LowTemperatureRadiant:SurfaceGroup) in which the hydronic tubing is embedded/contained. This specification attaches the source or sink from the radiant system to a particular surface and the contribution of the system to the heat balances of that surface. If this field is a surface list, then the source or sink is attached to all of the surfaces in the list with the radiant system surface group defining the breakdown of how flow rate is split between the various surfaces. Base surfaces (e.g., BuildingSurface:Detailed), door surfaces and internal mass are valid. Window surfaces are not valid surface types for embedded radiant systems.
+
+\paragraph{Field: Hydronic Tubing Inside Diameter}\label{field-hydronic-tubing-inside-diameter-1-000}
+
+This field is the inside diameter of the tubes through which water is circulated for the system being defined by this statement. The inside diameter should be recorded in meters and is used to determine the convective heat transfer from the water to the inside surface of the hydronic tubing.
+
+\paragraph{Field: Hydronic Tubing Length}\label{field-hydronic-tubing-length-1}
+
+This field is the total length of pipe embedded in the surface named above in the surface name field. The length of the tube should be entered in meters and is used to determine the effectiveness of heat transfer from the fluid being circulated through the tubes and the tube/surface. Longer tubing lengths result in more heat being transferred to/from the radiant surface to the circulating fluid. This field is autosizable.
+
+\paragraph{Field: Temperature Control Type}\label{field-temperature-control-type-1}
+
+This field specifies along with setpoint (control) and water schedules how the user wishes to control the constant flow radiant system. The temperature denoted in the setpoint schedule can refer to one of five different temperatures: the zone mean air temperature, the zone mean radiant temperature, the zone operative temperature, the outdoor dry-bulb temperature, or the outdoor wet-bulb temperature. The choice of temperature is controlled by the current field---temperature control type. The user must select from the following options:
+
+\begin{itemize}
+\item
+  MeanAirTemperature
+\item
+  MeanRadiantTemperature
+\item
+  OperativeTemperature
+\item
+  OutdoorDryBulbTemperature
+\item
+  OutdoorWetBulbTemperature
+\end{itemize}
+
+Operative temperature for radiant system controls is the average of Mean Air Temperature and Mean Radiant Temperature. If the user does not select a control type, \textbf{MeanAirTemperature} control is assumed by EnergyPlus. See the throttling range and control temperature schedule fields below for more information.
+
+\paragraph{Field: Rated Flow Rate}\label{field-rated-flow-rate}
+
+This field is the maximum flow rate of water through the radiant system in m\(^{3}\)/sec.~This flow rate is held constant by the local component pump, but the user has the option of varying this flow rate via a schedule (see next input field). The constant flow system will accept this flow rate and control the inlet temperature based on the control and water temperature schedules defined below. This field is autosizable.
+
+\paragraph{Field: Pump Flow Rate Schedule Name}\label{field-pump-flow-rate-schedule-name-001}
+
+This field modifies the maximum flow rate of water through the radiant system in m\(^{3}\)/sec.~This input is ``optional''. If the user does not enter a schedule, the flow rate through the radiant system is assumed to be constant during all hours that it is operating based on the value entered in the previous input field. Note that the values for this schedule must be between zero and one. The values in this schedule are multipliers on the previous field -- Rated Flow Rate.
+
+\paragraph{Field: Rated Pump Head}\label{field-rated-pump-head}
+
+This numeric field contains the pump's rated head in Pascals.
+
+\paragraph{Field: Rated Power Consumption}\label{field-rated-power-consumption-000}
+
+This numeric field contains the pump's rated power consumption in Watts.
+
+\paragraph{Field: Motor Efficiency}\label{field-motor-efficiency-001}
+
+This numeric field contains the pump's efficiency in decimal form (0 = 0\%, 1 = 100\%).
+
+\paragraph{Field: Fraction of Motor Inefficiencies to Fluid Stream}\label{field-fraction-of-motor-inefficiencies-to-fluid-stream-000}
+
+This numeric field contains the pump's fraction of power loss to the fluid.
+
+\paragraph{Field: Heating Water Inlet Node Name}\label{field-heating-water-inlet-node-name-1}
+
+This field contains the name of the hot water inlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a heating coil.
+
+\paragraph{Field: Heating Water Outlet Node Name}\label{field-heating-water-outlet-node-name-1}
+
+This field contains the name of the hot water outlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a heating coil.
+
+\paragraph{Field: Heating High Water Temperature Schedule Name}\label{field-heating-high-water-temperature-schedule-name}
+
+This field specifies the high water temperature in degrees Celsius for the temperature control of a constant flow radiant heating system. Water and control temperatures for heating work together to provide a linear function that determines the water temperature sent to the radiant system. The current control temperature (see Temperature Control Type above) is compared to the high and low control temperatures at the current time. If the control temperature is above the high temperature, then the system will be turned off and the water mass flow rate will be zero. If the control temperature is below the low temperature, then the inlet water temperature is set to the high water temperature. If the control temperature is between the high and low value, then the inlet water temperature is linearly interpolated between the low and high water temperature values.~ For more information and a graph of how the water and control schedules affect the system operation, please consult the Engineering Reference document.
+
+\paragraph{Field: Heating Low Water Temperature Schedule Name}\label{field-heating-low-water-temperature-schedule-name}
+
+This field specifies the low water temperature in degrees Celsius for the temperature control of a constant flow heating radiant system. For more information on its interpretation, see Heating High Water Temperature Schedule above.
+
+\paragraph{Field: Heating High Control Temperature Schedule Name}\label{field-heating-high-control-temperature-schedule-name}
+
+This field specifies the high control temperature in degrees Celsius for the temperature control of a constant flow heating radiant system. For more information on its interpretation, see Heating High Water Temperature Schedule above.
+
+\paragraph{Field: Heating Low Control Temperature Schedule Name}\label{field-heating-low-control-temperature-schedule-name}
+
+This field specifies the low control temperature in degrees Celsius for the temperature control of a constant flow heating radiant system. For more information on its interpretation, see Heating High Water Temperature Schedule above.
+
+\paragraph{Field: Cooling Water Inlet Node Name}\label{field-cooling-water-inlet-node-name-1}
+
+This field contains the name of the cold water inlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a cooling coil. As with the maximum cold water flow rate, this field is optional and not required for a heating only system.
+
+\paragraph{Field: Cooling Water Outlet Node Name}\label{field-cooling-water-outlet-node-name-1}
+
+This field contains the name of the cold water outlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a cooling coil. As with the maximum cold water flow rate, this field is optional and not required for a heating only system.
+
+\paragraph{Field: Cooling High Water Temperature Schedule Name}\label{field-cooling-high-water-temperature-schedule-name}
+
+This field specifies the high water temperature in degrees Celsius for the temperature control of a constant flow radiant cooling system. Water and control temperatures for heating work together to provide a linear function that determines the water temperature sent to the radiant system. The current control temperature (see Temperature Control Type above) is compared to the high and low control temperatures at the current time. If the control temperature is above the high temperature, then the inlet water temperature is set to the low water temperature. If the control temperature is below the low temperature, then system will be turned off and the water mass flow rate will be zero. If the control temperature is between the high and low value, then the inlet water temperature is linearly interpolated between the low and high water temperature values.~ For more information and a graph of how the water and control schedules affect the system operation, please consult the Engineering Reference document.
+
+\paragraph{Field: Cooling Low Water Temperature Schedule Name}\label{field-cooling-low-water-temperature-schedule-name}
+
+This field specifies the low water temperature in degrees Celsius for the temperature control of a constant flow cooling radiant system. For more information on its interpretation, see Cooling High Water Temperature Schedule above.
+
+\paragraph{Field: Cooling High Control Temperature Schedule Name}\label{field-cooling-high-control-temperature-schedule-name}
+
+This field specifies the high control temperature in degrees Celsius for the temperature control of a constant flow cooling radiant system. For more information on its interpretation, see Cooling High Water Temperature Schedule above.
+
+\paragraph{Field: Cooling Low Control Temperature Schedule Name}\label{field-cooling-low-control-temperature-schedule-name}
+
+This field specifies the low control temperature in degrees Celsius for the temperature control of a constant flow cooling radiant system. For more information on its interpretation, see Cooling High Water Temperature Schedule above.
+
+\paragraph{Field: Condensation Control Type}\label{field-condensation-control-type-1}
+
+When radiant systems do cooling, there is the possibility that condensation will occur on the surface that is being cooled.~ This is due to the fact that the surface temperature may drop below the dew-point temperature of the space.~ When this occurs, condensation on the surface will occur.~ In EnergyPlus, users have several options for handling this situation including: Off and SimpleOff.~ When the user chooses the Off option, EnergyPlus will not do anything other than produce a warning message when condensation is predicted to occur.~ The program will simply continue on; no moisture will be removed from the zone air and there will be no adjustment of the surface temperature as a result of the condensation.~ When the user chooses the SimpleOff option, the program will predict cases where condensation will occur and shut-off the radiant system to avoid this situation.~ With this option, the users also have the opportunity to adjust when the system will shut down.~ This is specified with the next parameter (field: condensation differential parameter). This parameter is optional and EnergyPlus will use the SimpleOff strategy when this parameter is not specified.
+
+\paragraph{Field: Condensation Control Dewpoint Offset}\label{field-condensation-control-dewpoint-offset-1}
+
+This optional parameter is only valid with the SimpleOff condensation handling algorithm (see previous input parameter).~ It establishes the difference between the calculated dew-point temperature of the space and the allowed surface temperature to which the surface can drop before the radiant system shuts down in degrees Celsius.~ This parameter can be any positive, negative, or zero value.~ When this parameter is zero, the radiant system will shut down when the surface temperature drops to the dew-point temperature or below.~ When this parameter is positive, the radiant system will shut down when the surface is the number of degrees Celsius above the dew-point temperature.~ This allows some extra safety to avoid condensation.~ When this parameter is negative, the radiant system will shut down when the surface temperature is the number of degrees Celsius below the dew-point temperature.~ While not recommended, this strategy allows the user to simulate a situation where small amounts of condensation are tolerable.
+
+\paragraph{Field: Number of Circuits}\label{field-number-of-circuits-1}
+
+This optional input allows the user to choose between modeling each surface in the radiant system as a single hydronic circuit or to allow the program to divide the surface into multiple parallel hydronic circuits based on the next input field \emph{Circuit Length}. To model as a single circuit choose \emph{OnePerSurface}. To model as multiple circuits choose \emph{CalculateFromCircuitLength}. It is recommended that \emph{CalculateFromCircuitLength} be chosen. The default is \emph{OnePerSurface} for backward compatibility with older versions of EnergyPlus.
+
+\paragraph{Field: Circuit Length}\label{field-circuit-length-1}
+
+The length in meters of each parallel hydronic circuit in a surface. Used when the previous input field is set to \emph{CalculateFromCircuitLength}. The default is 106.7 meters (350 feet), which is the maximum circuit length allowed in Title 24.
+
+An example IDF with a constant flow low temperature radiant system is shown below.
+
+\begin{lstlisting}
+
+ZoneHVAC:LowTemperatureRadiant:ConstantFlow,
+      Resistive Zone Radiant Floor,  !- name of CONSTANT FLOW low temperature radiant system
+      RadiantSysAvailSched,  !- availability schedule
+      Resistive Zone,  !- Zone name
+      Zn001:Flr001,  !- Surface name or group
+      0.012,  !- Hydronic tubing inside diameter {m}
+      400.0,  !- Hydronic tubing length {m}
+      MeanAirTemperature,  !- temperature control type
+      0.0004,  !- maximum water volumetric flow rate {m3/s}
+      ,  !-schedule for flow rate (optional, non-existent means constant)
+      30000, !-Rated Pump Head in Pa
+      50,  !-Rated Power Consumption in W
+      0.87,  !-Motor Efficiency
+      0.1,  !-Fraction of Motor Inefficiencies to Fluid Stream
+      Resistive Zone Radiant Water Inlet Node,  !- heating water inlet node
+      Resistive Zone Radiant Water Outlet Node,  !- heating water outlet node
+      RadHeatHighWaterTemp,  !-high water temperature schedule
+      RadHeatLowWaterTemp,   !-low water temperature schedule
+      RadHeatHighControlTemp, !-high control temperature schedule
+      RadHeatLowControlTemp,  !-low control temperature schedule
+      Zone 1 Cooling Water Inlet Node,  !- cooling water inlet node
+      Zone 1 Cooling Water Outlet Node,  !- cooling water outlet node
+      RadCoolHighWaterTemp, !-cooling high water temperature schedule
+      RadCoolLowWaterTemp,  !-cooling low water temperature schedule
+      RadCoolHighControlTemp, !- cooling high control temperature schedule
+      RadCoolLowControlTemp,  !- cooling low control temperature schedule
+      SimpleOff,              !- condensation control type
+      0.5,                    !- condensation control dewpoint offset
+      CalculateFromCircuitLength,   !- Number of Circuits
+      106.7;                   !- Circuit Length
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-007}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Radiant HVAC Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Injection Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Recirculation Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Pump Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Pump Electric Power{[}W{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Pump Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Radiant HVAC Pump Fluid Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Pump Fluid Heat Gain Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Moisture Condensation Time {[}s{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Cooling Fluid Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Heating Fluid Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Zone Radiant HVAC Heating Rate {[}W{]}}\label{zone-radiant-hvac-heating-rate-w-1}
+
+This field reports the heating input rate to the low temperature radiant system in Watts. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions and the control scheme defined in the user input.
+
+\paragraph{Zone Radiant HVAC Heating Energy {[}J{]}}\label{zone-radiant-hvac-heating-energy-j-1}
+
+This field reports the heating input to the low temperature radiant system in Joules. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
+
+\paragraph{Zone Radiant HVAC Cooling Rate {[}W{]}}\label{zone-radiant-hvac-cooling-rate-w-1}
+
+This field reports the cooling input rate to the low temperature radiant system in Watts. This is the heat sink to the surface that is defined as the radiant system. The cooling rate is determined by the zone conditions and the control scheme defined in the user input.
+
+\paragraph{Zone Radiant HVAC Cooling Energy {[}J{]}}\label{zone-radiant-hvac-cooling-energy-j-1}
+
+This field reports the cooling input to the low temperature radiant system in Joules. This is the heat sink to the surface that is defined as the radiant system. The cooling rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
+
+\paragraph{Zone Radiant HVAC Mass Flow Rate {[}kg/s{]}}\label{zone-radiant-hvac-mass-flow-rate-kgs}
+
+This field reports the mass flow rate of water through the low temperature radiant system in kilograms per second. This should be identical to the pump flow rate for the system.
+
+\paragraph{Zone Radiant HVAC Injection Mass Flow Rate {[}kg/s{]}}\label{zone-radiant-hvac-injection-mass-flow-rate-kgs}
+
+This field reports the mass flow rate of water that is injected into the radiant system from the main loop. A valve will control the injection and recirculation mass flow rates (see next field) to match the temperature controls specified by the user and dictated by the current simulation conditions.
+
+\paragraph{Zone Radiant HVAC Recirculation Mass Flow Rate {[}kg/s{]}}\label{zone-radiant-hvac-recirculation-mass-flow-rate-kgs}
+
+This field reports the mass flow rate of water that is recirculated from the radiant system outlet and mixed with the injection flow from the main loop. A valve will control the injection and recirculation mass flow rates (see next field) to match the temperature controls specified by the user and dictated by the current simulation conditions.
+
+\paragraph{Zone Radiant HVAC Inlet Temperature {[}C{]}}\label{zone-radiant-hvac-inlet-temperature-c-1}
+
+This field reports the temperature of water entering the low temperature radiant system in Celsius. This may differ from the inlet node temperature for the component since this component has its own local secondary loop.
+
+\paragraph{Zone Radiant HVAC Outlet Temperature {[}C{]}}\label{zone-radiant-hvac-outlet-temperature-c-1}
+
+This field reports the temperature of water leaving the low temperature radiant system in Celsius. This may differ from the outlet node temperature for the component since this component has its own local secondary loop.
+
+\paragraph{Zone Radiant HVAC Pump Inlet Temperature {[}C{]}}\label{zone-radiant-hvac-pump-inlet-temperature-c}
+
+This field reports the temperature of water entering the low temperature radiant system pump in Celsius. This may differ from the inlet node temperature for the component since this component has its own local secondary loop. It is assumed that the pump is upstream of the radiant system.
+
+\paragraph{Zone Radiant HVAC Pump Electric Power {[}W{]}}\label{zone-radiant-hvac-pump-electric-power-w}
+
+This field reports the rate of electric power consumption for the pump which supplies flow to the constant flow radiant system in Watts.
+
+\paragraph{Zone Radiant HVAC Pump Electric Energy {[}J{]}}\label{zone-radiant-hvac-pump-electric-energy-j}
+
+This field reports the electric power consumption for the pump which supplies flow to the constant flow radiant system in Joules.
+
+\paragraph{Zone Radiant HVAC Pump Mass Flow Rate {[}kg/s{]}}\label{zone-radiant-hvac-pump-mass-flow-rate-kgs}
+
+This field reports the mass flow rate of water through the low temperature radiant system pump in kilograms per second. This should be identical to the flow rate for the system.
+
+\paragraph{Zone Radiant HVAC Pump Fluid Heat Gain Rate {[}W{]}}\label{zone-radiant-hvac-pump-fluid-heat-gain-rate-w}
+
+This field reports the rate at which heat is added to the fluid stream as it passes through the pump in Watts. This heat is reflected in the radiant system inlet temperature which will be different from the pump inlet temperature if this field has a non-zero value.
+
+\paragraph{Zone Radiant HVAC Pump Fluid Heat Gain Energy {[}J{]}}\label{zone-radiant-hvac-pump-fluid-heat-gain-energy-j}
+
+This field reports the amount of heat energy added to the fluid stream as it passes through the pump in Joules. This heat is reflected in the radiant system inlet temperature which will be different from the pump inlet temperature if this field has a non-zero value.
+
+\paragraph{Zone Radiant HVAC Moisture Condensation Time {[}s{]}}\label{zone-radiant-hvac-moisture-condensation-time-s}
+
+This field reports the amount of time when condensation is occurring.~ When using the Off condensation control, this simply reports the amount of time when condensation occurs.~ When using the SimpleOff condensation control, this indicates the amount of time when the system has been shut off because of the potential danger of condensation.
+
+\paragraph{Zone Radiant HVAC Cooling Fluid Heat Transfer Energy {[}J{]}}\label{zone-radiant-hvac-cooling-fluid-heat-transfer-energy-j}
+
+The heat transfer energy for the cooling fluid connection, in Joules.
+
+\paragraph{Zone Radiant HVAC Heating Fluid Heat Transfer Energy {[}J{]}}\label{zone-radiant-hvac-heating-fluid-heat-transfer-energy-j}
+
+The heat transfer energy for the heating fluid connection, in Joules.
+
+\subsection{ZoneHVAC:LowTemperatureRadiant:Electric}\label{zonehvaclowtemperatureradiantelectric}
+
+This low temperature radiant system (electric) is a component of zone equipment that is intended to model any ``radiant system'' where electric resistance heating is used to supply energy (heat) to a building surface (wall, ceiling, or floor). The component is controlled by the radiant system controls that are defined in the syntax below and this control does not require the use of a zone thermostat unless the unit is being autosized. Note also that because this unit does not require a thermostat that in cases where no other systems are serving the zone in which this system resides that it will use the heating equipment priority to determine which system will run first.~ If the radiant system is serving a zone with forced air equipment, the radiant system will follow the priority order established by the zone thermostat but will still base its response on the controls defined by the user for the radiant system.
+
+The control is accomplished by varying the electrical power supplied to the unit. This model covers either a radiant panel system or wires embedded in entire walls, floors, or ceilings. It is not intended to simulate high temperature electric or gas radiant heaters. Those devices will be handled by a separate model and different input syntax. Low temperature radiant systems that use water flowing through tubes to provide heat to the system should also be defined using separate input syntax (ref: Low Temp Radiant System:Hydronic).
+
+\subsubsection{Inputs}\label{inputs-7-019}
+
+\paragraph{Field: Name}\label{field-name-7-015}
+
+This field is an unique user assigned name for an instance of an electric low temperature radiant system. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-7-003}
+
+This field is the name of the schedule (ref: Schedule) that denotes whether the electric low temperature radiant system can operate during a given time period. A schedule value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for that time period. A value greater than 0 (usually 1 is used) denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-2-005}
+
+This field is the name of the zone (Ref: Zone) in which the electric low temperature radiant system is principally located and intended to affect. A system that is between two zones will still act upon each zone; however, the zone name referenced here should be the zone that controls the radiant system response.
+
+\paragraph{Field: Surface Name or Radiant Surface Group Name}\label{field-surface-name-or-radiant-surface-group-name-2}
+
+This field is the name of the surface (Ref: BuildingSurface) or surface list (Ref: ZoneHVAC:LowTemperatureRadiant:SurfaceGroup) in which the hydronic tubing is embedded/contained. This specification attaches the source or sink from the radiant system to a particular surface and the contribution of the system to the heat balances of that surface. If this field is a surface list, then the source or sink is attached to all of the surfaces in the list with the radiant system surface group defining the breakdown of how flow rate is split between the various surfaces. Base surfaces (e.g., BuildingSurface:Detailed), door surfaces and internal mass are valid. Window surfaces are not valid surface types for embedded radiant systems.
+
+\paragraph{Field: Heating Design Capacity Method}\label{field-heating-design-capacity-method-6}
+
+Enter the method used to determine the maximum electrical power (heating design capacity ) or enter the method for scalable sizing the maximum electrical power of low temperature radiant electric unit. Input allowed is either \emph{HeatingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedHeatingCapacity}. If this input field is left blank or zero, then autosizing is assumed. \emph{HeatingDesignCapacity} means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the maximum or nominal design heating capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the low temperature radiant electric unit. \emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is \emph{HeatingDesignCapacity}.
+
+\paragraph{Field: Heating Design Capacity \{W\}}\label{field-heating-design-capacity-w-6}
+
+This field is for the maximum amount of electric energy rate (electric power) converted into heat in low temperature radiant electric unit in watts. This input field is autosizable. The controls for the radiant system will vary the amount of power supplied to the surface between zero input and the maximum power specified in this field as the lower and upper bounds, respectively. Note that if the user elects to autosize this field that a standard zone thermostat such as would be used for a forced air system must be defined as autosizing calculations are based on the zone thermostat value and not on the low temperature radiant electric unit control values. The default input for this input field is autosize.
+
+\paragraph{Field: Heating Design Capacity Per Floor Area \{W/m2\}}\label{field-heating-design-capacity-per-floor-area-wm2-6}
+
+Enter the heating capacity per unit floor area in m3/s-m2 of low temperature radiant electric system. This field is required field when the Heating Design Capacity Method is \emph{CapacityPerFloorArea}. The program calculates the heating capacity from floor area of the zone served by the low temperature radiant electric unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
+
+\paragraph{Field: Fraction of Autosized Heating Design Capacity}\label{field-fraction-of-autosized-heating-design-capacity-6}
+
+Enter the heating capacity as a fraction of the autosized heating capacity of low temperature radiant electric unit. This input field is required when the Heating Design Capacity Method is \emph{FractionOfAutosizedHeatingCapacity}. The program calculates the heating capacity from the design autosized heating capacity and user specified fraction. Design day sizing must be specified. This field may be left blank. The default value is 1.0.
+
+\paragraph{Field: Temperature Control Type}\label{field-temperature-control-type-2}
+
+This field specifies along with the throttling range and setpoint schedules how the user wishes to control the low temperature electric radiant system. The temperature denoted in the setpoint schedule can refer to one of three different temperatures: the zone mean air temperature, the zone mean radiant temperature, the zone operative temperature, the outdoor dry-bulb temperature, or the outdoor wet-bulb temperature. The choice of temperature is controlled by the current field---temperature control type. The user must select from the following options:
+
+\begin{itemize}
+\item
+  MeanAirTemperature
+\item
+  MeanRadiantTemperature
+\item
+  OperativeTemperature
+\item
+  OutdoorDryBulbTemperature
+\item
+  OutdoorWetBulbTemperature
+\end{itemize}
+
+Operative temperature for radiant system controls is the average of Mean Air Temperature and Mean Radiant Temperature. If the user does not select a control type, \textbf{MeanAirTemperature} control is assumed by EnergyPlus. See the throttling range and control temperature schedule fields below for more information.
+
+\paragraph{Field: Heating Throttling Range}\label{field-heating-throttling-range}
+
+This field specifies the range of temperature in degrees Celsuis over which the radiant system throttles from zero heat input via the electric resistance wires up to the maximum defined by the maximum electrical power field described above. The throttling range parameter is used in conjunction with the control temperature (see below) to define the response of the system to various zone conditions. The heating control temperature schedule specifies the ``setpoint'' temperature where the power input to the system is at half of the maximum power input. For example, if the heating control temperature setpoint is currently 15°C and the heating throttling range is 2°C, the electrical power supplied to the radiant system will be zero when the controlling temperature (MAT, MRT, Operative Temperature, ODB, or OWB; see control type field above) is at or above 16°C and the maximum power input when the controlling temperature is at or below 14°C. This represents a throttling range of 2°C around the setpoint of 15°C. In between 14°C and 16°C, the power input to the radiant system is varied linearly.
+
+\paragraph{Field: Heating Setpoint Temperature Schedule Name}\label{field-heating-setpoint-temperature-schedule-name}
+
+This field specifies the heating setpoint or control temperature for the radiant system in degrees Celsius. Used in conjunction with the previous field (heating throttling range), it will define whether or not the system is running and the current power input to the radiant surface. Power input to the system is varied linearly around the setpoint temperature based on the throttling range and the maximum electrical power parameters (see above). It should be noted that this control schedule will allow different setpoint temperatures throughout the year for heating. In addition, this schedule may be different that the thermostatic control schedule defined for overall operation of components serving the zone in which the radiant system is located. The thermostatic control determines whether or not there is a heating or cooling load in the space and thus whether the systems should be operating. This field simply controls the flow rate to the radiant system.
+
+An example IDF with an electric low temperature radiant system is shown below.
+
+\begin{lstlisting}
+
+ZoneHVAC:LowTemperatureRadiant:Electric, Zone 2 Radiant Floor,
+           RadiantPanelAvailSched ,    ! Availability schedule
+           EAST ZONE ,                 ! Zone name (name of zone system is serving)
+           Zn002:Flr001 ,              ! Surface name (name of surface system is embedded in)
+           HeatingDesignCapacity,      !- Heating Design Capacity Method
+           10000,                      !- Heating Design Capacity{ W }
+           ,                           !- Heating Design Capacity Per Floor Area{ W / m2 }
+           ,                           !- Fraction of Autosized Heating Design Capacity{ -}
+           MeanAirTemperature,         ! control type (control on mean air temperature)
+           2.0 ,                       ! heating throttling range (in C)
+           Radiant Heating Setpoints ; ! heating setpoint temperatures
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-007}
+
+\begin{itemize}
+\item
+  HVAC,Average, Zone Radiant HVAC Electric Power{[}W{]}
+\item
+  HVAC,Sum, Zone Radiant HVAC Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Radiant HVAC Heating Energy {[}J{]}
+\item
+  HVAC,Average, Zone Radiant HVAC Heating Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Zone Radiant HVAC Electric Power {[}W{]}}\label{zone-radiant-hvac-electric-power-w}
+
+This field reports the rate at which electric energy is ``burned'' in the low temperature radiant system in Watts. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions and the control scheme defined in the user input.
+
+\paragraph{Zone Radiant HVAC Electric Energy {[}J{]}}\label{zone-radiant-hvac-electric-energy-j}
+
+This field reports the amount of electric energy ``burned'' in the low temperature radiant system in Joules. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
+
+\paragraph{Zone Radiant HVAC Heating Energy {[}J{]}}\label{zone-radiant-hvac-heating-energy-j-2}
+
+\paragraph{Zone Radiant HVAC Heating Rate {[}W{]}}\label{zone-radiant-hvac-heating-rate-w-2}
+
+These outputs are the heating provided by the low temperature radiant system to the zone, in Watts or Joules.
+
+\subsection{ZoneHVAC:LowTemperatureRadiant:SurfaceGroup}\label{zonehvaclowtemperatureradiantsurfacegroup}
+
+A low temperature radiant system (hydronic or electric) may consist of multiple active surfaces that are serving to condition the space. Surfaces that act serially can be specified as multiple radiant systems using the standard radiant system input described above. However, if the multiple surfaces act in parallet, the Radiant System Surface Group input line is used to specify which surfaces are acting in a coordinated fashion and how flow rate is split between the surfaces. This list of surfaces (the name it is assigned) replaces the name of a single surface in the radiant system input described above. Note that all of the surfaces within a single list must be a part of the same zone and that the zone of these surfaces must also match the zone the radiant system is attempting to condition.
+
+\subsubsection{Inputs}\label{inputs-8-017}
+
+\paragraph{Field: Name}\label{field-name-8-015}
+
+This field is an unique user assigned name for the list of surfaces that are acting in coordination with one another. Any reference to this list by a radiant system will use this name.
+
+\paragraph{Field Set: Surface Name, Flow Fraction to Surface}\label{field-set-surface-name-flow-fraction-to-surface}
+
+The pairs of Surface Name, Flow Fraction to Surface are used in several objects. There can be up to 10 specified. The object is extensible so more can be added.
+
+\paragraph{Field: Surface \textless{}x\textgreater{} Name}\label{field-surface-x-name-2}
+
+This field is the name of a surface in the zone being conditioned by the radiant system. Base surfaces (e.g., BuildingSurface:Detailed), door surfaces and internal mass are valid. Window surfaces are not valid surface types for embedded radiant systems.
+
+\paragraph{Field: Flow Fraction for Surface \textless{}x\textgreater{}}\label{field-flow-fraction-for-surface-x}
+
+This field is the fraction of the total radiant system flow rate that is being sent to this particular surface. Note that the Surface Name/Surface Flow Fraction pair can be repeated up to 10 times. Flow rate fractions must sum to unity, otherwise the program will not accept the input as valid.
+
+An example IDF with an electric low temperature radiant system is shown below.
+
+\begin{lstlisting}
+
+ZoneHVAC:LowTemperatureRadiant:SurfaceGroup,
+      Zone 1 Radiant Surfaces, !- name of surface list
+      Zn001:Flr001,            !- Surface name 1
+      0.75,                    !- Flow fraction for surface 1
+      Zn001:Roof001,           !- Surface name 2
+      0.25;                    !- Flow fraction for surface 2
+\end{lstlisting}
+
+\subsection{ZoneHVAC:HighTemperatureRadiant}\label{zonehvachightemperatureradiant}
+
+The high temperature radiant system (gas-fired or electric) is a component of zone equipment that is intended to model any ``high temperature'' or ``high intensity'' radiant system where electric resistance or gas-fired combustion heating is used to supply energy (heat) to a building occupants directly as well as the building surfaces (wall, ceiling, or floor). The component is controlled by the radiant system controls defined in the syntax below and this control does not require the use of a zone thermostat unless the unit is being autosized. Note also that because this unit does not require a thermostat that in cases where no other systems are serving the zone in which this system resides that it will use the heating equipment priority to determine which system will run first.~ If the radiant system is serving a zone with forced air equipment, the radiant system will follow the priority order established by the zone thermostat but will still base its response on the controls defined by the user for the radiant system.
+
+The control is accomplished by varying the electrical power supplied to or gas consumed by the unit. It is not intended to simulate low temperature electric or hydronic radiant systems. Those devices will be handled by a separate model and different input syntax (ref: the low temperature systems described elsewhere).
+
+\subsubsection{Inputs}\label{inputs-9-015}
+
+\paragraph{Field: Name}\label{field-name-9-013}
+
+This field is an unique user assigned name for an instance of the high temperature radiant system. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-8-003}
+
+This field is the name of the schedule (ref: Schedule) that denotes whether the high temperature radiant system can operate during a given time period. A schedule value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for that time period. A value greater than 0 (usually 1 is used) denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-3-004}
+
+This field is the name of the zone (Ref: Zone) in which the high temperature radiant system is principally located and intended to affect.
+
+\paragraph{Field: Heating Design Capacity Method}\label{field-heating-design-capacity-method-7}
+
+Enter the method used to determine the maximum electrical power (heating design capacity ) or enter the method for scalable sizing the maximum electrical power of high temperature radiant system unit. Input allowed is either \emph{HeatingDesignCapacity}, \emph{CapacityPerFloorArea}, and \emph{FractionOfAutosizedHeatingCapacity}. If this input field is left blank or zero, then autosizing is assumed. \emph{HeatingDesignCapacity} means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the maximum or nominal design heating capacity if autosize is specified. \emph{CapacityPerFloorArea} means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the high temperature radiant electric unit. \emph{FractionOfAutosizedHeatingCapacity} means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is \emph{HeatingDesignCapacity}.
+
+\paragraph{Field: Heating Design Capacity \{W\}}\label{field-heating-design-capacity-w-7}
+
+This field is for the maximum amount of electric energy rate (electric power) converted into heat in high temperature radiant electric unit in watts. This input field is autosizable. The controls for the radiant system will vary the amount of power supplied to the surface between zero input and the maximum power specified in this field as the lower and upper bounds, respectively. Note that if the user elects to autosize this field that a standard zone thermostat such as would be used for a forced air system must be defined as autosizing calculations are based on the zone thermostat value and not on the radiant system control values. The default input for this field is autosize.
+
+\paragraph{Field: Heating Design Capacity Per Floor Area \{W/m2\}}\label{field-heating-design-capacity-per-floor-area-wm2-7}
+
+Enter the heating capacity per unit floor area in m3/s-m2 of high temperature radiant electric unit. This field is required field when the Heating Design Capacity Method is \emph{CapacityPerFloorArea}. The program calculates the heating capacity from floor area of the zone served by the high temperature radiant electric unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
+
+\paragraph{Field: Fraction of Autosized Heating Design Capacity}\label{field-fraction-of-autosized-heating-design-capacity-7}
+
+Enter the heating capacity as a fraction of the autosized heating capacity for high temperature radiant electric unit. This input field is required when the Heating Design Capacity Method is \emph{FractionOfAutosizedHeatingCapacity}. The program calculates the heating capacity from the design autosized heating capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. The default value is 1.0.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-003}
+
+This field denotes the type of high temperature radiant heater: gas or electric. The user must specify this by inputting either the keyword ``\textbf{NaturalGas}'' or ``\textbf{Electricity}'' for this field.
+
+\paragraph{Field: Combustion Efficiency}\label{field-combustion-efficiency}
+
+This field is the combustion efficiency for a gas high temperature radiant heater. This value should be greater than 0 and less than or equal to 1. It is intended to take into account any potential inefficiencies in the combustion process inside the radiant heater. The heater gas consumption is the ratio of heater output over the combustion efficiency. This parameter has no meaning for an electric high temperature radiant heater and is ignored when the previous field is equal to ``Electric''.
+
+\paragraph{Field: Fraction of Input Converted to Radiant Energy}\label{field-fraction-of-input-converted-to-radiant-energy}
+
+This field specifies what fraction of the power input to the high temperature radiant heater is actually radiant heat transfer. The fraction should be between 0 and 1. In conjunction with the next two parameters, it defines the breakdown of how the power input to the heater is distributed to the rest of the zone. The sum of these fractions must be less than or equal to 1. If the fractions are less than one, the remaining energy is added to the zone as convective heat transfer. The radiant heat transfer from the heat is distributed to people and surfaces using the distribution fractions listed below.
+
+\paragraph{Field: Fraction of Input Converted to Latent Energy}\label{field-fraction-of-input-converted-to-latent-energy}
+
+This field specifies the fraction of the power input to the high temperature radiant heater that is converted to a latent heat gain within the space. This may be appropriate when a combustion process produces moisture that is transferred into the space. The latent heat addition from a high temperature radiant heater is handled as any other latent heat gain within the space, affecting the moisture balance on the zone air.
+
+\paragraph{Field: Fraction of Input that Is Lost}\label{field-fraction-of-input-that-is-lost}
+
+This field specifies the fraction of power input to the high temperature radiant heater that is ``lost''. This energy is a loss term, and this fraction of the input power has no effect on the zone heat balances.
+
+\paragraph{Field: Temperature control type}\label{field-temperature-control-type-3}
+
+This field specifies along with the throttling range and setpoint schedules how the user wishes to control the high temperature radiant system. The temperature denoted in the setpoint schedule can refer to one of three different temperatures: a mean air temperature, a mean radiant temperature, or an operative temperature. The choice of temperature is controlled by the current field---temperature control type. The user must select from the following options:
+
+\begin{itemize}
+\item
+  MeanAirTemperature
+\item
+  MeanRadiantTemperature
+\item
+  OperativeTemperature
+\item
+  MeanAirTemperatureSetpoint
+\item
+  MeanRadiantTemperatureSetpoint
+\item
+  OperativeTemperatureSetpoint
+\end{itemize}
+
+If the user does not select a control type, OperativeTemperature control is assumed by EnergyPlus. For the setpoint control strategies (those ending in Setpoint above), EnergyPlus will attempt to find the correct heater output to meet the heating setpoint temperature (see below) through iteration and interpolation. This will more closely match the operation of an actual thermostat, but it will require significantly longer execution times.~ For more information on the standard piecewise linear control algorithm used by the Mean Air Temperature, Mean Radiant Temperature, and Operative Temperature control types (the ``non-Setpoint'' controls), see the throttling range and control temperature schedule fields below for more information.
+
+\paragraph{Field: Heating Throttling Range}\label{field-heating-throttling-range-1}
+
+This field specifies the range of temperature in degrees Celsuis over which the radiant system throttles from zero heat input via the electric resistance wires up to the maximum defined by the maximum electrical power field described above. The throttling range parameter is used in conjunction with the control temperature (see below) to define the response of the system to various zone conditions. The heating control temperature schedule specifies the ``setpoint'' temperature where the power input to the system is at half of the maximum power input. For example, if the heating control temperature setpoint is currently 15°C and the heating throttling range is 2°C, the electrical power supplied to the radiant system will be zero when the controlling temperature (Mean Air Temperature, Mean Radiant Temperature, and Operative Temperature; see control type field above) is at or above 16°C and the maximum power input when the controlling temperature is at or below 14°C. This represents a throttling range of 2°C around the setpoint of 15°C. In between 14°C and 16°C, the power input to the radiant system is varied linearly.
+
+\paragraph{Field: Heating Setpoint Temperature Schedule Name}\label{field-heating-setpoint-temperature-schedule-name-1}
+
+This field specifies the heating setpoint or control temperature for the radiant system in degrees Celsius. Used in conjunction with the previous field (heating throttling range), it will define whether or not the system is running and the current power input to the radiant surface. Power input to the system is varied linearly around the setpoint temperature based on the throttling range and the maximum electrical power parameters (see above). It should be noted that this control schedule will allow different setpoint temperatures throughout the year for heating. In addition, this schedule may be different that the thermostatic control schedule defined for overall operation of components serving the zone in which the radiant system is located. The thermostatic control determines whether or not there is a heating or cooling load in the space and thus whether the systems should be operating. This field simply controls the flow rate to the radiant system.
+
+\paragraph{Field: Fraction of Radiant Energy Incident on People}\label{field-fraction-of-radiant-energy-incident-on-people-3}
+
+This field specifies the fraction of radiant heat transfer to the zone from the radiant heater that is incident directly on people within the space. This has an impact on the predicted thermal comfort of the zone occupants. Note that since the thermal comfort models only use the results of the zone heat balances this energy is accounted for within the heat balance as convective energy, directly affecting the zone air heat balance. The basic assumption here is that most radiant energy falling on people will most likely be convected to the surroundings. This is a simplification of reality, but it maintains the overall energy balance.
+
+\paragraph{Field Set: Surface Name, Fraction of radiant energy to Surface}\label{field-set-surface-name-fraction-of-radiant-energy-to-surface-3}
+
+The pairs of Surface Name, Fraction of Radiant Energy to Surface are used in several objects. There can be up to 20 specified.
+
+\paragraph{Field: Surface \textless{}x\textgreater{} Name}\label{field-surface-x-name-3}
+
+This field is the name of the first surface to which radiant heat transfer from the high temperature radiant heater is distributed. Used in conjunction with the next field, it helps to define the distribution of the radiant energy on the surfaces within the zone. Note that up to 20 pairs of surface names and corresponding fractions may be entered for a single radiant heater system.
+
+\paragraph{Field: Fraction of Radiant Energy to Surface \textless{}x\textgreater{}}\label{field-fraction-of-radiant-energy-to-surface-x-2}
+
+This field is paired with the preceding surface name (previous field) to define the fraction of radiant heat transfer leaving the high temperature radiant system that is incident on a particular surface. Users should take into account the directionality of high temperature radiant heaters and their location when defining the value for this input field. Note that the sum of all fractions plus the fraction of radiant energy incident on people must add up to less than or equal to 1.
+
+An example IDF with a high temperature radiant system is shown below.
+
+\begin{lstlisting}
+
+ZoneHVAC:HighTemperatureRadiant, Zone 2 Radiant Heater,
+           RadiantPanelAvailSched ,   ! Availability schedule
+           EAST ZONE ,                ! Zone name (name of zone system is serving)
+           10000,                     !- Heating Design Capacity{ W }
+           ,                          !- Heating Design Capacity Per Floor Area{ W / m2 }
+           ,                          !- Fraction of Autosized Heating Design Capacity{ -}
+           Gas,                       ! type of heater (either gas or electric)
+           0.8,                       ! combustion efficiency (ignored for electric radiant heaters)
+           0.80,                      ! fraction radiant
+           0.00,                      ! fraction latent
+           0.00,                      ! fraction lost
+           OperativeTemperature,      ! temperature control type (controls on operative temperature)
+           2.0 ,                      ! heating throttling range (in C)
+           Radiant Heating Setpoints, ! heating setpoint temperatures
+           0.04,                      ! fraction of radiant energy that is incident directly on people
+           Zn002:Flr001, 0.80,        ! fraction of radiant energy that is incident on the surface indicated
+           Zn002:Wall001, 0.04,       ! fraction of radiant energy that is incident on the surface indicated
+           Zn002:Wall002, 0.04,       ! fraction of radiant energy that is incident on the surface indicated
+           Zn002:Wall003, 0.04,       ! fraction of radiant energy that is incident on the surface indicated
+           Zn002:Wall004, 0.04;       ! fraction of radiant energy that is incident on the surface indicated
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8-006}
+
+\begin{itemize}
+\item
+  HVAC,Average, Zone Radiant HVAC Heating Rate {[}W{]}
+\item
+  HVAC,Sum, Zone Radiant HVAC Heating Energy {[}J{]}
+\item
+  HVAC,Average, Zone Radiant HVAC Gas Rate {[}W{]}
+\item
+  HVAC,Sum, Zone Radiant HVAC Gas Energy {[}J{]}
+\item
+  HVAC,Average, Zone Radiant HVAC Electric Power{[}W{]}
+\item
+  HVAC,Sum, Zone Radiant HVAC Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Zone Radiant HVAC Heating Rate {[}W{]}}\label{zone-radiant-hvac-heating-rate-w-3}
+
+This field reports the rate at which energy is transferred from the high temperature radiant system to the zone in Watts. This rate is determined by the zone conditions and the control scheme defined in the user input. Note that this amount takes into account any combustion inefficiency and thus could be different that the gas consumption rate in a high temperature gas radiant system.
+
+\paragraph{Zone Radiant HVAC Heating Energy {[}J{]}}\label{zone-radiant-hvac-heating-energy-j-3}
+
+This field reports the amount of energy transferred from the high temperature gas radiant system to the zone in Joules. This amount is determined by the zone conditions, the control scheme defined in the user input, and the timestep. Note that this amount takes into account any combustion inefficiency and thus could be different that the gas consumption in a high temperature gas radiant system.
+
+\paragraph{Zone Radiant HVAC Gas Rate {[}W{]}}\label{zone-radiant-hvac-gas-rate-w}
+
+This field reports the rate at which gas is ``burned'' in a high temperature gas radiant system in Watts. This rate is determined by the zone conditions and the control scheme defined in the user input.
+
+\paragraph{Zone Radiant HVAC Gas Energy {[}J{]}}\label{zone-radiant-hvac-gas-energy-j}
+
+This field reports the amount of gas ``burned'' in a high temperature gas radiant system in Joules. This amount is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
+
+\paragraph{Zone Radiant HVAC Electric Power{[}W{]}}\label{zone-radiant-hvac-electric-powerw}
+
+This field reports the rate at which electric energy is ``burned'' in a high temperature electric radiant system in Watts. This rate is determined by the zone conditions and the control scheme defined in the user input.
+
+\paragraph{Zone Radiant HVAC Electric Energy {[}J{]}}\label{zone-radiant-hvac-electric-energy-j-1}
+
+This field reports the amount of electric energy ``burned'' in a high temperature electric radiant system in Joules. This amount is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
+
+\subsection{ZoneHVAC:VentilatedSlab}\label{zonehvacventilatedslab}
+
+Ventilated slab systems in general use outdoor air to ``precool'' slabs with colder nighttime air.~ This method of precooling the thermal mass of a space can be very effective when nighttime temperatures are low and the mass of the system is high enough to provide a significant amount of cooling potential during the day to counteract internal heat gains within a zone.~ Nearly all ventilated slabs are simple systems such as that shown in the right side of Figure~\ref{fig:ventilated-slab-model-basic-system}.~ The fan is shown in a blow through position, but the model will allow either a blow or draw through configuration.
+
+\begin{figure}[hbtp] % fig 128
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image321.png}
+\caption{Ventilated Slab model - basic system \protect \label{fig:ventilated-slab-model-basic-system}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-10-014}
+
+\paragraph{Field: Name}\label{field-name-10-012}
+
+This field is a unique user assigned name for an instance of a ventilated slab system. Any reference to this unit by another object will use this name. Other objects that use this ventilated slab system will reference it by this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-9-001}
+
+This field is the name of the schedule (ref: Schedule) that denotes whether the ventilated slab system can run during a given time period. A schedule value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for that time period. A value greater than 0 (usually 1 is used) denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\begin{figure}[hbtp] % fig 129
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image322.png}
+\caption{Example operating schedule for Ventilated Slab \protect \label{fig:example-operating-schedule-for-ventilated}}
+\end{figure}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-4-004}
+
+This field is the name of the zone (Ref: Zone) in which the ventilated slab system is principally located and intended to affect. A system that is between two zones will still act upon each zone; however, the zone name referenced here should be the zone that controls the system response.
+
+\paragraph{Field: Surface Name or Radiant Surface Group Name}\label{field-surface-name-or-radiant-surface-group-name-3}
+
+This field is the name of the surface (Ref: Surface) or surface list (Ref: ZoneHVAC:VentilatedSlab:SlabGroup) in which the hollow cores are embedded/contained. This specification attaches the source or sinks from the radiant system to a particular surface and the contribution of the system to the heat balances of that surface. If this field is a surface list, then the source or sink is attached to all of the surfaces in the list with the radiant system surface group defining the breakdown of how flow rate is split between the various surfaces. Only base surfaces (Walls, Roofs, Floors) are valid. Window/Door surfaces and Internal Mass are not valid surface types for embedded radiant systems.
+
+\paragraph{Field: Maximum Air Flow Rate}\label{field-maximum-air-flow-rate-001}
+
+This field allows the user to enter the maximum volumetric flow rate of air through the ventilated slab system in m\(^{3}\)/sec.~ This parameter should be some real number greater than zero.
+
+\paragraph{Field: Outdoor Air Control Type}\label{field-outdoor-air-control-type}
+
+This field allows the user to control how outdoor air is used in the ventilated slab system.~ The ventilated slab system described by this syntax has its own outdoor air handler.~ The three options for outdoor air control are ``\textbf{VariablePercent}'', ``\textbf{FixedTemperature}'' and ``\textbf{FixedAmount}''. Those keywords are the only allowed choices for this parameter.~ In general, the variable percent control will attempt to vary the amount of outdoor air between some minimum and maximum schedules of fractions (see next two fields) to best meet the current heating or cooling load. The fixed temperature control will vary the amount of outdoor air between the minimum schedule (fraction of maximum, see next field) and 100\% available outdoor air to come as close as possible to a desired mixed air temperature (see two fields down) that can be scheduled. The fixed amount control will fix the outdoor air flow rate as minimum outdoor air flow rate and schedule specified by the user and automatically set the maximum and minimum outside flow rate to be equal by ignoring the maximum outdoor air flow rate. More information on the controls and operation of the ventilated slab are given in the section above (preceding the IDF description).
+
+\paragraph{Field: Minimum Outdoor Air Flow Rate}\label{field-minimum-outdoor-air-flow-rate-001}
+
+This field allows the user to enter the minimum volumetric flow rate of outdoor air (in m\(^{3}\)/sec) that will be brought in to the ventilated slab. The actual minimum outdoor air flow rate will be this number multiplied by the schedule value from the minimum outdoor air schedule. If ``FixedAmount'' type is selected as the outdoor air control strategy, the outdoor air flow rate will be fixed at the value of this field and the ventilated slab will automatically set the maximum and minimum outside flow rate to be equal by ignoring the maximum outdoor air flow rate.
+
+\paragraph{Field: Minimum Outdoor Air Schedule Name}\label{field-minimum-outdoor-air-schedule-name-001}
+
+This field contains a schedule name (ref: Schedule) that should contain values for the minimum outdoor air used by the ventilated slab system for IAQ or other reasons.~ Note that if the ventilated slab is scheduled off or if there is no load sensed in the zone that the system will not operate even to achieve the minimum air fraction.~ However, if the system is operating, it will always bring in at least this fraction of the minimum air flow rate (see minimum air flow rate field above). If ``FixedAmount'' type is selected as the outdoor air control strategy, the actual outdoor air flow rate will be this number multiplied by the minimum outdoor air flow rate in the field above. The ventilated slab will automatically set the maximum and minimum outdoor air schedule to be equal by ignoring the maximum outdoor air schedule.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-001}
+
+This field allows the user to enter the maximum volumetric flow rate of outdoor air that can be brought into the ventilated slab in m\(^{3}\)/sec.~ This parameter should be some real number greater than zero.~ Note that the value for this parameter may be less than the maximum air flow rate of the ventilated slab and this may affect the maximum fraction of outdoor air within the control strategy defined above. This parameter is an absolute maximum and will supercede any scheduled fraction of the ventilated slab maximum airflow rate. If ``FixedAmount'' type is selected as the outdoor air control strategy, this field will be ignored and be automatically set to be equal to the minimum outdoor air flow rate specified in the field above.
+
+\paragraph{Field: Maximum Outdoor Air Fraction or Temperature Schedule Name}\label{field-maximum-outdoor-air-fraction-or-temperature-schedule-name}
+
+This field can have one of two meanings depending the type of control selected in the outdoor air control type parameter above.~ If ``VariablePercent'' or ``FixedAmount'' was selected, then this field is a schedule name (ref: Schedule) corresponding to a maximum air fraction schedule. Furthermore, if ``FixedAmount'' type is selected as the outdoor air control strategy, this field will be ignored and be automatically set to be equal to the minimum outdoor air fraction specified in the field below. Note that this is a fraction of the maximum airflow rate field (see parameter above) for the ventilated slab. If ``FixedTemperature'' control was selected, then this field is still a schedule name (ref: Schedule), but it corresponds to a schedule of mixed air temperatures that the outdoor air control will try to attain.
+
+\paragraph{Field: System Configuration Type}\label{field-system-configuration-type}
+
+This field allows the user to control how the air is circulated using the ventilated slab system.~ The options for system configuration are
+
+\begin{itemize}
+\item
+  SlabOnly
+\item
+  SlabAndZone
+\item
+  SeriesSlabs
+\end{itemize}
+
+In the \textbf{SlabOnly}, the ventilation air is sent to the slab only and does not enter the zone.~ In the \textbf{SlabAndZone}, the air first enters the slab and then is delivered to the zone before returning to the system. With the \textbf{SeriesSlabs} option, the user specifies a list of slabs (ZoneHVAC:VentilatedSlab:SlabGroup). This list determines the order of slabs through which the air passes.~ In this option, air is not delivered to any zone.
+
+\paragraph{Field: Hollow Core Inside Diameter}\label{field-hollow-core-inside-diameter}
+
+This field is the inside diameter of the cores through which air is circulated for the system being defined by this statement.~ The inside diameter should be recorded in meters and is used to determine the convective heat transfer from the circulated air to the inside surface of the ventilated slab.
+
+\paragraph{Field: Hollow Core Length}\label{field-hollow-core-length}
+
+This field is the length of core embedded in the surface named above in the surface name field.~ In other words, this should be the distance that air travels as it through the slab.~ The length of the hollow core in the slab should be entered in meters and is used to determine the effectiveness of heat transfer from the air being circulated through the cores and the core inside surface.~ Longer core lengths result in more heat transferred to/from the radiant surface to the circulating fluid.
+
+\paragraph{Field: Number of Cores}\label{field-number-of-cores}
+
+This field allows the user to specify how many cores there are in the ventilated slab.~ Air flow will be divided equally among the different cores.
+
+\paragraph{Field: Temperature Control Type}\label{field-temperature-control-type-4}
+
+This field specifies along with the throttling range and setpoint schedules how the user wishes to control the ventilated slab system.~ The temperature denoted in the set temperature schedule can refer to one of seven different temperatures: the zone mean air temperature, the zone mean radiant temperature, the zone operative temperature, the surface temperature of the ventilated slab, the outdoor dry-bulb temperature, the outdoor wet-bulb temperature, or the dewpoint temperature of zone mean air temperature.~ The choice of temperature is controlled by the current field---temperature control type.~ The user must select from the following options:
+
+\begin{itemize}
+\item
+  MeanAirTemperature
+\item
+  MeanRadiantTemperature
+\item
+  OperativeTemperature
+\item
+  OutdoorDryBulbTemperature
+\item
+  OutdoorWetBulbTemperature
+\item
+  SurfaceTemperature
+\item
+  ZoneAirDewPointTemperature
+\end{itemize}
+
+If the user does not select a control type, \textbf{MeanAirTemperature} control is assumed by EnergyPlus. See the control temperature schedule fields below for more information.
+
+\paragraph{Field: Heating High Air Temperature Schedule Name}\label{field-heating-high-air-temperature-schedule-name}
+
+This field specifies the high air temperature in degrees Celsius for the temperature control of a ventilated slab system. Air and control temperatures for heating work together to provide a linear function that determines the air temperature sent to the ventilated slab. The current control temperature (see Temperature Control Type above) is compared to the high and low control temperatures at the current time.~~~~~ If the control temperature is above the high temperature, then the inlet air temperature is set to the low air temperature. If the control temperature is below the low temperature, then the inlet air temperature is set to the high air temperature. If the control temperature is between the high and low value, then the inlet air temperature is linearly interpolated between the low and high air temperature values.
+
+\paragraph{Field: Heating Low Air Temperature Schedule Name}\label{field-heating-low-air-temperature-schedule-name}
+
+This field specifies the low air temperature in degrees Celsius for the temperature control of a ventilated slab. For more information on its interpretation, see Heating High Air Temperature Schedule above.
+
+\paragraph{Field: Heating High Control Temperature Schedule Name}\label{field-heating-high-control-temperature-schedule-name-1}
+
+This field specifies the high control temperature in degrees Celsius for the temperature control of a ventilated slab. For more information on its interpretation, see Heating High Air Temperature Schedule above.
+
+\paragraph{Field: Heating Low Control Temperature Schedule Name}\label{field-heating-low-control-temperature-schedule-name-1}
+
+This field specifies the low control temperature in degrees Celsius for the temperature control of a ventilated slab. For more information on its interpretation, see Heating High Air Temperature Schedule above.
+
+\paragraph{Field: Cooling High Air Temperature Schedule Name}\label{field-cooling-high-air-temperature-schedule-name}
+
+This field specifies the high air temperature in degrees Celsius for the temperature control of a ventilated slab system. Air and control temperatures for cooling work together to provide a linear function that determines the air temperature sent to the ventilated slab system. The current control temperature (see Temperature Control Type above) is compared to the high and low control temperatures at the current time. If the control temperature is above the high temperature, then the inlet air temperature is set to the low air temperature. If the control temperature is below the low temperature, then the inlet air temperature is set to the high air temperature. If the control temperature is between the high and low value, then the inlet air temperature is linearly interpolated between the low and high air temperature values.
+
+\paragraph{Field: Cooling Low Air Temperature Schedule Name}\label{field-cooling-low-air-temperature-schedule-name}
+
+This field specifies the low air temperature in degrees Celsius for the temperature control of a constant flow cooling radiant system. For more information on its interpretation, see Cooling High Air Temperature Schedule above.
+
+\paragraph{Field: Cooling High Control Temperature Schedule Name}\label{field-cooling-high-control-temperature-schedule-name-1}
+
+This field specifies the high control temperature in degrees Celsius for the temperature control of a constant flow cooling radiant system. For more information on its interpretation, see Cooling High Air Temperature Schedule above.
+
+\paragraph{Field: Cooling Low Control Temperature Schedule Name}\label{field-cooling-low-control-temperature-schedule-name-1}
+
+This field specifies the low control temperature in degrees Celsius for the temperature control of a ventilated slab system. For more information on its interpretation, see Cooling High Air Temperature Schedule above.
+
+\paragraph{Field: Return Air Node Name}\label{field-return-air-node-name-000}
+
+This field is a node name used to identify the node that serves as the zone return air inlet to the ventilated slab system. This node is one of the inlets to the outdoor air mixer which is implicit in the ventilated slab system model. For ``SlabAndZone'' configuration, the Return Air Node will typically be the same node as a zone exhaust node. For ``SlabOnly'' or ``SeriesSlabs'' configuration, this node name is required but will have zero flow.
+
+\paragraph{Field: Slab In Node Name}\label{field-slab-in-node-name}
+
+This field is a node name used to identify the node that serves as the inlet of the ventilated slab or series of slabs, after the outdoor air mixer, fan, and optional coils.
+
+\paragraph{Field: Zone Supply Air Node Name}\label{field-zone-supply-air-node-name-000}
+
+This field is a node name used to identify the node that serves as the outlet from the ventilated slab system to the zone when using the ``SlabAndZone'' configuration. It is the node exiting the slab section of the system. This node will typically be the same node as a zone inlet node. In the case of ``SlabOnly'' or ``SeriesSlabs'' configuration, this field will be ignored and it should be left BLANK.
+
+\paragraph{Field: Outdoor Air Node Name}\label{field-outdoor-air-node-name}
+
+This field is a node name used to identify the node associated with fresh outdoor air brought into the ventilated slab system outdoor air mixer.~ This node should also be specified in an OutdoorAir:Node or OutdoorAir:NodeList object.
+
+\paragraph{Field: Relief Air Node Name}\label{field-relief-air-node-name}
+
+This field is a node name used to identify the node associated with air exhausted out of the ventilated slab system to the outdoor environment.
+
+\paragraph{Field: Outdoor Air Mixer Outlet Node Name}\label{field-outdoor-air-mixer-outlet-node-name}
+
+This field is a node name used to identify the node associated with the ``mixed'' air of the ventilated slab.~ These conditions are post-``mixing box'' since they are the conditions of the fraction of return air combined with the outdoor air.~ Since this is a simple system, this can also be viewed as the conditions of the air being sent to the coils.
+
+\paragraph{Field: Fan Outlet Node Name}\label{field-fan-outlet-node-name}
+
+This field is a node name used to identify the node that serves as the air outlet from the fan.
+
+\paragraph{Field: Fan Name}\label{field-fan-name-003}
+
+This field is the name of a fan (ref: Fan:ConstantVolume) that is part of the ventilated slab system.~ This name links the ventilated slab to particular fan data entered elsewhere in the input data file.~ A fan name is required since it is the prime mover of air in the ventilated slab system.
+
+\paragraph{Field: Coil Option Type}\label{field-coil-option-type}
+
+This field allows the user to specify the coil operating options as one of the following options:
+
+\begin{itemize}
+\item
+  None
+\item
+  Heating
+\item
+  Cooling
+\item
+  HeatingAndCooling
+\end{itemize}
+
+If \textbf{None} is selected, the ventilated slab does not have any coils, and any other input will be ignored. If either \textbf{Heating} or \textbf{Cooling} is selected, only a heating or cooling coil, respectively, is present.~ Thus, only four more inputs will be expected. If \textbf{HeatingAndCooling} is selected, both heating and cooling coil input must be entered, and the ventilated slab will have both a heating and a cooling coil.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-001}
+
+This field is the type of coil (ref: Coil:Heating:Water, Coil:Heating:Electric, Coil:Heating:Gas, Coil:Heating:Steam) that is used for heating in the ventilated slab system. This field must be one of the following keywords: Coil:Heating:Water, Coil:Heating:Electric, Coil:Heating:Gas, Coil:Heating:Steam.~ It is used in conjunction with the heating coil name (see next field) to specify the heating coil present within the system.
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-001}
+
+This field is the name of the heating coil that is part of the ventilated slab system.~ It is assumed that there is always some sort of heating coil associated with a ventilated slab system.~ This name links the ventilated slab to particular heating coil data entered elsewhere in the input data file.
+
+\paragraph{Field: Hot Water or Steam Inlet Node Name}\label{field-hot-water-or-steam-inlet-node-name}
+
+This field corresponds to the water inlet node to the heating coil for a water coil.~ The water inlet node controls how a water heating coil operates.~ This field is ignored/not needed for gas and electric heating coils.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-001}
+
+This field is the name of the cooling coil (ref: Coil:Cooling:Water, Coil:Cooling:Water:DetailedGeometry, CoilSystem:Cooling:Water:HeatExchangerAssisted) that is part of the ventilated slab system.~ This name links the ventilated slab system to particular cooling coil data entered elsewhere in the input data file. If no cooling coil is present, the previous field may be followed by a semi-colon and the remaining parameters in this statement may be ignored.
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-001}
+
+This field is the name of the cooling coil that is part of the ventilated slab system.~ It is assumed that there is always some sort of cooling coil associated with a ventilated slab system.~ This name links the ventilated slab to particular cooling coil data entered elsewhere in the input data file.
+
+\paragraph{Field: Cold Water Inlet Node Name}\label{field-cold-water-inlet-node-name}
+
+This field corresponds to the water inlet node to the cooling coil.~ The water inlet node controls how a water cooling coil operates and is required for the ventilated slab system that has a cooling coil associated with it to function properly.
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-001}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this ventilated slab object's fan. If the ventilated slab is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this ventilated slab object should be on or off.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Maximum Air Flow Rate in this Ventilated Slab zone HVAC object. The scaled Maximum Air Flow Rate in turn is used to size cooling and heating capacity of the coils.
+
+An example IDF with a ventilated slab is shown below.
+
+\begin{lstlisting}
+
+  ZoneHVAC:VentilatedSlab,
+      Zone4VentSlab,           !- Name
+      VentSlabAvailability,    !- Availability Schedule Name
+      SPACE4-1,                !- Zone Name
+      F4-1,                    !- Surface Name or Radiant Surface Group Name
+      0.84,                    !- Maximum Air Flow Rate {m3/s}
+      VariablePercent,         !- Outdoor Air Control Type
+      0.168,                   !- Minimum Outdoor Air Flow Rate {m3/s}
+      U2MinOASched,            !- Minimum Outdoor Air Schedule Name
+      0.84,                    !- Maximum Outdoor Air Flow Rate {m3/s}
+      VentSlabMaxOA,           !- Maximum Outdoor Air Fraction or Temperature Schedule Name
+      SlabAndZone,             !- System Configuration Type
+      0.050,                   !- Hollow Core Inside Diameter {m}
+      15.0,                    !- Hollow Core Length {m}
+      50.0,                    !- Number of Cores
+      MeanRadiantTemperature,  !- Temperature Control Type
+      VentSlabHotHighAir,      !- Heating High Air Temperature Schedule Name
+      VentSlabHotLowAir,       !- Heating Low Air Temperature Schedule Name
+      VentSlabHotHighControl,  !- Heating High Control Temperature Schedule Name
+      VentSlabHotLowControl,   !- Heating Low Control Temperature Schedule Name
+      VentSlabCoolHighAir,     !- Cooling High Air Temperature Schedule Name
+      VentSlabCoolLowAir,      !- Cooling Low Air Temperature Schedule Name
+      VentSlabCoolHighControl, !- Cooling High Control Temperature Schedule Name
+      VentSlabCoolLowControl,  !- Cooling Low Control Temperature Schedule Name
+      Zone4VentSlabReturnAirNode,  !- Return Air Node Name
+      Zone4VentslabSlabInNode, !- Slab In Node Name
+      Zone4Inlets,             !-Zone Supply Air Node Name
+      Zone4VentSlabOAInNode,   !- Outdoor Air Node Name
+      Zone4VentSlabExhNode,    !- Relief Air Node Name
+      Zone4VentSlabOAMixerOutletNode,  !-Outdoor Air Mixer Outlet Node Name
+      Zone4VentSlabFanOutletNode,  !- Fan Outlet Node Name
+      Zone4VentSlabFan,        !- Fan Name
+      HeatingAndCooling,       !- Coil Option Type
+      Coil:Heating:Electric,   !- Heating Coil Object Type
+      Zone4VentSlabHeatingCoil,!- Heating Coil Name
+      ,                        !- Hot Water or Steam Inlet Node Name
+      Coil:Cooling:Water,      !- Cooling Coil Object Type
+      Zone4VentSlabCoolingCoil,!- Cooling Coil Name
+      Zone4VentSlabChWInletNode;  !- Cold Water Inlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-9-006}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Ventilated Slab Radiant Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilated Slab Radiant Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Radiant Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilated Slab Radiant Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Coil Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilated Slab Coil Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilated Slab Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilated Slab Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Coil Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilated Slab Coil Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Zone Ventilated Slab Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average, Zone Ventilated Slab Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilated Slab Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Inlet Air Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Outlet Air Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Zone Inlet Air Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Return Air Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Fan Outlet Air Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Ventilated Slab Fan Availability Status {[]}
+\end{itemize}
+
+\paragraph{Zone Ventilated Slab Radiant Heating Rate~ {[}W{]}}\label{zone-ventilated-slab-radiant-heating-rate-w}
+
+This field reports the radiant heating input rate of the ventilated slab system to the zone it is serving in Watts.~ This is determined by outlet and zone air conditions and the mass flow rate through the ventilated slab system.
+
+\paragraph{Zone Ventilated Slab Radiant Heating Energy {[}J{]}}\label{zone-ventilated-slab-radiant-heating-energy-j}
+
+This field is the heating radiant input of the ventilated slab system to the zone it is serving in Joules over the timestep being reported.~ This is determined by outlet and zone air conditions, the mass flow rate through the ventilated slab system, and the timestep.
+
+\paragraph{Zone Ventilated Slab Radiant Cooling Rate {[}W{]}}\label{zone-ventilated-slab-radiant-cooling-rate-w}
+
+This field reports the radiant cooling input rate to the ventilated slab system in Watts. This is the heat sink to the surface that is defined as the ventilated slab system. The cooling rate is determined by the zone conditions and the control scheme defined in the user input.
+
+\paragraph{Zone Ventilated Slab Radiant Cooling Energy {[}J{]}}\label{zone-ventilated-slab-radiant-cooling-energy-j}
+
+This field reports the radiant cooling input to the ventilated slab system in Joules. This is the heat sink to the surface that is defined as the radiant system. The cooling rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
+
+\paragraph{Zone Ventilated Slab Coil Heating Rate {[}W{]}}\label{zone-ventilated-slab-coil-heating-rate-w}
+
+This field reports the heating input rate of the heating coil of ventilated slab system the zone it is serving in Watts.~ This is determined by return air and zone air conditions and the mass flow rate through the ventilation slab system.
+
+\paragraph{Zone Ventilated Slab Coil Heating Energy {[}J{]}}\label{zone-ventilated-slab-coil-heating-energy-j}
+
+This field is the heating output of the heating coil of the ventilated slab system the zone it is serving in Joules over the timestep being reported.~ This is determined by return air and zone air conditions, the mass flow rate through the ventilation slab system, and the timestep.
+
+\paragraph{Zone Ventilated Slab Coil Total Cooling Rate {[}W{]}}\label{zone-ventilated-slab-coil-total-cooling-rate-w}
+
+This field reports the total cooling (sensible plus latent) output rate of the cooling coil of the ventilated slab system to the zone it is serving in Watts.~ This is determined by outlet and zone air conditions and the mass flow rate through the ventilation slab system.
+
+\paragraph{Zone Ventilated Slab Coil Total Cooling Energy {[}J{]}}\label{zone-ventilated-slab-coil-total-cooling-energy-j}
+
+This field is the total cooling (sensible plus latent) output of the cooling coil of the ventilated slab system to the zone it is serving in Joules over the timestep being reported.~ This is determined by outlet and zone air conditions, the mass flow rate through the ventilation slab system, and the timestep.
+
+\paragraph{Zone Ventilated Slab Coil Sensible Cooling Rate {[}W{]}}\label{zone-ventilated-slab-coil-sensible-cooling-rate-w}
+
+This field reports the sensible cooling output rate of the cooling coil of the ventilated slab system to the zone it is serving in Watts.~ This is determined by outlet and zone air conditions and the mass flow rate through the ventilation slab system.
+
+\paragraph{Zone Ventilated Slab Coil Sensible Cooling Energy {[}J{]}}\label{zone-ventilated-slab-coil-sensible-cooling-energy-j}
+
+This field is the sensible cooling output of the cooling coli of the ventilated slab system to the zone it is serving in Joules over the timestep being reported.~ This is determined by outlet and zone air conditions, the mass flow rate through the ventilation slab system, and the timestep.
+
+\paragraph{Zone Ventilated Slab Coil Latent Cooling Rate {[}W{]}}\label{zone-ventilated-slab-coil-latent-cooling-rate-w}
+
+This field reports the latent cooling output rate of the cooling coil of the ventilated slab system to the zone it is serving in Watts.~ This is determined by outlet and zone air conditions and the mass flow rate through the ventilation slab system.
+
+\paragraph{Zone Ventilated Slab Coil Latent Cooling Energy {[}J{]}}\label{zone-ventilated-slab-coil-latent-cooling-energy-j}
+
+This field is the latent cooling output of the cooling coli of the ventilated slab system to the zone it is serving in Joules over the timestep being reported.~ This is determined by outlet and zone air conditions, the mass flow rate through the ventilation slab system, and the timestep.
+
+\paragraph{Zone Ventilated Slab Air Mass Flow Rate {[}kg/s{]}}\label{zone-ventilated-slab-air-mass-flow-rate-kgs}
+
+This field reports the mass flow rate of air through the ventilated slab system in kilograms per second.
+
+\paragraph{Zone Ventilated Slab Fan Electric Power {[}W{]}}\label{zone-ventilated-slab-fan-electric-power-w}
+
+This field reports the electric power consumption rate of the fan of the ventilated slab system in Watts.
+
+\paragraph{Zone Ventilated Slab Fan Electric Energy {[}J{]}}\label{zone-ventilated-slab-fan-electric-energy-j}
+
+This field reports the electric power consumed by the fan of the ventilated slab system over the timestep in Joules.
+
+\paragraph{Zone Ventilated Slab Inlet Air Temperature {[}C{]}}\label{zone-ventilated-slab-inlet-air-temperature-c}
+
+This field reports the temperature of air entering the ventilated slab system in Celsius.
+
+\paragraph{Zone Ventilated Slab Outlet Air Temperature {[}C{]}}\label{zone-ventilated-slab-outlet-air-temperature-c}
+
+This field reports the temperature of air leaving the ventilated slab system in Celsius.
+
+\paragraph{Zone Ventilated Slab Zone Inlet Air Temperature {[}C{]}}\label{zone-ventilated-slab-zone-inlet-air-temperature-c}
+
+This field reports the temperature of air entering the zone in Celsius.
+
+\paragraph{Zone Ventilated Slab Return Air Temperature {[}C{]}}\label{zone-ventilated-slab-return-air-temperature-c}
+
+This field reports the temperature of air leaving the zone in Celsius. When system does not circulate air to zone(``SlabOnly'' Configuration), the slab outlet temperature and return air temperature will be the same.
+
+\paragraph{Zone Ventilated Slab Fan Outlet Air Temperature {[}C{]}}\label{zone-ventilated-slab-fan-outlet-air-temperature-c}
+
+This field reports the fan outlet air temperature for the ventilated slab system in Celsius.
+
+\paragraph{\texorpdfstring{Zone Ventilated Slab Fan Availability Status {[]}}{Zone Ventilated Slab Fan Availability Status }}\label{zone-ventilated-slab-fan-availability-status}
+
+This is the availability status of the ventilated slab fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the ventilated slab object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List along with Hybrid Ventilation Manager, rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\subsection{ZoneHVAC:VentilatedSlab:SlabGroup}\label{zonehvacventilatedslabslabgroup}
+
+A ventilated slab system may consist of multiple active slabs that are serving to condition the zone. Slabs that act serially can be specified as multiple radiant systems using the standard ventilated slab input described above. This list of surfaces (the name it is assigned) replcaces the name of a single surface in the ventilated slab system input described above.
+
+\subsubsection{Inputs}\label{inputs-11-013}
+
+\paragraph{Field : Name of Ventilated Slab Surface Group}\label{field-name-of-ventilated-slab-surface-group}
+
+This field is a unique user assigned name for the list of surfaces that are acting in coordination with one another. Any reference to this list by a ventilated slab system will use this name.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-5-003}
+
+This field is the name of the zone in which the surface is principally located and intended to affect.
+
+\paragraph{Field: Surface Name}\label{field-surface-name-003}
+
+This field is the name of a surface in the zone being conditioned by the ventilated slab system. Only base surfaces like walls, floors and roofs are valid. Door/Window Surface and Internal Mass are not valid surface types for the ventilated slab system.
+
+\paragraph{Field: Core Diameter}\label{field-core-diameter}
+
+This field is the inside diameter of the cores through which air is circulated for the surface being defined by this statement.~ The inside diameter should be recorded in meters and is used to determine the convective heat transfer from the circulated air to the inside surface of the ventilated slab.
+
+\paragraph{Field: Core length}\label{field-core-length}
+
+This field is the length of core embedded in the surface named above in the surface name field.~ In other words, this should be the distance that air travels as it through the slab.~ The length of the hollow core in the surface should be entered in meters and is used to determine the effectiveness of heat transfer from the air being circulated through the cores and the core inside surface.~ Longer core lengths result in more heat transferred to/from the radiant surface to the circulating fluid.
+
+\paragraph{Field: Number of Cores}\label{field-number-of-cores-1}
+
+This field allows the user to specify how many cores there are in the ventilated slab.~ Air flow will be divided equally among the different cores.
+
+\paragraph{Field: Slab Inlet Node Name}\label{field-slab-inlet-node-name}
+
+This field is a node name (character string) used to identify the node that serves as the inlet (air side) to the surface.~ In EnergyPlus, nodes represent points between components or at various points in the loops.~ While a node name may be referenced more than once in an input data file, each node must have a unique name.
+
+\paragraph{Field: Slab Outlet Node Name}\label{field-slab-outlet-node-name}
+
+This field is a node name (character string) used to identify the node that serves as the outlet (air side) of the surface.~ In EnergyPlus, nodes represent points between components or at various points in the loops.~ While a node name may be referenced more than once in an input data file, each node must have a unique name.
+
+An Example IDF with a ventilated slab system is shown below
+
+\begin{lstlisting}
+
+ZoneHVAC:VentilatedSlab:SlabGroup,
+      Z125,                    !- Name
+      SPACE1-1,                !- Zone 1 Name
+      C1-1,                    !- Surface 1 Name
+      0.05,                    !- Core Diameter for Surface 1
+      30,                      !- Core Length for Surface 1
+      20,                      !- Core Numbers for Surface 1
+      Z1VentslabIn,            !- Slab In Node Name for Surface 1
+      Z1VentSlabout,           !- Slab Outlet Node Name for Surface 1
+      SPACE2-1,                !- Zone 2 Name
+      C2-1,                    !- Surface 2 Name
+      0.05,                    !- Core Diameter for Surface 2
+      15,                      !- Core Length for Surface 2
+      20,                      !- Core Numbers for Surface 2
+      Z2VentSlabIn,            !- Slab In Node Name for Surface 2
+      Z2VentSlabOut,           !- Slab Outlet Node Name for Surface 2
+      SPACE5-1,                !- Zone 3 Name
+      C5-1,                    !- Surface 3 Name
+      0.05,                    !- Core Diameter for Surface 3
+      30,                      !- Core Length for Surface 3
+      20,                      !- Core Numbers for Surface 3
+      Z5VentSlabIn,            !- Slab In Node Name for Surface 3
+      Z5VentSlabOut;           !- Slab Outlet Node Name for Surface 3
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-refrigeration.tex b/doc/input-output-reference/src/overview/group-refrigeration.tex
new file mode 100644
index 00000000000..2c9239a89c6
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-refrigeration.tex
@@ -0,0 +1,4351 @@
+\section{Group -- Refrigeration}\label{group-refrigeration}
+
+There are two ways to model a supermarket refrigeration system.~ The first, and simplest, approach models the combination of compressor(s) and condenser as a single refrigeration compressor rack object. (A list is used to enter multiple case or walk-in names.)
+
+For the first approach, the input objects needed are:
+
+\begin{itemize}
+\item
+  One Refrigeration:CompressorRack object
+\item
+  At least one refrigeration load, which may be any combination of:
+\item
+  Refrigeration:Case or
+\item
+  Refrigeration:WalkIn or
+\item
+  Refrigeration:CaseAndWalkInList objects .
+\end{itemize}
+
+The second approach requires more input objects but also allows the user to model more complex systems.~ This detailed approach must be used whenever loads are transferred from one system to another, such as with secondary loops, cascade condensers, or mechanical subcoolers. Again lists are used to enter multiple load or compressor names.
+
+For the detailed approach, the input objects needed are:
+
+\begin{itemize}
+\item
+  One Refrigeration:System object
+\item
+  At least one refrigeration load object which may include any combination of:
+\item
+  Refrigeration:Case,
+\item
+  Refrigeration:WalkIn,
+\item
+  Refrigeration:CaseAndWalkInList (may include any combination of cases and walk in cooler names, OR, a list of air chiller names)
+\item
+  Refrigeration:SecondarySystem,
+\item
+  Refrigeration:Condenser:Cascade (as a load, cooling a lower-temperature system) objects,
+\item
+  Refrigeration:TransferLoadList (may include cascade condenser loads and/or secondary loop loads)
+\item
+  Refrigeration:AirChiller
+\item
+  At least one Refrigeration:Compressor object (multiple compressors are entered using a Refrigeration:CompressorList),
+\item
+  One condenser object which may be either:
+\item
+  Refrigeration:Condenser:AirCooled,
+\item
+  Refrigeration:Condenser:EvaporativeCooled,
+\item
+  Refrigeration:Condenser:WaterCooled, or
+\item
+  Refrigeration:Condenser:Cascade (rejecting heat from this system)
+\item
+  The object Refrigeration:Subcooler may optionally be included to describe either a liquid suction or mechanical subcooler.
+\end{itemize}
+
+Output variables are also available to describe the total heat exchange between all refrigeration objects and the zones containing these objects. These variables are described at the end of this section after all the refrigeration objects.
+
+\subsection{Refrigeration:CompressorRack}\label{refrigerationcompressorrack}
+
+The refrigeration compressor rack object works in conjunction with the refrigeration case and walkin objects (Ref. Refrigeration:Case and Refrigeration:WalkIn) to simulate the performance of a refrigerated case system. This object models the electric consumption of the rack compressors and the condenser fans. Heat removed from the refrigerated cases, walkins, and compressor/condenser fan heat can be rejected either outdoors or to a zone. Compressor rack waste heat can also be reclaimed for use by an optional air- or water-heating coil (Ref. Coil:Heating:Desuperheater and Coil:WaterHeating:Desuperheater).
+
+If heat is rejected outdoors, condenser cooling can either be accomplished by direct air flow, evaporative water cooling, or a by water-cooled condenser with appropriate plant loop piping. With evaporative cooling, water is sprayed through the air stream to effectively lower the air temperature experienced by the condenser coil as a result of water evaporation. The use of a water-cooled condenser requires the definition of a plant loop to supply cooling to the condenser.~ Waste heat can be reclaimed and stored using a water storage device.
+
+The inputs for the compressor rack object include a name, the heat rejection location, the compressor rack coefficient of performance (COP) at design conditions, the design condenser fan power, and the type of condenser cooling. The model requires two curve objects to describe performance at off-design conditions. If the condenser is water-cooled, the inlet and outlet node names as well as the water outlet temperature schedule name are required.~ If the condenser has evaporative cooling, additional inputs for evaporative condenser effectiveness, condenser air flow rate, basin heater parameters, water pump power, water source, and an evaporative cooling availability schedule are available. The names of refrigerated cases and walkins connected to the compressor rack are the final inputs to the model.
+
+\subsubsection{Inputs}\label{inputs-039}
+
+\paragraph{Field: Name}\label{field-name-038}
+
+A unique user-assigned name for an instance of a refrigeration compressor rack. Any reference to this compressor rack by another object will use this name.
+
+\paragraph{Field: Heat Rejection Location}\label{field-heat-rejection-location}
+
+The location of the compressor rack's condenser. The compressor rack condenser heat can be directed ``Outdoors'' to model an outdoor air or water-cooled condenser or ``Zone'' to model a condenser located in a zone (e.g., a stand-alone packaged refrigerated case with integral condenser located in a conditioned zone). The default for this field is ``Outdoors''. If the heat rejection location is ``Zone'' and no walk-in coolers are served by this compressor rack, then all refrigerated cases connected to this compressor rack must be located in the same zone. If however, walk-in coolers are also served by this compressor rack, then the heat rejection zone name must be specified (see Heat Rejection Zone Name field below) and cases and walk-ins can be located in multiple zones.
+
+NOTE: When modeling a heat reclaim coil, the heat rejection location must be ``Outdoors''. If the heat rejection location is ``Zone'', the total amount of waste heat available for reclaim (e.g., by a desuperheater heating coil) is set to zero by this compressor rack object and the simulation proceeds.
+
+\paragraph{Field: Design Compressor Rack COP}\label{field-design-compressor-rack-cop}
+
+The coefficient of performance (COP) for the compressor rack at design conditions (compressors only, excluding condenser fan power). This value must be greater than zero, with a default value of 2.0 if this field is left blank. This value should represent the compressor rack COP corresponding to the lowest evaporating temperature of any case or walkin served by the rack.
+
+\paragraph{Field: Compressor Rack COP Function of Temperature Curve Name}\label{field-compressor-rack-cop-function-of-temperature-curve-name}
+
+The name of the curve object defining the change in compressor rack COP as a function of the temperature of air entering the condenser. The curve object will be evaluated using the zone air dry-bulb temperature when rack heat rejection location equals ``Zone'' and the outdoor air dry-bulb temperature when rack heat rejection location equals ``Outdoors'' and the condenser type is air-cooled. As explained below, if the condenser is cooled by evaporative or water loop cooling, the curve object is evaluated using an effective temperature. The output from this curve is multiplied by the design compressor rack COP to yield the actual COP at the specific air temperature entering the condenser. This curve must be cubic or quadratic (Curve:Cubic or Curve:Quadratic), and should be normalized to 1.0 at the condenser entering air temperature at which the design compressor rack COP occurs. This curve should represent the compressor rack COP corresponding to the lowest evaporating temperature of any case served by the rack.
+
+\paragraph{Field: Design Condenser Fan Power}\label{field-design-condenser-fan-power}
+
+This field defines the design power for the condenser fan(s) in Watts. This field is applicable for air or evaporative cooling only.~ If the condenser is water-cooled, the fan power is captured in the cooling object (e.g., cooling tower).~ If applicable, this value must be greater than 0.0, with a default value of 250 Watts if this field is left blank.
+
+\paragraph{Field: Condenser Fan Power Function of Temperature Curve Name}\label{field-condenser-fan-power-function-of-temperature-curve-name}
+
+This field is the name of the curve object defining the change in condenser fan power as a function of the temperature of air entering the condenser. This curve is used to simulate the modulation of air flow by the condenser fans (e.g., staging, multi-speed, or variable speed) as a function of temperature.~ The curve object will be evaluated using the zone air dry-bulb temperature when rack heat rejection location equals ``Zone'' and the outdoor air dry-bulb temperature when rack heat rejection location equals ``Outdoors'' and the condenser type is air-cooled. As explained below, if the condenser is cooled by evaporative cooling, the curve object is evaluated using an effective temperature. The output from this curve is multiplied by the design condenser fan power to yield the actual fan power at the specific air temperature entering the condenser. This curve must be cubic or quadratic (Curve:Cubic or Curve:Quadratic), and should be normalized to 1.0 at the condenser entering air temperature at which the design condenser fan power occurs. The actual condenser fan power is not allowed to exceed the design condenser fan power defined in the previous input field or go below zero (i.e., the output of the curve object is limited to values from 0.0 to 1.0). If this field is left blank, then the model assumes the condenser fan power is at the design power level when any of the refrigerated cases connected to this rack are operating.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-002}
+
+When the heat rejection location is ``Outdoors'', the condenser may be either cooled by dry air by specifying ``AirCooled'', by wet evaporative cooling by specifying ``EvaporativelyCooled'', or by a water loop by specifying ``WaterCooled''.~ If the condenser type is ``WaterCooled'', then a plant cooling loop will need to be defined using other EnergyPlus objects, e.g., plant loop, pump, cooling tower, etc.~ The default value is ``AirCooled''.
+
+\paragraph{Field: Water-cooled Condenser Inlet Node Name}\label{field-water-cooled-condenser-inlet-node-name}
+
+When the condenser type is ``WaterCooled'', a node name for the water-side condenser inlet must be provided.
+
+\paragraph{Field: Water-cooled Condenser Outlet Node Name}\label{field-water-cooled-condenser-outlet-node-name}
+
+When the condenser type is ``WaterCooled'', a node name for the water-side condenser outlet must be provided.
+
+\paragraph{Field: Water-cooled Loop Flow Type}\label{field-water-cooled-loop-flow-type}
+
+When the condenser type is ``WaterCooled'', the type of flow loop should be specified.~ The two choices are \textbf{VariableFlow}, in which a Pump:VariableSpeed needs to~ be included in the plant loop, or \textbf{ConstantFlow}, in which the loop circuit has a constant flow rate, typically associated with a Pump:ConstantSpeed object.~ If the flow type is VariableFlow, the flow needed to remove the condenser heat energy will be calculated and requested of the pump.~ If the flow type is Constant Flow, the outlet water temperature will be determined based on the fixed loop flow rate and heat energy to be removed.~ The default type is \textbf{VariableFlow}. Refer to additional discussion in the Engineering Reference.
+
+\paragraph{Field: Water-cooled Condenser Outlet Temperature Schedule Name}\label{field-water-cooled-condenser-outlet-temperature-schedule-name}
+
+When the condenser type is ``WaterCooled'', and when the water-cooled loop flow type is ``Variable Flow'', the name of a schedule (Ref: Schedule) that defines the desired condenser water outlet temperature must be provided.~ The schedule may define an outlet temperature that varies through time.
+
+\paragraph{Field: Water-cooled Condenser Design~ Flow Rate}\label{field-water-cooled-condenser-design-flow-rate}
+
+When the condenser type is ``WaterCooled'', and when the water-cooled loop flow type is ``Constant Flow'', this is the design water flow rate in m\(^{3}\)/s that will be requested initially.~ This requested flow will be passed to the loop simulation, and resulting actual flow will be dependent upon supply system capabilities (e.g., pump capability).~ The design flow rate must always be less than the maximum flow rate, defined below.
+
+\paragraph{Field: Water-cooled Condenser Maximum~ Flow Rate}\label{field-water-cooled-condenser-maximum-flow-rate}
+
+When the condenser type is ``Water Cooled'', this is the maximum water flow rate in m\(^{3}\)/s that will be allowed through the condenser.~ When the loop flow type is Variable Flow, if the calculated flow rate is higher than the maximum flow rate, an error message will be generated, and the flow rate will be reset to the maximum flow rate.
+
+\paragraph{Field: Water-cooled Condenser Maximum Water Outlet Temperature}\label{field-water-cooled-condenser-maximum-water-outlet-temperature}
+
+When the condenser type is ``WaterCooled'', this field specifies the maximum allowed water temperature in degrees C leaving the compressor rack condenser. The default value is 55 degrees C.
+
+\paragraph{Field: Water-cooled Condenser Minimum Water Inlet Temperature}\label{field-water-cooled-condenser-minimum-water-inlet-temperature}
+
+When the condenser type is ``WaterCooled'', this field specifies the minimum allowed water temperature in degrees C entering the compressor rack condenser. The default value is 10 degrees C.~ Refer to additional discussion in the Engineering Reference.
+
+\paragraph{Field: Evaporative Condenser Availability Schedule Name}\label{field-evaporative-condenser-availability-schedule-name}
+
+When the condenser type is ``EvaporativelyCooled'', the name of the optional schedule (Ref: Schedule) that specifies the time periods that evaporative cooling is available/unavailable. In some colder climates, evaporative cooling is periodically discontinued and the basin sumps drained to avoid freezing. In these times, the condenser runs as a typical dry air cooled condenser, and related evaporative cooling systems (e.g., water pump, basin heaters) do not operate. Use of this optional schedule permits modeling of planned, seasonal interruptions of evaporative cooling. All schedule values must be greater than or equal to zero. Typically, an ON/OFF schedule type is used with values being either 0 or 1. A schedule value of 1 indicates that evaporative cooling is available during the defined time period, and a value of 0 denotes that evaporative cooling is not available during the defined time period. If the schedule name is omitted (blank) and Condenser Type = ``Evap Cooled'', then the model assumes that evaporative cooling of the condenser is available for the entire simulation period.
+
+\paragraph{Field: Evaporative Condenser Effectiveness}\label{field-evaporative-condenser-effectiveness-001}
+
+When the condenser type is ``EvaporativelyCooled'', this field specifies the effectiveness of the evaporative system in modifying the temperature of the air entering the condenser coil. The resulting effective temperature is determined as
+
+\begin{equation}
+{T_{effective}} = {T_{owb}} + (1 - \varepsilon )*[{T_{odb}} - {T_{owb}}]
+\end{equation}
+
+where:
+
+\({T_{effective}}\) ~~~~~~ = effective dry-bulb temperature of air entering the condenser cooling coil (°C)
+
+\({T_{owb}}\) ~~~~~~~~~~ = outdoor air wet-bulb temperature (°C)
+
+\({T_{odb}}\) ~~~~~~~~~~ = outdoor air dry-bulb temperature (°C)
+
+\(\varepsilon\) ~~~~~~~~~~~~~~ = evaporative condenser effectiveness.
+
+The resulting condenser inlet air temperature is used by the Compressor Rack COP as a Function of Temperature Curve and the Condenser Fan Power as a Function of Temperature Curve. The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0.
+
+If the two function-of-temperature curves (i.e., Compressor Rack COP as a Function of Temperature Curve and Condenser Fan Power as a Function of Temperature Curve) are based on wet-bulb temperature rather than dry-bulb temperature, the evaporative condenser effectiveness should be set to 1.0 for consistency.
+
+\paragraph{Field: Evaporative Condenser Air Flow Rate}\label{field-evaporative-condenser-air-flow-rate-001}
+
+When the condenser type is ``EvaporativelyCooled'', the air volume flow rate, in m\(^{3}\)per second, entering the evaporative condenser. This value is used to calculate the amount of water evaporated when evaporatively cooling the condenser inlet air. The value for this field must be greater than zero. This input field is also autocalculatable, equivalent to 0.000144 m\(^{3}\)/s per watt of total cooling capacity {[}850 cfm/ton{]} where the total cooling capacity is the sum of the rated total cooling capacities for the refrigerated cases connected to this compressor rack (Ref. Refrigeration:Case).
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-003}
+
+When the condenser type is ``EvaporativelyCooled'', this field defines the power level of the basin heater, if applicable, used to avoid water freezing in an outdoor evaporative cooler basin. This numeric field contains the capacity of the electric basin heater in Watts per degree Kelvin. This field is used in conjunction with the Basin Heater Set Point Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the dry-bulb temperature of the condenser coil inlet air. The basin heater only operates when the condenser fan is off (i.e., no compressor heat rejection). The basin heater capacity must be greater than or equal to zero, with a default value of 200 W/K if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-003}
+
+When the condenser type is ``EvaporativelyCooled'', this numeric field contains the set point temperature (°C) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this set point temperature, as long as the condenser fan is off. The default value is 2°C if this field is left blank.
+
+\paragraph{Field: Design Evaporative Condenser Water Pump Power}\label{field-design-evaporative-condenser-water-pump-power}
+
+When the condenser type is ``EvaporativelyCooled'', the rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The value for this field must be greater than or equal to 0, with a default value of 1000 Watts if this field is left blank. This input field is also autocalculatable, equivalent to 0.004266 W per watt {[}15 W/ton{]} of total cooling capacity where the total cooling capacity is the sum of the rated total cooling capacities for the refrigerated cases and walk-ins connected to this compressor rack (Ref. Refrigeration:Case and Refrigeration:WalkIn)).
+
+\paragraph{Field: Evaporative Water Supply Tank Name}\label{field-evaporative-water-supply-tank-name}
+
+When the condenser type is ``EvaporativelyCooled'', this field is used to define where the compressor rack obtains water used for evaporative cooling of its condenser. If this field is left blank, the unit will obtain water directly from the mains (Ref. Water Mains Temperatures). If the name of a Water Storage Tank object is used here, then the unit will obtain its water from that tank.
+
+\paragraph{Field: Condenser Air Inlet Node Name}\label{field-condenser-air-inlet-node-name-000}
+
+This optional alpha field contains the name of the node from which the outdoor compressor rack condenser draws its outdoor air. This field is applicable only when the heat rejection location is ``Outdoors'' (if the heat rejection location is ``Zone'', this field is disregarded). If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, this node name must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-003}
+
+This field allows the specification of a user-defined end-use subcategory (e.g., ``Low Temperature Rack''). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Refrigeration Case Name or WalkIn Name or CaseAndWalkInList Name}\label{field-refrigeration-case-name-or-walkin-name-or-caseandwalkinlist-name}
+
+This alpha field is the name of a single refrigerated case, a single walk in cooler,~ the name of a CaseAndWalkInList for multiple refrigerated cases and/or walk-ins, the name of a refrigeration chiller, or the name of a CaseAndWalkInList for multiple refrigeration chillers connected to this compressor rack. Note that if a CaseAndWalkInList contains the name(s) of refrigeration chillers, it CANNOT have the name(s) or any refrigerated cases or walkins . This field is required.
+
+\paragraph{Field: Heat Rejection Zone Name}\label{field-heat-rejection-zone-name}
+
+If the Heat Rejection Location is ``Zone'' and any walk-in coolers are connected to this compressor rack, then this field is required. The compressor rack heat rejection will impact the air heat balance in this zone.
+
+The following is an example input for a~ Refrigeration Compressor Rack with water cooled condenser.
+
+\begin{lstlisting}
+
+Refrigeration:CompressorRack,
+      MediumTempRack,          !- Name
+      Outdoors,                !- Heat Rejection Location
+      1.7,                     !- Design Compressor Rack COP {W/W}
+      RackCOPfTCurve,          !- Compressor Rack COP as a Function of Temperature Curve Name
+      1025.0,                  !- Design Condenser Fan Power {W}
+      RackCondFanCurve,        !- Condenser Fan Power as a Function of Temperature Curve Name
+      WaterCooled,             !- Condenser Type
+      Condenser Inlet Node,    !- Water-cooled Condenser Inlet Node Name
+      Condenser Outlet Node,   !- Water-cooled Condenser Outlet Node Name
+      VariableFlow,            !- Water-cooled Loop Flow Type
+      Cond Outlet Temp Sch,    !- Water-cooled Condenser Outlet Temperature Schedule Name
+      ,                        !- Water-cooled Condenser Design Flow Rate {m3/s}
+      0.003,                   !- Water-cooled Condenser Maximum Flow Rate {m3/s}
+      55,                      !- Water-cooled Condenser Maximum Water Outlet Temperature {C}
+      ,                        !- Water-cooled Condenser Minimum Water Inlet Temperature {C}
+      ,                        !- Evaporative Condenser Availability Schedule Name
+      ,                        !- Evaporative Condenser Effectiveness {dimensionless}
+      ,                        !- Evaporative Condenser Air Volume Flow Rate {m3/s}
+      ,                        !- Basin Heater Capacity {W/K}
+      ,                        !- Basin Heater Set Point Temperature {C}
+      ,                        !- Design Evaporative Condenser Water Pump Power {W}
+      ,                        !- Evaporative Water Supply Tank Name
+      ,                        !- Condenser Air Inlet Node Name
+      ,                        !- End-Use Subcategory
+      MediumTempCaseList;      !- Refrigeration Case Name or WalkIn Name or CaseAndWalkInList Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-028}
+
+If Condenser Type = Water Cooled:
+
+\begin{itemize}
+\item
+  System,Average, Refrigeration Compressor Rack Condenser Refrigerant Mass Flow Rate {[}kg/s{]}
+\item
+  System,Average, Refrigeration Compressor Rack Condenser Heat Transfer Rate {[}W{]}
+\item
+  System,Sum, Refrigeration Compressor Rack Condenser Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+IF THE RACK SERVES CASES AND/OR WALKINS:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration Compressor Rack Electric Power {[}W{]}
+\item
+  Zone,Sum, Refrigeration Compressor Rack Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Compressor Rack Condenser Fan Electric Power {[}W{]}
+\item
+  Zone,Sum, Refrigeration Compressor Rack Condenser Fan Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Compressor Rack Total Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Compressor Rack Total Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Compressor Rack COP {[}W/W{]}
+\end{itemize}
+
+If Condenser Type = Evap Cooled:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration Compressor Rack Evaporative Condenser Pump Electric Power {[}W{]}
+\item
+  Zone,Sum, Refrigeration Compressor Rack Evaporative Condenser Pump Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Compressor Rack Evaporative Condenser Basin Heater Electric Power {[}W{]}
+\item
+  Zone,Sum, Refrigeration Compressor Rack Evaporative Condenser Basin Heater Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Compressor Rack Evaporative Condenser Water Volume Flow Rate {[}m\(^{3}\)/s{]}
+\item
+  Zone,Sum, Refrigeration Compressor Rack Evaporative Condenser Water Volume {[}m\(^{3}\){]}
+\end{itemize}
+
+If Heat Rejection Location = Zone:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration Compressor Rack Zone Sensible Heating Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Compressor Rack Zone Sensible Heating Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Compressor Rack Return Air Sensible Heating Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Compressor Rack Return Air Sensible Heating Energy {[}J{]}
+\end{itemize}
+
+IF THE RACK SERVES REFRIGERATION CHILLERS
+
+\begin{itemize}
+\item
+  HVAC,Average, Refrigeration Air Chiller Compressor Rack Electric Power {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller Compressor Rack Electric Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Compressor Runtime Fraction {[]}
+\item
+  HVAC,Average, Refrigeration Air Chiller Compressor Rack Condenser Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller Compressor Rack Condenser Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller Compressor Rack Total Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller Compressor Rack Total Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller Compressor Rack COP {[}W/W{]}
+\end{itemize}
+
+If Condenser Type = Evap Cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average, Refrigeration Air Chiller Compressor Rack Evaporative Condenser Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller Compressor Rack Evaporative Condenser Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller Compressor Rack Evaporative Condenser Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller Compressor Rack Electric PowerRefrigeration Air Chiller Compressor Rack Evaporative Condenser Basin Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller Compressor Rack Evaporative Condenser Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller Compressor Rack Evaporative Condenser Water Volume {[}m3{]}
+\end{itemize}
+
+If Heat Rejection Location = Zone:
+
+\begin{itemize}
+\item
+  HVAC,Average, Refrigeration Air Chiller Compressor Rack Zone Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Air Chiller Compressor Rack Zone Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller Compressor Rack Return Air Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Air Chiller Compressor Rack Return Air Sensible Heating Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Refrigeration Compressor Rack Condenser Mass Flow Rate {[}kg/s{]}}\label{refrigeration-compressor-rack-condenser-mass-flow-rate-kgs}
+
+When condenser type is Water Cooled, this is the mass flow rate of water flowing through the water cooled condenser.
+
+\paragraph{Refrigeration Compressor Rack Condenser Heat Transfer Rate {[}W{]}}\label{refrigeration-compressor-rack-condenser-heat-transfer-rate-w}
+
+When condenser type is Water Cooled, this is the total heat transfer across the condenser (i.e., compressor energy and case cooling).
+
+\paragraph{Refrigeration Compressor Rack Condenser Heat Transfer Energy {[}J{]}}\label{refrigeration-compressor-rack-condenser-heat-transfer-energy-j}
+
+When condenser type is Water Cooled, this is the total heat energy flowing across the condenser for the timestep being reported.
+
+\paragraph{IF THE RACK SERVES CASES AND OR WALKINS:}\label{if-the-rack-serves-cases-and-or-walkins}
+
+\paragraph{Refrigeration Compressor Rack Electric Power {[}W{]}}\label{refrigeration-compressor-rack-electric-power-w}
+
+This output is the electric power input to the rack compressor(s) in Watts.
+
+\paragraph{Refrigeration Compressor Rack Electric Energy {[}J{]}}\label{refrigeration-compressor-rack-electric-energy-j}
+
+This is the electricity consumption of the rack compressor(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Refrigeration Compressor Runtime Fraction {[]}}{Refrigeration Compressor Runtime Fraction }}\label{refrigeration-compressor-runtime-fraction}
+
+This is the runtime operating ratio for the compressor.
+
+\paragraph{Refrigeration Compressor Rack Condenser Fan Electric Power {[}W{]}}\label{refrigeration-compressor-rack-condenser-fan-electric-power-w}
+
+This output is the electric input to the rack condenser fan(s) in Watts.
+
+\paragraph{Refrigeration Compressor Rack Condenser Fan Electric Energy {[}J{]}}\label{refrigeration-compressor-rack-condenser-fan-electric-energy-j}
+
+This is the electricity consumption of the rack condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Compressor Rack Total Heat Transfer Rate {[}W{]}}\label{refrigeration-compressor-rack-total-heat-transfer-rate-w}
+
+This output is the total heat transfer rate of the~ refrigeration compressor rack in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases and walk-ins that are connected to this rack. This value does not include compressor or condenser fan heat.
+
+\paragraph{Refrigeration Compressor Rack Total Heat Transfer Energy {[}J{]}}\label{refrigeration-compressor-rack-total-heat-transfer-energy-j}
+
+This is the total heat transfer of the~ refrigeration compressor rack in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Compressor Rack COP {[}W/W{]}}\label{refrigeration-compressor-rack-cop-ww}
+
+This field is the~ refrigeration compressor rack coefficient of performance. It is the actual compressor rack COP for the timestep being reported, accounting for the COP variation as a function of temperature. It is calculated as the Design Compressor Rack COP times the Compressor Rack COP as a Function of Temperature Curve evaluated at the effective condenser entering air temperature for the timestep being reported.
+
+\paragraph{Refrigeration Compressor Rack Evaporative Condenser Pump Electric Power {[}W{]}}\label{refrigeration-compressor-rack-evaporative-condenser-pump-electric-power-w}
+
+This is the electrical power requirement in Watts for the timestep being reported for the water pump used with evaporative cooling of the compressor rack condenser.
+
+\paragraph{Refrigeration Compressor Rack Evaporative Condenser Pump Electric Energy {[}J{]}}\label{refrigeration-compressor-rack-evaporative-condenser-pump-electric-energy-j}
+
+This is the electricity consumption in Joules of the water pump used with evaporative cooling of the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Compressor Rack Evaporative Condenser Basin Heater Electric Power {[}W{]}}\label{refrigeration-compressor-rack-evaporative-condenser-basin-heater-electric-power-w}
+
+This is the electrical power requirement in Watts for the timestep being reported for the water heater in the basin of the evaporative system used to cool the compressor rack condenser.
+
+\paragraph{Refrigeration Compressor Rack Evaporative Condenser Basin Heater Electric Energy {[}J{]}}\label{refrigeration-compressor-rack-evaporative-condenser-basin-heater-electric-energy-j}
+
+This is the electricity consumption in Joules of the water heater used to prevent freezing of the evaporative cooling system for the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Compressor Rack Evaporative Condenser Water Volume Flow Rate {[}m3/s{]}}\label{refrigeration-compressor-rack-evaporative-condenser-water-volume-flow-rate-m3s}
+
+The volumetric flow rate in m\(^{3}\)/s of water consumed while providing evaporative cooling of the compressor rack condenser.
+
+\paragraph{Refrigeration Compressor Rack Evaporative Condenser Water Volume {[}m3{]}}\label{refrigeration-compressor-rack-evaporative-condenser-water-volume-m3}
+
+This is the water consumed by evaporation in m\(^{3}\) while providing evaporative cooling of the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Water, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Compressor Rack Zone Sensible Heating Rate {[}W{]}}\label{refrigeration-compressor-rack-zone-sensible-heating-rate-w}
+
+This field is the rate of sensible heating in Watts provided to the zone by condenser waste heat rejection, which impacts the zone air heat balance.
+
+\paragraph{Refrigeration Compressor Rack Zone Sensible Heating Energy {[}J{]}}\label{refrigeration-compressor-rack-zone-sensible-heating-energy-j}
+
+This field is the sensible heating energy in Joules provided to the zone by condenser waste heat rejection for the timestep being reported.
+
+\paragraph{Refrigeration Compressor Rack Return Air Sensible Heating Rate {[}W{]}}\label{refrigeration-compressor-rack-return-air-sensible-heating-rate-w}
+
+This field is the rate of sensible heating in Watts provided by condenser waste heat rejection to the HVAC return air (zone return air path outlet node), which impacts the HVAC return air temperature. If the HVAC system is off for a simulation timestep (no return air mass flow), then this sensible heating is actually provided to the zone air instead (even though a non-zero value is reported here).
+
+\paragraph{Refrigeration Compressor Rack Return Air Sensible Heating Energy {[}J{]}}\label{refrigeration-compressor-rack-return-air-sensible-heating-energy-j}
+
+This field is the sensible heating energy in Joules provided by condenser waste heat rejection to the HVAC return air (zone return air path outlet node) for the timestep being reported. If the HVAC system is off for a simulation timestep (no return air mass flow), then this sensible heating is actually provided to the zone air instead (even though a non-zero value is reported here).
+
+\paragraph{IF THE RACK SERVES CHILLERS}\label{if-the-rack-serves-chillers}
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Electric Power {[}W{]}}\label{refrigeration-air-chiller-compressor-rack-electric-power-w}
+
+This output is the electric power input to the rack compressor(s) in Watts.
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Electric Energy {[}J{]}}\label{refrigeration-air-chiller-compressor-rack-electric-energy-j}
+
+This is the electricity consumption of the rack compressor(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Refrigeration Air Chiller System Compressor Runtime Fraction {[]}}{Refrigeration Air Chiller System Compressor Runtime Fraction }}\label{refrigeration-air-chiller-system-compressor-runtime-fraction}
+
+This is the runtime fraction for the compressor serving air chillers.
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Condenser Fan Electric Power {[}W{]}}\label{refrigeration-air-chiller-compressor-rack-condenser-fan-electric-power-w}
+
+This output is the electric input to the rack condenser fan(s) in Watts.
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Condenser Fan Electric Energy {[}J{]}}\label{refrigeration-air-chiller-compressor-rack-condenser-fan-electric-energy-j}
+
+This is the electricity consumption of the rack condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Total Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-compressor-rack-total-heat-transfer-rate-w}
+
+This output is the total heat transfer rate of the ~refrigeration compressor rack in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases and walk-ins that are connected to this rack. This value does not include compressor or condenser fan heat.
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Total Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-compressor-rack-total-heat-transfer-energy-j}
+
+This is the total heat transfer of the~ refrigeration compressor rack in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller Compressor Rack COP {[}W/W{]}}\label{refrigeration-air-chiller-compressor-rack-cop-ww}
+
+This field is the~ refrigeration compressor rack coefficient of performance. It is the actual compressor rack COP for the timestep being reported, accounting for the COP variation as a function of temperature. It is calculated as the Design Compressor Rack COP times the Compressor Rack COP as a Function of Temperature Curve evaluated at the effective condenser entering air temperature for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Evaporative Condenser Pump Electric Power {[}W{]}}\label{refrigeration-air-chiller-compressor-rack-evaporative-condenser-pump-electric-power-w}
+
+This is the electrical power requirement in Watts for the timestep being reported for the water pump used with evaporative cooling of the compressor rack condenser.
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Evaporative Condenser Pump Electric Energy {[}J{]}}\label{refrigeration-air-chiller-compressor-rack-evaporative-condenser-pump-electric-energy-j}
+
+This is the electricity consumption in Joules of the water pump used with evaporative cooling of the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Evaporative Condenser Basin Heater Electric Power {[}W{]}}\label{refrigeration-air-chiller-compressor-rack-evaporative-condenser-basin-heater-electric-power-w}
+
+This is the electrical power requirement in Watts for the timestep being reported for the water heater in the basin of the evaporative system used to cool the compressor rack condenser.
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Evaporative Condenser Basin Heater Electric Energy {[}J{]}}\label{refrigeration-air-chiller-compressor-rack-evaporative-condenser-basin-heater-electric-energy-j}
+
+This is the electricity consumption in Joules of the water heater used to prevent freezing of the evaporative cooling system for the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Refrigeration Air Chiller Compressor Rack Evaporative Condenser Water Volume Flow Rate {[}m\(^{3}\)/s{]}}{Refrigeration Air Chiller Compressor Rack Evaporative Condenser Water Volume Flow Rate {[}m\^{}\{3\}/s{]}}}\label{refrigeration-air-chiller-compressor-rack-evaporative-condenser-water-volume-flow-rate-m3s}
+
+The volumetric flow rate in m\(^{3}\)/s of water consumed while providing evaporative cooling of the compressor rack condenser.
+
+\paragraph{\texorpdfstring{Refrigeration Air Chiller Compressor Rack Evaporative Condenser Water Volume {[}m\(^{3}\){]}}{Refrigeration Air Chiller Compressor Rack Evaporative Condenser Water Volume {[}m\^{}\{3\}{]}}}\label{refrigeration-air-chiller-compressor-rack-evaporative-condenser-water-volume-m3}
+
+This is the water consumed by evaporation in m\(^{3}\) while providing evaporative cooling of the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Water, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Zone Sensible Heating Rate {[}W{]}}\label{refrigeration-air-chiller-compressor-rack-zone-sensible-heating-rate-w}
+
+This field is the rate of sensible heating in Watts provided to the zone by condenser waste heat rejection, which impacts the zone air heat balance.
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Zone Sensible Heating Energy {[}J{]}}\label{refrigeration-air-chiller-compressor-rack-zone-sensible-heating-energy-j}
+
+This field is the sensible heating energy in Joules provided to the zone by condenser waste heat rejection for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Return Air Sensible Heating Energy {[}J{]}}\label{refrigeration-air-chiller-compressor-rack-return-air-sensible-heating-energy-j}
+
+\paragraph{Refrigeration Air Chiller Compressor Rack Return Air Sensible Heating Rate {[}W{]}}\label{refrigeration-air-chiller-compressor-rack-return-air-sensible-heating-rate-w}
+
+These are the sensible heating energy, in Joules or Watts, provided to the HVAC system return air node by condenser heat rejection at the compressor rack.
+
+\subsection{Refrigeration:Case}\label{refrigerationcase}
+
+The Refrigeration Case object works in conjunction with a compressor rack, a refrigeration system, or a secondary loop object (Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem) to simulate the performance of a refrigerated case system. The refrigerated case model uses performance information at rated conditions along with performance curves for latent case credits and defrost heat load to determine performance at off-rated conditions. Energy use for lights, fans and anti-sweat heaters is modeled based on inputs for nominal power, schedules, and control type. The refrigerated case model accounts for the sensible and latent heat exchange with the surrounding environment (termed ``case credits'') which impacts the temperature and humidity in the zone where the case is located.
+
+\textbf{\emph{A dataset has been provided containing refrigerated case input data for a large number of refrigerated cases from multiple manufacturers. See RefrigerationCases.idf.}}
+
+The Refrigeration Case object inputs include a case name, an availability schedule name, the zone name for the location of the case, and the temperature and relative humidity of the ambient (zone) air surrounding the refrigerated case at the rating conditions for case performance. Additional inputs include the total cooling capacity, latent heat ratio, and run time fraction of the refrigerated case at rated conditions. The case length and operating temperature (average temperature of air/products within the case) must also be specified.
+
+The refrigerated case model requires two curves to describe performance at off-rated conditions (i.e., at different zone temperature and humidity levels): the latent case credit curve and the defrost energy correction curve. The user must enter cubic performance curves with the independent variable being user selectable (case temperature, zone relative humidity, or zone dewpoint temperature).
+
+The user can select from eight case defrost types, with additional inputs being required depending on the type selected. The user must enter a defrost schedule (unless Case Defrost Type = None), and an optional defrost drip-down schedule can be specified to allow additional time for melted frost to drain from the cooling coil following the regular defrost period.
+
+Inputs are required for case fans, lights, and anti-sweat heaters. Case lighting can be controlled by the user through entering a schedule. The case fans operate whenever the cooling coil is operating and during defrost periods for certain case defrost types. Anti-sweat heater power can be controlled by several methods which are user selectable. The model assumes that the fans are contained within the thermal envelope of the case and provide a direct heat load on the case cooling coil. For lighting and anti-sweat heaters, the user can specify the fraction of their respective heat loads that directly impact the case cooling coil (with the remainder of their heat load impacting the surrounding zone air).
+
+The user has the option of specifying a case restocking schedule and a schedule for modifying the case credits if needed. Finally, the user can specify the under case HVAC return air fraction which determines the portion of the case credits that directly impact the HVAC return air conditions (with the remainder of the case credits impacting the zone sensible and latent loads).
+
+\subsubsection{Inputs}\label{inputs-1-036}
+
+\paragraph{Field: Name}\label{field-name-1-035}
+
+A unique user-assigned name for an instance of a refrigerated case. Any reference to this case by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-014}
+
+The name of the schedule (ref: Schedule) that denotes whether the refrigerated case can operate during a given time period. A schedule value greater than 0 (maximum schedule value of 1.0 is typically used) indicates that the case will operate during a given time period. A value equal to 0 denotes that the case does not operate (everything is OFF: refrigeration, fans, lights, anti-sweat, etc.). Typically the refrigerated case will operate throughout the day (i.e., the schedule will contain 1 for all time periods); however, cases require maintenance and/or cleaning and this can be modeled accordingly using this schedule if desired. If this field is left blank, the case is assumed to be available at all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-010}
+
+The name of the zone where the refrigerated case is located. The refrigerated case will impact the air heat balance in this zone. When modeling multiple refrigerated cases connected to a single compressor rack where the condenser heat is rejected to the zone (ref: Refrigeration:CompressorRack), \textbf{all} of the refrigerated cases connected to that compressor rack must be located in the same zone.
+
+\paragraph{Field: Rated Ambient Temperature}\label{field-rated-ambient-temperature}
+
+Dry-bulb temperature of the ambient (zone) air surrounding the refrigerated case at the rating conditions for refrigerated case performance. The default value for this field is 23.9ËšC (75ËšF). This temperature must be greater than 0ËšC and greater than the case operating temperature.
+
+\paragraph{Field: Rated Ambient Relative Humidity}\label{field-rated-ambient-relative-humidity}
+
+Relative humidity of the ambient (zone) air surrounding the refrigerated case at the rating conditions for refrigerated case performance. The default value for this field is 55\% RH.
+
+\paragraph{Field: Rated Total Cooling Capacity per Unit Length}\label{field-rated-total-cooling-capacity-per-unit-length}
+
+The total, full load cooling capacity (sensible plus latent) in watts per unit length of refrigerated case (W/m) at rated conditions (i.e., at the Rated Ambient Temperature, Rated Ambient Relative Humidity, Case Operating Temperature, and with the Standard Case Fan Power per Unit Length and the Standard Case Lighting Power per Unit Length). The value entered for this field must be greater than zero, with a default value of 1900 W/m if the field is blank.
+
+\paragraph{Field: Rated Latent Heat Ratio}\label{field-rated-latent-heat-ratio}
+
+The latent heat ratio (LHR = latent capacity divided by total cooling capacity) of the refrigerated case at rated conditions (i.e., at the Rated Ambient Temperature, Rated Ambient Relative Humidity, Case Operating Temperature, and with the Standard Case Fan Power per Unit Length and the Standard Case Lighting Power per Unit Length). The value for this field can range from zero to 1.0, with a default value of 0.3 if the field is blank.
+
+\paragraph{Field: Rated Runtime Fraction}\label{field-rated-runtime-fraction}
+
+The runtime fraction of the refrigerated case at rated conditions (i.e., at the Rated Ambient Temperature, Rated Ambient Relative Humidity, and Case Operating Temperature). Even at rated conditions, refrigerated cases typically include additional cooling capacity to account for product stocking and recovery from defrost. The rated runtime fraction for refrigerated cases typically ranges from 0.8 to 0.9. The entered value for this field must be greater than 0.0 and less than or equal to 1.0, and the default value is 0.85 if the field is blank.
+
+\paragraph{Field: Case Length}\label{field-case-length}
+
+The length of the refrigerated case in meters. The entered value for this field must be greater than 0.0, and the default value is 3 meters if the field is blank.
+
+\paragraph{Field: Case Operating Temperature}\label{field-case-operating-temperature}
+
+The average temperature of the air and products within the refrigerated case in ËšC. The refrigerated case manufacturer typically provides this information in the product literature. Typical operating temperatures for medium temperature cases are 1.6ËšC to 7.2ËšC (35ËšF to 45ËšF). Typical operating temperatures for low temperatures cases are -28.9ËšC to -17.8ËšC~~~~~~~ (-20ËšF to 0ËšF). The entered value for this field must be less than 20ËšC and lower than the Rated Ambient Temperature. The default value is 1.1ËšC if the field is blank.
+
+\paragraph{Field: Latent Case Credit Curve Type}\label{field-latent-case-credit-curve-type}
+
+This alpha field defines the form of the curve used to modify the latent case credits (latent heat removed from the zone where the refrigerated case is located) at off-rated conditions. The valid choices for this field are:
+
+\begin{itemize}
+\tightlist
+\item
+  CaseTemperatureMethod
+\end{itemize}
+
+This method defines the variation in latent case credits as a cubic function of Case Operating Temperature. The result from the cubic curve is multiplied by the difference between the rated ambient relative humidity and the actual zone relative humidity, and one minus this value is multiplied by the Rated LHR to give the operating LHR at the actual zone humidity condition. (Representative cooefficient values for single-shelf horizontal and multi-shelf vertical display cases are given in the EnergyPlus Engineering Reference.)
+
+\begin{itemize}
+\tightlist
+\item
+  RelativeHumidityMethod
+\end{itemize}
+
+This method defines the variation in latent case credits as a cubic function of ambient (zone) air relative humidity.
+
+\begin{itemize}
+\tightlist
+\item
+  DewpointMethod
+\end{itemize}
+
+This method defines the variation in latent case credits as a cubic function of ambient (zone) air dewpoint temperature.
+
+The default curve type is the Case Temperature Method. Refer to the Engineering Reference for further information on how latent case credits are modeled.
+
+\paragraph{Field: Latent Case Credit Curve Name}\label{field-latent-case-credit-curve-name}
+
+The name of a \textbf{cubic} performance curve (ref: Performance Curves) that parameterizes the variation of the latent case credits at off-rated conditions. The curve should be normalized to have a value of 1.0 at the rated ambient air conditions defined above.
+
+\paragraph{Field: Standard Case Fan Power per Unit Length}\label{field-standard-case-fan-power-per-unit-length}
+
+The total standard fan power in Watts per unit length of refrigerated case (W/m). This value represents the fan power included in the field Rated Total Cooling Capacity per Unit Length, and is used to determine the sensible case credits. The entered value for this field must be greater than or equal to zero, and the default value is 75.0 W/m if the field is blank.
+
+\paragraph{Field: Operating Case Fan Power per Unit Length}\label{field-operating-case-fan-power-per-unit-length}
+
+The total operating fan power in Watts per unit length of refrigerated case (W/m). Enter the actual power for the installed fans. The entered value for this field must be greater than or equal to zero, and the value is set equal to the standard case fan powers if the field is blank.
+
+\paragraph{Field: Standard Case Lighting Power per Unit Length}\label{field-standard-case-lighting-power-per-unit-length}
+
+The total standard lighting power in Watts per unit length of refrigerated case (W/m). This value should represent the lighting power provided by the case manufacturer and included in the ``Rated Total Cooling Capacity per Unit Length'' field and is used to determine the sensible case credits. For cases where the manufacturer does not include the lights in the Rated Total Cooling Capacity, this value should be zero (0.0). The entered value for this field must be greater than or equal to zero, and the default value is 90.0 W/m if the field is blank.
+
+\paragraph{Field: Installed Case Lighting Power per Unit Length}\label{field-installed-case-lighting-power-per-unit-length}
+
+The total installed lighting power in Watts per unit length of refrigerated case (W/m). Enter the actual power for the installed lights. This number may be greater or less than the standard lighting power value, depending upon the manufacturer's practice in specifying the case rated cooling capacity and whether or not energy-efficient lights are being modeled.~ The next field (i.e.~Case Lighting Schedule Name) may be used to specify the name of a schedule that contains the fraction of the Installed Case Lighting Power per Unit Length to be modeled for each timestep of the simulation period. The entered value for this field must be greater than or equal to zero, and the value is set equal to the standard case lighting power if the field is blank.
+
+\paragraph{Field: Case Lighting Schedule Name}\label{field-case-lighting-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes the fraction of installed refrigerated case lights that operate during a given time period. A schedule value greater than 0 indicates that the lights will operate during that time period (maximum schedule value of 1.0 means lights are fully on at the Installed Case Lighting Power per Unit Length level). A schedule value of zero denotes that the lights are off. The refrigerated case lights will typically operate only when the store is open for business and can be scheduled off as desired via this schedule. If this field is left blank, the default schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Fraction of Lighting Energy To Case}\label{field-fraction-of-lighting-energy-to-case}
+
+The fraction of the lighting energy that directly contributes to the case heat load. The remainder of the lighting energy (1 -- fraction) is a heating load to the zone where the case is located. This field can be used to model lighting ballasts and bulbs located outside the air curtain of the refrigerated case. The value for this field can range from zero to 1.0, with a default value of 1.0 if the field is blank.
+
+\paragraph{Field: Case Anti-Sweat Heater Power per Unit Length}\label{field-case-anti-sweat-heater-power-per-unit-length}
+
+The electric anti-sweat heater power in watts per unit length of refrigerated case (W/m). The entered value for this field must be greater than or equal to zero, and the default value is 0 W/m if the field is blank.
+
+\paragraph{Field: Minimum Anti-Sweat Heater Power per Unit Length}\label{field-minimum-anti-sweat-heater-power-per-unit-length}
+
+The minimum electric anti-sweat heater power in watts per unit length of refrigerated case (W/m). Anti-sweat heater power will remain at or above this value for anti-sweat heater control types linear, dewpoint method, or heat balance method. Other anti-sweat heater control types disregard this field. The entered value for this field must be greater than or equal to zero, and the default value is 0 W/m if the field is blank.
+
+\paragraph{Field: Anti-Sweat Heater Control Type}\label{field-anti-sweat-heater-control-type}
+
+The type of anti-sweat heater control used for this refrigerated case. Valid choices are None, Constant, Linear, DewpointMethod, or HeatBalanceMethod. The default is None if the field is blank. Refer to the Engineering Reference for further information on how the different anti-sweat heater controls are modeled.
+
+\paragraph{Field: Humidity at Zero Anti-Sweat Heater Energy}\label{field-humidity-at-zero-anti-sweat-heater-energy}
+
+The value of this numeric field is only used when the Linear anti-sweat heater control type is selected. Enter the zone relative humidity where anti-sweat heater energy use is zero. Negative values for relative humidity may be entered. Other anti-sweat heater control types disregard this field. The value entered for this field must be less than the Rated Ambient Relative Humidity specified above. The default for this field is -10.0.
+
+\paragraph{Field: Case Height}\label{field-case-height}
+
+The value of this numeric field is used when Heat Balance Method anti-sweat heater control is selected. Enter the case height in meters. Other anti-sweat heater control types disregard this field. The entered value for this field must be greater than zero when Heat Balance Method anti-sweat heater control is selected, and the default value is 1.5 meters if the field is blank.
+
+\paragraph{Field: Fraction of Anti-Sweat Heater Energy To Case}\label{field-fraction-of-anti-sweat-heater-energy-to-case}
+
+This value denotes the fraction of anti-sweat heater energy that results in a direct heat load to the refrigerated case. The remainder of the anti-sweat heater energy (1-fraction) is a heating load to the zone where the refrigerated case is located. The value for this field can range from zero to 1.0, with a default value of 1.0 if the field is blank.
+
+\paragraph{Field: Case Defrost Power per Unit Length}\label{field-case-defrost-power-per-unit-length}
+
+The defrost power in watts per unit length of refrigerated case (W/m). This input is required for hot-gas, hot-fluid, or electric defrost types and is used to evaluate the load on the case as well as power or heat consumption. Refrigerated case manufacturers do not typically provide information on the heat input for hot-gas and hot-fluid defrost. Information provided for electric defrost power can be substituted here for refrigerated cases using hot-gas or hot-fluid defrost if other information is not available. Only electric Case Defrost Types consume electricity during the defrost period. The entered value for this field must be greater than or equal to zero, and the default value is 0 W/m if the field is blank.
+
+\paragraph{Field: Case Defrost Type}\label{field-case-defrost-type}
+
+The type of defrost used for this refrigerated case. Valid choices are None, OffCycle, HotGas, HotGaswithTemperatureTermination, Electric, ElectricwithTemperatureTermination, HotFluid, and HotFluidwithTemperatureTermination. The default defrost type is OffCycle if the field is blank. Refer to the Engineering Reference for further information on how the different case defrost types are modeled. In particular, hot-fluid defrost systems may be effective with much shorter defrost times than other systems, which should be reflected in the defrost and drip-down schedules.
+
+\paragraph{Field: Case Defrost Schedule Name}\label{field-case-defrost-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes whether the refrigerated case requires defrosting. A schedule value of 1.0 indicates that defrost will be on during a given time period. A value equal to 0 denotes that the defrost is off. Defrost schedules normally repeat the duration and number of defrost cycles for each day of the year. The refrigerated case manufacturer typically provides this information with the product literature. The use of Compact Schedules (ref. Schedules) are ideal for this purpose. In a typical supermarket with many cases, it is important to diversify the defrost schedules in order to avoid large swings in the load placed upon the remainder of the refrigeration system.
+
+\paragraph{Field: Case Defrost Drip-Down Schedule Name}\label{field-case-defrost-drip-down-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes whether the refrigerated case requires additional time for draining condensate after the defrost period. A schedule value of 1.0 indicates that the defrost drip-down period is on during a given time period. A value equal to 0 denotes that the defrost drip-down period is over. The refrigerated case manufacturer typically provides this information with the product literature.
+
+Each defrost drip-down period specified in this schedule should start at the same time as the corresponding defrost period specified in the schedule for Case Defrost Schedule, and the drip-down schedule defrost period should always be longer than or equal to the length of the defrost schedule time period. For example, if the case defrost schedule contains a defrost period from 7:00 to 7:15, you would specify a case defrost drip-down period from 7:00 to 7:20 if you wanted to model a 5 minute condensate drip-down period after the regular defrost period. If no drip-down schedule is entered, then the case defrost schedule (specified for the previous input field) will be used. The use of Compact Schedules (ref. Schedules) are ideal for this purpose.
+
+\paragraph{Field: Defrost Energy Correction Curve Type}\label{field-defrost-energy-correction-curve-type}
+
+This alpha field defines the form of the correction curve used to modify the defrost energy use (and the associated load on the case cooling coil) at off-rated conditions. The valid choices for this field are:
+
+\begin{itemize}
+\tightlist
+\item
+  None
+\end{itemize}
+
+This choice specifies that a defrost energy correction curve will not be used.
+
+\begin{itemize}
+\tightlist
+\item
+  CaseTemperatureMethod
+\end{itemize}
+
+This method defines the variation in defrost energy as a cubic function of Case Operating Temperature. The result from the cubic curve is multiplied by the difference between the rated ambient relative humidity and the actual zone relative humidity, and one minus this value is multiplied by the Case Defrost Power to give the (average) operating defrost power at the actual zone humidity condition. (Representative cooefficient values for single-shelf horizontal and multi-shelf vertical display cases are given in the EnergyPlus Engineering Reference.)
+
+\begin{itemize}
+\tightlist
+\item
+  RelativeHumidityMethod
+\end{itemize}
+
+This method defines the variation in defrost energy as a cubic function of ambient (zone) air relative humidity.
+
+\begin{itemize}
+\tightlist
+\item
+  DewpointMethod
+\end{itemize}
+
+This method defines the variation in defrost energy as a cubic function of ambient (zone) air dewpoint temperature.
+
+The default curve type is None. The methods described here (e.g.~Case Temperature, Relative Humidity, and Dewpoint) are applicable only to Electric with Temperature Termination, Hot-Gas with Temperature Termination, and Hot-Brine with Temperature Termination case defrost types. Refer to the Engineering Reference for further information on how the defrost energy correction types are modeled.
+
+\paragraph{Field: Defrost Energy Correction Curve Name}\label{field-defrost-energy-correction-curve-name}
+
+The name of a \textbf{cubic} performance curve (ref: Performance Curves) that parameterizes the variation of the defrost energy (and the associated load on the case cooling coil) at off-rated conditions. The curve should be normalized to have the value of 1.0 at the rated ambient air conditions defined above. The defrost energy correction curve name is used only for the Electric with Temperature Termination, Hot-Gas with Temperature Termination, and Hot-Brine with Temperature Termination case defrost types.
+
+\paragraph{Field: Under Case HVAC Return Air Fraction}\label{field-under-case-hvac-return-air-fraction}
+
+This field denotes the fraction of HVAC system (air loop) return air that passes beneath the refrigerated case, if any. At times it is necessary to design HVAC systems with under case returns to avoid overcooling the area around the refrigerated case, thus providing a more comfortable environment for the zone occupants. This return air fraction affects the portion of the case credits (sensible and latent) that are applied to the air returning to the HVAC system, while the remainder of the case credits directly impacts the zone air heat balance. Refer to the Engineering Reference for further information on how this is modeled. The sum of the Under Case HVAC Return Air Fractions for all refrigerated cases located in a single zone must be less than or equal to 1.0. The value for this field can range from zero to 1.0, with a default value of 0 if the field is blank.
+
+\paragraph{Field: Refrigerated Case Restocking Schedule Name}\label{field-refrigerated-case-restocking-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes whether the refrigerated case is being restocked with product. The schedule should contain values in units of Watts per unit length of refrigerated case (W/m). This field can be used to denote the additional load imposed on the refrigerated case from stocking the case with product that is warmer than the refrigerated case temperature. This information is difficult to find and may require additional research for proper modeling; however, this schedule is available for this purpose if desired. If restocking of the refrigerated case will not be simulated, enter a schedule with values of zero for all time periods or leave this field blank.
+
+\paragraph{Field: Case Credit Fraction Schedule Name}\label{field-case-credit-fraction-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes a fraction of both the sensible and latent case credits to be applied to the zone and/or the HVAC system return air. Schedule values must be from 0 to 1. This allows correction of the case credits for various refrigerated case types. For instance, if glass door refrigerated display cases are installed in a store that is operated 12 hours per day, then the doors will remain closed during the unoccupied times and would therefore reduce the sensible and latent case credits during the unoccupied time. Leaving this field blank will result in no case credit fraction being applied during the simulation.
+
+\paragraph{Field: Design Evaporator Temperature or Brine Inlet Temperature}\label{field-design-evaporator-temperature-or-brine-inlet-temperature}
+
+The value of this numeric field is used only with the detailed refrigeration system and is not read for the compressor-rack system. For the refrigeration system, it is used to evaluate compressor performance and is also used when the evaporator pressure and temperature are allowed to float at loads less than the design load. If the case is cooled by a secondary system (ref: Refrigeration:SecondarySystem), this value is the brine inlet temperature. The minimum value is -70C and the maximum value is 40C.~ The default value is 5C less than the case temperature.
+
+\paragraph{Field: Average Refrigerant Charge Inventory}\label{field-average-refrigerant-charge-inventory}
+
+The value of this optional field is the refrigerant inventory present in the refrigerated case during ordinary operation. The value is used to produce an estimate of the total refrigerant present in the refrigeration system. The value is entered in kg/m.
+
+The following is an example input for a refrigerated case.
+
+\begin{lstlisting}
+
+ Refrigeration:Case,
+    Multi-Deck Dairy/Deli Merchandiser with Synergy-E,  !- Name [Based on Hill Phoenix 6DMLH-NRG]
+    ,   !- Availability Schedule [Used to turn case on/off including all power draws (ie fans, lights, etc)]
+    UserProvideZoneName,    !- Zone Name [Location of Fixture]
+    23.89,                  !- Rated Ambient Temperature {C}  [75øF]
+    55,                     !- Rated Ambient Relative Humidity {percent}
+    1394,         !- Rated Total Cooling Capacity per Unit length {W/m}  [1,450 Btu/hr/ft = 11,600 Btu/hr]
+    0.30,                   !- Rated Latent Heat Ratio  [ Rated Latent Capacity]
+    0.85,                   !- Rated Runtime Fraction
+    2.4,                    !- Case Length {m}  [8 ft]
+    3.33,                   !- Case Operating Temperature {C}  [38øF]
+    CaseTemperatureMethod,  !- Latent Case Credit Curve Type
+    Multi_Shelf_Vertical_Latent_Case_Credit_Curve,            !- Latent Case Credit Curve Name
+    27.3,                   !- Standard Case Fan Power per Unit Length {W/m}  [8.3 W/ft]
+    27.3,                   !- Operating Case Fan Power per Unit Length {W/m}  [8.3 W/ft = 67 W]
+    0.0,                    !- Standard Case Lighting Power per Unit Length {W/m}  [0.0 W/ft]
+    114.8,                  !- Installed Case Lighting Power per Unit Length {W/m}  [35.0 W/ft = 280 W]
+    ,                       !- Case Lighting Schedule Name
+    1.0,                    !- Fraction Of Lighting Energy To Case
+    0.0,                    !- Case Anti-Sweat Heater Power per Unit Length {W/m}  [0.0 W/ft = 0 W]
+    ,                       !- Minimum Anti-Sweat Heater Power per Unit Length {W/m}  []
+    None,                   !- Anti-Sweat Heater Control Type
+    ,                       !- Humidity At Zero Anti-Sweat Heater Energy {%}
+    ,                       !- Case Height {m}  []
+    1.0,                    !- Fraction of Anti-Sweat Heater Energy To Case
+    0.0,                    !- Case Defrost Power per Unit Length {W/m}  [0.0 W/ft  0 W]
+    Off Cycle,              !- Case Defrost Type
+    UserProvideDefSched6PerDay45MinEa,                        !- Case Defrost Schedule Name
+    UserProvideDefSched4PerDay42MinEa,                        !- Case Defrost Drip-Down Schedule
+    CaseTemperatureMethod,  !- Defrost Energy Correction Curve Type
+    Multi Shelf Vertical,   !- Defrost Energy Correction Curve Name
+    0.00,                   !- Under Case HVAC Return Air Fraction
+    ,                       !- Refrigerated Case Restocking Schedule Name  [Not modeling any restocking]
+    ,                       !- Case Credit Fraction Schedule Name
+    -3.33,                  !- Design Evaporator Temperature or Brine Inlet Temperature {C}  [26øF]
+    ;                       !- Average Refrigerant Charge Inventory {kg/m}  [ = ]
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-022}
+
+\begin{itemize}
+\item
+  Zone,Average,Refrigeration Case Evaporator Total Cooling Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Evaporator Total Cooling Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Case Evaporator Sensible Cooling Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Evaporator Sensible Cooling Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Case Evaporator Latent Cooling Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Case Evaporator Latent Cooling Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Case Zone Sensible Cooling Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Zone Sensible Cooling Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Case Zone Sensible Heating Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Zone Sensible Heating Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Case Zone Latent Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Zone Latent Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Case Return Air Sensible Cooling Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Return Air Sensible Cooling Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Case Return Air Sensible Heating Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Return Air Sensible Heating Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Case Return Air Latent Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Return Air Latent Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Case Evaporator Fan Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Evaporator Fan Electric Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Case Lighting Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Lighting Electric Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Case Latent Credit Curve Value {[]}
+\end{itemize}
+
+If case defrost type is Electric, Hot-Gas, or Hot-Brine with Temperature Termination
+
+\begin{itemize}
+\tightlist
+\item
+  Zone,Average,Refrigeration Case Defrost Energy Correction Curve Value
+\end{itemize}
+
+If anti-sweat heater control type is not equal to None:
+
+\begin{itemize}
+\item
+  Zone,Average,Refrigeration Case Anti Sweat Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Anti Sweat Electric Energy {[}J{]}
+\end{itemize}
+
+If case defrost type is Electric or Electric with Temperature Termination:
+
+\begin{itemize}
+\item
+  Zone,Average,Refrigeration Case Defrost Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Case Defrost Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Refrigeration Case Evaporator Total Cooling Rate {[}W{]}}\label{refrigeration-case-evaporator-total-cooling-rate-w}
+
+This field is the total (sensible plus latent) cooling rate of the refrigerated case evaporator coil in Watts.
+
+\paragraph{Refrigeration Case Evaporator Total Cooling Energy {[}J{]}}\label{refrigeration-case-evaporator-total-cooling-energy-j}
+
+This field is the total (sensible plus latent) cooling of the refrigerated case evaporator coil in Joules over the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Case Evaporator Sensible Cooling Rate {[}W{]}}\label{refrigeration-case-evaporator-sensible-cooling-rate-w}
+
+This field is the sensible cooling rate of the refrigerated case evaporator coil in Watts.
+
+\paragraph{Refrigeration Case Evaporator Sensible Cooling Energy {[}J{]}}\label{refrigeration-case-evaporator-sensible-cooling-energy-j}
+
+This field is the sensible cooling of the refrigerated case evaporator coil in Joules over the timestep being reported.
+
+\paragraph{Refrigeration Case Evaporator Latent Cooling Rate {[}W{]}}\label{refrigeration-case-evaporator-latent-cooling-rate-w}
+
+This field is the latent cooling (dehumidification) rate of the refrigerated case evaporator coil in Watts.
+
+\paragraph{Refrigeration Case Evaporator Latent Cooling Energy {[}J{]}}\label{refrigeration-case-evaporator-latent-cooling-energy-j}
+
+This field is the latent cooling (dehumidification) of the refrigerated case evaporator coil in Joules over the timestep being reported.
+
+\paragraph{Refrigeration Case Zone Sensible Cooling Rate {[}W{]}}\label{refrigeration-case-zone-sensible-cooling-rate-w}
+
+This field is the rate of sensible cooling case credits delivered to the zone in Watts. If an under case return duct is simulated, only a portion of the sensible case credits are applied to the zone. A positive value is reported when the zone is cooled by sensible case credits, otherwise a zero is reported.
+
+\paragraph{Refrigeration Case Zone Sensible Cooling Energy {[}J{]}}\label{refrigeration-case-zone-sensible-cooling-energy-j}
+
+This field is the amount of sensible cooling case credit energy delivered to the zone in Joules. If an under case return duct is simulated, only a portion of the sensible case credits are applied to the zone. A positive value is reported when the zone is cooled by sensible case credits, otherwise a zero is reported.
+
+\paragraph{Refrigeration Case Zone Sensible Heating Rate {[}W{]}}\label{refrigeration-case-zone-sensible-heating-rate-w}
+
+This field is the rate of sensible heating case credits delivered to the zone in Watts. If an under case return duct is simulated, only a portion of the sensible case credits are applied to the zone. A positive value is reported when the zone is heated by sensible case credits, otherwise a zero is reported.
+
+\paragraph{Refrigeration Case Zone Sensible Heating Energy {[}J{]}}\label{refrigeration-case-zone-sensible-heating-energy-j}
+
+This field is the amount of sensible heating case credit energy delivered to the zone in Joules. If an under case return duct is simulated, only a portion of the sensible case credits are applied to the zone. A positive value is reported when the zone is heated by sensible case credits, otherwise a zero is reported.
+
+\paragraph{Refrigeration Case Zone Latent Rate {[}W{]}}\label{refrigeration-case-zone-latent-rate-w}
+
+This field is the rate of latent cooling (dehumidification) case credits delivered to the zone in Watts. If an under case return duct is simulated, only a portion of the latent case credits are applied to the zone. A negative value (or zero) will be reported when the refrigerated case provides dehumidification (thereby reducing the zone latent load).
+
+\paragraph{Refrigeration Case Zone Latent Energy {[}J{]}}\label{refrigeration-case-zone-latent-energy-j}
+
+This field is the amount of latent cooling (dehumidification) case credit energy delivered to the zone in Joules. If an under case return duct is simulated, only a portion of the latent case credits are applied to the zone. A negative value (or zero) will be reported when the refrigerated case provides dehumidification (thereby reducing the zone latent load).
+
+\paragraph{Refrigeration Case Return Air Sensible Cooling Rate {[}W{]}}\label{refrigeration-case-return-air-sensible-cooling-rate-w}
+
+This field is the rate of sensible cooling case credits delivered to the return air duct (zone return air node) in Watts. If an under case return duct is simulated, a portion of the sensible case credits are applied to the HVAC (zone) return air. A positive value is reported when the return air is cooled by sensible case credits, otherwise a zero is reported. If the HVAC system is off for a simulation timestep (no return air mass flow), then this sensible cooling is actually provided to the zone air instead (even though a non-zero value is reported here).
+
+\paragraph{Refrigeration Case Return Air Sensible Cooling Energy {[}J{]}}\label{refrigeration-case-return-air-sensible-cooling-energy-j}
+
+This field is the amount of sensible cooling case credit energy delivered to the return air duct (zone return air node) in Joules. If an under case return duct is simulated, a portion of the sensible case credits are applied to the HVAC (zone) return air. A positive value is reported when the return air is cooled by sensible case credits, otherwise a zero is reported. If the HVAC system is off for a simulation timestep (no return air mass flow), then this sensible cooling is actually provided to the zone air instead (even though a non-zero value is reported here).
+
+\paragraph{Refrigeration Case Return Air Sensible Heating Rate {[}W{]}}\label{refrigeration-case-return-air-sensible-heating-rate-w}
+
+This field is the rate of sensible heating case credits delivered to the return air duct (zone return air node) in Watts. If an under case return duct is simulated, a portion of the sensible case credits are applied to the HVAC (zone) return air. A positive value is reported when the return air is heated by sensible case credits, otherwise a zero is reported. If the HVAC system is off for a simulation timestep (no return air mass flow), then this sensible heating is actually provided to the zone air instead (even though a non-zero value is reported here).
+
+\paragraph{Refrigeration Case Return Air Sensible Heating Energy {[}J{]}}\label{refrigeration-case-return-air-sensible-heating-energy-j}
+
+This field is the amount of sensible heating case credit energy delivered to the return air duct (thereby reducing the zone latent load). If the HVAC system is off for a simulation timestep (no return air mass flow), then this latent energy is actually provided to the zone air instead (even though a non-zero value is reported here).
+
+\paragraph{Refrigeration Case Return Air Latent Energy {[}J{]}}\label{refrigeration-case-return-air-latent-energy-j}
+
+\paragraph{Refrigeration Case Return Air Latent Rate {[}W{]}}\label{refrigeration-case-return-air-latent-rate-w}
+
+These are the amount of latent cooling (dehumidification) case credit energy delivered to the return air duct (zone return air node) in Joules or Watts. If an under case return duct is simulated, only a portion of the latent case credits are applied to the HVAC (zone) return air. A negative value (or zero) will be reported since the refrigerated case provides dehumidification (thereby reducing the zone latent load). If the HVAC system is off for a simulation timestep (no return air mass flow), then this latent energy is actually provided to the zone air instead (even though a non-zero value is reported here).
+
+\paragraph{Refrigeration Case Evaporator Fan Electric Power {[}W{]}}\label{refrigeration-case-evaporator-fan-electric-power-w}
+
+This field is the electric power input to the refrigerated case fan(s) in Watts.
+
+\paragraph{Refrigeration Case Evaporator Fan Electric Energy {[}J{]}}\label{refrigeration-case-evaporator-fan-electric-energy-j}
+
+This field is the electricity consumption of the refrigerated case fan(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Case Lighting Electric Power {[}W{]}}\label{refrigeration-case-lighting-electric-power-w}
+
+This field is the electric power input to the refrigerated case lights in Watts.
+
+\paragraph{Refrigeration Case Lighting Electric Energy {[}J{]}}\label{refrigeration-case-lighting-electric-energy-j}
+
+This field is the electricity consumption of the refrigerated case lights in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Case Defrost Energy Correction Curve Value}\label{refrigeration-case-defrost-energy-correction-curve-value}
+
+This field is the output of the Defrost Energy Correction Curve which denotes the variation in defrost energy at off-rated conditions. The output of the defrost energy correction curve directly impacts the energy used during the defrost time period. It does not, however, impact the duration of the defrost period. This output is available only for Electric with Temperature Termination, Hot-Gas with Temperature Termination, or Hot-Brine with Temperature Termination case defrost types.
+
+\paragraph{\texorpdfstring{Refrigeration Case Latent Credit Curve Value {[]}}{Refrigeration Case Latent Credit Curve Value }}\label{refrigeration-case-latent-credit-curve-value}
+
+This field is the output of the Latent Case Credit Curve which denotes the variation in latent case credits at off-rated conditions. The output of the latent case credit curve directly impacts the amount of frost formation on the refrigerated case evaporator coil and the requirement for defrost.
+
+\paragraph{Refrigeration Case Anti Sweat Electric Power {[}W{]}}\label{refrigeration-case-anti-sweat-electric-power-w}
+
+This field is the electric power input to the refrigerated case anti-sweat heater in Watts. This output is available unless anti-sweat heater control type is specified as NONE.
+
+\paragraph{Refrigeration Case Anti Sweat Electric Energy {[}J{]}}\label{refrigeration-case-anti-sweat-electric-energy-j}
+
+This field is the total electricity consumption of the refrigerated case anti-sweat heater in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects). This output is available unless anti-sweat heater control type is specified as NONE.
+
+\paragraph{Refrigeration Case Defrost Electric Power {[}W{]}}\label{refrigeration-case-defrost-electric-power-w}
+
+This field is the electric power input to the refrigerated case electric defrost heater(s) in Watts. This output is available if case defrost type is Electric or Electric with Temperature Termination.
+
+\paragraph{Refrigeration Case Defrost Electric Energy {[}J{]}}\label{refrigeration-case-defrost-electric-energy-j}
+
+This field is the total electricity consumption of the refrigerated case electric defrost heater(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects). This output is available if case defrost type is Electric or Electric with Temperature Termination.
+
+\subsection{Refrigeration:CaseAndWalkInList}\label{refrigerationcaseandwalkinlist}
+
+This object provides a list of all the refrigerated cases and/or walk in coolers cooled by a single refrigeration system (ref: Refrigeraion:CompressorRack and Refrigeration:System). This list is extensible. Note that the names of all cases, walk-ins,air chillers, and caseandwalkinlists must be unique.~ That is, you cannot give a list the same name as one of the cases.~ Similarly, a walkin cannot have the same name as a case.This list may contain a combination of case and walk-in names OR a list of air chiller names.~ Air chillers may not be included in any list that also includes cases or walk-ins.
+
+\subsubsection{Inputs}\label{inputs-2-033}
+
+\paragraph{Field: Name}\label{field-name-2-032}
+
+A unique user-assigned name for an instance of a CaseAndWalkInList. Any reference to this list by another object will use this name.
+
+\paragraph{Field: Case or WalkIn or Air Chiller \textless{}x\textgreater{} Name}\label{field-case-or-walkin-or-air-chiller-x-name}
+
+Identifies a particular refrigerated case or walk-in. The name will be validated against the~ Refrigeration Case, Refrigeration WalkIn, and Air Chiller names (ref: Refrigeration:Case,~ Refrigeration:WalkIn, and Refrigeration:AirChiller) in the input file. Up to 20 are provided in the IDD; this object is extensible.
+
+The following is an example input for a CaseAndWalkInList.
+
+\begin{lstlisting}
+
+Refrigeration:CaseAndWalkInList,
+      MediumTempCaselist,      !- Name
+      UprightDairyCase,        !- Refrigeration Case or WalkIn Name \#1
+      LunchmeatCase,           !- Refrigeration Case or WalkIn Name \#2
+      MeatWalkIn,              !- Refrigeration Case or WalkIn Name \#3
+      DeliCaseOne;             !- Refrigeration Case or WalkIn Name \#4
+\end{lstlisting}
+
+\subsection{Refrigeration:WalkIn}\label{refrigerationwalkin}
+
+The Refrigeration WalkIn object works in conjunction with a compressor rack, a refrigeration system, or a refrigeration secondary system object (Ref. Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem) to simulate the performance of a walk-in cooler. The walk-in cooler model uses information at rated conditions along with input descriptions for heat transfer surfaces facing multiple zones to determine performance. Energy use for lights, fans, and floor and anti-sweat heaters is modeled based on inputs for nominal power, schedules, and control type. The walk-in cooler model accounts for the sensible and latent heat exchange with the surrounding environment (termed ``case credits'') which impacts the temperature and humidity in each zone adjacent to the walk-in.
+
+The walk-in cooler object inputs include a name, an availability schedule name, the rated cooling capacity, the rated operating temperature, the rated cooling source temperature, the rated total heating power and heating power schedule, the rated fan and lighting power and schedules, defrost type, defrost control type, defrost schedule name, drip-down schedule name, defrost power, the portion of the defrost energy used to melt ice (only for temperature termination control type), restocking schedule, refrigerant inventory, and the floor area and U-value.
+
+For each zone adjacent to the walk-in, the user must input the zone name and the insulated surface area and U-value facing that zone. The user must also specify, for two types of doors, the door area, height, U-value, door opening schedule name, and any door opening protection.
+
+Under case HVAC return air fraction, available for refrigerated cases, is not available for walk-in coolers.
+
+\subsubsection{Field: Name}\label{field-name-3-026}
+
+A unique user-assigned name for an instance of a refrigerated walk-in. Any reference to this walk-in by another object will use this name.
+
+\subsubsection{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-011}
+
+The name of the schedule (ref: Schedule) that denotes whether the walk in can operate during a given time period. A schedule value greater than 0 (maximum schedule value of 1.0 is typically used) indicates that the walkin will operate during a given time period. A value equal to 0 denotes that the case does not operate (everything is OFF: refrigeration, fans, lights, anti-sweat, etc.). Typically the walkin will operate throughout the day (i.e., the schedule will contain 1 for all time periods); however, walkins require maintenance and/or cleaning and this can be modeled accordingly using this schedule if desired. If this field is left blank, the default schedule has a value of 1 for all time periods.
+
+\subsubsection{Field: Rated Coil Cooling Capacity}\label{field-rated-coil-cooling-capacity}
+
+The total, full load cooling capacity (sensible plus latent) in watts (W) at rated conditions The value entered for this field must be greater than zero, with no default value.
+
+\subsubsection{Field: Operating Temperature}\label{field-operating-temperature}
+
+The rated average temperature of the air and products within the walk-in cooler in ËšC. The entered value for this field must be less than 20ËšC. There is no default value.
+
+\subsubsection{Field: Rated Cooling Source Temperature}\label{field-rated-cooling-source-temperature}
+
+For a DX evaporator coil, enter the saturated evaporating temperature in ËšC.~ For a fluid coil, enter the fluid coil entrance temperature in ËšC. There is no default value. This number is used, with temperatures for other refrigeration loads on any one system, to set that system's minimum suction pressure or minimum circulating fluid temperature. (This value is not used if the walkin is cooled by a compressor rack object.)
+
+\subsubsection{Field: Rated Total Heating Power}\label{field-rated-total-heating-power}
+
+The total heating power in watts including all anti-sweat, door, drip-pan, and floor heaters (W). This value is required and has no default value.
+
+\subsubsection{Field: Heating Power Schedule Name}\label{field-heating-power-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes the fraction of heater power that operates during a given time period. A schedule value of zero denotes that all heaters are off. A schedule value greater than 0 indicates that some portion of the total heater power will operate during that time period (maximum schedule value of 1.0 means all heaters are fully on). For example, if door and floor heaters represent 50\% of the total heater power and are on all the time, the minimum schedule value would be 0.5. If anti-sweat heaters represent 40\% of the total heater power and are only on during certain hours, the schedule value during those hours would be increased by 0.4. If this field is left blank, the default schedule has a value of 1 for all time periods.
+
+\subsubsection{Field: Rated Cooling Coil Fan Power}\label{field-rated-cooling-coil-fan-power}
+
+The cooling coil fan power in watts (W). This value has a default value of 375W. This fan is assumed to run continuously except during electric, hot brine, or hot gas defrost periods.
+
+\subsubsection{Field: Rated Circulation Fan Power}\label{field-rated-circulation-fan-power}
+
+The circulation fan power in watts (W). This value has a default value of 0 W. This fan is assumed to run continuously.
+
+\subsubsection{Field: Rated Total Lighting Power}\label{field-rated-total-lighting-power}
+
+The total lighting power in watts including both display and task lighting (W). This value is required and has no default value.
+
+\subsubsection{Field: Lighting Schedule Name}\label{field-lighting-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes the fraction of walk-in lights that operate during a given time period. A schedule value greater than 0 indicates that the lights will operate during that time period (maximum schedule value of 1.0 means lights are fully on). A schedule value of zero denotes that the lights are off. If this field is left blank, the default schedule has a value of 1 for all time periods.
+
+\subsubsection{Field: Defrost Type}\label{field-defrost-type}
+
+The type of defrost used for this walk-in. Valid choices are None, Off-Cycle, HotFluid, and Electric. The default defrost type is Electric if the field is blank. HotFluid includes both hot gas and hot brine defrost systems. Refer to the Engineering Reference for further information on how the different defrost types are modeled.
+
+\subsubsection{Field: Defrost Control Type}\label{field-defrost-control-type}
+
+The type of defrost control used for this walkin. Valid choices are TimeSchedule and TemperatureTermination. The default is TimeSchedule if the field is blank. Refer to the Engineering Reference for further information on how the different defrost controls are modeled.
+
+\subsubsection{Field: Defrost Schedule Name}\label{field-defrost-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes when the walkin requires defrosting. A schedule value of 1.0 indicates that defrost will be on during a given time period if the defrost control type is ``TimeSchedule''. For the TemperatureTermination defrost control type, the defrost will start with the schedule value changes from 0 to 1, but will end when the ice is melted. A value equal to 0 denotes that the defrost is off. Defrost schedules normally repeat the duration and number of defrost cycles for each day of the year. The walkin manufacturer typically provides this information with the product literature. If TemperatureTermination control type is used, the defrost schedule is used for the defrost cycle start time and the defrost cycle end time is not allowed to extend beyond the scheduled off time. The use of Compact Schedules (ref. Schedules) are ideal for this purpose.
+
+\subsubsection{Field: Defrost Drip-Down Schedule Name}\label{field-defrost-drip-down-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes whether the walkin requires additional time for draining condensate after the defrost period. A schedule value of 1.0 indicates that the defrost drip-down period is on during a given time period. A value equal to 0 denotes that the defrost drip-down period is over. The walkin manufacturer typically provides this information with the product literature.
+
+Each defrost drip-down period specified in this schedule should start at the same time as the corresponding defrost period specified in the schedule for Defrost Schedule, and the drip-down schedule defrost period should always be longer than or equal to the length of the defrost schedule time period. For example, if the defrost schedule contains a defrost period from 7:00 to 7:15, you would specify a case defrost drip-down period from 7:00 to 7:20 if you wanted to model a 5 minute condensate drip-down period after the regular defrost period. If no drip-down schedule is entered, then the defrost schedule (specified for the previous input field) will be used. The use of Compact Schedules (ref. Schedules) are ideal for this purpose.
+
+\subsubsection{Field: Defrost Power}\label{field-defrost-power}
+
+The defrost power in watts. This input is required for hot-fluid (hot gas or hot brine), or electric defrost types. Walkin manufacturers do not typically provide information on the heat input for hot gas and hot brine defrost. Information provided for electric defrost power can be substituted here for walkins using hot-gas or hot-brine defrost if other information is not available. Only electric Defrost Types consume electricity during the defrost period. The entered value for this field must be greater than or equal to zero.
+
+\subsubsection{Field: Temperature Termination Defrost Fraction to Ice}\label{field-temperature-termination-defrost-fraction-to-ice}
+
+When cooling coils go through a defrost cycle, only a portion of the defrost energy is actually used to melt the ice.~ The rest of the defrost energy goes to increasing the temperature of the coils themselves and to the walkin environment. The Temperature Termination defrost control type calculates the end of the defrost cycle that corresponds to melting all the ice. Therefore, the user must input this fractional value. The default value is 0.7 for electric defrost and 0.3 for hot fluid defrost. Refer to the Engineering Reference for further information on how the defrost energy control types are modeled.
+
+\subsubsection{Field: Restocking Schedule Name}\label{field-restocking-schedule-name}
+
+The name of the schedule (ref: Schedule) that denotes whether the walkin is being restocked with product. The schedule should contain values in units of Watts (note this is different from the restocking schedule values for cases that are entered per unit length). This field can be used to denote the additional load imposed on the walkin from stocking the walkin with product that is warmer than the walkin temperature. This information is difficult to find and may required additional research for proper modeling; however, this schedule is available for this purpose if desired. If restocking of the refrigerated walkin will not be simulated, enter a schedule with values of zero for all time periods or leave this field blank.
+
+\subsubsection{Field: Average Refrigerant Charge Inventory}\label{field-average-refrigerant-charge-inventory-1}
+
+The value of this optional field is the refrigerant inventory present in the walkin during ordinary operation. The value is used to produce an estimate of the total refrigerant present in the refrigeration system. The value is entered in kg.
+
+\subsubsection{Field: Insulated Floor Surface Area}\label{field-insulated-floor-surface-area}
+
+The floor area in square meters. This value is required and has no default value.
+
+\subsubsection{Field: Insulated Floor U-Value}\label{field-insulated-floor-u-value}
+
+The floor themal transmittance (in W/m\(^{2}\)-K). This value has a default value of 0.3154. (This corresponds to R18 in Archaic American Insulation Units.~ To convert other R-values to thermal transmittance, divide 5.678 by the R-value.~ For example, R15 is 0.3785 W/m\(^{2}\)-K and R5 is 1.136 W/m\(^{2}\)-K.)
+
+\textbf{\emph{THE REMAINING 12 FIELDS FOR THE WALK-IN COOLER MUST BE REPEATED FOR EACH ZONE WHICH IS IN CONTACT WITH A WALK-IN WALL, CEILING, OR DOOR. The IDD includes fields for 3 zones, but can be extended by repeating the last 12 values in the object.}}
+
+\subsubsection{Field: Zone \textless{}x\textgreater{} Name}\label{field-zone-x-name}
+
+The name of a zone adjoining the walkin. The walkin will impact the air heat balance in this zone. This zone must represent a conditioned space, that is, it must appear in a ZoneHVAC:EquipmentConnections object.
+
+\subsubsection{Field: Total Insulated Surface Area Facing~ Zone \textless{}x\textgreater{}}\label{field-total-insulated-surface-area-facing-zone-x}
+
+The total surface area (walls and ceilings) facing this particular zone in square meters. This value is required and has no default value.
+
+\subsubsection{Field: Insulated Surface U-Value Facing Zone \textless{}x\textgreater{}}\label{field-insulated-surface-u-value-facing-zone-x}
+
+The surface (walls and ceilings) themal transmittance (in W/m\(^{2}\)-K). This value has a default value of 0.3154. (This corresponds to R18 in Archaic American Insulation Units.~ To convert other R-values to thermal transmittance, divide 5.678 by the R-value.~ For example, R15 is 0.3785 W/m\(^{2}\)-K and R5 is 1.136 W/m\(^{2}\)-K.)
+
+\subsubsection{Field: Area of Glass Reach In Doors Facing Zone \textless{}x\textgreater{}}\label{field-area-of-glass-reach-in-doors-facing-zone-x}
+
+The total area of glass doors facing this particular zone in square meters. The default is 0.0.
+
+\subsubsection{Field: Height of Glass Reach In Doors Facing Zone \textless{}x\textgreater{}}\label{field-height-of-glass-reach-in-doors-facing-zone-x}
+
+The glass reach in door height in meters. The default is 1.5.
+
+\subsubsection{Field: Glass Reach In Door U-Value Facing Zone \textless{}x\textgreater{}}\label{field-glass-reach-in-door-u-value-facing-zone-x}
+
+The glass door themal transmittance (in W/m\(^{2}\)-K). This field has a default value of 1.136. (This corresponds to R5 in Archaic American Insulation Units.)
+
+\subsubsection{Field: Glass Reach In Door Opening Schedule Name Facing Zone \textless{}x\textgreater{}}\label{field-glass-reach-in-door-opening-schedule-name-facing-zone-x}
+
+The name of the schedule (ref: Schedule) that denotes the fraction of time glass doors are open during a given time period. The schedule values should be between 0 and 1.0. If no schedule is specified, the doors are assumed to be open 5\% of the time (corresponding to a schedule value of 0.05).
+
+\subsubsection{Field: Area of Stocking Doors Facing Zone \textless{}x\textgreater{}}\label{field-area-of-stocking-doors-facing-zone-x}
+
+The total area of stock doors facing this particular zone in square meters. The default is 0.0.
+
+\subsubsection{Field: Height of Stocking Doors Facing Zone \textless{}x\textgreater{}}\label{field-height-of-stocking-doors-facing-zone-x}
+
+The stocking door height in meters. The default is 2.0.
+
+\subsubsection{Field: Stocking Door U-Value Facing Zone \textless{}x\textgreater{}}\label{field-stocking-door-u-value-facing-zone-x}
+
+The stocking door themal transmittance (in W/m\(^{2}\)-K). This value has a default value of 0.3785. (This corresponds to R15 in Archaic American Insulation Units.)
+
+\subsubsection{Field: Stocking Door Opening Schedule Name Facing Zone \textless{}x\textgreater{}}\label{field-stocking-door-opening-schedule-name-facing-zone-x}
+
+The name of the schedule (ref: Schedule) that denotes the fraction of time stocking doors are open during a given time period. The schedule values should be between 0 and 1.0. If no schedule is specified, the doors are assumed to be open 5\% of the time (corresponding to a schedule value of 0.05).
+
+\subsubsection{Field: Stocking Door Opening Protection Type Facing Zone \textless{}x\textgreater{}}\label{field-stocking-door-opening-protection-type-facing-zone-x}
+
+The type of stocking door opening protection used for this walkin. Valid choices are None, AirCurtain, and StripCurtain. The default is AirCurtain if the field is blank. Use the type, StripCurtain, for both hanging strips and airlock vestibules. Refer to the Engineering Reference for further information on how the door protection types are modeled.
+
+The following is an example input for a refrigeration walkin.
+
+\begin{lstlisting}
+
+   Refrigeration:WalkIn,
+      WalkInFreezer,           !- Name
+      CaseOperatingSched,      !- Availability Schedule Name
+      4690.,                   !- Rated Coil Cooling Capacity {W}
+      -2.22,                   !- Operating Temperature {C}
+      -6.67,                   !- Rated Cooling Source Temperature {C}
+      0.0,                     !- Rated Total Heating Power {W}
+      CaseOperatingSched,      !- Heating Power Schedule Name
+      735.,                    !- Rated Cooling Coil Fan Power {W}
+      0.0,                     !- Rated Circulation Fan Power {W}
+      120.,                    !- Rated Total Lighting Power {W}
+      CaseLightingSched2,      !- Lighting Schedule Name
+      Electric,                !- Defrost Type
+      TimeSchedule,            !- Defrost Control Type
+      CaseDefrostSched3,       !- Defrost Schedule Name
+      CaseDripDownSched3,      !- Defrost Drip-Down Schedule Name
+      5512.,                   !- Defrost Power {W}
+      ,                        !- Temperature Termination Defrost Fraction to Ice {dimensionless}
+      WalkInStockingSched,     !- Restocking Schedule Name
+      ,                        !- Average Refrigerant Charge Inventory {kg}
+      13.0,                    !- Insulated Floor Surface Area {m2}
+      0.207,                   !- Insulated Floor U-Value {W/m2-C}
+      BackRoom,                !- Zone Name
+      43.4,                    !- Total Insulated Surface Area Facing this Zone {m2}
+      .235,                    !- Insulated Surface U-Value Facing this Zone {W/m2-C}
+      ,                        !- Area of Glass Reach In Doors Facing this Zone {m2}
+      ,                        !- Height of Glass Reach In Doors Facing this Zone {m}
+      ,                        !- Glass Reach In Door U Value Facing this Zone {W/m2-C}
+      ,                        !- Glass Reach In Door Opening Schedule Name Facing this Zone
+      2.0,                     !- Area of Stocking Doors Facing this Zone {m2}
+      2.0,                     !- Height of Stocking Doors Facing this Zone {m}
+      ,                        !- Stocking Door U Value Facing this Zone {W/m2-C}
+      WIStockDoorOpenSch,      !- Stocking Door Opening Schedule Name Facing this Zone
+      StripCurtain;            !- Stocking Door Opening Protection Type Facing this Zone
+\end{lstlisting}
+
+\subsection{Refrigeration Case and WalkIn Outputs}\label{refrigeration-case-and-walkin-outputs}
+
+\begin{itemize}
+\item
+  Zone,Average,Refrigeration Walk In Evaporator Total Cooling Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Evaporator Total Cooling Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Walk In Evaporator Sensible Cooling Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Evaporator Sensible Cooling Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Walk In Evaporator Latent Cooling Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Evaporator Latent Cooling Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Walk In Ancillary Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Ancillary Electric Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Walk In Fan Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Fan Electric Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Walk In Lighting Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Lighting Electric Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Walk In Heater Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Heater Electric Energy {[}J{]}
+\end{itemize}
+
+\emph{Report only for WalkIns using electric defrost}
+
+\begin{itemize}
+\item
+  Zone,Average,Refrigeration Walk In Defrost Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Defrost Electric Energy {[}J{]}
+\end{itemize}
+
+\textbf{\emph{Report for each Zone exchanging energy with the WalkIn}}
+
+\begin{itemize}
+\item
+  Zone,Average,Refrigeration Walk In Zone Sensible Cooling Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Zone Sensible Cooling Energy {[}J{]}
+\item
+  Zone,Average, Zone,Average,Refrigeration Walk In Zone Sensible Heating Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Zone Sensible Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone,Average,Refrigeration Walk In Zone Latent Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Walk In Zone Latent Energy {[}J{]}
+\end{itemize}
+
+\subsubsection{Refrigeration Walk In Evaporator Total Cooling Rate {[}W{]}}\label{refrigeration-walk-in-evaporator-total-cooling-rate-w}
+
+This field is the total (sensible plus latent) cooling rate of the WalkIn evaporator coil in Watts.
+
+\subsubsection{Refrigeration Walk In Evaporator Total Cooling Energy {[}J{]}}\label{refrigeration-walk-in-evaporator-total-cooling-energy-j}
+
+This field is the total (sensible plus latent) cooling of the WalkIn evaporator coil in Joules over the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
+
+\subsubsection{Refrigeration Walk In Evaporator Sensible Cooling Rate {[}W{]}}\label{refrigeration-walk-in-evaporator-sensible-cooling-rate-w}
+
+This field is the sensible cooling rate of the WalkIn evaporator coil in Watts.
+
+\subsubsection{Refrigeration Walk In Evaporator Sensible Cooling Energy {[}J{]}}\label{refrigeration-walk-in-evaporator-sensible-cooling-energy-j}
+
+This field is the sensible cooling of the WalkIn evaporator coil in Joules over the timestep being reported.
+
+\subsubsection{Refrigeration Walk In Evaporator Latent Cooling Rate {[}W{]}}\label{refrigeration-walk-in-evaporator-latent-cooling-rate-w}
+
+This field is the latent cooling (dehumidification) rate of the WalkIn evaporator coil in Watts.
+
+\subsubsection{Refrigeration Walk In Evaporator Latent Cooling Energy {[}J{]}}\label{refrigeration-walk-in-evaporator-latent-cooling-energy-j}
+
+This field is the latent cooling (dehumidification) of the WalkIn evaporator coil in Joules over the timestep being reported.
+
+\subsubsection{Refrigeration Walk In Ancillary Electric Power {[}W{]}}\label{refrigeration-walk-in-ancillary-electric-power-w}
+
+This field is the total electricity (fan, heaters, lights, and electric defrost) used by the walkin in Watts.
+
+\subsubsection{Refrigeration Walk In Ancillary Electric Energy {[}J{]}}\label{refrigeration-walk-in-ancillary-electric-energy-j}
+
+This field is the electricity (fan, heaters, lights, and electric defrost)used by the WalkIn in Joules over the timestep being reported.
+
+\subsubsection{Refrigeration Walk In Fan Electric Power {[}W{]}}\label{refrigeration-walk-in-fan-electric-power-w}
+
+This field is the electric power input to the WalkIn fan(s) in Watts.
+
+\subsubsection{Refrigeration Walk In Fan Electric Energy {[}J{]}}\label{refrigeration-walk-in-fan-electric-energy-j}
+
+This field is the electricity consumption of the WalkIn fan(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
+
+\subsubsection{Refrigeration Walk In Lighting Electric Power {[}W{]}}\label{refrigeration-walk-in-lighting-electric-power-w}
+
+This field is the electric power input to the WalkIn lights in Watts.
+
+\subsubsection{Refrigeration Walk In Lighting Electric Energy {[}J{]}}\label{refrigeration-walk-in-lighting-electric-energy-j}
+
+This field is the electricity consumption of the WalkIn lights in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
+
+\subsubsection{Refrigeration Walk In Heater Electric Power {[}W{]}}\label{refrigeration-walk-in-heater-electric-power-w}
+
+This field is the electric power input to the WalkIn heaters in Watts.
+
+\subsubsection{Refrigeration Walk In Heater Electric Energy {[}J{]}}\label{refrigeration-walk-in-heater-electric-energy-j}
+
+This field is the total electricity consumption of the WalkIn heaters in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
+
+\subsubsection{Refrigeration Walk In Defrost Electric Power {[}W{]}}\label{refrigeration-walk-in-defrost-electric-power-w}
+
+This field is the electric power input to the WalkIn electric defrost heater(s) in Watts. This output is available if case defrost type is Electric.
+
+\subsubsection{Refrigeration Walk In Defrost Electric Energy {[}J{]}}\label{refrigeration-walk-in-defrost-electric-energy-j}
+
+This field is the total electricity consumption of the WalkIn electric defrost heater(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects). This output is available if case defrost type is Electric.
+
+\emph{The following output variables are available for each zone adjacent to the walkin. An output variable identification is created for each zone exchanging energy with the walkin.~ For example if the walkin, ``DairyWalkIn'', were exchanging energy with the zone, ``SalesArea'', the output variable identification would be ``DairyWalkInInZoneSalesArea''.}
+
+\subsubsection{Refrigeration Walk In Zone Sensible Cooling Rate {[}W{]}}\label{refrigeration-walk-in-zone-sensible-cooling-rate-w}
+
+This field is the rate of sensible cooling case credits delivered to the zone in Watts. A positive value is reported when the zone is cooled by sensible case credits, otherwise a zero is reported.
+
+\subsubsection{Refrigeration Walk In Zone Sensible Cooling Energy {[}J{]}}\label{refrigeration-walk-in-zone-sensible-cooling-energy-j}
+
+This field is the amount of sensible cooling case credit energy delivered to the zone in Joules. A positive value is reported when the zone is cooled by sensible case credits, otherwise a zero is reported.
+
+\subsubsection{Refrigeration Walk In Zone Sensible Heating Rate {[}W{]}}\label{refrigeration-walk-in-zone-sensible-heating-rate-w}
+
+This field is the rate of sensible heating case credits delivered to the zone in Watts. A positive value is reported when the zone is heated by sensible case credits, otherwise a zero is reported.
+
+\subsubsection{Refrigeration Walk In Zone Sensible Heating Energy {[}J{]}}\label{refrigeration-walk-in-zone-sensible-heating-energy-j}
+
+This field is the amount of sensible heating case credit energy delivered to the zone in Joules. A positive value is reported when the zone is heated by sensible case credits, otherwise a zero is reported.
+
+\subsubsection{Refrigeration Walk In Zone Latent Rate {[}W{]}}\label{refrigeration-walk-in-zone-latent-rate-w}
+
+This field is the rate of latent cooling (dehumidification) case credits delivered to the zone in Watts. A negative value (or zero) will be reported when the WalkIn provides dehumidification (thereby reducing the zone latent load).
+
+\subsubsection{Refrigeration Walk In Zone Latent Energy {[}J{]}}\label{refrigeration-walk-in-zone-latent-energy-j}
+
+This field is the amount of latent cooling (dehumidification) case credit energy delivered to the zone in Joules. A negative value (or zero) will be reported when the WalkIn provides dehumidification (thereby reducing the zone latent load).
+
+\subsection{Refrigeration:System}\label{refrigerationsystem}
+
+The refrigeration system object simulates the performance of a supermarket refrigeration system when used along with other objects to define the refrigeration load(s), the compressor(s), and the condenser.
+
+At least one refrigeration load object must be defined which may be one of four types of load, a refrigerated case, a walk-in cooler, a chiller providing refrigeration to a secondary loop, or a cascade condenser which absorbs heat rejected by a lower-temperature system (Ref. Refrigeration:Case, Refrigeration:WalkIn, Refrigeration:SecondarySystem,~ and Refrigeration:Condenser:Cascade) If multiple loads are served by the same system , the user should use one or both of the list objects available to assign loads to the system. The first list includes all cases and walkins cooled directly by this system (Ref. Refrigeration:CaseAndWalkInList). The second list includes any `transfer' loads, that is refrigeration loads borne by this system that are transferred from another refrigeration system via either a secondary loop chiller or a cascade condenser (Ref. Refrigeration:TransferLoadList, see the Engineering Reference for more information about these types of systems).
+
+The refrigeration system object is capable of modeling both single-stage and two-stage compression refrigeration systems.~ The name of at least one compressor must be defined and a list object is available if the system is served by more than one compressor (Ref. Refrigeration:Compressor and Refrigeration:CompressorList).
+
+Heat is rejected outdoors in a condenser by direct air flow, evaporative water cooling, by a water-cooled condenser with appropriate plant loop piping, or to a cascade condenser cooled by another refrigeration system(ref: Refrigeration:Condenser:AirCooled, Refrigeration:Condenser:EvaporativeCooled, Refrigeration:Condenser:WaterCooled, Refrigeration:Condenser:Cascade). With evaporative cooling, water is sprayed through the air stream to effectively lower the air temperature experienced by the condenser coil as a result of water evaporation. The use of a water-cooled condenser requires the definition of a plant loop to supply cooling to the condenser.~ If a cascade condenser is specified, the refrigeration system absorbing the rejected heat must also be defined.
+
+The refrigeration system may also include a liquid suction and/or mechanical subcooler (Ref. Refrigeration:Subcooler).
+
+The system object coordinates the energy flows between the other refrigeration objects and is used to set system parameters. Compressor waste heat can also be reclaimed for use by an optional air- or water-heating coil (Ref. Coil:Heating:Desuperheater and Coil:WaterHeating:Desuperheater).
+
+The inputs for the refrigeration system object, in addition to the names of the other refrigeration objects described above, include a name for this system, the minimum condensing temperature, the refrigeration system working fluid, and the type of saturated suction temperature control. Optional input fields are also provided for users seeking to keep track of refrigerant inventory and suction pipe heat gains.
+
+\subsubsection{Inputs}\label{inputs-3-029}
+
+\paragraph{Field: Name}\label{field-name-4-023}
+
+A unique user-assigned name for an instance of a refrigeration system. Any reference to this refrigeration system by another object will use this name.
+
+\paragraph{Field: Refrigerated Case or WalkIn or CaseAndWalkInList Name}\label{field-refrigerated-case-or-walkin-or-caseandwalkinlist-name}
+
+Identifies a single case, a single walkin, single air chiller, or a particular list of refrigerated cases and walkins or air chillers, that is cooled by this refrigeration system. The name will be validated against the case, walkin, air chiller and CaseAndWalkInList names ~(ref: Refrigeration:Case, Refrigeration:WalkIn, Refrigeration:AirChiller, and Refrigeration:CaseAndWalkInList) in the input file. Only cases and walkins or air chillers served directly by the system should be included in this list.~ Any cases, walkins, or air chillers served indirectly via a secondary loop should NOT be included in this list. Note that any system that serves an air chiller cannot also serve a case or walkin.
+
+\paragraph{Field: Refrigeration Transfer Load or TransferLoad List Name}\label{field-refrigeration-transfer-load-or-transferload-list-name}
+
+Identifies a single SecondarySystem, a single Cascade Condenser, OR or a list of Transfer Loads (where the list is comprised of SecondarySystems and/or Cascade Condensers) that are cooled by this refrigeration system. The name will be validated against the secondary system, cascade condenser, and TransferLoad list names (ref: Refrigeration:SecondarySystem, Refrigeration:Condenser:Cascade, and Refrigeration:TransferLoadList) in the input file. Only secondary systems and cascade condensers served directly by the system should be included in this list. (NOTE -- this entry is for a cascade condenser \emph{cooled by} this system, not a condenser \emph{absorbing heat rejected by} this system.)
+
+\paragraph{Field: Condenser Name}\label{field-condenser-name}
+
+The name of the condenser that is used to \emph{reject heat from} this refrigeration system. The name will be validated against the condenser names (ref: Refrigeration:Condenser:AirCooled, Refrigeration:Condenser:WaterCooled, Refrigeration:Condenser:EvaporativeCooled, and Refrigeration:Condenser:Cascade) in the input file.
+
+\paragraph{Field:Compressor or ~Compressor List Name}\label{fieldcompressor-or-compressor-list-name}
+
+Identifies a single compressor, or a particular list of compressors, that provide cooling energy to this refrigeration system. The name will be validated against the compressor list names (ref: List:Refrigeration:Compressors) in the input file.~ If the refrigeration systems contains two stages of compression, this field identifies the low-stage compressors connected to the two-stage system.
+
+\paragraph{Field: Minimum Condensing Temperature}\label{field-minimum-condensing-temperature}
+
+This numeric field specifies the minimum condensing temperature (C), which is usually determined by the temperature required to maintain acceptable thermal expansion valve performance.
+
+\paragraph{Field: Refrigeration System Working Fluid Type}\label{field-refrigeration-system-working-fluid-type}
+
+The type of refrigerant used by the system.~ Valid choices are R11, R123, R134A, R12, R22, R404A, R507A, or R410A. This name will be validated against Fluid Names (ref: Fluid Properties section) in the input file. Note that the corresponding property data, available in FluidPropertiesRefData.idf, must by supplied in the input file.
+
+\paragraph{Field: Suction Temperature Control Type}\label{field-suction-temperature-control-type}
+
+The type of saturated suction temperature control used by the system. Valid choices are \textbf{FloatSuctionTemperature} and \textbf{ConstantSuctionTemperature}.~ If the field is blank, the default will be \textbf{ConstantSuctionTemperature}. See the Engineering Reference section, Variable Evaporator Temperature, for a discussion of this option.
+
+\paragraph{Field: Mechanical Subcooler Name}\label{field-mechanical-subcooler-name}
+
+This optional field identifies a mechanical subcooler that absorbs heat from this refrigeration system. This field should not be used for a mechanical subcooler that absorbs heat from another system. The name will be validated against the subcooler names (ref: Refrigeration:Subcooler) in the input file.
+
+\paragraph{Field: Liquid Suction Heat Exchanger Subcooler Name}\label{field-liquid-suction-heat-exchanger-subcooler-name}
+
+This optional field Identifies a particular liquid suction heat exchanger (LSHX) subcooler present in this refrigeration system. The name will be validated against the subcooler names (ref: Refrigeration:Subcooler) in the input file.
+
+\paragraph{Field: Sum UA Suction Piping}\label{field-sum-ua-suction-piping}
+
+This optional field is typically used when trying to determine the impact of pipe heat gains on system performance and zone heat balance, particularly in comparing a DX system to a secondary system. Enter the value for suction piping heat gain (in W/C).~ That is, sum up the product of the pipe wall insulation conductance times the outer surface area of the pipe insulation. Please see the Engineering Reference for guidance in calculating this value. If the Sum UA Suction Piping is entered, the Suction Piping Zone Name is also required.
+
+\paragraph{Field: Suction Piping Zone Name}\label{field-suction-piping-zone-name}
+
+This optional field is typically used when trying to determine the impact of pipe heat gains on system performance, particularly in comparing a DX system to a secondary system. (If the previous field, Sum UA Suction Piping, is blank, this field will not be used.) Enter the name of the zone where the suction piping is located. The suction piping heat gains will be calculated based upon the air temperature within this zone. The heat balance of this zone will also be affected by the piping heat exchange. Additional output variables are described at the end of this ``Group-Refrigeration'' section for the total impact of refrigeration on zones, including suction pipe heat exchange.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-1-002}
+
+This field allows the specification of a user-defined end-use subcategory (e.g., ``Low Temperature Rack''). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Number of Compressor Stages}\label{field-number-of-compressor-stages}
+
+This field determines whether the refrigeration system contains one or two stages of compression.~ In this field, enter either ``1'' for single-stage compression systems or ``2'' for two-stage compression systems.~ If two stages of compression are selected, then an intercooler will be used between the compressor stages to cool the discharge of the low-stage compressors.~ The default value is ``1''.
+
+\paragraph{Field: Intercooler Type}\label{field-intercooler-type}
+
+This field determines the type of intercooler which is used for two-stage compression systems.~ Valid choices for this field include ``None'', ``Flash Intercooler'' or ``Shell-and-Coil Intercooler''.~ Single-stage systems require ``None'' while two-stage systems require either ``Flash Intercooler'' or ``Shell-and-Coil Intercooler''.~ The default selection is ``None'', corresponding to a single-stage compression system.
+
+\paragraph{Field: Shell-and-Coil Intercooler Effectiveness}\label{field-shell-and-coil-intercooler-effectiveness}
+
+When a shell-and-coil intercooler is selected for two-stage compression systems, this field allows the specification of the shell-and-coil intercooler effectiveness.~ Values in this field will only be valid if ``Shell-and-Coil Intercooler'' is selected in the ``Intercooler Type'' field above.~ The valid range of values for this field is between 0.0 and 1.0.~ A default value of 0.80 will be used if none is specified.
+
+\paragraph{Field: High-Stage Compressor or CompressorList Name}\label{field-high-stage-compressor-or-compressorlist-name}
+
+Identifies a single compressor, or a particular list of compressors, that comprise the high-stage compression of a two-stage compression refrigeration system. The name will be validated against the compressor list names (ref: List:Refrigeration:Compressors) in the input file.~ Names in this field are only valid if two compressor stages have been specified in the ``Number of Compressor Stages'' field above.
+
+The following is an example input for a single-stage compression refrigeration system.
+
+\begin{lstlisting}
+
+ Refrigeration:System,
+      MediumTempSystem,        !- Refrigeration System Name
+      MediumTempCaselist,      !-  Refrigeration Case or Walkin or CaseAndWalkInList Name
+      ,                        !- Refrigeration Transfer Load or TransferLoad List Name
+      AirCooledCondenserA,     !- Refrigeration Condenser Name
+      MediumTempCompressorlist, !- Refrigeration Compressor or CompressorList Name
+      25.0,                    !- Minimum Condensing Temperture {C}
+      R134a,                   !- Refrigeration System Working Fluid
+      ConstantSuctionTemperature,  !- Suction Temperature Control Type
+      ,                        !- Optional mechanical subcooler name
+      ,                        !- Optional LSHX subcooler name
+      ,                        !- Sum UA Distribution Piping {W/K}
+      ,                        !- Distribution Piping Zone Name
+      MedTempRefrig;           !- End-Use Subcategory
+\end{lstlisting}
+
+The following is an example input for a two-stage compression refrigeration system.
+
+\begin{lstlisting}
+
+ Refrigeration:System,
+      LowTempSystem,           !- Refrigeration System Name
+      LowTempCaselist,         !-  Refrigeration Case or Walkin or CaseAndWalkInList Name
+      ,                        !- Refrigeration Transfer Load or TransferLoad List Name
+      AirCooledCondenserB,     !- Refrigeration Condenser Name
+      LowStageCompressorList,  !- Refrigeration Compressor or CompressorList Name
+      25.0,                    !- Minimum Condensing Temperture {C}
+      R404A,                   !- Refrigeration System Working Fluid
+      ConstantSuctionTemperature,  !- Suction Temperature Control
+      ,                        !- Optional mechanical subcooler name
+      ,                        !- Optional LSHX subcooler name
+      ,                        !- Sum UA Distribution Piping {W/K}
+      ,                        !- Distribution Piping Zone Name
+      LowTempRefrig,           !- End-Use Subcategory
+      2,                       !- Number of Compressor Stages
+      Shell-and-Coil Intercooler,  !- Intercooler Type
+      0.7,                     !- Shell-and-Coil Intercooler Effectiveness
+      HiStageCompressorList    !- High-Stage Compressor or CompressorList Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-018}
+
+THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE CASES AND/OR WALKINS:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration System Total Compressor Electric Power {[}W{]}
+\item
+  Zone,Sum, Refrigeration System Total Compressor Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Average Compressor COP {[}W/W{]}
+\item
+  Zone,Average, Refrigeration System Total Compressor Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration System Total Compressor Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Total Cases and Walk Ins Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration System Total Cases and Walk Ins Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Total Transferred Load Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration System Total Transferred Load Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Total Suction Pipe Heat Gain Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration System Total Suction Pipe Heat Gain Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Net Rejected Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration System Net Rejected Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration System Estimated Refrigerant Inventory Mass {[}kg{]}
+\item
+  Zone,Average, Refrigeration System Liquid Suction Subcooler Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Liquid Suction Subcooler Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Estimated Refrigerant Inventory {[}kg{]}
+\item
+  Zone,Average, Refrigeration System Estimated Refrigerant Mass Flow Rate {[}kg/s{]}
+\item
+  Zone,Average, Refrigeration System Condensing Temperature {[}C{]}'
+\item
+  Zone,Average, Refrigeration System Evaporating Temperature {[}C{]}
+\item
+  Zone,Average, Refrigeration System Suction Pipe Suction Temperature {[}C{]}
+\item
+  Zone,Average, Refrigeration System Thermostatic Expansion Valve Liquid Temperature {[}C{]}
+\item
+  Zone,Average, Refrigeration System Estimated High Stage Refrigerant Mass Flow Rate {[}kg/s{]}
+\item
+  Zone,Sum,Refrigeration System Total High Stage Compressor Electric Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration System Total High Stage Compressor Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration System Total High Stage Compressor Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration System Total High Stage Compressor Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration System Total Low and High Stage Compressor Electric Energy {[}J{]}
+\item
+  Zone,Sum,Refrigeration System Total Low Stage Compressor Electric Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration System Total Low Stage Compressor Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration System Total Low Stage Compressor Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration System Total Low Stage Compressor Heat Transfer Rate {[}W{]}
+\item
+  Zone,Average,Refrigeration System Estimated Low Stage Refrigerant Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE AIR CHILLERS:
+
+\begin{itemize}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Total Compressor Electric Power {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller System Total Compressor Electric Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Average Compressor COP {[}W/W{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Total Compressor Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller System Total Compressor Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Total Air Chiller Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller System Total Case and Walk In Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Total Transferred Load Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller System Total Transferred Load Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Total Suction Pipe Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller System Total Suction Pipe Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Net Rejected Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller System Net Rejected Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Liquid Suction Subcooler Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Liquid Suction Subcooler Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Estimated Refrigerant Inventory Mass {[}kg{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Estimated Refrigerant Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Intercooler Temperature {[}C{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Intercooler Pressure {[}Pa{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condensing Temperature {[}C{]}'
+\item
+  HVAC,Average, Refrigeration Air Chiller System Evaporating Temperature {[}C{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Suction Temperature {[}C{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System TXV Liquid Temperature {[}C{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Estimated High Stage Refrigerant Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum,Refrigeration Air Chiller System Total High Stage Compressor Electric Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Total High Stage Compressor Electric Power {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Air Chiller System Total High Stage Compressor Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Total High Stage Compressor Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller System Total Low and High Stage Compressor Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Refrigeration Air Chiller System Total Low Stage Compressor Electric Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Total Low Stage Compressor Electric Power {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Air Chiller System Total Low Stage Compressor Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Total Low Stage Compressor Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Estimated Low Stage Refrigerant Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE CASES AND/OR WALKINS}\label{the-following-outputs-are-available-for-systems-that-serve-cases-andor-walkins}
+
+\paragraph{Refrigeration System Total Compressor Electric Power {[}W{]}}\label{refrigeration-system-total-compressor-electric-power-w}
+
+This output is the total electric power input to the system compressor(s) in Watts.
+
+\paragraph{Refrigeration System Total Compressor~Electric Energy {[}J{]}}\label{refrigeration-system-total-compressorelectric-energy-j}
+
+This is the electricity consumption of the system's compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration System Total Low Stage Compressor Electric Power {[}W{]}}\label{refrigeration-system-total-low-stage-compressor-electric-power-w}
+
+This output is the total electric power input to the system's low-stage compressor(s) in Watts.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Total Low Stage Compressor Electric Energy {[}J{]}}\label{refrigeration-system-total-low-stage-compressor-electric-energy-j}
+
+This is the electricity consumption of the system's low-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Total High Stage Compressor Electric Power {[}W{]}}\label{refrigeration-system-total-high-stage-compressor-electric-power-w}
+
+This output is the total electric power input to the system's high-stage compressor(s) in Watts.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Total High Stage Compressor Electric Energy {[}J{]}}\label{refrigeration-system-total-high-stage-compressor-electric-energy-j}
+
+This is the electricity consumption of the system's high-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Total Low and High Stage Compressor Electric Energy~ {[}J{]}}\label{refrigeration-system-total-low-and-high-stage-compressor-electric-energy-j}
+
+This is the total electricity consumption of the system's low- and high-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Average Compressor COP {[}W/W{]}}\label{refrigeration-system-average-compressor-cop-ww}
+
+This output is the system average compressor COP, the total refrigeration effect divided by the total power to the compressors.
+
+\paragraph{Refrigeration System Total Compressor Heat Transfer Rate {[}W{]}}\label{refrigeration-system-total-compressor-heat-transfer-rate-w}
+
+This output is the total heat transfer rate of the Refrigeration Compressor rack in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.
+
+\paragraph{Refrigeration System Total Compressor Heat Transfer Energy {[}J{]}}\label{refrigeration-system-total-compressor-heat-transfer-energy-j}
+
+This is the total heat transfer of the Refrigeration Compressor rack in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration System Total Low Stage Compressor Heat Transfer Rate {[}W{]}}\label{refrigeration-system-total-low-stage-compressor-heat-transfer-rate-w}
+
+This output is the total heat transfer rate of the low-stage compressors in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Total Low Stage Compressor Heat Transfer Energy {[}J{]}}\label{refrigeration-system-total-low-stage-compressor-heat-transfer-energy-j}
+
+This is the total heat transfer of the low-stage compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Total High Stage Compressor Heat Transfer Rate {[}W{]}}\label{refrigeration-system-total-high-stage-compressor-heat-transfer-rate-w}
+
+This output is the total heat transfer rate of the high-stage compressors in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Total High Stage Compressor Heat Transfer Energy {[}J{]}}\label{refrigeration-system-total-high-stage-compressor-heat-transfer-energy-j}
+
+This is the total heat transfer of the high-stage compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Total Cases and Walk Ins Heat Transfer Rate {[}W{]}}\label{refrigeration-system-total-cases-and-walk-ins-heat-transfer-rate-w}
+
+This output is the total heat transfer rate from the refrigerated cases and walk-ins served directly by this system in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases and walk-ins that are connected directly to this system. This value does not include compressor or condenser fan heat or the heat transfer for cases and walk-ins served by any connected secondary systems.
+
+\paragraph{Refrigeration System Total Cases and Walk Ins Heat Transfer Energy {[}J{]}}\label{refrigeration-system-total-cases-and-walk-ins-heat-transfer-energy-j}
+
+This output is the total heat transfer energy from the refrigerated cases and walk-ins served directly by this system in Joules. It is the sum of all of the heat transfered for the refrigerated cases and walk-ins that are connected directly to this system. This value does not include compressor or condenser fan heat or the heat transfer for cases and walk-ins served by any connected secondary systems.
+
+\paragraph{Refrigeration System Total Transferred Load Heat Transfer Rate {[}W{]}}\label{refrigeration-system-total-transferred-load-heat-transfer-rate-w}
+
+This output is the sum of the heat transfer rates for any secondary loops, cascade condensers, and mechanical subcoolers cooled by this system, minus the benefit of any mechanical subcooler providing cooling to this system in Watts. Therefore, if the only transfer load between two systems is a mechanical subcooler, the same amount will show as a negative value for the system receiving the cooling effect and as a positive number for the system serving that cooling load. It also includes the pump energy for any secondary loops and the compressor energy for any cascade condenser systems that are cooled by this system. (See the Engineering Reference for more details about the loads placed by secondary systems upon the primary system.)
+
+\paragraph{Refrigeration System Total Transferred Load Heat Transfer Energy {[}J{]}}\label{refrigeration-system-total-transferred-load-heat-transfer-energy-j}
+
+This output is the sum of the heat transfered for any secondary loops, cascade condensers, and mechanical subcoolers cooled by this system, minus the benefit of any mechanical subcooler providing cooling to this system in Joules. Therefore, if the only transfer load between two systems is a mechanical subcooler, the same amount will show as a negative value for the system receiving the cooling effect and as a positive number for the system serving that cooling load. It also includes the pump energy for any secondary loops and the compressor energy for any cascade condenser systems that are cooled by this system. (See the Engineering Reference for more details about the loads placed by secondary systems upon the primary system.)
+
+\paragraph{Refrigeration System Total Suction Pipe Heat Gain Rate {[}W{]}}\label{refrigeration-system-total-suction-pipe-heat-gain-rate-w}
+
+This output is the total heat transfer rate for suction piping served by this system in Watts. Note this is an optional input, and is only available if the user has described the suction piping heat gain characteristics in the input.
+
+\paragraph{Refrigeration System Total Suction Pipe Heat Gain Energy {[}J{]}}\label{refrigeration-system-total-suction-pipe-heat-gain-energy-j}
+
+This output is the total heat transfer rate for suction piping served by this system in Watts. Note this is an optional input, and is only available if the user has described the suction piping heat gain characteristics in the input.
+
+\paragraph{Refrigeration System Net Rejected Heat Transfer Rate {[}W{]}}\label{refrigeration-system-net-rejected-heat-transfer-rate-w}
+
+This output is the total heat rejected by this system to the system condenser in Watts. It does not include system heat rejection that has been recovered for useful purposes. However, if a water-cooled condenser was used to provide heat to a separate water loop, the energy transferred to that loop is included here.
+
+\paragraph{Refrigeration System Net Rejected Heat Transfer Energy {[}J{]}}\label{refrigeration-system-net-rejected-heat-transfer-energy-j}
+
+This output is the total heat rejected by this system to the system condenser in Joules for the timestep being reported. It does not include system heat rejection that has been recovered for useful purposes. However, if a water-cooled condenser was used to provide heat to a separate water loop, the energy transferred to that loop is included here.
+
+\paragraph{Refrigeration System Liquid Suction Subcooler Heat Transfer Rate {[}W{]}}\label{refrigeration-system-liquid-suction-subcooler-heat-transfer-rate-w}
+
+This output is the total heat transferred from the liquid condensate before the thermal expansion valve to the suction gas.
+
+\paragraph{Refrigeration System Liquid Suction Subcooler Heat Transfer Energy {[}J{]}}\label{refrigeration-system-liquid-suction-subcooler-heat-transfer-energy-j}
+
+This output is the total heat transferred from the liquid condensate before the thermal expansion valve to the suction gas.
+
+\paragraph{Refrigeration System Estimated Refrigerant Inventory Mass {[}kg{]}}\label{refrigeration-system-estimated-refrigerant-inventory-mass-kg}
+
+This output is the sum of the input inventory values for the condenser, receiver, cases, and liquid pipes that are a part of this system.
+
+\paragraph{Refrigeration System Estimated Refrigerant Mass Flow Rate {[}kg/s{]}}\label{refrigeration-system-estimated-refrigerant-mass-flow-rate-kgs}
+
+This output is the calculated refrigerant mass flow through the compressors for this system.
+
+\paragraph{Refrigeration System Estimated Low Stage Refrigerant Mass Flow Rate {[}kg/s{]}}\label{refrigeration-system-estimated-low-stage-refrigerant-mass-flow-rate-kgs}
+
+This output is the calculated refrigerant mass flow through the low-stage compressors for this system.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Estimated High Stage Refrigerant Mass Flow Rate {[}kg/s{]}}\label{refrigeration-system-estimated-high-stage-refrigerant-mass-flow-rate-kgs}
+
+This output is the calculated refrigerant mass flow through the high-stage compressors for this system.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Intercooler Temperature {[}C{]}}\label{refrigeration-system-intercooler-temperature-c}
+
+This is the saturation temperature in the intercooler.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Intercooler Pressure {[}Pa{]}}\label{refrigeration-system-intercooler-pressure-pa}
+
+This is the saturation pressure in the intercooler.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration System Condensing Temperature {[}C{]}}\label{refrigeration-system-condensing-temperature-c}
+
+This is the saturated condensing temperature.
+
+\paragraph{Refrigeration System Evaporating Temperature {[}C{]}}\label{refrigeration-system-evaporating-temperature-c}
+
+This is the saturated evaporating temperature.
+
+\paragraph{Refrigeration System Suction Pipe Suction Temperature {[}C{]}}\label{refrigeration-system-suction-pipe-suction-temperature-c}
+
+This is the temperature at the compressor inlet including superheat after the cases and superheat from any liquid suction heat exchangers.
+
+\paragraph{Refrigeration System Thermostatic Expansion Valve Liquid Temperature {[}C{]}}\label{refrigeration-system-thermostatic-expansion-valve-liquid-temperature-c}
+
+This is the temperature entering the thermal expansion valve before the cases, equal to the condensing temperature minus any subcooling included in the condenser or provided by mechanical and/or liquid suction heat exchanger subcoolers.
+
+\paragraph{THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE AIR CHILLERS}\label{the-following-outputs-are-available-for-systems-that-serve-air-chillers}
+
+\paragraph{Refrigeration Air Chiller System Total Compressor Electric Power {[}W{]}}\label{refrigeration-air-chiller-system-total-compressor-electric-power-w}
+
+This output is the total electric power input to the system compressor(s) in Watts.
+
+\paragraph{Refrigeration Chiller System Total Compressor~Electric Energy {[}J{]}}\label{refrigeration-chiller-system-total-compressorelectric-energy-j}
+
+This is the electricity consumption of the system's compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller System Total Low Stage Compressor Electric Power {[}W{]}}\label{refrigeration-air-chiller-system-total-low-stage-compressor-electric-power-w}
+
+This output is the total electric power input to the system's low-stage compressor(s) in Watts.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Total Low Stage Compressor Electric Energy {[}J{]}}\label{refrigeration-air-chiller-system-total-low-stage-compressor-electric-energy-j}
+
+This is the electricity consumption of the system's low-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Total High Stage Compressor Electric Power {[}W{]}}\label{refrigeration-air-chiller-system-total-high-stage-compressor-electric-power-w}
+
+This output is the total electric power input to the system's high-stage compressor(s) in Watts.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Total High Stage Compressor Electric Energy {[}J{]}}\label{refrigeration-air-chiller-system-total-high-stage-compressor-electric-energy-j}
+
+This is the electricity consumption of the system's high-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Total Low and High Stage Compressor Electric Energy {[}J{]}}\label{refrigeration-air-chiller-system-total-low-and-high-stage-compressor-electric-energy-j}
+
+This is the total electricity consumption of the system's low- and high-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Average Compressor COP {[}W/W{]}}\label{refrigeration-air-chiller-system-average-compressor-cop-ww}
+
+This output is the system average compressor COP, the total refrigeration effect divided by the total power to the compressors
+
+\paragraph{Refrigeration Air Chiller System Total Compressor Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-total-compressor-heat-transfer-rate-w}
+
+This output is the total heat transfer rate of the Refrigeration Compressor rack in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.
+
+\paragraph{Refrigeration Air Chiller System Total Compressor Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-total-compressor-heat-transfer-energy-j}
+
+This is the total heat transfer of the Refrigeration Compressor rack in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller System Total Low Stage Compressor Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-total-low-stage-compressor-heat-transfer-rate-w}
+
+This output is the total heat transfer rate of the low-stage compressors in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Total Low Stage Compressor Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-total-low-stage-compressor-heat-transfer-energy-j}
+
+This is the total heat transfer of the low-stage compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Total High Stage Compressor Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-total-high-stage-compressor-heat-transfer-rate-w}
+
+This output is the total heat transfer rate of the high-stage compressors in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Total High Stage Compressor Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-total-high-stage-compressor-heat-transfer-energy-j}
+
+This is the total heat transfer of the high-stage compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Total Air Chiller Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-total-air-chiller-heat-transfer-rate-w}
+
+This output is the total heat transfer rate from the refrigerated cases and walk-ins served directly by this system in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases and walk-ins that are connected directly to this system. This value does not include compressor or condenser fan heat or the heat transfer for cases and walk-ins served by any connected secondary systems.
+
+\paragraph{Refrigeration Air Chiller System Total Case and Walk In Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-total-case-and-walk-in-heat-transfer-energy-j}
+
+This output is the total heat transfer energy from the refrigerated cases and walk-ins served directly by this system in Joules. It is the sum of all of the heat transfered for the refrigerated cases and walk-ins that are connected directly to this system. This value does not include compressor or condenser fan heat or the heat transfer for cases and walk-ins served by any connected secondary systems.
+
+\paragraph{Refrigeration Air Chiller System Total Transferred Load Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-total-transferred-load-heat-transfer-rate-w}
+
+This output is the sum of the heat transfer rates for any secondary loops, cascade condensers, and mechanical subcoolers cooled by this system, minus the benefit of any mechanical subcooler providing cooling to this system in Watts. Therefore, if the only transfer load between two systems is a mechanical subcooler, the same amount will show as a negative value for the system receiving the cooling effect and as a positive number for the system serving that cooling load. It also includes the pump energy for any secondary loops and the compressor energy for any cascade condenser systems that are cooled by this system. (See the Engineering Reference for more details about the loads placed by secondary systems upon the primary system.)
+
+\paragraph{Refrigeration Air Chiller System Total Transferred Load Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-total-transferred-load-heat-transfer-energy-j}
+
+This output is the sum of the heat transfered for any secondary loops, cascade condensers, and mechanical subcoolers cooled by this system, minus the benefit of any mechanical subcooler providing cooling to this system in Joules. Therefore, if the only transfer load between two systems is a mechanical subcooler, the same amount will show as a negative value for the system receiving the cooling effect and as a positive number for the system serving that cooling load. It also includes the pump energy for any secondary loops and the compressor energy for any cascade condenser systems that are cooled by this system. (See the Engineering Reference for more details about the loads placed by secondary systems upon the primary system.)
+
+\paragraph{Refrigeration Air Chiller System Total Suction Pipe Heat Gain Rate {[}W{]}}\label{refrigeration-air-chiller-system-total-suction-pipe-heat-gain-rate-w}
+
+This output is the total heat transfer rate for suction piping served by this system in Watts. Note this is an optional input, and is only available if the user has described the suction piping heat gain characteristics in the input.
+
+\paragraph{Refrigeration Air Chiller System Total Suction Pipe Heat Gain Energy {[}J{]}}\label{refrigeration-air-chiller-system-total-suction-pipe-heat-gain-energy-j}
+
+This output is the total heat transfer rate for suction piping served by this system in Watts. Note this is an optional input, and is only available if the user has described the suction piping heat gain characteristics in the input.
+
+\paragraph{Refrigeration Air Chiller System Net Rejected Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-net-rejected-heat-transfer-rate-w}
+
+This output is the total heat rejected by this system to the system condenser in Watts. It does not include system heat rejection that has been recovered for useful purposes. However, if a water-cooled condenser was used to provide heat to a separate water loop, the energy transferred to that loop is included here.
+
+\paragraph{Refrigeration Air Chiller System Net Rejected Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-net-rejected-heat-transfer-energy-j}
+
+This output is the total heat rejected by this system to the system condenser in Joules for the timestep being reported. It does not include system heat rejection that has been recovered for useful purposes. However, if a water-cooled condenser was used to provide heat to a separate water loop, the energy transferred to that loop is included here.
+
+\paragraph{Refrigeration Air Chiller System Liquid Suction Subcooler Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-liquid-suction-subcooler-heat-transfer-rate-w}
+
+This output is the total heat transferred from the liquid condensate before the thermal expansion valve to the suction gas.
+
+\paragraph{Refrigeration Air Chiller System Liquid Suction Subcooler Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-liquid-suction-subcooler-heat-transfer-energy-j}
+
+This output is the total heat transferred from the liquid condensate before the thermal expansion valve to the suction gas.
+
+\paragraph{Refrigeration Air Chiller System Mechanical Subcooler Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-mechanical-subcooler-heat-transfer-energy-j}
+
+\paragraph{Refrigeration Air Chiller System Estimated Refrigerant Inventory Mass {[}kg{]}}\label{refrigeration-air-chiller-system-estimated-refrigerant-inventory-mass-kg}
+
+This output is the sum of the input inventory values for the condenser, receiver, cases, and liquid pipes that are a part of this system.
+
+\paragraph{Refrigeration Air Chiller System Estimated Refrigerant Mass Flow Rate {[}kg/s{]}}\label{refrigeration-air-chiller-system-estimated-refrigerant-mass-flow-rate-kgs}
+
+This output is the calculated refrigerant mass flow through the compressors for this system.
+
+\paragraph{Refrigeration Air Chiller System Estimated Low Stage Refrigerant Mass Flow Rate {[}kg/s{]}}\label{refrigeration-air-chiller-system-estimated-low-stage-refrigerant-mass-flow-rate-kgs}
+
+This output is the calculated refrigerant mass flow through the low-stage compressors for this system.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Estimated High Stage Refrigerant Mass Flow Rate {[}kg/s{]}}\label{refrigeration-air-chiller-system-estimated-high-stage-refrigerant-mass-flow-rate-kgs}
+
+This output is the calculated refrigerant mass flow through the high-stage compressors for this system.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Intercooler Temperature {[}C{]}}\label{refrigeration-air-chiller-system-intercooler-temperature-c}
+
+This is the saturation temperature in the intercooler.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Intercooler Pressure {[}Pa{]}}\label{refrigeration-air-chiller-system-intercooler-pressure-pa}
+
+This is the saturation pressure in the intercooler.~ This output is valid only for two-stage compression systems.
+
+\paragraph{Refrigeration Air Chiller System Condensing Temperature {[}C{]}}\label{refrigeration-air-chiller-system-condensing-temperature-c}
+
+This is the saturated condensing temperature.
+
+\paragraph{Refrigeration Air Chiller System Evaporating Temperature {[}C{]}}\label{refrigeration-air-chiller-system-evaporating-temperature-c}
+
+This is the saturated evaporating temperature.
+
+\paragraph{Refrigeration Air Chiller System Suction Temperature {[}C{]}}\label{refrigeration-air-chiller-system-suction-temperature-c}
+
+This is the temperature at the compressor inlet including superheat after the cases and superheat from any liquid suction heat exchangers.
+
+\paragraph{Refrigeration Air Chiller System TXV Liquid Temperature {[}C{]}}\label{refrigeration-air-chiller-system-txv-liquid-temperature-c}
+
+This is the temperature entering the thermal expansion valve before the cases, equal to the condensing temperature minus any subcooling included in the condenser or provided by mechanical and/or liquid suction heat exchanger subcoolers.
+
+\subsection{Refrigeration:TranscriticalSystem}\label{refrigerationtranscriticalsystem}
+
+The Refrigeration:TranscriticalSystem object allows users to model detailed transcritical carbon dioxide (CO\(_{2}\)) booster refrigeration systems used in supermarkets.~ The object allows for modeling either a single stage system with medium-temperature loads or a two stage system with both medium- and low-temperature loads.
+
+The input objects required to model a detailed transcritical CO\(_{2}\) refrigeration system include the following:
+
+\begin{itemize}
+\item
+  One Refrigeration:TranscriticalSystem object,
+\item
+  At least one refrigeration load object which may include any combination of the following:
+\item
+  Refrigeration:Case,
+\item
+  Refrigeration:WalkIn,
+\item
+  Refrigeration:CaseAndWalkInList (may include both cases and/or walk-in cooler names),
+\item
+  At least one Refrigeration:Compressor object (multiple compressors are entered using a Refrigeration:CompressorList),
+\item
+  One Refrigeration:GasCooler:AirCooled object,
+\end{itemize}
+
+Output variables are available to describe the total heat exchange between all the refrigeration objects and the zones containing these objects.~ These variables are described at the end of this section.
+
+At least one refrigeration load object must be defined which may be one of two types of loads, including a refrigerated display case and a walk-in cooler, (Ref. Refrigeration:Case, and Refrigeration:WalkIn).~ If multiple loads are served by the same system, the user should use the refrigerated case and walk-in list object available to assign all cases and walk-ins cooled directly by this system (Ref. Refrigeration:CaseAndWalkInList).
+
+The name of at least one compressor must be defined and a list object is available if the system is served by more than one compressor (Ref. Refrigeration:Compressor and Refrigeration:CompressorList).
+
+Heat is rejected to the outdoors via an air-cooled gas cooler (Ref. Refrigeration:GasCooler:AirCooled).
+
+The Refrigeration:TranscriticalSystem object coordinates the energy flows between the other refrigeration objects and is used to set system parameters.
+
+The inputs for the refrigeration system object, in addition to the names of the other refrigeration objects described above, include a name for this system, the receiver pressure, the subcooler effectiveness, and the refrigeration system working fluid.~ Optional input fields are also provided for users seeking to keep track of suction pipe heat gains.
+
+A detailed description of the transcritical CO\(_{2}\) booster refrigeration system may be found in the Refrigeration section of the Engineering Reference.
+
+\subsubsection{Inputs}\label{inputs-4-026}
+
+\paragraph{Field: Name}\label{field-name-5-019}
+
+A unique user-assigned name for an instance of a transcritical CO\(_{2}\) refrigeration system.~ Any reference to this refrigeration system by another object will use this name.
+
+\paragraph{Field: System Type}\label{field-system-type}
+
+Identifies the transcritical CO\(_{2}\) refrigeration system as either a single-stage system with only medium-temperature loads, or a two-stage system with both medium- and low-temperature loads.~ Valid choices are:~ SingleStage for single stage systems or TwoStage for two stage systems.
+
+\paragraph{Field: Medium Temperature Refrigerated Case or WalkIn or CaseAndWalkInList Name}\label{field-medium-temperature-refrigerated-case-or-walkin-or-caseandwalkinlist-name}
+
+Identifies a single case, a single walk-in, or a particular list of refrigerated cases and walk-ins, that is cooled by the medium-temperature stage of the refrigeration system.~ The name will be validated against the case, walk-in, and CaseAndWalkInList names (Ref. Refrigeration:Case, Refrigeration:WalkIn, and Refrigeration:CaseAndWalkInList) in the input file.~ Only medium temperature cases and walk-ins served directly by the system should be included in this list.~ Note that this entry is required for both single-stage and two-stage systems.
+
+\paragraph{Field: Low Temperature Refrigerated Case or WalkIn or CaseAndWalkInList Name}\label{field-low-temperature-refrigerated-case-or-walkin-or-caseandwalkinlist-name}
+
+Identifies a single case, a single walk-in, or a particular list of refrigerated cases and walk-ins, that is cooled by the low-temperature stage of the refrigeration system.~ The name will be validated against the case, walk-in, and CaseAndWalkInList names (Ref. Refrigeration:Case, Refrigeration:WalkIn, and Refrigeration:CaseAndWalkInList) in the input file.~ Only low temperature cases and walk-ins served directly by the system should be included in this list.~ Note that this entry is valid only for two-stage systems.
+
+\paragraph{Field: Refrigeration Gas Cooler Name}\label{field-refrigeration-gas-cooler-name}
+
+The name of the gas cooler that is used to reject heat from the transcritical refrigeration system.~ The name will be validated against the gas cooler names (Ref. Refrigeration:GasCooler:AirCooled) in the input file.
+
+\paragraph{Field: High Pressure Compressor or Compressor List Name}\label{field-high-pressure-compressor-or-compressor-list-name}
+
+Identifies a single compressor, or a particular list of compressors, that provides compression for a single-stage system or the high pressure stage of a two-stage system.~ The name will be validated against the compressor list names (Ref. List:Refrigeration:Compressors) in the input file.~ Note that this entry is required for both single-stage and two-stage systems.
+
+\paragraph{Field: Low Pressure Compressor or Compressor List Name}\label{field-low-pressure-compressor-or-compressor-list-name}
+
+Identifies a single compressor, or a particular list of compressors, that provides compression for the low pressure stage of a two-stage system.~ The name will be validated against the compressor list names (Ref. List:Refrigeration:Compressors) in the input file.~ Note that this entry is valid only for two-stage systems.
+
+\paragraph{Field: Receiver Pressure}\label{field-receiver-pressure}
+
+This numeric field specifies the refrigerant pressure (Pa) in the receiver.~ The default value for the receiver pressure is 4.0~×~10\(^{6}\)~Pa.
+
+\paragraph{Field: Subcooler Effectiveness}\label{field-subcooler-effectiveness}
+
+This numeric field specifies the heat exchanger effectiveness of the subcooler.~ The default value for the subcooler effectiveness is 0.4.
+
+\paragraph{Field: Refrigeration System Working Fluid Type}\label{field-refrigeration-system-working-fluid-type-1}
+
+The type of refrigerant used by the system.~ It is assumed that carbon dioxide will be the refrigerant used in the transcritical CO\(_{2}\) refrigeration system.~ However, the user must specify the name used in the input file which refers to carbon dioxide.~ This name will be validated against Fluid Names (Ref. Fluid Properties section) in the input file.~ Note that the corresponding property data for carbon dioxide (R744), available in FluidPropertiesRefData.idf, must be supplied in the input file.
+
+\paragraph{Field: Sum UA Suction Piping for Medium Temperature Loads}\label{field-sum-ua-suction-piping-for-medium-temperature-loads}
+
+This optional field is typically used to determine the impact of pipe heat gains on system performance and zone heat balance.~ Enter the value for suction piping heat gain (in W/C) for the medium-temperature suction line, i.e., sum up the product of the pipe wall insulation conductance times the outer surface area of the pipe insulation.~ Please see the Engineering Reference for guidance in calculating this value.~ If the Sum UA Suction Piping for Medium Temperature Loads is entered, the Medium Temperature Suction Piping Zone Name is also required.
+
+\paragraph{Field: Medium Temperature Suction Piping Zone Name}\label{field-medium-temperature-suction-piping-zone-name}
+
+This optional field is typically used to determine the impact of pipe heat gains on system performance.~ If the previous field, Sum UA Suction Piping for Medium Temperature Loads, is blank, this field will not be used.~ Enter the name of the zone where the medium-temperature suction piping is located.~ The suction piping heat gains will be calculated based upon the air temperature within this zone.~ The heat balance of this zone will also be affected by the piping heat exchange.~ Additional output variables are described at the end of this section for the total impact of refrigeration on zones, including suction pipe heat exchange.
+
+\paragraph{Field: Sum UA Suction Piping for Low Temperature Loads}\label{field-sum-ua-suction-piping-for-low-temperature-loads}
+
+This optional field is typically used to determine the impact of pipe heat gains on system performance and zone heat balance.~ Enter the value for suction piping heat gain (in W/C) for the low-temperature suction line, i.e., sum up the product of the pipe wall insulation conductance times the outer surface area of the pipe insulation.~ Please see the Engineering Reference for guidance in calculating this value.~ If the Sum UA Suction Piping for Low Temperature Loads is entered, the Low Temperature Suction Piping Zone Name is also required.~ Note that this entry is valid only for two-stage systems.
+
+\paragraph{Field: Low Temperature Suction Piping Zone Name}\label{field-low-temperature-suction-piping-zone-name}
+
+This optional field is typically used to determine the impact of pipe heat gains on system performance.~ If the previous field, Sum UA Suction Piping for Low Temperature Loads, is blank, this field will not be used.~ Enter the name of the zone where the low-temperature suction piping is located. The suction piping heat gains will be calculated based upon the air temperature within this zone.~ The heat balance of this zone will also be affected by the piping heat exchange.~ Additional output variables are described at the end of this section for the total impact of refrigeration on zones, including suction pipe heat exchange.~ Note that this entry is valid only for two-stage systems.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-2-002}
+
+This field allows the specification of a user-defined end-use subcategory (e.g., ``Medium Temperature System'').~ A new meter for reporting is created for each unique subcategory (Ref. Output:Meter objects).~ Subcategories are also reported in the ABUPS table.~ If this field is left blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+The following is an example input for a transcritical CO\(_{2}\) refrigeration system.
+
+\begin{lstlisting}
+
+Refrigeration:TranscriticalSystem,
+      TransRefrigSys,          !- Name
+      TwoStage,                !- System Type
+      MTLoads,                 !- Medium Temperature Refrigerated Case or Walkin or CaseAndWalkInList Name
+      LTLoads,                 !- Low Temperature Refrigerated Case or Walkin or CaseAndWalkInList Name
+      RefrigGasCooler,         !- Refrigeration Gas Cooler Name
+      HPCompressors,           !- High Pressure Compressor or CompressorList Name
+      LPCompressors,           !- Low Pressure Compressor or CompressorList Name
+      4000000,                 !- Receiver Pressure
+      0.4,                     !- Subcooler Effectiveness
+      R744,                    !- Refrigeration System Working Fluid Type
+      ,                        !- Sum UA Suction Piping for Medium Temperature Loads
+      ,                        !- Medium Temperature Suction Piping Zone Name
+      ,                        !- Sum UA Suction Piping for Low Temperature Loads
+      ,                        !- Low Temperature Suction Piping Zone Name
+      TransRefrigSys;          !- End-Use Subcategory
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-016}
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration Transcritical System Total High Pressure Compressor Electric Power {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Total High Pressure Compressor Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Low Pressure Compressor Electric Power {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Low Pressure Compressor Electric Energy {[}J{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Total Compressor Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Average COP {[}W/W{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Medium Temperature Cases and Walk Ins Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Medium Temperature Cases and Walk Ins Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Low Temperature Cases and Walk Ins Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Low Temperature Cases and Walk Ins Heat Transfer Energy {[}J{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Total Cases and Walk Ins Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Medium Temperature Suction Pipe Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Medium Temperature Suction Pipe Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Low Temperature Suction Pipe Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Low Temperature Suction Pipe Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System High Pressure Compressor Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System High Pressure Compressor Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Low Pressure Compressor Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Low Pressure Compressor Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Net Rejected Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Net Rejected Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Estimated Refrigerant Inventory Mass {[}kg{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Refrigerant Mass Flow Rate {[}kg/s{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Medium Temperature Evaporating Temperature {[}C{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Medium Temperature Suction Temperature {[}C{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Low Temperature Evaporating Temperature {[}C{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Low Temperature Suction Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Refrigeration Transcritical System Total High Pressure Compressor Electric Power {[}W{]}}\label{refrigeration-transcritical-system-total-high-pressure-compressor-electric-power-w}
+
+This output is the total electric power input to the system's high pressure compressor(s) in Watts.
+
+\paragraph{Refrigeration Transcritical System Total High Pressure Compressor Electric Energy {[}J{]}}\label{refrigeration-transcritical-system-total-high-pressure-compressor-electric-energy-j}
+
+This is the electricity consumption of the system's high pressure compressor(s) in Joules for the timestep being reported.~ The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Transcritical System Low Pressure Compressor Electric Power {[}W{]}}\label{refrigeration-transcritical-system-low-pressure-compressor-electric-power-w}
+
+This output is the total electric power input to the system's low pressure compressor(s) in Watts.
+
+\paragraph{Refrigeration Transcritical System Low Pressure Compressor Electric Energy {[}J{]}}\label{refrigeration-transcritical-system-low-pressure-compressor-electric-energy-j}
+
+This is the electricity consumption of the system's low pressure compressor(s) in Joules for the timestep being reported.~ The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Transcritical System Total Compressor Electric Energy {[}J{]}}\label{refrigeration-transcritical-system-total-compressor-electric-energy-j}
+
+This output is the total electric power input to all of the system's compressor(s) in Watts.
+
+\paragraph{Refrigeration Transcritical System Average COP {[}W/W{]}}\label{refrigeration-transcritical-system-average-cop-ww}
+
+This output is the system average compressor COP, which is the total refrigeration effect divided by the total power to all of the compressors.
+
+\paragraph{Refrigeration Transcritical System Medium Temperature Cases and Walk Ins Heat Transfer Rate {[}W{]}}\label{refrigeration-transcritical-system-medium-temperature-cases-and-walk-ins-heat-transfer-rate-w}
+
+This output is the total heat transfer rate from the medium temperature refrigerated cases and walk-ins served directly by this system in Watts.~ It is the sum of all of the heat transfer rates for the medium temperature refrigerated cases and walk-ins that are connected directly to this system.
+
+\paragraph{Refrigeration Transcritical System Medium Temperature Cases and Walk Ins Heat Transfer Energy {[}J{]}}\label{refrigeration-transcritical-system-medium-temperature-cases-and-walk-ins-heat-transfer-energy-j}
+
+This output is the total heat transfer energy from the medium temperature refrigerated cases and walk-ins served directly by this system in Joules. It is the sum of all of the heat transferred for the medium temperature refrigerated cases and walk-ins that are connected directly to this system.
+
+\paragraph{Refrigeration Transcritical System Low Temperature Cases and Walk Ins Heat Transfer Rate {[}W{]}}\label{refrigeration-transcritical-system-low-temperature-cases-and-walk-ins-heat-transfer-rate-w}
+
+This output is the total heat transfer rate from the low temperature refrigerated cases and walk-ins served directly by this system in Watts.~ It is the sum of all of the heat transfer rates for the low temperature refrigerated cases and walk-ins that are connected directly to this system.
+
+\paragraph{Refrigeration Transcritical System Low Temperature Cases and Walk Ins Heat Transfer Energy {[}J{]}}\label{refrigeration-transcritical-system-low-temperature-cases-and-walk-ins-heat-transfer-energy-j}
+
+This output is the total heat transfer energy from the low temperature refrigerated cases and walk-ins served directly by this system in Joules. It is the sum of all of the heat transferred for the low temperature refrigerated cases and walk-ins that are connected directly to this system.
+
+\paragraph{Refrigeration Transcritical System Total Cases and Walk Ins Heat Transfer Energy {[}J{]}}\label{refrigeration-transcritical-system-total-cases-and-walk-ins-heat-transfer-energy-j}
+
+This output is the total heat transfer energy from all the low- and medium-temperature refrigerated cases and walk-ins served directly by this system in Joules. It is the sum of all of the heat transferred for all the refrigerated cases and walk-ins that are connected directly to this system.
+
+\paragraph{Refrigeration Transcritical System Medium Temperature Suction Pipe Heat Transfer Rate {[}W{]}}\label{refrigeration-transcritical-system-medium-temperature-suction-pipe-heat-transfer-rate-w}
+
+This output is the total heat transfer rate for the medium-temperature suction piping served by this system in Watts.~ Note this is an optional input, and is only available if the user has described the medium-temperature suction piping heat gain characteristics in the input.
+
+\paragraph{Refrigeration Transcritical System Medium Temperature Suction Pipe Heat Transfer Energy {[}J{]}}\label{refrigeration-transcritical-system-medium-temperature-suction-pipe-heat-transfer-energy-j}
+
+This output is the total heat transfer rate for the medium-temperature suction piping served by this system in Watts.~ Note this is an optional input, and is only available if the user has described the medium-temperature suction piping heat gain characteristics in the input.
+
+\paragraph{Refrigeration Transcritical System Low Temperature Suction Pipe Heat Transfer Rate {[}W{]}}\label{refrigeration-transcritical-system-low-temperature-suction-pipe-heat-transfer-rate-w}
+
+This output is the total heat transfer rate for the low-temperature suction piping served by this system in Watts.~ Note this is an optional input, and is only available if the user has described the low-temperature suction piping heat gain characteristics in the input.
+
+\paragraph{Refrigeration Transcritical System Low Temperature Suction Pipe Heat Transfer Energy {[}J{]}}\label{refrigeration-transcritical-system-low-temperature-suction-pipe-heat-transfer-energy-j}
+
+This output is the total heat transfer rate for the low-temperature suction piping served by this system in Watts.~ Note this is an optional input, and is only available if the user has described the low-temperature suction piping heat gain characteristics in the input.
+
+\paragraph{Refrigeration Transcritical System High Pressure Compressor Heat Transfer Rate {[}W{]}}\label{refrigeration-transcritical-system-high-pressure-compressor-heat-transfer-rate-w}
+
+This output is the total heat transfer rate of the high pressure Compressors in Watts.~ It is the sum of all of the heat transfer rates for the low- and medium-temperature refrigerated cases and walk-ins as well as the low pressure compressors that are cooled by this system.~ This value does not include compressor or condenser fan heat.~ If specified as in input value, the suction pipe heat gains are included in this value.
+
+\paragraph{Refrigeration Transcritical System High Pressure Compressor Heat Transfer Energy {[}J{]}}\label{refrigeration-transcritical-system-high-pressure-compressor-heat-transfer-energy-j}
+
+This is the total heat transfer of the high pressure compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Transcritical System Low Pressure Compressor Heat Transfer Rate {[}W{]}}\label{refrigeration-transcritical-system-low-pressure-compressor-heat-transfer-rate-w}
+
+This output is the total heat transfer rate of the low pressure Compressors in Watts.~ It is the sum of all of the heat transfer rates for the low temperature refrigerated cases and walk-ins that are cooled by this system.~ This value does not include compressor or condenser fan heat.~ If specified as in input value, the suction pipe heat gains are included in this value.
+
+\paragraph{Refrigeration Transcritical System Low Pressure Compressor Heat Transfer Energy {[}J{]}}\label{refrigeration-transcritical-system-low-pressure-compressor-heat-transfer-energy-j}
+
+This is the total heat transfer of the low pressure compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Transcritical System Net Rejected Heat Transfer Rate {[}W{]}}\label{refrigeration-transcritical-system-net-rejected-heat-transfer-rate-w}
+
+This output is the total heat rejected by this system to the system gas cooler in Watts.~ It does not include system heat rejection that has been recovered for useful purposes.
+
+\paragraph{Refrigeration Transcritical System Net Rejected Heat Transfer Energy {[}J{]}}\label{refrigeration-transcritical-system-net-rejected-heat-transfer-energy-j}
+
+This output is the total heat rejected by this system to the system gas cooler in Joules for the timestep being reported.~ It does not include system heat rejection that has been recovered for useful purposes.
+
+\paragraph{Refrigeration Transcritical System Estimated Refrigerant Inventory Mass {[}kg{]}}\label{refrigeration-transcritical-system-estimated-refrigerant-inventory-mass-kg}
+
+This output is the sum of the input refrigerant inventory values for the gas cooler, receiver, cases, and liquid pipes that are a part of this system.
+
+\paragraph{Refrigeration Transcritical System Refrigerant Mass Flow Rate {[}kg/s{]}}\label{refrigeration-transcritical-system-refrigerant-mass-flow-rate-kgs}
+
+This output is the calculated refrigerant mass flow rate through the high pressure compressors for this system.
+
+\paragraph{Refrigeration Transcritical System Medium Temperature Evaporating Temperature {[}C{]}}\label{refrigeration-transcritical-system-medium-temperature-evaporating-temperature-c}
+
+This is the saturated evaporating temperature for the medium temperature loads.
+
+\paragraph{Refrigeration Transcritical System Medium Temperature Suction Temperature {[}C{]}}\label{refrigeration-transcritical-system-medium-temperature-suction-temperature-c}
+
+This is the temperature at the high pressure compressor inlet including superheat after the display cases and superheat from the suction line heat exchanger.
+
+\paragraph{Refrigeration Transcritical System Low Temperature Evaporating Temperature {[}C{]}}\label{refrigeration-transcritical-system-low-temperature-evaporating-temperature-c}
+
+This is the saturated evaporating temperature for the low-temperature loads.
+
+\paragraph{Refrigeration Transcritical System Low Temperature Suction Temperature {[}C{]}}\label{refrigeration-transcritical-system-low-temperature-suction-temperature-c}
+
+This is the temperature at the low pressure compressor inlet including superheat after the display cases.
+
+\subsection{Refrigeration:Compressor}\label{refrigerationcompressor}
+
+The compressors are described here using manufacturer's data for curves that provide the efficiency, cooling capacity, and power consumption.~ The corresponding rated values for cycle superheat and subcooling are also required.
+
+\textbf{A dataset has been provided containing the compressor rating data, including the performance curve inputs, for a large number of compressors.~ See RefrigerationCompressorCurves.idf.}
+
+\subsubsection{Inputs}\label{inputs-5-023}
+
+\paragraph{Field: Name}\label{field-name-6-017}
+
+A unique user-assigned name for an instance of a compressor. Any reference to this compressor by another object will use this name.
+
+\paragraph{Field: Refrigeration Compressor Power Curve Name}\label{field-refrigeration-compressor-power-curve-name}
+
+This required field provides the name of the curve object that describes the compressor power as a function of the evaporating and condensing temperatures, as specified in ARI 540. The curve is of the bicubic form(ref: Curve:Bicubic).~ However, the input order for the Energy Plus bicubic curve does not match the ARI 540 standard order. When this curve is entered, the user should use the following assignments:
+
+N1 is ARI C1 and N2 is ARI C2.
+
+N3 is ARI C4 and N4 is ARI C3.
+
+N5 is ARI C6 and N6 is ARI C5,
+
+N7 is ARI C7.
+
+N8 is ARI C10, N9 is ARI C8, and N10 is ARI C9.
+
+N11 is the Minimum evaporating temperature and N12 is the Maximum evaporating temperature.
+
+N13 is the the Minimum condensing temperature and N14 is the Maximum condensing temperature
+
+\paragraph{Field: Refrigeration Compressor Capacity Curve Name}\label{field-refrigeration-compressor-capacity-curve-name}
+
+This required field provides the name of the curve object that describes the compressor cooling capacity as a function of the evaporating and condensing temperatures, as specified in ARI 540. The curve is of the bicubic form(ref: Curve:Bicubic).~ However, the input order for the Energy Plus bicubic curve does not match the ARI 540 standard order. When this curve is entered, the user should use the following assignments:
+
+N1 is ARI C1 and N2 is ARI C2.
+
+N3 is ARI C4 and N4 is ARI C3.
+
+N5 is ARI C6 and N6 is ARI C5,
+
+N7 is ARI C7.
+
+N8 is ARI C10, N9 is ARI C8, and N10 is ARI C9.
+
+N11 is the Minimum evaporating temperature and N12 is Maximum evaporating temperature.
+
+N13 is the Minimum condensing temperature and N14 is the Maximum condensing temperature
+
+\paragraph{Field: Rated Superheat}\label{field-rated-superheat}
+
+Some manufacturers specify a constant return gas temperature while others specify a constant superheat (the difference between the saturated evaporating temperature and the actual return gas temperature). Use this field for compressors that provide their rated superheat. (Do NOT use both this field and the Rated Return Gas Temperature field.) The rated superheat is specified in units of delta C.
+
+\paragraph{Field: Rated Return Gas Temperature}\label{field-rated-return-gas-temperature}
+
+Some manufacturers specify a constant return gas temperature ( which may also be called the Rated Suction Temperature) while others specify a constant superheat.~ Use this field for compressors that provide their rated return gas temperature. (Do NOT use both this field and the Rated Superheat field.) The rated return gas temperature is specified in units of C.
+
+\paragraph{Field: Rated Liquid Temperature}\label{field-rated-liquid-temperature}
+
+Some compressor manufactures rate their equipment according to a constant subcooling (the difference between the saturated condensing temperature and the actual liquid temperature entering the thermal expansion valve before the refrigeration load). Other manufacturers specify a constant liquid temperature.Use this field if the manufacturer specifies the rated liquid temperature.~ (Do NOT use both this field and the Rated Subcooling field.) The units for this field are degrees C.
+
+\paragraph{Field: Rated Subcooling}\label{field-rated-subcooling}
+
+Some compressor manufactures rate their equipment according to a constant subcooling (the difference between the saturated condensing temperature and the actual liquid temperature entering the thermal expansion valve before the refrigeration load). Other manufacturers specify a constant liquid temperature.Use this field if the manufacturer specifies the rated subcooling.~ (Do NOT use both this field and the Rated Liquid Temperature field.) The units for this field are delta C.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-3-001}
+
+This field allows the specification of a user-defined end-use subcategory (e.g., ``Low Temperature System''). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+The following is an example input for a refrigeration compressor.
+
+\begin{lstlisting}
+
+Refrigeration:Compressor,
+      CompressorA,             !- Name
+      PowerCurveCompA,         !- Refrigeration Compressor Power Curve Name
+      CapCurveCompA,           !- Refrigeration Compressor Capacity Curve Name
+      10.0,                    ! – Rated Superheat {delta C}
+      ,                        !- Rated Return Gas Temperature {C}
+      ,                        ! – Rated Liquid Temperature{C}
+      15.0,                    !- Rated Subcooling {delta C}
+      MedTempRefrig;           !- End-Use Subcategory
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-013}
+
+THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE CASES AND/OR WALKINS:
+
+\begin{itemize}
+\item
+  Zone,Average,Refrigeration Compressor Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Compressor Electric Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Compressor Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Compressor Heat Transfer Energy {[}J{]}
+\item
+  Zone,Sum,Refrigeration Compressor Run Time~Fraction {[]}
+\end{itemize}
+
+THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE AIR CHILLERS:
+
+\begin{itemize}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Compressor Electric Power {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Air Chiller System Compressor Electric Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller System Compressor Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Air Chiller System Compressor Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Chiller Compressor Run TimeFraction {[]}
+\end{itemize}
+
+\paragraph{THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE CASES AND/OR WALKINS}\label{the-following-outputs-are-available-for-systems-that-serve-cases-andor-walkins-1}
+
+\paragraph{Refrigeration Compressor Electric Power {[}W{]}}\label{refrigeration-compressor-electric-power-w}
+
+This output is the electric power input to the compressor in Watts.
+
+\paragraph{Refrigeration Compressor Electric Energy {[}J{]}}\label{refrigeration-compressor-electric-energy-j}
+
+This is the electric energy consumed by the compressor in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Compressor Heat Transfer Rate {[}W{]}}\label{refrigeration-compressor-heat-transfer-rate-w}
+
+This output is the heat removed from the refrigerated cases by the compressor in Watts.
+
+\paragraph{Refrigeration Compressor~ Heat Transfer Energy {[}J{]}}\label{refrigeration-compressor-heat-transfer-energy-j}
+
+This is the heat removed from the refrigerated cases by the compressor in Joules for the timestep being reported.
+
+\paragraph{\texorpdfstring{Refrigeration Compressor Run Time~ Fraction {[]}}{Refrigeration Compressor Run Time~ Fraction }}\label{refrigeration-compressor-run-time-fraction}
+
+This is the fraction of the time step when the compressor ran to meet the load.~ It is a value between 0.0 and 1.0.
+
+\paragraph{THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE AIR CHILLERS}\label{the-following-outputs-are-available-for-systems-that-serve-air-chillers-1}
+
+\paragraph{Refrigeration Air Chiller System Compressor Electric Power {[}W{]}}\label{refrigeration-air-chiller-system-compressor-electric-power-w}
+
+This output is the electric power input to the compressor in Watts.
+
+\paragraph{Refrigeration Air Chiller System Compressor Electric Energy {[}J{]}}\label{refrigeration-air-chiller-system-compressor-electric-energy-j}
+
+This is the electric energy consumed by the compressor in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller System Compressor Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-compressor-heat-transfer-rate-w}
+
+This output is the heat removed from the refrigerated cases by the compressor in Watts.
+
+\paragraph{Refrigeration Air Chiller System Compressor Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-compressor-heat-transfer-energy-j}
+
+This is the heat removed from the refrigerated cases by the compressor in Joules for the timestep being reported.
+
+\paragraph{\texorpdfstring{Refrigeration Chiller Compressor Run Time~ Fraction {[]}}{Refrigeration Chiller Compressor Run Time~ Fraction }}\label{refrigeration-chiller-compressor-run-time-fraction}
+
+This is the fraction of the time step when the compressor ran to meet the load.~ It is a value between 0.0 and 1.0.
+
+\subsection{Refrigeration:CompressorList}\label{refrigerationcompressorlist}
+
+This object provides a list of all the compressors included within a single refrigeration system (Ref: Refrigeration:System). Each list must contain at least one compressor. The order in which the individual compressors are listed here will be the order in which the compressors are dispatched to meet the system load.~ That is, at very low loads, only compressor \#1 will be operating.~ As the load increases, the first two compressors will be operating, and so on. This list is extensible.
+
+\subsubsection{Inputs}\label{inputs-6-020}
+
+\paragraph{Field: Name}\label{field-name-7-016}
+
+A unique user-assigned name for an instance of a compressor list. Any reference to this compressor list by another object will use this name. The compressor list cannot have the same name as any individual compressor.
+
+\paragraph{Field: Refrigeration Compressor \textless{}x\textgreater{} Name}\label{field-refrigeration-compressor-x-name}
+
+Identifies a particular compressor that works in conjunction with the other compressors on this list to provides cooling to a single refrigeration system. The name will be validated against the compressor names (ref: Refrigeration:Compressor) in the input file. Up to 20 are available in the IDD; this object is extensible.
+
+The following is an example input for a compressor list.
+
+\begin{lstlisting}
+
+Refrigeration:CompressorList,
+      MediumTempCompressorlist, !- Refrigeration Compressor List Name
+      CompressorA,             !- Refrigeration Compressor Name \#1
+      CompressorB,             !- Refrigeration Compressor Name \#2
+      CompressorC;             !- Refrigeration Compressor Name \#3
+\end{lstlisting}
+
+\subsection{Refrigeration:Subcooler}\label{refrigerationsubcooler}
+
+Two types of subcoolers are modeled by the detailed refrigeration system.~ As described in the Engineering Reference, the liquid suction heat exchanger uses cool suction gas to subcool the hot condensate after it leaves the condenser and before it reaches the thermal expansion valve.~ For the liquid suction heat exchanger, both the source and sink of energy are located within the same refrigeration system.~ In contrast, a mechanical subcooler is used to transfer cooling capacity from one refrigeration system to another. The mechanical subcooler is listed as a part of the system for which the condensate is cooled.~ However, the input data for the mechanical subcooler includes a field that identifies the system that provides the cooling capacity.
+
+\subsubsection{Inputs}\label{inputs-7-020}
+
+\paragraph{Field: Name}\label{field-name-8-016}
+
+A unique user-assigned name for an instance of a subcooler. Any reference to this subcooler by another object will use this name.
+
+\paragraph{Field: Subcooler Type}\label{field-subcooler-type}
+
+The type of subcooler. Valid choices are Mechanical and LiquidSuction.~ If the field is blank, the default will be LiquidSuction.
+
+\paragraph{Field: Liquid Suction Design Subcooling Temperature Difference}\label{field-liquid-suction-design-subcooling-temperature-difference}
+
+This numeric field is the design subcooling temperature difference (DeltaC) for a liquid suction heat exchanger and should be blank for a mechanical subcooler.
+
+\paragraph{Field: Design Liquid Inlet Temperature}\label{field-design-liquid-inlet-temperature}
+
+This numeric field is the design inlet temperature (C) for the hot liquid entering a liquid suction heat exchanger and should be blank for a mechanical subcooler.
+
+\paragraph{Field: Design Vapor Inlet Temperature}\label{field-design-vapor-inlet-temperature}
+
+This numeric field is the design inlet temperature (C) for the cool vapor entering a liquid suction heat exchanger and should be blank for a mechanical subcooler.
+
+\paragraph{Field: Capacity-Providing System}\label{field-capacity-providing-system}
+
+This field is the name of the refrigeration system object that provides the cooling capacity for the mechanical subcooler (ref: Refrigeration:System Name). This field should be blank for a liquid suction heat exchanger.
+
+\paragraph{Field: Outlet Control Temperature}\label{field-outlet-control-temperature}
+
+This numeric field is the controlled outlet temperature (C) for subcooled liquid exiting a mechanical subcooler. This field should be blank for a liquid suction heat exchanger.
+
+The following is example input for both liquid suction and mechanical subcoolers.
+
+\begin{lstlisting}
+
+REFRIGERATION:SUBCOOLER,
+         SampleLSHx,          !Subcooler Name
+         LiquidSuction,             !subcooler type
+         6,                   !design liquid suction subcooling {deltaC}
+         16,                  !design inlet temperature on liquid side {C}
+         0,                   !design inlet temperature on vapor side {C}
+         ,                    !Refrigeration System Detailed Name providing cooling capacity
+         ;                    !Control Temperature Out for subcooled liquid {C}
+\end{lstlisting}
+
+! Mechanical Subcooler (uses Med Temp System to cool low temp liquid to 10C)
+
+\begin{lstlisting}
+
+  REFRIGERATION:SUBCOOLER,
+         SampleMSC,           !Subcooler Name
+         Mechanical,          !subcooler type
+         ,                    !design liquid suction subcooling {C}
+         ,                    !design inlet temperature on liquid side {C}
+         ,                    !design inlet temperature on vapor side {C}
+         MediumTempSystem,    !Refrigeration System Detailed Name providing cooling capacity
+         10;                  !Control Temperature Out for subcooled liquid {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-008}
+
+FOR SUBCOOLERS ON SYSTEMS SERVING CASES AND/OR WALKINS:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration System Mechanical Subcooler Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration System Mechanical Subcooler Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+FOR SUBCOOLERS ON SYSTEMS SERVING AIR CHILLERS:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration Air Chiller System Mechanical Subcooler Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Air Chiller System Mechanical Subcooler Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{FOR SUBCOOLERS ON SYSTEMS SERVING CASES AND/OR WALKINS:}\label{for-subcoolers-on-systems-serving-cases-andor-walkins}
+
+\paragraph{Refrigeration System Mechanical Subcooler Heat Transfer Rate {[}W{]}}\label{refrigeration-system-mechanical-subcooler-heat-transfer-rate-w}
+
+This output is the cooling energy transferred from one system's compressor group to the refrigerant leaving the condenser for another refrigeration system in Watts.
+
+\paragraph{Refrigeration System Mechanical Subcooler Heat Transfer Energy {[}J{]}}\label{refrigeration-system-mechanical-subcooler-heat-transfer-energy-j}
+
+This output is the cooling energy transferred from one system's compressor group to the refrigerant leaving the condenser for another refrigeration system in Joules.
+
+\paragraph{FOR SUBCOOLERS ON SYSTEMS SERVING AIR CHILLERS}\label{for-subcoolers-on-systems-serving-air-chillers}
+
+\paragraph{Refrigeration Air Chiller System Mechanical Subcooler Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-mechanical-subcooler-heat-transfer-rate-w}
+
+This output is the cooling energy transferred from one system's compressor group to the refrigerant leaving the condenser for another refrigeration system in Watts.
+
+\paragraph{Refrigeration Air Chiller System Mechanical Subcooler Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-mechanical-subcooler-heat-transfer-energy-j-1}
+
+This output is the cooling energy transferred from one system's compressor group to the refrigerant leaving the condenser for another refrigeration system in Joules.
+
+\subsection{Refrigeration:Condenser:AirCooled}\label{refrigerationcondenseraircooled}
+
+The refrigeration system requires a single condenser to reject the system heat.~ The air cooled condenser object is one of four options for this condenser. In an air-cooled condenser, the total heat of rejection is characterized by a linear relationship between the difference between the inlet air (usually the outside drybulb) and condensing temperatures. This curve is commonly found in the condenser manufacturers' literature. This rating curve, which corresponds to ARI 460 standards, also has an associated rated value for subcooling that should be entered. The rated condenser fan power and fan speed control type must be specified. If the condenser is not at ground level, the user may specify an air inlet node name (ref: OutdoorAir:Node name). If the condenser is located inside a conditioned zone, the zone name may be specified(ref: bbbZoneNamebbb). Optional input is provided to help the user compare refrigerant inventories for different systems.~ These inputs represent the design values for the refrigerant inventory within the condenser, within a receiver beneath the condenser, and in the liquid pipes between the condenser and the refrigerated cases.
+
+\subsubsection{Inputs}\label{inputs-8-018}
+
+\paragraph{Field: Name}\label{field-name-9-014}
+
+Identifies a particular condenser that rejects heat for a one or more refrigeration system(s). The name must be unique and will be validated against all the condenser names (ref: Refrigeration:Condenser:*) in the input file, including names used for evaporative-cooled, water-cooled, and cascade-cooled condensers.
+
+\paragraph{Field: Rated Effective Total Heat Rejection Rate Curve Name}\label{field-rated-effective-total-heat-rejection-rate-curve-name}
+
+This field is the name of a curve object defining the condenser heat rejection as a function of the difference between the condensing and entering air temperatures. The curve should be linear (Curve:Linear). See the Engineering Reference for more discussion on the curve coefficients.
+
+\paragraph{Field: Rated Subcooling Temperature Difference}\label{field-rated-subcooling-temperature-difference}
+
+This numeric field specifies the rated subcooling (DeltaC) specified by the manufacturer, consistent with the heat rejection curve rating data.
+
+\paragraph{Field: Condenser Fan Speed Control Type}\label{field-condenser-fan-speed-control-type}
+
+The type of fan speed control used by the condenser fan. Valid choices are \textbf{Fixed}, \textbf{FixedLinear,} \textbf{VariableSpeed}, and \textbf{TwoSpeed}.~ If the field is blank, \textbf{Fixed} will be used. See the Engineering Reference for a discussion of this option's effect on fan energy consumption.
+
+\paragraph{Field: Rated Fan Power}\label{field-rated-fan-power-000}
+
+This numeric field specifies the rated fan power (W) specified by the manufacturer, under standard rating conditions.
+
+\paragraph{Field: Minimum Fan Air Flow Ratio}\label{field-minimum-fan-air-flow-ratio}
+
+Fan controls often include a minimum air flow ratio to avoid overheating the fan motor or for other reasons. This numeric field should be between 0. and 1. and has a default value of 0.2\textbf{.}
+
+\paragraph{Field: Air Inlet Node Name or Zone Name}\label{field-air-inlet-node-name-or-zone-name}
+
+This optional alpha field contains the name of the node from which the condenser draws its outdoor air or the name of the conditioned zone where the condenser is located. If this field is left blank, the outdoor air drybulb temperature entering the condenser is taken directly from the weather data. If this field is not blank and an outdoor air node name is entered, this node name must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If a zone name is entered, the temperature of that zone is used.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-4-001}
+
+This field allows the specification of a user-defined end-use subcategory (e.g., ``Low Temperature Rack''). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Condenser Refrigerant Operating Charge Inventory}\label{field-condenser-refrigerant-operating-charge-inventory}
+
+This numeric field specifies the amount of refrigerant present within the condenser (kg) specified by the manufacturer, under standard rating conditions.
+
+\paragraph{Field: Condensate Receiver Refrigerant Inventory}\label{field-condensate-receiver-refrigerant-inventory}
+
+This numeric field specifies the amount of refrigerant present within the condensate receiver (kg) specified by the manufacturer or system designer, under standard rating conditions.
+
+\paragraph{Field: Condensate Piping Refrigerant Inventory}\label{field-condensate-piping-refrigerant-inventory}
+
+This numeric field specifies the amount of refrigerant present within the condensate piping (kg) specified by the system designer, under standard rating conditions.
+
+The following is an example input for an air-cooled condenser.
+
+\begin{lstlisting}
+
+Refrigeration:Condenser:AirCooled,
+      MediumTempCondenser,     !- Name of condenser
+      MediumTempCondenserHRCurve, !-name of condenser heat of rejection curve, linear
+      0.,                      ! Rated subcooling {deltaC}
+      VariableSpeed,           ! Fan speed control type
+      4000.,                   ! Design condenser fan power {W}
+      0.25,                    !Minimum air flow fraction through condenser fan {dimensionless}
+      Refrigeration MediumTempSystem CondenserNode,  !- Condenser Air Inlet Node Name or Zone Name
+      MediumTempRefrig;        !- End-Use Subcategory
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-008}
+
+FOR CONDENSERS COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration System Condenser Fan Electric Power {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Fan Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Total Recovered Heat Transfer Rate {[}W{]} Zone, Sum, Refrigeration System Condenser Total Recovered Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Heat Recovered for Non-Refrigeration Purposes Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Defrost Recovered Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+FOR CONDENSERS COOLING SYSTEMS SERVING AIR CHILLERS:
+
+\begin{itemize}
+\item
+  HVAC,Average, Refrigeration System Condenser Fan Electric Power {[}W{]}
+\item
+  HVAC, Sum, Refrigeration System Condenser Fan Electric Consumption {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate {[}W{]} HVAC, Sum, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{FOR CONDENSERS ON SYSTEMS SERVING CASES AND/OR WALKINS:}\label{for-condensers-on-systems-serving-cases-andor-walkins}
+
+\paragraph{Refrigeration System Condenser Fan Electric Power {[}W{]}}\label{refrigeration-system-condenser-fan-electric-power-w}
+
+This output is the electric input to the system's condenser fan(s) in Watts.
+
+\paragraph{Refrigeration System Condenser Fan Electric Consumption {[}J{]}}\label{refrigeration-system-condenser-fan-electric-consumption-j}
+
+This is the electricity consumption of the system's condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration System Condenser Heat Transfer Rate {[}W{]}}\label{refrigeration-system-condenser-heat-transfer-rate-w}
+
+This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration load minus any heat recovered for defrost or other purposes).
+
+\paragraph{Refrigeration System Condenser Heat Transfer Energy {[}J{]}}\label{refrigeration-system-condenser-heat-transfer-energy-j}
+
+This is the total heat energy flowing across the condenser for the timestep being reported~ (i.e., compressor energy and refrigeration load minus any heat recovered for defrost or other purposes).
+
+\paragraph{Refrigeration System Condenser Total Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-system-condenser-total-recovered-heat-transfer-rate-w}
+
+This is the total heat recovered from the condenser inlet flow for all purposes including defrost and water or air heating.
+
+\paragraph{Refrigeration System Condenser Total Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-system-condenser-total-recovered-heat-transfer-energy-j}
+
+This is the total heat recovered from the condenser inlet flow for all purposes including defrost and water or air heating for the timestep being reported.
+
+\paragraph{Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate~ {[}W{]}}\label{refrigeration-system-condenser-non-refrigeration-recovered-heat-transfer-rate-w}
+
+This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating.
+
+\paragraph{Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-system-condenser-non-refrigeration-recovered-heat-transfer-energy-j}
+
+This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating for the timestep being reported.
+
+\paragraph{Refrigeration System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-system-condenser-defrost-recovered-heat-transfer-rate-w}
+
+This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system.
+
+\paragraph{Refrigeration System Condenser Defrost Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-system-condenser-defrost-recovered-heat-transfer-energy-j}
+
+This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
+
+\paragraph{FOR CONDENSERS ON SYSTEMS SERVING AIR CHILLERS:}\label{for-condensers-on-systems-serving-air-chillers}
+
+\paragraph{Refrigeration Air Chiller System Condenser Fan Electric Power {[}W{]}}\label{refrigeration-air-chiller-system-condenser-fan-electric-power-w}
+
+This output is the electric input to the system's condenser fan(s) in Watts.
+
+\paragraph{Refrigeration Air Chiller System Condenser Fan Electric Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-fan-electric-energy-j}
+
+This is the electricity consumption of the system's condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller System Condenser Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-condenser-heat-transfer-rate-w}
+
+This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration load minus any heat recovered for defrost or other purposes).
+
+\paragraph{Refrigeration Air Chiller System Condenser Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-heat-transfer-energy-j}
+
+This is the total heat energy flowing across the condenser for the timestep being reported~ (i.e., compressor energy and refrigeration load minus any heat recovered for defrost or other purposes).
+
+\paragraph{Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-condenser-total-recovered-heat-transfer-rate-w}
+
+This is the total heat recovered from the condenser inlet flow for all purposes including defrost and water or air heating.
+
+\paragraph{Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-total-recovered-heat-transfer-energy-j}
+
+This is the total heat recovered from the condenser inlet flow for all purposes including defrost and water or air heating for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate~ {[}W{]}}\label{refrigeration-air-chiller-system-condenser-non-refrigeration-recovered-heat-transfer-rate-w}
+
+This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating.
+
+\paragraph{Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-non-refrigeration-recovered-heat-transfer-energy-j}
+
+This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-condenser-defrost-recovered-heat-transfer-rate-w}
+
+This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system.
+
+\paragraph{Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-defrost-recovered-heat-transfer-energy-j}
+
+This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
+
+\subsection{Refrigeration:Condenser:EvaporativeCooled}\label{refrigerationcondenserevaporativecooled}
+
+Each refrigeration system requires a single condenser.~ The evaporative cooled condenser object is one of four options for this condenser. In an evaporative-cooled condenser, the total heat of rejection is characterized by a four-factor relationship between the condensing temperature and the difference between the outside wetbulb and condensing temperatures. This curve must be developed by regression from the condenser manufacturers' literature. This rating curve, which is based upon rated data taken according to ARI 460 standards, also has an associated rated value for subcooling that should be entered. The rated condenser fan power and fan speed control type must be specified. If the condenser is not at ground level, the user may specify an air inlet node name (ref: OutdoorAir:Node name). Optional input is provided to help the user compare refrigerant inventories for different systems.~ These input represent the design values for the refrigerant inventory within the condenser, within a receiver beneath the condenser, and in the liquid pipes between the condenser and the refrigerated cases.
+
+Additional inputs are needed for basin heater parameters, water pump power, and water source. An evaporative cooling availability schedule is available.
+
+\subsubsection{Inputs}\label{inputs-9-016}
+
+\paragraph{Field: Name}\label{field-name-10-013}
+
+Identifies a particular condenser that rejects heat for a one or more refrigeration system(s). The name must be unique and will be validated against all the condenser names (ref: Refrigeration:Condenser:*) in the input file, including names used for air-cooled, water-cooled and cascade-cooled condensers.
+
+\paragraph{Field: Rated Effective Total Heat Rejection Rate}\label{field-rated-effective-total-heat-rejection-rate}
+
+This numeric field should be the rated heat rejection effect (W) at standard rating conditions per ARI 490.~ Be sure the rating corresponds to the correct refrigerant.
+
+\paragraph{Field: Rated Subcooling Temperature Difference}\label{field-rated-subcooling-temperature-difference-1}
+
+This numeric field specifies the rated subcooling (DeltaC) specified by the manufacturer, consistent with the rated value for total heat rejection.
+
+\paragraph{Field: Fan Speed Control Type}\label{field-fan-speed-control-type}
+
+The type of fan speed control used by the condenser fan. Valid choices are \textbf{Fixed}, \textbf{FixedLinear}, \textbf{VariableSpeed}, and \textbf{TwoSpeed}.~ If the field is blank, \textbf{Fixed} will be used. See the Engineering Reference for a discussion of this option's effect on fan energy consumption.
+
+\paragraph{Field: Rated Fan Power}\label{field-rated-fan-power-1-000}
+
+This numeric field specifies the rated fan power (W) specified by the manufacturer, under standard rating conditions.
+
+\paragraph{Field: Minimum Fan Air Flow Ratio}\label{field-minimum-fan-air-flow-ratio-1}
+
+Fan controls often include a minimum air flow ratio to avoid overheating the fan motor or for other reasons. This numeric field has a minimum value of 0. and a default value of 0.2.
+
+\paragraph{Field: Approach Temperature Constant Term}\label{field-approach-temperature-constant-term}
+
+As described in the Engineering Reference (ref Refrigeration:Condenser:Evaporative), the heat rejection capacity factor is specified according to the form (where Twetbulb and Tcondense are in C):
+
+Tcondense = A1 + A2(hrcf) + A3/(hrcf) + (1 + A4)(Twb)
+
+This numeric field is the value for A1 and has a default value of 6.63, a minimum of 0. and a maximum of 20. (C)
+
+\paragraph{Field: Approach Temperature Coefficient 2}\label{field-approach-temperature-coefficient-2}
+
+As described in the Engineering Reference (ref Refrigeration:Condenser:Evaporative), the heat rejection capacity factor is specified according to the form (where Twetbulb and Tcondense are in C):
+
+Tcondense = A1 + A2(hrcf) + A3/(hrcf) + (1 + A4)(Twb)
+
+This numeric field is the value for A2 and has a default value of 0.468, a minimum of 0, and a maximum of 20 (C).
+
+\paragraph{Field: Approach Temperature Coefficient 3}\label{field-approach-temperature-coefficient-3}
+
+As described in the Engineering Reference (ref Refrigeration:Condenser:Evaporative), the heat rejection capacity factor is specified according to the form (where Twetbulb and Tcondense are in C):
+
+Tcondense = A1 + A2(hrcf) + A3/(hrcf) +(1 + A4)(Twb)
+
+This numeric field is the value for A3 and has a default value of 17.93, a minimum of 0, and a maximum of 30 (C).
+
+\paragraph{Field: Approach Temperature Coefficient 4}\label{field-approach-temperature-coefficient-4}
+
+As described in the Engineering Reference (ref Refrigeration:Condenser:Evaporative), the heat rejection capacity factor is specified according to the form (where Twetbulb and Tcondense are in C):
+
+Tcondense = A1 + A2(hrcf) + A3/(hrcf) + (1 + A4)(Twb)
+
+This numeric field is the value for A4 and has a default value of -0.322, a minimum of -20., and a maximum of 20 (dimensionless).
+
+\paragraph{Field: Minimum Capacity Factor}\label{field-minimum-capacity-factor}
+
+This numeric field is the minimum heat rejection capacity factor in the manufacturer's data used to develop the equation described in the preceding four fields. The default value is 0.5.
+
+\paragraph{Field: Maximum Capacity Factor}\label{field-maximum-capacity-factor}
+
+This numeric field is the maximum heat rejection capacity factor in the manufacturer's data used to develop the equation described in the preceding four fields. The default value is 5.0.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-005}
+
+This optional alpha field contains the name of the node from which the condenser draws its outdoor air. If this field is left blank, the outdoor air drybulb temperature entering the condenser is taken directly from the weather data. If this field is not blank, this node name must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
+
+\paragraph{Field: Rated Air Flow Rate}\label{field-rated-air-flow-rate-000}
+
+The air volume flow rate, in m\(^{3}\)per second, entering the evaporative condenser. This value is used to calculate the amount of water evaporated when evaporatively cooling the condenser inlet air. The value for this field must be greater than zero. This input field is also autocalculatable, equivalent to 0.000144 m\(^{3}\)/s per watt of total cooling capacity {[}850 cfm/ton{]} where the total cooling capacity is the total heat of rejection.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-1-002}
+
+This field defines the power level of the basin heater, if applicable, used to avoid water freezing in an outdoor evaporative cooler basin. This numeric field contains the capacity of the electric basin heater in Watts per degree C. This field is used in conjunction with the Basin Heater Set Point Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the dry-bulb temperature of the condenser coil inlet air. The basin heater only operates when the condenser fan is off (i.e., no compressor heat rejection). The basin heater capacity must be greater than or equal to zero, with a default value of 200 W/C if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-1-002}
+
+This numeric field contains the set point temperature (°C) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this set point temperature, as long as the condenser fan is off. The default value is 2°C if this field is left blank.
+
+\paragraph{Field: Rated Water Pump Power}\label{field-rated-water-pump-power}
+
+The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The value for this field must be greater than or equal to 0, with a default value of 1000 Watts if this field is left blank. This input field is also autocalculatable, equivalent to 0.004266 W per Watt {[}15 W/ton{]} of total cooling capacity.
+
+\paragraph{Field: Evaporative Water Supply Tank Name}\label{field-evaporative-water-supply-tank-name-1}
+
+This field is used to define where the condenser obtains water used for evaporative cooling. If this field is left blank, the unit will obtain water directly from the mains (Ref. Water Mains Temperatures). If the name of a Water Storage Tank object is used here, then the unit will obtain its water from that tank.
+
+\paragraph{Field: Evaporative Condenser Availability Schedule Name}\label{field-evaporative-condenser-availability-schedule-name-1}
+
+For evaporative cooled condensers, the name of the optional schedule (Ref: Schedule) that specifies the time periods that evaporative cooling is available/unavailable. In some colder climates, evaporative cooling is periodically discontinued and the basin sumps drained to avoid freezing and to avoid ice formation on the condenser. In these times, the condenser runs as a typical dry air cooled condenser, and related evaporative cooling systems (e.g., water pump, basin heaters) do not operate. Use of this optional schedule permits modeling of planned, seasonal interruptions of evaporative cooling. All schedule values must be greater than or equal to zero. Typically, an ON/OFF schedule type is used with values being either 0 or 1. A schedule value of 1 indicates that evaporative cooling is available during the defined time period, and a value of 0 denotes that evaporative cooling is not available during the defined time period. If the schedule name is omitted (blank), then the model assumes that evaporative cooling of the condenser is available for the entire simulation period. Note: the use of this schedule is the correct way to model an evaporative condenser in a climate subject to freezing weather.~ However, because some users will take a single model description and run it for a multiple climates, the code also includes an automatic switch from wet to dry operation, as described in the Engineering Reference.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-5-000}
+
+This field allows the specification of a user-defined end-use subcategory (e.g., ``Low Temperature Rack''). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Condenser Refrigerant Operating Charge Inventory}\label{field-condenser-refrigerant-operating-charge-inventory-1}
+
+This numeric field specifies the amount of refrigerant present within the condenser (kg) specified by the manufacturer, under standard rating conditions.
+
+\paragraph{Field: Condensate Receiver Refrigerant Inventory}\label{field-condensate-receiver-refrigerant-inventory-1}
+
+This numeric field specifies the amount of refrigerant present within the condensate receiver (kg) specified by the manufacturer or system designer, under standard rating conditions.
+
+\paragraph{Field: Condensate Piping Refrigerant Inventory}\label{field-condensate-piping-refrigerant-inventory-1}
+
+This numeric field specifies the amount of refrigerant present within the condensate piping (kg) specified by the system designer, under standard rating conditions.
+
+The following is an example input for an evaporative condenser
+
+\begin{lstlisting}
+
+Refrigeration:Condenser:EvaporativeCooled,
+      MedTempEvapCooledCondenser ,  !- Refrigeration Condenser Name
+      64800. ,                    !- Rated Total Heat Rejection Effect, {W}
+      0. ,                        !- Rated Subcooling
+      VariableSpeed ,             !- Condenser Fan Speed Control
+      746.,                       !- Rated Condenser Fan Power
+      0.25,                       !- Minimum air flow fraction through condenser fan {dimensionless}
+      6.63  ,                     !- Evaporative Condenser Approach Temp Const, {C}
+      0.468 ,                     !- Evaporative Condenser Approach Temp HRCF Cooefficient
+      17.93 ,                     !- Evaporative Condenser Approach Temp 1/hrcf coefficient
+      -0.322,                     !- Evaporative Condenser Approach Temp Twb coefficient {1/C}
+      0.6  ,                      !- Minimum Condenser Capacity Factor
+      4.8  ,                      !- Maximum Condenser Capacity Factor
+      Outside Air Inlet Node,     !- Condenser Air Inlet Node Name
+      1.79 ,                      !- Rated Air Flow Rate {m3/s}
+      66.7 ,                      !- Basin Heater Capacity {W/C}
+      1.0  ,                      !- Basin Heater Set Point Temperature {C}
+      250. ,                      !- Rated Water Pump Power {W}
+      EvapWaterStorageTank,       !- Evaporative Water Supply Tank Name
+      EvapCondAvail,              !- Evaporative Condenser Availability Schedule Name
+      ,                           !- End-UseSubcategory
+      21.9 ,                      !- Condenser Refrigerant Operating Charge {kg}
+      10.  ,                      !- Condensate Receiver Refrigerant Inventory
+      25. ;                       !- Condensate Piping Refrigerant Inventory
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-008}
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration System Condenser Fan Electric Power {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Fan Electric Consumption {[}J{]}
+\end{itemize}
+
+FOR CONDENSERS COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration System Condenser Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Total Recovered Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Total Recovered Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Defrost Recovered Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Pump Electric Power {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Pump Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Basin Heater Electric Power {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Basin Heater Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Evaporated Water Volume Flow Rate~ {[}m3/s{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Evaporated Water Volume {[}m3{]}
+\end{itemize}
+
+FOR CONDENSERS COOLING SYSTEMS SERVING AIR CHILLERS:
+
+\begin{itemize}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Pump Electric Power {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Basin Heater Electric Power {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Basin Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Evaporated Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Evaporated Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{FOR CONDENSERS ON SYSTEMS SERVING CASES AND/OR WALKINS:}\label{for-condensers-on-systems-serving-cases-andor-walkins-1}
+
+\paragraph{Refrigeration System Condenser Fan Electric Power {[}W{]}}\label{refrigeration-system-condenser-fan-electric-power-w-1}
+
+This output is the electric input to the system's condenser fan(s) in Watts.
+
+\paragraph{Refrigeration System Condenser Fan Electric Energy {[}J{]}}\label{refrigeration-system-condenser-fan-electric-energy-j}
+
+This is the electricity consumption of the system's condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration System Condenser Heat Transfer Rate {[}W{]}}\label{refrigeration-system-condenser-heat-transfer-rate-w-1}
+
+This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
+
+\paragraph{Refrigeration System Condenser Heat Transfer Energy {[}J{]}}\label{refrigeration-system-condenser-heat-transfer-energy-j-1}
+
+This is the total heat energy flowing across the condenser for the timestep being reported.
+
+\paragraph{Refrigeration System Condenser Total Recovered Heat Transfer Rate~ {[}W{]}}\label{refrigeration-system-condenser-total-recovered-heat-transfer-rate-w-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for any purpose.
+
+\paragraph{Refrigeration System Condenser Total Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-system-condenser-total-recovered-heat-transfer-energy-j-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for any purpose for the timestep being reported.
+
+\paragraph{Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate~ {[}W{]}}\label{refrigeration-system-condenser-non-refrigeration-recovered-heat-transfer-rate-w-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for purposes such as water or air heating.
+
+\paragraph{Refrigeration System Condenser Heat Recovered for Non-Refrigeration Purposes Energy {[}J{]}}\label{refrigeration-system-condenser-heat-recovered-for-non-refrigeration-purposes-energy-j}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for purposes such as water or air heating for the timestep being reported.
+
+\paragraph{Refrigeration System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-system-condenser-defrost-recovered-heat-transfer-rate-w-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for defrost purposes within the refrigeration system..
+
+\paragraph{Refrigeration System Condenser Defrost Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-system-condenser-defrost-recovered-heat-transfer-energy-j-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
+
+\paragraph{Refrigeration System Condenser Pump Electric Power {[}W{]}}\label{refrigeration-system-condenser-pump-electric-power-w}
+
+This is the electrical power requirement in Watts for the timestep being reported for the water pump used with evaporative cooling of the condenser.
+
+\paragraph{Refrigeration System Condenser Pump Electric Energy {[}J{]}}\label{refrigeration-system-condenser-pump-electric-energy-j}
+
+This is the electricity consumption in Joules of the water pump used with evaporative cooling of the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration System Condenser Basin Heater Electric Power {[}W{]}}\label{refrigeration-system-condenser-basin-heater-electric-power-w}
+
+This is the electrical power requirement in Watts for the timestep being reported for the water heater in the basin of the evaporative system used to cool the condenser.
+
+\paragraph{Refrigeration System Condenser Basin Heater Electric Energy {[}J{]}}\label{refrigeration-system-condenser-basin-heater-electric-energy-j}
+
+This is the electricity consumption in Joules of the water heater used to prevent freezing of the evaporative cooling system for the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Refrigeration System Condenser Evaporated Water Volume Flow Rate {[}m\(^{3}\)/s{]}}{Refrigeration System Condenser Evaporated Water Volume Flow Rate {[}m\^{}\{3\}/s{]}}}\label{refrigeration-system-condenser-evaporated-water-volume-flow-rate-m3s}
+
+The volumetric flow rate in m\(^{3}\)/s of water consumed while providing evaporative cooling of the condenser.
+
+\paragraph{\texorpdfstring{Refrigeration System Condenser Evaporated Water Volume {[}m\(^{3}\){]}}{Refrigeration System Condenser Evaporated Water Volume {[}m\^{}\{3\}{]}}}\label{refrigeration-system-condenser-evaporated-water-volume-m3}
+
+This is the water consumed by evaporation in m\(^{3}\) while providing evaporative cooling of the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Water, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{FOR CONDENSERS ON SYSTEMS SERVING AIR CHILLERS:}\label{for-condensers-on-systems-serving-air-chillers-1}
+
+\paragraph{Refrigeration Air Chiller System Condenser Fan Electric Power {[}W{]}}\label{refrigeration-air-chiller-system-condenser-fan-electric-power-w-1}
+
+This output is the electric input to the system's condenser fan(s) in Watts.
+
+\paragraph{Refrigeration Air Chiller System Condenser Fan Electric Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-fan-electric-energy-j-1}
+
+This is the electricity consumption of the system's condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller System Condenser Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-condenser-heat-transfer-rate-w-1}
+
+This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
+
+\paragraph{Refrigeration Air Chiller System Condenser Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-heat-transfer-energy-j-1}
+
+This is the total heat energy flowing across the condenser for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate~ {[}W{]}}\label{refrigeration-air-chiller-system-condenser-total-recovered-heat-transfer-rate-w-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for any purpose.
+
+\paragraph{Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-total-recovered-heat-transfer-energy-j-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for any purpose for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate~ {[}W{]}}\label{refrigeration-air-chiller-system-condenser-non-refrigeration-recovered-heat-transfer-rate-w-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for purposes such as water or air heating.
+
+\paragraph{Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-non-refrigeration-recovered-heat-transfer-energy-j-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for purposes such as water or air heating for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-condenser-defrost-recovered-heat-transfer-rate-w-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for defrost purposes within the refrigeration system.
+
+\paragraph{Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-defrost-recovered-heat-transfer-energy-j-1}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller System Condenser Pump Electric Power {[}W{]}}\label{refrigeration-air-chiller-system-condenser-pump-electric-power-w}
+
+This is the electrical power requirement in Watts for the timestep being reported for the water pump used with evaporative cooling of the condenser.
+
+\paragraph{Refrigeration Air Chiller System Condenser Pump Electric Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-pump-electric-energy-j}
+
+This is the electricity consumption in Joules of the water pump used with evaporative cooling of the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller System Condenser Basin Heater Electric Power {[}W{]}}\label{refrigeration-air-chiller-system-condenser-basin-heater-electric-power-w}
+
+This is the electrical power requirement in Watts for the timestep being reported for the water heater in the basin of the evaporative system used to cool the condenser.
+
+\paragraph{Refrigeration Air Chiller System Condenser Basin Heater Electric Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-basin-heater-electric-energy-j}
+
+This is the electricity consumption in Joules of the water heater used to prevent freezing of the evaporative cooling system for the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller System Condenser Evaporated Water Volume Flow Rate {[}m3/s{]}}\label{refrigeration-air-chiller-system-condenser-evaporated-water-volume-flow-rate-m3s}
+
+The volumetric flow rate in m\(^{3}\)/s of water consumed while providing evaporative cooling of the condenser.
+
+\paragraph{Refrigeration Air Chiller System Condenser Evaporated Water Volume {[}m3{]}}\label{refrigeration-air-chiller-system-condenser-evaporated-water-volume-m3}
+
+This is the water consumed by evaporation in m\(^{3}\) while providing evaporative cooling of the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Water, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
+
+\subsection{Refrigeration:Condenser:WaterCooled}\label{refrigerationcondenserwatercooled}
+
+The refrigeration system requires a single condenser.~ The water cooled condenser object is one of four options for this condenser. Manufacturer's data is required for the rated total heat rejection, the rated condensing temperature, and the rated leaving liquid refrigerant temperature, all per ARI 450.~ These values are used to calculate the subcooling included in the rated capacity. The inlet and outlet node names as well as the water outlet temperature schedule name are required.~ Optional input is provided to help the user compare refrigerant inventories for different systems.~ These input represent the design values for the refrigerant inventory within the condenser, within a receiver beneath the condenser, and in the liquid pipes between the condenser and the refrigerated cases.
+
+\subsubsection{Inputs}\label{inputs-10-015}
+
+\paragraph{Field: Name}\label{field-name-11-011}
+
+Identifies a particular condenser that rejects heat for one or more refrigeration system(s). The name must be unique and will be validated against all the condenser names (ref: Refrigeration:Condenser) in the input file, including names used for air-cooled, evaporative-cooled, and cascade-cooled condensers.
+
+\paragraph{Field: Rated Effective Total Heat Rejection Rate}\label{field-rated-effective-total-heat-rejection-rate-1}
+
+This numeric field should be the rated heat rejection effect (W) at standard rating conditions per ARI 450.~ Be sure the rating corresponds to the correct refrigerant.
+
+\paragraph{Field: Rated Condensing Temperature}\label{field-rated-condensing-temperature}
+
+This numeric field provides the rated condensing temperature (C) corresponding to the rated heat rejection capacity.
+
+\paragraph{Field: Rated Subcooling Temperature Difference}\label{field-rated-subcooling-temperature-difference-2}
+
+This numeric field provides the rated liquid refrigerant subcooling (DeltaC) corresponding to the rated heat rejection capacity. Note this is equal to the difference between the saturated condensing temperature and the leaving liquid refrigerant temperature.
+
+\paragraph{Field: Rated Water Inlet Temperature}\label{field-rated-water-inlet-temperature}
+
+This numeric field provides the rated water inlet temperature (C) corresponding to the rated heat rejection capacity at the rated condensing temperature.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-002}
+
+A node name for the water-side condenser inlet must be provided.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-001}
+
+A node name for the water-side condenser outlet must be provided.
+
+\paragraph{Field: Water-Cooled Loop Flow Type}\label{field-water-cooled-loop-flow-type-1}
+
+The type of flow loop should be specified.~ The two choices are \textbf{VariableFlow}, in which a Pump:VariableSpeed must be included in the plant loop, or \textbf{ConstantFlow}, in which the loop circuit has a constant flow rate, typically associated with a Pump:ConstandSpeed object.~ If the flow type is VariableFlow, the flow needed to remove the condenser heat energy will be calculated and requested of the pump.~ If the flow type is ConstantFlow, the outlet water temperature will be determined based on the fixed loop flow rate and heat energy to be removed.~ The default type is VariableFlow. Refer to additional discussion in the Engineering Reference.
+
+\paragraph{Field: Water Outlet Temperature Schedule Name}\label{field-water-outlet-temperature-schedule-name}
+
+When the water-cooled loop flow type is ``VariableFlow'', the name of a schedule (Ref: Schedule) that defines the desired condenser water outlet temperature must be provided.~ The schedule may define an outlet temperature that varies through time.
+
+\paragraph{Field: Water Design Flow Rate}\label{field-water-design-flow-rate}
+
+When the water-cooled loop flow type is ``ConstantFlow'', this is the design water flow rate in m\(^{3}\)/s that will be requested initially.~ This requested flow will be passed to the loop simulation, and resulting actual flow will be dependent upon supply system capabilities (e.g., pump capability).~ The design flow rate must always be less than the maximum flow rate, defined below.
+
+\paragraph{Field: Water Maximum Flow Rate}\label{field-water-maximum-flow-rate}
+
+This numeric field is the maximum water flow rate in m\(^{3}\)/s that will be allowed through the condenser.~ When the loop flow type is Variable Flow, if the calculated flow rate is higher than the maximum flow rate, an error message will be generated, and the flow rate will be reset to the maximum flow rate.
+
+\paragraph{Field: Maximum Water Outlet Temperature}\label{field-maximum-water-outlet-temperature}
+
+This numeric field specifies the maximum allowed water temperature in degrees C leaving the condenser. The default value is 55 degrees C.
+
+\paragraph{Field: Minimum Water Inlet Temperature}\label{field-minimum-water-inlet-temperature}
+
+This numeric field specifies the minimum allowed water temperature in degrees C entering the compressor rack condenser. The default value is 10 degrees C.~ Refer to additional discussion in the Engineering Reference.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-6}
+
+This field allows the specification of a user-defined end-use subcategory (e.g., ``Low Temperature System''). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Condenser Refrigerant Operating Charge Inventory}\label{field-condenser-refrigerant-operating-charge-inventory-2}
+
+This numeric field specifies the amount of refrigerant present within the condenser (kg) specified by the manufacturer, under standard rating conditions.
+
+\paragraph{Field: Condensate Receiver Refrigerant Inventory}\label{field-condensate-receiver-refrigerant-inventory-2}
+
+This numeric field specifies the amount of refrigerant present within the condensate receiver (kg) specified by the manufacturer or system designer, under standard rating conditions.
+
+\paragraph{Field: Condensate Piping Refrigerant Inventory}\label{field-condensate-piping-refrigerant-inventory-2}
+
+This numeric field specifies the amount of refrigerant present within the condensate piping (kg) specified by the system designer, under standard rating conditions.
+
+The following is an example input for a water cooled condenser.
+
+\begin{lstlisting}
+
+Refrigeration:Condenser:WaterCooled,
+      MediumTempCondenser ,    !- Name
+      58000. ,                 !- Rated Effective Total Heat Rejection Rate {W}
+      29.4 ,                   !- Rated Condensing Temperature {C}
+      0.0 ,                    !- Rated Subcooling Temperature Difference{deltaC}
+      10.0,                    !- Rated Water Inlet Temperature {C}
+      Condenser Inlet Node,    !- Water Inlet Node Name
+      Condenser Outlet Node,   !- Water- Outlet Node Name
+      Variable Flow,           !- Water-cooled Loop Flow Type
+      Cond Outlet Temp Sch,    !- Water Outlet Temperature Schedule Name
+      ,                        !- Water Design Flow Rate {m3/s}
+      0.003,                   !- Water Maximum Flow Rate {m3/s}
+      55.,                     !- Maximum Water Outlet Temperature {C}
+      ,                        !- Minimum Water Inlet Temperature {C}
+      ,                        !- End-Use Subcategory
+      30. ,                    !- Condenser Refrigerant Operating Charge {kg}
+      65. ,                    !- Condensate Receiver Refrigerant Inventory {kg}
+      20. ;                    !- Condensate Piping Refrigerant Inventory {kg}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8-007}
+
+FOR CONDENSERS COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration System Condenser Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Total Recovered Heat Transfer Rate {[}W{]} Zone, Sum, Refrigeration System Condenser Total Recovered Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Heat Recovered for Non-Refrigeration Purposes Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Defrost Recovered Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration System Condenser Water Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+FOR CONDENSERS COOLING SYSTEMS SERVING AIR CHILLERS:
+
+\begin{itemize}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate {[}W{]} HVAC, Sum, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Fluid Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{FOR CONDENSERS ON SYSTEMS SERVING CASES AND/OR WALKINS:}\label{for-condensers-on-systems-serving-cases-andor-walkins-2}
+
+\paragraph{Refrigeration System Condenser Heat Transfer Rate {[}W{]}}\label{refrigeration-system-condenser-heat-transfer-rate-w-2}
+
+This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
+
+\paragraph{Refrigeration System Condenser Heat Transfer Energy {[}J{]}}\label{refrigeration-system-condenser-heat-transfer-energy-j-2}
+
+This is the total heat energy flowing across the condenser for the timestep being reported.
+
+\paragraph{Refrigeration System Condenser Total Recovered Heat Transfer Rate~ {[}W{]}}\label{refrigeration-system-condenser-total-recovered-heat-transfer-rate-w-2}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for any purpose.
+
+\paragraph{Refrigeration System Condenser Total Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-system-condenser-total-recovered-heat-transfer-energy-j-2}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for any purpose for the timestep being reported.
+
+\paragraph{Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-system-condenser-non-refrigeration-recovered-heat-transfer-rate-w-2}
+
+This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating.
+
+\paragraph{Refrigeration System Condenser Heat Recovered for Non-Refrigeration Purposes Energy~ {[}J{]}}\label{refrigeration-system-condenser-heat-recovered-for-non-refrigeration-purposes-energy-j-1}
+
+This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating for the timestep being reported.
+
+\paragraph{Refrigeration System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-system-condenser-defrost-recovered-heat-transfer-rate-w-2}
+
+This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system..
+
+\paragraph{Refrigeration System Condenser Heat Energy Recovered for Refrigeration Defrost Energy {[}J{]}}\label{refrigeration-system-condenser-heat-energy-recovered-for-refrigeration-defrost-energy-j}
+
+This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
+
+\paragraph{Refrigeration System Condenser Water Mass Flow Rate {[}kg/s{]}}\label{refrigeration-system-condenser-water-mass-flow-rate-kgs}
+
+This is the mass flow rate of the water used to cool the condenser in kg/s.
+
+\paragraph{FOR CONDENSERS ON SYSTEMS SERVING AIR CHILLERS:}\label{for-condensers-on-systems-serving-air-chillers-2}
+
+\paragraph{Refrigeration Air Chiller System Condenser Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-condenser-heat-transfer-rate-w-2}
+
+This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
+
+\paragraph{Refrigeration Air Chiller System Condenser Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-heat-transfer-energy-j-2}
+
+This is the total heat energy flowing across the condenser for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate~ {[}W{]}}\label{refrigeration-air-chiller-system-condenser-total-recovered-heat-transfer-rate-w-2}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for any purpose.
+
+\paragraph{Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-total-recovered-heat-transfer-energy-j-2}
+
+This is the total heat recovered from the condenser refrigerant inlet flow for any purpose for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-condenser-non-refrigeration-recovered-heat-transfer-rate-w-2}
+
+This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating.
+
+\paragraph{Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy~ {[}J{]}}\label{refrigeration-air-chiller-system-condenser-non-refrigeration-recovered-heat-transfer-energy-j-2}
+
+This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-condenser-defrost-recovered-heat-transfer-rate-w-2}
+
+This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system.
+
+\paragraph{Refrigeration Chiller System Condenser Heat Energy Recovered for Refrigeration Defrost Energy {[}J{]}}\label{refrigeration-chiller-system-condenser-heat-energy-recovered-for-refrigeration-defrost-energy-j}
+
+This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller System Condenser Fluid Mass Flow Rate {[}kg/s{]}}\label{refrigeration-air-chiller-system-condenser-fluid-mass-flow-rate-kgs}
+
+This is the mass flow rate of the water used to cool the condenser in kg/s.
+
+\subsection{Refrigeration:Condenser:Cascade}\label{refrigerationcondensercascade}
+
+The refrigeration system requires a single condenser.~ The cascade condenser object is one of four options for this condenser. The cascade condenser is unlike the other condenser options because it rejects heat to another, higher-temperature, refrigeration system. That is, the cascade condenser acts as a heat rejection object for one system, but acts as a refrigeration load for another system.~ Therefore, this object will be referenced twice: first for the system rejecting heat (see the field Refrigeration Condenser Name for the object Refrigeration:System), and second for the system absorbing the heat (see the input for the field Refrigeration Transfer Load or TransferLoad List Name for the object Refrigeration:System or the field Cascade Condenser Name or Secondary System Name for the object Refrigeration:TransferLoadList).
+
+Manufacturer's data is required for the rated condensing temperature and the rated approach temperature difference. The user must also specify the condensing temperature control type.~ There are two choices. The user can specify ``Fixed'' and the condensing temperature will be held constant at the input value.~ The user can specify ``Float'' if they want the condensing temperature to be set by other refrigeration loads served by the higher-temperature system.
+
+The rated heat rejection capacity is not used except as a rough input value check on the overall system sizing. Optional input is provided to help the user compare refrigerant inventories for different systems.~ These inputs represent the design values for the refrigerant inventory within the condenser, within a receiver beneath the condenser, and in the liquid pipes between the condenser and the refrigerated cases.
+
+\subsubsection{Inputs}\label{inputs-11-014}
+
+\paragraph{Field: Name}\label{field-name-12-009}
+
+Identifies a particular condenser that rejects heat for a single refrigeration system. The name must be unique and will be validated against all the condenser names (ref: Refrigeration:Condenser:*) in the input file, including names used for air-cooled, evaporative-cooled, and water-cooled condensers.
+
+\paragraph{Field: Rated Condensing Temperature}\label{field-rated-condensing-temperature-1}
+
+This numeric field provides the rated condensing temperature (C).
+
+\paragraph{Field: Rated Approach Temperature Difference}\label{field-rated-approach-temperature-difference}
+
+This numeric field provides the rated difference (Delta C) between the saturated condensing temperature for the system rejecting heat and the saturated evaporating refrigerant temperature for the system absorbing heat. The default value is 3.0 C.
+
+\paragraph{Field: Rated Effective Total Heat Rejection Rate}\label{field-rated-effective-total-heat-rejection-rate-2}
+
+This numeric field should be the rated heat rejection effect (W).~ Be sure the rating corresponds to the correct refrigerant(s). This value is used for system sizing error checking.
+
+\paragraph{Field: Condensing Temperature Control Type}\label{field-condensing-temperature-control-type}
+
+The type of control used to set the saturated condensing temperature. Valid choices are \textbf{Fixed} and \textbf{Float}.~ If the field is blank, \textbf{Fixed} will be used. Fixed will hold the condensing temperature constant at the value specified.~ \textbf{Float} will consider the specified input as a minimum condensing temperature.~ This value will be compared to the evaporating temperatures required by other loads on the higher-temperature refrigeration system, and will use the lowest temperature required to meet those loads, along with the Approach Temperature Difference, to set the condensing temperature.
+
+\paragraph{Field: Condenser Refrigerant Operating Charge Inventory}\label{field-condenser-refrigerant-operating-charge-inventory-3}
+
+This numeric field specifies the amount of refrigerant present within the condenser (kg) specified by the manufacturer, under standard rating conditions. This refrigerant is on the side of the condenser rejecting heat, not on the side of the condenser absorbing the heat.
+
+\paragraph{Field: Condensate Receiver Refrigerant Inventory}\label{field-condensate-receiver-refrigerant-inventory-3}
+
+This numeric field specifies the amount of refrigerant present within the condensate receiver (kg) specified by the manufacturer or system designer, under standard rating conditions.
+
+\paragraph{Field: Condensate Piping Refrigerant Inventory}\label{field-condensate-piping-refrigerant-inventory-3}
+
+This numeric field specifies the amount of refrigerant present within the condensate piping (kg) specified by the system designer, under standard rating conditions.
+
+The following is an example input for a cascade condenser.
+
+\begin{lstlisting}
+
+Refrigeration:Condenser:Cascade,
+      CascadeCondenser1 ,      !- Name
+      -4. ,                    !- Rated Condensing Temperature {C}
+      3. ,                     !- Rated Approach Temperature Difference {DeltaC}
+      20000.0 ,                !- Rated Effective Total Heat Rejection Rate {W}
+      Fixed;                   !- Condensing Temperature Control Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-9-007}
+
+FOR CONDENSERS COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration System Condenser Heat Transfer Rate {[}W{]}
+\item
+  Zone, Sum, Refrigeration System Condenser Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+FOR CONDENSERS COOLING SYSTEMS SERVING AIR CHILLERS:
+
+\begin{itemize}
+\item
+  HVAC,Average, Refrigeration Air Chiller System Condenser Heat Transfer Rate {[}W{]}
+\item
+  HVAC, Sum, Refrigeration Air Chiller System Condenser Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{FOR CONDENSERS ON SYSTEMS SERVING CASES AND/OR WALKINS:}\label{for-condensers-on-systems-serving-cases-andor-walkins-3}
+
+\paragraph{Refrigeration System Condenser Heat Transfer Rate {[}W{]}}\label{refrigeration-system-condenser-heat-transfer-rate-w-3}
+
+This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
+
+\paragraph{Refrigeration System Condenser Heat Transfer Energy {[}J{]}}\label{refrigeration-system-condenser-heat-transfer-energy-j-3}
+
+This is the total heat energy flowing across the condenser for the timestep being reported.
+
+\paragraph{FOR CONDENSERS ON SYSTEMS SERVING AIR CHILLERS:}\label{for-condensers-on-systems-serving-air-chillers-3}
+
+\paragraph{Refrigeration Air Chiller System Condenser Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-system-condenser-heat-transfer-rate-w-3}
+
+This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
+
+\paragraph{Refrigeration Air Chiller System Condenser Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-system-condenser-heat-transfer-energy-j-3}
+
+This is the total heat energy flowing across the condenser for the timestep being reported.
+
+\subsection{Refrigeration:GasCooler:AirCooled}\label{refrigerationgascooleraircooled}
+
+The transcritical refrigeration system requires a single gas cooler to reject the system heat.~ The total heat of rejection is characterized by a linear relationship between the difference between the outside dry-bulb and gas cooler outlet temperatures.~ The rated gas cooler fan power and fan speed control type must be specified.~ If the gas cooler is not at ground level, the user may specify an air inlet node name (Ref. OutdoorAir:Node name).~ Optional input is provided to help the user track refrigerant inventories.~ These inputs represent the design values for the refrigerant inventory within the gas cooler, within a receiver, and in the liquid pipes between the gas cooler and the refrigerated cases.
+
+\subsubsection{Inputs}\label{inputs-12-013}
+
+\paragraph{Field: Name}\label{field-name-13-008}
+
+Identifies a particular gas cooler that rejects heat for a single refrigeration system.~ The name must be unique and will be validated against all the gas cooler names (Ref. Refrigeration:GasCooler:AirCooled) in the input file.
+
+\paragraph{Field: Rated Total Heat Rejection Rate Curve Name}\label{field-rated-total-heat-rejection-rate-curve-name}
+
+This field is the name of a curve object defining the gas cooler heat rejection as a function of the difference between the gas cooler outlet and entering air temperatures. The curve should be linear (Curve:Linear). See the Engineering Reference for more discussion on the curve coefficients.
+
+\paragraph{Field: Gas Cooler Fan Speed Control Type}\label{field-gas-cooler-fan-speed-control-type}
+
+The type of fan speed control used by the gas cooler fan.~ Valid choices are Fixed, FixedLinear, VariableSpeed, and TwoSpeed.~ If the field is blank, Fixed will be used.~ Note that fan energy consumption for the air-cooled gas cooler is computed in the same way as that of the air-cooled condenser.~ For further information on fan energy calculations, see the discussion regarding air-cooled condenser fan energy in the Engineering Reference.
+
+\paragraph{Field: Rated Fan Power}\label{field-rated-fan-power-2}
+
+This numeric field specifies the rated fan power (W) specified by the manufacturer, under standard rating conditions.~ If this field is blank, the default value of 5000~W will be used
+
+\paragraph{Field: Minimum Fan Air Flow Ratio}\label{field-minimum-fan-air-flow-ratio-2}
+
+Fan controls often include a minimum air flow ratio to avoid overheating the fan motor or for other reasons.~ This numeric field should be between 0. and 1. and has a default value of 0.2.
+
+\paragraph{Field: Transition Temperature}\label{field-transition-temperature}
+
+This is the temperature (C) at which the gas cooler and the refrigeration system transitions between subcritical and transcritical operation.~ If this field is blank, the default value of 27.0°C will be used.
+
+\paragraph{Field: Transcritical Approach Temperature}\label{field-transcritical-approach-temperature}
+
+This is the temperature difference (C) between the refrigerant (CO\(_{2}\)) exiting the gas cooler and the air entering the gas cooler during transcritical operation.~ If this field is blank, the default value of 3.0°C will be used.
+
+\paragraph{Field: Subcritical Temperature Difference}\label{field-subcritical-temperature-difference}
+
+This is the temperature difference (C) between the condensing temperature and the ambient air temperature during subcritical operation.~ If this field is blank, the default value of 10.0°C will be used.
+
+\textbf{\emph{Field: Minimum Condensing Temperature}}
+
+This numeric field specifies the minimum condensing temperature (C) required to maintain stable subcritical operation.~ If this field is blank, the default value of 10.0°C will be used.
+
+\textbf{\emph{Field: Air Inlet Node Name}}
+
+This optional alpha field contains the name of the node from which the gas cooler draws its outdoor air.~ If this field is left blank, the outdoor air dry-bulb temperature entering the gas cooler is taken directly from the weather data.~ If this field is not blank, this node name must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data.~ Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-7}
+
+This field allows the specification of a user-defined end-use subcategory (e.g., ``Low Temperature Rack'').~ A new meter for reporting is created for each unique subcategory (Ref. Output:Meter objects). Subcategories are also reported in the ABUPS table.~ If this field is left blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Gas Cooler Refrigerant Operating Charge Inventory}\label{field-gas-cooler-refrigerant-operating-charge-inventory}
+
+This numeric field specifies the amount of refrigerant present within the gas cooler (kg) specified by the manufacturer, under standard rating conditions.~ If this field is blank, the default value of 0.0~kg will be used.
+
+\paragraph{Field: Gas Cooler Receiver Refrigerant Inventory}\label{field-gas-cooler-receiver-refrigerant-inventory}
+
+This numeric field specifies the amount of refrigerant present within the gas cooler receiver (kg) specified by the manufacturer or system designer, under standard rating conditions.~ If this field is blank, the default value of 0.0~kg will be used.
+
+\paragraph{Field: Gas Cooler Outlet Piping Refrigerant Inventory}\label{field-gas-cooler-outlet-piping-refrigerant-inventory}
+
+This numeric field specifies the amount of refrigerant present within the gas cooling outlet piping (kg) specified by the system designer, under standard rating conditions.~ If this field is blank, the default value of 0.0~kg will be used.
+
+The following is an example input for an air-cooled gas cooler.
+
+\begin{lstlisting}
+
+Refrigeration:GasCooler:AirCooled,
+      RefrigGasCooler,         !- Name
+      GasCoolerHRCurve,        !- Rated Total Heat Rejection Rate Curve Name
+      Fixed,                   !- Gas Cooler Fan Speed Control Type
+      6400,                    !- Rated Fan Power
+      0.2,                     !- Minimum Fan Air Flow Ratio
+      27.0,                    !- Transition Temperature
+      3.0,                     !- Transcritical Approach Temperature
+      10.0,                    !- Subcritical Temperature Difference
+      10.0,                    !- Minimum Condensing Temperature
+      ,                        !- Air Inlet Node Name
+      RefrigGasCooler,         !- End-Use Subcategory
+      ,                        !- Gas Cooler Refrigerant Operating Charge Inventory
+      ,                        !- Gas Cooler Receiver Refrigerant Inventory
+      ;                        !- Gas Cooler Outlet Piping Refrigerant Inventory
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-10-006}
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration Transcritical System Gas Cooler Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Gas Cooler Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Gas Cooler Fan Electric Power {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Gas Cooler Fan Electric Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Gas Cooler Outlet Temperature {[}C{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Gas Cooler Outlet Pressure {[}Pa{]}
+\item
+  Zone,Average, Refrigeration Transcritical System Gas Cooler Defrost Recovered Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Transcritical System Gas Cooler Defrost Recovered Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Refrigeration Transcritical System Gas Cooler Heat Transfer Rate {[}W{]}}\label{refrigeration-transcritical-system-gas-cooler-heat-transfer-rate-w}
+
+This output is the total heat transfer rate from the gas cooler in Watts, and includes compressor energy and the refrigeration load.
+
+\paragraph{Refrigeration Transcritical System Gas Cooler Heat Transfer Energy {[}J{]}}\label{refrigeration-transcritical-system-gas-cooler-heat-transfer-energy-j}
+
+This output is the total heat transferred from the gas cooler to the surroundings, in Joules, for the timestep being reported.
+
+\paragraph{Refrigeration Transcritical System Gas Cooler Fan Electric Power {[}W{]}}\label{refrigeration-transcritical-system-gas-cooler-fan-electric-power-w}
+
+This output is the electric input to the system's gas cooler fan(s) in Watts.
+
+\paragraph{Refrigeration Transcritical System Gas Cooler Fan Electric Energy {[}J{]}}\label{refrigeration-transcritical-system-gas-cooler-fan-electric-energy-j}
+
+This is the electricity consumption of the system's gas cooler fan(s) in Joules for the timestep being reported.~ This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Transcritical System Gas Cooler Outlet Temperature {[}C{]}}\label{refrigeration-transcritical-system-gas-cooler-outlet-temperature-c}
+
+This output is the temperature (in C) of the refrigerant exiting the gas cooler.
+
+\paragraph{Refrigeration Transcritical System Gas Cooler Outlet Pressure {[}Pa{]}}\label{refrigeration-transcritical-system-gas-cooler-outlet-pressure-pa}
+
+This output is the pressure (in Pa) of the refrigerant exiting the gas cooler.
+
+\paragraph{Refrigeration Transcritical System Gas Cooler Defrost Recovered Heat Transfer Rate {[}W{]}}\label{refrigeration-transcritical-system-gas-cooler-defrost-recovered-heat-transfer-rate-w}
+
+This is the total heat recovered from the gas cooler inlet flow for defrost purposes within the refrigeration system.
+
+\paragraph{Refrigeration Transcritical System Gas Cooler Defrost Recovered Heat Transfer Energy {[}J{]}}\label{refrigeration-transcritical-system-gas-cooler-defrost-recovered-heat-transfer-energy-j}
+
+This is the total heat recovered from the gas cooler inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
+
+\subsection{Refrigeration:TransferLoadList}\label{refrigerationtransferloadlist}
+
+A refrigeration system may provide cooling to other, secondary, systems through either a secondary loop or a cascade condenser (Ref. Refrigeration:SecondarySystem and Refrigeration:Condenser:Cascade). If multiple transfer loads are served by a single primary system, use this list to group them together for reference by the primary system (see the field ``Refrigeration Transfer Load or TransferLoad List Name'' in the Refrigeration:System object).
+
+\subsubsection{Inputs}\label{inputs-13-011}
+
+\paragraph{Field: Name}\label{field-name-14-007}
+
+A unique user-assigned name for an instance of a refrigeration transfer load list. Any reference to this list by another object will use this name. In particular, the primary refrigeration system absorbing the heat from all the loads listed here will use this name to reference those loads.
+
+\paragraph{Field: Cascade Condenser Name or Secondary System Name}\label{field-cascade-condenser-name-or-secondary-system-name}
+
+Identifies a cascade condenser or secondary loop that is cooled, along with the other transfer loads listed here, by a single system. The name will be validated against the Refrigeration:SecondarySystem and Refrigeration:Condenser:Cascade names in the input file (the name will also be compared against all the other condenser names, but an error will be issued if it refers to any type of condenser other than a cascade condenser).
+
+The list is extensible; ten fields are provided in the IDD.
+
+The following is an example input for a transfer load list.
+
+\begin{lstlisting}
+
+Refrigeration:TransferLoadList,
+      MedTempTransferLoads ,   !- Name
+      CascadeCondFrozen,       !- Cascade Condenser Name or Secondary System Name
+      SecondLoopDairy;         !- Cascade Condenser Name or Secondary System Name
+\end{lstlisting}
+
+\subsection{Refrigeration:SecondarySystem}\label{refrigerationsecondarysystem}
+
+A refrigeration secondary system works in conjunction with refrigerated cases and walkins (Ref. Refrigeration:SecondarySystem, Refrigeration:CaseAndWalkInList, Refrigeration:Case, and Refrigeration:WalkIn) to simulate the performance of a secondary loop supermarket refrigeration system. Heat from the refrigeration loads served by the secondary loop is absorbed by a primary refrigeration system (ref: Refrigeration:System). The SecondarySystem object simulates a heat exchanger that is an evaporator, or refrigeration load, on the primary refrigeration system.
+
+The inputs for the refrigeration secondary system object include a name, which is also referenced to identify the load placed upon the primary refrigeration system. The inputs that describe the loads placed upon the secondary loop include the name of a single refrigerated case, the name of a single walk-in cooler, or a list of cases and walkin coolers.~ The circulating fluid type specifies whether or not the secondary fluid remains in the liquid state throughout the loop (e.g., a glycol or brine solution) or undergoes a partial phase change while serving the refrigeration loads (e.g., a CO\(_{2}\) liquid overfeed system). The circulating fluid name must also be specified and must correspond to a name used to provide the fluid properties.
+
+If the secondary fluid remains a liquid, the heat exchanger between the primary and secondary systems functions as an evaporator on the primary side and chills the circulating fluid on the secondary side. Inputs that describe the evaporator performance at rated conditions are used to calculate the heat exchanger effectiveness. These values include the rated evaporator capacity (which can be specified in terms of energy or fluid flow rate), the rated evaporating temperature, the rated approach temperature difference, and the rated range temperature difference.
+
+If the secondary fluid undergoes a partial phase change, the heat exchanger between the primary and secondary systems functions as an evaporator on the primary side and as a condenser on the secondary side. The evaporator capacity, evaporating temperature, and approach temperature difference, all at full-load design conditions, are input.
+
+The balance of the secondary system object describes the pumping system. The pumping options include a single constant speed pump, multiple constant speed pumps, or a variable frequency-drive pump.~ The user can also keep track of distribution piping and receiver shell heat gains.
+
+\subsubsection{Inputs}\label{inputs-14-011}
+
+\paragraph{Field: Name}\label{field-name-15-007}
+
+A unique user-assigned name for an instance of a refrigeration secondary system. Any reference to this refrigeration secondary system by another object will use this name. In particular, the primary refrigeration system absorbing the heat from this system will use this name to define that load.
+
+\paragraph{Field: Refrigerated Case or WalkIn or CaseAndWalkInList Name}\label{field-refrigerated-case-or-walkin-or-caseandwalkinlist-name-1}
+
+Identifies a single case, or walkin, or a particular list of refrigerated cases and walkins, that are cooled by this refrigeration secondary system. The name will be validated against the case, walkin, and CaseAndWalkInList names (ref. Refrigeration:Case, Refrigeration:WalkIn and Refrigeration:CaseAndWalkInList) in the input file.
+
+\paragraph{Field: Circulating Fluid Type}\label{field-circulating-fluid-type}
+
+Specifies whether the fluid is always liquid (e.g., glycol solution), or undergoes a partial phase change (e.g., CO\(_{2}\) liquid overfeed system).~ The options are ``FluidAlwaysLiquid'' and ``FluidPhaseChange''.
+
+\paragraph{Field: Circulating Fluid Name}\label{field-circulating-fluid-name}
+
+The name of the secondary circulating fluid.
+
+For ``FluidAlwaysLiquid'', this name must correspond to either an ethylene or propylene glycol (ref: FluidProperties:GlycolConcentration) or to a user-defined glycol (ref: FluidProperties:Name and FluidProperties: GlycolConcentration) in the input file. Note that the corresponding property data, including FluidProperties:Concentration, FluidProperties:Temperatures, and FluidProperties:GlycolConcentration must also be included in the input file and are provided in GlycolPropertiesRefData.idf for typical ethylene and propylene glycols.
+
+For ``FluidPhaseChange'', the refrigerant used by the secondary system must be listed in the FluidProperties:Name object.~ The corresponding property data must also be supplied in the input file. Property data for many refrigererants, including R11, R123, R134A, R12, R22, R404A, R507A, R410A, and R744, are available in FluidPropertiesRefData.idf.
+
+\paragraph{Field: Evaporator Capacity}\label{field-evaporator-capacity}
+
+For ``FluidAlwaysLiquid'', this numeric field should be the rated heat evaporator capacity (W).~ Be sure the rating corresponds to the correct refrigerant and secondary circulating fluid. If this variable is specified and the rated evaporator flow rate for secondary fluid is not, then the flow rate will be calculated.~ At least one of these two input variables is required.
+
+For ``FluidPhaseChange'', this numeric field should be the evaporator capacity (W) at full-load design conditions. If this input is left blank, the capacity will be set to the sum of the capacities of the cases and walk-ins served by the secondary loop plus the pump motor load at full-load design conditions.
+
+\paragraph{Field: Evaporator Flow Rate for Secondary Fluid}\label{field-evaporator-flow-rate-for-secondary-fluid}
+
+For ``FluidAlwaysLiquid'' systems, this is the rated evaporator secondary fluid flow rate in m\(^{3}\)/s.~ If this variable is specified and the rated evaporator capacity in watts is not, then the rated capacity will be calculated. At least one of these two input variables is required.
+
+For ``FluidPhaseChange'', this field is not used (see ``Phase Cange Circulating Rate'').
+
+\paragraph{Field:Evaporator Evaporating Temperature}\label{fieldevaporator-evaporating-temperature}
+
+This numeric field provides the evaporating temperature (C) corresponding to the evaporator capacity. This is the evaporating temperature on the primary side of the heat exchanger used to chill or condense the secondary loop circulating fluid.~ It is NOT the temperature in any cases or walkins served by the secondary loop.
+
+\paragraph{Field: Evaporator Approach Temperature Difference}\label{field-evaporator-approach-temperature-difference}
+
+For ``FluidAlwaysLiquid'', this numeric field is the rated temperature difference (DeltaC) between the circulating secondary fluid leaving the heat exchanger and the heat exchanger's evaporating temperature.
+
+For ``FluidPhaseChange'', this is the temperature difference (DeltaC) between the primary refrigerant evaporating and secondary refrigerant condensing temperatures at full-load design conditions.
+
+\paragraph{Field: Evaporator ~Range Temperature Difference}\label{field-evaporator-range-temperature-difference}
+
+For ``FluidAlwaysLiquid'', this numeric field is the rated temperature difference (DeltaC) between the circulating secondary fluid entering and leaving the heat exchanger. This value is not used for ``FluidPhaseChange''.
+
+\paragraph{Field: Number of Pumps in Loop}\label{field-number-of-pumps-in-loop}
+
+This numeric field provides the integer number of pumps used to circulate the secondary heat transfer fluid. The default value is 1. Unless a variable speed pump is specified, pump energy will be calculated in linear steps to achieve the necessary flow rate.
+
+\paragraph{Field: Total Pump Flow Rate}\label{field-total-pump-flow-rate}
+
+This is the secondary fluid circulating flow rate in m\(^{3}\)/s at full-load design conditions.~ For ``FluidAlwaysLiquid'', if no value is input, the Evaporator Flow Rate for Secondary Fluid will be used. For ``FluidPhaseChange'', if no value is input, the flow rate will be calculated using the Evaporator Capacity and the PhaseChange Circulating Rate.
+
+\paragraph{Field: Total Pump Power}\label{field-total-pump-power}
+
+This numeric field should be the pump power (W) at full-load design conditions.~ Be sure the rating corresponds to the correct secondary circulating fluid at the design fluid temperature. EITHER the Total Pump Power OR the Total Pump Head is required.
+
+\paragraph{Field: Total Pump Head}\label{field-total-pump-head}
+
+This numeric field should be the design pressure drop, or head, across the secondary loop (Pa) at full load design conditions.~ Be sure the rating corresponds to the correct secondary circulating fluid at the design fluid temperature. EITHER the Total Pump Power OR the Total Head is required.
+
+\paragraph{Field: PhaseChange Circulating Rate}\label{field-phasechange-circulating-rate}
+
+This field is not used for ``FluidAlwaysLiquid''.
+
+For ``FluidPhaseChange'', the Circulating Rate is defined as the total mass flow at the pump divided by the mass flow rate of vapor returning to the separator. Values between 2.1 and 3 are common for CO\(_{2}\) systems and the default is 2.5. If Total Pump Flow Rate is also defined, the PhaseChange Circulating Rate will only be used to check whether the two values are consistent.
+
+\paragraph{Field: Pump Drive Type}\label{field-pump-drive-type}
+
+Specifies whether the pump(s) is constant speed or variable speed.~ The options are ``Constant'' and ``Variable''. The default is ``Constant''.
+
+\paragraph{Field: Variable Speed Pump Cubic Curve Name}\label{field-variable-speed-pump-cubic-curve-name}
+
+The name of a \textbf{cubic} performance curve (ref: Performance Curves) that parameterizes the variation of the variable speed pump power (and the associated load on the secondary refrigeration load) at off-rated conditions. The curve should be normalized to have the value of 1.0 at full-load design conditions. The variable speed pump cubic curve name is used only for the a pump drive type of ``Variable''.
+
+\paragraph{Field: Pump Motor Heat to Fluid}\label{field-pump-motor-heat-to-fluid}
+
+This choice field determines how much of the pump motor heat will be added to the circulating secondary fluid. This represents the motor efficiency for a non-hermetic motor. The default is 0.85.~ For a semi-hermetic motor, enter 1.0. The value entered must be between 0.5 and 1.0.
+
+\paragraph{Field: Sum UA Distribution Piping}\label{field-sum-ua-distribution-piping}
+
+This optional field is typically used when trying to compare the impact of pipe heat gains on system performance, particularly in comparing a DX system to a secondary system. Enter the value for secondary loop distribution piping heat gain (in W/C).~ That is, sum up the product of the pipe insulation conductance times the outer piping insulation surface area. Please see the Engineering Reference for guidance in calculating this value.
+
+\paragraph{Field: Distribution Piping Zone Name}\label{field-distribution-piping-zone-name}
+
+This optional field is used when trying to determine the impact of pipe heat gains on system performance, particularly in comparing a DX system to a secondary system. (If the previous field, Sum UA Distribution Piping, is blank, this field will not be used.) Enter the name of the zone where the Distribution piping is located. The distribution piping heat gains will be calculated based upon the air temperature within this zone and will count as a cooling credit for this zone.
+
+\paragraph{Field: Sum UA Receiver/Separator Shell}\label{field-sum-ua-receiverseparator-shell}
+
+This optional field is typically used when trying to compare the impact of refrigeration component heat gains on system performance, particularly in comparing a conventional primary DX system to a secondary system. Enter the value for receiver/separator heat gain (in W/C).~ That is, sum up the product of the tank insulaton conductance times the outer tank insulation surface area. Please see the Engineering Reference for guidance in calculating this value.
+
+\paragraph{Field: Receiver/Separator Zone Name}\label{field-receiverseparator-zone-name}
+
+This optional field is used when trying to determine the impact of refrigeration component heat gains on system performance, particularly in comparing a conventional primary DX system to a secondary system. (If the previous field, Sum UA Receiver/Separator, is blank, this field will not be used.) Enter the name of the zone where the receiver/separator is located. The heat gains will be calculated based upon the air temperature within this zone and will count as a cooling credit for this zone.
+
+\paragraph{Field: Evaporator Refrigerant Inventory}\label{field-evaporator-refrigerant-inventory}
+
+The secondary loop is chilled by a primary system via a heat exchanger.~ This field is the refrigerant inventory on the cold (primary) side of that heat exchanger, in kg. The default value is zero.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-8}
+
+This field allows the specification of a user-defined end-use subcategory (e.g., ``Low Temperature Rack''). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the ``General'' end-use subcategory.
+
+The following is an example input for a brine-type (``FluidAlwaysLiquid'')refrigeration secondary system.
+
+\begin{lstlisting}
+
+  Refrigeration:SecondarySystem,
+      SecondaryMedLoop,        !- Name
+      MedTempCaseList,         !- Refrigerated Case or Walkin or CaseAndWalkInList Name
+      FluidAlwaysLiquid,       !- Circulating Fluid Type
+      ProGly30Percent,         !- Circulating Fluid Name
+      3.5E4,                   !- Evaporator Capacity {W}
+      0.0021,                  !- Evaporator Flow Rate for Secondary Fluid {M3/s}
+      -12.6,                   !- Evaporator Evaporating Temperature {C}
+      2.7,                     !- Evaporator Approach Temperature Difference {DeltaC}
+      4.,                      !- Evaporator Range Temperature Difference {DeltaC}
+      3,                       !- Number of Pumps in Loop
+      .0023,                   !- Total Pump Flow Rate {M3/s}
+      ,                        !- Total Pump Power {W}
+      2.09E5,                  !- Total Pump Head {Pa}
+      ,                        !- PhaseChange Circulating Rate
+      ,                        !- Pump Drive Type
+      ,                        !- Variable Speed Pump Cubic Curve Name
+      1.0,                     !- Pump Motor Heat to Fluid
+      21.,                     !- Sum UA Distribution Piping {W/C}
+      SalesFloor,              !- Distribution Piping Zone Name
+      ,                        !- Sum UA Receiver/Separator Shell
+      ,                        !- Receiver/Separator Zone Name
+      ,                        !- Evaporator Refrigerant Inventory {kg}
+      ;                        !- End-Use Subcategory
+\end{lstlisting}
+
+The following is an example input for a liquid-overfeed-type (``FluidPhaseChange'') refrigeration secondary system.
+
+\begin{lstlisting}
+
+  Refrigeration:SecondarySystem,
+      SecondaryLowLoop,        !- Name
+      LowTempCaseList,         !- Refrigerated Case or Walkin or CaseAndWalkInList Name
+      FluidPhaseChange,        !- Circulating Fluid Type
+      R744,                    !- Circulating Fluid Name
+      ,                        !- Evaporator Capacity {W}
+      ,                        !- Evaporator Flow Rate for Secondary Fluid {M3/s}
+      -39.2,                   !- Evaporator Evaporating Temperature {C}
+      2.,                      !- Evaporator Approach Temperature Difference {DeltaC}
+      ,                        !- Evaporator Range Temperature Difference {DeltaC}
+      3,                       !- Number of Pumps in Loop
+      ,                        !- Total Pump Flow Rate {M3/s}
+      ,                        !- Total Pump Power {W}
+      2.09E5,                  !- Total Pump Head {Pa}
+      2.5,                     !- PhaseChange Circulating Rate
+      Variable,                !- Pump Drive Type
+      SecondaryVarSpeedPump,   !- Variable Speed Pump Cubic Curve Name
+      1.0,                     !- Pump Motor Heat to Fluid
+      10.4,                    !- Sum UA Distribution Piping {W/C}
+      SalesFloor,              !- Distribution Piping Zone Name
+      1.4,                     !- Sum UA Receiver/Separator Shell
+      BackRoom,                !- Receiver/Separator Zone Name
+      ,                        !- Evaporator Refrigerant Inventory {kg}
+      ;                        !- End-Use Subcategory
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-11-005}
+
+FOR SECONDARY SYSTEMS SERVING CASES AND/OR WALKINS:
+
+\begin{itemize}
+\item
+  Zone,Average,Refrigeration Secondary Loop Pump Electric Power {[}W{]}
+\item
+  Zone,Sum,Refrigeration Secondary Loop Pump Electric Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Secondary Loop Load Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Secondary Loop Load Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Secondary Loop Total Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum,Refrigeration Secondary Loop Total Heat Transfer Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Secondary Loop Estimated Refrigerant Inventory Mass{[}kg{]} Zone,Average,Refrigeration Secondary Loop Volume Flow Rate {[}m3/s{]}
+\item
+  Zone,Average,Refrigeration Secondary Loop Pipe Heat Gain Rate {[}W{]}
+\item
+  Zone,Average,Refrigeration Secondary Loop Pipe Heat Gain Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Secondary Loop Receiver Heat Gain Rate {[}W{]}
+\item
+  Zone,Average,Refrigeration Secondary Loop Receiver Heat Gain Energy {[}J{]}
+\end{itemize}
+
+FOR SECONDARY SYSTEMS SERVING AIR CHILLERS:
+
+\begin{itemize}
+\item
+  HVAC,Average,Refrigeration Air Chiller Secondary Loop Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Air Chiller Secondary Loop Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller Secondary Loop Load Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Air Chiller Secondary Loop Load Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller Secondary Loop Total Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Air Chiller Secondary Loop Total Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller Secondary Loop Estimated Refrigerant Inventory Mass{[}kg{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller Secondary Loop Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller Secondary Loop Pipe Heat Gain Rate {[}W{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller Secondary Loop Pipe Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller Secondary Loop Receiver Heat Gain Rate {[}W{]}
+\item
+  HVAC,Average,Refrigeration Air Chiller Secondary Loop Receiver Heat Gain Energy {[}J{]}
+\end{itemize}
+
+\paragraph{FOR SECONDARY SYSTEMS SERVING CASES AND/OR WALKINS:}\label{for-secondary-systems-serving-cases-andor-walkins}
+
+\paragraph{Refrigeration Secondary Loop Pump Electric Power {[}W{]}}\label{refrigeration-secondary-loop-pump-electric-power-w}
+
+This output is the total electric power input to the pump(s) in Watts.
+
+\paragraph{Refrigeration Secondary Loop Pump Electric Energy {[}J{]}}\label{refrigeration-secondary-loop-pump-electric-energy-j}
+
+This is the electricity consumption of the system's pump(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Secondary Loop Load Heat Transfer Rate {[}W{]}}\label{refrigeration-secondary-loop-load-heat-transfer-rate-w}
+
+This is the amount of refrigeration provided to the cases and walkins served by the secondary loop in W.
+
+\paragraph{Refrigeration Secondary Loop Load Heat Transfer Energy {[}J{]}}\label{refrigeration-secondary-loop-load-heat-transfer-energy-j}
+
+This is the amount of refrigeration provided to the cases and walkins served by the secondary loop in Joules for the timestep being reported.
+
+\paragraph{Refrigeration Secondary Loop Total Heat Transfer Rate {[}W{]}}\label{refrigeration-secondary-loop-total-heat-transfer-rate-w}
+
+This is the total amount of refrigeration load placed upon the primary refrigeration system (including loads due to the cases and walkins plus the loads from the secondary loop pumps and any energy absorbed by the loop via pipe heat gains) in W.
+
+\paragraph{Refrigeration Secondary Loop Total Heat Transfer Energy {[}J{]}}\label{refrigeration-secondary-loop-total-heat-transfer-energy-j}
+
+This is the total amount of energy placed upon the primary refrigeration system by the secondary loop in Joules for the timestep being reported.
+
+\paragraph{Refrigeration Secondary Loop Estimated Refrigerant Inventory Mass {[}kg{]}}\label{refrigeration-secondary-loop-estimated-refrigerant-inventory-mass-kg}
+
+This output is the sum of the input inventory values for the cases and walkins and the refrigerant circulating through the loop.
+
+\paragraph{Refrigeration Secondary Loop Volume Flow Rate {[}m3/{]}s}\label{refrigeration-secondary-loop-volume-flow-rate-m3s}
+
+This output is the calculated volume flow through the pumps for this secondary loop.
+
+\paragraph{Refrigeration Secondary Loop Pipe Heat Gain Rate~ {[}W{]}}\label{refrigeration-secondary-loop-pipe-heat-gain-rate-w}
+
+This output is the total heat transferred to the pipes in Watts.
+
+\paragraph{Refrigeration Secondary Loop Pipe Heat Gain Energy {[}J{]}}\label{refrigeration-secondary-loop-pipe-heat-gain-energy-j}
+
+This is the total heat transferred to the pipes in Joules for the timestep being reported.
+
+\paragraph{Refrigeration Secondary Loop Receiver Heat Gain Rate~ {[}W{]}}\label{refrigeration-secondary-loop-receiver-heat-gain-rate-w}
+
+This output is the total heat transferred to the receiver in Watts.
+
+\paragraph{Refrigeration Secondary Loop Receiver Heat Gain Energy {[}J{]}}\label{refrigeration-secondary-loop-receiver-heat-gain-energy-j}
+
+This is the total heat transferred to the receiver in Joules for the timestep being reported.
+
+\paragraph{FOR SECONDARY SYSTEMS SERVING AIR CHILLERS:}\label{for-secondary-systems-serving-air-chillers}
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Pump Electric Power {[}W{]}}\label{refrigeration-air-chiller-secondary-loop-pump-electric-power-w}
+
+This output is the total electric power input to the pump(s) in Watts.
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Pump Electric Energy {[}J{]}}\label{refrigeration-air-chiller-secondary-loop-pump-electric-energy-j}
+
+This is the electricity consumption of the system's pump(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Load Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-secondary-loop-load-heat-transfer-rate-w}
+
+This is the amount of refrigeration provided to the air chillers served by the secondary loop in W.
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Load Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-secondary-loop-load-heat-transfer-energy-j}
+
+This is the amount of refrigeration provided to the air chillers served by the secondary loop in Joules for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Total Heat Transfer Rate {[}W{]}}\label{refrigeration-air-chiller-secondary-loop-total-heat-transfer-rate-w}
+
+This is the total amount of refrigeration load placed upon the primary refrigeration system (including loads due to the air chillers plus the loads from the secondary loop pumps and any energy absorbed by the loop via pipe heat gains) in W.
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Total Heat Transfer Energy {[}J{]}}\label{refrigeration-air-chiller-secondary-loop-total-heat-transfer-energy-j}
+
+This is the total amount of energy placed upon the primary refrigeration system by the secondary loop in Joules for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Estimated Refrigerant Inventory Mass {[}kg{]}}\label{refrigeration-air-chiller-secondary-loop-estimated-refrigerant-inventory-mass-kg}
+
+This output is the sum of the input inventory values for the air chillers~ and the refrigerant circulating through the loop.
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Volume Flow Rate {[}m3/{]}s}\label{refrigeration-air-chiller-secondary-loop-volume-flow-rate-m3s}
+
+This output is the calculated volume flow of coolant through the pumps for this secondary loop.
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Pipe Heat Gain Rate~ {[}W{]}}\label{refrigeration-air-chiller-secondary-loop-pipe-heat-gain-rate-w}
+
+This output is the total heat transferred to the pipes in Watts.
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Pipe Heat Gain Energy {[}J{]}}\label{refrigeration-air-chiller-secondary-loop-pipe-heat-gain-energy-j}
+
+This is the total heat transferred to the pipes in Joules for the timestep being reported.
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Receiver Heat Gain Rate~ {[}W{]}}\label{refrigeration-air-chiller-secondary-loop-receiver-heat-gain-rate-w}
+
+This output is the total heat transferred to the receiver in Watts.
+
+\paragraph{Refrigeration Air Chiller Secondary Loop Receiver Heat Gain Energy {[}J{]}}\label{refrigeration-air-chiller-secondary-loop-receiver-heat-gain-energy-j}
+
+This is the total heat transferred to the receiver in Joules for the timestep being reported.
+
+\subsection{Additional Refrigeration Outputs Available for Each Zone}\label{additional-refrigeration-outputs-available-for-each-zone}
+
+Multiple refrigeration cases and walkins may be located within a single zone.~ Each zone may also exchange heat with refrigeration system suction piping, secondary loop distribution piping, and secondary loop receivers. Output variables have been prepared to sum up the total heat exchange due to all refrigeration objects within a single zone.~ The output variables that start with ``Zone Refrigeration'' do not account for refrigeration provided by refrigeration chiller sets or any piping from systems serving air chillers.~ The output variables that start with ``Zone Chillers'' account for all the refrigeration system elements serving air chillers.
+
+\subsection{Additional Refrigeration Outputs for Each Zone}\label{additional-refrigeration-outputs-for-each-zone}
+
+FOR THE SUM OF ALL COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
+
+\begin{itemize}
+\item
+  Zone,Average, Refrigeration Zone Case and Walk In Sensible Cooling Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Zone Case and Walk In Sensible Cooling Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Zone Case and Walk In Heating Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Zone Case and Walk In Heating Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Zone Case and Walk In Total Sensible Cooling Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Zone Case and Walk In Total Sensible Cooling Energy {[}J{]}
+\item
+  Zone,Average, Refrigeration Zone Case and Walk In Total Latent Cooling Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Zone Case and Walk In Total Latent Cooling Energy {[}J{]}
+\item
+  Zone,Sum, Refrigeration Zone Case and Walk In Total Cooling Energy {[}J{]}
+\item
+  Zone,Average,Refrigeration Zone Case and Walk In Total Cooling Rate {[}W{]}
+\item
+  Zone,Average, Refrigeration Zone Case and Walk In Total Heat Transfer Rate {[}W{]}
+\item
+  Zone,Sum, Refrigeration Zone Case and Walk In Total Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+FOR THE SUM OF ALL COOLING SYSTEMS SERVING CHILLERS:
+
+\begin{itemize}
+\item
+  HVAC,Average, Refrigeration Zone Air Chiller Sensible Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum, Refrigeration Zone Air Chiller Sensible Heat Transfer Energy ~{[}J{]}
+\item
+  HVAC,Average, Refrigeration Zone Air Chiller Latent Cooling Rate~{[}W{]}
+\item
+  HVAC,Sum, Refrigeration Zone Air Chiller Latent Cooling Energy~{[}J{]}
+\item
+  HVAC,Average, Refrigeration Zone Air Chiller Total Cooling Rate~{[}W{]}
+\item
+  HVAC,Sum, Refrigeration Zone Air Chiller Total Cooling Energy~{[}J{]}
+\end{itemize}
+
+\subsubsection{FOR THE SUM OF ALL COOLING SYSTEMS SERVING CASES AND/OR WALKINS:}\label{for-the-sum-of-all-cooling-systems-serving-cases-andor-walkins}
+
+\subsubsection{Refrigeration Zone Case and Walk In Total Sensible Cooling Rate {[}W{]}}\label{refrigeration-zone-case-and-walk-in-total-sensible-cooling-rate-w}
+
+This output is the total sensible heat transfer between all refrigeration objects located in the zone in Watts. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
+
+\textbf{\emph{Refrigeration Zone Case and Walk In Total Sensible Cooling Energy {[}J{]}}}
+
+This is the total sensible heat transfer between all refrigeration objects located in the zone in Joules for for the timestep being reported. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
+
+\subsubsection{Refrigeration Zone Case and Walk In Total Latent Cooling Rate {[}W{]}}\label{refrigeration-zone-case-and-walk-in-total-latent-cooling-rate-w}
+
+This output is the total latent heat transfer between all refrigeration objects located in the zone in Watts. A negative value will be reported when the refrigeration equipment provides dehumidification (thereby reducing the zone latent load).
+
+\textbf{\emph{Refrigeration Zone Case and Walk In Total Latent Cooling Energy {[}J{]}}}
+
+This is the total latent heat transfer between all refrigeration objects located in the zone in Joules for for the timestep being reported. A negative value will be reported when the refrigeration equipment provides dehumidification (thereby reducing the zone latent load).
+
+\subsubsection{Refrigeration Zone Case and Walk In Total Heat Transfer Rate {[}W{]}}\label{refrigeration-zone-case-and-walk-in-total-heat-transfer-rate-w}
+
+This output is the total heat transfer (sensible plus latent) between all refrigeration objects located in the zone in Watts. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
+
+\textbf{\emph{Refrigeration Zone Case and Walk In Total Heat Transfer Energy {[}J{]}}}
+
+This is the total heat transfer (sensible plus latent) between all refrigeration objects located in the zone in Joules for for the timestep being reported. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
+
+\subsubsection{Refrigeration Zone Case and Walk In Sensible Cooling Rate {[}W{]}}\label{refrigeration-zone-case-and-walk-in-sensible-cooling-rate-w}
+
+This output is the total sensible cooling from all refrigeration objects located in the zone in Watts.
+
+\textbf{\emph{Refrigeration Zone Case and Walk In Sensible Cooling Energy {[}J{]}}}
+
+This is the total sensible cooling from all refrigeration objects located in the zone in Joules for for the timestep being reported.
+
+\subsubsection{Refrigeration Zone Case and Walk In Heating Rate {[}W{]}}\label{refrigeration-zone-case-and-walk-in-heating-rate-w}
+
+This output is the total heating from all refrigeration objects located in the zone in Watts.
+
+\textbf{\emph{Refrigeration Zone Case and Walk In Heating Energy {[}J{]}}}
+
+This is the total heating from all refrigeration objects located in the zone in Joules for for the timestep being reported.
+
+\subsubsection{Refrigeration Zone Case and Walk In Total Cooling Rate {[}W{]}}\label{refrigeration-zone-case-and-walk-in-total-cooling-rate-w}
+
+This output is the total cooling (sensible plus latent) from all refrigeration objects located in the zone in Watts.
+
+\textbf{\emph{Refrigeration Zone Case and Walk In Total Cooling Energy {[}J{]}}}
+
+This is the total cooling (sensible plus latent) from all refrigeration objects located in the zone in Joules for for the timestep being reported.
+
+\subsubsection{FOR THE SUM OF ALL COOLING SYSTEMS SERVING AIR CHILLERS:}\label{for-the-sum-of-all-cooling-systems-serving-air-chillers}
+
+\subsubsection{Refrigeration Zone Air Chiller Heating Rate ~{[}W{]}}\label{refrigeration-zone-air-chiller-heating-rate-w}
+
+This output is the total heating from all air chillers located in the zone in Watts.
+
+\textbf{\emph{Refrigeration Zone Air Chiller Heating Energy {[}J{]}}}
+
+This is the total heating from all air chillers located in the zone in Joules for for the timestep being reported.
+
+\subsubsection{Refrigeration Zone Air Chiller Sensible Cooling Rate~~ {[}W{]}}\label{refrigeration-zone-air-chiller-sensible-cooling-rate-w}
+
+This output is the total sensible cooling from all air chillers located in the zone in Watts.
+
+\textbf{\emph{Refrigeration Zone Air Chiller Sensible Cooling Energy {[}J{]}}}
+
+This is the total sensible cooling from all air chillers located in the zone in Joules for for the timestep being reported.
+
+\subsubsection{Refrigeration Zone Air Chiller Sensible Heat Transfer Rate ~{[}W{]}}\label{refrigeration-zone-air-chiller-sensible-heat-transfer-rate-w}
+
+This output is the total sensible heat transfer from all air chillers located in the zone in Watts. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
+
+\subsubsection{Refrigeration Zone Air Chiller Sensible Heat Transfer Energy ~{[}J{]}}\label{refrigeration-zone-air-chiller-sensible-heat-transfer-energy-j}
+
+This is the total sensible heat transfer from all air chillers located in the zone in Joules for for the timestep being reported. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
+
+\subsubsection{Refrigeration Zone Air Chiller Latent Cooling Rate ~{[}W{]}}\label{refrigeration-zone-air-chiller-latent-cooling-rate-w}
+
+This output is the total latent cooling from all air chillers located in the zone in Watts.
+
+\textbf{\emph{Refrigeration Zone Air Chiller Latent Cooling Energy {[}J{]}}}
+
+This is the total latent cooling from all air chillers located in the zone in Joules for for the timestep being reported.
+
+\subsubsection{Refrigeration Zone Air Chiller Water Removed Mass Flow Rate~ {[}kg/s{]}}\label{refrigeration-zone-air-chiller-water-removed-mass-flow-rate-kgs}
+
+This is the total amount of water removed by all air chillers located in the zone in kg/s for for the timestep being reported.
+
+\subsubsection{Refrigeration Zone Air Chiller Total Cooling Rate ~{[}W{]}}\label{refrigeration-zone-air-chiller-total-cooling-rate-w}
+
+This output is the total cooling (sensible plus latent) from all air chillers located in the zone in Watts.
+
+\textbf{\emph{Refrigeration Zone Air Chiller Total Cooling Energy {[}J{]}}}
+
+This is the total cooling (sensible plus latent) from all air chillers located in the zone in Joules for for the timestep being reported.
+
+\subsection{Refrigeration:AirChiller}\label{refrigerationairchiller}
+
+The Refrigeration:AirChiller object works in conjunction with a refrigeration chiller set, compressor rack, a refrigeration system, or a refrigeration secondary system object (Ref. ZoneHvac:RefrigerationChillerSet, and a Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem) to simulate the performance of an air chiller, similar to one found in a refrigerated warehouse. The air chiller model uses information at rated conditions along with the zone conditions to determine performance. Energy use for fans and heaters is modeled based on inputs for nominal power, schedules, and control type. The refrigeration chiller model accounts for the sensible and latent heat exchange with the surrounding environment.
+
+The refrigeration chiller cooler object inputs include a name, an availability schedule name, the rated cooling capacity, the rated operating temperature, the rated cooling source temperature, the rated total heating power and heating power schedule, the rated fan power and schedules, defrost type, defrost control type, defrost schedule name, drip-down schedule name, defrost power, the portion of the defrost energy used to melt ice (only for temperature termination control type), and refrigerant inventory.
+
+Chiller coils are rated under multiple conventions. Each rating is typically based upon a selected fin material and refrigerant cycle, with correction factors for other materials or refrigerants. Fields are provided here for those correction factors. The performance of all chiller coils depends upon the inlet air temperature, relative humidity, and flow rate. Multiple methods of expressing this relationship are provided here to accommodate the way information is provided by different manufacturers.
+
+\subsubsection{Inputs}\label{inputs-15-011}
+
+\paragraph{Field: Name}\label{field-name-16-007}
+
+A unique user-assigned name for an instance of a refrigeration chiller. Any reference to this refrigeration chiller by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-2-007}
+
+The name of the schedule (ref: Schedule) that denotes whether the refrigeration chiller can operate during a given time period. A schedule value greater than 0 (maximum schedule value of 1.0 is typically used) indicates that the refrigeration chiller will operate during a given time period. A value equal to 0 denotes that the case does not operate (everything is OFF: refrigeration, fans, lights, anti-sweat, etc.). Typically the refrigeration chiller will operate throughout the day (i.e., the schedule will contain 1 for all time periods); however, refrigeration chillers require maintenance and/or cleaning and this can be modeled accordingly using this schedule if desired. If this field is left blank, the default schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Capacity Rating Type}\label{field-capacity-rating-type}
+
+The type of capacity rating used for this refrigeration chiller. Valid choices are UnitLoadFactorSensibleOnly, CapacityTotalSpecificConditions, EuropeanSC1Standard, EuropeanSC1NominalWet, EuropeanSC2Standard, EuropeanSC2NominalWet, EuropeanSC3Standard, EuropeanSC3NominalWet, EuropeanSC4Standard, EuropeanSC4NominalWet, EuropeanSC5Standard, and EuropeanSC5NominalWet. In each case, select the rating option that corresponds to the expected service conditions.~ For example, U.S. manufacturers quote a separate Unit Load Factor for wet or frosted coils.~ If the evaporating temperature is less than 0C, input the frosted coil value. Within the European convention, select SC1, 2, 3, 4, or 5 depending upon the expected evaporating temperature. This field is required and there is no default value. Refer to the Engineering Reference for further information on these rating types. NOTE: If the CapacityTotalSpecificConditions rating type is specified, the input file must include the manufacturer's coil capacity correction curve in tabular form using the Table:MultiVariableLookup object. An example of this may be found in the RefrigeratedWarehouse.idf example file.
+
+\paragraph{NOTE -- ONLY ONE OF THE FOLLOWING TWO FIELDS IS USED}\label{note-only-one-of-the-following-two-fields-is-used}
+
+\paragraph{Field: Rated Unit Load Factor}\label{field-rated-unit-load-factor}
+
+The sensible cooling capacity in watts (W/C) at rated conditions. The value entered for this field must be greater than zero, with no default value. This value is only used if the Capacity Rating Type is UnitLoadFactorSensibleOnly. The value given must be based upon the difference between the chiller inlet and outlet air temperatures, not on the difference between the zone mean temperature and the outlet air temperature.
+
+\paragraph{Field: Rated Capacity}\label{field-rated-capacity-001}
+
+The cooling capacity in watts (W) at rated conditions. The value entered for this field must be greater than zero, with no default value. This field is only used if the Capacity Rating Type is CapacityTotalSpecificConditions, EuropeanSC1Standard, EuropeanSC1NominalWet, EuropeanSC2Standard, EuropeanSC2NominalWet, EuropeanSC3Standard, EuropeanSC3NominalWet, EuropeanSC4Standard, EuropeanSC4NominalWet, EuropeanSC5Standard, or EuropeanSC5NominalWet. For CapacityTotalSpecificConditions, this capacity includes both sensible and latent at the conditions given in the next two fields.~ Note that the European Standard ratings are sensible only and the European Nominal ratings include latent capacity as well. The value given here must correspond to the capacity rating type given previously.
+
+\paragraph{Field: Rated Relative Humidity}\label{field-rated-relative-humidity}
+
+This field is ONLY used if the Capacity Rating Type is CapacityTotalSpecificConditions and represents the relative humidity at rated conditions, expressed as a percent. The default is 85.
+
+\paragraph{Field: Rated Cooling Source Temperature}\label{field-rated-cooling-source-temperature-1}
+
+For a DX evaporator coil, enter the saturated evaporating temperature in ËšC.~ For a fluid coil, enter the fluid coil entrance temperature in ËšC. There is no default value. This number is used, with temperatures for other refrigeration loads on any one system, to set that system's minimum suction pressure or minimum circulating fluid temperature.
+
+\paragraph{Field: Rated Temperature Difference DT1}\label{field-rated-temperature-difference-dt1}
+
+The rated difference between the air entering the refrigeration chiller and the cooling source temperature in ËšC. The entered value for this field must be less than 20ËšC. There is no default value.
+
+\paragraph{Field: Maximum Difference Between Inlet Air and Evaporating Temperature}\label{field-maximum-difference-between-inlet-air-and-evaporating-temperature}
+
+The maximum difference between the air entering the refrigeration chiller and the cooling source temperature in °C used to limit capacity during pull-down. The default is 1.3 times the Rated Temperature Difference DT1.
+
+\paragraph{Field: Coil~ Material Correction Factor}\label{field-coil-material-correction-factor}
+
+This field is used to enter the manufacturer's correction factor for coil material corresponding to the rating previously input. The default is 1.0 (dimensionless).
+
+\paragraph{Field: Refrigerant Correction Factor}\label{field-refrigerant-correction-factor}
+
+This field is used to enter the manufacturer's correction factor for refrigerant corresponding to the rating previously input. The default is 1.0 (dimensionless). (Note, the refrigerant itself is specified for the detailed system or secondary loop providing the refrigerant to this coil.)
+
+\paragraph{Field: Capacity Correction Curve Type}\label{field-capacity-correction-curve-type}
+
+The type of capacity correction curve used to account for the impact of the room air conditions on the chiller capacity. Valid choices are LinearSHR60, QuadraticSHR, European, and TabularRHxDT1xTRoom. This field will default to LinearSHR60, unless the CapacityTotalSpecificConditions rating type is specified, in which case, the TabularRHxDT1xTRoom correction curve type must be used. Refer to the Engineering Reference for further information on these curve types. The resulting correction factor for LinearSHR60, QuadraticSHR, and European types will be applied to the sensible capacity and must have output values between 1 and 2. The resulting correction factor for TabularRHxDT1xTRoom will be applied to the CapacityTotalSpecificConditions capacity and can have values between 0.2 and 2. If TabularRHxDT1xTRoom is used, the curve type within the table must be specified as ``Quadratic''.
+
+\paragraph{Field: Capacity Correction Curve Name}\label{field-capacity-correction-curve-name}
+
+The name of the curve object defining the total refrigerating capacity. For correction curve types LinearSHR60 and QuadraticSHR, the independent variable is the Sensible Heat Ratio and the output values are between 1.0 and 2.0. For correction curve type European, EnergyPlus contains built-in capacity correction curves and specification of a capacity correction curve name is not required. For correction curve type TabularRHxDT1xTRoom, enter the name of a Table:MultiVariableLookup object that gives the total capacity (in W) as a function of RH, DT1, and Room Temperature; IN THAT ORDER. An example of a TabularRHxDT1xTRoom correction curve using the Table:MultiVariableLoopkup object may be found in the RefrigeratedWarehouse.idf example file.
+
+\paragraph{Field: SHR60 Correction Factor}\label{field-shr60-correction-factor}
+
+This field is only used when the capacity correction curve type is LinearSHR60. It should correspond to the capacity factor, that is, the total capacity divided by the sensible capacity corresponding to a Sensible Heat Ratio of 0.6. The default is 1.48 (dimensionless).
+
+\paragraph{Field: Rated Total Heating Power}\label{field-rated-total-heating-power-1}
+
+The total heating power in watts including drip-pan and any other heaters (W). This value is required and has no default value.
+
+\paragraph{Field: Heating Power Schedule Name}\label{field-heating-power-schedule-name-1}
+
+The name of the schedule (ref: Schedule) that denotes the fraction of heater power that operates during a given time period. A schedule value of zero denotes that all heaters are off. A schedule value greater than 0 indicates that some portion of the total heater power will operate during that time period (maximum schedule value of 1.0 means all heaters are fully on). If this field is left blank, the default schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Fan Speed Control Type}\label{field-fan-speed-control-type-1}
+
+The type of fan speed control used by the cooling coil's fan(s). Valid choices are \textbf{Fixed}, \textbf{FixedLinear}, \textbf{VariableSpeed}, and \textbf{TwoSpeed}.~ If the field is blank, \textbf{Fixed} will be used. See the Engineering Reference for a discussion of this option's effect on fan energy consumption.
+
+\paragraph{Field: Rated Fan Power}\label{field-rated-fan-power-3}
+
+The cooling coil fan power in watts (W). This value has a default value of 375W. This fan is assumed to run continuously except during electric, hot brine, or hot gas defrost periods.
+
+\paragraph{Field: Rated Air Flow}\label{field-rated-air-flow}
+
+The cooling coil fan rated air flow in cubic meters per second (m\(^{3}\)/s). This value has no default value and must be input.
+
+\paragraph{Field: Minimum Fan Air Flow Ratio}\label{field-minimum-fan-air-flow-ratio-3}
+
+The minimum fraction of the rated air flow for part-load fan operation, must be between 0. and 1.0. The default value is 0.2.
+
+\paragraph{Field: Defrost Type}\label{field-defrost-type-1}
+
+The type of defrost used for this refrigeration chiller. Valid choices are None, Off-Cycle, HotFluid, and Electric. The default defrost type is Electric if the field is blank. HotFluid includes both hot gas and hot brine defrost systems. Refer to the Engineering Reference for further information on how the different defrost types are modeled.
+
+\paragraph{Field: Defrost Control Type}\label{field-defrost-control-type-1}
+
+The type of defrost control used for this refrigeration chiller. Valid choices are TimeSchedule and TemperatureTermination. The default is TimeSchedule if the field is blank. Refer to the Engineering Reference for further information on how the different defrost controls are modeled.
+
+\paragraph{Field: Defrost Schedule Name}\label{field-defrost-schedule-name-1}
+
+The name of the schedule (ref: Schedule) that denotes when the refrigeration chiller requires defrosting. A schedule value of 1.0 indicates that defrost can be on during a given time period. A value equal to 0 denotes that the defrost is off. Defrost schedules normally repeat the duration and number of defrost cycles for each day of the year. The refrigeration chiller manufacturer typically provides this information with the product literature. If TemperatureTermination control type is used, the defrost schedule is used for the defrost cycle start time and the defrost cycle end time is not allowed to extend beyond the scheduled off time. The use of Compact Schedules (ref. Schedules) are ideal for this purpose.
+
+\paragraph{Field: Defrost Drip-Down Schedule Name}\label{field-defrost-drip-down-schedule-name-1}
+
+The name of the schedule (ref: Schedule) that denotes whether the refrigeration chiller requires additional time for draining condensate after the defrost period. A schedule value of 1.0 indicates that the defrost drip-down period is on during a given time period. A value equal to 0 denotes that the defrost drip-down period is over. The refrigeration chiller manufacturer typically provides this information with the product literature.
+
+Each defrost drip-down period specified in this schedule should start at the same time as the corresponding defrost period specified in the schedule for Defrost Schedule, and the drip-down schedule defrost period should always be longer than or equal to the length of the defrost schedule time period. For example, if the defrost schedule contains a defrost period from 7:00 to 7:15, you would specify a case defrost drip-down period from 7:00 to 7:20 if you wanted to model a 5 minute condensate drip-down period after the regular defrost period. If no drip-down schedule is entered, then the defrost schedule (specified for the previous input field) will be used. The use of Compact Schedules (ref. Schedules) are ideal for this purpose.
+
+\paragraph{Field: Defrost Power}\label{field-defrost-power-1}
+
+The defrost power in watts. This input is required for hot-fluid (hot gas or hot brine), or electric defrost types. Refrigeration chiller manufacturers do not typically provide information on the heat input for hot gas and hot brine defrost. Information provided for electric defrost power can be substituted here for refrigeration chillers using hot-gas or hot-brine defrost if other information is not available. Only electric Defrost Types consume electricity during the defrost period. The entered value for this field must be greater than or equal to zero.
+
+\paragraph{Field: Temperature Termination Defrost Fraction to Ice}\label{field-temperature-termination-defrost-fraction-to-ice-1}
+
+When cooling coils go through a defrost cycle, only a portion of the defrost energy is actually used to melt the ice.~ The rest of the defrost energy goes to increasing the temperature of the coils themselves and to the refrigeration chiller environment. The Temperature Termination defrost control type calculates the end of the defrost cycle that corresponds to melting all the ice. Therefore, the user must input this fractional value. The default value is 0.7 for electric defrost and 0.3 for hot fluid defrost. Refer to the Engineering Reference for further information on how the defrost energy control types are modeled.
+
+\paragraph{Field: Vertical Location}\label{field-vertical-location}
+
+The vertical location for this refrigeration chiller. Valid choices are Floor, Middle, and Ceiling. The default is Middle if the field is blank. The vertical location is used to transform the mixed zone air temperature to the coil inlet air temperature. Refer to the Engineering Reference for further information on how the different vertical locations are modeled.
+
+\paragraph{Field: Average Refrigerant Charge Inventory}\label{field-average-refrigerant-charge-inventory-2}
+
+The value of this optional field is the refrigerant inventory present in the refrigeration chiller during ordinary operation. The value is used to produce an estimate of the total refrigerant present in the refrigeration system. The value is entered in kg.
+
+The following is an example input for a refrigeration air chiller.
+
+\begin{lstlisting}
+
+   Refrigeration:AirChiller,
+      Freezer_1AirChiller_1,    !- Name
+      AvailAllYear,             !- Availability Schedule Name
+      UnitLoadFactorSensibleOnly, !- Capacity Rating Type
+      10900.,                   !- Rated Unit Load Factor {W/deltaC}
+      ,                         !- Rated Capacity {W}
+      ,                         !- Rated Relative Humidity
+      -26.,                     !- Rated Cooling Source Temperature {C}
+      8.,                       !- Rated Temperature Difference DT1 {DeltaC}
+      11.,                      !- Maximum Temperature Difference DT1 {DeltaC}
+      ,                         !- Material Correction Factor
+      ,                         !- Refrigerant Correction Factor
+      LinearSHR60,              !- Capacity Correction Curve Type
+      ,                         !- Capacity Correction Curve Name
+      1.5,                      !- SHR60 Correction Factor {dimensionless}
+      200.,                     !- Rated Total Heating Power {W}
+      AirChillerDripDownSched1,    !- Heating Power Schedule Name
+      ,                         !- Fan Speed Control Type
+      375.,                     !- Rated Fan Power {W}
+      12.4,                     !- Rated Air Flow {m3/s}
+      ,                         !- Minimum Fan Air Flow Ratio
+      Electric,                 !- Defrost Type
+      TimeSchedule,             !- Defrost Control Type
+      AirChillerDefrostSched1,  !- Defrost Schedule Name
+      AirChillerDripDownSched1, !- Defrost Drip-Down Schedule Name
+      55066.,                  !- Defrost Power {W}
+      ,                         !- Temperature Termination Defrost Fraction to Ice
+      ,                         !- Vertical Location
+      ;                         !- Average Refrigerant Charge Inventory {kg}
+\end{lstlisting}
+
+The following is an example input for a refrigeration air chiller.
+
+\begin{lstlisting}
+
+   Refrigeration:AirChiller,
+      Freezer_1AirChiller_1,    !- Name
+      AvailAllYear,             !- Availability Schedule Name
+      UnitLoadFactorSensibleOnly, !- Capacity Rating Type
+      10900.,                   !- Rated Unit Load Factor {W/deltaC}
+      ,                         !- Rated Capacity {W}
+      ,                         !- Rated Relative Humidity
+      -26.,                     !- Rated Cooling Source Temperature {C}
+      8.,                       !- Rated Temperature Difference DT1 {DeltaC}
+      11.,                      !- Maximum Temperature Difference DT1 {DeltaC}
+      ,                         !- Material Correction Factor
+      ,                         !- Refrigerant Correction Factor
+      LinearSHR60,              !- Capacity Correction Curve Type
+      ,                         !- Capacity Correction Curve Name
+      1.5,                      !- SHR60 Correction Factor {dimensionless}
+      200.,                     !- Rated Total Heating Power {W}
+      AirChillerDripDownSched1,    !- Heating Power Schedule Name
+      ,                         !- Fan Speed Control Type
+      375.,                     !- Rated Fan Power {W}
+      12.4,                     !- Rated Air Flow {m3/s}
+      ,                         !- Minimum Fan Air Flow Ratio
+      Electric,                 !- Defrost Type
+      TimeSchedule,             !- Defrost Control Type
+      AirChillerDefrostSched1,  !- Defrost Schedule Name
+      AirChillerDripDownSched1, !- Defrost Drip-Down Schedule Name
+      55066.,                  !- Defrost Power {W}
+      ,                         !- Temperature Termination Defrost Fraction to Ice
+      ,                         !- Vertical Location
+      ;                         !- Average Refrigerant Charge Inventory {kg}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-12-005}
+
+\begin{itemize}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Zone Air Chiller Water Removed Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Total Electric Power {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Total Electric Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Sensible Heat Ratio {[]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Frost Accumulation Mass {[}kg{]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Zone Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Zone Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Zone Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Zone Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Zone Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Zone Heating Energy {[}J{]}
+\end{itemize}
+
+\emph{Report only for Air Chillers using electric defrost}
+
+\begin{itemize}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Defrost Electric Power {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Defrost Electric Energy {[}J{]}
+\end{itemize}
+
+\textbf{\emph{Report for each Zone exchanging energy with the Air Chiller}}
+
+\begin{itemize}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Zone Air Chiller Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Heating Energy {[}J{]}
+\item
+  HVAC,Average, Refrigeration Zone Air Chiller Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Latent Cooling Energy {[}J
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Refrigeration Zone Air Chiller Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Refrigeration Zone Air Chiller Water Removed Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Refrigeration Zone Air Chiller Total Cooling Rate {[}W{]}}\label{refrigeration-zone-air-chiller-total-cooling-rate-w-1}
+
+This field is the total (sensible plus latent) cooling rate of the Air Chiller evaporator coil in Watts.
+
+\paragraph{Refrigeration Zone Air Chiller Total Cooling Energy {[}J{]}}\label{refrigeration-zone-air-chiller-total-cooling-energy-j}
+
+This field is the total (sensible plus latent) cooling of the Air Chiller evaporator coil in Joules over the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Zone Air Chiller Sensible Cooling Rate {[}W{]}}\label{refrigeration-zone-air-chiller-sensible-cooling-rate-w-1}
+
+\paragraph{Refrigeration Zone Air Chiller Sensible Heat Transfer Rate {[}W{]}}\label{refrigeration-zone-air-chiller-sensible-heat-transfer-rate-w-1}
+
+This field is the sensible cooling rate of the Air Chiller evaporator coil in Watts.
+
+\paragraph{Refrigeration Zone Air Chiller Sensible Cooling Energy ~{[}J{]}}\label{refrigeration-zone-air-chiller-sensible-cooling-energy-j}
+
+\paragraph{Refrigeration Zone Air Chiller Sensible Heat Transfer Energy {[}J{]}}\label{refrigeration-zone-air-chiller-sensible-heat-transfer-energy-j-1}
+
+This field is the sensible cooling of the Air Chiller evaporator coil in Joules over the timestep being reported.
+
+\paragraph{Refrigeration Zone Air Chiller Latent Cooling Rate ~{[}W{]}}\label{refrigeration-zone-air-chiller-latent-cooling-rate-w-1}
+
+This field is the latent cooling (dehumidification) rate of the Air Chiller evaporator coil in Watts.
+
+\paragraph{Refrigeration Zone Air Chiller Latent Cooling Energy ~{[}J{]}}\label{refrigeration-zone-air-chiller-latent-cooling-energy-j}
+
+This field is the latent cooling (dehumidification) of the Air Chiller evaporator coil in Joules over the timestep being reported.
+
+\paragraph{Refrigeration Zone Air Chiller Water Removed Mass Flow Rate ~{[}kg/s{]}}\label{refrigeration-zone-air-chiller-water-removed-mass-flow-rate-kgs-1}
+
+This field is the latent cooling (dehumidification) of the Air Chiller evaporator coil in kilograms per second over the timestep being reported.
+
+\paragraph{Refrigeration Zone Air Chiller Total Electric Power {[}W{]}}\label{refrigeration-zone-air-chiller-total-electric-power-w}
+
+This field is the total electricity (fan, heaters, lights, and electric defrost) used by the Air Chiller in Watts.
+
+\paragraph{Refrigeration Zone Air Chiller Total Electric Energy {[}J{]}}\label{refrigeration-zone-air-chiller-total-electric-energy-j}
+
+This field is the electricity (fan, heaters, lights, and electric defrost)used by the Refrigeration chiller in Joules over the timestep being reported.
+
+\paragraph{Refrigeration Zone Air Chiller Fan Electric Power {[}W{]}}\label{refrigeration-zone-air-chiller-fan-electric-power-w}
+
+This field is the electric power input to the Air Chiller fan(s) in Watts.
+
+\paragraph{Refrigeration Zone Air Chiller Fan Electric Energy ~{[}J{]}}\label{refrigeration-zone-air-chiller-fan-electric-energy-j}
+
+This field is the electricity consumption of the Air Chiller fan(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Zone Air Chiller Heater Electric Power~ {[}W{]}}\label{refrigeration-zone-air-chiller-heater-electric-power-w}
+
+This field is the electric power input to the Air Chiller heaters in Watts.
+
+\paragraph{Refrigeration Zone Air Chiller Heater Electric Energy {[}J{]}}\label{refrigeration-zone-air-chiller-heater-electric-energy-j}
+
+This field is the total electricity consumption of the Air Chiller heaters in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
+
+\paragraph{Refrigeration Zone Air Chiller Defrost Electric Power~ {[}W{]}}\label{refrigeration-zone-air-chiller-defrost-electric-power-w}
+
+This field is the electric power input to the Air Chiller electric defrost heater(s) in Watts. This output is available if case defrost type is Electric.
+
+\paragraph{Refrigeration Zone Air Chiller Defrost Electric Energy {[}J{]}}\label{refrigeration-zone-air-chiller-defrost-electric-energy-j}
+
+This field is the total electricity consumption of the Air Chiller electric defrost heater(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects). This output is available if case defrost type is Electric.
+
+\paragraph{Refrigeration Zone Air Chiller Sensible Heat Ratio}\label{refrigeration-zone-air-chiller-sensible-heat-ratio}
+
+This field is the Sensible Cooling Energy ~Rate divided by the Total Cooling Energy Rate.
+
+\paragraph{Refrigeration Zone Air Chiller Frost Accumulation Mass {[}kg{]}}\label{refrigeration-zone-air-chiller-frost-accumulation-mass-kg}
+
+This field is the total amount of frost present on the coil during the timestep being reported.
+
+\paragraph{Refrigeration Zone Air Chiller Zone Total Cooling Rate {[}W{]}}\label{refrigeration-zone-air-chiller-zone-total-cooling-rate-w}
+
+This field is the rate of total cooling delivered to the zone in Watts. A positive value is reported when the zone is cooled by the air chiller, otherwise a zero is reported.
+
+\paragraph{Refrigeration Zone Air Chiller Zone Total Cooling Energy ~{[}J{]}}\label{refrigeration-zone-air-chiller-zone-total-cooling-energy-j}
+
+This field is the amount of total cooling energy delivered to the zone in Joules. A positive value is reported when the zone is cooled by the air chiller, otherwise a zero is reported.
+
+\paragraph{Refrigeration Zone Air Chiller Zone Sensible Cooling Rate {[}W{]}}\label{refrigeration-zone-air-chiller-zone-sensible-cooling-rate-w}
+
+This field is the rate of sensible cooling delivered to the zone in Watts. A positive value is reported when the zone is cooled by the air chiller, otherwise a zero is reported.
+
+\paragraph{Refrigeration Zone Air Chiller Zone Sensible Cooling Energy {[}J{]}}\label{refrigeration-zone-air-chiller-zone-sensible-cooling-energy-j}
+
+This field is the amount of sensible cooling energy delivered to the zone in Joules. A positive value is reported when the zone is cooled by the air chiller, otherwise a zero is reported.
+
+\paragraph{Refrigeration Zone Air Chiller Zone Heating Rate {[}W{]}}\label{refrigeration-zone-air-chiller-zone-heating-rate-w}
+
+This field is the rate of sensible heating delivered to the zone in Watts. A positive value is reported when the zone is heated by the air chiller (typically only occurs during defrost), otherwise a zero is reported.
+
+\paragraph{Refrigeration Zone Air Chiller Zone Heating Energy {[}J{]}}\label{refrigeration-zone-air-chiller-zone-heating-energy-j}
+
+This field is the amount of sensible heating energy delivered to the zone in Joules. A positive value is reported when the zone is heated by the air chiller (typically only occurs during defrost), otherwise a zero is reported.
+
+\emph{The following output variables are available for each zone served by any Air Chiller. An output variable identification is created for each zone exchanging energy with the Air Chiller.~ For example if the Air Chiller, ``DairyRefrigeration chiller'', were exchanging energy with the zone, ``SalesArea'', the output variable identification would be ``DairyRefrigeration chillerInZoneSalesArea''.}
+
+\paragraph{Refrigeration Zone Air Chiller Sensible Cooling Rate~ {[}W{]}}\label{refrigeration-zone-air-chiller-sensible-cooling-rate-w-2}
+
+This field is the rate of sensible cooling delivered to the zone, net of any auxiliary heat input,~ in Watts..
+
+\paragraph{Refrigeration Zone Air Chiller Sensible Cooling Energy {[}J{]}}\label{refrigeration-zone-air-chiller-sensible-cooling-energy-j-1}
+
+This field is the amount of sensible cooling energy, net of any auxiliary heat input, delivered to the zone in Joules.
+
+\paragraph{Refrigeration Zone Air Chiller Latent Cooling Rate {[}W{]}}\label{refrigeration-zone-air-chiller-latent-cooling-rate-w-2}
+
+This field is the rate of latent cooling (dehumidification) delivered to the zone in Watts. A negative value will be reported when the Air Chiller provides dehumidification (thereby reducing the zone latent load).
+
+\paragraph{Refrigeration Zone Air Chiller Water Removed Mass Flow Rate~ {[}kg/s{]}}\label{refrigeration-zone-air-chiller-water-removed-mass-flow-rate-kgs-2}
+
+This field is the rate of latent cooling (dehumidification) delivered to the zone in kg/s. A negative value (or zero) will be reported when the Air Chiller provides dehumidification (thereby reducing the zone latent load).
+
+\paragraph{Refrigeration Zone Air Chiller Latent Cooling Energy {[}J{]}}\label{refrigeration-zone-air-chiller-latent-cooling-energy-j-1}
+
+This field is the amount of latent cooling (dehumidification) energy delivered to the zone in Joules. A negative value (or zero) will be reported when the Air Chiller provides dehumidification (thereby reducing the zone latent load).
+
+\paragraph{Refrigeration Zone Air Chiller Total Cooling Rate {[}W{]}}\label{refrigeration-zone-air-chiller-total-cooling-rate-w-2}
+
+This field is the total rate of cooling, sensible plus latent, delivered to the zone in Watts.
+
+\paragraph{Refrigeration Zone Air Chiller Total Cooling Energy {[}J{]}}\label{refrigeration-zone-air-chiller-total-cooling-energy-j-1}
+
+This field is the total amount of cooling, sensible plus latent, energy delivered to the zone in Joules.
+
+\paragraph{Refrigeration Zone Air Chiller Heating Rate~ {[}W{]}}\label{refrigeration-zone-air-chiller-heating-rate-w-1}
+
+This field is the rate of net heating due to any auxiliary or defrost heat input delivered to the zone,~ in Watts.
+
+\paragraph{Refrigeration Zone Air Chiller Heating Energy {[}J{]}}\label{refrigeration-zone-air-chiller-heating-energy-j}
+
+This field is the amount of net heating energy due to any auxiliary heat input, delivered to the zone in Joules.
diff --git a/doc/input-output-reference/src/overview/group-room-air-models.tex b/doc/input-output-reference/src/overview/group-room-air-models.tex
new file mode 100644
index 00000000000..fb9f71fccba
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-room-air-models.tex
@@ -0,0 +1,1316 @@
+\section{Group -- Room Air Models}\label{group-room-air-models}
+
+\subsection{Room Air Models}\label{room-air-models}
+
+The group of input objects described in this section is used to account for non-uniform room air temperatures that may occur within the interior air volume of a zone. Room air modeling was added to EnergyPlus starting with Version 1.2. Although there are many types of analyses (comfort, indoor air quality, etc) that might benefit from localized modeling of how room air varies across space, only the \emph{temperature} distribution of room air within the zone is currently addressed in EnergyPlus. This allows surface heat transfer and air system heat balance calculations to be made taking into account natural thermal stratification of air and different types of intentional air distribution designs such as under-floor and side-wall displacement ventilation that purport to extract room air at higher-than-mean temperatures. Note that EnergyPlus does \textbf{not} have completely general methods of modeling room air that are applicable to every conceivable type of airflow that might occur in a zone. Such models (e.g.~RANS-CFD) are too computationally expensive to use with EnergyPlus for the foreseeable future. The models that are available in EnergyPlus offer only limited modeling capabilities for select room airflow configurations. Also note that because the complete mixing model for room air has long been the standard in building energy simulation, there is not currently a consensus on how to best model non-uniform air temperatures in buildings. Therefore, it is up to the user to have a good understanding of when, where, and how to apply the room air models available in EnergyPlus. The rest of this section provides some guidance in the way of examples and further discussion of the models available in EnergyPlus.
+
+EnergyPlus offers the different types of air models listed in the table below along with the input objects associated with the use of that model.
+
+% table 10
+{\scriptsize
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Summary of Room Air Models \label{table:summary-of-room-air-models}} \tabularnewline
+\toprule 
+Air Model Key & Air model Algorithm & Applicability & Input Objects Required \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Summary of Room Air Models} \tabularnewline
+\toprule 
+Air Model Key & Air model Algorithm & Applicability & Input Objects Required \tabularnewline
+\midrule
+\endhead
+
+Mixing & Well-Mixed & All zones & None, default \tabularnewline
+UserDefined & User Defined & All zones & `Room\-Air\-Model\-Type', `Room\-Air:\-Temperature\-Pattern:\-User\-Defined', `Room\-Air:\-Temperature\-Pattern:***' \tabularnewline
+One\-Node\-Displacement\-Ventilation & Mundt & displacement ventilation & `Room\-Air\-Model\-Type', `Room\-Air\-Settings:\-One\-Node\-Displacement\-Ventilation', `Room\-Air:Node' \tabularnewline
+Three\-Node\-Displacement\-Ventilation & UCSD Displacement Ventilation & displacement ventilation & `Room\-Air\-Model\-Type', `Room\-Air\-Settings:\-Three\-Node\-Displacement\-Ventilation' \tabularnewline
+Under\-Floor\-Air\-Distribution\-Interior & UCSD UFAD Interior Model & Interior zones served by a UFAD system & `Room\-Air\-Model\-Type', `Room\-Air\-Settings:\-Under\-Floor\-Air\-Distribution\-Interior' \tabularnewline
+Under\-Floor\-Air\-Distribution\-Exterior & UCSD UFAD Exterior Model & Exterior zones served by a UFAD system & `Room\-Air\-Model\-Type', `Room\-Air\-Settings:\-Under\-Floor\-Air\-Distribution\-Exterior' \tabularnewline
+Cross\-Ventilation & UCSD Cross Ventilation & cross ventilation & `Room\-Air\-Model\-Type', `Room\-Air\-Settings:\-Cross\-Ventilation' \tabularnewline
+\bottomrule
+\end{longtable}
+}
+
+\subsection{RoomAirModelType}\label{roomairmodeltype}
+
+EnergyPlus uses the Room\-Air\-Model\-Type object to determine which air model is available for use in a given zone during the simulation. If no Room\-Air\-Model\-Type object is specified (for each zone or the whole building), then EnergyPlus will run with the conventional, completely mixing air model (for each zone or the whole building). Include a Room\-Air\-Model\-Type for each zone that the user wants modeled using a more detailed method. Currently only a single Room\-Air\-Model\-Type object can be specified for each zone; you cannot switch between models during a simulation. However, the UCSD Displacement, Cross Ventilation and UFAD models switch from displacement to mixing ventilation when the operating conditions do not give rise to unmixed flow. The following parameters are fields required by the Room\-Air\-Model\-Type object.
+
+\subsubsection{Inputs}\label{inputs-041}
+
+\paragraph{Field: Name}\label{field-name-040}
+
+This alpha field is the air model name selected by user. It is used as an identifier
+
+\paragraph{Field: Zone Name}\label{field-zone-name-011}
+
+This alpha field indicates the unique name of a Zone object defined elsewhere in the input file. The type of room air model selected will be applied to this zone.
+
+\paragraph{Field: Room-Air Modeling Type}\label{field-room-air-modeling-type}
+
+This alpha field indicates the room-air model used for the specified zone. Currently, there are three options for different air models. Entering the keyword `Mixing' specifies the conventional complete-mixing air model. Note that Mixing is the default and no Room\-Air\-Model\-Type object would be needed to use the complete-mixing model. Entering the keyword `UserDefined `specifies the User Defined Room Air Temperature Patterns. Entering the keyword `OneNodeDisplacementVentilation `specifies the Mundt one node displacement ventilation air model for displacement ventilation. Entering the keyword `ThreeNodeDisplacementVentilation` specifies the three-node displacement ventilation model developed by the University of California, San Diego (UCSD DV). Entering the keyword `CrossVentilation' specifies the two-zone cross ventilation model developed by the University of California, San Diego (UCSD CV). Entering the keyword `UnderFloorAirDistributionInterior` specifies the two-node interior zone under floor air distribution model developed by the University of California, San Diego (UCSD UFI). Entering the keyword `UnderFloorAirDistributionExterior` specifies the two-node exterior zone under floor air distribution model developed by the University of California, San Diego (UCSD UFE).
+
+\paragraph{Field: Air Temperature Coupling Strategy}\label{field-air-temperature-coupling-strategy}
+
+This alpha field indicates how air temperatures predicted by the air models are used by the surface heat balance calculation. Two different coupling schemes are available: Direct (also known as \emph{T-couple}) or Indirect (\emph{DT-couple}). In general, indirect coupling is more suited to situations where room air is well controlled and/or the room air model is less robust. Direct coupling is more suited for floating zone air temperatures and/or accurate room air models.
+
+The Mundt model can use either coupling scheme; the UCSD DV, UCSD CV, UCSD UFI, and UCSD UFE models ignore this field and use direct coupling.
+
+Input either \emph{Direct} or \emph{Indirect}
+
+An example idf entry follows
+
+\begin{lstlisting}
+RoomAirModelType,
+  MOD1,                             !- Room-Air Model Name
+  ZONE ONE,                         !- Zone Name
+  ThreeNodeDisplacementVentilation, !- Room-Air Modeling Type
+  Direct;                           !- Air Temperature Coupling Strategy
+\end{lstlisting}
+
+\subsection{RoomAir:TemperaturePattern:UserDefined}\label{roomairtemperaturepatternuserdefined}
+
+This object is used to explicitly define temperature patterns that are to be applied to the mean air temperature within a thermal zone. This Room Air modeling option is made available for a number of reasons. It allows modeling the consequences of air temperature variations during the design phase when little information is available about the specifics of the air distribution system or positioning of various loads. This option can be used to evaluate the energy implications of different design targets for the temperature patterns. It also provides a method of modeling the annual energy use implications for air temperature distributions determined using separate analyses or measurements. For example, this option could be used to understand the annual energy implications of an air distribution system that has been previously analyzed using Computational Fluid Dynamics.
+
+This approach differs from the other Room Air modeling in that the static temperature pattern is not really \emph{modeled} so that it will respond to conditions that develop during the simulation. More sophisticated dynamic Room Air models will adjust the temperature pattern based on various factors, such as air system flow rate, floor temperature, or rates of internal heat gains. The user-defined temperature distribution patterns are fixed at the beginning and EnergyPlus simply provides results that include the implications of those patterns. This user-defined distribution option may also be useful for checking dynamic Room Air models by using ``bounding'' analysis.
+
+Note that using this object carries a certain degree of responsibility. It would be very easy to define a pattern that is non-physical and will lead to erroneous results. The user-defined temperature distributions should (probably) be balanced about the mean so that basic conservation of energy laws are not violated.
+
+\subsubsection{Inputs}\label{inputs-1-038}
+
+\paragraph{Field: Name}\label{field-name-1-037}
+
+This field provides a unique name for this object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-008}
+
+This field provides the unique name of a zone described elsewhere in the file.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-015}
+
+This field provides the name of a schedule that will determine if this model is available. When not available the room air is modeled as completely mixed. When it is available, then a user-defined temperature distribution will be applied. This schedule should be set to ``1.0'' when model is available and ``0.0'' when the model is not to be used. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Pattern Control Schedule Name}\label{field-pattern-control-schedule-name}
+
+This field provides the name of schedule that will be used to control which user-defined RoomAir temperature pattern will be applied at any given time. This schedule needs to have integer values that are closely coordinated with those defined as the second field in one of the RoomAir:TemperaturePattern:* objects described below. These schedule values provide the link to the actual patterns to be used throughout the day. This allows controlling which user-defined pattern is used at different times during the simulation. For example, one could use one pattern when the air system is scheduled to be on, and a different pattern when the air system is schedule to be off. Or if the user has knowledge of how the air temperature pattern changes over the course of day in response to changing thermal loads, then this schedule can be used to control when individual patterns are used. For example, a control schedule could use a pattern designated as number 100 from 18:00 to 6:00, pattern number 200 from 6:00 to 12:00, and pattern number 300 from 12:00 to 18:00.
+
+An example of this object is
+
+\begin{lstlisting}
+RoomAir:TemperaturePattern:UserDefined,
+  Ground Floor South Air Temp Contrls,  ! Name
+  ZN2_S_1,                              ! Zone Name
+  Always_on,                            ! Availability Schedule Name
+  Roomair Pattern 1;                    ! Pattern Control Schedule Name
+\end{lstlisting}
+
+\subsection{RoomAir:TemperaturePattern:ConstantGradient}\label{roomairtemperaturepatternconstantgradient}
+
+This object is used to model room air with a fixed temperature gradient in the vertical direction. This fixed-slope method is about the simplest distribution pattern.
+
+In addition to the vertical temperature gradient, there are three other parameters included in the pattern that are important. The first two might affect how the air system conditioning the room is operated. The first describes the temperature difference between the mean air temperature and the point where the sensor of a drybulb thermostat is situated. The second describes the temperature difference between the mean and the point where system air is being extracted from the zone. This is considered important because the changes in temperature difference between supply and return can affect how an air system is controlled to meet the loads. The third parameter can affect the zone air heat balance by altering the temperature of the air leaving the zone through exhaust fans.
+
+One example of a source of input data for the vertical temperature gradient is ANSI/ASHRAE Standard 55-2004 Thermal Environmental Conditions for Human Occupancy. Table 5.2.4.3 in this Standard specifies an allowable vertical temperature difference between head level and ankle level of 3ºC (5ºF). If we assume a head to ankle length scale of 1.5 m (5 ft), this leads to a temperature gradient of 3ºC/1.5m, or 2.0 ºC/m.
+
+\subsubsection{Inputs}\label{inputs-2-035}
+
+\paragraph{Field: Name}\label{field-name-2-033}
+
+This field provides a unique name for this object.
+
+\paragraph{Field: Control Integer for Pattern Control Schedule Name}\label{field-control-integer-for-pattern-control-schedule-name}
+
+This field should contain an integer value that is unique among all other RoomAir:TemperaturePattern:* objects. The value used here needs to be in the Pattern Control Schedule for those times when this pattern is to be used for the Room Air Temperature Distribution.
+
+\paragraph{Field: Thermostat Offset}\label{field-thermostat-offset}
+
+This field specifies the temperature difference between where the thermostat is situated and the mean air temperature.
+
+\paragraph{Field: Return Air Offset}\label{field-return-air-offset}
+
+This field specifies the temperature difference between the air leaving the zone and returning to the air system and the mean air temperature.
+
+\paragraph{Field: Exhaust Air Offset}\label{field-exhaust-air-offset}
+
+This field specifies the temperature difference between the air leaving the zone and being exhausted out of the building and the mean air temperature.
+
+\paragraph{Field: Temperature Gradient}\label{field-temperature-gradient}
+
+This field specifies the gradient, or slope, of temperature changes in the vertical direction in ºK/m.
+
+An example of this object is:
+
+\begin{lstlisting}
+RoomAir:TemperaturePattern:ConstantGradient,
+  half C per Meter,     ! Name
+  10005,                ! Control Integer for Pattern Control Schedule Name
+  0.0,                  ! Thermostat Offset (Temp at thermostat- Mean Air Temp) [C]
+  1.0,                  ! Return Air Offset (Tleaving - Mean Air Temp )  [C]
+  1.0,                  ! Exhaust Air Offset (Texhaust - Mean Air Temp)  [C]
+  0.5;                  ! Temperature Gradient [K/m]
+\end{lstlisting}
+
+\subsection{RoomAir:TemperaturePattern:TwoGradient}\label{roomairtemperaturepatterntwogradient}
+
+This object provides various controls over the value of the gradient used for determining the pattern of room air temperatures. It is similar to previous object RoomAir:TemperaturePattern:ConstantGradient object but simplifies the potentially arduous task of preparing and scheduling a large number of those objects. With this object, two different gradients are entered and user is given several options for controlling how the program will interpolate between the two bounds. The user inputs the height of the location of thermostat, return air, and exhaust air in meters rather than the temperature offset.
+
+\subsubsection{Inputs}\label{inputs-3-031}
+
+\paragraph{Field: Name}\label{field-name-3-027}
+
+This field provides a unique name for this object.
+
+\paragraph{Field: Control Integer for Pattern Control Schedule Name}\label{field-control-integer-for-pattern-control-schedule-name-1}
+
+This field should contain an integer value that is unique among all other RoomAir:TemperaturePattern:* objects. The value used here needs to be in the Pattern Control Schedule for those times when this pattern is to be used for the Room Air Temperature Distribution.
+
+\paragraph{Field: Thermostat Height}\label{field-thermostat-height}
+
+This field specifies the distance above the floor where the thermostat is situated. This height is used by the model to determine the thermostat temperature relative to the mean air temperature by applying the gradient.
+
+\paragraph{Field: Return Air Height}\label{field-return-air-height}
+
+This field specifies the distance above the floor where the air leaves the zone and returns to the air system. and the mean air temperature. This height is used by the model to determine the return air temperature relative to the mean air temperature by applying the gradient.
+
+\paragraph{Field: Exhaust Air Height}\label{field-exhaust-air-height}
+
+This field specifies the distance above the floor where the air leaves the zone and enters and exhaust device such as an exhaust fan. This height is used by the model to determine the exhaust air temperature relative to the mean air temperature by applying the gradient.
+
+\paragraph{Field: Temperature Gradient Lower Bound}\label{field-temperature-gradient-lower-bound}
+
+This field specifies the gradient, or slope, of temperature changes in the vertical direction in ºC/m.
+
+\paragraph{Field: Temperature Gradient Upper Bound}\label{field-temperature-gradient-upper-bound}
+
+This field specifies the gradient, or slope, of temperature changes in the vertical direction in ºC/m.
+
+\paragraph{Field: Gradient Interpolation Mode}\label{field-gradient-interpolation-mode}
+
+This field specifics how the program will vary between the two gradients. Select one of the following keywords to choose the simulation data used to scale: `Outdoor Environment Drybulb Temperature', `Zone Drybulb Temperature', `Delta Outdoor and Zone Temperature', `Sensible Cooling Load', and `Sensible Heating Load'. These are explained in detail below. All of these options have several things in common. They are essentially hard-coded. There is no support for a general method. The interpolation scheme is based on some variable that might reasonably be expected to correlate with gradient changes. This variable's current value is used to continually adjust the value of the vertical gradient for room air temperature.
+
+\textbf{OutdoorDryBulbTemperature:} This key directs the program to interpolate between upper and lower values of the vertical gradient based on the outdoor air temperature. If the outdoor temperature exceeds the upper limit set in the next field, then the gradient entered in the `Temperature Gradient Upper Bound' field is used. Similarly if the outdoor air temperature is below the value set in the `Lower Temperature' field, then the gradient entered in the `Temperature Gradient Lower Bound' is used. For outdoor temperatures that lie between the upper and lower bounds, the gradient is determined by linear interpolation between the two.
+
+\textbf{ZoneDryBulbTemperature}: This key directs the program to interpolate between upper and lower values of the vertical gradient based on the mean zone air temperature. If the mean zone air temperature exceeds the upper limit set in the next field, then the gradient entered in the `Temperature Gradient Upper Bound' field is used. Similarly if the mean zone air temperature is below the value set in the `Lower Temperature' field, then the gradient entered in the `Temperature Gradient Lower Bound' is used. For mean zone air temperatures that lie between the upper and lower bounds, the gradient is determined by linear interpolation between the two.
+
+\textbf{ZoneAndOutdoorTemperatureDifference}: This key directs the program to interpolate between upper and lower values of the vertical gradient based on the difference between the outdoor environment and the mean zone air temperature. If the temperature difference exceeds the upper limit set in the next field, then the gradient entered in the `Temperature Gradient Upper Bound' field is used. Similarly if the temperature difference is below the value set in the `Lower Temperature' field, then the gradient entered in the `Temperature Gradient Lower Bound' is used. For temperature differences that lie between the upper and lower bounds, the gradient is determined by linear interpolation between the two.
+
+\textbf{SensibleCoolingLoad}: This key directs the program to interpolate between upper and lower values of the vertical gradient based on the sensible cooling load. If the cooling load exceeds the upper limit set in the next field, then the gradient entered in the `Temperature Gradient Upper Bound' field is used. Similarly if the cooling load is below the value set in the `Lower Temperature' field, then the gradient entered in the `Temperature Gradient Lower Bound' is used. For cooling loads that lie between the upper and lower bounds, the gradient is determined by linear interpolation between the two.
+
+\textbf{SensibleHeatingLoad}: This key directs the program to interpolate between upper and lower values of the vertical gradient based on the sensible heating load. If the heating load exceeds the upper limit set in the next field, then the gradient entered in the `Temperature Gradient Upper Bound' field is used. Similarly if the heating load is below the value set in the `Lower Temperature' field, then the gradient entered in the `Temperature Gradient Lower Bound' is used. For heating loads that lie between the upper and lower bounds, the gradient is determined by linear interpolation between the two.
+
+\paragraph{Field: Upper Temperature Bound}\label{field-upper-temperature-bound}
+
+This field is used to enter the upper bound on temperature values in Celsius. It is required for the interpolation modes based on temperature.
+
+\paragraph{Field: Lower Temperature Bound}\label{field-lower-temperature-bound}
+
+This field is used to enter the lower bound on temperature values in Celsius. It is required for the interpolation modes based on temperature.
+
+\paragraph{Field: Upper Heat Rate Bound}\label{field-upper-heat-rate-bound}
+
+This field is used to enter the upper bound on heat rate values. It is required for the interpolation modes based on load. Both heating and cooling loads are entered as positive numbers (in watts).
+
+\paragraph{Field: Lower Heat Rate Bound}\label{field-lower-heat-rate-bound}
+
+This field is used to enter the lower bound on heat rate values. It is required for the interpolation modes based on load. Both heating and cooling loads are entered as positive numbers (in watts).
+
+An example of this object follows. This pattern will apply no gradient (effectively the mixing model) if zone air temperatures are 22.5 C or lower. It will apply a gradient of 1 K/m if zone temperatures are 26.0 C or higher. For zone air temperatures between 22.5 and 26.0 it will determine the gradient by linear interpolation and use a gradient between 0.0 and 1.0 K/m depending on where the zone air temperature is in the range.
+
+\begin{lstlisting}
+RoomAir:TemperaturePattern:TwoGradient,
+  Mixed to one C per M by Zone DB, ! Name
+  2002,                   ! Control Integer for Pattern Control Schedule
+  1.1,                    ! Thermostat Height meters
+  4.5,                    ! Return Air Height
+  3.5,                    ! Exhaust Air Height
+  0.0,                    ! Temperature Gradient Lower Bound K/m
+  1.0,                    ! Temperature Gradient Upper  Bound K/m
+  ZoneDrybulbTemperature, ! Gradient Interpolation Mode
+  26.0,                   ! Upper Temperature [C]
+  22.5,                   ! Lower Temperature [C]
+  ,                       ! Upper Heat Rate [W]
+  ;                       ! Lower Heat Rate [W]
+\end{lstlisting}
+
+\subsection{RoomAir:TemperaturePattern:NondimensionalHeight}\label{roomairtemperaturepatternnondimensionalheight}
+
+This object defines a distribution pattern for air temperatures relative to the current mean air temperature as a function of height. The height, referred to as Zeta, is non-dimensional by normalizing with the zone ceiling height. (The actual zone ceiling height can be explicitly entered in the `Zone' object but if not it is calculated by EnergyPlus from the surfaces attached to the zone.) The temperature differences are not non-dimensional and remain in units of degrees Celsius.
+
+An example of a vertical temperature pattern is shown in the figure below. The pattern itself is treated as a piecewise, linear model of air temperature as a function of height. This Zeta-DeltaTai curve, or lookup table, is then mapped to surfaces defined elsewhere in the file. The centroid of each surface and zone ceiling height are used to automatically assign Zeta values within the program. The zone named in the referencing RoomAir:TemperaturePattern:UserDefined object is used to determine which surfaces will be associated with the pattern when it is applied. A single pattern object can be reused for multiple zones and times.
+
+In addition to the vertical temperature pattern there are three other parameters included in the pattern that are important. The first two might affect how the air system conditioning the room is operated. The first describes the temperature difference between the mean air temperature and the point where the sensor of a drybulb thermostat is situated. The second describes the temperature difference between the mean and the point where system air is being extracted from the zone. This is considered important because the changes in temperature difference between supply and return can affect how an air system is controlled to meet the loads. The third parameter can affect the zone air heat balance by altering the temperature of the air leaving the zone through exhaust fans.
+
+\begin{figure}[hbtp] % fig 44
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image079.png}
+\caption{Example of a Vertical Air Temperature Pattern \protect \label{fig:example-of-a-vertical-air-temperature-pattern}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-4-028}
+
+\paragraph{Field: Name}\label{field-name-4-024}
+
+This field provides a unique name for this object.
+
+\paragraph{Field: Control Integer for Pattern Control Schedule Name}\label{field-control-integer-for-pattern-control-schedule-name-2}
+
+This field should contain an integer value that is unique among all other RoomAir Temperature Pattern objects. The value used here needs to be in the Pattern Control Schedule for those times when this pattern is to be used for the Room Air Temperature Distribution.
+
+\paragraph{Field: Thermostat Offset}\label{field-thermostat-offset-1}
+
+This field specifies the temperature difference between where the thermostat is situated and the mean air temperature.
+
+\paragraph{Field: Return Air Offset}\label{field-return-air-offset-1}
+
+This field specifies the temperature difference between the air leaving the zone and returning to the air system and the mean air temperature.
+
+\paragraph{Field: Exhaust Air Offset}\label{field-exhaust-air-offset-1}
+
+This field specifies the temperature difference between the air leaving the zone and being exhausted out of the building and the mean air temperature.
+
+\paragraph{Field Set Zeta and Temperature Difference}\label{field-set-zeta-and-temperature-difference}
+
+The remaining fields contain pairs of values that define a lookup table for the temperature pattern in the vertical direction. The first value is Zeta and the second value is DeltaTai. This object is extensible, by duplicating the last two fields and revising the IDD -- note that you will have to replace ``inner'' semi-colons with commas.
+
+\paragraph{Field: Pair \textless{}\#\textgreater{} Zeta non-dimensional Height}\label{field-pair-zeta-non-dimensional-height}
+
+Zeta is the normalized height and should be a fractional value from 0.0 to 1.0. A value of 0.0 corresponds to the floor and a value of 1.0 corresponds to the ceiling. The Zeta values need to be in increasing value.
+
+\paragraph{Field: Pair \textless{}\#\textgreater{} Delta Adjacent Air Temperature}\label{field-pair-delta-adjacent-air-temperature}
+
+DeltaT\(_{ai}\) is the temperature difference between the air temperature at the associated Zeta (T\(_{ai}\)) and the mean air temperature and is given in degrees Celsius.
+
+An example of this object corresponding to the figure above is:
+
+\begin{lstlisting}
+RoomAir:TemperaturePattern:NondimensionalHeight,
+  Rough UFAD Approx,    ! Name
+  3001,                 ! Control Integer for Pattern Control Schedule
+                        ! note reference this entry in Schedule
+  -1.0 ,                ! Thermostat Offset
+  1.5 ,                 ! Return Air Offset (Tleaving - Mean Air Temp ) deg C
+  1.75,                 ! Exhaust Air Offset (Texhaust - Mean Air Temp) deg C
+  0.05,  -1.8,          ! pair 1 (Zeta , DeltaTai)
+  0.1,   -1.7,          ! pair 2 (Zeta , DeltaTai)
+  0.2,   -0.8,          ! pair 3 (Zeta , DeltaTai)
+  0.3,   -0.2,          ! pair 4 (Zeta , DeltaTai)
+  0.4,    0.5,          ! pair 5 (Zeta , DeltaTai)
+  0.5,    0.8,          ! pair 6 (Zeta , DeltaTai)
+  0.6,    1.2,          ! pair 7 (Zeta , DeltaTai)
+  0.7,    1.4,          ! pair 8 (Zeta , DeltaTai)
+  0.8,    1.4,          ! pair 9 (Zeta , DeltaTai)
+  0.9,   1.42,          ! pair 10 (Zeta , DeltaTai)
+  0.95,  1.44;          ! pair 11 (Zeta , DeltaTai)
+\end{lstlisting}
+
+\subsection{RoomAir:TemperaturePattern:SurfaceMapping}\label{roomairtemperaturepatternsurfacemapping}
+
+This object defines a distribution pattern for the air temperatures adjacent to individual surfaces. This object uses the specific names of individual surfaces defined elsewhere in the model. This pattern allows controlling the adjacent air temperature on a surface-by-surface basis rather than by height. This allows modeling different adjacent air temperatures on the opposite sides of the zone.
+
+In addition to the surface mappings there are three other parameters included in the pattern that are important. The first two might affect how the air system conditioning the room is operated. The first describes the temperature difference between the mean air temperature and the point where the sensor of a drybulb thermostat is situated. The second describes the temperature difference between the mean and the point where system air is being extracted from the zone. This is considered important because the changes in temperature difference between supply and return can affect how an air system is controlled to meet the loads. The third parameter can affect the zone air heat balance by altering the temperature of the air leaving the zone through exhaust fans.
+
+\subsubsection{Inputs}\label{inputs-5-025}
+
+\paragraph{Field: Name}\label{field-name-5-020}
+
+This field provides a unique name for this object.
+
+\paragraph{Field: Control Integer for Pattern Control Schedule Name}\label{field-control-integer-for-pattern-control-schedule-name-3}
+
+This field should contain an integer value that is unique among all other RoomAir Temperature Pattern objects. The value used here needs to be in the Pattern Control Schedule for those times when this pattern is to be used for the RoomAir Temperature Distribution.
+
+\paragraph{Field: Thermostat Offset}\label{field-thermostat-offset-2}
+
+This field specifies the temperature difference between where the thermostat is situated and the mean air temperature.
+
+\paragraph{Field: Return Air Offset}\label{field-return-air-offset-2}
+
+This field specifies the temperature difference between the air leaving the zone and returning to the air system and the mean air temperature.
+
+\paragraph{Field: Exhaust Air Offset}\label{field-exhaust-air-offset-2}
+
+This field specifies the temperature difference between the air leaving the zone and being exhausted out of the building and the mean air temperature.
+
+\paragraph{Field Set: Surface Name, Temperature Difference}\label{field-set-surface-name-temperature-difference}
+
+\paragraph{Fields (6 and on): Pairs of Surface Names and Temperature Differences}\label{fields-6-and-on-pairs-of-surface-names-and-temperature-differences}
+
+The remaining fields contain pairs that define a lookup table for the temperature pattern on a surface-by-surface basis. This object is extensible, by duplicating the last two fields and revising the IDD -- note that you will have to replace ``inner'' semi-colons with commas.
+
+\paragraph{Field: Surface Name Pair \textless{}\#\textgreater{}}\label{field-surface-name-pair}
+
+The name of a surface defined elsewhere in the input file.
+
+\paragraph{Field: Delta Adjacent Air Temperature Pair \textless{}\#\textgreater{}}\label{field-delta-adjacent-air-temperature-pair}
+
+DeltaT\(_{ai}\) is the temperature difference between the air temperature adjacent to the associated surface (T\(_{ai}\)) and the mean air temperature and is given in degrees Celsius.
+
+An example of this object, which might be used to elevate temperatures near west windows in the afternoon, is:
+
+\begin{lstlisting}
+
+RoomAir:TemperaturePattern:SurfaceMapping,
+    GroundFloor SW Corner Hot Near West Wall, ! Name
+    4001, ! Control Integer for Pattern Control Schedule Name
+    0.0, ! Thermostat Offset(Temp at thermostat- Mean Air Temp)
+    0.0, ! Return Air Offset  deg C
+    0.0, ! Exhaust Air Offset
+    ZN1_SW_1:W_ExtWall:1 ,  0.8,  ! pair 1 (Surface Name , DeltaTai)
+    ZN1_SW_1:W_ExtWall:2 ,  0.9,  ! pair 2 (Surface Name , DeltaTai)
+    ZN1_SW_1:W_ExtWall:3 ,  1.0,  ! pair 3 (Surface Name , DeltaTai)
+    ZN1_SW_1:W_ExtWall:4,   1.1,  ! pair 4 (Surface Name , DeltaTai)
+    ZN1_SW_1:W_ExtWall:5,   1.3,  ! pair 5 (Surface Name , DeltaTai)
+    ZN1_SW_1:W_ExtWall:6,   1.5,  ! pair 6 (Surface Name , DeltaTai)
+    ZN1_SW_1:W_ExtWall:7,   1.7,  ! pair 7 (Surface Name , DeltaTai)
+    ZN1_SW_1:W_ExtWall:8,   2.1,  ! pair 8 (Surface Name , DeltaTai)
+    ZN1_SW_1:W_ExtWall:9,   2.4 ; ! pair 8 (Surface Name , DeltaTai)
+\end{lstlisting}
+
+\subsection{RoomAir:Node}\label{roomairnode}
+
+The RoomAir:Node object is used to define air nodes for a nodal air model. The number of air node objects that need to be specified depends on the nodal air model selected. (However, currently only the Mundt model uses this object). In order to use the Mundt model, the user must specify six or more RoomAir:Node objects of different types for each zone. The exact number of RoomAir:Node in the model will vary based on the resolution of walls. If walls (heat transfer surfaces) are split into separate segments in the vertical direction, then more air nodes of type `MundtRoom' will be useful. At a minimum, for the Mundt model RoomAir Nodes of the following type are required: `Inlet, `Floor, `Control, `Ceiling, `MundtRoom, and `Return.'
+
+\subsubsection{Inputs}\label{inputs-6-022}
+
+\paragraph{Field: Name}\label{field-name-6-018}
+
+This alpha field is a name for the air node. It should be unique and is used as an identifier
+
+\paragraph{Field: Node Type}\label{field-node-type}
+
+This alpha field indicates the type of this air node. The following explains options available for use with the Mundt nodal air model.
+
+\textbf{Inlet} is specified for the air node located where the system air enters the zone.
+
+\textbf{Floor} is specified for the air node located near the floor.
+
+\textbf{Control} is specified for the air node located near the thermostat.
+
+\textbf{Ceiling} is specified for the air node located near the ceiling.
+
+\textbf{MundtRoom} is specified for the air node located adjacent to the wall(s).
+
+\textbf{Return} is specified for the air node located where the system air leaves the zone.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-2-006}
+
+This field indicates the name of the zone (Ref: Zone) that this air node belongs to. This should be the unique name of a zone object defined elsewhere in the input file.
+
+\paragraph{Field: Height of Nodal Control Volume Center}\label{field-height-of-nodal-control-volume-center}
+
+This numeric field indicates the height of the air node center. Air models such as the Mundt model compute the air temperature as a function of height and the value entered here will be used to determine a result for this node. The value should be specified in meters and relative to the floor of the zone.
+
+\paragraph{Field: Surface \textless{}\#\textgreater{} Name}\label{field-surface-name-004}
+
+These remaining alpha fields indicate the names of the surfaces (Ref: Surface) that are interacting convectively with this air node. This field is optional and related to the previous field. Currently, at most 20 surfaces are allowed to interact with a single air node. Only those nodes that interact with the inside faces of surfaces need to specify surface names. Each surface should couple to no more than 1 node.
+
+An IDF example:
+
+\begin{lstlisting}
+
+RoomAir:Node,
+      WESTZN:FLOORAIR,    !- Node Name
+      Floor,      !- Node Type
+      WEST ZONE,  !- Name of Zone to Which the Air Node Belongs
+      0.1,        !- Height of Nodal Control Volume Center {m}
+      WESTZN:FLOOR:LEFF,  !- surface name
+      WESTZN:FLOOR:RIGHT; !- surface name
+\end{lstlisting}
+
+\subsection{RoomAirSettings:OneNodeDisplacementVentilation}\label{roomairsettingsonenodedisplacementventilation}
+
+The RoomAirSettings:OneNodeDisplacementVentilation object is used to specify additional input parameters required by the Mundt model that are not available in other input objects in EnergyPlus. A single object will be used for the zone.
+
+\subsubsection{Inputs}\label{inputs-7-022}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-3-005}
+
+This alpha field indicates the name of the zone (Ref: Zone) for the required input parameters as specified in the following fields.
+
+\paragraph{Field: Fraction of Convective Internal Loads Added to Floor Air}\label{field-fraction-of-convective-internal-loads-added-to-floor-air}
+
+This numeric field indicates what fraction of the convective part of the internal gains is added to the air near the floor in the zone specified.
+
+\paragraph{Field: Fraction of Infiltration Internal Loads Added to Floor Air}\label{field-fraction-of-infiltration-internal-loads-added-to-floor-air}
+
+This numeric field indicates what fraction of the infiltration air enters near the floor in the zone specified.
+
+An IDF example:
+
+\begin{lstlisting}
+
+RoomAirSettings:OneNodeDisplacementVentilation,
+      WEST ZONE,  !- Zone Name
+      0.1,  !- Fraction of internal loads from the convective Floor Air
+      0.1;  !- Fraction of internal loads from the Infiltration Air
+\end{lstlisting}
+
+\subsection{RoomAirSettings:ThreeNodeDisplacementVentilation}\label{roomairsettingsthreenodedisplacementventilation}
+
+This model is applicable to spaces that are served by a low velocity floor-level displacement ventilation air distribution system. Furthermore, the dominant sources of heat gain should be from people and other localized sources located in the occupied part of the room. The model should be used with caution in zones which have large heat gains or losses through exterior walls or windows or which have considerable direct solar gain. The model predicts three temperatures in the room:
+
+\begin{itemize}
+\item
+  A foot level temperature (T\(_{\rm{FLOOR}}\)). The floor region is 0.2 meters deep and T\(_{\rm{FLOOR}}\) represents the temperature at the mid-point of the region.
+\item
+  An occupied subzone temperature (T\(_{\rm{OC}}\)), representing the temperature in the region between the floor layer and the upper, mixed layer.
+\item
+  An upper node representing the mixed-layer/outflow temperature (T\(_{\rm{MX}}\)) essential for overall energy budget calculations and for modeling comfort effects of the upper layer temperature.
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 45
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image080.png}
+\caption{Schematic representation of the three temperature points and temperature gradients \protect \label{fig:schematic-representation-of-the-three}}
+\end{figure}
+
+The following fields are used to define an instance of the `UCSD Displacement Ventilation Model Controls' object.
+
+\subsubsection{Inputs}\label{inputs-8-020}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-4-005}
+
+This field provides the unique name of a zone described elsewhere in the file. A single instance of the `UCSD Displacement Ventilation Model Controls' object is needed for each zone that is to be modeled using this method.
+
+\paragraph{Field: Gain Distribution Schedule Name}\label{field-gain-distribution-schedule-name}
+
+This field specifies the unique name of schedule defined elsewhere in the input file. The schedule values are the fractions of the convective portion of the internal gains in the occupied subzone that remain in the occupied subzone. The remainder of the convective portion of the internal gains in the occupied subzone enters the plumes and is carried to the upper subzone. The types of internal gains that are assumed to be located in the occupied subzone are:
+
+\begin{itemize}
+\item
+  people
+\item
+  task lights
+\item
+  electric equipment
+\item
+  gas equipment
+\item
+  hot water equipment
+\item
+  steam equipment
+\item
+  other equipment
+\item
+  baseboard heat
+\end{itemize}
+
+Types of internal gains that are assumed to be in the upper subzone are:
+
+\begin{itemize}
+\item
+  general lights
+\item
+  tubular daylighting devices
+\item
+  high temperature radiant heaters
+\end{itemize}
+
+The schedule values should be between 0 and 1. A value of 1 means that all the convection gains from equipment, task lights and people are dispersed in the lower occupied subzone. Conversely a value of 0 puts all the lower subzone convective gains into the plumes rising into the upper well-mixed subzone.
+
+\paragraph{Field: Number of Plumes per Occupant}\label{field-number-of-plumes-per-occupant}
+
+This field specifies number of plumes per occupant. Plumes are associated with localized sources of convective heat gain from people and equipment. For example, a value of 2.0 would be used if each occupant has a computer that generates a separate plume that does not merge with the plume from the occupant in the lower, occupied, subzone.
+
+\paragraph{Field: Thermostat Height}\label{field-thermostat-height-1}
+
+This field is the height in meters of the thermostat/temperature control sensor above the floor.
+
+\paragraph{Field: Comfort Height}\label{field-comfort-height}
+
+The height in meters above the floor at which air temperature is calculated for comfort purposes. The air temperature at this height is used in calculating the available measures of comfort: Fanger, Pierce or KSU. The default is 1.1 meters.
+
+\paragraph{Field: Temperature Difference Threshold for Reporting}\label{field-temperature-difference-threshold-for-reporting}
+
+This field specifies a minimum temperature difference between the upper mixed subzone and the occupied subzone that will be used to trigger whether or not the displacement ventilation auxiliary outputs will be calculated. These outputs are \emph{Room Air Zone Transition Height}, \emph{Room Air Zone Recommended Minimum Flow Fraction}, \emph{Room Air Zone Average Temperature Gradient} and \emph{Room Air Zone Maximum Temperature Gradient}. They are set to negative values when the temperature difference is less than the threshold and the output \emph{Room Air Zone Is Mixed Status} is set to 1.
+
+The value should be greater than or equal to zero and is in units of degrees Centigrade. The default value is 0.4 degrees C.
+
+An example input:
+
+\begin{lstlisting}
+
+RoomAirSettings:ThreeNodeDisplacementVentilation,
+      ZONE ONE,  !- Zone Name
+      Constant - .2,  !- Gain Distribution Schedule Name
+       1,  !- Number of Plumes per Occupant
+        ,  !- Thermostat Height
+        ,  !- Comfort Height
+      .3;  !- Temp. Difference Threshold for Displacement Ventilation
+\end{lstlisting}
+
+\subsection{RoomAirSettings:CrossVentilation}\label{roomairsettingscrossventilation}
+
+The UCSD Cross Ventilation Room Air Model provides a simple model for heat transfer and temperature prediction in cross ventilated rooms. Cross Ventilation (CV) is common in many naturally ventilated buildings, with air flowing through windows, open doorways and large internal apertures across rooms and corridors in the building.
+
+The CV model is used in EnergyPlus in the context of natural ventilation simulations using the AirflowNetwork airflow prediction model. Typical CV room flows are characterized by two clearly distinguishable flow regions that have different airflow velocities and temperature:
+
+\begin{itemize}
+\item
+  Jet regions in front of the inflow windows
+\item
+  Recirculation regions in the portions of the room that are not directly in front of the windows.
+\end{itemize}
+
+Each inflow aperture has one jet region while the recirculation regions are treated as a whole, with a single temperature and characteristic velocity. The default EnergyPlus perfectly mixed single temperature node room air approach is not suitable for these partially mixed flows. The proposed CV model uses multiple nodes with distinct air temperature and airflow velocity (one node for the recirculations plus one additional node for each inflow aperture).
+
+\begin{figure}[hbtp] % fig 46
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image081.png}
+\caption{Schematic representation of room air geometry a) schematic representation of a room geometry that generates cross ventilation airflow. b) the proposed model distinguishes two regions in the flow: jet and recirculation (shown here in a CFD simulation of one half of a symmetrical room). \protect \label{fig:schematic-representation-of-room-air-geometry}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 47
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image082.png}
+\caption{Schematic top view --- possible airflow patterns in cross-ventilation. \protect \label{fig:schematic-top-view-possible-airflow-patterns}}
+\end{figure}
+
+The following fields are used to define an instance of the `UCSD Cross Ventilation Model Controls' object.
+
+\subsubsection{Inputs}\label{inputs-9-018}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-5-004}
+
+This field provides the name of the zone to which this object applies. A single instance of the `UCSD Cross Ventilation Model Controls' object is needed for each zone modeled using this method.
+
+\paragraph{Field: Gain Distribution Schedule Name}\label{field-gain-distribution-schedule-name-1}
+
+This field specifies the unique name of schedule defined elsewhere in the input file. The schedule values define the fractions of the convective portion of the internal gains in the jet and recirculation regions.
+
+The schedule values should be between 0 and 1. A value of 1 means that all the convective gains are dispersed in the jet region. Conversely a value of 0 puts all the convective gains into the recirculation region.
+
+\paragraph{Field: Airflow Region Used for Thermal Comfort Evaluation}\label{field-airflow-region-used-for-thermal-comfort-evaluation}
+
+Required field whenever thermal comfort is predicted. Defines air temperature and mean airflow velocity that will be used in the Fanger model. Conditions must refer to one of the two regions defined in the model: jet or recirculation.
+
+Possible choices: Jet or Recirculation.
+
+\subsubsection{Outputs}\label{outputs-030}
+
+\begin{lstlisting}
+Zone,Average,Room Air Zone Jet Region Temperature [C]
+Zone,Average,Room Air Zone Recirculation Region Temperature [C]
+Zone,Average,Room Air Zone Jet Region Average Air Velocity [m/s]
+Zone,Average,Room Air Zone Recirculation Region Average Air Velocity [m/s]
+Zone,Average,Room Air Window Jet Region Average Air Velocity [m/s]
+Zone,Average,Room Air Zone Recirculation and Inflow Rate Ratio
+Zone,Average,Room Air Zone Inflow Opening Area [m2]
+Zone,Average,Room Air Zone Room Length [m]
+Zone,Average,Room Air Zone Is Mixing Status
+Zone,Average,Room Air Zone Is Recirculating Status
+\end{lstlisting}
+
+\paragraph{Room Air Zone Jet Region Temperature {[}C{]}}\label{room-air-zone-jet-region-temperature-c}
+
+Average air temperature in the jet region of the flow in degrees C. If there is more than one inflow window this output will be the inflow-area-weighted average of the jet region temperature.
+
+\paragraph{Room Air Zone Recirculation Region Temperature {[}C{]}}\label{room-air-zone-recirculation-region-temperature-c}
+
+Average air temperature in the recirculation region of the flow in degrees C.
+
+\paragraph{Room Air Zone Jet Region Average Air Velocity {[}m/s{]}}\label{room-air-zone-jet-region-average-air-velocity-ms}
+
+Average airflow velocity in the jet region of the flow in meters per second. If there is more than one inflow window this output will be the inflow area weighted area of the jet inflow velocities.
+
+\paragraph{Room Air Window Jet Region Average Air Velocity {[}m/s{]}}\label{room-air-window-jet-region-average-air-velocity-ms}
+
+Average airflow velocity in the jet region in front of the window, in meters per second.
+
+\paragraph{Room Air Zone Recirculation Region Average Air Velocity {[}m/s{]}}\label{room-air-zone-recirculation-region-average-air-velocity-ms}
+
+Average airflow velocity in the recirculation region of the flow in meters per second.
+
+\paragraph{\texorpdfstring{Room Air Zone Recirculation and Inflow Rate Ratio {[]}}{Room Air Zone Recirculation and Inflow Rate Ratio }}\label{room-air-zone-recirculation-and-inflow-rate-ratio}
+
+Ratio between airflow rate in the recirculation regions and the total inflow rate, non-dimensional.
+
+\paragraph{Room Air Zone Inflow Opening Area {[}m2{]}}\label{room-air-zone-inflow-opening-area-m2}
+
+Area of the inflow aperture in square meters. This area can change due to variation in wind direction (as inflow aperture changes) or variations in the opening schedule.
+
+\paragraph{Room Air Zone Room Length {[}m{]}}\label{room-air-zone-room-length-m}
+
+Length of the room along the cross ventilation direction, in meters.
+
+\paragraph{\texorpdfstring{Room Air Zone Is Mixing Status {[]}}{Room Air Zone Is Mixing Status }}\label{room-air-zone-is-mixing-status}
+
+An integer flag that indicates whether the zone is mixed (single node well-mixed zone model used) or significant momentum conservation is occurring (UCSD CV model used). The value 1 means well-mixed; 0 means cross ventilation is present. Transition to mixed flow can occur due to three mechanism: reduction in inflow velocity, reduction in inflow aperture area and dominance of buoyancy effects. A value of 1 is yes, a value of 0 is no.
+
+\paragraph{\texorpdfstring{Room Air Zone Is Recirculating Status {[]}}{Room Air Zone Is Recirculating Status }}\label{room-air-zone-is-recirculating-status}
+
+An integer flag that indicates whether recirculations are present in the flow. A cross ventilation flow does not have recirculations whenever the inflow area is similar to the room cross section area (such as airflow in a typical corridor). A value of 1 is yes, a value of 0 is no.
+
+\subsection{RoomAirSettings:UnderFloorAirDistributionInterior}\label{roomairsettingsunderfloorairdistributioninterior}
+
+This model is applicable to interior spaces that are served by an underfloor air distribution system. The dominant sources of heat gain should be from people, equipment, and other localized sources located in the occupied part of the room. The model should be used with caution in zones which have large heat gains or losses through exterior walls or windows or which have considerable direct solar gain. The model predicts two temperatures in the room:
+
+\begin{itemize}
+\item
+  An occupied subzone temperature (T\(_{\rm{OC}}\)), representing the temperature in the region between the floor and the boundary of the upper subzone.
+\item
+  An upper subzone temperature (T\(_{\rm{MX}}\)) essential for overall energy budget calculations and for modeling comfort effects of the upper layer temperature.
+\end{itemize}
+
+The following fields are used to define an instance of the `UCSD UFAD Interior Model Controls' object.
+
+\subsubsection{Inputs}\label{inputs-10-017}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-6-003}
+
+This field provides the unique name of a zone described elsewhere in the file. A single instance of the `RoomAirSettings:UnderFloorAirDistributionInterior' object is needed for each zone that is to be modeled using this method.
+
+\paragraph{Field: Number of Diffusers}\label{field-number-of-diffusers}
+
+The total number of diffusers in this zone. This field can allowed to Autocalculate (in which case it is set to the design occupancy level; i.e., number of people). If the design occupancy is low or zero but there are still heat sources that could generate buoyancy driven plumes, the user should input a value based on the design supply air flow rate of the zone and the design flow rate of an individual diffuser. In the absence of any other information, divide the zone area by 100 ft\(^{2}\). The default for this field is Autocalculate.
+
+\paragraph{Field: Power per Plume}\label{field-power-per-plume}
+
+The power in watts incorporated in a buoyancy driven thermal plume. Normally we assume all the loads of a workstation create a single plume so that this represents the convective heat gain from a workstation -- 1 person, 1 computer terminal, plus any task lighting. A typical value would be 220 watts. However, the model assumes an ``equivalent'' plume derived from the zone extraction rate normalized to the number of workstations/occupants. This field should be allowed to default -- the program will calculate a value based upon the occupancy and the extraction rate. The default is Autocalculate.
+
+\paragraph{Field: Design Effective Area of Diffuser}\label{field-design-effective-area-of-diffuser}
+
+This is the design air flow opening area in square meters of a single diffuser. The default value depends on the diffuser type. For swirl diffusers it is 0075 m\(^{2}\), for variable area diffusers 0.035 m\(^{2}\), for horizontal swirl diffusers 0.006 m\(^{2}\), and for linear bar grilles 0.03 m\(^{2}\). The default is \emph{Autocalculate}..
+
+\paragraph{Field: Diffuser Slot Angle from Vertical}\label{field-diffuser-slot-angle-from-vertical}
+
+This input describes the angle at which air emerges from the diffusers. It should be the angle in degrees between the vertical and the diffuser slots. The defaults depend on the diffuser type: for swirl diffusers it is 28 degrees, for variable area diffusers 45 degrees, for DV diffusers 73 degrees, and for linear bar grilles 15 degrees.
+
+\paragraph{Field: Thermostat Height}\label{field-thermostat-height-2}
+
+This field is the height in meters of the thermostat/temperature control sensor above the floor. The default is 1.2 meters.
+
+\paragraph{Field: Comfort Height}\label{field-comfort-height-1}
+
+The height in meters above the floor at which air temperature is calculated for comfort purposes. The air temperature at this height is used in calculating the available measures of comfort: Fanger, Pierce or KSU. The default is 1.1 meters.
+
+\paragraph{Field: Temperature Difference Threshold for Reporting}\label{field-temperature-difference-threshold-for-reporting-1}
+
+This field specifies a minimum temperature difference between the upper subzone and the occupied subzone that will be used to trigger whether or not the UFAD auxiliary outputs will be calculated. These outputs are \emph{Room Air Zone Transition Height} and \emph{Room Air Zone Average Temperature Gradient}. They are set to zero when the temperature difference is less than the threshold and the output \emph{Room Air Zone Is Mixed Status} is set to 1.
+
+The value should be greater than or equal to zero and is in units of degrees Centigrade. The default value is 0.4 degrees C.
+
+\paragraph{Field: Diffuser Type}\label{field-diffuser-type}
+
+The choices for this alpha field are \textbf{Swirl} \textbar{} \textbf{VariableArea} \textbar{} \textbf{HorizontalSwirl \textbar{} LinearBarGrille \textbar{} Custom.} The swirl and displacement diffusers are fixed area diffusers. The variable area diffusers maintain an approximately constant exit velocity. Linear bar grilles are normally used in exterior zonesand are fixed area diffusers. Custom is used to signify that the user intends to input the coefficients A -- E (see below) rather than let the program set the coefficients based on diffuser type. The default is \emph{Swirl}.
+
+\paragraph{Field: Transition Height}\label{field-transition-height}
+
+An optional field to allow the user to specify the transition height (meters above floor) rather than have the program calculate it. The default is 1.7 meters.
+
+\paragraph{Field: Coefficient A}\label{field-coefficient-a}
+
+The coefficient A in the formula: Kc = A*Gamma**B + C + D*Gamma + E*Gamma**2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is \emph{autocalculate}.
+
+\paragraph{Field: Coefficient B}\label{field-coefficient-b}
+
+The coefficient B in the formula: Kc = A*Gamma**B + C + D*Gamma + E*Gamma**2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is \emph{autocalculate}.
+
+\paragraph{Field: Coefficient C}\label{field-coefficient-c}
+
+The coefficient C in the formula: Kc = A*Gamma**B + C + D*Gamma + E*Gamma**2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is \emph{autocalculate}.
+
+\paragraph{Field: Coefficient D}\label{field-coefficient-d}
+
+The coefficient D in the formula: Kc = A*Gamma**B + C + D*Gamma + E*Gamma**2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is \emph{autocalculate}.
+
+\paragraph{Field: Coefficient E}\label{field-coefficient-e}
+
+The coefficient E in the formula: Kc = A*Gamma**B + C + D*Gamma + E*Gamma**2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is \emph{autocalculate}.
+
+An example input is:
+
+\begin{lstlisting}
+
+  RoomAirModelType,
+      SPACE5-1 RoomAir Model,  !- Name
+      SPACE5-1,                !- Zone Name
+      UnderFloorAirDistributionInterior,  !- Room-Air Modeling Type
+      DIRECT;                  !- Air Temperature Coupling Strategy
+
+  RoomAirSettings:UnderFloorAirDistributionInterior,
+      SPACE5-1,                !- Zone Name
+      Autocalculate,           !- Number of Diffusers
+      Autocalculate,           !- Power per Plume
+      Autocalculate,           !- Design Effective Area of Diffuser {m2}
+      Autocalculate,           !- Diffuser Slot Angle from Vertical {deg}
+      ,                        !- Thermostat Height {m}
+      ,                        !- Comfort Height {m}
+      0.001,         !- Temperature Difference Threshold for Reporting {deltaC}
+      Swirl,                   !- Diffuser Type
+      1.7,                     !- Transition Height {m}
+      Autocalculate,           !- Coefficient A
+      Autocalculate,           !- Coefficient B
+      Autocalculate,           !- Coefficient C
+      Autocalculate,           !- Coefficient D
+     Autocalculate;           !- Coefficient E
+\end{lstlisting}
+
+\subsection{RoomAirSettings:UnderFloorAirDistributionExterior}\label{roomairsettingsunderfloorairdistributionexterior}
+
+This model is applicable to exterior spaces that are served by an underfloor air distribution system. The dominant sources of heat gain should be from people, equipment, and other localized sources located in the occupied part of the room, as well as convective gain coming from a warm window. The model predicts two temperatures in the room:
+
+\begin{itemize}
+\item
+  An occupied subzone temperature (T\(_{\rm{OC}}\)), representing the temperature in the region between the floor and the boundary of the upper subzone..
+\item
+  An upper subzone temperature (T\(_{\rm{MX}}\)) essential for overall energy budget calculations and for modeling comfort effects of the upper layer temperature.
+\end{itemize}
+
+The following fields are used to define an instance of the `UCSD UFAD Exterior Model Controls' object.
+
+\subsubsection{Inputs}\label{inputs-11-016}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-7-003}
+
+This field provides the unique name of a zone described elsewhere in the file. A single instance of the `RoomAirSettings:UnderFloorAirDistributionExterior' object is needed for each zone that is to be modeled using this method.
+
+\paragraph{Field: Number of Diffusers}\label{field-number-of-diffusers-1}
+
+The total number of diffusers in this zone. This field can allowed to Autocalculate (in which case it is set to the design occupancy level; i.e., number of people). If the design occupancy is low or zero but there are still heat sources that could generate buoyancy driven plumes, the user should input a value based on the design supply air flow rate of the zone and the design flow rate of an individual diffuser. In the absence of any other information, divide the zone area by 100 ft\(^{2}\). The default for this field is Autocalculate.
+
+\paragraph{Field: Power per Plume}\label{field-power-per-plume-1}
+
+The power in watts incorporated in a buoyancy driven thermal plume. Normally we assume all the loads of a workstation create a single plume so that this represents the convective heat gain from a workstation -- 1 person, 1 computer terminal, plus any task lighting. A typical value would be 220 watts. However, the model assumes an ``equivalent'' plume derived from the zone extraction rate normalized to the number of workstations/occupants. This field should be allowed to default -- the program will calculate a value based upon the occupancy and the extraction rate. The default is Autocalculate.
+
+\paragraph{Field: Design Effective Area of Diffuser}\label{field-design-effective-area-of-diffuser-1}
+
+This is the design air flow opening area in square meters of a single diffuser. The default value depends on the diffuser type. For swirl diffusers it is 0075 m\(^{2}\), for variable area diffusers 0.035 m\(^{2}\), for horizontal swirl diffusers 0.006 m\(^{2}\), and for linear bar grilles 0.03 m\(^{2}\). The default is \emph{Autocalculate}..
+
+\paragraph{Field: Diffuser Slot Angle from Vertical}\label{field-diffuser-slot-angle-from-vertical-1}
+
+This input describes the angle at which air emerges from the diffusers. It should be the angle in degrees between the vertical and the diffuser slots. The defaults depend on the diffuser type: for swirl diffusers it is 28 degrees, for variable area diffusers 45 degrees, for DV diffusers 73 degrees, and for linear bar grilles 15 degrees.
+
+\paragraph{Field: Thermostat Height}\label{field-thermostat-height-3}
+
+This field is the height in meters of the thermostat/temperature control sensor above the floor. The default is 1.2 meters.
+
+\paragraph{Field: Comfort Height}\label{field-comfort-height-2}
+
+The height in meters above the floor at which air temperature is calculated for comfort purposes. The air temperature at this height is used in calculating the available measures of comfort: Fanger, Pierce or KSU. The default is 1.1 meters.
+
+\paragraph{Field: Temperature Difference Threshold for Reporting}\label{field-temperature-difference-threshold-for-reporting-2}
+
+This field specifies a minimum temperature difference between the upper subzone and the occupied subzone that will be used to trigger whether or not the UFAD auxiliary outputs will be calculated. These outputs are \emph{Room Air Zone Transition Height} and \emph{Room Air Zone Average Temperature Gradient}. They are set to zero when the temperature difference is less than the threshold and the output \emph{Room Air Zone Is Mixed Status} is set to 1.
+
+The value should be greater than or equal to zero and is in units of degrees Centigrade. The default value is 0.4 degrees C.
+
+The value should be greater than or equal to zero and is in units of degrees Centigrade. The default value is 0.4 degrees C.
+
+\paragraph{Field: Diffuser Type}\label{field-diffuser-type-1}
+
+The choices for this alpha field are \textbf{Swirl} \textbar{} \textbf{VariableArea} \textbar{} \textbf{HorizontalSwirl \textbar{} LinearBarGrille \textbar{} Custom.} The swirl and displacement diffusers are fixed area diffusers. The variable area diffusers maintain an approximately constant exit velocity. Linear bar grilles are normally used in exterior zonesand are fixed area diffusers. Custom is used to signify that the user intends to input the coefficients A -- E (see below) rather than let the program set the coefficients based on diffuser type. The default is \emph{Swirl}.
+
+\paragraph{Field: Transition Height}\label{field-transition-height-1}
+
+An optional field to allow the user to specify the transition height (meters above floor) rather than have the program calculate it. The default is 1.7 meters.
+
+\paragraph{Field: Coefficient A}\label{field-coefficient-a-1}
+
+The coefficient A in the formula: Kc = A*Gamma**B + C + D*Gamma + E*Gamma**2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is \emph{autocalculate}.
+
+\paragraph{Field: Coefficient B}\label{field-coefficient-b-1}
+
+The coefficient B in the formula: Kc = A*Gamma**B + C + D*Gamma + E*Gamma**2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is \emph{autocalculate}.
+
+\paragraph{Field: Coefficient C}\label{field-coefficient-c-1}
+
+The coefficient C in the formula: Kc = A*Gamma**B + C + D*Gamma + E*Gamma**2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is \emph{autocalculate}.
+
+\paragraph{Field: Coefficient D}\label{field-coefficient-d-1}
+
+The coefficient D in the formula: Kc = A*Gamma**B + C + D*Gamma + E*Gamma**2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is \emph{autocalculate}.
+
+\paragraph{Field: Coefficient E}\label{field-coefficient-e-1}
+
+The coefficient E in the formula: Kc = A*Gamma**B + C + D*Gamma + E*Gamma**2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is \emph{autocalculate}.
+
+An example input is:
+
+\begin{lstlisting}
+RoomAirSettings:UnderFloorAirDistributionExterior,
+      SPACE1-1,                !- Zone Name
+      Autocalculate,           !- Number of Diffusers per Zone
+      Autocalculate,           !- Power per Plume
+      Autocalculate,           !- Design Effective Area of Diffuser {m2}
+      Autocalculate,           !- Diffuser Slot Angle from Vertical {deg}
+      ,                        !- Thermostat Height {m}
+      ,                        !- Comfort Height {m}
+      0.001,                   !- Temperature Difference Threshold for Reporting {deltaC}
+      LinearBarGrille,         !- Diffuser Type
+      1.7,                     !- Transition Height {m}
+      Autocalculate,           !- Coefficient A
+      Autocalculate,           !- Coefficient B
+      Autocalculate,           !- Coefficient C
+      Autocalculate,           !- Coefficient D
+      Autocalculate;           !- Coefficient E
+\end{lstlisting}
+
+\subsection{RoomAirflowNetwork Model}\label{roomairflownetwork-model}
+
+This model simulates a thermal zone using a network approach by assuming intra-zone nodes connected by user-defined patterns of airflows. The new model also allows users to specify a node to be connected to surfaces to have convective heat transfer between surfaces and the node, portion of internal gains and supply air and return air fractions from zone equipment. The model requires following objects to work together:
+
+\begin{itemize}
+  \item
+    RoomAirSettings:AirflowNetwork
+  \item
+    RoomAir:Node:AirflowNetwork
+  \item
+    Room\-Air\-:Node:\-Air\-flow\-Net\-work:\-Ad\-jacent\-Sur\-face\-List
+  \item
+    RoomAir:Node:Air\-flow\-Net\-work:\-Internal\-Gains
+  \item
+    RoomAir:Node:Air\-flow\-Net\-work:\-HVAC\-Equipment
+  \item
+    AirflowNetwork:Intrazone:Node
+  \item
+    Airflow\-Net\-work:\-Intra\-zone:\-Link\-age
+\end{itemize}
+
+The first \emph{five} \textbf{objects} are described below. The last two objects are described in the Airflow Network Model section.
+
+\subsection{RoomAirSettings:AirflowNetwork}\label{roomairsettingsairflownetwork}
+
+This object provides inputs in a thermal zone needed for the RoomAirflowNetwork model. The inputs specify a thermal zone and a list of RoomAir nodes. The object gives a summary of the model configuration in a zone.
+
+\subsubsection{Inputs}\label{inputs-12-015}
+
+\paragraph{Field: Name}\label{field-name-7-017}
+
+This is a unique character string associated with this instance of the Room\-Air\-Settings:\-Air\-flow\-Net\-work object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-8-002}
+
+The name of the EnergyPlus thermal zone corresponding to the RoomAir model zone.
+
+\paragraph{Field: Control Point RoomAir:Node Name}\label{field-control-point-roomairnode-name}
+
+This is the name of a RoomAir:Node:AirflowNetwork object that contains the sensor for zone HVAC controls. The conditions at this node will be used for thermostatic, humidistatic, or comfort based control decisions. The zone node defined in a Zone object is required.
+
+\paragraph{Field: RoomAir:Node:AirflowNetwork x Name}\label{field-roomairnodeairflownetwork-x-name}
+
+The name of a RoomAir:Node:AirflowNetwork object defined elsewhere. This node will receive the fraction of internal gains, and HVAC equipment, and a list of surface names exposed to this node with convective heat transfer.
+
+An IDF example input is:
+
+\begin{lstlisting}
+
+RoomAirSettings:AirflowNetwork,
+  NORTH_ZONE,     !- Name 
+  NORTH_ZONE,              !- Zone Name
+  RoomAir Schedule,        !- Availability Schedule Name
+  NORTH_ZONE,              !- Control Point RoomAir:Node Name
+  LeftUpper,               !- RoomAir:Node:AirflowNetwork 1 Name
+  CentralUpper,            !- RoomAir:Node:AirflowNetwork 2 Name
+  NORTH_ZONE,              !- RoomAir:Node:AirflowNetwork 3 Name
+  LeftMiddle,              !- RoomAir:Node:AirflowNetwork 4 Name
+  LeftLower,               !- RoomAir:Node:AirflowNetwork 5 Name
+  CentralLower;            !- RoomAir:Node:AirflowNetwork 6 Name
+\end{lstlisting}
+
+\subsection{RoomAir:Node:AirflowNetwork}\label{roomairnodeairflownetwork}
+
+This object is used to define a node in a thermal zone. The input specifies the fraction of zone volume and provides a list of names to define fraction of internal gains, surface connection and HVAC equipment.
+
+\subsubsection{Inputs}\label{inputs-13-012}
+
+\paragraph{Field: Name}\label{field-name-8-017}
+
+This is a unique character string associated with this instance of the Room\-Air\-Settings:\-Air\-flow\-Net\-work object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-9-000}
+
+The name of the EnergyPlus thermal zone and is defined in an Room\-Air\-Settings:\-Air\-flow\-Net\-work object.
+
+\paragraph{Field: Fraction of Zone Air Volume}\label{field-fraction-of-zone-air-volume}
+
+The field specifies a fraction of the overall zone air volume that is assigned to this RoomAir:Node:AirflowNetwork object. The fraction will be used to calculate zone air storage term. See corresponding sections in Engineering Reference for its use in the node energy and moisture balance equations.
+
+\paragraph{Field: RoomAir:Node:AirflowNetwork:AdjacentSurfaceList Name}\label{field-roomairnodeairflownetworkadjacentsurfacelist-name}
+
+The field specifies a name to provide a list of connected adjacent surfaces with convective heat transfer between surfaces and this particular node. When a moisture mode is assigned to surfaces, convective moisture transfer will be calculated. See corresponding sections in Engineering Reference for its use in the node energy and moisture balance equations.
+
+\paragraph{Field: RoomAir:Node:AirflowNetwork:InternalGains Name}\label{field-roomairnodeairflownetworkinternalgains-name}
+
+The field specifies a name to provide a list of internal gain objects and associated fractions assigned to this particular node. See corresponding sections in Engineering Reference for its use in the node energy and moisture balance equations.
+
+\paragraph{Field: RoomAir:Node:AirflowNetwork:HVACEquipment Name}\label{field-roomairnodeairflownetworkhvacequipment-name}
+
+The field specifies a name to provide a list of HVAC equipment, including AirLoop terminals and zone equipment. See corresponding sections in Engineering Reference for its use in the node energy and moisture balance equations.
+
+\begin{lstlisting}
+RoomAir:Node:AirflowNetwork,
+  LeftUpper,         !- Name
+  NORTH_ZONE,        !- Zone Name
+  0.15,              !- Fraction of Zone Air Volume
+  Surface_18_T_List, !- RoomAir:Node:AirflowNetwork:AdjacentSurfaceList Name
+  LeftUpper_Gain,    !- RoomAir:Node:AirflowNetwork:InternalGains Name
+  LeftUpper_HVAC;    !- RoomAir:Node:AirflowNetwork:HVACEquipment Name
+\end{lstlisting}
+
+\subsection{RoomAir:Node:AirflowNetwork:AdjacentSurfaceList}\label{roomairnodeairflownetworkadjacentsurfacelist}
+
+This object is used to provide a list of connected adjacent surfaces with convective heat transfer between surfaces and this particular node. When a moisture mode is assigned to surfaces, convective moisture transfer will be calculated. It should be pointed out that a fraction of a surface exposed to this particular node is not allowed.
+
+\subsubsection{Field: Name}\label{field-name-9-015}
+
+This is a unique character string associated with this instance of the Room\-Air\-:Node:\-Airflow\-Network:\-Adjacent\-Surface\-List object.
+
+\subsubsection{Field: Surface x Name}\label{field-surface-x-name-000}
+
+The field specifies a surface name based on the order from 1 to 21. The maximum number of surfaces can be extensible.
+
+\begin{lstlisting}
+
+RoomAir:Node:AirflowNetwork:AdjacentSurfaceList,
+  Surface_18_T_List, !- Name
+  Surface_18_T;      !- Surface 1 Name
+\end{lstlisting}
+
+\subsection{RoomAir:Node:AirflowNetwork:InternalGains}\label{roomairnodeairflownetworkinternalgains}
+
+This object is used to define a list of internal gains in the same zone and associated fraction assigned to this particular node.
+
+\subsubsection{Inputs}\label{inputs-14-012}
+
+\paragraph{Field: Name}\label{field-name-10-014}
+
+This is a unique character string associated with this instance of the Room\-Air:\-Node:\-Air\-flow\-Net\-work:\-Internal\-Gains object.
+
+\paragraph{Field: Internal Gain Object x Type}\label{field-internal-gain-object-x-type}
+
+The field specifies an internal gain object type based on the list in the Energy+.
+
+\paragraph{Field: Internal Gain Object x Name}\label{field-internal-gain-object-x-name}
+
+The field specifies an internal gain object name based on the list in the Energy+.
+
+\paragraph{Field: Fraction of Gains to Node x}\label{field-fraction-of-gains-to-node-x}
+
+The field specifies a fraction of the particular internal gain object assigned to this node.
+
+\begin{lstlisting}
+RoomAir:Node:AirflowNetwork:InternalGains,
+  CentralUpper_Gain,    !- Name
+  People,               !- Internal Gain Object 1 Type
+  NORTH_ZONE People,    !- Internal Gain Object 1 Name
+  0.15,                 !- Fraction of Gains to Node 1
+  Lights,               !- Internal Gain Object 2 Type
+  NORTH_ZONE Lights,    !- Internal Gain Object 2 Name
+  0.15,                 !- Fraction of Gains to Node 2
+  ElectricEquipment,    !- Internal Gain Object 3 Type
+  NORTH_ZONE Equip,     !- Internal Gain Object 3 Name
+  0.15;                 !- Fraction of Gains to Node 3
+\end{lstlisting}
+
+\{Field set: 3 fields (Internal Gain Object x Type, Internal Gain Object x Name, and Fraction of Gains to Node x). are extensible.\}
+
+\subsection{RoomAir:Node:AirflowNetwork:HVACEquipment}\label{roomairnodeairflownetworkhvacequipment}
+
+This object is used to define a list of HVAC equipment objects in the same zone and associated fractions assigned to this particular node.
+
+\subsubsection{Inputs}\label{inputs-15-012}
+
+\paragraph{Field: Name}\label{field-name-11-012}
+
+This is a unique character string associated with this instance of the Room\-Air:\-Node:\-Air\-flow\-Net\-work:\-HVAC\-Equipment object.
+
+\paragraph{Field: ZoneHVAC or Air Terminal Equipment Object Type x}\label{field-zonehvac-or-air-terminal-equipment-object-type-x}
+
+The field specifies an object type of ZoneHVAC equipment or terminal type based on the list in the Energy+.idd.
+
+\paragraph{Field: ZoneHVAC or Air Terminal Equipment Object Name x}\label{field-zonehvac-or-air-terminal-equipment-object-name-x}
+
+The field specifies the object name based on the object type defined in the previous field.
+
+\paragraph{Field: Fraction of Output or Supply Air from HVAC Equipment x}\label{field-fraction-of-output-or-supply-air-from-hvac-equipment-x}
+
+The field specifies a fraction of supply air from the particular equipment to this node.
+
+\paragraph{Field: Fraction of Input or Return Air from HVAC Equipment x}\label{field-fraction-of-input-or-return-air-from-hvac-equipment-x}
+
+The field specifies a fraction of return air from the particular equipment to this node.
+
+\begin{lstlisting}
+
+RoomAir:Node:AirflowNetwork:HVACEquipment,
+  CentralUpper_HVAC,        !- Name
+  ZoneHVAC:PackagedTerminalAirConditioner, !- ZoneHVAC or Air Terminal Equipment Object Type 1
+  NORTH_ZONE PTAC,       !- ZoneHVAC or Air Terminal Equipment Object Name 1
+  0.14,                   !- Fraction of Output or Supply Air from HVAC Equipment 1 
+  0.14;                   !- Fraction of Input or Return Air to HVAC Equipment 1
+\end{lstlisting}
+
+\{Field set: 4 fields (ZoneHVAC or Air Terminal Equipment Object Type x, ZoneHVAC or Air Terminal Equipment Object Name x, Fraction of Output or Supply Air from HVAC Equipment x, and Fraction of Input or Return Air from HVAC Equipment x) are extensible.\}
+
+\subsubsection{Outputs}\label{outputs-1-023}
+
+Each room air model sets up outputs specific to that model. The effect of room air modeling is usually to adjust the adjacent air temperature along the inside surface of heat transfer surfaces. The output report ``Surface Int Adjacent Air Temperature {[}C{]}'' is provided for this and described under Surface Outputs.
+
+\paragraph{Zone Predicted Sensible Load Room Air Correction Factor}\label{zone-predicted-sensible-load-room-air-correction-factor}
+
+This output variable provides the value of the correction factor applied to the predicted zone loads. Predicted zone load to setpoint is (usually) used to control HVAC air systems and the presence of a room air model has an impact on the loads. The predicited loads are multiplied by the factor in this output variable. The value is always 1.0 when there is no Room Air model. When there is a Room Air model, this output shows how that model is increasing or decreasing overall zone loads experienced by the air system.
+
+\subsubsection{Outputs}\label{outputs-2-019}
+
+The user-defined air temperature pattern that interpolates between two gradients produces the following output variable.
+
+\begin{lstlisting}
+HVAC,Average,Room Air Zone Vertical Temperature Gradient [K/m]
+\end{lstlisting}
+
+\paragraph{Room Air Zone Vertical Temperature Gradient {[}K/m{]}}\label{room-air-zone-vertical-temperature-gradient-km}
+
+This output variable is the result of the interpolation performed by the user-defined roomair model using RoomAir:TemperaturePattern:TwoGradient. This is the temperature gradient in the vertical direction. The units are degrees Kelvin per meter.
+
+\subsubsection{Outputs}\label{outputs-3-017}
+
+The following output is available for the Mundt model.
+
+\begin{lstlisting}
+Room Air Node Air Temperature {[}C{]}
+\end{lstlisting}
+
+\paragraph{Room Air Node Air Temperature {[}C{]}}\label{room-air-node-air-temperature-c}
+
+This output variable provides the drybulb air temperature used in, or calculated by, the Mundt model. The selection key is the name of an air node defined in a ROOMAIR Node object.
+
+\subsubsection{Outputs}\label{outputs-4-014}
+
+\begin{lstlisting}
+HVAC,Average,Room Air Zone Mixed Subzone Temperature [C]
+HVAC,Average,Room Air Zone Occupied Subzone Temperature [C]
+HVAC,Average,Room Air Zone Floor Subzone Temperature [C]
+HVAC,Average,Room Air Zone Transition Height [m]
+HVAC,Average,Room Air Zone Recommended Minimum Flow Fraction
+HVAC,Average,Room Air Zone Is Mixed Status \protect\hyperlinksection-1
+HVAC,Average,Room Air Zone Average Temperature Gradient [K/m]
+HVAC,Average,Room Air Zone Maximum Temperature Gradient [K/m]
+HVAC,Average,Room Air Zone Thermal Comfort Effective Air Temperature [C]
+HVAC,Average,Room Air Zone Thermostat Temperature [C]
+\end{lstlisting}
+
+\paragraph{Room Air Zone Mixed Subzone Temperature {[}C{]}}\label{room-air-zone-mixed-subzone-temperature-c}
+
+The temperature of the upper well-mixed subzone in degrees C.
+
+\paragraph{Room Air Zone Occupied Subzone Temperature {[}C{]}}\label{room-air-zone-occupied-subzone-temperature-c}
+
+The average temperature of the lower, stratified, occupied subzone in degrees C.
+
+\paragraph{Room Air Zone Floor Subzone Temperature {[}C{]}}\label{room-air-zone-floor-subzone-temperature-c}
+
+The temperature of the region near the floor in degrees C.
+
+\paragraph{Room Air Zone Transition Height {[}m{]}}\label{room-air-zone-transition-height-m}
+
+The height above the floor, in meters, of the boundary between the lower occupied subzone and the upper well-mixed subzone.
+
+\paragraph{\texorpdfstring{Room Air Zone Recommended Minimum Flow Fraction {[]}}{Room Air Zone Recommended Minimum Flow Fraction }}\label{room-air-zone-recommended-minimum-flow-fraction}
+
+The ratio of the minimum recommended flow rate to the actual flow rate. Here flow rate means the sum of infiltration, ventilation, mixing and system air flow rates. The minimum flow is the flow needed to establish the boundary between the occupied and mixed subzones at 1.5 meters.
+
+\paragraph{\texorpdfstring{Room Air Zone Is Mixed Status {[]}}{Room Air Zone Is Mixed Status }}\label{room-air-zone-is-mixed-status}
+
+An integer flag that indicates whether the zone is mixed (single node well-mixed zone model used) or stratified (UCSD DV model used). The value 1 means well-mixed; 0 means stratified.
+
+\paragraph{Room Air Zone Average Temperature Gradient {[}K/m{]}}\label{room-air-zone-average-temperature-gradient-km}
+
+The temperature gradient between the middle of the floor region and the middle of the well-mixed upper subzone in degrees Kelvin per meter.
+
+\paragraph{Room Air Zone Maximum Temperature Gradient {[}K/m{]}}\label{room-air-zone-maximum-temperature-gradient-km}
+
+The maximum of the temperature gradient between the middle of the floor region and the middle of the occupied subzone and the temperature gradient between the middle of the occupied subzone and the middle of the well-mixed subzone. The gradient is in degrees Kelvin per meter.
+
+\paragraph{Room Air Zone Thermal Comfort Effective Air Temperature {[}C{]}}\label{room-air-zone-thermal-comfort-effective-air-temperature-c}
+
+The temperature at the user specified comfort height in degrees C.
+
+\paragraph{Room Air Zone Thermostat Temperature {[}C{]}}\label{room-air-zone-thermostat-temperature-c}
+
+The temperature at the height of the thermostat (specified by user input) in degrees C.
+
+\subsubsection{Outputs}\label{outputs-5-009}
+
+\begin{itemize}
+\item
+  Zone,Average,Room Air Zone Jet Region Temperature {[}C{]}
+\item
+  Zone,Average,Room Air Zone Recirculation Region Temperature {[}C{]}
+\item
+  Zone,Average,Room Air Zone Jet Region Average Air Velocity {[}m/s{]}
+\item
+  Zone,Average,Room Air Zone Recirculation Region Average Air Velocity {[}m/s{]}
+\item
+  Zone,Average,Room Air Zone Inflow Opening Area{[}m2{]}
+\item
+  Zone,Average,Room Air Zone Room Length {[}m{]}
+\item
+  Zone,Average,Room Air Zone Recirculation and Inflow Rate Ratio
+\item
+  Zone,Average,Room Air Zone Is Mixing Status
+\item
+  Zone,Average,Room Air Zone Is Recirculating Status
+\end{itemize}
+
+\paragraph{Room Air Zone Jet Region Temperature {[}C{]}}\label{room-air-zone-jet-region-temperature-c-1}
+
+Average air temperature in the jet region of the flow in degrees C.
+
+\paragraph{Room Air Zone Recirculation Region Temperature {[}C{]}}\label{room-air-zone-recirculation-region-temperature-c-1}
+
+Average air temperature in the recirculation region of the flow in degrees C.
+
+\paragraph{Room Air Zone Jet Region Average Air Velocity {[}m/s{]}}\label{room-air-zone-jet-region-average-air-velocity-ms-1}
+
+Average airflow velocity in the jet region of the flow in meters per second.
+
+\paragraph{Room Air Zone Recirculation Region Average Air Velocity {[}m/s{]}}\label{room-air-zone-recirculation-region-average-air-velocity-ms-1}
+
+Average airflow velocity in the recirculation region of the flow in meters per second.
+
+\paragraph{Room Air Zone Inflow Opening Area {[}m2{]}}\label{room-air-zone-inflow-opening-area-m2-1}
+
+Area of the inflow aperture in square meters. This area can change due to variation in wind direction (as inflow aperture changes) or variations in the opening schedule.
+
+\paragraph{Room Air Zone Room Length {[}m{]}}\label{room-air-zone-room-length-m-1}
+
+Length of the room along the cross ventilation direction, in meters.
+
+\paragraph{\texorpdfstring{Room Air Zone Recirculation and Inflow Rate Ratio {[]}}{Room Air Zone Recirculation and Inflow Rate Ratio }}\label{room-air-zone-recirculation-and-inflow-rate-ratio-1}
+
+Ratio between airflow rate in the recirculation region and inflow rate, non-dimensional.
+
+\paragraph{\texorpdfstring{Room Air Zone Is Mixing Status {[]}}{Room Air Zone Is Mixing Status }}\label{room-air-zone-is-mixing-status-1}
+
+An integer flag that indicates whether the zone is mixed (single node well-mixed zone model used) or significant momentum conservation is occurring (UCSD CV model used). The value 1 means well-mixed; 0 means cross ventilation is present. Transition to mixed flow can occur due to three mechanism: reduction in inflow velocity, reduction in inflow aperture area and dominance of buoyancy effects. A value of 1 is yes, a value of 0 is no.
+
+\paragraph{\texorpdfstring{Room Air Zone Is Recirculating Status {[]}}{Room Air Zone Is Recirculating Status }}\label{room-air-zone-is-recirculating-status-1}
+
+An integer flag that indicates whether recirculations are present in the flow. A cross ventilation flow does not have recirculations whenever the inflow area is similar to the room cross section area (such as airflow in a typical corridor). A value of 1 is yes, a value of 0 is no.
+
+\subsubsection{Outputs}\label{outputs-6-009}
+
+\begin{itemize}
+\item
+  HVAC,Average,Room Air Zone Mixed Subzone Temperature {[}C{]}
+\item
+  HVAC,Average,Room Air Zone Occupied Subzone Temperature {[}C{]}
+\item
+  HVAC,Average,Room Air Zone Transition Height {[}m{]}
+\item
+  HVAC,Average,Room Air Zone Is Mixed Status {[]}
+\item
+  HVAC,Average,Room Air Zone Average Temperature Gradient {[}K/m{]}
+\item
+  HVAC,Average,Room Air Zone Effective Comfort Air Temperature {[}C{]}
+\item
+  HVAC,Average,Room Air Zone Thermostat Temperature {[}C{]}
+\item
+  HVAC,Average,Room Air Zone Transition Height Gamma Value {[]}
+\item
+  HVAC,Average,Room Air Zone Plume Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Room Air Zone Temperature Stratification Fraction {[]}
+\item
+  HVAC,Average,Room Air Zone Window Plume Heat Transfer Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Room Air Zone Mixed Subzone Temperature {[}C{]}}\label{room-air-zone-mixed-subzone-temperature-c-1}
+
+The temperature of the upper subzone in degrees C.
+
+\paragraph{Room Air Zone Occupied Subzone Temperature {[}C{]}}\label{room-air-zone-occupied-subzone-temperature-c-1}
+
+The temperature of the lower, occupied subzone in degrees C.
+
+\paragraph{Room Air Zone Transition Height {[}m{]}}\label{room-air-zone-transition-height-m-1}
+
+The height above the floor, in meters, of the boundary between the lower occupied subzone and the upper subzone..
+
+\paragraph{\texorpdfstring{Room Air Zone Is Mixed Status {[]}}{Room Air Zone Is Mixed Status }}\label{room-air-zone-is-mixed-status-1}
+
+An integer flag that indicates whether the zone is mixed (single node well-mixed zone model used) or stratified (UCSD UFI model used). The value 1 means well-mixed; 0 means stratified.
+
+\paragraph{Room Air Zone Average Temperature Gradient {[}K/m{]}}\label{room-air-zone-average-temperature-gradient-km-1}
+
+The temperature gradient between the middle of the occupied subzone and the middle of the upper subzone in degrees Kelvin per meter.
+
+\paragraph{Room Air Zone Effective Comfort Air Temperature {[}C{]}}\label{room-air-zone-effective-comfort-air-temperature-c}
+
+The temperature at the user specified comfort height in degrees C.
+
+\paragraph{Room Air Zone Thermostat Temperature {[}C{]}}\label{room-air-zone-thermostat-temperature-c-1}
+
+The temperature at the height of the thermostat (specified by user input) in degrees C.
+
+\paragraph{\texorpdfstring{Room Air Zone Transition Height Gamma Value {[]}}{Room Air Zone Transition Height Gamma Value }}\label{room-air-zone-transition-height-gamma-value}
+
+Value of gamma -- a dimensionless ``height'' used in calculating the transition height. Lower values of gamma indicate increased stratification, higher values less. Generally the values should be between 2 and 30.
+
+\paragraph{Room Air Zone Plume Heat Transfer Rate {[}W{]}}\label{room-air-zone-plume-heat-transfer-rate-w}
+
+The heat in watts driving the plumes in the occupied subzone.
+
+\paragraph{Room Air Zone Window Plume Heat Transfer Rate {[}W{]}}\label{room-air-zone-window-plume-heat-transfer-rate-w}
+
+The convective heat gain from windows in an UnderFloorAirDistributionExterior zone.
+
+\paragraph{\texorpdfstring{Room Air Zone Temperature Stratification Fraction {[]}}{Room Air Zone Temperature Stratification Fraction }}\label{room-air-zone-temperature-stratification-fraction}
+
+This output, (Phi) is a measure of temperature stratification in the space. It is the difference between the occupied subzone temperature and the supply temperature divided by difference between the return temperature and the supply temperature. Technically it is equal to Kc. As phi approaches 1, the space is fully mixed. As phi approaches 0, the space becomes fully stratified. Expressed as an equation:
+
+\begin{equation}
+  \frac{T_{occ} - T_{sup}}{T_{ret} - T_{sup}}
+\end{equation}
+
+\subsubsection{Outputs}\label{outputs-7-009}
+
+\begin{itemize}
+\item
+  HVAC,Average,RoomAirflowNetwork Node Temperature {[}C{]}
+\item
+  HVAC,Average,RoomAirflowNetwork Node Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,RoomAirflowNetwork Node Relative Humidity {[}\%{]}
+\item
+  HVAC,Average,RoomAirflowNetwork Node SumIntSensibleGain {[}W{]}
+\item
+  HVAC,Average,RoomAirflowNetwork Node SumIntLatentGain {[}W{]}
+\item
+  HVAC,Average,RoomAirflowNetwork Node NonAirSystemResponse {[}W{]}
+\item
+  HVAC,Average,RoomAirflowNetwork Node SysDepZoneLoadsLagged {[}W{]}
+\item
+  HVAC,Average,RoomAirflowNetwork Node HVAC Supply Fraction {[]}
+\item
+  HVAC,Average,RoomAirflowNetwork Node HVAC Return Fraction {[]}
+\end{itemize}
+
+\paragraph{RoomAirflowNetwork Node Temperature {[}C{]}}\label{roomairflownetwork-node-temperature-c-000}
+
+The temperature at a Room Air Node in a zone in degrees C.
+
+\paragraph{HVAC,Average,RoomAirflowNetwork Node Humidity Ratio {[}kgWater/kgDryAir{]}}\label{hvacaverageroomairflownetwork-node-humidity-ratio-kgwaterkgdryair}
+
+The humidity ratio at a Room Air Node in a zone in kgWater/kgDryAir.
+
+\paragraph{RoomAirflowNetwork Node Relative Humidity {[}\%{]}}\label{roomairflownetwork-node-relative-humidity}
+
+The relative humidity ratio at a Room Air Node in a zone in percent.
+
+\paragraph{HVAC,Average,RoomAirflowNetwork Node SumIntSensibleGain {[}W{]}}\label{hvacaverageroomairflownetwork-node-sumintsensiblegain-w}
+
+A sum of internal sensible gains assigned to a Room Air node in a zone.
+
+\paragraph{HVAC,Average,RoomAirflowNetwork Node SumIntLatentGain {[}W{]}}\label{hvacaverageroomairflownetwork-node-sumintlatentgain-w}
+
+A sum of internal latent gains assigned to a Room Air node in a zone.
+
+\paragraph{HVAC,Average,RoomAirflowNetwork Node NonAirSystemResponse {[}W{]}}\label{hvacaverageroomairflownetwork-node-nonairsystemresponse-w}
+
+A sum of system convective gains, collected via NonAirSystemResponse, and assigned to a Room Air node in a zone.
+
+\paragraph{HVAC,Average,RoomAirflowNetwork Node SysDepZoneLoadsLagged {[}W{]}}\label{hvacaverageroomairflownetwork-node-sysdepzoneloadslagged-w}
+
+A sum of SysDepZoneLoads saved to be added to zone heat balance at the next HVAC time step. A typical system is a zone dehumidifier.
diff --git a/doc/input-output-reference/src/overview/group-schedules.tex b/doc/input-output-reference/src/overview/group-schedules.tex
new file mode 100644
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+\section{Group -- Schedules}\label{group-schedules}
+
+This group of objects allows the user to influence scheduling of many items (such as occupancy density, lighting, thermostatic controls, occupancy activity). In addition, schedules are used to control shading element density on the building.
+
+EnergyPlus schedules consist of three pieces: a day description, a week description, and an annual description. An optional element is the schedule type. Each description level builds off the previous sub-level. The day description is simply a name and the values that span the 24 hours in a day to be associated with that name. The week description also has an identifier (name) and twelve additional names corresponding to previously defined day descriptions. There are names for each individual day of the week plus holiday, summer design day, winter design day and two more custom day designations. Finally, the annual schedule contains an identifier and the names and FROM-THROUGH dates of the week schedules associate with this annual schedule. The annual schedule can have several FROM-THROUGH date pairs. One type of schedule reads the values from an external file to facilitate the incorporation of monitored data or factors that change throughout the year.
+
+Schedules are processed by the EnergyPlus Schedule Manager, stored within the Schedule Manager and are accessed through module routines to get the basic values (timestep, hourly, etc). Values are resolved at the Zone Timestep frequency and carry through any HVAC timesteps.
+
+\subsection{Day Type}\label{day-type}
+
+A brief description of ``Day Type'' which is used in the SizingPeriod objects, RunPeriodControl:SpecialDays object, the Sizing objects and also used by reference in the Schedule:Week:Daily object (discussed later in this section).
+
+Schedules work on days of the week as well as certain specially designated days. Days of the week are the normal -- Sunday, Monday, Tuesday, Wednesday, Thursday, Friday and Saturday. Special day types that can be designated are: Holiday, SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2. These day types can be used at the user's convenience to designate special scheduling (e.g.~lights, electric equipment, set point temperatures) using these days as reference.
+
+For example, a normal office building may have normal ``occupancy'' rules during the weekdays but significantly different use on weekend. For this, you would set up rules/schedules based on the weekdays (Monday through Friday, in the US) and different rules/schedules for the weekend (Saturday and Sunday, in the US). However, you could also specially designate SummerDesignDay and WinterDesignDay schedules for sizing calculations. These schedules can be activated by setting the Day Type field in the Design Day object to the appropriate season (\textbf{SummerDesignDay} for cooling design calculations; \textbf{WinterDesignDay} for heating design calculations).
+
+In a different building, such as a theater/playhouse, the building may only have occupancy during certain weeks of the year and/or certain hours of certain days. If it was every week, you could designate the appropriate values during the ``regular'' days (Sunday through Saturday). But this would also be an ideal application for the ``CustomDay1'' and/or ``CustomDay2''. Here you would set the significant occupancy, lighting, and other schedules for the custom days and use unoccupied values for the normal weekdays. Then, using a weather file and setting special day periods as appropriate, you will get the ``picture'' of the building usage during the appropriate periods.
+
+\subsection{ScheduleTypeLimits}\label{scheduletypelimits}
+
+Schedule types can be used to validate portions of the other schedules. Hourly day schedules, for example, are validated by range -- minimum/maximum (if entered) -- as well as numeric type (continuous or discrete). Annual schedules, on the other hand, are only validated for range -- as the numeric type validation has already been done.
+
+\subsubsection{Inputs}\label{inputs-042}
+
+\paragraph{Field: Name}\label{field-name-041}
+
+This alpha field should contain a unique (within the schedule types) designator. It is referenced wherever Schedule Type Limits Names can be referenced.
+
+\paragraph{Field: Lower Limit Value}\label{field-lower-limit-value}
+
+In this field, the lower (minimum) limit value for the schedule type should be entered. If this field is left blank, then the schedule type is not limited to a minimum/maximum value range.
+
+\paragraph{Field: Upper Limit Value}\label{field-upper-limit-value}
+
+In this field, the upper (maximum) limit value for the schedule type should be entered. If this field is left blank, then the schedule type is not limited to a minimum/maximum value range.
+
+\paragraph{Field: Numeric Type}\label{field-numeric-type}
+
+This field designates how the range values are validated. Using \textbf{Continuous} in this field allows for all numbers, including fractional amounts, within the range to be valid. Using \textbf{Discrete} in this field allows only integer values between the minimum and maximum range values to be valid.
+
+\paragraph{Field: Unit Type}\label{field-unit-type}
+
+This field is used to indicate the kind of units that may be associated with the schedule that references the ScheduleTypeLimits object. It is used by IDF Editor to display the appropriate SI and IP units. This field is not used by EnergyPlus. The available options are shown below. If none of these options are appropriate, select \textbf{Dimensionless.}
+
+\begin{itemize}
+\item
+  Dimensionless
+\item
+  Temperature
+\item
+  DeltaTemperature
+\item
+  PrecipitationRate
+\item
+  Angle
+\item
+  Convection Coefficient
+\item
+  Activity Level
+\item
+  Velocity
+\item
+  Capacity
+\item
+  Power
+\item
+  Availability
+\item
+  Percent
+\item
+  Control
+\item
+  Mode
+\end{itemize}
+
+Several IDF Examples will illustrate the use:
+
+\begin{lstlisting}
+ScheduleTypeLimits,Any Number;  ! Not limited
+ScheduleTypeLimits,Fraction, 0.0 , 1.0 ,CONTINUOUS;
+ScheduleTypeLimits,Temperature,-60,200,CONTINUOUS;
+ScheduleTypeLimits,Control Type,0,4,DISCRETE;
+ScheduleTypeLimits,On/Off,0,1,DISCRETE;
+\end{lstlisting}
+
+\subsection{Day Schedules}\label{day-schedules}
+
+The day schedules perform the assignment of pieces of information across a 24 hour day. This can occur in various fashions including a 1-per hour assignment, a user specified interval scheme or a list of values that represent an hour or portion of an hour.
+
+\subsection{Schedule:Day:Hourly}\label{scheduledayhourly}
+
+The Schedule:Day:Hourly contains an hour-by-hour profile for a single simulation day.
+
+\subsubsection{Inputs}\label{inputs-1-039}
+
+\paragraph{Field: Name}\label{field-name-1-038}
+
+This field should contain a unique (within all DaySchedules) designation for this schedule. It is referenced by WeekSchedules to define the appropriate schedule values.
+
+\paragraph{Field: Schedule Type Limits Name}\label{field-schedule-type-limits-name-000}
+
+This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
+
+\paragraph{Field: Hour Values (1-24)}\label{field-hour-values-1-24}
+
+These fields contain the hourly values for each of the 24 hours in a day. (Hour field 1 represents clock time 00:00:01 AM to 1:00:00 AM, hour field 2 is 1:00:01 AM to 2:00:00 AM, etc.) The values in these fields will be passed to the simulation as indicated for ``scheduled'' items.
+
+An IDF example:
+
+\begin{lstlisting}
+Schedule:Day:Hourly, Day On Peak, Fraction,
+  0.,0.,0.,0.,0.,0.,0.,0.,0.,1.,1.,1.,1.,1.,1.,1.,1.,1.,0.,0.,0.,0.,0.,0.;
+\end{lstlisting}
+
+\subsection{Schedule:Day:Interval}\label{scheduledayinterval}
+
+The Schedule:Day:Interval introduces a slightly different way of entering the schedule values for a day. Using the intervals, you can shorten the ``hourly'' input of the ``Schedule:Day:Hourly'' object to 2 fields. And, more importantly, you can enter an interval that represents only a portion of an hour. Schedule values are ``given'' to the simulation at the zone timestep, so there is also a possibility of ``interpolation'' from the entries used in this object to the value used in the simulation.
+
+\subsubsection{Inputs}\label{inputs-2-036}
+
+\paragraph{Field: Name}\label{field-name-2-034}
+
+This field should contain a unique (within all DaySchedules) designation for this schedule. It is referenced by WeekSchedules to define the appropriate schedule values.
+
+\paragraph{Field: Schedule Type Limits Name}\label{field-schedule-type-limits-name-1-000}
+
+This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
+
+\paragraph{Field: Interpolate to Timestep}\label{field-interpolate-to-timestep}
+
+The value contained in this field directs how to apply values that aren't coincident with the given timestep (ref: Timestep) intervals. If ``Yes'' is entered, then any intervals entered here will be interpolated/averaged and that value will be used at the appropriate minute in the hour. If ``No'' is entered, then the value that occurs on the appropriate minute in the hour will be used as the schedule value.
+
+For example, if ``yes'' is entered and the interval is every 15 minutes (say a value of 0 for the first 15 minutes, then .5 for the second 15 minutes) AND there is a 10 minute timestep for the simulation: the value at 10 minutes will be 0 and the value at 20 minutes will be .25. For the same input entries but ``no'' for this field, the value at 10 minutes will be 0 and the value at 20 minutes will be .5.
+
+\paragraph{Field-Set: Time and Value (extensible object)}\label{field-set-time-and-value-extensible-object}
+
+To specify each interval, both an ``until'' time (which includes the designated time) and the value must be given.
+
+\paragraph{Field: Time}\label{field-time}
+
+The value of each field should represent clock time (standard) in the format ``Until: HH:MM''. 24 hour clock format (i.e.~1PM is 13:00) is used. Note that Until: 7:00 includes all times up through 07:00 or 7am.
+
+\paragraph{Field: Value}\label{field-value}
+
+This represents the actual value to be passed to the simulation at the appropriate timestep. (Using interpolation value as shown above). Limits on the values are indicated by the Schedule Type Limits Name field of this object.
+
+And an example of use:
+
+\begin{lstlisting}
+Schedule:Day:Interval,
+  dd winter rel humidity, !- Name
+  Percent,                !- Schedule Type Limits Name
+  No,                     !- Interpolate to Timestep
+  until: 24:00,           !- Time 1
+  74;                     !- Value Until Time 1
+\end{lstlisting}
+
+\subsection{Schedule:Day:List}\label{scheduledaylist}
+
+To facilitate possible matches to externally generated data intervals, this object has been included. In similar fashion to the Schedule:Day:Interval object, this object can also include ``sub-hourly'' values but must represent a complete day in its list of values.
+
+\subsubsection{Inputs}\label{inputs-3-032}
+
+\paragraph{Field: Name}\label{field-name-3-028}
+
+This field should contain a unique (within all day schedules) designation for this schedule. It is referenced by week schedules to define the appropriate schedule values.
+
+\paragraph{Field: Schedule Type Limits Name}\label{field-schedule-type-limits-name-2-000}
+
+This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
+
+\paragraph{Field: Interpolate to Timestep}\label{field-interpolate-to-timestep-1}
+
+The value contained in this field directs how to apply values that aren't coincident with the given timestep (ref: Timestep) intervals. If ``Yes'' is entered, then any intervals entered here will be interpolated/averaged and that value will be used at the appropriate minute in the hour. If ``No'' is entered, then the value that occurs on the appropriate minute in the hour will be used as the schedule value.
+
+For example, if ``yes'' is entered and the minutes per item is 15 minutes (say a value of 0 for the first 15 minutes, then .5 for the second 15 minutes) AND there is a 10 minute timestep for the simulation: the value at 10 minutes will be 0 and the value at 20 minutes will be .25. For the same input entries but ``no'' for this field, the value at 10 minutes will be 0 and the value at 20 minutes will be .5.
+
+\paragraph{Field: Minutes Per Item}\label{field-minutes-per-item}
+
+This field allows the ``list'' interval to be specified in the number of minutes for each item. The value here must be \textless{} = 60 and evenly divisible into 60 (same as the timestep limits).
+
+\paragraph{Field Value 1 (same definition for each value -- up to 1440 (24*60) allowed)}\label{field-value-1-same-definition-for-each-value-up-to-1440-2460-allowed}
+
+This is the value to be used for the specified number of minutes.
+
+For example:
+
+\begin{lstlisting}
+Schedule:Day:List,
+  Myschedule, ! name
+  Fraction,   ! Schedule type
+  No,         ! Interpolate value
+  30,         ! Minutes per item
+  0.0,        ! from 00:01 to 00:30
+  0.5,        ! from 00:31 to 01:00
+  <snipped>
+\end{lstlisting}
+
+\subsection{Week Schedule(s)}\label{week-schedules}
+
+The week schedule object(s) perform the task of assigning the day schedule to day types in the simulation. The basic week schedule is shown next.
+
+\subsection{Schedule:Week:Daily}\label{scheduleweekdaily}
+
+\subsubsection{Inputs}\label{inputs-4-029}
+
+\paragraph{Field: Name}\label{field-name-4-025}
+
+This field should contain a unique (within all WeekSchedules) designation for this schedule. It is referenced by Schedules to define the appropriate schedule values.
+
+\paragraph{Field: Schedule Day Name Fields (12 day types -- Sunday, Monday, \ldots{} )}\label{field-schedule-day-name-fields-12-day-types-sunday-monday}
+
+These fields contain day schedule names for the appropriate day types. Days of the week (or special days as described earlier) will then use the indicated hourly profile as the actual schedule value.
+
+An IDF example:
+
+\begin{lstlisting}
+Schedule:Week:Daily, Week on Peak,
+  Day On Peak,Day On Peak,Day On Peak,
+  Day On Peak,Day On Peak,Day On Peak,
+  Day On Peak,Day On Peak,Day On Peak,
+  Day On Peak,Day On Peak,Day On Peak;
+\end{lstlisting}
+
+\subsection{Schedule:Week:Compact}\label{scheduleweekcompact}
+
+Further flexibility can be realized by using the Schedule:Week:Compact object. In this the fields, after the name is given, a ``for'' field is given for the days to be assigned and then a dayschedule name is used.
+
+\subsubsection{Inputs}\label{inputs-5-026}
+
+\paragraph{Field:Name}\label{fieldname}
+
+This field should contain a unique (within all WeekSchedules) designation for this schedule. It is referenced by Schedules to define the appropriate schedule values.
+
+\paragraph{Field-Set -- DayType List\#, Schedule:Day Name \#}\label{field-set-daytype-list-scheduleday-name}
+
+Each assignment is made in a pair-wise fashion. First the ``days'' assignment and then the dayschedule name to be assigned. The entire set of day types must be assigned or an error will result.
+
+\paragraph{Field: DayType List \#}\label{field-daytype-list}
+
+This field can optionally contain the prefix ``For'' for clarity. Multiple choices may then be combined on the line. Choices are: Weekdays, Weekends, Holidays, Alldays, SummerDesignDay, WinterDesignDay, Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday, CustomDay1, CustomDay2. In fields after the first ``for'', AllOtherDays may also be used. Note that the colon (:) after the For is optional but is suggested for readability.
+
+\paragraph{Field: Schedule:Day Name \#}\label{field-scheduleday-name}
+
+This field contains the name of the day schedule (any of the Schedule:Day object names) that is to be applied for the days referenced in the prior field.
+
+Some IDF examples:
+
+\begin{lstlisting}
+Schedule:Week:Compact, Week on Peak,
+  For: AllDays,
+  Day On Peak;
+
+Schedule:Week:Compact, WeekDays on Peak,
+  WeekDays,
+  Day On Peak,
+  AllOtherDays
+  Day Off Peak;
+\end{lstlisting}
+
+\subsection{Schedule:Year}\label{scheduleyear}
+
+The yearly schedule is used to cover the entire year using references to week schedules (which in turn reference day schedules). If the entered schedule does not cover the entire year, a fatal error will result.
+
+\subsubsection{Inputs}\label{inputs-6-023}
+
+\paragraph{Field: Name}\label{field-name-5-021}
+
+This field should contain a unique (between Schedule:Year, Schedule:Compact, and Schedule:File) designation for the schedule. It is referenced by various ``scheduled'' items (e.g.~Lights, People, Infiltration) to define the appropriate schedule values.
+
+\paragraph{Field: Schedule Type Limits Name}\label{field-schedule-type-limits-name-3}
+
+This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
+
+\paragraph{Field Set (WeekSchedule, Start Month and Day, End Month and Day)}\label{field-set-weekschedule-start-month-and-day-end-month-and-day}
+
+Each of the designated fields is used to fully define the schedule values for the indicated time period). Up to 53 sets can be used. An error will be noted and EnergyPlus will be terminated if an incomplete set is entered. Missing time periods will also be noted as warning errors; for these time periods a zero (0.0) value will be returned when a schedule value is requested. Each of the sets has the following 5 fields:
+
+\paragraph{Field: Schedule Week Name \#}\label{field-schedule-week-name}
+
+This field contains the appropriate WeekSchedule name for the designated time period.
+
+\paragraph{Field: Start Month \#}\label{field-start-month}
+
+This numeric field is the starting month for the schedule time period.
+
+\paragraph{Field: Start Day \#}\label{field-start-day}
+
+This numeric field is the starting day for the schedule time period.
+
+\paragraph{Field: End Month \#}\label{field-end-month-000}
+
+This numeric field is the ending month for the schedule time period.
+
+\paragraph{Field: End Day \#}\label{field-end-day}
+
+This numeric field is the ending day for the schedule time period.
+
+Note that there are many possible periods to be described. An IDF example with a single period:
+
+\begin{lstlisting}
+Schedule:Year, On Peak, Fraction,
+  Week On Peak, 1,1, 12,31;
+\end{lstlisting}
+
+And a multiple period illustration:
+
+\begin{lstlisting}
+Schedule:Year,CoolingCoilAvailSched,Fraction,
+  FanAndCoilAllOffWeekSched, 1,1, 3,31,
+  FanAndCoilSummerWeekSched, 4,1, 9,30,
+  FanAndCoilAllOffWeekSched, 10,1, 12,31;
+\end{lstlisting}
+
+The following definition will generate an error (if any scheduled items are used in the simulation):
+
+\begin{lstlisting}
+Schedule:Year,MySchedule,Fraction,4,1,9,30;
+\end{lstlisting}
+
+\subsection{Schedule:Compact}\label{schedulecompact}
+
+For flexibility, a schedule can be entered in ``one fell swoop''. Using the Schedule:Compact object, all the features of the schedule components are accessed in a single command. Like the ``regular'' schedule object, each schedule:compact entry must cover all the days for a year. Additionally, the validations for DaySchedule (i.e.~must have values for all 24 hours) and WeekSchedule (i.e.~must have values for all day types) will apply. Schedule values are ``given'' to the simulation at the zone timestep, so there is also a possibility of ``interpolation'' from the entries used in this object to the value used in the simulation.
+
+This object is an unusual object for description. For the data the number of fields and position are not set, they cannot really be described in the usual Field \# manner. Thus, the following description will list the fields and order in which they must be used in the object. The name and schedule type are the exceptions:
+
+\subsubsection{Inputs}\label{inputs-7-023}
+
+\paragraph{Field: Name}\label{field-name-6-019}
+
+This field should contain a unique (between Schedule:Year, Schedule:Compact, and Schedule:File) designation for the schedule. It is referenced by various ``scheduled'' items (e.g.~Lights, People, Infiltration) to define the appropriate schedule values.
+
+\paragraph{Field: Schedule Type Limits Name}\label{field-schedule-type-limits-name-4}
+
+This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
+
+\paragraph{Field-Set (Through, For, Interpolate, Until, Value)}\label{field-set-through-for-interpolate-until-value}
+
+Each compact schedule must contain the elements Through (date), For (days), Interpolate (optional), Until (time of day) and Value. In general, each of the ``titled'' fields must include the ``title''. Note that the colon (:) after these elements (Through, For, Until) is optional but is suggested for readability.
+
+\paragraph{Field: Through}\label{field-through}
+
+This field starts with ``Through:'' and contains the ending date for the schedule period (may be more than one). Refer to Table~\ref{table:date-field-interpretation}. Date Field Interpretation for information on date entry -- note that only Month-Day combinations are allowed for this field. Each ``through'' field generates a new WeekSchedule named ``Schedule Name''\_wk\_\# where \# is the sequential number for this compact schedule.
+
+\paragraph{Field: For}\label{field-for}
+
+This field starts with ``For:'' and contains the applicable days (reference the compact week schedule object above for complete description) for the 24 hour period that must be described. Each ``for'' field generates a new DaySchedule named ``Schedule Name''\_dy\_\# where \# is the sequential number for this compact schedule.
+
+\paragraph{Field: Interpolate (optional)}\label{field-interpolate-optional}
+
+This field, if used, starts with ``Interpolate:'' and contains the word ``Yes'' or ``No''. If this field is not used, it should not be blank -- rather just have the following field appear in this slot. The definition of ``Interpolate'' in this context is shown in the interval day schedule above.
+
+\paragraph{Field: Until}\label{field-until}
+
+This field contains the ending time (again, reference the interval day schedule discussion above) for the current days and day schedule being defined.
+
+\paragraph{Field: Value}\label{field-value-1}
+
+Finally, the value field is the schedule value for the specified time interval.
+
+And, some IDF examples:
+
+\begin{lstlisting}
+Schedule:Compact,
+  POFF,       !- Name
+  Fraction,   !- Schedule Type Limits Name
+  Through: 4/30,
+  For: AllDays,
+  Until: 24:00, 1.0,
+  Through: 12/31,
+  For: Weekdays,
+    Until: 7:00,   .1,
+    Until: 17:00, 1.0,
+    Until: 24:00,  .1,
+  For: Weekends Holidays,
+    Until: 24:00,  .1,
+  For: AllOtherDays,
+    Until: 24:00,  .1;
+
+! Schedule Continuous
+Schedule:Compact,
+  Continuous,
+  on/off,
+  Through: 12/31,
+  For: AllDays,
+    Until: 24:00, 1.0;
+
+! Schedule Daytime Ventilation
+Schedule:Compact,
+  Daytime Ventilation,
+  Fraction,
+  Through: 12/31,
+  For: Weekdays SummerDesignDay,
+    Until: 08:00, 0.0,
+    Until: 18:00, 1.0,
+    Until: 24:00, 0.0,
+  For: Weekends WinterDesignDay,
+    Until: 10:00, 0.0,
+    Until: 16:00, 1.0,
+    Until: 24:00, 0.0,
+  For: Holidays AllOtherDays,
+    Until: 24:00, 0.0;
+\end{lstlisting}
+
+\subsection{Schedule:Constant}\label{scheduleconstant}
+
+The constant schedule is used to assign a constant hourly value. This schedule is created when a fixed hourly value is desired to represent a period of interest (e.g., always on operation mode for supply air fan).
+
+\subsubsection{Inputs}\label{inputs-8-021}
+
+\paragraph{Field: Name}\label{field-name-7-018}
+
+This field should contain a unique name designation for this schedule. It is referenced by Schedules to define the appropriate schedule value.
+
+\paragraph{Field: Schedule Type Limits Name}\label{field-schedule-type-limits-name-5}
+
+This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
+
+\paragraph{Field: Hourly Value}\label{field-hourly-value}
+
+This field contains a constant real value. A fixed value is assigned as an hourly value.
+
+An IDF example:
+
+\begin{lstlisting}
+Schedule:Constant,
+  AlwaysOn,     !- Name
+  On/Off,       !- Schedule Type Limits Name
+  1.0;          !- Hourly Value
+
+ScheduleTypeLimits,
+  On/Off,       !- Name
+  0,            !- Lower Limit Value
+  1,            !- Upper Limit Value
+  DISCRETE,     !- Numeric Type
+  Availability; !- Unit Type
+\end{lstlisting}
+
+\subsection{Schedule:File}\label{schedulefile}
+
+At times, data is available from a building being monitored or for factors that change throughout the year. The Schedule:File object allows this type of data to be used in EnergyPlus as a schedule. Schedule:File can also be used to read in hourly or sub-hourly schedules computed by other software or developed in a spreadsheet or other utility.
+
+The format for the data file referenced is a text file with values separated by commas (or other optional delimiters) with one line per hour. The file may contain header lines that are skipped. The file should contain values for an entire year (8760 or 8784 hours of data) or a warning message will be issued. Multiple schedules may be created using a single external data file or multiple external data files may be used. The first row of data must be for January 1, hour 1 (or timestep 1 for subhourly files).
+
+Schedule:File may be used along with the FuelFactors object and TDV files in the DataSets directory to compute Time Dependent Valuation based source energy as used by the California Energy Commission's Title 24 Energy Code. See Fuel Factor for more discussion on Time Dependent Valuation.
+
+Two optional fields: \textbf{Interpolate to Timestep} and \textbf{Minutes per Item} allow for the input of sub-hourly schedules (similar to the Schedule:Day:List object).
+
+\subsubsection{Inputs}\label{inputs-9-019}
+
+\paragraph{Field: Name}\label{field-name-8-018}
+
+This field should contain a unique (between Schedule:Year, Schedule:Compact, and Schedule:File) designation for the schedule. It is referenced by various ``scheduled'' items (e.g.~Lights, People, Infiltration, FuelFactors) to define the appropriate schedule values.
+
+\paragraph{Field: Schedule Type Limits Name}\label{field-schedule-type-limits-name-6}
+
+This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
+
+\paragraph{Field: File Name}\label{field-file-name}
+
+This field contains the name of the file that contains the data for the schedule. The field should include a full path with file name, for best results. The field must be \(\le\) 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
+
+\paragraph{Field: Column Number}\label{field-column-number}
+
+The column that contains the value to be used in the schedule. The first column is column one. If no data for a row appears for a referenced column the value of zero is used for the schedule value for that hour.
+
+\paragraph{Field: Rows to Skip at Top}\label{field-rows-to-skip-at-top}
+
+Many times the data in a file contains rows (lines) that are describing the files or contain the names of each column. These rows need to be skipped and the number of skipped rows should be entered for this field. The next row after the skipped rows must contain data for January 1, hour 1.
+
+\paragraph{Field: Number of Hours of Data}\label{field-number-of-hours-of-data}
+
+The value entered in this field should be either 8760 or 8784 as the number of hours of data. 8760 does not include the extra 24 hours for a leap year (if needed). 8784 will include the possibility of leap year data which can be processed according to leap year indicators in the weather file or specified elsewhere. Note if the simulation does not have a leap year specified but the schedule file contains 8784 hours of data, the first 8760 hours of data will be used. The schedule manager will not know to skip the 24 hours representing Feburary 29.
+
+\paragraph{Field: Column Separator}\label{field-column-separator-001}
+
+This field specifies the character used to separate columns of data if the file has more than one column. The choices are: Comma, Tab, Fixed (spaces fill each column to a fixed width), or Semicolon. The default is Comma.
+
+\paragraph{Field: Interpolate to Timestep}\label{field-interpolate-to-timestep-2}
+
+The value contained in this field directs how to apply values that aren't coincident with the given timestep (ref: TimeStep object) intervals. If ``Yes'' is entered, then any intervals entered here will be interpolated/averaged and that value will be used at the appropriate minute in the hour. If ``No'' is entered, then the value that occurs on the appropriate minute in the hour will be used as the schedule value.
+
+For example, if ``yes'' is entered and the minutes per item is 15 minutes (say a value of 0 for the first 15 minutes, then .5 for the second 15 minutes) AND there is a 10 minute timestep for the simulation: the value at 10 minutes will be 0 and the value at 20 minutes will be .25. For the same input entries but ``no'' for this field, the value at 10 minutes will be 0 and the value at 20 minutes will be .5.
+
+\paragraph{Field: Minutes Per Item}\label{field-minutes-per-item-1}
+
+This field represents the number of minutes for each item -- in this case each line of the file. The value here must be \(\le\) 60 and evenly divisible into 60 (same as the timestep limits).
+
+Here is an IDF example:
+
+\begin{lstlisting}
+Schedule:File,
+  elecTDVfromCZ01res, !- Name
+  Any Number,         !- ScheduleType
+  TDV_kBtu_CTZ01.csv, !- Name of File
+  2,                  !- Column Number
+  4,                  !- Rows to Skip at Top
+  8760,               !- Number of Hours of Data
+  Comma;              !- Column Separator
+\end{lstlisting}
+
+or with a relational path:
+
+\begin{lstlisting}
+Schedule:File,
+  elecTDVfromCZ01res, !- Name
+  Any Number,         !- ScheduleType
+  DataSets\TDV\TDV_kBtu_CTZ01.csv,  !- Name of File
+  2,                  !- Column Number
+  4;                  !- Rows to Skip at Top
+\end{lstlisting}
+
+A sub-hourly indication. Note that this is identical to an hourly file because there are 60 minutes per item -- the number of hours defaults to 8760 and the column separator defaults to a comma. If the number of minutes per item had been, say, 15, then the file would need to contain 8760*4 or 35,040 rows for this item.
+
+\begin{lstlisting}
+Schedule:File,
+  elecTDVfromCZ06com, !- Name
+  Any Number,         !- Schedule Type Limits Name
+  DataSets\TDV\TDV_2008_kBtu_CTZ06.csv, !- File Name
+  1,                  !- Column Number
+  4,                  !- Rows to Skip at Top
+  ,                   !- Number of Hours of Data
+  ,                   !- Column Separator
+  ,                   !- Interpolate to Timestep
+  60;                 !- Minutes per Item
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-031}
+
+An optional report can be used to gain the values described in the previous Schedule objects. This is a condensed reporting that illustrates the full range of schedule values -- in the style of input: DaySchedule, WeekSchedule, Annual Schedule.
+
+\begin{lstlisting}
+! will give them on hourly increments (day schedule resolution)
+Output:Reports, Schedules, Hourly;
+! will give them at the timestep of the simulation
+Output:Reports, Schedules, Timestep;
+\end{lstlisting}
+
+This report is placed on the eplusout.eio file. Details of this reporting are shown in the Output Details and Examples document.
+
+\paragraph{Schedule Value Output}\label{schedule-value-output}
+
+\begin{lstlisting}
+Zone,Average,Schedule Value {[]}
+\end{lstlisting}
+
+\paragraph{Schedule Value}\label{schedule-value}
+
+This is the schedule value (as given to whatever entity that uses it). It has no units in this context because values may be many different units (i.e.~temperatures, fractions, watts). For best results, you may want to apply the schedule name when you use this output variable to avoid output proliferation. For example, the following reporting should yield the values shown above, depending on day of week and day type:
+
+\begin{lstlisting}
+Output:Variable,People_Shopping_Sch,Schedule Value,hourly;
+Output:Variable,Activity_Shopping_Sch,Schedule Value,hourly;
+\end{lstlisting}
+
diff --git a/doc/input-output-reference/src/overview/group-setpoint-managers.tex b/doc/input-output-reference/src/overview/group-setpoint-managers.tex
new file mode 100644
index 00000000000..020174e9ad1
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-setpoint-managers.tex
@@ -0,0 +1,1742 @@
+\section{Group Setpoint Managers}\label{group-setpoint-managers}
+
+Setpoint Managers are one of the high-level control constructs in EnergyPlus. A Setpoint Manager is able to access data from any of the HVAC system nodes and use this data to calculate a setpoint (usually a temperature setpoint) for one or more other HVAC system nodes. Setpoints are then used by Controllers or Plant or Condenser Loops as a goal for their control actions.
+
+Setpoint Managers are executed at the start of each HVAC timestep, and they reside outside the HVAC system iteration loops. Thus, the Setpoint Managers are executed once per HVAC timestep, and they use previous timestep information (except for zone load) to calculate their setpoints.
+
+The following situations require the use of a Setpoint Manager:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  any use of Controller:WaterCoil; either in Temperature control only or 2 Setpoint Managers for the " TemperatureAndHumidityRatio " control variable option.
+\item
+  use of Controller:OutdoorAir with \emph{Economizer Control Type} set to anything but \emph{NoEconomizer};
+\item
+  use of Coil:Heating:Gas or Coil: Heating: Electric with the field \emph{Temperature Setpoint Node Name} set to a node name;
+\item
+  any use of CoilSystem:Cooling:DX;
+\item
+  any use of Humidifier:Steam:Electric.
+\item
+  Any use of PlantLoop or CondenserLoop which doesn't use an environment reference such as AIR or GROUND as a set point
+\end{enumerate}
+
+Setpoint managers will place a calculated or scheduled setpoint value on the setpoint node and overwrite any previous value. This value may represent one of several control types (e.g., Temperature, HumidityRatio, MassFlowRate, etc.). No two setpoint managers should use the same setpoint node for like control types.
+
+For the case when two setpoint managers place a setpoint on the same setpoint node (e.g., a temperature setpoint placed on the same node by two different setpoint managers), the setpoint value on the node is calculated by the last setpoint manager simulated. Within a specific type of setpoint manager (e.g., Scheduled), the setpoint managers are simulated in the order found in the input data file (idf) when viewed using a text editor. It is also possible for two different types of setpoint managers to place setpoints of like control variable on the same node. In this case, the order of simulation for the type of setpoint manager determines which setpoint manager is the last to write a setpoint value to the node. This conflict in setpoint node data is most likely to cause inaccurate simulation results. For this reason, a conflicting setpoint node name warning message is issued so that the conflict can be resolved. Duplicate setpoint node names found within a specific node list will not typically cause problems with the simulation (the same value is written twice to the same node). In this case a duplicate setpoint node name warning is issued, however, this could be an error in the spelling of the node name and should be corrected.
+
+Simulation order for setpoint managers:
+
+\begin{itemize}
+\item
+  SetpointManager:Scheduled
+\item
+  SetpointManager:Scheduled:DualSetpoint
+\item
+  SetpointManager:OutdoorAirReset
+\item
+  SetpointManager:SingleZone:Reheat
+\item
+  SetpointManager: SingleZone:Heating
+\item
+  SetpointManager: SingleZone:Cooling
+\item
+  SetpointManager: SingleZone:Humidity:Minimum
+\item
+  SetpointManager: SingleZone:Humidity:Maximum
+\item
+  SetpointManager:Warmest
+\item
+  SetpointManager:Coldest
+\item
+  SetpointManager:WarmestTemperatureFlow
+\item
+  SetpointManager:ReturnAirBypassFlow
+\item
+  SetpointManager:MultiZone:Cooling:Average
+\item
+  SetpointManager:MultiZone:Heating:Average
+\item
+  SetpointManager:MultiZone:MinimumHumidity:Average
+\item
+  SetpointManager:MultiZone:MaximumHumidity:Average
+\item
+  SetpointManager:MultiZone:Humidity:Minimum
+\item
+  SetpointManager:MultiZone:Humidity:Maximum
+\item
+  SetpointManager:FollowOutdoorAirTemperature
+\item
+  SetpointManager:FollowSystemNodeTemperature
+\item
+  SetpointManager:FollowGroundTemperature
+\item
+  SetpointManager:CondenserEnteringReset
+\item
+  SetpointManager:CondenserEnteringReset:Ideal
+\item
+  SetpointManager:MixedAir
+\item
+  SetpointManager:OutdoorAirPretreat
+\item
+  SetpointManager:ReturnTemperature:ChilledWater,
+\item
+  SetpointManager:ReturnTemperature:HotWater
+\end{itemize}
+
+\subsection{SetpointManager:Scheduled}\label{setpointmanagerscheduled}
+
+The simplest Setpoint Manager simply uses a schedule to determine one or more setpoints. No node data is used as input. The input consists of the Setpoint Manager name, the control variable, the schedule name, and the name of a node list. The node list contains the name of those nodes at which the setpoint is to be applied. Of course, a node list name can always be simply the name of a single node.
+
+Note that although this object provides a very general method of setting the values of many different control variables on nodes, the component models and system solvers may or may not be able to use them. Therefore, it is important to understand that simply setting a control variable using this object will not necessarily always produce the desired behavior.
+
+\subsubsection{Inputs}\label{inputs-043}
+
+\paragraph{Field: Name}\label{field-name-042}
+
+A unique, user-assigned name for an instance of a scheduled setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-000}
+
+The type of variable that will be controlled. There are several choices for this type of set point manager. The most common control variable is Temperature but other major choices include: HumidityRatio and MassFlowRate. The versatility of control variables available here (probably) exceeds what is actually available in the component and systems models. However, a large number of possible control variables are made available here for maximum flexibility and because some (but not all) component models will be able to use them. The complete list of key words and the units required in the associated schedules follow.
+
+\begin{itemize}
+\item
+  Temperature Temperture of fluid at node ( °C)
+\item
+  MaximumTemperature Maximum temperature of fluid at node ( °C)
+\item
+  MinimumTemperature Minimum temperature of fluid at node ( °C)
+\item
+  HumidityRatio Humidity ratio of fluid at node (kgWater/kgDryAir)
+\item
+  MaximumHumidityRatio Maximum humidity ratio of fluid at node (kgWater/kgDryAir)
+\item
+  MinimumHumidityRatio Minimum humidity ratio of fluid at node (kgWater/kgDryAir)
+\item
+  MassFlowRate Mass flow rate of fluid at node (kg/s)
+\item
+  MaximumMassFlowRate Maximum mass flow rate of fluid at node (kg/s)
+\item
+  MinimumMassFlowRate Minimum mass flow rate of fluid at node (kg/s)
+\end{itemize}
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-005}
+
+The name of a schedule whose values are to be used as setpoints on the node or node list. The schedule value for each time period is the setpoint for this type of setpoint manager. The schedule must have values that are in the appropriate units as defined in the previous field.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which setpoints will be established by this setpoint manager.
+
+Following is an example of the input for a Scheduled Setpoint Manager.
+
+\begin{lstlisting}
+
+SetpointManager:Scheduled,
+  Supply Air Temp Manager 1,   !- Name
+  Temperature,                               !- Control Variable
+  Seasonal Reset Supply Air Temp Sch,   !- Schedule Name
+  VAV Sys 1 Outlet Node;           !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:Scheduled:DualSetpoint}\label{setpointmanagerscheduleddualsetpoint}
+
+This setpoint manager places a high and low schedule value on one or more nodes. The input consists of the Setpoint Manager name, the control variable, the high and low set point schedule names, and the name of a node list. The node list contains the name of those nodes at which the setpoint is to be applied. Of course, a node list name can simply be the name of a single node. Currently the DualSetpoint Manager will be used with PlantLoop when the Plant Loop Demand Calculation Scheme is set to DualSetpointDeadband .
+
+\subsubsection{Inputs}\label{inputs-1-040}
+
+\paragraph{Field: Name}\label{field-name-1-039}
+
+A unique, user-assigned name for an instance of this scheduled setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-1}
+
+The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
+
+\paragraph{Field: High Setpoint Schedule Name}\label{field-high-setpoint-schedule-name}
+
+The name of a schedule that contains the high setpoint values. The schedule value for each time period is the high setpoint for this type of setpoint manager.
+
+\paragraph{Field: Low Setpoint Schedule Name}\label{field-low-setpoint-schedule-name}
+
+The name of a schedule that contains the low setpoint values. The schedule value for each time period is the low setpoint for this type of setpoint manager.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-1}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
+
+Following is an example of the input for a SetpointManager:Scheduled:DualSetpoint object.
+
+\begin{lstlisting}
+
+SetpointManager:Scheduled:DualSetpoint,
+  Water Loop Setpoint Manager,       !- Name
+  Temperature,                                       !- Control Variable
+  Plant Loop High Temp Schedule,   !- High Setpoint Schedule Name
+  Plant Loop Low Temp Schedule,     !- Low Setpoint Schedule Name
+  Plant Supply Outlet Node;             !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:OutdoorAirReset}\label{setpointmanageroutdoorairreset}
+
+The Outdoor Air Reset Setpoint Manager sets the supply air temperature according to the outdoor air temperature using a reset rule. The reset rule is determined by 2 points: the supply air setpoint temperature at the outdoor high temperature (SATOH) and the supply air setpoint temperature at the outdoor low temperature (SATOL). If the outdoor temperature is above the outdoor high temperature, the supply air temperature is set to SATOH. If the outdoor temperature is below the outdoor low temperature, the supply air temperature is set to SATOL. If the outdoor temperature is between the outdoor high and outdoor low temperatures, the supply air temperature is linearly interpolated between SATOH and SATOL.
+
+The input consists of the setpoint manager name, the type of control variable, a node list name of the nodes affected by the setpoint, and the data for the reset rule: the supply air setpoint temperature at the outdoor low temperature, the outdoor low temperature, the supply air setpoint temperature at the outdoor high temperature, and the outdoor high temperature.
+
+There are optional inputs for a second reset rule. First there is the name of a schedule that indicates which rule to use: a schedule value of 1 means use the first rule; a schedule value of 2 means use the second rule. Next, there are the 4 inputs specifying the second reset rule.
+
+\subsubsection{Inputs}\label{inputs-2-037}
+
+\paragraph{Field: Name}\label{field-name-2-035}
+
+A unique, user-assigned name for an instance of an outdoor air reset setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-2}
+
+The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
+
+\paragraph{Field: Setpoint at Outdoor Low Temperature}\label{field-setpoint-at-outdoor-low-temperature}
+
+The supply air temperature setpoint in \(^{o}\)C at the outdoor low temperature for the first reset rule.
+
+\paragraph{Field: Outdoor Low Temperature}\label{field-outdoor-low-temperature}
+
+The outdoor air low temperature in \(^{o}\)C for the first supply air temperature reset rule. Generally, at this outdoor air temperature the supply temperature is at its maximum.
+
+\paragraph{Field: Setpoint at Outdoor High Temperature}\label{field-setpoint-at-outdoor-high-temperature}
+
+The supply air temperature setpoint in \(^{o}\)C at the outdoor high temperature for the first reset rule.
+
+\paragraph{Field: Outdoor High Temperature}\label{field-outdoor-high-temperature}
+
+The outdoor air high temperature in \(^{o}\)C for the first supply air temperature reset rule. Generally, at this outdoor air temperature the supply temperature is at its minimum.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-2}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-1-002}
+
+The name of a schedule whose values indicate which reset rule to use. Schedule values of 1 indicate that the first reset rule will be used. Schedule values of 2 select the second reset rule.
+
+\paragraph{Field: Setpoint at Outdoor Low Temperature 2}\label{field-setpoint-at-outdoor-low-temperature-2}
+
+The supply air temperature setpoint in \(^{o}\)C at the outdoor low temperature for the second reset rule.
+
+\paragraph{Field: Outdoor Low Temperature 2}\label{field-outdoor-low-temperature-2}
+
+The outdoor air low temperature in \(^{o}\)C for the second supply air temperature reset rule. Generally, at this outdoor air temperature the supply temperature is at its maximum.
+
+\paragraph{Field: Setpoint at Outdoor High Temperature 2}\label{field-setpoint-at-outdoor-high-temperature-2}
+
+The supply air temperature setpoint in \(^{o}\)C at the outdoor high temperature for the second reset rule.
+
+\paragraph{Field: Outdoor High Temperature 2}\label{field-outdoor-high-temperature-2}
+
+The outdoor air high temperature in \(^{o}\)C for the second supply air temperature reset rule. Generally, at this outdoor air temperature the supply temperature is at its minimum.
+
+Below is an example of the input for an Outdoor Air Reset Setpoint Manager:
+
+\begin{lstlisting}
+
+SetpointManager:OutdoorAirReset,
+  Supply Air Temp Manager 1,   !- Name
+  Temperature,   !- Control Variable
+  16.7,   !- Setpoint at Outdoor Low Temperature {C}
+  0.0,     !- Outdoor Low Temperature {C}
+  12.8,   !- Setpoint at Outdoor High Temperature {C}
+  32.0,   !- Outdoor High Temperature {C}
+  Supply Air Temp Nodes;   !- Setpoint Node or NodeList Name
+
+  NodeList,
+  Supply Air Temp Nodes, !- Name
+  Air Loop Outlet Node;   !- Node 1 Name
+\end{lstlisting}
+
+\subsection{SetpointManager:SingleZone:Reheat}\label{setpointmanagersinglezonereheat}
+
+The Single Zone Reheat Setpoint Manager allows the simulation of a single zone reheat system. This setpoint manager detects the control zone load, zone inlet node flow rate, and zone node temperature and calculates a setpoint temperature for the supply air that will satisfy the zone load for the control zone. This setpoint manager creates a variable temperature system. The input consists of the setpoint manager name, the control variable type, the minimum and maximum supply air temperatures, the name of the control zone, the name of the control zone node, the name of the control zone inlet node, and the name of a node or node list containing the nodes whose setpoint temperatures are to be set by this manager.
+
+\subsubsection{Inputs}\label{inputs-3-033}
+
+\paragraph{Field: Name}\label{field-name-3-029}
+
+A unique, user-assigned name for an instance of this setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-3}
+
+The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
+
+\paragraph{Field: Minimum Supply Air Temperature}\label{field-minimum-supply-air-temperature}
+
+The minimum supply air temperature (in \(^{o}\)C) that is allowed for this system (as set by this setpoint manager).
+
+\paragraph{Field: Maximum Supply Air Temperature}\label{field-maximum-supply-air-temperature}
+
+The maximum supply air temperature (in \(^{o}\)C) that is allowed for this system (as set by this setpoint manager)
+
+\paragraph{Field: Control Zone Name}\label{field-control-zone-name}
+
+The name of the control zone for this single zone reheat system. The heating or cooling load for this zone determines the supply air temperature setpoint.
+
+\paragraph{Field: Zone Node Name}\label{field-zone-node-name-000}
+
+The name of the zone node for the control zone.
+
+\paragraph{Field: Zone Inlet Node Name}\label{field-zone-inlet-node-name}
+
+The name of the zone inlet node that is supplying air to the control zone.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-3}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
+
+Below is an example input for a SetpointManager:SingleZone:Reheat object.
+
+\begin{lstlisting}
+
+SetpointManager:SingleZone:Reheat,
+  Supply Air Temp Manager,   !- Name
+  Temperature,  !- Control Variable
+  13.,  !- Minimum Supply Air Temperature {C}
+  45.,  !- Maximum Supply Air Temperature {C}
+  NORTH ZONE,     !- Control Zone Name
+  Zone 3 Node,   !- Zone Node Name
+  Zone 3 Inlet Node,  !- Zone Inlet Node Name
+  Supply Air Temp Nodes;  !- Setpoint Node or NodeList Name
+
+
+  NodeList,
+  Supply Air Temp Nodes, !- Name
+  Heating Coil Air Inlet Node,   !- Node 1 Name
+  Air Loop Outlet Node; !- Node 2 Name
+\end{lstlisting}
+
+\subsection{SetpointManager:SingleZone:Heating}\label{setpointmanagersinglezoneheating}
+
+The Single Zone Heating Setpoint Manager allows a component to be controlled based on the load required to meet the zone heating setpoint. Ths setpoint manager detects the control zone load to meet the current heating setpoint, zone inlet node flow rate, and zone node temperature, and calculates a setpoint temperature for the supply air that will satisfy the zone heating load for the control zone. This setpoint manager creates a variable temperature system. The input consists of the setpoint manager name, the controlled variable type, the minimum and maximum supply air temperatures, the name of the control zone, the name of the control zone node, the name of the control zone inlet node, and the name of a node or node list containing the nodes whose setpoint temperatures are to be set by this manager.
+
+\subsubsection{Inputs}\label{inputs-4-030}
+
+\paragraph{Field: Name}\label{field-name-4-026}
+
+A unique, user-assigned name for an instance of a single zone heating setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-4}
+
+The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
+
+\paragraph{Field: Minimum Supply Air Temperature}\label{field-minimum-supply-air-temperature-1}
+
+The minimum supply air temperature (in \(^{o}\)C) that is allowed for this system (as set by this setpoint manager).
+
+\paragraph{Field: Maximum Supply Air Temperature}\label{field-maximum-supply-air-temperature-1}
+
+The maximum supply air temperature (in \(^{o}\)C) that is allowed for this system (as set by this setpoint manager)
+
+\paragraph{Field: Control Zone Name}\label{field-control-zone-name-1}
+
+The name of the control zone for this setpoint manager. The heating load for this zone (to meet the zone heating setpoint) determines the supply air temperature setpoint.
+
+\paragraph{Field: Zone Node Name}\label{field-zone-node-name-1-000}
+
+The name of the zone node for the control zone.
+
+\paragraph{Field: Zone Inlet Node Name}\label{field-zone-inlet-node-name-1}
+
+The name of the zone inlet node that is supplying air to the control zone.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-4}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
+
+Below is an example input for a SetpointManager:SingleZone:Heating object.
+
+\begin{lstlisting}
+
+SetpointManager:SingleZone:Heating,
+  Zone 1 Heating Supply Air Temp Manager,   !- Name
+  Temperature,                         !- Control Variable
+  7.22,                                       !- Minimum Supply Air Temperature {C}
+  45.,                                         !- Maximum Supply Air Temperature {C}
+  Zone 1,                                   !- Control Zone Name
+  Zone 1 Zone Node,               !- Zone Node Name
+  Zone 1 Supply Inlet,         !- Zone Inlet Node Name
+  Zone 1 Heating Coil Outlet;   !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:SingleZone:Cooling}\label{setpointmanagersinglezonecooling}
+
+The Single Zone Cooling Setpoint Manager allows a component to be controlled based on the load required to meet the zone cooling setpoint. This setpoint manager detects the control zone load to meet the current cooling setpoint, zone inlet node flow rate, and zone node temperature, and calculates a setpoint temperature for the supply air that will satisfy the zone cooling load for the control zone. This setpoint manager creates a variable temperature system. The input consists of the setpoint manager name, the controlled variable type, the minimum and maximum supply air temperatures, the name of the control zone, the name of the control zone node, the name of the control zone inlet node, and the name of a node or node list containing the nodes whose setpoint temperatures are to be set by this manager.
+
+\subsubsection{Inputs}\label{inputs-5-027}
+
+\paragraph{Field: Name}\label{field-name-5-022}
+
+A unique, user-assigned name for an instance of a single zone cooling setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-5}
+
+The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
+
+\paragraph{Field: Minimum Supply Air Temperature}\label{field-minimum-supply-air-temperature-2}
+
+The minimum supply air temperature (in \(^{o}\)C) that is allowed for this system (as set by this setpoint manager).
+
+\paragraph{Field: Maximum Supply Air Temperature}\label{field-maximum-supply-air-temperature-2}
+
+The maximum supply air temperature (in \(^{o}\)C) that is allowed for this system (as set by this setpoint manager)
+
+\paragraph{Field: Control Zone Name}\label{field-control-zone-name-2}
+
+The name of the control zone for this setpoint manager. The cooling load of this zone (to meet the zone cooling set point) determines the supply air temperature setpoint.
+
+\paragraph{Field: Zone Node Name}\label{field-zone-node-name-2}
+
+The name of the zone node for the control zone.
+
+\paragraph{Field: Zone Inlet Node Name}\label{field-zone-inlet-node-name-2}
+
+The name of the zone inlet node that is supplying air to the control zone.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-5}
+
+The name of a Node List object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
+
+Below is an example input for a SetpointManager:SingleZone:Cooling object.
+
+\begin{lstlisting}
+
+SetpointManager:SingleZone:Cooling,
+  Zone 1 Cooling Supply Air Temp Manager,   !- Name
+  Temperature,                         !- Control Variable
+  7.22,                                       !- Minimum Supply Air Temperature {C}
+  45.,                                         !- Maximum Supply Air Temperature {C}
+  Zone 1,                                   !- Control Zone Name
+  Zone 1 Zone Node,               !- Zone Node Name
+  Zone 1 Supply Inlet,         !- Zone Inlet Node Name
+  Zone 1 Cooling Coil Outlet;   !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:SingleZone:Humidity:Minimum}\label{setpointmanagersinglezonehumidityminimum}
+
+The Single Zone Minimum Humidity Setpoint Manager allows the control of a single zone minimum humidity level. This setpoint manager detects the humidity level in a control zone and, using air and moisture mass balance, calculates the supply air humidity ratio needed to maintain the zone relative humidity at or above a given setpoint. The calculated supply air humidity ratio is then used as the setpoint for the designated setpoint node. A humidifier component placed upstream of the setpoint node can then use the humidity ratio setpoint to control its moisture addition rate.
+
+The use of this object requires that a ZoneControl:Humidistat object be specified with a humidifying relative humidity schedule for the controlling zone. The humidistat s controlling zone must correspond with the control zone air node name specified in this setpoint manager.
+
+\subsubsection{Inputs}\label{inputs-6-024}
+
+\paragraph{Field: Name}\label{field-name-6-020}
+
+A unique, user-assigned name for an instance of a single zone minimum humidity setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-6}
+
+Deprecated Field. This field is not used and will be deleted in a future release.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-2-002}
+
+Deprecated Field. This field is not used and will be deleted in a future release.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-6}
+
+The name of the HVAC system node where the calculated humidity ratio setpoint is set. If the setpoint is being placed on more than one node, this input should be the name of a NodeList.
+
+\paragraph{Field: Control Zone Air Node Name}\label{field-control-zone-air-node-name}
+
+The name of the zone node for the humidity control zone (as specified in the object ZoneHVAC:EquipmentConnections).
+
+An IDF example for this setpoint manager is shown below with the required humidistat:
+
+\begin{lstlisting}
+
+SetpointManager:SingleZone:Humidity:Minimum,
+  Zone Min Set Point Manager,   !- Name
+  ,   !- Control Variable
+  ,   !- Schedule Name
+  Air Loop Outlet Node,   !- Setpoint Node or NodeList Name
+  Zone 2 Node;                     !- Control Zone Air Node Name
+
+
+  ZoneControl:Humidistat,
+  Zone 2 Humidistat,             !- Name
+  ZONE 2,                                   !-Zone Name
+  Min rel Hum Set Sch2;       !- Humidifying Relative Humidity Setpoint Schedule Name
+\end{lstlisting}
+
+\subsection{SetpointManager:SingleZone:Humidity:Maximum}\label{setpointmanagersinglezonehumiditymaximum}
+
+The Single Zone Maximum Humidity Setpoint Manager allows the control of a single zone maximum humidity level. This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level in a single control zone and uses air/moisture mass balances to calculate the supply air humidity ratio needed to maintain the zone relative humidity at or below a given setpoint. The calculated supply air humidity ratio is then used as the setpoint for the designated setpoint node. A dehumidification component placed upstream of this node can then use the humidity ratio setpoint to control its moisture removal rate (e.g., desiccant dehumidifiers).
+
+In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determine the minimum supply air temperature required to meet both the temperature (sensible) and humidity (latent) load in the control zone. See object Controller:WaterCoil in the EnergyPlus Engineering Reference for a detailed discussion of how this is achieved.
+
+The use of this object requires that a ZoneControl:Humidistat object be specified with a relative humidity setpoint schedule for the controlling zone. The humidistat s controlling zone must correspond with the control zone air node name specified in this setpoint manager..
+
+\subsubsection{Inputs}\label{inputs-7-024}
+
+\paragraph{Field: Name}\label{field-name-7-019}
+
+A unique, user-assigned name for an instance of a single zone maximum humidity setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-7}
+
+Deprecated Field. This field is not used and will be deleted in a future release.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-3-001}
+
+Deprecated Field. This field is not used and will be deleted in a future release.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-7}
+
+The name of the HVAC system node where the calculated humidity ratio setpoint is set. If the setpoint is being placed on more than one node, this input should be the name of a NodeList.
+
+\paragraph{Field: Control Zone Air Node Name}\label{field-control-zone-air-node-name-1}
+
+The name of the zone air node for the humidity control zone (as specified in the object ZoneHVAC:EquipmentConnections).
+
+An example of this object in an input data file (IDF), along with a temperature set point manager, humidistat, and a simple controller, is shown below:
+
+\begin{lstlisting}
+
+SetpointManager:SingleZone:Humidity:Maximum,
+  Zone Max Set Point Manager,                     !- Name
+  ,                                                                         !- Control Variable
+  ,                                                                         !- Schedule Name
+  VAV Sys 1 Outlet Node,                               !- Setpoint Node or NodeList Name
+  Zone 2 Node;                                                   !-Control Zone Air Node Name
+
+
+  SetpointManager:Scheduled,
+  Scheduled Set Point Manager 1,               !- Name
+  Temperature,                                                   !- Control Variable
+  Seasonal Reset Supply Air Temp Sch,     !- Schedule Name
+  VAV Sys 1 Outlet Node;                               !- Setpoint Node or NodeList Name
+
+
+  ZoneControl:Humidistat,
+  Zone 2 Humidistat,             !-Name
+  ZONE 2,                                   !- Zone Name
+  Min rel Hum Set Sch2;       !- Humidifying Relative Humidity Setpoint Schedule Name
+
+
+  Controller:WaterCoil,
+  Central Cooling Coil Contoller 1,         !- Name
+  TEMPandHUMRAT,                                               !- Control Variable
+  Reverse,                                                           !- Action
+  FLOW,                                                                 !- Actuator Variable
+  VAV Sys 1 Outlet Node,                               !- Sensor Node Name
+  Main Cooling Coil 1 Water Inlet Node, !- Actuator Node Name
+  0.002,                                                               !- Controller Convergence Tolerance {deltaC}
+  0.025,                                                               !- Maximum Actuated Flow {m3/s}
+  0.0;                                                                   !- Minimum Actuated Flow {m3/s}
+\end{lstlisting}
+
+\subsection{SetpointManager:MixedAir}\label{setpointmanagermixedair}
+
+The Mixed Air Setpoint Manager is meant to be used in conjunction with a Controller:OutdoorAir object. This setpoint manager is used to establish a temperature setpoint at the mixed air node. The Controller:OutdoorAir then operates the outdoor air damper to attempt to meet this setpoint.
+
+In EnergyPlus the relief and outdoor air dampers, the economizer, and any outdoor air conditioning equipment form a separate subsystem of an air loop system (ref. AirLoopHVAC). The outdoor air controller operates within the subsystem. Consequently the mixed air temperature setpoint must take into account any downstream system fan heat if it is to meet a desired system supply air leaving temperature. The Mixed Air Setpoint Manager accomplishes this by referencing a supply air setpoint set by another setpoint manager (most likely at the AirLoopHVAC outlet node). The supply fan inlet and outlet nodes are also inputs to the Mixed Air Setpoint Manager. From this information the Mixed Air Setpoint Manager calculates the supply fan air temperature rise, subtracts it from the reference setpoint temperature, and sets the result as the mixed air node setpoint temperature.
+
+Of course any type of setpoint manager can be used to establish a temperature setpoint at the mixed air node. But the Mixed Air Setpoint Manager is likely to be the most useful.
+
+When optional inputs of Cooling Coil Inlet Node Name, Cooling coil Outlet Node Name, and Minimum Temperature at Cooling Coil Outlet Node are provided, the setpoint temperature at the mixed air node is calculated based on the maximum of both the reference setpoint temperature and minimum cooling coil outlet temperature, minus the cooling coil air temperature reduction and the supply fan air temperature rise if the supply fan placement is blow through. The setpoin temperature at the mixed air node is used to calculate the maximum outdoor air flow fraction in the corresponding Controller:OutdoorAir object. The outdoor air flow fraction is capped at the maximum outdoor air flow fraction to prevent the cooling coil from freezing, even though the fraction is below the minimum outdoor air flow fraction.
+
+\subsubsection{Inputs}\label{inputs-8-022}
+
+\paragraph{Field: Name}\label{field-name-8-019}
+
+A unique, user-assigned name for an instance of a mixed air setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-8}
+
+The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
+
+\paragraph{Field: Reference Setpoint Node Name}\label{field-reference-setpoint-node-name}
+
+The name of an HVAC system node where the system supply air temperature is set. Normally this would be the AirLoopHVAC outlet node. The temperature setpoint at this reference node is set by a different setpoint manager.
+
+\paragraph{Field: Fan Inlet Node Name}\label{field-fan-inlet-node-name}
+
+The name of the supply fan inlet node.
+
+\paragraph{Field: Fan Outlet Node Name}\label{field-fan-outlet-node-name-000}
+
+The name of the supply fan outlet node.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-8}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name where temperature setpoints will be established by this setpoint manager.
+
+\paragraph{Field: Cooling Coil Inlet Node Name}\label{field-cooling-coil-inlet-node-name}
+
+The name of the cooling coil inlet node.
+
+\paragraph{Field: Cooling Coil Outlet Node Name}\label{field-cooling-coil-outlet-node-name}
+
+The name of the cooling coil outlet node.
+
+\paragraph{Field: Minimum Temperature at Cooling Coil Outlet Node}\label{field-minimum-temperature-at-cooling-coil-outlet-node}
+
+In order to prevent cooling coil freezing during economizer operation, the minimum temperature at the cooling coil outlet is required based on requirement of ASHRAE Standard 90.1. The default value is 7.2C.
+
+Below is an example input for a Mixed Air Setpoint Manager.
+
+\begin{lstlisting}
+
+SetpointManager:SingleZone:Reheat, ! establishes the setpoint at the system outlet node
+  Supply Air Temp Manager,   !- Name
+  Temperature,   !- Control Variable
+  13.,  !- Minimum Supply Air Temperature
+  45.,  !- Maximum Supply Air Temperature
+  NORTH ZONE,  !- Control Zone Name
+  Zone 3 Node,  !- Zone Node Name
+  Zone 3 Inlet Node,  !- Zone Inlet Node Name
+  Supply Air Temp Nodes;   !- Setpoint Node or NodeList Name
+
+
+  SetpointManager:MixedAir, ! uses the system outlet setpoint to establish the mixed air setpoint
+  Mixed Air Temp Manager 1,   !- Name
+  Temperature,   !- Control Variable
+  Air Loop Outlet Node,                   !- Reference Setpoint Node Name
+  Heating Coil Air Outlet Node,   !- Fan Inlet Node Name
+  Air Loop Outlet Node,                   !- Fan Outlet Node Name
+  Mixed Air Nodes;                             !- Setpoint Node or NodeList Name
+
+
+  NodeList, Supply Air Temp Nodes,
+  Air Loop Outlet Node; ! Setpoint Nodes
+  NodeList, Mixed Air Nodes,
+  Mixed Air Node; ! Setpoint Nodes
+\end{lstlisting}
+
+\subsection{SetpointManager:OutdoorAirPretreat}\label{setpointmanageroutdoorairpretreat}
+
+The OutdoorAir Pretreat Setpoint Manager is meant to be used in conjunction with an OutdoorAir:Mixer object. The Outdoor air Pretreat Setpoint Manager is used to establish a temperature or humidity ratio setpoint in the outdoor air stream flowing into the ``Outdoor Air Stream Node'' of an OutdoorAir:Mixer object. This setpoint manager determines the required setpoint in the outdoor air stream to produce the reference setpoint in the mixed air stream after mixing with return air. For example, if the temperature setpoint at the mixed air node is 15 °C, the return air temperature is 20 °C, and the outdoor air flow fraction is 0.5, the Outdoor Air Pretreat setpoint would be set to 10 °C.
+
+Of course any type of setpoint manager can be used to establish setpoints in the outdoor air stream, but this setpoint manager is likely to be the most useful for systems which precondition outdoor air with equipment such as a DX cooling coil or desiccant dehumidifier.
+
+\subsubsection{Inputs}\label{inputs-9-020}
+
+\paragraph{Field: Name}\label{field-name-9-016}
+
+A unique, user-assigned name for an instance of an outdoor air pretreat setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-9}
+
+The type of variable that will be controlled. The choices are:
+
+\begin{itemize}
+\item
+  Temperature references and sets the ``System Node Setpoint Temperature'' property. This single temperature setpoint is set and used by all temperature setpoint managers and equipment controls except dual-setpoint equipment.
+\item
+  MaximumHumidityRatio references and sets the ``System Node Humidity Ratio Max'' property. This type of reference setpoint may be set using SetpointManager:SingleZone:Humidity:Maximum, SetpointManager:MultiZone:MaximumHumidity:Average, or SetpointManager:MultiZone:Humidity:Maximum and is used by equipment such as Controller:WaterCoil (with control variable TemperatureAndHumidityRatio ) and Dehumidifier:Desiccant:NoFans.
+\item
+  MinimumHumidityRatio references and sets the ``System Node Humidity Ratio Min'' property. This type of reference setpoint may be set using SetpointManager:SingleZone:Humidity:Minimum, SetpointManager:Multizone:MinimumHumidity:Average or SetpointManager:MultiZone:Humidity:Minimum and is used by equipment such as Humidifier:Steam:Electric.
+\item
+  HumidityRatio references and sets the ``System Node Setpoint Humidity Ratio'' property. This type of reference setpoint may be set using (no applicable setpoint managers at this time) and is used by equipment such as Controller:WaterCoil (with control variable HumidityRatio ).
+\end{itemize}
+
+The system node properties listed above are all available as an Output:Variable to facilitate tracking these setpoints both at the reference node and the setpoint nodes.
+
+\paragraph{Field: Minimum Setpoint Temperature}\label{field-minimum-setpoint-temperature}
+
+The minimum temperature (in \(^{o}\)C) that is allowed by this setpoint manager. Applicable only if Control variable is Temperature.
+
+\paragraph{Field: Maximum Setpoint Temperature}\label{field-maximum-setpoint-temperature}
+
+The maximum temperature (in \(^{o}\)C) that is allowed by this setpoint manager. Applicable only if Control variable is Temperature.
+
+\paragraph{Field: Minimum Setpoint Humidity Ratio}\label{field-minimum-setpoint-humidity-ratio}
+
+The minimum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager. Applicable only if Control variable is MaximumHumidityRatio, MinimumHumidityRatio, or HumidityRatio. Note that zero is not allowed as the computed setpoint humidity ratio, because zero is used as a special value to indicate that no humidification or dehumidification is needed. If the reference humidity ratio setpoint value is zero, the zero value will be passed directly to the Set Point Node(s).
+
+\paragraph{Field: Maximum Setpoint Humidity Ratio}\label{field-maximum-setpoint-humidity-ratio}
+
+The maximum humidity ratio (kgWater/kgDryAir) that is allowed by this set point manager. Applicable only if Control variable is MaximumHumidityRatio, MinimumHumidityRatio, or HumidityRatio.
+
+\paragraph{Field: Reference Setpoint Node Name}\label{field-reference-setpoint-node-name-1}
+
+The name of an HVAC system node where the desired mixed air condition has been set. Normally this would be the mixed air node leaving the OutdoorAir:Mixer. The temperature or humidity setpoint at this reference node must be set by a different setpoint manager of the appropriate type (see Control Variable above).
+
+\paragraph{Field: Mixed Air Stream Node Name}\label{field-mixed-air-stream-node-name}
+
+The name of the mixed air node. This node is used to obtain the flow rate of the combined air stream. This node is usually the same node at the Reference Setpoint Node Name, but does not have to be.
+
+\paragraph{Field: Outdoor Air Stream Node Name}\label{field-outdoor-air-stream-node-name-000}
+
+The name of a node in the outdoor air stream. This node is used to obtain the flow rate of the outdoor air stream.
+
+\paragraph{Field: Return Air Stream Node Name}\label{field-return-air-stream-node-name-000}
+
+The name of a node in the return air stream. This node is used to obtain the flow rate of the return air stream.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-9}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature or humidity ratio setpoints will be established by this setpoint manager.
+
+Below is an example input for an Outdoor Air Pretreat Setpoint Manager.
+
+\begin{lstlisting}
+
+SetpointManager:OutdoorAirPretreat,
+  DXSystem 1 Desiccant Set Point Manager,   !- Name
+  MaximumHumidityRatio,       !- Control Variable
+  -99,                                         !- Minimum Setpoint Temperature {C}
+  99,                                           !- Maximum Setpoint Temperature {C}
+  0.00001,                                 !- Minimum Setpoint Humidity Ratio (kgWater/kgDryAir)
+  1.0,                                         !- Maximum Setpoint Humidity Ratio (kgWater/kgDryAir)
+  DXSystem 1 Fan Air Inlet Node,   !- Reference Setpoint Node Name
+  DXSystem 1 Mixed Air Node,           !- Mixed Air Stream Node Name
+  Heat Recovery Outlet Node,           !- Outdoor Air Stream Node Name
+  DXSystem 1 Air Loop Inlet Node, !- Return Air Stream Node Name
+  Desiccant Process Outlet Node;   !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:Warmest}\label{setpointmanagerwarmest}
+
+The Warmest Setpoint Manager resets the cooling supply air temperature of a central forced air HVAC system according to the cooling demand of the warmest zone. For each zone in the system at each system timestep, the manager calculates a supply air temperature that will meet the zone cooling load at the maximum zone supply air flow rate. The lowest of the possible supply air temperatures becomes the new supply air temperature setpoint, subject to minimum and maximum supply air temperature constraints. The resulting temperature setpoint is the highest supply air temperature that will meet the cooling requirements of all the zones. When compared to a fixed cooling supply air temperature setpoint, this strategy minimizes zone reheat coil energy (or overcooling) and central chiller energy consumption (if the chilled water temperature is also reset) at the cost of possible increased fan energy.
+
+\subsubsection{Inputs}\label{inputs-10-018}
+
+\paragraph{Field: Name}\label{field-name-10-015}
+
+A unique, user-assigned name for an instance of a warmest setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-10}
+
+The type of variable that will be controlled. Currently there is only one choice: Temperature.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name}
+
+The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its cooling supply air temperature.
+
+\paragraph{Field: Minimum Setpoint Temperature}\label{field-minimum-setpoint-temperature-1}
+
+The minimum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is less than this minimum, the setpoint is set to the minimum.
+
+\paragraph{Field: Maximum Setpoint Temperature}\label{field-maximum-setpoint-temperature-1}
+
+The maximum allowed setpoint temperature in degrees C. If the calculated setpoint is greater than this value the setpoint is set to the maximum. This value is also used as the setpoint temperature when none of the zones have a cooling load.
+
+\paragraph{Field: Strategy}\label{field-strategy}
+
+Currently, the only choice for this field is MaximumTemperature.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-10}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
+
+Below is an example input for a Warmest Setpoint Manager.
+
+\begin{lstlisting}
+
+SetpointManager:Warmest,
+  Supply Air Temperature Manager 1,   !- Name
+  Temperature,   !- Control Variable
+  VAV Sys 1,   !- HVAC Air Loop Name
+  11.2,   !- Minimum Setpoint Temperature
+  16.,   !- Maximum Setpoint Temperature
+  MaximumTemperature,   !- Strategy
+  Supply Air Temp Nodes 1;   !- Setpoint Node or NodeList Name
+
+
+  SetpointManager:MixedAir,
+  Mixed Air Temp Manager 1,   !- Name
+  Temperature,   !- Control Variable
+  VAV Sys 1 Outlet Node,   !- Reference Setpoint Node Name
+  Main Heating Coil 1 Outlet Node,   !- Fan Inlet Node Name
+  VAV Sys 1 Outlet Node,   !- Fan Outlet Node Name
+  Mixed Air Node 1;             !- Setpoint Node or NodeList Name
+
+
+  NodeList, Supply Air Temp Nodes 1,
+  VAV Sys 1 Outlet Node; ! Setpoint Node
+\end{lstlisting}
+
+\subsection{SetpointManager:Coldest}\label{setpointmanagercoldest}
+
+The Coldest Setpoint Manager is used in dual duct systems to reset the setpoint temperature of the air in the heating supply duct. Usually it is used in conjunction with a SetpointManager:Warmest resetting the temperature of the air in the cooling supply duct. For each zone in the system at each system timestep, the manager calculates a supply air temperature that will meet the zone heating load at the maximum zone supply air flow rate. The highest of the possible supply air temperatures becomes the new supply air temperature setpoint, subject to minimum and maximum supply air temperature constraints. The resulting temperature setpoint is the lowest supply air temperature that will meet the heating requirements of all the zones. When compared to a fixed heating supply air temperature setpoint, this strategy minimizes central boiler energy consumption (if the hot water temperature is also reset or there are variable speed pumps) at the cost of possible increased fan energy (if there is variable volume control in the air system).
+
+\subsubsection{Inputs}\label{inputs-11-017}
+
+\paragraph{Field: Name}\label{field-name-11-013}
+
+A unique, user-assigned name for an instance of a coldest setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-11}
+
+The type of variable that will be controlled. Currently there is only one choice: Temperature.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name-1}
+
+The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its heating supply air temperature.
+
+\paragraph{Field: Minimum Setpoint Temperature}\label{field-minimum-setpoint-temperature-2}
+
+The minimum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is less than this minimum, the setpoint is set to the minimum. This value is also used as the setpoint temperature when none of the zones have a heating load.
+
+\paragraph{Field: Maximum Setpoint Temperature}\label{field-maximum-setpoint-temperature-2}
+
+The maximum allowed setpoint temperature in degrees C. If the calculated setpoint is greater than this value the setpoint is set to the maximum.
+
+\paragraph{Field: Strategy}\label{field-strategy-1}
+
+Currently, the only choice for this field is MinimumTemperature.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-11}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
+
+Below is an example input for a Coldest Setpoint Manager.
+
+\begin{lstlisting}
+
+Controller:Simple,
+  Central Cooling Coil Controller 1,   !- Name
+  Temperature,   !- Control Variable
+  Reverse,   !- Action
+  Flow,         !- Actuator Variable
+  VAV Sys 1 Cold Outlet Node,                       !- Sensor Node Name
+  Main Cooling Coil 1 Water Inlet Node,   !- Actuator Node Name
+  0.001,       !- Controller Convergence Tolerance {deltaC}
+  autosize, !- Maximum Actuated Flow {m3/s}
+  0.0;           !- Minimum Actuated Flow {m3/s}
+
+
+  Controller:WaterCoil,
+  Central Heating Coil Controller 1,   !- Name
+  Temperature,   !- Control Variable
+  Normal,   !- Action
+  Flow,       !- Actuator Variable
+  VAV Sys 1 Hot Outlet Node,                         !- Sensor Node Name
+  Main Heating Coil 1 Water Inlet Node,   !- Actuator Node Name
+  0.001,         !- Controller Convergence Tolerance {deltaC}
+  autosize,   !- Maximum Actuated Flow {m3/s}
+  0.0;             !- Minimum Actuated Flow {m3/s}
+
+
+  SetpointManager:Warmest,
+  Supply Air Temperature Manager 1,   !- Name
+  Temperature,             !- Control Variable
+  VAV Sys 1,   !- HVAC Air Loop Name
+  11.2,             !- Minimum Setpoint Temperature {C}
+  16.,               !- Maximum Setpoint Temperature {C}
+  MaximumTemperature,             !- Strategy
+  Supply Air Temp Nodes 1;   !- Setpoint Node or NodeList Name
+
+
+  NodeList,
+  Supply Air Temp Nodes 1,         !- Name
+  VAV Sys 1 Cold Outlet Node;   !- Node 1 Name
+
+
+  SetpointManager:Coldest,
+  Supply Air Temperature Manager 2,   !- Name
+  Temperature,             !- Control Variable
+  VAV Sys 1,   !- HVAC Air Loop Name
+  25.,               !- Minimum Setpoint Temperature {C}
+  50.,               !- Maximum Setpoint Temperature {C}
+  MinimumTemperature,             !- Strategy
+  Supply Air Temp Nodes 2;   !- Setpoint Node or NodeList Name
+
+
+  NodeList,
+  Supply Air Temp Nodes 2,       !- Name
+  VAV Sys 1 Hot Outlet Node;   !- Node 1 Name
+\end{lstlisting}
+
+\subsection{SetpointManager:ReturnAirBypassFlow}\label{setpointmanagerreturnairbypassflow}
+
+This manager is user in conjunction with a return air bypass configuration. This type of air system is basically a standard single duct system with the addition of a bypass duct that bypasses return air around the main system components in particular, the central cooling coil. This allows the central cooling coil to sufficiently dehumidify the mixed air; the bypassed air is then added to the supply air stream to bring the supply air temperature up to the desired temperature set point. This scheme is very useful in situations where an higher than normal supply air temperature is used for instance, in underfloor air distribution systems.
+
+This manager relies on the program to figure out the system configuration and to extract the needed data from the system nodes. All the user needs to input is the name of the air system and a schedule giving the desired supply air temperature setpoint. No node names are required. The manager will establish a bypass air flow rate that upon mixing with the non-bypassed air will yield the temperature given in the schedule.
+
+\subsubsection{Inputs}\label{inputs-12-016}
+
+\paragraph{Field: Name}\label{field-name-12-010}
+
+A unique, user-assigned name for an instance of an Return Air Bypass Flow setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-12}
+
+The type of variable that will be controlled. Currently there is only one choice: Flow.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name-2}
+
+The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its return air bypass flow rate.
+
+\paragraph{Field: Temperature Setpoint Schedule Name}\label{field-temperature-setpoint-schedule-name}
+
+The name of a schedule whose values are temperatures in \(^{o}\)C. The schedule value for the time period is the setpoint for this type of setpoint manager. The setpoint is assumed to be at the air handler outlet.
+
+The following shows an example input for SetpointManager:ReturnAirBypassFlow.
+
+\begin{lstlisting}
+
+SetpointManager:ReturnAirBypassFlow,
+  RETURN AIR BYPASS Manager 1,   !- Name
+  Flow,   !- Control Variable
+  VAV Sys 1,   !- HVAC Air Loop Name
+  Seasonal Reset Supply Air Temp Sch;   !- Temperature Setpoint Schedule Name
+\end{lstlisting}
+
+\subsection{SetpointManager:WarmestTemperatureFlow}\label{setpointmanagerwarmesttemperatureflow}
+
+The Warmest Temperature Flow Setpoint Manager resets the cooling supply air temperature of a central forced air HVAC system according to the cooling demand of the warmest zone. The user can select one of two strategies: \emph{TemperatureFirst} or \emph{FlowFirst}.
+
+For \emph{TemperatureFirst} the manager tries to find the highest setpoint temperature that will satisfy all the zone cooling loads at minimum supply air flow rate. If this setpoint temperature is less than the minimum, the setpoint temperature is set to the minimum, and the supply air flow rate is increased to meet the loads.
+
+For \emph{FlowFirst} the manager tries to find the lowest supply air flow rate that will satisfy all the zone cooling loads at the maximum setpoint temperature. If this flow is greater than the maximum, the flow is set to the maximum and the setpoint temperature is reduced to satisfy the cooling loads.
+
+When compared to a fixed cooling supply air temperature setpoint, the \emph{TemperatureFirst} strategy minimizes fan energy at the cost of possible increased zone reheat coil energy (or overcooling) and central chiller energy consumption, whereas the \emph{FlowFirst} strategy minimizes zone reheat coil energy (or overcooling) and central chiller energy consumption at the cost of possible increased fan energy.
+
+\subsubsection{Inputs}\label{inputs-13-013}
+
+\paragraph{Field: Name}\label{field-name-13-009}
+
+A unique, user-assigned name for an instance of this setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-13}
+
+The type of variable that will be controlled. For this setpoint manager, this input should be Temperature.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name-3}
+
+he name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its cooling supply air temperature.
+
+\paragraph{Field: Minimum Setpoint Temperature}\label{field-minimum-setpoint-temperature-3}
+
+The minimum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is less than this minimum, the setpoint is set to the minimum.
+
+\paragraph{Field: Maximum Setpoint Temperature}\label{field-maximum-setpoint-temperature-3}
+
+The maximum allowed setpoint temperature in degrees C. If the calculated setpoint is greater than this value the setpoint is set to the maximum. This value is also used as the setpoint temperature when none of the zones have a cooling load.
+
+\paragraph{Field: Strategy}\label{field-strategy-2}
+
+The choices for this field are \emph{TemperatureFirst} and \emph{FlowFirst}. See discussion above for a description of what each strategy does.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-12}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
+
+\paragraph{Field: Minimum Turndown Ratio}\label{field-minimum-turndown-ratio}
+
+The minimum value of the ratio of the actual air flow rate to the maximum air flow rate, either for the supply fan if there are no VAV terminal boxes, or for the VAV boxes if present. If there are VAV boxes, it is assumed that the same value of minimum turndown applies to all boxes.
+
+Below is an example input for a SetpointManager:WarmestTemperatureFlow object.
+
+\begin{lstlisting}
+
+SetpointManager:WarmestTemperatureFlow,
+  Supply Air Temperature Manager 1,   !- Name
+  Temperature,   !- Control Variable
+  VAV Sys 1,   !- HVAC Air Loop Name
+  11.2,   !- Minimum Setpoint Temperature
+  16.,     !- Maximum Setpoint Temperature
+  TemperatureFirst,   !- Strategy
+  Supply Air Temp Nodes 1,   !- Setpoint Node or NodeList Name
+  0.3;   !- Minimum Turndown Ratio
+
+
+  SetpointManager:MixedAir,
+  Mixed Air Temp Manager 1,   !- Name
+  Temperature,   !- Control Variable
+  VAV Sys 1 Outlet Node,   !- Reference Setpoint Node Name
+  Main Heating Coil 1 Outlet Node,   !- Fan Inlet Node Name
+  VAV Sys 1 Outlet Node,   !- Fan Outlet Node Name
+  Mixed Air Node 1;   !- Setpoint Node or NodeList Name
+
+
+  NodeList, Supply Air Temp Nodes 1,
+  VAV Sys 1 Outlet Node; ! Set Point Node
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-032}
+
+\paragraph{\texorpdfstring{Setpoint Manager Warmest Temperature Critical Zone Number {[]}}{Setpoint Manager Warmest Temperature Critical Zone Number }}\label{setpoint-manager-warmest-temperature-critical-zone-number}
+
+This is the number of the zone that was the critical zone for the setpoint manager.
+
+\paragraph{\texorpdfstring{Setpoint Manager Warmest Temperature Turndown Flow Fraction {[]}}{Setpoint Manager Warmest Temperature Turndown Flow Fraction }}\label{setpoint-manager-warmest-temperature-turndown-flow-fraction}
+
+This is the fraction that flow was reduced by the setpoint manager. This is the actual air flow rate divided by the maximum air flow rate.
+
+\subsection{SetpointManager:MultiZone:Cooling:Average}\label{setpointmanagermultizonecoolingaverage}
+
+This setpoint manager is used to establish a supply air temperature setpoint for a central forced air HVAC system (air loop) based on the predicted sensible cooling loads and actual supply air mass flow rates for all zones served by the system. For all controlled zones in the air loop (i.e., zones with a thermostat object), the setpoint manager calculates an average supply air temperature that will meet the zone cooling loads based on the actual zone supply air mass flow rates (lagged by one time step). The calculated setpoint temperature is subject to the minimum and maximum setpoint temperature constraints specified by the user. When compared to a fixed cooling supply air temperature setpoint, this strategy may reduce zone reheat coil energy (or overcooling) and central chiller energy consumption (if the chilled water temperature is also reset) at the cost of possible increased fan energy.
+
+\subsubsection{Inputs}\label{inputs-14-013}
+
+\paragraph{Field: Name}\label{field-name-14-008}
+
+A unique, user-assigned name for an instance of this multizone average cooling setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name-4}
+
+The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its cooling supply air temperature.
+
+\paragraph{Field: Minimum Setpoint Temperature}\label{field-minimum-setpoint-temperature-4}
+
+The minimum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is less than this minimum, the setpoint is set to the minimum. The default value is 12C.
+
+\paragraph{Field: Maximum Setpoint Temperature}\label{field-maximum-setpoint-temperature-4}
+
+The maximum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is greater than this value, the setpoint is set to this maximum value. The default value is 18C.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-13}
+
+The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which temperature setpoints will be established by this setpoint manager.
+
+Below is an example of this object in an input file.
+
+\begin{lstlisting}
+
+SetpointManager:MultiZone:Cooling:Average,
+  Cooling Coil Air Sys Branch Set Point,   !- Name
+  Main Dual Duct Air Loop, !- HVAC Air Loop Name
+  12.0,                                       !- Minimum Setpoint Temperature {C}
+  22.0,                                       !- Maximum Setpoint Temperature {C}
+  Cooling Coil Supply Air Temp Nodes;   !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:MultiZone:Heating:Average}\label{setpointmanagermultizoneheatingaverage}
+
+This setpoint manager is used to establish a supply air temperature setpoint for a central forced air HVAC system (air loop) based on the predicted sensible heating loads and actual supply air mass flow rates for all zones served by the system. For all controlled zones in the air loop (i.e., zones with a thermostat object), the setpoint manager calculates an average supply air temperature that will meet the zone heating loads based on the actual zone supply air mass flow rates (lagged by one time step). The calculated setpoint temperature is subject to the minimum and maximum setpoint temperature constraints specified by the user. When compared to a fixed heating supply air temperature setpoint, this strategy may reduce central boiler energy consumption (if the hot water temperature is also reset or there are variable speed pumps) at the cost of possible increased fan energy (if there is variable volume control for the air system).
+
+\subsubsection{Inputs}\label{inputs-15-013}
+
+\paragraph{Field: Name}\label{field-name-15-008}
+
+A unique, user-assigned name for an instance of a multizone average heating setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name-5}
+
+The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its heating supply air temperature.
+
+\paragraph{Field: Minimum Setpoint Temperature}\label{field-minimum-setpoint-temperature-5}
+
+The minimum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is less than this minimum, the setpoint is set to the minimum. The default value is 20C.
+
+\paragraph{Field: Maximum Setpoint Temperature}\label{field-maximum-setpoint-temperature-5}
+
+The maximum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is greater than this value, the setpoint is set to this maximum value. The default value is 50C.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-14}
+
+The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which temperature setpoints will be established by this setpoint manager.
+
+Below is an example of this object in an input file.
+
+\begin{lstlisting}
+
+SetpointManager:MultiZone:Heating:Average,
+  Heating Coil Air Sys Branch Set Point,   !- Name
+  Main Dual Duct Air Loop, !- HVAC Air Loop Name
+  24.0,                                       !- Minimum Setpoint Temperature {C}
+  41.0,                                       !- Maximum Setpoint Temperature {C}
+  Heating Coil Supply Air Temp Nodes;   !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:MultiZone:MinimumHumidity:Average}\label{setpointmanagermultizoneminimumhumidityaverage}
+
+This setpoint manager allows for controlling the minimum humidity level is multiple zones served by a central forced air HVAC system (air loop). This setpoint manager, used in conjunction with one or more ZoneControl:Humidistat objects, detects the air humidity level in multiple controlled zones served by the HVAC air loop and uses air/moisture mass balances to calculate an average supply air humidity ratio needed to maintain the zone relative humidity levels near their respective humidifying setpoints. The calculated humidity ratio is then used as the minimum humidity ratio setpoint for the designated setpoint node(s). A humidification component (e.g., Humidifier:Steam:Electric) placed upstream of the setpoint node can then use the minimum humidity ratio setpoint to control humidification rate. The use of this object requires that a ZoneControl:Humidistat object be specified with a humidifying relative humidity schedule for one or more controlled zones served by the HVAC air loop.
+
+\subsubsection{Inputs}\label{inputs-16-009}
+
+\paragraph{Field: Name}\label{field-name-16-008}
+
+A unique, user-assigned name for an instance of an average minimum humidity (humidifying) multizone setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name-6}
+
+The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its humidification setpoint (minimum air humidity ratio).
+
+\paragraph{Field: Minimum Setpoint Humidity Ratio}\label{field-minimum-setpoint-humidity-ratio-1}
+
+The minimum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager. If the calculated setpoint humidity ratio is less than this value, then the setpoint is set to this minimum value. The default value is 0.005 (kgWater/kgDryAir).
+
+\paragraph{Field: Maximum Setpoint Humidity Ratio}\label{field-maximum-setpoint-humidity-ratio-1}
+
+The maximum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager. If the calculated setpoint humidity ratio is greater than this value, then the setpoint is set to this maximum value. The default value is 0.012 (kgWater/kgDryAir).
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-15}
+
+The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which humidity ratio setpoints will be established by this setpoint manager.
+
+An example of this object in an input data file (IDF), along with a humidistat object, is shown below.
+
+\begin{lstlisting}
+
+SetpointManager:MultiZone:MinimumHumidity:Average,
+  VAV_1 Humidifier HUMRAT setpoint, !- Name
+  VAV_1,                                                       !- HVAC Air Loop Name
+  0.003,                                                       !- Minimum Setpoint Humidity Ratio (kgWater/kgDryAir)
+  0.012,                                                       !- Maximum Setpoint Humidity Ratio (kgWater/kgDryAir)
+  VAV_1 Humidifier-Outlet Nodes List;           !- Setpoint Node or NodeList Name
+
+
+  ZoneControl:Humidistat,
+  ICU_NURSESTN_LOBBY_FLR_2 Humidistat,   !- Name
+  ICU_NURSESTN_LOBBY_FLR_2,   !- Zone Name
+  MinRelHumSetSch,   !- Humidifying Relative Humidity Setpoint Schedule Name
+  MaxRelHumSetSch;   !- Dehumidifying Relative Humidity Setpoint Schedule Name
+\end{lstlisting}
+
+\subsection{SetpointManager:MultiZone:MaximumHumidity:Average}\label{setpointmanagermultizonemaximumhumidityaverage}
+
+This setpoint manager allows for controlling the maximum humidity level is multiple zones served by a central forced air HVAC system (air loop). This setpoint manager, used in conjunction with one or more ZoneControl:Humidistat objects, detects the air humidity level in multiple controlled zones served by the HVAC air loop and uses air/moisture mass balances to calculate an average supply air humidity ratio needed to maintain the zone relative humidity levels near their respective dehumidifying setpoints. The calculated humidity ratio is then used as the maximum humidity ratio setpoint for the designated setpoint node(s). A dehumidification component (e.g., desiccant dehumidifiers) placed upstream of the setpoint node can then use the maximum humidity ratio setpoint to control its moisture removal rate. The use of this object requires that a ZoneControl:Humidistat object be specified with a dehumidifying relative humidity schedule for one or more controlled zones served by the HVAC air loop.
+
+In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determine the supply air temperature required to meet both the temperature (sensible) and humidity (latent) load in the control zone. See object Controller:WaterCoil in the EnergyPlus Engineering Reference for a detailed discussion of how this is achieved.
+
+\subsubsection{Inputs}\label{inputs-17-007}
+
+\paragraph{Field: Name}\label{field-name-17-006}
+
+A unique, user-assigned name for an instance of an average maximum humidity ratio (dehumidifying) multizone setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name-7}
+
+The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its dehumidification setpoint (maximum air humidity ratio).
+
+\paragraph{Field: Minimum Setpoint Humidity Ratio}\label{field-minimum-setpoint-humidity-ratio-2}
+
+The minimum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager. If the calculated setpoint humidity ratio is less than this value, then the setpoint is set to this minimum value. The default value is 0.008 (kgWater/kgDryAir).
+
+\paragraph{Field: Maximum Setpoint Humidity Ratio}\label{field-maximum-setpoint-humidity-ratio-2}
+
+The maximum humidity ratio (kgWater/kgDryAir) that is allowed by this set point manager. If the calculated setpoint humidity ratio is greater than this value, then the setpoint is set to this maximum value. The default value is 0.015 (kgWater/kgDryAir).
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-16}
+
+The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which humidity ratio setpoints will be established by this setpoint manager.
+
+An example of this object in an input data file (IDF), along with a humidistat object, is shown below:
+
+\begin{lstlisting}
+
+SetpointManager:MultiZone:MaximumHumidity:Average,
+  VAV_1_CoolC HUMRAT setpoint,           !- Name
+  VAV_1,                                                       !- HVAC Air Loop Name
+  0.005,                                                       !- Minimum Setpoint Humidity Ratio (kgWater/kgDryAir)
+  0.015,                                                       !- Maximum Setpoint Humidity Ratio (kgWater/kgDryAir)
+  VAV_1 DeHumidifier-Outlet Nodes List;       !- Setpoint Node or NodeList Name
+
+
+  ZoneControl:Humidistat,
+  ICU_NURSESTN_LOBBY_FLR_2 Humidistat,   !- Name
+  ICU_NURSESTN_LOBBY_FLR_2,   !- Zone Name
+  MinRelHumSetSch,   !- Humidifying Relative Humidity Setpoint Schedule Name
+  MaxRelHumSetSch;   !- Dehumidifying Relative Humidity Setpoint Schedule Name
+\end{lstlisting}
+
+\subsection{SetpointManager:MultiZone:Humidity:Minimum}\label{setpointmanagermultizonehumidityminimum}
+
+This setpoint manager allows for controlling the minimum humidity level in multiple zones served by a central forced air HVAC system (air loop). This setpoint manager, used in conjunction with one or more ZoneControl:Humidistat objects, detects the air humidity level in multiple controlled zones served by the HVAC air loop and uses air/moisture mass balances to calculate a supply air minimum humidity ratio based on a zone with the critical humidification requirement (i.e., a zone with the highest humidity ratio setpoint) to maintain the zone relative humidity levels near their respective humidifying setpoints. The calculated humidity ratio is then used as the minimum humidity ratio setpoint for the designated setpoint node(s). A humidification component (e.g., Humidifier:Steam:Electric) placed upstream of the setpoint node can then use the minimum humidity ratio setpoint to control humidification rate. The use of this object requires that a ZoneControl:Humidistat object be specified with a humidifying relative humidity schedule for one or more controlled zones served by the HVAC air loop. If ZoneControl:Humidistat object is defined for only one of the zones served by the air loop then the SetpointManager:MultiZone:Humidity:Minimum perform as SepointManager:SingleZone:Humidity:Minimum.
+
+\subsubsection{Inputs}\label{inputs-18-007}
+
+\paragraph{Field: Name}\label{field-name-18-006}
+
+A unique, user-assigned name for an instance of a multizone minimum humidity (humidifying) setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name-8}
+
+The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its humidification setpoint (minimum air humidity ratio).
+
+\paragraph{Field: Minimum Setpoint Humidity Ratio}\label{field-minimum-setpoint-humidity-ratio-3}
+
+The minimum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager. If the calculated setpoint humidity ratio is less than this value, then the setpoint is set to this minimum value. The default value is 0.005 (kgWater/kgDryAir).
+
+\paragraph{Field: Maximum Setpoint Humidity Ratio}\label{field-maximum-setpoint-humidity-ratio-3}
+
+The maximum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager. If the calculated setpoint humidity ratio is greater than this value, then the setpoint is set to this maximum value. The default value is 0.012 (kgWater/kgDryAir).
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-17}
+
+The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which humidity ratio setpoints will be established by this setpoint manager.
+
+An example of this object in an input data file (IDF), along with a humidistat object, is shown below.
+
+\begin{lstlisting}
+
+SetpointManager:MultiZone:Humidity:Minimum,
+  Main Humidifier setpoint Mgr,     !- Name
+  VAV Sys 1,                                           !- HVAC Air Loop Name
+  0.003,                                                   !- Minimum Setpoint Humidity Ratio (kgWater/kgDryAir)
+  0.015,                                                   !- Maximum Setpoint Humidity Ratio (kgWater/kgDryAir)
+  Main Humidifier Outlet Node;       !- Setpoint Node or NodeList Name
+
+
+  ZoneControl:Humidistat,
+  Space5-1 Humidistat,         !- Name
+  SPACE5-1,                               !- Zone Name
+  HumidifyingHumSetSch,       !- Humidifying Relative Humidity Setpoint Schedule Name
+  DehumidifyingHumSetSch;   !- Dehumidifying Relative Humidity Setpoint Schedule Name
+\end{lstlisting}
+
+\subsection{SetpointManager:MultiZone:Humidity:Maximum}\label{setpointmanagermultizonehumiditymaximum}
+
+This setpoint manager allows for controlling the maximum humidity level in multiple zones served by a central forced air HVAC system (air loop). This setpoint manager, used in conjunction with one or more ZoneControl:Humidistat objects, detects the air humidity level in multiple controlled zones served by the HVAC air loop and uses air/moisture mass balances to calculate the maximum supply air humidity ratio based on a zone with the critical dehumidification requirement (i.e., a zone with the lowest humidity ratio setpoint) to maintain the zone relative humidity levels near their respective dehumidifying setpoints. The calculated humidity ratio is then used as the maximum humidity ratio setpoint for the designated setpoint node(s). A dehumidification component (e.g., desiccant dehumidifiers) placed upstream of the setpoint node can then use the maximum humidity ratio setpoint to control its moisture removal rate. The use of this object requires that a ZoneControl:Humidistat object be specified with a dehumidifying relative humidity schedule for one or more controlled zones served by the HVAC air loop. If ZoneControl:Humidistat object is defined for only one of the zones served by the air loop then the SetpointManager:MultiZone:Humidity:Maximum perform as SetpointManager:SingleZone:Humidity:Maximum.
+
+In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determine the supply air temperature required to meet both the temperature (sensible) and dehumidification (latent) load in the control zone. See object Controller:WaterCoil in the EnergyPlus Engineering Reference for a detailed discussion of how this is achieved.
+
+\subsubsection{Inputs}\label{inputs-19-005}
+
+\paragraph{Field: Name}\label{field-name-19-003}
+
+A unique, user-assigned name for an instance of a multizone maximum humidity ratio (dehumidifying) setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name-9}
+
+The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its dehumidification setpoint (maximum air humidity ratio).
+
+\paragraph{Field: Minimum Setpoint Humidity Ratio}\label{field-minimum-setpoint-humidity-ratio-4}
+
+The minimum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager. If the calculated setpoint humidity ratio is less than this value, then the setpoint is set to this minimum value. The default value is 0.008 (kgWater/kgDryAir).
+
+\paragraph{Field: Maximum Setpoint Humidity Ratio}\label{field-maximum-setpoint-humidity-ratio-4}
+
+The maximum humidity ratio (kgWater/kgDryAir) that is allowed by this set point manager. If the calculated setpoint humidity ratio is greater than this value, then the setpoint is set to this maximum value. The default value is 0.015 (kgWater/kgDryAir).
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-18}
+
+The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which humidity ratio setpoints will be established by this setpoint manager.
+
+An example of this object in an input data file (IDF), along with a humidistat object, is shown below.
+
+\begin{lstlisting}
+
+SetpointManager:MultiZone:Humidity:Maximum,
+  Maximum Mzone HUMRAT setpoint,   !- Name
+  VAV Sys 1,                                           !- HVAC Air Loop Name
+  0.003,                                                   !- Minimum Setpoint Humidity Ratio (kgWater/kgDryAir)
+  0.015,                                                   !- Maximum Setpoint Humidity Ratio (kgWater/kgDryAir)
+  DeHumidifier-Outlet Nodes;           !- Setpoint Node or NodeList Name
+
+
+  ZoneControl:Humidistat,
+  Space5-1 Humidistat,         !- Name
+  SPACE5-1,                               !- Zone Name
+  HumidifyingHumSetSch,       !- Humidifying Relative Humidity Setpoint Schedule Name
+\end{lstlisting}
+
+\subsection{SetpointManager:FollowOutdoorAirTemperature}\label{setpointmanagerfollowoutdoorairtemperature}
+
+This setpoint manager is used to place a temperature setpoint on a system node that is derived from the current outdoor air environmental conditions. The outdoor air conditions are obtained from the weather information during the simulation.
+
+\subsubsection{Inputs}\label{inputs-20-005}
+
+\paragraph{Field: Name}\label{field-name-20-002}
+
+A unique user-defined name for an instance of this setpoint manager.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-14}
+
+The type of variable that will be controlled. There are three choices available: Temperature, MaximumTemperature, or MinimumTemperature.
+
+\paragraph{Field: Reference Temperature Type}\label{field-reference-temperature-type}
+
+The field specifies the type of temperature value to obtain from the system node referenced in the previous field. The two available options are OutdoorDryBulb and OutdoorWetBulb.
+
+\paragraph{Field: Offset Temperature Difference}\label{field-offset-temperature-difference}
+
+This field provides a temperature offset that will be applied to the value of the reference temperature (outdoor air wetbulb/drybulb). If this value is zero, and the limits are met, then the resulting setpoint will be exactly the same as the outdoor air wetbulb/drybulb temperature. The sign convention is that a positive value here will increase the resulting setpoint to higher than the outdoor air wetbulb/drybulb.
+
+\paragraph{Field: Maximum Setpoint Temperature}\label{field-maximum-setpoint-temperature-6}
+
+This field provides an upper limit to the resulting setpoint value.
+
+\paragraph{Field: Minimum Setpoint Temperature}\label{field-minimum-setpoint-temperature-6}
+
+This field provides a lower limit to the resulting setpoint value.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-19}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which setpoints will be established by this setpoint manager.
+
+An IDF example of use:
+
+\begin{lstlisting}
+
+SetpointManager:FollowOutdoorAirTemperature,
+  MyCondenserControl,         !- Name
+  Temperature,                       !- Control Variable
+  OutdoorAirDryBulb,           !- Reference Temperature Type
+  0.5,                                       !- Offset Temperature Difference {deltaC}
+  200,                                       !- Maximum Setpoint Temperature {C}
+  21.1,                                     !- Minimum Setpoint Temperature {C}
+  CondSupplyOutletNode;     !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:FollowSystemNodeTemperature}\label{setpointmanagerfollowsystemnodetemperature}
+
+This setpoint manager is used to place a temperature setpoint on a system node that is derived from the current temperatures at a separate system node. The current value of the temperature at a reference node is obtained and used to generate setpoint on a second system node. If the reference node is also designated to be an outdoor air (intake) node, then this setpoint manager can be used to follow outdoor air conditions that are adjusted for altitude.
+
+\subsubsection{Inputs}\label{inputs-21-005}
+
+\paragraph{Field: Name}\label{field-name-21-002}
+
+A unique user-defined name for an instance of this setpoint manager.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-15}
+
+The type of variable that will be controlled. There are three choices available: Temperature, MaximumTemperature, or MinimumTemperature.
+
+\paragraph{Field: Reference Node Name}\label{field-reference-node-name}
+
+The name of a system node where this setpoint manager will obtain a reference temperature to follow. Note that the temperature to obtained is the current temperature on the node and not the current value of a temperature \emph{setpoint}.
+
+\paragraph{Field: Reference Temperature Type}\label{field-reference-temperature-type-1}
+
+The field specifies the type of temperature value to obtain from the system node referenced in the previous field. The two available options are NodeDryBulb and NodeWetBulb.
+
+\paragraph{Field: Offset Temperature Difference}\label{field-offset-temperature-difference-1}
+
+This field provides a temperature offset that will be applied to the value obtained from the reference system node. If this value is zero, and the limits are met, then the resulting setpoint will be exactly the same as the reference system node temperature. The sign convention is that a positive value here will increase the resulting setpoint to higher than the temperature at the reference node.
+
+\paragraph{Field: Maximum Limit Setpoint Temperature}\label{field-maximum-limit-setpoint-temperature}
+
+This field provides an upper limit to the resulting setpoint value.
+
+\paragraph{Field: Minimum Limit Setpoint Temperature}\label{field-minimum-limit-setpoint-temperature}
+
+This field provides a lower limit to the resulting setpoint value.
+
+\paragraph{Field: Setpoint System Node or NodeList Name}\label{field-setpoint-system-node-or-nodelist-name}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which setpoints will be established by this setpoint manager.
+
+An IDF example of use:
+
+\begin{lstlisting}
+
+SetpointManager:FollowSystemNodeTemperature,
+  MyCondenserControl,         !- Name
+  Temperature,                       !- Control Variable
+  MyOAinletNode,                   !- Reference Node Name
+  NodeDryBulb,                       !- Reference Temperature Type
+  0.5,                                       !- Offset Temperature Difference {deltaC}
+  200,                                       !- Maximum Setpoint Temperature {C}
+  24.0,                                     !- Minimum Setpoint Temperature {C}
+  CondSupplyOutletNode;     !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:FollowGroundTemperature}\label{setpointmanagerfollowgroundtemperature}
+
+This setpoint manager is used to place a temperature setpoint on a system node that is derived from a current ground temperature. The ground temperatures are specified in different Site:GroundTemperature:* objects and used during the simulation. This setpoint manager is primarily intended for condenser or plant loops using some type of ground heat exchanger.
+
+\subsubsection{Inputs}\label{inputs-22-004}
+
+\paragraph{Field: Name}\label{field-name-22-002}
+
+A unique user-defined name for an instance of this setpoint manager.
+
+\paragraph{Field: Control Variable}\label{field-control-variable-16}
+
+The type of variable that will be controlled. There are three choices available: Temperature, MaximumTemperature, or MinimumTemperature.
+
+\paragraph{Field: Reference Ground Temperature Object Type}\label{field-reference-ground-temperature-object-type}
+
+This field is used to specify the type of ground temperature to be used by the setpoint manager. There are four options, Site:GroundTemperature:BuildingSurface, Site:GroundTemperature:Shallow, Site:GroundTemperature:Deep, or Site:GroundTemperature:FCfactorMethod. Generally the deep ground temperatures are the most useful for a plant loop serving a vertical borehole ground heat exchanger.
+
+\paragraph{Field: Offset Temperature Difference}\label{field-offset-temperature-difference-2}
+
+This field provides a temperature offset that will be applied to the value of the ground temperature. If this value is zero, and the limits are met, then the resulting setpoint will be exactly the same as the ground temperature. The sign convention is that a positive value here will increase the resulting setpoint to higher than the ground temperature.
+
+\paragraph{Field: Maximum Setpoint Temperature}\label{field-maximum-setpoint-temperature-7}
+
+This field provides an upper limit to the resulting setpoint value.
+
+\paragraph{Field: Minimum Setpoint Temperature}\label{field-minimum-setpoint-temperature-7}
+
+This field provides a lower limit to the resulting setpoint value.
+
+\paragraph{Field: Setpoint System Node or NodeList Name}\label{field-setpoint-system-node-or-nodelist-name-1}
+
+The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which setpoints will be established by this setpoint manager.
+
+An IDF example of use:
+
+\begin{lstlisting}
+
+SetpointManager:FollowGroundTemperature,
+  MyCondenserControl,                   !- Name
+  Temperature,                                 !- Control Variable
+  Site:GroundTemperature:Deep, !- Reference Ground Temperature Object Type
+  1.5,                                                 !- Offset Temperature Difference {deltaC}
+  50.0,                                               !- Maximum Setpoint Temperature {C}
+  10.0,                                               !- Minimum Setpoint Temperature {C}
+  CondSupplyOutletNode;               !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:CondenserEnteringReset}\label{setpointmanagercondenserenteringreset}
+
+The object resets the condenser entering water temperature setpoint to the optimal setpoint temperature that will result in minimum net energy consumption for the chiller and cooling tower plant. This chiller-tower optimization scheme uses one curve to determine the optimum condenser entering water temperature for a given time step and two other curves to place limit conditions on the optimized setpoint value. Note that this object will work with only one cooling tower object in a plant loop.
+
+\subsubsection{Inputs}\label{inputs-23-004}
+
+\paragraph{Field: Name}\label{field-name-23-002}
+
+A unique, user assigned name for an instance of the optimized condenser entering water setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control variable}\label{field-control-variable-17}
+
+The type of variable that will be controlled. The only valid choice for this setpoint manager is \textbf{Temperature}.
+
+\paragraph{Field: Default Condenser Entering Water Temperature Schedule Name}\label{field-default-condenser-entering-water-temperature-schedule-name}
+
+This schedule should define the default condenser entering water temperature setpoint. This scheduled setpoint value is only used in a given time step if the optimized setpoint value (see the Optimized Condenser Entering Water Temperature Curve Name field) does not fall within its prescribed boundary conditions.
+
+\paragraph{Field: Minimum Design Wetbulb Temperature Curve Name}\label{field-minimum-design-wetbulb-temperature-curve-name}
+
+The curve name associated with the coefficients in the equation used to determine the minimum design tower wetbulb referenced by the minimum outside air wetbulb temperature curve below. The value from this curve is compared to the tower design wet bulb each timestep to establish one of the governing boundaries over the optimized condenser entering water temperature setpoint calculation. This curve must be quad-linear (Curve:QuadLinear) and is defined as:
+
+\begin{equation}
+T = {C_1} + {C_2}\cdot OaWb + {C_3}\cdot WPLR + {C_4}TwrWb + {C_5}NF
+\end{equation}
+
+where,
+
+OaWb = Outside air wet bulb for current timestep, ËšC
+
+WPLR = Weighted Part Load Ratio, dimensionless
+
+TwrWb = Design tower wet bulb boundary condition, ËšC
+
+NF = Normalized condenser water flow per unit of tower capacity, m3/s-W
+
+\paragraph{Field: Minimum Outside Air Wetbulb Temperature Curve Name}\label{field-minimum-outside-air-wetbulb-temperature-curve-name}
+
+The curve name associated with the coefficients in the equation used to determine the minimum actual wetbulb referenced by the optimized condenser entering water temperature curve. The value from this curve is compared the actual outside wet bulb each timestep to establish one of the governing boundaries over the optimized condenser entering water temperature setpoint calculation. This curve must be quad-linear (Curve:QuadLinear) and is defined as:
+
+\begin{equation}
+T = {C_1} + {C_2}\cdot MinWb + {C_3}\cdot WPLR + {C_4}\cdot TwrWb + {C_5}NF
+\end{equation}
+
+Where
+
+MinWb = Minimum design wetbulb for current timestep, ËšC
+
+WPLR = Weighted Part Load Ratio, dimensionless
+
+TwrWb = Design tower wet bulb boundary condition, ËšC
+
+NF = Normalized condenser water flow per unit of tower capacity, m3/s-W
+
+\paragraph{Field: Optimized Condenser Entering Temperature Curve Name}\label{field-optimized-condenser-entering-temperature-curve-name}
+
+The curve name associated with the coefficients in the optimized condenser entering water temperature equation. The value from this curve is used to calculate the optimized condenser entering water temperature for each timestep. If this optimized setpoint does not fall within the bounds established by the two boundary conditions, then the value from the Default Condenser Entering Water Temperature Schedule is used for the Condenser Entering Water Setpoint for that timestep. This curve must be quad-linear (Curve:QuadLinear) and is defined as:
+
+\begin{equation}
+T = {C_1} + {C_2}OaWb + {C_3}WPLR + {C_4}TwrWb + {C_5}NF
+\end{equation}
+
+where,
+
+OaWb = Outside air wet bulb for current timestep, ËšC
+
+WPLR = Weighted Part Load Ratio, dimensionless
+
+TwrWb = Design tower wet bulb boundary condition, ËšC
+
+NF = Normalized condenser water flow per unit of tower capacity, m3/s-W
+
+\paragraph{Field: Minimum Lift}\label{field-minimum-lift}
+
+This field establishes the minimum Lift allowed. Lift is generally thought of as the difference between condenser refrigerant pressure and the evaporator refrigerant pressure. Using defined pressure and temperature relationships, lift also can be related to the difference between the leaving chilled water and the leaving condenser water temperature. Further, when the leaving condenser water temperature and condenser water flow are constant, the entering condenser temperature can be used as a proxy for lift. Because most condenser water systems are designed for constant flow, entering condenser temperature is the most common metric for lift, and that is what meant here. If the calculated Condenser Entering Water Setpoint falls below (TEvapLvgWater+ MinimumLift), then the Condenser Entering Water Setpoint is reset to equal TEvapLvgWater+ MinimumLift. The units for this field are deg C TD. Default is 11.1 ËšC (20 F).
+
+\paragraph{Field: Maximum Condenser Entering Temperature}\label{field-maximum-condenser-entering-temperature}
+
+This field establishes the maximum condenser entering water setpoint temperature allowed. If the scheduled or calculated setpoint is above TCondEntMax, then TCondEntSetpoint is reset to equal TCondEntMax. The units for this field are deg C.
+
+\paragraph{Field: Cooling Tower Design Inlet Air Wet-Bulb Temperature}\label{field-cooling-tower-design-inlet-air-wet-bulb-temperature}
+
+This field defines the reference wet bulb temperature used to size the cooling tower. Typically, the design condenser entering water temperature equals TwrRefOaWb + TowerApproachTD. The units for this field are deg C.
+
+\paragraph{Field: Setpoint Node or Node List Name}\label{field-setpoint-node-or-node-list-name}
+
+This field defines the condenser node being controlled.
+
+Below is an example input for a CondenserEnteringReset Setpoint Manager.
+
+\begin{lstlisting}
+
+SetpointManager:CondenserEnteringReset,
+  Condenser Optimized Setpoint Manager,   !- Name
+  Temperature,                   !- Control Variable
+  DefaultCondEntSch,       !- Default Condenser Entering Water Temperature Schedule Name
+  MinDsnWBCurveName,       !- Minimum Design Wetbulb Temperature Curve Name
+  MinActWBCurveName,       !- Minimum Outside Air Wetbulb Temperature Curve Name
+  OptCondEntCurveName,   !- Optimized Cond Entering Water Temperature Curve Name
+  12,                                     !- Minimum Lift, C
+  32,                                     !- Maximum Condenser Entering Water Temp, C
+  25.56,                               !- Cooling Tower Design Inlet Air Wetbulb Temperature, C
+  Cond Water Setpoint Node;   !- Setpoint Node or Node List Name
+\end{lstlisting}
+
+\subsection{SetpointManager:CondenserEnteringReset:Ideal}\label{setpointmanagercondenserenteringresetideal}
+
+The object determines a near-optimal condenser water entering setpoint at each time step that will result in minimum net energy consumption for the chiller and coolingtower plant. The ideal chiller-tower optimization scheme uses a search algorithm to find the ideal optimal setpoint at a given timestep. Note that this object will work with only one chiller object and only one cooling tower object in a plant loop.
+
+\subsubsection{Inputs}\label{inputs-24-002}
+
+\paragraph{Field: Name}\label{field-name-24-001}
+
+A unique, user assigned name for an instance of the optimized condenser entering water setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
+
+\paragraph{Field: Control variable}\label{field-control-variable-18}
+
+The type of variable that will be controlled. There is only one choice for this type of setpoint manager: \textbf{Temperature}.
+
+\paragraph{Field: Minimum Lift}\label{field-minimum-lift-1}
+
+This field establishes the minimum lift allowed. Lift is generally thought of as the difference between condenser refrigerant pressure and the evaporator refrigerant pressure. Using defined pressure and temperature relationships, lift also can be related to the difference between the leaving chilled water and the leaving condenser water temperature. Further, when the leaving condenser water temperature and condenser water flow are constant, the entering condenser temperature can be used as a proxy for lift. Because most condenser water systems are designed for constant flow, entering condenser temperature is the most common metric for lift, and that is what meant here. If the optimized condenser entering water setpoint falls below leaving evaporator water temperature plus minimum lift, then the condenser entering water setpoint is reset to equal this field value plus leaving evaporator water temperature. This determines the minimum boundary of condenser entering water setpoint. The unit for this field is deg C TD. Default is 11.1 deg C (20 deg F).
+
+\paragraph{Field: Maximum Condenser Entering Water Temperature}\label{field-maximum-condenser-entering-water-temperature}
+
+This field establishes the maximum condenser entering water setpoint temperature allowed. If the optimized condenser entering water setpoint is above this field value, then the condenser entering water setpoint is reset to equal this filed value. The units for this field are deg C. Default is 34 deg C
+
+\paragraph{Field: Setpoint Node or Node List Name}\label{field-setpoint-node-or-node-list-name-1}
+
+This field defines the condenser node being controlled.
+
+Below is an example input for a IdealCondenserEnteringReset Setpoint Manager.
+
+\begin{lstlisting}
+
+SetpointManager:CondenserEnteringReset:Ideal,
+  Condenser Optimized Setpoint Manager,   !- Name
+  Temperature,                   !- Control Variable
+  12,                                     !- Minimum Lift, C
+  32,                                     !- Maximum Condenser Entering Water Temp, C
+  Cond Water Setpoint Node;   !- Setpoint Node or Node List Name
+\end{lstlisting}
+
+\subsection{SetpointManager:SingleZone:OneStageCooling}\label{setpointmanagersinglezoneonestagecooling}
+
+The singe-zone, one-stage cooling setpoint manager allows a component to be controlled based on thermostatic control using the object ZoneControl:Thermostat:StagedDualSetpoint. This setpoint manager differs from other parts of EnergyPlus that control based on predicted loads to setpoint. This setpoint manager allows modeling on/off cycling of DX coils using CoilSystem:Cooling:DX in continuous fan air handlers. This setpoint manger detects if the zone is calling for a cooling stage and applies one setpoint value if cooling is called for and another setpoint value if cooling is not called for.
+
+This method of control is much more like real world thermostatic control but it requires short zone timesteps. Models using this type of control should use 60 timesteps per hour and will run much slower because of that.
+
+\subsubsection{Inputs}\label{inputs-25-002}
+
+\paragraph{Field: Name}\label{field-name-25-001}
+
+This alpha field is a unique, user-assigned name for an instance of a single zone one stage cooling setpoint manager.
+
+\paragraph{Field: Cooling Stage On Supply Air Setpoint Temperature}\label{field-cooling-stage-on-supply-air-setpoint-temperature}
+
+This numeric field is the setpoint temperature to apply when the manager intends to turn on cooling, in degrees Celsius. The default is -99.0 °C.
+
+\paragraph{Field: Cooling Stage Off Supply Air Setpoint Temperature}\label{field-cooling-stage-off-supply-air-setpoint-temperature}
+
+This numeric field is the setpoint temperature to apply when the manager intends to turn off cooling, in degrees Celsius. The value in this field must be higher than the value in the previous field. The default is 99.0 °C.
+
+\paragraph{Field: Control Zone Name}\label{field-control-zone-name-3}
+
+This alpha field is the name of the control zone for this setpoint manager. This zone needs to be controlled using ZoneControl:Thermostat:StagedDualSetpoint.
+
+\paragraph{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-20}
+
+This alpha field is the name of a NodeList objet containing the names of the HVAC system nodes, or the name of a system node, for which temperature setpoints will be established by this setpoint manager.
+
+An example input follows.
+
+\begin{lstlisting}
+
+SetpointManager:SingleZone:OneStageCooling,
+  ZSF2 cooling on_off , !- Name
+  -99.0 , !- Cooling Stage On Supply Air Setpoint Temperature
+  99.0 , !- Cooling Stage Off Supply Air Setpoint Temperature
+  ZSF2 , !- Control Zone Name
+  DX Cooling Coil 3 Outlet Node ; !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:SingleZoneOneStageHeating}\label{setpointmanagersinglezoneonestageheating}
+
+The singe-zone, one-stage heating setpoint manager allows a component to be controlled based on thermostatic control using the object ZoneControl:Thermostat:StagedDualSetpoint. This setpoint manager differs from other parts of EnergyPlus that control based on predicted loads to setpoint. This setpoint manager allows modeling on/off cycling of heating coils in continuous fan air handlers. This setpoint manger detects if the zone is calling for a heating stage and applies one setpoint value if heating is called for and another setpoint value if heating is not called for.
+
+This method of control is much more like real world thermostatic control but it requires short zone timesteps. Models using this type of control should use 60 timesteps per hour and will run much slower because of that.
+
+\subsubsection{Field: Name}\label{field-name-26-001}
+
+This alpha field is a unique, user-assigned name for an instance of a single zone one stage heating setpoint manager.
+
+\subsubsection{Field: Heating Stage On Supply Air Setpoint Temperature}\label{field-heating-stage-on-supply-air-setpoint-temperature}
+
+This numeric field is the setpoint temperature to apply when the manager intends to turn on heating, in degrees Celsius. The default is 99.0 °C.
+
+\subsubsection{Field: Heating Stage Off Supply Air Setpoint Temperature}\label{field-heating-stage-off-supply-air-setpoint-temperature}
+
+This numeric field is the setpoint temperature to apply when the manager intends to turn off heating, in degrees Celsius. The value in this field must be lower than the value in the previous field. The default is -99.0 °C.
+
+\subsubsection{Field: Control Zone Name}\label{field-control-zone-name-4}
+
+This alpha field is the name of the control zone for this setpoint manager. This zone needs to be controlled using ZoneControl:Thermostat:StagedDualSetpoint.
+
+\subsubsection{Field: Setpoint Node or NodeList Name}\label{field-setpoint-node-or-nodelist-name-21}
+
+This alpha field is the name of a NodeList objet containing the names of the HVAC system nodes, or the name of a system node, for which temperature setpoints will be established by this setpoint manager.
+
+An example input follows.
+
+\begin{lstlisting}
+
+SetpointManager:SingleZone:OneStageHeating,
+  ZNF1 heating on_off , !- Name
+  99.0 , !- Heating Stage On Supply Air Setpoint Temperature
+  -99.0 , !- Heating Stage Off Supply Air Setpoint Temperature
+  ZNF1 , !- Control Zone Name
+  Main Heating Coil 2 Air Outlet Node ; !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\subsection{SetpointManager:ReturnTemperature:ChilledWater}\label{setpointmanagerreturntemperaturechilledwater}
+
+This setpoint manager allows for the central plant simulation in EnergyPlus to target a specific return water temperature entering the plant supply equipment. This setpoint manager is specifically for ``chilled water'' (although it could be any fluid) applications. This setpoint manager senses the current supply and return temperatures, calculates the current demand on the loop, and assuming this load remains constant for this time step, it predicts what set-point temperature would provide the desired target return temperature.
+
+Because this is predictive, and the setpoint is only updated once per system timestep (frequency of the call to ManageSetPoints), the longer the time step, the less accurate the prediction will be. To make tighter control, the time step can be reduced down even to one minute. However, as described in the EngineeringReference, for most realistic building profiles the control works quite well under normal timestep size. If your load profile is highly jagged with step changes in demand, a smaller timestep could help achieve tight control.
+
+\subsubsection{Inputs}\label{inputs-26-001}
+
+\paragraph{Field: Name}\label{field-name-27-001}
+
+This alpha field is a unique, user-assigned name for an instance of a chilled water return temperature reset setpoint manager.
+
+\paragraph{Plant Loop Supply Outlet Node}\label{plant-loop-supply-outlet-node}
+
+This alpha field is the name of the plant loop supply side outlet node for the plant being managed by this setpoint manager. The current temperature of this node is sensed in order to calculate current loop demand. This node is typically also where the plant loop setpoint is specified, but not necessarily. This setpoint manager looks up the actual setpoint node from the PlantLoop internal data structures as it is specified on the PlantLoop object. If the plant loop setpoint is on a different node than the supply outlet node, the loop may not maintain return temperature control as expected.
+
+\paragraph{Plant Loop Supply Inlet Node}\label{plant-loop-supply-inlet-node}
+
+This alpha field is the name of the plant loop supply side inlet node whose temperature is controlled using this setpoint manager by resetting the supply setpoint temperature. The current temperature of this node is also sensed in order to calculate current loop demand.
+
+\paragraph{Minimum Supply Temperature Setpoint}\label{minimum-supply-temperature-setpoint}
+
+This numeric field plays multiple roles. During initialization, such as before the plant data structures are fully established, this is used as the default plant supply setpoint temperature. During normal calculation, this is used as the minimum chilled water supply temperature to avoid resetting the setpoint too low. During times of no-load, or odd conditions such as a negative load, the setpoint is reset to this design setpoint.
+
+\paragraph{Maximum Supply Temperature Setpoint}\label{maximum-supply-temperature-setpoint}
+
+This numeric field is the maximum value to which the supply setpoint can be reset. This ensures that the chilled water temperature does not go too high during reset operations.
+
+\paragraph{Return Temperature Setpoint Input Type}\label{return-temperature-setpoint-input-type}
+
+This alpha field must be one of three strings: ``Constant'', ``Scheduled'', or ``ReturnTemperatureSetpoint''. If the choice is ``Constant'', the constant value in the next field is used as the target return temperature. If the choice is ``Scheduled'', the current value of the schedule named in the following field is used as the target return temperature. If the choice is ``ReturnTemperatureSetpoint'', the actual setpoint temperature on the ``Plant Loop Supply Inlet Node'' specified above is retrieved and used as the target return temperature. This is convenient as a separate setpoint manager could be established to pre-calculate the desired return temperature, and will assign the Setpoint internally. Then when this return temperature manager executes, the setpoint will be updated and utilized.
+
+\paragraph{Return Temperature Setpoint Constant Value}\label{return-temperature-setpoint-constant-value}
+
+If the ``Return Temperature Setpoint Input Type'' field is ``constant'', the numeric value entered here is used as the target return temperature throughout the simulation.
+
+\paragraph{Return Temperature Setpoint Schedule Name}\label{return-temperature-setpoint-schedule-name}
+
+If the ``Return Temperature Setpoint Input Type'' field is ``scheduled'', this alpha field defines the name of a user-defined schedule storing values of return target temperature. The ``current'' value is looked up throughout the simulation. This is especially useful as EMS can be employed to do additional sensing and override the schedule value in a given timestep to a new dynamically-calculated return temperature.
+
+An example idf input for a constant return reset setpoint manager is shown here:
+
+\begin{lstlisting}
+
+SetpointManager:ReturnTemperature:ChilledWater,
+  Main Loop Setpoint Manager, !- Name
+  Supply Outlet Node,      !- Plant Loop Supply Outlet Node
+  Supply Inlet Node,       !- Plant Loop Supply Inlet Node
+  7.0,                     !- Minimum Supply Temperature Setpoint
+  10.0,                    !- Maximum Supply Temperature Setpoint
+  Constant,                !- Return Temperature Setpoint Input Type
+  12.0,                    !- Return Temperature Setpoint Constant Value
+  ;                        !- Return Temperature Setpoint Schedule Name
+\end{lstlisting}
+
+Another example which uses the ``ReturnTemperatureSetpoint'' is shown here with the accompanying setpoint being used to set the setpoint on the return node:
+
+\begin{lstlisting}
+  SetpointManager:Scheduled,
+    Return Temperature Setpoint Manager,  !- Name
+    Temperature,             !- Control Variable
+    Return Temperature Sch,  !- Schedule Name
+    Supply Inlet Node;       !- Setpoint Node or NodeList Name
+\end{lstlisting}
+
+\begin{lstlisting}
+  Schedule:Constant,
+    Return Temperature Sch,  !- Name
+    Any Number,              !- Schedule Limits
+    11.75;                   !- Value
+\end{lstlisting}
+
+\begin{lstlisting}
+  SetpointManager:ReturnTemperature:ChilledWater,
+    Main Loop Setpoint Manager, !- Name
+    Supply Outlet Node,      !- Plant Loop Supply Outlet Node
+    Supply Inlet Node,       !- Plant Loop Supply Inlet Node
+    7.0,                     !- Minimum Supply Temperature Setpoint
+    10.0,                    !- Maximum Supply Temperature Setpoint
+    ReturnTemperatureSetpoint, !- Return Temperature Setpoint Input Type
+    ,                        !- Return Temperature Setpoint Constant Value
+    ;                        !- Return Temperature Setpoint Schedule Name
+\end{lstlisting}
+
+\subsection{SetpointManager:ReturnTemperature:HotWater}\label{setpointmanagerreturntemperaturehotwater}
+
+This setpoint manager allows for the central plant simulation in EnergyPlus to target a specific return water temperature entering the plant supply equipment. This setpoint manager is specifically for ``hot water'' (although it could be any fluid) applications. This setpoint manager senses the current supply and return temperatures, calculates the current demand on the loop, and assuming this load remains constant for this time step, it predicts what supply set-point temperature would provide the desired target return temperature.
+
+Because this is predictive, and the setpoint is only updated once per system timestep (frequency of the call to ManageSetPoints), the longer the time step, the less accurate the prediction will be. To make tighter control, the time step can be reduced down even to one minute. However, as described in the EngineeringReference, for most realistic building profiles the control works quite well under normal timestep size. If your load profile is highly jagged with step changes in demand, a smaller timestep could help achieve tight control.
+
+\subsubsection{Inputs}\label{inputs-27-001}
+
+\paragraph{Field: Name}\label{field-name-28-000}
+
+This alpha field is a unique, user-assigned name for an instance of a hot water return temperature reset setpoint manager.
+
+\paragraph{Plant Loop Supply Outlet Node}\label{plant-loop-supply-outlet-node-1}
+
+This alpha field is the name of the plant loop supply side outlet node for the plant being managed by this setpoint manager. The current temperature of this node is sensed in order to calculate current loop demand. This node is typically also where the plant loop setpoint is specified, but not necessarily. This setpoint manager looks up the actual setpoint node from the PlantLoop internal data structures as it is specified on the PlantLoop object. If the plant loop setpoint is on a different node than the supply outlet node, the loop may not maintain return temperature control as expected.
+
+\paragraph{Plant Loop Supply Inlet Node}\label{plant-loop-supply-inlet-node-1}
+
+This alpha field is the name of the plant loop supply side inlet node whose temperature is controlled using this setpoint manager by resetting the supply setpoint temperature. The current temperature of this node is also sensed in order to calculate current loop demand.
+
+\paragraph{Minimum Supply Temperature Setpoint}\label{minimum-supply-temperature-setpoint-1}
+
+This numeric field is the minimum value to which the supply setpoint can be reset. This ensures that the hot water temperature does not go too low during reset operations.
+
+\paragraph{Maximum Supply Temperature Setpoint}\label{maximum-supply-temperature-setpoint-1}
+
+This numeric field plays multiple roles. During initialization, such as before the plant data structures are fully established, this is used as the default plant supply setpoint temperature. During normal calculation, this is used as the maximum hot water supply temperature to avoid resetting the setpoint too high. During times of no-load, or odd conditions such as a negative load, the setpoint is reset to this design setpoint.
+
+\paragraph{Return Temperature Setpoint Input Type}\label{return-temperature-setpoint-input-type-1}
+
+This alpha field must be one of three strings: ``Constant'', ``Scheduled'', or ``ReturnTemperatureSetpoint''. If the choice is ``Constant'', the constant value in the next field is used as the target return temperature. If the choice is ``Scheduled'', the current value of the schedule named in the following field is used as the target return temperature. If the choice is ``ReturnTemperatureSetpoint'', the actual setpoint temperature on the ``Plant Loop Supply Inlet Node'' specified above is retrieved and used as the target return temperature. This is convenient as a separate setpoint manager could be established to pre-calculate the desired return temperature, and will assign the Setpoint internally. Then when this return temperature manager executes, the setpoint will be updated and utilized.
+
+\paragraph{Return Temperature Setpoint Constant Value}\label{return-temperature-setpoint-constant-value-1}
+
+If the ``Return Temperature Setpoint Input Type'' field is ``constant'', the numeric value entered here is used as the target return temperature throughout the simulation.
+
+\paragraph{Return Temperature Setpoint Schedule Name}\label{return-temperature-setpoint-schedule-name-1}
+
+If the ``Return Temperature Setpoint Input Type'' field is ``scheduled'', this alpha field defines the name of a user-defined schedule storing values of return target temperature. The ``current'' value is looked up throughout the simulation. This is especially useful as EMS can be employed to do additional sensing and override the schedule value in a given timestep to a new dynamically-calculated return temperature.
+
+An example idf input for a scheduled return reset setpoint manager is shown here:
+
+\begin{lstlisting}
+
+SetpointManager:ReturnTemperature:HotWater,
+  Main Loop Setpoint Manager, !- Name
+  Supply Outlet Node,      !- Plant Loop Supply Outlet Node
+  Supply Inlet Node,       !- Plant Loop Supply Inlet Node
+  57.0,                    !- Minimum Supply Temperature Setpoint
+  60.0,                    !- Maximum Supply Temperature Setpoint
+  Scheduled,               !- Return Temperature Setpoint Input Type
+  ,                        !- Return Temperature Setpoint Constant Value
+  ReturnTempSchedule;      !- Return Temperature Setpoint Schedule Name
+
+  Schedule:Compact,
+  ReturnTempSchedule,  !- Name
+  Any Number,              !- Schedule Type Limits Name
+  THROUGH: 12/31,          !- Field 1
+  FOR: AllDays,            !- Field 2
+  UNTIL: 12:00, 55,        !- Field 3
+  UNTIL: 17:00, 53,        !- Field 3
+  UNTIL: 24:00, 55;        !- Field 3
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-simulation-parameters.tex b/doc/input-output-reference/src/overview/group-simulation-parameters.tex
new file mode 100644
index 00000000000..55a156a2ffa
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+++ b/doc/input-output-reference/src/overview/group-simulation-parameters.tex
@@ -0,0 +1,926 @@
+\section{Group -- Simulation Parameters}\label{group-simulation-parameters}
+
+This group of objects influences the simulation in various ways.
+
+\subsection{Version}\label{version}
+
+\subsubsection{Inputs}\label{inputs-044}
+
+\paragraph{Field: Version Identifier}\label{field-version-identifier}
+
+The Version object allows you to enter the proper version that your IDF was created for. This is checked against the current version of EnergyPlus and a Severe error issued (non-terminating) if it does not match the current version string. Note that versions are often significant and there is no guarantee that the older file will run in the newer versions of the program. See IDF Version Updater (Auxiliary Programs Document) for methods of changing the older files to newer versions.
+
+\subsection{Timestep}\label{timestep}
+
+\subsubsection{Inputs}\label{inputs-1-041}
+
+\paragraph{Field: Number of Timesteps per Hour}\label{field-number-of-timesteps-per-hour}
+
+The Timestep object specifies the ``basic'' timestep for the simulation. The value entered here is usually known as the Zone Timestep. This is used in the Zone Heat Balance Model calculation as the driving timestep for heat transfer and load calculations. The value entered here is the number of timesteps to use within an hour. Longer length timesteps have lower values for Number of Timesteps per Hour. For example a value of 6 entered here directs the program to use a zone timestep of 10 minutes and a value of 60 means a 1 minute timestep. The user's choice for Number of Timesteps per Hour must be evenly divisible into 60; the allowable choices are 1, 2, 3, 4, 5, 6, 10, 12, 15, 20, 30, and 60.
+
+The choice made for this field has important implications for modeling accuracy and the overall time it takes to run a simulation. Here are some considerations when choosing a value:
+
+\begin{itemize}
+\item
+  The solution technique used in EnergyPlus has been designed to be stable with zone timesteps of up to sixty minutes (Number Timesteps in Hour = 1). However, 60 minutes is considered a ``long'' timestep and it should only be used in rare occasions where there is no HVAC system, accuracy is not a concern, and short run times are critical. Such long timesteps are not recommended to use because simulation results are more accurate for shorter timesteps, of say 10 minutes or less (Number of Timesteps per Hour of 6 or more). Shorter zone timesteps improve the numerical solution of the Zone Heat Balance Model because they improve how models for surface temperature and zone air temperature are coupled together. Longer timesteps introduce more lag and lead to more a dampened dynamic response.
+\item
+  Simulation run time increases with shorter timesteps or larger values for Number of Timesteps per Hour. The effect varies with the nature of the model. The user can test out different values on their particular model to understand the implications for his or her particular case. Sometimes large models with multizone HVAC and Plant systems execute nearly as fast with 15 minute timesteps as with 60 minute timesteps because fewer iterations are required in the system modeling since the prior timestep's results are close to the final outcome of next timestep.
+\item
+  The weather data files usually have 60-minute (or hourly) data. However, it does not follow that this should be used as the basis for choosing the zone timestep because:
+\item
+  EnergyPlus carefully interpolates the weather data between data points for use at shorter timesteps. This is discussed in a later section: Weather Data Hourly Interpolation
+\item
+  Many aspects of a model have time scales that differ from the that of the weather data. A goal of the modeling is to predict how the building will respond to the weather. However, the building's response is not \emph{governed} by the time scale that the weather data are available at, but rather the time scales of the dynamic performance of the thermal envelope as well as things like schedules for internal gains, thermostats, and equipment availability.
+\item
+  If the model will include calculating the cost of electricity, then the user should be aware that many electric utility tariffs base charges on demand windows of a specified length of time. If the choice of Number of Timesteps per Hour is not consistent with the demand window, then unexpected results may be obtained. For reasonable prediction of the maximum rates for electricity use for in calculating demand charges, the length of the zone timestep needs to be consistent with the tariff's demand window. The following table lists what values are consistent with various demand windows.
+\end{itemize}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Demand Window & Applicable Number of Timesteps per Hour \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Demand Window & Applicable Number of Timesteps per Hour \tabularnewline
+\midrule
+\endhead
+
+QuarterHour & 4, 12, 20, or 60 \tabularnewline
+HalfHour & 2, 4, 6, 10, 12, 20, 30, or 60 \tabularnewline
+FullHour, Day, Week & Any \tabularnewline
+\bottomrule
+\end{longtable}
+
+There is also second type of timestep inside EnergyPlus that is known as the System Timestep. This is a variable-length timestep that governs the driving timestep for HVAC and Plant system modeling. The user cannot directly control the system timestep (except by use of the ConvergenceLimits object). When the HVAC portion of the simulation begins its solution for the current zone timestep, it uses the zone timestep as its maximum length but then can reduce the timestep, as necessary, to improve the solution.  The technical details of the approach are explained in the Engineering Documentation under ``Integrated Solution Manager''.
+
+Users can see the system timestep used if they select the ``detailed'' frequency option on an HVAC output variable (e.g. Zone Air Temperature). To contrast, the ``Zone'' variables will only be reported on the zone timestep (e.g. Zone Mean Air Temperature).
+
+And, the IDF example:
+
+\begin{lstlisting}
+Timestep, 6;  !- Suggested default for most system simulations
+\end{lstlisting}
+
+Suggested defaults are 4 for non-HVAC simulations, 6 for simulations with HVAC, 20 is the minimum for ConductionFiniteDifference and HeatAndMoistureFiniteElement simulations. Green roof (ref: Material:RoofVegetation) also may require more timesteps.
+
+Note that hourly data (such as outdoor conditions expressed by Design Days or Weather data) are interpolated to the Zone Timestep. This is discussed in a later section: Weather Data Hourly Interpolation
+
+\subsection{ConvergenceLimits}\label{convergencelimits}
+
+This item is an ``advanced'' feature that should be used only with caution. It is specifically included to assist some users ``speed up'' calculations while not overly compromising accuracy. The user must judge for him/herself whether the reduced run time is useful.
+
+\subsubsection{Inputs}\label{inputs-2-038}
+
+\paragraph{Field: Minimum System Timestep}\label{field-minimum-system-timestep}
+
+Usually the minimum system timestep is allowed to vary from the zone timestep (as maximum) to a minimum timestep of 1 minute during certain system calculations. This might be when the system turns on or off, for example. Entering 0 in this field sets the minimum system timestep to be the same as the zone timestep. Otherwise the units of the field are minutes. It's probably a good idea to have any minimum entered be a divisor of the zone timestep.
+
+\paragraph{Field: Maximum HVAC Iterations}\label{field-maximum-hvac-iterations}
+
+The HVAC Manager will iterate to a solution or up to a set number of iterations. If not ``converged'', then a warning error appears:
+
+\begin{lstlisting}
+SimHVAC: Maximum iterations (20) exceeded for all HVAC loops, at CHICAGO IL USA TMY2-94846 WMO# = 725300, 10/07 14:06 - 14:08
+\end{lstlisting}
+
+In order to reduce time used in simulating your building, you may choose to enter a lesser number than the default of 20 for the maximum number of iterations to be used. Or, you may wish to enter a bigger number for certain buildings. To get more information printed with a ``max iteration'' message, you need to enter a ``Output:Diagnostics, DisplayExtraWarnings;'' command (which may also generate other warnings than just this one).
+
+\paragraph{Field: Minimum Plant Iterations}\label{field-minimum-plant-iterations}
+
+The plant system modeling includes a solver that iterates within a single HVAC manager iteration. This input field and the next one provide some control over how the plant solver iterates. This field sets a minimum threshold for plant interations. The default for this field is the value ``2'' which indicates that a minimum of two full plant model interations will be performed every time plant is called by the HVAC manager. For faster performance with simple plant systems, this input field could be set to the value ``1''. For complicated plant systems that present difficulties to solve, this value may need to be set higher to ensure accuracy but at the expense of speed. Complicated plant systems include those with several interconnected loops, sizing miss-matches such that plant components are starved of flow compared to their desired flow, heat recovery systems, and thermal load following onsite generators.
+
+\paragraph{Field: Maximum Plant Iterations}\label{field-maximum-plant-iterations}
+
+The plant system solver iterates within a single HVAC manager iteration. This input field and the previous one provide some control over how the plant model iterates. This field sets a maximum limit for plant interations. The default for this field is the value ``8'' which indicates that the plant solver will exit after having completed eight full iterations. This value can be raised for better accuracy with complex plants or lowered for faster speed with simple plants. The output variable called ``Plant Solver Sub Iteration Count'' (typically reported at the ``detailed'' frequency) is useful for understanding how many plant solver iterations are actually being used during a particular simulation. The lower limit of the value for this field is ``2.''
+
+Use in an IDF:
+
+\begin{lstlisting}
+ConvergenceLimits,
+  0,        !- Minimum System Timestep (0 = same as zone timestep)
+  25,       !- Maximum HVAC Iterations
+  3,        !- Minimum Plant Iterations
+  9;        !- Maximum Plant Iterations
+\end{lstlisting}
+
+\subsection{Building}\label{building}
+
+The Building object describes parameters that are used during the simulation of the building. There are necessary correlations between the entries for this object and some entries in the Site:WeatherStation and Site:HeightVariation objects, specifically the Terrain field.
+
+\subsubsection{Inputs}\label{inputs-3-034}
+
+\paragraph{Field: Building Name}\label{field-building-name}
+
+Building name is specified for output convenience.
+
+\paragraph{Field: North Axis}\label{field-north-axis}
+
+The Building North Axis is specified \textbf{relative to true North}. Buildings frequently do not line up with true north. For convenience, one may enter surfaces in a ``regular'' coordinate system and then shift them via the use of the North Axis. The value is specified in degrees from ``true north'' (clockwise is positive).
+
+The figure below shows how the building north axis can be rotated to correspond with one of the major axes of an actual building. The relevance of this field is described more completely under ``GlobalGeometryRules''; in particular, the value of ``North Axis'' is \emph{ignored} if a coordinate system other than ``relative'' is used.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image001.png}
+\caption{Illustration of Building North Axis \protect \label{fig:illustration-of-building-north-axis}}
+\end{figure}
+
+\paragraph{Field: Terrain}\label{field-terrain}
+
+The site's terrain affects how the wind hits the building -- as does the building height. In addition, the external conduction method usually has its own parameters for the calculation. Please see the Engineering Documentation, External Conduction section for particulars. The legal values for this field are shown in the following table.
+
+% table 1
+\begin{longtable}[c]{@{}ll@{}}
+\caption{Values for ``Terrain'' \label{table:values-for-terrain}} \tabularnewline
+\toprule 
+Terrain Type Value & Terrain Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Values for ``Terrain''} \tabularnewline
+\toprule 
+Terrain Type Value & Terrain Description \tabularnewline
+\midrule
+\endhead
+
+Country & Flat, Open Country \tabularnewline
+Suburbs & Rough, Wooded Country, Suburbs \tabularnewline
+City & Towns, city outskirts, center of large cities \tabularnewline
+Ocean & Ocean, Bayou flat country \tabularnewline
+Urban & Urban, Industrial, Forest \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Warmup Convergence}\label{warmup-convergence}
+
+The following two fields along with the minimum and maximum number of warmup days (also in this object) define the user specified criteria for when EnergyPlus will ``converge'' at each environment (each sizing period or run period set as Yes in the SimulationControl object). EnergyPlus ``runs'' the first day of the environment (starting with a set of hard-coded initial conditions: temperatures are initialized to 23C and zone humidity ratios are initialized to the outdoor humidity ratio) until the loads/temperature convergence tolerance values are satisfied (next two fields) or until it reaches ``maximum number of warmup days''. Note that setting the convergence tolerance values too loose will cause the program to be satisifed too early and you may not get the results you expect from the actual simulation.
+
+\paragraph{Field: Loads Convergence Tolerance Value}\label{field-loads-convergence-tolerance-value}
+
+This value represents the number at which the loads values must agree before ``convergence'' is reached. Loads tolerance value is a fraction of the load.
+
+\paragraph{Field: Temperature Convergence Tolerance Value}\label{field-temperature-convergence-tolerance-value}
+
+This value represents the number at which the zone temperatures must agree (from previous iteration) before ``convergence'' is reached. (Units for this field is delta C).
+
+Convergence of the simultaneous heat balance/HVAC solution is reached when either the loads or temperature criterion is satisfied.
+
+All tolerances have units so the temperature tolerance is in degrees C (or degrees K) and the loads tolerance is in Watts. Both tolerances work the same way, just one looks at temperatures and one looks at heating and cooling loads. After the second warm-up day, the program compares the maximum temperature experienced in a space with the maximum temperature from the previous day. If those two temperatures are within the tolerance, then it has passed the first warm-up check.
+
+It does a similar comparison with lowest temperatures experience within all the zones. If the current simulation day and the previous day values are within the tolerance, then it has passed the second warm-up check. Similar things are done with the loads tolerance and the maximum heating and cooling loads that are experienced within the spaces. Those are compared individually to the values for the previous day. If they are both in tolerance, then the simulation has passed the third and fourth warm-up check. The simulation stays in the warm-up period until ALL FOUR checks have been passed. See Engineering Reference and Output Details document for further explanation and outputs.
+
+Please note--other ``convergence tolerance'' inputs are required for certain HVAC equipment (unit ventilator, unit heater, window AC, etc.). The purpose and units of these parameters are different from ``load convergence tolerance'' and ``temperature convergence tolerance'' in the BUILDING object.
+
+\paragraph{Field: Solar Distribution}\label{field-solar-distribution}
+
+Setting this value determines how EnergyPlus treats beam solar radiation and reflectances from exterior surfaces that strike the building and, ultimately, enter the zone. There are five choices: \textbf{MinimalShadowing}, \textbf{FullExterior} and \textbf{FullInteriorAndExterior, FullExteriorWithReflections, FullInteriorAndExteriorWithReflections}.
+
+\textbf{MinimalShadowing}
+
+In this case, there is no exterior shadowing except from window and door reveals. All beam solar radiation entering the zone is assumed to fall on the floor, where it is absorbed according to the floor's solar absorptance. Any reflected by the floor is added to the transmitted diffuse radiation, which is assumed to be uniformly distributed on all interior surfaces. If no floor is present in the zone, the incident beam solar radiation is absorbed on all interior surfaces according to their absorptances. The zone heat balance is then applied at each surface and on the zone's air with the absorbed radiation being treated as a flux on the surface.
+
+\textbf{FullExterior, FullExteriorWithReflections}
+
+In this case, shadow patterns on exterior surfaces caused by detached shading, wings, overhangs, and exterior surfaces of all zones are computed. As for MinimalShadowing, shadowing by window and door reveals is also calculated. Beam solar radiation entering the zone is treated as for MinimalShadowing -- All beam solar radiation entering the zone is assumed to fall on the floor, where it is absorbed according to the floor's solar absorptance. Any reflected by the floor is added to the transmitted diffuse radiation, which is assumed to be uniformly distributed on all interior surfaces. If no floor is present in the zone, the incident beam solar radiation is absorbed on all interior surfaces according to their absorptances. The zone heat balance is then applied at each surface and on the zone's air with the absorbed radiation being treated as a flux on the surface.
+
+\textbf{FullInteriorAndExterior, FullInteriorAndExteriorWithReflections}
+
+This is the same as FullExterior except that instead of assuming all transmitted beam solar falls on the floor the program calculates the amount of beam radiation falling on each surface in the zone, including floor, walls and windows, by projecting the sun's rays through the exterior windows, taking into account the effect of exterior shadowing surfaces and window shading devices.
+
+If this option is used, you should be sure that the surfaces of the zone totally enclose a space. This can be determined by viewing the \textbf{eplusout.dxf} file with a program like AutoDesk's Volo View Express. You should also be sure that the zone is \textbf{convex}. Examples of convex and non-convex zones are shown in Figure~\ref{fig:illustration-of-convex-and-non-convex-zones}. The most common non-convex zone is an L-shaped zone. (A formal definition of convex is that any straight line passing through the zone intercepts at most two surfaces.) If the zone's surfaces do not enclose a space or if the zone is not convex you should use Solar Distribution = \textbf{FullExterior} instead of \textbf{FullInteriorAndExterior}.
+
+If you use \textbf{FullInteriorAndExterior} the program will also calculate how much beam radiation falling on the inside of an exterior window (from other windows in the zone) is absorbed by the window, how much is reflected back into the zone, and how much is transmitted to the outside. In this calculation the effect of a shading device, if present, is accounted for.
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image002.png}
+\caption{Illustration of Convex and Non-convex Zones \protect \label{fig:illustration-of-convex-and-non-convex-zones}}
+\end{figure}
+
+\textbf{Reflection calculations}
+
+Note: Using the reflection calculations can be very time-consuming. Even error-prone. As a possible alleviation, you can use the Output:Diagnostics,DoNotMirrorDetachedShading; in many cases to get past a fatal error.
+
+If using reflections, the program calculates beam and sky solar radiation that is reflected from exterior surfaces and then strikes the building. These reflecting surfaces fall into three categories:
+
+1) \textbf{Shadowing surfaces}. These are surfaces like overhangs or neighboring buildings entered with Shad\-ing:\-Site, Shad\-ing:\-Build\-ing, Shad\-ing:\-Site:\-Detailed, Shad\-ing:\-Build\-ing:\-Detailed, Shad\-ing:\-Over\-hang, Shad\-ing:\-Over\-hang:Pro\-jection, Shad\-ing:\-Fin, Shad\-ing:\-Fin:\-Pro\-jection or Shad\-ing:\-Zone:\-Detailed objects. See Figure~\ref{fig:solar-reflection-from-shadowing-surfaces.}.
+
+These surfaces can have diffuse and/or specular (beam-to-beam) reflectance values that are specified with the Shad\-ing\-Property:\-Re\-flectance object which specifies those parameters. They have a default value of .2 for both visible and diffuse reflection.
+
+2) \textbf{Exterior building surfaces}. In this case one section of the building reflects solar radiation onto another section (and vice-versa). See Figure~\ref{fig:solar-reflection-from-building-surfaces-onto}.
+
+The building surfaces are assumed to be diffusely reflecting if they are opaque (walls, for example) and specularly reflecting if they are windows or glass doors. The reflectance values for opaque surfaces are calculated by the program from the Solar Absorptance and Visible Absorptance values of the outer material layer of the surface's construction (ref: Material object properties). The reflectance values for windows and glass doors are calculated by the program from the reflectance properties of the individual glass layers that make up surface's construction assuming no shading device is present and taking into account inter-reflections among the layers (ref: Window Properties).
+
+3) \textbf{The ground surface}. Reflection from the ground is calculated even if reflections option is not used;l but then the ground plane is considered unobstructed, i.e., the shadowing of the ground by the building itself or by obstructions such as neighboring buildings is ignored. Shadowing by the building itself or neighboring buildings is taken into account when the ``with reflections'' option is used but then the ``view factor to ground'' is NOT used. This is shown in Figure~\ref{fig:shadowing-from-building-affects-beam-solar}.
+
+\begin{figure}[hbtp] % fig 3
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image003.png}
+\caption{  Solar reflection from shadowing surfaces. Solid arrows are beam solar radiation; dashed arrows are diffuse solar radiation. (a) Diffuse reflection of beam solar radiation from the top of an overhang. (b) Diffuse reflection of sky solar radiation from the top of an overhang. (c) Beam-to-beam (specular) reflection from the façade of an adjacent highly-glazed building represented by a vertical shadowing surface. \protect \label{fig:solar-reflection-from-shadowing-surfaces.}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 4
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image004.png}
+\caption{  Solar reflection from building surfaces onto other building surfaces. In this example beam solar reflects from a vertical section of the building onto a roof section. The reflection from the window is specular. The reflection from the wall is diffuse. \protect \label{fig:solar-reflection-from-building-surfaces-onto}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 5
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image005.png}
+\caption{Shadowing from building affects beam solar reflection from the ground. Beam-to-diffuse reflection from the ground onto the building occurs only for sunlit areas, A and C, not from shaded area, B. \protect \label{fig:shadowing-from-building-affects-beam-solar}}
+\end{figure}
+
+\paragraph{Field: Maximum Number of Warmup Days}\label{field-maximum-number-of-warmup-days}
+
+This field specifies the number of ``warmup'' days that might be used in the simulation before ``convergence'' is achieved. The default number, 25, is usually more than sufficient for this task; however, some complex buildings (with complex constructions) may require more days. If you enter less than 25 as a maximum, that is the number of maximum warmup days that will be used. An error message will occur when the simulation ``runs'' out of days and has not converged:
+
+\begin{lstlisting}
+CheckWarmupConvergence: Loads Initialization, Zone = "MAIN ZONE" did not converge after 30 warmup days.
+See Warmup Convergence Information in .eio file for details
+..Environment(SizingPeriod) = "DENVER CENTENNIAL  GOLDEN   N ANN CLG 1% CONDNS DB = >MWB"
+..Max Temp Comparison = 2.06E-002 vs Temperature Convergence Tolerance = 0.50 – Pass Convergence
+..Min Temp Comparison = 5.95E-003 vs Temperature Convergence Tolerance = 0.50 – Pass Convergence
+..Max Cool Load Comparison = 9.5082E-002 vs Loads Convergence Tolerance = 5.00E-002 – Fail Convergence
+\end{lstlisting}
+
+As noted in the message, there will be more information in the .eio file. (Refer to Output Details document as well for examples.)
+
+You may be able to increase the Maximum Number of Warmup Days and get convergence, but some anomalous buildings may still not converge. Simulation proceeds for x warmup days until ``convergence'' is reached (see the discussion under the Temperature Convergence Tolerance Value field in this object, just above).
+
+\paragraph{Field: Minimum Number of Warmup Days}\label{field-minimum-number-of-warmup-days}
+
+This field specifies the minimum number of ``warmup'' days before EnergyPlus will check if it has achieved convergence and can thus start simulating the particular environment (design day, annual run) in question. Research into the minimum number of warmup days indicates that 6 warmup days is generally enough on the minimum end of the spectrum to avoid false predictions of convergence and thus to produce enough temperature and flux history to start EnergyPlus simulation. This was based on a study that used the benchmark reference buildings. It also was observed that convergence performance improved when the number of warmup days increased. As a result, the default value for the minimum warmup days has been set to 6. Users should decrease this number only if they have knowledge that a specific file converges more quickly than 6 days. Users may wish to increase the value in certain situations when, based on the output variables described in the Output Details document, it is determined that EnergyPlus has not converged. While this parameter should be less than the previous parameter, a value greater than the value entered in the field ``Maximum Number of Warmup Days'' above may be used when users wish to increase warmup days more than the previous field. In this particular case, the previous field will be automatically reset to the value entered in this field and EnergyPlus will run exactly the number of warmup days specified in this field.
+
+An example from an IDF:
+
+\begin{lstlisting}
+
+Building,
+    PSI HOUSE DORM AND OFFICES,  !- Name
+    36.87000,               !- North Axis {deg}
+    Suburbs,                !- Terrain
+    0.04,                   !- Loads Convergence Tolerance Value
+    0.4000000,              !- Temperature Convergence Tolerance Value {deltaC}
+    FullInteriorAndExterior, !- Solar Distribution
+    40,                     !- Maximum Number of Warmup Days
+    6;                      !- Minimum Number of Warmup Days
+\end{lstlisting}
+
+\subsection{SurfaceConvectionAlgorithm:Inside}\label{surfaceconvectionalgorithminside}
+
+This input object is used control the choice of models used for surface convection at the inside face of all the heat transfer surfaces in the model. This object sets the selection for convection correlations in a global way. The Zone Inside Convection Algorithm input field in the Zone object may be used to selectively override this value on a zone-by-zone basis. Further, individual surfaces can refine the choice by each surface or surface lists -- see object SurfaceProperty:ConvectionCoefficients and object SurfaceProperty:ConvectionCoefficients:MultipleSurface.
+
+\subsubsection{Inputs}\label{inputs-4-031}
+
+\paragraph{Field: Algorithm}\label{field-algorithm-000}
+
+The model specified in this field is the default algorithm for the inside face all the surfaces.. The key choices are \textbf{Simple}, \textbf{TARP}, \textbf{CeilingDiffuser}, and \textbf{AdaptiveConvectionAlgorithm}.
+
+The \textbf{Simple} model applies constant heat transfer coefficients depending on the surface orientation.
+
+The \textbf{TARP} model correlates the heat transfer coefficient to the temperature difference for various orientations. This model is based on flat plate experiments.
+
+The \textbf{CeilingDiffuser} model is a mixed and forced convection model for ceiling diffuser configurations. The model correlates the heat transfer coefficient to the air change rate for ceilings, walls and floors. These correlations are based on experiments performed in an isothermal room with a cold ceiling jet. To avoid discontinuities in surface heat transfer rate calculations, all of correlations have been extrapolated beyond the lower limit of the data set (3 ACH) to a natural convection limit that is applied during the hours when the system is off.
+
+The \textbf{AdaptiveConvectionAlgorithm} model is an dynamic algorithm that organizes a large number of different convection models and automatically selects the one that best applies. The adaptive convection algorithm can also be customized using the SurfaceConvectionAlgorithm:Inside:AdaptiveModelSelections input object. These models are explained in detail in the EnergyPlus Engineering Reference Document.
+
+The default is \textbf{TARP}.
+
+IDF Example:
+
+\begin{lstlisting}
+
+SurfaceConvectionAlgorithm:Inside,TARP;
+\end{lstlisting}
+
+\subsection{SurfaceConvectionAlgorithm:Outside}\label{surfaceconvectionalgorithmoutside}
+
+Various exterior convection models may be selected for global use. The optional Zone Outside Convection Algorithm input field in the Zone object may be used to selectively override this value on a zone-by-zone basis. Further, individual surfaces can refine the choice by each surface or surface lists -- see object SurfaceProperty:ConvectionCoefficients and object SurfaceProperty:ConvectionCoefficients:MultipleSurface.
+
+\subsubsection{Inputs}\label{inputs-5-028}
+
+\paragraph{Field: Algorithm}\label{field-algorithm-1-000}
+
+The available key choices are \textbf{SimpleCombined}, \textbf{TARP}, \textbf{MoWiTT}, \textbf{DOE-2}, and \textbf{AdaptiveConvectionAlgorithm}.
+
+The \textbf{Simple} convection model applies heat transfer coefficients depending on the roughness and windspeed. This is a combined heat transfer coefficient that includes radiation to sky, ground, and air. The correlation is based on Figure~\ref{fig:schematic-of-the-energyplus-unitary-system}, Page 25.1 (Thermal and Water Vapor Transmission Data), 2001 ASHRAE Handbook of Fundamentals. Note that if \textbf{Simple} is chosen here or in the Zone field and a SurfaceProperty:ConvectionCoefficients object attempts to override the caulcation with a different choice, the action will still be one of combined calculation. To change this, you must select one of the other methods for the global default.
+
+All other convection models apply heat transfer coefficients depending on the roughness, windspeed, and terrain of the building's location. These are \emph{convection only} heat transfer coefficients; radiation heat transfer coefficients are calculated automatically by the program.
+
+The \textbf{TARP} algorithm was developed for the TARP software and combines natural and wind-driven convection correlations from laboratory measurements on flat plates.
+
+The \textbf{DOE-2} and \textbf{MoWiTT} were derived from field measurements. DOE-2 uses a correlation from measurements by Klems and Yazdanian for rough surfaces. MoWitt uses a correlation from measurements by Klems and Yazdanian for smooth surfaces and, therefore, is most appropriate for windows (see SurfaceProperty:ConvectionCoefficients:MultipleSurface for how to apply to only windows).
+
+The \textbf{AdaptiveConvectionAlgorithm} model is an dynamic algorithm that organizes a large number of different convection models and automatically selects the one that best applies. The adaptive convection algorithm can also be customized using the SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections input object. All algorithms are described more fully in the Engineering Reference.
+
+The default is \textbf{DOE-2}.
+
+Note that when the surface is wet (i.e. it is raining and the surface is exposed to wind) then the convection coefficient appears as a very large number (1000) and the surface is exposed to the Outdoor Wet-bulb Temperature rather than the Outdoor Dry-bulb Temperature.
+
+IDF Example:
+
+\begin{lstlisting}
+
+SurfaceConvectionAlgorithm:Outside, AdaptiveConvectionAlgorithm;
+\end{lstlisting}
+
+\subsection{HeatBalanceAlgorithm}\label{heatbalancealgorithm}
+
+The HeatBalanceAlgorithm object provides a way to select what type of heat and moisture transfer algorithm will be used for calculating the performance of the building's surface assemblies. This input controls the overall algorithm used for all the surfaces unless one or more of the SurfaceProperty:HeatTransferAlgorithm:* objects are used to alter the selection for particular surfaces.
+
+\subsubsection{Inputs}\label{inputs-6-025}
+
+\paragraph{Field: Algorithm}\label{field-algorithm-2-000}
+
+Four values are allowed to select which solution will be used.
+
+\begin{itemize}
+\item
+  The \textbf{ConductionTransferFunction} selection is a sensible heat only solution and does not take into account moisture storage or diffusion in the construction elements.
+\item
+  The \textbf{MoisturePenetrationDepthConductionTransferFunction} selection is a sensible heat diffusion and an inside surface moisture storage algorithm that also needs additional moisture material property information. Sometimes, this is referred to as the Effective Moisture Penetration Depth or EMPD. See the moisture material property object for additional information and description of outputs:
+\item
+  MaterialProperty:MoisturePenetrationDepth:Settings
+\item
+  \textbf{Advanced/Research usage:}The \textbf{ConductionFiniteDifference} selection is a sensible heat only solution and does not take into account moisture storage or diffusion in the construction elements. This solution technique uses a 1-D finite difference solution in the construction elements. Outputs for the surfaces are described with the material property objects. The Conduction Finite Difference (aka CondFD) property objects are:
+\item
+  MaterialProperty:PhaseChange
+\item
+  MaterialProperty:VariableThermalConductivity
+\item
+  \textbf{Advanced/Research usage:} The \textbf{CombinedHeatAndMoistureFiniteElement} is a coupled heat and moisture transfer and storage solution. The solution technique uses a one dimensional finite difference solution in the construction elements and requires further materialproperties described in the Heat and Moisture Transfer material properties objects. Outputs from the algorithm are described with these objects. The Heat and Moisture Transfer property objects are:
+\item
+  MaterialProperty:HeatAndMoistureTransfer:Settings
+\item
+  MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm
+\item
+  MaterialProperty:HeatAndMoistureTransfer:Suction
+\item
+  MaterialProperty:HeatAndMoistureTransfer:Redistribution
+\item
+  MaterialProperty:HeatAndMoistureTransfer:Diffusion
+\item
+  MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity
+\end{itemize}
+
+\paragraph{Field: Surface Temperature Upper Limit}\label{field-surface-temperature-upper-limit}
+
+This field is a bit ``advanced''. It should only be used when the simulation fails AND you cannot determine a cause for the failure. That is, you receive an error similar to:
+
+\begin{lstlisting}
+   ** Severe  ** Temperature out of bounds (202.91) for surface = Wall1
+   **   ~~~   ** in Zone = Zone01
+   **   ~~~   **  Occurrence info = NEW YORK CITY NY SUMMER, 07/21 16:00 - 16:01
+   **   ~~~   ** A temperature out of bounds problem can be caused by several things.  The user
+   **   ~~~   ** should check the weather environment, the level of internal gains with respect
+   **   ~~~   ** to the zone, and the thermal properties of their materials among other things.
+   **   ~~~   ** A common cause is a building with no thermal mass -- all materials with
+   **   ~~~   ** Regular-R definitions.
+\end{lstlisting}
+
+And, after careful perusal, you cannot find a solution as suggested in the error description. You may then want to enter a higher number than the default for this field.
+
+\paragraph{Field: Minimum Surface Convection Heat Transfer Coefficient Value}\label{field-minimum-surface-convection-heat-transfer-coefficient-value}
+
+This optional field is used to set an overall minimum for the value of the coefficient for surface convection heat transfer (Hc) in W/m2-K. A minimum is necessary for numerical robustness because some correlations for Hc can result in zero values and create numerical problems. This field can be used to support specialized validation testing to suppress convection heat transfer and to investigate the implications of different minimum Hc values. The default is 0.1.
+
+\paragraph{Field: Maximum Surface Convection Heat Transfer Coefficient Value}\label{field-maximum-surface-convection-heat-transfer-coefficient-value}
+
+This optional field is used to set an overall maximum for the value of the coefficient for surface convection heat transfer (Hc) in W/m2-K. High Hc values are used in EnergyPlus to approximate fixed surface temperature boundary conditions. This field can be used to alter the accepted range of user-defined Hc values.
+
+And, a default IDF example
+
+\begin{lstlisting}
+HeatBalanceAlgorithm,ConductionTransferFunction; ! Solution Algorithm
+\end{lstlisting}
+
+\subsection{HeatBalanceSettings:ConductionFiniteDifference}\label{heatbalancesettingsconductionfinitedifference}
+
+This object is used to control the behavior of the Conduction Finite Difference algorithm for surface heat transfer. The settings are global and affect how the model behaves for all the surfaces.
+
+\subsubsection{Inputs}\label{inputs-7-025}
+
+\paragraph{Field: Difference Scheme}\label{field-difference-scheme}
+
+This field determines the solution scheme used by the Conduction Finite Difference model. There are two options CrankNicholsonSecondOrder and FullyImplicitFirstOrder. The CrankNicholsonSecondOrder scheme is second order in time and may be faster. But it can be unstable over time when boundary conditions change abruptly and severely. The FullyImplicitFirstOrder scheme is first order in time and is more stable over time. But it may be slower. The default is FullyImplicitFirstOrder when ConductionFiniteDifference is selected as the Heat Balance Algorithm.
+
+\paragraph{Field: Space Discretization Constant}\label{field-space-discretization-constant}
+
+This field controls how the model determines spatial discretization, or the count of nodes across each material layer in the construction. The model calculates the nominal distance associated with a node, \(\Delta x\), using
+
+\begin{equation}
+\Delta x = \sqrt {C\alpha \Delta t}
+\end{equation}
+
+Where
+
+\(\alpha\) is the thermal diffusivity of the material layer, in m\(^{2}\)/s
+
+\(\Delta t\) is the length of the timestep in seconds.
+
+\emph{C} is a constant set by this field.
+
+The default is 3. Typical values are from 1 to 3. Lower values for this constant lead to more nodes and finer-grained space discretization.
+
+\paragraph{Field: Relaxation Factor}\label{field-relaxation-factor}
+
+The finite difference solver includes under-relaxation for improved stability for interactions with the other surfaces. This input field can optionally be used to modify the starting value for the relaxation factor. Larger numbers may solve faster, while smaller numbers may be more stable. The default is 1.0. If the program detects numerical instability, it may reduce the value entered here to something lower and more stable.
+
+\paragraph{Field: Inside Face Surface Temperature Convergence Criteria}\label{field-inside-face-surface-temperature-convergence-criteria}
+
+The surface heat balance model at the inside face has a numerical solver that uses a convergence parameter for a maximum allowable differences in surface temperature. This field can optionally be used to modify this convergence criteria. The default value is 0.002 and was selected for stability. Lower values may further increase stability at the expense of longer runtimes, while higher values may decrease runtimes but lead to possible instabilities. The units are in degrees Celsius.
+
+An example IDF object follows.
+
+\begin{lstlisting}
+HeatBalanceSettings:ConductionFiniteDifference,
+  FullyImplicitFirstOrder, !- Difference Scheme
+  3.0,                     !- Space Discretization Constant
+  1.0,                     !- Relaxation Factor
+  0.002;                   !- Inside Face Surface Temperature Convergence Criteria
+\end{lstlisting}
+
+\subsection{ZoneAirHeatBalanceAlgorithm}\label{zoneairheatbalancealgorithm}
+
+The ZoneAirHeatBalanceAlgorithm object provides a way to select what type of solution algorithm will be used to calculate zone air temperatures and humidity ratios. This object is an optional object. If the default algorithm is used, this object is not required in an input file.
+
+\subsubsection{Inputs}\label{inputs-8-023}
+
+\paragraph{Field: Algorithm}\label{field-algorithm-3-000}
+
+Three choices are allowed to select which solution algorithm will be used. The \textbf{ThirdOrderBackwardDifference} selection is the default selection and uses the third order finite difference approximation to solve the zone air energy and moisture balance equations. The \textbf{AnalyticalSolution} selection uses the integration approach to solve the zone air energy and moisture balance equations. The \textbf{EulerMethod} selection uses the first order finite backward difference approximation to solve the zone air energy and moisture balance equations.
+
+And, a default IDF example is shown below:
+
+\begin{lstlisting}
+ZoneAirHeatBalanceAlgorithm, ThirdOrderBackwardDifference; !- Algorithm
+\end{lstlisting}
+
+\subsection{ZoneAirContaminantBalance}\label{zoneaircontaminantbalance}
+
+The ZoneAirContaminantBalance object provides a way to select which contaminant type will be simulated. Although carbon dioxide is not considered as an indoor contaminant but it is used as an indicator of indoor air quality in buildings. From modeling point of view EnergyPlus treats carbon dioxide as a type of contaminant. In addition to carbon dioxide, a generic contaminant type model was also added. This object is optional, only required in the input data file if the user wishes to model contaminant concentration levels as part of their simulation.
+
+\subsubsection{Inputs}\label{inputs-9-021}
+
+\paragraph{Field: Carbon Dioxide Concentration}\label{field-carbon-dioxide-concentration}
+
+Input is Yes or No. The default is No. If Yes, simulation of carbon dioxide concentration levels will be performed. If No, simulation of carbon dioxide concentration levels will not be performed.
+
+\paragraph{Field: Outdoor Carbon Dioxide Schedule Name}\label{field-outdoor-carbon-dioxide-schedule-name}
+
+This field specifies the name of a schedule that contains outdoor air carbon dioxide level values in units of ppm. One source of monthly average CO\(_{2}\) levels in the atmosphere is available at a NOAA ftpsite as .
+
+\paragraph{Field: Generic Contaminant Concentration}\label{field-generic-contaminant-concentration}
+
+Input is Yes or No. The default is No. If Yes, simulation of generic contaminant concentration levels will be performed. If No, simulation of generic contaminant concentration levels will not be performed.
+
+\paragraph{Field: Outdoor Generic Contaminant Schedule Name}\label{field-outdoor-generic-contaminant-schedule-name}
+
+This field specifies the name of a schedule that contains outdoor air generic contaminant level values in units of ppm.
+
+An IDF example:
+
+\begin{lstlisting}
+ZoneAirContaminantBalance,
+  Yes,                          !- Carbon Dioxide Concentration
+  Outdoor CO2 Schedule,         !- Outdoor Carbon Dioxide Schedule Name
+  Yes,                          !- Generic Contaminant Concentration
+  Generic Contaminant Schedule; !- Outdoor Generic Contaminant Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-033}
+
+The following output variables are available when Carbon Dioxide Concentration = Yes.
+
+\begin{lstlisting}
+HVAC,Average,Zone Air CO2 Internal Gain Volume Flow Rate
+HVAC,Average,Zone Air CO2 Concentration [ppm]
+\end{lstlisting}
+
+\paragraph{Zone Air CO2 Concentration {[}ppm{]}}\label{zone-air-co2-concentration-ppm}
+
+This output variable represents the carbon dioxide concentration level in parts per million (ppm) for each zone. This is calculated and reported from the Correct step in the Zone Air Contaminant Predictor-Corrector module.
+
+\paragraph{Zone Air CO2 Internal Gain Volume Flow Rate {[}m3/s{]}}\label{zone-air-co2-internal-gain-volume-flow-rate-m3s}
+
+This is the rate of carbon dioxide added to a zone from all types of sources or sinks, in m\(^{3}\)/s.
+
+\subsubsection{Outputs}\label{outputs-1-024}
+
+The following output variable is available when Generic Contaminant Concentration = Yes.
+
+HVAC,Average,Zone Generic Air Contaminant Generation Volume Flow Rate {[}m3/s{]}
+
+HVAC,Average,Zone Air Generic Air Contaminant Concentration {[}ppm{]}
+
+\paragraph{Zone Air Generic Air Contaminant Concentration {[}ppm{]}}\label{zone-air-generic-air-contaminant-concentration-ppm}
+
+This output variable represents the generic contaminant concentration level in parts per million (ppm) for each zone. This is calculated and reported from the Correct step in the Zone Air Contaminant Predictor-Corrector module.
+
+\paragraph{Zone Generic Air Contaminant Generation Volume Flow Rate {[}m3/s{]}}\label{zone-generic-air-contaminant-generation-volume-flow-rate-m3s}
+
+This is the rate of generic air contaminant added (or subtracted) to a zone from all types of sources or sinks.
+
+\subsection{ShadowCalculation}\label{shadowcalculation}
+
+This object is used to control some details of EnergyPlus's solar, shadowing and daylighting models. There are two basic methods available for the calculations. In order to speed up the calculations, shadowing calculations (sun position, etc.) for the default method are performed over a period of days. Note that this value may be very important for determining the amount of sun entering your building and by inference the amount of cooling or heating load needed for maintaining the building. Though termed ``shadowing'' calculations, it in affect determines the sun position for a particular day in a weather file period simulation. (Each design day will use the date of the design day object). Even though weather file data contains the amount of solar radiation, the internal calculation of sun position will govern how that affects various parts of the building. By default, the calculations are done for every 20 days throughout a weather run period; an average solar position is chosen and the solar factors (such as sunlit areas of surfaces) remain the same for that number of days. When more integrated calculations are needed for controlling dynamic windows or shades, a secod method is available where solar calculations are performed at each zone timestep.
+
+\subsubsection{Inputs}\label{inputs-10-019}
+
+\paragraph{Field: Calculation Method}\label{field-calculation-method-000}
+
+This field is used to control how the solar, shading, and daylighting models are calculated with respect to the time of calculations during the simulation. The default and fastest method is selected using the keyword AverageOverDaysInFrequency. A more detailed and slower method can be selected using the keyword DetailedTimestepIntegration. The later method is useful modeling dynamic fenestration and shading surfaces.
+
+\paragraph{Field: Calculation Frequency}\label{field-calculation-frequency}
+
+This numeric field will cause the shadowing calculations to be done periodically using the number in the field as the number of days in each period. This field is only used if the default method AverageOverDaysInFrequency is used in the previous field. Using this field will allow you to synchronize the shadowing calculations with changes in shading devices. Using the default of 20 days in each period is the average number of days between significant changes in solar position angles. For these shadowing calculations, an ``average'' (over the time period) of solar angles, position, equation of time are also used.
+
+\paragraph{Field: Maximum Figures in Shadow Overlap Calculations}\label{field-maximum-figures-in-shadow-overlap-calculations}
+
+This numeric field will allow you to increase the number of figures in shadow overlaps. Due to the shadowing algorithm, the number of shadows in a figure may grow quite large even with fairly reasonable looking structures. Of course, the inclusion of more allowed figures will increase calculation time. Likewise, too few figures may not result in as accurate calculations as you desire.
+
+\paragraph{Field: Polygon Clipping Algorithm}\label{field-polygon-clipping-algorithm}
+
+This is an advanced feature. Prior to V7, the internal polygon clipping method was a special case of the Weiler-Atherton method. Now, two options are available: \textbf{SutherlandHodgman} (default) and \textbf{ConvexWeilerAtherton}. Theoretically, Sutherland-Hodgman is a simpler algorithm but it works well in cases where receiving surfaces (of shadows) are non-convex. The Weiler-Atherton implementation is only accurate where both casting and receiving surfaces are convex. Warnings/severe errors are displayed when necessary. More details on polygon clipping are contained in the Engineering Reference.
+
+\paragraph{Field: Sky Diffuse Modeling Algorithm}\label{field-sky-diffuse-modeling-algorithm}
+
+Two choices are available here: SimpleSkyDiffuseModeling and DetailedSkyDiffuseModeling. \textbf{SimpleSkyDiffuseModeling} (default) performs a one-time calculation for sky diffuse properties. This has implications if you have shadowing surfaces with changing transmittance (i.e. not all opaque or not all transparent) during the year. The program checks to see if this might be the case and automatically selects \textbf{DetailedSkyDiffuseModeling} if the shading transmittance varies. Even if the transmittance doesn't vary and the option for detailed modeling is used, that option is retained (though it will increase execution time) because you may be using EMS to vary the transmittance. When the detailed modeling is done, there will be a warning posted if the Calculation Frequency (above) is \textgreater{} 1.
+
+In general (and you should also read the previous field description), if shadowing surfaces are used with the transmittance property, the user should be careful to synchronize this calculation with the scheduled occurrence of the transmittance (if any) (or use 1, which will be the most accurate but will cause more time in the calculations).
+
+This field applies to the method called ``AverageOverDaysInFrequency.'' When the method called ``DetailedTimestepIntegration'' is used the diffuse sky modeling always uses DetailedSkyDiffuseModeling.
+
+Examples of this object in IDF: (note this object must be unique in an IDF)
+
+\begin{lstlisting}
+ShadowCalculation,AverageOverDaysInFrequency,1;
+
+ShadowCalculation, AverageOverDaysInFrequency, 1, , SutherlandHodgman, DetailedSkyDiffuseModeling;
+\end{lstlisting}
+
+Note that the use of ``1'' in the examples is NOT the same as using DetailedTimestepIntegration -- ``1'' causes daily calculation of the sun position variables but does not change the shadowing calculations more frequently than daily.
+
+\subsection{Output:Diagnostics}\label{outputdiagnostics}
+
+Sometimes, messages only confuse users -- especially new users. Likewise, sometimes certain output variables exist for only a certain condition but some take them at face value/name. Some features may be very important but under certain instances cause problems. Thus, we have added the \textbf{diagnostic output} object to be able to turn on or off certain messages, variables, and features depending on conditions.
+
+Both fields of the Output:Diagnostics command can accept all the applicable keys. More than one object may be entered.
+
+\subsubsection{Inputs}\label{inputs-11-018}
+
+\paragraph{Field: key1, key2}\label{field-key1-key2}
+
+Allowable choices are:
+
+\textbf{DisplayAllWarnings} -- use this to get all warnings (except the developer warnings ``DisplayZoneAirHeatBalanceOffBalance''). This key sets all other display warning values to on.
+
+\textbf{DisplayExtraWarnings} -- use this to get all extra warnings. An example of an extra warning is when a user enters a ceiling height or volume with the Zone object and EnergyPlus calculates something significantly different based on the entered zone geometry.
+
+\textbf{DisplayUnusedSchedules} -- use this to have the unused schedules (by name) listed at the end of the simulation.
+
+\textbf{DisplayUnusedObjects} -- use this to have unused (orphan) objects (by name) listed at the end of the simulation.
+
+\textbf{DisplayAdvancedReportVariables} -- use this to be able to use certain advanced output variables where the name may be misleading and you need to understand the concepts or reasons for use. If you put in this field, then you will be able to report on these features. They are noted in the descriptions of objects or output variables.
+
+\textbf{DisplayZoneAirHeatBalanceOffBalance} -- this is a developer diagnostic which you can turn on, if you desire.
+
+\textbf{DoNotMirrorDetachedShading} -- use this to turn off the automatic mirroring of detached shading surfaces. These surfaces are automatically mirrored so that the user does not need to worry about facing direction of the surface and the shading surface will shade the building as appropriate. Note that Shading:Zone:Detailed surfaces are also mirrored and there is no way to turn that ``off''.
+
+\textbf{DisplayWeatherMissingDataWarnings} -- use this to turn on the missing data warnings from the read of the weather file.
+
+\textbf{ReportDuringWarmup} -- use this to allow reporting during warmup days. This can show you exactly how your facility is converging (or not) during the initial ``warmup'' days of the simulation. Generally, only developers or expert simulation users would need this kind of detail.
+
+\textbf{ReportDetailedWarmupConvergence} -- use this to produce detailed reporting (essentially each warmup day for each zone) for warmup convergence.
+
+\textbf{ReportDuringHVACSizingSimulation} -- use this to allow controlling reporting to SQLite database during sizing period simulations done for HVAC Sizing Simulation. The regular reporting is done in the usual way. This can show details of how advanced sizing adjustments were determined by documenting how the systems operated when doing the intermediate sizing periods. Depending on the number of iterations performed for HVAC Sizing Simulation, there will be a number of sets of results with each set containing all the Sizing Periods.
+
+In IDF use:
+
+\begin{lstlisting}
+Output:Diagnostics,
+  DisplayExtraWarnings;
+\end{lstlisting}
+
+\subsection{Output:DebuggingData}\label{outputdebuggingdata}
+
+There may be times when a particular input file requires additional debugging. The Output:DebuggingData object may be used to report all available node data (e.g., temperature, mass flow rate, set point, pressure, etc.). The debug data is reported to the DBG text file. The debug file first reports the node number and name, and then all available node information for each zone time step (Ref. Timestep).
+
+The 2 fields of the Output:DebuggingData object can accept either a 1 (turn on) or any other value (turn off). Only one object may be entered.
+
+\subsubsection{Inputs}\label{inputs-12-017}
+
+\paragraph{Field: Report Debugging Data}\label{field-report-debugging-data}
+
+This field turns on debug reporting when a value of 1 is entered. Any other value (usually 0) disables debug reporting.
+
+\paragraph{Field: Report During Warmup}\label{field-report-during-warmup}
+
+This field allows the debug data to be reported during the warmup period. When a value of 1 is entered the data is reported at all times, even during warmup. Any other value (usually 0) disables ``reporting at all time'' and debug data is only reported for each environment (RunPeriod or SizingPeriod:DesignDay).
+
+In IDF use:
+
+\begin{lstlisting}
+Output:DebuggingData,
+  1,1;
+\end{lstlisting}
+
+\subsection{Output:PreprocessorMessage}\label{outputpreprocessormessage}
+
+The Output:PreprocessorMessage object can be used by preprocessor programs to EnergyPlus for passing certain conditions/errors that might not be detected by scripts executing the EnergyPlus system of programs. This allows EnergyPlus to intercept problems and terminate gracefully rather than the user having to track down the exact conditions.
+
+There is no reason for a user to enter an Output:PreprocessorMessage object but you should encourage interface developers to use this feature. More than one Output:PreprocessorMessage objects may be entered. Of course, no preprocessor message objects are necessary if there is no error information to be passed.
+
+\subsubsection{Inputs}\label{inputs-13-014}
+
+\paragraph{Field: Preprocessor Name}\label{field-preprocessor-name}
+
+The preprocessor name (e.g. EPMacro, ExpandObjects) is entered here. Case is retained so that messages from EnergyPlus look very similar to what a preprocessor would produce.
+
+\paragraph{Field: Error Severity}\label{field-error-severity}
+
+This is the error severity. If Fatal, EnergyPlus will terminate after showing all preprocessor messages.
+
+\paragraph{Fields: Message Line 1 through Message Line 10}\label{fields-message-line-1-through-message-line-10}
+
+Each line is limited to 100 characters and an appropriate message can be composed.
+
+An IDF Example:
+
+\begin{lstlisting}
+
+Output:PreprocessorMessage,
+     No Preprocessor Used,     !- preprocessor name
+     Information,              !- error severity
+     Illustrative Message,     !- message line 1
+     No problems for processing;  !- message line 2
+\end{lstlisting}
+
+And would appear in output:
+
+\begin{lstlisting}
+Preprocessor = "No Preprocessor Used" has the following Information messages:
+Illustrative Message
+No problems for processing
+\end{lstlisting}
+
+\subsection{ZoneCapacitanceMultiplier:ResearchSpecial}\label{zonecapacitancemultiplierresearchspecial}
+
+This object is an advanced feature that can be used to control the effective storage capacity of the zone. Capacitance multipliers of 1.0 indicate the capacitance is that of the (moist) air in the volume of the specified zone. This multiplier can be increased if the zone air capacitance needs to be increased for stability of the simulation or to allow modeling higher or lower levels of damping of behavior over time. The multipliers are applied to the base value corresponding to the total capacitance for the zone's volume of air at current zone (moist) conditions.
+
+\subsubsection{Inputs}\label{inputs-14-014}
+
+\paragraph{Field: Temperature Capacity Multiplier}\label{field-temperature-capacity-multiplier}
+
+This field is used to alter the effective heat capacitance of the zone air volume. This affects the transient calculations of zone air temperature. Values greater than 1.0 have the effect of smoothing or damping the rate of change in the temperature of zone air from timestep to timestep. Note that sensible heat capacity can also be modeled using internal mass surfaces.
+
+\paragraph{Field: Humidity Capacity Multiplier}\label{field-humidity-capacity-multiplier}
+
+This field is used to alter the effective moisture capacitance of the zone air volume. This affects the transient calculations of zone air humidity ratio. Values greater than 1.0 have the effect of smoothing, or damping, the rate of change in the water content of zone air from timestep to timestep.
+
+\paragraph{Field: Carbon Dioxide Capacity Multiplier}\label{field-carbon-dioxide-capacity-multiplier}
+
+This field is used to alter the effective carbon dioxide capacitance of the zone air volume. This affects the transient calculations of zone air carbon dioxide concentration. Values greater than 1.0 have the effect of smoothing or damping the rate of change in the carbon dioxide level of zone air from timestep to timestep.
+
+\paragraph{Field: Generic Contaminant Capacity Multiplier}\label{field-generic-contaminant-capacity-multiplier}
+
+This field is used to alter the effective generic contaminantcapacitance of the zone air volume. This affects the transient calculations of zone air generic contaminantconcentration. Values greater than 1.0 have the effect of smoothing or damping the rate of change in the generic contaminantlevel of zone air from timestep to timestep.
+
+\subsection{SimulationControl}\label{simulationcontrol}
+
+The input for SimulationControl allows the user to specify what kind of calculations a given EnergyPlus simulation will perform. For instance the user may want to perform one or more of the sizing calculations but not proceed to an annual weather file simulation. Or the user might have all flow rates and equipment sizes already specified and desire an annual weather without any preceding sizing calculations. Sizing runs, even for large projects, are quickly run -- they do not add much to the overall simulation time. The SimulationControl input allows all permutations of run selection by means of 5 yes/no inputs.
+
+\begin{callout}
+Only one SimulationControl object is permitted for each EnergyPlus input file. While a SimulationControl is needed to trigger sizing calculations, it is optional for other runs (design days, run periods). The actions will still be shown in the eplusout.eio file (see Output Details and Examples Document).
+\end{callout}
+
+\subsubsection{Inputs}\label{inputs-15-014}
+
+\paragraph{Field: Do Zone Sizing Calculation}\label{field-do-zone-sizing-calculation}
+
+Input is Yes or No. The default is No. Zone Sizing (see Sizing:Zone object) performs a special calculation, using a theoretical ideal zonal system, and determines the zone design heating and cooling flow rates and loads, saving the results in the zone sizing arrays.
+
+\paragraph{Field: Do System Sizing Calculation}\label{field-do-system-sizing-calculation}
+
+Input is Yes or No. The default is No. System Sizing (see Sizing:System object) also performs a special calculation that, to oversimplify, sums up the results of the zone sizing calculation and saves the results in the system sizing arrays for reporting on component size requirements. Thus, in order to perform the system sizing calculations, the zone sizing arrays need to be filled and hence the zone sizing calculations must be performed in the same run. (This requirement is enforced by the program).
+
+\paragraph{Field: Do Plant Sizing Calculation}\label{field-do-plant-sizing-calculation}
+
+Input is Yes or No. The default is No. Unlike Zone and System Sizing, Plant Sizing does not use the Zone or System sizing arrays. Plant Sizing uses the Sizing:Plant object fields and data on the maximum component flow rates. The data on component (such as coil) flow rates is saved and made available to the Plant code whether or not component autosizing is performed and whether or not zone sizing and/or system sizing is performed. Therefore, you can specify Plant Sizing without also specifying to do Zone Sizing or System Sizing calculations.
+
+\paragraph{Field: Run Simulation for Sizing Periods}\label{field-run-simulation-for-sizing-periods}
+
+Input is Yes or No. The default is Yes. Yes implies that the simulation will be run on all the included SizingPeriod objects (i.e., Sizing\-Period:\-Design\-Day, Sizing\-Period:\-Weather\-File\-Days, and Sizing\-Period:\-Weather\-File\-Condition\-Type). Note that each Sizing\-Period object constitutes an ``environment'' and warmup convergence (see earlier topic under the Building object) will occur for each.
+
+\paragraph{Field: Run Simulation for Weather File Run Periods}\label{field-run-simulation-for-weather-file-run-periods}
+
+Input is Yes or No. The default is Yes. Yes implies the simulation will be run on all the included RunPeriod objects. Note that each RunPeriod object constitutes an ``environment'' and warmup convergence (see earlier topic under the Building object) will occur for each.
+
+\paragraph{Field: Do HVAC Sizing Simulation for Sizing Periods}\label{field-do-hvac-sizing-simulation-for-sizing-periods}
+
+This field is optional. It can be used to enable certain advanced sizing calculations that rely on simulating the sizing periods to collect information. This is currently only applicable when sizing plant loops using the sizing option called Coincident.
+
+\paragraph{Field: Maximum Number of HVAC Sizing Simulation Passes}\label{field-maximum-number-of-hvac-sizing-simulation-passes}
+
+This field is optional and is only used if the previous field is set to Yes. The HVAC Sizing Simulation approach can use iteration to improve sizing calculations. Each iteration is a Sizing Pass. This field is used to manually place an upper limit the number of passes that the sizing algorithms can use.
+
+An IDF example:
+
+\begin{lstlisting}
+SimulationControl,
+  No,                      !- Do Zone Sizing Calculation
+  No,                      !- Do System Sizing Calculation
+  No,                      !- Do Plant Sizing Calculation
+  Yes,                     !- Run Simulation for Sizing Periods
+  Yes,                     !- Run Simulation for Weather File Run Periods
+  No,                      !- Do HVAC Sizing Simulation for Sizing Periods
+  2;                       !- Maximum Number of HVAC Sizing Simulation Passes
+\end{lstlisting}
+
+\subsection{ProgramControl}\label{programcontrol}
+
+This object is currently disabled. The ProgramControl object can be used to control how the EnergyPlus program executes on the computer. Portions of EnergyPlus have been programmed to use more than one processor, or CPU core, at the same time during a single simulation. This multithreading may not be desireable when running more than one simulation at a time on the same computer (because it can actually run more slowly). This input object is optional and allows controlling the number of threads (or cores, or processors) that EnergyPlus will use so that conflicts can be managed. When this object is used, its input for the number of threads will take precedent over the value of the environment variable \textbf{``EP\_OMP\_NUM\_THREADS''} which is an alternate method of controlling the program's threading. Since the primary method for OpenMP simulations currently (V7.1 and V7.2) is the interior radiant exchange to solve for inside surface temperatures, EnergyPlus sets the threads to 1 if the nominal number of surfaces is \textless{} = 30.
+
+\subsubsection{Inputs}\label{inputs-16-010}
+
+\paragraph{Field: Number of Threads Allowed}\label{field-number-of-threads-allowed}
+
+This field is used to specify a limit on the number of threads EnergyPlus will use. If a zero is entered then the program will set the number of threads to the maximum available on the computer. If the number entered is larger than the number of processors or cores, then the hardware limits will take precedent over this limit.
+
+An example IDF object that sets the program to use only one thread follows.
+
+\begin{lstlisting}
+ProgramControl,
+  1; !- Number of Threads Allowed
+\end{lstlisting}
+
+\subsection{Meter:Custom}\label{metercustom}
+
+A custom meter allows the user to group variables or meters onto a virtual meter that can be used just like a normal meter created by EnergyPlus. For consistency, the items being grouped must all be similar.
+
+\subsubsection{Inputs}\label{inputs-17-008}
+
+\paragraph{Field: Name}\label{field-name-043}
+
+This is a user defined name for the custom meter. Names for custom meters cannot duplicate internal meter names.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-004}
+
+A fuel type should be specified for the meter. All assignments to this meter will be checked to assure that the same fuel type is used. Additionally, this may be used in other objects (such as the Demand Limiting). Valid choices for this field are:
+
+\begin{itemize}
+\item
+  Electricity
+\item
+  NaturalGas
+\item
+  PropaneGas
+\item
+  FuelOil\#1
+\item
+  FuelOil\#2
+\item
+  Coal
+\item
+  Diesel
+\item
+  Gasoline
+\item
+  Water
+\item
+  Generic
+\item
+  OtherFuel1
+\item
+  OtherFuel2
+\end{itemize}
+
+Fuel types are generally self-explanatory. Generic is included for convenience when a custom meter is defined that doesn't quite fit the ``fuel'' categories. See the examples below.
+
+\paragraph{Field: group(s) Key Name-Output Variable/Meter Name}\label{field-groups-key-name-output-variablemeter-name}
+
+The rest of the object is filled with parameters of the key name/output variable or meter names. When a meter name is used, the key name field is left blank.
+
+\paragraph{Field: Key Name \#}\label{field-key-name}
+
+A key name field is used when the following field specifies an output variable. If the field is left blank, then all the output variables in the following field are assigned to the meter.
+
+\paragraph{Field: Output Variable or Meter Name \#}\label{field-output-variable-or-meter-name}
+
+This field must be a valid output variable name or a valid meter name.
+
+\subsection{Meter:CustomDecrement}\label{metercustomdecrement}
+
+The decrement custom meter is very similar to the custom meter specification but additionally allows a predefined meter to be used as the ``source'' meter and the remaining items subtract from that predefined meter.
+
+\subsubsection{Inputs}\label{inputs-18-008}
+
+\paragraph{Field: Name}\label{field-name-1-040}
+
+This is a user defined name for the custom meter. Names for custom meters cannot duplicate internal meter names.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-1-003}
+
+A fuel type should be specified for the meter. All assignments to this meter will be checked to assure that the same fuel type is used. Additionally, this may be used in other objects (such as the Demand Limiting). Valid choices for this field are:
+
+\begin{itemize}
+\item
+  Electricity
+\item
+  NaturalGas
+\item
+  PropaneGas
+\item
+  FuelOil\#1
+\item
+  FuelOil\#2
+\item
+  Coal
+\item
+  Diesel
+\item
+  Gasoline
+\item
+  Water
+\item
+  Generic
+\item
+  OtherFuel1
+\item
+  OtherFuel2
+\end{itemize}
+
+\paragraph{Field: Source Meter Name}\label{field-source-meter-name}
+
+This name specifies the meter that will be used as the main source for the decrement custom meter. The remainder of the fields are subtracted from the value of this meter to create the meter value named above. The Source Meter is not changed in any way by including this custom meter.
+
+\paragraph{Field: group(s) Key Name-Output Variable/Meter Name}\label{field-groups-key-name-output-variablemeter-name-1}
+
+The rest of the object is filled with parameters of the key name/output variable or meter names. When a meter name is used, the key name field is left blank.
+
+\paragraph{Field: Key Name \#}\label{field-key-name-1}
+
+A key name field is used when the following field specifies an output variable. If the field is left blank, then all the output variables in the following field are assigned to the meter.
+
+\paragraph{Field: Output Variable or Meter Name \#}\label{field-output-variable-or-meter-name-1}
+
+This field must be a valid output variable name or a valid meter name. Additionally, it must be contained on the Source Meter. Note that, if an error occurs, only the Variable in error will show -- confusing things if what was entered was a meter name.
+
+\subsection{Custom Meter Examples}\label{custom-meter-examples}
+
+Details of the Meter:Custom/Meter:CustomDecrement are shown on the Meter Details file.
+
+In the following examples, the custom meters are set up to illustrate the capabilities of custom meters. Custom meter ``\textbf{MyGeneralLights}'' duplicates the InteriorLights:Electricity meter. Custom meter ``\textbf{MyBuildingElectric}'' duplicates the Electricity:Building meter (by specifying that meter). Custom Meter (Decrement) ``\textbf{MyBuildingOther}'' uses the Electricity:Building meter as the source meter and subtracts out the values for MyGeneralLights (aka InteriorLights:Electricity). The resultant value for the MyBuildingOther meter should be equal to the value for the meters Electricity:Building -- InteriorLights:Electricity.
+
+\begin{lstlisting}
+Meter:Custom,
+  MyGeneralLights,         !- Name
+  Electricity,             !- Fuel Type
+  SPACE1-1,                !- Key Name 1
+  Lights Electric Energy,  !- Output Variable or Meter Name 1
+  SPACE2-1,                !- Key Name 2
+  Lights Electric Energy,  !- Output Variable or Meter Name 2
+  SPACE3-1,                !- Key Name 3
+  Lights Electric Energy,  !- Output Variable or Meter Name 3
+  SPACE4-1,                !- Key Name 4
+  Lights Electric Energy,  !- Output Variable or Meter Name 4
+  SPACE5-1,                !- Key Name 5
+  Lights Electric Energy;  !- Output Variable or Meter Name 5
+
+Meter:Custom,
+  MyBuildingElectric,      !- Name
+  Electricity,             !- Fuel Type
+  ,                        !- Key Name #1
+  Electricity:Building;    !- Output Variable or Meter Name #1
+
+Meter:CustomDecrement,
+  MyBuildingOther,         !- Name
+  Electricity,             !- Fuel Type
+  Electricity:Building,    !- Source Meter Name
+  ,                        !- Key Name #1
+  MyGeneralLights;         !- Output Variable or Meter Name #1
+\end{lstlisting}
+
+For an example of ``generic'' fuel type, one might put the Building Infiltration Heat Loss \& Heat Gain on a set of custom meters:
+
+\begin{lstlisting}
+Meter:Custom,
+  Building Infiltration Heat Loss,          !- Name
+  Generic,                                  !- Fuel Type
+  *,                                        !- Key Name 1
+  Zone Infiltration Total Heat Loss Energy; !- Output Variable Name 1
+
+Meter:Custom,
+  Building Infiltration Heat Gain,          !- Name
+  Generic,                                  !- Fuel Type
+  *,                                        !- Key Name 1
+  Zone Infiltration Total Heat Gain Energy; !- Output Variable Name 1
+\end{lstlisting}
+
+One can then report these values the same way one reports other standard meters.
+
+\subsection{Simulation Parameter Outputs}\label{simulation-parameter-outputs}
+
+These appear in the \textbf{eplusout.eio} file. For details of the reporting, please see the Output Details and Examples document.
diff --git a/doc/input-output-reference/src/overview/group-solar-collectors.tex b/doc/input-output-reference/src/overview/group-solar-collectors.tex
new file mode 100644
index 00000000000..45a68bf81ce
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-solar-collectors.tex
@@ -0,0 +1,1005 @@
+\section{Group Solar Collectors}\label{group-solar-collectors}
+
+Solar collectors are thermal devices that convert solar energy into thermal energy by raising the temperature of a circulating heat transfer fluid. The fluid can then be used to heat water for domestic hot water usage or space heating.
+
+In EnergyPlus solar collectors are components that are connected to the plant loop. A solar heating system can be constructed with a combination of solar collectors, pumps, and hot water tanks.
+
+Flate plate solar collectors are defined using two objects: SolarCollector:FlatPlate:Water and SolarCollectorPerformance:FlatPlate. Similarly, Integral-Collector-Storage (ICS) solar collectors are defined using two objects: SolarCollector:IntegralCollectorStorage, and SolarCollectorPerformance:IntegralCollectorStorage. The SolarCollector:FlatPlate:Water and SolarCollector:IntegralCollectorStorage objects describe the plant component connections. These object also reference SolarCollectorPerformance:FlatPlate and SolarCollectorPerformance:IntegralCollectorStorage performance objects which contains the thermal and optical performance test data for a specific make and model of collector. Parameters are defined separately so that these values can be organized into a reference data set and need only be entered once if for an array of the same type of collectors.
+
+\subsection{SolarCollector:FlatPlate:Water}\label{solarcollectorflatplatewater}
+
+The flat-plate solar collector model simulates glazed, unglazed, and tubular (i.e.~evacuated tube) collectors. The SolarCollector:FlatPlate:Water object represents a single collector module connected to the plant loop. The thermal and optical properties of the collector module are taken from the referenced SolarCollectorPerformance:FlatPlate object. A surface or shading object defines the collector tilt, azimuth, and gross area. The collector surface participates normally in all shading calculations if the ``FullExterior,'' ``FullInteriorAndExterior,'' FullExteriorWithReflections , or FullInteriorAndExteriorWithReflections flags are set in the Solar Distribution field of the Building object. Inlet and outlet nodes are specified for plant connections on the demand side of the plant loop.
+
+\subsubsection{Inputs}\label{inputs-045}
+
+\paragraph{Field: Name}\label{field-name-044}
+
+The unique name of the SolarCollector:FlatPlate:Water object.
+
+\paragraph{Field: Solar Collector Performance Name}\label{field-solar-collector-performance-name}
+
+Reference name of a SolarCollectorPerformance:FlatPlate object that defines the thermal and optical properties of the collector.
+
+\paragraph{Field: Surface Name}\label{field-surface-name-005}
+
+Reference to one of the many different types of surfaces such as the BuildingSurface:Detailed or the Shading:Zone:Detailed objects. The surface named here is used to define the solar collector tilt, azimuth, and gross area.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-007}
+
+The name of the inlet node connection to the plant loop.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-008}
+
+The name of the outlet node connection to the plant loop.
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate-002}
+
+The maximum flow rate {[}m\(^{3}\)/s{]} allowed through the collector. This field is optional. If not specified, the collector will allow as much flow as the rest of the plant can deliver.
+
+An example follows.
+
+\begin{lstlisting}
+
+SolarCollector:FlatPlate:Water,
+  Collector 1,                                                       !- Name
+  ACR Solar International Fireball 2001,   !- Solar Collector Performance Name
+  Collector Surface,                                           !- Surface Name
+  Collector Inlet Node,                                     !- Inlet Node Name
+  Collector Outlet Node,                                   !- Outlet Node Name
+  0.00005;                                                               !- Maximum Flow Rate (m3/s)
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-034}
+
+The following output variables are reported for the SolarCollector:FlatPlate:Water object:
+
+\begin{itemize}
+\item
+  HVAC,Average,Solar Collector Incident Angle Modifier {[]}
+\item
+  HVAC,Average,Solar Collector Efficiency {[]}
+\item
+  HVAC,Average,Solar Collector Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Solar Collector Heat Gain Rate {[}W{]}
+\item
+  HVAC,Average,Solar Collector Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,Solar Collector Heat Transfer Energy {[}J{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Solar Collector Incident Angle Modifier {[]}}{Solar Collector Incident Angle Modifier }}\label{solar-collector-incident-angle-modifier}
+
+The incident angle modifier is an important intermediate value used in the SRCC calculation of solar collector performance. The value reported here is the combined result for the current time that includes incident angles of beam solar, diffuse solar from sky, and diffuse solar from ground.
+
+\paragraph{\texorpdfstring{Solar Collector Efficiency {[]}}{Solar Collector Efficiency }}\label{solar-collector-efficiency}
+
+The overall collector efficiency. This is the ratio of collected energy and the incident solar energy. The efficiency can be greater than 1 at times when the outdoor air temperature is warm enough.
+
+\paragraph{Solar Collector Heat Transfer Rate {[}W{]}}\label{solar-collector-heat-transfer-rate-w}
+
+\paragraph{Solar Collector Heat Transfer Energy {[}J{]}}\label{solar-collector-heat-transfer-energy-j}
+
+These are the overall rate (in W) and amount of energy ( in J) transferred to the collector s circulating fluid. Positive values indicate heating of the fluid while negative values indicate cooling of the fluid.
+
+\paragraph{Solar Collector Heat Gain Rate {[}W{]}}\label{solar-collector-heat-gain-rate-w}
+
+This is the overall rate of heat addition to the collector s circulating fluid in Watts. Values are always positive or zero. If the fluid is actually cooled then the value is zero.
+
+\paragraph{Solar Collector Heat Loss Rate {[}W{]}}\label{solar-collector-heat-loss-rate-w}
+
+This is the overall rate of heat loss from the collector s circulating fluid in Watts. Values are always positive or zero. If the fluid is actually heated then the value is zero.
+
+In addition, several surface variables are also relevant for the collector s surface object (BuildingSurface:Detailed or Shading:Zone:Detailed):
+
+\begin{itemize}
+\item
+  Zone,Average,Surface Outside Face Sunlit Area {[}m2{]}
+\item
+  Zone,Average,Surface Outside Face Sunlit Fraction {[]}
+\item
+  Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area {[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Beam Solar Radiation Rate per Area {[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area {[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area {[}W/m2{]}
+\item
+  Zone,Average,Surface Outside Face Beam Solar Incident Angle Cosine Value {[]}
+\end{itemize}
+
+The temperatures at the inlet and outlet nodes and the collector mass flow rate can be monitored using the system node output variables:
+
+\begin{itemize}
+\item
+  HVAC,Average,System Node Temperature {[}C{]}
+\item
+  HVAC,Average,System Node Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\subsection{SolarCollectorPerformance:FlatPlate}\label{solarcollectorperformanceflatplate}
+
+The SolarCollectorPerformance:FlatPlate object contains the thermal and optical performance parameters for a single collector module. These parameters are based on the testing methodologies described in ASHRAE Standards 93 and 96. The Solar Rating and Certification Corporation (SRCC) applies these standards in their rating procedures of solar collectors. The ratings for commercially available collectors in North America are published in the \emph{Directory of SRCC Certified Solar Collector Ratings}. The SRCC database has also been converted into an EnergyPlus data set of SolarCollectorPerformance:FlatPlate objects that is included with the program (see SolarCollectors.idf in the DataSets folder).
+
+The coefficients for the energy conversion efficiency and incident angle modifier allow first order (linear) or second order (quadratic) correlations. To use a first order correlation, the second order coefficient must be left blank or set to zero.
+
+In order for the model to work correctly, the test conditions for which the performance coefficients were measured must be specified in the fields: \emph{Test Fluid}, \emph{Test Volumetric Flow Rate}, and \emph{Test Correlation Type}. Currently, only water is allowed as the \emph{Test Fluid}.
+
+For more detailed information about the performance coefficients, see the \emph{EnergyPlus Engineering Reference Document}.
+
+\subsubsection{Inputs}\label{inputs-1-042}
+
+\paragraph{Field: Name}\label{field-name-1-041}
+
+The unique name of the SolarCollectorPerformance:FlatPlate object.
+
+\paragraph{Field: Gross Area}\label{field-gross-area}
+
+The gross area of the collector module {[}m\(^{2}\){]}. This value is mainly for reference. The area of the associated collector surface object is used in all calculations.
+
+\paragraph{Field: Test Fluid}\label{field-test-fluid}
+
+The fluid that was used in the testing procedure that resulted in the thermal and optical performance coefficients below. Currently only Water is allowed. This the fluid during the collector testing, not the fluid used during a particular EnergyPlus run.
+
+\paragraph{Field: Test Flow Rate}\label{field-test-flow-rate}
+
+The volumetric flow rate during testing {[}m\(^{3}\)/s{]}. If the value is available as flow rate per unit area, it is recommended to multiply by the \emph{Gross Area} of the collector module, not the net aperture area.
+
+\paragraph{Field: Test Correlation Type}\label{field-test-correlation-type}
+
+This field specifies type of temperature used to develop the correlation equations. The testing procedure is based on an experimental correlation using either Inlet, Average, or Outlet temperature. Enter one of these choices. The ASHRAE Standards 93 and 96 always use Inlet temperature.
+
+\paragraph{Field: Coefficient 1 of Efficiency Equation}\label{field-coefficient-1-of-efficiency-equation}
+
+First coefficient of efficiency equation for energy conversion {[}dimensionless{]}. This is the Y-intercept term.
+
+\paragraph{Field: Coefficient 2 of Efficiency Equation}\label{field-coefficient-2-of-efficiency-equation}
+
+Second coefficient of efficiency equation for energy conversion {[}W/m\(^{2}\)-K{]}. This is the first-order term.
+
+\paragraph{Field: Coefficient 3 of Efficiency Equation}\label{field-coefficient-3-of-efficiency-equation}
+
+Third coefficient of efficiency equation for energy conversion {[}W/m\(^{2}\)-K\(^{2}\){]}. This field is optional. This is the second-order term. If left blank or set to zero, a first-order linear correlation is used.
+
+\paragraph{Field: Coefficient 2 of Incident Angle Modifier}\label{field-coefficient-2-of-incident-angle-modifier}
+
+Second coefficient of the incident angle modifier equation. This the first-order term. (There is no \emph{Coefficient 1 of Incident Angle Modifier} because that number is always 1.0.)
+
+\paragraph{Field: Coefficient 3 of Incident Angle Modifier}\label{field-coefficient-3-of-incident-angle-modifier}
+
+Third coefficient of the incident angle modifier equation. This is the second-order term. This field is optional. If left blank or set to zero, a first order linear correlation is used.
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+SolarCollectorPerformance:FlatPlate,
+  Alternate Energy Technologies AE-32,   !- Name
+  2.9646,                                   !- Gross Area {m2}
+  WATER,                                     !- Test Fluid
+  0.0000388,                             !- Test Flow Rate {m3/s}
+  INLET,                                     !- Test Correlation Type
+  0.691,                                     !- Coefficient 1 of Efficiency Equation {dimensionless}
+  -3.396,                                   !- Coefficient 2 of Efficiency Equation {W/m2-K}
+  -0.00193,                               !- Coefficient 3 of Efficiency Equation {W/m2-K2}
+  -0.1939,                                 !- Coefficient 2 of Incident Angle Modifier
+  -0.0055;                                 !- Coefficient 3 of Incident Angle Modifier
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-025}
+
+This object does not generate any output; see SolarCollector:FlatPlate:Water Output
+
+\subsection{SolarCollector:IntegralCollectorStorage}\label{solarcollectorintegralcollectorstorage}
+
+The Integral-Collector-Storage (ICS) solar collector model simulates glazed collectors with integral storage unit. The SolarCollector:IntegralCollectorStorage object represents a single collector module connected to the plant loop. The thermal and optical properties of the collector module are calculated from inputs in SolarCollectorPerformance:IntegralCollectorStorage object. A surface or shading object defines the collector tilt, and azimuth. The collector surface participates normally in all shading calculations if the ``FullExterior,'' ``FullInteriorAndExterior,'' FullExteriorWithReflections , or FullInteriorAndExteriorWithReflections flags are set in the Solar Distribution field of the Building object. Inlet and outlet nodes are specified for plant connections on the demand side of the plant loop. The SurfaceProperty:ExteriorNaturalVentedCavity, object is required to describe the surface properties, the characteristics of the cavity and opening for natural ventilation if OtherSideConditionsModel is specified as the collector bottom surface outside boundary condition type.
+
+\subsubsection{Inputs}\label{inputs-2-039}
+
+\paragraph{Field: Name}\label{field-name-2-036}
+
+The unique name of the SolarCollector:IntegralCollectorStorage object.
+
+\paragraph{Field: Solar Collector Performance Name}\label{field-solar-collector-performance-name-1}
+
+Reference name of a SolarCollectorPerformance:IntegralCollectorStorage object that defines the thermal and optical properties of the collector.
+
+\paragraph{Field: Surface Name}\label{field-surface-name-1-001}
+
+Reference to one of the many different types of surfaces such as the BuildingSurface:Detailed or the Shading:Zone:Detailed objects. The surface named here is used to define the solar collector tilt, and azimuth. The collector shades the surface it is mounted on and hence impacts the surface heat balance.
+
+\paragraph{Field: Bottom surface Boundary Conditions Type}\label{field-bottom-surface-boundary-conditions-type}
+
+This field contains the type of boundary conditions applicable to the ICS collector bottom surface. Allowed boundary condition types are: AmbientAir and OtherSideConditionsModel. If the other side conditions model is selected, specify the name of the SurfaceProperty:OtherSideConditionsModel object in the next input field, otherwise, leave the next input field blank. The AmbientAir boundary condition uses outdoor air temperature as boundary condition, hence the subsurface is assumed to be exposed to the sun and wind.
+
+\paragraph{Field: Other Side Conditions Model Name}\label{field-other-side-conditions-model-name}
+
+This field contains the name of a SurfaceProperty:OtherSideConditionsModel object declared elsewhere in the input file. This will connect the collector to the exterior boundary conditions for the underlying heat transfer surface specified above..
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-1-004}
+
+The name of the inlet node connection to the plant loop.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-1-005}
+
+The name of the outlet node connection to the plant loop.
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate-1-000}
+
+The maximum flow rate {[}m3/s{]} allowed through the collector. This field is optional. If not specified, the collector will allow as much flow as the rest of the plant can deliver.
+
+An example follows.
+
+\begin{lstlisting}
+
+SolarCollector:IntegralCollectorStorage,
+  Collector 1,                                                       !- Name
+  ICS Solar Collector,                                       !- Solar Collector Performance Name
+  ICS Collector Surface,                                   !- Surface Name
+  OtherSideConditionsModel,                             !- Bottom Surface Boundary Conditions Type
+  ICS OSCM,                                                             !- Boundary Condition Model Name
+  Collector Inlet Node,                                     !- Inlet Node Name
+  Collector Outlet Node,                                   !- Outlet Node Name
+  0.00005;                                                               !- Maximum Flow Rate (m3/s)
+\end{lstlisting}
+
+\subsection{SolarCollectorPerformance:IntegralCollectorStorage}\label{solarcollectorperformanceintegralcollectorstorage}
+
+The SolarCollectorPerformance:IntegralCollectorStorage object contains the thermal and optical performance parameters for a single collector module. The transmittance-absorptance product of the absorber and cover system is determined from optical properties specified. For more detailed information about the calculation procedure, see the \emph{EnergyPlus Engineering Reference} Document.
+
+\subsubsection{Inputs}\label{inputs-3-035}
+
+\paragraph{Field: Name}\label{field-name-3-030}
+
+The unique name of the SolarCollectorPerformance:IntegralCollectorStorage object.
+
+\paragraph{Field: ICS Collector Type}\label{field-ics-collector-type}
+
+This input field is the ICS collector type. Currently only RectangularTank type is allowed.
+
+\paragraph{Field: Gross Area}\label{field-gross-area-1}
+
+This input field is the gross area of the collector module in m2. This gross area is used in the energy balance equations.
+
+\paragraph{Field: Collector Water Volume}\label{field-collector-water-volume}
+
+This input field is the volume of water in the solar collector in m3.
+
+\paragraph{Field: Bottom Heat Loss Conductance}\label{field-bottom-heat-loss-conductance}
+
+This input field is the collector bottom heat loss conductance in W/m2K. This value is calculated from thermal conductivity and thickness of the bottom insulation.
+
+\paragraph{Field: Side Heat Loss Conductance}\label{field-side-heat-loss-conductance}
+
+This input field is the collector side heat loss conductance in W/m2K. This value is calculated from thermal conductivity and thickness of the side insulation.
+
+\paragraph{Field: Collector Aspect Ratio}\label{field-collector-aspect-ratio}
+
+This input field is the ratio of the short side (width) of the collector to the long side (length) of the collector. This value is used only for calculating the collector side area along with the collector side height specified in the next input filed. This ratio is less or equal to 1.0.
+
+\paragraph{Field: Collector Side Height}\label{field-collector-side-height}
+
+This input field is height of collector side in m. This height is used to estimate the collector side area for heat loss calculations along with heat loss coefficient specified in the input field above.
+
+\paragraph{Field: Thermal Mass of Absorber Plate}\label{field-thermal-mass-of-absorber-plate}
+
+This input field is thermal-mass of the absorber plate per unit area of the collector in {[}J/m2×K{]}. This input value multiplied by the absorber gross area determines the thermal mass of the absorber plate. It is estimated from the specific heat, density and average thickness of the absorber plate. If zero is specified then the absorber plate energy balance reduces to steady state form.
+
+\paragraph{Field: Number of Covers}\label{field-number-of-covers}
+
+Number of transparent collector covers. Common practice is to use two covers: glass as the outer cover and Teflon as the inner cover. If single cover is specified leave the inner cover optical and thermal properties input fields blank.
+
+\paragraph{Field: Cover Spacing}\label{field-cover-spacing}
+
+This input field provides the spacing between the two transparent covers, and the spacing between the inner cover and the absorber plate in m. Default value is 0.05m.
+
+\paragraph{Field: Refractive Index of Outer Cover}\label{field-refractive-index-of-outer-cover}
+
+This is the average Refractive index for solar spectrum range of the outer transparent cover material. Glass is used as the outer cover. Average refractive index value for non-absorbing glass used in solar collectors over solar spectrum range is 1.526.
+
+\paragraph{Field: Extinction Coefficient Times Thickness of Outer Cover}\label{field-extinction-coefficient-times-thickness-of-outer-cover}
+
+This input field is the product of the extinction coefficient and the thickness of the out cover material. The extinction coefficient for glass types approximately varies from 4m\(^{-1}\) to 32 m\(^{-1}\). The extinction coefficient for low-iron glass, which is the default outer cover material, is 15 m\(^{-1}\). The default value for extinction coefficient times thickness (KL) is 0.045 ( = 15.0 x0.003), which is the product of the default extinction coefficient of 15m\(^{-1}\) and 3.0mm thick glass.
+
+\paragraph{Field: Emissivity of Outer Cover}\label{field-emissivity-of-outer-cover}
+
+This input field value is thermal emissivity of the outer collector cover. The default value assumes low-iron glass with thermal emissivity of 0.88.
+
+\paragraph{Field: Refractive Index of Inner Cover}\label{field-refractive-index-of-inner-cover}
+
+This input field is the average Refractive index of the inner transparent cover of the collector. Commonly Teflon (PolytetraFluoroethylene) is used as the inner cover. The average refractive index value over the solar spectrum range for Teflon is 1.37.
+
+\paragraph{Field: Extinction Coefficient Times Thickness of Inner Cover}\label{field-extinction-coefficient-times-thickness-of-inner-cover}
+
+This input field is the product of the extinction coefficient (K) and the thickness (L) of the inner cover material. The inner cover material is more transparent than the out cover, very thin and hence their thickness can be assumed to be negligible. The default value for extinction coefficient times thickness (KL) is 0.008 ( = 40.0x0.0002), which is the product of extinction coefficient of 40m\(^{-1}\) and a thickness of 0.2mm.
+
+\paragraph{Field: Emissivity of Inner Cover}\label{field-emissivity-of-inner-cover}
+
+This input field value is thermal emissivity of the inner transparent collector cover. The default value assumes plastic sheet with thermal emissivity of 0.30. This value is used in the thermal analysis only.
+
+\paragraph{Field: Absorptance of Absorber Plate}\label{field-absorptance-of-absorber-plate}
+
+This input field is shortwave or solar absorptance of the absorber plate. The default value is 0.96.
+
+\paragraph{Field: Emissivity of Absorber Plate}\label{field-emissivity-of-absorber-plate}
+
+This input field value is thermal emissivity of the absorber plate. Default value is 0.30. This input value is used in the thermal analysis only.
+
+An example follows.
+
+\begin{lstlisting}
+
+SolarCollectorPerformance:IntegralCollectorStorage,
+  ICS Experimental,               !- Name
+  RectangularTank,                 !- ICS Collector Type
+  0.37275,                                 !- Gross Area {m2}
+  0.0195875,                             !- Collector Water Volume {m3}
+  0.10,                                       !- Bottom Heat Loss Conductance
+  1.00,                                       !- Side Heat Loss Conductance
+  0.8,                                         !- Collector Aspect Ratio {dimensionless}
+  0.08,                                       !- Collector Side Height {m}
+  5800.0,                                         !- Thermal Mass of Absorber Plate {J/m2K}
+  1,                                             !- Number of Covers {dimensionless}
+  0.05,                                       !- Cover Spacing {m}
+  1.526,                                     !- Refractive Index of Outer Cover {dimensionless}
+  0.0125,           !- Extinction Coefficient Times Thickness of Outer Cover {dimensionless}
+  0.88,                                       !- Emissivity of Outer Cover
+  1.126,                                     !- Refractive Index of Inner Cover {dimensionless}
+  0.0126,           !- Extinction Coefficient Times Thickness of Inner Cover {dimensionless}
+  0.88,                                       !- Emissivity of Inner Cover {dimensionless}
+  0.96,                                       !- Absorptance of Absorber Plate {dimensionless}
+  0.60;                                       !- Emissivity of Absorber Plate {dimensionless}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-020}
+
+The following output variables are reported for the SolarCollector:IntegralCollectorStorage object:
+
+\begin{itemize}
+\item
+  HVAC,Average,Solar Collector Storage Water Temperature {[}C{]}
+\item
+  HVAC,Average,Solar Collector Absorber Plate Temperature {[}C{]}
+\item
+  HVAC,Average,Solar Collector Overall Top Heat Loss Coefficient {[}W/m2-C{]}
+\item
+  HVAC,Average,Solar Collector Thermal Efficiency {[]}
+\item
+  HVAC,Average,Solar Collector Storage Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Solar Collector Storage Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Solar Collector Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Solar Collector Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Solar Collector Skin Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum, Solar Collector Skin Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Solar Collector Transmittance Absorptance Product {[]}
+\end{itemize}
+
+\paragraph{Solar Collector Storage Water Temperature {[}C{]}}\label{solar-collector-storage-water-temperature-c}
+
+This output variable is the ICS collector stored water average temperature at a given time steps in degree Celsius. This temperature is the same as the collector ICS collector leaving water temperature.
+
+\paragraph{Solar Collector Absorber Plate Temperature {[}C{]}}\label{solar-collector-absorber-plate-temperature-c}
+
+This output variable is the ICS collector absorber plate average temperature at a given time steps in degree Celsius.
+
+\paragraph{\texorpdfstring{Solar Collector Thermal Efficiency {[]}}{Solar Collector Thermal Efficiency }}\label{solar-collector-thermal-efficiency}
+
+This output variable is the instantaneous thermal efficiency of the ICS solar collector in per cent. This value is determined from net useful energy collected and the total incident solar radiation for each time step. The net useful energy collected is the sum of the energy stored in the collector and net useful energy delivered.
+
+\paragraph{Solar Collector Storage Heat Transfer Rate {[}W{]}}\label{solar-collector-storage-heat-transfer-rate-w}
+
+\paragraph{Solar Collector Storage Heat Transfer Energy {[}J{]}}\label{solar-collector-storage-heat-transfer-energy-j}
+
+These output variables are the instantaneous rate of change of the energy and the change in energy of the water in the ICS solar collector in Watts, and Joules, respectively.
+
+\paragraph{Solar Collector Skin Heat Transfer Rate {[}W{]}}\label{solar-collector-skin-heat-transfer-rate-w}
+
+\paragraph{Solar Collector Skin Heat Transfer Energy {[}J{]}}\label{solar-collector-skin-heat-transfer-energy-j}
+
+These output variables are the instantaneous skin heat loss rate and the heat loss energy of the ICS solar collector for each time steps in Watts, and Joules respectively. The skin heat loss rate is the sum of the heat losses through the top, bottom and sides of the collector surfaces. This value is mostly negative, but can have a positive value (heat gain) when the outdoor air temperature is warmer than the collector.
+
+\paragraph{Solar Collector Heat Transfer Rate {[}W{]}}\label{solar-collector-heat-transfer-rate-w-1}
+
+\paragraph{Solar Collector Heat Transfer Energy {[}J{]}}\label{solar-collector-heat-transfer-energy-j-1}
+
+This output variable is the heat rate and Energy transferred from the ICS collector to the collector loop fluid (water) in Watts and Joule, respectively. This value is determined from the collector water mass flow rate, specific heat of water and the temperature difference between the collector water outlet and inlet nodes at each time step. The value is positive when the fluid is heated or negative when cooled.
+
+\paragraph{\texorpdfstring{Solar Collector Transmittance Absorptance Product {[]}}{Solar Collector Transmittance Absorptance Product }}\label{solar-collector-transmittance-absorptance-product}
+
+This output variable is the transmittance-absorptance product of the covers and absorber system of the ICS solar collector. This value ranges from 0.0 to less than 1.0.
+
+\paragraph{Solar Collector Overall Top Heat Loss Coefficient {[}W/m2-C{]}}\label{solar-collector-overall-top-heat-loss-coefficient-wm2-c}
+
+This output variable is the overall heat loss coefficient from the absorber plate to the ambient air calculated for each time step.
+
+\subsection{SolarCollector:FlatPlate:PhotovoltaicThermal}\label{solarcollectorflatplatephotovoltaicthermal}
+
+This object is used to model hybrid photovoltaic-thermal (PVT) solar collectors that convert incident solar energy into both electricity and useful thermal energy. This object describes the PVT solar collector by referencing other objects that provide more detail or connections to other parts of the EnergyPlus model.
+
+The PVT solar collectors need to be connected to either an HVAC air system or a plant loop for collected thermal energy to be utilized. The input field for the type of thermal working fluid informs the program how the PVT collector is expected to be connected. If the the working fluid is air, then the PVT collectors are modeled as a ventilation air pretreatment component and connected to an outdoor air system. If the working fluid is water, then the PVT collectors are modeled as a hot water solar collector and are connected to a plant loop with a water thermal storage tank.
+
+\subsubsection{Inputs}\label{inputs-4-032}
+
+\paragraph{Field: Name}\label{field-name-4-027}
+
+This field should contain a unique name chosen by the user to identify a specific PVT collector in the building model.
+
+\paragraph{Field: Surface Name}\label{field-surface-name-2-001}
+
+This field is the user-defined name of a surface object (defined elsewhere) to which the PVT module is attached. These can be any type of building surface that is exposed to the exterior environment. The model uses the named surface s geometry for the PVT solar collector.
+
+\paragraph{Field: Photovoltaic-Thermal Model Performance Name}\label{field-photovoltaic-thermal-model-performance-name}
+
+This field is the user-defined name of an object (defined elsewhere) that provides the performance details of the PVT module. This should be the name of a SolarCollectorPerformance:PhotovoltaicThermal:Simple object. Multiple different SolarCollector:FlatPlate:PhotovoltaicThermal objects can reference the same object that provides performance details.
+
+\paragraph{Field: Photovoltaic Generator Name}\label{field-photovoltaic-generator-name}
+
+This field is the user-defined name of a Generator:Photovoltaic object (defined elsewhere) that will be used to model the solar electric portion of the PVT solar collector. The PVT models make any adjustments needed to model PV performance in the context of the PVT collector.
+
+\paragraph{Field: Thermal Working Fluid Type}\label{field-thermal-working-fluid-type}
+
+This field is the user s choice for the type of fluid used to collect thermal energy. PVT solar collectors can capture thermal energy in either air or water streams. The choices available for this field are Water or Air. If the choice is Air then the PVT collector needs to be connected to an HVAC air system loop. The PVT collector should be situated as the first component on an outdoor air inlet stream. If the choice is Water then the PVT collector needs to be connected to a Plant water system loop. The connections are made via node names which are defined in the following fields, depending on the working fluid type.
+
+\paragraph{Field: Water Inlet Node Name}\label{field-water-inlet-node-name-003}
+
+This field is the name of Plant loop node that serves as the inlet to the PVT collector. This field is only used if the Thermal Working Fluid Type is set to Plant/Water.
+
+\paragraph{Field: Water Outlet Node Name}\label{field-water-outlet-node-name-002}
+
+This field is the name of a plant loop node that seves as the outlet from the PVT collector. This field is only used if the Thermal Working Fluid Type is set to Plant/Water.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-006}
+
+This field is the name of HVAC air loop node that serves as the inlet to the PVT collector. This field is only used if the Thermal Working Fluid Type is set to HVAC/Air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-005}
+
+This field is the name of HVAC air loop node that serves as the outlet from the PVT collector. This field is only used if the Thermal Working Fluid Type is set to HVAC/Air.
+
+\paragraph{Field: Design Flow Rate}\label{field-design-flow-rate-003}
+
+This field is used to describe the nominal volume flow rate of the thermal working fluid. The units are m3/s. The volume flow rate is autosizable.
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+SolarCollector:FlatPlate:PhotovoltaicThermal,
+  PVT: 1_Ceiling ,                                             !- Name
+  1_Ceiling ,                                                       !- Surface Name
+  30percentPVThalfArea ,                                 !- Photovoltaic-Thermal Model Performance Name
+  PV:ZN_1_FLR_1_SEC_1_Ceiling ,                   !- Photovoltaic Name
+  Air ,                                                                   !- Thermal Working Fluid Type
+  ,                                                                           !- Water Inlet Node Name
+  ,                                                                           !- Water Outlet Node Name
+  ZN_1_FLR_1_SEC_1:Sys_OAInlet Node ,       !- Air Inlet Node Name
+  PVT:ZN_1_FLR_1_SEC_1_Ceiling Outlet ,   !- Air Outlet Node Name
+  Autosize ;                                                         !- Design Flow Rate
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-018}
+
+The output variables that are available for flat plate PVT include the following.
+
+\begin{itemize}
+\item
+  HVAC,Average,Generator Produced Thermal Rate {[}W{]}
+\item
+  HVAC,Sum,Generator Produced Thermal Energy {[}J{]}
+\item
+  HVAC,Average,Generator PVT Fluid Bypass Status {[]}
+\item
+  HVAC,Average,Generator PVT Fluid Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator PVT Fluid Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Generator PVT Fluid Mass Flow Rate {[}kg/s{]}
+\end{itemize}
+
+\paragraph{Generator Produced Thermal Rate {[}W{]}}\label{generator-produced-thermal-rate-w-000}
+
+\paragraph{Generator Produced Thermal Energy {[}J{]}}\label{generator-produced-thermal-energy-j-000}
+
+These outputs are the thermal energy and power produced by the PVT collector. PVT collectors are a type of cogenerator, producing both electrical and thermal power and these variables report the thermal portion in the same manner as other fuel-based cogenerators. The thermal energy is placed on HeatProduced meter and is attributed to SolarWater or SolarAir depending on the type of working fluid. The generator thermal production is also reported at the load center level.
+
+\paragraph{\texorpdfstring{Generator PVT Fluid Bypass Status {[]}}{Generator PVT Fluid Bypass Status }}\label{generator-pvt-fluid-bypass-status}
+
+This output variable indicates the status a bypass damper. It is only available for air-based PVT. There are no dimensions and the range is between 0.0 and 1.0. If the value is 0.0, then there is no bypassing and all the working fluid goes through the collector. If the value is 1.0, then there is complete bypassing and all the working fluid goes around the collector. If the value is between 0.0 and 1.0, then the model is effectively mixing bypass and collector streams to target a temperature setpoint placed on the outlet node.
+
+\paragraph{Generator PVT Fluid Inlet Temperature {[}C{]}}\label{generator-pvt-fluid-inlet-temperature-c}
+
+This report is the inlet temperature of the working fluid that enters the PVT collector
+
+\paragraph{Generator PVT Fluid Outlet Temperature {[}C{]}}\label{generator-pvt-fluid-outlet-temperature-c}
+
+This report is the outlet temperature of the working fluid that leaves the PVT collector
+
+\paragraph{Generator PVT Fluid Mass Flow Rate {[}kg/s{]}}\label{generator-pvt-fluid-mass-flow-rate-kgs}
+
+This report is the mass flow rate of the working fluid through the PVT collector. This is the overall mass flow rate, portions of the flow may be internally bypassed around the collector itself for control modulation.
+
+\subsection{SolarCollectorPerformance:PhotovoltaicThermal:Simple}\label{solarcollectorperformancephotovoltaicthermalsimple}
+
+This object is used to provide performance details for the simple PVT model. This is a simple user-defined efficiency model. Thermal conversion efficiency is a constant or scheduled value. There are no output variable for this object, reporting is done by the parent PVT object.
+
+\subsubsection{Inputs}\label{inputs-5-029}
+
+\paragraph{Field: Name}\label{field-name-5-023}
+
+This field is the unique name for this object.
+
+\paragraph{Field: Fraction of Surface Area with Active Thermal Collector}\label{field-fraction-of-surface-area-with-active-thermal-collector}
+
+This field is the fraction of the surface area that is active. It should be a decimal fraction between 0.0 and 1.0. The area of the PVT s surface will be multiplied by this fraction to determine the active area of the PVT collector(s).
+
+\paragraph{Field: Thermal Conversion Efficiency Input Mode Type}\label{field-thermal-conversion-efficiency-input-mode-type}
+
+This field is used to determine how the thermal efficiency is input. There are two choices, Fixed or Scheduled. If this field is set to Fixed, then a constant value for thermal efficiency will be used (set in next field). If this field is set to Scheduled, then the thermal efficiency values are defined in a schedule.
+
+\paragraph{Field: Value for Thermal Conversion Efficiency if Fixed}\label{field-value-for-thermal-conversion-efficiency-if-fixed}
+
+This field is used to provide a value for the efficiency with which solar energy is collected in the working fluid. This field is only used if the input mode is set to Fixed in the previous field. Efficiency is defined as the thermal energy collected divided by the incident solar radiation. The value should be between 0.0 and 1.0. The user should be careful that the thermal efficiency and the electrical efficiency be consistent with each other because the overall efficiency of the PVT collector is the combination of both thermal and electrical.
+
+\paragraph{Field: Name of Schedule for Thermal Conversion Efficiency}\label{field-name-of-schedule-for-thermal-conversion-efficiency}
+
+This field is used for the name of a schedule that provides values for the efficiency with which solar energy is collected in the working fluid. This field is only used if the input mode is set to Scheduled in the field above. Efficiency is defined as the thermal energy collected divided by the incident solar radiation. The values in the named schedule should be between 0.0 and 1.0. The user should be careful that the thermal efficiency and the electrical efficiency be consistent with each other because the overall efficiency of the PVT collector is the combination of both thermal and electrical.
+
+\paragraph{Field: Front Surface Emittance}\label{field-front-surface-emittance}
+
+This field is used to describe an average value for the total hemispherical emittance of the collector s front face exposed to the sky. This is used to model cooling applications where the PVT collectors are operated at night to cool the working fluid.
+
+An example input object follows.
+
+\begin{lstlisting}
+
+SolarCollectorPerformance:PhotovoltaicThermal:Simple,
+  20percentEffPVhalfArea ,                 !- Name
+  0.5 ,                                                       !- Fraction of Surface Area with Active Thermal Collector
+  Fixed ,                                                   !- Thermal Conversion Efficiency Input Mode Type
+  0.2 ,                                                       !- Value for Thermal Conversion Efficiency if Fixed
+  ,                                                             !- Name of Schedule for Thermal Conversion Efficiency
+  0.84 ;                                                     !- Front Surface Emittance
+\end{lstlisting}
+
+\subsection{Solar Collector Heating System Plant Connections}\label{solar-collector-heating-system-plant-connections}
+
+This section provides an overview of how to model solar heating systems. A solar heating system can be constructed using a combination of solar collectors, pumps, water tanks and water heaters. The solar collector must be connected on the demand side of the plant loop. Multiple collector modules can be combined in series and parallel using the normal plant connection rules. The supply side of the plant loop should contain a water heater with the solar collector loop connecting to the \emph{Source Side Inlet} and \emph{Source Side Outlet} nodes. As usual, the pump must be the first component on the supply side.
+
+If the solar heating system is for domestic hot water (or service water heating) usage only, the field \emph{Use Flow Rate Fraction Schedule Name} of the WaterHeater:Mixed object can be used to avoid additional plant connections. If the system has more complicated hot water requirements or if the system is for space heating, the \emph{Use Side Inlet} and \emph{Use Side Outlet} nodes must be connected to another plant loop to serve zone and non-zone equipment. (See the WaterHeater:Mixed object documentation for more information.)
+
+\begin{figure}[hbtp] % fig 132
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image339.png}
+\caption{Solar Collector Plant Loop Connection Diagram \protect \label{fig:solar-collector-plant-loop-connection-diagram}}
+\end{figure}
+
+NOTE: The EnergyPlus plant simulation requires the pump to be the first component on the supply side. This may be different from the way the solar heating system is actually configured. This should not affect the validity of the simulation results.
+
+In order to realize energy savings with a solar heating system, it is best to use a two-tank system with a storage tank and auxiliary water heater. The storage tank gathers heat directly from the solar collectors and stores it for later use. The storage tank is modeled using a WaterHeater:Mixed object with the \emph{Heater Maximum Capacity} set to zero. The auxiliary water heater is positioned downstream of the storage tank on the supply side of the main plant loop. The auxiliary water heater, or booster water heater, provides additional heat if the storage tank water is not hot enough. The auxiliary water heater can be modeled as an instantaneous/tankless water heater or as a standard tanked water heater with heating source (see WaterHeater:Mixed).
+
+\begin{figure}[hbtp] % fig 133
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image340.png}
+\caption{Two-Tank Solar Heating System Connection Diagram \protect \label{fig:two-tank-solar-heating-system-connection}}
+\end{figure}
+
+Another strategy to consider for solar heating systems is to allow the storage tank to reach a much higher temperature than necessary for the end use. This allows the tank to store more energy from the solar collectors, when it is available. However, for applications such as domestic hot water, it is undesirable and unsafe to supply excessive hot water temperatures at the point of demand. To take advantage of higher storage temperatures, yet still avoid scalding temperatures at the faucet, the hot water leaving the storage tank can be tempered with cold water using a three-way valve to achieve the target temperature. See the TemperingValve object documentation for more details.
+
+A complete two-tank solar heating system with tempering valve is shown below.
+
+\begin{figure}[hbtp] % fig 134
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image341.png}
+\caption{Two-Tank Solar Heating System with Tempering Valve \protect \label{fig:two-tank-solar-heating-system-with-tempering}}
+\end{figure}
+
+\subsection{Solar Heating System Control}\label{solar-heating-system-control}
+
+There are several options for controlling a solar heating system in EnergyPlus. Since the solar collectors request a constant flow demand based on their \emph{Maximum Flow Rate}, the limiting factor is actually the flow rate determined by the loop pump. Therefore the entire system can be controlled using the \emph{Pump Flow Rate Schedule} of the pump. If the schedule is omitted, the pump and system will run all the time (without any other controls specified). This is usually not the best way to operate a solar heating system.
+
+To better control the collector loop, a differential thermostat can be used to compare the temperature in the water heater to the temperature in the collector so that the pump is only turned on when there is a useful heat gain. The differential thermostat is simulated using the AvailabilityManager:DifferentialThermostat object. For a typical system, the \emph{Hot Node Name} field refers to an outlet node of one of the collector modules. The \emph{Cold Node Name} field refers to the \emph{Source Side Outlet} node, i.e.~the cold storage water leaving the water heater. The fields \emph{Temperature Difference On Limit} and \emph{Temperature Difference Off Limit} are usually 8 12 C and 1 3 C respectively. If the two temperature differences are too close, it is possible for the system to turn on and off rapidly without much useful heat gain. This can also occur if the flow rate through the collector is too high. Without flow the fluid in the collector heats up more quickly; when high flow is turned on, all of the hot fluid is removed and the temperature drops, forcing the system off again.
+
+Another control method is to use a photovoltaic panel to power the pump. The system begins pumping when there is enough solar radiation to operate the pump. This is not yet implemented in EnergyPlus.
+
+\subsubsection{Freeze Prevention}\label{freeze-prevention}
+
+In climates with a cold season, the solar heating system must be designed to avoid the risk of fluid freezing in the solar collector or exposed pipes and causing damage. This is not a problem if air is the heat transfer fluid. With water, however, there are several strategies that can minimize the risk.
+
+\emph{Seasonal schedule}. The simplest strategy is to not use the system during the cold season. This is a hassle because it requires the collector to be manually drained of all fluid. The benefits of the solar heating system are also lost during this time. This can be simulated in EnergyPlus with the appropriate pump schedule for the collector system.
+
+\emph{Antifreeze}. The freezing point of the liquid is decreased by adding antifreeze to the water or using a different heat transfer liquid with a lower freezing point. This cannot yet be simulated in EnergyPlus because only pure water is currently allowed in plant loops.
+
+\emph{Drain-back system}. This strategy automatically empties the collector when the pump is not running. This scenario is modeled by default in EnergyPlus, although the extra pump energy required to start the system is not taken into account.
+
+\emph{Recirculation system}. This strategy automatically recirculates warm liquid from the storage tank back through the collector to maintain the system above the freezing point. There are system losses using this method. This can be simulated in EnergyPlus by using AvailabilityManager:LowTemperatureTurnOn to force the system to turn on when the outdoor air temperature or collector outlet temperature falls below a specified minimum.
+
+\subsubsection{Additional Controls}\label{additional-controls}
+
+In addition to freeze prevention, it is also necessary to prevent the system from becoming too hot. This is usually a safety issue for the water heater. For this case it is important to have a high temperature cutoff to stop the pump before damaging the water heater. This is accomplished with a AvailabilityManager:HighTemperatureTurnOff.
+
+\subsubsection{System Availability Manager List Example}\label{system-availability-manager-list-example}
+
+To use the availability managers for the control cases described above, a AvailabilityManagerAssignmentList must be defined and referenced in the PlantLoop object of the collector loop. An example of a differential thermostat, recirculation for freeze prevention, and high temperature cutoff is shown below:
+
+\begin{lstlisting}
+
+AvailabilityManagerAssignmentList,
+  Collector Loop Availability Manager List,             !- Name
+  AvailabilityManager:HighTemperatureTurnOff,         !- Availability Manager 1 Object Type
+  High Temperature Turn Off Availability Manager, !- Availability Manager 1 Name
+  AvailabilityManager:HighTemperatureTurnOn,           !- Availability Manager 2 Object Type
+  Low Temperature Turn On Availability Manager,     !- Availability Manager 2 Name
+  AvailabilityManager:DifferentialThermostat,         !- Availability Manager 3 Object Type
+  Differential Thermostat Availability Manager;     !- Availability Manager 3 Name
+
+
+  AvailabilityManager:HighTemperatureTurnOff,           ! For water heater safety
+  High Temperature Turn Off Availability Manager, !- Name
+  Water Heater Use Outlet Node,                                     !- Sensor Node Name
+  60.0;                                                                                     !- Temperature (C)
+
+
+  AvailabilityManager:HighTemperatureTurnOn,             ! For freeze prevention by recirculation
+  Low Temperature Turn On Availability Manager,     !- Name
+  Collector Outlet Node,                                                   !- Sensor Node Name
+  0.0;                                                                                       !- Temperature (C)
+
+
+  AvailabilityManager:DifferentialThermostat,           ! For useful heat gain from collector to tank
+  Differential Thermostat Availability Manager,     !- Name
+  Collector Outlet Node,                                                   !- Hot Node Name
+  Water Heater Source Outlet Node,                               !- Cold Node Name
+  10.0,                                                                                     !- Temperature Difference On Limit (delta C)
+  2.0;                                                                                       !- Temperature Difference Off Limit (delta C)
+\end{lstlisting}
+
+The AvailabilityManager:DifferentialThermostat object must always be the last manager in the availability manager list. See the AvailabilityManagerAssignmentList object documentation for more information.
+
+\subsection{SolarCollector:UnglazedTranspired}\label{solarcollectorunglazedtranspired}
+
+This object is used to model unglazed transpired solar collectors (UTSC) used to condition outdoor air. These collectors are generally used to heat air drawn through perforated absorbers that are heated by the sun and also recover heat conducted out through the underlying wall. The SolarCollector:UnglazedTranspired****object represents a single collector attached to one or more BuildingSurface:Detailed objects and to one or more outdoor air systems. Therefore the transpired collector is part of both the thermal envelope and the HVAC system. An example file is provided called TranspiredCollectors.idf.
+
+The area and orientation of the collector is obtained from BuildingSurface:Detailed objects, which are referenced by name. Although the collector surface itself is slightly detached from the underlying building wall (or roof), no additional surface object is needed to represent the collector itself. When modeling transpired collectors, it is important to consider the size of the collector when developing the building model s BuildingSurface:Detailed objects because the underlying surfaces must match the collector. For example, if the collector covers only part of the wall, then that wall should be split into separate surfaces where one matches the size of the collector. A single collector can be associated with as many BuildingSurface:Detailed objects as desired (although if you need to use more than 10 surfaces, then the IDD will need to be extended). The collector can be arranged at any tilt angle by describing the surfaces appropriately. The surfaces need not be contiguous nor have the same orientation, but the program will issue warnings if surfaces have widely ranging tilts and azimuths.
+
+The collector conditions outdoor air and is connected to the outdoor air system using the usual method of specifying node names. Using the UTSC model requires specifying a relatively complete HVAC air system that includes an outdoor air path. This will typically require using a set of objects that, at a minimum, will include: AirLoopHVAC:ControllerList, AirLoopHVAC:OutdoorAirSystem:EquipmentList, AirLoopHVAC:OutdoorAirSystem, OutdoorAir:NodeList, OutdoorAir:Mixer, SetpointManager:MixedAir, and Controller:OutdoorAir. A single UTSC can serve more than one outdoor air system but requires also using a separate object, called SolarCollector:UnglazedTranspired:MultiSystem to specify node connections.
+
+Controls for the UTSC involve setting the rate of air flow and the status of a bypass damper. If the bypass damper is open, then all the ventilation air goes straight into the outdoor air mixer; if it closed, then all the air first passes through the UTSC. The bypass damper is modeled as completely open or completely closed. The UTSC bypass damper control is determined by an availability manager, the airflow set by the outdoor air mixer controls, and thermostatic type controls that decide if heating is useful. An availability schedule is used to bypass the collector for certain times of the year, eg. summer cooling season. The air flow rates are set by controls associated with the outdoor air mixer (see SetpointManager:MixedAir, and Controller:OutdoorAir). Thermostatic type control decides if the collector will provide useful heating based on either of two types of setpoints. The first type of temperature setpoint is managed by SetpointManager:MixedAir, where the UTSC model looks at a control node, usually the mixed air node. The second type is an extra setpoint especially for free heating that is managed within this object where the UTSC model looks at the zone air node.
+
+\subsubsection{Inputs}\label{inputs-6-026}
+
+\paragraph{Field: Name}\label{field-name-6-021}
+
+This field contains a unique name for the unglazed transpired solar collector.
+
+\paragraph{Field: Boundary Conditions Model Name}\label{field-boundary-conditions-model-name-000}
+
+This field contains the name of a SurfaceProperty:OtherSideConditionsModel object declared elsewhere in the input file. This will connect the collector to the exterior boundary conditions for the underlying heat transfer surface.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-016}
+
+This field contains the name of a schedule that determines whether or not the UTSC is available. When the schedule value is less than or equal to zero, the UTSC is always bypassed. When the schedule value is greater than zero, the UTSC is available and will be used when other conditions are met, such as outdoor air requested by mixer and preheating has been determined to be beneficial based on thermostatic control. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-2-003}
+
+This field contains the name of an air node that provides air into the UTSC. This node name should also be assigned to be an outdoor air node using the OutdoorAir:NodeList or OutdoorAir:Node objects. This node should also be named as the actuated node in a Controller:OutdoorAir object. If the UTSC is connected to more than one air system, then this field can be left blank and the SolarCollector:UnglazedTranspired:MultiSystem object should be used to define the nodes.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-2-003}
+
+This field contains the name of an air node that is the outlet of the UTSC. This node name will typically be the inlet to the OutdoorAir:Mixer (if there is no other equipment on the outdoor air path). If the UTSC is connected to more than one air system, then this field can be left blank and the SolarCollector:UnglazedTranspired:MultiSystem object should be used to define the nodes.
+
+\paragraph{Field: Setpoint Node Name}\label{field-setpoint-node-name-000}
+
+This field contains the name of an air node that has a setpoint manager controlling its temperature setpoint. This node name will typically be named as the control node in a a Controller:OutdoorAir object. If the UTSC is connected to more than one air system, then this field can be left blank and the SolarCollector:UnglazedTranspired:MultiSystem object should be used to define the nodes.
+
+\paragraph{Field: Zone Node Name}\label{field-zone-node-name-001}
+
+This field contains the name of an air node for a thermal zone that is ultimately connected to the air system. This node is used with the setpoint schedule, defined in the following field, to provide an added layer of thermostatic control for the UTSC without affecting the control of auxiliary heating. If there is a single air system that is connected to more than one zone, then a single zone should be selected based on where the thermostat might be located. If the UTSC is connected to more than one air system, then this field can be left blank and the SolarCollector:UnglazedTranspired:MultiSystem object should be used to define the nodes.
+
+\paragraph{Field: Free Heating Setpoint Schedule Name}\label{field-free-heating-setpoint-schedule-name}
+
+This field contains the name of a temperature schedule defined elsewhere in the input file. This schedule should define temperatures \emph{desired} in the zone, but not necessarily \emph{required}. This secondary setpoint schedule is used to allow the UTSC to operate as if it has its own thermostat that is separate from the primary control mechanism. When the UTSC is used with auxiliary heating, the usual setpoint managers and temperature controllers will determine how the auxiliary heaters are controlled. This allows using a higher zone air temperature setpoint for controlling UTSC bypass than for the auxiliary heating system.
+
+\paragraph{Field: Diameter of Perforations in Collector}\label{field-diameter-of-perforations-in-collector}
+
+This field is used to enter the effective diameter of the perforations in the collector surface. The diameter should be entered in meters. For perforations other than round, use an equivalent diameter for a round hole that would have the same area.
+
+\paragraph{Field: Distance Between Perforations in Collector}\label{field-distance-between-perforations-in-collector}
+
+This field is used to enter the pitch, or average, shortest distance between perforations.
+
+\paragraph{Field: Thermal Emissivity of Collector Surface}\label{field-thermal-emissivity-of-collector-surface}
+
+This field is used to enter the thermal emissivity of the collector. This surface property is for longwave infrared radiation. The property is used for both sides of collector. Most painted materials have an emissivity of 0.9.
+
+\paragraph{Field: Solar Absorbtivity of Collector Surface}\label{field-solar-absorbtivity-of-collector-surface}
+
+This field is used to enter the solar absorbtivity of the collector. This surface property is for shortwave, solar radiation. The property is used for the front side of the collector that faces the environment. Darker colors have a higher absorbtivity. While black is the highest performance, other colors might be used to match the color scheme of the rest of the facade. The following table provides sample solar absorbtivities for different colors (source: Conserval Engineering Inc., Toronto, Ontario, Canada).
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+Color Name of Kynar(R) [[1]](\#\_ftn1) Paint & Solar Absorptivity \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Color Name of Kynar(R) [[1]](\#\_ftn1) Paint & Solar Absorptivity \tabularnewline
+\midrule
+\endhead
+
+Black & 0.94 \tabularnewline
+Classic Bronze & 0.91 \tabularnewline
+Chocolate Brown & 0.9 \tabularnewline
+Hartford Green & 0.9 \tabularnewline
+Med. Bronze & 0.89 \tabularnewline
+Boysenberry & 0.86 \tabularnewline
+Rocky Grey & 0.85 \tabularnewline
+Regal Blue & 0.85 \tabularnewline
+Forest Green & 0.84 \tabularnewline
+Hemlock Green & 0.82 \tabularnewline
+Slate Blue & 0.8 \tabularnewline
+Redwood & 0.79 \tabularnewline
+Teal & 0.79 \tabularnewline
+Slate Grey & 0.79 \tabularnewline
+Patina Green & 0.77 \tabularnewline
+Mint Green & 0.71 \tabularnewline
+Dove Grey & 0.69 \tabularnewline
+Mission Red & 0.69 \tabularnewline
+Sierra Tan & 0.65 \tabularnewline
+Brite Red & 0.59 \tabularnewline
+Rawhide & 0.57 \tabularnewline
+Sandstone & 0.54 \tabularnewline
+Silversmith & 0.53 \tabularnewline
+Coppertone & 0.51 \tabularnewline
+Concord Cream & 0.45 \tabularnewline
+Ascot White & 0.4 \tabularnewline
+Bone White & 0.3 \tabularnewline
+\bottomrule
+\end{longtable}
+
+(\protect\hyperlink{ux5fftnref1}{{[}1{]}} Kynar is a registered trademark of Elf Atochem North America, Inc.)
+
+\paragraph{Field: Effective Overall Height of Collector}\label{field-effective-overall-height-of-collector}
+
+This field is used to enter a nominal height for the collector. This value is used in the program to determine a length scale in the vertical direction for the buoyancy-driven portion of natural ventilation that occurs when the collector is inactive. (Note that most of the geometry information is obtained from the underlying surfaces.) The value entered here is adjusted inside the program to account for tilt of the collector. While the value here would generally correspond to the actual distance/height, its value is not critical and it can be used to adjust modeling the air exchange rates in passive mode. If the collector is horizontal, then the length scale is obtained from the following field.
+
+\paragraph{Field: Effective Gap Thickness of Plenum Behind Collector}\label{field-effective-gap-thickness-of-plenum-behind-collector}
+
+This field is used to enter a nominal gap thickness for the collector. This distance value is only used when the collector is near horizontal to determine a length scale in the vertical direction for buoyancy calculations. For example, if the collector is mounted on a flat roof, its tilt-adjusted height is zero and the program will use this gap thickness as a length scale rather than the height from the previous field.
+
+\paragraph{Field: Effective Cross Section Area of Plenum Behind Collector}\label{field-effective-cross-section-area-of-plenum-behind-collector}
+
+This field is used to enter the nominal cross sectional area of the gap behind the collector. This area is used to determine a velocity scale for surface convection heat transfer correlations when the collector is active. This value is generally the average gap thickness times the average width of the collector.
+
+\paragraph{Field: Hole Layout Pattern for Pitch}\label{field-hole-layout-pattern-for-pitch}
+
+This field is used to describe the pattern of perforations in the collector surface. There are currently two choices available: Square and Triangle. Note that the hole layout pattern should be consistent with how the value for pitch was determined.
+
+\paragraph{Field: Heat Exchange Effectiveness Correlation}\label{field-heat-exchange-effectiveness-correlation}
+
+This field is used to select which correlation is used to model heat transfer from the collector surface to the incoming air when the collector is active. There are two choices available: Kutscher1994, and VanDeckerHollandsBrunger2001. See the Engineering Reference for details and references.
+
+\paragraph{Field: Ratio of Actual Collector Surface Area to Projected Surface Area}\label{field-ratio-of-actual-collector-surface-area-to-projected-surface-area}
+
+This field is used to enter a factor that accounts for the extra surface area resulting from corrugations in the collector surface. Corrugations help stiffen the collector. The projected surface area is obtained by the program from the (flat) underlying surfaces. If the collector is flat then this ratio is 1.0. If the collector is corrugated, then this ratio will be greater than one. A typical value might be 1.165.
+
+\paragraph{Field: Roughness of Collector}\label{field-roughness-of-collector}
+
+This field is used to describe the relative roughness of the collector material. This field is similar to one in the Material object. This parameter only influences the convection coefficients, more specifically the outside convection coefficient. A special keyword is expected in this field with the options being VeryRough , Rough , MediumRough , MediumSmooth , Smooth , and VerySmooth in order of roughest to smoothest options.
+
+\paragraph{Field: Collector Thickness}\label{field-collector-thickness}
+
+This field is used to enter the thickness of the collector material. This value is only needed for the Van Decker Hollands Brunger 2001 correlation. The material thickness should be entered in meters.
+
+\paragraph{Field: Effectiveness for Perforations with Respect to Wind}\label{field-effectiveness-for-perforations-with-respect-to-wind-000}
+
+This field is used to enter a value for the coefficient used to determine natural air exchanges from wind, or Cv. When the collector is inactive, wind will cause exterior air to move in and out of the collector. Cv is an arbitrary coefficient used to model the effectiveness of openings and depends on opening geometry and the orientation with respect to the wind. Cv should probably be in the range 0.25 to 0.65. Increasing Cv will increase the amount of natural ventilation.
+
+\paragraph{Field: Discharge Coefficient for Openings with Respect to Buoyancy Driven Flow}\label{field-discharge-coefficient-for-openings-with-respect-to-buoyancy-driven-flow-000}
+
+This field is used to enter a value for the coefficient used to determine natural air exchanges from buoyancy, or Cd. When the collector is inactive, stack or buoyancy effects will cause exterior air to move in and out of the collector. Cd is an arbitrary discharge coefficient that depends on the geometry of the opening. Cd should probably be in the range 0.4 to 1.0. Increasing Cd will increase the amount of natural ventilation.
+
+\paragraph{Field: Surface \textless{}\#\textgreater{} Name}\label{field-surface-name-3-001}
+
+The remaining fields are used to name the BuildingSurface:Detailed objects that are associated with the UTSC. These are the underlying heat transfer surfaces and are defined elsewhere in the input file. These other surfaces should all specify OtherSideConditionsModel as their exterior environment. The input object can currently accommodate up to ten surfaces, but it is extensible.
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+SolarCollector:UnglazedTranspired,
+  Shop OA UTSC ZN11,                               ! Name
+  UTSC OSCM ZN11,                                     ! Boundary Conditions Model Name
+  HeatingAvailSched ,                             ! Availability Schedule Name
+  Outside Air Inlet Node ZN11 ,         ! Inlet Node Name
+  UTSC Outlet Node ZN11 ,                     ! Outlet Node Name
+  Mixed Air Node ZN11 ,                         ! Setpoint Node Name
+  ZN11 Node,                                               ! Zone Node Name
+  ShopFreeHeatingSetpoints,                 ! Free Heating Setpoint Schedule Name
+  0.0016,                                                     ! Diameter of Perforations in Collector
+  0.01689,                                                   ! Distance Between Perforations in Collector
+  0.9,                                                           ! Thermal Emissivity of Collector Surface
+  0.9,                                                           ! Solar Absorbtivity of Collector Surface
+  4.0,                                                           ! Effective Overall Height of Collector
+  0.1,                                                           ! Effective Gap Thickness of Plenum Behind Collector
+  2.0,                                                           ! Effective Cross Section Area of Plenum Behind Collector
+  Triangle,                                                 ! Hole Layout Pattern for Pitch
+  Kutscher1994,                                         ! Heat Exchange Effectiveness Correlation
+  1.165,                                           ! Ratio of Actual Collector Surface Area to Projected Surface Area
+  MediumRough ,                                         ! Roughness of Collector
+  0.00086,                                                   ! Collector Thickness
+  0.25,                                                         ! Effectiveness for Perforations with Respect to Wind
+  0.5,                                 ! Discharge Coefficient for Openings with Respect to Buoyancy Driven Flow
+  ZN11_Shop_1:ExtWall:South;               ! Surface 1 Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-015}
+
+In addition to related output that can be obtained for air nodes and surfaces, these outputs are available for UTSC systems:
+
+\begin{itemize}
+\item
+  HVAC,Average,Solar Collector Heat Exchanger Effectiveness {[]}
+\item
+  HVAC,Average,Solar Collector Leaving Air Temperature {[}C{]}
+\item
+  HVAC,Average,Solar Collector Outside Face Suction Velocity {[}m/s{]}
+\item
+  HVAC,Average,Solar Collector Surface Temperature {[}C{]}
+\item
+  HVAC,Average,Solar Collector Plenum Air Temperature {[}C{]}
+\item
+  HVAC,Average,Solar Collector Sensible Heating Rate {[}W{]}
+\item
+  Zone,Meter,SolarAir:Facility {[}J{]}
+\item
+  Zone,Meter,SolarAir:HVAC {[}J{]}
+\item
+  Zone,Meter,HeatProduced:SolarAir {[}J{]}
+\item
+  HVAC,Sum,Solar Collector Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Solar Collector Natural Ventilation Air Change Rate {[}ACH{]}
+\item
+  HVAC,Average,Solar Collector Natural Ventilation Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Solar Collector Wind Natural Ventilation Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Solar Collector Buoyancy Natural Ventilation Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Solar Collector Incident Solar Radiation {[}W/m2{]}
+\item
+  HVAC,Average,Solar Collector System Efficiency {[]}
+\item
+  HVAC,Average,Solar Collector Surface Efficiency {[]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Solar Collector Heat Exchanger Effectiveness {[]}}{Solar Collector Heat Exchanger Effectiveness }}\label{solar-collector-heat-exchanger-effectiveness}
+
+The results from UTSC correlations defined by \({\varepsilon_{HX}} = \frac{{{T_{a,HX}} - {T_{amb}}}}{{{T_{s,coll}} - {T_{amb}}}}\) .
+
+\paragraph{Solar Collector Leaving Air Temperature {[}C{]}}\label{solar-collector-leaving-air-temperature-c}
+
+The temperature of air entering the plenum after being heated by the collector.
+
+\paragraph{Solar Collector Outside Face Suction Velocity {[}m/s{]}}\label{solar-collector-outside-face-suction-velocity-ms}
+
+The bulk velocity of air approaching the collector.
+
+\paragraph{Solar Collector Surface Temperature {[}C{]}}\label{solar-collector-surface-temperature-c}
+
+The surface temperature of the collector itself.
+
+\paragraph{Solar Collector Plenum Air Temperature {[}C{]}}\label{solar-collector-plenum-air-temperature-c}
+
+The temperature of air inside, and leaving, the plenum behind the collector.
+
+\paragraph{Solar Collector Sensible Heating Rate {[}W{]}}\label{solar-collector-sensible-heating-rate-w}
+
+The overall rate at which heat is being added to the outdoor air stream.
+
+\paragraph{SolarAir:Facility {[}J{]}}\label{solarairfacility-j}
+
+A meter that includes the heating energy provided by the UTSC.
+
+\paragraph{SolarAir:HVAC {[}J{]}}\label{solarairhvac-j}
+
+A meter that includes the heating energy provided by the UTSC.
+
+\paragraph{HeatProduced:SolarAir {[}J{]}}\label{heatproducedsolarair-j}
+
+A meter that includes the heating energy provided by the UTSC.
+
+\paragraph{Solar Collector Sensible Heating Energy {[}J{]}}\label{solar-collector-sensible-heating-energy-j}
+
+The overall sum of energy added to the outdoor air stream.
+
+\paragraph{Solar Collector Natural Ventilation Air Change Rate {[}ACH{]}}\label{solar-collector-natural-ventilation-air-change-rate-ach}
+
+The rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive in Air Changes per Hour.
+
+\paragraph{Solar Collector Natural Ventilation Mass Flow Rate {[}kg/s{]}}\label{solar-collector-natural-ventilation-mass-flow-rate-kgs}
+
+The mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive.
+
+\paragraph{Solar Collector Wind Natural Ventilation Mass Flow Rate {[}kg/s{]}}\label{solar-collector-wind-natural-ventilation-mass-flow-rate-kgs}
+
+The part of mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive due to wind-driven forces.
+
+\paragraph{Solar Collector Buoyancy Natural Ventilation Mass Flow Rate {[}kg/s{]}}\label{solar-collector-buoyancy-natural-ventilation-mass-flow-rate-kgs}
+
+The part of mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive due to buoyancy-driven forces.
+
+\paragraph{Solar Collector Incident Solar Radiation {[}W/m2{]}}\label{solar-collector-incident-solar-radiation-wm2}
+
+The intensity of solar radiation incident on the UTSC collector from all sources.
+
+\paragraph{\texorpdfstring{Solar Collector System Efficiency {[]}}{Solar Collector System Efficiency }}\label{solar-collector-system-efficiency}
+
+The overall efficiency of the UTSC system including collected solar energy and heat recovered from the underlying surface.
+
+\paragraph{\texorpdfstring{Solar Collector Surface Efficiency {[]}}{Solar Collector Surface Efficiency }}\label{solar-collector-surface-efficiency}
+
+The efficiency of the UTSC solar collector.
+
+\subsection{SolarCollector:UnglazedTranspired:MultiSystem}\label{solarcollectorunglazedtranspiredmultisystem}
+
+This object is used to model unglazed transpired solar collectors (UTSC) that are connected to multiple outdoor air systems. This object supplements the SolarCollector:UnglazedTranspired object and is only necessary if more than one air system is connected to a single transpired collector. After the name field, there are sets of four node names used to define the connections of each air system. Each set contains node names for inlet, outlet, control, and zone. If more than five air systems are needed, this object is extensible.
+
+\subsubsection{Field: Solar Collector Name}\label{field-solar-collector-name}
+
+This field is used to identify the name of the SolarCollector:UnglazedTranspired object that needs to be connected to more than one air system. This field must match the name.
+
+\subsubsection{Field Set: Inlet Node, Outlet Node, Mixed Air Node, Zone Node}\label{field-set-inlet-node-outlet-node-mixed-air-node-zone-node}
+
+The following four fields form a repeating set of four fields. One set is used for each outdoor air system that is connected to the collector.
+
+\subsubsection{Field: Outdoor Air System \textless{}\#\textgreater{} Collector Inlet Node}\label{field-outdoor-air-system-collector-inlet-node}
+
+This field contains the name of an air node that provides air into the UTSC. This node name should also be assigned to be an outdoor air node using the OutdoorAir:NodeList and OutdoorAir:Node objects. This node is also be named as the actuator node in a Controller:OutdoorAir object.
+
+\subsubsection{Field: Outdoor Air System \textless{}\#\textgreater{} Collector Outlet Node}\label{field-outdoor-air-system-collector-outlet-node}
+
+This field contains the name of an air node that is the outlet of the UTSC. This node name will typically be the Outdoor Air Stream Node Name in the OutdoorAir:Mixer (if there is no other equipment on the outdoor air path).
+
+\subsubsection{Field: Outdoor Air System \textless{}\#\textgreater{} Mixed Air Node}\label{field-outdoor-air-system-mixed-air-node}
+
+This field contains the name of an air node that has a setpoint manager controlling its temperature setpoint. This node name will typically be named as the mixed air node in a Controller:OutdoorAir object.
+
+\subsubsection{Field: Outdoor Air System \textless{}\#\textgreater{} Zone Node}\label{field-outdoor-air-system-zone-node}
+
+This field contains the name of an air node for a thermal zone that is ultimately connected to the air system. This node is used with the setpoint schedule, defined in the following field, to provide an added layer of thermostatic control for the UTSC without affecting the control of auxiliary heating. If there is a single air system that is connected to more than one zone, then a single zone should be selected based on where the thermostat might be located.
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+SolarCollector:UnglazedTranspired:Multisystem,
+  OFFICE MultiSystem OA UTSC ,   ! Solar Collector Name
+  Outside Air Inlet Node ZN1,     ! Outdoor Air System 1 Collector Inlet Node
+  UTSC Outlet Node ZN1,                 ! Outdoor Air System 1 Collector Outlet Node
+  Mixed Air Node ZN1,                     ! Outdoor Air System 1 Mixed Air Node
+  ZN1 Node,                                         ! Outdoor Air System 1 Zone Node
+  Outside Air Inlet Node ZN2,     ! Outdoor Air System 2 Collector Inlet Node
+  UTSC Outlet Node ZN2,                 ! Outdoor Air System 2 Collector Outlet Node
+  Mixed Air Node ZN2,                     ! Outdoor Air System 2 Mixed Air Node
+  ZN2 Node,                                         ! Outdoor Air System 2 Zone Node
+  Outside Air Inlet Node ZN3,     ! Outdoor Air System 3 Collector Inlet Node
+  UTSC Outlet Node ZN3,                 ! Outdoor Air System 3 Collector Outlet Node
+  Mixed Air Node ZN3,                     ! Outdoor Air System 3 Mixed Air Node
+  ZN3 Node,                                         ! Outdoor Air System 3 Zone Node
+  Outside Air Inlet Node ZN4,     ! Outdoor Air System 4 Collector Inlet Node
+  UTSC Outlet Node ZN4,                 ! Outdoor Air System 4 Collector Outlet Node
+  Mixed Air Node ZN4,                     ! Outdoor Air System 4 Mixed Air Node
+  ZN4 Node,                                         ! Outdoor Air System 4 Zone Node
+  Outside Air Inlet Node ZN5,     ! Outdoor Air System 5 Collector Inlet Node
+  UTSC Outlet Node ZN5,                 ! Outdoor Air System 5 Collector Outlet Node
+  Mixed Air Node ZN5,                     ! Outdoor Air System 5 Mixed Air Node
+  ZN5 Node;                                         ! Outdoor Air System 5 Zone Node
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-surface-construction-elements.tex b/doc/input-output-reference/src/overview/group-surface-construction-elements.tex
new file mode 100644
index 00000000000..4bce174292e
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-surface-construction-elements.tex
@@ -0,0 +1,4288 @@
+\section{Group -- Surface Construction Elements}\label{group-surface-construction-elements}
+
+This group of objects describes the physical properties and configuration for the building envelope and interior elements. That is, the walls, roofs, floors, windows, doors for the building.
+
+\subsection{Specifying the Building Envelope}\label{specifying-the-building-envelope}
+
+Building element constructions in EnergyPlus are built from the basic thermal and other material property parameters in physical constructions. Materials are specified by types~ and named. Constructions are defined by the composition of materials. Finally, surfaces are specified for the building with geometric coordinates as well as referenced constructions.
+
+\subsection{Material and Material Properties}\label{material-and-material-properties}
+
+There are several material ``types'' which may be used to describe layers within opaque construction elements. The choice of which of these types to use is left up to the user. However, some guidance as to which material type to use is appropriate before describing each in detail. The opaque types are:
+
+\begin{itemize}
+\item
+  Material
+\item
+  Material:NoMass
+\item
+  Material:AirGap
+\item
+  Material:RoofVegetation
+\item
+  Material:InfraredTransparent
+\end{itemize}
+
+Material is the ``preferred'' type of material. This requires knowledge of many of the thermal properties of the material, but it allows EnergyPlus to take into account the thermal mass of the material and thus allows the evaluation of transient conduction effects. Material:NoMass is similar in nature but only requires the thermal resistance (R-value) rather than the thickness, thermal conductivity, density, and specific heat. Note that using a simple R-value only material forces EnergyPlus to assume steady state heat conduction through this material layer. Finally, Material:AirGap should only be used for an air gap between other layers in a construction. This type assumes that air is sufficiently lightweight to require only an R-value. In addition, since it is not exposed to any external environment, surface properties such as absorptance are not necessary. Material:RoofVegetation is used to help model ``green roofs''. Material:InfraredTransparent is used similarly to the NoMass materials. Each of these materials is described in more detail below.
+
+There are several material additions that can be made to the basic material properties. These additional material types are:
+
+\begin{itemize}
+\item
+  MaterialProperty:MoisturePenetrationDepth:Settings
+\item
+  Material\-Prop\-erty:\-Heat\-And\-Moisture\-Trans\-fer:\-Sorp\-tion\-Iso\-therm
+\item
+  MaterialProperty:HeatAndMoistureTransfer:Diffusion
+\item
+  MaterialProperty:HeatAndMoistureTransfer:Settings
+\item
+  Material\-Prop\-erty:\-Heat\-And\-Moisture\-Trans\-fer:\-Re\-dist\-ribu\-tion
+\item
+  MaterialProperty:HeatAndMoistureTransfer:Suction
+\item
+  Material\-Prop\-erty:\-Heat\-And\-Moisture\-Trans\-fer:\-Thermal\-Con\-ductivity
+\item
+  MaterialProperty:PhaseChange
+\end{itemize}
+
+These material property objects are used in conjunction with the basic material specification and reference back to the name of the basic material type. Without the basic material type specified the program, will give a severe error and terminate. For example, specifying the moisture materials and changing the HeatBalanceAlgorithm to a moisture simulation will allow the moisture simulation to take place.
+
+\subsection{Material}\label{material}
+
+This definition should be used when the four main thermal properties (thickness, conductivity, density, and specific heat) of the material are known. This syntax is used to describe opaque construction elements only.
+
+When a Material is used for the Construction of a building surface, care should be taken to not attempt to model assemblies that were not included in the intended scope of applicability for the underlying heat transfer models.~ The building surface models are for normal applications to building energy efficiency where the main focus is on assemblies with some thermal resistance. Extremely thin and/or highly conductive material layers should be neglected from the Construction rather than included because they will not contribute to the assembly's overall thermal resistance or heat capacity. For some cases, thin and/or highly conductive materials are a serious problem for the heat transfer modeling and the values for thickness, conductivity, density and specific heat are checked for appropriateness. This check calculates the Material's thermal diffusivity from the inputs for conductivity, density, and specific heat and compares it to a maximum threshold of 1.E-5 (m\(^{2}\)/s). If the diffusivity is above this threshold, then the program checks if the layer is sufficiently thick and may issue a warning if it is too thin and highly conductive.
+
+The absorptance values in this object impart surface properties to the construction and should be applied to the thermally significant inner and outer layers in the overall assembly.~ Attempting to trick the program by modeling thin ``paint'' layers to apply surface properties is not a good idea; the models were not intended to support such strategies.
+
+\subsubsection{Inputs}\label{inputs-046}
+
+\paragraph{Field: Name}\label{field-name-045}
+
+This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data (ref: Construction object).
+
+\paragraph{Field: Roughness}\label{field-roughness-000}
+
+This alpha field defines the relative roughness of a particular material layer. This parameter only influences the convection coefficients, more specifically the exterior convection coefficient. A special keyword is expected in this field with the options being ``VeryRough'', ``Rough'', ``MediumRough'', ``MediumSmooth'', ``Smooth'', and ``VerySmooth'' in order of roughest to smoothest options.
+
+\paragraph{Field: Thickness}\label{field-thickness}
+
+This field characterizes the thickness of the material layer in meters. This should be the dimension of the layer in the direction perpendicular to the main path of heat conduction. This value must be a positive. \textbf{Modeling layers thinner (less) than 0.003 m is not recommended; rather, add those properties to one of the adjacent layers.}
+
+\paragraph{Field: Conductivity}\label{field-conductivity}
+
+This field is used to enter the thermal conductivity of the material layer. Units for this parameter are W/(m-K). Thermal conductivity must be greater than zero. \textbf{Modeling layers with conductivity higher than 5.0 W/(m-K) is not recommended; however, this may be appropriate for non-surfaces such as pipes and TDDs (ref. DaylightingDevice:Tubular object).}
+
+\paragraph{Field: Density}\label{field-density}
+
+This field is used to enter the density of the material layer in units of kg/m\(^{3}\). Density must be a positive quantity. \textbf{In some cases textbooks and references may use g/m\(^{3}\): be careful to not confuse units.}
+
+\paragraph{Field: Specific Heat}\label{field-specific-heat}
+
+This field represents the specific heat of the material layer in units of J/(kg-K). Note that these units are most likely different than those reported in textbooks and references which tend to use kJ/(kg-K) or J/(g-K). They were chosen for internal consistency within EnergyPlus. \textbf{Only values of specific heat of 100 or larger are allowed. Typical ranges are from 800 to 2000 J/(kg-K).}
+
+\paragraph{Field: Thermal Absorptance}\label{field-thermal-absorptance}
+
+The thermal absorptance field in the Material input syntax represents the fraction of incident long wavelength radiation that is absorbed by the material. This parameter is used when calculating the long wavelength radiant exchange between various surfaces and affects the surface heat balances (both inside and outside as appropriate). For long wavelength radiant exchange, thermal emissivity and thermal emittance are equal to thermal absorptance. Values for this field must be between 0.0 and 1.0 (with 1.0 representing ``black body'' conditions). The default value for this field is 0.9.
+
+\paragraph{Field: Solar Absorptance}\label{field-solar-absorptance}
+
+The solar absorptance field in the Material input syntax represents the fraction of incident~ solar radiation that is absorbed by the material. Solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident solar radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate). If solar reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.0 and 1.0. The default value for this field is 0.7.
+
+\paragraph{Field: Visible Absorptance}\label{field-visible-absorptance}
+
+The visible absorptance field in the Material input syntax represents the fraction of incident visible wavelength radiation that is absorbed by the material. Visible wavelength radiation is slightly different than solar radiation in that the visible band of wavelengths is much more narrow while solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident visible radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate) as well as the daylighting calculations. If visible reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.0 and 1.0. The default value for this field is 0.7.
+
+An IDF example:
+
+\begin{lstlisting}
+
+Material,A2 - 4 IN DENSE FACE BRICK,  ! Material Name
+   Rough,  ! Roughness
+    0.1014984    ,  ! Thickness {m}
+     1.245296    ,   ! Conductivity {W/M*K}
+     2082.400    ,   ! Density {Kg/M**3}
+    920.4800    ,   ! Specific Heat {J/Kg*K}
+    0.9000000    ,   ! Thermal Absorptance
+    0.9300000    ,   ! Solar Absorptance
+    0.9300000    ;   ! Visible Absorptance
+\end{lstlisting}
+
+\subsection{Material:NoMass}\label{materialnomass}
+
+Use this definition when only the thermal resistance (R value) of the material is known. This object is used to describe opaque construction elements.
+
+\subsubsection{Inputs}\label{inputs-1-043}
+
+\paragraph{Field: Name}\label{field-name-1-042}
+
+This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data (ref: Construction object).
+
+\paragraph{Field: Roughness}\label{field-roughness-1}
+
+This alpha field defines the relative roughness of a particular material layer. This parameter only influences the convection coefficients, more specifically the exterior convection coefficient. A~ keyword is expected in this field with the options being ``\textbf{VeryRough}'', ``\textbf{Rough}'', ``\textbf{MediumRough}'', ``\textbf{MediumSmooth}'', ``\textbf{Smooth}'', and ``\textbf{VerySmooth}'' in order of roughest to smoothest options.
+
+\paragraph{Field: Thermal Resistance}\label{field-thermal-resistance}
+
+This field is used to enter the thermal resistance (R-value) of the material layer. Units for this parameter are (m\(^{2}\)-K)/W. Thermal resistance must be greater than zero. Note that most R-values in the USA are calculated in Inch-Pound units and must be converted to the SI equivalent.
+
+\paragraph{Field: Thermal Absorptance}\label{field-thermal-absorptance-1}
+
+The thermal absorptance field in the Material input syntax represents the fraction of incident long wavelength radiation that is absorbed by the material. This parameter is used when calculating the long wavelength radiant exchange between various surfaces and affects the surface heat balances (both inside and outside as appropriate). For long wavelength radiant exchange, thermal emissivity and thermal emittance are equal to thermal absorptance. Values for this field must be between 0.0 and 1.0 (with 1.0 representing ``black body'' conditions). The default value for this field is 0.9.
+
+\paragraph{Field: Solar Absorptance}\label{field-solar-absorptance-1}
+
+The solar absorptance field in the Material input syntax represents the fraction of incident~ solar radiation that is absorbed by the material. Solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident solar radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate). If solar reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.0 and 1.0. The default value for this field is 0.7.
+
+\paragraph{Field: Visible Absorptance}\label{field-visible-absorptance-1}
+
+The visible absorptance field in the Material input syntax represents the fraction of incident visible wavelength radiation that is absorbed by the material. Visible wavelength radiation is slightly different than solar radiation in that the visible band of wavelengths is much more narrow while solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident visible radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate) as well as the daylighting calculations. If visible reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.0 and 1.0. The default value for this field is 0.7.
+
+An IDF example:
+
+\begin{lstlisting}
+
+Material:NoMass,R13LAYER,  ! Material Name
+   Rough,  ! Roughness
+     2.290965    ,  ! Resistance {M**2K/W}
+    0.9000000    ,   ! Thermal Absorptance
+    0.7500000    ,   ! Solar Absorptance
+    0.7500000    ;   ! Visible Absorptance
+\end{lstlisting}
+
+\subsection{Material:InfraredTransparent}\label{materialinfraredtransparent}
+
+A Infrared Transparent surface is similar to a resistance-only surface.~ The idd object for this type of surface is shown below.~ The surface will actually participate in the transfer of visible and solar radiation by doing a wavelength transformation and making all short wave length radiation that is incident on the surface into long wave length radiation and having it participate in the long wavelength radiant exchange.~ \textbf{Note the ConvectionCoefficient instructions that follow the Infrared Transparent construction object below}.
+
+\subsubsection{Inputs}\label{inputs-2-040}
+
+\paragraph{Field: Name}\label{field-name-2-037}
+
+This field contains the unique name (across all Material objects) for the Infrared Transparent material.
+
+A Infrared Transparent surface should not participate in a convective/conductive exchange between the zones it separates.~ In order to minimize this effect, the ConvectionCoefficients object must be used for the surfaces referencing the Infrared Transparent (IRT) construction.
+
+An example idf object specification for use with the IRT surface is shown below. Note that surfaces are not described in this example
+
+\begin{lstlisting}
+
+Material:InfraredTransparent,
+      IRTMaterial1;            !- Name
+
+
+  Construction,
+      IRTSurface,              !- Name
+      IRTMaterial1;            !- Outside Layer
+
+
+  SurfaceProperty:ConvectionCoefficients,
+      Bottom:Top,              !- SurfaceName
+      Outside,                 !- Convection Type 1
+      value,                   !- Convection Value Type 1
+      0.1,                     !- Convection value 1 {W/m2-K}
+      ,                        !- Convection Schedule 1
+      Inside,                  !- Convection Type 2
+      value,                   !- Convection Value Type 2
+      0.1;                     !- Convection value 2 {W/m2-K}
+
+
+  SurfaceProperty:ConvectionCoefficients,
+      SecondLevel:Bottom,      !- SurfaceName
+      Outside,                 !- Convection Type 1
+      value,                   !- Convection Value Type 1
+      0.1,                     !- Convection value 1 {W/m2-K}
+      ,                        !- Convection Schedule 1
+      Inside,                  !- Convection Type 2
+      value,                   !- Convection Value Type 2
+      0.1;                     !- Convection value 2 {W/m2-K}
+
+
+  SurfaceProperty:ConvectionCoefficients,
+      SecondLevel:Top,         !- SurfaceName
+      Outside,                 !- Convection Type 1
+      value,                   !- Convection Value Type 1
+      0.1,                     !- Convection value 1 {W/m2-K}
+      ,                        !- Convection Schedule 1
+      Inside,                  !- Convection Type 2
+      value,                   !- Convection Value Type 2
+      0.1;                     !- Convection value 2 {W/m2-K}
+
+
+  SurfaceProperty:ConvectionCoefficients,
+      ThirdLevel:Bottom,       !- SurfaceName
+      Outside,                 !- Convection Type 1
+      value,                   !- Convection Value Type 1
+      0.1,                     !- Convection value 1 {W/m2-K}
+      ,                        !- Convection Schedule 1
+      Inside,                  !- Convection Type 2
+      value,                   !- Convection Value Type 2
+      0.1;                     !- Convection value 2 {W/m2-K}
+\end{lstlisting}
+
+\subsection{Material:AirGap}\label{materialairgap}
+
+This material is used to describe the air gap in an opaque construction element. Glass elements use a different property (WindowGas) to describe the air between two glass layers.
+
+\subsubsection{Inputs}\label{inputs-3-036}
+
+\paragraph{Field: Name}\label{field-name-3-031}
+
+This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data (ref: Construction object).
+
+\paragraph{Field: Thermal Resistance}\label{field-thermal-resistance-1}
+
+This field is used to enter the thermal resistance (R-value) of the material layer. Units for this parameter are (m\(^{2}\)-K)/W. Thermal resistance must be greater than zero. Note that most R-values in the USA are calculated in Inch-Pound units and must be converted to the SI equivalent.
+
+An IDF example:
+
+\begin{lstlisting}
+
+Material:AirGap,B1 - AIRSPACE RESISTANCE,  ! Material Name
+    0.1603675    ;  ! Resistance {M**2K/W}
+\end{lstlisting}
+
+\subsection{MaterialProperty:MoisturePenetrationDepth:Settings}\label{materialpropertymoisturepenetrationdepthsettings}
+
+This material is used to describe the five moisture material properties that are used in the EMPD (Effective Moisture Penetration Depth) heat balance solution algorithm (known there as MoisturePenetrationDepthConductionTransferFunction). The EMPD algorithm is a simplified, lumped moisture model that simulates moisture storage and release from interior surfaces. The model uses ``actual'' convective mass transfer coefficients that are determined by existing heat and mass transfer relationships, e.g.~the Lewis relation. An effective moisture penetration depth may be determined from either experimental or detailed simulation data by using actual surface areas and moisture sorption isotherms.
+
+This moisture model will be used when the appropriate EMPD moisture materials are specified and the Solution Algorithm parameter is set to EMPD.
+
+\subsubsection{Inputs}\label{inputs-4-033}
+
+\paragraph{Field: Name}\label{field-name-4-028}
+
+This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data (ref: Construction object).
+
+\paragraph{Field: Moisture Penetration Depth}\label{field-moisture-penetration-depth}
+
+This field is used to enter the effective moisture penetration depth of the material layer. Units for this parameter are (m).
+
+\paragraph{Field: Constants to Define Moisture Equilibrium Equation}\label{field-constants-to-define-moisture-equilibrium-equation}
+
+The next four fields, coefficients ``a'', ``b'', ``c'', and ``d'', help define the sorption isotherm curve used for building materials under equilibrium conditions. They are used to define the relationship between the material's moisture content and the surface air relative humidity (ref: Effective Moisture Penetration Depth (EMPD) Model in the Engineering Reference):
+
+\begin{equation}
+U = a{\varphi ^b} + c{\varphi ^d}
+\end{equation}
+
+where
+
+a,b,c,d~~~~~~~~~ ~~~~ = Coefficients to define the relationship between the material's moisture content and the surface air relative humidity
+
+U~~~~~~~~~~~~~~~~~~~~~ = Moisture content defined as the mass fraction of water contained in a material {[}kg/kg{]}
+
+\(\varphi\) ~~~~~~~~~~~~~~~~~~~ = Surface air relative humidity {[}0 to 1{]}
+
+\paragraph{The next four fields are dimensionless coefficients:}\label{the-next-four-fields-are-dimensionless-coefficients}
+
+\paragraph{Field: Moisture Equation Coefficient a}\label{field-moisture-equation-coefficient-a}
+
+\paragraph{Field: Moisture Equation Coefficient b}\label{field-moisture-equation-coefficient-b}
+
+\paragraph{Field: Moisture Equation Coefficient c}\label{field-moisture-equation-coefficient-c}
+
+\paragraph{Field: Moisture Equation Coefficient d}\label{field-moisture-equation-coefficient-d}
+
+Ann IDF example showing how it is used in conjunction with Material in synchronous pairs:
+
+\begin{lstlisting}
+
+  Material,
+      E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Name
+      Smooth,                  !- Roughness
+      1.9050000E-02,           !- Thickness {m}
+      0.7264224,               !- Conductivity {W/m-K}
+      1601.846,                !- Density {kg/m3}
+      836.8000,                !- Specific Heat {J/kg-K}
+      0.9000000,               !- Thermal Absorptance
+      0.9200000,               !- Solar Absorptance
+      0.9200000;               !- Visible Absorptance
+
+
+
+
+   MaterialProperty:MoisturePenetrationDepth:Settings,
+      E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Name
+      0.004,                   !- Effective Moisture Penetration Depth {m}
+      0.072549,           !- Moisture Equation Coefficient a {dimensionless}
+      0.397173,           !- Moisture Equation Coefficient b {dimensionless}
+      0.007774,           !- Moisture Equation Coefficient c {dimensionless}
+      11.7057;            !- Moisture Equation Coefficient d {dimensionless}
+
+
+    Material,
+      C10 - 8 IN HW CONCRETE,  !- Name
+      MediumRough,             !- Roughness
+      0.2033016,               !- Thickness {m}
+      1.729577,                !- Conductivity {W/m-K}
+      2242.585,                !- Density {kg/m3}
+      836.8000,                !- Specific Heat {J/kg-K}
+      0.9000000,               !- Thermal Absorptance
+      0.6500000,               !- Solar Absorptance
+      0.6500000;               !- Visible Absorptance
+
+
+   MaterialProperty:MoisturePenetrationDepth:Settings,
+      C10 - 8 IN HW CONCRETE,  !- Name
+      0.004,                   !- Effective Moisture Penetration Depth {m}
+      0.018062,             !- Moisture Equation Coefficient a {dimensionless}
+      0.451879,             !- Moisture Equation Coefficient b {dimensionless}
+      0.026178,             !- Moisture Equation Coefficient c {dimensionless}
+      10.8356;              !- Moisture Equation Coefficient d {dimensionless}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-035}
+
+Output variables applicable to heat transfer surfaces using EMPD model:
+
+\begin{itemize}
+\item
+  Zone,Average,EMPD Surface Inside Face Water Vapor Density {[}kg/m3{]}
+\item
+  Zone,Average,EMPD Surface Inside Face Humidity Ratio {[}kgWater/kgDryAir{]}
+\item
+  Zone,Average,EMPD Surface Inside Face Relative Humidity {[}\%{]}
+\end{itemize}
+
+The following variables apply only to surfaces, where the material assigned to the inside layers is MaterialProperty:MoisturePenetrationDepth:Settings. The EMPD (Effective Moisture Penetration Depth) moisture balance solution algorithm is used to calculate the inside surface moisture levels.
+
+\paragraph{EMPD Surface Inside Face Water Vapor Density {[}kg/m3{]}}\label{empd-surface-inside-face-water-vapor-density-kgm3}
+
+The vapor density at the inside surface, where the EMPD moisture balance solution algorithm is applied.
+
+\paragraph{EMPD Surface Inside Face Humidity Ratio {[}kgWater/kgDryAir{]}}\label{empd-surface-inside-face-humidity-ratio-kgwaterkgdryair}
+
+The humidity ratio at the inside surface, where the EMPD moisture balance solution algorithm is applied.
+
+\paragraph{EMPD Surface Inside Face Relative Humidity {[}\%{]}}\label{empd-surface-inside-face-relative-humidity}
+
+The relative humidity at the inside surface, where the EMPD moisture balance solution algorithm is applied.
+
+\subsection{MaterialProperty:PhaseChange}\label{materialpropertyphasechange}
+
+\textbf{Advanced/Research Usage:} This material is used to describe the temperature dependent material properties that are used in the Conduction Finite Difference solution algorithm. This conduction model is done when the appropriate materials are specified and the Solution Algorithm parameter is set toConductionFiniteDifference. This permits simulating temperature dependent thermal conductivity and phase change materials (PCM) in EnergyPlus.
+
+\subsubsection{Inputs}\label{inputs-5-030}
+
+\paragraph{Field: Name}\label{field-name-5-024}
+
+This field is a regular material name specifying the material with which this additional temperature dependent property information will be associated.
+
+\paragraph{Field: Temperature Coefficient for Thermal Conductivity}\label{field-temperature-coefficient-for-thermal-conductivity}
+
+This field is used to enter the temperature dependent coefficient for thermal conductivity of the material.~ Units for this parameter are (W/(m-K\(^{2}\)). This is the thermal conductivity change per unit temperature excursion from 20 C. The conductivity value at 20 C is the one specified with the basic material properties of the regular material specified in the name field. The thermal conductivity is obtained from:
+
+\begin{equation}
+k = {k_o} + {k_1}({T_i} - 20)
+\end{equation}
+
+where:
+
+k\(_{o}\) is the 20C value of thermal conductivity(normal idf~ input)
+
+k\(_{1}\) is the change in conductivity per degree temperature difference from 20C
+
+(this field).
+
+\paragraph{Field Set: Temperature-Enthalpy}\label{field-set-temperature-enthalpy}
+
+The temperature -- enthalpy set of inputs specify a two column tabular temperature-enthalpy function for the basic material. Sixteen pairs can be specified. Specify only the number of pairs necessary. The tabular function must cover the entire temperature range that will be seen by the material in the simulation. It is suggested that the function start at a low temperature, and extend to 100C. Note that the function has no negative slopes and the lowest slope that will occur is the base material specific heat. Temperature values should be strictly increasing. Enthalpy contributions of the phase change are always added to the enthalpy that would result from a constant specific heat base material. An example of a simple enthalpy temperature function is shown below.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image024.png}
+\caption{Temp-Enth Example \protect \label{fig:temp-enth-example}}
+\end{figure}
+
+\paragraph{Field: Temperature x}\label{field-temperature-x}
+
+This field is used to specify the temperature of the temperature-enthalpy function for the basic material. Units are C.
+
+\paragraph{Field: Enthalpy x}\label{field-enthalpy-x}
+
+This field specifies the enthalpy that corresponds to the previous temperature of the temperature-enthalpy function. Units are J/kg.
+
+And, an IDF example showing how it is used in conjunction with the Material:
+
+Note, the following Heat Balance Algorithm is necessary (only specified once). Also, when using ConductionFiniteDifference, it is more efficient to set the zone timestep shorter than those used for the ConductionTransferFunction solution algorithm. It should be set to 12 timesteps per hour or greater, and can range up to 60.
+
+\begin{lstlisting}
+
+HeatBalanceAlgorithm,
+  ConductionFiniteDifference;
+
+
+  Timestep,
+  12;
+
+
+  Material,
+      E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Name
+      Smooth,                  !- Roughness
+      1.9050000E-02,           !- Thickness {m}
+      0.7264224,               !- Conductivity {W/m-K}
+      1601.846,                !- Density {kg/m3}
+      836.8000,                !- Specific Heat {J/kg-K}
+      0.9000000,               !- Thermal Absorptance
+      0.9200000,               !- Solar Absorptance
+      0.9200000;               !- Visible Absorptance
+
+
+  MaterialProperty:PhaseChange,
+      E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Name
+      0.0,             !- Temperature coefficient,thermal conductivity(W/m K2)
+      -20.,            !- Temperature 1, C
+      0.01,            !- Enthalpy 1 at –20C, (J/kg)
+      20.,             !- Temperature 2, C
+      33400,           !- Enthalpy 2, (J/kg)
+      20.5,            !- temperature 3, C
+      70000,           !- Ethalpy 3, (J/kg)
+      100.,            !- Temperature 4, C
+      137000;          !- Enthalpy 4, (J/kg)
+\end{lstlisting}
+
+\subsection{MaterialProperty:VariableThermalConductivity}\label{materialpropertyvariablethermalconductivity}
+
+This object is used to describe the temperature dependent material properties that are used in the CondFD (Conduction Finite Difference) solution algorithm. This conduction model is used when the appropriate CondFD materials are specified and the Solution Algorithm parameter is set to condFD.
+
+\subsubsection{Inputs}\label{inputs-6-027}
+
+\paragraph{Field: Name}\label{field-name-6-022}
+
+This field is a regular material name specifying the material with which this additional temperature dependent property information will be associated.
+
+\paragraph{Field Set: Temperature-Thermal Conductivity}\label{field-set-temperature-thermal-conductivity}
+
+The temperature -- conductivity set of inputs specify a two column tabular temperature-thermal conductivity function for the basic material. Ten pairs can be specified. Specify only the number of pairs necessary. Temperature values should be strictly increasing.
+
+\paragraph{Field: Temperature x}\label{field-temperature-x-1}
+
+This field is used to specify the temperature of the temperature-conductivity function for the basic material. Units are C.
+
+\paragraph{Field: Thermal Conductivity x}\label{field-thermal-conductivity-x}
+
+This field specifies the conductivity that corresponds to the temperature (previous field) of the temperature-conductivity function. Units are W/m-K.
+
+And, an IDF example showing how it is used in conjunction with the Materials:
+
+Note, the following Heat Balance Algorithm is necessary (only specified once). Also, when using Conduction Finite Difference, it is more efficient to set the zone time step shorter than those used for the Conduction Transfer Function solution algorithm. It should be set to 12 time steps per hour or greater, and can range up to 60.
+
+\begin{lstlisting}
+
+HeatBalanceAlgorithm,
+  ConductionFiniteDifference;
+
+
+  Timestep,
+  12;
+
+
+  Material,
+      PCMPlasterBoard ,      !- Name
+      Smooth,                  !- Roughness
+      1.9050000E-02,           !- Thickness {m}
+      4.2,                     !- Conductivity {W/m-K}
+      1601.846,                !- Density {kg/m3}
+      836.8000,                !- Specific Heat {J/kg-K}
+      0.9000000,               !- Thermal Absorptance
+      0.9200000,               !- Solar Absorptance
+      0.9200000;               !- Visible Absorptance
+
+
+  MaterialProperty:VariableThermalConductivity,
+      PCMPlasterBoard,         !- Name
+      0,                       !- Temperature 1 {C}
+      4.2,                     !- Thermal Conductivity 1 {W/m-K}
+      22,                      !- Temperature 2 {C}
+      4.2,                     !- Thermal Conductivity 2 {W/m-K}
+      22.1,                    !- Temperature 3 {C}
+      2.5,                     !- Thermal Conductivity 3 {W/m-K}
+      100,                     !- Temperature 4 {C}
+      2.5;                     !- Thermal Conductivity 4 {W/m-K}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-026}
+
+The Conduction Finite Difference solution algorithm uses a finite difference solution technique, the surfaces are divided into a nodal arrangement. The only output specific to Conduction Finite Difference solution (that is not include in other surface outputs) is node temperatures.
+
+The following output variables are applicable to all opaque heat transfer surfaces when using Solution Algorithms ConductionFiniteDifference:
+
+\begin{itemize}
+\item
+  Zone,Sum,CondFD Inner Solver Loop Iteration Count {[]}
+\item
+  Zone,Average,CondFD Surface Temperature Node \textless{}1\textgreater{} {[}C{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{CondFD Inner Solver Loop Iteration Count {[]}}{CondFD Inner Solver Loop Iteration Count }}\label{condfd-inner-solver-loop-iteration-count}
+
+This outputs the count of iterations on the inner solver loop of CondFD for each surface.
+
+\paragraph{CondFD Surface Temperature Node \textless{}X\textgreater{} {[}C{]}}\label{condfd-surface-temperature-node-x-c}
+
+This will output temperatures for a node in the surfaces being simulated with ConductionFiniteDifference. The key values for this output variable are the surface name. The nodes are numbered from outside to inside of the surface. The full listing will appear in the RDD file
+
+\paragraph{CondFD Surface Heat Flux Node \textless{}X\textgreater{} {[}W/m2{]}}\label{condfd-surface-heat-flux-node-x-wm2}
+
+This will output heat flux at each node in surfaces being simulated with ConductionFiniteDifference. The key values for this output variable are the surface name. The nodes are numbered from outside to inside of the surface. The full listing will appear in the RDD file. A positive value indicates heat flowing towards the inside face of the surface. Note that this matches the sign convention for Surface Inside Face Conduction Heat Transfer Rate per Area and is opposite the sign of Surface OUtside Face Conduction Heat Transfer Rate per Area.
+
+\paragraph{CondFD Surface Heat Capacitance Outer Half Node \textless{}X\textgreater{} {[}W/m2-K{]}}\label{condfd-surface-heat-capacitance-outer-half-node-x-wm2-k}
+
+\paragraph{CondFD Surface Heat Capacitance Inner Half Node \textless{}X\textgreater{} {[}W/m2-K{]}}\label{condfd-surface-heat-capacitance-inner-half-node-x-wm2-k}
+
+These will output the half-node heat capacitance in surfaces being simulated with ConductionFiniteDifference. The key values for this output variable are the surface name. The nodes are numbered from outside to inside of the surface. The full listing will appear in the RDD file. For this output, the heat capacitance is defined as the product of specific heat, density, and node thickness. Zero is reported for R-layer half-nodes and for undefined half-nodes. There is no outer half-node for Node 1 which is the outside face of the surface, and there is no inner half-node for Node N which is the inside face of the surface. CondFD Surface Heat Capacitance is only available with Output:Diagnostics,DisplayAdvancedReportVariables.
+
+\subsection{MaterialProperty:HeatAndMoistureTransfer:Settings}\label{materialpropertyheatandmoisturetransfersettings}
+
+\textbf{Advanced/Research Usage:} This object is used to describe two of the seven additional material properties needed for the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm. The settings object is used when the solutions algorithm is set to CombinedHeatAndMoistureFiniteElement and the appropriate material properties are assigned to each material. This permits the simulation of the moisture dependant thermal properties of the material as well as the transfer of moisture through, into and out of the material into the zone or exterior.
+
+In addition to the Porosity and Initial Water content properties described here, five additional properties, described by tabulated relationships between variables, are required. These properties are;
+
+\begin{itemize}
+\item
+  MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm
+\item
+  MaterialProperty:HeatAndMoistureTransfer:Suction
+\item
+  MaterialProperty:HeatAndMoistureTransfer:Redistribution
+\item
+  MaterialProperty:HeatAndMoistureTransfer:Diffusion
+\item
+  MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity
+\end{itemize}
+
+All materials in a construction are required to have all material properties defined for HAMT to work.
+
+Within the MaterialProperty:HeatAndMoistureTransfer:Settings object the following fields are defined.
+
+\subsubsection{Inputs}\label{inputs-7-026}
+
+\paragraph{Field: Material Name}\label{field-material-name-000}
+
+This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
+
+\paragraph{Field: Porosity}\label{field-porosity}
+
+The porosity of a material is the maximum fraction, by volume, of a material that can be taken up with water. The units are {[}m3/m3{]}.
+
+\paragraph{Field: Initial Water Content Ratio}\label{field-initial-water-content-ratio}
+
+For this solution algorithm, the initial water content is assumed to be distributed evenly through the depth of the material. The units are {[}kg/kg{]}.
+
+Below is an example input for the porosity and initial water content of a material.
+
+\begin{lstlisting}
+
+MaterialProperty:HeatAndMoistureTransfer:Settings,
+        Concrete,     !- Name
+        0.76,     !- Porosity
+        0.2;     !- Initial (or typical) Water content
+\end{lstlisting}
+
+\subsection{MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm}\label{materialpropertyheatandmoisturetransfersorptionisotherm}
+
+\textbf{Advanced/Research Usage:} This material property is used in conjunction with the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm.
+
+The Isotherm data relates the moisture, or water content {[}kg/m3{]} of a material with the relative humidity (RH). The water content is expected to increase as relative humidity increases, starting at zero content at 0.0relative humidity fraction and reaching a maximum, defined by the porosity, at 1.0 relative humidity fraction, which corresponds to 100\% relatve humidity. Relative humidities are entered as fraction for this object ranging from 0.0 to 1.0. These two extremes (0.0 and 1.0) are automatically set by the HAMT solution. However, if they are entered they will be used as extra data points. Data should be provided with increasing RH and moisture content up to as high an RH as possible to provide a stable solution. One possible reason for the following error message may be that a material has a very rapid increase in water content for a small change in RH, which can happen if the last entered water content point is at a low RH and the material has a very high porosity.
+
+\begin{lstlisting}
+  ** Warning ** HeatAndMoistureTransfer: Large Latent Heat for Surface ROOF
+\end{lstlisting}
+
+Another potential reason for this error being generated is the use of inappropriate values for Vapor Transfer Coefficients. See the SurfaceProperties:VaporCoefficients object in the Advanced Surface Concepts group.
+
+\subsubsection{Inputs}\label{inputs-8-024}
+
+\paragraph{Field: Material Name}\label{field-material-name-1}
+
+This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
+
+\paragraph{Field: Number of data ~Coordinates}\label{field-number-of-data-coordinates}
+
+A maximum of 25 coordinates can be specified.
+
+\paragraph{Field Set: Relative Humidity-Moisture Content}\label{field-set-relative-humidity-moisture-content}
+
+\paragraph{Field: Relative Humidity Fraction x}\label{field-relative-humidity-fraction-x}
+
+The relative humidity of the x\(^{th}\) coordinate. The relative humidity is entered as fraction, not in percent.
+
+\paragraph{Field: Moisture Content x}\label{field-moisture-content-x}
+
+The Moisture Content of the x\(^{th}\) coordinate. The units are {[}kg/m3{]}
+
+Below is an example input for a material isotherm
+
+\begin{lstlisting}
+
+MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm,
+        Concrete,     !- Name
+        10,     !- Number of data Coordinates
+        0.2205,    !- Relative Humidity fraction #1
+        22.31,     !- Moisture content #1
+        0.202,     !- Relative Humidity fraction #2
+        19.665,    !- Moisture content #2
+        0.449,     !- Relative Humidity fraction #3
+        40.02,     !- Moisture content #3
+        0.454,     !- Relative Humidity fraction #4
+        36.915,    !- Moisture content #4
+        0.6506,    !- Relative Humidity fraction #5
+        56.005,    !- Moisture content #5
+        0.655,     !- Relative Humidity fraction #6
+        52.325,    !- Moisture content #6
+        0.824,     !- Relative Humidity fraction #7
+        72.565,    !- Moisture content #7
+        0.8725,    !- Relative Humidity fraction #8
+        85.1,      !- Moisture content #8
+        0.924,     !- Relative Humidity fraction #9
+        91.08,     !- Moisture content #9
+        0.964,     !- Relative Humidity fraction #10
+        100.28;    !- Moisture content #10
+\end{lstlisting}
+
+\subsection{MaterialProperty:HeatAndMoistureTransfer:Suction}\label{materialpropertyheatandmoisturetransfersuction}
+
+\textbf{Advanced/Research Usage:}This material property is used in conjunction with the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm.
+
+The suction data relates the liquid transport coefficient, under suction, to the water content of a material. A data point at zero water content is required. The liquid transport coefficient at the highest entered water content value is used for all liquid transport coefficient values above this water content. These coefficients are used by HAMT when the rain flag is set in the weather file.
+
+\subsubsection{Inputs}\label{inputs-9-022}
+
+\paragraph{Field: Material Name}\label{field-material-name-2}
+
+This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
+
+\paragraph{Field: Number of Suction points}\label{field-number-of-suction-points}
+
+A maximum of 25 points can be specified.
+
+\paragraph{Field Set: Moisture Content-Liquid Transport Coefficient}\label{field-set-moisture-content-liquid-transport-coefficient}
+
+\paragraph{Field: Moisture Content x}\label{field-moisture-content-x-1}
+
+The moisture content of the x\(^{th}\) point. The units are {[}kg/m3{]}.
+
+\paragraph{Field: Liquid Transport Coefficient x}\label{field-liquid-transport-coefficient-x}
+
+The Liquid Transport Coefficient of the x\(^{th}\) point. The units are {[}m2/s{]}.
+
+Below is an example input for a material liquid transport coefficient under suction.
+
+\begin{lstlisting}
+
+MaterialProperty:HeatAndMoistureTransfer:Suction,
+        Concrete,     !- Name
+        5,     !- Number of Suction points
+        0,     !- Moisture content 1
+        0,     !- Liquid Transport Coefficient 1
+        72,     !- Moisture content 2
+        0.0000000000741,     !- Liquid Transport Coefficient 2
+        85,     !- Moisture content 3
+        0.000000000253,     !- Liquid Transport Coefficient 3
+        100,     !- Moisture content 4
+        0.00000000101,     !- Liquid Transport Coefficient 4
+        118,     !- Moisture content 5
+        0.00000000128;     !- Liquid Transport Coefficient 5
+\end{lstlisting}
+
+\subsection{MaterialProperty:HeatAndMoistureTransfer:Redistribution}\label{materialpropertyheatandmoisturetransferredistribution}
+
+\textbf{Advanced/Research Usage:}This material property is used in conjunction with the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm.
+
+The redistribution data relates the liquid transport coefficient to the water content of a material under normal conditions. A data point at zero water content is required. The liquid transport coefficient at the highest entered water content value is used for all liquid transport coefficient values above this water content. These coefficients are used by the Heat and Moisture Transfer algorithm when the rain flag is NOT set in the weather file.
+
+\subsubsection{Inputs}\label{inputs-10-020}
+
+\paragraph{Field: Material Name}\label{field-material-name-3}
+
+This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
+
+\paragraph{Field: Number of Redistribution points}\label{field-number-of-redistribution-points}
+
+A maximum of 25 points can be specified.
+
+\paragraph{Field Set: Moisture Content-- Liquid Transport Coefficient}\label{field-set-moisture-content-liquid-transport-coefficient-1}
+
+\paragraph{Field: Moisture Content x}\label{field-moisture-content-x-2}
+
+The moisture content of the x\(^{th}\) point. The units are {[}kg/m3{]}.
+
+\paragraph{Field: Liquid Transport Coefficient x}\label{field-liquid-transport-coefficient-x-1}
+
+The Liquid Transport Coefficient of the x\(^{th}\) point. The units are {[}m2/s{]}.
+
+Below is an example input for the object.
+
+\begin{lstlisting}
+
+MaterialProperty:HeatAndMoistureTransfer:Redistribution,
+        Concrete,     !- Name
+        5,     !- Number of Redistribution points
+        0,     !- Moisture content 1
+        0,     !- Liquid Transport Coefficient 1
+        72,     !- Moisture content 2
+        0.00000000000741,     !- Liquid Transport Coefficient 2
+        85,     !- Moisture content 3
+        0.0000000000253,     !- Liquid Transport Coefficient 3
+        100,     !- Moisture content 4
+        0.000000000101,     !- Liquid Transport Coefficient 4
+        118,     !- Moisture content 5
+        0.000000000128;     !- Liquid Transport Coefficient 5
+\end{lstlisting}
+
+\subsection{MaterialProperty:HeatAndMoistureTransfer:Diffusion}\label{materialpropertyheatandmoisturetransferdiffusion}
+
+\textbf{Advanced/Research Usage:}This material property is used in conjunction with the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm.
+
+The MU data relates the vapor diffusion resistance factor (dimensionless) to the relative humidity as fraction(RH). A data point at zero RH is required. The vapor diffusion resistance factor at the highest entered relative humidity (RH) value is used for all vapor diffusion resistance factor values above this RH.~ The relative humidity maximum value in fraction is 1.0.
+
+\subsubsection{Inputs}\label{inputs-11-019}
+
+\paragraph{Field: Material Name}\label{field-material-name-4}
+
+This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
+
+\paragraph{Field: Number of Data Pairs}\label{field-number-of-data-pairs}
+
+A maximum of 25 pairs can be specified.
+
+\paragraph{Field Set: Relative Humidity-Vapor Diffusion Resistance Factor}\label{field-set-relative-humidity-vapor-diffusion-resistance-factor}
+
+\paragraph{Field: Relative Humidity Fraction \#x}\label{field-relative-humidity-fraction-x-1}
+
+The moisture content of the x\(^{th}\) pair. The relative humidity is entered as fraction, not in percent.
+
+\paragraph{Field: Vapor Diffusion Resistance Factor \#x}\label{field-vapor-diffusion-resistance-factor-x}
+
+The Liquid Transport Coefficient of the x\(^{th}\) pair.
+
+Below are some examples of the values for materials.
+
+\begin{lstlisting}
+
+MaterialProperty:HeatAndMoistureTransfer:Diffusion,
+        Plywood,     !- Name
+        3,     !- Number of data Points
+        0,     !- Relative Humidity Fraction 1
+        700,     !- Water Vapor Diffusion Resistance Factor 1
+        0.5,     !- Relative Humidity Fraction 2
+        200,     !- Water Vapor Diffusion Resistance Factor 2
+        1,     !- Relative Humidity Fraction 3
+        20;     !- Water Vapor Diffusion Resistance Factor 3
+
+  MaterialProperty:HeatAndMoistureTransfer:Diffusion,
+        Concrete,     !- Name
+        1,     !- Number of Mu Points
+        0,     !- Relative Humidity Fraction 1
+        180;     !- Water Vapor Diffusion Resistance Factor 1
+\end{lstlisting}
+
+\subsection{MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity}\label{materialpropertyheatandmoisturetransferthermalconductivity}
+
+\textbf{Advanced/Research Usage:}This material property is used in conjunction with the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm.
+
+The thermal data relates the thermal conductivity {[}W/m-K{]} of a material to the moisture or water content {[}kg/m3{]}. A data point at zero water content is required. The thermal conductivity at the highest entered water content value is used for all thermal conductivity values above this water content. If this object is not defined for a material then the algorithm will use a constant value entered in the Material object for all water contents.
+
+\subsubsection{Inputs}\label{inputs-12-018}
+
+\paragraph{Field: Material Name}\label{field-material-name-5}
+
+This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
+
+\paragraph{Field: Number of Thermal Coordinates}\label{field-number-of-thermal-coordinates}
+
+A maximum of 25 coordinates can be specified.
+
+\paragraph{Field Set: Moisture Content- Thermal Conductivity}\label{field-set-moisture-content--thermal-conductivity}
+
+\paragraph{Field: Moisture Content x}\label{field-moisture-content-x-3}
+
+The moisture content of the x\(^{th}\) coordinate. The units are {[}kg/m3{]}
+
+\paragraph{Field: Thermal Conductivity x}\label{field-thermal-conductivity-x-1}
+
+The Thermal Conductivity of the x\(^{th}\) coordinate. The units are {[}W/m-K{]}
+
+Below is an example of values for a material.
+
+\begin{lstlisting}
+
+MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity
+        Concrete,     !- Name
+        2,     !- Number of Thermal Coordinates
+        0,     !- Moisture content \#1
+        1.6,     !- Thermal Conductivity \#1
+        180,     !- Moisture content \#2
+        2.602;     !- Thermal Conductivity \#2
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-021}
+
+\begin{itemize}
+\item
+  Zone,Average,HAMT Surface Average Water Content Ratio {[}kg/kg{]}
+\item
+  Zone,Average,HAMT Surface Inside Face Temperature {[}C{]}
+\item
+  Zone,Average,HAMT Surface Inside Face Relative Humidity {[}\%{]}
+\item
+  Zone,Average,HAMT Surface Inside Face Vapor Pressure {[}Pa{]}
+\item
+  Zone,Average,HAMT Surface Outside Face Temperature {[}C{]}
+\item
+  Zone,Average,HAMT Surface Outside Face Relative Humidity {[}\%{]}
+\item
+  Zone,Average,HAMT Surface Inside Face Relative Humidity {[}\%{]}
+\end{itemize}
+
+\paragraph{HAMT Surface Average Water Content Ratio {[}kg/kg{]}}\label{hamt-surface-average-water-content-ratio-kgkg}
+
+This output is the summed water content {[}kg/kg{]} of all cells in a surface expressed as a fraction of the mass of the water to the material mass.
+
+\paragraph{HAMT Surface Inside Face Temperature {[}C{]}}\label{hamt-surface-inside-face-temperature-c}
+
+This output is the temperature {[}C{]} on the internal ``surface'' of the surface.
+
+\paragraph{HAMT Surface Inside Face Relative Humidity {[}\%{]}}\label{hamt-surface-inside-face-relative-humidity}
+
+\paragraph{HAMT Surface Inside Face Relative Humidity {[}\%{]}}\label{hamt-surface-inside-face-relative-humidity-1}
+
+This output is the relative humidity on the internal ``surface'' of the surface expressed as a percentage.
+
+\paragraph{HAMT Surface Inside Face Vapor Pressure {[}Pa{]}}\label{hamt-surface-inside-face-vapor-pressure-pa}
+
+This output is the vapor pressure {[}Pa{]} on the internal ``surface'' of the surface.
+
+\paragraph{HAMT Surface Outside Face Temperature {[}C{]}}\label{hamt-surface-outside-face-temperature-c}
+
+This output is the temperature on the external ``surface'' of the surface.
+
+\paragraph{HAMT Surface Outside Face Relative Humidity {[}\%{]}}\label{hamt-surface-outside-face-relative-humidity}
+
+This output is the relative humidity on the external ``surface'' of the surface.
+
+Zone,Average,HAMT Surface Temperature Cell N {[}C{]}
+
+Zone,Average,HAMT Surface Water Content Cell N {[}kg/kg{]}
+
+Zone,Average,HAMT Surface Relative Humidity Cell N {[}\%{]}
+
+Detailed profile data for the variables Temperature {[}C{]}, Relative Humidity {[}\%{]} and Water Content {[}kg/kg{]} within each surface can also be reported. To calculate the heat and moisture transfer through surfaces HAMT splits up surfaces into discrete cells. Each cell is composed of a single material and has a position within the surface. HAMT automatically assigns cells to construction objects so that there are more cells closer to boundaries between materials and also at the ``surfaces'' of the surface. It is not possible for users to define their own cells.
+
+\paragraph{HAMT Surface Relative Humidity Cell \textless{}N\textgreater{} {[}\%{]}}\label{hamt-surface-relative-humidity-cell-n}
+
+This is the relative humidity of the cell in the surface.
+
+\paragraph{HAMT Surface Temperature Cell \textless{}N\textgreater{} {[}C{]}}\label{hamt-surface-temperature-cell-n-c}
+
+This is the temperature of the cell in the surface.
+
+\paragraph{HAMT Surface Water Content Cell \textless{}N\textgreater{} {[}kg/kg{]}}\label{hamt-surface-water-content-cell-n-kgkg}
+
+This is the relative water content of the cell in the surface.
+
+Each surface is made from a particular construction. The construction-surface relationship is output by HAMT to the eplusout.eio file with the following format.
+
+\begin{lstlisting}
+! <HAMT cells>, Surface Name, Construction Name, Cell Numbers
+! <HAMT origins>, Surface Name, Construction Name, Cell origins (m)
+\end{lstlisting}
+
+The output also contains the HAMT cell origins and cell number for each construction -- surface combination. The coordinate system origin is defined as the exterior surface of the construction. Users can select any one of the Temperature, Relative Humidity or Water Content variables for any cell to be reported, using the following naming scheme for the output variable.
+
+HAMT Profile Construction \textless{}Variable\textgreater{} Cell \textless{}Cell\#\textgreater{}
+
+It is better to specify the ``key'' or Surface Name in this output.
+
+So for example to output the temperature of the 10\(^{th}\) cell in a surface, eg ``East Wall'' would require the following output variable.
+
+\begin{lstlisting}
+
+Output:Variable,
+      East Wall,               !- Key Value
+      HAMT Profile Construction Temperature Cell 10,  !- Variable Name
+      Hourly;                  !- Reporting Frequency
+\end{lstlisting}
+
+By selecting a whole range of these reports and using the information in the eplusout.eio file it is possible to build up a temperature profile of the surface.
+
+\subsection{Materials for Glass Windows and Doors}\label{materials-for-glass-windows-and-doors}
+
+All the materials for glass windows and doors have the prefix ``WindowMaterial''. The following~ WindowMaterial descriptions (Glazing, Glazing:RefractionExtinctionMethod, Gas, GasMixture, Shade, Screen and Blind) apply to glass windows and doors. The property definitions described herein for Glazing, Gas and GasMixture are supported by the National Fenestration Rating Council as standard.
+
+``Front side'' is the side of the layer opposite the zone in which the window is defined. ``Back side'' is the side closest to the zone in which the window is defined. Therefore, for exterior windows, ``front side'' is the side closest to the outdoors. For interior windows, ``front side'' is the side closest to the zone adjacent to the zone in which the window is defined.
+
+The solar radiation transmitted by the window layers enters the zone and is a component of the zone load. The solar radiation absorbed in each solid layer (glass, shade, screen or blind) participates in the window layer heat balance calculation. The visible transmittance and reflectance properties of the window are used in the daylighting calculation.
+
+\subsection{WindowMaterial:Glazing}\label{windowmaterialglazing}
+
+In the following, for exterior windows, ``front side'' is the side of the glass closest to the outside air and ``back side'' is the side closest to the zone the window is defined in. For interzone windows, ``front side'' is the side closest to the zone adjacent to the zone the window is defined in and ``back side'' is the side closest to the zone the window is defined in.
+
+\subsubsection{Inputs}\label{inputs-13-015}
+
+\paragraph{Field: Name}\label{field-name-7-020}
+
+The name of the glass layer. It corresponds to a layer in a window construction.
+
+\paragraph{Field: Optical Data Type}\label{field-optical-data-type}
+
+Valid values for this field are SpectralAverage, Spectral, BSDF.
+
+If Optical Data Type = SpectralAverage, the values you enter for solar transmittance and reflectance are assumed to be averaged over the solar spectrum, and the values you enter for visible transmittance and reflectance are assumed to be averaged over the solar spectrum and weighted by the response of~ the human eye. There is an EnergyPlus Reference Data Set for WindowMaterial:Glazing that contains spectral average properties for many different types of glass.
+
+If Optical Data Type = Spectral, then, in the following field, you must enter the name of a spectral data set defined with the WindowGlassSpectralData object. In this case, the values of~ solar and visible transmittance and reflectance in the fields below should be blank.
+
+If Optical Data Type = BSDF, the Construction:ComplexFenestrationState object must be used to define the window construction layers. The Construction:ComplexFenestrationState object contains references to the BSDF files which contain the optical properties of the Complex Fenestration layers. In this case,
+
+\paragraph{Field: Window Glass Spectral Data Set Name}\label{field-window-glass-spectral-data-set-name}
+
+If Optical Data Type = Spectral, this is the name of a spectral data set defined with a WindowGlassSpectralData object.
+
+\paragraph{Field: Thickness}\label{field-thickness-1}
+
+The surface-to-surface thickness of the glass (m).
+
+\paragraph{Field: Solar Transmittance at Normal Incidence}\label{field-solar-transmittance-at-normal-incidence}
+
+Transmittance at normal incidence averaged over the solar spectrum. Used only when Optical Data Type = SpectralAverage.
+
+For uncoated glass, when alternative optical properties are available---such as thickness, solar index of refraction, and solar extinction coefficient---they can be converted to equivalent solar transmittance and reflectance values using the equations given in ``Conversion from Alternative Specification of Glass Optical Properties.'')
+
+\paragraph{Field: Front Side Solar Reflectance at Normal Incidence}\label{field-front-side-solar-reflectance-at-normal-incidence}
+
+Front-side reflectance at normal incidence averaged over the solar spectrum. Used only when Optical Data Type = SpectralAverage.
+
+\paragraph{Field: Back Side Solar Reflectance at Normal Incidence}\label{field-back-side-solar-reflectance-at-normal-incidence}
+
+Back-side reflectance at normal incidence averaged over the solar spectrum. Used only when Optical Data Type = SpectralAverage.
+
+\paragraph{Field: Visible Transmittance at Normal Incidence}\label{field-visible-transmittance-at-normal-incidence}
+
+Transmittance at normal incidence averaged over the solar spectrum and weighted by the response of the human eye. Used only when Optical Data Type = SpectralAverage.
+
+For uncoated glass, when alternative optical properties are available---such as thickness, visible index of refraction, and visible extinction coefficient---they can be converted to equivalent visible transmittance and reflectance values using the equations given in ``Conversion from Alternative Specification of Glass Optical Properties.'')
+
+\paragraph{Field: Front Side Visible Reflectance at Normal Incidence}\label{field-front-side-visible-reflectance-at-normal-incidence}
+
+Front-side reflectance at normal incidence averaged over the solar spectrum and weighted by the response of the human eye. Used only when Optical Data Type = SpectralAverage.
+
+\paragraph{Field: Back Side Visible Reflectance at Normal Incidence}\label{field-back-side-visible-reflectance-at-normal-incidence}
+
+Back-side reflectance at normal incidence averaged over the solar spectrum and weighted by the response of the human eye. Used only when Optical Data Type = SpectralAverage.
+
+\paragraph{Field: Infrared Transmittance at Normal Incidence}\label{field-infrared-transmittance-at-normal-incidence}
+
+Long-wave transmittance at normal incidence.
+
+\paragraph{Field: Front Side Infrared Hemispherical Emissivity}\label{field-front-side-infrared-hemispherical-emissivity}
+
+Front-side long-wave emissivity.
+
+\paragraph{Field: Back Side Infrared Hemispherical Emissivity}\label{field-back-side-infrared-hemispherical-emissivity}
+
+Back-side long-wave emissivity.
+
+\paragraph{Field: Conductivity}\label{field-conductivity-1}
+
+Thermal conductivity (W/m-K).
+
+\paragraph{Field: Dirt Correction Factor for Solar and Visible Transmittance}\label{field-dirt-correction-factor-for-solar-and-visible-transmittance}
+
+This is a factor that corrects for the presence of dirt on the glass. The program multiplies the fields ``Solar Transmittance at Normal Incidence'' and ``Visible Transmittance at Normal Incidence'' by this factor if the material is used as the \underline{outer} glass layer of an \underline{exterior} window or glass door.\footnote{If Optical Data Type = Spectral, the program multiplies the solar and visible transmittance at each wavelength by the dirt correction factor.} If the material is used as an inner glass layer (in double glazing, for example), the dirt correction factor is not applied because inner glass layers are assumed to be clean. Using a material with dirt correction factor \textless{} 1.0 in the construction for an interior window will result in an error message.
+
+Representative values of the dirt correction factor are shown in Table~\ref{table:dirt-correction-factors}.
+
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Dirt Correction Factors \protect \label{table:dirt-correction-factors}} \\
+\toprule 
+Type of Location & \multicolumn{3}{c}{Angle of Glazing} \\ \cmidrule(r){2-4}
+                 & Vertical & 45$^{o}$ & Horizontal \\ \midrule
+\endhead
+Non-industrial & 0.9 & 0.8 & 0.7 \\
+Industrial & 0.7 & 0.6 & 0.5 \\
+Very Dirty & 0.6 & 0.5 & 0.4 \\
+\bottomrule
+{\tiny From Appendix A, ``Daylighting in Sports Halls, Report 2,'' SportScotland, Nov. 2002 (www.sportscotland.org.uk)}
+\end{longtable}
+
+The default value of the dirt correction factor is 1.0, which means the glass is clean.
+
+It is assumed that dirt, if present, has no effect on the IR properties of the glass.
+
+\paragraph{Field: Solar Diffusing}\label{field-solar-diffusing}
+
+Takes values No (the default) and Yes. If No, the glass is \underline{transparent} and beam solar radiation incident on the glass is transmitted as beam radiation with no diffuse component. If Yes, the glass is \underline{translucent} and beam solar radiation incident on the glass is transmitted as hemispherically diffuse radiation with no beam component.\footnote{EnergyPlus does not model the ``partially translucent'' case in which beam solar radiation incident on the glass is transmitted as a combination of beam and diffuse.} See Figure~\ref{fig:comparison-between-transmittance-properties}. Solar Diffusing = Yes should only be used on the \emph{innermost} pane of glass in an exterior window; it does not apply to interior windows.
+
+For both Solar Diffusing = No and Yes, beam is reflected as beam with no diffuse component (see Figure~\ref{fig:comparison-between-transmittance-properties}). Solar Diffusing cannot be used with Window Shading Control devices (except Switchable Glazing). When attempted, the window property will be set to No for Solar Diffusing. The Surface Details report will reflect the override.
+
+If, in the Building object, Solar Distribution = FullInteriorAndExterior, use of Solar Diffusing = Yes for glass in an exterior window will change the distribution of interior solar radiation from the window. The result is that beam solar radiation that would be transmitted by a transparent window and get absorbed by particular interior surfaces will be diffused by a translucent window and be spread over more interior surfaces. This can change the time dependence of heating and cooling loads in the zone.
+
+In a zone with Daylighting:Detailed, translucent glazing---which is often used in skylights---will provide a more uniform daylight illuminance over the zone and will avoid patches of sunlight on the floor.
+
+\begin{figure}[hbtp] % fig 10
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image025.png}
+\caption{Comparison between transmittance properties of transparent glass (Solar Diffusing = No) and translucent glass (Solar Diffusing = Yes). \protect \label{fig:comparison-between-transmittance-properties}}
+\end{figure}
+
+\paragraph{Field: Young's modulus}\label{field-youngs-modulus}
+
+A measure of the stiffness of an elastic material.~ It is defined as the ratio of the unaxial stress over the uniaxial strain in the range of stress in which Hooke's Law holds. It is used only with complex fenestration systems defined through the Construction:ComplexFenestrationState object. The default value for glass is 7.2e10 Pa.
+
+\paragraph{Field: Poisson's ratio}\label{field-poissons-ratio}
+
+The ratio, when a sample object is stretched, of the contraction or transverse strain (perpendicular to the applied load), to the extension or axial strain (in the direction of the applied load). This value is used only with complex fenestration systems defined through the Construction:ComplexFenestrationState object. The default value for glass is 0.22.
+
+IDF examples of Spectral average and using a Spectral data set:
+
+\begin{lstlisting}
+
+MATERIAL:WINDOWGLASS, GLASS - CLEAR SHEET 1 / 8 IN,
+    SpectralAverage, ! Optical data type
+    0.003, ! Thickness {m} 1/8"
+    0.850, ! Solar transmittance at normal incidence
+    0.075, ! Solar reflectance at normal incidence: front side
+    0.075, ! Solar reflectance at normal incidence: back side
+    0.901, ! Visible transmittance at normal incidence
+    0.081, ! Visible reflectance at normal incidence: front side
+    0.081, ! Visible reflectance at normal incidence: back side
+    0.0,   ! IR transmittance at normal incidence
+    0.84,  ! IR hemispherical emissivity: front side
+    0.84,  ! IR hemispherical emissivity: back side
+    0.9;   ! Conductivity {W/m-K}
+
+
+  WindowMaterial:Glazing ,SPECTRAL GLASS INNER PANE, ! Material name
+      Spectral, ! Optical data type {SpectralAverage or Spectral}
+      TestSpectralDataSet, ! Name of spectral data set
+      0.0099, ! Thickness {m}
+      ,  ! Solar transmittance at normal incidence
+      ,  ! Solar reflectance at normal incidence: front side
+      ,  ! Solar reflectance at normal incidence: back side
+      ,  ! Visible transmittance at normal incidence
+      ,  ! Visible reflectance at normal incidence: front side
+      ,  ! Visible reflectance at normal incidence: back side
+      0.0,   ! IR transmittance at normal incidence
+      0.84,  ! IR emissivity: front side
+      0.84,  ! IR emissivity: back side
+      0.798; ! Conductivity {W/m-K}
+\end{lstlisting}
+
+IDF example of Spectral Data Type = BSDF
+
+\begin{lstlisting}
+
+WindowMaterial:Glazing,
+    Glass_5012_Layer,        !- Layer name : CLEAR_6.PPG
+    BSDF,                    !- Optical Data Type
+    ,                        !- Spectral Data name
+    0.005664,                !- Thickness
+    ,                        !- Solar Transmittance
+    ,                        !- Solar Front Reflectance
+    ,                        !- Solar Back Reflectance
+    ,                        !- Visible Transmittance
+    ,                        !- Visible Front Reflectance
+    ,                        !- Visible Back reflectance
+    0.000000,                !- IR Transmittance
+    0.840000,                !-Front Emissivity
+    0.840000,                !-Back Emissivity
+    1.000000,                !-Conductivity
+    ,                        !-Dirt Correction Factor for Sol/Vis Transmittance
+    ,                        !-Solar Diffusing
+    7.2e10,                  !-Young’s modulus
+    0.22;                    !-Poisson’s ratio
+\end{lstlisting}
+
+\subsection{WindowMaterial:Glazing:RefractionExtinctionMethod}\label{windowmaterialglazingrefractionextinctionmethod}
+
+This is an alternative way of specifying glass properties. Index of refraction and extinction coefficient are given instead of the transmittance and reflectance values used in WindowMaterial:Glazing. However, unlike WindowMaterial:Glazing, WindowMaterial:Glazing:RefractionExtinctionMethod is restricted to cases where the front and back optical properties of the glass are the same. This means it cannot be used for glass with a coating on one side. In that case WindowMaterial:Glazing should be used. Also, unlike WindowMaterial:Glazing, WindowMaterial:Glazing:RefractionExtinctionMethod does not allow input of glass wavelength-by-wavelength (spectral) properties.
+
+\subsubsection{Inputs}\label{inputs-14-015}
+
+\paragraph{Field: Name}\label{field-name-8-020}
+
+The name of the glass layer. It corresponds to a layer in a window construction.
+
+\paragraph{Field: Thickness}\label{field-thickness-2}
+
+The surface-to-surface thickness of the glass (m).
+
+\paragraph{Field: Solar Index of Refraction}\label{field-solar-index-of-refraction}
+
+Index of refraction averaged over the solar spectrum.
+
+\paragraph{Field: Solar Extinction Coefficient}\label{field-solar-extinction-coefficient}
+
+Extinction coefficient averaged over the solar spectrum (m\(^{-1}\)).
+
+\paragraph{Field: Visible Index of Refraction}\label{field-visible-index-of-refraction}
+
+Index of refraction averaged over the solar spectrum and weighted by the response of the human eye.
+
+\paragraph{Field: Visible Extinction Coefficient}\label{field-visible-extinction-coefficient}
+
+Extinction coefficient averaged over the solar spectrum and weighted by the response of the human eye (m\(^{-1}\)).
+
+\paragraph{Field: Infrared Transmittance at Normal Incidence}\label{field-infrared-transmittance-at-normal-incidence-1}
+
+Long-wave transmittance at normal incidence.
+
+\paragraph{Field: Infrared Hemispherical Emissivity}\label{field-infrared-hemispherical-emissivity}
+
+Long-wave hemispherical emissivity, assumed the same on both sides of the glass.
+
+\paragraph{Field: Conductivity}\label{field-conductivity-2}
+
+Thermal conductivity (W/m-K).
+
+\paragraph{Field: Dirt Correction Factor for Solar and Visible Transmittance}\label{field-dirt-correction-factor-for-solar-and-visible-transmittance-1}
+
+This is a factor that corrects for the presence of dirt on the glass. It multiplies the solar and visible transmittance at normal Incidence (which the program calculates from the input values of thickness, solar index of refraction, solar extinction coefficient, etc.) if the material is used as the \underline{outer} glass layer of an \underline{exterior} window or glass door. If the material is used as an inner glass layer (in double glazing, for example), the dirt correction factor is not applied because inner glass layers are assumed to be clean. Using a material with dirt correction factor \textless{} 1.0 in the construction for an interior window will result in an error message.
+
+Representative values of the direct correction factor are shown in Table~\ref{table:dirt-correction-factors}.
+
+The default value of the dirt correction factor is 1.0, which means the glass is clean. It is assumed that dirt, if present, has no effect on the IR properties of the glass.
+
+\paragraph{Field: Solar Diffusing}\label{field-solar-diffusing-1}
+
+Takes values No (the default) and Yes. If No, the glass is transparent. If Yes, the glass is translucent and beam solar radiation incident on the glass is transmitted as hemispherically diffuse radiation with no beam component. (EnergyPlus does not model the ``partially translucent'' case in which beam solar radiation incident on the glass is transmitted as a combination of beam and diffuse.) Solar Diffusing = Yes should only be used on the innermost pane of glass in an exterior window; it does not apply to interior windows.
+
+If, in the Building object, Solar Distribution = FullInteriorAndExterior, use of Solar Diffusing = Yes for glass in an exterior window will change the distribution of interior solar radiation from the window. The result is that beam solar radiation that would be transmitted by a transparent window and get absorbed by particular interior surfaces will be diffused by a translucent window and be spread over more interior surfaces. This can change the time dependence of heating and cooling loads in the zone.
+
+In a zone with Daylighting:Detailed, translucent glazing, which is often used in skylights, will provide a more uniform daylight illuminance over the zone and will avoid patches of sunlight on the floor.
+
+An IDF example:
+
+\begin{lstlisting}
+WindowMaterial:Glazing:RefractionExtinctionMethod,
+  4MM CLEAR GLASS,  !- Material name
+  0.004,            !- Thickness {m}
+  1.526,            !- Solar index of refraction
+  30.0 ,            !- Solar extinction coefficient (1/m)
+  1.526,            !- Visible index of refraction
+  30.0 ,            !- Visible extinction coefficient (1/m)
+  0.0,              !- IR transmittance at normal incidence
+  0.84,             !- IR emissivity
+  0.9;              !- Conductivity {W/m-K}
+\end{lstlisting}
+
+\subsection{Glass Optical Properties Conversion}\label{glass-optical-properties-conversion}
+
+\subsubsection{Conversion from Glass Optical Properties Specified as Index of Refraction and Transmittance at Normal Incidence}\label{conversion-from-glass-optical-properties-specified-as-index-of-refraction-and-transmittance-at-normal-incidence}
+
+The optical properties of uncoated glass are sometimes specified by index of refraction, n, and transmittance at normal incidence, T.
+
+The following equations show how to convert from this set of values to the transmittance and reflectance values required by WindowMaterial:Glazing. These equations apply only to \underline{uncoated} glass, and can be used to convert either spectral-average solar properties or spectral-average visible properties (in general, \(n\) and \(T\) are different for the solar and visible). Note that since the glass is uncoated, the front and back reflectances are the same and equal to the \(R\) that is solved for in the following equations.
+
+Given \(n\) and \(T\), find \(R\):
+
+\begin{equation*}
+r = \left( \frac{n - 1}{n + 1} \right)^2
+\end{equation*}
+
+\begin{equation*}
+\tau = \frac{ \left[ (1 - r)^4 + 4 r^2 T^2 \right]^{1/2} - (1 - r)^2}{2 r^2 T}
+\end{equation*}
+
+\begin{equation*}
+R = r + \frac{(1 - r)^2 r \tau ^2}{1 - r^2 \tau ^2}
+\end{equation*}
+
+\textbf{Example:}
+
+\begin{equation*}
+T = 0.86156
+\end{equation*}
+
+\begin{equation*}
+n = 1.526
+\end{equation*}
+
+\begin{equation*}
+r = \left( \frac{1.526 - 1}{1.526 + 1} \right)^2
+\end{equation*}
+
+\begin{equation*}
+\tau = 0.93974
+\end{equation*}
+
+\begin{equation*}
+R = 0.07846
+\end{equation*}
+
+\subsection{WindowMaterial:GlazingGroup:Thermochromic}\label{windowmaterialglazinggroupthermochromic}
+
+Thermochromic (TC) materials have active, reversible optical properties that vary with temperature. Thermochromic windows are adaptive window systems for incorporation into building envelopes. Thermochromic windows respond by absorbing sunlight and turning the sunlight energy into heat. As the thermochromic film warms it changes its light transmission level from less absorbing to more absorbing. The more sunlight it absorbs the lower the light level going through it. By using the suns own energy the window adapts based solely on the directness and amount of sunlight. Thermochromic materials will normally reduce optical transparency by absorption and/or reflection, and are specular (maintaining vision).
+
+A thermochromic window is defined with a Construction object which references a special layer defined with a WindowMaterial:GlazingGroup:Thermochromic object. The WindowMaterial:GlazingGroup:Thermochromic object further references a series of WindowMaterial:Glazing objects corresponding to each specification temperature of the TC layer.
+
+This object specifies a layer of thermochromic glass, part of a thermochromic window. An example file ThermochromicWindow.idf is included in the EnergyPlus installation.
+
+\subsubsection{Inputs}\label{inputs-15-015}
+
+\paragraph{Field: Name}\label{field-name-9-017}
+
+A unique user assigned name for a particular thermochromic glass material.
+
+\paragraph{Field Set (Optical Data Temperature, Window Material Glazing Name) is extensible.}\label{field-set-optical-data-temperature-window-material-glazing-name-is-extensible.}
+
+\paragraph{Field:Optical Data Temperature \textless{}N\textgreater{}}\label{fieldoptical-data-temperature-n}
+
+The temperature of the TC glass layer corresponding to the optical data of the TC layer. Unit is °C.
+
+\paragraph{Field: Window Material Glazing Name \textless{}N\textgreater{}}\label{field-window-material-glazing-name-n}
+
+The window glazing (defined with WindowMaterial:Glazing) name that provides the TC glass layer performance at the above specified temperature.
+
+IDF Examples
+
+\begin{lstlisting}
+Construction,
+  window_const,     !- Name
+  Usual Glass,      !- Layer 1
+  AIR 6MM,          !- Layer 2
+  TCGlazings,       !- Layer 3
+  AIR 6MM,          !- Layer 4
+  Usual Glass;      !- Layer 5
+
+WindowMaterial:Gas,
+  AIR 6MM,          !- Name
+  Air,              !- Gas Type
+  0.0063;           !- Thickness {m}
+
+! Added for thermochromic glazings
+WindowMaterial:GlazingGroup:Thermochromic,
+  TCGlazings,
+  0 ,  TCGlazing0,
+  20,  TCGlazing20,
+  25,  TCGlazing25,
+  30,  TCGlazing30,
+  35,  TCGlazing35,
+  40,  TCGlazing40,
+  45,  TCGlazing45,
+  50,  TCGlazing50,
+  55,  TCGlazing55,
+  60,  TCGlazing60,
+  65,  TCGlazing65,
+  75,  TCGlazing75,
+  85,  TCGlazing85;
+
+WindowMaterial:Glazing,
+  TCGlazing0,       !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing20,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing25,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing30,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing35,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing40,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing45,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing50,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing55,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing60,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing65,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing75,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+
+WindowMaterial:Glazing,
+  TCGlazing85,      !- Name
+  SpectralAverage,  !- Optical Data Type
+  ,                 !- Window Glass Spectral Data Set Name
+  0.0030,           !- Thickness
+  0.2442,           !- Solar Transmittance at Normal Incidence
+  0.7058,           !- Front Side Solar Reflectance at Normal Incidence
+  0.7058,           !- Back Side Solar Reflectance at Normal Incidence
+  0.3192,           !- Visible Transmittance at Normal Incidence
+  0.6308,           !- Front Side Visible Reflectance at Normal Incidence
+  0.6308,           !- Back Side Visible Reflectance at Normal Incidence
+  0.0000,           !- Infrared Transmittance at Normal Incidence
+  0.9000,           !- Front Side Infrared Hemispherical Emissivity
+  0.9000,           !- Back Side Infrared Hemispherical Emissivity
+  0.0199,           !- Conductivity
+  1.0000,           !- Dirt Correction Factor for Solar and Visible Transmittance
+  No;               !- Solar Diffusing
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-019}
+
+\paragraph{Surface Window Thermochromic Layer Temperature {[}C{]}}\label{surface-window-thermochromic-layer-temperature-c}
+
+The temperature of the TC glass layer of a TC window at each time step.
+
+\paragraph{Surface Window Thermochromic Layer Property Specification Temperature {[}C{]}}\label{surface-window-thermochromic-layer-property-specification-temperature-c}
+
+The temperature under which the optical data of the TC glass layer are specified.
+
+The overall properties (U-factor/SHGC/VT) of the thermochromic windows at different specification temperatures are reported in the EIO file. These window constructions are created by EnergyPlus during run time. They have similar names with suffix ``\_TC\_XX'' where XX represents a specification temperature.
+
+\subsection{WindowMaterial:Gas}\label{windowmaterialgas}
+
+This object specifies the properties of the gas between the panes of a multi-pane window. Gas Type = Custom allows you to specify the properties of gases other than air, Argon, Krypton or Xenon. There is an EnergyPlus Reference Data Set for Material:WindowGas that contains several types of gas of different thicknesses. See Material:WindowGasMixture for the case that the gas fill is a mixture of different gases.
+
+\subsubsection{Inputs}\label{inputs-16-011}
+
+\paragraph{Field: Name}\label{field-name-10-016}
+
+The name of the gas fill. It refers to a layer in a window construction.
+
+\paragraph{Field: Gas Type}\label{field-gas-type}
+
+The type of gas. The choices are Air, Argon, Krypton, or Xenon. If Gas Type = Custom you can use Conductivity Coefficient A, etc. to specify the properties of a different type of gas.
+
+\paragraph{Field: Thickness}\label{field-thickness-3}
+
+The thickness (m) of the gas layer.
+
+\paragraph{Properties for Custom Gas Types}\label{properties-for-custom-gas-types}
+
+The following entries are used only if Gas Type = Custom. The A and B coefficients are those in the following expression that gives a property value as a function of temperature in degrees K:
+
+\begin{equation}
+Property = Coefficien{t_A} + Coefficien{t_B}*Temperatur{e_K}
+\end{equation}
+
+\paragraph{Field: Conductivity Coefficient A}\label{field-conductivity-coefficient-a}
+
+The A coefficient for gas conductivity (W/m-K). Used only if Gas Type = Custom.
+
+\paragraph{Field: Conductivity Coefficient B}\label{field-conductivity-coefficient-b}
+
+The B coefficient for gas conductivity (W/m-K\(^{2}\)). Used only if Gas Type = Custom.
+
+\paragraph{Field: Conductivity Coefficient C}\label{field-conductivity-coefficient-c}
+
+The C coefficient for gas conductivity (W/m-K\(^{3}\)).~ Used only if Gas Type = Custom.
+
+\paragraph{Field: Viscosity Coefficient A}\label{field-viscosity-coefficient-a}
+
+The A coefficient for gas viscosity (kg/m-s). Used only if Gas Type = Custom.
+
+\paragraph{Field: Viscosity Coefficient B}\label{field-viscosity-coefficient-b}
+
+The B coefficient for gas viscosity (kg/m-s-K). Used only if Gas Type = Custom.
+
+\paragraph{Field: Viscosity Coefficient C}\label{field-viscosity-coefficient-c}
+
+The C coefficient for gas viscosity (kg/m-s-K\(^{2}\)).~ Used only if Gas Type = Custom.
+
+\paragraph{Field: Specific Heat Coefficient A}\label{field-specific-heat-coefficient-a}
+
+The A coefficient for gas specific heat (J/kg-K). Used only if Gas Type = Custom.
+
+\paragraph{Field: Specific Heat Coefficient B}\label{field-specific-heat-coefficient-b}
+
+The B coefficient for gas specific heat (J/kg-K\(^{2}\)). Used only if Gas Type = Custom.
+
+\paragraph{Field: Specific Heat Coefficient C}\label{field-specific-heat-coefficient-c}
+
+The C coefficient for gas specific heat (J/kg-K\(^{3}\)).~ Used only if Gas Type = Custom.
+
+\paragraph{Field: Specific Heat Ratio}\label{field-specific-heat-ratio}
+
+The specific heat ratio for gas.~ Used only if Gas Type = Custom.
+
+\paragraph{Field: Molecular Weight}\label{field-molecular-weight}
+
+The molecular weight for gas.~ The molecular weight is the mass of 1 mol of the substance.~ This has a numerical value which is the average molecular mass of the molecules in the substance multiplied by Avogadro's constant. (kg/kmol) (Shown in the IDD as g/mol for consistency)
+
+\paragraph{Field: Specific Heat Ratio}\label{field-specific-heat-ratio-1}
+
+The specific heat ratio for gas.~ The specific heat ratio of a gas is the ratio of the specific heat at contant pressure, to the specific heat at constant volume.~ Used only if Gas Type = Custom.
+
+An IDF example:
+
+\begin{lstlisting}
+
+WindowMaterial:Gas,AIRGAP,
+    AIR,      ! Gas type (Air - Argon - Krypton - Xenon - Custom)]
+    0.0125;   ! Thickness {m} 1/2 inch
+\end{lstlisting}
+
+An IDF example to be used with a WindowMaterial:Gap definition (see below)
+
+\begin{lstlisting}
+
+WindowMaterial:Gas,
+  Gas_1_W_0_0100,                                     !- gap name - Air
+  Air,                                                !- type
+  0.0100;                                             !- thickness
+\end{lstlisting}
+
+An IDF example for a Custom Gas
+
+\begin{lstlisting}
+
+WindowMaterial:Gas,
+  Gas_16_W_0_0003,                   !- gap name
+  Custom,                            !- type
+  0.0003,                            !- thickness
+  2.873000e-003,                     !- Conductivity Coefficient A
+  7.760000e-005,                     !- Conductivity Coefficient B
+  0.000000e+000,                     !- Conductivity Coefficient C
+  3.723000e-006,                     !- Conductivity Viscosity A
+  4.940000e-008,                     !- Conductivity Viscosity B
+  0.000000e+000,                     !- Conductivity Viscosity C
+  1002.737000,                       !- Specific Heat Coefficient A
+  0.012324,                          !- Specific Heat Coefficient B
+  0.000000,                          !- Specific Heat Coefficient C
+  28.969999,                         !- Molecular Weight
+  1.400000;                          !- Specific Heat Ratio
+\end{lstlisting}
+
+\subsection{WindowMaterial:GasMixture}\label{windowmaterialgasmixture}
+
+This object allows you to specify the fill between the panes of a multi-pane window to be a mixture of two, three or four different gases chosen from air, argon, krypton and xenon. It can also be used if only one type of gas in the fill. In this case you can also use WindowMaterial:Gas. Note that the fractions of gas types in the mixture should add up to 1.0.
+
+\subsubsection{Inputs}\label{inputs-17-009}
+
+\paragraph{Field: Name}\label{field-name-11-014}
+
+The name of the gas mixture. It refers to a layer in a window construction.
+
+\paragraph{Field: Thickness}\label{field-thickness-4}
+
+The thickness (m) of the gas mixture layer.
+
+\paragraph{Field: Number of Gases in Mixture}\label{field-number-of-gases-in-mixture}
+
+The number of different types of gas in the mixture ( a value from 1 to 4)
+
+\paragraph{Set: Gas Type-Fraction (up to 4)}\label{set-gas-type-fraction-up-to-4}
+
+\paragraph{Field: Gas 1 Type}\label{field-gas-1-type}
+
+The type of~ the first gas in the mixture. Choices are Air, Argon, Krypton and Xenon.
+
+\paragraph{Field: Gas 1 Fraction}\label{field-gas-1-fraction}
+
+The fraction of the first gas in the mixture.
+
+An IDF example:
+
+\begin{lstlisting}
+
+WindowMaterial:GasMixture,ArgonKryptonMix,
+  0.0125,   ! Thickness {m} 1/2 inch
+  2,        ! Number of Gases in Mixture
+  Argon,    ! Gas 1 Type
+  0.6,      ! Gas 1 Fraction
+  Krypton,  ! Gas 2 Type
+  0.4;      ! Gas 2 Fraction
+\end{lstlisting}
+
+\subsection{WindowMaterial:Gap}\label{windowmaterialgap}
+
+This input object is used to define the gap between two layers in a complex fenestration system, where the Construction:ComplexFenestrationState object is used. It references the gas or gas mixtures defined in the WindowMaterial:Gas and WindowMaterial:GasMixture objects. It is referenced as a layer in the Construction:ComplexFenestrationState object ;it cannot be referenced as a layer from the Construction object.
+
+\subsubsection{Inputs}\label{inputs-18-009}
+
+\paragraph{Field: Name}\label{field-name-12-011}
+
+Unique name of the gap.
+
+\paragraph{Field: Thickness}\label{field-thickness-5}
+
+The thickness (m) of the gap layer.
+
+\paragraph{Field: Pressure}\label{field-pressure-000}
+
+The pressure (Pa) of the gas in the gap layer, used to calculate the gas properties of the glazing system gap. Default is atmospheric pressure, 101325 Pa.When modeling vacuum glazing, this value should represent the pressure in the evacuated glazing system. If this pressure is less that the ThermalModelParams:PressureLimit value, the the glazing system will be modeled as a vacuum glazing.
+
+\paragraph{Field: Deflection State}\label{field-deflection-state}
+
+This field is used when modeling the deflection of the glass layers in a window if the WinodowThermalModel:Params value for ``deflection model'' is ``MeasuredDeflection''.
+
+\paragraph{Field: Support Pillar}\label{field-support-pillar}
+
+References the support pillar of the gap layer if vacuum glazing is being modeled.~ If left empty, then it is considered that gap layer does not have support pillars.
+
+\paragraph{Field: Gas (or GasMixture)}\label{field-gas-or-gasmixture}
+
+References gas (WindowMaterial:Gas) or gas mixture (WindowMaterial:GasMixture) of the gap layer.
+
+An IDF example for simple glazing:
+
+\begin{lstlisting}
+
+WindowMaterial:Gas,
+  Gas_1_W_0_0120,                                !- gap name - Air
+  Air,                                           !- type
+  0.0120;                                        !- thickness
+
+
+  WindowMaterial:Gap,
+  Gap_1_Layer,                                   !- gap name: Air
+  0.0120,                                        !- thickness
+  Gas_1_W_0_0120,                                !- Gas (or Gas Mixture) name
+  101325.0000;                                   !- pressure
+\end{lstlisting}
+
+An IDF example for vacuum glazing:
+
+\begin{lstlisting}
+
+WindowMaterial:Gap,
+  Gap_16_Layer,                     !- gap name: Vacuum_0.001_pr-0.5_ps-50.8
+  0.0003,                                             !- thicknessGas_16_W_0_0003,                                    !- Gas (or Gas Mixture) name
+  0.1333,                                             !- pressure
+  ,                                                   !- deflection state
+  SupportPillar_16_Gap_1;                             !- SupportPillar
+
+
+  WindowGap:SupportPillar,
+  SupportPillar_16_Gap_1,                             !- Name
+  0.0508,                                             !- spacing
+  0.0005;                                             !- radius
+\end{lstlisting}
+
+\subsection{WindowGap:DeflectionState}\label{windowgapdeflectionstate}
+
+This input object is used to enter data describing deflection state of the gap.~ It is referenced from WindowMaterial:Gap object only and it is used only when deflection model is set to MeasuredDeflection (see WindowThermalModel:Params), otherwise it is ignored.
+
+\subsubsection{Inputs}\label{inputs-19-006}
+
+\paragraph{Field: Name}\label{field-name-13-010}
+
+Unique name of the deflection state.
+
+\paragraph{Field: Deflected Thickness}\label{field-deflected-thickness}
+
+The thickness (m) of the gap in deflected state.~ It represents value of deflection at point of maximum which is usualy at the center poing of glazing system.~ It is used only with tarcog algorithm set to Measured Deflection (WindowThermalModel:Params), otherwise this field will be ignored.
+
+An IDF example where WindowThermalModel:Params Deflection Model = MeasuredDeflection:
+
+\begin{lstlisting}
+
+WindowMaterial:Gap,
+  Gap_1_Layer,                                  !- gap name: Air
+  0.0120,                                       !- thickness
+  Gas_1_W_0_0120,                               !- Gas (or Gas Mixture) name
+  101325.0000,                                  !- pressure
+  Gap_1_Deflection;                              !- deflection state
+
+
+  WindowGap:DeflectionState,       !- deflection state of gap
+    Gap_1_Deflection,              !- name
+    0.011;                         !- gap thickness in deflected state
+\end{lstlisting}
+
+\subsection{WindowGap:SupportPillar}\label{windowgapsupportpillar}
+
+This input object is used to enter data describing support pillar of the gap.~ Support pillars are used in vacuum glazing in order to prevent deflection of glass layers.
+
+\begin{figure}[hbtp] % fig 11
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image029.png}
+\caption{Support Pillar \protect \label{fig:support-pillar}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-20-006}
+
+\paragraph{Field: Name}\label{field-name-14-009}
+
+Unique name of the support pillar.
+
+\paragraph{Field: Spacing}\label{field-spacing}
+
+Distance (m) between support pillar centers (see the Engineering reference document for more information).
+
+\paragraph{Field: Radius}\label{field-radius}
+
+The radius (m) of the support pillar (see Engineering reference document for more information).
+
+An IDF example for vacuum glazing (see Vacuum Glazing example in WindowMaterial:Gap above)
+
+\begin{lstlisting}
+
+WindowGap:SupportPillar,       !- gap support pillar
+    SupportPillar_16_Gap_1,      !- basis matrix name
+    0.05,                        !- pillar spacing
+    0.005;                       !- pillar radius
+\end{lstlisting}
+
+\subsection{WindowMaterial:SimpleGlazingSystem}\label{windowmaterialsimpleglazingsystem}
+
+\warning{This model should be used with caution. There may be significant differences in performance between the simple window system and the usual more detailed model.}
+
+This input object differs from the other WindowMaterial objects in that it describes an entire glazing system rather than individual layers. This object is used when only very limited information is available on the glazing layers or when specific performance levels are being targeted. The layer by layer description offers superior method of modeling windows that should be used instead of this object when sufficient data are available. This object accesses a model that turns simple performance indices into a fuller model of the glazing system.
+
+The performance indices are U-factor and Solar Heat Gain Coefficient, and optionally Visible Transmittance. The values for these performance indices can be selected by the user to represent either glazing-only windows (with no frame) or an average window performance that includes the frame. Inside the program the model produces an equivalent window glazing layer with no frame. The properties of the modeled glazing layer are reported to the EIO file using the IDF input object syntax for the WindowMaterial:Glazing input object. This equivalent layer could be reused in subsequent models if desired, however there will be important differences in the modeled window performance because the simple glazing system model includes its own special model for angular dependence when incident beam solar is not normal to the plane of the window.
+
+When this object is referenced in a Construction object, it cannot be used with other glazing or gas material layers. Shades or blinds cannot be located between the glass, but these can be used on the inside or the outside of the glazing system.~~ If the glazing system does have between-the-glass shades or blinds, then the U and SHGC values entered in this object should include the impacts of those layers. Adding window treatment layers such as shades or screens will alter the overall performance to be different than the performance levels prescribed in this object.
+
+\subsubsection{Inputs}\label{inputs-21-006}
+
+\paragraph{Field: Name}\label{field-name-15-009}
+
+The name of the glazing system.~ This value is unique across all constructions.
+
+\paragraph{Field: U-Factor}\label{field-u-factor}
+
+This field describes the value for window system U-Factor, or overall heat transfer coefficient. Units are in W/m\(^{2}\)·K. This is the rated (NFRC) value for U-factor under winter heating conditions. The U-factor is assumed to be for vertically mounted products. Although the maximum allowable input is U-7.0 W/m\(^{2}\)·K, the effective upper limit of the glazings generated by the underlying model is around U-5.8 W/m\(^{2}\)·K.
+
+\paragraph{Field: Solar Heat Gain Coefficient}\label{field-solar-heat-gain-coefficient}
+
+This field describes the value for SHGC, or solar heat gain coefficient. There are no units. This is the rated (NFRC) value for SHGC under summer cooling conditions and represents SHGC for normal incidence and vertical orientation.
+
+\paragraph{Field: Visible Transmittance}\label{field-visible-transmittance}
+
+This field is optional. If it is omitted, then the visible transmittance properties are taken from the solar properties. If it is included then the model includes it when developing properties for the glazing system. This is the rated (NFRC) value for visible transmittance at normal incidence.
+
+An example of this object.
+
+\begin{lstlisting}
+
+WindowMaterial:SimpleGlazingSystem,
+      SimpleWindow:DOUBLE PANE WINDOW , !- Name
+      2.716 , !-  U-Factor
+      0.763 , !-  Solar Heat Gain Coefficient
+      0.812 ; !-  Visible Transmittance
+\end{lstlisting}
+
+\subsection{WindowMaterial:Shade}\label{windowmaterialshade}
+
+This object specifies the properties of window shade materials. Reflectance and emissivity properties are assumed to be the same on both sides of the shade. Shades are considered to be perfect diffusers (all transmitted and reflected radiation is hemispherically-diffuse) with transmittance and reflectance independent of angle of incidence. There is an EnergyPlus Reference Data Set for WindowMaterial:Shade that contains properties of generic window shades.
+
+Window shades can be on the inside of the window (``interior shades''), on the outside of the window (``exterior shades''), or between glass layers (``between-glass shades''). When in place, the shade is assumed to cover all of the glazed part of the window, including dividers; it does not cover any of the window frame, if present. The plane of the shade is assumed to be parallel to the glazing.
+
+WindowMaterial:Shade can be used for diffusing materials such as drapery and translucent roller shades. For slat-type shading devices, like Venetian blinds, that have a strong angular dependence of transmission, absorption and reflection, it is better to use WindowMaterial:Blind. WindowMaterial:Screen should be used to model wire mesh insect screens where the solar and visible transmission and reflection properties vary with the angle of incidence of solar radiation.
+
+Transmittance and reflectance values for drapery material with different color and openness of weave can be obtained from manufacturers or determined from 2001 ASHRAE Fundamentals, Chapter 30, Fig. 31.
+
+There are two methods of assigning a shade to a window:
+
+\subsubsection{Inputs}\label{inputs-22-005}
+
+\paragraph{Method 1:}\label{method-1}
+
+1)~~~Define the construction of the window without the shade, the so-called ``bare'' construction.
+
+2)~~~Reference the bare construction in the FenestrationSurface:Detailed for the window.
+
+3)~~~Define the WindowMaterial:Shade.
+
+4)~~~Define a WindowProperty:ShadingControl for the window in which you (a) specify that this WindowMaterial:Shade is the window's shading device and (b) specify how the shade is controlled.
+
+\paragraph{Method 2:}\label{method-2}
+
+1)~~~Define the Construction of the window without the shade, the so-called ``bare'' construction.
+
+2)~~~Reference the bare construction in the FenestrationSurface:Detailed for the window.
+
+3)~~~Define the WindowMaterial:Shade.
+
+4)~~~Define another Construction, called the ``shaded construction,'' that includes the WindowMaterial:Shade.
+
+5)~~~Define a WindowProperty:ShadingControl for the window in which you (a) reference the shaded construction and (b) specify how the shade is controlled.
+
+Note that WindowProperty:ShadingControl has to be used with either method, even if the shade is in place at all times. You will get an error message if you try to reference a shaded construction directly from FenestrationSurface:Detailed.
+
+\paragraph{Field: Name}\label{field-name-16-009}
+
+Name of the shade. It is referenced as an inside or outside layer in a window construction.
+
+\paragraph{Field: Solar Transmittance}\label{field-solar-transmittance}
+
+Transmittance averaged over the solar spectrum. Assumed independent of incidence angle.
+
+\paragraph{Field: Solar Reflectance}\label{field-solar-reflectance}
+
+Reflectance averaged over the solar spectrum. Assumed same on both sides of shade and independent of incidence angle.
+
+\paragraph{Field: Visible Transmittance}\label{field-visible-transmittance-1}
+
+Transmittance averaged over the solar spectrum and weighted by the response of the human eye. Assumed independent of incidence angle.
+
+\paragraph{Field: Visible Reflectance}\label{field-visible-reflectance}
+
+Reflectance averaged over the solar spectrum and weighted by the response of the human eye. Assumed same on both side of shade and independent of incidence angle.
+
+\paragraph{Field: Thermal Hemispherical Emissivity}\label{field-thermal-hemispherical-emissivity}
+
+Effective long-wave emissivity. Assumed same on both sides of shade. We can approximate this~ effective emissivity, \(\varepsilon_{eff}\), as follows. Let \(\eta\) be the ``openness'' the shade, i.e.,~ the ratio of the area of openings in the shade to the overall shade area (see Field: Air-Flow Permeability, below). Let the emissivity of the shade material be \(\varepsilon\). Then
+
+\begin{equation}
+{\varepsilon_{{\rm{eff}}}} \approx \varepsilon \left( {1 - \eta } \right)
+\end{equation}
+
+For most non-metallic materials \(\varepsilon\) is about 0.9.
+
+\paragraph{Field: Thermal Transmittance}\label{field-thermal-transmittance}
+
+Effective long-wave transmittance. Assumed independent of incidence angle. We can approximate this effective long-wave transmittance, \(T_{\rm{eff}}\) as follows. Let \(\eta\) be the ``openness'' of the shade, i.e., the ratio of the area of openings in the shade to the overall shade area. Let the long-wave transmittance of the shade material be \(T\). Then
+
+\begin{equation}
+T_{\rm{eff}} \approx \eta + T \left( 1 - \eta \right)
+\end{equation}
+
+For most materials \(T\) is very close to zero, which gives
+
+\begin{equation}
+T_{\rm{eff}} \approx \eta
+\end{equation}
+
+\paragraph{Field: Thickness}\label{field-thickness-6}
+
+Thickness of the shade material (m). If the shade is not flat, such as for pleated pull-down shades or folded drapery, the average thickness normal to the plane of the shade should be used.
+
+\paragraph{Field: Conductivity}\label{field-conductivity-3}
+
+Shade material conductivity (W/m-K).
+
+\paragraph{Field: Shade to Glass Distance}\label{field-shade-to-glass-distance}
+
+Distance from shade to adjacent glass (m). This is denoted by \emph{s} in Figure~\ref{fig:vertical-section-a-and-perspective-view-b-of} and Figure~\ref{fig:examples-of-air-flow-openings-for-an-interior}, below. If the shade is not flat, such as for pleated pull-down shades or folded drapery, the average shade-to-glass distance should be used. (The shade-to-glass distance is used in calculating the natural convective air flow between glass and shade produced by buoyancy effects.). Note used for between-glass shades.
+
+In the following, \emph{H} is the glazing height and \emph{W} is the glazing width.
+
+\paragraph{Field: Top Opening Multiplier}\label{field-top-opening-multiplier}
+
+Effective area for air flow at the top of the shade divided by \emph{sW}, the horizontal area between glass and shade (see Figures below).
+
+\paragraph{Field: Bottom Opening Multiplier}\label{field-bottom-opening-multiplier}
+
+Effective area for air flow at the bottom of the shade divided by \emph{sW}, the horizontal area between glass and shade (see Figures below).
+
+\paragraph{Field: Left-Side Opening Multiplier}\label{field-left-side-opening-multiplier}
+
+Effective area for air flow at the left side of the shade divided by \emph{sH}, the vertical area between glass and shade (see Figures below).
+
+\paragraph{Field: Right-Side Opening Multiplier}\label{field-right-side-opening-multiplier}
+
+Effective area for air flow at the right side of the shade divided by \emph{sH}, the vertical area between glass and shade (see Figures below).
+
+\paragraph{Field: Field: Air-Flow Permeability}\label{field-field-air-flow-permeability}
+
+The fraction of the shade surface that is open to air flow, i.e., the total area of openings (``holes'') in the shade surface divided by the shade area, \emph{HW}. If air cannot pass through the shade material, Air-Flow Permeability = 0. For drapery fabric and screens the Air-Flow Permeability can be taken as the ``openness'' of the fabric (see 2001 ASHRAE Fundamentals, Chapter 30, Fig. 31), which is 0.0 to 0.07 for closed weave, 0.07 to 0.25 for semi-open weave, and 0.25 and higher for open weave.
+
+\begin{figure}[hbtp] % fig 12
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image033.png}
+\caption{Vertical section (a) and perspective view (b) of glass  and interior shade layers  showing variables used in the gap air flow analysis. In (b), the air-flow opening areas \(A_{\rm{bot}}\), \(A_{\rm{top}}\), \(A_{l}\), \(A_{r}\) and \(A_{h}\) are shown schematically. See \emph{Engineering Manual} for definition of thermal variables. \protect \label{fig:vertical-section-a-and-perspective-view-b-of}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 13
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image034.png}
+\caption{Examples of air-flow openings for an interior shade covering glass of height \(H\) and width \(W\). Not to scale. (a) Horizontal section through shade with openings on the left and right sides (top view). (b) Vertical section through shade with openings at the top and bottom (side view). In (a) Left-Side Opening Multiplier = \(A_{l}/sH = min(l/s, 1)\) and Right-Side Opening Multiplier = \(A_{r}/sH = min(r/s, 1)\). In (b) Top Opening Multiplier = \(A_{\rm{top}}/sW = t/s\) and Bottom Opening Multiplier = \(A_{\rm{bot}}/sW = b/s\). \protect \label{fig:examples-of-air-flow-openings-for-an-interior}}
+\end{figure}
+
+An IDF example:
+
+\begin{lstlisting}
+WindowMaterial:Shade,
+  DRAPES - CLOSE WEAVE MEDIUM,  !- Name
+  0.05,                         !- Solar transmittance
+  0.3000000,                    !- Solar Reflectance
+  .05,                          !- Visible transmittance
+  0.3000000,                    !- Visible reflectance
+  0.9000000,                    !- Thermal Hemispherical Emissivity
+  0.0,                          !- Thermal Transmittance
+  0.003,                        !- Thickness {m}
+  0.1,                          !- Conductivity {W/m-K}
+  0.050,                        !- Shade to glass distance {m}
+  1.0,                          !- Top opening multiplier
+  1.0,                          !- Bottom opening multiplier
+  0.0,                          !- Left-side opening multiplier
+  0.0,                          !- Right-side opening multiplier
+  0.0;                          !- Air flow permeability
+\end{lstlisting}
+
+\subsection{WindowMaterial:Blind}\label{windowmaterialblind}
+
+This object specifies the properties of a window blind consisting of flat, equally-spaced slats. Unlike window shades, which are modeled as perfect diffusers, window blinds have solar and visible transmission and reflection properties that strongly depend on slat angle and angle of incidence of solar radiation. There is an EnergyPlus Reference Data Set for WindowMaterial:Blind that contains properties of generic window blinds.
+
+Blinds can be located on the inside of the window (``interior blinds''), on the outside of the window (``exterior blinds''), or between two layers of glass (``between-glass blinds''). When in place, the blind is assumed to cover all of the glazed part of the window, including dividers; it does not cover any of the window frame, if present. The plane of the blind is assumed to be parallel to the glazing. When the blind is retracted it is assumed to cover none of the window. The solar and thermal effects of the blind's support strings, tapes or rods are ignored. Slat curvature, if present, is ignored.
+
+There are two methods of assigning a blind to a window:
+
+\subsubsection{Inputs}\label{inputs-23-005}
+
+\paragraph{Method 1:}\label{method-1-1}
+
+1)~~~Define the construction of the window without the blind, the so-called ``bare'' construction.
+
+2)~~~Reference the bare construction in the FenestrationSurface:Detailed for the window.
+
+3)~~~Define the WindowMaterial:Blind.
+
+4)~~~Define a WindowProperty:ShadingControl for the window in which you (a) specify that this WindowMaterial:Blind is the window's shading device and (b) specify how the blind is controlled.
+
+\paragraph{Method 2:}\label{method-2-1}
+
+1)~~~Define the Construction of the window without the blind, the so-called ``bare'' construction.
+
+2)~~~Reference the bare construction in the FenestrationSurface:Detailed for the window.
+
+3)~~~Define the WindowMaterial:Blind.
+
+4)~~~Define another Construction, called the ``shaded construction,'' that includes the WindowMaterial:Blind.
+
+5)~~~Define a WindowProperty:ShadingControl for the window in which you (a) reference the shaded construction and (b) specify how the blind is controlled.
+
+Note that WindowProperty:ShadingControl has to be used with either method, even if the blind is in place at all times. You will get an error message if you try to reference a construction with a blind directly from Window objects (FenestrationSurface:Detailed or Window).
+
+Note also that WindowProperty:ShadingControl is used to determine not only when the blind is in place, but how its slat angle is controlled.
+
+\paragraph{Field: Name}\label{field-name-17-007}
+
+Name of the blind. It is referenced as a layer in a window construction (ref: Construction object) or as a ``Material Name of Shading Device'' in a WindowProperty:ShadingControl object.
+
+\paragraph{Field: Slat Orientation}\label{field-slat-orientation}
+
+The choices are Horizontal and Vertical. ``Horizontal'' means the slats are parallel to the bottom of the window; this is the same as saying that the slats are parallel to the X-axis of the window. ``Vertical'' means the slats are parallel to Y-axis of the window.
+
+\paragraph{Field: Slat Width}\label{field-slat-width}
+
+The width of the slat measured from edge to edge (m). See Figure~\ref{fig:a-side-view-of-a-window-blind-with-horizontal}.
+
+\paragraph{Field: Slat Separation}\label{field-slat-separation}
+
+The distance between the front of a slat and the back of the adjacent slat (m). See Figure~\ref{fig:a-side-view-of-a-window-blind-with-horizontal}.
+
+\paragraph{Field: Slat Thickness}\label{field-slat-thickness}
+
+The distance between the faces of a slat (m). See Figure~\ref{fig:a-side-view-of-a-window-blind-with-horizontal}.
+
+\paragraph{Field: Slat Angle}\label{field-slat-angle}
+
+The angle (degrees) between the glazing outward normal and the slat outward normal, where the outward normal points away from the front face of the slat (degrees). See Figure~\ref{fig:a-side-view-of-a-window-blind-with-horizontal}.
+
+If the WindowProperty:ShadingControl for the blind has Type of Slat Angle Control for Blinds = FixedSlatAngle, the slat angle is fixed at ``Slat Angle.''
+
+If Type of Slat Angle Control for Blinds = BlockBeamSolar, the program automatically adjusts the slat angle so as just block beam solar radiation. In this case the value of ``Slat Angle'' is used only when the blind is in place and there is no beam solar radiation incident on the blind.
+
+If Type of Slat Angle Control for Blinds = ScheduledSlatAngle, the slat angle is variable. In this case ``Slat Angle'' is not applicable and the field should be blank.
+
+If Type of Slat Angle Control for Blinds = FixedSlatAngle and ``Slat Angle'' is less than the minimum or greater than the maximum allowed by Slat Width, Slat Separation and Slat Thickness, the slat angle will be reset to the corresponding minimum or maximum and a warning will be issued.
+
+\paragraph{Field: Slat Conductivity}\label{field-slat-conductivity}
+
+The thermal conductivity of the slat (W/m-K).
+
+\paragraph{Field: Slat Beam Solar Transmittance}\label{field-slat-beam-solar-transmittance}
+
+The beam solar transmittance of the slat, assumed to be independent of angle of incidence on the slat. Any transmitted beam radiation is assumed to be 100\% diffuse (i.e., slats are translucent).
+
+\paragraph{Field: Front Side Slat Beam Solar Reflectance}\label{field-front-side-slat-beam-solar-reflectance}
+
+The beam solar reflectance of the front side of the slat, assumed to be independent of angle of incidence (matte finish). This means that slats with a large specularly-reflective component (shiny slats) are not well modeled.
+
+\paragraph{Field: Back Side Slat Beam Solar Reflectance}\label{field-back-side-slat-beam-solar-reflectance}
+
+The beam solar reflectance of the back side of the slat, assumed to be independent of angle of incidence (matte finish). This means that slats with a large specularly-reflective component (shiny slats) are not well modeled.
+
+\paragraph{Field: Slat Diffuse Solar Transmittance}\label{field-slat-diffuse-solar-transmittance}
+
+The slat transmittance for hemispherically diffuse solar radiation. This value should equal ``Slat Beam Solar Transmittance.''
+
+\paragraph{Field: Front Side Slat Diffuse Solar Reflectance}\label{field-front-side-slat-diffuse-solar-reflectance}
+
+The front-side slat reflectance for hemispherically diffuse solar radiation. This value should equal ``Front Side Slat Beam Solar Reflectance.''
+
+\paragraph{Field: Back Side Slat Diffuse Solar Reflectance}\label{field-back-side-slat-diffuse-solar-reflectance}
+
+The back-side slat reflectance for hemispherically diffuse solar radiation. This value should equal ``Back Side Slat Beam Solar Reflectance.''
+
+\paragraph{Field: Slat Beam Visible Transmittance}\label{field-slat-beam-visible-transmittance}
+
+The beam visible transmittance of the slat, assumed to be independent of angle of incidence on the slat. Any transmitted visible radiation is assumed to be 100\% diffuse (i.e., slats are translucent).
+
+\paragraph{Field: Front Side Slat Beam Visible Reflectance}\label{field-front-side-slat-beam-visible-reflectance}
+
+The beam visible reflectance on the front side of the slat, assumed to be independent of angle of incidence (matte finish). This means that slats with a large specularly-reflective component (shiny slats) are not well modeled.
+
+\paragraph{Field: Back Side Slat Beam Visible Reflectance}\label{field-back-side-slat-beam-visible-reflectance}
+
+The beam visible reflectance on the front side of the slat, assumed to be independent of angle of incidence (matte finish). This means that slats with a large specularly-reflective component (shiny slats) are not well modeled.
+
+\paragraph{Field: Slat Diffuse Visible Transmittance}\label{field-slat-diffuse-visible-transmittance}
+
+The slat transmittance for hemispherically diffuse visible radiation. This value should equal ``Slat Beam Visible Transmittance.''
+
+\paragraph{Field: Front Side Slat Diffuse Visible Reflectance}\label{field-front-side-slat-diffuse-visible-reflectance}
+
+The front-side slat reflectance for hemispherically diffuse visible radiation. This value should equal ``Front Side Slat Beam Visible Reflectance.''
+
+\paragraph{Field: Back Side Slat Diffuse Visible Reflectance}\label{field-back-side-slat-diffuse-visible-reflectance}
+
+The back-side slat reflectance for hemispherically diffuse visible radiation. This value should equal ``Back Side Slat Beam Visible Reflectance..''
+
+\paragraph{Field: Slat Infrared Hemispherical Transmittance}\label{field-slat-infrared-hemispherical-transmittance}
+
+The slat Infrared transmittance. It is zero for solid metallic, wooden or glass slats, but may be non-zero in some cases (e.g., thin plastic slats).
+
+\paragraph{Field: Front Side Slat Infrared~ Hemispherical Emissivity}\label{field-front-side-slat-infrared-hemispherical-emissivity}
+
+Front-side hemispherical emissivity of the slat. Approximately 0.9 for most materials. The most common exception is bare (unpainted) metal slats or slats finished with a metallic paint.
+
+\paragraph{Field: Back Side Slat Infrared~ Hemispherical Emissivity}\label{field-back-side-slat-infrared-hemispherical-emissivity}
+
+Back-side hemispherical emissivity of the slat. Approximately 0.9 for most materials. The most common exception is bare (unpainted) metal slats or slats finished with a metallic paint.
+
+\paragraph{Field: Blind to Glass Distance}\label{field-blind-to-glass-distance}
+
+For interior and exterior blinds, the distance from the mid-plane of the blind to the adjacent glass (m). See Figure~\ref{fig:a-side-view-of-a-window-blind-with-horizontal}. Not used for between-glass blinds. As for window shades (ref: WindowMaterial:Shade) this distance is used in calculating the natural convective air flow between glass and blind that is produced by buoyancy effects.
+
+\paragraph{Opening Multipliers}\label{opening-multipliers}
+
+The following opening multipliers are defined in the same way as for window shades (see WindowMaterial:Shade, Figure~\ref{fig:vertical-section-a-and-perspective-view-b-of} and Figure~\ref{fig:examples-of-air-flow-openings-for-an-interior}). Note that, unlike window shades, there is no input for Air-Flow Permeability; this is automatically calculated by the program from slat angle, width and separation.
+
+\paragraph{Field: Blind Top Opening Multiplier}\label{field-blind-top-opening-multiplier}
+
+Defined as for Material:WindowShade.
+
+\paragraph{Field: Blind Bottom Opening Multiplier}\label{field-blind-bottom-opening-multiplier}
+
+Defined as for Material:WindowShade.
+
+\paragraph{Field: Blind Left-Side Opening Multiplier}\label{field-blind-left-side-opening-multiplier}
+
+Defined as for Material:WindowShade.
+
+\paragraph{Field: Blind Right-Side Opening Multiplier}\label{field-blind-right-side-opening-multiplier}
+
+Defined as for Material:WindowShade.
+
+\paragraph{Field: Minimum Slat Angle}\label{field-minimum-slat-angle}
+
+The minimum allowed slat angle (degrees). Used only if WindowProperty:ShadingControl (for the window that incorporates this blind) varies the slat angle (i.e., the WindowProperty:ShadingControl has Type of Slat Angle Control for Blinds = ScheduledSlatAngle or BlockBeamSolar). In this case, if the program tries to select a slat angle less than Minimum Slat Angle it will be reset to Minimum Slat Angle. (Note that if the Minimum Slat Angle itself is less than the minimum allowed by Slat Width, Slat Separation and Slat Thickness, it will be reset to that minimum.)
+
+\paragraph{Field: Maximum Slat Angle}\label{field-maximum-slat-angle}
+
+The maximum allowed slat angle (degrees). Used only if WindowProperty:ShadingControl (for the window that incorporates this blind) varies the slat angle (i.e., the WindowProperty:ShadingControl has Type of Slat Angle Control for Blinds = ScheduledSlatAngle or BlockBeamSolar). In this case, if the program tries to select a slat angle greater than Maximum Slat Angle the slat angle will be reset to Maximum Slat Angle. (Note that if the Maximum Slat Angle itself is greater than the maximum allowed by Slat Width, Slat Separation and Slat Thickness, it will be reset to that maximum.)
+
+An IDF example:
+
+\begin{lstlisting}
+
+WindowMaterial:Blind,
+   White Painted Metal Blind,   !- Name
+   HORIZONTAL, !- Slat orientation
+   0.025   , !- Slat width (m)
+   0.01875 , !- Slat separation (m)
+   0.001   , !- Slat thickness (m)
+   45.0    , !- Slat angle (deg)
+   44.9    , !- Slat conductivity (W/m-K)
+   0.0     , !- Slat beam solar transmittance
+   0.8     , !- Front Side Slat beam solar reflectance
+   0.8     , !- Back Side Slat beam solar reflectance
+   0.0     , !- Slat diffuse solar transmittance
+   0.8     , !- Front Side Slat diffuse solar reflectance
+   0.8     , !- Back Side Slat diffuse solar reflectance
+   0.0     , !- Slat beam visible transmittance
+   0.7     , !- Front Side Slat beam visible reflectance
+   0.7     , !- Back Side Slat beam visible reflectance
+   0.0     , !- Slat diffuse visible transmittance
+   0.7     , !- Front Side Slat diffuse visible reflectance
+   0.7     , !- Back Side Slat diffuse visible reflectance
+   0.0     , !- Slat Infrared hemispherical transmittance
+   0.9     , !- Front Side Slat Infrared hemispherical emissivity
+   0.9     , !- Back Side Slat Infrared hemispherical emissivity
+   0.050   , !- Blind-to-glass distance
+   0.0     , !- Blind top opening multiplier
+   0.0     , !- Blind bottom opening multiplier
+   0.5     , !- Blind left-side opening multiplier
+   0.5     , !- Blind right-side opening multiplier
+   ,         !- Minimum slat angle (deg)
+   ;         !- Maximum slat angle (deg)
+\end{lstlisting}
+
+\begin{figure}[hbtp] % fig 14
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image035.png}
+\caption{(a) Side view of a window blind with horizontal slats (or top view of blind with vertical slats) showing slat geometry. The front face of a slat is shown by a heavy line. The slat angle is defined as the angle between the glazing outward normal and the slat outward normal, where the outward normal points away from the front face of the slat. (b) Slat orientations for representative slat angles. The slat angle varies from 0\(^{o}\), when the front of the slat is parallel to the glazing and faces toward the outdoors,  to 90\(^{o}\), when the slat is perpendicular to the glazing, to 180\(^{o}\), when the front of the slat is parallel to the glazing and faces toward the indoors. The minimum and maximum slat angles are determined by the slat thickness, width and separation. \protect \label{fig:a-side-view-of-a-window-blind-with-horizontal}}
+\end{figure}
+
+\subsection{WindowMaterial:ComplexShade}\label{windowmaterialcomplexshade}
+
+This input object is used to define shade layers used in the Construction:ComplexFenestrationState object.
+
+\subsubsection{Inputs}\label{inputs-24-003}
+
+\paragraph{Field: Name}\label{field-name-18-007}
+
+Unique name of the shading layer.
+
+\paragraph{Field: Shading Layer Type}\label{field-shading-layer-type}
+
+The type of shading layer. The options are:
+
+\begin{itemize}
+\item
+  Venetian -- for modeling venetian blinds
+\item
+  Woven -- for modeling shading systems with a regular weave
+\item
+  Perforated -- for modeling perforated screens
+\item
+  BSDF -- for modeling shades whose properties are represented by a BSDF file
+\item
+  OtherShadingType -- for modeling shading systems which do not belong to the any of the previous group
+\end{itemize}
+
+\paragraph{Field: Thickness}\label{field-thickness-7}
+
+The thickness (m) of the shading layer. This value is ignored for ShadingLayerType = Venetian, because the program will calculate the thickness based on the slat angle. This value is needed for ShadingLayerType = Woven and Perforated
+
+\paragraph{Field: Conductivity}\label{field-conductivity-4}
+
+The conductivity (W/mK) of the shading layer material. Default: 1.0
+
+\begin{itemize}
+\item
+  Venetian -- the conductivity of the venetian blind slat material
+\item
+  Woven -- the conductivity of the woven shade material (such as the thread for a fabric shade)
+\item
+  Perforated -- for modeling perforated screens
+\item
+  BSDF -- for modeling shades whose properties are represented by a BSDF file
+\item
+  OtherShadingType -- for modeling shading systems which do not belong to the any of the previous group
+\end{itemize}
+
+\paragraph{Field: IR Transmittance}\label{field-ir-transmittance}
+
+The IR transmittance of the shading layer. Minimum value: 0. Maximum value: 1. Default: 0.
+
+\paragraph{Field: Front Emissivity}\label{field-front-emissivity}
+
+The front emissivity of the shading layer. Minimum value: 0. Maximum value: 1. Default: 0.90.
+
+\paragraph{Field: Back Emissivity}\label{field-back-emissivity}
+
+The back emissivity of the shading layer. Minimum value: 0. Maximum value: 1. Default: 0.90.
+
+\paragraph{Field: Top Opening Multiplier}\label{field-top-opening-multiplier-1}
+
+The top opening multiplier value will depend on the location of the shading device within the glazing system. There are several possible scenarios which can occur and they can be divided into two groups:
+
+\textbf{Shading device on the indoor/outdoor side of the window}
+
+In this case the opening multiplier is calculated as the smallest distance between the shading device and the frame (d\(_{top}\)), divided by the gap width (S). There are three possible cases for the position of a shading device the on indoor/outdoor side (see Figure~\ref{fig:three-cases-for-the-dp-calculation-for-an-indoor-outdoor-shade}).
+
+\begin{figure}[htbp]
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/three-cases-for-the-dtop-calculation-for-an-indoor-outdoor-shade-collage.png}
+\caption{Three cases for the D\(_{top}\) calculation for an indoor/outdoor shade: Case a) A shading device between the frame; Case b) A shading device outside the frame, covering the frame; Case c) a shading device outside the frame, not covering the frame. \protect \label{fig:three-cases-for-the-dp-calculation-for-an-indoor-outdoor-shade}}
+\end{figure}
+
+In the case where the distance between the frame and the shading device is bigger than the gap width, the d\(_{top}\) multiplier is equal to one. Therefore, the calculation of the D\(_{top}\) opening multiplier is:
+
+\begin{equation*}
+A_{top} = min(d_{top}/S, 1)
+\end{equation*}
+
+\textbf{Shading device between glass layers}
+
+In this case the opening multiplier is calculated as the smallest distance between the shading device and the frame or spacer (d\(_{top}\)), divided by the smaller gap width (the minimum of (S\(_{1}\) andS\(_{2}\))).
+
+\begin{figure}[htbp]
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/calculation-of-dtop-for-a-shading-device-collage.png}
+\caption{Calculation of Dtop for a shading device between glass layers \protect \label{fig:calculation-of-dtop-for-a-shading-device-between-glass-layers}}
+\end{figure}
+
+The D\(_{top}\) opening multiplier for a between glass shade is calculated as:
+
+\begin{equation*}
+A_{top} = min(d_{top}/S_{min}, 1)
+\end{equation*}
+
+Where
+
+\begin{equation*}
+S_{min} = min(S_1, S_2)
+\end{equation*}
+
+\paragraph{Field: Bottom Opening Multiplier}\label{field-bottom-opening-multiplier-1}
+
+The bottom opening multiplier (d\(_{bot}\)) is calculated in the same way as the top opening multiplier, with the rules applied to the bottom of the shading device.
+
+\paragraph{Field: Left Side Opening Multiplier}\label{field-left-side-opening-multiplier-1}
+
+The left side opening multiplier (d\(_{left}\)) is calcuated in the same way as the top opening multiplier, with the rules applied to the left side of the shading device.
+
+\paragraph{Field: Right Side Opening Multiplier}\label{field-right-side-opening-multiplier-1}
+
+The right side opening multiplier (d\(_{right}\)) is calcuated in the same way as the top opening multiplier, with the rules applied to the right side of the shading device.
+
+\paragraph{Field: Front Opening Multiplier}\label{field-front-opening-multiplier}
+
+The fraction of glazing system area that is open on the front of the shading layer (see Figure~\ref{fig:front-view-of-shading-layer-openings.}). This fraction is calculated as follows: Afront / (W * H), where Afront = Area of the front of the glazing system that is not covered by the shading system, W = the width of the glazing system (IGU) and H is height of the glazing system (IGU).
+
+\begin{figure}[hbtp] % fig 17
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image041.png}
+\caption{Front view of shading layer openings. \protect \label{fig:front-view-of-shading-layer-openings.}}
+\end{figure}
+
+\paragraph{Field: Slat Width}\label{field-slat-width-1}
+
+The width (m) of the venetian slats.~ Used only for ShadingLayerType = Venetian.
+
+\paragraph{Field: Slat Spacing}\label{field-slat-spacing}
+
+The distance (m) between front sides of the venetian slats.~ Used only for ShadingLayerType = Venetian.
+
+\paragraph{Field: Slat Thickness}\label{field-slat-thickness-1}
+
+The thickness (m) of the venetian slats.~ Used only for ShadingLayerType = Venetian.
+
+\paragraph{Field: Slat Angle}\label{field-slat-angle-1}
+
+The slat tilt angle (degrees) of the venetian slats.~ Used only for ShadingLayerType = Venetian.~ Range of slat angle is from -90 to 90 degrees.
+
+\paragraph{Field: Slat Conductivity}\label{field-slat-conductivity-1}
+
+The conductivity (W/mK) of the venetian slats.~ Used only for ShadingLayerType = Venetian.
+
+\paragraph{Field: Slat Curve}\label{field-slat-curve}
+
+The curvature radius (m) of the venetian slats.~ Setting this value to zero means there is no curvature in the slat (it is flat), while a non-zero value is the radius of the slat curve.~ This value cannot be smaller than Slat Width / 2.~ Used only for ShadingLayerType = Venetian.
+
+\begin{figure}[hbtp] % fig 18
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image042.png}
+\caption{Side view of horizontal venetian blind slats or top view of blinds with vertical slats.  Front face of slats is marked with red line. \protect \label{fig:side-view-of-horizontal-venetian-blind-slats}}
+\end{figure}
+
+An IDF example for ShadingLayerType = Venetian
+
+\begin{lstlisting}
+
+WindowMaterial:ComplexShade,       !- venetian blind layer
+    Shade_30001_Layer,               !- name
+    Venetian,                        !- shading layer type
+    0.005,                           !- thickness
+    160,                             !- layer conductivity
+    0.0,                             !- IR transmittance
+    0.9,                             !- front emissivity
+    0.9,                             !- back emissivity
+    0.0,                             !- top opening multiplier
+    0.0,                             !- bottom opening multiplier
+    0.0,                             !- left side opening multiplier
+    0.0,                             !- right side opening multiplier
+    0.05,                            !- front opening multiplier
+    0.016,                           !- venetian slat width
+    0.012,                           !- venetian slat spacing
+    0.0006,                          !- venetian slat thickness
+    -45.00,                          !- venetian slat angle
+    160.00,                          !- venetian slat conductivity
+    0.0000;                          !- venetian slat curve
+\end{lstlisting}
+
+An IDF example for ShadingLayerType = Woven
+
+(Note that it is not necessary to include ``blank'' lines for the venetian blind input for a Woven shade definition).
+
+\begin{lstlisting}
+
+WindowMaterial:ComplexShade,       !- woven shade layer
+    Shade_30002_Layer,               !- name
+    Woven,                           !- shading layer type
+    0.011,                           !- thickness
+    1,                               !- layer conductivity
+    0.0,                             !- IR transmittance
+    0.9,                             !- front emissivity
+    0.9,                             !- back emissivity
+    0.0,                             !- top opening multiplier
+    0.0,                             !- bottom opening multiplier
+    0.0,                             !- left side opening multiplier
+    0.0,                             !- right side opening multiplier
+    0.17;                            !- front opening multiplier
+\end{lstlisting}
+
+\subsection{WindowMaterial:Screen}\label{windowmaterialscreen}
+
+This object specifies the properties of exterior window screen materials. The window screen model assumes the screen is made up of intersecting orthogonally-crossed cylinders. The surface of the cylinders is assumed to be diffusely reflecting, having the optical properties of a Lambertian surface.
+
+The beam solar radiation transmitted through a window screen varies with sun angle and is made up of two distinct elements: a direct beam component and a reflected beam component. The direct beam transmittance component is modeled using the geometry of the screen material and the incident angle of the sun to account for shadowing of the window by the screen material. The reflected beam component is an empirical model that accounts for the inward reflection of solar beam off the screen material surface. This component is both highly directional and small in magnitude compared to the direct beam transmittance component (except at higher incident angles, for which case the magnitude of the direct beam component is small or zero and the reflected beam component, though small in absolute terms can be many times larger than the direct beam component). For this reason, the reflected beam transmittance component calculated by the model can be a. disregarded, b. treated as an additive component to direct beam transmittance (and in the same direction), or c. treated as hemispherically-diffuse transmittance based on a user input to the model.
+
+\begin{figure}[hbtp] % fig 19
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image043.png}
+\caption{Direct beam and reflected beam transmittance components \protect \label{fig:direct-beam-and-reflected-beam-transmittance}}
+\end{figure}
+
+The window screen ``assembly'' properties of overall beam solar reflectance and absorptance (including the screen material `cylinders' and open area) also change with sun angle and are calculated based on the values of the beam solar transmittance components (direct and reflected components described above) and the physical properties of the screen material (i.e., screen material diameter, spacing, and reflectance).
+
+Transmittance, reflectance, and absorptance of diffuse solar radiation are considered constant values and apply to both the front and back surfaces of the screen. These properties are calculated by the model as an average value by integrating the screen's beam solar properties over a quarter hemisphere of incident radiation. Long-wave emissivity is also assumed to be the same for both sides of the screen.
+
+There is an EnergyPlus Reference Data Set for WindowMaterial:Screen that contains properties for generic window screens. Window screens of this type can only be used on the outside surface of the window (``exterior screens''). When in place, the screen is assumed to cover all of the glazed part of the window, including dividers; it does not cover any of the window frame, if present. The plane of the screen is assumed to be parallel to the glazing.
+
+WindowMaterial:Screen can be used to model wire mesh insect screens where the solar and visible transmission and reflection properties vary with the angle of incidence of solar radiation. For diffusing materials such as drapery and translucent roller shades it is better to use the WindowMaterial:Shade object. For slat-type shading devices like Venetian blinds, which have solar and visible transmission and reflection properties that strongly depend on slat angle and angle of incidence of solar radiation, it is better to use WindowMaterial:Blind.
+
+There are two methods of assigning a screen to a window:
+
+\subsubsection{Inputs}\label{inputs-25-003}
+
+\paragraph{Method 1:}\label{method-1-2}
+
+1)~~~Define the construction of the window without the screen, the so-called ``bare'' construction.
+
+2)~~~Reference the bare construction in the FenestrationSurface:Detailed for the window.
+
+3)~~~Define the WindowMaterial:Screen object.
+
+4)~~~Define a WindowProperty:ShadingControl for the window in which you (a) specify that this Material:WindowScreen is the window's shading device, and (b) specify how the screen is controlled.
+
+\paragraph{Method 2:}\label{method-2-2}
+
+1)~~~Define the Construction of the window without the screen, the so-called ``bare'' construction.
+
+2)~~~Reference the bare construction in the FenestrationSurface:Detailed for the window.
+
+3)~~~Define the WindowMaterial:Screen object.
+
+4)~~~Define another Construction, called the ``shaded construction,'' that includes the WindowMaterial:Screen.
+
+5)~~~Define a WindowProperty:ShadingControl for the window in which you (a) reference the shaded construction, and (b) specify how the screen is controlled.
+
+Note that WindowProperty:ShadingControl has to be used with either method, even if the screen is in place at all times. You will get an error message if you try to reference a shaded construction directly from a FenestrationSurface:Detailed object.
+
+\paragraph{Field: Name}\label{field-name-19-004}
+
+Enter a unique name for the screen. This name is referenced as an outside layer in a window construction.
+
+\paragraph{Field: Reflected Beam Transmittance Accounting Method}\label{field-reflected-beam-transmittance-accounting-method}
+
+This input specifies the method used to account for screen-reflected beam solar radiation that is transmitted through the window screen (as opposed to being reflected back outside the building). Since this inward reflecting beam solar is highly directional and is not modeled in the direction of the actual reflection, the user is given the option of how to account for the directionality of this component of beam solar transmittance. Valid choices are DoNotModel, ModelAsDirectBeam (i.e., model as an additive component to direct solar beam and in the same direction), or ModelAsDiffuse (i.e., model as hemispherically-diffuse radiation). The default value is ModelAsDiffuse.
+
+\paragraph{Field: Diffuse Solar Reflectance}\label{field-diffuse-solar-reflectance}
+
+This input specifies the solar reflectance (beam-to-diffuse) of the screen material itself (not the effective value for the overall screen ``assembly'' including open spaces between the screen material). The outgoing diffuse radiation is assumed to be Lambertian (distributed angularly according to Lambert's cosine law). The solar reflectance is assumed to be the same for both sides of the screen. This value must be from 0 to less than 1.0. In the absence of better information, the input value for diffuse solar reflectance should match the input value for diffuse visible reflectance.
+
+\paragraph{Field: Diffuse Visible Reflectance}\label{field-diffuse-visible-reflectance}
+
+This input specifies the visible reflectance (beam-to-diffuse) of the screen material itself (not the effective value for the overall screen ``assembly'' including open spaces between the screen material) averaged over the solar spectrum and weighted by the response of the human eye. The outgoing diffuse radiation is assumed to be Lambertian (distributed angularly according to Lambert's cosine law). The visible reflectance is assumed to be the same for both sides of the screen. This value must be from 0 to less than 1.0.
+
+If diffuse visible reflectance for the screen material is not available, then the following guidelines can be used to estimate this value:
+
+\begin{itemize}
+\item
+  Dark-colored screen (e.g., charcoal):~~~~~~~~~~~~~~~~~ 0.08 -- 0.10
+\item
+  Medium-colored screen (e.g., gray):~~~~~~~~~~~~~~~~~~ 0.20 -- 0.25
+\item
+  Light-colored screen (e.g., bright aluminum):~~~~~~ 0.60 -- 0.65
+\end{itemize}
+
+Commercially-available gray scale or grayscale reflecting chart references can be purchased for improved accuracy in estimating visible reflectance (by visual comparison of screen reflected brightness with that of various known-reflectance portions of the grayscale).
+
+\paragraph{Field: Thermal Hemispherical Emissivity}\label{field-thermal-hemispherical-emissivity-1}
+
+Long-wave emissivity \(\varepsilon\) of the screen material itself (not the effective value for the overall screen ``assembly'' including open spaces between the screen material). The emissivity is assumed to be the same for both sides of the screen.
+
+For most non-metallic materials, \(\varepsilon\) is about 0.9. For metallic materials, \(\varepsilon\) is dependent on material, its surface condition, and temperature. Typical values for metallic materials range from 0.05 -- 0.1 with lower values representing a more finished surface (e.g.~low oxidation, polished surface). Material emissivities may be found in Table~\ref{table:atmospheric-variables-at-two-different} from the 2005 ASHRAE Handbook of Fundamentals, page 3.9. The value for this input field must be between 0 and 1, with a default value of 0.9 if this field is left blank.
+
+\paragraph{Field: Conductivity}\label{field-conductivity-5}
+
+Screen material conductivity (W/m-K). This input value must be greater than 0. The default value is 221 W/m-K (aluminum).
+
+\paragraph{Field: Screen Material Spacing}\label{field-screen-material-spacing}
+
+The spacing, S, of the screen material (m) is the distance from the center of one strand of screen to the center of the adjacent one. The spacing of the screen material is assumed to be the same in both directions (e.g., vertical and horizontal). This input value must be greater than the non-zero screen material diameter. If the spacing is different in the two directions, use the average of the two values.
+
+\begin{figure}[hbtp] % fig 20
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image044.png}
+\caption{Screen Material Spacing and Diameter \protect \label{fig:screen-material-spacing-and-diameter}}
+\end{figure}
+
+\paragraph{Field: Screen Material Diameter}\label{field-screen-material-diameter}
+
+The diameter, D, of individual strands or wires of the screen material (m). The screen material diameter is assumed to be the same in both directions (e.g., vertical and horizontal). This input value must be greater than 0 and less than the screen material spacing. If the diameter is different in the two directions, use the average of the two values.
+
+\paragraph{Field: Screen to Glass Distance}\label{field-screen-to-glass-distance}
+
+Distance from the window screen to the adjacent glass surface (m). If the screen is not flat, the average screen to glass distance should be used. The screen-to-glass distance is used in calculating the natural convective air flow between the glass and the screen produced by buoyancy effects. This input value must be from 0.001 m to 1 m, with a default value of 0.025 m if this field is left blank.
+
+\paragraph{Field: Top Opening Multiplier}\label{field-top-opening-multiplier-2}
+
+Effective area for air flow at the top of the screen divided by the horizontal area between the glass and screen (see the same field for the Material:WindowShade object for additional description). The opening multiplier fields can be used to simulate a shading material that is offset from the window frame. Since window screens are typically installed against the window frame, the default value is equal to 0.This input value can range from 0 to 1.
+
+\paragraph{Field: Bottom Opening Multiplier}\label{field-bottom-opening-multiplier-2}
+
+Effective area for air flow at the bottom of the screen divided the horizontal area between the glass and screen (see the same field for the Material:WindowShade object for additional description). The opening multiplier fields can be used to simulate a shading material that is offset from the window frame. Since window screens are typically installed against the window frame, the default value is equal to 0. This input value can range from 0 to 1.
+
+\paragraph{Field: Left-Side Opening Multiplier}\label{field-left-side-opening-multiplier-2}
+
+Effective area for air flow at the left side of the screen divided the vertical area between the glass and screen (see the same field for the Material:WindowShade object for additional description). The opening multiplier fields can be used to simulate a shading material that is offset from the window frame. Since window screens are typically installed against the window frame, the default value is equal to 0. This input value can range from 0 to 1.
+
+\paragraph{Field: Right-Side Opening Multiplier}\label{field-right-side-opening-multiplier-2}
+
+Effective area for air flow at the right side of the screen divided the vertical area between the glass and screen (see the same field for the Material:WindowShade object for additional description). The opening multiplier fields can be used to simulate a shading material that is offset from the window frame. Since window screens are typically installed against the window frame, the default value is equal to 0. This input value can range from 0 to 1.
+
+\paragraph{Field: Angle of Resolution for Screen Transmittance Output Map}\label{field-angle-of-resolution-for-screen-transmittance-output-map}
+
+Angle of resolution, in degrees, for the overall screen beam transmittance (direct and reflected) output map. The comma-separated variable file eplusscreen.csv (Ref. OutputDetailsandExamples.pdf) will contain the direct beam and reflected beam solar radiation that is transmitted through the window screen as a function of incident sun angle (0 to 90 degrees relative solar azimuth and 0 to 90 degrees relative solar altitude) in sun angle increments specified by this input field. The default value is 0, which means no transmittance map is generated. Other valid choice inputs are 1, 2, 3 and 5 degrees.
+
+An IDF example for this object, along with Construction and WindowProperty:ShadingControl objects, is shown below:
+
+\begin{lstlisting}
+
+WindowMaterial:Screen,
+      EXTERIOR SCREEN,         !- Name
+      ModelAsDiffuse,        !- Reflected Beam Transmittance Accounting Method
+      0.6,                     !- Diffuse Solar Reflectance
+      0.6,                     !- Diffuse Visible Reflectance
+      0.9,                     !- Thermal Hemispherical Emissivity
+      221.0,                   !- Conductivity {W/m-K}
+      0.00154,                 !- Screen Material Spacing (m)
+      0.000254,                !- Screen Material Diameter (m)
+      0.025,                   !- Screen-to-Glass Distance {m}
+      0.0,                     !- Top Opening Multiplier
+      0.0,                     !- Bottom Opening Multiplier
+      0.0,                     !- Left-Side Opening Multiplier
+      0.0,                     !- Right-Side Opening Multiplier
+      0;                   !- Angle of Resolution for Output Map {deg}
+
+  Construction,
+      DOUBLE PANE WITHOUT SCREEN,     !- Name
+      GLASS - CLEAR SHEET 1 / 8 IN,   !- Outside Layer
+      WinAirB1 - AIRSPACE RESISTANCE, !- Layer \#2
+      GLASS - CLEAR SHEET 1 / 8 IN;   !- Layer \#3
+
+  WindowProperty:ShadingControl,
+      DOUBLE PANE WITH SCREEN, !- User Supplied Shading Control Name
+      ExteriorScreen,          !- Shading Type
+      ,                        !- Name of construction with shading
+      AlwaysOn,                !- Shading Control Type
+      ScreenSchedule,          !- Schedule Name
+      20.0,                    !- SetPoint {W/m2, W or deg C}
+      YES,                     !- Shading Control Is Scheduled
+      NO,                      !- Glare Control Is Active
+      EXTERIOR SCREEN,         !- Material Name of Shading Device
+      ,                        !- Type of Slat Angle Control for Blinds
+      ;                        !- Slat Angle Schedule Name
+\end{lstlisting}
+
+\subsection{WindowMaterial:Shade:EquivalentLayer}\label{windowmaterialshadeequivalentlayer}
+
+This object specifies the properties of Equivalent Layer window shade (roller blind) materials. Shades are considered to be thin, flat and perfect diffusers (all transmitted and reflected radiation is hemispherically-diffuse). However, shades can have beam-beam transmittance by virtue of their material openness.~ The beam-beam transmittnec is assumed to be the same for both sides of the shade and is the same as the openness area fraction. Beam-dffuse transmittance and reflectance, and emissivity properties can be different for front and back side of the shade.Window shades can be placed on the inside of the window, on the outside of the window, or between glass layers. WindowMaterial:Shade:EquivalentLayer is used for roller blinds. The off-normal solar property calculation of shades (roller blind) is based on a set of correlations developed from measurement of samples of commercially produced roller blind material with openness fraction less than 0.14. The model is not intended for materials with unusually high values of openness and should be limited to a mximum openness fraction of 0.20. The visible spectrum solar properties input fields are not used currently hence can be left blank.
+
+\subsubsection{Inputs}\label{inputs-26-002}
+
+\paragraph{Field: Name}\label{field-name-20-003}
+
+Name of the shade. It is referenced as an inside, inbetween or outside layer in an equivalent layer~ window construction.
+
+\paragraph{Field: Shade Beam-Beam Solar Transmittance}\label{field-shade-beam-beam-solar-transmittance}
+
+This value is the beam-beam transmittance of the shade at normal incidence and it is the same as the openness area fraction of the shade material. Assumed to be the same for front and back sides of the roller blinds.~ The minimum value is 0.0 and maximum value is less than 1.0.~ The default value is 0.0. For most common shade materials (e.g.~Roller Blinds) the material oppeness fraction doesn't exceed 0.20.
+
+\paragraph{Field: Front Side Shade Beam-Diffuse Solar Transmittance}\label{field-front-side-shade-beam-diffuse-solar-transmittance}
+
+This value is the front side beam-diffuse transmittance of the shade material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.~ The default value is 0.0.
+
+\paragraph{Field: Back Side Shade Beam-Diffuse Solar Transmittance}\label{field-back-side-shade-beam-diffuse-solar-transmittance}
+
+This value is the back side beam-diffuse transmittance of the shade material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.~ The default value is 0.0.
+
+\paragraph{Field: Front Side Shade Beam-Diffuse Solar Reflectance}\label{field-front-side-shade-beam-diffuse-solar-reflectance}
+
+This value is the front side beam-diffuse reflectance of the shade material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
+
+\paragraph{Field: Back Side Shade Beam-Diffuse Solar Reflectance}\label{field-back-side-shade-beam-diffuse-solar-reflectance}
+
+This value is the back side beam-diffuse reflectance of the shade material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
+
+\paragraph{Field: Shade Beam-Beam Visible Transmittance}\label{field-shade-beam-beam-visible-transmittance}
+
+This value is the beam-beam transmittance at normal incidence averaged over the visible spectrum of solar radiation. Assumed to be the same for front and back sides. The minimum value is 0.0 and maximum value is less than 1.0.~ Currently this input field is not used.
+
+\paragraph{Field: Shade Beam-Diffuse Visible Transmittance}\label{field-shade-beam-diffuse-visible-transmittance}
+
+This value is the beam-diffuse transmittance at normal incidence averaged over the visible spectrum of solar radiation. Assumed to be the same for front and back sides. The minimum value is 0.0 and maximum value is less than 1.0.~ Currently this input field is not used.
+
+\paragraph{Field: Shade Beam-Diffuse Visible Reflectance}\label{field-shade-beam-diffuse-visible-reflectance}
+
+This value is the beam-diffuse reflectance at normal incidence averaged over the visible spectrum of solar radiation. Assumed to be the same for front and back sides. The minimum value is 0.0 and maximum value is less than 1.0.~ Currently this input field is not used.
+
+\paragraph{Field: Shade Material Infrared Transmittance}\label{field-shade-material-infrared-transmittance}
+
+This value is the long-wave transmittance of the shade material and assumed to be the same for front and back sides of the shade. The minimum value is 0.0 and maximum value is less than 1.0. Default value is 0.05.
+
+\paragraph{Field: Front Side Shade Material Infrared Emissivity}\label{field-front-side-shade-material-infrared-emissivity}
+
+This value is the front side long-wave hemispherical emissivity of shade material. The minimum value is 0.0 and maximum value is less than 1.0. Default value is 0.91. The front side effective emissivity of the shade layer is calculated using this value and the material openness specified above.
+
+\paragraph{Field: Back Side Shade Material Infrared Emissivity}\label{field-back-side-shade-material-infrared-emissivity}
+
+This value is the back side long-wave hemispherical emissivity of shade material. The minimum value is 0.0 and maximum value is less than 1.0. Default value is 0.91. The back side effective emissivity of the shade is calculated using this value and the material openness specified above.
+
+An IDF example for this object is shown below:
+
+\begin{lstlisting}
+
+WindowMaterial:Shade:EquivalentLayer,
+    Shade1,        !- Name
+    0.190,         !- Shade Beam-Beam Solar Transmittance
+    0.206,         !- Front Side Shade Beam-Diffuse Solar Transmittance
+    0.206,         !- Back Side Shade Beam-Diffuse Solar Transmittance
+    0.499,         !- Front Side Shade Beam-Diffuse Solar Reflectance
+    0.499,         !- Back Side Shade Beam-Diffuse Solar Reflectance
+    0.0,           !- Shade Beam-Beam Visible Transmittance
+    0.0,           !- Shade Beam-Diffuse Vissible Transmittance
+    0.0,           !- Shade Vissible Reflectance
+    0.0,           !- Shade Material Infrared Transmittance
+    0.84,          !- Front Side Shade Material Infrared Emissivity
+    0.84;          !- Back Side Shade Material Infrared Emissivity
+\end{lstlisting}
+
+\subsection{WindowMaterial:Drape:EquivalentLayer}\label{windowmaterialdrapeequivalentlayer}
+
+Specifies the optical and thermal properties of equivalent layer window drape fabric materials.
+
+Drapery fabric shades are commonly placed on the the inside of the window. The long-wave (infrared) properties for commonly used drapery fabrics are assumed to be the same on both sides but different values can be specified when required. Drape fabric shade layers are considered to be perfect diffusers (reflected radiation is hemispherically-diffuse independent of angle of incidence). Unpleated drape fabric is treated as thin and flat layer.The off-normal optical properties of drapery fabric is determined from user specified optical properties at normal incidence using empirical correlations. Pleated drape fabric requires entering the pleated section average width and length as showsn in Figure~\ref{fig:geometry-used-for-pleated-drape-analysis}.For pleated drapes the effective beam-beam and beam-diffuse solar properties are determined by tracking both radiation components, for a given incident angle solar radiation, through various interactions with a fabric pleated in a rectangular geometry shown in Figure~\ref{fig:geometry-used-for-pleated-drape-analysis}.~ The solar properties of the two different pleat facets are evaluated on the basis of the local solar incidence angle.~ Therefore, the effective layer properties are influenced not just by horizontal solar profile angle, but also by incidence angle. The correlations used for drape fabrics optical property calculations reqiure that the solar absorptance of the fabric, at normal incidence, is not less than 1\%.
+
+\begin{figure}[hbtp] % fig 21
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image045.png}
+\caption{Geometry used for Pleated Drape Analysis \protect \label{fig:geometry-used-for-pleated-drape-analysis}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-27-002}
+
+\paragraph{Field: Name}\label{field-name-21-003}
+
+Name of the drape fabric shade layer. It is referenced as an inside, in between or outside layer in an equivalent layer window construction.
+
+\paragraph{Field: Drape Beam-Beam Solar Transmittance}\label{field-drape-beam-beam-solar-transmittance}
+
+This value is the drape fabric beam-beam transmittance at normal incidence, and it is the same as the drape fabric openness area fraction.~ Assumed to be the same for front and back sides of the drape fabric layer.~ The minimum value is 0.0 and maximum value is less than 1.0. For most drape fabric materials the maximum frabric openness fraction do not exceed 0.2.~ The default value is 0.0.
+
+\paragraph{Field: Front Side Drape Beam-Diffuse Solar Transmittance}\label{field-front-side-drape-beam-diffuse-solar-transmittance}
+
+This value is the front side beam-diffuse solar transmittance of the drape fabric material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
+
+\paragraph{Field: Back Side Drape Beam-Diffuse Solar Transmittance}\label{field-back-side-drape-beam-diffuse-solar-transmittance}
+
+This value is the back side beam-diffuse solar transmittance of the drape fabric material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
+
+\paragraph{Field: Front Side Drape Beam-Diffuse Solar Reflectance}\label{field-front-side-drape-beam-diffuse-solar-reflectance}
+
+This value is the front side beam-diffuse solar reflectance of the drape fabric material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
+
+\paragraph{Field: Back Side Drape Beam-Diffuse Solar Reflectance}\label{field-back-side-drape-beam-diffuse-solar-reflectance}
+
+This value is the back side beam-diffuse solar reflectance of the drape fabric material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
+
+\paragraph{Field: Drape Beam-Beam Visible Transmittance}\label{field-drape-beam-beam-visible-transmittance}
+
+This value is the drape fabric beam-beam visible transmittance at normal incidence averaged over the visible spectrum range of solar radiation.~ Assumed to be the same for front and back sides of the drape fabric layer.~ The minimum value is 0.0 and maximum value is less than 1.0.~ The default value is 0.0.~ This input field is not used currently.
+
+\paragraph{Field: Front Side Drape Beam-Diffuse Visible Reflectance}\label{field-front-side-drape-beam-diffuse-visible-reflectance}
+
+This value is the front side drape fabric beam-diffuse visible reflectance at normal incidence averaged over the visible spectrum range of solar radiation.~ Assumed to be the same for front and back sides of the drape.~ The minimum value is 0.0 and maximum value is less than 1.0.~ The default value is 0.0.~ This input field is not used currently.
+
+\paragraph{Field: Back Side Drape Diffuse-Diffuse Visible Reflectance}\label{field-back-side-drape-diffuse-diffuse-visible-reflectance}
+
+This value is the back side drape fabric diffuse-diffuse visible reflectance at normal incidence averaged over the visible spectrum range of solar radiation.~ Assumed to be the same for front and back sides of the drape.~ The minimum value is 0.0 and maximum value is less than 1.0.~ The default value is 0.0.~ This input field is not used currently.
+
+\paragraph{Field: Drape Material Infrared Transmittance}\label{field-drape-material-infrared-transmittance}
+
+This value is the long-wave hemispherical transmittance of the fabric material at zero fabric openness fraction.~ Assumed to be the same for front and back sides of the drape fabric material layer. The minimum value is 0.0 and maximum value is less than 1.0.~ The default value is 0.05.
+
+\paragraph{Field: Front Side Drape Material Infrared Emissivity}\label{field-front-side-drape-material-infrared-emissivity}
+
+This value is the front side long-wave hemispherical emissivity of fabric material at zero shade opennes. The minimum value is 0.0 and maximum value is less than 1.0. the default value is 0.87. The front side effective emissivity of the drape fabric layer is calculated using this value and the fabric openness area fraction specified above.
+
+\paragraph{Field: Back Side Drape Material Infrared Emissivity}\label{field-back-side-drape-material-infrared-emissivity}
+
+This value is the back side long-wave hemispherical emissivity of fabric material at zero fabric openness fraction. The minimum value is 0.0 and maximum value is less than 1.0. The default value is 0.87. The back side effective emissivity of the drape fabric layer is calculated using this value and the fabric openness area fraction specified above.
+
+\paragraph{Field: Width of Pleated Fabric}\label{field-width-of-pleated-fabric}
+
+This value is the width of the pleated section of the draped fabric, w(m). If the drape fabric is flat (unpleated), then the pleated section width is set to zero. The default value is 0.0, i.e., assumes flat drape fabric.
+
+\paragraph{Field: Length of Pleated Fabric}\label{field-length-of-pleated-fabric}
+
+This value is the length of the pleated section of the draped fabric, s(m). If the drape fabric is flat (unpleated), then the pleated section length is set to zero.~ The default value is 0.0, i.e., assumes flat drape fabric.
+
+An IDF example for this object is shown below:
+
+\begin{lstlisting}
+WindowMaterial:Drape:EquivalentLayer,
+  Drape02,            !- Name
+  0.14,               !- Shade Beam-Beam Solar Transmittance
+  0.10,               !- Front Side Shade Beam-Diffuse Solar Transmittance
+  0.10,               !- Back Side Shade Beam-Diffuse Solar Transmittance
+  0.40,               !- Front Side Shade Beam-Diffuse Solar Reflectance
+  0.50,               !- Back Side Shade Beam-Diffuse Solar Reflectance
+  0.0,                !- Shade Beam-Beam Visible Transmittance
+  0.0,                !- Shade Beam-Diffuse Visible Transmittance
+  0.0,                !- Shade Beam-Diffuse Visible Reflectance
+  0.10,               !- Shade Material Infrared Transmittance
+  0.90,               !- Front Side Shade Material Infrared Emissivity
+  0.80,               !- Back Side Shade Material Infrared Emissivity
+  0.01,               !- Width of Pleated Fabric
+  0.025;              !- Length of Pleated Fabric
+\end{lstlisting}
+
+\subsection{WindowMaterial:Blind:EquivalentLayer}\label{windowmaterialblindequivalentlayer}
+
+This object specifies the properties of an Equivalent Layer window blind consisting of thin and equally-spaced slats. The the model assumes that slats are flat and thin, and applies correction for the slat curvature effect based on the user specified slat crwon. Slats are assumed to transmit and reflect diffusely.The effective shortwave optical and longwave optical properties of venetian blind layer is estimated analytically. The Equivalent Layer blind model requires optical properties and geometry of the slats shown in Figure~\ref{fig:geometry-and-properties-used-for-venetian}. Likewise, effective longwave properties are obtained for the layer knowing longwave properties of the slats.
+
+\begin{figure}[hbtp] % fig 22
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image047.png}
+\caption{Geometry and Properties used for venetian blind analysis \protect \label{fig:geometry-and-properties-used-for-venetian}}
+\end{figure}
+
+The input data required to characterize a venetian blind are: front and back side reflectance and transmittance of the slat, geometry (Slat width, w, slat spacing, s, slat crown, c, and slat angle, f, and long wave emittance and transmittance of the slat. Blinds can be located on the inside of the window, on the outside of the window, or between two layers of glass. The blind is assumed to cover all of the glazed part of the window.
+
+\subsubsection{Inputs}\label{inputs-28-001}
+
+\paragraph{Field: Name}\label{field-name-22-003}
+
+Name of the venetian blind. It is referenced as an inside, outside or in between layers in an equivalent layer window construction.
+
+\paragraph{Field: Slat Orientation}\label{field-slat-orientation-1}
+
+The choices are Horizontal and Vertical. ``Horizontal'' means the slats are parallel to the bottom of the window; this is the same as saying that the slats are parallel to the X-axis of the window. ``Vertical'' means the slats are parallel to Y-axis of the window. The default is ``Horizontal''.
+
+\paragraph{Field: Slat Width}\label{field-slat-width-2}
+
+This value is the width of the slat measured from edge to edge (m). The default value is 0.0254.
+
+\paragraph{Field: Slat Separation}\label{field-slat-separation-1}
+
+The distance between the front of a slat and the back of the adjacent slat (m). The default value is 0.025. The slat separation should not be greater than the slat width.
+
+\paragraph{Field: Slat Crown}\label{field-slat-crown}
+
+The perpendicular length between the slat cord ~and the curve (m). Crown = 0.0625x``Slat width''. Slat is assumed to be rectangular in cross section and flat. The crown accounts for curvature of the slat.~ The minimum value is 0.0, and the default value is 0.0015m.
+
+\paragraph{Field: Slat Angle}\label{field-slat-angle-2}
+
+The angle (degrees) between the glazing outward normal and the slat outward normal, where the outward normal points away from the front face of the slat (degrees). If the ``Slat Angle Control'' input field below specified is ``FixedSlatAngle'', then the slat angle is fixed at ``Slat Angle'' value entered.~ Minimum value is zero, and the maximum value allowed is 180.0 degrees.~ The default value is 45 degrees.
+
+\paragraph{Field: Front Side Slat Beam-Diffuse Solar Transmittance}\label{field-front-side-slat-beam-diffuse-solar-transmittance}
+
+This value is the slat front side beam-diffuse solar transmittance at normal incidence averaged over the entire spectrum of solar radiation. Any transmitted beam radiation is assumed to be 100\% diffuse (i.e., slats are translucent). Minimum value is 0.0, and the maximum value is less than 1.0. The default value is 0.0.
+
+\paragraph{Field: Back Side Slat Beam-Diffuse Solar Transmittance}\label{field-back-side-slat-beam-diffuse-solar-transmittance}
+
+This value is the slat back side beam-diffuse solar transmittance at normal incidence averaged over the entire spectrum of solar radiation. Any transmitted beam radiation is assumed to be 100\% diffuse (i.e., slats are translucent). Minimum value is 0.0,~ and the maximum value is less than 1.0. The default value is 0.0.
+
+\paragraph{Field: Front Side Slat Beam-Diffuse Solar Reflectance}\label{field-front-side-slat-beam-diffuse-solar-reflectance}
+
+This value is slat front side beam-diffuse solar reflectance at normal incidence averaged over the entire spectrum of solar radiation. All the reflected component is assumed to be diffuse. Minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Back Side Slat Beam-Diffuse Solar Reflectance}\label{field-back-side-slat-beam-diffuse-solar-reflectance}
+
+This value is the slat back side beam-diffuse solar reflectance at normal incidence averaged over the entire spectrum of solar radiation. All the reflected component is assumed to be diffuse. Minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Front Side Slat Beam-Diffuse Visible Solar Transmittance}\label{field-front-side-slat-beam-diffuse-visible-solar-transmittance}
+
+This value is the slat front side beam-diffuse visible transmittance at normal incidence averaged over the visible spectrum range of solar radiation. Any transmitted beam radiation is assumed to be 100\% diffuse (i.e., slats are translucent). Minimum value is 0.0, and the maximum value is less than 1.0. The default value is 0.0.
+
+\paragraph{Field: Back Side Slat Beam-Diffuse Visible Solar Transmittance}\label{field-back-side-slat-beam-diffuse-visible-solar-transmittance}
+
+This value is the slat back side beam-diffuse visible transmittance at normal incidence averaged the visible spectrum range of solar radiation. Any transmitted beam radiation is assumed to be 100\% diffuse (i.e., slats are translucent). Minimum value is 0.0, and the maximum value is less than 1.0. The default value is 0.0.
+
+\paragraph{Field: Front Side Slat Beam-Diffuse Visible Solar Reflectance}\label{field-front-side-slat-beam-diffuse-visible-solar-reflectance}
+
+This value is the slat front side beam-diffuse visible reflectance at normal incidence averaged over the visible spectrum range of solar radiation. All the reflected component is assumed to be diffuse. Minimum value is 0.0, and the maximum value is less than 1.0
+
+\paragraph{Field: Back Side Slat Beam-Diffuse Visible Solar Reflectance}\label{field-back-side-slat-beam-diffuse-visible-solar-reflectance}
+
+This value is the slat back side beam-diffuse visible reflectance at normal incidence averaged over the visible spectrum range of solar radiation. All the reflected component is assumed to be diffuse. Minimum value is 0.0,~ and the maximum value is less than 1.0
+
+\paragraph{Field: Slat Diffuse-Diffuse Solar Transmittance}\label{field-slat-diffuse-diffuse-solar-transmittance}
+
+This value is the slat diffuse-diffuse solar transmittance for hemispherically diffuse solar radiation. This value is the same for front and back side of the slat.~ Minimum value is 0.0,~ and the maximum value is less than 1.0.
+
+\paragraph{Field: Front Side Slat Diffuse-Diffuse Solar Reflectance}\label{field-front-side-slat-diffuse-diffuse-solar-reflectance}
+
+This value is the slat front side diffuse-diffuse solar reflectance for hemispherically diffuse solar radiation. Minimum value is 0.0,~ and the maximum value is less than 1.0.
+
+\paragraph{Field: Back Side Slat Diffuse-Diffuse Solar Reflectance}\label{field-back-side-slat-diffuse-diffuse-solar-reflectance}
+
+This value is the slat back side diffuse-diffuse solar reflectance for hemispherically diffuse solar radiation. Minimum value is 0.0,~ and the maximum value is less than 1.0.
+
+\paragraph{Field: Slat Diffuse-Diffuse Visible Transmittance}\label{field-slat-diffuse-diffuse-visible-transmittance}
+
+This value is the slat diffuse-diffuse visible transmittance for hemispherically diffuse visible spectrum range of solar radiation. This value is the same for front and back side of the slat.~ Minimum value is 0.0,~ and the maximumvalue is less than 1.0. This input field is not used currently.
+
+\paragraph{Field: Front Side Slat Diffuse-Diffuse Visible Reflectance}\label{field-front-side-slat-diffuse-diffuse-visible-reflectance}
+
+This value is the slat front side diffuse-diffuse visible reflectance for hemispherically diffuse visible spectrum range of solar radiation. Minimum value is 0.0, and the maximum value is less than 1.0.~ This input field is not used currently.
+
+\paragraph{Field: Back Side Slat Diffuse-Diffuse Visible Reflectance}\label{field-back-side-slat-diffuse-diffuse-visible-reflectance}
+
+This value is the slat back side diffuse-diffuse visible reflectance for hemispherically diffuse visible spectrum range of solar radiation. Minimum value is 0.0, and the maximum value is less than 1.0.~ This input field is not used currently.
+
+\paragraph{Field: Slat Infrared Transmittance}\label{field-slat-infrared-transmittance}
+
+This value is the long-wave hemispherical transmittance of the slat material. Assumed to be the same for both sides of the slat. The minimum value is 0.0, the maximum value is less than 1.0.~ The default value is 0.0.
+
+\paragraph{Field: Front Side Slat Infrared Emissivity}\label{field-front-side-slat-infrared-emissivity}
+
+This value is the front side long-wave hemispherical emissivity of the slat material. The minimum value is 0.0, the maximum value is less than 1.0. The default value is 0.9.
+
+\paragraph{Field: Back Side Slat Infrared Emissivity}\label{field-back-side-slat-infrared-emissivity}
+
+This value is the back side long-wave hemispherical emissivity of the slat material. The minimum value is 0.0, the maximum value is less than 1.0.~ The default value is 0.9.
+
+\paragraph{Field: Slat Angle Control}\label{field-slat-angle-control}
+
+This input field is used only if slat angle control is desired.~ The three key choice inputsallowed are ``FixedSlatAngle'', ``MaximizeSolar'', and ``BlockBeamSolar''.~ The default value is ``FixedSlatAngle''.If Type of Slat Angle Control for Blinds = MaximizeSolar the slat angle is adjusted to maximize solar gain.~If Type of Slat Angle Control for Blinds = BlockBeamSolar, the slat angle is adjusted to maximize visibiity while eliminating beam solar radiation.~If Type of Slat Angle Control for Blinds = FixedSlatAngle, then the model uses a fixed slat angle specified above.
+
+An IDF example for this object, is shown below:
+
+\begin{lstlisting}
+
+WindowMaterial:Blind:EquivalentLayer,
+    VBU8D6+45SW1,      ! - Name
+    Horizontal,        ! - Slat Orientation
+    0.025,             ! - Slat Width
+    0.025,             ! - Slat Separation
+    0.0,               ! - Slat Crown
+    45.0,              ! - Slat Angle
+    0.0,               ! - Front Side Slat Beam-Diffuse Solar Transmittance
+    0.0,               ! - Back Side Slat Beam-Diffuse Solar Transmittance
+    0.0,               ! - Front Side Slat Beam-Diffuse Solar Reflectance
+    0.0,               ! - Back Side Slat Beam-Diffuse Solar Reflectance
+    0.0,               ! - Front Side Slat Beam-Diffuse Visible Transmittance
+    0.0,               ! - Back Side Slat Beam-Diffuse Visible Transmittance
+    0.0,               ! - Front Side Slat Beam-Diffuse Visible Reflectance
+    0.0,               ! - Back Side Slat Beam-Diffuse Visible  Reflectance
+    0.0,               ! - Slat Diffuse-Diffuse Solar Transmittance
+    0.80,              ! - Front Side Slat Diffuse-Diffuse Solar Reflectance
+    0.60,              ! - Back Side Slat Diffuse-Diffuse Solar Reflectance
+    0.0,               ! - Slat Diffuse-Diffuse Visible Transmittance
+    0.0,               ! - Front Side Slat Diffuse-Diffuse Visible Reflectance
+    0.0,               ! - Back Side Slat Diffuse-Diffuse Visible Reflectance
+    0.0,               ! - Slat Infrared Transmittance
+    0.90,              ! - Front Side Slat Infrared Emissivity
+    0.90,              ! - Back Side Slat Infrared Emissivity
+    FixedSlatAngle;    ! - Slat Angle Control
+\end{lstlisting}
+
+\subsection{WindowMaterial:Screen:EquivalentLayer}\label{windowmaterialscreenequivalentlayer}
+
+This object specifies the optical and thermal properties of exterior screen materials for Equivalent Layer Window. Can only be placed on the exterior side of window construction. The window screen model assumes the screen is made up of intersecting orthogonally-crossed cylinders. The surface of the cylinders is assumed to be diffusely reflecting. The beam solar radiation transmitted through an equivalent Layer window screen varies with sun angle and is made up of two distinct elements: a beam-beam component and a beam-difuse component. The beam-beam transmittance component is calculated using screen openness area fraction determined from the geometry of the screen and the incident angle of the sun. Empirical correlations are used to obtain the effective off-normal solar and longwave properties of insect screens.~ Insect screen geometry is shown in Figure~\ref{fig:geometry-used-for-insect-screen-analysis}.~ The calculation of effective solar properties requires a set of properties measured at normal incidence.
+
+\begin{figure}[hbtp] % fig 23
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image048.png}
+\caption{Geometry used for insect screen analysis \protect \label{fig:geometry-used-for-insect-screen-analysis}}
+\end{figure}
+
+The formulation of the model, assumption and correlations used to calculate effective solar and longwave properties of insect screens are described in the Engineering Reference.
+
+\subsubsection{Inputs}\label{inputs-29-001}
+
+\paragraph{Field: Name}\label{field-name-23-003}
+
+Name of the insect screen. It is referenced as an outside layer in an equivalent layer window construction.
+
+\paragraph{Field: Screen Beam-Beam Solar Transmittance}\label{field-screen-beam-beam-solar-transmittance}
+
+This value is the beam-beam transmittance of the screen material at normal incidence. This value is the same as the screen oppenness area fraction.~ This value can be autocalculated from the wire spacing and wire diameter. It is the same for both sides of the screen. The minimum value is 0.0, and maximum value is less than 1.0.
+
+\paragraph{Field: Screen Beam-Diffuse Solar Transmittance}\label{field-screen-beam-diffuse-solar-transmittance}
+
+This value is the beam-diffuse solar transmittance of the screen material at normal incidence averaged over the entire spectrum of solar radiation. Assumed to be the same for both sides of the screen. The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Screen Beam-Diffuse Solar Reflectance}\label{field-screen-beam-diffuse-solar-reflectance}
+
+This value is the beam-diffuse solar reflectance of the screen material at normal incidence averaged over the entire spectrum of solar radiation. Assumed to be the same for both sides of the screen. The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Screen Beam-Beam Visible Transmittance}\label{field-screen-beam-beam-visible-transmittance}
+
+This value is the beam-beam visible transmittance of the screen material at normal incidence averaged over the visible spectrum range of solar radiation.~ Assumed to be the same for both sides of the screen. The minimum value is 0.0, and maximum value is less than 1.0. This input input field is not used currently.
+
+\paragraph{Field: Screen Beam-Diffuse Visible Transmittance}\label{field-screen-beam-diffuse-visible-transmittance}
+
+This value is the beam-diffuse visible reflectance of the screen material at normal incidence averaged over the visible spectrum range of solar radiation. Assumed to be the same for both sides of the screen. The minimum value is 0.0, and the maximum value is less than 1.0. This input input field is not used currently.
+
+\paragraph{Field: Screen Beam-Diffuse Visible Reflectance}\label{field-screen-beam-diffuse-visible-reflectance}
+
+This value is the beam-diffuse visible reflectance of the screen material at normal incidence averaged over the visible spectrum range of solar radiation. Assumed to be the same for both sides of the screen. The minimum value is 0.0, and the maximum value is less than 1.0. This input input field is not used currently.
+
+\paragraph{Field: Screen Infrared Transmittance}\label{field-screen-infrared-transmittance}
+
+This value is the long-wave hemispherical transmittance of the the screen material. Assumed to be the same for both sides of the screen material. The minimum value is 0.0, the maximum value is less than 1.0.~ The default value is 0.02
+
+\paragraph{Field: Screen Infrared Emissivity}\label{field-screen-infrared-emissivity}
+
+This value is the long-wave hemispherical emissivity of the screen material. Assumed to be the same for both sides of the screen material. The minimum value is 0.0, the maximum value is less than 1.0. The default value is 0.93.
+
+\paragraph{Field: Screen Wire Spacing}\label{field-screen-wire-spacing}
+
+The spacing, S (m), of the screen material is the distance from the center of one strand of screen to the center of the adjacent one. The spacing of the screen material is assumed to be the same in both directions (e.g., vertical and horizontal). This input value must be greater than the non-zero screen material diameter. If the spacing is different in the two directions, use the average of the two values. Default value is 0.0025m.
+
+\paragraph{Field: Screen Wire Diameter}\label{field-screen-wire-diameter}
+
+The diameter, D (m), of individual strands or wires of the screen material. The screen material diameter is assumed to be the same in both directions (e.g., vertical and horizontal). This input value must be greater than 0 and less than the screen wire spacing. If the diameter is different in the two directions, use the average of the two values. Default value is 0.005m.
+
+An IDF example for this object, is shown below:
+
+\begin{lstlisting}
+
+WindowMaterial:Screen:EquivalentLayer,
+    INSCRN,                !- Name
+    0.763,                 !- Screen Beam-Beam Solar Transmittance
+    0.052,                 !- Screen Beam-Diffuse Solar Transmittance
+    0.076,                 !- Screen Beam-Diffuse Solar Reflectance
+    0.0,                   !- Screen Beam-Beam Visible Transmittance
+    0.0,                   !- Screen Beam-Diffuse Visible Transmittance
+    0.0,                   !- Screen Beam-Diffuse Visible Reflectance
+    0.0,                   !- Screen Infrared Transmittance
+    0.84,                  !- Screen Infrared Emissivity
+    0.025,                 !- Screen Wire Spacing
+    0.005;                 !- Screen Wire Diameter
+\end{lstlisting}
+
+\subsection{WindowMaterial:Glazing:EquivalentLayer}\label{windowmaterialglazingequivalentlayer}
+
+Glass material properties for equivalent layer window model.~ Uses transmittance/reflectance input method.~ For exterior windows, ``front side'' is the side of the glass closest to the outside air and ``back side'' is the side closest to the zone the window is defined in. For interzone windows, ``front side'' is the side closest to the zone adjacent to the zone the window is defined in and ``back side'' is the side closest to the zone the window is defined in.
+
+\subsubsection{Inputs}\label{inputs-30-001}
+
+\paragraph{Field: Name}\label{field-name-24-002}
+
+The name of the glass layer. It corresponds to a layer in an equivalent layer window construction.
+
+\paragraph{Field: Optical Data Type}\label{field-optical-data-type-1}
+
+Valid values for this field are SpectralAverage, or Spectral. If Optical Data Type = SpectralAverage, the values you enter for solar transmittance and reflectance are assumed to be averaged over the solar spectrum, and the values you enter for visible transmittance and reflectance are assumed to be averaged over the solar spectrum and weighted by the response of~ the human eye. The spectral data input is not supported now.
+
+\paragraph{Field: Window Glass Spectral Data Set Name}\label{field-window-glass-spectral-data-set-name-0}
+
+This input field is not used currently.
+
+\paragraph{Field: Front Side Beam-Beam Solar Transmittance}\label{field-front-side-beam-beam-solar-transmittance}
+
+This value is the front side beam-beam solar transmittance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Back Side Beam-Beam Solar Transmittance}\label{field-back-side-beam-beam-solar-transmittance}
+
+This value is the back side beam-beam solar transmittance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Front Side Beam-Beam Solar Reflectance}\label{field-front-side-beam-beam-solar-reflectance}
+
+This value is the front side beam-beam solar reflectance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Back Side Beam-Beam Solar Reflectance}\label{field-back-side-beam-beam-solar-reflectance}
+
+This value is the back side beam-beam solar reflectance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Front Side Beam-Beam Visible Transmittance}\label{field-front-side-beam-beam-visible-transmittance}
+
+This value is the front side beam-beam visible transmittance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Back Side Beam-Beam Visible Transmittance}\label{field-back-side-beam-beam-visible-transmittance}
+
+This value is the back side beam-beam visible transmittance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Front Side Beam-Beam Visible Reflectance}\label{field-front-side-beam-beam-visible-reflectance}
+
+This value is the front side beam-beam visible reflectance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Back Side Beam-Beam Visible Reflectance}\label{field-back-side-beam-beam-visible-reflectance}
+
+This value is the back side beam-beam visible reflectance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Front Side Beam-Diffuse Solar Transmittance}\label{field-front-side-beam-diffuse-solar-transmittance}
+
+This value is the front side beam-diffuse solar transmittance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ For clear glazing the beam-diffuse transmittance is zero. The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.
+
+\paragraph{Field: Back Side Beam-Diffuse Solar Transmittance}\label{field-back-side-beam-diffuse-solar-transmittance}
+
+This value is the back side beam-diffuse solar transmittance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ For clear glazing the beam-diffuse solar transmittance is zero. The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.
+
+\paragraph{Field: Front Side Beam-Diffuse Solar Reflectance}\label{field-front-side-beam-diffuse-solar-reflectance}
+
+This value is the front side beam-diffuse solar reflectance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.
+
+\paragraph{Field: Back Side Beam-Diffuse Solar Reflectance}\label{field-back-side-beam-diffuse-solar-reflectance}
+
+This value is the back side beam-diffuse solar reflectance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.
+
+\paragraph{Field: Front Side Beam-Diffuse Visible Transmittance}\label{field-front-side-beam-diffuse-visible-transmittance}
+
+This value is the front side beam-diffuse visible transmittance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ For clear glazing the beam-diffuse visible transmittance is zero. The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.~ This input field is not used currently.
+
+\paragraph{Field: Back Side Beam-Diffuse Visible Transmittance}\label{field-back-side-beam-diffuse-visible-transmittance}
+
+This value is the back side beam-diffuse visible transmittance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ For clear glazing the beam-diffuse visible transmittance is zero. The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.~ This input field is not used currently.
+
+\paragraph{Field: Front Side Beam-Diffuse Visible Reflectance}\label{field-front-side-beam-diffuse-visible-reflectance}
+
+This value is the front side beam-diffuse visible reflectance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0. This input field is not used currently.
+
+\paragraph{Field: Back Side Beam-Diffuse Visible Reflectance}\label{field-back-side-beam-diffuse-visible-reflectance}
+
+This value is the back side beam-diffuse visible reflectance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage.~ The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0. This input field is not used currently.
+
+\paragraph{Field: Diffuse-Diffuse Solar Transmittance}\label{field-diffuse-diffuse-solar-transmittance}
+
+This value is the diffuse-diffuse solar transmittance of the glazing averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage. The diffuse-diffuse transmittance is assumed to be the same for both sides of the glazing.~ EnergyPlus automatically estimates the diffuse-diffuse solar transmittance from other inputs. If this input field is specified as ``Autocalculate'', then the calculated transmittance will be used. The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Front Side Diffuse-Diffuse Solar Reflectance}\label{field-front-side-diffuse-diffuse-solar-reflectance}
+
+This value is the front side diffuse-diffuse solar reflectance of the glazing averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage. EnergyPlus automatically estimates the diffuse-diffuse reflectance from other inputs. If this input field is specified as ``Autocalculate'', then the calculated reflectance will be used. The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Back Side Diffuse-Diffuse Solar Reflectance}\label{field-back-side-diffuse-diffuse-solar-reflectance}
+
+This value is the back side diffuse-diffuse solar reflectance of the glazing averaged over the entire spectrum of solar radiation.~ Used only when Optical Data Type = SpectralAverage. EnergyPlus automatically estimates the diffuse-diffuse reflectance from other inputs. If this input field is specified as ``Autocalculate'', then the calculated reflectance will be used. The minimum value is 0.0, and the maximum value is less than 1.0.
+
+\paragraph{Field: Diffuse-Diffuse Visible Solar Transmittance}\label{field-diffuse-diffuse-visible-solar-transmittance}
+
+This value is the diffuse-diffuse visible transmittance of the glazing averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage. The diffuse-diffuse visible transmittance is assumed to be the same for both sides of the glazing.~ If this input field is specified as ``Autocalculate'', then the calculated transmittance will be used. The minimum value is 0.0, and the maximum value is less than 1.0. This input field is not used currently.
+
+\paragraph{Field: Front Side Diffuse-Diffuse Visible Reflectance}\label{field-front-side-diffuse-diffuse-visible-reflectance}
+
+This value is the front side diffuse-diffuse visible reflectance of the glazing averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage. EnergyPlus automatically estimates the front side diffuse-diffuse visible reflectance from front side beam-beam visible reflectance at normal incidence specified above. If this input field is specified as ``Autocalculate'', then the calculated reflectance will be used. The minimum value is 0.0, and the maximum value is less than 1.0. This input field is not used currently.
+
+\paragraph{Field: Back Side Diffuse-Diffuse Visible Reflectance}\label{field-back-side-diffuse-diffuse-visible-reflectance}
+
+This value is the back side diffuse-diffuse visible reflectance of the glazing averaged over the visible spectrum range of solar radiation.~ Used only when Optical Data Type = SpectralAverage. EnergyPlus automatically estimates the back side diffuse-diffuse visible reflectance from back side beam-beam visible reflectance at normal incidence specified above. If this input field is specified as ``Autocalculate'', then the calculated reflectance will be used. The minimum value is 0.0, and the maximum value is less than 1.0. This input field is not used currently.
+
+\paragraph{Field: Infrared Transmittance (applies to front and back)}\label{field-infrared-transmittance-applies-to-front-and-back}
+
+This value is the long-wave hemispherical transmittance of the glazing. Assumed to be the same for both sides of the glazing. The minimum value is 0.0, the maximum value is less than 1.0.~ The default value is 0.0.
+
+\paragraph{Field: Front Side Infrared Emissivity}\label{field-front-side-infrared-emissivity}
+
+This value is the front side long-wave hemispherical emissivity of the glazing. The minimum value is 0.0, the maximum value is less than 1.0.~ The default value is 0.84.
+
+\paragraph{Field: Back Side Infrared Emissivity}\label{field-back-side-infrared-emissivity}
+
+This value is the back side long-wave hemispherical emissivity of the glazing. The minimum value is 0.0, the maximum value is less than 1.0.~ The default value is 0.84.
+
+An IDF example for this object, is shown below:
+
+\begin{lstlisting}
+
+WindowMaterial:Glazing:EquivalentLayer,
+    GLZCLR,                  !- Name
+    SpectralAverage,         !- Optical Data Type
+    ,                        !- Window Glass Spectral Data Set Name
+    0.83,                    !- Front Side Beam-Beam Solar Transmittance
+    0.83,                    !- Back Side Beam-Beam Solar Transmittance
+    0.08,                    !- Front Side Beam-Beam Solar Reflectance
+    0.08,                    !- Back Side Beam-Beam Solar Reflectance
+    0.0,                     !- Front Side Beam-Beam Visible Transmittance
+    0.0,                     !- Back Side Beam-Beam Visible Transmittance
+    0.0,                     !- Front Side Beam-Beam Visible Reflectance
+    0.0,                     !- Back Side Beam-Beam Visible Reflectance
+    0.0,                     !- Front Side Beam-Diffuse Solar Transmittance
+    0.0,                     !- Back Side Beam-Diffuse Solar Transmittance
+    0.0,                     !- Front Side Beam-Diffuse Solar Reflectance
+    0.0,                     !- Back Side Beam-Diffuse Solar Reflectance
+    0.0,                     !- Front Side Beam-Diffuse Visible Transmittance
+    0.0,                     !- Back Side Beam-Diffuse Visible Transmittance
+    0.0,                     !- Front Side Beam-Diffuse Visible Reflectance
+    0.0,                     !- Back Side Beam-Diffuse Visible Reflectance
+    0.76,                    !- Diffuse-Diffuse Solar Transmittance
+    0.14,                    !- Front Side Diffuse-Diffuse Solar Reflectance
+    0.14,                    !- Back Side Diffuse-Diffuse Solar Reflectance
+    0.0,                     !- Diffuse-Diffuse Visible Transmittance
+    0.0,                     !- Front Side Diffuse-Diffuse Visible Reflectance
+    0.0,                     !- Back Side Diffuse-Diffuse Visible Reflectance
+    0.0,                     !- Infrared Transmittance
+    0.84,                    !- Front Side Infrared Emissivity
+    0.84;                    !- Back Side Infrared Emissivity
+\end{lstlisting}
+
+\subsection{WindowMaterial:Gap:EquivalentLayer}\label{windowmaterialgapequivalentlayer}
+
+This object is used in windows equivalent layer construction object andspecifies the properties of the gap between the layers in multi-layer equivalent layer window object. There is an EnergyPlus Reference Data Set for Material:WindowGas that contains several types of gas. This object uses the gas types: Air, Argon, Xenon, Crypton, and Custom.~ For Custom gas type users are required to entering the thermophicial properties.
+
+\subsubsection{Inputs}\label{inputs-31-001}
+
+\paragraph{Field: Name}\label{field-name-25-002}
+
+The name of the gap. It refers to a layer in a window construction equivalent layer.
+
+\paragraph{Field: Gas Type}\label{field-gas-type-1}
+
+The type of gas. The choices allowed are AIR, ARGON, XENON, KRYPTON, or CUSTOM.
+
+\paragraph{Field: Thickness}\label{field-thickness-8}
+
+The thickness (m) of the gap layer.
+
+\paragraph{Field: Gap Vent Type}\label{field-gap-vent-type}
+
+This inputfiled contains the valid key choice for gap vent type.~ The valid vent types are: Sealed, VentedIndoor, and VentedOutdoor.~ Sealed means the gap is enclosed and gas tight, i.e., no venting to indoor or outdoor environment. The gap types ``VentedIndoor'' and ``VentedOutdoor'' are used with gas type ``Air'' only. VentedIndoor means the air in the gap is naturally vented to indoor environment, and~ VentedOutdoor means the air in the gap is naturally vented to the outdoor environment.
+
+\paragraph{Properties for Custom Gas Types}\label{properties-for-custom-gas-types-1}
+
+The following entries are used only if Gas Type = Custom. The A, B and C coefficients are those in the following expression that gives a property value as a function of temperature in degrees K:
+
+\begin{equation}
+Property = Coef{f_A} + Coef{f_B} \times Temperatur{e_K} + Coef{f_C} \times Temperature_K^2
+\end{equation}
+
+\paragraph{Field: Conductivity Coefficient A}\label{field-conductivity-coefficient-a-1}
+
+The A coefficient for gas conductivity (W/m-K). Used only if Gas Type = Custom.
+
+\paragraph{Field: Conductivity Coefficient B}\label{field-conductivity-coefficient-b-1}
+
+The B coefficient for gas conductivity (W/m-K\(^{2}\)). Used only if Gas Type = Custom.
+
+\paragraph{Field: Conductivity Coefficient C}\label{field-conductivity-coefficient-c-1}
+
+The C coefficient for gas conductivity (W/m-K\(^{3}\)).~ Used only if Gas Type = Custom.
+
+\paragraph{Field: Viscosity Coefficient A}\label{field-viscosity-coefficient-a-1}
+
+The A coefficient for gas viscosity (kg/m-s). Used only if Gas Type = Custom.
+
+\paragraph{Field: Viscosity Coefficient B}\label{field-viscosity-coefficient-b-1}
+
+The B coefficient for gas viscosity (kg/m-s-K). Used only if Gas Type = Custom.
+
+\paragraph{Field: Viscosity Coefficient C}\label{field-viscosity-coefficient-c-1}
+
+The C coefficient for gas viscosity (kg/m-s-K\(^{2}\)).~ Used only if Gas Type = Custom.
+
+\paragraph{Field: Specific Heat Coefficient A}\label{field-specific-heat-coefficient-a-1}
+
+The A coefficient for gas specific heat (J/kg-K). Used only if Gas Type = Custom.
+
+\paragraph{Field: Specific Heat Coefficient B}\label{field-specific-heat-coefficient-b-1}
+
+The B coefficient for gas specific heat (J/kg-K\(^{2}\)). Used only if Gas Type = Custom.
+
+\paragraph{Field: Specific Heat Coefficient C}\label{field-specific-heat-coefficient-c-1}
+
+The C coefficient for gas specific heat (J/kg-K\(^{2}\)).~ Used only if Gas Type = Custom.
+
+\paragraph{Field: Specific Heat Ratio}\label{field-specific-heat-ratio-2}
+
+The specific heat ratio for gas.~ Used only if Gas Type = Custom.
+
+\paragraph{Field: Molecular Weight}\label{field-molecular-weight-1}
+
+The molecular weight for gas.~ The molecular weight is the mass of 1 mol of the substance.~ This has a numerical value which is the average molecular mass of the molecules in the substance multiplied by Avogadro's constant. (kg/kmol) (Shown in the IDD as g/mol for consistency)
+
+\paragraph{Field: Specific Heat Ratio}\label{field-specific-heat-ratio-3}
+
+The specific heat ratio for gas.~ The specific heat ratio of a gas is the ratio of the specific heat at contant pressure, to the specific heat at constant volume.~ Used only if Gas Type = Custom.
+
+An IDF example for this object, is shown below:
+
+\begin{lstlisting}
+
+WindowMaterial:Gap:EquivalentLayer,
+    Custom CO2 Sealed 12mm,    !- Name
+    CUSTOM,                    !- Gas Type
+    0.0120,                    !- Thickness {m}
+    Sealed,                    !- Gap Vent Type
+   -5.8181E-3,                 !- Conductivity Coefficient A {W/m-K}
+    7.4714E-5,                 !- Conductivity Coefficient B {W/m-K2}
+    0.0,                       !- Conductivity Coefficient C {W/m-K3}
+    8.5571E-7,                 !- Viscosity Coefficient A {kg/m-s}
+    4.7143E-8,                 !- Viscosity Coefficient B {kg/m-s-K}
+    0.0,                       !- Viscosity Coefficient C {kg/m-s-K2}
+    5.76903E2,                 !- Specific Heat Coefficient A {J/kg-K}
+    9.18088E-2,                !- Specific Heat Coefficient B {J/kg-K2}
+    0.0,                       !- Specific Heat Coefficient C {J/kg-K3}
+    44.01;                     !- Molecular Weight {g/mol}
+\end{lstlisting}
+
+\subsection{Material:RoofVegetation}\label{materialroofvegetation}
+
+This definition must be used in order to simulate the green roof (ecoroof) model. The material becomes the outside layer in a green roof construction (see example below). In the initial release of the green roof model, only one material may be used as a green roof layer though, of course, several constructions using that material may be used. In addition, the model has only been tested with the ConductionTransferFunction solution algorithm -- a warning will be issued for other solution algorithm choices. This model was developed for low-sloped exterior surfaces (roofs). It is not recommended for high-sloped exterior surfaces (e.g., walls).
+
+\subsubsection{Inputs}\label{inputs-32-000}
+
+\paragraph{Field: Name}\label{field-name-26-002}
+
+This field is a unique reference name that the user assigns to a particular ecoroof material. This name can then be referred to by other input data.
+
+\paragraph{Field: Height of Plants}\label{field-height-of-plants}
+
+This field defines the height of plants in units of meters. This field is limited to values in the range 0.005 \textless{} Height \textless{} 1.00 m. Default is .2 m.
+
+\paragraph{Field: Leaf Area Index}\label{field-leaf-area-index}
+
+This is the projected leaf area per unit area of soil surface. This field is dimensionless and is limited to values in the range of 0.001 \textless{} LAI \textless{} 5.0. Default is 1.0. At the present time the fraction vegetation cover is calculated directly from LAI (Leaf Area Index) using an empirical relation. The user may find it necessary to increase the specified value of LAI in order to represent high fractional coverage of the surface by vegetation.
+
+\paragraph{Field: Leaf Reflectivity}\label{field-leaf-reflectivity}
+
+This field represents the fraction of incident solar radiation that is reflected by the individual leaf surfaces (albedo). Solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. Values for this field must be between 0.05 and 0.5. Default is .22. Typical values are .18 to .25.
+
+\paragraph{Field: Leaf Emissivity}\label{field-leaf-emissivity}
+
+This field is the ratio of thermal radiation emitted from leaf surfaces to that emitted by an ideal black body at the same temperature. This parameter is used when calculating the long wavelength radiant exchange at the leaf surfaces. Values for this field must be between 0.8 and 1.0 (with 1.0 representing ``black body'' conditions). Default is .95.
+
+\paragraph{Field: Minimum Stomatal Resistance}\label{field-minimum-stomatal-resistance}
+
+This field represents the resistance of the plants to moisture transport. It has units of s/m. Plants with low values of stomatal resistance will result in higher evapotranspiration rates than plants with high resistance. Values for this field must be in the range of 50.0 to 300.0. Default is 180.
+
+\paragraph{Field: Soil Layer Name}\label{field-soil-layer-name}
+
+This field is a unique reference name that the user assigns to the soil layer for a particular ecoroof. This name can then be referred to by other input data. Default is \textbf{Green Roof Soil}.
+
+\paragraph{Field: Roughness}\label{field-roughness-2}
+
+This alpha field defines the relative roughness of a particular material layer. This parameter only influences the convection coefficients, more specifically the exterior convection coefficient. A keyword is expected in this field with the options being ``VeryRough'', ``Rough'', ``MediumRough'', ``MediumSmooth'', ``Smooth'', and ``VerySmooth'' in order of roughest to smoothest options. Default is MediumRough.
+
+\paragraph{Field: Thickness}\label{field-thickness-9}
+
+This field characterizes the thickness of the material layer in meters. This should be the dimension of the layer in the direction perpendicular to the main path of heat conduction. This value must be a positive number. Depths of .10m (4 inches) and .15m (6 inches) are common. Default if this field is left blank is .1. Maximum is .7m. Must be greater than .05 m.
+
+\paragraph{Field: Conductivity of Dry Soil}\label{field-conductivity-of-dry-soil}
+
+This field is used to enter the thermal conductivity of the material layer. Units for this parameter are W/(m-K). Thermal conductivity must be greater than zero. Typical soils have values from .3 to .5. Minimum is .2 (specified in IDD). Default is .35 and maximum (in IDD) is 1.5.
+
+\paragraph{Field: Density of Dry Soil}\label{field-density-of-dry-soil}
+
+This field is used to enter the density of the material layer in units of kg/m\(^{3}\). Density must be a positive quantity. Typical soils range from 400 to 1000 (dry to wet). Minimum is 300, maximum is 2000 and default if field is left blank is 1100.
+
+\paragraph{Field: Specific Heat of Dry Soil}\label{field-specific-heat-of-dry-soil}
+
+This field represents the specific heat of the material layer in units of J/(kg-K). Note that these units are most likely different than those reported in textbooks and references which tend to use kJ/(kg-K) or J/(g-K). They were chosen for internal consistency within EnergyPlus. Only positive values of specific heat are allowed.
+
+\paragraph{Field: Thermal Absorptance}\label{field-thermal-absorptance-2}
+
+The thermal absorptance field in the Material input syntax represents the fraction of incident long wavelength radiation that is absorbed by the material. This parameter is used when calculating the long wavelength radiant exchange between various surfaces and affects the surface heat balances (both inside and outside as appropriate). For long wavelength radiant exchange, thermal emissivity and thermal emittance are equal to thermal absorptance. Values for this field must be between 0.0 and 1.0 (with 1.0 representing ``black body'' conditions). Typical values are from .9 to .98. The default value for this field is 0.9.
+
+\paragraph{Field: Solar Absorptance}\label{field-solar-absorptance-2}
+
+The solar absorptance field in the Material input syntax represents the fraction of incident~ solar radiation that is absorbed by the material. Solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident solar radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate). If solar reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.0 and 1.0. Typical values are from .6 to .85. The default value for this field is 0.7.
+
+\paragraph{Field: Visible Absorptance}\label{field-visible-absorptance-2}
+
+The visible absorptance field in the Material input syntax represents the fraction of incident visible wavelength radiation that is absorbed by the material. Visible wavelength radiation is slightly different than solar radiation in that the visible band of wavelengths is much more narrow while solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident visible radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate) as well as the daylighting calculations. If visible reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.5 and 1.0. The default value for this field is 0.75.
+
+\paragraph{Field: Saturation Volumetric Moisture Content of the Soil Layer}\label{field-saturation-volumetric-moisture-content-of-the-soil-layer}
+
+The field allows for user input of the saturation moisture content of the soil layer. Maximum moisture content is typically less than .5. Range is {[}.1,.5{]} with the default being .3.
+
+\paragraph{Field: Residual Volumetric Moisture Content of the Soil Layer}\label{field-residual-volumetric-moisture-content-of-the-soil-layer}
+
+The field allows for user input of the residual moisture content of the soil layer. Default is .01, range is {[}.01,.1{]}.
+
+\paragraph{Field: Initial Volumetric Moisture Content of the Soil Layer}\label{field-initial-volumetric-moisture-content-of-the-soil-layer}
+
+The field allows for user input of the initial moisture content of the soil layer. Range is (.05, .5{]} with the defaulte being .1.
+
+\paragraph{Field: Moisture Diffusion Calculation Method}\label{field-moisture-diffusion-calculation-method}
+
+The field allows for two models to be selected: \textbf{Simple} or \textbf{Advanced}.
+
+\textbf{Simple} is the original Ecoroof model - based on a constant diffusion of moisture through the soil.~ This model starts with the soil in two layers.~ Every time the soil properties update is called, it will look at the two soils moisture layers and asses which layer has more moisture in it. It then takes moisture from the higher moisture layer and redistributes it to the lower moisture layer at a constant rate.
+
+\textbf{Advanced} is the later Ecoroof model. If you use it, you will need to increase your number of timesteps in hour for the simulation with a recommended value of 20. This moisture transport model is based on a project which looked at the way moisture transports through soil.~ It uses a finite difference method to divide the soil into layers (nodes). It redistributes the soil moisture according the model described in:
+
+Marcel G Schaap and Martinus Th. van Genuchten, 2006, `A modified Maulem-van Genuchten Formulation for Improved Description of the Hydraulic Conductivity Near Saturation', Vadose Zone Journal 5 (1), p 27-34.
+
+An IDF example:
+
+\begin{lstlisting}
+
+Material:RoofVegetation,
+      BaseEco,                 !- Name
+      0.5,                     !- Height of Plants {m}
+      5,                       !- Leaf Area Index {dimensionless}
+      0.2,                     !- Leaf Reflectivity {dimensionless}
+      0.95,                    !- Leaf Emissivity
+      180,                     !- Minimum Stomatal Resistance {s/m}
+      EcoRoofSoil,             !- Soil Layer Name
+      MediumSmooth,            !- Roughness
+      0.18,                    !- Thickness {m}
+      0.4,                     !- Conductivity of Dry Soil {W/m-K}
+      641,                     !- Density of Dry Soil {kg/m3}
+      1100,                    !- Specific Heat of Dry Soil {J/kg-K}
+      0.95,                    !- Thermal Absorptance
+      0.8,                     !- Solar Absorptance
+      0.7,                     !- Visible Absorptance
+     0.4,                     !- Saturation Volumetric Moisture Content of the Soil Layer
+      0.01,                    !- Residual Volumetric Moisture Content of the Soil Layer
+      0.2,                     !- Initial Volumetric Moisture Content of the Soil Layer
+      Advanced;                !- Moisture Diffusion Calculation Method
+
+
+    Material:RoofVegetation,
+      LowLAI,                  !- Name
+      0.5,                     !- Height of Plants {m}
+      0.5,                     !- Leaf Area Index {dimensionless}
+      0.2,                     !- Leaf Reflectivity {dimensionless}
+      0.95,                    !- Leaf Emissivity
+      180,                     !- Minimum Stomatal Resistance {s/m}
+      EcoRoofSoil,             !- Soil Layer Name
+      MediumSmooth,            !- Roughness
+      0.18,                    !- Thickness {m}
+      0.4,                     !- Conductivity of Dry Soil {W/m-K}
+      641,                     !- Density of Dry Soil {kg/m3}
+      1100,                    !- Specific Heat of Dry Soil {J/kg-K}
+      0.95,                    !- Thermal Absorptance
+      0.8,                     !- Solar Absorptance
+      0.7,                     !- Visible Absorptance
+     0.4,          !- Saturation Volumetric Moisture Content of the Soil Layer
+      0.01,         !- Residual Volumetric Moisture Content of the Soil Layer
+      0.2,          !- Initial Volumetric Moisture Content of the Soil Layer
+      Advanced;                !- Moisture Diffusion Calculation Method
+\end{lstlisting}
+
+And construction using the ecoroof material:
+
+\begin{lstlisting}
+
+Construction,
+      ASHRAE 90.1-2004_Sec 5.5-2_Roof,  !- Name
+      BaseEco,                 !- Outside Layer
+      ASHRAE 90.1-2004_Sec 5.5-2_Roof Insulation_1,  !- Layer \#2
+      ASHRAE 90.1-2004_Sec 5.5-2_MAT-METAL;  !- Layer \#3
+\end{lstlisting}
+
+\subsection{Ecoroof / RoofVegetation outputs}\label{ecoroof-roofvegetation-outputs}
+
+The following outputs are available for the Roof Vegetation surface.
+
+\begin{itemize}
+\item
+  Zone,Average,Green Roof Soil Temperature {[}C{]}
+\item
+  Zone,Average,Green Roof Vegetation Temperature {[}C{]}
+\item
+  Zone,Average,Green Roof Soil Root Moisture Ratio {[]}
+\item
+  Zone,Average,Green Roof Soil Near Surface Moisture Ratio {[]}
+\item
+  Zone,Average,Green Roof Soil Sensible Heat Transfer Rate per Area {[}W/m2{]}
+\item
+  Zone,Average,Green Roof Vegetation Sensible Heat Transfer Rate per Area {[}W/m2{]}
+\item
+  Zone,Average,Green Roof Vegetation Moisture Transfer Rate {[}m/s{]}
+\item
+  Zone,Average,Green Roof Soil Moisture Transfer Rate {[}m/s{]}
+\item
+  Zone,Average,Green Roof Vegetation Latent Heat Transfer Rate per Area {[}W/m2{]}
+\item
+  Zone,Average,Green Roof Soil Latent Heat Transfer Rate per Area {[}W/m2{]}
+\item
+  Zone,Sum,Green Roof Cumulative Precipitation Depth {[}m{]}
+\item
+  Zone,Sum,Green Roof Cumulative Irrigation Depth {[}m{]}
+\item
+  Zone,Sum,Green Roof Cumulative Runoff Depth {[}m{]}
+\item
+  Zone,Sum,Green Roof Cumulative Evapotranspiration Depth {[}m{]}
+\item
+  Zone,Sum,Green Roof Current Precipitation Depth {[}m{]}
+\item
+  Zone,Sum,Green Roof Current Irrigation Depth {[}m{]}
+\item
+  Zone,Sum,Green Roof Current Runoff Depth {[}m{]}
+\item
+  Zone,Sum,Green Roof Current Evapotranspiration Depth {[}m{]}
+\end{itemize}
+
+\subsubsection{Green Roof Soil Temperature {[}C{]}}\label{green-roof-soil-temperature-c}
+
+Temperature of the Soil layer temperature in C.
+
+\subsubsection{Green Roof Vegetation Temperature {[}C{]}}\label{green-roof-vegetation-temperature-c}
+
+Temperature of the Vegetation layer temperature in C.
+
+\subsubsection{\texorpdfstring{Green Roof Soil Root Moisture Ratio {[]}}{Green Roof Soil Root Moisture Ratio }}\label{green-roof-soil-root-moisture-ratio}
+
+Mean value of root moisture (m\(^{3}\)/m\(^{3}\))
+
+\subsubsection{\texorpdfstring{Green Roof Soil Near Surface Moisture Ratio {[]}}{Green Roof Soil Near Surface Moisture Ratio }}\label{green-roof-soil-near-surface-moisture-ratio}
+
+The moisture content in the soil near the surface (m\(^{3}\)/m\(^{3}\))
+
+\subsubsection{Green Roof Soil Sensible Heat Transfer Rate per Area {[}W/m2{]}}\label{green-roof-soil-sensible-heat-transfer-rate-per-area-wm2}
+
+Sensible heat flux to ground (W/m\(^{2}\))
+
+\subsubsection{Green Roof Vegetation Sensible Heat Transfer Rate per Area {[}W/m2{]}}\label{green-roof-vegetation-sensible-heat-transfer-rate-per-area-wm2}
+
+Sensible heat transfer to foliage (W/m\(^{2}\))
+
+\subsubsection{Green Roof Vegetation Moisture Transfer Rate {[}m/s{]}}\label{green-roof-vegetation-moisture-transfer-rate-ms}
+
+Water evapotranspiration rate associated with latent heat from vegetation (m/s)
+
+\subsubsection{Green Roof Soil Moisture Transfer Rate {[}m/s{]}}\label{green-roof-soil-moisture-transfer-rate-ms}
+
+Water evapotranspiration rate associated with latent heat from ground surface (m/s)
+
+\subsubsection{Green Roof Vegetation Latent Heat Transfer Rate per Area {[}W/m2{]}}\label{green-roof-vegetation-latent-heat-transfer-rate-per-area-wm2}
+
+Latent heat flux from vegetation (W/m\(^{2}\))
+
+\subsubsection{Green Roof Soil Latent Heat Transfer Rate per Area {[}W/m2{]}}\label{green-roof-soil-latent-heat-transfer-rate-per-area-wm2}
+
+Latent heat flux from ground surface (W/m\(^{2}\))
+
+\subsubsection{Green Roof Cumulative Precipitation Depth {[}m{]}}\label{green-roof-cumulative-precipitation-depth-m}
+
+\subsubsection{Green Roof Current Precipitation Depth {[}m{]}}\label{green-roof-current-precipitation-depth-m}
+
+Cumulative or current precipitation (m)
+
+\subsubsection{Green Roof Cumulative Irrigation Depth {[}m{]}}\label{green-roof-cumulative-irrigation-depth-m}
+
+\subsubsection{Green Roof Current Irrigation Depth {[}m{]}}\label{green-roof-current-irrigation-depth-m}
+
+Cumulative or current irrigation (m)
+
+\subsubsection{Green Roof Cumulative Runoff Depth {[}m{]}}\label{green-roof-cumulative-runoff-depth-m}
+
+\subsubsection{Green Roof Current Runoff Depth {[}m{]}}\label{green-roof-current-runoff-depth-m}
+
+Cumulative or current runoff (m). Multiply by roof area to get volume.
+
+\subsubsection{Green Roof Cumulative Evapotranspiration Depth {[}m{]}}\label{green-roof-cumulative-evapotranspiration-depth-m}
+
+\subsubsection{Green Roof Current Evapotranspiration Depth {[}m{]}}\label{green-roof-current-evapotranspiration-depth-m}
+
+Cumulative or current evapotranspiration from soil and plants (m).
+
+\subsection{MaterialProperty:GlazingSpectralData}\label{materialpropertyglazingspectraldata}
+
+With the MaterialProperty:GlazingSpectralData object, you can specify the wavelength-by-wavelength transmittance and reflectance properties of a glass material. To determine the~ overall optical properties of a glazing system (solar and visible transmittance and solar absorptance vs.~angle of incidence) EnergyPlus first calculates transmittance and absorptance vs.~angle of incidence for each wavelength. This is then weighted by a standard solar spectrum to get the solar transmittance and absorptance vs.~angle of incidence (for use in the solar heat gain calculations), and further weighted by the response of the human eye to get the visible transmittance vs.~angle of incidence (for use in the daylighting calculation).
+
+MaterialProperty:GlazingSpectralData should be used for multi-pane windows when one or more of the glass layers is \emph{spectrally selective}, i.e., the transmittance depends strongly on wavelength. An example is glass with a coating that gives high transmittance in the daylight part of the solar spectrum (roughly 0.4 to 0.7 microns) and low transmittance at longer wavelengths, thus providing better solar heat gain control than uncoated glass. If spectral data is not used in case, the overall optical properties of the glazing system that EnergyPlus calculates will not be correct.
+
+You can input up to 450 sets of values for wavelengths covering the solar spectrum. Each set consists of~ \{wavelength (microns), transmittance, front reflectance, back reflectance\}
+
+Spectral data of this kind are routinely measured by glass manufacturers. Data sets for over 800 commercially available products are contained in an Optical Data Library maintained by the Windows Group at Lawrence Berkeley National Laboratory. This library can be downloaded from http://windows.lbl.gov/. You will have to edit entries from this library to put them in the format required by the EnergyPlus WindowGlassSpectralData object.
+
+An alternative to using the MaterialProperty:GlazingSpectralData object is to run the WINDOW window analysis program. This program has built-in access to the Optical Data Library and let's you easily create customized, multi-layer glazing systems that can be exported for use in EnergyPlus. For more details, see ``StormWindow''.
+
+\subsubsection{Inputs}\label{inputs-33-000}
+
+\paragraph{Field: Name}\label{field-name-27-002}
+
+The name of the spectral data set. It is referenced by WindowMaterial:Glazing when Optical Data Type = Spectral.
+
+\paragraph{Fields 1-4 (repeated up to 450 times)}\label{fields-1-4-repeated-up-to-450-times}
+
+Sets of values for wavelengths covering the solar spectrum (from about 0.25 to 2.5 microns {[}10\(^{-6}\) m{]}). Each set consists of
+
+\textbf{\{wavelength (microns), transmittance, front reflectance, back reflectance\}}
+
+The wavelength values must be in ascending order. The transmittance and reflectance values are at normal incidence. ``Front reflectance'' is the reflectance for radiation striking the glass from the outside, i.e., from the side opposite the zone in which the window is defined. ``Back reflectance'' is the reflectance for radiation striking the glass from the inside, i.e., from the zone in which the window is defined. Therefore, for exterior windows, ``front'' is the side closest to the outdoors and ``back'' is the side closest to the zone in which the window is defined. For interior windows, ``front'' is the side closest to the adjacent zone and ``back'' is the side closest to the zone in which the window is defined.
+
+An IDF example:
+
+\begin{lstlisting}
+
+MaterialProperty:GlazingSpectralData,
+        TestSpectralDataSet,
+         ! { from WINDOW 4 library }
+         ! { actual 9.91mm clear laminate: 15_mil PVB, ID:37966/50032-39-9 } 10.38
+         ! { conductivity PVB adjusted, W/M/K  } 0.798
+         ! { thermal IR transmittance, assumed } tir = 0.00
+         ! { thermal IR hemispherical emittance, assumed } emis = 0.84 0.84
+
+
+         ! WL   T     Rfront Rback
+         .300, 0.000, 0.045, 0.045,
+         .310, 0.000, 0.044, 0.044,
+         .320, 0.000, 0.044, 0.044,
+         .330, 0.000, 0.042, 0.042,
+         .340, 0.000, 0.041, 0.041,
+         .350, 0.000, 0.040, 0.040,
+  <snip>
+        2.450, 0.200, 0.040, 0.040,
+        2.500, 0.214, 0.039, 0.039;
+\end{lstlisting}
+
+\subsection{Construction}\label{construction-000}
+
+For walls, roofs, floors, windows, and doors, constructions are ``built'' from the included materials. Each layer of the construction is a material name listed in order from ``outside'' to ``inside''. Up to ten layers (eight for windows) may be specified (one of the few limitations in EnergyPlus!). ``Outside'' is the layer furthest away from the Zone air (not necessarily the outside environment). ``Inside'' is the layer next to the Zone air. In the example floor below, for example, the outside layer is the acoustic tile below the floor, the next layer is the air space above the tile, and the inside layer is the concrete floor deck.
+
+\begin{figure}[hbtp] % fig 24
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image050.png}
+\caption{Example Floor Construction illustration. \protect \label{fig:example-floor-construction-illustration.}}
+\end{figure}
+
+Window constructions are similarly built up from items in the Window Materials set using similar layers.. See Figure~\ref{fig:illustration-for-material-ordering-in}. Illustration for material ordering in windows, which shows the case where an interior shading layer such as a blind is present. The gap between the inside glass layer (layer \#3) and the interior shading layer is not entered. Similarly, for an exterior shading layer, the gap between the outside glass layer and the shading layer is not entered.
+
+\begin{figure}[hbtp] % fig 25
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image051.png}
+\caption{Illustration for material ordering in windows. \protect \label{fig:illustration-for-material-ordering-in}}
+\end{figure}
+
+However, for a between-glass shading device the gaps on either side of the shading layer must be entered and they must have the same gas type. In addition, the gap widths with and without the between-glass shading layer must be consistent (see Figure~\ref{fig:window-construction-with-and-without-a}).
+
+A maximum of four glass layers and one shading layer is allowed. A gas layer must always separate adjacent glass layers in a multi-pane glazing without a between-glass shading layer.
+
+\begin{figure}[hbtp] % fig 26
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image052.png}
+  \caption{Window construction with and without a between-glass shading layer. Shown are gap widths \(g\), \(g_1\) and \(g_2\), and shading layer width, \(w\). An error will result if \(g_1 + g_2 +w\) is not equal to \(g\), where \(w\) is zero for a blind and greater than zero for a shade. \protect \label{fig:window-construction-with-and-without-a}}
+\end{figure}
+
+Outside and inside air film resistances are never given as part of a construction definitions since they are calculated during the EnergyPlus simulation. Note also that constructions are assumed to be one-dimensional in a direction perpendicular to the surface.
+
+\subsubsection{Inputs}\label{inputs-34-000}
+
+\paragraph{Field: Name}\label{field-name-28-001}
+
+This field is a user specified name that will be used as a reference by other input syntax. For example, a heat transfer surface (ref: Building Surfaces) requires a construction name to define what the make-up of the wall is. This name must be identical to one of the Construction definitions in the input data file.
+
+\paragraph{Field: Outside Layer}\label{field-outside-layer}
+
+Each construction must have at least one layer. This field defines the material name associated with the layer on the outside of the construction---outside referring to the side that is not exposed to the zone but rather the opposite side environment, whether this is the outdoor environment or another zone. Material layers are defined based on their thermal properties elsewhere in the input file (ref: Material and Material Properties and Zone,Average,HAMT Surface Average Water Content Ratio {[}kg/kg{]}
+
+Zone,Average,HAMT Surface Inside Face Temperature {[}C{]}
+
+Zone,Average,HAMT Surface Inside Face Relative Humidity {[}\%{]}
+
+Zone,Average,HAMT Surface Inside Face Vapor Pressure {[}Pa{]}
+
+Zone,Average,HAMT Surface Outside Face Temperature {[}C{]}
+
+Zone,Average,HAMT Surface Outside Face Relative Humidity {[}\%{]}
+
+Zone,Average,HAMT Surface Inside Face Relative Humidity {[}\%{]}
+
+\paragraph{HAMT Surface Average Water Content Ratio {[}kg/kg{]}}\label{hamt-surface-average-water-content-ratio-kgkg-1}
+
+This output is the summed water content {[}kg/kg{]} of all cells in a surface expressed as a fraction of the mass of the water to the material mass.
+
+\paragraph{HAMT Surface Inside Face Temperature {[}C{]}}\label{hamt-surface-inside-face-temperature-c-1}
+
+This output is the temperature {[}C{]} on the internal ``surface'' of the surface.
+
+\paragraph{HAMT Surface Inside Face Relative Humidity {[}\%{]}}\label{hamt-surface-inside-face-relative-humidity-2}
+
+\paragraph{HAMT Surface Inside Face Relative Humidity {[}\%{]}}\label{hamt-surface-inside-face-relative-humidity-3}
+
+This output is the relative humidity on the internal ``surface'' of the surface expressed as a percentage.
+
+\paragraph{HAMT Surface Inside Face Vapor Pressure {[}Pa{]}}\label{hamt-surface-inside-face-vapor-pressure-pa-1}
+
+This output is the vapor pressure {[}Pa{]} on the internal ``surface'' of the surface.
+
+\paragraph{HAMT Surface Outside Face Temperature {[}C{]}}\label{hamt-surface-outside-face-temperature-c-1}
+
+This output is the temperature on the external ``surface'' of the surface.
+
+\paragraph{HAMT Surface Outside Face Relative Humidity {[}\%{]}}\label{hamt-surface-outside-face-relative-humidity-1}
+
+This output is the relative humidity on the external ``surface'' of the surface.
+
+Zone,Average,HAMT Surface Temperature Cell N {[}C{]}
+
+Zone,Average,HAMT Surface Water Content Cell N {[}kg/kg{]}
+
+Zone,Average,HAMT Surface Relative Humidity Cell N {[}\%{]}
+
+Detailed profile data for the variables Temperature {[}C{]}, Relative Humidity {[}\%{]} and Water Content {[}kg/kg{]} within each surface can also be reported. To calculate the heat and moisture transfer through surfaces HAMT splits up surfaces into discrete cells. Each cell is composed of a single material and has a position within the surface. HAMT automatically assigns cells to construction objects so that there are more cells closer to boundaries between materials and also at the ``surfaces'' of the surface. It is not possible for users to define their own cells.
+
+\paragraph{HAMT Surface Relative Humidity Cell \textless{}N\textgreater{} {[}\%{]}}\label{hamt-surface-relative-humidity-cell-n-1}
+
+This is the relative humidity of the cell in the surface.
+
+\paragraph{HAMT Surface Temperature Cell \textless{}N\textgreater{} {[}C{]}}\label{hamt-surface-temperature-cell-n-c-1}
+
+This is the temperature of the cell in the surface.
+
+\paragraph{HAMT Surface Water Content Cell \textless{}N\textgreater{} {[}kg/kg{]}}\label{hamt-surface-water-content-cell-n-kgkg-1}
+
+This is the relative water content of the cell in the surface.
+
+Each surface is made from a particular construction. The construction-surface relationship is output by HAMT to the eplusout.eio file with the following format.
+
+! \textless{}HAMT cells\textgreater{}, Surface Name, Construction Name, Cell Numbers
+
+! \textless{}HAMT origins\textgreater{}, Surface Name, Construction Name, Cell origins (m)
+
+The output also contains the HAMT cell origins and cell number for each construction -- surface combination. The coordinate system origin is defined as the exterior surface of the construction. Users can select any one of the Temperature, Relative Humidity or Water Content variables for any cell to be reported, using the following naming scheme for the output variable.
+
+HAMT Profile Construction \textless{}Variable\textgreater{} Cell \textless{}Cell\#\textgreater{}
+
+It is better to specify the ``key'' or Surface Name in this output.
+
+So for example to output the temperature of the 10\(^{th}\) cell in a surface, eg ``East Wall'' would require the following output variable.
+
+\begin{lstlisting}
+
+Output:Variable,
+      East Wall,               !- Key Value
+      HAMT Profile Construction Temperature Cell 10,  !- Variable Name
+      Hourly;                  !- Reporting Frequency
+\end{lstlisting}
+
+By selecting a whole range of these reports and using the information in the eplusout.eio file it is possible to build up a temperature profile of the surface.
+
+Materials for Glass Windows and Doors). As noted above, the outside layer should NOT be a film coefficient since EnergyPlus will calculate outside convection and radiation heat transfer more precisely.
+
+\paragraph{Field(s) 2-10: Layers}\label{fields-2-10-layers}
+
+The next fields are optional and the number of them showing up in a particular Construction definition depends solely on the number of material layers present in that construction. The data expected is identical to the outside layer field (see previous field description). The order of the remaining layers is important and should be listed in order of occurrence from the one just inside the outside layer until the inside layer is reached. As noted above, the inside layer should NOT be a film coefficient since EnergyPlus will calculate inside convection and radiation heat transfer more precisely.
+
+IDF Example (floor construction):
+
+\begin{lstlisting}
+
+Construction, FLOOR38,  ! Material layer names follow:
+        E5 - ACOUSTIC TILE,
+        E4 - CEILING AIRSPACE,
+        C12 - 2 IN HW CONCRETE;
+\end{lstlisting}
+
+IDF Example (window construction, no shade):
+
+\begin{lstlisting}
+
+Construction, DOUBLE PANE WINDOW,  !- Material layer names follow:
+        GLASS - CLEAR SHEET 1 / 8 IN,
+        WinAirB1 - AIRSPACE RESISTANCE,
+        GLASS - CLEAR SHEET 1 / 8 IN;
+\end{lstlisting}
+
+IDF Example (window construction, with interior shade):
+
+\begin{lstlisting}
+
+Construction, DOUBLE PANE WITH ROLL SHADE,  !- Material layer names follow:
+        GLASS - CLEAR SHEET 1 / 8 IN,
+        WinAirB1 - AIRSPACE RESISTANCE,
+        GLASS - CLEAR SHEET 1 / 8 IN,
+        ROLL SHADE - LIGHT
+\end{lstlisting}
+
+\subsection{Site:GroundTemperature:FCfactorMethod}\label{sitegroundtemperaturefcfactormethod-000}
+
+Site:GroundTemperature:FCfactorMethod is used only by the underground walls or slabs-on-grade or underground floors defined with C-factor (Construction:CfactorUndergroundWall) and F-factor (Construction:FfactorGroundFloor) method for code compliance calculations where detailed construction layers are unknown. Only one such ground temperature object can be included. The monthly ground temperatures for this object are close to the monthly outside air temperatures delayed by three months. If user does not input this object in the IDF file, it will be defaulted to the 0.5m set of monthly ground temperatures from the weather file if they are available.
+
+\subsubsection{Inputs}\label{inputs-35-000}
+
+\paragraph{Field: Month Temperature(s) -- 12 fields in all}\label{field-month-temperatures-12-fields-in-all-000}
+
+Each numeric field is the monthly ground temperature (degrees Celsius) used for the indicated month (January = 1\(^{st}\) field, February = 2\(^{nd}\) field, etc.)
+
+And, the IDF example:
+
+\begin{lstlisting}
+Site:GroundTemperature:FCfactorMethod,  9.5,3.5,-0.7,-1.7,-0.6,3.6,9.3,14,18.2,22.7,21.2,16.8;
+\end{lstlisting}
+
+\subsection{Constructions - Modeling Underground Walls and Ground Floors Defined with C and F Factors for Building Energy Code Compliance}\label{constructions---modeling-underground-walls-and-ground-floors-defined-with-c-and-f-factors-for-building-energy-code-compliance}
+
+Building energy code and standards like ASHRAE 90.1, 90.2 and California Title 24 require the underground wall constructions and slabs-on-grade or underground floors not to exceed certain maximum values of C-factor and F-factor, which do not specify detailed layer-by-layer materials for the constructions.
+
+A simplified approach is introduced to create equivalent constructions and model the ground heat transfer through underground walls and ground floors for the building energy code compliance calculations. The approach is to create constructions based on the user defined C or F factor with two layers: one concrete layer (0.15 m thick) with thermal mass, and one fictitious insulation layer with no thermal mass. Three new objects were created for such purpose: \textbf{Construction:CfactorUndergroundWall}, \textbf{Construction:FfactorGroundFloor}, and \textbf{Site:GroundTemperature:FCfactorMethod}. Details of the approach are described in the Engineering Reference document. The wall and floor construction objects are described in this section; the ground temperature object is described with the other ground temperature objects.
+
+When a underground wall or ground floor surface (BuildingSurface:Detailed, Floor:Detailed, and Wall:Detailed) references one of the two construction objects, its field `Outside Boundary Condition' needs to be set to GroundFCfactorMethod. For simple (rectangular) wall and floor objects, the outside boundary condition is inferred from the construction type.
+
+The Site:GroundTemperature:FCfactorMethod is described in the section for ground temperatures, the following section describes the two new construction objects.
+
+\subsection{Construction:CfactorUndergroundWall}\label{constructioncfactorundergroundwall}
+
+This input object differs from the usual wall construction object in that it describes an entire construction rather than individual layers. This object is used when only the wall height (depth to the ground) and the C-factor are available.~ This object accesses a model that creates an equivalent layer-by-layer construction for the underground wall to approximate the heat transfer through the wall considering the thermal mass of the earth soil.
+
+This object is referenced by underground wall surfaces with their fields `Outside Boundary Condition' set to GroundFCfactorMethod.
+
+\subsubsection{Inputs}\label{inputs-36}
+
+\paragraph{Field: Name}\label{field-name-29-000}
+
+The name of the underground wall construction.
+
+\paragraph{Field: C-Factor}\label{field-c-factor}
+
+C-Factor is the time rate of steady-state heat flow through unit area of the construction, induced by a unit temperature difference between the body surfaces. The C-Factor unit is W/m\(^{2}\)·K. The C-factor does not include soil or air films. ASHRAE Standard 90.1 and California Title 24 specify maximum C-factors for underground walls depending on space types and climate zones.
+
+\paragraph{Field: Height}\label{field-height}
+
+This field describes the height of the underground wall, i.e.~the depth to the ground surface. The unit is meters.
+
+IDF Example:
+
+\begin{lstlisting}
+
+Construction:CfactorUndergroundWall,
+      CfactorUGWall,
+      0.436,           ! C-factor (W/m2K), does not include soil or air films
+      4.57;            ! Height (m)
+
+
+    BuildingSurface:Detailed,
+      Zn001:Wall001,           !- Name
+      Wall,                    !- Surface Type
+      CfactorUGWall,           !- Construction Name
+      ZONE ONE,                !- Zone Name
+      GroundFCfactorMethod,    !- Outside Boundary Condition
+      ,                        !- Outside Boundary Condition Object
+      NoSun,                   !- Sun Exposure
+      NoWind,                  !- Wind Exposure
+      0.0,                     !- View Factor to Ground
+      4,                       !- Number of Vertices
+      0.0,0.0,4.572,           !- X,Y,Z = = > Vertex 1
+      0.0,0.0,0.0,             !- X,Y,Z = = > Vertex 2
+      15.24,0.0,0.0,           !- X,Y,Z = = > Vertex 3
+      15.24,0.0,4.572;         !- X,Y,Z = = > Vertex 4
+\end{lstlisting}
+
+\subsection{Construction:FfactorGroundFloor}\label{constructionffactorgroundfloor}
+
+This input object differs from the usual ground floor construction object in that it describes an entire construction rather than individual layers. This object is used when only the floor area, exposed perimeter, and the F-factor are available.~ This object accesses a model that creates an equivalent layer-by-layer construction for the slab-on-grade or underground floor to approximate the heat transfer through the floor considering the thermal mass of the earth soil.
+
+This object is referenced by slab-on-grade or underground floor surfaces with their fields `Outside Boundary Condition' set to GroundFCfactorMethod.
+
+\subsubsection{Inputs}\label{inputs-37}
+
+\paragraph{Field: Name}\label{field-name-30-000}
+
+The name of the ground floor construction.
+
+\paragraph{Field: F-Factor}\label{field-f-factor}
+
+F-Factor represents the heat transfer through the floor, induced by a unit temperature difference between the outside and inside air temperature, on the per linear length of the exposed perimeter of the floor. The unit for this input is W/m·K. ASHRAE Standard 90.1 and California Title 24 specify maximum F-factors for slab-on-grade or underground floors depending on space types and climate zones.
+
+\paragraph{Field: Area}\label{field-area}
+
+This field describes the area (in square meters) of the slab-on-grade or underground floor.
+
+\paragraph{Field: PerimeterExposed}\label{field-perimeterexposed}
+
+This field describes the exposed (direct contact with ambient air) perimeter (in meters) of the slab-on-grade or underground floor.
+
+IDF Example:
+
+\begin{lstlisting}
+
+Construction:FfactorGroundFloor,
+      slabconst,
+      0.12,     !F-factor in W/m-K
+      232.26,   !Area in m2
+      61.0;     !Exposed perimeter in m
+
+
+    BuildingSurface:Detailed,
+      Zn001:Flr001,            !- Name
+      Floor,                   !- Surface Type
+      slabconst,               !- Construction Name, FLOOR
+      ZONE ONE,                !- Zone Name
+      GroundFCfactorMethod,    !- Outside Boundary Condition, Surface
+      ,                        !- Outside Boundary Condition Object, Zn001:Flr001
+      NoSun,                   !- Sun Exposure
+      NoWind,                  !- Wind Exposure
+      0,                       !- View Factor to Ground
+      4,                       !- Number of Vertices
+      15.24,0.0,0.0,           !- X,Y,Z = = > Vertex 1
+      0.0,0.0,0.0,             !- X,Y,Z = = > Vertex 2
+      0.0,15.240,0.0,          !- X,Y,Z = = > Vertex 3
+      15.24,15.24,0.0;         !- X,Y,Z = = > Vertex 4
+\end{lstlisting}
+
+\subsection{Construction:InternalSource}\label{constructioninternalsource}
+
+In some cases such as radiant systems, a construction will actually have resistance wires or hydronic tubing embedded within the construction. Heat is then either added or removed from this building element to provide heating or cooling to the zone in question. In the case of building-integrated photovoltaics, the energy removed in the form of electricity will form a sink. It is possible to enter such constructions into EnergyPlus with the syntax described below. The definition is similar to the Construction definition with a few additions related to radiant or other systems that will lead to source/sink terms. The internal source capability is available with both the \textbf{ConductionTransferFunction} and \textbf{ConductionFiniteDifference} solution algorithms.~ The only difference is that the two dimensional pipe arrangements are not available to ConductionFiniteDifference. Those fields are ignored in that implementation.
+
+\subsubsection{Inputs}\label{inputs-38}
+
+\paragraph{Field: Name}\label{field-name-31-000}
+
+This field is a user specified name that will be used as a reference by other input syntax. For example, a heat transfer surface (ref: Building Surfaces) requires a construction name to define what the make-up of the wall is.
+
+\paragraph{Field: Source Present After Layer Number}\label{field-source-present-after-layer-number}
+
+This field is an integer that relates the location of the heat source or sink. The integer refers to the list of material layers that follow later in the syntax and determines the layer after which the source is present. If a source is embedded within a single homogenous layer (such as concrete), that layer should be split into two layers and the source added between them. For example, a value of ``2'' in this field tells EnergyPlus that the source is located between the second and third material layers listed later in the construction description (see layer fields below).
+
+\paragraph{Field: Temperature Calculation Requested After Layer Number}\label{field-temperature-calculation-requested-after-layer-number}
+
+The nature of this field is similar to the source interface parameter (see previous field) in that it is an integer, refers to the list of material layers that follow, and defines a location after the layer number identified by the user-defined number. In this case, the user is specifying the location for a separate temperature calculation rather than the location of the heat source/sink. This feature is intended to allow users to calculate a temperature within the construction. This might be important in a radiant cooling system where condensation could be a problem. This temperature calculation can assist users in making that determination in absence of a full heat and mass balance calculation.
+
+\paragraph{Field: Dimensions for the CTF Calculation}\label{field-dimensions-for-the-ctf-calculation}
+
+This field is also an integer and refers to the detail level of the calculation. A value of ``1'' states that the user is only interested in a one-dimensional calculation. This is appropriate for electric resistance heating and for hydronic heating (when boiler/hot water heater performance is not affected by return and supply water temperatures). A value of ``2'' will trigger a two-dimensional solution for this surface only. This may be necessary for hydronic radiant cooling situations since chiller performance is affected by the water temperatures provided.
+
+A few things should be noted about requesting two-dimensional solutions. First, the calculation of the conduction transfer functions (CTF) is fairly intensive and will require a significant amount of computing time. Second, the solution regime is two-dimensional internally but it has a one-dimensional boundary condition imposed at the inside and outside surface (i.e., surface temperatures are still isothermal is if the surface was one-dimensional).
+
+\paragraph{Field: Tube Spacing}\label{field-tube-spacing}
+
+This field defines how far apart in meters the hydronic tubing or electrical resistance wires are spaced in the direction perpendicular to the main direction of heat transfer. Note that this parameter is only used for two-dimensional solutions (see previous field).
+
+\paragraph{Field: Outside Layer}\label{field-outside-layer-1}
+
+Each construction must have at least one layer. This field defines the material name associated with the layer on the outside of this construction---outside referring to the side that is not exposed to the zone but rather the opposite side environment, whether this is the outdoor environment or another zone. Material layers are defined based on their thermal properties elsewhere in the input file (ref: Material and Material Properties and Zone,Average,HAMT Surface Average Water Content Ratio {[}kg/kg{]}
+
+Zone,Average,HAMT Surface Inside Face Temperature {[}C{]}
+
+Zone,Average,HAMT Surface Inside Face Relative Humidity {[}\%{]}
+
+Zone,Average,HAMT Surface Inside Face Vapor Pressure {[}Pa{]}
+
+Zone,Average,HAMT Surface Outside Face Temperature {[}C{]}
+
+Zone,Average,HAMT Surface Outside Face Relative Humidity {[}\%{]}
+
+Zone,Average,HAMT Surface Inside Face Relative Humidity {[}\%{]}
+
+\paragraph{HAMT Surface Average Water Content Ratio {[}kg/kg{]}}\label{hamt-surface-average-water-content-ratio-kgkg-2}
+
+This output is the summed water content {[}kg/kg{]} of all cells in a surface expressed as a fraction of the mass of the water to the material mass.
+
+\paragraph{HAMT Surface Inside Face Temperature {[}C{]}}\label{hamt-surface-inside-face-temperature-c-2}
+
+This output is the temperature {[}C{]} on the internal ``surface'' of the surface.
+
+\paragraph{HAMT Surface Inside Face Relative Humidity {[}\%{]}}\label{hamt-surface-inside-face-relative-humidity-4}
+
+\paragraph{HAMT Surface Inside Face Relative Humidity {[}\%{]}}\label{hamt-surface-inside-face-relative-humidity-5}
+
+This output is the relative humidity on the internal ``surface'' of the surface expressed as a percentage.
+
+\paragraph{HAMT Surface Inside Face Vapor Pressure {[}Pa{]}}\label{hamt-surface-inside-face-vapor-pressure-pa-2}
+
+This output is the vapor pressure {[}Pa{]} on the internal ``surface'' of the surface.
+
+\paragraph{HAMT Surface Outside Face Temperature {[}C{]}}\label{hamt-surface-outside-face-temperature-c-2}
+
+This output is the temperature on the external ``surface'' of the surface.
+
+\paragraph{HAMT Surface Outside Face Relative Humidity {[}\%{]}}\label{hamt-surface-outside-face-relative-humidity-2}
+
+This output is the relative humidity on the external ``surface'' of the surface.
+
+Zone,Average,HAMT Surface Temperature Cell N {[}C{]}
+
+Zone,Average,HAMT Surface Water Content Cell N {[}kg/kg{]}
+
+Zone,Average,HAMT Surface Relative Humidity Cell N {[}\%{]}
+
+Detailed profile data for the variables Temperature {[}C{]}, Relative Humidity {[}\%{]} and Water Content {[}kg/kg{]} within each surface can also be reported. To calculate the heat and moisture transfer through surfaces HAMT splits up surfaces into discrete cells. Each cell is composed of a single material and has a position within the surface. HAMT automatically assigns cells to construction objects so that there are more cells closer to boundaries between materials and also at the ``surfaces'' of the surface. It is not possible for users to define their own cells.
+
+\paragraph{HAMT Surface Relative Humidity Cell \textless{}N\textgreater{} {[}\%{]}}\label{hamt-surface-relative-humidity-cell-n-2}
+
+This is the relative humidity of the cell in the surface.
+
+\paragraph{HAMT Surface Temperature Cell \textless{}N\textgreater{} {[}C{]}}\label{hamt-surface-temperature-cell-n-c-2}
+
+This is the temperature of the cell in the surface.
+
+\paragraph{HAMT Surface Water Content Cell \textless{}N\textgreater{} {[}kg/kg{]}}\label{hamt-surface-water-content-cell-n-kgkg-2}
+
+This is the relative water content of the cell in the surface.
+
+Each surface is made from a particular construction. The construction-surface relationship is output by HAMT to the eplusout.eio file with the following format.
+
+! \textless{}HAMT cells\textgreater{}, Surface Name, Construction Name, Cell Numbers
+
+! \textless{}HAMT origins\textgreater{}, Surface Name, Construction Name, Cell origins (m)
+
+The output also contains the HAMT cell origins and cell number for each construction -- surface combination. The coordinate system origin is defined as the exterior surface of the construction. Users can select any one of the Temperature, Relative Humidity or Water Content variables for any cell to be reported, using the following naming scheme for the output variable.
+
+HAMT Profile Construction \textless{}Variable\textgreater{} Cell \textless{}Cell\#\textgreater{}
+
+It is better to specify the ``key'' or Surface Name in this output.
+
+So for example to output the temperature of the 10\(^{th}\) cell in a surface, eg ``East Wall'' would require the following output variable.
+
+\begin{lstlisting}
+
+Output:Variable,
+      East Wall,               !- Key Value
+      HAMT Profile Construction Temperature Cell 10,  !- Variable Name
+      Hourly;                  !- Reporting Frequency
+\end{lstlisting}
+
+By selecting a whole range of these reports and using the information in the eplusout.eio file it is possible to build up a temperature profile of the surface.
+
+Materials for Glass Windows and Doors). As noted above, the outside layer should NOT be a film coefficient since EnergyPlus will calculate convection and radiation heat transfer more precisely.
+
+\paragraph{Field(s) 2-10: Layers}\label{fields-2-10-layers-1}
+
+The next fields are optional and the number of them showing up in a particular Construction definition depends solely on the number of material layers present in that particular construction. The data expected is identical to the outside layer field (see previous field description). The order of the remaining layers is important and should be listed in order of occurrence from the one just inside the outside layer until the inside layer is reached. As noted above, the inside layer should NOT be a film coefficient since EnergyPlus will calculate convection and radiation heat transfer more precisely.
+
+\subsection{Composite Wall Constructions}\label{composite-wall-constructions}
+
+Standard constructions in EnergyPlus are built with the materials and layers described earlier. However, some configurations will not be adequately represented by using this approach. The Reference Data Set CompositeWallConstructions.idf contains constructions and associated materials for a set of \textbf{composite} walls. These are walls---such as stud walls---that have complicated heat-flow paths so that the conduction is two- or three-dimensional. Thermal bridges are one of the common terms for these complicated heat-flow paths; this dataset will help you represent these in EnergyPlus.
+
+The materials here are \textbf{not} real materials but are ``equivalent'' materials obtained from finite-difference modeling. (The thickness, conductivity, density and specific heat values of the material layers for the different constructions have been taken from the ASHRAE report ``Modeling Two- and Three-Dimensional Heat Transfer through Composite Wall and Roof Assemblies in Hourly Energy Simulation Programs (1145-TRP),'' by Enermodal Engineering Limited, Oak Ridge National Laboratory, and the Polish Academy of Sciences, January 2001.). EnergyPlus will calculate conduction transfer functions using these materials. The heat transfer based on these conduction transfer functions will then be very close to what would be calculated with a two- or three-dimensional heat transfer calculation.
+
+For stud walls, using these composite constructions will give more accurate heat flow than you would get by manually dividing the wall into a stud section and a non-stud section.
+
+If your wall's exterior or interior roughness or thermal, solar or visible absorptances are different from those in the data set, you can make the appropriate changes to the first material (the outside layer) or the third material (the inside layer). \textbf{None of the other values should be changed.}
+
+\begin{callout}
+Complete description of the CompositeWallConstructions data set are found in the OutputDetailsAndExamples document.
+\end{callout}
+
+\subsection{Construction:ComplexFenestrationState}\label{constructioncomplexfenestrationstate}
+
+This input object is used to describe the properties of a single state for complex fenestration.~ There are two parts to the input, 1) layer-by-layer physical description of fenestration system and 2) a set of matrices that describe overall system optical performance.~ Each layer also has associated with it two matrices that give the layer absorptance (for front and back incidence on the system.
+
+The optical properties are given as a two-dimensional matrix describing the basis and four two-dimensional matrices of system bidirectional optical properties.
+
+These input objects will generally be exported directly from the WINDOW program and it is expected that users usually will not develop the input themselves. However, this is an option for users who prefer to use a different method (e.g., Monte-Carlo ray-trace or measurement) of determining optical properties.
+
+Multiple instances of this object are used to define the separate operating states of complex fenestration.~ For example, blinds could be deployed or redirected to create a new state, or electrochromic glazings could change transmittance.~ Each separate state defines the materials present and the overall optical performance.~ If the glazing system has only one state, then only one of these objects is needed.
+
+If there is more than one complex fenestration state, it will be controlled using the EMS actuator called ``Surface'' with the control type ``Construction State'' and the EMS input object called EnergyManagementSystem:ConstructionIndexVariable.
+
+\subsubsection{Inputs}\label{inputs-39}
+
+\paragraph{Field: Name}\label{field-name-32-000}
+
+Unique name of this construction.~ Used to identify type of window in surface objects.
+
+\paragraph{Field: Basis Type keyword}\label{field-basis-type-keyword}
+
+Only value currently implemented is ``LBNLWINDOW''. More options may be added in the future.
+
+\paragraph{Field: Basis Symmetry, keyword}\label{field-basis-symmetry-keyword}
+
+Only value currently implemented is ``None''. More options will be added in the future.
+
+\paragraph{Field: Thermal Parameters}\label{field-thermal-parameters}
+
+This field gives the name of WindowThermalModel:Params object used to keep common data necessary for thermal simulation.
+
+\paragraph{Field: Basis Matrix Name}\label{field-basis-matrix-name}
+
+This field gives the name of an 2 x N matrix object that defines the basis~ For a fenestration basis, N would be the number of theta (polar angle) values, the first of the two elements for each of the i = 1,..,N would be the theta value, and the second would be the number of phi (azimuthal angle) values that 360º is divided into for that theta.
+
+\paragraph{Field: Solar Optical Complex Front Transmittance Matrix Name}\label{field-solar-optical-complex-front-transmittance-matrix-name}
+
+This field contains the name of matrix object that describes the solar transmittance at different incident angles.~ This is from the outside toward the inside.
+
+\paragraph{Field: Solar Optical Complex Back Reflectance Matrix Name}\label{field-solar-optical-complex-back-reflectance-matrix-name}
+
+This field contains the name of matrix object that describes the solar back reflectance at different incident angles.~ This is from the inside toward the outside.
+
+\paragraph{Field: Visible Optical Complex Front Transmittance Matrix Name}\label{field-visible-optical-complex-front-transmittance-matrix-name}
+
+This field contains the name of matrix object that describes the visible transmittance at different incident angles.~ This is from the outside toward the inside.
+
+\paragraph{Field: Visible Optical Complex Back Reflectance Matrix Name}\label{field-visible-optical-complex-back-reflectance-matrix-name}
+
+This field contains the name of vector object that describes the visible back reflectance at different incident angles.~ This is from the inside toward the outside.
+
+\paragraph{Field: Outside Layer \textless{}x = 1\textgreater{}}\label{field-outside-layer-x-1}
+
+Each construction must have at least one layer. The layer order is from outside to inside, with the first layer being either WindowMaterial:Glazing or WindowMaterial:ComplexShade. The next layer is a WindowMaterial:Gap layer, and the following layers then alternate between WindowMaterial:Glazing or WindowMaterial:ComplexShade and WindowMaterial:Gap. The last layer cannot be WindowMaterial:Gap.
+
+\paragraph{Field: Outside Layer Directional Front Absorptance Matrix Name}\label{field-outside-layer-directional-front-absorptance-matrix-name}
+
+Points to an Nbasis x 1 matrix object.
+
+\paragraph{Field: Outside Layer Directional Back Absorptance Matrix Name}\label{field-outside-layer-directional-back-absorptance-matrix-name}
+
+Points to an Nbasis x 1 matrix object.
+
+\paragraph{Above 3 fields are optionally repeated for layers 2-10}\label{above-3-fields-are-optionally-repeated-for-layers-2-10}
+
+These layers include gaps, which do not need to have matrix data specified.
+
+An IDF example of complex fenestration with single layer:
+
+\begin{lstlisting}
+
+Construction:ComplexFenestrationState,       !- single layer example
+    CFS_Glz_1,                 !- name
+    LBNLWindow,                !- basis type
+    None,                      !- basis symmetry type
+    ThermParam_1,              !- window thermal model
+    CFS_Glz_1_Basis,           !- basis matrix name
+    CFS_Glz_1_TfSol,           !- Tfsol
+    CFS_Glz_1_RbSol,           !- Rbsol
+    CFS_Glz_1_Tfvis,           !- Tfvis
+    CFS_Glz_1_Tbvis,           !- Tbvis
+    Glass_102_Layer,           !- layer 1 name
+    CFS_Glz_1_Layer_1_fAbs,    !- fAbs
+    CFS_Glz_1_Layer_1_bAbs;    !- bAbs
+\end{lstlisting}
+
+An complex fenestration IDF example with double layer (first layer is shading device):
+
+\begin{lstlisting}
+
+Construction:ComplexFenestrationState,       !- double layer example
+    CFS_Glz_59,                    !- name
+    LBNLWindow,                    !- basis type
+    None,                          !- basis symmetry type
+    ThermParam_59,                 !- window thermal model
+    CFS_Glz_59_Basis,              !- basis matrix name
+    CFS_Glz_59_TfSol,              !- Tfsol
+    CFS_Glz_59_RbSol,              !- Rbsol
+    CFS_Glz_59_Tfvis,              !- Tfvis
+    CFS_Glz_59_Tbvis,              !- Tbvis
+    Shade_30001_Layer,             !- layer 1 name (shading device)
+    CFS_Glz_59_Layer_1_fAbs,       !- fAbs
+    CFS_Glz_59_Layer_1_bAbs,       !- bAbs
+    Gap_1_Layer,                   !- layer 1 name
+    ,                 !- absorptance matrices for gaps should be empty for now
+    ,                              !- it is for future use
+    Glass_3110_Layer,              !- layer 2 name
+    CFS_Glz_59_Layer_3110_fAbs,    !- fAbs
+    CFS_Glz_59_Layer_3110_bAbs;    !- bAbs
+\end{lstlisting}
+
+\subsection{WindowThermalModel:Params}\label{windowthermalmodelparams}
+
+This input object is used with the Construction:ComplexFenestrationState
+
+\subsubsection{Inputs}\label{inputs-40}
+
+\paragraph{Field: Name}\label{field-name-33-000}
+
+Unique name of the window thermal model parameters.
+
+\paragraph{Field: Calculation Standard}\label{field-calculation-standard}
+
+The type of the calculation standard.~ The choices are:
+
+\begin{itemize}
+\item
+  ISO15099
+\item
+  EN673Declared
+\item
+  EN673Design
+\end{itemize}
+
+The default is ISO15099.
+
+\paragraph{Field: Thermal Model}\label{field-thermal-model}
+
+The type of thermal model.~ The choices are:
+
+\begin{itemize}
+\item
+  ISO15099
+\item
+  ScaledCavityWidth
+\item
+  ConvectiveScalarModel\_NoSDThickness
+\item
+  ConvectiveScalarModel\_withSDThickness
+\end{itemize}
+
+The default is ISO15099.
+
+\paragraph{Field: SD Scalar}\label{field-sd-scalar}
+
+Shading Device Scalar Factor. Only used for~ Thermal Model = Convective Scalar Model.~ Factor of venetian shading device layer contribution to convection. Real value between 0 (where the shading device contribution to convection is neglected) and 1 (where the shading device treated as ``closed'' -- as if it is a glass layer with thermal properties of SD slat material). Default: 1.0
+
+\paragraph{Field: Deflection Model}\label{field-deflection-model}
+
+The type of deflection model used to model deflection in windows and glass.~ The choices are:
+
+\begin{itemize}
+\item
+  NoDeflection
+\item
+  TemperatureAndPressureInput
+\item
+  MeasuredDeflection
+\end{itemize}
+
+The default is NoDeflection.
+
+\paragraph{Field: Vacuum Pressure Limit}\label{field-vacuum-pressure-limit}
+
+The pressure (Pa) which will be considered to be the limit for vacuum glazing pressure.~ All pressures less than or equal to this pressure will be considered to be vacuum. Default: 13.238 Pa.
+
+\paragraph{Field: Initial Temperature}\label{field-initial-temperature}
+
+The temperature (\(^{o}\)C) of the gap in the time of fabrication.~ It is used only when WindowThermalModel:Params DeflectionModel = TemperatureAndPressureInput
+
+\paragraph{Field: Initial Pressure}\label{field-initial-pressure}
+
+The pressure (Pa) of the gap at the time of fabrication of the sealed glazing system unitIt is used only when WindowThermalModel:Params DeflectionModel = TemperatureAndPressureInput.
+
+An IDF example for WindowThermalModel:Params (without deflection):
+
+\begin{lstlisting}
+
+WindowThermalModel:Params,
+    ThermParam_59,                   !- name
+    ISO15099,                        !- standard
+    ISO15099,                        !- thermal model standard
+    1.00,                            !- SD scalar
+    NoDeflection;                    !- deflection model
+\end{lstlisting}
+
+An IDF example for thermal paramters (with deflection):
+
+\begin{lstlisting}
+
+WindowThermalModel:Params,
+    ThermParam_59,                   !- name
+    ISO15099,                        !- standard
+    ISO15099,                        !- thermal model standard
+    1.00,                            !- SD scalar
+    TemperatureAndPressureInput,     !- deflection model
+    ,                                !- vacuum pressure limit
+    21.00,                           !- temperature at time of fabrication
+    10000.00;                        !- pressure at time of fabrication
+\end{lstlisting}
+
+An IDF example for WindowThermalModel:Params for modeling vacuum glazing
+
+\begin{lstlisting}
+
+WindowThermalModel:Params,
+  ThermParam_1006,                                    !- name
+  ISO15099,                                           !- standard
+  ISO15099,                                           !- thermal model
+  1.0000,                                             !- SDScalar
+  NoDeflection,                                       !- deflection model
+  13.238;                                             !- vacuum pressure limit
+\end{lstlisting}
+
+\subsection{Matix:TwoDimension}\label{matixtwodimension}
+
+This is input object is only used with Construction:ComplexFenestrationState object to enter a two-dimensional matrix of values.
+
+It is used to define the Basis Matrix for BSDF input data, and is also used to define the actual BSDF matrices data for the complete fenestration definition as well as the individual layers of the system.
+
+The data are entered in row-major order: all the elements of row 1, followed by all the elements of row 2, etc.~ The number of values to be entered depends on the number of rows and the number of columns.~ Blank fields are treated as having been set to zero.
+
+See example IDF file ``SmOff\_ CmplxGlz\_IntExtShading.idf'' for the definition of two complex shading layers with matrix data defined.
+
+\subsubsection{Field: Name}\label{field-name-34-000}
+
+Unique name of matrix input object.
+
+\subsubsection{Field: Number of Rows}\label{field-number-of-rows}
+
+This field is the number of rows in the matrix.
+
+\subsubsection{Field: Number of Columns}\label{field-number-of-columns}
+
+This field is the number of columns in the matrix
+
+\subsubsection{\textless{} Field Set: Value \# N \textgreater{}}\label{field-set-value-n}
+
+Repeat entering value exactly the same number of times as the number of rows times the number of columns.
+
+\subsubsection{Field: Value \# 1}\label{field-value-1-000}
+
+This is the value of the matrix at the first row and first column.
+
+\subsubsection{Field: Value \#2}\label{field-value-2}
+
+This is the value of the matrix at the first row and the second column.
+
+An IDF example of matrix for defining BSDF basis:
+
+\begin{lstlisting}
+
+Matrix:TwoDimension,       !- matrix for basis definition
+    CFS_Glz_1_Basis,         !- basis matrix name
+    9,                       !- number of rows
+    2,                       !- number of colums
+    0.00000, 1.00000,
+    10.00000, 8.00000,
+    20.00000, 16.00000,
+    30.00000, 20.00000,
+    40.00000, 24.00000,
+    50.00000, 24.00000,
+    60.00000, 24.00000,
+    70.00000, 16.00000,
+    82.50000, 12.00000;
+\end{lstlisting}
+
+\subsection{Construction:WindowEquivalentLayer}\label{constructionwindowequivalentlayer}
+
+This object defines the construction for equivalent layer window (ASHWAT) model. This window can model various mix of glazing and shading layers combination. Shadings are defined as an integral part of the construction. The construction is defined by listing the layers name starting with outside layer and work your way to the inside Layer. Up to six solid layers (glazing and shade) and up to five gaps, i.e., a total of up to 11 layers maximum are allowed in equivalent layer window object. The solid layer types allowed are: Glazing, Insect Screen, Roller Blinds, Venetian Blind, and Drape Fabrics. This window model requires optical data of the individual glazing and shading layers to calculate the effective optical properties of the composite fenestration construction. Venetian blinds in equivalent layer window model can be in a fixed slat angle or has the option to control the slat angle in order to maximize visibility, or maximize solar gains. An equivalent-layer concept can simulate wide range of multiple glazing and shading layers combination and provides unlimited flexibility to combine different types of shading layers in a fenestration. For the gap layer object any one of the five different Gas types can be specified: AIR, ARGON, XENON, KRYPTON, or CUSTOM.This window object is referenced by fenestration surfaces. For details of the model description refer to Equivalent Layer Fenestration Model section in Engineering Reference. The various layer objects that can be referenced in Equivalent Layer window model are:
+
+\begin{lstlisting}
+WindowMaterial:Glass:EquivalentLayer
+WindowMaterial:Shade:EquivalentLayer
+WindowMaterial:Drape:EquivalentLayer
+WindowMaterial:Blind:EquivalentLayer
+WindowMaterial:Screen:EquivalentLayer
+WindowMaterial:Gap:EquivalentLayer
+\end{lstlisting}
+
+\subsubsection{Inputs}\label{inputs-41}
+
+\paragraph{Field: Name}\label{field-name-35}
+
+This field is a user specified name that will be used as a reference by other input syntax. For example, a heat transfer surface (ref: Fenestration) requires a construction name to define what the make-up of the fenestration is. This name must be identical to one of the Window Construction Equivalent Layer definitions in the input data file.
+
+\paragraph{Field: Outside Layer}\label{field-outside-layer-2}
+
+Each equivalent layer window construction must have at least one layer. This field defines the material name associated with the layer on the outside of the construction---outside referring to the side that is exposed to the outdoor environment or another zone. Material layers for equivalent layer window model are defined based on their thermal properties elsewhere in the input file (ref: WindowEquivalentLayerMaterialNames)
+
+\paragraph{Field: Layer 2 - Layer11}\label{field-layer-2---layer11}
+
+The next fields are optional and the number of them showing up in a particular equivalent layer window construction definition depends solely on the number of material layers present in that construction. The data expected is identical to the outside layer field (see previous field description). The order of the remaining layers is important and should be listed in order of occurrence from the one just inside the outside layer until the inside layer is reached. As noted above, the inside layer should NOT be a film coefficient since EnergyPlus will calculate inside convection and radiation heat transfer more precisely.
+
+An IDF example for this object, is shown below:
+
+\begin{lstlisting}
+
+Construction:WindowEquivalentLayer,
+    Six Solid Layers Window,   !- Name
+    INSCRN,                    !- Outside Layer
+    Air GAP Outdoor 12.7mm,    !- Layer 2
+    GLZGRY,                    !- Layer 3
+    Argon GAP Sealed 12.7mm,   !- Layer 4
+    FEP,                       !- Layer 5
+    Xenon GAP Sealed 12.7mm,   !- Layer 6
+    LOF1436,                   !- Layer 7
+    Krypton GAP Sealed 12.7mm, !- Layer 8
+    GLZCLR,                    !- Layer 9
+    Air GAP Indoor 12.7mm,     !- Layer 10
+    ShadeTrns;                 !- Layer 11
+\end{lstlisting}
+
+\subsection{Construction:WindowDataFile}\label{constructionwindowdatafile}
+
+The WINDOW program, which does a thermal and optical analysis of a window under different design conditions, writes a data file (``Window data file'') containing a description of the window that was analyzed. The Construction:WindowDataFile object allows a window to be read in from the WINDOW data file---see ``Importing Windows from WINDOW.'' For information on adding a shading device to the window see ``WindowProperty:ShadingControl.''
+
+\subsubsection{Inputs}\label{inputs-42}
+
+\paragraph{Field: Name}\label{field-name-36}
+
+This is the name of a window on the Window data file. An error will result if EnergyPlus cannot find a window of this name on the file, or if the file, shown in the next field, is not present. The location of the data file should be specified in the File Name field. For details on what is done with the data if a matching window is found on the file see ``Importing Windows from WINDOW.''
+
+\paragraph{Field: File Name}\label{field-file-name-000}
+
+This is the file name of the Window data file that contains the Window referenced in the previous field. The field may include a full path with file name, for precise results. The field must be \textless{} = 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
+
+If this field is left blank, the file name is defaulted to Window5DataFile.dat.
+
+Input Example
+
+\begin{lstlisting}
+Construction:WindowDataFile,
+  DoubleClear;            !- Name of a Window on the Window Data File
+  ! Note -- Window5DataFile.dat is presumed to be in the "run" folder where EnergyPlus.exe is
+
+FenestrationSurface:Detailed,
+  Zn001:Wall001:Win001, !- Name
+  Window,               !- Class
+  DoubleClear,          !- Construction Name
+  Zn001:Wall001,        !- Base Surface Name, and Target (if applicable)
+  0.5,                  !- View Factor to Ground
+  ,                     !- Window Shading Control name
+  ,                     !- Frame/Divider name
+   1.0,                 !- Multiplier
+  4,                    !- Number of vertices
+  0.548, 0.0, 2.5000,   !- X,Y,Z of Vertices
+  0.548, 0.0, 0.5000,
+  5.548, 0.0, 0.5000,
+  5.548, 0.0, 2.5000;
+\end{lstlisting}
+
+An example showing use of specific data file name and complete path location follows:
+
+\begin{lstlisting}
+Construction:WindowDataFile,
+  DoubleClear,          !- Name of a Window on the Window Data File
+  C:\EnergyPlusData\DataSets\MyWindow.dat;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-016}
+
+An optional report (contained in \textbf{eplusout.eio}) gives calculational elements for the materials and constructions used in the input. These reports are explained fully in the Output Details and Examples document.
diff --git a/doc/input-output-reference/src/overview/group-system-availability-managers.tex b/doc/input-output-reference/src/overview/group-system-availability-managers.tex
new file mode 100644
index 00000000000..9f4a9d561a9
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-system-availability-managers.tex
@@ -0,0 +1,692 @@
+\section{Group System Availability Managers}\label{group-system-availability-managers}
+
+System Availability Managers are one of the high-level control constructs in EnergyPlus. A System Availability Manager is able to access data from any of the HVAC system nodes and use this data to to make a decision on whether an entire AirLoopHVAC or PlantLoop should be on or off. Some of the zone component objects (e.g.~unit heater, unit ventilator, packaged terminal air conditioner, packaged terminal heat pump, zone water source heat pump,window air conditioner, zone terminal unit (variable refrigerant flow), energy recovery ventilator, outdoor air unit, fan coil unit, and ventilated slab) can also individually use availability managers to make a decision regarding whether their fan should be on or off.
+
+System Availability Managers are executed at the start of each HVAC timestep. They reside outside the HVAC system iteration loops. Thus, the System Availability Managers are executed once per HVAC timestep, and they use previous timestep information (except for zone load) to calculate their set points.
+
+Some of the managers monitor the temperature at an air or plant node to determine whether the system should be on or off. If the system is to be controlled on the outdoor dry-bulb temperature, an OutdoorAir:NodeList object can be used to define a node which will have the current outdoor air conditions.
+
+The output from each System Availability Manager is an availability status flag. This flag can have the values \emph{NoAction}, \emph{ForceOff}, \emph{CycleOn}, or \emph{CycleOnZoneFansOnly}. The availability status flags for the System Availability Managers referenced by an air or plant loop are used to set the availability status flag for each loop. For the air loops and zone components, \emph{ForceOff} takes precedence: if any of the loop s (or zone component s) availability managers are showing status \emph{ForceOff}, the loop (or zone component fan) status will be \emph{ForceOff}. Next in precedence is \emph{CycleOnZoneFansOnly} (only for air loop), followed by \emph{CycleOn,} and \emph{NoAction}. For the plant loops, there is no precedence among the System Availability Manager status flag values. Instead, the first availability manager giving a status flag value other than \emph{NoAction} sets the status for the loop. The System Availability Managers are executed in AvailabilityManagerAssignmentList order.
+
+The actual action of turning on or off a loop is taken by the loop prime movers: fans for AirLoopHVACs and zone components, and pumps for plant loops. For instance when a fan is deciding whether it is on or off, it checks its on/off schedule and whether the loop availability status flag is \emph{CycleOn} or \emph{ForceOff}. If the schedule is on and the status flag is \emph{ForceOff}, the fan will be off. If the fan schedule says off and the status flag is \emph{CycleOn}, the fan will be on. Thus the availability managers overrule the fan on/off schedule. The availability managers, air loops, and plant loops all have output variables which may be used to verify the action of the loop.
+
+Availability managers for AirLoopHVAC systems also control the availability of zone exhaust fans (Ref. Fan:ZoneExhaust) and terminal unit fans (Ref. AirTerminal:SingleDuct:SeriesPIU: Reheat, AirTerminal:SingleDuct:ParallelPIU:Reheat, and AirTerminal:SingleDuct:VAV: Reheat:VariableSpeedFan) in the zones served by the AirLoopHVAC system.
+
+\subsection{AvailabilityManager:Scheduled}\label{availabilitymanagerscheduled}
+
+The simplest System Availability Manager is when the availability is determined by an on/off schedule.The syntax for implementing such an availability manager is shown below. The identifying name refers back to the name recorded in the AvailabilityManagerAssignmentList statement described in the \textbf{Group Air Distribution} section. The schedule must be the name of a schedule defined elsewhere in the input.
+
+\subsubsection{Inputs}\label{inputs-047}
+
+\paragraph{Field: Name}\label{field-name-046}
+
+The unique, user-assigned name of an instance of a scheduled availability manager. Other objects that use this scheduled availability manager will reference it by this name.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-006}
+
+The name of a schedule defined elsewhere in the input. Schedule values greater than zero (usually 1 is used) indicate that the system is on. Schedule values less than or equal to zero (usually 0 is used) denote that the system is off. This schedule overides the central fan schedule for determining whether the fan is on.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+AvailabilityManager:Scheduled,
+  VAV Sys 1 Avail, !- Name
+  FanAvailSched;     !- Schedule Name
+\end{lstlisting}
+
+AvailabilityManager:Scheduled Outputs
+
+The scheduled availability manager has one output variable.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Availability Manager Scheduled Control Status
+\end{itemize}
+
+\paragraph{Availability Manager Scheduled Control Status}\label{availability-manager-scheduled-control-status}
+
+A value of 1 indicates the manager is signaling \emph{ForceOff}. A value of 2 means the manager is signaling \emph{CycleOn}.
+
+\subsection{AvailabilityManager:ScheduledOn}\label{availabilitymanagerscheduledon}
+
+The Schedule On Availability Manager is used when equipment must be turned on during a given time period. This availability manager will not turn the equipment off, a separate availability manager must be used to disable the equipment as necessary. The scheduled on availability is determined by an on schedule. Schedule values other than 0 set a \emph{CycleOn} availability status. Schedule values equal to 0 set a \emph{NoAction} availability status. The syntax for implementing such an availability manager is shown below. The identifying name refers back to the name recorded in the AvailabilityManagerAssignmentList statement described in the \textbf{Group Air Distribution} section. The schedule must be the name of a schedule defined elsewhere in the input.
+
+\subsubsection{Inputs}\label{inputs-1-044}
+
+\paragraph{Field: Name}\label{field-name-1-043}
+
+The unique, user-assigned name of an instance of a scheduled on availability manager. Other objects that use this scheduled on availability manager will reference it by this name.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-1-003}
+
+The name of a schedule defined elsewhere in the input. Schedule values greater than zero (usually 1 is used) indicate that the system is on. Schedule values less than or equal to zero (usually 0 is used) denote that \emph{NoAction} is desired. This schedule overides the central fan schedule for determining whether the fan is on.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+AvailabilityManager:ScheduledOn,
+  VAV Sys 1 Avail On,   !- Name
+  FanAvailSched;             !- Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-036}
+
+The scheduled on availability manager has one output variable.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Availability Manager Scheduled On Control Status
+\end{itemize}
+
+\paragraph{\texorpdfstring{Availability Manager Scheduled On Control Status {[]}}{Availability Manager Scheduled On Control Status }}\label{availability-manager-scheduled-on-control-status}
+
+A value of 0 indicates the manager is signaling \emph{NoAction}. A value of 2 means the manager is signaling \emph{CycleOn}.
+
+\subsection{AvailabilityManager:ScheduledOff}\label{availabilitymanagerscheduledoff}
+
+The Schedule Off Availability Manager is used when equipment must be turned off during a given time period. This availability manager will not turn the equipment on, a separate availability manager must be used to enable the equipment as necessary. The scheduled off availability is determined by an off schedule. Schedule values equal to 0 set a \emph{ForceOff} availability status. Schedule values other than 0 (usually a 1 is used) set a \emph{NoAction} availability status. The syntax for mplementing such an availability manager is shown below. The identifying name refers back to the name recorded in the AvailabilityManagerAssignmentList statement described in the \textbf{Group Air Distribution} section. The schedule must be the name of a schedule defined elsewhere in the input.
+
+\subsubsection{Inputs}\label{inputs-2-041}
+
+\paragraph{Field: Name}\label{field-name-2-038}
+
+The unique, user-assigned name of an instance of a scheduled off availability manager. Other objects that use this scheduled off availability manager will reference it by this name.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-2-003}
+
+The name of a schedule defined elsewhere in the input. Schedule values equal to zero indicate that the system is off. Schedule values other than (usually 0 is used) denote that \emph{NoAction} is desired.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+AvailabilityManager:ScheduledOff,
+  VAV Sys 1 Avail Off,     !- Name
+  FanAvailSched;                 !- Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-027}
+
+The scheduled off availability manager has one output variable.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Availability Manager Scheduled Off Control Status
+\end{itemize}
+
+\paragraph{\texorpdfstring{Availability Manager Scheduled Off Control Status {[]}}{Availability Manager Scheduled Off Control Status }}\label{availability-manager-scheduled-off-control-status}
+
+A value of 0 indicates the manager is signaling \emph{NoAction}. A value of 1 means the manager is signaling \emph{ForceOff}.
+
+\subsection{AvailabilityManager:NightCycle}\label{availabilitymanagernightcycle}
+
+This manager is used for cycling on an air system when one or more zones become too hot or too cold. The usual situation is that the central air handler is turned off at night. However if the building gets too cold there might be condensation on the walls and other damage. Thus the control system is usually programmed to turn the system on if 1 control thermostat or any thermostat shows a zone temperature of less than a night time set point. Similarly there might be a concern about a building getting too hot. Again the control system is programmed to turn the air handler back on if one or any zone temperature exceeds a night time cooling set point.
+
+This object gives the user considerable flexibility in determining how the night time on/off decision will be made. The manager can look at the temperature in 1 zone or it can sample all the zones connected to the air handler. The user can specify a temperature tolerance and a run time for the system once it switches on. There is also an applicability schedule the user can schedule whether or not this availability manager itself is being applied.
+
+\textbf{\emph{Field: Name}}
+
+A unique, user-assigned name for an instance of a night cycle availability manager. Other objects that use this availability manager will reference it by this name.
+
+\textbf{\emph{Field: Applicability Schedule Name}}
+
+The name of a schedule defined elsewhere in the input file. This schedule determines whether or not for a given time period this availability manager is to be applied. Schedule values greater than zero (usually 1 is used) indicate the availability manager is to be applied. Schedule values less than or equal to zero (usually 0 is used) denote that the availability manager is not used for this time period.
+
+\textbf{\emph{Field: Fan Schedule Name}}
+
+The name of the central fan on/off schedule for the air system that this availability manager will affect.
+
+\textbf{\emph{Field: Control Type}}
+
+The possible inputs are \emph{StayOff}, \emph{CycleOnAny}, \emph{CycleOnControlZone}, \emph{CycleOnAnyZoneFansOnly}. \emph{StayOff} means the availability manager will have no effect air handler on/off will be determined by the fan schedule. \emph{CycleOnAny} means that if any zone served by a system whose AvailabilityManagerAssignmentList references this system availability manager has an air temperature outside the cooling or heating set points the central fan will turn on even though the fan schedule indicates the fan is off. \emph{CycleOnControlZone} means the same thing except the availability manager looks at the temperature in only one zone. \emph{CycleOnAnyZoneFansOnly} is the same as \emph{CycleOnAny} except that only the zone fans are cycled on and the central air handler fan is left off. The default is \emph{StayOff}.
+
+\textbf{\emph{Field: Thermostat Tolerance}}
+
+The Thermostat Tolerance defines the amount by which the zone temperature must fall outside the current zone heating and cooling setpoints for the Night Cycle manager to turn the system on. The zone temperature must exceed the cooling set point or fall below the heating set point by 1/2 the Thermostat Tolerance in order for the availability manager to signal that the system should turn on. The Thermostat Tolerance is specified in degrees Celsius. The default is 1 degree C.
+
+\textbf{\emph{Field: Cycling Run Time}}
+
+The time in seconds for which the system will run after it has cycled on. The default is 3600 seconds (1 hour).
+
+\textbf{\emph{Field: Control Zone Name}}
+
+For the option \emph{CycleOnControlZone} this is the name of the control zone.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+AvailabilityManager:NightCycle,
+  VAV Sys 1 Avail,         ! Name
+  SysAvailApplicSch,     !Applicability Schedule Name
+  FanAvailSched,             ! Fan Schedule Name
+  CycleOnAny,                   ! Control Type
+  4.0,                                 ! Temperature Tolerance {delta C}
+  7200.;                             ! Cycle Run Time {s}
+\end{lstlisting}
+
+\subsubsection{Inputs}\label{inputs-3-037}
+
+\subsubsection{Outputs}\label{outputs-2-022}
+
+The night cycle availability manager has one output variable.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Availability Manager Night Cycle Control Status
+\end{itemize}
+
+\paragraph{Availability Manager Night Cycle Control Status}\label{availability-manager-night-cycle-control-status}
+
+A value of 0 indicates the manager is signaling \emph{NoAction}. A value of 2 means the manager is signaling \emph{CycleOn}. A value of 3 says that the manager is signaling \emph{CycleOnZoneFansOnly}.
+
+\subsection{AvailabilityManager:DifferentialThermostat}\label{availabilitymanagerdifferentialthermostat}
+
+The differential thermostat compares the temperatures at two different system nodes. If the temperature difference (DT) is above the \emph{Temperature Difference On Limit}, the system is turned on. If the DT is below the \emph{Temperature Difference Off Limit}, the system is turned off. Between the \emph{On Limit} and \emph{Off Limit} the system is either on or off depending on the previous state of the thermostat. Unlike other availability managers, the differential thermostat is always either ``On'' or ``Off''; it does not use the ``No Action'' state. Therefore, the differential thermostat must be the last manager in the AvailabilityManagerAssignmentList. Any availability managers after the differential thermostat manager will never be simulated.
+
+One application of the differential thermostat is to ensure a useful heat gain for solar heating systems, i.e.~the system is only turned on when there is a significant temperature difference between the solar collector outlet node and the storage tank outlet node.
+
+\subsubsection{Inputs}\label{inputs-4-034}
+
+\paragraph{Field: Name}\label{field-name-3-032}
+
+The name of the object. This is referenced in the AvailabilityManagerAssignmentList.
+
+\paragraph{Field: Hot Node Name}\label{field-hot-node-name}
+
+The sensor node with the higher temperature.
+
+\paragraph{Field: Cold Node Name}\label{field-cold-node-name}
+
+The sensor node with the colder temperature.
+
+\paragraph{Field: Temperature Difference On Limit}\label{field-temperature-difference-on-limit}
+
+Temperature difference {[}deltaC{]} between hot and cold nodes necessary to turn the system on.
+
+\paragraph{Field: Temperature Difference Off Limit}\label{field-temperature-difference-off-limit}
+
+Temperature difference {[}deltaC{]} between hot and cold nodes necessary to turn the system off. This field defaults to the \emph{Temperature Difference On Limit}.
+
+An example of this object in an IDF is:
+
+\begin{lstlisting}
+
+AvailabilityManager:DifferentialThermostat,
+  Differential Thermostat Availability Manager,   !- Name
+  Collector Outlet Node,                       !- Hot Node Name
+  Water Heater Source Outlet Node,   !- Cold Node Name
+  10.0,   !- Temperature Difference On Limit {delta C}
+  2.0;     !- Temperature Difference Off Limit {delta C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-020}
+
+The differential thermostat availability manager has one output variable.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Availability Manager Differential Thermostat Control Status
+\end{itemize}
+
+\paragraph{Availability Manager Differential Thermostat Control Status}\label{availability-manager-differential-thermostat-control-status}
+
+A value of 1 indicates the manager is signaling \emph{ForceOff}. A value of 2 means the manager is signaling \emph{CycleOn}.
+
+\subsection{AvailabilityManager:HighTemperatureTurnOff}\label{availabilitymanagerhightemperatureturnoff}
+
+This manager turns the system off if the temperature at the sensor node is above the specified setpoint temperature.
+
+\subsubsection{Inputs}\label{inputs-5-031}
+
+\paragraph{Field: Name}\label{field-name-4-029}
+
+The name of the object. This is referenced in the AvailabilityManagerAssignmentList.
+
+\paragraph{Field: Sensor Node Name}\label{field-sensor-node-name-002}
+
+The air or plant node where the temperature is monitored.
+
+\paragraph{Field: Temperature}\label{field-temperature}
+
+The setpoint temperature {[}C{]} at which the system is turned off.
+
+An example of this object in an IDF is:
+
+\begin{lstlisting}
+
+AvailabilityManager:HighTemperatureTurnOff,
+  High Temperature Turn Off Availability Manager,   !- Name
+  Water Heater Use Outlet Node,   !- Sensor Node Name
+  60.0;   !- Temperature {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-017}
+
+The high temperature turn off availability manager has one output variable.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Availability Manager High Temperature Turn Off Control Status
+\end{itemize}
+
+\paragraph{\texorpdfstring{Availability Manager High Temperature Turn Off Control Status {[]}}{Availability Manager High Temperature Turn Off Control Status }}\label{availability-manager-high-temperature-turn-off-control-status}
+
+A value of 0 indicates the manager is signaling \emph{NoAction}. A value of 1 means the manager is signaling \emph{ForceOff.}
+
+\subsection{AvailabilityManager:HighTemperatureTurnOn}\label{availabilitymanagerhightemperatureturnon}
+
+This manager turns the system on if the temperature at the sensor node is above the specified setpoint temperature.
+
+\subsubsection{Inputs}\label{inputs-6-028}
+
+\paragraph{Field: Name}\label{field-name-5-025}
+
+The name of the object. This is referenced in the AvailabilityManagerAssignmentList.
+
+\paragraph{Field: Sensor Node Name}\label{field-sensor-node-name-1-000}
+
+The air or plant node where the temperature is monitored.
+
+\paragraph{Field: Temperature}\label{field-temperature-1}
+
+The setpoint temperature {[}C{]} at which the system is turned on.
+
+An example of this object in an IDF is:
+
+\begin{lstlisting}
+
+AvailabilityManager:HighTemperatureTurnOn,
+  High Temperature Turn On Availability Manager,   !- Name
+  Outside Air Inlet Node,   !- Sensor Node
+  30.0;   !- Temperature {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-010}
+
+The high temperature turn on availability manager has one output variable.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Availability Manager High Temperature Turn On Control Status
+\end{itemize}
+
+\paragraph{\texorpdfstring{Availability Manager High Temperature Turn On Control Status {[]}}{Availability Manager High Temperature Turn On Control Status }}\label{availability-manager-high-temperature-turn-on-control-status}
+
+A value of 0 indicates the manager is signaling \emph{NoAction}. A value of 2 means the manager is signaling \emph{CycleOn.}
+
+\subsection{AvailabilityManager:LowTemperatureTurnOff}\label{availabilitymanagerlowtemperatureturnoff}
+
+This manager turns the system off if the temperature at the sensor node is below the specified setpoint temperature.
+
+\subsubsection{Inputs}\label{inputs-7-027}
+
+\paragraph{Field: Name}\label{field-name-6-023}
+
+The name of the object. This is referenced in the AvailabilityManagerAssignmentList.
+
+\paragraph{Field: Sensor Node Name}\label{field-sensor-node-name-2}
+
+The air or plant node where the temperature is monitored.
+
+\paragraph{Field: Temperature}\label{field-temperature-2}
+
+The setpoint temperature {[}C{]} at which the system is turned off.
+
+\paragraph{Field: Applicability Schedule Name}\label{field-applicability-schedule-name}
+
+The name of a schedule defined elsewhere in the input file. This schedule determines whether or not for a given time period this availability manager is to be applied. Schedule values greater than zero (usually 1 is used) indicate the availability manager is to be applied. Schedule values less than or equal to zero (usually 0 is used) denote that the availability manager is not used for this time period. If this field is left blank, this availability manager is always active.
+
+An example of this object in an IDF is:
+
+\begin{lstlisting}
+
+AvailabilityManager:LowTemperatureTurnOff,
+  Low Temperature Turn Off Availability Manager,   !- Name
+  Outside Air Inlet Node,   !- Sensor Node Name
+  0.0,   !- Temperature {C}
+  Low Temp Control Schedule;   !- Applicability Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-010}
+
+The low temperature turn off availability manager has one output variable.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Availability Manager Low Temperature Turn Off Control Status
+\end{itemize}
+
+Availability Manager Low Temperature Turn Off Control Status {[]}
+
+A value of 0 indicates the manager is signaling NoAction. A value of 1 means the manager is signaling ForceOff.
+
+\subsection{AvailabilityManager:LowTemperatureTurnOn}\label{availabilitymanagerlowtemperatureturnon}
+
+This manager turns the system on if the temperature at the sensor node is below the specified setpoint temperature.
+
+\subsubsection{Inputs}\label{inputs-8-025}
+
+\paragraph{Field: Name}\label{field-name-7-021}
+
+The name of the object. This is referenced in the AvailabilityManagerAssignmentList.
+
+\paragraph{Field: Sensor Node Name}\label{field-sensor-node-name-3}
+
+The air or plant node where the temperature is monitored.
+
+\paragraph{Field: Temperature}\label{field-temperature-3}
+
+The setpoint temperature {[}C{]} at which the system is turned on.
+
+An example of this object in an IDF is:
+
+\begin{lstlisting}
+
+AvailabilityManager:LowTemperatureTurnOn,
+  Low Temperature Turn On Availability Manager,   !- Name
+  Collector Outlet Node,   !- Sensor Node Name
+  0.0;   !- Temperature {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-010}
+
+The low temperature turn on availability manager has one output variable.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Availability Manager Low Temperature Turn On Control Status {[]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Availability Manager Low Temperature Turn On Control Status {[]}}{Availability Manager Low Temperature Turn On Control Status }}\label{availability-manager-low-temperature-turn-on-control-status}
+
+A value of 0 indicates the manager is signaling NoAction. A value of 2 means the manager is signaling CycleOn.
+
+\subsection{AvailabilityManager:NightVentilation}\label{availabilitymanagernightventilation}
+
+This manager allows the user to implement a strategy for precooling a building at night using outdoor air. This strategy can consist of running the system fans with the outdoor air dampers open when outdoor conditions are favorable for a precooling strategy. The zone terminal unit air dampers may also be held at their fully open position to minimize fan energy consumption while precooling. Fan energy consumption is the critical parameter in deciding whether a precooling strategy will save energy.
+
+The inputs for the night ventilation manager consist of an applicability schedule name (determining when the manager is active), a fan schedule name (for the fan(s) that the manager can switch on), a ventilation temperature schedule name (one zone must be above this temperature for night venting to be active), a ventilation temperature difference (indoor outdoor temperature difference for night venting), a low limit temperature (no conditioned zone may fall below this temperature during night venting), a night venting flow fraction (fraction of the design flow rate at which the fans run during night venting), and the zone name of a control zone.
+
+The night ventilation manager is used in conjunction with another object: FanPerformance:NightVentilation. The performance of the fan during night venting may be very different than during normal operation (a different fan might even be used). The FanPerformance:NightVentilation object allows the user to specify alternate fan performance parameters for use during night ventilation.
+
+\subsubsection{Inputs}\label{inputs-9-023}
+
+\paragraph{Field: Name}\label{field-name-8-021}
+
+A unique, user-assigned name for an instance of a night ventilation availability manager. Other objects that use this availability manager will reference it by this name.
+
+\paragraph{Field: Applicability Schedule Name}\label{field-applicability-schedule-name-1}
+
+The name of a schedule defined elsewhere in the input file. This schedule determines whether or not for a given time period this availability manager is to be applied. Schedule values greater than zero (usually 1 is used) indicate the availability manager is to be applied. Schedule values less than or equal to zero (usually 0 is used) denote that the availability manager is not used for this time period.
+
+\paragraph{Field: Fan Schedule Name}\label{field-fan-schedule-name}
+
+The name of the central fan on/off schedule for the air system that this availability manager will affect.
+
+\paragraph{Field: Ventilation Temperature Schedule Name}\label{field-ventilation-temperature-schedule-name}
+
+The name of a temperature schedule defined elsewhere in the input file. At least one conditioned zone in the forced air system using this availability manager must be above the current temperature specified in this schedule for night ventilation to occur or to continue occurring.
+
+\paragraph{Field: Ventilation Temperature Difference}\label{field-ventilation-temperature-difference}
+
+This field specifies an indoor / outdoor temperature difference (in degrees C). The control zone temperature minus the outdoor air temperature must be greater than the Ventilation Temperature Difference for night ventilation to occur or to continue occurring. The default is 2 degrees C.
+
+\paragraph{Field: Ventilation Temperature Low Limit}\label{field-ventilation-temperature-low-limit}
+
+This field specifies a lower limit (in degrees C) on zone temperatures for night ventilation. If any conditioned zone served by the air system using this availability manager is below the ventilation temperature low limit, night ventilation will not occur or will switch off. The default is 15 degrees C.
+
+\paragraph{Field: Night Venting Flow Fraction}\label{field-night-venting-flow-fraction}
+
+The fraction (could be greater than 1) of the design flow rate at which the night ventilation will be done. The default is 1.
+
+\paragraph{Field: Control Zone Name}\label{field-control-zone-name-000}
+
+The name of the control zone used in the ventilation temperature difference check.
+
+An example of this object in an input file:
+
+\begin{lstlisting}
+
+AvailabilityManager:NightVentilation,
+  VAV Sys 1 Avail,                 !- Name
+  NightVentSched,                   !- Applicability Schedule Name
+  FanAvailSched,                     !- Fan Schedule Name
+  VentTempSched,                     !- Ventilation Temperature Schedule Name
+  2.0,                                         !- Ventilation Temperature Difference   {C}
+  15.,                                         !- Ventilation Temperature Low Limit
+  0.3333,                                   !- Night Venting Flow Fraction
+  SPACE3-1;                               !- Control Zone Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8-008}
+
+The night ventilation availability manager has one output variable.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Availability Manager Night Ventilation Control Status {[]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Availability Manager Night Ventilation Control Status {[]}}{Availability Manager Night Ventilation Control Status }}\label{availability-manager-night-ventilation-control-status}
+
+A value of 0 indicates the manager is signaling NoAction. A value of 2 means the manager is signaling CycleOn.
+
+\subsection{AvailabilityManager:HybridVentilation}\label{availabilitymanagerhybridventilation}
+
+This availability manager is executed at the start of each HVAC system timestep, before EnergyPlus calculates airflows defined in the objects ZoneInfiltration:*, ZoneVentilation:*, ZoneMixing, and ZoneCrossMixing, and before the AirflowNetwork model calculates multizone airflows. It serves two purposes: 1) prevents simultaneous natural ventilation and HVAC system operation, and 2) allows users to examine various ventilation strategies to maximize natural ventilation in order to reduce heating/cooling loads. The natural ventilation objects controlled by this availability manager have two groups: simple airflow group and AirflowNetwork group. The simple airflow group consists of the ZoneVentilation;* and ZoneMixing objects. The AirflowNetwork group consists of AirflowNetwork:MultiZone:Component:DetailedOpening and AirflowNetwork:MultiZone:Component:SimpleOpening objects used in the AirflowNetwork model. These two groups are not allowed to work simultaneously (see restrictions in the Airflow Network model section). Basically, this object overrides the controls for these opening objects or ZoneVentilation:* and ZoneMixing objects, closing the openings or shutting off ventilation/mixing airflows under certain conditions and allowing the HVAC system (AirLoopHVAC) to operate. If the availability manager determines that conditions are favorable for natural ventilation, then the HVAC system (AirLoopHVAC) is disabled and the opening objects or ventilation/mixing objects are able to operate based on the controls specified for those objects.
+
+Each AirLoopHVAC can have a corresponding hybrid ventilation availability manager. Each hybrid ventilation manager can control natural ventilation in the zones served by the AirLoopHVAC. The hybrid ventilation availability manager is triggered by zone air conditions for the controlled zone specified in an object input field. If there is no air loop, hybrid ventilation manager can still be applied to controlled zone specified in the object. To apply hybrid ventilation manager to the controlled zone not served by any air loop, the HVAC air loop name input field must be left blank. Currently, zone component objects such as unit heater, unit ventilator, packaged terminal air conditioner, packaged terminal heat pump, zone water source heat pump, window air conditioner, variable refrigerant flow, energy recovery ventilator, outdoor air unit, fan coil unit, and ventilated slab can individually use hybrid ventilation managers to make a decision regarding whether their fan should be on or off. Also, hybrid ventilation managers can be applied to zones served by ideal load zone components to turn them off when natural ventilation is active. Currently, hybrid ventilation manager is restricted to one per zone. It can either be applied through the air loop or directly to the zone. If hybrid ventilation manager is applied to an air loop and one of the zones served by the air loop also has hybrid ventilation manager, then zone hybrid ventilation manager is disabled. Presently, this availability manager must be used either with the ZoneVentilation:* and ZoneMixing objects or with the AirflowNetwork model.
+
+The inputs for this availability manager consist of the name for the air loop (AirLoopHVAC) being controlled, the controlled zone name to determine which zone air conditions are used to determine system availability, a ventilation control mode schedule, maximum wind speed and rain indicator to determine whether natural ventilation is allowed or not, a low limit and high limit for dry-bulb temperature, enthalpy and dewpoint temperature to determine the hybrid ventilation control, and a minimum outdoor air ventilation schedule. The last control allows user to use a wind speed modifier to adjust openness when the AirflowNetwork opening objects are selected. The other inputs include how to control simple airflow objects and AirflowNetwork opening objects.
+
+The hybrid ventilation availability manager works independently of all other system availability manager objects, so this manager is not a valid system availability manager type in the AvailabilityManagerAssignmentList object.
+
+\subsubsection{Inputs}\label{inputs-10-021}
+
+\paragraph{Field: Name}\label{field-name-9-018}
+
+A unique, user-assigned name for an instance of a hybrid ventilation availability manager. Other objects that use this availability manager will reference it by this name.
+
+\paragraph{Field: HVAC Air Loop Name}\label{field-hvac-air-loop-name-000}
+
+The name of the air loop (AirLoopHVAC object) to be controlled by this system availability manager. If this field is left blank, hybrid ventilation manager will be applied to the controlled zone specified in the field below.
+
+\paragraph{Field: Controlled Zone Name}\label{field-controlled-zone-name}
+
+The name of a controlled zone served by the air loop defined in the previous field. The air conditions in this zone are used to determine if natural ventilation should be provided.
+
+\paragraph{Field: Ventilation Control Mode Schedule Name}\label{field-ventilation-control-mode-schedule-name}
+
+The name of a schedule defined elsewhere in the input file. This schedule determines whether or not for a given time the hybrid ventilation control mode is to be applied. Schedule values equal to zero indicate no ventilation control, resulting in natural ventilation and HVAC system operation being performed based on their own controls. Schedule values equal to one denote temperature control for either cooling or heating, which is determined internally based on thermostat set point and temperature control type. The temperature control is restricted between the minimum and maximum outdoor temperatures provided in two additional input fields (below). Schedule values equal to two denote enthalpy control, which is restricted between minimum and maximum outdoor enthalpy values given in two additional input fields (below). Schedule values equal to three denote dewpoint control for either dehumidification or humidification. Schedule values equal to four represent outdoor ventilation air control. The outdoor ventilation air control works with AirflowNetwork opening objects only, and is not allowed to work with ZoneVentilation:* and ZoneMixing objects.
+
+The detailed control logic is given in the EnergyPlus Engineering Reference.
+
+\paragraph{Field: Use Weather File Rain Indicators}\label{field-use-weather-file-rain-indicators-000}
+
+This logical alpha field indicates whether or not the rain indicator is used to shut off natural ventilation or not. The valid choices for Rain Indicator are Yes and No, with the default being Yes. This can help simulate conditions where one would normally close windows to avoid rain penetration in a space. Any possible rain getting into a space will not be counted as a zone load.
+
+\paragraph{Field: Maximum Wind Speed}\label{field-maximum-wind-speed-000}
+
+This is the wind speed (m/s) above which hybrid ventilation is shut off. This can help simulate conditions where one would normally close windows to avoid wind problems in a space (papers blowing around, etc).
+
+\paragraph{Field: Minimum Outdoor Temperature}\label{field-minimum-outdoor-temperature-000}
+
+This is the outdoor temperature (in Celsius) below which hybrid ventilation is shut off when the ventilation control mode = 1 (Temperature). This lower temperature limit is intended to avoid overcooling a space, which could result in a heating load.
+
+\paragraph{Field: Maximum Outdoor Temperature}\label{field-maximum-outdoor-temperature-000}
+
+This is the outdoor temperature (in Celsius) above which hybrid ventilation is shut off when the ventilation control mode = 1 (Temperature). This upper temperature limit is intended to avoid overheating a space, which could result in a cooling load.
+
+\paragraph{Field: Minimum Outdoor Enthalpy}\label{field-minimum-outdoor-enthalpy}
+
+This is the outdoor enthalpy (in J/kg) below which hybrid ventilation is shut off when the ventilation control mode = 2 (Enthalpy).
+
+\paragraph{Field: Maximum Outdoor Enthalpy}\label{field-maximum-outdoor-enthalpy}
+
+This is the outdoor enthalpy (in J/kg) above which hybrid ventilation is shut off when the ventilation control mode = 2 (Enthalpy).
+
+\paragraph{Field: Minimum Outdoor Dewpoint}\label{field-minimum-outdoor-dewpoint}
+
+This is the outdoor dewpoint (in Celsius) below which hybrid ventilation is shut off when the ventilation control mode = 3 (Dewpoint). This lower dewpoint temperature limit is intended to avoid dehumidifying a space.
+
+\paragraph{Field: Maximum Outdoor Dewpoint}\label{field-maximum-outdoor-dewpoint}
+
+This is the outdoor dewpoint temperature (in Celsius) above which hybrid ventilation is shut off when the ventilation control mode = 3 (Dewpoint). This upper dewpoint temperature limit is intended to avoid humidifying a space.
+
+\paragraph{Field: Minimum Outdoor Ventilation Air Schedule Name}\label{field-minimum-outdoor-ventilation-air-schedule-name}
+
+The name of a schedule defined elsewhere in the input file. This field applies only if Ventilation Control Mode = 4 (Outdoor Ventilation Air Control). This schedule determines the minimum outdoor ventilation air for a given time in the units of air change per hour (ACH). The program calculates the natural (outdoor) ventilation in the controlled zone first and compares the amount of outdoor air introduced by opening windows or doors and other small openings to this minimum value. If the amount of outdoor air from natural ventilation is less than the minimum value, the natural ventilation is shut off (i.e., the window or door openings are closed) and the HVAC system may operate if needed. Otherwise, the natural ventilation is on and the HVAC system is shut off. The amount of outdoor ventilation air entering the controlled zone is determined as air from outdoors and not from other adjacent zones. Therefore, this option is only applied to a zone having a window or door exposed to outdoors.
+
+\paragraph{Field: Opening Factor Function of Wind Speed Curve Name}\label{field-opening-factor-function-of-wind-speed-curve-name}
+
+The name of a linear or quadratic performance curve (ref: Performance Curves) that parameterizes the variation of opening factor as a function of outdoor wind speed. The output of this curve is multiplied by the opening factor of opening objects to give the final openness. This field only works with the AirflowNetwork opening objects.
+
+\paragraph{Field: AirflowNetwork Control Type Schedule Name}\label{field-airflownetwork-control-type-schedule-name}
+
+The name of a schedule defined elsewhere in the input file. This field works with the AirflowNetwork opening objects only. This schedule determines for a given simulation timestep how the opening objects respond to the hybrid ventilation control when the hybrid ventilation control allows the objects to operate.
+
+Schedule values equal to zero indicate individual ventilation control based on the control requirements specified for each individual AirflowNetwork opening object. Schedule values equal to one denote group control. The opening objects exposed to outdoors in the controlled zone served by the primary air loop (Ref. Field HVAC Air Loop Name ) will be considered as a master to provide group control.
+
+\paragraph{Field: Simple Airflow Control Type Schedule Name}\label{field-simple-airflow-control-type-schedule-name}
+
+The name of a schedule defined elsewhere in the input file. This field works with ZoneVentilation:* and ZoneMixing objects only. This schedule determines for a given simulation timestep how the ZoneVentilation:* and ZoneMixing objects respond to the hybrid ventilation control when the hybrid ventilation control allows the objects to operate.
+
+Schedule values equal to zero indicate the individual ventilation control based on the control requirements from their own objects. Schedule values equal to one denote group control. The ZoneVentilation:* and ZoneMixing objects in the zones served by the primary air loop defined in a previous input field (Ref. Field HVAC Air Loop Name ) are controlled by a single object, whose name is provided in the following input field.
+
+\paragraph{Field: ZoneVentilation Object Name}\label{field-zoneventilation-object-name}
+
+The name of a ZoneVentilation:* object whose zone name is the controlled zone name defined in a previous input field for this availability manager object (Ref. Field Controlled Zone Name ). The controls defined for this specific ZoneVentilation:* object to enable ventilation air will be applied to other ZoneVentilation:* and ZoneMixing objects served by the air loop controlled by this availability manager, regardless of the controls defined for the other ZoneVentilation:* and ZoneMixing objects. In other words, when ventilation is enabled by this specific ZoneVentilation:* object, the other ZoneVentilation:* and ZoneMixing objects in the zones served by the primary air loop are also enabled.
+
+\textbf{Note:} A \textbf{ZoneInfiltration:*} object indicates any one of \textbf{ZoneInfiltration:DesignFlowRate}, \textbf{ZoneInfiltration:EffectiveLeakageArea},and \textbf{ZoneInfiltration:FlowCoefficient} objects.A object of\textbf{ZoneVentilation:*} indicates any one of \textbf{ZoneVentilation:DesignFlowRate} and \textbf{ZoneVentilation:WindandStackOpenArea} objects.
+
+\subsubsection{Outputs}\label{outputs-9-008}
+
+The hybrid ventilation availability manager has two output variables.
+
+HVAC,Average,Availability Manager Hybrid Ventilation Control Mode {[]}
+
+HVAC,Average,Availability Manager Hybrid Ventilation Control Status {[]}
+
+\paragraph{\texorpdfstring{Availability Manager Hybrid Ventilation Control Mode {[]}}{Availability Manager Hybrid Ventilation Control Mode }}\label{availability-manager-hybrid-ventilation-control-mode}
+
+This is the hybrid ventilation control mode given in the Ventilation Control Mode Schedule.
+
+\paragraph{\texorpdfstring{Availability Manager Hybrid Ventilation Control Status {[]}}{Availability Manager Hybrid Ventilation Control Status }}\label{availability-manager-hybrid-ventilation-control-status}
+
+This is the hybrid ventilation control status, which can have three integer values: 0, 1, and 2. A zero value indicates no hybrid ventilation control, corresponding to zero value defined in the previous output variable. A value of one indicates that natural ventilation is allowed. A value of two denotes that the natural ventilation is not allowed, so all window/door openings are closed.
+
+\subsection{AvailabilityManager:OptimumStart}\label{availabilitymanageroptimumstart}
+
+When night time temperature setback and/or setup are employed, the optimum start availability manager is used to start the HVAC system prior to occupancy to ensure that the space is comfortable when people appear in the building.
+
+\subsubsection{Inputs}\label{inputs-11-020}
+
+\paragraph{Field: Name}\label{field-name-10-017}
+
+A unique, user-defined name for an instance of this availability manager.
+
+\paragraph{Field: Applicability Schedule Name}\label{field-applicability-schedule-name-2}
+
+This schedule decides whether for a given time period this availability manager is to be applied. Schedule value of 1 specifies the availability manager is to be applied. Schedule value of 0 indicates that the availability manager is not used for this time period
+
+\paragraph{Field: Fan Schedule Name}\label{field-fan-schedule-name-1}
+
+The name of the central fan schedule for the air system that this availability manager will govern.
+
+\paragraph{Field: Control Type}\label{field-control-type-003}
+
+The possible inputs are StayOff, MaximumofZoneList, and ControlZone. StayOff means the availability manager will have no effect air handler on/off will be determined by the fan schedule. ControlZone means a specific zone mentioned in the field will govern the start time. The default is ControlZone. MaximumofZoneList means that from all zones mentioned in the zone list field in this availability manager maximum value of start time will be used to start the fan.
+
+\paragraph{Field: Control Zone Name}\label{field-control-zone-name-1-000}
+
+For Control type ControlZone the name of zone is added here. Start time for this zone will be used for the air loop.
+
+\paragraph{Field: Zone List Name}\label{field-zone-list-name}
+
+Zones mentioned in this list will be used to determine the start time. Maximum value of start time for the zones mentioned in this list will be used for the air loop.
+
+\paragraph{Field: Maximum Value for Optimum Start Time}\label{field-maximum-value-for-optimum-start-time}
+
+To limit too early start of the system maximum value for the start time can be entered here. Optional input, defaults to 6 hours. This is the maximum number of hours that a system can start before occupancy.
+
+\paragraph{Field: Control Algorithm}\label{field-control-algorithm}
+
+The four possible inputs are \textbf{ConstantTemperatureGradient, AdaptiveTemperatureGradient, AdaptiveASHRAE,} and \textbf{ConstantStartTime}. In ConstantTemperatureGradient algorithm the temperature gradient entered by the user will be constant throughout the simulation. The response to heating and cooling operation can be non-linear thus two separate fields for temperature gradients are used. AdaptiveTemperatureGradient algorithm will modify the temperature gradients based on the arithmetic average of the actual temperature gradients calculated for the specified number of previous days. For this algorithm user should enter two initial start values. AdaptiveASHRAE algorithm implements equations suggested in ASHRAE Handbook HVAC Applications (2007). This algorithm will calculate the coefficients of the equation within the code and users need not provide temperature response related inputs. ConstantStartTime method calculates the start time based on specified number of hours before occupancy for each day. \textbf{The AdaptiveASHRAE algorithm has not been implemented yet.}
+
+\paragraph{Field: Constant Temperature Gradient during Cooling}\label{field-constant-temperature-gradient-during-cooling}
+
+This input is required if ConstantTemperatureGradient algorithm is selected in the above field. Temperature gradient ( °C/hour) for cooling operation is entered here. Such gradient may be obtained for existing buildings from EMCS or pre-calculated by other programs. This gradient remains constant throughout the simulation.
+
+\paragraph{Field: Constant Temperature Gradient during Heating}\label{field-constant-temperature-gradient-during-heating}
+
+This input is required if ConstantTemperatureGradient algorithm is selected in the Control Algorithm field. Temperature gradient ( °C/hour) for heating operation is entered here. This gradient remains constant throughout the simulation.
+
+\paragraph{Field: Initial Temperature Gradient during Cooling}\label{field-initial-temperature-gradient-during-cooling}
+
+This input is required if AdaptiveTemperatureGradient algorithm is selected in Control Algorithm field. Initial value of temperature gradient ( °C/hour) for cooling operation is entered here. This value is used as initial guess value to start the adaptive method. Depending on performance, this value is modified and used in the simulation.
+
+\paragraph{Field: Initial Temperature Gradient during Heating}\label{field-initial-temperature-gradient-during-heating}
+
+This input is required if AdaptiveTemperatureGradient algorithm is selected in Control Algorithm field. Initial value of temperature gradient ( °C/hour) for heating operation is entered here. This value is used as initial guess value to start the adaptive method. Depending on performance, this value is modified and used in the simulation.
+
+\paragraph{Field: Constant Start Time}\label{field-constant-start-time}
+
+This input is required if ConstantStartTime algorithm is selected in the Control Algorithm field. Start time, the number of hours before occupancy occurs for a system, for heating and cooling operation is entered here. Irrespective of thermal response, the heating or cooling operation starts before the occupancy at this fixed time. This start time value remains constant throughout the simulation.
+
+\paragraph{Field: Number of Previous Days}\label{field-number-of-previous-days}
+
+This input is required if AdaptiveTemperatureGradient algorithm is selected in the Control Algorithm field. The values of optimal start time for number of days entered here will be used to determine the adaptive gradients.
+
+Sample IDFs:
+
+\begin{lstlisting}
+
+AvailabilityManager:OptimumStart,
+  AdaptiveSetbackRecovery, !- Name
+  AppliSch,                                             !- Applicability Schedule Name
+  FanSch,                                                 !- Fan Schedule Name
+  ControlZone,                                       !- Control Type
+  MainZone,                                             !- Control Zone Name
+  ,                                                             !- Zone List Name
+  4,                                                           !- Maximum Value for Optimum Start Time
+  AdaptiveTemperatureGradient,       !- Control Algorithm
+  ,                                                             !- Constant Temperature Gradient during Cooling
+  ,                                                             !- Constant Temperature Gradient during Heating
+  5,                                                           !- Initial Temperature Gradient during Cooling
+  5;                                                           !- Initial Temperature Gradient during Heating
+
+  AvailabilityManager:OptimumStart,
+  SetbackRecovery,                               !- Name
+  AppliSch,                                             !- Applicability Schedule Name
+  FanSch,                                                 !- Fan Schedule Name
+  MaximumofZoneList,             !- Control Type
+  ,                                                            !- Control Zone Name
+  ZoneList,                                             !- Zone List Name
+  ,                                                             !- Maximum Value for Optimum Start Time
+  AdaptiveASHRAE;                                 !- Control Algorithm
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-10-007}
+
+The optimum start availability manager has two output variables.
+
+\paragraph{Availability Manager Night Ventilation Control Status}\label{availability-manager-night-ventilation-control-status-1}
+
+A value of 0 indicates the manager is signaling NoAction. A value of 2 means the manager is signaling CycleOn.
+
+\paragraph{Availability Manager Optimum Start Time Before Occupancy}\label{availability-manager-optimum-start-time-before-occupancy}
+
+The current time before occupancy. Occupancy is the first zone timestep after midnight when the Fan Schedule is \textgreater{} 0.0. The units are hours.
diff --git a/doc/input-output-reference/src/overview/group-thermal-zone-description-geometry.tex b/doc/input-output-reference/src/overview/group-thermal-zone-description-geometry.tex
new file mode 100644
index 00000000000..77c3ccd7dc2
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+++ b/doc/input-output-reference/src/overview/group-thermal-zone-description-geometry.tex
@@ -0,0 +1,4841 @@
+\section{Group -- Thermal Zone Description/Geometry}\label{group-thermal-zone-descriptiongeometry}
+
+Without thermal zones and surfaces, the building can't be simulated. This group of objects (Zone, BuildingSurface) describes the thermal zone characteristics as well as the details of each surface to be modeled. Included here are shading surfaces.
+
+\subsection{Zone}\label{zone}
+
+This element sets up the parameters to simulate each thermal zone of the building.
+
+\subsubsection{Inputs}\label{inputs-048}
+
+\paragraph{Field: Direction of Relative North}\label{field-direction-of-relative-north}
+
+The Zone North Axis is specified \textbf{relative to the Building North Axis}. This value is specified in degrees (clockwise is positive). For more information, see the figure below as well as the description under ``GlobalGeometryRules''.
+
+\paragraph{Field(s): (X,Y,Z) Origin}\label{fields-xyz-origin}
+
+The X,Y,Z coordinates of a zone origin can be specified, for convenience in vertice entry. Depending on the values in ``GlobalGeometryRules'' (see description later in this section), these will be used to completely specify the building coordinates in ``world coordinate'' or not. Zone Origin coordinates are specified \textbf{relative to the Building Origin (which always 0,0,0)}. The following figure illustrates the use of Zone North Axis as well as Zone Origin values.
+
+\begin{figure}[hbtp] % fig 27
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image053.png}
+\caption{Illustration of Zone North Axis and Origins \protect \label{fig:illustration-of-zone-north-axis-and-origins}}
+\end{figure}
+
+\paragraph{Field: Type}\label{field-type-000}
+
+Zone type is currently unused.
+
+\paragraph{Field: Multiplier}\label{field-multiplier}
+
+Zone Multiplier is designed as a ``multiplier'' for floor area, zone loads, and energy consumed by internal gains. It takes the calculated load for the zone and multiplies it, sending the multiplied load to the attached HVAC system. The HVAC system size is specified to meet the entire multiplied zone load and will report the amount of the load met in the Zone Air System Sensible Heating or Cooling Energy/Rate output variable. Autosizing automatically accounts for multipliers. Metered energy consumption by internal gains objects such as Lights or Electric Equipment will be mutliplied. The default is 1.
+
+\paragraph{Field: Ceiling Height}\label{field-ceiling-height}
+
+Zone ceiling height is used in several areas within EnergyPlus (such as various room models, some convection coefficient calculations and, primarily, in calculating zone volume in the absence of other parameters). Energyplus automatically calculates the zone ceiling height (m) from the average height of the zone. If this field is 0.0, negative or \textbf{autocalculate}, then the calculated zone ceiling height will be used in subsequent calculations. If this field is positive, then the calculated zone ceiling height will not be used -- the number entered here will be used as the zone ceiling height. If this number differs significantly from the calculated ceiling height, then a warning message will be issued. If a zone ceiling height is entered, but no Volume is entered, then the floor area (if there is one) times the zone ceiling height will be used as the volume.
+
+Note that the Zone Ceiling Height is the distance from the Floor to the Ceiling in the Zone, not an absolute height from the ground.
+
+\paragraph{Field: Volume}\label{field-volume}
+
+Zone volume is used in several areas within EnergyPlus (such as calculating air change rates for reporting or flow when air change rates are chosen as input, daylighting calculations, some convection coefficient calculations). EnergyPlus automatically calculates the zone volume (m\(^{3}\)) from the zone geometry given by the surfaces that belong to the zone. If this field is 0.0, negative or \textbf{autocalculate}, then the calculated zone volume will be used in subsequent calculations. If this field is positive, then it will be used as the zone volume. If this number differs significantly from the calculated zone volume a warning message will be issued. For autocalculate to work properly, the zone must be enclosed by the entered walls. Note that indicating the volume to be calculated but entering a positive ceiling height in the previous field will cause the volume to be calculated as the floor area (if \textgreater{} 0) times the entered ceiling height; else the volume will be calculated from the described surfaces. If this field is positive, any ceiling height positive value will not be used in volume calculations.
+
+\paragraph{Field: Floor Area}\label{field-floor-area}
+
+Zone floor area is used in many places within EnergyPlus. EnergyPlus automatically calculates the zone floor area (m\(^{2}\)) from the zone geometry given by the surfaces that belong to the zone. If this field is 0.0, negative or \textbf{autocalculate}, then the calculated zone floor area will be used in subsequent calculations. If this field is positive, then it will be used as the zone floor area. If this number differs significantly from the calculated zone floor area a warning message will be issued.
+
+\paragraph{Field: Zone Inside Convection Algorithm}\label{field-zone-inside-convection-algorithm}
+
+The Zone Inside Convection Algorithm field is optional. This field specifies the convection model to be used for the inside face of heat transfer surfaes associated with this zone. The choices are: \textbf{Simple} (constant natural convection - ASHRAE), \textbf{Detailed} (variable natural convection based on temperature difference - ASHRAE), \textbf{CeilingDiffuser} (ACH based forced and mixed convection correlations for ceiling diffuser configuration with simple natural convection limit), \textbf{AdaptiveConvectionAlgorithm} (complex arrangement of various models that adapt to various zone conditions and can be customized) and \textbf{TrombeWall} (variable natural convection in an enclosed rectangular cavity). See the Inside Convection Algorithm object for further descriptions of the available models.
+
+If omitted or blank, the algorithm specified in the SurfaceConvectionAlgorithm:Inside object is the default.
+
+\paragraph{Field: Zone Outside Convection Algorithm}\label{field-zone-outside-convection-algorithm}
+
+The Zone Outside Convection Algorithm field is optional. This field specifies the convection model to be used for the outside face of heat transfer surfaces associated with this zone. The choices are: \textbf{SimpleCombined}, \textbf{TARP}, \textbf{DOE-2}, \textbf{MoWiTT, and AdaptiveConvectionAlgorithm}. The simple convection model applies heat transfer coefficients depending on the roughness and windspeed. This is a combined heat transfer coefficient that includes radiation to sky, ground, and air. The correlation is based on Figure~\ref{fig:schematic-of-the-energyplus-unitary-system}, Page 25.1 (Thermal and Water Vapor Transmission Data), 2001 ASHRAE Handbook of Fundamentals.
+
+The other convection models apply heat transfer coefficients depending on the roughness, windspeed, and terrain of the building's location. These are \emph{convection only} heat transfer coefficients; radiation heat transfer coefficients are calculated automatically by the program. The TARP algorithm was developed for the TARP software and combines natural and wind-driven convection correlations from laboratory measurements on flat plates. The DOE-2 and MoWiTT were derived from field measurements. The AdaptiveConvectionAlgorithm model is an dynamic algorithm that organizes a large number of different convection models and automatically selects the one that best applies. The adaptive convection algorithm can also be customized using the SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections input object. All algorithms are described more fully in the Engineering Reference.
+
+If omitted or blank, the algorithm specified in the SurfaceConvectionAlgorithm:Outside object is the default.
+
+\paragraph{Field: Part of Total Floor Area}\label{field-part-of-total-floor-area}
+
+This optional field defaults to Yes if not specified. The field is used to show when a zone is not part of the Total Floor Area as shown in the Annual Building Utility Performance Summary tables. Specifically, when No is specified, the area is excluded from both the conditioned floor area and the total floor area in the Building Area sub table and the Normalized Metrics sub tables.
+
+And, an IDF example:
+
+\begin{lstlisting}
+
+  Zone,
+      DORM ROOMS AND COMMON AREAS,  !- Name
+      0.0000000E+00,           !- Direction of Relative North {deg}
+      0.0000000E+00,           !- X Origin {m}
+      6.096000,                !- Y Origin {m}
+      0.0000000E+00,           !- Z Origin {m}
+      1,                       !- Type
+      1,                       !- Multiplier
+      autocalculate,           !-Ceiling Height {m}
+      autocalculate;           !- Volume {m3}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-037}
+
+\begin{itemize}
+\item
+  Zone,Average,Zone Outdoor Air Drybulb Temperature {[}C{]}
+\item
+  Zone,Average,Zone Outdoor Air Wetbulb Temperature {[}C{]}
+\item
+  Zone,Average,Zone Outdoor Air Wind Speed {[}m/s{]}
+\end{itemize}
+
+\paragraph{Zone Outdoor Air Drybulb Temperature {[}C{]}}\label{zone-outdoor-air-drybulb-temperature-c-000}
+
+The outdoor air dry-bulb temperature calculated at the height above ground of the zone centroid.
+
+\paragraph{Zone Outdoor Air Wetbulb Temperature {[}C{]}}\label{zone-outdoor-air-wetbulb-temperature-c-000}
+
+The outdoor air wet-bulb temperature calculated at the height above ground of the zone centroid.
+
+\paragraph{Zone Outdoor Air Wind Speed {[}m/s{]}}\label{zone-outdoor-air-wind-speed-ms-000}
+
+The outdoor wind speed calculated at the height above ground of the zone centroid.
+
+\subsection{Zone Thermal Output(s)}\label{zone-thermal-outputs}
+
+In addition to the canned Surface reports (view the Reports section later in this document) and surface variables (above), the following variables are available for all zones:
+
+\begin{itemize}
+\item
+  Zone,Sum,Zone Total Internal Radiant Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Total Internal Radiant Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Total Internal Visible Radiation Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Total Internal Visible Radiation Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Total Internal Convective Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Total Internal Convective Heating Rate {[}W{]}
+\item
+  Zone,Sum,Zone Total Internal Latent Gain Energy {[}J{]}
+\item
+  Zone,Average,Zone Total Internal Latent Gain Rate {[}W{]}
+\item
+  Zone,Sum,Zone Total Internal Total Heating Energy {[}J{]}
+\item
+  Zone,Average,Zone Total Internal Total Heating Rate {[}W{]}
+\item
+  Zone,Average,Zone Mean Air Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Air Temperature {[}C{]}
+\item
+  Zone,Average,Zone Mean Air Dewpoint Temperature {[}C{]}
+\item
+  Zone,Average,Zone Mean Radiant Temperature {[}C{]}
+\item
+  Zone,Average,Zone Operative Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Air Heat Balance Internal Convective Heat Gain Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air Heat Balance Surface Convection Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air Heat Balance Interzone Air Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air Heat Balance Outdoor Air Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air Heat Balance System Air Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air Heat Balance System Convective Heat Gain Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air Heat Balance Air Energy Storage Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air Heat Balance Deviation Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Air System Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Air System Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Air System Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air System Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air Humidity Ratio{[}kgWater/kgDryAir{]}
+\item
+  HVAC,Average,Zone Air Relative Humidity{[}\%{]}
+\end{itemize}
+
+Two of these are of particular interest:
+
+\begin{lstlisting}
+Zone,Average,Zone Mean Air Temperature [C]
+HVAC,Average,Zone Air Temperature [C]
+\end{lstlisting}
+
+These two variable outputs are/should be identical. However, note that they can be reported at different time intervals. ``Zone Mean Air Temperature'' is only available on the Zone/HB timestep (Number of Timesteps per Hour) whereas ``Zone Air Temperature'' can be reported at the HVAC timestep (which can vary).
+
+\subsubsection{Zone Mean Air Temperature {[}C{]}}\label{zone-mean-air-temperature-c}
+
+From the code definition, the zone mean air temperature is the average temperature of the air temperatures at the system timestep. Remember that the zone heat balance represents a ``well stirred'' model for a zone, therefore there is only one mean air temperature to represent the air temperature for the zone.
+
+\subsubsection{Zone Air Temperature {[}C{]}}\label{zone-air-temperature-c}
+
+This is very similar to the mean air temperature in the last field. The ``well stirred'' model for the zone is the basis, but this temperature is also available at the ``detailed'' system timestep.
+
+\subsubsection{Zone Mean Air Dewpoint Temperature {[}C{]}}\label{zone-mean-air-dewpoint-temperature-c}
+
+This is the dewpoint temperature of the zone calculated from the Zone Mean Air Temperature (above), the Zone Air Humidity Ratio (below) and the outdoor barometric pressure.
+
+\subsubsection{Zone Thermostat Air Temperature {[}C{]}}\label{zone-thermostat-air-temperature-c}
+
+This is the zone air node temperature for the well-mixed room air model, which is the default room air model type (RoomAirModelType = Mixing). But for other types of Room Air Model (the RoomAir:TemperaturePattern:* and RoomAirSettings:* objects) the zone thermostat air temperature may depend on the Thermostat Height and Thermostat Offset.
+
+\subsubsection{Zone Mean Radiant Temperature {[}C{]}}\label{zone-mean-radiant-temperature-c}
+
+The Mean Radiant Temperature (MRT) in degrees Celsius of a space is a measure of the combined effects of temperatures of surfaces within that space. Specifically it is the surface area × emissivity weighted average of the zone inside surface temperatures (ref. Surface Inside Temperature), where emissivity is the Thermal Absorptance of the inside material layer of each surface.
+
+\subsubsection{Zone Operative Temperature {[}C{]}}\label{zone-operative-temperature-c}
+
+Zone Operative Temperature (OT) is the average of the Zone Mean Air Temperature (MAT) and Zone Mean Radiant Temperature (MRT), OT = 0.5*MAT + 0.5*MRT. This output variable is not affected by the type of thermostat controls in the zone, and does not include the direct effect of high temperature radiant systems. See also Zone Thermostat Operative Temperature.
+
+\subsubsection{Zone Air Heat Balance Internal Convective Heat Gain Rate {[}W{]}}\label{zone-air-heat-balance-internal-convective-heat-gain-rate-w}
+
+The Zone Air Heat Balance Internal Convective Heat Gain Rate is the sum, in watts, of heat transferred to the zone air from all types of internal gains, including people, lights, equipment etc. This and the following provide results on the load components of the zone air heat balance. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air Heat Balance Surface Convection Rate {[}W{]}}\label{zone-air-heat-balance-surface-convection-rate-w}
+
+The Zone Air Heat Balance Surface Convection Rate is the sum, in watts, of heat transferred to the zone air from all the surfaces. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air Heat Balance Interzone Air Transfer Rate {[}W{]}}\label{zone-air-heat-balance-interzone-air-transfer-rate-w}
+
+The Zone Air Heat Balance Interzone Air Transfer Rate is the sum, in watts, of heat transferred to the zone air from all the transfers of air from other thermal zones. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air Heat Balance Outdoor Air Transfer Rate {[}W{]}}\label{zone-air-heat-balance-outdoor-air-transfer-rate-w}
+
+The Zone Air Heat Balance Outdoor Air Transfer Rate is the sum, in watts, of heat transferred to the zone air from all the transfers of air from the out side, such as infiltration. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air Heat Balance System Air Transfer Rate {[}W{]}}\label{zone-air-heat-balance-system-air-transfer-rate-w}
+
+The Zone Air Heat Balance System Air Transfer Rate is the sum, in watts, of heat transferred to the zone air by HVAC forced-air systems and air terminal units. Such HVAC systems are connected to the zone by an inlet node (see ZoneHVac:EquipmentConnections input field called Zone Air Inlet Node or Node List Name) This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air Heat Balance System Convective Heat Gain Rate {[}W{]}}\label{zone-air-heat-balance-system-convective-heat-gain-rate-w}
+
+The Zone Air Heat Balance System Convective Heat Gain Rate is the sum, in watts, of heat transferred directly to the zone air by ``non-air'' HVAC systems. Such HVAC systems are not connected to the zone by an inlet node but rather add or subtract heat directly to the zone air in a manner similar to internal gains. These include the convective fraction of zone HVAC baseboards and high temperature radiant systems, zone HVAC refrigeration chiller set, and the extra convective cooling provided by the cooled beam air terminal unit. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air Heat Balance Air Energy Storage Rate {[}W{]}}\label{zone-air-heat-balance-air-energy-storage-rate-w}
+
+The Zone Air Heat Balance Air Energy Storage Rate is the heat stored, in watts, in the zone air as result of zone air temperature changing from one timestep to the next. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air Heat Balance Deviation Rate {[}W{]}}\label{zone-air-heat-balance-deviation-rate-w}
+
+The Zone Air Heat Balance Deviation Rate is the imbalance, in watts, in the energy balance for zone air. The value should be near zero but will become non-zero if zone conditions are changing rapidly or erratically. This field is not multiplied by zone or group multipliers. (This output variable is only generated if the user has set a computer system environment variable DisplayAdvancedReportVariables equal to ``yes''.)
+
+\subsubsection{Zone Air System Sensible Heating Energy {[}J{]}}\label{zone-air-system-sensible-heating-energy-j}
+
+This output variable represents the sensible heating energy in Joules that is actually supplied by the system to that zone for the timestep reported. This is the sensible heating rate multiplied by the simulation timestep. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module. This field is not multiplied by zone or group multipliers.
+
+\begin{callout}
+Zone Air System Sensible Heating (and Cooling) Energy (and Rate) all report the heating or cooling delivered by the HVAC system to a zone. These values are calculated by multiplying the supply air mass flow rate by the difference between the supply air temperature and the zone air temperature. This does not always indicate the operation of heating or cooling coils. For example, cooling will be reported if the supply air is cooled due to the introduction of outside air, even if all coils are off.
+
+Note that these variables are calculated at the system timestep. When reported at the ``detailed'' reporting frequency, these variable will never show heating and cooling both in the same system timestep. If reported at a frequency less than ``Detailed'' (for example, Hourly) values may appear in both the heating and cooling variable for the same hour if the system cooled the zone for part of the reporting period and heated the zone for another part of the reporting period.
+\end{callout}
+
+\subsubsection{Zone Air System Sensible Cooling Energy {[}J{]}}\label{zone-air-system-sensible-cooling-energy-j}
+
+This output variable represents the sensible cooling energy in Joules that is actually supplied by the system to that zone for the timestep reported. This is the sensible cooling rate multiplied by the simulation timestep. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air System Sensible Heating Rate {[}W{]}}\label{zone-air-system-sensible-heating-rate-w}
+
+This output variable represents the sensible heating rate in Watts that is actually supplied by the system to that zone for the timestep reported. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air System Sensible Cooling Rate {[}W{]}}\label{zone-air-system-sensible-cooling-rate-w}
+
+This output variable represents the sensible cooling rate in Watts that is actually supplied by the system to that zone for the timestep reported. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air Humidity Ratio {[}kgWater/kgDryAir{]}}\label{zone-air-humidity-ratio-kgwaterkgdryair}
+
+This output variable represents the air humidity ratio after the correct step for each zone. The humidity ratio is the mass of water vapor to the mass of dry air contained in the zone in (kg water/kg air) and is unitless.
+
+\subsubsection{Zone Air Relative Humidity {[}\%{]}}\label{zone-air-relative-humidity}
+
+This output variable represents the air relative humidity after the correct step for each zone. The relative humidity is in percent and uses the Zone Air Temperature, the Zone Air Humidity Ratio and the Outside Barometric Pressure for calculation.
+
+\subsubsection{Zone Total Internal Radiant Heating Rate {[}W{]}}\label{zone-total-internal-radiant-heating-rate-w}
+
+\subsubsection{Zone Total Internal Radiant Heating Energy {[}J{]}}\label{zone-total-internal-radiant-heating-energy-j}
+
+These output variables represent the sum of radiant gains from specific internal sources (e.g.~equipment) throughout the zone in Watts (for rate) or joules. This includes radiant gain from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
+
+\subsubsection{Zone Total Internal Visible Radiation Heating Rate {[}W{]}}\label{zone-total-internal-visible-radiation-heating-rate-w}
+
+\subsubsection{Zone Total Internal Visible Radiation Heating Energy {[}J{]}}\label{zone-total-internal-visible-radiation-heating-energy-j}
+
+These output variables expresse the sum of heat gain in Watts (for rate) or joules that is the calculated short wavelength radiation gain from lights in the zones. This calculation uses the total energy from lights and the fraction visible to realize this value, summed over the zones in the simulation.
+
+\subsubsection{Zone Total Internal Convective Heating Rate {[}W{]}}\label{zone-total-internal-convective-heating-rate-w}
+
+\subsubsection{Zone Total Internal Convective Heating Energy {[}J{]}}\label{zone-total-internal-convective-heating-energy-j}
+
+These output variables represent the sum of convective gains from specific sources (e.g.~equipment) throughout the zone in Watts (for rate) or joules. This includes convective gain from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
+
+\subsubsection{Zone Total Internal Latent Gain Rate {[}W{]}}\label{zone-total-internal-latent-gain-rate-w}
+
+\subsubsection{Zone Total Internal Latent Gain Energy {[}J{]}}\label{zone-total-internal-latent-gain-energy-j}
+
+These output variables represent the sum of latent gains from specific internal sources (e.g.~equipment) throughout the zone in Watts (for rate) or joules. This includes latent gain from People, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
+
+\subsubsection{Zone Total Internal Total Heating Rate {[}W{]}}\label{zone-total-internal-total-heating-rate-w}
+
+\subsubsection{Zone Total Internal Total Heating Energy {[}J{]}}\label{zone-total-internal-total-heating-energy-j}
+
+These output variables represent the sum of all heat gains throughout the zone in Watts (for rate) or joules. This includes all heat gains from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
+
+\subsection{ZoneList}\label{zonelist}
+
+The ZoneList object defines a list of Zone objects. It is primarily used with the ZoneGroup object to provide a generalized way for doing ``Floor Multipliers''. (See the ZoneGroup description below.) The associated ZoneList output variables also provide a way to aggregate and organize zone loads.
+
+Zone lists are not exclusive. A zone can be referenced be more than one ZoneList object.
+
+\subsubsection{Inputs}\label{inputs-1-045}
+
+\paragraph{Field: Zone List Name}\label{field-zone-list-name-000}
+
+The name of the ZoneList object. Must be unique across ZoneLists.
+
+\paragraph{Field: Zone 1 - Zone 20 Name}\label{field-zone-1---zone-20-name}
+
+Reference to a Zone object. This field is extensible; for greater than 20 zones, edit the IDD to add more \emph{Zone Name} fields.
+
+\begin{lstlisting}
+
+ZoneList,
+  Mid Floor List,  !- Name
+  Mid West Zone,   !- Zone 1 Name
+  Mid Center Zone, !- Zone 2 Name
+  Mid East Zone;   !- Zone 3 Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-028}
+
+The following output variables are reported by the ZoneList object:
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone List Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone List Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone List Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone List Sensible Cooling Energy {[}J{]}
+\end{itemize}
+
+All ZoneList variables are the sum of the corresponding Zone variables. \emph{Zone Multiplier} fields in the Zone objects are also taken into account.
+
+\subsection{ZoneGroup}\label{zonegroup}
+
+The ZoneGroup object adds a multiplier to a ZoneList. This can be used to reduce the amount of input necessary for simulating repetitive structures, such as the identical floors of a multi-story building. To create a ``Floor Multiplier'', use the ZoneList object to organize several zones into a typical floor. Then use the \emph{Zone List Multiplier} field in the ZoneGroup object to multiply the system load for the zones in the list will also be multiplied. Zones with a \emph{Multiplier} field greater than one in the Zone object are effectively double-multiplied.
+
+\begin{callout}
+NOTE: Although ZoneLists are not exclusive by themselves, ZoneLists used to form a ZoneGroup are exclusive; the ZoneLists used with a ZoneGroup must not have any zones in common.
+\end{callout}
+
+\subsubsection{Inputs}\label{inputs-2-042}
+
+\paragraph{Tips for Multi-Story Simulations:}\label{tips-for-multi-story-simulations}
+
+\begin{itemize}
+\item
+  For floors that are multiplied, connect exterior boundary conditions of the floor to the ceiling and vice versa.
+\item
+  Since exterior convection coefficients vary with elevation, locate the typical middle floor zones midheight between the lowest and highest middle floors to be modeled.
+\item
+  Shading must be identical for all multiplied floors or less accurate results may be obtained by using the zone list multiplier.
+\end{itemize}
+
+ZoneGroup and ZoneList can also be used to simulate other repetitive cases, such as clusters of zones on the ground.
+
+\paragraph{Field: Zone Group Name}\label{field-zone-group-name}
+
+The name of the ZoneGroup object. This must be unique across ZoneGroups.
+
+\paragraph{Field: Zone List Name}\label{field-zone-list-name-1}
+
+Reference to a ZoneList object. The zones in the list constitute the zones in the group.
+
+\paragraph{Field: Zone List Multiplier}\label{field-zone-list-multiplier}
+
+An integer multiplier. Zone List Multiplier is designed as a ``multiplier'' for floor area, zone loads, and energy consumed by internal gains. It takes the calculated load for the zone and multiplies it, sending the multiplied load to the attached HVAC system. The HVAC system size is specified to meet the entire multiplied zone load and will report the amount of the load met in the Zone Air System Sensible Heating or Cooling Energy/Rate output variable. Autosizing automatically accounts for multipliers. Metered energy consumption by internal gains objects such as Lights or Electric Equipment will be mutliplied. The default is 1.
+
+\begin{lstlisting}
+
+ZONE GROUP,
+    Mid Floor,  !- Zone Group Name
+    Mid Floor List,  !- Zone List Name
+    8;  !- Zone List Multiplier
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-023}
+
+The following output variables are reported by the ZoneGroup object:
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Group Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Group Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Group Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Group Sensible Cooling Energy {[}J{]}
+\end{itemize}
+
+All ZoneGroup variables report the associated ZoneList value multiplied by the \emph{Zone List Multiplier}.
+
+\subsection{Surface(s)}\label{surfaces}
+
+What's a building without surfaces?
+
+EnergyPlus allows for several surface types:
+
+\begin{itemize}
+\item
+  \textbf{BuildingSurface:Detailed}
+\item
+  \textbf{FenestrationSurface:Detailed}
+\item
+  \textbf{Shading:Site:Detailed}
+\item
+  \textbf{Shading:Building:Detailed}
+\item
+  \textbf{Shading:Zone:Detailed}
+\end{itemize}
+
+Each of the preceding surfaces has ``correct'' geometry specifications. BuildingSurface and Fenestration surfaces (heat transfer surfaces) are used to describe the important elements of the building (walls, roofs, floors, windows, doors) that will determine the interactions of the building surfaces with the outside environment parameters and the internal space requirements. These surfaces are also used to represent ``interzone'' heat transfer. All surfaces are modeled as a thin plane (with no thickness) except that material thicknesses are taken into account for heat transfer calculations.
+
+During specification of surfaces, several ``outside'' environments may be chosen:
+
+\begin{itemize}
+\item
+  \textbf{Ground} -- when the surface is in touch with the ground (e.g.~slab floors)
+\item
+  \textbf{Outdoors} -- when the surface is an external surface (e.g.~walls, roofs, windows directly exposed to the outdoor conditions)
+\item
+  \textbf{Surface} -- when the surface is
+  \begin{itemize}
+    \item
+      An adiabatic internal zone surface
+    \item
+      A interzone surface
+  \end{itemize}
+\item
+  \textbf{Zone --} when the surface is
+  \begin{itemize}
+    \item
+      A interzone surface in which the other surface is not put in the input file.
+  \end{itemize}
+\item
+  \textbf{OtherSideCoefficients} -- when using a custom profile to describe the external conditions of the surface (advanced concept -- covered in subject: SurfaceProperty:OtherSideCoefficients)
+\item
+  \textbf{OtherSideConditionsModel} -- when using specially modeled components, such as active solar systems, that cover the outside surface and modify the conditions it experiences.
+\end{itemize}
+
+\textbf{Surface} items must also specify an ``outside face object''. This is
+
+\begin{itemize}
+\tightlist
+\item
+  Current surface name -- for adiabatic internal surfaces.
+\item
+  A surface name in another zone -- for interzone heat transfer.
+\item
+  An ``opposing'' surface name (in the current zone) -- for representing ``middle'' zones.
+\end{itemize}
+
+\textbf{Zone} items must also specify an ``outside face object''. This is
+
+\begin{itemize}
+\tightlist
+\item
+  The zone that contains the other surface that is adjactent to this surface but is not entered in input.
+\end{itemize}
+
+\begin{callout}
+Note that heat transfer surfaces are fully represented with each description. As stated earlier in the Construction description, materials in the construction (outside to inside) are included but film coeffients neither inside nor outside are used in the description -- these are automatically calculated during the EnergyPlus run. Interzone surfaces which do not have a symmetrical construction (such as a ceiling/floor) require two Construction objects with the layers in reverse order. For example, CEILING with carpet, concrete, ceiling tile and FLOOR with ceiling tile, concrete, carpet. If interzone surfaces have a symmetrical construction, the specification for the two surfaces can reference the same Construction. When a surface is connected as the outside boundary condition for another surface, the two surfaces may be in the same plane, or they may be separated to imply thickness.
+\end{callout}
+
+\textbf{Shading} surfaces are used to describe aspects of the site which do not directly impact the physical interactions of the environmental parameters but may significantly shade the building during specific hours of the day or time so the year (e.g.~trees, bushes, mountains, nearby buildings which aren't being simulated as part of this facility, etc.)
+
+\begin{callout}
+Note that surfaces which are part of the simulated building automatically shade other parts of the building as geometry and time of day dictate -- there is no need on the user's part to include surfaces that might be in other zones for shading.
+\end{callout}
+
+Another surface type:
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{InternalMass}
+\end{itemize}
+
+is used to specify the construction/material parameters and area of items within the space that are important to heat transfer calculations but not necessarily important geometrically. (For example, furniture within the space -- particularly for large spaces). Internal mass can also be used for internal walls that are not needed (when FullInteriorAndExterior Solar Distribution is in effect) for solar distribution or to represent many, if not all, interior walls when solar is distributed to the floors only.
+
+\subsection{Interzone Surfaces}\label{interzone-surfaces}
+
+EnergyPlus can quite accurately simulate the surface heat exchange between two zones. However, this accuracy is not always required and using interzonal heat transfer does add to the complexity of the calculations -- thus requiring more CPU time to simulate. More information about interzonal heat transfer calculations is contained in the Engineering Reference. Some simple guidelines are presented here -- for three cases: adiabatic surfaces, surfaces in ``middle'' zones, and surfaces where heat transfer is ``expected'' (e.g.~between a residence and an unheated, attached garage).
+
+\begin{itemize}
+\item
+  Adiabatic Surfaces -- These surfaces would be represented as common surfaces (between two zones) where both zones are typically the same temperature. Thus, no transfer is expected in the surface from one zone to the next. These surfaces should be described as simply internal surfaces for the zone referencing as their Outside Boundary Condition Object (see later description in individual surface objects) their own surface names.
+\item
+  Surfaces in Middle Zones -- Middle zones in a building can be simulated using a judicious use of surfaces and zone multipliers to effect the correct ``loads'' for the building. Thus, middle zone behavior can be simulated without modeling the adjacent zones. This is done by specifying a surface within the zone. For example, a middle floor zone can be modeled by making the floor the Outside Boundary Condition Object for the ceiling, and the ceiling the Outside Boundary Condition Object for the floor.
+\item
+  Surfaces between Zones with differing temperatures -- These zones represent the true use of interzone surfaces. In a residence that has an attached garage, the garage may be unheated/uncooled or at least not conditioned to the same degree as the residence interior. In this case, EnergyPlus can be used to accurately calculate the effects of the differently conditioned space to the other spaces.
+\end{itemize}
+
+\subsection{Surface View Factors}\label{surface-view-factors}
+
+EnergyPlus uses an area weighted approximation to calculate ``view factors'' between surfaces within a thermal zone. Each surface uses the total area that it can ``see'' among the other surfaces. The approximate view factor from this surface to each other surface is then the area of the receiving surface over the sum of areas that is visible to the sending surface.
+
+In order to account in some limited way for the fact that certain surfaces will not see each other, several assumptions have been built into this simple view factor approximation. First, a surface cannot see itself. Second, surfaces with approximately the same azimuth (facing direction) and tilt (``same'' being within a built in limit) will not see each other. This means that a window will not see the wall that it is placed on, for example. Third, floors cannot see each other. Fourth, if the surface is a floor, ceiling, roof, or internal mass, the rule for the same azimuth and tilt eliminating radiant exchange between surface is waived when the receiving surface is floor, roof, ceiling, or internal mass as long as both surfaces are not floors.
+
+Note that this does not take into account that surfaces may be ``around the corner'' from each other and in reality not see each other at all. Rooms are assumed to be convex rather than concave in this method.
+
+To summarize, using the Surface ``Class'', the approximate view factors have:
+
+\begin{enumerate}
+\item
+  No surface sees itself.
+\item
+  No Floor sees another floor.
+\item
+  All other surface types see Internal Mass.
+\item
+  All other surface types see floors.
+\item
+  Floors always see ceilings.
+\item
+  Floors always see roofs.
+\item
+  All other surfaces whose tilt or facing angle differences are greater than 10 degrees see each other.
+\end{enumerate}
+
+If geometry is correct, conditions 1, 3, and 7 should take care of all surfaces, but the other conditions supply common sense when the geometry is incorrect. More information about the EnergyPlus view factor calculation is contained in the Engineering Reference document.
+
+\subsection{GlobalGeometryRules}\label{globalgeometryrules}
+
+Before the surface objects are explained in detail, a description of geometric parameters used in EnergyPlus will be given. Since the input of surface vertices is common to most of the surface types, it will also be given a separate discussion.
+
+Some flexibility is allowed in specifying surface vertices. This flexibility is embodied in the GlobalGeometryRules class/object in the input file. Note that the parameters specified in this statement are used for all surface vertice inputs -- there is no further ``flexibility'' allowed.
+
+In order to perform shadowing calculations, the building surfaces must be specified. EnergyPlus uses a three dimensional (3D) Cartesian coordinate system for surface vertex specification. This Right Hand coordinate system has the X-axis pointing east, the Y-axis pointing north, and the Z-axis pointing up. See figure below.
+
+\begin{figure}[hbtp] % fig 28
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image054.png}
+\caption{EnergyPlus Coordinate System \protect \label{fig:energyplus-coordinate-system}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-3-038}
+
+\paragraph{Field: Starting Vertex Position}\label{field-starting-vertex-position}
+
+The shadowing algorithms in EnergyPlus rely on surfaces having vertices in a certain order and positional structure. Thus, the surface translator needs to know the starting point for each surface entry. The choices are: UpperLeftCorner, LowerLeftCorner , UpperRightCorner, or LowerRightCorner. Since most surfaces will be 4 sided, the convention will specify this position as though each surface were 4 sided. Extrapolate 3 sided figures to this convention. For 5 and more sided figures, again, try to extrapolate the best ``corner'' starting position.
+
+\paragraph{Field: Vertex Entry Direction}\label{field-vertex-entry-direction}
+
+Surfaces are always specified as being viewed from the outside of the zone to which they belong. (Shading surfaces are specified slightly differently and are discussed under the particular types). EnergyPlus needs to know whether the surfaces are being specified in counterclockwise or clockwise order (from the Starting Vertex Position). EnergyPlus uses this to determine the outward facing normal for the surface (which is the \emph{facing angle} of the surface -- very important in shading and shadowing calculations.
+
+\paragraph{Field: Coordinate System}\label{field-coordinate-system}
+
+Vertices can be specified in two ways: using ``Absolute''/``World'' coordinates, or a \textbf{relative} coordinate specification. Relative coordinates allow flexibility of rapid change to observe changes in building results due to orientation and position. ``World'' coordinates will facilitate use within a CADD system structure.
+
+\textbf{Relative} coordinates make use of both Building and Zone North Axis values as well as Zone Origin values to locate the surface in 3D coordinate space. \textbf{World} coordinates do not use these values.
+
+Typically, all zone origin values for ``World'' coordinates will be (0,0,0) but Building and Zone North Axis values may be used in certain instances (namely the Daylighting Coordinate Location entries).
+
+\paragraph{Field: Daylighting Reference Point Coordinate System}\label{field-daylighting-reference-point-coordinate-system}
+
+Daylighting reference points need to be specified as well. Again, there can be two flavors; \textbf{relative} and \textbf{world}. Daylighting reference points must fit within the zone boundaries.
+
+\textbf{Relative} coordinates make use of both Building and Zone North Axis values as well as Zone Origin values to locate the reference point in 3D coordinate space. \textbf{World} coordinates do not use these values.
+
+\paragraph{Field: Rectangular Surface Coordinate System}\label{field-rectangular-surface-coordinate-system}
+
+Simple, rectangular surfaces (Wall:Exterior, Wall:Adiabatic, Wall:Underground, Wall:Interzone, Roof, Ceiling:Adiabatic, Ceiling:Interzone, Floor:GroundContact, Floor:Adiabatic, Floor:Interzone) can be specified with their Lower Left Corner as \textbf{relative} or \textbf{world}.
+
+\textbf{Relative} (default) corners are specified relative to the Zone Origin for each surface. \textbf{World} corners would specify the absolute/world coordinate for this corner.
+
+\subsection{Surfaces}\label{surfaces-1}
+
+Surfaces make up the buildings and the elements that shade buildings. There are several methods to inputting surfaces, ranging from simple rectangular surfaces to detailed descriptions that describe each vertex in the order specified in the GlobalGeometryRules object. The simple, rectangular surface objects are described first with the more detailed descriptions following.
+
+\subsection{Walls}\label{walls}
+
+Walls are usually vertical (tilt = 90 degrees). These objects are used to describe exterior walls, interior walls (adiabatic), underground walls, and walls adjacent to other zones.
+
+\subsection{Wall:Exterior}\label{wallexterior}
+
+The Wall:Exterior object is used to describe walls that are exposed to the external environment. They receive sun, wind -- all the characteristics of the external world.
+
+\subsubsection{Inputs}\label{inputs-4-035}
+
+\paragraph{Field: Name}\label{field-name-047}
+
+This is a unique name associated with the exterior wall. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-003}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-012}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Azimuth Angle}\label{field-azimuth-angle}
+
+The Azimuth Angle indicates the direction that the wall faces (outward normal). The angle is specified in degrees where East = 90, South = 180, West = 270, North = 0.
+
+\paragraph{Field: Tilt Angle}\label{field-tilt-angle}
+
+The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground). Normally, walls are tilted 90 degrees and that is the default for this field.
+
+\begin{callout}
+\textbf{Starting Corner for the surface}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
+\end{callout}
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Y Coordinate}\label{field-starting-y-coordinate}
+
+This field is the Y coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-000}
+
+This field is the length of the wall in meters.
+
+\paragraph{Field: Height}\label{field-height-000}
+
+This field is the height of the wall in meters.
+
+\subsection{Wall:Adiabatic}\label{walladiabatic}
+
+The Wall:Adiabatic object is used to describe interior walls and partitions. Adiabatic walls are used to describe walls next to zones that have the same thermal conditions (thus, no heat transfer).
+
+\subsubsection{Inputs}\label{inputs-5-032}
+
+\paragraph{Field: Name}\label{field-name-1-044}
+
+This is a unique name associated with the interior wall. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-1-001}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-009}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Azimuth Angle}\label{field-azimuth-angle-1}
+
+The Azimuth Angle indicates the direction that the wall faces (outward normal). The angle is specified in degrees where East = 90, South = 180, West = 270, North = 0.
+
+\paragraph{Field: Tilt Angle}\label{field-tilt-angle-1}
+
+The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground). Normally, walls are tilted 90 degrees and that is the default for this field.
+
+\begin{callout}
+\textbf{Starting Corner for the surface}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
+\end{callout}
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-1}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Y Coordinate}\label{field-starting-y-coordinate-1}
+
+This field is the Y coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-1}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-1}
+
+This field is the length of the wall in meters.
+
+\paragraph{Field: Height}\label{field-height-1}
+
+This field is the height of the wall in meters.
+
+\subsection{Wall:Underground}\label{wallunderground}
+
+The Wall:Underground object is used to describe walls with ground contact. The temperature at the outside of the wall is the temperature in the GroundTemperature:BuildingSurface object.
+
+\subsubsection{Inputs}\label{inputs-6-029}
+
+\paragraph{Field: Name}\label{field-name-2-039}
+
+This is a unique name associated with the underground wall. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-2-001}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones. Note that if the construction is \textbf{Construction:CfactorUndergroundWall} then the GroundFCfactoreMethod will be used for this wall.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-2-007}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Azimuth Angle}\label{field-azimuth-angle-2}
+
+The Azimuth Angle indicates the direction that the wall faces (outward normal). The angle is specified in degrees where East = 90, South = 180, West = 270, North = 0.
+
+\paragraph{Field: Tilt Angle}\label{field-tilt-angle-2}
+
+The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground). Normally, walls are tilted 90 degrees and that is the default for this field.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-2}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-2}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Y Coordinate}\label{field-starting-y-coordinate-2}
+
+This field is the Y coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-2}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-2}
+
+This field is the length of the wall in meters.
+
+\paragraph{Field: Height}\label{field-height-2}
+
+This field is the height of the wall in meters.
+
+\subsection{Wall:Interzone}\label{wallinterzone}
+
+The Wall:Interzone object is used to describe walls adjacent to zones that are significantly different conditions than the zone with this wall.
+
+\subsubsection{Inputs}\label{inputs-7-028}
+
+\paragraph{Field: Name}\label{field-name-3-033}
+
+This is a unique name associated with the interzone wall. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-3}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-3-006}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object}
+
+The Outside Boundary Condition Object field is the name of a wall in an adjacent zone or the name of the adjacent zone. If the adjacent zone option is used, the adjacent wall is automatically generated in the adjacent zone. If the surface name is used, it must be in the adjacent zone.
+
+\paragraph{Field: Azimuth Angle}\label{field-azimuth-angle-3}
+
+The Azimuth Angle indicates the direction that the wall faces (outward normal). The angle is specified in degrees where East = 90, South = 180, West = 270, North = 0.
+
+\paragraph{Field: Tilt Angle}\label{field-tilt-angle-3}
+
+The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground). Normally, walls are tilted 90 degrees and that is the default for this field.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-3}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-3}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Y Coordinate}\label{field-starting-y-coordinate-3}
+
+This field is the Y coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-3}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-3}
+
+This field is the length of the wall in meters.
+
+\paragraph{Field: Height}\label{field-height-3}
+
+This field is the height of the wall in meters.
+
+\subsection{Roofs/Ceilings}\label{roofsceilings}
+
+Roofs and ceilings are, by default, flat (tilt = 0 degrees). These objects are used to describe roofs, interior ceilings (adiabatic) and ceilings adjacent to other zones.
+
+\subsection{Roof}\label{roof}
+
+The Roof object is used to describe roofs that are exposed to the external environment.
+
+\subsubsection{Inputs}\label{inputs-8-026}
+
+\paragraph{Field: Name}\label{field-name-4-030}
+
+This is a unique name associated with the roof. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-4}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-4-006}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Azimuth Angle}\label{field-azimuth-angle-4}
+
+The Azimuth Angle indicates the direction of the outward normal for the roof. The angle is specified in degrees where East = 90, South = 180, West = 270, North = 0.
+
+\paragraph{Field: Tilt Angle}\label{field-tilt-angle-4}
+
+The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground). Flat roofs are tilted 0 degrees and that is the default for this field.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-4}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-4}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Y Coordinate}\label{field-starting-y-coordinate-4}
+
+This field is the Y coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-4}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-4}
+
+This field is the length of the roof in meters.
+
+\paragraph{Field: Width}\label{field-width}
+
+This field is the width of the roof in meters.
+
+\subsection{Ceiling:Adiabatic}\label{ceilingadiabatic}
+
+The Ceiling:Adiabatic object is used to describe interior ceilings that separate zones of like conditions.
+
+\subsubsection{Inputs}\label{inputs-9-024}
+
+\paragraph{Field: Name}\label{field-name-5-026}
+
+This is a unique name associated with the ceiling. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-5}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-5-005}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Azimuth Angle}\label{field-azimuth-angle-5}
+
+The Azimuth Angle indicates the direction of the outward normal for the roof. The angle is specified in degrees where East = 90, South = 180, West = 270, North = 0.
+
+\paragraph{Field: Tilt Angle}\label{field-tilt-angle-5}
+
+The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground). Flat ceilings are tilted 0 degrees and that is the default for this field.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-5}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-5}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Y Coordinate}\label{field-starting-y-coordinate-5}
+
+This field is the Y coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-5}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-5}
+
+This field is the length of the ceiling in meters.
+
+\paragraph{Field: Width}\label{field-width-1}
+
+This field is the width of the ceiling in meters.
+
+\subsection{Ceiling:Interzone}\label{ceilinginterzone}
+
+The Ceiling:Interzone object is used to describe interior ceilings that separate zones of differing conditions (and expect heat transfer through the ceiling from the adjacent zone).
+
+\subsubsection{Inputs}\label{inputs-10-022}
+
+\paragraph{Field: Name}\label{field-name-6-024}
+
+This is a unique name associated with the interzone ceiling. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-6}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-6-004}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object-1}
+
+The Outside Boundary Condition Object field is the name of a floor in an adjacent zone or the name of the adjacent zone. If the adjacent zone option is used, the adjacent floor is automatically generated in the adjacent zone. If the surface name is used, it must be in the adjacent zone.
+
+\paragraph{Field: Azimuth Angle}\label{field-azimuth-angle-6}
+
+The Azimuth Angle indicates the direction of the outward normal for the roof. The angle is specified in degrees where East = 90, South = 180, West = 270, North = 0.
+
+\paragraph{Field: Tilt Angle}\label{field-tilt-angle-6}
+
+The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground). Flat ceilings are tilted 0 degrees and that is the default for this field.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-6}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-6}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Y Coordinate}\label{field-starting-y-coordinate-6}
+
+This field is the Y coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-6}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-6}
+
+This field is the length of the ceiling in meters.
+
+\paragraph{Field: Width}\label{field-width-2}
+
+This field is the width of the ceiling in meters.
+
+\subsection{Floors}\label{floors}
+
+Floors are, by default, flat (tilt = 180 degrees). These objects are used to describe floors on the ground, interior floors (adiabatic) and floors adjacent to other zones.
+
+\subsection{Floor:GroundContact}\label{floorgroundcontact}
+
+The Floor:GroundContact object is used to describe floors that have ground contact (usually called slabs). The temperature at the outside of the floor is the temperature in the GroundTemperature:BuildingSurface object.
+
+\subsubsection{Inputs}\label{inputs-11-021}
+
+\paragraph{Field: Name}\label{field-name-7-022}
+
+This is a unique name associated with the floor.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-7}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones. Note that if the construction is \textbf{Construction:FfactorGroundFloor,} then the GroundFCfactorMethod will be used with this floor.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-7-004}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Azimuth Angle}\label{field-azimuth-angle-7}
+
+The Azimuth Angle indicates the direction of the outward normal for the roof. The angle is specified in degrees where East = 90, South = 180, West = 270, North = 0.
+
+\paragraph{Field: Tilt Angle}\label{field-tilt-angle-7}
+
+The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground). Flat floors are tilted 180 degrees and that is the default for this field.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-7}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-7}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Y Coordinate}\label{field-starting-y-coordinate-7}
+
+This field is the Y coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-7}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-7}
+
+This field is the length of the floor in meters.
+
+\paragraph{Field: Width}\label{field-width-3}
+
+This field is the width of the floor in meters.
+
+\subsection{Floor:Adiabatic}\label{flooradiabatic}
+
+The Floor:Adiabatict object is used to describe interior floors or floors that you wish to model with no heat transfer from the exterior to the floor.
+
+\subsubsection{Inputs}\label{inputs-12-019}
+
+\paragraph{Field: Name}\label{field-name-8-022}
+
+This is a unique name associated with the floor.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-8}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-8-003}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Azimuth Angle}\label{field-azimuth-angle-8}
+
+The Azimuth Angle indicates the direction of the outward normal for the roof. The angle is specified in degrees where East = 90, South = 180, West = 270, North = 0.
+
+\paragraph{Field: Tilt Angle}\label{field-tilt-angle-8}
+
+The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground). Flat floors are tilted 180 degrees and that is the default for this field.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-8}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-8}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Y Coordinate}\label{field-starting-y-coordinate-8}
+
+This field is the Y coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-8}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-8}
+
+This field is the length of the floor in meters.
+
+\paragraph{Field: Width}\label{field-width-4}
+
+This field is the width of the floor in meters.
+
+\subsection{Floor:Interzone}\label{floorinterzone}
+
+The Floor:Interzone object is used to describe floors that are adjacent to other zones that have differing conditions and you wish to model the heat transfer through the floor.
+
+\subsubsection{Inputs}\label{inputs-13-016}
+
+\paragraph{Field: Name}\label{field-name-9-019}
+
+This is a unique name associated with the floor.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-9}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-9-001}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object-2}
+
+The Outside Boundary Condition Object field is the name of a ceiling in an adjacent zone or the name of the adjacent zone. If the adjacent zone option is used, the adjacent ceiling is automatically generated in the adjacent zone. If the surface name is used, it must be in the adjacent zone.
+
+\paragraph{Field: Azimuth Angle}\label{field-azimuth-angle-9}
+
+The Azimuth Angle indicates the direction of the outward normal for the roof. The angle is specified in degrees where East = 90, South = 180, West = 270, North = 0.
+
+\paragraph{Field: Tilt Angle}\label{field-tilt-angle-9}
+
+The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground). Flat floors are tilted 180 degrees and that is the default for this field.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-9}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-9}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Y Coordinate}\label{field-starting-y-coordinate-9}
+
+This field is the Y coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-9}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-9}
+
+This field is the length of the floor in meters.
+
+\paragraph{Field: Width}\label{field-width-5}
+
+This field is the width of the floor in meters.
+
+\subsection{Windows/Doors}\label{windowsdoors}
+
+The following window and door objects can be used to specify simple, rectangular doors and windows. In each case, the lower left corner (locator coordinate) of the window or door is specified \textbf{relative} to the surface it is on. Viewing the base surface as a planar surface, base the relative location from the lower left corner of the base surface. Vertex entry description as well as provisions for a few other surface types can be entered with the FenestrationSurface:Detailed object.
+
+\subsection{Window}\label{window}
+
+The Window object is used to place windows on surfaces that can have windows, including exterior walls, interior walls, interzone walls, roofs, floors that are exposed to outdoor conditions, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
+
+\subsubsection{Inputs}\label{inputs-14-016}
+
+\paragraph{Field: Name}\label{field-name-10-018}
+
+This is a unique name associated with the window.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-10}
+
+This is the name of the subsurface's construction (ref: objects: Construction, Construction:WindowDataFile, Construction:CompexFenestrationState).
+
+For windows, if Construction Name is not found among the constructions on the input (.idf) file, the Window Data File (ref. Construction:WindowDataFile object) will be searched for that Construction Name (see ``Importing Windows from WINDOW''). If that file is not present or if the Construction Name does not match the name of an entry on the file, an error will result. If there is a match, a window construction and its corresponding glass and gas materials will be created from the information read from the file.
+
+\paragraph{Field: Building Surface Name}\label{field-building-surface-name-000}
+
+This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. For example, a surface in contact with the ground (e.g., Outside Boundary Condition = Ground) cannot contain a window. The window assumes the outward facing angle as well as the tilt angle of the base surface.
+
+\paragraph{Field: Shading Control Name}\label{field-shading-control-name}
+
+This field, if not blank, is the name of the window shading control (ref: WindowProperty:ShadingControl object) for this subsurface. It is used for Surface Type = Window and GlassDoor. To assign a shade to a window or glass door, see WindowMaterial: Shade. To assign a screen, see WindowMaterial:Screen. To assign a blind, see WindowMaterial:Blind. To assign switchable glazing, such as electrochromic glazing, see WindowProperty:ShadingControl.
+
+\paragraph{Field: Frame and Divider Name}\label{field-frame-and-divider-name}
+
+This field, if not blank, can be used to specify window frame, divider and reveal-surface data (ref: WindowProperty:FrameAndDivider object). It is used only for exterior GlassDoors and rectangular exterior Windows, i.e., those with OutsideFaceEnvironment = Outdoors.
+
+This field should be blank for triangular windows.
+
+\paragraph{Field: Multiplier}\label{field-multiplier-1}
+
+This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
+
+Multiplier should be used with caution. Multiplier \textgreater{} 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
+
+If Multiplier \textgreater{} 1, you will get
+
+--a \emph{warning} if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
+
+--an \emph{error} if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-10}
+
+The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate. This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-10}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-10}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-10}
+
+This field is the length of the window in meters.
+
+\paragraph{Field: Height}\label{field-height-4}
+
+This field is the height of the window in meters.
+
+\subsection{Door}\label{door}
+
+The Door object is used to place opaque doors on surfaces that can have doors, including exterior walls, interior walls, interzone walls, roofs, floors that are exposed to outdoor conditions, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
+
+\subsubsection{Inputs}\label{inputs-15-016}
+
+\paragraph{Field: Name}\label{field-name-11-015}
+
+This is a unique name associated with the door.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-11}
+
+This is the name of the subsurface's construction (ref: Construction object)
+
+\paragraph{Field: Building Surface Name}\label{field-building-surface-name-1}
+
+This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. The door assumes the outward facing angle as well as the tilt angle of the base surface.
+
+\paragraph{Field: Multiplier}\label{field-multiplier-2}
+
+This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
+
+Multiplier should be used with caution. Multiplier \textgreater{} 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
+
+If Multiplier \textgreater{} 1, you will get
+
+--a \emph{warning} if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
+
+--an \emph{error} if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-11}
+
+The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate. This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-11}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-11}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-11}
+
+This field is the length of the door in meters.
+
+\paragraph{Field: Height}\label{field-height-5}
+
+This field is the height of the door in meters.
+
+\subsection{GlazedDoor}\label{glazeddoor}
+
+The GlazedDoor object is used to place doors on surfaces that can have doors, including exterior walls, interior walls, interzone walls, roofs, floors that are exposed to outdoor conditions, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
+
+\subsubsection{Inputs}\label{inputs-16-012}
+
+\paragraph{Field: Name}\label{field-name-12-012}
+
+This is a unique name associated with the glass door.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-12}
+
+This is the name of the subsurface's construction (ref: objects: Construction, Construction:WindowDataFile, Construction:CompexFenestrationState).
+
+For windows, if Construction Name is not found among the constructions on the input (.idf) file, the Window Data File (ref. Construction:WindowDataFile object) will be searched for that Construction Name (see ``Importing Windows from WINDOW''). If that file is not present or if the Construction Name does not match the name of an entry on the file, an error will result. If there is a match, a window construction and its corresponding glass and gas materials will be created from the information read from the file.
+
+\paragraph{Field: Building Surface Name}\label{field-building-surface-name-2}
+
+This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. For example, a surface in contact with the ground (Outside Boundary Condition = Ground) cannot contain a window. The door assumes the outward facing angle as well as the tilt angle of the base surface.
+
+\paragraph{Field: Shading Control Name}\label{field-shading-control-name-1}
+
+This field, if not blank, is the name of the window shading control (ref: WindowProperty:ShadingControl object) for this subsurface. It is used for Surface Type = Window and GlassDoor. To assign a shade to a window or glass door, see WindowMaterial: Shade. To assign a screen, see WindowMaterial:Screen. To assign a blind, see WindowMaterial:Blind. To assign switchable glazing, such as electrochromic glazing, see WindowProperty:ShadingControl.
+
+\paragraph{Field: Frame and Divider Name}\label{field-frame-and-divider-name-1}
+
+This field, if not blank, can be used to specify window frame, divider and reveal-surface data (ref: WindowProperty:FrameAndDivider object). It is used only for exterior GlassDoors and rectangular exterior Windows, i.e., those with OutsideFaceEnvironment = Outdoors.
+
+This field should be blank for triangular windows.
+
+\paragraph{Field: Multiplier}\label{field-multiplier-3}
+
+This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
+
+Multiplier should be used with caution. Multiplier \textgreater{} 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
+
+If Multiplier \textgreater{} 1, you will get
+
+--a \emph{warning} if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
+
+--an \emph{error} if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-12}
+
+The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate. This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-12}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-12}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-12}
+
+This field is the length of the door in meters.
+
+\paragraph{Field: Height}\label{field-height-6}
+
+This field is the height of the door in meters.
+
+\subsection{Window:Interzone}\label{windowinterzone}
+
+The Window:Interzone object is used to place windows on surfaces that can have windows, including interzone walls, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
+
+\subsubsection{Inputs}\label{inputs-17-010}
+
+\paragraph{Field: Name}\label{field-name-13-011}
+
+This is a unique name associated with the window.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-13}
+
+This is the name of the subsurface's construction (ref: objects: Construction, Construction:WindowDataFile, Construction:CompexFenestrationState).
+
+For windows, if Construction Name is not found among the constructions on the input (.idf) file, the Window Data File (ref. Construction:WindowDataFile object) will be searched for that Construction Name (see ``Importing Windows from WINDOW''). If that file is not present or if the Construction Name does not match the name of an entry on the file, an error will result. If there is a match, a window construction and its corresponding glass and gas materials will be created from the information read from the file.
+
+\paragraph{Field: Building Surface Name}\label{field-building-surface-name-3}
+
+This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. For example, a surface in contact with the ground (Outside Boundary Condition = Ground) cannot contain a window. The window assumes the outward facing angle as well as the tilt angle of the base surface.
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object-3}
+
+The Outside Boundary Condition Object field is the name of a window in an adjacent zone or the name of the adjacent zone. If the adjacent zone option is used, the adjacent ceiling is automatically generated in the adjacent zone. If the surface name is used, it must be in the adjacent zone.
+
+\paragraph{Field: Multiplier}\label{field-multiplier-4}
+
+This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
+
+Multiplier should be used with caution. Multiplier \textgreater{} 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
+
+If Multiplier \textgreater{} 1, you will get
+
+--a \emph{warning} if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
+
+--an \emph{error} if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-13}
+
+The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate. This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-13}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-13}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-13}
+
+This field is the length of the window in meters.
+
+\paragraph{Field: Height}\label{field-height-7}
+
+This field is the height of the window in meters.
+
+\subsection{Door:Interzone}\label{doorinterzone}
+
+The Door:Interzone object is used to place opaque doors on surfaces that can have doors, including interzone walls, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
+
+\subsubsection{Inputs}\label{inputs-18-010}
+
+\paragraph{Field: Name}\label{field-name-14-010}
+
+This is a unique name associated with the door.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-14}
+
+This is the name of the subsurface's construction (ref: Construction object).
+
+\paragraph{Field: Building Surface Name}\label{field-building-surface-name-4}
+
+This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. The door assumes the outward facing angle as well as the tilt angle of the base surface.
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object-4}
+
+The Outside Boundary Condition Object field is the name of a door in an adjacent zone or the name of the adjacent zone. If the adjacent zone option is used, the adjacent ceiling is automatically generated in the adjacent zone. If the surface name is used, it must be in the adjacent zone.
+
+\paragraph{Field: Multiplier}\label{field-multiplier-5}
+
+This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
+
+Multiplier should be used with caution. Multiplier \textgreater{} 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
+
+If Multiplier \textgreater{} 1, you will get
+
+--a \emph{warning} if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
+
+--an \emph{error} if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-14}
+
+The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate. This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-14}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-14}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-14}
+
+This field is the length of the door in meters.
+
+\paragraph{Field: Height}\label{field-height-8}
+
+This field is the height of the door in meters.
+
+\subsection{GlazedDoor:Interzone}\label{glazeddoorinterzone}
+
+The GlazedDoor:Interzone object is used to place doors on surfaces that can have doors, including interzone walls, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
+
+\subsubsection{Inputs}\label{inputs-19-007}
+
+\paragraph{Field: Name}\label{field-name-15-010}
+
+This is a unique name associated with the glass door.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-15}
+
+This is the name of the subsurface's construction (ref: objects: Construction, Construction:WindowDataFile, Construction:ComplexFenestrationState).
+
+For windows, if Construction Name is not found among the constructions on the input (.idf) file, the Window Data File (ref. Construction:WindowDataFile object) will be searched for that Construction Name (see ``Importing Windows from WINDOW''). If that file is not present or if the Construction Name does not match the name of an entry on the file, an error will result. If there is a match, a window construction and its corresponding glass and gas materials will be created from the information read from the file.
+
+\paragraph{Field: Building Surface Name}\label{field-building-surface-name-5}
+
+This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. For example, a surface in contact with the ground (Outside Boundary Condition = Ground) cannot contain a window. The door assumes the outward facing angle as well as the tilt angle of the base surface.
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object-5}
+
+The Outside Boundary Condition Object field is the name of a glazed (glass) door in an adjacent zone or the name of the adjacent zone. If the adjacent zone option is used, the adjacent ceiling is automatically generated in the adjacent zone. If the surface name is used, it must be in the adjacent zone.
+
+\paragraph{Field: Multiplier}\label{field-multiplier-6}
+
+This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
+
+Multiplier should be used with caution. Multiplier \textgreater{} 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
+
+If Multiplier \textgreater{} 1, you will get
+
+--a \emph{warning} if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
+
+--an \emph{error} if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
+
+\paragraph{Starting Corner for the surface}\label{starting-corner-for-the-surface-15}
+
+The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate. This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
+
+\paragraph{Field: Starting X Coordinate}\label{field-starting-x-coordinate-15}
+
+This field is the X coordinate (in meters).
+
+\paragraph{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-15}
+
+This field is the Z coordinate (in meters).
+
+\paragraph{Field: Length}\label{field-length-15}
+
+This field is the length of the door in meters.
+
+\paragraph{Field: Height}\label{field-height-9}
+
+This field is the height of the door in meters.
+
+Examples of the rectangular surfaces are found in the example files 4ZoneWithShading\_Simple\_1.idf and 4ZoneWithShading\_Simple\_2. Some examples:
+
+\begin{lstlisting}
+
+  Wall:Exterior,
+      Zn001:Wall001,           !- Name
+      EXTERIOR,                !- Construction Name
+      ZONE 1,                  !- Zone Name
+      180,                     !- Azimuth Angle {deg}
+      90,                      !- Tilt Angle {deg}
+      0,                       !- Starting X Coordinate {m}
+      0,                       !- Starting Y Coordinate {m}
+      0,                       !- Starting Z Coordinate {m}
+      20,                      !- Length {m}
+      10;                      !- Height {m}
+
+    Window,
+      Zn001:Wall001:Win001,    !- Name
+      SINGLE PANE HW WINDOW,   !- Construction Name
+      Zn001:Wall001,           !- Building Surface Name
+      ,                        !- Shading Control Name
+      ,                        !- Frame and Divider Name
+      1,                       !- Multiplier
+      4,                       !- Starting X Coordinate {m}
+      3,                       !- Starting Z Coordinate {m}
+      3,                       !- Length {m}
+      5;                       !- Height {m}
+
+    Door,
+      Zn001:Wall001:Door001,   !- Name
+      HOLLOW WOOD DOOR,        !- Construction Name
+      Zn001:Wall001,           !- Building Surface Name
+      1,                       !- Multiplier
+      14,                      !- Starting X Coordinate {m}
+      0,                       !- Starting Z Coordinate {m}
+      3,                       !- Length {m}
+      5;                       !- Height {m}
+
+    Wall:Adiabatic,
+      Zn001:Wall004,           !- Name
+      INTERIOR,                !- Construction Name
+      ZONE 1,                  !- Zone Name
+      90,                      !- Azimuth Angle {deg}
+      90,                      !- Tilt Angle {deg}
+      20,                      !- Starting X Coordinate {m}
+      0,                       !- Starting Y Coordinate {m}
+      0,                       !- Starting Z Coordinate {m}
+      20,                      !- Length {m}
+      10;                      !- Height {m}
+
+    Floor:Adiabatic,
+      Zn001:Flr001,            !- Name
+      FLOOR,                   !- Construction Name
+      ZONE 1,                  !- Zone Name
+      90,                      !- Azimuth Angle {deg}
+      180,                     !- Tilt Angle {deg}
+      0,                       !- Starting X Coordinate {m}
+      0,                       !- Starting Y Coordinate {m}
+      0,                       !- Starting Z Coordinate {m}
+      20,                      !- Length {m}
+      20;                      !- Width {m}
+
+    Ceiling:Interzone,
+      Zn001:Roof001,           !- Name
+      CEILING34,               !- Construction Name
+      ZONE 1,                  !- Zone Name
+      Zn003:Flr001,            !- Outside Boundary Condition Object
+      180,                     !- Azimuth Angle {deg}
+      0,                       !- Tilt Angle {deg}
+      0,                       !- Starting X Coordinate {m}
+      0,                       !- Starting Y Coordinate {m}
+      10,                      !- Starting Z Coordinate {m}
+      20,                      !- Length {m}
+      20;                      !- Width {m}
+
+    Window,
+      Zn002:Wall001:Win001,    !- Name
+      SINGLE PANE HW WINDOW,   !- Construction Name
+      Zn002:Wall001,           !- Building Surface Name
+      ,                        !- Shading Control Name
+      ,                        !- Frame and Divider Name
+      1,                       !- Multiplier
+      4,                       !- Starting X Coordinate {m}
+      3,                       !- Starting Z Coordinate {m}
+      3,                       !- Length {m}
+      5;                       !- Height {m}
+\end{lstlisting}
+
+\subsection{Surface Vertices}\label{surface-vertices}
+
+Each of the following surfaces:
+
+\begin{itemize}
+\item
+  BuildingSurface:Detailed
+\item
+  Wall:Detailed
+\item
+  RoofCeiling:Detailed
+\item
+  Floor:Detailed
+\item
+  FenstrationSurface:Detailed
+\item
+  Shading:Site:Detailed
+\item
+  Shading:Building:Detailed
+\item
+  Shading:Zone:Detailed
+\end{itemize}
+
+use the same vertex input. The numeric parameters indicated below are taken from the BuildingSurface:Detailed definition; the others may not be exactly the same but are identical in configuration. They are also ``extensible'' -- so, if you want more vertices for these surfaces, you may add to the IDD definition as indicated in the ``extensible'' comment or, as EnergyPlus is ``auto-extensible'' just add the number of vertices into your input file.. Note that FenestrationSurface:Detailed is not extensible and is limited to 4 (max) vertices. If you leave the Number of Surface Vertex groups blank or enter \textbf{autocalculate}, EnergyPlus looks at the number of groups entered and figures out how many coordinate groups are entered.
+
+\begin{callout}
+\warning{Note that the resolution on the surface vertex input is 1 millimeter (.001 meter). Therefore, using vertices that are very close together (\textless{} 1 mm) may result in invalid dot product and fatal errors during shading calculations.}
+\end{callout}
+
+\begin{figure}[hbtp] % fig 29
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image055.png}
+\caption{Illustration for Surface Vertices \protect \label{fig:illustration-for-surface-vertices}}
+\end{figure}
+
+The figure above will help illustrate Surface Vertex entry. The convention used in ``GlobalGeometryRules'' dictates the order of the vertices (ref: GlobalGeometryRules). In this example, the conventions used are Starting Vertex Position = UpperLeftCorner and Vertex Entry Direction = CounterClockwise. The surfaces for this single zone are:
+
+\begin{lstlisting}
+4,0,0,H, 0,0,0, A,0,0, A,0,H; ! (4 vertices, South Wall)
+4,A,0,H,A,0,0,A,B,0,A,B,H; ! (4 vertices, East Wall)
+     ignore other walls that are not shown in this figure
+4,C,0,J,A,0,H,A,B,H,C,B,J; ! (4 vertices, roof)
+3,C,0,J,0,0,H,A,0,H; ! (3 vertices, gable end)
+4,0,0,H, 0,0,0, A,0,0, A,0,H; ! (4 vertices, South Wall)
+\end{lstlisting}
+
+Note that in this example, point 1 of the entry is the Upper Left Corner of the rectangular surfaces and the point of the triangle for the 3 sided surface. The east wall shows the order of vertex entry. For horizontal surfaces, any vertex may be chosen as the starting position, but the Vertex Entry Direction convention must be followed. The surface details report (Output: Surfaces:List, Details;) is very useful for reviewing the accuracy of surface geometry inputs (ref: Surface Output Variables/Reports and Variable Dictionary Reports).
+
+From the detailed vertices, EnergyPlus tries to determine the ``height'' and ``width'' of the surface. Obviously, this doesn't work well for \textgreater{}4 sided surfaces; for these, if the calculated height and width are not close to the gross area for the surface, the height and width shown will be the square root of the area (and thus a square).
+
+\subsection{Building Surfaces - Detailed}\label{building-surfaces---detailed}
+
+A building surface is necessary for all calculations. There must be at least one building surface per zone. You can use the detailed descriptions as shown below or the simpler, rectangular surface descriptions shown earlier.
+
+\subsection{Wall:Detailed}\label{walldetailed}
+
+The Wall:Detailed object is used to describe walls.
+
+\subsubsection{Inputs}\label{inputs-20-007}
+
+\paragraph{Field: Name}\label{field-name-16-010}
+
+This is a unique name associated with each building surface. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-16}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-10-000}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Outside Boundary Condition}\label{field-outside-boundary-condition}
+
+This value can be one of several things depending on the actual kind of surface.
+
+\begin{enumerate}
+  \item
+    \textbf{Surface} -- if this surface is an internal surface, then this is the choice. The value will either be a surface in the base zone or a surface in another zone. The heat balance between two zones can be accurately simulated by specifying a surface in an adjacent zone. EnergyPlus will simulate a group of zones simultaneously and will include the heat transfer between zones. However, as this increases the complexity of the calculations, it is not necessary to specify the other zone unless the two zones will have a significant temperature difference. If the two zones will not be very different (temperature wise), then the surface should use itself as the outside environment or specify this field as \textbf{Adiabatic}. The surface name on the ``outside'' of this surface (adjacent to) is placed in the next field.
+  \item
+    \textbf{Adiabatic} -- an internal surface in the same Zone. This surface will not transfer heat out of the zone, but will still store heat in thermal mass. Only the inside face of the surface will exchange heat with the zone (i.e.~two adiabatic surfaces are required to model internal partitions where both sides of the surface are exchanging heat with the zone). The Outside Boundary Condition Object can be left blank.
+  \item
+    \textbf{Zone} -- this is similar to Surface but EnergyPlus will automatically create the required surface in the adjacent zone when this is entered for the surface. If there are windows or doors on the surface, EnergyPlus automatically creates appropriate sub-surfaces as well.
+  \item
+    \textbf{Outdoors} -- if this surface is exposed to outside temperature conditions, then this is the choice. See Sun Exposure and Wind Exposure below for further specifications on this kind of surface.
+  \item
+    \textbf{Ground} -- if this surface is exposed to the ground, then this is the usual choice. The temperature on the outside of this surface will be the Site:GroundTemperature:Surface value for the month. For more information on ground contact surfaces, reference the Auxiliary Programs document section on ``Ground Heat Transfer in EnergyPlus''.
+  \item
+    \textbf{GroundFCfactorMethod} -- if this surface is exposed to the ground and using the \textbf{Construction:CfactorUndergroundWall}, then this is the choice. The temperature on the outside of this surface will be the Site:GroundTemperature:FcfactorMethod value for the month.
+  \item
+    \textbf{OtherSideCoefficients} -- if this surface has a custom, user specified temperature or other parameters (See SurfaceProperty:OtherSideCoefficients specification), then this is the choice. The outside boundary condition will be the name of the SurfaceProperty:OtherSideCoefficients specification.
+  \item
+    \textbf{OtherSideConditionsModel} -- if this surface has a specially-modeled multi-skin component, such as a transpired collector or vented photovoltaic panel, attached to the outside (See SurfaceProperty:OtherSideConditionsModel specification), then this the choice. The outside face environment will be the name of the SurfaceProperty:OtherSideConditionsModelspecification.
+  \item
+    \textbf{GroundSlabPreprocessorAverage} -- uses the average results from the Slab preprocessor calculations.
+  \item
+    \textbf{GroundSlabPreprocessorCore} -- uses the core results from the Slab preprocessor calculations.
+  \item
+    \textbf{GroundSlabPreprocessorPerimeter} -- uses the perimeter results from the Slab preprocessor calculations.
+  \item
+    \textbf{GroundBasementPreprocessorAverageWall} -- uses the average wall results from the Basement preprocessor calculations.
+  \item
+    \textbf{GroundBasementPreprocessorAverageFloor} -- uses the average floor results from the Basement preprocessor calculations.
+  \item
+    \textbf{GroundBasementPreprocessorUpperWall} -- uses the upper wall results from the Basement preprocessor calculations.
+  \item
+    \textbf{GroundBasementPreprocessorLowerWall} -- uses the lower wall results from the Basement preprocessor calculations.
+\end{enumerate}
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object-6}
+
+If neither Surface, OtherSideCoefficients, or OtherSideConditionsModel are specified for the Outside Boundary Condition (previous field), then this field should be left blank.
+
+As stated above, if the Outside Boundary Condition is ``Surface'', then this field's value must be the surface name whose inside face temperature will be forced on the outside face of the base surface. This permits heat exchange between adjacent zones (interzone heat transfer) when multiple zones are simulated, but can also be used to simulate middle zone behavior without modeling the adjacent zones. This is done by specifying a surface within the zone. For example, a middle floor zone can be modeled by making the floor the Outside Boundary Condition Object for the ceiling, and the ceiling the Outside Boundary Condition Object for the floor.
+
+If the Outside Boundary Condition is Zone, then this field should contain the zone name of the adjacent zone for the surface.
+
+\begin{callout}
+Note: Zones with interzone heat transfer are not adiabatic and the internal surfaces contribute to gains or losses. Adiabatic surfaces are modeled by specifying the base surface itself in this field. Also, for interzone heat transfer, both surfaces must be represented -- for example, if you want interzone heat transfer to an attic space, the ceiling in the lower zone must have a surface object with the outside face environment as the floor in the attic and, likewise, there must be a floor surface object in the attic that references the ceiling surface name in the lower zone.
+\end{callout}
+
+Equally, if the Outside Boundary Condition is ``OtherSideCoefficients'', then this field's value must be the SurfaceProperty:OtherSideCoefficients name. Or if the Outside Boundary Condition is ``OtherSideConditionsModel'' then this field's value must be the SurfaceProperty:OtherSideConditionsModel name.
+
+\paragraph{Field: Sun Exposure}\label{field-sun-exposure-000}
+
+If the surface is exposed to the sun, then ``SunExposed'' should be entered in this field. Otherwise, ``NoSun'' should be entered.
+
+Note, a cantilevered floor could have ``Outdoors'' but ``NoSun'' exposure.
+
+\paragraph{Field: Wind Exposure}\label{field-wind-exposure}
+
+If the surface is exposed to the Wind, then ``WindExposed'' should be entered in this field. Otherwise, ``NoWind'' should be entered.
+
+\begin{callout}
+Note: When a surface is specified with ``NoWind'', this has several implications. Within the heat balance code, this surface will default to using the simple ASHRAE exterior convection coefficient correlation with a zero wind speed. In addition, since the ASHRAE simple method does not have a separate value for equivalent long wavelength radiation to the sky and ground, using ``NoWind'' also eliminates long wavelength radiant exchange from the exterior of the surface to both the sky and the ground. Thus, only simple convection takes place at the exterior face of a surface specified with ``NoWind''.
+\end{callout}
+
+\paragraph{Field: View Factor to Ground}\label{field-view-factor-to-ground}
+
+The fraction of the ground plane (assumed horizontal) that is visible from a heat-transfer surface. It is used to calculate the diffuse solar radiation from the ground that is incident on the surface.
+
+For example, if there are no obstructions, a vertical surface sees half of the ground plane and so View Factor to Ground = 0.5. A horizontal downward-facing surface sees the entire ground plane, so View Factor to Ground = 1.0. A horizontal upward-facing surface (horizontal roof) does not see the ground at all, so View Factor to Ground = 0.0.
+
+Unused if reflections option in Solar Distribution field in Building object input unless a DaylightingDevice:Shelf or DaylightingDevice:Tubular has been specified.
+
+If you do not use the reflections option in the Solar Distribution field in your Building object input, you are responsible for entering the View Factor to Ground for each heat-transfer surface. Typical values for a surface that is not shadowed are obtained by the simple equation:
+
+View Factor to Ground = (1-cos(SurfTilt))/2
+
+For example, this gives 0.5 for a wall of tilt 90°. If the tilt of the wall changes, then the View Factor to Ground must also change.
+
+If you enter \textbf{autocalculate} in this field, EnergyPlus will automatically calculate the view factor to ground based on the tilt of the surface.
+
+If \textbf{you do use the reflections option in the Solar Distribution field} in your Building object input, you do \textbf{not} have to enter View Factor to Ground values. In this case the program will automatically calculate the value to use for each exterior surface taking into account solar shadowing (including shadowing of the ground by the building) and reflections from obstructions (ref: Building, Field: Solar Distribution).
+
+However, if you do use the reflections option AND you are modeling a DaylightingDevice:Shelf or DaylightingDevice:Tubular, then you still need to enter some values of View Factor to Ground. For DaylightingDevice:Shelf you need to enter View Factor to Ground for the window associated with the shelf. And for DaylightingDevice:Tubular you need to enter the View Factor to Ground for the FenestrationSurface:Detailed corresponding to the dome of the tubular device.
+
+Note 1: The corresponding view factor to the sky for diffuse solar radiation is not a user input; it is calculated within EnergyPlus based on surface orientation, sky solar radiance distribution, and shadowing surfaces.
+
+Note 2: The view factors to the sky and ground for thermal infrared (long-wave) radiation are not user inputs; they are calculated within EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground IR view factor.
+
+\paragraph{Field: Number of Vertices}\label{field-number-of-vertices}
+
+This field specifies the number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on ``Surface Vertices'' above.
+
+\subsection{RoofCeiling:Detailed}\label{roofceilingdetailed}
+
+The RoofCeiling:Detailed object is used to describe walls.
+
+\subsubsection{Inputs}\label{inputs-21-007}
+
+\paragraph{Field: Name}\label{field-name-17-008}
+
+This is a unique name associated with each building surface. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-17}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-11-000}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Outside Boundary Condition}\label{field-outside-boundary-condition-1}
+
+This value can be one of several things depending on the actual kind of surface.
+
+\begin{enumerate}
+  \item
+    \textbf{Surface} -- if this surface is an internal surface, then this is the choice. The value will either be a surface in the base zone or a surface in another zone. The heat balance between two zones can be accurately simulated by specifying a surface in an adjacent zone. EnergyPlus will simulate a group of zones simultaneously and will include the heat transfer between zones. However, as this increases the complexity of the calculations, it is not necessary to specify the other zone unless the two zones will have a significant temperature difference. If the two zones will not be very different (temperature wise), then the surface should use itself as the outside environment or specify this field as \textbf{Adiabatic}. The surface name on the ``outside'' of this surface (adjacent to) is placed in the next field.
+  \item
+    \textbf{Adiabatic} -- an internal surface in the same Zone. This surface will not transfer heat out of the zone, but will still store heat in thermal mass. Only the inside face of the surface will exchange heat with the zone (i.e.~two adiabatic surfaces are required to model internal partitions where both sides of the surface are exchanging heat with the zone). The Outside Boundary Condition Object can be left blank.
+  \item
+    \textbf{Zone} -- this is similar to Surface but EnergyPlus will automatically create the required surface in the adjacent zone when this is entered for the surface. If there are windows or doors on the surface, EnergyPlus automatically creates appropriate sub-surfaces as well.
+  \item
+    \textbf{Outdoors} -- if this surface is exposed to outside temperature conditions, then this is the choice. See Sun Exposure and Wind Exposure below for further specifications on this kind of surface.
+  \item
+    \textbf{Ground} -- if this surface is exposed to the ground, then this is the choice. The temperature on the outside of this surface will be the Ground Temperature.
+  \item
+    \textbf{OtherSideCoefficients} -- if this surface has a custom, user specified temperature or other parameters (See SurfaceProperty:OtherSideCoefficients specification), then this is the choice. The outside boundary condition will be the name of the SurfaceProperty:OtherSideCoefficients specification.
+  \item
+    \textbf{OtherSideConditionsModel} -- if this surface has a specially-modeled multi-skin component, such as a transpired collector or vented photovoltaic panel, attached to the outside (See SurfaceProperty:OtherSideConditionsModel specification), then this the choice. The outside face environment will be the name of the SurfaceProperty:OtherSideConditionsModelspecification.
+  \item
+    \textbf{GroundSlabPreprocessorAverage} -- uses the average results from the Slab preprocessor calculations.
+  \item
+    \textbf{GroundSlabPreprocessorCore} -- uses the core results from the Slab preprocessor calculations.
+  \item
+    \textbf{GroundSlabPreprocessorPerimeter} -- uses the perimeter results from the Slab preprocessor calculations.
+  \item
+    \textbf{GroundBasementPreprocessorAverageWall} -- uses the average wall results from the Basement preprocessor calculations.
+  \item
+    \textbf{GroundBasementPreprocessorAverageFloor} -- uses the average floor results from the Basement preprocessor calculations.
+  \item
+    \textbf{GroundBasementPreprocessorUpperWall} -- uses the upper wall results from the Basement preprocessor calculations.
+  \item
+    \textbf{GroundBasementPreprocessorLowerWall} -- uses the lower wall results from the Basement preprocessor calculations.
+\end{enumerate}
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object-7}
+
+If neither Surface, OtherSideCoefficients, or OtherSideConditionsModel are specified for the Outside Boundary Condition (previous field), then this field should be left blank.
+
+As stated above, if the Outside Boundary Condition is ``Surface'', then this field's value must be the surface name whose inside face temperature will be forced on the outside face of the base surface. This permits heat exchange between adjacent zones (interzone heat transfer) when multiple zones are simulated, but can also be used to simulate middle zone behavior without modeling the adjacent zones. This is done by specifying a surface within the zone. For example, a middle floor zone can be modeled by making the floor the Outside Boundary Condition Object for the ceiling, and the ceiling the Outside Boundary Condition Object for the floor.
+
+If the Outside Boundary Condition is Zone, then this field should contain the zone name of the adjacent zone for the surface.
+
+\begin{callout}
+Note: Zones with interzone heat transfer are not adiabatic and the internal surfaces contribute to gains or losses. Adiabatic surfaces are modeled by specifying the base surface itself in this field. Also, for interzone heat transfer, both surfaces must be represented -- for example, if you want interzone heat transfer to an attic space, the ceiling in the lower zone must have a surface object with the outside face environment as the floor in the attic and, likewise, there must be a floor surface object in the attic that references the ceiling surface name in the lower zone.
+\end{callout}
+
+Equally, if the Outside Boundary Condition is ``OtherSideCoefficients'', then this field's value must be the SurfaceProperty:OtherSideCoefficients name. Or if the Outside Boundary Condition is ``OtherSideConditionsModel'' then this field's value must be the SurfaceProperty:OtherSideConditionsModel name.
+
+\paragraph{Field: Sun Exposure}\label{field-sun-exposure-1}
+
+If the surface is exposed to the sun, then ``SunExposed'' should be entered in this field. Otherwise, ``NoSun'' should be entered.
+
+Note, a cantilevered floor could have ``Outdoors'' but ``NoSun'' exposure.
+
+\paragraph{Field: Wind Exposure}\label{field-wind-exposure-1}
+
+If the surface is exposed to the Wind, then ``WindExposed'' should be entered in this field. Otherwise, ``NoWind'' should be entered.
+
+\begin{callout}
+Note: When a surface is specified with ``NoWind'', this has several implications. Within the heat balance code, this surface will default to using the simple ASHRAE exterior convection coefficient correlation with a zero wind speed. In addition, since the ASHRAE simple method does not have a separate value for equivalent long wavelength radiation to the sky and ground, using ``NoWind'' also eliminates long wavelength radiant exchange from the exterior of the surface to both the sky and the ground. Thus, only simple convection takes place at the exterior face of a surface specified with ``NoWind''.
+\end{callout}
+
+\paragraph{Field: View Factor to Ground}\label{field-view-factor-to-ground-1}
+
+The fraction of the ground plane (assumed horizontal) that is visible from a heat-transfer surface. It is used to calculate the diffuse solar radiation from the ground that is incident on the surface.
+
+For example, if there are no obstructions, a vertical surface sees half of the ground plane and so View Factor to Ground = 0.5. A horizontal downward-facing surface sees the entire ground plane, so View Factor to Ground = 1.0. A horizontal upward-facing surface (horizontal roof) does not see the ground at all, so View Factor to Ground = 0.0.
+
+Unused if reflections option in Solar Distribution field in Building object input unless a DaylightingDevice:Shelf or DaylightingDevice:Tubular has been specified.
+
+If you do not use the reflections option in the Solar Distribution field in your Building object input, you are responsible for entering the View Factor to Ground for each heat-transfer surface. Typical values for a surface that is not shadowed are obtained by the simple equation:
+
+View Factor to Ground = (1-cos(SurfTilt))/2
+
+For example, this gives 0.5 for a wall of tilt 90°. If the tilt of the wall changes, then the View Factor to Ground must also change.
+
+If you enter \textbf{autocalculate} in this field, EnergyPlus will automatically calculate the view factor to ground based on the tilt of the surface.
+
+If \textbf{you do use the reflections option in the Solar Distribution field} in your Building object input, you do \textbf{not} have to enter View Factor to Ground values. In this case the program will automatically calculate the value to use for each exterior surface taking into account solar shadowing (including shadowing of the ground by the building) and reflections from obstructions (ref: Building, Field: Solar Distribution).
+
+However, if you do use the reflections option AND you are modeling a DaylightingDevice:Shelf or DaylightingDevice:Tubular, then you still need to enter some values of View Factor to Ground. For DaylightingDevice:Shelf you need to enter View Factor to Ground for the window associated with the shelf. And for DaylightingDevice:Tubular you need to enter the View Factor to Ground for the FenestrationSurface:Detailed corresponding to the dome of the tubular device.
+
+Note 1: The corresponding view factor to the sky for diffuse solar radiation is not a user input; it is calculated within EnergyPlus based on surface orientation, sky solar radiance distribution, and shadowing surfaces.
+
+Note 2: The view factors to the sky and ground for thermal infrared (long-wave) radiation are not user inputs; they are calculated within EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground IR view factor.
+
+\paragraph{Field: Number of Vertices}\label{field-number-of-vertices-1}
+
+This field specifies the number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on ``Surface Vertices'' above.
+
+\subsection{Floor:Detailed}\label{floordetailed}
+
+The Floor:Detailed object is used to describe walls.
+
+\subsubsection{Inputs}\label{inputs-22-006}
+
+\paragraph{Field: Name}\label{field-name-18-008}
+
+This is a unique name associated with each building surface. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Construction Name}\label{field-construction-name-18}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-12-000}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Outside Boundary Condition}\label{field-outside-boundary-condition-2}
+
+This value can be one of several things depending on the actual kind of surface.
+
+1)~~~\textbf{Surface} -- if this surface is an internal surface, then this is the choice. The value will either be a surface in the base zone or a surface in another zone. The heat balance between two zones can be accurately simulated by specifying a surface in an adjacent zone. EnergyPlus will simulate a group of zones simultaneously and will include the heat transfer between zones. However, as this increases the complexity of the calculations, it is not necessary to specify the other zone unless the two zones will have a significant temperature difference. If the two zones will not be very different (temperature wise), then the surface should use itself as the outside environment or specify this field as \textbf{Adiabatic}. The surface name on the ``outside'' of this surface (adjacent to) is placed in the next field.
+
+2)~~~\textbf{Adiabatic} -- an internal surface in the same Zone. This surface will not transfer heat out of the zone, but will still store heat in thermal mass. Only the inside face of the surface will exchange heat with the zone (i.e.~two adiabatic surfaces are required to model internal partitions where both sides of the surface are exchanging heat with the zone). The Outside Boundary Condition Object can be left blank.
+
+3)~~~\textbf{Zone} -- this is similar to Surface but EnergyPlus will automatically create the required surface in the adjacent zone when this is entered for the surface. If there are windows or doors on the surface, EnergyPlus automatically creates appropriate sub-surfaces as well.
+
+4)~~~\textbf{Outdoors} -- if this surface is exposed to outside temperature conditions, then this is the choice. See Sun Exposure and Wind Exposure below for further specifications on this kind of surface.
+
+5)~~~\textbf{Ground} -- if this surface is exposed to the ground, then this is the usual choice. The temperature on the outside of this surface will be the Site:GroundTemperature:Surface value for the month. For more information on ground contact surfaces, reference the Auxiliary Programs document section on ``Ground Heat Transfer in EnergyPlus''.
+
+6)~~~\textbf{GroundFCfactorMethod} -- if this surface is exposed to the ground and using the \textbf{Construction:FfactorGroundFloor}, then this is the choice. The temperature on the outside of this surface will be the Site:GroundTemperature:FcfactorMethod value for the month.
+
+7)~~~\textbf{OtherSideCoefficients} -- if this surface has a custom, user specified temperature or other parameters (See SurfaceProperty:OtherSideCoefficients specification), then this is the choice. The outside boundary condition will be the name of the SurfaceProperty:OtherSideCoefficients specification.
+
+8)~~~\textbf{OtherSideConditionsModel} -- if this surface has a specially-modeled multi-skin component, such as a transpired collector or vented photovoltaic panel, attached to the outside (See SurfaceProperty:OtherSideConditionsModel specification), then this the choice. The outside face environment will be the name of the SurfaceProperty:OtherSideConditionsModelspecification.
+
+9)~~~\textbf{GroundSlabPreprocessorAverage} -- uses the average results from the Slab preprocessor calculations.
+
+10)\textbf{GroundSlabPreprocessorCore} -- uses the core results from the Slab preprocessor calculations.
+
+11)\textbf{GroundSlabPreprocessorPerimeter} -- uses the perimeter results from the Slab preprocessor calculations.
+
+12)\textbf{GroundBasementPreprocessorAverageWall} -- uses the average wall results from the Basement preprocessor calculations.
+
+13)\textbf{GroundBasementPreprocessorAverageFloor} -- uses the average floor results from the Basement preprocessor calculations.
+
+14)\textbf{GroundBasementPreprocessorUpperWall} -- uses the upper wall results from the Basement preprocessor calculations.
+
+15)\textbf{GroundBasementPreprocessorLowerWall} -- uses the lower wall results from the Basement preprocessor calculations.
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object-8}
+
+If neither Surface, OtherSideCoefficients, or OtherSideConditionsModel are specified for the Outside Boundary Condition (previous field), then this field should be left blank.
+
+As stated above, if the Outside Boundary Condition is ``Surface'', then this field's value must be the surface name whose inside face temperature will be forced on the outside face of the base surface. This permits heat exchange between adjacent zones (interzone heat transfer) when multiple zones are simulated, but can also be used to simulate middle zone behavior without modeling the adjacent zones. This is done by specifying a surface within the zone. For example, a middle floor zone can be modeled by making the floor the Outside Boundary Condition Object for the ceiling, and the ceiling the Outside Boundary Condition Object for the floor.
+
+If the Outside Boundary Condition is Zone, then this field should contain the zone name of the adjacent zone for the surface.
+
+\begin{callout}
+Note: Zones with interzone heat transfer are not adiabatic and the internal surfaces contribute to gains or losses. Adiabatic surfaces are modeled by specifying the base surface itself in this field. Also, for interzone heat transfer, both surfaces must be represented -- for example, if you want interzone heat transfer to an attic space, the ceiling in the lower zone must have a surface object with the outside face environment as the floor in the attic and, likewise, there must be a floor surface object in the attic that references the ceiling surface name in the lower zone.
+\end{callout}
+
+Equally, if the Outside Boundary Condition is ``OtherSideCoefficients'', then this field's value must be the SurfaceProperty:OtherSideCoefficients name. Or if the Outside Boundary Condition is ``OtherSideConditionsModel'' then this field's value must be the SurfaceProperty:OtherSideConditionsModel name.
+
+\paragraph{Field: Sun Exposure}\label{field-sun-exposure-2}
+
+If the surface is exposed to the sun, then ``SunExposed'' should be entered in this field. Otherwise, ``NoSun'' should be entered.
+
+Note, a cantilevered floor could have ``Outdoors'' but ``NoSun'' exposure.
+
+\paragraph{Field: Wind Exposure}\label{field-wind-exposure-2}
+
+If the surface is exposed to the Wind, then ``WindExposed'' should be entered in this field. Otherwise, ``NoWind'' should be entered.
+
+\begin{callout}
+Note: When a surface is specified with ``NoWind'', this has several implications. Within the heat balance code, this surface will default to using the simple ASHRAE exterior convection coefficient correlation with a zero wind speed. In addition, since the ASHRAE simple method does not have a separate value for equivalent long wavelength radiation to the sky and ground, using ``NoWind'' also eliminates long wavelength radiant exchange from the exterior of the surface to both the sky and the ground. Thus, only simple convection takes place at the exterior face of a surface specified with ``NoWind''.
+\end{callout}
+
+\paragraph{Field: View Factor to Ground}\label{field-view-factor-to-ground-2}
+
+The fraction of the ground plane (assumed horizontal) that is visible from a heat-transfer surface. It is used to calculate the diffuse solar radiation from the ground that is incident on the surface.
+
+For example, if there are no obstructions, a vertical surface sees half of the ground plane and so View Factor to Ground = 0.5. A horizontal downward-facing surface sees the entire ground plane, so View Factor to Ground = 1.0. A horizontal upward-facing surface (horizontal roof) does not see the ground at all, so View Factor to Ground = 0.0.
+
+Unused if reflections option in Solar Distribution field in Building object input unless a DaylightingDevice:Shelf or DaylightingDevice:Tubular has been specified.
+
+If you do not use the reflections option in the Solar Distribution field in your Building object input, you are responsible for entering the View Factor to Ground for each heat-transfer surface. Typical values for a surface that is not shadowed are obtained by the simple equation:
+
+View Factor to Ground = (1-cos(SurfTilt))/2
+
+For example, this gives 0.5 for a wall of tilt 90°. If the tilt of the wall changes, then the View Factor to Ground must also change.
+
+If you enter \textbf{autocalculate} in this field, EnergyPlus will automatically calculate the view factor to ground based on the tilt of the surface.
+
+If \textbf{you do use the reflections option in the Solar Distribution field} in your Building object input, you do \textbf{not} have to enter View Factor to Ground values. In this case the program will automatically calculate the value to use for each exterior surface taking into account solar shadowing (including shadowing of the ground by the building) and reflections from obstructions (ref: Building, Field: Solar Distribution).
+
+However, if you do use the reflections option AND you are modeling a DaylightingDevice:Shelf or DaylightingDevice:Tubular, then you still need to enter some values of View Factor to Ground. For DaylightingDevice:Shelf you need to enter View Factor to Ground for the window associated with the shelf. And for DaylightingDevice:Tubular you need to enter the View Factor to Ground for the FenestrationSurface:Detailed corresponding to the dome of the tubular device.
+
+Note 1: The corresponding view factor to the sky for diffuse solar radiation is not a user input; it is calculated within EnergyPlus based on surface orientation, sky solar radiance distribution, and shadowing surfaces.
+
+Note 2: The view factors to the sky and ground for thermal infrared (long-wave) radiation are not user inputs; they are calculated within EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground IR view factor.
+
+\paragraph{Field: Number of Vertices}\label{field-number-of-vertices-2}
+
+This field specifies the number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on ``Surface Vertices'' above.
+
+Some examples of using these objects:
+
+\begin{lstlisting}
+
+Floor:Detailed,
+      Floor_NorthZone_1stFloor,!- Name
+      FLOOR-SLAB-ASSEMBLY,     !- Construction Name
+      NorthZone_1stFloor,      !- Zone Name
+      Ground,                  !- Outside Boundary Condition
+      ,                        !- Outside Boundary Condition Object
+      NoSun,                   !- Sun Exposure
+      NoWind,                  !- Wind Exposure
+      0.0,                     !- View Factor to Ground
+      4,                       !- Number of Vertices
+      0, 11, 0,                           !- X,Y,Z  1 {m}
+      25, 11, 0,                          !- X,Y,Z  2 {m}
+      25, 5.5, 0,                         !- X,Y,Z  3 {m}
+     0, 5.5, 0;                          !- X,Y,Z  4 {m}
+
+  RoofCeiling:Detailed,
+      Ceiling_SouthZone_1stFloor,  !- Name
+      CEILING-FLOOR-ASSEMBLY,  !- Construction Name
+      SouthZone_1stFloor,      !- Zone Name
+      Surface,                 !- Outside Boundary Condition
+      Floor_SouthZone_2ndFloor,!- Outside Boundary Condition Object
+      NoSun,                   !- Sun Exposure
+      NoWind,                  !- Wind Exposure
+      0.0,                     !- View Factor to Ground
+      4,                       !- Number of Vertices
+      0, 0, 3.4,                          !- X,Y,Z  1 {m}
+      25, 0, 3.4,                         !- X,Y,Z  2 {m}
+      25, 5.5, 3.4,                       !- X,Y,Z  3 {m}
+     0, 5.5, 3.4;                        !- X,Y,Z  4 {m}
+
+  Wall:Detailed,
+      InteriorWall_SouthZone_1stFloor,  !- Name
+      INTERIOR-WALL-ASSEMBLY,  !- Construction Name
+      SouthZone_1stFloor,      !- Zone Name
+      Surface,                 !- Outside Boundary Condition
+      InteriorWall_NorthZone_1stFloor,  !- Outside Boundary Condition Object
+      NoSun,                   !- Sun Exposure
+      NoWind,                  !- Wind Exposure
+      0,                       !- View Factor to Ground
+      4,                       !- Number of Vertices
+      25, 5.5, 3.7,                       !- X,Y,Z  1 {m}
+      25, 5.5, 0,                         !- X,Y,Z  2 {m}
+      0, 5.5, 0,                          !- X,Y,Z  3 {m}
+     0, 5.5, 3.7;                        !- X,Y,Z  4 {m}
+\end{lstlisting}
+
+\subsection{BuildingSurface:Detailed}\label{buildingsurfacedetailed}
+
+The BuildingSurface:Detailed object can more generally describe each of the surfaces.
+
+\subsubsection{Inputs}\label{inputs-23-006}
+
+\paragraph{Field: Name}\label{field-name-19-005}
+
+This is a unique name associated with each building surface. It is used in several other places as a reference (e.g.~as the base surface name for a Window or Door).
+
+\paragraph{Field: Surface Type}\label{field-surface-type-000}
+
+Used primarily for convenience, the surface type can be one of the choices illustrated above -- Wall, Floor, Ceiling, Roof. Azimuth (facing) and Tilt are determined from the vertex coordinates. Note that ``normal'' floors will be tilted 180° whereas flat roofs/ceilings will be tilted 0°. EnergyPlus uses this field's designation, along with the calculated tilt of the surface, to issue warning messages when tilts are ``out of range''. Calculations in EnergyPlus use the actual calculated tilt values for the actual heat balance calculations. Note, however, that a floor tilted 0° is really facing ``into'' the zone and is not what you will desire for the calculations even though the coordinate may appear correct in the viewed DXF display.
+
+``Normal'' tilt for walls is 90° -- here you may use the calculated Azimuth to make sure your walls are facing away from the zone's interior.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-19}
+
+This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the ``full'' construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g.~drywall) as the material that shows in zone y and then the layers to the inside layer -- the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-13}
+
+This is the zone name to which the surface belongs.
+
+\paragraph{Field: Outside Boundary Condition}\label{field-outside-boundary-condition-3}
+
+This value can be one of several things depending on the actual kind of surface.
+
+1)~~~\textbf{Surface} -- if this surface is an internal surface, then this is the choice. The value will either be a surface in the base zone or a surface in another zone. The heat balance between two zones can be accurately simulated by specifying a surface in an adjacent zone. EnergyPlus will simulate a group of zones simultaneously and will include the heat transfer between zones. However, as this increases the complexity of the calculations, it is not necessary to specify the other zone unless the two zones will have a significant temperature difference. If the two zones will not be very different (temperature wise), then the surface should use itself as the outside environment or specify this field as \textbf{Adiabatic}. In either case, the surface name on the ``outside'' of this surface (adjacent to) is placed in the next field.
+
+2)~~~\textbf{Adiabatic} -- an internal surface in the same Zone. This surface will not transfer heat out of the zone, but will still store heat in thermal mass. Only the inside face of the surface will exchange heat with the zone (i.e.~two adiabatic surfaces are required to model internal partitions where both sides of the surface are exchanging heat with the zone). The Outside Boundary Condition Object can be left blank.
+
+3)~~~\textbf{Zone} -- this is similar to Surface but EnergyPlus will automatically create the required surface in the adjacent zone when this is entered for the surface. If there are windows or doors on the surface, EnergyPlus automatically creates appropriate sub-surfaces as well.
+
+4)~~~\textbf{Outdoors} -- if this surface is exposed to outside temperature conditions, then this is the choice. See Sun Exposure and Wind Exposure below for further specifications on this kind of surface.
+
+5)~~~\textbf{Ground} -- if this surface is exposed to the ground, then this is the usual choice. The temperature on the outside of this surface will be the Site:GroundTemperature:Surface value for the month. For more information on ground contact surfaces, reference the Auxiliary Programs document section on ``Ground Heat Transfer in EnergyPlus''.
+
+6)~~~\textbf{GroundFCfactorMethod} -- if this surface is exposed to the ground and using the \textbf{Construction:CfactorUndergroundWall} or \textbf{Construction:FfactorGroundFloor} (depending on surface type), then this is the choice. The temperature on the outside of this surface will be the Site:GroundTemperature:FcfactorMethod value for the month.
+
+7)~~~\textbf{OtherSideCoefficients} -- if this surface has a custom, user specified temperature or other parameters (See SurfaceProperty:OtherSideCoefficients specification), then this is the choice. The outside boundary condition will be the name of the SurfaceProperty:OtherSideCoefficients specification.
+
+8)~~~\textbf{OtherSideConditionsModel} -- if this surface has a specially-modeled multi-skin component, such as a transpired collector or vented photovoltaic panel, attached to the outside (See SurfaceProperty:OtherSideConditionsModel specification), then this the choice. The outside face environment will be the name of the SurfaceProperty:OtherSideConditionsModelspecification.
+
+9)~~~\textbf{GroundSlabPreprocessorAverage} -- uses the average results from the Slab preprocessor calculations.
+
+10)\textbf{GroundSlabPreprocessorCore} -- uses the core results from the Slab preprocessor calculations.
+
+11)\textbf{GroundSlabPreprocessorPerimeter} -- uses the perimeter results from the Slab preprocessor calculations.
+
+12)\textbf{GroundBasementPreprocessorAverageWall} -- uses the average wall results from the Basement preprocessor calculations.
+
+13)\textbf{GroundBasementPreprocessorAverageFloor} -- uses the average floor results from the Basement preprocessor calculations.
+
+14)\textbf{GroundBasementPreprocessorUpperWall} -- uses the upper wall results from the Basement preprocessor calculations.
+
+15)\textbf{GroundBasementPreprocessorLowerWall} -- uses the lower wall results from the Basement preprocessor calculations.
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object-9}
+
+If neither Surface, OtherSideCoefficients, or OtherSideConditionsModel are specified for the Outside Boundary Condition (previous field), then this field should be left blank.
+
+As stated above, if the Outside Boundary Condition is ``Surface'', then this field's value must be the surface name whose inside face temperature will be forced on the outside face of the base surface. This permits heat exchange between adjacent zones (interzone heat transfer) when multiple zones are simulated, but can also be used to simulate middle zone behavior without modeling the adjacent zones. This is done by specifying a surface within the zone. For example, a middle floor zone can be modeled by making the floor the Outside Boundary Condition Object for the ceiling, and the ceiling the Outside Boundary Condition Object for the floor.
+
+If the Outside Boundary Condition is Zone, then this field should contain the zone name of the adjacent zone for the surface.
+
+\begin{callout}
+Note: Zones with interzone heat transfer are not adiabatic and the internal surfaces contribute to gains or losses. Adiabatic surfaces are modeled by specifying the base surface itself in this field. Also, for interzone heat transfer, both surfaces must be represented -- for example, if you want interzone heat transfer to an attic space, the ceiling in the lower zone must have a surface object with the outside face environment as the floor in the attic and, likewise, there must be a floor surface object in the attic that references the ceiling surface name in the lower zone.
+\end{callout}
+
+Equally, if the Outside Boundary Condition is ``OtherSideCoefficients'', then this field's value must be the SurfaceProperty:OtherSideCoefficients name. Or if the Outside Boundary Condition is ``OtherSideConditionsModel'' then this field's value must be the SurfaceProperty:OtherSideConditionsModel name.
+
+\paragraph{Field: Sun Exposure}\label{field-sun-exposure-3}
+
+If the surface is exposed to the sun, then ``SunExposed'' should be entered in this field. Otherwise, ``NoSun'' should be entered.
+
+Note, a cantilevered floor could have ``Outdoors'' but ``NoSun'' exposure.
+
+\paragraph{Field: Wind Exposure}\label{field-wind-exposure-3}
+
+If the surface is exposed to the Wind, then ``WindExposed'' should be entered in this field. Otherwise, ``NoWind'' should be entered.
+
+\begin{callout}
+Note: When a surface is specified with ``NoWind'', this has several implications. Within the heat balance code, this surface will default to using the simple ASHRAE exterior convection coefficient correlation with a zero wind speed. In addition, since the ASHRAE simple method does not have a separate value for equivalent long wavelength radiation to the sky and ground, using ``NoWind'' also eliminates long wavelength radiant exchange from the exterior of the surface to both the sky and the ground. Thus, only simple convection takes place at the exterior face of a surface specified with ``NoWind''.
+\end{callout}
+
+\paragraph{Field: View Factor to Ground}\label{field-view-factor-to-ground-3}
+
+The fraction of the ground plane (assumed horizontal) that is visible from a heat-transfer surface. It is used to calculate the diffuse solar radiation from the ground that is incident on the surface.
+
+For example, if there are no obstructions, a vertical surface sees half of the ground plane and so View Factor to Ground = 0.5. A horizontal downward-facing surface sees the entire ground plane, so View Factor to Ground = 1.0. A horizontal upward-facing surface (horizontal roof) does not see the ground at all, so View Factor to Ground = 0.0.
+
+Unused if reflections option in Solar Distribution field in Building object input unless a DaylightingDevice:Shelf or DaylightingDevice:Tubular has been specified.
+
+If you do not use the reflections option in the Solar Distribution field in your Building object input, you are responsible for entering the View Factor to Ground for each heat-transfer surface. Typical values for a surface that is not shadowed are obtained by the simple equation:
+
+View Factor to Ground = (1-cos(SurfTilt))/2
+
+For example, this gives 0.5 for a wall of tilt 90°. If the tilt of the wall changes, then the View Factor to Ground must also change.
+
+If you enter \textbf{autocalculate} in this field, EnergyPlus will automatically calculate the view factor to ground based on the tilt of the surface.
+
+If \textbf{you do use the reflections option in the Solar Distribution field} in your Building object input, you do \textbf{not} have to enter View Factor to Ground values. In this case the program will automatically calculate the value to use for each exterior surface taking into account solar shadowing (including shadowing of the ground by the building) and reflections from obstructions (ref: Building, Field: Solar Distribution).
+
+However, if you do use the reflections option AND you are modeling a DaylightingDevice:Shelf or DaylightingDevice:Tubular, then you still need to enter some values of View Factor to Ground. For DaylightingDevice:Shelf you need to enter View Factor to Ground for the window associated with the shelf. And for DaylightingDevice:Tubular you need to enter the View Factor to Ground for the FenestrationSurface:Detailed corresponding to the dome of the tubular device.
+
+Note 1: The corresponding view factor to the sky for diffuse solar radiation is not a user input; it is calculated within EnergyPlus based on surface orientation, sky solar radiance distribution, and shadowing surfaces.
+
+Note 2: The view factors to the sky and ground for thermal infrared (long-wave) radiation are not user inputs; they are calculated within EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground IR view factor.
+
+\paragraph{Field: Number of Vertices}\label{field-number-of-vertices-3}
+
+This field specifies the number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on ``Surface Vertices'' above.
+
+IDF example of three walls (first is an exterior wall, second and third are interzone partitions):
+
+\begin{lstlisting}
+
+BuildingSurface:Detailed,Zn001:Wall001,  !- Base Surface Name
+    Wall,EXTERIOR,  !- Class and Construction Name
+    ZONE 1 @ 200 601 0 T,  !- Zone
+    Outdoors,,  !- Outside Boundary Condition  and Target (if applicable)
+     SunExposed,  !- Solar Exposure
+     WindExposed,  !- Wind Exposure
+    0.5000000    ,  !- VF to Ground
+             4, !-Rectangle
+    0.0000000E+00,  0.0000000E+00,   3.048000    ,
+    0.0000000E+00,  0.0000000E+00,  0.0000000E+00,
+     6.096000    ,  0.0000000E+00,  0.0000000E+00,
+     6.096000    ,  0.0000000E+00,   3.048000    ;
+
+  BuildingSurface:Detailed,Zn001:Wall006,  !-Base Surface Name
+    Wall,INTERIOR,  !- Class and Construction Name
+    HEARTLAND AREA,  !- Zone
+    Surface,Zn004:Wall005,  !- Outside Boundary Conditions and Target (if applicable)
+     NoSun,  !- Solar Exposure
+     NoWind,  !- Wind Exposure
+    0.5000000    ,  !- VF to Ground
+             4, !-Rectangle
+     38.01000    ,   28.25000    ,   10.00000    ,
+     38.01000    ,   28.25000    ,  0.0000000E+00,
+     38.01000    ,   18.25000    ,  0.0000000E+00,
+     38.01000    ,   18.25000    ,   10.00000    ;
+
+  BuildingSurface:Detailed,Zn001:Wall007,  !- Base Surface Name
+    Wall,INTERIOR,  !- Class and Construction Name
+    HEARTLAND AREA,  !- Zone
+    Surface,Zn003:Wall006,  !- Outside Boundary Conditions and Target (if applicable)
+     NoSun,  !- Solar Exposure
+     NoWind,  !- Wind Exposure
+    0.5000000    ,  !- VF to Ground
+             4, !-Rectangle
+     58.01000    ,   18.25000    ,   10.00000    ,
+     58.01000    ,   18.25000    ,  0.0000000E+00,
+     58.01000    ,   28.25000    ,  0.0000000E+00,
+     58.01000    ,   28.25000    ,   10.00000    ;
+\end{lstlisting}
+
+\subsection{FenestrationSurface:Detailed}\label{fenestrationsurfacedetailed}
+
+This surface class is used for subsurfaces, which can be of five different types: Windows, Doors, GlassDoors, TubularDaylightDomes, and TubularDaylightDiffusers. A subsurface (such as a window) of a base surface (such as a wall) inherits several of the properties (such as Outside Boundary Condition, Sun Exposure, etc.) of the base surface. Windows, GlassDoors, TubularDaylightDomes, and TubularDaylightDiffusers are considered to have one or more glass layers and so transmit solar radiation. Doors are considered to be opaque.
+
+\subsubsection{Inputs}\label{inputs-24-004}
+
+\paragraph{Field: Name}\label{field-name-20-004}
+
+This is a unique name associated with the heat transfer subsurface. It may be used in other places as a reference (e.g.~as the opposing subsurface of an interzone window or door).
+
+\paragraph{Field: Surface Type}\label{field-surface-type-1}
+
+The choices for Surface Type are Window, Door, GlassDoor, TubularDaylightDome, and TubularDaylightDiffuser. Doors are assumed to be opaque (do not transmit solar radiation) whereas the other surface types do transmit solar radiation. Windows and Glass Doors are treated identically in the calculation of conduction heat transfer, solar gain, daylighting, etc. A Window or GlassDoor, but not a Door, can have a movable interior, exterior or between-glass shading device, such as blinds (ref: WindowMaterial:Blind object), and can have a frame and/or a divider (ref: WindowProperty:FrameAndDivider object). TubularDaylightDomes and TubularDaylightDomes are specialized subsurfaces for use with the DaylightingDevice:Tubular object to simulate Tubular Daylighting Devices (TDDs). TubularDaylightDomes and TubularDaylightDomes cannot have shades, screens or blinds. In the following, the term ``window'' applies to Window, GlassDoor, TubularDaylightDome, and TubularDaylightDome, if not otherwise explicitly mentioned.
+
+As noted in the description of the BuildingSurface:Detailed, Azimuth (facing angle) and Tilt are calculated from the entered vertices. Tilts of subsurfaces will normally be the same as their base surface. If these are significantly beyond the ``normals'' for the base surface, warning messages may be issued. If the facing angles are not correct, you may have a window pointing ``into'' the zone rather than out of it -- this would cause problems in the calculations. Note, too, that a ``reveal'' (inset or outset) may occur if the plane of the subsurface is not coincident with the base surface; the reveal has an effect on shading of the subsurface.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-20}
+
+This is the name of the subsurface's construction (ref: Construction object {[}for Door{]} and Construction, Construction:ComplexFenestrationState, Construction:WindowDataFile objects {[}for Window and GlassDoor{]}).
+
+For windows, if Construction Name is not found among the constructions on the input (.idf) file, the Window Data File (ref. Construction:WindowDataFile object) will be searched for that Construction Name (see ``Importing Windows from WINDOW''). If that file is not present or if the Construction Name does not match the name of an entry on the file, an error will result. If there is a match, a window construction and its corresponding glass and gas materials will be created from the information read from the file.
+
+\paragraph{Field: Building Surface Name}\label{field-building-surface-name-6}
+
+This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. For example, a surface in contact with the ground (Outside Boundary Condition = Ground) cannot contain a window.
+
+\paragraph{Field: Outside Boundary Condition Object}\label{field-outside-boundary-condition-object-10}
+
+If the base surface has Outside Boundary Condition = Surface or OtherSideCoefficients, then this field must also be specified for the subsurface. Otherwise, it can be left blank.
+
+If the base surface has Outside Boundary Condition = Zone, then this surface retains that characteristic and uses the same zone of the base surface. It can be entered here for clarity or it can be left blank.
+
+If Outside Boundary Condition for the base surface is Surface, this field should specify the subsurface in the opposing zone that is the counterpart to this subsurface. The constructions of the subsurface and opposing subsurface must match, except that, for multi-layer constructions, the layer order of the opposing subsurface's construction must be the reverse of that of the subsurface.
+
+If Outside Boundary Condition for the base surface is OtherSideCoefficients, this field could specify the set of SurfaceProperty:OtherSideCoefficients for this subsurface. If this is left blank, then the Other Side Coefficients of the base surface will be used for this subsurface. \emph{Windows and GlassDoors are not allowed to have Other Side Coefficients.}
+
+\paragraph{Field: View Factor to Ground}\label{field-view-factor-to-ground-4}
+
+The fraction of the ground plane (assumed horizontal) that is visible from a heat-transfer surface. It is used to calculate the diffuse solar radiation from the ground that is incident on the surface.
+
+For example, if there are no obstructions, a vertical surface sees half of the ground plane and so View Factor to Ground = 0.5. A horizontal downward-facing surface sees the entire ground plane, so View Factor to Ground = 1.0. A horizontal upward-facing surface (horizontal roof) does not see the ground at all, so View Factor to Ground = 0.0.
+
+Unused if reflections option in Solar Distribution field in Building object input unless a Daylighting Device:Shelf or Daylighting Device:Tubular has been specified.
+
+If you do not use the reflections option in the Solar Distribution field in your Building object input, you are responsible for entering the View Factor to Ground for each heat-transfer surface. Typical values for a surface that is not shadowed are obtained by the simple equation:
+
+View Factor to Ground = (1-cos(SurfTilt))/2
+
+For example, this gives 0.5 for a wall of tilt 90°. If the tilt of the wall changes, then the View Factor to Ground must also change.
+
+If you enter \textbf{autocalculate} in this field, EnergyPlus will automatically calculate the view factor to ground based on the tilt of the surface.
+
+If \textbf{you do use the reflections option in the Solar Distribution field} in your BUILDING object input, you do \textbf{not} have to enter View Factor to Ground values. In this case the program will automatically calculate the value to use for each exterior surface taking into account solar shadowing (including shadowing of the ground by the building) and reflections from obstructions (ref: Building, Field: Solar Distribution).
+
+However, if you do use the reflections option AND you are modeling a DaylightingDevice:Shelf or DaylightingDevice:Tubular, then you still need to enter some values of View Factor to Ground. For DaylightingDevice:Shelf you need to enter View Factor to Ground for the window associated with the shelf. And for DaylightingDevice:Tubular you need to enter the View Factor to Ground for the FenestrationSurface:Detailed corresponding to the dome of the tubular device (ref: DaylightingDevice:Tubular).
+
+Note 1: The corresponding view factor to the sky for diffuse solar radiation is not a user input; it is calculated within EnergyPlus based on surface orientation, sky solar radiance distribution, and shadowing surfaces.
+
+Note 2: The view factors to the sky and ground for thermal infrared (long-wave) radiation are not user inputs; they are calculated within EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground infrared view factor.
+
+\paragraph{Field: Shading Control Name}\label{field-shading-control-name-2}
+
+This field, if not blank, is the name of the window shading control (ref: WindowProperty:ShadingControl object) for this subsurface. It is used for Surface Type = Window and GlassDoor. To assign a shade to a window or glass door, see WindowMaterial: Shade. To assign a screen, see WindowMaterial:Screen. To assign a blind, see WindowMaterial:Blind. To assign switchable glazing, such as electrochromic glazing, see WindowProperty:ShadingControl.
+
+\paragraph{Field: Frame and Divider Name}\label{field-frame-and-divider-name-2}
+
+This field, if not blank, can be used to specify window frame, divider and reveal-surface data (ref: WindowProperty:FrameAndDivider object). It is used only for exterior GlassDoors and rectangular exterior Windows, i.e., those with OutsideFaceEnvironment = Outdoors.
+
+This field should be blank for triangular windows.
+
+\paragraph{Field: Multiplier}\label{field-multiplier-7}
+
+Used only for Surface Type = Window, Door or Glass Door. It is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
+
+Multiplier should be used with caution. Multiplier \textgreater{} 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
+
+If Multiplier \textgreater{} 1, you will get
+
+--a \emph{warning} if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
+
+--an \emph{error} if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
+
+\paragraph{Field: Number of Vertices}\label{field-number-of-vertices-4}
+
+The number of sides the surface has (number of X,Y,Z vertex groups). For further information, see the discussion on ``Surface Vertices'' above. Door and GlassDoor subsurfaces are rectangular and therefore have four vertices. Window subsurfaces can be rectangular or triangular and therefore have four or three vertices, respectively.
+
+\paragraph{Fields: Vertex Coordinates}\label{fields-vertex-coordinates}
+
+This is a total of twelve fields giving the x,y,z coordinate values of the four vertices of rectangular subsurfaces {[}m{]}, or a total of nine fields giving the x,y,z coordinate values of the three vertices of triangular windows.
+
+For triangular windows the first vertex listed can be any of the three vertices, but the order of the vertices should be counter-clockwise if VertexEntry is CounterClockWise and clockwise if VertexEntry is ClockWise (ref: GlobalGeometryRules).
+
+An IDF example of a rectangular subsurface (Window):
+
+\begin{lstlisting}
+
+FenestrationSurface:Detailed,
+   Zn001:Wall001:Win001,  !- SubSurface Name
+    Window,SINGLE PANE HW WINDOW,  !- Class and Construction Name
+    Zn001:Wall001,,         !- Base Surface Name and Target (if applicable)
+    0.5000000    ,          !- VF to Ground
+    WINDOW-CONTROL-DRAPES,  !- Window Shading Control
+    TestFrameAndDivider,    !- Frame/Divider name
+    5,                      !- Multiplier
+    4,                      !- Rectangle (number of sides)
+     1.524000    ,  0.1520000    ,   2.743000    ,
+     1.524000    ,  0.1520000    ,  0.3050000    ,
+     4.572000    ,  0.1520000    ,  0.3050000    ,
+     4.572000    ,  0.1520000    ,   2.743000    ;
+\end{lstlisting}
+
+\subsection{Window Modeling Options}\label{window-modeling-options}
+
+The following table shows what input objects/fields to use to model different window options. It also gives the name of an example input, if available, that demonstrates the option.
+
+% table 8
+\begin{longtable}[c]{p{2.0in}p{2.0in}p{2.0in}}
+\caption{Window Modeling Options \label{table:window-modeling-options}} \tabularnewline
+\toprule 
+Option & Object/Field or Output Variable & Input File (distributed with install) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Window Modeling Options} \tabularnewline
+\toprule 
+Option & Object/Field or Output Variable & Input File (distributed with install) \tabularnewline
+\midrule
+\endhead
+
+Build up a window from \textbf{layers} & Window\-Material:\-Glazing, Window\-Material:-Gas, Window\-Material:\-Shade, Window\-Material:\-Screen, Window\-Material:\-Blind, Construction & Window\-Tests.idf \tabularnewline
+Add an \textbf{overhang} & Shading:\-Zone:\-Detailed & 5Zone\-Air\-Cooled.idf \tabularnewline
+Add a \textbf{shading device} & Window\-Material:\-Shade, Window\-Material:\-Screen or Window\-Material:\-Blind; Window\-Property:\-Shading\-Control & Window\-Tests.idf, Purch\-Air\-Window\-Blind.idf \tabularnewline
+\textbf{Control} a shading device & Window\-Property:\-Shading\-Control & Purch\-Air\-WindowBlind.idf \tabularnewline
+Determine when a shading device is on in a particular timestep & Print the variable ``Surface Shading Device Is On Time Fraction'' & Purch\-Air\-Window\-Blind.idf \tabularnewline
+Control the \textbf{slat angle} of a blind & Window\-Property:\-Shading\-Control & Purch\-Air\-Window\-Blind.idf \tabularnewline
+Add a \textbf{frame} & Window\-Property:\-FrameAndDivider & Purch\-Air\-With\-Day\-lighting.idf \tabularnewline
+Add a \textbf{divider} & Window\-Property:\-Frame\-And\-Divider & Purch\-Air\-With\-Day\-lighting.idf \tabularnewline
+Allow window to \textbf{daylight} a zone & Day\-lighting:Controls, Day\-lighting:\-DELight:\-Controls & Purch\-Air\-With\-Day\-lighting.idf, DElight-\-Detailed-\-Comparison.idf \tabularnewline
+Find \textbf{solar reflected} onto window from neighboring buildings & Building/\-Solar\-Distribution field – uses ``WithReflections'' & Reflective\-Adjacent\-Building.idf \tabularnewline
+Model \textbf{switchable glazing} (e.g., electrochromic glass) & Window\-Property:\-Shading\-Control & Purch\-Air\-With\-Day\-lighting.idf \tabularnewline
+Add an \textbf{interior window} & Define two Fenestration\-Surface:\-Detailed's, one for each associated interior wall & Purch\-Air\-With\-Double\-Facade\-Day\-lighting.idf \tabularnewline
+\textbf{Track} how beam solar falls on interior surfaces & Building/\-Solar Distribution = Full\-Interior\-And\-Exterior & Purch\-Air\-With\-Double\-Facade\-Day\-lighting.idf \tabularnewline
+\textbf{Track} beam solar transmitted through interior windows & Building/Solar Distribution = Full\-Interior\-And\-Exterior & Purch\-Air\-With\-Double\-Facade\-Day\-lighting.idf \tabularnewline
+Add a \textbf{shading device on an interior window} & Not allowed & \tabularnewline
+Model an \textbf{airflow window} (aka, heat extract window) & Window\-Property:\-Air\-flow\-Control & Air\-flow\-Windows\-And\-Between\-Glass\-Blinds.idf \tabularnewline
+Add a \textbf{storm window} glass layer & Window\-Property:\-Storm\-Window & Storm\-Window.idf \tabularnewline
+Add \textbf{natural ventilation} through an open window & Ventilation or Airflow\-Network objects (Airflow\-Network:\-Multizone:\-Surface, Airflow\-Network:\-Multi\-Zone:\-Component:\-Detailed\-Opening, etc.) & Airflow\-Network\-3zvent.idf \tabularnewline
+Add \textbf{diffusing glass} & Window\-Material:\-Glazing/\-Solar Diffusing = Yes & \tabularnewline
+Add \textbf{dirt on window} & Window\-Material:\-Glazing/\-Dirt Correction Factor for Solar and Visible Transmittance & \tabularnewline
+Import window (and frame/divider if present) from \textbf{WINDOW} program & See ``Importing Windows from WINDOW program'' & \tabularnewline
+Find \textbf{daylighting through interior windows} & See ``Double Facades: Daylighting through Interior Windows'' & Purch\-Air\-With\-Double\-Facade\-Daylighting.idf \tabularnewline
+Determine when \textbf{condensation} occurs & Print the variables ``Surface Window Inside Face Glazing Condensation Status,'' ``Surface Window Inside Face Frame Condensation Status,'' ``Surface Window Inside Face Divider Condensation Status'' & \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{InternalMass}\label{internalmass}
+
+Any surface that would logically be described as an interior wall, floor or ceiling can just as easily be described as Internal Mass. Internal Mass surface types only exchange energy with the zone in which they are described; they do not see any other zones. There are two approaches to using internal mass. The first approach is to have several pieces of internal mass with each piece having a different construction type. The other approach is to choose an average construction type and combine all of the interior surfaces into a single internal mass. Similar to internal surfaces with an adiabatic boundary condtion, the zone will only exchange energy with the inside of the Internal Mass construction. If both sides of the surface exchange energy with the zone then the user should input twice the area when defining the Internal Mass object. Note that furniture and other large objects within a zone can be described using internal mass. However, simplifying calculations using internal mass must be used with caution when the ``FullInteriorAndExterior'' or ``FullInteriorAndExteriorWithReflections'' Solar Distribution model (see Building parameters) is chosen.
+
+\subsubsection{Inputs}\label{inputs-25-004}
+
+\textbf{Example}
+
+When zoning an office building, five west-facing offices have been combined into one zone. All of the offices have interior walls made of the same materials. As shown in the figure below, this zone may be described with 5 exterior walls and 11 internal walls or 1 exterior wall and 1 internal mass. Note that fewer surfaces will speed up the EnergyPlus calculations.
+
+\begin{figure}[hbtp] % fig 30
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image056.png}
+\caption{Representing 11 internal walls as internal mass \protect \label{fig:representing-11-internal-walls-as-internal}}
+\end{figure}
+
+\textbf{Example}
+
+A five-story building has the same ceiling/floor construction separating each of the levels. Zones that are on floors 2 through 4 may be described using a single piece of internal mass to represent both the floor and ceiling. The construction for this internal mass would be identical to the ceiling/floor construction that would be used to describe separate surfaces and the area of the internal mass surface would be the total surface area of the combined ceilings/floors (i.e.~twice the total floor area).
+
+\paragraph{Field: Name}\label{field-name-21-004}
+
+This is a unique character string associated with the internal mass surface. Though it must be unique from other surface names, it is used primarily for convenience with internal mass surfaces.
+
+\paragraph{Field: Construction Name}\label{field-construction-name-21}
+
+This is the name of the construction (ref: Construction object) used in the surface.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-14}
+
+This is the name of the zone in which the internal mass is represented.
+
+\paragraph{Field: Surface Area}\label{field-surface-area}
+
+This field is the surface area of the internal mass. The area that is specified must be the entire surface area that is exposed to the zone. If both sides of a wall are completely within the same zone, then the area of both sides must be included when describing that internal wall.
+
+IDF examples of Internal Mass surfaces:
+
+\begin{lstlisting}
+InternalMass,
+  Zn002:IntM001,                !- Surface Name
+  INTERIOR,                     !- Construction Name
+  DORM ROOMS AND COMMON AREAS,  !- Zone
+  408.7734;                     !- Total area exposed to Zone {m2}
+
+InternalMass,
+  Zn002:IntM002,                !- Surface Name
+  PARTITION02,                  !- Construction Name
+  DORM ROOMS AND COMMON AREAS,  !- Zone
+  371.6122;                     !- Total area exposed to Zone {m2}
+\end{lstlisting}
+
+\subsection{Surface Output Variables/Reports}\label{surface-output-variablesreports}
+
+Note that Surface Outputs from specialized algorithms (such as Effective Moisture Penetration Depth (EMPD), Combined Heat and Moisture Transport (HAMT) and Conduction Finite Difference (CondFD) are discussed under the objects that describe the specialized inputs for these algorithms). You can access them via these links:
+
+\begin{itemize}
+\tightlist
+\item
+  Moisture Penetration Depth (EMPD) Outputs
+\item
+  Conduction Finite Difference (CondFD) Outputs
+\item
+  Heat and Moisture (HAMT) Outputs
+\end{itemize}
+
+Additionally, the output variables applicable to all heat transfer surfaces:
+
+\begin{lstlisting}
+Zone,Sum,Surface Inside Face Heat Balance Calculation Iteration Count []
+Zone,Average,Surface Inside Face Temperature [C]
+Zone,Average,Surface Outside Face Temperature [C]
+Zone,Average,Surface Inside Face Adjacent Air Temperature [C]
+Zone,Average,Surface Inside Face Convection Heat Transfer Coefficient [W/m2-K]
+Zone,Average,Surface Inside Face Convection Heat Gain Rate [W]
+Zone,Average,Surface Inside Face Convection Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Inside Face Convection Heat Gain Energy [J]
+Zone,Average,Surface Inside Face Net Surface Thermal Radiation Heat Gain Rate [W]
+Zone,Average,Surface Inside Face Net Surface Thermal Radiation Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Inside Face Net Surface Thermal Radiation Heat Gain Energy [J]
+Zone,Average,Surface Inside Face Solar Radiation Heat Gain Rate [W]
+Zone,Average,Surface Inside Face Solar Radiation Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Inside Face Solar Radiation Heat Gain Energy [J]
+Zone,Average,Surface Inside Face Lights Radiation Heat Gain Rate [W]
+Zone,Average,Surface Inside Face Lights Radiation Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Inside Face Lights Radiation Heat Gain Energy [J]
+Zone,Average,Surface Inside Face Internal Gains Radiation Heat Gain Rate [W]
+Zone,Average,Surface Inside Face Internal Gains Radiation Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Inside Face Internal Gains Radiation Heat Gain Energy [J]
+Zone,Average,Surface Inside Face System Radiation Heat Gain Rate [W]
+Zone,Average,Surface Inside Face System Radiation Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Inside Face System Radiation Heat Gain Energy [J]
+Zone,Average,Surface Outside Face Convection Heat Transfer Coefficient [W/m2-K]
+Zone,Average,Surface Outside Face Convection Heat Gain Rate [W]
+Zone,Average,Surface Outside Face Convection Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Outside Face Convection Heat Gain Energy [J]
+Zone,Average,Surface Outside Face Net Thermal Radiation Heat Gain Rate [W]
+Zone,Average,Surface Outside Face Net Thermal Radiation Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Outside Face Net Thermal Radiation Heat Gain Energy [J]
+Zone,Average,Surface Outside Face Thermal Radiation to Air Heat Transfer Coefficient [W/m2-K]
+Zone,Average,Surface Outside Face Thermal Radiation to Sky Heat Transfer Coefficient [W/m2-K]
+Zone,Average,Surface Outside Face Thermal Radiation to Ground Heat Transfer Coefficient [W/m2-K]
+Zone,Average,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate [W]
+Zone,Sum,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Energy [J]
+Zone,Average,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate per Area[W/m2]
+Zone,Average,Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate [W]
+Zone,Average,Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate per Area[W/m2]
+Zone, Sum,Surface Inside Face Interior Windows Incident Beam Solar Radiation Energy [J]
+Zone,Average,Surface Inside Face Initial Transmitted Diffuse Absorbed Solar Radiation Rate [W]
+Zone,Average,Surface Inside Face Initial Transmitted Diffuse Transmitted Out Window Solar Radiation Rate [W]
+Zone,Average,Surface Inside Face Absorbed Shortwave Radiation Rate [W]
+\end{lstlisting}
+
+Output variables applicable to all exterior heat transfer surfaces:
+
+\begin{lstlisting}
+Zone,Average,Surface Outside Face Outdoor Air Drybulb Temperature [C]
+Zone,Average,Surface Outside Face Outdoor Air Wetbulb Temperature [C]
+Zone,Average,Surface Outside Face Outdoor Air Wind Speed [m/s]
+Zone,Average,Surface Outside Face Sunlit Area [m2]
+Zone,Average,Surface Outside Face Sunlit Fraction \protect\hyperlinksection-1
+Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area[W/m2]
+Zone,Average,Surface Outside Face Solar Radiation Heat Gain Rate [W]
+Zone,Average,Surface Outside Face Solar Radiation Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Outside Face Solar Radiation Heat Gain Energy [J]
+Zone,Average,Surface Outside Face Incident Beam Solar Radiation Rate per Area[W/m2]
+Zone,Average,Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area[W/m2]
+Zone,Average,Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area[W/m2]
+Zone,Average,Surface Ext Diff Sol From Bm-To-Diff Refl From Ground[W/m2]
+Zone,Average,Surface Outside Face Incident Sky Diffuse Ground Reflected Solar Radiation Rate per Area[W/m2]
+Zone,Average,Surface Outside Face Incident Sky Diffuse Surface Reflected Solar Radiation Rate per Area[W/m2]
+Zone,Average,Surface Outside Face Incident Beam To Beam Surface Reflected Solar Radiation Rate per Area[W/m2]
+Zone,Average,Surface Outside Face Incident Beam To Diffuse Surface Reflected Solar Radiation Rate per Area[W/m2]
+Zone,Average,Surface Outside Face Beam Solar Incident Angle Cosine Value[] 
+Zone,Average,Surface Anisotropic Sky Multiplier []
+Zone,Average,Surface Window BSDF Beam Direction Number []
+Zone,Average,Surface Window BSDF Beam Theta Angle [rad]
+Zone,Average,Surface Window BSDF Beam Phi Angle [rad]
+\end{lstlisting}
+
+Output variables applicable to opaque heat transfer surfaces (FLOOR, WALL, ROOF, DOOR). \textbf{Note -- these are advanced variables -- you must read the descriptions and understand before use -- then you must use the Diagnostics object to allow reporting.}
+
+\begin{lstlisting}
+Zone,Average,Surface Inside Face Solar Radiation Heat Gain Rate [W]
+Zone,Average,Surface Inside Face Solar Radiation Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Inside Face Solar Radiation Heat Gain Energy [J]
+Zone,Average,Surface Inside Face Lights Radiation Heat Gain Rate [W]
+Zone,Average,Surface Inside Face Lights Radiation Heat Gain Rate per Area [W/m2]
+Zone,Sum,Surface Inside Face Lights Radiation Heat Gain Energy [J]
+Zone,Average,Surface Inside Face Conduction Heat Transfer Rate [W]
+Zone,Average,Surface Inside Face Conduction Heat Gain Rate [W]
+Zone,Average,Surface Inside Face Conduction Heat Loss Rate [W]
+Zone,Average,Surface Inside Face Conduction Heat Transfer Rate per Area [W/m2]
+Zone,Sum,Surface Inside Face Conduction Heat Transfer Energy [J]
+Zone,Average,Surface Outside Face Conduction Heat Transfer Rate [W]
+Zone,Average,Surface Outside Face Conduction Heat Gain Rate [W]
+Zone,Average,Surface Outside Face Conduction Heat Loss Rate [W]
+Zone,Average,Surface Outside Face Conduction Heat Transfer Rate per Area [W/m2]
+Zone,Sum,Surface Outside Face Conduction Heat Transfer Energy [J]
+Zone,Average,Surface Average Face Conduction Heat Transfer Rate [W]
+Zone,Average,Surface Average Face Conduction Heat Gain Rate [W]
+Zone,Average,Surface Average Face Conduction Heat Loss Rate [W]
+Zone,Average,Surface Average Face Conduction Heat Transfer Rate per Area [W/m2]
+Zone,Sum,Surface Average Face Conduction Heat Transfer Energy [J]
+Zone,Average,Surface Heat Storage Rate [W]
+Zone,Average,Surface Heat Storage Gain Rate [W]
+Zone,Average,Surface Heat Storage Loss Rate [W]
+Zone,Average,Surface Heat Storage Rate per Area [W/m2]
+Zone,Sum,Surface Heat Storage Energy [J]
+Zone,Average,Surface Internal Source Location Temperature [C]
+Zone,Average,Zone Opaque Surface Inside Face Conduction [W]
+Zone,Average,Zone Opaque Surface Inside Faces Total Conduction Heat Gain Rate [W]
+Zone,Average,Zone Opaque Surface Inside Faces Total Conduction Heat Loss Rate [W]
+Zone,Sum,Zone Opaque Surface Inside Faces Total Conduction Heat Gain Energy [J]
+Zone,Sum,Zone Opaque Surface Inside Faces Total Conduction Heat Loss Energy [J]
+Zone,Average,Zone Opaque Surface Outside Face Conduction [W]
+Zone,Average,Zone Opaque Surface Outside Face Conduction Gain[W]
+Zone,Average,Zone Opaque Surface Outside Face Conduction Loss[W]
+Zone,Average, Surface Inside Face Beam Solar Radiation Heat Gain Rate [W]
+\end{lstlisting}
+
+\subsection{Window Output Variables}\label{window-output-variables}
+
+Output variables applicable only to exterior windows and glass doors:
+
+\begin{lstlisting}
+Zone,Average,Zone Windows Total Transmitted Solar Radiation Rate [W]
+Zone,Sum,Zone Transmitted Solar Energy [J]
+Zone,Average,Zone Windows Total Heat Gain Rate [W]
+Zone,Sum,Zone Windows Total Heat Gain Energy [J]
+Zone,Average,Zone Windows Total Heat Loss Rate [W]
+Zone,Sum,Zone Windows Total Heat Loss Energy [J]
+Zone,Average,Zone Exterior Windows Total Transmitted Beam Solar Radiation Rate [W]
+Zone,Sum,Zone Exterior Windows Total Transmitted Beam Solar Radiation Energy [J]
+Zone,Average,Zone Interior Windows Total Transmitted Beam Solar Radiation Rate [W]
+Zone,Sum,Zone Interior Windows Total Transmitted Beam Solar Radiation Energy [J]
+Zone,Average,Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Rate [W]
+Zone,Sum,Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Energy [J]
+Zone,Average,Zone Interior Windows Total Transmitted Diffuse Solar Radiation Rate [W]
+Zone,Average,Surface Window Total Glazing Layers Absorbed Solar Radiation Rate [W]
+Zone,Average,Surface Window Total Glazing Layers Absorbed Shortwave Radiation Rate [W]
+Zone,Sum,Surface Window Total Glazing Layers Absorbed Solar Radiation Energy [J]
+Zone,Average,Surface Window Shading Device Absorbed Solar Radiation Rate [W]
+Zone,Sum,Surface Window Shading Device Absorbed Solar Radiation Energy [J]
+Zone,Average, Surface Window Transmitted Solar Radiation Rate [W]
+Zone,Sum,Surface Window Transmitted Solar Radiation Energy [J]
+Zone,Average,Surface Window Transmitted Beam Solar Radiation Rate [W]
+Zone,Average,Surface Window Transmitted Beam To Beam Solar Radiation Rate [W]
+Zone,Average,Surface Window Transmitted Beam To Diffuse Solar Radiation Rate [W]
+Zone,Sum,Surface Window Transmitted Beam Solar Radiation Energy [J]
+Zone,Sum,Surface Window Transmitted Beam To Beam Solar Radiation Energy [J]
+Zone,Sum,Surface Window Transmitted Beam To Diffuse Solar Radiation Energy [J]
+Zone,Average,Surface Window Transmitted Diffuse Solar Radiation Rate [W]
+Zone,Sum,Surface Window Transmitted Diffuse Solar Radiation Energy [J]
+Zone,Average,Surface Window System Solar Transmittance []
+Zone,Average,Surface Window System Solar Absorptance []
+Zone,Average,Surface Window System Solar Reflectance []
+Zone,Average,Surface Window Gap Convective Heat Transfer Rate [W]
+Zone,Sum,Surface Window Gap Convective Heat Transfer Energy [J]
+Zone,Average,Surface Window Heat Gain Rate [W]
+Zone,Sum,Surface Window Heat Gain Energy [J]
+Zone,Average,Surface Window Heat Loss Rate [W]
+Zone,Sum,Surface Window Heat Loss Energy [J]
+Zone,Average,Surface Window Glazing Beam to Beam Solar Transmittance[]
+Zone,Average,Surface Window Glazing Beam to Diffuse Solar Transmittance []
+Zone,Average,Surface Window Glazing Diffuse to Diffuse Solar Transmittance[]
+Zone,Average,Surface Window Model Solver Iteration Count []
+Zone,Average,Surface Window Solar Horizontal Profile Angle[deg]
+Zone,Average,Surface Window Solar Vertical Profile Angle[deg]
+Zone,Average,Surface Window Outside Reveal Reflected Beam Solar Radiation Rate [W]
+Zone,Sum,Surface Window Outside Reveal Reflected Beam Solar Radiation Energy
+Zone,Average,Surface Window Inside Reveal Reflected Beam Solar Radiation Rate [W]
+Zone,Sum,Surface Window Inside Reveal Reflected Beam Solar Radiation Energy [J]
+Zone,Average,Surface Window Inside Reveal Absorbed Beam Solar Radiation Rate [W]
+Zone,Average,Surface Window Inside Face Glazing Condensation Status []
+Zone,Average,Surface Window Inside Face Frame Condensation Status []
+Zone,Average,Surface Window Inside Face Divider Condensation Status []
+Zone,Average,Surface Shading Device Is On Time Fraction[]
+Zone,Average,Surface Window Blind Slat Angle [deg]
+Zone,Average,Surface Window Blind Beam to Beam Solar Transmittance[]
+Zone,Average,Surface Window Blind Beam to Diffuse Solar Transmittance[]
+Zone,Average,Surface Window Blind Diffuse to Diffuse Solar Transmittance[]
+Zone,Average,Surface Window Blind and Glazing System Beam Solar Transmittance[]
+Zone,Average,Surface Window Blind and Glazing System Diffuse Solar Transmittance[]
+Zone,Average,Surface Window Screen Beam to Beam Solar Transmittance []
+Zone,Average,Surface Window Screen Beam to Diffuse Solar Transmittance []
+Zone,Average,Surface Window Screen Diffuse to Diffuse Solar Transmittance []
+Zone,Average,Surface Window Screen and Glazing System Beam Solar Transmittance []
+Zone,Average,Surface Window Screen and Glazing System Diffuse Solar Transmittance []
+Zone,State,Surface Storm Window On Off Status []
+Zone,Average,Surface Window Inside Face Frame and Divider Zone Heat Gain Rate [W]
+Zone,Average,Surface Window Frame Heat Gain Rate [W]
+Zone,Average,Surface Window Frame Heat Loss Rate [W]
+Zone,Average,Surface Window Divider Heat Gain Rate [W]
+Zone,Average,Surface Window Divider Heat Loss Rate [W]
+Zone,Average,Surface Window Frame Inside Temperature [C]
+Zone,Average,Surface Window Frame Outside Temperature [C]
+Zone,Average,Surface Window Divider Inside Temperature [C]
+Zone,Average,Surface Window Divider Outside Temperature [C]
+\end{lstlisting}
+
+If the user requests to display advanced report/output variables (e.g.~see Output:Diagnostics keyword DisplayAdvancedReportVariables) the the following additional output variables are available for exterior windows and glass doors
+
+\begin{lstlisting}
+Zone,Average,Surface Window Inside Face Glazing Zone Convection Heat Gain Rate [W]
+Zone,Average,Surface Window Inside Face Glazing Net Infrared Heat Transfer Rate [W]
+Zone,Average,Surface Window Shortwave from Zone Back Out Window Heat Transfer Rate [W]
+Zone,Average,Surface Window Inside Face Frame and Divider Zone Heat Gain Rate [W]
+Zone,Average,Surface Window Inside Face Gap between Shade and Glazing Zone Convection Heat Gain Rate [W]
+Zone,Average,Surface Window Inside Face Shade Zone Convection Heat Gain Rate [W]
+Zone,Average,Surface Window Inside Face Shade Net Infrared Heat Transfer Rate [W]
+\end{lstlisting}
+
+Output variables applicable only to interior windows and glass doors:
+
+\begin{lstlisting}
+Zone,Average, Surface Window Transmitted Beam Solar Radiation Rate [W]
+Zone,Sum,Surface Window Transmitted Beam Solar Radiation Energy [J]
+\end{lstlisting}
+
+If the user requests to display advanced report/output variables (e.g.~see Output:Diagnostics keyword DisplayAdvancedReportVariables) the the following additional output variable is available for Equivalent Layer Window;
+
+\begin{lstlisting}
+Zone,Average, Surface Window Inside Face Other Convection Heat Gain Rate [W]
+\end{lstlisting}
+
+Output variables applicable to interior and exterior windows and doors are:
+
+\begin{lstlisting}
+Zone,Average,Surface Window Total Absorbed Shortwave Radiation Rate Layer <x> [W]
+Zone,Average,Surface Window Front Face Temperature Layer <x> [C]
+Zone,Average,Surface Window Back Face Temperature Layer <x> [C]
+\end{lstlisting}
+
+\subsubsection{Surface Window Total Absorbed Shortwave Radiation Rate Layer \textless{}x\textgreater{} {[}W{]}}\label{surface-window-total-absorbed-shortwave-radiation-rate-layer-x-w}
+
+This will output shortwave radiation absorbed in a window layer. The key values for this output variable are the surface name. Layers are numbered from the outside to the inside of the surface. The full listing will appear in the RDD file.
+
+\subsubsection{Surface Window Front Face Temperature Layer \textless{}x\textgreater{} {[}C{]}}\label{surface-window-front-face-temperature-layer-x-c}
+
+This will output a temperature for the front face of the layer. The layer front face is considered to be the face closest to the outside environment. The full listing will appear in the RDD file.
+
+\subsubsection{Surface Window Back Face Temperature Layer \textless{}x\textgreater{} {[}C{]}}\label{surface-window-back-face-temperature-layer-x-c}
+
+This will output a temperature for the back face of the layer. The layer back face is considered to be the face closest to the inside environment. The full listing will appear in the RDD file.
+
+\subsection{Surface Output Variables (all heat transfer surfaces)}\label{surface-output-variables-all-heat-transfer-surfaces}
+
+The various output variables related to surface heat transfer are organized around the inside and outside face of each surface. The zone heat balance model draws energy balances at each side, or face, of a surface and so each surface essentially has two sets of results. The inside face is the side of a heat transfer surface that faces toward the thermal zone. The outside face is the side of a heat transfer surface that faces away from the thermal zone, typically facing outdoors. The Key Value for these is generally the user-defined name of the surface.
+
+\subsubsection{\texorpdfstring{Surface Inside Face Heat Balance Calculation Iteration Count {[]}}{Surface Inside Face Heat Balance Calculation Iteration Count }}\label{surface-inside-face-heat-balance-calculation-iteration-count}
+
+This output is the number of iterations used in a part of the solution for surface heat transfer that accounts for thermal radiation heat transfer between zone surfaces. This is simply a counter on the iteration loop for inside face surface modeling. There is only one instance of this output in a given run and the Key Value is ``Simulation.''
+
+\subsubsection{Surface Inside Face Temperature {[}C{]}}\label{surface-inside-face-temperature-c}
+
+This is the temperature of the surface's inside face, in degrees Celsius. Former Name: Prior to version 7.1 this output was called Surface Inside Temperature.
+
+\subsubsection{Surface Outside Face Temperature {[}C{]}}\label{surface-outside-face-temperature-c}
+
+This is the temperature of the surface's outside face, in degrees Celsius. Former Name: Prior to version 7.1, this output was called Surface Outside Temperature.
+
+\subsubsection{Surface Inside Face Adjacent Air Temperature {[}C{]}}\label{surface-inside-face-adjacent-air-temperature-c}
+
+This is the effective bulk air temperature used for modeling the inside surface convection heat transfer. This is the same as the zone mean air temperature when using the mixing model for roomair. However, if more advanced roomair models are used, this variable will report the air temperature predicted by the roomair model as it was used in the surface heat balance model calculations. Former Name: Prior to version 7.1, this output was called Surface Int Adjacent Air Temperature.
+
+\subsubsection{Surface Inside Face Convection Heat Gain Rate {[}W{]}}\label{surface-inside-face-convection-heat-gain-rate-w}
+
+\subsubsection{Surface Inside Face Convection Heat Gain Rate per Area {[}W/m2{]}}\label{surface-inside-face-convection-heat-gain-rate-per-area-wm2}
+
+\subsubsection{Surface Inside Face Convection Heat Gain Energy {[}J{]}}\label{surface-inside-face-convection-heat-gain-energy-j}
+
+These ``inside face convection heat gain'' output variables describe the heat transferred by convection between the inside face and the zone air. The values can be positive or negative with positive indicating heat is being added to the surface's face by convection. Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
+
+Former Name: Prior to version 7.1, these outputs were called ``Surface Int Convection Heat *'' and had used the opposite sign convention.
+
+\subsubsection{Surface Inside Face Convection Heat Transfer Coefficient {[}W/m2-K{]}}\label{surface-inside-face-convection-heat-transfer-coefficient-wm2-k}
+
+This is the coefficient that describes the convection heat transfer. It is the value of ``Hc'' in the classic convection model Q = Hc* A* (T -- T). This is the result of the surface convection algorithm used for the inside face. Former Name: Prior to version 7.1, this output was called ``Surface Int Convection Coeff.''
+
+\subsubsection{Surface Inside Face Net Surface Thermal Radiation Heat Gain Rate {[}W{]}}\label{surface-inside-face-net-surface-thermal-radiation-heat-gain-rate-w}
+
+\subsubsection{Surface Inside Face Net Surface Thermal Radiation Heat Gain Rate per Area {[}W/m2{]}}\label{surface-inside-face-net-surface-thermal-radiation-heat-gain-rate-per-area-wm2}
+
+\subsubsection{Surface Inside Face Net Surface Thermal Radiation Heat Gain Energy {[}J{]}}\label{surface-inside-face-net-surface-thermal-radiation-heat-gain-energy-j}
+
+These ``inside face net surface thermal radiation heat gain'' output variables describe the heat transferred by longwave infrared thermal radiation exchanges between the inside faces of other surfaces in the zone. The values can be positive or negative with positive indicating heat is being added to the surface's face by thermal radiation. Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
+
+\subsubsection{Surface Inside Face Solar Radiation Heat Gain Rate {[}W{]}}\label{surface-inside-face-solar-radiation-heat-gain-rate-w}
+
+\subsubsection{Surface Inside Face Solar Radiation Heat Gain Rate per Area {[}W/m2{]}}\label{surface-inside-face-solar-radiation-heat-gain-rate-per-area-wm2}
+
+\subsubsection{Surface Inside Face Solar Radiation Heat Gain Energy {[}J{]}}\label{surface-inside-face-solar-radiation-heat-gain-energy-j}
+
+These ``inside face solar radiation heat gain'' output variables describe the heat transferred by solar radiation onto the inside face. The values are always positive and indicate heat is being added to the surface's face by solar radiation. This is sunlight that has entered the zone through a window and been absorbed on the inside face of the surface. Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
+
+\subsubsection{Surface Inside Face Lights Radiation Heat Gain Rate {[}W{]}}\label{surface-inside-face-lights-radiation-heat-gain-rate-w}
+
+\subsubsection{Surface Inside Face Lights Radiation Heat Gain Rate per Area {[}W/m2{]}}\label{surface-inside-face-lights-radiation-heat-gain-rate-per-area-wm2}
+
+\subsubsection{Surface Inside Face Lights Radiation Heat Gain Energy {[}J{]}}\label{surface-inside-face-lights-radiation-heat-gain-energy-j}
+
+These ``inside face lights radiation heat gain'' output variables describe the heat transferred by shortwave radiation onto the inside face. The values are always positive and indicate heat is being added to the surface's face by shortwave radiation that emanated from electric lighting equipment and was absorbed by the surface. Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
+
+\subsubsection{Surface Inside Face Internal Gains Radiation Heat Gain Rate {[}W{]}}\label{surface-inside-face-internal-gains-radiation-heat-gain-rate-w}
+
+\subsubsection{Surface Inside Face Internal Gains Radiation Heat Gain Rate per Area {[}W/m2{]}}\label{surface-inside-face-internal-gains-radiation-heat-gain-rate-per-area-wm2}
+
+\subsubsection{Surface Inside Face Internal Gains Radiation Heat Gain Energy {[}J{]}}\label{surface-inside-face-internal-gains-radiation-heat-gain-energy-j}
+
+These ``inside face internal gains radiation heat gain'' output variables describe the heat transferred by longwave infrared thermal radiation onto the inside face that emanated from internal gains such as lights, electric equipment, and people. The values are always positive and indicate heat is being added to the surface's face by the absorption of longwave thermal radiation. Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
+
+\subsubsection{Surface Inside Face System Radiation Heat Gain Rate {[}W{]}}\label{surface-inside-face-system-radiation-heat-gain-rate-w}
+
+\subsubsection{Surface Inside Face System Radiation Heat Gain Rate per Area {[}W/m2{]}}\label{surface-inside-face-system-radiation-heat-gain-rate-per-area-wm2}
+
+\subsubsection{Surface Inside Face System Radiation Heat Gain Energy {[}J{]}}\label{surface-inside-face-system-radiation-heat-gain-energy-j}
+
+These ``inside face system radiation heat gain'' output variables describe the heat transferred by infrared thermal radiation onto the inside face that emanated from HVAC equipment such as baseboard heaters or high-temperature radiant heating panels. The values are always positive and indicate heat is being added to the surface's face by the absorption of thermal radiation. Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
+
+\subsubsection{Surface Outside Face Convection Heat Gain Rate {[}W{]}}\label{surface-outside-face-convection-heat-gain-rate-w}
+
+\subsubsection{Surface Outside Face Convection Heat Gain Rate per Area {[}W/m2{]}}\label{surface-outside-face-convection-heat-gain-rate-per-area-wm2}
+
+\subsubsection{Surface Outside Face Convection Heat Gain Energy {[}J{]}}\label{surface-outside-face-convection-heat-gain-energy-j}
+
+These ``outside face convection'' output variables describe heat transferred by convection between the outside face and the surrounding air. The values can be positive or negative with positive values indicating heat is added to the surface face by convection heat transfer. Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m\(^{2}\)), and an energy version (J).
+
+Former Name: Prior to version 7.1, these outputs were called ``Surface Ext Convection Heat *'' and used the opposite sign convention.
+
+\subsubsection{Surface Outside Face Convection Heat Transfer Coefficient {[}W/m2-K{]}}\label{surface-outside-face-convection-heat-transfer-coefficient-wm2-k}
+
+This is the coefficient that describes the convection heat transfer. It is the value of ``Hc'' in the classic convection model Q = Hc* A* (T -- T). This is the result of the surface convection algorithm used for the outside face. Former Name: Prior to Version 7.1, this output was called ``Surface Ext Convection Coeff.''
+
+\subsubsection{Surface Outside Face Net Thermal Radiation Heat Gain Rate {[}W{]}}\label{surface-outside-face-net-thermal-radiation-heat-gain-rate-w}
+
+\subsubsection{Surface Outside Face Net Thermal Radiation Heat Gain Rate per Area {[}W/m2{]}}\label{surface-outside-face-net-thermal-radiation-heat-gain-rate-per-area-wm2}
+
+\subsubsection{Surface Outside Face Net Thermal Radiation Heat Gain Energy {[}J{]}}\label{surface-outside-face-net-thermal-radiation-heat-gain-energy-j}
+
+These ``outside face net thermal radiation'' output variables describe the heat transferred by longwave infrared thermal radiation exchanges between the surface and the surroundings of the outside face. This is the net of all forms of longwave thermal infrared radiation heat transfer. The values can be positive or negative with positive indicating the net addition of heat to the outside face. Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
+
+Former Name: Prior to version 7.1, these outputs were called ``Surface Ext Thermal Radiation Heat *'' and used the opposite sign convention.
+
+\subsubsection{Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate {[}W{]}}\label{surface-inside-face-exterior-windows-incident-beam-solar-radiation-rate-w}
+
+\subsubsection{Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-inside-face-exterior-windows-incident-beam-solar-radiation-rate-per-area-wm2}
+
+\subsubsection{Surface Inside Face Exterior Windows Incident Beam Solar Radiation Energy {[}J{]}}\label{surface-inside-face-exterior-windows-incident-beam-solar-radiation-energy-j}
+
+Beam solar radiation from the exterior windows in a zone incident on the inside face of a surface in the zone. If Solar Distribution in the BUILDING object is equal to MinimalShadowing or FullExterior, it is assumed that all beam solar from exterior windows falls on the floor. In this case the value of this output variable can be greater than zero only for floor surfaces. If Solar Distribution equals FullInteriorExterior the program tracks where beam solar from exterior windows falls inside the zone, in which case the value of this variable can be greater than zero for floor as well as wall surfaces. Different versions of the report are available including the basic incident rate (W), a per unit area flux (W/m2), and an energy version (J).
+
+\subsubsection{Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate {[}W{]}}\label{surface-inside-face-interior-windows-incident-beam-solar-radiation-rate-w}
+
+\subsubsection{Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-inside-face-interior-windows-incident-beam-solar-radiation-rate-per-area-wm2}
+
+\subsubsection{Surface Inside Face Interior Windows Incident Beam Solar Radiation Energy {[}J{]}}\label{surface-inside-face-interior-windows-incident-beam-solar-radiation-energy-j}
+
+Beam solar radiation from the interior (i.e., interzone) windows in a zone incident on the inside face of a surface in the zone. This value is calculated only if Solar Distribution in the BUILDING object is equal to FullInteriorExterior. However, the program does not track where this radiation falls. Instead, it is treated by the program as though it were diffuse radiation uniformly distributed over all of the zone surfaces. See \textbf{Figure~\ref{fig:beam-solar-radiation-entering-a-zone-through}}. Different versions of the report are available including the basic incident rate (W), a per unit area flux (W/m2), and an energy version (J).
+
+\begin{figure}[hbtp] % fig 31
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image057.png}
+\caption{Beam solar radiation entering a zone through an interior window is distributed inside the zone as though it were diffuse radiation. \protect \label{fig:beam-solar-radiation-entering-a-zone-through}}
+\end{figure}
+
+\subsubsection{Surface Inside Face Initial Transmitted Diffuse Absorbed Solar Radiation Rate {[}W{]}}\label{surface-inside-face-initial-transmitted-diffuse-absorbed-solar-radiation-rate-w}
+
+As of Version 2.1, diffuse solar transmitted through exterior and interior windows is no longer uniformly distributed. Instead, it is distributed according to the approximate view factors between the transmitting window and all other heat transfer surfaces in the zone. This variable is the amount of transmitted diffuse solar that is initially absorbed on the inside of each heat transfer surface. The portion of this diffuse solar that is reflected by all surfaces in the zone is subsequently redistributed uniformly to all heat transfer surfaces in the zone, along with interior reflected beam solar and shortwave radiation from lights. The total absorbed shortwave radiation is given by the next variable.
+
+\subsubsection{Surface Inside Face Absorbed Shortwave Radiation Rate {[}W{]}}\label{surface-inside-face-absorbed-shortwave-radiation-rate-w}
+
+As of Version 2.1, the previous variable plus absorbed shortwave radiation from uniformly distributed initially-reflected diffuse solar, reflected beam solar, and shortwave radiation from lights. This sum is the power of all sources of solar and visible radiation absorbed by the surface at the inside face.
+
+\subsection{Surface Output Variables (exterior heat transfer surfaces)}\label{surface-output-variables-exterior-heat-transfer-surfaces}
+
+\subsubsection{Surface Outside Face Outdoor Air Drybulb Temperature {[}C{]}}\label{surface-outside-face-outdoor-air-drybulb-temperature-c}
+
+The outdoor air dry-bulb temperature calculated at the height above ground of the surface centroid. Former Name: Prior to version 7.1, this output was called ``Surface Ext Outdoor Dry Bulb.''
+
+\subsubsection{Surface Outside Face Outdoor Air Wetbulb Temperature {[}C{]}}\label{surface-outside-face-outdoor-air-wetbulb-temperature-c}
+
+The outdoor air wet-bulb temperature calculated at the height above ground of the surface centroid. Former Name: Prior to version 7.1, this output was called ``Surface Ext Outdoor Wet Bulb.''
+
+\subsubsection{Surface Outside Face Outdoor Air Wind Speed {[}m/s{]}}\label{surface-outside-face-outdoor-air-wind-speed-ms}
+
+The outdoor wind speed calculated at the height above ground of the surface centroid. Former Name: Prior to version 7.1, this output was called ``Surface Ext Wind Speed.''
+
+\subsubsection{Surface Outside Face Sunlit Area {[}m2{]}}\label{surface-outside-face-sunlit-area-m2}
+
+The outside area of an exterior surface that is illuminated by (unreflected) beam solar radiation.
+
+\subsubsection{\texorpdfstring{Surface Outside Face Sunlit Fraction {[]}}{Surface Outside Face Sunlit Fraction }}\label{surface-outside-face-sunlit-fraction}
+
+The fraction of the outside area of an exterior surface that is illuminated by (unreflected) beam solar radiation. Equals Surface Outside Face Sunlit Area divided by total surface area.
+
+\subsubsection{Surface Outside Face Thermal Radiation to Air Heat Transfer Coefficient {[}W/m2-K{]}}\label{surface-outside-face-thermal-radiation-to-air-heat-transfer-coefficient-wm2-k}
+
+This is the coefficient that describes thermal radiation heat transfer between the outside face and the air mass surrounding the surface. It is the value of ``Hr'' in the classic linearized model for thermal radiation Q = Hr * A * (T\_surf -- T\_surfodb) when applied to the ambient air. Where T\_surf = Surface Outside Face Temperature, and T\_surfodb = Surface Outside Face Outdoor Air Drybulb Temperature. Former Name: Prior to version 7.1, this output was called ``Surface Ext Rad to Air Coeff.''
+
+\subsubsection{Surface Outside Face Thermal Radiation to Sky Heat Transfer Coefficient {[}W/m2-K{]}}\label{surface-outside-face-thermal-radiation-to-sky-heat-transfer-coefficient-wm2-k}
+
+This is the coefficient that describes thermal radiation heat transfer between the outside face and the sky surrounding the surface. It is the value of ``Hr'' in the classic linearized model for thermal radiation Q = Hr * A * (T\_surf -- T\_sky) when applied to the sky. Where T\_surf = Surface Outside Face Temperature, and T\_sky = Site Sky Temperature. Former Name: Prior to version 7.1, this output was called ``Surface Ext Rad to Sky Coeff.''
+
+\subsubsection{Surface Outside Face Thermal Radiation to Ground Heat Transfer Coefficient {[}W/m2-K{]}}\label{surface-outside-face-thermal-radiation-to-ground-heat-transfer-coefficient-wm2-k}
+
+This is the coefficient that describes thermal radiation heat transfer between the outside face and the ground surrounding the surface. It is the value of ``Hr'' in the classic linearized model for thermal radiation Q = Hr * A * (T\_surf -- T\_odb) when applied to the ground. Where T\_surf = Surface Outside Face Temperature, and T\_odb = Site Outdoor Air Drybulb Temperature (used as an approximation for the ground surface temperature). Former Name: Prior to version 7.1, this output was called ``Surface Ext Rad to Ground Coeff.''
+
+\subsubsection{Surface Outside Face Solar Radiation Heat Gain Rate {[}W{]}}\label{surface-outside-face-solar-radiation-heat-gain-rate-w}
+
+\subsubsection{Surface Outside Face Solar Radiation Heat Gain Rate per Area {[}W/m2{]}}\label{surface-outside-face-solar-radiation-heat-gain-rate-per-area-wm2}
+
+\subsubsection{Surface Outside Face Solar Radiation Heat Gain Energy {[}J{]}}\label{surface-outside-face-solar-radiation-heat-gain-energy-j}
+
+These ``outside face solar radiation'' output variables describe the heat transferred by the absorption of solar radiation at the outside face. This is the result of incident solar radiation being absorbed at the surface face. The values are always positive.
+
+\subsubsection{Surface Outside Face Incident Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-outside-face-incident-solar-radiation-rate-per-area-wm2}
+
+The total solar radiation incident on the outside of an exterior surface. It is the sum of:
+
+\begin{itemize}
+\item
+  Surface Outside Face Incident Beam Solar Radiation Rate per Area
+\item
+  Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area
+\item
+  Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area
+\item
+  Surface Outside Face Incident Sky Diffuse Surface Reflected Solar Radiation Rate per Area
+\item
+  Surface Outside Face Incident Beam To Beam Surface Reflected Solar Radiation Rate per Area
+\item
+  Surface Outside Face Incident Sky Diffuse Surface Reflected Solar Radiation Rate per Area
+\end{itemize}
+
+\subsubsection{Surface Outside Face Incident Beam Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-outside-face-incident-beam-solar-radiation-rate-per-area-wm2}
+
+The solar beam radiation incident on the outside of an exterior surface, including the effects of shadowing, if present. The beam here is that directly from the sun; it excludes beam specularly reflected from obstructions.
+
+\subsubsection{Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-outside-face-incident-sky-diffuse-solar-radiation-rate-per-area-wm2}
+
+The solar diffuse radiation from the sky incident on the outside of an exterior surface, including the effects of shadowing, if present.
+
+\subsubsection{Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-outside-face-incident-ground-diffuse-solar-radiation-rate-per-area-wm2}
+
+The solar diffuse radiation incident on the outside of an exterior surface that arises from reflection of beam solar and sky diffuse solar from the ground. This is the sum of the next two output variables, ``Surface Outside Face Incident Beam To Diffuse Ground Reflected Solar Radiation Rate per Area'' and ``Surface Outside Face Incident Sky Diffuse Ground Reflected Solar Radiation Rate per Area.'' The reflected solar radiation from the ground is assumed to be diffuse and isotropic (there is no specular component).
+
+If ``Reflections'' option is not chosen in the Solar Distribution Field in the BUILDING object, the effects of shadowing are accounted for by the user-specified value of View Factor to Ground for the surface. If ``Reflections'' option is chosen, the program determines the effects of shadowing, including time-varying shadowing of the ground plane by the building itself.
+
+\subsubsection{Surface Outside Face Incident Beam To Diffuse Ground Reflected Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-outside-face-incident-beam-to-diffuse-ground-reflected-solar-radiation-rate-per-area-wm2}
+
+The solar diffuse radiation incident on the outside of an exterior surface that arises from beam-to-diffuse reflection from the ground. It is assumed that there is no beam-to-beam (specular) component. The beam here is that directly from the sun; it excludes beam specularly reflected from obstructions.
+
+\subsubsection{Surface Outside Face Incident Sky Diffuse Ground Reflected Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-outside-face-incident-sky-diffuse-ground-reflected-solar-radiation-rate-per-area-wm2}
+
+The solar diffuse radiation incident on the outside of an exterior surface that arises from sky diffuse solar reflection from the ground. The sky diffuse here is that directly from the sky; it excludes reflection of sky diffuse from obstructions.
+
+\subsubsection{Surface Outside Face Incident Sky Diffuse Surface Reflected Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-outside-face-incident-sky-diffuse-surface-reflected-solar-radiation-rate-per-area-wm2}
+
+The solar diffuse radiation incident on the outside of an exterior surface that arises from sky diffuse reflection from one or more obstructions. This value will be non-zero only if ``Reflections'' option is chosen in the BUILDING object.
+
+\subsubsection{Surface Outside Face Incident Beam To Beam Surface Reflected Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-outside-face-incident-beam-to-beam-surface-reflected-solar-radiation-rate-per-area-wm2}
+
+The solar beam radiation incident on the outside of an exterior surface that arises from beam-to-beam (specular) reflection from one or more obstructions. This value will be non-zero only if ``Reflections'' option is chosen in the BUILDING object. For windows, the program treats this beam radiation as diffuse radiation in calculating its transmission and absorption.
+
+\subsubsection{Surface Outside Face Incident Beam To Diffuse Surface Reflected Solar Radiation Rate per Area {[}W/m2{]}}\label{surface-outside-face-incident-beam-to-diffuse-surface-reflected-solar-radiation-rate-per-area-wm2}
+
+The solar diffuse radiation incident on the outside of an exterior surface that arises from beam-to-diffuse reflection from building shades or building surfaces. This value will be non-zero only if ``Reflections'' option is chosen in the BUILDING object.
+
+\subsubsection{\texorpdfstring{Surface Outside Face Beam Solar Incident Angle Cosine Value {[]}}{Surface Outside Face Beam Solar Incident Angle Cosine Value }}\label{surface-outside-face-beam-solar-incident-angle-cosine-value}
+
+The cosine of the angle of incidence of (unreflected) beam solar radiation on the outside of an exterior surface. The value varies from 0.0 for beam parallel to the surface (incidence angle = 90\(^{O}\)) to 1.0 for beam perpendicular to the surface (incidence angle = 0\(^{O}\)). Negative values indicate the sun is behind the surface, i.e the surface does not see the sun.
+
+\subsubsection{\texorpdfstring{Surface Anisotropic Sky Multiplier {[]}}{Surface Anisotropic Sky Multiplier }}\label{surface-anisotropic-sky-multiplier}
+
+This is the view factor multiplier for diffuse sky irradiance on exterior surfaces taking into account the anisotropic radiance of the sky. The diffuse sky irradiance on a surface is given by Anisotropic Sky Multiplier * Diffuse Solar Irradiance.
+
+\subsubsection{\texorpdfstring{Surface Window BSDF Beam Direction Number {[]}}{Surface Window BSDF Beam Direction Number }}\label{surface-window-bsdf-beam-direction-number}
+
+\subsubsection{Surface Window BSDF Beam Phi Angle {[}rad{]}}\label{surface-window-bsdf-beam-phi-angle-rad}
+
+\subsubsection{Surface Window BSDF Beam Theta Angle {[}rad{]}}\label{surface-window-bsdf-beam-theta-angle-rad}
+
+\subsection{Opaque Surface Output Variables}\label{opaque-surface-output-variables}
+
+The following variables apply only to opaque surfaces, where an opaque surface is considered here to be an exterior or interzone heat transfer surface of class FLOOR, WALL, ROOF or DOOR. \textbf{Note -- these are advanced variables -- you must read the descriptions and understand before use -- then you must use the} \textbf{Output:Diagnostics} \textbf{object to allow reporting.}
+
+\subsubsection{Surface Inside Face Conduction Heat Transfer Rate {[}W{]}}\label{surface-inside-face-conduction-heat-transfer-rate-w}
+
+\subsubsection{Surface Inside Face Conduction Heat Transfer Rate per Area {[}W/m2{]}}\label{surface-inside-face-conduction-heat-transfer-rate-per-area-wm2}
+
+\subsubsection{Surface Inside Face Conduction Heat Gain Rate {[}W{]}}\label{surface-inside-face-conduction-heat-gain-rate-w}
+
+\subsubsection{Surface Inside Face Conduction Heat Loss Rate {[}W{]}}\label{surface-inside-face-conduction-heat-loss-rate-w}
+
+These ``inside face conduction'' output variables describe heat flow by conduction right at the inside face of an opaque heat transfer surface. A positive value means that the conduction is from just inside the inside face toward the inside face. A negative value means that the conduction is from the inside face into the core of the heat transfer surface.
+
+Note that Inside Face Conduction, when positive, does \textbf{not} indicate the heat flow from the surface to the zone air, which is governed by the inside face convection coefficient and the difference in temperature between the inside face and the zone air.
+
+Different versions of the reports are available. The basic heat gain rate (W) and a per unit area flux (W/m\(^{2}\)) can have positive or negative values with the sign convention that positive indicates heat flowing toward the face itself. There are also directed ``gain'' and ``loss'' versions that have only positive values or zero when the heat flow direction opposes.
+
+Former Name: Prior to version 7.1, these outputs were called ``Opaque Surface Inside Face Conduction *.''
+
+Former Name: For Conduction Finite Difference simulations (CondFD), CondFD Inside Surface Heat Flux is replaced with Surface Inside Face Conduction Heat Transfer Rate Per Area. Likewise for CondFD Inside Heat Flux to Surface.
+
+\subsubsection{Surface Outside Face Conduction Heat Transfer Rate {[}W{]}}\label{surface-outside-face-conduction-heat-transfer-rate-w}
+
+\subsubsection{Surface Outside Face Conduction Heat Transfer Rate per Area {[}W/m2{]}}\label{surface-outside-face-conduction-heat-transfer-rate-per-area-wm2}
+
+\subsubsection{Surface Outside Face Conduction Heat Gain Rate {[}W{]}}\label{surface-outside-face-conduction-heat-gain-rate-w}
+
+\subsubsection{Surface Outside Face Conduction Heat Loss Rate {[}W{]}}\label{surface-outside-face-conduction-heat-loss-rate-w}
+
+These ``outside face conduction'' output variables describe heat flow by conduction right at the outside face of an opaque heat transfer surface. A positive value means that the conduction is from just inside the outside face toward the outside face. A negative value means that the conduction is from the outside face into the core of the heat transfer surface.
+
+Note that outside face conduction, when positive, does \textbf{not} indicate the heat flow from the surface to the surrounding air, which is governed by the outside face convection coefficient and the difference in temperature between the inside face and the surrounding air.
+
+Different versions of the reports are available. The basic heat transfer rate (W) and a per unit area flux (W/m\(^{2}\)) can have positive or negative values with the sign convention that positive indicates heat flowing toward the face itself. There are also directed ``gain'' and ``loss'' versions that have only positive values or zero when the heat flow direction opposes.
+
+Former Name: For Conduction Finite Difference simulations (CondFD), CondFD Outside Surface Heat Flux is replaced with Surface Outside Face Conduction Heat Transfer Rate Per Area. Likewise for CondFD Outside Heat Flux to Surface.
+
+\subsubsection{Surface Average Face Conduction Heat Transfer Rate {[}W{]}}\label{surface-average-face-conduction-heat-transfer-rate-w}
+
+\subsubsection{Surface Average Face Conduction Heat Transfer Rate per Area {[}W/m2{]}}\label{surface-average-face-conduction-heat-transfer-rate-per-area-wm2}
+
+\subsubsection{Surface Average Face Conduction Heat Gain Rate {[}W{]}}\label{surface-average-face-conduction-heat-gain-rate-w}
+
+\subsubsection{Surface Average Face Conduction Heat Loss Rate {[}W{]}}\label{surface-average-face-conduction-heat-loss-rate-w}
+
+\subsubsection{Surface Average Face Conduction Heat Transfer Energy {[}J{]}}\label{surface-average-face-conduction-heat-transfer-energy-j}
+
+These ``average face conduction'' output variables combine the inside face conduction and outside face conduction reports together to describe the conduction situation in a heat transfer surface in a nominal way. This is simply the average of the inside and outside face conduction rates, but with the sign convention for the outside face switched to match the inside face so that positive values here indicate heat flowing into the thermal zone.
+
+Different versions of the reports are available. The basic heat conduction rate (W) and a per unit area flux (W/m\(^{2}\)) can have positive or negative values with the sign convention that positive indicates heat flowing toward the thermal zone. There are also directed ``gain'' and ``loss'' versions that have only positive values or zero when the heat flow direction opposes (W). Finally there is a version for total energy transfer (J).
+
+\subsubsection{Surface Heat Storage Rate {[}W{]}}\label{surface-heat-storage-rate-w}
+
+\subsubsection{Surface Heat Storage Rate per Area {[}W/m2{]}}\label{surface-heat-storage-rate-per-area-wm2}
+
+\subsubsection{Surface Heat Storage Gain Rate {[}W{]}}\label{surface-heat-storage-gain-rate-w}
+
+\subsubsection{Surface Heat Storage Loss Rate {[}W{]}}\label{surface-heat-storage-loss-rate-w}
+
+\subsubsection{Surface Heat Storage Energy {[}J{]}}\label{surface-heat-storage-energy-j}
+
+These ``heat storage'' output variables combine the inside face conduction and outside face conduction reports together to describe the thermal storage situation in a heat transfer surface in a nominal way. This is simply the difference between the inside and outside face conduction, but with the sign convention arranged so that positive values indicate heat being added to the core of the surface.
+
+Different versions of the reports are available. The basic heat storage rate (W) and a per unit area flux (W/m\(^{2}\)) can have positive or negative values with the sign convention that positive indicates heat being added to the surface's mass. There are also directed ``gain'' and ``loss'' versions that have only positive values or zero when the heat storage direction opposes (W). Finally there is a version for total energy stored (J).
+
+\subsubsection{Surface Internal Source Location Temperature {[}C{]}}\label{surface-internal-source-location-temperature-c}
+
+When a surface has an internal source or sink (defined using Construction:InternalSource) then this output is available for the temperature within the surface at the location of the source/sink.
+
+\subsubsection{Zone Opaque Surface Inside Face Conduction {[}W{]}}\label{zone-opaque-surface-inside-face-conduction-w}
+
+The sum of the Opaque Surface Inside Face Conduction values for all opaque surfaces in a zone for both positive and negative sums. For example, assume a zone has six opaque surfaces with Opaque Surface Inside Face Conduction values of 100, -200, 400, 50, 150 and --300 W. Then Zone Opaque Surface Inside Face Conduction = 700 - 500 = 200 W. Or if a zone has six opaque surfaces with Opaque Surface Inside Face Conduction values of -100, -200, 400, -50, 150 and --300W. Then Zone Opaque Surface Inside Face Conduction = 550 -- 650 = -100 W.
+
+\subsubsection{Zone Opaque Surface Inside Faces Total Conduction Heat Gain Rate {[}W{]}}\label{zone-opaque-surface-inside-faces-total-conduction-heat-gain-rate-w}
+
+\subsubsection{Zone Opaque Surface Inside Faces Total Conduction Heat Gain Energy {[}J{]}}\label{zone-opaque-surface-inside-faces-total-conduction-heat-gain-energy-j}
+
+These are the power and energy sums for the Opaque Surface Inside Face Conduction values for all opaque surfaces in a zone when that sum is positive. For example, assume a zone has six opaque surfaces with Opaque Surface Inside Face Conduction values of 100, -200, 400, 50, 150 and --300 W. Then Zone Opaque Surface Inside Faces Total Conduction Heat Gain Rate = 700 - 500 = 200 W.
+
+\subsubsection{Zone Opaque Surface Inside Faces Total Conduction Heat Loss Rate {[}W{]}}\label{zone-opaque-surface-inside-faces-total-conduction-heat-loss-rate-w}
+
+\subsubsection{Zone Opaque Surface Inside Faces Total Conduction Heat Loss Energy {[}J{]}}\label{zone-opaque-surface-inside-faces-total-conduction-heat-loss-energy-j}
+
+These are the power and energy absolute value for the sums of the Opaque Surface Inside Face Conduction values for all opaque surfaces in a zone when that sum is negative. For example, assume a zone has six opaque surfaces with Opaque Surface Inside Face Conduction values of -100, -200, 400, -50, 150 and --300W. Then Zone Opaque Surface Inside Faces Total Conduction Heat Loss Rate = \textbar{}550 -- 650\textbar{} = \textbar{}-100\textbar{} = 100 W.
+
+\subsubsection{Zone Opaque Surface Outside Face Conduction {[}W{]}}\label{zone-opaque-surface-outside-face-conduction-w}
+
+The sum of the Opaque Surface Outside Face Conduction values for all opaque surfaces in a zone for both positive and negative sums. For example, assume a zone has six opaque surfaces with Opaque Surface Outside Face Conduction values of 100, -200, 400, 50, 150 and --300 W. Then Zone Opaque Surface Outside Face Conduction = 700 - 500 = 200 W. Or if a zone has six opaque surfaces with Opaque Surface Outside Face Conduction values of -100, -200, 400, -50, 150 and --300W. Then Zone Opaque Surface Outside Face Conduction = 550 -- 650 = -100 W.
+
+\subsubsection{Zone Opaque Surface Outside Face Conduction Gain {[}W{]}}\label{zone-opaque-surface-outside-face-conduction-gain-w}
+
+\subsubsection{Zone Opaque Surface Outside Face Conduction Gain Energy {[}J{]}}\label{zone-opaque-surface-outside-face-conduction-gain-energy-j}
+
+These are the power and energy sums for the Opaque Surface Outside Face Conduction values for all opaque surfaces in a zone when that sum is positive. For example, assume a zone has six opaque surfaces with Opaque Surface Outside Face Conduction values of 100, -200, 400, 50, 150 and --300 W. Then Zone Opaque Surface Outside Face Conduction Gain = 700 - 500 = 200 W.
+
+\subsubsection{Zone Opaque Surface Outside Face Conduction Loss {[}W{]}}\label{zone-opaque-surface-outside-face-conduction-loss-w}
+
+\subsubsection{Zone Opaque Surface Outside Face Conduction Loss Energy {[}J{]}}\label{zone-opaque-surface-outside-face-conduction-loss-energy-j}
+
+These are the power and energy absolute value for the sums of the Opaque Surface Outside Face Conduction values for all opaque surfaces in a zone when that sum is negative. For example, assume a zone has six opaque surfaces with Opaque Surface Outside Face Conduction values of -100, -200, 400, -50, 150 and -300W. Then Zone Opaque Surface Outside Face Conduction Loss = \textbar{}550 -- 650\textbar{} = \textbar{}-100\textbar{} = 100 W.
+
+\subsubsection{Surface Inside Face Beam Solar Radiation Heat Gain Rate {[}W{]}}\label{surface-inside-face-beam-solar-radiation-heat-gain-rate-w}
+
+Beam solar radiation from exterior windows absorbed on the inside face of an opaque heat transfer surface. For Solar Distribution = FullInteriorAndExterior, this quantity can be non-zero for both floor and wall surfaces. Otherwise, for Solar Distribution = FullExterior or MinimalShadowing, it can be non-zero only for floor surfaces since in this case all entering beam solar is assumed to fall on the floor. Note that this variable will not be operational (have a real value) unless there are exterior windows in the zone.
+
+\subsection{Window Output Variables}\label{window-output-variables-1}
+
+The following output variables apply to subsurfaces that are windows or glass doors. These two subsurface types are called ``window'' here. ``Exterior window'' means that the base surface of the window is an exterior wall, floor, roof or ceiling (i.e., the base surface is a BuildingSurface:Detailed with OutsideFaceEnvironment = ExteriorEnvironment). ``Interior window'' means that the base surface of the window is an inter-zone wall, floor or ceiling. ``Glass'' means a transparent solid layer, usually glass, but possibly plastic or other transparent material. ``Shading device'' means an interior, exterior or between-glass shade or blind, or an exterior screen (only exterior windows can have a shading device).
+
+\subsubsection{Zone Windows Total Transmitted Solar Radiation Rate {[}W{]}}\label{zone-windows-total-transmitted-solar-radiation-rate-w}
+
+\subsubsection{Zone Windows Total Transmitted Solar Radiation Energy {[}J{]}}\label{zone-windows-total-transmitted-solar-radiation-energy-j}
+
+The total Surface Window Transmitted Solar Radiation Rate of all the exterior windows in a zone.
+
+\subsubsection{Zone Windows Total Heat Gain Rate {[}W{]}}\label{zone-windows-total-heat-gain-rate-w}
+
+\subsubsection{Zone Windows Total Heat Gain Energy {[}J{]}}\label{zone-windows-total-heat-gain-energy-j}
+
+The sum of the heat flow from all of the exterior windows in a zone when that sum is positive. (See definition of ``heat flow'' under ``Window Heat Gain,'' below.)
+
+\subsubsection{Zone Windows Total Heat Loss Rate {[}W{]}}\label{zone-windows-total-heat-loss-rate-w}
+
+\subsubsection{Zone Windows Total Heat Loss Energy {[}J{]}}\label{zone-windows-total-heat-loss-energy-j}
+
+The absolute value of the sum of the heat flow from all of the exterior windows in a zone when that sum is negative.
+
+\subsubsection{Surface Window Total Glazing Layers Absorbed Shortwave Radiation Rate {[}W{]}}\label{surface-window-total-glazing-layers-absorbed-shortwave-radiation-rate-w}
+
+\subsubsection{Surface Window Total Glazing Layers Absorbed Solar Radiation Rate {[}W{]}}\label{surface-window-total-glazing-layers-absorbed-solar-radiation-rate-w}
+
+\subsubsection{Surface Window Total Glazing Layers Absorbed Solar Radiation Energy {[}J{]}}\label{surface-window-total-glazing-layers-absorbed-solar-radiation-energy-j}
+
+The total exterior beam and diffuse solar radiation absorbed in all of the glass layers of an exterior window.
+
+\subsubsection{Surface Window Shading Device Absorbed Solar Radiation Rate {[}W{]}}\label{surface-window-shading-device-absorbed-solar-radiation-rate-w}
+
+Surface Window Shading Device Absorbed Solar Radiation Energy {[}J{]}
+
+The exterior beam and diffuse solar radiation absorbed in the shading device, if present, of an exterior window.
+
+\subsubsection{Surface Window Transmitted Solar Radiation Rate {[}W{]}}\label{surface-window-transmitted-solar-radiation-rate-w}
+
+\subsubsection{Surface Window Transmitted Solar Radiation Energy {[}J{]}}\label{surface-window-transmitted-solar-radiation-energy-j}
+
+The amount of beam and diffuse solar radiation entering a zone through an exterior window. It is the sum of the following two variables, ``Surface Window Transmitted Beam Solar Radiation Rate'' and ``Surface Window Transmitted Diffuse Solar Radiation Rate.''
+
+\subsubsection{Surface Window Transmitted Beam Solar Radiation Rate {[}W{]}}\label{surface-window-transmitted-beam-solar-radiation-rate-w}
+
+\subsubsection{Surface Window Transmitted Beam Solar Radiation Energy {[}J{]}}\label{surface-window-transmitted-beam-solar-radiation-energy-j}
+
+The solar radiation transmitted by an exterior window whose source is beam solar incident on the outside of the window. For a bare window, this transmitted radiation consists of beam radiation passing through the glass (assumed transparent) and diffuse radiation from beam reflected from the outside window reveal, if present. For a window with a shade, this transmitted radiation is totally diffuse (shades are assumed to be perfect diffusers). For a window with a blind, this transmitted radiation consists of beam radiation that passes between the slats and diffuse radiation from beam-to-diffuse reflection from the slats. For a window with a screen, this value consists of direct beam radiation that is transmitted through the screen (gaps between the screen material) and diffuse radiation from beam-to-diffuse reflection from the screen material.
+
+For each zone time step,
+
+Surface Window Transmitted Beam Solar Radiation Rate = Surface Window Transmitted Beam To Beam Solar Radiation Rate + Surface Window Transmitted Beam To Diffuse Solar Radiation Rate
+
+Surface Window Transmitted Beam Solar Radiation Energy = Surface Window Transmitted Beam To Beam Solar Radiation Energy + Surface Window Transmitted Beam To Diffuse Solar Radiation Energy
+
+\subsubsection{Surface Window Transmitted Beam To Beam Solar Radiation Rate {[}W{]}}\label{surface-window-transmitted-beam-to-beam-solar-radiation-rate-w}
+
+\subsubsection{Surface Window Transmitted Beam To Beam Solar Radiation Energy {[}J{]}}\label{surface-window-transmitted-beam-to-beam-solar-radiation-energy-j}
+
+For a window with a blind, this transmitted radiation consists of beam radiation that passes between the slats. For a window with a screen, this value consists of direct beam radiation that is transmitted through the screen (gaps between the screen material).
+
+\subsubsection{Surface Window Transmitted Beam To Diffuse Solar Radiation Rate {[}W{]}}\label{surface-window-transmitted-beam-to-diffuse-solar-radiation-rate-w}
+
+\subsubsection{Surface Window Transmitted Beam To Diffuse Solar Radiation Energy {[}J{]}}\label{surface-window-transmitted-beam-to-diffuse-solar-radiation-energy-j}
+
+For a window with a blind, this transmitted radiation consists of diffuse radiation reflected from beam by the slats. For a window with a screen, this value consists of diffuse radiation reflected by the screen material.
+
+\subsubsection{Zone Exterior Windows Total Transmitted Beam Solar Radiation Rate {[}W{]}}\label{zone-exterior-windows-total-transmitted-beam-solar-radiation-rate-w}
+
+\subsubsection{Zone Exterior Windows Total Transmitted Beam Solar Radiation Energy {[}J{]}}\label{zone-exterior-windows-total-transmitted-beam-solar-radiation-energy-j}
+
+The sum of the Surface Window Transmitted Beam Solar Radiation Rate (see definition above) from all exterior windows in a zone.
+
+\subsubsection{Zone Interior Windows Total Transmitted Beam Solar Radiation Rate {[}W{]}}\label{zone-interior-windows-total-transmitted-beam-solar-radiation-rate-w}
+
+\subsubsection{Zone Interior Windows Total Transmitted Beam Solar Radiation Energy {[}J{]}}\label{zone-interior-windows-total-transmitted-beam-solar-radiation-energy-j}
+
+The sum of the Surface Window Transmitted Beam Solar Radiation Rate (see definition above) from all interior windows in a zone.
+
+\subsubsection{Surface Window Transmitted Diffuse Solar Radiation Rate {[}W{]}}\label{surface-window-transmitted-diffuse-solar-radiation-rate-w}
+
+\subsubsection{Surface Window Transmitted Diffuse Solar Radiation Energy {[}J{]}}\label{surface-window-transmitted-diffuse-solar-radiation-energy-j}
+
+The solar radiation transmitted by an exterior window whose source is diffuse solar incident on the outside of the window. For a bare window, this transmitted radiation consists of diffuse radiation passing through the glass. For a window with a shade, this transmitted radiation is totally diffuse (shades are assumed to be perfect diffusers). For a window with a blind, this transmitted radiation consists of diffuse radiation that passes between the slats and diffuse radiation from diffuse-to-diffuse reflection from the slats. For a window with a screen, this value consists of diffuse radiation transmitted through the screen (gaps between the screen material) and diffuse radiation from diffuse-to-diffuse reflection from the screen material.
+
+\subsubsection{Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Rate {[}W{]}}\label{zone-exterior-windows-total-transmitted-diffuse-solar-radiation-rate-w}
+
+\subsubsection{Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Energy {[}J{]}}\label{zone-exterior-windows-total-transmitted-diffuse-solar-radiation-energy-j}
+
+The combined beam and diffuse solar that first entered adjacent zones through exterior windows in the adjacent zones, was subsequently reflected from interior surfaces in those zones (becoming diffuse through that reflection), and was then transmitted through interior windows into the current zone.
+
+\subsubsection{Zone Interior Windows Total Transmitted Diffuse Solar Radiation Rate {[}W{]}}\label{zone-interior-windows-total-transmitted-diffuse-solar-radiation-rate-w}
+
+\subsubsection{Zone Interior Windows Total Transmitted Diffuse Solar Radiation Energy {[}J{]}}\label{zone-interior-windows-total-transmitted-diffuse-solar-radiation-energy-j}
+
+The sum of the Surface Window Transmitted Diffuse Solar Radiation Rate (see definition above) from all interior windows in a zone.
+
+\subsubsection{\texorpdfstring{Surface Window System Solar Transmittance {[]}}{Surface Window System Solar Transmittance }}\label{surface-window-system-solar-transmittance}
+
+Effective solar transmittance of an exterior window, including effect of shading device, if present. Equal to ``Surface Window Transmitted Solar Radiation Rate'' divided by total exterior beam plus diffuse solar radiation incident on the window (excluding frame, if present).
+
+\subsubsection{\texorpdfstring{Surface Window System Solar Absorptance {[]}}{Surface Window System Solar Absorptance }}\label{surface-window-system-solar-absorptance}
+
+Effective solar absorptance of an exterior window, including effect of shading device, if present. Equal to ``Window Solar Absorbed: All Glass Layers'' plus ``Window Solar Absorbed: Shading Device'' divided by total exterior beam plus diffuse solar radiation incident on window (excluding frame, if present)
+
+\subsubsection{\texorpdfstring{Surface Window System Solar Reflectance {[]}}{Surface Window System Solar Reflectance }}\label{surface-window-system-solar-reflectance}
+
+Effective solar reflectance of an exterior window, including effect of shading device, if present. Equal to: {[}1.0 -- ``Surface Window System Solar Transmittance'' -- ``Surface Window System Solar Absorptance''{]}.
+
+\subsubsection{Surface Window Gap Convective Heat Transfer Rate {[}W{]}}\label{surface-window-gap-convective-heat-transfer-rate-w}
+
+\subsubsection{Surface Window Gap Convective Heat Transfer Energy {[}J{]}}\label{surface-window-gap-convective-heat-transfer-energy-j}
+
+For an airflow window, the forced convective heat flow from the gap through which airflow occurs. This is the heat gained (or lost) by the air from the glass surfaces (and between-glass shading device surfaces, if present) that the air comes in contact with as it flows through the gap. If the gap airflow goes to the zone indoor air, the gap convective heat flow is added to the zone load. Applicable to exterior windows only.
+
+\subsubsection{Surface Window Heat Gain Rate {[}W{]}}\label{surface-window-heat-gain-rate-w}
+
+\subsubsection{Surface Window Heat Gain Energy {[}J{]}}\label{surface-window-heat-gain-energy-j}
+
+The total heat flow to the zone from the glazing, frame and divider of an exterior window when the total heat flow is positive.
+
+For a window \emph{without an interior shading device}, this heat flow is equal to:
+
+{[}Surface Window Transmitted Solar Radiation Rate (see definition, above){]}
+
+\begin{itemize}
+\item
+  {[}Convective heat flow to the zone from the zone side of the glazing{]}
+\item
+  {[}Net IR heat flow to the zone from zone side of the glazing{]}
+\end{itemize}
+
+-- {[}Short-wave radiation from zone transmitted back out the window{]}
+
+\begin{itemize}
+\tightlist
+\item
+  {[}Conduction to zone from window frame and divider, if present{]}
+\end{itemize}
+
+Here, short-wave radiation is that from lights and diffuse interior solar radiation.
+
+For a window \emph{with an interior shading device}, this heat flow is equal to:
+
+{[}Surface Window Transmitted Solar Radiation Rate{]}
+
+\begin{itemize}
+\item
+  {[}Convective heat flow to the zone from the air flowing through the gap between glazing and shading device{]}
+\item
+  {[}Convective heat flow to the zone from the zone side of the shading device{]}
+\item
+  {[}Net IR heat flow to the zone from the zone side of the glazing{]}
+\item
+  {[}Net IR heat flow to the zone from the zone side of the shading device{]}
+\end{itemize}
+
+-- {[}Short-wave radiation from zone transmitted back out the window{]}
+
+\begin{itemize}
+\tightlist
+\item
+  {[}Conduction to zone from window frame and divider, if present{]}
+\end{itemize}
+
+The total window heat flow can also be thought of as the sum of the solar and conductive gain from the window glazing.
+
+\subsubsection{Surface Window Heat Loss Rate {[}W{]}}\label{surface-window-heat-loss-rate-w}
+
+\subsubsection{Surface Window Heat Loss Energy {[}J{]}}\label{surface-window-heat-loss-energy-j}
+
+The absolute value of the total heat flow through an exterior window when the total heat flow is negative. (See definition of ``total heat flow'' under ``Surface Window Heat Gain Rate,'' above.)
+
+\subsubsection{\texorpdfstring{Surface Window Glazing Beam to Beam Solar Transmittance {[]}}{Surface Window Glazing Beam to Beam Solar Transmittance }}\label{surface-window-glazing-beam-to-beam-solar-transmittance}
+
+The fraction of exterior beam solar radiation incident on the glass of an exterior window that is transmitted through the glazing as beam radiation. This is for the base window without shading. Takes into account the angle of incidence of beam solar radiation on the glass.
+
+\subsubsection{\texorpdfstring{Surface Window Glazing Beam to Diffuse Solar Transmittance {[]}}{Surface Window Glazing Beam to Diffuse Solar Transmittance }}\label{surface-window-glazing-beam-to-diffuse-solar-transmittance}
+
+The fraction of exterior beam solar radiation incident on the glazing of an exterior window that is transmitted through the glazing as diffuse radiation.
+
+\subsubsection{\texorpdfstring{Surface Window Glazing Diffuse to Diffuse Solar Transmittance {[]}}{Surface Window Glazing Diffuse to Diffuse Solar Transmittance }}\label{surface-window-glazing-diffuse-to-diffuse-solar-transmittance}
+
+The fraction of exterior diffuse solar radiation incident on the glass of an exterior window that is transmitted through the glass assuming that the window has no shading device. It is assumed that incident diffuse solar is transmitted only as diffuse with no beam component.
+
+\subsubsection{\texorpdfstring{Surface Window Model Solver Iteration Count {[]}}{Surface Window Model Solver Iteration Count }}\label{surface-window-model-solver-iteration-count}
+
+The number of iterations needed by the window-layer heat balance solution to converge.
+
+\subsubsection{Surface Window Solar Horizontal Profile Angle {[}deg{]}}\label{surface-window-solar-horizontal-profile-angle-deg}
+
+For a vertical exterior window, this is an angle appropriate for calculating beam solar quantities appropriate to horizontal window elements such as horizontal reveal surfaces, horizontal frame and divider elements and horizontal slats of window blinds. It is defined as the angle between the window outward normal and the projection of the sun's ray on the vertical plane containing the outward normal. See Figure~\ref{fig:vertical-exterior-window-showing-solar}.
+
+For an exterior window of arbitrary tilt, it is defined as the angle between the window outward normal the projection of the sun's ray on the plane that contains the outward normal and is perpendicular to the ground.
+
+If the sun is behind the window, the horizontal profile angle is not defined and is reported as 0.0.
+
+Note that in most texts what we call ``horizontal profile angle'' is called ``vertical profile angle.''
+
+\subsubsection{Surface Window Solar Vertical Profile Angle {[}deg{]}}\label{surface-window-solar-vertical-profile-angle-deg}
+
+For a vertical exterior window, this is an angle appropriate for calculating beam solar quantities appropriate to vertical window elements such as vertical reveal surfaces, vertical frame and divider elements and vertical slats of window blinds. It is defined as the angle between the window outward normal and the projection of the sun's ray on the horizontal plane containing the outward normal. See \textbf{Figure~\ref{fig:vertical-exterior-window-showing-solar}.}
+
+For an exterior window of arbitrary tilt, it is defined as the angle between the window outward normal the projection of the sun's ray on the plane that contains the outward normal and is perpendicular to the plane defined above for Surface Window Solar Horizontal Profile Angle for a window of arbitrary tilt.
+
+If the sun is behind the window, the vertical profile angle is not defined and is reported as 0.0.
+
+Note that in most texts what we call ``vertical profile angle'' is called ``horizontal profile angle.''
+
+\begin{figure}[hbtp] % fig 32
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image058.png}
+\caption{Vertical exterior window showing solar horizontal profile angle, solar vertical profile angle and solar incidence angle. \protect \label{fig:vertical-exterior-window-showing-solar}}
+\end{figure}
+
+\subsubsection{Surface Window Outside Reveal Reflected Beam Solar Radiation Rate {[}W{]}}\label{surface-window-outside-reveal-reflected-beam-solar-radiation-rate-w}
+
+\subsubsection{Surface Window Outside Reveal Reflected Beam Solar Radiation Energy {[}J{]}}\label{surface-window-outside-reveal-reflected-beam-solar-radiation-energy-j}
+
+Beam solar radiation reflected from the outside reveal surfaces of a window (ref: Reveal Surfaces under WindowProperty:FrameAndDivider object). There are both rate and energy versions.
+
+\subsubsection{Surface Window Inside Reveal Reflected Beam Solar Radiation Rate {[}W{]}}\label{surface-window-inside-reveal-reflected-beam-solar-radiation-rate-w}
+
+\subsubsection{Surface Window Inside Reveal Reflected Beam Solar Radiation Energy {[}J{]}}\label{surface-window-inside-reveal-reflected-beam-solar-radiation-energy-j}
+
+Beam solar radiation reflected from the inside reveal surfaces of a window (ref: Reveal Surfaces under WindowProperty:FrameAndDivider object). There are both rate and energy versions.
+
+\subsubsection{Surface Window Inside Reveal Absorbed Beam Solar Radiation Rate {[}W{]}}\label{surface-window-inside-reveal-absorbed-beam-solar-radiation-rate-w}
+
+Beam solar radiation absorbed at the inside reveal surfaces of a window, in Watts.
+
+\subsubsection{Surface Window Inside Reveal Reflected Diffuse Zone Solar Radiation Rate {[}W{]}}\label{surface-window-inside-reveal-reflected-diffuse-zone-solar-radiation-rate-w}
+
+Diffuse solar radiation reflected from inside reveal surfaces of a window into the zone, in Watts.
+
+\subsubsection{Surface Window Inside Reveal Reflected Diffuse Frame Solar Radiation Rate {[}W{]}}\label{surface-window-inside-reveal-reflected-diffuse-frame-solar-radiation-rate-w}
+
+Diffuse solar radiation reflected from inside reveal surfaces onto the frame surfaces of a window, in Watts.
+
+\subsubsection{Surface Window Inside Reveal Reflected Diffuse Glazing Solar Radiation Rate {[}W{]}}\label{surface-window-inside-reveal-reflected-diffuse-glazing-solar-radiation-rate-w}
+
+Diffuse solar radiation reflected from inside reveal surfaces onto the glazing surfaces of a window, in Watts.
+
+\subsubsection{\texorpdfstring{Surface Window Inside Face Glazing Condensation Status {[]}}{Surface Window Inside Face Glazing Condensation Status }}\label{surface-window-inside-face-glazing-condensation-status}
+
+A value of 1 means that moisture condensation will occur on the innermost glass face of an exterior window (i.e., on the glass face in contact with the zone air). Otherwise the value is 0. The condition for condensation is glass inside face temperature \textless{} zone air dewpoint temperature.
+
+For airflow exterior windows, in which forced air passes between adjacent glass faces in double- and triple-pane windows, a value of 1 means that condensation will occur on one or both of the glass faces in contact with the airflow. In this case the condition for condensation is:
+
+\begin{itemize}
+\item
+  \emph{For airflow source = indoorair}, temperature of either face in contact with airflow \textless{} zone air dewpoint temperature.
+\item
+  \emph{For airflow source = outdoorair}, temperature of either face in contact with airflow \textless{} outside air dewpoint temperature.
+\end{itemize}
+
+As for regular windows, the value will also be 1 if condensation occurs on the innermost glass face.
+
+\subsubsection{\texorpdfstring{Surface Window Inside Face Frame Condensation Status {[]}}{Surface Window Inside Face Frame Condensation Status }}\label{surface-window-inside-face-frame-condensation-status}
+
+If an exterior window has a frame and the value of this flag is 1, condensation will occur on the inside surface of the frame. The condition for condensation is frame inside surface temperature \textless{} zone air dewpoint temperature.
+
+\subsubsection{\texorpdfstring{Surface Window Inside Face Divider Condensation Status {[]}}{Surface Window Inside Face Divider Condensation Status }}\label{surface-window-inside-face-divider-condensation-status}
+
+If an exterior window has a divider and the value of this flag is 1, condensation will occur on the inside surface of the divider. The condition for condensation is divider inside surface temperature \textless{} zone air dewpoint temperature.
+
+\subsubsection{\texorpdfstring{Surface Shading Device Is On Time Fraction {[]}}{Surface Shading Device Is On Time Fraction }}\label{surface-shading-device-is-on-time-fraction}
+
+The fraction of time that a shading device is on an exterior window. For a particular simulation timestep, the value is 0.0 if the shading device is off (or there is no shading device) and the value is 1.0 if the shading device is on. (It is assumed that the shading device, if present, is either on or off for the entire timestep.) If the shading device is switchable glazing, a value of 0.0 means that the glazing is in the unswitched (light colored) state, and a value of 1.0 means that the glazing is in the switched (dark colored) state.
+
+For a time interval longer a timestep, this is the fraction of the time interval that the shading device is on. For example, take the case where the time interval is one hour and the timestep is 10 minutes. Then if the shading device is on for two timesteps in the hour and off for the other four timesteps, then the fraction of time that the shading device is on = 2/6 = 0.3333.
+
+\subsubsection{Surface Window Blind Slat Angle {[}deg{]}}\label{surface-window-blind-slat-angle-deg}
+
+For an exterior window with a blind, this is the angle in degrees between the glazing outward normal and the blind slat angle outward normal, where the outward normal points away from the front face of the slat. The slat angle varies from 0 to 180 deg. If the slat angle is 0 deg or 180 deg, the slats are parallel to the glazing and the slats are said to be ``closed''. If the slat angle is 90 deg, the slats are perpendicular to the glazing and the slats are said to be ``fully open''. See illustrations under WindowMaterial:Blind. For blinds with a fixed slat angle, the value reported here will be constant.
+
+\subsubsection{\texorpdfstring{Surface Window Blind Beam to Beam Solar Transmittance {[]}}{Surface Window Blind Beam to Beam Solar Transmittance }}\label{surface-window-blind-beam-to-beam-solar-transmittance}
+
+For an exterior window with a blind, this is the fraction of exterior beam solar radiation incident on the blind that is transmitted through the blind as beam solar radiation when the blind is isolated (i.e., as though the window glass were not present). Depends on various factors, including slat angle, width, separation, and thickness, and horizontal solar profile angle (for blinds with horizontal slats) or vertical solar profile angle (for blinds with vertical slats). The transmittance value reported here will be non-zero only when some beam solar can pass through the blind without hitting the slats.
+
+\subsubsection{\texorpdfstring{Surface Window Blind Beam to Diffuse Solar Transmittance {[]}}{Surface Window Blind Beam to Diffuse Solar Transmittance }}\label{surface-window-blind-beam-to-diffuse-solar-transmittance}
+
+For an exterior window with a blind, the fraction of exterior beam solar radiation incident on the blind that is transmitted through the blind as diffuse solar radiation when the blind is isolated (i.e., as though the window glass were not present). Depends on various factors, including slat angle, width, separation, thickness and reflectance, and horizontal solar profile angle (for blinds with horizontal slats) or vertical solar profile angle (for blinds with vertical slats).
+
+\subsubsection{\texorpdfstring{Surface Window Blind Diffuse to Diffuse Solar Transmittance {[]}}{Surface Window Blind Diffuse to Diffuse Solar Transmittance }}\label{surface-window-blind-diffuse-to-diffuse-solar-transmittance}
+
+For an exterior window with a blind, the fraction of exterior diffuse solar radiation incident on the blind that is transmitted through the blind as diffuse solar radiation when the blind is isolated (i.e., as though the window glass were not present). Depends on various factors, including slat angle, width, separation, thickness and reflectance. For blinds with a fixed slat angle the transmittance value reported here will be constant.
+
+\subsubsection{\texorpdfstring{Surface Window Blind and Glazing System Beam Solar Transmittance {[]}}{Surface Window Blind and Glazing System Beam Solar Transmittance }}\label{surface-window-blind-and-glazing-system-beam-solar-transmittance}
+
+The fraction of exterior beam solar radiation incident on an exterior window with a blind (excluding window frame, if present) that is transmitted through the blind/glass system as beam solar radiation. Depends on various factors, including type of glass; solar incidence angle; slat angle, width, separation, and thickness; and horizontal solar profile angle (for blinds with horizontal slats) or vertical solar profile angle (for blinds with vertical slats).
+
+\subsubsection{\texorpdfstring{Surface Window Blind and Glazing System Diffuse Solar Transmittance {[]}}{Surface Window Blind and Glazing System Diffuse Solar Transmittance }}\label{surface-window-blind-and-glazing-system-diffuse-solar-transmittance}
+
+The fraction of exterior diffuse solar radiation incident on an exterior window with a blind (excluding window frame, if present) that is transmitted through the blind/glass system as diffuse solar radiation. Depends on various factors, including type of glass and slat angle, width, separation, thickness and reflectance. For blinds with a fixed slat angle the transmittance value reported here will be constant.
+
+\subsubsection{\texorpdfstring{Surface Window Screen Beam to Beam Solar Transmittance {[]}}{Surface Window Screen Beam to Beam Solar Transmittance }}\label{surface-window-screen-beam-to-beam-solar-transmittance}
+
+For an exterior window with a screen, this is the fraction of exterior beam solar radiation incident on the screen that is transmitted through the screen as beam solar radiation when the screen is isolated (i.e., as though the window glass were not present). Depends on various factors, including the screen reflectance and the relative angle of the incident beam with respect to the screen. This value will include the amount of inward reflection of solar beam off the screen material surface if the user specifies this modeling option (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method = Model as Direct Beam).
+
+\subsubsection{\texorpdfstring{Surface Window Screen Beam to Diffuse Solar Transmittance{[]}}{Surface Window Screen Beam to Diffuse Solar Transmittance}}\label{surface-window-screen-beam-to-diffuse-solar-transmittance}
+
+For an exterior window with a screen, the fraction of exterior beam solar radiation incident on the screen that is transmitted through the screen as diffuse solar radiation when the screen is isolated (i.e., as though the window glass were not present). Depends on various factors, including the screen reflectance and the relative angle of the incident beam with respect to the screen. This value is the amount of inward reflection of solar beam off the screen material surface if the user specifies this modeling option (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method = Model as Diffuse); otherwise, this value will be zero.
+
+\subsubsection{\texorpdfstring{Surface Window Screen Diffuse to Diffuse Solar Transmittance{[]}}{Surface Window Screen Diffuse to Diffuse Solar Transmittance}}\label{surface-window-screen-diffuse-to-diffuse-solar-transmittance}
+
+For an exterior window with a screen, the fraction of exterior diffuse solar radiation incident on the screen that is transmitted through the screen as diffuse solar radiation when the screen is isolated (i.e., as though the window glass were not present). Depends on various factors including screen material geometry and reflectance. This value is calculated as an average, constant For a window with a screen, this value consists of diffuse radiation transmitted through the screen (gaps between the screen material) and diffuse radiation from diffuse-to-diffuse reflection from the screen material. For a window with a screen, this value consists of diffuse radiation transmitted through the screen (gaps between the screen material) and diffuse radiation from diffuse-to-diffuse reflection from the screen material.
+
+\subsubsection{\texorpdfstring{Surface Window Screen and Glazing System Beam Solar Transmittance{[]}}{Surface Window Screen and Glazing System Beam Solar Transmittance}}\label{surface-window-screen-and-glazing-system-beam-solar-transmittance}
+
+The fraction of exterior beam solar radiation incident on an exterior window with a screen (excluding window frame, if present) that is transmitted through the screen/glass system as beam solar radiation. Depends on various factors, including the screen reflectance and the relative angle of the incident beam with respect to the screen. This value will include the amount of inward reflection of solar beam off the screen material surface if the user specifies this modeling option (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method = Model as Direct Beam).
+
+\subsubsection{\texorpdfstring{Surface Window Screen and Glazing System Diffuse Solar Transmittance {[]}}{Surface Window Screen and Glazing System Diffuse Solar Transmittance }}\label{surface-window-screen-and-glazing-system-diffuse-solar-transmittance}
+
+The fraction of exterior diffuse solar radiation incident on an exterior window with a screen (excluding window frame, if present) that is transmitted through the screen/glass system as diffuse solar radiation. Depends on various factors including screen material geometry and reflectance.
+
+\subsubsection{Surface Window Transmitted Beam Solar Radiation Rate {[}W{]}}\label{surface-window-transmitted-beam-solar-radiation-rate-w-1}
+
+\subsubsection{Surface Window Transmitted Beam Solar Radiation Energy {[}J{]}}\label{surface-window-transmitted-beam-solar-radiation-energy-j-1}
+
+The beam solar radiation transmitted through an interior window. Calculated only if Solar Distribution = FullInteriorAndExterior in your Building input. The origin of this radiation is beam solar that enters through an exterior window in a zone and then passes through an interior window into the adjacent zone. The amount of this radiation depends on several factors, including sun position, intensity of beam solar incident on the exterior window (including effects of shadowing, if present), relative position of the exterior and interior window, and the size and transmittance of the windows. Note that if there are two or more exterior windows in a zone, then beam solar from one or more of them may pass through the same interior window. Likewise, if there are more than two or more interior windows in a zone then beam solar from a single exterior window may pass through one or more of the interior windows. There are both rate and energy versions of the output.
+
+\subsubsection{\texorpdfstring{Surface Storm Window On Off Status {[]}}{Surface Storm Window On Off Status }}\label{surface-storm-window-on-off-status}
+
+Indicates whether a storm window glass layer is present (ref: StormWindow object). The value is \textbf{0} if the storm window glass layer is off, \textbf{1} if it is on, and \textbf{--1} if the window does not have an associated storm window. Applicable only to exterior windows and glass doors.
+
+\subsubsection{Surface Inside Face Initial Transmitted Diffuse Transmitted Out Window Solar Radiation Rate {[}W{]}}\label{surface-inside-face-initial-transmitted-diffuse-transmitted-out-window-solar-radiation-rate-w}
+
+As of Version 2.1, the diffuse solar transmitted through exterior windows that is initially distributed to another window in the zone and transmitted out of the zone through that window. For exterior windows, this transmitted diffuse solar is ``lost'' to the exterior environment For interior windows, this transmitted diffuse solar is distributed to heat transfer surfaces in the adjacent zone, and is part of the Surface Inside Face Initial Transmitted Diffuse Absorbed Solar Radiation Rate for these adjacent zone surfaces.
+
+\subsubsection{Additional Window Outputs (Advanced)}\label{additional-window-outputs-advanced}
+
+The following output variables for windows or glass doors are available when the user requests to display advanced output variables. These seven reports show the individual components that are combined to determine overall Surface Window Heat Gain Rate and/or Surface Window Heat Loss Rate (described above).
+
+\subsubsection{Surface Window Inside Face Glazing Zone Convection Heat Gain Rate {[}W{]}}\label{surface-window-inside-face-glazing-zone-convection-heat-gain-rate-w}
+
+The surface convection heat transfer from the glazing to the zone in watts. This output variable is the term called ``{[}Convective heat flow to the zone from the zone side of the glazing{]}'' under the description above for Surface Window Heat Gain Rate output variable. If the window has an interior shade or blind, then this is zero and the glazing's convection is included in the report called ``Surface Window Inside Face Gap between Shade and Glazing Zone Convection Heat Gain Rate''.
+
+\subsubsection{Surface Window Inside Face Glazing Net Infrared Heat Transfer Rate {[}W{]}}\label{surface-window-inside-face-glazing-net-infrared-heat-transfer-rate-w}
+
+The net exchange of infrared radiation heat transfer from the glazing to the zone in watts. This output variable is the term called ``{[}Net IR heat flow to the zone from zone side of the glazing{]}'' under the description above for Surface Window Heat Gain Rate output variable.
+
+\subsubsection{Surface Window Shortwave from Zone Back Out Window Heat Transfer Rate {[}W{]}}\label{surface-window-shortwave-from-zone-back-out-window-heat-transfer-rate-w}
+
+This is the short-wave radiation heat transfer from the zone back out the window in watts. This is a measure of the diffuse short-wave light (from reflected solar and electric lighting) that leave the zone through the window. This output variable is the term called ``{[}Short-wave radiation from zone transmitted back out the window{]}'' under the description above for Surface Window Heat Gain Rate output variable.
+
+\subsubsection{Surface Window Inside Face Frame and Divider Zone Heat Gain Rate {[}W{]}}\label{surface-window-inside-face-frame-and-divider-zone-heat-gain-rate-w}
+
+This is the heat transfer from any frames and/or dividers to the zone in watts. This output variable is the term called ``{[}Conduction to zone from window frame and divider, if present{]}'' under the description above for Surface Window Heat Gain Rate output variable. (The word ``conduction'' here is used because the models is simplified compared to the complexities of surface convection and radiation.)
+
+\subsubsection{Surface Window Frame Heat Gain Rate {[}W{]}}\label{surface-window-frame-heat-gain-rate-w}
+
+This is the positive heat flow from window frames to the zone in watts. This is part of the Surface Window Inside Face Frame and Divider Zone Heat Gain Rate.
+
+\subsubsection{Surface Window Frame Heat Loss Rate {[}W{]}}\label{surface-window-frame-heat-loss-rate-w}
+
+This is the negative heat flow from window frames to the zone in watts. This is part of the Surface Window Inside Face Frame and Divider Zone Heat Gain Rate.
+
+\subsubsection{Surface Window Frame Inside Temperature {[}C{]}}\label{surface-window-frame-inside-temperature-c}
+
+This is the temperature of the inside surface of the window frames.
+
+\subsubsection{Surface Window Frame Outside Temperature {[}C{]}}\label{surface-window-frame-outside-temperature-c}
+
+This is the temperature of the outside surface of the window frames.
+
+\subsubsection{Surface Window Divider Heat Gain Rate {[}W{]}}\label{surface-window-divider-heat-gain-rate-w}
+
+This is the positive heat flow from window dividers to the zone in watts. This is part of the Surface Window Inside Face Frame and Divider Zone Heat Gain Rate.
+
+\subsubsection{Surface Window Divider Heat Loss Rate {[}W{]}}\label{surface-window-divider-heat-loss-rate-w}
+
+This is the negative heat flow from window dividers to the zone in watts. This is part of the Surface Window Inside Face Frame and Divider Zone Heat Gain Rate.
+
+\subsubsection{Surface Window Divider Inside Temperature {[}C{]}}\label{surface-window-divider-inside-temperature-c}
+
+This is the temperature of the inside surface of the window dividers.
+
+\subsubsection{Surface Window Divider Outside Temperature {[}C{]}}\label{surface-window-divider-outside-temperature-c}
+
+This is the temperature of the outside surface of the window dividers.
+
+\subsubsection{Surface Window Inside Face Gap between Shade and Glazing Zone Convection Heat Gain Rate {[}W{]}}\label{surface-window-inside-face-gap-between-shade-and-glazing-zone-convection-heat-gain-rate-w}
+
+This is the convection surface heat transfer from the both the glazing and the shade's back face to the zone in Watts. This output variable is the term called ``{[}Convective heat flow to the zone from the air flowing through the gap between glazing and shading device{]}'' under the description above for Surface Window Heat Gain Rate output variable. For Equivalent Layer window this output variable is the convection heat gain from vented interior air gap to the zone in Watts.
+
+\subsubsection{Surface Window Inside Face Shade Zone Convection Heat Gain Rate {[}W{]}}\label{surface-window-inside-face-shade-zone-convection-heat-gain-rate-w}
+
+This is the convection surface heat transfer from the front side of any interior shade or blind to the zone in Watts. This output variable is the term called ``{[}Convective heat flow to the zone from the zone side of the shading device{]}'' under the description above for Surface Window Heat Gain Rate output variable. For equivalent Layer window this output variable is the convection heat gain rate from the inside face of a glazing or a shade to the zone in Watts.
+
+\subsubsection{Surface Window Inside Face Shade Net Infrared Heat Transfer Rate {[}W{]}}\label{surface-window-inside-face-shade-net-infrared-heat-transfer-rate-w}
+
+The net exchange of infrared radiation heat transfer from the shade or blind to the zone in watts. This output variable is the term called ``{[}Net IR heat flow to the zone from the zone side of the shading device{]}'' under the description above for Surface Window Heat Gain Rate output variable.
+
+\subsubsection{Surface Window Inside Face Other Convection Heat Gain Rate {[}W{]}}\label{surface-window-inside-face-other-convection-heat-gain-rate-w}
+
+The other (extra) convection heat transfer rate from the inside face of a an equivalent layer window. This output is computed from the difference in convection flux when using equivalent inside surface temperature of a window instead of the inside surface temperature from the standard surface heat balance calculation.
+
+\subsection{Thermochomic Window Outputs}\label{thermochomic-window-outputs}
+
+\subsubsection{Window Thermochromic Layer Temperature {[}C{]}}\label{window-thermochromic-layer-temperature-c}
+
+The temperature of the TC glass layer of a TC window at each time step.
+
+\subsubsection{Surface Window Thermochromic Layer Property Specification Temperature {[}C{]}}\label{surface-window-thermochromic-layer-property-specification-temperature-c-000}
+
+The temperature under which the optical data of the TC glass layer are specified.
+
+The overall properties (U-factor/SHGC/VT) of the thermochromic windows at different specification temperatures are reported in the \textbf{.eio} file. These window constructions are created by EnergyPlus during run time. They have similar names with suffix ``\_TC\_XX'' where XX represents a specification temperature.
+
+\subsubsection{Switchable Window Outputs}\label{switchable-window-outputs}
+
+\subsubsection{\texorpdfstring{Surface Window Switchable Glazing Switching Factor{[]}}{Surface Window Switchable Glazing Switching Factor}}\label{surface-window-switchable-glazing-switching-factor}
+
+The switching factor (tint level) of the switchable window: 0 means no switching -- clear state; 1 means fully switched -- dark state.
+
+\subsubsection{\texorpdfstring{Surface Window Switchable Glazing Visible Transmittance{[]}}{Surface Window Switchable Glazing Visible Transmittance}}\label{surface-window-switchable-glazing-visible-transmittance}
+
+The visible transmittance of the switchable window.
+
+\subsection{Other Surface Outputs/Reports}\label{other-surface-outputsreports}
+
+Several reports can be selected for Surfaces. (See Group -- Report for details on how to specify). Examples are:
+
+\subsubsection{DXF}\label{dxf}
+
+This report produces a special file (\textbf{eplusout.dxf}) in the industry standard DXF (Drawing Interchange Format) for drawings. It is produced and accepted by many popular, commercial CAD programs. Detailed reference can be found on the AutoCADâ„¢ website at: http://www.autodesk.com/techpubs/autocad/acadr14/dxf/index.htm
+
+EnergyPlus produces this file from the Report command:
+
+\begin{lstlisting}
+
+Output:Reports, Surfaces, DXF;
+\end{lstlisting}
+
+\subsubsection{Details, Vertices, DetailsWithVertices}\label{details-vertices-detailswithvertices}
+
+This version of the report creates lines in the eplusout.eio file for each surface (except internal mass surfaces). Details of this reporting is shown in the Output Details and Examples document.
+
+\subsection{Shading Surfaces}\label{shading-surfaces}
+
+Shading surfaces are entities outside of the building that may cast shadows on the building's heat transfer surfaces. These entities do not typically have enough thermal mass to be described as part of the building's thermal makeup.
+
+The most important effect of shading surfaces is to reduce solar gain in windows that are shadowed. (However, in some cases, shading surfaces can reflect solar onto a wall or window and increase solar gain.)
+
+There are two kinds of shading surfaces in EnergyPlus: \textbf{detached} and \textbf{attached}. A \textbf{detached} shading surface, such as a tree or neighboring building, is not connected to the building. An \textbf{attached} shading surface is typically an overhang or fin that is attached to a particular base surface of the building, usually a wall; attached shading surfaces are usually designed to shade specific windows.
+
+Objects for detached shading surfaces:
+
+\begin{itemize}
+\item
+  Shading:Site
+\item
+  Shading:Building
+\item
+  Shading:Site:Detailed
+\item
+  Shading:Building:Detailed
+\end{itemize}
+
+Similarly to the surfaces, the detailed objects use vertex entry whereas the other objects are limited to rectangular representation.
+
+Objects for attached shading surfaces:
+
+\begin{itemize}
+\item
+  Shading:Overhang
+\item
+  Shading:Overhang:Projection
+\item
+  Shading:Fin
+\item
+  Shading:Fin:Projection
+\item
+  Shading:Zone:Detailed
+\end{itemize}
+
+EnergyPlus creates ``bi-directional'' shades from each shading surface entered. This means that the shade you input will cast a shadow no matter which side of the shade the sun is on. For example, a vertical fin will cast a shadow whether the sun is on the left side or right side of the fin. Prior to V1.0.2, a shading surface cast a shadow only in the hemisphere toward which the surface faced. This hemisphere is the one pointed to by the shading surface's outward normal vector, which is the cross product V23 x V21, where V23 is the vector from vertex 2 to vertex 3 of the shading surface and V21 is the vector from vertex 2 to vertex 1. Beginning with V1.0.2, the shades in EnergyPlus are ``bi-directional'' so that they can cast shadows in both hemispheres depending on the time-varying position of the sun relative to the shading surface.
+
+It is important to note that EnergyPlus will automatically account for ``self-shading'' effects---such as in L-shaped buildings---in which some of the building's wall and roof surfaces shade other parts of the building, especially windows. This means that you only need to describe shading elements that aren't building heat-transfer surfaces.
+
+Shading surfaces can also \textbf{reflect} solar radiation onto the building. This feature is simulated if you choose FullExteriorWithReflections or FullInteriorAndExteriorWithReflections in the Building object (ref: Building - Field: Solar Distribution). In this case, you may specify the reflectance properties of a shading surface with the ShadingProperty:Reflectance object. Note: If no ShadingProperty:Reflectance object is defined, then the shading surface reflectance values are assumed to be 0.2 and the fraction of shading surface that is glazed is assumed to be 0.0.
+
+Shading surfaces also automatically shade diffuse solar radiation (and long-wave radiation) from the sky. And they will automically shade diffuse solar radiation from the ground if Solar Distribution Field = FullExteriorWithReflections or FullInteriorAndExteriorWithReflections in the Building object. (If the reflections option for Solar Distribution is used, the program also takes into account the reduction of solar radiation reflected from the ground due to shading of the ground by shading surfaces and by the building itself.) Otherwise, shading surfaces will not shade diffuse radiation from the ground unless you enter a reduced value for View Factor to Ground for those building surfaces that are shaded (ref: BuildingSurface:Detailed - Field: View Factor to Ground and FenestrationSurface:Detailed - Field: View Factor to Ground).
+
+\subsection{Detached Shading Surfaces}\label{detached-shading-surfaces}
+
+\subsection{Shading:Site, Shading:Building}\label{shadingsite-shadingbuilding}
+
+These objects are used to describe rectangular shading elements that are external to the building. Examples are trees, high fences, near-by hills, and neighboring buildings.
+
+If relative coordinates are used (ref: Field: Coordinate System in GlobalGeometryRules), shading surfaces entered with Shading:Site remain stationary if the building is rotated, whereas those entered with Shading:Building rotate with the building. If world coordinates are used Shading:Site and Shading:Building are equivalent.
+
+These shading elements are always opaque.
+
+\subsubsection{Field: Name}\label{field-name-22-004}
+
+This is a unique character string associated with the detached shading surface. Though it must be unique from other surface names, it is used primarily for convenience with detached shading surfaces.
+
+\subsubsection{Field: Azimuth Angle}\label{field-azimuth-angle-10}
+
+Theoretically, this should face to the surface it is shading (i.e.~if a south wall, this should be a north facing shade) but since EnergyPlus automatically generates the mirror image, the facing angle per se' is not so important.
+
+\subsubsection{Field: Tilt Angle}\label{field-tilt-angle-10}
+
+The tilt angle is the angle (in degrees) that the shade is tilted from horizontal (or the ground). Default for this field is 90 degrees.
+
+\subsubsection{Starting Corner for the surface}\label{starting-corner-for-the-surface-16}
+
+The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. See the introductory paragraph for rules on this entry.
+
+\subsubsection{Field: Starting X Coordinate}\label{field-starting-x-coordinate-16}
+
+This field is the X coordinate (in meters).
+
+\subsubsection{Field: Starting Y Coordinate}\label{field-starting-y-coordinate-10}
+
+This field is the Y coordinate (in meters).
+
+\subsubsection{Field: Starting Z Coordinate}\label{field-starting-z-coordinate-16}
+
+This field is the Z coordinate (in meters).
+
+\subsubsection{Field: Length}\label{field-length-16}
+
+This field is the length of the shade in meters.
+
+\subsubsection{Field: Height}\label{field-height-10}
+
+This field is the width of the shade in meters.
+
+Examples of these (can be found in example files 4ZoneWithShading\_Simple\_1.idf and 4ZoneWithShading\_Simple\_2.idf)
+
+\begin{lstlisting}
+
+  Shading:Building,
+      Bushes-East,             !- Name
+      90,                      !- Azimuth Angle {deg}
+      90,                      !- Tilt Angle {deg}
+      45,                      !- Starting X Coordinate {m}
+      0,                       !- Starting Y Coordinate {m}
+      0,                       !- Starting Z Coordinate {m}
+      50,                      !- Length {m}
+      1;                       !- Height {m}
+
+    Shading:Site,
+      Bushes-North,            !- Name
+      0,                       !- Azimuth Angle {deg}
+      90,                      !- Tilt Angle {deg}
+      45,                      !- Starting X Coordinate {m}
+      50,                      !- Starting Y Coordinate {m}
+      0,                       !- Starting Z Coordinate {m}
+      50,                      !- Length {m}
+      1;                       !- Height {m}
+\end{lstlisting}
+
+\subsection{Shading:Site:Detailed, Shading:Building:Detailed}\label{shadingsitedetailed-shadingbuildingdetailed}
+
+These objects are used to describe shading elements that are external to the building. Examples are trees, high fences, near-by hills, and neighboring buildings.
+
+If relative coordinates are used (ref: Field: Coordinate System in GlobalGeometryRules), shading surfaces entered with Shading:Site:Detailed remain stationary if the building is rotated, whereas those entered with Shading:Building:Detailed rotate with the building. If world coordinates are used Shading:Site:Detailed and Shading:Building:Detailed are equivalent.
+
+While ``detached'' implies that shading surfaces are not part of the building, the detached shading sequence can be used to describe attached shading surfaces that may shade heat transfer surfaces in more than one zone. For example, wing A of a building might shade several zones of wing B but wing A (for whatever reason) is not described in the geometry for the simulation so it is represented by a detached shade to get its shadowing effect.
+
+\subsubsection{Field: Name}\label{field-name-23-004}
+
+This is a unique character string associated with the detached shading surface. Though it must be unique from other surface names, it is used primarily for convenience with detached shading surfaces.
+
+\subsubsection{Field: Transmittance Schedule Name}\label{field-transmittance-schedule-name}
+
+The name of a schedule of solar transmittance values from 0.0 to 1.0 for the shading surface. If a blank is entered in this field, the transmittance value defaults to 0.0, i.e., the shading surface is opaque at all times. This scheduling can be used to allow for seasonal transmittance change, such as for deciduous trees that have a higher transmittance in winter than in summer. Transmittance based on time of day can also be used---a movable awning, for example, where the transmittance is some value less than 1.0 when the awning is in place and is 1.0 when the awning is retracted.
+
+The following assumptions are made in the shading surface transmittance calculation:
+
+\begin{itemize}
+\item
+  Both sides of the shading surface have the same transmittance properties.
+\item
+  The transmittance is the same for both beam and diffuse solar radiation.
+\item
+  Beam solar transmittance is independent of angle of incidence on the shading surface.
+\item
+  Beam radiation incident on a shading surface is transmitted as beam radiation with no change in direction, i.e., there is no beam-to-diffuse component.
+\item
+  If two shading surfaces with non-zero transmittance overlap, the net transmittance is the product of the individual transmittances. Inter-reflection between the shading surfaces (and between the shading surfaces and the building) is ignored.
+\item
+  For the daylighting calculation (ref: Group -- Daylighting) the shading surface's visible transmittance is assumed to be the same as its solar transmittance.
+\item
+  Shading devices are assumed to be opaque to long-wave radiation no matter what the solar transmittance value is.
+\end{itemize}
+
+Note that shading devices only shade solar radiation when the sun is up, which is automatically determined by EnergyPlus from latitude, time of year, etc. The user need only account for the time-varying transmittance of the shading device in the transmittance schedule, not whether the sun is up or not.
+
+\subsubsection{Field: Number Vertices}\label{field-number-vertices}
+
+The number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on ``Surface Vertices'' above.
+
+IDF example of Detached Shading Surfaces:
+
+\begin{lstlisting}
+
+Shading:Building:Detailed,
+     EAST SIDE TREE,  !- Detached Shading
+     ShadingTransmittance:0002,  !- Shadowing Transmittance & Schedule
+     3, !-Triangle
+     33.52800    ,   10.66800    ,   10.05800    ,
+     33.52800    ,   13.71600    ,  0.9140000    ,
+     33.52800    ,   4.572000    ,  0.9140000    ;
+
+  Shading:Building:Detailed,
+     WEST SIDE TREE,  !- Detached Shading
+     ShadingTransmittance:0002,  !- Shadowing Transmittance & Schedule
+     3, !-Triangle
+    -3.048000    ,   7.620000    ,   10.05800    ,
+    -3.048000    ,   4.572000    ,  0.9140000    ,
+    -3.048000    ,   13.71600    ,  0.9140000    ;
+\end{lstlisting}
+
+\subsection{Attached Shading Surfaces}\label{attached-shading-surfaces}
+
+Overhangs are usually horizontal devices that are used to shade windows. Fins are usually vertical devices that similarly shade windows.
+
+\subsection{Shading:Overhang}\label{shadingoverhang}
+
+An overhang typically is used to shade a window in a building.
+
+\subsubsection{Inputs}\label{inputs-26-003}
+
+\paragraph{Field: Name}\label{field-name-24-003}
+
+This is the name of the overhang. It must be different from other surface names.
+
+\paragraph{Field: Window or Door Name}\label{field-window-or-door-name}
+
+The name of a window or door that this overhang shades.
+
+\paragraph{Field: Height above Window or Door}\label{field-height-above-window-or-door}
+
+This field is the height (meters) above the top of the door for the overhang.
+
+\paragraph{Field Tilt Angle from Window/Door}\label{field-tilt-angle-from-windowdoor}
+
+This field is the tilt angle from the Window/Door. For a flat overhang, this would be 90 (degrees).
+
+\paragraph{Field: Left Extension from Window/Door Width}\label{field-left-extension-from-windowdoor-width}
+
+This field is the width from the left edge of the window/door to the start of the overhang (meters).
+
+\paragraph{Field: Right Extension from Window/Door Width}\label{field-right-extension-from-windowdoor-width}
+
+This field is the width from the right edge of the window/door to the start of the overhang (meters).
+
+\paragraph{Field: Depth}\label{field-depth}
+
+This field is the depth of the overhang (meters) projecting out from the wall.
+
+\subsection{Shading:Overhang:Projection}\label{shadingoverhangprojection}
+
+An overhang typically is used to shade a window in a building. This object allows for specifying the depth of the overhang as a fraction of the window or door's height.
+
+\subsubsection{Inputs}\label{inputs-27-003}
+
+\paragraph{Field: Name}\label{field-name-25-003}
+
+This is the name of the overhang. It must be different from other surface names.
+
+\paragraph{Field: Window or Door Name}\label{field-window-or-door-name-1}
+
+The name of a window or door that this overhang shades.
+
+\paragraph{Field: Height above Window or Door}\label{field-height-above-window-or-door-1}
+
+This field is the height (meters) above the top of the door for the overhang.
+
+\paragraph{Field Tilt Angle from Window/Door}\label{field-tilt-angle-from-windowdoor-1}
+
+This field is the tilt angle from the Window/Door. For a flat overhang, this would be 90 (degrees).
+
+\paragraph{Field: Left Extension from Window/Door Width}\label{field-left-extension-from-windowdoor-width-1}
+
+This field is the width from the left edge of the window/door to the start of the overhang (meters).
+
+\paragraph{Field: Right Extension from Window/Door Width}\label{field-right-extension-from-windowdoor-width-1}
+
+This field is the width from the right edge of the window/door to the start of the overhang (meters).
+
+\paragraph{Field: Depth as Fraction of Window/Door Height}\label{field-depth-as-fraction-of-windowdoor-height}
+
+This field is the fraction of the window/door height to specify as the depth of the overhang (meters) projecting out from the wall.
+
+\subsection{Shading:Fin}\label{shadingfin}
+
+Fins shade either side of windows/doors in a building. This object allows for specification of both fins for the window. Fin placement is relative to the edge of the glass and user must include the frame width when a frame is present.
+
+\subsubsection{Inputs}\label{inputs-28-002}
+
+\paragraph{Field: Name}\label{field-name-26-003}
+
+This is the name of the overhang. It must be different from other surface names.
+
+\paragraph{Field: Window or Door Name}\label{field-window-or-door-name-2}
+
+The name of a window or door that this overhang shades.
+
+\paragraph{Field: Left Fin Extension from Window/Door}\label{field-left-fin-extension-from-windowdoor}
+
+This field is the width from the left edge of the window/door to the plane of the left fin (meters). The extension width is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Left Fin Distance Above Top of Window}\label{field-left-fin-distance-above-top-of-window}
+
+This field is the distance from the top of the window to the top of the left fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Left Fin Distance Below Bottom of Window}\label{field-left-fin-distance-below-bottom-of-window}
+
+This field is the distance from the bottom of the window to the bottom of the left fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Left Fin Tilt Angle from Window/Door}\label{field-left-fin-tilt-angle-from-windowdoor}
+
+This field is the tilt angle from the window / door for the left fin. Typically, a fin is 90 degrees (default) from its associated window/door.
+
+\paragraph{Field: Left Fin Depth}\label{field-left-fin-depth}
+
+This field is the depth (meters) of the left fin (projecting out from the wall).
+
+\paragraph{Field: Right Fin Extension from Window/Door}\label{field-right-fin-extension-from-windowdoor}
+
+This field is the width from the right edge of the window/door to the plane of the right fin (meters). The extension width is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Right Fin Distance Above Top of Window}\label{field-right-fin-distance-above-top-of-window}
+
+This field is the distance from the top of the window to the top of the right fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Right Fin Distance Below Bottom of Window}\label{field-right-fin-distance-below-bottom-of-window}
+
+This field is the distance from the bottom of the window to the bottom of the right fin (meters) and is relative to the edge of the glass and includes the frame width.
+
+\paragraph{Field: Right Fin Tilt Angle from Window/Door}\label{field-right-fin-tilt-angle-from-windowdoor}
+
+This field is the tilt angle from the window / door for the right fin. Typically, a fin is 90 degrees (default) from its associated window/door.
+
+\paragraph{Field: Right Fin Depth}\label{field-right-fin-depth}
+
+This field is the depth (meters) of the right fin (projecting out from the wall).
+
+\subsection{Shading:Fin:Projection}\label{shadingfinprojection}
+
+Fins shade either side of windows/doors in a building. This object allows for specification of both fins for the window. This object allows for specifying the depth of the overhang as a fraction of the window or door's width. Fin placement is relative to the edge of the glass and user must include the frame width when a frame is present.
+
+\subsubsection{Inputs}\label{inputs-29-002}
+
+\paragraph{Field: Name}\label{field-name-27-003}
+
+This is the name of the overhang. It must be different from other surface names.
+
+\paragraph{Field: Window or Door Name}\label{field-window-or-door-name-3}
+
+The name of a window or door that this overhang shades.
+
+\paragraph{Field: Left Fin Extension from Window/Door}\label{field-left-fin-extension-from-windowdoor-1}
+
+This field is the width from the left edge of the window/door to the plane of the left fin (meters). The extension width is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Left Fin Distance Above Top of Window}\label{field-left-fin-distance-above-top-of-window-1}
+
+This field is the distance from the top of the window to the top of the left fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Left Fin Distance Below Bottom of Window}\label{field-left-fin-distance-below-bottom-of-window-1}
+
+This field is the distance from the bottom of the window to the bottom of the left fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Left Fin Tilt Angle from Window/Door}\label{field-left-fin-tilt-angle-from-windowdoor-1}
+
+This field is the tilt angle from the window / door for the left fin. Typically, a fin is 90 degrees (default) from its associated window/door.
+
+\paragraph{Field: Left Fin Depth as Fraction of Window/Door Width}\label{field-left-fin-depth-as-fraction-of-windowdoor-width}
+
+This field is the fraction of the window/door width to specify as the depth of the left fin (meters) projecting out from the wall.
+
+\paragraph{Field: Right Fin Extension from Window/Door}\label{field-right-fin-extension-from-windowdoor-1}
+
+This field is the width from the right edge of the window/door to the plane of the right fin (meters).. The extension width is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Right Fin Distance Above Top of Window}\label{field-right-fin-distance-above-top-of-window-1}
+
+This field is the distance from the top of the window to the top of the right fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Right Fin Distance Below Bottom of Window}\label{field-right-fin-distance-below-bottom-of-window-1}
+
+This field is the distance from the bottom of the window to the bottom of the right fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
+
+\paragraph{Field: Right Fin Tilt Angle from Window/Door}\label{field-right-fin-tilt-angle-from-windowdoor-1}
+
+This field is the tilt angle from the window / door for the right fin. Typically, a fin is 90 degrees (default) from its associated window/door.
+
+\paragraph{Field: Right Fin Depth as Fraction of Window/Door Width}\label{field-right-fin-depth-as-fraction-of-windowdoor-width}
+
+This field is the fraction of the window/door width to specify as the depth of the right fin (meters) projecting out from the wall.
+
+zone.
+
+Examples of these (can be found in example files 4ZoneWithShading\_Simple\_1.idf and 4ZoneWithShading\_Simple\_2.idf)
+
+\begin{lstlisting}
+
+  Shading:Overhang:Projection,
+      Zn001:Wall001:Win001:Shade001,  !- Name
+      Zn001:Wall001:Win001,    !- Window or Door Name
+      .7,                      !- Height above Window or Door {m}
+      90,                      !- Tilt Angle from Window/Door {deg}
+      .2,                      !- Left extension from Window/Door Width {m}
+      .2,                      !- Right extension from Window/Door Width {m}
+      .6;                      !- Depth as Fraction of Window/Door Height {m}
+
+    Shading:Overhang,
+      Zn001:Wall001:Door001:Shade001,  !- Name
+      Zn001:Wall001:Door001,   !- Window or Door Name
+      .6,                      !- Height above Window or Door {m}
+      90,                      !- Tilt Angle from Window/Door {deg}
+      0,                       !- Left extension from Window/Door Width {m}
+      0,                       !- Right extension from Window/Door Width {m}
+      3;                       !- Depth {m}
+
+    Shading:Fin:Projection,
+      Zn001:Wall001:Shade003,  !- Name
+      Zn001:Wall001:Win001,    !- Window or Door Name
+      .1,                      !- Left Extension from Window/Door {m}
+      .1,                   !- Left Distance Above Top of Window {m}
+      .1,                   !- Left Distance Below Bottom of Window {m}
+      90,                   !- Left Tilt Angle from Window/Door {deg}
+      .6,                   !- Left Depth as Fraction of Window/Door Width {m}
+      .1,                   !- Right Extension from Window/Door {m}
+      .1,                   !- Right Distance Above Top of Window {m}
+      .1,                   !- Right Distance Below Bottom of Window {m}
+      90,                   !- Right Tilt Angle from Window/Door {deg}
+      .6;                   !- Right Depth as Fraction of Window/Door Width {m}
+\end{lstlisting}
+
+\subsection{Shading:Zone:Detailed}\label{shadingzonedetailed-000}
+
+This object is used to describe attached ``subsurfaces'' such as overhangs, wings or fins that project outward from a base surface. This classification is used for convenience; actually, a device of this type can cast shadows on the surface to which it is attached as well as on adjacent surfaces. For example, a fin may shade its parent wall as well as adjacent walls.
+
+Note that a zone surface can cast shadows on other zone surfaces. However, you don't have to worry about such effects---for example, one wall of an L-shaped building shading another wall--because EnergyPlus will automatically check for this kind of ``self shadowing'' and do the proper calculations.
+
+Unlike attached (or detached) shading surfaces, building surfaces can only cast shadows in the hemisphere towards which they face. This means, for example, that a roof that faces \emph{upward} will not cast a shadow \emph{downward}. (Thus, specifying an oversized roof in an attempt to account for the shading effects of overhangs will \emph{not} work). Interior surfaces do not cast shadows of any kind.
+
+\subsubsection{Inputs}\label{inputs-30-002}
+
+\paragraph{Field: Name}\label{field-name-28-002}
+
+This is the name of the attached shading surface. It must be different from other surface names.
+
+\paragraph{Field: Base Surface Name}\label{field-base-surface-name}
+
+This is the name of the surface to which this shading device is attached. This surface can be a wall (or roof) but not a window or door.
+
+\paragraph{Field: Transmittance Schedule Name}\label{field-transmittance-schedule-name-1}
+
+The name of a schedule of solar transmittance values from 0.0 to 1.0 for the shading surface. If a blank is entered in this field, the transmittance value defaults to 0.0, i.e., the shading surface is opaque at all times. This scheduling can be used to allow for seasonal transmittance change, such as for deciduous trees that have a higher transmittance in winter than in summer. Transmittance based on time of day can also be used---a movable awning, for example, where the transmittance is some value less than 1.0 when the awning is in place and is 1.0 when the awning is retracted.
+
+The following assumptions are made in the shading surface transmittance calculation:
+
+\begin{itemize}
+\item
+  Both sides of the shading surface have the same transmittance properties.
+\item
+  The transmittance is the same for both beam and diffuse solar radiation.
+\item
+  Beam solar transmittance is independent of angle of incidence on the shading surface.
+\item
+  Beam radiation incident on a shading surface is transmitted as beam radiation with no change in direction, i.e., there is no beam-to-diffuse component.
+\item
+  If two shading surfaces with non-zero transmittance overlap, the net transmittance is the product of the individual transmittances. Inter-reflection between the shading surfaces (and between the shading surfaces and the building) is ignored.
+\item
+  For the daylighting calculation (ref: Group -- Daylighting) the shading surface's visible transmittance is assumed to be the same as its solar transmittance.
+\item
+  Shading devices are assumed to be opaque to long-wave radiation no matter what the solar transmittance value is.
+\end{itemize}
+
+Note that shading devices only shade solar radiation when the sun is up, which is automatically determined by EnergyPlus from latitude, time of year, etc. The user need only account for the time-varying transmittance of the shading device in the transmittance schedule, not whether the sun is up or not.
+
+\paragraph{Field: Number Vertices}\label{field-number-vertices-1}
+
+The number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on ``Surface Vertices'' above. The example below shows the correct input for an overhang (to shade the appropriate portion of the base wall and window).
+
+\begin{figure}[hbtp] % fig 33
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image059.png}
+\caption{Illustration for Attached Shading Surface \protect \label{fig:illustration-for-attached-shading-surface}}
+\end{figure}
+
+Proper specification for this overhang (facing up) is:
+
+4,(C,0,D),(C,-B,D),(C+A,-B,D),(C+A,0,D); () used to illustrate each vertex.
+
+\begin{callout}
+Note that for horizontal surfaces, any corner may be chosen as the starting corner. The order of vertices determines whether the surface is facing up or down. Shading surfaces are mirrored automatically unless the user specifies ``DoNotMirrorDetachedShading'', so each shading surface need only be described once.
+\end{callout}
+
+Thus, another shading surface will be created (facing down):
+
+4,(C+A,-B,D),(C+A,0,D),(C,0,D),(C,-B,D);
+
+IDF example of attached shading surfaces (overhang, fin):
+
+\begin{lstlisting}
+Shading:Zone:Detailed,
+  Zn001:Wall001:Shade001,       !- Surface Name
+  Zn001:Wall001,                !- Base Surface Name
+  ShadingTransmittance:0001,    !- Shadowing Transmittance Schedule
+  4,                            !-RectangularOverhang
+  1.524000 , -0.3050000    , 2.865000,
+  1.524000 ,  0.0000000E+00, 2.865000,
+  4.572000 ,  0.0000000E+00, 2.865000,
+  4.572000 , -0.3050000    , 2.865000;
+
+Shading:Zone:Detailed,
+  Zn003:Wall001:Shade001,       !- Surface Name
+  Zn003:Wall001,                !- Base Surface Name
+  ShadingTransmittance:0001,    !- Shadowing Transmittance Schedule
+  4,                            !-RectangularLeftFin
+  57.97000 ,   8.450000    ,10.00000      ,
+  57.97000 ,   8.450000    , 0.0000000E+00,
+  57.97000 ,   6.450000    , 0.0000000E+00,
+  57.97000 ,   6.450000    ,10.00000      ;
+
+Shading:Zone:Detailed,
+  Zn003:Wall001:Shade002,       !- Surface Name
+  Zn003:Wall001,                !- Base Surface Name
+  ShadingTransmittance:0003,    !- Shadowing Transmittance Schedule
+  4,                            !-RectangularRightFin
+  77.97000 ,   6.450000    ,10.00000      ,
+  77.97000 ,   6.450000    , 0.0000000E+00,
+  77.97000 ,   8.450000    , 0.0000000E+00,
+  77.97000 ,   8.450000    ,10.00000      ;
+\end{lstlisting}
+
+\subsection{ShadingProperty:Reflectance}\label{shadingpropertyreflectance}
+
+Specifies the reflectance properties of a shading surface when the solar reflection calculation has requested, i.e., when if ``WithReflections'' option is chosen in the Building object (ref: Building - Field: Solar Distribution). It is assumed that shading surfaces are divided into an unglazed, diffusely reflecting portion and a glazed, specularly-reflecting portion, either of which may be zero. The reflectance properties are assumed to be the same on both sides of the shading surface.
+
+Note that a shadowing transmittance schedule (ref: Shading Surfaces, Field: Transmittance Schedule Name) can be used with a reflective shading surface. However, EnergyPlus assumes that the reflectance properties of the shading surface are constant even if the transmittance varies.
+
+If no ShadingProperty:Reflectance objects are entered, the default values shown here will be used for shading surfaces. Other surfaces have their reflectance properties defined by the materials in the outer layers of the constructions.
+
+\subsubsection{Inputs}\label{inputs-31-002}
+
+\paragraph{Field: Shading Surface Name}\label{field-shading-surface-name}
+
+The name of the Shading:Site, Shading:Building, Shading:Site:Detailed, Shading:Building:Detailed, Shading:Overhang, Shading:Overhang:Projection, Shading:Fin, Shading:Fin:Projection or Shading:Zone:Detailed object to which the following fields apply.
+
+If this ShadingProperty:Reflectance object is not defined for a shading surface the default values listed in each of the following fields will be used in the solar reflection calculation.
+
+\paragraph{Field: Diffuse Solar Reflectance of Unglazed Part of Shading Surface}\label{field-diffuse-solar-reflectance-of-unglazed-part-of-shading-surface}
+
+The diffuse solar reflectance of the unglazed part of the shading surface (default = 0.2). This reflectance is assumed to be the same for beam-to-diffuse and diffuse-to-diffuse reflection. Beam-to-diffuse reflection is assumed to be independent of angle of incidence of beam radiation. Diffuse-to-diffuse reflection is assumed to be independent of angular distribution of the incident of diffuse radiation. The outgoing diffuse radiation is assumed to be isotropic (hemispherically uniform).
+
+The sum of this reflectance and the shading surface transmittance should be less than or equal to 1.0.
+
+\paragraph{Field: Diffuse Visible Reflectance of Unglazed Part of Shading Surface}\label{field-diffuse-visible-reflectance-of-unglazed-part-of-shading-surface}
+
+The diffuse visible reflectance of the unglazed part of the shading surface (default = 0.2). This reflectance is assumed to be the same for beam-to-diffuse and diffuse-to-diffuse reflection. Beam-to-diffuse reflection is assumed to be independent of angle of incidence of beam radiation. Diffuse-to-diffuse reflection is assumed to be independent of angular distribution of the incident of diffuse radiation. The outgoing diffuse radiation is assumed to be isotropic (hemispherically uniform).
+
+This value if used only for the daylighting calculation (ref: Daylighting:Controls). The sum of this reflectance and the shading surface transmittance should be less than or equal to 1.0.
+
+\paragraph{Field: Fraction of Shading Surface That Is Glazed}\label{field-fraction-of-shading-surface-that-is-glazed}
+
+The fraction of the area of the shading surface that consists of windows (default = 0.0). It is assumed that the windows are evenly distributed over the surface and have the same glazing construction (see following ``Name of Glazing Construction''). This might be the case, for example, for reflection from the façade of a neighboring, highly-glazed building. For the reflection calculation the possible presence of shades, screens or blinds on the windows of the shading surface is ignored. Beam-to-beam (specular) reflection is assumed to occur only from the glazed portion of the shading surface. This reflection depends on angle of incidence as determined by the program from the glazing construction. Beam-to-diffuse reflection from the glazed portion is assumed to be zero. The diffuse-to-diffuse reflectance of the glazed portion is determined by the program from the glazing construction.
+
+\paragraph{Field: Glazing Construction Name}\label{field-glazing-construction-name}
+
+The name of the construction of the windows on the shading surface. Required if Fraction of Shading Surface That Is Glazed is greater than 0.0.
+
+IDF example of Shading Surface Reflectance for shading surface with specular reflection
+
+\begin{lstlisting}
+
+Shading:Site:Detailed,
+  Adjacent Glazed Facade,  !- User Supplied Surface Name
+  ,   !- Shadowing Transmittance Schedule
+  4,  !- Number of Surface Vertex Groups -- Number of (X,Y,Z) groups
+  0,-24,30, !- Vertex 1 X,Y,Z coordinates
+  0,-24,0,  !- Vertex 2 X,Y,Z coordinates
+  0,0,0,    !- Vertex 3 X,Y,Z coordinates
+  0,0,30;   !-Vertex 3 X,Y,Z coordinates
+
+
+  ShadingProperty:Reflectance,
+  Adjacent Glazed Facade, !- Name of Surface:Shading Object
+  0.3,  !- Diffuse Solar Reflectance of Unglazed Part of Shading Surface
+  0.3,  !- Diffuse Visible Reflectance of Unglazed Part of Shading Surface
+  0.7,  !- Fraction of Shading Surface That Is Glazed
+  GlassCon-1; !- Name of Glazing Construction
+\end{lstlisting}
+
+IDF example of Shading Surface Reflectance for shading surface without specular reflection
+
+\begin{lstlisting}
+
+Shading:Site:Detailed,
+  Adjacent Blank Facade,  !- User Supplied Surface Name
+  ,   !- Shadowing Transmittance Schedule
+  4,  !- Number of Surface Vertex Groups -- Number of (X,Y,Z) groups
+  0,-24,30,
+  0,-24,0,
+  0,0,0,
+  0,0,30;
+
+
+  ShadingProperty:Reflectance,
+  Adjacent Blank Facade, !- Name of Surface:Shading Object
+  0.4,  !- Diffuse Solar Reflectance of Unglazed Part of Shading Surface
+  0.4,  !- Diffuse Visible Reflectance of Unglazed Part of Shading Surface
+  0.0,  !- Fraction of Shading Surface That Is Glazed
+  ;     !- Name of glazing construction
+\end{lstlisting}
+
+\subsection{WindowProperty:ShadingControl}\label{windowpropertyshadingcontrol}
+
+Window shading with coverings like drapes, blinds, screens or pull-down shades can be used to reduce the amount of solar radiation entering the window or reduce daylighting glare. It can also be used to reduce heat loss through the window (movable insulation). Leaving the window covering open in the winter can maximize solar heat gain and thereby reduce heating loads.
+
+With WindowProperty:ShadingControl---which is referenced by windows and glass doors (ref: FenestrationSurface:Detailed with Type = Window or GlassDoor)--you specify the type and location of the shading device, what variable or combination of variables controls deployment of the shading device, and what the control setpoint is. If the shading device is a blind, you also specify how the slat angle is controlled.
+
+NOTE: WindowProperty:ShadingControl does not work with complex fenestration systems. Controlled complex fenestration systems can be made only with Energy Management Systems objects. Inserting WindowProperty:ShadingControl in FenestrationSurface:Detailed while using complex fenestration systems will be ignored by program.
+
+As shown in Figure~\ref{fig:allowed-locations-of-a-window-shading-device.}, a shading device can be inside the window (Shading Type = InteriorShade or InteriorBlind), outside the window (Shading Type = ExteriorShade or ExteriorBlind), or between panes of glass (Shading Type = BetweenGlassShade or BetweenGlassBlind). The exception is window screens which can only be outside the window (Shading Type = ExteriorScreen).
+
+\begin{figure}[hbtp] % fig 34
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image060.png}
+\caption{Allowed locations of a window shading device. \protect \label{fig:allowed-locations-of-a-window-shading-device.}}
+\end{figure}
+
+When a shading device is present it is either retracted or activated. When it is retracted it covers none of the window. When it is activated it covers the entire glazed part of the window (but not the frame). Whether the shading device is retracted or activated in a particular timestep depends on the control mechanism: see ``Shading Control Type,'' below. To model a case in which the shading device, when activated, covers only \textbf{part} of the window you will have to divide the window into two separate windows, one with the shading device and one without the shading device.
+
+A shading device can also be of a kind in which the optical properties of the glazing switch from one set of values to another in order to increase or decrease solar or visible transmittance (Shading Type = SwitchableGlazing).
+
+There are two ways of specifying the actual shading device:
+
+\begin{itemize}
+  \item
+\textbf{Specify ``Name of Construction with Shading''}
+
+This is the name of a window Construction that has the shading device as one of its layers. The thermal and solar-optical properties of the shading device are given by the shading material referenced in that Construction (ref: Construction, WindowMaterial:Shade, WindowMaterial:Screen and WindowMaterial:Blind). To use this method you have to define two Constructions for the window, one without the shading device and one with it. See Example 1, below.
+
+The Construction without the shading device is referenced in the FenestrationSurface:Detailed input for the window (see IDF example, below). The Construction with the shading device is referenced by the window's WindowProperty:ShadingControl.
+
+For Shading Type = InteriorShade, InteriorBlind, ExteriorShade, ExteriorScreen and ExteriorBlind these two Constructions must be identical expect for the presence of the shading layer in the shaded Construction, otherwise you will get an error message. You will also get an error message if the Construction referenced by the window has a shading layer.
+
+  \item
+\textbf{Specify the ``Material Name of the Shading Device''}
+
+This is the name of a WindowMaterial:Shade, WindowMaterial:Screen or WindowMaterial:Blind. This method can be used with Shading Type = InteriorShade, InteriorBlind, ExteriorShade and ExteriorBlind. It cannot be used with Shading Type = BetweenGlassShade, BetweenGlassBlind, or SwitchableGlazing. If Shading Type = InteriorShade or ExteriorShade, then you specify the name of a WindowMaterial:Shade. If Shading Type = InteriorBlind or ExteriorBlind, then you specify the name of a WindowMaterial:Blind. If Shading Type = ExteriorScreen, then you specify the name of a WindowMaterial:Screen. See Example 2, below. This method is simpler to use since you don't have to specify two Constructions that differ only by the shading layer.
+
+When this method is used, the program will automatically create a shaded window construction by adding a shading layer to the outside or inside of the construction corresponding to the window referencing the WindowProperty:ShadingControl. The name, created by the program, of this shaded construction is composed as follows: if the name of the window construction is CCC and the material name of the shading device is DDD, then the shaded construction name is CCC:DDD:INT for an interior shading device and CCC:DDD:EXT for an exterior shading device.
+
+This method is the required if you want to add a shading device to a construction brought in from a WINDOW Data File (ref:Construction:WindowDataFile).
+
+Note that if both ``Name of Construction with Shading'' and ``Material Name of Shading Device'' are specified, the former takes precedence.
+\end{itemize}
+
+Most Shading Control Types allow you to specify a schedule that determines when the control is active. One example is a control that is active seasonally. For example, to deploy shading only in the summer when the incident solar is high enough, use Shading Control Type = OnIfHighSolarOnWindow with a schedule that is 1 during the summer months and 0 otherwise and specify Shading Control Is Scheduled = YES.
+
+In addition, most Shading Control Types also allow you to specify that glare control is active in addition to the specified Control Type. For example, you might want to deploy shading when the solar incident on a window is too high OR the glare from the window is too high. This type of joint control requires that the window be in a daylit zone, that the maximum allowed glare be specified in the Daylighting object for the zone, and that Glare Control Is Active = YES in WindowProperty:ShadingControl.
+
+If Shading Type = InteriorBlind, ExteriorBlind or BetweenGlassBlind you can use WindowProperty:ShadingControl to specify how the slat angle of the blind is controlled when the blind is in place.
+
+A special type of WindowProperty:ShadingControl is SwitchableGlazing. An example is electrochromic glazing in which the transmittance and reflectance of the glass is controlled electronically. For example, you could have electrochromic glazing switch from clear (high transmittance) to dark (low transmittance) to control solar gain. If you choose the Shading Type = SwitchableGlazing option for WindowProperty:ShadingControl, the unswitched (clear) state is specified by the Construction referenced by the window and the switched (dark) state is specified by the Construction referenced by WindowProperty:ShadingControl for that window. For example, if you specify Shading Type = SwitchableGlazing and Shading Control Type = OnIfHighSolarOnWindow, then the glazing will switch to the dark state whenever the solar radiation striking the window exceeds the Setpoint value.
+
+For Shading Type = SwitchableGlazing the state of the window is either clear (unswitched) or dark (fully switched) for all Shading Control Types except MeetDaylightIlluminanceSetpoint. In this case, the transmittance of the glazing is adjusted to just meet the daylight illuminance set point at the first daylighting reference point (see Daylighting). This type of control assures that there is just enough solar gain to meet the daylighting requirements in a zone, and no more, thus reducing the cooling load.
+
+\subsubsection{Inputs}\label{inputs-32-001}
+
+\paragraph{Field: Name}\label{field-name-29-001}
+
+Name of the window shading control. It is referenced by a window (ref: Field: Shading Control Name).
+
+\paragraph{Field: Shading Type}\label{field-shading-type}
+
+The type of shading device. The choices are:
+
+\emph{InteriorShade}: A diffusing shade is on the inside of the window. (In the shaded Construction the shading layer must be a WindowMaterial:Shade.)
+
+\emph{ExteriorShade}: A diffusing shade is on the outside of the window. (In the shaded Construction the shading layer must be a WindowMaterial:Shade.)
+
+\emph{BetweenGlassShade}: A diffusing shade is between two glass layers. (In the shaded Construction the shading layer must be a WindowMaterial:Shade.) This shading type is allowed only for double- and triple-glazing. For triple-glazing the shade must be between the two inner glass layers.
+
+\emph{ExteriorScreen}: An insect screen is on the outside of the window. (In the shaded Construction the shadling layer must be a WindowMaterial:Screen.)
+
+\emph{InteriorBlind}: A slat-type shading device, such as a Venetian blind, is on the inside of the window. (In the shaded Construction the shading layer must be a WindowMaterial:Blind.)
+
+\emph{ExteriorBlind}: A slat-type shading device is on the outside of the window. (In the shaded Construction the shading layer must be a WindowMaterial:Blind.)
+
+\emph{BetweenGlassBlind}: A slat-type shading device is between two glass layers. (In the shaded Construction the shading layer must be a WindowMaterial:Blind.) This shading type is allowed only for double- and triple-glazing. For triple-glazing the blind must be between the two inner glass layers.
+
+\emph{SwitchableGlazing}: Shading is achieved by changing the characteristics of the window glass, such as by darkening it.
+
+\paragraph{Field: Construction with Shading Name}\label{field-construction-with-shading-name}
+
+Name of the window Construction that has the shading in place. The properties of the shading device are given by the shading material referenced in that Construction (ref: Construction, WindowMaterial:Shade, WindowMaterial:Screen and WindowMaterial:Blind). For Shading Type = SwitchableGlazing, this is the name of the Construction that corresponds to the window in its fully-switched (darkest) state.
+
+Specifying ``Name of Construction with Shading'' is required if Shading Type = BetweenGlassShade, BetweenGlassBlind, or SwitchableGlazing. For other Shading Types, you may alternatively specify ``Material Name of Shading Device'' (see below).
+
+\paragraph{Field: Shading Control Type}\label{field-shading-control-type}
+
+Specifies how the shading device is controlled, i.e., it determines whether the shading device is ``on'' or ``off.'' For blinds, screens and shades, when the device is ``on'' it is assumed to cover all of the window except its frame; when the device is ``off'' it is assumed to cover none of the window (whether ``on'' or ``off'' the shading device is assumed to cover none of the wall that the window is on).
+
+For switchable glazing, ``on'' means that the glazing is in the fully-switched state and ``off'' means that it is in the unswitched state; for example, for electrochromic glazing, ``on'' means the glazing is in its darkest state and ``off'' means it is in its lightest state.
+
+The choices for Shading Control Type are the following. If SetPoint is applicable its units are shown in parentheses.
+
+\emph{AlwaysOn}: Shading is always on.
+
+\emph{AlwaysOff}: Shading is always off.
+
+The following six control types are used primarily to reduce zone cooling load due to window solar gain.
+
+\emph{OnIfScheduleAllows}: Shading is on if schedule value is non-zero. Requires that Schedule Name be specified and Shading Control Is Scheduled = Yes.
+
+Note: For exterior window screens \emph{AlwaysOn, AlwaysOff, and OnIfScheduleAllows} are the only valid shading control types.
+
+\emph{OnIfHighSolarOnWindow}: Shading is on if beam plus diffuse solar radiation incident on the window exceeds SetPoint (W/m\(^{2}\)) and schedule, if specified, allows shading.
+
+\emph{OnIfHighHorizontalSolar}: Shading is on if total (beam plus diffuse) horizontal solar irradiance exceeds SetPoint (W/m\(^{2}\)) and schedule, if specified, allows shading.
+
+\emph{OnIfHighOutdoorAirTemperature}: Shading is on if outside air temperature exceeds SetPoint (C) and schedule, if specified, allows shading.
+
+\emph{OnIfHighZoneAirTemperature}: Shading is on if zone air temperature in the previous timestep exceeds SetPoint (C) and schedule, if specified, allows shading.
+
+\emph{OnIfHighZoneCooling}: Shading is on if zone cooling rate in the previous timestep exceeds SetPoint (W) and schedule, if specified, allows shading.
+
+\emph{OnIfHighGlare}: Shading is on if the total daylight glare index at the zone's first daylighting reference point from all of the exterior windows in the zone exceeds the maximum glare index specified in the daylighting input for zone (ref: Group -- Daylighting). Applicable only to windows in zones with daylighting.
+
+Note: Unlike other Shading Control Types, glare control is active whether or not a schedule is specified.
+
+\emph{MeetDaylightIlluminanceSetpoint}: Used only with ShadingType = SwitchableGlazing in zones with daylighting controls. In this case the transmittance of the glazing is adjusted to just meet the daylight illuminance set point at the first daylighting reference point. Note that the daylight illuminance set point is specified in the Daylighting:Controls object for the Zone; it is not specified as a WindowProperty:ShadingControl SetPoint. When the glare control is active, if meeting the daylight illuminance set point at the first daylighting reference point results in higher discomfort glare index (DGI) than the specified zone's maximum allowable DGI for either of the daylight reference points, the glazing will be further dimmed until the DGI equals the specified maximum allowable value.
+
+The following three control types can be used to reduce zone heating load during the winter by reducing window conductive heat loss at night and leaving the window unshaded during the day to maximize solar gain. They are applicable to any Shading Type except ExteriorScreen but are most appropriate for interior or exterior shades with high insulating value (``movable insulation''). ``Night'' means the sun is down and ``day'' means the sun is up.
+
+\emph{OnNightIfLowOutdoorTempAndOffDay}: Shading is on at night if the outside air temperature is less than SetPoint (C) and schedule, if specified, allows shading. Shading is off during the day.
+
+\emph{OnNightIfLowInsideTempAndOffDay}: Shading is on at night if the zone air temperature in the previous timestep is less than SetPoint (C) and schedule, if specified, allows shading. Shading is off during the day.
+
+\emph{OnNightIfHeatingAndOffDay}: Shading is on at night if the zone heating rate in the previous timestep exceeds SetPoint (W) and schedule, if specified, allows shading. Shading is off during the day.
+
+The following two control types can be used to reduce zone heating and cooling load. They are applicable to any Shading Type except ExteriorScreen but are most appropriate for translucent interior or exterior shades with high insulating value (``translucent movable insulation'').
+
+\emph{OnNightIfLowOutdoorTempAndOnDayIfCooling}: Shading is on at night if the outside air temperature is less than SetPoint (C). Shading is on during the day if the zone cooling rate in the previous timestep is non-zero. Night and day shading is subject to schedule, if specified.
+
+\emph{OnNightIfHeatingAndOnDayIfCooling}: Shading is on at night if the zone heating rate in the previous timestep exceeds SetPoint (W). Shading is on during the day if the zone cooling rate in the previous timestep is non-zero. Night and day shading is subject to schedule, if specified.
+
+The following control types can be used to reduce zone cooling load. They are applicable to any Shading Type except ExteriorScreen but are most appropriate for interior or exterior blinds, interior or exterior shades with low insulating value, or switchable glazing.
+
+\emph{OffNightAndOnDayIfCoolingAndHighSolarOnWindow}: Shading is off at night. Shading is on during the day if the solar radiation incident on the window exceeds SetPoint (W/m\(^{2}\)) and if the zone cooling rate in the previous timestep is non-zero. Daytime shading is subject to schedule, if specified.
+
+\emph{OnNightAndOnDayIfCoolingAndHighSolarOnWindow}: Shading is on at night. Shading is on during the day if the solar radiation incident on the window exceeds SetPoint (W/m\(^{2}\)) and if the zone cooling rate in the previous timestep is non-zero. Day and night shading is subject to schedule, if specified. (This Shading Control Type is the same as the previous one, except the shading is on at night rather than off.)
+
+\emph{OnIfHighOutdoorAirTempAndHighSolarOnWindow:} Shading is on if the outside air temperature exceeds the Setpoint (C) and if if the solar radiation incident on the window exceeds SetPoint 2 (W/m\(^{2}\)).
+
+\emph{OnIfHighOutdoorAirTempAndHighHorizontalSolar:} Shading is on if the outside air temperature exceeds the Setpoint (C) and if if the horizontal solar radiation exceeds SetPoint 2 (W/m\(^{2}\)).
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-007}
+
+Required if Shading Control Is Scheduled = Yes. If schedule value \textgreater{} 0 , shading control is active, i.e., shading can be on only if the shading control test passes. If schedule value = 0, shading is off whether or not the control test passes. If Schedule Name is not specified, shading control is assumed to be active at all times.
+
+\paragraph{Field: Setpoint}\label{field-setpoint}
+
+The setpoint for activating window shading. The units depend on the type of trigger:
+
+\begin{itemize}
+\item
+  W/m\(^{2}\) for solar-based controls
+\item
+  W for cooling- or heating-based controls
+\item
+  Degrees C for temperature-based controls
+\end{itemize}
+
+SetPoint is unused for Shading Control Type = OnIfScheduleAllows, OnIfHighGlare and DaylightIlluminance.
+
+\paragraph{Field: Shading Control Is Scheduled}\label{field-shading-control-is-scheduled}
+
+Accepts values YES and NO. The default is NO. Not applicable for Shading Control Type = OnIfHighGlare and should be blank in that case.
+
+If YES, Schedule Name is required and that schedule determines whether the shading control specified by Shading Control Type is active or inactive (see Schedule Name, above).
+
+If NO, Schedule Name is not applicable (should be blank) and the shading control is unscheduled.
+
+Shading Control Is Scheduled = YES is required if Shading Control Type = OnIfScheduleAllows.
+
+\paragraph{Field: Glare Control Is Active}\label{field-glare-control-is-active}
+
+Accepts values YES and NO. The default is NO.
+
+If YES and the window is in a daylit zone, shading is on if the zone's discomfort glare index exceeds the maximum discomfort glare index specified in the Daylighting object referenced by the zone. For switchable windows with \emph{MeetDaylightIlluminanceSetpoint} shading control, if Glare Control is active, the windows are always continuously dimmed as necessary to meet the zone's maximum allowable DGI while providing appropriate amount of daylight for the zone.
+
+The glare test is OR'ed with the test specified by Shading Control Type. For example, if Glare Control Is Active = YES and Shading Control Type = OnIfHighZoneAirTemp, then shading is on if glare is too high OR if the zone air temperature is too high.
+
+Glare Control Is Active = YES is required if Shading Control Type = OnIfHighGlare.
+
+\paragraph{Field: Shading Device Material Name}\label{field-shading-device-material-name}
+
+The name of a WindowMaterial:Shade, WindowMaterial:Screen or WindowMaterial:Blind. Required if ``Name of Construction with Shading'' is not specified. Not applicable if Shading Type = BetweenGlassShade, BetweenGlassBlind or SwitchableGlazing and should be blank in this case. If both ``Name of Construction with Shading'' and ``Material Name of Shading Device'' are entered the former takes precedence.
+
+\paragraph{Field: Type of Slat Angle Control for Blinds}\label{field-type-of-slat-angle-control-for-blinds}
+
+Applies only to Shading Type = InteriorBlind, ExteriorBlind or BetweenGlassBlind. Specifies how the slat angle is controlled. The choices are FixedSlatAngle, ScheduledSlatAngle and BlockBeamSolar.
+
+If FixedSlatAngle (the default), the angle of the slat is fixed at the value input for the WindowMaterial:Blind that is contained in the construction specified by Name of Construction with Shading or is specified by Material Name of Shading Device.
+
+If ScheduledSlatAngle, the slat angle varies according to the schedule specified by Slat Angle Schedule Name, below.
+
+If BlockBeamSolar, the slat angle is set each timestep to just block beam solar radiation. If there is no beam solar on the window the slat angle is set to the value input for the WindowMaterial:Blind that is contained in the construction specified by Name of Construction with Shading or is specified by Material Name of Shading Device. The BlockBeamSolar option prevents beam solar from entering the window and causing possible unwanted glare if the beam falls on work surfaces while at the same time allowing near-optimal indirect radiation for daylighting.
+
+\paragraph{Field: Slat Angle Schedule Name}\label{field-slat-angle-schedule-name}
+
+This is the name of a schedule of slat angles that is used when Type of Slat Angle Control for Blinds = ScheduledSlatAngle. You should be sure that the schedule values fall within the range given by the Minimum Slat Angle and Maximum Slat Angle values entered in the corresponding WindowMaterial:Blind. If not, the program will force them into this range.
+
+\paragraph{Field: Setpoint 2}\label{field-setpoint-2}
+
+Used only as the second setpoint for the following two-setpoint control types: OnIfHighOutdoorAirTempAndHighSolarOnWindow, OnIfHighOutdoorAirTempAndHighHorizontalSolar, OnIfHighZoneAirTempAndHighSolarOnWindow,
+
+and OnIfHighZoneAirTempAndHighHorizontalSolar
+
+An IDF example: window with interior roll shade that is deployed when solar incident on the window exceeds 50 W/m\(^{2}\).
+
+\begin{lstlisting}
+! Example 1: Interior movable shade specified by giving name of shaded construction
+! in WindowProperty:ShadingControl
+
+WindowMaterial:Glazing, GLASS - CLEAR SHEET 1 / 8 IN,  !- Material Name
+       SpectralAverage,! Optical data type {SpectralAverage or Spectral}
+       ,               ! Name of spectral data set when Optical Data Type = Spectral
+       0.003        ,  !- Thickness {m}
+       0.837        ,  !- Solar Transmittance at Normal Incidence
+       0.075        ,  !- Solar Reflectance at Normal Incidence: Front Side
+       0.075        ,  !- Solar Reflectance at Normal Incidence: Back Side
+       0.898        ,  !- Visible Transmittance at Normal Incidence
+       0.081        ,  !- Visible Reflectance at Normal Incidence: Front Side
+       0.081        ,  !- Visible Reflectance at Normal Incidence: Back Side
+       0.0          ,  !- IR Transmittance
+       0.8400000    ,  !- IR Emissivity: Front Side
+       0.8400000    ,  !- IR Emissivity: Back Side
+       0.9000000    ;  !- Conductivity {W/m-K}
+
+WindowMaterial:Shade, ROLL SHADE,  !- Material Name
+       0.3          ,   !- Solar Transmittance at normal incidence
+       0.5000000    ,   !- Solar Reflectance (same for front and back side)
+       0.3          ,   !- Visible Transmittance at normal incidence
+       0.5000000    ,   !- Visible reflectance (same for front and back side)
+       0.9000000    ,   !- IR Emissivity (same for front and back side)
+       0.05         ,   !- IR Transmittance
+       0.003        ,   !- Thickness
+       0.1          ,   !- Conductivity {W/m-K}
+       0.0          ,   !- Top Opening Multiplier
+       0.0          ,   !- Bottom Opening Multiplier
+       0.5          ,   !- Left-Side Opening Multiplier
+       0.5          ,   !- Right-Side Opening Multiplier
+       0.0          ;   !- Air-Flow Permeability
+
+Construction, SINGLE PANE WITH NO SHADE,  ! Name of construction without shade
+       GLASS - CLEAR SHEET 1 / 8 IN;  !- First material layer
+
+Construction, SINGLE PANE WITH INT SHADE, ! Name of construction with shade
+       GLASS - CLEAR SHEET 1 / 8 IN,  !- First material layer
+       ROLL SHADE                  ;  !- Second material layer
+
+WindowProperty:ShadingControl, CONTROL ON INCIDENT SOLAR,  !- Name of Shading Control
+       InteriorShade,                !- Shading Type
+       SINGLE PANE WITH INT SHADE,   !- Name of construction with shading device
+       OnIfHighSolarOnWindow,        !- Shading Control Type
+       ,                             !- Schedule name
+       50.0,                         !- Setpoint {W/m2}
+       NO,                           !- Shading Control Is Scheduled
+       NO,                           !- Glare Control Is Active
+       ,                             !- Material Name of Shading Device
+       ,                             !- Type of Slat Angle Control for Blinds
+       ;                             !- Slat Angle Schedule Name
+
+FenestrationSurface:Detailed, Zn001:Wall001:Win001,  !- SubSurface Name
+       Window                   ,    !- Class
+       SINGLE PANE WITH NO SHADE,    !- Name of construction without shading device
+       Zn001:Wall001            ,    !- Base Surface Name
+       ,                             !- Target
+       0.5000000                ,    !- VF to Ground
+       CONTROL ON INCIDENT SOLAR,    !- Window Shading Control name
+       ,                             !- Frame/Divider name
+       1.0                      ,    !- Multiplier
+       4                        ,    !- Number of vertices (assumed rectangular)
+       0.548 ,  0.0 ,   2.5     ,    !- x,y,z of vertices {m}
+       0.548 ,  0.0 ,   0.5     ,
+       5.548 ,  0.0 ,   0.5     ,
+       5.548 ,  0.0 ,   2.5     ;
+\end{lstlisting}
+
+\begin{lstlisting}
+! Example 2: Interior movable shade specified by giving name of shading device in WindowProperty:ShadingControl
+
+WindowMaterial:Glazing, GLASS - CLEAR SHEET 1 / 8 IN,  !- Material Name
+       SpectralAverage,! Optical data type {SpectralAverage or Spectral}
+       ,               ! Name of spectral data set when Optical Data Type = Spectral
+       0.003        ,  !- Thickness {m}
+       0.837        ,  !- Solar Transmittance at Normal Incidence
+       0.075        ,  !- Solar Reflectance at Normal Incidence: Front Side
+       0.075        ,  !- Solar Reflectance at Normal Incidence: Back Side
+       0.898        ,  !- Visible Transmittance at Normal Incidence
+       0.081        ,  !- Visible Reflectance at Normal Incidence: Front Side
+       0.081        ,  !- Visible Reflectance at Normal Incidence: Back Side
+       0.0          ,  !- IR Transmittance
+       0.8400000    ,  !- IR Emissivity: Front Side
+       0.8400000    ,  !- IR Emissivity: Back Side
+       0.9000000    ;  !- Conductivity {W/m-K}
+
+WindowMaterial:Shade, ROLL SHADE,  !- Material Name
+       0.3          ,   !- Solar Transmittance at normal incidence
+       0.5000000    ,   !- Solar Reflectance (same for front and back side)
+       0.3          ,   !- Visible Transmittance at normal incidence
+       0.5000000    ,   !- Visible reflectance (same for front and back side)
+       0.9000000    ,   !- IR Emissivity (same for front and back side)
+       0.05         ,   !- IR Transmittance
+       0.003        ,   !- Thickness
+       0.1          ,   !- Conductivity {W/m-K}
+       0.0          ,   !- Top Opening Multiplier
+       0.0          ,   !- Bottom Opening Multiplier
+       0.5          ,   !- Left-Side Opening Multiplier
+       0.5          ,   !- Right-Side Opening Multiplier
+       0.0          ;   !- Air-Flow Permeability
+
+Construction, SINGLE PANE WITH NO SHADE,  ! Name of construction without shade
+       GLASS - CLEAR SHEET 1 / 8 IN;  !- First material layer
+
+WINDOWPROPERTY:SHADINGCONTROL, CONTROL ON INCIDENT SOLAR,  !- Name of Shading Control
+       InteriorShade,                !- Shading Type
+       ,                             !- Name of shaded construction
+       OnIfHighSolarOnWindow,        !- Shading Control Type
+       ,                             !- Schedule name
+       50.0,                         !- Setpoint {W/m2}
+       NO,                           !- Shading Control Is Scheduled
+       NO,                           !- Glare Control Is Active
+       ROLL SHADE,                   !- Material Name of Shading Device
+       ,                             !- Type of Slat Angle Control for Blinds
+       ;                             !- Slat Angle Schedule Name
+
+FenestrationSurface:Detailed, Zn001:Wall001:Win001,  !- SubSurface Name
+       Window                   ,    !- Class
+       SINGLE PANE WITH NO SHADE,    !- Name of construction without shade
+       Zn001:Wall001            ,    !- Base Surface Name
+       ,                             !- Target
+       0.5000000                ,    !- VF to Ground
+       CONTROL ON INCIDENT SOLAR,    !- Window Shading Control name
+       ,                             !- Frame/Divider name
+       1.0                      ,    !- Multiplier
+       4                        ,    !- Number of vertices (assumed rectangular)
+       0.548 ,  0.0 ,   2.5     ,    !- x,y,z of vertices {m}
+       0.548 ,  0.0 ,   0.5     ,
+       5.548 ,  0.0 ,   0.5     ,
+       5.548 ,  0.0 ,   2.5     ;
+\end{lstlisting}
+
+\subsection{WindowProperty:FrameAndDivider}\label{windowpropertyframeanddivider}
+
+The WindowProperty:FrameAndDivider object is referenced by exterior windows that have
+
+\begin{itemize}
+\item
+  a frame, and/or
+\item
+  a divider, and/or
+\item
+  reveal surfaces that reflect beam solar radiation.
+\end{itemize}
+
+A \textbf{\emph{frame}} surrounds the glazing in a window (see Figure~\ref{fig:a-window-with-a-frame-and-divider.} and Figure~\ref{fig:illustration-showing-frame-and-divider}). It is assumed that all frame characteristics---such as width, conductance and solar absorptance---are the same for the top, bottom and side elements of the frame. If the frame elements are not the same then you should enter area-weighted average values for the frame characteristics.
+
+The window vertices that you specify in the FenestrationSurface:Detailed object are those of the glazed part of the window, not the frame. EnergyPlus automatically subtracts the area of the frame---determined from the glazing dimensions and the frame width---from the area of the wall containing the window.
+
+A \textbf{\emph{divider}}, as shown in Figure~\ref{fig:a-window-with-a-frame-and-divider.}, Figure~\ref{fig:illustration-showing-frame-and-divider} and Figure~\ref{fig:illustration-showing-divider-types.}, divides the glazing up into separate lites. It is assumed that all divider elements have the same characteristics. If not, area-weighted average values should be used. EnergyPlus automatically subtracts the divider area from the glazed area of the window.
+
+\textbf{\emph{Reveal surfaces}}, as shown in Figure~\ref{fig:a-vertical-section-through-a-window-with}, are associated with the setback of the glazing from the outside and/or inside surface of the parent wall. If the depth and solar absorptance of these surfaces are specified, the program will calculate the reflection of beam solar radiation from these surfaces. The program also calculates the shadowing (onto the window) of beam and diffuse solar radiation by outside reveal surfaces.
+
+In EnergyPlus, a window can have any combination of frame, divider and reveal surfaces, or none of these.
+
+The best source of frame and divider characteristics is the WINDOW program, which will calculate the values required by EnergyPlus for different frame and divider types. In particular, the THERM program within the WINDOW program will calculate the effective conductance of frames and dividers; this is the conductance taking 2-D heat transfer effects into account.
+
+Note that a window's frame and divider characteristics, along with other window information, can be read in from the Window Data File (see ``Importing Windows from the WINDOW program'' and ``Construction:WindowDataFile object''). In this case the WindowProperty:FrameAndDivider referenced by the window is not applicable and should be blank unless you want to specify reveal surfaces for beam solar reflection.
+
+\begin{figure}[hbtp] % fig 35
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image061.png}
+\caption{A window with a frame and divider. \protect \label{fig:a-window-with-a-frame-and-divider.}}
+\end{figure}
+
+In the illustration above, the divider has two horizontal elements and one vertical element.
+
+\subsubsection{Inputs}\label{inputs-33-001}
+
+\paragraph{Field: Name}\label{field-name-30-001}
+
+The name of the frame/divider object. It is referenced by WindowProperty:FrameAndDivider Name in FenestrationSurface:Detailed.
+
+\textbf{\emph{Frame Fields}}
+
+\paragraph{Field: Frame Width}\label{field-frame-width}
+
+The width of the frame elements when projected onto the plane of the window. It is assumed that the top, bottom and side elements of the frame have the same width. If not, an average frame width should be entered such that the projected frame area calculated using the average value equals the sum of the areas of the frame elements.
+
+\paragraph{Field: Frame Outside Projection}\label{field-frame-outside-projection}
+
+The amount by which the frame projects outward from the outside surface of the window glazing. If the outer surface of the frame is flush with the glazing, Frame Outside Projection = 0.0. Used to calculate shadowing of frame onto glass, solar absorbed by frame, IR emitted and absorbed by frame, and convection from frame.
+
+\paragraph{Field: Frame Inside Projection}\label{field-frame-inside-projection}
+
+The amount by which the frame projects inward from the inside surface of the window glazing. If the inner surface of the frame is flush with the glazing, Frame Inside Projection = 0.0. Used to calculate solar absorbed by frame, IR emitted and absorbed by frame, and convection from frame.
+
+\begin{figure}[hbtp] % fig 36
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image062.png}
+\caption{Illustration showing frame and divider dimensioning. \protect \label{fig:illustration-showing-frame-and-divider}}
+\end{figure}
+
+\paragraph{Field: Frame Conductance}\label{field-frame-conductance}
+
+The effective thermal conductance of the frame measured from inside to outside frame surface (no air films) and taking 2-D conduction effects into account. Obtained from the WINDOW program or other 2-D calculation.
+
+\paragraph{Field: Ratio of Frame-Edge Glass Conductance to Center-Of-Glass Conductance}\label{field-ratio-of-frame-edge-glass-conductance-to-center-of-glass-conductance}
+
+The glass conductance near the frame (excluding air films) divided by the glass conductance at the center of the glazing (excluding air films). Used only for multi-pane glazing constructions. This ratio is greater than 1.0 because of thermal bridging from the glazing across the frame and across the spacer that separates the glass panes. Values can be obtained from the WINDOW program the user-selected glazing construction and frame characteristics.
+
+\paragraph{Field: Frame Solar Absorptance}\label{field-frame-solar-absorptance}
+
+The solar absorptance of the frame. The value is assumed to be the same on the inside and outside of the frame and to be independent of angle of incidence of solar radiation. If solar reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials).
+
+\paragraph{Field: Frame Visible Absorptance}\label{field-frame-visible-absorptance}
+
+The visible absorptance of the frame. The value is assumed to be the same on the inside and outside of the frame and to be independent of angle of incidence of solar radiation. If visible reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials).
+
+\paragraph{Field: Frame Thermal Hemispherical Emissivity}\label{field-frame-thermal-hemispherical-emissivity}
+
+The thermal emissivity of the frame, assumed the same on the inside and outside.
+
+\textbf{\emph{Divider Fields}}
+
+\paragraph{Field: Divider Type}\label{field-divider-type}
+
+The type of divider (see figure below). Divider Type = Suspended is applicable only to multi-pane glazing. It means that the divider is suspended between the panes. (If there are more than two glass layers, the divider is assumed to be placed between the two outermost layers.)
+
+Divider Type = DividedLite means that the divider elements project out from the outside and inside surfaces of the glazing and divide the glazing into individual lites. For multi-pane glazing, this type of divider also has between-glass elements that separate the panes.
+
+\begin{figure}[hbtp] % fig 37
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image063.png}
+\caption{Illustration showing divider types. \protect \label{fig:illustration-showing-divider-types.}}
+\end{figure}
+
+\paragraph{Field: Divider Width}\label{field-divider-width}
+
+The width of the divider elements when projected onto the plane of the window. It is assumed that the horizontal and vertical divider elements have the same width. If not, an average divider width should be entered such that the projected divider area calculated using the average value equals the sum of the areas of the divider elements.
+
+\paragraph{Field: Number of Horizontal Dividers}\label{field-number-of-horizontal-dividers}
+
+The number of divider elements parallel to the top and bottom of the window.
+
+\paragraph{Field: Number of Vertical Dividers}\label{field-number-of-vertical-dividers}
+
+The number of divider elements parallel to the sides of the window.
+
+\paragraph{Field: Divider Outside Projection}\label{field-divider-outside-projection}
+
+The amount by which the divider projects out from the outside surface of the window glazing. For Divider Type = Suspended, Divider Projection = 0.0. Used to calculate shadowing of divider onto glass, solar absorbed by divider, IR emitted and absorbed by divider, and convection from divider.
+
+\paragraph{Field: Divider Inside Projection}\label{field-divider-inside-projection}
+
+The amount by which the divider projects inward from the inside surface of the window glazing. If the inner surface of the divider is flush with the glazing, Divider Inside Projection = 0.0. Used to calculate solar absorbed by divider, IR emitted and absorbed by divider, and convection from divider.
+
+\paragraph{Field: Divider Conductance}\label{field-divider-conductance}
+
+The effective thermal conductance of the divider measured from inside to outside divider surface (no air films) and taking 2-D conduction effects into account. Obtained from the WINDOW program or other 2-D calculation.
+
+\paragraph{Field: Ratio of Divider-Edge Glass Conductance to Center-Of-Glass Conductance}\label{field-ratio-of-divider-edge-glass-conductance-to-center-of-glass-conductance}
+
+The glass conductance near the divider (excluding air films) divided by the glass conductance at the center of the glazing (excluding air films). Used only for multi-pane glazing constructions. This ratio is greater than 1.0 because of thermal bridging from the glazing across the divider and across the spacer that separates the glass panes. Values can be obtained from the WINDOW program for the user-selected glazing construction and divider characteristics.
+
+\paragraph{Field: Divider Solar Absorptance}\label{field-divider-solar-absorptance}
+
+The solar absorptance of the divider. The value is assumed to be the same on the inside and outside of the divider and to be independent of angle of incidence of solar radiation. If solar reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials).
+
+\paragraph{Field: Divider Visible Absorptance}\label{field-divider-visible-absorptance}
+
+The visible absorptance of the divider. The value is assumed to be the same on the inside and outside of the divider and to be independent of angle of incidence of solar radiation. If visible reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials).
+
+\paragraph{Field: Divider Thermal Hemispherical Emissivity}\label{field-divider-thermal-hemispherical-emissivity}
+
+The thermal emissivity of the divider, assumed the same on the inside and outside.
+
+\textbf{\emph{Reveal Surface Fields}}
+
+The following fields specify the properties of the window reveal surfaces (reveals occur when the window is not in the same plane as the base surface). From this information and from the geometry of the window and the sun position, the program calculates beam solar radiation absorbed and reflected by the top, bottom, right and left sides of outside and inside window reveal surfaces. In doing this calculation, the shadowing on a reveal surface by other reveal surfaces is determined using the orientation of the reveal surfaces and the sun position.
+
+It is assumed that:
+
+\begin{itemize}
+\item
+  The window is an exterior window.
+\item
+  The reveal surfaces are perpendicular to the window plane.
+\item
+  If an exterior shade, screen or blind is in place it shades exterior and interior reveal surfaces so that in this case there is no beam solar on these surfaces.
+\item
+  If an interior shade or blind is in place it shades the interior reveal surfaces so that in this case there is no beam solar on these surfaces.
+\item
+  The possible shadowing on inside reveal surfaces by a window divider is ignored.
+\item
+  The outside reveal surfaces (top, bottom, left, right) have the same solar absorptance and depth. This depth is not input here but is automatically determined by the program---from window and wall vertices--as the distance between the plane of the outside face of the glazing and plane of the outside face of the parent wall.
+\item
+  The inside reveal surfaces are divided into two categories: (1) the bottom reveal surface, called here the ``inside sill;'' and (2) the other reveal surfaces (left, right and top).
+\item
+  The left, right and top inside reveal surfaces have the same depth and solar absorptance. The inside sill is allowed to have depth and solar absorptance values that are different from the corresponding values for the other inside reveal surfaces.
+\item
+  The inside sill depth is required to be greater than or equal to the depth of the other inside reveal surfaces. If the inside sill depth is greater than zero the depth of the other inside reveal surfaces is required to be greater than zero.
+\item
+  The reflection of beam solar radiation from all reveal surfaces is assumed to be isotropic diffuse; there is no specular component.
+\item
+  Half of the beam solar reflected from outside reveal surfaces is goes towards the window; the other half goes back to the exterior environment (i.e., reflection of this outward-going component from other outside reveal surfaces is not considered).
+\item
+  The half that goes towards the window is added to the other solar radiation incident on the window. Correspondingly, half of the beam solar reflected from inside reveal surfaces goes towards the window, with the other half going into the zone. The portion going towards the window that is not reflected is absorbed in the glazing or is transmitted back out into the exterior environment.
+\item
+  The beam solar that is absorbed by outside reveal surfaces is added to the solar absorbed by the outside surface of the window's parent wall; similarly, the beam solar absorbed by the inside reveal surfaces is added to the solar absorbed by the inside surface of the parent wall.
+\end{itemize}
+
+The net effect of beam solar reflected from outside reveal surfaces is to increase the heat gain to the zone, whereas the effect of beam solar reflected from inside reveal surfaces is to decrease the heat gain to the zone since part of this reflected solar is transmitted back out the window.
+
+~If the window has a frame, the absorption of reflected beam solar by the inside and outside surfaces of the frame is considered. The shadowing of the frame onto interior reveal surfaces is also considered.
+
+\paragraph{Field: Outside Reveal Solar Absorptance}\label{field-outside-reveal-solar-absorptance}
+
+The solar absorptance of outside reveal surfaces.
+
+\paragraph{Field: Inside Sill Depth}\label{field-inside-sill-depth}
+
+The depth of the inside sill, measured from the inside surface of the glazing to the edge of the sill (see Figure~\ref{fig:a-vertical-section-through-a-window-with}).
+
+\paragraph{Field: Inside Sill Solar Absorptance}\label{field-inside-sill-solar-absorptance}
+
+The solar absorptance of the inside sill.
+
+\textbf{\emph{Field: Inside Reveal Depth}}
+
+The depth of the inside reveal surfaces other than the sill, measured from the inside surface of the glazing to the edge of the reveal surface (see Figure~\ref{fig:a-vertical-section-through-a-window-with}).
+
+\paragraph{Field: Inside Reveal Solar Absorptance}\label{field-inside-reveal-solar-absorptance}
+
+The solar absorptance of the inside reveal surfaces other than the sill.
+
+\begin{figure}[hbtp] % fig 38
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image064.png}
+\caption{(a) Vertical section through a window (with frame) showing outside and inside reveal surfaces and inside sill. (b) Perspective view looking from the outside of a window (without frame) showing reveal surfaces. Note that “Outside Reveal Depth� is not a user input; it is calculated by the program from the window and wall vertices. \protect \label{fig:a-vertical-section-through-a-window-with}}
+\end{figure}
+
+An IDF example:
+
+\begin{lstlisting}
+
+  WindowProperty:FrameAndDivider,
+        TestFrameAndDivider, ! Frame/Divider Name
+        0.05, ! Frame Width
+        0.04, ! Frame Outside Projection
+        0.03, ! Frame Inside Projection
+        5.0,  ! Frame Conductance
+        1.3,  ! Ratio of Frame-Edge Glass Conductance to Center-Of-Glass Conductance
+        0.8,  ! Frame Solar Absorptance
+        0.8,  ! Frame Visible Absorptance
+        0.9,  ! Frame Thermal Emissivity
+        DividedLite, ! Divider Type
+        0.03, ! Divider Width
+        2,    ! Number of Horizontal Dividers
+        2,    ! Number of Vertical Dividers
+        0.03, ! Divider Outside Projection
+        0.03, ! Divider Inside Projection
+        5.0,  ! Divider Conductance
+        1.3,  ! Ratio of Divider-Edge Glass Conductance to Center-Of-Glass Conductance
+        0.8,  ! Divider Solar Absorptance
+        0.8,  ! Divider Visible Absorptance
+        0.9,  ! Divider Thermal Emissivity
+        0.7,  ! Outside Reveal Solar Absorptance
+        0.25, ! Inside Sill Depth (m)
+        0.6,  ! Inside Sill Solar Absorptance
+        0.2,  ! Inside Reveal Depth (m)
+        0.5;  ! Inside Reveal Solar Absorptance
+\end{lstlisting}
+
+\subsection{WindowProperty:AirflowControl}\label{windowpropertyairflowcontrol}
+
+This object is used to specify the control mechanism for windows in which forced air flows in the gap between adjacent layers of glass. Such windows are called ``airflow windows.'' They are also known as ``heat-extract windows'' or ``climate windows.''
+
+A common application is to reduce the zone load by exhausting indoor air through the window. In the cooling season this picks up and expels some of the solar heat absorbed by the window glass (and by the between-glass shade or blind, if present). In the heating season this warms the window, reducing the heat loss from the window. A side benefit is increased thermal comfort. This is because the inside surface of the window will generally be cooler in summer and warmer in winter.
+
+The surface output variable ``Surface Window Gap Convective Heat Transfer Rate'' gives the heat picked up (or lost) by the gap airflow.
+
+\subsubsection{Inputs}\label{inputs-34-001}
+
+\paragraph{Field: Name}\label{field-name-31-001}
+
+Name of the window that this WindowProperty:AirflowControl refers to. It must be a window with two or three glass layers, i.e., double- or triple-glazing. For triple-glazing the airflow is assumed to be between the two inner glass layers.
+
+An error will result if the gas in the airflow gap is other than air. If an airflow window has a between-glass shade or blind, the gas in the gap on either side of the shade or blind must be air.
+
+\paragraph{Field: Airflow Source}\label{field-airflow-source}
+
+The source of the gap airflow. The choices are:
+
+\emph{IndoorAir}: Indoor air from the window's zone is passed through the window.
+
+\emph{OutdoorAir}: Outdoor air is passed through the window.
+
+\paragraph{Field: Airflow Destination}\label{field-airflow-destination}
+
+This is where the gap air goes after passing through the window. The choices are:
+
+\emph{IndoorAir}: The gap air goes to the indoor air of the window's zone.
+
+\emph{OutdoorAir}: The gap air goes to the outside air.
+
+\emph{ReturnAir}. The gap air goes to the return air for the window's zone. This choice is allowed only if Airflow Source = InsideAir. If the return air flow is zero, the gap air goes to the indoor air of the window's zone. If the sum of the gap airflow for all of the windows in a zone with Airflow Destination = ReturnAir exceeds the return airflow, then the difference between this sum and the return airflow goes to the indoor air.
+
+Figure~\ref{fig:gap-airflow-configurations-for-airflow} shows the allowed combinations of Airflow Source and Airflow Destination. The allowed combinations of Airflow Source and Airflow Destination are:
+
+IndoorAir -\textgreater{} OutdoorAir
+
+IndoorAir -\textgreater{} IndoorAir
+
+IndoorAir -\textgreater{} ReturnAir
+
+OutdoorAir -\textgreater{} IndoorAir
+
+OutdoorAir -\textgreater{} OutdoorAir
+
+\paragraph{Field: Maximum Flow Rate}\label{field-maximum-flow-rate-003}
+
+The maximum value of the airflow, in m\(^{3}\)/s per m of glazing width. The value is typically 0.006 to 0.009 m\(^{3}\)/s-m (4 to 6 cfm/ft).
+
+The airflow can be modulated by specifying Airflow Has Multiplier Schedule = Yes and giving the name of the Airflow Multiplier Schedule (see below).
+
+The fan energy used to move the air through the gap is generally very small and so is ignored.
+
+\paragraph{Field: Airflow Control Type}\label{field-airflow-control-type}
+
+Specifies how the airflow is controlled. The choices are:
+
+\emph{AlwaysOnAtMaximumFlow}. The airflow is always equal to Maximum Airflow.
+
+\emph{AlwaysOff}. The airflow is always zero.
+
+\emph{ScheduledOnly}. The airflow in a particular timestep equals Maximum Airflow times the value of the Airflow Multiplier Schedule for that timestep.
+
+\paragraph{Field: Airflow Is Scheduled}\label{field-airflow-is-scheduled}
+
+Specifies if the airflow is scheduled. The choices are:
+
+\emph{Yes}. The airflow is scheduled.
+
+\emph{No}. The airflow is not scheduled.
+
+If Yes, Airflow Multiplier Schedule Name is required.
+
+\paragraph{Field: Airflow Multiplier Schedule Name}\label{field-airflow-multiplier-schedule-name}
+
+The name of a schedule with values between 0.0 and 1.0. The timestep value of the airflow is Maximum Airflow times the schedule value. Required if Airflow Is Scheduled = Yes. Unused if Airflow Is Scheduled = No. This schedule should have a ScheduleType with Numeric Type = Continuous and Range = 0.0 : 1.0.
+
+\begin{figure}[hbtp] % fig 39
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image065.png}
+  \caption{Gap airflow configurations for airflow windows. (a) \textbf{Air exhaust window}: Airflow Source = InsideAir, Airflow Destination = OutsideAir; (b) \textbf{Indoor air curtain window}: Airflow Source = InsideAir, Airflow Destination = InsideAir; (c) \textbf{Air supply window}: Airflow Source = OutsideAir, Airflow Destination = InsideAir; (d) \textbf{Outdoor air curtain window}: Airflow Source = OutsideAir, Airflow Destination = OutsideAir; (e) \textbf{Airflow to Return Air}: Airflow Source = InsideAir, Airflow Destination = ReturnAir. Based on ``Active facades,'' Version no. 1, Belgian Building Research Institute, June 2002. \protect \label{fig:gap-airflow-configurations-for-airflow}}
+\end{figure}
+
+An IDF example: window with a constant airflow from inside to outside at 0.008 m\(^{3}\)/s-m.
+
+\begin{lstlisting}
+WindowProperty:AirflowControl,   !- Used to control forced airflow through a gap between glass layers
+      Zn001:Wall001:Win002,   !- Name of Associated Window
+      InsideAir,              !- Airflow Source
+      OutsideAir,             !- Airflow Destination
+      0.008,                  !- Maximum Airflow (m3/s per m of glazing width)
+      AlwaysOnAtMaxFlow,      !- Airflow Control Type
+      No,                     !- Airflow Has Multiplier Schedule?
+      ;                       !- Name of Airflow Multiplier Schedule
+\end{lstlisting}
+
+\subsection{WindowProperty:StormWindow}\label{windowpropertystormwindow}
+
+This object allows you to assign a movable exterior glass layer (``storm window'' or ``storm glass'') that is usually applied to a window in the winter to reduce heat loss and removed in the summer. A WindowProperty:StormWindow object is required for each window that has an associated storm window. It is assumed that:
+
+\begin{itemize}
+\item
+  When the storm glass is in place it is the outermost layer of the window, it covers only the glazed part of the window and not the frame, and it forms a tight seal. See Figure~\ref{fig:section-through-a-single-glazed-window}.
+\item
+  When the storm glass is not in place it is completely removed and has no effect on window heat transfer.
+\item
+  The gap between the storm glass and rest of the glazing is filled with air.
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 40
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image066.png}
+\caption{Section through a single-glazed window without (left) and with (right) a storm glass layer. Not to scale. \protect \label{fig:section-through-a-single-glazed-window}}
+\end{figure}
+
+With the addition of a storm window, single glazing effectively becomes double glazing, double glazing becomes triple glazing, etc.
+
+The presence of a storm window is indicated by the output variable ``Surface Storm Window On Off Status'' (see ``Window Output Variables''). This flag is \textbf{0} if the storm window is off, \textbf{1} if it is on, and \textbf{--1} if the window does not have an associated storm window.
+
+The program automatically creates a window construction (ref: Construction) that consists of the storm window glass layer and its adjacent air layer added to the original (unshaded, or ``bare'') window construction. In the eplusout.eio file this construction is called BARECONSTRUCTIONWITHSTORMWIN:\emph{n}, where \emph{n} is the number of the associated StormWin object. If the window has a shaded construction, the program creates a construction called SHADEDCONSTRUCTIONWITHSTORMWIN:\emph{n} that consists of the storm window glass layer and its adjacent air layer added to the original shaded window construction.
+
+The program also creates a WindowMaterial:Gas layer corresponding to the air layer adjacent to the storm glass. In the eplusout.eio file this layer is called AIR:STORMWIN:\emph{k}MM, where \emph{k} is the thickness of the air layer expressed as an integer number of millimeters.
+
+\subsubsection{Inputs}\label{inputs-35-001}
+
+\paragraph{Field: Window Name}\label{field-window-name-000}
+
+This is the name of a window (or glass door) to which the storm glass is applied. Not all windows can accept WindowProperty:StormWindow. The rules are:
+
+\begin{itemize}
+\item
+  The window must be an exterior window. WindowProperty:StormWindow is not applicable to interior (interzone) windows.
+\item
+  The window construction (without the storm glass layer) can have up to three glass layers.
+\item
+  If the window has an associated shaded construction (ref: WindowProperty:ShadingControl), that construction can have an interior shade or blind and up to three glass layers, or a between-glass shade or blind and two glass layers. The shaded construction cannot have an exterior shade or blind, cannot have a between-glass shade or blind and three glass layers, and cannot be switchable glazing.
+\item
+  The window cannot be an airflow window, i.e., a window that has an associated WindowProperty:AirflowControl.
+\end{itemize}
+
+\paragraph{Field: Storm Glass Layer Name}\label{field-storm-glass-layer-name}
+
+This is the name of a window glass material. Storm windows are assumed to consist of a single layer of glass. A storm window frame, if present, is ignored.
+
+\paragraph{Field: Distance Between Storm Glass Layer and Adjacent Glass}\label{field-distance-between-storm-glass-layer-and-adjacent-glass}
+
+The separation between the storm glass and the rest of the window (Figure~\ref{fig:section-through-a-single-glazed-window}). It is measured from the inside of the storm glass layer to the outside of the adjacent glass layer.
+
+\paragraph{Field: Month that Storm Glass Layer Is Put On}\label{field-month-that-storm-glass-layer-is-put-on}
+
+The number of the month (January = 1, February = 2, etc.) during which the storm window is put in place.
+
+\paragraph{Field: Day of Month that Storm Glass Layer Is Put On}\label{field-day-of-month-that-storm-glass-layer-is-put-on}
+
+The day of the month that the storm window is put in place. It is assumed that the storm window is put in place at the beginning of this day, i.e., during the first simulation timestep of the day, and remains in place until that month and day given by the following two fields.
+
+\paragraph{Field: Month that Storm Glass Layer Is Taken Off}\label{field-month-that-storm-glass-layer-is-taken-off}
+
+The number of the month (January = 1, February = 2, etc.) during which the storm window is removed.
+
+\paragraph{Field: Day of Month that Storm Glass Layer Is Taken Off}\label{field-day-of-month-that-storm-glass-layer-is-taken-off}
+
+The day of the month that the storm window is removed. It is assumed that the storm window is removed at the beginning of this day, i.e., during the first simulation timestep of the day, and stays off until the month and day given by Month that Storm Glass Layer Is Put On, Day of Month that Storm Glass Layer Is Put On.
+
+In the northern hemisphere, the month the storm window is put on is generally greater than the month it is taken off (for example put on in month 10, when it starts to get cold, and taken off in month 5, when it starts to warm up). In the southern hemisphere this is reversed: month on is less than month off.
+
+An IDF example of WindowProperty:StormWindow. The storm window is put in place on October 15 and removed on May 1.
+
+\begin{lstlisting}
+WindowProperty:StormWindow,
+   Window1, !- Name of Window to Which Storm Window Glass Layer is Applied
+   GlassA,  !- Name of Material:WindowGlass or MATERIAL:WindowGlass:AltInput that is the storm window layer
+   0.060,   !- Distance from storm window to adjacent glass (m)
+   10,      !- Month that Storm Window Is Put On
+   15,      !- Day of Month that Storm Window Is Put On
+   5,       !- Month that Storm Window Is Taken Off
+   1;       !- Day of Month that Storm Window Is Taken Off
+\end{lstlisting}
+
+\subsection{Importing Windows from WINDOW program}\label{importing-windows-from-window-program}
+
+\begin{callout}
+WINDOW v6.3 and later is capable of writing IDF excerpts for Window data. This is the preferred method as no external file is necessary. See the Tips document for details on obtaining the IDF excerpt.
+\end{callout}
+
+The WINDOW program calculates the U-value, Solar Heat Gain Coefficient, solar transmission/absorption characteristics, visible transmission characteristics and other properties of a window under standard indoor and outdoor conditions. WINDOW treats the whole window system---glazing, frame and divider. A sub-program of WINDOW called THERM uses a 2-D finite element calculation to determine the effective conductance of frame, divider and edge-of-glass elements. Another sub-program, OPTICS, determines the solar-optical properties of glazing, including laminates and coated glass.
+
+WINDOW can write a data file containing a description of the window that was analyzed. An example of this file (which is no longer the preferred method) is shown in the Tips document under WINDOW generated files. is shown below. This file, which can be named by the user, can be read by EnergyPlus. For more complete description and examples, see the object description -- Construction:WindowDataFile.
+
+In this way, the same window that was created in WINDOW can be imported into EnergyPlus for annual energy analysis without having to re-input the window data. To obtain WINDOW, THERM, or OPTICS go to http://windows.lbl.gov and choose the software link. A major advantage of using WINDOW to create window input for EnergyPlus is that you will have direct access to WINDOW's expanding database of over 1000 different glass types; and you will be able to browse through this database according to different criteria (color, transmittance, solar heat gain coefficient, etc.) to help you select the best glass type for your application.
+
+Although WINDOW writes only one window entry on the WINDOW data file, EnergyPlus users can combine two or more of these files to end up with a single data file with multiple window entries of different types. In this way a library of windows from WINDOW can be built up if so desired. If you combine files like this you should be sure not to leave out or change any of lines from the original files.
+
+There are four methods for inputting window constructions in EnergyPlus:
+
+\begin{enumerate}
+\tightlist
+\item
+  input full spectral data for each layer in the IDF,
+\item
+  input spectral average data for each layer in the IDF,
+\item
+  items 1 and 2 can be accomplished by reporting the IDF excerpt method from WINDOW
+\item
+  import WINDOW report containing layer-by-layer calculated values and overall glazing system angular values.
+\end{enumerate}
+
+\begin{callout}
+  \warning{Note: When using method 4, the overall glazing system angular dependent properties, including Tsol, Abs, Rfsol, Rbsol, Tvis, Rfvis, and Rbvis, are not used by EnergyPlus. Therefore, methods 1 and 2 and preferably 3 are recommended.}
+\end{callout}
+
+\begin{itemize}
+\item
+  The SHGC calculations in EnergyPlus for window layers input using full spectral data use a spectral weighting data set (derived from Optics5 data file ISO-9845GlobalNorm.std) that is different from the WINDOW default spectral weighting data set (W5\_NFRC\_2003.std). This difference accounts for most of the variation in SHGC values reported by EnergyPlus and WINDOW for full spectral data window layer input. This variation is more pronounced for window constructions of three glass layers or more.
+\item
+  Users intending to select a window construction based on SHGC value for energy code compliance should base their selection on the value reported by WINDOW since this is the officially recognized value.
+\end{itemize}
+
+In EnergyPlus, the Window data file is searched for each ``Construction:WindowDataFile'' object in the EnergyPlus input. This object has a very simple form:
+
+\begin{lstlisting}
+Construction:WindowDataFile,
+  ConstructionName,
+  FileName; ! Default is Window5DataFile.dat in the "run" folder.
+\end{lstlisting}
+
+If there is a window called ConstructionName on the Window data file, the data for that window is read from the file and the following EnergyPlus objects and their names are created. The ``W5'' prefixed to these names indicates that the object originated in the Window data file.
+
+\subsection{Zone Thermal Output(s)}\label{zone-thermal-outputs-1}
+
+In addition to the canned Surface reports (view the Reports section later in this document) and surface variables (above), the following variables are available for all zones:
+
+\begin{lstlisting}
+Zone,Sum,Zone Total Internal Radiant Heating Energy [J]
+Zone,Sum,Zone Total Internal Visible Radiation Heating Energy [J]
+Zone,Sum,Zone Total Internal Convective Heating Energy [J]
+Zone,Sum,Zone Total Internal Latent Gain Energy [J]
+Zone,Sum,Zone Total Internal Total Heating Energy [J]
+Zone,Average,Zone Mean Air Temperature [C]
+HVAC,Average,Zone Air Temperature [C]
+Zone,Average,Zone Mean Radiant Temperature [C]
+Zone,Average,Zone Operative Temperature [C]
+HVAC,Sum,Zone Air System Sensible Heating Energy [J]
+HVAC,Sum,Zone Air System Sensible Cooling Energy [J]
+HVAC,Average,Zone Air System Sensible Heating Rate [W]
+HVAC,Average,Zone Air System Sensible Cooling Rate [W]
+HVAC,Average,Zone Air Humidity Ratio[kgWater/kgDryAir]
+HVAC,Average,Zone Air Relative Humidity[%]
+\end{lstlisting}
+
+Two of these are of particular interest:
+
+\begin{lstlisting}
+Zone,Average,Zone Mean Air Temperature [C]
+HVAC,Average,Zone Air Temperature [C]
+\end{lstlisting}
+
+These two variable outputs are/should be identical. However, note that they can be reported at different time intervals. ``Zone Mean Air Temperature'' is only available on the Zone/HB timestep (Number of Timesteps per Hour) whereas ``Zone Air Temperature'' can be reported at the HVAC timestep (which can vary).
+
+\subsubsection{Zone Mean Air Temperature {[}C{]}}\label{zone-mean-air-temperature-c-1}
+
+From the code definition, the zone mean air temperature is the average temperature of the air temperatures at the system timestep. Remember that the zone heat balance represents a ``well stirred'' model for a zone, therefore there is only one mean air temperature to represent the air temperature for the zone.
+
+\subsubsection{Zone Air Temperature {[}C{]}}\label{zone-air-temperature-c-1}
+
+This is very similar to the mean air temperature in the last field. The ``well stirred'' model for the zone is the basis, but this temperature is also available at the ``detailed'' system timestep.
+
+\subsubsection{Zone Mean Radiant Temperature {[}C{]}}\label{zone-mean-radiant-temperature-c-1}
+
+The Mean Radiant Temperature (MRT) in degrees Celsius of a space is really the measure of the combined effects of temperatures of surfaces within that space. The larger the surface area and the closer one is to it, the more effect the surface temperature of that surface has on each other. The MRT is the measure of all these surface areas and temperatures.
+
+\subsubsection{Zone Operative Temperature {[}C{]}}\label{zone-operative-temperature-c-1}
+
+Zone Operative Temperature (OT) is the average of the Zone Mean Air Temperature (MAT) and Zone Mean Radiant Temperature (MRT), OT = 0.5*MAT + 0.5*MRT. This output variable is not affected by the type of thermostat controls in the zone, and does not include the direct effect of high temperature radiant systems.~ See also Zone Thermostat Operative Temperature.
+
+\subsubsection{Zone Air System Sensible Heating Energy {[}J{]}}\label{zone-air-system-sensible-heating-energy-j-1}
+
+This field represents the sensible heating energy in Joules that is actually supplied by the system to that zone for the timestep reported. This is the sensible heating rate multiplied by the simulation timestep. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module. This field is not multiplied by zone or group multipliers.
+
+\begin{callout}
+Zone Air System Sensible Heating (and Cooling) Energy (and Rate) all report the heating or cooling delivered by the HVAC system to a zone. These values are calculated by multiplying the supply air mass flow rate by the difference between the supply air temperature and the zone air temperature. This does not always indicate the operation of heating or cooling coils. For example, cooling will be reported if the supply air is cooled due to the introduction of outside air, even if all coils are off.
+
+Note that these variables are calculated at the system timestep. When reported at the ``detailed'' reporting frequency, these variable will never show heating and cooling both in the same system timestep. If reported at a frequency less than ``Detailed'' (for example, Hourly) values may appear in both the heating and cooling variable for the same hour if the system cooled the zone for part of the reporting period and heated the zone for another part of the reporting period.
+\end{callout}
+
+\subsubsection{Zone Air System Sensible Cooling Energy {[}J{]}}\label{zone-air-system-sensible-cooling-energy-j-1}
+
+This field represents the sensible cooling energy in Joules that is actually supplied by the system to that zone for the timestep reported. This is the sensible cooling rate multiplied by the simulation timestep. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air System Sensible Heating Rate {[}W{]}}\label{zone-air-system-sensible-heating-rate-w-1}
+
+This field represents the sensible heating rate in Watts that is actually supplied by the system to that zone for the timestep reported. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air System Sensible Cooling Rate {[}W{]}}\label{zone-air-system-sensible-cooling-rate-w-1}
+
+This field represents the sensible cooling rate in Watts that is actually supplied by the system to that zone for the timestep reported. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module. This field is not multiplied by zone or group multipliers.
+
+\subsubsection{Zone Air Humidity Ratio{[}kgWater/kgDryAir{]}}\label{zone-air-humidity-ratiokgwaterkgdryair}
+
+This field represents the air humidity ratio after the correct step for each zone. The humidity ratio is the mass of water vapor to the mass of dry air contained in the zone in (kg water/kg air) and is unitless.
+
+\subsubsection{Zone Air Relative Humidity{[}\%{]}}\label{zone-air-relative-humidity-1}
+
+This field represents the air relative humidity ratio after the correct step for each zone. The relative humidity is in percent and uses the Zone Air Temperature, the Zone Air Humidity Ratio and the Outside Barometric Pressure for calculation.
+
+\subsubsection{Zone Total Internal Radiant Heating Energy {[}J{]}}\label{zone-total-internal-radiant-heating-energy-j-1}
+
+This field represents the sum of radiant gains from specific internal sources (e.g.~equipment) throughout the zone in joules. This includes radiant gain from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
+
+\subsubsection{Zone-Total Internal Visible Heat Gain {[}J{]}}\label{zone-total-internal-visible-heat-gain-j}
+
+This field expresses the sum of heat gain in joules that is the calculated short wavelength radiation gain from lights in the zones. This calculation uses the total energy from lights and the fraction visible to realize this value, summed over the zones in the simulation.
+
+\subsubsection{Zone Total Internal Convective Heating Energy {[}J{]}}\label{zone-total-internal-convective-heating-energy-j-1}
+
+This field represents the sum of convective gains from specific sources (e.g.~equipment) throughout the zone in joules. This includes convective gain from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
+
+\subsubsection{Zone Total Internal Latent Gain Energy {[}J{]}}\label{zone-total-internal-latent-gain-energy-j-1}
+
+This field represents the sum of latent gains from specific internal sources (e.g.~equipment) throughout the zone in joules. This includes latent gain from People, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
+
+\subsubsection{Zone Total Internal Total Heating Energy {[}J{]}}\label{zone-total-internal-total-heating-energy-j-1}
+
+This field represents the sum of all heat gains throughout the zone in joules. This includes all heat gains from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
diff --git a/doc/input-output-reference/src/overview/group-unitary-equipment.tex b/doc/input-output-reference/src/overview/group-unitary-equipment.tex
new file mode 100644
index 00000000000..50eb4764359
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-unitary-equipment.tex
@@ -0,0 +1,3230 @@
+\section{Group -- Unitary Equipment}\label{group-unitary-equipment}
+
+\subsection{Furnace and Unitary Systems}\label{furnace-and-unitary-systems}
+
+The components
+
+\begin{itemize}
+\item
+  AirLoopHVAC:UnitarySystem
+\item
+  AirLoopHVAC:Unitary:Furnace:HeatOnly
+\item
+  AirLoopHVAC:Unitary:Furnace:HeatCool
+\item
+  AirLoopHVAC:UnitaryHeatOnly
+\item
+  AirLoopHVAC:UnitaryHeatCool
+\item
+  AirLoopHVAC:UnitaryHeatPump:AirToAir
+\item
+  AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed
+\end{itemize}
+
+are compound components usually placed in the primary air loop as the sole component. On the zone equipment side they are usually connected to one or more zones through uncontrolled terminal units (i.e., AirTerminal:SingleDuct:Uncontrolled objects). The maximum or design air flow rate through the furnace or unitary system should usually be set equal to the sum of the maximum air flow rates through the terminal unit objects. However, the simulation program can usually account for unequal air flows if the user wishes to model this scenario.
+
+The following HVAC equipment types are allowed in the air loop. The component matrix shows which coils and fans are allowed with which equipment models.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/AirLoopComponentMatrix.png}
+\caption{}
+\end{figure}
+
+\subsection{AirLoopHVAC:UnitarySystem}\label{airloophvacunitarysystem}
+
+The AirloopHVAC:UnitarySystem object is intended to replace all other air loop equipment, although other system types are still available. This system is unique in that it can accommodate all fan and coil types whereas other system types are specific to the type of fan and coil available for simulation. Additionally, although the AirloopHVAC:UnitarySystem is intended for use in the primary airloop, this object can be modeled as zone equipment (i.e., listed in a ZoneHVAC:EquipmentList) or as an outside air system component (i.e., listed in a AirLoopHVAC:OutdoorAirSystem:EquipmentList).
+
+The AirLoopHVAC:UnitarySystem object is a ``virtual'' component that consists of a fan component (OnOff, ConstantVolume, VariableVolume, or ComponentModel), a cooling coil component, a heating coil component, and a reheat coil as shown in Figure~\ref{fig:schematic-of-blow-through-heatcool-unitary}. When a draw through configuration is desired, the fan is placed directly after the heating coil. If dehumidification control is selected, a reheat coil component is also required. If the reheat coil is present and the dehumidification control type input is not specified as CoolReheat, the reheat coil will not be active. All of the fan and coil components are optional which allows the AirLoopHVAC:UnitarySystem object to be configured for fan-only, heating-only, cooling-only, or both heating and cooling. It may also be applied without a fan, controlling one or more coils, similar to the function of CoilSystem:Cooling:DX.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image294.png}
+\caption{Schematic of the EnergyPlus Unitary System \protect \label{fig:schematic-of-the-energyplus-unitary-system}}
+\end{figure}
+
+Links to the fan, cooling coil, heating coil and reheat coil specifications are provided in the unitary system input data syntax. In addition, the control zone name and the system design operating conditions are specified by the unitary system inputs.
+
+\subsubsection{Inputs}\label{inputs-049}
+
+\paragraph{Multi-Speed Fan and Water Coils In Unitary System}\label{multi-speed-fan-and-water-coils-in-unitary-system}
+
+Multi-speed fan chilled and hot water coils Air Handling Unit (AHU) can be modeled using Airloop Unitary System HVAC object (AirloopHVAC:UnitarySystem). AHU with chilled and hot water coils is setup by specifying Fan:OnOff and DesignSpecificationPerformance:MultiSpeed objects in Unitary System. The design specification performance object allows running the chilled and hot water coils capacity control using a multi-speed supply air fan. The multi-speed fan capacity control for chilled and hot water coil AHU is performed by modulating the supply air flow rate while maintaining a constant water flow rate. The chilled or hot water flow rates is set at maximum fixed flow rate when there is cooling or heating load and the water flow rate is set to zero when there is no load. Such control strategy is called two-position cooling or heating coil control. The fan speed selection depends on the current load, at lower load the fan is operated at minimum speed (Speed = 1) and the fan speed level increases progressively as the load increases until it reaches the maximum speed level specified. The multi-speed fan operation is modulated between the speeds to meet the current load. When the supply air fan is cycling between consecutive speeds levels, the speed ratio is calculated that indicates what fraction of the time step that the system run at the higher of the two speeds. At lower load, the fan may cycle on-off or run continuously depending the fan operating schedule specified. When the fan is cycling a part-load ratio is calculated to reflect the proportion of the system timestep the fan and coils were operating. In continuous fan operating mode only the coil cycles on-off and the part-load ratio applies to the coil only. Multi-speed fan capacity control is allowed with load based control type only.
+
+\paragraph{Field: Name}\label{field-name-048}
+
+This alpha field contains the identifying name for the unitary system.
+
+\paragraph{Field: Control Type}\label{field-control-type-004}
+
+This alpha field contains control type i.e.~load based or setpoint based for the unitary system. Valid choices are Load and SetPoint. Load control requires a Controlling Zone name and SetPoint control requires set points at each coil outlet node. A single set point at the outlet of the system is allowed but not recommended.
+
+\paragraph{Field: Controlling Zone or Thermostat Location}\label{field-controlling-zone-or-thermostat-location}
+
+This alpha field contains the identifying zone name where the thermostat controlling the unitary system is located.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-001}
+
+This alpha field contains the type of dehumidification control. The following options are valid for this field:
+
+\textbf{None} - meet sensible load only, no active dehumidification control
+
+\textbf{Multimode} - activate enhanced dehumidification mode as needed and meet sensible load. This option is used to model DX equipment with a controllable heat exchanger assisting the DX cooling coil for improved dehumidification. It is valid only with cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted.
+
+\textbf{CoolReheat} - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. If cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted, then the heat exchanger is assumed to always transfer energy between the cooling coil's inlet and outlet airstreams when the cooling coil is operating.
+
+The default is \textbf{None}. For the other dehumidification control modes, the maximum humidity setpoint is used. This must be set using a \textbf{ZoneControl:Humidistat} object. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate. If the dehumidification control type is specified as \textbf{CoolReheat}, then two additional inputs (reheat coil type and name) are also required as shown below. Although the reheat coil is required only when \textbf{CoolReheat} is selected, the optional reheat coil may be present for any of the allowed Dehumidification Control Types. If the reheat coil is present and the dehumidification control type is not specified as \textbf{CoolReheat}, the reheat coil will not be active,
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-017}
+
+This alpha field contains the schedule name which contains information on the availability of the unitary system to operate. A schedule value equal to 0 denotes that the unitary system must be off for that time period. A value greater than 0 denotes that the unitary system is available to operate during that time period. This schedule may be used to completely disable the unitary system as required. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Unitary System Air Inlet Node Name}\label{field-unitary-system-air-inlet-node-name}
+
+This alpha field contains the unitary system inlet node name.
+
+\paragraph{Field: Unitary System Air Outlet Node Name}\label{field-unitary-system-air-outlet-node-name}
+
+This alpha field contains the unitary system outlet node name.
+
+\paragraph{Field: Supply Fan Object Type}\label{field-supply-fan-object-type-000}
+
+This alpha field contains the identifying type of supply air fan specified for the unitary system. Fan type must be \textbf{Fan:OnOff,} \textbf{Fan:ConstantVolume, Fan:VariableVolume, or Fan:ComponentModel}. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e.~Supply Air Fan Operating Mode Schedule values are at times 0). Fan:VariableVolume is used for variable air volume systems or multi- or variable-speed coils. The Fan:ComponentModel may be used in place of the ConstantVolume or VariableVolume fan types to more accurately represent fan performance.
+
+\paragraph{Field: Supply Fan Name}\label{field-supply-fan-name}
+
+This alpha field contains the identifying name given to the unitary system fan.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice stands for ``blow through fan''. This means that the unit consists of a fan followed by the main cooling and heating coils and supplemental heating coil. The fan ``blows through'' the cooling and heating coils. The second choice stands for ``draw through fan''. This means that the unit consists of the main cooling/heating coil(s) followed by a fan, with the supplemental heater located at the outlet of the fan. The fan ``draws air through'' the cooling/heating coil(s). If this field is left blank, the default is blow through.
+
+\textbf{\emph{Field: Supply Air Fan Operating Mode Schedule Name}}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the unitary system supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-002}
+
+This alpha field contains the identifying type of heating coil specified in the unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. Allowable coil types are:
+
+\begin{itemize}
+\item
+  Coil:Heating:DX:SingleSpeed
+\item
+  Coil:Heating:DX:TwoSpeed
+\item
+  Coil:Heating:DX:MultiSpeed
+\item
+  Coil:Heating:DX:VariableSpeed
+\item
+  Coil:Heating:WaterToAirHeatPump:ParameterEstimation
+\item
+  Coil:Heating:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Gas:MultiStage
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Electric:MultiStage
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\item
+  Coil:Heating:Desuperheater
+\item
+  Coil:UserDefined
+\end{itemize}
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-002}
+
+This alpha field contains the identifying name given to the unitary system heating coil.
+
+\paragraph{Field: DX Heating Coil Sizing Ratio}\label{field-dx-heating-coil-sizing-ratio}
+
+This numeric field is used to adjust heat pump heating capacity with respect to DX cooling capacity. It is used only for DX heat pump configurations (i.e., a DX cooling and heating coil is used).
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-002}
+
+This alpha field contains the identifying type of cooling coil specified in the unitary system. Allowable coil types are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  Coil:Cooling:DX:SingleSpeed:ThermalStorage
+\item
+  Coil:Cooling:DX:TwoSpeed
+\item
+  Coil:Cooling:DX:MultiSpeed
+\item
+  Coil:Cooling:DX:VariableSpeed
+\item
+  Coil:Cooling:DX:TwoStageWithHumidityControlMode
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted
+\item
+  Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
+\item
+  Coil:Cooling:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit
+\item
+  Coil:Cooling:Water
+\item
+  Coil:Cooling:Water:DetailedGeometry
+\item
+  CoilSystem:Cooling:Water:HeatExchangerAssisted
+\item
+  Coil:UserDefined
+\end{itemize}
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-002}
+
+This alpha field contains the identifying name given to the unitary system cooling coil.
+
+\paragraph{Field: Use DOAS DX Cooling Coil}\label{field-use-doas-dx-cooling-coil}
+
+This input field eanbles DX Cooling coils to be used for 100\% outdoor air dedicated outdor air system applications. There are two choices Yes or No. If Yes, the DX coil is used as 100\% outdoor DX coil. If No, the DX coil is used as regular DX coil. This input file d is optional and the default is No.
+
+\paragraph{Field: DOAS DX Cooling Coil Leaving Minimum Air Temperature}\label{field-doas-dx-cooling-coil-leaving-minimum-air-temperature}
+
+This input field is DX Cooling coils leaving minimum air temperature for frost control. The DX cooling coil leaving air temperature is not allowed to exceed this minimum air temperature. The DX cooling coil frost controller adjusts or limits the desired coil outlet air setpoint temperature when the coil outlet temperature exceeds this minimum temperature limit specified. This input field is optional and only used along with in the input field above. The minimum and maximum values of this input field are 0.0\(^{o}\)C and 7.2\(^{o}\)C, and the default value is 2.0°C.
+
+\paragraph{Field: Latent Load Control}\label{field-latent-load-control}
+
+This alpha field defines the latent load control method. Available choices are SensibleOnlyLoadControl, LatentOnlyLoadControl, LatentWithSensibleLoadControl, or LatentOrSensibleLoadControl. The default choice is SensibleOnlyLoadControl. The SensibleOnlyLoadControl choice will operate to meet only a sensible load, and the LatentOnlyLoadConrol will operate to meet only a latent load. The LatentWithSensibleLoadControl will operate to meet the latent load only if there is a sensible load. The LatentOrSensibleLoadControl will operate to meet either a latent or sensible load.
+
+\paragraph{Field: Supplemental Heating Coil Object Type}\label{field-supplemental-heating-coil-object-type}
+
+This alpha field contains the identifying type of supplemental heating coil specified in the unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The Coil:UserDefined object must be configured as a heating coil. Supplemental heating type must be one of:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Desuperheater
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\item
+  Coil:UserDefined
+\end{itemize}
+
+\paragraph{Field: Supplemental Heating Coil Name}\label{field-supplemental-heating-coil-name}
+
+This alpha field contains the identifying name given to the unitary system reheat coil.
+
+\paragraph{Field: Cooling Supply Air Flow Rate Method}\label{field-cooling-supply-air-flow-rate-method-000}
+
+This alpha field defines the supply air flow method during cooling operation. Available choices are SupplyAirFlowRate, FlowPerFloorArea, FractionOfAutosizedCoolingValue, FlowPerCoolingCapacity. For each of the choices, a corresponding air flow rate for cooling must be specified.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-001}
+
+This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when the cooling coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Cooling Supply Air Flow Rate Method is \textbf{SupplyAirFlowRate}.
+
+\paragraph{Field: Cooling Supply Air Flow Rate Per Floor Area}\label{field-cooling-supply-air-flow-rate-per-floor-area}
+
+This numeric field defines the supply air flow rate per floor area leaving the unitary system in meters per second when the cooling coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Cooling Supply Air Flow Rate Method is \textbf{FlowPerFloorArea}.
+
+\paragraph{Field: Cooling Fraction of Autosized Design Cooling Supply Air Flow Rate}\label{field-cooling-fraction-of-autosized-design-cooling-supply-air-flow-rate}
+
+This numeric field defines the fraction of autosized supply air flow rate leaving the unitary system when the cooling coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Cooling Supply Air Flow Rate Method is \textbf{FractionOfAutosizedCoolingValue}.
+
+\paragraph{Field: Cooling Supply Air Flow Rate Per Unit of Capacity}\label{field-cooling-supply-air-flow-rate-per-unit-of-capacity}
+
+This numeric field defines the supply air flow rate per unit of capacity leaving the unitary system when the cooling coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Cooling Supply Air Flow Rate Method is \textbf{FlowPerCoolingCapacity}.
+
+\paragraph{Field: Heating Supply Air Flow Rate Method}\label{field-heating-supply-air-flow-rate-method-000}
+
+This alpha field defines the supply air flow method during heating operation. Available choices are SupplyAirFlowRate, FlowPerFloorArea, FractionOfAutosizedHeatingValue, FlowPerHeatingCapacity. For each of the choices, a corresponding air flow rate for heating must be specified.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-001}
+
+This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when the heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Heating Supply Air Flow Rate Method is \textbf{SupplyAirFlowRate}.
+
+\paragraph{Field: Heating Supply Air Flow Rate Per Floor Area}\label{field-heating-supply-air-flow-rate-per-floor-area}
+
+This numeric field defines the supply air flow rate per floor area leaving the unitary system in meters per second when the heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Heating Supply Air Flow Rate Method is \textbf{FlowPerFloorArea}.
+
+\paragraph{Field: Heating Fraction of Autosized Design Heating Supply Air Flow Rate}\label{field-heating-fraction-of-autosized-design-heating-supply-air-flow-rate}
+
+This numeric field defines the fraction of autosized supply air flow rate leaving the unitary system when the heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Heating Supply Air Flow Rate Method is \textbf{FractionOfAutosizedHeatingValue}.
+
+\paragraph{Field: Heating Supply Air Flow Rate Per Unit of Capacity}\label{field-heating-supply-air-flow-rate-per-unit-of-capacity}
+
+This numeric field defines the supply air flow rate per unit of capacity leaving the unitary system when the heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Heating Supply Air Flow Rate Method is \textbf{FlowPerHeatingCapacity}.
+
+\paragraph{Field: No Load Supply Air Flow Rate Method}\label{field-no-load-supply-air-flow-rate-method}
+
+This alpha field defines the supply air flow method when neither cooling or heating is required. Available choices are SupplyAirFlowRate, FlowPerFloorArea, FractionOfAutosizedCoolingValue, FractionOfAutosizedHeatingValue, FlowPerCoolingCapacity, FlowPerHeatingCapacity. For each of the choices, a corresponding air flow rate must be specified.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-000}
+
+This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when neither cooling or heating is required (i.e., main cooling/heating coils and supplemental heater are off but the supply air fan operates). This field is only used when the unitary system operating mode is specified as continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the unitary system operating mode is specified as continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the compressor was last operating (for cooling operation or heating operation).
+
+\paragraph{Field: No Load Supply Air Flow Rate Per Floor Area}\label{field-no-load-supply-air-flow-rate-per-floor-area}
+
+This numeric field defines the supply air flow rate per floor area leaving the unitary system in meters per second when neither cooling or heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when No Load Supply Air Flow Rate Method During is \textbf{FlowPerFloorArea}.
+
+\paragraph{Field: No Load Fraction of Autosized Cooling Supply Air Flow Rate}\label{field-no-load-fraction-of-autosized-cooling-supply-air-flow-rate}
+
+This numeric field defines the fraction of autosized supply air flow rate leaving the unitary system when neither cooling or heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when No Load Supply Air Flow Rate Method is \textbf{FractionOfAutosizedCoolingValue}.
+
+\paragraph{Field: No Load Fraction of Autosized Heating Supply Air Flow Rate}\label{field-no-load-fraction-of-autosized-heating-supply-air-flow-rate}
+
+This numeric field defines the fraction of autosized supply air flow rate leaving the unitary system when the neither cooling or heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when No Load Supply Air Flow Rate Method is \textbf{FractionOfAutosizedHeatingValue}.
+
+\paragraph{Field: No Load Supply Air Flow Rate Per Unit of Capacity During Cooling Operation}\label{field-no-load-supply-air-flow-rate-per-unit-of-capacity-during-cooling-operation}
+
+This numeric field defines the supply air flow rate per unit of capacity leaving the unitary system when neither cooling or heating is operating. Values must be greater than 0 or this field is autosizable. Required field when No Load Supply Air Flow Rate Method is \textbf{FlowPerCoolingCapacity}.
+
+\paragraph{Field: No Load Supply Air Flow Rate Per Unit of Capacity During Heating Operation}\label{field-no-load-supply-air-flow-rate-per-unit-of-capacity-during-heating-operation}
+
+This numeric field defines the supply air flow rate per unit of capacity leaving the unitary system when neither cooling or heating is operating. Values must be greater than 0 or this field is autosizable. Required field when No Load Supply Air Flow Rate Method is \textbf{FlowPerHeatingCapacity}.
+
+\paragraph{Field: Maximum Supply Air Temperature}\label{field-maximum-supply-air-temperature-000}
+
+This numeric field contains the design operating air outlet temperature in degrees C when the unitary system is heating. If this input field is left blank, the default value is 80 C.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-supplemental-heater-operation}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the heat pump supplemental heating coil is disabled.~ The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
+
+\paragraph{Field: Outdoor Dry-Bulb Temperature Sensor Node Name}\label{field-outdoor-dry-bulb-temperature-sensor-node-name}
+
+This alpha field specifies the name of the outdoor node which controls the operation of the supplemental heating coil. If this field is left blank, the outdoor temperature is based solely on the weather data. If this field is not blank, the node name specified must also be listed in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor temperature from the weather data. Alternately, the node name must be specified in an OutdoorAir:NodeList object where the outdoor temperature is taken directly from the weather data.
+
+\paragraph{Field: Maximum Cycling Rate}\label{field-maximum-cycling-rate-001}
+
+This numeric field contains the maximum on-off cycling rate for the compressor, which occurs at 50\% run time fraction. Suggested values are shown below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image295.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Heat Pump Time Constant}\label{field-heat-pump-time-constant-000}
+
+This numeric field contains the time constant for the cooling coil's capacity to reach steady state after startup. Suggested values are shown below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image296.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Fraction of On-Cycle Power Use}\label{field-fraction-of-on-cycle-power-use-000}
+
+This numeric field contains the fraction of on-cycle power use to adjust the part load fraction based on the off-cycle power consumption due to crankcase heaters, controls, fans, and etc. Suggested value values are below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image297.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Heat Pump Fan Delay Time}\label{field-heat-pump-fan-delay-time-000}
+
+This numeric field contains the time delay for the heat pump supply air fan to shut off after the compressor cycles off in seconds. This value can be obtained from the manufacturer or the heat pump catalog. Enter a value of zero when the heat pump's fan operating mode is continuous. Suggested value is 60 seconds.
+
+\paragraph{Field: Ancillary On-Cycle Electric Power}\label{field-ancillary-on-cycle-electric-power}
+
+This field defines ancillary electrical power (W) consumed during the on-cycle period (i.e., when the cooling or heating coil is operating). The model assumes that this ancillary power does not contribute to heating the supply air. The minimum value for this field is 0.0, and the default value is also 0.0 if the field is left blank.
+
+\paragraph{Field: Ancillary Off-Cycle Electric Power}\label{field-ancillary-off-cycle-electric-power}
+
+This field defines ancillary electrical power (W) consumed during the off-cycle period (i.e., when the cooling and heating coil are not operating). The model assumes that this ancillary power does not contribute to heating the supply air. The minimum value for this field is 0.0, and the default value is also 0.0 if the field is left blank.
+
+\paragraph{Field: Design Heat Recovery Water Flow Rate}\label{field-design-heat-recovery-water-flow-rate-001}
+
+This optional input field defines the design water flow rate used if the heat recovery option is being simulated. If this value is greater than 0.0 then a heat recovery loop must be specified and attached to the multispeed heat pump using the next 2 node fields. To determine how the heat recovery algorithm works, refer to the EnergyPlus Engineering Reference in the AirLoopHVAC:UnitarySystem with Heat Recovery section. The units for this input value are cubic meters per second.
+
+\paragraph{Field: Maximum Temperature for Heat Recovery}\label{field-maximum-temperature-for-heat-recovery}
+
+This field sets the maximum temperature (in degrees C) that this heat pump can produce for heat recovery. The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit. This temperature limit puts an upper bound on the recovered heat and limits the max temperature leaving the component.
+
+As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting. This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply.
+
+\paragraph{Field: Heat Recovery Water Inlet Node Name}\label{field-heat-recovery-water-inlet-node-name-000}
+
+This alpha field contains the identifying name for the heat recovery side inlet node.
+
+\paragraph{Field: Heat Recovery Water Outlet Node Name}\label{field-heat-recovery-water-outlet-node-name-000}
+
+This alpha field contains the identifying name for the heat recovery side outlet node.
+
+\paragraph{Field: Design Specification Multispeed Object Type}\label{field-design-specification-multispeed-object-type}
+
+This alpha field contains the identifying type for the design specification multispeed object. This field is only needed when multispeed cooling or heating coil is specified.
+
+\paragraph{Field: Design Specification Multispeed Object Name}\label{field-design-specification-multispeed-object-name}
+
+This alpha field contains the identifying name for the design specification multispeed object. This field is only needed when multispeed cooling or heating coil is specified.
+
+As shown in the example below, correct specification of the heat/cool unitary system requires specification of the following objects in addition to the unitary system object:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Fan (Fan:OnOff or Fan:ConstantVolume)
+\item
+  Cooling coil
+\item
+  Heating coil
+\item
+  Reheat coil
+\item
+  Direct air unit (AirTerminal:SingleDuct:Uncontrolled) for each zone served by the unitary system
+\end{enumerate}
+
+\begin{lstlisting}
+
+AirLoopHVAC:UnitarySystem,
+  DXAC Heat Pump 1,        !- Name
+  Load,                    !- Control Type
+  East Zone,               !- Controlling Zone or Thermostat Location
+  ,                        !- Dehumidification Control Type
+  FanAndCoilAvailSched,    !- Availability Schedule Name
+  Mixed Air Node,          !- Air Inlet Node Name
+  Air Loop Outlet Node,    !- Air Outlet Node Name
+  Fan:OnOff,               !- Supply Air Fan Object Type
+  Supply Fan 1,            !- Supply Air Fan Name
+  BlowThrough,             !- Fan Placement
+  FanModeSchedule,         !- Supply Air Fan Operating Mode Schedule Name
+  Coil:Heating:DX:MultiSpeed,  !- Heating Coil Object Type
+  Heat Pump DX Heating Coil 1, !- Heating Coil Name
+  ,                            !- DX Heating Coil Sizing Ratio
+  Coil:Cooling:DX:MultiSpeed,  !- Cooling Coil Object Type
+  Heat Pump ACDXCoil 1,    !- Cooling Coil Name
+  ,                        !- Use DOAS DX Cooling Coil
+  ,                        !- DOAS DX Cooling Coil Leaving Minimum Air Temperature
+  ,                        !- Latent Load Control
+  Coil:Heating:Gas,        !- Supplemental Heating Coil Object Type
+  Supp Gas Heating Coil 1, !- Supplemental Heating Coil Name
+  SupplyAirFlowRate,       !- Cooling Supply Air Flow Rate Method
+  1.7,                     !- Cooling Supply Air Flow Rate {m3/s}
+  ,                        !- Cooling Supply Air Flow Rate Per Floor Area
+  ,                        !- Cooling Fraction of Autosized Cooling Supply Air Flow Rate
+  ,                        !- Cooling Supply Air Flow Rate Per Unit of Cooling Capacity
+  SupplyAirFlowRate,       !- Heating Supply Air Flow Rate Method
+  1.7,                     !- Heating Supply Air Flow Rate {m3/s}
+  ,                        !- Heating Supply Air Flow Rate Per Floor Area
+  ,                        !- Heating Fraction of Autosized Heating Supply Air Flow Rate
+  ,                        !- Heating Supply Air Flow Rate Per Unit of Heating Capacity
+  SupplyAirFlowRate,       !- No Load Supply Air Flow Rate Method
+  0.2,                     !- No Load Supply Air Flow Rate {m3/s}
+  ,                        !- No Load Supply Air Flow Rate Per Floor Area
+  ,                        !- No Load Fraction of Autosized Cooling Supply Air Flow Rate
+  ,                        !- No Load Fraction of Autosized Heating Supply Air Flow Rate
+  ,                        !- No Load Supply Air Flow Rate Per Unit of Cooling Capacity
+  ,                        !- No Load Supply Air Flow Rate Per Unit of Heating Capacity
+  50,                      !- Maximum Supply Air Temperature {C}
+  21,  !- Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation
+  ,  !- Outdoor Dry-Bulb Temperature Sensor Node Name
+  ,  !- Maximum Cycling Rate
+  ,  !- Heat Pump Time Constant
+  ,  !- Fraction of On-Cycle Power Use
+  ,  !- Heat Pump Fan Delay Time
+  ,  !- Ancillary On-Cycle Electric Power
+  ,  !- Ancillary Off-Cycle Electric Power
+  ,  !- Design Heat Recovery Water Flow Rate
+  ,  !- Maximum Temperature for Heat Recovery (Maximum Heat Recovery Outlet Temperature?)
+  ,  !- Heat Recovery Water Inlet Node Name
+  ,  !- Heat Recovery Water Outlet Node Name
+  UnitarySystemPerformance:Multispeed,  !- Design Specification Multispeed Heat Pump Object Type
+  MyMultispeedHPSpec;  !- Design Specification Multispeed Heat Pump Object Name
+
+  UnitarySystemPerformance:Multispeed,
+  MyMultispeedHPSpec,      !- Name
+  4,                       !- Number of Speeds for Heating
+  4,                       !- Number of Speeds for Cooling
+  No,                      !- Single Mode Operation
+  0.235294118,             !- Heating Speed 1 Supply Air Flow Rate {m3/s}
+  0.235294118,             !- Cooling Speed 1 Supply Air Flow Rate {m3/s}
+  0.470588235,             !- Heating Speed 2 Supply Air Flow Rate {m3/s}
+  0.470588235,             !- Cooling Speed 2 Supply Air Flow Rate {m3/s}
+  0.705882353,             !- Heating Speed 3 Supply Air Flow Rate {m3/s}
+  0.705882353,             !- Cooling Speed 3 Supply Air Flow Rate {m3/s}
+  1.0,                     !- Heating Speed 4 Supply Air Flow Rate {m3/s}
+  1.0;                     !- Cooling Speed 4 Supply Air Flow Rate {m3/s}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-038}
+
+\begin{itemize}
+\item
+  HVAC,Average, Unitary System Fan Part Load Ratio {[]}
+\item
+  HVAC,Average, Unitary System Compressor Part Load Ratio
+\item
+  HVAC,Average,Unitary System Total Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Total Heating Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Latent Heating Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Ancillary Electric Power{[}W{]}
+\end{itemize}
+
+Two speed coil outputs
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Unitary System Cycling Ratio {[]}
+\end{itemize}
+
+Multi speed coil outputs
+
+\begin{itemize}
+\item
+  HVAC,Average,Unitary System DX Coil Cycling Ratio {[]}
+\item
+  HVAC,Average,Unitary System DX Coil Speed Ratio {[]}
+\item
+  HVAC,Average,Unitary System DX Coil Speed Level {[]}
+\item
+  HVAC,Average,Unitary System Electric Power{[}W{]}
+\item
+  HVAC,Sum,Unitary System Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Unitary System Cooling Ancillary Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Unitary System Heating Ancillary Electric Energy {[}J{]}
+\end{itemize}
+
+Multi speed coil outputs(If heat recovery is specified)
+
+\begin{itemize}
+\item
+  HVAC,Average, Unitary System Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Average, Unitary System Heat Recovery Inlet Temperature {[}C{]}
+\item
+  HVAC,Average, Unitary System Heat Recovery Outlet Temperature {[}C{]}
+\item
+  HVAC,Average, Unitary System Heat Recovery Fluid Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum, Unitary System Heat Recovery Energy {[}J{]}
+\end{itemize}
+
+Water to air heat pump outputs
+
+\begin{itemize}
+\item
+  HVAC,Average, Unitary System Requested Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average, Unitary System Requested Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Average, Unitary System Requested Heating Rate {[}W{]}
+\item
+  HVAC,Average, Unitary System Water Coil Cycling Ratio {[]}
+\item
+  HVAC,Average, Unitary System Water Coil Speed Ratio {[]}
+\item
+  HVAC,Average, Unitary System Water Coil Speed Level {[]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Unitary System Fan Part Load Ratio {[]}}{Unitary System Fan Part Load Ratio }}\label{unitary-system-fan-part-load-ratio}
+
+This output variable is the ratio of actual air mass flow rate through the unitary system to the unitary system's design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the unitary system is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating (or cooling) load to the steady-state unitary system heating (or cooling) capacity. For the cycling fan mode, the runtime fraction for the unitary system fan may be different from the fan part-load ratio reported here due the part-load performance of the unitary system's heating (or cooling) coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff). When the speed number is greater than 1, the value is 1.0.
+
+\paragraph{\texorpdfstring{Unitary System Compressor Part Load Ratio {[]}}{Unitary System Compressor Part Load Ratio }}\label{unitary-system-compressor-part-load-ratio}
+
+This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the unitary system's DX heating or cooling coil at Speed 1. The runtime fraction for the unitary system compressor may be different from the compressor part-load ratio reported here due the part-load performance of the heating/cooling coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate. When the speed number is greater than 1, the value is 1.0.
+
+\paragraph{\texorpdfstring{Unitary System DX Coil Cycling Ratio {[]}}{Unitary System DX Coil Cycling Ratio }}\label{unitary-system-dx-coil-cycling-ratio}
+
+This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the unitary system's DX heating or cooling coil (Speed 1) for the entire system timestep. The value is between 0.0 and 1.0 when the unitary system is cycling on and off its lowest speed (Speed 1) and 1.0 when the unitary system operates at speeds above 1.
+
+When Single Mode Operation is specified, the value is between 0.0 and 1.0 when the heat pump is cycling on at any given speed.
+
+\paragraph{\texorpdfstring{Unitary System DX Coil Speed Ratio {[]}}{Unitary System DX Coil Speed Ratio }}\label{unitary-system-dx-coil-speed-ratio}
+
+This output variable is the ratio of time in a system timestep that the compressor is at rated speed between two consecutive speed numbers ( {[}Compressor Speed - Compressor speed at Speed i-1{]} / {[}Compressor speed at Speed i - Compressor speed at Speed i-1{]}). The compressor speed ratio reports (1.0 is max, 0.0 is min) and any value in between as it is averaged over the timestep. The value is 0.0 during Speed 1 operation.
+
+The physical meaning of the speed ratio is dependent on the compressor configuration defined in the field of child coil object: Apply Part Load Fraction to Speeds greater than 1. The allowed choice is either Yes or No. When No is entered, one compressor is assumed for all speeds. ~The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the lower speed runs in the rest of the system timestep. When Yes is entered, multiple compressors are assumed, and each compressor has associated speed. The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the low speed runs in a whole system timestep.
+
+When Single Mode Operation is specified, the speed ratio is set to 0 at Speed 1 and 1 at Speed \textgreater{} 1.
+
+\paragraph{\texorpdfstring{Unitary System DX Coil Speed Level {[]}}{Unitary System DX Coil Speed Level }}\label{unitary-system-dx-coil-speed-level}
+
+This output variable reports the maximum speed needed when the unitary system operates to meet the sensible load (heating or cooling) in a system timestep. When the value is 1, the unitary system operates at Speed 1 (lowest speed). For this case the cycling ratio is between 0.0 and 1.0, while the speed ratio is 0.0. When the speed number output variable is above one, such as i, the unitary system operation is determined by the speed ratio through linear interpolation. For example, when the speed ratio is 0.4 and the speed number is 3, the unitary system operates at Speed 3 for 40\% of a system timestep and at Speed 2 for 60\% of a system timestep for a single compressor. For multiple compressors, the unitary system operates at Speed 3 in the 40\% of a system timestep and at Speed 2 in the whole system timestep.
+
+\paragraph{Unitary System Total Heating Rate {[}W{]}}\label{unitary-system-total-heating-rate-w}
+
+This output field is the total (enthalpy) heat addition rate of the unitary system to the zones it is serving in Watts. This value is calculated using the enthalpy difference of the unitary system outlet air and inlet air streams, and the air mass flow rate through the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Total Cooling Rate {[}W{]}}\label{unitary-system-total-cooling-rate-w}
+
+This output field is the total (enthalpy) heat extraction rate of the unitary system from the zones it is serving in Watts. This value is calculated using the enthalpy difference of the unitary system outlet air and inlet air streams, and the air mass flow rate through the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Sensible Heating Rate {[}W{]}}\label{unitary-system-sensible-heating-rate-w}
+
+This output field reports the sensible heat addition rate of the unitary system to the zones it is serving in Watts. This value is calculated using the enthalpy difference of the unitary system outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Sensible Cooling Rate {[}W{]}}\label{unitary-system-sensible-cooling-rate-w}
+
+This output field reports the moist air sensible heat extraction rate of the unitary system from the zones it is serving in Watts. This value is calculated using the enthalpy difference of the unitary system outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Latent Heating Rate {[}W{]}}\label{unitary-system-latent-heating-rate-w}
+
+This output field is the latent heat addition (humidification) rate of the unitary system in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Latent Cooling Rate {[}W{]}}\label{unitary-system-latent-cooling-rate-w}
+
+This output field is the latent heat extraction (dehumidification) rate of the unitary system in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Electric Power {[}W{]}}\label{unitary-system-electric-power-w}
+
+This output field is the electricity consumption rate of the unitary system in Watts. The consumption includes electricity used by the DX coils (including crankcase heater if the fuel type is electricity), fans (indoor supply air fan and the condenser fans associated with the DX coil{[}s{]}), auxiliary power during on and off period, and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported. Any non-electric energy use is not reported by the unitary system object but is reported in the associated coil objects as appropriate.
+
+\paragraph{Unitary System Electric Energy {[}J{]}}\label{unitary-system-electric-energy-j}
+
+This output field is the electricity consumption of the unitary system in Joules for the timestep being reported. The consumption includes electricity used by the DX compressor (including crankcase heater if the fuel type is electricity), fans (indoor supply air fan and the condenser fans associated with the DX coil{[}s{]}), auxiliary power during on and off period, and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are summed for the timestep being reported. Any non-electric energy use is not reported by the unitary system object but is reported in the associated coil objects as appropriate.
+
+\paragraph{Unitary System Ancillary Electric Power {[}W{]}}\label{unitary-system-ancillary-electric-power-w}
+
+This output field is the average auxiliary electricity consumption rate (including both on-cycle and off-cycle) in Watts for the timestep being reported.
+
+\paragraph{Unitary System Cooling Ancillary Electric Energy {[}J{]}}\label{unitary-system-cooling-ancillary-electric-energy-j}
+
+This is the auxiliary electricity consumption in Joules for the timestep being reported. This is the auxiliary electricity consumption during periods when the unitary system is providing cooling (DX cooling coil is operating). This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Unitary System Heating Ancillary Electric Energy {[}J{]}}\label{unitary-system-heating-ancillary-electric-energy-j}
+
+This is the auxiliary electricity consumption in Joules for the timestep being reported. This is the auxiliary electricity consumption during periods when the unitary system is providing heating (DX heating coil is operating). This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Unitary System Heat Recovery Inlet Temperature {[}C{]}}\label{unitary-system-heat-recovery-inlet-temperature-c}
+
+\paragraph{Unitary System Heat Recovery Outlet Temperature {[}C{]}}\label{unitary-system-heat-recovery-outlet-temperature-c}
+
+\paragraph{Unitary System Heat Recovery Fluid Mass Flow Rate {[}kg/s{]}}\label{unitary-system-heat-recovery-fluid-mass-flow-rate-kgs}
+
+These outputs are the heat recovery inlet and outlet temperatures and water mass flow rate for unitary systems with heat recovery.
+
+\paragraph{Unitary System Heat Recovery Rate {[}W{]}}\label{unitary-system-heat-recovery-rate-w}
+
+\paragraph{Unitary System Heat Recovery Energy {[}J{]}}\label{unitary-system-heat-recovery-energy-j}
+
+For multispeed unitary systems with heat recovery, these outputs are the recoverable energy rate (in Watts) and energy (in Joules).
+
+\paragraph{Unitary System Requested Sensible Cooling Rate {[}W{]}}\label{unitary-system-requested-sensible-cooling-rate-w}
+
+This output variable is the sensible cooling requested from the zone thermostat in watts. This value is calculated using the unitary system outlet air and zone conditions, the specific heat of the zone air, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{Unitary System Requested Latent Cooling Rate {[}W{]}}\label{unitary-system-requested-latent-cooling-rate-w}
+
+This output variable is the latent cooling requested from the zone humidistat in watts. This value is calculated using the unitary system outlet air and zone conditions, the heat of vaporization of water at the current zone conditions, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{Unitary System Requested Heating Rate {[}W{]}}\label{unitary-system-requested-heating-rate-w}
+
+This output variable is the sensible heating requested from the zone thermostat in watts. This value is calculated using the unitary system outlet air and zone conditions, the specific heat of the zone air, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{\texorpdfstring{Unitary System Water Coil Cycling Ratio {[]}}{Unitary System Water Coil Cycling Ratio }}\label{unitary-system-water-coil-cycling-ratio}
+
+This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the multispeed fan chilled water or hot water coil for the entire system timestep. The value is between 0.0 and 1.0 when the AHU is cycling on and off its lowest speed (fan speed 1) and 1.0 when the multispeed fan chilled water or hot water AHU operates at speed levels above 1.
+
+\paragraph{\texorpdfstring{Unitary System Water Coil Speed Ratio {[]}}{Unitary System Water Coil Speed Ratio }}\label{unitary-system-water-coil-speed-ratio}
+
+This output variable is the ratio of time in a system timestep that the AHU fan is at rated speed between two consecutive speed levels ( {[}System Load -- Capacity at Fan Speed i-1{]} / {[}Capacity at Fan Speed i -- Capacity at Fan Speed i-1{]}). The fan speed ratio reports (1.0 is max, 0.0 is min) and any value in between as it is averaged over the timestep. The value is 0.0 during Speed 1 operation. AHU speed ratio depends on the system load and the supply air fan speed. The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the lower speed runs in the rest of the system timestep.
+
+\paragraph{\texorpdfstring{Unitary System Water Coil Speed Level {[]}}{Unitary System Water Coil Speed Level }}\label{unitary-system-water-coil-speed-level}
+
+This output variable reports the maximum speed needed when the system operates to meet the sensible load (heating or cooling) in a system timestep. When the value is 1, the AHU operates at Speed 1 (lowest speed). For this case the cycling ratio is between 0.0 and 1.0, while the speed ratio is 0.0. When the speed level is above the minimum (speed = 1), the system operation is determined by the speed ratio. For example, when the speed ratio is 0.4 and the speed lever is 3, then the supply air fan and water coil operate at Speed 3 for 40\% of a system timestep and at Speed 2 for 60\% of a system timestep.
+
+\subsection{UnitarySystemPerformance:Multispeed}\label{unitarysystemperformancemultispeed}
+
+\subsubsection{Inputs}\label{inputs-1-046}
+
+\paragraph{Field: Name}\label{field-name-1-045}
+
+This alpha field contains the identifying name for the multispeed performance specification.
+
+\paragraph{Field: Number of Speeds for Heating}\label{field-number-of-speeds-for-heating}
+
+This field defines the number of heating speeds for the heat pump, and must match the number of heating speeds defined in the associated heating coil. The value for this input field defines the number of airflow rate ratios that must be defined for heating in the fields below. The minimum value for this field is one and the maximum value is the number specified in the coil object. If the heating coil type used in the unitary system object is not a multispeed coil type, then this field should be 1.
+
+\paragraph{Field: Number of Speeds for Cooling}\label{field-number-of-speeds-for-cooling-000}
+
+This field defines the number of cooling speeds for the heat pump, and must match the number of cooling speeds defined in the associated DX cooling coil. The value for this input field defines the number of airflow rate ratios that must be defined for cooling in the fields below. The minimum value for this field is one and the maximum value is the number specified in the coil object. If the cooling coil type used in the unitary system object is not a multispeed coil type, then this field should be 1.
+
+\paragraph{Field: Single Mode Operation}\label{field-single-mode-operation}
+
+This field specifies the coil operation mode for multiple speed DX cooling and heating coils during each HVAC timestep. The allowed choice is Yes or No. The No choice allows a coil works between two adjacent speeds when a system load is greater than the coil capacity at speed 1. The Yes choice allows a coil works with a single capacity at a different speed. The speed number is determined by a system load.
+
+The allowed cooling and heating coil types are restricted to the following combinations:
+
+Coil:Cooling:DX:MultiSpeed and Coil:Heating:DX:MultiSpeed or Coil:Cooling:DX:MultiSpeed and Coil:Heating:Gas. 
+
+\paragraph{Field: Heating Speed 1 Supply Air Flow Ratio}\label{field-heating-speed-1-supply-air-flow-ratio}
+
+This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the heating coil and/or supplemental heater are operating at Speed 1 (lowest speed). Values must be greater than 0.
+
+\paragraph{Field: Cooling Speed 1 Supply Air Flow Ratio}\label{field-cooling-speed-1-supply-air-flow-ratio}
+
+This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the DX cooling coil is operating at Speed 1 (lowest speed). Values must be greater than 0.
+
+\paragraph{Field: Heating Speed 2 Supply Air Flow Ratio}\label{field-heating-speed-2-supply-air-flow-ratio}
+
+This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the heating coil and/or supplemental heater are operating at Speed 2. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for heating speed 1.
+
+\paragraph{Field: Cooling Speed 2 Supply Air Flow Ratio}\label{field-cooling-speed-2-supply-air-flow-ratio}
+
+This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the DX cooling coil is operating at Speed 2. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for cooling speed 1.
+
+\paragraph{Field: Heating Speed 3 Supply Air Flow Ratio}\label{field-heating-speed-3-supply-air-flow-ratio}
+
+This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the heating coil and/or supplemental heater are operating at Speed 3. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for heating speed 2.If the `Number of Speeds for Heating' is less than 3, then this field can be left blank.
+
+\paragraph{Field: Cooling Speed 3 Supply Air Flow Ratio}\label{field-cooling-speed-3-supply-air-flow-ratio}
+
+This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the DX cooling coil is operating at Speed 3. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for cooling speed 2.If the `Number of Speeds for Cooling' is less than 3, then this field can be left blank.
+
+\paragraph{Field: Heating Speed 4 Supply Air Flow Ratio}\label{field-heating-speed-4-supply-air-flow-ratio}
+
+This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the DX heating coil and/or supplemental heater are operating at Speed 3. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for heating Speed 3.If the `Number of Speeds for Heating' is less than 4, then this field can be left blank.
+
+\paragraph{Field: Cooling Speed 4 Supply Air Flow Ratio}\label{field-cooling-speed-4-supply-air-flow-ratio}
+
+This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the DX cooling coil is operating at Speed 4. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for cooling Speed 3.If the `Number of Speeds for Cooling' is less than 4, then this field can be left blank.
+
+\subsection{AirLoopHVAC:Unitary:Furnace:HeatCool}\label{airloophvacunitaryfurnaceheatcool}
+
+The heat/cool furnace is a ``virtual'' component that consists of a fan component (OnOff or ConstantVolume), a DX cooling coil component, and a Gas or Electric heating coil component. The blow through furnace configuration is shown in Figure~\ref{fig:schematic-of-energyplus-heatcool-furnace} below. When a draw through furnace configuration is desired, the fan is placed directly after the heating coil. If the dehumidification control type is specified as CoolReheat, a reheat coil component is also required. If the reheat coil is present and the dehumidification control type input is not specified as CoolReheat, the reheat coil will not be active,
+
+\begin{figure}[hbtp] % fig 116
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image298.png}
+\caption{Schematic of EnergyPlus Heat/Cool Furnace \protect \label{fig:schematic-of-energyplus-heatcool-furnace}}
+\end{figure}
+
+Note: the coil order shown here has been revised from previous versions (prior to V4.0) of Energyplus to configure the cooling coil upstream of the heating coil. This configuration provides uniformity with all unitary equipment. However, for unitary HeatCool systems that do not use a reheat coil, the heating coil can also be placed upstream of the cooling coil. This optional coil placement is retained to allow compatibility with previous versions of Energyplus. For input files developed using previous versions of Energyplus, it is recommended that the coil order be revised according to the figure above.
+
+Links to the fan, heating coil, DX cooling coil and optional reheat coil specifications are provided in the furnace input data syntax. In addition, the control zone name and the furnace design operating conditions are specified by the furnace inputs.
+
+\subsubsection{Inputs}\label{inputs-2-043}
+
+\paragraph{Field: Name}\label{field-name-2-040}
+
+This alpha field contains the identifying name for the unit.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-012}
+
+This alpha field contains the schedule name which contains information on the availability of the furnace to operate. A schedule value equal to 0 denotes that the furnace must be off for that time period. A value greater than 0 denotes that the furnace is available to operate during that time period. This schedule may be used to completely disable the furnace as required. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Furnace Air Inlet Node Name}\label{field-furnace-air-inlet-node-name}
+
+This alpha field contains the furnace inlet node name.
+
+\paragraph{Field: Furnace Air Outlet Node Name}\label{field-furnace-air-outlet-node-name}
+
+This alpha field contains the furnace outlet node name.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the furnace supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.
+
+\paragraph{Field: Maximum Supply Air Temperature}\label{field-maximum-supply-air-temperature-1-000}
+
+This numeric field contains the design operating furnace air outlet temperature in degrees C when the furnace is heating. If this input field is left blank, the default value is 80 C.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-1-000}
+
+This numeric field defines the supply air flow rate leaving the furnace in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-1-000}
+
+This numeric field defines the supply air flow rate leaving the furnace in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-1-000}
+
+This numeric field defines the supply air flow rate leaving the furnace in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the furnace operating mode is specified as continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the furnace operating mode is specified as continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the compressor was last operating (for cooling operation or heating operation).
+
+\paragraph{Field: Controlling Zone or Thermostat Location}\label{field-controlling-zone-or-thermostat-location-1}
+
+This alpha field contains the identifying zone name where the thermostat controlling the furnace is located.
+
+\paragraph{Field: Supply Fan Object Type}\label{field-supply-fan-object-type-1}
+
+This alpha field contains the identifying type of supply air fan specified for the furnace. Fan type must be \textbf{Fan:OnOff} or \textbf{Fan:ConstantVolume}. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e.~Supply Air Fan Operating Mode Schedule values are at times 0).
+
+\paragraph{Field: Supply Fan Name}\label{field-supply-fan-name-1}
+
+This alpha field contains the identifying name given to the furnace fan.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-1}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice stands for ``blow through fan''. This means that the unit consists of a fan followed by the DX coils and supplemental heating coil. The fan ``blows through'' the cooling and heating coils. The second choice stands for ``draw through fan''. This means that the unit consists of the DX coil(s) followed by a fan, with the supplemental heater located at the outlet of the fan. The fan ``draws air through'' the DX coil(s). If this field is left blank, the default is blow through.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-1-000}
+
+This alpha field contains the identifying type of heating coil specified in the furnace. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat and Cool Furnace) itself provides the ``controller'' function of modulating water flow. Allowable coil types are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-1-000}
+
+This alpha field contains the identifying name given to the furnace heating coil.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-1-000}
+
+This alpha field contains the identifying type of cooling coil specified in the furnace. Only allowable coil types are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted
+\item
+  Coil:Cooling:DX:VariableSpeed
+\end{itemize}
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-1-000}
+
+This alpha field contains the identifying name given to the furnace cooling coil.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-1-000}
+
+This alpha field contains the type of dehumidification control. The following options are valid for this field:
+
+\begin{itemize}
+\item
+  \textbf{None} - meet sensible load only, no active dehumidification control
+\item
+  \textbf{Multimode} - activate enhanced dehumidification mode as needed and meet sensible load. This option is used to model DX equipment with a controllable heat exchanger assisting the DX cooling coil for improved dehumidification. It is valid only with cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted.
+\item
+  \textbf{CoolReheat} - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. If cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted, then the heat exchanger is assumed to always transfer energy between the cooling coil's inlet and outlet airstreams when the cooling coil is operating.
+\end{itemize}
+
+The default is \textbf{None}. For the other dehumidification control modes, the maximum humidity setpoint is used. This must be set using a \textbf{ZoneControl:Humidistat} object. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate. If the dehumidification control type is specified as \textbf{CoolReheat}, then two additional inputs (reheat coil type and name) are also required as shown below. Although the reheat coil is required only when \textbf{CoolRheat} is selected, the optional reheat coil may be present for any of the allowed Dehumidification Control Types. If the reheat coil is present and the dehumidification control type is not specified as \textbf{CoolReheat}, the reheat coil will not be active,
+
+\paragraph{Field: Reheat Coil Object Type}\label{field-reheat-coil-object-type-000}
+
+This alpha field contains the identifying type of reheat coil specified in the furnace. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the reheat coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat and Cool Furnace) itself provides the ``controller'' function of modulating water flow. Reheat coil type must be one of:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Desuperheater
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Reheat Coil Name}\label{field-reheat-coil-name-000}
+
+This alpha field contains the identifying name given to the furnace reheat coil.
+
+As shown in the example below, correct specification of the heat/cool furnace requires specification of the following objects in addition to the furnace object:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  fan (Fan:OnOff or Fan:ConstantVolume)
+\item
+  cooling coil (Coil:Cooling:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted)
+\item
+  heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
+\item
+  reheat coil (optional, Coil:Heating:Gas, Coil:Heating:Electric, or Coil:Heating:Desuperheater)
+\item
+  terminal unit (AirTerminal:SingleDuct:Uncontrolled) for each zone served by the furnace
+\end{enumerate}
+
+Note: the furnace's fan, cooling coil, heating coil and optional reheat coil must be connected in the air loop according to the configuration shown above (Figure~\ref{fig:schematic-of-energyplus-heatcool-furnace}) when CoolReheat is selected as the dehujmidificaiton control type. In addition, the volumetric air flow rate specified in the terminal air unit for the controlling zone should properly reflect the fractional volumetric air flow rate specified in the furnace object.
+
+\begin{lstlisting}
+
+AirLoopHVAC:Unitary:Furnace:HeatCool,
+  GasHeat DXAC Furnace 1, !- Name of furnace
+  FanAndCoilAvailSched,   !- Availability schedule
+  Air Loop Inlet Node,    !- Furnace inlet node name
+  Air Loop Outlet Node,   !- Furnace outlet node name
+  CycFanSchedule,         !- Supply Air Fan Operating Mode Schedule Name
+  80,                     !- Maximum supply air temperature from furnace heater {C}
+  1.3,                    !- Cooling Supply Air Flow Rate {m3/s}
+  1.3,                    !- Heating Supply Air Flow Rate {m3/s}
+  0.0,                    !- No Load Supply Air Flow Rate {m3/s}
+  East Zone,              !- Controlling zone or thermostat location
+  Fan:OnOff,              !- Supply fan type
+  Supply Fan 1,           !- Supply fan name
+  BlowThrough,            !- Fan Placement
+  Coil:Heating:Gas,       !- Heating coil type
+  Furnace Heating Coil 1, !- Heating coil name
+  Coil:Cooling:DX:SingleSpeed,  !- Cooling coil type
+  Furnace ACDXCoil 1,     !- Cooling coil name
+  None;                   !- Dehumidificatioin Control Type
+
+
+  Coil:Heating:Gas,
+      Furnace Heating Coil 1,         !- Coil Name
+      FanAndCoilAvailSched,           !- Availability Schedule Name
+      0.8,    !- Gas Burner Efficiency of the Coil
+      25000,  !- Nominal Capacity of the Coil {W}
+      Heating Coil Air Inlet Node,    !- Coil\_Air\_Inlet\_Node
+      Air Loop Outlet Node;           !- Coil\_Air\_Outlet\_Node
+
+    Coil:Cooling:DX:SingleSpeed,
+      Furnace ACDXCoil 1,    !- Coil Name
+      FanAndCoilAvailSched,  !- Availability Schedule
+      25000,  !- Rated Total Cooling Capacity (gross) {W}
+      0.75,   !- Rated SHR
+      3.0,    !- Rated COP
+      1.3,    !- Rated Air Volume Flow Rate {m3/s}
+      DX Cooling Coil Air Inlet Node, !- Coil Air Inlet Node
+      Heating Coil Air Inlet Node,    !- Coil Air Outlet Node
+      WindACCoolCapFT,  !- Total Cooling Capacity Modifier Curve (function of temperature)
+      WindACCoolCapFFF, !- Total Cooling Capacity Modifier Curve (function of flow fraction)
+      WindACEIRFT,      !- Energy Input Ratio Modifier Curve (function of temperature)
+      WindACEIRFFF,     !- Energy Input Ratio Modifier Curve (function of flow fraction)
+      WindACPLFFPLR,    !- Part Load Fraction Correlation (function of part load ratio)
+      CyclingFanAndCompressor;    !- Supply Air Fan Operation Mode
+
+    Fan:OnOff,
+      Supply Fan 1,                !- Fan Name
+      FanAndCoilAvailSched,        !- Availability Schedule Name
+      0.7,    !- Fan Total Efficiency
+      600.0,  !- Delta Pressure {Pa}
+      1.3,    !- Max Flow Rate {m3/s}
+      0.9,    !- Motor Efficiency
+      1.0,    !- Motor In Airstream Fraction
+      Air Loop Inlet Node,         !- Fan\_Inlet\_Node
+      DX Cooling Coil Air Inlet Node; !- Fan\_Outlet\_Node
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone1DirectAir,        !- Direct Air Name
+      FanAndCoilAvailSched,  !- Schedule name for on/off schedule
+      Zone 1 Inlet Node,     !- Zone Supply Air Node Name
+     0.47;  !- Maximum air flow rate {m3/s}
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone2DirectAir,        !- Direct Air Name
+      FanAndCoilAvailSched,  !- Schedule name for on/off schedule
+      Zone 2 Inlet Node,     !- Zone Supply Air Node Name
+      0.36;  !- Maximum air flow rate {m3/s}
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone3DirectAir,        !- Direct Air Name
+      FanAndCoilAvailSched,  !- Schedule name for on/off schedule
+      Zone 3 Inlet Node,     !- Zone Supply Air Node Name
+     0.47;  !- Maximum air flow rate {m3/s}
+\end{lstlisting}
+
+~Example of Heat/Cool Furnace Specification
+
+\subsubsection{Outputs}\label{outputs-1-029}
+
+HVAC,Average,Unitary System Fan Part Load Ratio {[]}
+
+HVAC,Average,Unitary System Compressor Part Load Ratio {[]}
+
+\paragraph{Unitary System Fan Part Load Ratio}\label{unitary-system-fan-part-load-ratio-1}
+
+This output variable is the ratio of actual air mass flow rate through the furnace to the furnace's design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the furnace is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating (or cooling) load to the steady-state furnace heating (or cooling) capacity. For the cycling fan mode, the runtime fraction for the furnace fan may be different from the fan part-load ratio reported here due the part-load performance of the furnace's heating (or cooling) coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff).
+
+Unitary System Compressor Part Load Ratio {[]}
+
+\subsection{~AirLoopHVAC:UnitaryHeatCool}\label{airloophvacunitaryheatcool}
+
+The AirLoopHVAC:UnitaryHeatCool object is the identical model to the AirLoopHAVC:Unitary:Furnace:HeatCool object. The heat/cool unitary system is a ``virtual'' component that consists of a fan component (OnOff or ConstantVolume), a DX cooling coil component and a Gas or Electric heating coil component as shown in Figure~\ref{fig:schematic-of-blow-through-heatcool-unitary}. When a draw through configuration is desired, the fan is placed directly after the heating coil. If dehumidification control is selected, a reheat coil component is also required. If the reheat coil is present and the dehumidification control type input is not specified as CoolReheat, the reheat coil will not be active,
+
+\begin{figure}[hbtp] % fig 117
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image299.png}
+\caption{Schematic of Blow Through Heat/Cool Unitary System \protect \label{fig:schematic-of-blow-through-heatcool-unitary}}
+\end{figure}
+
+Note: the coil order shown here has been revised from previous versions (prior to V4.0) of Energyplus to configure the cooling coil upstream of the heating coil. This configuration provides uniformity with all unitary equipment. However, for unitary HeatCool systems that do not use a reheat coil, the heating coil can also be placed upstream of the cooling coil. This optional coil placement is retained to allow compatibility with previous versions of Energyplus. For input files developed using previous versions of Energyplus, it is recommended that the coil order be revised according to the figure above.
+
+Links to the fan, DX cooling coil, heating coil and optional reheat coil specifications are provided in the unitary system input data syntax. In addition, the control zone name and the system design operating conditions are specified by the unitary system inputs.
+
+\subsubsection{Field: Name}\label{field-name-3-034}
+
+This alpha field contains the identifying name for the unitary system.
+
+\subsubsection{Field: Availability Schedule Name}\label{field-availability-schedule-name-2-008}
+
+This alpha field contains the schedule name which contains information on the availability of the unitary system to operate. A schedule value equal to 0 denotes that the unitary system must be off for that time period. A value greater than 0 denotes that the unitary system is available to operate during that time period. This schedule may be used to completely disable the unitary system as required. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\subsubsection{Field: Unitary System Air Inlet Node Name}\label{field-unitary-system-air-inlet-node-name-1}
+
+This alpha field contains the unitary system inlet node name.
+
+\subsubsection{Field: Unitary System Air Outlet Node Name}\label{field-unitary-system-air-outlet-node-name-1}
+
+This alpha field contains the unitary system outlet node name.
+
+\textbf{\emph{Field: Supply Air Fan Operating Mode Schedule Name}}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the unitary system supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.
+
+\subsubsection{Field: Maximum Supply Air Temperature}\label{field-maximum-supply-air-temperature-2-000}
+
+This numeric field contains the design operating air outlet temperature in degrees C when the unitary system is heating. If this input field is left blank, the default value is 80 C.
+
+\subsubsection{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-2-000}
+
+This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
+
+\subsubsection{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-2-000}
+
+This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than 0 or this field is autosizable.
+
+\subsubsection{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-2-000}
+
+This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the unitary system operating mode is specified as continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the unitary system operating mode is specified as continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the compressor was last operating (for cooling operation or heating operation).
+
+\subsubsection{Field: Controlling Zone or Thermostat Location}\label{field-controlling-zone-or-thermostat-location-2}
+
+This alpha field contains the identifying zone name where the thermostat controlling the unitary system is located.
+
+\subsubsection{Field: Supply Fan Object Type}\label{field-supply-fan-object-type-2}
+
+This alpha field contains the identifying type of supply air fan specified for the unitary system. Fan type must be \textbf{Fan:OnOff} or \textbf{Fan:ConstantVolume}. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e.~Supply Air Fan Operating Mode Schedule values are at times 0).
+
+\subsubsection{Field: Supply Fan Name}\label{field-supply-fan-name-2}
+
+This alpha field contains the identifying name given to the unitary system fan.
+
+\subsubsection{Field: Fan Placement}\label{field-fan-placement-2}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice stands for ``blow through fan''. This means that the unit consists of a fan followed by the DX coils and supplemental heating coil. The fan ``blows through'' the cooling and heating coils. The second choice stands for ``draw through fan''. This means that the unit consists of the DX coil(s) followed by a fan, with the supplemental heater located at the outlet of the fan. The fan ``draws air through'' the DX coil(s). If this field is left blank, the default is blow through.
+
+\subsubsection{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-2}
+
+This alpha field contains the identifying type of heating coil specified in the unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat and Cool System) itself provides the ``controller'' function of modulating water flow. Allowable coil types are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\subsubsection{Field: Heating Coil Name}\label{field-heating-coil-name-2}
+
+This alpha field contains the identifying name given to the unitary system heating coil.
+
+\subsubsection{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-2-000}
+
+This alpha field contains the identifying type of cooling coil specified in the unitary system. Only allowable coil types are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted
+\item
+  Coil:Cooling:DX:VariableSpeed
+\end{itemize}
+
+\subsubsection{Field: Cooling Coil Name}\label{field-cooling-coil-name-2-000}
+
+This alpha field contains the identifying name given to the unitary system cooling coil.
+
+\subsubsection{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-2-000}
+
+This alpha field contains the type of dehumidification control. The following options are valid for this field:
+
+\begin{itemize}
+\item
+  \textbf{None} - meet sensible load only, no active dehumidification control
+\item
+  \textbf{Multimode} - activate enhanced dehumidification mode as needed and meet sensible load. This option is used to model DX equipment with a controllable heat exchanger assisting the DX cooling coil for improved dehumidification. It is valid only with cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted.
+\item
+  \textbf{CoolReheat} - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. If cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted, then the heat exchanger is assumed to always transfer energy between the cooling coil's inlet and outlet airstreams when the cooling coil is operating.
+\end{itemize}
+
+The default is \textbf{None}. For the other dehumidification control modes, the maximum humidity setpoint is used. This must be set using a \textbf{ZoneControl:Humidistat} object. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate. If the dehumidification control type is specified as \textbf{CoolReheat}, then two additional inputs (reheat coil type and name) are also required as shown below. Although the reheat coil is required only when \textbf{CoolReheat} is selected, the optional reheat coil may be present for any of the allowed Dehumidification Control Types. If the reheat coil is present and the dehumidification control type is not specified as \textbf{CoolReheat}, the reheat coil will not be active,
+
+\subsubsection{Field: Reheat Coil Object Type}\label{field-reheat-coil-object-type-1-000}
+
+This alpha field contains the identifying type of reheat coil specified in the unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the reheat coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat and Cool System) itself provides the ``controller'' function of modulating water flow. Reheat coil type must be one of:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Desuperheater
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\subsubsection{Field: Reheat Coil Name}\label{field-reheat-coil-name-1-000}
+
+This alpha field contains the identifying name given to the unitary system reheat coil.
+
+As shown in the example below, correct specification of the heat/cool unitary system requires specification of the following objects in addition to the unitary system object:
+
+1)~~~Fan (Fan:OnOff or Fan:ConstantVolume)
+
+2)~~~Cooling coil (Coil:Cooling:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted)
+
+3)~~~Heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
+
+4)~~~Reheat coil (optional, Coil:Heating:Gas, Coil:Heating:Electric, or Coil:Heating:Desuperheater)
+
+5)~~~Direct air unit (AirTerminal:SingleDuct:Uncontrolled) for each zone served by the unitary system
+
+Note: the unitary system's fan, cooling coil, heating coil and optional reheat coil must be connected in the air loop according to the configuration shown above (Figure~\ref{fig:schematic-of-blow-through-heatcool-unitary}). In addition, the volumetric air flow rate specified in the direct air unit for the controlling zone should properly reflect the fractional volumetric air flow rate specified in the unitary system object.
+
+\begin{lstlisting}
+
+AirLoopHVAC:Unitary:Furnace:HeatCool,
+  GasHeat DXAC Unitary System 1, !- Name of unitary system
+  FanAndCoilAvailSched,   !- Availability schedule
+  Air Loop Inlet Node,    !- Unitary system inlet node name
+  Air Loop Outlet Node,   !- Unitary system outlet node name
+  CycFanSchedule,         !- Supply Air Fan Operating Mode Schedule Name
+  80,                     !- Maximum supply air temperature from unitary system heater {C}
+  1.3,                    !- Cooling Supply Air Flow Rate {m3/s}
+  1.3,                    !- Heating Supply Air Flow Rate {m3/s}
+  0.0,                    !- No Load Supply Air Flow Rate {m3/s}
+  East Zone,              !- Controlling zone or thermostat location
+  Fan:OnOff,              !- Supply fan type
+  Supply Fan 1,           !- Supply fan name
+  BlowThrough,            !- Fan Placement
+  Coil:Heating:Gas,       !- Heating coil type
+  Unitary System Heating Coil 1,   !- Heating coil name
+  Coil:Cooling:DX:SingleSpeed,  !- Cooling coil type
+  Unitary System ACDXCoil 1,       !- Cooling coil name
+  None;        !- High humidity control
+
+    Coil:Heating:Gas,
+      Unitary System Heating Coil 1,  !- Coil Name
+      FanAndCoilAvailSched,           !- Availability Schedule Name
+      0.8,    !- Gas Burner Efficiency of the Coil
+      25000,  !- Nominal Capacity of the Coil {W}
+      Heating Coil Air Inlet Node,    !- Coil\_Air\_Inlet\_Node
+      Air Loop Outlet Node;           !- Coil\_Air\_Outlet\_Node
+
+
+    Coil:Cooling:DX:SingleSpeed,
+      Unitary System ACDXCoil 1,      !- Coil Name
+      FanAndCoilAvailSched,  !- Availability Schedule
+      25000,  !- Rated Total Cooling Capacity (gross) {W}
+      0.75,   !- Rated SHR
+      3.0,    !- Rated COP
+      1.3,    !- Rated Air Volume Flow Rate {m3/s}
+      DX Cooling Coil Air Inlet Node, !- Coil Air Inlet Node
+      Heating Coil Air Inlet Node,    !- Coil Air Outlet Node
+      WindACCoolCapFT,  !- Total Cooling Capacity Modifier Curve (function of temperature)
+      WindACCoolCapFFF, !- Total Cooling Capacity Modifier Curve (function of flow fraction)
+      WindACEIRFT,      !- Energy Input Ratio Modifier Curve (function of temperature)
+      WindACEIRFFF,     !- Energy Input Ratio Modifier Curve (function of flow fraction)
+      WindACPLFFPLR,    !- Part Load Fraction Correlation (function of part load ratio)
+      CyclingFanAndCompressor;    !- Supply Air Fan Operation Mode
+
+
+    Fan:OnOff,
+      Supply Fan 1,                !- Fan Name
+      FanAndCoilAvailSched,        !- Availability Schedule Name
+      0.7,    !- Fan Total Efficiency
+      600.0,  !- Delta Pressure {Pa}
+      1.3,    !- Max Flow Rate {m3/s}
+      0.9,    !- Motor Efficiency
+      1.0,    !- Motor In Airstream Fraction
+      Air Loop Inlet Node,         !- Fan\_Inlet\_Node
+      DX Cooling Coil Air Inlet Node; !- Fan\_Outlet\_Node
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone1DirectAir,        !- Direct Air Name
+      FanAndCoilAvailSched,  !- Schedule name for on/off schedule
+      Zone 1 Inlet Node,     !- Zone Supply Air Node Name
+     0.47;  !- Maximum air flow rate {m3/s}
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone2DirectAir,        !- Direct Air Name
+      FanAndCoilAvailSched,  !- Schedule name for on/off schedule
+      Zone 2 Inlet Node,     !- Zone Supply Air Node Name
+     0.36;  !- Maximum air flow rate {m3/s}
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone3DirectAir,        !- Direct Air Name
+      FanAndCoilAvailSched,  !- Schedule name for on/off schedule
+      Zone 3 Inlet Node,     !- Zone Supply Air Node Name
+     0.47;  !- Maximum air flow rate {m3/s}
+\end{lstlisting}
+
+Example of Heat/Cool Unitary System Specification
+
+\subsection{Unitary System Heat and Cool (AirLoopHVAC) Outputs}\label{unitary-system-heat-and-cool-airloophvac-outputs}
+
+\begin{itemize}
+\item
+  HVAC,Average, Unitary System Fan Part Load Ratio {[]}
+\item
+  HVAC,Average, Unitary System Compressor Part Load Ratio
+\end{itemize}
+
+\subsubsection{\texorpdfstring{Unitary System Fan Part Load Ratio {[]}}{Unitary System Fan Part Load Ratio }}\label{unitary-system-fan-part-load-ratio-2}
+
+This output variable is the ratio of actual air mass flow rate through the unitary system to the system's design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the unitary system is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating (or cooling) load to the steady-state unitary system heating (or cooling) capacity. For the cycling fan mode, the runtime fraction for the unitary system fan may be different from the fan part-load ratio reported here due the part-load performance of the system's heating (or cooling) coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff).
+
+\subsubsection{\texorpdfstring{Unitary System Compressor Part Load Ratio {[]}}{Unitary System Compressor Part Load Ratio }}\label{unitary-system-compressor-part-load-ratio-1}
+
+This output variable is the ratio of the sensible cooling load to the steady-state cooling capacity of the unitary system's DX cooling coil. The runtime fraction for the DX cooling coil compressor may be different from the compressor part-load ratio reported here due the part-load performance of the cooling coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
+
+\subsection{AirLoopHVAC:UnitaryHeatPump:AirToAir}\label{airloophvacunitaryheatpumpairtoair}
+
+The unitary air-to-air heat pump is a ``virtual'' component that consists of a fan component (OnOff or ConstantVolume), a DX cooling coil component, a DX heating coil component, and a Gas or Electric supplementary heating coil component as shown in the Figure below.
+
+~\includegraphics{media/image300.png}
+
+Figure 118. Schematic of EnergyPlus Unitary Air-to-Air Heat Pump (Blow Through Configuration)
+
+Links to the fan, DX cooling coil, DX heating coil, and supplementary heating coil specifications are provided in the heat pump's input data syntax. In addition the control zone name and the system design operating conditions are specified by the heat pump inputs.
+
+\subsubsection{Inputs}\label{inputs-3-039}
+
+\paragraph{~Field: Name}\label{field-name-4-031}
+
+This alpha field contains the identifying name for the unitary system heat pump.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-3-006}
+
+This alpha field contains the schedule name (ref. Schedule objects) that contains information on the availability of the heat pump to operate. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the hour. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the hour. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-007}
+
+This alpha field contains the~ name of the HVAC system node from which the heat pump draws its inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-006}
+
+This alpha field contains the~ name of the HVAC system node to which the heat pump sends its outlet air.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-3-000}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-3-000}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-3-000}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the heat pump operating mode is specified as continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the heat pump operating mode is specified as continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the compressor was last operating (for cooling operation or heating operation).
+
+\paragraph{Field: Controlling Zone or Thermostat Location}\label{field-controlling-zone-or-thermostat-location-3}
+
+This alpha field contains the identifying zone name where the thermostat controlling the heat pump is located.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type}
+
+This alpha field contains the identifying type of supply air fan specified for the heat pump. Fan type must be \textbf{Fan:OnOff} or \textbf{Fan:ConstantVolume}. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e.~Supply Air Fan Operating Mode Schedule values are at times 0).
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name}
+
+This alpha field contains the identifying name given to the heat pump supply air fan, and should match the name specified in the corresponding fan object.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-3}
+
+This alpha field contains the identifying type of heating coil specified in the heat pump. Heating coil type must be either Coil:Heating:DX:SingleSpeed or Coil:Heating:DX:VariableSpeed.
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-3}
+
+This alpha field contains the identifying name given to the heat pump DX heating coil, and should match the name specified in the corresponding DX heating coil object.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-3}
+
+This alpha field contains the identifying type of cooling coil specified in the heat pump. There are three valid choices for this field:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted
+\item
+  Coil:Cooling:DX:VariableSpeed
+\end{itemize}
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-3}
+
+This alpha field contains the identifying name given to the heat pump cooling coil, and should match the name specified in the corresponding DX cooling coil object.
+
+\paragraph{Field: Supplemental Heating Coil Object Type}\label{field-supplemental-heating-coil-object-type-1}
+
+This alpha field contains the identifying type of supplemental heating coil specified in the heat pump. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the supplemental heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Airloop Air to Air Heat Pump) itself provides the ``controller'' function of modulating water flow. Heating coil type must be:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Supplemental Heating Coil Name}\label{field-supplemental-heating-coil-name-1}
+
+This alpha field contains the identifying name given to the heat pump supplemental heating coil, and should match the name specified in the corresponding heating coil object.
+
+\paragraph{Field: Maximum Supply Air Temperature from Supplemental Heater}\label{field-maximum-supply-air-temperature-from-supplemental-heater}
+
+This numeric field defines the maximum allowed supply air temperature exiting the heat pump supplemental heating coil.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-supplemental-heater-operation-1}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the heat pump supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-3}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice represents a blow through system where the supply air fan is before the DX cooling/heating coil and the supplementary heating coil. The second choice represents a draw through system where the supply air fan is between the DX cooling/heating coil and the supplementary heating coil. If this input field is left blank, the default is blow through.
+
+\textbf{\emph{Field: Supply Air Fan Operating Mode Schedule Name}}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the unitary system supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.
+
+As shown in the example below, correct specification of the air-to-air heat pump requires specification of the following objects in addition to the heat pump object:
+
+1)~~~Fan (Fan:OnOff or Fan:ConstantVolume)
+
+2)~~~Heating coil (Coil:Heating:DX:SingleSpeed)
+
+3)~~~Cooling coil (Coil:Cooling:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted)
+
+4)~~~Supplemental heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
+
+5)~~~Direct air unit (AirTerminal:SingleDuct:Uncontrolled)for each zone served by the unitary system
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-3-000}
+
+This alpha input field contains the type of dehumidification control. The following options are valid for this field:
+
+\begin{itemize}
+\item
+  \textbf{None} - meet sensible load only, no active dehumidification control
+\item
+  \textbf{Multimode} - activate enhanced dehumidification mode as needed and meet sensible cooling load. This option is used to model DX equipment with a controllable heat exchanger assisting the DX cooling coil for improved dehumidification. It is valid only with cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted.
+\item
+  \textbf{CoolReheat} - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. The excess cooling beyond the cooling set point temperature is offset by the supplemental heating coil. If cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted, then the heat exchanger is assumed to always transfer energy between the cooling coil's inlet and outlet airstreams when the cooling coil is operating.
+\end{itemize}
+
+The default is \textbf{None}. For the other dehumidification control modes, the maximum humidity setpoint is required. This must be set using a \textbf{ZoneControl:Humidistat} object. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate. Supplemental heating coil (supplemental heating coil type and name) is a required input in AirToAir HeatPumps. The supplemental heating coil capacity must be adequate enough to meet the heating coil load and offset the excess cooling load due to extra dehumidification required to meet the high relative humidity setpoint.
+
+Note: the air-to-air heat pump's fan, cooling coil, heating coil and supplementary heating coil must be connected in the air loop according to the configuration shown above (Figure 118) for the blow-through fan configuration. The only other valid configuration is with a draw-through fan placement, where the fan is located between the DX heating coil and the supplementary heating coil.
+
+\paragraph{AirLoopHVAC:UnitaryHeatPump:AirToAir Example Specification}\label{airloophvacunitaryheatpumpairtoair-example-specification}
+
+\begin{lstlisting}
+
+AirLoopHVAC:UnitaryHeatPump:AirToAir,
+        DXAC Heat Pump 1,            ! Heat Pump name
+        FanAndCoilAvailSched,        ! Heat Pump availability schedule
+        Mixed Air Node,              ! Heat Pump air inlet  node
+        Air Loop Outlet Node,        ! Heat Pump air outlet  node
+        1.3,                  !- Cooling Supply Air Flow Rate {m3/s}
+        1.3,                  !- Heating Supply Air Flow Rate {m3/s}
+        0.0,                  !- No Load Suuply Air Flow Rate {m3/s}
+        East Zone,                   ! Controlling zone or thermostat location
+        Fan:OnOff,            ! Supply air fan type
+        Supply Fan 1,                ! Supply air fan name –- same name used in fan object
+        Coil:Heating:DX:SingleSpeed,    ! Heating coil type
+        Heat Pump DX Heating Coil 1, ! Heating coil name –- same name used in DX heating coil object
+        Coil:Cooling:DX:SingleSpeed, !  Cooling coil type
+        Heat Pump ACDXCoil 1,        ! Cooling coil name –- same name used in DX cooling coil object
+        Coil:Heating:Gas,            ! Supplemental heating coil type
+        Heat Pump DX Supp Heating Coil 1, ! Supplemental heating coil name–- same as in heating coil object
+        50,                          ! Maximum supply air temperature from supplemental heater [C]
+        21,                      ! Maximum outdoor dry-bulb temp for supplemental heating coil operation [C]
+        BlowThrough,                ! Fan  placement
+        CycFanSchedule,              ! Supply air fan operating mode schedule name
+        CoolReheat;                  !- Dehumidification Control Type
+
+     Coil:Heating:DX:SingleSpeed,
+        Heat Pump DX Heating Coil 1,     ! Name of heating coil
+        FanAndCoilAvailSched,            ! Heating coil schedule
+        35000,                           ! Rated total heating capacity [W] (at 21.11C/8.33C)
+        2.75,                            ! Rated heating COP
+        1.7,                             ! Rated air flow rate [m3/s]
+        Heating Coil Air Inlet Node,     ! Coil air inlet node
+        SuppHeating Coil Air Inlet Node, ! Coil air outlet node
+        HPACHeatCapFT,                   ! Heating capacity modifier curve (temperature,C)
+        HPACHeatCapFFF,                  ! Heating capacity modifier curve (flow fraction)
+        HPACHeatEIRFT,                   ! Energy input ratio modifier curve (temperature,C)
+        HPACHeatEIRFFF,                  ! Energy input ratio modifier curve (flow fraction)
+        HPACCoolPLFFPLR,                 ! Part load fraction modifier curve (function of part-load ratio)
+        ,                         ! defrost EIR modifier curve (temp, C) not required for resistive defrost
+        CyclingFanAndCompressor,                   ! Operation mode (cycling fan, cycling compressor)
+        -5.0,                            ! Minimum OAT for heat pump compressor operation [C]
+        5.0,                             ! Maximum outdoor dry-bulb temp for defrost operation [C]
+        200.0,                           ! Crankcase heater capacity[W]
+        10.0,                            ! Maximum OAT for crankcase heater operation [C]
+        resistive,                       ! Defrost strategy (resistive or reverse-cycle)
+        timed,                           ! Defrost control (timed or on-demand)
+        0.166667,                        !Defrost time period fraction (used for timed defrost control only)
+        20000;                           ! Resistive defrost heater capacity [W]
+
+     Coil:Cooling:DX:SingleSpeed,
+        Heat Pump ACDXCoil 1,            ! Name of cooling coil
+        FanAndCoilAvailSched,            ! Availability schedule
+        32000,                           ! Rated total cooling capacity [W]
+        0.75,                            ! Rated sensible heat ratio
+        3.0,                             ! Rated COP
+        1.7,                             ! Rated air flow rate [m3/s]
+        DX Cooling Coil Air Inlet Node,  ! Coil air inlet node
+        Heating Coil Air Inlet Node,     ! Coil air outlet node
+        HPACCoolCapFT,                   ! Cooling capacity modifier curve (temperature,C)
+        HPACCoolCapFFF,                  ! Cooling capacity modifier curve (flow fraction)
+        HPACCoolEIRFT,                   ! Energy input ratio modifier curve (temperature,C)
+        HPACCoolEIRFFF,                  ! Energy input ratio modifier curve (flow fraction)
+        HPACCoolPLFFPLR,                 ! Part load factor modifier curve (function of part-load ratio)
+        CyclingFanAndCompressor;                   ! Operation mode (cycling fan, cycling compressor)
+
+     Coil:Heating:Gas,
+        Heat Pump DX Supp Heating Coil 1, ! Name of heating coil
+        FanAndCoilAvailSched,             ! Availability schedule
+        0.8 ,                             ! Gas Burner Efficiency of the Coil
+        32000,                            ! Nominal Capacity of the Coil [W]
+        SuppHeating Coil Air Inlet Node,  ! Supplementary heating coil air side inlet node
+        Air Loop Outlet Node;             ! Supplementary heating coil air side outlet node
+
+     Fan:OnOff,
+        Supply Fan 1,                    ! Fan Name
+        FanAndCoilAvailSched,            ! Fan Schedule
+        0.7,                             ! Fan Total Efficiency
+        300.0,                           ! Delta Pressure [N/M^2]
+        1.7,                             ! Max Vol Flow Rate  [m^3/Sec]
+        0.9,                             ! motor efficiency
+        1.0,                             ! motor in air stream fraction
+        Mixed Air Node,                  ! fan inlet node
+        DX Cooling Coil Air Inlet Node;  ! fan outlet node
+
+     AirTerminal:SingleDuct:Uncontrolled,
+        Zone1DirectAir,                  ! direct air unit name
+       FanAndCoilAvailSched,            ! schedule name for on/off schedule
+        Zone 1 Inlet Node,               ! zone supply air node name
+       0.612;                           ! maximum air flow rate, m3/s
+
+     AirTerminal:SingleDuct:Uncontrolled,
+        Zone2DirectAir,                  ! direct air unit name
+       FanAndCoilAvailSched,            ! schedule name for on/off schedule
+        Zone 2 Inlet Node,               ! zone supply air node name
+       0.476;                           ! maximum air flow rate, m3/s
+
+     AirTerminal:SingleDuct:Uncontrolled,
+        Zone3DirectAir,                  ! direct air unit name
+       FanAndCoilAvailSched,            ! schedule name for on/off schedule
+        Zone 3 Inlet Node,               ! zone supply air node name
+       0.612;                           ! maximum air flow rate, m3/s
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-024}
+
+\begin{itemize}
+\item
+  HVAC, Average, Unitary System Fan Part Load Ratio {[]}
+\item
+  HVAC, Average, Unitary System Compressor Part Load Ratio {[]}
+\item
+  HVAC, Average, Unitary System Dehumidification Induced Heating Demand Rate {[}W{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Unitary System Fan Part Load Ratio {[]}}{Unitary System Fan Part Load Ratio }}\label{unitary-system-fan-part-load-ratio-3}
+
+This output variable is the ratio of actual air mass flow rate through the heat pump to the heat pump's design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the furnace is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating (or cooling) load to the steady-state heat pump heating (or cooling) capacity. For the cycling fan mode, the runtime fraction for the heat pump fan may be different from the fan part-load ratio reported here due the part-load performance of the heat pump's heating (or cooling) coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff).
+
+\paragraph{\texorpdfstring{Unitary System Compressor Part Load Ratio {[]}}{Unitary System Compressor Part Load Ratio }}\label{unitary-system-compressor-part-load-ratio-2}
+
+This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the heat pump's DX heating or cooling coil. The runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due the part-load performance of the heating/cooling coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
+
+\paragraph{Unitary System Dehumidification Induced Heating Demand Rate {[}W{]}}\label{unitary-system-dehumidification-induced-heating-demand-rate-w}
+
+This output variable is the additional heating demand rate of the supplemental heating coil of an Air-to-Air heat pumps in Watts.~ This additional heating demand is induced when zone air overshoots the heating setpoint due to extra dehumidification requirement to meet the high humidity setpoint. This value is always positive. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
+
+\subsection{AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed}\label{airloophvacunitaryheatpumpairtoairmultispeed}
+
+The multispeed air-to-air heat pump is a ``virtual'' component that consists of a fan component (On/Off or ConstVolume), a DX multispeed cooling coil component, a DX multispeed heating coil component, and a Gas or Electric supplemental heating coil component. This system also includes the option to use available waste energy to heat water. A schematic diagram of the air-to-air multispeed heat pump is shown below. The component connection sequence for the blow through option (shown below) from inlet to outlet is fan, cooling coil, heating coil, and supplemental heater. The connection sequence for the draw through option is cooling coil, heating coil, fan, and supplemental heater.
+
+The main difference between this heat pump object and other EnergyPlus heat pump objects is that this object allows from two to four discrete compressor speeds for heating and cooling operation (instead of a single speed for each mode). The lowest speed is called Speed 1, and the highest speed is called Speed n (2, 3 or 4 as specified in the input syntax). This object allows a different number of speeds for cooling and heating, and each speed has an associated airflow rate. The airflow rates for the various heating speeds can be different from the airflow rates for the cooling speeds. In addition, the airflow rate when no cooling or heating is needed can also be defined. The number of cooling and heating speeds defined by the user in this heat pump object must equal the number of speeds defined in the associated coils (child objects). For example, the number of speeds for cooling defined in this heat pump object must be equal to the number of speeds defined in the associated cooling coil object.
+
+Links to the fan, DX multispeed cooling coil, DX multispeed heating coil, and supplementary heating coil specifications are provided in the heat pump's input data syntax. In addition, the control zone name and airflow rates at the corresponding compressor speeds are specified by the heat pump syntax.
+
+If the ZoneControl:Thermostat:StagedDualSetpoint object and other zone control thermostat and humidistat are assigned to the same controlled zone in the Controlling Zone or Thermostat Location field, the ZoneControl:Thermostat:StagedDualSetpoint object takes precedence and the stage number provided by the the ZoneControl:Thermostat:StagedDualSetpoint object is used to set the speed number.
+
+\begin{figure}[hbtp] % fig 119
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image301.png}
+\caption{Schematic of EnergyPlus Unitary Air-to-Air Multi Speed Heat Pump \protect \label{fig:schematic-of-energyplus-unitary-air-to-air}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-4-036}
+
+\paragraph{Field: Name}\label{field-name-5-027}
+
+This alpha field contains the identifying name for the multispeed heat pump.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-4-006}
+
+This alpha field contains the schedule name (ref. Schedule objects) that contains information on the availability of the heat pump to operate. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-1-005}
+
+This alpha field contains the name of the HVAC system node from which the heat pump draws its inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-1-004}
+
+This alpha field contains the name of the HVAC system node to which the heat pump sends its outlet air.
+
+\paragraph{Field: Controlling Zone or Thermostat Location}\label{field-controlling-zone-or-thermostat-location-4}
+
+This alpha field contains the identifying zone name where the thermostat controlling the multispeed heat pump is located.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-1}
+
+This alpha field contains the identifying type of supply air fan specified for the heat pump. Fan type must be Fan:OnOff or Fan:ConstantVolume. Fan:ConstantVolume can only be used when the supply air fan operating mode is continuous (see field `Supply air fan operating mode schedule name).
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-1}
+
+This alpha field contains the identifying name given to the heat pump supply air fan, and should match the name specified in the corresponding fan object.
+
+\paragraph{Field: Supply Air Fan Placement}\label{field-supply-air-fan-placement}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice stands for ``blow through fan''. This means that the unit consists of a fan followed by a DX multispeed cooling coil, DX multispeed heating coil, and a supplemental heating coil. The fan ``blows through'' the cooling and heating coils. The second choice stands for ``draw through fan''. This means that the unit consists of the DX cooling and heating coils followed by a fan, with the supplemental heater located at the outlet of the fan.~ The fan ``draws'' air through the DX coils.
+
+\textbf{Note}: the multispeed heat pump's supply air fan, cooling coil, heating coil and supplemental heating coil must be connected according to the configuration shown above (Figure~\ref{fig:schematic-of-energyplus-unitary-air-to-air}) for the `blow through' fan configuration. For the `draw through' fan configuration the fan must be located between the DX heating coil and the supplemental heater, whose outlet node is the system outlet node. In addition, the DX cooling coil and DX heating coil operation mode must be specified consistently with the heat pump's supply air fan operating mode (e.g., with the heat pump's supply air fan set to cycle on and off with the cooling/heating load, the DX cooling and heating coil operation mode must be CyclingFanAndCompressor). If the operation modes in the parent (heat pump) and child (coil) objects are specified differently, the operation mode in the parent object prevails.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-1}
+
+This alpha field contains the schedule name (ref. Schedule objects) that contains information to control the supply air fan. Schedule values of zero mean that the supply air fan will cycle off if there is no cooling or heating load in the control zone. Non-zero schedule values mean that the supply air fan will operate continuously even if there is no cooling or heating load in the control zone. If this field is left blank, the supply air fan will operate continuously for the entire simulation period.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-4}
+
+This alpha field contains the identifying type of heating coil specified in the heat pump.~ Allowable choices for Heating coil type~ are \textbf{Coil:Heating:DX:MultiSpeed}, \textbf{Coil:Heating:Electric:MultiStage}, \textbf{Coil:Heating:Gas:MultiStage}, \textbf{Coil:Heating:Water}, and~ \textbf{Coil:Heating:Steam}.
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-4}
+
+This alpha field contains the identifying name given to the DX heating coil, and should match the name specified in the corresponding DX heating coil object.
+
+\paragraph{Field: Minimum Outdoor Dry-Bulb Temperature for Compressor Operation}\label{field-minimum-outdoor-dry-bulb-temperature-for-compressor-operation-000}
+
+This numeric field defines the outdoor air dry-bulb temperature below which the DX heating coil turns off.~ The temperature for this input field must be greater than or equal to --20 C.~ If this input field is left blank, the default value is -8 C. This temperature should match the minimum compressor operating temperature specified for the multispeed heat pump's DX heating coil. This field is only needed when Heating Coil Object Type above is \textbf{Coil:Heating:DX:MultiSpeed}.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-4}
+
+This alpha field contains the identifying type of cooling coil specified in the heat pump.~ Cooling coil type must be Coil:Cooling:DX:MultiSpeed.
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-4}
+
+This alpha field contains the identifying name given to the heat pump cooling coil, and should match the name specified in the corresponding DX cooling coil object.
+
+\paragraph{Field: Supplemental Heating Coil Object Type}\label{field-supplemental-heating-coil-object-type-2}
+
+This alpha field contains the identifying type of supplemental heating coil specified in the heat pump. The hot water and steam heating coils require specifying plant loop, branches, and connectors objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the supplemental heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary MultiSpeed Air to Air Heat Pump) itself provides the ``controller'' function of modulating water flow. Heating coil type must be:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Supplemental Heating Coil Name}\label{field-supplemental-heating-coil-name-2}
+
+This alpha field contains the identifying name given to the heat pump supplemental heating coil, and should match the name specified in the corresponding heating coil object.
+
+\paragraph{Field: Maximum Supply Air Temperature from Supplemental Heater}\label{field-maximum-supply-air-temperature-from-supplemental-heater-1}
+
+This numeric field defines the maximum allowed supply air temperature (in degrees C) exiting the heat pump supplemental heating coil. If the calculated supply air temperature exiting the supplemental heater exceeds this value, then it is reset to this maximum temperature. This field is autosizable.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-supplemental-heater-operation-2}
+
+This numeric field defines the outdoor air dry-bulb temperature above which the heat pump supplemental heating coil is disabled.~ The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
+
+\paragraph{Field: Auxiliary On-Cycle Electric Power}\label{field-auxiliary-on-cycle-electric-power}
+
+This field defines auxiliary electrical power (W) consumed during the on-cycle period (i.e., when the cooling or heating coil is operating). The model assumes that this auxiliary power does not contribute to heating the supply air. The minimum value for this field is 0.0, and the default value is also 0.0 if the field is left blank.
+
+\paragraph{Field: Auxiliary Off-Cycle Electric Power}\label{field-auxiliary-off-cycle-electric-power}
+
+This field defines auxiliary electrical power (W) consumed during the off-cycle period (i.e., when the cooling and heating coil are not operating). The model assumes that this auxiliary power does not contribute to heating the supply air. The minimum value for this field is 0.0, and the default value is also 0.0 if the field is left blank.
+
+\paragraph{Field: Design Heat Recovery Water Flow Rate}\label{field-design-heat-recovery-water-flow-rate-1-001}
+
+This optional input field defines the design water flow rate used if the heat recovery option is being simulated. If this value is greater than 0.0 then a heat recovery loop must be specified and attached to the multispeed heat pump using the next 2 node fields. To determine how the heat recovery algorithm works, refer to the EnergyPlus Engineering Reference in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed with Heat Recovery section. The units for this input value are cubic meters per second.
+
+\paragraph{Field: Maximum Temperature for Heat Recovery}\label{field-maximum-temperature-for-heat-recovery-1}
+
+This field sets the maximum temperature (in degrees C) that this heat pump can produce for heat recovery. The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit. This temperature limit puts an upper bound on the recovered heat and limits the max temperature leaving the component.
+
+As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting. This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply.
+
+\paragraph{Field: Heat Recovery Water Inlet Node Name}\label{field-heat-recovery-water-inlet-node-name-1-000}
+
+This alpha field contains the identifying name for the heat recovery side inlet node.
+
+\paragraph{Field: Heat Recovery Water Outlet Node Name}\label{field-heat-recovery-water-outlet-node-name-1-000}
+
+This alpha field contains the identifying name for the heat recovery side outlet node.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-4-000}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when neither cooling nor heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the heat pump supply air fan is scheduled to operate continuously regardless of DX coil operation (ref. field ``Supply Air Fan Operating Mode Schedule). Values must be greater than or equal to zero, or this field is autosizable. If the heat pump supply air fan is scheduled to operate continuously and the input value for this field is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the compressor was last operating (for cooling operation or heating operation).
+
+\paragraph{Field: Number of Speeds for Heating}\label{field-number-of-speeds-for-heating-1}
+
+This field defines the number of heating speeds for the heat pump, and must match the number of heating speeds defined in the associated heating coil. The value for this input field defines the number of airflow rates that must be defined for heating in the field below. The minimum value for this field is one and the maximum value is four. If the Heating Coil Object Type above are \textbf{Coil:Heating:Water} or \textbf{Coil:Heating:Steam}, then this field should be 1.
+
+\paragraph{Field: Number of Speeds for Cooling}\label{field-number-of-speeds-for-cooling-1}
+
+This field defines the number of cooling speeds for the heat pump, and must match the number of cooling speeds defined in the associated DX cooling coil. The value for this input field defines the number of airflow rates that must be defined for cooling in the field below. The minimum value for this field is two and the maximum value is four.
+
+\paragraph{Field: Heating Speed 1 Supply Air Flow Rate}\label{field-heating-speed-1-supply-air-flow-rate}
+
+This required numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating at Speed 1 (lowest speed). Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: Heating Speed 2 Supply Air Flow Rate}\label{field-heating-speed-2-supply-air-flow-rate}
+
+This required numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating at Speed 2. Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for heating Speed 1.
+
+\paragraph{Field: Heating Speed 3 Supply Air Flow Rate}\label{field-heating-speed-3-supply-air-flow-rate}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating at Speed 3. Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for heating Speed 2. If the `Number of Speeds for Heating' is less than 3, then this field can be left blank.
+
+\paragraph{Field: Heating Speed 4 Supply Air Flow Rate}\label{field-heating-speed-4-supply-air-flow-rate}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating at Speed 4 (high speed). Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for heating Speed 3. If the `Number of Speeds for Heating' is less than 4, then this field can be left blank.
+
+\textbf{Note}: When autosizable is selected for any of the supply air volumetric flow rate fields, all supply air flow fields at the different speeds must be specified as autosizable. Otherwise, a fatal error will be issued and the simulation will terminate.
+
+\paragraph{Field: Cooling Speed 1 Supply Air Flow Rate}\label{field-cooling-speed-1-supply-air-flow-rate}
+
+This required numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating at Speed 1 (lowest speed). Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: Cooling Speed 2 Supply Air Flow Rate}\label{field-cooling-speed-2-supply-air-flow-rate}
+
+This required numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating at Speed 2. Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for cooling Speed 1.
+
+\paragraph{Field: Cooling Speed 3 Supply Air Flow Rate}\label{field-cooling-speed-3-supply-air-flow-rate}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating at Speed 3. Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for cooling Speed 2. If the `Number of Speeds for Cooling' is less than 3, then this field can be left blank.
+
+\paragraph{Field: Cooling Speed 4 Supply Air Flow Rate}\label{field-cooling-speed-4-supply-air-flow-rate}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating at Speed 4 (highest speed). Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for cooling Speed 3. If the `Number of Speeds for Cooling' is less than 4, then this field can be left blank.
+
+Following is an example input for the object and its associated components.
+
+\begin{lstlisting}
+
+AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed,
+  DXAC Heat Pump 1,        !- Name of multispeed heat pump
+  FanAndCoilAvailSched,    !- Availability schedule
+  Mixed Air Node,          !- Heat pump air inlet node name
+  Air Loop Outlet Node,    !- Heat pump air outlet node name
+  East Zone,               !- Controlling zone or thermostat location
+  Fan:OnOff,               !- Supply air fan type
+  Supply Fan 1,            !- Supply air fan name
+  BlowThrough,             !- Supply air fan placement
+  FanModeSchedule,         !- Supply air fan operating mode schedule name
+  Coil:Heating:DX:MultiSpeed, Heat Pump DX Heating Coil 1,  !- Heating coil type & name
+  -8.0,                    !- Minimum outdoor dry-bulb temperature for compressor operation
+  Coil:Cooling:DX:MultiSpeed, Heat Pump ACDXCoil 1,    !- Cooling coil type & name
+  Coil:Heating:Gas,        !- Supplemental heating coil type
+  Supp Gas Heating Coil 1, !- Supplemental heating coil name
+  50.0,                    !- Maximum supply air temperature from supplemental heater
+  21,                      !- Maximum outdoor dry-bulb temperature for supplemental heater operation
+  0,                       !- Auxiliary On-Cycle Electric Power {W}
+  0,                       !- Auxiliary Off-Cycle Electric Power {W}
+  0.00,                    !- Design Heat Recovery Water Flow Rate {m3/s}
+  80.0,,,                    !- Maximum Temp for Heat Recovery {C} & Node names (none)
+  0.2,                     !- Supply air volumetric flow rate when no cooling or heating is needed
+  4,                       !- Number of speeds for heating
+  4,                       !- Number of speeds for cooling
+  0.4,                     !- Heating Speed 1 Supply Air Flow Rate
+  0.8,                     !- Heating Speed 2 Supply Air Flow Rate
+  1.2,                     !- Heating Speed 3 Supply Air Flow Rate
+  1.7,                     !- Heating Speed 4 Supply Air Flow Rate
+  0.4,                     !- Cooling Speed 1 Supply Air Flow Rate
+  0.8,                     !- Cooling Speed 2 Supply Air Flow Rate
+  1.2,                     !- Cooling Speed 3 Supply Air Flow Rate
+  1.7;                     !- Cooling Speed 4 Supply Air Flow Rate
+
+  Coil:Heating:DX:MultiSpeed,
+      Heat Pump DX Heating Coil 1,  !- Name of heat pump heating coil
+      FanAndCoilAvailSched,    !- Availability Schedule
+      Heating Coil Air Inlet Node,  !- Coil Air Inlet Node
+      SuppHeating Coil Air Inlet Node,  !- Coil Air Outlet Node
+      CyclingFanAndCompressor,           !- Supply Air Fan Operation Mode
+      -8.0,                    !- Minimum Outdoor Dry-bulb Temperature for Compressor Operation {C}
+      200.0,                   !- Crankcase Heater Capacity {W}
+      10.0,                    !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater
+                           !- Operation {C}
+      HPACDefrostCAPFT,        !- Defrost energy input ratio modifier curve (temperature)
+      7.22,                    !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation
+      reverse-cycle,           !- Defrost Strategy
+      timed,                   !- Defrost Control
+      0.058333,                !- Defrost Time Period Fraction
+      2000.0,                  !- Resistive Defrost Heater Capacity {W}
+      No,                      !- Apply Part Load Fraction to Speeds greater than 1
+      NaturalGas,              !- Fuel type
+      4,                       !- Number of speeds
+      7500,                    !- Rated Total Heating Capacity, Speed 1 {W}
+      2.75,                    !- Rated COP, Speed 1
+      0.45,                    !- Rated Air Volume Flow Rate, Speed 1 {m3/s}
+      HPACHeatCapFT Speed 1,   !- Total Heating Capacity Modifier Curve, Speed 1 (temperature)
+      HPACHeatCapFF Speed 1,   !- Total Heating capacity modifier curve, Speed 1 (flow fraction)
+      HPACHeatEIRFT Speed 1,   !- Energy input ratio modifier curve, Speed 1 (temperature)
+      HPACHeatEIRFF Speed 1,   !- Energy input ratio modifier curve, Speed 1 (flow fraction)
+      HPACHeatPLFFPLR Speed 1, !- Part load fraction correlation, Speed 1 (part load ratio)
+      0.2,                     !- Rated waste heat fraction of power input, Speed 1
+      HAPCHeatWHFT Speed 1,    !- Waste heat modifier curve, Speed 1 (temperature)
+      17500,                   !- Rated Total Heating Capacity, Speed 2 {W}
+      2.75,                    !- Rated COP, Speed 2
+      0.85,                    !- Rated Air Volume Flow Rate, Speed 2 {m3/s}
+      HPACHeatCapFT Speed 2,   !- Total Heating Capacity Modifier Curve, Speed 2 (temperature)
+      HPACHeatCapFF Speed 2,   !- Total Heating capacity modifier curve, Speed 2 (flow fraction)
+      HPACHeatEIRFT Speed 2,   !- Energy input ratio modifier curve, Speed 2 (temperature)
+      HPACHeatEIRFF Speed 2,   !- Energy input ratio modifier curve, Speed 2 (flow fraction)
+      HPACHeatPLFFPLR Speed 2, !- Part load fraction correlation, Speed 2 (part load ratio)
+      0.2,                     !- Rated waste heat fraction of power input, Speed 2
+      HAPCHeatWHFT Speed 2,    !- Waste heat modifier curve, Speed 2 (temperature)
+      25500,                   !- Rated Total Heating Capacity, Speed 3 {W}
+      2.75,                    !- Rated COP, Speed 3
+      1.25,                    !- Rated Air Volume Flow Rate, Speed 3 {m3/s}
+      HPACHeatCapFT Speed 3,   !- Total Heating Capacity Modifier Curve, Speed 3 (temperature)
+      HPACHeatCapFF Speed 3,   !- Total Heating capacity modifier curve, Speed 3 (flow fraction)
+      HPACHeatEIRFT Speed 3,   !- Energy input ratio modifier curve, Speed 3 (temperature)
+      HPACHeatEIRFF Speed 3,   !- Energy input ratio modifier curve, Speed 3 (flow fraction)
+      HPACHeatPLFFPLR Speed 3, !- Part load fraction correlation, Speed 3 (part load ratio)
+      0.2,                     !- Rated waste heat fraction of power input, Speed 3
+      HAPCHeatWHFT Speed 3,    !- Waste heat modifier curve, Speed 3 (temperature)
+      35500,                   !- Rated Total Heating Capacity, Speed 4 {W}
+      2.75,                    !- Rated COP, Speed 4
+      1.75,                    !- Rated Air Volume Flow Rate, Speed 4 {m3/s}
+      HPACHeatCapFT Speed 4,   !- Total Heating Capacity Modifier Curve, Speed 4 (temperature)
+      HPACHeatCapFF Speed 4,   !- Total Heating capacity modifier curve, Speed 4 (flow fraction)
+      HPACHeatEIRFT Speed 4,   !- Energy input ratio modifier curve, Speed 4 (temperature)
+      HPACHeatEIRFF Speed 4,   !- Energy input ratio modifier curve, Speed 4 (flow fraction)
+      HPACHeatPLFFPLR Speed 4, !- Part load fraction correlation, Speed 4 (part load ratio)
+      0.2,                     !- Rated waste heat fraction of power input, Speed 4
+      HAPCHeatWHFT Speed 4;    !- Waste heat modifier curve, Speed 4 (temperature)
+
+
+    COIL:Cooling:DX:MultiSpeed,
+      Heat Pump ACDXCoil 1,    !- Coil Name
+      FanAndCoilAvailSched,    !- Availability Schedule
+      DX Cooling Coil Air Inlet Node,  !- Coil Air Inlet Node
+      Heating Coil Air Inlet Node,  !- Coil Air Outlet Node
+      CyclingFanAndCompressor,           !- Supply Air Fan Operation Mode
+      Outdoor Condenser Air Node, !- Condenser Air Inlet Node Name
+      AirCooled,              !- Condenser Type
+      ,                        !- Name of Water Storage Tank for Supply
+      ,                        !- Name of Water Storage Tank for Condensate Collection
+      No,                      !- Apply Part Load Fraction to Speeds greater than 1
+      No,                      !- Apply Latent Degradation to Speeds greater than 1
+      200.0,                   !- Crankcase Heater Capacity {W}
+      10.0,                    !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
+      NaturalGas,              !- Fuel type
+      4,                       !- Number of speeds
+      7500,                    !- Rated Total Cooling Capacity, Speed 1 (gross) {W}
+      0.75,                    !- Rated SHR, Speed 1
+      3.0,                     !- Rated COP, Speed 1
+      0.40,                    !- Rated Air Volume Flow Rate, Speed 1 {m3/s}
+      HPACCoolCapFT Speed 1,   !- Total Cooling Capacity Modifier Curve, Speed 1 (temperature)
+      HPACCoolCapFF Speed 1,   !- Total Cooling Capacity Modifier Curve, Speed 1 (flow fraction)
+      HPACCOOLEIRFT Speed 1,   !- Energy Input Ratio Modifier Curve, Speed 1 (temperature)
+      HPACCOOLEIRFF Speed 1,   !- Energy Input Ratio Modifier Curve, Speed 1 (flow fraction)
+      HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 1 (part load ratio)
+      1000.0,                  !- Nominal Time for Condensate Removal to Begin, Speed 1 {s}
+      1.5,                     !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity, Speed 1 {dimensionless}
+      3.0,                     !- Maximum ON/OFF Cycling Rate, Speed 1 {cycles/hr}
+      45.0,                    !- Latent Capacity Time Constant, Speed 1 {s}
+      0.2,                     !- Rated waste heat fraction of power input, Speed 1 {dimensionless}
+      HAPCCoolWHFT Speed 1,    !- Waste heat modifier curve, Speed 1 (temperature)
+      0.9,                     !- Evaporative Condenser Effectiveness, Speed 1 {dimensionless}
+      0.05,                    !- Evaporative Condenser Air Volume Flow Rate, Speed 1 {m3/s}
+      50,                      !- Evaporative Condenser Pump Rated Power Consumption, Speed 1 {W}
+      17500,                   !- Rated Total Cooling Capacity, Speed 2 (gross) {W}
+      0.75,                    !- Rated SHR, Speed 2
+      3.0,                     !- Rated COP, Speed 2
+      0.85,                    !- Rated Air Volume Flow Rate, Speed 2 {m3/s}
+      HPACCoolCapFT Speed 2,   !- Total Cooling Capacity Modifier Curve, Speed 2 (temperature)
+      HPACCoolCapFF Speed 2,   !- Total Cooling Capacity Modifier Curve, Speed 2 (flow fraction)
+      HPACCOOLEIRFT Speed 2,   !- Energy Input Ratio Modifier Curve, Speed 2 (temperature)
+      HPACCOOLEIRFF Speed 2,   !- Energy Input Ratio Modifier Curve, Speed 2 (flow fraction)
+      HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 2 (part load ratio)
+      1000.0,                  !- Nominal Time for Condensate Removal to Begin, Speed 2 {s}
+      1.5,                     !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity, Speed 2 {dimensionless}
+      3.0,                     !- Maximum ON/OFF Cycling Rate, Speed 2 {cycles/hr}
+      45.0,                    !- Latent Capacity Time Constant, Speed 2 {s}
+      0.2,                     !- Rated waste heat fraction of power input, Speed 2 {dimensionless}
+      HAPCCoolWHFT Speed 2,    !- Waste heat modifier curve, Speed 2 (temperature)
+      0.9,                     !- Evaporative Condenser Effectiveness, Speed 2 {dimensionless}
+      0.1,                     !- Evaporative Condenser Air Volume Flow Rate, Speed 2 {m3/s}
+      60,                      !- Evaporative Condenser Pump Rated Power Consumption, Speed 2 {W}
+      25500,                   !- Rated Total Cooling Capacity, Speed 3 (gross) {W}
+      0.75,                    !- Rated SHR, Speed 3
+      3.0,                     !- Rated COP, Speed 3
+      1.25,                    !- Rated Air Volume Flow Rate, Speed 3 {m3/s}
+      HPACCoolCapFT Speed 3,   !- Total Cooling Capacity Modifier Curve, Speed 3 (temperature)
+      HPACCoolCapFF Speed 3,   !- Total Cooling Capacity Modifier Curve, Speed 3 (flow fraction)
+      HPACCOOLEIRFT Speed 3,   !- Energy Input Ratio Modifier Curve, Speed 3 (temperature)
+      HPACCOOLEIRFF Speed 3,   !- Energy Input Ratio Modifier Curve, Speed 3 (flow fraction)
+      HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 3 (part load ratio)
+      1000.0,                  !- Nominal Time for Condensate Removal to Begin, Speed 3 {s}
+      1.5,                     !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity, Speed 3 {dimensionless}
+      3.0,                     !- Maximum ON/OFF Cycling Rate, Speed 3 {cycles/hr}
+      45.0,                    !- Latent Capacity Time Constant, Speed 3 {s}
+      0.2,                     !- Rated waste heat fraction of power input, Speed 3 {dimensionless}
+      HAPCCoolWHFT Speed 3,    !- Waste heat modifier curve, Speed 3 (temperature)
+      0.9,                     !- Evaporative Condenser Effectiveness, Speed 3 {dimensionless}
+      0.2,                     !- Evaporative Condenser Air Volume Flow Rate, Speed 3 {m3/s}
+      80,                      !- Evaporative Condenser Pump Rated Power Consumption, Speed 3 {W}
+      35500,                   !- Rated Total Cooling Capacity, Speed 4 (gross) {W}
+      0.75,                    !- Rated SHR, Speed 4
+      3.0,                     !- Rated COP, Speed 4
+      1.75,                    !- Rated Air Volume Flow Rate, Speed 4 {m3/s}
+      HPACCoolCapFT Speed 4,   !- Total Cooling Capacity Modifier Curve, Speed 4 (temperature)
+      HPACCoolCapFF Speed 4,   !- Total Cooling Capacity Modifier Curve, Speed 4 (flow fraction)
+      HPACCOOLEIRFT Speed 4,   !- Energy Input Ratio Modifier Curve, Speed 4 (temperature)
+      HPACCOOLEIRFF Speed 4,   !- Energy Input Ratio Modifier Curve, Speed 4 (flow fraction)
+      HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 4 (part load ratio)
+      1000.0,                  !- Nominal Time for Condensate Removal to Begin, Speed 4 {s}
+      1.5,                     !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity, Speed 4 {dimensionless}
+      3.0,                     !- Maximum ON/OFF Cycling Rate, Speed 4 {cycles/hr}
+      45.0,                    !- Latent Capacity Time Constant, Speed 4 {s}
+      0.2,                     !- Rated waste heat fraction of power input, Speed 4 {dimensionless}
+      HAPCCoolWHFT Speed 4,    !- Waste heat modifier curve, Speed 4 (temperature)
+      0.9,                     !- Evaporative Condenser Effectiveness, Speed 4 {dimensionless}
+      0.3,                     !- Evaporative Condenser Air Volume Flow Rate, Speed 4 {m3/s}
+      100;                     !- Evaporative Condenser Pump Rated Power Consumption, Speed 4 {W}
+
+  Coil:Heating:Gas,
+      Supp Gas Heating Coil 1,  !- Coil Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      0.8,                     !- Gas Burner Efficiency of the Coil
+      45000,                   !- Nominal Capacity of the Coil {W}
+      SuppHeating Coil Air Inlet Node,  !- Coil\_Air\_Inlet\_Node
+      Air Loop Outlet Node;    !- Coil\_Air\_Outlet\_Node
+
+  Fan:OnOff,
+      Supply Fan 1,            !- Fan Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      0.7,                     !- Fan Total Efficiency
+      300.0,                   !- Delta Pressure {Pa}
+      1.7,                     !- Max Flow Rate {m3/s}
+      0.9,                     !- Motor Efficiency
+      1.0,                     !- Motor In Airstream Fraction
+      Mixed Air Node,          !- Fan\_Inlet\_Node
+      DX Cooling Coil Air Inlet Node;  !- Fan\_Outlet\_Node
+
+  AirTerminal:SingleDuct:Uncontrolled,
+      Zone1DirectAir,                  ! direct air unit name
+      FanAndCoilAvailSched,            ! schedule name for on/off schedule
+      Zone 1 Inlet Node,               ! zone supply air node name
+      0.612;                           ! maximum air flow rate, m3/s
+
+  AirTerminal:SingleDuct:Uncontrolled,
+      Zone2DirectAir,                  ! direct air unit name
+      FanAndCoilAvailSched,            ! schedule name for on/off schedule
+      Zone 2 Inlet Node,               ! zone supply air node name
+      0.476;                           ! maximum air flow rate, m3/s
+
+  AirTerminal:SingleDuct:Uncontrolled,
+      Zone3DirectAir,                  ! direct air unit name
+      FanAndCoilAvailSched,            ! schedule name for on/off schedule
+      Zone 3 Inlet Node,               ! zone supply air node name
+      0.612;                           ! maximum air flow rate, m3/s
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-021}
+
+\begin{itemize}
+\item
+  HVAC,Average,Unitary System Fan Part Load Ratio {[]}
+\item
+  HVAC,Average,Unitary System Compressor Part Load Ratio {[]}
+\item
+  HVAC,Average,Unitary System DX Coil Cycling Ratio {[]}
+\item
+  HVAC,Average,Unitary System DX Coil Speed Ratio {[]}
+\item
+  HVAC,Average,Unitary System DX Coil Speed Level {[]}
+\item
+  HVAC,Average,Unitary System Electric Power{[}W{]}
+\item
+  HVAC,Sum,Unitary System Electric Energy {[}J{]}
+\item
+  HVAC,Average,Unitary System Total Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Total Heating Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Latent Heating Rate {[}W{]}
+\item
+  HVAC,Average,Unitary System Ancillary Electric Power{[}W{]}
+\item
+  HVAC,Sum,Unitary System Cooling Ancillary Electric Energy {[}J{]}
+\item
+  HVAC,Sum,Unitary System Heating Ancillary Electric Energy {[}J{]}
+\end{itemize}
+
+If heat recovery is specified:
+
+\begin{itemize}
+\item
+  HVAC,Average, Unitary System Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Average, Unitary System Heat Recovery Inlet Temperature {[}C{]}
+\item
+  HVAC,Average, Unitary System Heat Recovery Outlet Temperature {[}C{]}
+\item
+  HVAC,Average, Unitary System Heat Recovery Fluid Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum, Unitary System Heat Recovery Energy {[}J{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Unitary System Fan Part Load Ratio {[]}}{Unitary System Fan Part Load Ratio }}\label{unitary-system-fan-part-load-ratio-4}
+
+This output variable is the ratio of actual air mass flow rate through the multispeed heat pump to the heat pump's design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate) at Speed 1. For continuous fan operation mode, this variable is always 1.0 when the heat pump is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating (or cooling) load to the steady-state heat pump heating (or cooling) capacity. For the cycling fan mode, the runtime fraction for the heat pump fan may be different from the fan part-load ratio reported here due the part-load performance of the heat pump's heating (or cooling) coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff). When the speed number is greater than 1, the value is 1.0.
+
+\paragraph{\texorpdfstring{Unitary System Compressor Part Load Ratio {[]}}{Unitary System Compressor Part Load Ratio }}\label{unitary-system-compressor-part-load-ratio-3}
+
+This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the multispeed heat pump's DX heating or cooling coil at Speed 1. The runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due the part-load performance of the heating/cooling coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate. When the speed number is greater than 1, the value is 1.0.
+
+\paragraph{\texorpdfstring{Unitary System DX Coil Cycling Ratio {[]}}{Unitary System DX Coil Cycling Ratio }}\label{unitary-system-dx-coil-cycling-ratio-1}
+
+This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the multispeed heat pump's DX heating or cooling coil (Speed 1) for the entire system timestep. The value is between 0.0 and 1.0 when the heat pump is cycling on and off its lowest speed (Speed 1) and 1.0 when the multispeed heat pump operates at speeds above 1.
+
+When Single Mode Operation is specified, the value is between 0.0 and 1.0 when the heat pump is cycling on at any given speed.
+
+\paragraph{\texorpdfstring{Unitary System DX Coil Speed Ratio {[]}}{Unitary System DX Coil Speed Ratio }}\label{unitary-system-dx-coil-speed-ratio-1}
+
+This output variable is the ratio of time in a system timestep that the compressor is at rated speed between two consecutive speed numbers ( {[}Compressor Speed - Compressor speed at Speed i-1{]} / {[}Compressor speed at Speed i - Compressor speed at Speed i-1{]}). The compressor speed ratio reports (1.0 is max, 0.0 is min) and any value in between as it is averaged over the timestep. The value is 0.0 during Speed 1 operation.
+
+The physical meaning of the speed ratio is dependent on the compressor configuration defined in the field of child coil object: Apply Part Load Fraction to Speeds greater than 1. The allowed choice is either Yes or No. When No is entered, one compressor is assumed for all speeds. ~The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the lower speed runs in the rest of the system timestep. When Yes is entered, multiple compressors are assumed, and each compressor has associated speed. The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the low speed runs in a whole system timestep.
+
+When Single Mode Operation is specified, the speed ratio is set to 0 at Speed 1, and 1 at Speed \textgreater{} 1
+
+\paragraph{\texorpdfstring{Unitary System DX Coil Speed Level {[]}}{Unitary System DX Coil Speed Level }}\label{unitary-system-dx-coil-speed-level-1}
+
+This output variable reports the maximum speed needed when the heat pump operates to meet the sensible load (heating or cooling) in a system timestep. When the value is 1, the heat pump operates at Speed 1 (lowest speed). For this case the cycling ratio is between 0.0 and 1.0, while the speed ratio is 0.0. When the speed number output variable is above one, such as i, the heat pump operation is determined by the speed ratio through linear interpolation. For example, when the speed ratio is 0.4 and the speed number is 3, the heat pump operates at Speed 3 for 40\% of a system timestep and at Speed 2 for 60\% of a system timestep for a single compressor. For multiple compressors, the heat pump operates at Speed 3 in the 40\% of a system timestep and at Speed 2 in the whole system timestep.
+
+\paragraph{Unitary System Total Heating Rate {[}W{]}}\label{unitary-system-total-heating-rate-w-1}
+
+This output field is the total (enthalpy) heat addition rate of the multispeed heat pump to the zones it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Total Cooling Rate {[}W{]}}\label{unitary-system-total-cooling-rate-w-1}
+
+This output field is the total (enthalpy) heat extraction rate of the multispeed heat pump from the zones it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Sensible Heating Rate {[}W{]}}\label{unitary-system-sensible-heating-rate-w-1}
+
+This output field reports the sensible heat addition rate of the multispeed heat pump to the zones it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Sensible Cooling Rate {[}W{]}}\label{unitary-system-sensible-cooling-rate-w-1}
+
+This output field reports the moist air sensible heat extraction rate of the multispeed heat pump from the zones it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Latent Heating Rate {[}W{]}}\label{unitary-system-latent-heating-rate-w-1}
+
+This output field is the latent heat addition (humidification) rate of the multispeed heat pump in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the multispeed heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Latent Cooling Rate {[}W{]}}\label{unitary-system-latent-cooling-rate-w-1}
+
+This output field is the latent heat extraction (dehumidification) rate of the multispeed heat pump in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the multispeed heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Electric Power {[}W{]}}\label{unitary-system-electric-power-w-1}
+
+This output field is the electricity consumption rate of the multispeed heat pump in Watts. The consumption includes electricity used by the DX coils (including crankcase heater if the fuel type is electricity), fans (indoor supply air fan and the condenser fans associated with the DX coil{[}s{]}), auxiliary power during on and off period, and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported. Any non-electric energy use is not reported by the heat pump object but is reported in the associated coil objects as appropriate.
+
+\paragraph{Unitary System Electric Energy {[}J{]}}\label{unitary-system-electric-energy-j-1}
+
+This output field is the electricity consumption of the multispeed heat pump in Joules for the timestep being reported. The consumption includes electricity used by the DX compressor (including crankcase heater if the fuel type is electricity), fans (indoor supply air fan and the condenser fans associated with the DX coil{[}s{]}), auxiliary power during on and off period, and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are summed for the timestep being reported. Any non-electric energy use is not reported by the heat pump object but is reported in the associated coil objects as appropriate.
+
+\paragraph{Unitary System Ancillary Electric Power {[}W{]}}\label{unitary-system-ancillary-electric-power-w-1}
+
+This output field is the average auxiliary electricity consumption rate (including both on-cycle and off-cycle) in Watts for the timestep being reported.
+
+\paragraph{Unitary System Cooling Ancillary Electric Energy {[}J{]}}\label{unitary-system-cooling-ancillary-electric-energy-j-1}
+
+This is the auxiliary electricity consumption in Joules for the timestep being reported. This is the auxiliary electricity consumption during periods when the heat pump is providing cooling (DX cooling coil is operating). This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Unitary System Heating Ancillary Electric Energy {[}J{]}}\label{unitary-system-heating-ancillary-electric-energy-j-1}
+
+This is the auxiliary electricity consumption in Joules for the timestep being reported. This is the auxiliary electricity consumption during periods when the heat pump is providing heating (DX heating coil is operating). This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Unitary System Heat Recovery Inlet Temperature {[}C{]}}\label{unitary-system-heat-recovery-inlet-temperature-c-1}
+
+\paragraph{Unitary System Heat Recovery Outlet Temperature {[}C{]}}\label{unitary-system-heat-recovery-outlet-temperature-c-1}
+
+\paragraph{Unitary System Heat Recovery Fluid Mass Flow Rate {[}kg/s{]}}\label{unitary-system-heat-recovery-fluid-mass-flow-rate-kgs-1}
+
+These outputs are the heat recovery inlet and outlet temperatures and water mass flow rate for multispeed heat pumps with heat recovery.
+
+\paragraph{Unitary System Heat Recovery Rate {[}W{]}}\label{unitary-system-heat-recovery-rate-w-1}
+
+\paragraph{Unitary System Heat Recovery Energy {[}J{]}}\label{unitary-system-heat-recovery-energy-j-1}
+
+For multispeed heat pumps with heat recovery, these outputs are the recoverable energy rate (in Watts) and energy (in Joules).
+
+\subsection{AirLoopHVAC:Unitary:Furnace:HeatOnly}\label{airloophvacunitaryfurnaceheatonly}
+
+The EnergyPlus furnace is a ``virtual'' component that consists of a fan component~ (OnOff or ConstantVolume) and a Gas or Electric heating coil component. The blow through furnace configuration is shown in the Figure below.
+
+\begin{figure}[hbtp] % fig 120
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image302.png}
+\caption{Schematic of Blow Through Furnace Model \protect \label{fig:schematic-of-blow-through-furnace-model}}
+\end{figure}
+
+Links to the fan and heating coil specifications are provided in the furnace input data syntax. In addition the control zone name and the furnace design operating conditions are specified by the furnace inputs.
+
+\subsubsection{Inputs}\label{inputs-5-033}
+
+\paragraph{Field: Name}\label{field-name-6-025}
+
+This alpha field contains the identifying name for the furnace.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-5-004}
+
+This alpha field contains the schedule name which contains information on the availability of the furnace to operate. A schedule value equal to 0 denotes that the furnace must be off for that time period. A value greater than 0 denotes that the furnace is available to operate during that time period. This schedule may be used to completely disable the unitary system as required. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Furnace Inlet Node Name}\label{field-furnace-inlet-node-name}
+
+This alpha field contains the furnace inlet node name.
+
+\paragraph{Field: Furnace Outlet Node Name}\label{field-furnace-outlet-node-name}
+
+This alpha field contains the furnace outlet node name.
+
+\textbf{\emph{Field: Supply Air Fan Operating Mode Schedule Name}}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the furnace supply air fan and the heating coil cycle on and off together to meet the heating load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating coil cycles to meet the load.
+
+\paragraph{Field: Maximum Supply Air Temperature}\label{field-maximum-supply-air-temperature-3}
+
+This numeric field contains the design operating furnace air outlet temperature in degrees C when the furnace is heating. If this input field is left blank, the default value is 80 C.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-4-000}
+
+This numeric field contains the design volumetric flow rate of the furnace in cubic meters per second. This volumetric flow rate should match the flow rate specified for the furnace fan.
+
+\paragraph{Field: Controlling Zone or Thermostat Location}\label{field-controlling-zone-or-thermostat-location-5}
+
+This alpha field contains the identifying zone name where the thermostat controlling the furnace is located.
+
+\paragraph{Field: Supply Fan Object Type}\label{field-supply-fan-object-type-3}
+
+This alpha field contains the identifying type of supply air fan specified for the furnace. Fan type must be \textbf{Fan:OnOff} or \textbf{Fan:ConstantVolume}. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e.~Supply Air Fan Operating Mode Schedule values are at times 0).
+
+\paragraph{Field: Supply Fan Name}\label{field-supply-fan-name-3}
+
+This alpha field contains the identifying name given to the furnace fan.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-4}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice stands for ``blow through fan''. This means that the unit consists of a fan followed by the heating coil. The fan ``blows through'' the heating coil. The second choice stands for ``draw through fan''. This means that the unit consists of the heating coil followed by a fan. The fan ``draws air through'' the heating coil. If this field is left blank, the default is blow through.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-5}
+
+This alpha field contains the identifying type of heating coil specified in the furnace. The hot water and steam heating coils require specifying plant loop, branches, and connectors objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat Only Furnace) itself provides the ``controller'' function of modulating water flow. Heating coil type must be:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-5}
+
+This alpha field contains the identifying name given to the furnace heating coil.
+
+As shown in the example below, correct specification of the furnace requires specification of the following objects in addition to the furnace object:
+
+1)~~~fan (Fan:OnOff or Fan:ConstantVolume)
+
+2)~~~heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
+
+3)~~~direct air unit (AirTerminal:SingleDuct:Uncontrolled) for each zone served by the furnace
+
+Note: the furnace's fan and heating coil must be connected in the air loop according to the configuration shown above (Figure~\ref{fig:schematic-of-blow-through-furnace-model}) when a blow through fan configuration is specified. If a draw through fan is used, the fan is located down stream of the heating coil. In addition, the volumetric air flow rate specified in the direct air unit for the controlling zone should properly reflect the fractional volumetric air flow rate specified in the furnace object.
+
+\begin{lstlisting}
+
+AirLoopHVAC:Unitary:Furnace:HeatOnly,
+      Gas Furnace 1,        !- Name
+      FanAndCoilAvailSched, !- Availability Schedule Name
+      Air Loop Inlet Node,  !- Furnace Air Inlet Node Name
+      Air Loop Outlet Node, !- Furnace Air Outlet Node Name
+      CycFanSchedule,       !- Supply Air Fan Operating Mode Schedule Name
+      80,                   !- Maximum Supply Air Temperature {C}
+      1.3,                  !- Heating Supply Air Flow Rate {m3/s}
+      East Zone,            !- Controlling Zone or Thermostat Location
+      Fan:OnOff,            !- Supply Fan Object Type
+      Supply Fan 1,         !- Supply Fan Fame
+      BlowThrough,          !- Fan Placement
+      Coil:Heating:Gas,     !- Heating Coil Object Type
+      Furnace Coil;         !- Heating Coil Name
+
+
+    Coil:Heating:Gas,
+      Furnace Coil,          !- Coil Name
+      FanAndCoilAvailSched,  !- Availability Schedule Name
+      0.8,                   !- Gas Burner Efficiency of the Coil
+      20000,                 !- Nominal Capacity of the Coil {W}
+      Heating Coil Air Inlet Node,  !- Coil_Air_Inlet_Node
+      Air Loop Outlet Node,         !- Coil_Air_Outlet_Node
+      ,                      !- Coil_Temp_Setpoint_Node
+      100,                   !- Parasitic Electric Load {W}
+      PLFCurveforGasFurnace, !- Part load fraction correlation (function of part load ratio)
+      10;                    !- Parasitic Gas Load {W}
+
+
+  Curve:Cubic,
+      PLFCurveforGasFurnace, !- Name
+      0.8,  !- Coefficient1 Constant
+      0.2,  !- Coefficient2 x
+      0.0,  !- Coefficient3 x**2
+      0.0,  !- Coefficient4 x**3
+      0,  !- Minimum Value of x
+      1;  !- Maximum Value of x
+
+
+    Fan:OnOff,
+      Supply Fan 1,          !- Fan Name
+      FanAndCoilAvailSched,  !- Availability Schedule Name
+      0.7,    !- Fan Total Efficiency
+      600.0,  !- Delta Pressure {Pa}
+      1.3,    !- Max Flow Rate {m3/s}
+      0.9,    !- Motor Efficiency
+      1.0,    !- Motor In Airstream Fraction
+      Air Loop Inlet Node,          !- Fan_Inlet_Node
+      Heating Coil Air Inlet Node;  !- Fan_Outlet_Node
+
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone1DirectAir,       !-Direct Air Name
+      FanAndCoilAvailSched, !- Schedule name for on/off schedule
+      Zone 1 Inlet Node,    !- Zone Supply Air Node Name
+      0.47;   !- Maximum air flow rate {m3/s}
+
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone2DirectAir,       !- Direct Air Name
+      FanAndCoilAvailSched, !- Schedule name for on/off schedule
+      Zone 2 Inlet Node,    !- Zone Supply Air Node Name
+      0.36;   !- Maximum air flow rate {m3/s}
+
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone3DirectAir,       !- Direct Air Name
+      FanAndCoilAvailSched, !- Schedule name for on/off schedule
+      Zone 3 Inlet Node,    !- Zone Supply Air Node Name
+      0.47;   !- Maximum air flow rate {m3/s}
+\end{lstlisting}
+
+Example of Heat-Only Furnace Specification
+
+\subsubsection{Outputs}\label{outputs-4-018}
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Unitary System Fan Part Load Ratio {[]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Unitary System Fan Part Load Ratio {[]}}{Unitary System Fan Part Load Ratio }}\label{unitary-system-fan-part-load-ratio-5}
+
+This output variable is the ratio of actual air mass flow rate through the furnace to the furnace's design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the furnace is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating load to the furnace heating capacity. For the cycling fan mode, the runtime fraction for the furnace fan may be different from the fan part-load ratio reported here due the part-load performance of the furnace's heating coil (delay at start-up to reach steady-state heating output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff).
+
+\subsection{AirLoopHVAC:UnitaryHeatOnly}\label{airloophvacunitaryheatonly}
+
+The AirLoopHVAC:UnitaryHeatOnly is identical to the AirLoopHVAC:Unitary:Furnace:HeatOnly model. The heat-only unitary system is a ``virtual'' component that consists of a fan component (OnOff or ConstantVolume) and a Gas or Electric heating coil component. The blow through unitary system configuraion is shown in the Figure below.
+
+\begin{figure}[hbtp] % fig 121
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image303.png}
+\caption{Schematic of Blow Through Heat-Only Unitary System \protect \label{fig:schematic-of-blow-through-heat-only-unitary}}
+\end{figure}
+
+Links to the fan and heating coil specifications are provided in the unitary system input data syntax. In addition, the control zone name and the unitary system design operating conditions are specified by the unitary system syntax.
+
+\subsubsection{Inputs}\label{inputs-6-030}
+
+\paragraph{Field: Name}\label{field-name-7-023}
+
+This alpha field contains the identifying name for the unitary system.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-6-004}
+
+This alpha field contains the schedule name which contains information on the availability of the unitary system to operate. A schedule value equal to 0 denotes that the unitary system must be off for that time period. A value greater than 0 denotes that the unitary system is available to operate during that time period. This schedule may be used to completely disable the unitary system as required. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Unitary System Air Inlet Node Name}\label{field-unitary-system-air-inlet-node-name-2}
+
+This alpha field contains the unitary system inlet node name.
+
+\paragraph{Field: Unitary System Air Outlet Node Name}\label{field-unitary-system-air-outlet-node-name-2}
+
+This alpha field contains the unitary system outlet node name.
+
+\textbf{\emph{Field: Supply Air Fan Operating Mode Schedule Name}}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the furnace supply air fan and the heating coil cycle on and off together to meet the heating load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating coil cycles to meet the load.
+
+\paragraph{Field: Maximum Supply Air Temperature}\label{field-maximum-supply-air-temperature-4}
+
+This numeric field contains the design~ air outlet temperature in degrees C when the unitary system is heating. If this input field is left blank, the default value is 80 C.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-5-000}
+
+This numeric field contains the design volumetric flow rate of the unitary system in cubic meters per second. This volumetric flow rate should match the flow rate specified for the unitary system fan.
+
+\paragraph{Field: Controlling Zone or Thermostat Location}\label{field-controlling-zone-or-thermostat-location-6}
+
+This alpha field contains the identifying zone name where the thermostat controlling the unitary system is located.
+
+\paragraph{Field: Supply Fan Object Type}\label{field-supply-fan-object-type-4}
+
+This alpha field contains the identifying type of supply air fan specified for the unitary system. Fan type must be \textbf{Fan:OnOff} or \textbf{Fan:ConstantVolume}. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e.~Supply Air Fan Operating Mode Schedule values are at times 0).
+
+\paragraph{Field: Supply Fan Name}\label{field-supply-fan-name-4}
+
+This alpha field contains the identifying name given to the unitary system fan.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-5}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice stands for ``blow through fan''. This means that the unit consists of a fan followed by the heating coil. The fan ``blows through'' the heating coil. The second choice stands for ``draw through fan''. This means that the unit consists of the heating coil followed by a fan. The fan ``draws air through'' the heating coil. If this field is left blank, the default is blow through.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-6}
+
+This alpha field contains the identifying type of heating coil specified in the unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connectors objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat Only) itself provides the ``controller'' function of modulating water flow. Heating coil type must be:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-6}
+
+This alpha field contains the identifying name given to the unitary system heating coil.
+
+As shown in the example below, correct specification of the heat-only unitary system requires specification of the following objects in addition to the unitary system object:
+
+1)~~~fan (Fan:OnOff or Fan:ConstantVolume)
+
+2)~~~heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
+
+3)~~~direct air unit (AirTerminal:SingleDuct:Uncontrolled) for each zone served by the furnace
+
+Note: the unitary system's fan and heating coil must be connected in the air loop according to the configuration shown above (Figure~\ref{fig:schematic-of-blow-through-heat-only-unitary}) when a blow through fan configuration is specified. If a draw through fan is used, the fan is located down stream of the heating coil. In addition, the volumetric air flow rate specified in the direct air unit for the controlling zone should properly reflect the fractional volumetric air flow rate specified in the unitary system object.
+
+\begin{lstlisting}
+
+AirLoopHVAC:UnitaryHeatOnly,
+      Gas Unitary System 1, !- Name
+      FanAndCoilAvailSched, !- Availability Schedule Name
+      Air Loop Inlet Node,  !- Unitary System Air Inlet Node Name
+      Air Loop Outlet Node, !- Unitary System Air Outlet Node Name
+      CycFanSchedule,       !- Supply Air Fan Operating Mode Schedule Name
+      80,                   !- Maximum Supply Air Temperature {C}
+      1.3,                  !- Heating Supply Air Flow Rate {m3/s}
+      East Zone,            !- Controlling Zone or Thermostat Location
+      Fan:OnOff,            !- Supply Fan Object Type
+      Supply Fan 1,         !- Supply Fan Name
+      BlowThrough,          !- Fan Placement
+      Coil:Heating:Gas,     !- Heating Coil Object Type
+      Unitary System Heating Coil; !- Heating Coil Name
+
+
+    Coil:Heating:Gas,
+      Unitary System Heating Coil, !- Coil Name
+      FanAndCoilAvailSched,        !- Availability Schedule Name
+      0.8,                         !- Gas Burner Efficiency of the Coil
+      20000,                       !- Nominal Capacity of the Coil {W}
+      Heating Coil Air Inlet Node, !- Coil_Air_Inlet_Node
+      Air Loop Outlet Node,        !- Coil_Air_Outlet_Node
+      ,                            !- Coil_Temp_Setpoint_Node
+      100,                         !- Parasitic Electric Load {W}
+      PLFCurveforUnitarySystem,    !- Part load fraction correlation (function of part load ratio)
+      10;                          !- Parasitic Gas Load {W}
+
+
+  Curve:Cubic,
+      PLFCurveforUnitarySystem,  !- Name
+      0.8,  !- Coefficient1 Constant
+      0.2,  !- Coefficient2 x
+      0.0,  !- Coefficient3 x**2
+      0.0,  !- Coefficient4 x**3
+      0,  !- Minimum Value of x
+      1;  !- Maximum Value of x
+
+
+  Fan:OnOff,
+      Supply Fan 1,          !- Fan Name
+      FanAndCoilAvailSched,  !- Availability Schedule Name
+      0.7,    !- Fan Total Efficiency
+      600.0,  !- Delta Pressure {Pa}
+      1.3,    !- Max Flow Rate {m3/s}
+      0.9,    !- Motor Efficiency
+      1.0,    !- Motor In Airstream Fraction
+      Air Loop Inlet Node,          !- Fan_Inlet_Node
+      Heating Coil Air Inlet Node;  !- Fan_Outlet_Node
+
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone1DirectAir,       !-Direct Air Name
+      FanAndCoilAvailSched, !- Schedule name for on/off schedule
+      Zone 1 Inlet Node,    !- Zone Supply Air Node Name
+      0.47;   !- Maximum air flow rate {m3/s}
+
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone2DirectAir,       !- Direct Air Name
+      FanAndCoilAvailSched, !- Schedule name for on/off schedule
+      Zone 2 Inlet Node,    !- Zone Supply Air Node Name
+      0.36;   !- Maximum air flow rate {m3/s}
+
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone3DirectAir,       !- Direct Air Name
+      FanAndCoilAvailSched, !- Schedule name for on/off schedule
+      Zone 3 Inlet Node,    !- Zone Supply Air Node Name
+      0.47;   !- Maximum air flow rate {m3/s}
+\end{lstlisting}
+
+Example of Heat-Only Unitary System Specification
+
+\subsubsection{Outputs}\label{outputs-5-011}
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Unitary System Fan Part Load Ratio {[]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Unitary System Fan Part Load Ratio {[]}}{Unitary System Fan Part Load Ratio }}\label{unitary-system-fan-part-load-ratio-6}
+
+This output variable is the ratio of actual air mass flow rate through the unitary system to the unitary system's design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the unitary system is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating load to the unitary system heating capacity. For the cycling fan mode, the runtime fraction for the unitary system fan may be different from the fan part-load ratio reported here due the part-load performance of the unitary system's heating coil (delay at start-up to reach steady-state heating output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff).
+
+\subsection{AirLoopHVAC:UnitaryHeatPump:WaterToAir}\label{airloophvacunitaryheatpumpwatertoair}
+
+The unitary water-to-air heat pump is similar to the unitary air-to-air heat pump except water is used on the source side. Links to the fan, WaterToAirHeatPump cooling coil, WaterToAirHeatPump heating coil, and supplementary heating coil specifications are provided in the heat pump's input data syntax. The heat pump switches between cooling and heating depending on the zone's demand. The load side (air) of the unitary water-to-air heat pump consists of an On/Off fan component, a WaterToAirHeatPump cooling coil component, a WaterToAirHeatPump heating coil component, and a Gas, Electric, Steam, or Hot Water supplemental heating coil component. The source side (water) of the heat pump is connected to a condenser loop with a heat exchanger (ground heat exchanger or other type) or a plant loop with a heating source such as a boiler and a cooling source such as a chiller or cooling tower. The diagram below shows the setup and connection of the heat pump for the source side and load side for a ground heat exchanger configuration. Note that on the load side, the WaterToAirHeatPump cooling coil must always be placed before the WaterToAirHeatPump heating coil.
+
+There are three type of WaterToAirHeatPump coil models available:
+
+\begin{itemize}
+\item
+  Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
+\item
+  Coil:Heating:WaterToAirHeatPump:ParameterEstimation
+\item
+  Coil:Cooling:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Heating:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Cooling:WatertoAirHeatPump:VariableSpeedEquationFit
+\item
+  Coil:Heating:WatertoAirHeatPump:VariableSpeedEquationFit
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 122
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image304.png}
+\caption{Water to Air Heat Pump Schematic for a BlowThrough Configuration with Ground Heat Exchanger \protect \label{fig:water-to-air-heat-pump-schematic-for-a}}
+\end{figure}
+
+In addition, the control zone name and the system design operating conditions are specified by the heat pump inputs.
+
+\subsubsection{Inputs}\label{inputs-7-029}
+
+\paragraph{Field: Name}\label{field-name-8-023}
+
+This alpha field contains the identifying name for the unitary system heat pump.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-7-004}
+
+This alpha field contains the schedule name (ref. Schedule objects) that contains information on the availability of the heat pump to operate. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-2-002}
+
+This alpha field contains the name of the HVAC system node from which the heat pump draws its inlet air.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-2-002}
+
+This alpha field contains the name of the HVAC system node to which the heat pump sends its outlet air.
+
+\paragraph{Field: Supply Air Flow Rate}\label{field-supply-air-flow-rate}
+
+This numeric field contains the design volumetric flow rate through the heat pump in cubic meters per second. This volume flow rate is only used when the cooling and heating coil object type is Coil:*:WaterToAirHeatPump:ParameterEstimation. Although a value greater than 0 is required (input cannot be blank or 0), this input is not used for the EquationFit model. Instead, the supply air flow rate is determined by the input in the corresponding Coil:*:WaterToAirHeatPump:EquationFit objects.
+
+\paragraph{Field: Controlling Zone or Thermostat Location}\label{field-controlling-zone-or-thermostat-location-7}
+
+This alpha field contains the identifying zone name where the thermostat controlling the heat pump is located.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-2}
+
+This alpha field contains the identifying type of supply air fan specified in the heat pump. Fan type must be Fan:OnOff.
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-2}
+
+This alpha field contains the identifying name given to the heat pump supply air fan, and should match the name specified in the corresponding fan object.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-7}
+
+This alpha field contains the identifying type of heating coil specified in the heat pump. Heating coil types are:
+
+\begin{itemize}
+\item
+  Coil:Heating:WaterToAirHeatPump:ParameterEstimation
+\item
+  Coil:Heating:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit
+\end{itemize}
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-7}
+
+This alpha field contains the identifying name given to the WaterToAirHeatPump heating coil, and should match the name specified in the corresponding WaterToAirHeatPump heating coil object.
+
+\paragraph{Field: Heating Convergence}\label{field-heating-convergence}
+
+This numeric value allows the user to determine how close the air side has to be controlled. Lower the value of convergence better the control of air side conditions and less the zone temperature fluctuations. However in a poorly designed system, a lower convergence might result in warning errors which are caused due to the iteration limit for run time fraction calculation is limited to 20.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-5}
+
+This alpha field contains the identifying type of cooling coil specified in the heat pump. Cooling coil types are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
+\item
+  Coil:Cooling:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit
+\end{itemize}
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-5}
+
+This alpha field contains the identifying name given to the WaterToAirHeatPump cooling coil, and should match the name specified in the corresponding WaterToAirHeatPump cooling coil object.
+
+\paragraph{Field: Cooling Convergence}\label{field-cooling-convergence}
+
+This numeric value allows the user to determine how close the air side has to be controlled. Lower the value of convergence better the control of air side conditions and less the zone temperature fluctuations. However in a poorly designed system, a lower convergence might result in warning errors which are caused due to the iteration limit for run time fraction calculation is limited to 20.
+
+\paragraph{Field: Maximum Cycling Rate}\label{field-maximum-cycling-rate-1-000}
+
+This numeric field contains the maximum on-off cycling rate for the compressor, which occurs at 50\% run time fraction. Suggested values are shown below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image305.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Heat Pump Time Constant}\label{field-heat-pump-time-constant-1}
+
+This numeric field contains the time constant for the cooling coil's capacity to reach steady state after startup. Suggested values are shown below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image306.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Fraction of On-Cycle Power Use}\label{field-fraction-of-on-cycle-power-use-1}
+
+This numeric field contains the fraction of on-cycle power use to adjust the part load fraction based on the off-cycle power consumption due to crankcase heaters, controls, fans, and etc. Suggested value values are below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image307.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Heat Pump Fan Delay Time}\label{field-heat-pump-fan-delay-time-1}
+
+This numeric field contains the time delay for the heat pump supply air fan to shut off after the compressor cycles off in seconds. This value can be obtained from the manufacturer or the heat pump catalog. Enter a value of zero when the heat pump's fan operating mode is continuous. Suggested value is 60 seconds.
+
+\paragraph{Field: Supplemental Heating Coil Object Type}\label{field-supplemental-heating-coil-object-type-3}
+
+This is the object type of the supplemental heating coil. The hot water and steam heating coils require specifying plant loop, branches, and connectors objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the supplemental heating coil does not require additional controller or Controller:WaterCoil object. The parent object (AirLoop Unitary Water to Air Heat Pump) itself provides the ``controller'' function of modulating water flow. The valid choices are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Supplemental Heating Coil Name}\label{field-supplemental-heating-coil-name-3}
+
+This alpha field contains the identifying name given to the supplemental heating coil, and should match the name specified in the corresponding supplemental heating coil object.
+
+\paragraph{Field: Maximum Supply Air Temperature from Supplemental Heater}\label{field-maximum-supply-air-temperature-from-supplemental-heater-2}
+
+This numeric field defines the maximum allowed supply air temperature exiting the heat pump supplemental heating coil in degrees Celsius.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-supplemental-heater-operation-3}
+
+This numeric field defines the outdoor air dry-bulb temperature in degrees Celsius above which the heat pump supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21°C. If this input field is left blank, the default value is 21°C.
+
+\paragraph{Field: Outdoor Dry-Bulb Temperature Sensor Node Name}\label{field-outdoor-dry-bulb-temperature-sensor-node-name-1}
+
+This alpha field specifies the name of the outdoor node which controls the operation of the supplemental heating coil. If this field is left blank, the outdoor temperature is based solely on the weather data. If this field is not blank, the node name specified must also be listed in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor temperature from the weather data. Alternately, the node name must be specified in an OutdoorAir:NodeList object where the outdoor temperature is taken directly from the weather data.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-6}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice represents a blow through system where the supply air fan is before the WaterToAirHeatPump cooling/heating coil and the supplementary heating coil. The second choice represents a draw through system where the supply fan is between the WaterToAirHeatPump cooling/heating coil and the supplementary heating coil. If this input field is left blank, the default is blow through.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-2}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating/cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply air fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, the model assumes the supply air fan cycles with the heating or cooling coil throughout the simulation period.
+
+As shown in the example below, correct specification of the water-to-air heat pump requires specification of the following objects in addition to the AirLoopHVAC:UnitaryHeatPump:WaterToAir object:
+
+\begin{itemize}
+\item
+  On/Off fan
+\item
+  WaterToAirHeatPump cooling coil
+\item
+  WaterToAirHeatPump heating coil
+\item
+  Supplementary heating coil
+\item
+  Direct air unit for each zone served by the heat pump
+\item
+  Condenser demand branches
+\end{itemize}
+
+It should be noted that the volumetric air flow rate specified in the direct air unit for the controlling zone should properly reflect the fractional volumetric air flow rate specified in the heat pump object.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-4-000}
+
+This alpha input field contains the type of dehumidification control. The following options are valid for this field:
+
+\textbf{None} - meet sensible load only, no active dehumidification control
+
+\textbf{CoolReheat} - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. The excess cooling beyond the cooling set point temperature is offset by the supplemental heating coil.
+
+The default is \textbf{None}. For \textbf{CoolReheat} dehumidification control modes, the maximum humidity setpoint is required. This must be set using a \textbf{ZoneControl:Humidistat} object. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate. Supplemental heating coil (supplemental heating coil type and name) is a required input in WaterToAir HeatPumps. When dehumidification control is active the heating and the reheat load due to extra dehumidification are met with supplemetal heating coil. The supplemental heating coil capacity must be adequate enough to meet the heating coil load and offset the excess cooling load due to~ extra dehumidification. The dehumidification control type CoolReheat works only with Coil:Cooling:WaterToAirHeatPump:EquationFit cooling coil type.
+
+\paragraph{Field: Heat Pump Coil Water Flow Mode}\label{field-heat-pump-coil-water-flow-mode-000}
+
+This field specifies the way in which water flow through the heat pump coils will be modeled.~ This field is only used when WatertoAirHeatPump:EquationFit coils are used. There are three options:
+
+\begin{itemize}
+\item
+  Cycling
+\item
+  Constant
+\item
+  CyclingOnDemand
+\end{itemize}
+
+\textbf{Cycling} varies water flow through the coil based on the heat pump Part Load Ratio.~ This control method is appropriate for modeling heat pumps that are outfitted with a soleniod valve which allows water to flow through the coil only when the compressor is active. This is the default for EnergyPlus V8 and later.
+
+\textbf{Constant} provides a constant water flow regardless of heat pump operation.~ Remember that EnergyPlus has two coils (a heating coil and a cooling coil) to approximate the operation of one coil that can operate in either heating mode or cooling mode.~ Therefore, when the water flow mode is constant, there will be full flow through either the heating coil or the cooling coil, but not both at the same time.
+
+\textbf{ConstantOnDemand} provides full flow through the coil whenever there is a load.~ When there is no load, there is zero flow through the coil.~ This control strategy represents the way EnergyPlus modeled heat pump water flow prior to Version 8.
+
+Following is an example of IDF usage:
+
+\begin{lstlisting}
+
+AirLoopHVAC:UnitaryHeatPump:WaterToAir,
+      DXAC Heat Pump 1,        !- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      Mixed Air Node,          !- Air Inlet Node Name
+      Air Loop Outlet Node,    !- Air Outlet Node Name
+      2,                       !- Supply Air Flow Fate {m3/s}
+      East Zone,               !- Controlling Zone or Thermostat Location
+      Fan:OnOff,        !- Supply Air Fan Object Type
+      Supply Fan 1,            !- Supply Air Fan Name
+      Coil:Heating:WaterToAirHeatPump:ParameterEstimation,  !- Heating Coil Object Type
+      Heat Pump Heating Mode,  !- Heating Coil Name
+      0.001,                   !- Heating Convergence
+      Coil:Cooling:WaterToAirHeatPump:ParameterEstimation,  !- Cooling Coil Object Type
+      Heat Pump Cooling Mode,  !- Cooling Coil Name
+      0.001,                   !- Cooling Convergence
+      2.5, !- Maximum Cycling Rate {cycles/hr}
+      60, !- Heat Pump Time Constant {s}
+      0.01, !- Fraction of On-Cycle Power Use
+      60,    !- Heat Pump Fan Delay Time {s}
+      Coil:Heating:Gas,        !- Supplemental Heating Coil Object Type
+      Heat Pump DX Supp Heating Coil 1,  !- Supplemental Heating Coil Name
+      50,                      !- Maximum Supply Air Temperature from Supplemental Heater {C}
+      21,                      !- Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation {C}
+      Outside Air Inlet Node, !- Outdoor Dry-Bulb Temperature Sensor Node Name
+      BlowThrough,             !- Fan Placement
+      CyclingFanSch,           !- Supply Air Fan Operating Mode Schedule Name
+      CoolReheat;              !- Dehumidification Control Type
+
+
+  Schedule:Compact,
+      CyclingFanSch,           !- Name
+      Fraction,                !- Schedule Type Limits Name
+      Through: 12/31,          !- Field 1
+      For: AllDays,            !- Field 2
+      Until: 24:00,            !- Field 3
+      0.0;                     !- Field 4
+
+
+
+
+    Coil:Cooling:WaterToAirHeatPump:ParameterEstimation,
+      Heat Pump Cooling Mode,  !- Name
+      Scroll,                !- Compressor Type
+      R22,                   !- Refrigerant Type
+      0.0015,                  !- Design Source Side Flow Rate {m3/s}
+      38000,  !- Nominal Cooling Coil Capacity {W)
+      0,            !- Nominal Time for Condensate Removal to Begin {s}
+      0,      !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity
+      3000000,                 !- High Pressure CutOff {Pa}
+      0,                       !- Low Pressure CutOff {Pa}
+      Water to Air Heat Pump Source Side1 Inlet Node,  !- Water Inlet Node Name
+      Water to Air Heat Pump Source Side1 Outlet Node,  !- Water Outlet Node Name
+      Cooling Coil Air Inlet Node,  !- Air Inlet Node Name
+      Heating Coil Air Inlet Node,  !- Air Outlet Node Name
+      3.78019E+03,!-Parameter 1 {W/K}
+      2.80303E+03,!- Parameter 2 {W/K}
+     7.93591E-01,!- Parameter 3 {C}
+      1.91029E+03,!- Parameter 4 {W}
+      2.66127E+00,!- Parameter 5
+      1.06009E-02,!- Parameter 6
+      1.65103E+00,!- Parameter 7
+      9.73887E-03,!- Parameter 8
+      1.04563E+03;!- Parameter 9
+
+
+
+
+   Coil:Heating:WaterToAirHeatPump:ParameterEstimation,
+      Heat Pump HEATING Mode,  !- Name
+      Scroll,                !- Compressor Type
+      R22,                   !- Refrigerant Type
+      0.0015,                  !- Design Source Side Flow Rate {m3/s}
+      38000,                   !- Nominal Heating Coil Capacity {W}
+      3000000,                 !- High Pressure CutOff
+      0,                       !- Low Pressure CutOff {Pa}
+      Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
+      Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
+      Heating Coil Air Inlet Node,  !- Air Inlet Node Name
+      SuppHeating Coil Air Inlet Node,  !- Air Outlet Node Name
+      3.91379E+03,  !-Parameter 1 {W/K}
+      5.94753E-01,  !- Parameter 2 {C}
+      2.49945E+03,  !- Parameter 3 {W}
+      8.68734E-01,  !- Parameter 4
+      7.23595E-03,  !- Parameter 5
+      3.69126E+00,  !- Parameter 6
+      1.75701E-05,  !- Parameter 7
+      3.65348E+03;  !-Parameter 8
+
+
+
+
+    Coil:Heating:Gas,
+      Heat Pump DX Supp Heating Coil 1,  !- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      0.8,                     !- Gas Burner Efficiency
+      32000,                   !- Nominal Capacity {W}
+      SuppHeating Coil Air Inlet Node,  !- Air Inlet Node Name
+      Air Loop Outlet Node;    !- Air Outlet Node Name
+
+
+
+
+    BRANCH,
+      Gshp Cooling Condenser Branch,  !- Name
+      0,  !- Maximum Flow Rate {m3/s}
+       , !- Pressure Drop Curve Name
+      Coil:Cooling:WaterToAirHeatPump:ParameterEstimation,  !- Component 1 Object Type
+      Heat Pump Cooling Mode,  !- Component 1 Name
+      Water to Air Heat Pump Source Side1 Inlet Node, !- Component 1 Inlet Node Name
+      Water to Air Heat Pump Source Side1 Outlet Node, !- Component 1 Outlet Node Name
+      ACTIVE;  !- Component 1 Branch Control Type
+
+
+    BRANCH,
+      Gshp Heating Condenser Branch,  !- Name
+      0,  !- Maximum Flow Rate {m3/s}
+      , !- Pressure Drop Curve Name
+      Coil:Heating:WaterToAirHeatPump:ParameterEstimation,  !- Component 1 Object Type
+      Heat Pump Heating Mode,  !- Component 1 Name
+      Water to Air Heat Pump Source Side2 Inlet Node,  !- Component 1 Inlet Node Name
+      Water to Air Heat Pump Source Side2 Outlet Node,  !- Component 1 Outlet Node Name
+      ACTIVE;  !- Component 1 Branch Control Type
+
+
+
+
+    Fan:OnOff,
+      Supply Fan 1,          !- Name
+      FanAndCoilAvailSched,  !- Availability Schedule Name
+      0.7,                   !- FanTotal Efficiency
+      300.0,                 !– Pressure Rise {Pa}
+      2.0,                   !- Maximum Flow Rate {m3/s}
+      0.9,                   !- Motor Efficiency
+      1.0,                   !- Motor In Airstream Fraction
+      Mixed Air Node,        !- Air Inlet_Node Name
+      Cooling Coil Air Inlet Node;  !- Air Outlet Node Name
+
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone1DirectAir,        !- Name
+      FanAndCoilAvailSched,  !- Availability Schedule Name
+      Zone 1 Inlet Node,     !- Zone Supply Air Node Name
+      0.7;                   !- Maximum Air Flow Rate {m3/s}
+
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone2DirectAir,        !- Name
+      FanAndCoilAvailSched,  !- Availability Schedule Name
+      Zone 2 Inlet Node,     !- Zone Supply Air Node Name
+      0.6;                   !- Maximum Air Flow Rate {m3/s}
+
+
+    AirTerminal:SingleDuct:Uncontrolled,
+      Zone3DirectAir,        !- Name
+      FanAndCoilAvailSched,  !- Availability Schedule Name
+      Zone 3 Inlet Node,     !- Zone Supply Air Node Name
+      0.7;                   !- Maximum Air Flow Rate {m3/s}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-011}
+
+Energy use reporting for the water-to-air heat pump is documented under the heat pump coil object types:
+
+\begin{itemize}
+\item
+  Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
+\item
+  Coil:Heating:WaterToAirHeatPump:ParameterEstimation
+\item
+  Coil:Cooling:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Heating:WaterToAirHeatPump:EquationFit
+\end{itemize}
+
+The heat pump \emph{demand} as well as the compressor and fan part-load ratios may be obtained with the output variables shown below.
+
+\begin{itemize}
+\item
+  HVAC,Average, Unitary System Requested Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average, Unitary System Requested Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Average, Unitary System Requested Heating Rate {[}W{]}
+\item
+  HVAC,Average, Unitary System Compressor Part Load Ratio {[]}
+\item
+  HVAC,Average, Unitary System Fan Part Load Ratio
+\item
+  HVAC,Average, Unitary System Dehumidification Induced Heating Demand Rate {[}W{]}
+\end{itemize}
+
+\paragraph{Unitary System Requested Sensible Cooling Rate {[}W{]}}\label{unitary-system-requested-sensible-cooling-rate-w-1}
+
+This output variable is the sensible cooling requested from the zone thermostat in watts. This value is calculated using the unitary heat pump outlet air and zone conditions, the specific heat of the zone air, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{Unitary System Requested Latent Cooling Rate {[}W{]}}\label{unitary-system-requested-latent-cooling-rate-w-1}
+
+This output variable is the latent cooling requested from the zone humidistat in watts. This value is calculated using the unitary heat pump outlet air and zone conditions, the heat of vaporization of water at the current zone conditions, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{Unitary System Requested Heating Rate {[}W{]}}\label{unitary-system-requested-heating-rate-w-1}
+
+This output variable is the sensible heating requested from the zone thermostat in watts. This value is calculated using the unitary heat pump outlet air and zone conditions, the specific heat of the zone air, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{\texorpdfstring{Unitary System Compressor Part Load Ratio {[]}}{Unitary System Compressor Part Load Ratio }}\label{unitary-system-compressor-part-load-ratio-4}
+
+This output variable is the ratio of actual load on the unitary system to the unitary system's steady state output.~ This ratio is based on the nominal capacity of the unit.
+
+\paragraph{\texorpdfstring{Unitary System Fan Part Load Ratio {[]}}{Unitary System Fan Part Load Ratio }}\label{unitary-system-fan-part-load-ratio-7}
+
+This output variable is the ratio of actual air mass flow rate through the unitary system to the unitary system's design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the unitary system is available (based on the availability schedule).
+
+\paragraph{Unitary System Dehumidification Induced Heating Demand Rate {[}W{]}}\label{unitary-system-dehumidification-induced-heating-demand-rate-w-1}
+
+This output variable is the additional heating demand rate of the supplemental heating coil of a Water-to-Air heat pumps in Watts.~ This additional heating demand is induced when zone air overshoots the heating setpoint due to extra dehumidification requirement to meet the high humidity setpoint. This value is always positive. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
+
+\subsection{AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass}\label{airloophvacunitaryheatcoolvavchangeoverbypass}
+
+The changeover-bypass variable air volume (CBVAV) unitary system is a compound object made up of other components. Each CBVAV system consists of an outdoor air mixer, direct expansion (DX) cooling coil, heating coil, and a supply air fan as shown in the figures below. Zone thermostats and terminal units are required in each zone served by this system. The terminal units are specific to this system type and are either AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat or AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat. A zone humidistat and single zone max humidity set point manager may also be specified to help control high humidity levels. These individual components are described elsewhere in this document. The CBVAV unitary system object coordinates the operation of these components and is modeled as a type of air loop equipment (Ref. AirLoopHVAC).
+
+\begin{figure}[hbtp] % fig 123
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image308.png}
+\caption{Schematic of a CBVAV unitary system (draw through fan placement) \protect \label{fig:schematic-of-a-cbvav-unitary-system-draw}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 124
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image309.png}
+\caption{Schematic of a CBVAV unitary system (blow through fan placement) \protect \label{fig:schematic-of-a-cbvav-unitary-system-blow}}
+\end{figure}
+
+Links to the CBVAV system's supply air fan, coils, and outdoor air mixer specifications are provided in the object's input syntax. Additional inputs include system and outdoor air flow rates during heating and cooling operation, the priority control mode, and dehumidification control type. A description of each input field for the CBVAV unitary system compound object is provided below.
+
+\subsubsection{Inputs}\label{inputs-8-027}
+
+\paragraph{Field: Name}\label{field-name-9-020}
+
+This alpha field defines a unique user-assigned name for an instance of a changeover-bypass VAV system. Any reference to this system by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-8-004}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the system operates during a given time period. A schedule value equal to 0 denotes that the system must be off for that time period, and a schedule value greater than 0 denotes that the system is available to operate during that time period. This schedule may be used to completely disable the system (all of its coils and the supply air fan) as required. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-4-000}
+
+This numeric field defines the air flow rate through the system (i.e., through the fan and heating/cooling coils) in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0, or this field is autosizable.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-6}
+
+This numeric field defines the air flow rate through the system (i.e., through the fan and heating/cooling coils) in cubic meters per second when the heating coil is operating. Values must be greater than 0, or this field is autosizable.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-5}
+
+This numeric field defines the air flow rate through the system (i.e., through the fan and heating/cooling coils) in cubic meters per second when neither cooling nor heating is required (i.e., the DX cooling coil and heating coil are off but the supply air fan operates). Values must be greater than or equal to zero, or this field is autosizable. This field is only used when the unitary system's supply air fan operating mode is specified as continuous fan operation (Ref. Field: Supply air fan operating mode schedule name). If the system's supply air fan operating mode is specified as continuous fan operation and this value is set to zero or the field is left blank, then the model assumes that the system air flow rate when no heating/cooling is needed is equal to the system air flow rate when the coils were last operating (for cooling operation or heating operation).
+
+\paragraph{Field: Cooling Outdoor Air Flow Rate}\label{field-cooling-outdoor-air-flow-rate-000}
+
+This numeric field defines the outdoor air flow rate through the system (i.e., through the Outdoor air Mixer's Outside\_Air\_Stream\_Node) in cubic meters per second when the DX cooling coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Cooling Outdoor Air Flow Rate can be changed during the simulation using a multiplier schedule (Ref. Field: Outdoor air volumetric flow rate multiplier schedule name). For any simulation timestep, the Cooling Outdoor Air Flow Rate cannot exceed the system air volumetric flow rate during cooling operation.
+
+\paragraph{Field: Heating Outdoor Air Flow Rate}\label{field-heating-outdoor-air-flow-rate-000}
+
+This numeric field defines the outdoor air flow rate through the system (i.e., through the Outdoor air Mixer's Outside\_Air\_Stream\_Node) in cubic meters per second when the heating coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Heating Outdoor Air Flow Rate can be changed during the simulation using a multiplier schedule (Ref. Field: Outdoor air volumetric flow rate multiplier schedule name). For any simulation timestep, the Heating Outdoor Air Flow Rate cannot exceed the system air volumetric flow rate during heating operation.
+
+\paragraph{Field: No Load Outdoor Air Flow Rate When No Cooling or Heating is Needed}\label{field-no-load-outdoor-air-flow-rate-when-no-cooling-or-heating-is-needed}
+
+This numeric field defines the outdoor air flow rate through the system (i.e., through the Outdoor air Mixer's Outside\_Air\_Stream\_Node) in cubic meters per second when neither cooling nor heating is required (i.e., the DX cooling coil and heating coil are off but the supply air fan operates). Values must be greater than or equal to 0, or this field is autosizable. Note that the no load outdoor air flow rate can be changed during the simulation using a multiplier schedule (Ref. Field: Outdoor air volumetric flow rate multiplier schedule name). For any simulation timestep, the no load outdoor air flow rate cannot exceed the no load supply air flow rate. This field is only used when the unitary system's supply air fan operating mode is specified as continuous fan operation (Ref. Field: Supply air fan operating mode schedule name). If the system's supply air fan operating mode is specified as continuous fan operation and this value is set to zero or the field is left blank, then the model assumes that the no load outdoor air flow rate is equal to the outdoor air flow rate when the coils were last operating (for cooling operation {[}i.e.~Cooling outdoor air flow rate{]} or heating operation {[}i.e.~Heating outdoor air flow rate{]}) and this field is not used.
+
+\paragraph{Field: Outdoor Air Flow Rate Multiplier Schedule Name}\label{field-outdoor-air-flow-rate-multiplier-schedule-name}
+
+This alpha field defines the name of a schedule (ref: Schedule) that contains multipliers for the outdoor air volume flow rates (heating, cooling, no heating/cooling). Schedule values must be from zero to 1. If this field is left blank, then the model assumes that the outdoor air multiplier is 1 for the entire simulation period.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-3-002}
+
+This alpha field defines the name of the HVAC system node from which the system draws its inlet air.
+
+\paragraph{Field: Bypass Duct Mixer Node Name}\label{field-bypass-duct-mixer-node-name}
+
+This alpha field defines the name of the HVAC system node where the bypass air mixes with the unitary system's inlet air. This name should match the name of the Return Air Stream Node Name for the OutdoorAir:Mixer associated with this system. This node name must be different from the system's air inlet node name.
+
+\paragraph{Field: Bypass Duct Splitter Node Name}\label{field-bypass-duct-splitter-node-name}
+
+This alpha field defines the name of the HVAC system node where the conditioned air is split into bypass air and supply air leaving the system (e.g., delivered to the terminal units). This splitter air node name should match the outlet node name for the last component (furthest downstream) in this unitary system. For blow through fan placement, the splitter air node is the outlet node of the heating coil. For draw through fan placement, the splitter node is the outlet node of the supply air fan.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-3-002}
+
+This alpha field defines the name of the HVAC system node to which the system sends its outlet air.
+
+\paragraph{Field: Outdoor Air Mixer Object Type}\label{field-outdoor-air-mixer-object-type}
+
+This field specifies the type of outdoor air mixer used by this CBVAV unitary system. The outdoor air mixer component is part of the CBVAV unitary compound object. The only available outdoor air mixer type is:
+
+\begin{itemize}
+\tightlist
+\item
+  OutdoorAir:Mixer
+\end{itemize}
+
+\paragraph{Field: Outdoor Air Mixer Name}\label{field-outdoor-air-mixer-name}
+
+This alpha field defines the name of an outdoor air mixer component that composes part of the CBVAV system. The name of the outdoor air mixer's Return\_Air\_Stream\_Node should match the bypass duct mixer node name, and be different from the CBVAV system's air inlet node name. The Mixed Air Node Name of the outdoor air mixer should be the same as the CBVAV system's supply fan inlet air node (for blow through fan placement) or the system's DX cooling coil inlet node (for draw through fan placement).
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-3}
+
+This alpha field defines the type of fan used by this unitary system. The only valid choices are \textbf{Fan:OnOff} and \textbf{Fan:ConstantVolume}. The input requirements for these fan objects are described elsewhere in this document.
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-3}
+
+This alpha field defines the name of the fan component that composes part of this unitary system. Note that the fan component's maximum flow rate should be greater than or equal to the largest system air volumetric flow rate specified for this unitary system (heating, cooling, and no heating/cooling). In addition, the fan's inlet air node should be the same as the outdoor air mixer's Mixed Air Node (for blow through fan placement) or the heating coil's outlet node (for draw through fan placement). The fan outlet air node should be the same as the DX cooling coil's air inlet node (for blow through fan placement) or the system's bypass duct splitter node (for draw through fan placement).
+
+\paragraph{Field: Supply Air Fan Placement}\label{field-supply-air-fan-placement-1}
+
+This alpha field defines the placement of the supply air fan within this unitary system. The only valid choices are \textbf{BlowThrough} and \textbf{DrawThrough}. With blow through placement, the supply air fan is located immediately upstream of the system's cooling coil. With draw through placement, the supply air fan is located immediately downstream of the heating coil.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-3}
+
+This alpha field defines the name of a schedule that specifies the supply air fan operating mode during the simulation. A schedule value of 0 denotes the fan cycles off when no cooling or heating is required, and any other value denotes that the fan runs continuously regardless of the need for heating or cooling. If this field is left blank, the model assumes continuous supply air fan operation for the entire simulation period.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-6}
+
+This alpha field defines the type of cooling coil used by this unitary system. There are three valid choices for this field:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted
+\item
+  Coil:Cooling:DX:TwoStageWithHumidityControlMode
+\end{itemize}
+
+The input requirements for these cooling coil objects are described elsewhere in this document.
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-6}
+
+This alpha field defines the name of the cooling coil used by this unitary system, and this name should match the name specified in the corresponding cooling coil object.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-8}
+
+This alpha field defines the type of heating coil used by this unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (CBVAV Unitary System) itself provides the ``controller'' function of modulating water flow. The valid choices are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:DX:SingleSpeed
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+The input requirements for these heating coil objects are described elsewhere in this document.
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-8}
+
+This alpha field defines the name of the heating coil used by this unitary system, and this name should match the name specified in the corresponding heating coil object.
+
+\paragraph{Field: Priority Control Mode}\label{field-priority-control-mode}
+
+This choice field defines the cooling or heating priority control mode for the unitary system. Valid choices are:
+
+\begin{itemize}
+\item
+  CoolingPriority
+\item
+  HeatingPriority
+\item
+  ZonePriority
+\end{itemize}
+
+If CoolingPriority is selected, the system operates to meet the cooling load if any zone served by this system (air loop) requires cooling. If no zones require cooling, then the system operates in heating mode if needed. If HeatingPriority is selected, the system operates to meet the heating load if any zone requires heating. If no zones require heating, then the system operates in cooling mode if needed. If ZonePriority is selected, the system operates based on the maximum number of zones requiring either heating or cooling. If the number of zones requiring cooling is greater than the number of zones requiring heating, then the system operates in cooling mode. If the number of zones requiring heating is greater than the number of zones requiring cooling, then the system operates in heating mode. If the number of zones requiring cooling equals the number of zones requiring heating, then the largest combined load (i.e., the sum of the cooling loads for zones requiring cooling compared to the sum of the heating loads for zones that require heating) sets the cooling or heating operating mode for the system during that simulation timestep.
+
+\paragraph{Field: Minimum Outlet Air Temperature During Cooling Operation}\label{field-minimum-outlet-air-temperature-during-cooling-operation}
+
+This numeric field defines the minimum outlet air temperature leaving the system when the unit is operating to provide cooling. Values are specified in degrees Celsius and must be greater than 0. The default value is 8°C. This value must be less than or equal to the maximum outlet air temperature during heating operation.
+
+\paragraph{Field: Maximum Outlet Air Temperature During Heating Operation}\label{field-maximum-outlet-air-temperature-during-heating-operation}
+
+This numeric field defines the maximum outlet air temperature leaving the system when the unit is operating to provide heating. Values are specified in degrees Celsius and must be greater than 0. The default value is 50°C. This value must be greater than or equal to the minimum outlet air temperature during cooing operation.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-5-000}
+
+This alpha field contains the type of dehumidification control. The following options are valid for this field:
+
+\textbf{None} - meet sensible load only, no active dehumidification control
+
+\textbf{Multimode} - activate enhanced dehumidification mode as needed and meet sensible load. This option is used to model DX equipment with a controllable heat exchanger assisting the DX cooling coil for improved dehumidification. It is valid only with cooling coil type = Coil:Cooling:DX:TwoStageWithHumidityControlMode.
+
+\textbf{CoolReheat} - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. It is valid only with cooling coil type = Coil:Cooling:DX:TwoStageWithHumidityControlMode.
+
+The default is \textbf{None}. For the other dehumidification control modes, the maximum humidity setpoint on the CBVAV system's air outlet node is used. This must be set using a \textbf{ZoneControl:Humidistat} and one of:
+
+\begin{itemize}
+\item
+  \textbf{SetpointManager:SingleZone:Humidity:Maximum}
+\item
+  \textbf{SetpointManager:MultiZone:Humidity:Maximum}
+\item
+  \textbf{SetpointManager:MultiZone:MaximumHumidity:Average}
+\end{itemize}
+
+objects. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate.
+
+As shown in the example below, correct specification of the CBVAV unitary system requires specification of the following objects in addition to the AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass object:
+
+1)~~~outdoor air mixer (OutdoorAir:Mixer)
+
+2)~~~fan (Fan:OnOff or Fan:ConstantVolume)
+
+3)~~~cooling coil (Coil:Cooling:DX:SingleSpeed, CoilSystem:Cooling:DX:HeatExchangerAssisted, or Coil:Cooling:DX:TwoStageWithHumidityControlMode)
+
+4)~~~heating coil (Coil:Heating:Gas, Coil:Heating:Electric, or Coil:Heating:DX:SingleSpeed)
+
+5)~~~terminal unit for each zone being served by this system (AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat or AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat)
+
+Note: The fan, heating coil, cooling coil, and outdoor air mixer must be connected in the air loop according to the configurations shown above (Figure~\ref{fig:schematic-of-a-cbvav-unitary-system-draw} and Figure~\ref{fig:schematic-of-a-cbvav-unitary-system-blow}).
+
+\begin{lstlisting}
+
+AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass,
+  GasHeat CBVAV System,  !- Name of unitary system
+  FanAndCoilAvailSched,  !- Availability schedule name
+  1.8,                   !- Cooling Supply Air Flow Rate {m3/s}
+  1.7,                   !- Heating Supply Air Flow Rate {m3/s}
+  1.6,                   !- No Load Supply Air Flow Rate {m3/s}
+  0.32,                  !- Cooling Outdoor Air Flow Rate {m3/s}
+  0.3,                   !- Heating Outdoor Air Flow Rate {m3/s}
+  0.27,                  !- No Load Outdoor Air Flow Rate {m3/s}
+  Outdoor Air Multiplier Schedule, !- Outdoor air volumetric flow rate multiplier schedule name
+  Air Loop Inlet Node,     !- Air inlet node name
+  Mixer Inlet Node,        !- Bypass duct mixer node name
+  Heating Coil Air Outlet Node,    !- Bypass duct splitter node name
+  Air Loop Outlet Node,    !- Air outlet node name
+  OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type
+  Outdoor air Mixer,       !- Outdoor air mixer name
+  Fan:OnOff,        !- Supply air fan type
+  Supply Fan 1,            !- Supply air fan name
+  BlowThrough,            !- Supply air fan placement
+  Fan OpMode Schedule,     !- Supply air fan operating mode schedule name
+  Coil:Cooling:DX:TwoStageWithHumidityControlMode,  !- Cooling coil type
+  ACDXCoil 2,              !- Cooling coil name
+  Coil:Heating:Gas,        !- Heating coil type
+  Furnace Heating Coil 1,  !- Heating coil name
+  CoolingPriority,        !- Priority control mode
+  10.0,                    !- Minimum outlet air temperature during cooling operation {C}
+  50.0,                    !- Maximum outlet air temperature during heating operation {C}
+  None;                    !- Dehumidification control type
+
+  OutdoorAir:Mixer,
+      Outdoor air Mixer,       !- Name
+      Mixed Air Node,          !- Mixed Air Node Name
+      Outdoor air Inlet Node,  !- Outdoor Air Stream Node
+      Relief Air Outlet Node,  !- Relief Air Stream Node Name
+      Mixer Inlet Node;        !- Return Air Stream Node Name
+
+  Fan:OnOff,
+      Supply Fan 1,            !- Fan Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      0.7,                     !- Fan Total Efficiency
+      600.0,                   !- Delta Pressure {Pa}
+      1.8,                     !- Max Flow Rate {m3/s}
+      0.9,                     !- Motor Efficiency
+      1.0,                     !- Motor In Airstream Fraction
+      Mixed Air Node,          !- Fan\_Inlet\_Node
+      DX Cooling Coil Air Inlet Node;  !- Fan\_Outlet\_Node
+
+  Coil:Cooling:DX:TwoStageWithHumidityControlMode,
+      ACDXCoil 2,              !- Coil Name
+      FanAndCoilAvailSched,    !- Availability Schedule
+      DX Cooling Coil Air Inlet Node, !- Coil Air Inlet Node
+      Heating Coil Air Inlet Node,    !- Coil Air Outlet Node
+      ,                        !- Crankcase Heater Capacity {W}
+      ,                        !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
+      2,                       !- Number of Capacity Stages
+      0,                       !- Number of Enhanced Dehumidification Modes
+      CoilPerformance:DX:Cooling,  !- Normal Mode Stage 1 Coil Performance Object Type
+      ACDXCoil 2 Standard Mode-Stage 1,  !- Normal Mode Stage 1 Coil Performance Object Name
+      CoilPerformance:DX:Cooling,  !- Normal Mode Stage 1+2 Coil Performance Object Type
+      ACDXCoil 2 Standard Mode-Stage 1&2;  !- Normal Mode Stage 1+2 Coil Performance Object Name
+
+  Coil:Heating:Gas,
+      Furnace Heating Coil 1,  !- Coil Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      0.8,                     !- Gas Burner Efficiency of the Coil
+      35000,                   !- Nominal Capacity of the Coil {W}
+      Heating Coil Air Inlet Node,  !- Coil\_Air\_Inlet\_Node
+      Heating Coil Air Outlet Node; !- Coil\_Air\_Outlet\_Node
+
+  AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat,
+      Zone 1 VAV System,       !- Name of System
+      FanAndCoilAvailSched,    !- System Availability schedule
+      Zone 1 Reheat Air Inlet Node,  !- DAMPER Air Outlet Node
+      Zone 1 VAV Inlet Node,   !-UNIT Air Inlet Node
+      0.583,                   !- Maximum air flow rate {m3/s}
+      0.25,                    !- Zone Minimum Air Flow Fraction
+      ,                        !- Control node
+      Coil:Heating:Electric,   !- Reheat Component Object
+      Reheat Coil Zone 1,      !- Name of Reheat Component
+      0.0,                     !- Max Reheat Water Flow {m3/s}
+      0.0,                     !- Min Reheat Water Flow {m3/s}
+      Zone 1 Reheat Air Outlet Node,  !- UNIT Air Outlet Node
+      0.001;                   !- Convergence Tolerance
+
+  AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat,
+      Zone 2 VAV System,       !- Name of System
+      FanAndCoilAvailSched,    !- System Availability schedule
+      Zone 2 Reheat Air Inlet Node,  !- DAMPER Air Outlet Node
+      Zone 2 VAV Inlet Node,   !-UNIT Air Inlet Node
+      0.583,                   !- Maximum air flow rate {m3/s}
+      0.25,                    !- Zone Minimum Air Flow Fraction
+      ,                        !- Control node
+      Coil:Heating:Electric,   !- Reheat Component Object
+      Reheat Coil Zone 2,      !- Name of Reheat Component
+      0.0,                     !- Max Reheat Water Flow {m3/s}
+      0.0,                     !- Min Reheat Water Flow {m3/s}
+      Zone 2 Reheat Air Outlet Node,  !- UNIT Air Outlet Node
+      0.001;                   !- Convergence Tolerance
+
+  AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat,
+      Zone 3 VAV System,       !- Name of System
+      FanAndCoilAvailSched,    !- System Availability schedule
+      Zone 3 Reheat Air Outlet Node,  !- UNIT Air Outlet Node
+      Zone 3 VAV Inlet Node,   !-UNIT Air Inlet Node
+      0.584,                   !- Maximum air flow rate {m3/s}
+      0.25;                    !- Zone Minimum Air Flow Fraction
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-011}
+
+\begin{itemize}
+\item
+  HVAC,Average,Unitary System Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Unitary System Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Unitary System Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Unitary System Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Unitary System Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Unitary System Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Unitary System Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Unitary System Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Unitary System Latent Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Unitary System Latent Heating Energy {[}J{]}
+\item
+  HVAC,Average,Unitary System Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Unitary System Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Unitary System Electric Power {[}W{]}
+\item
+  HVAC,Sum,Unitary System Electric Energy {[}J{]}
+\item
+  HVAC,Average,Unitary System Fan Part Load Ratio {[]}
+\item
+  HVAC,Average,Unitary System Compressor Part Load Ratio {[]}
+\item
+  HVAC,Average,Unitary System Bypass Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Unitary System Air Outlet Setpoint Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Unitary System Total Heating Rate {[}W{]}}\label{unitary-system-total-heating-rate-w-2}
+
+This output field is the total (enthalpy) heat addition rate of the CBVAV system in Watts. This value is calculated using the enthalpy difference of the outlet air and inlet air streams, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Total Heating Energy {[}J{]}}\label{unitary-system-total-heating-energy-j}
+
+This output field is the total (enthalpy) heat addition of the CBVAV system in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the outlet air and inlet air streams, the supply air mass flow rate entering/leaving the system, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are summed for the timestep being reported.
+
+\paragraph{Unitary System Total Cooling Rate {[}W{]}}\label{unitary-system-total-cooling-rate-w-2}
+
+This output field is the total (enthalpy) heat extraction rate of the CBVAV system in Watts. This value is calculated using the enthalpy difference of the outlet air and inlet air streams, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Total Cooling Energy {[}J{]}}\label{unitary-system-total-cooling-energy-j}
+
+This output field is the total (enthalpy) heat extraction of the CBVAV system in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the outlet air and inlet air streams, the supply air mass flow rate entering/leaving the system, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are summed for the timestep being reported.
+
+\paragraph{Unitary System Sensible Heating Rate {[}W{]}}\label{unitary-system-sensible-heating-rate-w-2}
+
+This output field is the sensible heat addition rate of the CBVAV system in Watts. This value is calculated using the enthalpy difference of the outlet air and inlet air streams at a constant humidity ratio, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Sensible Heating Energy {[}J{]}}\label{unitary-system-sensible-heating-energy-j}
+
+This output field is the sensible heat addition of the CBVAV system in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the outlet air and inlet air streams at a constant humidity ratio, the supply air mass flow rate entering/leaving the system, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are summed for the timestep being reported.
+
+\paragraph{Unitary System Sensible Cooling Rate {[}W{]}}\label{unitary-system-sensible-cooling-rate-w-2}
+
+This output field reports the moist air sensible heat extraction rate of the CBVAV system in Watts. This value is calculated using the enthalpy difference of the outlet air and inlet air streams at a constant humidity ratio, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Sensible Cooling Energy {[}J{]}}\label{unitary-system-sensible-cooling-energy-j}
+
+This output field reports the moist air sensible heat extraction of the CBVAV system in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the outlet air and inlet air streams at a constant humidity ratio, the supply air mass flow rate entering/leaving the system, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are summed for the timestep being reported.
+
+\paragraph{Unitary System Latent Heating Rate {[}W{]}}\label{unitary-system-latent-heating-rate-w-2}
+
+This output field is the latent heat addition (humidification) rate of the CBVAV system in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Latent Heating Energy {[}J{]}}\label{unitary-system-latent-heating-energy-j}
+
+This output field is the latent heat addition (humidification) of the CBVAV system in Joules over the timestep being reported. This value is calculated as the difference between the total energy and the sensible energy delivered by the system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are summed for the timestep being reported.
+
+\paragraph{Unitary System Latent Cooling Rate {[}W{]}}\label{unitary-system-latent-cooling-rate-w-2}
+
+This output field is the latent heat extraction (dehumidification) rate of the CBVAV system in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
+
+\paragraph{Unitary System Latent Cooling Energy {[}J{]}}\label{unitary-system-latent-cooling-energy-j}
+
+This output field is the latent heat extraction (dehumidification) of the CBVAV system in Joules over the timestep being reported. This value is calculated as the difference between the total energy and the sensible energy delivered by the system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are summed for the timestep being reported.
+
+\paragraph{Unitary System Electric Power {[}W{]}}\label{unitary-system-electric-power-w-2}
+
+This output field is the electricity consumption rate of the CBVAV system in Watts. The consumption includes electricity used by the DX compressor (including crankcase heater), fans (indoor supply air fan and the condenser fans associated with the DX coil{[}s{]}), and the heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{Unitary System Electric Energy {[}J{]}}\label{unitary-system-electric-energy-j-2}
+
+This output field is the electricity consumption of the CBVAV system in Joules for the time period being reported. The consumption includes electricity used by the DX compressor (including crankcase heater), fans (indoor supply air fan and the condenser fans associated with the DX coil{[}s{]}), and the heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are summed for the timestep being reported.
+
+\paragraph{\texorpdfstring{Unitary System Fan Part Load Ratio {[]}}{Unitary System Fan Part Load Ratio }}\label{unitary-system-fan-part-load-ratio-8}
+
+This output field is the part-load ratio of the supply air fan, which will be either zero or 1 for each simulation timestep. For this system, the fan will operate continuously for the simulation timestep if the system is available (ref. Field: Availability schedule name) and there is a cooling or heating load to be met (i.e., fan part-load ratio will equal 1). When the system is available but there is no cooling or heating load to be met, the fan will either be off for the entire timestep or on for the entire timestep depending on the supply air fan operating mode schedule (ref. Field: Supply Air Fan Operating Mode Schedule Name). This value is set for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{\texorpdfstring{Unitary System Compressor Part Load Ratio {[]}}{Unitary System Compressor Part Load Ratio }}\label{unitary-system-compressor-part-load-ratio-5}
+
+This output field is the part-load ratio of the compressor used by the DX coils (cooling and heating). The compressor part-load ratio is defined as the total coil load divided by the coil steady-state capacity (steady-state capacity of first stage for multi-mode coils). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{Unitary System Bypass Air Mass Flow Rate {[}kg/s{]}}\label{unitary-system-bypass-air-mass-flow-rate-kgs}
+
+This output field is the mass flow rate of air, in kg/s, being bypassed from the supply air path and blended with the air entering the CBVAV system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{Unitary System Air Outlet Setpoint Temperature {[}C{]}}\label{unitary-system-air-outlet-setpoint-temperature-c}
+
+This output field is the dry-bulb set point temperature in degrees Celsius. This set point temperature is calculated by the model based on the zone cooling/heating loads calculated by EnergyPlus, and the priority control mode and the dehumidification control type specified for this unitary system. The CBVAV system attempts to achieve the outlet air set point temperature to the extent possible.
diff --git a/doc/input-output-reference/src/overview/group-user-defined-hvac-and-plant-component.tex b/doc/input-output-reference/src/overview/group-user-defined-hvac-and-plant-component.tex
new file mode 100644
index 00000000000..87941c04e7e
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-user-defined-hvac-and-plant-component.tex
@@ -0,0 +1,493 @@
+\section{Group User Defined HVAC and Plant Component Models}\label{group-user-defined-hvac-and-plant-component-models}
+
+This group of EnergyPlus input objects provides methods for users to include their own custom models for HVAC and plant components as well as plant equipment operation. This is helpful because not every conceivable type of HVAC equipment or system configuration has already had models implemented in EnergyPlus. HVAC or plant components, or even entire system configurations, might be so new, unusual, or proprietary that no model has yet been implemented in the software. An analyst faced with project that needs to model such a device or system could do so using one or more of the user defined components described in this section.
+
+Some building energy performance rating systems allow analysts to option of using exceptional calculation methods when a simulation program cannot perform the function required to be modeled. These user defined component models are intended to provide a means for including such exceptional calculations within the context of a full EnergyPlus model. This allows using EnergyPlus for everything it can model and extending it yourself to include a new type of HVAC or Plant component.
+
+These objects are advanced. Making good use of them requires the user to have a detailed understanding of EnergyPlus HVAC and Plant models as well as the Energy Management System (EMS). The EnergyPlus Runtime Language (Erl) is used to program the component model. The Application Guide for EMS provides more discussion of how to use the objects in this group see the chapter called User-Defined Component Models.
+
+\subsection{ZoneHVAC:ForcedAir:UserDefined}\label{zonehvacforcedairuserdefined}
+
+This object is used to define a generic zone air unit for custom component models. This object has a primary air connection that connects to a zone through exhaust and inlet nodes. There is an optional secondary air connection that can be used as an air-based source or heat rejection connection. As many has three different plant connections can be made to the zone unit. Water storage tanks can be connected for supply or collection. An ambient zone can be connected for skin losses to be treated as separate internal gains.
+
+\subsubsection{Inputs}\label{inputs-050}
+
+\paragraph{Field: Name}\label{field-name-049}
+
+This field defines a unique user-assigned name for an instance of a custom, forced-air zone conditioning unit. Any reference to this zone unit by another object will use this name.
+
+\paragraph{Field: Overall Model Simulation Program Calling Manager Name}\label{field-overall-model-simulation-program-calling-manager-name}
+
+This field specifies the Erl programs that are used to model the custom zone unit. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere. The program manager referenced here should include all the Erl programs that are to be run each time the component is simulated and use the calling point called UserDefinedComponentModel.
+
+\paragraph{Field: Model Setup and Sizing Program Calling Manager Name}\label{field-model-setup-and-sizing-program-calling-manager-name}
+
+This field specifies the Erl programs that are used to initialize and size the custom zone unit. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere and uses the calling point called UserDefinedComponentModel. The program manager referenced here should include all the Erl programs that are needed to do any initial setup that should occur before the main modeling programs are run. These include calculating and setting values for things that do not vary over time such as component sizes, control parameters, modeling constants etc. The user defined component will trigger this calling manager at the beginning of each new environment period.
+
+\paragraph{Field: Primary Air Inlet Node Name}\label{field-primary-air-inlet-node-name-001}
+
+This field defines the name of the HVAC system node from which the zone unit draws its inlet air from the zone. This node must be the name of a zone air exhaust node (ref. ZoneHVAC:EquipmentConnection). This field is required.
+
+\paragraph{Field: Primary Air Outlet Node Name}\label{field-primary-air-outlet-node-name-001}
+
+This field defines the name of the HVAC system node to which the zone unit sends its outlet air to the zone. This node must be the name of a zone air inlet node (ref. ZoneHVAC:EquipmentConnection). This field is required.
+
+\paragraph{Field: Secondary Air Inlet Node Name}\label{field-secondary-air-inlet-node-name-002}
+
+This field defines the name of a HVAC system node from which the zone unit can draw additional air. This air inlet stream has a variety of possible uses including outdoor air supply for ventilation or a condenser inlet for heat rejection. This field is optional.
+
+\paragraph{Field: Secondary Air Outlet Node Name}\label{field-secondary-air-outlet-node-name-001}
+
+This field defines the name of a HVAC system node to which the zone unit can send additional air. This air outlet stream has a variety of possible uses including outdoor air relief for exhaust or a condenser outlet for heat rejection. This field is optional.
+
+\paragraph{Field: Number of Plant Loop Connections}\label{field-number-of-plant-loop-connections}
+
+This fields defines the number of different plant loop connections that the zone unit will use. Up to three separate loops can be connected if desired. This field is required. Enter a 0 if the unit does not use plant at all.
+
+\paragraph{Field: Plant Connection 1 Inlet Node Name}\label{field-plant-connection-1-inlet-node-name}
+
+This field defines the name of a plant system node from which the zone unit can draw fluid. This is the inlet to the component model from the first plant loop that is connected to the zone unit.
+
+\paragraph{Field: Plant Connection 1 Outlet Node Name}\label{field-plant-connection-1-outlet-node-name}
+
+This field defines the name of a plant system node to which the zone unit can send fluid. This is the outlet from the component model to the first plant loop that is connected to the zone unit.
+
+\paragraph{Field: Plant Connection 2 Inlet Node Name}\label{field-plant-connection-2-inlet-node-name}
+
+This field defines the name of a plant system node from which the zone unit can draw fluid. This is the inlet to the component model from the second plant loop that is connected to the zone unit.
+
+\paragraph{Field: Plant Connection 2 Outlet Node Name}\label{field-plant-connection-2-outlet-node-name}
+
+This field defines the name of a plant system node to which the zone unit can send fluid. This is the outlet from the component model to the second plant loop that is connected to the zone unit.
+
+\paragraph{Field: Plant Connection 3 Inlet Node Name}\label{field-plant-connection-3-inlet-node-name}
+
+This field defines the name of a plant system node from which the zone unit can draw fluid. This is the inlet to the component model from the third plant loop that is connected to the zone unit.
+
+\paragraph{Field: Plant Connection 3 Outlet Node Name}\label{field-plant-connection-3-outlet-node-name}
+
+This field defines the name of a plant system node to which the zone unit can send fluid. This is the outlet from the component model to the third plant loop that is connected to the zone unit.
+
+\paragraph{Field: Supply Inlet Water Storage Tank Name}\label{field-supply-inlet-water-storage-tank-name}
+
+This field is used to describe where the zone unit obtains water if it is to be connected to a water storage tank. This water could be used for evaporative cooling. If a name of a WaterUse:Storage object is used here, then the unit can obtain its water from that tank. This field is optional.
+
+\paragraph{Field: Collection Outlet Water Storage Tank Name}\label{field-collection-outlet-water-storage-tank-name}
+
+This field is used to describe where the zone unit sends water it has collected if is to be stored in a tank. This water could be collected from coil condensate. If a name of a WaterUse:Storage object is used here, then the unit can send water to that tank. This field is optional.
+
+\paragraph{Field: Ambient Zone Name}\label{field-ambient-zone-name}
+
+This field is used to connect ancillary losses from the zone unit to a thermal zone. The unit may have inefficiencies, leaks, or other non-ideal operation that results in some untended impact on the space surrounding the unit. These skin losses can be assigned to a thermal zone and appear as internal gains for the zone named here. This does not need to be the same thermal zone as the zone that unit is intended to condition.
+
+An example of this input object follows.
+
+\begin{lstlisting}
+
+ZoneHVAC:ForcedAir:UserDefined,
+  Zone1WindAC,   !- Name
+  Zone 1 Window AC Model Program Manager , !- Overall Model Simulation Program Calling Manager Name
+  Zone 1 Window AC Init Program Manager , !- Model Setup and Sizing Program Calling Manager Name
+  Zone1WindACAirInletNode , !- Primary Air Inlet Node Name
+  Zone1WindACAirOutletNode, !- Primary Air Outlet Node Name
+  Zone1WindACOAInNode,   !- Secondary Air Inlet Node Name
+  Zone1WindACExhNode,   !- Secondary Air Outlet Node Name
+  0 ; !- Number of Plant Loop Connections
+\end{lstlisting}
+
+\subsection{AirTerminal:SingleDuct:UserDefined}\label{airterminalsingleductuserdefined}
+
+This object is used to define a generic single duct air terminal unit for custom component models. This object has a primary air connection that connects a multi-zone air handler to a zone. There is an optional secondary air connection that can be used and an air-based source or heat rejection connection. As many as two different plant connections can be made to the air terminal unit. Water storage tanks can be connected for supply or collection. An ambient zone can be connected for skin losses to be treated as separate internal gains.
+
+\subsubsection{Field: Name}\label{field-name-1-046}
+
+This field defines a unique user-assigned name for an instance of a custom, air terminal unit. Any reference to this air terminal by another object will use this name.
+
+\subsubsection{Field: Overall Model Simulation Program Calling Manager Name}\label{field-overall-model-simulation-program-calling-manager-name-1}
+
+This field specifies the Erl programs that are used to model the custom air terminal unit. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere. The program manager referenced here should include all the Erl programs that are to be run each time the component is simulated and use the calling point called UserDefinedComponentModel.
+
+\subsubsection{Field: Model Setup and Sizing Program Calling Manager Name}\label{field-model-setup-and-sizing-program-calling-manager-name-1}
+
+This field specifies the Erl programs that are used to initialize and size the custom air terminal unit. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere and uses the calling point called UserDefinedComponentModel. The program manager referenced here should include all the Erl programs that are needed to do any initial setup that should occur before the main modeling programs are run. These include calculating and setting values for things that do not vary over time such as component sizes, control parameters, modeling constants etc. The user defined component will trigger this calling manager at the beginning of each new environment period.
+
+\subsubsection{Field: Primary Air Inlet Node Name}\label{field-primary-air-inlet-node-name-1-000}
+
+This field defines the name of the HVAC system node from which the air terminal unit draws its inlet air. This node must be the name of a HVAC system node that is listed in a zone splitter (ref. AirLoopHVAC:ZoneSplitter). This field is required.
+
+\subsubsection{Field: Primary Air Outlet Node Name}\label{field-primary-air-outlet-node-name-1-000}
+
+This field defines the name of the HVAC system node to which the air terminal unit sends its outlet air to the zone. This node must be the name of a zone air inlet node (ref. ZoneHVAC:EquipmentConnection). This field is required.
+
+\subsubsection{Field: Secondary Air Inlet Node Name}\label{field-secondary-air-inlet-node-name-1-001}
+
+This field defines the name of a HVAC system node from which the air terminal unit can draw additional air. This air inlet stream has a variety of possible uses including outdoor air supply for ventilation or a condenser inlet for heat rejection. This field is optional.
+
+\subsubsection{Field: Secondary Air Outlet Node Name}\label{field-secondary-air-outlet-node-name-1}
+
+This field defines the name of a HVAC system node to which the air terminal unit can send additional air. This air outlet stream has a variety of possible uses including outdoor air relief for exhaust or a condenser outlet for heat rejection. This field is optional.
+
+\subsubsection{Field: Number of Plant Loop Connections}\label{field-number-of-plant-loop-connections-1}
+
+This fields defines the number of different plant loop connections that the air terminal unit will use. Up to two separate loop can be connected if desired. This field is required. Enter a 0 if the unit does not use plant at all.
+
+\subsubsection{Field: Plant Connection 1 Inlet Node Name}\label{field-plant-connection-1-inlet-node-name-1}
+
+This field defines the name of a plant system node from which the air terminal unit can draw fluid. This is the inlet to the component model from the first plant loop that is connected to the air terminal unit.
+
+\subsubsection{Field: Plant Connection 1 Outlet Node Name}\label{field-plant-connection-1-outlet-node-name-1}
+
+This field defines the name of a plant system node to which the air terminal unit can send fluid. This is the outlet from the component model to the first plant loop that is connected to the air terminal unit.
+
+\subsubsection{Field: Plant Connection 2 Inlet Node Name}\label{field-plant-connection-2-inlet-node-name-1}
+
+This field defines the name of a plant system node from which the air terminal unit can draw fluid. This is the inlet to the component model from the second plant loop that is connected to the air terminal unit.
+
+\subsubsection{Field: Plant Connection 2 Outlet Node Name}\label{field-plant-connection-2-outlet-node-name-1}
+
+This field defines the name of a plant system node to which the air terminal unit can send fluid. This is the outlet from the component model to the second plant loop that is connected to the air terminal unit.
+
+\subsubsection{Field: Supply Inlet Water Storage Tank Name}\label{field-supply-inlet-water-storage-tank-name-1}
+
+This field is used to describe where the air terminal unit obtains water if it is to be connected to a water storage tank. This water could be used for evaporative cooling. If a name of a WaterUse:Storage object is used here, then the unit can obtain its water from that tank. This field is optional.
+
+\subsubsection{Field: Collection Outlet Water Storage Tank Name}\label{field-collection-outlet-water-storage-tank-name-1}
+
+This field is used to describe where the air terminal unit sends water it has collected if is to be stored in a tank. This water could be collected from coil condensate. If a name of a WaterUse:Storage object is used here, then the unit can send water to that tank. This field is optional.
+
+\subsubsection{Field: Ambient Zone Name}\label{field-ambient-zone-name-1}
+
+This field is used to connect ancillary losses from the air terminal unit to a thermal zone. The unit may have inefficiencies, leaks, or other non-ideal operation that results in some untended impact on the space surrounding the unit. These skin losses can be assigned to a thermal zone and appear as internal gains for the zone named here. This does not need to be the same thermal zone as the zone that terminal unit is intended to condition.
+
+An example of this input object follows.
+
+\begin{lstlisting}
+
+AirTerminal:SingleDuct:UserDefined,
+  SPACE1-1 VAV Reheat,   !- Name
+  Space1 ATU Sim Programs , !- Overall Model Simulation Program Calling Manager Name
+  Space1 ATU Init Programs , !- Model Setup and Sizing Program Calling Manager Name
+  SPACE1-1 ATU In Node , !- Primary Air Inlet Node Name
+  SPACE1-1 In Node , !- Primary Air Outlet Node Name
+  ,   !- Secondary Air Inlet Node Name
+  ,   !- Secondary Air Outlet Node Name
+  1,   !- Number of Plant Loop Connections
+  SPACE1-1 Zone Coil Water In Node , !- Plant Connection 1 Inlet Node Name
+  SPACE1-1 Zone Coil Water Out Node; !- Plant Connection 1 Outlet Node Name
+\end{lstlisting}
+
+\subsection{Coil:UserDefined}\label{coiluserdefined}
+
+This object is used to define a generic coil for custom component modeling of a device that processes air as part of an air handeler. The Coil:UserDefined object appears directly on a Branch object used to define the supply side of an air handler, or in the AirLoopHVAC:OutdoorAirSystem:EquipmentList object used to define outdoor air systems. This object has one or two air connections and an optional plant connection. Water storage tanks can be connected for supply or collection. An ambient zone can be connected for skin losses to be treated as separate internal gains.
+
+\subsubsection{Field: Name}\label{field-name-2-041}
+
+This field defines a unique user-assigned name for an instance of a custom air coil. Any reference to this coil by another object will use this name.
+
+\subsubsection{Field: Overall Model Simulation Program Calling Manager Name}\label{field-overall-model-simulation-program-calling-manager-name-2}
+
+This field specifies the Erl programs that are used to model the custom coil. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere. The program manager referenced here should include all the Erl programs that are to be run each time the component is simulated and use the calling point called UserDefinedComponentModel.
+
+\subsubsection{Field: Model Setup and Sizing Program Calling Manager Name}\label{field-model-setup-and-sizing-program-calling-manager-name-2}
+
+This field specifies the Erl programs that are used to initialize and size the custom coil. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere and uses the calling point called UserDefinedComponentModel. The program manager referenced here should include all the Erl programs that are needed to do any initial setup that should occur before the main modeling programs are run. These include calculating and setting values for things that do not vary over time such as component sizes, control parameters, modeling constants etc. The user defined component will trigger this calling manager at the beginning of each new environment period.
+
+\subsubsection{Field: Number of Air Connections}\label{field-number-of-air-connections}
+
+This field defines the number of air loop connections that the coil will use. The coil must have at least one connection but a second can be used by entering a 2.
+
+\subsubsection{Field: Air Connection 1 Inlet Node Name}\label{field-air-connection-1-inlet-node-name}
+
+This field defines the name of the HVAC system node from which the coil draws its inlet air for its first air loop connection. This node must be the outlet of the HVAC system component located upstream, if there is one. This field is required.
+
+\subsubsection{Field: Air Connection 1 Outlet Node Name}\label{field-air-connection-1-outlet-node-name}
+
+This field defines the name of the HVAC system node to which the coil sends its outlet air for its first air loop connection. This node must be the inlet of the HVAC system component located downstream, if there is one. This field is required.
+
+\subsubsection{Field: Air Connection 2 Inlet Node Name}\label{field-air-connection-2-inlet-node-name}
+
+This field defines the name of the HVAC system node from which the coil draws its inlet air for its second air loop connection. This node must be the outlet of the HVAC system component located upstream, if there is one. This field is optional.
+
+\subsubsection{Field: Air Connection 2 Outlet Node Name}\label{field-air-connection-2-outlet-node-name}
+
+This field defines the name of the HVAC system node to which the coil sends its outlet air for its second air loop connection. This node must be the inlet of the HVAC system component located downstream, if there is one. This field is optional.
+
+\subsubsection{Field: Plant Connection is Used}\label{field-plant-connection-is-used}
+
+This field defines whether or not the plant loop connection is going to be used. Enter a Yes if the coil will use plant, enter No if not. This field is required.
+
+\subsubsection{Field: Plant Connection Inlet Node Name}\label{field-plant-connection-inlet-node-name}
+
+This field defines the name of a plant system node from which the coil can draw fluid. This is the inlet to the component model from the plant loop that is connected to the coil.
+
+\subsubsection{Field: Plant Connection Outlet Node Name}\label{field-plant-connection-outlet-node-name}
+
+This field defines the name of a plant system node to which the coil can send fluid. This is the outlet from the component model to the plant loop that is connected to the coil.
+
+\subsubsection{Field: Supply Inlet Water Storage Tank Name}\label{field-supply-inlet-water-storage-tank-name-2}
+
+This field is used to describe where the coil obtains water if it is to be connected to a water storage tank. This water could be used for evaporative cooling. If a name of a WaterUse:Storage object is used here, then the unit can obtain its water from that tank. This field is optional.
+
+\subsubsection{Field: Collection Outlet Water Storage Tank Name}\label{field-collection-outlet-water-storage-tank-name-2}
+
+This field is used to describe where the coil sends water it has collected if is to be stored in a tank. This water could be collected from coil condensate. If a name of a WaterUse:Storage object is used here, then the unit can send water to that tank. This field is optional.
+
+\subsubsection{Field: Ambient Zone Name}\label{field-ambient-zone-name-2}
+
+This field is used to connect ancillary losses from the coil to a thermal zone. The coil may have inefficiencies, leaks, or other non-ideal operation that results in some untended impact on the space surrounding the unit. These skin losses can be assigned to a thermal zone and appear as internal gains for the zone named here. For example, this would be the mechanical room where the coil is located, not necessarily one of the zone served by the air handler.
+
+An example of this input object follows.
+
+\begin{lstlisting}
+
+Coil:UserDefined,
+  Main Cooling Coil 1, !- Name
+  Main Cooling Coil Model Program Manager , !- Overall Model Simulation Program Calling Manager Name
+  Main Cooling Coil Init Program Manager , !- Model Setup and Sizing Program Calling Manager Name
+  1 , !- Number of Air Connections
+  Mixed Air Node 1 , !- Air Connection 1 Inlet Node Name
+  Main Cooling Coil 1 Outlet Node , !- Air Connection 1 Outlet Node Name
+  , !- Air Connection 2 Inlet Node Name
+  , !- Air Connection 2 Outlet Node Name
+  Yes , !- Plant Connection is Used
+  Main Cooling Coil 1 Water Inlet Node, !- Plant Connection Inlet Node Name
+  Main Cooling Coil 1 Water Outlet Node; !- Plant Connection Outlet Node Name
+\end{lstlisting}
+
+Note that the Coil:UserDefined needs to be specifically configured in EnergyManagementSystem:MeteredOutputVariable, in order to be included in the meters such as HeatingCoils:EnergyTransfer.
+
+An example of this input object follows.
+
+\begin{lstlisting}
+
+EnergyManagementSystem:Program,
+  MainHWCoil1_ModelOuput,  !- Name
+  Set HWcoil1_Water_MdotRequest = Water_MdotRequest,  !- Program Line 1
+  Set HWcoil1_Air_Tout          = Air_Tout,  !- Program Line 2
+  Set HWcoil1_Air_Wout          = Air_Wout,  !- <none>
+  Set HWcoil1_tot_heat_Power    = Tot_heat_Power,  !- <none>
+  Set HWcoil1_tot_heat_Energy   = Tot_heat_Power * SystemTimestep * 3600,  !- <none>
+  Set HWcoil1_Air_MdotOut       = Air_Mdot,  !- <none>
+  Set HWcoil1_Water_Tout        = Water_Tout;!- <none>
+
+  EnergyManagementSystem:MeteredOutputVariable,
+  HWcoil1 tot heat Energy, !- Name
+  HWcoil1_tot_heat_Energy, !- EMS Variable Name
+  SystemTimestep,          !- Update Frequency
+  MainHWCoil1_ModelOuput,  !- EMS Program or Subroutine Name
+  ENERGYTRANSFER,          !- Resource Type
+  System,                  !- Group Type
+  HEATINGCOILS,            !- End-Use Category
+  ,                        !- End-Use Subcategory
+  J;                       !- Units
+\end{lstlisting}
+
+\subsection{PlantComponent:UserDefined}\label{plantcomponentuserdefined}
+
+This object is used to define a generic plant component for custom component models. This object can connect to up to four different plant loops. There is an optional air connection that can be used as an air-based source or heat rejection connection. Water storage tanks can be connected for supply or collection. An ambient zone can be connected for skin losses to be treated as separate internal gains.
+
+The PlantComponent:UserDefined object appears directly on the Branch object used to describe the plant.
+
+\subsubsection{Field: Name}\label{field-name-3-035}
+
+This field defines a unique user-assigned name for an instance of a custom plant component. Any reference to this component by another object will use this name.
+
+\subsubsection{Field: Main Model Program Calling Manager Name}\label{field-main-model-program-calling-manager-name}
+
+This field specifies the Erl programs that are used to model the plant component any time that the device is called to simulate. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere. The program manager referenced here should include all the Erl programs that are to be run each time the component is simulated and use the calling point called UserDefinedComponentModel.
+
+\subsubsection{Field: Number of Plant Loop Connections}\label{field-number-of-plant-loop-connections-2}
+
+This fields defines the number of different plant loop connections that the component will use. Up to four separate loops can be connected if desired. This field is required.
+
+\subsubsection{FeildSet: \{inlet node name, outlet node name, loading mode, flow request mode, initialization program calling manager, simulation program calling manager.\}}\label{feildset-inlet-node-name-outlet-node-name-loading-mode-flow-request-mode-initialization-program-calling-manager-simulation-program-calling-manager.}
+
+Each of the plant loop connections used is defined by a set of 6 input fields that contain and inlet node, and outlet node, a loading mode, a flow request mode, a program calling manager for setup and sizing, and a program calling manager for model calculations that should run when this loop is being simulated.
+
+\subsubsection{Field: Plant Connection X Inlet Node Name}\label{field-plant-connection-x-inlet-node-name}
+
+This field defines the name of a plant system node from which the component can draw fluid. This is the inlet to the component model from the x plant loop that is connected to the component.
+
+\subsubsection{Field: Plant Connection X Outlet Node Name}\label{field-plant-connection-x-outlet-node-name}
+
+This field defines the name of a plant system node to which the component can send fluid. This is the outlet from the component model to the first plant loop that is connected to the component.
+
+\subsubsection{Field: Plant Connection X Loading Mode}\label{field-plant-connection-x-loading-mode}
+
+This field defines the nature of the plant component with respect to how it affects the loads experienced by the X plant loop connection. One of the following choices must be selected depending on the purpose of the component model and this particular plant loop connection.
+
+\begin{itemize}
+\item
+  \textbf{DemandsLoad}. This type of loading is used for plant connections that place a load on the loop.
+\item
+  \textbf{MeetsLoadWithPassiveCapacity}. This type of loading is used for plant connections where the component has some capacity to meet loads but it is not really of the type that could be actively controlled.
+\item
+  \textbf{MeetsLoadWithNominalCapacity}. This type of loading is used for plant connections where the component has controllable capacity to meet loads and no outlet temperature restrictions.
+\item
+  \textbf{MeetsLoadWithNominalCapacityLowOutLimit}. This type of loading is used for plant connections where the component has controllable capacity to meet loads but with a lower limit on the fluid temperature at the outlet node.
+\item
+  \textbf{MeetsLoadWithNominalCapacityHiOutLimit}. This type of loading is used for plant connections where the component has controllable capacity to meet loads but with an upper limit on the fluid temperature at the outlet node.
+\end{itemize}
+
+\subsubsection{Field: Plant Connection X Loop Flow Request Mode}\label{field-plant-connection-x-loop-flow-request-mode}
+
+This field defines the nature of the plant component with respect to how it affects the overall flow rate for the loop. One of the following three choices must be made depending on the nature of the plant component and this particular loop connection.
+
+\begin{itemize}
+\item
+  \textbf{NeedsFlowIfLoopOn}. Devices with this flow request mode will contribute to the overall loop flow rate but will not initiate flow themselves.
+\item
+  \textbf{NeedsFlowAndTurnsLoopOn}. Devices with this flow request mode will contribute to the overall loop flow rate and initiate flow.
+\item
+  \textbf{ReceivesWhateverFlowAvailable}. Devices with this flow request mode will not contribute to the overall loop flow rate and do not initiate flow themselves.
+\end{itemize}
+
+\subsubsection{Field: Plant Connection X Initialization Program Calling Manager Name}\label{field-plant-connection-x-initialization-program-calling-manager-name}
+
+This field specifies the Erl programs that are used to model the plant component and should execute when the component is called to simulate by this particular loop connection. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere. The program manager referenced here should include all the Erl programs that are to be run for this X plant loop connection and use the calling point called UserDefinedComponentModel.
+
+\subsubsection{Field: Plant Connection X Simulation Program Calling Manager Name}\label{field-plant-connection-x-simulation-program-calling-manager-name}
+
+This field specifies the Erl programs that are used to initialize and size the plant component with regard to this particular plant connection. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere and uses the calling point called UserDefinedComponentModel. The program manager referenced here should include all the Erl programs that are needed to do any initial setup that should occur before the main modeling programs are run. These include calculating and setting values for things that do not vary over time such as component sizes, control parameters, modeling constants etc. The user defined component will trigger this calling manager during the intitial setup routines for plant systems.
+
+\subsubsection{Field: Air Connection Inlet Node Name}\label{field-air-connection-inlet-node-name}
+
+This field defines the name of the HVAC system node from which the plant component draws its inlet air for its air loop connection. This field is optional.
+
+\subsubsection{Field: Air Connection Outlet Node Name}\label{field-air-connection-outlet-node-name}
+
+This field defines the name of the HVAC system node to which the plant component sends its outlet air for its air loop connection. This field is optional.
+
+\subsubsection{Field: Supply Inlet Water Storage Tank Name}\label{field-supply-inlet-water-storage-tank-name-3}
+
+This field is used to describe where the plant component obtains water if it is to be connected to a water storage tank. This water could be used for evaporative cooling. If a name of a WaterUse:Storage object is used here, then the component can obtain its water from that tank. This field is optional.
+
+\subsubsection{Field: Collection Outlet Water Storage Tank Name}\label{field-collection-outlet-water-storage-tank-name-3}
+
+This field is used to describe where the plant component sends water it has collected if is to be stored in a tank. This water could be collected from coil condensate. If a name of a WaterUse:Storage object is used here, then the unit can send water to that tank. This field is optional.
+
+\subsubsection{Field: Ambient Zone Name}\label{field-ambient-zone-name-3}
+
+This field is used to connect ancillary losses from the plant component to a thermal zone. The component may have inefficiencies, leaks, or other non-ideal operation that results in some untended impact on the space surrounding the device. These skin losses can be assigned to a thermal zone and appear as internal gains for the zone named here. For example, this would be the mechanical room where the plant component is located.
+
+An example of this input object follows:
+
+\begin{lstlisting}
+
+PlantComponent:UserDefined,
+  Central Chiller,   !- Name
+  , !- Main Model Program Calling Manager Name
+  1 ,   !- Number of Plant Loop Connections
+  Central Chiller Inlet Node,     !- Plant Connection 1 Inlet Node Name
+  Central Chiller Outlet Node , !- Plant Connection 1 Outlet Node Name
+  MeetsLoadWithNominalCapacityLowOutLimit, !- Plant Connection 1 Loading Mode
+  NeedsFlowIfLoopOn , !- Plant Connection 1 Loop Flow Request Mode
+  Chiller model init programs, !- Plant Connection 1 Initialization Program Calling Manager Name
+  Chiller model simulation programs ,!- Plant Connection 1 Simulation Program Calling Manager Name
+  , !- Plant Connection 2 Inlet Node Name
+  , !- Plant Connection 2 Outlet Node Name
+  , !- Plant Connection 2 Loading Mode
+  , !- Plant Connection 2 Loop Flow Request Mode
+  , !- Plant Connection 2 Initialization Program Calling Manager Names
+  , !- Plant Connection 2 Simulation Program Calling Manager Name
+  , !- Plant Connection 3 Inlet Node Name
+  , !- Plant Connection 3 Outlet Node Name
+  , !- Plant Connection 3 Loading Mode
+  , !- Plant Connection 3 Loop Flow Request Mode
+  , !- Plant Connection 3 Initialization Program Calling Manager Name
+  , !- Plant Connection 3 Simulation Program Calling Manager Name
+  , !- Plant Connection 4 Inlet Node Name
+  , !- Plant Connection 4 Outlet Node Name
+  , !- Plant Connection 4 Loading Mode
+  , !- Plant Connection 4 Loop Flow Request Mode
+  , !- Plant Connection 4 Initialization Program Calling Manager Name
+  , !- Plant Connection 4 Simulation Program Calling Manager Name
+  Central Chiller Condenser Inlet Node, !- Air Connection Inlet Node Name
+  Central Chiller Condenser Outlet Node, !- Air Connection Outlet Node Name
+  , !- Supply Inlet Water Storage Tank Name
+  , !- Collection Outlet Water Storage Tank Name
+  ; !- Ambient Zone Name
+\end{lstlisting}
+
+\subsection{PlantEquipmentOperation:UserDefined}\label{plantequipmentoperationuserdefined}
+
+This object is used to define a generic plant equipment operation scheme. The PlantEquipmentOperation:UserDefined object appears directly in either a PlantEquipmentOperationSchemes or a CondenserEquipmentOperationSchemes object. The user can configure exactly how supply side equipment is dispatched to meet loads by writing EnergyPlus Runtime Language programs and using the EMS features. There are no output variables specifically associated with this object but the outcome of load distribution actuators can be examined using the output variable called Plant Component Distributed Demand Rate.
+
+\subsubsection{Inputs}\label{inputs-1-047}
+
+\paragraph{Field: Name}\label{field-name-4-032}
+
+This field specifies the unique user-assigned name of the custom operation scheme.
+
+\paragraph{Field: Main Model Program Calling Manager Name}\label{field-main-model-program-calling-manager-name-1}
+
+This field specifies the Erl programs that are used to model the custom plant operation scheme. The field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere. The program manager referenced here should include all the Erl programs that are to be run each time the operation scheme is simulated and use the calling point called UserDefinedComponentModel.
+
+\paragraph{Field: Initialization Program Calling Manager Name}\label{field-initialization-program-calling-manager-name}
+
+This field specifies the Erl programs that are used to initialize and do an one-time setup needed for the custom operation scheme. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere and uses the calling point called UserDefinedComponentModel. The program manager referenced here should include all the Erl programs that are needed to do any initial setup that should occur before the main programs are run. These include calculating and setting values for things that do not vary over time such as component capacities, control range parameters, various constants etc. The user defined operation scheme will trigger this calling manager at the beginning of each new environment period.
+
+\paragraph{Field Set: (Equipment Object Type, Equipment Name)}\label{field-set-equipment-object-type-equipment-name}
+
+Up to ten pairs of fields can be used to define the equipment governed by this custom operation scheme.
+
+\paragraph{Field: Equipment \textless{}\#\textgreater{} Object Type}\label{field-equipment-object-type-000}
+
+This field specifies the type of equipment, or object name, for each machine to be controlled by the scheme.
+
+\paragraph{Field: Equipment \textless{}\#\textgreater{} Name}\label{field-equipment-name-000}
+
+This field specifies the user selected name of the equipment to be controlled by the scheme.
+
+The following example shows control of a chilled water plant with two chillers that have different sizes and load dispatch is scaled so that each chiller runs at the same part load ratio.
+
+\begin{lstlisting}
+
+PlantEquipmentOperation:UserDefined,
+  CoolSys1 Operation Scheme,  !- Name
+  Cooling_dispatch , !- Main Model Program Calling Manager Name
+  Init_Chiller_Capacity, !- Initialization Program Calling Manager Name
+  Chiller:Electric:ReformulatedEIR, !- Equipment 1 Object Type
+  CoolSys1 Chiller 1,    !- Equipment 1 Name
+  Chiller:Electric:ReformulatedEIR,* !- Equipment 2 Object Type
+  CoolSys1 Chiller 2;    !- Equipment 2 Name
+
+  EnergyManagementSystem:ProgramCallingManager,
+  Init_Chiller_Capacity,
+  UserDefinedComponentModel,
+  Init_Chiller_Capacity_Values;
+
+  EnergyManagementSystem:Program,
+  Init_Chiller_Capacity_Values,
+  Set totChilCap = Chil1_Cap + Chil2_Cap;
+
+  EnergyManagementSystem:GlobalVariable,
+  totChilCap;
+
+  EnergyManagementSystem:ProgramCallingManager,
+  Cooling_dispatch,
+  UserDefinedComponentModel,
+  Cooling_dispatch_Values;
+
+  EnergyManagementSystem:Program,
+  Cooling_dispatch_Values,
+  IF CoolSys1_LoopDmnd < 0.0,
+  Set UniformPLR* = CoolSys1_LoopDmnd / totChilCap,
+  Set UniformPLR* = * @min UniformPLR 1.0,
+  SET Chil1_Disptch = UniformPLR\*Chil1_Cap,
+  SET Chil2_Disptch = UniformPLR\*Chil2_Cap,
+  ELSE,
+  SET Chil1_Disptch = 0.0 ,
+  SET Chil2_Disptch = 0.0 ,
+  ENDIF;
+
+  EnergyManagementSystem:InternalVariable, CoolSys1_LoopDmnd,CoolSys1 Operation Scheme,Supply Side Current Demand Rate; !,[W]
+
+  EnergyManagementSystem:InternalVariable, Chil1_Cap, CoolSys1 Chiller 1, Chiller Nominal Capacity;
+
+  EnergyManagementSystem:InternalVariable, Chil2_Cap, CoolSys1 Chiller 2, Chiller Nominal Capacity;
+
+  EnergyManagementSystem:Actuator, Chil1_Disptch,CoolSys1 Operation Scheme:CoolSys1 Chiller 1,Plant Equipment Operation,Distributed Load Rate; ! [W]
+
+  EnergyManagementSystem:Actuator, Chil2_Disptch,CoolSys1 Operation Scheme:CoolSys1 Chiller 2,Plant Equipment Operation,Distributed Load Rate; ! [W]
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-variable-refrigerant-flow-equipment.tex b/doc/input-output-reference/src/overview/group-variable-refrigerant-flow-equipment.tex
new file mode 100644
index 00000000000..cbe5638a6d1
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-variable-refrigerant-flow-equipment.tex
@@ -0,0 +1,1193 @@
+\section{Group -- Variable Refrigerant Flow Equipment}\label{group-variable-refrigerant-flow-equipment}
+
+This group of EnergyPlus input objects describes the configurations of Variable Refrigerant Flow (VRF, or Variable Refrigerant Volume) air-conditioning systems.
+
+A VRF system is an air-conditioning system that varies the refrigerant flow rate using variable speed compressor(s) in the outdoor unit, and the electronic expansion valves (EEVs) located in each indoor unit. The system meets the space cooling or heating load requirements by maintaining the zone air temperature at the setpoint. The ability to control the refrigerant mass flow rate according to the cooling and/or heating load enables the use of as many as 60 or more indoor units with differing capacities in conjunction with one single outdoor unit. This unlocks the possibility of having individualized comfort control, simultaneous heating and cooling in different zones, and heat recovery from one zone to another. It may also lead to more efficient operations during part-load conditions.
+
+There are two alternative VRF models in EnergyPlus:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  \textbf{System curve based model (VRF-SysCurve)}. In this model, a number of system level curves are used to describe the VRF system performance. This model corresponds to the \emph{AirConditioner:VariableRefrigerantFlow} object.
+\item
+  \textbf{Physics based model (VRF-FluidTCtrl)}. This model is able to consider the dynamics of more operational parameters and is applicable for fluid temperature control. This model corresponds to the \emph{AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl} object.
+\end{enumerate}
+
+( Please refer to the engineering reference for more technical details of the two models).
+
+In the VRF system model, direct-expansion cooling and/or heating coils are configured in a zone terminal unit, which is connected to a zone via the zone inlet and exhaust nodes. The zone terminal units are identified in a \emph{ZoneTerminalUnitList} object, the name of which is entered as an input to the \emph{AirConditioner:VariableRefrigerantFlow} or \emph{AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl} object.
+
+The Energyplus connection methodology is shown as dashed and greyed arrows in the figure below according to the following rules:
+
+\begin{itemize}
+\item
+  The zone inlet and zone exhaust node names are defined in a \emph{ZoneHVAC:EquipmentConnections} object (bottom of figure).
+\item
+  A \emph{ZoneHVAC:TerminalUnit:VariableRefrigerantFlow} object will identify these zone exhaust and zone inlet node names as the terminal unit's air inlet and air outlet nodes, respectively.
+\item
+  All zone terminal units that are connected to the same \emph{AirConditioner:VariableRefrigerantFlow} or \emph{AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl} object are listed in a \emph{ZoneTerminalUnitList} object.
+\item
+  The name of the \emph{ZoneTerminalUnitList} object is an input to the \emph{AirConditioner:VariableRefrigerantFlow} or \emph{AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl} object.
+\item
+  The \emph{AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl} or \emph{AirConditioner:VariableRefrigerantFlow} object is not listed in an AirloopHVAC object, and therefore, can only be simulated if the terminal units are connected to the \emph{AirConditioner:VariableRefrigerantFlow} or \emph{AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl} object using the ZoneTerminalUnitList.
+\item
+  Secondary ZoneHVAC equipment objects may be used in the same zones as the terminal units for other purposes (e.g., code compliance)
+\end{itemize}
+
+The following schematic demonstrates these connection rules.
+
+\begin{figure}[hbtp] % fig 125
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image310.png}
+\caption{Variable Refrigerant Flow Schematic \protect \label{fig:variable-refrigerant-flow-schematic}}
+\end{figure}
+
+Energyplus object type and object name, and node name relationships are also shown in the following figure to aid in the assembly of this HVAC system type.
+
+\includegraphics{media/image311.png}
+
+\emph{(a) VRF model based on system curves (VRF-SysCurve)}
+
+\includegraphics{media/image312.png}
+
+\emph{(b) VRF model based on physics (VRF-FluidTCtrl)}
+
+Figure 126. Variable Refrigerant Flow Object Links
+
+\subsection{AirConditioner:VariableRefrigerantFlow}\label{airconditionervariablerefrigerantflow}
+
+\subsubsection{Inputs}\label{inputs-051}
+
+\paragraph{Field: Heat Pump Name}\label{field-heat-pump-name}
+
+This alpha field defines a unique user-assigned name for an instance of a variable refrigerant flow heat pump. Any reference to this heat pump will use this name. Since this object is not listed in an AirloopHVAC object, the most likely use of this name would be for reporting purposes.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-018}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump operates during a given time period. A schedule value equal to 0 denotes that the heat pump must be off for that time period. A value other than 0 denotes that the heat pump is available to operate during that time period. This schedule may be used to completely disable the heat pump (and all of its terminal units) as required. If this field is blank, the unit is enabled the entire simulation.
+
+\paragraph{Field: Gross Rated Total Cooling Capacity}\label{field-gross-rated-total-cooling-capacity-001}
+
+This numeric field defines the total cooling capacity (sensible + latent) of the heat pump at rated conditions in watts. The cooling capacity must be greater than 0 or set to autosize.
+
+\paragraph{Field: Gross Rated Cooling COP}\label{field-gross-rated-cooling-cop-001}
+
+This numeric field defines the cooling coefficient of performance at rated conditions. The cooling coefficient of performance includes compressor power and condenser fan power. This COP value does not account for impacts due to the supply air fan. The nominal heat pump cooling COP must be greater than 0. If this field is left blank, a default coefficient of performance of 3.3 is assumed.
+
+\paragraph{Field: Minimum Outdoor Temperature in Cooling Mode}\label{field-minimum-outdoor-temperature-in-cooling-mode-000}
+
+This numeric field defines the minimum source temperature allowed for cooling operation. For air-cooled equipment outdoor dry-bulb temperature is used. For water-cooled equipment inlet water temperature is used. Below this temperature, cooling is disabled. If this field is left blank, the default value is -6ºC.
+
+\paragraph{Field: Maximum Outdoor Temperature in Cooling Mode}\label{field-maximum-outdoor-temperature-in-cooling-mode-000}
+
+This numeric field defines the maximum source temperature allowed for cooling operation. For air-cooled equipment outdoor dry-bulb temperature is used. For water-cooled equipment inlet water temperature is used. Above this temperature, cooling is disabled. If this field is left blank, the default value is 43ºC.
+
+\paragraph{Field: Cooling Capacity Ratio Modifier Function of Low Temperature Curve Name}\label{field-cooling-capacity-ratio-modifier-function-of-low-temperature-curve-name}
+
+This alpha field defines the cooling capacity ratio modifier at low outdoor dry-bulb temperatures. This curve is a bi-quadratic equation using weighted average indoor wet-bulb temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air dry-bulb temperature as the independent variables. This performance curve can be used to describe the cooling capacity ratio at low outdoor temperatures (i.e., the following two curves are used) or can be used to describe the performance for all outdoor temperatures (i.e., the following two curves are not used). For this system type it is likely that all three of these performance curves will be required. See the Engineering Reference for more discussion on using this input field.
+
+\paragraph{Field: Cooling Capacity Ratio Boundary Curve Name}\label{field-cooling-capacity-ratio-boundary-curve-name}
+
+This alpha field defines the cooling capacity ratio boundary curve name. This curve is a linear, quadratic or cubic curve that defines a change in cooling capacity at a specific condenser entering air dry-bulb temperature as a function of indoor air wet-bulb temperature. This curve is used when the trend in cooling capacity changes dramatically as outdoor temperature changes. If the cooling capacity does not change dramatically with changes in outdoor conditions, this field may be left blank. See the Engineering Reference for more discussion on using this input field.
+
+\paragraph{Field: Cooling Capacity Ratio Modifier Function of High Temperature Curve Name}\label{field-cooling-capacity-ratio-modifier-function-of-high-temperature-curve-name}
+
+This alpha field defines the cooling capacity ratio modifier at high outdoor temperatures. This curve is a bi-quadratic equation using weighted average indoor wet-bulb temperature and condenser entering air dry-bulb temperature as the independent variables. This curve is used when the trend in cooling capacity changes dramatically as outdoor temperature changes. If the cooling capacity does not change dramatically with changes in outdoor conditions, this field may be left blank. See the Engineering Reference for more discussion on using this input field.
+
+\paragraph{Field: Cooling Energy Input Ratio Modifier Function of Low Temperature Curve Name}\label{field-cooling-energy-input-ratio-modifier-function-of-low-temperature-curve-name}
+
+This alpha field defines the cooling energy input ratio modifier at low outdoor temperatures. This curve is a bi-quadratic equation with a weighted average indoor wet-bulb temperature and condenser entering air dry-bulb temperature as the independent variables. This performance curve can be used to describe the cooling energy input ratio at low outdoor temperatures (i.e., the following two curves are used) or can be used to describe the performance for all outdoor temperatures (i.e., the following two curves are not used). For this system type it is likely that all three of these performance curves will be required. See the Engineering Reference for more discussion on using this input field.
+
+\paragraph{Field: Cooling Energy Input Ratio Boundary Name}\label{field-cooling-energy-input-ratio-boundary-name}
+
+This alpha field defines the cooling energy input ratio boundary curve name. This curve is a linear, quadratic or cubic curve that defines a change in cooling energy at a specific condenser entering air dry-bulb temperature as a function of indoor air wet-bulb temperature. This curve is used when the trend in cooling energy changes dramatically as outdoor temperature changes. If the cooling energy does not change dramatically with changes in outdoor conditions, this field may be left blank. See the Engineering Reference for more discussion on using this input field.
+
+\paragraph{Field: Cooling Energy Input Ratio Modifier Function of High Temperature Curve Name}\label{field-cooling-energy-input-ratio-modifier-function-of-high-temperature-curve-name}
+
+This alpha field defines the cooling energy input ratio modifier at high outdoor temperatures. This curve is a bi-quadratic equation with weighted average indoor wet-bulb temperature and condenser entering air dry-bulb temperature as the independent variables. This curve is used when the trend in cooling energy changes dramatically as outdoor temperature changes. If the cooling energy does not change dramatically with changes in outdoor conditions, this field may be left blank. See the Engineering Reference for more discussion on using this input field.
+
+\paragraph{Field: Cooling Energy Input Ratio Modifier Function of Low Part-Load Ratio Curve Name}\label{field-cooling-energy-input-ratio-modifier-function-of-low-part-load-ratio-curve-name}
+
+This alpha field defines the cooling energy input ratio modifier (function of part-load ratio when PLR is less than or equal to 1) curve name. This curve is a linear, quadratic or cubic equation with cooling part-load ratio used as the independent variable. The cooling energy input ratio modifier curve is normalized to 1 at a part-load ratio of 1 and is used only when the operating part-load ratio is less than or equal to 1.
+
+\paragraph{Field: Cooling Energy Input Ratio Modifier Function of HIgh Part-Load Ratio Curve Name}\label{field-cooling-energy-input-ratio-modifier-function-of-high-part-load-ratio-curve-name}
+
+This alpha field defines the cooling energy input ratio modifier (function of part-load ratio when PLR is greater than 1) curve name. This curve is a linear, quadratic or cubic equation with cooling part-load ratio used as the independent variable. The cooling energy input ratio modifier curve is normalized to 1 at a part-load ratio of 1 and is used only when the operating part-load ratio is greater than 1.
+
+\paragraph{Field: Cooling Combination Ratio Correction Factor Curve Name}\label{field-cooling-combination-ratio-correction-factor-curve-name}
+
+This alpha field defines the cooling combination ratio (CR) correction factor curve name for combination ratios greater than or equal to 1. The combination ratio is defined as the total rated indoor terminal unit cooling capacity divided by this heat pump's gross rated total cooling capacity. The curve is a linear, quadratic or cubic equation and uses the minimum value of x in the curve object to determine the maximum part-load ratio which is linearly proportional to capacity (i.e., the minimum value of x {[}CR{]} in the curve object must be ≥1). The output of this curve provides a multiplier (\textgreater{}1) which is applied to this heat pump's Gross Rated Total Cooling Capacity. Between a combination ratio of 1 and the curve's minimum value of x, the multiplier is linearly interpolated. For combination ratio's less than 1 (i.e., the total indoor terminal unit capacity is less than this heat pump's rated total capacity), capacity is directly proportional to part-load ratio and this curve will not be used.
+
+\paragraph{Field: Cooling Part-Load Fraction Correlation Curve Name}\label{field-cooling-part-load-fraction-correlation-curve-name}
+
+This alpha field defines the cooling part-load fraction correlation curve name. This curve is used to define the cycling losses when the condenser's compressors cycle on and off. The compressor cycles when the cooling part-load ratio is less than the Minimum Heat Pump Part-Load Ratio specified later in this object's inputs.
+
+\paragraph{Field: Gross Rated Heating Capacity}\label{field-gross-rated-heating-capacity-001}
+
+This numeric field defines the gross total heat pump heating capacity at rated conditions in watts. The nominal heat pump heating capacity must be greater than 0 or set to autosize.
+
+\paragraph{Field: Rated Heating Capacity Sizing Ratio}\label{field-rated-heating-capacity-sizing-ratio-000}
+
+This numeric field defines the ratio of gross heating to gross cooling capacity. The model assumes that when used, this value will be greater than 1. A similar input is available in the ZoneHVAC:TerminalUnit:VariableRefrigerantFlow object. When the heating capacity is autosized, if this field is non-blank, this ratio is used to scale the heating capacity to the gross rated total cooling capacity regardless of the value entered in the terminal unit objects. When the heating capacity is not autosized, the gross rated heating capacity will be equal to the value specified in the Gross Rated Heating Capacity input field and this value will be compared to the sum of the terminal unit heating coil size. If these values are more than 10\% different, a warning will be issued when Output:Diagnostics, DisplayExtraWarnings; is included in the input file. If this field is blank and the terminal unit sizing ratio input is also blank, then the heating capacity sizing ratio is assumed to be 1. If this field is not blank and the heating capacity sizing ratio in the terminal unit object(s) is blank, then this ratio also applies to each heating coil. If this field is not blank and the heating capacity sizing ratio in the terminal units is also not blank, then the terminal unit heating coil capacity sizing ratio input applies to each heating coil.
+
+\paragraph{Field: Gross Rated Heating COP}\label{field-gross-rated-heating-cop-001}
+
+This numeric field defines the heating coefficient of performance at rated conditions. The heating coefficient of performance includes compressor power and condenser fan power. This gross COP value does NOT account for~ the supply air fan. The nominal heat pump heating COP must be greater than 0. If this field is left blank, a coefficient of performance of 3.4 is assumed.
+
+\paragraph{Field: Minimum Outdoor Temperature in Heating Mode}\label{field-minimum-outdoor-temperature-in-heating-mode-000}
+
+This numeric field defines the minimum outdoor temperature allowed for heating operation. Below this temperature, heating is disabled. If this field is left blank, the default value is -20ºC.
+
+\paragraph{Field: Maximum Outdoor Temperature in Heating Mode}\label{field-maximum-outdoor-temperature-in-heating-mode-000}
+
+This numeric field defines the maximum outdoor temperature allowed for heating operation. Above this temperature, heating is disabled. If this field is left blank, the default value is 16ºC.
+
+\paragraph{Field: Heating Capacity Ratio Modifier Function of Low Temperature Curve Name}\label{field-heating-capacity-ratio-modifier-function-of-low-temperature-curve-name}
+
+This alpha field defines the heating capacity ratio modifier at low temperature curve name. This curve is a bi-quadratic equation with a weighted average indoor dry-bulb temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air dry-bulb or wet-bulb temperature as the independent variables. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This performance curve can be used to describe the heating capacity ratio at low outdoor temperatures (i.e., the following two curves are used) or can be used to describe the performance for all outdoor temperatures (i.e., the following two curves are not used). For this system type it is likely that all three of these performance curves will be required. See the Engineering Reference for more discussion on using this input field.
+
+\paragraph{Field: Heating Capacity Ratio Boundary Curve Name}\label{field-heating-capacity-ratio-boundary-curve-name}
+
+This alpha field defines the heating capacity ratio boundary curve name. This curve is a quadratic or cubic curve that defines a change in heating capacity at a specific condenser entering air dry-bulb or wet-bulb temperature as a function of indoor air dry-bulb temperature. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This curve is used when the trend in heating capacity changes dramatically as outdoor temperature changes. If the heating capacity does not change dramatically with changes in outdoor conditions, this field may be left blank.
+
+\paragraph{Field: Heating Capacity Ratio Modifier Function of High Temperature Curve Name}\label{field-heating-capacity-ratio-modifier-function-of-high-temperature-curve-name}
+
+This alpha field defines the heating capacity ratio modifier at high temperature curve name. This curve is a bi-quadratic equation with a weighted average indoor dry-bulb temperature and condenser entering air dry-bulb or wet-bulb temperature as the independent variables. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This curve is used when the trend in heating capacity changes dramatically as outdoor temperature changes. If the heating capacity does not change dramatically with changes in outdoor conditions, this field may be left blank.
+
+\paragraph{Field: Heating Energy Input Ratio Modifier Function of Low Temperature Curve Name}\label{field-heating-energy-input-ratio-modifier-function-of-low-temperature-curve-name}
+
+This alpha field defines the heating energy input ratio modifier at low temperature curve name. This curve is a bi-quadratic equation with a weighted average indoor dry-bulb temperature and condenser entering air dry-bulb or wet-bulb temperature as the independent variables. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This performance curve can be used to describe the heating energy input ratio at low outdoor temperatures (i.e., the following two curves are used) or can be used to describe the performance for all outdoor temperatures (i.e., the following two curves are not used).
+
+\paragraph{Field: Heating Energy Input Ratio Boundary Curve Name}\label{field-heating-energy-input-ratio-boundary-curve-name}
+
+This alpha field defines the heating energy input ratio boundary curve name. This curve is a quadratic or cubic curve that defines a change in heating energy at a specific condenser entering air dry-bulb or wet-bulb temperature as a function of indoor air dry-bulb temperature. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This curve is used when the trend in heating energy changes dramatically as outdoor temperature changes. If the heating energy does not change dramatically with changes in outdoor conditions, this field may be left blank.
+
+\paragraph{Field: Heating Energy Input Ratio Modifier Function of High Temperature Curve Name}\label{field-heating-energy-input-ratio-modifier-function-of-high-temperature-curve-name}
+
+This alpha field defines the heating energy input ratio modifier at high temperature curve name. This curve is a bi-quadratic equation with a weighted average indoor dry-bulb temperature and condenser entering air dry-bulb or wet-bulb temperature as the independent variables. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This curve is used when the trend in heating energy changes dramatically as outdoor temperature changes. If the heating energy does not change dramatically with changes in outdoor conditions, this field may be left blank.
+
+\paragraph{Field: Heating Performance Curve Outdoor Temperature Type}\label{field-heating-performance-curve-outdoor-temperature-type}
+
+This choice field defines the outdoor temperature type used for all performance curves. The valid choices are DryBulbTemperature and WetBulbTemperature. The default value is WetBulbTemperature. Manufacturers will typically provide heating performance data as a function of outdoor air wet-bulb temperatures. This means that the performance (e.g., capacity and energy input ratio) curves will use outdoor wet-bulb temperature as one of the independent variables. At times, manufacturers will only provide performance data as a function of outdoor dry-bulb temperatures. In this case, all performance curves shall be developed using outdoor dry-bulb temperature and this field shall be selected as DryBulbTemperature.
+
+\paragraph{Field: Heating Energy Input Ratio Modifier Function of Low Part-Load Ratio Curve Name}\label{field-heating-energy-input-ratio-modifier-function-of-low-part-load-ratio-curve-name}
+
+This alpha field defines the heating energy input ratio modifier (function of part-load ratio when PLR is less than or equal to 1) curve name. This curve is a linear, quadratic, or cubic equation with heating part-load ratio used as the independent variable. The heating energy input ratio modifier curve is normalized to 1 at a part-load ratio of 1 and is used only when the part-load ratio is less than or equal to 1.
+
+\paragraph{Field: Heating Energy Input Ratio Modifier Function of High Part-Load Ratio Curve Name}\label{field-heating-energy-input-ratio-modifier-function-of-high-part-load-ratio-curve-name}
+
+This alpha field defines the heating energy input ratio modifier (function of part-load ratio when PLR is greater than 1) curve name. This curve is a linear, quadratic, or cubic equation with heating part-load ratio used as the independent variable. The heating energy input ratio modifier curve is normalized to 1 at a part-load ratio of 1 and is used only when the part-load ratio is greater than 1.
+
+\paragraph{Field: Heating Combination Ratio Correction Factor Curve Name}\label{field-heating-combination-ratio-correction-factor-curve-name}
+
+This alpha field defines the heating combination ratio (CR) correction factor curve name for combination ratios greater than or equal to 1. The combination ratio is defined as the total rated indoor heating capacity divided by the rated heat pump heating capacity. The curve is either quadratic or cubic and uses the minimum value of x in the curve object to determine the maximum part-load ratio which is linearly proportional to capacity (i.e., the minimum value of x in the curve object must be ≥1). The output of this curve provides a multiplier (\textgreater{}1) which is applied to the Nominal Heat Pump Heating Capacity. Between a combination ratio of 1 and the curve's minimum value of x, the multiplier is linearly interpolated. For combination ratio's less than 1, capacity is directly proportional to part-load ratio and this curve will not be used. If this field is left blank, the Cooling Combination Ratio Correction factor will be used.
+
+\paragraph{Field: Heating Part-Load Fraction Correlation Curve Name}\label{field-heating-part-load-fraction-correlation-curve-name}
+
+This alpha field defines the heating part-load fraction correlation curve name. This curve is used to define the cycling losses when the condenser's compressors cycle on and off. The compressor cycles when the indoor to outdoor heating capacity ratio is less than the Minimum Heat Pump Part-Load Ratio specified in the following field.
+
+\paragraph{Field: Minimum Heat Pump Part-Load Ratio}\label{field-minimum-heat-pump-part-load-ratio-000}
+
+This numeric field specifies the minimum operating part-load ratio (PLR) of the heat pump. When the heat pump operates at a PLR below this value, the heat pump's compressor will cycle to meet the cooling or heating demand. Above this value, the heat pump's compressor operates the entire time step to meet the cooling or heating demand. The minimum value for this field is 0. If this field is left blank, the default value is 0.15. When the heat pump compressor cycles, the previous field is used to determine cycling losses.
+
+\paragraph{Field: Zone Name for Master Thermostat Location}\label{field-zone-name-for-master-thermostat-location-000}
+
+This alpha field defines the name of the zone where the ``master'' thermostat is located. When the heat pump is connected to multiple zone terminal units, one terminal unit must be selected as the master thermostat. The remaining thermostats are slaves and can operate only in the same mode as the master thermostat.
+
+\paragraph{Field: Master Thermostat Priority Control Type}\label{field-master-thermostat-priority-control-type-000}
+
+This choice field determines the logic used to simulate the ``master'' thermostat. Valid choices are LoadPriority, ZonePriority, ThermostatOffsetPriority, MasterThermostatPriority, and Scheduled. The default value is MasterThermostatPriority. When LoadPriority is selected, the total zone load is used to choose the operating mode as either cooling or heating. When ZonePriority is selected, the number of zones requiring cooling or heating determines the operating mode. When ThermostatOffsetPriority is selected, the zone farthest from the thermostat set point determines the operating mode. The MasterThermostatPriority choice operates the system according the zone load where the master thermostat is located. The heat pump can also be scheduled to operate in either cooling or heating mode. For scheduled operation, a schedule name is entered in the following field.
+
+\paragraph{Field: Thermostat Priority Schedule Name}\label{field-thermostat-priority-schedule-name-000}
+
+This alpha field identifies the schedule used when the previous field is set to Scheduled. Schedule values of 0 denote heating mode while values of 1 denote cooling mode. Any other values will force the system off.
+
+\paragraph{Field: Zone Terminal Unit List Name}\label{field-zone-terminal-unit-list-name}
+
+This alpha field defines the name of the zone terminal unit list. The name specified here should match the name of a valid ZoneTerminalUnitList object. In addition, each name specified in this list should match the name of a valid ZoneHVAC:TerminalUnit: VariableRefrigerantFlow object. All terminal units connected to this heat pump must be listed in this ZoneTerminalUnitList object.
+
+Note: the previous field is designated at the last field necessary to simulate the variable refrigerant flow heat pump. The following fields do not have to be entered, however, piping loses, defrost operation, crankcase heater operation, and basin heater operation will not be modeled. Defaults for fields not entered may also not apply. These remaining fields must be entered if that portion of the model is to be simulated.
+
+\paragraph{Field: Heat Pump Waste Heat Recovery}\label{field-heat-pump-waste-heat-recovery-000}
+
+This choice field defines the configuration of the heat pump refrigeration system. Valid choices are \textbf{Yes} and \textbf{No}. If Yes is selected, heat recovery is enabled and the heat pump can independently cool and heat different zones. If No is selected, the heat pump is only able to cool or heat for any given time step.
+
+\paragraph{Field: Equivalent Piping Length used for Piping Correction Factor in Cooling Mode}\label{field-equivalent-piping-length-used-for-piping-correction-factor-in-cooling-mode-000}
+
+This numeric field defines the equivalent pipe length in meters between the farthest terminal unit and the heat pump condenser. This value includes the gas refrigerant line length (for both horizontal and vertical distances), fitting losses, pipe bends, and other connections that contribute to piping losses. This field is used to calculate the piping correction factor in cooling mode. This value defines the head losses due to the pipe length between the farthest terminal unit and the heat pump condenser and impacts the maximum available capacity in cooling mode.
+
+\paragraph{Field: Vertical Height used for Piping Correction Factor}\label{field-vertical-height-used-for-piping-correction-factor-000}
+
+This numeric field defines the vertical pipe height in meters between the highest or lowest terminal unit and the heat pump condenser. This value defines the gravitational losses due to a change in height between the highest (positive value), or lowest (negative value) terminal unit and the heat pump condenser. The distance specified here is applied to the piping correction factor calculation for both cooling and heating. If the distance between the highest terminal unit above the heat pump condenser is greater than the distance between the lowest terminal unit below the condenser enter the difference between the highest and lowest terminal units as a positive distance, otherwise enter this difference as a negative distance. Example: if the distance from the heat pump condenser to the highest terminal unit above the condenser is 10 m and the distance from the heat pump condenser to the lowest terminal unit below the condenser is -15 m, then enter a value of -5 m in this field. This head loss impacts the maximum available capacity in cooling mode.
+
+\paragraph{Field: Piping Correction Factor for Length in Cooling Mode Curve Name}\label{field-piping-correction-factor-for-length-in-cooling-mode-curve-name}
+
+This alpha field defines the linear, quadratic, or cubic curve name used to calculate the piping correction factor for length in cooling mode. Piping losses are a function of piping length. If sufficient piping loss information is available where piping losses are also a function of combination ratio (i.e., in addition to length), a biquadratic performance curve may be used.
+
+\paragraph{Field: Piping Correction Factor for Height in Cooling Mode Coefficient}\label{field-piping-correction-factor-for-height-in-cooling-mode-coefficient}
+
+This numeric field defines the coefficient used to calculate the piping correction factor for height in cooling mode.
+
+\paragraph{Field: Equivalent Piping Length used for Piping Correction Factor in Heating Mode}\label{field-equivalent-piping-length-used-for-piping-correction-factor-in-heating-mode-000}
+
+This numeric field defines the equivalent pipe length in meters between the farthest terminal unit and the heat pump condenser. This value includes the liquid refrigerant line length (for both horizontal and vertical distances), fitting losses, pipe bends, and other connections that contribute to piping losses. This field is used to calculate the piping correction factor in heating mode. This value defines the head losses due to the pipe length between the farthest terminal unit and the heat pump condenser and impacts the maximum available capacity in heating mode.
+
+\paragraph{Field: Piping Correction Factor for Length in Heating Mode Curve Name}\label{field-piping-correction-factor-for-length-in-heating-mode-curve-name}
+
+This alpha field defines the linear, quadratic, or cubic curve name used to calculate the piping correction factor for length in heating mode. Piping losses are a function of piping length. If sufficient piping loss information is available where piping losses are also a function of combination ratio (i.e., in addition to length), a biquadratic performance curve may be used.
+
+\paragraph{Field: Piping Correction Factor for Height in Heating Mode Coefficient}\label{field-piping-correction-factor-for-height-in-heating-mode-coefficient}
+
+This numeric field defines the coefficient used to calculate the piping correction factor for height in heating mode.
+
+\paragraph{Field: Crankcase Heater Power per Compressor}\label{field-crankcase-heater-power-per-compressor-000}
+
+This numeric field defines the electrical power consumed by the crankcase heater in watts for \emph{each} compressor. This crankcase heater power is consumed when the outdoor temperature is below the maximum outdoor dry-bulb temperature for crankcase heater operation. The minimum value for this field is 0. If this field is left blank, the default value is 33 watts. Crankcase heater electrical consumption is applied only when the compressor is off or is applied during the off cycle when the compressor is cycling below the Minimum Heat Pump Part-Load Ratio. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Number of Compressors}\label{field-number-of-compressors-000}
+
+This numeric field defines the number of compressors in the heat pump condensing unit and is used exclusively to determine the operating characteristics of the crankcase heater. For example, if the number of compressors is 3, one crankcase heater will operate when the heat pump condensing unit's part-load ratio is less than or equal to 0.67 (when the ratio of compressor size to total compressor capacity input is 0.33) and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. Similarly, two crankcase heaters will operate when the heat pump condensing unit's PLR is less than or equal to 0.33 and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. If the heat pump condensing unit is off, all 3 crankcase heaters will operate if the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. The minimum value for this field is 1. If this field is left blank, the default value is 2. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Ratio of Compressor Size to Total Compressor Capacity}\label{field-ratio-of-compressor-size-to-total-compressor-capacity-000}
+
+This numeric field defines the size of the first stage compressor to the total compressor capacity and is used exclusively for calculating crankcase heater energy. If this field and the previous field are left blank, the default value is 0.5.~ If this field is left blank and the previous field is not blank, the compressors are assumed to be equally sized. When the number of compressors is greater than 2, the 2\(^{nd}\) stage compressor and all additional compressors are assumed to be equally sized. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Maximum Outdoor Dry-bulb Temperature for Crankcase Heater}\label{field-maximum-outdoor-dry-bulb-temperature-for-crankcase-heater-000}
+
+This numeric field defines the maximum outdoor temperature, in degrees Celsius, below which the crankcase heater will operate. If this field is left blank, the default value is 0°C. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Defrost Strategy}\label{field-defrost-strategy-001}
+
+This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse-cycle. Defrost can be disabled by entering a resistive defrost strategy using a timed defrost control, a 0 defrost time period fraction and a 0 resistive defrost heater capacity in the following inputs fields. This method is used when the Maximum Outdoor Dry-Bulb Temperature for Defrost Operation field value is greater than the expected minimum outdoor dry-bulb temperature simulated in the weather file.
+
+\paragraph{Field: Defrost Control}\label{field-defrost-control-001}
+
+This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value of compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field ``Defrost Time Period Fraction'' described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field ``Maximum Outdoor Dry-bulb Temperature for Defrost Operation'' described above. If this input field is left blank, the default defrost control is timed.
+
+\paragraph{Field: Defrost Energy Input Ratio Modifier Function of Temperature Curve Name}\label{field-defrost-energy-input-ratio-modifier-function-of-temperature-curve-name}
+
+This alpha field defines the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) during reverse-cycle defrost periods as a function of the outdoor air dry-bulb temperature and the weighted average wet-bulb temperature of the air entering the indoor terminal units. The output of this curve is multiplied by the coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the indoor and outdoor coils are operating. The curve is normalized to a value of 1.0 at the rating point conditions.
+
+\paragraph{Field: Defrost Time Period Fraction}\label{field-defrost-time-period-fraction-001}
+
+This numeric field defines the fraction of compressor runtime when the defrost cycle is active. For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
+
+\paragraph{Field: Resistive Defrost Heater Capacity}\label{field-resistive-defrost-heater-capacity-001}
+
+This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is `resistive' (see input field ``Defrost Strategy'' above). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.
+
+\paragraph{Field: Maximum Outdoor Dry-bulb Temperature for Defrost Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-defrost-operation-001}
+
+This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. If this input field is left blank, the default value is 5 C. Defrost can be completely eliminated by selecting a temperature lower than the minimum expected outdoor temperature found in the weather file.
+
+\paragraph{Field: Condenser Type}\label{field-condenser-type-003}
+
+This choice field defines the configuration of the heat pump condenser. Valid choices are \textbf{AirCooled}, \textbf{EvaporativelyCooled}, and \textbf{WaterCooled}.
+
+\paragraph{Field: Condenser Inlet Node Name}\label{field-condenser-inlet-node-name-000}
+
+This alpha field defines the name of the condenser inlet air or water node. For Condenser type = AirCooled, this node name should also be listed in an OutdoorAir:Node or OutdoorAir:NodeList object. If this field is blank, the model assumes an air-cooled condenser and the weather file is used to define the outdoor conditions entering the condenser. If this field is not blank, the node conditions are used to define the outdoor air or inlet water conditions entering the condenser. A node name is typically entered here for air-cooled systems when conditions other than those found in the weather file should be used (ref. OutdoorAir:Node related to height above ground).
+
+\paragraph{Field: Condenser Outlet Node Name}\label{field-condenser-outlet-node-name-000}
+
+This alpha field defines the name of the condenser outlet water node. This field is only used for water-cooled systems.
+
+\paragraph{Field: Water Condenser Volume Flow Rate}\label{field-water-condenser-volume-flow-rate-000}
+
+This numeric field defines the condenser water volume flow rate in cubic meters per second. This field is autosizable and only used for water-cooled systems.
+
+\paragraph{Field: Evaporative Condenser Effectiveness}\label{field-evaporative-condenser-effectiveness-002}
+
+The effectiveness of the evaporative condenser, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
+
+\begin{equation}
+Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectiveness} \right)\left( {Tdb,o\,\, - Twb,o} \right)
+\end{equation}
+
+where
+
+\emph{T\(_{cond\\ inlet}\)} = the temperature of the air entering the condenser coil (C)
+
+\emph{T\(_{wb,o}\)} = the wet-bulb temperature of the outdoor air (C)
+
+\emph{T\(_{db,o}\)} = the dry-bulb temperature of the outdoor air (C)
+
+The resulting condenser inlet air temperature is used by the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled and the simulation is calculating heating performance.
+
+If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
+
+If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = EvapCooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
+
+If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = EvapCooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Cooling Capacity and Cooling EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
+
+\paragraph{Field: Evaporative Condenser Air Flow Rate}\label{field-evaporative-condenser-air-flow-rate-002}
+
+The air volume flow rate, in m\(^{3}\) per second, entering the evaporative condenser. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000144 m\(^{3}\)/s per watt of rated total cooling capacity {[}850 cfm/ton{]}). This field is not used when Condenser Type = AirCooled.
+
+\paragraph{Field: Evaporative Condenser Pump Rated Power Consumption}\label{field-evaporative-condenser-pump-rated-power-consumption-001}
+
+The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt {[}15 W/ton{]} of rated total cooling capacity). This field is not used when Condenser Type = AirCooled.
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-001}
+
+This alpha field defines the name of the water storage tank when an evaporatively-cooled condenser is used.
+
+\paragraph{Field: Basin Heater Capacity}\label{field-basin-heater-capacity-004}
+
+This numeric field contains the capacity of the heat pump's electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the heat pump compressor(s) is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
+
+\paragraph{Field: Basin Heater Setpoint Temperature}\label{field-basin-heater-setpoint-temperature-004}
+
+This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the heat pump is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
+
+\paragraph{Field: Basin Heater Operating Schedule Name}\label{field-basin-heater-operating-schedule-name-003}
+
+This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the heat pump is off.
+
+\paragraph{Field: Fuel Type}\label{field-fuel-type-005}
+
+This alpha field determines the type of fuel that this variable refrigerant flow system uses.~ This field has seven choices: Electricity, NaturalGas, PropaneGas, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1, and OtherFuel2. The default is Electricity. The use of alternate fuel types assumes an engine drives the variable speed compression system and also accounts for condenser air flow (i.e., a fan attached to the engine provides air flow through the outdoor condenser.
+
+\paragraph{Field: Minimum Outdoor Temperature in Heat Recovery Mode}\label{field-minimum-outdoor-temperature-in-heat-recovery-mode-000}
+
+This numeric field defines the minimum outdoor dry-bulb temperature allowed for heat recovery operation. Below this temperature, heat recovery is disabled. This input must be greater than the larger of the minimum outdoor temperature in cooling or heating mode. If this field is left blank, the default value is the higher of the Minimum Outdoor Temperature in Cooling Mode or Minimum Outdoor Temperature in Heating Mode inputs. This system may still operate in cooling or heating only mode when outdoor temperatures are below the minimum outdoor temperature in heat recovery mode. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes.
+
+\paragraph{Field: Maximum Outdoor Temperature in Heat Recovery Mode}\label{field-maximum-outdoor-temperature-in-heat-recovery-mode-000}
+
+This numeric field defines the maximum outdoor dry-bulb temperature allowed for heat recovery operation. Above this temperature, heat recovery is disabled. This input must be less than the smaller of the maximum outdoor temperature in cooling or heating mode. If this field is left blank, the default value is the lower of the Maximum Outdoor Temperature in Cooling Mode or Maximum Outdoor Temperature in Heating Mode inputs.. This system may still operate in cooling or heating only mode when outdoor temperatures are above the maximum outdoor temperature in heat recovery mode. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes.
+
+\paragraph{Field: Heat Recovery Cooling Capacity Modifier Curve Name}\label{field-heat-recovery-cooling-capacity-modifier-curve-name}
+
+This alpha field defines the cooling capacity modifier when heat recovery mode is active. This modifier is used as a multiplier for available cooling capacity, and when in heat recovery mode, this modifier is usually less than 1. This curve is either a bi-quadratic equation using weighted average indoor temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air temperature as the independent variables or a cubic curve based on part-load ratio. This performance curve can be used to describe the cooling capacity modifier as either a constant (e.g., temperature or part-load ratio term coefficients are 0), a cooling modifier that varies with either indoor temperature and/or outdoor temperature, or part-load ratio (e.g., one or more temperature or part-load ratio term coefficients are 0), or varies with both indoor and outdoor temperatures or part-load ratio (e.g., all temperature or part-load ratio term coefficients are non-zero). If this field is left blank, and heat recovery operating mode is selected, the default constant modifier is 0.9. This modifier is applied only when heat recovery mode is active. To model a heat recovery system which has no degradation in cooling performance when heat recovery mode is active, or if the degradation is not constant at different operating conditions, a performance curve object must be used. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode.
+
+\paragraph{Field: Initial Heat Recovery Cooling Capacity Fraction}\label{field-initial-heat-recovery-cooling-capacity-fraction}
+
+This numeric field defines the fraction of cooling capacity available when the system transitions from cooling only operation to simultaneous cooling and heating. It is common for the cooling capacity to decrease before the system recovers. If this field is left blank, a default value of 0.5 is used (50\% reduction in cooling capacity at the start of heat recovery mode). The system will recovery according to the time constant entered in Heat Recovery Cooling Capacity Time Constant input field. If the transition period will not be modeled, this input field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
+
+\paragraph{Field: Heat Recovery Cooling Capacity Time Constant}\label{field-heat-recovery-cooling-capacity-time-constant}
+
+This numeric field defines the cooling capacity time constant, in hours, used to model the time it takes for the system to change from cooling only operation to simultaneous cooling and heating. Total response time is defined as 5 time constants. If this field is left blank, a default value of 0.083 is used. If the transition period will not be modeled, the Initial Heat Recovery Cooling Capacity Fraction field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
+
+\paragraph{Field: Heat Recovery Cooling Energy Modifier Curve Name}\label{field-heat-recovery-cooling-energy-modifier-curve-name}
+
+This alpha field defines the cooling energy modifier when heat recovery mode is active. This modifier is used as a multiplier for operating cooling energy, and when in heat recovery mode, this modifier is usually greater than 1. This curve is a bi-quadratic equation using weighted average indoor temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air temperature as the independent variables. This performance curve can be used to describe the cooling energy modifier as either a constant (e.g., temperature term coefficients are 0), a cooling energy modifier that varies with indoor and/or outdoor temperatures (e.g., one or more temperature term coefficients are 0), or varies with both indoor and outdoor temperatures (e.g., temperature term coefficients are non-zero). If this field is left blank, and heat recovery operating mode is selected, the default constant modifier is 1.1. This modifier is applied only when heat recovery mode is active. To model a heat recovery system which has no degradation in cooling performance when heat recovery mode is active, or if the degradation is not constant at different operating conditions, a performance curve object must be used. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode.
+
+\paragraph{Field: Initial Heat Recovery Cooling Energy Fraction}\label{field-initial-heat-recovery-cooling-energy-fraction}
+
+This numeric field defines the fraction of cooling energy consumed when the system transitions from cooling only operation to simultaneous cooling and heating. It is common for the cooling energy to drop before the system recovers. If this field is left blank, a default value of 1 is used (no change in energy at the start of heat recovery mode). If the transition period will not be modeled, this input field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
+
+\paragraph{Field: Heat Recovery Cooling Energy Time Constant}\label{field-heat-recovery-cooling-energy-time-constant}
+
+This numeric field defines the cooling energy time constant, in hours, used to model the time it takes for the system to transition from cooling only operation to simultaneous cooling and heating. Total response time is defined as 5 time constants. If this field is left blank, a default value of 0.0 is used. If the transition period will not be modeled, the Initial Heat Recovery Cooling Energy Fraction field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
+
+\paragraph{Field: Heat Recovery Heating Capacity Modifier Curve Name}\label{field-heat-recovery-heating-capacity-modifier-curve-name}
+
+This alpha field defines the heating capacity modifier when heat recovery mode is active. This modifier is used as a multiplier for available heating capacity, and when in heat recovery mode, this modifier is usually less than 1. This curve is a bi-quadratic equation using weighted average indoor temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air temperature as the independent variables. This performance curve can be used to describe the heating capacity modifier as either a constant (e.g., temperature term coefficients are 0), a heating modifier that varies with indoor and/or outdoor temperatures (e.g., one or more temperature term coefficients are 0), or varies with both indoor and outdoor temperatures (e.g., temperature term coefficients are non-zero). If this field is left blank, and heat recovery operating mode is selected, the default constant modifier is 0.9. This modifier is applied only when heat recovery mode is active. To model a heat recovery system which has no degradation in heating performance when heat recovery mode is active, or if the degradation is not constant at different operating conditions, a performance curve object must be used. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode.
+
+\paragraph{Field: Initial Heat Recovery Heating Capacity Fraction}\label{field-initial-heat-recovery-heating-capacity-fraction}
+
+This numeric field defines the fraction of heating capacity available when the system changes from heating only operation to simultaneous heating and cooling. It is common for the heating capacity to decrease before the system recovers. If this field is left blank, a default value of 0.5 is used (50\% reduction in heating capacity at the start of heat recovery mode). The system will recovery according to the time constant entered in Heat Recovery Heating Capacity Time Constant input field. If the transition period will not be modeled, this input field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
+
+\paragraph{Field: Heat Recovery Heating Capacity Time Constant}\label{field-heat-recovery-heating-capacity-time-constant}
+
+This numeric field defines the heating capacity time constant, in hours, used to model the time it takes for the system to transition from cooling only operation to simultaneous cooling and heating. Total response time is defined as 5 time constants. If this field is left blank, a default value of 0.083 is used. If the transition period will not be modeled, the Initial Heat Recovery Heating Capacity Fraction field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
+
+\paragraph{Field: Heat Recovery Heating Energy Modifier Curve Name}\label{field-heat-recovery-heating-energy-modifier-curve-name}
+
+This alpha field defines the heating energy modifier when heat recovery mode is active. This modifier is used as a multiplier for operating heating energy, and when in heat recovery mode, this modifier is usually greater than 1. This curve is a bi-quadratic equation using weighted average indoor temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air temperature as the independent variables. This performance curve can be used to describe the heating energy modifier as either a constant (e.g., temperature term coefficients are 0), a heating energy modifier that varies with indoor and/or outdoor temperatures (e.g., one or more temperature term coefficients are 0), or varies with both indoor and outdoor temperatures (e.g., temperature term coefficients are non-zero). If this field is left blank, and heat recovery operating mode is selected, the default constant modifier is 1.1. This modifier is applied only when heat recovery mode is active. To model a heat recovery system which has no degradation in heating performance when heat recovery mode is active, or if the degradation is not constant at different operating conditions, a performance curve object must be used. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode.
+
+\paragraph{Field: Initial Heat Recovery Heating Energy Fraction}\label{field-initial-heat-recovery-heating-energy-fraction}
+
+This numeric field defines the fraction of heating energy consumed when the system changes from heating only operation to simultaneous heating and cooling. It is common for the heating energy to decrease before the system recovers. If this field is left blank, a default value of 0.5 is used (50\% reduction in heating energy at the start of heat recovery mode). The system will recovery according to the time constant entered in Heat Recovery Heating Energy Time Constant input field. If the transition period will not be modeled, this input field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
+
+\paragraph{Field: Heat Recovery Heating Energy Time Constant}\label{field-heat-recovery-heating-energy-time-constant}
+
+This numeric field defines the heating energy time constant, in hours, used to model the time it takes for the system to change from cooling only operation to simultaneous cooling and heating. Total response time is defined as 5 time constants. If this field is left blank, a default value of 0.0 is used. If the transition period will not be modeled, the Initial Heat Recovery Heating Energy Fraction field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
+
+Following is an example input for a AirConditioner:VariableRefrigerantFlow system.
+
+\begin{lstlisting}
+
+AirConditioner:VariableRefrigerantFlow,
+    VRF Heat Pump,        !- Heat Pump Name
+    VRFCondAvailSched,    !- Availability Schedule Name
+    autosize,             !- Gross Rated Total Cooling Capacity {W}
+    3.16038,              !- Gross Rated Cooling COP {W}
+    -5,                   !- Minimum Outdoor Temperature in Cooling Mode {C}
+    43,                   !- Maximum Outdoor Temperature in Cooling Mode {C}
+    VRFCoolCapFT,         !- Cooling Capacity Ratio Modifier Function of Low Temperature Curve Name
+    VRFCoolCapFTBoundary, !- Cooling Capacity Ratio Boundary Curve Name
+    VRFCoolCapFTHi,       !- Cooling Capacity Ratio Modifier Function of High Temperature Curve Name
+    VRFCoolEIRFT,         !- Cooling Energy Input Ratio Modifier Function of Low Temperature Curve Name
+    VRFCoolEIRFTBoundary, !- Cooling Energy Input Ratio Boundary Curve Name
+    VRFCoolEIRFTHi,       !- Cooling Energy Input Ratio Modifier Function of High Temperature Curve Name
+    CoolingEIRLowPLR,     !- Cooling Energy Input Ratio Modifier Function of Low Part-Load Ratio Curve Name
+    CoolingEIRHiPLR,      !- Cooling Energy Input Ratio Modifier Function of High Part-Load Ratio Curve Name
+    CoolingCombRatio,     !- Cooling Combination Ratio Correction Factor Curve Name
+    VRFCPLFFPLR,          !- Cooling Part-Load Fraction Correlation Curve Name
+    autosize,             !- Gross Rated Heating Capacity {W}
+    ,                     !- Rated Heating Capacity Sizing Ratio (W/W)
+    3.40909,              !- Gross Rated Heating COP
+    -20,                  !- Minimum Outdoor Temperature in Heating Mode {C}
+    15.5,                 !- Maximum Outdoor Temperature in Heating Mode {C}
+    VRFHeatCapFT,         !- Heating Capacity Ratio Modifier Function of Low Temperature Curve Name
+    VRFHeatCapFTBoundary, !- Heating Capacity Ratio Boundary Curve Name
+    VRFHeatCapFTHi,       !- Heating Capacity Ratio Modifier Function of High Temperature Curve Name
+    VRFHeatEIRFT,         !- Heating Energy Input Ratio Modifier Function of Low Temperature Curve Name
+    VRFHeatEIRFTBoundary, !- Heating Energy Input Ratio Boundary Curve Name
+    VRFHeatEIRFTHi,       !- Heating Energy Input Ratio Modifier Function of High Temperature Curve Name
+    WetBulbTemperature,   !- Heating Performance Curve Outdoor Temperature Type
+    HeatingEIRLowPLR,     !- Heating Energy Input Ratio Modifier Function of Low Part-Load Ratio Curve Name
+    HeatingEIRHiPLR,      !- Heating Energy Input Ratio Modifier Function of High Part-Load Ratio Curve Name
+    HeatingCombRatio,     !- Heating Combination Ratio Correction Factor Curve Name
+    VRFCPLFFPLR,          !- Heating Part-Load Fraction Correlation Curve Name
+    0.25,                 !- Minimum Heat Pump Part-Load Ratio
+    SPACE1-1,             !- Zone Name for Master Thermostat Location
+    LoadPriority,         !- Master Thermostat Priority Control Type
+    ,                     !- Thermostat Priority Schedule Name
+    VRF Heat Pump TU List, !- Zone Terminal Unit List Name
+    No,                   !- Heat Pump Waste Heat Recovery
+    30,                   !- Equivalent Piping Length used for Piping Correction Factor in Cooling Mode {m}
+    10,                   !- Vertical Height used for Piping Correction Factor {m}
+    CoolingLengthCorrectionFactor,  !- Piping Correction Factor for Length in Cooling Mode Curve Name
+    -0.000386,            !- Piping Correction Factor for Height in Cooling Mode Coefficient
+    30,                   !- Equivalent Piping Length used for Piping Correction Factor in Heating Mode {m}
+    ,                     !- Piping Correction Factor for Length in Heating Mode Curve Name
+    ,                     !- Piping Correction Factor for Height in Heating Mode Coefficient
+    15,                   !- Crankcase Heater Power per Compressor {W}
+    3,                    !- Number of Compressors
+    0.33,                 !- Ratio of Compressor Size to Total Compressor Capacity
+    7,                    !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater {C}
+    Resistive,            !- Defrost Strategy
+    Timed,                !- Defrost Control
+    ,                     !- Defrost Energy Input Ratio Modifier Function of Temperature Curve Name
+    ,                     !- Defrost Time Period Fraction
+    autosize,             !- Resistive Defrost Heater Capacity {W}
+    7,                    !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation {C}
+    EvaporativelyCooled,  !- Condenser Type
+    MyVRFOANode,          !- Condenser Inlet Node Name
+    ,                     !- Condenser Outlet Node Name
+    ,                     !- Water Condenser Volume Flow Rate
+    ,                     !- Evaporative Condenser Effectiveness {dimensionless}
+    autosize,             !- Evaporative Condenser Air Flow Rate {m3/s}
+    autosize,             !- Evaporative Condenser Pump Rated Power Consumption {W}
+    ,                     !- Supply Water Storage Tank Name
+    200,                  !- Basin Heater Capacity {W/K}
+    ,                     !- Basin Heater Set Point Temperature (C)
+    ,                     !- Basin Heater Operating Schedule Name
+    ,                     !- Fuel Type
+    ,                     !- Minimum Outdoor Temperature in Heat Recovery Mode (C)
+    ,                     !- Maximum Outdoor Temperature in Heat Recovery Mode (C)
+    ,                     !- Heat Recovery Cooling Capacity Modifier Function of Temperature Curve Name
+    ,                     !- Initial Heat Recovery Cooling Capacity Fraction
+    ,                     !- Heat Recovery Cooling Capacity Time Constant (hr)
+    ,                     !- Heat Recovery Cooling Energy Modifier Function of Temperature Curve Name
+    ,                     !- Initial Heat Recovery Cooling Energy Fraction
+    ,                     !- Heat Recovery Cooling Energy Time Constant (hr)
+    ,                     !- Heat Recovery Heating Capacity Modifier Function of Temperature Curve Name
+    ,                     !- Initial Heat Recovery Heating Capacity Fraction
+    ,                     !- Heat Recovery Heating Capacity Time Constant (hr)
+    ,                     !- Heat Recovery Heating Energy Modifier Function of Temperature Curve Name
+    ,                     !- Initial Heat Recovery Heating Energy Fraction
+    ;                     !- Heat Recovery Heating Energy Time Constant (hr)
+\end{lstlisting}
+
+\subsection{AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl}\label{airconditionervariablerefrigerantflowfluidtemperaturecontrol}
+
+\subsubsection{Inputs}\label{inputs-1-048}
+
+\paragraph{Field: Heat Pump Name}\label{field-heat-pump-name-1}
+
+This alpha field defines a unique user-assigned name for an instance of a variable refrigerant flow heat pump. Any reference to this heat pump will use this name. Since this object is not listed in an AirloopHVAC object, the most likely use of this name would be for reporting purposes.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-013}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump operates during a given time period. A schedule value equal to 0 denotes that the heat pump must be off for that time period. A value other than 0 denotes that the heat pump is available to operate during that time period. This schedule may be used to completely disable the heat pump (and all of its terminal units) as required. If this field is blank, the unit is enabled the entire simulation.
+
+\paragraph{Field: Zone Terminal Unit List Name}\label{field-zone-terminal-unit-list-name-1}
+
+This alpha field defines the name of the zone terminal unit list. The name specified here should match the name of a valid ZoneTerminalUnitList object. In addition, each name specified in this list should match the name of a valid ZoneHVAC:TerminalUnit:VariableRefrigerantFlow object. All terminal units connected to this heat pump must be listed in this ZoneTerminalUnitList object.
+
+\paragraph{Field: Refrigerant Type}\label{field-refrigerant-type-000}
+
+This alpha field defines the name of the refrigerant used in the VRF system. The name specified here should match the name of a valid FluidProperties:Name object.
+
+\paragraph{Field: Rated Evaporative Capacity}\label{field-rated-evaporative-capacity}
+
+This numeric field defines the total evaporative capacity in watts at rated conditions. This is the capacity corresponding to the max compressor speed at rated conditions. The actual evaporative capacity is obtained by multiplying the rated capacity with the modification factor calculated by Evaporative Capacity Multiplier Function of Temperature Curve. The value must be greater than 0. If this field is left blank, a default value of 40,000 W is assumed.
+
+\paragraph{Field: Rated Compressor Power Per Unit of Rated Evaporative Capacity}\label{field-rated-compressor-power-per-unit-of-rated-evaporative-capacity}
+
+This numeric field defines the rated compressor power per Watt of rated evaporative capacity. Rated compressor power corresponds to the max compressor speed at rated conditions. The actual compressor power is obtained by multiplying the rated power with the modification factor calculated by Compressor Power Multiplier Function of Temperature Curve. The value must be greater than 0. If this field is left blank, a default value of 0.35 W/W is assumed.
+
+\paragraph{Field: Minimum Outdoor Air Temperature in Cooling Mode}\label{field-minimum-outdoor-air-temperature-in-cooling-mode}
+
+This numeric field defines the minimum source temperature allowed for heating operation. For air-cooled equipment outdoor dry-bulb temperature is used. For water-cooled equipment inlet water temperature is used. Below this temperature, heating is disabled. If this field is left blank, the default value is -20ºC.
+
+\paragraph{Field: Maximum Outdoor Air Temperature in Cooling Mode}\label{field-maximum-outdoor-air-temperature-in-cooling-mode}
+
+This numeric field defines the maximum source temperature allowed for heating operation. For air-cooled equipment outdoor dry-bulb temperature is used. For water-cooled equipment inlet water temperature is used. Above this temperature, heating is disabled. If this field is left blank, the default value is 16ºC.
+
+\paragraph{Field: Minimum Outdoor Air Temperature in Heating Mode}\label{field-minimum-outdoor-air-temperature-in-heating-mode}
+
+This numeric field defines the minimum outdoor temperature allowed for heating operation. Below this temperature, heating is disabled. If this field is left blank, the default value is -20ºC.
+
+\paragraph{Field: Maximum Outdoor Air Temperature in Heating Mode}\label{field-maximum-outdoor-air-temperature-in-heating-mode}
+
+This numeric field defines the maximum outdoor temperature allowed for heating operation. Above this temperature, heating is disabled. If this field is left blank, the default value is 16ºC.
+
+\paragraph{Field: Outdoor Unit Reference Superheating}\label{field-outdoor-unit-reference-superheating}
+
+This numeric field defines the reference superheating degrees of the outdoor unit. If this field is blank, the default value of 3.0ºC is used.
+
+\paragraph{Field: Outdoor Unit Reference Subcooling}\label{field-outdoor-unit-reference-subcooling}
+
+This numeric field defines the reference subcooling degrees of the outdoor unit. If this field is blank, the default value of 3.0ºC is used.
+
+\paragraph{Field: Refrigerant Temperature Control Algorithm for Indoor Unit}\label{field-refrigerant-temperature-control-algorithm-for-indoor-unit}
+
+This alpha field specifies the algorithm for the refrigerant temperature control. Two choices are available: ConstantTemp or VariableTemp. The indoor unit evaporating temperature at cooling mode or condensing temperature at heating are fixed in the ConstantTemp algorithm, while in VariableTemp algorithm they can be varied.
+
+\paragraph{Field: Reference Evaporating Temperature for Indoor Unit}\label{field-reference-evaporating-temperature-for-indoor-unit}
+
+This numeric field defines the reference evaporating temperature for the indoor unit when VRF runs at cooling mode. This field is required if Refrigerant Temperature Control Algorithm is ConstantTemp. If this field is blank, the default value of 6.0ºC is used.
+
+\paragraph{Field: Reference Condensing Temperature for Indoor Unit}\label{field-reference-condensing-temperature-for-indoor-unit}
+
+This numeric field defines the reference condensing temperature for the indoor unit when VRF runs at heating mode. This field is required if Refrigerant Temperature Control Algorithm is ConstantTemp. If this field is blank, the default value of 44.0ºC is used.
+
+\paragraph{Field: Variable Evaporating Temperature Minimum for Indoor Unit}\label{field-variable-evaporating-temperature-minimum-for-indoor-unit}
+
+This numeric field defines the minimum evaporating temperature for the indoor unit when VRF runs at cooling mode. This field is required if Refrigerant Temperature Control Algorithm is VariableTemp. If this field is blank, the default value of 4.0ºC is used.
+
+\paragraph{Field: Variable Evaporating Temperature Maximum for Indoor Unit}\label{field-variable-evaporating-temperature-maximum-for-indoor-unit}
+
+This numeric field defines the maximum evaporating temperature for the indoor unit when VRF runs at cooling mode. This field is required if Refrigerant Temperature Control Algorithm is VariableTemp. If this field is blank, the default value of 13.0ºC is used.
+
+\paragraph{Field: Variable Condensing Temperature Minimum for Indoor Unit}\label{field-variable-condensing-temperature-minimum-for-indoor-unit}
+
+This numeric field defines the minimum condensing temperature for the indoor unit when VRF runs at heating mode. This field is required if Refrigerant Temperature Control Algorithm is VariableTemp. If this field is blank, the default value of 42.0ºC is used.
+
+\paragraph{Field: Variable Condensing Temperature Maximum for Indoor Unit}\label{field-variable-condensing-temperature-maximum-for-indoor-unit}
+
+This numeric field defines the maximum condensing temperature for the indoor unit when VRF runs at heating mode. This field is required if Refrigerant Temperature Control Algorithm is VariableTemp. If this field is blank, the default value of 46.0ºC is used.
+
+\paragraph{Field: Outdoor Unit Fan Power Per Unit of Rated Evaporative Capacity}\label{field-outdoor-unit-fan-power-per-unit-of-rated-evaporative-capacity}
+
+This numeric field defines the outdoor unit fan power per watt of rated evaporative capacity. If this field is blank, the default value of 4.25E-3 W/W is used.
+
+\paragraph{Field: Outdoor Unit Fan Flow Rate Per Unit of Rated Evaporative Capacity}\label{field-outdoor-unit-fan-flow-rate-per-unit-of-rated-evaporative-capacity}
+
+This numeric field defines the outdoor unit fan volumetric flow rate per watt of rated evaporative capacity. If this field is blank, the default value of 7.50E-5 m\(^{3}\)/s-W is used.
+
+\paragraph{Field: Outdoor Unit Evaporating Temperature Function of Superheating Curve Name}\label{field-outdoor-unit-evaporating-temperature-function-of-superheating-curve-name}
+
+This alpha field defines the name of a quadratic performance curve that parameterizes the variation of outdoor unit evaporating temperature as a function of superheating degrees. The output of this curve is the temperature difference between the coil surface air temperature and the evaporating temperature.
+
+\paragraph{Field: Outdoor Unit Condensing Temperature Function of Subcooling Curve Name}\label{field-outdoor-unit-condensing-temperature-function-of-subcooling-curve-name}
+
+This alpha field defines the name of a quadratic performance curve that parameterizes the variation of outdoor unit condensing temperature as a function of subcooling degrees. The output of this curve is the temperature difference between the condensing temperature and the coil surface air temperature.
+
+\paragraph{Field: Diameter of Main Pipe Connecting Outdoor Unit to Indoor Units}\label{field-diameter-of-main-pipe-connecting-outdoor-unit-to-indoor-units}
+
+This numeric field defines the diameter of main pipe connecting outdoor unit to indoor units. This value is used to calculate the piping loss of the refrigerant when going through the main pipe, including the heat loss and pressure drop. If this field is blank, the default value of 0.0254m is used.
+
+\paragraph{Field: Length of Main Pipe Connecting Outdoor Unit to Indoor Units}\label{field-length-of-main-pipe-connecting-outdoor-unit-to-indoor-units}
+
+This numeric field defines the length of main pipe connecting outdoor unit to indoor units. This value is used to calculate the heat loss of the refrigerant when going through the main pipe. The value should be greater than 0. If this field is blank, the default value of 30m is used.
+
+\paragraph{Field: Equivalent Length of Main Pipe Connecting Outdoor Unit to Indoor Units}\label{field-equivalent-length-of-main-pipe-connecting-outdoor-unit-to-indoor-units}
+
+This numeric field defines the equivalent length of main pipe connecting outdoor unit to indoor units. This value is used to calculate the pressure drop of the refrigerant when going through the main pipe. The value should be greater than the real pipe length specified in the above field. If this field is blank, the default value of 36m is used.
+
+\paragraph{Field: Height Difference Between Outdoor Unit and Indoor Units}\label{field-height-difference-between-outdoor-unit-and-indoor-units}
+
+This numeric field defines the height difference between the outdoor unit node and indoor unit node of the main pipe. This value is used to calculate the piping loss of the refrigerant when going through the main pipe. The value can be positive, zero, or negative. Positive means outdoor unit is higher than indoor unit, while negative means outdoor unit is lower than indoor unit.
+
+\paragraph{Field: Main Pipe Insulation Thickness}\label{field-main-pipe-insulation-thickness}
+
+This numeric field defines the insulation thickness of the main pipe. This value is used to calculate the heat loss of the refrigerant when going through the main pipe. The value should be greater than 0. If this field is blank, the default value of 0.02m is used.
+
+\paragraph{Field: Main Pipe Insulation Thermal Conductivity}\label{field-main-pipe-insulation-thermal-conductivity}
+
+This numeric field defines the thermal conductivity of the main pipe insulation material. This value is used to calculate the heat loss of the refrigerant when going through the main pipe. The value should be greater than 0. If this field is blank, the default value of 0.032 W/m-K is used.
+
+\paragraph{Field: Crankcase Heater Power per Compressor}\label{field-crankcase-heater-power-per-compressor-1}
+
+This numeric field defines the electrical power consumed by the crankcase heater in watts for each compressor. This crankcase heater power is consumed to warm the refrigerant and oil when the compressor is off when the outdoor temperature is below the maximum outdoor dry-bulb temperature for crankcase heater operation. The minimum value for this field is 0. If this field is left blank, the default value is 33 watts. Crankcase heater electrical consumption is applied only when the compressor is off or is applied during the off cycle when the compressor is cycling below the Minimum Heat Pump Part-Load Ratio. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Number of Compressors}\label{field-number-of-compressors-1}
+
+This numeric field defines the number of compressors in the heat pump condensing unit and is used exclusively to determine the operating characteristics of the crankcase heater. For example, if the number of compressors is 3, one crankcase heater will operate when the heat pump condensing unit's part-load ratio is less than or equal to 0.67 (when the ratio of compressor size to total compressor capacity input is 0.33) and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. Similarly, two crankcase heaters will operate when the heat pump condensing unit's PLR is less than or equal to 0.33 and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. If the heat pump condensing unit is off, all 3 crankcase heaters will operate if the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. The minimum value for this field is 1. If this field is left blank, the default value is 2. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Ratio of Compressor Size to Total Compressor Capacity}\label{field-ratio-of-compressor-size-to-total-compressor-capacity-1}
+
+This numeric field defines the size of the first stage compressor to the total compressor capacity and is used exclusively for calculating crankcase heater energy. If this field and the previous field are left blank, the default value is 0.5. If this field is left blank and the previous field is not blank, the compressors are assumed to be equally sized. When the number of compressors is greater than 2, the 2\(^{nd}\) stage compressor and all additional compressors are assumed to be equally sized. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Maximum Outdoor Dry-bulb Temperature for Crankcase Heater}\label{field-maximum-outdoor-dry-bulb-temperature-for-crankcase-heater-1}
+
+This numeric field defines the maximum outdoor temperature, in degrees Celsius, below which the crankcase heater will operate. If this field is left blank, the default value is 5°C. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
+
+\paragraph{Field: Defrost Strategy}\label{field-defrost-strategy-1-000}
+
+This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse-cycle. Defrost can be disabled by entering a resistive defrost strategy using a timed defrost control, a 0 defrost time period fraction and a 0 resistive defrost heater capacity in the following inputs fields. This method is used when the Maximum Outdoor Dry-Bulb Temperature for Defrost Operation field value is greater than the expected minimum outdoor dry-bulb temperature simulated in the weather file.
+
+\paragraph{Field: Defrost Control}\label{field-defrost-control-1-000}
+
+This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value of compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field ``Defrost Time Period Fraction'' described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field ``Maximum Outdoor Dry-bulb Temperature for Defrost Operation'' described above. If this input field is left blank, the default defrost control is timed.
+
+\paragraph{Field: Defrost Energy Input Ratio Modifier Function of Temperature Curve Name}\label{field-defrost-energy-input-ratio-modifier-function-of-temperature-curve-name-1}
+
+This alpha field defines the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) during reverse-cycle defrost periods as a function of the outdoor air dry-bulb temperature and the weighted average wet-bulb temperature of the air entering the indoor terminal units. The output of this curve is multiplied by the coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the indoor and outdoor coils are operating. The curve is normalized to a value of 1.0 at the rating point conditions.
+
+\paragraph{Field: Defrost Time Period Fraction}\label{field-defrost-time-period-fraction-1-000}
+
+This numeric field defines the fraction of compressor runtime when the defrost cycle is active. For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
+
+\paragraph{Field: Resistive Defrost Heater Capacity}\label{field-resistive-defrost-heater-capacity-1-000}
+
+This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is `resistive' (see input field ``Defrost Strategy'' above). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.
+
+\paragraph{Field: Maximum Outdoor Dry-bulb Temperature for Defrost Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-defrost-operation-1-000}
+
+This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. If this input field is left blank, the default value is 5°C. Defrost can be completely eliminated by selecting a temperature lower than the minimum expected outdoor temperature found in the weather file.
+
+\paragraph{Field: Compressor maximum delta Pressure}\label{field-compressor-maximum-delta-pressure}
+
+This numeric field defines the maximum pressure increase that the compressor can provide. The value should be greater than 0. If this field is blank, the default value of 4,500,000 Pa is used.
+
+\paragraph{Field: Number of Compressor Loading Index Entries}\label{field-number-of-compressor-loading-index-entries}
+
+This numeric field defines the number of compressor loading index entries. Loading index specifies the VRF operational modes at various load conditions. In a single compressor system, loading index reflects the compressor speed. The model requires at least two loading indices. The first index represents the minimal capacity operation, while the last index represents full capacity operation.
+
+\paragraph{Field: Compressor Speed at Loading Index i}\label{field-compressor-speed-at-loading-index-i}
+
+This numeric field defines the compressor speed at the i-th loading index. The value must be greater than 0.
+
+\paragraph{Field: Loading Index i Evaporative Capacity Multiplier Function of Temperature Curve Name}\label{field-loading-index-i-evaporative-capacity-multiplier-function-of-temperature-curve-name}
+
+This alpha field defines the name of a BiQuadratic curve for the VRF operational mode corresponding to the i-th loading index. It parameterizes the variation of VRF evaporating capacity as a function of operating conditions, i.e., evaporating and condensing temperatures. The output of this curve is a dimensionless multiplier to be applied on the rated evaporative capacity to calculate the actual capacity.
+
+\paragraph{Field: Loading Index i Compressor Power Multiplier Function of Temperature Curve Name}\label{field-loading-index-i-compressor-power-multiplier-function-of-temperature-curve-name}
+
+This alpha field defines the name of a BiQuadratic curve for the VRF operational mode corresponding to the i-th loading index. It parameterizes the variation of compressor power as a function of operating conditions, i.e., evaporating and condensing temperatures. The output of this curve is a dimensionless multiplier to be applied on the rated compressor power to calculate the actual compressor power.
+
+Following is an example input for a AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl system.
+
+\begin{lstlisting}
+
+AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl,
+  VRF Heat Pump,           !- Heat Pump Name
+  VRFCondAvailSched,       !- Availability Schedule Name
+  VRF Heat Pump TU List,   !- Zone Terminal Unit List Name
+  R410A,                   !- Refrigerant Type
+  41300,                   !- Rated Evaporative Capacity {W}
+  0.344,                   !- Rated Compressor Power Per Unit of Rated Evaporative Capacity {W/W}
+  ,                        !- Minimum Outdoor Air Temperature in Cooling Mode {C}
+  ,                        !- Maximum Outdoor Air Temperature in Cooling Mode {C}
+  ,                        !- Minimum Outdoor Air Temperature in Heating Mode {C}
+  ,                        !- Maximum Outdoor Air Temperature in Heating Mode {C}
+  3,                       !- Reference Outdoor Unit Superheating Degrees {C}
+  3,                       !- Reference Outdoor Unit Subcooling Degrees {C}
+  VariableTemp,            !- Refrigerant Temperature Control Algorithm for Indoor Unit
+  ,                        !- Reference Evaporating Temperature for Indoor Unit {C}
+  ,                        !- Reference Condensing Temperature for Indoor Unit {C}
+  6,                       !- Variable Evaporating Temperature Minimum for Indoor Unit {C}
+  13,                      !- Variable Evaporating Temperature Maximum for Indoor Unit {C}
+  42,                      !- Variable Condensing Temperature Minimum for Indoor Unit {C}
+  46,                      !- Variable Evaporating Temperature Maximum for Indoor Unit {C}
+  4.12E-3,                 !- Outdoor Unit Fan Power Per Unit of Rated Evaporative Capacity {W/W}
+  7.26E-5,                 !- Outdoor Unit Fan Flow Rate Per Unit of Rated Evaporative Capacity {m3/s-W}
+  OUEvapTempCurve,         !- Outdoor Unit Evaporating Temperature Function of Superheating Curve Name
+  OUCondTempCurve,         !- Outdoor Unit Condensing Temperature Function of Subcooling Curve Name
+  0.0508,                  !- Diameter of main pipe connecting outdoor unit to indoor units {m}
+  30,                      !- Length of main pipe connecting outdoor unit to indoor units {m}
+  36,                      !- Equivalent length of main pipe connecting outdoor unit to indoor units {m}
+  5,                       !- Height difference between the outdoor unit node and indoor unit node of the main pipe {m}
+  0.02,                    !- Insulation thickness of the main pipe {m}
+  0.032,                   !- Thermal conductivity of the main pipe insulation material {W/m-K}
+  33,                      !- Crankcase Heater Power per Compressor {W}
+  1,                       !- Number of Compressors
+  0.33,                    !- Ratio of Compressor Size to Total Compressor Capacity
+  7,                       !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater {C}
+  ,                        !- Defrost Strategy
+  ,                        !- Defrost Control
+  ,                        !- Defrost Energy Input Ratio Modifier Function of Temperature Curve Name
+  ,                        !- Defrost Time Period Fraction
+  ,                        !- Resistive Defrost Heater Capacity {W}
+  ,                        !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation {C}
+  4500000,                 !- Compressor maximum delta Pressure {Pa}
+  3,                       !- Number of Compressor Loading Index Entries
+  1500,                    !- Compressor Speed at Loading Index 1 {rev/min}
+  MinSpdCooling,           !- Loading Index 1 Evaporative Capacity Multiplier Function of Temperature Curve Name
+  MinSpdPower,             !- Loading Index 1 Compressor Power Multiplier Function of Temperature Curve Name
+  3600,                    !- Compressor Speed at Loading Index 2 {rev/min}
+  Spd1Cooling,             !- Loading Index 2 Evaporative Capacity Multiplier Function of Temperature Curve Name
+  Spd1Power,               !- Loading Index 2 Compressor Power Multiplier Function of Temperature Curve Name
+  6000,                    !- Compressor Speed at Loading Index 3 {rev/min}
+  Spd2Cooling,             !- Loading Index 3 Evaporative Capacity Multiplier Function of Temperature Curve Name
+  Spd2Power;               !- Loading Index 3 Compressor Power Multiplier Function of Temperature Curve Name
+
+  Curve:Quadratic,
+  OUEvapTempCurve,         !- Name
+  0,                       !- Coefficient1 Constant
+  6.05E-1,                 !- Coefficient2 x
+  2.50E-2,                 !- Coefficient3 x**2
+  0,                       !- Minimum Value of x
+  15,                      !- Maximum Value of x
+  ,                        !- Minimum Curve Output
+  ,                        !- Maximum Curve Output
+  Temperature,             !- Input Unit Type for X
+  Temperature;             !- Output Unit Type
+
+  Curve:Quadratic,
+  OUCondTempCurve,         !- Name
+  0,                       !- Coefficient1 Constant
+  -2.91,                   !- Coefficient2 x
+  1.180,                   !- Coefficient3 x**2
+  0,                       !- Minimum Value of x
+  20,                      !- Maximum Value of x
+  ,                        !- Minimum Curve Output
+  ,                        !- Maximum Curve Output
+  Temperature,             !- Input Unit Type for X
+  Temperature;             !- Output Unit Type
+
+  Curve:Biquadratic,
+  MinSpdCooling,           !- Name
+  3.19E-01,                !- Coefficient1 Constant
+  -1.26E-03,               !- Coefficient2 x
+  -2.15E-05,               !- Coefficient3 x**2
+  1.20E-02,                !- Coefficient4 y
+  1.05E-04,                !- Coefficient5 y**2
+  -8.66E-05,               !- Coefficient6 x*y
+  15,                      !- Minimum Value of x
+  65,                      !- Maximum Value of x
+  -30,                     !- Minimum Value of y
+  15,                      !- Maximum Value of y
+  ,                        !- Minimum Curve Output
+  ,                        !- Maximum Curve Output
+  Temperature,             !- Input Unit Type for X
+  Temperature,             !- Input Unit Type for Y
+  Dimensionless;           !- Output Unit Type
+
+  Curve:Biquadratic,
+  MinSpdPower,             !- Name
+  8.79E-02 ,               !- Coefficient1 Constant
+  -1.72E-04,               !- Coefficient2 x
+  6.93E-05 ,               !- Coefficient3 x**2
+  -3.38E-05,               !- Coefficient4 y
+  -8.10E-06,               !- Coefficient5 y**2
+  -1.04E-05,               !- Coefficient6 x*y
+  15,                      !- Minimum Value of x
+  65,                      !- Maximum Value of x
+  -30,                     !- Minimum Value of y
+  15,                      !- Maximum Value of y
+  ,                        !- Minimum Curve Output
+  ,                        !- Maximum Curve Output
+  Temperature,             !- Input Unit Type for X
+  Temperature,             !- Input Unit Type for Y
+  Dimensionless;           !- Output Unit Type
+
+  Curve:Biquadratic,
+  Spd1Cooling,             !- Name
+  8.12E-01 ,               !- Coefficient1 Constant
+  -4.23E-03,               !- Coefficient2 x
+  -4.11E-05,               !- Coefficient3 x**2
+  2.97E-02 ,               !- Coefficient4 y
+  2.67E-04 ,               !- Coefficient5 y**2
+  -2.23E-04,               !- Coefficient6 x*y
+  15,                      !- Minimum Value of x
+  65,                      !- Maximum Value of x
+  -30,                     !- Minimum Value of y
+  15,                      !- Maximum Value of y
+  ,                        !- Minimum Curve Output
+  ,                        !- Maximum Curve Output
+  Temperature,             !- Input Unit Type for X
+  Temperature,             !- Input Unit Type for Y
+  Dimensionless;           !- Output Unit Type
+
+  Curve:Biquadratic,
+  Spd1Power,               !- Name
+  3.26E-01 ,               !- Coefficient1 Constant
+  -2.20E-03,               !- Coefficient2 x
+  1.42E-04 ,               !- Coefficient3 x**2
+  2.82E-03 ,               !- Coefficient4 y
+  2.86E-05 ,               !- Coefficient5 y**2
+  -3.50E-05,               !- Coefficient6 x*y
+  15,                      !- Minimum Value of x
+  65,                      !- Maximum Value of x
+  -30,                     !- Minimum Value of y
+  15,                      !- Maximum Value of y
+  ,                        !- Minimum Curve Output
+  ,                        !- Maximum Curve Output
+  Temperature,             !- Input Unit Type for X
+  Temperature,             !- Input Unit Type for Y
+  Dimensionless;           !- Output Unit Type
+
+  Curve:Biquadratic,
+  Spd2Cooling,             !- Name
+  1.32E+00 ,               !- Coefficient1 Constant
+  -6.20E-03,               !- Coefficient2 x
+  -7.10E-05,               !- Coefficient3 x**2
+  4.89E-02 ,               !- Coefficient4 y
+  4.59E-04 ,               !- Coefficient5 y**2
+  -3.67E-04,               !- Coefficient6 x*y
+  15,                      !- Minimum Value of x
+  65,                      !- Maximum Value of x
+  -30,                     !- Minimum Value of y
+  15,                      !- Maximum Value of y
+  ,                        !- Minimum Curve Output
+  ,                        !- Maximum Curve Output
+  Temperature,             !- Input Unit Type for X
+  Temperature,             !- Input Unit Type for Y
+  Dimensionless;           !- Output Unit Type
+
+  Curve:Biquadratic,
+  Spd2Power,               !- Name
+  6.56E-01 ,               !- Coefficient1 Constant
+  -3.71E-03,               !- Coefficient2 x
+  2.07E-04 ,               !- Coefficient3 x**2
+  1.05E-02 ,               !- Coefficient4 y
+  7.36E-05 ,               !- Coefficient5 y**2
+  -1.57E-04,               !- Coefficient6 x*y
+  15,                      !- Minimum Value of x
+  65,                      !- Maximum Value of x
+  -30,                     !- Minimum Value of y
+  15,                      !- Maximum Value of y
+  ,                        !- Minimum Curve Output
+  ,                        !- Maximum Curve Output
+  Temperature,             !- Input Unit Type for X
+  Temperature,             !- Input Unit Type for Y
+  Dimensionless;           !- Output Unit Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-039}
+
+\begin{itemize}
+\item
+  HVAC,Average,VRF Heat Pump Total Cooling Rate {[}W{]}
+\item
+  HVAC,Average,VRF Heat Pump Total Heating Rate {[}W{]}
+\item
+  HVAC,Average,VRF Heat Pump Cooling COP {[]}
+\item
+  HVAC,Average,VRF Heat Pump Heating COP {[]}
+\item
+  HVAC,Average,VRF Heat Pump COP {[]}
+\item
+  HVAC,Average,VRF Heat Pump Part Load Ratio {[]}
+\item
+  HVAC,Average,VRF Heat Pump Runtime Fraction {[]}
+\item
+  HVAC,Average,VRF Heat Pump Cycling Ratio {[]}
+\item
+  HVAC,Average,VRF Heat Pump Operating Mode {[]}
+\item
+  HVAC,Average,VRF Heat Pump Condenser Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,VRF Heat Pump Maximum Capacity Cooling Rate {[}W{]}
+\item
+  HVAC,Average,VRF Heat Pump Maximum Capacity Heating Rate {[}W{]}
+\item
+  HVAC,Average,VRF Heat Pump Crankcase Heater Electric Power {[}W{]}
+\item
+  HVAC,Sum,VRF Heat Pump Crankcase Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average,VRF Heat Pump Terminal Unit Heating Load Rate {[}W{]}
+\item
+  HVAC,Average,VRF Heat Pump Terminal Unit Cooling Load Rate {[}W{]}
+\end{itemize}
+
+Heat Recovery:
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,VRF Heat Pump Heat Recovery Status Change Multiplier {[]}
+\end{itemize}
+
+Evap-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Sum,VRF Heat Pump Evaporative Condenser Water Use Volume {[}m3{]}
+\item
+  HVAC,Average,VRF Heat Pump Evaporative Condenser Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,VRF Heat Pump Evaporative Condenser Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,VRF Heat Pump Basin Heater Electric Power {[}W{]}
+\item
+  HVAC,Average,VRF Heat Pump Basin Heater Electric Energy {[}J{]}
+\item
+  HVAC,Average,VRF Heat Pump Heat Recovery Status Change Multiplier {[]}
+\end{itemize}
+
+Water-cooled:
+
+\begin{itemize}
+\item
+  HVAC,Average,VRF Heat Pump Condenser Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,VRF Heat Pump Condenser Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum,VRF Heat Pump Condenser Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average, VRF Heat Pump Condenser Heat Transfer Rate {[}W{]}
+\end{itemize}
+
+Electric Fuel type (default):
+
+\begin{itemize}
+\item
+  HVAC,Average,VRF Heat Pump Cooling Electric Power {[}W{]}
+\item
+  HVAC,Sum,VRF Heat Pump Cooling Electric Energy {[}J{]}
+\item
+  HVAC,Average,VRF Heat Pump Heating Electric Power {[}W{]}
+\item
+  HVAC,Sum,VRF Heat Pump Heating Electric Energy {[}J{]}
+\end{itemize}
+
+Electric defrost always used for Defrost Strategy = Resistive regardless of fuel type
+
+\begin{itemize}
+\item
+  HVAC,Average,VRF Heat Pump Defrost Electric Power {[}W{]}
+\item
+  HVAC,Sum,VRF Heat Pump Defrost Electric Energy {[}J{]}
+\end{itemize}
+
+Alternate Fuel types (e.g., FuelType = NaturalGas):
+
+\begin{itemize}
+\item
+  HVAC,Average,VRF Heat Pump Cooling \textless{}FuelType\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,VRF Heat Pump Cooling \textless{}FuelType\textgreater{} Energy {[}J{]}
+\item
+  HVAC,Average,VRF Heat Pump Heating \textless{}FuelType\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,VRF Heat Pump Heating \textless{}FuelType\textgreater{} Energy {[}J{]}
+\item
+  HVAC,Average,VRF Heat Pump Defrost \textless{}FuelType\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,VRF Heat Pump Defrost \textless{}FuelType\textgreater{} Energy {[}J{]}
+\end{itemize}
+
+For the pysics based VRF model (VRF-FluidTCtrl) only:
+
+\begin{itemize}
+\item
+  VRF Heat Pump Indoor Unit Evaporating Temperature at Cooling Mode {[}C{]}
+\item
+  VRF Heat Pump Outdoor Unit Condensing Temperature at Cooling Mode {[}C{]}
+\item
+  VRF Heat Pump Indoor Unit Condensing Temperature at Heating Mode {[}C{]}
+\item
+  VRF Heat Pump Outdoor Unit Evaporating Temperature at Heating Mode {[}C{]}
+\item
+  VRF Heat Pump Compressor Electric Power at Cooling Mode {[}W{]}
+\item
+  VRF Heat Pump Compressor Electric Power at Heating Mode {[}W{]}
+\item
+  VRF Heat Pump Compressor Rotating Speed {[}rev/min{]}
+\item
+  VRF Heat Pump Outdoor Unit Fan Power {[}W{]}
+\end{itemize}
+
+Note: refer to the rdd file after a simulation for exact output variable names
+
+\paragraph{VRF Heat Pump Total Cooling Rate ~{[}W{]}}\label{vrf-heat-pump-total-cooling-rate-w}
+
+This output field is the operating total cooling capacity of the variable refrigerant flow heat pump in Watts. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. This value should match the sum of the individual zone terminal unit output variables for Zone VRF Air Terminal Total Cooling Rate.
+
+\paragraph{VRF Heat Pump Total Heating Rate {[}W{]}}\label{vrf-heat-pump-total-heating-rate-w}
+
+This output field is the operating total heating capacity of the variable refrigerant flow heat pump in Watts. The capacity includes any degradation due to defrost mode. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. This value should match the sum of the individual zone terminal unit output variables for Zone VRF Air Terminal Total Heating Rate.
+
+\paragraph{VRF Heat Pump Cooling Electric Power {[}W{]}}\label{vrf-heat-pump-cooling-electric-power-w}
+
+This output field is the cooling mode electricity consumption rate of the variable refrigerant flow heat pump in Watts. The consumption includes electricity used by the compressor and the condenser fan. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump Cooling NaturalGas Consumption Rate).
+
+\paragraph{VRF Heat Pump Cooling Electric Energy {[}J{]}}\label{vrf-heat-pump-cooling-electric-energy-j}
+
+This output field is the cooling mode electricity consumption of the variable refrigerant flow heat pump in Joules for the time period being reported. The consumption includes electricity used by the compressor and the condenser fan. This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (Ref. Output:Meter objects). The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump Cooling NaturalGas Consumption). The resource type meter will also be modified to reflect the chosen fuel type (e.g., Resource Type = NaturalGas).
+
+\paragraph{VRF Heat Pump Heating Electric Power {[}W{]}}\label{vrf-heat-pump-heating-electric-power-w}
+
+This output field is the heating mode electricity consumption rate of the variable refrigerant flow heat pump in Watts. The consumption includes electricity used by the compressor (including crankcase heater), additional energy required for defrost, and the condenser fan. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump Heating NaturalGas Consumption Rate).
+
+\paragraph{VRF Heat Pump Heating Electric Energy {[}J{]}}\label{vrf-heat-pump-heating-electric-energy-j}
+
+This output field is the heating mode electricity consumption of the variable refrigerant flow heat pump in Joules for the time period being reported. The consumption includes electricity used by the compressor (including crankcase heater), additional energy required for defrost, and the condenser fan. This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (Ref. Output:Meter objects). The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump Heating NaturalGas Consumption). The resource type meter will also be modified to reflect the chosen fuel type (e.g., Resource Type = NaturalGas).
+
+\paragraph{\texorpdfstring{VRF Heat Pump Cooling COP{[]}}{VRF Heat Pump Cooling COP}}\label{vrf-heat-pump-cooling-cop}
+
+This is the operating cooling coefficient of performance for the heat pump. This value is calculated using the ratio of VRF Heat Pump Total Cooling Rate and Variable Refrigerant Flow Heat Pump Cooling Electric Consumption Rate output variables. Crankcase heater (usually 0 in cooling mode), evaporative condenser water pump, and defrost (usually 0 in cooling mode) consumption rate output variables are included in this calculation. This value is specific to outdoor unit performance in cooling mode, is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{\texorpdfstring{VRF Heat Pump Heating COP{[]}}{VRF Heat Pump Heating COP}}\label{vrf-heat-pump-heating-cop}
+
+This is the operating heating coefficient of performance for the heat pump. This value is calculated using the ratio of VRF Heat Pump Total Heating Rate and Variable Refrigerant Flow Heat Pump Heating Electric Consumption Rate output variables. Crankcase heater, evaporative condenser water pump (usually 0 in heating mode), and defrost consumption rate output variables are included in this calculation. This value is specific to outdoor unit performance in heating mode, is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{\texorpdfstring{VRF Heat Pump COP{[]}}{VRF Heat Pump COP}}\label{vrf-heat-pump-cop}
+
+This is the operating coefficient of performance for the heat pump. This value is calculated using the ratio of the total terminal unit coil capacity (cooling plus heating and accounts for piping losses) and total system electric consumption rate (compressor, crankcase heater, evaporative condenser water pump, defrost, and terminal unit parasitic electric consumption rate). This output variable does not include pump power for a water-cooled system. This value is specific to overall system performance, is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{VRF Heat Pump Defrost Electric Power {[}W{]}}\label{vrf-heat-pump-defrost-electric-power-w}
+
+This is the electricity consumption rate of the heat pump defrost in Watts when the unit is in defrost mode (timed, reverse-cycle). . The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump NaturalGas Defrost Consumption Rate).
+
+\paragraph{VRF Heat Pump Defrost Electric Energy {[}J{]}}\label{vrf-heat-pump-defrost-electric-energy-j}
+
+This is the electricity consumption of the heat pump in Joules for the time step being reported. This consumption is applicable when the unit is in defrost mode (reverse-cycle or resistive). This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (Ref. Output:Meter objects). The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump NaturalGas Defrost Consumption). The resource type meter will also be modified to reflect the chosen fuel type (e.g., Resource Type = NaturalGas).
+
+\paragraph{VRF Heat Pump Part Load Ratio}\label{vrf-heat-pump-part-load-ratio}
+
+This output field is the part-load ratio of the heat pump condenser. Heat pump part-load ratio is defined as the total coil load divided by the heat pump's maximum available capacity at the current operating conditions. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{\texorpdfstring{VRF Heat Pump Runtime Fraction {[]}}{VRF Heat Pump Runtime Fraction }}\label{vrf-heat-pump-runtime-fraction}
+
+This output field is the runtime fraction of the heat pump condenser's first stage compressor. Heat pump runtime fraction is defined as the fraction of time the first stage compressor is on during a given time period and includes cycling losses. This value is calculated as the ratio of the VRF Heat Pump Cycling Ratio and the output of the Cooling Part-Load Fraction Correlation Curve object as the specific cycling ratio. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{\texorpdfstring{VRF Heat Pump Cycling Ratio {[]}}{VRF Heat Pump Cycling Ratio }}\label{vrf-heat-pump-cycling-ratio}
+
+This output field is the cycling ratio of the heat pump condenser's first stage compressor. Heat pump cycling ratio is defined as the fraction of time the first stage compressor is on during a given time period. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{\texorpdfstring{VRF Heat Pump Operating Mode {[]}}{VRF Heat Pump Operating Mode }}\label{vrf-heat-pump-operating-mode}
+
+This output field is an integer representation of the operating mode of the variable refrigerant flow heat pump. The operating mode for cooling mode is indicated by a 1 and heating mode is indicated by a 2. A value of 0 is reported if the heat pump is off. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{VRF Heat Pump Condenser Inlet Temperature {[}C{]}}\label{vrf-heat-pump-condenser-inlet-temperature-c}
+
+This is the inlet air temperature entering the condenser coil in degrees C. This value can represent the outdoor air dry-bulb temperature, wet-bulb temperature, or somewhere in between from the weather data being used, depending on the value used in the input field ``Evaporative Condenser Effectiveness''. The temperature reported here is used in the various modifier curves related to temperature (e.g., Total Cooling Capacity Modifier Curve {[}function of temperature{]}). (The use of the word \emph{Condenser} here is taken from cooling operation -- the same device can also be an evaporator during heating operation.)
+
+\paragraph{VRF Heat Pump Condenser Outlet Temperature {[}C{]}}\label{vrf-heat-pump-condenser-outlet-temperature-c}
+
+This is the condenser coil outlet water temperature in degrees C. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. This value is only reported for water-cooled systems.~ (The use of the word \emph{Condenser} here is taken from cooling operation -- the same device can also be an evaporator during heating operation.)
+
+\paragraph{VRF Heat Pump Condenser Mass Flow Rate {[}kg/s{]}}\label{vrf-heat-pump-condenser-mass-flow-rate-kgs}
+
+This is the condenser coil outlet water mass flow rate in kilograms per second. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. This value is only reported for water-cooled systems. (The use of the word \emph{Condenser} here is taken from cooling operation -- the same device can also be an evaporator during heating operation.)
+
+\paragraph{VRF Heat Pump Condenser Heat Transfer Rate {[}W{]}}\label{vrf-heat-pump-condenser-heat-transfer-rate-w}
+
+This is the condenser coil heat transfer rate in Watts. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. This value is only reported for water-cooled systems. (The use of the word \emph{Condenser} here is taken from cooling operation -- the same device can also be an evaporator during heating operation.)
+
+\paragraph{VRF Heat Pump Condenser Heat Transfer Energy {[}J{]}}\label{vrf-heat-pump-condenser-heat-transfer-energy-j}
+
+This is the condenser coil heat transfer in Joules. This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported. This value is only reported for water-cooled systems. (The use of the word \emph{Condenser} here is taken from cooling operation -- the same device can also be an evaporator during heating operation.)
+
+\paragraph{VRF Heat Pump Maximum Capacity Cooling Rate {[}W{]}}\label{vrf-heat-pump-maximum-capacity-cooling-rate-w}
+
+This output field is the maximum available terminal unit cooling capacity in Watts allowed for the current time step being reported. If the terminal units request more capacity than is actually available from the variable refrigerant flow heat pump, the individual terminal units will be limited to this value. A maximum limit of 1E+20 is reported when there is sufficient capacity available to meet all requests from the terminal units. This output variable easily identifies times when the total terminal unit cooling load exceeds the heat pump's available cooling capacity.
+
+\paragraph{VRF Heat Pump Maximum Capacity Heating Rate {[}W{]}}\label{vrf-heat-pump-maximum-capacity-heating-rate-w}
+
+This output field is the maximum available terminal unit heating capacity in Watts allowed for the current time step being reported. If the terminal units request more capacity than is actually available from the variable refrigerant flow heat pump, the individual terminal units will be limited to this value. A maximum limit of 1E+20 is reported when there is sufficient capacity available to meet all requests from the terminal units. This output variable easily identifies times when the total terminal unit heating load exceeds the heat pump's available heating capacity.
+
+\paragraph{VRF Heat Pump Terminal Unit Cooling Load Rate {[}W{]}}\label{vrf-heat-pump-terminal-unit-cooling-load-rate-w}
+
+This output field is the sum of the terminal unit cooling coil loads in Watts for the current time step being reported. This value is derived directly from the cooling coils and represents the total cooling load on the VRF system after piping losses have been accounted for. The total cooling load will be less than the variable refrigerant flow total cooling capacity reported when piping losses are modeled (i.e., when piping losses are \textless{} 1).
+
+\paragraph{VRF Heat Pump Terminal Unit Heating Load Rate {[}W{]}}\label{vrf-heat-pump-terminal-unit-heating-load-rate-w}
+
+This output field is the sum of the terminal unit heating coil loads in Watts for the current time step being reported. This value is derived directly from the heating coils and represents the total heating load on the VRF system after piping losses have been accounted for. The total heating load will be less than the variable refrigerant flow total heating capacity reported when piping losses are modeled (i.e., when piping losses are \textless{} 1).
+
+\paragraph{VRF Heat Pump Crankcase Heater Electric Power {[}W{]}}\label{vrf-heat-pump-crankcase-heater-electric-power-w}
+
+This output field is the average electricity consumption rate of the heat pump's crankcase heaters in Watts for the time step being reported.
+
+\paragraph{VRF Heat Pump Crankcase Heater Electric Energy {[}J{]}}\label{vrf-heat-pump-crankcase-heater-electric-energy-j}
+
+This output field is the electricity consumption rate of the heat pump's crankcase heaters in Joules for the time step being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{VRF Heat Pump Evaporative Condenser Water Use Volume {[}m3{]}}\label{vrf-heat-pump-evaporative-condenser-water-use-volume-m3}
+
+This output is the amount of water used to evaporatively cool the condenser coil inlet air, in cubic meters. This output is also added to a meter with Resource Type = Water, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{VRF Heat Pump Evaporative Condenser Pump Electric Power {[}W{]}}\label{vrf-heat-pump-evaporative-condenser-pump-electric-power-w}
+
+This is the average electricity consumption rate of the evaporative condenser water pump in Watts for the time step being reported.
+
+\paragraph{VRF Heat Pump Evaporative Condenser Pump Electric Energy {[}J{]}}\label{vrf-heat-pump-evaporative-condenser-pump-electric-energy-j}
+
+This is the electricity consumption rate of the evaporative condenser water pump in Joules for the time step being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{VRF Heat Pump Basin Heater Electric Power {[}W{]}}\label{vrf-heat-pump-basin-heater-electric-power-w}
+
+This output is the electric consumption rate of the heat pump's basin heater (for evaporatively-cooled condenser type) in Watts. This basin heater only operates when the variable refrigerant flow heat pump's compressor(s) is off and therefore is reported as 0 anytime the compressor operates. If the compressor is cycling (see VRF Heat Pump Cycling Ratio output variable above), the basin heater electric power is proportional to one minus the cycling ratio of the compressor (i.e., the basin heater is on when the compressor is off).
+
+\paragraph{VRF Heat Pump Basin Heater Electric Energy {[}J{]}}\label{vrf-heat-pump-basin-heater-electric-energy-j}
+
+This output is the electric consumption of the heat pump's basin heater (for evaporatively-cooled condenser type) in Joules. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (Ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{VRF Heat Pump Heat Recovery Status Change Multiplier {[]}}{VRF Heat Pump Heat Recovery Status Change Multiplier }}\label{vrf-heat-pump-heat-recovery-status-change-multiplier}
+
+This output applies only when heat recovery is used and represents the multiplier used to derate the capacity of the system when transitioning from cooling or heating mode to heat recovery mode. This value is 1 when derating does not apply (i.e., the system has not recently changed modes to provide heat recovery). Derating during a transition period is applied according to the inputs for Heat Recovery Fraction and Heat Recovery Time Constant. To turn transition derating off, set Heat Recovery Fraction to 1. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
+
+\paragraph{VRF Heat Pump Indoor Unit Evaporating Temperature at Cooling Mode {[}C{]}}\label{vrf-heat-pump-indoor-unit-evaporating-temperature-at-cooling-mode-c}
+
+This output only applies for the VRF-FluidTCtrl model. This is the evaporating temperature of the VRF system operating at cooling mode. This value is manipulated by the VRF system considering the load conditions of all the zones it serves. It affects the indoor unit cooling coil surface temperature and thus the cooling capacity of the indoor unit. It also affects the compressor operating conditions and thus the compressor energy consumption.
+
+\paragraph{VRF Heat Pump Outdoor Unit Condensing Temperature at Cooling Mode {[}C{]}}\label{vrf-heat-pump-outdoor-unit-condensing-temperature-at-cooling-mode-c}
+
+This output only applies for the VRF-FluidTCtrl model. This is the condensing temperature of the VRF system operating at cooling mode. This value is related with the outdoor air conditions as well as the system operational mode. It affects the condensing capacity of the outdoor unit. It also affects the compressor operating conditions and thus the compressor energy consumption.
+
+\paragraph{VRF Heat Pump Indoor Unit Condensing Temperature at Heating Mode {[}C{]}}\label{vrf-heat-pump-indoor-unit-condensing-temperature-at-heating-mode-c}
+
+This output only applies for the VRF-FluidTCtrl model. This is the condensing temperature of the VRF system operating at heating mode. This value is manipulated by the VRF system considering the load conditions of all the zones it serves. It affects the indoor unit heating coil surface temperature and thus the heating capacity of the indoor unit. It also affects the compressor operating conditions and thus the compressor energy consumption.
+
+\paragraph{VRF Heat Pump Outdoor Unit Evaporating Temperature at Heating Mode {[}C{]}}\label{vrf-heat-pump-outdoor-unit-evaporating-temperature-at-heating-mode-c}
+
+This output only applies for the VRF-FluidTCtrl model. This is the evaporating temperature of the VRF system operating at heating mode. This value is related with the outdoor air conditions as well as the system operational mode. It affects the evaporating capacity of the outdoor unit. It also affects the compressor operating conditions and thus the compressor energy consumption.
+
+\paragraph{VRF Heat Pump Compressor Electric Power at Cooling Mode {[}W{]}}\label{vrf-heat-pump-compressor-electric-power-at-cooling-mode-w}
+
+This output only applies for the VRF-FluidTCtrl model. This is the electric power of the compressor running at the cooling mode. This value is related with the compressor speed as well as the operational conditions, i.e., evaporating and condensing temperatures of the system.
+
+\paragraph{VRF Heat Pump Compressor Electric Power at Heating Mode {[}W{]}}\label{vrf-heat-pump-compressor-electric-power-at-heating-mode-w}
+
+This output only applies for the VRF-FluidTCtrl model. This is the electric power of the compressor running at the heating mode. This value is related with the compressor speed as well as the operational conditions, i.e., evaporating and condensing temperatures of the system.
+
+\paragraph{VRF Heat Pump Compressor Rotating Speed {[}rev/min{]}}\label{vrf-heat-pump-compressor-rotating-speed-revmin}
+
+This output only applies for the VRF-FluidTCtrl model. This is the rotating speed of the compressor, which indicates the loading index.
+
+\paragraph{VRF Heat Pump Outdoor Unit Fan Power {[}W{]}}\label{vrf-heat-pump-outdoor-unit-fan-power-w}
+
+This output only applies for the VRF-FluidTCtrl model. This is the power consumed by the fan located in the VRF outdoor unit.
+
+\subsection{ZoneTerminalUnitList}\label{zoneterminalunitlist}
+
+The zone terminal unit list defines the names of the terminal units connected to a single variable refrigerant flow air-conditioning system. The zone terminal unit list is used exclusively in the variable refrigerant flow (VRF) air conditioner object (ref: AirConditioner:VariableRefrigerantFlow). Up to 20 terminal units may be connected to a single VRF outdoor condensing unit. This list is extensible if additional indoor terminal units are required. The name of this zone terminal unit list object is then input into the corresponding variable refrigerant flow air conditioner object. The following figure demonstrates this concept.
+
+\begin{figure}[hbtp] % fig 127
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image313.png}
+\caption{Zone Terminal Unit List Diagram \protect \label{fig:zone-terminal-unit-list-diagram}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-2-044}
+
+\paragraph{Field: Zone Terminal List Name}\label{field-zone-terminal-list-name}
+
+This alpha field specifies the name of the zone terminal unit list. This name must be specified in the AirConditioner:VariableRefrigerantFlow object.
+
+\paragraph{Field: Zone Terminal Unit Name \textless{}x\textgreater{}}\label{field-zone-terminal-unit-name-x}
+
+This alpha field defines the name of the zone terminal unit used in a variable refrigerant air conditioner. The zone terminal unit must be connected to a zone using the ZoneHVAC:EquipmentConnections object. The terminal unit air inlet node is the same name as a zone exhaust node. The terminal unit air outlet node is the same name as a zone inlet node. The IDD is supplied with 20 fields for this.~ The object is extensible and you can change the IDD by adding more fields or, if you are using text editor for your input file, just add to the list of names.
+
+Following is an example input for a ZoneTerminalUnitList object.
+
+\begin{lstlisting}
+
+ZoneTerminalUnitList,
+     VRF Heat Pump TU List, !- Zone Terminal Unit List Name
+     TU3,                   !- Zone Terminal Unit Name 1
+     TU4,                   !- Zone Terminal Unit Name 2
+     TU1,                   !- Zone Terminal Unit Name 3
+     TU2,                   !- Zone Terminal Unit Name 4
+     TU5;                   !- Zone Terminal Unit Name 5
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-water-heaters.tex b/doc/input-output-reference/src/overview/group-water-heaters.tex
new file mode 100644
index 00000000000..c130d47d0ef
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-water-heaters.tex
@@ -0,0 +1,1864 @@
+\section{Group -- Water Heaters}\label{group-water-heaters}
+
+Water heater objects are components for storing and heating water. They can be coupled to a plant loop simulation or used stand-alone. Typical water heater applications are for domestic hot water heating, low-temperature radiant space heating, and energy storage for solar hot water systems or waste heat recovery.
+
+When coupled to the plant loop, the water heater has an inlet node and outlet node on the ``source side'' and an inlet node and outlet node on the ``use side''. The source side typically draws cold water from the tank and returns warmer water, for instance, from solar hot water systems or waste heat recovery systems. The use side typically draws hot water from the tank and returns cooler water from the cold water supply mains or from the outlet of a heating system. The distinction between source and use sides is merely a convenience for reporting. They can actually be used interchangeably. If so desired, either source side or use side can be used by itself, without the other side being connected to the plant loop.
+
+However, for a water heater that is indirectly heated (e.g.~with a separate boiler), the source side can be used to provide remotely heated water to the tank.~ The source side is configured to operate as a component on the demand side of a plant loop.~ The design flow rate through the source side can be set by the user or autosized.~ If autosized, then a Plant Sizing object is needed elsewhere in the input file for the Plant Loop serving the source side.~ The water heater input includes an additional design parameter that describes how rapidly the tank can recover.
+
+\begin{figure}[hbtp] % fig 80
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image191.png}
+\caption{Water Heater Configuration \protect \label{fig:water-heater-configuration}}
+\end{figure}
+
+If the use side only consists of domestic hot water usage, a simple scheduled use flow rate can be specified in lieu of the full plant loop connections. The scheduled use flow rate can be used simultaneously with source side plant connections, but cannot be used with use side plant connections.
+
+For stand-alone operation, there are no node connections to the plant loop on either source or use sides. The scheduled use flow rate determines all fluid exchange with the water tank.
+
+There are currently two water heater objects in EnergyPlus:
+
+\begin{itemize}
+\item
+  WaterHeater:Mixed
+\item
+  WaterHeater:Stratified
+\end{itemize}
+
+There are also compound objects that uses the WaterHeater:Mixed and/or WaterHeater:Stratified as part of their strategy:
+
+\begin{itemize}
+\tightlist
+\item
+  WaterHeater:HeatPump:PumpedCondenser (WaterHeater:Mixed or WaterHeater:Stratified)
+\item
+  WaterHeater:HeatPump:WrappedCondenser (WaterHeater:Stratified only)
+\end{itemize}
+
+The WaterHeater:Mixed object simulates a well-mixed, single-node water tank. The WaterHeater:Stratified object simulates a stratified, multi-node water tank. Both water heater objects can be appropriate for simulating many types of water heaters and storage tanks, including gas and electric residential water heaters, and a variety of large commercial water heaters. Both objects share similar features, such as stand-alone operation, on- and off-cycle parasitic loads, and thermal losses to the zone. However, each object has its advantages which may make one water heater object more appropriate than the other depending on the application.
+
+Advantages of \textbf{WaterHeater:Mixed}:
+
+\begin{itemize}
+\item
+  can simulate instantaneous/tankless water heaters
+\item
+  requires less input than the stratified tank
+\item
+  faster execution time than the stratified tank
+\item
+  adequate for modeling gas water heaters with no source connections.
+\end{itemize}
+
+Advantages of \textbf{WaterHeater:Stratified}:
+
+\begin{itemize}
+\item
+  better modeling of electric water heaters with two heating elements
+\item
+  better modeling of thermal storage applications which rely on stratification to improve heat transfer peformance.
+\end{itemize}
+
+\subsection{Standard Ratings}\label{standard-ratings}
+
+The EIO file reports the industry standard ratings of Recovery Efficiency and Energy Factor for water heater objects. The rating method is based on the GAMA and 10CFR430 test procedures. Under certain input parameters, the rating method will not succeed and a warning message will be generated. Problems occur when inputs do not allow the tank to recover to the setpoint temperature within the test period. This can occur if the maximum heater capacity is undersized, or if the deadband temperature difference is large enough that the first draw of the test does not trigger the heater to come on. In either case, the Recovery Efficiency test will not compute properly because recovery to the setpoint was not achieved.
+
+Standard ratings for storage-only water tanks (Heater Maximum Capacity = 0) cannot be calculated and do not report anything in the EIO file.
+
+\subsection{WaterHeater:Mixed}\label{waterheatermixed}
+
+The WaterHeater:Mixed object analytically solves the differential equation governing the energy balance of the water tank. Within a timestep, conditions are solved separately for when the heater element or burner is ``on'' (on-cycle) and when it is ``off'' (off-cycle). This approach allows ambient losses and parasitic loads to be divided into on-cycle and off-cycle effects and accounted for in detail.
+
+For losses to the ambient environment, the ambient air temperature can be taken from a schedule, a zone, or the exterior. When used with a zone, a fraction of the skin losses can be added to the zone heat balance as internal heat gains.
+
+Control options allow the heater to cycle or modulate to meet the load. When cycling, the heater element or burner is either on or off. The heater remains fully on while heating the tank up to the setpoint temperature. When the setpoint is reached, the heater turns off. The heater remains off until the tank temperature falls below the ``cut-in'' temperature, i.e., the setpoint temperature minus the deadband temperature difference. The heater continuously cycles on and off to maintain the tank temperature within the deadband. Most storage-tank water heaters cycle.
+
+When modulating, the heater power varies between the maximum and minimum heater capacities. The heater stays on as long as the required total demand is above the minimum capacity. Below the minimum capacity, the heater will begin to cycle on and off based on the deadband temperature difference. Equipment is usually designed and rated to avoid this condition. Most tankless/instantaneous water heaters modulate.
+
+\subsubsection{Inputs}\label{inputs-052}
+
+\paragraph{Field: Name}\label{field-name-050}
+
+The name of the WaterHeater:Mixed object.
+
+\paragraph{Field: Tank Volume}\label{field-tank-volume-000}
+
+The volume of the storage tank {[}m\(^{3}\){]}.~ This field is autosizable if used with a Water Heater:Sizing object.~ Although this field is allowed to go down to zero, even so-called ``tankless'' water heaters have some volume of water that is maintained around the heating elements or in the heat exchanger, typically around 0.00379 m\(^{3}\) (1 gallon).
+
+\paragraph{Field: Setpoint Temperature Schedule Name}\label{field-setpoint-temperature-schedule-name-001}
+
+The reference to the schedule object specifying the hot water temperature setpoint {[}°C{]}. Also known as the ``cut-out'' temperature.
+
+\paragraph{Field: Deadband Temperature Difference}\label{field-deadband-temperature-difference-000}
+
+The delta temperature difference {[}Δ°C{]} between the setpoint and the ``cut-in'' temperature at which the heater will turn on. In other words, the ``cut-in'' temperature is Setpoint -- Deadband.
+
+\paragraph{Field: Maximum Temperature Limit}\label{field-maximum-temperature-limit}
+
+The temperature {[}°C{]} at which the tank water becomes dangerously hot and is vented through boiling or an automatic safety. The tank temperature will never exceed the maximum. Any extra heat added to the tank is immediately vented. Note:~ The maximum temperature must be greater than the setpoint temperature at all times.
+
+\paragraph{Field: Heater Control Type}\label{field-heater-control-type}
+
+The control type can be \textbf{Cycle} or \textbf{Modulate}. Cycle is appropriate for most storage tank-type water heaters. Modulate is appropriate for most instantaneous/tankless water heaters.
+
+\paragraph{Field: Heater Maximum Capacity}\label{field-heater-maximum-capacity}
+
+The maximum heat rate {[}W{]} that can be supplied to the water, probably the same as the ``nominal'' capacity.~ This field is autosizable if used with a Water Heater:Sizing object.
+
+\paragraph{Field: Heater Minimum Capacity}\label{field-heater-minimum-capacity}
+
+The minimum heat rate {[}W{]} that can be supplied to the water. This field is only used when the Heater Control Type is \textbf{Modulate}. If the total demand rate for heating is less than the minimum, even a modulating water heater will begin to cycle.
+
+\paragraph{Field: Heater Ignition Minimum Flow Rate}\label{field-heater-ignition-minimum-flow-rate}
+
+NOT YET IMPLEMENTED.
+
+\paragraph{Field: Heater Ignition Delay}\label{field-heater-ignition-delay}
+
+NOT YET IMPLEMENTED.
+
+\paragraph{Field: Heater Fuel Type}\label{field-heater-fuel-type}
+
+The type of fuel used for heating. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating.
+
+\paragraph{Field: Heater Thermal Efficiency}\label{field-heater-thermal-efficiency}
+
+The thermal conversion efficiency from fuel energy to heat energy for the heater element or burner. This is not the same as the overall efficiency of the water heater.
+
+\paragraph{Field: Part Load Factor Curve Name}\label{field-part-load-factor-curve-name}
+
+The reference to the curve object that relates the overall efficiency of the water heater to the Runtime Fraction (if Control Type \textbf{Cycle}) or Part Load Ratio (if Control Type \textbf{Modulate}). This is an additional multiplier applied to the Heater Thermal Efficiency to compute fuel energy use. The Part Load Factor Curve should not have a value less than 0.1 in the domain from 0 to 1. If the Part Load Factor Curve accounts for ambient losses and/or parasitic fuel consumption, these effects should not also be input into the related fields in this object as that would result in double-counting.
+
+\paragraph{Field: Off-Cycle Parasitic Fuel Consumption Rate}\label{field-off-cycle-parasitic-fuel-consumption-rate}
+
+Off-cycle parasitics include parts of the water heater that consume fuel when the heater is off, for example, a pilot light, or stand-by electronic control circuits. The fuel consumption rate {[}W{]} is strictly the total fuel that is consumed by all of the off-cycle parasitics.
+
+\paragraph{Field: Off-Cycle Parasitic Fuel Type}\label{field-off-cycle-parasitic-fuel-type}
+
+The type of fuel used by the off-cycle parasitics. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating. The fuel type can be the same or different from the Heater Fuel Type.
+
+\paragraph{Field: Off-Cycle Parasitic Heat Fraction to Tank}\label{field-off-cycle-parasitic-heat-fraction-to-tank}
+
+The fraction of off-cycle parasitic fuel energy that is converted to heat energy that ends up in the tank water. For example, a pilot light would deliver most of its heat to the tank water, as long as the thermal conversion efficiency must be taken into account, so perhaps 0.80 is reasonable. Electronic control circuits, on the other hand, do not add any heat to the tank and should be 0.
+
+\paragraph{Field: On-Cycle Parasitic Fuel Consumption Rate}\label{field-on-cycle-parasitic-fuel-consumption-rate}
+
+On-cycle parasitics include parts of the water heater that consume fuel when the heater is on, for example, an induction fan, or stand-by electronic control circuits. The fuel consumption rate {[}W{]} is strictly the total fuel that is consumed by all of the on-cycle parasitics.
+
+\paragraph{Field: On-Cycle Parasitic Fuel Type}\label{field-on-cycle-parasitic-fuel-type}
+
+The type of fuel used by the on-cycle parasitics. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating. The fuel type can be the same or different from the Heater Fuel Type.
+
+\paragraph{Field: On-Cycle Parasitic Heat Fraction to Tank}\label{field-on-cycle-parasitic-heat-fraction-to-tank}
+
+The fraction of on-cycle parasitic fuel energy that is converted to heat energy that ends up in the tank water. For example, an induction fan might (maybe) deliver a small fraction of its energy to the tank water for a value of 0.05. Electronic control circuits, on the other hand, do not add any heat to the tank and should be 0.
+
+\paragraph{Field: Ambient Temperature Indicator}\label{field-ambient-temperature-indicator-000}
+
+The Ambient Temperature Indicator specifies how the ambient air temperature will be indicated. The field can be \textbf{Schedule}, \textbf{Zone}, or \textbf{Outdoors}. If \textbf{Schedule} is used, the Ambient Temperature Schedule field provides the ambient temperature. If \textbf{Zone} is used, the zone air temperature of the zone specified in the Ambient Temperature Zone field provides the ambient temperature. If \textbf{Outdoors} is used, the outdoor dry-bulb air temperature provides the ambient temperature.
+
+\paragraph{Field: Ambient Temperature Schedule Name}\label{field-ambient-temperature-schedule-name-001}
+
+The reference to the schedule object specifying the ambient air temperature around the tank for skin losses. This field is only used if Ambient Temperature Indicator is \textbf{Schedule}.
+
+\paragraph{Field: Ambient Temperature Zone Name}\label{field-ambient-temperature-zone-name-001}
+
+The reference to the zone object specifying the ambient air temperature around the tank for skin losses. This field is only used if Ambient Temperature Indicator is \textbf{Zone}.
+
+\paragraph{Field: Ambient Temperature Outdoor Air Node Name}\label{field-ambient-temperature-outdoor-air-node-name-000}
+
+This optional alpha field specifies the outdoor air node name used to define the ambient conditions surrounding the water heater tank. This field is applicable only when the Ambient Temperature Indicator is specified as \textbf{Outdoors}, otherwise this field should be left blank. The node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
+
+\paragraph{Field: Off-Cycle Loss Coefficient to Ambient Temperature}\label{field-off-cycle-loss-coefficient-to-ambient-temperature}
+
+The loss coefficient {[}W/K{]} to the ambient air temperature. Often this coefficient is identical to the ``UA'' for skin losses. However, it can also be used to model the loss effects of the flue in a combustion water heater, in addition to the skin losses.
+
+\paragraph{Field: Off-Cycle Loss Fraction to Zone}\label{field-off-cycle-loss-fraction-to-zone}
+
+If the Ambient Temperature Indicator is \textbf{Zone}, this field adds the specified fraction of the off-cycle losses to the zone heat balance as an internal gain.
+
+\paragraph{Field: On-Cycle Loss Coefficient to Ambient Temperature}\label{field-on-cycle-loss-coefficient-to-ambient-temperature}
+
+The loss coefficient {[}W/K{]} to the ambient air temperature. Often this coefficient is identical to the ``UA'' for skin losses. If the loss effects of the flue are being modeled in the Off-Cycle Loss Coefficient, than this field would have a different value accounting only for the skin losses.
+
+\paragraph{Field: On-Cycle Loss Fraction to Zone}\label{field-on-cycle-loss-fraction-to-zone}
+
+If the Ambient Temperature Indicator is \textbf{Zone}, this field adds the specified fraction of the on-cycle losses to the zone heat balance as an internal gain.
+
+\paragraph{Field: Peak Use Flow Rate}\label{field-peak-use-flow-rate}
+
+The peak flow rate {[}m\(^{3}\)/s{]} of domestic hot water usage for stand-alone operation, i.e., without plant loop node connections. The peak value is multiplied by the Use Flow Rate Fraction Schedule. If there are node connections, this field is not used.
+
+\paragraph{Field: Use Flow Rate Fraction Schedule Name}\label{field-use-flow-rate-fraction-schedule-name}
+
+The reference to the schedule object specifiying the current fraction of Peak Volumetric Use Flow Rate of domestic hot water usage for stand-alone operation.
+
+\paragraph{Field: Cold Water Supply Temperature Schedule Name}\label{field-cold-water-supply-temperature-schedule-name}
+
+The reference to the schedule object specifying the cold water temperature {[}°C{]} from the supply mains that makes up for the hot water lost down the drain. If blank, water temperatures are calculated by the Site:WaterMainsTemperature object. This field is for stand-alone operation only. If there are node connections, this field is not used.
+
+\paragraph{Field: Use Side Inlet Node Name}\label{field-use-side-inlet-node-name-000}
+
+The inlet node connection to the plant loop for the use side of the water heater. Typically the use side draws hot water from the tank and returns cooler water.
+
+\paragraph{Field: Use Side Outlet Node Name}\label{field-use-side-outlet-node-name-000}
+
+The outlet node connection to the plant loop for the use side of the water heater. Typically the use side draws hot water from the tank and returns cooler water.
+
+\paragraph{Field: Use Side Effectiveness}\label{field-use-side-effectiveness}
+
+This field specifies the heat transfer effectiveness between the use side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the use side water and the tank water. If the effectiveness is lower, then the use side outlet water temperature will not be as hot as the tank water, simulating a heat exchanger.
+
+\paragraph{Field: Source Side Inlet Node Name}\label{field-source-side-inlet-node-name-000}
+
+The inlet node connection to the plant loop for the source side of the water heater. Typically the source side draws cold water from the tank and returns warmer water.~ The source side volume flow rate is obtained from the plant loop.~ The magnitude of the flow rates through the source side can be controlled by setting the Maximum Branch Flow Rate field in the \textbf{Branch} object that connects the source inlet node.
+
+\paragraph{Field: Source Side Outlet Node Name}\label{field-source-side-outlet-node-name-000}
+
+The outlet node connection to the plant loop for the source side of the water heater. Typically the source side draws cold water from the tank and returns warmer water.
+
+\paragraph{Field: Source Side Effectiveness}\label{field-source-side-effectiveness}
+
+This field specifies the heat transfer effectiveness between the source side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the source side water and the tank water. If the effectiveness is lower, then the source side outlet water temperature will not be as hot as the tank water, simulating a heat exchanger.
+
+\paragraph{Field: Use Side Design Flow Rate}\label{field-use-side-design-flow-rate-000}
+
+This field is optional and is used to specify the design flow rate through the Use Side of the water heater.~ The volumetric design flow rate is specified in m\(^{3}\)/s.~ The field is needed when the Use Side is connected to a plant loop.~ The field can be autosized.~ If autosized, then the input file should include a Plant Sizing object for the plant loop.~ Sizing results are reported in the EIO file.
+
+\paragraph{Field: Source Side Design Flow Rate}\label{field-source-side-design-flow-rate-000}
+
+This field is optional and is used to specify the design flow rate through the Source Side of the water heater.~ The volumetric design flow rate is specified in m\(^{3}\)/s.~ The field is needed when the Source Side is connected to a plant loop.~ The field can be autosized.~ If autosized, then the input file should include a Plant Sizing object for the plant loop.~ Sizing results are reported in the EIO file.
+
+\paragraph{Field: Indirect Water Heating Recovery Time}\label{field-indirect-water-heating-recovery-time}
+
+This field is optional and is used to provide a design parameter for autosizing design flow rates when the water heater is connected to the demand side of a plant loop.~ The recovery time is expressed in hours.~ This is the time that the entire volume of the tank can be heated from 14.4ºC to 57.2ºC (58ºF to 135ºF) with an inlet temperature defined as the exit temperature in the associated Plant Sizing object.~ The default is 1.5 hours.~ The calculation is based on log-mean temperature difference (LMTD) and includes the heat transfer effectiveness factor entered above.
+
+\paragraph{Field: Source Side Flow Control Mode}\label{field-source-side-flow-control-mode}
+
+This field is optional and is used to provide control over the logic used by the source side of the water heater to request flow. There are three choices for different modes: IndirectHeatPrimarySetpoint, IndirectHeatAlternateSetpoint, or StorageTank.~~~ The mode called IndirectHeatPrimarySetpoint is the historical behavior prior to version 8.1.~ In this mode the water heater will request flow at the source side when the main setpoint, in the input field called Setpoint Temperature Schedule Name, and deadband call for the tank to be heated.~ This mode is typical for a water heater indirectly heated by a boiler.~ The mode called IndirectHeatAlternateSetpoint is similar but it bases its control decisions on an alternate setpoint given in the following field.~ This mode is useful when the indirect source of heat may not satisfy the load and an internal heater is used for backup.~ The mode called StorageTank is for a passive tank and it always requests flow unless the tank temperature is equal to or higher than the maximum limit given in the input field called Maximum Temperature Limit.
+
+\paragraph{Field: Indirect Alternate Setpoint Temperature Schedule Name}\label{field-indirect-alternate-setpoint-temperature-schedule-name}
+
+This field is optional and is used to provide a schedule with alternate setpoints for use with the IndirectHeatAlternateSetpoint mode in the previous field.~ The input field should contain a reference to a schedule object specifying the hot water temperature setpoint {[}°C{]} to use as the ``cut-out'' temperature for control logic at the source side.
+
+\begin{lstlisting}
+
+WaterHeater:Mixed,                     ! Stand-alone electric, outdoor example
+      Outdoor Electric Tank,  !- Name
+      0.151,  !- Tank Volume {m3}
+      Hot Water Setpoint Temp Schedule,  !- Setpoint Temperature Schedule
+      2.0,  !- Deadband Temperature Difference {deltaC}
+      82.2222,  !- Maximum Temperature Limit {C}
+      Cycle,  !- Heater Control Type {Cycle | Modulate}
+      11712,  !- Heater Maximum Capacity {W}
+      ,  !- Heater Minimum Capacity {W}
+      ,  !- Heater Ignition Minimum Flow Rate {m3/s}
+      ,  !- Heater Ignition Delay {s}
+      ELECTRICITY,  !- Heater Fuel Type
+      0.95,  !- Heater Thermal Efficiency
+      ,  !- Part Load Factor Curve
+      15,  !- Off-Cycle Parasitic Fuel Consumption Rate {W}
+      ELECTRICITY,  !- Off-Cycle Parasitic Fuel Type
+      0,  !- Off-Cycle Parasitic Heat Fraction To Tank
+      15,  !- On-Cycle Parasitic Fuel Consumption Rate {W}
+      ELECTRICITY,  !- On-Cycle Parasitic Fuel Type
+      0,  !- On-Cycle Parasitic Heat Fraction To Tank
+      Outdoors,  !- Ambient Temperature Indicator {Schedule | Zone | Outdoors}
+      ,  !- Ambient Temperature Schedule
+      ,  !- Ambient Temperature Zone
+      2.36,  !- Off-Cycle Loss Coefficient To Ambient Temperature {W/K}
+      ,  !- Off-Cycle Loss Fraction To Zone
+      2.36,  !- On-Cycle Loss Coefficient To Ambient Temperature {W/K}
+      ,  !- On-Cycle Loss Fraction To Zone
+      0.000379,  !- Peak Volumetric Use Flow Rate {m3/s}
+      Hot Water Demand Schedule,  !- Use Flow Rate Fraction Schedule
+      Constant Mains Temp Schedule;  !- Cold Water Supply Temperature Schedule
+
+
+
+
+  WaterHeater:Mixed,                     ! Stand-alone electric, tankless example
+      Tankless,  !- Name
+      0.003785,  !- Tank Volume {m3}
+      Hot Water Setpoint Temp Schedule,  !- Setpoint Temperature Schedule
+      ,  !- Deadband Temperature Difference {deltaC}
+      82.2222,  !- Maximum Temperature Limit {C}
+      Modulate,  !- Heater Control Type {Cycle | Modulate}
+      11712,  !- Heater Maximum Capacity {W}
+      0,  !- Heater Minimum Capacity {W}
+      ,  !- Heater Ignition Minimum Flow Rate {m3/s}
+      ,  !- Heater Ignition Delay {s}
+      ELECTRICITY,  !- Heater Fuel Type
+      0.95,  !- Heater Thermal Efficiency
+      ,  !- Part Load Factor Curve
+      10,  !- Off-Cycle Parasitic Fuel Consumption Rate {W}
+      ELECTRICITY,  !- Off-Cycle Parasitic Fuel Type
+      0,  !- Off-Cycle Parasitic Heat Fraction To Tank
+      30,  !- On-Cycle Parasitic Fuel Consumption Rate {W}
+      ELECTRICITY,  !- On-Cycle Parasitic Fuel Type
+      0,  !- On-Cycle Parasitic Heat Fraction To Tank
+      Schedule,  !- Ambient Temperature Indicator {Schedule | Zone | Outdoors}
+      Hot Water Ambient Temp Schedule,  !- Ambient Temperature Schedule
+      ,  !- Ambient Temperature Zone
+      ,  !- Off-Cycle Loss Coefficient To Ambient Temperature {W/K}
+      ,  !- Off-Cycle Loss Fraction To Zone
+      ,  !- On-Cycle Loss Coefficient To Ambient Temperature {W/K}
+      ,  !- On-Cycle Loss Fraction To Zone
+      0.000379,  !- Peak Volumetric Use Flow Rate {m3/s}
+      Hot Water Demand Schedule,  !- Use Flow Rate Fraction Schedule
+      ;  !- Cold Water Supply Temperature Schedule
+
+
+    WaterHeater:Mixed,                     ! Plant loop connected, gas example
+      Water Heater,  !- Name
+      0.454,  !- Tank Volume {m3}
+      Hot Water Setpoint Temp Schedule,  !- Setpoint Temperature Schedule
+      5.0,  !- Deadband Temperature Difference {deltaC}
+      82.2222,  !- Maximum Temperature Limit {C}
+      Cycle,  !- Heater Control Type {Cycle | Modulate}
+      2000,  !- Heater Maximum Capacity {W}
+      ,  !- Heater Minimum Capacity {W}
+      ,  !- Heater Ignition Minimum Flow Rate {m3/s}
+      ,  !- Heater Ignition Delay {s}
+      NATURALGAS,  !- Heater Fuel Type
+      0.80,  !- Heater Thermal Efficiency
+      ,  !- Part Load Factor Curve
+      ,  !- Off-Cycle Parasitic Fuel Consumption Rate {W}
+      ,  !- Off-Cycle Parasitic Fuel Type
+      ,  !- Off-Cycle Parasitic Heat Fraction To Tank
+      ,  !- On-Cycle Parasitic Fuel Consumption Rate {W}
+      ,  !- On-Cycle Parasitic Fuel Type
+      ,  !- On-Cycle Parasitic Heat Fraction To Tank
+      Schedule,  !- Ambient Temperature Indicator {Schedule | Zone | Outdoors}
+      Hot Water Ambient Temp Schedule,  !- Ambient Temperature Schedule
+      ,  !- Ambient Temperature Zone
+      5.0,  !- Off-Cycle Loss Coefficient To Ambient Temperature {W/K}
+      ,  !- Off-Cycle Loss Fraction To Zone
+      5.0,  !- On-Cycle Loss Coefficient To Ambient Temperature {W/K}
+      ,  !- On-Cycle Loss Fraction To Zone
+      ,  !- Peak Volumetric Use Flow Rate {m3/s}
+      ,  !- Use Flow Rate Fraction Schedule
+      ,  !- Cold Water Supply Temperature Schedule
+      Water Heater Use Inlet Node,  !- Use Side Inlet Node
+      Water Heater Use Outlet Node,  !- Use Side Outlet Node
+      1.0,  !- Use Side Effectiveness
+      Water Heater Source Inlet Node,  !- Source Side Inlet Node
+      Water Heater Source Outlet Node,  !- Source Side Outlet Node
+      1.0;  !- Source Side Effectiveness
+
+
+  WaterHeater:Mixed,
+      Indirect Water Heater,   !- Name
+      1.00,                    !- Tank Volume {m3}
+      Hot Water Setpoint Temperature Schedule,  !- Setpoint Temperature Schedule
+      5.0,                     !- Deadband Temperature Difference {deltaC}
+      82.2222,                 !- Maximum Temperature Limit {C}
+      Cycle,                   !- Heater Control Type
+      0.0,                     !- Heater Maximum Capacity {W}
+      ,                        !- Heater Minimum Capacity {W}
+      ,                        !- Heater Ignition Minimum Flow Rate {m3/s}
+      ,                        !- Heater Ignition Delay {s}
+      ELECTRICITY,             !- Heater Fuel Type
+      0.8,                     !- Heater Thermal Efficiency
+      ,                        !- Part Load Factor Curve
+      ,                        !- Off-Cycle Parasitic Fuel Consumption Rate {W}
+      ,                        !- Off-Cycle Parasitic Fuel Type
+      ,                        !- Off-Cycle Parasitic Heat Fraction To Tank
+      ,                        !- On-Cycle Parasitic Fuel Consumption Rate {W}
+      ,                        !- On-Cycle Parasitic Fuel Type
+      ,                        !- On-Cycle Parasitic Heat Fraction To Tank
+      Zone,                    !- Ambient Temperature Indicator
+      ,                        !- Ambient Temperature Schedule
+      SPACE5-1,                !- Ambient Temperature Zone
+      ,                        !- Ambient Temperature Outside Air Node
+      5.0,                     !- Off-Cycle Loss Coefficient To Ambient Temperature {W/K}
+      ,                        !- Off-Cycle Loss Fraction To Zone
+      5.0,                     !- On-Cycle Loss Coefficient To Ambient Temperature {W/K}
+      ,                        !- On-Cycle Loss Fraction To Zone
+      ,                        !- Peak Volumetric Use Flow Rate {m3/s}
+      ,                        !- Use Flow Rate Fraction Schedule
+      ,                        !- Cold Water Supply Temperature Schedule
+      SHWSys1 Pump-SHWSys1 Water HeaterNode,  !- Use Side Inlet Node
+      SHWSys1 Supply Equipment Outlet Node,  !- Use Side Outlet Node
+      1.0,                     !- Use Side Effectiveness
+      Indirect Water Heater SrcSideInletNode,  !- Source Side Inlet Node
+      Indirect Water Heater SrcSideOutletNode,  !- Source Side Outlet Node
+      0.9,                     !- Source Side Effectiveness
+      autosize,                !- Use Side Design Flow Rate
+      autosize,                !- Source Side Design Flow Rate
+      1.0;                     !- Indirect Water Heating Recovery Time
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-040}
+
+The following output variables are reported for the WaterHeater:Mixed object:
+
+\begin{itemize}
+\item
+  HVAC,Average,Water Heater Tank Temperature {[}C{]}
+\item
+  HVAC,Average,Water Heater Final Tank Temperature {[}C{]}
+\item
+  HVAC,Average,Water Heater Heat Loss Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Heat Loss Energy {[}J{]}
+\item
+  HVAC,Average, Water Heater Use Side Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water Heater Use Side Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Water Heater Use Side Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Water Heater Use Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Use Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Source Side Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water Heater Source Side Inlet Temperature {[}C{]}
+\item
+  HVAC,Average,Water Heater Source Side Outlet Temperature {[}C{]}
+\item
+  HVAC,Average,Water Heater Source Side Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Source Side Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Off Cycle Parasitic Tank Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Off Cycle Parasitic Tank Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater On Cycle Parasitic Tank Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater On Cycle Parasitic Tank Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Total Demand Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Total Demand Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Heating Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Unmet Demand Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Unmet Demand Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Venting Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Venting Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Net Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Net Heat Transfer Energy {[}J{]}
+\item
+  HVAC,Sum,Water Heater Cycle On Count {[]}
+\item
+  HVAC,Average,Water Heater Runtime Fraction {[]}
+\item
+  HVAC,Average,Water Heater Part Load Ratio {[]}
+\item
+  HVAC,Average,Water Heater Electric Power {[}W{]}
+\item
+  HVAC,Average,Water Heater \textless{}Fuel Type\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater \textless{}Fuel Type\textgreater{} Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Off Cycle Parasitic \textless{}Fuel Type\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Off Cycle Parasitic \textless{}Fuel Type\textgreater{} Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater On Cycle Parasitic \textless{}Fuel Type\textgreater{} Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater On Cycle Parasitic \textless{}Fuel Type\textgreater{} Energy {[}J{]}
+\item
+  HVAC,Average,Water Heater Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Water Heater Water Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Water Heater Tank Temperature {[}C{]}}\label{water-heater-tank-temperature-c}
+
+The average water tank temperature.
+
+\paragraph{Water Heater Final Tank Temperature {[}C{]}}\label{water-heater-final-tank-temperature-c}
+
+The final water tank temperature at the end of the system timestep. If reported at the ``Detailed'' interval, this output variable can be used to verify an exact energy balance on the water heater. Also see the output variable:~ Water Heater Net Heat Transfer Energy.
+
+\paragraph{Water Heater Heat Loss Rate {[}W{]}}\label{water-heater-heat-loss-rate-w}
+
+The average heat loss rate due to the off- and on-cycle loss coefficients to the ambient temperature.
+
+\paragraph{Water Heater Heat Loss Energy {[}J{]}}\label{water-heater-heat-loss-energy-j}
+
+The heat loss energy due to the off- and on-cycle loss coefficients to the ambient temperature.
+
+\paragraph{Water Heater Use Side Mass Flow Rate {[}kg/s{]}}\label{water-heater-use-side-mass-flow-rate-kgs}
+
+The use side mass flow rate. If stand-alone, this is the scheduled use flow rate.
+
+\paragraph{Water Heater Use Side Inlet Temperature {[}C{]}}\label{water-heater-use-side-inlet-temperature-c}
+
+The inlet temperature on the use side.
+
+\paragraph{Water Heater Use Side Outlet Temperature {[}C{]}}\label{water-heater-use-side-outlet-temperature-c}
+
+The outlet temperature on the use side.
+
+\paragraph{Water Heater Use Side Heat Transfer Rate {[}W{]}}\label{water-heater-use-side-heat-transfer-rate-w}
+
+The average heat transfer rate between the use side water and the tank water.
+
+\paragraph{Water Heater Use Side Heat Transfer Energy {[}J{]}}\label{water-heater-use-side-heat-transfer-energy-j}
+
+The heat transfer energy between the use side water and the tank water.
+
+\paragraph{Water Heater Source Side Mass Flow Rate {[}kg/s{]}}\label{water-heater-source-side-mass-flow-rate-kgs}
+
+The source side mass flow rate. If in stand-alone operation, this is 0.
+
+\paragraph{Water Heater Source Side Inlet Temperature {[}C{]}}\label{water-heater-source-side-inlet-temperature-c}
+
+The inlet temperature on the source side.
+
+\paragraph{Water Heater Source Side Outlet Temperature {[}C{]}}\label{water-heater-source-side-outlet-temperature-c}
+
+The outlet temperature on the source side.
+
+\paragraph{Water Heater Source Side Heat Transfer Rate {[}W{]}}\label{water-heater-source-side-heat-transfer-rate-w}
+
+The average heat transfer rate between the source side water and the tank water.
+
+\paragraph{Water Heater Source Side Heat Transfer Energy {[}J{]}}\label{water-heater-source-side-heat-transfer-energy-j}
+
+The heat transfer energy between the source side water and the tank water.
+
+\paragraph{Water Heater Off Cycle Parasitic Tank Heat Transfer Rate {[}W{]}}\label{water-heater-off-cycle-parasitic-tank-heat-transfer-rate-w}
+
+The average heat gain rate to the tank water due to off-cycle parasitics.
+
+\paragraph{Water Heater Off Cycle Parasitic Tank Heat Transfer Energy {[}J{]}}\label{water-heater-off-cycle-parasitic-tank-heat-transfer-energy-j}
+
+The heat gain energy to the tank water due to off-cycle parasitics.
+
+\paragraph{Water Heater On Cycle Parasitic Tank Heat Transfer Rate {[}W{]}}\label{water-heater-on-cycle-parasitic-tank-heat-transfer-rate-w}
+
+The average heat gain rate to the tank water due to on-cycle parasitics.
+
+\paragraph{Water Heater On Cycle Parasitic Tank Heat Transfer Energy {[}J{]}}\label{water-heater-on-cycle-parasitic-tank-heat-transfer-energy-j}
+
+The heat gain energy to the tank water due to on-cycle parasitics.
+
+\paragraph{Water Heater Total Demand Heat Transfer Rate {[}W{]}}\label{water-heater-total-demand-heat-transfer-rate-w}
+
+The average heating rate demanded to maintain the setpoint temperature.
+
+\paragraph{Water Heater Total Demand Energy {[}J{]}}\label{water-heater-total-demand-energy-j}
+
+The heating energy demanded to maintain the setpoint temperature.
+
+\paragraph{Water Heater Heating Rate {[}W{]}}\label{water-heater-heating-rate-w-000}
+
+The average heating rate supplied by the heater element or burner.
+
+\paragraph{Water Heater Heating Energy {[}J{]}}\label{water-heater-heating-energy-j-000}
+
+The heating energy supplied by the heater element or burner.
+
+\paragraph{Water Heater Unmet Demand Heat Transfer Rate {[}W{]}}\label{water-heater-unmet-demand-heat-transfer-rate-w}
+
+The average heating rate unmet by the heater element or burner. The difference between the Total Demand Rate and the Heating Rate.
+
+\paragraph{Water Heater Unmet Demand Heat Transfer Energy {[}J{]}}\label{water-heater-unmet-demand-heat-transfer-energy-j}
+
+The heating energy unmet by the heater element or burner. The difference between the Total Demand Energy and the Heating Energy.
+
+\paragraph{Water Heater Venting Heat Transfer Rate {[}W{]}}\label{water-heater-venting-heat-transfer-rate-w}
+
+The average venting rate to keep the tank below the Maximum Temperature Limit.
+
+\paragraph{Water Heater Venting Heat Transfer Energy {[}J{]}}\label{water-heater-venting-heat-transfer-energy-j}
+
+The venting energy to keep the tank below the Maximum Temperature Limit.
+
+\paragraph{Water Heater Net Heat Transfer Rate {[}W{]}}\label{water-heater-net-heat-transfer-rate-w}
+
+The average net heat transfer rate when considering all losses and gains.
+
+\paragraph{Water Heater Net Heat Transfer Energy {[}J{]}}\label{water-heater-net-heat-transfer-energy-j}
+
+The net heat transfer energy when considering all losses and gains.
+
+\paragraph{\texorpdfstring{Water Heater Cycle On Count {[]}}{Water Heater Cycle On Count }}\label{water-heater-cycle-on-count}
+
+The number of times that the heater turned on in the time period.
+
+\paragraph{\texorpdfstring{Water Heater Runtime Fraction {[]}}{Water Heater Runtime Fraction }}\label{water-heater-runtime-fraction}
+
+The fraction of the time period that the heater was running.
+
+\paragraph{\texorpdfstring{Water Heater Part Load Ratio {[]}}{Water Heater Part Load Ratio }}\label{water-heater-part-load-ratio}
+
+The fraction of the Heater Maximum Capacity.
+
+\paragraph{Water Heater \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{water-heater-fuel-type-rate-w}
+
+\paragraph{Water Heater Electric Power {[}W{]}}\label{water-heater-electric-power-w}
+
+The average fuel consumption rate for the heater element or burner.
+
+\paragraph{Water Heater \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{water-heater-fuel-type-energy-j}
+
+The fuel consumption energy for the heater element or burner.
+
+\paragraph{Water Heater Off Cycle Parasitic \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{water-heater-off-cycle-parasitic-fuel-type-rate-w}
+
+\paragraph{Water Heater Off Cycle Parasitic Electric Power {[}W{]}}\label{water-heater-off-cycle-parasitic-electric-power-w-000}
+
+The average fuel consumption rate for the off-cycle parasitics.
+
+\paragraph{Water Heater Off Cycle Parasitic \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{water-heater-off-cycle-parasitic-fuel-type-energy-j}
+
+The fuel consumption energy for the off-cycle parasitics.
+
+\paragraph{Water Heater On Cycle Parasitic \textless{}Fuel Type\textgreater{} Rate {[}W{]}}\label{water-heater-on-cycle-parasitic-fuel-type-rate-w}
+
+\paragraph{Water Heater On Cycle Parasitic Electric Power {[}W{]}}\label{water-heater-on-cycle-parasitic-electric-power-w-000}
+
+The average fuel consumption rate for the on-cycle parasitics.
+
+\paragraph{Water Heater On Cycle Parasitic \textless{}Fuel Type\textgreater{} Energy {[}J{]}}\label{water-heater-on-cycle-parasitic-fuel-type-energy-j}
+
+The fuel consumption energy for the on-cycle parasitics.
+
+\paragraph{\texorpdfstring{Water Heater Water Volume Flow Rate {[}m\(^{3}\)/s{]}}{Water Heater Water Volume Flow Rate {[}m\^{}\{3\}/s{]}}}\label{water-heater-water-volume-flow-rate-m3s}
+
+The water consumption rate for the use side, if in stand-alone operation.
+
+\paragraph{\texorpdfstring{Water Heater Water Volume {[}m\(^{3}\){]}}{Water Heater Water Volume {[}m\^{}\{3\}{]}}}\label{water-heater-water-volume-m3}
+
+The water consumption for the use side, if in stand-alone operation.
+
+\paragraph{Water Heater Mains Water Volume {[}m3{]}}\label{water-heater-mains-water-volume-m3}
+
+The volume of water consumption drawn from mains water service.
+
+\subsection{WaterHeater:Stratified}\label{waterheaterstratified}
+
+The WaterHeater:Stratified object divides the water tank into multiple nodes of equal volume. The nodes are coupled by vertical conduction effects, internode fluid flow, and temperature inversion mixing. The object simultaneously solves the differential equations governing the energy balances on the nodes using a numerical method. The system timestep is divided into many small substeps that allow the simulation to capture events that occur on a very short time scale. This approach allows ambient losses and parasitic loads to be divided into on-cycle and off-cycle effects and accounted for in detail.
+
+For losses to the ambient environment, the ambient air temperature can be taken from a schedule, a zone, or the exterior. When used with a zone, a fraction of the skin losses can be added to the zone heat balance as internal heat gains.
+
+The WaterHeater:Stratified object allows two heating elements to be simulated. The two elements can cycle on and off to maintain the node temperature within the deadband. The Heater Priority Control field determines how the heaters work together. There are two options:~ MasterSlave or Simultaneous. In the MasterSlave option, Heater 1 is the master and Heater 2 is the slave. That is, both heaters are not allowed to turn on at the same time. If the thermostats ask for heat at both Heater 1 and 2, only Heater 1 will turn on. Once Heater 1 has met the set point, it turns off and Heater 2 can turn on, if necessary. In the Simultaneousoption, Heater 1 and Heater 2 can turn on and off independently.~ Autosizing is available for only Heater 1.
+
+\subsubsection{Inputs}\label{inputs-1-049}
+
+\paragraph{Field: Name}\label{field-name-1-047}
+
+The name of the WaterHeater:Stratified object.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-004}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Laundry'', ``Dish Washing'', etc. A new meter for reporting is created for each unique subcategory~ (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table under the ``Water Systems'' end-use category. If this field is omitted or blank, the water use will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Tank Volume}\label{field-tank-volume-1-000}
+
+The actual volume {[}m3{]} of fluid in the tank. This field is autosizable if used with a Water Heater:Sizing object.~ The actual volume is typically not equal to the nominal volume specified by the manufacturer. Actual volume is almost always 10\% lower for electric water heaters, and 5\% lower for gas water heaters (Burch and Erickson 2004).
+
+Burch, J., and P. Erickson. 2004. ``Using Ratings Data to Derive Simulation-Model Inputs for Storage-Tank Water Heaters''. \emph{Proceedings of the Solar 2004 Conference, 11-14 July 2004, Portland, Oregon}, American Solar Energy Society (ASES), pp.~393-398.
+
+\paragraph{Field: Tank Height}\label{field-tank-height-000}
+
+The height {[}m{]} of the tank. For the \textbf{HorizontalCylinder} shape (see below) the height of the tank is the measure in the axial direction, i.e., the height if you were to stand the cylinder up on its end. This field is autosizable if used with a Water Heater:Sizing object.
+
+\paragraph{Field: Tank Shape}\label{field-tank-shape-000}
+
+The tank shape determines the size and skin losses of the stratified nodes. There are three options:~ \textbf{VerticalCylinder}, \textbf{HorizontalCylinder}, and \textbf{Other}.
+
+\textbf{VerticalCylinder} describes most upright residential water heaters.
+
+HorizontalCylinder describes a few specialty water heaters and large commercial storage tanks. HorizontalCylinder can also be used to model an outdoor storage tank located above a solar collector in a thermosiphon configuration. HorizontalCylinder implies that the tank is divided into nodes of equal mass, but not equal height.
+
+Other describes water heaters or storage tanks that have a uniform horizontal cross-section, but are not cylinders, e.g., a cuboid or other shape. The length of the perimeter is then specified by the Tank Perimeter field.
+
+If blank, the default shape is \textbf{VerticalCylinder}.
+
+\paragraph{Field: Tank Perimeter}\label{field-tank-perimeter-000}
+
+The length of the tank perimeter {[}m{]}. This field is only used if Tank Shape is \textbf{Other}.
+
+\paragraph{Field: Maximum Temperature Limit}\label{field-maximum-temperature-limit-1}
+
+The temperature {[}°C{]} at which the tank water becomes dangerously hot and is vented through boiling or an automatic safety. The tank temperature will never exceed the maximum. Any extra heat added to the tank is immediately vented. Note:~ The maximum temperature must be greater than the setpoint temperature at all times.
+
+\paragraph{Field: Heater Priority Control}\label{field-heater-priority-control}
+
+The heater priority control determines how Heater 1 and Heater 2 work together. There are two options:~ \textbf{MasterSlave} or \textbf{Simultaneous}. In the MasterSlave option, Heater 1 is the master and Heater 2 is the slave. In most residential electric water heaters, the heaters operate in a MasterSlave relationship. That is, both heaters are not allowed to turn on at the same time. If the thermostats ask for heat at both Heater 1 and 2, only Heater 1 will turn on. Once Heater 1 has met the set point, it turns off and Heater 2 can turn on, if necessary. In other words, only one heater can be on at any time, and Heater 1 is always has priority over Heater 2.
+
+In the Simultaneous option, Heater 1 and Heater 2 can turn on and off independently.
+
+If blank, the default is \textbf{MasterSlave}.
+
+\paragraph{Field: Heater 1 Set Point Temperature Schedule Name}\label{field-heater-1-set-point-temperature-schedule-name}
+
+The reference to the schedule object specifying the hot water temperature set point {[}°C{]} for Heater 1. Also known as the ``cut-out'' temperature.
+
+\paragraph{Field: Heater 1 Deadband Temperature Difference}\label{field-heater-1-deadband-temperature-difference}
+
+The delta temperature difference {[}Δ°C{]} between the set point and the ``cut-in'' temperature at which Heater 1 will turn on. In other words, the ``cut-in'' temperature is Set Point -- Deadband.
+
+\paragraph{Field: Heater 1 Capacity}\label{field-heater-1-capacity}
+
+The heat rate {[}W{]} supplied to the water for Heater 1, probably the same as the ``nominal'' capacity. For residential electric water heaters, heating elements are usually 4500 W.~ This field is autosizable if used with a Water Heater:Sizing object.
+
+\paragraph{Field: Heater 1 Height}\label{field-heater-1-height}
+
+The height {[}m{]} of Heater 1 in the tank.
+
+\paragraph{Field: Heater 2 Set Point Temperature Schedule Name}\label{field-heater-2-set-point-temperature-schedule-name}
+
+The reference to the schedule object specifying the hot water temperature set point {[}°C{]} for Heater 2. Also known as the ``cut-out'' temperature.
+
+\paragraph{Field: Heater 2 Deadband Temperature Difference}\label{field-heater-2-deadband-temperature-difference}
+
+The delta temperature difference {[}Δ°C{]} between the set point and the ``cut-in'' temperature at which Heater 2 will turn on. In other words, the ``cut-in'' temperature is Set Point -- Deadband.
+
+\paragraph{Field: Heater 2 Capacity}\label{field-heater-2-capacity}
+
+The heat rate {[}W{]} supplied to the water for Heater 1, probably the same as the ``nominal'' capacity. For residential electric water heaters, heating elements are usually 4500 W.
+
+\paragraph{Field: Heater 2 Height}\label{field-heater-2-height}
+
+The height {[}m{]} of Heater 2 in the tank.
+
+\paragraph{Field: Heater Fuel Type}\label{field-heater-fuel-type-1}
+
+The type of fuel used for both Heaters 1 and 2. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating.
+
+\paragraph{Field: Heater Thermal Efficiency}\label{field-heater-thermal-efficiency-1}
+
+The thermal conversion efficiency from fuel energy to heat energy for the heater element or burner (for both Heaters 1 and 2). This is not the same as the overall efficiency of the water heater.
+
+\paragraph{Field: Off-Cycle Parasitic Fuel Consumption Rate}\label{field-off-cycle-parasitic-fuel-consumption-rate-1}
+
+Off-cycle parasitics include parts of the water heater that consume fuel when the heater is off, for example, a pilot light, or stand-by electronic control circuits. The fuel consumption rate {[}W{]} is strictly the total fuel that is consumed by all of the off-cycle parasitics.
+
+\paragraph{Field: Off-Cycle Parasitic Fuel Type}\label{field-off-cycle-parasitic-fuel-type-1}
+
+The type of fuel used by the off-cycle parasitics. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating. The fuel type can be the same or different from the Heater Fuel Type.
+
+\paragraph{Field: Off-Cycle Parasitic Heat Fraction to Tank}\label{field-off-cycle-parasitic-heat-fraction-to-tank-1}
+
+The fraction of off-cycle parasitic fuel energy that is converted to heat energy that ends up in the tank water. For example, a pilot light would deliver most of its heat to the tank water, as long as the thermal conversion efficiency must be taken into account, so perhaps 0.80 is reasonable. Electronic control circuits, on the other hand, do not add any heat to the tank and should be 0.
+
+\paragraph{Field: Off-Cycle Parasitic Height}\label{field-off-cycle-parasitic-height}
+
+The height {[}m{]} where any off-cycle parasitic heat gains are added to the tank.
+
+\paragraph{Field: On-Cycle Parasitic Fuel Consumption Rate}\label{field-on-cycle-parasitic-fuel-consumption-rate-1}
+
+On-cycle parasitics include parts of the water heater that consume fuel when the heater is on, for example, an induction fan, or stand-by electronic control circuits. The fuel consumption rate {[}W{]} is strictly the total fuel that is consumed by all of the on-cycle parasitics.
+
+\paragraph{Field: On-Cycle Parasitic Fuel Type}\label{field-on-cycle-parasitic-fuel-type-1}
+
+The type of fuel used by the on-cycle parasitics. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating. The fuel type can be the same or different from the Heater Fuel Type.
+
+\paragraph{Field: On-Cycle Parasitic Heat Fraction to Tank}\label{field-on-cycle-parasitic-heat-fraction-to-tank-1}
+
+The fraction of on-cycle parasitic fuel energy that is converted to heat energy that ends up in the tank water. For example, an induction fan might (maybe) deliver a small fraction of its energy to the tank water for a value of 0.05. Electronic control circuits, on the other hand, do not add any heat to the tank and should be 0.
+
+\paragraph{Field: On-Cycle Parasitic Height}\label{field-on-cycle-parasitic-height}
+
+The height {[}m{]} where any on-cycle parasitic heat gains are added to the tank.
+
+\paragraph{Field: Ambient Temperature Indicator}\label{field-ambient-temperature-indicator-1-000}
+
+The Ambient Temperature Indicator specifies how the ambient air temperature will be indicated. The field can be \textbf{Schedule}, \textbf{Zone}, or \textbf{Outdoors}. If \textbf{Schedule} is used, the Ambient Temperature Schedule value provides the ambient temperature. If \textbf{Zone} is used, the zone air temperature of the zone specified in the Ambient Temperature Zone field provides the ambient temperature. If \textbf{Outdoors} is used, the outdoor dry-bulb air temperature of the outdoor air node specified in the Ambient Temperature OutdoorAir:Node field provides the ambient temperature.
+
+\paragraph{Field: Ambient Temperature Schedule Name}\label{field-ambient-temperature-schedule-name-1-000}
+
+The reference to the schedule object specifying the ambient air temperature around the tank for skin losses. This field is only used if Ambient Temperature Indicator is \textbf{Schedule}.
+
+\paragraph{Field: Ambient Temperature Zone}\label{field-ambient-temperature-zone}
+
+The reference to the zone object specifying the ambient air temperature around the tank for skin losses. This field is only used if Ambient Temperature Indicator is \textbf{Zone}.
+
+\paragraph{Field: Ambient Temperature Outdoor Air Node}\label{field-ambient-temperature-outdoor-air-node}
+
+The reference to the outdoor air node specifying the ambient air temperature around the tank for skin losses. An outdoor air node can be defined by an OutdoorAir:Node object or OutdoorAir:NodeList object. This field is only used if Ambient Temperature Indicator is \textbf{Outdoors}.
+
+\paragraph{Field: Uniform Skin Loss Coefficient Per Unit Area to Ambient Temperature}\label{field-uniform-skin-loss-coefficient-per-unit-area-to-ambient-temperature-000}
+
+The uniform skin loss coefficient {[}W/m2-K{]} or U-Value of the tank to the ambient air temperature. The uniform skin loss accounts for the tank insulation and applies during both off- and on-cycle operation. The overall losses at any particular node can be further modified using the Additional Loss Coefficient fields to account for thermal shorting due to pipe penetrations, water heater feet, and any other loss effects.
+
+\paragraph{Field: Skin Loss Fraction to Zone}\label{field-skin-loss-fraction-to-zone}
+
+If the Ambient Temperature Indicator is \textbf{Zone}, this field adds the specified fraction of the skin losses to the zone heat balance as an internal gain.
+
+\paragraph{Field: Off-Cycle Flue Loss Coefficient to Ambient Temperature}\label{field-off-cycle-flue-loss-coefficient-to-ambient-temperature}
+
+The off-cycle flue loss coefficient {[}W/K{]} to the ambient air temperature. This field mainly applies to gas water heaters that have a flue.
+
+\paragraph{Field: Off-Cycle Flue Loss Fraction to Zone}\label{field-off-cycle-flue-loss-fraction-to-zone}
+
+If the Ambient Temperature Indicator is \textbf{Zone}, this field adds the specified fraction of the off-cycle flue losses to the zone heat balance as an internal gain.
+
+\paragraph{Field: Peak Use Flow Rate}\label{field-peak-use-flow-rate-1}
+
+The peak flow rate {[}m\(^{3}\)/s{]} of domestic hot water usage for stand-alone operation, i.e., without plant loop node connections. The peak value is multiplied by the Use Flow Rate Fraction Schedule. If there are node connections, this field is not used.
+
+\paragraph{Field: Use Flow Rate Fraction Schedule Name}\label{field-use-flow-rate-fraction-schedule-name-1}
+
+The reference to the schedule object specifiying the current fraction of Peak Volumetric Use Flow Rate of domestic hot water usage for stand-alone operation. If blank, the fraction defaults to 1.0 at all times.
+
+\paragraph{Field: Cold Water Supply Temperature Schedule Name}\label{field-cold-water-supply-temperature-schedule-name-1}
+
+The reference to the schedule object specifying the cold water temperature {[}°C{]} from the supply mains that makes up for the hot water lost down the drain. If blank, water temperatures are calculated by the Site:WaterMainsTemperature object. This field is for stand-alone operation only. If there are node connections, this field is not used.
+
+\paragraph{Field: Use Side Inlet Node Name}\label{field-use-side-inlet-node-name-1-000}
+
+The inlet node connection to the plant loop for the use side of the water heater. Typically the use side draws hot water from the tank and returns cooler water.
+
+\paragraph{Field: Use Side Outlet Node Name}\label{field-use-side-outlet-node-name-1-000}
+
+The outlet node connection to the plant loop for the use side of the water heater. Typically the use side draws hot water from the tank and returns cooler water.
+
+\paragraph{Field: Use Side Effectiveness}\label{field-use-side-effectiveness-1}
+
+This field specifies the heat transfer effectiveness between the use side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the use side water and the tank water. If the effectiveness is less than 1.0, then the use side outlet water temperature will not be as hot as the tank water at the outlet node, simulating an external heat exchanger that is indirectly coupled to the water heater tank.
+
+\paragraph{Field: Use Side Inlet Height}\label{field-use-side-inlet-height-000}
+
+The height of the use side inlet to the tank. If blank, the inlet defaults to the bottom of the tank. The inlet height cannot be higher than the tank height.
+
+\paragraph{Field: Use Side Outlet Height}\label{field-use-side-outlet-height-000}
+
+The height of the use side outlet from the tank. If blank or \textbf{autocalculate}, the inlet defaults to the top of the tank. The outlet height cannot be higher than the tank height.
+
+\paragraph{Field: Source Side Inlet Node}\label{field-source-side-inlet-node}
+
+The inlet node connection to the plant loop for the source side of the water heater. Typically the source side draws cold water from the tank and returns warmer water.
+
+\paragraph{Field: Source Side Outlet Node}\label{field-source-side-outlet-node}
+
+The outlet node connection to the plant loop for the source side of the water heater. Typically the source side draws cold water from the tank and returns warmer water.
+
+\paragraph{Field: Source Side Effectiveness}\label{field-source-side-effectiveness-1}
+
+This field specifies the heat transfer effectiveness between the source side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the source side water and the tank water. If the effectiveness is less than 1.0, then the source side outlet water temperature will be higher than the tank water at the outlet node, simulating an external heat exchanger that is indirectly coupled to the water heater tank.
+
+\paragraph{Field: Source Side Inlet Height}\label{field-source-side-inlet-height-000}
+
+The height of the source side inlet to the tank. If blank or \textbf{autocalculate}, the inlet defaults to the top of the tank. The inlet height cannot be higher than the tank height.
+
+\paragraph{Field: Source Side Outlet Height}\label{field-source-side-outlet-height-000}
+
+The height of the source side outlet from the tank. If blank, the inlet defaults to the bottom of the tank. The outlet height cannot be higher than the tank height.
+
+\paragraph{Field: Inlet Mode}\label{field-inlet-mode-000}
+
+The inlet mode of entering fluid from the use and source sides. There are two options:~ \textbf{Fixed} or \textbf{Seeking}. In Fixed mode, the fluid enters at the fixed heights specified above. In Seeking mode, the fluid ``seeks out'' the stratified node that is closest to the inlet temperature and adds all flow to that node. The Seekingbmode provides maximum stratification. The default is \textbf{Fixed}.
+
+\paragraph{Field: Use Side Design Flow Rate}\label{field-use-side-design-flow-rate-1-000}
+
+This field is optional and is used to specify the design flow rate through the Use Side of the water heater.~ The volumetric design flow rate is specified in m\(^{3}\)/s.~ The field is needed when the Use Side is connected to a plant loop.~ The field can be autosized.~ If autosized, then the input file should include a Plant Sizing object for the plant loop.~ Sizing results are reported in the EIO file.
+
+\paragraph{Field: Source Side Design Flow Rate}\label{field-source-side-design-flow-rate-1-000}
+
+This field is optional and is used to specify the design flow rate through the Source Side of the water heater.~ The volumetric design flow rate is specified in m\(^{3}\)/s.~ The field is needed when the Source Side is connected to a plant loop.~ The field can be autosized.~ If autosized, then the input file should include a Plant Sizing object for the plant loop.~ Sizing results are reported in the EIO file.
+
+\paragraph{Field: Indirect Water Heating Recovery Time}\label{field-indirect-water-heating-recovery-time-1}
+
+This field is optional and is used to provide a design parameter for autosizing design flow rates when the water heater is connected to the demand side of a plant loop.~ The recovery time is expressed in hours.~ This is the time that the entire volume of the tank can be heated from 14.4ºC to 57.2ºC (58ºF to 135ºF) with an inlet temperature defined as the exit temperature in the associated Plant Sizing object.~ The default is 1.5 hours.~ The calculation is based on log-mean temperature difference (LMTD) and includes the heat transfer effectiveness factor entered above.
+
+\paragraph{Field: Number Of Nodes}\label{field-number-of-nodes-000}
+
+The number of stratified nodes in the tank. There must be at least one node. The maximum number of nodes is 12, although this limit can be increased by editing the IDD.
+
+\paragraph{Field: Additional Destratification Conductivity}\label{field-additional-destratification-conductivity-000}
+
+An additional destratification conductivity {[}W/m-K{]} is added to the fluid conductivity of water (0.6 W/m-K) to account for vertical conduction effects along the inside of the tank wall, and perhaps other vertical components such as the flue, the cold water inlet pipe (dip tube), and the anode rod.
+
+\paragraph{Field: Node 1-12 Additional Loss Coefficient}\label{field-node-1-12-additional-loss-coefficient}
+
+An additional loss coefficient {[}W/K{]} added to the skin losses for a given node to account for thermal shorting due to pipe penetrations, water heater feet, and any other loss effects.
+
+\paragraph{Field: Source Side Flow Control Mode}\label{field-source-side-flow-control-mode-1}
+
+This field is optional and is used to provide control over the logic used by the source side of the water heater to request flow. There are three choices for different modes: IndirectHeatPrimarySetpoint, IndirectHeatAlternateSetpoint, or StorageTank.~~~ The mode called IndirectHeatPrimarySetpoint is the historical behavior prior to version 8.1.~ In this mode the water heater will request flow at the source side when the main setpoint, in the input field called Setpoint Temperature Schedule Name, and deadband call for the tank to be heated.~ This mode is typical for a water heater indirectly heated by a boiler.~ The mode called IndirectHeatAlternateSetpoint is similar but it bases its control decisions on an alternate setpoint given in the following field.~ This mode is useful when the indirect source of heat may not satisfy the load and an internal heater is used for backup.~ The mode called StorageTank is for a passive tank and it always requests flow unless the tank temperature is equal to or higher than the maximum limit given in the input field called Maximum Temperature Limit.
+
+\paragraph{Field: Indirect Alternate Setpoint Temperature Schedule Name}\label{field-indirect-alternate-setpoint-temperature-schedule-name-1}
+
+This field is optional and is used to provide a schedule with alternate setpoints for use with the IndirectHeatAlternateSetpoint mode in the previous field.~ The input field should contain a reference to a schedule object specifying the hot water temperature setpoint {[}°C{]} to use as the ``cut-out'' temperature for control logic at the source side.
+
+\begin{lstlisting}
+
+WaterHeater:Stratified,
+      Electric Water Heater,  !- Name
+      Water Heater,  !- End-Use Subcategory
+      0.1893,  !- Tank Volume {m3}
+      1.4,  !- Tank Height {m}
+      VerticalCylinder,  !- Tank Shape
+      ,  !- Tank Perimeter {m}
+      82.2222,  !- Maximum Temperature Limit {C}
+      MasterSlave,  !- Heater Priority
+      Hot Water Set Point Temp Schedule,  !- Heater 1 Set Point Temperature Schedule
+      2.0,  !- Heater 1 Deadband Temperature Difference {deltaC}
+      4500,  !- Heater 1 Capacity {W}    (Master)
+      1.0,  !- Heater 1 Height {m}
+      Hot Water Set Point Temp Schedule,  !- Heater 2 Set Point Temperature Schedule
+      5.0,  !- Heater 2 Deadband Temperature Difference {deltaC}
+      4500,  !- Heater 2 Capacity {W}    (Slave)
+      0.0,  !- Heater 2 Height {m}
+      ELECTRICITY,  !- Heater Fuel Type
+      0.98,  !- Heater Thermal Efficiency
+      10,  !- Off-Cycle Parasitic Fuel Consumption Rate {W}
+      ELECTRICITY,  !- Off-Cycle Parasitic Fuel Type
+      0,  !- Off-Cycle Parasitic Heat Fraction To Tank
+      ,  !- Off-Cycle Parasitic Height {m}
+      10,  !- On-Cycle Parasitic Fuel Consumption Rate {W}
+      ELECTRICITY,  !- On-Cycle Parasitic Fuel Type
+      0,  !- On-Cycle Parasitic Heat Fraction To Tank
+      ,  !- On-Cycle Parasitic Height {m}
+      SCHEDULE,  !- Ambient Temperature Indicator
+      Ambient Temp Schedule,  !- Ambient Temperature Schedule
+      ,  !- Ambient Temperature Zone
+      ,  !- Ambient Temperature Outdoor Air Node
+      0.846,  !- Uniform Skin Loss Coefficient Per Unit Area To Ambient Temperature {W/m2-K}
+      ,  !- Skin Loss Fraction To Zone {}
+      ,  !- Off-Cycle Flue Loss Coefficient To Ambient Temperature {W/K}
+      ,  !- Off-Cycle Flue Loss Fraction To Zone {}
+      ,  !- Peak Volumetric Use Flow Rate {m3/s}
+      ,  !- Use Flow Rate Fraction Schedule
+      ,  !- Cold Water Supply Temperature Schedule
+      Water Heater Use Inlet Node,  !- Use Side Inlet Node
+      Water Heater Use Outlet Node,  !- Use Side Outlet Node
+      1.0,  !- Use Side Effectiveness {}
+      ,  !- Use Side Inlet Height {m}
+      ,  !- Use Side Outlet Height {m}
+      ,  !- Source Side Inlet Node
+      ,  !- Source Side Outlet Node
+      ,  !- Source Side Effectiveness {}
+      ,  !- Source Side Inlet Height {m}
+      ,  !- Source Side Outlet Height {m}
+      FIXED,  !- Inlet Mode {FIXED | SEEKING}
+      6,  !- Number Of Nodes
+      0.1,  !- Destratification Conductivity {W/m-K}
+      0.15,  !- Node 1 Additional Loss Coefficient {W/K}
+      ,  !- Node 2 Additional Loss Coefficient {W/K}
+      ,  !- Node 3 Additional Loss Coefficient {W/K}
+      ,  !- Node 4 Additional Loss Coefficient {W/K}
+      ,  !- Node 5 Additional Loss Coefficient {W/K}
+      0.1;  !- Node 6 Additional Loss Coefficient {W/K}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-030}
+
+All of the output variables reported for the WaterHeater:Mixed object also apply to the WaterHeater:Stratified object, with several qualifications noted below:
+
+\paragraph{Water Heater Tank Temperature {[}C{]}}\label{water-heater-tank-temperature-c-1}
+
+The average water tank temperature, i.e., the average of all of the node average temperatures.
+
+\paragraph{Water Heater Final Tank Temperature {[}C{]}}\label{water-heater-final-tank-temperature-c-1}
+
+The final water tank temperature at the end of the system timestep, i.e., the average of all of the final node temperatures at the end of the system timestep. If reported at the ``Detailed'' interval, this output variable can be used to verify an exact energy balance on the water heater.
+
+\paragraph{Water Heater Heating Rate {[}W{]}}\label{water-heater-heating-rate-w-1}
+
+The total average heating rate supplied by Heater 1 plus Heater 2.
+
+\paragraph{Water Heater Heating Energy {[}J{]}}\label{water-heater-heating-energy-j-1}
+
+The total heating energy supplied by Heater 1 plus Heater 2.
+
+\paragraph{\texorpdfstring{Water Heater Cycle On Count {[]}}{Water Heater Cycle On Count }}\label{water-heater-cycle-on-count-1}
+
+The number of times that either Heater 1 or Heater 2 turned on in the time period.
+
+\paragraph{\texorpdfstring{Water Heater Runtime Fraction {[]}}{Water Heater Runtime Fraction }}\label{water-heater-runtime-fraction-1}
+
+The fraction of the time period that either Heater 1 or Heater 2 was running.
+
+In addition, the WaterHeater:Stratified object also reports the following output variables:
+
+\begin{itemize}
+\item
+  HVAC,Average,Water Heater Heater 1 Heating Rate {[}W{]}
+\item
+  HVAC,Average,Water Heater Heater 2 Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Water Heater Heater 1 Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Water Heater Heater 2 Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Water Heater Heater 1 Cycle On Count {[]}
+\item
+  HVAC,Sum,Water Heater Heater 2 Cycle On Count~ {[]}
+\item
+  HVAC,Average,Water Heater Heater 1 Runtime Fraction {[]}
+\item
+  HVAC,Average,Water Heater Heater 2 Runtime Fraction {[]}
+\item
+  HVAC,Average,Water Heater Temperature Node \textless{}x\textgreater{} {[}C{]}
+\item
+  HVAC,Average,Water Heater Final Temperature Node \textless{}x\textgreater{} {[}C{]}
+\end{itemize}
+
+\paragraph{Water Heater Heater 1 Heating Rate {[}W{]}}\label{water-heater-heater-1-heating-rate-w}
+
+The average heating rate supplied by Heater 1.
+
+\paragraph{Water Heater Heater 2 Heating Rate {[}W{]}}\label{water-heater-heater-2-heating-rate-w}
+
+The average heating rate supplied by Heater 2.
+
+\paragraph{Water Heater Heater 1 Heating Energy {[}J{]}}\label{water-heater-heater-1-heating-energy-j}
+
+The heating energy supplied by Heater 1.
+
+\paragraph{Water Heater Heater 2 Heating Energy {[}J{]}}\label{water-heater-heater-2-heating-energy-j}
+
+The heating energy supplied by Heater 2.
+
+\paragraph{\texorpdfstring{Water Heater Heater 1 Cycle On Count {[]}}{Water Heater Heater 1 Cycle On Count }}\label{water-heater-heater-1-cycle-on-count}
+
+The number of times that Heater 1 turned on in the time period.
+
+\paragraph{\texorpdfstring{Water Heater Heater 2 Cycle On Count~ {[]}}{Water Heater Heater 2 Cycle On Count~ }}\label{water-heater-heater-2-cycle-on-count}
+
+The number of times that Heater 2 turned on in the time period.
+
+\paragraph{\texorpdfstring{Water Heater Heater 1 Runtime Fraction {[]}}{Water Heater Heater 1 Runtime Fraction }}\label{water-heater-heater-1-runtime-fraction}
+
+The fraction of the time period that Heater 1 was running.
+
+\paragraph{\texorpdfstring{Water Heater Heater 2 Runtime Fraction {[]}}{Water Heater Heater 2 Runtime Fraction }}\label{water-heater-heater-2-runtime-fraction}
+
+The fraction of the time period that Heater 2 was running.
+
+\paragraph{Water Heater Temperature Node 1-12 {[}C{]}}\label{water-heater-temperature-node-1-12-c}
+
+The average node temperature.
+
+\paragraph{Water Heater Final Temperature Node 1-12 {[}C{]}}\label{water-heater-final-temperature-node-1-12-c}
+
+The final node temperature at the end of the system timestep.
+
+\subsection{WaterHeater:Sizing}\label{waterheatersizing}
+
+The WaterHeater:Sizing object is used to provide additional input data needed for designing tank volume and/or heater capacity for either the Mixed or Stratified water heaters.~ This object is only needed if volume or capacity is being automatically sized.~ There are no output variable associated with this object --~ sizing results are reported to the EIO output file and some predefined summary reports.
+
+A source of design input data for use with this object can be found in the current ASHRAE Handbook HVAC Applications chapter on Service Water Heating.
+
+The idd entry for this object follows.
+
+\subsubsection{Inputs}\label{inputs-2-045}
+
+\paragraph{Field: WaterHeater Name}\label{field-waterheater-name}
+
+This field contains the unique name of the water heater being sized.~ This name should match the name of a Water Heater:Mixed or a Water Heater:Stratified input object defined elsewhere in the input file.
+
+\paragraph{Field: Design Mode}\label{field-design-mode}
+
+This field describes which of several methods are to be used for sizing the water heater.~ There are six possible choices and one of the following should be selected:
+
+\begin{itemize}
+\item
+  \textbf{PeakDraw}. This design method uses the design flow rates of all the different demands placed on the water heater.~ The tank size is based on how long it can meet the demand and how quickly it can recover.~ The user enters the time in hours that the water heater can meet the demands.~ Only the hot water uses connected to an individual water heater, or scheduled in the water heater object for stand-alone units, are included in that water heater's peak draw.
+\item
+  \textbf{ResidentialHUD-FHAMinimum} This design method is based on minimum permissible water heater sizes (established by HUD-FHA in its Minimum Property Standards for One- and Two-Family Living Units, No. 4900.1-1982).~ The user enters the number of bathrooms and bedrooms in this input object.~ The smallest allowable water heater sizes are used.
+\item
+  \textbf{PerPerson} This design method scales sizes based on the total number of people in all zones in the building.~ Each water heater in the model will be sized using the total (peak, design) number of people for the entire model.~ The number of people is determined from People objects defined elsewhere in the input file
+\item
+  \textbf{PerFloorArea} This design method scales sizes based on the total floor area in all the zones in the building.~ Each water heater in the model will be sized using all the floor area in the model.~ The floor areas are determined from the geometry input elsewhere in the input file.
+\item
+  \textbf{PerUnit} This design method scales sizes based on an arbitrary number of units.~ This can be used, for example, to size based on the number of rooms in a lodging building.~ The user provides the number of units in an input field in this object.
+\item
+  \textbf{PerSolarCollectorArea} This design method scales tank volume based on the collector area for a solar hot water collector.~ The collector area is summed for all the collectors in the model and each tank is sized for the total.~ The collector area is determined from input for Solar Collectors defined elsewhere in the input file.
+\end{itemize}
+
+\paragraph{Field: Time Storage Can Meet Peak Draw}\label{field-time-storage-can-meet-peak-draw}
+
+This field provides the time, in hours, that the tank's volume can sustain a peak draw.~ It is used to size the tank's volume which is the simple product of peak draw volume flow rate and the draw time.~ There is no assurance that the water will be at the desired temperature for the entire draw.~ This field is only used if the Design Mode is ``\textbf{PeakDraw}.'' For a water heater connected to a full plant loop, it should be on the supply side and the plant loop needs a Plant Sizing object and the draw rate is the Use side design flow rate. For a stand-alone water heater, the draw rate is the maximum scheduled peak use flow rate.
+
+\paragraph{Field: Time for Tank Recovery}\label{field-time-for-tank-recovery}
+
+This field provides the the time, in hours, that tank's heater needs to recover the volume of the tank. The temperatures used to define recovery are a starting temperature of 14.4ºC (58ºF) and a final temperature of 57.2ºC (135ºF). This field is only used if the Design Mode is ``\textbf{PeakDraw}.''
+
+\paragraph{Field: Nominal Tank Volume for Autosizing Plant Connections}\label{field-nominal-tank-volume-for-autosizing-plant-connections}
+
+This field is used in case the water heater is indirectly heated by its source side connections and they are also autosized.~ Because of the complexity of such a water heater and the timing for when sizing calculation happen inside EnergyPlus, the Source side connection flow rates need to be reported before the tank's volume can be sized to meet Peak Draw.~ This input field is used to provide a nominal tank volume to use temporarily while the flow connections are sized.~ This field is only used if the Design Mode is ``\textbf{PeakDraw}'' and the water heater has autosized plant connections on the demand side.
+
+\paragraph{Field: Number of Bedrooms}\label{field-number-of-bedrooms}
+
+This field is used to enter the numer of bedrooms in the model.~ This field is only used if the Design Mode is ``\textbf{ResidentialHUD-FHAMinimum}.''
+
+\paragraph{Field: Number of Bathrooms}\label{field-number-of-bathrooms}
+
+This field is used to enter the number of bathrooms in the model.~ This field is only used if the Design Mode is ``\textbf{ResidentialHUD-FHAMinimum}.''
+
+\paragraph{Field: Storage Capacity per Person}\label{field-storage-capacity-per-person}
+
+This field is used to enter the tank's storage volume on per-person basis.~ The units are m\(^{3}\)/person.~ This field is only used if the Design Mode is ``\textbf{PerPerson}.''
+
+\paragraph{Field: Recovery Capacity per Person}\label{field-recovery-capacity-per-person}
+
+This field is used to enter the recovery capacity per person in units of m\(^{3}\)/person/hr.~ This is the volume of water the heater can recover in one hour per person.~ Recovery is heating water from a starting temperature of 14.4ºC (58ºF) to a final temperature of 57.2ºC (135ºF).~ This field is only used if the Design Mode is ``\textbf{PerPerson}.''
+
+\paragraph{Field: Storage Capacity per Floor Area}\label{field-storage-capacity-per-floor-area}
+
+This field is used to enter the tank's storage volume on a per-floor-area basis.~ The units are m\(^{3}\) /m\(^{2}\) (water/floor area).~ This field is only used if the Design Mode is ``\textbf{PerFloorArea}.''
+
+\paragraph{Field: Recovery Capacity per Floor Area}\label{field-recovery-capacity-per-floor-area}
+
+This field is used to enter the recovery capacity per floor area in units of m\(^{3}\)/m\(^{2}\)/hr.~ This is the volume water the heater can recover in an hour per floor area.~ Recovery is heating water from a starting temperature of 14.4ºC (58ºF) to a final temperature of 57.2ºC (135ºF).~ This field is only used if the Design Mode is ``\textbf{PerFloorArea}.''
+
+\paragraph{Field: Number of Units}\label{field-number-of-units-000}
+
+This field is used to enter the number of Units for use in sizing on per-Unit basis with the next two fields.~ This field is only used if the Design Mode is ``\textbf{PerUnit}.''~ This can be used to account for any arbitrary item such as lodging rooms, desks, water fixtures, restrooms, etc.
+
+\paragraph{Field: Storage Capacity per Unit}\label{field-storage-capacity-per-unit}
+
+This field is used to enter the tanks' storage volume on per-Unit basis.~ The units are m\(^{3}\)/Unit.~ The number of Units is entered in the previous field.~ This field is only used if the Design Mode is ``\textbf{PerUnit}.''
+
+\paragraph{Field: Recovery Capacity per Unit}\label{field-recovery-capacity-per-unit}
+
+This field is used to enter the recover capacity per Unit in units of m\(^{3}\)/Unit/hr.~ This is the volume of water the heater can recover in an hour per Unit.~ Recovery is heating water from a starting temperature of 14.4ºC (58ºF) to a final temperature of 57.2ºC (135ºF).~ This field is only used if the Design Mode is ``\textbf{PerUnit}.''
+
+\paragraph{Field: Storage Capacity per Collector Area}\label{field-storage-capacity-per-collector-area}
+
+This field is used to enter the tank's storage volume on per-solar-collector-area basis.~ The units are m\(^{3}\)/m\(^{2}\).~ This field is only used if the Design Mode is ``\textbf{PerSolarCollectorArea}.''
+
+\paragraph{Field: Height Aspect Ratio}\label{field-height-aspect-ratio}
+
+This field is used to scale the height of a stratified tank to preserve relative geometry for different size tanks. The Height Aspect Ratio is defined at the length scale in the vertical direction (height) divided by the length scale in the horizontal direction (diameter).~ This field is only used if the water heater being sized is a Water Heater:Stratified, the tank height has been set to Autosize, and the tank shape is set to \textbf{VerticalCylinder}. This field can be used with any Design Mode.
+
+\subsection{WaterHeater:HeatPump:PumpedCondenser}\label{waterheaterheatpumppumpedcondenser}
+
+The heat pump water heater with pumped condenser (HPWH) is a compound object consisting of a water heater tank (e.g., \lstinline!WaterHeater:Mixed! or \lstinline!WaterHeater:Stratified!), a direct expansion (DX) ``coil'' (i.e., an air-to-water DX compression system which includes a water heating coil, air coil, compressor, and water pump), and a fan to provide air flow across the air coil associated with the DX compression system. These objects work together to model a system which heats water using zone air, outdoor air, or a combination of zone and outdoor air as the primary heat source. Numerous configurations of tank location, inlet air source, and DX coil compressor location can be modeled, with one common configuration shown below.
+
+\begin{figure}[hbtp] % fig 81
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image192.png}
+\caption{Schematic diagram for a heat pump water heater located in a zone \protect \label{fig:schematic-diagram-for-a-heat-pump-water}}
+\end{figure}
+
+In this model, the heat pump water heater's DX coil is considered the primary heat source and the water tank's heater (element or burner) provides supplemental heat as necessary. The model also assumes that the heat pump's fan and water pump cycle on and off with the compressor.
+
+To model a heat pump water heater, the input data file must include some combination of the following objects depending on the configuration to be modeled:
+
+\begin{itemize}
+\item
+  \lstinline!WaterHeater:HeatPump:PumpedCondenser! (required)
+\item
+  \lstinline!WaterHeater:Mixed! or \lstinline!WaterHeater:Stratified! (required)
+\item
+  \lstinline!Coil:WaterHeating:AirToWaterHeatPump:Pumped! or \lstinline!Coil:WaterHeating:AirToWaterHeatPump:VariableSpeed! (required)
+\item
+  \lstinline!Fan:OnOff! (required)
+\item
+  \lstinline!ZoneHVAC:EquipmentList! (when the HPWH draws some or all of its air from the zone, the heat pump water heater type and name must be in this list)
+\item
+  \lstinline!ZoneHVAC:EquipmentConnections! (when the HPWH draws some or all of its air from the zone, the HPWH air inlet and outlet node names must be provided in this object)
+\item
+  \lstinline!OutdoorAir:NodeList! (for HPWHs that use outdoor air as all or part of the heat source, the HPWH outdoor air node name must be provided in this list)
+\end{itemize}
+
+The input fields for the compound object are described in detail below:
+
+\subsubsection{Inputs}\label{inputs-3-040}
+
+\paragraph{Field: Name}\label{field-name-2-042}
+
+This alpha field contains a unique user-assigned name for an instance of a heat pump water heater. Any reference to this heat pump water heater by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-019}
+
+This alpha field contains the name of the schedule (ref: Schedule) that denotes whether the heat pump compressor is available to operate during a given time period. A schedule value equal to 0 denotes that the heat pump compressor is off for that time period. A value other than 0 denotes that the heat pump compressor is available to operate during that time period. During times when the heat pump compressor is scheduled off, the heater (element or burner) in the water tank object operates based on its tank set point temperature schedule and the heat pump's parasitic electric power is also off for that time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Compressor Setpoint Temperature Schedule Name}\label{field-compressor-setpoint-temperature-schedule-name}
+
+This alpha field contains the name of the schedule (ref: Schedule) that specifies the set point (or ``cut-out'') temperature for the heat pump compressor. Temperature values used in this schedule should be in degrees Celsius. The heat pump compressor cycles off when the tank water reaches this set point temperature. Once the heat pump compressor cycles off, the tank water temperature floats downward until it falls below the set point temperature minus the dead band temperature difference defined below (i.e., the ``cut-in'' temperature). At this point, the heat pump compressor cycles on and remains on until the heat pump compressor set point temperature is reached.
+
+\paragraph{Field: Dead Band Temperature Difference}\label{field-dead-band-temperature-difference-000}
+
+This numeric field contains the dead band temperature difference in degrees Celsius. The heat pump compressor ``cut-in'' temperature is defined as the compressor set point temperature defined above minus this dead band temperature difference. The heat pump compressor cycles on when the water temperature in the tank falls below the ``cut-in'' temperature. The heat pump compressor remains on until the water temperature in the tank rises above the compressor set point (``cut-out'') temperature defined above. The dead band temperature difference must be greater than 0°C and less than or equal to 20°C. If this field is left blank, the default value is 5°C.
+
+In this model, the heat pump water heater's DX compression system is considered the primary heat source and the water tank's heater (element or burner) provides supplemental heat as necessary. Therefore, the cut-in temperature for the heat pump compressor (set point minus dead band temperature difference) is usually higher than the set point temperature for the heater (element or burner) in the associated water heater tank object. At times when the water heater tank set point temperature is greater than the cut-in temperature of the heat pump compressor, the heat pump compressor is disabled and the tank's heater is used to heat the water.
+
+\paragraph{Field: Condenser Water Inlet Node Name}\label{field-condenser-water-inlet-node-name-000}
+
+This alpha field contains the name of the inlet water node for the heat pump's water heating coil (condenser). This node name must also be specified in the water heater tank object as the source outlet node name, and in the DX coil object as the condenser water inlet node name.
+
+\paragraph{Field: Condenser Water Outlet Node Name}\label{field-condenser-water-outlet-node-name-000}
+
+This alpha field contains the name of the outlet water node for the heat pump's water heating coil (condenser). This node name must also be specified in the water heater tank object as the source inlet node name, and in the DX coil object as the condenser water outlet node name.
+
+\paragraph{Field: Condenser Water Flow Rate}\label{field-condenser-water-flow-rate}
+
+This numeric field contains the heat pump's condenser water flow rate in cubic meters per second. It is the actual condenser water flow rate to be simulated, which may differ from the rated condenser water volumetric flow rate specified for the heat pump's DX coil (Ref. Coil:WaterHeating:AirToWaterHeatPump). This water flow rate must be greater than 0 or this field is autocalculatable. If autocalculated (field value = \textbf{autocalculate}), the condenser water flow rate is set equal to the rated heating capacity of the heat pump's DX coil multiplied by 4.487E-8 m\(^{3}\)/s/W. When this flow rate is different from the Rated Condenser Water Volumetric Flow Rate specified in the heat pump's DX coil object (Ref. Coil:WaterHeating:AirToWaterHeatPump), the user should also specify a Total Heating Capacity Modifier Curve Name (function of water flow fraction) and a Heating COP Modifier Curve Name (function of water flow fraction) in the associated DX coil object to account for differences in capacity and power consumption at the off-rated water flow rate.
+
+\paragraph{Field: Evaporator Air Flow Rate}\label{field-evaporator-air-flow-rate}
+
+This numeric field contains the air flow rate across the heat pump's air coil (evaporator) in cubic meters per second. It is the actual air flow rate to be simulated, which may differ from the rated evaporator air volumetric flow rate specified for the heat pump's DX coil (Ref. Coil:WaterHeating:AirToWaterHeatPump:Pumped). Values must be greater than 0 or this field is autocalculatable. If autocalculated (field value = \textbf{autocalculate}), the evaporator air flow rate is set equal to the rated heating capacity of the heat pump's DX coil multiplied by 5.035E-5 m\(^{3}\)/s/W. When this flow rate is different from the Rated Evaporator Air Volumetric Flow Rate specified in the heat pump's DX coil object (Ref. Coil:WaterHeating:AirToWaterHeatPump:Pumped), the user should also specify a Total Heating Capacity Modifier Curve Name (function of air flow fraction) and a Heating COP Modifier Curve Name (function of air flow fraction) in the associated DX coil object to account for differences in capacity and power consumption at the off-rated air flow rate.
+
+\paragraph{Field: Inlet Air Configuration}\label{field-inlet-air-configuration}
+
+This choice field defines the configuration of the air flow path through the heat pump air coil (evaporator) and fan section. Valid entries are \textbf{Schedule}, \textbf{ZoneAirOnly}, \textbf{OutdoorAirOnly}, or \textbf{ZoneAndOutdoorAir}. If `Schedule' is selected, names for an inlet air temperature schedule and an inlet air humidity schedule must be defined in the fields below. If `ZoneAirOnly' is selected, the corresponding zone name must be entered in the Inlet Air Zone Name field below. If `ZoneAndOutdoorAir' is selected, the corresponding Inlet Air Zone Name, Inlet Air Mixer Node Name, Outlet Air Splitter Node Name, and an Inlet Air Mixer Schedule Name must be entered in the corresponding fields below.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-008}
+
+This alpha field contains the name of the node from which the heat pump water heater draws its inlet air. If the Inlet Air Configuration field defined above is set to `ZoneAirOnly' or `ZoneAndOutdoorAir', then this node name should be the name of a zone air exhaust node (Ref. ZoneHVAC:EquipmentConnections). If the Inlet Air Configuration field is set to `OutdoorAirOnly', this node name should be left blank. If the Inlet Air Configuration field is set to `Schedule', this node name should simply be a unique name that allows the user to receive output on conditions at this node for verification purposes.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-007}
+
+This alpha field contains the name of the node to which the heat pump water heater sends its outlet air. If the Inlet Air Configuration field defined above is set to `ZoneAirOnly' or `ZoneAndOutdoorAir', then this node name should be the name of a zone air inlet node (Ref. ZoneHVAC:EquipmentConnections). If the Inlet Air Configuration field is set to `OutdoorAirOnly', this node name should be left blank. If the Inlet Air Configuration field is set to `Schedule', this node name should simply be a unique name that allows the user to receive output on conditions at this node for verification purposes.
+
+\paragraph{Field: Outdoor Air Node Name}\label{field-outdoor-air-node-name-000}
+
+This alpha field contains the name of the node from which the heat pump water heater draws its outdoor air. If the Inlet Air Configuration field defined above is set to `ZoneAirOnly' or `Schedule', this node name should be left blank. If the Inlet Air Configuration field is set to `ZoneAndOutdoorAir' or `OutdoorAirOnly', this node name should be the name of an outdoor air node (Ref. OutdoorAir:NodeList).
+
+\paragraph{Field: Exhaust Air Node Name}\label{field-exhaust-air-node-name}
+
+This alpha field contains the name of the node to which the heat pump water heater sends its exhaust air. If the Inlet Air Configuration field defined above is set to `ZoneAirOnly' or `Schedule', this node name should be left blank. If the Inlet Air Configuration field is set to `ZoneAndOutdoorAir' or `OutdoorAirOnly', then this node name should be a unique name that allows the user to receive output on conditions at this node for verification purposes.
+
+\paragraph{Field: Inlet Air Temperature Schedule Name}\label{field-inlet-air-temperature-schedule-name}
+
+This alpha field contains the name of a schedule used to define the dry-bulb temperature of the inlet air to the heat pump air coil (evaporator) and fan section. Schedule values should be in degrees Celsius. This field is only used when the Inlet Air Configuration defined above is specified as `Schedule', otherwise leave this field blank.
+
+\paragraph{Field: Inlet Air Humidity Schedule Name}\label{field-inlet-air-humidity-schedule-name}
+
+This alpha field contains the name of a schedule used to define the humidity of the inlet air to the heat pump evaporator and fan section. Schedule values must be entered as relative humidity fraction from 0 to 1 (e.g., a schedule value of 0.5 means 50\%RH). This field is only used when the Inlet Air Configuration defined above is specified as `Schedule', otherwise leave this field blank.
+
+\paragraph{Field: Inlet Air Zone Name}\label{field-inlet-air-zone-name}
+
+This alpha field contains the name of the zone from which the heat pump evaporator and fan section draws some or all of its inlet air. This field is only used when the Inlet Air Configuration defined above is specified as `ZoneAirOnly' or `ZoneAndOutdoorAir'.
+
+\paragraph{Field: Tank Object Type}\label{field-tank-object-type-000}
+
+This alpha (choice) field contains the type of water heater tank used by this heat pump water heater. Currently, the only valid choices are WaterHeater:Mixed or WaterHeater:Stratified.
+
+\paragraph{Field: Tank Name}\label{field-tank-name-000}
+
+This alpha field contains the name of the specific water heater tank used by this heat pump water heater. This must be a tank of type \lstinline!WaterHeater:Mixed! or \lstinline!WaterHeater:Stratified!.
+
+\paragraph{Field: Tank Use Side Inlet Node Name}\label{field-tank-use-side-inlet-node-name}
+
+This alpha field contains the name of the use side inlet node of the water heater tank used by this heat pump water heater. This name must match the Use Side Inlet Node Name in the water heater tank object (Ref. \lstinline!WaterHeater:Mixed!). This field is required if the water heater tank use side nodes are connected to a plant loop, otherwise leave this field blank. When used, the branch object should reflect that this node is part of a \lstinline!WaterHeater:HeatPump:PumpedCondenser! object (see branch object example below).
+
+\paragraph{Field: Tank Use Side Outlet Node Name}\label{field-tank-use-side-outlet-node-name}
+
+This alpha field contains the name of the use side outlet node of the water heater tank used by this heat pump water heater. This name must match the Use Side Outlet Node Name in the water heater tank object (Ref. \lstinline!WaterHeater:Mixed!). This field is required if the water heater tank use side nodes are connected to a plant loop, otherwise leave this field blank. When used, the branch object should reflect that this node is part of a \lstinline!WaterHeater:HeatPump:PumpedCondenser! object (see branch object example below).
+
+\paragraph{Field: DX Coil Object Type}\label{field-dx-coil-object-type}
+
+This alpha (choice) field contains the type of DX coil used by this heat pump water heater. Currently, the only valid choice is Coil:WaterHeating:AirToWaterHeatPump:Pumped.
+
+\paragraph{Field: DX Coil Name}\label{field-dx-coil-name}
+
+This alpha field contains the name of the specific DX coil (\lstinline!Coil:WaterHeating:AirToWaterHeatPump:Pumped! or \lstinline!Coil:WaterHeating:AirToWaterHeatPump:VariableSpeed! object) used by this heat pump water heater.
+
+\paragraph{Field: Minimum Inlet Air Temperature for Compressor Operation}\label{field-minimum-inlet-air-temperature-for-compressor-operation}
+
+This numeric field contains the minimum inlet air dry-bulb temperature entering the air coil (evaporator) and fan section, in degrees Celsius, below which the heat pump compressor does not operate. The minimum inlet air dry-bulb temperature should be greater than or equal to -5°C. If this field is left blank, the default value is 10°C.
+
+\paragraph{Field: Compressor Location}\label{field-compressor-location}
+
+This alpha (choice) field contains the location of the heat pump compressor and the air temperature for this location is used to control operation of the compressor's crankcase heater in the Coil:WaterHeating:AirToWaterHeatPump:Pumped object. Valid entries are \textbf{Schedule}, \textbf{Zone}, or \textbf{Outdoors}. If `Schedule' is selected, a compressor ambient temperature schedule name must be defined in the field below; otherwise, the field below should be left blank. If `Zone' is selected, the crankcase heater operation is controlled based on the air temperature in the zone defined in the field Inlet Air Zone Name, and the Inlet Air Configuration must be `ZoneAirOnly' or `ZoneAndOutdoorAir'. If `Outdoors' is selected, crankcase heater operation is controlled based on the outdoor air temperature.
+
+\paragraph{Field: Compressor Ambient Temperature Schedule Name}\label{field-compressor-ambient-temperature-schedule-name}
+
+This alpha field contains the name of a schedule that defines the ambient air temperature surrounding the heat pump compressor, which is used to control the compressor's crankcase heater operation. This field is only used when the compressor location field defined above is specified as `Schedule', otherwise it should be left blank.
+
+\paragraph{Field: Fan Object Type}\label{field-fan-object-type-001}
+
+This alpha (choice) field contains the type of fan used by this heat pump water heater. Currently, the only valid choice is Fan: OnOff.
+
+\paragraph{Field: Fan Name}\label{field-fan-name-004}
+
+This alpha field contains the name of the specific fan (\lstinline!Fan:OnOff! object) used by this heat pump water heater.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-000}
+
+This alpha (choice) field defines the placement of the fan in the heat pump water heater. Valid choices are \textbf{BlowThrough} (fan upstream of the air coil) and \textbf{DrawThrough} (fan downstream of the air coil). If this field is left blank, the default value is DrawThrough.
+
+\paragraph{Field: On Cycle Parasitic Electric Load}\label{field-on-cycle-parasitic-electric-load-000}
+
+This numeric field contains the on-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the heat pump water heater. This parasitic electric load is consumed whenever the heat pump compressor is operating and the model assumes that this parasitic power does not contribute to heating the water. This parasitic load does, however, affect the zone air heat balance when the heat pump water heater sends some or all of its outlet air to a zone (i.e., Inlet Air Configuration field specified as `ZoneAirOnly' or `ZoneAndOutdoorAir') and the Parasitic Heat Rejection Location field is specified as `Zone'. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
+
+\paragraph{Field: Off Cycle Parasitic Electric Load}\label{field-off-cycle-parasitic-electric-load-000}
+
+This numeric field contains the off-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the heat pump compressor. This parasitic electric load is consumed whenever the heat pump water heater is available but the compressor is not operating, and the model assumes that this parasitic power does not contribute to heating the water. This parasitic load does, however, affect the zone air heat balance when the heat pump water heater sends some or all of its outlet air to a zone (i.e., Inlet Air Configuration field specified as `ZoneAirOnly' or `ZoneAndOutdoorAir') and the Parasitic Heat Rejection Location field is specified as `Zone'. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
+
+\paragraph{Field: Parasitic Heat Rejection Location}\label{field-parasitic-heat-rejection-location}
+
+This alpha (choice) field determines where the on-cycle and off-cycle parasitic heat is rejected. Valid choices are Zone and Exterior. If `Zone' is selected, both the on-cycle and off-cycle parasitic heat is rejected to the zone defined in the field Inlet Air Zone Name, and the Inlet Air Configuration must be `ZoneAirOnly' or `ZoneAndOutdoorAir. If 'Outdoors' is selected, this parasitic heat is rejected outdoors (does not impact the zone air heat balance) regardless of the specified Inlet Air Configuration. If this field is left blank, the default value is 'Outdoors'.
+
+\paragraph{Field: Inlet Air Mixer Node Name}\label{field-inlet-air-mixer-node-name}
+
+This optional alpha field defines the name of the HVAC node which represents the mixture of outdoor air and zone air that enters the heat pump air coil (evaporator) and fan section. The model mixes outdoor air with zone air and places the result on this inlet air mixer node based on the Inlet Air Mixer Schedule defined below. When the schedule value is equal to 0, 100\% zone air enters the evaporator coil and fan section of the heat pump water heater. When the schedule value is equal to 1, 100\% outdoor air enters the evaporator coil and fan section. This node name must be provided if the Inlet Air Configuration field above is specified as `ZoneAndOutdoor Air', otherwise this field should be left blank.
+
+\paragraph{Field: Outlet Air Splitter Node Name}\label{field-outlet-air-splitter-node-name}
+
+This alpha field defines the name of the air node to which the heat pump air coil (evaporator) and fan sends all of its outlet air. The supply air flow downstream of this node is split between the zone and outdoors based on the Inlet Air Mixer schedule defined below. When the schedule value is equal to 0, the entire outlet air stream is diverted to the zone. When the schedule value is equal to 1, the entire outlet air stream is exhausted to outdoors. This node name must be provided if the Inlet Air Configuration field above is specified as `Zone and Outdoor Air', otherwise this field should be left blank.
+
+\paragraph{Field: Inlet Air Mixer Schedule Name}\label{field-inlet-air-mixer-schedule-name}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump draws its inlet air from the zone, outdoors, or a combination of zone and outdoor air. A schedule value equal to 0 indicates that the heat pump draws its inlet air from the zone. A schedule value equal to 1 denotes that the heat pump draws its inlet air from outdoors. Values between 0 and 1 denote a mixture of zone and outdoor air proportional to the schedule value. The Inlet Air Mixer schedule controls both the inlet air mixer and outlet air splitter nodes in unison to ensure that the operation of the heat pump does not contribute to zone pressurization or depressurization. For example if the Inlet Air Mixer schedule value is 0.4, then the inlet air mixer node is composed of 40\% outdoor air and 60\% zone air. For this same case, the outlet air splitter directs 60\% of the HPWH outlet air back to the zone and 40\% of the outlet air flow is exhausted outdoors. This schedule name must be provided if the Inlet Air Configuration field is specified as `Zone and Outdoor Air', otherwise this field should be left blank.
+
+\paragraph{Field: Tank Element Control Logic}\label{field-tank-element-control-logic}
+
+This alpha field defines settings for the control logic of when to run the tank element in relation to whether the heat pump is running.
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{MutuallyExclusive} means that once the tank heating element(s) are active, the heat pump is shut down until the heating element setpoint is reached.
+\item
+  \textbf{Simultaneous} (default) means that both the tank heating element and heat pump are used at the same time to recover the tank temperature.
+\end{itemize}
+
+\paragraph{Field: Control Sensor 1 Height In Stratified Tank}\label{field-control-sensor-1-height-in-stratified-tank}
+
+This alpha field defines where the tank temperature is sensed for heat pump control when the tank type is \lstinline!WaterHeater:Stratified!.~ The stratified tank model produces tank temperature at different nodes in the vertical direction and various options are available for how this temperature should be sensed to control the heat pump.~ This is measured in height from the bottom of the tank. Internally the appropriate node is determined based on this height. If omitted, this defaults to the height of Heater1.
+
+\paragraph{Field: Control Sensor 1 Weight}\label{field-control-sensor-1-weight}
+
+The model can optionally use two control sensor locations in stratified tanks. When that is the case, the temperature sensed at each location is weighted. This alpha input specifies the weight associated with Control Sensor 1. It is input as a value between 0 and 1. The weight of Control Sensor 2 is determined by subtracting this weight from 1. The default for this field is 1, indicating that only Control Sensor 1 is used.
+
+\paragraph{Field: Control Sensor 2 Height in Stratified Tank}\label{field-control-sensor-2-height-in-stratified-tank}
+
+This alpha field defines the optional second location where the tank temperature is sensed for heat pump control when the tank type is \lstinline!WaterHeater:Stratified!. If omitted, this defaults to the height of Heater2.
+
+Following is an example input for the \lstinline!WaterHeater:HeatPump:PumpedCondenser! compound object and the other required component objects that it references.
+
+\begin{lstlisting}
+
+WaterHeater:HeatPump:PumpedCondenser,
+      PlantHeatPumpWaterHeater,!- Name
+      PlantHPWHSch,            !- Availability Schedule Name
+      PlantHPWHTempSch,        !- Compressor Setpoint Temperature Schedule Name
+      2.0,                     !- Dead Band Temperature Difference {deltaC}
+      HPPlantWaterInletNode,   !- Condenser Water Inlet Node Name
+      HPPlantWaterOutletNode,  !- Condenser Water Outlet Node Name
+      0.00115525,              !- Condenser Water Flow Rate {m3/s}
+      1.00695,                 !- Evaporator Air Flow Rate {m3/s}
+      OutdoorAirOnly,          !- Inlet Air Configuration
+      ,                        !- Air Inlet Node Name
+      ,                        !- Air Outlet Node Name
+      HPPlantAirInletNode,     !- Outdoor Air Node Name
+      HPPlantAirOutletNode,    !- Exhaust Air Node Name
+      ,                        !- Inlet Air Temperature Schedule Name
+      ,                        !- Inlet Air Humidity Schedule Name
+      ,                        !- Inlet Air Zone Name
+      WaterHeater:Mixed,       !- Tank Object Type
+      HPWHPlantTank,           !- Tank Name
+      HPWH Use Inlet Node,     !- Tank Use Side Inlet Node Name
+      HPWH Use Outlet Node,    !- Tank Use Side Outlet Node Name
+      Coil:WaterHeating:AirToWaterHeatPump:Pumped,  !- DX Coil Object Type
+      HPWHPlantDXCoil,         !- DX Coil Name
+      11.0,                    !- Minimum Inlet Air Temperature for Compressor Operation {C}
+      Outdoors,                !- Compressor Location
+      ,                        !- Compressor Ambient Temperature Schedule Name
+      Fan:OnOff,               !- Fan Object Type
+      HPWHPlantFan,            !- Fan Name
+      BlowThrough,             !- Fan Placement
+      ,                        !- On Cycle Parasitic Electric Load {W}
+      ,                        !- Off Cycle Parasitic Electric Load {W}
+      ;                        !- Parasitic Heat Rejection Location
+\end{lstlisting}
+
+NOTE: branch object required only when tank use inlet nodes are used.
+
+\begin{lstlisting}
+
+  Branch,
+      Central HPWH Branch,     !- Name
+      0,                       !- Maximum Flow Rate {m3/s}
+      ,                        !- Pressure Drop Curve Name
+      WaterHeater:HeatPump:PumpedCondenser,    !- Component 1 Object Type
+      PlantHeatPumpWaterHeater,!- Component 1 Name
+      HPWH Use Inlet Node,     !- Component 1 Inlet Node Name
+      HPWH Use Outlet Node,    !- Component 1 Outlet Node Name
+      PASSIVE;                 !- Component 1 Branch Control Type
+
+
+
+
+    WaterHeater:Mixed,
+      HPWHPlantTank,           !- Name
+      0.757,                   !- Tank Volume {m3}
+      Plant Hot Water Setpoint Temp Schedule,  !- Setpoint Temperature Schedule Name
+      2.0,                     !- Deadband Temperature Difference {deltaC}
+      82.2222,                 !- Maximum Temperature Limit {C}
+      CYCLE,                   !- Heater Control Type
+      25000,                   !- Heater Maximum Capacity {W}
+      0,                       !- Heater Minimum Capacity {W}
+      ,                        !- Heater Ignition Minimum Flow Rate {m3/s}
+      ,                        !- Heater Ignition Delay {s}
+      ELECTRICITY,             !- Heater Fuel Type
+      0.98,                    !- Heater Thermal Efficiency
+      ,                        !- Part Load Factor Curve Name
+      10,                      !- Off Cycle Parasitic Fuel Consumption Rate {W}
+      ELECTRICITY,             !- Off Cycle Parasitic Fuel Type
+      0,                       !- Off Cycle Parasitic Heat Fraction to Tank
+      30,                      !- On Cycle Parasitic Fuel Consumption Rate {W}
+      ELECTRICITY,             !- On Cycle Parasitic Fuel Type
+      0,                       !- On Cycle Parasitic Heat Fraction to Tank
+      Outdoors,                !- Ambient Temperature Indicator
+      ,                        !- Ambient Temperature Schedule Name
+      ,                        !- Ambient Temperature Zone Name
+      HPWHPlantTank OA Node,   !- Ambient Temperature Outdoor Air Node Name
+      0.0,                     !- Off Cycle Loss Coefficient to Ambient Temperature {W/K}
+      0.0,                     !- Off Cycle Loss Fraction to Zone
+      0.0,                     !- On Cycle Loss Coefficient to Ambient Temperature {W/K}
+      0.0,                     !- On Cycle Loss Fraction to Zone
+      ,                        !- Peak Use Flow Rate {m3/s}
+      ,                        !- Use Flow Rate Fraction Schedule Name
+      ,                        !- Cold Water Supply Temperature Schedule Name
+      HPWH Use Inlet Node,     !- Use Side Inlet Node Name
+      HPWH Use Outlet Node,    !- Use Side Outlet Node Name
+      0.98,                    !- Use Side Effectiveness
+      HPPlantWaterOutletNode,  !- Source Side Inlet Node Name
+      HPPlantWaterInletNode,   !- Source Side Outlet Node Name
+      0.98,                    !- Source Side Effectiveness
+      autosize;                !- Use Side Design Flow Rate {m3/s}
+
+
+    OutdoorAir:Node,
+      HPWHPlantTank OA Node;   !- Name
+
+
+    Coil:WaterHeating:AirToWaterHeatPump:Pumped,
+      HPWHPlantDXCoil,         !- Name
+      25000.0,                 !- Rated Heating Capacity {W}
+      3.2,                     !- Rated COP {W/W}
+      0.736,                   !- Rated Sensible Heat Ratio
+      29.44,                   !- Rated Evaporator Inlet Air Dry-Bulb Temperature {C}
+      22.22,                   !- Rated Evaporator Inlet Air Wet-Bulb Temperature {C}
+      55.72,                   !- Rated Condenser Inlet Water Temperature {C}
+      1.00695,                 !- Rated Evaporator Air Flow Rate {m3/s}
+      0.00115525,              !- Rated Condenser Water Flow Rate {m3/s}
+      No,                      !- Evaporator Fan Power Included in Rated COP
+      No,                      !- Condenser Pump Power Included in Rated COP
+      No,                      !- Condenser Pump Heat Included in Rated Heating Capacity and Rated COP
+      150.0,                   !- Condenser Water Pump Power {W}
+      0.1,                     !- Fraction of Condenser Pump Heat to Water
+      HPPlantFanAirOutletNode, !- Evaporator Air Inlet Node Name
+      HPPlantAirOutletNode,    !- Evaporator Air Outlet Node Name
+      HPPlantWaterInletNode,   !- Condenser Water Inlet Node Name
+      HPPlantWaterOutletNode,  !- Condenser Water Outlet Node Name
+      100.0,                   !- Crankcase Heater Capacity {W}
+      5.0,                     !- Maximum Ambient Temperature for Crankcase Heater Operation {C}
+      WetBulbTemperature,      !- Evaporator Air Temperature Type for Curve Objects
+      HPWHHeatingCapFTemp,     !- Heating Capacity Function of Temperature Curve Name
+      ,                        !- Heating Capacity Function of Air Flow Fraction Curve Name
+      ,                        !- Heating Capacity Function of Water Flow Fraction Curve Name
+      HPWHHeatingCOPFTemp,     !- Heating COP Function of Temperature Curve Name
+      ,                        !- Heating COP Function of Air Flow Fraction Curve Name
+      ,                        !- Heating COP Function of Water Flow Fraction Curve Name
+      HPWHPLFFPLR;             !- Part Load Fraction Correlation Curve Name
+
+
+    Fan:OnOff,
+      HPWHPlantFan,            !- Name
+      PlantHPWHSch,            !- Availability Schedule Name
+      0.7,                     !- Fan Total Efficiency
+      100.0,                   !- Pressure Rise {Pa}
+      2.6852,                  !- Maximum Flow Rate {m3/s}
+      0.9,                     !- Motor Efficiency
+      1.0,                     !- Motor In Airstream Fraction
+      HPPlantAirInletNode,     !- Air Inlet Node Name
+      HPPlantFanAirOutletNode; !- Air Outlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-025}
+
+\begin{itemize}
+\item
+  \textbf{HVAC,Average,Water Heater Compressor Part Load Ratio}
+\item
+  \textbf{HVAC,Average,Water Heater On Cycle Ancillary Electric Power {[}W{]}}
+\item
+  \textbf{HVAC,Sum,Water Heater On Cycle Ancillary Electric Energy {[}J{]}}
+\item
+  \textbf{HVAC,Average,Water Heater Off Cycle Ancillary Electric Power {[}W{]}}
+\item
+  \textbf{HVAC,Sum,Water Heater Off Cycle Ancillary Electric Energy {[}J{]}}
+\end{itemize}
+
+\paragraph{Water Heater Compressor Part Load Ratio}\label{water-heater-compressor-part-load-ratio}
+
+This output is the average part-load ratio of the heat pump water heater's compressor (as well as its water pump and fan) for the timestep being reported. This output is independent of the ``Water Heater Part Load Ratio'' (Ref. Water Heater Outputs) which represents the part-load ratio of the supplemental heater (element or burner) in the water tank. When the water tank's (supplemental) heater set point temperature is higher than the cut-in temperature of the heat pump water heater's compressor, the heat pump compressor is disabled and the water tank's heater (element or burner) is used to heat the water. During these times the Water Heater Compressor Part Load Ratio is equal to 0.
+
+\paragraph{Water Heater On Cycle Ancillary Electric Power {[}W{]}}\label{water-heater-on-cycle-ancillary-electric-power-w}
+
+\paragraph{Water Heater On Cycle Ancillary Electric Energy {[}J{]}}\label{water-heater-on-cycle-ancillary-electric-energy-j}
+
+\paragraph{Water Heater Off Cycle Ancillary Electric Power {[}W{]}}\label{water-heater-off-cycle-ancillary-electric-power-w}
+
+\paragraph{Water Heater Off Cycle Ancillary Electric Energy {[}J{]}}\label{water-heater-off-cycle-ancillary-electric-energy-j}
+
+These outputs are the parasitic electric power and consumption associated with the heat pump water heater. Specific outputs represent parasitic electrical usage during the compressor/fan on and off cycles. These outputs represent electronic controls or other electric component. The model assumes that the parasitic power does not contribute to heating the water, but it can impact the zone air heat balance depending on user inputs. The parasitic electric consumption outputs are also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
+
+\subsection{WaterHeater:HeatPump:WrappedCondenser}\label{waterheaterheatpumpwrappedcondenser}
+
+The heat pump water heater with wrapped condenser is a compound object very similar to the \lstinline!WaterHeater:HeatPump:PumpedCondenser! object. It likewise combines a water heater tank, a direct expansion (DX) ``coil'', and a fan to provide air flow across the air coil associated with the DX compression system. The primary difference is that instead of pumping water through an external condenser, the heating coils are wrapped around or submerged in the tank. This type of HPWH is most common in packaged units meant for residential applications.
+
+To model a wrapped condenser heat pump water, the input data file must include some combination of the following objects depending on the configuration to be modeled:
+
+\begin{itemize}
+\item
+  \lstinline!WaterHeater:HeatPump:WrappedCondenser! (required)
+\item
+  \lstinline!WaterHeater:Stratified! (required)
+\item
+  \lstinline!Coil:WaterHeating:AirToWaterHeatPump:Wrapped! (required)
+\item
+  \lstinline!Fan:OnOff! (required)
+\item
+  \lstinline!ZoneHVAC:EquipmentList! (when the HPWH draws some or all of its air from the zone, the heat pump water heater type and name must be in this list)
+\item
+  \lstinline!ZoneHVAC:EquipmentConnections! (when the HPWH draws some or all of its air from the zone, the HPWH air inlet and outlet node names must be provided in this object)
+\item
+  \lstinline!OutdoorAir:NodeList! (for HPWHs that use outdoor air as all or part of the heat source, the HPWH outdoor air node name must be provided in this list)
+\end{itemize}
+
+The input fields for the compound object are described in detail below:
+
+\subsubsection{Inputs}\label{inputs-4-037}
+
+\paragraph{Field: Name}\label{field-name-3-036}
+
+This alpha field contains a unique user-assigned name for an instance of a heat pump water heater. Any reference to this heat pump water heater by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-014}
+
+This alpha field contains the name of the schedule (ref: Schedule) that denotes whether the heat pump compressor is available to operate during a given time period. A schedule value equal to 0 denotes that the heat pump compressor is off for that time period. A value other than 0 denotes that the heat pump compressor is available to operate during that time period. During times when the heat pump compressor is scheduled off, the heater (element or burner) in the water tank object operates based on its tank set point temperature schedule and the heat pump's parasitic electric power is also off for that time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Compressor Setpoint Temperature Schedule Name}\label{field-compressor-setpoint-temperature-schedule-name-1}
+
+This alpha field contains the name of the schedule (ref: Schedule) that specifies the set point (or ``cut-out'') temperature for the heat pump compressor. Temperature values used in this schedule should be in degrees Celsius. The heat pump compressor cycles off when the tank water reaches this set point temperature. Once the heat pump compressor cycles off, the tank water temperature floats downward until it falls below the set point temperature minus the dead band temperature difference defined below (i.e., the ``cut-in'' temperature). At this point, the heat pump compressor cycles on and remains on until the heat pump compressor set point temperature is reached.
+
+\paragraph{Field: Dead Band Temperature Difference}\label{field-dead-band-temperature-difference-1}
+
+This numeric field contains the dead band temperature difference in degrees Celsius. The heat pump compressor ``cut-in'' temperature is defined as the compressor set point temperature defined above minus this dead band temperature difference. The heat pump compressor cycles on when the water temperature in the tank falls below the ``cut-in'' temperature. The heat pump compressor remains on until the water temperature in the tank rises above the compressor set point (``cut-out'') temperature defined above. The dead band temperature difference must be greater than 0°C and less than or equal to 20°C. If this field is left blank, the default value is 5°C.
+
+In this model, the heat pump water heater's DX compression system is considered the primary heat source and the water tank's heater (element or burner) provides supplemental heat as necessary. Therefore, the cut-in temperature for the heat pump compressor (set point minus dead band temperature difference) is usually higher than the set point temperature for the heater (element or burner) in the associated water heater tank object. At times when the water heater tank set point temperature is greater than the cut-in temperature of the heat pump compressor, the heat pump compressor is disabled and the tank's heater is used to heat the water.
+
+\paragraph{Field: Condenser Bottom Location}\label{field-condenser-bottom-location}
+
+This numeric field contains the distance from the bottom of the tank to the bottom of the wrapped condenser.
+
+\paragraph{Field: Condenser Top Location}\label{field-condenser-top-location}
+
+This numeric field contains the distance from the bottom of the tank to the top of the wrapped condenser.
+
+\paragraph{Field: Evaporator Air Flow Rate}\label{field-evaporator-air-flow-rate-1}
+
+This numeric field contains the air flow rate across the heat pump's air coil (evaporator) in cubic meters per second. It is the actual air flow rate to be simulated, which may differ from the rated evaporator air volumetric flow rate specified for the heat pump's DX coil (Ref. Coil:WaterHeating:AirToWaterHeatPump:Wrapped). Values must be greater than 0 or this field is autocalculatable. If autocalculated (field value = \textbf{autocalculate}), the evaporator air flow rate is set equal to the rated heating capacity of the heat pump's DX coil multiplied by 5.035E-5 m\(^{3}\)/s/W. When this flow rate is different from the Rated Evaporator Air Volumetric Flow Rate specified in the heat pump's DX coil object (Ref. Coil:WaterHeating:AirToWaterHeatPump:Wrapped), the user should also specify a Total Heating Capacity Modifier Curve Name (function of air flow fraction) and a Heating COP Modifier Curve Name (function of air flow fraction) in the associated DX coil object to account for differences in capacity and power consumption at the off-rated air flow rate.
+
+\paragraph{Field: Inlet Air Configuration}\label{field-inlet-air-configuration-1}
+
+This choice field defines the configuration of the air flow path through the heat pump air coil (evaporator) and fan section. Valid entries are \textbf{Schedule}, \textbf{ZoneAirOnly}, \textbf{OutdoorAirOnly}, or \textbf{ZoneAndOutdoorAir}. If `Schedule' is selected, names for an inlet air temperature schedule and an inlet air humidity schedule must be defined in the fields below. If `ZoneAirOnly' is selected, the corresponding zone name must be entered in the Inlet Air Zone Name field below. If `ZoneAndOutdoorAir' is selected, the corresponding Inlet Air Zone Name, Inlet Air Mixer Node Name, Outlet Air Splitter Node Name, and an Inlet Air Mixer Schedule Name must be entered in the corresponding fields below.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-1-006}
+
+This alpha field contains the name of the node from which the heat pump water heater draws its inlet air. If the Inlet Air Configuration field defined above is set to `ZoneAirOnly' or `ZoneAndOutdoorAir', then this node name should be the name of a zone air exhaust node (Ref. ZoneHVAC:EquipmentConnections). If the Inlet Air Configuration field is set to `OutdoorAirOnly', this node name should be left blank. If the Inlet Air Configuration field is set to `Schedule', this node name should simply be a unique name that allows the user to receive output on conditions at this node for verification purposes.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-1-005}
+
+This alpha field contains the name of the node to which the heat pump water heater sends its outlet air. If the Inlet Air Configuration field defined above is set to `ZoneAirOnly' or `ZoneAndOutdoorAir', then this node name should be the name of a zone air inlet node (Ref. ZoneHVAC:EquipmentConnections). If the Inlet Air Configuration field is set to `OutdoorAirOnly', this node name should be left blank. If the Inlet Air Configuration field is set to `Schedule', this node name should simply be a unique name that allows the user to receive output on conditions at this node for verification purposes.
+
+\paragraph{Field: Outdoor Air Node Name}\label{field-outdoor-air-node-name-1}
+
+This alpha field contains the name of the node from which the heat pump water heater draws its outdoor air. If the Inlet Air Configuration field defined above is set to `ZoneAirOnly' or `Schedule', this node name should be left blank. If the Inlet Air Configuration field is set to `ZoneAndOutdoorAir' or `OutdoorAirOnly', this node name should be the name of an outdoor air node (Ref. OutdoorAir:NodeList).
+
+\paragraph{Field: Exhaust Air Node Name}\label{field-exhaust-air-node-name-1}
+
+This alpha field contains the name of the node to which the heat pump water heater sends its exhaust air. If the Inlet Air Configuration field defined above is set to `ZoneAirOnly' or `Schedule', this node name should be left blank. If the Inlet Air Configuration field is set to `ZoneAndOutdoorAir' or `OutdoorAirOnly', then this node name should be a unique name that allows the user to receive output on conditions at this node for verification purposes.
+
+\paragraph{Field: Inlet Air Temperature Schedule Name}\label{field-inlet-air-temperature-schedule-name-1}
+
+This alpha field contains the name of a schedule used to define the dry-bulb temperature of the inlet air to the heat pump air coil (evaporator) and fan section. Schedule values should be in degrees Celsius. This field is only used when the Inlet Air Configuration defined above is specified as `Schedule', otherwise leave this field blank.
+
+\paragraph{Field: Inlet Air Humidity Schedule Name}\label{field-inlet-air-humidity-schedule-name-1}
+
+This alpha field contains the name of a schedule used to define the humidity of the inlet air to the heat pump evaporator and fan section. Schedule values must be entered as relative humidity fraction from 0 to 1 (e.g., a schedule value of 0.5 means 50\%RH). This field is only used when the Inlet Air Configuration defined above is specified as `Schedule', otherwise leave this field blank.
+
+\paragraph{Field: Inlet Air Zone Name}\label{field-inlet-air-zone-name-1}
+
+This alpha field contains the name of the zone from which the heat pump evaporator and fan section draws some or all of its inlet air. This field is only used when the Inlet Air Configuration defined above is specified as `ZoneAirOnly' or `ZoneAndOutdoorAir'.
+
+\paragraph{Field: Tank Object Type}\label{field-tank-object-type-1}
+
+This alpha (choice) field contains the type of water heater tank used by this heat pump water heater. Currently, the only valid choice is WaterHeater:Stratified.
+
+\paragraph{Field: Tank Name}\label{field-tank-name-1}
+
+This alpha field contains the name of the specific water heater tank used by this heat pump water heater. This must be a tank of type \lstinline!WaterHeater:Stratified!.
+
+\paragraph{Field: Tank Use Side Inlet Node Name}\label{field-tank-use-side-inlet-node-name-1}
+
+This alpha field contains the name of the use side inlet node of the water heater tank used by this heat pump water heater. This name must match the Use Side Inlet Node Name in the water heater tank object (Ref. \lstinline!WaterHeater:Stratified!). This field is required if the water heater tank use side nodes are connected to a plant loop, otherwise leave this field blank. When used, the branch object should reflect that this node is part of a \lstinline!WaterHeater:HeatPump:WrappedCondenser! object (see branch object example below).
+
+\paragraph{Field: Tank Use Side Outlet Node Name}\label{field-tank-use-side-outlet-node-name-1}
+
+This alpha field contains the name of the use side outlet node of the water heater tank used by this heat pump water heater. This name must match the Use Side Outlet Node Name in the water heater tank object (Ref. \lstinline!WaterHeater:Stratified!). This field is required if the water heater tank use side nodes are connected to a plant loop, otherwise leave this field blank. When used, the branch object should reflect that this node is part of a \lstinline!WaterHeater:HeatPump:WrappedCondenser! object (see branch object example below).
+
+\paragraph{Field: DX Coil Object Type}\label{field-dx-coil-object-type-1}
+
+This alpha (choice) field contains the type of DX coil used by this heat pump water heater. Currently, the only valid choice is Coil:WaterHeating:AirToWaterHeatPump:Wrapped.
+
+\paragraph{Field: DX Coil Name}\label{field-dx-coil-name-1}
+
+This alpha field contains the name of the specific DX coil (\lstinline!Coil:WaterHeating:AirToWaterHeatPump:Wrapped!) used by this heat pump water heater.
+
+\paragraph{Field: Minimum Inlet Air Temperature for Compressor Operation}\label{field-minimum-inlet-air-temperature-for-compressor-operation-1}
+
+This numeric field contains the minimum inlet air dry-bulb temperature entering the air coil (evaporator) and fan section, in degrees Celsius, below which the heat pump compressor does not operate. The minimum inlet air dry-bulb temperature should be greater than or equal to -5°C. If this field is left blank, the default value is 10°C.
+
+\paragraph{Field: Compressor Location}\label{field-compressor-location-1}
+
+This alpha (choice) field contains the location of the heat pump compressor and the air temperature for this location is used to control operation of the compressor's crankcase heater in the Coil:WaterHeating:AirToWaterHeatPump:Wrapped object. Valid entries are \textbf{Schedule}, \textbf{Zone}, or \textbf{Outdoors}. If `Schedule' is selected, a compressor ambient temperature schedule name must be defined in the field below; otherwise, the field below should be left blank. If `Zone' is selected, the crankcase heater operation is controlled based on the air temperature in the zone defined in the field Inlet Air Zone Name, and the Inlet Air Configuration must be `ZoneAirOnly' or `ZoneAndOutdoorAir'. If `Outdoors' is selected, crankcase heater operation is controlled based on the outdoor air temperature.
+
+\paragraph{Field: Compressor Ambient Temperature Schedule Name}\label{field-compressor-ambient-temperature-schedule-name-1}
+
+This alpha field contains the name of a schedule that defines the ambient air temperature surrounding the heat pump compressor, which is used to control the compressor's crankcase heater operation. This field is only used when the compressor location field defined above is specified as `Schedule', otherwise it should be left blank.
+
+\paragraph{Field: Fan Object Type}\label{field-fan-object-type-1}
+
+This alpha (choice) field contains the type of fan used by this heat pump water heater. Currently, the only valid choice is Fan: OnOff.
+
+\paragraph{Field: Fan Name}\label{field-fan-name-1-000}
+
+This alpha field contains the name of the specific fan (\lstinline!Fan:OnOff! object) used by this heat pump water heater.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-1-000}
+
+This alpha (choice) field defines the placement of the fan in the heat pump water heater. Valid choices are \textbf{BlowThrough} (fan upstream of the air coil) and \textbf{DrawThrough} (fan downstream of the air coil). If this field is left blank, the default value is DrawThrough.
+
+\paragraph{Field: On Cycle Parasitic Electric Load}\label{field-on-cycle-parasitic-electric-load-1}
+
+This numeric field contains the on-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the heat pump water heater. This parasitic electric load is consumed whenever the heat pump compressor is operating and the model assumes that this parasitic power does not contribute to heating the water. This parasitic load does, however, affect the zone air heat balance when the heat pump water heater sends some or all of its outlet air to a zone (i.e., Inlet Air Configuration field specified as `ZoneAirOnly' or `ZoneAndOutdoorAir') and the Parasitic Heat Rejection Location field is specified as `Zone'. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
+
+\paragraph{Field: Off Cycle Parasitic Electric Load}\label{field-off-cycle-parasitic-electric-load-1}
+
+This numeric field contains the off-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the heat pump compressor. This parasitic electric load is consumed whenever the heat pump water heater is available but the compressor is not operating, and the model assumes that this parasitic power does not contribute to heating the water. This parasitic load does, however, affect the zone air heat balance when the heat pump water heater sends some or all of its outlet air to a zone (i.e., Inlet Air Configuration field specified as `ZoneAirOnly' or `ZoneAndOutdoorAir') and the Parasitic Heat Rejection Location field is specified as `Zone'. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
+
+\paragraph{Field: Parasitic Heat Rejection Location}\label{field-parasitic-heat-rejection-location-1}
+
+This alpha (choice) field determines where the on-cycle and off-cycle parasitic heat is rejected. Valid choices are Zone and Exterior. If `Zone' is selected, both the on-cycle and off-cycle parasitic heat is rejected to the zone defined in the field Inlet Air Zone Name, and the Inlet Air Configuration must be `ZoneAirOnly' or `ZoneAndOutdoorAir. If 'Outdoors' is selected, this parasitic heat is rejected outdoors (does not impact the zone air heat balance) regardless of the specified Inlet Air Configuration. If this field is left blank, the default value is 'Outdoors'.
+
+\paragraph{Field: Inlet Air Mixer Node Name}\label{field-inlet-air-mixer-node-name-1}
+
+This optional alpha field defines the name of the HVAC node which represents the mixture of outdoor air and zone air that enters the heat pump air coil (evaporator) and fan section. The model mixes outdoor air with zone air and places the result on this inlet air mixer node based on the Inlet Air Mixer Schedule defined below. When the schedule value is equal to 0, 100\% zone air enters the evaporator coil and fan section of the heat pump water heater. When the schedule value is equal to 1, 100\% outdoor air enters the evaporator coil and fan section. This node name must be provided if the Inlet Air Configuration field above is specified as `ZoneAndOutdoor Air', otherwise this field should be left blank.
+
+\paragraph{Field: Outlet Air Splitter Node Name}\label{field-outlet-air-splitter-node-name-1}
+
+This alpha field defines the name of the air node to which the heat pump air coil (evaporator) and fan sends all of its outlet air. The supply air flow downstream of this node is split between the zone and outdoors based on the Inlet Air Mixer schedule defined below. When the schedule value is equal to 0, the entire outlet air stream is diverted to the zone. When the schedule value is equal to 1, the entire outlet air stream is exhausted to outdoors. This node name must be provided if the Inlet Air Configuration field above is specified as `Zone and Outdoor Air', otherwise this field should be left blank.
+
+\paragraph{Field: Inlet Air Mixer Schedule Name}\label{field-inlet-air-mixer-schedule-name-1}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump draws its inlet air from the zone, outdoors, or a combination of zone and outdoor air. A schedule value equal to 0 indicates that the heat pump draws its inlet air from the zone. A schedule value equal to 1 denotes that the heat pump draws its inlet air from outdoors. Values between 0 and 1 denote a mixture of zone and outdoor air proportional to the schedule value. The Inlet Air Mixer schedule controls both the inlet air mixer and outlet air splitter nodes in unison to ensure that the operation of the heat pump does not contribute to zone pressurization or depressurization. For example if the Inlet Air Mixer schedule value is 0.4, then the inlet air mixer node is composed of 40\% outdoor air and 60\% zone air. For this same case, the outlet air splitter directs 60\% of the HPWH outlet air back to the zone and 40\% of the outlet air flow is exhausted outdoors. This schedule name must be provided if the Inlet Air Configuration field is specified as `Zone and Outdoor Air', otherwise this field should be left blank.
+
+\paragraph{Field: Tank Element Control Logic}\label{field-tank-element-control-logic-1}
+
+This alpha field defines settings for the control logic of when to run the tank element in relation to whether the heat pump is running.
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{MutuallyExclusive} means that once the tank heating element(s) are active, the heat pump is shut down until the heating element setpoint is reached.
+\item
+  \textbf{Simultaneous} (default) means that both the tank heating element and heat pump are used at the same time to recover the tank temperature.
+\end{itemize}
+
+\paragraph{Field: Control Sensor 1 Height In Stratified Tank}\label{field-control-sensor-1-height-in-stratified-tank-1}
+
+This alpha field defines where the tank temperature is sensed for heat pump control when the tank type is \lstinline!WaterHeater:Stratified!.~ The stratified tank model produces tank temperature at different nodes in the vertical direction and various options are available for how this temperature should be sensed to control the heat pump.~ This is measured in height from the bottom of the tank. Internally the appropriate node is determined based on this height. If omitted, this defaults to the height of Heater1.
+
+\paragraph{Field: Control Sensor 1 Weight}\label{field-control-sensor-1-weight-1}
+
+The model can optionally use two control sensor locations in stratified tanks. When that is the case, the temperature sensed at each location is weighted. This alpha input specifies the weight associated with Control Sensor 1. It is input as a value between 0 and 1. The weight of Control Sensor 2 is determined by subtracting this weight from 1. The default for this field is 1, indicating that only Control Sensor 1 is used.
+
+\paragraph{Field: Control Sensor 2 Height in Stratified Tank}\label{field-control-sensor-2-height-in-stratified-tank-1}
+
+This alpha field defines the optional second location where the tank temperature is sensed for heat pump control when the tank type is \lstinline!WaterHeater:Stratified!. If omitted, this defaults to the height of Heater2.
+
+Following is an example input for the \lstinline!WaterHeater:HeatPump:WrappedCondenser! compound object and the other required component objects that it references.
+
+\begin{lstlisting}
+
+WaterHeater:HeatPump:WrappedCondenser,
+  PlantHeatPumpWaterHeater,!- Name
+  PlantHPWHSch,            !- Availability Schedule Name
+  PlantHPWHTempSch,        !- Compressor Setpoint Temperature Schedule Name
+  3.89,                    !- Dead Band Temperature Difference {deltaC}
+  0.0664166667,            !- Condenser Bottom Location
+  0.8634166667,            !- Condenser Top Location
+  0.2279,                  !- Evaporator Air Flow Rate {m3/s}
+  OutdoorAirOnly,          !- Inlet Air Configuration
+  ,                        !- Air Inlet Node Name
+  ,                        !- Air Outlet Node Name
+  HPPlantAirInletNode,     !- Outdoor Air Node Name
+  HPPlantAirOutletNode,    !- Exhaust Air Node Name
+  ,                        !- Inlet Air Temperature Schedule Name
+  ,                        !- Inlet Air Humidity Schedule Name
+  ,                        !- Inlet Air Zone Name
+  WaterHeater:Stratified,  !- Tank Object Type
+  HPWHPlantTank,           !- Tank Name
+  HPWH Use Inlet Node,     !- Tank Use Side Inlet Node Name
+  HPWH Use Outlet Node,    !- Tank Use Side Outlet Node Name
+  Coil:WaterHeating:AirToWaterHeatPump:Wrapped,  !- DX Coil Object Type
+  HPWHPlantDXCoil,         !- DX Coil Name
+  7.2,                     !- Minimum Inlet Air Temperature for Compressor Operation {C}
+  Outdoors,                !- Compressor Location
+  ,                        !- Compressor Ambient Temperature Schedule Name
+  Fan:OnOff,               !- Fan Object Type
+  HPWHPlantFan,            !- Fan Name
+  DrawThrough,             !- Fan Placement
+  0,                       !- On Cycle Parasitic Electric Load {W}
+  0,                       !- Off Cycle Parasitic Electric Load {W}
+  ,                        !- Parasitic Heat Rejection Location
+  ,                        !- Inlet Air Mixer Node Name
+  ,                        !- Outlet Air Splitter Node Name
+  ,                        !- Inlet Air Mixer Schedule Name
+  MutuallyExclusive,       !- Tank Element Control Logic
+  1.262,                   !- Control Sensor 1 Height In Stratified Tank
+  0.75,                    !- Control Sensor 1 Weight
+  0.464;                   !- Control Sensor 2 Height In Stratified Tank
+\end{lstlisting}
+
+NOTE: branch object required only when tank use inlet nodes are used.
+
+\begin{lstlisting}
+
+Branch,
+      Central HPWH Branch,     !- Name
+      0,                       !- Maximum Flow Rate {m3/s}
+      ,                        !- Pressure Drop Curve Name
+      WaterHeater:HeatPump:WrappedCondenser,    !- Component 1 Object Type
+      PlantHeatPumpWaterHeater,!- Component 1 Name
+      HPWH Use Inlet Node,     !- Component 1 Inlet Node Name
+      HPWH Use Outlet Node,    !- Component 1 Outlet Node Name
+      PASSIVE;                 !- Component 1 Branch Control Type
+
+  WaterHeater:Stratified,
+  HPWHPlantTank,           !- Name
+  Water Heater,            !- End-Use Subcategory
+  0.287691,                !- Tank Volume {m3}
+  1.594,                   !- Tank Height {m}
+  VerticalCylinder,        !- Tank Shape
+  ,                        !- Tank Perimeter {m}
+  100,                     !- Maximum Temperature Limit {C}
+  MasterSlave,             !- Heater Priority Control
+  Plant Hot Water Setpoint Temp Schedule,  !- Heater 1 Setpoint Temperature Schedule Name
+  18.5,                      !- Heater 1 Deadband Temperature Difference {deltaC}
+  4500,                    !- Heater 1 Capacity {W}
+  1.129,                   !- Heater 1 Height {m}
+  Plant Hot Water Setpoint Temp Schedule,  !- Heater 2 Setpoint Temperature Schedule Name
+  18.5,                      !- Heater 2 Deadband Temperature Difference {deltaC}
+  0,                    !- Heater 2 Capacity {W}
+  0.266,                   !- Heater 2 Height {m}
+  Electricity,             !- Heater Fuel Type
+  1,                       !- Heater Thermal Efficiency
+  8.3,                     !- Off Cycle Parasitic Fuel Consumption Rate {W}
+  Electricity,             !- Off Cycle Parasitic Fuel Type
+  0,                       !- Off Cycle Parasitic Heat Fraction to Tank
+  1,                       !- Off Cycle Parasitic Height {m}
+  8.3,                     !- On Cycle Parasitic Fuel Consumption Rate {W}
+  Electricity,             !- On Cycle Parasitic Fuel Type
+  0,                       !- On Cycle Parasitic Heat Fraction to Tank
+  1,                       !- On Cycle Parasitic Height {m}
+  Outdoors,                !- Ambient Temperature Indicator
+  ,                        !- Ambient Temperature Schedule Name
+  ,                        !- Ambient Temperature Zone Name
+  ,                        !- Ambient Temperature Outdoor Air Node Name
+  0.7878,                  !- Uniform Skin Loss Coefficient per Unit Area to Ambient Temperature {W/m2-K}
+  1,                       !- Skin Loss Fraction to Zone
+  ,                        !- Off Cycle Flue Loss Coefficient to Ambient Temperature {W/K}
+  1,                       !- Off Cycle Flue Loss Fraction to Zone
+  0.001,                   !- Peak Use Flow Rate {m3/s}
+  ,                        !- Use Flow Rate Fraction Schedule Name
+  ,                        !- Cold Water Supply Temperature Schedule Name
+  HPWH Use Inlet Node,     !- Use Side Inlet Node Name
+  HPWH Use Outlet Node,    !- Use Side Outlet Node Name
+  1,                       !- Use Side Effectiveness
+  0,                       !- Use Side Inlet Height {m}
+  autocalculate,           !- Use Side Outlet Height {m}
+  HPPlantWaterOutletNode,  !- Source Side Inlet Node Name
+  HPPlantWaterInletNode,   !- Source Side Outlet Node Name
+  1,                       !- Source Side Effectiveness
+  0.7,                     !- Source Side Inlet Height {m}
+  0,                       !- Source Side Outlet Height {m}
+  Fixed,                   !- Inlet Mode
+  autosize,                !- Use Side Design Flow Rate {m3/s}
+  autosize,                !- Source Side Design Flow Rate {m3/s}
+  1.5,                     !- Indirect Water Heating Recovery Time {hr}
+  12;                      !- Number of Nodes
+
+  OutdoorAir:Node,
+      HPWHPlantTank OA Node;   !- Name
+
+  Coil:WaterHeating:AirToWaterHeatPump:Wrapped,
+  HPWHPlantDXCoil,               !- Name
+  2349.6,                  !- Rated Heating Capacity {W}
+  2.4,                     !- Rated COP {W/W}
+  0.981,                   !- Rated Sensible Heat Ratio
+  19.72,                   !- Rated Evaporator Inlet Air Dry-Bulb Temperature {C}
+  13.5,                    !- Rated Evaporator Inlet Air Wet-Bulb Temperature {C}
+  48.89,                   !- Rated Condenser Water Temperature {C}
+  0.189,                   !- Rated Evaporator Air Flow Rate {m3/s}
+  Yes,                     !- Evaporator Fan Power Included in Rated COP
+  HPPlantFanAirOutletNode, !- Evaporator Air Inlet Node Name
+  HPPlantAirOutletNode,    !- Evaporator Air Outlet Node Name
+  0,                       !- Crankcase Heater Capacity {W}
+  10,                      !- Maximum Ambient Temperature for Crankcase Heater Operation {C}
+  WetBulbTemperature,      !- Evaporator Air Temperature Type for Curve Objects
+  HPWH-Htg-Cap-fT,         !- Heating Capacity Function of Temperature Curve Name
+  ,                        !- Heating Capacity Function of Air Flow Fraction Curve Name
+  HPWH-Htg-COP-fT,         !- Heating COP Function of Temperature Curve Name
+  ,                        !- Heating COP Function of Air Flow Fraction Curve Name
+  HPWH-COP-fPLR;           !- Part Load Fraction Correlation Curve Name
+
+  Fan:OnOff,
+  HPWHPlantFan,            !- Name
+  PlantHPWHSch,            !- Availability Schedule Name
+  0.1722,                  !- Fan Total Efficiency
+  65,                      !- Pressure Rise {Pa}
+  0.2279,                  !- Maximum Flow Rate {m3/s}
+  1,                       !- Motor Efficiency
+  0,                       !- Motor In Airstream Fraction
+  HPPlantAirInletNode,     !- Air Inlet Node Name
+  HPPlantFanAirOutletNode; !- Air Outlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-022}
+
+\begin{itemize}
+\item
+  \textbf{HVAC,Average,Water Heater Compressor Part Load Ratio}
+\item
+  \textbf{HVAC,Average,Water Heater On Cycle Ancillary Electric Power {[}W{]}}
+\item
+  \textbf{HVAC,Sum,Water Heater On Cycle Ancillary Electric Energy {[}J{]}}
+\item
+  \textbf{HVAC,Average,Water Heater Off Cycle Ancillary Electric Power {[}W{]}}
+\item
+  \textbf{HVAC,Sum,Water Heater Off Cycle Ancillary Electric Energy {[}J{]}}
+\end{itemize}
+
+\paragraph{Water Heater Compressor Part Load Ratio}\label{water-heater-compressor-part-load-ratio-1}
+
+This output is the average part-load ratio of the heat pump water heater's compressor (as well as its water pump and fan) for the timestep being reported. This output is independent of the ``Water Heater Part Load Ratio'' (Ref. Water Heater Outputs) which represents the part-load ratio of the supplemental heater (element or burner) in the water tank. When the water tank's (supplemental) heater set point temperature is higher than the cut-in temperature of the heat pump water heater's compressor, the heat pump compressor is disabled and the water tank's heater (element or burner) is used to heat the water. During these times the Water Heater Compressor Part Load Ratio is equal to 0.
+
+\paragraph{Water Heater On Cycle Ancillary Electric Power {[}W{]}}\label{water-heater-on-cycle-ancillary-electric-power-w-1}
+
+\paragraph{Water Heater On Cycle Ancillary Electric Energy {[}J{]}}\label{water-heater-on-cycle-ancillary-electric-energy-j-1}
+
+\paragraph{Water Heater Off Cycle Ancillary Electric Power {[}W{]}}\label{water-heater-off-cycle-ancillary-electric-power-w-1}
+
+\paragraph{Water Heater Off Cycle Ancillary Electric Energy {[}J{]}}\label{water-heater-off-cycle-ancillary-electric-energy-j-1}
+
+These outputs are the parasitic electric power and consumption associated with the heat pump water heater. Specific outputs represent parasitic electrical usage during the compressor/fan on and off cycles. These outputs represent electronic controls or other electric component. The model assumes that the parasitic power does not contribute to heating the water, but it can impact the zone air heat balance depending on user inputs. The parasitic electric consumption outputs are also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
diff --git a/doc/input-output-reference/src/overview/group-water-systems.tex b/doc/input-output-reference/src/overview/group-water-systems.tex
new file mode 100644
index 00000000000..08b3a7f6855
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+++ b/doc/input-output-reference/src/overview/group-water-systems.tex
@@ -0,0 +1,867 @@
+\section{Group Water Systems}\label{group-water-systems}
+
+This group of objects is used to describe the water systems in the building. EnergyPlus offers water modeling capabilities than include not only hot water systems but also the overall water systems including cold water uses, on-site water collection (e.g., from rain, condensate, or well), and storage. HVAC components may consume or collect a significant portion of the water making it appropriate to include water modeling in EnergyPlus.
+
+All water systems are collected into an end use category called Water Systems . This category includes hot and cold water. Water consumed by an HVAC component will be assigned to the end use category for that component. End use subcategories are available to separate hot water from cold water if desired. Simple hot water systems can be configured as stand-alone or use a PlantLoop. The Water Systems can be connected to PlantLoops for modeling heated water end uses. However PlantLoops are not used to model cold water and the WaterUse:Storages portions of the water system. Cold water systems are connected together using WaterUse:Storage objects. WaterUse:Connections are used at the zone level to connect to both cold and hot water.
+
+In addition to the input objects described in this section below, there are a variety of HVAC components that can be configured to interact with the water systems. These component input objects include optional fields that allow describing how the water systems are connected to them by providing the name of a storage tank. The following table lists EnergyPlus input objects that include provisions for connecting to the water systems but are described elsewhere in this document:
+
+% table 34
+\begin{longtable}[c]{p{2.49in}p{3.5in}}
+\caption{Water Systems Objects \label{table:water-systems-objects}} \tabularnewline
+\toprule 
+Input Object Name & Type of Water Interactions \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Water Systems Objects} \tabularnewline
+\toprule 
+Input Object Name & Type of Water Interactions \tabularnewline
+\midrule
+\endhead
+
+Site:Precipitation & Describes rainfall for WaterUse:RainCollector \tabularnewline
+Coil:Cooling:Water & Condensate collection to WaterUse:Storage \tabularnewline
+Coil:Cooling:Water:DetailedGeometry & Condensate collection to WaterUse:Storage \tabularnewline
+Coil:Cooling:DX:SingleSpeed & Optional evaporative condenser can be supplied by WaterUse:Storage \tabularnewline
+Condensate collection to WaterUse:Storage \tabularnewline
+Coil:Cooling:DX:TwoSpeed & Evaporative condenser supplied by WaterUse:Storage \tabularnewline
+Condensate collection to WaterUse:Storage \tabularnewline
+Coil:Cooling:DX:TwoStageWithHumidityControlMode & Evaporative condenser supplied by WaterUse:Storage \tabularnewline
+Condensate collection to WaterUse:Storage \tabularnewline
+Coil:Cooling:DX:MultiSpeed & Evaporative condenser supplied by WaterUse:Storage \tabularnewline
+Condensate collection to WaterUse:Storage \tabularnewline
+Humidifier:Steam:Electric & Water supplied by WaterUse:Storage \tabularnewline
+CoolingTower:SingleSpeed & Water supplied by WaterUse:Storage \tabularnewline
+CoolingTower:TwoSpeed & Water supplied by WaterUse:Storage \tabularnewline
+CoolingTower:VariableSpeed & Water supplied by WaterUse:Storage \tabularnewline
+ZoneCoolTower:Shower & Water supplied by WaterUse:Storage \tabularnewline
+Refrigeration:CompressorRack & Water supplied by WaterUse:Storage \tabularnewline
+Refrigeration:Condenser:EvaporativeCooled & Water supplied by WaterUse:Storage \tabularnewline
+EvaporativeCooler:Direct:CelDekPad & Evaporation water supplied by WaterUse:Storage \tabularnewline
+EvaporativeCooler:Indirect:CelDekPad & Evaporation water supplied by WaterUse:Storage \tabularnewline
+EvaporativeCooler:Indirect:WetCoil & Evaporation water supplied by WaterUse:Storage \tabularnewline
+EvaporativeCooler:Indirect:ResearchSpecial & Evaporation water supplied by WaterUse:Storage \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{WaterUse:Equipment}\label{wateruseequipment}
+
+The WaterUse:Equipment object is a generalized object for simulating all water end uses. Hot and cold water uses are included, as well as controlled mixing of hot and cold water at the tap. The WaterUse:Equipment object can be used stand-alone, or coupled into a plant loop using the WaterUse:Connections object (see below). The WaterUse:Connections object allows water uses to be linked to WaterUse:Storage objects to store and draw reclaimed water. The WaterUse:Connections object can also simulate drainwater heat recovery.
+
+The WaterUse:Equipment object serves all of the same purposes as the existing objects: Exterior:WaterEquipment, and HotWaterEquipment.
+
+The WaterUse:Equipment object does a better job of modeling domestic hot water by allowing mixing at the tap in order to account for both hot \textbf{and cold} water used at sinks, showers, etc. It also improves on the stand-alone energy modeling of domestic hot water. Because all of the temperatures and flow rates can be solved, the energy usage can be accounted for as ``Purchased Heating''.
+
+In either stand-alone mode or used with the WaterUse:Connections object, the WaterUse:Equipment object will attempt to meet a scheduled target temperature at the tap by mixing hot and cold water flows. If the hot water flow is not hot enough, or if the flow is limited by plant loop constraints, the result is a cooler mixed water temperature and the target temperature will not be met. In stand-alone mode the hot and cold water temperatures are specified by schedules. However, if the cold water schedule is omitted, the water temperature will be calculated by the Site:WaterMainsTemperature object. If the hot water schedule or target temperature schedule are omitted, all water is delivered as cold water. If only using cold water, the WaterUse:Equipment object is similar to the Exterior:WaterEquipment object.
+
+The WaterUse:Equipment object improves on the internal gains object HotWaterEquipment by associating actual water usage with a sensible and latent gain to a zone. Equipment, such as showers, that generate a significant heat gain can be modeled using the Sensible Fraction Schedule and Latent Fraction Schedule fields. The schedules are used to set the fraction of the maximum possible heat gain (based on inlet water conditions and ambient zone conditions) that should be added to the zone. The split between sensible and latent will vary depending on the type of equipment that is to be modeled. Typically, both fractions should be small numbers.
+
+\subsubsection{Inputs}\label{inputs-053}
+
+\paragraph{Field: Name}\label{field-name-051}
+
+The unique object name for reference by other objects.
+
+\paragraph{Field: End-Use Subcategory}\label{field-end-use-subcategory-005}
+
+Allows you to specify a user-defined end-use subcategory, e.g., ``Laundry'', ``Dish Washing'', etc. A new meter for reporting is created for each unique subcategory (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table under the ``Water Systems'' end-use category. If this field is omitted or blank, the water use will be assigned to the ``General'' end-use subcategory.
+
+\paragraph{Field: Peak Flow Rate}\label{field-peak-flow-rate-000}
+
+The peak demanded hot water flow rate {[}m\(^{3}\)/s{]}. This value is multiplied by the Flow Rate Fraction Schedule (below) to determine the actual volumetric flow rate.
+
+\paragraph{Field: Flow Rate Fraction Schedule Name}\label{field-flow-rate-fraction-schedule-name-000}
+
+Reference to the schedule object specifying the flow rate fraction relative to the Peak Flow Rate (above). If blank, the schedule defaults to 1.0 at all times.
+
+\paragraph{Field: Target Temperature Schedule Name}\label{field-target-temperature-schedule-name}
+
+Reference to the schedule object specifying the target water temperature {[}C{]}. Hot and cold water are mixed at the tap to attain the target temperature. If insufficient hot water is available to reach the target temperature, the result is cooler water at the tap. If blank, the target temperature defaults to the hot water supply temperature.
+
+\paragraph{Field: Hot Water Supply Temperature Schedule Name}\label{field-hot-water-supply-temperature-schedule-name}
+
+Reference to the schedule object specifying the hot water temperature {[}C{]}. The hot water temperature is used to calculate the ``Purchased Heating'' energy usage in stand-alone mode. If blank in stand-alone mode, the hot water supply temperature defaults to the cold water supply temperature. This field is ignored if the object is used with the WaterUse:Connections object.
+
+\paragraph{Field: Cold Water Supply Temperature Schedule Name}\label{field-cold-water-supply-temperature-schedule-name-000}
+
+Reference to the Schedule object specifying the cold water temperature {[}C{]} from the supply mains that provides the cold water to the tap and makes up for all water lost down the drain. If blank, water temperatures are calculated by the Site:WaterMainsTemperature object. This field is ignored if the object is used with the WaterUse:Connections object.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-013}
+
+Reference to the zone name where the water equipment will be considered as latent load to the zone.
+
+\paragraph{Field: Sensible Fraction Schedule Name}\label{field-sensible-fraction-schedule-name}
+
+Reference to the schedule object specifying the fraction of the maximum possible sensible heat gain (based on inlet water conditions and ambient zone conditions) that is added to the zone. If blank, the schedule defaults to 0 at all times.
+
+\paragraph{Field: Latent Fraction Schedule Name}\label{field-latent-fraction-schedule-name}
+
+Reference to the schedule object specifying the fraction of the maximum possible latent heat gain (based on inlet water conditions and ambient zone conditions) that is added to the zone. If blank, the schedule defaults to 0 at all times.
+
+IDF examples:
+
+\begin{lstlisting}
+
+WaterUse:Equipment,
+  Landscaping,   !- Name
+  Landscaping,   !- End-Use Subcategory
+  0.003;               !- Peak Flow Rate {m3/s}
+
+  WaterUse:Equipment,
+  Dishwashing,   !- Name
+  Domestic Hot Water,   !- End-Use Subcategory
+  0.001,   !- Peak Flow Rate {m3/s}
+  Dishwashing Schedule,   !- Flow Rate Fraction Schedule Name
+  Dishwashing Target Temp,   !- Target Temperature Schedule Name
+  Hot Water Temp,   !- Hot Water Supply Temperature Schedule Name
+  Mains Water;   !- Cold Water Supply Temperature Schedule Name
+
+  WaterUse:Equipment,
+  Showers,   !- Name
+  Domestic Hot Water,   !- End-Use Subcategory
+  0.0002,   !- Peak Flow Rate {m3/s}
+  Shower Schedule,   !- Flow Rate Fraction Schedule Name
+  Shower Target Temp,   !- Target Temperature Schedule Name
+  Hot Water Temp,   !- Hot Water Supply Temperature Schedule Name
+  ,   !- Cold Water Supply Temperature Schedule Name
+  Shower Room,   !- Zone Name
+  Sensible Frac Schedule,   !- Sensible Fraction Schedule Name
+  Latent Frac Schedule;   !- Latent Fraction Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-041}
+
+The following output variables are reported for the WaterUse:Equipment object:
+
+\begin{itemize}
+\item
+  HVAC,Average,Water Use Equipment Hot Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water Use Equipment Cold Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water Use Equipment Total Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water Use Equipment Hot Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Water Use Equipment Cold Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Water Use Equipment Total Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Water Use Equipment Hot Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Water Use Equipment Cold Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Water Use Equipment Total Volume {[}m3{]}
+\item
+  HVAC,Sum,Water Use Equipment Mains Water Volume {[}m3{]}
+\item
+  HVAC,Average,Water Use Equipment Hot Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Equipment Cold Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Equipment Target Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Equipment Mixed Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Equipment Drain Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Equipment Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Water Use Equipment Heating Energy {[}J{]}
+\item
+  HVAC,Average,Water Use Equipment Zone Sensible Heat Gain Rate {[}W{]}
+\item
+  HVAC,Sum,Water Use Equipment Zone Sensible Heat Gain Energy {[}J{]}
+\item
+  HVAC,Average,Water Use Equipment Zone Latent Gain Rate {[}W{]}
+\item
+  HVAC,Sum,Water Use Equipment Zone Latent Gain Energy {[}J{]}
+\item
+  HVAC,Average,Water Use Equipment Zone Moisture Gain Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum,Water Use Equipment Zone Moisture Gain Mass {[}kg{]}
+\end{itemize}
+
+\paragraph{Water Use Equipment Hot Water Mass Flow Rate {[}kg/s{]}}\label{water-use-equipment-hot-water-mass-flow-rate-kgs}
+
+The mass flow rate of hot water supplied to the equipment, in units of kilograms per second (kg/s).
+
+\paragraph{Water Use Equipment Cold Water Mass Flow Rate {[}kg/s{]}}\label{water-use-equipment-cold-water-mass-flow-rate-kgs}
+
+The mass flow rate of cold water supplied to the equipment, in units of kilograms per second (kg/s).
+
+\paragraph{Water Use Equipment Total Mass Flow Rate {[}kg/s{]}}\label{water-use-equipment-total-mass-flow-rate-kgs}
+
+The total mass flow rate of water (hot + cold) supplied to the equipment, in units of kilograms per second (kg/s).
+
+\paragraph{Water Use Equipment Hot Water Volume Flow Rate {[}m3/s{]}}\label{water-use-equipment-hot-water-volume-flow-rate-m3s}
+
+The volumetric flow rate of hot water supplied to the equipment and consumed down the drain, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water Use Equipment Cold Water Volume Flow Rate {[}m3/s{]}}\label{water-use-equipment-cold-water-volume-flow-rate-m3s}
+
+The volumetric flow rate of cold water supplied to the equipment and consumed down the drain, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water Use Equipment Total Volume Flow Rate {[}m3/s{]}}\label{water-use-equipment-total-volume-flow-rate-m3s}
+
+The total volumetric flow rate of water (hot + cold) supplied to the equipment and consumed down the drain, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water Use Equipment Hot Water Volume {[}m3{]}}\label{water-use-equipment-hot-water-volume-m3}
+
+The volume of hot water supplied to the equipment and consumed down the drain, in units of cubic meters (m\(^{3}\)).
+
+\paragraph{Water Use Equipment Cold Water Volume {[}m3{]}}\label{water-use-equipment-cold-water-volume-m3}
+
+The volume of cold water supplied to the equipment and consumed down the drain, in units of cubic meters (m\(^{3}\)).
+
+\paragraph{Water Use Equipment Total Volume {[}m3{]}}\label{water-use-equipment-total-volume-m3}
+
+The total volume of water (hot+cold) supplied to the equipment and consumed down the drain, in units of cubic meters (m\(^{3}\)). This output is also added to a meter with Resource Type = Water, End Use Key = WaterSystems, and Group Key = Plant. The sub-categories may be entered as any type (e.g., Laundry, Dish Washing, etc. defined in WaterUse:Equipment object input for End-Use Subcategory) with General being the default sub-category (ref. Output Meter)
+
+\paragraph{Water Use Equipment Mains Water Volume {[}m3{]}}\label{water-use-equipment-mains-water-volume-m3}
+
+The total volume of water (hot+cold) supplied to the equipment and consumed down the drain, in units of cubic meters (m\(^{3}\)). This output is also added to a meter with Resource Type = MainsWater, End Use Key = WaterSystems, and Group Key = Plant. The sub-categories may be entered as any type (e.g., Laundry, Dish Washing, etc. defined in WaterUse:Equipment object input for End-Use Subcategory) with General being the default sub-category (ref. Output Meter)
+
+\paragraph{Water Use Equipment Hot Water Temperature {[}C{]}}\label{water-use-equipment-hot-water-temperature-c}
+
+The temperature of hot water supplied to the equipment, in units of degrees Celsius (C).
+
+\paragraph{Water Use Equipment Cold Water Temperature {[}C{]}}\label{water-use-equipment-cold-water-temperature-c}
+
+The temperature of cold water supplied to the equipment, in units of degrees Celsius (C).
+
+\paragraph{Water Use Equipment Target Water Temperature {[}C{]}}\label{water-use-equipment-target-water-temperature-c}
+
+The user-specified target temperature for the mixing of hot and cold supply flows, in units of degrees Celsius (C).
+
+\paragraph{Water Use Equipment Mixed Water Temperature {[}C{]}}\label{water-use-equipment-mixed-water-temperature-c}
+
+The actual mixed water temperature possible with the available hot and cold temperatures and flow rates, in units of degrees Celsius (C).
+
+\paragraph{Water Use Equipment Drain Water Temperature {[}C{]}}\label{water-use-equipment-drain-water-temperature-c}
+
+The water temperature at the drain equal to the mixed water temperature minus any heat loss to the zone, in units of degrees Celsius (C).
+
+\paragraph{Water Use Equipment Heating Rate {[}W{]}}\label{water-use-equipment-heating-rate-w}
+
+The heating rate defined by the hot water flow and the temperature difference between the hot water supply and the cold makeup return water, in units of watts (W).
+
+\paragraph{Water Use Equipment Heating Energy {[}J{]}}\label{water-use-equipment-heating-energy-j}
+
+The heating energy accumulated by the heating rate above, in units of Joules (J). This output is also added to a meter with End Use Key = WaterSystems, Group Key = Plant. If both of the node names specified in the WaterUse:Equipment object are blank, then this output is reported with Resource Type = DistrictHeating. If either of the node names are entered, then this output is reported with Resource Type = EnergyTransfer. The sub-categories may be entered as any type (e.g., Laundry, Dish Washing, etc. defined in WaterUse:Equipment object input for End-Use Subcategory) with General being the default sub-category (ref. Output Meter)
+
+\paragraph{Water Use Equipment Zone Sensible Heat Gain Rate {[}W{]}}\label{water-use-equipment-zone-sensible-heat-gain-rate-w}
+
+The sensible heat rate to the zone due to the water flow being exposed to zone air, in units of watts (W).
+
+\paragraph{Water Use Equipment Zone Sensible Heat Gain Energy {[}J{]}}\label{water-use-equipment-zone-sensible-heat-gain-energy-j}
+
+The sensible heat energy accumulated by the latent heat rate above, in units of Joules (J).
+
+\paragraph{Water Use Equipment Zone Latent Gain Rate {[}W{]}}\label{water-use-equipment-zone-latent-gain-rate-w}
+
+The latent heat rate to the zone due to the water flow being exposed to zone air, in units of watts (W).
+
+\paragraph{Water Use Equipment Zone Latent Gain Energy {[}J{]}}\label{water-use-equipment-zone-latent-gain-energy-j}
+
+The latent heat energy accumulated by the latent heat rate above, in units of Joules (J).
+
+\paragraph{Water Use Equipment Zone Moisture Gain Mass Flow Rate {[}kg/s{]}}\label{water-use-equipment-zone-moisture-gain-mass-flow-rate-kgs}
+
+The moisture rate of evaporation to the zone due to the water flow being exposed to zone air, in units of kilograms per second (kg/s).
+
+\paragraph{Water Use Equipment Zone Moisture Gain Mass {[}kg{]}}\label{water-use-equipment-zone-moisture-gain-mass-kg}
+
+The moisture mass accumulated by the moisture rate above, in units of kilograms (kg).
+
+\subsection{WaterUse:Connections}\label{wateruseconnections}
+
+The WaterUse:Connections object can be thought of as a subsystem that groups together multiple WaterUse:Equipment components. As its name suggests, the object provides connections that are shared by these components, including:
+
+\begin{itemize}
+\item
+  Inlet node and outlet node connections to a plant loop
+\item
+  Connections to WaterUse:Storage objects to store and draw reclaimed water
+\item
+  Internal connections to simulate drainwater heat recovery.
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 153
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image579.png}
+\caption{Diagram of internal connections for WaterUse:Connections \protect \label{fig:diagram-of-internal-connections-for-wateruse}}
+\end{figure}
+
+The WaterUse:Connections object can be used stand-alone or coupled into a plant loop. In stand-alone mode, the Hot and Cold Water Supply Temperature Schedules override the values for the listed WaterUse:Equipment objects. When coupled to the plant, the Hot Water Supply Temperature Schedule is overridden by the actual plant loop inlet water temperature. When coupled to the plant, the WaterUse:Connections object should be on a Branch object whose control type is set to Active.
+
+\subsubsection{Inputs}\label{inputs-1-050}
+
+\paragraph{Field: Name}\label{field-name-1-048}
+
+The unique object name for reference by other objects.
+
+\paragraph{Field: Inlet Node Name}\label{field-inlet-node-name-008}
+
+The hot water inlet node when connected to a plant loop. The hot water supplies all of the WaterUse:Equipment objects that demand hot water. Insufficient supply temperature or flow results in cooler water at the tap.
+
+\paragraph{Field: Outlet Node Name}\label{field-outlet-node-name-009}
+
+The cold water outlet node, i.e.~the cold water supply mains, when connected to a plant loop. The return node provides make-up water for the hot water lost down the drain.
+
+\paragraph{Field: Supply Water Storage Tank Name}\label{field-supply-water-storage-tank-name-002}
+
+Reference to the WaterUse:Storage object that supplies cold water to the listed WaterUse:Equipment objects. If the field is blank, or the tank is empty, fresh water is supplied from the water mains.
+
+\paragraph{Field: Reclamation Water Storage Tank Name}\label{field-reclamation-water-storage-tank-name}
+
+Reference to the WaterUse:Storage object that stores the resulting graywater from the listed WaterUse:Equipment objects. If the field is blank, the graywater is not reclaimed.
+
+\paragraph{Field: Hot Water Supply Temperature Schedule Name}\label{field-hot-water-supply-temperature-schedule-name-1}
+
+Reference to the schedule object specifying the hot water temperature {[}C{]}. If blank in stand-alone mode, the hot water supply temperature defaults to the cold water supply temperature. This field (even if blank) overrides the Hot Water Supply Temperature Schedule in all of the listed WaterUse:Equipment objects.
+
+\paragraph{Field: Cold Water Supply Temperature Schedule Name}\label{field-cold-water-supply-temperature-schedule-name-1-000}
+
+Reference to the schedule object specifying the cold water temperature {[}C{]} from the supply mains that provides the cold water to the tap and makes up for all water lost down the drain. If blank, water temperatures are calculated by the Site:WaterMainsTemperature object.
+
+This field (even if blank) overrides the Cold Water Supply Temperature Schedule in all of the listed WaterUse:Equipment objects.
+
+\paragraph{Field: Drain Water Heat Exchanger Type}\label{field-drain-water-heat-exchanger-type}
+
+The heat exchanger type to be used for drainwater heat recovery. None indicates no heat recovery is to be simulated. Ideal sets a heat exchanger effectiveness of 1.0. Effectiveness is calculated dynamically for CounterFlow and CrossFlow options.
+
+One popular type of drainwater heat exchanger is the Gravity-Film Heat Exchanger (GFX). The GFX is most closely approximated with the CounterFlow option, but keep in mind that the UA varies more with flow rate for the GFX than for most traditional heat exchangers.
+
+\paragraph{Field: Drain Water Heat Exchanger Destination}\label{field-drain-water-heat-exchanger-destination}
+
+The heat exchanger configuration to be used for drainwater heat recovery. The configuration determines where the heat will be used after it is recovered.
+
+Plant indicates that the all of the recovered heat will be sent to the return flow at the outlet node of the WaterUse:Connections object to preheat the make-up cold water from the water mains.
+
+Equipment indicates that the all of the recovered heat will be used to preheat the cold water flow side of the WaterUse:Equipment objects listed \emph{in this} WaterUse:Connections object
+
+PlantAndEquipment indicates the recovered heat will be divided between the plant and the WaterUse:Equipment objects, as described above. This is the only option where the flow rates are equal in the drain and the heat exchanger.
+
+\paragraph{Field: Drain Water Heat Exchanger U-Factor Times Area}\label{field-drain-water-heat-exchanger-u-factor-times-area}
+
+The UA is the heat transfer coefficient {[}W/K{]} for the heat exchanger and is the product of U, the overall heat transfer coefficient, and A, the heat exchanger surface area.
+
+\paragraph{Field: Water Use Equipment 1-10 Name}\label{field-water-use-equipment-1-10-name}
+
+References to WaterUse:Equipment objects.
+
+IDF examples:
+
+\begin{lstlisting}
+
+WaterUse:Connections,
+  Domestic Water Uses,   !- Name
+  Water Eq Inlet Node,   !- Inlet Node Name
+  Water Eq Outlet Node, !- Outlet Node Name
+  Rainwater Storage,   !- Supply Water Storage Tank Name
+  Graywater Storage,   !- Reclamation Water Storage Tank Name
+  ,   !- Hot Water Supply Temperature Schedule Name
+  ,   !- Cold Water Supply Temperature Schedule Name
+  CounterFlow,   !- Drain Water Heat Exchanger Type
+  Plant,   !- Drain Water Heat Exchanger Destination
+  1500,   !- Drain Water Heat Exchanger U-Factor Times Area {W/K}
+  Sinks,   !- Water Use Equipment 1 Name
+  Showers,   !- Water Use Equipment 2 Name
+  Dishwasher,   !-   Water Use Equipment 3 Name
+  Clotheswasher;   !- Water Use Equipment 4 Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-031}
+
+The following output variables are reported for the WaterUse:Connections object:
+
+\begin{itemize}
+\item
+  HVAC,Average,Water Use Connections Hot Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water Use Connections Cold Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water Use Connections Total Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water Use Connections Drain Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water Use Connections Heat Recovery Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Water Use Connections Hot Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Water Use Connections Cold Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Water Use Connections Total Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Water Use Connections Hot Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Water Use Connections Cold Water Volume {[}m3{]}
+\item
+  HVAC,Sum,Water Use Connections Total Volume {[}m3{]}
+\item
+  HVAC,Average,Water Use Connections Hot Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Connections Cold Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Connections Drain Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Connections Return Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Connections Waste Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Connections Heat Recovery Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water Use Connections Heat Recovery Effectiveness {[]}
+\item
+  HVAC,Average,Water Use Connections Heat Recovery Rate {[}W{]}
+\item
+  HVAC,Sum,Water Use Connections Heat Recovery Energy {[}J{]}
+\item
+  HVAC,Sum,Water Use Connections Plant Hot Water Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Water Use Connections Hot Water Mass Flow Rate {[}kg/s{]}}\label{water-use-connections-hot-water-mass-flow-rate-kgs}
+
+The mass flow rate of hot water supplied to all equipment, in units of kilograms per second (kg/s).
+
+\paragraph{Water Use Connections Cold Water Mass Flow Rate {[}kg/s{]}}\label{water-use-connections-cold-water-mass-flow-rate-kgs}
+
+The mass flow rate of cold water supplied to all equipment, in units of kilograms per second (kg/s).
+
+\paragraph{Water Use Connections Total Mass Flow Rate {[}kg/s{]}}\label{water-use-connections-total-mass-flow-rate-kgs}
+
+The total mass flow rate of water (hot + cold) supplied to all equipment, in units of kilograms per second (kg/s).
+
+\paragraph{Water Use Connections Drain Water Mass Flow Rate {[}kg/s{]}}\label{water-use-connections-drain-water-mass-flow-rate-kgs}
+
+The mass flow rate of drainwater from all equipment, in units of kilograms per second (kg/s).
+
+\paragraph{Water Use Connections Heat Recovery Mass Flow Rate {[}kg/s{]}}\label{water-use-connections-heat-recovery-mass-flow-rate-kgs}
+
+The mass flow rate of make-up water in the heat exchanger, in units of kilograms per second (kg/s).
+
+\paragraph{Water Use Connections Hot Water Volume Flow Rate {[}m3/s{]}}\label{water-use-connections-hot-water-volume-flow-rate-m3s}
+
+The volumetric flow rate of hot water supplied to all equipment and consumed down the drain, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water Use Connections Cold Water Volume Flow Rate {[}m3/s{]}}\label{water-use-connections-cold-water-volume-flow-rate-m3s}
+
+The volumetric flow rate of cold water supplied to all equipment and consumed down the drain, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water Use Connections Total Volume Flow Rate {[}m3/s{]}}\label{water-use-connections-total-volume-flow-rate-m3s}
+
+The total volumetric flow rate of water (hot + cold) supplied to all equipment and consumed down the drain, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water Use Connections Hot Water Volume {[}m3{]}}\label{water-use-connections-hot-water-volume-m3}
+
+The volume of hot water supplied to all equipment and consumed down the drain, in units of cubic meters (m\(^{3}\)).
+
+\paragraph{Water Use Connections Cold Water Volume {[}m3{]}}\label{water-use-connections-cold-water-volume-m3}
+
+The volume of cold water supplied to all equipment and consumed down the drain, in units of cubic meters (m\(^{3}\)).
+
+\paragraph{Water Use Connections Total Volume {[}m3{]}}\label{water-use-connections-total-volume-m3}
+
+The total volume of water (hot+cold) supplied to all equipment and consumed down the drain, in units of cubic meters (m\(^{3}\)).
+
+\paragraph{Water Use Connections Hot Water Temperature {[}C{]}}\label{water-use-connections-hot-water-temperature-c}
+
+The temperature of hot water supplied to all equipment, in units of degrees Celsius (C).
+
+\paragraph{Water Use Connections Cold Water Temperature {[}C{]}}\label{water-use-connections-cold-water-temperature-c}
+
+The temperature of cold water supplied to all equipment, in units of degrees Celsius (C).
+
+\paragraph{Water Use Connections Drain Water Temperature {[}C{]}}\label{water-use-connections-drain-water-temperature-c}
+
+The water temperature at the drain equal to the mixed water temperature minus any heat losses to the zone, in units of degrees Celsius (C).
+
+\paragraph{Water Use Connections Return Water Temperature {[}C{]}}\label{water-use-connections-return-water-temperature-c}
+
+The temperature of make-up water returned to the plant loop, in units of degrees Celsius (C).
+
+\paragraph{Water Use Connections Waste Water Temperature {[}C{]}}\label{water-use-connections-waste-water-temperature-c}
+
+The temperature of the water leaving the heat exchanger. If no heat exchanger, the waste water temperature equals the drain water temperature, in units of degrees Celsius (C).
+
+\paragraph{Water Use Connections Heat Recovery Water Temperature {[}C{]}}\label{water-use-connections-heat-recovery-water-temperature-c}
+
+The temperature of the water leaving the heat exchanger. If no heat exchanger, the waste water temperature equals the drain water temperature, in units of degrees Celsius (C).
+
+\paragraph{\texorpdfstring{Water Use Connections Heat Recovery Effectiveness {[]}}{Water Use Connections Heat Recovery Effectiveness }}\label{water-use-connections-heat-recovery-effectiveness}
+
+The effectiveness value of the heat exchanger. The units are dimensionless.
+
+\paragraph{Water Use Connections Heat Recovery Rate {[}W{]}}\label{water-use-connections-heat-recovery-rate-w}
+
+The heat recovered by the heat exchanger and used to preheat the cold make-up water, in units of watts (W).
+
+\paragraph{Water Use Connections Heat Recovery Energy {[}J{]}}\label{water-use-connections-heat-recovery-energy-j}
+
+The energy recovered by the heat exchanger and used to preheat the cold make-up water, in units of Joules (J).
+
+\paragraph{Water Use Connections Plant Hot Water Energy {[}J{]}}\label{water-use-connections-plant-hot-water-energy-j}
+
+The plant loop energy consumed by the hot water used, in units of Joules (J). This output is also added to a meter with Resource Type = PlantLoopHeatingDemand, End Use Key = WaterSystems, and Group Key = Plant (ref. Output Meter).
+
+\subsection{WaterUse:Storage}\label{waterusestorage}
+
+The WaterUse:Storage object is a central component for complex water systems. This object is not needed if the only use of water is directly from the mains, or utility service water. If the building model is to include any on-site collection or wells or storing and reuse of graywater, then a WaterUse:Storage is needed. Each WaterUse:Storage can serve as a central node and make connections to numerous sources of supply or numerous components with demand. If a maximum capacity is not specified, the tank is assumed to have unlimited capacity. This is useful for sizing.
+
+Storage tanks may handle a lot of water but show no use. This is because water usage is metered at the component level were water is used up. The only water a storage tank might use up is overflow water if it is discarded.
+
+\subsubsection{Inputs}\label{inputs-2-046}
+
+\paragraph{Field: Name}\label{field-name-2-043}
+
+The unique object name for reference by other objects.
+
+\paragraph{Field: Water Quality Subcategory}\label{field-water-quality-subcategory}
+
+Describes the quality of the water contained in the tank. Used for reporting and to check that the uses and supply match the category of water quality.
+
+\paragraph{Field: Maximum Capacity}\label{field-maximum-capacity}
+
+The maximum volumetric capacity {[}m3{]} of the water tank. If blank, this field defaults to unlimited capacity.
+
+\paragraph{Field: Initial Volume}\label{field-initial-volume}
+
+The volume of water in the storage tank at the beginning of each simulation environmental period {[}m3{]}. This provides a starting point for the amount of water in storage.
+
+\paragraph{Field: Design In Flow Rate}\label{field-design-in-flow-rate}
+
+The design flow rate {[}m3/s{]} of fittings that provide water into the tank from external sources. In a scenario where a heavy rain fall is being harvested, the actual reclamation rate might be limited by pipe size or filtration. If blank, this field defaults to unlimited rate.
+
+\paragraph{Field: Design Out Flow Rate}\label{field-design-out-flow-rate}
+
+The design flow rate {[}m3/s{]} of fitting that withdraw water from the tank to end uses. Heavy demand (landscaping?) might be limited by pipe size or filtration. If Blank, this field defaults to unlimited rate.
+
+\paragraph{Field: Overflow Destination}\label{field-overflow-destination}
+
+Name of a second WaterUse:Storage that would receive overflow. Overflow could occur if the maximum capacity is reached or if the design in flow rate is exceeded. If left blank, then the overflow is discarded and lost from the water system.
+
+\paragraph{Field: Type of Supply Controlled by Float Valve}\label{field-type-of-supply-controlled-by-float-valve}
+
+The storage tank can include the capability of modeling a float valve that will call for water to be added to the tank. This field is used to select the type of system used to respondto fill requests made by a float valve. The available options are None , Mains , GroundwaterWell , or OtherTank. The float valve settings are described in the next two fields.
+
+\paragraph{Field: Float Valve On Capacity}\label{field-float-valve-on-capacity}
+
+The volumetric capacity {[}m3{]} of the water tank when a floating valve would turn on to allow filling the tank.
+
+\paragraph{Field: Float Valve Off Capacity}\label{field-float-valve-off-capacity}
+
+The volumetric capacity {[}m3{]} of the water tank when a floating valve would turn off after having been filling the tank.
+
+\paragraph{Field: Backup Mains Capacity}\label{field-backup-mains-capacity}
+
+The volumetric capacity of the tank that indicates where a secondary float valve will maintain the volume by calling for mains water. Used if the well or other tank cannot keep up with the needs of the main float valve. If left blank or equal 0.0, then there is no mains water backup. If specified, then mains water will be drawn once the storage tank reaches this level and then the mains water will fill all the way to capacity specified in the previous field.
+
+\paragraph{Field: Other Tank Name}\label{field-other-tank-name}
+
+This field contains the name of another WaterUse:Storage defined elsewhere in the input file. This field is only used if the Type of Controlled Supply field is set to OtherTank and the current tank is to be configured to be supplied by a second tank in response to a float valve.
+
+\paragraph{Field: Water Thermal Mode}\label{field-water-thermal-mode}
+
+Controls the method of determining the temperature of the water in the storage tank. The only available option at the current time is ScheduledTemperature.
+
+\paragraph{Field: Water Temperature Schedule Name}\label{field-water-temperature-schedule-name-000}
+
+Reference to the schedule object specifying the temperature {[}C{]} of the water in the tank. This takes the place of a full thermal model of the tank.
+
+\paragraph{Field: Ambient Temperature Indicator}\label{field-ambient-temperature-indicator-001}
+
+Reserved for future use. The field can be Schedule, Zone, or Outdoors.
+
+\paragraph{Field: Ambient Temperature Schedule Name}\label{field-ambient-temperature-schedule-name-002}
+
+Reserved for future use. Schedule name for ambient temperature when previous field is Schedule.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-010}
+
+Reserved for future use. Name of zone where the tank is located.
+
+\paragraph{Field: Tank Surface Area}\label{field-tank-surface-area}
+
+Reserved for future zone thermal model.
+
+\paragraph{Field: Tank U Value}\label{field-tank-u-value}
+
+Reserved for future zone thermal model.
+
+\paragraph{Field: Tank Outside Surface Material Name}\label{field-tank-outside-surface-material-name}
+
+Reserved for future zone thermal model.
+
+IDF examples:
+
+\begin{lstlisting}
+
+WaterUse:Storage,
+  Tower 2 water tank, !- Name
+  Tower water make up Holding tank, !- Water Quality Subcategory
+  30.0 , !- Maximum Capacity {m3}
+  10.0 , !- Initial Volume   {m3}
+  20.0, !- Design In Flow Rate {m3}
+  20.0, !- Design Out Flow Rate {m3}
+  ,   !- Overflow Destination
+  Mains, !- Type of Supply Controlled by Float Valve
+  8.0 , !- Float Valve On Capacity {m3}
+  10.0,   !- Float Valve Off Capacity {m3}
+  3.0, !- Backup Mains Capacity {m3}
+  ,   !- Other Tank Name
+  ScheduledTemperature , !- Water Thermal Mode
+  Water Tank Temp Sched , !- Water Temperature Schedule Name
+  , !- Ambient Temperature Indicator
+  , !- Ambient Temperature Schedule Name
+  , !- Zone Name
+  , !- Tank Surface Area {m2}
+  , !- Tank U Value {W/m2-K}
+  ; !- Tank Outside Surface Material Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-026}
+
+The following output variables are available for reporting for each WaterUse:Storage object.
+
+\begin{itemize}
+\item
+  HVAC,Average,Water System Storage Tank Volume {[}m3{]}
+\item
+  HVAC,Average,Water System Storage Tank Net Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Water System Storage Tank Inlet Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Water System Storage Tank Outlet Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Water System Storage Tank Mains Water Volume {[}m3{]}
+\item
+  HVAC,Average,Water System Storage Tank Mains Water Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Water System Storage Tank Water Temperature {[}C{]}
+\item
+  HVAC,Average,Water System Storage Tank Overflow Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Water System Storage Tank Overflow Water Volume {[}m3{]}
+\item
+  HVAC,Average,Water System Storage Tank Overflow Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Water System Storage Tank Volume {[}m3{]}}\label{water-system-storage-tank-volume-m3}
+
+This is the volume of water stored in the storage tank, in units of cubic meters (m\(^{3}\)).
+
+\paragraph{Water System Storage Tank Net Volume Flow Rate {[}m3{]}}\label{water-system-storage-tank-net-volume-flow-rate-m3}
+
+This is the net rate of flows in and out of the storage tank, in units of cubic meters (m\(^{3}\)).
+
+\paragraph{Water System Storage Tank Inlet Volume Flow Rate {[}m3/s{]}}\label{water-system-storage-tank-inlet-volume-flow-rate-m3s}
+
+This is the rate of flows into the storage tank, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water System Storage Tank Outlet Volume Flow Rate {[}m3{]}}\label{water-system-storage-tank-outlet-volume-flow-rate-m3}
+
+This is the rate of flows out of the storage tank, in units of cubic meters (m\(^{3}\)).
+
+\paragraph{Water System Storage Tank Mains Water Volume {[}m3{]}}\label{water-system-storage-tank-mains-water-volume-m3}
+
+This is the volume of water drawn from the mains in order to fill the tank, in units of cubic meters per second (m\(^{3}\)/s). This output is also added to a meter with Resource Type = MainsWater, End Use Key = WaterSystem, and Group Key = System. The water quality sub-category may be entered as any type (defined in WaterUse:Storage object input for Water Quality Subcategory) (ref. Output Meter).
+
+\paragraph{Water System Storage Tank Mains Water Volume Flow Rate {[}m3/s{]}}\label{water-system-storage-tank-mains-water-volume-flow-rate-m3s}
+
+This is the rate of water draw from the mains in order to fill the tank, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water System Storage Tank Water Temperature {[}C{]}}\label{water-system-storage-tank-water-temperature-c}
+
+This is the temperature of the water in the tank, in units of degrees Celsius (C).
+
+\paragraph{Water System Storage Tank Overflow Volume Flow Rate {[}m3/s{]}}\label{water-system-storage-tank-overflow-volume-flow-rate-m3s}
+
+This is the rate of water flows that overflow the tank either because of limits on how fast the tank can fill or because the tank is full and cannot handle the water provided, in units of cubic meters per seconc (m\(^{3}\)/s).
+
+\paragraph{Water System Storage Tank Overflow Water Volume {[}m3{]}}\label{water-system-storage-tank-overflow-water-volume-m3}
+
+This is the volume of water overflowing the tank because of limits on how fast the tank can fill or because the tank is full and cannot handle the water provided, in units of cubic meters (m\(^{3}\)).
+
+\paragraph{Water System Storage Tank Overflow Temperature {[}C{]}}\label{water-system-storage-tank-overflow-temperature-c}
+
+This the temperature of overflow water leaving the tank.
+
+\subsection{WaterUse:RainCollector}\label{wateruseraincollector}
+
+The WaterUse:RainCollector object is used for harvesting rainwater falling on building surfaces. The rainwater is sent to a WaterUse:Storage object. In order to use this object it is necessary to also include a Site:Precipitation object to describe the rates of rainfall.
+
+\subsubsection{Inputs}\label{inputs-3-041}
+
+\paragraph{Field: Name}\label{field-name-3-037}
+
+The unique object name for reference by other objects.
+
+\paragraph{Field: Storage Tank Name}\label{field-storage-tank-name}
+
+A reference to a WaterUse:Storage object where the rainwater will be collected and stored for later use.
+
+\paragraph{Field: Loss Factor Mode}\label{field-loss-factor-mode}
+
+The WaterUse:RainCollector model includes a loss factor that indicates the portion of incident rain that is not successfully collected. Two modes are available: Constant and Scheduled. Enter Constant in this field for the model to use a simple fixed loss factor defined in the next field. For versatility, the loss factor can follow a schedule by entering Scheduled in this field and then the name of a schedule in the second field below.
+
+\paragraph{Field: Collection Loss Factor}\label{field-collection-loss-factor}
+
+Constant loss factor for how much of the incident rainwater is lost and not collected. The factor should be between 0 and 1.
+
+\paragraph{Field: Collection Loss Factor Schedule Name}\label{field-collection-loss-factor-schedule-name}
+
+Name of a schedule that defines a variable collection loss factor if the mode is selected as Scheduled.
+
+\paragraph{Field: Maximum Collection Rate}\label{field-maximum-collection-rate}
+
+The maximum flow rate {[}m3/s{]} for rainwater collection. In a scenario where a heavy rain fall is being harvested, the actual reclamation rate might be limited by pipe size or the filtration system.
+
+\paragraph{Field: Collection Surface 1-10 Name}\label{field-collection-surface-1-10-name}
+
+A reference to the name of a surface object which will collect the rain. Typically the collection surfaces would correspond to roof surfaces on the building. The effective area for rainwater collection is the horizontal component (area * cosine of the slope, etc.). More detailed modeling of rainwater collection can be added later to account for factors such as wind speed and direction, etc.
+
+IDF examples:
+
+\begin{lstlisting}
+
+WaterUse:RainCollector,
+  My Test Rain Collector ,!- Name
+  My Test Tank ,   !-   Storage Tank Name
+  CONSTANT,   !- Loss Factor Mode
+  0.9 ,   !- Collection Loss Factor
+  ,   !- Collection Loss Factor Schedule Name
+  1.0 ,   !- Maximum Collection Rate
+  SouthRoof ,   !- Collection Surface 1 Name
+  NorthRoof1,   !- Collection Surface 2 Name
+  NorthRoof3 ,   !- Collection Surface 3 Name
+  NorthRoof2 ;   !- Collection Surface 4 Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-023}
+
+\begin{itemize}
+\item
+  HVAC,Average,Water System Rainwater Collector Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Water System Rainwater Collector Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Water System Rainwater Collector Volume Flow Rate {[}m3/s{]}}\label{water-system-rainwater-collector-volume-flow-rate-m3s}
+
+This output variable provides the rate of water collected by the WaterUse:RainCollector, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water System Rainwater Collector Volume {[}m3{]}}\label{water-system-rainwater-collector-volume-m3}
+
+This output variable provides the volume of water collected by the WaterUse:RainCollector, in units of cubic meters per second (m\(^{3}\)/s). This output is also added to a meter with Resource Type = OnSiteWater, End Use Key = RainWater, and Group Key = System (ref. Output Meter).
+
+\subsection{WaterUse:Well}\label{waterusewell}
+
+The WaterUse:Well object is for simulating on-site water supply from a well. Well water is pumped out of the ground and into a WaterUse:Storage. The operation of the ground water well is controlled by the associated WaterUse:Storage which is assumed to be operated as a vented cistern with no pressure tank. The current implementation is very simple and only requires two numeric inputs: the rated pump flow and power. A more elaborate well model may be added and many input fields are reserved for this future expansion.
+
+\subsubsection{Inputs}\label{inputs-4-038}
+
+\paragraph{Field: Name}\label{field-name-4-033}
+
+Unique name of this well.
+
+\paragraph{Field: Storage Tank Name}\label{field-storage-tank-name-1}
+
+A reference to a WaterUse:Storage object where the rainwater will be collected and stored for later use.
+
+\paragraph{Field: Pump Depth}\label{field-pump-depth}
+
+Reserved for future use. Effective depth of well {[}m{]}
+
+\paragraph{Field: Pump Rated Flow Rate}\label{field-pump-rated-flow-rate}
+
+This is the nominal pump flow rate {[}m3/s{]}. This field is required.
+
+\paragraph{Field: Pump Rated Head}\label{field-pump-rated-head}
+
+Reserved for future use {[}Pa{]}. Pump head at rated conditions in Pascals.
+
+\paragraph{Field: Pump Rated Power Consumption}\label{field-pump-rated-power-consumption}
+
+This is the pump power at the nominal pump flow rate {[}W{]}. This field is required.
+
+\paragraph{Field: Pump Efficiency}\label{field-pump-efficiency}
+
+Reserved for future use.
+
+\paragraph{Field: Well Recovery Rate}\label{field-well-recovery-rate}
+
+Reserved for future use. Rate at which ground water enters well during a sustained draw, e.g., 2 hour well test {[}m3/s{]}.
+
+\paragraph{Field: Nominal Well Storage Volume}\label{field-nominal-well-storage-volume}
+
+Reserved for future use. Capacity in well after long period of inactivity and the usual water table depth. {[}m3{]}
+
+\paragraph{Field: Water Table Depth Mode}\label{field-water-table-depth-mode}
+
+Reserved for future use. Two options available: Constant or Scheduled
+
+\paragraph{Field: Water Table Depth}\label{field-water-table-depth}
+
+Reserved for future use. Depth of water table from WaterUse:Storage
+
+\paragraph{Field: Water Table Depth Schedule Name}\label{field-water-table-depth-schedule-name}
+
+Reserved for future use.
+
+An example input object:
+
+\begin{lstlisting}
+
+WaterUse:Well,
+  My Test Well,   !- Name
+  Tower 1 Water Tank,   !- Storage Tank Name
+  ,   !- Pump Depth
+  0.1,   !- Pump Rated Flow Rate {m3/s}
+  ,   !- Pump Rated Head {Pa}
+  120,   !- Pump Rated Power Consumption {W}
+  ,   !- Pump Efficiency
+  ,   !- Well Recovery Rate {m3/s}
+  ,   !- Nominal Well Storage Volume {m3}
+  ,   !- Water Table Depth Mode
+  ,   !- Water Table Depth
+  ;   !- Water Table Depth Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-019}
+
+The following output variables are available for reporting for each WaterUse:Well object.
+
+\begin{itemize}
+\item
+  HVAC,Average,Water System Groundwater Well Requested Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Water System Groundwater Well Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Water System Groundwater Well Volume {[}m3{]}
+\item
+  HVAC,Average,Water System Groundwater Well Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Water System Groundwater Well Pump Electric Energy {[}J{]}
+\end{itemize}
+
+\paragraph{Water System Groundwater Well Requested Volume Flow Rate {[}m3/s{]}}\label{water-system-groundwater-well-requested-volume-flow-rate-m3s}
+
+This is the volume flow rate that the water system requested from the well, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water System Groundwater Well Volume Flow Rate {[}m3/s{]}}\label{water-system-groundwater-well-volume-flow-rate-m3s}
+
+This is the volume flow water of water actually obtained from the well, in units of cubic meters per second (m\(^{3}\)/s).
+
+\paragraph{Water System Groundwater Well Volume {[}m3{]}}\label{water-system-groundwater-well-volume-m3}
+
+This is the volume of water obtained from the well, in units of cubic meters (m\(^{3}\)). This output is also added to a meter with Resource Type = OnSiteWater, End Use Key = WellWater, and Group Key = System (ref. Output Meter).
+
+\paragraph{Water System Groundwater Well Pump Electric Power {[}W{]}}\label{water-system-groundwater-well-pump-electric-power-w}
+
+This is the electrical power of the pump used to extract water from the well, in units of watts (W).
+
+\paragraph{Water System Groundwater Well Pump Electric Energy {[}J{]}}\label{water-system-groundwater-well-pump-electric-energy-j}
+
+This is the electricity energy used by the pump to extract water from the well, in units of Joules (J). This output is also added to a meter with Resource Type = Electricity, End Use Key = WaterSystems, and Group Key = System (ref. Output Meter).
diff --git a/doc/input-output-reference/src/overview/group-zone-controls-thermostats.tex b/doc/input-output-reference/src/overview/group-zone-controls-thermostats.tex
new file mode 100644
index 00000000000..4ca31989311
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+++ b/doc/input-output-reference/src/overview/group-zone-controls-thermostats.tex
@@ -0,0 +1,1103 @@
+\section{Group - Zone Controls - Thermostats and Humidistats}\label{group---zone-controls---thermostats-and-humidistats}
+
+Zone Control objects are used to control zone conditions to a specific setpoint. The six types of zone control are described in this section. They are, by name, ZoneControl:\textbf{\textless{}name\textgreater{}.}. These types are:
+
+\textbf{Thermostat} - The object provides the traditional approach to space control using air temperatures. Each controlled zone contains a thermostat object.
+
+\textbf{Humidistat} - The object is used to control a zone to a specified relative humidity.
+
+\textbf{Thermostat:ThermalComfort} - The object provides a method to control a zone to a dry-bulb temperature setpoint based on a thermal comfort model (e.g.~Fanger) and a user-specified thermal comfort setpoint schedule.
+
+\textbf{Thermostat:OperativeTemperature} - The operative temperature control is formulated to reuse all of the traditional thermostat objects. One input object will be used for each thermal zone to indicate if that zone s thermostat control mode should be overridden to effect operative temperature control rather than traditional air temperature control. The user will still have to input all the traditional ZoneControl:Thermostat and setpoint objects.
+
+\textbf{Thermostat:TemperatureAndHumidity} - This thermostat control works together with the traditional ZoneControl:Thermostat object to modify temperature control based on zone air humidity conditions. Currently, this object resets the thermostat s cooling setpoint temperature downward based on elevated zone air humidity levels, typically yielding additional cooling coil operation and associated dehumidification. A ZoneControl:Thermostat:TemperatureAndHumidity object should be specified to indicate if a zone s traditional thermostat control mode should be overridden to provide enhanced dehumidification. The user must still input the traditional ZoneControl:Thermostat and setpoint objects.
+
+\textbf{Thermostat}:\textbf{StagedDualSetpoint} - This thermostat control works alone with ``Dual Setpoint'' type only. The object provides heating and cooling setpoints, throttling range and offsets, so that zone temperature setpoint used for system load calculation is adjusted by the setpoint and throttling range based on the zone temperature at the previous time step. The stage number is determined by the temperature difference between the setpoint and zone temperature at the previous time step, and offset values. If this object and other zone control thermostat and humidistat are assigned to the same controlled zone, this object takes precedence when the controlled zone is specified in the Controlling Zone or Thermostat Location field of the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object.
+
+\subsection{ZoneControl:Thermostat}\label{zonecontrolthermostat}
+
+The thermostatic zone control object is used to control a zone to a specified temperature. ZoneControl:Thermostat references a control type schedule and one or more control type objects which in turn reference one or more setpoint schedules. The example at the end of this section illustrates a complete zone thermostat specification including the control type and setpoint schedules.
+
+The control type schedule and the list of control type/name pairs are directly related. The schedule defines the type of control that is to be used throughout the simulation. Valid Control Types are:
+
+0 - Uncontrolled (No specification or default)
+
+1 - Single Heating Setpoint
+
+2 - Single Cooling SetPoint
+
+3 - Single Heating/Cooling Setpoint
+
+4 - Dual Setpoint (Heating and Cooling) with deadband
+
+Thus, if the schedule referenced in the ZoneControl:Thermostat statement has a control type of 4 for a particular time period, this indicates that during that time period ``Dual Setpoint with deadband'' control is to be used. The specific ``Dual Setpoint (Heating and Cooling) with deadband'' control object to be used is specified in the list of control type/name pairs. Then the specific control type objects reference the thermostat setpoint temperature schedule to be used. Because only one control can be specified for each control type in a ZoneControl:Thermostat statement, there are only four pairs possible in a particular ZoneControl:Thermostat type/name list. This is because individual controls can be defined throughout the simulation, thus giving the user a full range of flexibility. Since putting in the name of the control type directly in the schedule would be very cumbersome, the control types are assigned a number which is used in the schedule profile.
+
+\subsubsection{Inputs}\label{inputs-054}
+
+\paragraph{Field: Name}\label{field-name-052}
+
+Unique identifying name for the thermostat.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-001}
+
+Name of the zone or set of zones that is being controlled. When the ZoneList option is used then this thermostat definition is applied to each of the zones in the zone list effecting a global definition for thermostatic control in the zone.
+
+\paragraph{Field: Control Type Schedule Name}\label{field-control-type-schedule-name}
+
+Schedule which defines what type of control is active during the simulation. Valid Control Types are:
+
+0 - Uncontrolled (No specification or default)
+
+1 - Single Heating Setpoint
+
+2 - Single Cooling SetPoint
+
+3 - Single Heating Cooling Setpoint
+
+4 - Dual Setpoint with Deadband (Heating and Cooling)
+
+Each non-zero control type which is used in this schedule must appear in the following fields which list the specific thermostat control objects to be used for this zone.
+
+\paragraph{Field Set (Control Object Type, Control Name)}\label{field-set-control-object-type-control-name}
+
+Up to four pairs of Control Object Type and Control Name may be listed to specify which control objects are used for this zone. This list is not order-dependent, and the position in this list has no impact on the control type schedule. In the control type schedule, a value of 1 always means ``Single Heating Setpoint'', even if that control type is not first in this list.
+
+\paragraph{Field: Control Object \textless{}x\textgreater{}Type}\label{field-control-object-xtype}
+
+This field specifies the control type to be used for this zone. Available control types are:
+
+ThermostatSetpoint:SingleHeating
+
+ThermostatSetpoint:SingleCooling
+
+ThermostatSetpoint:SingleHeatingOrCooling
+
+ThermostatSetpoint:DualSetpoint
+
+\paragraph{Field: Control \textless{}x\textgreater{} Name}\label{field-control-x-name}
+
+The corresponding control type name. The name is used in an object with the name of the control type and specifies the schedule.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+ZoneControl:Thermostat, Zone 3 Thermostat, NORTH ZONE,
+  Zone Control Type Sched,
+  DUAL SETPOINT WITH DEADBAND, VAV Setpoints;
+\end{lstlisting}
+
+An example of a global thermostat:
+
+\begin{lstlisting}
+
+ZoneList,AllControlledZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
+
+  ZoneControl:Thermostat,
+  AllControlledZones Thermostat,               !- Name
+  AllControlledZones,                               !- Zone Name
+  Zone Control Type Sched, !- Control Type Schedule Name
+  ThermostatSetpoint:SingleCooling,   !- Control 1 Object Type
+  CoolingSetPoint,                 !- Control 1 Name
+  ThermostatSetpoint:SingleHeating,   !- Control 2 Object Type
+  HeatingSetpoint,                 !- Control 2 Name
+  ThermostatSetpoint:DualSetpoint,   !- Control 3 Object Type
+  DualSetPoint;                       !- Control 3 Name
+\end{lstlisting}
+
+A complete zone thermostat example showing this statement and all of the objects it must reference is:
+
+\begin{lstlisting}
+
+! Zone control object which links thermostats to a particular zone
+  ZoneControl:Thermostat, Zone 2 Thermostat, EAST ZONE,
+  Zone Control Type Sched,
+  ThermostatSetpoint:SingleCooling, Cooling Setpoint with SB,
+  ThermostatSetpoint:SingleHeating; Heating Setpoint with SB;
+
+  ! Control type objects     these may be used in more than one zone
+  ThermostatSetpoint:SingleCooling,
+  Cooling Setpoint with SB,
+  Cooling Setpoints;
+
+  ThermostatSetpoint:SingleHeating,
+  Heating Setpoint with SB,
+  Heating Setpoints;
+
+  ! Schedule type definitions
+  ScheduleTypeLimits,Temperature,-60:200,CONTINUOUS;
+  ScheduleTypeLimits,Control Type,0:4,DISCRETE;
+
+  ! Control type schedule definition
+  Schedule:Compact, Zone Control Type Sched, Control Type,
+  Through: 3/31,
+  For: AllDays,
+  Until: 24:00, 1,   !- Single Heating
+  Through: 9/30,
+  For: AllDays,
+  Until: 24:00, 2,   !- Single Cooling
+  Through: 12/31,
+  For: AllDays,
+  Until: 24:00, 1;   !- Single Heating
+
+  ! Heating setpoint schedule definition
+  Schedule:Compact, Heating Setpoints, Temperature,
+  Through: 12/31,
+  For: AllDays,
+  Until: 7:00, 15.,
+  Until: 17:00,20.,
+  Until: 24:00,15.;
+
+  ! Cooling setpoint schedule definition
+  Schedule:Compact, Cooling Setpoints, Temperature,
+  Through: 12/31,
+  For: AllDays,
+  Until: 7:00, 30.,
+  Until: 20:00,23.,
+  Until: 24:00,30.;
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-042}
+
+Outputs available from controlled zones. The ``key'' in the below is the Zone Name.
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Predicted Sensible Load to Setpoint Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Zone Predicted Sensible Load to Heating Setpoint Heat Transfer Rate {[}W{]}
+\item
+  HVAC,Average,Zone Predicted Sensible Load to Cooling Setpoint Heat Transfer Rate {[}W{]}
+\item
+  Zone,Average,Zone Thermostat Control Type {[]}
+\item
+  Zone,Average,Zone Thermostat Heating Setpoint Temperature {[}C{]}
+\item
+  Zone,Average,Zone Thermostat Cooling Setpoint Temperature {[}C{]}
+\item
+  HVAC,Sum,Facility Any Zone Oscillating Temperatures Time {[}hr{]}
+\item
+  Zone,Sum,Zone Heating Setpoint Not Met Time {[}hr{]}
+\item
+  Zone,Sum,Zone Heating Setpoint Not Met While Occupied Time {[}hr{]}
+\item
+  Zone,Sum,Zone Cooling Setpoint Not Met Time {[}hr{]}
+\item
+  Zone,Sum,Zone Cooling Setpoint Not Met While Occupied Time {[}hr{]}
+\item
+  Zone,Sum,Facility Heating Setpoint Not Met Time {[}hr{]}
+\item
+  Zone,Sum,Facility Cooling Setpoint Not Met Time {[}hr{]}
+\item
+  Zone,Sum,Facility Heating Setpoint Not Met While Occupied Time {[}hr{]}
+\item
+  Zone,Sum,Facility Cooling Setpoint Not Met While Occupied Time {[}hr{]}
+\end{itemize}
+
+\paragraph{Zone Predicted Sensible Load to Setpoint Heat Transfer Rate {[}W{]}}\label{zone-predicted-sensible-load-to-setpoint-heat-transfer-rate-w}
+
+This is the predicted sensible load in W required to meet the current zone thermostat setpoint. A positive value indicates a heating load, a negative value indicates a cooling load. This is calculated and reported from the Predict step in the Zone Predictor-Corrector module. For nearly all equipment types, the Predictor-Corrector evaluates the active heating and/or cooling setpoints, determines if the zone requires heating or cooling or is in the deadband, and then passes this single load to the equipment. This value is not multiplied by zone or group multipliers.
+
+\paragraph{Zone Predicted Sensible Load to Heating Setpoint Heat Transfer Rate {[}W{]}}\label{zone-predicted-sensible-load-to-heating-setpoint-heat-transfer-rate-w}
+
+This is the predicted sensible load in W required to meet the current zone thermostat heating setpoint. A positive value indicates a heating load, a negative value indicates a cooling load. This is calculated and reported from the Predict step in the Zone Predictor-Corrector module. This value is not multiplied by zone or group multipliers.
+
+\paragraph{Zone Predicted Sensible Load to Cooling Setpoint Heat Transfer Rate {[}W{]}}\label{zone-predicted-sensible-load-to-cooling-setpoint-heat-transfer-rate-w}
+
+This is the predicted sensible load in W required to meet the current zone thermostat cooling setpoint. A positive value indicates a heating load, a negative value indicates a cooling load. This is calculated and reported from the Predict step in the Zone Predictor-Corrector module. This value is not multiplied by zone or group multipliers.
+
+\paragraph{\texorpdfstring{Zone Thermostat Control Type {[]}}{Zone Thermostat Control Type }}\label{zone-thermostat-control-type}
+
+This is the current zone thermostat control type (0 through 4). This value is set at each zone timestep. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
+
+\paragraph{Zone Thermostat Heating Setpoint Temperature {[}C{]}}\label{zone-thermostat-heating-setpoint-temperature-c}
+
+This is the current zone thermostat heating setpoint in degrees C. If there is no heating thermostat active, then the value will be 0. This value is set at each zone timestep. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
+
+When the Thermostat:StagedDualSetpoint object is applied to the current zone, this output variable reports staged zone heating setpoint. When the staged number is not equal to zero, both staged heating and cooling setpoints are the same. When no cooling or heating is required, the staged heating setpoint is equal to the scheduled heating setpoint 0.5 * heating throttling range, and the staged cooling setpoint is equal to the scheduled cooling setpoint + 0.5 * cooling throttling range.
+
+\paragraph{Zone Thermostat Cooling Setpoint Temperature {[}C{]}}\label{zone-thermostat-cooling-setpoint-temperature-c}
+
+This is the current zone thermostat cooling setpoint in degrees C. If there is no cooling thermostat active, then the value will be 0. This value is set at each zone timestep. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
+
+When the Thermostat:StagedDualSetpoint object is applied to the current zone, this output variable reports staged zone cooling setpoint. When the staged number is not equal to zero, both staged heating and cooling setpoints are the same. When no cooling or heating is required, the staged heating setpoint is equal to the scheduled heating setpoint 0.5 * heating throttling range, and the staged cooling setpoint is equal to the scheduled cooling setpoint + 0.5 * cooling throttling range.
+
+\paragraph{\texorpdfstring{Zone Thermostat Stage Number {[]}}{Zone Thermostat Stage Number }}\label{zone-thermostat-stage-number}
+
+This is the current zone thermostat stage number when the ZoneControl:Thermostat:StagedDualSetpoint object is specified in this zone. When no heating or cooling is required, the stage number is set to 0. When heating is required, the stage number is positive. When cooling is required, the stage number is negative. The absolute number is sent to the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object to specify the speed number accordingly.
+
+\paragraph{Zone Heating Setpoint Not Met Time {[}hr{]}}\label{zone-heating-setpoint-not-met-time-hr}
+
+Hours when the zone temperature is lower than 0.2 (default) degrees C below the heating setpoint. See the OutputControl:ReportingTolerances object to change the reporting range from 0.2 degrees C.
+
+\paragraph{Zone Heating Setpoint Not Met While Occupied Time {[}hr{]}}\label{zone-heating-setpoint-not-met-while-occupied-time-hr}
+
+Hours when the zone temperature is lower than 0.2 (default) degrees C below the heating setpoint and when people are present in the zone. To change the reporting range from 0.2 degrees C, see the OutputControl:ReportingTolerances object.
+
+\paragraph{Zone Cooling Setpoint Not Met Time {[}hr{]}}\label{zone-cooling-setpoint-not-met-time-hr}
+
+Hours when the zone temperature is greater than 0.2 (default) degrees C above the cooling setpoint. See the OutputControl:ReportingTolerances object to change the reporting range from 0.2 degrees C.
+
+\paragraph{Zone Cooling Setpoint Not Met While Occupied Time {[}hr{]}}\label{zone-cooling-setpoint-not-met-while-occupied-time-hr}
+
+Hours when the zone temperature is greater than 0.2 (default) degrees C above the cooling setpoint and when people are present in the zone. To change the reporting range from 0.2 degrees C, see the OutputControl:ReportingTolerances object.
+
+\paragraph{Facility Heating Setpoint Not Met Time {[}hr{]}}\label{facility-heating-setpoint-not-met-time-hr}
+
+Hours when the zone temperature is lower than 0.2 (default) degrees C below the heating setpoint in any one or more zones. See the OutputControl:ReportingTolerances object to change the reporting range from 0.2 degrees C.
+
+\paragraph{Facility Heating Setpoint Not Met While Occupied Time {[}hr{]}}\label{facility-heating-setpoint-not-met-while-occupied-time-hr}
+
+Hours when the zone temperature is lower than 0.2 (default) degrees C below the heating setpoint and when people are present in any one or more zones. To change the reporting range from 0.2 degrees C, see the OutputControl:ReportingTolerances object.
+
+\paragraph{Facility Cooling Setpoint Not Met Time {[}hr{]}}\label{facility-cooling-setpoint-not-met-time-hr}
+
+Hours when the zone temperature is greater than 0.2 (default) degrees C above the cooling setpoint in any one or more zones. See the OutputControl:ReportingTolerances object to change the reporting range from 0.2 degrees C.
+
+\paragraph{Facility Cooling Setpoint Not Met While Occupied Time {[}hr{]}}\label{facility-cooling-setpoint-not-met-while-occupied-time-hr}
+
+Hours when the zone temperature is greater than 0.2 (default) degrees C above the cooling setpoint and when people are present in any one or more zones. To change the reporting range from 0.2 degrees C, see the OutputControl:ReportingTolerances object.
+
+\paragraph{Zone Oscillating Temperatures Time{[}hr{]}}\label{zone-oscillating-temperatures-timehr}
+
+Hours when the temperature in the zone is oscillating back and forth. Oscillation is defined as times when the three differences between zone temperatures during successive timesteps are greater in magnitude than 0.15 degrees C and the sign of the differences changes from positive to negative to positive or from negative to positive to negative.
+
+This may indicate a simulation with reduced reliability during the oscillation. Some oscillating hours should be expected in all simulations but excessive oscillations call into question the overall validity of the results. If excessive oscillations are occurring, try reducing the minimum system timestep (see ConvergenceLimits object) and the zone timestep (see the TimeStep object). Reducing these timestep lengths does increase the total computer time needed to complete the simulation. Having the zone timestep and the minimum system timestep the same length of time can also cause more oscillations. What amount of oscillations is considered excessive is difficult to quantify. One approach is comparing the number of oscillations to the case with 15 minute zone timesteps (4 per hour) and 1 minute minimum system timesteps. Often this variable is used as an indicator of the validity of the results when trying to decrease the time needed to perform the simulation.
+
+\paragraph{Facility Any Zone Oscillating Temperatures Time{[}hr{]}}\label{facility-any-zone-oscillating-temperatures-timehr}
+
+Hours when any zone in the building has oscillations. See Zone Oscillating Temperatures Time definition above.
+
+\subsection{Zone Thermostat Setpoints}\label{zone-thermostat-setpoints}
+
+The syntax for the current set of four zone thermostat setpoint objects is given below. In each case, the keyword is accompanied by an identifying name and either one or two schedule names (depending on whether the control is a single or dual setpoint control). The schedule defines a temperature setpoint for the control type. The schedule would be defined through the standard schedule syntax described earlier in this document. For an uncontrolled zone no thermostat is specified or necessary.
+
+\subsection{ThermostatSetpoint:SingleHeating}\label{thermostatsetpointsingleheating}
+
+This would be for a heating only thermostat. The setpoint can be scheduled and varied throughout the simulation but only heating is allowed with this control type.
+
+\subsubsection{Inputs}\label{inputs-1-051}
+
+\paragraph{Field: Name}\label{field-name-1-049}
+
+Unique name for this control type.
+
+\paragraph{Field: Setpoint Temperature Schedule Name}\label{field-setpoint-temperature-schedule-name-002}
+
+The name of the associated schedule. Values in the schedule are temperatures \{C\}.
+
+\subsection{ThermostatSetpoint:SingleCooling}\label{thermostatsetpointsinglecooling}
+
+This would be for a cooling only thermostat. The setpoint can be scheduled and varied throughout the simulation but only cooling is allowed.
+
+\subsubsection{Inputs}\label{inputs-2-047}
+
+\paragraph{Field: Name}\label{field-name-2-044}
+
+Unique name for this control type.
+
+\paragraph{Field: Setpoint Temperature Schedule Name}\label{field-setpoint-temperature-schedule-name-1-000}
+
+The name of the associated schedule. Values in the schedule are temperatures \{C\}.
+
+\subsection{ThermostatSetpoint:SingleHeatingOrCooling}\label{thermostatsetpointsingleheatingorcooling}
+
+This would be for heating and cooling thermostat but only heating or cooling can be scheduled at any given time period. The setpoint can be scheduled and varied throughout the simulation for both heating and cooling.
+
+\subsubsection{Inputs}\label{inputs-3-042}
+
+\paragraph{Field: Name}\label{field-name-3-038}
+
+Unique name for this control type.
+
+\paragraph{Field: Setpoint Temperature Schedule Name}\label{field-setpoint-temperature-schedule-name-2}
+
+The name of the associated schedule. Values in the schedule are temperatures \{C\}.
+
+\subsection{ThermostatSetpoint:DualSetpoint}\label{thermostatsetpointdualsetpoint}
+
+This would be for heating and cooling thermostat where both a heating and cooling setpoint can be scheduled for any given time period. The setpoint can be scheduled and varied throughout the simulation for both heating and cooling.
+
+\subsubsection{Inputs}\label{inputs-4-039}
+
+\paragraph{Field: Name}\label{field-name-4-034}
+
+Unique name for this control type.
+
+\paragraph{Field: Heating Setpoint Temperature Schedule Name}\label{field-heating-setpoint-temperature-schedule-name-000}
+
+The heating temperature schedule. Values in the schedule are temperatures \{C\}.
+
+\paragraph{Field: Cooling Setpoint Temperature Schedule Name}\label{field-cooling-setpoint-temperature-schedule-name}
+
+The cooling temperature schedule. Values in the schedule are temperatures \{C\}.
+
+Examples of these statements in an IDF are:
+
+\begin{lstlisting}
+
+ThermostatSetpoint:SingleHeating, Heating Setpoint with SB, Heating Setpoints;
+  ThermostatSetpoint:SingleCooling, Cooling Setpoint with SB, Cooling Setpoints;
+  ThermostatSetpoint:SingleHeatingOrCooling, Heating Cooling Setpoint Sched, Heating Cooling Setpoints;
+  ThermostatSetpoint:DualSetpoint, VAV Setpoints, Heating Setpoints, Cooling Setpoints;
+\end{lstlisting}
+
+\subsection{ZoneControl:Thermostat:OperativeTemperature}\label{zonecontrolthermostatoperativetemperature}
+
+This object is used to modify the program s behavior for ZoneControl:Thermostat objects. One input object is used for each thermal zone to indicate if that zone s thermostat control mode should be overridden to effect operative temperature control rather than traditional air temperature control. Zone Control:Thermostatic and related set point objects also need to be included in the input file. When this object is used, the zone can be controlled by a weighted mixture of radiant and air temperatures (rather than just air temperatures).
+
+This thermostatic operative temperature, \({T_{OP}}\) , is defined as:
+
+\begin{equation}
+{T_{OP}} = \gamma {T_{MRT}} + (1 - \gamma ){T_{drybulb}}
+\end{equation}
+
+where,
+
+\(\gamma\) is the radiative fraction,
+
+\({T_{MRT}}\) is the mean radiant temperature for the thermal zone, and
+
+\({T_{drybulb}}\) is the mean zone air temperature.
+
+The radiative fraction \(\gamma\) is selected by the user and can be scheduled to vary during the simulation. A typical value is 0.5. The maximum value needs to be less than 0.9 and the minimum is 0.0. A value of 0.0 is the same as controlling on only zone air temperature. If air velocities are higher than 0.2 m/s, then lower values for radiative fraction might apply. Niu and Burnett (1998) cite International Standard ISO 77300 in recommending the values for this fraction listed in the following table.
+
+% table 28
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Radiative Fraction vs Air Velocity (Operative Temperature Control) \label{table:radiative-fraction-vs-air-velocity-operative}} \tabularnewline
+\toprule 
+Air Velocity (m/s) & <  0.2 & 0.2 to 0.6 & 0.6 to 1.0 \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Radiative Fraction vs Air Velocity (Operative Temperature Control)} \tabularnewline
+\toprule 
+Air Velocity (m/s) & <  0.2 & 0.2 to 0.6 & 0.6 to 1.0 \tabularnewline
+\midrule
+\endhead
+\(\gamma\) & 0.5 & 0.4 & 0.3 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Reference: J. Niu and J. Burnett. 1998. Integrating Radiant/Operative Temperature Controls into Building Energy Simulations. ASHRAE Transactions Vol. 104. Part 2. page 210. ASHRAE. Atlanta, GA.
+
+\subsubsection{Inputs}\label{inputs-5-034}
+
+\paragraph{Field: Thermostat Name}\label{field-thermostat-name-000}
+
+Name of ZoneControl:Thermostat object defined elsewhere in the input file whose operation is to be modified to effect control based on operative temperature. If the ZoneControl:Thermostat references a ZoneList (set of zones) then, this operative temperature thermostat will be applied to each of those zones. If only a single thermostat/zone is desired, then the name to be put here is \textless{}zone name\textgreater{} \textless{}Thermostat Name\textgreater{} where the Thermostat name is the thermostat that referenced the set of zones.
+
+\paragraph{Field: Radiative Fraction Input Mode}\label{field-radiative-fraction-input-mode}
+
+This field controls whether the input for radiative fraction is a constant value or if it is entered using a schedule. Enter \textbf{Constant} here to use a fixed radiative fraction defined in the following field. Enter \textbf{Scheduled} to vary the radiative fraction according to the schedule named in the second field below.
+
+\paragraph{Field: Fixed Radiative Fraction}\label{field-fixed-radiative-fraction}
+
+This is the fraction, \(\gamma\), of the operative temperature that is due to the mean radiant temperature in the zone. This field is used by the program if the previous field is set to \textbf{Constant}.
+
+\paragraph{Field: Radiative Fraction Schedule Name}\label{field-radiative-fraction-schedule-name}
+
+This field contains the name of a schedule, defined elsewhere, that determines the value for radiative fraction \(\gamma\) during the simulation period. This schedule should have fractional values from 0.0 to 0.9. When the value of this schedule is 0.0, the controlling will be equivalent to control based only on zone air temperature. This field is used by the program if the Input Mode field is set to \textbf{Scheduled}.
+
+Note that by setting the values in this schedule separately for design days, the user can control how operative temperature control is applied during autosizing. (Operative temperature control tends to increase the equipment capacities calculated during sizing.)
+
+An example of this object follows.
+
+\begin{lstlisting}
+ZoneControl:Thermostat:OperativeTemperature,
+  Zone 1 Thermostat,    !- ZoneControl:Thermostat Name
+  Constant,             !- Radiative Fraction Input Mode
+  0.5,                  !- Fixed Radiative Fraction
+  ;                     !- Radiative Fraction Schedule
+\end{lstlisting}
+
+Global operative temperature applied to all zones for a global thermostat:
+
+\begin{lstlisting}
+ZoneList,AllControlledZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
+
+ZoneControl:Thermostat,
+  AllControlledZones Thermostat,        !- Name
+  AllControlledZones,                   !- Zone Name
+  Zone Control Type Sched,              !- Control Type Schedule Name
+  ThermostatSetpoint:SingleCooling,     !- Control 1 Object Type
+  CoolingSetPoint,                      !- Control 1 Name
+  ThermostatSetpoint:SingleHeating,     !- Control 2 Object Type
+  HeatingSetpoint,                      !- Control 2 Name
+  ThermostatSetpoint:DualSetpoint,      !- Control 3 Object Type
+  DualSetPoint;                         !- Control 3 Name
+
+
+ZoneControl:Thermostat:OperativeTemperature,
+  AllControlledZones Thermostat,        !- Thermostat Name
+  CONSTANT,                             !- Radiative Fraction Input Mode
+  0.4;                                  !- Fixed Radiative Fraction
+\end{lstlisting}
+
+Global operative temperature referencing a single zone from the list:
+
+\begin{lstlisting}
+ZoneList,AllControlledZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
+\end{lstlisting}
+
+\begin{lstlisting}
+ZoneControl:Thermostat,
+  AllControlledZones Thermostat,        !- Name
+  AllControlledZones,                   !- Zone Name
+  Zone Control Type Sched,              !- Control Type Schedule Name
+  ThermostatSetpoint:SingleCooling,     !- Control 1 Object Type
+  CoolingSetPoint,                      !- Control 1 Name
+  ThermostatSetpoint:SingleHeating,     !- Control 2 Object Type
+  HeatingSetpoint,                      !- Control 2 Name
+  ThermostatSetpoint:DualSetpoint,      !- Control 3 Object Type
+   DualSetPoint;                        !- Control 3 Name
+
+ZoneControl:Thermostat:OperativeTemperature,
+  SPACE3-1 AllControlledZones Thermostat, !- Thermostat Name
+  CONSTANT,                               !- Radiative Fraction Input Mode
+  0.4;                                    !- Fixed Radiative Fraction
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-032}
+
+\begin{itemize}
+\tightlist
+\item
+  Zone,Average,Zone Thermostat Operative Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{Zone Thermostat Operative Temperature {[}C{]}}\label{zone-thermostat-operative-temperature-c}
+
+Operative temperature (OT) is a weighted mixture of Zone Mean Air Temperature (MAT) and Zone Mean Radiant Temperature (MRT), using the current value of Radiative Fraction (RF): OT = (1-RF)*MAT + RF*MAT. This output variable does not include the direct effect of high temperature radiant systems. See also Zone Operative Temperature.
+
+\subsection{ZoneControl:Thermostat:TemperatureAndHumidity}\label{zonecontrolthermostattemperatureandhumidity}
+
+This object is used to modify the behavior of ZoneControl:Thermostat objects (control types ThermostatSetpoint:SingleCooling and ThermostatSetpoint:DualSetpoint only) based on zone air humidity conditions. Specifically, this TemperatureAndHumidity zone control resets the ZoneControl:Thermostat s cooling setpoint temperature downward when the zone air relative humidity exceeds the Dehumidifying Relative Humidity Setpoint defined in this object. The reduced cooling setpoint temperature typically results in longer cooling coil runtimes and additional dehumidification. The rate at which the cooling setpoint temperature is reduced is dictated by the user-specified Overcool Control Ratio. The maximum reduction in cooling setpoint temperature is defined by the user-entered OverCool Range (user choice of a constant value for the entire simulation or a schedule that can define how the overcool range varies over time). For details regarding the calculations, see the EnergyPlus Engineering Reference.
+
+Note: As described above, this ZoneControl:Thermostat:TemperatureAndHumidity control object modifies the cooling setpoint temperature of ZoneControl:Thermostat objects. The ZoneControl:Thermostat:TemperatureAndHumidity object works independently of the ZoneControl:Humidistat object; that is, it does not replace the need for, or coordinate its input fields with, ZoneControl:Humidistat objects that are required for other types of high humidity control (e.g., ZoneControl:Humidstat objects are required for ZoneHVAC:Dehumidifier:DX objects, AirLoopHVAC:Unitary* objects with CoolReheat or MultiMode dehumidification control types, etc.)
+
+\subsubsection{Inputs}\label{inputs-6-031}
+
+\paragraph{Field: Thermostat Name}\label{field-thermostat-name-1}
+
+Name of ZoneControl:Thermostat object defined elsewhere in the input file whose operation is to be modified to effect temperature control based on zone air humidity conditions. If the ZoneControl:Thermostat references a ZoneList (set of zones), then simply enter the name of the ZoneControl:Thermostat object and this TemperatureAndHumidity thermostat control will be applied to all zones in the ZoneList. If the ZoneControl:Thermostat references a ZoneList but it is desired that only a single zone within the ZoneList be controlled based on TemperatureAndHumidity control, then the name to be put here is \textless{}zone name\textgreater{} \textless{}Thermostat Name\textgreater{} where the Thermostat Name is the name of the ZoneControl:Thermostat object.
+
+\paragraph{Field: Dehumidifying Relative Humidity Setpoint Schedule Name}\label{field-dehumidifying-relative-humidity-setpoint-schedule-name}
+
+Name of a schedule that defines the dehumidifying relative humidity setpoint, expressed as a percentage (0-100), for each timestep of the simulation. This input field is required. This input field has absolutely no relationship or influence on the Dehumidifying Relative Humidity Setpoint Schedule Name optional input field in the ZoneControl:Humidistat object.
+
+\paragraph{Field:Dehumidification Control Type}\label{fielddehumidification-control-type}
+
+This input field defines what type of dehumidification control is active during the simulation. Valid control types are None and Overcool. The default is Overcool if this field is left blank. Overcool resets the thermostat s cooling setpoint temperature lower based on the zone air relative humidity level. None means no overcooling (i.e., traditional zone air temperature control based on the associated ZoneControl:Thermostat object {[}Thermostat Name input field above{]} will be in effect).
+
+\paragraph{Field: Overcool Range Input Method}\label{field-overcool-range-input-method}
+
+This field controls whether the input for the overcool (temperature) range is a constant value or if it is entered using a schedule. Enter \textbf{Constant} here to use a constant overcool range defined in the Overcool Constant Range input field below. Enter \textbf{Scheduled} to vary the overcool range according to the schedule named in the Overcool Range Schedule Name input field below. The default is \textbf{Constant} if this field is left blank.
+
+\paragraph{Field: Overcool Constant Range}\label{field-overcool-constant-range}
+
+This field specifies a fixed maximum overcool temperature range for cooling setpoint temperature reduction for zone overcool dehumidification in units of deltaC. This field is used if the Overcool Range Input Method is specified as \textbf{Constant}. The Overcool dehumidification control type only works with ZoneControl:Thermostat control types ThermostatSetpoint:SingleCooling and ThermostatSetpoint:DualSetpoint . For ThermostatSetpoint:DualSetpoint , the model will use the \textbf{smaller} of the Overcool Constant Range input value or the difference between the cooling and heating setpoint temperatures specified in the ThermostatSetpoint:DualSetpoint object. The Overcool Constant Range must be greater than or equal to zero with a maximum value of 3 °C. A value of 0.0 indicates no zone air overcooling. The default value is 1.7 °C (3 °F) if this input field is left blank.
+
+\paragraph{Field: Overcool Range Schedule Name}\label{field-overcool-range-schedule-name}
+
+This field contains the name of a schedule, defined elsewhere, that determines the value for the overcool range during the simulation period. This schedule should contain values from 0.0 to \textless{} = 3.0 (deltaC). When the value of this schedule is 0.0, the zone air temperature control will be based only on zone air dry-bulb temperature (i.e., no zone overcooling). This field is used by the program if the Overcool Range Input Method field is set to \textbf{Scheduled}. Overcool dehumidification control type only works with ZoneControl:Thermostat control types ThermostatSetpoint:SingleCooling and ThermostatSetpoint:DualSetpoint . For ThermostatSetpoint:DualSetpoint , the model will use the \textbf{smaller} of the Overcool Range values specified in this schedule or the difference between the cooling and heating setpoint temperatures specified in the ThermostatSetpoint:DualSetpoint object.
+
+Note that by setting the values in this schedule separately for design days, the user can control how Overcool Dehumidification Control is applied during autosizing. (Overcool dehumidification control tends to increase the cooling equipment capacities calculated during sizing.)
+
+\paragraph{Field:Overcool Control Ratio}\label{fieldovercool-control-ratio}
+
+The value of this input field is used to adjust the cooling setpoint temperature (established by the associated ZoneControl:Thermostat object) downward based on the difference between the zone air relative humidity level and the Dehumidifying Relative Humidity Setpoint. This input field is only used with Dehumidification Control Type = Overcool. Input values must be greater than or equal to 0.0 \%RH/K. The default value is 3.6 if this field is left blank.
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+ZoneControl:Thermostat:TemperatureAndHumidity,
+  Zone Thermostat,                                 !- Thermostat Name
+  Seasonal Relative Humidity Sch,   !- Dehumidifying Relative Humidity Setpoint Schedule Name
+  Overcool,                                               !- Dehumidification Control Type
+  Constant,                                               !- Overcool Range Input Method
+  1.7,                                         !- Overcool Constant Range {deltaC}
+  ,                                               !- Overcool Range Schedule Name
+  3.0;                                         !- Overcool Control Ratio {percent/K}
+\end{lstlisting}
+
+\subsection{ZoneControl:Thermostat:StagedDualSetpoint}\label{zonecontrolthermostatstageddualsetpoint}
+
+The thermostatic zone control staged dual setpoint object is used to control a zone to a specified temperature based on multiple stages. The other types of ZoneControl:Thermostat objects reference a control type schedule and one or more control type objects which in turn reference one or more setpoint schedules. This control object does not require a control type schedule and associated one or more control type objects. Instead, the object is defined as a Dual Setpoint type only and has two fields to provide heating and cooling setpoints. The object also provides two fields to specify heating and cooling throttling temperature ranges, so that predicted zone loads may be varied within the throttling ranges for both heating and cooling. The number of stages for both heating and cooling varies from 1 to 4 for the time being to match the number of speeds used in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. The number of stages may be expanded later to accommodate other objects with the number of speeds higher than 4. The object requires inputs temperature offsets for both heating and cooling based on the number of stages. The stage number is determined by the temperature difference between the setpoint and zone temperature at the previous time step, and offset values. The staged number will be assigned to the speed number for the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed system type.
+
+It should be pointed out that If this object and other zone control thermostat and humidistat are assigned to the same controlled zone, this object takes precedence when the controlled zone is specified in the Controlling Zone or Thermostat Location field of the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object.
+
+\subsubsection{Inputs}\label{inputs-7-030}
+
+\paragraph{Field: Name}\label{field-name-5-028}
+
+Unique identifying name for the staged dual-setpoint thermostat.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-1-001}
+
+Name of the zone or set of zones that is being controlled. When the ZoneList option is used then this thermostat definition is applied to each of the zones in the zone list effecting a global definition for thermostatic control in the zone.
+
+\paragraph{Field: Number of Heating Stages}\label{field-number-of-heating-stages}
+
+This numerical field defines the number of heating stages, and must be less than or equal to the number of heating speeds defined in the associated heating coil, such as Coil:Heating:DX:MultiSpeed. The value for this input field defines the number of heating temperature offsets that must be defined for heating in the fields below. The minimum value for this field is one (1) and the maximum value is four (4).
+
+\paragraph{Field:Heating Temperature Setpoint Schedule Name}\label{fieldheating-temperature-setpoint-schedule-name}
+
+The name of the associated schedule to specify heating temperature setpoint. Values in the schedule are temperatures \{C\}.
+
+\paragraph{Field:Heating Throttling Temperature Range}\label{fieldheating-throttling-temperature-range}
+
+This numeric field defines the heating throttling temperature range in the units of deltaC. When the zone temperature at the previous time step is below the heating temperature setpoint, the zone heating setpoint will be set to the heating temperature setpoint + 0.5 * heating throttling temperature range. Otherwise, the zone heating setpoint will be set to the heating temperature setpoint - 0.5 * heating throttling temperature range. The zone heating setpoint is used in the predictor to calculate how much the heating system load is needed to maintain the zone at the heating setpoint.
+
+\paragraph{Field: Stage 1 Heating Temperature Offset}\label{field-stage-1-heating-temperature-offset}
+
+This numeric field defines the heating temperature offset in the units of deltaC for Stage 1. The value entered here must be equal to or less than 0. The heating temperature offset fields are used to determine the heating stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference between the heating setpoint and the controlled zone temperature at previous time step is less than Stage 1 offset value and greater than Stage 2 offset value, the heating stage number is 1. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 1 is specified.
+
+\paragraph{Field: Stage 2 Heating Temperature Offset}\label{field-stage-2-heating-temperature-offset}
+
+This numeric field defines the heating temperature offset in the units of deltaC for Stage 2. The value entered here must be less than the value at the previous field: Stage 1 Heating Temperature Offset. The heating temperature offset fields are used to determine the heating stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference between the heating setpoint and the controlled zone temperature at previous time step is less than Stage 2 offset value and greater than Stage 3 offset value, the heating stage number is 2. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 2 is specified.
+
+\paragraph{Field: Stage 3 Heating Temperature Offset}\label{field-stage-3-heating-temperature-offset}
+
+This numeric field defines the heating temperature offset in the units of deltaC for Stage 3. The value entered here must be less than the value at the previous field: Stage 3 Heating Temperature Offset. The heating temperature offset fields are used to determine the heating stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference between the heating setpoint and the controlled zone temperature at previous time step is less than Stage 3 offset value and greater than Stage 4 offset value, the heating stage number is 3. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 3 is specified.
+
+Note: If the stage number is not equal to the number of heating speed in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object, the minimum value is set to the speed number for the heat pump object.
+
+\paragraph{Field: Stage 4 Heating Temperature Offset}\label{field-stage-4-heating-temperature-offset}
+
+This numeric field defines the heating temperature offset in the units of deltaC for Stage 4. The value entered here must be less than the value at the previous field: Stage 4 Heating Temperature Offset. The heating temperature offset fields are used to determine the heating stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference between the heating setpoint and the controlled zone temperature at previous time step is less than Stage 4 offset value, the heating stage number is 4. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 4 is specified.
+
+Note: If the stage number is not equal to the number of heating speed in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object, the minimum value is set to the speed number for the heat pump object.
+
+\paragraph{Field: Number of Cooling Stages}\label{field-number-of-cooling-stages}
+
+This field defines the number of cooling stages, and must be less than or equal to the number of cooling speeds defined in the associated cooling coil, such as Coil:Cooling:DX:MultiSpeed. The value for this input field defines the number of cooling temperature offsets that must be defined for cooling in the fields below. The minimum value for this field is one (1) and the maximum value is four (4).
+
+\paragraph{Field:Cooling Temperature Setpoint Base Schedule Name}\label{fieldcooling-temperature-setpoint-base-schedule-name}
+
+The name of the associated schedule to specify cooling temperature base setpoint. Values in the schedule are temperatures \{C\}.
+
+\paragraph{Field:Cooling Throttling Temperature Range}\label{fieldcooling-throttling-temperature-range}
+
+This numeric field defines the cooling throttling temperature range in the units of deltaC. When the zone temperature at the previous time step is above the cooling temperature setpoint, the zone cooling setpoint will be set to the cooling temperature setpoint - 0.5 * cooling throttling temperature range. Otherwise, the zone cooling setpoint will be set to the cooling temperature setpoint + 0.5 * cooling throttling temperature range. The zone cooling setpoint is used in the predictor to calculate how much the cooling system load is needed to maintain the zone at the cooling setpoint.
+
+\paragraph{Field: Stage 1 Cooling Temperature Offset}\label{field-stage-1-cooling-temperature-offset}
+
+This numeric field defines the cooling temperature offset in the units of deltaC for Stage 1. The value entered here must be equal to or greater than 0. The cooling temperature offset fields are used to determine the cooling stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference of the cooling setpoint and the controlled zone temperature at previous time step is greater than Stage 1 offset value and less than Stage 2 offset value, the cooling stage number is 1. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 1 is specified.
+
+\paragraph{Field: Stage 2 Cooling Temperature Offset}\label{field-stage-2-cooling-temperature-offset}
+
+This numeric field defines the cooling temperature offset in the units of deltaC for Stage 2. The value entered here must be greater than the value at the previous field: Stage 1 Cooling Temperature Offset. When the number of cooling stage is equal to 1, this filed is not used in the program. The cooling temperature offset fields are used to determine the cooling stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference of the cooling setpoint and the controlled zone temperature at previous time step is greater than Stage 2 offset value and less than Stage 3 offset value, the cooling stage number is 2. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 2 is specified.
+
+\paragraph{Field: Stage 3 Cooling Temperature Offset}\label{field-stage-3-cooling-temperature-offset}
+
+This numeric field defines the cooling temperature offset in the units of deltaC for Stage 3. The value entered here must be greater than the value at the previous field: Stage 3 Cooling Temperature Offset. When the number of cooling stage is less than 3, this filed is not used in the program. The cooling temperature offset fields are used to determine the cooling stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference of the cooling setpoint and the controlled zone temperature at previous time step is greater than Stage 3 offset value and less than Stage 4 offset value, the cooling stage number is 3. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 3 is specified.
+
+Note: If the stage number is not equal to the number of cooling speed in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object, the minimum value is set to the speed number for the heat pump object.
+
+\paragraph{Field: Stage 4 Cooling Temperature Offset}\label{field-stage-4-cooling-temperature-offset}
+
+This numeric field defines the cooling temperature offset in the units of deltaC for Stage 4. The value entered here must be greater than the value at the previous field: Stage 4 Cooling Temperature Offset. When the number of cooling stage is less than 4, this filed is not used in the program. The cooling temperature offset fields are used to determine the cooling stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference of the cooling setpoint and the controlled zone temperature at previous time step is greater than Stage 4 offset value, the cooling stage number is 4. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 4 is specified.
+
+Note: If the stage number is not equal to the number of cooling speed in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object, the minimum value is set to the speed number for the heat pump object.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+ZoneControl:Thermostat:StagedDualSetpoint,
+  ZoneThermostat,                   !- Name
+  AllZones,                               !- Zone or ZoneList Name
+  2,                                             !- Number of Heating Stages
+  Heating Setpoints,             !- Heating Temperature Setpoint Schedule Name
+  1.1,                                         !- Heating Throttling Temperature Range {deltaC}
+  0.0,                                         !- Stage 1 Heating Temperature Offset {deltaC}
+  -0.5,                                       !- Stage 2 Heating Temperature Offset {deltaC}
+  -1.0,                                       !- Stage 3 Heating Temperature Offset {deltaC}
+  -1.5,                                       !- Stage 4 Heating Temperature Offset {deltaC}
+  4,                                             !- Number of Cooling Stages
+  Cooling Setpoints,             !- Cooling Setpoint Temperature Schedule Name
+  1.1,                                         !- Cooling Throttling Temperature Range {deltaC}
+  0.0,                                         !- Stage 1 Cooling Temperature Offset {deltaC}
+  1.0,                                         !- Stage 2 Cooling Temperature Offset {deltaC}
+  2.0,                                         !- Stage 3 Cooling Temperature Offset {deltaC}
+  3.0;                                         !- Stage 4 Cooling Temperature Offset {deltaC}
+\end{lstlisting}
+
+\subsection{ZoneControl:Humidistat}\label{zonecontrolhumidistat}
+
+The humidistat zone control object is used to control a zone to a single relative humidity setpoint schedule, or to dual humidity setpoint schedules (humidifying/ dehumidifying setpoints with deadband). The single setpoint humidistat requires single setpoint input only, and the dual-setpoint humidistat requires inputs of both humidifying and dehumidifying setpoints. The schedules consist of relative humidities, expressed as a percentage (0-100), to be used during the simulation for that zone s moisture prediction calculation. Only one humidistat control statement can be specified for each zone. For a single setpoint humidistat, if the zone relative humidity is below the control relative humidity setpoint and the equipment specified can humidify then that equipment will try and meet the zone s humidification load. The opposite is true if the zone relative humidity is above the control relative humidity setpoint and the equipment can dehumidify. For a dual setpoint humidistat, if the zone relative humidity is below the \textbf{humidifying} relative humidity setpoint and the equipment specified can humidify then that equipment will try and meet the zone s humidification load. The opposite is true if the zone relative humidity is above the \textbf{dehumidifying} relative humidity setpoint and the equipment can dehumidify.
+
+If the ZoneControl:Humidistat is used by a furnace or unitary system (Ref. Furnace and Unitary Systems) no other objects are required. The signal from the humidistat is used directly by that component. If the Zone Control:Humidistat object is used to control a Humidifier or used in conjunction with a Controller:WaterCoil object with control variable \textbf{TemperatureAndHumidityRatio} or \textbf{HumidityRatio}, the following objects are required to determine a setpoint for those components for a single setpoint humidistat:
+
+\begin{itemize}
+\item
+  SetpointManager:SingleZone:Humidity:Minimum
+\item
+  SetpointManager:MultiZone:MinimumHumidity:Average
+\item
+  SetpointManager:MultiZone:MaximumHumidity:Average
+\item
+  SetpointManager:MultiZone:Humidity:Minimum
+\item
+  SetpointManager:MultiZone:Humidity:Maximum
+\item
+  SetpointManager:SingleZone:Humidity:Minimum
+\end{itemize}
+
+For a dual setpoint humidistat, both a maximum humidity setpoint manager object:
+
+\begin{itemize}
+\item
+  SetpointManager:SingleZone:Humidity:Maximum
+\item
+  SetpointManager:MultiZone:MaximumHumidity:Average
+\item
+  SetpointManager:MultiZone:Humidity:Maximum
+\end{itemize}
+
+and a minimum humidity setpoint manager object:
+
+\begin{itemize}
+\item
+  SetpointManager:SingleZone:Humidity:Minimum
+\item
+  SetpointManager:MultiZone:MinimumHumidity:Average
+\item
+  SetpointManager:MultiZone:Humidity:Minimum
+\end{itemize}
+
+are required to determine the setpoints for the corresponding humidification and dehumidification components.
+
+\subsubsection{Inputs}\label{inputs-8-028}
+
+\paragraph{Field: Name}\label{field-name-6-026}
+
+Unique identifying name for the humidistat.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-014}
+
+Name of the zone that is being controlled.
+
+\paragraph{Field: Humidifying Relative Humidity Setpoint Schedule Name}\label{field-humidifying-relative-humidity-setpoint-schedule-name}
+
+Name of a schedule that defines the humidifying relative humidity setpoint, expressed as a percentage (0-100), for each timestep of the simulation.
+
+\textbf{Note}: If only a single setpoint humidistat is desired, then input the single schedule name in the Humidifying Setpoint Schedule Name field (and leave the Dehumidifying Setpoint Schedule Name blank).
+
+\paragraph{Field: Dehumidifying Relative Humidity Setpoint Schedule Name}\label{field-dehumidifying-relative-humidity-setpoint-schedule-name-1}
+
+Name of a schedule that defines the dehumidifying relative humidity setpoint, expressed as a percentage (0-100), for each timestep of the simulation. This field is optional, only used if a dual setpoint humidistat is to be modeled.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+ZoneControl:Humidistat,
+  Zone 2 Humidistat,             !- Humidistat Name
+  EAST ZONE,                             !- Zone Name
+  Min Rel Hum Set Sch,       !- Humidifying Relative Humidity Setpoint SCHEDULE Name
+  Max Rel Hum Set Sch;       !- Dehumidifying Relative Humidity Setpoint SCHEDULE Name
+\end{lstlisting}
+
+An example schedule for the Zone Control:Humidistat
+
+\begin{lstlisting}
+
+ScheduleTypeLimits,Humidity,0:100,CONTINUOUS;
+
+
+  Schedule:Compact,
+  Min Rel Hum Set Sch,       !- Name
+  Humidity,                               !- ScheduleType
+  Through: 12/31,                   !- Complex Field \#1
+  For: AllDays,                       !- Complex Field \#2
+  Until: 24:00,                       !- Complex Field \#3
+  30.0;                                       !- Complex Field \#4
+  Schedule:Compact,,
+  Max Rel Hum Set Sch,       !- Name
+  Humidity,                               !- ScheduleType
+  Through: 12/31,                   !- Complex Field \#1
+  For: AllDays,                       !- Complex Field \#2
+  Until: 24:00,                       !- Complex Field \#3
+  55.0;                                       !- Complex Field \#4
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-027}
+
+Outputs available from the ZoneControl:Humidistat:
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Predicted Moisture Load Moisture Transfer Rate {[}kgWater/s{]}
+\item
+  HVAC,Average,Zone Predicted Moisture Load to Humidifying Setpoint Moisture Transfer Rate {[}kgWater/s{]}
+\item
+  HVAC,Average,Zone Predicted Moisture Load to Dehumidifying Setpoint Moisture Transfer Rate {[}kgWater/s{]}
+\end{itemize}
+
+\paragraph{Zone Predicted Moisture Load Moisture Transfer Rate {[}kgWater/s{]}}\label{zone-predicted-moisture-load-moisture-transfer-rate-kgwaters}
+
+This is the predicted latent (moisture) load in kg\(_{r}\)/s required to meet the current zone humidistat setpoint. A positive value indicates a humidification load, a negative value indicates a dehumidification load. For a dual setpoint humidistat, the value is zero when the controlled zone s relative humidity is between the defined humidifying and dehumidifying setpoints. This moisture load rate is calculated and reported from the Predict step in the Zone Predictor-Corrector module. For nearly all equipment types, the Predictor-Corrector evaluates the active humidistat setpoints, determines if the zone requires humidification or dehumidification, and then passes this single load to the equipment for the single setpoint humidistat case. This value is not multiplied by zone or group multipliers.
+
+\paragraph{Zone Predicted Moisture Load to Humidifying Setpoint Moisture Transfer Rate {[}kgWater/s{]}}\label{zone-predicted-moisture-load-to-humidifying-setpoint-moisture-transfer-rate-kgwaters}
+
+This is the predicted latent (moisture) load in kg\(_{r}\)/s required to meet the current zone humidistat \textbf{humidifying} setpoint. This is calculated and reported from the Predict step in the Zone Predictor-Corrector module. For nearly all equipment types, the Predictor-Corrector evaluates the active humidistat humidifying setpoints, determines if the zone requires humidification or not, and then passes this load to the equipment for the case of a dual setpoint humidistat (see Zone Predicted Moisture Load Moisture Transfer Rate, above, for single setpoint humidistat case). This value is multiplied by zone or group multipliers.
+
+\paragraph{Zone Predicted Moisture Load to Dehumidifying Setpoint Moisture Transfer Rate {[}kgWater/s{]}}\label{zone-predicted-moisture-load-to-dehumidifying-setpoint-moisture-transfer-rate-kgwaters}
+
+This is the predicted latent (moisture) load in kg\(_{r}\)/s required to meet the current zone humidistat \textbf{dehumidifying} setpoint. This is calculated and reported from the Predict step in the Zone Predictor-Corrector module. For nearly all equipment types, the Predictor-Corrector evaluates the active humidistat humidifying setpoints, determines if the zone requires dehumidification or not, and then passes this load to the equipment for a dual setpoint humidistat (see Zone Predicted Moisture Load Moisture Transfer Rate, above, for single setpoint humidistat case). This value is multiplied by zone or group multipliers.
+
+\subsection{ZoneControl:Thermostat:ThermalComfort}\label{zonecontrolthermostatthermalcomfort}
+
+The thermal comfort zone control provides a method to control a zone to a dry-bulb temperature setpoint based on a thermal comfort model (e.g.~Fanger) and a user-specified thermal comfort setpoint schedule.
+
+This object references a control type schedule and one or more thermal comfort control type objects which in turn reference one or more setpoint schedules. The example at the end of this section illustrates a complete zone thermal comfort control specification including the control type and setpoint schedules. The control type schedule and the list of control type/name pairs are directly related. The schedule defines the type of control that is to be used during for each hour. Valid Control Types are
+
+0 - Uncontrolled (No thermal comfort control)
+
+1 - Single Thermal Comfort Heating Setpoint:Fanger
+
+2 - Single Thermal Comfort Cooling Setpoint:Fanger
+
+3 - Single Thermal Comfort Heating Cooling Setpoint:Fanger
+
+4 - Dual Thermal Comfort Setpoint with Deadband:Fanger
+
+Thus, if the schedule referenced in the ZoneControl:Thermostat:ThermalComfort statement has a value of 4 for a particular hour, this indicates that during that hour ``Dual Thermal Comfort Setpoint with Deadband:Fanger'' is to be used. The specific ``Dual Thermal Comfort Setpoint with Deadband:Fanger'' control object to be used is specified in the list of control type/name pairs. Then the specific control type objects reference the thermal comfort control setpoint schedule to be used. Because only one control can be specified for each control type in a ZoneControl:Thermostat:ThermalComfort statement, there are only four pairs possible in a particular ZoneControl:Thermostat:ThermalComfort type/name list. This is because individual controls can be defined hourly, thus giving the user a full range of flexibility. Since putting in the name of the control type directly in the schedule would be very cumbersome, the control types are assigned a number which is used in the hourly schedule profile.
+
+The ZoneControl:Thermostat:ThermalComfort object can be used alone, or with a ZoneControl:Thermostat object. When both control objects co-exist for a specific zone and the thermal comfort control type value in the thermal comfort control type schedule is non-zero the thermal comfort object will override the value from the zone thermostat object. If the thermal comfort control is specified as Uncontrolled (thermal comfort control type value of 0) for a particular period, then control will revert to thermostat control if specified. If the thermal comfort control is specified as Uncontrolled for a particular period and thermostat control is not specified in the input, then conditions will float.
+
+This object currently allows only Fanger comfort control (Ref. Thermal Comfort in Engineering Reference). It requires one or more people objects in a specific zone. It also requires inputs of Fields \emph{Activity Level Schedule Name, Work Efficiency Schedule Name, Clothing Insulation Schedule Name} and \emph{Air Velocity Schedule Name} in the people object(s). When thermal comfort control is used in a zone, the air velocity entered in the Air Velocity Schedule (Ref. People) should be greater than or equal to 0.1 and less than or equal to 0.5 m/s. A warning message will be issued if thermal comfort control is active and the air velocity is outside this range.
+
+This object reads input PMV values from a given PMV setpoint schedule to calculate a dry-bulb temperature setpoint based on the selected thermal comfort model. The dry-bulb temperature setpoint calculation uses zone air humidity ratio at the previous system timestep and surface temperatures at the previous zone timestep, along with other conditions at the current timestep (e.g., activity level, clothing level and air velocity from the PEOPLE object).
+
+\subsubsection{Inputs}\label{inputs-9-025}
+
+\paragraph{Field: Name}\label{field-name-7-024}
+
+Unique identifying name for this thermal comfort control object.
+
+\paragraph{Field: Zone or ZoneList Name}\label{field-zone-or-zonelist-name-2-000}
+
+Name of the zone or set of zones that is being controlled. When the ZoneList option is used then this thermostat definition is applied to each of the zones in the zone list effecting a global definition for thermostatic control in the zone.
+
+\paragraph{Field: Averaging Method}\label{field-averaging-method}
+
+This choice field specifies the method for calculating the thermal comfort dry-bulb temperature setpoint for a zone with multiple People objects defined. The available choices are: \textbf{SpecificObject}, \textbf{ObjectAverage}, and \textbf{PeopleAverage}. This field is only used when multiple people objects are defined for this zone. If this field is specified as \textbf{PeopleAverage} and the total number of people for all people objects is zero for a particular timestep, the PeopleAverage method cannot be applied and the program automatically uses the ObjectAverage method for this timestep. The default input is \textbf{PeopleAverage}.
+
+\paragraph{Field: Object Name for Specific Object Averaging Method}\label{field-object-name-for-specific-object-averaging-method}
+
+This choice field specifies the name of the specific People object to be used for calculating comfort control when multiple People objects are defined. Only used if the Averaging Method is specified as SpecificObject.
+
+\paragraph{Field: Minimum Dry-Bulb Temperature Setpoint}\label{field-minimum-dry-bulb-temperature-setpoint}
+
+This field specifies the minimum dry-bulb temperature setpoint allowed for this zone. If the dry-bulb temperature calculated by the thermal comfort setpoint model is below this value, then the temperature setpoint will be set to this value. The default value is 0 ËšC.
+
+\paragraph{Field: Maximum Dry-Bulb Temperature Setpoint}\label{field-maximum-dry-bulb-temperature-setpoint}
+
+This field specifies the maximum dry-bulb temperature setpoint allowed for this zone. If the dry-bulb temperature calculated by the thermal comfort setpoint model exceeds this value, then the temperature setpoint will be set to this value. The default value is 50 ËšC.
+
+Note the minimum and maximum temperature setpoint fields are provided to allow the user to bound the temperature control In a specific zone if necessary. These fields are used to provide boundaries for the dry-bulb temperature setpoint calculated at each system timestep when unrealistic inputs have been specified.
+
+\paragraph{Field: Thermal Comfort Control Type Schedule Name}\label{field-thermal-comfort-control-type-schedule-name}
+
+Schedule which defines what type of thermal comfort control is active during each simulation timestep.
+
+Valid Control Types are
+
+0 - No thermal comfort control
+
+1 - Single Thermal Comfort Heating Setpoint:Fanger
+
+2 - Single Thermal Comfort Cooling Setpoint:Fanger
+
+3 - Single Thermal Comfort Heating Cooling Setpoint:Fanger
+
+4 - Dual Thermal Comfort Setpoint with Deadband:Fanger
+
+Each non-zero control type used in this schedule must appear in the following fields which list the specific thermal comfort control objects to be used for this zone.
+
+\paragraph{Field Set (Thermal Comfort Control Object Type, Thermal Comfort Control Name)}\label{field-set-thermal-comfort-control-object-type-thermal-comfort-control-name}
+
+Up to four pairs of Thermal Comfort Control Type and Thermal Comfort Control Type Name fields may be listed to specify which thermal comfort control type objects are used for this zone. This list is not order-dependent, and the position in this list has no impact on the control type schedule. In the control type schedule, a value of 1 always means ``Single Thermal Comfort Heating Setpoint:Fanger'', even if that control type is not first in this list.
+
+\paragraph{Field: Thermal Comfort Control \textless{}x\textgreater{} Object Type}\label{field-thermal-comfort-control-x-object-type}
+
+This field specifies the first control type name to be used for this zone. Available control types are:
+
+ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating
+
+ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling
+
+ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling
+
+ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint
+
+\paragraph{Field: Thermal Comfort Control \textless{}x\textgreater{} Name}\label{field-thermal-comfort-control-x-name}
+
+The unique name for the corresponding thermal comfort control type.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+ZoneControl:Thermostat:ThermalComfort,
+  Zone 2 Comfort Control,                   !- Thermal Comfort Control Name
+  EAST ZONE,                                             !- Zone Name
+  SpecificObject,                                   !- Averaging Method for Zones with Multiple People Objects
+  EAST ZONE,                                             !- Object Name for Specific Object Averaging Method
+  12.8,                                                       !- Minimum dry-bulb temperature setpoint
+  40.0,                                                       !- Maximum dry-bulb temperature setpoint
+  Zone Comfort Control Type Sched, !- Thermal Comfort Control Type SCHEDULE Name
+  Dual Thermal Comfort Setpoint WITH DEADBAND:Fanger, !- Control Type #1
+  Dual Comfort Setpoint;                     !- Thermal Comfort Control Type Name #1
+\end{lstlisting}
+
+Global thermal comfort thermostat example:
+
+\begin{lstlisting}
+
+ZoneList,AllControlledZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
+
+
+  ZoneControl:Thermostat:ThermalComfort,
+  ControlledZones Comfort Control,   !- Name
+  AllControlledZones,                             !- Zone Name
+  PeopleAverage,                     !- Averaging Method
+  ,                                               !- Specific People Name
+  12.8,                                       !- Minimum Dry-Bulb Temperature Setpoint {C}
+  40.0,                                       !- Maximum Dry-Bulb Temperature Setpoint {C}
+  Zone Comfort Control Type Sched,   !- Thermal Comfort Control Type Schedule Name
+  ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating,   !- Thermal Comfort Control 1 Object Type
+  Single Heating Comfort Setpoint,   !- Thermal Comfort Control 1 Name
+  ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling,   !- Thermal Comfort Control 2 Object Type
+  Single Cooling Comfort Setpoint,   !- Thermal Comfort Control 2 Name
+  ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling,   !- Thermal Comfort Control 3 Object Type
+  Single Heating Cooling Comfort Setpoint,   !- Thermal Comfort Control 3 Name
+  ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint,   !- Thermal Comfort Control 4 Object Type
+  Dual Comfort Setpoint;     !- Thermal Comfort Control 4 Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-024}
+
+Three outputs are available from the ZoneControl:Thermostat:ThermalComfort object. Two output variables used primarily for the ZoneControl:Thermost object are also described here to explain their meaning when using thermal comfort control.
+
+\textbf{ZoneControl:ThermalComfort}
+
+\begin{itemize}
+\item
+  Zone,Average,Zone Thermal Comfort Control Type {[]}
+\item
+  Zone,Average,Zone Thermal Comfort Control Fanger Low Setpoint PMV {[]}
+\item
+  Zone,Average,Zone Thermal Comfort Control Fanger High Setpoint PMV {[]}
+\end{itemize}
+
+\textbf{ZoneControl:Thermostat}
+
+\begin{itemize}
+\item
+  Zone,Average,Zone Thermostat Heating Setpoint Temperature {[}C{]}
+\item
+  Zone,Average,Zone Thermostat Cooling Setpoint Temperature {[}C{]}
+\end{itemize}
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort Control Type {[]}}{Zone Thermal Comfort Control Type }}\label{zone-thermal-comfort-control-type}
+
+This is the current zone thermal comfort control type (0 through 4). This value is set at each system timestep and averaged over the reporting interval. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort Control Fanger Low Setpoint PMV {[]}}{Zone Thermal Comfort Control Fanger Low Setpoint PMV }}\label{zone-thermal-comfort-control-fanger-low-setpoint-pmv}
+
+This is the current zone thermal comfort low Predicted Mean Vote value. Values range between -3 and +3. If there is no heating thermal comfort active, then the value reported will be -999. This value is set at each system timestep and averaged over the reporting interval. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
+
+\paragraph{\texorpdfstring{Zone Thermal Comfort Control Fanger High Setpoint PMV {[]}}{Zone Thermal Comfort Control Fanger High Setpoint PMV }}\label{zone-thermal-comfort-control-fanger-high-setpoint-pmv}
+
+This is the current zone thermal comfort high Predicted Mean Vote value. Values range between -3 and +3. If there is no cooling thermal comfort active, then the value reported will be 999. This value is set at each system timestep and averaged over the reporting interval. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
+
+\paragraph{Zone Thermostat Heating Setpoint Temperature {[}C{]}}\label{zone-thermostat-heating-setpoint-temperature-c-1}
+
+The Zone Control:Thermal Comfort object shares the same output variable and overwrites the thermal setpoints defined in object Zone Control:Thermostatic when both objects of Zone Control:Thermostatic and Zone Control:Thermal Comfort co-exist. It outputs the current zone thermal comfort heating setpoint in degrees C when thermal comfort control is active, otherwise this output variable will report the thermostat heating setpoint (Ref. Zone Control:Thermostatic Outputs). If there is no heating thermal comfort active and no thermostat heating setpoint is defined for this zone, this value will be 0. This value is set at each system timestep and averaged over the reporting interval. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
+
+\paragraph{Zone Thermostat Cooling Setpoint Temperature {[}C{]}}\label{zone-thermostat-cooling-setpoint-temperature-c-1}
+
+This output variable defined in object Zone Control:Thermostatic. The Thermal Comfort object shares the same output variable and overwrites the thermal setpoints defined in object Zone Control:Thermostatic when both objects of Zone Control:Thermostatic and Zone Control:Thermal Comfort co-exist. It outputs the current zone thermal comfort cooling setpoint in degrees C when thermal comfort control is active, otherwise this output variable will report the thermostat cooling setpoint (Ref. Zone Control:Thermostatic Outputs). If there is no cooling thermal comfort active and no thermostat cooling setpoint is defined for this zone, this value will be 0. This value is set at each system timestep and averaged over the reporting interval. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
+
+\subsection{Thermal Comfort Setpoints}\label{thermal-comfort-setpoints}
+
+The syntax for the current set (4) of zone thermal comfort control types is given below. In each case, the keyword is accompanied by an identifying name and either one or two schedule names (depending on whether the control type is a single or dual setpoint control). The schedule defines a Predicted Mean Vote (PMV) setpoint for the control type. The schedule would be defined through the standard schedule syntax described earlier in this document. For an uncontrolled thermal comfort zone, no Fanger thermal comfort object is specified or necessary. However, the \lstinline!Fanger thermal comfort output variables, Zone Thermal Comfort Fanger Model PMV and Zone Thermal Comfort Fanger Model PPD, are reported for thermal comfort uncontrolled conditions as well (e.i., free floating thermal comfort condition) just like a free floating temperature and humidity ratio.   These are indicative of the actual thermal comfort level in uncontrolled thermal comfort zone, and are outputs variables under!People objects\lstinline!.!
+
+\subsection{ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating}\label{thermostatsetpointthermalcomfortfangersingleheating}
+
+This would be used for heating only thermal comfort control. The PMV setpoint can be scheduled and varied throughout the simulation but only heating is allowed with this control type.
+
+\subsubsection{Inputs}\label{inputs-10-023}
+
+\paragraph{Field: Name}\label{field-name-8-024}
+
+Unique name for this control type.
+
+\paragraph{Field: Fanger Thermal Comfort Schedule Name}\label{field-fanger-thermal-comfort-schedule-name}
+
+The name of the associated schedule containing \lstinline!Zone Thermal Comfort Fanger Model PMV! values.
+
+\subsection{ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling}\label{thermostatsetpointthermalcomfortfangersinglecooling}
+
+This would be used for cooling only thermal comfort control. The PMV setpoint can be scheduled and varied throughout the simulation but only cooling is allowed with this control type.
+
+\subsubsection{Inputs}\label{inputs-11-022}
+
+\paragraph{Field: Name}\label{field-name-9-021}
+
+Unique name for this control type.
+
+\paragraph{Field: Fanger Thermal Comfort Schedule Name}\label{field-fanger-thermal-comfort-schedule-name-1}
+
+The name of the associated schedule, containing \lstinline!Zone Thermal Comfort Fanger Model PMV! values.
+
+\subsection{ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling}\label{thermostatsetpointthermalcomfortfangersingleheatingorcooling}
+
+This would be used for heating and cooling thermal comfort control but only heating or cooling can be scheduled at any given time period. The PMV setpoint can be scheduled and varied throughout the simulation for both heating and cooling.
+
+\subsubsection{Inputs}\label{inputs-12-020}
+
+\paragraph{Field: Name}\label{field-name-10-019}
+
+Unique name for this control type.
+
+\paragraph{Field: Fanger Thermal Comfort Schedule Name}\label{field-fanger-thermal-comfort-schedule-name-2}
+
+The name of the associated schedule containing \lstinline!Zone Thermal Comfort Fanger Model PMV! values.
+
+\subsection{ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint}\label{thermostatsetpointthermalcomfortfangerdualsetpoint}
+
+This would be used for heating and cooling thermal comfort control where both a heating and cooling PMV setpoint can be scheduled for any given time period. The PMV setpoint can be scheduled and varied throughout the simulation for both heating and cooling.
+
+\subsubsection{Inputs}\label{inputs-13-017}
+
+\paragraph{Field: Name}\label{field-name-11-016}
+
+Unique name for this control type.
+
+\paragraph{Field: Fanger Thermal Comfort Heating Schedule Name}\label{field-fanger-thermal-comfort-heating-schedule-name}
+
+The name of the associated schedule containing heating setpoint \lstinline!Zone Thermal Comfort Fanger Model PMV! values.
+
+\paragraph{Field: Fanger Thermal Comfort Cooling Schedule Name}\label{field-fanger-thermal-comfort-cooling-schedule-name}
+
+The name of the associated schedule containing cooling setpoint \lstinline!Zone Thermal Comfort Fanger Model PMV! values.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating,
+  Heating Comfort Setpoint,!- Name
+  Heating PMV Setpoints;     !- Setpoint Temperature SCHEDULE Name
+
+
+  ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling,
+  Cooling Comfort Setpoint,!- Name
+  Cooling PMV Setpoints;     !- Setpoint Temperature SCHEDULE Name
+
+
+  ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling,
+  Heating Cooling Comfort Setpoint,!- Name
+  Heating Cooling PMV Setpoints;     !- Setpoint Temperature SCHEDULE Name
+
+
+  ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint,
+  Dual Comfort Setpoint,     !- Name
+  Heating PMV Setpoints,     !- Fanger Thermal Comfort Heating Setpoint PMV SCHEDULE Name
+  Cooling PMV Setpoints;     !- Fanger Thermal Comfort Cooling Setpoint PMV SCHEDULE Name
+\end{lstlisting}
+
+\subsection{ZoneControl:ContaminantController}\label{zonecontrolcontaminantcontroller}
+
+The ZoneControl:ContaminantController object is used for any of the following two purposes based on the system outdoor air method specified in the Controller:MechanicalVentilation.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  To control a zone to a specified indoor level of contaminants. When this zone is served by an AirLoopHVAC, the other zones served by the same AirLoopHVAC will have the same specified indoor level, if no objects in the other zones served by the same AirLoop are specified. Currently, the available contaminant controls are carbon dioxide and generic contaminant controls. The specified carbon dioxide setpoint is used to calculate the required outdoor airflow rate through the HVAC system to reach the setpoint. The AirLoopHVAC system outdoor flow rate is realized by the Controller:MechanicalVentilation object with System Outdoor Air Method = IndoorAirQualityProcedure.The specified generic contaminant setpoint is used to calculate the required outdoor airflow rate through the HVAC system to reach the setpoint. The AirLoopHVAC system outdoor flow rate is realized by the Controller:MechanicalVentilation object with System Outdoor Air Method = IndoorAirQualityProcedure-GenericContaminant.
+\item
+  To specify minimum CO2 concentration schedule name for a zone. The AirLoopHVAC system outdoor flow rate is realized by the Controller:MechanicalVentilation object with System Outdoor Air Method = ProportionalControlBasedonOccupancySchedule or ProportionalControlBasedOnDesignOccupancy. Carbon Dioxide Control Availability Schedule Name determines the availability of ProportionalControl .
+\end{enumerate}
+
+For the first purpose above, when multiple zones are served by an AirLoop, those zones that do not have a contaminant controller object specified in the input data file are automatically assigned a carbon dioxide setpoint. Zone objects entered in the input data file are internally assigned an index number from 1 to n (first defined Zone object = 1, next Zone object defined in the input file = 2, etc.). For zones served by an AirLoop that do not have a contaminant controller specified, the zone s carbon dioxide setpoint will be the same as the zone with the next highest zone index number that has a contaminant controller specified. If a zone with a higher index number and contaminant controller specified does not exist, then the zone with the next lowest zone index number that has a contaminant controller specified will be used. For example, assume an AirLoop serves zones 1 through 5, but one ZoneControl:ContaminantController object is specified for zone 2, a second ZoneControl:ContaminantController object is specified for zone 4, and no ZoneControl:ContaminantController objects are specified for zones 1, 3 and 5. In this case, zone 1 will be assigned the carbon dioxide setpoint schedule that was specified for zone 2, and zones 3 and 5 will be assigned the carbon dioxide setpoint schedule that was specified for zone 4.
+
+\subsubsection{Inputs}\label{inputs-14-017}
+
+\paragraph{Field: Name}\label{field-name-12-013}
+
+Unique identifying name for the ZoneControl:ContaminantController.
+
+\paragraph{Field: Controlled Zone Name}\label{field-controlled-zone-name-000}
+
+Name of the zone that is being controlled.
+
+\paragraph{Field:Carbon Dioxide Control Availability Schedule Name}\label{fieldcarbon-dioxide-control-availability-schedule-name}
+
+This field contains the name of a schedule that determines whether or not the ZoneControl:ContaminantController is available. When the schedule value is zero, the ZoneControl:ContaminantController is bypassed (not available to operate). When the schedule value is greater than zero, the ZoneControl:ContaminantController is available and will be used to calculate the required outdoor airflow rate to reach the carbon dioxide setpoint. If this field is left blank, the schedule has a value of 1 for all time periods. Schedule values must be between 0 and 1.
+
+\paragraph{Field:Carbon Dioxide Setpoint Schedule Name}\label{fieldcarbon-dioxide-setpoint-schedule-name}
+
+This field contains the name of a schedule that contains the zone carbon dioxide concentration setpoint as a function of time. The units for carbon dioxide setpoint are ppm. The setpoint values in the schedule must be between 0 and 2000 ppm. . This field is used when the field System Outdoor Air Method = IndoorAirQualityProcedure in the Controller:MechanicalVentilation object.
+
+\paragraph{Field:Minimum Carbon Dioxide Concentration Schedule Name}\label{fieldminimum-carbon-dioxide-concentration-schedule-name}
+
+This field contains the name of a schedule that contains the minimum zone carbon dioxide concentration setpoint as a function of time. The units for carbon dioxide setpoint are ppm. This field is used when the field System Outdoor Air Method = ProportionalControlBasedonOccupancySchedule or ProportionalControlBasedOnDesignOccupancy in the Controller:MechanicalVentilation object.
+
+\paragraph{Field: Generic Contaminant Control Availability Schedule Name}\label{field-generic-contaminant-control-availability-schedule-name}
+
+This field contains the name of a schedule that determines whether or not the ZoneControl:ContaminantController is available. When the schedule value is zero, the generic contaminant control will not be performed. When the schedule value is greater than zero, the ZoneControl:ContaminantController is available and will be used to calculate the required outdoor airflow rate to reach the generic contaminant setpoint. If this field is left blank, the schedule has a value of 1 for all time periods. Schedule values must be between 0 and 1.
+
+\paragraph{Field: Generic Contaminant Setpoint Schedule Name}\label{field-generic-contaminant-setpoint-schedule-name}
+
+This field contains the name of a schedule that contains the zone generic contaminant concentration setpoint as a function of time. The units for generic contaminant setpoint are ppm. The setpoint values in the schedule must be\textgreater{} = 0.
+
+An IDF example is provided below:
+
+\begin{lstlisting}
+
+ZoneControl:ContaminantController,
+  CO2 Controller1,                 !- Name
+  EAST ZONE,                             !- Controlled Zone Name
+  CO2AvailSchedule,               !- Carbon Dioxide Control Availability Schedule Name
+  CO2SetpointSchedule,         !- Carbon Dioxide Setpoint Schedule Name
+  ,                                               !- Minimum Carbon Dioxide Concentration Schedule Name
+  GCAvailSchedule,                 !- Generic Contaminant Control Availability Schedule Name
+  GCSetpointSchedule;           !- Generic Contaminant Setpoint Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-020}
+
+The following output variables are available when the ZoneControl:ContaminantController object is specified.
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Air CO2 Predicted Load to Setpoint Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Air CO2 Setpoint Concentration {[}ppm{]}
+\item
+  HVAC,Average,Zone Generic Air Contaminant Predicted Load to Setpoint Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Generic Air Contaminant Setpoint Concentration {[}ppm{]}
+\end{itemize}
+
+\paragraph{Zone Air CO2 Predicted Load to Setpoint Mass Flow Rate {[}kg/s{]}}\label{zone-air-co2-predicted-load-to-setpoint-mass-flow-rate-kgs}
+
+This output is the average predicted outdoor airflow rate in kg/s required to meet the current zone carbon dioxide setpoint for the time step being reported. This value is calculated and reported from the Predict step in the Zone Contaminant Predictor-Corrector module. The calculated outdoor airflow rate will be specified in the Controller:MechanicalVentilation object with System Outdoor Air Method = IndoorAirQualityProcedureto provide enough outdoor ventilation air to keep the zone air carbon dioxide concentration level at or below the setpoint.
+
+\paragraph{Zone Air CO2 Setpoint Concentration {[}ppm{]}}\label{zone-air-co2-setpoint-concentration-ppm}
+
+This output variable is the average carbon dioxide setpoint value, in parts per million, for the time step being reported.
+
+\paragraph{Zone Generic Air Contaminant Predicted Load to Setpoint Mass Flow Rate {[}kg/s{]}}\label{zone-generic-air-contaminant-predicted-load-to-setpoint-mass-flow-rate-kgs}
+
+This output is the average predicted outdoor airflow rate in kg/s required to meet the current zone generic contaminant setpoint for the time step being reported. This value is calculated and reported from the Predict step in the Zone Contaminant Predictor-Corrector module. The calculated outdoor airflow rate will be specified in the Controller:MechanicalVentilation object with System Outdoor Air Method = IndoorAirQualityProcedure-GenericContaminant****to provide enough outdoor ventilation air to keep the zone air generic contaminant concentration level at or below the setpoint.
+
+\paragraph{Zone Generic Air Contaminant Setpoint Concentration {[}ppm{]}}\label{zone-generic-air-contaminant-setpoint-concentration-ppm}
+
+This output variable is the averagegeneric contaminant setpoint value, in parts per million, for the time step being reported.
diff --git a/doc/input-output-reference/src/overview/group-zone-equipment.tex b/doc/input-output-reference/src/overview/group-zone-equipment.tex
new file mode 100644
index 00000000000..cdfc44ad0a0
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-zone-equipment.tex
@@ -0,0 +1,287 @@
+\section{Group - Zone Equipment}\label{group---zone-equipment}
+
+There are five main zone equipment statements that must be used to describe a block of zone equipment as shown in the below figure ``Zone Equipment Input Syntax Map''.
+
+Types of Zone equipment are listed below and shown below in figure ``Zone Equipment''.
+
+% table 26
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Available Zone Equipment Types \label{table:available-zone-equipment-types}} \tabularnewline
+\toprule 
+Air Distribution Equipment & AirTerminal:SingleDuct:Uncontrolled    AirTerminal:SingleDuct:ConstantVolume:Reheat    AirTerminal:SingleDuct:VAV:Reheat    AirTerminal:SingleDuct:VAV:NoReheat    AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan    AirTerminal:DualDuct:ConstantVolume    AirTerminal:DualDuct:VAV    Powered Induction Units (Series and Parallel) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Available Zone Equipment Types} \tabularnewline
+\toprule 
+Air Distribution Equipment & AirTerminal:SingleDuct:Uncontrolled    AirTerminal:SingleDuct:ConstantVolume:Reheat    AirTerminal:SingleDuct:VAV:Reheat    AirTerminal:SingleDuct:VAV:NoReheat    AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan    AirTerminal:DualDuct:ConstantVolume    AirTerminal:DualDuct:VAV    Powered Induction Units (Series and Parallel) \tabularnewline
+\midrule
+\endhead
+
+Zone Forced Air Units ~ & ZoneHVAC:IdealLoadsAirSystem    ZoneHVAC:FourPipeFanCoil    ZoneHVAC:WindowAirConditioner    ZoneHVAC:RefrigerationChillerSet    Unit Ventilator/Heater    Air-to-Air Heat Pumps    Unitary Systems (heat only and heat/cool)    Furnaces (heat only and heat/cool)    Energy Recovery Ventilator:Stand Alone    CoilSystem:Cooling:DX \tabularnewline
+Radiative/Convective Units & Baseboard Heaters    Low Temp Radiant Systems    High Temp Radiant System \tabularnewline
+\bottomrule
+\end{longtable}
+
+!{[}ZoneEquipmentSyntax (media/image261.png)
+
+Figure 99. Zone Equipment Input Syntax Map
+
+\begin{figure}[hbtp] % fig 100
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image262.png}
+\caption{Representative Zone Equipment \protect \label{fig:representative-zone-equipment}}
+\end{figure}
+
+The following figure (Air Loop/Zone Equipment Node Diagram) illustrates the connection between the zone equipment and the air loop systems.
+
+\begin{figure}[hbtp] % fig 101
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image263.png}
+\caption{Air Loop/Zone Equipment Node Diagram \protect \label{fig:air-loopzone-equipment-node-diagram}}
+\end{figure}
+
+Each zone served by an HVAC system must have three additional statements to complete the zone equipment specification. An ZoneHVAC:AirDistributionUnit allows equipment typically found within the zone inlet ductwork (such as dampers, reheat coils, etc.) to be attached to the supply air stream for a particular zone. A ZoneControl statement will allow the conditions in the zone to be managed. Finally, a ZoneHVAC:EquipmentConnections statement describes all of the pertinent information about the zone from an HVAC perspective. Each of these statements is described in more detail below.
+
+\subsection{ZoneHVAC:AirDistributionUnit}\label{zonehvacairdistributionunit}
+
+The ZoneHVAC:AirDistributionUnit object gives further information on what air loop equipment (air terminal units) will be serving a particular zone. The ZoneHVAC:AirDistributionUnit is the part of the system that is supplied from a common main air handler simulated in the Air Loop Simulation and includes the equipment that controls or tempers the air going to each individual zone according to the desired thermostatic control. The current options for ZoneHVAC:AirDistributionUnit terminal unit types are:
+
+\begin{itemize}
+\item
+  AirTerminal:DualDuct:ConstantVolume
+\item
+  AirTerminal:DualDuct:VAV
+\item
+  AirTerminal:DualDuct:VAV:OutdoorAir
+\item
+  AirTerminal:SingleDuct:ConstantVolume:Reheat
+\item
+  AirTerminal:SingleDuct:VAV:Reheat
+\item
+  AirTerminal:SingleDuct:VAV:NoReheat
+\item
+  AirTerminal:SingleDuct:SeriesPIU:Reheat
+\item
+  AirTerminal:SingleDuct:ParallelPIU:Reheat
+\item
+  AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction
+\item
+  AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan
+\item
+  AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat
+\item
+  AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat
+\end{itemize}
+
+Connections between the air distribution unit, the supply air duct, and the zone are specified in the input syntax for the air distribution unit and the AirLoopHVAC:ZoneSplitter. The input syntax also explicitly defines an outlet identifier. This implies a connection to a zone through a NodeList for zone inlets (see the ZoneHVAC:EquipmentConnections statement). The air distribution unit is limited to one combined component-controller unit; because controls are normally based on the zone thermostat and can work in parallel or series in complex fashion. Since the control and the flow resolution can be complex, each air distribution unit is unique in addressing these combinations and therefore only one is allowed per zone.
+
+The Air Distribution unit also allows the user to specify leaks in the supply air duct system. These inputs are used in the EnergyPlus Simplified Duct Leakage Model (SDLM). This model simulates a specific configuration: supply leaks to a return plenum in a commercial VAV or CV system. The system must have a constant static pressure setpoint. Within these limitations SDLM allows the user to easily evaluate the energy penalty due to duct leakage.
+
+\subsubsection{Inputs}\label{inputs-055}
+
+\paragraph{Field: Name}\label{field-name-053}
+
+Unique identifying name of the air distribution unit.
+
+\paragraph{Field: Air Distribution Unit Outlet Node Name}\label{field-air-distribution-unit-outlet-node-name}
+
+Outlet node name for the air distribution unit to the attached zone.
+
+\paragraph{Field: Air Terminal Object Type}\label{field-air-terminal-object-type}
+
+Single combined component/controller unit for that attached zone. Selection of components as listed above.
+
+\paragraph{Field: Air Terminal Name}\label{field-air-terminal-name}
+
+The unique identifying component name.
+
+\paragraph{Field: Nominal Upstream Leakage Fraction}\label{field-nominal-upstream-leakage-fraction}
+
+This is the leakage upstream of the terminal unit as a fraction of the design flow rate through the unit. It is the leakage fraction at the design flow rate. It is used to calculate a leakage flow rate which is then held constant while the system air flow varies. This input is optional; the default is zero.
+
+\paragraph{Field: Constant Downstream Leakage Fraction}\label{field-constant-downstream-leakage-fraction}
+
+This is the leakage downstream of the terminal unit as a fraction of the current flow rate through the terminal unit. This fraction is held constant, so the leakage flow rate will vary proportinally with the supply air flow rate. This input is optional; the default is zero.
+
+Two example IDF excerpts (one with duct leakage, one without):
+
+\begin{lstlisting}
+
+ZoneHVAC:AirDistributionUnit,
+      SPACE1-1 ATU,            !- Air Distribution Unit Name
+      SPACE1-1 In Node,        !- Air Dist Unit Outlet Node Name
+      AIRTERMINAL:SINGLEDUCT:VAV:REHEAT,  !- KEY--System Component Type 1
+      SPACE1-1 VAV Reheat;     !- Component Name 1
+
+  ZoneHVAC:AirDistributionUnit,
+      SPACE4-1 ATU,            !- Air Distribution Unit Name
+      SPACE4-1 In Node,        !- Air Dist Unit Outlet Node Name
+      AIRTERMINAL:SINGLEDUCT:VAV:REHEAT,  !- KEY--System Component Type 1
+      SPACE4-1 VAV Reheat,     !- Component Name 1
+      0.05,                    !- upstream nominal leakage fraction
+      0.07;                    !- downstream constant leakage fraction
+\end{lstlisting}
+
+\subsection{ZoneHVAC:EquipmentConnections}\label{zonehvacequipmentconnections}
+
+Finally, the ZoneHVAC:EquipmentConnections statement defines the remaining details about each thermal zone from an HVAC perspective (besides the controls which were defined above). As with other statements, the first two items in this object are the keyword and an identifying name which links the zone back to its geometrical input, internal gains, etc. and other statements in the HVAC section of the input. The next three items are names of lists (equipment, air inlet nodes, and air exhaust nodes) that are described in more detail below. Note that if there are no air exhaust nodes from the zone that field is left blank. And if there are no air inlet nodes, that field is left blank. Finally, two node names are necessary to complete the zone-HVAC description. The first node is the main air node for the zone upon which the air heat balance is performed. The other node begins the return air path from the zone.
+
+Note that all nodes mentioned in the ZoneHVAC:EquipmentConnections input must be unique.~ That is, all nodes in all the ZoneHVAC:EquipmentConnections statements referenced by the ``Zone Air Inlet Nodes'', ``Zone Air Exhaust Nodes'', ``Zone Air Node Name'' and ``Zone Return Air Node Name'' cannot have any node name appearing more than once.
+
+\subsubsection{Inputs}\label{inputs-1-052}
+
+\paragraph{Field: Zone Name}\label{field-zone-name-015}
+
+Name links this equipment list back to the heat balance for the zone.
+
+\paragraph{Field: Zone Conditioning Equipment List Name}\label{field-zone-conditioning-equipment-list-name}
+
+List of zone equipment for this zone in a ZoneHVAC:EquipmentList object. This list will consist of air distribution units or other direct convection or radiant equipment, i.e.~window air conditioner, baseboard, fan coils, etc.
+
+\paragraph{Field: Zone Air Inlet Node or NodeList Name}\label{field-zone-air-inlet-node-or-nodelist-name}
+
+There can be more than one air inlet node depending on how many pieces of equipment are in the ZoneHVAC:EquipmentList. Generally there will be one air inlet node for each piece of zone equipment that delivers conditioned air to the zone. Components such as electric or hot water baseboards and radiant systems do not require zone air inlet nodes. If there is only one node -- its name can be put in this field. If there is more than one node, this must be the name of a node list object (a node list object can also contain only one node name). If this field is not required (as in the baseboard system), it should be blank.
+
+\paragraph{Field: Zone Air Exhaust Node or NodeList Name}\label{field-zone-air-exhaust-node-or-nodelist-name}
+
+List of exhaust nodes leaving the zone for exhaust fans, zone energy recovery, etc. However these nodes are also used as sources of zone air for zone components such as fan coil units, unit heaters and ventilators, and window air conditioners. For each such component attached to a zone there should be a unique zone exhaust node acting as the inlet node to the component. If there is only one node -- its name can be put in this field. If there is more than one node, this must be the name of a node list object (a node list object can also contain only one node name). If there are no air exhaust nodes, this field should be blank.
+
+\paragraph{Field: Zone Air Node Name}\label{field-zone-air-node-name}
+
+The conditions at this node represent the average state of the air in the zone. For zones modeled as fully mixed the conditions at this node are assumed to represent the air in the entire zone. This field is required for all ZoneHVAC:EquipmentConnections statements.
+
+\paragraph{Field: Zone Return Air Node Name}\label{field-zone-return-air-node-name}
+
+The name of the return air node which attaches the zone to the return air path described above. Even if there is no return air or no return air path a unique name must be entered in this field. The conditions at this node represent the state of the air leaving the zone including any heat gain from light-heat-to-return.
+
+\paragraph{Field: Zone Return Air Flow Rate Fraction Schedule Name}\label{field-zone-return-air-flow-rate-fraction-schedule-name}
+
+The name of a schedule to specify the return air flow rate as a fraction of the base return air. If the next field is blank, then the return air flow rate is the total supply inlet flow rate to the zone less the total exhaust node flow rate from the zone multiplied by this schedule name. If this field is left blank, the schedule defaults to 1.0 at all times.
+
+\paragraph{Field: Zone Return Air Flow Rate Basis Node or NodeList Name}\label{field-zone-return-air-flow-rate-basis-node-or-nodelist-name}
+
+The name of a node or list of nodes (NodeList) that is used to calculate the return air flow rate for this zone. The sum of the current flow rates for this node(s) multiplied by the Zone Return Air Flow Rate Fraction Schedule determines the return air flow rate. If this field is blank, then the base return air flow rate is the total supply inlet flow rate to the zone less the total exhaust node flow rate from the zone.
+
+An example of this statement in an IDF is:
+
+\begin{lstlisting}
+
+ZoneHVAC:EquipmentConnections,
+      SPACE3-1,              !- Zone Name
+      SPACE3-1 Eq,           !- List Name: Zone Equipment
+      SPACE3-1 In Nodes,     !- List Name: Zone Air Inlet Nodes
+      ,                      !- List Name: Zone Air Exhaust Nodes
+      SPACE3-1 Node,         !- Zone Air Node Name
+      SPACE3-1 Out Node;     !- Zone Return Air Node Name
+\end{lstlisting}
+
+The following HVAC equipment types are allowed as zone equipment. The component matrix shows which coils and fans are allowed with which equipment models.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/ZoneComponentMatrix.png}
+\caption{}
+\end{figure}
+
+\subsection{ZoneHVAC:EquipmentList}\label{zonehvacequipmentlist}
+
+The first list encountered in the ZoneHVAC:EquipmentConnections statement is the ZoneHVAC:EquipmentList. This object lists all HVAC equipment serving the zone. Each item in the list has four fields associated with it: Object Type, Name, Cooling Sequence and Heating or No-Load Sequence The Object Type and Name identify the specific equipment object. Cooling Sequence and Heating or No-Load Sequence specify the order of simulation for zones with more than one type of HVAC equipment.
+
+Note that a ZoneHVAC:AirDistributionUnit or AirTerminal:SingleDuct:Uncontrolled must be listed in this statement if there is a forced air system serving the zone from an air loop.
+
+\subsubsection{Inputs}\label{inputs-2-048}
+
+\paragraph{Field: Name}\label{field-name-1-050}
+
+Unique identifying name.
+
+\paragraph{Field Set (Zone Equipment: Object Type, Name, Cooling Sequence, Heating or No-Load Sequence)}\label{field-set-zone-equipment-object-type-name-cooling-sequence-heating-or-no-load-sequence}
+
+This set is used together in order to sequence the equipment for heating and cooling. The \#1 sequence equipment will try to meet the entire demand with its capacity and then pass the results on to the \#2 and so on for both heating and cooling. This field set is extensible by duplicating the last four fields.
+
+Equipment is simulated in the order specified by Zone Equipment Cooling Sequence and Zone Equipment Heating or No-Load Sequence, depending on the current thermostat request. For equipment of similar type, assign sequence 1 to the first system intended to serve that type of load, assign sequence 2 to the next system, and so on. For situations where one or more equipment types has limited capacity or limited control capability, order the sequence so that the most controllable piece of equipment runs last. For example, with a dedicated outdoor air system (DOAS), the air terminal for the DOAS should be assigned Heating Sequence = 1 and Cooling Sequence = 1. Any other equipment should be assigned sequence 2 or higher so that it will see the net load after the DOAS air is added to the zone.
+
+\paragraph{Field: Zone Equipment \textless{}x\textgreater{} Object Type}\label{field-zone-equipment-x-object-type}
+
+Type of zone equipment such as air distribution unit, baseboard, window air conditioner, etc. The current legal types are listed in the following table:
+
+% table 27
+\begin{longtable}[c]{@{}l@{}}
+\caption{Legal Zone Equipment Types (ZoneHVAC:EquipmentList) \label{table:legal-zone-equipment-types-zonehvac}} \tabularnewline
+\toprule 
+Legal Zone Equipment Types \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Legal Zone Equipment Types (ZoneHVAC:EquipmentList)} \tabularnewline
+\toprule 
+Legal Zone Equipment Types \tabularnewline
+\midrule
+\endhead
+
+AirTerminal:SingleDuct:Uncontrolled \tabularnewline
+Fan:ZoneExhaust \tabularnewline
+WaterHeater:HeatPump:PumpedCondenser \tabularnewline
+WaterHeater:HeatPump:WrappedCondenser \tabularnewline
+ZoneHVAC:AirDistributionUnit \tabularnewline
+ZoneHVAC:Baseboard:Convective:Electric \tabularnewline
+ZoneHVAC:Baseboard:Convective:Water \tabularnewline
+ZoneHVAC:Baseboard:RadiantConvective:Electric \tabularnewline
+ZoneHVAC:Baseboard:RadiantConvective:Water \tabularnewline
+ZoneHVAC:Baseboard:RadiantConvective:Steam \tabularnewline
+ZoneHVAC:Dehumidifier:DX \tabularnewline
+ZoneHVAC:EnergyRecoveryVentilator \tabularnewline
+ZoneHVAC:FourPipeFanCoil \tabularnewline
+ZoneHVAC:HighTemperatureRadiant \tabularnewline
+ZoneHVAC:IdealLoadsAirSystem \tabularnewline
+ZoneHVAC:LowTemperatureRadiant:ConstantFlow \tabularnewline
+ZoneHVAC:LowTemperatureRadiant:Electric \tabularnewline
+ZoneHVAC:LowTemperatureRadiant:VariableFlow \tabularnewline
+ZoneHVAC:OutdoorAirUnit \tabularnewline
+ZoneHVAC:PackagedTerminalAirConditioner \tabularnewline
+ZoneHVAC:PackagedTerminalHeatPump \tabularnewline
+ZoneHVAC:RefrigerationChillerSet \tabularnewline
+ZoneHVAC:UnitHeater \tabularnewline
+ZoneHVAC:UnitVentilator \tabularnewline
+ZoneHVAC:WindowAirConditioner \tabularnewline
+ZoneHVAC:WaterToAirHeatPump \tabularnewline
+ZoneHVAC:VentilatedSlab \tabularnewline
+\bottomrule
+\end{longtable}
+
+\paragraph{Field: Zone Equipment \textless{}x\textgreater{} Name}\label{field-zone-equipment-x-name}
+
+Name of the zone equipment used in the object definition of its type.
+
+\paragraph{Field: Zone Equipment \textless{}x\textgreater{} Cooling Sequence}\label{field-zone-equipment-x-cooling-sequence}
+
+Specifies the zone equipment simulation order when the zone thermostat requests cooling.
+
+\paragraph{Field: Zone Equipment \textless{}x\textgreater{} Heating or No-Load Sequence}\label{field-zone-equipment-x-heating-or-no-load-sequence}
+
+Specifies the zone equipment simulation order when the zone thermostat requests heating or no load.
+
+Examples of this statement in an IDF are:
+
+\begin{lstlisting}
+
+  ZoneHVAC:EquipmentList,
+      Zone1Equipment,          !- Name
+      ZoneHVAC:AirDistributionUnit,  !- Zone Equipment 1 Object Type
+      Zone1TermReheat,         !- Zone Equipment 1 Name
+      1,                       !- Zone Equipment 1 Cooling Sequence
+      1;                       !- Zone Equipment 1 Heating or No-Load Sequence
+
+
+    ZoneHVAC:EquipmentList,
+      Zone1Equipment,          !- Name
+      AirTerminal:SingleDuct:Uncontrolled,  !- Zone Equipment 1 Object Type
+      Zone1DirectAir,          !- Zone Equipment 1 Name
+      1,                       !- Zone Equipment 1 Cooling Sequence
+      1,                       !- Zone Equipment 1 Heating or No-Load Sequence
+      ZoneHVAC:WaterToAirHeatPump,  !- Zone Equipment 2 Object Type
+      Zone1WTAHP,              !- Zone Equipment 2 Name
+      2,                       !- Zone Equipment 2 Cooling Sequence
+      2;                       !- Zone Equipment 2 Heating or No-Load Sequence
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/group-zone-forced-air-units.tex b/doc/input-output-reference/src/overview/group-zone-forced-air-units.tex
new file mode 100644
index 00000000000..47c2bf732bc
--- /dev/null
+++ b/doc/input-output-reference/src/overview/group-zone-forced-air-units.tex
@@ -0,0 +1,4083 @@
+\section{Group -- Zone Forced Air Units}\label{group-zone-forced-air-units}
+
+\subsection{ZoneHVAC:IdealLoadsAirSystem}\label{zonehvacidealloadsairsystem}
+
+The simplest piece of zone equipment is the ZoneHVAC:IdealLoadsAirSystem component. ZoneHVAC:IdealLoadsAirSystem is used in situations where the user wishes to study the performance of a building without modeling a full HVAC system. In such a case, the Ideal Loads Air System is usually the sole conditioning component: the user does not need to specify air loops, water loops, etc. All that is needed for the ideal system are zone controls, zone equipment configurations, and the ideal loads system component.
+
+This component can be operated with infinite or finite heating and cooling capacity. For either mode -- infinite or limited capacity -- the user can also specify on/off schedules for heating and cooling and outdoor air controls. There are also optional controls for dehumidification, humidification, economizer, and heat recovery. This component may be used in combination with other HVAC equipment serving the same zone.
+
+This component can be thought of as an ideal unit that mixes air at the zone exhaust condition with the specified amount of outdoor air and then adds or removes heat and moisture at 100\% efficiency in order to produce a supply air stream at the specified conditions. The energy required to condition the supply air is metered and reported as DistrictHeating and DistrictCooling.
+
+\textbf{Notes:} The ideal loads system uses the zone return node or an optional zone exhaust node to extract air from the zone. Every zone served by an HVAC component must have a return air node, even though this node may not be connected to anything.
+
+The ideal loads system was significantly expanded in version 7.0 (October 2011). As part of this upgrade, any change in the moisture content of the supply air stream results in a latent cooling (dehumidification) or latent heating (humidification) load which is metered as DistrictCooling and DistrictHeating energy consumption. Prior to version 7.0, when the ideal loads system was in heating mode, only the energy for sensible heating was metered. This results in significant changes in reported energy use compared to earlier versions, especially when using the \textbf{\emph{ConstantSupplyHumidityRatio}} option for Humidification Control Type.
+
+Older idf files which are transitioned to version 7.0 will automatically be set to use the \textbf{\emph{ConstantSupplyHumidityRatio}} option for both dehumidification and humidification controls, because this is equivalent to the controls used in the older version of this system. However, the user should review all of the humidity control options and select the one which best reflects the goal of the simulation.
+
+\subsubsection{Inputs}\label{inputs-056}
+
+\paragraph{Field: Name}\label{field-name-054}
+
+A unique user assigned name for each ideal loads air system component.~ This name is referenced in a ZoneHVAC:EquipmentList object.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-020}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether or not this component is available to operate during a given time period. If the schedule value is greater than zero then the system is available to operate; otherwise, the system is unavailable for that time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Zone Supply Air Node Name}\label{field-zone-supply-air-node-name-001}
+
+The name of the outlet air node of the ideal loads object. This should be the same as one of the zone air inlet nodes for the zone the ideal loads component is serving.
+
+\paragraph{Field: Zone Exhaust Air Node Name}\label{field-zone-exhaust-air-node-name}
+
+The name of the zone exhaust air node of the ideal loads object. This should be the same as one of the zone air exhaust nodes for the zone this component is serving. This node name is required if ZoneHVAC:IdealLoadsAirSystem is used in a zone which also has other forced air HVAC equipment. Otherwise this node name is optional but recommended.
+
+\paragraph{Field: Maximum Heating Supply Air Temperature}\label{field-maximum-heating-supply-air-temperature-000}
+
+The maximum air temperature (degrees C) of the air used for heating the zone. The default is 50C (122F).
+
+\paragraph{Field: Minimum Cooling Supply Air Temperature}\label{field-minimum-cooling-supply-air-temperature-000}
+
+The minimum air temperature (degrees C) of the air used for cooling the zone. The default is 13C (55.4F).
+
+\paragraph{Field: Maximum Heating Supply Air Humidity Ratio}\label{field-maximum-heating-supply-air-humidity-ratio-000}
+
+The maximum humidity ratio (kg of water per kg of dry air) of the hot supply air. The default is 0.0156 kgWater/kgDryAir which corresponds to a 20\%RH at 50C (122F) dry bulb.
+
+\paragraph{Field: Minimum Cooling Supply Air Humidity Ratio}\label{field-minimum-cooling-supply-air-humidity-ratio-000}
+
+The minimum humidity ratio (kg of water per kg of dry air) of the cool supply air. The default is 0.0077 kgWater/kgDryAir which corresponds to a 10C (50F) dew point.
+
+\paragraph{Field: Heating Limit}\label{field-heating-limit-000}
+
+The input must be either \textbf{\emph{LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity}} or \textbf{\emph{NoLimit}}. \textbf{\emph{LimitFlowRate}} means that the heating supply air flow rate will be limited to the value specified in the next input field. \textbf{\emph{LimitCapacity}} means that the sensible heating capacity will be limited to the value specified in the Maximum Sensible Heating Capacity field. \textbf{\emph{LimitFlowRateAndCapacity}} means that both flow rate and capacity will be limited. \textbf{\emph{NoLimit}} (the default) means that there will not be any limit on the heating supply air flow rate or capacity and the subsequent two fields will be ignored.
+
+\paragraph{Field: Maximum Heating Air Flow Rate}\label{field-maximum-heating-air-flow-rate-001}
+
+The maximum heating supply air flow rate in cubic meters per second if heating limit is set to \textbf{\emph{LimitFlowRate or LimitFlowRateAndCapacity}} \emph{.} This field may be autosized. This field is ignored if heating limit is set to \textbf{\emph{NoLimit}} or \textbf{\emph{LimitCapacity}}.~ If blank, there is no limit.
+
+\paragraph{Field: Maximum Sensible Heating Capacity}\label{field-maximum-sensible-heating-capacity-000}
+
+The maximum allowed sensible heating capacity in Watts if Heating Limit is set to \textbf{\emph{LimitCapacity}} or \textbf{\emph{LimitFlowRateAndCapacity}}. This field may be autosized. If blank, there is no limit. If Heating Limit \emph{is set to \textbf{NoLimit}} or \textbf{\emph{LimitFlowRate}}, this field is ignored.
+
+\paragraph{Field: Cooling Limit}\label{field-cooling-limit-000}
+
+The input must be either \textbf{\emph{LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity}} or \textbf{\emph{NoLimit}}. \textbf{\emph{LimitFlowrate}} means that the cooling supply air flow rate will be limited to the value specified in the next input field. \textbf{\emph{LimitCapacity}} means that the total cooling capacity will be limited to the value specified in the Maximum Total Cooling Capacity field. \textbf{\emph{LimitFlowRateAndCapacity}} means that both flow rate and capacity will be limited. \textbf{\emph{NoLimit}} (the default) means that there will not be any limit on the cooling supply air flow rate or capacity and the subsequent two fields will be ignored.
+
+\paragraph{Field: Maximum Cooling Air Flow Rate}\label{field-maximum-cooling-air-flow-rate-001}
+
+The maximum cooling supply air flow rate in cubic meters per second if Cooling Limit is set to \textbf{\emph{LimitFlowRate}} or \textbf{\emph{LimitFlowRateAndCapacity}}\emph{.} This field may be autosized. This field is ignored if cooling limit is set to \textbf{\emph{NoLimit}} or \textbf{\emph{LimitCapacity}}. If blank, there is no limit. If \emph{Cooling Limit is set to \textbf{NoLimit},} this field is ignored\emph{.} This field is required if Outdoor Air Control Type is \textbf{\emph{TemperatureEconomizer}} in order to establish an upper limit on outdoor air flow when the economizer is active\textbf{\emph{.}}
+
+\paragraph{Field: Maximum Total Cooling Capacity}\label{field-maximum-total-cooling-capacity-000}
+
+The maximum allowed total (sensible plus latent) cooling capacity in Watts if Cooling Limit is set to \textbf{\emph{LimitCapacity}} or \textbf{\emph{LimitFlowRateAndCapacity}}. This field may be autosized. If blank, there is no limit. If Cooling Limit \emph{is set to \textbf{NoLimit}} or \textbf{\emph{LimitFlowRate}}\emph{,} this field is ignored\emph{.}
+
+\paragraph{Field: Heating Availability Schedule Name}\label{field-heating-availability-schedule-name-001}
+
+The name of a schedule (ref: Schedule) that denotes whether heating is available. A schedule value greater than 0 (usually 1 is used) indicates that heating and humidification are available. A value less than or equal to 0 (usually 0 is used) denotes that heating and humidification are not available. If blank, heating and humidification are always available.
+
+\paragraph{Field: Cooling Availability Schedule Name}\label{field-cooling-availability-schedule-name-001}
+
+The name of a schedule (ref: Schedule) that denotes whether cooling is available. A schedule value greater than 0 (usually 1 is used) indicates that cooling and dehumidification are available. A value less than or equal to 0 (usually 0 is used) denotes that cooling and dehumidification is not available. If blank, cooling and dehumidification are always available.
+
+\paragraph{Field: Dehumidification Control Type}\label{field-dehumidification-control-type-002}
+
+Select from \textbf{\emph{ConstantSensibleHeatRatio}}, \textbf{\emph{Humidistat, None, or ConstantSupplyHumidityRatio}}. \textbf{\emph{ConstantSensibleHeatRatio}} (the default) means that the ideal loads system will be controlled to meet the sensible cooling load, and the latent cooling rate will be computed using a constant sensible heat ratio (SHR) (see next field). \textbf{\emph{Humidistat}} means that there is a ZoneControl:Humidistat for this zone and the ideal loads system will attempt to meet the humidistat request (i.e.~will dehumidify according to the Dehumidifying Relative Humidity Schedule in the ZoneControl:Humidistat object). \textbf{\emph{None}} means that there is no dehumidification. \textbf{\emph{ConstantSupplyHumidityRatio}} means that during cooling the supply air will always be at the Minimum Cooling Supply Humidity Ratio. For \textbf{\emph{ConstantSensibleHeatRatio}} and \textbf{\emph{Humidistat}}, if the mixed air humidity ratio is less than the target humidity ratio, then the mixed air humidity ratio will be used. For all options, the supply air humidity ratio will never be allowed to exceed saturation at the supply dry bulb temperature.
+
+The selected dehumidification control type is always applied when the unit is in cooling mode. If the unit is in deadband mode (not actively heating the supply air) control type \textbf{\emph{Humidistat}} will be active. If the unit is in heating mode, control type \textbf{\emph{Humidistat}} will be active if the Humidification Control Type field below is set to \emph{Humidistat} or \emph{None}.
+
+This allows the ideal loads system to heat and dehumidify at the same time.
+
+\paragraph{Field: Cooling Sensible Heat Ratio}\label{field-cooling-sensible-heat-ratio-000}
+
+When the Dehumidification Control Type is set to \textbf{\emph{ConstantSensibleHeatRatio}} the ideal loads system will be controlled to meet the sensible cooling load, and the latent cooling rate will be computed using the value of Cooling Sensible Heat Ratio (SHR), where SHR = Sensible Cooling divided by Total Cooling (sensible plus latent). The default is 0.7. If Dehumidification Control Type is set to something other than \textbf{\emph{ConstantSensibleHeatRatio}} then this field will be ignored.
+
+\paragraph{Field: Humidification Control Type}\label{field-humidification-control-type-000}
+
+Select from \textbf{\emph{None}}, \textbf{\emph{Humidistat, or ConstantSupplyHumidityRatio}}. \textbf{\emph{None}} means that there is no humidification. \textbf{\emph{Humidistat}} means that there is a ZoneControl:Humidistat for this zone and the ideal loads system will attempt to meet the humidistat request (i.e., humidify according to the Humidifying Relative Humidity Setpoint Schedule in the ZoneControl:Humidistat object). \textbf{\emph{ConstantSupplyHumidityRatio}} means that during heating the supply air will always be at the Maximum Heating Supply Humidity Ratio. The default is \textbf{\emph{None}}. For \textbf{\emph{Humidistat}}, if the mixed air humidity ratio is greater than the target humidity ratio, then the mixed air humidity ratio will be used. For all options, the supply air humidity ratio will never be allowed to exceed saturation at the supply dry bulb temperature.
+
+The selected humidification control type is always applied when the unit is in heating mode. If the unit is in deadband mode (not actively heating the supply air) control type \textbf{\emph{Humidistat}} will be active. If the unit is in cooling mode, control type \textbf{\emph{Humidistat}} will be active if the Dehumidification Control Type field above is set to \emph{Humidistat} or \emph{None}.
+
+This allows the ideal loads system to cool and humidify at the same time.
+
+\paragraph{Field: Design Specification Outdoor Air Object Name}\label{field-design-specification-outdoor-air-object-name-002}
+
+This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the outdoor air requirements and schedule for this system. The outdoor air flow rate may also be affected by the next two fields, Demand Controlled Ventilation Type and Outdoor Air Economizer Type. If this field is blank, this system will have no outdoor air, and all outdoor air control and heat recovery options will be ignored..
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-002}
+
+This alpha field specifies the node name of the outdoor air inlet node. This node name is also specified in an OutdoorAir:Node or OutdoorAir:NodeList object. If this field is blank, a node name will be created internally.
+
+\paragraph{Field: Demand Controlled Ventilation Type}\label{field-demand-controlled-ventilation-type-000}
+
+This field, along with the Design Specification Outdoor Air Object (if used) specifies how the minimum outdoor air flow rate is calculated. The choices are: \textbf{\emph{None, OccupancySchedule or CO2Setpoint}}. The default is \textbf{\emph{None}}.
+
+\begin{itemize}
+\item
+  \textbf{\emph{None}} means that the design occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field).
+\item
+  \textbf{\emph{OccupancySchedule}} means that the current occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field).
+\item
+  \textbf{\emph{CO2Setpoint}} means that the design occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field). In addition, the minimum outdoor air flow rate may be increased if necessary to maintain the level of indoor air carbon dioxide at or below the setpoint defined in a ZoneControl:ContaminantController object.
+\end{itemize}
+
+\paragraph{Field: Outdoor Air Economizer Type}\label{field-outdoor-air-economizer-type-000}
+
+This field specifies if there is an outdoor air economizer. The choices are: \textbf{\emph{NoEconomizer, DifferentialDryBulb,}} or \textbf{\emph{DifferentialEnthalpy}}. The default is \textbf{\emph{NoEconomizer}}. \textbf{\emph{DifferentialDryBulb}} and \textbf{\emph{DifferentialEnthalpy}} mean that the economizer will increase the outdoor air flow rate above the minimum outdoor air flow (see fields Design Specification Outdoor Air Object Name and Demand Controlled Ventilation Type) when there is a cooling load and the outdoor air temperature or enthalpy is below the zone exhaust air temperature or enthalpy. The \textbf{\emph{DifferentialDryBulb}} and \textbf{\emph{DifferentialEnthalpy}} options require that the Maximum Cooling Air Flow Rate be specified which will be used as the limit for maximum outdoor air flow rate.
+
+\paragraph{Field: Heat Recovery Type}\label{field-heat-recovery-type-000}
+
+Select from \textbf{\emph{None}}, \textbf{Sensible}, or \textbf{\emph{Enthalpy}}. \textbf{\emph{None}} means that there is no heat recovery. \textbf{\emph{Sensible}} means that there is sensible heat recovery whenever the zone exhaust air temperature is more favorable than the outdoor air temperature. \textbf{\emph{Enthalpy}} means that there is latent and sensible heat recovery whenever the zone exhaust air enthalpy is more favorable than the outdoor air enthalpy. The default is \textbf{\emph{None}}.
+
+\paragraph{Field: Sensible Heat Recovery Effectiveness}\label{field-sensible-heat-recovery-effectiveness-000}
+
+The sensible heat recovery effectiveness, where effectiveness is defined as the change in supply temperature divided by the difference in entering supply and relief air temperatures. The default is 0.70.
+
+\paragraph{Field: Latent Heat Recovery Effectiveness}\label{field-latent-heat-recovery-effectiveness-000}
+
+The latent heat recovery effectiveness, where effectiveness is defined as the change in supply humidity ratio divided by the difference in entering supply and relief air humidity ratios. The default is 0.65.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name-000}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Maximum Heating Air Flow Rate and Maximum Cooling Air Flow Rate in a Ideal Load Air System zone HVAC object. The scaled maximum heating and cooling air flow rates are used to size the heating and cooling capacities.
+
+An example of this object in an IDF is:
+
+\begin{lstlisting}
+
+  ZoneHVAC:IdealLoadsAirSystem,
+      Zone1 Ideal Loads System, !- Name
+      AlwaysOn,                !- Availability Schedule Name
+      Zone1 Ideal Loads Supply Node, !- Zone Supply Air Node Name
+      Zone1 Ideal Loads Return Node, ! Zone Exhaust Air Node Name
+      50,                      !- Maximum Heating Supply Air Temperature {C}
+      13,                      !- Minimum Cooling Supply Air Temperature {C}
+      0.0156,                  !- Maximum Heating Supply Air Humidity Ratio {kgWater/kgDryAir}
+      0.0077,                  !- Minimum Cooling Supply Air Humidity Ratio {kgWater/kgDryAir}
+      NoLimit,                 !- Heating Limit
+      ,                        !- Maximum Heating Air Flow Rate {m3/s}
+      ,                        !- Maximum Sensible Heating Capacity {W}
+      NoLimit,                 !- Cooling Limit
+      ,                        !- Maximum Cooling Air Flow Rate {m3/s}
+      ,                        !- Maximum Total Cooling Capacity {W}
+      ,                        !- Heating Availability Schedule Name
+      ,                        !- Cooling Availability Schedule Name
+      ConstantSensibleHeatRatio,  !- Dehumidification Control Type
+      0.7,                     !- Cooling Sensible Heat Ratio
+      None,                    !- Humidification Control Type
+      Office OA Specification, !- Design Specification Outdoor Air Object Name
+      Zone1 Ideal Loads OA Inlet Node, !- Outdoor Air Inlet Node Name
+      None,                    !- Demand Controlled Ventilation Type
+      NoEconomizer,            !- Outdoor Air Economizer Type
+      Enthalpy,                !- Heat Recovery Type
+      0.70,                    !- Sensible Heat Recovery Effectiveness
+      0.65;                    !- Latent Heat Recovery Effectiveness
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-043}
+
+\begin{itemize}
+\item
+  HVAC,Sum,Zone Ideal Loads Supply Air Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Supply Air Total Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Supply Air Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Supply Air Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Supply Air Total Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Supply Air Latent Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Zone Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Zone Latent Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Zone Total Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Zone Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Zone Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Zone Total Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Outdoor Air Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Outdoor Air Latent Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Outdoor Air Total Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Outdoor Air Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Outdoor Air Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Outdoor Air Total Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Heat Recovery Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Heat Recovery Latent Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Heat Recovery Total Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Heat Recovery Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Heat Recovery Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Heat Recovery Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ideal Loads Supply Air Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Supply Air Latent Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Supply Air Total Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Supply Air Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Supply Air Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Supply Air Total Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Zone Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Zone Latent Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Zone Total Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Zone Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Zone Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Zone Total Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Outdoor Air Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Outdoor Air Latent Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Outdoor Air Total Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Outdoor Air Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Outdoor Air Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Outdoor Air Total Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Heat Recovery Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Heat Recovery Latent Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Heat Recovery Total Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Heat Recovery Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Heat Recovery Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Ideal Loads Heat Recovery Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Economizer Active Time {[}hr{]}
+\item
+  HVAC,Sum,Zone Ideal Loads Heat Recovery Active Time {[}hr{]}
+\item
+  HVAC,Average,Zone Ideal Loads Hybrid Ventilation Available Status {[]}
+\item
+  HVAC,Average,Zone Ideal Loads Outdoor Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Ideal Loads Outdoor Air Standard Density Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Average,Zone Ideal Loads Supply Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Zone Ideal Loads Supply Air Standard Density Volume Flow Rate {[}m3/s{]}
+\end{itemize}
+
+\paragraph{Ideal Loads Output Variable Overview}\label{ideal-loads-output-variable-overview}
+
+All of the ZoneHVAC:IdealLoadsAirSystem loads and energy use are reported for Sensible Heating, Latent Heating, Total Heating, Sensible Cooling, Latent Cooling, and Total Cooling. To explain the relationship between the various outputs, Total Cooling Energy will be used.
+
+\emph{Zone Ideal Loads Supply Air Total Cooling Energy} is the district cooling energy consumed by the ideal loads system ``cooling coil'' to cool and dehumidify the supply air.
+
+\emph{Zone Ideal Loads Zone Total Cooling Energy} is the total (sensible plus latent) cooling energy delivered to the zone. If there is no outdoor air, then \emph{Zone Ideal Loads Supply Air Total Cooling Energy = Zone Ideal Loads Zone Total Cooling Energy.}
+
+\emph{Zone Ideal Loads Outdoor Air Total Cooling Energy} is the total (sensible plus latent) cooling energy required to cool the outdoor air to the zone exhaust air temperature and humidity ratio.
+
+\emph{Zone Ideal Loads Heat Recovery Total Cooling Energy} is the total (sensible plus latent) cooling energy supplied by heat recovery. This offsets a portion of the \emph{Zone Ideal Loads Outdoor Air Total Cooling Energy}.
+
+When the economizer is not active, these values are related by the following equation:
+
+\emph{Zone Ideal Loads Supply Air Total Cooling Energy + Zone Ideal Loads Heat Recovery Total Cooling Energy = Zone Ideal Loads Zone Total Cooling Energy+ Zone Ideal Loads Outdoor Air Total Cooling Energy}
+
+\paragraph{Zone Ideal Loads Supply Air Sensible Heating Energy {[}J{]}}\label{zone-ideal-loads-supply-air-sensible-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Supply Air Sensible Heating Rate {[}W{]}}\label{zone-ideal-loads-supply-air-sensible-heating-rate-w}
+
+The sensible heating energy (or rate) added to raise the temperature of the mixed air stream to the temperature of the supply air stream. This is the ideal ``heating coil'' load.
+
+\paragraph{Zone Ideal Loads Supply Air Latent Heating Energy {[}J{]}}\label{zone-ideal-loads-supply-air-latent-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Supply Air Latent Heating Rate {[}W{]}}\label{zone-ideal-loads-supply-air-latent-heating-rate-w}
+
+The latent heating energy (or rate) added to raise the humidity ratio of the mixed air stream to the temperature of the supply air stream. This is the ideal ``humidifier'' load.
+
+\paragraph{Zone Ideal Loads Supply Air Total Heating Energy {[}J{]}}\label{zone-ideal-loads-supply-air-total-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Supply Air Total Heating Rate {[}W{]}}\label{zone-ideal-loads-supply-air-total-heating-rate-w}
+
+The total (sensible and latent) heating energy (or rate) added to raise the mixed air stream to the temperature and humidity ratio of the supply air stream. \emph{Zone Ideal Loads Supply Air Total Heating Energy} is metered as DistrictHeating energy.
+
+\paragraph{Zone Ideal Loads Supply Air Sensible Cooling Energy {[}J{]}}\label{zone-ideal-loads-supply-air-sensible-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Supply Air Sensible Cooling Rate {[}W{]}}\label{zone-ideal-loads-supply-air-sensible-cooling-rate-w}
+
+The sensible cooling energy (or rate) removed to lower the temperature of the mixed air stream to the temperature of the supply air stream. This is the ideal ``cooling coil'' sensible load.
+
+\paragraph{Zone Ideal Loads Supply Air Latent Cooling Energy {[}J{]}}\label{zone-ideal-loads-supply-air-latent-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Supply Air Latent Cooling Rate {[}W{]}}\label{zone-ideal-loads-supply-air-latent-cooling-rate-w}
+
+The latent cooling energy (or rate) removed to lower the humidity ratio of the mixed air stream to the temperature of the supply air stream. This is the ideal ``cooling coil'' latent load.
+
+\paragraph{Zone Ideal Loads Supply Air Total Cooling Energy {[}J{]}}\label{zone-ideal-loads-supply-air-total-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Supply Air Total Cooling Rate {[}W{]}}\label{zone-ideal-loads-supply-air-total-cooling-rate-w}
+
+The total (sensible and latent) cooling energy (or rate) removed to lower the mixed air stream to the temperature and humidity ratio of the supply air stream. \emph{Zone Ideal Loads Supply Air Total Cooling Energy} is metered as DistrictCooling energy. This is the ideal ``cooling coil'' total load.
+
+\paragraph{Zone Ideal Loads Zone Sensible Heating Energy {[}J{]}}\label{zone-ideal-loads-zone-sensible-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Zone Sensible Heating Rate {[}W{]}}\label{zone-ideal-loads-zone-sensible-heating-rate-w}
+
+The sensible heating energy (or rate) added to the zone.
+
+\paragraph{Zone Ideal Loads Zone Latent Heating Energy {[}J{]}}\label{zone-ideal-loads-zone-latent-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Zone Latent Heating Rate {[}W{]}}\label{zone-ideal-loads-zone-latent-heating-rate-w}
+
+The latent heating energy (or rate) added to the zone.
+
+\paragraph{Zone Ideal Loads Zone Total Heating Energy {[}J{]}}\label{zone-ideal-loads-zone-total-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Zone Total Heating Rate {[}W{]}}\label{zone-ideal-loads-zone-total-heating-rate-w}
+
+The total (sensible and latent) heating energy (or rate) added to the zone.
+
+\paragraph{Zone Ideal Loads Zone Sensible Cooling Energy {[}J{]}}\label{zone-ideal-loads-zone-sensible-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Zone Sensible Cooling Rate {[}W{]}}\label{zone-ideal-loads-zone-sensible-cooling-rate-w}
+
+The sensible cooling energy (or rate) removed from the zone.
+
+\paragraph{Zone Ideal Loads Zone Latent Cooling Energy {[}J{]}}\label{zone-ideal-loads-zone-latent-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Zone Latent Cooling Rate {[}W{]}}\label{zone-ideal-loads-zone-latent-cooling-rate-w}
+
+The latent cooling energy (or rate) removed from the zone.
+
+\paragraph{Zone Ideal Loads Zone Total Cooling Energy {[}J{]}}\label{zone-ideal-loads-zone-total-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Zone Total Cooling Rate {[}W{]}}\label{zone-ideal-loads-zone-total-cooling-rate-w}
+
+The total (sensible and latent) cooling energy (or rate) removed from the zone.
+
+\paragraph{Zone Ideal Loads Outdoor Air Sensible Heating Energy {[}J{]}}\label{zone-ideal-loads-outdoor-air-sensible-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Outdoor Air Sensible Heating Rate {[}W{]}}\label{zone-ideal-loads-outdoor-air-sensible-heating-rate-w}
+
+The sensible heating energy (or rate) required to raise the temperature of the outdoor air to the zone exhaust air temperature. This value will be calculated only when heating is active.
+
+\paragraph{Zone Ideal Loads Outdoor Air Latent Heating Energy {[}J{]}}\label{zone-ideal-loads-outdoor-air-latent-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Outdoor Air Latent Heating Rate {[}W{]}}\label{zone-ideal-loads-outdoor-air-latent-heating-rate-w}
+
+The latent heating energy (or rate) required to raise the humidity ratio of the outdoor air to the zone exhaust air humidity ratio. This value will be calculated only when humidification is active.
+
+\paragraph{Zone Ideal Loads Outdoor Air Total Heating Energy {[}J{]}}\label{zone-ideal-loads-outdoor-air-total-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Outdoor Air Total Heating Rate {[}W{]}}\label{zone-ideal-loads-outdoor-air-total-heating-rate-w}
+
+The total (sensible and latent) heating energy (or rate) required to raise the temperature and humidity ratio of the outdoor air to the zone exhaust air humidity ratio. This value will be calculated only when heating or humidification is active.
+
+\paragraph{Zone Ideal Loads Outdoor Air Sensible Cooling Energy {[}J{]}}\label{zone-ideal-loads-outdoor-air-sensible-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Outdoor Air Sensible Cooling Rate {[}W{]}}\label{zone-ideal-loads-outdoor-air-sensible-cooling-rate-w}
+
+The sensible cooling energy (or rate) required to lower (or raise) the temperature of the outdoor air to the zone exhaust air temperature. This value will be calculated only when cooling is active.
+
+\paragraph{Zone Ideal Loads Outdoor Air Latent Cooling Energy {[}J{]}}\label{zone-ideal-loads-outdoor-air-latent-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Outdoor Air Latent Cooling Rate {[}W{]}}\label{zone-ideal-loads-outdoor-air-latent-cooling-rate-w}
+
+The latent cooling energy (or rate) required to lower (or raise) the humidity ratio of the outdoor air to the zone exhaust air humidity ratio. This will be calculated only when dehumidification is active.
+
+\paragraph{Zone Ideal Loads Outdoor Air Total Cooling Energy {[}J{]}}\label{zone-ideal-loads-outdoor-air-total-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Outdoor Air Total Cooling Rate {[}W{]}}\label{zone-ideal-loads-outdoor-air-total-cooling-rate-w}
+
+The total (sensible and latent) cooling energy (or rate) required to lower the temperature and humidity ratio of the outdoor air to the zone exhaust air temperature and humidity ratio. This value will be calculated only when cooling or dehumidification is active.
+
+\paragraph{Zone Ideal Loads Heat Recovery Sensible Heating Energy {[}J{]}}\label{zone-ideal-loads-heat-recovery-sensible-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Heat Recovery Sensible Heating Rate {[}W{]}}\label{zone-ideal-loads-heat-recovery-sensible-heating-rate-w}
+
+The sensible heating energy (or rate) added to the outdoor air stream from heat recovery.
+
+\paragraph{Zone Ideal Loads Heat Recovery Latent Heating Energy {[}J{]}}\label{zone-ideal-loads-heat-recovery-latent-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Heat Recovery Latent Heating Rate {[}W{]}}\label{zone-ideal-loads-heat-recovery-latent-heating-rate-w}
+
+The latent heating energy (or rate) added to the outdoor air stream from heat recovery.
+
+\paragraph{Zone Ideal Loads Heat Recovery Total Heating Energy {[}J{]}}\label{zone-ideal-loads-heat-recovery-total-heating-energy-j}
+
+\paragraph{Zone Ideal Loads Heat Recovery Total Heating Rate {[}W{]}}\label{zone-ideal-loads-heat-recovery-total-heating-rate-w}
+
+The total (sensible and latent) heating energy (or rate) added to the outdoor air stream from heat recovery.
+
+\paragraph{Zone Ideal Loads Heat Recovery Sensible Cooling Energy {[}J{]}}\label{zone-ideal-loads-heat-recovery-sensible-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Heat Recovery Sensible Cooling Rate {[}W{]}}\label{zone-ideal-loads-heat-recovery-sensible-cooling-rate-w}
+
+The sensible cooling energy (or rate) removed from the outdoor air stream from heat recovery.
+
+\paragraph{Zone Ideal Loads Heat Recovery Latent Cooling Energy {[}J{]}}\label{zone-ideal-loads-heat-recovery-latent-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Heat Recovery Latent Cooling Rate {[}W{]}}\label{zone-ideal-loads-heat-recovery-latent-cooling-rate-w}
+
+The latent cooling energy (or rate) removed from the outdoor air stream from heat recovery.
+
+\paragraph{Zone Ideal Loads Heat Recovery Total Cooling Energy {[}J{]}}\label{zone-ideal-loads-heat-recovery-total-cooling-energy-j}
+
+\paragraph{Zone Ideal Loads Heat Recovery Total Cooling Rate {[}W{]}}\label{zone-ideal-loads-heat-recovery-total-cooling-rate-w}
+
+The total (sensible and latent) cooling energy (or rate) removed from the outdoor air stream from heat recovery.
+
+\paragraph{Zone Ideal Loads Economizer Active Time {[}hr{]}}\label{zone-ideal-loads-economizer-active-time-hr}
+
+Hours when the Ideal Loads economizer increased the outdoor air flow rate above the minimum.
+
+\paragraph{Zone Ideal Loads Heat Recovery Active Time {[}hr{]}}\label{zone-ideal-loads-heat-recovery-active-time-hr}
+
+Hours when the Ideal Loads heat recovery was actively heating or cooling the outdoor air stream.
+
+\paragraph{\texorpdfstring{Zone Ideal Loads Hybrid Ventilation Available Status {[]}}{Zone Ideal Loads Hybrid Ventilation Available Status }}\label{zone-ideal-loads-hybrid-ventilation-available-status}
+
+This is the availability status of the ideal loads object as set by the hybrid ventilation manager. Rules to determine the availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 and 1. These integers represent NoAction (0) and ForceOff (1). When the availability status is ForceOff, the unit is turned off regardless of its availability schedule. The other status flag i.e.~NoAction does not control the unit and the controls of the unit turn it back on. Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\paragraph{Zone Ideal Loads Outdoor Air Mass Flow Rate {[}kg/s{]}}\label{zone-ideal-loads-outdoor-air-mass-flow-rate-kgs}
+
+The mass flow rate of the outdoor air stream in kg/s.
+
+\paragraph{Zone Ideal Loads Outdoor Air Standard Density Volume Flow Rate {[}m3/s{]}}\label{zone-ideal-loads-outdoor-air-standard-density-volume-flow-rate-m3s}
+
+The volume flow rate of the outdoor air stream in m3/s using the standard density. The standard density is determined for dry air at the standard barometric pressure for the location's elevation and a temperature of 20.0ºC. The standard density does not vary over time.
+
+\paragraph{Zone Ideal Loads Supply Air Mass Flow Rate {[}kg/s{]}}\label{zone-ideal-loads-supply-air-mass-flow-rate-kgs}
+
+The mass flow rate of the supply air stream in kg/s.
+
+\paragraph{Zone Ideal Loads Supply Air Standard Density Volume Flow Rate {[}m3/s{]}}\label{zone-ideal-loads-supply-air-standard-density-volume-flow-rate-m3s}
+
+The volume flow rate of the supply air stream in m3/s using the standard density. The standard density is determined for dry air at the standard barometric pressure for the location's elevation and a temperature of 20.0ºC. The standard density does not vary over time.
+
+\subsection{ZoneHVAC:FourPipeFanCoil}\label{zonehvacfourpipefancoil}
+
+What is a fan coil unit? Like many HVAC terms, ``fan coil unit'' is used rather loosely. Sometimes it is used for terminal units that would be better described as powered induction units. Carrier and others use the term for the room side of refrigerant-based split systems. Here we are modeling in-room forced-convection hydronic units. The hydronic heating coil may be replaced with an electric heating coil. Typically these units are small (200 -- 1200 cfm) and self-contained. They are mostly used in exterior zones, usually in hotels, apartments, or offices. They may be connected to ducted outside air, or have a direct outside air vent, but they do not have outside air economizers. Units with outside air economizers are marketed (in the United States) as unit ventilators. Unit ventilators are typically bigger than fan coils and are widely used in classrooms or other applications where ventilation is a priority. If a zonal unit with an outside economizer is desired, \emph{ZoneHVAC:UnitVentilator} should be used.
+
+The heating or cooling output of the unit ventilator is controlled by varying the air flow rate, the water flow rate, or both. Air flow rate can be controlled by cycling the fan on/off or with a variable speed fan drive. The most common setup is a two or three speed fan with the speed selected by hand. The fan then cycles on/off to control heating / cooling output. The controls are often a wall mounted thermostat with hand selection of heating/cooling and fan speed (off/low/medium/high). These controls may also be mounted on the unit.
+
+Carrier offers a retrofit VSD motor for fan coil units. It claims up to 45\% energy savings from such a retrofit, as well as increased comfort and less noise compared to a cycling fan (fan coil fans are typically noisy and inefficient). Some other manufacturers are also offering units with VSD fans. Variable speed fans appear to offer an easy way to significantly increase the efficiency of what have typically been very inefficient units.
+
+EnergyPlus provides 6 capacity control methods for this unit:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\item
+  multi-speed cycling fan with constant water flow rate
+\item
+  constant speed continuous fan with variable water flow rate
+\item
+  variable-speed fan with constant water flow rate
+\item
+  variable-speed fan with variable water flow rate
+\item
+  multi-speed fan with cycling between speeds and constant water flow.
+\item
+  fan speed control based on ASHRAE 90.1
+\end{enumerate}
+
+In EnergyPlus the fan coil units are modeled as compound components. That is, they are assembled from other components. Fan coils contain an outdoor air mixer, a fan, a heating coil and a cooling coil. These components are described elsewhere in this document. The fan coil input simply requires the names of these four components, which have to be described elsewhere in the input. The input also requires the name of an availability schedule, maximum airflow rate, outdoor airflow rate, and maximum and minimum hot (for hydronic heating coil only) and cold water volumetric flow rates. The unit is connected to the zone inlet and exhaust nodes and the outdoor air by specifying unit inlet, and outlet air node names and the outdoor air mixer object name. The outdoor air mixer child object provides the outdoor air and relief air nodes names. Note that the unit air inlet node should be the same as a zone exhaust node and the unit outlet node should be the same as a zone inlet node. The fan coil unit is connected to a hot water loop through its hot water coil or with no hot water loop when using an electric coil (demand side) and to a chilled water loop (demand side) through its cooling coil.
+
+Note that the type of fan component associated with the fan coil unit depends on the type of capacity control method chosen. For \emph{ConstantFanVariableFlow~} a \emph{Fan:OnOff} or \emph{Fan:ConstantVolume} should be used. For \emph{CyclingFan}, a \emph{Fan:OnOff} should be used, for \emph{VariableFanVariableFlow} or \emph{VariableFanConstantFlow} a \emph{Fan:VariableVolume}, for \emph{MultiSpeedFan} a \emph{Fan:OnOff} should be used, and for \emph{ASHRAE90VariableFan}, a \emph{Fan:OnOff} or \emph{Fan:VariableVolume} should be chosen.
+
+Fan coil units can be 4-pipe or 2-pipe. For 4-pipe units there are 2 supply pipes and 2 return pipes. For 2-pipe units there is a single supply pipe and a single return pipe and the supply is switched between hot and chilled water depending on the season. EnergyPlus models 4-pipe units, but the 4-pipe model can be used to model 2-pipe~units by using the coil availability schedules to make sure that either hot or chilled water is exclusively available. Fan coil units with hydronic heat can instead be modeled using an electric heating coil if desired (i.e., replace the hydronic heating coil with an electric heating coil).
+
+\subsubsection{Inputs}\label{inputs-1-053}
+
+\paragraph{Field: Name}\label{field-name-1-051}
+
+A unique user assigned name for an instance of a Fan Coil unit. Any reference to this Fan Coil unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-1-015}
+
+The name of the schedule (ref: Schedule) that denotes whether the fan coil unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\textbf{\emph{Field: Capacity Control~Method}}
+
+This input denotes how the unit's output is controlled in order to meet zone heating or cooling requirement. The choices are \textbf{\emph{ConstantFanVariableFlow}}, \textbf{\emph{CyclingFan}}, \textbf{\emph{VariableFanVariableFlow}}, \textbf{\emph{VariableFanConstantFlow}}, \textbf{\emph{MultiSpeedFan}}, or \textbf{\emph{ASHRAE90VariableFan}}. For \emph{ConstantFanVariableFlow}, the fan speed is held constant to produce a fixed air flow rate whenever the unit is scheduled on. The hot water or chilled flow rate is varied so that the unit output matches the zone heating or cooling requirement. For \emph{CyclingFan}, the fan speed is chosen so that the unit capacity is greater than or equal to the heating / cooling load and the fan is cycled to match unit output with the load. For \emph{VariableFanVariableFlow} ~both air and water flow rates are varied to match the load. For \emph{VariableFanConstantFlow,} the water flow rate is at full flow and the fan speed varies to meet the load. For \emph{MultiSpeedFan} the water flow rate is at full flow when there is load or fully closed when there is no load and the supply air flow rate is varied by varying the fan speed in order to match the load. For \emph{ASHRAE90VariableFan}, the fan air flow rate is reduced according to the low speed supply air flow ratio when the zone sensible load is less than the zone sensible load multiplied by the low speed supply air flow ratio. The water coil water flow rate, or the electric heating coil part-load ratio, is modulated to meet the zone load. If the zone sensible load is greater than the zone sensible load multiplied by the low speed supply air flow ratio, then the air and water flow rate is increased to meet the load. If the zone load is greater than the design sensible load, the fan air flow rate is maintained at the maximum value while the water flow rate is further increased to the maximum available while electric heating coils are maintained at the maximum output.
+
+\textbf{\emph{Note: when ASHRAE90VariableFan is selected, if the the Minimum Supply Air Temperature in Cooling/Heating Mode inputs are not specified, the simulation must include zone sizing to calculate the zone design sensible cooling and heating load used to modulate the fan speed and, for water coils, the water flow rate or for electric heating coils, the part load ratio.}}
+
+\textbf{\emph{MultiSpeedFan:}} for a given load, the fan cycles between speeds when fan speed selected is higher than the minimum speed or the fan cycles on-off when the fan speed selected is the minimum and the fan operating schedule is cycling fan. When the fan is operating as a continuous fan, then the fan runs at minimum speed even when there is no load to meet. When the speed selected is higher than the minimum speed, then the fan cycles between consecutive speed regardless of the fan operating schedule type. The model selects at what fan speed to run depending on cooling or heating load.
+
+\paragraph{Field: Maximum Supply Air Flow Rate}\label{field-maximum-supply-air-flow-rate}
+
+The maximum volumetric airflow rate (m\(^{3}\)/sec) through the fan coil unit. This is also the design, rated airflow rate of the unit.
+
+\paragraph{Field: Low Speed Supply Air Flow Ratio}\label{field-low-speed-supply-air-flow-ratio-000}
+
+This numerical field specifies the ratio of the low speed flow rate to the maximum supply air flow rate. This value should be less than the \emph{Medium Speed Supply Air Flow Ratio.} If left blank, the default value is 0.33. Leave this field blank if the capacity control method selected is not \emph{CyclingFan} or \emph{ASHRAE90VariableFan}. The suggested value is 0.5 when using the ASHRAE90VariableFan capacity control method.
+
+\paragraph{Field: Medium Speed Supply Air~ Flow Ratio}\label{field-medium-speed-supply-air-flow-ratio-000}
+
+This numerical field specifies the ratio of the medium speed flow rate to the maximum supply air flow rate. Its value should be greater than the \emph{Low Speed Supply Air Flow Ratio} but less than 1. If left blank, the default value is 0.66. Leave this field blank if the capacity control method selected is not \emph{CyclingFan} or \emph{MultiSpeedFan}.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-002}
+
+If the fan coil unit uses outdoor air, this field specifies the outdoor air volumetric flow rate (m\(^{3}\)/sec). This flow rate should be less than or equal to the maximum airflow rate. A value of zero specifies no outdoor air.
+
+\paragraph{Field: Outdoor Air Schedule Name}\label{field-outdoor-air-schedule-name-000}
+
+The name of a schedule whose values (0.0 to 1.0) are used as multipliers to alter the outdoor air flow rate. If this field is left blank, the values will default to 1.0.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-009}
+
+The name of the HVAC system node from which the fan coil unit draws its indoor air. This should be one of zone exhaust nodes for the zone which the fan coil unit is serving.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-008}
+
+The name of the HVAC system node to which the fan coil unit sends its outlet air. This should be one of the inlet air nodes of the zone which is being served.
+
+\paragraph{Field: Outdoor Air Mixer Object Type}\label{field-outdoor-air-mixer-object-type-000}
+
+This field specifies the type of outdoor air mixer used by this fan coil unit. The outdoor air mixer component is part of the fan coil compound object. The only available outdoor air mixer type is:
+
+OutdoorAir:Mixer
+
+\paragraph{Field: Outdoor Air Mixer Name}\label{field-outdoor-air-mixer-name-000}
+
+The name of an outdoor air mixer component (object:OutdoorAir:Mixer) which composes part of the fan coil unit. Note that the return air node of the outdoor air mixer should be the same node as the air inlet node of the fan coil unit. In addition, the outdoor air mixer's mixed air node should be the same as the inlet air node of the fan coil unit's fan.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-000}
+
+This field specifies the type of supply air fan object used by this fan coil. The supply air fan is part of the fan coil compound object. The only valid supply air fan types are:
+
+\begin{itemize}
+\item
+  Fan:OnOff
+\item
+  Fan:ConstantVolume
+\item
+  Fan:VariableVolume
+\end{itemize}
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-000}
+
+The name of a fan component that composes part of the fan coil unit. Note that the fan's maximum flow rate should be the same as the maximum airflow rate of the fan coil unit and the type of fan object should correspond to the capacity control method. Namely, for \emph{ConstantFanVariableFlow~} a \emph{Fan:OnOff} or \emph{Fan:ConstantVolume} should be used. For \emph{CyclingFan}, a \emph{Fan:OnOff} should be used. For \emph{VariableFanVariableFlow} or \emph{VariableFanConstantFlow} a \emph{Fan:VariableVolume} should be chosen. For \emph{MultiSpeedFan} a \emph{Fan:OnOff} should be used. And for \emph{ASHRAE90VariableFan}, a \emph{Fan:OnOff} or \emph{Fan:VariableVolume} should be chosen.
+
+\begin{lstlisting}
+The fan’s inlet node should be the same as the outdoor air mixer’s mixed air node.
+The fan’s outlet node should be the same as the cooling coil’s air inlet node.
+\end{lstlisting}
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-003}
+
+This field specifies the type of chilled water cooling coil to be modeled for this fan coil unit. Only the following coil types can be used:
+
+\begin{itemize}
+\item
+  Coil:Cooling:Water
+\item
+  Coil:Cooling:Water:DetailedGeometry
+\item
+  CoilSystem:Cooling:Water:HeatExchangerAssisted
+\end{itemize}
+
+The input requirements for these chilled water coil objects are described elsewhere in this document.
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-003}
+
+The name of the cooling coil component that composes part of the fan coil unit. The cooling coil air inlet node should be the same as the fan outlet node. The cooling coil air outlet node should be the same as the heating coil air inlet node.
+
+Only the following coil types can be used:
+
+\begin{itemize}
+\item
+  Coil:Cooling:Water
+\item
+  Coil:Cooling:Water:DetailedGeometry
+\item
+  CoilSystem:Cooling:Water:HeatExchangerAssisted
+\end{itemize}
+
+\paragraph{Field: Maximum Cold Water Flow Rate}\label{field-maximum-cold-water-flow-rate-000}
+
+The maximum cold water volumetric flow rate (m\(^{3}\)/sec) through the fan coil unit's cooling coil.
+
+\paragraph{Field: Minimum Cold Water Flow Rate}\label{field-minimum-cold-water-flow-rate-000}
+
+The minimum cold water volumetric flow rate (m\(^{3}\)/sec) through the fan coil unit's cooling coil.
+
+\paragraph{Field: Cooling Convergence Tolerance}\label{field-cooling-convergence-tolerance-000}
+
+The convergence tolerance for the control of the unit cooling output. The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The cooling convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {{Q_{fancoil,out}} - {Q_{zoneload}}} \right|}}{{{Q_{zoneload}}}} \le CoolingConvergenceTolerance
+\end{equation}
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-003}
+
+This field is the type of coil that is used for heating in the fan coil system. It is used in conjunction with the heating coil name (see next field) to specify the heating coil present within the system. The only allowable heating coil types are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\end{itemize}
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-003}
+
+The name of the heating coil component that composes part of the fan coil unit. The heating coil air inlet node should be the same as the cooling coil outlet node. The heating coil air outlet node should be the same as the fan coil air outlet node.
+
+Only the following coil types can be used:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\end{itemize}
+
+\paragraph{Field: Maximum Hot Water Flow Rate}\label{field-maximum-hot-water-flow-rate-000}
+
+The maximum hot water volumetric flow rate (m\(^{3}\)/sec) through the fan coil unit's heating coil. This field is not used with an electric heating coil.
+
+\paragraph{Field: Minimum Hot Water Flow Rate}\label{field-minimum-hot-water-flow-rate-000}
+
+The minimum hot water volumetric flow rate (m\(^{3}\)/sec) through the fan coil unit's heating coil. This field is not used with an electric heating coil.
+
+\paragraph{Field: Heating Convergence Tolerance}\label{field-heating-convergence-tolerance-000}
+
+The convergence tolerance for the control of the unit heating output. The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The heating convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {{Q_{fancoil,out}} - {Q_{zoneload}}} \right|}}{{{Q_{zoneload}}}} \le HeatingConvergenceTolerance
+\end{equation}
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-002}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this object's fan. If the fan coil is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this object should be on or off.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name-1}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Maximum Air Flow Rate in this Four Pipe FanCoil zone HVAC object. The scaled Maximum Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-000}
+
+This input field is the name of a schedule that controls fan operation. Schedule Name values of 0 denote cycling fan operation (fan cycles with heating or cooling coil). Schedule values greater than 0 denote constant fan operation (fan runs continually regardless of coil operation). The fan operating mode defaults to cycling fan operation if this field is left blank. This input field is currently used with \emph{MultiSpeedFan} capacity control method only.
+
+\paragraph{Field: Minimum Supply Air Temperature in Cooling Mode}\label{field-minimum-supply-air-temperature-in-cooling-mode}
+
+This optional input is used only when \emph{Capacity Control~Method = ASHRAE90VariableFan}. Specify the minimum supply air temperature in cooling mode. When the fan coil capacity is greater than the zone load, the fan speed will modulate down to the minimum fan speed, based on the Low Speed Supply Air Flow Ratio input field, and the water flow rate will also be reduced to maintain the zone thermostat set point temperature. When the zone load is one-half the fan coil capacity, the fan will operate at the minimum speed. When these fields are not entered, a zone sizing simulation must be performed. Both the cooling and heating supply air temperature must be entered or blank in unison. Values must be greater than 0 or this field is autosizable. A value of 0 (in both fields) will disregard these fields.
+
+\paragraph{Field: Maximum Supply Air Temperature in Heating Mode}\label{field-maximum-supply-air-temperature-in-heating-mode}
+
+This optional input is used only when \emph{Capacity Control~Method = ASHRAE90VariableFan}. Specify the maximum supply air temperature in heating mode. When the fan coil capacity is greater than the zone load, the fan speed will modulate down to the minimum fan speed, based on the Low Speed Supply Air Flow Ratio input field, and the water flow rate will also be reduced to maintain the zone thermostat set point temperature. When the zone load is one-half the fan coil capacity, the fan will operate at the minimum speed. When these fields are not entered, a zone sizing simulation must be performed. Both the cooling and heating supply air temperature must be entered or blank in unison. Values must be greater than 0 or this field is autosizable. A value of 0 (in both fields) will disregard these fields.
+
+An example input for a fan coil unit, including its constituent components, is shown below.
+
+\begin{lstlisting}
+
+  ZoneHVAC:FourPipeFanCoil,
+      Zone1FanCoil,            !- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      ConstantFanVariableFlow, !- Capacity Control Method
+      autosize,                !- Maximum Supply Air Flow Rate {m3/s}
+      ,                        !- Low Speed Supply Air Flow Ratio
+      ,                        !- Medium Speed Supply Air Flow Ratio
+      autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
+      OUTAIRFANCOILSCHEDULE,   !- Outdoor Air Schedule Name
+      Zone1FanCoilAirInletNode,!- Air Inlet Node Name
+      Zone1FanCoilAirOutletNode,  !- Air Outlet Node Name
+      OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type
+      Zone1FanCoilOAMixer,     !- Outdoor Air Mixer Name
+      Fan:ConstantVolume,      !- Supply Air Fan Object Type
+      Zone1FanCoilFan,         !- Supply Air Fan Name
+      Coil:Cooling:Water,      !- Cooling Coil Object Type
+      Zone1FanCoilCoolingCoil, !- Cooling Coil Name
+      autosize,                !- Maximum Cold Water Flow Rate {m3/s}
+      0.0,                     !- Minimum Cold Water Flow Rate {m3/s}
+      0.001,                   !- Cooling Convergence Tolerance
+      Coil:Heating:Water,      !- Heating Coil Object Type
+      Zone1FanCoilHeatingCoil, !- Heating Coil Name
+      autosize,                !- Maximum Hot Water Flow Rate {m3/s}
+      0.0,                     !- Minimum Hot Water Flow Rate {m3/s}
+      0.001;                   !- Heating Convergence Tolerance
+
+  OutdoorAir:Mixer,
+      Zone1FanCoilOAMixer, ! name
+      Zone1FanCoilOAMixerOutletNode, !Mixed Air Node Name
+      Zone1FanCoilOAInNode, !Outdoor Air Stream Node Name
+      Zone1FanCoilExhNode, !Relief Air Stream Node Name
+      Zone1FanCoilAirInletNode; !Return Air Stream Node Name
+
+  Fan:OnOff,
+      Zone1FanCoilFan,         !- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      0.5,                     !- Fan Total Efficiency
+      75.0,                    !- Pressure Rise {Pa}
+      autosize,                !- Maximum Flow Rate {m3/s}
+      0.9,                     !- Motor Efficiency
+      1.0,                     !- Motor In Airstream Fraction
+      Zone1FanCoilOAMixerOutletNode,  !- Air Inlet Node Name
+      Zone1FanCoilFanOutletNode,  !-Air Outlet Node Name
+      FanPowerRatioCurve,      !- Fan Power Ratio Function of Speed Ratio Curve Name
+      FanEffRatioCurve;        !- Fan Efficiency Ratio Function of Speed Ratio Curve Name
+
+  Coil:Cooling:Water,
+      Zone1FanCoilCoolingCoil, !- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      autosize,                !- Design Water Flow Rate {m3/s}
+      autosize,                !- Design Air Flow Rate {m3/s}
+      autosize,                !- Design Inlet Water Temperature {C}
+      autosize,                !- Design Inlet Air Temperature {C}
+      autosize,                !- Design Outlet Air Temperature {C}
+      autosize,                !- Design Inlet Air Humidity Ratio {kgWater/kgDryAir}
+      autosize,                !- Design Outlet Air Humidity Ratio {kgWater/kgDryAir}
+      Zone1FanCoilChWInletNode,!- Water Inlet Node Name
+      Zone1FanCoilChWOutletNode,  !- Water Outlet Node Name
+      Zone1FanCoilFanOutletNode,  !- Air Inlet Node Name
+      Zone1FanCoilCCOutletNode,!-Air Outlet Node Name
+      SimpleAnalysis,          !- Type of Analysis
+      CrossFlow;               !- Heat Exchanger Configuration
+
+  Coil:Heating:Water,
+      Zone1FanCoilHeatingCoil, !- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      autosize,                !- U-Factor Times Area Value {W/K}
+      autosize,                !- Maximum Water Flow Rate {m3/s}
+      Zone1FanCoilHWInletNode, !- Water Inlet Node Name
+      Zone1FanCoilHWOutletNode,!- Water Outlet Node Name
+      Zone1FanCoilCCOutletNode,!- Air Inlet Node Name
+      Zone1FanCoilAirOutletNode,  !-Air Outlet Node Name
+      UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
+      autosize,                !- Nominal Capacity {W}
+      82.2,                    !- Design Inlet Water Temperature {C}
+      16.6,                    !- Design Inlet Air Temperature {C}
+      71.1,                    !- Design Outlet Water Temperature {C}
+      32.2;                    !- Design Outlet Air Temperature {C}
+
+  Curve:Exponent,
+      FanPowerRatioCurve,      !- Name
+      0.0,                     !- Coefficient1 Constant
+      1.0,                     !- Coefficient2 Constant
+      3.0,                     !- Coefficient3 Constant
+      0.0,                     !- Minimum Value of x
+      1.5,                     !- Maximum Value of x
+      0.01,                    !- Minimum Curve Output
+      1.5;                     !- Maximum Curve Output
+
+  Curve:Cubic,
+     FanEffRatioCurve,        !- Name
+     0.33856828,              !- Coefficient1 Constant
+     1.72644131,              !- Coefficient2 x
+     -1.49280132,             !- Coefficient3 x**2
+     0.42776208,              !- Coefficient4 x**3
+     0.5,                     !- Minimum Value of x
+     1.5,                     !- Maximum Value of x
+     0.3,                     !- Minimum Curve Output
+     1.0;                     !- Maximum Curve Output
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-1-033}
+
+\begin{itemize}
+\item
+  HVAC,Average,Fan Coil Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Fan Coil Heating Energy {[}J{]}
+\item
+  HVAC,Average,Fan Coil Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Fan Coil Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Fan Coil Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Fan Coil Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Fan Coil Fan Electric Power{[}W{]}
+\item
+  HVAC,Sum,Fan Coil Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Fan Coil Runtime Fraction {[]}
+\item
+  HVAC,Average, Fan Coil Fan Speed Level {[]}
+\item
+  HVAC,Average, Fan Coil Part Load Ratio {[]}
+\item
+  HVAC,Average, Fan Coil Availability Status {[]}
+\item
+  HVAC,Average, Fan Coil Part Load Ratio {[]}
+\item
+  HVAC,Average, Fan Coil Speed Ratio {[]}
+\end{itemize}
+
+\paragraph{Fan Coil Heating Rate {[}W{]}}\label{fan-coil-heating-rate-w}
+
+This field reports the dry air heating addition rate of the fan coil unit to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the unit.
+
+\paragraph{Fan Coil Heating Energy {[}J{]}}\label{fan-coil-heating-energy-j}
+
+This field is the dry air heat addition of the fan coil unit to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit, and the timestep.
+
+\paragraph{Fan Coil Total Cooling Rate {[}W{]}}\label{fan-coil-total-cooling-rate-w}
+
+This field is the total (sensible and latent) heat extraction rate of the fan coil unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
+
+\paragraph{Fan Coil Total Cooling Energy {[}J{]}}\label{fan-coil-total-cooling-energy-j}
+
+This field is the total (sensible and latent)~ heat extraction of the fan coil unit from the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit, and the timestep.
+
+\paragraph{Fan Coil Sensible Cooling Rate {[}W{]}}\label{fan-coil-sensible-cooling-rate-w}
+
+This field reports the dry air sensible heat extraction rate of the fan coil unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
+
+\paragraph{Fan Coil Sensible Cooling Energy {[}J{]}}\label{fan-coil-sensible-cooling-energy-j}
+
+This field is the dry air sensible heat extraction of the fan coil unit from the zone it is serving in Joules over the timestep being reported. This is determined by the outlet and zone conditions, the mass flow rate through the unit, and the timestep.
+
+\paragraph{Fan Coil Fan Electric Power {[}W{]}}\label{fan-coil-fan-electric-power-w}
+
+This field reports the electricity consumption rate of the fan coil unit in Watts.
+
+\paragraph{Fan Coil Fan Electric Energy {[}J{]}}\label{fan-coil-fan-electric-energy-j}
+
+This field is the electricity consumption of the fan coil unit in Joules over the timestep being reported.
+
+\paragraph{\texorpdfstring{Fan Coil Runtime Fraction{[]}}{Fan Coil Runtime Fraction}}\label{fan-coil-runtime-fraction}
+
+This field is the fraction of the system timestep the fan coil unit is running for the \emph{CyclingFan} capacity control method.~ This variable is defined only for the \emph{CyclingFan} capacity control method.
+
+\paragraph{\texorpdfstring{Fan Coil Fan Speed Level {[]}}{Fan Coil Fan Speed Level }}\label{fan-coil-fan-speed-level}
+
+This field is indicates the speed chosen for the fan in the \emph{CyclingFan} and \emph{MultiSpeedFan} capacity control methods.~ A value of `0' means that the unit is off, `1' the fan is running at its low speed, `2' medium speed, and `3' high speed (maximum). This variable is defined only for the \emph{CyclingFan} and \emph{MultiSpeedFan} capacity control methods.
+
+\paragraph{\texorpdfstring{Fan Coil Part Load Ratio {[]}}{Fan Coil Part Load Ratio }}\label{fan-coil-part-load-ratio}
+
+When the capacity control method is \emph{VariableFanVariableFlow} or \emph{VariableFanConstantFlow,} this output variable reports the unit part load ratio (ratio of unit heating / cooling output to the maximum heating / cooling output). This variable is defined only for \emph{VariableFanVariableFlow}, \emph{VariableFanConstantFlow} or \emph{MultiSpeedFan} capacity control methods. The unit part load ratio is applicable to \emph{MultiSpeedFan} only when the fan speed level selected is the minimum (Speed 1).
+
+\paragraph{\texorpdfstring{Fan Coil Availability Status {[]}}{Fan Coil Availability Status }}\label{fan-coil-availability-status}
+
+This is the availability status of the fan coil unit fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the fan coil unit~ object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\paragraph{\texorpdfstring{Fan Coil Speed Ratio {[]}}{Fan Coil Speed Ratio }}\label{fan-coil-speed-ratio}
+
+This output variable is the ratio of time in a system timestep that the fan coil unit is at rated speed between two consecutive speed levels ( {[}load -- Capacity at Fan Speed i-1{]} / {[}Capacity at Fan Speed i -- Capacity at Fan Speed i-1{]}). The fan speed ratio has minimum value of 0.0, and a maximum value of 1.0 and any value in between as it is averaged over the timestep. The value is 0.0 during Speed Level 1 operation. Hydronic FanCoil units speed ratio depends on the fan speed and current load. The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the lower speed runs in the rest of the system timestep.
+
+\subsection{ZoneHVAC:UnitVentilator}\label{zonehvacunitventilator}
+
+Unit ventilators are zone equipment units which are assembled from other components. They contain a built-in outdoor air mixer, a fan, a heating coil, and a cooling coil. These components are described elsewhere in this document, except the built-in outdoor air mixer which is contained within the unit ventilator statement. The unit ventilator input simply requires the names of these other three components, which have to be described elsewhere in the input. The input also requires the name of an availability schedule, maximum airflow rate, outdoor air control information (control type and schedules), an outdoor airflow rate, and maximum and minimum hot and cold water mass flow rates. The unit is connected to the zone inlet and exhaust nodes and the outdoor air by specifying unit inlet, outlet, outdoor air and exhaust (relief) air node names. Note that the unit air inlet node should be the same as a zone exhaust node and the unit outlet node should be the same as a zone inlet node. In general, the unit ventilator input is very similar to the fan coil unit input, and the unit is connected to a hot water loop (demand side) through its hot water coil and to a chilled water loop (demand side) through its cooling coil.
+
+The main difference between the fan coil and unit ventilator input is that the unit ventilator has a built-in outdoor air mixer with its own specialized controls. The outdoor air control type can be selected from one of the following options: ``variable percent'', ``fixed temperature'' or ``fixed amount''. In fixed temperature control, the amount of outdoor air is varied between the minimum outdoor air fraction (specified by a schedule) and 100\% outdoor air to obtain a mixed air temperature as close as possible to the temperature schedule defined in the input. Variable percent control will also vary the amount of outdoor air between the minimum and maximum fractions (both specified in input by the user) to meet the load without the use of a coil if possible. In fixed amount control, the outdoor air flow rate is fixed to the specified value by the user. In this control strategy, the maximum outdoor air flow rate and schedule are automatically set to be equal to the minimum outdoor air flow rate and schedule. These control types are based on the 2004 ASHRAE Systems and Equipment Handbook (pp.~31.1-31.3) description of unit ventilator systems.
+
+The unit is controlled to meet the zone (remaining) heating or cooling demand. If there is a heating demand, the cooling coil is off and the hot water flow through the heating coil is throttled to meet the demand. The hot water control node must be specified (same as the hot water coil inlet node). If there is a cooling demand from the zone, the hot water coil is off and the chilled water flow through the cooling coil is throttled to meet the load. The cooling coil control node must be specified (same as the cooling coil inlet node). Finally both heating and cooling require a convergence tolerance, which is the tolerance denoting how closely the fan coil unit will meet the heating or cooling load. The tolerance is always relative to the zone load.
+
+Overall, control of the unit must consider the outdoor air. Here is a more detailed description of the overall unit control:
+
+\textbf{Off:} Unit is schedule off or there is no load on it. All flow rates are set to zero and the temperatures are set to zone conditions (except for the outdoor air inlet). Outdoor air requirements will not override this condition.
+
+\textbf{Heating/No Coil/VariablePercent:} The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and variable percent outdoor air control type has been specified. In this case, the variable percent outdoor air controls what happens with the outdoor air. If the outside temperature is greater than the return temperature, then the outdoor air is set to the maximum as defined by the user input. If the outdoor air temperature is less than the return temperature from the zone, then the outdoor air is set to the minimum outdoor air flow rate as defined by the user. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
+
+\textbf{Heating/No Coil/FixedTemperature:} The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate.
+
+\textbf{Heating/No Coil/FixedAmount:} The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
+
+\textbf{Heating /With Coil/VariablePercent:} The unit is on, there is a heating load, and variable percent control is specified. The outdoor air fraction is set to the minimum outdoor air fraction (schedule based), and the heating coil is activated. The heating coil attempts to meet the remaining load on the zone being served by the unit ventilator.
+
+\textbf{Heating /With Coil/FixedAmount:} The unit is on, there is a heating load, a heating coil is present and is scheduled on, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. The heating coil then attempts to meet any remaining zone heating load.
+
+\textbf{Cooling/No Coil/VariablePercent:} The unit is on, there is a cooling load, no coil is present or it has been scheduled off, and variable percent outdoor air control type has been specified. In this case, the variable percent outdoor air controls what happens with the outdoor air. If the outside temperature is greater than the return temperature, then the outdoor air is set to the minimum as defined by the user input. If the outdoor air temperature is less than the return temperature from the zone, then the outdoor air is set to the maximum outdoor air flow rate as defined by the user. This may be somewhat simplistic in that it could result in overcooling of the space. However, since a temperature goal was not established, this is the best that can be done by the simulation. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
+
+\textbf{Cooling/No Coil/FixedTemperature:} The unit is on, there is a cooling load, no cooling coil is present or it has been scheduled off, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate in the same fashion as the variable percent outdoor air control.
+
+\textbf{Cooling/No Coil/FixedAmount:} The unit is on, there is a cooling load, no cooling coil is present or it has been scheduled off, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outside air controls.
+
+\textbf{Cooling/With Coil/VariablePercent:} The unit is on, there is a cooling load, a coil is present and is scheduled on, and variable percent outdoor air control type has been specified. In this case, the percentage of outdoor air is set to the minimum flow outdoor air flow rate. The coil then attempts to meet any remaining zone load.
+
+\textbf{Cooling/With Coil/FixedTemperature:} The unit is on, there is a cooling load, a cooling coil is present and is scheduled on, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate in the same fashion as the fixed temperature outdoor air control for the ``no coil'' conditions. The cooling coil then attempts to meet any remaining zone load.
+
+\textbf{Cooling/With Coil/FixedAmount:} The unit is on, there is a cooling load, a cooling coil is present and is scheduled on, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. The cooling coil then attempts to meet any remaining zone cooling load.
+
+Note: the unit ventilator controls are strictly temperature based and do not factor humidity into the equation (not an enthalpy economy cycle but rather a simple return air economy cycle). In addition, temperature predictions are not strict energy balances here in the control routine though in the mixing routine an energy balance is preserved.
+
+\subsubsection{Inputs}\label{inputs-2-049}
+
+\paragraph{Field: Name}\label{field-name-2-045}
+
+This field is simply the identifying name that distinguishes one particular unit ventilator from another in the input data file. Like all other names in EnergyPlus, it is assumed that this is a unique character string and that no other unit ventilators use this same name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-2-009}
+
+This field is a schedule name (ref: Schedule) that determines whether the unit ventilator is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Maximum Supply Air Flow Rate}\label{field-maximum-supply-air-flow-rate-1}
+
+This field allows the user to enter the maximum volumetric flow rate of air through the unit ventilator system in m\(^{3}\)/sec.~This parameter should be some real number greater than zero.
+
+\paragraph{Field: Outdoor Air Control Type}\label{field-outdoor-air-control-type-000}
+
+This field allows the user to control how outdoor air is used in the unit ventilator system. The unit ventilator system described by this syntax has its own outdoor air handler. The three options for outdoor air control are ``\textbf{VariablePercent}'', ``\textbf{FixedTemperature}'' and ``\textbf{FixedAmount}''. Those keys are the only allowed choices for this parameter. In general, the variable percent control will attempt to vary the amount of outdoor air between some minimum and maximum schedules of fractions (see next two fields) to best meet the current heating or cooling load. The fixed temperature control will vary the amount of outdoor air between the minimum schedule (fraction of maximum, see next field) and 100\% available outdoor air to come as close as possible to a desired mixed air temperature (see 2 fields down) that can be scheduled. The fixed amount control will fix the outdoor air flow rate as minimum outdoor air flow rate and schedule specified by the user and automatically set the maximum and minimum outside flow rate to be equal by ignoring the maximum outdoor air flow rate. More information on the controls and operation of the unit ventilator are given in the introductory section above. For cycling fan operating mode, the outdoor air mass rate is capped by the actual supply air flow rate if the former is greater than the latter; otherwise, uses the amount calculated by the outdoor air control.
+
+\paragraph{Field: Minimum Outdoor Air Flow Rate}\label{field-minimum-outdoor-air-flow-rate-002}
+
+This field allows the user to enter the minimum volumetric flow rate of outdoor air (in m\(^{3}\)/sec) that will be brought in to the unit ventilator. The actual minimum outdoor air flow rate will be this number multiplied by the schedule value from the minimum outdoor air schedule. If ``\textbf{FixedAmount}'' type is selected as the outdoor air control strategy, the outdoor air flow rate will be fixed as this field and the unit ventilator will automatically set the maximum and minimum outside flow rate to be equal by ignoring the maximum outdoor air flow rate.
+
+\paragraph{Field: Minimum Outdoor Air Schedule Name}\label{field-minimum-outdoor-air-schedule-name-002}
+
+This field contains a schedule name (ref: Schedule) that should contain values for the minimum outdoor air used by the unit ventilator system for IAQ or other reasons. Note that if the unit ventilator is scheduled off or if there is no load sensed in the zone that the system will not operate even to achieve the minimum air fraction. However, if the system is operating, it will always bring in this fraction of the minimum air flow rate (see minimum air flow rate field above). If ``FixedAmount'' type is selected as the outdoor air control strategy, the actual outdoor air flow rate will be this number multiplied by the minimum outdoor air flow rate in the field above. The unit ventilator will automatically set the maximum and minimum outdoor air schedule to be equal by ignoring the maximum outdoor air schedule.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-1-000}
+
+This field allows the user to enter the maximum volumetric flow rate of outdoor air that can be brought into the unit ventilator system in m\(^{3}\)/sec.~This parameter should be some real number greater than zero. Note that the value for this parameter may be less than the maximum air flow rate of the unit ventilator and this may affect the maximum fraction of outdoor air within the control strategy defined above. This parameter is an absolute maximum and will supercede any scheduled fraction of the unit ventilator maximum airflow rate. If ``FixedAmount'' type is selected as the outdoor air control strategy, this field will be ignored and be automatically set to be equal to the minimum outdoor air flow rate specified in the field above.
+
+\paragraph{Field: Maximum Outdoor Air Fraction or Temperature Schedule Name}\label{field-maximum-outdoor-air-fraction-or-temperature-schedule-name-000}
+
+This field can have one of two meanings depending the type of control selected in the outdoor air control type parameter above. If ``VariablePercent'' or ``FixedAmount'' was selected, then this field is a schedule name (ref: Schedule) corresponding to a maximum air fraction schedule. Furthermore, if ``FixedAmount'' type is selected as the outdoor air control strategy, this field will be ignored and be automatically set to be equal to the minimum outdoor air fraction specified in the field below. Note that this is a fraction of the maximum airflow rate field (see parameter above) for the unit ventilator. If ``FixedTemperature'' control was selected, then this field is still a schedule name (ref: Schedule), but it corresponds to a schedule of mixed air temperatures that the outdoor air control will try to attain.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-1-007}
+
+This field is a node name used to identify the node that serves as the inlet (air side) to the unit ventilator. In EnergyPlus, nodes represent points between components or at various points in the loops. In a unit ventilator, the air inlet node to the system will typically be the same node as a zone outlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-1-006}
+
+This field is a node name used to identify the node that serves as the outlet (air side) to the unit ventilator. In EnergyPlus, nodes represent points between components or at various points in the loops. In a unit ventilator, the air outlet node from the system will typically be the same node as a zone inlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
+
+\paragraph{Field: Outdoor Air Node Name}\label{field-outdoor-air-node-name-001}
+
+This field is a node name used to identify the node associated with fresh air brought into the unit ventilator from the outdoor environment. You should also have defined an OutdoorAir:Node object with the same name and assign it an optional height (above ground).
+
+\paragraph{Field: Exhaust Air Node Name}\label{field-exhaust-air-node-name-000}
+
+This field is a node name used to identify the node associated with air exhausted out of the unit ventilator to the outdoor environment. While from a simulation standpoint this name is arbitrary and not a ``necessity'', assigning a name to this node allows the user to receive output on conditions at this node to verify the correct operation of the unit ventilator.
+
+\paragraph{Field: Mixed Air Node Name}\label{field-mixed-air-node-name-001}
+
+This field is a node name used to identify the node associated with the ``mixed'' air of the unit ventilator. These conditions are post-``mixing box'' since they are the conditions of the fraction of return air combined with the outdoor air. Since this is a simple system, this can also be viewed as the conditions of the air being sent to the coils. While from a simulation standpoint this name is arbitrary and not a ``necessity'', assigning a name to this node allows the user to receive output on conditions at this node to verify the correct operation of the unit ventilator.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-1-000}
+
+This field specifies the type of supply air fan used by this unit ventilator. The supply air fan is part of the unit ventilator compound object. The only valid supply air fan types are:
+
+\begin{itemize}
+\item
+  Fan:OnOff
+\item
+  Fan:ConstantVolume
+\item
+  Fan:VariableVolume
+\end{itemize}
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-1-000}
+
+This field is the name of a fan (ref: Fan:OnOff, Fan:ConstantVolume, Fan: VariableVolume) that is part of the unit ventilator system. This name links the unit ventilator to particular fan data entered elsewhere in the input data file. A fan name is required since it is the prime mover of air in the unit ventilator system.
+
+\paragraph{Field: Coil Option}\label{field-coil-option}
+
+This field allows the user to specify the coil operating options as one of the following options: \textbf{None}, \textbf{Heating}, \textbf{Cooling} or \textbf{HeatingAndCooling}. If \textbf{None} is selected, the unit ventilator does not have any coils, and any other input will be ignored. If either \textbf{Heating} or \textbf{Cooling} is selected, only a heating or cooling coil, respectively, is present. Thus, only four more inputs will be expected. If \textbf{HeatingAndCooling} is selected, both heating and cooling coil input must be entered, and the unit ventilator will have both a heating and a cooling coil.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-1-000}
+
+This field is a schedule name (ref: Schedule) that determines the operating modes of the unit ventilator's On:Off fan. A schedule value of 0 indicates cycling fan operation (fan cycles with cooling/heating coil). A schedule value greater than 0 (usually 1 is used) indicates constant fan operation (fan runs continually regardless of the coils operation). If this input field is left blank, then the operating mode of the On:Off fan type defaults to cycling operation.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-1-001}
+
+This field is the type of coil that is used for heating in the unit ventilator system. It is used in conjunction with the heating coil name (see next field) to specify the heating coil present within the system. Allowable heating coil types are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-1-001}
+
+This field is the name of the heating coil that is part of the unit ventilator system. It is assumed that there is always some sort of heating coil associated with a unit ventilator system. This name links the unit ventilator to particular heating coil data entered elsewhere in the input data file.
+
+\paragraph{Field: Heating Convergence Tolerance}\label{field-heating-convergence-tolerance-1}
+
+The control tolerance for the unit heating output. This field allows the user some control over how closely the heating coil will control the air side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in supply conditions (that could in turn result in excessive iterations). Initial experience with this parameter lends to the recommendation of using 0.001 as a starting point. This field is ignored for gas and electric heating coils.
+
+The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The heating convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {{Q_{UnitVentilator,Out}} - {Q_{ZoneLoad}}} \right|}}{{{Q_{ZoneLoad}}}} \le HeatingConvergenceTolerance
+\end{equation}
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-1-001}
+
+This field is the type of coil that is used for cooling in the unit ventilator system. It is used in conjunction with the cooling coil name (see next field) to specify the cooling coil present within the system.
+
+Only the following coil types can be used:
+
+\begin{itemize}
+\item
+  Coil:Cooling:Water
+\item
+  Coil:Cooling:Water:DetailedGeometry
+\item
+  CoilSystem:Cooling:Water:HeatExchangerAssisted
+\end{itemize}
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-1-001}
+
+This field is the name of the cooling coil that is part of the unit ventilator system. This name links the unit ventilator to particular cooling coil data entered elsewhere in the input data file. Note that a cooling coil is not a required part of a unit ventilator system. If no cooling coil is present, the previous field may be followed by a semi-colon and the remaining parameters in this statement may be ignored.
+
+\paragraph{Field: Cooling Convergence Tolerance}\label{field-cooling-convergence-tolerance-1}
+
+The convergence tolerance for the unit cooling output. This field allows the user some control over how closely the cooling coil will control the air side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in supply conditions (that could in turn result in excessive iterations). Initial experience with this parameter lends to the recommendation of using 0.001 as a starting point.
+
+The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The cooling convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {{Q_{UnitVentilator,Out}} - {Q_{ZoneLoad}}} \right|}}{{{Q_{ZoneLoad}}}} \le CoolingConvergenceTolerance
+\end{equation}
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-1-000}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this unit ventilator object's fan. If the unit ventilator is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this unit ventilator object should be on or off.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name-2}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Maximum Air Flow Rate in this Unit Ventilator zone HVAC object. The scaled Maximum Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
+
+An example input for a unit ventilator, including its constituent components, is shown below.
+
+\begin{lstlisting}
+
+ZoneHVAC:UnitVentilator,
+      Zone1UnitVent,           !- Name
+      UnitVentAvailability,    !- Availability Schedule Name
+      0.84,                    !- Maximum Supply Air Flow Rate {m3/s}
+      VariablePercent,         !- Outdoor Air Control Type
+      0.168,                   !- Minimum Outdoor Air Flow Rate {m3/s}
+      UnitVentMinOA,           !- Minimum Outdoor Air Schedule Name
+      0.84,                    !- Maximum Outdoor Air Flow Rate {m3/s}
+      UnitVentMaxOA,           !- Maximum Outdoor Air Fraction or Temperature Schedule Name
+      Zone1UnitVentAirInletNode,  !- Air Inlet Node Name
+      Zone1UnitVentAirOutletNode,  !- Air Outlet Node Name
+      Zone1UnitVentOAInNode,   !- Outdoor Air Node Name
+      Zone1UnitVentExhNode,    !- Exhaust Air Node Name
+      Zone1UnitVentOAMixerOutletNode,  !- Mixed Air Node Name
+      Fan: ConstantVolume,     !- Supply Air Fan Object Type
+      Zone1UnitVentFan,        !- Fan Name
+      HeatingAndCooling,       !- Coil Option
+      Coil:Heating:Water,      !- Heating Coil Object Type
+      Zone1UnitVentHeatingCoil,!- Heating Coil Name
+      0.001,                   !- Heating Convergence Tolerance
+      Coil:Cooling:Water,      !- Cooling Coil Object Type
+      Zone1UnitVentCoolingCoil,!- Cooling Coil Name
+      0.001;                   !- Cooling Convergence Tolerance
+
+  OutdoorAir:Node,
+      Zone1UnitVentOAInNode,   !- Name
+      -1.0;                    !- Height Above Ground {m}
+
+  Fan:ConstantVolume,
+      Zone1UnitVentFan,        !- Name
+      UnitVentAvailability,    !- Availability Schedule Name
+      0.5,                     !- Fan Total Efficiency
+      75.0,                    !- Pressure Rise {Pa}
+      0.84,                    !- Maximum Flow Rate {m3/s}
+      0.9,                     !- Motor Efficiency
+      1.0,                     !- Motor In Airstream Fraction
+      Zone1UnitVentOAMixerOutletNode,  !- Fan Inlet Node Name
+      Zone1UnitVentFanOutletNode;  !- Fan Outlet Node Name
+
+  Coil:Cooling:Water,
+      Zone1UnitVentCoolingCoil,!- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      0.0010,                  !- Design Water Flow Rate {m3/s}
+      0.84,                    !- Design Air Flow Rate {m3/s}
+      6.67,                    !- Design Inlet Water Temperature {C}
+      30,                      !- Design Inlet Air Temperature {C}
+      12,                      !- Design Outlet Air Temperature {C}
+      0.013,                   !- Design Inlet Air Humidity Ratio {kgWater/kgDryAir}
+      0.008,                   !- Design Outlet Air Humidity Ratio {kgWater/kgDryAir}
+      Zone1UnitVentChWInletNode,  !- Water Inlet Node Name
+      Zone1UnitVentChWOutletNode,  !- Water Outlet Node Name
+      Zone1UnitVentFanOutletNode,  !- Air Inlet Node Name
+      Zone1UnitVentCCOutletNode,  !- Air Outlet Node Name
+      SimpleAnalysis,          !- Type of Analysis
+      CrossFlow;               !- Heat Exchanger Configuration
+
+  Coil:Heating:Water,
+      Zone1UnitVentHeatingCoil,!- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      400.,                    !- U-Factor Times Area Value {W/K}
+      0.0005,                  !- Maximum Water Flow Rate {m3/s}
+      Zone1UnitVentHWInletNode,!- Water Inlet Node Name
+      Zone1UnitVentHWOutletNode,  !- Water Outlet Node Name
+      Zone1UnitVentCCOutletNode,  !- Air Inlet Node Name
+      Zone1UnitVentAirOutletNode,  !- Air Outlet Node Name
+      UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
+      autosize,                !- Nominal Capacity {W}
+      82.2,                    !- Design Inlet Water Temperature {C}
+      16.6,                    !- Design Inlet Air Temperature {C}
+      71.1,                    !- Design Outlet Water Temperature {C}
+      32.2;                    !- Design Outlet Air Temperature {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-2-028}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Unit Ventilator Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Unit Ventilator Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Unit Ventilator Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Unit Ventilator Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Unit Ventilator Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Unit Ventilator Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Unit Ventilator Fan Electric Power{[}W{]}
+\item
+  HVAC,Sum,Zone Unit Ventilator Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone Unit Ventilator Fan Availability Status {[]}
+\item
+  HVAC,Average, Zone Unit Ventilator Fan Part Load Ratio {[]}
+\end{itemize}
+
+\paragraph{Zone Unit Ventilator Heating Rate {[}W{]}}\label{zone-unit-ventilator-heating-rate-w}
+
+This field reports the heating output rate of the unit ventilator system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the unit ventilator.
+
+\paragraph{Zone Unit Ventilator Heating Energy {[}J{]}}\label{zone-unit-ventilator-heating-energy-j}
+
+This field is the heating output of the unit ventilator system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit ventilator, and the timestep.
+
+\paragraph{Zone Unit Ventilator Total Cooling Rate {[}W{]}}\label{zone-unit-ventilator-total-cooling-rate-w}
+
+This field reports the total cooling (sensible plus latent) output rate of the unit ventilator system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the unit ventilator.
+
+\paragraph{Zone Unit Ventilator Total Cooling Energy {[}J{]}}\label{zone-unit-ventilator-total-cooling-energy-j}
+
+This field is the total cooling (sensible plus latent) output of the unit ventilator system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit ventilator, and the timestep.
+
+\paragraph{Zone Unit Ventilator Sensible Cooling Rate {[}W{]}}\label{zone-unit-ventilator-sensible-cooling-rate-w}
+
+This field reports the sensible cooling output rate of the unit ventilator system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the unit ventilator.
+
+\paragraph{Zone Unit Ventilator Sensible Cooling Energy {[}J{]}}\label{zone-unit-ventilator-sensible-cooling-energy-j}
+
+This field is the sensible cooling output of the unit ventilator system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit ventilator, and the timestep.
+
+\paragraph{Zone Unit Ventilator Fan Electric Power {[}W{]}}\label{zone-unit-ventilator-fan-electric-power-w}
+
+This field reports the electric power consumption rate of the fan of the unit ventilator in Watts.
+
+\paragraph{Zone Unit Ventilator Fan Electric Energy {[}J{]}}\label{zone-unit-ventilator-fan-electric-energy-j}
+
+This field reports the electric power consumed by the fan of the unit ventilator over the timestep in Joules.
+
+\paragraph{\texorpdfstring{Zone Unit Ventilator Fan Availability Status {[]}}{Zone Unit Ventilator Fan Availability Status }}\label{zone-unit-ventilator-fan-availability-status}
+
+This is the availability status of the unit ventilator fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the unit ventilator~ object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\paragraph{\texorpdfstring{Zone Unit Ventilator Fan Part Load Ratio {[]}}{Zone Unit Ventilator Fan Part Load Ratio }}\label{zone-unit-ventilator-fan-part-load-ratio}
+
+This is the fan's part load ratio for the report timestep during which the fan had operated. This variable is available for OnOff supply air fan type only.
+
+\subsection{ZoneHVAC:UnitHeater}\label{zonehvacunitheater}
+
+Unit heaters are zone equipment units which are assembled from other components and are a simplification of unit ventilators. They contain only a fan and a heating coil. These components are described elsewhere in this document. The unit heater input simply requires the names of these components, which have to be described elsewhere in the input. The input also requires the name of an availability schedule, maximum airflow rate, and maximum and minimum hot water volumetric flow rates. The unit is connected to the zone inlet and exhaust nodes by specifying unit inlet and outlet node names. Note that the unit air inlet node should be the same as a zone exhaust node and the unit outlet node should be the same as a zone inlet node.
+
+While the control of the heating coil is similar to the fan coil units and the unit ventilator, the overall control of the unit heater is much different. There are four different modes in which a unit heat can operate based on the user input:
+
+\textbf{Off:} Unit is schedule off. All flow rates are set to zero and the temperatures are set to zone conditions.
+
+\textbf{NoLoad OR Cooling/''No''} is specified in input field ``Supply Air Fan Operation During No Heating''\textbf{:} Unit is available, but there is no heating load. With ``No'' specified for ``Supply Air Fan Operation During No Heating'' and the supply fan operating mode set to 0, the fan will be off since there is no heating load. All flow rates are set to zero and the temperatures are set to zone conditions.
+
+\textbf{NoLoad OR Cooling/''Yes''} is specified in input field ``Supply Air Fan Operation During No Heating''\textbf{:} Unit is available, the supply fan operating mode schedule value is greater than 0 (for OnOff Fan) and the fan is running (if it is scheduled to be available also). No heating is provided, only air circulation via the fan running. However, any heat added by the fan is introduced into the space with the circulation of the air.
+
+\textbf{Heating:} The unit is on/available and there is a heating load. The heating coil is modulated (constant fan speed) to meet the heating load. When the fan type is not an OnOff fan then the~ control of the heating coil and its flow rate is identical to the fan coil unit. In the case of OnOff fan, the fan cycles with heating coil if the current timestep supply fan operating mode is schedule value is 0, or else if the current timestep supply fan operating mode schedule value is greater than 0, then the supply fan runs continuously for the entire timestep.
+
+\subsubsection{Inputs}\label{inputs-3-043}
+
+\paragraph{Field: Name}\label{field-name-3-039}
+
+This field is simply the identifying name that distinguishes one particular unit heater from another in the input data file. Like all other names in EnergyPlus, it is assumed that this is a unique character string and that no other unit heaters use this same name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-3-007}
+
+This field is a schedule name (ref: Schedule) that determines whether the unit heater is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-2-003}
+
+This field is a node name used to identify the node that serves as the inlet (air side) to the unit heater. In EnergyPlus, nodes represent points between components or at various points in the loops. In a unit heater, the air inlet node to the system will typically be the same node as a zone outlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-2-003}
+
+This field is a node name used to identify the node that serves as the outlet (air side) to the unit heater. In EnergyPlus, nodes represent points between components or at various points in the loops. In a unit heater, the air outlet node from the system will typically be the same node as a zone inlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-2-000}
+
+This field specifies the type of supply air fan used by this unit heater. The supply air fan is part of the unit heater compound object. The only valid supply air fan types are:
+
+\begin{itemize}
+\item
+  Fan:OnOff
+\item
+  Fan:ConstantVolume
+\item
+  Fan:VariableVolume
+\end{itemize}
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-2-000}
+
+This field is the name of a fan (ref: Fan:ConstantVolume, Fan:VariableVolume) that is part of the unit heater system. This name links the unit heater to particular fan data entered elsewhere in the input data file. A fan name is required since it is the prime mover of air in the unit heater system.
+
+\paragraph{Field: Maximum Supply Air Flow Rate}\label{field-maximum-supply-air-flow-rate-2}
+
+This field allows the user to enter the maximum volumetric flow rate of air through the unit heater system in m\(^{3}\)/s. This parameter should be some real number greater than zero.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-2-000}
+
+This field is the type of coil that is used for heating in the unit heater system. It is used in conjunction with the heating coil name (see next field) to specify the heating coil present within the system. Allowable heating coil types are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-2-000}
+
+This field is the name of the heating coil that is part of the unit heater system. It is assumed that there is always some sort of heating coil associated with a unit heater system. This name links the unit ventilator to particular heating coil data entered elsewhere in the input data file.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-2-000}
+
+This field is a schedule name (ref: Schedule) that determines the operating modes of the unit heater's On:Off fan. A schedule value of 0 indicates cycling fan operation (fan cycles with cooling/heating coil). A schedule value greater than 0 (usually 1 is used) indicates constant fan operation (fan runs continually regardless of the coils operation). If this input field is left blank, then the operating mode of the On:Off fan type defaults to cycling operation.
+
+\paragraph{Field: Supply Air Fan Operation During No Heating}\label{field-supply-air-fan-operation-during-no-heating}
+
+This choice field allows the user to define how the unit heater will operate under ``no heating load'' or cooling conditions. The user may select from two options (``Yes'', ``No''). If the ``\textbf{No}'' control is selected, then the fan will not run unless there is a heating load. If the fan does not run, this effectively shuts the unit heater system off. If the ``\textbf{Yes}'' control is selected, the unit heater is available, and the fan is continuous, then the fan will always run. This will produce air movement in the zone but also add some amount of heat to the energy balance since the fan generates some heat. But if the ``\textbf{Yes}'' control is selected and the ``Supply Air Fan Operating Mode Schedule'' values is 0 (for OnOff fan), then the fan will NOT run.~ This allows the user to schedule the operation of the fan when there is no load.
+
+\paragraph{Field: Maximum Hot Water or Steam Flow Rate}\label{field-maximum-hot-water-or-steam-flow-rate-000}
+
+This field allows the user to enter a maximum hot water or steam volumetric flow rate through the heating coil in m\(^{3}\)/s. The steam volume flow rate is calculated at 100C and 101325 Pa. This number should be some number greater than zero and greater than the minimum hot water or steam volumetric flow rate (see next field). Note that this parameter has no meaning for either an electric or a gas heating coil.
+
+\paragraph{Field: Minimum Hot Water or Steam Flow Rate}\label{field-minimum-hot-water-or-steam-flow-rate-000}
+
+This field allows the user to enter a minimum hot water or steam volumetric flow rate through the heating coil in m\(^{3}\)/s. The steam volume flow rate is calculated at 100C and 101325 Pa. This number should be some number greater than zero and less than the maximum hot water or steam volumetric flow rate (see previous field). Note that this parameter has no meaning for either an electric or a gas heating coil.
+
+\paragraph{Field: Heating Convergence Tolerance}\label{field-heating-convergence-tolerance-2}
+
+The convergence tolerance for the unit heating output. This field allows the user some control over how closely the heating coil will control the air side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in supply conditions (that could in turn result in excessive iterations). Initial experience with this parameter lends to the recommendation of using 0.001 as a starting point. This field is ignored for gas and electric heating coils.
+
+The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The heating convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
+
+\begin{equation}
+\frac{{\left| {{Q_{unit{\kern 1pt} heater,out}} - {Q_{zoneload}}} \right|}}{{{Q_{zoneload}}}} \le HeatingConvergenceTolerance
+\end{equation}
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-2}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this unit heater object's fan. If the unit heater is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this unit heater object should be on or off.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name-3}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields \emph{Maximum Supply Air Flow Rate} in this Unit Heater zone HVAC object. The scaled maximum supply air flow rates is used to size Maximum Hot Water or Steam Flow Rate if specified as autosize. The scaled Maximum Air Flow Rate in turn is used to size heating capacity of the unit.
+
+An example input for a unit heater, including its constituent components, is shown below.
+
+\begin{lstlisting}
+
+ZoneHVAC:UnitHeater,
+      Zone1UnitHeat,           !- Name
+      UnitHeatAvailability,    !- Availability Schedule Name
+      Zone1UnitHeatAirInletNode,  !- Air Inlet Node Name
+      Zone1UnitHeatAirOutletNode,  !- Air Outlet Node Name
+      Fan: ConstantVolume,     !- Supply Air Fan Object Type
+      Zone1UnitHeatFan,        !- Fan Name
+      0.84,                    !- Maximum Supply Air Flow Rate {m3/s}
+      Continuous,              !- Fan Control Type
+      Coil:Heating:Water,      !- Heating Coil Object Type
+      Zone1UnitHeatHeatingCoil,!- Heating Coil Name
+      0.0005,                  !- Maximum Hot Water or Steam Flow Rate {m3/s}
+      0.0,                     !- Minimum Hot Water or Steam Flow Rate {m3/s}
+      0.001;                   !- Heating Convergence Tolerance
+
+
+  Fan:ConstantVolume,
+      Zone1UnitHeatFan,        !- Name
+      UnitHeatAvailability,    !- Availability Schedule Name
+      0.5,                     !- Fan Total Efficiency
+      75.0,                    !- Pressure Rise {Pa}
+      0.84,                    !- Maximum Flow Rate {m3/s}
+      0.9,                     !- Motor Efficiency
+      1.0,                     !- Motor In Airstream Fraction
+      Zone1UnitHeatAirInletNode,  !- Fan Inlet Node Name
+      Zone1UnitHeatFanOutletNode;  !- Fan Outlet Node Name
+
+
+  Coil:Heating:Water,
+      Zone1UnitHeatHeatingCoil,!- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      400.,                    !- U-Factor Times Area Value {W/K}
+      0.0005,                  !- Maximum Water Flow Rate {m3/s}
+      Zone1UnitHeatHWInletNode,!- Water Inlet Node Name
+      Zone1UnitHeatHWOutletNode,  !- Water Outlet Node Name
+      Zone1UnitHeatFanOutletNode,  !- Air Inlet Node Name
+      Zone1UnitHeatAirOutletNode,  !- Air Outlet Node Name
+      UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
+      autosize,                !- Nominal Capacity {W}
+      82.2,                    !- Design Inlet Water Temperature {C}
+      16.6,                    !- Design Inlet Air Temperature {C}
+      71.1,                    !- Design Outlet Water Temperature {C}
+      32.2;                    !- Design Outlet Air Temperature {C}
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-3-025}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Unit Heater Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Unit Heater Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Unit Heater Fan Electric Power{[}W{]}
+\item
+  HVAC,Sum,Zone Unit Heater Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average, Zone Unit Heater Fan Availability Status {[]}
+\item
+  HVAC,Average, Zone Unit Heater Fan Part Load Ratio {[]}
+\end{itemize}
+
+\paragraph{Zone Unit Heater Heating Rate {[}W{]}}\label{zone-unit-heater-heating-rate-w}
+
+This field reports the heating output rate of the unit heater system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the unit heater.
+
+\paragraph{Zone Unit Heater Heating Energy {[}J{]}}\label{zone-unit-heater-heating-energy-j}
+
+This field is the heating output of the unit heater system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit heater, and the timestep.
+
+\paragraph{Zone Unit Heater Fan Electric Power {[}W{]}}\label{zone-unit-heater-fan-electric-power-w}
+
+This field reports the electric power consumption rate of the fan of the unit heater in Watts.
+
+\paragraph{Zone Unit Heater Fan Electric Energy {[}J{]}}\label{zone-unit-heater-fan-electric-energy-j}
+
+This field reports the electric power consumed by the fan of the unit heater over the timestep in Joules.
+
+\paragraph{\texorpdfstring{Zone Unit Heater Fan Availability Status {[]}}{Zone Unit Heater Fan Availability Status }}\label{zone-unit-heater-fan-availability-status}
+
+This is the availability status of the unit heater fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the unit heater~ object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\paragraph{\texorpdfstring{Zone Unit Heater Fan Part Load Ratio {[]}}{Zone Unit Heater Fan Part Load Ratio }}\label{zone-unit-heater-fan-part-load-ratio}
+
+This is the fan's part load ratio for the report timestep during which the fan had operated. This variable is available for OnOff supply air fan type only.
+
+\subsection{ZoneHVAC:EvaporativeCoolerUnit}\label{zonehvacevaporativecoolerunit}
+
+The zone evaporative cooler unit is a compound object made up of a fan and one or two evaporative cooler components.~ This unit serves a single thermal zone as a forced-convection, cooling-only unit with supply fan.~ It always draws 100\% of its supply air from the outside, passes the air through a supply fan and evaporative cooler(s) and then into the zone.~ The fan can be positioned upstream of the cooler(s) for a blow through placement.~ Or it can be positioned downstream of the cooler(s) for a draw through placement.~ If there is more than one evaporative cooler, then should be in series with the first cooler immediately upstream of the second cooler. There is an option to include a relief zone exhaust node to balance the air in the zone.
+
+The unit can have either constant or variable speed fans.~ This zone unit differs from other constant speed forced-air zone units in that its controls are not based on a part-load formulation with averaged air flow rates. Instead the unit is completely on or off during the entire timestep.~ This means that it is beneficial to use relatively short timesteps. However for variable speed fans, the unit can modulate fan speed to just meet cooling loads and therefore operates similar to other zone HVAC units.
+
+\subsubsection{Inputs}\label{inputs-4-040}
+
+\paragraph{Field: Name}\label{field-name-4-035}
+
+This alpha field defines a unique user-assigned name for an instance of a zone evaporative cooler unit.~ References to this unit by other objects will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-4-007}
+
+This alpha field defines the name of a schedule that denotes whether the unit operates during a given time period. A schedule value equal to 0.0 denotes that the cooler unit must be off for that time period. A schedule value greater than 0.0 denotes that the cooler is available to operate during that time period. If this field is left blank, then the program assumes that the unit is always available as if the schedule was always set to 1.0.
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-3}
+
+This optional alpha input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name.~ The availability managers in the list apply to this evaporative cooler unit's operation. If this field is used and the cooler unit is scheduled to be available, based on the previous input field, then the unit will operate based on the result of the availability managers in the list.
+
+\paragraph{Field: Outdoor Air Inlet Node Name}\label{field-outdoor-air-inlet-node-name-1-000}
+
+This alpha input field defines the name of the HVAC system node from which the evaporative cooler unit draws its supply air.~ This node is usually declared to be an outdoor air node using OutdoorAir:Node or OutdoorAir:NodeList.
+
+\paragraph{Field: Cooler Outlet Node Name}\label{field-cooler-outlet-node-name}
+
+This alpha input field defines the name of the HVAC system node to which the evaporative cooler sends its outlet air.~ This node name must be the name of a zone air inlet node (Ref. ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Zone Relief Air Node Name}\label{field-zone-relief-air-node-name}
+
+This optional alpha input field defines the name of an HVAC system node which can extract air from the zone to balance the air supplied to the zone by the cooler outlet node.~ This node name would match the name of a zone exhaust air node.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-3-000}
+
+This alpha input field defines the type of fan used by the zone evaporative cooler unit.~ There are four valid choices: Fan:ConstantVolume, Fan:OnOff, Fan:VariableVolume, or Fan:ComponentModel.~ However the type of fan must be consistent with the control method defined below and a variable speed fan is needed with ZoneCoolingLoadVariableSpeedFan.
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-3-000}
+
+This alpha input field defines the user-defined name of the fan used by this cooler unit. The fan itself is defined elsewhere.~ Note that the fan's maximum flow rate should be greater than or equal to the Design Supply Air Flow Rate defined in the following field.~ For a blow-through fan placement, the fan's inlet node should be the same as the Outlet Air Inlet Node Name. For a draw-through fan placement, the fan's outlet node should be the same as the Cooler Outlet Node Name.
+
+\paragraph{\texorpdfstring{Field: Design Supply Air Flow Rate {[}m\(^{3}\)/s{]}}{Field: Design Supply Air Flow Rate {[}m\^{}\{3\}/s{]}}}\label{field-design-supply-air-flow-rate-m3s}
+
+This numeric input field defines the evaporative cooler unit's design supply air flow rate, in cubic meters per second.~ This value is typically consistent with the maximum air flow rate of the fan, but it can be less if desired.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-001}
+
+This alpha input field defines how the supply fan is arranged.~ There are two choices, BlowThrough or DrawThrough.~ The BlowThrough choice indicates that the fan is located upstream of the evaporative cooler(s). The DrawThrough choice indicates that the fan is located downstream of the evaporative cooler(s). These are the only configurations that are available and the HVAC system nodes used as inlets and outlet in the components must be arranged consistent with the flow path.
+
+\paragraph{Field: Cooler Unit Control Method}\label{field-cooler-unit-control-method}
+
+This alpha field is used to determine how the unit is to be controlled.~ There are three possible choices:
+
+\begin{itemize}
+\item
+  \textbf{ZoneTemperatureDeadbandOnOffCycling}. This control method determines whether or not to operate the cooler based on the thermostat setpoint and the zone air temperature.~ This thermostatic control method uses a throttling temperature range, determined in the following input field, to model hysteresis-type control to avoid excessive short-cycling.~ If the zone air temperature is warmer than the cooling setpoint temperature plus one-half of the throttling range, then the unit is operated for the entire timestep at the design air mass flow rate.~ If the zone air temperature is cooler than the cooling setpoint temperature minus one-half of the throttling range, then the unit is off for the entire timestep.~ When the zone air temperatures are within the throttling range, then the unit will stay off if it was not running during the previous timestep and will stay on if it was already running. This control method does not usually behave in a smooth manner and zone conditions will tend to oscillate considerably during periods of low load.
+\item
+  \textbf{ZoneCoolingLoadOnOffCycling}. This control method determines whether or not to operate the cooler based on the predicted zone load to cooling setpoint.~ If there is a cooling load (and the unit is available), then the unit is operated for the entire timestep at the design air mass flow rate. If there is no cooling load, then the unit is not operated at all.~ The magnitude of the cooling load that will trigger the unit to operate can be controlled using the field below called Cooling Load Control Threshold Heat Transfer Rate. This control method does not usually behave in a smooth manner and zone conditions will tend to oscillate considerably during periods of low load.
+\item
+  \textbf{ZoneCoolingLoadVariableSpeedFan}.~ This control method determines whether or not to operate the cooler based on the predicted zone load to cooling setpoint.~ If there is a cooling load (and the unit is available), then the unit is operated for the entire timestep at a fan speed that is controlled to meet the sensible cooling load (if possible). The magnitude of the cooling load that will trigger the unit to operate can be controlled using the field below called Cooling Load Control Threshold Heat Transfer Rate.~ This control method requires a variable speed fan and cannot be used with Fan:ConstantVolume or Fan:OnOff.
+\end{itemize}
+
+\paragraph{Field: Throttling Range Temperature Difference {[}DeltaC{]}}\label{field-throttling-range-temperature-difference-deltac}
+
+This numeric input field defines the throttling range to use for zone-temperature based control, in degrees Celsius. This value is used when the unit's control method is ZoneTemperatureDeadbandOnOffCycling.~ This temperature range is used for hysteresis thermostatic control.~ It is modeled as symmetric about the cooling setpoint. The default is 1.0°C.
+
+\paragraph{Field: Cooling Load Control Threshold Heat Transfer Rate {[}W{]}}\label{field-cooling-load-control-threshold-heat-transfer-rate-w}
+
+This numeric input field defines the magnitude, in Watts, of a significant zone cooling load to use with zone-load-to-setpoint based control.~ This value is used when the unit's control method is ZoneCoolingLoadOnOffCycling or ZoneCoolingLoadVariableSpeedFan.~ This is a sensible cooling load that is used as a threshold to determine when the cooling load is significant.~ When the predicted zone load to cooling setpoint is less than this threshold, the cooler unit's control will consider the load to be too small to trigger operation. The default is 100W.
+
+\paragraph{Field: First Evaporative Cooler Object Type}\label{field-first-evaporative-cooler-object-type}
+
+This alpha input field defines the type of evaporative cooler used in the unit. The zone evaporative cooler unit can have one or two separate cooler components and this field is for the first cooler. There are five types of evaporative cooler component models to choose from: EvaporativeCooler:Direct:CelDekPad, EvaporativeCooler:Direct:ResearchSpecial, EvaporativeCooler:Indirect:CelDekPad, EvaporativeCooler:Indirect:WetCoil, or EvaporativeCooler:Indirect:ResearchSpecial.
+
+\paragraph{Field: First Evaporative Cooler Object Name}\label{field-first-evaporative-cooler-object-name}
+
+This alpha input field defines the user-defined name of the first evaporative cooler component used by this zone unit.~ The cooler component itself is defined elsewhere. For a blow through fan placement, the inlet node for the evaporative cooler should be the same as the fan's outlet node.~ For a draw through fan placement, the inlet node for the evaporative cooler should be the same as the unit's Outdoor Air Inlet Node Name.
+
+\paragraph{Field: Second Evaporative Cooler Object Type}\label{field-second-evaporative-cooler-object-type}
+
+This optional alpha input field defines the type of evaporative cooler used in the unit. This field is used when the zone evaporative cooler unit has two separate evaporative cooler sections arranged in series. For example, some coolers are arranged with both direct and indirect evaporative coolers. If the unit has only one type of cooler, this field should be left blank. There are five types of evaporative cooler component models to choose from: EvaporativeCooler:Direct:CelDekPad, EvaporativeCooler:Direct:ResearchSpecial, EvaporativeCooler:Indirect:CelDekPad, EvaporativeCooler:Indirect:WetCoil, or EvaporativeCooler:Indirect:ResearchSpecial
+
+\paragraph{Field: Second Evaporative Cooler Name}\label{field-second-evaporative-cooler-name}
+
+This optional alpha input field defines the user-defined name of the second evaporative cooler component used by this zone unit.~ The cooler component itself is defined elsewhere. The inlet node for the second evaporative cooler should be the same as the outlet node for the first evaporative cooler.~ For a draw through fan placement, the outlet node for the second evaporative cooler should be the same as the unit's fan inlet node.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name-4}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object defined elsewhere. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input field \emph{Design Supply Air Flow Rate} in Evaportaive Cooler zone HVAC object. The scaled design supply air flow rates in turn is used to size capacity of the unit.
+
+An example input object follows.
+
+\begin{lstlisting}
+
+ZoneHVAC:EvaporativeCoolerUnit,
+     Zone Evap Unit, !- Name
+     System Availability Schedule , !- Availability Schedule Name
+     , !- Availability Manager List Name
+     Cooler Unit OA inlet , !- Outdoor Air Inlet Node Name
+     Main Zone Inlet Node, !- Cooler Outlet Node Name
+     Main Zone Relief Node , !- Zone Relief Air Node Name
+     Fan:ConstantVolume , !- Supply Air Fan Object Type
+     Supply Fan , !- Supply Air Fan Name
+     2.0, !- Design Supply Air Flow Rate
+     DrawThrough , !- Fan Placement
+     ZoneCoolingLoadOnOffCycling, !- Cooler Unit Control Method
+     1.1, !- Throttling Range Temperature Difference
+     100.0, !- Cooling Load Control Threshold Heat Transfer Rate
+     EvaporativeCooler:Direct:CelDekPad, !- First Evaporative Cooler Object Type
+     Evaporative Cooler, !- First Evaporative Cooler Object Name
+     , !- Second Evaporative Cooler Object Type
+     ; !- Second Evaporative Cooler Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-4-021}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Evaporative Cooler Unit Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Evaporative Cooler Unit Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Evaporative Cooler Unit Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Evaporative Cooler Unit Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Evaporative Cooler Unit Latent Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Evaporative Cooler Unit Latent Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Evaporative Cooler Unit Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Evaporative Cooler Unit Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Evaporative Cooler Unit Fan Speed Ratio {[]}
+\item
+  HVAC,Average,Zone Evaporative Cooler Unit Fan Availability Status {[]}
+\end{itemize}
+
+\paragraph{Zone Evaporative Cooler Unit Total Cooling Rate {[}W{]}}\label{zone-evaporative-cooler-unit-total-cooling-rate-w}
+
+This output is the total (enthalpy) heat extraction rate of the zone evaporative cooler unit from the zone it is serving, in Watts.~ This value is calculated using the enthalpy difference of the unit outlet air node and the zone air node and the air mass flow rate entering the zone.
+
+\paragraph{Zone Evaporative Cooler Unit Total Cooling Energy {[}J{]}}\label{zone-evaporative-cooler-unit-total-cooling-energy-j}
+
+This output is the total (enthalpy) heat extraction of the zone evaporative cooler unit from the zone it is serving, in Joules.~ This value is calculated using the enthalpy difference of the unit outlet air node and the zone air node and the air mass flow rate entering the zone.
+
+\paragraph{Zone Evaporative Cooler Unit Sensible Cooling Rate {[}W{]}}\label{zone-evaporative-cooler-unit-sensible-cooling-rate-w}
+
+This output is the moist air sensible-only heat extraction rate of the zone evaporative cooler unit from the zone it is serving, in Watts. This value is calculated using the enthalpy difference of the unit outlet air node and the zone air node based on a single, minimum humidity ratio along with the air mass flow rate entering the zone.
+
+\paragraph{Zone Evaporative Cooler Unit Sensible Cooling Energy {[}J{]}}\label{zone-evaporative-cooler-unit-sensible-cooling-energy-j}
+
+This output is the moist air sensible-only heat extraction of the zone evaporative cooler unit from the zone it is serving, in Joules. This value is calculated using the enthalpy difference of the unit outlet air node and the zone air node based on a single, minimum humidity ratio along with the air mass flow rate entering the zone.
+
+\paragraph{Zone Evaporative Cooler Unit Latent Heating Rate {[}W{]}}\label{zone-evaporative-cooler-unit-latent-heating-rate-w}
+
+This output is the latent heat addition (humidification) rate of the zone evaporative cooler unit to the zone it is serving in Watts.~ This value is calculated as the difference between the total cooling rate and the sensible cooling rate.~ Because an evaporative cooler can provide sensible cooling while adding moisture the zone air, a unit can operate with both a positive sensible cooling load and a positive latent heating rate.
+
+\paragraph{Zone Evaporative Cooler Unit Latent Heating Energy {[}J{]}}\label{zone-evaporative-cooler-unit-latent-heating-energy-j}
+
+This output is the latent heat addition (humidification) of the zone evaporative cooler unit to the zone it is serving in Joules.~ This value is calculated as the difference between the total cooling energy and the sensible cooling energy.
+
+\paragraph{Zone Evaporative Cooler Unit Latent Cooling Rate {[}W{]}}\label{zone-evaporative-cooler-unit-latent-cooling-rate-w}
+
+This output is the latent heat extraction (dehumidification) rate of the zone evaporative cooler unit to the zone it is serving in Watts.~ This value is calculated as the difference between the total cooling rate and the sensible cooling rate.
+
+\paragraph{Zone Evaporative Cooler Unit Latent Cooling Energy {[}J{]}}\label{zone-evaporative-cooler-unit-latent-cooling-energy-j}
+
+This output is the latent heat extraction (dehumidification) of the zone evaporative cooler unit to the zone it is serving in Joules.~ This value is calculated as the difference between the total cooling energy and the sensible cooling energy.
+
+\paragraph{\texorpdfstring{Zone Evaporative Cooler Unit Fan Speed Ratio {[]}}{Zone Evaporative Cooler Unit Fan Speed Ratio }}\label{zone-evaporative-cooler-unit-fan-speed-ratio}
+
+This output is the speed ratio of the fan for the zone evaporative cooler unit.~ The speed ratio is defined as the current supply air mass flow rate divided by the design air mass flow rate.
+
+\paragraph{\texorpdfstring{Zone Evaporative Cooler Unit Fan Availability Status {[]}}{Zone Evaporative Cooler Unit Fan Availability Status }}\label{zone-evaporative-cooler-unit-fan-availability-status}
+
+This output is the availability status of the zone evaporative cooler unit's fan.~ This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object.~ The AvailabilityManagerAssignmentList is an optional input in the zone evaporative cooler object.~ When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific manager.~ For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager)), rules to determine fan availability status are described in the section on system availability managers.~ The control status outputs are represented using integers 0 through 3.~ These integers represent NoAction (0), ForceOff (1), CycleOn(2), and CycleOneZoneFansOnly (3).~ It is recommend to report this output at the ``Detailed'' frequency because the integer status flags do not average out to meaningful values.
+
+\subsection{ZoneHVAC:OutdoorAirUnit}\label{zonehvacoutdoorairunit}
+
+The zone outdoor air unit (ZoneHVAC:OutdoorAirUnit) in EnergyPlus is intended to model dedicated outdoor air systems (DOAS) and other similar systems which aim to provide either additional outside air or some limited amount of sensible and/or latent conditioning.~ The zone outdoor air unit is a piece of zone equipment that can consist of a supply fan, an exhaust fan (optional), heating and cooling coils, and heat recovery.~ The outdoor air unit input simply requires information about flow rates, schedules, node names, and a list of component that are part of the unit.~ These components require additional input as per the requirements for these components.~ In addition, the input includes information about controls for the unit.~ It should be noted that the components that make up the zone outdoor air unit do not require additional controls or setpoints.~ The unit input defines how the unit outlet temperature is controlled as described below.
+
+\begin{figure}[hbtp] % fig 110
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image282.png}
+\caption{Zone Outdoor Air Unit Schematic \protect \label{fig:zone-outdoor-air-unit-schematic}}
+\end{figure}
+
+Zones may contain one or more zone outdoor air units.~ The user can choose to have each unit have its own exhaust fan or may choose to have only one unit have a exhaust fan that will handle the flow of all of the zone outdoor air units.~ Note that the user will need to account for any flow balance among the zone outdoor air units on the supply and exhaust sides.
+
+The full input for zone outdoor air units is described below using a variety of fields.
+
+\subsubsection{Inputs}\label{inputs-5-035}
+
+\paragraph{Field: Name}\label{field-name-5-029}
+
+This field is simply the identifying name that distinguishes one particular outdoor air unit from another in the input data file. Like all other names in EnergyPlus, it is assumed that this is a unique character string and that no other zone outdoor air units use this same name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-5-005}
+
+This field is a schedule name (ref: Schedule) that determines whether the zone outdoor air unit is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the outdoor air unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the outdoor air unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods. For any schedule value greater than zero, the outdoor air unit is considered available and will operate at the supply and exhaust flow rates defined by input field described below.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-016}
+
+This field is the name of the zone (Ref: Zone) in which the outdoor air unit is located and intended to affect.~ Zone outdoor air units impact only a single zone.
+
+\paragraph{Field: Outdoor Air Flow Rate}\label{field-outdoor-air-flow-rate}
+
+This field allows the user to enter the volumetric flow rate of outdoor air (in m\(^{3}\)/sec) that will be brought in through the outdoor air unit. The actual outdoor air flow rate will be this number multiplied by the schedule value from the outdoor air schedule. This field is autosizable.~ When autosized, the unit's outdoor air flow rate will match the minimum outdoor air requirements specified through the Sizing:Zone object.
+
+\paragraph{Field: Outdoor Air Schedule Name}\label{field-outdoor-air-schedule-name-1}
+
+This field contains a schedule name (ref: Schedule) that contains values for modifying the outdoor air flow rate.~ The supply air flow rate is the product of the outdoor air flow rate and the outdoor air schedule value for the time of interest. ~Note that if the outdoor air unit is scheduled off that the system will not operate regardless of the outdoor air schedule value. However, if the system is operating, it will always bring in this fraction of the outdoor air flow rate.
+
+\paragraph{Field: Supply Fan Name}\label{field-supply-fan-name-000}
+
+This field is the name of a fan (ref: Fan:ConstantVolume, Fan: VariableVolume) that is part of the zone outdoor air unit. This name links the outdoor air unit to particular fan data entered elsewhere in the input data file. A fan name is required since it is the prime mover of air in the outdoor air control unit.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-1-001}
+
+This field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice stands for ``blow through fan''. It means that the unit consists of outdoor air node followed by a supply fan followed by the equipment that are part of the system. The second choice stands for ``draw through fan''. It means that the supply fan placed at the end of supply air stream and supply fan outlet node is identified with the air outlet node. The fan ``draws air through'' the equipment system.
+
+\begin{itemize}
+\item
+  BlowThrough
+\item
+  DrawThrough
+\end{itemize}
+
+If the user does not select a fan placement type, \textbf{DrawThrough} is assumed as default by EnergyPlus.
+
+\paragraph{Field: Exhaust Fan Name}\label{field-exhaust-fan-name}
+
+This field is the name of a fan (ref: Fan:ConstantVolume, Fan: VariableVolume) that is part of the outdoor air unit. This name links the outdoor air unit to particular fan data entered elsewhere in the input data file. This field is optional.
+
+\paragraph{Field: Exhaust Air Flow Rate}\label{field-exhaust-air-flow-rate}
+
+This field allows the user to enter the volumetric flow rate of air (in m\(^{3}\)/sec) that will be exhausted to the outdoors. The actual exhaust air flow rate will be this number multiplied by the schedule value from the exhaust air schedule. If the exhaust fan name is left blank, this field will be ignored and automatically set to be equal to zero.
+
+\paragraph{Field: Exhaust Air Schedule Name}\label{field-exhaust-air-schedule-name}
+
+This field contains a schedule name (ref: Schedule) that should contain values for modifying the exhaust air flow rate.~ The actual exhaust air flow rate equals the exhaust air flow rate input (previous field) multiplied by the exhaust air schedule value. If the exhaust fan name is left blank, this field will be ignored and automatically set to be equal to zero.
+
+\paragraph{Field: Unit Control Type}\label{field-unit-control-type}
+
+The unit control type field determines with conditions in the zone being served what the response of the zone outdoor air system will be. It is important to note that this only controls the temperature of the air being delivered to the space not whether or not the system will operate.~ There are two options for this field: Neutral or Temperature. Neutral control tries to have no energy impact on the zone by delivering air at the temperature of the zone. This allows air to be delivered to the zone without affecting the zone air heat balance and thus provides outside air without impacting any other system providing conditioning to this zone. The temperature control option will supply air to the zone based on the high and low air control temperature schedules (see next two fields). For temperature control, when the outside air temperature is less than the low air control temperature, the zone outdoor air unit will provide whatever heating is available from its components to achieve the low air temperature value.~ When the outside air temperature is above the high air control temperature, the zone outdoor air unit will provide whatever cooling is available from its components to achieve the high air temperature value.~ When the outdoor air temperature is between the high and low air control temperatures, the unit will simply provide air at whatever the outdoor air conditions are, modified by any fan heat added by the supply fan. In summary, the user must select from the following two options:
+
+\begin{itemize}
+\item
+  NeutralControl
+\item
+  TemperatureControl
+\end{itemize}
+
+If the user does not select a unit control type, \textbf{NeutralControl} is assumed as the default by EnergyPlus.
+
+\paragraph{Field: High Air Control Temperature Schedule Name}\label{field-high-air-control-temperature-schedule-name}
+
+This field specifies the dry-bulb air temperature in degrees Celsius for the supply air temperature to the zone. When the outdoor air temperature or post-supply fan outlet temperature in the case of blow through is above the high air control temperature, a cooling coil, if available and specified by the user, is tuned on to conditioning the outdoor air to the high control temperature. This field only applies to zone outdoor air units that use Temperature Control (see previous field).
+
+\paragraph{Field: Low Air Control Temperature Schedule Name}\label{field-low-air-control-temperature-schedule-name}
+
+This field specifies the dry-bulb air temperature in degrees Celsius for the supply air temperature to the zone. When the outdoor air temperature or post-supply fan outlet temperature is below the low air control temperature, a heating coil, if available and specified by the user, is tuned on to conditioning the outdoor air to the low control temperature. This field only applies to zone outdoor air units that use Temperature Control (see two previous fields).
+
+\paragraph{Field: Outdoor Air Node Name}\label{field-outdoor-air-node-name-1-000}
+
+This field is a node name used to identify the node associated with fresh air brought into the outdoor air unit from the outdoor environment. It should also be defined in an OutdoorAir:Node object with the same name and assigned an optional height (above ground).
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-3-003}
+
+This field is a node name used to identify the node that serves as the outlet (air side) from the zone outdoor air unit. In EnergyPlus, nodes represent points between components or at various points in the loops. In an outdoor air unit, the air outlet node from the system will typically be the same node as a zone inlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-3-003}
+
+This field is a node name used to identify the node that serves as the inlet (air side) to the exhaust side of the outdoor air unit. In EnergyPlus, nodes represent points between components or at various points in the loops. In an outdoor air unit, the air inlet node of the system will typically be the same node as a zone outlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
+
+\paragraph{Field: Supply Fan Outlet Node Name}\label{field-supply-fan-outlet-node-name}
+
+This field is a node name used to identify the node that serves as the outlet (air side) of the supply fan for the zone outdoor air unit. In EnergyPlus, nodes represent points between components or at various points in the loops. While a node name may be referenced more than once in an input data file, each node must have a unique name.
+
+\paragraph{Field: Outdoor Air Unit List Name}\label{field-outdoor-air-unit-list-name}
+
+This field is the name of an ZoneHVAC:OutdoorAirUnit:EquipmentList object. An ZoneHVAC:OutdoorAirUnit:EquipmentList ~is simply a list of components giving both component name and type. This equipment list specifies all the components that will be simulated in this unit. The order of the components in the list is significant: components are simulated sequentially in the order given in the Equipment List.
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-4}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this outdoor air unit~ object's fan. If the outdoor air unit is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this outdoor air unit~ object should be on or off.
+
+An example of this object defined in an input data file is shown below\textbf{:}
+
+\begin{lstlisting}
+
+ZoneHVAC:OutdoorAirUnit,
+      Zone5DXOutAir,           !- Name
+      OAUnitOASched,           !- Availability Schedule Name
+      SPACE5-1,                !- Zone Name
+      0.42,                    !- Outdoor Air Flow Rate {m3/s}
+      OAUnitOASched,           !- Outdoor Air Schedule Name
+      Zone5OAUFan1,            !- Supply Fan Name
+      BlowThrough,             !- Supply Fan Placement
+      ,                        !- Exhaust Fan Name
+      ,                        !- Exhaust Air Flow Rate {m3/s}
+      ,                        !- Exhaust Air Schedule Name
+      TemperatureControl,      !- Unit Control Type
+      OAUHitemp2,              !- High Air Control Temperature Schedule Name
+      OAULotemp2,              !- Low Air Control Temperature Schedule Name
+      Zone5OAUOANode,          !- Outdoor Air Node Name
+      Zone5OAUZoneInletNode,   !- AirOutlet Node Name
+      Zone5OAUZoneOutletNode,  !- AirInlet Node Name
+      Zone5OAUFanOutletNode,   !- Supply FanOutlet Node Name
+      Zone5OAUEquip1;          !- Outdoor Air Unit List Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-5-012}
+
+\begin{itemize}
+\item
+  HVAC,Average, Zone Outdoor Air Unit Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum, Zone Outdoor Air Unit Total Heating Energy {[}J{]}
+\item
+  HVAC,Average, Zone Outdoor Air Unit Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Zone Outdoor Air Unit Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Zone Outdoor Air Unit Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Zone Outdoor Air Unit Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average, Zone Outdoor Air Unit Fan Electric Power {[}W{]}
+\item
+  HVAC,Sum, Zone Outdoor Air Unit Fan Electric Energy {[}J{]}
+\item
+  HVAC,Average, Zone Outdoor Air Unit Air Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average, Zone Outdoor Air Unit Fan Availability Status {[]}
+\item
+  Zone Outdoor Air Unit Latent Cooling Energy
+\end{itemize}
+
+\paragraph{Zone Outdoor Air Unit Total Heating Rate {[}W{]}}\label{zone-outdoor-air-unit-total-heating-rate-w}
+
+This field reports the heating output rate of the outdoor air unit system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the zone outdoor air unit.
+
+\paragraph{Zone Outdoor Air Unit Total Heating Energy {[}J{]}}\label{zone-outdoor-air-unit-total-heating-energy-j}
+
+This field is the heating output of the outdoor air unit system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the zone outdoor air unit, and the time step.
+
+\paragraph{Zone Outdoor Air Unit Total Cooling Rate {[}W{]}}\label{zone-outdoor-air-unit-total-cooling-rate-w}
+
+This field reports the total cooling (sensible plus latent) output rate of the outdoor air unit system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the zone outdoor air unit.
+
+\paragraph{Zone Outdoor Air Unit Total Cooling Energy {[}J{]}}\label{zone-outdoor-air-unit-total-cooling-energy-j}
+
+This field is the total cooling (sensible plus latent) output of the outdoor air unit system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the zone outdoor air unit, and the time step.
+
+\paragraph{Zone Outdoor Air Unit Sensible Cooling Energy {[}J{]}}\label{zone-outdoor-air-unit-sensible-cooling-energy-j}
+
+\paragraph{Zone Outdoor Air Unit Sensible Cooling Rate {[}W{]}}\label{zone-outdoor-air-unit-sensible-cooling-rate-w}
+
+These reports are the sensible cooling output rate of the outdoor air unit system to the zone it is serving in Joules or Watts. This is determined by outlet and zone air conditions and the mass flow rate through the zone outdoor air unit.
+
+\paragraph{Zone Outdoor Air Unit Sensible Heating Energy {[}J{]}}\label{zone-outdoor-air-unit-sensible-heating-energy-j}
+
+\paragraph{Zone Outdoor Air Unit Sensible Heating Rate {[}W{]}}\label{zone-outdoor-air-unit-sensible-heating-rate-w}
+
+These are the sensible heating output of the outdoor air unit system to the zone it is serving in Joules or Watts over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the zone outdoor air unit, and the time step.
+
+\paragraph{Zone Outdoor Air Unit Latent Cooling Energy {[}J{]}}\label{zone-outdoor-air-unit-latent-cooling-energy-j}
+
+\paragraph{Zone Outdoor Air Unit Latent Cooling Rate {[}W{]}}\label{zone-outdoor-air-unit-latent-cooling-rate-w}
+
+These are the latent cooling output of the outdoor air unit system to the zone it is serving, in Joules and Watts. This is determined by outlet and zone air conditions, the mass flow rate through the zone outdoor air unit, and the time step.
+
+\paragraph{Zone Outdoor Air Unit Latent Heating Energy {[}J{]}}\label{zone-outdoor-air-unit-latent-heating-energy-j}
+
+\paragraph{Zone Outdoor Air Unit Latent Heating Rate {[}W{]}}\label{zone-outdoor-air-unit-latent-heating-rate-w}
+
+These are the latent heating output of the outdoor air unit system to the zone it is serving, in Joules and Watts. This is determined by outlet and zone air conditions, the mass flow rate through the zone outdoor air unit, and the time step.
+
+\paragraph{Zone Outdoor Air Unit Fan Electric Power {[}W{]}}\label{zone-outdoor-air-unit-fan-electric-power-w}
+
+This field reports the electric power consumption rate of the fan of the outdoor air unit in Watts.
+
+\paragraph{Zone Outdoor Air Unit Fan Electric Energy {[}J{]}}\label{zone-outdoor-air-unit-fan-electric-energy-j}
+
+This field reports the electric power consumed by the fan of the outdoor air unit over the time step in Joules.
+
+\paragraph{Zone Outdoor Air Unit Air Mass Flow Rate {[}kg/s{]}}\label{zone-outdoor-air-unit-air-mass-flow-rate-kgs}
+
+This field reports the air mass flow rate of the zone outdoor air unit Outdoor Air Unit~ in kilograms per second.
+
+\paragraph{\texorpdfstring{Zone Outdoor Air Unit Fan Availability Status {[]}}{Zone Outdoor Air Unit Fan Availability Status }}\label{zone-outdoor-air-unit-fan-availability-status}
+
+This is the availability status of the outdoor air unit fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the outdoor air unit~ object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\subsection{ZoneHVAC:OutdoorAirUnit:EquipmentList}\label{zonehvacoutdoorairunitequipmentlist}
+
+This input syntax is used to specify the components in a zone outdoor air unit. The components will be simulated in the order in which they occur in this list.
+
+\subsubsection{Inputs}\label{inputs-6-032}
+
+\paragraph{Field: Name}\label{field-name-6-027}
+
+The user designated unique name of an instance of a zone outdoor air unit equipment list.
+
+\paragraph{Field Set (Component Object Type, Component Name, Control Node Name) up to 8}\label{field-set-component-object-type-component-name-control-node-name-up-to-8}
+
+After the identifying name, the list consists of up to 8 pairs of data items.
+
+\paragraph{Field: Component \textless{}x\textgreater{} Object Type}\label{field-component-x-object-type-000}
+
+This field specifies the keyword for the type of component used.
+
+\paragraph{Field: Component \textless{}x\textgreater{} Name}\label{field-component-x-name-000}
+
+This field is the unique name of the component specified in the previous field. This named object must appear in the IDF.
+
+Note: If any of the components use the autosized option at the component level, input data for zone sizing purposes are required for the proper sizing of the components. Please refer to the~Sizing:Zone~object for more information.
+
+An example from an IDF:
+
+\begin{lstlisting}
+
+ZoneHVAC:OutdoorAirUnit:EquipmentList,
+      Zone5OAUEquip1,          !- Name
+      Dehumidifier:Desiccant:NoFans,  !- Component 1 Object Type
+      Z5Dessicant,             !- Component 1 Name
+      HeatExchanger:AirToAir:FlatPlate,  !- Component 2 Object Type
+      Zone5A2AHeat Recovery,   !- Component 2 Name
+      CoilSystem:Cooling:DX,  !- Component 3 Object Type
+      DX Cooling Coil System 5,!- Component 3 Name
+      Coil:Heating:Electric,   !- Component 4 Object Type
+      Zone5DESHCoil;           !- Component 4 Name
+\end{lstlisting}
+
+\subsection{ZoneHVAC:WindowAirConditioner}\label{zonehvacwindowairconditioner}
+
+The Window Air Conditioner is a unit of zone equipment made up of other components. Each window air conditioner consists of an outdoor air mixer, a fan, and a direct expansion (DX) cooling coil. These components are described elsewhere in this document. The input for a window air conditioner requires the names of these three pieces of equipment, which are then specified individually elsewhere in the input. The input for a window air conditioner also requires the name of an availability schedule, the maximum unit airflow rate, and the maximum outdoor airflow rate for the unit. The unit is connected to a zone by specifying an air inlet node, which must be the same as a zone exhaust node; and an air outlet node, which must be the same as a zone inlet node (ref. ZoneHVAC:EquipmentConnections).
+
+A supply air fan operating mode schedule must also be specified. The supply air fan operating mode schedule value determines if the supply air fan can run continuously with the DX coil cycling on/off to match the zone cooling demand or the fan and DX coil can cycle on/off together to meet the cooling demand. The placement of the supply air fan, in relation to the DX coil, must also be specified (blow through or draw through). The cooling convergence tolerance is required, which is the tolerance denoting how closely the window air conditioner will meet the cooling load. The tolerance is always relative to the zone load (i.e., the unit will operate to meet the zone load to within the tolerance value times the zone load for each simulation timestep). Finally, the DX cooling coil type must be specified.
+
+\subsubsection{Inputs}\label{inputs-7-031}
+
+\paragraph{Field: Name}\label{field-name-7-025}
+
+A unique user assigned name for an instance of a window air conditioner unit. Any reference to this window air conditioner by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-6-005}
+
+The name of the schedule (ref: Schedule) that denotes whether the window air conditioner unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Maximum Supply Air Flow Rate}\label{field-maximum-supply-air-flow-rate-3}
+
+The maximum volumetric airflow rate through the window air conditioner in cubic meters per second. Since the unit operates by cycling on/off, this is also the design, rated airflow rate of the unit.
+
+\paragraph{Field: Maximum Outdoor Air Flow Rate}\label{field-maximum-outdoor-air-flow-rate-2-000}
+
+If the window air conditioner uses outdoor air, this field specifies the outdoor air volumetric flow rate in cubic meters per second. This flow rate should be less than or equal to the maximum airflow rate. A value of zero specifies no outdoor air. Note that the outdoor airflow rate is fixed: it cannot change during the simulation
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-4-002}
+
+The name of the HVAC system node (see Node) from which the window air conditioner draws its indoor air. This should be one of the zone exhaust nodes for the zone which the window air conditioner is cooling.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-4-002}
+
+The name of the HVAC system node (see Node) to which the window air conditioner sends its outlet air. This should be one of the inlet air nodes for the zone which is being cooled.
+
+\paragraph{Field: Outdoor Air Mixer Object Type}\label{field-outdoor-air-mixer-object-type-1}
+
+This field specifies the type of outdoor air mixer used by this window air conditioner unit. The outdoor air mixer component is part of the window air conditioner compound object. The only available outdoor air mixer type is:
+
+OutdoorAir:Mixer
+
+\paragraph{Field: Outdoor Air Mixer Name}\label{field-outdoor-air-mixer-name-1}
+
+The name of an outdoor air mixer component which composes part of the window air conditioner unit. Note that the return air node of the outdoor air mixer should be the same node as the air inlet node of the window air conditioner. In addition, the outdoor air mixer's mixed air node should be the same as the window air conditioner's fan inlet air node (for blow through) or the air conditioner's DX coil inlet node (for draw through)
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-4}
+
+This field specifies the type of supply air fan used by window air conditioner. The supply air fan is part of the window air conditioner compound object. The only valid supply air fan types are:
+
+\begin{itemize}
+\item
+  Fan:OnOff
+\item
+  Fan:ConstantVolume
+\end{itemize}
+
+\paragraph{Field:Supply Air Fan Name}\label{fieldsupply-air-fan-name}
+
+The name of a constant volume fan component that composes part of the window air conditioner. Note that the fan's maximum flow rate should be the same as the maximum airflow rate of the window air conditioner. A fan of type Fan:OnOff may be used with either cycling or continuous fan, and a fan of type Fan:ConstantVolume is used only with continuous fan (see Supply Air Fan Operating Mode Schedule field below). The fan's inlet node should be the same as the outdoor air mixer's mixed air node (for blow through) or the DX coil's outlet node (for draw through). The fan's outlet node should be the same as the DX coil's air inlet node (for blow through) or the window air conditioner's air outlet node (for draw through).
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-2-001}
+
+This field specifies the type of cooling coil to be modeled for this window air conditioner. The input requirements for these cooling coil objects are described elsewhere in this document. If the user wants to control the enhanced dehumidification performance of the Heat Exchanger Assisted coil type based on zone air humidity level, then the input file must include a humidistat object (ref. ZoneControl:Humidistat) for the zone being served by this air conditioner and a high humidity set point manager (ref. SetpointManager:SingleZone:Humidity:Maximum) with the high humidity set point placed on the outlet node of the heat exchanger assisted cooling coil. Only allowable coil types are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted
+\end{itemize}
+
+\paragraph{Field: DX Cooling Coil Name}\label{field-dx-cooling-coil-name}
+
+The name of a DX cooling coil component that composes part of the window air conditioner unit. The DX coil air inlet node should be the same as the fan outlet node (for blow through) or the outdoor air mixer's mixed air node (for draw through). The DX coil air outlet node should be the same as the window air conditioner's air outlet node (for blow through) or the fan's inlet node (for draw through).
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-3-000}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply air fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, the model assumes the supply air fan cycles with the heating or cooling coil throughout the simulation.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-2-000}
+
+This input field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice stands for ``blow through fan''. This means that the unit consists of an outdoor air mixer followed by a fan followed by a DX coil. The fan ``blows through'' the DX coil. The second choice stands for ``draw through fan''. This means that the unit consists of an outdoor air mixer followed by a DX coil followed by a fan. The fan ``draws air through'' the coil.
+
+\paragraph{Field: Cooling Convergence Tolerance}\label{field-cooling-convergence-tolerance-2}
+
+This input field defines the convergence tolerance for the unit's cooling output. This field allows the user some control over how closely the air conditioner will control the air-side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in zone air temperature. Initial experience with this parameter lends to the recommendation of using 0.001 as the starting point.
+
+The window air conditioner is controlled by matching its sensible (temperature) cooling output to the zone sensible load (demand). Because the performance of the DX coil is frequently non-linear, the air conditioner model must call the DX coil model several times (iterate) to determine the proper run time fraction to meet the zone load. The cooling convergence tolerance is the error tolerance used to terminate the iteration procedure when the following equation is satisfied:
+
+\begin{equation}
+\frac{{\left| {{Q_{ZoneLoad}} - {Q_{WindowAirConditioner,out}})} \right|}}{{{Q_{ZoneLoad}}}} \le Cooling{\kern 1pt} Convergence{\kern 1pt} Tolerance
+\end{equation}
+
+The maximum number of iterations is limited, with a warning message generated if the above equation is not satisfied within the maximum number of iterations.
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-5}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this window air conditioner or object's fan. If the window air conditioner is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this window air conditioner object should be on or off.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name-5}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Maximum Air Flow Rate in this Window Air Conditioner zone HVAC object. The scaled Maximum Air Flow Rate in turn is used to size cooling capacity of the unit.
+
+Following is an example input for the cycling window air conditioner, along with its constituent components.
+
+\begin{lstlisting}
+
+ZoneHVAC:WindowAirConditioner,
+         Zone3WindAC,                  ! name of window AC unit
+         FanAndCoilAvailSched,         ! Availability Schedule Name
+         0.6,                          ! Maximum Supply Air Flow Rate {m3/s}
+         0.05,                         ! Maximum Outdoor Air Flow Rate {m3/s}
+         Zone3WindACAirInletNode,      ! Air Inlet Node Name
+         Zone3WindACAirOutletNode,     ! Air Outlet Node Name
+         OutdoorAir:Mixer,             ! Outdoor Air Mixer Object Type
+         Zone3WindACOAMixer,           ! Outdoor Air Mixer Name
+         Fan:ConstantVolume,           ! Supply Air Fan Object Type
+         Zone3WindACFan,               ! Fan Name
+         Zone3WindACDXCoil,            ! DX Cooling Coil Name
+         CyclingFanSch,                ! Supply Air Fan Operation Mode Schedule Name
+         DrawThrough,                  ! Fan Placement
+         0.001,                        ! Cooling Convergence Tolerance
+         Coil:Cooling:DX:SingleSpeed;  ! Cooling Coil Object Type
+
+
+  Schedule:Compact,
+         CyclingFanSch,                !- Name
+         Fraction,                     !- ScheduleType
+         Through: 12/31,               !- Complex Field \#1
+         For: AllDays,                 !- Complex Field \#2
+         Until: 24:00,                 !- Complex Field \#7
+         0.0;                          !- Complex Field \#8
+
+
+  OutdoorAir:Mixer,
+         Zone3WindACOAMixer,           ! Name
+         Zone3WindACOAMixerOutletNode, ! Mixed Air Node Name
+         Zone3WindACOAInNode,          ! Outdoor Air Stream Node Name
+         Zone3WindACExhNode,           ! Relief Air Stream Node Name
+         Zone3WindACAirInletNode;      ! Return Air Stream Node Name
+
+
+  Fan:ConstantVolume,
+         Zone3WindACFan,               ! Name
+         FanAndCoilAvailSched,         ! Availability Schedule Name
+         0.5,                          ! Fan Total Efficiency
+         75.0,                         ! Pressure Rise {Pa}
+         0.6,                          ! Maximum Flow Rate {m3/s}
+         0.9,                          ! Motor Efficiency
+         1.0,                          ! Motor In Airstream Fraction
+         Zone3WindACDXOutletNode,      ! Air Inlet Node Name
+         Zone3WindACAirOutletNode;     ! Air Outlet Node Name
+
+
+  Coil:Cooling:DX:SingleSpeed,
+      Zone3WindACDXCoil,       !- Name
+      CoolingCoilAvailSched,   !- Availability Schedule Name
+      autosize,                !- Rated Total Cooling Capacity {W}
+      autosize,                !- Rated Sensible Heat Ratio
+      3.0,                     !- Rated COP
+      autosize,                !- Rated Air Flow Rate {m3/s}
+      Zone3WindACOAMixerOutletNode,  !- Air Inlet Node Name
+      Zone3WindACDXOutletNode, !- Air Outlet Node Name
+      WindACCoolCapFT,         !- Total Cooling Capacity Function of Temperature Curve Name
+      WindACCoolCapFFF,        !- Total Cooling Capacity Function of Flow Fraction Curve Name
+      WindACEIRFT,             !- Energy Input Ratio Function of Temperature Curve Name
+      WindACEIRFFF,            !- Energy Input Ratio Function of Flow Fraction Curve Name
+      WindACPLFFPLR;           !- Part Load Fraction Correlation Curve Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-6-012}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Window Air Conditioner Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Window Air Conditioner Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Window Air Conditioner Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Window Air Conditioner Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Window Air Conditioner Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Window Air Conditioner Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Window Air Conditioner Electric Power{[}W{]}
+\item
+  HVAC,Sum,Zone Window Air Conditioner Electric Energy {[}J{]}
+\item
+  HVAC,Average, Zone Window Air Conditioner Fan Part Load Ratio {[]}
+\item
+  HVAC,Average, Zone Window Air Conditioner Compressor Part Load Ratio {[]}
+\item
+  HVAC,Average,Zone Window Air Conditioner Fan Availability Status {[]}
+\end{itemize}
+
+\paragraph{Zone Window Air Conditioner Total Cooling Rate {[}W{]}}\label{zone-window-air-conditioner-total-cooling-rate-w}
+
+This field is the total (sensible and latent) heat extraction rate of the window air conditioner unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
+
+\paragraph{Zone Window Air Conditioner Total Cooling Energy {[}J{]}}\label{zone-window-air-conditioner-total-cooling-energy-j}
+
+This is the total (sensible and latent) heat extraction of the window air conditioner unit from the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit, and the timestep.
+
+\paragraph{Zone Window Air Conditioner Sensible Cooling Rate {[}W{]}}\label{zone-window-air-conditioner-sensible-cooling-rate-w}
+
+This field reports the moist air sensible heat extraction rate of the window air conditioner unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
+
+\paragraph{Zone Window Air Conditioner Sensible Cooling Energy {[}J{]}}\label{zone-window-air-conditioner-sensible-cooling-energy-j}
+
+This field reports the moist air sensible heat extraction of the window air conditioner unit from the zone it is serving in Joules over the timestep being reported. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
+
+\paragraph{Zone Window Air Conditioner Latent Cooling Rate {[}W{]}}\label{zone-window-air-conditioner-latent-cooling-rate-w}
+
+This output is the latent heat extraction rate of the window air conditioner unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
+
+\paragraph{Zone Window Air Conditioner Latent Cooling Energy {[}J{]}}\label{zone-window-air-conditioner-latent-cooling-energy-j}
+
+This is the latent heat extraction of the window air conditioner unit from the zone it is serving in Joules over the timestep being reported. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
+
+\paragraph{Zone Window Air Conditioner Electric Power{[}W{]}}\label{zone-window-air-conditioner-electric-powerw}
+
+This output is the electricity consumption rate of the window air conditioner unit in Watts. The consumption includes electricity used by the compressor and the fans (indoor supply air fan and the condenser fan).
+
+\paragraph{Zone Window Air Conditioner Electric Energy {[}J{]}}\label{zone-window-air-conditioner-electric-energy-j}
+
+This output is the electricity consumption of the window air conditioner unit in Joules for the time period being reported. The consumption includes electricity used by the compressor and the fans (indoor supply air fan and the condenser fan).
+
+\paragraph{\texorpdfstring{Zone Window Air Conditioner Fan Part Load Ratio {[]}}{Zone Window Air Conditioner Fan Part Load Ratio }}\label{zone-window-air-conditioner-fan-part-load-ratio}
+
+This is the fan's part load ratio for the report timestep during which the fan had operated.
+
+\paragraph{\texorpdfstring{Zone Window Air Conditioner Compressor Part Load Ratio {[]}}{Zone Window Air Conditioner Compressor Part Load Ratio }}\label{zone-window-air-conditioner-compressor-part-load-ratio}
+
+This is the part load ratio of the report timestep during which the DX unit compressor had operated.
+
+\textbf{\emph{Zone Window Air Conditioner Fan Availability Status {[]}}}
+
+This is the availability status of the window air conditioner fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the window air conditioner object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\subsection{ZoneHVAC:PackagedTerminalAirConditioner}\label{zonehvacpackagedterminalairconditioner}
+
+The packaged terminal air conditioner (PTAC) is a compound object made up of other components. Each PTAC consists of an outdoor air mixer, direct expansion (DX) cooling coil, heating coil (gas, electric, hot water, or steam) and a supply air fan. While the figure below shows the PTAC with draw through fan placement, blow through fan placement can also be modeled by positioning the supply air fan between the outdoor air mixer and the DX cooling coil. The packaged terminal air conditioner coordinates the operation of these components and is modeled as a type of zone equipment (Ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
+
+\begin{figure}[hbtp] % fig 111
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image284.png}
+\caption{  Schematic of a packaged terminal air conditioner with draw through fan placement \protect \label{fig:schematic-of-a-packaged-terminal-air-001}}
+\end{figure}
+
+Links to the PTAC's supply air fan, DX cooling coil, heating coil, and outdoor air mixer specifications are provided in the air conditioner's input syntax. Additional inputs include supply and outdoor air flow rates during cooling operation, heating operation, and when neither cooling or heating is required. A description of each input field for the packaged terminal air conditioner compound object is provided below.
+
+\subsubsection{Inputs}\label{inputs-8-029}
+
+\paragraph{Field: Name}\label{field-name-8-025}
+
+This alpha field defines a unique user-assigned name for an instance of a packaged terminal air conditioner. Any reference to this air conditioner by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-7-005}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the air conditioner operates during a given time period. A schedule value equal to 0 denotes that the air conditioner must be off for that time period. A value greater than 0 denotes that the air conditioner is available to operate during that time period. This schedule may be used to completely disable the air conditioner (all of its coils and the supply air fan) as required. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-5-001}
+
+This alpha field defines the name of the HVAC system node from which the air conditioner draws its inlet air. This node name must be the name of a zone air exhaust node (Ref. ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-5-001}
+
+This alpha field defines the name of the HVAC system node to which the air conditioner sends its outlet air. This node name must be the name of a zone air inlet node (Ref. ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Outdoor Air Mixer Object Type}\label{field-outdoor-air-mixer-object-type-2}
+
+This field specifies the type of outdoor air mixer used by this PTAC. The outdoor air mixer component is part of the PTAC unit. The only available outdoor air mixer type is:
+
+\begin{itemize}
+\tightlist
+\item
+  OutdoorAir:Mixer
+\end{itemize}
+
+\paragraph{Field: Outdoor Air Mixer Name}\label{field-outdoor-air-mixer-name-2}
+
+This alpha field defines the name of an outdoor air mixer component which composes part of the PTAC. The return air node of the outdoor air mixer should also be the same node as the air inlet node of the PTAC. Furthermore, the outdoor air mixer's mixed air node should be the same as the PTAC's fan inlet air node (for blow through fan placement) or the PTAC's DX cooling coil inlet node (for draw through fan placement).
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-002}
+
+This numeric field defines the supply air flow rate leaving the air conditioner in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-002}
+
+This numeric field defines the supply air flow rate leaving the air conditioner in cubic meters per second when the heating coil is operating. Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-001}
+
+This numeric field defines the supply air flow rate leaving the air conditioner in cubic meters per second when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the air conditioner's supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner's supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).
+
+\paragraph{Field: Cooling Outdoor Air Flow Rate}\label{field-cooling-outdoor-air-flow-rate-001}
+
+This numeric field defines the outdoor air flow rate through the air conditioner in cubic meters per second when the DX cooling coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Cooling Outdoor Air Flow Rate is fixed; it cannot change during the simulation. In addition, the Cooling Outdoor Air Flow Rate cannot be greater than the air conditioner's supply air volumetric flow rate during cooling operation.
+
+\paragraph{Field: Heating Outdoor Air Flow Rate}\label{field-heating-outdoor-air-flow-rate-001}
+
+This numeric field defines the outdoor air flow rate through the air conditioner in cubic meters per second when the heating coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Heating Outdoor Air Flow Rate is fixed; it cannot change during the simulation. In addition, the Heating Outdoor Air Flow Rate cannot be greater than the air conditioner's supply air volumetric flow rate during heating operation.
+
+\paragraph{Field: No Load Outdoor Air Flow Rate}\label{field-no-load-outdoor-air-flow-rate-000}
+
+This numeric field defines the outdoor air flow rate through the air conditioner in cubic meters per second when neither cooling nor heating is required (i.e., cooling and heating coils are off but the supply air fan operates). Values must be greater than or equal to 0, or this field is autosizable. Note that the outdoor air flow rate when no cooling/heating is needed is fixed; it cannot change during the simulation. In addition, the outdoor air flow rate when no cooling/heating is needed cannot be greater than the air conditioner's supply air volumetric flow rate when no cooling/heating is needed. This field is only used when the air conditioner's supply air fan operating mode schedule specifies continuous fan operation. If the air conditioner's supply air fan operating mode schedule specifies continuous fan operation and the field `Supply air volumetric flow rate when no cooling or heating is needed' is set to zero or is left blank, then the model assumes that the outdoor air flow rate when no cooling/heating is needed is equal to the outdoor air flow rate when the cooling or heating coil was last operating (for cooling operation {[}i.e., Cooling Outdoor Air Flow Rate{]} or heating operation {[}i.e., Heating Outdoor Air Flow Rate{]}) and this field is not used.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-5}
+
+This alpha field defines the type of fan used by this PTAC. The only valid choices are \textbf{Fan:OnOff} and \textbf{Fan:ConstantVolume}. A fan of type Fan:OnOff is used with cycling fan operating mode, and a fan of type Fan:ConstantVolume is used with continuous fan operating mode (see Supply Air Fan Operating Mode Schedule field below). The input requirements for these fan objects are described elsewhere in this document.
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-4}
+
+The name of a constant volume fan component that composes part of the PTAC. Note that the fan's maximum flow rate should be greater than or equal to the maximum supply air flow rate for the PTAC. The fan's inlet node should be the same as the outdoor air mixer's mixed air node (for blow through fan placement) or the heating coil's outlet node (for draw through fan placement). The fan's outlet node should be the same as the DX cooling coil's air inlet node (for blow through fan placement) or the PTAC's air outlet node (for draw through fan placement).
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-3-000}
+
+This alpha field defines the type of heating coil to be used by this PTAC. The input requirements for this heating coil object are described elsewhere in this document. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (PTAC) itself provides the ``controller'' function of modulating water flow. Allowable heating coil types are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-3-000}
+
+This alpha field defines the name of the heating coil used by this PTAC, and this name should match the name specified in the corresponding heating coil object.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-3-000}
+
+This alpha field defines the type of DX cooling coil used by this PTAC. The input requirements for these DX cooling coil objects are described elsewhere in this document. Only allowable coil types are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted
+\item
+  Coil:Cooling:DX:VariableSpeed
+\end{itemize}
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-2-001}
+
+This alpha field defines the name of the cooling coil used by this PTAC, and this name should match the name specified in the corresponding DX cooling coil object.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-3-000}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice stands for ``blow through fan''. This means that the unit consists of an outdoor air mixer followed by a fan followed by the DX cooling coil and heating coil. The fan ``blows through'' the DX cooling coil and the heating coil. The second choice stands for ``draw through fan''. This means that the unit consists of an outdoor air mixer followed by the DX cooling coil and heating coil with the fan located at the outlet of the PTAC. The fan ``draws air through'' the DX cooling coil and the heating coil. If this field is left blank, the default is draw through.
+
+Note: the packaged terminal air conditioner's supply air fan, cooling coil and heating coil must be connected according to the configuration shown above (Figure~\ref{fig:schematic-of-a-packaged-terminal-air-001}) for the draw through fan configuration. The only other valid configuration is with a blow through fan placement, where the fan is located between the outdoor air mixer and the DX cooling coil.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-4}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-6}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this packaged terminal air conditioner or object's fan. If the packaged terminal air conditioner is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this packaged terminal air conditioner object should be on or off.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name-6}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Cooling Supply Air Flow Rate in this Packaged Terminal Air Conditioner~ zone HVAC object. The scaled Supply Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
+
+As shown in the example below, correct specification of the packaged terminal air conditioner requires the following objects in addition to the compound object itself:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Fan (Fan:OnOff or Fan:ConstantVolume)
+\item
+  DX cooling coil (Coil:Cooling:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted)
+\item
+  Heating coil (Coil:Heating:Gas, Coil:Heating:Electric, Coil:Heating:Water, or Coil:Heating:Steam)
+\item
+  OutdoorAir:Mixer
+\end{enumerate}
+
+\begin{lstlisting}
+
+ZoneHVAC:PackagedTerminalAirConditioner,
+  Zone2PTAC,               !- Name
+  FanAndCoilAvailSched,    !- Availability Schedule Name
+  Zone2PTACAirInletNode,   !- Air Inlet Node Name
+  Zone2PTACAirOutletNode,  !- Air Outlet Node Name
+  OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type
+  Zone2PTACOAMixer,        !- Outdoor Air Mixer Name
+  autosize,              !- Cooling Supply Air Flow Rate {m3/s}
+  autosize,              !- Heating Supply Air Flow Rate operation {m3/s}
+  autosize,              !- No Load Supply Air Flow Rate {m3/s}
+  autosize,              !- Cooling Outdoor Air Flow Rate {m3/s}
+  autosize,              !- Heating Outdoor Air Flow Rate {m3/s}
+  autosize,              !- No Load Outdoor Air Flow Rate  {m3/s}
+  Fan:OnOff,                      !- Supply Air Fan Object Type
+  Zone2PTACFan,                          !- Supply Air Fan Name
+  Coil:Heating:Electric,                 !- Heating Coil Object Type
+  Zone2PTACHeatCoil,                     !- Heating Coil Name
+  Coil:Cooling:DX:SingleSpeed,  !- Cooling Coil Object Type
+  Zone2PTACDXCoolCoil,                   !- Cooling Coil Name
+  BlowThrough,                           !- Fan Placement
+  SupplyFanSch;                          !- Supply Air Fan Operating Mode Schedule Name
+
+
+  Schedule:Compact,
+      SupplyFanSch,            !- Name
+      Fraction,                !- ScheduleType
+      Through: 12/31,          !- Complex Field \#1
+      For: AllDays,            !- Complex Field \#2
+      Until:  7:00,            !- Complex Field \#3
+      0.0,                     !- Complex Field \#4
+      Until: 18:00,            !- Complex Field \#5
+      1.0,                     !- Complex Field \#6
+      Until: 24:00,            !- Complex Field \#7
+      0.0;                     !- Complex Field \#8
+
+  OutdoorAir:Mixer,
+      Zone2PTACOAMixer,            !- Name
+      Zone2PTACOAMixerOutletNode,  !-Mixed Air Node Name
+      Zone2PTACOAInNode,           !-Outdoor Air Stream Node Name
+      Zone2PTACExhNode,            !- Relief Air Stream Node Name
+      Zone2PTACAirInletNode;       !- Return Air Stream Node Name
+
+    Fan:OnOff,
+      Zone2PTACFan,                !- Name
+      FanAndCoilAvailSched,        !- Availability Schedule Name
+      0.5,                         !- Fan Total Efficiency
+      75.0,                        !- Pressure Rise {Pa}
+      autosize,                    !- Maximum Flow Rate{m3/s}
+      0.9,                         !- Motor Efficiency
+      1.0,                         !- Motor In Airstream Fraction
+      Zone2PTACOAMixerOutletNode,  !- Air Inlet Node Name
+      Zone2PTACFanOutletNode;      !- Air Outlet Node Name
+
+  Coil:Cooling:DX:SingleSpeed,
+      Zone2PTACDXCoolCoil,         !- Coil Name
+      CoolingCoilAvailSched,       !- Availability Schedule Name
+      autosize,                    !- Rated Total Cooling Capacity (gross) {W}
+      autosize,                    !- Rated SHR
+      3.0,                         !- Rated COP
+      autosize,                    !- Rated Air Volume Flow Rate {m3/s}
+      Zone2PTACFanOutletNode,      !- Coil Air Inlet Node
+      Zone2PTACCoolCoilOutletNode, !-Coil Air Outlet Node
+      HPACCoolCapFT,               !- Total Cooling Capacity Modifier Curve (function of temperature)
+      HPACCoolCapFFF,              !- Total Cooling Capacity Modifier Curve (function of flow fraction)
+      HPACEIRFT,                   !- Energy Input Ratio Modifier Curve (function of temperature)
+      HPACEIRFFF,                  !- Energy Input Ratio Modifier Curve (function of flow fraction)
+      HPACPLFFPLR;                 !- Part Load Fraction Correlation (function of part load ratio)
+
+  Coil:Heating:Electric,
+      Zone2PTACHeatCoil,           !- Coil Name
+      HeatingCoilAvailSched,       !- Availability Schedule Name
+      1.0,                         !- Efficiency
+      autosize,                    !- Nominal Capacity {W}
+      Zone2PTACCoolCoilOutletNode, !- Air Inlet Node Name
+      Zone2PTACAirOutletNode;      !- Air Outlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-7-012}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Packaged Terminal Air Conditioner Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Air Conditioner Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Air Conditioner Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Air Conditioner Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Air Conditioner Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Air Conditioner Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Air Conditioner Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Air Conditioner Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Air Conditioner Latent Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Air Conditioner Latent Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Air Conditioner Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Air Conditioner Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Air Conditioner Electric Power {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Air Conditioner Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Air Conditioner Fan Part Load Ratio {[]}
+\item
+  HVAC,Average,Zone Packaged Terminal Air Conditioner Compressor Part Load Ratio {[]}
+\item
+  HVAC,Average,Zone Packaged Terminal Air Conditioner Fan Availability Status {[]}
+\end{itemize}
+
+\paragraph{Zone Packaged Terminal Air Conditioner Total Heating Rate {[}W{]}}\label{zone-packaged-terminal-air-conditioner-total-heating-rate-w}
+
+This output field is the total (enthalpy) heat addition rate of the packaged terminal air conditioner to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams, and the air mass flow rate through the air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Total Heating Energy {[}J{]}}\label{zone-packaged-terminal-air-conditioner-total-heating-energy-j}
+
+This output field is the total (enthalpy) heat addition of the packaged terminal air conditioner to the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams, the air mass flow rate through the air conditioner, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Total Cooling Rate {[}W{]}}\label{zone-packaged-terminal-air-conditioner-total-cooling-rate-w}
+
+This output field is the total (enthalpy) heat extraction rate of the packaged terminal air conditioner from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams, and the air mass flow rate through the air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Total Cooling Energy {[}J{]}}\label{zone-packaged-terminal-air-conditioner-total-cooling-energy-j}
+
+This output field is the total (enthalpy) heat extraction of the packaged terminal air conditioner from the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams, the air mass flow rate through the air conditioner, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Sensible Heating Rate {[}W{]}}\label{zone-packaged-terminal-air-conditioner-sensible-heating-rate-w}
+
+This output field is the sensible heat addition rate of the packaged terminal air conditioner to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Sensible Heating Energy {[}J{]}}\label{zone-packaged-terminal-air-conditioner-sensible-heating-energy-j}
+
+This output field is the sensible heat addition of the packaged terminal air conditioner to the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the air conditioner, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Sensible Cooling Rate {[}W{]}}\label{zone-packaged-terminal-air-conditioner-sensible-cooling-rate-w}
+
+This output field reports the moist air sensible heat extraction rate of the packaged terminal air conditioner from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Sensible Cooling Energy {[}J{]}}\label{zone-packaged-terminal-air-conditioner-sensible-cooling-energy-j}
+
+This output field reports the moist air sensible heat extraction of the packaged terminal air conditioner from the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the air conditioner, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Latent Heating Rate {[}W{]}}\label{zone-packaged-terminal-air-conditioner-latent-heating-rate-w}
+
+This output field is the latent heat addition (humidification) rate of the packaged terminal air conditioner to the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the packaged terminal air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Latent Heating Energy {[}J{]}}\label{zone-packaged-terminal-air-conditioner-latent-heating-energy-j}
+
+This output field is the latent heat addition (humidification) of the packaged terminal air conditioner to the zone it is serving in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the packaged terminal air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Latent Cooling Rate {[}W{]}}\label{zone-packaged-terminal-air-conditioner-latent-cooling-rate-w}
+
+This output field is the latent heat extraction (dehumidification) rate of the packaged terminal air conditioner from the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the packaged terminal air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Latent Cooling Energy {[}J{]}}\label{zone-packaged-terminal-air-conditioner-latent-cooling-energy-j}
+
+This output field is the latent heat extraction (dehumidification) of the packaged terminal air conditioner from the zone it is serving in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the packaged terminal air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Electric Power {[}W{]}}\label{zone-packaged-terminal-air-conditioner-electric-power-w}
+
+This output field is the electricity consumption rate of the packaged terminal air conditioner in Watts. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the heating coil (includes electricity consumption rate for electric heating coil or parasitic electricity consumption rate for non-electric coils). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Air Conditioner Electric Energy {[}J{]}}\label{zone-packaged-terminal-air-conditioner-electric-energy-j}
+
+This output field is the electricity consumption of the packaged terminal air conditioner in Joules for the time period being reported. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the heating coil (includes electricity consumption for electric heating coil or parasitic electricity consumption for non-electric coils). This value is calculated for each HVAC system timestep being simulated, and the results are summed for the timestep being reported.
+
+\paragraph{\texorpdfstring{Zone Packaged Terminal Air Conditioner Fan Part Load Ratio {[]}}{Zone Packaged Terminal Air Conditioner Fan Part Load Ratio }}\label{zone-packaged-terminal-air-conditioner-fan-part-load-ratio}
+
+This output field is the part-load ratio of the fan. The fan part-load ratio is defined as the average supply air mass flow rate divided by the maximum supply air mass flow rate. The maximum supply air mass flow rate depends on whether heating, cooling, or no heating or cooling is required during the timestep. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{\texorpdfstring{Zone Packaged Terminal Air Conditioner Compressor Part Load Ratio {[]}}{Zone Packaged Terminal Air Conditioner Compressor Part Load Ratio }}\label{zone-packaged-terminal-air-conditioner-compressor-part-load-ratio}
+
+This output field is the part-load ratio used by the coils (cooling and heating). Part-load ratio is defined as the total coil load divided by the coil steady-state capacity. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{\texorpdfstring{Zone Packaged Terminal Air Conditioner Fan Availability Status {[]}}{Zone Packaged Terminal Air Conditioner Fan Availability Status }}\label{zone-packaged-terminal-air-conditioner-fan-availability-status}
+
+This is the availability status of the packaged terminal air conditioner fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the packaged terminal air conditioner~ object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\subsection{ZoneHVAC:PackagedTerminalHeatPump}\label{zonehvacpackagedterminalheatpump}
+
+The packaged terminal heat pump (PTHP) is a compound object made up of other components. Each PTHP consists of an outdoor air mixer, direct expansion (DX) cooling coil, DX heating coil, supply air fan, and a supplemental heating coil as shown in the figure below. These individual components are described elsewhere in this document. The packaged terminal heat pump coordinates the operation of these components and is modeled as a type of zone equipment (Ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
+
+\begin{figure}[hbtp] % fig 112
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image285.png}
+\caption{Schematic of a packaged terminal heat pump (draw through fan placement) \protect \label{fig:schematic-of-a-packaged-terminal-heat-pump-001}}
+\end{figure}
+
+Links to the PTHP's supply air fan, DX coils, supplemental heating coil, and outdoor air mixer specifications are provided in the heat pump's input syntax. Additional inputs include supply and outdoor air flow rates during cooling operation, heating operation, and when neither cooling or heating is required. A description of each input field for the packaged terminal heat pump compound object is provided below.
+
+\subsubsection{Inputs}\label{inputs-9-026}
+
+\paragraph{Field: Name}\label{field-name-9-022}
+
+This alpha field defines a unique user-assigned name for an instance of a packaged terminal heat pump. Any reference to this heat pump by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-8-005}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump operates during a given time period. A schedule value equal to 0 denotes that the heat pump must be off for that time period. A value greater than 0 denotes that the heat pump is available to operate during that time period. This schedule may be used to completely disable the heat pump (all of its coils and the supply air fan) as required. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-6-000}
+
+This alpha field defines the name of the HVAC system node from which the heat pump draws its inlet air. This node name must be the name of a zone air exhaust node (Ref. ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-6-001}
+
+This alpha field defines the name of the HVAC system node to which the heat pump sends its outlet air. This node name must be the name of a zone air inlet node (Ref. ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Outdoor Air Mixer Object Type}\label{field-outdoor-air-mixer-object-type-3}
+
+This field specifies the type of outdoor air mixer used by this PTHP. The outdoor air mixer component is part of the PTHP compound object. The only available outdoor air mixer type is:
+
+\begin{itemize}
+\tightlist
+\item
+  OutdoorAir:Mixer
+\end{itemize}
+
+\paragraph{Field: Outdoor Air Mixer Name}\label{field-outdoor-air-mixer-name-3}
+
+This alpha field defines the name of an outdoor air mixer component which composes part of the PTHP. Note that the return air node of the outdoor air mixer should also be the same node as the air inlet node of the PTHP. Furthermore, the outdoor air mixer's mixed air node should be the same as the PTHP's fan inlet air node (for blow through fan placement) or the PTHP's DX cooling coil inlet node (for draw through fan placement).
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-1-001}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-1-001}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-1-001}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the heat pump's supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the heat pump's supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).
+
+\paragraph{Field: Cooling Outdoor Air Flow Rate}\label{field-cooling-outdoor-air-flow-rate-1}
+
+This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when the DX cooling coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Cooling Outdoor Air Flow Rate is fixed; it cannot change during the simulation. In addition, the Cooling Outdoor Air Flow Rate cannot be greater than the heat pump's supply air volumetric flow rate during cooling operation.
+
+\paragraph{Field: Heating Outdoor Air Flow Rate}\label{field-heating-outdoor-air-flow-rate-1}
+
+This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Heating Outdoor Air Flow Rate is fixed; it cannot change during the simulation. In addition, the Heating Outdoor Air Flow Rate cannot be greater than the heat pump's supply air volumetric flow rate during heating operation.
+
+\paragraph{Field: No Load Outdoor Air Flow Rate}\label{field-no-load-outdoor-air-flow-rate-1}
+
+This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). Values must be greater than or equal to 0, or this field is autosizable. Note that the outdoor air flow rate when no cooling/heating is needed is fixed; it cannot change during the simulation. In addition, the outdoor air flow rate when no cooling/heating is needed cannot be greater than the heat pump's supply air volumetric flow rate when no cooling/heating is needed. This field is only used when the heat pump's supply air fan operating mode schedule specifies continuous fan operation. If the heat pump's supply air fan operating mode schedule specifies continuous fan operation and the field `Supply air volumetric flow rate when no cooling or heating is needed' is set to zero or is left blank, then the model assumes that the outdoor air flow rate when no cooling/heating is needed is equal to the outdoor air flow rate when the cooling or heating coil was last operating (for cooling operation {[}i.e., Cooling Outdoor Air Flow Rate{]} or heating operation {[}i.e., Heating Outdoor Air Flow Rate{]}) and this field is not used.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-6}
+
+This alpha field defines the type of fan used by this PTHP. The only valid choices are Fan:OnOff and Fan:ConstantVolume. A fan of type Fan:OnOff may be used with either cycling or continuous fan operating mode, and a fan of type Fan:ConstantVolume is used only with continuous fan operating mode (see Supply Air Fan Operating Mode Schedule field below). The input requirements for these fan objects are described elsewhere in this document.
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-5}
+
+The name of a constant volume fan component that composes part of the PTHP. Note that the fan's maximum flow rate should be greater than or equal to the maximum supply air flow rate for the PTHP. The fan's inlet node should be the same as the outdoor air mixer's mixed air node (for blow through fan placement) or the DX heating coil's outlet node (for draw through fan placement). The fan's outlet node should be the same as the DX cooling coil's air inlet node (for blow through fan placement) or the supplemental heater's air inlet node (for draw through fan placement).
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-4-000}
+
+This alpha field defines the type of DX heating coil to be used by this PTHP. The only valid choice are \textbf{Coil:Heating:DX:SingleSpeed} and \textbf{Coil:Heating:DX:VariableSpeed}. The input requirements for this DX heating coil object are described elsewhere in this document.
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-4-000}
+
+This alpha field defines the name of the DX heating coil used by this PTHP, and this name should match the name specified in the corresponding DX heating coil object.
+
+\paragraph{Field: Heating Convergence Tolerance}\label{field-heating-convergence-tolerance-3}
+
+This numeric field defines the convergence tolerance for the unit's heating output. This field allows the user some control over how closely the heat pump will control the air-side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in zone air temperature. Initial experience with this parameter lends to the recommendation of using 0.001 as the starting point.
+
+The heat pump is controlled by matching its sensible (temperature) heating output to the zone sensible load (demand). Because the performance of the DX heating coil is frequently non-linear, the heat pump model must call the DX heating coil model several times (iterate) to determine the proper run time fraction to meet the zone load. The heating convergence tolerance is the error tolerance used to terminate the iteration procedure when the following equation is satisfied:
+
+\begin{equation}
+\frac{{\left| {({Q_{ZoneLoad}} - {Q_{HeatPump,out}})} \right|}}{{{Q_{ZoneLoad}}}}\,\, \le \,\,Heating{\kern 1pt} Convergence{\kern 1pt} Tolerance
+\end{equation}
+
+The maximum number of iterations is limited, with a warning message generated if the above equation is not satisfied within the maximum number of iterations.
+
+\paragraph{Field: Minimum Outdoor Dry-Bulb Temperature for Compressor Operation}\label{field-minimum-outdoor-dry-bulb-temperature-for-compressor-operation-001}
+
+This numeric field defines the minimum outdoor dry-bulb temperature in degrees Celsius for PTHP compressor operation. The compressor will not operate (for DX heating or DX cooling) when outdoor dry-bulb temperatures fall below this value. The minimum value must be greater than or equal to -20 °C. If this field is left blank, the default value is -8°C. This temperature should match the minimum compressor operating temperature specified for the heat pump's DX heating coil (if they don't match, the highest of the two temperatures will be the cut-off temperature for compressor operation).
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-4-000}
+
+This alpha field defines the type of DX cooling coil used by this PTHP. The input requirements for these DX cooling coil objects are described elsewhere in this document. Only allowable coil types are:
+
+\begin{itemize}
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted
+\item
+  Coil:Cooling:DX:VariableSpeed
+\end{itemize}
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-3-000}
+
+This alpha field defines the name of the cooling coil used by this PTHP, and this name should match the name specified in the corresponding DX cooling coil object.
+
+\paragraph{Field: Cooling Convergence Tolerance}\label{field-cooling-convergence-tolerance-3}
+
+This numeric field defines the convergence tolerance for the unit's cooling output. This field allows the user some control over how closely the heat pump will control the air-side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in zone air temperature. Initial experience with this parameter lends to the recommendation of using 0.001 as the starting point.
+
+The heat pump is controlled by matching its sensible (temperature) cooling output to the zone sensible load (demand). Because the performance of the DX cooling coil is frequently non-linear, the heat pump model must call the DX cooling coil model several times (iterate) to determine the proper run time fraction to meet the zone load. The cooling convergence tolerance is the error tolerance used to terminate the iteration procedure when the following equation is satisfied:
+
+\begin{equation}
+\frac{{\left| {({Q_{ZoneLoad}} - {Q_{HeatPump,out}})} \right|}}{{{Q_{ZoneLoad}}}}\,\, \le \,\,Cooling{\kern 1pt} Convergence{\kern 1pt} Tolerance
+\end{equation}
+
+The maximum number of iterations is limited, with a warning message generated if the above equation is not satisfied within the maximum number of iterations.
+
+\paragraph{Field: Supplemental Heating Coil Object Type}\label{field-supplemental-heating-coil-object-type-000}
+
+This alpha field defines the type of supplemental heating coil to be used by this PTHP. The input requirements for these heating coil objects are described elsewhere in this document. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the supplemental heating coil does not require additional controller or Controller:WaterCoil object. The parent object (PTHP) itself provides the ``controller'' function of modulating water flow. Allowable coil types are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Supplemental Heating Coil Name}\label{field-supplemental-heating-coil-name-000}
+
+This alpha field defines the name of the supplemental heating coil used by this PTHP, and this name should match the name specified in the corresponding heating coil object.
+
+\paragraph{Field: Maximum Supply Air Temperature from Supplemental Heater}\label{field-maximum-supply-air-temperature-from-supplemental-heater-000}
+
+This numeric field defines the maximum supply air temperature in degrees Celsius exiting the heat pump supplemental heater coil. The supplemental heater will be controlled so that its supply air temperature does not exceed this value. This field is autosizable.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-supplemental-heater-operation-000}
+
+This numeric field defines the maximum outdoor dry-bulb temperature in degrees Celsius for PTHP supplemental heater operation. The supplemental heater will not operate when the outdoor dry-bulb temperature is above this value. The maximum value must be less than or equal to 21°C. If this field is left blank, the default value is 21°C.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-4-000}
+
+This alpha field has two choices: \textbf{BlowThough} or \textbf{DrawThrough}. The first choice stands for ``blow through fan''. This means that the unit consists of an outdoor air mixer followed by a fan followed by the DX coils and supplemental heating coil. The fan ``blows through'' the cooling and heating coils. The second choice stands for ``draw through fan''. This means that the unit consists of an outdoor air mixer followed by the DX coil(s) followed by a fan, with the supplemental heater located at the outlet of the fan. The fan ``draws air through'' the DX coil(s). If this field is left blank, the default is draw through.
+
+Note: the packaged terminal heat pump's supply air fan, cooling coil, heating coil and supplementary heating coil must be connected according to the configuration shown above (Figure~\ref{fig:schematic-of-a-packaged-terminal-heat-pump-001}) for the draw through fan configuration. The only other valid configuration is with a blow through fan placement, where the fan is located between the outdoor air mixer and the DX cooling coil.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-5}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply air fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, the model assumes the supply air fan cycles with the heating or cooling coil throughout the simulation.
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-7}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this packaged terminal heat pump or object's fan. If the packaged terminal heat pump is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this packaged terminal heat pump object should be on or off.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name-7}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Cooling Supply Air Flow Rate in this PTHP zone HVAC object. The scaled Supply Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
+
+As shown in the example below, correct specification of the packaged terminal heat pump requires the following objects in addition to the compound object itself:
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  Fan (Fan:OnOff or Fan:ConstantVolume)
+\item
+  DX cooling coil (Coil:Cooling:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted)
+\item
+  DX heating coil (Coil:Heating:DX:SingleSpeed)
+\item
+  Supplemental heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
+\item
+  OutdoorAir:Mixer
+\end{enumerate}
+
+\begin{lstlisting}
+
+ZoneHVAC:PackagedTerminalHeatPump,
+  Zone2PTHP,               !- Name
+  FanAndCoilAvailSched,    !- Availability Schedule Name
+  Zone2PTHPAirInletNode,   !- Air Inlet Node Name
+  Zone2PTHPAirOutletNode,  !- Air Outlet Node Name
+  OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type
+  Zone2PTHPOAMixer,        !- Outdoor Air Mixer Name
+  autosize,                !- Cooling Supply Air Flow Rate {m3/s}
+  autosize,                !- Heating Supply Air Flow Rate {m3/s}
+  autosize,                !- No Load Supply Air Flow Rate {m3/s}
+  autosize,                !- Cooling Outdoor Air Flow Rate {m3/s}
+  autosize,                !- Heating Outdoor Air Flow Rate {m3/s}
+  autosize,                !- No Load Outdoor Air Flow Rate {m3/s}
+  Fan:OnOff,               !- Supply Air Fan Object Type
+  Zone2PTHPFan,            !- Supply Air Fan Name
+  Coil:Heating:DX:SingleSpeed,  !- Heating Coil Object Type
+  Zone2PTHPDXHeatCoil,     !- Heating Coil Name
+  0.001,                   !- Heating Convergence Tolerance {dimensionless}
+  2.0,                     !- Minimum Outdoor Dry-Bulb Temperature for Compressor Operation {C}
+  Coil:Cooling:DX:SingleSpeed,  !- Cooling Coil Object Type
+  Zone2PTHPDXCoolCoil,     !- Cooling Coil Name
+  0.001,                   !- Cooling Convergence Tolerance {dimensionless}
+  Coil:Heating:Electric,   !- Supplemental Heating Coil Object Type
+  Zone2PTHPSupHeater,      !- Supplemental Heating Coil Name
+  autosize,                !- Maximum Supply Air Temperature from Supplemental Heater {C}
+  10.0,                    !- Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation {C}
+  BlowThrough,             !- Fan Placement
+  CyclingFanSch;           !- Supply Air Fan Operating Mode Schedule Name
+
+
+  Schedule:Compact,
+      CyclingFanSch,               !- Name
+      Fraction,                    !- ScheduleType
+      Through: 12/31,              !- Complex Field \#1
+      For: AllDays,                !- Complex Field \#2
+      Until: 24:00,                !- Complex Field \#7
+      0.0;                         !- Complex Field \#8
+
+  OutdoorAir:Mixer,
+      Zone2PTHPOAMixer,            !- Name
+      Zone2PTHPOAMixerOutletNode,  !-Mixed Air Node Name
+      Zone2PTHPOAInNode,           !-Outdoor Air Stream Node Name
+      Zone2PTHPExhNode,            !- Relief Air Stream Node Name
+      Zone2PTHPAirInletNode;       !- Return Air Stream Node Name
+
+  Fan:OnOff,
+      Zone2PTHPFan,                !- Name
+      FanAndCoilAvailSched,        !- Availability Schedule Name
+      0.5,                         !- Fan Total Efficiency
+      75.0,                        !- Pressure Rise {Pa}
+      autosize,                    !- Maximum Flow Rate {m3/s}
+      0.9,                         !- Motor Efficiency
+      1.0,                         !- Motor In Airstream Fraction
+      Zone2PTHPOAMixerOutletNode,  !- Air Inlet Node Name
+      Zone2PTHPFanOutletNode;      !- Air Outlet Node Name
+
+  Coil:Cooling:DX:SingleSpeed,
+      Zone2PTHPDXCoolCoil,         !- Coil Name
+      CoolingCoilAvailSched,       !- Availability Schedule
+      autosize,                    !- Rated Total Cooling Capacity (gross) {W}
+      autosize,                    !- Rated SHR
+      3.0,                         !- Rated COP
+      autosize,                    !- Rated Air Volume Flow Rate {m3/s}
+      Zone2PTHPFanOutletNode,      !- Coil Air Inlet Node
+      Zone2PTHPCoolCoilOutletNode, !- Coil Air Outlet Node
+      HPACCoolCapFT,               !- Total Cooling Capacity Modifier Curve (function of temperature)
+      HPACCoolCapFFF,              !- Total Cooling Capacity Modifier Curve (function of flow fraction)
+      HPACEIRFT,                   !- Energy Input Ratio Modifier Curve (function of temperature)
+      HPACEIRFFF,                  !- Energy Input Ratio Modifier Curve (function of flow fraction)
+      HPACPLFFPLR;                 !- Part Load Fraction Correlation (function of part load ratio)
+
+  COIL:Heating:DX:SingleSpeed,
+      Zone2PTHPDXHeatCoil,         !- Coil Name
+      HeatingCoilAvailSched,       !- Availability Schedule
+      autosize,                    !- Rated Total Heating Capacity {W}
+      2.75,                        !- Rated COP
+      autosize,                    !- Rated Air Volume Flow Rate {m3/s}
+      Zone2PTHPCoolCoilOutletNode, !- Coil Air Inlet Node
+      Zone2PTHPDXHeatCoilOutletNode, !- Coil Air Outlet Node
+      HPACHeatCapFT,              !- Total heating capacity modifier curve (function of temperature)
+      HPACHeatCapFFF,             !- Total heating capacity modifier curve (function of flow fraction)
+      HPACHeatEIRFT,              !- Energy input ratio modifier curve (function of temperature)
+      HPACHeatEIRFFF,             !- Energy input ratio modifier curve (function of flow fraction)
+      HPACCOOLPLFFPLR,            !- Part load fraction correlation (function of part load ratio)
+      ,                           !- Defrost energy input ratio modifier curve (function of temperature)
+      2.0,                        !- Minimum Outdoor Dry-bulb Temperature for Compressor Operation {C}
+      5.0,                        !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation {C}
+      200.0,                      !- Crankcase Heater Capacity {W}
+      10.0,                       !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
+      Resistive,                  !- Defrost Strategy
+      TIMED,                      !- Defrost Control
+      0.166667,                   !- Defrost Time Period Fraction
+      20000;                      !- Resistive Defrost Heater Capacity {W}
+
+  Coil:Heating:Electric,
+      Zone2PTHPSupHeater,          !- Name
+      HeatingCoilAvailSched,       !- Availability Schedule Name
+      1.0,                         !- Efficiency
+      autosize,                    !- Nominal Capacity {W}
+      Zone2PTHPDXHeatCoilOutletNode, !- Air Inlet Node Name
+      Zone2PTHPAirOutletNode;      !- Air Outlet Node Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-8-009}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Packaged Terminal Heat Pump Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Heat Pump Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Heat Pump Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Heat Pump Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Heat Pump Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Heat Pump Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Heat Pump Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Heat Pump Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Heat Pump Latent Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Heat Pump Latent Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Heat Pump Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Heat Pump Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Heat Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Zone Packaged Terminal Heat Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone Packaged Terminal Heat Pump Fan Part Load Ratio {[]}
+\item
+  HVAC,Average,Zone Packaged Terminal Heat Pump Compressor Part Load Ratio {[]}
+\item
+  HVAC,Average,Zone Packaged Terminal Heat Pump Fan Availability Status {[]}
+\end{itemize}
+
+\paragraph{Zone Packaged Terminal Heat Pump Total Heating Rate {[}W{]}}\label{zone-packaged-terminal-heat-pump-total-heating-rate-w}
+
+This output field is the total (enthalpy) heat addition rate of the packaged terminal heat pump to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Total Heating Energy {[}J{]}}\label{zone-packaged-terminal-heat-pump-total-heating-energy-j}
+
+This output field is the total (enthalpy) heat addition of the packaged terminal heat pump to the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, the air mass flow rate through the heat pump, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Total Cooling Rate {[}W{]}}\label{zone-packaged-terminal-heat-pump-total-cooling-rate-w}
+
+This output field is the total (enthalpy) heat extraction rate of the packaged terminal heat pump from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Total Cooling Energy {[}J{]}}\label{zone-packaged-terminal-heat-pump-total-cooling-energy-j}
+
+This output field is the total (enthalpy) heat extraction of the packaged terminal heat pump from the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, the air mass flow rate through the heat pump, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Sensible Heating Rate {[}W{]}}\label{zone-packaged-terminal-heat-pump-sensible-heating-rate-w}
+
+This output field is the sensible heat addition rate of the packaged terminal heat pump to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Sensible Heating Energy {[}J{]}}\label{zone-packaged-terminal-heat-pump-sensible-heating-energy-j}
+
+This output field is the sensible heat addition of the packaged terminal heat pump to the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the heat pump, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Sensible Cooling Rate {[}W{]}}\label{zone-packaged-terminal-heat-pump-sensible-cooling-rate-w}
+
+This output field reports the moist air sensible heat extraction rate of the packaged terminal heat pump from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Sensible Cooling Energy {[}J{]}}\label{zone-packaged-terminal-heat-pump-sensible-cooling-energy-j}
+
+This output field reports the moist air sensible heat extraction of the packaged terminal heat pump from the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the heat pump, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Latent Heating Rate {[}W{]}}\label{zone-packaged-terminal-heat-pump-latent-heating-rate-w}
+
+This output field is the latent heat addition (humidification) rate of the packaged terminal heat pump to the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the packaged terminal heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Latent Heating Energy {[}J{]}}\label{zone-packaged-terminal-heat-pump-latent-heating-energy-j}
+
+This output field is the latent heat addition (humidification) of the packaged terminal heat pump to the zone it is serving in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the packaged terminal heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Latent Cooling Rate {[}W{]}}\label{zone-packaged-terminal-heat-pump-latent-cooling-rate-w}
+
+This output field is the latent heat extraction (dehumidification) rate of the packaged terminal heat pump from the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the packaged terminal heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Latent Cooling Energy {[}J{]}}\label{zone-packaged-terminal-heat-pump-latent-cooling-energy-j}
+
+This output field is the latent heat extraction (dehumidification) of the packaged terminal heat pump from the zone it is serving in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the packaged terminal heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are summed for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Electric Power {[}W{]}}\label{zone-packaged-terminal-heat-pump-electric-power-w}
+
+This output field is the electricity consumption rate of the packaged terminal heat pump in Watts. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{Zone Packaged Terminal Heat Pump Electric Energy {[}J{]}}\label{zone-packaged-terminal-heat-pump-electric-energy-j}
+
+This output field is the electricity consumption of the packaged terminal heat pump in Joules for the time period being reported. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are summed for the timestep being reported.
+
+\paragraph{\texorpdfstring{Zone Packaged Terminal Heat Pump Fan Part Load Ratio {[]}}{Zone Packaged Terminal Heat Pump Fan Part Load Ratio }}\label{zone-packaged-terminal-heat-pump-fan-part-load-ratio}
+
+This output field is the part-load ratio of the fan. The fan part-load ratio is defined as the average supply air mass flow rate divided by the maximum supply air mass flow rate. The maximum supply air mass flow rate depends on whether heating, cooling, or no heating or cooling is required during the timestep. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{\texorpdfstring{Zone Packaged Terminal Heat Pump Compressor Part Load Ratio {[]}}{Zone Packaged Terminal Heat Pump Compressor Part Load Ratio }}\label{zone-packaged-terminal-heat-pump-compressor-part-load-ratio}
+
+This output field is the part-load ratio of the compressor used by the DX coils (cooling and heating). Compressor part-load ratio is defined as the total coil load divided by the coil steady-state capacity. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
+
+\paragraph{\texorpdfstring{Zone Packaged Terminal Heat Pump Fan Availability Status {[]}}{Zone Packaged Terminal Heat Pump Fan Availability Status }}\label{zone-packaged-terminal-heat-pump-fan-availability-status}
+
+This is the availability status of the packaged terminal heat pump~ fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the packaged terminal heat pump~ object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\subsection{ZoneHVAC:RefrigerationChillerSet}\label{zonehvacrefrigerationchillerset}
+
+The ZoneHVAC:RefrigerationChillerSet object works in conjunction with one or multiple air chillers, compressor racks, refrigeration systems, or refrigeration secondary system objects (Ref. Refrigeration:AirChiller Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem) to simulate the performance of a group of air chillers cooling a single zone. The chiller set model passes information about the zone conditions to determine the performance of individual chiller coils within the set, thus providing the sensible and latent heat exchange with the zone environment.
+
+The refrigeration chiller set object inputs include a name, an availability schedule name, the name of the zone cooled by the chiller set, the air inlet node name, the air outlet node name, and an extensible list of air chiller names (Ref. Refrigeration:AirChiller).
+
+\subsubsection{Inputs}\label{inputs-10-024}
+
+\paragraph{Field: Name}\label{field-name-10-020}
+
+A unique user-assigned name for an instance of a refrigeration chiller. Any reference to this refrigeration chiller by another object (may be listed in a Refrigeration:CaseAndWalkInList, Refrigeration:System, Refrigeration:SecondarySystem, or Refrigeration:CompressorRack) will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-9-002}
+
+The name of the schedule (ref: Schedule) that denotes whether the refrigeration chiller can operate during a given time period. A schedule value greater than 0 (maximum schedule value of 1.0 is typically used) indicates that the refrigeration chiller will operate during a given time period. A value equal to 0 denotes that the case does not operate (everything is OFF: refrigeration, fans, lights, anti-sweat, etc.). Typically the refrigeration chiller will operate throughout the day (i.e., the schedule will contain 1 for all time periods); however, refrigeration chillers require maintenance and/or cleaning and this can be modeled accordingly using this schedule if desired. If this field is left blank, the default schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Zone Name}\label{field-zone-name-1-011}
+
+A unique user-assigned name for the zone cooled by this refrigeration chiller. This zone must represent a conditioned space, that is, it must appear in a ZoneHVAC:EquipmentConnections object.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-7-000}
+
+Not used, reserved for future use.~ Current version exchanges energy directly with the zone, external of any air system. (Future: The name of the zone exhaust node (see Node) from which the refrigeration chiller draws its indoor air. This should be one of the zone exhaust nodes for the zone cooled by the chiller set.)
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-7-001}
+
+Not used, reserved for future use.~ Current version exchanges energy directly with the zone, external of any air system. (Future: The name of the node where the chiller coil sends its outlet air, which must be one of the inlet air nodes for the zone which is being cooled.)
+
+\paragraph{Field: Air Chiller \#1 ~Name}\label{field-air-chiller-1-name}
+
+The name of the first air chiller that will be used to meet the zone cooling load.
+
+\paragraph{Field: Air Chiller \#2 ~Name}\label{field-air-chiller-2-name}
+
+The name of the second air chiller that will be used to meet the zone cooling load.
+
+\paragraph{Field: Air Chiller \#3 ~Name}\label{field-air-chiller-3-name}
+
+The name of the third air chiller that will be used to meet the zone cooling load.
+
+\paragraph{Field: Air Chiller \#n ~Name (Extensible list, 20 provided in the IDD)}\label{field-air-chiller-n-name-extensible-list-20-provided-in-the-idd}
+
+The name of the nth air chiller that will be used to meet the zone cooling load.
+
+The following is an example input for a refrigeration chiller set.
+
+\begin{lstlisting}
+
+   ZoneHVAC:RefrigerationChillerSet,
+      SubFreezerChillerSet ,     !- Name
+      ,                         !- Availability Schedule Name
+      SubFreezer,                !- Zone Name
+      NODE_142,                   !- Air Inlet Node Name
+      NODE_141,                   !- Air Outlet Node Name
+      SubFreezerAirChiller_1,    !- Air Chiller \#1 Name
+      SubFreezerAirChiller_2,    !- Air Chiller \#2 Name
+      SubFreezerAirChiller_3;    !- Air Chiller \#3 Name
+\end{lstlisting}
+
+There are no outputs variables for a ZoneHVAC:RefrigerationChillerSet. Outputs for the refrigeration impact on any zone are listed in the Group:Refrigeration.
+
+\subsection{ZoneHVAC:WaterToAirHeatPump}\label{zonehvacwatertoairheatpump}
+
+The zone water-to-air heat pump is a compound component consisting of a fan, water-to-air cooling and heating coils, and a supplemental heating coil. Links to the fan, WaterToAirHeatPump cooling coil, WaterToAirHeatPump heating coil, and supplementary heating coil specifications are provided in the heat pump's input data syntax. The heat pump switches between cooling and heating depending on the zone's demand. The load side (air) of the zone water-to-air heat pump consists of an On/Off fan component, a WaterToAirHeatPump cooling coil component, a WaterToAirHeatPump heating coil component, and a Gas or Electric supplemental heating coil component. The source side (water) of the heat pump is connected to a condenser loop with a heat exchanger (ground heat exchanger or other type) or a plant loop with a heating source such as a boiler and a cooling source such as a chiller or cooling tower.~ The diagram below shows the setup and connection of the heat pump for the source side and load side for a ground heat exchanger configuration. Note that on the load side, the WaterToAirHeatPump cooling coil must always be placed before the WaterToAirHeatPump heating coil.
+
+For this zone heat pump,there are two types of WaterToAirHeatPump coil model allowed:
+
+\begin{itemize}
+\item
+  Coil:Cooling:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Heating:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit
+\item
+  Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit
+\end{itemize}
+
+\begin{figure}[hbtp] % fig 113
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image288.png}
+\caption{Zone Water to Air Heat Pump Schematic for a DrawThrough Configuration with Ground Heat Exchanger \protect \label{fig:zone-water-to-air-heat-pump-schematic-for-a}}
+\end{figure}
+
+\subsubsection{Inputs}\label{inputs-11-023}
+
+\paragraph{Field: Name}\label{field-name-11-017}
+
+This alpha field contains the identifying name for the zone system heat pump.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-10-001}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump operates during a given time period. A schedule value equal to 0 denotes that the heat pump must be off for that time period. A value greater than 0 denotes that the heat pump is available to operate during that time period. This schedule may be used to completely disable the heat pump (all of its coils and the supply air fan) as required. If this field is blank, the schedule has values of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-8-000}
+
+This alpha field contains the name of the HVAC system node from which the heat pump draws its inlet air. This node must be a zone exhaust node as specified in a ZoneHVAC:EquipmentConnections object.
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-8-001}
+
+This alpha field contains the name of the HVAC system node to which the heat pump sends its outlet air. This node must be a zone inlet node as specified in a ZoneHVAC:EquipmentConnections object.
+
+\paragraph{Field: Outdoor Air Mixer Object Type}\label{field-outdoor-air-mixer-object-type-4}
+
+This field specifies the type of outdoor air mixer used by this WaterToAirHeatPump unit. The outdoor air mixer component is part of the WaterToAirHeatPump compound object. The only available outdoor air mixer type is:
+
+\begin{itemize}
+\tightlist
+\item
+  OutdoorAir:Mixer
+\end{itemize}
+
+\paragraph{Field: Outdoor Air Mixer Name}\label{field-outdoor-air-mixer-name-4}
+
+This alpha field defines the name of an outdoor air mixer component which composes part of the zone WaterToAirHeatPump. The return air stream node of the outdoor air mixer should also be the same node as the air inlet node of the WaterToAirHeatPump. Furthermore, the outdoor air mixer's mixed air node should be the same as the WaterToAirHeatPump's fan inlet air node (for blow through fan placement) or the WaterToAirHeatPump's cooling coil inlet node (for draw through fan placement).
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-2-001}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-2-001}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than 0 or this field is autosizable.
+
+\paragraph{Field: No Load Supply Air Flow Rate}\label{field-no-load-supply-air-flow-rate-2-001}
+
+This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the heat pump's supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the heat pump's supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).
+
+\paragraph{Field: Cooling Outdoor Air Flow Rate}\label{field-cooling-outdoor-air-flow-rate-2}
+
+This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when the DX cooling coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the outside air flow rate during cooling operation is fixed; it cannot change during the simulation. In addition, the outside air flow rate during cooling operation cannot be greater than the heat pump's supply air flow rate during cooling operation.
+
+\paragraph{Field: Heating Outdoor Air Flow Rate}\label{field-heating-outdoor-air-flow-rate-2}
+
+This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the outside air flow rate during heating operation is fixed; it cannot change during the simulation. In addition, the outside air flow rate during heating operation cannot be greater than the heat pump's supply air flow rate during heating operation.
+
+\paragraph{Field: No Load Outdoor Air Flow Rate When No Cooling or Heating is Needed}\label{field-no-load-outdoor-air-flow-rate-when-no-cooling-or-heating-is-needed-000}
+
+This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). Values must be greater than or equal to 0, or this field is autosizable. Note that the no load outdoor air flow rate cannot change during the simulation. In addition, the no load outdoor air flow rate cannot be greater than the heat pump's no load supply air flow rate. This field is only used when the heat pump's supply air fan operating mode schedule specifies continuous fan operation. If the heat pump's supply air fan operating mode schedule specifies continuous fan operation and the field ``No Load Supply Air Flow Rate'' is set to zero or is left blank, then the model assumes that the no load outdoor air flow rate is equal to the outdoor air flow rate when the cooling or heating coil was last operating (for cooling operation {[}i.e., Cooling outdoor air flow rate{]} or heating operation {[}i.e., Heating outdoor air flow rate{]}) and this field is not used.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-7}
+
+This alpha field contains the identifying type of supply air fan specified in the heat pump. Fan type must be Fan:OnOff.
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-6}
+
+This alpha field contains the identifying name given to the heat pump supply air fan, and should match the name specified in the corresponding fan object.
+
+\paragraph{Field: Heating Coil Object Type}\label{field-heating-coil-object-type-5-000}
+
+This alpha field contains the identifying type of heating coil specified in the heat pump. The only valid types are Coil:Heating:WaterToAirHeatPump:EquationFit Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit..
+
+\paragraph{Field: Heating Coil Name}\label{field-heating-coil-name-5-000}
+
+This alpha field contains the identifying name given to the WaterToAirHeatPump heating coil, and should match the name specified in the corresponding WaterToAirHeatPump heating coil object.
+
+\paragraph{Field: Cooling Coil Object Type}\label{field-cooling-coil-object-type-5-000}
+
+This alpha field contains the identifying type of cooling coil specified in the heat pump. The only valid types are Coil:Cooling:WaterToAirHeatPump:EquationFit and Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit.
+
+\paragraph{Field: Cooling Coil Name}\label{field-cooling-coil-name-4-000}
+
+This alpha field contains the identifying name given to the WaterToAirHeatPump cooling coil, and should match the name specified in the corresponding WaterToAirHeatPump cooling coil object.
+
+\paragraph{Field: Maximum Cycling Rate}\label{field-maximum-cycling-rate-002}
+
+This numeric field contains the maximum on-off cycling rate for the compressor, which occurs at 50\% run time fraction. Suggested values are shown below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image289.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Heat Pump Time Constant}\label{field-heat-pump-time-constant-001}
+
+This numeric field contains the time constant for the cooling coil's capacity to reach steady state after startup. Suggested values are shown below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image290.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Fraction of On-Cycle Power Use}\label{field-fraction-of-on-cycle-power-use-001}
+
+This numeric field contains the fraction of on-cycle power use to adjust the part load fraction based on the off-cycle power consumption due to crankcase heaters, controls, fans, and etc. Suggested value values are below (Henderson et al. 1999):
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image291.png}
+\caption{}
+\end{figure}
+
+\paragraph{Field: Heat Pump Fan Delay Time}\label{field-heat-pump-fan-delay-time-001}
+
+This numeric field contains the time delay in seconds for the heat pump supply air fan to shut off after compressor cycle off. This value can be obtained from the manufacturer or the heat pump catalog. Suggested value is 60 seconds. This value is disregared at times when the WaterToAirHeatPump's fan operating mode schedule value is greater than 0 (i.e., continuous fan mode).
+
+\paragraph{Field: Supplemental Heating Coil Object Type}\label{field-supplemental-heating-coil-object-type-1-000}
+
+This is the object type of the supplemental heating coil. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the supplemental heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Zone Water to Air Heat Pump) itself provides the ``controller'' function of modulating water flow. The valid choices are:
+
+\begin{itemize}
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\end{itemize}
+
+\paragraph{Field: Supplemental Heating Coil Name}\label{field-supplemental-heating-coil-name-1-000}
+
+This alpha field contains the identifying name given to the supplemental heating coil, and should match the name specified in the corresponding supplemental heating coil object.
+
+\paragraph{Field: Maximum Supply Air Temperature from Supplemental Heater}\label{field-maximum-supply-air-temperature-from-supplemental-heater-1-000}
+
+This numeric field defines the maximum allowed supply air temperature exiting the heat pump supplemental heating coil in degrees Celsius.
+
+\paragraph{Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation}\label{field-maximum-outdoor-dry-bulb-temperature-for-supplemental-heater-operation-1-000}
+
+This numeric field defines the outdoor air dry-bulb temperature in degrees Celsius above which the heat pump supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21°C. If this input field is left blank, the default value is 21°C.
+
+\paragraph{Field: Outdoor Dry-Bulb Temperature Sensor Node Name}\label{field-outdoor-dry-bulb-temperature-sensor-node-name-000}
+
+This alpha field specifies the name of the outdoor node which controls the operation of the supplemental heating coil. If this field is left blank, the outdoor temperature is based solely on the weather data. If this field is not blank, the node name specified must also be listed in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor temperature from the weather data. Alternately, the node name must be specified in an OutdoorAir:NodeList object where the outdoor temperature is taken directly from the weather data.
+
+\paragraph{Field: Fan Placement}\label{field-fan-placement-5-000}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. The first choice represents a blow through system where the supply air fan is before the WaterToAirHeatPump cooling/heating coil and the supplementary heating coil. The second choice represents a draw through system where the supply fan is between the WaterToAirHeatPump cooling/heating coil and the supplementary heating coil. If this input field is left blank, the default is blow through.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-6}
+
+This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply air fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, the model assumes the supply air fan cycles with the heating or cooling coil throughout the simulation.
+
+As shown in the example below, correct specifications of the WatertoAirHeatPump requires specification of the following objects in addition to the ZoneHVAC:WaterToAirHeatPump object:
+
+\begin{itemize}
+\item
+  On/Off fan
+\item
+  WatertoAirHeatPump cooling coil (EquationFit only)
+\item
+  WatertoAirHeatPump heating coil (EquationFit only)
+\item
+  Supplementary heating coil
+\item
+  Outdoor air mixer
+\item
+  Condenser loop or plant loop demand branches
+\end{itemize}
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-8}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this WatertoAirHeatPump or object's fan. If the WatertoAirHeatPump is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this WatertoAirHeatPump object should be on or off.
+
+\paragraph{Field: Heat Pump Coil Water Flow Mode}\label{field-heat-pump-coil-water-flow-mode-001}
+
+This field specifies the way in which water flow through the heat pump coils will be modeled.~ This field is only used when WatertoAirHeatPump:EquationFit coils are used. There are three options:
+
+\begin{itemize}
+\item
+  Cycling
+\item
+  Constant
+\item
+  CyclingOnDemand
+\end{itemize}
+
+\textbf{Cycling} varies water flow through the coil based on the heat pump Part Load Ratio. This control method is appropriate for modeling heat pumps that are outfitted with a soleniod valve which allows water to flow through the coil only when the compressor is active. This is the default for EnergyPlus V8 and later.
+
+\textbf{Constant} provides a constant water flow regardless of heat pump operation. Remember that EnergyPlus has two coils (a heating coil and a cooling coil) to approximate the operation of one coil that can operate in either heating mode or cooling mode. Therefore, when the water flow mode is constant, there will be full flow through either the heating coil or the cooling coil, but not both at the same time.
+
+\textbf{ConstantOnDemand} provides full flow through the coil whenever there is a load. When there is no load, there is zero flow through the coil.~ This control strategy represents the way EnergyPlus modeled heat pump water flow prior to Version 8.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name-8}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Cooling Supply Air Flow Rate in this Water To Air Heat Pump zone HVAC object. The scaled Supply Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
+
+Examples of IDF use:
+
+\begin{lstlisting}
+
+ZoneHVAC:WaterToAirHeatPump,
+  Zone1WTAHP,               !- Name
+  FanAndCoilAvailSched,     !- Availability Schedule Name
+  Zone 1 Outlet Node,       !- Air Inlet Node Name
+  Zone 1 Inlet Node,        !- Air Outlet Node Name
+  OutdoorAir:Mixer,         !- Outdoor air mixer object type
+  Zone 1 Mixer,             !- Outdoor Air Mixer Name
+  Autosize,                 !- Cooling Supply Air Flow Rate {m3/s}
+  Autosize,                 !- Heating Supply Air Flow Rate {m3/s}
+  ,                         !- No Load Supply Air Flow Rate {m3/s}
+  0.0,                      !- Cooling Outdoor Air Flow Rate {m3/s}
+  0.0,                      !- Heating Outdoor Air Flow Rate {m3/s}
+  ,                         !- No Load Outdoor Air Flow Rate {m3/s}
+  Fan:OnOff,                !- Supply Air Fan Object Type
+  Zone 1 Fan,               !- Supply Air Fan Name
+  Coil:Heating:WaterToAirHeatPump:EquationFit,  !- Heating Coil Object Type
+  Sys 1 Heat Pump Heating Mode,  !- Heating Coil Name
+  Coil:Cooling:WaterToAirHeatPump:EquationFit, !- Cooling Coil Object Type
+  Sys 1 Heat Pump Cooling Mode, !- Cooling Coil Name
+  2.5,                      !- Maximum Cycling Rate
+  60.0,                     !- Heat Pump Time Constant
+  0.01,                     !- Fraction of On-Cycle Power Use
+  60,                       !- Heat Pump Fan Delay Time
+  Coil:Heating:Gas,         !- Supplemental Heating Coil Object Type
+  Heat Pump DX Supp Heating Coil 1, !- Supplemental Heating Coil Name
+  60.0,                  !- Maximum Supply Air Temperature from Supplemental Heater {C}
+  20.0,                  !- Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation {C}
+  Sys 1 Outside Air Inlet Node, !- Outdoor Dry-Bulb Temperature Sensor Node Name
+  BlowThrough,              !- Fan Placement
+  CyclingFanSch;            !- Supply Air Fan Operating Mode Schedule Name
+
+  Schedule:Compact,
+      CyclingFanSch,           !- Name
+      Fraction,                !- Schedule Type Limits Name
+      Through: 12/31,          !- Field 1
+      For: AllDays,            !- Field 2
+      Until: 24:00,            !- Field 3
+      0.0;                     !- Field 4
+
+    Coil:Heating:WaterToAirHeatPump:EquationFit,
+      Sys 1 Heat Pump Heating Mode,  !- Name
+      Sys 1 Water to Air Heat Pump Source Side2 Inlet Node,   !- Water Inlet Node Name
+      Sys 1 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
+      Sys 1 Heating Coil Air Inlet Node,      !- Air Inlet Node Name
+      Sys 1 SuppHeating Coil Air Inlet Node,  !- Air Outlet Node Name
+      Autosize,                !- Rated Air Flow Rate {m3/s}
+      Autosize,                !- Rated Water Flow Rate {m3/s}
+      Autosize,                !- Rated Heating Capacity {W}
+      4.75,                    !- Rated Heating Coefficient of Performance
+      -1.361311959,            !- Heating Capacity Coefficient 1
+      -2.471798046,            !- Heating Capacity Coefficient 2
+      4.173164514,             !- Heating Capacity Coefficient 3
+      0.640757401,             !- Heating Capacity Coefficient 4
+      0.0,                     !- Heating Capacity Coefficient 5
+      -2.176941116,            !- Heating Power Consumption Coefficient 1
+      0.832114286,             !- Heating Power Consumption Coefficient 2
+      1.570743399,             !- Heating Power Consumption Coefficient 3
+      0.690793651,             !- Heating Power Consumption Coefficient 4
+      0.0;                     !- Heating Power Consumption Coefficient 5
+
+    OutdoorAir:Mixer,
+      Zone 1 Mixer,          !- Name
+      Sys 1 Mixed Air Node,  !- Mixed Air Node Name
+      Sys 1 Outside Air Inlet Node,  !- Outdoor Air Stream Node Name
+      Sys 1 Relief Air Outlet Node,  !- Relief Air Stream Node Name
+      Zone 1 Outlet Node;  !- Return Air Stream Node Name
+
+    Fan:OnOff,
+      Zone 1 Fan,              !- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      0.7,                     !- Fan Total Efficiency
+      300.0,                   !- Pressure Rise {Pa}
+      Autosize,                !- Maximum Flow Rate {m3/s}
+      0.9,                     !- Motor Efficiency
+      1.0,                     !- Motor In Airstream Fraction
+      Sys 1 Mixed Air Node,    !- Air Inlet Node Name
+      Sys 1 Cooling Coil Air Inlet Node;  !- Air Outlet Node Name
+
+    Coil:Heating:Gas,
+      Heat Pump DX Supp Heating Coil 1,  !- Name
+      FanAndCoilAvailSched,    !- Availability Schedule Name
+      0.8,                     !- Gas Burner Efficiency
+      32000,                   !- Nominal Capacity {W}
+      Sys 1 SuppHeating Coil Air Inlet Node,  !- Air Inlet Node Name
+      Zone 1 Inlet Node;  !-Air Outlet Node Name
+
+    BRANCH,
+      Gshp Cooling Condenser Branch,  !- Name
+      0,  !- Maximum Flow Rate {m3/s}
+      ,  !- Pressure Drop Curve Name
+      Coil:Cooling:WaterToAirHeatPump:ParameterEstimation,  !- Component 1 Object Type
+      Heat Pump Cooling Mode,  !- Component 1 Name
+      Water to Air Heat Pump Source Side1 Inlet Node,  !- Component 1 Inlet Node Name
+      Water to Air Heat Pump Source Side1 Outlet Node, !- Component 1 Outlet Node Name
+      ACTIVE;  !- Component 1 Branch Control Type
+
+    BRANCH,
+      Gshp Heating Condenser Branch,  !- Name
+      0,  !- Maximum Flow Rate {m3/s}
+      ,  !- Pressure Drop Curve Name
+      Coil:Heating:WaterToAirHeatPump:ParameterEstimation,  !- Component 1 Object Type
+      Heat Pump Heating Mode,  !- Component 1 Name
+      Water to Air Heat Pump Source Side2 Inlet Node,   !- Component 1 Inlet Node Name
+      Water to Air Heat Pump Source Side2 Outlet Node,  !- Component 1 Outlet Node Name
+      ACTIVE;  !- Component 1 Branch Control Type
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-9-009}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Water to Air Heat Pump Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Water to Air Heat Pump Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Water to Air Heat Pump Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Water to Air Heat Pump Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Water to Air Heat Pump Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Water to Air Heat Pump Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Water to Air Heat Pump Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Water to Air Heat Pump Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Water to Air Heat Pump Latent Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Water to Air Heat Pump Latent Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Water to Air Heat Pump Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Water to Air Heat Pump Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Water to Air Heat Pump Electric Power {[}W{]}
+\item
+  HVAC,Sum,Zone Water to Air Heat Pump Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone Water to Air Heat Pump Fan Part Load Ratio {[]}
+\item
+  HVAC,Average,Zone Water to Air Heat Pump Compressor Part Load Ratio {[]}
+\item
+  HVAC,Average,Zone Water to Air Heat Pump Fan Availability Status {[]}
+\end{itemize}
+
+\paragraph{Zone Water to Air Heat Pump Total Heating Rate {[}W{]}}\label{zone-water-to-air-heat-pump-total-heating-rate-w}
+
+This output field is the total (enthalpy) heat addition rate of the Water to Air Heat Pump to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system time step being simulated, and the results (enthalpy addition only) are averaged for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Total Heating Energy {[}J{]}}\label{zone-water-to-air-heat-pump-total-heating-energy-j}
+
+This output field is the total (enthalpy) heat addition of the Water to Air Heat Pump to the zone it is serving in Joules over the time step being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, the air mass flow rate through the heat pump, and the HVAC simulation time step. This value is calculated for each HVAC system time step being simulated, and the results (enthalpy addition only) are summed for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Total Cooling Rate {[}W{]}}\label{zone-water-to-air-heat-pump-total-cooling-rate-w}
+
+This output field is the total (enthalpy) heat extraction rate of the Water to Air Heat Pump from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system time step being simulated, and the results (enthalpy extraction only) are averaged for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Total Cooling Energy {[}J{]}}\label{zone-water-to-air-heat-pump-total-cooling-energy-j}
+
+This output field is the total (enthalpy) heat extraction of the Water to Air Heat Pump from the zone it is serving in Joules over the time step being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, the air mass flow rate through the heat pump, and the HVAC simulation time step. This value is calculated for each HVAC system time step being simulated, and the results (enthalpy extraction only) are summed for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Sensible Heating Rate {[}W{]}}\label{zone-water-to-air-heat-pump-sensible-heating-rate-w}
+
+This output field is the sensible heat addition rate of the Water to Air Heat Pump to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system time step being simulated, and the results (heating only) are averaged for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Sensible Heating Energy {[}J{]}}\label{zone-water-to-air-heat-pump-sensible-heating-energy-j}
+
+This output field is the sensible heat addition of the Water to Air Heat Pump to the zone it is serving in Joules over the time step being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the heat pump, and the HVAC simulation time step. This value is calculated for each HVAC system time step being simulated, and the results (heating only) are summed for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Sensible Cooling Rate {[}W{]}}\label{zone-water-to-air-heat-pump-sensible-cooling-rate-w}
+
+This output field reports the moist air sensible heat extraction rate of the Water to Air Heat Pump from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system time step being simulated, and the results (cooling only) are averaged for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Sensible Cooling Energy {[}J{]}}\label{zone-water-to-air-heat-pump-sensible-cooling-energy-j}
+
+This output field reports the moist air sensible heat extraction of the Water to Air Heat Pump from the zone it is serving in Joules over the time step being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the heat pump, and the HVAC simulation time step. This value is calculated for each HVAC system time step being simulated, and the results (cooling only) are summed for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Latent Heating Rate {[}W{]}}\label{zone-water-to-air-heat-pump-latent-heating-rate-w}
+
+This output field is the latent heat addition (humidification) rate of the Water to Air Heat Pump to the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the WaterToAirHP heat pump. This value is calculated for each HVAC system time step being simulated, and the results (latent heat addition only) are averaged for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Latent Heating Energy {[}J{]}}\label{zone-water-to-air-heat-pump-latent-heating-energy-j}
+
+This output field is the latent heat addition (humidification) of the Water to Air Heat Pump to the zone it is serving in Joules over the time step being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the WaterToAirHP heat pump. This value is calculated for each HVAC system time step being simulated, and the results (latent heat addition only) are summed for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Latent Cooling Rate {[}W{]}}\label{zone-water-to-air-heat-pump-latent-cooling-rate-w}
+
+This output field is the latent heat extraction (dehumidification) rate of the Water to Air Heat Pump from the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the WaterToAirHP heat pump. This value is calculated for each HVAC system time step being simulated, and the results (latent heat extraction only) are averaged for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Latent Cooling Energy {[}J{]}}\label{zone-water-to-air-heat-pump-latent-cooling-energy-j}
+
+This output field is the latent heat extraction (dehumidification) of the Water to Air Heat Pump from the zone it is serving in Joules over the time step being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the WaterToAirHP heat pump. This value is calculated for each HVAC system time step being simulated, and the results (latent heat extraction only) are summed for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Electric Power {[}W{]}}\label{zone-water-to-air-heat-pump-electric-power-w}
+
+This output field is the electricity consumption rate of the Water to Air Heat Pump in Watts. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the supplemental heating coil (if electric). This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{Zone Water to Air Heat Pump Electric Energy {[}J{]}}\label{zone-water-to-air-heat-pump-electric-energy-j}
+
+This output field is the electricity consumption of the Water to Air Heat Pump in Joules for the time period being reported. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the supplemental heating coil (if electric). This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported.
+
+\paragraph{\texorpdfstring{Zone Water to Air Heat Pump Fan Part Load Ratio {[]}}{Zone Water to Air Heat Pump Fan Part Load Ratio }}\label{zone-water-to-air-heat-pump-fan-part-load-ratio}
+
+This output field is the part-load ratio of the fan. The fan part-load ratio is defined as the average supply air mass flow rate divided by the maximum supply air mass flow rate. The maximum supply air mass flow rate depends on whether heating, cooling, or no heating or cooling is required during the time step. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{\texorpdfstring{Zone Water to Air Heat Pump Compressor Part Load Ratio {[]}}{Zone Water to Air Heat Pump Compressor Part Load Ratio }}\label{zone-water-to-air-heat-pump-compressor-part-load-ratio}
+
+This output field is the part-load ratio of the compressor used by the DX coils (cooling and heating). Compressor part-load ratio is defined as the total coil load divided by the coil steady-state capacity. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
+
+\paragraph{\texorpdfstring{Zone Water to Air Heat Pump Fan Availability Status {[]}}{Zone Water to Air Heat Pump Fan Availability Status }}\label{zone-water-to-air-heat-pump-fan-availability-status}
+
+This is the availability status of the zone water source heat pump~ fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the zone water source heat pump~ object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\subsection{ZoneHVAC:Dehumidifier:DX}\label{zonehvacdehumidifierdx}
+
+This object can be used for modeling conventional mechanical dehumidifiers. These systems use a direct expansion (DX) cooling coil to cool and dehumidify an airstream. Heat from the DX system's condenser section is rejected into the cool/dehumidified airstream, resulting in warm dry air being supplied from the unit. In EnergyPlus, this object is modeled as a type of zone equipment (ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
+
+\begin{figure}[hbtp] % fig 114
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image292.png}
+\caption{Schematic of a mechanical dehumidifier \protect \label{fig:schematic-of-a-mechanical-dehumidifier}}
+\end{figure}
+
+The model has inputs for water removal, energy factor and air flow rate at rated conditions (26.7°C, 60\% RH). Curve objects must be specified to describe performance at off-rated conditions. A part-load cycling curve input must also be specified to account for inefficiencies due to cycling. Other inputs including minimum and maximum operating temperatures for dehumidifier operation, off-cycle parasitic load, and an input to direct the removed water to a storage tank.
+
+The model assumes that this equipment dehumidifies and heats the air. If used in tandem with another system that cools and dehumidifies the zone air, then the zone dehumidifier should be specified as the lowest cooling priority in the ZoneHVAC:EquipmentList object for best control of zone temperature and humidity levels (e.g., if there are 3 pieces of equipment in ZoneHVAC:EquipmentList, then the zone dehumidifier should have Cooling Priority = 3). With this zone equipment prioritization, the other cooling and dehumidification system would operate first to meet the temperature setpoint (and possibly meet the high humidity setpoint as well). If additional dehumidification is needed, then the zone dehumidifier would operate. The sensible heat generated by the dehumidifier is carried over to the zone air heat balance for the next HVAC time step.
+
+\subsubsection{Inputs}\label{inputs-12-021}
+
+\paragraph{Field: Name}\label{field-name-12-014}
+
+A unique user-assigned name for an instance of a zone DX dehumidifier unit. Any reference to this dehumidifier by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-11-001}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the dehumidifier operates during a given time period. A schedule value equal to 0 denotes that the dehumidifier will not operate for that time period. A value greater than 0 denotes that the dehumidifier is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Air Inlet Node Name}\label{field-air-inlet-node-name-9-000}
+
+This alpha field defines the name of the HVAC system node from which the dehumidifier draws its inlet air. This node name must be the name of a zone air exhaust node (ref. ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Air Outlet Node Name}\label{field-air-outlet-node-name-9-001}
+
+This alpha field defines the name of the HVAC system node to which the dehumidifier sends its outlet air. This node name must be the name of a zone air inlet node (ref. ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Rated Water Removal}\label{field-rated-water-removal}
+
+This numeric input is the full load water removal rate, in liters per day, at rated conditions (air entering the dehumidifier at 26.7°C {[}80°F{]} dry-bulb and 60\% relative humidity, and air flow rate as defined by field ``Rated Air Flow Rate'' below). This is a required input field and the entered value must be greater than zero.
+
+\paragraph{Field: Rated Energy Factor}\label{field-rated-energy-factor}
+
+This numeric input is the energy factor (liters of water removed per kWh of electricity consumed) at rated conditions (air entering the dehumidifier at 26.7°C {[}80°F{]} dry-bulb and 60\% relative humidity, and air flow rate as defined by field ``Rated Air Flow Rate'' below). This is a required input field and the entered value must be greater than zero.
+
+\paragraph{Field: Rated Air Flow Rate}\label{field-rated-air-flow-rate-001}
+
+This numeric input is the volumetric air flow rate through the dehumidifier, in m\(^{3}\) per second, at rated conditions (air entering the dehumidifier at 26.7°C {[}80°F{]} dry-bulb and 60\% relative humidity). This is a required input field and the entered value must be greater than zero.
+
+\paragraph{Field: Water Removal Curve Name}\label{field-water-removal-curve-name}
+
+This alpha field defines the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of water removal as a function of the dry-bulb temperature (°C) and relative humidity (\%) of the air entering the dehumidifier. The output of this curve is multiplied by the Rated Water Removal to give the water removal of the dehumidifier at specific operating conditions (i.e., at temperatures and relative humidity levels different from the rating point conditions). The curve should be normalized to have the value of 1.0 at the rating point (air entering the dehumidifier at 26.7°C {[}80°F{]} dry-bulb and 60\% relative humidity, and air flow rate as defined by field ``Rated Air Flow Rate'' above).
+
+\paragraph{Field: Energy Factor Curve Name}\label{field-energy-factor-curve-name}
+
+This alpha field defines the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy factor as a function of the dry-bulb temperature (°C) and relative humidity (\%) of the air entering the dehumidifier. The output of this curve is multiplied by the Rated Energy Factor to give the energy factor of the dehumidifier at specific operating conditions (i.e., at temperatures and relative humidity levels different from the rating point conditions). The curve should be normalized to have the value of 1.0 at the rating point (air entering the dehumidifier at 26.7°C {[}80°F{]} dry-bulb and 60\% relative humidity, and air flow rate as defined by field ``Rated Air Flow Rate'' above).
+
+\paragraph{Field: Part Load Fraction Correlation Curve Name}\label{field-part-load-fraction-correlation-curve-name-000}
+
+This alpha field defines the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of electrical power input to the dehumidifier as a function of the part load ratio (PLR, defined as the water removal load to be met (kg/s) divided by the dehumidifier's water removal rate (kg/s) at the current operating conditions). The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
+
+The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the dehumidifier runs continuously for the simulation timestep). For PLR values between 0 and 1 (0 \textless{} = PLR \textless{} 1), the following rules apply:
+
+0.7 \textless{} = PLF \textless{} = 1.0~~ and~~ PLF \textgreater{} = PLR
+
+If PLF \textless{} 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the dehumidifier is defined as PLR/PLF. If PLF \textless{} PLR, then a warning message is issued and the runtime fraction of the dehumidifier is set to 1.0.
+
+Mechanical dehumidifier typically have long runtimes with minimal compressor cycling. So, a typical part load fraction correlation might be:
+
+~~~~~ PLF = 0.95 + 0.05(PLR)
+
+If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
+
+~~~~~ PLF = 1.0 + 0.0(PLR)
+
+\paragraph{Field: Minimum Dry-Bulb Temperature for Dehumidifier Operation}\label{field-minimum-dry-bulb-temperature-for-dehumidifier-operation}
+
+This numeric field defines the minimum inlet air dry-bulb temperature for dehumidifier operation. The dehumidifier will not operate if the inlet air temperature is below this value. This input value must be less than the Maximum Dry-Bulb Temperature for Dehumidifier Operation, and the default value is 10°C.
+
+\paragraph{Field: Maximum Dry-Bulb Temperature for Dehumidifier Operation}\label{field-maximum-dry-bulb-temperature-for-dehumidifier-operation}
+
+This numeric field defines the maximum inlet air dry-bulb temperature for dehumidifier operation. The dehumidifier will not operate if the inlet air temperature is above this value. This input value must be greater than the Minimum Dry-Bulb Temperature for Dehumidifier Operation, and the default value is 35°C.
+
+\paragraph{Field: Off-Cycle Parasitic Electric Load}\label{field-off-cycle-parasitic-electric-load-001}
+
+This numeric field contains the off-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the dehumidifier. This parasitic electric load is consumed whenever the dehumidifier is available to operate, but is not operating. The model assumed that this parasitic power contributes to heating the zone air (i.e., affects the zone air heat balance). The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
+
+\paragraph{Field: Condensate Collection Water Storage Tank Name}\label{field-condensate-collection-water-storage-tank-name-000}
+
+This field is optional. It is used to specify where condensate from the dehumidifier is collected. If blank or omitted, then any water (condensate) removed is discarded. Enter the name of a Water Storage Tank (ref. WaterUse:Storage) object defined elsewhere and the condensate will then be collected in that tank.
+
+Following is an example input for a zone DX dehumidifier object. A ZoneControl:Humidistat object must also be specified for the zone to which the dehumidifier is connected (connect via a zone air exhaust node and a zone air inlet node, ref. ZoneHVAC:EquipmentConnections).
+
+\begin{lstlisting}
+
+  ZoneHVAC:Dehumidifier:DX,
+      North Zone Dehumidifier,  !- Name
+      ON,                       !- Availability Schedule Name
+      Zone3DehumidifierInlet,   !- Air Inlet Node Name
+      Dehumidifier Outlet Node, !- Air Outlet Node Name
+      50.16,                    !- Rated Water Removal {L/day} (106 pints/day)
+      3.412,                    !- Rated Energy Factor {L/kWh} (7.21 pints/kWh)
+      0.12036,                  !- Rated Air Flow Rate {m3/s} (255 cfm)
+      ZoneDehumidWaterRemoval,  !- Water Removal Curve Name
+      ZoneDehumidEnergyFactor,  !- Energy Factor Curve Name
+      ZoneDehumidPLFFPLR,        !- Part Load Fraction Correlation Curve Name
+      10.0,  !- Minimum Dry-Bulb Temperature for Compressor Operation {C}
+      32.0,  !- Maximum Dry-Bulb Temperature for Compressor Operation {C}
+      0.0;   !- Off Cycle Parasitic Electric Load {W}
+
+
+    ZoneControl:Humidistat,
+      Zone 3 Humidistat,       !- Name
+      NORTH ZONE,              !- Zone Name
+      Seasonal Relative Humidity Sch;  !- Relative Humidity Setpoint Schedule Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-10-008}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Dehumidifier Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Dehumidifier Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Dehumidifier Removed Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Sum,Zone Dehumidifier Removed Water Mass {[}kg{]}
+\item
+  HVAC,Average,Zone Dehumidifier Electric Power {[}W{]}
+\item
+  HVAC,Sum,Zone Dehumidifier Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone Dehumidifier Off Cycle Parasitic Electric Power {[}W{]}
+\item
+  HVAC,Sum,Zone Dehumidifier Off Cycle Parasitic Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone Dehumidifier Part Load Ratio {[]}
+\item
+  HVAC,Average,Zone Dehumidifier Runtime Fraction {[]}
+\item
+  HVAC,Average,Zone Dehumidifier Outlet Air Temperature {[}C{]}
+\end{itemize}
+
+If Condensate Collection Water Storage Tank Name is specified:
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Dehumidifier Condensate Volume Flow Rate {[}m3/s{]}
+\item
+  HVAC,Sum,Zone Dehumidifier Condensate Volume {[}m3{]}
+\end{itemize}
+
+\paragraph{Zone Dehumidifier Sensible Heating Rate {[}W{]}}\label{zone-dehumidifier-sensible-heating-rate-w}
+
+This output field is the sensible heating rate output of the dehumidifier in Watts. This is determined by the water removal rate, enthalpy of water evaporation, and the zone dehumidifier electric power. To reduce simulation time, this heating is carried over to the zone air heat balance for the next HVAC time step (i.e., it is reported here for the current time step but actually impacts the zone air heat balance on the following HVAC time step). This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
+
+\paragraph{Zone Dehumidifier Sensible Heating Energy {[}J{]}}\label{zone-dehumidifier-sensible-heating-energy-j}
+
+This output field is the sensible heating output of the dehumidifier in Joules over the timestep being reported. This is determined by the water removal rate, enthalpy of water evaporation, and the zone dehumidifier electric power. To reduce simulation time, this heating is carried over to the zone air heat balance for the next HVAC time step (i.e., it is reported here for the current time step but actually impacts the zone air heat balance on the following HVAC time step). This value is calculated for each HVAC system timestep, and the results are summed for the timestep being reported.
+
+\paragraph{Zone Dehumidifier Removed Water Mass Flow Rate {[}kg/s{]}}\label{zone-dehumidifier-removed-water-mass-flow-rate-kgs}
+
+This output field is the water removal rate by the dehumidifier in kg/s. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
+
+\paragraph{Zone Dehumidifier Removed Water Mass {[}kg{]}}\label{zone-dehumidifier-removed-water-mass-kg}
+
+This output field is the water removed by the dehumidifier in kg. This value is calculated for each HVAC system timestep, and the results are summed for the timestep being reported.
+
+\paragraph{Zone Dehumidifier Electric Power {[}W{]}}\label{zone-dehumidifier-electric-power-w}
+
+\paragraph{Zone Dehumidifier Electric Energy {[}J{]}}\label{zone-dehumidifier-electric-energy-j}
+
+These outputs are the electric power and electric consumption of the dehumidifier for the time period being reported. They include all electricity used by the dehumidifier (including off-cycle electric parasitics). These values are calculated for each HVAC system timestep, and the results are averaged (power) or summed (consumption) for the timestep being reported. The electric consumption output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Zone Dehumidifier Off Cycle Parasitic Electric Power {[}W{]}}\label{zone-dehumidifier-off-cycle-parasitic-electric-power-w}
+
+\paragraph{Zone Dehumidifier Off Cycle Parasitic Electric Energy {[}J{]}}\label{zone-dehumidifier-off-cycle-parasitic-electric-energy-j}
+
+These outputs are the parasitic electric power and electric consumption for controls or other electrical devices associated with the dehumidifier. This parasitic electric load is consumed whenever the dehumidifier is available to operate, but is not operating. The model assumes that this parasitic power contributes to heating the zone air (i.e., affects the zone air heat balance). These outputs values are included in the Zone Dehumidifier Electric Power and Zone Dehumidifier Electric Energy output variables.
+
+\paragraph{\texorpdfstring{Zone Dehumidifier Part Load Ratio {[]}}{Zone Dehumidifier Part Load Ratio }}\label{zone-dehumidifier-part-load-ratio}
+
+This output field is the part-load ratio for the dehumidifier. Part-load ratio is defined as the water removal load to be met (kg/s) divided by the dehumidifier's water removal rate (kg/s) at the current operating conditions. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
+
+\paragraph{\texorpdfstring{Zone Dehumidifier Runtime Fraction {[]}}{Zone Dehumidifier Runtime Fraction }}\label{zone-dehumidifier-runtime-fraction}
+
+This output field is the runtime fraction for the dehumidifier. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
+
+\paragraph{Zone Dehumidifier Outlet Air Temperature {[}C{]}}\label{zone-dehumidifier-outlet-air-temperature-c}
+
+This output field is dry-bulb temperature of the air leaving the dehumidifier in Celsius. This value represents the dry-bulb temperature of the air leaving the dehumidifier when it is operating. For periods when the dehumidifier is not operating, the outlet air temperature is set equal to the inlet air temperature. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
+
+\paragraph{Zone Dehumidifier Condensate Volume Flow Rate {[}m3/s{]}}\label{zone-dehumidifier-condensate-volume-flow-rate-m3s}
+
+\paragraph{Zone Dehumidifier Condensate Volume {[}m3{]}}\label{zone-dehumidifier-condensate-volume-m3}
+
+These outputs are the rate and volume of water removed as condensate by the dehumidifier. These reports only appear if a water storage tank is named in the input object. The condensate volume output is also added to a meter with Resource Type = OnSiteWater, End Use Key = Condensate, Group Key = System (ref. Output:Meter objects).
+
+\subsection{ZoneHVAC:EnergyRecoveryVentilator}\label{zonehvacenergyrecoveryventilator}
+
+The ZoneHVAC:EnergyRecoveryVentilator - stand alone energy recovery ventilator (ERV) is a single-zone HVAC component used for exhaust air heat recovery (Figure~\ref{fig:zonehvac-energyrecoveryventilator-compound}). This compound object consists of 3 required components: a generic air-to-air heat exchanger (see object Heat Exchanger:Air to Air:Generic), a supply air fan, and an exhaust air fan (see object Fan:OnOff).
+
+An optional controller (see object ZoneHVAC:EnergyRecoveryVentilator:Controller) may be used to simulate economizer (free cooling) operation, modify air flow rates based on high indoor humidity, or simulate a ``push-button'' type economizer controller.
+
+\begin{figure}[hbtp] % fig 115
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image293.png}
+\caption{ZoneHVAC:EnergyRecoveryVentilator compound object Schematic \protect \label{fig:zonehvac-energyrecoveryventilator-compound}}
+\end{figure}
+
+This compound object models the basic operation of supply and exhaust air fans and an air-to-air heat exchanger. The stand alone ERV operates whenever the unit is scheduled to be available (Availability schedule). The stand alone ERV object can be used in conjunction with an economizer feature whereby heat exchange is suspended whenever free cooling is available (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped). The economizer feature may also be activated based on a time-of-day schedule. Heat exchange is also suspended when air flow rates through the heat exchanger are modified in response to a zone humidistat. When an economizer is used in conjunction with high humidity control, high humidity control has the priority.
+
+To model a stand alone ERV connected to a single zone, the input data file should include the following objects:
+
+\begin{itemize}
+\item
+  ZoneHVAC:EnergyRecoveryVentilator
+\item
+  HeatExchanger:AirToAir:SensibleAndLatent
+\item
+  Fan:OnOff (supply air)
+\item
+  Fan:OnOff (exhaust air)
+\item
+  ZoneHVAC:EnergyRecoveryVentilator:Controller (if economizer {[}free cooling{]} mode or high humidity control operation is desired)
+\item
+  ZoneControl:Humidistat (required for high humidity control option)
+\item
+  SetpointManager:Scheduled (if supply air outlet temperature control is used, Ref. Heat Exchanger:Air to Air:Generic for additional guidance)
+\item
+  ZoneHVAC:EquipmentConnections
+\item
+  ZoneHVAC:EquipmentList
+\item
+  OutdoorAir:NodeList
+\end{itemize}
+
+A description of each input field for this compound object is provided below.
+
+\subsubsection{Inputs}\label{inputs-13-018}
+
+\paragraph{Field: Name}\label{field-name-13-012}
+
+A unique user-assigned name for the stand alone ERV unit. Any reference to this unit by another object will use this name.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-12-001}
+
+The name of the schedule (ref: Schedule) that denotes whether the unit can operate during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can operate during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit will not operate. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Heat Exchanger Name}\label{field-heat-exchanger-name-002}
+
+The user-assigned name corresponding to the air-to-air heat exchanger used in this compound object. The only allowable type is:.
+
+HeatExchanger:AirToAir:SensibleAndLatent
+
+\paragraph{Field: Supply Air Flow Rate}\label{field-supply-air-flow-rate-000}
+
+The supply air flow rate through the ERV unit in cubic meters per second at standard temperature and pressure (dry air at 20\(^{o}\) C drybulb). The program uses local barometric pressure to account for altitude using the equation for ``standard atmospheric'' pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
+
+p = 101325*(1-2.25577E-05*Z)**5.2559
+
+where p = pressure in Pa and Z = altitude in m
+
+Note that this flow rate must be within the valid air flow range for the heat exchanger (ref: HeatExchanger:AirToAir:SensibleAndLatent in the Engineering Document). In addition, this flow rate must be less than or equal to the supply fan air flow rate (Fan:OnOff). If the supply air flow rate is less than the exhaust air flow rate, the zone infiltration (ref: ZoneInfiltration) should be specified accordingly (the infiltration induced by imbalanced air flows is not accounted for automatically). The ERV supply air flow rate may also be autosized using the ventilation rate per floor area and/or ventilation rate per occupant fields below. When autosizing, the heat exchanger and fan air flow rates should also be autosized.
+
+Note: The supply air inlet node specified in the generic heat exchanger object must be an outdoor air node (ref: OutdoorAir:Node and OutdoorAir:NodeList). The supply air outlet node specified in the generic heat exchanger object must be a zone air inlet node (ref: ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Exhaust Air Flow Rate}\label{field-exhaust-air-flow-rate-1}
+
+The exhaust air flow rate through the ERV unit in cubic meters per second at standard temperature and pressure (dry air at 20\(^{o}\) C drybulb). The program uses local barometric pressure to account for altitude using the equation for ``standard atmospheric'' pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
+
+p = 101325*(1-2.25577E-05*Z)**5.2559
+
+where p = pressure in Pa and Z = altitude in m
+
+Note that this flow rate must be within the valid air flow range for the heat exchanger (ref: HeatExchanger:AirToAir:SensibleAndLatent in the Engineering Document). In addition, this flow rate must be less than or equal to the exhaust fan air flow rate (Fan:OnOff). If the exhaust air flow rate is greater than the supply air flow rate, the zone infiltration (ref: ZoneInfiltration) should be specified accordingly (the infiltration induced by imbalanced air flows is not accounted for automatically). The ERV exhaust air flow rate may also be autosized using the ventilation rate per floor area and/or ventilation rate per occupant fields below. When autosizing, the heat exchanger and fan air flow rates should also be autosized.
+
+Note: The exhaust air inlet node specified in the generic heat exchanger object must be a zone air exhaust node (ref: ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Supply Air Fan Name}\label{field-supply-air-fan-name-7}
+
+The name of the supply air fan used in this object. Fan type must be Fan:OnOff.
+
+\paragraph{Field: Exhaust Air Fan Name}\label{field-exhaust-air-fan-name}
+
+The name of the exhaust air fan used in this object. Fan type must be Fan:OnOff.
+
+\paragraph{Field: Controller Name}\label{field-controller-name}
+
+This optional field specifies the name of the controller used by this compound component if economizer (free cooling) mode or high humidity control operation is desired. Controller type must be ZoneHVAC:EnergyRecoveryVentilator:Controller.
+
+\paragraph{Field: Ventilation Rate per Unit Floor Area}\label{field-ventilation-rate-per-unit-floor-area}
+
+This optional numeric field defines the ventilation rate per unit floor area in cubic meters per second per square meter. This field is only used when the supply and exhaust air flow rates are autosized.
+
+\paragraph{Field: Ventilation Rate per Occupant}\label{field-ventilation-rate-per-occupant}
+
+This optional numeric field defines the ventilation rate per occupant in cubic meters per second per occupant. This field is only used when the supply and exhaust air flow rates are autosized.
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-9}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this Stand Alone ERV~ object's fan. If the Stand Alone ERV is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this Stand Alone ERV~ object should be on or off.
+
+Following is an example input for this compound object and associated objects that may be defined:
+
+\begin{lstlisting}
+
+ZoneHVAC:EnergyRecoveryVentilator,
+      Stand Alone ERV 1,                        !- Stand alone ERV name
+      FanAndCoilAvailSched,                     !- Availability schedule name
+      OA Heat Recovery 1,                       !- Heat exchanger name
+      0.05,                                     !- Supply air flow rate {m3/s}
+      0.05,                                     !- Exhaust air flow rate {m3/s}
+      Stand Alone ERV Supply Fan,               !- Supply air fan name
+      Stand Alone ERV Exhaust Fan,              !- Exhaust air fan name
+      ERV OA Controller 1;                      !- ERV controller name
+
+
+  OutdoorAir:NodeLine,
+      OutsideAirInletNodes;       !- 1st Node name or node list name
+
+
+  NodeList,
+      OutsideAirInletNodes,       !- Node List Name
+      ERV Outdoor air Inlet Node; !- Node_ID_1
+
+
+
+
+  ZoneHVAC:EquipmentConnections,
+      RESISTIVE ZONE,      !- Zone Name
+      Zone1Equipment,      !- List Name: Zone Equipment
+      Zone1Inlets,         !- List Name: Zone Inlet Nodes
+      Zone1Exhausts,       !- List Name: Zone Exhaust Nodes
+      Zone 1 Node,         !- Zone Air Node Name
+      Zone 1 Outlet Node;  !- Zone Return Air Node Name
+
+
+  ZoneHVAC:EquipmentList,
+      Zone1Equipment,                          !-Name
+      ZoneHVAC:EnergyRecoveryVentilator,  !- KEY--Zone Equipment Type 1
+      Stand Alone ERV 1,                       !- Type Name 1
+      1,                                       !- Cooling Priority
+      1;                                       !- Heating Priority
+
+
+  NodeList,
+      Zone1Inlets,                             !- Node List Name
+      Stand Alone ERV Supply Fan Outlet Node;  !- Node_ID_1
+
+
+  NodeList,
+      Zone1Exhausts,         !- Node List Name
+      Zone 1 Exhaust Node;   !- Node_ID_1
+
+
+  ZoneHVAC:EnergyRecoveryVentilator:Controller,
+      ERV OA Controller 1,           !- ERV controller name
+      0.05,                          !- Outdoor air flow rate {m3/s}
+      19.,                           !- Temperature high limit {C}
+      14.,                           !- Temperature low limit {C}
+      0.0,                           !- Enthalpy high limit {J/kg}
+      NoExhaustAirTemperatureLimit,     !- Exhaust air temperature limit
+      NoExhaustAirEnthalpyLimit; !- Exhaust air enthalpy limit
+
+
+
+
+  HeatExchanger:AirToAir:SensibleAndLatent,
+      OA Heat Recovery 1,            !- Heat exchanger name
+      FanAndCoilAvailSched,          !- Availability schedule name
+      0.05,                          !- Nominal supply air flow rate {m3/s}
+      .76,                           !- Sensible effectiveness at 100% airflow heating condition
+      .68,                           !- Latent effectiveness at 100% airflow heating condition
+      .81,                           !- Sensible effectiveness at 75% airflow heating condition
+      .73,                           !- Latent effectiveness at 75% airflow heating condition
+      .76,                           !- Sensible effectiveness at 100% airflow cooling condition
+      .68,                           !- Latent effectiveness at 100% airflow cooling condition
+      .81,                           !- Sensible effectiveness at 75% airflow cooling condition
+      .73,                           !- Latent effectiveness at 75% airflow cooling condition
+      ERV Outdoor air Inlet Node,    !- Supply air inlet node name
+      Heat Recovery Outlet Node,     !- Supply air outlet node name
+      Zone 1 Exhaust Node,           !- Exhaust air inlet node name
+      Heat Recovery Secondary Outlet Node,  !- Exhaust air outlet node name
+      50.0,                          !- Nominal electric power {W}
+      Yes,                           !- Supply air outlet temperature control
+      Rotary,                        !- Heat exchanger type
+      MinimumExhaustTemperature,   !- Frost control type
+      1.7;                           !- Threshold temperature
+
+
+
+
+  Fan:OnOff,
+      Stand Alone ERV Supply Fan,               !- Fan Name
+      FanAndCoilAvailSched,                     !- Availability Schedule Name
+      0.5,                                      !- Fan Total Efficiency
+      75.0,                                     !- Delta Pressure {Pa}
+      0.05,                                     !- Max Flow Rate {m3/s}
+      0.9,                                      !- Motor Efficiency
+      1.0,                                      !- Motor In Airstream Fraction
+      Heat Recovery Outlet Node,                !- Fan_Inlet_Node
+      Stand Alone ERV Supply Fan Outlet Node;   !- Fan_Outlet_Node
+
+
+  Fan:OnOff,
+      Stand Alone ERV Exhaust Fan,              !- Fan Name
+      FanAndCoilAvailSched,                     !- Availability Schedule Name
+      0.5,                                      !- Fan Total Efficiency
+      75.0,                                     !- Delta Pressure {Pa}
+      0.05,                                     !- Max Flow Rate {m3/s}
+      0.9,                                      !- Motor Efficiency
+      1.0,                                      !- Motor In Airstream Fraction
+      Heat Recovery Secondary Outlet Node,      !- Fan_Inlet_Node
+      Stand Alone ERV Exhaust Fan Outlet Node;  !- Fan_Outlet_Node
+
+
+  SetpointManager:Scheduled,
+      Heat Exhchanger Supply Air Temp Manager,  !- Name
+      Temperature,  !- Control variable
+      Heat Exchanger Supply Air Temp Sch,  !- Schedule Name
+      Heat Exchanger Supply Air Nodes;     !- Name of the set point Node List
+
+
+  NodeList,
+      Heat Exchanger Supply Air Nodes,  !- Node List Name
+      Heat Recovery Outlet Node;        !- Node_ID_1
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-11-006}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone Ventilator Electric Power{[}W{]}
+\item
+  HVAC,Sum,Zone Ventilator Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilator Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilator Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilator Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilator Total Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilator Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilator Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilator Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilator Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilator Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilator Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilator Latent Heating Rate {[}W{]}
+\item
+  HVAC,Sum,Zone Ventilator Latent Heating Energy {[}J{]}
+\item
+  HVAC,Average,Zone Ventilator Supply Fan Availability Status {[]}
+\end{itemize}
+
+\paragraph{Zone Ventilator Electric Power {[}W{]}}\label{zone-ventilator-electric-power-w}
+
+This output field is the electric consumption rate of the stand alone energy recovery ventilator in Watts. This rate includes the electric consumption by the supply air fan, exhaust air fan and the generic air-to-air heat exchanger.
+
+\paragraph{Zone Ventilator Electric Energy {[}J{]}}\label{zone-ventilator-electric-energy-j}
+
+This output field is the electric consumption of the stand alone energy recovery ventilator in Joules for the timestep being reported. This value includes the electric consumption by the supply air fan, exhaust air fan and the generic air-to-air heat exchanger.
+
+\paragraph{Zone Ventilator Total Cooling Rate {[}W{]}}\label{zone-ventilator-total-cooling-rate-w}
+
+This output field is the total (enthalpy) heat extraction rate of the stand alone energy recovery ventilator from the zone in Watts. This value is calculated using the supply air outlet mass flow rate, and the enthalpy difference of the supply outlet and exhaust inlet air streams. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
+
+\paragraph{Zone Ventilator Total Cooling Energy {[}J{]}}\label{zone-ventilator-total-cooling-energy-j}
+
+This output field is the total (enthalpy) heat extraction of the stand alone energy recovery ventilator from the zone in Joules over the timestep being reported. This value is calculated using the supply air outlet mass flow rate, the enthalpy difference of the supply outlet and exhaust inlet air streams, and the HVAC system timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are summed for the timestep being reported.
+
+\paragraph{Zone Ventilator Total Heating Rate {[}W{]}}\label{zone-ventilator-total-heating-rate-w}
+
+This output field is the total (enthalpy) heat addition rate of the stand alone energy recovery ventilator to the zone in Watts. This value is calculated using the supply air outlet mass flow rate, and the enthalpy difference of the supply outlet and exhaust inlet air streams. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
+
+\paragraph{Zone Ventilator Total Heating Energy {[}J{]}}\label{zone-ventilator-total-heating-energy-j}
+
+This output field is the total (enthalpy) heat addition of the stand alone energy recovery ventilator to the zone in Joules over the timestep being reported. This value is calculated using the supply air outlet mass flow rate, the enthalpy difference of the supply outlet and exhaust inlet air streams, and the HVAC system timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are summed for the timestep being reported.
+
+\paragraph{Zone Ventilator Sensible Cooling Rate {[}W{]}}\label{zone-ventilator-sensible-cooling-rate-w}
+
+This output is the moist air sensible heat extraction rate of the stand alone energy recovery ventilator from the zone in Watts. This value is calculated using the supply air outlet mass flow rate, and the enthalpy difference of the supply outlet and exhaust inlet air streams at a constant humidity ratio. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
+
+\paragraph{Zone Ventilator Sensible Cooling Energy {[}J{]}}\label{zone-ventilator-sensible-cooling-energy-j}
+
+This output is the moist air sensible heat extraction of the stand alone energy recovery ventilator from the zone in Joules over the timestep being reported. This value is calculated using the supply air outlet mass flow rate, the enthalpy difference of the supply outlet and exhaust inlet air streams at a constant humidity ratio, and the HVAC system timestep. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are summed for the timestep being reported.
+
+\paragraph{Zone Ventilator Sensible Heating Rate {[}W{]}}\label{zone-ventilator-sensible-heating-rate-w}
+
+This output is the sensible heat addition rate of the stand alone energy recovery ventilator to the zone in Watts. This value is calculated using the supply air outlet mass flow rate, and the enthalpy difference of the supply outlet and exhaust inlet air streams at a constant humidity ratio. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
+
+\paragraph{Zone Ventilator Sensible Heating Energy {[}J{]}}\label{zone-ventilator-sensible-heating-energy-j}
+
+This output is the sensible heat addition of the stand alone energy recovery ventilator to the zone in Joules over the timestep being reported. This value is calculated using the supply air outlet mass flow rate, the enthalpy difference of the supply outlet and exhaust inlet air streams at a constant humidity ratio, and the HVAC system timestep. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are summed for the timestep being reported.
+
+\paragraph{Zone Ventilator Latent Cooling Rate {[}W{]}}\label{zone-ventilator-latent-cooling-rate-w}
+
+This output is the latent heat extraction (dehumidification) rate of the stand alone energy recovery ventilator from the zone in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the stand alone ERV. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
+
+\paragraph{Zone Ventilator Latent Cooling Energy {[}J{]}}\label{zone-ventilator-latent-cooling-energy-j}
+
+This output is the latent heat extraction (dehumidification) of the stand alone energy recovery ventilator from the zone in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the stand alone ERV. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are summed for the timestep being reported.
+
+\paragraph{Zone Ventilator Latent Heating Rate {[}W{]}}\label{zone-ventilator-latent-heating-rate-w}
+
+This output is the latent heat addition (humidification) rate of the stand alone energy recovery ventilator to the zone in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the stand alone ERV. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
+
+\paragraph{Zone Ventilator Latent Heating Energy {[}J{]}}\label{zone-ventilator-latent-heating-energy-j}
+
+This output is the latent heat addition (humidification) of the stand alone energy recovery ventilator to the zone in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the stand alone ERV. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are summed for the timestep being reported.
+
+\paragraph{\texorpdfstring{Zone Ventilator Supply Fan Availability Status {[]}}{Zone Ventilator Supply Fan Availability Status }}\label{zone-ventilator-supply-fan-availability-status}
+
+This is the availability status of the Stand Alone ERV~ fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the Stand Alone ERV~ object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
+
+\subsection{ZoneHVAC:TerminalUnit:VariableRefrigerantFlow}\label{zonehvacterminalunitvariablerefrigerantflow}
+
+Zone terminal units with variable refrigerant flow DX coils are used exclusively with variable refrigerant flow (VRF) air conditioning systems (Ref. AirConditioner:VariableRefrigerantFlow object). The zone terminal units are connected to a zone using the inlet and exhaust node names specified in a ZoneHVAC:EquipmentConnections object. The zone exhaust node has the same name as the terminal unit air inlet node. The zone inlet node has the same name as the terminal unit air outlet node. The zone terminal unit is also listed in a zone's equipment list and will typically be the first equipment operating for both cooling and heating (i.e., Sequence = 1 in the ZoneHVAC:EquipmentList). Other ZoneHVAC equipment may be used in the same zone and should be sequenced to operate after the zone terminal units (i.e., sequence = 2 or higher)
+
+The terminal units operate to satisfy a heating or cooling load in a zone based on a zone thermostat temperature set point. A direct-expansion (DX) cooling and/or DX heating coil is specified depending on the operating mode required. Both a DX cooling and DX heating coil will typically be installed in the terminal unit, however only one may be used if desired. Outdoor ventilation air is modeled with the use of an optional outside air mixer object. Outside air may be provided to the zone only when the coil is operating or can be supplied continuously even when the coil is not operating. A supply air fan is also required and can be modeled as either draw through or blow through.
+
+\subsubsection{Inputs}\label{inputs-14-018}
+
+\paragraph{Field: Zone Terminal Unit Name}\label{field-zone-terminal-unit-name}
+
+This alpha field defines a unique user-assigned name for an instance of a variable refrigerant flow zone terminal unit. Any reference to this terminal unit by another object will use this name. The zone terminal unit name must be specified in a ZoneTerminalUnitList object to connect this terminal unit to an AirConditioner:VariableRefrigerantFlow object.
+
+\paragraph{Field: Availability Schedule Name}\label{field-availability-schedule-name-13-001}
+
+This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the terminal unit operates during a given time period. A schedule value equal to 0 denotes that the terminal unit must be off for that time period. A value greater than 0 denotes that the terminal unit is available to operate during that time period. This schedule may be used to completely disable the terminal unit as required. If this field is left blank, the schedule has a value of 1 for all time periods.
+
+\paragraph{Field: Terminal Unit Air Inlet Node Name}\label{field-terminal-unit-air-inlet-node-name}
+
+This alpha field defines the name of the terminal unit air inlet node. This node name should be the same as a zone exhaust node (ref: ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Terminal Unit Air Outlet Node Name}\label{field-terminal-unit-air-outlet-node-name}
+
+This alpha field defines the name of the terminal unit air outlet node. This node name should be the same as a zone inlet node (ref: ZoneHVAC:EquipmentConnections).
+
+\paragraph{Field: Cooling Supply Air Flow Rate}\label{field-cooling-supply-air-flow-rate-3-001}
+
+This numeric field defines the terminal unit's operating volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in cooling mode.
+
+\paragraph{Field: No Cooling Supply Air Flow Rate}\label{field-no-cooling-supply-air-flow-rate-000}
+
+This numeric field defines the terminal unit's operating volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit's cooling coil is not operating and the previous mode was cooling.
+
+\paragraph{Field: Heating Supply Air Flow Rate}\label{field-heating-supply-air-flow-rate-3-001}
+
+This numeric field defines the terminal unit's operating volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in heating mode.
+
+\paragraph{Field: No Heating Supply Air Flow Rate}\label{field-no-heating-supply-air-flow-rate-000}
+
+This numeric field defines the terminal unit's operating volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit's heating coil is not operating and the previous mode was heating.
+
+\paragraph{Field: Cooling Outdoor Air Flow Rate}\label{field-cooling-outdoor-air-flow-rate-3}
+
+This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in cooling mode.
+
+\paragraph{Field: Heating Outdoor Air Flow Rate}\label{field-heating-outdoor-air-flow-rate-3}
+
+This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in heating mode.
+
+\paragraph{Field: No Load Outdoor Air Flow Rate}\label{field-no-load-outdoor-air-flow-rate-2}
+
+This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is not operating in cooling or heating mode.
+
+\paragraph{Field: Supply Air Fan Operating Mode Schedule Name}\label{field-supply-air-fan-operating-mode-schedule-name-7}
+
+This alpha field defines the name of the supply air fan operating mode schedule. Schedule values equal to 0 denote cycling fan/cycling coil operation. All other schedule values denote constant fan/cycling coil operation.
+
+\paragraph{Field: Supply Air Fan Placement}\label{field-supply-air-fan-placement-000}
+
+This alpha field has two choices: \textbf{BlowThrough} or \textbf{DrawThrough}. If this field is left blank, the default is blow through.
+
+The first choice stands for ``blow through fan''. This means that the unit consists of a fan followed by the DX coils. The fan ``blows through'' the cooling and heating coils. If an outside air mixer is used, the fan inlet connects to the outside air mixer's mixed air node. If an outside air mixer is not used, the fan inlet connects to the zone exhaust node. For this configuration, the fan outlet always connects to the DX cooling coil inlet node (or if a DX cooling coil is not used, the DX heating coil inlet node).
+
+The second choice stands for ``draw through fan''. This means that the unit consists of the DX coil(s) followed by a fan. The fan ``draws air through'' the DX coil(s). In this case the fan inlet always connects to the DX heating coil outlet node (or if a DX heating coil is not use, the DX cooling coil outlet node) and the fan outlet node always connects to the zone inlet node.
+
+\paragraph{Field: Supply Air Fan Object Type}\label{field-supply-air-fan-object-type-8}
+
+This choice field contains the identifying type of supply air fan specified for the furnace. Fan type must be \textbf{Fan:OnOff} or \textbf{Fan:ConstantVolume}. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e.~Supply Air Fan Operating Mode Schedule values are at times 0).
+
+\paragraph{Field: Supply Air Fan Object Name}\label{field-supply-air-fan-object-name}
+
+This alpha field defines the name of the terminal unit's supply air fan.
+
+\paragraph{Field: Outside Air Mixer Object Type}\label{field-outside-air-mixer-object-type}
+
+This alpha field contains the identifying type of outside air mixer specified for the terminal unit. Outside air mixer type must be \textbf{OutsideAir:Mixer}. This field should be left blank when an outside air mixer is not simulated.
+
+\paragraph{Field: Outside Air Mixer Object Name}\label{field-outside-air-mixer-object-name}
+
+This alpha field defines the name of the terminal unit's outside air mixer. If this field is left blank, an outside air mixer is not simulated.
+
+\paragraph{Field: DX Cooling Coil Object Type}\label{field-dx-cooling-coil-object-type}
+
+This choice field contains the identifying type of the terminal unit's DX cooling coil. The only valid DX cooling coil type is \textbf{Coil:Cooling:DX:VariableRefrigerantFlow}. This field should be left blank when a DX cooling coil is not simulated.
+
+\paragraph{Field: DX Cooling Coil Name}\label{field-dx-cooling-coil-name-1}
+
+This alpha field defines the name of the terminal unit's DX cooling coil. If this field is left blank, a DX cooling coil is not simulated.
+
+\paragraph{Field: DX Heating Coil Object Type}\label{field-dx-heating-coil-object-type}
+
+This choice field contains the identifying type of the terminal unit's DX heating coil. The only valid DX heating coil type is \textbf{Coil:Heating:DX:VariableRefrigerantFlow}. This field should be left blank when a DX heating coil is not simulated.
+
+\paragraph{Field: DX Heating Coil Object Name}\label{field-dx-heating-coil-object-name}
+
+This alpha field defines the name of the terminal unit's DX heating coil. This field should be left blank when a DX heating coil is not simulated.
+
+\paragraph{Field: Zone Terminal Unit On Parasitic Electric Energy Use}\label{field-zone-terminal-unit-on-parasitic-electric-energy-use-000}
+
+This numeric field defines the parasitic electrical energy use of the zone terminal unit when either terminal unit coil is operating. When in cooling mode, this electric energy use is reported in a zone terminal unit cooling electric consumption output variable. When in heating mode, this electric energy use is reported in a zone terminal unit heating electric consumption output variable.
+
+\paragraph{Field: Zone Terminal Unit Off Parasitic Electric Energy Use}\label{field-zone-terminal-unit-off-parasitic-electric-energy-use-000}
+
+This numeric field defines the parasitic electrical energy use of the zone terminal unit when the terminal unit coil(s) is not operating. When the previous mode was cooling, this electric energy use is reported in a zone terminal unit cooling electric consumption output variable. When the previous mode was heating, this electric energy use is reported in a zone terminal unit heating electric consumption output variable.
+
+\paragraph{Field: Rated Total Heating Capacity Sizing Ratio}\label{field-rated-total-heating-capacity-sizing-ratio-000}
+
+This numeric field defines the ratio of the heating coil to cooling coil size when autosizing is used. The model assumes that when used, this value will be greater than 1. This field supersedes the Rated Total Heating Capacity Sizing Ratio entered in the AirConditioner:VariableRefrigerantFlow object. If this field is left blank, the value entered in the parent object is used for sizing. If neither field is used, the sizing ratio is assumed to be 1.
+
+\paragraph{Field: Availability Manager List Name}\label{field-availability-manager-list-name-10}
+
+This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this Zone Terminal Unit object's fan. If the Zone Terminal Unit is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this Zone Terminal Unit object should be on or off.
+
+\paragraph{Field: Design Specification ZoneHVAC Sizing Object Name}\label{field-design-specification-zonehvac-sizing-object-name-9}
+
+This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Cooling Supply Air Flow Rate in this VRF terminal unit zone HVAC object. The scaled Supply Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
+
+Following is an example input for a ZoneHVAC:TerminalUnit:VariableRefrigerantFlow object.
+
+\begin{lstlisting}
+
+ZoneHVAC:TerminalUnit:VariableRefrigerantFlow,
+  Zone 1 TU,               !- Zone Terminal Unit Name
+  TU Availability Schedule,!- Terminal Unit Availability schedule
+  TU1 Inlet Node,          !- Terminal Unit Air Inlet Node Name
+  TU1 Outlet Node,         !- Terminal Unit Air Outlet Node Name
+  0.005,                   !- Cooling Supply Air Flow Rate {m3/s}
+  0,                       !- No Cooling Supply Air Flow Rate {m3/s}
+  0.005,                   !- Heating Supply Air Flow Rate {m3/s}
+  0,                       !- No Heating Supply Air Flow Rate {m3/s}
+  0.001,                   !- Cooling Outdoor Air Flow Rate
+  0.001,                   !- Heating Outdoor Air Flow Rate
+  0,                       !- No Load Outdoor Air Flow Rate
+  TU1 Fan Op Schedule,     !- Supply Air Fan Operating Mode Schedule Name
+  drawthrough,             !- Supply Air Fan placement
+  Fan:ConstantVolume,      !- Supply Air Fan Object Type
+  TU1 SA Fan,              !- Supply Air Fan Object Name
+  OutdoorAir:Mixer,        !- Outside Air Mixer Object Type
+  TU1 OA Mixer,            !- Outside Air Mixer Object Name
+  COIL:Cooling:DX:VariableRefrigerantFlow,  !- Cooling Coil Object Type
+  TU1 VRF DX Cooling Coil, !- Cooling Coil Object Name
+  COIL:Heating:DX:VariableRefrigerantFlow,  !- Heating Coil Object Type
+  TU1 VRF DX Heating Coil, !- Heating Coil Object Name
+  30,                      !- Zone Terminal Unit On Parasitic Electric Energy Use {W}
+  20,                      !- Zone Terminal Unit Off Parasitic Electric Energy Use {W}
+  ,                        !- Rated Total Heating Capacity Sizing Ratio {W/W}
+  ;                        !- Availability Manager List Name
+\end{lstlisting}
+
+\subsubsection{Outputs}\label{outputs-12-006}
+
+\begin{itemize}
+\item
+  HVAC,Average,Zone VRF Air Terminal Total Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Zone VRF Air Terminal Total Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Zone VRF Air Terminal Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Zone VRF Air Terminal Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average, Zone VRF Air Terminal Latent Cooling Rate {[}W{]}
+\item
+  HVAC,Sum, Zone VRF Air Terminal Latent Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone VRF Air Terminal Total Heating Rate {[}W{]}
+\item
+  HVAC,Sum, Zone VRF Air Terminal Total Heating Energy {[}J{]}
+\item
+  HVAC,Average, Zone VRF Air Terminal Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Sum, Zone VRF Air Terminal Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Average, Zone VRF Air Terminal Latent Heating Rate {[}W{]}
+\item
+  HVAC,Sum, Zone VRF Air Terminal Latent Heating Energy {[}J{]}
+\item
+  HVAC,Average, Zone VRF Air Terminal Cooling Electric Power {[}W{]}
+\item
+  HVAC,Sum, Zone VRF Air Terminal Cooling Electric Energy {[}J{]}
+\item
+  HVAC,Average,Zone VRF Air Terminal Heating Electric Power {[}W{]}
+\item
+  HVAC,Sum,Zone VRF Air Terminal Heating Electric Energy {[}J{]}
+\item
+  HVAC,Average, Zone VRF Air Terminal Fan Availability Status {[]}
+\end{itemize}
+
+\paragraph{Zone VRF Air Terminal Total Cooling Rate {[}W{]}}\label{zone-vrf-air-terminal-total-cooling-rate-w}
+
+This field is the total (sensible and latent) cooling rate output of the terminal unit in Watts. This is determined by terminal unit inlet and outlet air conditions and the air mass flow rate through the unit. This value describes the total energy rate delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Total Cooling Energy {[}J{]}}\label{zone-vrf-air-terminal-total-cooling-energy-j}
+
+This is the total (sensible plus latent) cooling output of the terminal unit in Joules over the time step being reported. This is determined by the terminal unit inlet and outlet air conditions and the air mass flow rate through the unit. This value describes the total cooling energy delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Sensible Cooling Rate {[}W{]}}\label{zone-vrf-air-terminal-sensible-cooling-rate-w}
+
+This output is the moist air sensible cooling rate output of the terminal unit in Watts. This is determined by enthalpy difference between the inlet and outlet air temperature at a constant humidity ratio, using the minimum of the inlet and outlet air node humidity ratios, and the air mass flow rate through the unit. This value describes the sensible cooling energy rate delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Sensible Cooling Energy {[}J{]}}\label{zone-vrf-air-terminal-sensible-cooling-energy-j}
+
+This is the moist air sensible cooling output of the terminal unit in Joules for the time step being reported. This is determined by enthalpy difference between the inlet and outlet air temperature at a constant humidity ratio, using the minimum of the inlet and outlet air node humidity ratios, and the air mass flow rate through the unit. This value describes the sensible cooling energy delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Latent Cooling Rate {[}W{]}}\label{zone-vrf-air-terminal-latent-cooling-rate-w}
+
+This is the latent cooling rate output of the terminal unit in Watts. This is determined by the inlet and outlet air humidity ratios and the air mass flow rate through the unit. This value describes the latent cooling energy rate delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Latent Cooling Energy {[}J{]}}\label{zone-vrf-air-terminal-latent-cooling-energy-j}
+
+This is the latent cooling output of the terminal unit in Joules for the time step being reported. This is determined by the inlet and outlet air humidity ratios and the air mass flow rate through the unit. This value describes the latent cooling energy delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Total Heating Rate {[}W{]}}\label{zone-vrf-air-terminal-total-heating-rate-w}
+
+This field is the total enthalpic heating rate output of the terminal unit in Watts. This is determined by the terminal unit inlet and outlet air conditions and the air mass flow rate through the unit. This value describes the total heating energy rate delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Total Heating Energy {[}J{]}}\label{zone-vrf-air-terminal-total-heating-energy-j}
+
+This is the total enthalpic heating output of the terminal unit in Joules over the time step being reported. This is determined by the terminal unit inlet and outlet air conditions and the air mass flow rate through the unit. This value describes the total heating energy delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Sensible Heating Rate {[}W{]}}\label{zone-vrf-air-terminal-sensible-heating-rate-w}
+
+This output is the moist air sensible heating rate output of the terminal unit in Watts. This is determined by enthalpy difference between the inlet and outlet air temperature at a constant humidity ratio, using the minimum of the inlet and outlet air node humidity ratios, and the air mass flow rate through the unit. This value describes the sensible heating energy rate delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Sensible Heating Energy {[}J{]}}\label{zone-vrf-air-terminal-sensible-heating-energy-j}
+
+This is the moist air sensible heating output of the terminal unit in Joules for the time step being reported. This is determined by enthalpy difference between the inlet and outlet air temperature at a constant humidity ratio, using the minimum of the inlet and outlet air node humidity ratios, and the air mass flow rate through the unit. This value describes the sensible heating energy delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Latent Heating Rate {[}W{]}}\label{zone-vrf-air-terminal-latent-heating-rate-w}
+
+This is the latent heating rate output of the terminal unit in Watts. This is determined by the inlet and outlet air specific humidity ratios and the air mass flow rate through the unit. This value describes the latent heating energy rate delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Latent Heating Energy {[}J{]}}\label{zone-vrf-air-terminal-latent-heating-energy-j}
+
+This is the latent heating output of the terminal unit in Joules for the time step being reported. This is determined by the inlet and outlet air specific humidity ratios and the air mass flow rate through the unit. This value describes the latent heating energy delivered to the zone.
+
+\paragraph{Zone VRF Air Terminal Cooling Electric Power{[}W{]}}\label{zone-vrf-air-terminal-cooling-electric-powerw}
+
+This output field is the parasitic electricity consumption rate of the zone terminal unit in Watts. The consumption rate includes parasitic electricity used by the zone terminal unit's transformers, controls, or other electricity consuming devices. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. The terminal unit parasitic on and off electricity is reported in this cooling output variable when the unit operates in cooling mode or the most recent operation was for cooling.
+
+\paragraph{Zone VRF Air Terminal Cooling Electric Energy {[}J{]}}\label{zone-vrf-air-terminal-cooling-electric-energy-j}
+
+This output field is the electricity consumption of the zone terminal unit in Joules for the time period being reported. The consumption includes parasitic electricity used by the zone terminal unit's transformers, controls, or other electricity consuming devices. This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported. The terminal unit parasitic on and off electricity consumption is reported in this cooling output variable when the unit operates in cooling mode or the most recent operation was for cooling. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{Zone VRF Air Terminal Heating Electric Power{[}W{]}}\label{zone-vrf-air-terminal-heating-electric-powerw}
+
+This output field is the parasitic electricity consumption rate of the zone terminal unit in Watts. The consumption rate includes parasitic electricity used by the zone terminal unit's transformers, controls, or other electricity consuming devices. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. The terminal unit parasitic on and off electricity is reported in this heating output variable when the unit operates in heating mode or the most recent operation was for heating.
+
+\paragraph{Zone VRF Air Terminal Heating Electric Energy {[}J{]}}\label{zone-vrf-air-terminal-heating-electric-energy-j}
+
+This output field is the electricity consumption of the zone terminal unit in Joules for the time period being reported. The consumption includes parasitic electricity used by the zone terminal unit's transformers, controls, or other electricity consuming devices. This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported. The terminal unit parasitic on and off electricity consumption is reported in this heating output variable when the unit operates in heating mode or the most recent operation was for heating. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
+
+\paragraph{\texorpdfstring{Zone VRF Air Terminal Fan Availability Status {[]}}{Zone VRF Air Terminal Fan Availability Status }}\label{zone-vrf-air-terminal-fan-availability-status}
+
+This is the availability status of the Zone Terminal Unit fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the Zone Terminal Unit object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:* Outputs). For multiple availability managers in an Availability Manager Assignment List along with Hybrid Ventilation Manager, rules to determine fan availability status are described in the section `Group -- System Availability Managers'. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the ``detailed'' reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
diff --git a/doc/input-output-reference/src/overview/hvac-primary-and-secondary-systems.tex b/doc/input-output-reference/src/overview/hvac-primary-and-secondary-systems.tex
new file mode 100644
index 00000000000..b08642e9419
--- /dev/null
+++ b/doc/input-output-reference/src/overview/hvac-primary-and-secondary-systems.tex
@@ -0,0 +1,27 @@
+\section{HVAC: Primary and Secondary Systems}\label{hvac-primary-and-secondary-systems}
+
+The HVAC and equipment section of the EnergyPlus input data dictionary and input data file are slightly more complex than the description of building geometry, internal gains, etc. because of the interconnections of the various parts of an HVAC system. In EnergyPlus, there are several portions to the HVAC simulation. All of these parts must be correctly specified in order to arrive at a valid simulation model. The goal of this section is to provide interface developers and advanced users with guidelines on what input is expected and also provide some background on basic EnergyPlus simulation methodology.
+
+An EnergyPlus HVAC simulation consists of various components that are connected physically in the actual system by ducts, piping, etc. Every component in an HVAC system must have an inlet and outlet ``node''. In the actual system, a node might be a point in the system at which fluid properties can be measured. In an EnergyPlus simulation, the nodes are points at which fluid properties are evaluated and passed on to subsequent equipment.
+
+Components are linked together to form various loops within the simulation. Thus, the output node from one component also serves as the inlet node to the next component. Loops are constructed by defining these loops and also defining the components on the loops. The figure below shows a generic example of the loop-node concept.
+
+Loop nodes are a key defining feature in EnergyPlus. As a result, it is recommended that one of the first steps taken in defining an HVAC system in EnergyPlus be the definition of a node diagram or map. This is helpful for visualization of the entire system. Such a map could be created electronically within an interface or could be kept in the background out of the sight of the user.
+
+\begin{figure}[hbtp] % fig 72
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image134.png}
+\caption{Example Node Diagram \protect \label{fig:example-node-diagram}}
+\end{figure}
+
+So that these loops are manageable and more clearly defined both in the input and in the simulation, four different loop sections can be defined in an EnergyPlus input file. In general, these four types are in essence two pairs of loop sections that make up~ two distinct types of loops: a zone/air loop and a plant loop. As of Version 7, plant loops and condenser loops have been consolidated to be largely the same. The four loop section types are defined below.
+
+\textbf{Air Loop Supply Side:}~ The air loop is defined by the section of the zone/air loop that starts after the zone return streams are combined and continues on until just before any air stream(s) are branched off to individual zones. The starting point of the air loop is fairly straightforward. The ending point is slightly more complex but can be understood with some examples. For instance, in a terminal reheat system, the end of the air loop would typically be considered the node following the cooling coil. In a dual duct system, the air loop would have two ending points that would correspond to the nodes after the cooling coil and after the heating coil/humidifier. In most cases, the air loop has a single starting point and up to two ending points (for a 2 deck system).~ An outdoor air subsystem can be included in the supply side for ventilation and relief air.
+
+\textbf{Air Loop Zone Equipment:} ~The zone equipment section of the input file is defined as more or less the rest of the zone/air loop (outside air is handled separately as a subset of the air loop). This includes everything from where the ducts are split to serve various zones up through where the return ducts from various zones are mixed into a single return duct. Zone equipment can include dampers and reheat coils as well as zone specific conditioning systems such as thermostatic baseboard or a window air conditioner. Most control issues are typically dealt with in the zone equipment section of the simulation.
+
+\textbf{Plant Loop Demand Side:}~ One side of the plant is where energy is ``demanded'' by various components that make up the air loop or zone equipment. Typically, this is the water side of equipment such as coils, baseboard, radiant heating and cooling, etc. In the case of a condenser loop, energy is typically ``demanded'' by a chiller condenser or other water source heat pump. The demand side of this loop can also include mixers, flow splitters, and a bypass.
+
+\textbf{Plant Loop Supply Side:} ~The other side of the plant loop is where energy is ``supplied'' by various components. The components typically found on the supply side include pumps, boilers, chillers, purchased heating and cooling, ice storage, etc. In the case of a condenser, the components would be cooling tower, fluid cooler, or ground source heat exchanger, etc.~ As with the demand side, this loop can also include mixers, flow splitters, and a bypass.
+
+The section of the input file for describing the HVAC system tends to follow this structure presented above. Both plant and condenser loops are defined with a master description and then branch off into supply and demand side details. Linkage between the two sides is done using node names in the master statement. The air loop and zone equipment descriptions are slightly more complex due to the wide range of potential systems that are anticipated. Note that in every section controls become a key element and must be addressed. Each of the following sections details either a loop, a portion of a loop, or controls.
diff --git a/doc/input-output-reference/src/overview/idd-conventions.tex b/doc/input-output-reference/src/overview/idd-conventions.tex
new file mode 100644
index 00000000000..1860f3d5a59
--- /dev/null
+++ b/doc/input-output-reference/src/overview/idd-conventions.tex
@@ -0,0 +1,370 @@
+\section{IDD Conventions}\label{idd-conventions}
+
+The following is a basic description of the structure of the IDD (it's actually taken directly from the IDD file). As noted within, \textbf{!} signifies a comment character as does the \textbf{\textbackslash{}}. \textbf{\textbackslash{}} has also been adopted as a convention for including more specific comments about each field in an object. These have been used with success in the IDFEditor and it is hoped the flexibility will provide other interface developers with useful information.
+
+\begin{lstlisting}
+!IDD_Version **VERSION NUMBER**
+! **************************************************************************
+! This file is the Input Data Dictionary (IDD) for EnergyPlus.
+! The IDD defines the syntax and data model for each type of input "Object."
+! Lines in EnergyPlus input files (and IDD) are limited to 500 characters.
+!
+! Object Description
+! ------------------
+! To define an object (a record with data), develop a key word that is unique
+! Each data item to the object can be A (Alphanumeric string) or N (numeric)
+! Number each A and N.  This will show how the data items will be put into the
+! arrays that are passed to the Input Processor "Get" (GetObjectItem) routines.
+! All alpha fields are limited to 100 characters.  Numeric fields should be
+! valid numerics (can include such as 1.0E+05) and are placed into double
+! precision variables.
+!
+! NOTE: Even though a field may be optional, a comma representing that field
+!   must be included (unless it is the last field in the object).  Since the
+!   entire input is "field-oriented" and not "keyword-oriented", the EnergyPlus
+!   Input Processor must have some representation (even if blank) for each
+!   field.
+!
+! Object Documentation
+! --------------------
+! In addition, the following special comments appear one per line and
+! most are followed by a value.  Comments may apply to a field or the object
+! or a group of objects.
+!
+! Field-level comments:
+!
+!  \field           Name of field
+!                     (should be succinct and readable, blanks are encouraged)
+!
+!  \note            Note describing the field and its valid values. If multiple lines,
+!                   start each line with \note. Limit line length to 100 characters.
+!
+!  \required-field  To flag fields which may not be left blank
+!                     (this comment has no "value")
+!
+!  \begin-extensible  Marks the first field at which the object accepts an extensible
+!                   field set.  A fixed number of fields from this marker define the
+!                   extensible field set, see the object code \extensible for
+!                   more information.
+!
+!  \units           Units (must be from EnergyPlus standard units list)
+!                   EnergyPlus units are standard SI units
+!
+!  \ip-units        IP-Units (for use by input processors with IP units)
+!                   This is only used if the default conversion is not
+!                   appropriate.
+!
+!  \unitsBasedOnField  For fields that may have multiple possible units, indicates
+!                   the field in the object that can be used to determine
+!                   the units. The field reference is in the A2 form.
+!
+!  \minimum         Minimum that includes the following value
+!
+!  \minimum>        Minimum that must be > than the following value
+!
+!  \maximum         Maximum that includes the following value
+!
+!  \maximum<        Maximum that must be < than the following value
+!
+!  \default         Default for the field (if N/A then omit entire line)
+!
+!  \deprecated      This field is not really used and will be deleted from the object.
+!                   The required information is gotten internally or
+!                   not needed by the program.
+!
+!  \autosizable     Flag to indicate that this field can be used with the Auto
+!                   Sizing routines to produce calculated results for the
+!                   field.  If a value follows this, then that will be used
+!                   when the "Autosize" feature is flagged.  To trigger
+!                   autosizing for a field, enter Autosize as the field's
+!                   value.  Only applicable to numeric fields.
+!
+! \autocalculatable Flag to indicate that this field can be automatically
+!                   calculated. To trigger auto calculation for a field, enter
+!                   Autocalculate as the field's value.  Only applicable to
+!                   numeric fields.
+!
+!  \type            Type of data for the field -
+!                     integer
+!                     real
+!                     alpha       (arbitrary string),
+!                     choice      (alpha with specific list of choices, see
+!                                 \key)
+!                     object-list (link to a list of objects defined elsewhere,
+!                                  see \object-list and \reference)
+!                     external-list (uses a special list from an external source,
+!                                    see \external-list)
+!                     node        (name used in connecting HVAC components)
+!
+!  \retaincase      Retains the alphabetic case for alpha type fields
+!
+!  \key             Possible value for "\type choice" (blanks are significant)
+!                     use multiple \key lines to indicate all valid choices
+!
+!  \object-list     Name of a list of user-provided object names that are valid
+!                     entries for this field (used with "\reference")
+!                     see Zone and BuildingSurface:Detailed objects below for
+!                     examples.
+!                  ** Note that a field may have multiple \object-list commands.
+!
+!  \external-list   The values for this field should be selected from a special
+!                   list generated outside of the IDD file. The choices for the
+!                   special lists are:
+!                        autoRDDvariable
+!                        autoRDDmeter
+!                        autoRDDvariableMeter
+!                   When one of these are selected the options for the field
+!                   are taken from the RDD or MDD file or both.
+!
+!  \reference       Name of a list of names to which this object belongs
+!                     used with "\type object-list" and with "\object-list"
+!                     see Zone and BuildingSurface:Detailed objects below for
+!                     examples:
+!
+!                        Zone,
+!                          A1 , \field Name
+!                               \type alpha
+!                               \reference ZoneNames
+!
+!                        BuildingSurface:Detailed,
+!                          A4 , \field Zone Name
+!                               \note Zone the surface is a part of
+!                               \type object-list
+!                               \object-list ZoneNames
+!
+!             For each zone, the field "Name" may be referenced
+!             by other objects, such as BuildingSurface:Detailed, so it is
+!             commented with "\reference ZoneNames"
+!             Fields that reference a zone name, such as BuildingSurface:Detailed's
+!             "Zone Name", are commented as
+!             "\type object-list" and "\object-list ZoneNames"
+!             ** Note that a field may have multiple \reference commands.
+!             ** This is useful if the object belongs to a small specific
+!             object-list as well as a larger more general object-list.
+!
+! Object-level comments:
+!
+!  \memo            Memo describing the object. If multiple lines, start each line
+!                   with \memo.
+!                   Limit line length to 100 characters.
+!
+!  \unique-object   To flag objects which should appear only once in an idf
+!                     (this comment has no "value")
+!
+!  \required-object To flag objects which are required in every idf
+!                     (this comment has no "value")
+!
+!  \min-fields      Minimum number of fields that should be included in the
+!                   object.  If appropriate, the Input Processor will fill
+!                   any missing fields with defaults (for numeric fields).
+!                   It will also supply that number of fields to the "get"
+!                   routines using blanks for alpha fields (note -- blanks
+!                   may not be allowable for some alpha fields).
+!
+!  \obsolete        This object has been replaced though is kept (and is read)
+!                   in the current version.  Please refer to documentation as
+!                   to the dispersal of the object.  If this object is
+!                   encountered in an IDF, the InputProcessor will post an
+!                   appropriate message to the error file.
+!                   usage:  \obsolete New = >[New object name]
+!
+!  \extensible:<\#>  This object is dynamically extensible -- meaning, if you
+!           change the IDD appropriately (if the object has a simple list
+!           structure -- just add items to the list arguments (i.e. BRANCH
+!           LIST). These will be automatically redimensioned and used during
+!           the simulation. <\#> should be entered by the developer to signify
+!           how many of the last fields are needed to be extended (and EnergyPlus
+!           will attempt to auto-extend the object).  The first field of the first
+!           instance of the extensible field set is marked with \begin-extensible.
+!
+!  \begin-extensible See previous item, marks beginning of extensible fields in
+!                   an object.
+!
+!  \format          The object should have a special format when saved in
+!                   the IDF Editor with the special format option enabled.
+!                   The options include SingleLine, Vertices, CompactSchedule,
+!                   FluidProperties, ViewFactors, and Spectral.
+!                   The SingleLine option puts all the fields for the object
+!                   on a single line. The Vertices option is used in objects
+!                   that use X, Y and Z fields to format those three fields
+!                   on a single line.
+!                   The CompactSchedule formats that specific object.
+!                   The FluidProperty option formats long lists of fluid
+!                   properties to ten values per line.
+!                   The ViewFactor option formats three fields related to
+!                   view factors per line.
+!                   The Spectral option formats the four fields related to
+!                   window glass spectral data per line.
+!
+!   \reference-class-name Adds the name of the class to the reference list
+!                   similar to \reference.
+!
+! Group-level comments:
+!
+!  \group          Name for a group of related objects
+!
+!
+! Notes on comments
+! -----------------
+!
+! 1.  If a particular comment is not applicable (such as units, or default)
+! then simply omit the comment rather than indicating N/A.
+!
+! 2.  Memos and notes should be brief (recommend 5 lines or less per block).
+! More extensive explanations are expected to be in the user documentation
+\end{lstlisting}
+
+\subsection{IDD -- IP Units}\label{idd-ip-units}
+
+In addition, the IDD contains indications of IP (inch-pound) units for the EnergyPlus standard SI (Systems International) units. These may be used by input and output interfaces to display values in the IP system. As noted, if the IP units are ``standard'' (first block below), then no \textbackslash{}ip-units is expected in the field. Note that for some fields -- due to their multiple use (for example, schedule values) -- there cannot be a ip-unit designation.
+
+\begin{lstlisting}
+! Default IP conversions (no \ip-units necessary)
+!      $/(m3/s)               = >   $/(ft3/min)         0.000472000059660808
+!      $/(W/K)                = >   $/(Btu/h-F)         0.52667614683731
+!      $/kW                   = >   $/(kBtuh/h)         0.293083235638921
+!      $/m2                   = >   $/ft2               0.0928939733269818
+!      $/m3                   = >   $/ft3               0.0283127014102352
+!      (kg/s)/W                = >   (lbm/sec)/(Btu/hr)  0.646078115385742
+!      1/K                    = >   1/F                 0.555555555555556
+!      1/m                    = >   1/ft                0.3048
+!      A/K                    = >   A/F                 0.555555555555556
+!      C                      = >   F                   1.8 (plus 32)
+!      cm                     = >   in                  0.3937
+!      cm2                    = >   inch2               0.15500031000062
+!      deltaC                 = >   deltaF              1.8
+!      deltaJ/kg              = >   deltaBtu/lb         0.0004299
+!      g/GJ                   = >   lb/MWh              0.00793664091373665
+!      g/kg                   = >   grains/lb           7
+!      g/MJ                   = >   lb/MWh              7.93664091373665
+!      g/mol                  = >   lb/mol              0.0022046
+!      g/m-s                  = >   lb/ft-s             0.000671968949659
+!      g/m-s-K                = >   lb/ft-s-F           0.000373574867724868
+!      GJ                      = >   ton-hrs             78.9889415481832
+!      J                      = >   Wh                  0.000277777777777778
+!      J/K                    = >   Btu/F               526.565
+!      J/kg                   = >   Btu/lb              0.00042986
+!      J/kg-K                 = >   Btu/lb-F            0.000239005736137667
+!      J/kg-K2                = >   Btu/lb-F2           0.000132889924714692
+!      J/kg-K3                = >   Btu/lb-F3           7.38277359526066E-05
+!      J/m2-K                  = >   Btu/ft2-F           4.89224766847393E-05
+!      J/m3                   = >   Btu/ft3             2.68096514745308E-05
+!      J/m3-K                 = >   Btu/ft3-F           1.49237004739337E-05
+!      K                      = >   R                   1.8
+!      K/m                    = >   F/ft                0.54861322767449
+!      kg                     = >   lb                  2.2046
+!      kg/J                   = >   lb/Btu              2325.83774250441
+!      kg/kg-K                = >   lb/lb-F             0.555555555555556
+!      kg/m                   = >   lb/ft               0.67196893069637
+!      kg/m2                  = >   lb/ft2              0.204794053596664
+!      kg/m3                  = >   lb/ft3              0.062428
+!      kg/m-s                  = >   lb/ft-s             0.67196893069637
+!      kg/m-s-K               = >   lb/ft-s-F           0.373316072609094
+!      kg/m-s-K2              = >   lb/ft-s-F2          0.207397818116164
+!      kg/Pa-s-m2             = >   lb/psi-s-ft2        1412.00523459398
+!      kg/s                   = >   lb/s                2.20462247603796
+!      kg/s2                  = >   lb/s2               2.2046
+!      kg/s-m                 = >   lb/s-ft             0.67196893069637
+!      kJ/kg                  = >   Btu/lb              0.429925
+!      kPa                    = >   psi                 0.145038
+!      L/day                  = >   pint/day            2.11337629827348
+!      L/GJ                   = >   gal/kWh             0.000951022349025202
+!      L/kWh                  = >   pint/kWh            2.11337629827348
+!      L/MJ                   = >   gal/kWh             0.951022349025202
+!      lux                    = >   foot-candles        0.092902267
+!      m                      = >   ft                  3.28083989501312
+!      m/hr                   = >   ft/hr               3.28083989501312
+!      m/s                    = >   ft/min              196.850393700787
+!      m/s                    = >   miles/hr            2.2369362920544
+!      m/yr                    = >   inch/yr             39.3700787401575
+!      m2                     = >   ft2                 10.7639104167097
+!      m2/m                   = >   ft2/ft              3.28083989501312
+!      m2/person              = >   ft2/person          10.764961
+!      m2/s                   = >   ft2/s               10.7639104167097
+!      m2-K/W                 = >   ft2-F-hr/Btu        5.678263
+!      m3                     = >   ft3                 35.3146667214886
+!      m3                     = >   gal                 264.172037284185
+!      m3/GJ                  = >   ft3/MWh             127.13292
+!      m3/hr                  = >   ft3/hr              35.3146667214886
+!      m3/hr-m2               = >   ft3/hr-ft2          3.28083989501312
+!      m3/hr-person            = >   ft3/hr-person       35.3146667214886
+!      m3/kg                  = >   ft3/lb              16.018
+!      m3/m2                  = >   ft3/ft2             3.28083989501312
+!      m3/MJ                  = >   ft3/kWh             127.13292
+!      m3/person              = >   ft3/person          35.3146667214886
+!      m3/s                   = >   ft3/min             2118.88000328931
+!      m3/s-m                 = >   ft3/min-ft          645.89
+!      m3/s-m2                = >   ft3/min-ft2         196.85
+!      m3/s-person            = >   ft3/min-person      2118.6438
+!      m3/s-W                 = >   (ft3/min)/(Btu/h)   621.099127332943
+!      N-m                    = >   lbf-in              8.85074900525547
+!      N-s/m2                 = >   lbf-s/ft2           0.0208857913669065
+!      Pa                     = >   psi                 0.000145037743897283
+!      percent/K              = >   percent/F           0.555555555555556
+!      person/m2              = >   person/ft2          0.0928939733269818
+!      s/m                    = >   s/ft                0.3048
+!      V/K                    = >   V/F                 0.555555555555556
+!      W                      = >   Btu/h               3.4121412858518
+!      W/(m3/s)               = >   W/(ft3/min)         0.0004719475
+!      W/K                    = >   Btu/h-F             1.89563404769544
+!      W/m                    = >   Btu/h-ft            1.04072
+!      W/m2                   = >   Btu/h-ft2           0.316957210776545
+!      W/m2                   = >   W/ft2               0.09290304
+!      W/m2-K                 = >   Btu/h-ft2-F         0.176110194261872
+!      W/m2-K2                = >   Btu/h-ft2-F2        0.097826
+!      W/m-K                  = >   Btu-in/h-ft2-F      6.93481276005548
+!      W/m-K2                 = >   Btu/h-F2-ft         0.321418310071648
+!      W/m-K3                 = >   Btu/h-F3-ft         0.178565727817582
+!      W/person               = >   Btu/h-person        3.4121412858518
+!
+! Other conversions supported (needs the \ip-units code)
+!
+!      kPa                    = >   inHg                0.29523
+!      m                      = >   in                  39.3700787401575
+!      m3/s                   = >   gal/min             15850.3222370511
+!      Pa                     = >   ftH2O               0.00033455
+!      Pa                     = >   inH2O               0.00401463
+!      Pa                     = >   inHg                0.00029613
+!      Pa                     = >   Pa                  1
+!      W                      = >   W                   1
+!      W/m2                   = >   W/m2                1
+!      W/m-K                  = >   Btu/h-ft-F          0.577796066000163
+!      W/person               = >   W/person            1
+!
+! Units fields that are not translated
+!      $
+!      1/hr
+!      A
+!      Ah
+!      A/V
+!      Availability
+!      Control
+!      cycles/hr
+!      days
+!      deg
+!      dimensionless
+!      eV
+!      hr
+!      J/J
+!      kg/kg
+!      kg-H2O/kg-air
+!      kmol
+!      kmol/s
+!      m3/m3
+!      minutes
+!      Mode
+!      ms
+!      ohms
+!      percent
+!      ppm
+!      rev/min
+!      s
+!      V
+!      VA
+!      W/m2 or deg C
+!      W/m2, W or deg C
+!      W/s
+!      W/W
+!      years
+! **************************************************************************
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/overview/input-output-descriptions.tex b/doc/input-output-reference/src/overview/input-output-descriptions.tex
new file mode 100644
index 00000000000..8d819662201
--- /dev/null
+++ b/doc/input-output-reference/src/overview/input-output-descriptions.tex
@@ -0,0 +1,160 @@
+\section{Input -- Output Descriptions (Document)}\label{input-output-descriptions-document}
+
+\subsection{Input Descriptions}\label{input-descriptions}
+
+In the descriptions below, the fields for each input object will be described but the Energy+.idd descriptions will not be shown. Refer to the actual Energy+.idd file for complete specifications. Energy+.idd is a text file that can be viewed with many text editors or word processors. The Site:Location object will serve as an example.
+
+\begin{lstlisting}
+Site:Location,
+       \unique-object
+       \min-fields 5
+  A1 , \field Name
+       \required-field
+       \type  alpha
+  N1 , \field Latitude
+       \units deg
+       \minimum -90.0
+       \maximum +90.0
+       \default 0.0
+       \note + is North, - is South, degree minutes represented in decimal (i.e. 30 minutes is .5)
+       \type real
+  N2 , \field Longitude
+       \units deg
+       \minimum -180.0
+       \maximum +180.0
+       \default 0.0
+       \note - is West, + is East, degree minutes represented in decimal (i.e. 30 minutes is .5)
+       \type real
+  N3 , \field Time Zone
+       \note basic these limits on the WorldTimeZone Map (2003)
+       \units hr
+       \minimum -12.0
+       \maximum +14.0
+       \default 0.0
+       \note  Time relative to GMT. Decimal hours.
+       \type real
+  N4 ; \field Elevation
+       \units m
+       \minimum -300.0
+       \maximum< 8900.0
+       \default 0.0
+       \type real
+\end{lstlisting}
+
+The IDD excerpt above is the complete definition as seen in the IDD file.
+
+First, the object name is given. (Site:Location)~ This is followed by a comma in both the definition (IDD) and in an input file (IDF). In fact, all fields except the terminating field of an IDD class object and IDF object are followed by commas. The final field in an IDD class object or in an IDF object is terminated by a semi-colon.
+
+Next is an alpha field, the location name. As noted above, for input, spaces are significant in this field. The main inputs for Site:Location are numeric fields. These are numbered (as is the alpha field) for convenience. The \textbackslash{} designations will show various information about the objects as described above in the IDD conventions discussion. Of importance for reading this document are the units and possible minimum and maximum values for a~ field.
+
+There is automatic processing of the \textbackslash{}minimum, \textbackslash{}maximum and \textbackslash{}default data for numeric fields. Any infractions of the \textbackslash{}minimum, \textbackslash{}maximum fields are automatically detected and messages will appear in the standard error file. After all the input is checked, infractions will cause program termination (before the bulk of the simulation is completed). Defaults are also enforced if you leave the numeric field blank.
+
+Some objects need all the parameters listed by the definition; some do not. In the descriptions that follow, we will try to indicate which parts are optional. Usually, these will be the last fields in the object input or definition. Even if items are not used for a particular object (e.g.~Multiplier in the FenestrationSurface:Detailed and type = Door), the field must be included unless it is the \emph{last field in the object}. So, for this instance, one must include a multiplier field (must be numeric and would need to obey any \textbackslash{}minimum, \textbackslash{}maximum rules) for doors.
+
+Two spreadsheet files are included with the installation:
+
+\begin{itemize}
+\item
+  ExampleFiles.xls -- shows many details about the included example files including highlights of features.
+\item
+  ExampleFiles-ObjectsLink.xls -- shows, for each object, the first three occurrences of that object in an example file.
+\end{itemize}
+
+\subsection{Output Descriptions}\label{output-descriptions}
+
+In the descriptions below, we will endeavor to have each object's output displayed as well as each of the outputs described. The output variables for a run are selected by choosing the Output:VariableDictionary object. This object displays the available output variables for a run on the \textbf{eplusout.rdd} (regular variables) and \textbf{eplusout.mdd} (meter variables) files. Two significant styles are available for these displays and the descriptions below may have one for some objects and another for other objects. The variables are the same but will look a bit different.~ For clarity, the two displays are shown below:
+
+Note that the IDF-Editor can interpret both sets of files and assist you in getting output variables into your input files. But you will have to successfully run your input file first.
+
+The Simple (or regular) display looks like the following figure and is interpreted:
+
+\textbf{Zone/HVAC} -- when the output is produced at the ``Zone'' timestep (ref: number of timesteps in each hour) or at the ``HVAC'' aka System timestep (which can vary for each hour).
+
+\textbf{Average/Sum} -- whether this is a averaged value over the reporting period (such as a temperature or rate) or whether this is a summed value over the reporting period. Reporting periods are specified in the Output:Variable or Output:Meter objects.
+
+\textbf{\textless{}Variable Name\textgreater{}} -- The variable name one uses for reporting is displayed (e.g., Site Outdoor Drybulb Temperature) along with the units (e.g., {[}C{]}).
+
+Example from the \textbf{eplusout.rdd} file:
+
+\begin{itemize}
+\item
+  Zone,Average,Site Outdoor Air Drybulb Temperature {[}C{]}
+\item
+  Zone,Average,Site Outdoor Air Dewpoint Temperature {[}C{]}
+\item
+  Zone,Average,Site Outdoor Air Wetbulb Temperature {[}C{]}
+\item
+  Zone,Average,Site Outdoor Air Humidity Ratio {[}kgWater/kgAir{]}
+\item
+  Zone,Average,Site Outdoor Air Relative Humidity {[}\%{]}
+\item
+  Zone,Average,Site Outdoor Air Barometric Pressure {[}Pa{]}
+\item
+  Zone,Average,Wind Speed {[}m/s{]}
+\item
+  Zone,Average,Site Wind Direction {[}deg{]}
+\item
+  Zone,Average,Site Sky Temperature {[}C{]}
+\item
+  HVAC,Sum,Zone Air System Sensible Heating Energy {[}J{]}
+\item
+  HVAC,Sum,Zone Air System Sensible Cooling Energy {[}J{]}
+\item
+  HVAC,Average,Zone Air System Sensible Heating Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air System Sensible Cooling Rate {[}W{]}
+\item
+  HVAC,Average,Zone Air Temperature {[}C{]}
+\item
+  HVAC,Average,Zone Thermostat Air Temperature {[}C{]}
+\end{itemize}
+
+Note that the \textbf{eplusout.mdd} file is similar, but meters are only available at the Zone timestep.
+
+\begin{itemize}
+\item
+  Zone,Meter,Electricity:Facility {[}J{]}
+\item
+  Zone,Meter,ExteriorLights:Electricity {[}J{]}
+\item
+  Zone,Meter,Grounds Lights:ExteriorLights:Electricity {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Facility {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Building {[}J{]}
+\item
+  Zone,Meter,EnergyTransfer:Zone:R13WALL WALLS {[}J{]}
+\end{itemize}
+
+The IDF display has all the same information in an IDF-ready form (i.e., you could copy and paste it into your input file using a text editor).
+
+Example from the \textbf{eplusout.rdd} file:
+
+\begin{itemize}
+\item
+  Output:Variable,*,Site Outdoor Air Drybulb Temperature,hourly; !- Zone Average {[}C{]}
+\item
+  Output:Variable,*,Site Outdoor Air Dewpoint Temperature,hourly; !- Zone Average {[}C{]}
+\item
+  Output:Variable,*,Site Outdoor Air Wetbulb Temperature,hourly; !- Zone Average {[}C{]}
+\item
+  Output:Variable,*,Site Outdoor Air Humidity Ratio,hourly; !- Zone Average {[}kgWater/kgAir{]}
+\item
+  Output:Variable,*,Site Outdoor Air Relative Humidity,hourly; !- Zone Average {[}\%{]}
+\item
+  Output:Variable,*,Site Outdoor Air Barometric Pressure,hourly; !- Zone Average {[}Pa{]}
+\item
+  Output:Variable,*,Zone Air System Sensible Heating Energy,hourly; !- HVAC Sum {[}J{]}
+\item
+  Output:Variable,*,Zone Air System Sensible Cooling Energy,hourly; !- HVAC Sum {[}J{]}
+\item
+  Output:Variable,*,Zone Air System Sensible Heating Rate,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,Zone Air System Sensible Cooling Rate,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,Zone Air Temperature,hourly; !- HVAC Average {[}C{]}
+\item
+  Output:Variable,*,Zone Thermostat Air Temperature,hourly; !- HVAC Average {[}C{]}
+\end{itemize}
+
+All of the same information appears in a slightly different form and defaults to ``hourly'' reporting frequency (which, of course, can be changed when you put it into your input file). The ``*'' is preselected so that you would be reporting for all those items.
diff --git a/doc/input-output-reference/src/overview/what-s-different-about-energyplus-input.tex b/doc/input-output-reference/src/overview/what-s-different-about-energyplus-input.tex
new file mode 100644
index 00000000000..a172026d0c5
--- /dev/null
+++ b/doc/input-output-reference/src/overview/what-s-different-about-energyplus-input.tex
@@ -0,0 +1,67 @@
+\section{What's different about EnergyPlus Input and Output?}\label{whats-different-about-energyplus-input-and-output}
+
+The usual procedure for non-interactive programs is to process all the input necessary to ``do the job'', perform the actions required by the input, and somewhere along the way produce reports on the actions. Usually, there will be error messages on incorrect input statements and/or incorrect conditions detected during processing. Usually, the input is echoed in its entirety so that the context of errors is shown clearly.
+
+Results are typically output into reports as well as a compilation of various inputs reformatted into different groupings than were originally entered (defaults filled in, etc.)
+
+EnergyPlus does all the above. However, some nuances are different from the usual actions.
+
+\subsection{EnergyPlus Input Processing}\label{energyplus-input-processing}
+
+1)~~~~EnergyPlus reads the data dictionary (Energy+.idd) and the input data file (in.idf) prior to doing anything else. Only after this is done does processing start. HOWEVER, the input processor only knows as much as the data dictionary has told it. It knows which fields should be alpha and which should be numeric. All of this information (including the IDD) is echoed to the audit file (audit.out) in case errors occur. Most of the errors show up (out of context) in the standard error file (eplusout.err) -- there might be enough information to decipher where the error is or you may have to look at the more inclusive audit file. Invalid numeric fields are detected during this processing and default numeric fields are filled. For more information on the IDD, its structure and implications, please see the IDD Conventions discussion below.
+
+2)~~~~The biggest difference between EnergyPlus and more traditional input processing is that EnergyPlus is modular in its actual filling in the details for the simulation. Because of the modular structure of EnergyPlus, each module is responsible for ``getting'' its own input. It receives this input from the input processor in the form of alpha and numeric fields. Each module typically gets all its input the first time it is called. The implication for the user is that error messages may show up in somewhat peculiar places. A further implication is that no order is needed in the input data file!~ Data that is not needed by a particular simulation is not processed.
+
+3)~~~~The data dictionary has the capability to do ``automatic'' range checking on numeric fields as well as fill in numeric defaults. Both filling in defaults and ``automatic'' range checking are done when the data is read. Other checks may need a combination of fields and won't be done until the data is ``processed'' (after the simulation starts).
+
+4)~~~~A couple of other differences that might not be true in other programs:~ Blanks are significant in alpha fields \textbf{SO} DesignDay is not the same as Design Day (1 space between Design and Day) nor Design~ Day (2 spaces between Design and Day). Alpha objects, however, \emph{are} case insensitive SO DesignDay is the same as `designday' or `SizingPeriod:DesignDay'.
+
+\subsection{General Input Rules}\label{general-input-rules}
+
+Rules shown here are for the input data files. Rules about the Input Data Dictionary are shown in the Interface Developer's Guide (there is much similarity and overlap) but most users don't need to touch the IDD (Input Data Dictionary).
+
+The input data file is the primary file that EnergyPlus uses to create the building simulation. The only additional files are referenced by certain objects (such as the Schedule:File object). The input is order-independent; data can appear in any order and will be retrieved and sorted as necessary by the EnergyPlus simulation modules.~ In addition, EnergyPlus allocates everything dynamically, so there are no limitations as to number of zones, surfaces, etc.
+
+\begin{itemize}
+\item
+  The initial line of an input object MUST have a comma or semicolon.
+\item
+  Fields do not extend over line boundaries.~ Usually, if a comma or (as appropriate) semi-colon is not the last field value on a line, one will be inserted.~ Of course, several fields may appear on a single line as long as they are comma separated. (And the last could be followed by a semi-colon).
+\item
+  Commas delimit fields -- therefore, no fields can have embedded commas.~ No error will occur but you won't get what you want. You cannot surround a field with `` to accommodate commas in the fields.
+\item
+  Blank lines are allowed.
+\item
+  The comment character is a exclamation ``!''.~ Anything on a line after the exclamation is ignored.
+\item
+  Input records (aka input line length) can be up to 500 characters in length.~ If you go over that, no error will occur but you won't get what you want.
+\item
+  Each Alpha string in the input data file (aka alpha field length) can be up to 100 characters in length. Anything beyond that is truncated. This would apply to all names (such as zone name, node name, schedule name) in fields.
+\item
+  Each Alpha string (including Section and Class/Object keywords) is mapped to UPPER case during processing, unless the ``\emph{retaincase}'' flag marks the field in the IDD.~ Get routines from the EnergyPlus code that use the Section and Object keywords automatically map to UPPER case for finding the item.~ The primary drawback with this is that error messages coming out of the input processor will be in UPPER case and may not appear exactly as input.
+\item
+  Special characters, such as tabs, should NOT be included in the file.~ However, tabs can be accommodated and are turned into spaces.
+\item
+  All numbers can be flexibly input and are processed into single precision variables (i.e.~1.0, 1.000, 1, .1E+1 are all processed equally).
+\end{itemize}
+
+\subsection{EnergyPlus Output Processing}\label{energyplus-output-processing}
+
+\begin{enumerate}
+  \item
+    Unlike the usual formatted output text formatted reports, EnergyPlus usual output is either at the summary or at the detailed (variable) level. Summary reports exist for many inputs as well as sizing results. The more detailed variable level reporting is produced as ``stream of consciousness'' (as the simulation happens) and must be post-processed for more sensible viewing. Note that the terms ``output variable'' and ``output variable'' (accessed by the Output:Variable and/or Output:Meter objects) are used interchangably in this document.
+  \item
+    Most EnergyPlus reporting can be readily viewed in current spreadsheet programs -- or other software that can process ``delimited variable'' reports. In these kind of reports, each ``column'' is separated from the next by a ``delimiter''. Typical delimiters are ``comma'' and ``tab''. Gradually, EnergyPlus reporting is moving from all comma separated reports to allow the user to select the delimiter via ``style'' objects.
+  \item
+    Styled reports allow for more selectable output reporting but also increase the number of output files as we have chosen to create the report names with extensions that typify the actual reporting. Depending on the reporting, these can be:
+    \begin{itemize}
+      \item
+        Tab -- reports with a .tab extension have tabs as the delimiter. These report files (directly from EnergyPlus) will be named something like ``eplus\textless{}xxx\textgreater{}.tab'' where the \textless{}xxx\textgreater{} is a short name of the kind of report (e.g.~Zsz for Zone Sizing, Map for Daylighting Map)
+      \item
+        Csv -- reports with a .csv extension have commas as the delimiter. These are also specially formatted for use in spreadsheets (such as the compilation of results from the eplusout.eso file into the eplusout.csv file using the default post-processor program).
+      \item
+        Txt -- reports with a .txt extension have spaces as the ``delimiter'' but only certain of these are really formatted the way you might expect: where multiple spaces make printing with a non-proportional font would produce readable output.
+      \item
+        Html -- reports with a .html extension are ``web-browser'' ready.
+    \end{itemize}
+\end{enumerate}
diff --git a/doc/input-output-reference/src/parametric-objects.tex b/doc/input-output-reference/src/parametric-objects.tex
new file mode 100644
index 00000000000..7a5fa5d8136
--- /dev/null
+++ b/doc/input-output-reference/src/parametric-objects.tex
@@ -0,0 +1,399 @@
+\chapter{Parametric Objects}\label{parametric-objects}
+
+\section{Group -- Parametrics}\label{group-parametrics}
+
+In order to assess a group of alternatives, the Parametric objects can be used in a single file as an alternative of maintaining a group of files with small differences. Updating portions of the multiple files that do not change between permutations becomes tedious and error prone and may lead to incorrect conclusions concerning the energy savings of specific measures. The ParametricPreprocessor.exe program (described in the AuxiliaryPrograms document) interprets the following objects in a single file and creates the group of files automatically. The objects in the group are:
+
+\begin{itemize}
+\item
+  Parametric:SetValueForRun
+\item
+  Parametric:Logic
+\item
+  Parametric:RunControl
+\item
+  Parametric:FileNameSuffix
+\end{itemize}
+
+A simple example of part of an IDF file is shown below:
+
+\begin{lstlisting}
+
+  Parametric:SetValueForRun,
+      $insDepth,                  !- Parameter Name
+      0.0508,                     !- Value 1
+      0.0762,                     !- Value 2
+      0.1016,                     !- Value 3
+      0.1270;                     !- Value 4
+
+
+    Material,
+      IN1,                     !- Name
+      VeryRough,               !- Roughness
+      = $insDepth,              !- Thickness {m}
+      2.3000000E-02,           !- Conductivity {W/m-K}
+      24.00000,                !- Density {kg/m3}
+      1590.000,                !- Specific Heat {J/kg-K}
+      0.9000000,               !- Thermal Absorptance
+      0.5000000,               !- Solar Absorptance
+      0.5000000;               !- Visible Absorptance
+\end{lstlisting}
+
+In this example, the parameter \$insDepth is used in the Material object to describe the thickness of the material, in this case insulation.~ For the first simulation, \$insDepth is set to 0.0508 (2 inches) shown as the first value in the Parametric:SetValueForRun object. This value is then substituted in where ever the \$insDepth is shown in the file, in this example, in the Material object. The simulation would use this first value and produce a set of results based on this insulation thickness. The second simulation would use the second value of the Parametric:SetValueForRun object of 0.0762 (3 inches) for the thickness of the insulation described in the Material object. This would then be simulated with a second set of results. This would be repeated a third time with 0.1015 (4 inches) and 0.1270 (5 inches) of insulation.
+
+A new IDF file is created for each of these simulations and is named the original name of the file plus either a number or a user defined suffix (if Parametric:FileNameSuffix is used). Looking at how these created IDF files show the substituted values can help understand problems that may occur.
+
+The `` = \$insDepth'' is a simple substation but could also be a more complex expression involving operators and predefined functions such as
+
+~ = \$insDepth * 1.1 + 0.0004 * SQRT(12)
+
+Many sets of simulations can be defined just using different Parametric:SetValueForRun objects but for more advanced sets of parametric runs, the Parametric:Logic object can be used to perform additional calculations, logical operations, and to exclude entire objects in the file. The Parametric:RunControl allows individual runs to be performed or not. The Parametric:FileNameSuffix object controls the naming of the resulting sets of output files.
+
+\subsection{Expressions}\label{expressions}
+
+Expressions can occur anywhere in the IDF file as a field value if the expression begins with an equals sign ( = ) and can also occur in assignment statements in the Parametric:Logic object. The operators include: +, -, *, /, \^{} (exponent), \&\& (and), \textbar{}\textbar{} (or), = = , \textgreater{}, \textless{}, \textless{} = , \textgreater{} = ,~ \textless{}\textgreater{}, and //. These are computed using standard operator precedence rules. The parenthesis are used to execute sub-expressions with higher precedence. Some built in functions, such as ABS, ACOS, ASIN, ATAN, COS, EXP, INT, LEN, LOG, MOD, NOT, SIN, SQRT, TAN are supported in expressions. Theses built in functions all take a single argument.
+
+\subsection{Processing Order}\label{processing-order}
+
+The order that the parameters are processed is important to understand their values. Like other objects in EnergyPlus, the order that they occur in the file is not important.~ The order of evaluation is:
+
+1)~~~~Parameter values are based on Parametric:SetValueForRun
+
+2)~~~~All lines of the Parametric:Logic object are evaluated
+
+3)~~~~All embedded expressions in the file are evaluated
+
+\subsection{Parametric:SetValueForRun}\label{parametricsetvalueforrun}
+
+The core parametric object is Parametric:SetValueForRun which sets the parameters value to different values depending on which run is being simulated.
+
+For example
+
+\begin{lstlisting}
+
+Parametric:SetValueForRun
+    $ConstructionToUse,  !- Parameter Name
+    TiltUpConcreteWall,  !- Value for run 1
+    BlockWall,           !- Value for run 2
+    SteelFrameWall,      !- Value for run 3
+    WoodFrameWall;       !- Value for run 4
+
+
+  Parametric:SetValueForRun
+    $WallRValue,           !- Parameter Name
+    5,                     !- Value for run 1
+    8,                     !- Value for run 2
+    11,                    !- Value for run 3
+    17;                    !- Value for run 4
+\end{lstlisting}
+
+Using Parametric:SetValueForRun, the value is set based on the which run number is currently being simulated. Multiple objects can be used and a set of parameter values would be defined for a given simulation. For example, the 3rd simulation would assign the ``Value 3'' value, 11, to the parameter \$WallRValue and the ``Value 3'' value, ``SteelFrameWall'' to \$ConstructionToUse. Since many Parametric:SetValueForRun objects can be used at once, all of the~ 3rd values would be assigned to the appropriate parameters. In IDF Editor, this object will appear as a table of values with each row being all the parameter values for a specific simulation and each column belonging to a specific parameter.
+
+\subsubsection{Inputs}\label{inputs-030}
+
+\paragraph{Field: Parameter Name}\label{field-parameter-name}
+
+The name of the parameter. It must begin with the dollar sign character, and the second character must be a letter. The parameter name, unlike a typical EnergyPlus name, cannot contain spaces or any characters other than letters and numerals.
+
+\paragraph{Field: Value for run n}\label{field-value-for-run-n}
+
+The value that should be substituted for the parameter on the n-th simulation. If multiple Parametric:SetValueForRun objects exist and they have different number of fields, the last field value will be used for the remaining field values. This means that to set all values the same, only the first value needed to be entered.
+
+\subsection{Parametric:Logic}\label{parametriclogic}
+
+The approach of using parameters and expressions, by itself, is very flexible and allows for many possible parametric simulations but it does not allow for objects to be included for some parametric cases and not others. For example, you might want an overhang on a window in some parametric runs and not others. The Parametric:Logic object can help in that scenario.
+
+A single Parametric:Logic object is allowed per file. It has a freeform syntax including IF and SELECT blocks with each field in the object representing a single ``line'' of code. Essentially, this logic object looks like simple programming code.
+
+\begin{lstlisting}
+
+Parametric:Logic,
+    Main,                            !- name
+    IF $insDepth < 0.1,              !- parametric logic line 1
+       DISABLE “MaterialWallBoard�,  !- parametric logic line 2
+       DISABLE “MaterialExtFinish�,  !- parametric logic line 3
+    ENDIF;                           !- parametric logic line 4
+\end{lstlisting}
+
+In addition, lines could contain assignment statements in the form of
+
+parameter~ = expression such as the second control line in the following example.
+
+\begin{lstlisting}
+
+Parametric:Logic,
+    Main,                              !- name
+    PARAMETER $THICKNESS,              !- parametric logic line 1
+    $THICKNESS = 0.01 * $CMDEPTH,      !- parametric logic line 2
+    IF $THICKNESS > 0.5,               !- parametric logic line 3
+       DISABLE “MaterialWallBoard�,    !- parametric logic line 4
+       DISABLE “MaterialExtFinish�,    !- parametric logic line 5
+    ENDIF;                             !- parametric logic line 6
+\end{lstlisting}
+
+The statements include PARAMETER, IF, ELSE, ELSEIF, ENDIF, SELECT, CASE, DEFAULT, ENDSELECT, ENABLE, DISABLE, and REMARK. Nested IF and SELECT statements are allowed.~ All objects are enabled until they are specifically disabled using the DISABLE statement and could be later re-enabled with ENABLE. An object that is named with the DISABLE statement would not appear in that simulation run.
+
+The PARAMETER statement declares the name of the parameter. It is necessary that every parameter used in the Parametric:Logic object be initialized using the PARAMETER statement unless the parametes are created using the Parametric:SetValueForRun object. Requiring explicit parameter declaration reduces errors in software programming. Parameter names would not be case sensitive.
+
+The DISABLE and ENABLE commands can have one or two arguments. If a second argument is present it is the kind of object.
+
+\begin{lstlisting}
+DISABLE “MaterialWallBoard� “Material�,    !- parametric control line 4
+\end{lstlisting}
+
+The following sections describe each type of statement in more detail.
+
+\subsubsection{Inputs}\label{inputs-1-027}
+
+\paragraph{IF ENDIF Block}\label{if-endif-block}
+
+As previously shown, the simplest IF block is in the form of
+
+\begin{lstlisting}
+
+IF <conditional-expression>
+    <true-block-of-statements>
+  ENDIF
+\end{lstlisting}
+
+The \textless{}conditional-expression\textgreater{} usually contains a logical comparison operator such as:
+
+\begin{itemize}
+\item
+  ~ = = equal
+\item
+  ~ \textgreater{} greater than
+\item
+  ~ \textless{} less than
+\item
+  ~ \textless{} = less than or equal to
+\item
+  ~ \textgreater{} = greater than or equal to
+\item
+  ~ \textless{}\textgreater{} not equal to
+\end{itemize}
+
+The \textless{}true-block-of-statements\textgreater{} can contain other statements including other lines of IF and ENDIF. These statement are only executed when the \textless{}conditional-expression\textgreater{} evaluates to true. If the \textless{}conditional-expression\textgreater{} is false, none of the statements before the ENDIF are executed and instead execution begins again with the statement after the ENDIF statement.
+
+\paragraph{IF ELSE~ ENDIF Block}\label{if-else-endif-block}
+
+Another form of the IF block can contain the ELSE statement:
+
+\begin{lstlisting}
+
+IF <conditional-expression>
+    <true-block-of-statements>
+  ELSE
+    <false-block-of-statements>
+  ENDIF
+\end{lstlisting}
+
+Like the simpler IF ENDIF form the \textless{}conditional-expression\textgreater{} is computed and the \textless{}true-block-of-statements\textgreater{} are executed if it is true. The additional feature of this form is that if the \textless{}conditional-expression\textgreater{} is false, the \textless{}false-block-of-statements\textgreater{} is executed instead of the \textless{}true-block-of-statements\textgreater{}.
+
+\paragraph{IF ELSEIF ELSE ENDIF Block}\label{if-elseif-else-endif-block}
+
+The most complex form of the IF block contains both ELSEIF statement (or statements)~ and the ELSE statement:
+
+\begin{lstlisting}
+
+IF <conditional-expression-1>
+    <true-block-of-statements-1>
+  ELSEIF <conditional-expression-2>
+    <true-block-of-statements-2>
+  ELSEIF <conditional-expression-2>
+    <true-block-of-statements-2>
+  ELSE
+    <false-block-of-statements>
+  ENDIF
+\end{lstlisting}
+
+This form allows more complex logic to be expressed. If the \textless{}conditional-expression-1\textgreater{} is true then \textless{}true-block-of-statements-1\textgreater{} executed and when that is complete, execution resumes after the ENDIF statement. If \textless{}conditional-expression-1\textgreater{} is false then the ELSEIF \textless{}conditional-expression-2\textgreater{} is evaluated and if that is true then \textless{}true-block-of-statement-2\textgreater{} is executed. On the other hand, if \textless{}conditional-expression-2\textgreater{} is~ false, then the next ELSEIF conditional expression is evaluated following the same patter if another ELSEIF is present, otherwise, the \textless{}false-block-of-statements\textgreater{} after the ELSE are executed. Another way of thinking of this block is that the conditional expressions are evaluated from the top to the bottom until one is found to be true and then the associated block of statements are executed. If none of the conditional expressions is true, the \textless{}false-block-of-statements\textgreater{} are executed.
+
+\paragraph{SELECT CASE DEFAULT ENDSELECT Block}\label{select-case-default-endselect-block}
+
+The SELECT block is related to the IF block but is for the specific case of trying to match a variable with several specific values. The form of the SELECT block is:
+
+\begin{lstlisting}
+
+SELECT <expression>
+  CASE <constant-1>
+    <case-block-of-statements-1>
+  CASE <constant-2>
+    <case-block-of-statements-2>
+  CASE <constant-3>
+    <case-block-of-statements-3>
+  DEFAULT
+    <default-block-of-statements>
+  ENDSELECT
+\end{lstlisting}
+
+With any number of CASE statements. The \textless{}expression\textgreater{} is evaluated and compared to the constants with each CASE statement. If a match is found the corresponding \textless{}case-block-of-statements\textgreater{} are executed otherwise if no match if found the \textless{}default-block-of-statements\textgreater{} is excecuted. One one matching CASE statement for each SELECT block is executed. An example of how this works is shown below:
+
+\begin{lstlisting}
+
+Parametric:SetValueForRun,
+    $EndMonth,
+    2;
+
+
+  Parametric:Logic,
+    Main2,
+    PARAMETER $EndDay,
+    SELECT $EndMonth,
+     CASE 1,
+      $EndDay = 31,
+     CASE 2,
+      $EndDay = 28,
+     CASE 3,
+      $EndDay = 31,
+     CASE 4,
+      $EndDay = 30,
+     CASE 5,
+      $EndDay = 31,
+     CASE 6,
+      $EndDay = 30,
+     CASE 7,
+      $EndDay = 31,
+     CASE 8,
+      $EndDay = 31,
+     CASE 9,
+      $EndDay = 30,
+     CASE 10,
+      $EndDay = 31,
+     CASE 11,
+      $EndDay = 30,
+     CASE 12,
+      $EndDay = 31,
+     DEFAULT,
+      $EndDay = 30,
+     ENDSELECT;
+\end{lstlisting}
+
+With this example the \$EndDay value would be set to 28.
+
+\paragraph{ENABLE DISABLE}\label{enable-disable}
+
+The ENABLE and DISABLE statements specifically are for removing (and not removing) other objects that appear in the EnergyPlus IDF file. It has two syntaxes:
+
+\begin{lstlisting}
+
+DISABLE <objectname>
+\end{lstlisting}
+
+and
+
+\begin{lstlisting}
+
+DISABLE <objectname>, <kind-of-object>
+\end{lstlisting}
+
+The DISABLE statement removes the object identified with either \textless{}objectname\textgreater{} or the combination of \textless{}objectname\textgreater{} and \textless{}kind-of-object\textgreater{} if the \textless{}objectname\textgreater{} is not unique in the EnergyPlus input file. By default, all objects are enabled in the input file. Objects need to be specifically disabled using the DISABLE statement. After an object is disabled in can later be re-enabled with the ENABLE statement which has similar syntax.
+
+\begin{lstlisting}
+
+DISABLE <objectname>
+\end{lstlisting}
+
+and
+
+\begin{lstlisting}
+
+DISABLE <objectname>, <kind-of-object>
+\end{lstlisting}
+
+\begin{lstlisting}
+
+  Parametric:Logic,
+      Main,
+      DISABLE  "SOUTH WALL OVERHANG";
+
+
+    Shading:Zone:Detailed,
+      SOUTH WALL OVERHANG,     !- Name
+      ZONE SURFACE SOUTH,      !- Base Surface Name
+      SCH 2,                   !- Transmittance Schedule Name
+      4,                       !- Number of Vertices
+      0.0,-1.0,3.0,  !- X,Y,Z = = > Vertex 1 {m}
+      0.0,0.0,3.0,  !- X,Y,Z = = > Vertex 2 {m}
+      4.0,0.0,3.0,  !- X,Y,Z = = > Vertex 3 {m}
+      4.0,-1.0,3.0;  !- X,Y,Z = = > Vertex 4 {m}
+\end{lstlisting}
+
+An object that is named with the DISABLE statement would not appear in that simulation run.
+
+\paragraph{REMARK}\label{remark}
+
+The REMARK statement is simply a way to include a comment in the Parametric:Logic fields. The text that follows the REMARK statement is ignored.
+
+\paragraph{OBJECT DEFINITION}\label{object-definition}
+
+The definition of the Parametric:Logic object is shown below:
+
+\paragraph{Field: Name}\label{field-name-029}
+
+The name of the Parametric:Logic object.
+
+\paragraph{Field: Parametric Logic Line n}\label{field-parametric-logic-line-n}
+
+The line that contains one statement in one of the following forms:
+
+\begin{itemize}
+\item
+  \textless{}parameter\textgreater{} = \textless{}expression\textgreater{}
+\item
+  PARAMETER \textless{}parameter\textgreater{}
+\item
+  IF \textless{}expression\textgreater{}
+\item
+  ELSEIF \textless{}expression\textgreater{}
+\item
+  ELSE
+\item
+  ENDIF
+\item
+  SELECT \textless{}expression\textgreater{}
+\item
+  CASE \textless{}constant\textgreater{}
+\item
+  DEFAULT
+\item
+  ENDSELECT
+\item
+  ENABLE \textless{}constant\textgreater{}
+\item
+  ENABLE \textless{}constant\textgreater{} \textless{}constant\textgreater{}
+\item
+  DISABLE \textless{}constant\textgreater{}
+\item
+  DISABLE \textless{}constant\textgreater{} \textless{}constant\textgreater{}
+\item
+  REMARK \textless{}text to ignore\textgreater{}
+\end{itemize}
+
+\subsection{Parametric:RunControl}\label{parametricruncontrol}
+
+The following Parametric:RunControl object controls which runs are simulated. The series of entries indicate if the run should be performed or not. This object is optional and if it is not included all runs are performed.
+
+\subsubsection{Inputs}\label{inputs-2-025}
+
+\paragraph{Field: Name}\label{field-name-1-026}
+
+The name of the optional Parametric:RunControl object.
+
+\paragraph{Field: Perform run n}\label{field-perform-run-n}
+
+The value of the field can be either a yes or no.~ It cannot contain a parameter.
+
+\subsection{Parametric:FileNameSuffix}\label{parametricfilenamesuffix}
+
+The file name of the IDF files that are created for each run and the output files for each run are based on the name of the file plus a ``suffix''. The suffixes can be defined using the Parametric:FileNameSuffix object or if the object is missing will default to the run number.
+
+\subsubsection{Inputs}\label{inputs-3-023}
+
+\paragraph{Field: Name}\label{field-name-2-024}
+
+The name of the optional Parametric:FileNameSuffix object.
+
+\paragraph{Field: Suffix for file name in run n}\label{field-suffix-for-file-name-in-run-n}
+
+The value of the field is added to the IDF file name to create the resulting IDF file and output files.~ It cannot contain a parameter.
diff --git a/doc/input-output-reference/src/running-energyplus.tex b/doc/input-output-reference/src/running-energyplus.tex
new file mode 100644
index 00000000000..792fc58dda5
--- /dev/null
+++ b/doc/input-output-reference/src/running-energyplus.tex
@@ -0,0 +1,29 @@
+\chapter{Running EnergyPlus}\label{running-energyplus}
+
+EnergyPlus is written in C++, using many C++11 features. It runs as a console application on Windows, Mac, and Linux (tested on latest Ubuntu LTS). Details on running EnergyPlus are available in a separate document (Running EnergyPlus in Auxiliary Programs). The following files are needed to run EnergyPlus:
+
+\begin{itemize}
+\tightlist
+\item
+  EnergyPlus.exe (the executable file)
+\item
+  Energy+.ini (described below)
+\item
+  Energy+.idd (the input data dictionary file)
+\item
+  in.idf (the input file)
+\item
+  in.epw -- optional (weather data file)
+\end{itemize}
+
+The input data dictionary and input data file have been discussed in the previous sections of this document.
+
+For weather simulations, EnergyPlus accepts EnergyPlus weather files. The actual file name is \textbf{in.epw}.
+
+The usual release for Windows platform also includes a dependence on a shared library, EnergyPlusAPI.dll (.so on Linux).
+
+\input{src/running-energyplus/energy-ini}
+
+\input{src/running-energyplus/errors}
+
+\input{src/running-energyplus/energyplus-execution-time}
diff --git a/doc/input-output-reference/src/running-energyplus/energy-ini.tex b/doc/input-output-reference/src/running-energyplus/energy-ini.tex
new file mode 100644
index 00000000000..1d00537cfd6
--- /dev/null
+++ b/doc/input-output-reference/src/running-energyplus/energy-ini.tex
@@ -0,0 +1,40 @@
+\section{Energy+.ini}\label{energy.ini}
+
+The Energy+.ini file is read by the EnergyPlus.exe program and is \emph{very important} to the simulation run. In specific, this file contains a pointer to where the Energy+.idd file will be found. More description of the Energy+.ini contents is contained in the Auxiliary Programs document.
+
+For the advanced user, there is also the ``EPMacro'' program, described in the Auxiliary programs document. You run it as a separate program before EnergyPlus (the batch file included in the install and shown in the GettingStarted document contains the commands). It is automatically run if you use the EP-Launch program.
+
+EnergyPlus may create several output files. Whether some files are produced depends on the actual simulation (for example, the .rdd file is only produced when you request a Variable Dictionary using the Output:Report object). Similarly, the .dxf file is only produced when a DXF surface report is requested. Common output files are shown in the following table. A complete, up to date list is shown in the ``Output Details and Examples Document''.
+
+% table 47
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{EnergyPlus Output Files \label{table:energyplus-output-files}} \tabularnewline
+\toprule 
+FileName & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{EnergyPlus Output Files} \tabularnewline
+\toprule 
+FileName & Description \tabularnewline
+\midrule
+\endhead
+
+Eplusout.audit & Echo of input \tabularnewline
+Eplusout.err & Error file \tabularnewline
+Eplusout.eso & Standard Output File (contains results from both Output:Variable and Output:Meter objects). \tabularnewline
+Eplusout.eio & One time output file \tabularnewline
+Eplusout.rdd & Output variable Data Dictionary \tabularnewline
+Eplusout.dxf & DXF (from Output:Report,Surfaces,DXF;) \tabularnewline
+Eplusout.mtr & Similar to .eso but only has Meter outputs. \tabularnewline
+Eplusout.mtd & Meter details report – what variables are on what meters and vice versa. \tabularnewline
+Eplusout.end & A one line summary of success or failure (useful for Interface programs) \tabularnewline
+Eplusout.dbg & From Debug Output object – may be useful to support to help track down problems \tabularnewline
+Eplusout. < ext > & Not directly from EnergyPlus – produced by utility programs that read the .eso file and produce output files for spreadsheet programs \tabularnewline
+Eplusout.sln & Similar to DXF output but less “formatted�. Results of Report Surface, Lines object. \tabularnewline
+Epluszsz. < ext > & Results from the Zone Sizing object with extension noted by the Sizing Style object. This file is “spreadsheet� ready. \tabularnewline
+Eplusssz. < ext > & Results from the System Sizing object with extension noted by the Sizing Style object. This file is “spreadsheet� ready. \tabularnewline
+Eplusout.bnd & This file contains details about the nodes and branches. Useful in determining if all your nodes are connected correctly. \tabularnewline
+Eplustbl. < ext > & Results from various “Report Table� and a few other reporting commands. The extension is from the “style� command and this file is “spreadsheet� ready. \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/input-output-reference/src/running-energyplus/energyplus-execution-time.tex b/doc/input-output-reference/src/running-energyplus/energyplus-execution-time.tex
new file mode 100644
index 00000000000..3b715bf39c0
--- /dev/null
+++ b/doc/input-output-reference/src/running-energyplus/energyplus-execution-time.tex
@@ -0,0 +1,26 @@
+\section{EnergyPlus Execution Time}\label{energyplus-execution-time}
+
+Extensive timing studies and fine-tuning of EnergyPlus are an ongoing process. Remember that hourly simulations cannot be directly compared to EnergyPlus with its less than hourly timesteps.
+
+\subsection{Reducing Run Time Tips}\label{reducing-run-time-tips}
+
+Compared with creating energy models either by hand coding the IDF file or by using GUI tools or a combination of both, EnergyPlus run time is normally a small fraction of the total time needed to complete an energy modeling job. Therefore it is very important to build a clean and concise EnergyPlus model up front. Techniques of simplifying large and complex building and systems should be used during the creation of energy models, especially during the early design process when detailed zoning and other information is not available. Producing lots of hourly or sub-hourly reports from EnergyPlus runs can take significant amount of time. Modelers should only request time step reports when necessary. On the other hand, producing summary reports and typical monthly reports take relatively small amount of run time. These reports are valuable references for troubleshooting and model fine tuning.
+
+With powerful personal computers get more and more affordable, EnergyPlus modelers should choose to use current available PCs with 3 or more GHZ and 3 or more GB of RAM. For a large volume of EnergyPlus parametric runs, modelers can launch multiple runs in parallel. For modelers, most time is spent on troubleshooting and fine tuning energy models. During the early modeling process, it is recommended to keep the model as simple as possible and make quick runs to identify problems. Then modify the IDF file to fix problems and re-run the model. This is an iterative process until satisfactory solutions are found. The simulation process can be split into three phases: the diagnostic runs, the preliminary runs, and the final runs. The three phases would use different simulation settings. The diagnostic runs would use a set of simulation settings to speed up the runs with simulation accuracy being set as the second priority. The diagnostic runs will help catch most model problems by
+
+running simulations on summer and winter design days. The preliminary runs use a tighter set of simulation settings in order to catch problems missed in the diagnostic runs, and provide better results for quality assurance purpose. The final runs use the EnergyPlus recommended set of simulation settings in order to achieve better accuracy for simulation results ready for review and reporting.
+
+You might want to read the report on EnergyPlus run time at http://repositories.cdlib.org/lbnl/LBNL-1311E/
+
+Additional run-time tips may be found in the EnergyPlus ``Tips and Tricks'' document.~ Some more tips:
+
+\begin{itemize}
+\item
+  In the SimulationControl object, Run Simulation for Sizing Periods until everything is working well, then switch to Run Simulation for Weather File Run Periods.
+\item
+  Turn off (comment them out in the text editor using !) daylighting controls while developing the HVAC simulation.~ Then turn back on for final runs.
+\item
+  HeatBalanceAlgorithm: ConductionTransferFunction is the fastest option.
+\item
+  In the People object, the thermal comfort reports can be time consuming, especially the KSU model which is more computationally intensive.
+\end{itemize}
diff --git a/doc/input-output-reference/src/running-energyplus/errors.tex b/doc/input-output-reference/src/running-energyplus/errors.tex
new file mode 100644
index 00000000000..b0c2c0934ff
--- /dev/null
+++ b/doc/input-output-reference/src/running-energyplus/errors.tex
@@ -0,0 +1,186 @@
+\section{Errors}\label{errors}
+
+The \textbf{eplusout.err} file may contain three levels of errors (Information, Warning, Severe, Fatal) as well as the possibility of just message lines, see Table~\ref{table:energyplus-errors-and-required-actions}. EnergyPlus Errors and Required Actions. These errors may be duplicated in other files (such as the standard output file). These errors are described more completely in the Output Details and Examples document. An example .err file from the 1ZoneUncontrolled example input file:
+
+\begin{lstlisting}
+Program Version,EnergyPlus 7.0.0.024, 10/9/2011 4:04 PM,IDD\_Version 7.0.0.024
+   ** Warning ** IP: Note -- Some missing fields have been filled with defaults. See the audit output file for details.
+   ** Warning ** Weather file location will be used rather than entered Location object.
+   **   ~~~   ** ..Location object = DENVER STAPLETON INTL ARPT CO USA WMO = 724690
+   **   ~~~   ** ..Weather File Location = Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+   **   ~~~   ** ..due to location differences, Latitude difference = [3.00E-002] degrees, Longitude difference = [0.31] degrees.
+   **   ~~~   ** ..Time Zone difference = [0.0] hour(s), Elevation difference = [13.53] percent, [218.00] meters.
+   ************* Testing Individual Branch Integrity
+   ************* All Branches passed integrity testing
+   ************* Testing Individual Supply Air Path Integrity
+   ************* All Supply Air Paths passed integrity testing
+   ************* Testing Individual Return Air Path Integrity
+   ************* All Return Air Paths passed integrity testing
+   ************* No node connection errors were found.
+   ************* Beginning Simulation
+   ************* Simulation Error Summary *************
+   ************* EnergyPlus Warmup Error Summary. During Warmup: 0 Warning; 0 Severe Errors.
+   ************* EnergyPlus Sizing Error Summary. During Sizing: 0 Warning; 0 Severe Errors.
+   ************* EnergyPlus Completed Successfully-- 2 Warning; 0 Severe Errors; Elapsed Time = 00hr 00min  3.91sec
+\end{lstlisting}
+
+% table 48
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{EnergyPlus Errors and Required Actions \label{table:energyplus-errors-and-required-actions}} \tabularnewline
+\toprule 
+Error Level & Action \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{EnergyPlus Errors and Required Actions} \tabularnewline
+\toprule 
+Error Level & Action \tabularnewline
+\midrule
+\endhead
+
+Information, shown as ********* & Informative, usually a follow-on to one of the others. No action required. \tabularnewline
+**~~ \~{}\textbackslash\~{}\~{}~~** & This is a continuation of a previous message.~ String all the words/sentences together to form the complete message. \tabularnewline
+Warning & Take note. Fix as applicable. \tabularnewline
+Severe & Should Fix \tabularnewline
+Fatal & Program will abort, Must Fix \tabularnewline
+\bottomrule
+\end{longtable}
+
+EnergyPlus produces several messages as it is executing, as a guide to its progress. These message illustrate the sequence of execution as well as provides checkpoints should the simulation fail.
+
+For example, the run of the 1ZoneUncontrolled example input file produces the log:
+
+\begin{lstlisting}
+Running d:\eppgm\intcheck\energyplus.exe
+ET Start: Sun 10/09/2011 - 16:04:34.71
+Input File  : d:\devtests\inputfiles\checkin\1ZoneUncontrolled.idf
+Output Files: d:\devtests\inputfiles\outputs\
+Weather File: USA\_CO\_Golden-NREL.724666\_TMY3.epw
+ExpandObjects Started.
+No expanded file generated.
+ExpandObjects Finished. Time:     0.016
+ EnergyPlus Starting
+ EnergyPlus 7.0.0.024, 10/9/2011 4:04 PM
+ Processing Data Dictionary
+ Processing Input File
+ Initializing Simulation
+ Reporting Surfaces
+ Initializing New Environment Parameters
+ Warming up {1}
+ Warming up {2}
+ Warming up {3}
+ Warming up {4}
+ Warming up {5}
+ Warming up {6}
+ Warming up {7}
+ Warming up {8}
+ Warming up {9}
+ Warming up {10}
+ Warming up {11}
+ Warming up {12}
+ Warming up {13}
+ Warming up {14}
+ Warming up {15}
+ Warming up {16}
+ Warming up {17}
+ Warming up {18}
+ Warming up {19}
+ Warming up {20}
+ Warming up {21}
+ Warming up {22}
+ Starting Simulation at 12/21 for DENVER STAPLETON INTL ARPT ANN HTG 99% CONDNS DB
+ Initializing New Environment Parameters
+ Warming up {1}
+ Warming up {2}
+ Warming up {3}
+ Warming up {4}
+ Warming up {5}
+ Warming up {6}
+ Warming up {7}
+ Warming up {8}
+ Warming up {9}
+ Warming up {10}
+ Warming up {11}
+ Warming up {12}
+ Warming up {13}
+ Warming up {14}
+ Warming up {15}
+ Warming up {16}
+ Warming up {17}
+ Starting Simulation at 07/21 for DENVER STAPLETON INTL ARPT ANN CLG 1% CONDNS DB = >MWB
+ Initializing New Environment Parameters
+ Warming up {1}
+ Warming up {2}
+ Warming up {3}
+ Warming up {4}
+ Warming up {5}
+ Warming up {6}
+ Warming up {7}
+ Warming up {8}
+ Warming up {9}
+ Warming up {10}
+ Warming up {11}
+ Warming up {12}
+ Warming up {13}
+ Warming up {14}
+ Warming up {15}
+ Warming up {16}
+ Warming up {17}
+ Warming up {18}
+ Warming up {19}
+ Warming up {20}
+ Starting Simulation at 01/01 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 01/21
+ Continuing Simulation at 01/21 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 02/10
+ Continuing Simulation at 02/10 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 03/02
+ Continuing Simulation at 03/02 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 03/22
+ Continuing Simulation at 03/22 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 04/11
+ Continuing Simulation at 04/11 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 05/01
+ Continuing Simulation at 05/01 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 05/21
+ Continuing Simulation at 05/21 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 06/10
+ Continuing Simulation at 06/10 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 06/30
+ Continuing Simulation at 06/30 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 07/20
+ Continuing Simulation at 07/20 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 08/09
+ Continuing Simulation at 08/09 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 08/29
+ Continuing Simulation at 08/29 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 09/18
+ Continuing Simulation at 09/18 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 10/08
+ Continuing Simulation at 10/08 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 10/28
+ Continuing Simulation at 10/28 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 11/17
+ Continuing Simulation at 11/17 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 12/07
+ Continuing Simulation at 12/07 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Updating Shadowing Calculations, Start Date = 12/27
+ Continuing Simulation at 12/27 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\# = 724666
+ Writing tabular output file results using comma format.
+ Writing tabular output file results using tab format.
+ Writing tabular output file results using text format.
+ Writing tabular output file results using HTML format.
+ EnergyPlus Run Time = 00hr 00min  3.91sec
+ ReadVarsESO program starting.
+ ReadVars Run Time = 00hr 00min  0.39sec
+ ReadVarsESO program completed successfully.
+ ReadVarsESO program starting.
+ ReadVars Run Time = 00hr 00min  0.27sec
+ ReadVarsESO program completed successfully.
+  Started HVAC Diagram
+  Complete
+note: Pausing = N
+ET End: Sun 10/09/2011 - 16:04:39.34
+\end{lstlisting}
+
+In the example, the inclusion of the ``ReadVars'' program is also shown. It is run twice -- once for the \textbf{eplusout.eso} file and once for the \textbf{eplusout.mtr} file.
diff --git a/doc/input-output-reference/src/standard-output-reports.tex b/doc/input-output-reference/src/standard-output-reports.tex
new file mode 100644
index 00000000000..a6a3873cea0
--- /dev/null
+++ b/doc/input-output-reference/src/standard-output-reports.tex
@@ -0,0 +1,28 @@
+\chapter{Standard Output Reports}\label{standard-output-reports}
+
+The following objects allow standard reports to be defined and utilized in EnergyPlus:
+
+\begin{itemize}
+\item
+  Output:Table:TimeBins
+\item
+  Output:Table:Monthly
+\item
+  Output:Table:Annual
+\item
+  Output:Table:SummaryReports
+\item
+  OutputControl:Table:Style
+\end{itemize}
+
+No \textbf{Output:Meter} or \textbf{Output:Variable} objects need to be specified to use the standard reports. A good set of example reports are available in the StandardReports.idf file in the DataSets directory of EnergyPlus.
+
+\input{src/standard-output-reports/output-table-timebins}
+
+\input{src/standard-output-reports/output-table-monthly}
+
+\input{src/standard-output-reports/output-table-annual}
+
+\input{src/standard-output-reports/output-table-summaryreports}
+
+\input{src/standard-output-reports/outputcontrol-table-style}
diff --git a/doc/input-output-reference/src/standard-output-reports/output-table-annual.tex b/doc/input-output-reference/src/standard-output-reports/output-table-annual.tex
new file mode 100644
index 00000000000..796d9aa37c4
--- /dev/null
+++ b/doc/input-output-reference/src/standard-output-reports/output-table-annual.tex
@@ -0,0 +1,97 @@
+\section{Output:Table:Annual}\label{outputtableannual}
+
+The Output:Table:Annual object provides a generic method of setting up tables of annual results with each row corresponding to an instance of an object. These tables are good for creating reports that broadly summarize the building performance. At the bottom of the tables, three rows are added for the sum or average depending on the type of variable, the maximum and the minimum of each column. The report produced has multiple columns that are each defined using a repeated group of fields. The fields for the variable name and the aggregation type can be repeated for any number of columns. If the variables from different type of objects are specified in a single Output:Table:Annual, all the object names for each type of objects will be shown as rows. Variables that don't apply for certain objects will be left blank for that cell.
+
+\subsection{Inputs}\label{inputs-062}
+
+\paragraph{Field: Name}\label{field-name-060}
+
+The Name field allows the user to give the output table a label that is shown in the output file.
+
+\paragraph{Field: Filter}\label{field-filter}
+
+An optional text string that is compared to the names of the objects referenced by the variables and if they match are included in the table. A footnote will appear that indicates that the objects shown may not be all the objects that of that type that occur in the file.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-008}
+
+Optional schedule name. If left blank, aggregation is performed for all hours simulated. If a schedule is specified, aggregation is performed for non-zero hours in the schedule.
+
+\paragraph{Field Set: Variable and Aggregation Type}\label{field-set-variable-and-aggregation-type}
+
+The Variable Name field and the Aggregation Type field may be repeated for each column desired in the report. These two fields define each column of the report. The IDD object has been set up to allow up to 25 columns. This object is extensible, so the number of columns may be increased by editing the IDD file and adding the desired number of fields at the end of the object.
+
+\paragraph{Field: Variable or Meter \textless{}\#\textgreater{} Name}\label{field-variable-or-meter-name}
+
+The remainder of this input object consists of pairs of fields that can be repeatedVariable Or Meter Name fields contain the name of a variable (see Output:Variable and eplusout.rdd), meter (see Output:Meter and eplusout.mdd), or schedule. This value is shown using the aggregation method specified. If the selected name is used for both a variable or a meter and a schedule name, the variable or meter will be used.
+
+\paragraph{Field: Aggregation Type for Variable or Meter \textless{}\#\textgreater{}}\label{field-aggregation-type-for-variable-or-meter}
+
+The aggregation type determines how the variable is aggregated in the table. The choices for aggregation type are described below:
+
+\emph{Simple Aggregation Types}
+
+\textbf{SumOrAverage} -- For ``sum'' type variables adds up the values for each timestep and reports the sum of the value. For ``average'' type variables, the value shown will be the average for the month. SumOrAverage is probably the most common choice for aggregation type.
+
+\textbf{Maximum} -- Reports the maximum value and the time that the maximum value occurred. When the maximum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the maximum for a variable in Joules is reported in Watts.
+
+\textbf{Minimum} -- Reports the minimum value and the time that the minimum value occurred. When the minimum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the minimum for a variable in Joules is reported in Watts.
+
+\textbf{HoursNonZero} -- The HoursNonZero option adds up the elapsed time during the month that this variable is non-zero and would be appropriate to determine the number of hour that a fan operates.
+
+\textbf{HoursZero} -- The HoursZero option adds up the elapsed time during the month that this variable has a zero value and would be appropriate to determine the number of hour that a fan does not operate.
+
+\textbf{HoursPositive} -- The HoursPositive option adds up the elapsed time during the month that this variable has a positive value. Hours with a zero value are not included.
+
+\textbf{HoursNonPositive} -- The HoursNonPositive option adds up the elapsed time during the month that this variable has non-positive value. Hours with a negative value and hours with a zero value are all included.
+
+\textbf{HoursNegative} -- The HoursNegative option adds up the elapsed time during the month that this variable has a negative value. Hours with a zero value are not included.
+
+\textbf{HoursNonNegative} -- The HoursNonNegative option adds up the elapsed time during the month that this variable has non-negative value. Hours with a positive value and hours with a zero value are all included.
+
+\textbf{HourInTenBinsMinToMax} - Creates 10 columns for the specified variable and shows the number of hours in each of 10 bins based on the minimum and maximum value. The bin sizes will be rounded up to the next most signficant digit value (if the min is 0 and the max is 28786.3, the bin size would be 3000 not 2878.63). A table of the bin ranges would be generated below the main table when this option is selected.
+
+\textbf{HourInTenBinsZeroToMax} - Creates 11 columns for the specified variable and shows the number of hours in each of 10 bins from zero to the maximum value and a bin for hours below zero. The bin sizes will be rounded up to the next most significant digit value (if the min is 0 and the max is 28786.3, the bin size would be 3000 not 2878.63). A table of the bin ranges would be generated below the main table when this option is selected.
+
+\textbf{HourInTenBinsMinToZero} - Creates 11 columns for the specified variable and shows the number of hours in each of 10 bins from zero to the minimum value and a bin for hours above zero. The bin sizes will be rounded up to the next most significant digit value (if the min is 0 and the min is -28786.3, the bin size would be 3000 not 2878.63). A table of the bin ranges would be generated below the main table when this option is selected.
+
+\emph{Advanced Aggregation Types}
+
+The advanced aggregation types are described below. These aggregation types rely on doing an operation on the current variable but only during the time or times defined by a previously defined field. The ValueWhenMaxOrMin displays the value of one variable at the same time as the maximum or minimum is set on a previous field that is defined as either a maximum or minimum. The ``Hours---`` aggregation types (not including binning) display then number of hours that a variable meets a condition. The ``---DuringHoursShown'' aggregation types perform those aggregations but instead of for all the hours in the month, only for the hours that the previous ``Hours---`` entry applies. Multiple ``---DuringHoursShown'' after an ``Hours---`` will all be based on that single ``Hours---`` entry, in fact the ``---DuringHoursShown'' is based on the next column to the left that contains an ``Hours---`` entry even if other types of aggregations are used in intermediate columns. Order of the variables in the report is important when using the advanced aggregation types since they often depend on a previous entry.
+
+\textbf{ValueWhenMaximumOrMinimum} -- The ValueWhenMaximumOrMinimum option looks at the previous variable in the report that sets a maximum or minimum and displays the value of the current variable at that same timestep. Order of the variables in the report is important when using ValueWhenMaxMin. This can be used, for example, when an outdoor temperature should be reported for the time of the maximum cooling load.
+
+\textbf{SumOrAverageDuringHoursShown} -- Provides the sum or average of the named variable when during the hours that the previous variable displayed with any of the aggregation types starting with ``Hours''. For ``sum'' type variables adds up the values for each timestep and reports the sum of the value during the hours reported on the previous variable. For ``average'' type variables, the value shown will be the average for the month during the hours reported on the previous variable. Order of the variables in the report is important when using this aggregation type.
+
+\textbf{MaximumDuringHoursShown} -- Reports the maximum value and the time that the maximum value occurred but only during the hours reported with the previous ``hours-`` aggregation type. When the maximum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the maximum for a variable in Joules is reported in Watts. Order of the variables in the report is important when using this aggregation type.
+
+\textbf{MinimumDuringHoursShown} - Reports the minimum value and the time that the minimum value occurred but only during the hours reported with the previous ``hours-`` aggregation type. When the minimum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the minimum for a variable in Joules is reported in Watts. Order of the variables in the report is important when using this aggregation type.
+
+\paragraph{Field: Digits After Decimal for Variable or Meter \textless{}\#\textgreater{}}\label{field-digits-after-decimal-for-variable-or-meter}
+
+The Digits After Decimal field is a numeric value that indicates how many digits after the decimal point should be shown for that column.
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+Output:Table:Annual,
+  Custom Annual Window Report,  !- Name
+  , !- Report Group Name
+  , !- Filter
+  , !- Schedule Name
+  SURFACE WINDOW TRANSMITTED SOLAR RADIATION RATE,  !- Variable, Meter, EMS Int Var, IDF field Name 1
+  SumOrAverage,  !- Aggregation Type for 1
+  2,  !- Digits After Decimal for 1
+  SURFACE WINDOW TRANSMITTED BEAM SOLAR RADIATION RATE,  !- Variable, Meter, EMS Int Var, IDF field Name 2
+  SumOrAverage,  !- Aggregation Type for 2
+  2,  !- Digits After Decimal for 2
+  SURFACE WINDOW TRANSMITTED DIFFUSE SOLAR RADIATION RATE,  !- Variable, Meter, EMS Int Var, IDF field Name 3
+  SumOrAverage,  !- Aggregation Type for 3
+  2,  !- Digits After Decimal for 3
+  SURFACE WINDOW HEAT GAIN RATE,  !- Variable, Meter, EMS Int Var, IDF field Name 4
+  SumOrAverage,  !- Aggregation Type for 4
+  2,  !- Digits After Decimal for 4
+  ACE WINDOW HEAT LOSS RATE,  !- Variable, Meter, EMS Int Var, IDF field Name 5
+  SumOrAverage,  !- Aggregation Type for 5
+  2;  !- Digits After Decimal for 5
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/standard-output-reports/output-table-monthly.tex b/doc/input-output-reference/src/standard-output-reports/output-table-monthly.tex
new file mode 100644
index 00000000000..025d7cb7868
--- /dev/null
+++ b/doc/input-output-reference/src/standard-output-reports/output-table-monthly.tex
@@ -0,0 +1,72 @@
+\section{Output:Table:Monthly}\label{outputtablemonthly}
+
+The Output:Table:Monthly object provides a generic method of setting up tables of monthly results. These tables are good for creating reports that broadly summarize the building performance. At the bottom of the tables, three rows are added for the sum or average depending on the type of variable, the maximum and the minimum of each column. The report produced has multiple columns that are each defined using a repeated group of fields. The fields for the variable name and the aggregation type can be repeated for any number of columns. A single Output:Table:Monthly object often produces multiple tables in the output. A table is produced for every ``key'' for a particular output variable. A single table of results shows values only for a specific ``key''. The exception to this are environment variables, such as outdoor air temperature, that are included in each table, no matter what the key.
+
+\subsection{Inputs}\label{inputs-063}
+
+\paragraph{Field: Name}\label{field-name-061}
+
+The Name field allows the user to give the output table a label that is shown in the output file.
+
+\paragraph{Field: Digits After Decimal}\label{field-digits-after-decimal}
+
+The Digits After Decimal field is a numeric value that indicates how many digits after the decimal point should be shown on the table of values.
+
+\paragraph{Field Set: Variable or Meter and Aggregation Type}\label{field-set-variable-or-meter-and-aggregation-type}
+
+The VariableOrMeterName field and the AggregationType field may be repeated for each column desired in the monthly report. These two fields define each column of the report. The IDD object has been set up to allow up to 25 columns. This object is extensible, so the number of columns may be increased by editing the IDD file and adding the desired number of fields at the end of the object.
+
+\paragraph{Field: Variable or Meter \textless{}\#\textgreater{} Name}\label{field-variable-or-meter-name-000}
+
+The remainder of this input object consists of pairs of fields that can be repeatedVariable Or Meter Name fields contain the name of a variable (see Output:Variable and eplusout.rdd), meter (see Output:Meter and eplusout.mdd), or schedule. This value is shown on a monthly basis using the aggregation method specified. If the selected name is used for both a variable or a meter and a schedule name, the variable or meter will be used.
+
+\paragraph{Field: Aggregation Type for Variable or Meter \textless{}\#\textgreater{}}\label{field-aggregation-type-for-variable-or-meter-000}
+
+The aggregation type determines how the variable is aggregated in the table. The choices for aggregation type are described below:
+
+Simple Aggregation Types
+
+\textbf{SumOrAverage} -- For ``sum'' type variables adds up the values for each timestep and reports the sum of the value monthly. For ``average'' type variables, the value shown will be the average for the month. SumOrAverage is probably the most common choice for aggregation type.
+
+\textbf{Maximum} -- Reports the maximum value and the time that the maximum value occurred. When the maximum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the maximum for a variable in Joules is reported in Watts.
+
+\textbf{Minimum} -- Reports the minimum value and the time that the minimum value occurred. When the minimum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the minimum for a variable in Joules is reported in Watts.
+
+\textbf{HoursNonZero} -- The HoursNonZero option adds up the elapsed time during the month that this variable is non-zero and would be appropriate to determine the number of hour that a fan operates.
+
+\textbf{HoursZero} -- The HoursZero option adds up the elapsed time during the month that this variable has a zero value and would be appropriate to determine the number of hour that a fan does not operate.
+
+\textbf{HoursPositive} -- The HoursPositive option adds up the elapsed time during the month that this variable has a positive value. Hours with a zero value are not included.
+
+\textbf{HoursNonPositive} -- The HoursNonPositive option adds up the elapsed time during the month that this variable has non-positive value. Hours with a negative value and hours with a zero value are all included.
+
+\textbf{HoursNegative} -- The HoursNegative option adds up the elapsed time during the month that this variable has a negative value. Hours with a zero value are not included.
+
+\textbf{HoursNonNegative} -- The HoursNonNegative option adds up the elapsed time during the month that this variable has non-negative value. Hours with a positive value and hours with a zero value are all included.
+
+\emph{Advanced Aggregation Types}
+
+The advanced aggregation types are described below. These aggregation types rely on doing an operation on the current variable but only during the time or times defined by a previously defined field. The ValueWhenMaxOrMin displays the value of one variable at the same time as the maximum or minimum is set on a previous field that is defined as either a maximum or minimum. The ``Hours---`` aggregation types display then number of hours that a variable meets a condition. The ``---DuringHoursShown'' aggregation types perform those aggretations but instead of for all the hours in the month, only for the hours that the previous ``Hours---`` entry applies. Multiple ``---DuringHoursShown'' after an ``Hours---`` will all be based on that single ``Hours---`` entry, in fact the ``---DuringHoursShown'' is based on the next column to the left that contains an ``Hours---`` entry even if other types of aggregations are used in intermediate columns. Order of the variables in the report is important when using the advanced aggregation types since they often depend on a previous entry.
+
+\textbf{ValueWhenMaximumOrMinimum} -- The ValueWhenMaximumOrMinimum option looks at the previous variable in the report that sets a maximum or minimum and displays the value of the current variable at that same timestep. Order of the variables in the report is important when using ValueWhenMaxMin. This can be used, for example, when an outdoor temperature should be reported for the time of the maximum cooling load.
+
+\textbf{SumOrAverageDuringHoursShown} -- Provides the sum or average of the named variable when during the hours that the previous variable displayed with any of the aggregation types starting with ``Hours''. For ``sum'' type variables adds up the values for each timestep and reports the sum of the value monthly during the hours reported on the previous variable. For ``average'' type variables, the value shown will be the average for the month during the hours reported on the previous variable. Order of the variables in the report is important when using this aggregation type.
+
+\textbf{MaximumDuringHoursShown} -- Reports the maximum value and the time that the maximum value occurred but only during the hours reported with the previous ``hours-`` aggregation type. When the maximum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the maximum for a variable in Joules is reported in Watts. Order of the variables in the report is important when using this aggregation type.
+
+\textbf{MinimumDuringHoursShown} - Reports the minimum value and the time that the minimum value occurred but only during the hours reported with the previous ``hours-`` aggregation type. When the minimum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the minimum for a variable in Joules is reported in Watts. Order of the variables in the report is important when using this aggregation type.
+
+An example of this object follows.
+
+\begin{lstlisting}
+
+Output:Table:Monthly,
+    Building Monthly Cooling Load Report,               ! Name
+    3,                                                  ! Digits After Decimal
+    Zone Air System Sensible Cooling Energy,                   ! Variable or Meter 1 Name
+    SumOrAverage,                                       ! Aggregation Type for Variable or Meter 1
+    Zone Air System Sensible Cooling Energy,                   ! Variable or Meter 2 Name
+    Maximum,                                            ! Aggregation Type for Variable or Meter 2
+    Site Outdoor Air Drybulb Temperature,                                   ! Variable or Meter 3 Name
+    ValueWhenMaxMin;                                    ! Aggregation Type for Variable or Meter 3
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/standard-output-reports/output-table-summaryreports.tex b/doc/input-output-reference/src/standard-output-reports/output-table-summaryreports.tex
new file mode 100644
index 00000000000..e6f07332ed0
--- /dev/null
+++ b/doc/input-output-reference/src/standard-output-reports/output-table-summaryreports.tex
@@ -0,0 +1,1542 @@
+\section{Output:Table:SummaryReports}\label{outputtablesummaryreports}
+
+The Output:Table:SummaryReports object controls which predefined tabular reports are produced.~ The easiest option is to specify ``AllSummary'' which will produce all of the summary reports described in this section and does not include the Zone Component Load report. In addition, ``AllMonthly'' will produce all of the monthly reports described. If all predefined reports are needed. ``AllSummaryAndMonthly'' shows all of the summary and monthly predefined reports and does not include the Zone Component Load report. The ``AllSummaryAndSizingPeriod'' option and ``AllSummaryMonthlyAndSizingPeriod'' option are similar and add the Zone Component Load report. Including the Zone Component Load Summary report may increase the simulation run time.
+
+\subsection{Inputs}\label{inputs-064}
+
+\paragraph{Field: Report \textless{}\#\textgreater{} Name}\label{field-report-name}
+
+All of the fields in the Output:Table:SummaryReports are the same. A long list of predefined summary reports is available by entering one of the available key choices described below. Each one indicates the name of the predefined reports that should be output. The input AllSummary will cause all the reports described below to be created.~ The Report \textless{}\#\textgreater{} Name field can be repeated.
+
+\subsubsection{Predefined Annual Summary Reports}\label{predefined-annual-summary-reports}
+
+\paragraph{Annual Building Utility Performance Summary (sometimes called ABUPS)}\label{annual-building-utility-performance-summary-sometimes-called-abups}
+
+The Annual Building Utility Performance Summary report often called ABUPS -- (key: AnnualBuildingUtilityPerformanceSummary) produces a report that is an overall summary of the utility consumption of the building. It contains a number of subtables that are each described below.
+
+\begin{itemize}
+\item
+  Site and Source Energy -- Indicates the total site and source energy use. For electricity the net electricity from the utility is used for the electric contribution. The site to source conversion factors are based on those entered by the user. These are entered in the EnvironmentalImpactFactors object and FuelFactors objects.
+\item
+  Building Area -- Shows the total floorspace of the building and the conditioned floorspace.
+\item
+  End Uses -- This shows the total use of electricity, natural gas, other fuels, purchased cooling, purchased heating and water for each major end-use category. The end-use categories are Heating, Cooling, Interior Lighting, Exterior Lighting, Interior Equipment, Exterior Equipment, Fans, Pumps, Heat Rejection, Humidification, Heat Recovery, Hot Water, Refrigeration, and Generators. Not all fuels have corresponding end uses. The values in this sub-table are from output meters. To determine which components are attached to each end-use meter, consult the meter details output file (*.mtd). The source of the resource does not affect this table -- the amount of electricity used for lights does not change if the electricity is from the utility or from an on-site generator. The Other Fuel column includes fuel oil\#1, fuel oil\#2, gasoline, coal, propane, diesel, otherfuel1 and otherfuel2. The district heating column also~ includes steam.
+\item
+  End Uses By Subcategory -- Shows a breakdown of the major end uses by user-defined category. If an end-use subcategory was not input for an object, it is automatically added to the General subcategory for that major end-use category.
+\item
+  Utility Use Per Floor Area -- These two sub-tables show the results from the end-uses table divided by the total floor area defined for the building and for the total conditioned floor area. Only three categories for end-uses are used for these sub-tables, lighting, HVAC and other. HVAC includes fans, pumps, heating, cooling, heat rejection, humidification, and domestic hot water heating. The Other Fuel column includes fuel oil\#1, fuel oil\#2, gasoline, coal, propane, diesel, otherfuel1 and otherfuel2. The district heating column also~ includes steam.
+\item
+  Electric Loads Satisfied -- Shows the different methods that electric loads are satisfied in the building. The values shown for on site power generation are: Fuel-Fired Power Generation, High Temperature Geothermal, Photovoltaic Power, and Wind Power. The flows to and from the electric utility are shown next and finally the total electricity used at the site is compared to the total generated on site plus the net amount from the electric utility. The percentages shown are based on the total electricity used by the end-uses. Note that High Temperature Geothermal and Wind Power are not yet implemented in EnergyPlus.
+\item
+  On-Site Thermal Sources -- Shows the on-site thermal sources of energy such as Water-Side Heat Recovery, Air to Air Heat Recovery for Cooling, Air to Air Heat Recovery for Heating, High-Temperature Geothermal, Solar Water Thermal, Solar Air Thermal. Note that High-Temperature Geothermal Solar Water Thermal, and Solar Air Thermal are not yet implemented in EnergyPlus.
+\item
+  Water Loads Summary -- Shows the different methods the water loads were satisfied. This table shows all zeros because water use is not yet implemented in EnergyPlus.
+\end{itemize}
+
+\paragraph{Input Verification and Results Summary (or IVRS)}\label{input-verification-and-results-summary-or-ivrs}
+
+The Input Verification and Results Summary report (key: InputVerificationandResultsSummary) produces a report with several tables including:
+
+\begin{itemize}
+\item
+  General which includes general information like the Program Version and Build, Weather, Latitude, Longitude, Elevation, Time Zone, North Axis Angle, and Hours Simulated.
+\item
+  Window-Wall Ratio table for envelope which includes the wall area, the window area and the ratio of the two. These are computed for all walls and for walls that are oriented generally north, south, east and west. All walls are categorized into one of these four cardinal directions. This is computed for walls that have a tilt of 60 to 120 degrees.
+\item
+  Skylight-Roof Ratio table for envelope which includes the roof area and the skylight area and the ratio of the two. This includes all surfaces with a tilt of less than 60 degrees.
+\item
+  Zone Summary includes internal load summary for each zone including area, if conditioned, volume, multipliers, gross wall area, window area, design lighting, design people, design plug and process.
+\end{itemize}
+
+\paragraph{Source Energy End Use Components Summary}\label{source-energy-end-use-components-summary}
+
+The Source Energy End Use Components Summary report produces a report (key: SourceEnergyEndUseComponentsSummary) that includes three tables. These tables display source energy by fuel type that is calculated based on site to source energy factors specified by the user in the EnvironmentalImpactFactors and FuelFactors objects. The last two tables display the source energy in terms of area normalized metrics. Following is a description of each table:
+
+\begin{itemize}
+\item
+  Source Energy End Use Components -- This shows the total use of source electricity, source natural gas, source values of other fuels, source purchased cooling~~ and purchased heating for each major end-use category. The end-use categories are Heating, Cooling, Interior Lighting, Exterior Lighting, Interior Equipment, Exterior Equipment, Fans, Pumps, Heat Rejection, Humidification, Heat Recovery, Hot Water, Refrigeration, and Generators. Not all fuels have corresponding end uses. The values in this sub-table are from output meters. To determine which components are attached to each end-use meter, consult the meter details output file (*.mtd). The source of the resource will affect this table -- the amount of electricity used for lights will change if the electricity is from the utility or from an on-site generator. The Other Fuel column includes FuelOil\#1, FuelOil\#2, Gasoline, Coal, Propane, Diesel, OtherFuel1 and OtherFuel2. The district heating column also~ includes steam.
+\item
+  Source Energy End Use Components normalized by Conditioned Floor Area -- This table shows the total end uses in source energy normalized by conditioned floor area.
+\item
+  Source Energy End Use Components normalized by Total Floor Area -- This table shows the total end uses in source energy normalized by total floor area.
+\end{itemize}
+
+\paragraph{Climatic Data Summary}\label{climatic-data-summary}
+
+The Climate Summary or Climatic Data Summary report (key: ClimaticDataSummary) produces a report that includes some of the details on each of the design days including: maximum dry-bulb, daily temperature range, humidity value, humidity type, wind speed, and wind direction.
+
+\paragraph{Envelope Summary}\label{envelope-summary}
+
+The Envelope Summary report (key: EnvelopeSummary) produces a report that includes the following tables:
+
+\begin{itemize}
+\item
+  Opaque which includes all opaque surfaces and includes the name of the construction, reflectance, U-Factor, gross area, azimuth, tilt, cardinal direction.
+\item
+  Fenestration which includes all non-opaque surfaces and includes the name of the construction, areas (glass, frame, divider, single opening, multiplied openings), U-Factor, SHGC (the solar heat gain coefficient based on summer conditions), visible transmittance, conductance (frame, divider), indication of shade control, the name of the parent surface, azimuth, tilt, cardinal direction.
+\end{itemize}
+
+\paragraph{Surface Shadowing Summary}\label{surface-shadowing-summary}
+
+The Surface Shadowing Summary report (key: SurfaceShadowingSummary) produces a report that includes two tables. Note that surfaces starting with ``Mir-`` are automatically generated by EnergyPlus and are the mirror images of user entered surfaces.
+
+\begin{itemize}
+\item
+  Surfaces (Walls, Roofs, etc) that may be Shadowed by Other Surfaces and includes the name of the surface and a list of surfaces that may possibly cast shadows on that named surface. The list of possible shadow casters does not necessarily mean that they do cast shadows during the simulation, only that their relative position makes it possible that shadows from a surface in the list may fall on the named surface.
+\item
+  Subsurfaces (Windows and Doors) that may be Shadowed by Surfaces, includes the name of the subsurface such as a window or a door and a corresponding list of surfaces that may be casting shadows on the windows and doors.
+\end{itemize}
+
+\paragraph{Shading Summary}\label{shading-summary}
+
+The Shading Summary report (key: ShadingSummary) produces a report that includes the following tables:
+
+\begin{itemize}
+\item
+  Sunlit Fraction which shows a list of windows and the fraction of the window that is sunlit for nine specific times of the year. The nine specific times include 9am, noon and 3pm on March 21, June 21, and December 21. These nine times were chosen to represent the range of sun angles. The simulation must include those times for the value to be included in the report.
+\item
+  Window control includes the names of all windows that have a window shading control (see WindowProperty:ShadingControl) and includes the name of the control, the type of shading, the shaded construction, the kind of control, and if glare control is used.
+\end{itemize}
+
+\paragraph{Lighting Summary}\label{lighting-summary}
+
+The Lighting Summary report (key: LightingSummary) produces a report that includes the following tables:
+
+\begin{itemize}
+\item
+  Interior Lighting which includes the name of the lights object, the zone that it is used in, the lighting power density, zone area, total power, end use subcategory, schedule name, average hours per week, return air fraction, and whether the zone is conditioned.
+\item
+  Daylighting which includes the names of the daylighting objects, the zone they are used in, the type of daylighting being used, the control type, the fraction of the lighting controlled, the total power of the lighting installed in the zone and the lighting power that is controlled by the daylighting object.
+\item
+  Exterior Lighting which includes the name of the ExteriorLights object, the total watts described by the object, if the ExteriorLights uses an astronomical clock or just a schedule, the name of the schedule used, and the average hours per week for the named schedule for the year. The effect of the astronomical clock does not get included in the averaged hours per week shown.
+\end{itemize}
+
+\paragraph{Equipment Summary}\label{equipment-summary}
+
+The Equipment Summary report (key: EquipmentSummary) produces a report that includes some details on the major HVAC equipment present. The report has seven parts.
+
+\begin{itemize}
+\item
+  Central Plant includes details on chillers, boilers, and cooling towers including the capacity and efficiency. For Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR, IPLV at AHRI standard test conditions is reported.
+\item
+  Cooling Coils includes the nominal total, sensible and latent capacities, the nominal sensible heat ratio, the nominal efficiency, nominal UA value, and nominal~ surface area for each cooling coil. These values are calculated by calling the cooling coil simulation routine with the rated inlet conditions: inlet air dry bulb temperature = 26.67C, inlet air wet bulb temperature = 19.44C, inlet chilled water temperature = 6.67C.
+\item
+  DX Cooling Coils summarizes the Standard Rating (Net) Cooling Capacity, SEER, EER and IEER values at AHRI standard test. Currently, these values are only reported for coil type = Coil:Cooling:DX:SingleSpeed with condenser type = AirCooled.
+\item
+  DX Heating Coils summarizes the High Temperature Heating Standard (Net) Rating Capacity, Low Temperature Heating Standard (Net) Rating Capacity and Heating Seasonal Performance Factor (HSPF) values at AHRI standard test. Currently, these values are only reported for coil type = Coil:Heating:DX:SingleSpeed.
+\item
+  Heating Coils includes the nominal capacity and efficiency for each heating coil. The capacity is calculated by calling the heating coil simulation routine at the rated inlet conditions: inlet air dry bulb temperature = 16.6C, inlet relative humidity = 50\%, inlet hot water temperature = 82.2C.
+\item
+  Fan includes the type of fan, the total efficiency, delta pressure, max flow rate, motor heat in air fraction, and end use.
+\item
+  Pumps includes the type of pump, control type, head pressure, electric power, and motor efficiency for each pump.
+\item
+  Service Water Heating includes the type of water heater, the storage volume, input, thermal efficiency, recovery efficiency, and energy factor.
+\end{itemize}
+
+\paragraph{HVAC Sizing Summary}\label{hvac-sizing-summary}
+
+The HVAC Sizing Summary report (key: HVACSizingSummary) produces a report that includes the following tables:
+
+\begin{itemize}
+\item
+  Zone Cooling which includes the following columns for each zone: the calculated design load, the user specified design load, the calculated design air flow, the user specified design air flow, the name of the sizing period, the time of the peak load during the sizing period, the temperature at the time of the peak load during the sizing period, and the humidity ratio at the time of the peak load during the sizing period used.
+\item
+  Zone Heating which includes the following columns for each zone: the calculated design load, the user specified design load, the calculated design air flow, the user specified design air flow, the name of the sizing period, the time of the peak load during the sizing period, the temperature at the time of the peak load during the sizing period, and the humidity ratio at the time of the peak load during the sizing period used.
+\item
+  System Design Air Flow Rates which includes the following columns for each air loop: the calculated cooling air flow rate, the user specified air flow rate for cooling, the calculated heating air flow rate, the user specified air flow rate for heating.
+\item
+  \emph{Note:} values listed as ``calculated'' are the unaltered result of the zone or system sizing calculations, using the design sizing period weather and schedules specified in the input. Values listed as ``user specified'' are either the calculated values modified by global or zone sizing factors or values specified with the \emph{flow/zone} or \emph{flow/system} design air flow method.
+\end{itemize}
+
+\paragraph{Component Sizing Summary}\label{component-sizing-summary}
+
+The Component Sizing Summary report (key: ComponentSizingSummary) produces a report that includes different tables depending on the kinds of HVAC components that exist in the input file. A table is shown for each type of HVAC component that is sized. The table lists the objects of that type of component that appear in the input file and one or more parameters related to that component.~ For example, the AirTerminal:SingleDuct:VAV:Reheat component creates a table showing the maximum air flow rate from the sizing calculations and the maximum reheat water flow rate. Another example is the Fan:VariableVolume object which shows a table with both the maximum and minimum flow rates for each fan based on the results from the sizing calculations.
+
+\paragraph{Outdoor Air Summary}\label{outdoor-air-summary}
+
+The Outdoor Air Summary report (key: OutdoorAirSummary) produces a report that includes the following tables:
+
+\begin{itemize}
+\item
+  Average Outside Air During Occupied Hours table shows for each zone the average and nominal number of occupants, the zone volume, the average air change rate based on mechanical ventilation, infiltration and simple ventilation during occupied hours.
+\item
+  Minimum Outside Air During Occupied Hours table shows for each zone the average and nominal number of occupants, the zone volume, the minimum air change rate based on mechanical ventilation, infiltration and simple ventilation during occupied hours.
+\end{itemize}
+
+\paragraph{System Summary}\label{system-summary}
+
+The System Summary Report (key: SystemSummary) produces a report that includes the following tables:
+
+\begin{itemize}
+\item
+  Economizer which includes the following columns for each Controller:OutdoorAir object: the high limit shutoff control, the minimum outdoor air flow, the maximum outdoor air flow, if the return air temperature has a control limit, if the return air has an enthalpy limit, the outdoor air temperature limit, and the outdoor air enthalpy limit.
+\item
+  Demand Controlled Ventilation table is for each Controller:MechanicalVentilation object and shows the name, the nominal outdoor air per person and the nominal outdoor air per zone area.
+\item
+  Time Not Comfortable Based on Simple ASHRAE 55-2004 table shows how many hours that the space is not comfortable for each zone under the criteria of assuming winter clothes, summer clothes or both summer and winter clothes.~ See the People object for more information about this thermal comfort calculation.
+\item
+  Time Setpoint is Not Met table shows how many hours the space is more than 0.2C from the setpoint during heating and during cooling.~ The last two columns indicate those hours that the setpoint is not met while the space is occupied.
+\end{itemize}
+
+\paragraph{Adaptive Comfort Summary}\label{adaptive-comfort-summary}
+
+The Adaptive Comfort Summary report (key: AdaptiveComfortSummary) produces a report tabulating the sum of occupied hours not meeting adaptive comfort acceptability limits for each relevant People object (People objects for which adaptive comfort calculations are requested). These acceptability limits include ASHRAE Std. 55 80\%, ASHRAE Std. 55 90\%, CEN-15251 Category I, CEN-15251 Category II, and CEN-15251 Category III.
+
+\paragraph{Sensible Heat Gain Summary}\label{sensible-heat-gain-summary}
+
+The Sensible Heat Gain Summary (key: SensibleHeatGainSummary) provides results for each zone and the overall building for some of the major heat gain components. The first four columns show the loads satisfied by sensible air heating and cooling as well as radiant heating and cooling surfaces in the zone. The heat gains from people, lighting, equipment, windows, interzone air flow, and infiltration are shown when adding heat to the zone and separately when removing heat from the zone (for applicable components). Finally the balance is shown as ``Opaque Surface Conduction and Other Heat Addition'' and ``Opaque Surface Conduction and Other Heat Removal'' which is a term indicating the affect of the walls, floors and ceilings/roof to the zone as well as the impact of the delay between heat gains/losses and loads on the HVAC equipment serving the zone.~ The following shows each output variable that is used for each column. For each timestep in the simulation, positive values are shown as additions and negative values are shown as removal for most variables.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC Input Sensible Air Heating
+\end{itemize}
+
+Zone Air Heat Balance System Air Transfer Rate
+
+Zone Air Heat Balance System Convective Heat Gain Rate
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC Input Sensible Air Cooling
+\end{itemize}
+
+Zone Air Heat Balance System Air Transfer Rate
+
+Zone Air Heat Balance System Convective Heat Gain Rate
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC Input Heated Surface Heating
+\end{itemize}
+
+Zone Radiant HVAC Heating Energy
+
+Zone Ventilated Slab Radiant Heating Energy
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC Input Cooled Surface Cooling
+\end{itemize}
+
+Zone Radiant HVAC Cooling Energy
+
+Zone Ventilated Slab Radiant Cooling Energy
+
+\begin{itemize}
+\tightlist
+\item
+  People Sensible Heat Addition
+\end{itemize}
+
+Zone People Sensible Heating Energy
+
+\begin{itemize}
+\tightlist
+\item
+  Lights Sensible Heat Addition
+\end{itemize}
+
+Zone Lights Total Heating Energy
+
+\begin{itemize}
+\tightlist
+\item
+  Equipment Sensible Heat Addition \& Equipment Sensible Heat Removal
+\end{itemize}
+
+Zone Electric Equipment Radiant Heating Energy
+
+Zone Gas Equipment Radiant Heating Energy
+
+Zone Steam Equipment Radiant Heating Energy
+
+Zone Hot Water Equipment Radiant Heating Energy
+
+Zone Other Equipment Radiant Heating Energy
+
+Zone Electric Equipment Convective Heating Energy
+
+Zone Gas Equipment Convective Heating Energy
+
+Zone Steam Equipment Convective Heating Energy
+
+Zone Hot Water Equipment Convective Heating Energy
+
+Zone Other Equipment Convective Heating Energy
+
+\begin{itemize}
+\tightlist
+\item
+  Window Heat Addition \& Window Heat Removal
+\end{itemize}
+
+Zone Windows Total Heat Gain Energy
+
+\begin{itemize}
+\tightlist
+\item
+  Interzone Air Transfer Heat Addition \& Interzone Air Transfer Heat Removal
+\end{itemize}
+
+Zone Air Heat Balance Interzone Air Transfer Rate
+
+\begin{itemize}
+\tightlist
+\item
+  Infiltration Heat Addition \& Infiltration Heat Removal
+\end{itemize}
+
+Zone Air Heat Balance Outdoor Air Transfer Rate
+
+The Opaque Surface Conduction and Other Heat Addition and Opaque Surface Conduction and Other Heat Removal columns are also calculated on an timestep basis as the negative value of the other removal and gain columns so that the total for the timestep sums to zero. These columns are derived strictly from the other columns.
+
+\paragraph{Zone Component Load Summary}\label{zone-component-load-summary}
+
+The Zone Component Loads Summary provides an estimate of the heating and cooling peak loads for each zone broken down into various components. This report may help determine which components of the load have the largest impact for the heating and cooling peak design conditions. When specified, the Zone Component Loads Summary report is created for each zone that is conditioned. The difference between the peak design sensible load and the estimated instant + delayed sensible load (as shown in the \emph{Peak Conditions} subtable) is an indication of how consistent the overall total estimate may be to the computed total peak loads for the zone. When the report is called the zone sizing calculations are repeated twice so this may result in longer simulation times.~ The key used to obtain this report is ZoneComponentLoadSummary. Since including this report may increase the simulation time, new key options have been added that will display all reports but the Zone Component Load Summary those keys used are AllSummaryButZoneComponentLoad and AllSummaryAndMonthlyButZoneComponentLoad.
+
+The report has four parts:
+
+\begin{itemize}
+\tightlist
+\item
+  Estimated Cooling Peak Load Components
+\end{itemize}
+
+Contains the sensible-instant, sensible-delay, sensible-return air, latent, total and \%grand total for people, lights, equipment, refrigeration, water use equipment, HVAC equipment loads, power generation equipment, infiltration, zone ventilation, interzone mixing, roof, interzone ceiling, other roof, exterior wall, interzone wall, ground contact wall, other wall, exterior floor, interzone floor, ground contact floor, other floor, fenestration conduction, fenestration solar, opaque door. The values in the sensible-delay column are estimated using a procedure shown in the Engineering Reference.
+
+\begin{itemize}
+\tightlist
+\item
+  Cooling Peak Conditions
+\end{itemize}
+
+Contains the time of the peak load and the outside dry bulb and wet bulb temperatures as well as the outside humidity ratio for that time. It also shows the zone temperature and relative humidity and humidity ratio for that time.
+
+\begin{itemize}
+\tightlist
+\item
+  Estimated Heating Peak Load Components
+\end{itemize}
+
+Contains the sensible-instant, sensible-delay, sensible-return air, latent, total and \%grand total for people, lights, equipment, refrigeration, water use equipment, HVAC equipment loads, power generation equipment, infiltration, zone ventilation, interzone mixing, roof, interzone ceiling, other roof, exterior wall, interzone wall, ground contact wall, other wall, exterior floor, interzone floor, ground contact floor, other floor, fenestration conduction, fenestration solar, opaque door. The values in the sensible-day column are estimated using a procedure shown in the Engineering Reference.
+
+\begin{itemize}
+\tightlist
+\item
+  Heating Peak Conditions
+\end{itemize}
+
+Contains the time of the peak load and the outside dry bulb and wet bulb temperatures as well as the outside humidity ratio for that time. It also shows the zone temperature and the relative humidity and humidity ratio for that time.
+
+\paragraph{Standard 62.1 Summary}\label{standard-62.1-summary}
+
+The Standard 62.1 Summary (key: Standard62.1Summary) produces a report that is consistent with many of the outputs needed when doing calculations consistent with ASHRAE Standard 62.1-2010. The report is generated when sizing calculations are specified. The abbreviations used in the report are consistent with the abbreviations used in Appendix A4 of the Standard. The following tables are part of the report:
+
+\begin{itemize}
+\item
+  System Ventilation Requirements for Cooling containing: Sum of Zone Primary Air Flow - Vpz-sum, System Population -- Ps, Sum of Zone Population - Pz-sum, Occupant Diversity -- D, Uncorrected Outdoor Air Intake Airflow -- Vou, System Primary Airflow -- Vps, Average Outdoor Air Fraction -- Xs, System Ventilation Efficiency -- Ev, Outdoor Air Intake Flow -- Vot, Percent Outdoor Air - \%OA.
+\item
+  System Ventilation Requirements for Heating containing: Sum of Zone Primary Air Flow - Vpz-sum, System Population -- Ps, Sum of Zone Population - Pz-sum, Occupant Diversity -- D, Uncorrected Outdoor Air Intake Airflow -- Vou, System Primary Airflow -- Vps, Average Outdoor Air Fraction -- Xs, System Ventilation Efficiency -- Ev, Outdoor Air Intake Flow -- Vot, Percent Outdoor Air - \%OA.
+\item
+  Zone Ventilation Parameters containing: AirLoop Name, People Outdoor Air Rate -- Rp, ~Zone Population -- Pz, Area Outdoor Air Rate -- Ra, Zone Floor Area -- Az, Breathing Zone Outdoor Airflow -- Vbz, Cooling Zone Air Distribution Effectiveness - Ez-clg, Cooling Zone Outdoor Airflow - Voz-clg, Heating Zone Air Distribution Effectiveness - Ez-htg, Heating Zone Outdoor Airflow - Voz-htg.
+\item
+  System Ventilation Parameters containing: People Outdoor Air Rate -- Rp, Sum of Zone Population - Pz-sum, Area Outdoor Air Rate -- Ra, Sum of Zone Floor Area - Az-sum, Breathing Zone Outdoor Airflow -- Vbz, Cooling Zone Outdoor Airflow - Voz-clg, Heating Zone Outdoor Airflow - Voz-htg.
+\item
+  Zone Ventilation Calculations for Cooling Design containing: AirLoop Name, Box Type, Zone Primary Airflow -- Vpz, Zone Discharge Airflow -- Vdz, Minimum Zone Primary Airflow - Vpz-min, Zone Outdoor Airflow Cooling - Voz-clg, Primary Outdoor Air Fraction -- Zpz, Primary Air Fraction -- Ep, Secondary Recirculation Fraction- Er, Supply Air Fraction- Fa, Mixed Air Fraction -- Fb, Outdoor Air Fraction -- Fc, Zone Ventilation Efficiency -- Evz.
+\item
+  System Ventilation Calculations for Cooling Design containing: Sum of Zone Primary Airflow - Vpz-sum, System Primary Airflow -- Vps, Sum of Zone Discharge Airflow - Vdz-sum, Minimum Zone Primary Airflow - Vpz-min, Zone Outdoor Airflow Cooling - Voz-clg, Zone Ventilation Efficiency - Evz-min.
+\item
+  Zone Ventilation Calculations for Heating Design containing: AirLoop Name, Box Type, Zone Primary Airflow -- Vpz, Zone Discharge Airflow -- Vdz, Minimum Zone Primary Airflow - Vpz-min, Zone Outdoor Airflow Cooling - Voz-clg, Primary Outdoor Air Fraction -- Zpz, Primary Air Fraction -- Ep, Secondary Recirculation Fraction- Er, Supply Air Fraction- Fa, Mixed Air Fraction -- Fb, Outdoor Air Fraction -- Fc, Zone Ventilation Efficiency -- Evz.
+\item
+  System Ventilation Calculations for Heating Design containing: Sum of Zone Primary Airflow - Vpz-sum, System Primary Airflow -- Vps, Sum of Zone Discharge Airflow - Vdz-sum, Minimum Zone Primary Airflow - Vpz-min, Zone Outdoor Airflow Cooling - Voz-clg, Zone Ventilation Efficiency - Evz-min.
+\end{itemize}
+
+\paragraph{Energy Meters Summary}\label{energy-meters-summary}
+
+The Energy Meters Summary (key: EnergyMeters) (which is a slight misnomer as some meters may not be strictly energy) provides the annual period (runperiod) results for each meter (reference the meter data dictionary file (.mdd) and/or the meter details file (.mtd). The results are broken out by fuel type (resource type) in this report.
+
+\paragraph{LEED Summary}\label{leed-summary}
+
+The LEED Summary report provides many of the simulation results required for certification of Energy and Atmosphere Credit 1 Optimized Energy Performance according to the LEED Green Building Rating Systemâ„¢. The report can be produced by specifying LEEDSummary in Output:Table:SummaryReports which is also part of the AllSummary option. Directly following is an example of this report.
+
+\paragraph{Object Count Summary}\label{object-count-summary}
+
+The Object Count Summary provides the count on the number of specific objects in the file. The key used to obtain this report is ObjectCountSummary.
+
+\paragraph{Component Cost Economics Summary}\label{component-cost-economics-summary}
+
+The Component Cost Economics Summary provides the construction cost estimate summary for the project. The costs are broken into eight catagories and the reference building costs are provided as a comparison. A second table is also produced that provides line item details with one line for every line item object. The key used to obtain this report is ComponentCostEconomicsSummary.
+
+\subsubsection{Predefined Monthly Summary Reports}\label{predefined-monthly-summary-reports}
+
+The predefined monthly report options are shown below. The key name of the predefined monthly report is all that is needed to have that report appear in the tabular output file. After each report name below are the output variables and aggregation types used. These cannot be modified when using the predefined reports but if changes are desired, a Output:Table:Monthly can be used instead. The StandardReports.idf file in the DataSets directory includes a Output:Table:Monthly that exactly corresponds to the predefined monthly reports shown below. They can be copied into an IDF file and extended if additional variables are desired. A listing of each available key for predefined monthly summary reports follows with a discrption of the variables included.
+
+\paragraph{ZoneCoolingSummaryMonthly}\label{zonecoolingsummarymonthly}
+
+\begin{itemize}
+\item
+  Zone Air System Sensible Cooling Energy (SumOrAverage)
+\item
+  Zone Air System Sensible Cooling Rate (Maximum)
+\item
+  Site Outdoor Air Drybulb Temperature (ValueWhenMaxMin)
+\item
+  Site Outdoor Air Wetbulb Temperature (ValueWhenMaxMin)
+\item
+  Zone Total Internal Latent Gain Energy (SumOrAverage)
+\item
+  Zone Total Internal Latent Gain Energy (Maximum)
+\item
+  Site Outdoor Air Drybulb Temperature (ValueWhenMaxMin)
+\item
+  Site Outdoor Air Wetbulb Temperature (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{ZoneHeatingSummaryMonthly}\label{zoneheatingsummarymonthly}
+
+\begin{itemize}
+\item
+  Zone Air System Sensible Heating Energy (SumOrAverage)
+\item
+  Zone Air System Sensible Heating Rate (Maximum)
+\item
+  Site Outdoor Air Drybulb Temperature (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{ZoneElectricSummaryMonthly}\label{zoneelectricsummarymonthly}
+
+\begin{itemize}
+\item
+  Zone Lights Electric Energy (SumOrAverage)
+\item
+  Zone Lights Electric Energy (Maximum)
+\item
+  Zone Electric Equipment Electric Energy (SumOrAverage)
+\item
+  Zone Electric Equipment Electric Energy (Maximum)
+\end{itemize}
+
+\paragraph{SpaceGainsMonthly}\label{spacegainsmonthly}
+
+\begin{itemize}
+\item
+  Zone People Total Heating Energy (SumOrAverage)
+\item
+  Zone Lights Total Heating Energy (SumOrAverage)
+\item
+  Zone Electric Equipment Total Heating Energy (SumOrAverage)
+\item
+  Zone Gas Equipment Total Heating Energy (SumOrAverage)
+\item
+  Zone Hot Water Equipment Total Heating Energy (SumOrAverage)
+\item
+  Zone Steam Equipment Total Heating Energy (SumOrAverage)
+\item
+  Zone Other Equipment Total Heating Energy (SumOrAverage)
+\item
+  Zone Infiltration Sensible Heat Gain Energy (SumOrAverage)
+\item
+  Zone Infiltration Sensible Heat Loss Energy (SumOrAverage)
+\end{itemize}
+
+\paragraph{PeakSpaceGainsMonthly}\label{peakspacegainsmonthly}
+
+\begin{itemize}
+\item
+  Zone People Total Heating Energy (Maximum)
+\item
+  Zone Lights Total Heating Energy (Maximum)
+\item
+  Zone Electric Equipment Total Heating Energy (Maximum)
+\item
+  Zone Gas Equipment Total Heating Energy (Maximum)
+\item
+  Zone Hot Water Equipment Total Heating Energy (Maximum)
+\item
+  Zone Steam Equipment Total Heating Energy (Maximum)
+\item
+  Zone Other Equipment Total Heating Energy (Maximum)
+\item
+  Zone Infiltration Sensible Heat Gain Energy (Maximum)
+\item
+  Zone Infiltration Sensible Heat Loss Energy (Maximum)
+\end{itemize}
+
+\paragraph{SpaceGainComponentsAtCoolingPeakMonthly}\label{spacegaincomponentsatcoolingpeakmonthly}
+
+\begin{itemize}
+\item
+  Zone Air System Sensible Cooling Rate (Maximum)
+\item
+  Zone People Total Heating Energy (ValueWhenMaxMin)
+\item
+  Zone Lights Total Heating Energy (ValueWhenMaxMin)
+\item
+  Zone Electric Equipment Total Heating Energy (ValueWhenMaxMin)
+\item
+  Zone Gas Equipment Total Heating Energy (ValueWhenMaxMin)
+\item
+  Zone Hot Water Equipment Total Heating Energy (ValueWhenMaxMin)
+\item
+  Zone Steam Equipment Total Heating Energy (ValueWhenMaxMin)
+\item
+  Zone Other Equipment Total Heating Energy (ValueWhenMaxMin)
+\item
+  Zone Infiltration Sensible Heat Gain Energy (ValueWhenMaxMin)
+\item
+  Zone Infiltration Sensible Heat Loss Energy (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{EnergyConsumptionElectricityNaturalGasMonthly}\label{energyconsumptionelectricitynaturalgasmonthly}
+
+\begin{itemize}
+\item
+  Electricity:Facility (SumOrAverage)
+\item
+  Electricity:Facility (Maximum)
+\item
+  Gas:Facility (SumOrAverage)
+\item
+  Gas:Facility (Maximum)
+\end{itemize}
+
+\paragraph{EnergyConsumptionElectricityGeneratedPropaneMonthly}\label{energyconsumptionelectricitygeneratedpropanemonthly}
+
+\begin{itemize}
+\item
+  ElectricityProduced:Facility (SumOrAverage)
+\item
+  ElectricityProduced:Facility (Maximum)
+\item
+  Propane:Facility (SumOrAverage)
+\item
+  Propane:Facility (Maximum)
+\end{itemize}
+
+\paragraph{EnergyConsumptionDieselFuel OilMonthly}\label{energyconsumptiondieselfuel-oilmonthly}
+
+\begin{itemize}
+\item
+  Diesel:Facility (SumOrAverage)
+\item
+  Diesel:Facility (Maximum)
+\item
+  FuelOil\#1:Facility (SumOrAverage)
+\item
+  FuelOil\#1:Facility (Maximum)
+\item
+  FuelOil\#2:Facility (SumOrAverage)
+\item
+  FuelOil\#2:Facility (Maximum)
+\end{itemize}
+
+\paragraph{EnergyConsumptionDisctrictHeatingCoolingMonthly}\label{energyconsumptiondisctrictheatingcoolingmonthly}
+
+\begin{itemize}
+\item
+  DistrictCooling:Facility (SumOrAverage)
+\item
+  DistrictCooling:Facility (Maximum)
+\item
+  DistrictHeating:Facility (SumOrAverage)
+\item
+  DistrictHeating:Facility (Maximum)
+\end{itemize}
+
+\paragraph{EnergyConsumptionCoalGasolineMonthly}\label{energyconsumptioncoalgasolinemonthly}
+
+\begin{itemize}
+\item
+  Coal:Facility (SumOrAverage)
+\item
+  Coal:Facility (Maximum)
+\item
+  Gasoline:Facility (SumOrAverage)
+\item
+  Gasoline:Facility (Maximum)
+\end{itemize}
+
+\paragraph{EnergyConsumptionOtherFuelsMonthly}\label{energyconsumptionotherfuelsmonthly}
+
+\begin{itemize}
+\item
+  OtherFuel1:Facility (SumOrAverage)
+\item
+  OtherFuel1:Facility (Maximum)
+\item
+  OtherFuel2:Facility (SumOrAverage)
+\item
+  OtherFuel2:Facility (Maximum)
+\end{itemize}
+
+\paragraph{EndUseEnergyConsumptionElectricityMonthly}\label{enduseenergyconsumptionelectricitymonthly}
+
+\begin{itemize}
+\item
+  InteriorLights:Electricity (SumOrAverage)
+\item
+  ExteriorLights:Electricity (SumOrAverage)
+\item
+  InteriorEquipment:Electricity (SumOrAverage)
+\item
+  ExteriorEquipment:Electricity (SumOrAverage)
+\item
+  Fans:Electricity (SumOrAverage)
+\item
+  Pumps:Electricity (SumOrAverage)
+\item
+  Heating:Electricity (SumOrAverage)
+\item
+  Cooling:Electricity (SumOrAverage)
+\item
+  HeatRejection:Electricity (SumOrAverage)
+\item
+  Humidifier:Electricity (SumOrAverage)
+\item
+  HeatRecovery:Electricity (SumOrAverage)
+\item
+  WaterSystems:Electricity (SumOrAverage)
+\item
+  Cogeneration:Electricity (SumOrAverage)
+\end{itemize}
+
+\paragraph{EndUseEnergyConsumptionNaturalGasMonthly}\label{enduseenergyconsumptionnaturalgasmonthly}
+
+\begin{itemize}
+\item
+  InteriorEquipment:Gas (SumOrAverage)
+\item
+  ExteriorEquipment:Gas (SumOrAverage)
+\item
+  Heating:Gas (SumOrAverage)
+\item
+  Cooling:Gas (SumOrAverage)
+\item
+  WaterSystems:Gas (SumOrAverage)
+\item
+  Cogeneration:Gas (SumOrAverage)
+\end{itemize}
+
+\paragraph{EndUseEnergyConsumptionDieselMonthly}\label{enduseenergyconsumptiondieselmonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:Diesel (SumOrAverage)
+\item
+  Cooling:Diesel (SumOrAverage)
+\item
+  Heating:Diesel (SumOrAverage)
+\item
+  WaterSystems:Diesel (SumOrAverage)
+\item
+  Cogeneration:Diesel (SumOrAverage)
+\end{itemize}
+
+\paragraph{EndUseEnergyConsumptionFuelOilMonthly}\label{enduseenergyconsumptionfueloilmonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:FuelOil\#1 (SumOrAverage)
+\item
+  Cooling:FuelOil\#1 (SumOrAverage)
+\item
+  Heating:FuelOil\#1 (SumOrAverage)
+\item
+  WaterSystems:FuelOil\#1 (SumOrAverage)
+\item
+  Cogeneration:FuelOil\#1 (SumOrAverage)
+\item
+  ExteriorEquipment:FuelOil\#2 (SumOrAverage)
+\item
+  Cooling:FuelOil\#2 (SumOrAverage)
+\item
+  Heating:FuelOil\#2 (SumOrAverage)
+\item
+  WaterSystems:FuelOil\#2 (SumOrAverage)
+\item
+  Cogeneration:FuelOil\#2 (SumOrAverage)
+\end{itemize}
+
+\paragraph{EndUseEnergyConsumptionCoalMonthly}\label{enduseenergyconsumptioncoalmonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:Coal (SumOrAverage)
+\item
+  Heating:Coal (SumOrAverage)
+\item
+  WaterSystems:Coal (SumOrAverage)
+\end{itemize}
+
+\paragraph{EndUseEnergyConsumptionPropaneMonthly}\label{enduseenergyconsumptionpropanemonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:Propane (SumOrAverage)
+\item
+  Cooling:Propane (SumOrAverage)
+\item
+  Heating:Propane (SumOrAverage)
+\item
+  WaterSystems:Propane (SumOrAverage)
+\item
+  Cogeneration:Propane (SumOrAverage)
+\end{itemize}
+
+\paragraph{EndUseEnergyConsumptionGasolineMonthly}\label{enduseenergyconsumptiongasolinemonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:Gasoline (SumOrAverage)
+\item
+  Cooling:Gasoline (SumOrAverage)
+\item
+  Heating:Gasoline (SumOrAverage)
+\item
+  WaterSystems:Gasoline (SumOrAverage)
+\item
+  Cogeneration:Gasoline (SumOrAverage)
+\end{itemize}
+
+\paragraph{EndUseEnergyConsumptionOtherFuelsMonthly}\label{enduseenergyconsumptionotherfuelsmonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:OtherFuel1 (SumOrAverage)
+\item
+  Cooling:OtherFuel1 (SumOrAverage)
+\item
+  Heating:OtherFuel1 (SumOrAverage)
+\item
+  WaterSystems:OtherFuel1 (SumOrAverage)
+\item
+  Cogeneration:OtherFuel1 (SumOrAverage)
+\item
+  ExteriorEquipment:OtherFuel1 (SumOrAverage)
+\item
+  Cooling:OtherFuel2 (SumOrAverage)
+\item
+  Heating:OtherFuel2 (SumOrAverage)
+\item
+  WaterSystems:OtherFuel2 (SumOrAverage)
+\item
+  Cogeneration:OtherFuel2 (SumOrAverage)
+\end{itemize}
+
+\paragraph{PeakEnergyEndUseElectricityPart1Monthly}\label{peakenergyenduseelectricitypart1monthly}
+
+\begin{itemize}
+\item
+  InteriorLights:Electricity (Maximum)
+\item
+  ExteriorLights:Electricity (Maximum)
+\item
+  InteriorEquipment:Electricity (Maximum)
+\item
+  ExteriorEquipment:Electricity (Maximum)
+\item
+  Fans:Electricity (Maximum)
+\item
+  Pumps:Electricity (Maximum)
+\item
+  Heating:Electricity (Maximum)
+\end{itemize}
+
+\paragraph{PeakEnergyEndUseElectricityPart2Monthly}\label{peakenergyenduseelectricitypart2monthly}
+
+\begin{itemize}
+\item
+  Cooling:Electricity (Maximum)
+\item
+  HeatRejection:Electricity (Maximum)
+\item
+  Humidifier:Electricity (Maximum)
+\item
+  HeatRecovery:Electricity (Maximum)
+\item
+  WaterSystems:Electricity (Maximum)
+\item
+  Cogeneration:Electricity (Maximum)
+\end{itemize}
+
+\paragraph{ElectricComponentsOfPeakDemandMonthly}\label{electriccomponentsofpeakdemandmonthly}
+
+\begin{itemize}
+\item
+  Electricity:Facility (Maximum)
+\item
+  InteriorLights:Electricity (ValueWhenMaxMin)
+\item
+  InteriorEquipment:Electricity (ValueWhenMaxMin)
+\item
+  ExteriorLights:Electricity (ValueWhenMaxMin)
+\item
+  ExteriorEquipment:Electricity (ValueWhenMaxMin)
+\item
+  Fans:Electricity (ValueWhenMaxMin)
+\item
+  Pumps:Electricity (ValueWhenMaxMin)
+\item
+  Heating:Electricity (ValueWhenMaxMin)
+\item
+  Cooling:Electricity (ValueWhenMaxMin)
+\item
+  HeatRejection:Electricity (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{PeakEnergyEndUseNaturalGasMonthly}\label{peakenergyendusenaturalgasmonthly}
+
+\begin{itemize}
+\item
+  InteriorEquipment:Gas (Maximum)
+\item
+  ExteriorEquipment:Gas (Maximum)
+\item
+  Heating:Gas (Maximum)
+\item
+  Cooling:Gas (Maximum)
+\item
+  WaterSystems:Gas (Maximum)
+\item
+  Cogeneration:Gas (Maximum)
+\end{itemize}
+
+\paragraph{PeakEnergyEndUseDieselMonthly}\label{peakenergyendusedieselmonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:Diesel (Maximum)
+\item
+  Cooling:Diesel (Maximum)
+\item
+  Heating:Diesel (Maximum)
+\item
+  WaterSystems:Diesel (Maximum)
+\item
+  Cogeneration:Diesel (Maximum)
+\end{itemize}
+
+\paragraph{PeakEnergyEndUseFuelOilMonthly}\label{peakenergyendusefueloilmonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:FuelOil\#1 (Maximum)
+\item
+  Cooling:FuelOil\#1 (Maximum)
+\item
+  Heating:FuelOil\#1 (Maximum)
+\item
+  WaterSystems:FuelOil\#1 (Maximum)
+\item
+  Cogeneration:FuelOil\#1 (Maximum)
+\item
+  ExteriorEquipment:FuelOil\#2 (Maximum)
+\item
+  Cooling:FuelOil\#2 (Maximum)
+\item
+  Heating:FuelOil\#2 (Maximum)
+\item
+  WaterSystems:FuelOil\#2 (Maximum)
+\item
+  Cogeneration:FuelOil\#2 (Maximum)
+\end{itemize}
+
+\paragraph{PeakEnergyEndUseCoalMonthly}\label{peakenergyendusecoalmonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:Coal (Maximum)
+\item
+  Heating:Coal (Maximum)
+\item
+  WaterSystems:Coal (Maximum)
+\end{itemize}
+
+\paragraph{PeakEnergyEndUsePropaneMonthly}\label{peakenergyendusepropanemonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:Propane (Maximum)
+\item
+  Cooling:Propane (Maximum)
+\item
+  Heating:Propane (Maximum)
+\item
+  WaterSystems:Propane (Maximum)
+\item
+  Cogeneration:Propane (Maximum)
+\end{itemize}
+
+\paragraph{PeakEnergyEndUseGasolineMonthly}\label{peakenergyendusegasolinemonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:Gasoline (Maximum)
+\item
+  Cooling:Gasoline (Maximum)
+\item
+  Heating:Gasoline (Maximum)
+\item
+  WaterSystems:Gasoline (Maximum)
+\item
+  Cogeneration:Gasoline (Maximum)
+\end{itemize}
+
+\paragraph{PeakEnergyEndUseOtherFuelsMonthly}\label{peakenergyenduseotherfuelsmonthly}
+
+\begin{itemize}
+\item
+  ExteriorEquipment:OtherFuel1 (Maximum)
+\item
+  Cooling:OtherFuel1 (Maximum)
+\item
+  Heating:OtherFuel1 (Maximum)
+\item
+  WaterSystems:OtherFuel1 (Maximum)
+\item
+  Cogeneration:OtherFuel1 (Maximum)
+\item
+  ExteriorEquipment:OtherFuel1 (Maximum)
+\item
+  Cooling:OtherFuel1 (Maximum)
+\item
+  Heating:OtherFuel1 (Maximum)
+\item
+  WaterSystems:OtherFuel1 (Maximum)
+\item
+  Cogeneration:OtherFuel1 (Maximum)
+\end{itemize}
+
+\paragraph{SetpointsNotMetWithTemperaturesMonthly}\label{setpointsnotmetwithtemperaturesmonthly}
+
+\begin{itemize}
+\item
+  Zone Heating Setpoint Not Met Time (HoursNonZero)
+\item
+  Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
+\item
+  Zone Heating Setpoint Not Met While Occupied Time (HoursNonZero)
+\item
+  Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
+\item
+  Zone Cooling Setpoint Not Met Time (HoursNonZero)
+\item
+  Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
+\item
+  Zone Cooling Setpoint Not Met While Occupied Time (HoursNonZero)
+\item
+  Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
+\end{itemize}
+
+\paragraph{ComfortReportSimple55Monthly}\label{comfortreportsimple55monthly}
+
+\begin{itemize}
+\item
+  Zone Thermal Comfort ASHRAE 55 Simple Model Summer Clothes Not Comfortable Time (HoursNonZero)
+\item
+  Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
+\item
+  Zone Thermal Comfort ASHRAE 55 Simple Model Winter Clothes Not Comfortable Time (HoursNonZero)
+\item
+  Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
+\item
+  Zone Thermal Comfort ASHRAE 55 Simple Model Summer or Winter Clothes Not Comfortable Time (HoursNonZero)
+\item
+  Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
+\end{itemize}
+
+\paragraph{UnglazedTranspiredSolarCollectorSummaryMonthly}\label{unglazedtranspiredsolarcollectorsummarymonthly}
+
+\begin{itemize}
+\item
+  Solar Collector System Efficiency (HoursNonZero)
+\item
+  Solar Collector System Efficiency (SumOrAverageDuringHoursShown)
+\item
+  Solar Collector Outside Face Suction Velocity (SumOrAverageDuringHoursShown)
+\item
+  Solar Collector Sensible Heating Rate (SumOrAverageDuringHoursShown)
+\end{itemize}
+
+\paragraph{OccupantComfortDataSummaryMonthly}\label{occupantcomfortdatasummarymonthly}
+
+\begin{itemize}
+\item
+  Zone People Occupant Count (HoursNonZero)
+\item
+  Zone Air Temperature (SumOrAverageDuringHoursShown)
+\item
+  Zone Air Relative Humidity (SumOrAverageDuringHoursShown)
+\item
+  Zone Thermal Comfort Fanger Model PMV (SumOrAverageDuringHoursShown)
+\item
+  Zone Thermal Comfort Fanger Model PPD (SumOrAverageDuringHoursShown)
+\end{itemize}
+
+\paragraph{ChillerReportMonthly}\label{chillerreportmonthly}
+
+\begin{itemize}
+\item
+  Chiller Electric Energy (SumOrAverage)
+\item
+  Chiller Electric Power (Maximum)
+\item
+  Chiller Electric Energy (HoursNonZero)
+\item
+  Chiller Evaporator Cooling Energy (SumOrAverage)
+\item
+  Chiller Condenser Heat Transfer Energy (SumOrAverage)
+\item
+  Chiller COP (SumOrAverage)
+\item
+  Chiller COP (Maximum)
+\end{itemize}
+
+\paragraph{TowerReportMonthly}\label{towerreportmonthly}
+
+\begin{itemize}
+\item
+  Tower Fan Electric Consumption (SumOrAverage)
+\item
+  Tower Fan Electric Consumption (HoursNonZero)
+\item
+  Cooling Tower Fan Electric Power (Maximum)
+\item
+  Cooling Tower Heat Transfer Rate (Maximum)
+\item
+  Cooling Tower Inlet Temperature (SumOrAverage)
+\item
+  Cooling Tower Outlet Temperature (SumOrAverage)
+\item
+  Cooling Tower Mass Flow Rate (SumOrAverage)
+\end{itemize}
+
+\paragraph{BoilerReportMonthly}\label{boilerreportmonthly}
+
+\begin{itemize}
+\item
+  Boiler Heating Energy (SumOrAverage)
+\item
+  Boiler Gas Consumption (SumOrAverage)
+\item
+  Boiler Heating Energy (HoursNonZero)
+\item
+  Boiler Heating Rate (Maximum)
+\item
+  Boiler Gas Consumption Rate (Maximum)
+\item
+  Boiler Inlet Temperature (SumOrAverage)
+\item
+  Boiler Outlet Temperature (SumOrAverage)
+\item
+  Boiler Mass Flow Rate (SumOrAverage)
+\item
+  Boiler Ancillary Electric Power (SumOrAverage)
+\end{itemize}
+
+\paragraph{DXReportMonthly}\label{dxreportmonthly}
+
+\begin{itemize}
+\item
+  Cooling Coil Total Cooling Energy (SumOrAverage)
+\item
+  Cooling Coil Electric Energy (SumOrAverage)
+\item
+  Cooling Coil Total Cooling Energy (HoursNonZero)
+\item
+  Cooling Coil Sensible Cooling Energy (SumOrAverage)
+\item
+  Cooling Coil Latent Cooling Energy (SumOrAverage)
+\item
+  Cooling Coil Crankcase Heater Electric Energy (SumOrAverage)
+\item
+  Cooling Coil Runtime Fraction (Maximum)
+\item
+  Cooling Coil Runtime Fraction (Minimum)
+\item
+  DX Coil Total Cooling Rate (Maximum)
+\item
+  Cooling Coil Sensible Cooling Rate (Maximum)
+\item
+  Cooling Coil Latent Cooling Rate (Maximum)
+\item
+  Cooling Coil Electric Power (Maximum)
+\item
+  Cooling Coil Crankcase Heater Electric Power (Maximum)
+\end{itemize}
+
+\paragraph{WindowReportMonthly}\label{windowreportmonthly}
+
+\begin{itemize}
+\item
+  Surface Window Transmitted Solar Radiation Rate (SumOrAverage)
+\item
+  Surface Window Transmitted Beam Solar Radiation Rate (SumOrAverage)
+\item
+  Surface Window Transmitted Diffuse Solar Radiation Rate (SumOrAverage)
+\item
+  Surface Window Heat Gain Rate (SumOrAverage)
+\item
+  Surface Window Heat Loss Rate (SumOrAverage)
+\item
+  Surface Window Inside Face Glazing Condensation Status (HoursNonZero)
+\item
+  Surface Shading Device Is On Time Fraction (HoursNonZero)
+\item
+  Surface Storm Window On Off Status (HoursNonZero)
+\end{itemize}
+
+\paragraph{WindowEnergyReportMonthly}\label{windowenergyreportmonthly}
+
+\begin{itemize}
+\item
+  Surface Window Transmitted Solar Radiation Energy (SumOrAverage)
+\item
+  Surface Window Transmitted Beam Solar Radiation Rate Energy (SumOrAverage)
+\item
+  Surface Window Transmitted Diffuse Solar Radiation Energy (SumOrAverage)
+\item
+  Surface Window Heat Gain Energy (SumOrAverage)
+\item
+  Surface Window Heat Loss Energy (SumOrAverage)
+\end{itemize}
+
+\paragraph{WindowZoneSummaryMonthly}\label{windowzonesummarymonthly}
+
+\begin{itemize}
+\item
+  Zone Windows Total Heat Gain Rate (SumOrAverage)
+\item
+  Zone Windows Total Heat Loss Rate (SumOrAverage)
+\item
+  Zone Windows Total Transmitted Solar Radiation Rate (SumOrAverage)
+\item
+  Zone Exterior Windows Total Transmitted Beam Solar Radiation Rate (SumOrAverage)
+\item
+  Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Rate (SumOrAverage)
+\item
+  Zone Interior Windows Total Transmitted Diffuse Solar Radiation Rate (SumOrAverage)
+\item
+  Zone Interior Windows Total Transmitted Beam Solar Radiation Rate (SumOrAverage)
+\end{itemize}
+
+\paragraph{WindowEnergyZoneSummaryMonthly}\label{windowenergyzonesummarymonthly}
+
+\begin{itemize}
+\item
+  Zone Windows Total Heat Gain Energy (SumOrAverage)
+\item
+  Zone Windows Total Heat Loss Energy (SumOrAverage)
+\item
+  Zone Windows Total Transmitted Solar Radiation Energy (SumOrAverage)
+\item
+  Zone Exterior Windows Total Transmitted Beam Solar Radiation Energy (SumOrAverage)
+\item
+  Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Energy (SumOrAverage)
+\item
+  Zone Interior Windows Total Transmitted Diffuse Solar Radiation Energy (SumOrAverage)
+\item
+  Zone Interior Windows Total Transmitted Beam Solar Radiation Energy (SumOrAverage)
+\end{itemize}
+
+\paragraph{AverageOutdoorConditionsMonthly}\label{averageoutdoorconditionsmonthly}
+
+\begin{itemize}
+\item
+  Site Outdoor Air Drybulb Temperature (SumOrAverage)
+\item
+  Site Outdoor Air Wetbulb Temperature (SumOrAverage)
+\item
+  Site Outdoor Air Dewpoint Temperature (SumOrAverage)
+\item
+  Wind Speed (SumOrAverage)
+\item
+  Site Sky Temperature (SumOrAverage)
+\item
+  Site Diffuse Solar Radiation Rate per Area (SumOrAverage)
+\item
+  Site Direct Solar Radiation Rate per Area (SumOrAverage)
+\item
+  Raining (SumOrAverage)
+\end{itemize}
+
+\paragraph{OutdoorConditionsMaximumDryBulbMonthly}\label{outdoorconditionsmaximumdrybulbmonthly}
+
+\begin{itemize}
+\item
+  Site Outdoor Air Drybulb Temperature (Maximum)
+\item
+  Site Outdoor Air Wetbulb Temperature (ValueWhenMaxMin)
+\item
+  Site Outdoor Air Dewpoint Temperature (ValueWhenMaxMin)
+\item
+  Wind Speed (ValueWhenMaxMin)
+\item
+  Site Sky Temperature (ValueWhenMaxMin)
+\item
+  Site Diffuse Solar Radiation Rate per Area (ValueWhenMaxMin)
+\item
+  Site Direct Solar Radiation Rate per Area (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{OutdoorConditionsMinimumDryBulbMonthly}\label{outdoorconditionsminimumdrybulbmonthly}
+
+\begin{itemize}
+\item
+  Site Outdoor Air Wetbulb Temperature (ValueWhenMaxMin)
+\item
+  Site Outdoor Air Dewpoint Temperature (ValueWhenMaxMin)
+\item
+  Wind Speed (ValueWhenMaxMin)
+\item
+  Site Sky Temperature (ValueWhenMaxMin)
+\item
+  Site Diffuse Solar Radiation Rate per Area (ValueWhenMaxMin)
+\item
+  Site Direct Solar Radiation Rate per Area (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{OutdoorConditionsMaximumWetBulbMonthly}\label{outdoorconditionsmaximumwetbulbmonthly}
+
+\begin{itemize}
+\item
+  Site Outdoor Air Wetbulb Temperature (Maximum)
+\item
+  Site Outdoor Air Drybulb Temperature (ValueWhenMaxMin)
+\item
+  Site Outdoor Air Dewpoint Temperature (ValueWhenMaxMin)
+\item
+  Wind Speed (ValueWhenMaxMin)
+\item
+  Site Sky Temperature (ValueWhenMaxMin)
+\item
+  Site Diffuse Solar Radiation Rate per Area (ValueWhenMaxMin)
+\item
+  Site Direct Solar Radiation Rate per Area (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{OutdoorConditionsMaximumDewPointMonthly}\label{outdoorconditionsmaximumdewpointmonthly}
+
+\begin{itemize}
+\item
+  Site Outdoor Air Dewpoint Temperature (Maximum)
+\item
+  Site Outdoor Air Drybulb Temperature (ValueWhenMaxMin)
+\item
+  Site Outdoor Air Wetbulb Temperature (ValueWhenMaxMin)
+\item
+  Wind Speed (ValueWhenMaxMin)
+\item
+  Site Sky Temperature (ValueWhenMaxMin)
+\item
+  Site Diffuse Solar Radiation Rate per Area (ValueWhenMaxMin)
+\item
+  Site Direct Solar Radiation Rate per Area (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{OutdoorGroundConditionsMonthly}\label{outdoorgroundconditionsmonthly}
+
+\begin{itemize}
+\item
+  Site Ground Temperature (SumOrAverage)
+\item
+  Site Surface Ground Temperature (SumOrAverage)
+\item
+  Site Deep Ground Temperature (SumOrAverage)
+\item
+  Site Mains Water Temperature (SumOrAverage)
+\item
+  Site Ground Reflected Solar Radiation Rate per Area (SumOrAverage)
+\item
+  Snow On Ground (SumOrAverage)
+\end{itemize}
+
+\paragraph{WindowACReportMonthly}\label{windowacreportmonthly}
+
+\begin{itemize}
+\item
+  Zone Window Air Conditioner Total Cooling Energy (SumOrAverage)
+\item
+  Zone Window Air Conditioner Electric Energy (SumOrAverage)
+\item
+  Zone Window Air Conditioner Total Cooling Energy (HoursNonZero)
+\item
+  Zone Window Air Conditioner Sensible Cooling Energy (SumOrAverage)
+\item
+  Zone Window Air Conditioner Latent Cooling Energy (SumOrAverage)
+\item
+  Zone Window Air Conditioner Total Cooling Rate (Maximum)
+\item
+  Zone Window Air Conditioner Sensible Cooling Rate (ValueWhenMaxMin)
+\item
+  Zone Window Air Conditioner Latent Cooling Rate (ValueWhenMaxMin)
+\item
+  Zone Window Air Conditioner Electric Power (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{WaterHeaterReportMonthly}\label{waterheaterreportmonthly}
+
+\begin{itemize}
+\item
+  Water Heater Total Demand Energy (SumOrAverage)
+\item
+  Water Heater Use Side Heat Transfer Energy (SumOrAverage)
+\item
+  Water Heater Burner Heating Energy (SumOrAverage)
+\item
+  Water Heater Gas Consumption (SumOrAverage)
+\item
+  Water Heater Total Demand Energy (HoursNonZero)
+\item
+  Water Heater Loss Demand Energy (SumOrAverage)
+\item
+  Water Heater Heat Loss Energy (SumOrAverage)
+\item
+  Water Heater Tank Temperature (SumOrAverage)
+\item
+  Water Heater Heat Recovery Supply Energy (SumOrAverage)
+\item
+  Water Heater Source Side Heat Transfer Energy (SumOrAverage)
+\end{itemize}
+
+\paragraph{GeneratorReportMonthly}\label{generatorreportmonthly}
+
+\begin{itemize}
+\item
+  Generator Produced Electric Energy (SumOrAverage)
+\item
+  Generator Diesel Energy (SumOrAverage)
+\item
+  Generator Gas Consumption (SumOrAverage)
+\item
+  Generator Produced Electric Energy (HoursNonZero)
+\item
+  Generator Total Heat Recovery (SumOrAverage)
+\item
+  Generator Jacket Heat Recovery Energy (SumOrAverage)
+\item
+  Generator Lube Heat Recovery Energy (SumOrAverage)
+\item
+  Generator Exhaust Heat Recovery Energy (SumOrAverage)
+\item
+  Generator Exhaust Air Temperature (SumOrAverage)
+\end{itemize}
+
+\paragraph{DaylightingReportMonthly}\label{daylightingreportmonthly}
+
+\begin{itemize}
+\item
+  Site Exterior Beam Normal Illuminance (HoursNonZero)
+\item
+  Daylighting Lighting Power Multiplier (SumOrAverageDuringHoursShown)
+\item
+  Daylighting Lighting Power Multiplier (MinimumDuringHoursShown)
+\item
+  Daylighting Reference Point 1 Illuminance (SumOrAverageDuringHoursShown)
+\item
+  Daylighting Reference Point 1 Glare Index (SumOrAverageDuringHoursShown)
+\item
+  Daylighting Reference Point 2 Illuminance (SumOrAverageDuringHoursShown)
+\item
+  Daylighting Reference Point 2 Glare Index (SumOrAverageDuringHoursShown)
+\item
+  Daylighting Reference Point 1 Glare Index Setpoint Exceeded Time
+\item
+  Daylighting Reference Point 2 Glare Index Setpoint Exceeded Time
+\item
+  Daylighting Reference Point 1 Daylight Illuminance Setpoint Exceeded Time
+\item
+  Daylighting Reference Point 2 Daylight Illuminance Setpoint Exceeded Time
+\end{itemize}
+
+\paragraph{CoilReportMonthly}\label{coilreportmonthly}
+
+\begin{itemize}
+\item
+  Heating Coil Heating Energy (SumOrAverage)
+\item
+  Heating Coil Heating Rate (Maximum)
+\item
+  Cooling Coil Total Cooling Energy (SumOrAverage)
+\item
+  Cooling Coil Sensible Cooling Energy (SumOrAverage)
+\item
+  Cooling Coil Total Cooling Rate (Maximum)
+\item
+  Cooling Coil Sensible Cooling Rate (ValueWhenMaxMin)
+\item
+  Cooling Coil Wetted Area Fraction (SumOrAverage)
+\end{itemize}
+
+\paragraph{PlantLoopDemandReportMonthly}\label{plantloopdemandreportmonthly}
+
+\begin{itemize}
+\item
+  Plant Supply Side Cooling Demand Rate (SumOrAverage)
+\item
+  Plant Supply Side Cooling Demand Rate (Maximum)
+\item
+  Plant Supply Side Heating Demand Rate (SumOrAverage)
+\item
+  Plant Supply Side Heating Demand Rate (Maximum)
+\end{itemize}
+
+\paragraph{FanReportMonthly}\label{fanreportmonthly}
+
+\begin{itemize}
+\item
+  Fan Electric Consumption (SumOrAverage)
+\item
+  Fan Rise in Air Temperature (SumOrAverage)
+\item
+  Fan Electric Power (Maximum)
+\item
+  Fan Rise in Air Temperature (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{PumpReportMonthly}\label{pumpreportmonthly}
+
+\begin{itemize}
+\item
+  Pump Electric Energy (SumOrAverage)
+\item
+  Pump Fluid Heat Gain Energy (SumOrAverage)
+\item
+  Pump Electric Power (Maximum)
+\item
+  Pump Shaft Power (ValueWhenMaxMin)
+\item
+  Pump Fluid Heat Gain Rate (ValueWhenMaxMin)
+\item
+  Pump Outlet Temperature (ValueWhenMaxMin)
+\item
+  Pump Mass Flow Rate (ValueWhenMaxMin)
+\end{itemize}
+
+\paragraph{CondLoopDemandReportMonthly}\label{condloopdemandreportmonthly}
+
+\begin{itemize}
+\item
+  Plant Supply Side Cooling Demand Rate (SumOrAverage)
+\item
+  Plant Supply Side Cooling Demand Rate (Maximum)
+\item
+  Plant Supply Side Inlet Temperature (ValueWhenMaxMin)
+\item
+  Plant Supply Side Outlet Temperature (ValueWhenMaxMin)
+\item
+  Plant Supply Side Heating Demand Rate (SumOrAverage)
+\item
+  Plant Supply Side Heating Demand Rate (Maximum)
+\end{itemize}
+
+\paragraph{ZoneTemperatureOscillationReportMonthly}\label{zonetemperatureoscillationreportmonthly}
+
+\begin{itemize}
+\item
+  Zone Oscillating Temperatures Time (HoursNonZero)
+\item
+  Zone People Occupant Count (SumOrAverageDuringHoursShown)
+\end{itemize}
+
+\paragraph{AirLoopSystemEnergyAndWaterUseMonthly}\label{airloopsystemenergyandwaterusemonthly}
+
+\begin{itemize}
+\item
+  Air System Hot Water Energy (SumOrAverage)
+\item
+  Air System Steam Energy (SumOrAverage)
+\item
+  Air System Chilled Water Energy (SumOrAverage)
+\item
+  Air System Electric Energy (SumOrAverage)
+\item
+  Air System Gas Energy (SumOrAverage)
+\item
+  Air System Water Volume (SumOrAverage)
+\end{itemize}
+
+\paragraph{AirLoopSystemComponentLoadsMonthly}\label{airloopsystemcomponentloadsmonthly}
+
+\begin{itemize}
+\item
+  Air System Fan Air Heating Energy (SumOrAverage)
+\item
+  Air System Cooling Coil Total Cooling Energy (SumOrAverage)
+\item
+  Air System Heating Coil Total Heating Energy (SumOrAverage)
+\item
+  Air System Heat Exchanger Total Heating Energy (SumOrAverage)
+\item
+  Air System Heat Exchanger Total Cooling Energy (SumOrAverage)
+\item
+  Air System Humidifier Total Heating Energy (SumOrAverage)
+\item
+  Air System Evaporative Cooler Total Cooling Energy (SumOrAverage)
+\item
+  Air System Desiccant Dehumidifier Total Cooling Energy (SumOrAverage)
+\end{itemize}
+
+\paragraph{AirLoopSystemComponentEnergyUseMonthly}\label{airloopsystemcomponentenergyusemonthly}
+
+\begin{itemize}
+\item
+  Air System Fan Electric Energy (SumOrAverage)
+\item
+  Air System Heating Coil Hot Water Energy (SumOrAverage)
+\item
+  Air System Cooling Coil Chilled Water Energy (SumOrAverage)
+\item
+  Air System DX Heating Coil Electric Energy (SumOrAverage)
+\item
+  Air System DX Cooling Coil Electric Energy (SumOrAverage)
+\item
+  Air System Heating Coil Electric Energy (SumOrAverage)
+\item
+  Air System Heating Coil Gas Energy (SumOrAverage)
+\item
+  Air System Heating Coil Steam Energy (SumOrAverage)
+\item
+  Air System Humidifier Electric Energy (SumOrAverage)
+\item
+  Air System Evaporative Cooler Electric Energy (SumOrAverage)
+\item
+  Air System Desiccant Dehumidifier Electric Energy (SumOrAverage)
+\end{itemize}
+
+\paragraph{MechanicalVentilationLoadsMonthly}\label{mechanicalventilationloadsmonthly}
+
+\begin{itemize}
+\item
+  Zone Mechanical Ventilation No Load Heat Removal Energy (SumOrAverage)
+\item
+  Zone Mechanical Ventilation Cooling Load Increase Energy (SumOrAverage)
+\item
+  Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy (SumOrAverage)
+\item
+  Zone Mechanical Ventilation Cooling Load Decrease Energy (SumOrAverage)
+\item
+  Zone Mechanical Ventilation No Load Heat Addition Energy (SumOrAverage)
+\item
+  Zone Mechanical Ventilation Heating Load Increase Energy (SumOrAverage)
+\item
+  Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy (SumOrAverage)
+\item
+  Zone Mechanical Ventilation Heating Load Decrease Energy (SumOrAverage)
+\item
+  Zone Mechanical Ventilation Air Changes per Hour (SumOrAverage)
+\end{itemize}
+
+Sample IDF Input -- Output:Table:SummaryReports
+
+\begin{lstlisting}
+
+Output:Table:SummaryReports,
+          AllSummary,  !- Report 1 Name
+          AllMonthly;  !- Report 2 Name
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/standard-output-reports/output-table-timebins.tex b/doc/input-output-reference/src/standard-output-reports/output-table-timebins.tex
new file mode 100644
index 00000000000..16c05e9b6fa
--- /dev/null
+++ b/doc/input-output-reference/src/standard-output-reports/output-table-timebins.tex
@@ -0,0 +1,60 @@
+\section{Output:Table:TimeBins}\label{outputtabletimebins}
+
+The Output:Table:TimeBins report shows the amount of time in hours that occurs in different bins for the single specific variable or meter specified. Two different types of binning occur: by month and by hour of the day.
+
+The IntervalStart, IntervalSize and IntervalCount determine the size of the bins for many of the types of reports that can be generated. The IntervalStart value is the lowest value of the first bin. The first bin is for all values greater or equal to IntervalStart and less than IntervalStart+IntervalSize. This gets repeated IntervalCount times. A bin for below the first interval and above the last interval is automatically created. Each table also has totals for the column and the rows. The report produced by Report:Table:TimeBins also indicates the total time simulated (for an annual simulation this would be 8760 hours).
+
+NOTE:~ For summed variables, such as meters, the values are divided by the length of the timestep in seconds before binning. For example, the bins for a variable in Joules are reported in Joules per second (Watts). The interval values must then be entered accordingly.
+
+\subsection{Inputs}\label{inputs-065}
+
+\paragraph{Field: Key Value}\label{field-key-value-000}
+
+The Key Value field indicates which instance of a variable is reported. An asterisk indicates that a table would be produced for every key.
+
+\paragraph{Field: Variable Name}\label{field-variable-name-000}
+
+The variable name to be reported. Reference the eplusout.rdd file for names that are specific to your simulation input file. You do not need to include the units {[]} field in your names here.
+
+\paragraph{Field: Interval Start}\label{field-interval-start}
+
+The lower value of the first bin. The first bin is for all values greater or equal to the IntervalStart and less than IntervalStart + IntervalSize. See note above regarding summed variables.
+
+\paragraph{Field: Interval Size}\label{field-interval-size}
+
+The amount by which each bin range is to increase, i.e.~the difference between the upper and lower limits of each bin. See note above regarding summed variables.
+
+\paragraph{Field: Interval Count}\label{field-interval-count}
+
+The number of bins desired.
+
+\paragraph{Field: Schedule Name}\label{field-schedule-name-009}
+
+Optional schedule name. If left blank, binning is performed for all hours simulated. If a schedule is specified, binning is performed for non-zero hours in the schedule.
+
+\paragraph{Field: Variable Type}\label{field-variable-type}
+
+This field is used to indicate the kind of units that may be associated with the variable. It is used by IDF Editor to display the appropriate SI and IP units for the Interval Start and Interval Size values. The available options are shown below.
+
+\begin{itemize}
+\item
+  Energy
+\item
+  Temperature
+\item
+  Flowrate
+\item
+  Demand
+\end{itemize}
+
+An example of a time bins input object follows.
+
+\begin{lstlisting}
+
+Output:Table:TimeBins,
+    *,                     ! Key Value
+    Electricity:HVAC,      ! Variable Name
+    4000000,               ! Interval Start
+    500000,                ! Interval Size
+    20;                    ! Interval Count
+\end{lstlisting}
diff --git a/doc/input-output-reference/src/standard-output-reports/outputcontrol-table-style.tex b/doc/input-output-reference/src/standard-output-reports/outputcontrol-table-style.tex
new file mode 100644
index 00000000000..0f2c13b708a
--- /dev/null
+++ b/doc/input-output-reference/src/standard-output-reports/outputcontrol-table-style.tex
@@ -0,0 +1,74 @@
+\section{OutputControl:Table:Style}\label{outputcontroltablestyle}
+
+The OutputControl:Table:Style object controls how all standardized reports are produced.
+
+\subsection{Inputs}\label{inputs-066}
+
+\paragraph{Field: Column Separator}\label{field-column-separator-002}
+
+You have nine different options:
+
+\begin{itemize}
+\item
+  Comma
+\item
+  Tab
+\item
+  Fixed
+\item
+  HTML
+\item
+  XML
+\item
+  CommaAndHTML
+\item
+  TabAndHTML
+\item
+  XMLAndHTML
+\item
+  All
+\end{itemize}
+
+The Comma style produces a text file (eplustbl.csv) with the values of the table separated by commas. This is a good format for importing the results into a spreadsheet. If you do open the file with a spreadsheet, make sure you close the file prior to rerunning EnergyPlus otherwise the file will not be updated.
+
+The Tab style produces a text file (eplustbl.tab) with the values separated by tabs. It is also a good format for using with a spreadsheet program but has the advantage of being more readable in a text editor.
+
+The Fixed style produces a text file (eplustbl.txt) with the values at specific columns. It is the easiest to view using a text editor.
+
+The HTML style produces a file (eplustbl.htm) that can be opened with an internet browser program. The values are shown in a tabular format that is easy to view. One advantage of the HTML style is that the results can be viewed in an internet browser program and EnergyPlus can be rerun and the ``refresh'' button pressed in the internet browser program to see the new results. . When the HTML style is specified, a Table of Contents for the file is generated and placed near the top of the file after the Annual Building Utility Performance Summary (aka ABUPS) report. The Table of Contents includes the names of each report and links for each table in the file.
+
+The XML style produces a file (eplustbl.xml) that can be opened by any XML editor and many internet browser programs. The XML output is specifically intended for use by other software programs to make it simple to extract specific results.
+
+The last four options combine the previous styles and allow multiple reports with different styles to be produced during a single simulation.
+
+\paragraph{Field: Unit Conversion}\label{field-unit-conversion}
+
+This field is optional and if not specified defaults to no unit conversions. Four different input options are available:
+
+\begin{itemize}
+\item
+  None -- no conversions performed
+\item
+  JtoKWH -- Joules converted into kWh (1 / 3,600,000)
+\item
+  JtoMJ -- Joules converted into Megajoules (1 / 1,000,000)
+\item
+  JtoGJ -- Joules converted into Gigajoules (1 / 1,000,000,000)
+\item
+  InchPound -- convert all annual, monthly, economics and timebins tabular values to common Inch-Pound equivalent
+\end{itemize}
+
+The current options are limited to just how the energy is being reported. The default is to report energy in the form of Joules but since the magnitude of those numbers for many buildings is very large, these other conversion factors are available.
+
+The JtoKWH, JtoMJ and JtoGJ unit conversion input option applies only to the Output:Table:Monthly reports and partially to the ABUPS report. For ABUPS, the JtoKWH option changes the report but the JtoMJ and JtoGJ options do not change the report since they it is already in MJ/m2 and GJ.. The InchPound unit conversion input option applies to all annual, monthly, timebins and economic reports that appear in the tabular output file.~ In addition, this option does not effect the standard eplusout.eso file. The eplusout.eso file may be converted by using the ConvertESOMTR utility.
+
+An example IDF input object follows.
+
+\begin{lstlisting}
+
+OutputControl:Table:Style,
+    Comma,                     ! Column Separator
+    InchPound;                 ! Unit Conversion
+\end{lstlisting}
+
+Examples of the tabular reports and descriptions are contained in the Output Details and Examples document.
diff --git a/doc/input-output-reference/src/title.tex b/doc/input-output-reference/src/title.tex
new file mode 100644
index 00000000000..63f37402bb8
--- /dev/null
+++ b/doc/input-output-reference/src/title.tex
@@ -0,0 +1 @@
+\input{../title}
diff --git a/doc/input-output-reference/src/weather-data.tex b/doc/input-output-reference/src/weather-data.tex
new file mode 100644
index 00000000000..1ba113c68d3
--- /dev/null
+++ b/doc/input-output-reference/src/weather-data.tex
@@ -0,0 +1,9 @@
+\chapter{Weather Data}\label{weather-data}
+
+The description of the weather data format (a simple text-based format) is well described in the Auxiliary Programs document and won't be repeated here. Descriptions here will be pertinent to running the EnergyPlus program but you may wish to peruse the other descriptions as the statistics reports from the weather files may be useful during design and simulation.
+
+\input{src/weather-data/missing-weather-file-data}
+
+\input{src/weather-data/weather-data-hourly-interpolation}
+
+\input{src/weather-data/weather-file-data-reporting-errors-during}
diff --git a/doc/input-output-reference/src/weather-data/missing-weather-file-data.tex b/doc/input-output-reference/src/weather-data/missing-weather-file-data.tex
new file mode 100644
index 00000000000..bd8e95b0707
--- /dev/null
+++ b/doc/input-output-reference/src/weather-data/missing-weather-file-data.tex
@@ -0,0 +1,38 @@
+\section{Missing Weather File Data}\label{missing-weather-file-data}
+
+The weather description of data contains ``missing'' descriptors, a new concept not introduced previously in our IDD conventions. In this case, it will be processed as though those values are ``missing'' in the weather conversions and/or EnergyPlus weather processing. This may not always be desirable though EnergyPlus will fill in ``missing'' value with something ``appropriate''. Eventually, these missing values will be available through the IDD and users will be able to supply their own values or EnergyPlus will calculate those values (such as radiation and illuminance) that are not a simple value replacement. Until then, the following are used:
+
+% table 44
+\begin{longtable}[c]{p{1.83in}p{2.67in}p{1.5in}}
+\caption{Missing weather replacement values \label{table:missing-weather-replacement-values}} \tabularnewline
+\toprule 
+Data item & Supplied Value & Units \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Missing weather replacement values} \tabularnewline
+\toprule 
+Data item & Supplied Value & Units \tabularnewline
+\midrule
+\endhead
+
+Dry-bulb Temperature & 6 & C \tabularnewline
+Dewpoint Temperature & 3 & C \tabularnewline
+Relative Humidity & 50 & \% \tabularnewline
+Atmospheric Pressure & Standard** Barometric Pressure (altitude based) & Pa \tabularnewline
+Wind Speed & 2.5 & m/s \tabularnewline
+Wind Direction & 180 & Deg \tabularnewline
+Total Sky Cover & 5 & (tenths) \tabularnewline
+Opaque Sky Cover & 5 & (tenths) \tabularnewline
+Visibility & 777.7 & Km \tabularnewline
+Ceiling Height & 77777 & m \tabularnewline
+Precipitable Water & 0 & Mm \tabularnewline
+Aerosol Optical Depth & 0 & Broadband turbidity \tabularnewline
+Snow Depth & 0 & Cm \tabularnewline
+Days Since Last Snow & 88 & Days \tabularnewline
+Radiation Values (Direct/Diffuse) & 0.0 & Wh/m2 \tabularnewline
+Illuminance Values & 0.0 & lux (or CD/m2) \tabularnewline
+\bottomrule
+\end{longtable}
+
+**Standard Barometric pressure based on location elevation is taken from ASHRAE 2001 Handbook of Fundamentals, Page 6.1 \& 2.
diff --git a/doc/input-output-reference/src/weather-data/weather-data-hourly-interpolation.tex b/doc/input-output-reference/src/weather-data/weather-data-hourly-interpolation.tex
new file mode 100644
index 00000000000..32295be6f30
--- /dev/null
+++ b/doc/input-output-reference/src/weather-data/weather-data-hourly-interpolation.tex
@@ -0,0 +1,75 @@
+\section{Weather Data Hourly Interpolation}\label{weather-data-hourly-interpolation}
+
+Much of the existing weather data is produced in hourly format (refer to the discussion of data formats and weather conversion processing in the Auxiliary Programs Document). In order to match the hourly data in a continuous manner for EnergyPlus (where the timesteps might be less than hourly), simple interpolation between ``last hour's'' values and ``this hour's'' values is performed; we will refer to this as ``Last Hour Interpolation''.
+
+Note that in versions prior to V1.0.3, the interpolation was done between ``this hour'' and ``next hour''. If required, we will refer to this as ``Next Hour Interpolation''.
+
+Remember that hour 1 for EnergyPlus is the time interval 00:00:01AM to 1:00:00AM. Hour 2 is 1:00:01AM to 2:00:00AM (hh:mm:ss). With the interpolation scheme (Last Hour Interpolation) and reporting weather data values at timestep resolution, the ``hour'' values reported should match with the hourly weather data values. (Note that reporting ``hourly'' resolution will not do this unless your ``Number of Timesteps per Hour'' is 1).
+
+Note that this interpolation applies to outdoor data only -- schedule values are not interpolated in this manner.
+
+The weighting scheme / interpolation is simply:
+
+\begin{equation}
+Valu{e_{TimeStep}} = LastHourValue\cdot Weigh{t_{LastHour}} + ThisHourValue\cdot Weigh{t_{ThisHour}}
+\end{equation}
+
+where
+
+\begin{equation}
+Weigh{t_{ThisHour}} = \frac{{CurrentTimeStep}}{{Number\,of\,TimeSteps\,in\,Hour}}
+\end{equation}
+
+\begin{equation}
+Weigh{t_{LastHour}} = 1.0 - Weigh{t_{ThisHour}}
+\end{equation}
+
+To explain further, the weighting for four (4) timesteps in hour is:
+
+% table 45
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Illustration of Data Interpolation for 15 minute timesteps \label{table:illustration-of-data-interpolation-for-15}} \tabularnewline
+\toprule 
+TimeStep & Time (mm:ss) & Weight & Weight \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Illustration of Data Interpolation for 15 minute timesteps} \tabularnewline
+\toprule 
+TimeStep & Time (mm:ss) & Weight & Weight \tabularnewline
+\midrule
+\endhead
+
+1 & 00:01 to 15:00 & .75 & .25 \tabularnewline
+2 & 15:01 to 30:00 & .5 & .5 \tabularnewline
+3 & 30:01 to 45:00 & .25 & .75 \tabularnewline
+4 & 45:01 to 60:00 & 0 & 1.0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+And similarly for six (6) timesteps in hour:
+
+% table 46
+\begin{longtable}[c]{@{}llll@{}}
+\caption{Illustration of Data Interpolation for 10 minute timesteps \label{table:illustration-of-data-interpolation-for-10}} \tabularnewline
+\toprule 
+TimeStep & Time (mm:ss) & Weight & Weight \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Illustration of Data Interpolation for 10 minute timesteps} \tabularnewline
+\toprule 
+TimeStep & Time (mm:ss) & Weight & Weight \tabularnewline
+\midrule
+\endhead
+
+1 & 00:01 to 10:00 & 0.833333333333333 & 0.166666666666667 \tabularnewline
+2 & 10:01 to 20:00 & 0.666666666666667 & 0.333333333333333 \tabularnewline
+3 & 20:01 to 30:00 & .5 & .5 \tabularnewline
+4 & 30:01 to 40:00 & 0.333333333333333 & 0.666666666666667 \tabularnewline
+5 & 40:01 to 50:00 & 0.166666666666667 & 0.833333333333333 \tabularnewline
+6 & 50:01 to 60:00 & 0 & 1.0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+This interpolation gives a smooth, continuous look to the outdoor data. For day boundaries (i.e.~from hour 24 to hour 1), the values from the previous day's last hour (23:00:01 to 24:00:00). For the a design day, this is the values for hour 24. For the first day of a weather simulation, it is likewise values for hour 24 of that day. For subsequent weather days, it will be the last hour of the previous day.
diff --git a/doc/input-output-reference/src/weather-data/weather-file-data-reporting-errors-during.tex b/doc/input-output-reference/src/weather-data/weather-file-data-reporting-errors-during.tex
new file mode 100644
index 00000000000..81552c1caa2
--- /dev/null
+++ b/doc/input-output-reference/src/weather-data/weather-file-data-reporting-errors-during.tex
@@ -0,0 +1,17 @@
+\section{Weather File Data Reporting (errors) during Simulation}\label{weather-file-data-reporting-errors-during-simulation}
+
+Missing data on the weather file used will be summarized on the \textbf{eplusout.err} file. In EnergyPlus, ``missing data'' is shown only for fields that EnergyPlus will use. For the ``WeatherCodes'', an invalid field count (where the number of items in the field does not = 9) will be shown. The number of items count refers to the number of records on the weather file that are in error or missing -- for an hourly weather file, this is the number of hours. Likewise out of range values (see specific fields in the previous definition) will be counted for each occurance and summarized. Note that the out of range values will not be changed by EnergyPlus and could affect your simulation results.
+
+For example:
+
+\begin{lstlisting}
+   ** Warning ** Missing Data Found on Weather Data File
+   ************* Missing Atmospheric Pressure, Number of items =    48
+   ************* Missing Dry Bulb Temperatures, Number of items =    4
+   ** Warning ** Out of Range Data Found on Weather Data File
+\end{lstlisting}
+
+\begin{lstlisting}
+   ************* Out of Range Dry Bulb Temperature [&gt;-70,&lt;70], Number of items =    1
+\end{lstlisting}
+
diff --git a/doc/interface-developer/CMakeLists.txt b/doc/interface-developer/CMakeLists.txt
new file mode 100644
index 00000000000..1b7fc3056c4
--- /dev/null
+++ b/doc/interface-developer/CMakeLists.txt
@@ -0,0 +1,47 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/interface-developer.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/guide-for-interface-developers.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/introduction.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/introduction/interface-expectations.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/energyplus-install-contents.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/input-overview.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/input-overview/general-input-rules.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/input-overview/input-data-dictionary.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/input-overview/input-data-file.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/input-details.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/input-details/idd-conventions.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/input-details/standard-energyplus-units.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/input-details/energyplus-reports.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/output.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/weather-data.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/running-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/licensing.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/src/appendix-a-simple-idf-file.tex
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/../title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/media/image001.png
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/media/image002.jpg
+  ${CMAKE_SOURCE_DIR}/doc/interface-developer/media/image003.png
+) 
+
+SET( SOURCE_FILENAME "interface-developer" )
+SET( OUTPUT_FILENAME "InterfaceDeveloper" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/interface-developer/interface-developer.tex b/doc/interface-developer/interface-developer.tex
new file mode 100644
index 00000000000..8a052803846
--- /dev/null
+++ b/doc/interface-developer/interface-developer.tex
@@ -0,0 +1,52 @@
+\input{../header}
+
+\title{Guide for Interface Developers}
+
+\hypersetup{unicode=true,
+            pdftitle={Guide for Interface Developers},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/guide-for-interface-developers}
+
+\input{src/introduction}
+
+\input{src/introduction/interface-expectations}
+
+\input{src/energyplus-install-contents}
+
+\input{src/input-overview}
+
+\input{src/input-overview/general-input-rules}
+
+\input{src/input-overview/input-data-dictionary}
+
+\input{src/input-overview/input-data-file}
+
+\input{src/input-details}
+
+\input{src/input-details/idd-conventions}
+
+\input{src/input-details/standard-energyplus-units}
+
+\input{src/input-details/energyplus-reports}
+
+\input{src/output}
+
+\input{src/weather-data}
+
+\input{src/running-energyplus}
+
+\input{src/licensing}
+
+\input{src/appendix-a-simple-idf-file}
+
+\end{document}
diff --git a/doc/src/docs/InterfaceDeveloper/media/ep.gif b/doc/interface-developer/media/ep.gif
similarity index 100%
rename from doc/src/docs/InterfaceDeveloper/media/ep.gif
rename to doc/interface-developer/media/ep.gif
diff --git a/doc/interface-developer/media/ep.png b/doc/interface-developer/media/ep.png
new file mode 100644
index 00000000000..a808760c870
Binary files /dev/null and b/doc/interface-developer/media/ep.png differ
diff --git a/doc/src/docs/InterfaceDeveloper/media/image001.png b/doc/interface-developer/media/image001.png
similarity index 100%
rename from doc/src/docs/InterfaceDeveloper/media/image001.png
rename to doc/interface-developer/media/image001.png
diff --git a/doc/src/docs/InterfaceDeveloper/media/image002.jpg b/doc/interface-developer/media/image002.jpg
similarity index 100%
rename from doc/src/docs/InterfaceDeveloper/media/image002.jpg
rename to doc/interface-developer/media/image002.jpg
diff --git a/doc/src/docs/InterfaceDeveloper/media/image003.png b/doc/interface-developer/media/image003.png
similarity index 100%
rename from doc/src/docs/InterfaceDeveloper/media/image003.png
rename to doc/interface-developer/media/image003.png
diff --git a/doc/interface-developer/src/appendix-a-simple-idf-file.tex b/doc/interface-developer/src/appendix-a-simple-idf-file.tex
new file mode 100644
index 00000000000..f2f75f213ae
--- /dev/null
+++ b/doc/interface-developer/src/appendix-a-simple-idf-file.tex
@@ -0,0 +1,576 @@
+\chapter{Appendix A.~ Simple IDF file}\label{appendix-a.-simple-idf-file}
+
+\begin{lstlisting}
+
+!1ZoneUncontrolled.idf
+  ! Basic file description:  Basic test for EnergyPlus.  Resistive Walls.  Regular (no ground contact) floor.
+  !                          Regular roof.  No Windows.
+  !
+  ! Highlights:              Very basic test to see that EnergyPlus "works".
+  !
+  !
+  ! Simulation Location/Run: DENVER_STAPLETON_CO_USA_WMO_724690, 2 design days, 1 run period,
+  !                          Run Control executes two design days (see RUN PERIOD object)
+  !
+  ! Location:                Denver, CO
+  !
+  ! Design Days:             DENVER_STAPLETON_CO_USA Annual Heating 99%, MaxDB = -16°C
+  !                          DENVER_STAPLETON_CO_USA Annual Cooling (DB = >MWB) 1%, MaxDB = 32.6°C MWB = 15.5°C
+  !
+  ! Run Period (Weather File): Full Annual Simulation, DENVER_STAPLETON_CO_USA_WMO_724690
+  !
+  ! Run Control:             No zone or system sizing, design day run control (no weather file simulation)
+  !
+  ! Building: Fictional 1 zone building with resistive walls.
+  !
+  !           The building is oriented due north.
+  !
+  ! Floor Area:        232.25 m2
+  ! Number of Stories: 1
+  !
+  ! Zone Description Details:
+  !
+  !       (0,15.24,0)                 (15.24,15.24,0)
+  !              _____________________________
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |                             |
+  !             |_____________________________|
+  !
+  !          (0,0,0)                      (15.24,0,0)
+  !
+  ! Internal gains description:     NA
+  !
+  ! Interzone Surfaces:             None
+  ! Internal Mass:                  None
+  ! People:                         None
+  ! Lights:                         None
+  ! Equipment:                      None
+  ! Windows:                        0
+  ! Detached Shading:               None
+  ! Daylight:                       None
+  ! Natural Ventilation:            None
+  ! Compact Schedules:              NA (Example of non-Compact Schedules)
+  ! Solar Distribution:             MinimalShadowing
+  !
+  ! HVAC:                           NA
+  !
+  ! Zonal Equipment:                NA
+  ! Central Air Handling Equipment: No
+  ! System Equipment Autosize:      No
+  ! Purchased Cooling:              No
+  ! Purchased Heating:              No
+  ! Purchased Chilled Water:        No
+  ! Purchased Hot Water:            No
+  ! Coils:                          None
+  ! Pumps:                          None
+  ! Boilers:                        None
+  ! Chillers:                       None
+  ! Towers:                         None
+  !
+  ! Results:
+  ! Standard Reports:               Variable Dictionary, Surfaces (dxf-wireframe), Meter File
+  ! Timestep or Hourly Variables:   Hourly and Daily
+  ! Time bins Report:               None
+  ! HTML Report:                    None
+  ! Environmental Emissions:        None
+  ! Utility Tariffs:                None
+
+
+    Output:PreprocessorMessage,
+      No Preprocessor Used,    !- Preprocessor Name
+      Information,             !- Error Severity
+      Illustrative Message,    !- Message Line 1
+      No problems for processing;  !- Message Line 2
+
+
+    Version,
+      3.0;                     !- Version Identifier
+
+
+    Timestep,
+      4;                       !- Number of Timesteps per Hour
+
+
+    Building,
+      Simple One Zone (Wireframe DXF),  !- Name
+      0.0000000E+00,           !- North Axis {deg}
+      Suburbs,                 !- Terrain
+      .04,                     !- Loads Convergence Tolerance Value
+      .004,                    !- Temperature Convergence Tolerance Value {deltaC}
+      MinimalShadowing,        !- Solar Distribution
+      30;                      !- Maximum Number of Warmup Days
+
+
+    HeatBalanceAlgorithm,
+      ConductionTransferFunction;  !- Algorithm
+
+
+    SurfaceConvectionAlgorithm:Inside,
+      Detailed;                !- Algorithm
+
+
+    SurfaceConvectionAlgorithm:Outside,
+      Detailed;                !- Algorithm
+
+
+    SimulationControl,
+      No,                      !- Do Zone Sizing Calculation
+      No,                      !- Do System Sizing Calculation
+      No,                      !- Do Plant Sizing Calculation
+      Yes,                     !- Run Simulation for Sizing Periods
+      Yes;                     !- Run Simulation for Weather File Run Periods
+
+
+    RunPeriod,
+      1,                       !- Begin Month
+      1,                       !- Begin Day of Month
+      12,                      !- End Month
+      31,                      !- End Day of Month
+      Tuesday,                 !- Day of Week for Start Day
+      Yes,                     !- Use Weather File Holidays and Special Days
+      Yes,                     !- Use Weather File Daylight Saving Period
+      No,                      !- Apply Weekend Holiday Rule
+      Yes,                     !- Use Weather File Rain Indicators
+      Yes;                     !- Use Weather File Snow Indicators
+
+
+    Site:Location,
+      DENVER_STAPLETON_CO_USA_WMO_724690,  !- Name
+      39.77,                   !- Latitude {deg}
+      -104.87,                 !- Longitude {deg}
+      -7.00,                   !- Time Zone {hr}
+      1611.00;                 !- Elevation {m}
+
+
+   !  WMO = 724690 Time Zone = NAM        (GMT-07:00) Mountain Time (US & Canada)
+   !  Data Source = ASHRAE 2005 Annual Design Conditions
+   ! Using Design Conditions from "Climate Design Data 2005 ASHRAE Handbook"
+   ! DENVER_STAPLETON_CO_USA Extreme Annual Wind Speeds, 1% = 10.9m/s, 2.5% = 8.8m/s, 5% = 7.7m/s
+   ! DENVER_STAPLETON_CO_USA Extreme Annual Temperatures, Max Drybulb = 37.2°C Min Drybulb = -24.6°C
+   ! DENVER_STAPLETON_CO_USA Annual Heating Design Conditions Wind Speed = 2.3m/s Wind Dir = 180
+   ! Coldest Month = December
+   ! DENVER_STAPLETON_CO_USA Annual Heating 99%, MaxDB = -16°C
+
+
+    SizingPeriod:DesignDay,
+      DENVER_STAPLETON Ann Htg 99% Condns DB,  !- Name
+      -16,                     !- Maximum Dry-Bulb Temperature {C}
+      0.0,                     !- Daily Temperature Range {deltaC}
+      -16,                     !- Humidity Indicating Conditions at Maximum Dry-Bulb
+      83411.,                  !- Barometric Pressure {Pa}
+      2.3,                     !- Wind Speed {m/s}
+      180,                     !- Wind Direction {deg}
+      0.00,                    !- Sky Clearness
+      0,                       !- Rain Indicator
+      0,                       !- Snow Indicator
+      21,                      !- Day of Month
+      12,                      !- Month
+      WinterDesignDay,         !- Day Type
+      0,                       !- Daylight Saving Time Indicator
+      WetBulb;                 !- Humidity Indicating Type
+
+
+   ! DENVER_STAPLETON Annual Cooling Design Conditions Wind Speed = 4m/s Wind Dir = 120
+   ! Hottest Month = July
+   ! DENVER_STAPLETON_CO_USA Annual Cooling (DB = >MWB) 1%, MaxDB = 32.6°C MWB = 15.5°C
+
+
+    SizingPeriod:DesignDay,
+      DENVER_STAPLETON Ann Clg 1% Condns DB = >MWB,  !- Name
+      32.6,                    !- Maximum Dry-Bulb Temperature {C}
+      15.2,                    !- Daily Temperature Range {deltaC}
+      15.5,                    !- Humidity Indicating Conditions at Maximum Dry-Bulb
+      83411.,                  !- Barometric Pressure {Pa}
+      4,                       !- Wind Speed {m/s}
+      120,                     !- Wind Direction {deg}
+      1.00,                    !- Sky Clearness
+      0,                       !- Rain Indicator
+      0,                       !- Snow Indicator
+      21,                      !- Day of Month
+      7,                       !- Month
+      SummerDesignDay,         !- Day Type
+      0,                       !- Daylight Saving Time Indicator
+      WetBulb;                 !- Humidity Indicating Type
+
+
+    Material:NoMass,
+      R13LAYER,                !- Name
+      Rough,                   !- Roughness
+      2.290965,                !- Thermal Resistance {m2-K/W}
+      0.9000000,               !- Thermal Absorptance
+      0.7500000,               !- Solar Absorptance
+      0.7500000;               !- Visible Absorptance
+
+
+    Material:NoMass,
+      R31LAYER,                !- Name
+      Rough,                   !- Roughness
+      5.456,                   !- Thermal Resistance {m2-K/W}
+      0.9000000,               !- Thermal Absorptance
+      0.7500000,               !- Solar Absorptance
+      0.7500000;               !- Visible Absorptance
+
+
+    Material,
+      C5 - 4 IN HW CONCRETE,   !- Name
+      MediumRough,             !- Roughness
+      0.1014984,               !- Thickness {m}
+      1.729577,                !- Conductivity {W/m-K}
+      2242.585,                !- Density {kg/m3}
+      836.8000,                !- Specific Heat {J/kg-K}
+      0.9000000,               !- Thermal Absorptance
+      0.6500000,               !- Solar Absorptance
+      0.6500000;               !- Visible Absorptance
+
+
+    Construction,
+      R13WALL,                 !- Name
+      R13LAYER;                !- Outside Layer
+
+
+    Construction,
+      FLOOR,                   !- Name
+      C5 - 4 IN HW CONCRETE;   !- Outside Layer
+
+
+    Construction,
+      ROOF31,                  !- Name
+      R31LAYER;                !- Outside Layer
+
+
+    Site:GroundTemperature:BuildingSurface,
+      18.89,                   !- January Ground Temperature {C}
+      18.92,                   !- February Ground Temperature {C}
+      19.02,                   !- March Ground Temperature {C}
+      19.12,                   !- April Ground Temperature {C}
+      19.21,                   !- May Ground Temperature {C}
+      19.23,                   !- June Ground Temperature {C}
+      19.07,                   !- July Ground Temperature {C}
+      19.32,                   !- August Ground Temperature {C}
+      19.09,                   !- September Ground Temperature {C}
+      19.21,                   !- October Ground Temperature {C}
+      19.13,                   !- November Ground Temperature {C}
+      18.96;                   !- December Ground Temperature {C}
+
+
+    Zone,
+      ZONE ONE,                !- Name
+      0.0000000E+00,           !- Direction of Relative North {deg}
+      0.0000000E+00,           !- X Origin {m}
+      0.0000000E+00,           !- Y Origin {m}
+      0.0000000E+00,           !- Z Origin {m}
+      1,                       !- Type
+      1,                       !- Multiplier
+      autocalculate,           !- Ceiling Height {m}
+      autocalculate;           !- Volume {m3}
+
+
+    ScheduleTypeLimits,
+      Fraction,                !- Name
+      0.0 : 1.0,               !- Range
+      CONTINUOUS;              !- Numeric Type
+
+
+    GlobalGeometryRules,
+      UpperLeftCorner,         !- Starting Vertex Position
+      CounterClockWise,        !- Vertex Entry Direction
+      WorldCoordinateSystem;   !- Coordinate System
+
+
+    BuildingSurface:Detailed,
+      Zn001:Wall001,           !- Name
+      Wall,                    !- Surface Type
+      R13WALL,                 !- Construction Name
+      ZONE ONE,                !- Zone Name
+      Outdoors,                !- Outside Boundary Condition
+      ,                        !- Outside Boundary Condition Object
+      SunExposed,              !- Sun Exposure
+      WindExposed,             !- Wind Exposure
+      0.5000000,               !- View Factor to Ground
+      4,                       !- Number of Vertices
+      0.0000000E+00,0.0000000E+00,4.572000,  !- X,Y,Z = = > Vertex 1
+      0.0000000E+00,0.0000000E+00,0.0000000E+00,  !- X,Y,Z = = > Vertex 2
+      15.24000,0.0000000E+00,0.0000000E+00,  !- X,Y,Z = = > Vertex 3
+      15.24000,0.0000000E+00,4.572000;  !- X,Y,Z = = > Vertex 4
+
+
+    BuildingSurface:Detailed,
+      Zn001:Wall002,           !- Name
+      Wall,                    !- Surface Type
+      R13WALL,                 !- Construction Name
+      ZONE ONE,                !- Zone Name
+      Outdoors,                !- Outside Boundary Condition
+      ,                        !- Outside Boundary Condition Object
+      SunExposed,              !- Sun Exposure
+      WindExposed,             !- Wind Exposure
+      0.5000000,               !- View Factor to Ground
+      4,                       !- Number of Vertices
+      15.24000,0.0000000E+00,4.572000,  !- X,Y,Z = = > Vertex 1
+      15.24000,0.0000000E+00,0.0000000E+00,  !- X,Y,Z = = > Vertex 2
+      15.24000,15.24000,0.0000000E+00,  !- X,Y,Z = = > Vertex 3
+      15.24000,15.24000,4.572000;  !- X,Y,Z = = > Vertex 4
+
+
+    BuildingSurface:Detailed,
+      Zn001:Wall003,           !- Name
+      Wall,                    !- Surface Type
+      R13WALL,                 !- Construction Name
+      ZONE ONE,                !- Zone Name
+      Outdoors,                !- Outside Boundary Condition
+      ,                        !- Outside Boundary Condition Object
+      SunExposed,              !- Sun Exposure
+      WindExposed,             !- Wind Exposure
+      0.5000000,               !- View Factor to Ground
+      4,                       !- Number of Vertices
+      15.24000,15.24000,4.572000,  !- X,Y,Z = = > Vertex 1
+      15.24000,15.24000,0.0000000E+00,  !- X,Y,Z = = > Vertex 2
+      0.0000000E+00,15.24000,0.0000000E+00,  !- X,Y,Z = = > Vertex 3
+      0.0000000E+00,15.24000,4.572000;  !- X,Y,Z = = > Vertex 4
+
+
+    BuildingSurface:Detailed,
+      Zn001:Wall004,           !- Name
+      Wall,                    !- Surface Type
+      R13WALL,                 !- Construction Name
+      ZONE ONE,                !- Zone Name
+      Outdoors,                !- Outside Boundary Condition
+      ,                        !- Outside Boundary Condition Object
+      SunExposed,              !- Sun Exposure
+      WindExposed,             !- Wind Exposure
+      0.5000000,               !- View Factor to Ground
+      4,                       !- Number of Vertices
+      0.0000000E+00,15.24000,4.572000,  !- X,Y,Z = = > Vertex 1
+      0.0000000E+00,15.24000,0.0000000E+00,  !- X,Y,Z = = > Vertex 2
+      0.0000000E+00,0.0000000E+00,0.0000000E+00,  !- X,Y,Z = = > Vertex 3
+      0.0000000E+00,0.0000000E+00,4.572000;  !- X,Y,Z = = > Vertex 4
+
+
+    BuildingSurface:Detailed,
+      Zn001:Flr001,            !- Name
+      Floor,                   !- Surface Type
+      FLOOR,                   !- Construction Name
+      ZONE ONE,                !- Zone Name
+      Surface,                 !- Outside Boundary Condition
+      Zn001:Flr001,            !- Outside Boundary Condition Object
+      NoSun,                   !- Sun Exposure
+      NoWind,                  !- Wind Exposure
+      1.000000,                !- View Factor to Ground
+      4,                       !- Number of Vertices
+      15.24000,0.000000,0.0,  !- X,Y,Z = = > Vertex 1
+      0.000000,0.000000,0.0,  !- X,Y,Z = = > Vertex 2
+      0.000000,15.24000,0.0,  !- X,Y,Z = = > Vertex 3
+      15.24000,15.24000,0.0;  !- X,Y,Z = = > Vertex 4
+
+
+    BuildingSurface:Detailed,
+      Zn001:Roof001,           !- Name
+      Roof,                    !- Surface Type
+      ROOF31,                  !- Construction Name
+      ZONE ONE,                !- Zone Name
+      Outdoors,                !- Outside Boundary Condition
+      ,                        !- Outside Boundary Condition Object
+      SunExposed,              !- Sun Exposure
+      WindExposed,             !- Wind Exposure
+      0.0000000E+00,           !- View Factor to Ground
+      4,                       !- Number of Vertices
+      0.000000,15.24000,4.572,  !- X,Y,Z = = > Vertex 1
+      0.000000,0.000000,4.572,  !- X,Y,Z = = > Vertex 2
+      15.24000,0.000000,4.572,  !- X,Y,Z = = > Vertex 3
+      15.24000,15.24000,4.572;  !- X,Y,Z = = > Vertex 4
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      outdoor dry bulb,        !- Variable Name
+      hourly;                  !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      Daylight Saving Time Indicator,  !- Variable Name
+      daily;                   !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      DayType Index,           !- Variable Name
+      daily;                   !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      Zone Mean Air Temperature,  !- Variable Name
+      hourly;                  !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      Zone Total Internal Latent Gain,  !- Variable Name
+      hourly;                  !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      Zone Mean Radiant Temperature,  !- Variable Name
+      hourly;                  !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      Zone Air Balance Surface Convection Rate,  !- Variable Name
+      hourly;                  !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      Zone Air Balance Air Energy Storage Rate,  !- Variable Name
+      hourly;                  !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      Surface Inside Temperature,  !- Variable Name
+      daily;                   !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      Surface Outside Temperature,  !- Variable Name
+      daily;                   !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      Surface Int Convection Coeff,  !- Variable Name
+      daily;                   !- Reporting Frequency
+
+
+    Output:Variable,
+      *,                       !- Key Value
+      Surface Ext Convection Coeff,  !- Variable Name
+      daily;                   !- Reporting Frequency
+
+
+    Output:Reports,
+      VariableDictionary,      !- Type of Report
+      IDF;                     !- Report Name
+
+
+    Output:Reports,
+      surfaces,                !- Type of Report
+      dxf:wireframe;           !- Report Name
+
+
+    Output:Reports,
+      construction;            !- Type of Report
+
+
+    Output:Meter:MeterFileOnly,
+      ExteriorLights:Electricity,  !- Name
+      hourly;                  !- Reporting Frequency
+
+
+    Output:Meter:MeterFileOnly,
+      Carbon Equivalent:Facility,  !- Name
+      hourly;                  !- Reporting Frequency
+
+
+    Output:Meter:MeterFileOnly,
+      EnergyTransfer:Building, !- Name
+      hourly;                  !- Reporting Frequency
+
+
+    Output:Meter:MeterFileOnly,
+      EnergyTransfer:Facility, !- Name
+      hourly;                  !- Reporting Frequency
+
+
+    OutputControl:Table:Style,
+      HTML;                    !- Column Separator
+
+
+    Output:Table:SummaryReports,
+      AllSummary;              !- Report 1 Name
+
+
+    Exterior:Lights,
+      ExtLights,               !- Name
+      AlwaysOn,                !- Schedule Name
+      5250,                    !- Design Level {W}
+      AstronomicalClock,       !- Control Option
+      Grounds Lights;          !- End-Use Subcategory
+
+
+    ScheduleTypeLimits,
+      On/Off,                  !- Name
+      0:1,                     !- Range
+      DISCRETE;                !- Numeric Type
+
+
+    Schedule:Day:Hourly,
+      On,                      !- Name
+      On/Off,                  !- Schedule Type Limits Name
+      1.,                      !- Hour 1
+      1.,                      !- Hour 2
+      1.,                      !- Hour 3
+      1.,                      !- Hour 4
+      1.,                      !- Hour 5
+      1.,                      !- Hour 6
+      1.,                      !- Hour 7
+      1.,                      !- Hour 8
+      1.,                      !- Hour 9
+      1.,                      !- Hour 10
+      1.,                      !- Hour 11
+      1.,                      !- Hour 12
+      1.,                      !- Hour 13
+      1.,                      !- Hour 14
+      1.,                      !- Hour 15
+      1.,                      !- Hour 16
+      1.,                      !- Hour 17
+      1.,                      !- Hour 18
+      1.,                      !- Hour 19
+      1.,                      !- Hour 20
+      1.,                      !- Hour 21
+      1.,                      !- Hour 22
+      1.,                      !- Hour 23
+      1.;                      !- Hour 24
+
+
+    Schedule:Week:Daily,
+      On Weeks,                !- Name
+      On,                      !- Sunday Schedule:Day Name
+      On,                      !- Monday Schedule:Day Name
+      On,                      !- Tuesday Schedule:Day Name
+      On,                      !- Wednesday Schedule:Day Name
+      On,                      !- Thursday Schedule:Day Name
+      On,                      !- Friday Schedule:Day Name
+      On,                      !- Saturday Schedule:Day Name
+      On,                      !- Holiday Schedule:Day Name
+      On,                      !- SummerDesignDay Schedule:Day Name
+      On,                      !- WinterDesignDay Schedule:Day Name
+      On,                      !- CustomDay1 Schedule:Day Name
+      On;                      !- CustomDay2 Schedule:Day Name
+
+
+    Schedule:Year,
+      AlwaysOn,                !- Name
+      On/Off,                  !- Schedule Type Limits Name
+      On Weeks,                !- Schedule:Week Name 1
+      1,                       !- Start Month 1
+      1,                       !- Start Day 1
+      12,                      !- End Month 1
+      31;                      !- End Day 1
+\end{lstlisting}
diff --git a/doc/interface-developer/src/energyplus-install-contents.tex b/doc/interface-developer/src/energyplus-install-contents.tex
new file mode 100644
index 00000000000..2be5d1a6fd1
--- /dev/null
+++ b/doc/interface-developer/src/energyplus-install-contents.tex
@@ -0,0 +1,23 @@
+\chapter{EnergyPlus Install Contents}\label{energyplus-install-contents}
+
+EnergyPlus Interfaces will naturally need to access the installed EnergyPlus programs, library files, documentation.~ It will help to describe how EnergyPlus is installed (on a Windowsâ„¢ computer).~ The EnergyPlus install is written using the WISEâ„¢ installation software.
+
+The scheme of installing EnergyPlus includes a ``root'' directory/folder and all subsequent programs installed as part of the installation are child folders under the parent/root folder.~ Several optional components can be selected during install.
+
+The basic (required) installation has crucial files installed in the parent folder -- these include \textbf{EnergyPlus.exe}, \textbf{Energy+.idd} (the input data dictionary), \textbf{EPMacro.exe}.~ The basic installation also includes a child folder ``DataSets'' that contains the EnergyPlus ``libraries''.~ As distributed, EnergyPlus includes several library files, formatted in the standard EnergyPlus IDF format.~ These include thermal material properties, moisture material properties, glass and other properties for windows, constructions (material sandwiches which describe walls, windows, roofs), fluid properties, locations, design day definitions, and basic schedule definitions.~ There, of course, may be additional data sets added as well as future datasets edited for selectable use from the EPMacro program.~ The Templates folder is also included in the basic install.~ Currently, the Templates folder contains documentation and the HVAC Template files.~ These files can be used somewhat ``automatically'' to produce HVAC loop structures for running with EnergyPlus.
+
+Optional components of the EnergyPlus install: \textbf{Documentation}, \textbf{EP-Launch}, \textbf{IDFEditor}, \textbf{Sample} \textbf{Files}, \textbf{Weather} \textbf{Converter}, and other auxiliary type programs.~ All the components are selected by default; to not install them the user must ``un-select'' them individually.~ Highlights of several:
+
+\textbf{Documentation:}~ The EnergyPlus package includes a comprehensive set of documents intended to help the user and others understand the EnergyPlus program, usage, and other appropriate information.~ All documents are created in PDF (Portable Document Format).~ There is ``index'' to all documents to make searching for a subject easier.~A shortcut to the Documentation folder and the ``main-menu'' document is included.~ The main-menu document is a navigation aid to the remainder of the documents.~ We may want to make the documentation a non-optional component.
+
+\textbf{EP-Launch:~} The components of EP-Launch are installed in the parent directory (help files installed in the documentation directory).~ Because the basic EnergyPlus program runs as a console application, many beta users did not understand how to make the program execute.~ While the developers may be able to tailor the EnergyPlus executable to be more callable under the Windowsâ„¢ platform, this is still a useful program.~ EP-Launch uses the EPL-Run.bat file and prepends several ``set'' commands that are used in the bat file.~ It creates the actual batch file for the run as ``RunEP.bat'' and then calls the operating system to execute the file.~~ Having the EPL-Run.bat file as external to the EP-Launch program means that others may tailor the batch file more appropriately to how things are run though this may not be preserved with a future EnergyPlus install. EP-Launch can also execute several utility programs from the ``Utilities'' tab.
+
+\textbf{IDFEditor:~} The IDFEditor is the simple editor that is distributed with EnergyPlus.~ As an interface, it is crude.~ However, it gets the job done.~ It uses the IDD and then reads and/or creates an IDF file.~ The objects are shown in the groups (see \textbackslash{}group discussion below) and, when an existing file is used, will display how many of an object is found in the IDF.~ This program is installed in the Parent \textbackslash{} PreProcess \textbackslash{} IDFEditor folder.
+
+\textbf{Sample Files:}~ The sample files include several IDF files along with the files the installed version of EnergyPlus created using these files.~ There are several possible child folders here, including the Misc child folder that will contain all the development sample files -- but without having been run for the install.~ These files are installed in the Parent \textbackslash{} ExampleFiles folder and any appropriate child folders under that.
+
+\textbf{Weather Converter:}~ The WeatherConverter program can process raw weather data in several formats into the EnergyPlus weather data format (epw).~ In addition, the WeatherConverter program can be used to generate a simple report of the weather data as well as produce a .csv file of the format.~ The .csv (comma separated variable) format can easily be imported into spread sheet programs or other tables.~ This program is installed in the Parent \textbackslash{} PreProcess \textbackslash{} WeatherConverter folder.~ The WeatherConverter also has a DLL file which could be used directly by an external interface.
+
+\textbf{BLAST Translator:~} The BLAST translator program can be used to convert a BLAST input file into a format that can be executed from EnergyPlus.~ Extensive system translation is not done with this program -- mostly geometry and other space gain elements as well as zone oriented (i.e.~People) schedules.~ If the BLAST input file contains thermostatic controls in the zones, then the EnergyPlus IDF file will include a purchased-air solution of that BLAST input file.~ This program is no longer part of the EnergyPlus install but is available with each new release.
+
+\textbf{DOE-2 Translator:}~ The DOE-2 translator program is similar to the BLAST Translator program but for DOE-2 files.~ DOE-2 translator output must be processed by the EPMacro program prior to running in EnergyPlus (the EP-Launch program/EPL-Run procedure does this automatically for all ``.imf'' files).~ This program is no longer part of the EnergyPlus install but is available with each new release.
diff --git a/doc/interface-developer/src/guide-for-interface-developers.tex b/doc/interface-developer/src/guide-for-interface-developers.tex
new file mode 100644
index 00000000000..63f37402bb8
--- /dev/null
+++ b/doc/interface-developer/src/guide-for-interface-developers.tex
@@ -0,0 +1 @@
+\input{../title}
diff --git a/doc/interface-developer/src/input-details.tex b/doc/interface-developer/src/input-details.tex
new file mode 100644
index 00000000000..eee719330a0
--- /dev/null
+++ b/doc/interface-developer/src/input-details.tex
@@ -0,0 +1,7 @@
+\chapter{Input Details}\label{input-details}
+
+This document does not cover the input ``classes'' in detail.~ For details on each class and examples of both input and output resulting from that class/object, please view the \href{file:///E:/Docs4PDFs/InputOutputReference.pdf}{Input Output Reference} document.~ In this document, we will show the ``conventions'' used in the IDD and provide limited examples for illustration purposes. Even the list of objects is dynamic, so we give you a method to see them from the IDFEditor.
+
+An intelligent editor (IDFEditor) has been written and can be used as an illustration of how the comments in the IDD might be used by Interface Developers to guide their developments.~ IDFEditor is described in the \href{file:///E:/Docs4PDFs/GettingStarted.pdf}{Getting Started} document.
+
+A full example of a very simple IDF is included in Appendix A to this document.
diff --git a/doc/interface-developer/src/input-details/energyplus-reports.tex b/doc/interface-developer/src/input-details/energyplus-reports.tex
new file mode 100644
index 00000000000..8c5ef18d16c
--- /dev/null
+++ b/doc/interface-developer/src/input-details/energyplus-reports.tex
@@ -0,0 +1,3 @@
+\section{EnergyPlus Reports}\label{energyplus-reports}
+
+Several items are used to specify what will appear in the output file(s).~ The output is described in the next section of this document.~ What appears here is a sample of outputs -- more detailed and complete versions can be found in the ``Output Details and Examples'' document. In addition to the individual reports, there are sets of predefined reports that can appear.~ View the Input for Output section and the Tabular reports section in the Input Output Reference document for more details.
diff --git a/doc/interface-developer/src/input-details/idd-conventions.tex b/doc/interface-developer/src/input-details/idd-conventions.tex
new file mode 100644
index 00000000000..00e8d83ed25
--- /dev/null
+++ b/doc/interface-developer/src/input-details/idd-conventions.tex
@@ -0,0 +1,480 @@
+\section{IDD Conventions}\label{idd-conventions}
+
+The following is a basic description of the structure of the IDD (it's actually taken directly from the IDD file). As noted within, \textbf{!} signifies a comment character as does the \textbf{\textbackslash{}}. \textbf{\textbackslash{}} has also been adopted as a convention for including more specific comments about each field in an object. These have been used with success in the IDFEditor and it is hoped the flexibility will provide other interface developers with useful information.
+
+\begin{lstlisting}
+!IDD_Version VERSION NUMBER
+! **************************************************************************
+! This file is the Input Data Dictionary (IDD) for EnergyPlus.
+! The IDD defines the syntax and data model for each type of input "Object."
+! Lines in EnergyPlus input files (and IDD) are limited to 500 characters.
+!
+! Object Description
+! ------------------
+! To define an object (a record with data), develop a key word that is unique
+! Each data item to the object can be A (Alphanumeric string) or N (numeric)
+! Number each A and N.  This will show how the data items will be put into the
+! arrays that are passed to the Input Processor "Get" (GetObjectItem) routines.
+! All alpha fields are limited to 100 characters.  Numeric fields should be
+! valid numerics (can include such as 1.0E+05) and are placed into double
+! precision variables.
+!
+! NOTE: Even though a field may be optional, a comma representing that field
+!   must be included (unless it is the last field in the object).  Since the
+!   entire input is "field-oriented" and not "keyword-oriented", the EnergyPlus
+!   Input Processor must have some representation (even if blank) for each
+!   field.
+!
+! Object Documentation
+! --------------------
+! In addition, the following special comments appear one per line and
+! most are followed by a value.  Comments may apply to a field or the object
+! or a group of objects.
+!
+! Field-level comments:
+!
+!  \field           Name of field
+!                     (should be succinct and readable, blanks are encouraged)
+!
+!  \note            Note describing the field and its valid values. If multiple lines,
+!                   start each line with \note. Limit line length to 100 characters.
+!
+!  \required-field  To flag fields which may not be left blank
+!                     (this comment has no "value")
+!
+!  \begin-extensible  Marks the first field at which the object accepts an extensible
+!                   field set.  A fixed number of fields from this marker define the
+!                   extensible field set, see the object code \extensible for
+!                   more information.
+!
+!  \units           Units (must be from EnergyPlus standard units list)
+!                   EnergyPlus units are standard SI units
+!
+!  \ip-units        IP-Units (for use by input processors with IP units)
+!                   This is only used if the default conversion is not
+!                   appropriate.
+!
+!  \unitsBasedOnField  For fields that may have multiple possible units, indicates
+!                   the field in the object that can be used to determine
+!                   the units. The field reference is in the A2 form.
+!
+!  \minimum         Minimum that includes the following value
+!
+!  \minimum>        Minimum that must be > than the following value
+!
+!  \maximum         Maximum that includes the following value
+!
+!  \maximum<        Maximum that must be < than the following value
+!
+!  \default         Default for the field (if N/A then omit entire line)
+!
+!  \deprecated      This field is not really used and will be deleted from the object.
+!                   The required information is gotten internally or
+!                   not needed by the program.
+!
+!  \autosizable     Flag to indicate that this field can be used with the Auto
+!                   Sizing routines to produce calculated results for the
+!                   field.  If a value follows this, then that will be used
+!                   when the "Autosize" feature is flagged.  To trigger
+!                   autosizing for a field, enter Autosize as the field's
+!                   value.  Only applicable to numeric fields.
+!
+!  \autocalculatable Flag to indicate that this field can be automatically
+!                   calculated. To trigger auto calculation for a field, enter
+!                   Autocalculate as the field's value.  Only applicable to
+!                   numeric fields.
+!
+!  \type            Type of data for the field -
+!                     integer
+!                     real
+!                     alpha       (arbitrary string),
+!                     choice      (alpha with specific list of choices, see
+!                                 \key)
+!                     object-list (link to a list of objects defined elsewhere,
+!                                  see \object-list and \reference)
+!                     external-list (uses a special list from an external source,
+!                                    see \external-list)
+!                     node        (name used in connecting HVAC components)
+!
+!  \retaincase      Retains the alphabetic case for alpha type fields
+!
+!  \key             Possible value for "\type choice" (blanks are significant)
+!                     use multiple \key lines to indicate all valid choices
+!
+!  \object-list     Name of a list of user-provided object names that are valid
+!                     entries for this field (used with "\reference")
+!                     see Zone and BuildingSurface:Detailed objects below for
+!                     examples.
+!                  ** Note that a field may have multiple \object-list commands.
+!
+!  \external-list   The values for this field should be selected from a special
+!                   list generated outside of the IDD file. The choices for the
+!                   special lists are:
+!                        autoRDDvariable
+!                        autoRDDmeter
+!                        autoRDDvariableMeter
+!                   When one of these are selected the options for the field
+!                   are taken from the RDD or MDD file or both.
+!
+!  \reference       Name of a list of names to which this object belongs
+!                     used with "\type object-list" and with "\object-list"
+!                     see Zone and BuildingSurface:Detailed objects below for
+!                     examples:
+!
+!                        Zone,
+!                          A1 , \field Name
+!                               \type alpha
+!                               \reference ZoneNames
+!
+!                        BuildingSurface:Detailed,
+!                          A4 , \field Zone Name
+!                               \note Zone the surface is a part of
+!                               \type object-list
+!                               \object-list ZoneNames
+!
+!             For each zone, the field "Name" may be referenced
+!             by other objects, such as BuildingSurface:Detailed, so it is
+!             commented with "\reference ZoneNames"
+!             Fields that reference a zone name, such as BuildingSurface:Detailed's
+!             "Zone Name", are commented as
+!             "\type object-list" and "\object-list ZoneNames"
+!             ** Note that a field may have multiple \reference commands.
+!             ** This is useful if the object belongs to a small specific
+!             object-list as well as a larger more general object-list.
+!
+! Object-level comments:
+!
+!  \memo            Memo describing the object. If multiple lines, start each line
+!                   with \memo.
+!                   Limit line length to 100 characters.
+!
+!  \unique-object   To flag objects which should appear only once in an idf
+!                     (this comment has no "value")
+!
+!  \required-object To flag objects which are required in every idf
+!                     (this comment has no "value")
+!
+!  \min-fields      Minimum number of fields that should be included in the
+!                   object.  If appropriate, the Input Processor will fill
+!                   any missing fields with defaults (for numeric fields).
+!                   It will also supply that number of fields to the "get"
+!                   routines using blanks for alpha fields (note -- blanks
+!                   may not be allowable for some alpha fields).
+!
+!  \obsolete        This object has been replaced though is kept (and is read)
+!                   in the current version.  Please refer to documentation as
+!                   to the dispersal of the object.  If this object is
+!                   encountered in an IDF, the InputProcessor will post an
+!                   appropriate message to the error file.
+!                   usage:  \obsolete New = >[New object name]
+!
+!  \extensible:<\#>  This object is dynamically extensible -- meaning, if you
+!           change the IDD appropriately (if the object has a simple list
+!           structure -- just add items to the list arguments (i.e. BRANCH
+!           LIST). These will be automatically redimensioned and used during
+!           the simulation. <\#> should be entered by the developer to signify
+!           how many of the last fields are needed to be extended (and EnergyPlus
+!           will attempt to auto-extend the object).  The first field of the first
+!           instance of the extensible field set is marked with \begin-extensible.
+!
+!  \begin-extensible See previous item, marks beginning of extensible fields in
+!                   an object.
+!
+!  \format          The object should have a special format when saved in
+!                   the IDF Editor with the special format option enabled.
+!                   The options include SingleLine, Vertices, CompactSchedule,
+!                   FluidProperties, ViewFactors, and Spectral.
+!                   The SingleLine option puts all the fields for the object
+!                   on a single line. The Vertices option is used in objects
+!                   that use X, Y and Z fields to format those three fields
+!                   on a single line.
+!                   The CompactSchedule formats that specific object.
+!                   The FluidProperty option formats long lists of fluid
+!                   properties to ten values per line.
+!                   The ViewFactor option formats three fields related to
+!                   view factors per line.
+!                   The Spectral option formats the four fields related to
+!                   window glass spectral data per line.
+!
+!   \reference-class-name Adds the name of the class to the reference list
+!                   similar to \reference.
+!
+! Group-level comments:
+!
+!  \group          Name for a group of related objects
+!
+!
+! Notes on comments
+! -----------------
+!
+! 1.  If a particular comment is not applicable (such as units, or default)
+! then simply omit the comment rather than indicating N/A.
+!
+! 2.  Memos and notes should be brief (recommend 5 lines or less per block).
+! More extensive explanations are expected to be in the user documentation
+\end{lstlisting}
+
+\subsection{IDD -- IP Units}\label{idd-ip-units}
+
+In addition, the IDD contains indications of IP (inch-pound) units for the EnergyPlus standard SI (Systems International) units. These may be used by input and output interfaces to display values in the IP system. As noted, if the IP units are ``standard'' (first block below), then no \textbackslash{}ip-units is expected in the field. Note that for some fields -- due to their multiple use (for example, schedule values) -- there cannot be a ip-unit designation.
+
+\begin{lstlisting}
+
+! Default IP conversions (no \ip-units necessary)
+  !      $/(m3/s)               = >   $/(ft3/min)         0.000472000059660808
+  !      $/(W/K)                = >   $/(Btu/h-F)         0.52667614683731
+  !      $/kW                   = >   $/(kBtuh/h)         0.293083235638921
+  !      $/m2                   = >   $/ft2               0.0928939733269818
+  !      $/m3                   = >   $/ft3               0.0283127014102352
+  !      (kg/s)/W               = >   (lbm/sec)/(Btu/hr)  0.646078115385742
+  !      1/K                    = >   1/F                 0.555555555555556
+  !      1/m                    = >   1/ft                0.3048
+  !      A/K                     = >   A/F                 0.555555555555556
+  !      C                      = >   F                   1.8 (plus 32)
+  !      cm                     = >   in                  0.3937
+  !      cm2                    = >   inch2               0.15500031000062
+  !      deltaC                 = >   deltaF              1.8
+  !      deltaJ/kg              = >   deltaBtu/lb         0.0004299
+  !      g/GJ                   = >   lb/MWh              0.00793664091373665
+  !      g/kg                   = >   grains/lb           7
+  !      g/MJ                   = >   lb/MWh              7.93664091373665
+  !      g/mol                  = >   lb/mol              0.0022046
+  !      g/m-s                  = >   lb/ft-s             0.000671968949659
+  !      g/m-s-K                = >   lb/ft-s-F           0.000373574867724868
+  !      GJ                     = >   ton-hrs             78.9889415481832
+  !      J                      = >   Wh                  0.000277777777777778
+  !      J/K                    = >   Btu/F               526.565
+  !      J/kg                   = >   Btu/lb              0.00042986
+  !      J/kg-K                 = >   Btu/lb-F            0.000239005736137667
+  !      J/kg-K2                = >   Btu/lb-F2           0.000132889924714692
+  !      J/kg-K3                = >   Btu/lb-F3           7.38277359526066E-05
+  !      J/m2-K                 = >   Btu/ft2-F           4.89224766847393E-05
+  !      J/m3                   = >   Btu/ft3             2.68096514745308E-05
+  !      J/m3-K                 = >   Btu/ft3-F           1.49237004739337E-05
+  !      K                      = >   R                   1.8
+  !      K/m                    = >   F/ft                0.54861322767449
+  !      kg                     = >   lb                  2.2046
+  !      kg/J                   = >   lb/Btu              2325.83774250441
+  !      kg/kg-K                = >   lb/lb-F             0.555555555555556
+  !      kg/m                   = >   lb/ft               0.67196893069637
+  !      kg/m2                  = >   lb/ft2              0.204794053596664
+  !      kg/m3                   = >   lb/ft3              0.062428
+  !      kg/m-s                 = >   lb/ft-s             0.67196893069637
+  !      kg/m-s-K               = >   lb/ft-s-F           0.373316072609094
+  !      kg/m-s-K2              = >   lb/ft-s-F2          0.207397818116164
+  !      kg/Pa-s-m2             = >   lb/psi-s-ft2        1412.00523459398
+  !      kg/s                   = >   lb/s                2.20462247603796
+  !      kg/s2                  = >   lb/s2               2.2046
+  !      kg/s-m                 = >   lb/s-ft             0.67196893069637
+  !      kJ/kg                  = >   Btu/lb              0.429925
+  !      kPa                    = >   psi                 0.145038
+  !      L/day                  = >   pint/day            2.11337629827348
+  !      L/GJ                   = >   gal/kWh             0.000951022349025202
+  !      L/kWh                  = >   pint/kWh            2.11337629827348
+  !      L/MJ                   = >   gal/kWh             0.951022349025202
+  !      lux                    = >   foot-candles        0.092902267
+  !      m                      = >   ft                  3.28083989501312
+  !      m/hr                   = >   ft/hr               3.28083989501312
+  !      m/s                    = >   ft/min              196.850393700787
+  !      m/s                    = >   miles/hr            2.2369362920544
+  !      m/yr                   = >   inch/yr             39.3700787401575
+  !      m2                     = >   ft2                 10.7639104167097
+  !      m2/m                   = >   ft2/ft              3.28083989501312
+  !      m2/person              = >   ft2/person          10.764961
+  !      m2/s                   = >   ft2/s               10.7639104167097
+  !      m2-K/W                 = >   ft2-F-hr/Btu        5.678263
+  !      m3                     = >   ft3                 35.3146667214886
+  !      m3                     = >   gal                 264.172037284185
+  !      m3/GJ                  = >   ft3/MWh             127.13292
+  !      m3/hr                  = >   ft3/hr              35.3146667214886
+  !      m3/hr-m2               = >   ft3/hr-ft2          3.28083989501312
+  !      m3/hr-person           = >   ft3/hr-person       35.3146667214886
+  !      m3/kg                  = >   ft3/lb              16.018
+  !      m3/m2                  = >   ft3/ft2             3.28083989501312
+  !      m3/MJ                  = >   ft3/kWh             127.13292
+  !      m3/person              = >   ft3/person          35.3146667214886
+  !      m3/s                   = >   ft3/min             2118.88000328931
+  !      m3/s-m                 = >   ft3/min-ft          645.89
+  !      m3/s-m2                = >   ft3/min-ft2         196.85
+  !      m3/s-person            = >   ft3/min-person      2118.6438
+  !      m3/s-W                 = >   (ft3/min)/(Btu/h)   621.099127332943
+  !      N-m                    = >   lbf-in              8.85074900525547
+  !      N-s/m2                 = >   lbf-s/ft2           0.0208857913669065
+  !      Pa                     = >   psi                 0.000145037743897283
+  !      percent/K              = >   percent/F           0.555555555555556
+  !      person/m2              = >   person/ft2          0.0928939733269818
+  !      s/m                    = >   s/ft                0.3048
+  !      V/K                    = >   V/F                 0.555555555555556
+  !      W                      = >   Btu/h               3.4121412858518
+  !      W/(m3/s)               = >   W/(ft3/min)         0.0004719475
+  !      W/K                    = >   Btu/h-F             1.89563404769544
+  !      W/m                    = >   Btu/h-ft            1.04072
+  !      W/m2                   = >   Btu/h-ft2           0.316957210776545
+  !      W/m2                   = >   W/ft2               0.09290304
+  !      W/m2-K                 = >   Btu/h-ft2-F         0.176110194261872
+  !      W/m2-K2                = >   Btu/h-ft2-F2        0.097826
+  !      W/m-K                   = >   Btu-in/h-ft2-F      6.93481276005548
+  !      W/m-K2                 = >   Btu/h-F2-ft         0.321418310071648
+  !      W/m-K3                 = >   Btu/h-F3-ft         0.178565727817582
+  !      W/person               = >   Btu/h-person        3.4121412858518
+  !
+  ! Other conversions supported (needs the \ip-units code)
+  !
+  !      kPa                    = >   inHg                0.29523
+  !      m                      = >   in                  39.3700787401575
+  !      m3/s                   = >   gal/min             15850.3222370511
+  !      Pa                     = >   ftH2O               0.00033455
+  !      Pa                     = >   inH2O               0.00401463
+  !      Pa                     = >   inHg                0.00029613
+  !      Pa                     = >   Pa                  1
+  !      W                      = >   W                   1
+  !      W/m2                   = >   W/m2                1
+  !      W/m-K                  = >   Btu/h-ft-F          0.577796066000163
+  !      W/person               = >   W/person            1
+  !
+  ! Units fields that are not translated
+  !      $
+  !      1/hr
+  !      A
+  !      Ah
+  !      A/V
+  !      Availability
+  !      Control
+  !      cycles/hr
+  !      days
+  !      deg
+  !      dimensionless
+  !      eV
+  !      hr
+  !      J/J
+  !      kg/kg
+  !      kg-H2O/kg-air
+  !      kmol
+  !      kmol/s
+  !      m3/m3
+  !      minutes
+  !      Mode
+  !      ms
+  !      ohms
+  !      percent
+  !      ppm
+  !      rev/min
+  !      s
+  !      V
+  !      VA
+  !      W/m2 or deg C
+  !      W/m2, W or deg C
+  !      W/s
+  !      W/W
+  !      years
+  ! **************************************************************************
+\end{lstlisting}
+
+\subsection{Example Object}\label{example-object}
+
+The Site:Location object will serve as an example.
+
+\begin{lstlisting}
+Site:Location,
+       \unique-object
+       \min-fields 5
+  A1 , \field Name
+       \required-field
+       \type  alpha
+  N1 , \field Latitude
+       \units deg
+       \minimum -90.0
+       \maximum +90.0
+       \default 0.0
+       \note + is North, - is South, degree minutes represented in decimal (i.e. 30 minutes is .5)
+       \type real
+  N2 , \field Longitude
+       \units deg
+       \minimum -180.0
+       \maximum +180.0
+       \default 0.0
+       \note - is West, + is East, degree minutes represented in decimal (i.e. 30 minutes is .5)
+       \type real
+  N3 , \field Time Zone
+       \note basic these limits on the WorldTimeZone Map (2003)
+       \units hr
+       \minimum -12.0
+       \maximum +14.0
+       \default 0.0
+       \note  Time relative to GMT. Decimal hours.
+       \type real
+  N4 ; \field Elevation
+       \units m
+       \minimum -300.0
+       \maximum< 6096.0
+       \default 0.0
+       \type real
+\end{lstlisting}
+
+First, the object name is given.~ (Site:Location)~ This is followed by a comma in both the definition (IDD) and in an input file (IDF).~ In fact, all fields except the terminating field of an IDD class object and IDF object are followed by commas.~ The final field in an IDD class object or in an IDF object is terminated by a semi-colon.
+
+Next is an alpha field, the location name.~ As noted above, for input, spaces are significant in this field.~ The main inputs for Location are numeric fields.~ These are numbered (as is the alpha field) for convenience.~ The \textbackslash{} designations will show various information about the objects as described above in the IDD conventions discussion.~ Of importance for reading this document are the units and possible minimum and maximum values for a~ field.~ Defaults are produced if applicable and if the field is blank in the IDF.~ For this example, that won't work because there is no default AND the Location name is a required field.
+
+The \textbackslash{}minimum, \textbackslash{}maximum and \textbackslash{}default comments are automatically processed in the Inptu Processor for numeric fields.~ Any infractions of the \textbackslash{}minimum, \textbackslash{}maximum fields will be automatically detected and messages will appear in the standard error file.~ After all the input is checked, infractions will cause program termination (before the bulk of the simulation is completed).~ Defaults are also enforced if you leave the numeric field blank.
+
+\textbackslash{}min-fields deserves some explanation.~ This has object level enforcement.~ When min-fields is specified for an object, it has meaning to the InputProcessor -- telling the IP the number of fields that must be returned to a GetInput routine regardless of how many fields may actually appear in the IDF.~ So, min-fields is actually an automatic assistance in most instances.
+
+Some objects need all the parameters listed by the definition; some do not.~ In the descriptions that are contained in the Input Output Reference, we try to indicate which parts are optional.~ Usually, these will be the last fields in the object input or definition.
+
+\subsection{Using the Input-Output Reference Document}\label{using-the-input-output-reference-document}
+
+To assist you in using the \href{file:///E:/Docs4PDFs/InputOutputReference.pdf}{Input Output Reference} document, it is grouped similarly to the IDD file.
+
+To determine the latest set of groups and objects, it will be useful for you to open the IDFEditor (an intelligent editor that is installed with EnergyPlus) and write out the current object list.~ The following figure shows the screen shot of the IDFEditor and the help menu to select the objectlist.~ Select ``\textbf{create objectlist.txt}'' to create the object list -- it will be put into the IDFEditor program folder.
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image002.jpg}
+\caption{Using IDFEditor to find the latest groups and objects for the Energy+.idd \protect \label{fig:using-idfeditor-to-find-the-latest-groups}}
+\end{figure}
+
+The produced list will look something like:
+
+Simulation Parameters
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+{[}------{]}~ Version
+
+{[}------{]}~ SimulationControl
+
+{[}------{]}~ Building
+
+{[}------{]}~ ShadowCalculation
+
+{[}------{]}~ SurfaceConvectionAlgorithm:Inside
+
+{[}------{]}~ SurfaceConvectionAlgorithm:Outside
+
+{[}------{]}~ HeatBalanceAlgorithm
+
+{[}------{]}~ ZoneCapacitanceMultiplier
+
+{[}------{]}~ Timestep
+
+{[}------{]}~ ConvergenceLimits
+
+Location - Climate - Weather File Access
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+{[}------{]}~ Site:Location
+
+{[}------{]}~ SizingPeriod:DesignDay
+
+{[}------{]}~ SizingPeriod:WeatherFileDays
+
+{[}------{]}~ SizingPeriod:WeatherFileConditionType
+
+{[}------{]}~ RunPeriod
+
+{[}------{]}~ RunPeriodControl:SpecialDays
+
+{[}------{]}~ RunPeriodControl:DaylightSavingTime
+
+``Simulation Parameters'' and ``Location -- Climate -- Weather File Access'' are groups. Version, Building, etc are objects.
diff --git a/doc/interface-developer/src/input-details/standard-energyplus-units.tex b/doc/interface-developer/src/input-details/standard-energyplus-units.tex
new file mode 100644
index 00000000000..62f67b3121a
--- /dev/null
+++ b/doc/interface-developer/src/input-details/standard-energyplus-units.tex
@@ -0,0 +1,62 @@
+\section{Standard EnergyPlus Units}\label{standard-energyplus-units}
+
+EnergyPlus expects information in a single unit system (SI).~ This requires interface developers to convert user inputs from those preferred by architects and engineers into the standard metric units of EnergyPlus.~ EnergyPlus will not perform any units conversions and will not have any unit conversion routines.
+
+ASCII with no spaces is used for abbreviations.~ Note that exponents appear without any indication of exponentiation: i.e., kg/m3 not kg/m\^{}3 or kg/m**3.~ Also note the use of dashes.~ We have W/m2-K not W/m2*K or W/(m2*K).
+
+At the end we note the ``problem'' variables -- the inputs that have non-standard units. Inputs using these units will have to be changed and the code checked to see how the quantities are used internally.
+
+% table 1
+\begin{longtable}[c]{p{1.59in}p{2.9in}p{1.5in}}
+\caption{Standard EnergyPlus Units \label{table:standard-energyplus-units}} \tabularnewline
+\toprule 
+Quantity & unit & abbreviation \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Standard EnergyPlus Units} \tabularnewline
+\toprule 
+Quantity & unit & abbreviation \tabularnewline
+\midrule
+\endhead
+
+angular degrees & degree & deg \tabularnewline
+Length & meter & m \tabularnewline
+Area & square meter & m2 \tabularnewline
+Volume & cubic meter & m3 \tabularnewline
+Time & seconds & s \tabularnewline
+Frequency & Hertz & Hz \tabularnewline
+Temperature & Celsius & C \tabularnewline
+absolute temperature & Kelvin & K \tabularnewline
+temperature difference & Kelvin & delK \tabularnewline
+speed & meters per second & m/s \tabularnewline
+energy (or work) & Joules & J \tabularnewline
+power & Watts & W \tabularnewline
+mass & kilograms & kg \tabularnewline
+force & Newton & N \tabularnewline
+mass flow & kilograms per second & kg/s \tabularnewline
+volume flow & cubic meters per second & m3/s \tabularnewline
+pressure & Pascals & Pa \tabularnewline
+pressure difference & Pascals & delPa \tabularnewline
+specific enthalpy & Joules per kilogram & J/kg \tabularnewline
+density & kilograms per cubic meter & kg/m3 \tabularnewline
+heat flux & watts per square meter & W/m2 \tabularnewline
+specific heat & ------------------------------------------------------------------------ & J/kg-K \tabularnewline
+conductivity & ------------------------------------------------------------------------ & W/m-K \tabularnewline
+diffusivity & ------------------------------------------------------------------------ & m2/s \tabularnewline
+heat transfer coefficient & ------------------------------------------------------------------------ & W/m2-K \tabularnewline
+R-value & ------------------------------------------------------------------------ & m2-K/W \tabularnewline
+heating or cooling capacity & Watts & W \tabularnewline
+electric potential & volts & V \tabularnewline
+electric current & Amperes & A \tabularnewline
+illuminace & lux & lx \tabularnewline
+luminous flux & lumen & lm \tabularnewline
+luminous intensity & candelas & cd \tabularnewline
+luminance & candelas per square meter & cd/m2 \tabularnewline
+vapor diffusivity & m2/s & ~ \tabularnewline
+viscosity & ------------------------------------------------------------------------ & kg/m-s \tabularnewline
+porosity & ------------------------------------------------------------------------ & m3/m3 \tabularnewline
+thermal gradient coeff for moisture capacity & ------------------------------------------------------------------------ & kg/kg-K \tabularnewline
+isothermal moisture capacity & ------------------------------------------------------------------------ & m3/kg \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/interface-developer/src/input-overview.tex b/doc/interface-developer/src/input-overview.tex
new file mode 100644
index 00000000000..572a984e099
--- /dev/null
+++ b/doc/interface-developer/src/input-overview.tex
@@ -0,0 +1,20 @@
+\chapter{Input Overview}\label{input-overview}
+
+The general structure of the input files for EnergyPlus is plain text.~ Fields are comma delimited and each ``line'' is terminated with a semicolon.~ This allows for a very rudimentary input processor that can be instantly flexible to developer's needs.~ However, it puts more burdens on the EnergyPlus developers to process the input information, supply defaults as needed, and perform validity checks.~ Guidelines were established for the input:
+
+\begin{itemize}
+\item
+  Input will be a flat ASCII file with comma-delimited columns and each ``line'' (where each line can run over several physical file records) terminated with a semicolon.
+\item
+  Input should be ``readable'', ``editable'', ``simply parsed with few value checks or consistency checks''.
+\item
+  Input, to the extent possible, should be easily maintainable and extendable.
+\item
+  Input will be ``object based''.
+\item
+  Definitions in a data dictionary will define the input.~ The data dictionary should be self-documenting.
+\item
+  All input units will be metric (SI).~ Conversions from ``user units'' will be done in the interface agents.
+\end{itemize}
+
+Two input files are necessary for the input processing.~ The first is the ``data dictionary'' which will specify the requirements for each item.~ The EnergyPlus Input Processor uses these requirements to process the ``input data file'' and report any anomalies found.~ Both input files have similar structures: 1) Sections -- single lines/commands, which may help group the simulation input for readability and 2) Classes/Objects -- data attributes for the simulation.~ Classes are the term used in the data dictionary -- each class will specify the kind of data (alpha or numeric) that will be included in the simulation input.~ Objects are instances of these classes and appear in the IDF with appropriate data.
diff --git a/doc/interface-developer/src/input-overview/general-input-rules.tex b/doc/interface-developer/src/input-overview/general-input-rules.tex
new file mode 100644
index 00000000000..e45370009b3
--- /dev/null
+++ b/doc/interface-developer/src/input-overview/general-input-rules.tex
@@ -0,0 +1,26 @@
+\section{General Input Rules}\label{general-input-rules}
+
+The following rules apply to both the Input Data Dictionary and the Input Data File.
+
+\begin{itemize}
+\item
+  The initial line of a definition or input MUST have a comma or semicolon.
+\item
+  Fields do not extend over line boundaries.~ Usually, if a comma or (as appropriate) semi-colon is not the last field value on a line, one will be inserted.~ Of course, several fields may appear on a single line as long as they are comma separated.
+\item
+  Commas delimit fields -- therefore, no fields can have embedded commas.~ No error will occur but you won't get what you want.
+\item
+  Blank lines are allowed.
+\item
+  The comment character is a exclamation ``!''.~ Anything on a line after the exclamation is ignored.
+\item
+  A special type of comment using the character combination: ``!-`` in the input file is a special form of comment that is followed by the field name(s) and units and should not include user provided text. This form is used to indicate automatic comments which may be written by interfaces and other utilities as an endline comment after a field value.
+\item
+  Input records can be up to 500 characters in length.~ If you go over that, no error will occur but you won't get what you want.
+\item
+  Each Section and Class/Object keyword can be up to 100 characters in length.~ Embedded spaces are allowed, but are significant (if you have 2 spaces in the section keyword -- you must have 2 when you write the object keyword).
+\item
+  Each Alpha string (including Section and Class/Object keywords) is mapped to UPPER case during processing, unless the ``retaincase'' flag marks the field in the IDD. ~Get routines from the EnergyPlus code that use the Section and Object keywords automatically map to UPPER case for finding the item.~ The primary drawback with this is that error messages coming out of the input processor will be in UPPER case and may not appear exactly as input.
+\item
+  Special characters, such as tabs, should NOT be included in the file.~ However, tabs can be accommodated and are turned into spaces.
+\end{itemize}
diff --git a/doc/interface-developer/src/input-overview/input-data-dictionary.tex b/doc/interface-developer/src/input-overview/input-data-dictionary.tex
new file mode 100644
index 00000000000..0658f92c8bb
--- /dev/null
+++ b/doc/interface-developer/src/input-overview/input-data-dictionary.tex
@@ -0,0 +1,17 @@
+\section{Input Data Dictionary}\label{input-data-dictionary}
+
+The input data dictionary specifies the ``definitions'' for each line that will be processed in the input data file.
+
+Structure in the input data dictionary allows for descriptions that may be useful for interface developers.~ The Input Processor ignores everything but the essentials for getting the ``right stuff'' into the program.~ Developers have been (and will continue to be) encouraged to include comments and other documentation in the IDD.
+
+Internal to the data dictionary (using special ``comment'' characters) is a structured set of conventions for including information on each object.~ This is shown in section on Input Details below.
+
+\subsection{Rules specific to the Input Data Dictionary}\label{rules-specific-to-the-input-data-dictionary}
+
+In addition to the rules for both files (listed above), the IDD also has the limitation:
+
+\begin{itemize}
+\tightlist
+\item
+  Duplicate Section names and Duplicate Class names are not allowed.~ That is, the first class of an item named X will be the one used during processing.~ Error messages will appear if you try to duplicate definitions.
+\end{itemize}
diff --git a/doc/interface-developer/src/input-overview/input-data-file.tex b/doc/interface-developer/src/input-overview/input-data-file.tex
new file mode 100644
index 00000000000..8b9af9f0759
--- /dev/null
+++ b/doc/interface-developer/src/input-overview/input-data-file.tex
@@ -0,0 +1,14 @@
+\section{Input Data File}\label{input-data-file}
+
+This is the only file that EnergyPlus uses to create the building simulation.~ The input is order-independent; data can appear in any order and will be retrieved and sorted as necessary by the EnergyPlus simulation modules.~ In addition, EnergyPlus allocates everything dynamically, so there are no limitations as to number of zones, surfaces, etc.
+
+All numbers can be flexibly input and are processed into single precision variables (i.e.~1.0, 1.000, 1, .1E+1 are all processed equally).
+
+\subsection{Rules specific to Input Data file:}\label{rules-specific-to-input-data-file}
+
+\begin{itemize}
+\item
+  Each Alpha string in the input data file can be up to 100 characters in length.~ Anything beyond that is truncated.
+\item
+  A special combination of characters ``!-`` indicates a comment that contains the name and units of the field after each field value. These, like normal comments, are ignored by EnergyPlus. This type of comment containing the field names are created automatically with IDF Editor, IDF Version Updater (transition) and other user interfaces. Comments added by the user should not use ``!-`` because they are deleted and replaced with the field name when the file is saved using IDF Editor. For an example of this syntax, see the example file in Appendix A.
+\end{itemize}
diff --git a/doc/interface-developer/src/introduction.tex b/doc/interface-developer/src/introduction.tex
new file mode 100644
index 00000000000..fc80f32b25d
--- /dev/null
+++ b/doc/interface-developer/src/introduction.tex
@@ -0,0 +1,23 @@
+\chapter{Introduction}\label{introduction}
+
+This document is intended for developers who are creating user interfaces for EnergyPlus.~ It provides an overview of the essentials of the input-output structure of EnergyPlus and describes the parts of each in detail.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image001.png}
+\caption{EnergyPlus Input/Output Overview \protect \label{fig:energyplus-inputoutput-overview}}
+\end{figure}
+
+The diagram shown above should give the reader an overall picture of input-output in EnergyPlus.~ It can be seen as a linear process that includes the following steps:
+
+1)~~~The user enters building description (including internal space gains, HVAC arrangements, and Plant equipment properties) using the interface of their choice.~ In addition, the user specifies which non-default reports are desired and any optional variables from a predefined list of available simulation quantities.
+
+2)~~~The interface program writes the Input Data File (IDF) file, which includes the specification of any report items desired by the user.
+
+3)~~~EnergyPlus processes both the Input Data Dictionary (IDD) and the Input Data File (IDF) files with the ``InputProcessor''.~ The InputProcessor uses the specifications/rules defined in the IDD and interprets the IDF raw data.~ The InputProcessor is really quite ``dumb'' and only understands a few things about each field (alpha or numeric) qualified by certain key elements in the IDD (\textbackslash{} comments which are discussed later).
+
+4)~~~Each module in EnergyPlus has one or several routines (normally called ``GetInput'' routines) that obtain the information from the IDF file data.~ These subroutines decode the portion of the IDF file that is pertinent to the local module.~ These GetInput routines are more context sensitive than the InputProcessor and may perform further error detection.~ For example, the cooling coil module may read in the coil type and its associated parameters (number of rows, tube diameter, fin spacing, etc.).
+
+5)~~~EnergyPlus performs the simulation elements specified in the IDF.~ Output is generated as a continuous stream (for the most part) and must be interpreted into a more cohesive form by output processing.~ The user has control over which outputs are produced and when/how often.
+
+6)~~~EnergyPlus produces output as required by the user into one of the output files.~ These files can be readily processed into spreadsheet formats for graphing and other summarizing.
diff --git a/doc/interface-developer/src/introduction/interface-expectations.tex b/doc/interface-developer/src/introduction/interface-expectations.tex
new file mode 100644
index 00000000000..3ed4cf55d3f
--- /dev/null
+++ b/doc/interface-developer/src/introduction/interface-expectations.tex
@@ -0,0 +1,46 @@
+\section{Interface Expectations}\label{interface-expectations}
+
+The input-output interfaces may be combined into a single program or may be available separately.~ The following attributes are expected from these interfaces.
+
+\subsection{Input Interface Attributes}\label{input-interface-attributes}
+
+The input interface agents will be expected to fulfill two main requirements:
+
+\begin{itemize}
+\item
+  Ability to produce the input file for the simulation.
+\item
+  Perform the consistency and value checks necessary to assure that the input file conforms to EnergyPlus requirements.
+\end{itemize}
+
+Additionally, the input interface agent might:
+
+\begin{itemize}
+\item
+  Ability to warn users about potential output file size.~ It is expected that the data files generated by the EnergyPlus program will be significantly larger than the output files from its parent programs.~ As a result, users may be unaware that selecting too many reports could lead to enormous output files.~ It is recommended that some sort of checking be done to alert users when the term of the simulation and the number of reports selected eclipse some reasonable file size limit.
+\item
+  Ability to perform parametric runs.
+\end{itemize}
+
+The method used by the input interface agent to accomplish these goals is left to the discretion of the interface developer.
+
+\subsection{Post-processing Interface Attributes}\label{post-processing-interface-attributes}
+
+The post-processing agents will be expected to fulfill the main requirement:
+
+\begin{itemize}
+\tightlist
+\item
+  Ability to read all or selected output formats.
+\end{itemize}
+
+Additionally, a post-processing agent might:
+
+\begin{itemize}
+\item
+  Ability to combine and summarize data (average, peak, total, etc.) and produce the various text and graphical reports requested by the user.
+\item
+  Ability to handle multiple output files.
+\end{itemize}
+
+The method used by the post-processing agent to accomplish these goals is left to the discretion of the interface developer.
diff --git a/doc/interface-developer/src/licensing.tex b/doc/interface-developer/src/licensing.tex
new file mode 100644
index 00000000000..e79f91798f8
--- /dev/null
+++ b/doc/interface-developer/src/licensing.tex
@@ -0,0 +1,5 @@
+\chapter{Licensing}\label{licensing}
+
+In order to make efficient distribution of your interface, you should consider licensing EnergyPlus.~ First, you must license/register to use EnergyPlus.~ Since we are distributing EnergyPlus via the World Wide Web, at no charge, it will be easy to get your hands on a copy for testing out your interface.~ However, you may wish to understand more of the internals and, to make a complete distribution package, will need to at least execute a distribution license.
+
+https://energyplus.net/licensing contains the details on licensing EnergyPlus for commercial or non-commercial use.
diff --git a/doc/interface-developer/src/output.tex b/doc/interface-developer/src/output.tex
new file mode 100644
index 00000000000..7daaf43e33e
--- /dev/null
+++ b/doc/interface-developer/src/output.tex
@@ -0,0 +1,87 @@
+\chapter{Output}\label{output}
+
+EnergyPlus produces several output files as shown in the section on ``Running EnergyPlus''.~~ This section will discuss the data contained in the ``standard'' output file (\textbf{eplusout.eso}).~ It, too, has a data dictionary but unlike the input files, the output data dictionary is contained within the output file.~ Thus, the basic structure of the standard output file is:
+
+\begin{lstlisting}
+Data Dictionary Information
+End of Data Dictionary
+Data
+…
+Data
+End of Data
+\end{lstlisting}
+
+As with the IDF structure, there are rules associated with the interpretation of the standard output data dictionary.~ These rules are summarized as follows:
+
+\begin{itemize}
+\item
+  The first item on each line is an integer which represents the ``report code''.~ This ``report code'' will be listed in the data section where it will also be the first item on each line, identifying the data.~ Only 2 lines in the output file will not have an integer as the first item (``End of Data Dictionary'' and ``End of Data'' lines).
+\item
+  The second item on each line is also an integer.~ This integer corresponds to the number of items left on the dictionary line.~ Each string consists of a variable name and units in square brackets.~ Square brackets are required for all strings.~ If there are no units associated with a particular variable, then there are no characters between the brackets.
+\end{itemize}
+
+Six standard items appear at the start of every EnergyPlus Standard Output File Data Dictionary:
+
+\begin{lstlisting}
+Program Version,EnergyPlus, 1.0, Beta 2, Build 017
+1,5,Environment Title[],Latitude[degrees],Longitude[degrees],Time Zone[],Elevation[m]
+2,6,Day of Simulation[],Month[],Day of Month[],DST Indicator[1 = yes 0 = no], Hour[], StartMinute[], EndMinute[], DayType
+3,3,Cumulative Day of Simulation[],Month[],Day of Month[],DST Indicator[1 = yes 0 = no],DayType
+4,2,Cumulative Days of Simulation[],Month[]
+5,1,Cumulative Days of Simulation[]
+\end{lstlisting}
+
+\begin{itemize}
+\item
+  Item 0 is the program version statement.
+\item
+  Item 1 is produced at the beginning of each new ``environment'' (design day, run period).
+\item
+  Item 2 is produced prior to any variable reported at the timestep or hourly intervals.~ Hourly intervals will be shown with a start minute of 0.0 and an end minute of 60.0.~ Timestep intervals will show the appropriate start and end minutes.
+\item
+  Item 3 is produced prior to any variable reported at the daily interval.
+\item
+  Item 4 is produced prior to any variable reported at the monthly interval.
+\item
+  Item 5 is produced prior to any variable reported at the end of the ``environment''.
+\end{itemize}
+
+Following these five standard lines will be the variables requested for reporting from the input file (ref. Report Variable).~ For example:
+
+\begin{lstlisting}
+6,2,Environment,Outdoor Dry Bulb [C] !Hourly
+21,2,ZONE ONE,Mean Air Temperature[C] !Hourly
+22,2,ZONE ONE,Zone-Total Latent Gain[J] !Hourly
+26,2,ZONE ONE,Zone-Total Electric Consumption[J] !Hourly
+\end{lstlisting}
+
+This example illustrates the non-consecutive nature of the ``report codes''.~ Internally, EnergyPlus counts each variable that \emph{could} be reported.~ This is the assigned ``report code''.~ However, the user may not request each possible variable for reporting.~ Note that, currently, the requested reporting frequency is shown as a comment (!) line in the standard output file.
+
+The data is produced when the actual simulation is performed (after the warmup days).~ Data output is simpler in format than the data dictionary lines.~ From the dictionary above:
+
+\begin{lstlisting}
+1,DENVER COLORADO WINTER,  39.75,-104.87,  -7.00,1610.26
+2,  1, 1,21, 0, 1, 0.00,60.00,Monday
+6,-17.22222
+21,-17.22219
+22,0.0000000E+00
+26,0.0000000E+00
+2,  1, 1,21, 0, 2, 0.00,60.00,Monday
+6,-17.22222
+21,-17.22219
+22,0.0000000E+00
+26,0.0000000E+00
+2,  1, 1,21, 0, 3, 0.00,60.00,Monday
+6,-17.22222
+21,-17.22219
+22,0.0000000E+00
+26,0.0000000E+00
+\end{lstlisting}
+
+This output file can be easily turned into a form that is read into commonly used spreadsheet programs where it can be further analyzed, graphed, etc.
+
+\begin{figure}[hbtp] % fig 3
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image003.png}
+\caption{  Example Chart from Standard Output File \protect \label{fig:example-chart-from-standard-output-file}}
+\end{figure}
diff --git a/doc/interface-developer/src/running-energyplus.tex b/doc/interface-developer/src/running-energyplus.tex
new file mode 100644
index 00000000000..9e8a4236632
--- /dev/null
+++ b/doc/interface-developer/src/running-energyplus.tex
@@ -0,0 +1,117 @@
+\chapter{Running EnergyPlus}\label{running-energyplus}
+
+EnergyPlus is written in C++ and runs as a console application. More explicit details on running EnergyPlus are available in a separate document (Running EnergyPlus in Auxiliary Programs document). Optional command-line arguments are available (energyplus --help, or man energyplus on Linux systems). The following files are used to run EnergyPlus:
+
+\begin{itemize}
+\item
+  EnergyPlus.exe (the executable file)
+\item
+  Energy+.ini (described below)
+\item
+  Energy+.idd (the input data dictionary file)
+\item
+  In.idf (the input file)
+\item
+  In.epw -- optional (weather data file)
+\end{itemize}
+
+The input data dictionary and input data file have been discussed in the previous sections of this document.
+
+For weather simulations, EnergyPlus accepts EnergyPlus weather files. Previous versions accepted BLAST formatted weather files and now a BLASTWeatherConverter program is provided.~ The actual file name is \textbf{in.epw}.
+
+The Energy+.ini file is a ``standard'' Windowsâ„¢ ini file and can be manipulated using the Windows API calls though EnergyPlus uses standard Fortran to manipulate it.~ It is a very simple ini file and is fully described in the \href{file:///E:/Docs4PDFs/AuxiliaryPrograms.pdf}{Auxiliary Programs} document. Energy+.ini and in.idf file should be in the directory from which you are running EnergyPlus.exe.
+
+For the advanced user, there is also the ``EPMacro'' program, described in the Auxiliary Programs Document.~ You run it as a separate program before EnergyPlus (the batch file included in the install and shown in the GettingStarted document contains the commands).
+
+EnergyPlus creates the following files (plus more):
+
+% table 2
+\begin{longtable}[c]{@{}ll@{}}
+\caption{EnergyPlus Output Files \label{table:energyplus-output-files}} \tabularnewline
+\toprule 
+FileName & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{EnergyPlus Output Files} \tabularnewline
+\toprule 
+FileName & Description \tabularnewline
+\midrule
+\endhead
+
+Audit.out & Echo of input \tabularnewline
+Eplusout.err & Error file \tabularnewline
+Eplusout.eso & Standard Output File \tabularnewline
+Eplusout.eio & One time output file \tabularnewline
+Eplusout.rdd & Report Variable Data Dictionary \tabularnewline
+Eplusout.dxf & DXF (from Report,Surfaces,DXF;) \tabularnewline
+Eplusout.end & A one line summary of success or failure \tabularnewline
+\bottomrule
+\end{longtable}
+
+The eplusout.err file may contain three levels of errors (Warning, Severe, Fatal) as well as the possibility of just message lines.~ These errors may be duplicated in other files (such as the standard output file).
+
+% table 3
+\begin{longtable}[c]{@{}ll@{}}
+\caption{EnergyPlus Errors \label{table:energyplus-errors}} \tabularnewline
+\toprule 
+Error Level & Action \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{EnergyPlus Errors} \tabularnewline
+\toprule 
+Error Level & Action \tabularnewline
+\midrule
+\endhead
+
+Warning & Take note \tabularnewline
+Severe & Should Fix \tabularnewline
+Fatal & Program will abort \tabularnewline
+\bottomrule
+\end{longtable}
+
+EnergyPlus produces several messages as it is executing, as a guide to its progress.~ For example, the run of the 1ZoneUncontrolled input file from Appendix A produces:
+
+\begin{lstlisting}
+
+EnergyPlus Starting
+   EnergyPlus 1.3.0.011, 4/5/2006 2:59 PM
+   Initializing New Environment Parameters
+   Warming up {1}
+   Initializing Response Factors
+   Initializing Window Optical Properties
+   Initializing Solar Calculations
+   Initializing HVAC
+   Warming up {2}
+   Warming up {3}
+   Warming up {4}
+   Starting Simulation at 12/21 for DENVER_STAPLETON ANN HTG 99% CONDNS DB
+   Initializing New Environment Parameters
+   Warming up {1}
+   Warming up {2}
+   Warming up {3}
+   Starting Simulation at 07/21 for DENVER_STAPLETON ANN CLG 1% CONDNS DB = >MWB
+   EnergyPlus Run Time = 00hr 00min  1.00sec
+\end{lstlisting}
+
+Extensive timing studies and fine-tuning of EnergyPlus is NOT complete.~ To give you an idea of comparable run times, we present the following (does not include HVAC) with an early version of EnergyPlus running on a 450MHZ machine.~ Remember, BLAST would be 1 calculation per hour, EnergyPlus (in this case) was 4 calculations per hour.~ Obviously, these are quite out of date.~ However, a recent change in a developer's test machine illustrates the importance of maximum memory.~ A 5 zone full year run on a 1.8GHZ, 1GB machine was running about 8 minutes -- with a new 2.1GHZ, 2GB machine the same file takes about 2 minutes.
+
+% table 4
+\begin{longtable}[c]{p{3.0in}p{1.5in}p{1.5in}}
+\caption{Timings Comparison (EnergyPlus vs. BLAST) \label{table:timings-comparison-energyplus-vs.-blast}} \tabularnewline
+\toprule 
+File & BLAST Per Zone & EnergyPlus Per Zone \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Timings Comparison (EnergyPlus vs. BLAST)} \tabularnewline
+\toprule 
+File & BLAST Per Zone & EnergyPlus Per Zone \tabularnewline
+\midrule
+\endhead
+
+GeometryTest (5 Zones, 2 Design Day, Full Weather Year) & 13 sec & 33 sec \tabularnewline
+SolarShadingTest (9 Zones, Full Weather Year) & 7 sec & 25 sec \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/interface-developer/src/weather-data.tex b/doc/interface-developer/src/weather-data.tex
new file mode 100644
index 00000000000..07e48bbc00e
--- /dev/null
+++ b/doc/interface-developer/src/weather-data.tex
@@ -0,0 +1,5 @@
+\chapter{Weather Data}\label{weather-data}
+
+Weather data in EnergyPlus is a simple text-based format, similar to the input data and output data files. The weather data format includes basic location information in the first eight lines: location (name, state/province/region, country), data source, latitude, longitude, time zone, elevation, peak heating and cooling design conditions, holidays, daylight saving period, typical and extreme periods, two lines for comments, and period covered by the data. The data are also comma-separated and contain much of the same data in the TMY2 weather data set (NREL 1995). EnergyPlus does not require a full year or 8760 (or 8784) hours in its weather files. In fact, EnergyPlus allows and reads subsets of years and even sub-hourly (5 minute, 15 minute) data---the weather format includes a `minutes' field. EnergyPlus comes with a utility that reads standard weather service file types such as TMY2, IWEC and WYEC2 files, as examples, as well as being able to read a user defined custom format.
+
+The ``data dictionary'' for EnergyPlus Weather Data is shown in the Auxiliary Programs document -- please review that document for further information.
diff --git a/doc/module-developer/CMakeLists.txt b/doc/module-developer/CMakeLists.txt
new file mode 100644
index 00000000000..9558181e4de
--- /dev/null
+++ b/doc/module-developer/CMakeLists.txt
@@ -0,0 +1,100 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/module-developer.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/guide-for-module-developers.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/introduction.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/modules-in-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/modules-in-energyplus/what-is-a-module-anyway.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/modules-in-energyplus/what-is-a-module-developer.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/modules-in-energyplus/adding-new-features.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/input-concepts.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/input-concepts/input-data-dictionary.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/input-concepts/data-dictionary-naming-conventions.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/input-concepts/input-data-file.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/input-concepts/input-considerations.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/input-concepts/advanced-input-considerations.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/input-concepts/datasets.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/module-structure.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/module-structure/module-outline.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/module-structure/module-example.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/module-structure/changing-existing-code.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/module-structure/considerations-for-legacy-codes.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/module-structure/code-readability-vs-speed-of-execution.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/module-structure/how-it-fits-together.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-calling-structure.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-calling-structure/top-level-calling-tree.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-calling-structure/high-level-hvac-calling-tree-schematic-not.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-calling-structure/air-system-calling-tree-schematic-not-all.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-calling-structure/plant-calling-tree-schematic-not-all-routines.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-calling-structure/zone-equipment-calling-tree-schematic-not-all.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-calling-structure/inserting-the-new-module-into-the-program.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/hvac-network.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/hvac-network/branches-connectors-and-nodes.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/hvac-network/nodes-in-the-simulation.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/hvac-network/getting-nodes.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/hvac-network/data-flow-in-an-hvac-component-module.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/hvac-network/interfacing-with-plant.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/hvac-network/node-mass-flow-variables.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/utility-routines-functions.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/input-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/object-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/branch-node-checking-and-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/schedule-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/data-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/other-useful-utilities.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/error-messages.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/display-strings.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/performance-curve-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/fluid-property-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/weather-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/global-data-flags-and-parameters.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/psychrometric-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/tabular-output-utilities.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energyplus-services/internal-zone-gains-services.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/output.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/output/how-do-i-output-my-variables.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/output/output-variable-dos-and-don-ts.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energy-management-system.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/energy-management-system/ems-actuator-interface.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/running-testing-energyplus-for-developers.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/running-testing-energyplus-for-developers/environment-variables-to-assist-running.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/running-testing-energyplus-for-developers/air-loop-simulation-environment-variables.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/quick-procedure-outline-for-making-code.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/important-rules-for-module-developers.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments/dataglobals.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments/dataenvironment.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/appendix-b-submissions-and-check-ins.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/appendix-c-documentation-specifics.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/appendix-d-module-subroutine-function.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/appendix-e-test-file-documentation.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/appendix-f-new-or-changed-proposal-feature.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/src/appendix-g.tex
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/../title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/media/image001.png
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/media/image002.png
+  ${CMAKE_SOURCE_DIR}/doc/module-developer/media/image003.jpg
+) 
+
+SET( SOURCE_FILENAME "module-developer" )
+SET( OUTPUT_FILENAME "ModuleDeveloper" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/src/docs/ModuleDeveloper/media/ep.gif b/doc/module-developer/media/ep.gif
similarity index 100%
rename from doc/src/docs/ModuleDeveloper/media/ep.gif
rename to doc/module-developer/media/ep.gif
diff --git a/doc/module-developer/media/ep.png b/doc/module-developer/media/ep.png
new file mode 100644
index 00000000000..a808760c870
Binary files /dev/null and b/doc/module-developer/media/ep.png differ
diff --git a/doc/src/docs/ModuleDeveloper/media/image001.png b/doc/module-developer/media/image001.png
similarity index 100%
rename from doc/src/docs/ModuleDeveloper/media/image001.png
rename to doc/module-developer/media/image001.png
diff --git a/doc/src/docs/ModuleDeveloper/media/image002.png b/doc/module-developer/media/image002.png
similarity index 100%
rename from doc/src/docs/ModuleDeveloper/media/image002.png
rename to doc/module-developer/media/image002.png
diff --git a/doc/src/docs/ModuleDeveloper/media/image003.jpg b/doc/module-developer/media/image003.jpg
similarity index 100%
rename from doc/src/docs/ModuleDeveloper/media/image003.jpg
rename to doc/module-developer/media/image003.jpg
diff --git a/doc/module-developer/module-developer.tex b/doc/module-developer/module-developer.tex
new file mode 100644
index 00000000000..59463df8521
--- /dev/null
+++ b/doc/module-developer/module-developer.tex
@@ -0,0 +1,158 @@
+\input{../header}
+
+\title{Guide for Module Developers}
+
+\hypersetup{unicode=true,
+            pdftitle={Guide for Module Developers},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/guide-for-module-developers}
+
+\input{src/introduction}
+
+\input{src/modules-in-energyplus}
+
+\input{src/modules-in-energyplus/what-is-a-module-anyway}
+
+\input{src/modules-in-energyplus/what-is-a-module-developer}
+
+\input{src/modules-in-energyplus/adding-new-features}
+
+\input{src/input-concepts}
+
+\input{src/input-concepts/input-data-dictionary}
+
+\input{src/input-concepts/data-dictionary-naming-conventions}
+
+\input{src/input-concepts/input-data-file}
+
+\input{src/input-concepts/input-considerations}
+
+\input{src/input-concepts/advanced-input-considerations}
+
+\input{src/input-concepts/datasets}
+
+\input{src/module-structure}
+
+\input{src/module-structure/module-outline}
+
+\input{src/module-structure/module-example}
+
+\input{src/module-structure/changing-existing-code}
+
+\input{src/module-structure/considerations-for-legacy-codes}
+
+\input{src/module-structure/code-readability-vs-speed-of-execution}
+
+\input{src/module-structure/how-it-fits-together}
+
+\input{src/energyplus-calling-structure}
+
+\input{src/energyplus-calling-structure/top-level-calling-tree}
+
+\input{src/energyplus-calling-structure/high-level-hvac-calling-tree-schematic-not}
+
+\input{src/energyplus-calling-structure/air-system-calling-tree-schematic-not-all}
+
+\input{src/energyplus-calling-structure/plant-calling-tree-schematic-not-all-routines}
+
+\input{src/energyplus-calling-structure/zone-equipment-calling-tree-schematic-not-all}
+
+\input{src/energyplus-calling-structure/inserting-the-new-module-into-the-program}
+
+\input{src/hvac-network}
+
+\input{src/hvac-network/branches-connectors-and-nodes}
+
+\input{src/hvac-network/nodes-in-the-simulation}
+
+\input{src/hvac-network/getting-nodes}
+
+\input{src/hvac-network/data-flow-in-an-hvac-component-module}
+
+\input{src/hvac-network/interfacing-with-plant}
+
+\input{src/hvac-network/node-mass-flow-variables}
+
+\input{src/energyplus-services}
+
+\input{src/energyplus-services/utility-routines-functions}
+
+\input{src/energyplus-services/input-services}
+
+\input{src/energyplus-services/object-services}
+
+\input{src/energyplus-services/branch-node-checking-and-services}
+
+\input{src/energyplus-services/schedule-services}
+
+\input{src/energyplus-services/data-services}
+
+\input{src/energyplus-services/other-useful-utilities}
+
+\input{src/energyplus-services/error-messages}
+
+\input{src/energyplus-services/display-strings}
+
+\input{src/energyplus-services/performance-curve-services}
+
+\input{src/energyplus-services/fluid-property-services}
+
+\input{src/energyplus-services/weather-services}
+
+\input{src/energyplus-services/global-data-flags-and-parameters}
+
+\input{src/energyplus-services/psychrometric-services}
+
+\input{src/energyplus-services/tabular-output-utilities}
+
+\input{src/energyplus-services/internal-zone-gains-services}
+
+\input{src/output}
+
+\input{src/output/how-do-i-output-my-variables}
+
+\input{src/output/output-variable-dos-and-don-ts}
+
+\input{src/energy-management-system}
+
+\input{src/energy-management-system/ems-actuator-interface}
+
+\input{src/running-testing-energyplus-for-developers}
+
+\input{src/running-testing-energyplus-for-developers/environment-variables-to-assist-running}
+
+\input{src/running-testing-energyplus-for-developers/air-loop-simulation-environment-variables}
+
+\input{src/quick-procedure-outline-for-making-code}
+
+\input{src/important-rules-for-module-developers}
+
+\input{src/appendix-a-dataglobals-and-dataenvironments}
+
+\input{src/appendix-a-dataglobals-and-dataenvironments/dataglobals}
+
+\input{src/appendix-a-dataglobals-and-dataenvironments/dataenvironment}
+
+\input{src/appendix-b-submissions-and-check-ins}
+
+\input{src/appendix-c-documentation-specifics}
+
+\input{src/appendix-d-module-subroutine-function}
+
+\input{src/appendix-e-test-file-documentation}
+
+\input{src/appendix-f-new-or-changed-proposal-feature}
+
+\input{src/appendix-g}
+
+\end{document}
diff --git a/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments.tex b/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments.tex
new file mode 100644
index 00000000000..8910dd44f3b
--- /dev/null
+++ b/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments.tex
@@ -0,0 +1,3 @@
+\chapter{Appendix A.~ DataGlobals and DataEnvironments Modules}\label{appendix-a.-dataglobals-and-dataenvironments-modules}
+
+Rather than include the code of the DataGlobals and DataEnvironments modules, they will be described here.
diff --git a/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments/dataenvironment.tex b/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments/dataenvironment.tex
new file mode 100644
index 00000000000..fac4c797f4b
--- /dev/null
+++ b/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments/dataenvironment.tex
@@ -0,0 +1,3 @@
+\section{DataEnvironment}\label{dataenvironment}
+
+DataEnvironment is intended to address global environmental variables (such as current outdoor temperature, barometric pressure, and so forth).~ It is also extends the concept of a ``data only'' module a bit to encompass a few functions that calculate values for the site atmospheric variation concept.
diff --git a/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments/dataglobals.tex b/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments/dataglobals.tex
new file mode 100644
index 00000000000..8057b17bc2e
--- /dev/null
+++ b/doc/module-developer/src/appendix-a-dataglobals-and-dataenvironments/dataglobals.tex
@@ -0,0 +1,17 @@
+\section{DataGlobals}\label{dataglobals}
+
+DataGlobals contains parameters, variables, Interface descriptors that could be used by every part of the program.~ For example, this is where the ``MaxNameLength'' (maximum name length (characters) of objects.~ All other pieces of the code that need this will need to
+
+USE DataGlobals
+
+and, if that's the only piece it needs, can say
+
+USE DataGlobals, ONLY: MaxNameLength
+
+Interface specifications for the ShowError routines are here because there are optional parameters in these routines.~ Then,
+
+USE DataGlobals, ONLY: ShowWarningError, ShowFatalError
+
+can be used safely from any routine.~ Constants such as Pi (p), Degrees To Radians, and Number of Seconds in Hour are also stored there.~ Remember that we suggest compiling EnergyPlus in double precision and these constants (as should all constants) are representative of double precision (even if someone were to compile in single precision).
+
+Finally, the interface specifications for the Setup Report Variables is contained in this module.~ The interface allows for a single call for accomplishing that while actually forking to call several different routines based on the type of data being used.
diff --git a/doc/module-developer/src/appendix-b-submissions-and-check-ins.tex b/doc/module-developer/src/appendix-b-submissions-and-check-ins.tex
new file mode 100644
index 00000000000..fcf6a5f5dd4
--- /dev/null
+++ b/doc/module-developer/src/appendix-b-submissions-and-check-ins.tex
@@ -0,0 +1,125 @@
+\chapter{Appendix B.~ Submissions and Check-ins}\label{appendix-b.-submissions-and-check-ins}
+
+There are two methods by which new modules are entered into the EnergyPlus (publicly available) program.
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Checkin:} Part of the core development team may create or modify an existing module.~ As we use a configuration management system -- this is called a check in.
+\end{itemize}
+
+\emph{Note --- to save people grief and rework effort and to work toward consistency in approach, new features or changes to existing features must be proposed in a documented way for discussion during one of the bi-weekly conference calls.}
+
+\begin{itemize}
+\tightlist
+\item
+  \textbf{Submission:} When someone outside the core development team submits a module or modification of an existing module for inclusion, this is termed a submission.
+\end{itemize}
+
+\emph{Submissions are subjected to the same kind of scrutiny as team checkins and usually will require rework by the submitter.~ We welcome outside developers to send their ideas as early documents for comment with the understanding that revising does not guarantee automatic inclusion.~ See the proposed feature outline document in Appendix F and/or the ``doc'' file in the Documents for Developers Zip file.}
+
+Both kinds of inclusions need to follow the checklist procedure for new inclusions:
+
+ü~\textbf{Source Code Rules}
+
+Shall follow programming standard
+
+Shall follow F90/95 or later standards~ (use ``allocatable'' for allocatable structures within Derived Types)
+
+Shall follow the Template standards (documentation, naming conventions)
+
+Shall follow the guidelines shown in this document
+
+All items shall be directly initialized (exception: derived type elements may be staticly initialized)
+
+There shall be no ``unused'' variables.~ If you put in a variable that you ``might use later'' -- comment it out and comment it to be used later.
+
+No Tabs in source code!!!
+
+Lines shall be less than 133 characters in length.~ (Some compilers allow longer lines without warning).
+
+Suggest using F95 standards checking during compiles -- you may use the compiler option to generate warnings for non-standard code.
+
+\textbf{Permission to use the code shall be supplied -- written, even email, is required.~ LBNL is monitoring this aspect -- so a grant-back letter can also be obtained from them.}
+
+ü~\textbf{Energy+.IDD rules}
+
+Standard Units shall be used (SI only on Input)
+
+Show units with the \textbf{\textbackslash{}units} field.~ Supply \textbf{\textbackslash{}ip-units} only if your input would require it (see comments at top of the Energy+.idd).
+
+Use \textbf{\textbackslash{}minimum} and \textbf{\textbackslash{}maximum}
+
+The first field following the object name should contain ``\textbf{name}'' as part of the field name
+
+Use \textbf{\textbackslash{}default, \textbackslash{}min-fields} and \textbf{\textbackslash{}required-field} appropriately
+
+Object changes during minor releases (x.x.xxx) should not change fields in the middle -- only at the end
+
+Surface objects may not add further fields to the end (the end is reserved for vertices and extension to the current limits)
+
+Note that changes in the Energy+.idd will require a ``transition'' rule change in the Rules Spreadsheet file (Rules\ldots{}xls).~ Likewise, changes in report variable names must be documented in the ``report variables'' change file that is a companion to the Rules spreadsheet.
+
+ü~\textbf{Testing}
+
+Shall run the full test suite for all new features and unless you are absolutely, positively sure that your change will not impact other parts of the code.~ We have a python script that can compare between two run versions (using the .csv files output from ReadVarsESO).
+
+If you need a script, look under StarTeam\ldots{}Test Files\textgreater{}ScriptMaker.~ Other scripts are mentioned in the section on ``Running EnergyPlus for Developers'' (Module Developer's Guide).
+
+If you modify objects, you must change all test suite files that are impacted by your object modifications.
+
+ü~\textbf{New Features need a new example file}
+
+You must create a new input file for your changes---input files shall include appropriate internal documentation!~ (Test files have a document template as well seeAppendix E.~ Test File Documentation).~ Some features may be appropriately added to an existing file but documentation must be updated.
+
+You must fill out a line in the ``ExampleFiles.xls'' spreadsheet for your new input file.
+
+You must run a full annual run with your test file even if that is not the configuration that ends up in the internal test suite.~ Annual runs have been known to fail -- obviously, your input file should not.
+
+You must try to minimize the number of errors shown in the eplusout.err file for your files.
+
+Reverse DD Compliance Test: You must run a test that reverses a run of two environments (design days) and make sure that the results (when you also reverse the results files) are identical.~ (Identical means \emph{exactly} the same.)~ Several scripts and automated programs to accomplish this feat are available.
+
+ü~\textbf{Documentation (must be included at the same time as code!!!)}
+
+A document template is available for use -- only the styles in that document should be used.~ (Microsoftâ„¢ Word is our standard word processing software).
+
+Equations -- limited in IORef, necessary in Engineering Doc -- limit the number of ``references'' though.~ You can use standard Equation formatting from Microsoftâ„¢ Word or Mathtypeâ„¢ is an acceptable alternate.
+
+Figures -- Though AutoShapes may draw nice pictures, they are not often ``captionable'' without undue editing.~ Please make figures into Jpegs or GIFs.~ Use ``insert caption'' (below the figure) so that auto-numbering of figures is used (these will transfer automatically to EnergyPlus documents).
+
+Tables -- use ``insert caption'' (above the table) so that auto-numbering of figures is used (these will transfer automatically to EnergyPlus documents).
+
+Cross-References -- limit your ``insert cross references''.~ You should highlight these so that ``editing'' from your inclusion is more obvious -- use a different color to help them stand out.
+
+IORef -- See the InputOutputReference document for indications of what is included.
+
+Eng Ref -- New modules shall include an engineering document reference.~ See the Engineering Reference for indications of typical writeups.
+
+Output Details and Examples -- this can help illustrate your changes.~ Any new files \emph{must} be detailed in here.~ Likewise, changes to the .eio file must be described.
+
+ü~\textbf{FeatureChanges.csv}
+
+Every change to source code, example files, datsets, utilities (any change other than documentation) must include a line in the ``featurechanges.csv'' file.
+
+ü~\textbf{Checked in?}
+
+A courtesy message to the EnergyPlus team should be done for each check in, with details of files checked in, etc.~ Save one of the emails you have received if you don't know how many to send it to.
+
+ü~\textbf{Defect fixing?}
+
+If you fix a defect or ``fix'' a suggested change (CR), you should mark it ``fixed'' in StarTeam and the responsibility should automatically change back to the author of the CR.~ If you fix your own CR, assign it to someone else for verification.
+
+If you fix a defect or ``fix'' a suggested change, you should provide a ``synopsis for users'' (on the ``Custom'' tab in the CR edit dialog) so that when we release the version with your fix, we can provide something descriptive for the users.
+
+~ If a defect has a workaround, you should enter this in the ``Workaround'' field (on the ``Solution'' tab) to inform users until the fix is released in a public version.
+
+ü~\textbf{Rules\ldots{}xls}
+
+If a transition rule will be needed (or a deleted / obsolete / renamed object is needed) -- a line (or more) in this spreadsheet must be used.~ See example rules files from previous releases.~ If in doubt, put something in.
+
+ü~\textbf{ReportVariables\ldots{}csv}
+
+If you change the name of a report variable, the transition program for release can automatically transition older input files \textbf{IF} you put the old and new names into this file.
+
+If you delete a report variable, that detail should go in this file.~ Note that you must consult others on the core development team before deleting a reported variable.
diff --git a/doc/module-developer/src/appendix-c-documentation-specifics.tex b/doc/module-developer/src/appendix-c-documentation-specifics.tex
new file mode 100644
index 00000000000..a3faa518435
--- /dev/null
+++ b/doc/module-developer/src/appendix-c-documentation-specifics.tex
@@ -0,0 +1,52 @@
+\chapter{Appendix C.~ Documentation Specifics}\label{appendix-c.-documentation-specifics}
+
+Documents that module developers will typically be updating or changing are the: Input Output Reference, Engineering Documentation, and Output Details and Examples.~ You may, of course, note revisions to other documents.
+
+All of the EnergyPlus documentation follows a Wordâ„¢ template -- report.dot.
+
+This template takes care of many of the nuances of formatting so that the documents all retain the same ``look and feel''.~ The template itself will contain examples for the IORef and Engineering Documentation.
+
+General guidelines:
+
+\begin{itemize}
+\item
+  Don't get fancy with formatting.~ No extra ``enters'' are needed to space the paragraphs.
+\item
+  Submit your pictures as pictures (jpeg, tif, gif).~ This will allow you to ``insert captions'' below them and have them automatically numbered.~ (This also allows them to be re-numbered once inside the EnergyPlus documents).~ Don't use Text boxes.
+\item
+  Likewise, use an ``insert caption'' on tables.
+\item
+  Table captions go above the table.~ Figure captions go below.
+\item
+  If you want to reference a table or figure in your text, use ``insert cross reference'' and select table or figure as appropriate.~ Usually, just use the ``label and number'' option.
+\item
+  Body Text is the expected style for most text.~ DO NOT put object names in a different font (such as Courier) or as a different size though you may bold them for emphasis.
+\item
+  Headings are used judiciously to help separate text.
+\item
+  Object names (IOReference) are Heading 3.
+\item
+  Each field must be described and shown as Heading 4 followed by the description.~ Form should be ``Field: \textless{}field Name\textgreater{}''. (Exception: if your object has a repeating set of fields -- you may describe the initial field set in detail such as is done for the branch specifications fields in the Branch object).
+\item
+  Each object's IDD must be shown and use the format ``IDD Definition''.
+\item
+  An excerpt IDF using the object must be shown.
+\item
+  Output variables for the object must be shown (heading 4) with a heading 3 \textless{}object name\textgreater{} Output variables preceding.
+\item
+  Equations may be inserted using the Microsoftâ„¢ Equation Editor.~ Internally we use software called ``MathType'' -- that also may be used for Equations.~ It is not desirable to number every equation.~ If you want to reference the equations, of course, you will need to number them -- it is best to number them in plain text and then we can edit them into the rest of the documents.
+\item
+  Each Engineering Reference section should contain a ``References'' section and should be formatted in author style (not numbered).
+\end{itemize}
+
+Example References:
+
+ASHRAE. 1993. 1993 ASHRAE Handbook -- Fundamentals. Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
+
+Chapman, A. J. 1984. Heat Transfer, 4\(^{th}\) Edition, New York: Macmillan Publishing Company.
+
+Lienhard, J. H. 1981. A Heat Transfer Textbook, Englewood Cliffs, N.J.: Prentice-Hall, Inc.
+
+McClellan, T. M., and C. O. Pedersen. 1997. Investigation of Outside Heat Balance Models for Use in a Heat Balance Cooling Load Calculation. ASHRAE Transactions, Vol. 103, Part 2, pp.~469-484.
+
+Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards.
diff --git a/doc/module-developer/src/appendix-d-module-subroutine-function.tex b/doc/module-developer/src/appendix-d-module-subroutine-function.tex
new file mode 100644
index 00000000000..923a7281c13
--- /dev/null
+++ b/doc/module-developer/src/appendix-d-module-subroutine-function.tex
@@ -0,0 +1,667 @@
+\chapter{Appendix D.~ Module, Subroutine, Function Templates}\label{appendix-d.-module-subroutine-function-templates}
+
+The following module template can and should be used to create new modules.~ Following the module template are subroutine and function templates.~ You should be able to copy the template for your own use (or you can get a plain text version).
+
+\textbf{MODULE \textless{}module\_name\textgreater{}}
+
+~~~~~~~~~ ! Module containing the routines dealing with the \textless{}module\_name\textgreater{}
+
+~~~~~~~~~ ! MODULE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ \textless{}author\textgreater{}
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ \textless{}date\_written\textgreater{}
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS MODULE:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! OTHER NOTES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! \textless{}use statements for data only modules\textgreater{}
+
+USE DataGlobals, ONLY: ShowWarningError, ShowSevereError, ShowFatalError, \&
+
+~~~~~~~~~~~~~~~~~~~~~~ MaxNameLength, \ldots{}
+
+~~~~~~~~~ ! \textless{}use statements for access to subroutines in other modules\textgreater{}
+
+IMPLICIT NONE ! Enforce explicit typing of all variables
+
+PRIVATE ! Everything private unless explicitly made public
+
+~~~~~~~~~ ! MODULE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! MODULE VARIABLE DECLARATIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE SPECIFICATIONS FOR MODULE:
+
+~~~~ ! Driver/Manager Routines
+
+PUBLIC~ Sim\textless{}module\_name\textgreater{}
+
+~~~~ ! Get Input routines for module
+
+PRIVATE Get\textless{}module\_name\textgreater{}
+
+~~~~ ! Initialization routines for module
+
+PRIVATE Init\textless{}module\_name\textgreater{}
+
+PRIVATE Size\textless{}module\_name\textgreater{}
+
+~~~~ ! Algorithms/Calculation routines for the module
+
+PRIVATE Calc\textless{}module\_name\textgreater{}
+
+~~~~ ! Update routines to check convergence and update nodes
+
+PRIVATE Update\textless{}module\_name\textgreater{}
+
+~~~~ ! Reporting routines for module
+
+PRIVATE Report\textless{}module\_name\textgreater{}
+
+~~~~ ! Utility routines for module
+
+! these would be public such as:
+
+! PUBLIC~ Get\textless{}module\textgreater{}InletNode
+
+! PUBLIC~ Get\textless{}module\textgreater{}OutletNode
+
+\textbf{CONTAINS}
+
+\textbf{SUBROUTINE Sim\textless{}module\_name\textgreater{}}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ \textless{}author\textgreater{}
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ \textless{}date\_written\textgreater{}
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~ LOGICAL,SAVE~~~~~ :: GetInputFlag = .true.~ ! First time, input is ``gotten''
+
+~ IF (GetInputFlag) THEN
+
+~~~ CALL Get\textless{}module\_name\textgreater{}Input
+
+~~~ GetInputFlag = .false.
+
+~ ENDIF
+
+~ \textless{}\ldots{} insert any necessary code here\textgreater{}
+
+~ CALL Init\textless{}module\_name\textgreater{}(Args)
+
+~ CALL Calc\textless{}module\_name\textgreater{}(Args)
+
+~ CALL Update\textless{}module\_name\textgreater{}(Args)
+
+~ CALL Report\textless{}module\_name\textgreater{}(Args)
+
+~ RETURN
+
+\textbf{END SUBROUTINE Sim\textless{}module\_name\textgreater{}}
+
+\textbf{SUBROUTINE Get\textless{}module\_name\textgreater{}Input}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ \textless{}author\textgreater{}
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ \textless{}date\_written\textgreater{}
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~ USE InputProcessor, ONLY: GetNumObjectsFound, GetObjectItem ! might also use FindItemInList
+
+~ USE DataIPShortCuts
+
+~ IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~ CHARACTER(len = *), PARAMETER :: RoutineName = `PutRoutineNameHere'
+
+~ CHARACTER(len = *), PARAMETER :: CurrentModuleObject = `GetModuleObject'
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~ INTEGER~~~~~~~~~~~~~~~~~~~~~~~ :: Item~~~ ! Item to be ``gotten''
+
+~ !~ Instead of below, use Variables in IPShortCuts
+
+!~ CHARACTER(len = MaxNameLength), \&
+
+!~~~~~~~~~~~~~~~~~~~ DIMENSION(x) :: Alphas~ ! Alpha items for object
+
+!~ REAL, DIMENSION(y)~~~~~~~~~~~~ :: Numbers ! Numeric items for object
+
+~ INTEGER~~~~~~~~~~~~~~~~~~~~~~~ :: NumAlphas~ ! Number of Alphas for each GetObjectItem call
+
+~ INTEGER~~~~~~~~~~~~~~~~~~~~~~~ :: NumNumbers ! Number of Numbers for each GetObjectItem call
+
+~ INTEGER~~~~~~~~~~~~~~~~~~~~~~~ :: IOStatus~~ ! Used in GetObjectItem
+
+~ LOGICAL~~~~~~~~~~~~~~~~~~~~~~~ :: ErrorsFound = .false.~ ! Set to true if errors in input, fatal at end of routine
+
+~ \textless{}NumItems\textgreater{} = GetNumObjectsFound(CurrentModuleObject)
+
+~ DO Item = 1,\textless{}NumItems\textgreater{}
+
+~~~ CALL GetObjectItem(CurrentModuleObject,Item,cAlphaArgs,NumAlphas, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ rNumericArgs,NumNumbers,IOStatus,~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ AlphaBlank = lAlphaFieldBlanks,NumBlank = lNumericFieldBlanks,~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ AlphaFieldnames = cAlphaFieldNames,NumericFieldNames = cNumericFieldNames)
+
+~~~ \textless{}process, noting errors\textgreater{}
+
+~~~ ! Errors should be formatted as (alpha 1 should hold the name of the object)
+
+~~~ CALL ShowSevereError(RoutineName//`:'//CurrentModuleObject//' = ``'//trim(cAlphaArgs(1)))//~ \&
+
+~~~~~ `\,``, invalid '//trim(cAlphaFieldNames(x))//' =''\,'//trim(cAlphaArgs(x))//`" \textless{}condition\textgreater{}.')
+
+~~~ ! likewise for numeric fields
+
+~ ENDDO
+
+~ \textless{}SetupOutputVariables here\ldots{}\textgreater{}
+
+~ IF (ErrorsFound) THEN
+
+~~~ CALL ShowFatalError(RoutineName//`:'//CurrentModuleObject//`: Errors found in input.')
+
+~ ENDIF
+
+~ RETURN
+
+\textbf{END SUBROUTINE Get\textless{}module\_name\textgreater{}Input}
+
+\textbf{SUBROUTINE Init\textless{}module\_name\textgreater{}}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ \textless{}author\textgreater{}
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ \textless{}date\_written\textgreater{}
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~~~~~ ! na
+
+~ RETURN
+
+\textbf{END SUBROUTINE Init\textless{}module\_name\textgreater{}}
+
+\textbf{SUBROUTINE Size\textless{}module\_name\textgreater{}}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ \textless{}author\textgreater{}
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ \textless{}date\_written\textgreater{}
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~~~~~ ! na
+
+~ RETURN
+
+\textbf{END SUBROUTINE Size\textless{}module\_name\textgreater{}}
+
+\textbf{SUBROUTINE Calc\textless{}module\_name\textgreater{}}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ \textless{}author\textgreater{}
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ \textless{}date\_written\textgreater{}
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~~~~~ ! na
+
+~ RETURN
+
+\textbf{END SUBROUTINE Calc\textless{}module\_name\textgreater{}}
+
+\textbf{SUBROUTINE Update\textless{}module\_name\textgreater{}}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ \textless{}author\textgreater{}
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ \textless{}date\_written\textgreater{}
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~~~~~ ! na
+
+~ RETURN
+
+\textbf{END SUBROUTINE Update\textless{}module\_name\textgreater{}}
+
+\textbf{SUBROUTINE Report\textless{}module\_name\textgreater{}}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ \textless{}author\textgreater{}
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ \textless{}date\_written\textgreater{}
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! \textless{}description\textgreater{}
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~~~~~ ! na
+
+~! \textless{}this routine is typically needed only for those cases where you must transform the internal data to a reportable form\textgreater{}
+
+~ RETURN
+
+\textbf{END SUBROUTINE Report\textless{}module\_name\textgreater{}}
+
+\textbf{! = = = = = = = = = = = = = = = = = = = = = ~ Utility/Other routines for module.}
+
+! Insert as appropriate
+
+! Insert Standard Copyright Notice here.
+
+\textbf{END MODULE \textless{}module\_name\textgreater{}}
+
+The Subroutine Template:
+
+SUBROUTINE \textless{}name\textgreater{}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ \textless{}author\textgreater{}
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ \textless{}date\_written\textgreater{}
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! This subroutine needs a description.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! Needs description, as appropriate.
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~~~~~ ! na
+
+~ RETURN
+
+END SUBROUTINE \textless{}name\textgreater{}
+
+And the Function Template:
+
+\textless{}type\textgreater{} FUNCTION \textless{}name\textgreater{}
+
+~~~~~~~~~ ! FUNCTION INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ \textless{}author\textgreater{}
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ \textless{}date\_written\textgreater{}
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS FUNCTION:
+
+~~~~~~~~~ ! This function needs a description.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! Needs description, as appropriate.
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! FUNCTION ARGUMENT DEFINITIONS:
+
+~ ~~~~~~~~! na
+
+~~~~~~~~~ ! FUNCTION PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! FUNCTION LOCAL VARIABLE DECLARATIONS:
+
+~~~~~~~~~ ! na
+
+~ RETURN
+
+END FUNCTION \textless{}name\textgreater{}
diff --git a/doc/module-developer/src/appendix-e-test-file-documentation.tex b/doc/module-developer/src/appendix-e-test-file-documentation.tex
new file mode 100644
index 00000000000..3d0f6da5ac5
--- /dev/null
+++ b/doc/module-developer/src/appendix-e-test-file-documentation.tex
@@ -0,0 +1,97 @@
+\chapter{Appendix E.~ Test File Documentation}\label{appendix-e.-test-file-documentation}
+
+Each test file, whether released to the public or not, should be a best practice model and documented (comments at the top of the file) following the guidelines below.~ The document template file is also included with each installation in the ``ExampleFiles'' folder -- ExampleFilesDoc.txt
+
+! \textless{}name of file\textgreater{}
+
+! Basic file description: \textless{}specify number of zones, stories in building, etc\textgreater{}
+
+! Highlights: \textless{}Purpose of this example file\textgreater{}
+
+! Simulation Location/Run: \textless{}location information, design days, run periods\textgreater{}
+
+! Location:
+
+! Design Days (should have SummerDesignDay,WinterDesignDay designations):
+
+! Run Period (Weather File):
+
+! Run Control (should include this):
+
+!
+
+! Building: \textless{}more details about building.~ metric units, if also english enclose in {[}{]}\{\} or ()\textgreater{}
+
+! Floor Area:
+
+! Number of Stories:
+
+!
+
+! Zone Description Details:
+
+! Internal gains description: \textless{}lighting level, equipment, number of occupants, infiltration, daylighting, etc\textgreater{}
+
+! Interzone Surfaces:
+
+! Internal Mass:
+
+! People:
+
+! Lights:
+
+! Windows:
+
+! Detached Shading:
+
+! Daylight:
+
+! Natural Ventilation~~~~~~~~~ :
+
+! Compact Schedules (preferred):
+
+! Solar Distribution:
+
+!
+
+! HVAC: \textless{}HVAC description and plant supply, as appropriate\textgreater{}
+
+! Purchased Air:
+
+! Zonal Equipment:
+
+! Central Air Handling Equipment:
+
+! System Equipment Autosize:
+
+! Purchased Cooling:
+
+! Purchased Heating:
+
+! Coils:
+
+! Pumps:
+
+! Boilers:
+
+! Chillers:
+
+! Towers:
+
+!
+
+! Results: \textless{}how are results reported\textgreater{}
+
+! Standard Reports:
+
+! Timestep or Hourly Variables:
+
+! Time bins Report:
+
+! HTML Report:
+
+! Environmental Emissions:
+
+! Utility Tariffs:
+
+Most of the example files have completed their documentation requirements and include plan views of the building.~ Our naming convention uses an underscore (\_) as the first character of an input file ``not for publication''.
diff --git a/doc/module-developer/src/appendix-f-new-or-changed-proposal-feature.tex b/doc/module-developer/src/appendix-f-new-or-changed-proposal-feature.tex
new file mode 100644
index 00000000000..4c381e553c9
--- /dev/null
+++ b/doc/module-developer/src/appendix-f-new-or-changed-proposal-feature.tex
@@ -0,0 +1,57 @@
+\chapter{Appendix F. New or Changed Proposal Feature Template}\label{appendix-f.-new-or-changed-proposal-feature-template}
+
+\textless{}TITLE\textgreater{}
+
+\textless{}organization\textgreater{}
+
+\textless{}Date(s), Original, Revision, etc\textgreater{}
+
+\textbf{Justification for Feature Update:}
+
+\textless{}Required\textgreater{}
+
+\textbf{Conference Call Conclusions:}
+
+\textless{}Optional -- note date of conference call where talked about\textgreater{}
+
+\textbf{Other Conference Call Topics (not in scope of current proposal):}
+
+\textless{}Optional\textgreater{}
+
+\textbf{Overview:}
+
+\textless{}Include Description of Feature and references\textgreater{}
+
+\textbf{Approach:}
+
+\textbf{Testing/Validation/Data Source(s):}
+
+\textless{}required\textgreater{}
+
+\textbf{IO Ref (draft):}
+
+\textless{}required\textgreater{}
+
+\textbf{IDD Object (New):}
+
+\textless{}include as appropriate\textgreater{}
+
+\textbf{IDD Object(s) (Revised):}
+
+\textless{}include as appropriate\textgreater{}
+
+\textbf{Proposed Report Variables:}
+
+\textbf{Proposed additions to Meters:}
+
+\textbf{EngRef (draft):}
+
+\textless{}required\textgreater{}
+
+\textbf{Example File and Transition changes:}
+
+As needed.
+
+\textbf{Other documents:}
+
+As needed.
diff --git a/doc/module-developer/src/appendix-g.tex b/doc/module-developer/src/appendix-g.tex
new file mode 100644
index 00000000000..228559d05cf
--- /dev/null
+++ b/doc/module-developer/src/appendix-g.tex
@@ -0,0 +1 @@
+\chapter{Appendix G.}\label{appendix-g.}
diff --git a/doc/module-developer/src/energy-management-system.tex b/doc/module-developer/src/energy-management-system.tex
new file mode 100644
index 00000000000..b4387602ac8
--- /dev/null
+++ b/doc/module-developer/src/energy-management-system.tex
@@ -0,0 +1,3 @@
+\chapter{Energy Management System}\label{energy-management-system}
+
+The Energy Management System (EMS) feature in EnergyPlus is an advanced user feature that many users will not need (but may try anyway). Custom programming features are written in the EMS runtime language (Erl). Most of the features have been added to the modules as appropriate. Further ``actuators'' may need to be added (or desired to be added) and new component developers should review the following information and determine if actuators are useful for the component.
diff --git a/doc/module-developer/src/energy-management-system/ems-actuator-interface.tex b/doc/module-developer/src/energy-management-system/ems-actuator-interface.tex
new file mode 100644
index 00000000000..64a47ebd63c
--- /dev/null
+++ b/doc/module-developer/src/energy-management-system/ems-actuator-interface.tex
@@ -0,0 +1,71 @@
+\section{EMS Actuator Interface}\label{ems-actuator-interface}
+
+New component models may need to register certain control variables with the Energy Management System. In many cases, a component model will be controlled by setpoints placed on a system node, such as the component outlet, and the setpoints placed on the nodes can already be actuated by the EMS. But a given new component may have internal controls that should be made to work with EMS. When this is the case, the developer needs to register the control point as an actuator that EMS users can reference. The content of registered actuators is reported to the EDD file when EMS is used in a model and the Output:EnergyManagementSystem object is configured to do so.
+
+The EMS actuator interface is similar to SetupOutputVariable. Here is the syntax:
+
+CALL SetupEMSActuator(\textless{}component type\textgreater{}, \textless{}component unique name\textgreater{},
+
+~~~~~~ \textless{}control type name\textgreater{}, \textless{}units\textgreater{}, \textless{}logical variable on flag\textgreater{},
+
+~~~~~~ \textless{} variable to be controlled\textgreater{}~ )
+
+\textbf{\textless{}component type\textgreater{}}is a string representing the type of component or entity being registered. This is usually the class name of the IDF object. Or it could be another identifying string, if not directly associated with an object. For example the call to setup actuator for nodes uses ``System Node Setpoint.'
+
+\textbf{\textless{}component unique name\textgreater{}}is the local user-specified object name that identifies a unique instance among a set of the same or similar components.
+
+\textbf{\textless{}control type name\textgreater{}} is the string identifying the type of actuator. A model may have more than one type of control and this argument clarifys which one is being registered. A thermostat object could, for instance, have several actuators for that object type: ``On/Off'', ``Heating Set Point Temperature'', and ``Cooling Set Point Temperature''.
+
+~\textbf{\textless{}units\textgreater{}} is the string for the units of the control variable, used for reporting.
+
+~\textbf{\textless{}logical variable ON flag\textgreater{}} is a local variable attached to the object data structure that says whether or not the actuator value should be used (see below). This becomes a pointer in the EMS data structure so that the EMS can set the value of this variable remotely. The variable type needs to be LOGICAL.
+
+~\textbf{\textless{}variable to be controlled\textgreater{}}~ is another variable attached to the object data structure that specifies the value or state of the actuator, used in conjunction with the flag above. Similar to above, this also becomes a pointer in the EMS data structure so that the EMS can set the value of this variable remotely. A Fortran INTERFACE is used to overload the call the SetupEMSActuator so that this can be either a real, integer, or logical value.
+
+However, it is not desirable to register EMS actuators in every simulation because if there is no use of the EMS then this just adds to memory and computation. Therefore, we wrap calls to SetupEMSActuator inside logical checks using a global variable called ``AnyEnergyManagementSystemInModel.''
+
+Here is an example to create an actuator that can set the power on EXTERIORLIGHTS:
+
+if (AnyEnergyManagementSystemInModel) Then
+
+~CALL SetupEMSActuator(`ExteriorLights', ExteriorLights(Item)\%Name, \&
+
+~~~ `Electric Power', `W',~ ExteriorLights(Item)\%PowerActuatorOn, \&
+
+~~~~ ExteriorLights(Item)\%PowerActuatorValue)
+
+ENDIF
+
+Variables analogous to ``PowerActuatorOn'' and ``PowerActuatorValue'' are added to data structure for the component model.
+
+Code must then be written at the object or component level to react to the variables that are being actuated by the EMS Manager. Often it only requires one or two lines of code per actuator. ExteriorLights is particularly simple:
+
+~ IF (ExteriorLights(Item)\%PowerActuatorOn) THEN
+
+~~~ ExteriorLights(Item)\%Power = \&
+
+~~~~~~~~~~ ExteriorLights(Item)\%PowerActuatorValue
+
+~ END IF
+
+Finally, once SetupEMSActuator is called, several things happen:
+
+~ 1. Two pointers are created in the EMS Manager
+
+~ 2. The actuator is made available for use Erl programs.
+
+~ 3. The actuator name and associated information are logged in the EDD output file
+
+All of the available actuators that can be accessed are shown in the EDD output file. Like the RDD, the list changes depending on what objects you have in your input file.
+
+In addition to setting up actuators, component model developers can also register design data for components and systems to be made available for possible use in Erl programs. These are generally static data that do not vary across an environment period but might vary from one run to the next. These are registered using calls to SetupEMSInternalVariable such as:
+
+~~~~~ \textbf{CALL} SetupEMSInternalVariable(`Zone Floor Area', Zone(ZoneNum)\%Name, `{[}m2{]}', \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Zone(ZoneNum)\%FloorArea )
+
+~~~~~ \textbf{CALL} SetupEMSInternalVariable(`Zone Air Volume', Zone(ZoneNum)\%Name, `{[}m3{]}', \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Zone(ZoneNum)\%Volume )
+
+The calls to SetupEMSInternalVariable should also be protected by logic that uses the AnyEnergyManagementSystemInModel logic flag. The internal data available can also be listed in the EDD output file.
diff --git a/doc/module-developer/src/energyplus-calling-structure.tex b/doc/module-developer/src/energyplus-calling-structure.tex
new file mode 100644
index 00000000000..8a457057d0d
--- /dev/null
+++ b/doc/module-developer/src/energyplus-calling-structure.tex
@@ -0,0 +1 @@
+\chapter{EnergyPlus Calling Structure}\label{energyplus-calling-structure}
diff --git a/doc/module-developer/src/energyplus-calling-structure/air-system-calling-tree-schematic-not-all.tex b/doc/module-developer/src/energyplus-calling-structure/air-system-calling-tree-schematic-not-all.tex
new file mode 100644
index 00000000000..a6e98d49cfc
--- /dev/null
+++ b/doc/module-developer/src/energyplus-calling-structure/air-system-calling-tree-schematic-not-all.tex
@@ -0,0 +1,72 @@
+\section{Air System Calling Tree (schematic -- not all routines are shown)}\label{air-system-calling-tree-schematic-not-all-routines-are-shown}
+
+ManageAirLoops (in SimAirServingZones)
+
+\begin{itemize}
+\item
+  GetAirPathData~ (in SimAirServingZones)
+\item
+  InitAirLoops (in SimAirServingZones)
+\item
+  SimAirLoops (in SimAirServingZones)
+\item
+  SimAirLoopComponent (in SimAirServingZones)
+\item
+  UpdateBranchConnections (in SimAirServingZones)
+\item
+  ManageOutsideAirSystem (in MixedAir)
+\item
+  SimOutsideAirSys (in MixedAir)
+\item
+  SimOAController (in MixedAir)
+\item
+  SimOAComponent (in Mixed Air)
+\item
+  SimOAMixer (in MixedAir)
+\item
+  SimulateFanComponents(in FanSimulation; file HVACFanComponent)
+\item
+  SimulateWaterCoilComponents (in WaterCoilSimulation; file HVACWaterCoilComponent)
+\item
+  SimHeatRecovery (in HeatRecovery)
+\item
+  SimDesiccantDehumidifier (in DesiccantDehumidifiers)
+\item
+  SimulateFanComponents (in FanSimulation; file HVACFanComponent)
+\item
+  SimulateWaterCoilComponents (in WaterCoilSimulation; file HVACWaterCoilComponent)
+\item
+  SimulateHeatingCoilComponents (in HeatingCoils; file HVACHeatingCoils)
+\item
+  SimDXCoolingSystem (in HVACDXSystem)
+\item
+  SimFurnace (in Furnaces; file HVACFurnace)
+\item
+  SimHumidifier (in Humidifiers)
+\item
+  SimEvapCooler (in EvaporativeCoolers; file HVACEvapComponent)
+\item
+  SimDesiccantDehumidifier (in DesiccantDehumidifiers)
+\item
+  SimHeatRecovery (in HeatRecovery)
+\item
+  ManageControllers (in Controllers)
+\item
+  GetControllerInput (in Controllers)
+\item
+  InitController (in Controllers)
+\item
+  SimpleController (in Controllers)
+\item
+  LimitController (in Controllers)
+\item
+  UpdateController (in Controllers)
+\item
+  Report Controller (in Controllers)
+\item
+  ResolveSysFlow (in SimAirServingZones)
+\item
+  UpdateHVACInterface (in HVACInterfaceManager)
+\item
+  ReportAirLoops (in SimAirServingZones)
+\end{itemize}
diff --git a/doc/module-developer/src/energyplus-calling-structure/high-level-hvac-calling-tree-schematic-not.tex b/doc/module-developer/src/energyplus-calling-structure/high-level-hvac-calling-tree-schematic-not.tex
new file mode 100644
index 00000000000..8e6cddf4aa8
--- /dev/null
+++ b/doc/module-developer/src/energyplus-calling-structure/high-level-hvac-calling-tree-schematic-not.tex
@@ -0,0 +1,36 @@
+\section{High Level HVAC Calling Tree (schematic -- not all routines are shown)}\label{high-level-hvac-calling-tree-schematic-not-all-routines-are-shown}
+
+ManageHVAC (in HVACManager)
+
+\begin{itemize}
+\tightlist
+\item
+  ZoneAirUpdate(`PREDICT', . . .) (in HVACManager)
+\end{itemize}
+
+\emph{estimate the zone heating or cooling demand}
+
+\emph{~}
+
+\begin{itemize}
+\item
+  SimHVAC (in HVACManager)
+\item
+  ManageSetPoints (in SetPointManager)
+\item
+  SimSelectedEquipment (in HVACManager)
+\item
+  ManageAirLoops (in SimAirServingZones)
+\item
+  ManageZoneEquipment (in ZoneEquipmentManager)
+\item
+  ManageElectricLoadCenters (in ElectricPowerManager)
+\item
+  ManagePlantLoops (in PlantManager)
+\item
+  ZoneAirUpdate(`CORRECT', . . .) (in HVACManager)
+\end{itemize}
+
+From the amount of heating and cooling actually provided by the HVAC system, calculate the zone temperatures.
+
+Each of the ``Manage'' routines has a different structure, since the simulation to be performed is different in each case.~ We will show schematic calling trees for several of the ``Manage'' routines.
diff --git a/doc/module-developer/src/energyplus-calling-structure/inserting-the-new-module-into-the-program.tex b/doc/module-developer/src/energyplus-calling-structure/inserting-the-new-module-into-the-program.tex
new file mode 100644
index 00000000000..f1b05937a2c
--- /dev/null
+++ b/doc/module-developer/src/energyplus-calling-structure/inserting-the-new-module-into-the-program.tex
@@ -0,0 +1,163 @@
+\section{Inserting the New Module into the Program}\label{inserting-the-new-module-into-the-program}
+
+Let us return to our example new module NewHVACComponent.~ Since the module gets its own input and output, adding the NewHVACComponent model to the program simply means adding a call to the driver routine SimNewHVACComponent from the correct place in EnergyPlus.~ In the simplest case, there is only one location from which the driver routine should be called. In some cases, though, more than one HVAC simulation block will need to use the new component model.~ SimulateWaterCoilComponents, for instance, can be used in both zone equipment and air systems for heating, reheating and cooling coils. In the air system simulation it is called from two places: the main air system simulation, and the mixed air simulation -- the outside air duct might contain a separate cooling coil.
+
+Let us assume that the NewHVACComponent will be part of the air system -- perhaps it is a solid desiccant wheel.~ Examining the air system calling tree we see that SimAirLoopComponent is one routine that will invoke the new component, and - if we want the component to possibly be in the outside air stream -- then SimOAComponent is the other routine that will need to call the new component simulation. Generally, all that is involved is adding a new CASE statement to a Fortran SELECT construct.~ For instance in SimAirLoopComponent this would look like:
+
+SELECT CASE(CompType\_Num)
+
+~ CASE(OAMixer\_Num)~ ! `OUTSIDE AIR SYSTEM'
+
+~~~ CALL ManageOutsideAirSystem( \ldots{})
+
+! Fan Types for the air sys simulation
+
+~ CASE(Fan\_Simple\_CV)~ ! `FAN:SIMPLE:CONSTVOLUME'
+
+~~~ CALL SimulateFanComponents(\ldots{})
+
+~ CASE(Fan\_Simple\_VAV)~ ! `FAN:SIMPLE:VARIABLEVOLUME'
+
+~~~ CALL SimulateFanComponents(\ldots{})
+
+! Coil Types for the air sys simulation
+
+!~~~~~~~~~~~~~~~~~~~~~~~~ `COIL:DX:COOLINGHEATEXCHANGERASSISTED'
+
+~ CASE(DXCoil\_CoolingHXAsst)
+
+~~~~~ CALL SimHXAssistedCoolingCoil(\ldots{})
+
+!~~~~~~~~~~~~~~~~~~~~~~~~ `COIL:WATER:COOLINGHEATEXCHANGERASSISTED'~ CASE(WaterCoil\_CoolingHXAsst)
+
+~~~ CALL SimHXAssistedCoolingCoil(\ldots{})
+
+~ CASE(WaterCoil\_SimpleHeat)~ ! `COIL:WATER:SIMPLEHEATING'
+
+~~~ CALL SimulateWaterCoilComponents(\ldots{})
+
+~ CASE(SteamCoil\_AirHeat)~ ! `COIL:STEAM:AIRHEATING'
+
+~~~ CALL SimulateSteamCoilComponents(\ldots{})
+
+~ CASE(WaterCoil\_DetailedCool)~ ! `COIL:WATER:DETAILEDFLATCOOLING'
+
+~~~ CALL SimulateWaterCoilComponents(\ldots{})
+
+~ CASE(WaterCoil\_Cooling)~ ! `COIL:WATER:COOLING'
+
+~~~ CALL SimulateWaterCoilComponents(\ldots{})
+
+~ CASE(Coil\_ElectricHeat)~ ! `COIL:ELECTRIC:HEATING'
+
+~~~ CALL SimulateHeatingCoilComponents(\ldots{})
+
+~ CASE(Coil\_GasHeat)~ ! `COIL:GAS:HEATING'
+
+~~~ CALL SimulateHeatingCoilComponents(\ldots{})
+
+! Heat reclaim
+
+~ CASE(Coil\_DeSuperHeat)~ ! `COIL:DESUPERHEATER:HEATING'
+
+~~~ CALL SimulateHeatingCoilComponents(\ldots{})
+
+~ CASE(DXSystem)~ ! `DXSYSTEM:AIRLOOP'
+
+~~~ CALL SimDXCoolingSystem(\ldots{})
+
+~ CASE(Furnace\_UnitarySys)~ ! `FURNACE:BLOWTHRU:HEATONLY',
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ ! `FURNACE:BLOWTHRU:HEATCOOL',
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ ! `UNITARYSYSTEM:BLOWTHRU:HEATONLY',
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ ! `UNITARYSYSTEM:BLOWTHRU:HEATCOOL'
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ ! `UNITARYSYSTEM:HEATPUMP:AIRTOAIR',
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ ! `UNITARYSYSTEM:HEATPUMP:WATERTOAIR'
+
+~~~ CALL SimFurnace(\ldots{})
+
+! Humidifier Types for the air system simulation
+
+~ CASE(Humidifier)~ ! `HUMIDIFIER:STEAM:ELECTRICAL'
+
+~~~ CALL SimHumidifier(\ldots{})
+
+! Evap Cooler Types for the air system simulation
+
+~ CASE(EvapCooler)~ ! `EVAPCOOLER:DIRECT:CELDEKPAD',
+
+~~~~~~~~~~~~~~~~~~~ ! `EVAPCOOLER:INDIRECT:CELDEKPAD'
+
+~~~~~~~~~~~~~~~~~~~ ! `EVAPCOOLER:INDIRECT:WETCOIL',
+
+~~~~~~~~~~~~~~~ ~~~~! `EVAPCOOLER:INDIRECT:RDDSPECIAL'
+
+~~~ CALL SimEvapCooler(\ldots{})
+
+! Desiccant Dehumidifier Types for the air system simulation
+
+~ CASE(Desiccant)~ ! `DESICCANT DEHUMIDIFIER:SOLID'
+
+~~~ CALL SimDesiccantDehumidifier(\ldots{})
+
+! Heat recovery
+
+~ CASE(HeatXchngr)~ ! `HEAT EXCHANGER:AIR TO AIR:FLAT PLATE'
+
+~~~ CALL SimHeatRecovery(\ldots{})
+
+! Ducts
+
+~ CASE(Duct)~ ! `DUCT'
+
+~~~ CALL SimDuct(\ldots{})
+
+\emph{! New HVAC Component}
+
+\emph{~ CASE (NewHVACCompNum) ! `NEW HVAC COMPONENT'}
+
+\emph{~~~ CALL SimNewHVACComponent(\ldots{})}
+
+~ DEFAULT
+
+END SELECT
+
+The new code is italicized.~ Do the same thing in SimOAComponent and you are done!~ Note that ``NEW HVAC COMPONENT'' is the class name (keyword) for the new component in the IDD file.~ The class names are converted to upper case in EnergyPlus, so the CASE statement must have the class name in upper case.~ The actual class name on the IDD file would probably be ``New HVAC Component''.
+
+If the new HVAC component is a piece of zone equipment -- a cooled beam system, for instance -- then the zone equipment calling tree indicates that the call to SimNewHVACComponent would be in SimZoneEquipment. If the new component is a gas fired absorption chiller, the call would be in SimPlantEquip.
+
+In every case, since NewHVACComponent is a new module, a USE statement must be added to the calling subroutine. For instance in SimAirLoopComponent this would look like:
+
+SUBROUTINE SimAirLoopComponent(CompType, CompName, FirstHVACIteration, LastSim)
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION
+
+~~~~~~~~~ !~~~~~~~~~~~~ AUTHOR:~ Russ Taylor, Dan Fisher, Fred Buhl
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN:~ Oct 1997
+
+~~~~~~~~~ !~~~~~~~~~~ MODIFIED:~ Dec 1997 Fred Buhl
+
+~~~~~~~~~ !~~~~~ RE-ENGINEERED:~ This is new code, not reengineered
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! Calls the individual air loop component simulation routines
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED: None
+
+~~~~~~~~~ ! REFERENCES: None
+
+~~~~~~~~~ ! USE Statements
+
+~ USE Fans,~~~~~~ Only:SimulateFanComponents
+
+~ USE WaterCoils, Only:SimulateWaterCoilComponents
+
+~ USE MixedAir,~~ Only:ManageOutsideAirSystem
+
+~ \emph{USE NewHVACComponent,~~~ Only:SimNewHVACComponent}
diff --git a/doc/module-developer/src/energyplus-calling-structure/plant-calling-tree-schematic-not-all-routines.tex b/doc/module-developer/src/energyplus-calling-structure/plant-calling-tree-schematic-not-all-routines.tex
new file mode 100644
index 00000000000..36173ba6231
--- /dev/null
+++ b/doc/module-developer/src/energyplus-calling-structure/plant-calling-tree-schematic-not-all-routines.tex
@@ -0,0 +1,42 @@
+\section{Plant Calling Tree (schematic -- not all routines are shown)}\label{plant-calling-tree-schematic-not-all-routines-are-shown}
+
+ManagePlantLoops (in PlantManager)
+
+\begin{itemize}
+\item
+  PlantHalfLoopSolver (in PlantLoopSolver)
+\item
+  InitLoadDistribution (in PlantCondLoopOperation)
+\item
+  SetupLoopFlowRequest (in PlantLoopSolver)
+\item
+  SimulateAllLoopSidePumps (in PlantLoopSolver)
+\item
+  SimulateAllLoopSideBranches (in PlantLoopSolver)
+\item
+  ManagePlantLoadDistribution (in PlantCondLoopOperation)
+\item
+  SimPlantEquip (in PlantLoopEquipment)
+\item
+  Component simulation routines (in various component models)
+\item
+  UpdateAnyLoopDemandAlterations (in PlantLoopSolver)
+\item
+  SimPressureDropSystem (in PlantPressureSystem)
+\item
+  ResolveParallelFlows (in PlantLoopSolver)
+\item
+  SimulateAllLoopSideBranches (in PlantLoopSolver)
+\item
+  ManagePlantLoadDistribution (in PlantCondLoopOperation)
+\item
+  SimPlantEquip (in PlantLoopEquipment)
+\item
+  Component simulation routines (in various component models)
+\item
+  UpdateAnyLoopDemandAlterations (in PlantLoopSolver)
+\item
+  SimPressureDropSystem (in PlantPressureSystem)
+\item
+  UpdatePlantLoopInterface (in HVACInterfaceManager)
+\end{itemize}
diff --git a/doc/module-developer/src/energyplus-calling-structure/top-level-calling-tree.tex b/doc/module-developer/src/energyplus-calling-structure/top-level-calling-tree.tex
new file mode 100644
index 00000000000..ce80a169d21
--- /dev/null
+++ b/doc/module-developer/src/energyplus-calling-structure/top-level-calling-tree.tex
@@ -0,0 +1,24 @@
+\section{Top Level Calling Tree}\label{top-level-calling-tree}
+
+EnergyPlus
+
+\begin{itemize}
+\item
+  ProcessInput (in InputProcessor)
+\item
+  ManageSimulation (in SimulationManager)
+\item
+  ManageWeather (in WeatherManager)
+\item
+  ManageHeatBalance (in HeatBalanceManager)
+\item
+  ManageSurfaceHeatBalance (in HeatBalanceSurfaceManager)
+\item
+  ManageAirHeatBalance (in HeatBalanceAirManager)
+\item
+  CalcHeatBalanceAir (in HeatBalanceAirManager)
+\item
+  ManageHVAC (in HVACManager)
+\end{itemize}
+
+The HVAC part of EnergyPlus is divided into a number of simulation blocks.~ At this point, there are blocks for the air system, the zone equipment, the plant equipment, and the on-site electrical equipment.~ There will be simulation blocks for waste heat supply and usage as well as electricity and gas.~ Within each HVAC time step, the blocks are simulated repeatedly until the conditions on each side of each block interface match up.~ The following calling tree represents the high level HVAC simulation structure.~ It is schematic -- not all routines are shown.
diff --git a/doc/module-developer/src/energyplus-calling-structure/zone-equipment-calling-tree-schematic-not-all.tex b/doc/module-developer/src/energyplus-calling-structure/zone-equipment-calling-tree-schematic-not-all.tex
new file mode 100644
index 00000000000..be6c9e69216
--- /dev/null
+++ b/doc/module-developer/src/energyplus-calling-structure/zone-equipment-calling-tree-schematic-not-all.tex
@@ -0,0 +1,106 @@
+\section{Zone Equipment Calling Tree (schematic -- not all routines are shown)}\label{zone-equipment-calling-tree-schematic-not-all-routines-are-shown}
+
+ManageZoneEquipment (in ZoneEquipmentManager)
+
+\begin{itemize}
+\item
+  GetZoneEquipment (in ZoneEquipmentManager)
+\item
+  InitZoneEquipment (in ZoneEquipmentManager)
+\item
+  SimZoneEquioment (in ZoneEquipmentManager)
+\item
+  SimAirLoopSplitter (in Splitters; file HVACSplitterComponent)
+\item
+  SimAirZonePlenum (in ZonePlenum; file ZonePlenumComponent)
+\item
+  SetZoneEquipSimOrder (in ZoneEquipmentManager)
+\item
+  InitSystemOutputRequired (in ZoneEquipmentManager)
+\item
+  ManageZoneAirLoopEquipment (in ZoneAirLoopEquipmentManager)
+\item
+  GetZoneAirLoopEquipment (in ZoneAirLoopEquipmentManager)
+\item
+  SimZoneAirLoopEquipment (in ZoneAirLoopEquipmentManager)
+\item
+  SimulateDualDuct (in DualDuct; file HVACDualDuctSystem)
+\item
+  GetDualDuctInput (in DualDuct; file HVACDualDuctSystem)
+\item
+  InitDualDuct (in DualDuct; file HVACDualDuctSystem)
+\item
+  SimDualDuctConstVol (in DualDuct; file HVACDualDuctSystem)
+\item
+  SimDualDuctVarVol (in DualDuct; file HVACDualDuctSystem)
+\item
+  UpdateDualDuct (in DualDuct; file HVACDualDuctSystem)
+\item
+  ReportDualDuct (in DualDuct; file HVACDualDuctSystem)
+\item
+  SimulateSingleDuct (in SingleDuct; file HVACSingleDuctSystem)
+\item
+  GetSysInput (in SingleDuct; file HVACSingleDuctSystem)
+\item
+  InitSys (in SingleDuct; file HVACSingleDuctSystem)
+\item
+  SimConstVol (in SingleDuct; file HVACSingleDuctSystem)
+\item
+  SimVAV (in SingleDuct; file HVACSingleDuctSystem)
+\item
+  ReportSys (in SingleDuct; file HVACSingleDuctSystem)
+\item
+  SimPIU (in PoweredInductionUnits)
+\item
+  GetPIUs (in PoweredInductionUnits)
+\item
+  InitPIUs (in PoweredInductionUnits)
+\item
+  CalcSeriesPIU (in PoweredInductionUnits)
+\item
+  CalcParallelPIU (in PoweredInductionUnits)
+\item
+  ReportPIU (in PoweredInductionUnits)
+\item
+  SimDirectAir (in DirectAirManager; file DirectAir)
+\item
+  SimPurchasedAir (in PurchasedAirManager)
+\item
+  SimWindowAC (in WindowAC)
+\item
+  SimFanCoilUnit (in FanCoilUnits)
+\item
+  SimUnitVentilator (in UnitVentilator)
+\item
+  SimUnitHeater (in UnitHeater)
+\item
+  SimBaseboard (in BaseboardRadiator)
+\item
+  SimHighTempRadiantSystem (in HighTempRadiantSystem; file RadiantSystemHighTemp)
+\item
+  SimLowTempRadiantSystem (in LowTempRadiantSystem; file RadiantSystemLowTemp)
+\item
+  SimulateFanComponents (in Fans; file HVACFanComponent)
+\item
+  SimHeatRecovery (in HeatRecovery)
+\item
+  UpdateSystemOutputRequired (in ZoneEquipmentManager)
+\item
+  SimAirLoopSplitter (in Splitters; file HVACSplitterComponent)
+\item
+  SimAirZonePlenum (in ZonePlenum; file ZonePlenumComponent)
+\item
+  CalcZoneMassBalance (in ZoneEquipmentManager)
+\item
+  CalcZoneLeavingConditions (in ZoneEquipmentManager)
+\item
+  SimReturnAirPath (in ReturnAirPathManager; file ReturnAirPath)
+\item
+  SimAirMixer (in Mixers; HVACMixerComponent)
+\item
+  SimAirZonePlenum (in ZonePlenum; file ZonePlenumComponent)
+\item
+  RecordZoneEquipment (in ZoneEquipmentManager)
+\item
+  ReportZoneEquipment (in ZoneEquipmentManager)
+\end{itemize}
diff --git a/doc/module-developer/src/energyplus-services.tex b/doc/module-developer/src/energyplus-services.tex
new file mode 100644
index 00000000000..298963f0c4a
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services.tex
@@ -0,0 +1,3 @@
+\chapter{EnergyPlus Services}\label{energyplus-services}
+
+EnergyPlus provides some standard services that make the developer's task much easier.~ The developer can concentrate on the new simulation algorithm rather than have to deal with details of input file structure, writing output, obtaining scheduled data, and accessing weather variables.
diff --git a/doc/module-developer/src/energyplus-services/branch-node-checking-and-services.tex b/doc/module-developer/src/energyplus-services/branch-node-checking-and-services.tex
new file mode 100644
index 00000000000..bc25b552a2e
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/branch-node-checking-and-services.tex
@@ -0,0 +1,934 @@
+\section{Branch \& Node Checking and Services}\label{branch-node-checking-and-services}
+
+\subsection{BranchInputManager}\label{branchinputmanager}
+
+For the most part, new modules do not use the BranchInputManager directly.~ Branches are ``gotten'' at a high management level.~ The main routines that might be used from the BranchInputManager are: NumBranchesInBranchList, GetBranchList and GetBranchData.~ The BranchInputManager also houses the Splitter and Mixer data: GetLoopSplitter and GetLoopMixer.
+
+\subsection{NumBranchesInBranchList}\label{numbranchesinbranchlist}
+
+This routine is used to get the number of branches in a branch list name (so that an appropriate array can be allocated).
+
+INTEGER FUNCTION NumBranchesInBranchList(BranchListName)
+
+An example of use:
+
+= = = Example = = =
+
+USE BranchInputManager, ONLY: NumBranchesInBranchList,. . .
+
+. . .
+
+PrimeAirSys(ASysNum)\%NumBranches = ~ \&
+
+~~~~~~~~~~~~~ \textbf{NumBranchesInBranchList}(BranchListName)
+
+IF (PrimeAirSys(ASysNum)\%NumBranches.EQ.0) THEN
+
+~ CALL ShowSevereError(`There must be at least 1 branch in system' \&
+
+~~~~~~~~~~~~~~~~~~ ~~~~~~//TRIM(PrimeAirSys(ASysNum)\%Name))
+
+~ ErrorsFound = .true.
+
+END IF
+
+ALLOCATE(BranchNames(PrimeAirSys(ASysNum)\%NumBranches))
+
+BranchNames = `'
+
+\subsection{GetBranchList}\label{getbranchlist}
+
+This routine is used to get the names of the branches on a Loop.
+
+SUBROUTINE GetBranchList(LoopName, BranchListName, NumBranchNames, BranchNames, LoopType)
+
+= = = Example = = =
+
+USE BranchInputManager, ONLY: GetBranchList, . . .
+
+. . .
+
+(NumBranches from NumBranchesInBranchList)
+
+! get the branch lists
+
+CALL \textbf{GetBranchList}(PrimeAirSys(ASysNum)\%Name,BranchListName, ~\&
+
+~~~~~~~ PrimeAirSys(ASysNum)\%NumBranches,BranchNames,`Air')
+
+ALLOCATE(PrimeAirSys(ASysNum)\%Branch(NumBranches))
+
+. . . . . . . .
+
+The first argument is the loop name, the 2\(^{nd}\) argument is the name of the Branch List, the 3\(^{rd}\) argument is an output: the number of branch names, the 4\(^{th}\) argument is an output: the names of the branches in the list, the 5\(^{th}\) argument is the loop type.
+
+\subsection{GetBranchData}\label{getbranchdata}
+
+This routine is used to get pieces of data about a branch.
+
+SUBROUTINE GetBranchData(LoopName, BranchName, BranchMaxFlow, NumComps, CompType, CompName, CompCtrlType, CompInletNodeNames, CompInletNodeNums, CompOutletNodeNames, CompOutletNodeNums, ErrorsFound)
+
+= = = Example = = =
+
+! Cycle through all of the branches and set up the branch data
+
+DO BNum = 1,PrimeAirSys(ASysNum)\%NumBranches
+
+~ PrimeAirSys(ASysNum)\%Branch(BNum)\%Name = BranchNames(BNum)
+
+~ NumBComps = NumCompsInBranch(BranchNames(BNum))
+
+~ ALLOCATE(CompTypes(NumBComps))
+
+~ CompTypes = `'
+
+~ ALLOCATE(CompNames(NumBComps))
+
+~ CompNames = `'
+
+~ ALLOCATE(CompCtrls(NumBComps))
+
+~ CompCtrls = `'
+
+~ ALLOCATE(InletNodeNames(NumBComps))
+
+~ InletNodeNames = `'
+
+~ ALLOCATE(InletNodeNumbers(NumBComps))
+
+~ InletNodeNumbers = 0
+
+~ ALLOCATE(OutletNodeNames(NumBComps))
+
+~ OutletNodeNames = `'
+
+~ ALLOCATE(OutletNodeNumbers(NumBComps))
+
+~ OutletNodeNumbers = 0
+
+~ CALL GetBranchData(PrimeAirSys(ASysNum)\%Name,~ \&
+
+~~~~ BranchNames(BNum),~~~~~~~~~~~~ \&
+
+~~~~ PrimeAirSys(ASysNum)\%Branch(BNum)\%MaxVolFlowRate, \&
+
+~~~~ NumBComps,~~~~~~~~~~~~~~~~~~ \&
+
+~~~~ CompTypes,CompNames,CompCtrls, ~~~~~\&
+
+~~~~ InletNodeNames,InletNodeNumbers,~~~ \&
+
+~~~~ OutletNodeNames,OutletNodeNumbers,ErrorsFound)
+
+~ ALLOCATE \&
+
+~(PrimeAirSys(ASysNum)\%Branch(BNum)\%Comp(NumBComps))
+
+~ PrimeAirSys(ASysNum)\%Branch(BNum)\%TotalComponents = ~ \&
+
+~~~~~~~~~~~~~~~~~~ NumBComps
+
+~~PrimeAirSys(ASysNum)\%Branch(BNum)\%TotalNodes = ~~ \&
+
+~~~~~~~~~~~~~~~~~~ NumBComps+1
+
+~ ALLOCATE (PrimeAirSys(ASysNum)\%Branch(BNum)\%NodeNum(NumBComps+1))
+
+~ PrimeAirSys(ASysNum)\%Branch(BNum)\%NodeNum(1) = ~~ \&
+
+~~~~~~~~~~~~~~~~~~ InletNodeNumbers(1)
+
+~ PrimeAirSys(ASysNum)\%Branch(BNum)\%DuctType = Main
+
+~ DO CNum = 1,PrimeAirSys(ASysNum)\%Branch(BNum)\%TotalComponents
+
+~~~ PrimeAirSys(ASysNum)\%Branch(BNum)\%Comp(CNum)\%TypeOf = \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ CompTypes(CNum)
+
+~~~ PrimeAirSys(ASysNum)\%Branch(BNum)\%Comp(CNum)\%Name~ = ~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ = CompNames(CNum)
+
+~~~ PrimeAirSys(ASysNum)\%Branch(BNum)\%Comp(CNum)\%Index = 0
+
+~~~ PrimeAirSys(ASysNum)\%Branch(BNum)\%Comp(CNum)\%FlowCtrl = \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ CompCtrls(CNum)
+
+~~~ PrimeAirSys(ASysNum)\%Branch(BNum)\%Comp(CNum)\%NodeNameIn = \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ InletNodeNames(CNum)
+
+~~~ PrimeAirSys(ASysNum)\%Branch(BNum)\%Comp(CNum)\%NodeNumIn = \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ InletNodeNumbers(CNum)
+
+~~~ PrimeAirSys(ASysNum)\%Branch(BNum)\%Comp(CNum)\%NodeNameOut = \&
+
+~~~~~~~ ~~~~~~~~~~~~~~~~~OutletNodeNames(CNum)
+
+~~~ PrimeAirSys(ASysNum)\%Branch(BNum)\%Comp(CNum)\%NodeNumOut = \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ OutletNodeNumbers(CNum)
+
+~~~ PrimeAirSys(ASysNum)\%Branch(BNum)\%NodeNum(CNum+1) = \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ OutletNodeNumbers(CNum)
+
+\subsection{NodeInputManager}\label{nodeinputmanager}
+
+The NodeInputManager is responsible for getting all the node names and assigning each a number.~ Node names are learned in random order -- which can make validation difficult.~ Internally nodes are referenced as number and should be integers in any data structure or reference.~ Two key routines are used for obtaining node numbers:~ GetOnlySingleNode and GetNodeNums.
+
+\subsection{Node Information Arguments}\label{node-information-arguments}
+
+Both routines need some extra information about the node as the number is obtained.This information is used to support fluid property calculations, the HVAC Diagram utility, and various diagnostic checks.
+
+\subsubsection{NodeFluidType}\label{nodefluidtype}
+
+This argument defines the type of fluid at this node such as air or water.~ The node fluid type is used for fluid property calculations and is reported in the list of nodes in the bnd output file.~~ Parameter definitions for this argument can be found in DataLoopNode.~ As of version 1.3, the list of valid choices is:
+
+~ ! Valid Fluid Types for Nodes
+
+~ INTEGER, PARAMETER :: NodeType\_Unknown = 0~ ! `blank'
+
+~ INTEGER, PARAMETER :: NodeType\_Air~~~~ = 1~ ! `Air'
+
+~ INTEGER, PARAMETER :: NodeType\_Water~~ = 2~ ! `Water'
+
+~ INTEGER, PARAMETER :: NodeType\_Steam~~ = 3~ ! `Steam'
+
+~ INTEGER, PARAMETER :: NodeType\_Electric = 4~ ! `Electric'
+
+~ CHARACTER(len = *), PARAMETER, DIMENSION(0:4) :: ValidNodeFluidTypes = ~ \&
+
+~~~~~~~~~~~~~~~~~~~~ (/`blank~~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `Air~~~~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `Water~~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `Steam~~',~ \&
+
+~~~~ ~~~~~~~~~~~~~~~~~~`Electric'/)
+
+~ INTEGER, PARAMETER :: NumValidNodeFluidTypes = 4
+
+Note that the argument passed in is an integer value -- you can ``USE DataLoopNode'' and use the above definitions (preferred over either defining your own or passing in a number).~ In many cases, a component may not know the fluid type.~ For example, most SET POINT MANAGERS are applicable to both air and water nodes.~ In this case, NodeType\_Unknown should be used.~ It is assumed that for any given node, at least one object referencing it will know the fluid type.~ Once a known fluid type is passed for a given node, it cannot be changed.~ All references to the same node must specify the same fluid type or unknown.~ When all input has been gotten, all node fluid types should be known, but this is not being validated currently.
+
+\subsubsection{NodeObjectType}\label{nodeobjecttype}
+
+This is the type of object which is referencing the node (e.g.~Chiller:Electric).~ This information is used to generate the list of Parent and Non-Parent Node Connections in the bnd output file.~ This list is used by the HVAC Diagram utility.
+
+\subsubsection{NodeObjectName}\label{nodeobjectname}
+
+This is the name of the object which is referencing the node (e.g.~My Chiller).~ This information is used to generate the list of Parent and Non-Parent Node Connections in the bnd output file.~ This list is used by the HVAC Diagram utility.
+
+\subsubsection{NodeConnectionType}\label{nodeconnectiontype}
+
+Parameter definitions for this argument can be found in DataLoopNode. .As of version 1.2.0, the current list of choices is:
+
+~ ! Valid Connection Types for Nodes
+
+~ CHARACTER(len = *), PARAMETER, DIMENSION(13) :: ValidConnectionTypes = ~ \&
+
+~~~~~~~~~~~~~~~~~~~~ (/`Inlet~~~~~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `Outlet~~~~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `Internal~~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `ZoneNode~~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `Sensor~~~~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `Actuator~~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `OutsideAir',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `ReliefAir~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `ZoneInlet~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `ZoneReturn',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `ZoneExhaust',~ \&
+
+~~~~~~~~~ ~~~~~~~~~~~~~`Setpoint~~',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `Electric~~'/)
+
+~ INTEGER, PARAMETER :: NumValidConnectionTypes = 13
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_Inlet = 1
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_Outlet = 2
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_Internal = 3
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_ZoneNode = 4
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_Sensor = 5
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_Actuator = 6
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_OutsideAir = 7
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_ReliefAir = 8
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_ZoneInlet = 9
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_ZoneReturn = 10
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_ZoneExhaust = 11
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_Setpoint = 12
+
+~ INTEGER, PARAMETER :: NodeConnectionType\_Electric = 13
+
+This information is used to generate the list of Parent and Non-Parent Node Connections in the bnd output file.~ This list is used by the HVAC Diagram utility.
+
+After all input has been gotten, node connection types are also validated in CheckNodeConnections in NodeInputManager according to the following rules. The rules are intended to catch user input errors without placing unnecessary constraints on system configurations. The validation checks are not exhaustive, so it is possible to pass all of the checks yet have a misconnected simulation. The main goal here is to prevent dangling nodes which do not behave as the user expects and can often go undetected without scrutinizing detailed outputs.
+
+\begin{itemize}
+\item
+  For any node which is used as an actuator, the same node must also be used at least once as a node type which is not sensor or actuator or outsideair.
+\item
+  For any node which is used as a setpoint, the same node must also be used at least once as a node type which is not a setpoint or outsideair.
+\item
+  Every ZoneInlet must appear as an outlet from something, otherwise it will do nothing.
+\item
+  Every ZoneExhaust must appear as an inlet to something, otherwise it will do nothing.
+\item
+  Every inlet node should match either an Outlet, ZoneReturn, ZoneExhaust, ReliefAir, or OutsideAir node, with the following exceptions:
+\item
+  If an InletNode's object is AIR PRIMARY LOOP, CONDENSER LOOP, or PLANT LOOP, then skip the test.
+\item
+  If an InletNode's object is not one of the above types, it is valid if the same node name appears as an INLET to an AIR PRIMARY LOOP, CONDENSER LOOP, or PLANT LOOP.
+\end{itemize}
+
+If a node fails any of the above tests, a severe error message is generated. If a new module generates unexpected errors, check the node connection types used by a similar module. \emph{If a given node is used in more than one way by an object, it may be necessary to register the node more than once by successive calls to GetOnlySingleNode or GetNodeNums with different arguments in each call.}
+
+NodeConnectionType\_OutsideAir is intended to specify nodes which are connected to the outside air.~ For example, OUTSIDE AIR MIXER has an Outside\_Air\_Stream\_Node which is registered as NodeConnectionType\_Inlet, because it may have other components such as a preheat coil between it and the outside air. Whichever node ultimately connects to the outside air in this case will be registered as NodeConnectionType\_OutsideAir by an OUTSIDE AIR INLET NODE LIST object.
+
+Some types of equipment take in outside air directly without relying on OUTSIDE AIR INLET NODE LIST to set the conditions on that node.~ For example, UNIT VENTILATOR and chillers with air cooled condensers do not require the use of an OUTSIDE AIR INLET NODE LIST. In these cases, the component registers the outside air node directly as NodeConnectionType\_OutsideAir. Given that the use of outside air nodes is not consistent throughout the code, it may be necessary at some point to relax or alter the validation rules associated with outside air nodes to accommodate a new type of module. Please consult with the team before changing these rules.
+
+\subsubsection{NodeFluidStream}\label{nodefluidstream}
+
+This is an integer indicating which fluid stream this node belongs to (1, 2, 3). For components with a single fluid stream, such as a fan, set this to one for the inlet and outlet nodes.~ For components with multiple fluid streams, such as a water coil, matching inlets and outlets should use the same fluid stream number.~ For example, the air inlet and air outlet would be stream 1, and the water inlet and water outlet would be stream 2. This information is used to generate the list of Parent and Non-Parent Node Connections in the bnd output file.~ This list is used by the HVAC Diagram utility.
+
+\subsubsection{ObjectIsParent}\label{objectisparent}
+
+True If the object is a parent object, false if not. Parameters are defined in DataLoopNode. As of version 1.2.0, the current list of choices is:
+
+~ ! Valid IsParent Types for Node Connections
+
+~ LOGICAL, PARAMETER :: ObjectIsParent = .TRUE.
+
+~ LOGICAL, PARAMETER :: ObjectIsNotParent = .FALSE.
+
+What is a parent object?~ A parent object is one which encloses and references other objects.~ For example, FAN COIL UNIT:4 PIPE is a parent to a fan, a heating coil, a cooling coil, and an outside air mixer. In most cases, all nodes referenced by a parent object are duplicated in the non-parent objects which are the components which ultimately act on the fluid stream. From the perspective of the HVAC Diagram utility, every fluid loop must be a continuous connection of non-parent objects and zones. In this example, the nodes of the mixer, fan, coils, and zone form a complete loop. Some components, such as UNIT VENTILATOR are part parent and part non-parent. It is a parent to a fan, a heating coil, and a cooling coil, but it does not reference an explicit outside air mixer. The mixer is an implied component within the unit ventilator. In these cases, to facilitate drawing a loop in HVAC Diagram, it is necessary to create a non-parent component to carry the fluid. So, the unit ventilator uses the following approach as illustrated by the comments and source code. Note that Alphas(3), the air inlet node, is registered twice, once as an inlet to parent object UNIT VENTILATOR, and once as an inlet to the implicit non-parent object UNIT VENTILATOR-OA MIXER.
+
+Excerpt from GetUnitVentilatorInput in UnitVentilator
+
+~~~~~~~~~ ! Main air nodes (except outside air node):
+
+~~~~~~~~~ ! For node connections, this object is both a parent and a non-parent, because the
+
+~~~~~~~~~ ! OA mixing box is not called out as a separate component, its nodes must be connected
+
+~~~~~~~~~ ! as ObjectIsNotParent.~ But for the fan and coils, the nodes are connected as ObjectIsParent
+
+~~~~~~~~~ ! To support the diagramming tool, the unit ventilator inlet node must appear both as
+
+~~~~~~~~~ ! an inlet to the unit ventilator parent object and as an inlet to the implied
+
+~~~~~~~~~ ! non-parent OA mixing box within the unit ventilator.
+
+~~~~~~~~~ ! Because there is overlap between the nodes that are parent and non-parent, use a different
+
+~~~~~~~~~ ! object type for the non parent nodes
+
+~~~ UnitVent(UnitVentNum)\%AirInNode = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(Alphas(3),ErrorsFound,`UNIT VENTILATOR',Alphas(1), \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsParent)
+
+~~~ UnitVent(UnitVentNum)\%AirInNode = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(Alphas(3),ErrorsFound,`UNIT VENTILATOR-OA MIXER',Alphas(1), \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsNotParent)
+
+~~~ UnitVent(UnitVentNum)\%AirOutNode = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(Alphas(4),ErrorsFound,`UNIT VENTILATOR',Alphas(1), \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Outlet,1,ObjectIsParent)
+
+~~~ UnitVent(UnitVentNum)\%FanOutletNode = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(Alphas(5),ErrorsFound,`UNIT VENTILATOR',Alphas(1), \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Internal,1,ObjectIsParent)
+
+\subsection{GetOnlySingleNode}\label{getonlysinglenode}
+
+This is used when only one node is expected as the input point.~ If this name points to a NodeList, an appropriate error message will be issued and errFlag (the second argument) will be set .true.
+
+\textbf{GetOnlySingleNode}(NodeName,errFlag,NodeObjectType,NodeObjectName,NodeFluidType,NodeConnectionType,NodeFluidStream,ObjectIsParent)
+
+It is used:
+
+Example:
+
+USE NodeInputManager, ONLY: GetOnlySingleNode
+
+. . .
+
+! get inlet node number
+
+Baseboard(BaseboardNum)\%WaterInletNode~ = \&
+
+~~~~~~~~~~~~~~ \textbf{GetOnlySingleNode}(AlphArray(3),ErrorsFound,~ \&
+
+~~~~~~~~~~~~~~~~~~~ `Baseboard Heater:Water:Convective',AlphArray(1), \&
+
+~~~~~ ~~~~~~~~~~~~~~~NodeType\_Water,NodeConnectionType\_Inlet,~ \&
+
+~~~~~~~~~~~~~~~~~~~~ 1,ObjectIsNotParent)
+
+! get outlet node number
+
+Baseboard(BaseboardNum)\%WaterOutletNode~ = \&
+
+~~~~~~~~~~~~~~ \textbf{GetOnlySingleNode}(AlphArray(4),ErrorsFound,~ \&
+
+~~~~~~~~~~~~~~~~~~~~ `Baseboard Heater:Water:Convective',AlphArray(1), \&
+
+~~~~~~~~~~~~~~~~~~~~~ NodeType\_Water,NodeConnectionType\_Outlet,~ \& ~~~~~~~~~~~~~~~~~~~~~ 1,ObjectIsNotParent)
+
+The first argument is the node name, the 2\(^{nd}\) argument is the error flag variable, the 3\(^{rd}\) argument is the object type, the 4\(^{th}\) argument is the object name -- the remainder arguments are as listed above.
+
+\subsection{GetNodeNums}\label{getnodenums}
+
+This is used when more than one node is valid for an input. Like the GetOnlySingleNode invocation, GetNodeNums needs the extra information for a node:
+
+SUBROUTINE GetNodeNums(Name,NumNodes,NodeNumbers,ErrorsFound,~ \&
+
+~~~~~~~~~~~~~~ NodeFluidType,NodeObjectType,NodeObjectName,~ \&
+
+~~~~~~~~~~~~~~ NodeConnectionType,NodeFluidStream,ObjectIsParent)
+
+Example:
+
+USE NodeInputManager, ONLY: GetNodeNums
+
+. . .
+
+CHARACTER(len = MaxNameLength), DIMENSION(4) :: AlphArray
+
+INTEGER :: NumNodes
+
+INTEGER, DIMENSION(25) :: NodeNums
+
+. . . . . . . .
+
+! Get the supply nodes
+
+ErrInList = .false.
+
+CALL \textbf{GetNodeNums}(Names(8),NumNodes,NodeNums,ErrInList,NodeType\_Air,~ \&
+
+~~~~~~~~~~~~~~~ `AIR PRIMARY LOOP',PrimaryAirSystem(AirSysNum)\%Name,~ \&
+
+~~~~~~~~~~~~~~~ NodeConnectionType\_Inlet,1,ObjectIsParent)
+
+IF (ErrInList) THEN
+
+~CALL ShowContinueError(`Invalid Node Name or Node List in Air System =' \&
+
+~~~~~~~~~~~~~~~~~~~~~~~ //TRIM(PrimaryAirSystem(AirSysNum)\%Name))
+
+~ErrorsFound = .true.
+
+ENDIF
+
+! Allow at most 3 supply nodes (for a 3 deck system)
+
+IF (NumNodes \textgreater{} 3) THEN
+
+~ CALL ShowSevereError(`Air System:Only 1st 3 Nodes will be used from:' \&
+
+~~~~~~~~~~~~~ ~~~~~~~~~~//TRIM(Names(8)))
+
+~ CALL ShowContinueError(`Occurs in Air System ='//~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ TRIM(PrimaryAirSystem(AirSysNum)\%Name))
+
+~ ErrorsFound = .true.
+
+ENDIF
+
+IF (NumNodes.EQ.0) THEN
+
+~ CALL ShowSevereError('Air System:there must be at least 1 `// \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `supply node in system'//TRIM(Names(1)))
+
+~ CALL ShowContinueError(`Occurs in Air System ='//~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ TRIM(PrimaryAirSystem(AirSysNum)\%Name))
+
+~ ErrorsFound = .true.
+
+END IF
+
+. . . . . . . .
+
+The first argument is a node name or the name of a Node List, the 2\(^{nd}\) argument is the number of nodes in the Node List (1 for a single node), the 3\(^{rd}\) argument is the output: a list of node numbers -- these are followed by the arguments shown above.
+
+\subsection{Unique Node Checking}\label{unique-node-checking}
+
+A set of routines will allow you to use the NodeInputManager to check for unique node names across a set of inputs.~ This is used currently in the CONTROLLED ZONE EQUIP CONFIGURATION object where each zone node mentioned must be unique.~ Three routines comprise the unique node check:~ InitUniqueNodeCheck, CheckUniqueNodes, EndUniqueNodeCheck
+
+\subsection{InitUniqueNodeCheck}\label{inituniquenodecheck}
+
+A call to this routine starts the collection and detection of unique/non-unique nodes by the NodeInputManager:
+
+USE NodeInputManager, ONLY: InitUniqueNodeCheck, CheckUniqueNodes, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ EndUniqueNodeCheck
+
+. . .
+
+CALL \textbf{InitUniqueNodeCheck}(`CONTROLLED ZONE EQUIP CONFIGURATION')
+
+The only argument is a simple string that will help with error messages that may come from the NodeInputManager.~ Unique node checking can only be done for one context (`CONTROLLED ZONE EQUIP CONFIGURATION') at a time.
+
+\subsection{CheckUniqueNodes}\label{checkuniquenodes}
+
+SUBROUTINE CheckUniqueNodes(NodeTypes,CheckType,ErrorsFound,~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ CheckName,CheckNumber)
+
+This is the routine called during the getting of the nodes.~ The CheckType argument can be `Nodename' or `NodeNumber' and then pass in the appropriate argument to CheckName or CheckNumber.~ CheckName and CheckNumber are optional arguments -- only the necessary one need be supplied.
+
+Argument 1, NodeTypes, is the type of node being looked for -- this argument is used for error messages within the NodeInput processing.~ Argument 2, ErrorsFound, will be set to true of this node is not unique in the current context.
+
+Example:
+
+~~~ UniqueNodeError = .false.
+
+~~~ CALL \textbf{CheckUniqueNodes}(`Zone Air Node',`NodeName',UniqueNodeError,~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~ CheckName = AlphArray(5))
+
+~~~ IF (UniqueNodeError) THEN
+
+~~~~~ CALL ShowContinueError(`Occurs for Zone ='//TRIM(AlphArray(1)))
+
+~~~~~ ErrorsFound = .true.
+
+~~~ ENDIF
+
+\subsection{EndUniqueNodeCheck}\label{enduniquenodecheck}
+
+This routine terminates the unique node check -- allows arrays to be deallocated, etc.
+
+CALL \textbf{EndUniqueNodeCheck}(`CONTROLLED ZONE EQUIP CONFIGURATION')
+
+The only argument is the Context String -- which must match the string given in the InitUniqueNodeCheck routine.
+
+\subsection{SetUpCompSets and TestCompSet}\label{setupcompsets-and-testcompset}
+
+SetUpCompSets and TestCompSet are used to develop a list of hierarchical relationships between HVAC objects.~ The CompSet routines are housed in the BranchInputManager.~ A list of component sets is built which contains the following information:
+
+Parent Object Type (Currently cannot be SPLITTER or MIXER)
+
+Parent Object Name
+
+Child Component Type (Currently cannot be SPLITTER or MIXER)
+
+Child Component Name
+
+Child Component InletNodeName
+
+Child Component OutletNodeName
+
+Node Description
+
+Parent and child refer to a hierarchical relationship of two HVAC objects.~ For example, a branch is the parent to a pump, and a fan coil is the parent to a fan.~ The component sets do not include peer-to-peer connections such as a splitter connected to a branch, or a zone supply air path connected to an air loop.
+
+The following rules apply to component sets:
+
+\begin{itemize}
+\item
+  Each parent/child component set is unique.~ The same pair of components should never appear in the component sets list more than once.
+\item
+  Each set of child component plus inlet and outlet nodes is unique.
+\item
+  Each child component must have a parent component.
+\item
+  A given component may appear in multiple component sets as a parent component.
+\item
+  A given component may appear in multiple component sets as a child component only if there is a different set of inlet/outlet nodes.~ \emph{(This was originally the intent, but some new components do not fit this rule well and it may need to be relaxed.)}
+\item
+  If a given node name appears more than once as an inlet node, the two components which use it must share a parent/child relationship.
+\item
+  If a given node name appears more than once as an outlet node, the two components which use it must share a parent/child relationship.
+\item
+  After the program has read all the input data, there should be no ``UNDEFINED'' values in the list of component sets.
+\end{itemize}
+
+When any of these rules are violated, a warning is issued indicating a possible node connection error.
+
+** Warning ** Potential Node Connection Error for object PIPE, name = CW\_BYPASS
+
+~~ **~~ \textsubscript{\textasciitilde{}}~~ **~~ Node Types are still UNDEFINED -- See Branch/Node Details file for further information
+
+~~ **~~ \textsubscript{\textasciitilde{}}~~ **~~ Inlet Node : CW\_BYPASS\_INLET
+
+~~ **~~ \textsubscript{\textasciitilde{}}~~ **~~ Outlet Node: CW\_BYPASS\_OUTLET
+
+The component sets are reported in the eplusout.bnd file:
+
+! \textless{}Component Set\textgreater{},\textless{}Component Set Count\textgreater{},\textless{}Parent Object Type\textgreater{},\textless{}Parent Object Name\textgreater{},\textless{}Component Type\textgreater{},\textless{}Component Name\textgreater{},\textless{}Inlet Node ID\textgreater{},\textless{}Outlet Node ID\textgreater{},\textless{}Description\textgreater{}
+
+~Component Set,1,BRANCH,COOLING SUPPLY INLET BRANCH,PUMP:VARIABLE SPEED,CHW CIRC PUMP,CHW SUPPLY INLET NODE,CHW PUMP OUTLET NODE,Water Nodes
+
+Component Set,21,FAN COIL UNIT:4 PIPE,ZONE1FANCOIL,FAN:SIMPLE:CONSTVOLUME,ZONE1FANCOILFAN,ZONE1FANCOILOAMIXEROUTLETNODE,ZONE1FANCOILFANOUTLETNODE,Air Nodes
+
+\subsubsection{SetUpCompSets}\label{setupcompsets}
+
+SetUpCompSets should be called any time a parent object such as a branch or a compound object (e.g.~furnace) references a child component which is connected to it.~ If an object has more than one child component, then SetUpCompSets is called once for each child.
+
+SetUpCompSets first looks for the child component in the existing list of component sets by looking for a matching component type and name.~ If it is found, then the parent name and type are filled in.~ If the child component is not found is the exisiting list, then a new component set is created.
+
+SUBROUTINE SetUpCompSets(ParentType,ParentName,CompType,CompName,InletNode,OutletNode,Description)
+
+The arguments are:
+
+ParentType ~~~ Parent Object Type
+
+ParentName ~ Parent Object Name
+
+CompType ~~~~ Child Component Type
+
+CompName ~~ Child Component Name
+
+InletNode ~~~~~~~ Child Component Inlet Node Name
+
+OutletNode ~~~~ Child Component Outlet Node Name
+
+Description~~~~~ Description of nodes (optional)
+
+For example, AirLoopHVAC:Unitary:Furnace:HeatOnly references a fan and a heating coil:
+
+\textbf{AirLoopHVAC:Unitary:Furnace:HeatOnly},
+
+~~~~~~~ \textbackslash{}memo identical to the AirLoopHVAC:UnitaryHeatOnly object
+
+~~~~~~~ \textbackslash{}min-fields 13
+
+~~ A1,~ \textbackslash{}field Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type alpha
+
+~~ A2,~ \textbackslash{}field Availability Schedule Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type object-list
+
+~~~~~~~ \textbackslash{}object-list ScheduleNames
+
+~~ A3,~ \textbackslash{}field Furnace Air Inlet Node Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type node
+
+~~ A4,~ \textbackslash{}field Furnace Air Outlet Node Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type node
+
+~~ A5,~ \textbackslash{}field Supply Air Fan Operating Mode Schedule Name
+
+~~~~~~~ \textbackslash{}type object-list
+
+~~~~~~~ \textbackslash{}object-list ScheduleNames
+
+~~~~~~~ \textbackslash{}note A fan operating mode schedule value of 0 indicates cycling fan mode (supply air
+
+~~~~~~~ \textbackslash{}note fan cycles on and off in tandem with the heating coil).
+
+~~~~~~~ \textbackslash{}note Any other schedule value indicates continuous fan mode (supply air fan operates
+
+~~~~~~~ \textbackslash{}note continuously regardless of heating coil operation).
+
+~~~~~~~ \textbackslash{}note Leaving this schedule name blank will default to cycling fan mode for the
+
+~~~~~~~ \textbackslash{}note entire simulation period.
+
+~~ N1,~ \textbackslash{}field Maximum Supply Air Temperature
+
+~~~~~~~ \textbackslash{}type real
+
+~~~~~~~ \textbackslash{}units C
+
+~~~~~~~ \textbackslash{}autosizable
+
+~~~~~~~ \textbackslash{}default 80.0
+
+~~ N2,~ \textbackslash{}field Supply Air Flow Rate
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type real
+
+~~~~~~~ \textbackslash{}note~ This value should be \textgreater{} 0 and \textless{} = than the fan air flow rate.
+
+~~~~~~~ \textbackslash{}units m3/s
+
+~~~~~~~ \textbackslash{}minimum\textgreater{} 0.0
+
+~~~~~~~ \textbackslash{}autosizable
+
+~~ A6,~ \textbackslash{}field Controlling Zone or Thermostat Location
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type object-list
+
+~~~~~~~ \textbackslash{}object-list ZoneNames
+
+~~ A7,~ \textbackslash{}field Supply Fan Object Type
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type choice
+
+~~~~~~~ \textbackslash{}key Fan:OnOff
+
+~~~~~~~ \textbackslash{}key Fan:ConstantVolume
+
+~~~~~~~ \textbackslash{}note Fan:ConstantVolume only works with continuous fan operating mode (i.e.~fan
+
+~~~~~~~ \textbackslash{}note operating mode schedule values are greater than 0).
+
+~~ A8,~ \textbackslash{}field Supply Fan Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type object-list
+
+~~~~~~~ \textbackslash{}object-list FansCVandOnOff
+
+~~ A9 , \textbackslash{}field Fan Placement
+
+~~~~~~~ \textbackslash{}type choice
+
+~~~~~~~ \textbackslash{}key BlowThrough
+
+~~~~~~~ \textbackslash{}key DrawThrough
+
+~~~~~~~ \textbackslash{}default BlowThrough
+
+~~ A10, \textbackslash{}field Heating Coil Object Type
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type choice
+
+~~~~~~~ \textbackslash{}key Coil:Heating:Gas
+
+~~~~~~~ \textbackslash{}key Coil:Heating:Electric
+
+~~~~~~~ \textbackslash{}key Coil:Heating:Water
+
+~~~~~~~ \textbackslash{}key Coil:Heating:Steam
+
+~~~~~~~ \textbackslash{}note works with gas, electric, hot water and steam heating coils
+
+~~ A11; \textbackslash{}field Heating Coil Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type object-list
+
+~~~~~~~ \textbackslash{}object-list HeatingCoilName
+
+In this case, the furnace is the parent object to the fan and the heating coil.~ To set up the component set for the furnace and its fan, the furnace type and name, the fan type and name (A7 and A8), and the furnace/fan inlet and fan outlet nodes (A3 and A9) are passed to SetUpCompSets:
+
+Example:
+
+USE BranchInputManager, ONLY: SetUpCompSets
+
+. . .
+
+CALL SetUpCompSets( Furnace(FurnaceNum)\%FurnaceType,Furnace(FurnaceNum)\%Name, AlphArray(7),AlphArray(8),AlphArray(3),AlphArray(9))
+
+In some cases, the inlet or outlet node names may not be known by the parent object.~ In this case, ``UNDEFINED'' is passed to SetUpCompSets.
+
+Examples:
+
+USE BranchInputManager, ONLY: SetUpCompSets
+
+. . .
+
+CALL SetUpCompSets( Furnace(FurnaceNum)\%FurnaceType,Furnace(FurnaceNum)\%Name, AlphArray(8),AlphArray(9),`UNDEFINED',`UNDEFINED')
+
+CALL SetUpCompSets( Furnace(FurnaceNum)\%FurnaceType,Furnace(FurnaceNum)\%Name, AlphArray(12),AlphArray(13),`UNDEFINED',AlphArray(4))
+
+\subsubsection{TestCompSet}\label{testcompset}
+
+TestCompSet should be called by every HVAC object which has a parent object.~ A given object may be both a parent and a child.~ For example, \textbf{AirLoopHVAC:Unitary:Furnace:HeatOnly} is a child to a branch and a parent to a fan and coils.
+
+TestCompSet first looks for the calling component in the existing list of component sets by looking for a matching component type and name.~ If the found compset has inlet and outlet nodes defined, then these must also match.~ If~ a match is found, then any undefined node names are filled in and the description string for the nodes is added.~ If the component is not found, then a new component set is created with undefined parent object type and name.
+
+SUBROUTINE TestCompSet(CompType,CompName,InletNode,OutletNode,Description)
+
+The arguments are:
+
+\begin{itemize}
+\item
+  CompType ~~~~~~~~~~ Child Component Type
+\item
+  CompName ~~~~~~~~ Child Component Name
+\item
+  InletNode ~ ~~~~~~~~~~~ Child Component Inlet Node Name
+\item
+  OutletNode ~~~~~~~~~~ Child Component Outlet Node Name
+\item
+  Description~~~~~~~~~~~ Description of nodes
+\end{itemize}
+
+For example, \textbf{AirLoopHVAC:Unitary:Furnace:HeatOnly} is a child component with inlet and outlet nodes:
+
+\textbf{AirLoopHVAC:Unitary:Furnace:HeatOnly,}
+
+~~~~~~~ \textbackslash{}memo identical to the AirLoopHVAC:UnitaryHeatOnly object
+
+~~~~~~~ \textbackslash{}min-fields 14
+
+~~ A1,~ \textbackslash{}field Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type alpha
+
+~~ A2,~ \textbackslash{}field Availability Schedule Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type object-list
+
+~~~~~~~ \textbackslash{}object-list ScheduleNames
+
+~~ A3,~ \textbackslash{}field Furnace Air Inlet Node Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type alpha
+
+~~ A4,~ \textbackslash{}field Furnace Air Outlet Node Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type alpha
+
+To register the component set for the furnace (as a child component), the furnace type and name, and the furnace inlet and outlet nodes (A3 and A4) along with a node descriptor are passed to TestCompSets:
+
+Example:
+
+USE BranchInputManager, ONLY: TestCompSet
+
+CALL TestCompSet (Furnace(FurnaceNum)\%FurnaceType,AlphArray(1), \&
+
+~~~~~~~~~~~~~~~~~ AlphArray(3),AlphArray(4),`Air Nodes')
+
+\subsection{CheckOutAirNodeNumber}\label{checkoutairnodenumber}
+
+Outside Air Nodes are special nodes connected to the outside environment.~ With the introduction of the Site Atmospheric Variation parameters, it becomes important to know whether the node name (e.g.~Condenser Inlet Node on Air Cooled Chillers) is a legitimate outside air node or not.~ CheckOutAirNodeNumber allows you to determine if an entered node is, in fact, a proper outside air node.
+
+Declaration:
+
+FUNCTION CheckOutAirNodeNumber(NodeNumber) RESULT(Okay)
+
+Example:
+
+USE OutAirNodeManager, ONLY: CheckOutAirNodeNumber
+
+! outdoor condenser node
+
+~ IF (lAlphaBlanks(10)) THEN
+
+~~~ DXCoil(DXCoilNum)\%CondenserInletNodeNum(1) = 0
+
+~ ELSE
+
+~~~ DXCoil(DXCoilNum)\%CondenserInletNodeNum(1) = \&
+
+~~~~ ~~GetOnlySingleNode(Alphas(10),ErrorsFound,TRIM(CurrentModuleObject),DXCoil(DXCoilNum)\%Name, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_OutsideAirReference,1,ObjectIsNotParent)
+
+~~~ IF (.not. CheckOutAirNodeNumber(DXCoil(DXCoilNum)\%CondenserInletNodeNum(1))) THEN
+
+~~~~~ CALL ShowWarningError(RoutineName//trim(CurrentModuleObject)//`= ``'//trim(DXCoil(DXCoilNum)\%Name)//''', may be invalid')
+
+~~~~~ CALL ShowContinueError(TRIM(cAlphaFields(10))//' = ``'//TRIM(Alphas(10))// \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ ~~~~'``, node does not appear in an OutdoorAir:NodeList or as an OutdoorAir:Node.')
+
+~~~~~ CALL ShowContinueError(`This node needs to be included in an air system or the coil model will not be valid' \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~ //`, and the simulation continues')
+
+~~~ END IF
+
+~ ENDIF
+
+Note that GetOnlySingleNode is used to get the proper node number, then the node number is used in the outside air node verification.
+
+\subsection{CheckAndAddAirNodeNumber}\label{checkandaddairnodenumber}
+
+Should you feel really nice about your users (or more likely be updating older code that may have allowed blanks in places that are properly outside air nodes), you can use the CheckAndAddAirNodeNumber routine to not only check to see if it is an outside air node but also add it at the same time.
+
+Declaration:
+
+SUBROUTINE CheckAndAddAirNodeNumber(NodeNumber,Okay)
+
+USE OutAirNodeManager, ONLY: CheckAndAddAirNodeNumber
+
+Example:
+
+ElectricChiller(ChillerNum)\%CondInletNodeNum~~~ = \&
+
+~GetOnlySingleNode(AlphArray(5),ErrorsFound,~ \&
+
+~~ `Chiller:Electric',AlphArray(1), NodeType\_Air, \&
+
+~~~ NodeConnectionType\_OutsideAirReference, 2, ObjectIsNotParent)
+
+CALL CheckAndAddAirNodeNumber(~ \&
+
+ElectricChiller(ChillerNum)\%CondInletNodeNum, \&
+
+Okay)
+
+IF (.not. Okay) THEN
+
+~ CALL ShowWarningError(`Chiller:Electric, Adding Outside Air Node ='//~ \&
+
+AlphArray(5)))
+
+ENDIF
+
+Note that here ``not Okay'' is not an error condition but rather the opportunity to notify the user that you are adding an air node.
diff --git a/doc/module-developer/src/energyplus-services/data-services.tex b/doc/module-developer/src/energyplus-services/data-services.tex
new file mode 100644
index 00000000000..a22a57109df
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/data-services.tex
@@ -0,0 +1,105 @@
+\section{Data Services}\label{data-services}
+
+For the most part, modules are independent and only need the data they have within or \textbf{USE} from other modules.~ Occasionally, this may take on more complicated needs such as accessing ``real-time'' values for meters and/or custom meters or current report variable names/values..~ Meter names are standard; you may have to use user input to get custom meter names.
+
+\subsection{Global variable: MetersHaveBeenInitialized}\label{global-variable-metershavebeeninitialized}
+
+Meters are a bit peculiar and aren't fully set until the first run through the first time step of the HVAC simulation.~ Therefore, there is a global variable ``MetersHaveBeenInitialized'' which is set to \textbf{true} after meters have been set up.~ If you have a call to your routine that must use meter values as part of the simulation, you must use this variable before your items can be set.
+
+Example:
+
+\ldots{}
+
+If (MetersHaveBeenInitialized) CALL ManageDemand
+
+Only the first time step will be missed in your routine and that time step will be part of ``warming up'' the simulation, so there is minimal impact due to this limitation.
+
+\subsection{GetMeterIndex}\label{getmeterindex}
+
+You use the GetMeterIndex to check if a meter is valid for a particular simulation or if the user has entered a custom meter of that name.~ You use the index returned in later calls to get the value of the meter.~ Returns 0 if there is no meter of that name.
+
+Example:
+
+INTEGER, EXTERNAL :: GetMeterIndex
+
+\ldots{}
+
+thismeter = GetMeterIndex(`Electricity:Facility')
+
+\subsection{GetVariableKeyCountAndType}\label{getvariablekeycountandtype}
+
+This subroutine returns the variable type (real, integer, meter, etc.) (varType) whether it is an averaged or summed variable (varAvgSum), whether it is a zone or HVAC time step (varStepType), and the number of keynames for a given report variable or report meter name (varName).~ The variable type (varType) and number of keys (numKeys) are used when calling subroutine GetVariableKeys to obtain a list of the keynames for a particular variable and a corresponding list of indexes.~ An INTERFACE statement exists in the module OPInterfaces.
+
+Declaration:
+
+SUBROUTINE GetVariableKeyCountandType(varName, numKeys, varType,~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ varAvgSum, varStepType, varUnits)
+
+Example:
+
+USE OPInterfaces, ONLY: GetVariableKeyCountAndType
+
+~~~ ! call the key count function but only need count during this pass
+
+~~~ CALL GetVariableKeyCountandType(AlphArray(fldIndex),~ \&
+
+~~~~~~~~~~~~~~~~ KeyCount,TypeVar,AvgSumVar,StepTypeVar,UnitsVar)
+
+~~~ ALLOCATE(NamesOfKeys(KeyCount))
+
+~~~ ALLOCATE(IndexesForKeyVar(KeyCount))
+
+\subsection{GetVariableKeys}\label{getvariablekeys}
+
+This subroutine returns a list of keynames and indexes associated with a particular report variable or report meter name (varName). This routine assumes that the variable type (real, integer, meter, etc.) may be determined by calling GetVariableKeyCountandType.~ The variable type and index can then be used with function GetInternalVariableValue to to retrieve the current value of a particular variable/keyname combination. ~An INTERFACE statement exists in the module OPInterfaces.
+
+Declaration:
+
+SUBROUTINE GetVariableKeys(varName,varType,keyNames,keyVarIndexes)
+
+Example:
+
+USE OPInterfaces, ONLY: GetVariableKeys
+
+CALL GetVariableKeys(AlphArray(fldIndex), TypeVar, NamesOfKeys,~ \&
+
+~~~~~~~~~~~~~~~~~~~ IndexesForKeyVar)
+
+! See earlier GetVariableKeyCountandType as well.
+
+\subsection{GetCurrentMeterValue}\label{getcurrentmetervalue}
+
+You use the GetCurrentMeterValue to obtain the value of a meter at its last ``reported value'' (timestep).~ Note that all meters are reported on the zone time step.~ Returns 0.0 if the MeterNumber passed is \textless{} = 0.
+
+Example:
+
+INTEGER, EXTERNAL :: GetCurrentMeterValue
+
+\ldots{}
+
+thismetervalue = GetCurrentMeterValue(ElecFacilityMtrIndex)
+
+\subsection{GetInstantMeterValue}\label{getinstantmetervalue}
+
+You use the GetInstantMeterValue to get a component of a meter's value by index type. The values returned are ``raw'' (that is, not weighted by time step values).~ In these calls, 1 is a zone time step index, 2 is a system time step index.
+
+Example:
+
+INTEGER, EXTERNAL :: GetInstantMeterValue
+
+\ldots{}
+
+FuelType\%ElecFacility = \&~~~ GetInstantMeterValue(FuelType\%ElecFacilityIndex,1)*FracTimeStepZone + \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ GetInstantMeterValue(FuelType\%ElecFacilityIndex,2)
+
+\subsection{GetInternalVariableValue}\label{getinternalvariablevalue}
+
+This function returns the current value of the Internal Variable assigned to the varType and keyVarIndex.~ Values may be accessed for real and integer report variables and meter variables.~ The variable type (varType) may be determined by calling subroutine and GetVariableKeyCountandType.~ The index (keyVarIndex) may be determined by calling subroutine GetVariableKeys. ~To use, there is an INTERFACE statement in DataGlobals.f90
+
+Example:
+
+USE DataGlobals, ONLY: GetInternalVariableValue
+
+~~~~~ curValue = GetInternalVariableValue(curTypeOfVar,curVarNum)
diff --git a/doc/module-developer/src/energyplus-services/display-strings.tex b/doc/module-developer/src/energyplus-services/display-strings.tex
new file mode 100644
index 00000000000..9c9ff9cc21c
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/display-strings.tex
@@ -0,0 +1,9 @@
+\section{Display Strings}\label{display-strings}
+
+Two display routines are useful for displaying to the ``run'' log the progress of the simulation.~ Since EnergyPlus usually runs as a ``console'' mode application, users may monitor progress of the simulation.~ Thus, at times it is useful to have messages displayed there.~ These should be minimal in number though can be used effectively during debugging of new modules.
+
+~ subroutine DisplayString(String)
+
+~ subroutine DisplayNumberandString(Number,String)
+
+The ``String'' parameters are normal strings.~ The ``Number'' parameter must be an integer.
diff --git a/doc/module-developer/src/energyplus-services/error-messages.tex b/doc/module-developer/src/energyplus-services/error-messages.tex
new file mode 100644
index 00000000000..bf636074ac5
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/error-messages.tex
@@ -0,0 +1,309 @@
+\section{Error Messages}\label{error-messages}
+
+Several error message routines are provided for the developer, indicating three different levels of error severity: Show\textbf{Fatal}Error, Show\textbf{Severe}Error, Show\textbf{Severe}Message, Show\textbf{Warning}Error and Show\textbf{Warning}Message. Each takes a string as an argument. The string is printed out as the message body on the file ``eplusout.err''. There are two additional optional arguments, which are file unit numbers on which the message will also be printed. In practice, most modules will not use either file unit number argument -- but the Input Processor may use these to make sure some files contain a notice. ~\textbf{ShowFatalError} causes the program to immediately abort.
+
+Two other error messages can be used to help make the error file more readable: ShowContinueError and ShowContinueErrorTimeStamp.~ Finally, another similar ShowMessage call can be used to display an informative string to the error file (eplusout.err).
+
+As indicated, all of the ``show'' error calls look the same:
+
+SUBROUTINE \textbf{\textless{}ErrorMessageCall\textgreater{}}(ErrorMessage,OutUnit1,OutUnit2)
+
+Or
+
+SUBROUTINE \textbf{ShowWarningError}(ErrorMessage,OutUnit1,OutUnit2)
+
+SUBROUTINE \textbf{ShowWarningMessage}(ErrorMessage,OutUnit1,OutUnit2)
+
+SUBROUTINE \textbf{ShowSevereError}(ErrorMessage,OutUnit1,OutUnit2)
+
+SUBROUTINE \textbf{ShowSevereMessage}(ErrorMessage,OutUnit1,OutUnit2)
+
+SUBROUTINE \textbf{ShowFatalError}(ErrorMessage,OutUnit1,OutUnit2)
+
+SUBROUTINE \textbf{ShowContinueError}(ErrorMessage,OutUnit1,OutUnit2)
+
+SUBROUTINE \textbf{ShowContinueErrorTimeStamp}(ErrorMessage,OutUnit1,OutUnit2)
+
+SUBROUTINE \textbf{ShowMessage}(Message,OutUnit1,OutUnit2)
+
+As stated previously, you would likely never use either of the optional ``OutUnit'' arguments.~ One use might be if you were, in addition to the normal EnergyPlus output files, writing your own output file that would be processed separately.
+
+Format of the error messages should be such that it makes it easy for the developer or user to realize the context of the error.~ Obviously, it is usually easier for the developer as he/she can search the code for the error string, but hard for many users.~ Current suggested format is to include the Module Name and/or the Routine name.~ (see section Standard Message Format for more details). This is particularly useful when two or more places in the code have the same main error string but may mean different things: where one might be in a Plant Loop context and the other in a Condenser Loop context, for example.
+
+Due to the optional parameters, Interface statements are set in DataGlobals and you must enter USE statements defining which of the error calls you wish to use.
+
+Example:
+
+USE DataGlobals, ONLY: ShowSevereError
+
+. . .
+
+IF (Construct(ConstrNum)\%LayerPoint(Layer) = = 0) THEN
+
+~~ CALL ShowSevereError(`Did not find matching material for construct ` \&
+
+~~~~~~~~~~~~~~~~~~~~~~~ //TRIM(Construct(ConstrNum)\%Name)// \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `, missing material = ` \&
+
+~~~~~~~~~~~~~~~~~~~~~~ //TRIM(ConstructAlphas(Layer)))
+
+~~ ErrorsFound = .true.
+
+ENDIF
+
+This code segment will produce (with proper conditions) the message onto the error file:
+
+** Warning ** Did not find matching material for construct XYZ, missing material = ABC
+
+The ShowContinueError is used in conjunction with either ShowSevereError or ShowWarningError.~ The ``\textsubscript{\textasciitilde{}}'' characters represent the continuation:
+
+** Warning ** The total number of floors, walls, roofs and internal mass surfaces in Zone ZONE ONE
+
+**~~ \textsubscript{\textasciitilde{}}~~ ** is \textless{} 6. This may cause an inaccurate zone heat balance calculation.
+
+** Warning ** No floor exists in Zone = ZONE ONE
+
+** Warning ** Surfaces in Zone = ``ZONE ONE'' do not define an enclosure.
+
+**~~ \textsubscript{\textasciitilde{}}~~ ** Number of surfaces is \textless{} = 4 in this zone. View factor reciprocity forced
+
+The ShowContinueError is particularly useful with some of the previous routines that, in addition to signaling an error, produce their own error message.~ For example, see the example code in the ValidateComponent excerpt above.~ Note that no ShowContinueError should be used with the ShowFatalError as it immediately terminates the program.~ Instead, a Severe-Continue-Fatal sequence should be used.
+
+Each GetInput routine is responsible for verifying its input.~ Rather than terminating with the first illegal value, however, it is better to have an ``ErrorsFound'' logical that gets set to true for error conditions during the main routine processing and terminates at the end of the GetInput routine.~ Of course during simulation, conditions should also be checked and terminated if necessary.~ Try to give the user as much information as possible with the set of error routine calls.
+
+Quite a complex message can be constructed using concatenation. These routines can also be used to output numeric fields by writing the numeric variables to a string variable, although this isn't very convenient.
+
+A good use of the ContinueErrorTimeStamp as well as ``counting'' errors is shown below:
+
+~~~~~ IF(OutDryBulbTemp .LT. 0.0) THEN
+
+~~~~~~~ CINErrCount1 = CINErrCount1+1
+
+~~~~~~~ IF (CINErrCount1 \textless{} 15) THEN
+
+~~~~~~~~~ CALL ShowWarningError('ElectricChillerModel:Air Cooled `// \&
+
+~~~~~~~~~~~~~~~ `Condenser Inlet Temperature below 0C')
+
+~~~~~~~~~ CALL ShowContinueErrorTimeStamp(`OutDoor Dry Bulb ='//~ \&
+
+~~~~~~~~~~~~~~~~~~~~~ TRIM(RoundSigDigits(OutDryBulbTemp,2)//`,'))
+
+~~~~~~~ ELSE
+
+~~~~~~~~~ IF (MOD(CINErrCount1,50) = = 0) THEN
+
+~~~~~~~~~~~ WRITE(CINCharErrOut,*) CINErrCount1
+
+~~~~~~~~~~~ CINCharErrOut = ADJUSTL(CINCharErrOut)
+
+~~~~~~~~~~~~~ CALL ShowWarningError('ElectricChillerModel:Air Cooled`// \&
+
+~~~~~~~~~~~~~~~~~~ `Condenser Inlet Temperature below 0C continues\ldots{}' \&
+
+~~~~~~~~~~ ~~~~~~~~//CINCharErrOut)
+
+~~~~~~~~~ ENDIF
+
+~~~~~~~ ENDIF
+
+~~~~~ ENDIF
+
+\subsection{ShowWarningError, ShowWarningMessage}\label{showwarningerror-showwarningmessage}
+
+Both of these calls produce messages onto the .err file that signal a warning:
+
+~~ ** Warning ** Processing Monthly Tabular Reports: PEAK SPACE GAINS
+
+The important difference between the two calls is that the ``Error'' call will incrase the ``number of warnings'' counter whereas the ``Message'' call does not incrase the counter.~ The ``Message'' call can, therefore, be used ro ``start'' off a recurring sequence without disturbing the total warning count.~ To do this, one would place the calls:
+
+CALL ShowWarningMessage(xxx)
+
+\textless{}more messages that describe the basic problem\textgreater{}
+
+CALL ShowRecurringWarningErrorAtEnd(xxx,msgindex)
+
+As indicated, this first call can also show significantly more information about the situation than will be captured by using the Recurring error sequence.
+
+\subsection{ShowSevereError, ShowSevereMessage}\label{showsevereerror-showseveremessage}
+
+Both of these calls produce messages onto the .err file that signal a warning:
+
+~~ ** Severe~ ** Node Connection Error, Node = ``SOFC AIR INLET NODE'', ZoneExhaust node did not find a matching inlet node.
+
+The important difference between the two calls is that the ``Error'' call will incrase the ``number of severe errors'' counter whereas the ``Message'' call does not incrase the counter.~ The ``Message'' call can, therefore, be used ro ``start'' off a recurring sequence without disturbing the total warning count.~ To do this, one would place the calls:
+
+CALL ShowSevereMessage(xxx)
+
+\textless{}more messages that describe the basic problem\textgreater{}
+
+CALL ShowRecurringSevereErrorAtEnd(xxx,msgindex)
+
+As indicated, this first call can also show significantly more information about the situation than will be captured by using the Recurring error sequence.
+
+\subsection{ShowFatalError}\label{showfatalerror}
+
+This error terminates the program.
+
+~~ **~ Fatal~ ** EMS user program halted simulation with error code = 9001.30
+
+For clarity, the sequence ending in the fatal error, should start with a Severe error and give the user a good indication of the problem.~ During execution, this Severe error may immediately preceed the Fata call. During get input, errors may be found previously in the input, interspersed with Warning errors.~ The last Severe error is stored and displayed as the program terminates.
+
+\subsection{ShowContinueError, ShowContinueErrorTimeStamp}\label{showcontinueerror-showcontinueerrortimestamp}
+
+Continue errors are shown after the initial condition and formatted in a fashion that a post processor could detect and string all the errors about a single condition together.
+
+The basic format is simple:
+
+~~ **~~ \textsubscript{\textasciitilde{}}~~ ** ..Location object = DENVER STAPLETON INTL ARPT CO USA WMO = 724690
+
+The continue error with time stemp adds the time stamp information to the initial message. (It also might show if the error occurred during ``warmup'').
+
+~~ **~~ \textsubscript{\textasciitilde{}}~~ **~ CalcMultiSpeedDXCoil:lowspeedoutlet Occurrence info = Chicago Ohare Intl Ap IL USA TMY3 WMO\# = 725300, 04/24 15:45 - 16:00
+
+\subsection{ShowMessage}\label{showmessage}
+
+This call is strictly for informative messages that are displayed to the .err file. For example:
+
+~~ ************* Beginning Zone Sizing Calculations
+
+~~ ************* Beginning System Sizing Calculations
+
+~~ ************* Testing Individual Branch Integrity
+
+~~ ************* All Branches passed integrity testing
+
+The indicated messages help establish context for other errors that may be shown.
+
+\subsection{Recurring Error Handling}\label{recurring-error-handling}
+
+One method of showing recurring errors is shown in the initial error section description with the illustration of counting the number of times the error occurs, printing the first few times and then only printing every x times (e.g.~100) that it occurs after that.
+
+In addition to that method, three routines will help you automate the task.~ These routines rely on the error message being displayed and can also keep track of values (min/max/sum) (and units thereof). And an error message index (pointer to the message in the recurring error structure) that is stored in your data structure is used.
+
+SUBROUTINE ShowRecurringSevereErrorAtEnd(Message,MsgIndex,ReportMaxOf,ReportMinOf,ReportSumOf,~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ReportMaxUnits,ReportMinUnits,ReportSumUnits)
+
+SUBROUTINE ShowRecurringWarningErrorAtEnd(Message,MsgIndex,ReportMaxOf,ReportMinOf,ReportSumOf, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ReportMaxUnits,ReportMinUnits,ReportSumUnits)
+
+SUBROUTINE ShowRecurringContinueErrorAtEnd(Message,MsgIndex,ReportMaxOf,ReportMinOf,ReportSumOf, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ReportMaxUnits,ReportMinUnits,ReportSumUnits)
+
+The first two parameters (Message, MsgIndex) are required.~ The remaining six arguments (ReportMaxOf, ReportMinOf, ReportSumOf, ReportMaxUnits, ReportMinUnits, ReportSumUnits) are optional. To illustrate, we re-write the above call using the recurring error routines.~ (Note that we still do the first few counted because we are using the TimeStamp routine -- however a message buffer is set up in this instance.).
+
+!~~ Print warning messages only when valid and only for the first ocurrance. Let summary provide statistics.
+
+!~~ Wait for next time step to print warnings. If simulation iterates, print out
+
+!~~ the warning for the last iteration only. Must wait for next time step to accomplish this.
+
+!~~ If a warning occurs and the simulation down shifts, the warning is not valid.
+
+~~~ IF(CurrentEndTime .GT. CurrentEndTimeLast .AND. TimeStepSys .GE. TimeStepSysLast)THEN
+
+~~~~~ IF(ElectricChiller(ChillNum)\%PrintMessage)THEN
+
+~~~~~~~~~ ElectricChiller(ChillNum)\%MsgErrorCount = \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ ElectricChiller(ChillNum)\%MsgErrorCount + 1
+
+!~~~~~~ Show single warning and pass additional info to ShowRecurringWarningErrorAtEnd
+
+~~~~~~~ IF (ElectricChiller(ChillNum)\%MsgErrorCount \textless{} 2) THEN
+
+~~~~~~~~~~ CALL ShowWarningError(TRIM(ElectricChiller(ChillNum)\%MsgBuffer1)//`.')
+
+~~~~~~~~~~ CALL ShowContinueError(TRIM(ElectricChiller(ChillNum)\%MsgBuffer2))
+
+~~~~~~~ ELSE
+
+~~~~~~~~~ CALL ShowRecurringWarningErrorAtEnd(TRIM(ElectricChiller(ChillNum)\%MsgBuffer1)//`error continues.', \&
+
+~~~~~~~~~~~~ ElectricChiller(ChillNum)\%ErrCount1,ReportMaxOf = ElectricChiller(ChillNum)\%MsgDataLast,~ \&
+
+~~~~~~~~~~~~ ReportMinOf = ElectricChiller(ChillNum)\%MsgDataLast,ReportMaxUnits = `{[}C{]}',ReportMinUnits = `{[}C{]}')
+
+~~~~~~~ END IF
+
+~~~~~ END IF
+
+~~~ END IF
+
+Illustrations of use of these calls is seen in the Chiller modules, PurchasedAir modules, DXCoil modules and others.
+
+Another example is seen in the Dessicant routines:
+
+~ IF (Node(DesicDehum(DesicDehumNum)\%RegenAirInNode)\%MassFlowRate .NE. \&
+
+~~~~~~~~~~~~~~ RegenAirMassFlowRate) THEN
+
+~~~ ! Initialize standard air density
+
+~~~ IF (MyOneTimeFlag) THEN
+
+~~~~~ RhoAirStdInit = PsyRhoAirFnPbTdbW(StdBaroPress,20.0,0.0)
+
+~~~ ENDIF
+
+~~~ CALL \textbf{ShowRecurringSevereErrorAtEnd}( \&
+
+~~~~~ 'Improper flow delivered by desiccant regen fan - RESULTS INVALID!
+
+~~~~~~~~~~~~ Check regen fan capacity and schedule.', \&
+
+~~~~~~~~~~ DesicDehum(DesicDehumNum)\%RegenFanErrorIndex1)
+
+~~~ CALL \textbf{ShowRecurringContinueErrorAtEnd}( \&
+
+~~~~~~~~~~ TRIM(DesicDehum(DesicDehumNum)\%DehumType)//`='//~ \&
+
+~~~~~~~~~~~~ TRIM(DesicDehum(DesicDehumNum)\%Name), \&
+
+~~~~~~~~~~ DesicDehum(DesicDehumNum)\%RegenFanErrorIndex2)
+
+~~~ RhoAirStdInit = PsyRhoAirFnPbTdbW(StdBaroPress,20.0,0.0)
+
+~~~ CALL \textbf{ShowRecurringContinueErrorAtEnd}( \&
+
+~~~~~~~~~~ TRIM(`Flow requested {[}m3/s{]} from'//~ \&
+
+~~~~~~~~~~~ DesicDehum(DesicDehumNum)\%RegenFanType)//`='// \&
+
+~~~~~~~~~~ TRIM(DesicDehum(DesicDehumNum)\%RegenFanName), \&
+
+~~~~~~~~~~ DesicDehum(DesicDehumNum)\%RegenFanErrorIndex3, \&
+
+~~~~~~~~~~ \textbf{ReportMaxOf} = (RegenAirMassFlowRate / RhoAirStdInit))
+
+~~~ CALL \textbf{ShowRecurringContinueErrorAtEnd}( \&
+
+~~~~~~~~~~ `Flow request varied from delivered by {[}m3/s{]}', \&
+
+~~~~~~~~~~ DesicDehum(DesicDehumNum)\%RegenFanErrorIndex4, \&
+
+~~~ \textbf{ReportMaxOf} = ((RegenAirMassFlowRate - Node(DesicDehum(DesicDehumNum)\%RegenAirInNode)\%MassFlowRate)/ RhoAirStdInit), \&
+
+~~~ \textbf{ReportMinOf} = ((RegenAirMassFlowRate - Node(DesicDehum(DesicDehumNum)\%RegenAirInNode)\%MassFlowRate)/ RhoAirStdInit))
+
+~ ENDIF
+
+\subsection{Standard Message Format}\label{standard-message-format}
+
+With the advent of using the field names as provided from the Input Processor, some of the message formatting has gotten easier for the developer, but harder for the person who might be searching the code to determine a user's problem.
+
+Suggestion is that the error messages contain the Routine Name. And, for get input routines, the initial portion contain the Object Name and the Name of the object.~ For example,
+
+** Warning ** GetPlantLoopData/GetPlantAvailabilityManager: AvailabilityManagerAssignmentList = ALWAYS\_ON not found in lists.~ No availability will be used.
+
+Similarly, note that this is a summary message after surfaces have been gotten:
+
+** Warning ** GetSurfaceData:The total number of floors, walls, roofs and internal mass surfaces in Zone GARAGE ZONE
+
+**~~ \textsubscript{\textasciitilde{}}~~ ** is \textless{} 6. This may cause an inaccurate zone heat balance calculation.
+
+Not all of the code is using this style yet.
diff --git a/doc/module-developer/src/energyplus-services/fluid-property-services.tex b/doc/module-developer/src/energyplus-services/fluid-property-services.tex
new file mode 100644
index 00000000000..515ea44481d
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/fluid-property-services.tex
@@ -0,0 +1,573 @@
+\section{Fluid Property Services}\label{fluid-property-services}
+
+Fluid property routines have been implemented within EnergyPlus with the goal of making the specification of new fluids relatively easy for the user and not require the user to specify data for the most common loop fluids.~ Common refrigerants are listed within an extensive Reference Data Set (RDS) that is provided with the EnergyPlus program.
+
+Fluids in EnergyPlus are broken into two categories: \textbf{refrigerants} and \textbf{glycols}.~ This relates back to the amount of information needed to determine the properties of the various fluid types inside the program.~ The decision to define or use one class of fluids or another relates back to whether or not one expects the fluid to change phase (liquid and/or vapor) or remain a liquid.~ When a developer feels that a fluid may change phase, all code should access the Refrigerant class of fluid property routines.~ When the developer is certain that the fluid will remain a liquid and wishes to abide by that assumption (generally, this is the case for most larger loops), all code from such modules should access the Glycol class of fluid property routines.~ Each of these classes will be described in separate sections below since each class has different subroutine access to the main module.
+
+Internally, both the refrigerant and glycol classes of fluids use ``table lookup'' and interpolation to find the appropriate value of a fluid property.~ No curve fits are done internally and the interpolation search routines are currently not optimized (no interval halving or special fast searching techniques are used to find the values).
+
+HOWEVER, if values out of range (too low or too high) are passed to the routines, the value returned is a valid value at the lowest or highest (respectively) input parameter (that was passed in out of range).
+
+You will also note in the succeeding descriptions that IP units can be entered by some editors (IDF Editor) using predefined unit conversions.
+
+\subsection{Using Fluid Property Routines in EnergyPlus Modules}\label{using-fluid-property-routines-in-energyplus-modules}
+
+The routines are contained within a single module:\textbf{FluidProperties.f90}
+
+Developers can use the routines anywhere inside EnergyPlus through the following USE statement:
+
+\textbf{USE FluidProperties}
+
+Access to this module may be limited by expanding this line of code with the ONLY designator.
+
+\subsection{Fluid Properties Functions for Refrigerant Class Fluids}\label{fluid-properties-functions-for-refrigerant-class-fluids}
+
+In EnergyPlus, a refrigerant fluid is capable of being either in the liquid or vapor phase.~ Due to this definition, data must be available for both of these regions in order for the program to accurately calculate the various fluid properties.~ There are eight possible functions that may be used to obtain refrigerant data using the Fluid Properties module.~ They include:
+
+\textbf{GetSatPressureRefrig}(Refrigerant,Temperature,RefrigIndex,calledfrom)
+
+\textbf{GetSatTemperatureRefrig} (Refrigerant,Pressure,RefrigIndex,calledfrom)
+
+\textbf{GetSatEnthalpyRefrig} (Refrigerant,Temperature,Quality,RefrigIndex,calledfrom)
+
+\textbf{GetSatDensityRefrig} (Refrigerant,Temperature,Quality,RefrigIndex,calledfrom)
+
+\textbf{GetSatSpecificHeatRefrig} (Refrigerant,Temperature,Quality,RefrigIndex,calledfrom)
+
+\textbf{GetSupHeatEnthalpyRefrig} (Refrigerant,Temperature,Pressure,RefrigIndex,calledfrom)
+
+\textbf{GetSupHeatPressureRefrig} (Refrigerant,Temperature,Enthalpy,RefrigIndex,calledfrom)
+
+\textbf{GetSupHeatDensityRefrig} (Refrigerant,Temperature,Pressure,RefrigIndex,calledfrom)
+
+While most of the variables passed into the routine are self-explanatory, the three variables that are common to each of these functions are Refrigerant, RefrigIndex and calledfrom.~ \textbf{Refrigerant} in this case is the character string name of the refrigerant in question as listed in the input file using the FluidNames object.~ This must be passed into the function to identify the fluid being referenced.~ \textbf{RefrigIndex} is an internal variable.~ On the first call to the fluid property routine, it is zero.~ All of the fluid property routines are set-up to find a non-zero index in the local fluid property data structure that corresponds to this refrigerant name.~ Since finding the proper fluid from the fluid name each and every time is computationally slow, the index allows the code to quickly find the right data without doing an inordinate number of string comparisons.~ Thus, module developers should store the RefrigIndex in their own local data structure in addition to the refrigerant name. calledfrom is a string variable passed to the routine so that error messages coming from the above functions can give a better context for errors when they happen.
+
+Units for these other variables in these function calls are: Joules per kilogram for enthalpy, degrees Celsius for temperature, Pascals for pressure, kilograms per cubic meter for density, and Joules per kilogram-degree Celsius for specific heat.~ Quality and concentration are dimensionless fractions.~ All variables are considered input variables.
+
+Module developers should use the functions listed above to first determine whether they are in the saturated region or the superheated region.~ The GetSatPressureRefrig and GetSatTemperatureRefrig functions should assist the users in determining whether they are in or beyond the saturated region.~ Once this is determined, the developer can call the appropriate function to obtain the quantity of interest: in the saturated region this includes the enthalpy, density, or specific heat; in the superheated region this includes the enthalpy, pressure, or density.
+
+\subsection{Reference Data Set (RDS) Values for Refrigerant Class Fluids}\label{reference-data-set-rds-values-for-refrigerant-class-fluids}
+
+The data for refrigerants that are included in the reference data set that comes with EnergyPlus are as follows (temperatures in Celsius, pressure in MegaPascals):
+
+% table 3
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Regions for Fluid Properties \label{table:regions-for-fluid-properties}} \tabularnewline
+\toprule 
+Refrigerant & Sat. Temp range \{C\} & Super Temp range* \{C\} & Super Pressure range* \{Pa\} \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Regions for Fluid Properties} \tabularnewline
+\toprule 
+Refrigerant & Sat. Temp range \{C\} & Super Temp range* \{C\} & Super Pressure range* \{Pa\} \tabularnewline
+\midrule
+\endhead
+
+R11 & -110 to 198 & -110 to 255 & 6.8 to 1.6E6 \tabularnewline
+R11(specheat) & -110 to 190 & ~ & ~ \tabularnewline
+R12 & -157 to 112 & -156 to 169 & .3 to 1.6E7 \tabularnewline
+R12(specheat) & -157 to 104 & ~ & ~ \tabularnewline
+R22 & -157 to 96 & -157 to 153 & 0.4 to 1.7E7 \tabularnewline
+R22(specheat) & -157 to 88 & ~ & ~ \tabularnewline
+R123 & -107 to 184 & -106 to 240 & 4.9 to 1.5E7 \tabularnewline
+R134a & -103 to 101 & -103 to 158 & 400 to 1.6E7 \tabularnewline
+R404a & -72 to 72 & -72 to 72 & 2.3E4 to 3.7E6 \tabularnewline
+R410a & -72 to 69 & -72 to 69 & 3.1E4 to 4.7E6 \tabularnewline
+R507a & -72 to 69 & -72 to 69 & 2.5E4 to 3.6E6 \tabularnewline
+NH3 & -77 to 132 & -77 to 189 & 6.3E3 to 2.2E7 \tabularnewline
+NH3(specheat) & -73 to 124 & ~ & ~ \tabularnewline
+Steam & 0 to 370 & 0 to 500 & 610 to 4.0E8 \tabularnewline
+Steam(specheat) & 0 to 370 & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+*Obviously data for all temperatures at all pressures isn't loaded.~ The entire range of pressures given above will work, but the temperature range for a given pressure will be some subset of the Super Temp range shown above.
+
+Subcooled region actually only returns h(f) or the saturated liquid value at the temperature you input.
+
+\subsection{Fluid Property Data and Expanding the Refrigerants Available to EnergyPlus}\label{fluid-property-data-and-expanding-the-refrigerants-available-to-energyplus}
+
+The Fluid Property routines have been reengineered to allow other users to add refrigerants to the input file without having to make any changes to the program code.~ The only requirement on input is that in order to add a new refrigerant, a user must enter a full set of data.~ The exact definition of a full set of data is given below.
+
+As with all EnergyPlus input, the fluid properties data has both an input data description and a reference data set that must show up in the input file.~ All of the ``standard'' refrigerants listed above must show up in the in.idf file for it to be available to the rest of the simulation.~ Below is the description of the input data description syntax for the fluid properties entries.
+
+The first syntax item lists all of the fluids present in an input file and categorizes them as either a refrigerant (such as R11, R12, etc.) or a glycol (such as ethylene glycol, propylene glycol, etc.).~ A refrigerant or glycol must be in this list in order to be used as a valid fluid in other loops in the input file.
+
+\textbf{FluidProperties:Names,}
+
+~~~~~~ \textbackslash{}unique-object
+
+~~~~~~ \textbackslash{}extensible:2 repeat last two fields
+
+~~~~~~ \textbackslash{}memo list of potential fluid names/types in the input file, maximum of ten
+
+~ A1,~ \textbackslash{}field Fluid 1 Name
+
+~~~~~~ \textbackslash{}type alpha
+
+~ A2,~ \textbackslash{}field Fluid 1 Type
+
+~~~~~~ \textbackslash{}type choice
+
+~~~~~~ \textbackslash{}key Refrigerant
+
+~~~~~~ \textbackslash{}key Glycol
+
+~ A3,~ \textbackslash{}field Fluid 2 Name
+
+~~~~~~ \textbackslash{}type alpha
+
+~ A4,~ \textbackslash{}field Fluid 2 Type
+
+~~~~~~ \textbackslash{}type choice
+
+~~~~~~ \textbackslash{}key Refrigerant
+
+~~~~~~ \textbackslash{}key Glycol
+
+~ A5,~ \textbackslash{}field Fluid 3 Name
+
+~~~~~~ \textbackslash{}type alpha
+
+~ A6,~ \textbackslash{}field Fluid 3 Type
+
+~~~~~~ \textbackslash{}type choice
+
+~~~~~~ \textbackslash{}key Refrigerant
+
+~~~~~~ \textbackslash{}key Glycol
+
+An example of this statement in an input data file is:
+
+FluidProperties:Names,
+
+~ R11, REFRIGERANT,
+
+~ R12, REFRIGERANT,
+
+~ R22, REFRIGERANT,
+
+~ NH3, REFRIGERANT,
+
+~ Steam, REFRIGERANT,
+
+~ NewGlycol, GLYCOL,
+
+~ SuperGlycol, GLYCOL;
+
+All fluid properties vary with temperature.~ As a result, the following syntax allows the user to list the temperatures at which the data points are valid.~ Since in many cases, the temperatures will be similar, this provides a more compact input structure and avoids listing the temperatures multiple times.~ The name associated with the temperature list is the piece of information that will allow the actual fluid property data statements to refer back to or link to the temperatures.~ Up to 250 points may be entered with this syntax and temperatures must be entered in ascending order.~ Units for the temperatures are degrees Celsius.~ The same temperature list may be used by more than one refrigerant.
+
+\textbf{FluidProperties:Temperatures,}
+
+~~~~~ \textbackslash{}memo property values for fluid properties
+
+~~~~~ \textbackslash{}memo list of up to 250 temperatures, note that number of property values must match the number of properties
+
+~~~~~ \textbackslash{}memo in other words, there must be a one-to-one correspondence between the property values in this list and
+
+~~~~~ \textbackslash{}memo the actual properties list in other syntax
+
+~~~~~ \textbackslash{}memo degrees C (for all temperature inputs)
+
+~~~~~ \textbackslash{}format FluidProperty
+
+~ A1, \textbackslash{}field Name
+
+~~~~~ \textbackslash{}type alpha
+
+~ N1, \textbackslash{}field Temperature 1
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}units C
+
+\textless{} same thing repeated over and over again\textgreater{}
+
+~ N250; \textbackslash{}field Temperature 250
+
+~~~~~~~ \textbackslash{}type real
+
+An example of this statement in an input data file is:
+
+FluidProperties:Temperatures,
+
+~~~~~ R11Temperatures,
+
+~~~~~ -70,-65,-60,-55,-50,-45,-40,-35,-30,-25,-20,-15,-10,-5,0,2,4,6,8,10,12,14,16,18,
+
+~~~~~ 20,22,24,26,28,30,32,34,36,38,40,42,44,46,48,50,55,60,65,70,75,80,85,90,95,100,
+
+~~~~~ 105,110,115,120,125,130,135,140,145,150,155,160,165,170,175,180,185,190,198;
+
+Property data for the saturated region is entered with the following syntax.~ Before the actual data is entered, this line of input must identify the refrigerant the data is to be associated with, what the data represents (choice of one of three keywords), the phase of the data (either fluid or gas), and the temperature list reference that links each data point with a temperature.
+
+\textbf{FluidProperties:Saturated,}
+
+~~~~~ \textbackslash{}memo fluid properties for the saturated region
+
+~~~~~ \textbackslash{}format FluidProperty
+
+~ A1, \textbackslash{}field Name
+
+~~~~~ \textbackslash{}type object-list
+
+~~~~~ \textbackslash{}object-list FluidNames
+
+~ A2, \textbackslash{}field Fluid Property Type
+
+~~~~~ \textbackslash{}note Enthalpy Units are J/kg
+
+~~~~~ \textbackslash{}note Density Units are kg/m3
+
+~~~~~ \textbackslash{}note SpecificHeat Units are J/kg-K
+
+~~~~~ \textbackslash{}note Pressure Units are Pa
+
+~~~~~ \textbackslash{}type choice
+
+~~~~~ \textbackslash{}key Enthalpy~~~~ ! Units are J/kg
+
+~~~~~ \textbackslash{}key Density~~~~~ ! Units are kg/m3
+
+~~~~~ \textbackslash{}key SpecificHeat ! Units are J/kg-K
+
+~~~~~ \textbackslash{}key Pressure~~~~ ! Units are Pa
+
+~ A3, \textbackslash{}field Fluid Phase
+
+~~~~~ \textbackslash{}note Fluid = saturated fluid
+
+~~~~~ \textbackslash{}note FluidGas = saturated vapor
+
+~~~~~ \textbackslash{}type choice
+
+~~~~~ \textbackslash{}key Fluid ~~~~~~~! saturated fluid
+
+~~~~~ \textbackslash{}key FluidGas~~~~ ! saturated vapor
+
+~ A4, \textbackslash{}field Temperature Values Name
+
+~~~~~ \textbackslash{}note Enter the name of a FluidProperties:Temperatures object.
+
+~~~~~ \textbackslash{}type object-list
+
+~~~~~ \textbackslash{}object-list FluidPropertyTemperatures
+
+~ N1, \textbackslash{}field Property Value 1
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}unitsBasedOnField A2
+
+~ N2, \textbackslash{}field Property Value 2
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}unitsBasedOnField A2
+
+\textless{} same thing repeated over and over again\textgreater{}
+
+~ N250; \textbackslash{}field Property Value 250
+
+~~~~~~~ \textbackslash{}type real
+
+~~~~~~~ \textbackslash{}unitsBasedOnField A2
+
+An example of this statement in an input data file is:
+
+FluidProperties:Saturated,
+
+~~~~~ R11,ENTHALPY,FLUID,R11Temperatures, ! Enthalpy in J/kg
+
+~~~~~ 153580,154600,156310,158580,161300,164380,167740,171330,175100,179020,183060,
+
+~~~~~ 187190,191400,195680,200000,201740,203490,205240,207000,208770,210530,212310,
+
+~~~~~ 214080,215870,217650,219860,221230,223030,224830,226630,228860,230250,232060,
+
+~~~~~ 233860,235700,237520,239350,241180,243010,246350,249450,254080,258730,263480,
+
+~~~ ~~268110,272860,277000,282410,287240,292120,297030,302000,307090,312080,317210,
+
+~~~~~ 322400,327670,333020,338460,344010,349680,355500,361480,367690,374100,381060,
+
+~~~~~ 388850,397280,426300;
+
+The format of the data for the superheated region is almost identical to that of the saturated region with one addition---a pressure.~ The pressure is listed before the rest of the data and has units of Pa.
+
+\textbf{FluidProperties:Superheated,}
+
+~~~~~ \textbackslash{}memo fluid properties for the superheated region
+
+~~~~~ \textbackslash{}format FluidProperty
+
+~ A1, \textbackslash{}field Fluid Name
+
+~~~~~ \textbackslash{}type object-list
+
+~~~~~ \textbackslash{}object-list FluidNames
+
+~ A2, \textbackslash{}field Fluid Property Type
+
+~~~~~ \textbackslash{}note Enthalpy Units are J/kg
+
+~~~~~ \textbackslash{}note Density Units are kg/m3
+
+~~~~~ \textbackslash{}type choice
+
+~~~~~ \textbackslash{}key Enthalpy~~~~ ! Units are J/kg
+
+~~~~~ \textbackslash{}key Density~~~~~ ! Units are kg/m3
+
+~ A3, \textbackslash{}field Temperature Values Name
+
+~~~~~ \textbackslash{}note Enter the name of a FluidProperties:Temperatures object.
+
+~~~~~ \textbackslash{}type object-list
+
+~~~~~ \textbackslash{}object-list FluidPropertyTemperatures
+
+~ N1, \textbackslash{}field Pressure
+
+~~~~~ \textbackslash{}note pressure for this list of properties
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}units Pa
+
+~~~~~ \textbackslash{}minimum\textgreater{} 0.0
+
+~ N2, \textbackslash{}field Property Value 1
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}unitsBasedOnField A2
+
+~ N3, \textbackslash{}field Property Value 2
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}unitsBasedOnField A2
+
+\textless{} same thing repeated over and over again\textgreater{}
+
+~ N250; \textbackslash{}field Property Value 250
+
+~~~~~~~ \textbackslash{}type real
+
+~~~~~~ \textbackslash{}unitsBasedOnField A2
+
+An example of this statement in an input data file is:
+
+FluidProperties:Superheated,
+
+~~~ R11,DENSITY,SuperR11Temperatures, ! Density in kg/m\^{}3
+
+~~~ 62000., !Pressure = 62000Pa
+
+~~~ 0,0,0,0,0,0,0,0.0139,0.0134,0.0129,0.0124,0.012,0.0116,0.0112,0.0109,0.0105,
+
+~~~ 0.0102,0.0099,0.0097,0.0094,0.0092,0.0089,0,0,0,0,0,0,0,0,0,0;
+
+\subsection{Fluid Properties Functions for Glycol Class Fluids}\label{fluid-properties-functions-for-glycol-class-fluids}
+
+In EnergyPlus, a glycol fluid is assumed to remain in the liquid phase.~ As a result, data is only required for fluids in the liquid state.~ There are four possible functions that may be used to obtain glycol data using the Fluid Properties module.~ These correspond to the fluid property of interest and include:
+
+\textbf{GetSpecificHeatGlycol} (Glycol,Temperature,GlycolIndex,calledfrom)
+
+\textbf{GetConductivityGlycol} (Glycol,Temperature,GlycolIndex,calledfrom)
+
+\textbf{GetDensityGlycol} (Glycol,Temperature,GlycolIndex,calledfrom)
+
+\textbf{GetViscosityGlycol} (Glycol,Temperature,GlycolIndex,calledfrom)
+
+All of these functions are used in exactly the same way.~ The module developer should send the glycol name (as listed in the GlycolConcentrations object in the input file) to the routine and the GlycolIndex (sent as 0 the first time and then set by the fluid property routine; see RefrigIndex discussion above).~ The calledfrom parameter is also used as discussed in the Refrigerant parameter discussion above. In addition, the functions require the temperature of the glycol in degrees Celsius.
+
+\subsection{Default Values for Glycol Class Fluids}\label{default-values-for-glycol-class-fluids}
+
+There are default values for specific heat, density, conductivity, and viscosity for Water, Ethylene Glycol, and Propylene Glycol.~ This means that if users accept the values as published in the ASHRAE Handbook of Fundamentals, then the only information the user must include in their input file is a description of the concentration of glycol used (via the GlycolConcentrations object).~ If water is used in a loop, the user does not need to enter anything other than WATER as the fluid type in the appropriate input syntax.~ Data for various concentrations of these three default fluids encompasses the range over with these fluids and their combinations are in the liquid phase (-35 to 125 degrees Celsius).~ When the glycol combination in question is indeed a fluid, the functions will return the appropriate value for the parameter in question.~ If the glycol is either a solid or vapor, the routine will return a zero value.~ Units for the different properties are: Joules per kilogram-Kelvin for specific heat, Pascal-seconds for viscosity, Watts per meter-Kelvin for conductivity, and kilograms per cubic meter for density.~ In contrast to the refrigerant data which is included in the RDS and must be copied into the user input file if it is to be used, the glycol default data has been hardwired into EnergyPlus and does not need to be entered into the input file.
+
+\subsection{Fluid Property Data and Expanding the Glycols Available to EnergyPlus}\label{fluid-property-data-and-expanding-the-glycols-available-to-energyplus}
+
+The format of the data for the glycols is almost identical to that of the superheated region for refrigerants with one exception---concentration replaces pressure.~ The concentration is listed before the rest of the data and is dimensionless.
+
+\textbf{FluidProperties:Concentration,}
+
+~~~~~ \textbackslash{}memo fluid properties for water/other fluid mixtures
+
+~~~~~ \textbackslash{}format FluidProperty
+
+~ A1, \textbackslash{}field Fluid Name
+
+~~~~~ \textbackslash{}type object-list
+
+~~~~~ \textbackslash{}object-list FluidNames
+
+~~~~~ \textbackslash{}note should not be any of the defaults (Water, EthyleneGlycol, or PropyleneGlycol)
+
+~ A2, \textbackslash{}field Fluid Property Type
+
+~~ ~~~\textbackslash{}note Density Units are kg/m3
+
+~~~~~ \textbackslash{}note SpecificHeat Units are J/kg-K
+
+~~~~~ \textbackslash{}note Conductivity Units are W/m-K
+
+~~~~~ \textbackslash{}note Viscosity Units are N-s/m2
+
+~~~~~ \textbackslash{}type choice
+
+~~~~~ \textbackslash{}key Density~~~~~ ! Units are kg/m3
+
+~~~~~ \textbackslash{}key SpecificHeat ! Units are J/kg-K
+
+~~~~~ \textbackslash{}key Conductivity ! Units are W/m-K
+
+~~~~~ \textbackslash{}key Viscosity~~~ ! Units are N-s/m2
+
+~ A3, \textbackslash{}field Temperature Values Name
+
+~~~~~ \textbackslash{}note Enter the name of a FluidProperties:Temperatures object.
+
+~~~~~ \textbackslash{}type object-list
+
+~~~~~ \textbackslash{}object-list FluidPropertyTemperatures
+
+~ N1, \textbackslash{}field Concentration
+
+~~~~~ \textbackslash{}note Glycol concentration for this list of properties entered as a fraction
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}units dimensionless
+
+~~~~~ \textbackslash{}minimum 0.0
+
+~~~~~ \textbackslash{}maximum 1.0
+
+~ N2, \textbackslash{}field Property Value 1
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}unitsBasedOnField A2
+
+~ N3, \textbackslash{}field Property Value 2
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}unitsBasedOnField A2
+
+\textless{} same thing repeated over and over again\textgreater{}
+
+~ N250; \textbackslash{}field Property Value 250
+
+~~~~~~~ \textbackslash{}type real
+
+~~~~~~ \textbackslash{}unitsBasedOnField A2
+
+An example of this statement in an input data file is:
+
+FluidProperties:Concentration,
+
+~~~~ MyPropyleneGlycol,SPECIFICHEAT ,GlycolTemperatures, ! Specific heat in J/kg-K
+
+~~~~ 0.8, ! Concentration
+
+~~~~ 2572,2600,2627,2655,2683,2710,2738,2766,2793,2821,2849,2876,2904,2931,2959,
+
+~~~~ 2987,3014,3042,3070,3097,3125,3153,3180,3208,3236,3263,3291,3319,3346,3374,
+
+~~~~ 3402,3429,3457;
+
+The above input syntax is used to define data for a particular new fluid beyond the default glycol fluids.~ It would be repeated at other appropriate concentration values, if necessary, to define the fluid.~ It should be noted that in order to enter a fluid, the user must specify all four of the properties: conductivity, specific heat, viscosity, and density.
+
+In addition to specifying the raw data for a new glycol, the user must list the fluid in the FluidNames object and then specify the concentration in the GlycolConcentrations object as shown below:
+
+FluidProperties:Names,
+
+~ MyPropyleneGlycol, GLYCOL;
+
+GlycolConcentrations,
+
+~ MyPropyleneGlycol, GLYCOL;
+
+The IDD description for the FluidProperties:GlycolConcentrations object is given below:
+
+\textbf{FluidProperties:GlycolConcentrations,}
+
+~~~~~~ \textbackslash{}unique-object
+
+~~~~~~ \textbackslash{}memo list of glycols and what concentration they are, maximum of ten
+
+~ A1,~ \textbackslash{}field Fluid 1 Name
+
+~~~ ~~~\textbackslash{}type alpha
+
+~~~~~~ \textbackslash{}reference GlycolConcentrations
+
+~ A2,~ \textbackslash{}field Glycol 1 Name
+
+~~~~~~ \textbackslash{}type choice
+
+~~~~~~ \textbackslash{}key EthyleneGlycol
+
+~~~~~~ \textbackslash{}key PropyleneGlycol
+
+~~~~~~ \textbackslash{}memo or UserDefined Fluid (must show up as a glycol in FluidProperties:Names list)
+
+~ N1,~ \textbackslash{}field Glycol 1 Concentration
+
+~~~~~~ \textbackslash{}type real
+
+~~~~~~ \textbackslash{}minimum 0.0
+
+~~~~~~ \textbackslash{}maximum 1.0
+
+~ A3,~ \textbackslash{}field Fluid 2 Name
+
+~~~~~~ \textbackslash{}type alpha
+
+~~~~~~ \textbackslash{}reference GlycolConcentrations
+
+\textless{} . . . repeated up to 10 times . . .\textgreater{}
+
+~ A19, \textbackslash{}field Fluid 10 Name
+
+~~~~~~ \textbackslash{}type alpha
+
+~ A20, \textbackslash{}field Glycol 10 Name
+
+~~~~~~ \textbackslash{}type choice
+
+~~~~~~ \textbackslash{}key EthyleneGlycol
+
+~~~~~~ \textbackslash{}key PropyleneGlycol
+
+~~~~~~ \textbackslash{}memo or UserDefined Fluid (must show up as a glycol in FluidProperties:Names list)
+
+~ N10; \textbackslash{}field Glycol 10 Concentration
+
+~~~~~~ \textbackslash{}type real
+
+~~~~~~ \textbackslash{}minimum 0.0
+
+~~~~~~ \textbackslash{}maximum 1.0
+
+An example of how this would be used in an actual IDF is:
+
+FluidProperties:GlycolConcentrations,
+
+~ MyProGly80Percent,~ !- fluid name 1
+
+~ MyPropyleneGlycol,~ !- glycol name 1
+
+~ 0.8,
+
+~ EthGly30Percent,~ !- fluid name 2
+
+~ EthyleneGlycol,~ !- glycol name 2
+
+~ 0.3;~ !- concentration 2
+
+The key relationship in this syntax is how FluidNames relates to GlycolConcentrations and how to have modules access through the proper name.~ FluidNames are used to define raw data, whether for refrigerants or glycols.~ With a glycol, it is not enough to define raw data since this does not necessarily define the actual concentration of glycol being used.~ Thus, the GlycolConcentrations object is needed.~ It defines a name for the actual glycol and then refers back to the FluidNames (first fluid listed in the above example) or to one of the default glycol fluids (second fluid listed in the above example).~ It is critical that module developers refer to the ``fluid name'' listed in the GlycolConcentrations object.~ This is the name used inside the fluid property module to access the proper data.~ Note that when the GlycolConcentrations object is read in during execution that the module will interpolate down from a two-dimensional array of data (variation on temperature and concentration) to a one-dimensional array of data (with temperature as the only independent variable, concentration of a glycol fluid on any loop is assumed to be constant).~ This means that only the temperature (along with the glycol fluid name and index) must be passed into the fluid property module and also saves execution time since only a one-dimensional interpolation is needed.
diff --git a/doc/module-developer/src/energyplus-services/global-data-flags-and-parameters.tex b/doc/module-developer/src/energyplus-services/global-data-flags-and-parameters.tex
new file mode 100644
index 00000000000..956f4f1f65b
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/global-data-flags-and-parameters.tex
@@ -0,0 +1,81 @@
+\section{Global Data: Flags and Parameters}\label{global-data-flags-and-parameters}
+
+Global data is used sparsely in EnergyPlus, according to our goals and programming standards.~ Data-only modules should be used to share data, usually across a limited number of other modules.~ Two critical data-only modules have been used:
+
+\textbf{DataGlobals} -- contains truly global data (such as number of zones, current hour, simulation status flags, interface statements to error and output routines)
+
+\textbf{DataEnvironment} -- contains weather data that is global (such as current outdoor dry-bulb temperature, barometric pressure, etc.)
+
+As an example of a limited data-only module, \textbf{DataSurfaces} contains data that is used in the modules that reference surfaces e.g., shadowing calculations, heat balance calculations.
+
+Module excerpts in this document show uses of these data-only modules.
+
+\subsection{Parameters}\label{parameters}
+
+Constants that might be useful throughout the program are defined as Fortran parameters in the DataGlobals data module. Examples include \emph{PI}, \emph{PiOvr2}, \emph{DegToRadians}, and \emph{MaxNameLength}. DataHVACGlobals contains parameters that might be useful anywhere in the HVAC simulation. Some examples are \emph{SmallTempDiff} and \emph{SmallMassFlow} that can be used for preventing divide by zero errors. The full set of global parameters can be obtained by examining the modules DataGlobals and DataHVACGlobals.
+
+\subsection{Simulation Flags}\label{simulation-flags}
+
+A number of logical flags (variables that are either \emph{true} or \emph{false}) are used throughout EnergyPlus. These flags are normally used to indicate the start or end of a time or simulation period. The following shows a complete list.
+
+\textbf{In DataGlobals:}
+
+BeginSimFlag
+
+Set to true until the actual simulation has begun, set to false after first heat balance time step.
+
+BeginFullSimFlag
+
+Set to true until a full simulation begins (as opposed to a sizing simulation); set to false after the first heat balance time step of the full simulation.
+
+EndSimFlag
+
+Normally false, but set to true at the end of the simulation (last heat balance time step of last hour of last day of last environment).
+
+WarmupFlag
+
+Set to true during the warmup portion of a simulation; otherwise false.
+
+BeginEnvrnFlag
+
+Set to true at the start of each environment (design day or run period), set to false after first heat balance time step in environment. This flag should be used for beginning of environment initializations in most HVAC components. See the example module for correct usage.
+
+EndEnvrnFlag
+
+Normally false, but set to true at the end of each environment (last heat balance time step of last hour of last day of environment).
+
+BeginDayFlag
+
+Set to true at the start of each day, set to false after first heat balance time step in day.
+
+EndDayFlag
+
+Normally false, but set to true at the end of each day (last heat balance time step of last hour of day).
+
+BeginHourFlag
+
+Set to true at the start of each hour, set to false after first heat balance time step in hour.
+
+EndHourFlag
+
+Normally false, but set to true at the end of each hour (last heat balance time step of hour)
+
+BeginTimeStepFlag
+
+Set to true at the start of each heat balance time step, set to false after first HVAC step in the heat balance time step.
+
+\textbf{In DataHVACGlobals:}
+
+FirstTimeStepSysFlag
+
+Set to true at the start of the first HVAC time step within each heat balance time step, false at the end of the HVAC time step.~ In other words, this flag is true during the first HVAC time step in a heat balance time step, and is false otherwise.
+
+\textbf{In Subroutine SimHVAC:}
+
+FirstHVACIteration
+
+True when HVAC solution technique on first iteration, false otherwise. Passed as a subroutine argument into the HVAC equipment simulation driver routines.
+
+The most commonly used logical flag in the HVAC simulation is FirstHVACIteration that is passed around as an argument among the HVAC simulation subroutines. The HVAC simulation is solved iteratively each HVAC time step. FirstHVACIteration is true for the first iteration in each time step and false for the remaining iterations.
+
+Finally, each developer must define and set a ``GetInput'' flag to make sure input data is read in only once. In the example module Fans the GetInput flag is GetInputFlag; the new developer can follow this example in using such a flag.
diff --git a/doc/module-developer/src/energyplus-services/input-services.tex b/doc/module-developer/src/energyplus-services/input-services.tex
new file mode 100644
index 00000000000..0c370a9a89e
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/input-services.tex
@@ -0,0 +1,307 @@
+\section{Input Services}\label{input-services}
+
+The module \emph{InputProcessor} processes the input data files (IDFs).~ It also reads and parses the IDD file.~ The InputProcessor uses the definition lines in the IDD as directives on how to process each input object in the IDF.~ The InputProcessor also turns all alpha strings into all UPPER CASE.~ Currently, it does nothing else to those strings -- so the number of blanks in a string must match what the calculational modules expect.~ The InputProcessor processes all numeric strings into single precision real numbers.~ Special characters, such as tabs, should \emph{not} be included in the IDF.
+
+The EnergyPlus module \emph{InputProcessor} provides several routines - generically called the ``get'' routines -- that enable the developer to readily access the data for a new module.~ These routines are made available by including a ``USE InputProcessor'' statement in the module or in the routine that will use the ``get'' routines.~ The GetFanInput subroutine in the example illustrates some of the uses of the ``get'' routines.
+
+\subsection{InputProcessor}\label{inputprocessor}
+
+The following objects use public routines from the InputProcessor.~ To access these, the code has:
+
+Use InputProcessor, ONLY: \textless{}routine1\textgreater{}, \textless{}routine2\textgreater{}
+
+Where the \textless{}routine\textgreater{} is one or more of the following:
+
+\subsection{GetNumObjectsFound}\label{getnumobjectsfound}
+
+This function returns the number of objects in the input belonging to a particular class.~ In other terms, it returns the number of instances in the input of a particular component.
+
+Example:
+
+USE InputProcessor, ONLY: GetNumObjectsFound
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+NumVAVSys = \textbf{GetNumObjectsFound}(`SINGLE DUCT:VAV:REHEAT')
+
+Here NumVAVSys will contain the number of single duct VAV terminal units in the input data file (IDF). SINGLE DUCT:VAV:REHEAT is the class name or keyword defining VAV terminal unit input on the IDD file.
+
+\subsection{GetObjectItem}\label{getobjectitem}
+
+This subroutine is used to obtain the actual alphanumeric and numeric data for a particular object.
+
+Example:
+
+~~~ USE InputProcessor
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+~~~ INTEGER :: SysNum = 0~~~~ ! The Sys that you are currently loading input into
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+~~~ CHARACTER(Len = MaxNameLength)~ :: CurrentModuleObject
+
+~~~ CHARACTER(Len = MaxNameLength), ALLOCATABLE, DIMENSION(:) :: Alphas
+
+~~~ CHARACTER(Len = MaxNameLength), ALLOCATABLE, DIMENSION(:) :: cAlphaFields
+
+~~~ CHARACTER(Len = MaxNameLength), ALLOCATABLE, DIMENSION(:) :: cNumericFields
+
+~~~ REAL(r64), ALLOCATABLE, DIMENSION(:) :: Numbers
+
+~~~ LOGICAL, ALLOCATABLE, DIMENSION(:)~~ :: lAlphaBlanks
+
+~~~ LOGICAL, ALLOCATABLE, DIMENSION(:)~~ :: lNumericBlanks
+
+~~~ INTEGER~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ :: MaxNums = 0
+
+~~~ INTEGER~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ :: MaxAlphas = 0
+
+~~~ INTEGER~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ :: TotalArgs = 0
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+~~~ CALL \textbf{GetObjectDefMaxArgs} \&
+
+(`AirTerminal:SingleDuct:VAV:Reheat', TotalArgs, NumAlphas, NumNums)
+
+~~~ MaxNums = MAX(MaxNums,NumNums)
+
+~~~ MaxAlphas = MAX(MaxAlphas,NumAlphas)
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+~~~~~ !Start Loading the System Input
+
+~~~~~~~ CurrentModuleObject = `AirTerminal:SingleDuct:VAV:Reheat'
+
+~~~~~ DO SysIndex = 1,~ NumVAVSys
+
+~~~~~~~ CALL \textbf{GetObjectItem} \& (TRIM(CurrentModuleObject),SysIndex,Alphas,NumAlphas,Numbers,NumNums, \&
+
+~~~ IOSTAT,AlphaBlank = lAlphaBlanks,NumBlank = lNumericBlanks,~ \&
+
+~~~ AlphaFieldnames = cAlphaFields,NumericFieldNames = cNumericFields)
+
+~~~~~~~ SysNum = SysIndex
+
+---~~~~ Check to make sure no duplicate names entered
+
+~~~~~~~ Sys(SysNum)\%SysName~~~~ = Alphas(1)
+
+~~~~~~~ Sys(SysNum)\%SysType~~~~ = TRIM(CurrentModuleObject)
+
+~~~ ~~~~Sys(SysNum)\%SysType\_Num = SingleDuctVAVReheat
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+~~~~~ END DO
+
+Here GetObjectItem is called with inputs (`AirTerminal:SingleDuct:VAV:Reheat') ~-- passed as CurrentModuleObject the class of object we want to input -- and SysIndex -- the index of the object on the input file. If SysIndex is 3, the call to GetObjectItem will get the data for the third VAV terminal unit on the input file. Output is returned in the remaining arguments. AlphArray contains in order all the alphanumeric data items for a single VAV terminal unit. NumArray contains all the numeric data items. NumAlphas is the number of alphanumeric items read; NumNums is the number of numeric data items read.~ IOSTAT is a status flag: -1 means there was an error; +1 means the input was OK. AlphArray and NumArray should be dimensioned to handle the largest expected input for the item -- which in this case is set from a call to \textbf{GetObjectDefMaxArgs}. NumBlank is an optional argument to the routine -- it can be used to determine if a numeric field was entered as ``blank'' rather than the filled value of 0.0. Likewise for NumFields and the others.
+
+These are used to make the potential error messages from the GetInput routine correspond more closely to the IDD nomenclature, but look a bit funny in use:
+
+IF (Sys(SysNum)\%SchedPtr = = 0) THEN
+
+~~ CALL ShowSevereError(~ \&
+
+~~~~ RoutineName//trim(CurrentModuleObject)//' = ``'//~ \&
+
+~~~~ TRIM(Sys(SysNum)\%SysName)//'``, invalid schedule.')
+
+~~ CALL ShowContinueError(TRIM(cAlphaFields(2))//`='//~ \&
+
+~~~~ TRIM(Alphas(2))//`not found.')
+
+~~ ErrorsFound = .true.
+
+ENDIF
+
+More information about standard error message formatting is contained in the \href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details and Examples} document (for the user) and (for the developer) in this document section: Standard Message Format.
+
+\subsection{GetObjectDefMaxArgs}\label{getobjectdefmaxargs}
+
+\subsubsection{Extensible input techniques}\label{extensible-input-techniques}
+
+While developers do their best to guess how many items are needed in an object, users will often want to extend that object with far more fields than were dreamed of.~ Using Allocatable arrays in Fortran usually makes this feasible, the special \textbackslash{}extensible field makes it possible.
+
+Example:
+
+USE InputProcessor, ONLY: GetObjectDefMaxArgs
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+CHARACTER(len = MaxNameLength), ALLOCATABLE, DIMENSION(:) :: Alphas
+
+REAL, ALLOCATABLE, DIMENSION(:)~~~~~~~~~~~~~~~~~~~~~~~~ :: Numbers
+
+! You supply the object word, routine returns numargs, numalpha, numnumeric
+
+CALL \textbf{GetObjectDefMaxArgs}(`DAYSCHEDULE:INTERVAL',NumArgs,NumAlpha,NumNumeric)
+
+ALLOCATE(Alphas(NumAlpha))
+
+ALLOCATE(Numbers(NumNumeric))
+
+!~ Then, usual get calls\ldots{}
+
+Thus, you can determine how many arguments that the IDD has defined as ``maximum'' for a given object.
+
+\subsection{GetObjectItemNum}\label{getobjectitemnum}
+
+GetObjectItem, described above, requires the input file index of the desired object in order to get the object's data. Sometimes this index may be unknown, but the name of the object is known. GetObjectItemNum returns the input file index given the class name and object name.
+
+Example:
+
+USE InputProcessor, ONLY: GetObjectItemNum
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+ListNum = \textbf{GetObjectItemNum}(`CONTROLLER LIST',ControllerListName)
+
+In the example, ListNum will contain the input file index of the `CONTROLLER LIST' whose name is contained in the string variable ControllerListName.
+
+\subsection{FindItemInList}\label{finditeminlist}
+
+This function looks up a string in a similar list of items and returns the index of the item in the list, if found. It is case sensitive.
+
+Example:
+
+USE InputProcessor, ONLY: FindItemInList
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+SysNum = \textbf{FindItemInList}(CompName,Sys\%SysName,NumSys)
+
+CompName is the input string, Sys\%SysName is the list of names to be searched, and NumSys is the size of the list.
+
+\subsection{FindItem}\label{finditem}
+
+Case insensitive version of the FindItemInList.
+
+Example:
+
+USE InputProcessor, ONLY: FindItem
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+SysNum = \textbf{FindItem}(CompName,Sys\%SysName,NumSys)
+
+CompName is the input string, Sys\%SysName is the list of names to be searched, and NumSys is the size of the list.
+
+\subsection{FindItemInSortedList}\label{finditeminsortedlist}
+
+This function looks up a string in a sorted list of items and returns the index of the item in the list, if found. It is case sensitive.
+
+Example:
+
+USE InputProcessor, ONLY: FindItemInSortedList
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+SysNum = \textbf{FindItemInSortedList}(CompName,Sys\%SysName,NumSys)
+
+CompName is the input string, Sys\%SysName is the list of names to be searched, and NumSys is the size of the list. See quick sort utility -- most lists are NOT sorted in EnergyPlus.
+
+\subsection{SameString}\label{samestring}
+
+This function returns true if two strings are equal (case insensitively).
+
+Example:
+
+USE InputProcessor, ONLY: SameString
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+IF (\textbf{SameString}(InputRoughness,`VeryRough')) THEN
+
+~~~ Material(MaterNum)\%Roughness = VeryRough
+
+ENDIF
+
+\subsection{VerifyName}\label{verifyname}
+
+This subroutine checks that an object name is unique; that is, it hasn't already been used for the same class of object and the name is not blank.
+
+Example:
+
+USE InputProcessor, ONLY: VerifyName
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+CALL \textbf{VerifyName}(AlphArray(1),Fan\%FanName, \&
+
+~ FanNum-1,IsNotOK,IsBlank,`FAN:SIMPLE:CONSTVOLUME Name')
+
+The first argument is the name to be checked, the second is the list of names to search, the third argument is the number of entries in the list, the 4\(^{th}\) argument is set to TRUE if verification fails, the 5\(^{th}\) argument is set to true if the name is blank, and the last argument is part of the error message written to the error file when verification fails.
+
+\subsection{RangeCheck}\label{rangecheck}
+
+The routine RangeCheck can be used to produce a reasonable error message to describe the situation in addition to setting the ErrorsFound variable to true.~ Errors found can then be checked in the calling routine and the program terminated if desired.
+
+SUBROUTINE RangeCheck(ErrorsFound,WhatFieldString,WhatObjectString,ErrorLevel,~ \&
+
+~~~~~~~~~~~~~~~~~~~~~ LowerBoundString,LowerBoundCondition,UpperBoundString,UpperBoundCondition)
+
+It can be used in a variety of places when the \textbackslash{}minimum and \textbackslash{}maximum fields will not work (e.g.~different min/max dependent on some other field).
+
+USE InputProcessor, ONLY: RangeCheck
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+ErrorsFound = .false.
+
+CALL RangeCheck(ErrorsFound,`DryBulb Temperature',`WeatherFile',~ \&
+
+~~~~~~~~~~~~~~~ `SEVERE',`\textgreater{} -70',(Drybulb\textgreater{}-70.),`\textless{} 70',(DryBulb \textless{}70.))
+
+CALL RangeCheck(ErrorsFound,`DewPoint Temperature',`WeatherFile',~ \&
+
+~~~~~~~~~~~~~~~ `SEVERE',`\textgreater{} -70',(Dewpoint\textgreater{}-70.),`\textless{} 70',(Dewpoint \textless{}70.))
+
+CALL RangeCheck(ErrorsFound,`Relative Humidity',`WeatherFile',~ \&
+
+~~~~~~~~~~~~~~~ `SEVERE',`\textgreater{} 0',(RelHum\textgreater{} = 0.),`\textless{} = 110',(RelHum\textless{} = 110.))
+
+To examine one call:
+
+The variable \textbf{DryBulb} is set to its value.~ In this case, it is coming from the \textbf{Weather File}.~ The \textbf{LowerBoundString} is `\textgreater{} - 70' and the \textbf{LowerBoundCondition} is (DryBulb\textgreater{}-70.) {[}this expression will yield true or false depending\ldots{}{]}
+
+The LowerBounds (\textbf{LowerBoundString}, \textbf{LowerBoundCondition}) are optional as are the UpperBounds (\textbf{UpperBoundString}, \textbf{UpperBoundCondition}).~ If we were only testing one set of ranges, the call would look like:
+
+Call \textbf{RangeCheck}(ErrorsFound,'DryBulb Temperature','WeatherFile','SEVERE',~ \&
+
+~ UpperBoundString = '\textless{} 70', UpperBoundCondition = (DryBulb\textless{}70.))
+
+ErrorLevel can be one of the usual Error levels:
+
+WARNING -- would be a simple warning message -- the calling routine might reset the value to be within bounds
+
+SEVERE -- a severe error.~ Usually the program would terminate if this is in a ``GetInput'' routine.~ If during execution, the calling program could reset the value but RangeCheck contains too many string comparisons to be called for an execution problem.
+
+FATAL -- not likely to be used.~ You want to provide a context to the error and if really a fatal type error, you'd like to execute the RangeCheck call and then terminate from the calling program.
+
+And the context for the message may be shown in the calling routine by checking the value of ErrorsFound:
+
+ErrFound = .false.
+
+Call \textbf{RangeCheck}(ErrFound,`This field',`SEVERE',`\textless{} = 100',(Value\textless{}100.))
+
+IF (ErrFound) THEN
+
+~ CALL ShowContinueError(`Occurs in routine xyz')
+
+~ ErrorsFound = .true.~ ! for later termination
+
+ENDIF
+
+\subsection{MakeUPPERCase}\label{makeuppercase}
+
+This function can be used to make sure an upper case string is being used.~ (Note this is not needed when using ``SameString'').~ Parameter 1 to the function is the string to be upper cased:
+
+USE InputProcessor, ONLY: MakeUPPERCase
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+UCString = \textbf{MakeUPPERCase}(`lower string')
diff --git a/doc/module-developer/src/energyplus-services/internal-zone-gains-services.tex b/doc/module-developer/src/energyplus-services/internal-zone-gains-services.tex
new file mode 100644
index 00000000000..469a1ea8ad7
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/internal-zone-gains-services.tex
@@ -0,0 +1,39 @@
+\section{Internal Zone Gains Services}\label{internal-zone-gains-services}
+
+Services are available to help with modeling internal gains.~ Internal gains include the usual sources such as people, lights, plug loads, etc., but in EnergyPlus there can also be zone gains from the skin losses from certain equipment such as thermal tanks, electric load center equipment and refrigeration case credits.~ Developers adding new device models, or adding skin loss modeling to exisiting device models, need to use a call to SetupZoneInternalGains.~ This call is defined in DataInterfaces.f90 and contains a number of optional arguments depending on the type of internal gains involved.~ The types of gains that can be added with this call include convection, radiation, and latent gains to the zone, convection and latent gains to the return air, carbon dioxide gains to the zone and generic air contaminant gains to the zone.~ For example, the call to register gains for the People object includes convection(sensible), thermal radiation, latent, and CO2 and is:
+
+\textbf{CALL} SetupZoneInternalGain(People(Loop)\%ZonePtr, \&
+
+~~~~ \textbf{`People'}, \&
+
+~~~~ People(Loop)\%Name, \&
+
+~~~~ IntGainTypeOf\_People, \&
+
+~~~~ ConvectionGainRate~~~~~~ = People(Loop)\%ConGainRate,\&
+
+~~~~ ThermalRadiationGainRate = People(Loop)\%RadGainRate, \&
+
+~~~~ LatentGainRate~~~~~~~~~~ = People(Loop)\%LatGainRate, \&
+
+~~~~ CarbonDioxideGainRate~~~ = People(Loop)\%CO2GainRate)
+
+The refrigerated case model includes terms for sensible and latent gains to both the zone and the return air.~ These are really negative gains, or sinks, and the call to register them is:
+
+\textbf{CALL} SetupZoneInternalGain(RefrigCase(CaseNum)\%ActualZoneNum, \&
+
+~~~~ \textbf{`Refrigeration:Case'},~ \&
+
+~~~~ RefrigCase(CaseNum)\%Name , \&
+
+~~~~ IntGainTypeOf\_RefrigerationCase,~~~~~~~~ \&
+
+~~~~ ConvectionGainRate~~~~~~~~~ = RefrigCase(CaseNum)\%SensZoneCreditRate , \&
+
+~~~~ ReturnAirConvectionGainRate = RefrigCase(CaseNum)\%SensHVACCreditRate , \&
+
+~~~~ LatentGainRate~~~~~~~~~~~~~ = RefrigCase(CaseNum)\%LatZoneCreditRate~ , \&
+
+~~~~ ReturnAirLatentGainRate~~~~ = RefrigCase(CaseNum)\%LatHVACCreditRate )
+
+The module developer needs to program the model to update the variable in their module, the one being registered by the call, and central routines use pointers to include the term in the appropriate energy balances elsewhere in the model.~ When adding a new type of internal gain, the new device needs to be added to arrays in \textbf{DataHeatBalance.f90} called \textbf{ZoneIntGainDeviceTypes} and \textbf{ccZoneIntGainDeviceTypes} and a new unique \textbf{``IntGainTypeOf\_''} parameter.
diff --git a/doc/module-developer/src/energyplus-services/object-services.tex b/doc/module-developer/src/energyplus-services/object-services.tex
new file mode 100644
index 00000000000..8b03b278185
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/object-services.tex
@@ -0,0 +1,393 @@
+\section{Object Services}\label{object-services}
+
+It is standard practice in EnergyPlus that only objects associated with a given module be accessed from the input data file using a GetObjectItem function call and that this type of function call only be executed during GetInput. For example, the module HVACDXSystem would only access the object DXSystem:AirLoop in the GetInput subroutine or the module HVACFanComponent would only access the different fan objects as shown in the example below. This programming standard requires that all modules be ``responsible'' for specific objects and no other module accesses the input data file for this specific object. Using this technique, maintenance of the EnergyPlus modules is limited to specific areas of software as input data for objects evolve for any reason.
+
+\emph{Module HVACDXSystem - SUBROUTINE GetDXCoolingSystemInput:}
+
+~~~ CALL GetObjectItem(`DXSYSTEM:AIRLOOP',DXCoolSysNum,AlphArray, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ NumAlphas,NumArray,NumNums,IOSTAT)
+
+\emph{Module HVACFanComponent -- SUBROUTINE GetFanInput:}
+
+~~~ CALL GetObjectItem(`FAN:SIMPLE:CONSTVOLUME',SimpFanNum,AlphArray, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ NumAlphas,NumArray,NumNums,IOSTAT)
+
+~~~ CALL GetObjectItem(`FAN:SIMPLE:VARIABLEVOLUME',VarVolFanNum, \&
+
+~~~~~~~~~~~ ~~~~~~~~~~~~~~~AlphArray,NumAlphas,NumArray,NumNums,IOSTAT)
+
+~~~ CALL GetObjectItem(`ZONE EXHAUST FAN',ExhFanNum,AlphArray, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ NumAlphas,NumArray,NumNums,IOSTAT)
+
+~~~ CALL GetObjectItem(`FAN:SIMPLE:ONOFF',OnOffFanNum,AlphArray, \&
+
+~ ~~~~~~~~~~~~~~~~~~~~~~~~~NumAlphas,NumArray,NumNums,IOSTAT)
+
+If module developers were allowed to access the input data file for other objects not related to a particular module, both the original module and the alternate module would have to be corrected each time the object changed. This poses a severe hazard for future development of EnergyPlus.
+
+Module developers may at times require information for specific objects from other modules. When this occurs, the Information is ``mined'' through function or subroutine calls located in the other module. Existing function calls may be used or added to EnergyPlus as needed. In this way, a module developer could confirm that node information provided in a parent object matched the node information specified for its children object. Other error checking may also be performed in this manner. For example, if the module HVACDXSystem needed to know the capacity of the DX cooling coil, a function call to GetCoilCapacity in the DXCoil module would provide this information. The function GetCoilCapacity would the ``Get'' the input from the input data file if it has not already been accessed and provide the information back to the calling module.
+
+A variety of examples exist to aid the module developer in this area of programming.
+
+\begin{itemize}
+\tightlist
+\item
+  DXCoil.f90:
+\end{itemize}
+
+FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
+
+FUNCTION GetMinOATCompressor(CoilType,CoilName,ErrorsFound) RESULT(MinOAT)
+
+FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
+
+FUNCTION GetCoilOutletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
+
+FUNCTION GetSupplyAirFanOperatingMode(CoilType,CoilName,ErrorsFound) RESULT(OpMode)
+
+FUNCTION GetCoilCondenserNode(CoilType,CoilName,ErrorsFound) RESULT(CondNode)
+
+FUNCTION GetHPCoolingCoilIndex(HeatingCoilType, HeatingCoilName, HeatingCoilIndex) ~~~~~~~~~~~~~ RESULT(DXCoolingCoilIndex)
+
+\begin{itemize}
+\tightlist
+\item
+  FanCoilUnits.f90:
+\end{itemize}
+
+INTEGER FUNCTION GetFanCoilZoneInletAirNode(FanCoilNum)
+
+INTEGER FUNCTION GetFanCoilOutAirNode(FanCoilNum)
+
+INTEGER FUNCTION GetFanCoilReturnAirNode(FanCoilNum)
+
+INTEGER FUNCTION GetFanCoilMixedAirNode(FanCoilNum)
+
+\begin{itemize}
+\tightlist
+\item
+  HeatRecovery.f90:
+\end{itemize}
+
+FUNCTION GetSupplyInletNode(HXName,ErrorsFound)
+
+FUNCTION GetSupplyOutletNode(HXName,ErrorsFound)
+
+FUNCTION GetSecondaryInletNode(HXName,ErrorsFound)
+
+FUNCTION GetSecondaryOutletNode(HXName,ErrorsFound)
+
+\begin{itemize}
+\tightlist
+\item
+  HVACFanComponent.f90:
+\end{itemize}
+
+FUNCTION GetFanDesignVolumeFlowRate(FanType,FanName,ErrorsFound) RESULT(DesignVolumeFlowRate
+
+FUNCTION GetFanInletNode(FanType,FanName,ErrorsFound) RESULT(NodeNumber)
+
+FUNCTION GetFanOutletNode(FanType,FanName,ErrorsFound) RESULT(NodeNumber)
+
+SUBROUTINE GetFanVolFlow(FanIndex, FanVolFlow)
+
+SUBROUTINE GetFanType(FanName,FanType,ErrorsFound,ThisObjectType)
+
+\begin{itemize}
+\tightlist
+\item
+  HVACHeatingCoils.f90:
+\end{itemize}
+
+FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
+
+FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
+
+FUNCTION GetCoilOutletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
+
+SUBROUTINE GetHeatingCoilIndex(HeatingCoilName,HeatingCoilIndex,ErrorsFound)
+
+\begin{itemize}
+\tightlist
+\item
+  HVACHXAssistedCoolingCoil.f90:
+\end{itemize}
+
+FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
+
+FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
+
+FUNCTION GetCoilOutletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
+
+FUNCTION GetHXDXCoilName(CoilType,CoilName,ErrorsFound) RESULT(DXCoilName)
+
+FUNCTION GetCoilMaxWaterFlowRate(CoilType,CoilName,ErrorsFound) RESULT(MaxWaterFlowRate)
+
+\begin{itemize}
+\tightlist
+\item
+  HVACStandAloneERV.f90
+\end{itemize}
+
+FUNCTION GetSupplyAirFlowRate(ERVType,ERVCtrlName,ErrorsFound) RESULT(AirFlowRate)
+
+FUNCTION GetSupplyAirInletNode(ERVType,ERVCtrlName,ErrorsFound) RESULT(AirInletNode)
+
+FUNCTION GetExhaustAirInletNode(ERVType,ERVCtrlName,ErrorsFound) RESULT(AirInletNode)
+
+INTEGER FUNCTION GetStandAloneERVOutAirNode(StandAloneERVNum)
+
+INTEGER FUNCTION GetStandAloneERVZoneInletAirNode(StandAloneERVNum)
+
+INTEGER FUNCTION GetStandAloneERVReturnAirNode(StandAloneERVNum)
+
+\begin{itemize}
+\tightlist
+\item
+  HVACSteamCoilComponent.f90:
+\end{itemize}
+
+FUNCTION GetCoilMaxWaterFlowRate(CoilType,CoilName,ErrorsFound) RESULT(MaxWaterFlowRate)
+
+\begin{itemize}
+\tightlist
+\item
+  HVACWaterCoilComponent.f90:
+\end{itemize}
+
+FUNCTION GetCoilMaxWaterFlowRate(CoilType,CoilName,ErrorsFound) RESULT(MaxWaterFlowRate)
+
+FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
+
+FUNCTION GetCoilOutletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
+
+\begin{itemize}
+\tightlist
+\item
+  HVACWaterToAir.f90:
+\end{itemize}
+
+FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
+
+FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
+
+FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
+
+FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
+
+\begin{itemize}
+\tightlist
+\item
+  MixedAir.f90:
+\end{itemize}
+
+FUNCTION GetOAMixerNodeNumbers(OAMixerName,ErrorsFound) RESULT(OANodeNumbers)
+
+FUNCTION GetNumOAMixers() RESULT(NumberOfOAMixers)
+
+FUNCTION GetNumOAControllers() RESULT(NumberOfOAControllers)
+
+FUNCTION GetOAMixerReliefNodeNumber(OAMixerNum) RESULT(ReliefNodeNumber)
+
+FUNCTION GetOASystemNumber(OASysName) RESULT(OASysNumber)
+
+FUNCTION GetOAMixerInletNodeNumber(OAMixerNumber) RESULT(OAMixerInletNodeNumber)
+
+FUNCTION GetOAMixerReturnNodeNumber(OAMixerNumber) RESULT(OAMixerReturnNodeNumber)
+
+FUNCTION GetOAMixerMixedNodeNumber(OAMixerNumber) RESULT(OAMixerMixedNodeNumber)
+
+\begin{itemize}
+\tightlist
+\item
+  PackagedTerminalHeatPump.f90:
+\end{itemize}
+
+INTEGER FUNCTION GetPTHPZoneInletAirNode(PTHPNum)
+
+INTEGER FUNCTION GetPTHPOutAirNode(PTHPNum)
+
+INTEGER FUNCTION GetPTHPReturnAirNode(PTHPNum)
+
+INTEGER FUNCTION GetPTHPMixedAirNode(PTHPNum)
+
+\begin{itemize}
+\tightlist
+\item
+  PurchasedAirManager.f90:
+\end{itemize}
+
+FUNCTION GetPurchasedAirOutAirMassFlow(PurchAirNum) RESULT(OutAirMassFlow)
+
+\begin{itemize}
+\tightlist
+\item
+  SetpointManager.f90:
+\end{itemize}
+
+LOGICAL FUNCTION IsNodeOnSetPtManager(NodeNum,SetPtType)
+
+\begin{itemize}
+\tightlist
+\item
+  UnitVentilator.f90:
+\end{itemize}
+
+INTEGER FUNCTION GetUnitVentilatorOutAirNode(UnitVentNum)
+
+INTEGER FUNCTION GetUnitVentilatorZoneInletAirNode(UnitVentNum)
+
+INTEGER FUNCTION GetUnitVentilatorMixedAirNode(UnitVentNum)
+
+INTEGER FUNCTION GetUnitVentilatorReturnAirNode(UnitVentNum)
+
+\begin{itemize}
+\tightlist
+\item
+  WindowAC.f90:
+\end{itemize}
+
+INTEGER FUNCTION GetWindowACZoneInletAirNode(WindACNum)
+
+INTEGER FUNCTION GetWindowACOutAirNode(WindACNum)
+
+INTEGER FUNCTION GetWindowACReturnAirNode(WindACNum)
+
+INTEGER FUNCTION GetWindowACMixedAirNode(WindACNum)
+
+These kinds of calls are highly encouraged so that data is mined from the other modules rather than being declared public.
+
+The function call for GetCoilCapacity in module DXCoil.f90 is shown below. Note that the format for these function calls have the same format as other subroutines throughout the EnergyPlus software. The example function shown below is declared as a public routine in module DXCoils for use by other modules through a USE statement.
+
+\emph{Module DXCoils.f90:}
+
+PUBLIC~ GetCoilCapacity
+
+FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
+
+~~~~~~~~~ ! FUNCTION INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Linda Lawrie
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ February 2006
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS FUNCTION:
+
+~~~~~~~~~ ! This function looks up the coil capacity for the given
+
+~~~~~~~~~ ! coil and returns it.~ If incorrect coil type or name
+
+~~~~~~~~~ ! is given, errorsfound is returned as true and capacity
+
+~~~~~~~~~ ! is returned as negative.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~ USE InputProcessor,~ ONLY: FindItemInList
+
+~ IMPLICIT NONE ! Enforce explicit typing of all variables in
+
+~~~~~~~~~~~~~~~ ! this routine
+
+~~~~~~~~~ ! FUNCTION ARGUMENT DEFINITIONS:
+
+~ CHARACTER(len = *), INTENT(IN) :: CoilType~~ ! must match coil
+
+~~~~~~~~~~ ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~! types in this module
+
+~ CHARACTER(len = *), INTENT(IN) :: CoilName~~ ! must match coil
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ! names for the coil type
+
+~ LOGICAL, INTENT(INOUT)~~~~ :: ErrorsFound~ ! set to true if problem
+
+~ REAL~~~~~~~~~~~~~~~~~~~~~~ :: CoilCapacity ! returned capacity of
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ! matched coil
+
+~~~~~~~~~ ! FUNCTION PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS:
+
+~~~~~~~~~ ! na
+
+~ ~~~~~~~~! DERIVED TYPE DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! FUNCTION LOCAL VARIABLE DECLARATIONS:
+
+~ INTEGER :: WhichCoil
+
+~ ! Obtains and Allocates DXCoils
+
+~ IF (GetCoilsInputFlag) THEN
+
+~~~ CALL GetDXCoils
+
+~~~ GetCoilsInputFlag = .FALSE.
+
+~ END IF
+
+~ IF (CoilType = = `COIL:DX:HEATINGEMPIRICAL' .or.~~ \&
+
+~~~~~ CoilType = = `COIL:DX:COOLINGBYPASSFACTOREMPIRICAL') THEN
+
+~~~ WhichCoil = FindItemInList(CoilName,DXCoil\%Name,NumDXCoils)
+
+~~~ IF (WhichCoil / = 0) THEN
+
+~~~~~ CoilCapacity = DXCoil(WhichCoil)\%RatedTotCap(1)
+
+~~~ ENDIF
+
+~ ELSE
+
+~~~ WhichCoil = 0
+
+~ ENDIF
+
+~ IF (WhichCoil = = 0) THEN
+
+~~~ CALL ShowSevereError('Could not find CoilType = ``' \&
+
+~~~~~~~~~~~~ //TRIM(CoilType)//`" with Name = ``'//TRIM(CoilName)//'''\,')
+
+~~~ ErrorsFound = .true.
+
+~~~ CoilCapacity = -1000.
+
+~ ENDIF
+
+~ RETURN
+
+END FUNCTION GetCoilCapacity
+
+Note that the function name in one module can be the same as a function name in a different module. In fact, for EnergyPlus this should be the case -- the module should use a generic name that is typical of its function. The calling module should use a ``local name'' that better specifies the type of item it is accessing. For example, if module HVACFurnace required node or capacity information from identical functions contained in modules HVACHeatingCoils and DXCoils, these function names could easily be assigned more descriptive names in the HVACFurnace module as follows.
+
+\emph{Module HVACFurnace.f90:}
+
+USE HeatingCoils,~~~ ONLY:~~~~~~~~ GetHeatingCoilCapacity = \textgreater{}GetCoilCapacity,
+
+GetHeatingCoilInletNode = \textgreater{}GetCoilInletNode
+
+USE DXCoils,~~~~~~~ ~~~~ONLY:~~~~~~~ GetDXCoilCapacity = \textgreater{}GetCoilCapacity,
+
+GetDXCoilInletNode = \textgreater{}GetCoilInletNode
diff --git a/doc/module-developer/src/energyplus-services/other-useful-utilities.tex b/doc/module-developer/src/energyplus-services/other-useful-utilities.tex
new file mode 100644
index 00000000000..445ca5e5f14
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/other-useful-utilities.tex
@@ -0,0 +1,279 @@
+\section{Other Useful Utilities}\label{other-useful-utilities}
+
+\subsection{GetNewUnitNumber}\label{getnewunitnumber}
+
+Rather than attempt to keep track of all open files and distribute this list to everyone, we have chosen to use a routine that does this operation.~ If you need to have a scratch file (perhaps when porting legacy code into EnergyPlus modules), you can use the GetNewUnitNumber function to determine a logical file number for the OPEN and READ/WRITE commands.~ The function works by looking at all open assigned files and returning a number that isn't being used.~ This implies that you will OPEN the unit immediately after calling the function (and you should!).
+
+Example:
+
+INTEGER, EXTERNAL :: GetNewUnitNumber
+
+\ldots{}
+
+myunit = GetNewUnitNumber()
+
+OPEN(Unit = myunit,File = 'myscratch')
+
+\subsection{FindUnitNumber}\label{findunitnumber}
+
+If you want to find out a unit number for a file you think is already open, you can use the FindUnitNumber function.~ For example, rather than creating a new unit for debug output, you could latch onto the same unit as currently used for the ``eplusout.dbg'' file.
+
+Example:
+
+INTEGER, EXTERNAL :: FindUnitNumber
+
+\ldots{}
+
+myunit = FindUnitNumber(`eplusout.dbg')
+
+If that file is already opened, it will get back the unit number it is currently assigned to.~ If it is not opened or does not exist, it will go ahead, get a unit number, and OPEN the file.~ (Should not be used for Direct Access or Binary files!)
+
+\subsection{FindNumberinList}\label{findnumberinlist}
+
+Sometimes you would like to find a number in a list.~ This is applicable to integers only (e.g.~Index numbers of some item).
+
+Example:
+
+INTEGER, EXTERNAL :: FindNumberInList
+
+\ldots{}
+
+MatchingCooledZoneNum = ~ \&
+
+~~ \textbf{FindNumberinList}(CtrlZoneNum,~ \&
+
+~~~~ AirToZoneNodeInfo(AirLoopNum)\%CoolCtrlZoneNums,NumZonesCooled)
+
+The location/index in the array \textbf{AirToZoneNodeInfo\%CoolCtrlZoneNums} will be returned if it finds the number in the array.~ If 0 is returned, it did not find that number in the list.
+
+\subsection{ValidateComponent}\label{validatecomponent}
+
+Many objects specify a component type as well as a component name.~ Or, an object might have only a component name.~ The ValidateComponent routine will allow for objects outside the scope of a current ``GetInput'' routine to verify that the specific component does exist in the input file.
+
+SUBROUTINE ValidateComponent(CompType,CompName,IsNotOK,CallString)
+
+CompType, CompName are the typical nomenclature for ``Component Type'' (e.g.~Fan:Simple:OnOff) and ``Component Name'' (e.g. ``my fan'' -- user specified).~ IsNotOk is a logical from the calling program that is set to true when the component is not on the input file.~ CallString should specify the calling object -- so that an appropriate error message can be issued.
+
+Example:
+
+~ ! No USE needed -- straightforward routine in GeneralRoutines
+
+~ CALL \textbf{ValidateComponent}(Furnace(FurnaceNum)\%FanType,~ \&
+
+~~~~~~~~~~~~~~~~~~ Furnace(FurnaceNum)\%FanName,IsNotOK,~ \&
+
+~~~~~~~~~~~~~~~~~~ `Furnace:BlowThru:HeatOnly')
+
+~ IF (IsNotOK) THEN
+
+~~~ CALL ShowContinueError(`In Furnace ='//~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ TRIM(Furnace(FurnaceNum)\%Name))
+
+~~~ ErrorsFound = .true.
+
+~ ENDIF
+
+Note that in the example, the FanType is entered by the user.~ This allows for ultimate flexibility though the example could also include appropriate fan types that are inherent to the code (an acceptable, if somewhat inflexible, practice).
+
+\subsection{CheckComponent}\label{checkcomponent}
+
+This routine is exactly like ValidateComponent but doesn't generate an error message.~ It could be used instead of ValidateComponent and you could use the ``IsNoOK'' to generate your own error message.~ However, the intended use is for checking out different components when you don't have the component type as a field for the object.~ Thus, you can easily check if there is an object (component type) with the name entered in your field.
+
+SUBROUTINE CheckComponent(CompType,CompName,IsNotOK)
+
+CompType, CompName are the typical nomenclature for ``Component Type'' (e.g.~Fan:OnOff) and ``Component Name'' (e.g. ``my fan'' -- user specified).~ IsNotOk is a logical from the calling program that is set to true when the component is not on the input file.
+
+Example:
+
+~ ! No USE needed -- straightforward routine in GeneralRoutines
+
+~ CALL \textbf{CheckComponent}(`Furnace:BlowThru:HeatOnly',~ \&
+
+~~~~~~~~~~~~~~~~~~ FurnaceRefName,IsNotOK)
+
+~ IF (IsNotOK) THEN
+
+~~~ CALL \textbf{CheckComponent}(`Furnace:BlowThru:HeatCool',~ \&
+
+~~~~~~~~~~~~~~~~~~ FurnaceRefName,IsNotOK)
+
+~~ . . . more checks on IsNotOK
+
+~~~~~~~~ ELSE
+
+~~~~~~~~~~ FurnaceType = `Furnace:BlowThru:HeatOnly'
+
+~ ENDIF
+
+. . .
+
+Note that in the example, the FurnaceRefName is entered by the user.~ And this module knows what kind of components it might be.
+
+\subsection{CreateSysTimeIntervalString}\label{createsystimeintervalstring}
+
+A very important part of EnergyPlus simulation is to be able to alert the user to problems during the simulation.~ The CreateSysTimeIntervalString will help do that though a better use is the ShowContinueErrorTimeStamp routine.~ The routine has no argument -- a string is returned.~ The example below also illustrates the preferred method of counting how many times an error is produced and not printing each occurrence.
+
+Example:
+
+USE General, ONLY: CreateSysTimeInterval
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+!The warning message will be suppressed during the warm up days.
+
+If (.NOT.WarmUpFlag) Then
+
+~ ErrCount = ErrCount + 1
+
+~ IF (ErrCount \textless{} 15) THEN
+
+~~~ CALL ShowWarningError(`SimAirLoops: Max iterations exceeded for'// \&
+
+~~~~~~~ TRIM(PrimaryAirSystem(AirLoopNum)\%Name)//`, at'//~ \&
+
+~~~~~~~ TRIM(EnvironmentName)//`,'//TRIM(CurMnDy)//`'//~~ \&
+
+~~~~~~~ TRIM(\textbf{CreateSysTimeIntervalString}()))
+
+~ ELSE
+
+~~~ IF (MOD(ErrCount,50) = = 0) THEN
+
+~~~~~ WRITE(CharErrOut,*) ErrCount
+
+~~~~~ CharErrOut = ADJUSTL(CharErrOut)
+
+~~~~~ CALL ShowWarningError (`SimAirLoops: Exceeding max iterations'// \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ `continues\ldots{}'//CharErrOut)
+
+~~~ ENDIF
+
+~ ENDIF
+
+End If
+
+\subsection{TrimSigDigits}\label{trimsigdigits}
+
+Along with error messages to alert the user, oftentimes you'd like to include values that are in error.~ You can use what some of the examples have shown -- Write(string,*) value but that will produce many digits in real numbers.~ The TrimSigDigits routine will allow for easy modification to a set of digits.~ Note that there are two flavors (INTERFACE statement in module General) so that you can easily get the string value of an integer.
+
+FUNCTION TrimSigDigits(RealValue,SigDigits) RESULT(OutputString)
+
+And
+
+FUNCTION TrimSigDigits(IntegerValue) RESULT(OutputString)
+
+As seen in the following example of use in code, a real value is passed in as argument 1 and the number of digits desired is passed in as argument 2.~ Note that the routine will preserve any ``E+xx'' outputs when a value like .000000004 might be passed in.
+
+USE General, ONLY: TrimSigDigits
+
+. . .
+
+CALL ShowWarningError(`COIL:Water:DetailedFlatCooling in Coil ='//~ \&
+
+~~~~~~~~~~~~~~~~~~~~ TRIM(WaterCoil(coilNum)\%Name))
+
+CALL ShowContinueError('Air Flow Rate Velocity has greatly exceeded `// \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `upper design guildelines of \textasciitilde{}2.5 m/s')
+
+CALL ShowContinueError(`Air MassFlowRate{[}kg/s{]} ='//~ \&
+
+~~~~~~~~~~~~~~~~~~~~ TRIM(\textbf{TrimSigDigits}(AirMassFlow,6)))
+
+~~~~~~ AirVelocity = AirMassFlow*AirDensity/WaterCoil(CoilNum)\%MinAirFlowArea
+
+CALL ShowContinueError(`Air Face Velocity{[}m/s{]} ='//~ \&
+
+~~~~~~~~~~~~~~~~~~~~ TRIM(\textbf{TrimSigDigits}(AirVelocity,6)))
+
+CALL ShowContinueError('Approximate MassFlowRate limit for Face `// \&
+
+~~~~~~~~~~~~~~~~~~~~~~ Area{[}kg/s{]} = '//~ \&~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ TRIM(\textbf{TrimSigDigits}(2.5*WaterCoil(CoilNum)\%MinAirFlowArea/AirDensity,6)))
+
+CALL ShowContinueError('COIL:Water:DetailedFlatCooling could be `// \&
+
+~~~~~~~~~~~~~~~~~~~~~~ `resized/autosized to handle capacity')
+
+CoilWarningOnceFlag(CoilNum) = .False.
+
+\subsection{RoundSigDigits}\label{roundsigdigits}
+
+Similar to TrimSigDigits, the RoundSigDigits function may be used when you want to ``round'' the output string -- perhaps for reporting and/or error messages.~ Note that there are two flavors (INTERFACE statement in module General) so that you can easily get the string value of an integer.
+
+FUNCTION RoundSigDigits(RealValue,SigDigits) RESULT(OutputString)
+
+And
+
+FUNCTION RoundSigDigits(IntgerValue) RESULT(OutputString)
+
+As seen in the following example of use in code, a real value is passed in as argument 1 and the number of digits desired is passed in as argument 2.~~~ Note that the routine will preserve any ``E+xx'' outputs when a value like .000000004 might be passed in.
+
+USE General, ONLY: RoundSigDigits
+
+. . .
+
+~~~ LatOut = \textbf{RoundSigDigits}(Latitude,2)
+
+~~~ LongOut = \textbf{RoundSigDigits}(Longitude,2)
+
+~~~ TZOut = \textbf{RoundSigDigits}(TimeZoneNumber,2)
+
+~~~ NumOut = \textbf{RoundSigDigits}(Elevation,2)
+
+~~~ PressOut = \textbf{RoundSigDigits}(StdBaroPress,0)
+
+~~~ Write(OutputFileInits,LocFormat) Trim(LocationTitle),TRIM(LatOut),~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ TRIM(LongOut),~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ TRIM(TZOut),~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ TRIM(NumOut),~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ TRIM(PressOut)
+
+\subsection{SafeDivide}\label{safedivide}
+
+SafeDivide can be used when you might not be sure that the denominator in a divide will not be zero.
+
+FUNCTION SafeDivide(a, b) RESULT (c)
+
+USE General, ONLY: SafeDivide
+
+. . .
+
+Result = SafeDivide(A,B)
+
+\subsection{SetupAndSort}\label{setupandsort}
+
+SetupAndSort can be called to order/sort a character array.~ A companion index array goes along with it so that one does not have to supply an entire derived type to be sorted.~ This companion array is then used to point to the proper element of such structures.
+
+SUBROUTINE SetupAndSort(CharacterList, iCharacterList)
+
+USE SortAndStringUtilities, ONLY: SetupAndSort
+
+. . .
+
+A use:
+
+ALLOCATE(iCharacterList(number of entries))
+
+Do item = 1,number of entries
+
+~ iCharacterList(item) = item
+
+end do
+
+! routine sorts this array and its companion
+
+CALL SetUpAndSort(CharacterList,iCharacterList)
+
+Do item = 1,number of entries
+
+~ ! iCharacterList now points to actual structure
+
+~ Write(output,*) Structure(iCharacterList(item))\%Name
+
+Enddo
diff --git a/doc/module-developer/src/energyplus-services/performance-curve-services.tex b/doc/module-developer/src/energyplus-services/performance-curve-services.tex
new file mode 100644
index 00000000000..da1951b518b
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/performance-curve-services.tex
@@ -0,0 +1,73 @@
+\section{Performance Curve Services}\label{performance-curve-services}
+
+Some HVAC equipment models in EnergyPlus use performance curves. These are polynomials in one or two independent variables that are used to modify rated equipment performance for performance at the current, off-rated conditions. Most often the curves are functions of temperature -- entering wetbulb and outside drybulb, for instance -- or of the part load fraction. EnergyPlus provides services to input, store, and retrieve curve data and to evaluate curves given values of the independent variables. There are 3 curve objects: CURVE:QUADRATIC, CURVE:CUBIC, and CURVE:BIQUADRATIC.
+
+\subsection{GetCurveIndex}\label{getcurveindex}
+
+This function takes a curve name as input and returns an internal pointer to the curve. Curve values will always be accessed via the pointer not the name during the simulation for reasons of efficiency. This function is usually called once for each curve during the input phase.
+
+USE CurveManage, ONLY: GetCurveIndex
+
+. . .
+
+DXCoil(DXCoilNum)\%CCapFTemp = \textbf{GetCurveIndex}(Alphas(5))
+
+~ IF (DXCoil(DXCoilNum)\%CCapFTemp .EQ. 0) THEN
+
+~~~ CALL ShowSevereError(`COIL:DX:BF-Empirical not found =' \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ //TRIM(Alphas(5)))
+
+~~~ ErrorsFound = .TRUE.
+
+~ END IF
+
+\subsection{GetCurveCheck}\label{getcurvecheck}
+
+This function uses a curve name as well as an error indicator and object name to ``get'' a curve index and perform error checking in one call.~ The calling routine will need to check the value of the error flag and perform appropriate action.
+
+FUNCTION GetCurveCheck(alph, errFlag, ObjName)~ \&
+
+~~~~~~~~~~~~ RESULT (GetCurveCheckOut)
+
+The curve index (as in GetCurveIndex) is the result. Curve values will always be accessed via the pointer not the name during the simulation for reasons of efficiency. This function would be called during an input phase for an object.
+
+USE CurveManager, ONLY: GetCurveCheck
+
+\ldots{}
+
+GasAbsorber(AbsorberNum)\%CoolCapFTCurve~~~~~ = ~~ \&
+
+~~~~~ \textbf{GetCurveCheck}(AlphArray(8),~ ErrorsFound, ChillerName)
+
+GasAbsorber(AbsorberNum)\%FuelCoolFTCurve~~~~ = ~~ \&
+
+~~~~~ \textbf{GetCurveCheck}(AlphArray(9),~ ErrorsFound, ChillerName)
+
+\subsection{GetCurveType}\label{getcurvetype}
+
+This function will tell the calling routine what the ``curve type'' that was input.~ This function may be useful if your module does different calculations depending on a curve type (i.e.~cubic vs quadratic) or if it should not use a specific curve type.~ This function would be called during input phase for an object.
+
+CHARACTER(len = 20) FUNCTION GetCurveType (CurveIndex)
+
+Example of use:
+
+USE CurveManager,~~ ONLY: GetCurveIndex, GetCurveType
+
+\ldots{}
+
+SELECT CASE(\textbf{GetCurveType}(DXCoil(DXCoilNum)\%CCapFTemp))
+
+\subsection{CurveValue}\label{curvevalue}
+
+This function takes the curves index and one or two independent variables as input and returns the curve value.
+
+USE CurveManage, ONLY: CurveValue
+
+. . .
+
+!~ Get total capacity modifying factor (function of temperature)
+
+!~ for off-rated conditions
+
+50 TotCapTempModFac = \textbf{CurveValue}(DXCoil(DXCoilNum)\%CCapFTemp, ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ InletAirWetbulbC, \& ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ OutDryBulbTemp)
diff --git a/doc/module-developer/src/energyplus-services/psychrometric-services.tex b/doc/module-developer/src/energyplus-services/psychrometric-services.tex
new file mode 100644
index 00000000000..327e1688733
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/psychrometric-services.tex
@@ -0,0 +1,145 @@
+\section{Psychrometric services}\label{psychrometric-services}
+
+EnergyPlus has a full complement of psychrometric functions. All the routines are Fortran functions returning a single precision real value.~ All arguments and results are in SI units.
+
+Note that each of the psychrometric routines has a ``calledfrom'' optional parameter -- this has been implemented in some of the calling routines and is useful when errors are detected during simulation for support personnel to figure out where the psych routine is called from.
+
+The Names for the different Psychrometric Routines are based on the following self-explanatory format; the different variables used in the Psych Routine taxonomy are as follows.
+
+\begin{itemize}
+\tightlist
+\item
+  H = Enthalpy
+\item
+  W = Humidity Ratio
+\item
+  Rh = Relative Humidity
+\item
+  V = Specific Volume
+\item
+  Rhov = Vapor Density of Air
+\item
+  Hfg = Latent energy (heat of vaporization for moist air)
+\item
+  Hg = Enthalpy of gaseous moisture
+\item
+  Pb = Barometric Pressure
+\item
+  Twb = Temperature Wet Bulb
+\item
+  Twd = Temperature Dry Bulb
+\item
+  Tdp = Temperature Dew Point
+\item
+  Tsat and Psat = Saturation Temperature and Saturation Pressure
+\item
+  Psy\#\# Fn \#\#~~~~ = Psy \{\#\# is a Function of~ \#\#\}
+\item
+  Note: Each of the two capital alphabets together have different meaning
+\end{itemize}
+
+~~~~~~ Eg:~~~~ \textbf{\{Psy \#\# Fn HW\} = \{Psy \#\# Function of~ \emph{Enthalpy and Humidity Ratio}\}}
+
+\subsection{PsyRhoAirFnPbTdbW (Pb,Tdb,W,calledfrom)}\label{psyrhoairfnpbtdbw-pbtdbwcalledfrom}
+
+Returns the density of air in kilograms per cubic meter as a function of barometric pressure {[}Pb{]} (in Pascals), dry bulb temperature {[}Tdb{]} (in Celsius), and humidity ratio {[}W{]} (kilograms of water per kilogram of dry air).
+
+\subsection{PsyCpAirFnWTdb (W,Tdb,calledfrom)}\label{psycpairfnwtdb-wtdbcalledfrom}
+
+Returns the specific heat of air in Joules per kilogram degree Celsius as a function of humidity ratio {[}W{]} (kilograms of water per kilogram of dry air) and dry bulb temperature {[}Tdb{]} (Celsius).
+
+\subsection{PsyHfgAirFnWTdb (W,Tdb,calledfrom)}\label{psyhfgairfnwtdb-wtdbcalledfrom}
+
+Returns the Latent energy of air \href{Joules\%20per\%20kilogram}{Hfg} as a function of humidity ratio {[}W{]} (kilograms of water per kilogram of dry air) and dry bulb temperature {[}Tdb{]} (Celsius).~ It calculates hg and then hf and the difference is Hfg.
+
+\subsection{PsyHgAirFnWTdb (W,Tdb,calledfrom)}\label{psyhgairfnwtdb-wtdbcalledfrom}
+
+Returns the specific enthalpy of the moisture as a gas in the air in Joules per kilogram as a function of humidity ratio {[}W{]} (kilograms of water per kilogram of dry air) and dry bulb temperature {[}Tdb{]} (Celsius).
+
+\subsection{PsyTdpFnTdbTwbPb (Tdb,Twb,Pb,calledfrom)}\label{psytdpfntdbtwbpb-tdbtwbpbcalledfrom}
+
+Returns the dew point temperature in Celsius as a function of dry bulb temperature {[}Tdb{]} (Celsius), wet bulb temperature {[}Twb{]} (Celsius), and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyTdpFnWPb (W,Pb,calledfrom)}\label{psytdpfnwpb-wpbcalledfrom}
+
+Returns the dew point temperature in Celsius as a function of humidity ratio {[}W{]} (kilograms of water per kilogram of dry air) and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyHFnTdbW (Tdb,W,calledfrom)}\label{psyhfntdbw-tdbwcalledfrom}
+
+Returns the specific enthalpy of air in Joules per kilogram as a function of dry bulb temperature {[}Tdb{]} (Celsius) and humidity ratio {[}W{]} (kilograms of water per kilogram of dry air).
+
+\subsection{PsyHFnTdbRhPb (Tdb,Rh,Pb,calledfrom)}\label{psyhfntdbrhpb-tdbrhpbcalledfrom}
+
+Returns the specific enthalpy of air in Joules per kilogram as a function of dry bulb temperature {[}Tdb{]} (Celsius), relative humidity {[}Rh{]} (fraction), and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyTdbFnHW~ (H,W,calledfrom)}\label{psytdbfnhw-hwcalledfrom}
+
+Returns the air temperature in Celsius as a function of air specific enthalpy {[}H{]} (Joules per kilogram) and humidity ratio {[}W{]} (kilograms of water per kilogram of dry air).
+
+\subsection{PsyRhovFnTdbRh (Tdb,Rh,calledfrom)}\label{psyrhovfntdbrh-tdbrhcalledfrom}
+
+Returns the Vapor Density in air \href{kilograms\%20of\%20water\%20per\%20cubic\%20meter\%20of\%20air}{RhoVapor} as a function of dry bulb temperature \href{Celcius}{Tdb}, Relative Humidity {[}Rh{]} (fraction).
+
+\subsection{PsyRhovFnTdbWP (Tdb,W,Pb,calledfrom)}\label{psyrhovfntdbwp-tdbwpbcalledfrom}
+
+Returns the Vapor Density in air \href{kilograms\%20of\%20water\%20per\%20cubic\%20meter\%20of\%20air}{RhoVapor} as a function of dry bulb temperature \href{Celcius}{Tdb}, humidity ratio {[}W{]} (kilograms of water per kilogram of dry air) and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyRhFnTdbRhov (Tdb,Rhov,calledfrom)}\label{psyrhfntdbrhov-tdbrhovcalledfrom}
+
+Returns the Relative Humidity {[}Rh{]} (fraction) in air as a function of dry bulb temperature {[}Tdb{]} (Celcius) and Vapor Density in air \href{kilograms\%20of\%20water\%20per\%20cubic\%20meter\%20of\%20air}{RhoVapor}.
+
+\subsection{PsyRhFnTdbWPb (Tdb,W,Pb,calledfrom)}\label{psyrhfntdbwpb-tdbwpbcalledfrom}
+
+Returns the relative humifity (fraction) as a function of of dry bulb temperature {[}Tdb{]} (Celsius), humidity ratio {[}W{]} (kilograms of water per kilogram of dry air) and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyTwbFnTdbWPb (Tdb,W,Pb,calledfrom)}\label{psytwbfntdbwpb-tdbwpbcalledfrom}
+
+Returns the air wet bulb temperatute in Celsius as a function of dry bulb temperature {[}Tdb{]} (Celsius), humidity ratio {[}W{]} (kilograms of water per kilogram of dry air) and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyVFnTdbWPb (Tdb,W,Pb,calledfrom)}\label{psyvfntdbwpb-tdbwpbcalledfrom}
+
+Returns the specific volume in cubic meters per kilogram as a function of dry bulb temperature {[}Tdb{]} (Celsius), humidity ratio {[}W{]} (kilograms of water per kilogram of dry air) and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyWFnTdpPb (Tdp,Pb,calledfrom)}\label{psywfntdppb-tdppbcalledfrom}
+
+Returns the humidity ratio in kilograms of water per kilogram of dry air as a function of the dew point temperature {[}Tdp{]} (Celsius) and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyWFnTdbH (Tdb,H,calledfrom)}\label{psywfntdbh-tdbhcalledfrom}
+
+Returns the humidity ratio in kilograms of water per kilogram of dry air as a function of dry bulb temperature {[}Tdb{]} (Celsius) and air specific enthalpy {[}H{]} (Joules per kilogram).
+
+\subsection{PsyWFnTdbTwbPb (Tdb,Twb,Pb,calledfrom)}\label{psywfntdbtwbpb-tdbtwbpbcalledfrom}
+
+Returns the humidity ratio in kilograms of water per kilogram of dry air as a function of dry bulb temperature {[}Tdb{]} (Celsius), wet bulb temperature {[}Twb{]} (Celsius), and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyWFnTdbRhPb (Tdb,Rh,Pb,calledfrom)}\label{psywfntdbrhpb-tdbrhpbcalledfrom}
+
+Returns the humidity ratio in kilograms of water per kilogram of dry air as a function of dry bulb temperature {[}Tdb{]} (Celsius), relative humidity {[}RH{]} (fraction), and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyPsatFnTemp (T,calledfrom)}\label{psypsatfntemp-tcalledfrom}
+
+Returns the saturation pressure in Pascals as a function of the air saturation temperature {[}T{]} (Celsius).
+
+\subsection{PsyTsatFnHPb~ (H,Pb,calledfrom)}\label{psytsatfnhpb-hpbcalledfrom}
+
+Returns the air saturation temperature in Celsius as a function of air specific enthalpy {[}H{]} (Joules per kilogram) and barometric pressure {[}Pb{]} (Pascals).
+
+\subsection{PsyTsatFnPb (P,calledfrom)}\label{psytsatfnpb-pcalledfrom}
+
+Returns the air saturation temperature in Celsius as a function of saturation pressure {[}P{]} (Pascals).
+
+\subsection{CPCW (Temp,calledfrom)}\label{cpcw-tempcalledfrom}
+
+Returns Specific heat capacity~~ (Joule/kilogram/kelvin) for chilled water as function of temperature {[}T{]} (Celsius).
+
+\subsection{CPHW (Temp,calledfrom)}\label{cphw-tempcalledfrom}
+
+Returns Specific heat capacity (Joule/kilogram/kelvin) for hot water as function of temperature {[}T{]} (Celsius).
+
+\subsection{CVHW (Temp,calledfrom)}\label{cvhw-tempcalledfrom}
+
+Returns Specific heat capacity (Joule/kilogram/kelvin) for hot water at constant volume as function of temperature {[}T{]} (Celsius).
+
+\subsection{RhoH2O (Temp,calledfrom)}\label{rhoh2o-tempcalledfrom}
+
+Returns density of water (kg/m3) as function of Temperature {[}T{]} (Celsius).
diff --git a/doc/module-developer/src/energyplus-services/schedule-services.tex b/doc/module-developer/src/energyplus-services/schedule-services.tex
new file mode 100644
index 00000000000..bbd78e2f8ef
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/schedule-services.tex
@@ -0,0 +1,277 @@
+\section{Schedule Services}\label{schedule-services}
+
+Schedules are widely used in specifying input for building simulation programs. For instance heat gains from lighting, equipment and occupancy are usually specified using schedules. Schedules are used to indicate when equipment is on or off. Schedules are also used to specify zone and system set points. EnergyPlus uses schedules in all these ways and provides services that make using schedules very easy for the developer.
+
+Schedules are specified in a three level hierarchy in EnergyPlus input.
+
+\textbf{Day Schedules} (IDD Objects: Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List)
+
+\textbf{Week Schedules} (IDD Objects: Schedule:Week:Daily, Schedule:Week:Compact)
+
+\textbf{Annual Schedules} (IDD Objects: Schedule:Year, Schedule:Compact, Schedule:File)
+
+In addition, a \textbf{ScheduleTypeLimits} object can specify certain limits on the schedules.~ This is a mostly optional input but can be used effectively.~ (That is, if your examples include it, users will probably use it too.)
+
+An example from an input (IDF) file:
+
+~ \textbf{ScheduleTypeLimits},
+
+~~~ Fraction,~ !- ScheduleType Name
+
+~~~ 0.0 : 1.0,~ !- range
+
+~~~ CONTINUOUS;~ !- Numeric Type
+
+~ \textbf{ScheduleTypeLimits},
+
+~~~ On/Off,~ !- ScheduleType Name
+
+~~~ 0:1,~ !- range
+
+~~~ DISCRETE;~ !- Numeric Type
+
+! Schedule Constant
+
+~ \textbf{SCHEDULE:COMPACT},
+
+~ Constant,
+
+~ on/off,
+
+~ Through: 12/31,
+
+~ For: AllDays,
+
+~ Until: 24:00, 1.0;
+
+! Schedule Daytime Ventilation
+
+~ \textbf{SCHEDULE:COMPACT},
+
+~ Daytime Ventilation,
+
+~ Fraction,
+
+~ Through: 12/31,
+
+~ For: Weekdays SummerDesignDay,
+
+~ Until: 08:00, 0.0,
+
+~ Until: 18:00, 1.0,
+
+~ Until: 24:00, 0.0,
+
+~ For: Weekends WinterDesignDay,
+
+~ Until: 10:00, 0.0,
+
+~ Until: 16:00, 1.0,
+
+~ Until: 24:00, 0.0,
+
+~ For: Holidays AllOtherDays,
+
+~ Until: 24:00, 0.0;
+
+! Schedule Intermittent
+
+~ \textbf{SCHEDULE:COMPACT},
+
+~ Intermittent,
+
+~ Fraction,
+
+~ Through: 12/31,
+
+~ For: AllDays,
+
+~ Until: 08:00, 0.0,
+
+~ Until: 18:00, 1.0,
+
+~ Until: 24:00, 0.0;
+
+The day schedule elements assign numbers that span a full day (24 hours). The week schedule elements indicate which day schedules are applicable to each day of the week plus holiday and some special days. Schedule elements indicate which week schedules are applicable to various periods of the year. Both day schedules and schedules reference a schedule type. A schedule type is characterized by a range (e.g.~0 to 1) and whether it is continuous (can assume any value) or discrete (can assume integer values only). The following routines from the ScheduleManager module enable the developer to use schedules in a simulation.
+
+\subsection{GetScheduleIndex}\label{getscheduleindex}
+
+This function takes a schedule name as input and returns an internal pointer to the schedule. Schedule values will always be accessed via the pointer not the name during the simulation for reasons of efficiency. This function should be called once for each schedule during the input phase and the returned value stored in the appropriate data structure.
+
+Example:
+
+USE ScheduleManager, ONLY: GetScheduleIndex
+
+. . .
+
+Baseboard(BaseboardNum)\%SchedPtr = \textbf{GetScheduleIndex}(AlphArray(2))
+
+Here the schedule pointer for the schedule name contained in AlphArray(2) is stored in the baseboard data structure for later use.~ If a 0 is returned, this is not a valid schedule.~ Objects should also typically check for ``blank'' schedules.
+
+\subsection{GetDayScheduleIndex}\label{getdayscheduleindex}
+
+This function takes a ``day schedule'' name as input and returns an internal pointer to the schedule. Day schedule values will always be accessed via the pointer not the name during the simulation for reasons of efficiency. This function should be called once for each schedule during the input phase and the returned value stored in the appropriate data structure.
+
+Example:
+
+USE ScheduleManager, ONLY: GetDayScheduleIndex
+
+. . .~~~~~~~ DesDayInput(EnvrnNum)\%RelHumSchPtr = GetDayScheduleIndex(DDNames(4))
+
+Here the day schedule pointer for the day schedule name contained in DDNames(4) is stored in the design day data structure for later use.~ If a 0 is returned, this is not a valid day schedule.~ Objects should also typically check for ``blank'' schedules.
+
+\subsection{CheckScheduleValueMinMax}\label{checkschedulevalueminmax}
+
+Since you can't always rely on a user to input the ScheduleType, the ScheduleManager can be used to check the minimum and/or maximum values for a schedule.
+
+LOGICAL FUNCTION \textbf{CheckScheduleValueMinMax}(ScheduleIndex,~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~ MinString,Minimum,MaxString,Maximum)
+
+The pair of specifications (MinString, Minimum) and (MaxString, Maximum) is optional -- only one set need be given.
+
+Examples from the code:
+
+USE ScheduleManager, ONLY: CheckScheduleValueMinMax
+
+. . .
+
+IF (.NOT. \textbf{CheckScheduleValueMinMax}(ScheduleIndex,`\textgreater{} =',0.,`\textless{} =',1.)) THEN
+
+~ CALL ShowSevereError(RoutineName//trim(currentModuleObject)//','//~ \&
+
+~~~ Trim(cAlphaFieldName(3))//'..')
+
+~ CALL ShowContinueError(`Error found in schedule ='//TRIM(Alphas(3)))
+
+~ CALL ShowContinueError(`setpoint values must be (\textgreater{} = 0., \textless{} = 1.)')
+
+~ ErrorsFound = .true.
+
+END IF
+
+\subsection{CheckScheduleValue}\label{checkschedulevalue}
+
+There are times when the ``CheckScheduleValueMinMax'' will not be sufficient to verify proper values.~ A good example is the ``control type'' schedules -- valid values might be 0 through 4, but just checking the min/max will not tell you if it contains a specific value (say, 3).~ This function allows you to check the entire schedule for a specific value -- this will be more useful for discrete schedules than for schedule types of a continuous nature but can be used for both.
+
+LOGICAL FUNCTION CheckScheduleValue(ScheduleIndex,Value)
+
+Example of use:
+
+~IF (\textbf{CheckScheduleValue}(CTIndex,REAL(SingleHeatingSetPoint))) THEN
+
+Here, the CTIndex is a schedule index for the Control Type schedules.~ SingleHeatingSetPoint is an integer value for that control type.~ ``CheckScheduleValue'' is used to determine if the schedule does, in fact, contain that value.
+
+\subsection{GetScheduleMinValue}\label{getscheduleminvalue}
+
+There are times when you don't necessarily want to issue an error message but might like to find out what the minimum value of a given schedule is.~ For example, if the schedule allowed for \textgreater{}1 multipliers on a given input.
+
+FUNCTION GetScheduleMinValue(ScheduleIndex) RESULT(MinimumValue)
+
+Example of use:
+
+USE ScheduleManager, ONLY: GetScheduleMinValue
+
+. . .
+
+Value = \textbf{GetScheduleMinValue}(ScheduleIndex)
+
+The only argument needed is the ScheduleIndex for the schedule.~ Note that all schedule values are stored as real numbers -- if you have a discrete/integer valued schedule, you may wish to do some special checking of the min value.
+
+\subsection{GetScheduleMaxValue}\label{getschedulemaxvalue}
+
+There are times when you don't necessarily want to issue an error message but might like to find out what the maximum value of a given schedule is.~ For example, if the schedule allowed for \textgreater{}1 multipliers on a given input.
+
+FUNCTION GetScheduleMaxValue(ScheduleIndex) RESULT(MaximumValue)
+
+Example of use:
+
+USE ScheduleManager, ONLY: GetScheduleMaxValue
+
+. . .
+
+Value = \textbf{GetScheduleMaxValue}(ScheduleIndex)
+
+The only argument needed is the ScheduleIndex for the schedule.~ Note that all schedule values are stored as real numbers -- if you have a discrete/integer valued schedule, you may wish to do some special checking of the min value.
+
+\subsection{GetCurrentScheduleValue}\label{getcurrentschedulevalue}
+
+This function returns the current schedule value for the current day and time, given the schedule pointer as input.
+
+REAL FUNCTION GetCurrentScheduleValue(ScheduleIndex)
+
+Example of use:
+
+USE ScheduleManager, ONLY: GetCurrentScheduleValue
+
+. . .
+
+CloUnit = \textbf{GetCurrentScheduleValue}(People(PeopleNum)\%ClothingPtr)
+
+Notice that the developer doesn't have to keep track of hour of the day, day of the month, or month. The program does all of that. The only input needed is the pointer to the schedule.
+
+\subsection{GetScheduleValuesForDay}\label{getschedulevaluesforday}
+
+This function returns the schedule values for a specific day, given the schedule index as input.
+
+SUBROUTINE GetScheduleValuesForDay(ScheduleIndex,DayValues,JDay)
+
+Example of use:
+
+~~~ ALLOCATE(SVals1(24,NumOfTimeStepInHour))
+
+~~~ SVals1 = 0.0
+
+~~~ \ldots{}
+
+~~~~~~~ DO JDay = 1,366
+
+~~~~~~~~~ CALL \textbf{GetScheduleValuesForDay}(CrossMixing(Loop)\%SchedPtr,~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ~~~~~~~~~~SVals1,JDay)
+
+~~~~~~~~~ IF (.not. ANY(SVals1\textgreater{}0.0)) CYCLE
+
+~~~~~~~ \ldots{}
+
+~~~~~~~ END DO
+
+\subsection{GetSingleDayScheduleValues}\label{getsingledayschedulevalues}
+
+This function returns the schedule values for a specific day schedule (used in Design Day input, for example).
+
+SUBROUTINE GetSingleDayScheduleValues(DayScheduleIndex,DayValues)
+
+Example of use:
+
+~~ ALLOCATE (DDRelHumValues(TotDesDays,24,NumOfTimeStepInHour))
+
+~~ DDRelHumValues = 0.0
+
+~~ \ldots{}
+
+~~~ CALL \textbf{GetSingleDayScheduleValues}(DesDayInput(EnvrnNum)\%RelHumSchPtr, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ DDRelHumValues(EnvrnNum,:,:))
+
+\subsection{LookUpScheduleValue}\label{lookupschedulevalue}
+
+This function can be used to look up a schedule value for the current time or optionally for any specific hour, timestep, day of year.
+
+REAL FUNCTION LookUpScheduleValue(ScheduleIndex, ThisHour, ThisTimeStep, ThisDayOfYear)
+
+\ldots{}
+
+~~~~~~~~~ ! FUNCTION ARGUMENT DEFINITIONS:
+
+~ INTEGER ScheduleIndex
+
+~ INTEGER, OPTIONAL :: ThisHour
+
+~ INTEGER, OPTIONAL :: ThisTimeStep
+
+~ INTEGER, OPTIONAL :: ThisDayOfYear
+
+Example of use:
+
+~~~~~ SchValue = \textbf{LookUpScheduleValue}(Surface(SNR)\%SchedShadowSurfIndex,IHOUR,TS)
diff --git a/doc/module-developer/src/energyplus-services/tabular-output-utilities.tex b/doc/module-developer/src/energyplus-services/tabular-output-utilities.tex
new file mode 100644
index 00000000000..0a42cbb73e3
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/tabular-output-utilities.tex
@@ -0,0 +1,19 @@
+\section{Tabular Output Utilities}\label{tabular-output-utilities}
+
+Several utility routines are available to help generate tabular reports. To create tabular reports, the developer needs to create a routine called something like WriteTabularX.~ The WriteTabularX routine should appear in SimulationManger between the OpenOutputTabularFile and CloseOutputTabularFile calls.~ The WriteTabularX routine should make use of several utilities described below.~ The ``USE'' statement reference OutputReportTabular module.~ Good example of how to use this facility are in the OutputReportTabular file and the EconomicTariff file.
+
+\subsection{WriteReportHeaders(reportName,objectName,averageOrSum)}\label{writereportheadersreportnameobjectnameaverageorsum}
+
+Where reportName is the name that you want the report to be called and the objectName is the name of the object that appears after the ``For: `` for each instance of the report. The averageOrSum flag when set to SUM adds the phrase ``per second'' after the reportName.
+
+\subsection{WriteSubtitle(subtitle)}\label{writesubtitlesubtitle}
+
+Where the subtitle is a string that usually appears before a specific table. This is useful if the report includes multiple tables.
+
+\subsection{WriteTable(body,rowLabels,columnLabels,widthColumn)}\label{writetablebodyrowlabelscolumnlabelswidthcolumn}
+
+The WriteTable routine actually generates the tables that appear in the tabular output file (CSV, HTML, or TXT).~ The rowLabels and columnLables are both one dimensional string arrays that contain the appropriate labels. If the column labels strings include the vertical bar symbol ``\textbar{}'' then when creating a text report, the labels will be split between lines at the vertical bar.~ For HTML and CSV output, the vertical bar symbols are removed prior to display.
+
+The body array is a two dimensional array (row,column order) containing the cells in the body of the table.~ It must be strings so conversion utilities such as RealToStr should be used to convert from numeric values.
+
+WidthColumn is a one dimensional integer array containing the column widths for use only with the fixed width text output option.
diff --git a/doc/module-developer/src/energyplus-services/utility-routines-functions.tex b/doc/module-developer/src/energyplus-services/utility-routines-functions.tex
new file mode 100644
index 00000000000..3c91e07586d
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/utility-routines-functions.tex
@@ -0,0 +1,257 @@
+\section{Utility Routines/Functions}\label{utility-routinesfunctions}
+
+EnergyPlus supplies an extensive set of routines to help module developers get input, check values, get schedule values, get and check nodes.~ These are summarized in the following table and in more detail in the following sections.~ The table indicates the routine/function name, times of most likely use, and the module (if applicable) that you must USE in the code in order to make the routine available to you.~ Most of the items mentioned in this table are of particular use in ``GetInput'' processing.~ A few later tables will highlight similar functions/routines for simulation purposes.
+
+Table 2.~ Table of Utility Functions
+
+Routine/Function Name
+
+Use during
+
+Module
+
+GetNumObjectsFound
+
+``GetInput'' Processing
+
+InputProcessor
+
+GetObjectItem
+
+``GetInput'' Processing
+
+InputProcessor
+
+GetObjectDefMaxArgs
+
+``GetInput'' Processing
+
+InputProcessor
+
+GetObjectItemNum
+
+``GetInput'' Processing
+
+InputProcessor
+
+FindItemInList
+
+``GetInput'' Processing (best) though some are currently used in Simulation
+
+InputProcessor
+
+FindItem
+
+``GetInput'' Processing
+
+InputProcessor
+
+FindItemInSortedList
+
+``Special processing'' -- list must be sorted.
+
+InputProcessor
+
+SameString
+
+``GetInput'' Processing
+
+InputProcessor
+
+VerifyName
+
+``GetInput'' Processing
+
+InputProcessor
+
+RangeCheck
+
+``GetInput'' Processing
+
+InputProcessor
+
+MakeUPPERCase
+
+``GetInput'' Processing
+
+InputProcessor
+
+GetOnlySingleNode
+
+``GetInput'' Processing
+
+NodeInputManager
+
+GetNodeNums
+
+``GetInput'' Processing
+
+NodeInputManager
+
+InitUniqueNodeCheck, CheckUniqueNodes, EndUniqueNodeCheck
+
+``GetInput'' Processing
+
+NodeInputManager
+
+SetupCompSets
+
+``GetInput'' Processing
+
+NodeInputManager
+
+TestCompSets
+
+``GetInput'' Processing
+
+NodeInputManager
+
+GetNewUnitNumber
+
+(automatically retrieve an available unit number)
+
+EXTERNAL integer function
+
+FindUnitNumber
+
+Find a unit number when you know the name of the file
+
+EXTERNAL integer function
+
+FindNumberinList
+
+``GetInput'' Processing/Init processing
+
+EXTERNAL integer function
+
+ValidateComponent
+
+``GetInput'' Processing
+
+Subroutine CALL
+
+CheckComponent
+
+``GetInput'' Processing -- like ValidateComponent but doesn't generate error message if failure
+
+Subroutine CALL
+
+CreateSysTimeIntervalString
+
+Simulation -- Error Messages
+
+General
+
+TrimSigDigits
+
+Simulation -- Error Messages
+
+General
+
+RoundSigDigits
+
+Simulation -- Error Messages
+
+General
+
+GetScheduleIndex
+
+``GetInput'' Processing
+
+ScheduleManager
+
+GetDayScheduleIndex
+
+``GetInput'' Processing
+
+ScheduleManager
+
+GetCurrentScheduleValue
+
+Simulation
+
+ScheduleManager
+
+GetScheduleValuesForDay
+
+Simulation
+
+ScheduleManager
+
+GetSingleDayScheduleValues
+
+Simulation/''GetInput''
+
+ScheduleManager
+
+CheckScheduleValueMinMax
+
+``GetInput'' Processing
+
+ScheduleManager
+
+CheckScheduleValue
+
+``GetInput'' Processing
+
+ScheduleManager
+
+GetScheduleMinValue
+
+``GetInput'' Processing
+
+ScheduleManager
+
+GetScheduleMaxValue
+
+``GetInput'' Processing
+
+ScheduleManager
+
+LookUpScheduleValue
+
+Simulation
+
+ScheduleManager
+
+CheckOutAirNodeNumber
+
+``GetInput'' Processing
+
+OutAirNodeManager
+
+GetCurveIndex
+
+``GetInput'' Processing
+
+CurveManager
+
+GetCurveCheck
+
+``GetInput'' Processing
+
+CurveManager
+
+GetCurveType
+
+``GetInput'' Processing
+
+CurveManager
+
+CurveValue
+
+Simulation
+
+CurveManager
+
+SetupAndSort
+
+Sorting lists of character values
+
+SortAndStringUtilities
+
+SetupZoneInternalGain
+
+``GetInput'' Processing
+
+DataInterfaces
diff --git a/doc/module-developer/src/energyplus-services/weather-services.tex b/doc/module-developer/src/energyplus-services/weather-services.tex
new file mode 100644
index 00000000000..0b92fd1bd5d
--- /dev/null
+++ b/doc/module-developer/src/energyplus-services/weather-services.tex
@@ -0,0 +1,3 @@
+\section{Weather Services}\label{weather-services}
+
+All weather data (including SizingPeriod:DesignDay and Site:Location validation) are processed by the WeatherManager module.~ The SimulationManager invokes the WeatherManager at the proper times to retrieve data.~ The WeatherManager will retrieve the proper data for the current timestep/hour/day/month from the proper data source (design day definition, weather data file).~ The WeatherManager puts weather-type data (outside dry bulb, outside wet bulb, humidity, barometric pressure) into the DataEnvironment global data area.~ There is no need for other modules to call the WeatherManager directly.~ However, if there is some weather-type data that is needed and not provided in the DataEnvironment global area, contact us.
diff --git a/doc/module-developer/src/guide-for-module-developers.tex b/doc/module-developer/src/guide-for-module-developers.tex
new file mode 100644
index 00000000000..63f37402bb8
--- /dev/null
+++ b/doc/module-developer/src/guide-for-module-developers.tex
@@ -0,0 +1 @@
+\input{../title}
diff --git a/doc/module-developer/src/hvac-network.tex b/doc/module-developer/src/hvac-network.tex
new file mode 100644
index 00000000000..aff95dd01e1
--- /dev/null
+++ b/doc/module-developer/src/hvac-network.tex
@@ -0,0 +1 @@
+\chapter{HVAC Network}\label{hvac-network}
diff --git a/doc/module-developer/src/hvac-network/branches-connectors-and-nodes.tex b/doc/module-developer/src/hvac-network/branches-connectors-and-nodes.tex
new file mode 100644
index 00000000000..1df46d99bbc
--- /dev/null
+++ b/doc/module-developer/src/hvac-network/branches-connectors-and-nodes.tex
@@ -0,0 +1,263 @@
+\section{Branches, Connectors, and Nodes}\label{branches-connectors-and-nodes}
+
+In EnergyPlus, the HVAC system and plant form a network (technically, a graph). The individual pieces of equipment -- the fans, coils, chillers, etc. -- are connected together by air ducts and fluid pipes. In EnergyPlus nomenclature, the air and fluid circuits are called loops. Specifying how an individual system and plant are connected is done in the EnergyPlus input (IDF) file. The overall structure of the network is defined with Branch and Connector objects. The detail is filled with components and their inlet and outlet nodes. A Branch consists of one or more components arranged sequentially along a pipe or duct. A Connector specifies how three or more branches are connected through a Splitter or Mixer. Nodes connect components along a branch: the outlet node of one component is the inlet node of the next downstream component. The nodes represent conditions at a point on a loop. Each component has one or more inlet and outlet nodes, depending on how many loops it interacts with. A fan, for instance, has one inlet node and one outlet node, since it interacts with a single air loop. A water coil will have 2 inlet and 2 outlet nodes, since it interacts with an air and a fluid loop. Figure~\ref{fig:hvac-input-diagram} shows a diagram of an EnergyPlus HVAC input.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image002.png}
+\caption{  HVAC Input Diagram \protect \label{fig:hvac-input-diagram}}
+\end{figure}
+
+As an illustration of how such a network is built up on the IDF, here is the section of the IDF that describes the supply fan, splitter, and heating and cooling coil section of the dual duct air system.
+
+\textbf{BranchList,}
+
+~~~ Dual Duct Air Loop Branches,~ !- Name
+
+~~~ Air Loop Main Branch,~~~ !- Branch 1 Name
+
+~~~ Heating Coil Air Sys Branch,~ !- Branch 2 Name
+
+~~~ Cooling Coil Air Sys Branch;~ !- Branch 3 Name
+
+\textbf{ConnectorList,}
+
+~~~ Dual Duct Connectors,~~~ !- Name
+
+~~~ Connector:Splitter,~~~~~ !- Connector 1 Object Type
+
+~~~ DualDuctAirSplitter;~~~~ !- Connector 1 Name
+
+\textbf{NodeList,}
+
+~~~ Zone Equipment Inlet Node List,~ !- Name
+
+~~~ Main Hot Air Inlet,~~~~~ !- Node 1 Name
+
+~~~ Main Cold Air Inlet;~~~~ !- Node 2 Name
+
+\textbf{NodeList,}
+
+~~~ Air Loop Outlet Node List,~ !- Name
+
+~~~ Heating Coil Outlet Node,!- Node 1 Name
+
+~~~ Cooling Coil Outlet Node;!- Node 2 Name
+
+\textbf{Branch,}
+
+~~~ Air Loop Main Branch,~~~ !- Name
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Maximum Flow Rate \{m3/s\}
+
+~~~ Fan:ConstantVolume,~~~~~ !- Component 1 Object Type
+
+~~~ Supply Fan 1,~~~~~~~~~~~ !- Component 1 Name
+
+~~~ Supply Fan Inlet Node,~~ !- Component 1 Inlet Node Name
+
+~~~ Supply Fan Outlet Node,~ !- Component 1 Outlet Node Name
+
+~~~ PASSIVE;~~~~~~~~~~~~~~~~ !- Component 1 Branch Control Type
+
+\textbf{Branch,}
+
+~~~ Heating Coil Air Sys Branch,~ !- Name
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Maximum Flow Rate \{m3/s\}
+
+~~~ Coil:Heating:Water,~~~~~ !- Component 1 Object Type
+
+~~~ Main Heating Coil,~~~~~~ !- Component 1 Name
+
+~~~ Heating Coil Inlet Node, !- Component 1 Inlet Node Name
+
+~~~ Heating Coil Outlet Node,!- Component 1 Outlet Node Name
+
+~~~ ACTIVE;~~~~~~~~~~~~~~~~~ !- Component 1 Branch Control Type
+
+\textbf{Branch,}
+
+~~~ Cooling Coil Air Sys Branch,~ !- Name
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Maximum Flow Rate \{m3/s\}
+
+~~~ Coil:Cooling:Water,~~~~~ !- Component 1 Object Type
+
+~~~ Simple Cooling Coil,~~~~ !- Component 1 Name
+
+~~~ Cooling Coil Inlet Node, !- Component 1 Inlet Node Name
+
+~~~ Cooling Coil Outlet Node,!- Component 1 Outlet Node Name
+
+~~~ ACTIVE;~~~~~~~~~~~~~~~~~ !- Component 1 Branch Control Type
+
+\textbf{Connector:Splitter,}
+
+~~~ DualDuctAirSplitter,~~~~ !- Name
+
+~~~ Air Loop Main Branch,~~~ !- Inlet Branch Name
+
+~~~ Heating Coil Air Sys Branch,~ !- Outlet Branch 1 Name
+
+~~~ Cooling Coil Air Sys Branch;~ !- Outlet Branch 2 Name
+
+\textbf{Fan:ConstantVolume,}
+
+~~~ Supply Fan 1,~~~~~~~~~~~ !- Name
+
+~~~ FanAndCoilAvailSched,~~~ !- Availability Schedule Name
+
+~~~ 0.7,~~~~~~~~~~~~~~~~~~~~ !- Fan Efficiency
+
+~~~ 600.0,~~~~~~~~~~~~~~~~~~ !- Pressure Rise \{Pa\}
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Maximum Flow Rate \{m3/s\}
+
+~~~ 0.9,~~~~~~~~~~~~~~~~~~~~ !- Motor Efficiency
+
+~~~ 1.0,~~~~~~~~~~~~~~~~~~~~ !- Motor In Airstream Fraction
+
+~~~ Supply Fan Inlet Node,~~ !- Fan Inlet Node Name
+
+~~~ Supply Fan Outlet Node;~ !- Fan Outlet Node Name
+
+\textbf{Coil:Cooling:Water,}
+
+~~~ Simple Cooling Coil,~~~~ !- Name
+
+~~~ CoolingCoilAvailSched,~~ !- Availability Schedule Name
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Design Water Flow Rate \{m3/s\}
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Design Air Flow Rate \{m3/s\}
+
+~~~ autosize,~~~~~~~~ !- Design Inlet Water Temperature \{C\}
+
+~~~ autosize,~~~~~~~~ !- Design Inlet Air Temperature \{C\}
+
+~~~ autosize,~~~~~~~~ !- Design Outlet Air Temperature \{C\}
+
+~~~ autosize,~~~~ !- Design Inlet Air Humidity Ratio \{kg-H2O/kg-air\}
+
+~~~ autosize,~~~~ !- Design Outlet Air Humidity Ratio \{kg-H2O/kg-air\}
+
+~~~ Cooling Coil Water Inlet Node,~ !- Water Inlet Node Name
+
+~~~ Cooling Coil Water Outlet Node,~ !- Water Outlet Node Name
+
+~~~ Cooling Coil Inlet Node, !- Air Inlet Node Name
+
+~~~ Cooling Coil Outlet Node,!- Air Outlet Node Name
+
+~~~ SimpleAnalysis,~~~~~~~~~ !- Type of Analysis
+
+~~~ CrossFlow;~~~~~~~~~~~~~~ !- Heat Exchanger Configuration
+
+\textbf{AirLoopHVAC:ZoneSplitter,}
+
+~~~ ZoneColdAirSupplySplitter,~ !- Name
+
+~~~ Main Cold Air Inlet,~~~~ !- Inlet Node Name
+
+~~~ Zone 1 Dual Duct Cold Inlet,~ !- Outlet 1 Node Name
+
+~~~ Zone 2 Dual Duct Cold Inlet,~ !- Outlet 2 Node Name
+
+~~~ Zone 3 Dual Duct Cold Inlet;~ !- Outlet 3 Node Name
+
+\textbf{AirLoopHVAC:ZoneSplitter,}
+
+~~~ ZoneHotAirSupplySplitter,!- Name
+
+~~~ Main Hot Air Inlet,~~~~~ !- Inlet Node Name
+
+~~~ Zone 1 Dual Duct Hot Inlet,~ !- Outlet 1 Node Name
+
+~~~ Zone 2 Dual Duct Hot Inlet,~ !- Outlet 2 Node Name
+
+~~~ Zone 3 Dual Duct Hot Inlet;~ !- Outlet 3 Node Name
+
+\textbf{AirLoopHVAC:ZoneMixer,}
+
+~~~ ZoneReturnAirMixer,~~~~~ !- Name
+
+~~~ Return Air Mixer Outlet, !- Outlet Node Name
+
+~~~ Zone 1 Outlet Node,~~~~~ !- Inlet 1 Node Name
+
+~~~ Zone 2 Outlet Node,~~~~~ !- Inlet 2 Node Name
+
+~~~ Zone 3 Outlet Node;~~~~~ !- Inlet 3 Node Name
+
+\textbf{Coil:Heating:Water,}
+
+~~~ Main Heating Coil,~~~~~~ !- Name
+
+~~~ FanAndCoilAvailSched,~~~ !- Availability Schedule Name
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- U-Factor Times Area Value \{W/K\}
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Maximum Water Flow Rate \{m3/s\}
+
+~~~ Heating Coil Water Inlet,!- Water Inlet Node Name
+
+~~~ Heating Coil Water Outlet,~ !- Water Outlet Node Name
+
+~~~ Heating Coil Inlet Node, !- Air Inlet Node Name
+
+~~~ Heating Coil Outlet Node,!- Air Outlet Node Name
+
+~~~ UFactorTimesAreaAndDesignWaterFlowRate,~ !- Performance Input Method
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Nominal Capacity \{W\}
+
+~~~ 82.2,~~~~~~~~~~~~~~~~~~~ !- Design Inlet Water Temperature \{C\}
+
+~~~ 16.6,~~~~~~~~~~~~~~~~~~~ !- Design Inlet Air Temperature \{C\}
+
+~~~ 71.1,~~~~~~~~~~~~~~~~~~~ !- Design Outlet Water Temperature \{C\}
+
+~~~ 32.2;~~~~~~~~~~~~~~~~~~~ !- Design Outlet Air Temperature \{C\}
+
+\textbf{Controller:WaterCoil,}
+
+~~~ Main Cooling Coil Controller,~ !- Name
+
+~~~ Temperature,~~~~~~~~~~~~ !- Control Variable
+
+~~~ Reverse,~~~~~~~~~~~~~~~~ !- Action
+
+~~~ FLOW,~~~~~~~~~~~~~~~~~~~ !- Actuator Variable
+
+~~~ Cooling Coil Outlet Node,!- Sensor Node Name
+
+~~~ Cooling Coil Water Inlet Node, ~!- Actuator Node Name
+
+~~~ 0.001,~~~~~~~~~~~~ !- Controller Convergence Tolerance \{deltaC\}
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Maximum Actuated Flow \{m3/s\}
+
+~~~ 0.0;~~~~~~~~~~~~~~~~~~~~ !- Minimum Actuated Flow \{m3/s\}
+
+\textbf{Controller:WaterCoil,}
+
+~~~ Main Heating Coil Controller,~ !- Name
+
+~~~ Temperature,~~~~~~~~~~~~ !- Control Variable
+
+~~~ Normal,~~~~~~~~~~~~~~~~~ !- Action
+
+~~~ FLOW,~~~~~~~~~~~~~~~~~~~ !- Actuator Variable
+
+~~~ Heating Coil Outlet Node,!- Sensor Node Name
+
+~~~ Heating Coil Water Inlet,!- Actuator Node Name
+
+~~~ 0.01,~~~~~~~~~~~~~ !- Controller Convergence Tolerance \{deltaC\}
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Maximum Actuated Flow \{m3/s\}
+
+~~~ 0.0;~~~~~~~~~~~~~~~~~~~~ !- Minimum Actuated Flow \{m3/s\}
+
+Obviously, the creation of such a system/plant network description is best handled by a graphical user interface (GUI). However, for testing purposes a developer may have to create the input for a component by hand and insert it into an existing IDF. Then the developer must be careful to choose unique names for the branches and nodes and make sure the entire network makes physical sense.
diff --git a/doc/module-developer/src/hvac-network/data-flow-in-an-hvac-component-module.tex b/doc/module-developer/src/hvac-network/data-flow-in-an-hvac-component-module.tex
new file mode 100644
index 00000000000..92334438128
--- /dev/null
+++ b/doc/module-developer/src/hvac-network/data-flow-in-an-hvac-component-module.tex
@@ -0,0 +1,253 @@
+\section{Data Flow in an HVAC Component Module}\label{data-flow-in-an-hvac-component-module}
+
+The data in an EnergyPlus HVAC component module resides in three places.
+
+1.~~~The component inlet nodes -- this is where the data input to the model resides.
+
+2.~~~The component internal data structure(s) -- one or more arrays of data structures which contain all the data needed for the component simulation. This includes data from the input file, data from the inlet nodes, and any schedule values. In addition, these data structure(s) store the results of the calculation.
+
+3.~~~The component outlet nodes -- data is moved from the internal data structure(s) to the outlet nodes at the completion of each component simulation.
+
+The data flows from the inlet nodes into the component internal data structure(s) and then into the outlet nodes. Let us see how this works in our example module Fans.
+
+At the start of the module, the component internal data structure is defined.
+
+TYPE FanEquipConditions
+
+~ CHARACTER(len = MaxNameLength) :: FanName~ ! Name of the fan
+
+~ CHARACTER(len = MaxNameLength) :: FanType~ ! Type of Fan ie. Simple, Vane axial, Centrifugal, etc.
+
+~ CHARACTER(len = MaxNameLength) :: Schedule ! Fan Operation Schedule
+
+~ CHARACTER(len = MaxNameLength) :: Control~ ! ie. Const Vol, Variable Vol
+
+~ Integer~~~~~ :: SchedPtr ! Pointer to the correct schedule
+
+~ REAL(r64)~~~ :: InletAirMassFlowRate~ !MassFlow through the Fan being Simulated {[}kg/Sec{]}
+
+~ REAL(r64)~~~ :: OutletAirMassFlowRate
+
+~ REAL(r64)~~~ :: MaxAirFlowRate~ !Max Specified Volume Flow Rate of Fan {[}m\^{}3/sec{]}
+
+~ REAL(r64)~~~ :: MinAirFlowRate~ !Min Specified Volume Flow Rate of Fan {[}m\^{}3/sec{]}
+
+~ REAL(r64)~~~ :: MaxAirMassFlowRate ! Max flow rate of fan in kg/sec
+
+~ REAL(r64)~~~ :: MinAirMassFlowRate ! Min flow rate of fan in kg/sec
+
+~ REAL(r64)~~~ :: InletAirTemp
+
+~ REAL(r64)~~~ :: OutletAirTemp
+
+~ REAL(r64)~~~ :: InletAirHumRat
+
+~ REAL(r64)~~~ :: OutletAirHumRat
+
+~ REAL(r64)~~~ :: InletAirEnthalpy
+
+~ REAL(r64)~~~ :: OutletAirEnthalpy
+
+~ REAL(r64)~~~ :: FanPower~~~~~~~~~~~~ !Power of the Fan being Simulated {[}kW{]}
+
+~ REAL(r64)~~~ :: FanEnergy~~~~~~~~~~~ !Fan energy in {[}kJ{]}
+
+~ REAL(r64)~~~ :: DeltaTemp~~~~~~~~~~~ !Temp Rise across the Fan {[}C{]}
+
+~ REAL(r64)~~~ :: DeltaPress~~~~~~~~~~ !Delta Pressure Across the Fan {[}N/M\^{}2{]}
+
+~ REAL(r64)~~~ :: FanEff~~~~~~~~~~~~~~ !Fan total efficiency; motor and mechanical
+
+~ REAL(r64)~~~ :: MotEff~~~~~~~~~~~~~~ !Fan motor efficiency
+
+~ REAL(r64)~~~ :: MotInAirFrac~~~~~~~~ !Fraction of motor heat entering air stream
+
+~ REAL(r64), Dimension(5):: FanCoeff~~~~~~~ !Fan Part Load Coefficients to match fan type
+
+~ ! Mass Flow Rate Control Variables
+
+~ REAL(r64)~~~ :: MassFlowRateMaxAvail
+
+~ REAL(r64)~~~ :: MassFlowRateMinAvail
+
+~ INTEGER~~~~~ :: InletNodeNum
+
+~ INTEGER~~~~~ :: OutletNodeNum ~END TYPE FanEquipConditions
+
+!MODULE VARIABLE DECLARATIONS:
+
+~ INTEGER :: NumFans~~~~ ! The Number of Fans found in the Input
+
+~ TYPE (FanEquipConditions), ALLOCATABLE, DIMENSION(:) :: Fan
+
+In this case, there is only one structure that stores all of the fan data. We could have chosen to divide this rather large structure up into separate structures -- one for input file data, one for inlet data, and one for outlet data, for instance. Note that in Fortran 90 structures are called defined type.~ The TYPE -- END TYPE construct defines a new data structure. Then an allocatable array \emph{Fan} of the defined type is created. This one-dimensional array will contain an entry for each fan in the problem.
+
+The internal data array is allocated (sized) in the ``GetInput'' routine GetFanInput.
+
+NumSimpFan~~ = GetNumObjectsFound(`FAN:SIMPLE:CONSTVOLUME')
+
+~~~ NumVarVolFan = GetNumObjectsFound(`FAN:SIMPLE:VARIABLEVOLUME')
+
+~~~ NumOnOff = GetNumObjectsFound(`FAN:SIMPLE:ONOFF')
+
+~~~ NumZoneExhFan = GetNumObjectsFound(`ZONE EXHAUST FAN')
+
+~~~ NumFans = NumSimpFan + NumVarVolFan + NumZoneExhFan+NumOnOff
+
+~~~ IF (NumFans.GT.0) ALLOCATE(Fan(NumFans))
+
+The remainder of the ``GetInput'' routine moves input file data into the Fan array. The ``Init'' routine transfers data from the inlet nodes into the same array in preparation for performing the calculation.
+
+~ ! Load the node data in this section for the component simulation
+
+~ !
+
+~ !First need to make sure that the massflowrate is between the max and min avail.
+
+~ IF (Fan(FanNum)\%FanType\_Num / = FanType\_ZoneExhaust ) THEN
+
+~~~ Fan(FanNum)\%InletAirMassFlowRate = Min(Node(InletNode)\%MassFlowRate, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Fan(FanNum)\%MassFlowRateMaxAvail)
+
+~~~ Fan(FanNum)\%InletAirMassFlowRate = Max(Fan(FanNum)\%InletAirMassFlowRate, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Fan(FanNum)\%MassFlowRateMinAvail)
+
+~ ELSE~ ! zone exhaust fans - always run at the max
+
+~~~ Fan(FanNum)\%MassFlowRateMaxAvail = Fan(FanNum)\%MaxAirMassFlowRate
+
+~~~ Fan(FanNum)\%MassFlowRateMinAvail = 0.0
+
+~~~ Fan(FanNum)\%InletAirMassFlowRate = Fan(FanNum)\%MassFlowRateMaxAvail
+
+~~~ IF (Fan(FanNum)\%EMSMaxMassFlowOverrideOn) Fan(FanNum)\%InletAirMassFlowRate = \&
+
+~~~~~~ MIN(Fan(FanNum)\%EMSAirMassFlowValue,Fan(FanNum)\%MassFlowRateMaxAvail)
+
+~ END IF
+
+~ !Then set the other conditions
+
+~ Fan(FanNum)\%InletAirTemp~~~~~~~~ = Node(InletNode)\%Temp
+
+~ Fan(FanNum)\%InletAirHumRat~~~~~~ = Node(InletNode)\%HumRat
+
+~ Fan(FanNum)\%InletAirEnthalpy~~~~ = Node(InletNode)\%Enthalpy
+
+The ``Calc'' routines do the actual component simulation. All the data they need has been stored in the internal data array ready to be used. The results of the calculation are, in this case, stored in the same array. The ``Calc'' routine always does pure calculation/simulation -- it never retrieves or stores data.
+
+DeltaPress = Fan(FanNum)\%DeltaPress
+
+~~ FanEff~~~~ = Fan(FanNum)\%FanEff
+
+~~ ! For a Constant Volume Simple Fan the Max Flow Rate is the Flow Rate for the fan
+
+~~ Tin~~~~~~~ = Fan(FanNum)\%InletAirTemp
+
+~~ Win~~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ RhoAir~~~~ = Fan(FanNum)\%RhoAirStdInit
+
+~~ MassFlow~~ = MIN(Fan(FanNum)\%InletAirMassFlowRate,Fan(FanNum)\%MaxAirMassFlowRate)
+
+~~ MassFlow~~ = MAX(MassFlow,Fan(FanNum)\%MinAirMassFlowRate)
+
+~~ !
+
+~~ !Determine the Fan Schedule for the Time step
+
+~ If( ( GetCurrentScheduleValue(Fan(FanNum)\%SchedPtr)\textgreater{}0.0 .and. Massflow\textgreater{}0.0 .or. TurnFansOn .and. Massflow\textgreater{}0.0) \&
+
+~~~~~~~ .and. .NOT.TurnFansOff ) Then
+
+~~ !Fan is operating
+
+~~ Fan(FanNum)\%FanPower = MassFlow*DeltaPress/(FanEff*RhoAir) ! total fan power
+
+~~ FanShaftPower = Fan(FanNum)\%MotEff * Fan(FanNum)\%FanPower~ ! power delivered to shaft
+
+~~ PowerLossToAir = FanShaftPower + (Fan(FanNum)\%FanPower - FanShaftPower) * \&
+
+~~~~ Fan(FanNum)\%MotInAirFrac
+
+~~ Fan(FanNum)\%OutletAirEnthalpy = Fan(FanNum)\%InletAirEnthalpy + PowerLossToAir/MassFlow
+
+~~ ! This fan does not change the moisture or Mass Flow across the component
+
+~~ Fan(FanNum)\%OutletAirHumRat~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ Fan(FanNum)\%OutletAirMassFlowRate = MassFlow
+
+~~ Fan(FanNum)\%OutletAirTemp = PsyTdbFnHW (Fan(FanNum)\%OutletAirEnthalpy,Fan(FanNum)\%OutletAirHumRat)
+
+~Else
+
+~~ !Fan is off and not operating no power consumed and mass flow rate.
+
+~~ Fan(FanNum)\%FanPower = 0.0
+
+~~ FanShaftPower = 0.0
+
+~~ PowerLossToAir = 0.0
+
+~~ Fan(FanNum)\%OutletAirMassFlowRate = 0.0
+
+~~ Fan(FanNum)\%OutletAirHumRat~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ Fan(FanNum)\%OutletAirEnthalpy~~~~ = Fan(FanNum)\%InletAirEnthalpy
+
+~~ Fan(FanNum)\%OutletAirTemp = Fan(FanNum)\%InletAirTemp
+
+~~ ! Set the Control Flow variables to 0.0 flow when OFF.
+
+~~ Fan(FanNum)\%MassFlowRateMaxAvail = 0.0
+
+~~ Fan(FanNum)\%MassFlowRateMinAvail = 0.0
+
+~~End If
+
+Finally, the ``Update'' routine (UpdateFan) moves the results from the internal data array into the outlet node(s).
+
+~~ OutletNode = Fan(FanNum)\%OutletNodeNum
+
+~~ InletNode = Fan(FanNum)\%InletNodeNum
+
+~~ ! Set the outlet air nodes of the fan
+
+~~ Node(OutletNode)\%MassFlowRate~ = Fan(FanNum)\%OutletAirMassFlowRate
+
+~~ Node(OutletNode)\%Temp~~~~~~~~~ = Fan(FanNum)\%OutletAirTemp
+
+~~ Node(OutletNode)\%HumRat~~~~~~~ = Fan(FanNum)\%OutletAirHumRat
+
+~~ Node(OutletNode)\%Enthalpy~~~~~ = Fan(FanNum)\%OutletAirEnthalpy
+
+~~ ! Set the outlet nodes for properties that just pass through \& not used
+
+~~ Node(OutletNode)\%Quality~~~~~~~~ = Node(InletNode)\%Quality
+
+~~ Node(OutletNode)\%Press~~~~~~~~~~ = Node(InletNode)\%Press
+
+~~ ! Set the Node Flow Control Variables from the Fan Control Variables
+
+~~ Node(OutletNode)\%MassFlowRateMaxAvail = Fan(FanNum)\%MassFlowRateMaxAvail
+
+~~ Node(OutletNode)\%MassFlowRateMinAvail = Fan(FanNum)\%MassFlowRateMinAvail
+
+Certain data items must always be transferred from inlet nodes to outlet nodes even if the data item is unaltered by the component model. The data items that must be transferred are:
+
+1.~~~Temp
+
+2.~~~HumRat
+
+3.~~~Enthalpy
+
+4.~~~Press
+
+5.~~~MassFlowRate
+
+6.~~~MassFlowRateMaxAvail
+
+7.~~~MassFlowRateMinAvail
diff --git a/doc/module-developer/src/hvac-network/getting-nodes.tex b/doc/module-developer/src/hvac-network/getting-nodes.tex
new file mode 100644
index 00000000000..0d1e21375b3
--- /dev/null
+++ b/doc/module-developer/src/hvac-network/getting-nodes.tex
@@ -0,0 +1 @@
+\section{Getting Nodes}\label{getting-nodes}
diff --git a/doc/module-developer/src/hvac-network/interfacing-with-plant.tex b/doc/module-developer/src/hvac-network/interfacing-with-plant.tex
new file mode 100644
index 00000000000..b5b0d36bdd4
--- /dev/null
+++ b/doc/module-developer/src/hvac-network/interfacing-with-plant.tex
@@ -0,0 +1,132 @@
+\section{Interfacing with Plant}\label{interfacing-with-plant}
+
+Beginning with Version 7.0, EnergyPlus's plant routines were reengineered and this section discusses protocols for how component models should interact with plant loop modeling.~ Component models that reject or obtain heat from a liquid fluid stream, such as hot or chilled water, condenser water, and steam (but not refrigeration), are ``plant components'' that will need to interface with the central plant solver routines.~ This section describes a number of utility routines and concepts for developers of plant component models.
+
+The node structure discussed above is reused for plant.~ Each component model related to plant has inlet and outlet nodes that describe how it is connected to the loop.~ Many of the routines pass in node indexes as arguments as well as other indexes into the main plant data structure.
+
+\subsection{Plant Loop Data Structure}\label{plant-loop-data-structure}
+
+For plant components, in addition to inlet nodes, outlet nodes, and the component's internal data structure, there is a fourth aspect to data flow that includes central data structures defined in DataPlant.f90.~~ The main data structure is called PlantLoop.~ Both condenser loops and plant loops are treated the same and share the PlantLoop structure.~ The PlantLoop structure stores information on the loop topology as well as various control and dispatch input and operational data.~~ The data structure is nested and component information is stored at this level:
+
+PlantLoop()\%LoopSide()\%Branch()\%Comp()\%xxx
+
+Where,
+
+PlantLoop is the top level and will be sized to the total number of plant and condenser loops.
+
+LoopSide is the second level and will be sized to two, one loop side is for the demand side and one loop side is for the supply side.
+
+Branch is the third level and will be sized to the total number of branches on that loop side
+
+Comp is the fourth level and will be sized to the total number of components on the branch.
+
+There are four indices that indentify each component's location for each of the plant loops it is connected with: : loop number, loop side number, branch number, and component number.~ A water cooled chiller will be connected to two loops and so the component itself will appear twice in the data structure and one set of indices will identify its location on the chilled water loop while a second set of indices will locate it on the condenser loop.~~
+
+\subsection{Initialization}\label{initialization}
+
+Component models should store indexes that describe their location in the plant data structure.~ To obtain these indices, call the routine ScanPlantLoopsForObjectonce for each instance of the component.~ The component model's data structure should store a set of indices for: loop number, loop side number, branch number, and component number.~~ If the component is connected to more than one plant loop, then there should be set of indices and a call to ScanPlantLoopsForObject for each plant loop it is connected to.~ If a component model only has a single node name, the required indices can be similarly obtained using the a call to ScanPlantLoopsForNodeNum.
+
+Component models generally need to do a thorough re-initialization at the start of each new environment.~ Component models can call InitComponentNodesto coordinate initializing inlet and outlet nodes. This routine has arguments for the minimum and maximum flow and these should be mass flow rates, in kg/s, that correspond to the ``hardware'' limits of the device.
+
+Some components are connected to more than one plant loop creating dependencies between loops. For example a water-cooled chiller is connected to both a chilled water loop and a condenser water loop.~ The chilled water loop places demands on the condenser water loop so it is beneficial to model the chilled water loop's supply side before the condenser water loop's demand side is modeled.~ An initialization routine called InterConnectTwoPlantLoopSides~is used by the component models to inform the central plant routines of these situations.~ One call to this routine describes a connection between two half-loops. The component model developer needs to decide which of the half loops places demands on the other and set the logical argument Loop1DemandsOnLoop2appropriately.~ The central plant routines use this information to determine an appropriate calling order for simulating individual half-loops.
+
+\subsection{Sizing}\label{sizing}
+
+Component models need to interact with centralized routines that relate to sizes. ~This section provides an overview of how EnergyPlus performs automatic sizing of plant systems and components so that the broader context can be understood when implementing plant components. As of EnergyPlus version 8.3, the plant sizing methods were changed significantly.~ We first describe some of the variables involved, then describe the overall process steps, and finally discuss implications for component models.
+
+The following variables are used to help control plant sizing:
+
+\begin{itemize}
+\item
+  PlantFirstSizesOkayToFinalizePlantSizeNotComplete This public logical boolean flag is declared in DataPlant. It starts out FALSE TRUEfalse and is set to TRUE FALSEtrue only after all some intial plant sizing actions iterations have been completed and the first set of sizes can be finalized. Component models should delay first filling autosized values until this flag is true. The -9999 values that indicate an autosized variable are not filled until this is TRUE.
+\item
+  PlantFirstSizesOkayToReportPlantSizesOkayToFinalize This public logical boolean flag is declared in DataPlant. It starts out false FALSE and is set to TRUE true after the main iterative phase of sizing is completed but before the final finishing passes are made. This flag is only used for advanced sizing methods based on HVAC Sizing Simulations, where the program should report both the ``Initial'' sizes and the final sizes. Component models should delay final reporting first sizes and filling of autosized values until this is set to TRUEtrue. The -9999 values that indicate an autosized variable are not filled until this is TRUE. The first, or intial, cCalls to report the outcome of sizing are not made until this is TRUEtrue.
+\item
+  PlantFinalSizesOkayToReport This public boolean flag is declared in DataPlant. It starts out false and is set to true when all the sizing is done and it is okay to report the final size values. Component models should delay reporting final sizes until this is set to true.
+\item
+  InitLoopEquip This logical flag is passed as an argument with SimPlantEquip and carries through to the main simulation calls for component models. This argument is set to TRUE when the plant sizing is being conducted. The component model needs to handle this argument such that when TRUE the get input, initialization and sizing routines are run, but the calculation routine does not. When TRUE most supply side component models need to return values for the minimum, maximum, and optimal capacities (in terms of loop loads that the device can meet). For plant components with more than one connection to a plant loop, a leading loop connection must be determined and the component sizing routine called with InitLoopEquip is called for only that plant loop. For a example, a chiller only calls its sizing routine when called from a the chilled water loop and does not call it sizing routine when called from the condenser loop.
+\item
+  GetSizingFactor This logical flag is passed as an argument with SimPlantEquip and carries through to the main simulation calls for component models. This is arguementargument set TRUE during some portions of the plant sizing calls and signals the intent to obtain the value of a component-level sizing factor. When this argument is TRUE, InitLoopEquip will also be TRUE. It can be ignored if the component model has no component-level sizing factor as part of its input. If the component does offer a sizing factor, then the implementation needs to handle this argument such that when TRUE the model returns the value of the SizingFactor as an argument to the simulation routine that is called from SimPlantEquip.
+\item
+  CurLoopNum This public integer variable is declared in DataSizing. It is used to communicate to the component models which of the plant loops is actively being sized at the moment.
+\item
+  LoopNum and LoopSide These arguments are optional to the main simulation routine
+\end{itemize}
+
+Plant sizing routines use the approach outlined in the following steps.~ These steps occur at a point during the program's procedural flow when:~ zone and system sizing is completed, much of the plant loop input has been read in and processed but the main plant manager is being called for the first time, none of the pure plant component's simulation routines have yet been called (but components on the air side may have been), and an initial attempt at determining loop calling order has been made in SetupInitialPlantCallingOrder.
+
+1.~~~~Initialize the indices that map between the central plant sizing data structures and the PlantLoop data structure.~ This uses the subroutine called InitOneTimePlantSizingInfo.~This ensures that the PlantLoop\%PlantSizNumvariable is filled before any component models are called.
+
+(steps 2 thru 4 are sequentially repeated for four iterations)
+
+2.~~~~Call each component model in calling order.~~ InitLoopEquipis TRUE.~ The components on each half loop are called in flow order.~ Each half loop in the model is called in the order set up for simulation.~ These calls are typically the first time certain component models have been called and should trigger input processing and plant loop topology processing including loop interconnections.
+
+3.~~~~Revise the calling order for the sequence with which the various plant loop sides are called for sizing and normal simulation.~ Components that connect two loops will have been processed in Step 2 and that information is now available to refine loop side calling order
+
+4.~~~~Call loop sizing routines in calling order.~ Component will have registered their design flow rates in step 2 and now the overall loop sizes are determined from the sum of the components on the loop.
+
+5.~~~~A final pass thru each loop side is made in calling order with the flag PlantFirstSizesOkayToFinalize set to true. At this point the findings are not expected to change (unless doing HVAC Sizing Simulations). Component models now finalize their findings and store the results for use during the simulation. Overall plant loops are finished. If doing coincident plant sizing using HVAC Sizing Simulations, set the flag PlantFirstSizesOkayToReport and report the ``Initial'' sizes. If not doing coincident plant sizing using HVAC Sizing Simulations, the sizes won't change again and set the flag PlantFinalSizesOkayToReport and report the final sizes.
+
+6.~~~~Sizing finished and PlantSizeNotCompleteset FALSE
+
+In earlier versions, component sizing routines were only called once and one had to take care not call them repeatedly (or else their flow request would get doubled each time). However, now plant component models should be designed for multiple executions of their component-level sizing routine. This allows for an iterative approach to plant sizing that is used to solve complex problems raised by inter-connected loops and the interdependence of sizing information. As of version 8.3, the addition of HVAC Sizing Simulation method makes it very explicit that not only do sizing routines need to be able to rerun, the autosized values need to be set to useable values and then changed. It is therefore now necessary to store whether or not the original input was set to autosize and so autosizable input now needs to add a boolean ``*WasAutoSized'' version of the variable to keep track of the user input.
+
+After the component model has determined a design value for the flow rate, this flow rate needs to be registered with the larger plant routines by calling RegisterPlantCompDesignFlow.~This is a volume flow rate in m\(^{3}\)/s.~ The flow rate is associated with the inlet node.~ This call can be repeated and the design flow will be updated with the latest request.
+
+Calls to InitComponentNodesshould be done after sizing is complete so that valid sizes are passed for initialing nodes.
+
+\subsection{Component Flow Rates}\label{component-flow-rates}
+
+Plant components models need knowledge of the rate of plant fluid flows through the device for each of loops involved. Some components will need to request the flow they desire while others just need to know the mass flow rate.~ However, components do not necessarily have complete control over the resulting flow rates because they depend on the state of the entire plant and not just on the individual component model.~ Component models need to be implemented to handle situations where they do not get the exact flow rate they requested or expected to get.~ For example there could be a shortage of flow and components are starved and get less than they desire. Or a component could be in series with another that is making a larger flow request and therefore a component receives more flow than expected.~ Even if a component is usually passive and takes what flow it gets, the user might have placed a component on a branch that is in parallel with other branches making it necessary for even a passive component to make a flow ``request'' in order for its parallel branch to receive flow when a splitter distributes flow across a set of branches.
+
+SetComponentFlowRate collects code for how to properly deal with plant flow rates.~ The idea is to use a central routine that actually changes the various mass flow rate variables on the node and checks against all the constraints.~ As of Version 7, component models should no longer assign flows to the Node data structure. (Component models can get data from Node data structure but should not set flow rate data on the Node directly.)~ The SetComponentFlowRate subroutine's argument for fluid mass flow is INOUT; the component model makes a request and if it cannot be satisfied, the mass flow rate variable will be returned with the corrected flow that the plant can actually provide at the moment.
+
+Some models, such as a water coil controller, may only have information about one control node.~ If a model does not really represent a single device with inlet and outlet nodes, then there is another useful routine called SetActuatedBranchFlowRate which serves a role similar to SetComponentFlowRate.~ This routine handles mass flow issues for all the components on the branch that contains the actuated node but is otherwise similar in concept.
+
+\subsection{Controls}\label{controls}
+
+Plant component models have different types of control interactions depending on the type of component.~~ Plant components that are led by the air side of HVAC models will generally be controlled by circumstances on the air side.~ A water-based cooling coil will be targeting the achievement of certain air conditions and while the state of the chilled water plant serving the coil will matter in the model calculations, the component itself is not controlled by plant but things outside of plant.
+
+Components that need to be operated to meet the loads placed on plant loops will often be controlled based on some combination of node setpoints and dispatched loads.~ The main entry routine (called from PlantLoopEquipment.f90)~ for most such primary components should include and use arguments for ``MyLoad'' and ``RunFlag.''~ Central routines for operation schemes and availability managers will determine if a component is available (e.g.~RunFlag) and what power level the device is being asked to provide (e.g.~MyLoad).~~ MyLoad is now signed as of version 7; a negative value of MyLoad is a cooling load; a positive value of MyLoad is a heating load.
+
+\subsection{Updating}\label{updating}
+
+Plant component update routines should no longer be setting mass flow rates in the update routine.~ The flow setting routines should be called during initialization or calculation routines and should not need to be called again during update.~ The state of the outlet node should be updated, such as outlet temperature, but mass flow rate should not be.~ Prior to version 7 it was common in EnergyPlus to write
+
+~~ Node(OutletNode)~ = Node(InletNode)
+
+However this is no longer acceptable practice and is not allowed for plant nodes.~ Instead this can be replaced with a call to SafeCopyPlantNode.~ This avoids problems when two components are in series and the outlet of one is the inlet of another. We cannot allow unsafe node copying because it will wipe out information stored on the inlet node of the second component.
+
+\subsection{Reporting}\label{reporting}
+
+A component model connected to plant via nodes will inherit a great deal of reporting that already occurs for each node.~ The output variables that start out ``System Node'' will already be available to the user.~~ In general, the focus of reporting should be on data that are internal to the component model.
+
+\subsection{Central Routine Modifications}\label{central-routine-modifications}
+
+When adding a new plant component, there are several places where the central routines' code needs to be modified so that the new model can properly interact with them.~ The following sections of the code should be expanded when adding a new plant component:
+
+1.~~~~DataPlant.f90.~ A new component will need to modify DataPlant.f90 in these places:
+
+a.~~~~Parameter NumSimPlantEquipTypes. Increment up to include new component.
+
+b.~~~Array SimPlantEquipTypes.~ Add array element with new object's class name in upper case.
+
+c.~~~~Array ccSimPlantEquipTypes.Add array element with new object's class name in camel case.
+
+d.~~~Array ValidLoopEquipTypes.~ Add array element with classification for what type of loop this component is intended for, primarily with respect to the type of loop it is intended to meet loads.
+
+e.~~~~Parameter TypeOf\_xxxx .~ Add an integer parameter to identify ``TypeOf'' number for subsequent use to identify component type without having to do string comparisions.
+
+2.~~~~PlantManager.f90
+
+a.~~~~GetPlantInput.~ There is a large IF-ELSEIF block in this routine that will need to be extended to process the new component.~ This is where the ``TypeOf'' number gets set for subsequent use.~ Choose a general equipment type for the component.~ Initialize the value for Comp\%CurOpSchemeType depending on which loop side is involved and/or the nature of the component
+
+b.~~~SetupBranchControlTypes.~ There is a large Case block in this routine that will need to be extended to process the new component.~ Prior to Version 7, the user had to input a branch control type in the IDF.~ Now this information is set in code in this routine.~ There are three different control classifications that need to be set in this routine:
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~i.~~~Comp\%FlowCtrl.~ This is the branch control type input for versions prior to version 7.~ Plant components that have some influence over the mass flows should be set to ControlType\_Active.~ There are also ControlType\_Passive~ and ControlType\_ByPass options that may apply.~ The branches are further processed by routines that automatically detect series active situations.
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ii.~~~Comp\%FlowPriority.~ New for version 7 is a plant modeling concept that treats flow requests differently depending on the nature of the component's priority.~ The idea is that when determining the overall flow rate in a loop, some mass flow requests need to be handled differently than others.~ The three flow priority options for components are LoopFlowStatus\_NeedyAndTurnsLoopOn, LoopFlowStatus\_NeedyIfLoopOn, and LoopFlowStatus\_TakesWhatGets.~ The first is typically a demand side component that when it requests flow will dictate that the loop operate and try to meet its request.~ The second is typically a supply side component with a minimum flow requirement that should necessarily turn on the loop, but if it is running already then the overall flow rate needs to satisfy the minimum on the component.~ The third is typically a passive device like a water tank.
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~iii.~~~Comp\%HowLoadServed.~ This variable informs the load dispatch routines about the component. Some components are intended to serve loads in slightly different ways and this information is stored in the plant data structure as different parameters for HowLoadsServed.~ HowMet\_NoneDemandis used for demand components or others than never meet a load.~ HowMet\_PassiveCap is used for components that can meet a load but are not generally explicitly controllable to meet a certain level of load, such as a ground heat exchanger.~ HowMet\_ByNominalCap is used for components that can be controlled to meet a desired load and do not have any additional layers of constraints.~ HowMet\_ByNominalCapLowOutLimit~is used for components that can be controlled to meet a desired load but have low temperature limit on their outlet node.~ HowMet\_ByNominalCapHiOutLimit is used for components that can be controlled to meet a desired load but have a hi temperature limit on their outlet node.
+
+3.~~~~PlantLoopEquipment.f90.~ The routine SimPlantEquip includes a large Case statement that will need to expanded to include the new component.~ Some demand components, such as a water coil, may not need to actually call a routine from here but a placeholder must be added to the Case statement.~ Most plant components will call the main simulation entry point for the component model from SimPlantEquip and new components need to add that call here.~ Note that the Case statement are broken up into General equipment and the specific equipment.~~~ Code should support use of InitLoopEquip and GetCompSizFac as appropriate.
diff --git a/doc/module-developer/src/hvac-network/node-mass-flow-variables.tex b/doc/module-developer/src/hvac-network/node-mass-flow-variables.tex
new file mode 100644
index 00000000000..b8d224a9c7e
--- /dev/null
+++ b/doc/module-developer/src/hvac-network/node-mass-flow-variables.tex
@@ -0,0 +1,14 @@
+\section{Node Mass Flow Variables}\label{node-mass-flow-variables}
+
+The node mass flow variables merit a little more discussion. Six mass flow variables are defined at each node. They are: MassFlowRate, MassFlowRateMin, MassFlowRateMax, MassFlowRateMinAvail, MassFlowRateMaxAvail and MassFlowRateRequest. These variables hold loop mass flow rate information according to the following definitions.
+
+\begin{itemize}
+\item
+  MassFlowRate -- this node variable holds the simulation mass flow rate for the current timestep. The remaining four variables serve as limits to MassFlowRate.
+\item
+  MassFlowRateMax, MassFlowRateMin -- These node variables hold the maximum possible and the minimum allowable flow rates for a particular component. As such, they represent the ``hardware limit'' on the flow rate for the component.
+\item
+  MassFlowRateMaxAvail, MassFlowRateMinAvail -- these node variables represent the \emph{loop} maximum and minimum flow rate for the current configuration of the loop on which the component resides.
+\item
+  MassFlowRateRequest~ --~ this node variable applies only to plant and holds the desired mass flow rate for the current timestep.~ This stores a record of what flow was desired.
+\end{itemize}
diff --git a/doc/module-developer/src/hvac-network/nodes-in-the-simulation.tex b/doc/module-developer/src/hvac-network/nodes-in-the-simulation.tex
new file mode 100644
index 00000000000..ae31d511ccc
--- /dev/null
+++ b/doc/module-developer/src/hvac-network/nodes-in-the-simulation.tex
@@ -0,0 +1,179 @@
+\section{Nodes in the simulation}\label{nodes-in-the-simulation}
+
+In the EnergyPlus data structure, the nodes are where each component model gets its input and where it places its output. The module \emph{DataLoopNode} contains all the node related data. In particular, the array \emph{Node} contains the state variables and mass flows for all the nodes in the problem being simulated.
+
+~ ! Valid Fluid Types for Nodes
+
+~ INTEGER, PARAMETER :: NodeType\_Unknown = 0~ ! `blank'
+
+~ INTEGER, PARAMETER :: NodeType\_Air~~~~ = 1~ ! `Air'
+
+~ INTEGER, PARAMETER :: NodeType\_Water~~ = 2~ ! `Water'
+
+~ INTEGER, PARAMETER :: NodeType\_Steam~~ = 3~ ! `Steam'
+
+~ INTEGER, PARAMETER :: NodeType\_Electric = 4~ ! `Electric'
+
+~\textbf{TYPE} NodeData
+
+~~ \textbf{INTEGER}~ :: FluidType~~~~~~~~~~~~~~~~ = 0~~ ! must be one of the valid parameters
+
+~~ \textbf{INTEGER}~ :: FluidIndex~~~~~~~~~~~~~~~ = 0~~ ! For Fluid Properties
+
+~~ REAL(r64)~~~~ :: Temp~~~~~~~~~~~~~~~~~~~~~ = 0.d0 ! \{C\}
+
+~~ REAL(r64)~~~~ :: TempMin~~~~~~~~~~~~~~~~~~ = 0.d0 ! \{C\}
+
+~~ REAL(r64)~~~~ :: TempMax~~~~~~~~~~~~~~~~~~ = 0.d0 ! \{C\}
+
+~~ REAL(r64)~~~~ :: TempSetPoint~~~~~~~~~~~~~ = SensedNodeFlagValue ! \{C\}
+
+~~ REAL(r64)~~~~ :: TempLastTimestep~~~~~~~~~ = 0.d0 ! {[}C\}~~ DSU
+
+~~ REAL(r64)~~~~ :: MassFlowRateRequest~~~~~~ = 0.d0 ! \{kg/s\}~ DSU
+
+~~ REAL(r64)~~~~ :: MassFlowRate~~~~~~~~~~~~~ = 0.d0 ! \{kg/s\}
+
+~~ REAL(r64)~~~~ :: MassFlowRateMin~~~~~~~~~~ = 0.d0 ! \{kg/s\}
+
+~~ REAL(r64)~~~~ :: MassFlowRateMax~~~~~~~~~~ = SensedNodeFlagValue ! \{kg/s\}
+
+~~ REAL(r64)~~~~ :: MassFlowRateMinAvail~~~~~ = 0.d0 ! \{kg/s\}
+
+~~ REAL(r64)~~~~ :: MassFlowRateMaxAvail~~~~~ = 0.d0 ! \{kg/s\}
+
+~~ REAL(r64)~~~~ :: MassFlowRateSetPoint~~~~~ = 0.d0 ! \{kg/s\}
+
+~~ REAL(r64)~~~~ :: Quality~~~~~~~~~~~~~~~~~~ = 0.d0 ! \{0.0-1.0 vapor fraction/percent\}
+
+~~ REAL(r64)~~~~ :: Press~~~~~ ~~~~~~~~~~~~~~~ = 0.d0 ! \{Pa\}
+
+~~ REAL(r64)~~~~ :: Enthalpy~~~~~~~~~~~~~~~~~ = 0.d0 ! \{J/kg\}
+
+~~ REAL(r64)~~~~ :: EnthalpyLastTimestep~~~~~ = 0.d0 ! \{J/kg\}~ DSU for steam?
+
+~~ REAL(r64)~~~~ :: HumRat~~~~~~~~~~~~~~~~~~~ = 0.d0 ! \{\}
+
+~~ REAL(r64)~~~~ :: HumRatMin~~~~~~~~~~~~~~~~ = SensedNodeFlagValue ! \{\}
+
+~~ REAL(r64)~~~~ :: HumRatMax~~~~~~~~~~~~~~~~ = SensedNodeFlagValue ! \{\}
+
+~~ REAL(r64)~~~~ :: HumRatSetPoint~~~~~~~~~~~ = SensedNodeFlagValue ! \{\}
+
+~~ REAL(r64)~~~~ :: TempSetPointHi~~~~~~~~~~~ = SensedNodeFlagValue ! \{C\}
+
+~~ REAL(r64)~~~~ :: TempSetPointLo~~~~~~~~~~~ = SensedNodeFlagValue ! \{C\}
+
+~~ REAL(r64)~~~~ :: Height~~~~~~~~~~~~~~~~~~~ = -1.d0 !~ \{m\}
+
+~~ !~ Following are for Outdoor Air Nodes ``read only''
+
+~~ REAL(r64)~~~~ :: OutAirDryBulb~~~~~~~~~~~~ = 0.d0 ! \{C\}
+
+~~ \textbf{LOGICAL}~~~~~~ :: EMSOverrideOutAirDryBulb~ = .FALSE. ! if true, the EMS is calling to override outdoor air node drybulb setting
+
+~~ REAL(r64)~~~~ :: EMSValueForOutAirDryBulb~ = 0.d0 ! value EMS is directing to use for outdoor air node's drybulb \{C\}
+
+~~ REAL(r64)~~~~ :: OutAirWetBulb~~~~~~~~~~~~ = 0.d0 ! \{C\}
+
+~~ \textbf{LOGICAL}~~~~~~ :: EMSOverrideOutAirWetBulb~ = .FALSE. ! if true, the EMS is calling to override outdoor air node wetbulb setting
+
+~~ REAL(r64)~~~~ :: EMSValueForOutAirWetBulb~ = 0.d0 ! value EMS is directing to use for outdoor air node's wetbulb \{C\}
+
+~~ ! Contaminant
+
+~~ REAL(r64)~~~~ :: CO2~~~~~~~~~~~~~~~~~~~~~~ = 0.d0 ! \{ppm\}
+
+~~ REAL(r64)~~~~ :: CO2SetPoint~~~~~~~~~~~~~~ = 0.d0 ! \{ppm\}
+
+~\textbf{END} \textbf{TYPE} NodeData
+
+\textbf{TYPE} MoreNodeData
+
+~~ REAL(r64)~~~~ :: RelHumidity~~~~~~~~~~~~~~ = 0.d0 ! \{\%\}
+
+~~ REAL(r64)~~~~ :: ReportEnthalpy~~~~~~~~~~~ = 0.d0 ! specific enthalpy calculated at the HVAC timestep {[}J/kg{]}
+
+~~ REAL(r64)~~~~ :: VolFlowRateStdRho~~~~~~~~ = 0.d0 ! volume flow rate at standard density {[}m3/s{]}
+
+~~ REAL(r64)~~~~ :: VolFlowRateCrntRho~~~~~~~ = 0.d0 ! volume flow rate at current density, only used for air nodes {[}m3/s{]}
+
+~~ REAL(r64)~~~~ :: WetbulbTemp~~~~~~~~~~~~~~ = 0.d0 ! wetbulb temperature {[}C{]}
+
+~~ REAL(r64)~~~~ :: AirDensity~~~~~~~~~~~~~~~ = 0.d0 ! reported air density at standard density {[}kg/m3{]}
+
+~\textbf{END} \textbf{TYPE} MoreNodeData
+
+\textbf{TYPE} (NodeData), \textbf{ALLOCATABLE}, \textbf{DIMENSION}(:) :: Node !dim to num nodes in SimHVAC
+
+~\textbf{TYPE} (NodeData) :: DefaultNodeValues = ~ \&
+
+~~~~ NodeData(0, ~~~~~~~~~\& ! FluidType
+
+~~~~~~~~~~~~~ 0,~~~~~~~~~ \& ! FluidIndex
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! Temp \{C\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! TempMin \{C\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! TempMax \{C\}
+
+~~~~ SensedNodeFlagValue,~~ \& ! TempSetPoint \{C\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! TempLastTimeStep \{C\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! MassFlowRateRequest \{kg/s\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! MassFlowRate \{kg/s\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! MassFlowRateMin \{kg/s\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! MassFlowRateMax \{kg/s\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! MassFlowRateMinAvail \{kg/s\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! MassFlowRateMaxAvail \{kg/s\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! MassFlowRateSetPoint \{kg/s\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! Quality \{0.0-1.0 vapor fraction/percent\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! Press \{Pa\}~~ REAL(r64)~~~~ ::
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! Enthalpy \{J/kg\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! EnthalpyLastTimeStep \{J/kg\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! HumRat \{\}
+
+~~~~ SensedNodeFlagValue,~~ \& ! HumRatMin \{\}
+
+~~~~ SensedNodeFlagValue,~~ \& ! HumRatMax \{\}
+
+~~~~ SensedNodeFlagValue,~~ \& ! HumRatSetPoint \{\}
+
+~~~~ SensedNodeFlagValue,~~ \& ! TempSetPointHi \{C\}
+
+~~~~ SensedNodeFlagValue,~~ \& ! TempSetPointLo \{C\}
+
+~~~~~~~~~~~~ -1.0D0,~~~~~~~ \& ! Height \{m\}
+
+~~ ~~~~~~~~~~~0.0D0,~~~~~~~ \& ! OutAirDryBulb \{C\}
+
+~~~~~~~~~~~~~ .FALSE.,~~~~~ \& ! EMSOverrideOutAirDryBulb
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! EMSValueForOutAirDryBulb \{C\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~~~ \& ! OutAirWetBulb \{C\}
+
+~~~~~~~~~~~~~ .FALSE.,~~~~~ \& ! EMSOverrideOutAirWetBulb
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! EMSValueForOutAirWetBulb \{C\}
+
+~~~~~~~~~~~~~ 0.0D0,~~~~~~~ \& ! CO2 \{ppm\}
+
+~~~~~~~~~~~~~ 0.0D0)~~~~~~~~~ ! CO2 setpoint \{ppm\}
+
+~TYPE (MoreNodeData), ALLOCATABLE, DIMENSION(:) :: MoreNodeInfo
+
+In our example module \emph{NewHVACComponent,} the subroutine \emph{InitNewHVACComponent} is responsible for obtaining the input data from the inlet node(s) and putting it into the component data structure for use in C\emph{alcNewHVACComponent}. Then \emph{UpdateNewHVACComponent} takes the calculated data and moves it to the outlet nodes for use by other components. EnergyPlus component models are assumed to be direct models: inlets are input to the calculation and outlets are output from the calculations.
diff --git a/doc/module-developer/src/important-rules-for-module-developers.tex b/doc/module-developer/src/important-rules-for-module-developers.tex
new file mode 100644
index 00000000000..cb9dcf6f897
--- /dev/null
+++ b/doc/module-developer/src/important-rules-for-module-developers.tex
@@ -0,0 +1,19 @@
+\chapter{Important Rules for Module Developers}\label{important-rules-for-module-developers}
+
+1.~~~INITIALIZE!!!!!~ INITIALIZE either fully or ``invalidly'' when you ALLOCATE the array/derived type.~ Two items have been set up to help you: BigNumber and DBigNumber are in DataGlobals.~ They get initialized before anything happens in the main routine (EnergyPlus). An invalid initialization can use one of these, appropriately (i.e.~set and test for ``BigNumber'').~ Another example of ``invalid'' initialization is a value that shouldn't be legal for the item (-999).
+
+2.~~~Warning errors during ``get input'' should only be used when program termination is not required (this is rare). Each GetInput routine should be structured so that errors detected (such as an invalid schedule name which currently is just a warning) cause a fatal error after all the input for that item/module/etc is gotten.~ (See HBManager, BaseboardRadiator, others)~ In addition, don't make GetInputFlag a module variable.~ Make it as ``local'' as possible.~ Look at BaseboardRadiator for an example.
+
+3.~~~Error messages during simulation should be semi-intelligent.~ No one wants to see 5,000 messages saying ``this flow invalid''.~ If the error condition might happen a lot (especially during debugging), count each occurrence and only put out a message every 50 or so.~~ It is better to use the ``Recurring Error Handling'' routines. (See examples of both above in the Error Messages section).~ Also, if you are putting the same message in two modules, identify the error message with some designation.~ For Example,
+
+~CALL ShowWarningError (\textbf{'SimRoutinename}: this condition happened again')
+
+will help everyone track it down.~~ Use the ShowContinueErrorTimeStamp so the time/date/environment of occurrence is known, as appropriate for the condition.
+
+4.~~~Use the templates for documentation!~ Modules, subroutines, functions templates all have been checked into StarTeam.~ Use them.~ Put INTENTs on your Subroutine Arguments.~ Document variables.
+
+\textbf{5.~~~Add ``meter'' variables as appropriate!~ If your module uses fuel or electricity and that energy is not accounted for by other components (i.e.~pumps, coils, chillers, etc), then you need to report it onto a ``meter''.}
+
+\textbf{6.~~~Avoid the use of string comparisons in subroutines other than GetInput.~ Check string comparisons in the GetInput subroutines and assign an integer parameter for comparisons elsewhere in the module. Character strings in structures are not allowed (except for name of object) -- any exceptions must be approved. Schedule names, curve object names, and child object types MUST all be referenced by an integer. Existing code must be changed as you change any of the code within a module.~}
+
+\textbf{7.~~~If you are submitting code for insertion in the public version of EnergyPlus, make sure that the proper ``Grant-Back'' procedure has been followed so that the correct attributions of code authorship are given as well as permission to use this code in publicly available software is assured. (see Appendix G, Code/Module Contribution Questionnaire -- also available separately)}
diff --git a/doc/module-developer/src/input-concepts.tex b/doc/module-developer/src/input-concepts.tex
new file mode 100644
index 00000000000..5784459a5a4
--- /dev/null
+++ b/doc/module-developer/src/input-concepts.tex
@@ -0,0 +1,9 @@
+\chapter{Input Concepts}\label{input-concepts}
+
+In EnergyPlus, input and output are accomplished by means of ASCII (text) files. On the input side, there are two files:
+
+1)~~~the Input Data Dictionary (IDD) that describes the types (classes) of input objects and the data associated with each object;
+
+2)~~~the Input Data File (IDF) that contains all the data for a particular simulation.
+
+Each EnergyPlus module is responsible for getting its own input. Of course, EnergyPlus provides services to the module that make this quite easy. The first task of a module developer is to design and insert a new entry into the Input Data Dictionary.
diff --git a/doc/module-developer/src/input-concepts/advanced-input-considerations.tex b/doc/module-developer/src/input-concepts/advanced-input-considerations.tex
new file mode 100644
index 00000000000..d21c766d4f3
--- /dev/null
+++ b/doc/module-developer/src/input-concepts/advanced-input-considerations.tex
@@ -0,0 +1,77 @@
+\section{Advanced Input Considerations}\label{advanced-input-considerations}
+
+Creating a new module/adding a new feature to EnergyPlus is a good accomplishment.~ However, it is likely that future additions will be done and will impact any objects created.~ In this regard, we ask that module developers take a longer view than ``just getting my thing'' going.
+
+For example, in the ``Fan Coil'' object, prior to the V1.2 release, the object definition specified a cooilng coil name.~ \emph{But it did not specify a cooling coil type.}~ Rather than restrict coil names to be unique over all coils (which becomes difficult as more coil types are added), the developers only have unique names within a type.~ Thus, it would become difficult for the Fan Coil module to get the proper link to the correct cooling coil.
+
+In the V1.2 release, a cooling coil type was added to the object.~ But the resulting object is less readable now. For upwards compatibility, the coil type was placed at the end of the object whereas the coil name is in the middle.~ If this had been thought of earlier, then the coil type and coil name could be in succeeding fields in the object definition.
+
+The ``standard'' for describing such fields would be to list the ``coil type'' and then the ``coil name'' fields, such as in the UNITARYSYSTEM:HEATPUMP:AIRTOAIR object.
+
+The point -- try to envision future changes in making up objects, even if you think ``that will never happen''.~ You do not have to try to address every future case, only the most likely.
+
+\textbf{ZoneHVAC:FourPipeFanCoil,}
+
+~~~~~~~ \textbackslash{}min-fields 21
+
+~~ A1 , \textbackslash{}field Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~ A2 , \textbackslash{}field Availability Schedule Name
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type object-list
+
+~~~~~~~ \textbackslash{}object-list ScheduleNames
+
+~~ N1 , \textbackslash{}field Maximum Supply Air Flow Rate
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}autosizable
+
+~~~~~~~ \textbackslash{}units m3/s
+
+~~ N2 , \textbackslash{}field Maximum Outdoor Air Flow Rate
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}autosizable
+
+~~~~~~~ \textbackslash{}units m3/s
+
+~~ \textless{}snip\textgreater{}
+
+\textbf{~~ A11, \textbackslash{}field Cooling Coil Name}
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type object-list
+
+~~~~~~~ \textbackslash{}object-list CoolingCoilsWater
+
+~~ N3 , \textbackslash{}field Maximum Cold Water Flow Rate
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~ ~~~~\textbackslash{}autosizable
+
+~~~~~~~ \textbackslash{}units m3/s
+
+~~~~~~~ \textbackslash{}ip-units gal/min
+
+~ \textless{}snip\textgreater{}
+
+~~ \textbf{A13; \textbackslash{}field Cooling Coil Object Type}
+
+~~~~~~~ \textbackslash{}required-field
+
+~~~~~~~ \textbackslash{}type choice
+
+~~~~~~~ \textbackslash{}key Coil:Cooling:Water
+
+~~~~~~~ \textbackslash{}key Coil:Cooling:Water:DetailedGeometry
+
+~~~~~~~ \textbackslash{}key CoilSystem:Cooling:Water:HeatExchangerAssisted
diff --git a/doc/module-developer/src/input-concepts/data-dictionary-naming-conventions.tex b/doc/module-developer/src/input-concepts/data-dictionary-naming-conventions.tex
new file mode 100644
index 00000000000..d151caff91b
--- /dev/null
+++ b/doc/module-developer/src/input-concepts/data-dictionary-naming-conventions.tex
@@ -0,0 +1,57 @@
+\section{Data Dictionary Naming Conventions}\label{data-dictionary-naming-conventions}
+
+\subsection{Class (Object) Names}\label{class-object-names}
+
+Class names shall be written in camel case where words are joined together without spaces and each word is capitalized. The colon shall be used to delimit hierarchy moving from general to specific. Natural language terminology shall be used when possible for each member separated by colons.
+
+Example: ZoneHVAC:PackagedTerminalHeatPump
+
+\subsection{Field Names}\label{field-names}
+
+Field names shall be written in title case where every major word is capitalized (exceptions: ``a'', ``the'', ``for'', etc.) with spaces separating words.~ Field names shall be written using natural language terminology but should be relatively concise (no unnecessary abbreviations or acronyms).~ If the field is for the name of this object, the field name shall simply be ``Name'' to eliminate redundancy.~ The nature of an alpha field shall be explicit, for instance, ``Availability Schedule Name'' instead of merely ``Availability Schedule''. Generally, the object is not also included as the field name.
+
+Example: Availability Schedule Name
+
+When object names/types are included as part of the input, then the field name should contain ``Object Type'':
+
+Example: Zone Equipment 1 Object Type
+
+\subsection{Choice Names}\label{choice-names}
+
+When field choices list object references, the field choices shall list the class/object type name the same as its class definition in the IDD.~ When field choices list other key words, the field choice names shall be written in camel case where words are joined together without spaces and each word is capitalized.~ Field choice names shall be written using natural language terminology but should be relatively concise (no unnecessary abbreviations or acronyms) and avoid overly lengthy key words.~ Field choice names shall only use alphanumeric characters with the addition of the forward slash (``/'') character as a concise alternative to the word ``per''; colons shall be allowed if the field choices are class names.
+
+~ A2 , \textbackslash{}field Period Selection
+
+~~~~~~ \textbackslash{}retaincase
+
+~~~~~~ \textbackslash{}note Following is a list of all possible types of Extreme and Typical periods that
+
+~~~~~~ \textbackslash{}note might be identified in the Weather File. Not all possible types are available
+
+~~~~~~ \textbackslash{}note for all weather files.
+
+~~~~~~ \textbackslash{}type choice
+
+~~~~~~ \textbackslash{}key SummerExtreme
+
+~~~~~~ \textbackslash{}key SummerTypical
+
+~~~~~~ \textbackslash{}key WinterExtreme
+
+~~~~~~ \textbackslash{}key WinterTypical
+
+~~~~~~ \textbackslash{}key AutumnTypical
+
+~~~~~~ \textbackslash{}key SpringTypical
+
+~~~~~~ \textbackslash{}key WetSeason
+
+~~~~~~ \textbackslash{}key DrySeason
+
+~~~~~~ \textbackslash{}key NoDrySeason
+
+~~~~~~ \textbackslash{}key NoWetSeason
+
+~~~~~~ \textbackslash{}key TropicalHot
+
+~~~~~~ \textbackslash{}key TropicalCold
diff --git a/doc/module-developer/src/input-concepts/datasets.tex b/doc/module-developer/src/input-concepts/datasets.tex
new file mode 100644
index 00000000000..95b0f15dd03
--- /dev/null
+++ b/doc/module-developer/src/input-concepts/datasets.tex
@@ -0,0 +1,22 @@
+\section{DataSets}\label{datasets}
+
+Akin to the libraries of other programs, EnergyPlus uses data sets.~ Data sets are similar to libraries but many items are contained in a single file (usually input file format or sometimes macro format).~ Developers are encouraged, as appropriate, to submit data sets along with new features.~ Some of the existing data sets include:
+
+\begin{itemize}
+\item
+  Materials properties
+\item
+  Construction elements (layers of materials)
+\item
+  Composite construction definitions (equivalent constructions for complex elements)
+\item
+  Solar Collector parameters
+\item
+  Economic Tariffs
+\item
+  Design Day definitions
+\item
+  Location definitions
+\item
+  Standard report definitions
+\end{itemize}
diff --git a/doc/module-developer/src/input-concepts/input-considerations.tex b/doc/module-developer/src/input-concepts/input-considerations.tex
new file mode 100644
index 00000000000..f4b2c9c751e
--- /dev/null
+++ b/doc/module-developer/src/input-concepts/input-considerations.tex
@@ -0,0 +1,88 @@
+\section{Input Considerations}\label{input-considerations}
+
+The IDD/IDF concept allows the module developer much flexibility.~ Along with this flexibility comes a responsibility to the overall development of EnergyPlus. Developers must take care not to obstruct other developers with their additions or changes.~ Major changes in the IDD require collaboration among the developers (both module and interface).
+
+In many cases, the developer may be creating a new model -- a new HVAC component, for instance. Then the most straightforward approach is to create a new object class in the IDD with its own unique, self-contained input. This will seldom impact other developers.
+
+In some cases, the developer may be adding a calculation within an existing module or for an existing class of objects. This calculation may require new or different input fields. Then the developer has a number of choices. This section will present some ideas for adding to the IDD that will minimize impact to other developers.
+
+For example, consider the implementation of Other Side Coefficients (OSC) in the IDD.~ Other side coefficients are a simplification for the surface heat balance and were used mostly in BLAST 2.0 before we had interzone surfaces.~ We have carried this forward into EnergyPlus for those users that understand and can use it.~ We'll use it as an example of approaches to adding data items to the IDD.~ Moreover, we'll try to give some hints on which approaches might be used for future additions.
+
+So, you're adding something to EnergyPlus and it is part of an existing module or object class.~ What do you do with your required inputs to your model?~ There are at least four options:
+
+\begin{itemize}
+\item
+  Embed your values in a current object class definition.
+\item
+  Put something in the current definition that will trigger a ``GetInput'' for your values.
+\item
+  Put something in the current definition that will signal a ``special'' case and embed a name (of your item) in the definition (this adds 1 or 2 properties to the object).
+\item
+  Just get your input and have each of those inputs reference a named object.
+\end{itemize}
+
+For example, using the OSC option in surfaces, in the beta 2 version of EnergyPlus we had
+
+~ A8 , \textbackslash{}field Exterior environment
+
+~~~~~~ \textbackslash{}type alpha
+
+~~~~~~ \textbackslash{}note \textless{}for Interzone Surface:Adjacent surface name\textgreater{}
+
+~~~~~~ \textbackslash{}note For non-interzone surfaces enter:
+
+~~~~~~ \textbackslash{}note ExteriorEnvironment, Ground, or OtherSideCoeff
+
+~~~~~~ \textbackslash{}note OSC won't use CTFs
+
+~ N24, \textbackslash{}field User selected Constant Temperature
+
+~ N25, \textbackslash{}field Coefficient modifying the user selected constant
+
+~~~~~~~~~~~~~ temperature
+
+~ N26, \textbackslash{}field Coefficient modifying the external dry bulb temperature
+
+~ N27, \textbackslash{}field Coefficient modifying the ground temperature
+
+~ N28, \textbackslash{}field Combined convective/radiative film coefficient
+
+~~~~~~ \textbackslash{}note if = 0, use other coefficients
+
+~ N29, \textbackslash{}field Coefficient modifying the wind speed term (s/m)
+
+~ N30, \textbackslash{}field Coefficient modifying the zone air temperature part of
+
+~~~~~~~~~~~~~ the equation
+
+\textbf{1)~~}We have done option 1: embed the values in the input.~ (We have also embedded these values in each and every surface derived type (internal data structure) but that can be discussed elsewhere).
+
+When to use:~ It makes sense to embed these values when each and every object (SURFACE) needs these values (e.g.~we need to specify Vertices for Every Surface -- so these clearly should be embedded).
+
+After beta 2, the definition of Surfaces was changed. Obviously option 1 was not a good choice for the OSC data: the data would be rarely used. Our other options were:
+
+\textbf{2)~~}Obviously the ExteriorEnvironment field will remain (but its name was changed to Outside Face Environment).
+
+However, we do not want to embed the values for OtherSideCoef in the Surface items.~ So, if the ExteriorEnvironment continues to reference OtherSideCoef, we can easily trigger a ``GetInput'' for them.~ An additional object class would be necessary for this case.
+
+OtherSideCoef,~ A1, \textbackslash{}field name of OtherSideCoef,
+
+~ A2, \textbackslash{}field SurfaceName (reference to surface using OSC)
+
+~ \ldots{}.
+
+When to use:~ This option can be used for many cases.~ The same object definition will work for option 4 below.~ Obviously, if there is not a convenient trigger in SURFACE but you want to add a feature, this would let you do it without embedding it in the Surface Definition.~ If there is a trigger, such as exists with the ExteriorEnvironment, the A2 field might not be needed.~ This approach would become a bit cumbersome if you expected there to be a lot of these or if there were a one-to-many relationship (i.e.~a single set of OSCs could be used for many surfaces).~ Nevertheless, the approach provides a convenient ``data check''/cross reference that can be validated inside the code.
+
+\textbf{3)~~}We could also have the SURFACE definition reference an OSC name (in this instance).
+
+So, we'd add a field to the Surface that would be the name in the OtherSideCoef object above.~ Then, the OtherSideCoef objects wouldn't need a Surface Name. This is the most straightforward approach: including data in one object by referencing another and it was the approach chosen for the redefined Surface class.
+
+When to use:~ when there is a set of parameters that would be used extensively, then this would provide a name for those.~ If hand editing, then you only would need to change one set of these parameters rather than having to go through many.~ Of course, the OtherSideCoef object wouldn't also have to have the true numbers but could reference yet a third named object\ldots{}\ldots{} (starting to get messy).
+
+\textbf{4)~~}We could have the OtherSideCoef object as above and just ``get'' it as a matter of course.~ (e.g., in the case where we don't have a convenient trigger such as ExteriorEnvironment).
+
+When to use:~ Note that the same structure for 2 works here too.~ It's just not triggered (to get the input) by a value in the other object (SURFACE).
+
+\textbf{Summary}
+
+There are several approaches to adding items to the IDD.~ Developers need to consider impacts to other developers and users early in the implementation planning.
diff --git a/doc/module-developer/src/input-concepts/input-data-dictionary.tex b/doc/module-developer/src/input-concepts/input-data-dictionary.tex
new file mode 100644
index 00000000000..79355de5d85
--- /dev/null
+++ b/doc/module-developer/src/input-concepts/input-data-dictionary.tex
@@ -0,0 +1,161 @@
+\section{Input Data Dictionary}\label{input-data-dictionary}
+
+An entry in the IDD consists of comma-separated text terminated by a semicolon. For instance:
+
+\textbf{Coil:Heating:Water,}
+
+~~~~~~ \textbackslash{}min-fields 14
+
+~ A1 , \textbackslash{}field Name
+
+~~~~~~ \textbackslash{}required-field
+
+~~~~~~ \textbackslash{}type alpha
+
+~~~~~~ \textbackslash{}reference HeatingCoilName
+
+~~~~~~ \textbackslash{}reference HeatingCoilsWater
+
+~ A2 , \textbackslash{}field Availability Schedule Name
+
+~~~~~~ \textbackslash{}type object-list
+
+~~~~~~ \textbackslash{}object-list ScheduleNames
+
+~ N1 , \textbackslash{}field U-Factor Times Area Value
+
+~~~~~~ \textbackslash{}units W/K
+
+~~~~~~ \textbackslash{}autosizable
+
+~~~~~~ \textbackslash{}default Autosize
+
+~ N2 , \textbackslash{}field Maximum Water Flow Rate
+
+~~~~~~ \textbackslash{}units m3/s
+
+~~~~~~ \textbackslash{}autosizable
+
+~~~~~~ \textbackslash{}ip-units gal/min
+
+~~~~~~ \textbackslash{}default Autosize
+
+~ A3 , \textbackslash{}field Water Inlet Node Name
+
+~~~~~~ \textbackslash{}required-field
+
+~ A4 , \textbackslash{}field Water Outlet Node Name
+
+~~~~~~ \textbackslash{}required-field
+
+~ A5 , \textbackslash{}field Air Inlet Node Name
+
+~~~~~~ \textbackslash{}required-field
+
+~ A6 , \textbackslash{}field Air Outlet Node Name
+
+~~~~~~ \textbackslash{}required-field
+
+~ A7 , \textbackslash{}field Performance Input Method
+
+~~~~~~ \textbackslash{}type Choice
+
+~~~~~~ \textbackslash{}key UFactorTimesAreaAndDesignWaterFlowRate
+
+~~~~~~ \textbackslash{}key NominalCapacity
+
+~~~~~~ \textbackslash{}default UFactorTimesAreaAndDesignWaterFlowRate
+
+~ N3 , \textbackslash{}field Nominal Capacity
+
+~~~~~~ \textbackslash{}type real
+
+~~~~~~ \textbackslash{}units W
+
+~~~~~~ \textbackslash{}autosizable
+
+~~~~~~ \textbackslash{}minimum 0
+
+~~~~~~ \textbackslash{}default Autosize
+
+~ N4 , \textbackslash{}field Design Inlet Water Temperature
+
+~~~~~~ \textbackslash{}units C
+
+~~~~~~ \textbackslash{}type real
+
+~~~~~~ \textbackslash{}default 82.2
+
+~ N5, \textbackslash{}field Design Inlet Air Temperature
+
+~~~~~ \textbackslash{}units C
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}default 16.6
+
+~ N6, \textbackslash{}field Design Outlet Water Temperature
+
+~~~~~ \textbackslash{}units C
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}default 71.1
+
+~ N7; \textbackslash{}field Design Outlet Air Temperature
+
+~~~~~ \textbackslash{}units C
+
+~~~~~ \textbackslash{}type real
+
+~~~~~ \textbackslash{}default 32.2
+
+This entry defines a simple water-heating coil and specifies all of the input data needed to model it. The following rules apply.
+
+\begin{itemize}
+\item
+  The first element Coil:Heating:Water is the class name (also called a keyword or key).~ This class name must be unique in the IDD.~ The maximum length for the class name is 100 characters.~ Embedded spaces are allowed and are significant.
+\item
+  In most cases, one should have fields following the object name.~ An object name by itself (terminated with a semicolon) is a ``section'' -- there may be uses for sections in input but the ``Getting'' of input is not hierarchical -- one typically gets all objects of one type and then all objects of the next type.
+\item
+  In most cases, the second field of an object should be an ``alpha'' and the field name should contain the word ``name''.~ (This will allow for certain validations later on.)
+\item
+  Commas separate fields.~ They always act as separators -- thus there is no way to include a comma in a class name or as part of a data field.
+\item
+  Similarly, semicolons are terminators -- a semicolon is always interpreted as the end of an EnergyPlus ``sentence''. So, avoid embedded semicolons in class names or data fields.
+\item
+  Blank lines are allowed.
+\item
+  Each line can be up to 500 characters in length.
+\item
+  The comment character is an exclamation or a backslash.~ Anything on a line after an ``!'' or a ``\textbackslash{}'' is ignored during EnergyPlus input.
+\end{itemize}
+
+The only significant syntax elements are the commas, the semicolon, the N's (denoting numeric data), and the A's (denoting alphanumeric data) and the exclamation and backslash.~ Everything else including blanks, end of lines, or even text that is not a comma, semicolon, N, or A is ignored.~ There are several style conventions in use however.
+
+\begin{itemize}
+\item
+  Sequence numbers are appended to the letters A or N denoting each data element.~ Thus, A2 is the second alphanumeric data item and N3 is the third numeric data item.
+\item
+  The class name contains a naming convention: type:subtype:subsubtype. For further naming conventions, please see the next section of this document.
+\item
+  Backslashes denote specially formatted comments. These comments provide information about the input, such as a description of the item, units, limits, mins \& maxes, etc., in a form that can be processed by an input editor or interface. A complete description of the backslash comment format is given at the start of the IDD file and in the Guide for Interface Developers.~ While these are ``comments'', they are quite important and allow the InputProcessor module to do some error checking for you.~~ They are also used by the IDFEditor that many users continue to use and by interface developers in understanding EnergyPlus.
+\item
+  \textbf{\textbackslash{}default} -- the number (N fields) or phrase (A fields) after this special field will be filled for any input file that has a blank in that field.
+\item
+  \textbf{\textbackslash{}minimum} or \textbf{\textbackslash{}minimum\textgreater{}} -- the number following this special field will be automatically checked during input
+\item
+  \textbf{\textbackslash{}maximum} or \textbf{\textbackslash{}maximum\textless{}} -- the number following this special field will be automatically checked during input
+\item
+  \textbf{\textbackslash{}extensible:\#} -- allows you to structure your GetInput routine so that the object arguments can be expanded (you include the number of fields in the ``extension'' and the Input Processor can automatically extend IDD definitions) -- you will still need to determine how many maximum arguments are in the object. The IDF Editor does not use this field and cannot auto-extend such objects if an IDF is encountered that has a greater number of fields than IDD allows.
+\item
+  \textbf{\textbackslash{}type integer} -- (or \textbf{real} or \textbf{alpha}) -- this field has gained increased importance after a user kept hitting an internal maximum detected by the program and kept increasing their input number until it overflowed the system's integer size. Until all types are shown on numeric fields it will be hard for the InputProcessor to provide proper error detection.
+\item
+  \textbf{There are many more \textbackslash{} fields} -- these are described at the top of the IDD.
+\end{itemize}
+
+Overall, the IDD file has very little structure.~ Generally, a new entry should be placed next to entries describing similar components.~ \emph{Coil:Heating:Water}, for instance, is grouped with entries describing other water coils.
+
+\textbf{Summary}
+
+One of the early tasks for a module developer is to create a new entry in the Input Data Dictionary.~ This entry defines the data needed to model the new component.
diff --git a/doc/module-developer/src/input-concepts/input-data-file.tex b/doc/module-developer/src/input-concepts/input-data-file.tex
new file mode 100644
index 00000000000..6f0c6bd7480
--- /dev/null
+++ b/doc/module-developer/src/input-concepts/input-data-file.tex
@@ -0,0 +1,101 @@
+\section{Input Data File}\label{input-data-file}
+
+The Input Data File (IDF) is the file containing the data for an actual simulation.~ This file is also a text (ASCII) file with a syntax ``filling in the blanks'' of the definitions in the IDD.~ A portion of an IDF with input data for the hot water coil defined in the IDD example looks like:
+
+~ Coil:Heating:Water,
+
+~~~ SPACE1-1 Zone Coil,~~~~~ !- Name
+
+~~~ ReheatCoilAvailSched,~~~ !- Availability Schedule Name
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- U-Factor Times Area Value \{W/K\}
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Maximum Water Flow Rate \{m3/s\}
+
+~~~ SPACE1-1 Zone Coil Water In Node,~ !- Water Inlet Node Name
+
+~~~ SPACE1-1 Zone Coil Water Out Node,~ !- Water Outlet Node Name
+
+~~~ SPACE1-1 Zone Coil Air In Node,~ !- Air Inlet Node Name
+
+~~~ SPACE1-1 In Node,~~~~~~~ !- Air Outlet Node Name
+
+~~~ UFactorTimesAreaAndDesignWaterFlowRate,~ !- Performance Input Method
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Nominal Capacity \{W\}
+
+~~~ 82.2,~~~~~~~~~~~~~~~~~~~ !- Design Inlet Water Temperature \{C\}
+
+~~~ 16.6,~~~~~~~~~~~~~~~~~~~ !- Design Inlet Air Temperature \{C\}
+
+~~~ 71.1,~~~~~~~~~~~~~~~~~~~ !- Design Outlet Water Temperature \{C\}
+
+~~~ 32.2;~~~~~~~~~~~~~~~~~~~ !- Design Outlet Air Temperature \{C\}
+
+~ Coil:Heating:Water,
+
+~~~ SPACE2-1 Zone Coil,~~~~~ !- Name
+
+~~~ ReheatCoilAvailSched,~~~ !- Availability Schedule Name
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- U-Factor Times Area Value \{W/K\}
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Maximum Water Flow Rate \{m3/s\}
+
+~~~ SPACE2-1 Zone Coil Water In Node,~ !- Water Inlet Node Name
+
+~~~ SPACE2-1 Zone Coil Water Out Node,~ !- Water Outlet Node Name
+
+~~~ SPACE2-1 Zone Coil Air In Node,~ !- Air Inlet Node Name
+
+~~~ SPACE2-1 In Node,~~~~~~~ !- Air Outlet Node Name
+
+~~~ UFactorTimesAreaAndDesignWaterFlowRate,~ !- Performance Input Method
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Nominal Capacity \{W\}
+
+~~~ 82.2,~~~~~~~~~~~~~~~~~~~ !- Design Inlet Water Temperature \{C\}
+
+~~~ 16.6,~~~~~~~~~~~~~~~~~~~ !- Design Inlet Air Temperature \{C\}
+
+~~~ 71.1,~ ~~~~~~~~~~~~~~~~~~!- Design Outlet Water Temperature \{C\}
+
+~~~ 32.2;~~~~~~~~~~~~~~~~~~~ !- Design Outlet Air Temperature \{C\}
+
+~ Coil:Heating:Water,
+
+~~~ SPACE3-1 Zone Coil,~~~~~ !- Name
+
+~~~ ReheatCoilAvailSched,~~~ !- Availability Schedule Name
+
+~~~ autosize, ~~~~~~~~~~~~~~~!- U-Factor Times Area Value \{W/K\}
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Maximum Water Flow Rate \{m3/s\}
+
+~~~ SPACE3-1 Zone Coil Water In Node,~ !- Water Inlet Node Name
+
+~~~ SPACE3-1 Zone Coil Water Out Node,~ !- Water Outlet Node Name
+
+~~~ SPACE3-1 Zone Coil Air In Node,~ !- Air Inlet Node Name
+
+~~~ SPACE3-1 In Node,~~~~~~~ !- Air Outlet Node Name
+
+~~~ UFactorTimesAreaAndDesignWaterFlowRate,~ !- Performance Input Method
+
+~~~ autosize,~~~~~~~~~~~~~~~ !- Nominal Capacity \{W\}
+
+~~~ 82.2,~~~~~~~~~~~~~~~~~~~ !- Design Inlet Water Temperature \{C\}
+
+~~~ 16.6,~~~~~~~~~~~~~~~~~~~ !- Design Inlet Air Temperature \{C\}
+
+~~~ 71.1,~~~~~~~~~~~~~~~~~~~ !- Design Outlet Water Temperature \{C\}
+
+~~~ 32.2;~~~~~~~~~~~~~~~~~~~ !- Design Outlet Air Temperature \{C\}
+
+Each coil entry begins with the class name (keyword) specifying the type of coil.~ Next is the coil name -- a user (or interface) created name that is unique within the given class.~ Generally in EnergyPlus, objects within a class are distinguished by unique names.~ The object name is usually the first data element following the class name.~ Any alphanumeric data item in the IDF can be up to 100 characters long.~ Any characters past 100 are truncated (lost). After the object name comes the real data.~ If we look at the IDD we see that the first data item after the object name is expected to be an alphanumeric -- a schedule name. In the IDF, we see the corresponding field is ``ReheatCoilAvailSched'', the object name of a schedule elsewhere in the IDF file. In EnergyPlus, all references to other data entries (objects) are via object names.~ The next two data items are numeric: the coil UA and the maximum water mass flow rate. The final four items are again alphanumeric -- the names of the coil inlet and outlet nodes. Nodes are used in EnergyPlus to connect HVAC components together into HVAC systems.
+
+The example illustrates the use of comments to create clear input.~ The IDF is intended to be human readable, largely for development and debugging purposes.~ Of course, most users will never see an IDF -- they will interact with EnergyPlus through a Graphical User Interface (GUI), which will write the IDF for them.~ However, a module developer is a special kind of user.~ The module developer will need to create a portion of an IDF by hand very early in the development process in order to begin testing the module under development.~ Thus, it is important to understand the IDF syntax and to use comments to create readable test IDF files.
+
+\textbf{Summary}
+
+One of the early tasks of a module developer is to create input (most likely by hand) for the new component and to insert it into an existing IDF file in order to test the new component model.~ The IDF syntax resembles the syntax for the IDD.~ The data follows the IDD class description.~ Comments should be used to make the IDF readable.
diff --git a/doc/module-developer/src/introduction.tex b/doc/module-developer/src/introduction.tex
new file mode 100644
index 00000000000..3d853eb1d97
--- /dev/null
+++ b/doc/module-developer/src/introduction.tex
@@ -0,0 +1,7 @@
+\chapter{Introduction}\label{introduction}
+
+EnergyPlus is a modular simulation program designed to model the performance, energy consumption and pollutant production of a building. EnergyPlus models energy transport through the building envelope, heat gains within the building, and all the HVAC equipment used to heat and cool the building. The program is designed for ease of development. The concept is that many people will contribute to EnergyPlus and the program structure has been designed to make this possible.
+
+EnergyPlus is written entirely in Fortran 90 with updates to Fortran 95 -- all of EnergyPlus code should be at minimum Fortran 90 compliant and can accept the newer features of Fortran 95 as well. Fortran 90/95 is a powerful modern programming language with many features. Using Fortran 90/95 it is possible to program in many different styles. The EnergyPlus team has chosen a particular style that emphasizes code extensibility (ease of development), understandability, maintainability, and robustness. Less emphasis was placed on program speed and size. Fortran 90/95 has all the features that permit the creation of readable, maintainable, and extensible code. In particular, the ability to create data and program modules with various levels of data hiding allows EnergyPlus to be built out of semi-independent modules. This allows a new EnergyPlus developer to concentrate on programming a single component without having to learn the entire program and data structure.
+
+The EnergyPlus programming style is described in the \emph{EnergyPlus Programming Standard.} The \emph{Programming Standard} should be consulted for details such as variable and subroutine naming conventions. In this document, we will describe the steps a developer must follow to create a new EnergyPlus component model. In particular, we will assume the developer wishes to simulate an HVAC component that cannot yet be modeled by EnergyPlus.
diff --git a/doc/module-developer/src/module-structure.tex b/doc/module-developer/src/module-structure.tex
new file mode 100644
index 00000000000..210d7074cdc
--- /dev/null
+++ b/doc/module-developer/src/module-structure.tex
@@ -0,0 +1,5 @@
+\chapter{Module Structure}\label{module-structure}
+
+Let us assume that the novice EnergyPlus developer wishes to model a new HVAC component called \emph{NewHVACComponent}.~ Right at the start there is a choice to make: whether to insert the new model into an existing module or to create an entirely new EnergyPlus component simulation model.~ Creating a new module is the easier option to explain, implement and test. We will discuss this option in this document.~ The discussion should also impart enough information to allow a new developer to insert a model into an existing EnergyPlus module if that option is chosen.
+
+If you intend that the module will become part of the distributed EnergyPlus, follow the guidance in the Programming Standard document.~ Even if you don't intend that your module will become part of EnergyPlus -- but you might want some advice from one of the core development team, follow the guidance in the Programming Standard.
diff --git a/doc/module-developer/src/module-structure/changing-existing-code.tex b/doc/module-developer/src/module-structure/changing-existing-code.tex
new file mode 100644
index 00000000000..9bd8e708b57
--- /dev/null
+++ b/doc/module-developer/src/module-structure/changing-existing-code.tex
@@ -0,0 +1,3 @@
+\section{Changing existing code}\label{changing-existing-code}
+
+It may be that your new module or your new feature impacts existing code.~ Should that happen, follow the guidance in the Programming Standard about positioning of ``global data''.~ Likewise, any code written should follow the guidance outlined in the Programming Standard.
diff --git a/doc/module-developer/src/module-structure/code-readability-vs-speed-of-execution.tex b/doc/module-developer/src/module-structure/code-readability-vs-speed-of-execution.tex
new file mode 100644
index 00000000000..37621b02be3
--- /dev/null
+++ b/doc/module-developer/src/module-structure/code-readability-vs-speed-of-execution.tex
@@ -0,0 +1,89 @@
+\section{Code Readability vs.~Speed of Execution}\label{code-readability-vs.speed-of-execution}
+
+Programmers throughout time have had to deal with speed of code execution and it's an ongoing concern.~ However, compilers are pretty smart these days and, often, can produce speedier code for the hardware platform than the programmer can when he or she uses ``speed up'' tips.~ The EnergyPlus development team would rather the code be more ``readable'' to all than to try to outwit the compilers for every platform.~ First and foremost, the code is the true document of what EnergyPlus does -- other documents will try to explain algorithms and such but must really take a back seat to the code itself.
+
+However, many people may read the code -- as developers, we should try to make it as readable at first glance as possible.~ For a true example from the code and a general indication of preferred style, take the case of the zone temperature update equation.~ In the \href{file:///E:/Docs4PDFs/EngineeringReference.pdf}{Engineering Reference} document, the form is recognizable and usual:
+
+\includegraphics{media/image001.png}And, this equation appears in the code (ZoneTempPredictorCorrector Module), as:
+
+ZT(ZoneNum) = (CoefSumhat +~~ CoefAirrat*(3.0*ZTM1(ZoneNum) - (3.0/2.0)*ZTM2(ZoneNum) \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ + (1./3.)* ZTM3(ZoneNum))) \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~ / ((11.0/6.0)*CoefAirrat+CoefSumha)
+
+Somewhat abbreviated here due to lack of page width but still recognizable from the original.~ A better version would actually be:
+
+ZT(ZoneNum) = (CoefSumhat -~~ CoefAirrat*(-3.0*ZTM1(ZoneNum) + (3.0/2.0)*ZTM2(ZoneNum) \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ - (1./3.)* ZTM3(ZoneNum))) \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~ / ((11.0/6.0)*CoefAirrat+CoefSumha)
+
+Whereas the natural tendency of programming would lead to the less readable:
+
+ZT(ZoneNum) = (CoefSumhat + CoefAirrat*(3.0*ZTM1(ZoneNum) -- 1.5*ZTM2(ZoneNum) + .333333* ZTM3(ZoneNum))) \&
+
+~~~~~~~~~~ / (1.83333*CoefAirrat+CoefSumha)
+
+The final version is a correct translation (more or less) from the Engineering/usual representation but much harder to look at in code and realize what is being represented.
+
+\subsection{Speed of Execution}\label{speed-of-execution}
+
+\textbf{A critical consideration in speed of execution is character string comparisons.}~ These are typically quite slow and should not be used in the core routines (i.e.~those that are executed every zone or hvac time step). An alternative to string comparisons is to define module-level integer parameters, equate a string to a parameter during the initial subroutine call (e.g.~GetInput), and then do integer comparisons through the remainder of the calls to the module.~ Doing this does not deter readability, yet assists in reducing execution time.
+
+For example, in the module shown previously (Module Fans), the parameters for fan types are set as Integers:
+
+~ !MODULE PARAMETER DEFINITIONS
+
+INTEGER, PARAMETER :: FanType\_SimpleConstVolume = 1
+
+INTEGER, PARAMETER :: FanType\_SimpleVAV~~~~~~~~ = 2
+
+INTEGER, PARAMETER :: FanType\_SimpleOnOff~~~~~~ = 3
+
+INTEGER, PARAMETER :: FanType\_ZoneExhaust~~~~~~ = 4
+
+During the GetInput, string types are shown (this is getting these objects):
+
+~~~~~~~ CALL GetObjectItem(`FAN:SIMPLE:CONSTVOLUME',~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ SimpFanNum,AlphArray, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ ~~NumAlphas,NumArray,NumNums,IOSTAT)
+
+~~~~~~~ . . .
+
+~~~~~~~ Fan(FanNum)\%FanName = AlphArray(1)
+
+~~~~~~~ Fan(FanNum)\%FanType = `SIMPLE'
+
+~~~~~~~ . . .
+
+~~~~~~~ Fan(FanNum)\%Control = `CONSTVOLUME'
+
+~~~~~~~ Fan(FanNum)\%FanType\_Num = FanType\_SimpleConstVolume
+
+Then, during the simulation the integer parameters are used:
+
+~ ! Calculate the Correct Fan Model with the current FanNum
+
+~ IF (Fan(FanNum)\%FanType\_Num = = FanType\_SimpleConstVolume) THEN
+
+~~~ Call SimSimpleFan(FanNum)
+
+~ Else IF (Fan(FanNum)\%FanType\_Num = = FanType\_SimpleVAV) THEN
+
+~~~ Call SimVariableVolumeFan(FanNum)
+
+~ Else If (Fan(FanNum)\%FanType\_Num = = FanType\_SimpleOnOff) THEN
+
+~~~ Call SimOnOffFan(FanNum)
+
+~ Else If (Fan(FanNum)\%FanType\_Num = = FanType\_ZoneExhaust) THEN
+
+~~~ Call SimZoneExhaustFan(FanNum)
+
+~ End If
+
+This does not detract from code readability at all but execution is much speedier with this versus the string comparisons.
diff --git a/doc/module-developer/src/module-structure/considerations-for-legacy-codes.tex b/doc/module-developer/src/module-structure/considerations-for-legacy-codes.tex
new file mode 100644
index 00000000000..9ebdc616091
--- /dev/null
+++ b/doc/module-developer/src/module-structure/considerations-for-legacy-codes.tex
@@ -0,0 +1,7 @@
+\section{Considerations for Legacy Codes}\label{considerations-for-legacy-codes}
+
+Those module developers who are adding to EnergyPlus's capabilities by adapting existing codes into the module structure should take special considerations.
+
+\textbf{First and foremost, who owns the legacy code that you are adapting?\emph{~ More on this is covered in Appendix C -- Submissions and Check-ins.~ One must be very careful when developing modules to be implemented in the publicly-available version of EnergyPlus.}}
+
+Legacy codes will typically come with their own input and output structures.~ In adapting a legacy code to use with EnergyPlus, the module developer will usually want to bypass these routines by embedding the code into EnergyPlus and using input entirely from the IDD/IDF structure.~ During original transition, you can consider doing a parallel effort of writing a simple input file for the legacy code while testing results with your developing EnergyPlus transition code.
diff --git a/doc/module-developer/src/module-structure/how-it-fits-together.tex b/doc/module-developer/src/module-structure/how-it-fits-together.tex
new file mode 100644
index 00000000000..a4f4e46bf12
--- /dev/null
+++ b/doc/module-developer/src/module-structure/how-it-fits-together.tex
@@ -0,0 +1,3 @@
+\section{How it fits together}\label{how-it-fits-together}
+
+Although we have designed the EnergyPlus modules to be as independent as possible, obviously they cannot be completely independent.~ How does an EnergyPlus HVAC module fit in with the rest of the program?~ In the next section we examine and describe the calling structure of the program, with particular emphasis on HVAC/Plant elements.
diff --git a/doc/module-developer/src/module-structure/module-example.tex b/doc/module-developer/src/module-structure/module-example.tex
new file mode 100644
index 00000000000..ed06dfd4650
--- /dev/null
+++ b/doc/module-developer/src/module-structure/module-example.tex
@@ -0,0 +1,2685 @@
+\section{Module Example}\label{module-example}
+
+This example can be used as a template for new HVAC component modules. In particular, the commenting structure in the module and within the subroutines should be followed closely. Of course, there is no perfect example module -- this one is particularly simple. Some others that might be examined are in files Humidifiers.f90, HVACHeatingCoils.f90 and PlantChillers.f90. Templates are also available as separate files.
+
+In particular, the module template with routines contains structure and information pertinent to module development.
+
+Note that in the following module, the ``Data IPShortcuts'' is not used -- rather those variables are allocated within this module -- likely because another module calls this one during input.
+
+\textbf{Module Fans}
+
+~ ! Module containing the fan simulation routines
+
+~ ! MODULE INFORMATION:
+
+~ !~~~~~~ AUTHOR~~~~~~~~ Richard J. Liesen
+
+~ !~~~~~~ DATE WRITTEN~~ April 1998
+
+~ !~~~~~~ MODIFIED~~~~~~ Shirey, May 2001
+
+~ !~~~~~~ RE-ENGINEERED~ na
+
+~ ! PURPOSE OF THIS MODULE:
+
+~ ! To encapsulate the data and algorithms required to
+
+~ ! manage the Fan System Component
+
+~ ! REFERENCES: none
+
+~ ! OTHER NOTES: none
+
+~ ! USE STATEMENTS:
+
+~ ! Use statements for data only modules
+
+USE DataPrecisionGlobals
+
+USE DataLoopNode
+
+USE DataHVACGlobals, ONLY: TurnFansOn, TurnFansOff, Main, Cooling, Heating, Other, \&
+
+~~~~~~~~~ OnOffFanPartLoadFraction, SmallAirVolFlow, UnbalExhMassFlow, NightVentOn, cFanTypes, \&
+
+~~~~~~~~~ FanType\_SimpleConstVolume, FanType\_SimpleVAV, FanType\_SimpleOnOff, FanType\_ZoneExhaust
+
+USE DataGlobals,~~~~ ONLY: SetupOutputVariable, BeginEnvrnFlag, BeginDayFlag, MaxNameLength, \&
+
+~~~~~~ ShowWarningError, ShowFatalError, ShowSevereError, HourofDay, SysSizingCalc, CurrentTime, \&
+
+~~~~~~ OutputFileDebug, ShowContinueError, ShowRecurringWarningErrorAtEnd, WarmupFlag, \&
+
+~ ~~~~~~~~~~~~~~~~~~~~~~~~~ShowContinueErrorTimeStamp
+
+Use DataEnvironment, ONLY: StdBaroPress, DayofMonth, Month, StdRhoAir
+
+USE Psychrometrics,~ ONLY:PsyRhoAirFnPbTdbW, PsyTdbFnHW, PsyCpAirFnWTdb
+
+~ ! Use statements for access to subroutines in other modules
+
+USE ScheduleManager
+
+IMPLICIT NONE~~~~~~~~ ! Enforce explicit typing of all variables
+
+PRIVATE ! Everything private unless explicitly made public
+
+~ !MODULE PARAMETER DEFINITIONS
+
+~ !na
+
+~ ! DERIVED TYPE DEFINITIONS
+
+TYPE FanEquipConditions
+
+~ CHARACTER(len = MaxNameLength) :: FanName~ = `'~ ! Name of the fan
+
+~ CHARACTER(len = MaxNameLength) :: FanType~ = `'~ ! Type of Fan ie. Simple, Vane axial, Centrifugal, etc.
+
+~ CHARACTER(len = MaxNameLength) :: Schedule = `'~ ! Fan Operation Schedule
+
+~ INTEGER ~~~~~:: FanType\_Num~~~~~~~~~~~~~ = 0~~~ ! DataHVACGlobals fan type
+
+~ Integer~~~~~ :: SchedPtr~~~~~~~~~~~~~~~~ = 0~~~ ! Pointer to the correct schedule
+
+~ REAL(r64)~~~ :: InletAirMassFlowRate~~~~ = 0.0~ !MassFlow through the Fan being Simulated {[}kg/Sec{]}
+
+~ REAL(r64)~~~ :: OutletAirMassFlowRate~~~ = 0.0
+
+~ REAL(r64)~~~ :: MaxAirFlowRate~~~~~~~~~~ = 0.0~ !Max Specified Volume Flow Rate of Fan {[}m3/sec{]}
+
+~ REAL(r64)~~~ :: MinAirFlowRate~~~~~~~~~~ = 0.0~ !Min Specified Volume Flow Rate of Fan {[}m3/sec{]}
+
+~ REAL(r64)~~~ :: MaxAirMassFlowRate~~~~~~ = 0.0~ ! Max flow rate of fan in kg/sec
+
+~ REAL(r64)~~~ :: MinAirMassFlowRate~~~~~~ = 0.0~ ! Min flow rate of fan in kg/sec
+
+~ REAL(r64)~~~ :: InletAirTemp~~~~~~~~~~~~ = 0.0
+
+~ REAL(r64)~~~ :: OutletAirTemp~~~~~~~~~~~ = 0.0
+
+~ REAL(r64)~~~ :: InletAirHumRat~~~~~~~~~~ = 0.0
+
+~ REAL(r64)~~~ :: OutletAirHumRat~~~~~~~~~ = 0.0
+
+~ REAL(r64)~~~ :: InletAirEnthalpy~~~~~~~~ = 0.0
+
+~ REAL(r64)~~~ :: OutletAirEnthalpy~~~~~~~ = 0.0
+
+~ REAL(r64)~~~ :: FanPower~~~~~~~~~~~~~~~~ = 0.0~ !Power of the Fan being Simulated {[}kW{]}
+
+~ REAL(r64)~~~ :: FanEnergy~~~~~~~~~~~~~~~ = 0.0~ !Fan energy in {[}kJ{]}
+
+~ REAL(r64)~~~ :: FanRuntimeFraction~~~~~~ = 0.0~ !Fraction of the timestep that the fan operates
+
+~ REAL(r64)~~~ :: DeltaTemp~~~~~~~~~~~~~~~ = 0.0~ !Temp Rise across the Fan {[}C{]}
+
+~ REAL(r64)~~~ :: DeltaPress~~~~~~~~~~~~~~ = 0.0~ !Delta Pressure Across the Fan {[}N/m2{]}
+
+~ REAL(r64)~~~ :: FanEff~~~~~~~~~~~~~~~~~~ = 0.0~ !Fan total efficiency; motor and mechanical
+
+~ REAL(r64)~~~ :: MotEff~~~~~~~~~~~~~~~~~~ = 0.0~ !Fan motor efficiency
+
+~ REAL(r64)~~~ :: MotInAirFrac~~~~~~~~~~~~ = 0.0~ !Fraction of motor heat entering air stream
+
+~ REAL(r64), Dimension(5):: FanCoeff~~~~~~~~~~~ = 0.0~ !Fan Part Load Coefficients to match fan type
+
+~ ! Mass Flow Rate Control Variables
+
+~ REAL(r64)~~~ :: MassFlowRateMaxAvail~~~~ = 0.0
+
+~ REAL(r64)~~~ :: MassFlowRateMinAvail~~~~ = 0.0
+
+~ REAL(r64)~~~ :: RhoAirStdInit~~~~~~~~~~~ = 0.0
+
+~ INTEGER~~~~~ :: InletNodeNum~~~~~~~~~~~~ = 0
+
+~ INTEGER~~~~~ :: OutletNodeNum~~~~~~~~~~~ = 0
+
+~ INTEGER~~~~~ :: NVPerfNum~~~~~~~~~~~~~~~ = 0
+
+~ INTEGER~~~~~ :: FanPowerRatAtSpeedRatCurveIndex~ = 0
+
+~ INTEGER~~~~~ :: FanEffRatioCurveIndex~~~ = 0
+
+~ CHARACTER(len = MaxNameLength) :: EndUseSubcategoryName = `'
+
+~ LOGICAL~~~~~ :: OneTimePowerRatioCheck = .TRUE. ! one time flag used for error message
+
+~ LOGICAL~~~~~ :: OneTimeEffRatioCheck = .TRUE.~~ ! one time flag used for error message
+
+END TYPE FanEquipConditions
+
+TYPE NightVentPerfData
+
+~ CHARACTER(len = MaxNameLength) :: FanName~ = `' ! Name of the fan that will use this data
+
+~ REAL(r64)~~~ :: FanEff~~~~~~~~~~~~~~~~~~ = 0.0 !Fan total efficiency; motor and mechanical
+
+~ REAL(r64)~~~ :: DeltaPress~~~~~~~~~~~~~~ = 0.0 !Delta Pressure Across the Fan {[}N/m2{]}
+
+~ REAL(r64)~~~ :: MaxAirFlowRate~~~~~~~~~~ = 0.0 !Max Specified Volume Flow Rate of Fan {[}m3/s{]}
+
+~ REAL(r64)~~~ :: MaxAirMassFlowRate~~~~~~ = 0.0 ! Max flow rate of fan in kg/sec
+
+~ REAL(r64)~~~ :: MotEff~~~~~~~~~~~~~~~~~~ = 0.0 !Fan motor efficiency
+
+~ REAL(r64)~~~ :: MotInAirFrac~~~~~~~~~~~~ = 0.0 !Fraction of motor heat entering air stream
+
+END TYPE NightVentPerfData
+
+~ !MODULE VARIABLE DECLARATIONS:
+
+~ INTEGER :: NumFans~~~~ = 0 ! The Number of Fans found in the Input
+
+~ INTEGER :: NumNightVentPerf = 0 ! number of FAN:NIGHT VENT PERFORMANCE objects found in the input
+
+~ TYPE (FanEquipConditions), ALLOCATABLE, DIMENSION(:) :: Fan
+
+~ TYPE (NightVentPerfData), ALLOCATABLE, DIMENSION(:)~ :: NightVentPerf
+
+~ LOGICAL :: GetFanInputFlag = .True.~ ! Flag set to make sure you get input once
+
+! Subroutine Specifications for the Module
+
+~~~~~~~~~ ! Driver/Manager Routines
+
+\textbf{Public~ SimulateFanComponents}
+
+~~~~~~~~~ ! Get Input routines for module
+
+PRIVATE GetFanInput
+
+~~~~~~~~~ ! Initialization routines for module
+
+PRIVATE InitFan
+
+PRIVATE SizeFan
+
+~~~~~~~~~ ! Algorithms for the module
+
+Private SimSimpleFan
+
+PRIVATE SimVariableVolumeFan
+
+PRIVATE SimZoneExhaustFan
+
+~~~~~~~~~ ! Update routine to check convergence and update nodes
+
+Private UpdateFan
+
+~~~~~~~~~ ! Reporting routines for module
+
+Private ReportFan
+
+CONTAINS
+
+! MODULE SUBROUTINES:
+
+!*************************************************************************
+
+\textbf{SUBROUTINE SimulateFanComponents(CompName,FirstHVACIteration)}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Richard Liesen
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ February 1998
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! This subroutine manages Fan component simulation.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~ USE InputProcessor, ONLY: FindItemInList
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~ CHARACTER(len = *), INTENT(IN) :: CompName
+
+~ LOGICAL,~~~~~ INTENT (IN):: FirstHVACIteration
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~ INTEGER~~~~~~~~~~~~ :: FanNum~~~~ ! current fan number
+
+~ LOGICAL,SAVE~~~~~~~ :: GetInputFlag = .True.~ ! Flag set to make sure you get input once
+
+~~~~~~~~~ ! FLOW:
+
+~ ! Obtains and Allocates fan related parameters from input file
+
+~ IF (GetInputFlag) THEN~ !First time subroutine has been entered
+
+~~~ CALL GetFanInput
+
+~~~ GetInputFlag = .false.
+
+~ End If
+
+~ ! Find the correct FanNumber with the AirLoop \& CompNum from AirLoop Derived Type
+
+~ !FanNum = AirLoopEquip(AirLoopNum)\%ComponentOfTypeNum(CompNum)
+
+~ ! Determine which Fan given the Fan Name
+
+~ FanNum = ~~ FindItemInList(CompName,Fan\%FanName,NumFans)
+
+~ IF (FanNum = = 0) THEN
+
+~~~ CALL ShowFatalError(`Fan not found ='//TRIM(CompName))
+
+~ ENDIF
+
+~ ! With the correct FanNum Initialize
+
+~ CALL InitFan(FanNum,FirstHVACIteration)~ ! Initialize all fan related parameters
+
+~ ! Calculate the Correct Fan Model with the current FanNum
+
+~ IF (Fan(FanNum)\%FanType\_Num = = FanType\_SimpleConstVolume) THEN
+
+~~~ Call SimSimpleFan(FanNum)
+
+~ Else IF (Fan(FanNum)\%FanType\_Num = = FanType\_SimpleVAV) THEN
+
+~~~ Call SimVariableVolumeFan(FanNum)
+
+~ Else If (Fan(FanNum)\%FanType\_Num = = FanType\_SimpleOnOff) THEN
+
+~~~ Call SimOnOffFan(FanNum)
+
+~ Else If (Fan(FanNum)\%FanType\_Num = = FanType\_ZoneExhaust) THEN
+
+~~~ Call SimZoneExhaustFan(FanNum)
+
+~ End If
+
+~ ! Update the current fan to the outlet nodes
+
+~ Call UpdateFan(FanNum)
+
+~ ! Report the current fan
+
+~ Call ReportFan(FanNum)
+
+~ RETURN
+
+\textbf{END SUBROUTINE SimulateFanComponents}
+
+! Get Input Section of the Module
+
+!******************************************************************************
+
+\textbf{SUBROUTINE GetFanInput}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Richard Liesen
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ April 1998
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ Shirey, May 2001
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! Obtains input data for fans and stores it in fan data structures
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! Uses ``Get'' routines to read in data.
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~ USE InputProcessor
+
+~~~ USE NodeInputManager,~~~~~ ONLY: GetOnlySingleNode
+
+~~~ USE CurveManager,~~~~~~~~~ ONLY: GetCurveIndex
+
+~~~ USE BranchNodeConnections, ONLY: TestCompSet
+
+!~~~ USE DataIPShortCuts
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~ INTEGER :: FanNum~~~~~ ! The fan that you are currently loading input into
+
+~~~ INTEGER :: NumSimpFan~ ! The number of Simple Const Vol Fans
+
+~~~ INTEGER :: NumVarVolFan ! The number of Simple Variable Vol Fans
+
+~~~ INTEGER :: NumOnOff~~~~ ! The number of Simple on-off Fans
+
+~~~ INTEGER :: NumZoneExhFan
+
+~~~ INTEGER :: SimpFanNum
+
+~~~ INTEGER :: OnOffFanNum
+
+~~~ INTEGER :: VarVolFanNum
+
+~~~ INTEGER :: ExhFanNum
+
+~~~ INTEGER :: NVPerfNum
+
+~~~ LOGICAL :: NVPerfFanFound
+
+~~~ INTEGER :: NumAlphas
+
+~~~ INTEGER :: NumNums
+
+~~~ INTEGER :: IOSTAT
+
+~~~ LOGICAL :: ErrorsFound = .false.~~ ! If errors detected in input
+
+~~~ LOGICAL :: IsNotOK~~~~~~~~~~~~~~ ! Flag to verify name
+
+~~~ LOGICAL :: IsBlank~~~~~~~~~~~~~~ ! Flag for blank name
+
+~~~ CHARACTER(len = *), PARAMETER~~~ :: RoutineName = `GetFanInput:' ! include trailing blank space
+
+~~~ CHARACTER(len = MaxNameLength+40),ALLOCATABLE, DIMENSION(:) :: cAlphaFieldNames
+
+~~~ CHARACTER(len = MaxNameLength+40),ALLOCATABLE, DIMENSION(:) :: cNumericFieldNames
+
+~~~ LOGICAL, ALLOCATABLE, DIMENSION(:) :: lNumericFieldBlanks
+
+~~~ LOGICAL, ALLOCATABLE, DIMENSION(:) :: lAlphaFieldBlanks
+
+~~~ CHARACTER(len = MaxNameLength),ALLOCATABLE, DIMENSION(:) :: cAlphaArgs
+
+~~~ REAL(r64),ALLOCATABLE, DIMENSION(:) :: rNumericArgs
+
+~~~ CHARACTER(len = MaxNameLength) :: cCurrentModuleObject
+
+~~~ INTEGER :: NumParams
+
+~~~ INTEGER :: MaxAlphas
+
+~~~ INTEGER :: MaxNumbers
+
+~~~~~~~~~ ! Flow
+
+~~~ MaxAlphas = 0
+
+~~~ MaxNumbers = 0
+
+~~~ NumSimpFan~~ = GetNumObjectsFound(`Fan:ConstantVolume')
+
+~~~ IF (NumSimpFan \textgreater{} 0) THEN
+
+~~~~~ CALL GetObjectDefMaxArgs(`Fan:ConstantVolume',NumParams,NumAlphas,NumNums)
+
+~~~~~ MaxAlphas = MAX(MaxAlphas,NumAlphas)
+
+~~~~~ MaxNumbers = MAX(MaxNumbers,NumNums)
+
+~~~ ENDIF
+
+~~~ NumVarVolFan = GetNumObjectsFound(`Fan:VariableVolume')
+
+~~~ IF (NumVarVolFan \textgreater{} 0) THEN
+
+~~~~~ CALL GetObjectDefMaxArgs(`Fan:VariableVolume',NumParams,NumAlphas,NumNums)
+
+~~~~~ MaxAlphas = MAX(MaxAlphas,NumAlphas)
+
+~~~~~ MaxNumbers = MAX(MaxNumbers,NumNums)
+
+~~~ ENDIF
+
+~~~ NumOnOff = GetNumObjectsFound(`Fan:OnOff')
+
+~~~ IF (NumOnOff \textgreater{} 0) THEN
+
+~~~~~ CALL GetObjectDefMaxArgs(`Fan:OnOff',NumParams,NumAlphas,NumNums)
+
+~~~~~ MaxAlphas = MAX(MaxAlphas,NumAlphas)
+
+~~~~~ MaxNumbers = MAX(MaxNumbers,NumNums)
+
+~~~ ENDIF
+
+~~~ NumZoneExhFan = GetNumObjectsFound(`Fan:ZoneExhaust')
+
+~~~ IF (NumZoneExhFan \textgreater{} 0) THEN
+
+~~~~~ CALL GetObjectDefMaxArgs(`Fan:ZoneExhaust',NumParams,NumAlphas,NumNums)
+
+~~~~~ MaxAlphas = MAX(MaxAlphas,NumAlphas)
+
+~~~~~ MaxNumbers = MAX(MaxNumbers,NumNums)
+
+~~~ ENDIF
+
+~~~ NumNightVentPerf = GetNumObjectsFound(`FanPerformance:NightVentilation')
+
+~~~ IF (NumNightVentPerf \textgreater{} 0) THEN
+
+~~~~~ CALL GetObjectDefMaxArgs(`FanPerformance:NightVentilation',NumParams,NumAlphas,NumNums)
+
+~~~~~ MaxAlphas = MAX(MaxAlphas,NumAlphas)
+
+~~~~~ MaxNumbers = MAX(MaxNumbers,NumNums)
+
+~~~ ENDIF
+
+~~~ ALLOCATE(cAlphaArgs(MaxAlphas))
+
+~~~ cAlphaArgs = `'
+
+~~~ ALLOCATE(cAlphaFieldNames(MaxAlphas))
+
+~~~ cAlphaFieldNames = `'
+
+~~~ ALLOCATE(lAlphaFieldBlanks(MaxAlphas))
+
+~~~ lAlphaFieldBlanks = .false.
+
+~~~ ALLOCATE(cNumericFieldNames(MaxNumbers))
+
+~~~ cNumericFieldNames = `'
+
+~~~ ALLOCATE(lNumericFieldBlanks(MaxNumbers))
+
+~~~ lNumericFieldBlanks = .false.
+
+~~~ ALLOCATE(rNumericArgs(MaxNumbers))
+
+~~~ rNumericArgs = 0.0
+
+~~~ NumFans = NumSimpFan + NumVarVolFan + NumZoneExhFan+NumOnOff
+
+~~~ IF (NumFans \textgreater{} 0) THEN
+
+~~~~~ ALLOCATE(Fan(NumFans))
+
+~~~ ENDIF
+
+~~~~~ DO SimpFanNum = 1,~ NumSimpFan
+
+~~~~~~~ FanNum = SimpFanNum
+
+~~~~~~~ cCurrentModuleObject = `Fan:ConstantVolume'
+
+~~~~~~~ CALL GetObjectItem(TRIM(cCurrentModuleObject),SimpFanNum,cAlphaArgs,NumAlphas, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ rNumericArgs,NumNums,IOSTAT, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ NumBlank = lNumericFieldBlanks,AlphaBlank = lAlphaFieldBlanks, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ AlphaFieldNames = cAlphaFieldNames,NumericFieldNames = cNumericFieldNames)
+
+~~~~~~~ IsNotOK = .false.
+
+~~~~~~~ IsBlank = .false.
+
+~~~~~~~ CALL VerifyName(cAlphaArgs(1),Fan\%FanName,FanNum-1,IsNotOK,IsBlank,TRIM(cCurrentModuleObject)//`Name')
+
+~~~~~~~ IF (IsNotOK) THEN
+
+~~~~~~~~~ ErrorsFound = .true.
+
+~~~~~~~~~ IF (IsBlank) cAlphaArgs(1) = `xxxxx'
+
+~~~~~~~ ENDIF
+
+~~~~~~~ Fan(FanNum)\%FanName~ = cAlphaArgs(1)
+
+~~~~~~~ Fan(FanNum)\%FanType = ~ cCurrentModuleObject
+
+~~~~~~~ Fan(FanNum)\%Schedule = cAlphaArgs(2)
+
+~~~~~~~ Fan(FanNum)\%SchedPtr = GetScheduleIndex(cAlphaArgs(2))
+
+~~~~~~~ IF (Fan(FanNum)\%SchedPtr = = 0) THEN
+
+~~~~~~~~~ IF (lAlphaFieldBlanks(2)) THEN
+
+~~~~~~~~~~~ CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//`:'//TRIM(cAlphaFieldNames(2))//~ \&
+
+~~~~~~~~~~~~~~~~ `is required, missing for'//TRIM(cAlphaFieldNames(1))//`='//TRIM(cAlphaArgs(1)))
+
+~~~~~~~~~ ELSE
+
+~~~~~~~~~~~ CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//`: invalid'//TRIM(cAlphaFieldNames(2))//~ \&
+
+~~~~~~~~~~~~~~ `entered ='//TRIM(cAlphaArgs(2))// \&
+
+~~~~~~~~~~~~~~ `for'//TRIM(cAlphaFieldNames(1))//`='//TRIM(cAlphaArgs(1)))
+
+~~~~~~~~~ END IF
+
+~~~~~~~~~ ErrorsFound = .true.
+
+~~~~~~~ END IF
+
+!~~~~~~~ Fan(FanNum)\%Control = `CONSTVOLUME'
+
+~~~~~~~ Fan(FanNum)\%FanType\_Num = FanType\_SimpleConstVolume
+
+~~~~~~~ Fan(FanNum)\%FanEff~~~~~~~ = rNumericArgs(1)
+
+~~~~~~~ Fan(FanNum)\%DeltaPress~~~ = rNumericArgs(2)
+
+~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = rNumericArgs(3)
+
+~~~~~~~ IF (Fan(FanNum)\%MaxAirFlowRate = = 0.0) THEN
+
+~~~~~~~~~ CALL ShowWarningError(TRIM(cCurrentModuleObject)//' = ``'//TRIM(Fan(FanNum)\%FanName)//~ \&
+
+~~~~~~~~~~~~ `" has specified 0.0 max air flow rate. It will not be used in the simulation.')
+
+~~~~~~~ ENDIF
+
+~~~~~~~ Fan(FanNum)\%MotEff~~~~~~~ = rNumericArgs(4)
+
+~~~~~~~ Fan(FanNum)\%MotInAirFrac~ = rNumericArgs(5)
+
+~~~~~~~ Fan(FanNum)\%MinAirFlowRate = 0.0
+
+~~~~~~~ Fan(FanNum)\%InletNodeNum~ = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(cAlphaArgs(3),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),~ \&
+
+~~~~~~~~ ~~~~~~~~~~~~~~~~~~~NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsNotParent)
+
+~~~~~~~ Fan(FanNum)\%OutletNodeNum = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(cAlphaArgs(4),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Outlet,1,ObjectIsNotParent)
+
+~~~~~~~ IF (NumAlphas \textgreater{} 4) THEN
+
+~~~~~~~~~ Fan(FanNum)\%EndUseSubcategoryName = cAlphaArgs(5)
+
+~~~~~~~ ELSE
+
+~~~~~~~~~ Fan(FanNum)\%EndUseSubcategoryName = `General'
+
+~~~~~~~ END IF
+
+~~~~~~~ CALL TestCompSet(TRIM(cCurrentModuleObject),cAlphaArgs(1),cAlphaArgs(3),cAlphaArgs(4),`Air Nodes')
+
+~~~~~ END DO~~ ! end Number of Simple FAN Loop
+
+~~~~~ DO VarVolFanNum = 1,~ NumVarVolFan
+
+~~~~~~~ FanNum = NumSimpFan + VarVolFanNum
+
+~~~~~~~ cCurrentModuleObject = `Fan:VariableVolume'
+
+~~~~~~~ CALL GetObjectItem(TRIM(cCurrentModuleObject),VarVolFanNum,cAlphaArgs,NumAlphas, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ rNumericArgs,NumNums,IOSTAT, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ NumBlank = lNumericFieldBlanks,AlphaBlank = lAlphaFieldBlanks, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ AlphaFieldNames = cAlphaFieldNames,NumericFieldNames = cNumericFieldNames)
+
+~~~~~~~ IsNotOK = .false.
+
+~~~~~~~ IsBlank = .false.
+
+~~~~~~~ CALL VerifyName(cAlphaArgs(1),Fan\%FanName,FanNum-1,IsNotOK,IsBlank,TRIM(cCurrentModuleObject)//`Name')
+
+~~~~~~~ IF (IsNotOK) THEN
+
+~~~~~~~~~ ErrorsFound = .true.
+
+~~~~~~~~~ IF (IsBlank) cAlphaArgs(1) = `xxxxx'
+
+~~~~~~~ ENDIF
+
+~~~~~~~ Fan(FanNum)\%FanName = cAlphaArgs(1)
+
+~~~~~~~ Fan(FanNum)\%FanType = cCurrentModuleObject
+
+~~~~~~~ Fan(FanNum)\%Schedule = cAlphaArgs(2)
+
+~~~~~~~ Fan(FanNum)\%SchedPtr = GetScheduleIndex(cAlphaArgs(2))
+
+~~~~~~~ IF (Fan(FanNum)\%SchedPtr = = 0) THEN
+
+~~~~~~~~~ IF (lAlphaFieldBlanks(2)) THEN
+
+~~~~~~~~~~~ CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//`:'//TRIM(cAlphaFieldNames(2))//~ \&
+
+~~~~~~~~~~~~~~~~ `is required, missing for'//TRIM(cAlphaFieldNames(1))//`='//TRIM(cAlphaArgs(1)))
+
+~~~~~~~~~ ELSE
+
+~~~~~~~~~~~ CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//`: invalid'//TRIM(cAlphaFieldNames(2))//~ \&
+
+~~~~~~~~~~~~~~ `entered ='//TRIM(cAlphaArgs(2))// \&
+
+~~~~~~~~~~~~~~ `for'//TRIM(cAlphaFieldNames(1))//`='//TRIM(cAlphaArgs(1)))
+
+~~~~~~~~~ END IF
+
+~~~~~~~~~ ErrorsFound = .true.
+
+~~~~~~~ ENDIF
+
+!~~~~~~~ Fan(FanNum)\%Control = `VARIABLEVOLUME'
+
+~~~~~~~ Fan(FanNum)\%FanType\_Num = FanType\_SimpleVAV
+
+~~~~~~~ Fan(FanNum)\%FanEff~~~~~~~ = rNumericArgs(1)
+
+~~~~~~~ Fan(FanNum)\%DeltaPress~~~ = rNumericArgs(2)
+
+~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = rNumericArgs(3)
+
+~~~~~~~ IF (Fan(FanNum)\%MaxAirFlowRate = = 0.0) THEN
+
+~~~~~~~~~ CALL ShowWarningError(TRIM(cCurrentModuleObject)//' = ``'//TRIM(Fan(FanNum)\%FanName)//~ \&
+
+~~~~~~~~~~~~ `" has specified 0.0 max air flow rate. It will not be used in the simulation.')
+
+~~~~~~~ ENDIF
+
+~~~~~~~ Fan(FanNum)\%MinAirFlowRate = rNumericArgs(4)
+
+~~~~~~~ Fan(FanNum)\%MotEff~~~~~~~ = rNumericArgs(5)
+
+~~~~~~~ Fan(FanNum)\%MotInAirFrac~ = rNumericArgs(6)
+
+~~~~~~~ Fan(FanNum)\%FanCoeff(1)~~ = rNumericArgs(7)
+
+~~~~~~~ Fan(FanNum)\%FanCoeff(2)~~ = rNumericArgs(8)
+
+~~~~~~~ Fan(FanNum)\%FanCoeff(3)~~ = rNumericArgs(9)
+
+~~~~~~~ Fan(FanNum)\%FanCoeff(4)~~ = rNumericArgs(10)
+
+~~~~~~~ Fan(FanNum)\%FanCoeff(5)~~ = rNumericArgs(11)
+
+~~~~~~~ IF (Fan(FanNum)\%FanCoeff(1) = = 0.0 .and. Fan(FanNum)\%FanCoeff(2) = = 0.0 .and.~ \&
+
+~~~~~~~~~~~ Fan(FanNum)\%FanCoeff(3) = = 0.0 .and. Fan(FanNum)\%FanCoeff(4) = = 0.0 .and.~ \&
+
+~~~~~~~~~~~ Fan(FanNum)\%FanCoeff(5) = = 0.0)~ THEN
+
+~~~~~~~~~~~ CALL ShowWarningError(`Fan Coefficients are all zero.~ No Fan power will be reported.')
+
+~~~~~~~~~~~ CALL ShowContinueError(`For'//TRIM(cCurrentModuleObject)//`, Fan ='//TRIM(cAlphaArgs(1)))
+
+~~~~~~~ ENDIF
+
+~~~~~~~ Fan(FanNum)\%InletNodeNum~ = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(cAlphaArgs(3),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsNotParent)
+
+~~~~~~~ Fan(FanNum)\%OutletNodeNum = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(cAlphaArgs(4),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Outlet,1,ObjectIsNotParent)
+
+~~~~~~~ IF (NumAlphas \textgreater{} 4) THEN
+
+~~~~~~~~~ Fan(FanNum)\%EndUseSubcategoryName = cAlphaArgs(5)
+
+~~~~~~~ ELSE
+
+~~~~~~~~~ Fan(FanNum)\%EndUseSubcategoryName = `General'
+
+~~~~~~~ END IF
+
+~~~~~~~ CALL TestCompSet(TRIM(cCurrentModuleObject),cAlphaArgs(1),cAlphaArgs(3),cAlphaArgs(4),`Air Nodes')
+
+~~~~~ END DO~~ ! end Number of Variable Volume FAN Loop
+
+~~~~~ DO ExhFanNum = 1,~ NumZoneExhFan
+
+~~~~~~~ FanNum = NumSimpFan + NumVarVolFan + ExhFanNum
+
+~~~~~~~ cCurrentModuleObject = `Fan:ZoneExhaust'
+
+~~~~~~~ CALL GetObjectItem(TRIM(cCurrentModuleObject),ExhFanNum,cAlphaArgs,NumAlphas, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ rNumericArgs,NumNums,IOSTAT, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ NumBlank = lNumericFieldBlanks,AlphaBlank = lAlphaFieldBlanks, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ AlphaFieldNames = cAlphaFieldNames,NumericFieldNames = cNumericFieldNames)
+
+~~~~~~~ IsNotOK = .false.
+
+~~~~~~~ IsBlank = .false.
+
+~~~~~~~ CALL VerifyName(cAlphaArgs(1),Fan\%FanName,FanNum-1,IsNotOK,IsBlank,TRIM(cCurrentModuleObject)//`Name')
+
+~~~~~~~ IF (IsNotOK) THEN
+
+~~~~~~~~~ ErrorsFound = .true.
+
+~~~~~~~~~ IF (IsBlank) cAlphaArgs(1) = `xxxxx'
+
+~~~~~~~ ENDIF
+
+~~~~~~~ Fan(FanNum)\%FanName = cAlphaArgs(1)
+
+~~~~~~~ Fan(FanNum)\%FanType = cCurrentModuleObject
+
+~~~~~~~ Fan(FanNum)\%Schedule = cAlphaArgs(2)
+
+~~~~~~~ Fan(FanNum)\%SchedPtr = GetScheduleIndex(cAlphaArgs(2))
+
+~~~~~~~ IF (Fan(FanNum)\%SchedPtr = = 0) THEN
+
+~~~~~~~~~ IF (lAlphaFieldBlanks(2)) THEN
+
+~~~~~~~~~~~ CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//`:'//TRIM(cAlphaFieldNames(2))//~ \&
+
+~~~~~~~~~~~~~~~~ `is required, missing for'//TRIM(cAlphaFieldNames(1))//`='//TRIM(cAlphaArgs(1)))
+
+~~~~~~~~~ ELSE
+
+~~~~~~~~~~~ CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//`: invalid'//TRIM(cAlphaFieldNames(2))//~ \&
+
+~~~~~~~~~~~~~~ `entered ='//TRIM(cAlphaArgs(2))// \&
+
+~~~~~~~~~~~~~~ `for'//TRIM(cAlphaFieldNames(1))//`='//TRIM(cAlphaArgs(1)))
+
+~~~~~~~~~ END IF
+
+~~~~~~~~~ ErrorsFound = .true.
+
+~~~~~~~ ELSE
+
+~~~~~~~~~ IF (HasFractionalScheduleValue(Fan(FanNum)\%SchedPtr)) THEN
+
+~~~~~~~~~~~ CALL ShowWarningError(TRIM(cCurrentModuleObject)//' = ``'//TRIM(Fan(FanNum)\%FanName)//~ \&
+
+~~~~~~~~~~~~~ `" has fractional values in Schedule ='//TRIM(cAlphaArgs(2))//`. Only 0.0 in the schedule value turns the fan off.')
+
+~~~~~~~~~ ENDIF
+
+~~~~~~~ ENDIF
+
+!~~~~~~~ Fan(FanNum)\%Control = `CONSTVOLUME'
+
+~~~~~~~ Fan(FanNum)\%FanType\_Num = FanType\_ZoneExhaust
+
+~~~~~~~ Fan(FanNum)\%FanEff~~~~~~~ = rNumericArgs(1)
+
+~~~~~~~ Fan(FanNum)\%DeltaPress~~~ = rNumericArgs(2)
+
+~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = rNumericArgs(3)
+
+~~~~~~~ Fan(FanNum)\%MotEff~~~~~~~ = 1.0
+
+~~~~~~~ Fan(FanNum)\%MotInAirFrac~ = 1.0
+
+~~~~~~~ Fan(FanNum)\%MinAirFlowRate = 0.0
+
+~~~~~~~ Fan(FanNum)\%RhoAirStdInit = StdRhoAir
+
+~~~~~~~ Fan(FanNum)\%MaxAirMassFlowRate = Fan(FanNum)\%MaxAirFlowRate * Fan(FanNum)\%RhoAirStdInit
+
+~~~~~~~ IF (Fan(FanNum)\%MaxAirFlowRate = = 0.0) THEN
+
+~~~~~~~~~ CALL ShowWarningError(TRIM(cCurrentModuleObject)//' = ``'//TRIM(Fan(FanNum)\%FanName)//~ \&
+
+~~~~~~~~~~~~~ `" has specified 0.0 max air flow rate. It will not be used in the simulation.')
+
+~~~~~~~ ENDIF
+
+~~~~~~~ Fan(FanNum)\%InletNodeNum~ = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(cAlphaArgs(3),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsNotParent)
+
+~~~~~~~ Fan(FanNum)\%OutletNodeNum = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(cAlphaArgs(4),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Outlet,1,ObjectIsNotParent)
+
+~~~~~~~ IF (NumAlphas \textgreater{} 4) THEN
+
+~~~~~~~~~ Fan(FanNum)\%EndUseSubcategoryName = cAlphaArgs(5)
+
+~~~~~~~ ELSE
+
+~~~~~~~~~ Fan(FanNum)\%EndUseSubcategoryName = `General'
+
+~~~~~~~ END IF
+
+~~~~~~~ ! Component sets not setup yet for zone equipment
+
+~~~~~~~ ! CALL TestCompSet(TRIM(cCurrentModuleObject),cAlphaArgs(1),cAlphaArgs(3),cAlphaArgs(4),`Air Nodes')
+
+~~~~~ END DO~~ ! end of Zone Exhaust Fan loop
+
+~~~~~ DO OnOffFanNum = 1,~ NumOnOff
+
+~~~~~~~ FanNum = NumSimpFan + NumVarVolFan + NumZoneExhFan + OnOffFanNum
+
+~~~~~~~ cCurrentModuleObject = `Fan:OnOff'
+
+~~~~~~~ CALL GetObjectItem(TRIM(cCurrentModuleObject),OnOffFanNum,cAlphaArgs,NumAlphas, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ rNumericArgs,NumNums,IOSTAT, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ NumBlank = lNumericFieldBlanks,AlphaBlank = lAlphaFieldBlanks, \&
+
+~~~~~~~~~~~~~~~~~~~ ~~~~~~~AlphaFieldNames = cAlphaFieldNames,NumericFieldNames = cNumericFieldNames)
+
+~~~~~~~ IsNotOK = .false.
+
+~~~~~~~ IsBlank = .false.
+
+~~~~~~~ CALL VerifyName(cAlphaArgs(1),Fan\%FanName,FanNum-1,IsNotOK,IsBlank,TRIM(cCurrentModuleObject)//`Name')
+
+~~~~~~~ IF (IsNotOK) THEN
+
+~~~~~~~~~ ErrorsFound = .true.
+
+~~~~~~~~~ IF (IsBlank) cAlphaArgs(1) = `xxxxx'
+
+~~~~~~~ ENDIF
+
+~~~~~~~ Fan(FanNum)\%FanName~ = cAlphaArgs(1)
+
+~~~~~~~ Fan(FanNum)\%FanType~ = cCurrentModuleObject
+
+~~~~~~~ Fan(FanNum)\%Schedule = cAlphaArgs(2)
+
+~~~~~~~ Fan(FanNum)\%SchedPtr = GetScheduleIndex(cAlphaArgs(2))
+
+~~~~~~~ IF (Fan(FanNum)\%SchedPtr = = 0) THEN
+
+~~~~~~~~~ IF (lAlphaFieldBlanks(2)) THEN
+
+~~~~~~~~~~~ CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//`:'//TRIM(cAlphaFieldNames(2))//~ \&
+
+~~~~~~~~~~~~~~ ~~`is required, missing for'//TRIM(cAlphaFieldNames(1))//`='//TRIM(cAlphaArgs(1)))
+
+~~~~~~~~~ ELSE
+
+~~~~~~~~~~~ CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//`: invalid'//TRIM(cAlphaFieldNames(2))//~ \&
+
+~~~~~~~~~~~~~~ `entered ='//TRIM(cAlphaArgs(2))// \&
+
+~~~~~~~~~~~~~~ `for'//TRIM(cAlphaFieldNames(1))//`='//TRIM(cAlphaArgs(1)))
+
+~~~~~~~~~ END IF
+
+~~~~~~~~~ ErrorsFound = .true.
+
+~~~~~~~ ENDIF
+
+!~~~~~~~ Fan(FanNum)\%Control = `ONOFF'
+
+~~~~~~~ Fan(FanNum)\%FanType\_Num = FanType\_SimpleOnOff
+
+~~~~~~~ Fan(FanNum)\%FanEff~~~~~~~ = rNumericArgs(1)
+
+~~~~~~~ Fan(FanNum)\%DeltaPress~~~ = rNumericArgs(2)
+
+~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = rNumericArgs(3)
+
+~~~~~~~ IF (Fan(FanNum)\%MaxAirFlowRate = = 0.0) THEN
+
+~~~~~~~~~ CALL ShowWarningError(TRIM(cCurrentModuleObject)//' = ``'//TRIM(Fan(FanNum)\%FanName)//~ \&
+
+~~~~~~~~~~~~~ `" has specified 0.0 max air flow rate. It will not be used in the simulation.')
+
+~~~~~~~ ENDIF
+
+!~~~~~~ the following two structure variables are set here, as well as in InitFan, for the Heat Pump:Water Heater object
+
+!~~~~~~ (Standard Rating procedure may be called before BeginEnvirFlag is set to TRUE, if so MaxAirMassFlowRate = 0)
+
+~~~~~~~ Fan(FanNum)\%RhoAirStdInit = StdRhoAir
+
+~~~~~~~ Fan(FanNum)\%MaxAirMassFlowRate = Fan(FanNum)\%MaxAirFlowRate * Fan(FanNum)\%RhoAirStdInit
+
+~~~~~~~ Fan(FanNum)\%MotEff~~~~~~~ = rNumericArgs(4)
+
+~~~~~~~ Fan(FanNum)\%MotInAirFrac~ = rNumericArgs(5)
+
+~~~~~~~ Fan(FanNum)\%MinAirFlowRate = 0.0
+
+~~~~~~~ Fan(FanNum)\%InletNodeNum~ = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(cAlphaArgs(3),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1), \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsNotParent)
+
+~~~~~~~ Fan(FanNum)\%OutletNodeNum = \&
+
+~~~~~~~~~~~~~~ GetOnlySingleNode(cAlphaArgs(4),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1), \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~ NodeType\_Air,NodeConnectionType\_Outlet,1,ObjectIsNotParent)
+
+~~~~~~~ IF (NumAlphas \textgreater{} 4 .AND. .NOT. lAlphaFieldBlanks(5)) THEN
+
+~~~~~~~~~ Fan(FanNum)\%FanPowerRatAtSpeedRatCurveIndex~ = GetCurveIndex(cAlphaArgs(5))
+
+~~~~~~~ END IF
+
+~~~~~~~ IF (NumAlphas \textgreater{} 5 .AND. .NOT. lAlphaFieldBlanks(6)) THEN
+
+~~~~~~~~~ Fan(FanNum)\%FanEffRatioCurveIndex~ = GetCurveIndex(cAlphaArgs(6))
+
+~~~~~~~ END IF
+
+~~~~~~~ IF (NumAlphas \textgreater{} 6 .AND. .NOT. lAlphaFieldBlanks(7)) THEN
+
+~~~~~~~~~ Fan(FanNum)\%EndUseSubcategoryName = cAlphaArgs(7)
+
+~~~~~~~ ELSE
+
+~~~~~~~~~ Fan(FanNum)\%EndUseSubcategoryName = `General'
+
+~~~~~~~ END IF
+
+~~~~~~~ CALL TestCompSet(TRIM(cCurrentModuleObject),cAlphaArgs(1),cAlphaArgs(3),cAlphaArgs(4),`Air Nodes')
+
+~ ~~~~END DO~~ ! end Number of Simple~ ON-OFF FAN Loop
+
+~~~~~ cCurrentModuleObject = `FanPerformance:NightVentilation'
+
+~~~~~ NumNightVentPerf = GetNumObjectsFound(TRIM(cCurrentModuleObject))
+
+~~~~~ IF (NumNightVentPerf \textgreater{} 0) THEN
+
+~~~~~~~ ALLOCATE(NightVentPerf(NumNightVentPerf))
+
+~~~~~~~ NightVentPerf\%FanName = `'
+
+~~~~~~~ NightVentPerf\%FanEff = 0.0
+
+~~~~~~~ NightVentPerf\%DeltaPress = 0.0
+
+~~~~~~~ NightVentPerf\%MaxAirFlowRate = 0.0
+
+~~~~~~~ NightVentPerf\%MotEff = 0.0
+
+~~~~~~~ NightVentPerf\%MotInAirFrac = 0.0
+
+~~~~~~~ NightVentPerf\%MaxAirMassFlowRate = 0.0
+
+~~~~~ END IF
+
+~~~~~ ! input the night ventilation performance objects
+
+~~~~~ DO NVPerfNum = 1,NumNightVentPerf
+
+~~~~~~~~ CALL GetObjectItem(TRIM(cCurrentModuleObject),NVPerfNum,cAlphaArgs,NumAlphas, \&
+
+~~~~~~~~~~~~ ~~~~~~~~~~~~~~rNumericArgs,NumNums,IOSTAT, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ NumBlank = lNumericFieldBlanks,AlphaBlank = lAlphaFieldBlanks, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ AlphaFieldNames = cAlphaFieldNames,NumericFieldNames = cNumericFieldNames)
+
+~~~~~~~ IsNotOK = .false.
+
+~~~~~~~ IsBlank = .false.
+
+~~~~~~~ CALL VerifyName(cAlphaArgs(1),NightVentPerf\%FanName,NVPerfNum-1,IsNotOK,IsBlank,TRIM(cCurrentModuleObject)//`Name')
+
+~~~~~~~ IF (IsNotOK) THEN
+
+~~~~~~~~~ ErrorsFound = .true.
+
+~~~~~~~~~ IF (IsBlank) cAlphaArgs(1) = `xxxxx'
+
+~~~~~~~ ENDIF
+
+~~~~~~~ NightVentPerf(NVPerfNum)\%FanName~~~~~~~ = cAlphaArgs(1)
+
+~~~~~~~ NightVentPerf(NVPerfNum)\%FanEff~~~~~~~~ = rNumericArgs(1)
+
+~~~~~~~ NightVentPerf(NVPerfNum)\%DeltaPress~~~~ = rNumericArgs(2)
+
+~~~~~~~ NightVentPerf(NVPerfNum)\%MaxAirFlowRate = rNumericArgs(3)
+
+~~~~~~~ NightVentPerf(NVPerfNum)\%MotEff~~~~~~~~ = rNumericArgs(4)
+
+~~~~~~~ NightVentPerf(NVPerfNum)\%MotInAirFrac~~ = rNumericArgs(5)
+
+~~~~~~~ ! find the corresponding fan
+
+~~~~~~~ NVPerfFanFound = .FALSE.
+
+~~~~~~~ DO FanNum = 1,NumFans
+
+~~~~~~~~~ IF (NightVentPerf(NVPerfNum)\%FanName = = Fan(FanNum)\%FanName) THEN
+
+~~~~~~~~~~~ NVPerfFanFound = .TRUE.
+
+~~~~~~~~~~~ Fan(FanNum)\%NVPerfNum = NVPerfNum
+
+~~~~~~~~~~~ EXIT
+
+~~~~~~~~~ END IF
+
+~~~~~~~ END DO
+
+~~~~~~~ IF ( .NOT. NVPerfFanFound) THEN
+
+~~~~~~~~~ CALL ShowSevereError(TRIM(cCurrentModuleObject)//`, fan name not found ='//TRIM(cAlphaArgs(1)))
+
+~~~~~~~~~ ErrorsFound = .true.
+
+~~~~~~~ END IF
+
+~~~~~ END DO
+
+~~~~~ DEALLOCATE(cAlphaArgs)
+
+~~~~~ DEALLOCATE(cAlphaFieldNames)
+
+~~~~~ DEALLOCATE(lAlphaFieldBlanks)
+
+~~~~~ DEALLOCATE(cNumericFieldNames)
+
+~~~~~ DEALLOCATE(lNumericFieldBlanks)
+
+~~~~~ DEALLOCATE(rNumericArgs)
+
+~~~~~ IF (ErrorsFound) THEN
+
+~~~~~~~~~~~ CALL ShowFatalError(RoutineName//`Errors found in input.~ Program terminates.')
+
+~~~~~ ENDIF
+
+~~~~~ Do FanNum = 1,NumFans
+
+~~~~~~~~~~~~ ! Setup Report variables for the Fans
+
+~~~~~~ CALL SetupOutputVariable(`Fan Electric Power{[}W{]}', Fan(FanNum)\%FanPower, `System',`Average',Fan(FanNum)\%FanName)
+
+~~~~~~ CALL SetupOutputVariable(`Fan Delta Temp{[}C{]}', Fan(FanNum)\%DeltaTemp, `System',`Average',Fan(FanNum)\%FanName)
+
+~~~~~~ CALL SetupOutputVariable(`Fan Electric Consumption{[}J{]}', Fan(FanNum)\%FanEnergy, `System',`Sum',Fan(FanNum)\%FanName, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ ResourceTypeKey = `Electric',GroupKey = `System', \&
+
+~~ ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~EndUseKey = `Fans',EndUseSubKey = Fan(FanNum)\%EndUseSubcategoryName)
+
+~~~~~ END DO
+
+~~~~~ DO OnOffFanNum = 1,~ NumOnOff
+
+~~~~~~ FanNum = NumSimpFan + NumVarVolFan + NumZoneExhFan + OnOffFanNum
+
+~~~~~~ CALL SetupOutputVariable(`On/Off Fan Runtime Fraction', Fan(FanNum)\%FanRuntimeFraction, `System',`Average', \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Fan(FanNum)\%FanName)
+
+~~~~~ END DO
+
+~ RETURN
+
+\textbf{END SUBROUTINE GetFanInput}
+
+! End of Get Input subroutines for the HB Module
+
+!******************************************************************************
+
+! Beginning Initialization Section of the Module
+
+!******************************************************************************
+
+\textbf{SUBROUTINE InitFan(FanNum,FirstHVACIteration)}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Richard J. Liesen
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ February 1998
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! This subroutine is for initializations of the Fan Components.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! Uses the status flags to trigger initializations.
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~ USE DataSizing, ONLY: CurSysNum
+
+~ USE DataAirLoop, ONLY: AirLoopControlInfo
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~ LOGICAL, INTENT (IN):: FirstHVACIteration
+
+~ Integer, Intent(IN) :: FanNum
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~ Integer~~~~~~~~~~~~ :: InletNode
+
+~ Integer~~~~~~~~~~~~ :: OutletNode
+
+~ Integer~~~~~~~~~~~~ :: InNode
+
+~ Integer~~~~~~~~~~~~ :: OutNode
+
+~ LOGICAL,SAVE~~~~~~~ :: MyOneTimeFlag = .true.
+
+~ LOGICAL, ALLOCATABLE,Save, DIMENSION(:) :: MyEnvrnFlag
+
+~ LOGICAL, ALLOCATABLE,Save, DIMENSION(:) :: MySizeFlag
+
+~~~~~~~~~ ! FLOW:
+
+~ IF (MyOneTimeFlag) THEN
+
+~~~ ALLOCATE(MyEnvrnFlag(NumFans))
+
+~~~ ALLOCATE(MySizeFlag(NumFans))
+
+~~~ MyEnvrnFlag = .TRUE.
+
+~~~ MySizeFlag = .TRUE.
+
+~~~ MyOneTimeFlag = .false.
+
+~ END IF
+
+~ IF ( .NOT. SysSizingCalc .AND. MySizeFlag(FanNum)) THEN
+
+~~~ CALL SizeFan(FanNum)
+
+~~~ ! Set the loop cycling flag
+
+~~~ IF (Fan(FanNum)\%Control = = `ONOFF') THEN
+
+~~~~~ IF (CurSysNum \textgreater{} 0) THEN
+
+~~~~~~~ AirLoopControlInfo(CurSysNum)\%CyclingFan = .TRUE.
+
+~ ~~~~END IF
+
+~~~ END IF
+
+~~~ MySizeFlag(FanNum) = .FALSE.
+
+~ END IF
+
+! Do the Begin Environment initializations
+
+~ IF (BeginEnvrnFlag .and. MyEnvrnFlag(FanNum)) THEN
+
+~~~ !For all Fan inlet nodes convert the Volume flow to a mass flow
+
+~~~ InNode = Fan(FanNum)\%InletNodeNum
+
+~~~ OutNode = Fan(FanNum)\%OutletNodeNum
+
+~~~ Fan(FanNum)\%RhoAirStdInit = PsyRhoAirFnPbTdbW(StdBaroPress,20.0,0.0)
+
+~~~ !Change the Volume Flow Rates to Mass Flow Rates
+
+~~~ Fan(FanNum)\%MaxAirMassFlowRate = Fan(FanNum)\%MaxAirFlowRate *~ Fan(FanNum)\%RhoAirStdInit
+
+~~~ Fan(FanNum)\%MinAirMassFlowRate = Fan(FanNum)\%MinAirFlowRate *~ Fan(FanNum)\%RhoAirStdInit
+
+~~~ !Init the Node Control variables
+
+~~~ Node(OutNode)\%MassFlowRateMax~~~~~ = Fan(FanNum)\%MaxAirMassFlowRate
+
+~~~ Node(OutNode)\%MassFlowRateMin~~~~~ = Fan(FanNum)\%MinAirMassFlowRate
+
+~~~ !Initialize all report variables to a known state at beginning of simulation
+
+~~~ Fan(FanNum)\%FanPower = 0.0
+
+~~~ Fan(FanNum)\%DeltaTemp = 0.0
+
+~~~ Fan(FanNum)\%FanEnergy = 0.0
+
+~~~ MyEnvrnFlag(FanNum) = .FALSE.
+
+~ END IF
+
+~ IF (.not. BeginEnvrnFlag) THEN
+
+~~~ MyEnvrnFlag(FanNum) = .true.
+
+~ ENDIF
+
+~ ! Do the Begin Day initializations
+
+~~~ ! none
+
+~ ! Do the begin HVAC time step initializations
+
+~~~ ! none
+
+~ ! Do the following initializations (every time step): This should be the info from
+
+~ ! the previous components outlets or the node data in this section.
+
+~ ! Do a check and make sure that the max and min available(control) flow is
+
+~ ! between the physical max and min for the Fan while operating.
+
+~ InletNode = Fan(FanNum)\%InletNodeNum
+
+~ OutletNode = Fan(FanNum)\%OutletNodeNum
+
+~ Fan(FanNum)\%MassFlowRateMaxAvail = MIN(Node(OutletNode)\%MassFlowRateMax, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Node(InletNode)\%MassFlowRateMaxAvail)
+
+~ Fan(FanNum)\%MassFlowRateMinAvail = MIN(MAX(Node(OutletNode)\%MassFlowRateMin, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Node(InletNode)\%MassFlowRateMinAvail), \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Node(InletNode)\%MassFlowRateMaxAvail)
+
+~ ! Load the node data in this section for the component simulation
+
+~ !
+
+~ !First need to make sure that the massflowrate is between the max and min avail.
+
+~ IF (Fan(FanNum)\%FanType .NE. `ZONE EXHAUST FAN') THEN
+
+~~~ Fan(FanNum)\%InletAirMassFlowRate = Min(Node(InletNode)\%MassFlowRate, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Fan(FanNum)\%MassFlowRateMaxAvail)
+
+~~~ Fan(FanNum)\%InletAirMassFlowRate = Max(Fan(FanNum)\%InletAirMassFlowRate, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ ~~~~~~~~~~~~~~~~~~Fan(FanNum)\%MassFlowRateMinAvail)
+
+~ ELSE~ ! zone exhaust fans - always run at the max
+
+~~~ Fan(FanNum)\%MassFlowRateMaxAvail = Fan(FanNum)\%MaxAirMassFlowRate
+
+~~~ Fan(FanNum)\%MassFlowRateMinAvail = 0.0
+
+~~~ Fan(FanNum)\%InletAirMassFlowRate = Fan(FanNum)\%MassFlowRateMaxAvail
+
+~ END IF
+
+~ !Then set the other conditions
+
+~ Fan(FanNum)\%InletAirTemp~~~~~~~~ = Node(InletNode)\%Temp
+
+~ Fan(FanNum)\%InletAirHumRat~~~~~~ = Node(InletNode)\%HumRat
+
+~ Fan(FanNum)\%InletAirEnthalpy~~~~ = Node(InletNode)\%Enthalpy
+
+~ RETURN
+
+\textbf{END SUBROUTINE InitFan}
+
+\textbf{SUBROUTINE SizeFan(FanNum)}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Fred Buhl
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ September 2001
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! This subroutine is for sizing Fan Components for which flow rates have not been
+
+~~~~~~~~~ ! specified in the input.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! Obtains flow rates from the zone or system sizing arrays.
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~ USE DataSizing
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~ Integer, Intent(IN) :: FanNum
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~ REAL :: FanMinAirFlowRate
+
+~ EXTERNAL ReportSizingOutput
+
+~ FanMinAirFlowRate = 0.0
+
+~ IF (Fan(FanNum)\%MaxAirFlowRate = = AutoSize) THEN
+
+~~~ IF (CurSysNum \textgreater{} 0) THEN
+
+~~~~~ CALL CheckSysSizing(`FAN:'//TRIM(Fan(FanNum)\%FanType)// `:' // TRIM(Fan(FanNum)\%Control), \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ Fan(FanNum)\%FanName)
+
+~~~~~ SELECT CASE(CurDuctType)
+
+~~~~~~~ CASE(Main)
+
+~~~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = FinalSysSizing(CurSysNum)\%DesMainVolFlow
+
+~~~~~~~~~ FanMinAirFlowRate = CalcSysSizing(CurSysNum)\%SysAirMinFlowRat * CalcSysSizing(CurSysNum)\%DesMainVolFlow
+
+~~~~~~~ CASE(Cooling)
+
+~~~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = FinalSysSizing(CurSysNum)\%DesCoolVolFlow
+
+~~~~~~~~~ FanMinAirFlowRate = CalcSysSizing(CurSysNum)\%SysAirMinFlowRat * CalcSysSizing(CurSysNum)\%DesCoolVolFlow
+
+~~~~~~~ CASE(Heating)
+
+~~~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = FinalSysSizing(CurSysNum)\%DesHeatVolFlow
+
+~~~~~~~~~ FanMinAirFlowRate = CalcSysSizing(CurSysNum)\%SysAirMinFlowRat * CalcSysSizing(CurSysNum)\%DesHeatVolFlow
+
+~~~~~~~ CASE(Other)
+
+~~~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = FinalSysSizing(CurSysNum)\%DesMainVolFlow
+
+~~~~~~~~~ FanMinAirFlowRate = CalcSysSizing(CurSysNum)\%SysAirMinFlowRat * CalcSysSizing(CurSysNum)\%DesMainVolFlow
+
+~~~~~~~ CASE DEFAULT
+
+~~~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = FinalSysSizing(CurSysNum)\%DesMainVolFlow
+
+~~~~~~~~~ FanMinAirFlowRate = CalcSysSizing(CurSysNum)\%SysAirMinFlowRat * CalcSysSizing(CurSysNum)\%DesMainVolFlow
+
+~~~~~ END SELECT
+
+~~~ ELSE IF (CurZoneEqNum \textgreater{} 0) THEN
+
+~~~~~ CALL CheckZoneSizing(`FAN:' // TRIM(Fan(FanNum)\%FanType) // `:' // TRIM(Fan(FanNum)\%Control), \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~ Fan(FanNum)\%FanName)
+
+~~~~~ IF (.NOT. ZoneHeatingOnlyFan) THEN
+
+~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = MAX(FinalZoneSizing(CurZoneEqNum)\%DesCoolVolFlow, \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ FinalZoneSizing(CurZoneEqNum)\%DesHeatVolFlow)
+
+~~~~~ ELSE
+
+~~~~~~~ Fan(FanNum)\%MaxAirFlowRate = FinalZoneSizing(CurZoneEqNum)\%DesHeatVolFlow
+
+~~~~~ END IF
+
+~~~ END IF
+
+~~~ IF (Fan(FanNum)\%MaxAirFlowRate \textless{} SmallAirVolFlow) THEN
+
+~~~~~ Fan(FanNum)\%MaxAirFlowRate = 0.0
+
+~~~ END IF
+
+~~~ CALL ReportSizingOutput(`FAN:' // TRIM(Fan(FanNum)\%FanType) // `:' // TRIM(Fan(FanNum)\%Control), \&
+
+~~~ ~~~~~~~~~~~~~~~~~~~~~~~~Fan(FanNum)\%FanName, `Max Flow Rate {[}m3/s{]}', Fan(FanNum)\%MaxAirFlowRate)
+
+~~~ IF (Fan(FanNum)\%Control = = `VARIABLEVOLUME') THEN
+
+~~~~~ CALL CheckSysSizing(`FAN:' // TRIM(Fan(FanNum)\%FanType) // `:' // TRIM(Fan(FanNum)\%Control), \&
+
+~~ ~~~~~~~~~~~~~~~~~~~~~~~~Fan(FanNum)\%FanName)
+
+~~~~~ Fan(FanNum)\%MinAirFlowRate = FanMinAirFlowRate
+
+~~~~~ CALL ReportSizingOutput(`FAN:' // TRIM(Fan(FanNum)\%FanType) // `:' // TRIM(Fan(FanNum)\%Control), \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Fan(FanNum)\%FanName, `Min Flow Rate {[}m3/s{]}', Fan(FanNum)\%MinAirFlowRate)
+
+~~~ END IF
+
+~ END IF
+
+~ RETURN
+
+\textbf{END SUBROUTINE SizeFan}
+
+! End Initialization Section of the Module
+
+!******************************************************************************
+
+! Begin Algorithm Section of the Module
+
+!******************************************************************************
+
+\textbf{SUBROUTINE SimSimpleFan(FanNum)}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Unknown
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ Unknown
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! This subroutine simulates the simple constant volume fan.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! Converts design pressure rise and efficiency into fan power and temperature rise
+
+~~~~~~~~~ ! Constant fan pressure rise is assumed.
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! ASHRAE HVAC 2 Toolkit, page 2-3 (FANSIM)
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~ Integer, Intent(IN) :: FanNum
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~ Real RhoAir
+
+~~~~~ Real DeltaPress~ ! {[}N/M\^{}2{]}
+
+~~~~~ Real FanEff
+
+~~~~~ Real MassFlow~~~ ! {[}kg/sec{]}
+
+~~~~~ Real Tin~~~~~~~~ ! {[}C{]}
+
+~~~~~ Real Win
+
+~~~~~ Real FanShaftPower ! power delivered to fan shaft
+
+~~~~~ Real PowerLossToAir ! fan and motor loss to air stream (watts)
+
+~~ DeltaPress = Fan(FanNum)\%DeltaPress
+
+~~ FanEff~~~~ = Fan(FanNum)\%FanEff
+
+~~ ! For a Constant Volume Simple Fan the Max Flow Rate is the Flow Rate for the fan
+
+~~ Tin~~~~~~~ = Fan(FanNum)\%InletAirTemp
+
+~~ Win~~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ RhoAir~~~~ = Fan(FanNum)\%RhoAirStdInit
+
+~~ MassFlow~~ = MIN(Fan(FanNum)\%InletAirMassFlowRate,Fan(FanNum)\%MaxAirMassFlowRate)
+
+~~ MassFlow~~ = MAX(MassFlow,Fan(FanNum)\%MinAirMassFlowRate)
+
+~~ !
+
+~~ !Determine the Fan Schedule for the Time step
+
+~ If( ( GetCurrentScheduleValue(Fan(FanNum)\%SchedPtr)\textgreater{}0.0 .and. Massflow\textgreater{}0.0 .or. TurnFansOn .and. Massflow\textgreater{}0.0) \&
+
+~~~~~~~ .and. .NOT.TurnFansOff ) Then
+
+~~ !Fan is operating
+
+~~ Fan(FanNum)\%FanPower = MassFlow*DeltaPress/(FanEff*RhoAir) ! total fan power
+
+~~ FanShaftPower = Fan(FanNum)\%MotEff * Fan(FanNum)\%FanPower~ ! power delivered to shaft
+
+~~ PowerLossToAir = FanShaftPower + (Fan(FanNum)\%FanPower - FanShaftPower) * Fan(FanNum)\%MotInAirFrac
+
+~~ Fan(FanNum)\%OutletAirEnthalpy = Fan(FanNum)\%InletAirEnthalpy + PowerLossToAir/MassFlow
+
+~~ ! This fan does not change the moisture or Mass Flow across the component
+
+~~ Fan(FanNum)\%OutletAirHumRat~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ Fan(FanNum)\%OutletAirMassFlowRate = MassFlow
+
+~~ Fan(FanNum)\%OutletAirTemp = PsyTdbFnHW(Fan(FanNum)\%OutletAirEnthalpy,Fan(FanNum)\%OutletAirHumRat)
+
+~Else
+
+~~ !Fan is off and not operating no power consumed and mass flow rate.
+
+~~ Fan(FanNum)\%FanPower = 0.0
+
+~~ FanShaftPower = 0.0
+
+~~ PowerLossToAir = 0.0
+
+~~ Fan(FanNum)\%OutletAirMassFlowRate = 0.0
+
+~~ Fan(FanNum)\%OutletAirHumRat~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ Fan(FanNum)\%OutletAirEnthalpy~~~~ = Fan(FanNum)\%InletAirEnthalpy
+
+~~ Fan(FanNum)\%OutletAirTemp = Fan(FanNum)\%InletAirTemp
+
+~~ ! Set the Control Flow variables to 0.0 flow when OFF.
+
+~~ Fan(FanNum)\%MassFlowRateMaxAvail = 0.0
+
+~~ Fan(FanNum)\%MassFlowRateMinAvail = 0.0
+
+~End If
+
+~RETURN
+
+\textbf{END SUBROUTINE SimSimpleFan}
+
+\textbf{SUBROUTINE SimVariableVolumeFan(FanNum)}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Unknown
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ Unknown
+
+~~~~~~ ~~~!~~~~~~ MODIFIED~~~~~~ Phil Haves
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! This subroutine simulates the simple variable volume fan.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! Converts design pressure rise and efficiency into fan power and temperature rise
+
+~~~~~~~~~ ! Constant fan pressure rise is assumed.
+
+~~~~~~~~~ ! Uses curves of fan power fraction vs.~fan part load to determine fan power at
+
+~~~~~~~~~ ! off design conditions.
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! ASHRAE HVAC 2 Toolkit, page 2-3 (FANSIM)
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~ Integer, Intent(IN) :: FanNum
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~ Real RhoAir
+
+~~~~~ Real DeltaPress~ ! {[}N/M\^{}2 = Pa{]}
+
+~~~~~ Real FanEff~~~~~ ! Total fan efficiency - combined efficiency of fan, drive train,
+
+~~~~~~~~~~~~~~~~~~~~~~ ! motor and variable speed controller (if any)
+
+~~~~~ Real MassFlow~~~ ! {[}kg/sec{]}
+
+~~~~~ Real Tin~~~~~~~~ ! {[}C{]}
+
+~~~~~ Real Win
+
+~~~~~ Real PartLoadFrac
+
+~~~~~ REAL MaxFlowFrac~~ !Variable Volume Fan Max Flow Fraction {[}-{]}
+
+~~~~~ REAL MinFlowFrac~~ !Variable Volume Fan Min Flow Fraction {[}-{]}
+
+~~~~~ REAL FlowFrac~~~~~ !Variable Volume Fan Flow Fraction {[}-{]}
+
+~~~~~ Real FanShaftPower ! power delivered to fan shaft
+
+~~~~~ Real PowerLossToAir ! fan and motor loss to air stream (watts)
+
+! Simple Variable Volume Fan - default values from DOE-2
+
+! Type of Fan~~~~~~~~~ Coeff1~~~~~~ Coeff2~~~~~~ Coeff3~~~~~~~ Coeff4~~~~~ Coeff5
+
+! INLET VANE DAMPERS~~ 0.35071223~~ 0.30850535~~ -0.54137364~~ 0.87198823~ 0.000
+
+! DISCHARGE DAMPERS~~~ 0.37073425~~ 0.97250253~~ -0.34240761~~ 0.000~~~~~~ 0.000
+
+! VARIABLE SPEED MOTOR 0.0015302446 0.0052080574~ 1.1086242~~ -0.11635563~ 0.000
+
+~~ DeltaPress~ = Fan(FanNum)\%DeltaPress
+
+~~ FanEff~~~~~ = Fan(FanNum)\%FanEff
+
+~~ Tin~~~~~~~~ = Fan(FanNum)\%InletAirTemp
+
+~~ Win~~~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ RhoAir~~~~~ = Fan(FanNum)\%RhoAirStdInit
+
+~~ MassFlow~~~ = MIN(Fan(FanNum)\%InletAirMassFlowRate,Fan(FanNum)\%MaxAirMassFlowRate)
+
+~~ ! MassFlow~~~ = MAX(MassFlow,Fan(FanNum)\%MinAirMassFlowRate)
+
+~ ! Calculate and check limits on fraction of system flow
+
+~ MaxFlowFrac = 1.0
+
+~ ! MinFlowFrac is calculated from the ration of the volume flows and is non-dimensional
+
+~ MinFlowFrac = Fan(FanNum)\%MinAirFlowRate/Fan(FanNum)\%MaxAirFlowRate
+
+~ ! The actual flow fraction is calculated from MassFlow and the MaxVolumeFlow * AirDensity
+
+~ FlowFrac = MassFlow/(Fan(FanNum)\%MaxAirMassFlowRate)
+
+! Calculate the part Load Fraction~~~~~~~~~~~~ (PH 7/13/03)
+
+~ FlowFrac = MAX(MinFlowFrac,MIN(FlowFrac,1.0))~ ! limit flow fraction to allowed range
+
+~ PartLoadFrac = Fan(FanNum)\%FanCoeff(1) + Fan(FanNum)\%FanCoeff(2)*FlowFrac +~ \&
+
+~~~~~~~~~~~~~~~~~ Fan(FanNum)\%FanCoeff(3)*FlowFrac**2 + Fan(FanNum)\%FanCoeff(4)*FlowFrac**3 + \&
+
+~~~~~~~~~~~~~~~~~ Fan(FanNum)\%FanCoeff(5)*FlowFrac**4
+
+~~ !Determine the Fan Schedule for the Time step
+
+~ If( ( GetCurrentScheduleValue(Fan(FanNum)\%SchedPtr)\textgreater{}0.0 .and. Massflow\textgreater{}0.0 .or. TurnFansOn .and. Massflow\textgreater{}0.0) \&
+
+~~~~~~~ .and. .NOT.TurnFansOff ) Then
+
+~~ !Fan is operating - calculate power loss and enthalpy rise
+
+!~~ Fan(FanNum)\%FanPower = PartLoadFrac*FullMassFlow*DeltaPress/(FanEff*RhoAir) ! total fan power
+
+~~ Fan(FanNum)\%FanPower = PartLoadFrac*Fan(FanNum)\%MaxAirMassFlowRate*DeltaPress/(FanEff*RhoAir) ! total fan power (PH 7/13/03)
+
+~~ FanShaftPower = Fan(FanNum)\%MotEff * Fan(FanNum)\%FanPower~ ! power delivered to shaft
+
+~~ PowerLossToAir = FanShaftPower + (Fan(FanNum)\%FanPower - FanShaftPower) * Fan(FanNum)\%MotInAirFrac
+
+~~ Fan(FanNum)\%OutletAirEnthalpy = Fan(FanNum)\%InletAirEnthalpy + PowerLossToAir/MassFlow
+
+~~ ! This fan does not change the moisture or Mass Flow across the component
+
+~~ Fan(FanNum)\%OutletAirHumRat~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ Fan(FanNum)\%OutletAirMassFlowRate = MassFlow
+
+~~ Fan(FanNum)\%OutletAirTemp = PsyTdbFnHW(Fan(FanNum)\%OutletAirEnthalpy,Fan(FanNum)\%OutletAirHumRat)
+
+~ Else
+
+~~ !Fan is off and not operating no power consumed and mass flow rate.
+
+~~ Fan(FanNum)\%FanPower = 0.0
+
+~~ FanShaftPower = 0.0
+
+~~ PowerLossToAir = 0.0
+
+~~ Fan(FanNum)\%OutletAirMassFlowRate = 0.0
+
+~~ Fan(FanNum)\%OutletAirHumRat~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ Fan(FanNum)\%OutletAirEnthalpy~~~~ = Fan(FanNum)\%InletAirEnthalpy
+
+~~ Fan(FanNum)\%OutletAirTemp = Fan(FanNum)\%InletAirTemp
+
+~~ ! Set the Control Flow variables to 0.0 flow when OFF.
+
+~~ Fan(FanNum)\%MassFlowRateMaxAvail = 0.0
+
+~~ Fan(FanNum)\%MassFlowRateMinAvail = 0.0
+
+~ End If
+
+~ RETURN
+
+\textbf{END SUBROUTINE SimVariableVolumeFan}
+
+\textbf{SUBROUTINE SimOnOffFan(FanNum)}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Unknown
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ Unknown
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ Shirey, May 2001
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! This subroutine simulates the simple on/off fan.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! Converts design pressure rise and efficiency into fan power and temperature rise
+
+~~~~~~~~~ ! Constant fan pressure rise is assumed.
+
+~~~~~~~~~ ! Uses curves of fan power fraction vs.~fan part load to determine fan power at
+
+~~~~~~~~~ ! off design conditions.
+
+~~~~~~~~~ ! Same as simple (constant volume) fan, except added part-load curve input
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! ASHRAE HVAC 2 Toolkit, page 2-3 (FANSIM)
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~ USE CurveManager, ONLY: CurveValue
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~ Integer, Intent(IN) :: FanNum
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~ Real RhoAir
+
+~~~~~ Real DeltaPress~ ! {[}N/M\^{}2{]}
+
+~~~~~ Real FanEff
+
+~~~~~ Real MassFlow~~~ ! {[}kg/sec{]}
+
+~~~~~ Real Tin~~~~~~~~ ! {[}C{]}
+
+~~~~~ Real Win
+
+~~~~~ Real PartLoadRatio !Ratio of actual mass flow rate to max mass flow rate
+
+~~~~~ REAL FlowFrac~~~~~ !Actual Fan Flow Fraction = actual mass flow rate / max air mass flow rate
+
+~~~~~ Real FanShaftPower ! power delivered to fan shaft
+
+~~~~~ Real PowerLossToAir ! fan and motor loss to air stream (watts)
+
+~~ DeltaPress = Fan(FanNum)\%DeltaPress
+
+~~ FanEff~~~~ = Fan(FanNum)\%FanEff
+
+~~ Tin~~~~~~~ = Fan(FanNum)\%InletAirTemp
+
+~~ Win~~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ RhoAir~~~~ = Fan(FanNum)\%RhoAirStdInit
+
+~~ MassFlow~~ = MIN(Fan(FanNum)\%InletAirMassFlowRate,Fan(FanNum)\%MaxAirMassFlowRate)
+
+~~ MassFlow~~ = MAX(MassFlow,Fan(FanNum)\%MinAirMassFlowRate)
+
+~~ Fan(FanNum)\%FanRuntimeFraction = 0.0
+
+~ ! The actual flow fraction is calculated from MassFlow and the MaxVolumeFlow * AirDensity
+
+~ FlowFrac = MassFlow/(Fan(FanNum)\%MaxAirMassFlowRate)
+
+~ ! Calculate the part load ratio, can't be greater than 1
+
+~ PartLoadRatio = MIN(1.0,FlowFrac)
+
+~ ! Determine the Fan Schedule for the Time step
+
+~ IF( ( GetCurrentScheduleValue(Fan(FanNum)\%SchedPtr)\textgreater{}0.0 .and. Massflow\textgreater{}0.0 .or. TurnFansOn .and. Massflow\textgreater{}0.0) \&
+
+~~~ ~~~~.and. .NOT.TurnFansOff ) THEN
+
+~~ ! Fan is operating
+
+~~ IF (OnOffFanPartLoadFraction \textless{} = 0.0) THEN
+
+~~~~ CALL ShowWarningError(`FAN:SIMPLE:ONOFF, OnOffFanPartLoadFraction \textless{} = 0.0, Reset to 1.0')
+
+~~~~ OnOffFanPartLoadFraction = 1.0 ! avoid divide by zero or negative PLF
+
+~~ END IF
+
+~~ IF (OnOffFanPartLoadFraction \textless{} 0.7) THEN
+
+~~~~~~~ OnOffFanPartLoadFraction = 0.7 ! a warning message is already issued from the DX coils or gas heating coil
+
+~~ END IF
+
+~~ ! Keep fan runtime fraction between 0.0 and 1.0
+
+~~ Fan(FanNum)\%FanRuntimeFraction = MAX(0.0,MIN(1.0,PartLoadRatio/OnOffFanPartLoadFraction))
+
+~~ ! Fan(FanNum)\%FanPower = MassFlow*DeltaPress/(FanEff*RhoAir*OnOffFanPartLoadFraction)! total fan power
+
+~~ Fan(FanNum)\%FanPower = Fan(FanNum)\%MaxAirMassFlowRate*Fan(FanNum)\%FanRuntimeFraction*DeltaPress/(FanEff*RhoAir)!total fan power
+
+~~ ! OnOffFanPartLoadFraction is passed via DataHVACGlobals from the cooling or heating coil that is
+
+~~ !~~ requesting the fan to operate in cycling fan/cycling coil mode
+
+~~ OnOffFanPartLoadFraction = 1.0 ! reset to 1 in case other on/off fan is called without a part load curve
+
+~~ FanShaftPower = Fan(FanNum)\%MotEff * Fan(FanNum)\%FanPower~ ! power delivered to shaft
+
+~~ PowerLossToAir = FanShaftPower + (Fan(FanNum)\%FanPower - FanShaftPower) * Fan(FanNum)\%MotInAirFrac
+
+~~ Fan(FanNum)\%OutletAirEnthalpy = Fan(FanNum)\%InletAirEnthalpy + PowerLossToAir/MassFlow
+
+~~ ! This fan does not change the moisture or Mass Flow across the component
+
+~~ Fan(FanNum)\%OutletAirHumRat~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ Fan(FanNum)\%OutletAirMassFlowRate = MassFlow
+
+!~~ Fan(FanNum)\%OutletAirTemp = Tin + PowerLossToAir/(MassFlow*PsyCpAirFnWTdb(Win,Tin))
+
+~~ Fan(FanNum)\%OutletAirTemp = PsyTdbFnHW(Fan(FanNum)\%OutletAirEnthalpy,Fan(FanNum)\%OutletAirHumRat)
+
+~ ELSE
+
+~~ ! Fan is off and not operating no power consumed and mass flow rate.
+
+~~ Fan(FanNum)\%FanPower = 0.0
+
+~~ FanShaftPower = 0.0
+
+~~ PowerLossToAir = 0.0
+
+~~ Fan(FanNum)\%OutletAirMassFlowRate = 0.0
+
+~~ Fan(FanNum)\%OutletAirHumRat~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ Fan(FanNum)\%OutletAirEnthalpy~~~~ = Fan(FanNum)\%InletAirEnthalpy
+
+~~ Fan(FanNum)\%OutletAirTemp = Fan(FanNum)\%InletAirTemp
+
+~~ ! Set the Control Flow variables to 0.0 flow when OFF.
+
+~~ Fan(FanNum)\%MassFlowRateMaxAvail = 0.0
+
+~~ Fan(FanNum)\%MassFlowRateMinAvail = 0.0
+
+~ END IF
+
+~ RETURN
+
+\textbf{END SUBROUTINE SimOnOffFan}
+
+\textbf{SUBROUTINE SimZoneExhaustFan(FanNum)}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Fred Buhl
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ Jan 2000
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! This subroutine simulates the Zone Exhaust Fan
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! Converts design pressure rise and efficiency into fan power and temperature rise
+
+~~~~~~~~~ ! Constant fan pressure rise is assumed.
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! ASHRAE HVAC 2 Toolkit, page 2-3 (FANSIM)
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~ Integer, Intent(IN) :: FanNum
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~ Real RhoAir
+
+~~~~~ Real DeltaPress~ ! {[}N/M\^{}2{]}
+
+~~~~~ Real FanEff
+
+~~~~~ Real MassFlow~~~ ! {[}kg/sec{]}
+
+~~~~~ Real Tin~~~~~~~~ ! {[}C{]}
+
+~~~~~ Real Win
+
+~~~ ~~Real PowerLossToAir ! fan and motor loss to air stream (watts)
+
+~~ DeltaPress = Fan(FanNum)\%DeltaPress
+
+~~ FanEff~~~~ = Fan(FanNum)\%FanEff
+
+~~ ! For a Constant Volume Simple Fan the Max Flow Rate is the Flow Rate for the fan
+
+~~ Tin~~~~~~~ = Fan(FanNum)\%InletAirTemp
+
+~~ Win~~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ RhoAir~~~~ = Fan(FanNum)\%RhoAirStdInit
+
+~~ MassFlow~~ = Fan(FanNum)\%InletAirMassFlowRate
+
+~~ !
+
+~~ !Determine the Fan Schedule for the Time step
+
+~ If( ( GetCurrentScheduleValue(Fan(FanNum)\%SchedPtr)\textgreater{}0.0 .or. TurnFansOn ) \&
+
+~~~~~~~ .and. .NOT.TurnFansOff ) Then
+
+~~ !Fan is operating
+
+~~ Fan(FanNum)\%FanPower = MassFlow*DeltaPress/(FanEff*RhoAir) ! total fan power
+
+~~ PowerLossToAir = Fan(FanNum)\%FanPower
+
+~~ Fan(FanNum)\%OutletAirEnthalpy = Fan(FanNum)\%InletAirEnthalpy + PowerLossToAir/MassFlow
+
+~~ ! This fan does not change the moisture or Mass Flow across the component
+
+~~ Fan(FanNum)\%OutletAirHumRat~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ Fan(FanNum)\%OutletAirMassFlowRate = MassFlow
+
+~~ Fan(FanNum)\%OutletAirTemp = PsyTdbFnHW(Fan(FanNum)\%OutletAirEnthalpy,Fan(FanNum)\%OutletAirHumRat)
+
+~Else
+
+~~ !Fan is off and not operating no power consumed and mass flow rate.
+
+~~ Fan(FanNum)\%FanPower = 0.0
+
+~~ PowerLossToAir = 0.0
+
+~~ Fan(FanNum)\%OutletAirMassFlowRate = 0.0
+
+~~ Fan(FanNum)\%OutletAirHumRat~~~~~~ = Fan(FanNum)\%InletAirHumRat
+
+~~ Fan(FanNum)\%OutletAirEnthalpy~~~~ = Fan(FanNum)\%InletAirEnthalpy
+
+~~ Fan(FanNum)\%OutletAirTemp = Fan(FanNum)\%InletAirTemp
+
+~~ ! Set the Control Flow variables to 0.0 flow when OFF.
+
+~~ Fan(FanNum)\%MassFlowRateMaxAvail = 0.0
+
+~~ Fan(FanNum)\%MassFlowRateMinAvail = 0.0
+
+~~ Fan(FanNum)\%InletAirMassFlowRate = 0.0
+
+~End If
+
+~RETURN
+
+\textbf{END SUBROUTINE SimZoneExhaustFan}
+
+! End Algorithm Section of the Module
+
+! *****************************************************************************
+
+! Beginning of Update subroutines for the Fan Module
+
+! *****************************************************************************
+
+\textbf{SUBROUTINE UpdateFan(FanNum)}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Richard Liesen
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ April 1998
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! This subroutine updates the fan outlet nodes.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! Data is moved from the fan data structure to the fan outlet nodes.
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~~~~~~~~~ ! na
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~ Integer, Intent(IN) :: FanNum
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~ Integer~~~~~~~~~~~~ :: OutletNode
+
+~ Integer~~~~~~~~~~~~ :: InletNode
+
+~~ OutletNode = Fan(FanNum)\%OutletNodeNum
+
+~~ InletNode = Fan(FanNum)\%InletNodeNum
+
+~~ ! Set the outlet air nodes of the fan
+
+~~ Node(OutletNode)\%MassFlowRate~ = Fan(FanNum)\%OutletAirMassFlowRate
+
+~~ Node(OutletNode)\%Temp~~~~~~~~~ = Fan(FanNum)\%OutletAirTemp
+
+~~ Node(OutletNode)\%HumRat~~~~~~~ = Fan(FanNum)\%OutletAirHumRat
+
+~~ Node(OutletNode)\%Enthalpy~~~~~ = Fan(FanNum)\%OutletAirEnthalpy
+
+~~ ! Set the outlet nodes for properties that just pass through \& not used
+
+~~ Node(OutletNode)\%Quality~~~~~~~~ = Node(InletNode)\%Quality
+
+~~ Node(OutletNode)\%Press~~~~~~~~~~ = Node(InletNode)\%Press
+
+~~ ! Set the Node Flow Control Variables from the Fan Control Variables
+
+~~ Node(OutletNode)\%MassFlowRateMaxAvail = Fan(FanNum)\%MassFlowRateMaxAvail
+
+~~ Node(OutletNode)\%MassFlowRateMinAvail = Fan(FanNum)\%MassFlowRateMinAvail
+
+~~ IF (Fan(FanNum)\%FanType .EQ. `ZONE EXHAUST FAN') THEN
+
+~~~~ Node(InletNode)\%MassFlowRate = Fan(FanNum)\%InletAirMassFlowRate
+
+~~ END IF
+
+~ RETURN
+
+\textbf{END Subroutine UpdateFan}
+
+!~~~~~~~ End of Update subroutines for the Fan Module
+
+! *****************************************************************************
+
+! Beginning of Reporting subroutines for the Fan Module
+
+! *****************************************************************************
+
+\textbf{SUBROUTINE ReportFan(FanNum)}
+
+~~~~~~~~~ ! SUBROUTINE INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Richard Liesen
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ April 1998
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS SUBROUTINE:
+
+~~~~~~~~~ ! This subroutine updates the report variables for the fans.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~ Use DataHVACGlobals, ONLY: TimeStepSys, FanElecPower
+
+~ IMPLICIT NONE~~~ ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! SUBROUTINE ARGUMENT DEFINITIONS:
+
+~~ Integer, Intent(IN) :: FanNum
+
+~~~~~~~~~ ! SUBROUTINE PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+
+~~~~~~~~~ ! na
+
+~~~ Fan(FanNum)\%FanEnergy = Fan(FanNum)\%FanPower*TimeStepSys*3600
+
+~~~ Fan(FanNum)\%DeltaTemp = Fan(FanNum)\%OutletAirTemp - Fan(FanNum)\%InletAirTemp
+
+~~~ FanElecPower = Fan(FanNum)\%FanPower
+
+~ RETURN
+
+\textbf{END Subroutine ReportFan}
+
+!~~~~~~~ End of Reporting subroutines for the Fan Module
+
+! *****************************************************************************
+
+! Beginning of Utility subroutines for the Fan Module
+
+! *****************************************************************************
+
+\textbf{FUNCTION GetFanDesignVolumeFlowRate(FanType,FanName,ErrorsFound) RESULT(DesignVolumeFlowRate)}
+
+~~~~~~~~~ ! FUNCTION INFORMATION:
+
+~~~~ ~~~~~!~~~~~~ AUTHOR~~~~~~~~ Linda Lawrie
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ February 2006
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS FUNCTION:
+
+~~~~~~~~~ ! This function looks up the design volume flow rate for the given fan and returns it.~ If
+
+~~~~~~~~~ ! incorrect fan type or name is given, errorsfound is returned as true and value is returned
+
+~~~~~~~~~ ! as negative.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~ ~! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~ USE InputProcessor,~ ONLY: FindItemInList
+
+~ IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! FUNCTION ARGUMENT DEFINITIONS:
+
+~ CHARACTER(len = *), INTENT(IN) :: FanType~~~~~ ! must match fan types in this module
+
+~ CHARACTER(len = *), INTENT(IN) :: FanName~~~~~ ! must match fan names for the fan type
+
+~ LOGICAL, INTENT(INOUT)~~~~~~ :: ErrorsFound~ ! set to true if problem
+
+~ REAL~~~~~~~~~~~~~~~~~~~~~~~~ :: DesignVolumeFlowRate ! returned flow rate of matched fan
+
+~~~~~~~~~ ! FUNCTION PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS:
+
+~~~~~ ~~~~! na
+
+~~~~~~~~~ ! FUNCTION LOCAL VARIABLE DECLARATIONS:
+
+~ INTEGER :: WhichFan
+
+~ ! Obtains and Allocates fan related parameters from input file
+
+~ IF (GetFanInputFlag) THEN~ !First time subroutine has been entered
+
+~~~ CALL GetFanInput
+
+~~~ GetFanInputFlag = .false.
+
+~ End If
+
+~ WhichFan = FindItemInList(FanName,Fan\%FanName,NumFans)
+
+~ IF (WhichFan / = 0) THEN
+
+~~~ DesignVolumeFlowRate = Fan(WhichFan)\%MaxAirFlowRate
+
+~ ENDIF
+
+~ IF (WhichFan = = 0) THEN
+
+~~~ CALL ShowSevereError(`Could not find FanType = ``'//TRIM(FanType)//''' with Name = ``'//TRIM(FanName)//'''\,')
+
+~~~ ErrorsFound = .true.
+
+~~~ DesignVolumeFlowRate = -1000.
+
+~ ENDIF
+
+~ RETURN
+
+\textbf{END FUNCTION GetFanDesignVolumeFlowRate}
+
+\textbf{FUNCTION GetFanInletNode(FanType,FanName,ErrorsFound) RESULT(NodeNumber)}
+
+~~~~~~~~~ ! FUNCTION INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Linda Lawrie
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ February 2006
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS FUNCTION:
+
+~~~~~~~~~ ! This function looks up the given fan and returns the inlet node.~ If
+
+~~~~~~~~~ ! incorrect fan type or name is given, errorsfound is returned as true and value is returned
+
+~~~~~~~~~ ! as zero.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~ USE InputProcessor,~ ONLY: FindItemInList
+
+~ IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! FUNCTION ARGUMENT DEFINITIONS:
+
+~ CHARACTER(len = *), INTENT(IN) :: FanType~~~~~ ! must match fan types in this module
+
+~ CHARACTER(len = *), INTENT(IN) :: FanName~~~~~ ! must match fan names for the fan type
+
+~ LOGICAL, INTENT(INOUT)~~~~~~ :: ErrorsFound~ ! set to true if problem
+
+~ INTEGER~~ ~~~~~~~~~~~~~~~~~~~:: NodeNumber~~ ! returned outlet node of matched fan
+
+~~~~~~~~~ ! FUNCTION PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~ ~~! FUNCTION LOCAL VARIABLE DECLARATIONS:
+
+~ INTEGER :: WhichFan
+
+~ ! Obtains and Allocates fan related parameters from input file
+
+~ IF (GetFanInputFlag) THEN~ !First time subroutine has been entered
+
+~~~ CALL GetFanInput
+
+~~~ GetFanInputFlag = .false.
+
+~ End If
+
+~ WhichFan = FindItemInList(FanName,Fan\%FanName,NumFans)
+
+~ IF (WhichFan / = 0) THEN
+
+~~~ NodeNumber = Fan(WhichFan)\%InletNodeNum
+
+~ ENDIF
+
+~ IF (WhichFan = = 0) THEN
+
+~~~ CALL ShowSevereError(`Could not find FanType = ``'//TRIM(FanType)//''' with Name = ``'//TRIM(FanName)//'''\,')
+
+~~~ ErrorsFound = .true.
+
+~~~ NodeNumber = 0
+
+~ ENDIF
+
+~ RETURN
+
+\textbf{END FUNCTION GetFanInletNode}
+
+\textbf{FUNCTION GetFanOutletNode(FanType,FanName,ErrorsFound) RESULT(NodeNumber)}
+
+~~~~~~~~~ ! FUNCTION INFORMATION:
+
+~~~~~~~~~ !~~~~~~ AUTHOR~~~~~~~~ Linda Lawrie
+
+~~~~~~~~~ !~~~~~~ DATE WRITTEN~~ February 2006
+
+~~~~~~~~~ !~~~~~~ MODIFIED~~~~~~ na
+
+~~~~~~~~~ !~~~~~~ RE-ENGINEERED~ na
+
+~~~~~~~~~ ! PURPOSE OF THIS FUNCTION:
+
+~~~~ ~~~~~! This function looks up the given fan and returns the outlet node.~ If
+
+~~~~~~~~~ ! incorrect fan type or name is given, errorsfound is returned as true and value is returned
+
+~~~~~~~~~ ! as zero.
+
+~~~~~~~~~ ! METHODOLOGY EMPLOYED:
+
+~~~~~~~~~ ! na
+
+~~~ ~~~~~~! REFERENCES:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! USE STATEMENTS:
+
+~ USE InputProcessor,~ ONLY: FindItemInList
+
+~ IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
+
+~~~~~~~~~ ! FUNCTION ARGUMENT DEFINITIONS:
+
+~ CHARACTER(len = *), INTENT(IN) :: FanType~~~~~ ! must match fan types in this module
+
+~ CHARACTER(len = *), INTENT(IN) :: FanName~~~~~ ! must match fan names for the fan type
+
+~ LOGICAL, INTENT(INOUT)~~~~~~ :: ErrorsFound~ ! set to true if problem
+
+~ INTEGER~~ ~~~~~~~~~~~~~~~~~~~:: NodeNumber~~ ! returned outlet node of matched fan
+
+~~~~~~~~~ ! FUNCTION PARAMETER DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! INTERFACE BLOCK SPECIFICATIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~~~ ! DERIVED TYPE DEFINITIONS:
+
+~~~~~~~~~ ! na
+
+~~~~~~~ ~~! FUNCTION LOCAL VARIABLE DECLARATIONS:
+
+~ INTEGER :: WhichFan
+
+~ ! Obtains and Allocates fan related parameters from input file
+
+~ IF (GetFanInputFlag) THEN~ !First time subroutine has been entered
+
+~~~ CALL GetFanInput
+
+~~~ GetFanInputFlag = .false.
+
+~ End If
+
+~ WhichFan = FindItemInList(FanName,Fan\%FanName,NumFans)
+
+~ IF (WhichFan / = 0) THEN
+
+~~~ NodeNumber = Fan(WhichFan)\%OutletNodeNum
+
+~ ENDIF
+
+~ IF (WhichFan = = 0) THEN
+
+~~~ CALL ShowSevereError(`Could not find FanType = ``'//TRIM(FanType)//''' with Name = ``'//TRIM(FanName)//'''\,')
+
+~~~ ErrorsFound = .true.
+
+~~~ NodeNumber = 0
+
+~ ENDIF
+
+~ RETURN
+
+\textbf{END FUNCTION GetFanOutletNode}
+
+! End of Utility subroutines for the Fan Module
+
+! *****************************************************************************
+
+!~~~~ NOTICE
+
+!
+
+!~~~~ Copyright © 1996-xxxx The Board of Trustees of the University of Illinois
+
+!~~~~ and The Regents of the University of California through Ernest Orlando Lawrence
+
+!~~~~ Berkeley National Laboratory.~ All rights reserved.
+
+!
+
+!~~~~ Portions of the EnergyPlus software package have been developed and copyrighted
+
+!~~~~ by other individuals, companies and institutions.~ These portions have been
+
+!~~~~ incorporated into the EnergyPlus software package under license.~~ For a complete
+
+!~~~~ list of contributors, see ``Notice'' located in EnergyPlus.f90.
+
+!
+
+!~~~~ NOTICE: The U.S. Government is granted for itself and others acting on its
+
+!~~~~ behalf a paid-up, nonexclusive, irrevocable, worldwide license in this data to
+
+!~~~~ reproduce, prepare derivative works, and perform publicly and display publicly.
+
+!~~~~ Beginning five (5) years after permission to assert copyright is granted,
+
+!~~~~ subject to two possible five year renewals, the U.S. Government is granted for
+
+!~~~~ itself and others acting on its behalf a paid-up, non-exclusive, irrevocable
+
+!~~~~ worldwide license in this data to reproduce, prepare derivative works,
+
+!~~~~ distribute copies to the public, perform publicly and display publicly, and to
+
+!~~~~ permit others to do so.
+
+!
+
+!~~~~ TRADEMARKS: EnergyPlus is a trademark of the US Department of Energy.
+
+!
+
+\textbf{End Module Fans}
diff --git a/doc/module-developer/src/module-structure/module-outline.tex b/doc/module-developer/src/module-structure/module-outline.tex
new file mode 100644
index 00000000000..17629bac7a5
--- /dev/null
+++ b/doc/module-developer/src/module-structure/module-outline.tex
@@ -0,0 +1,71 @@
+\section{Module Outline}\label{module-outline}
+
+The developer will create a new file NewHVACComponent.f90.~ The file shall contain the following elements:
+
+Note -- even if your component does not need some of the suggested modules, you should include ``stub'' routines for these.
+
+\textbf{MODULE}NewHVACComponent
+
+\emph{Documentation:} Fortran comments describing and documenting the module. Included are sections showing module author, module creation date, date modified and modification author.~ Each routine and/or function should also follow the documentation guidelines as shown in the templates.
+
+\emph{USE Statements:} Fortran statements naming other modules that this module can access, either for data or for routines.
+
+\emph{Module Parameters:} If you will be implementing more than one ``type'' of component in the module, it is a good idea to assign numeric parameters to each type so as to retain readability yet reduce alpha comparisons which are notoriously slow for most systems.~ Assign numeric parameters to alphanumeric fields within a class type (.e.g.~object UnitarySystem:HeatPump, field Fan Placement: ``blow through'' or ``draw through'') when this information is required in init, calc, update or report subroutines to further reduce alpha comparisons.~ Use string comparison only in GetInput subroutines.
+
+\emph{Module Data structure Definitions:} Using the Fortran TYPE statement define the data structures needed in the module that will not be available from other modules. Define all module level variables that will be needed.
+
+Typically, you define your module's data structure within the module.~ If this data must be used by multiple modules, you should define a separate Data module for the data.
+
+Character strings in structures are not allowed (except for name of object) -- any exceptions must be approved. Schedule names, curve object names, and child object types MUST all be referenced by an integer.
+
+For existing code, convert all character string structure variables to integer parameters and delete the character variable from the structure. Also delete unused strings rather than converting to integer. Do not use structure variable to store information used only during GetInput even if you think it could be used in the future, use local variables instead. Usually won't hurt anything until some user puts a large number of objects in their input (memory use impact).
+
+Currently, the furnace structure includes many that should not be there. SuppHeatCoilType is an example of a character string structure variable that is only used in GetInput and is not needed in the structure. Should have been a local instead. And CoolingPLFFPLR and HeatingPLFFPLR structure variables are not even used.
+
+\textbf{\emph{CONTAINS}}
+
+\textbf{\emph{SUBROUTINE}} \emph{SimNewHVACComponent}
+
+This routine selects the individual component being simulated and calls the other module subroutines that do the real work. This routine is the only routine in the module that is accessible outside the module (\emph{PUBLIC}). All other routines in the module are \emph{PRIVATE} and are only callable within the module. This routine is sometimes called the ``driver'' routine for the module.
+
+\textbf{\emph{END SUBROUTINE}} \emph{SimNewHVACComponent}
+
+\textbf{\emph{SUBROUTINE}} \emph{GetNewHVACComponentInput}
+
+This routine uses the ``get'' routines from the InputProcessor module to obtain input for NewHVACComponent. The module data arrays are allocated and the data is moved into the arrays.
+
+\textbf{\emph{END SUBROUTINE}} \emph{GetNewHVACComponentInput}
+
+\textbf{\emph{SUBROUTINE}} \emph{InitNewHVACComponent}
+
+This routine performs whatever initialization calculations that may be needed at various points in the simulation. For instance, some calculations may only need to be done once; some may need to be done at the start of each simulation weather period; some at the start of each HVAC simulation time step; and some at the start of each loop solution. This routine also transfers data from the component inlet nodes to the component data arrays every time the component is simulated, in preparation for the actual component simulation.
+
+\textbf{\emph{END SUBROUTINE}} \emph{InitNewHVACComponent}
+
+\textbf{\emph{SUBROUTINE}} \emph{SizeNewHVACComponent}
+
+This routine can create the sizing options (if applicable) for the component or be left as a placeholder for later manipulation for sizing purposes.
+
+\textbf{\emph{END SUBROUTINE}} \emph{SizeNewHVACComponent}
+
+\textbf{\emph{SUBROUTINE}} \emph{CalcNewHVACComponent}
+
+This routine does the actual calculations to simulate the performance of the component. Only calculation is done -- there is no moving of data from or to input or output areas. There may be more than one ``\emph{CALC}'' subroutine if more than one component is being modeled within this module.
+
+\textbf{\emph{END SUBROUTINE}} \emph{CalcNewHVACComponent}
+
+\textbf{\emph{SUBROUTINE}} \emph{UpdateNewHVACComponent}
+
+This routine moves the results of the ``\emph{Calc}'' routine(s) to the component outlet nodes.
+
+\textbf{\emph{END SUBROUTINE}} \emph{UpdateNewHVACComponent}
+
+\textbf{\emph{SUBROUTINE}} \emph{ReportNewHVACComponent}
+
+This routine performs any special calculations that are needed purely for reporting purposes.
+
+\textbf{\emph{END SUBROUTINE}} \emph{ReportNewHVACComponent}
+
+\textbf{\emph{Utility Routines (as appropriate) -- in the Fan module we allow outside modules to access internal fan inlets, outlets, and design volume flow rate.}}
+
+\textbf{\emph{END MODULE}} \emph{NewHVACComponent}
diff --git a/doc/module-developer/src/modules-in-energyplus.tex b/doc/module-developer/src/modules-in-energyplus.tex
new file mode 100644
index 00000000000..2ff9af57b2c
--- /dev/null
+++ b/doc/module-developer/src/modules-in-energyplus.tex
@@ -0,0 +1 @@
+\chapter{Modules in EnergyPlus}\label{modules-in-energyplus}
diff --git a/doc/module-developer/src/modules-in-energyplus/adding-new-features.tex b/doc/module-developer/src/modules-in-energyplus/adding-new-features.tex
new file mode 100644
index 00000000000..ff16e19cd82
--- /dev/null
+++ b/doc/module-developer/src/modules-in-energyplus/adding-new-features.tex
@@ -0,0 +1,39 @@
+\section{Adding new features}\label{adding-new-features}
+
+The process for adding new features or significantly changing some features goes through a development team discussion period where the new feature is outlined, discussed and (hopefully) approved for inclusion.
+
+The team has a New Feature Proposal template document that is available to anyone wishing to add a new feature to EnergyPlus (or to auxiliary programs around EnergyPlus). The full New Feature Proposal format is shown in Appendix F.
+
+The sections of the New Feature Proposal are summarized in the following table:
+
+% table 1
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Sections of a New Feature Proposal \label{table:sections-of-a-new-feature-proposal}} \tabularnewline
+\toprule 
+Section & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Sections of a New Feature Proposal} \tabularnewline
+\toprule 
+Section & Description \tabularnewline
+\midrule
+\endhead
+
+Justification & Why is the feature important.~ Impact on energy use. What energy aspects the feature is using. \tabularnewline
+Conference Call Conclusions & Conclusions from the discussions (email or conference call) \tabularnewline
+Other Conference Call topics & Items outside the scope of the feature might be brought up but not able to be accomplished. \tabularnewline
+Overview & Description of the feature and references \tabularnewline
+Approach & What approach will be used. \tabularnewline
+Testing/Validation data Sources & Required \tabularnewline
+IORef/Draft & IDD Objects (new or revised) as well as full IOReference text \tabularnewline
+Proposed Report Variables & What outputs will come out of this feature. \tabularnewline
+Proposed additions to meters & How the outputs will affect the meter output \tabularnewline
+Engineering Reference Draft & Draft text for the Engineering Reference document \tabularnewline
+Example File & What/how many example files will be included or used to support this feature \tabularnewline
+Transition changes & What will be the required changes for current input files for this feature \tabularnewline
+Other documents & Other references. \tabularnewline
+\bottomrule
+\end{longtable}
+
+Then, of course, the document in Appendix G must be filled out and given to the proper people as well -- to show that rights to the intellectual property of the new feature are owned by the developer.
diff --git a/doc/module-developer/src/modules-in-energyplus/what-is-a-module-anyway.tex b/doc/module-developer/src/modules-in-energyplus/what-is-a-module-anyway.tex
new file mode 100644
index 00000000000..21c74bdcb63
--- /dev/null
+++ b/doc/module-developer/src/modules-in-energyplus/what-is-a-module-anyway.tex
@@ -0,0 +1,15 @@
+\section{What is a module anyway?}\label{what-is-a-module-anyway}
+
+\subsection{Program Modules}\label{program-modules}
+
+A module is a Fortran 90/95 programming construct that can be used in various ways. In EnergyPlus, its primary use is to segment a rather large program into smaller, more manageable pieces. Each module is a separate package of source code stored on a separate file. The entire collection of modules, when compiled and linked, forms the executable code of EnergyPlus.
+
+Each module contains source code for closely related data structures and procedures. For instance, the WeatherManager module contains all the weather handling routines in EnergyPlus. The module is contained in the file WeatherManager.f90.~ Another example is PlantPumps. This module contains all the code to simulate pumps in EnergyPlus. It is contained in file PlantPumps.f90.
+
+Of course dividing a program into modules can be done in various ways. We have attempted to create modules that are as self-contained as possible. The philosophy that has been used in creating EnergyPlus is contained in the \href{file:///E:/Docs4PDFs/ProgrammingStandards.pdf}{Programming Standard} reference document.~ Logically, the modules in EnergyPlus form an inverted tree structure. At the top is EnergyPlus. Just below that are ProcessInput and ManageSimulation. At the bottom are the modules such as HVACDamperComponent that model the actual HVAC components.
+
+\subsection{Data Only Modules}\label{data-only-modules}
+
+EnergyPlus also uses modules that primary contain data and data structures that may be used by several modules. These modules form one of the primary ways data is structured and shared in EnergyPlus. An example is the DataEnvironment module. Many parts of the program need access to the outdoor conditions. All of that data is encapsulated in DataEnvironment. Modules that need this data obtain access through a Fortran USE statement. Without such access, modules cannot use or change this data.
+
+Sometimes data modules are extended to perform certain utilities or even getting input for the data structures that are the primary focus of the module but this is not a standard approach.
diff --git a/doc/module-developer/src/modules-in-energyplus/what-is-a-module-developer.tex b/doc/module-developer/src/modules-in-energyplus/what-is-a-module-developer.tex
new file mode 100644
index 00000000000..1a9a45b2b72
--- /dev/null
+++ b/doc/module-developer/src/modules-in-energyplus/what-is-a-module-developer.tex
@@ -0,0 +1,5 @@
+\section{What is a module developer?}\label{what-is-a-module-developer}
+
+A module developer is someone who is going to add to the simulation capabilities of EnergyPlus. Someone, for instance, who is interested in adding code to model a new type of HVAC equipment. The most straightforward way of doing this is to create a new program module -- hence the term ``module developer''.~~ Another kind of module developer would be the adaptation of an existing ``legacy'' code to EnergyPlus.
+
+In EnergyPlus, one of the first steps in creating a new component model is to define the input. So, before we discuss modules in more detail, we must first describe the EnergyPlus input.
diff --git a/doc/module-developer/src/output.tex b/doc/module-developer/src/output.tex
new file mode 100644
index 00000000000..36f79d7186c
--- /dev/null
+++ b/doc/module-developer/src/output.tex
@@ -0,0 +1,9 @@
+\chapter{Output}\label{output}
+
+There are several output files available in EnergyPlus.~ As you can see in Appendix A, DataGlobals contains OutputFileStandard, OutputFileInits, and OutputFileDebug.
+
+OutputFileDebug is initialized very early in the EnergyPlus execution and is available for any debugging output the developer might need.
+
+OutputFileInits is intended for ``one-time'' outputs.~ If the value is calculated or entered and should be echoed to output, this file is the place for it.~ The structure is similar to the IDD/IDF structure in that there is a ``definition'' line followed by the data being reported. Since the data may be produced in several places during the simulation, the actual file looks a bit hodge-podge but can be easily imported into a spreadsheet program and grouped.
+
+OutputFileStandard is the reporting variable output file from EnergyPlus.~ You can read more details from the \href{file:///E:/Docs4PDFs/InterfaceDeveloper.pdf}{\emph{Guide for Interface Developers}} document and in the \href{file:///E:/Docs4PDFs/InputOutputReference.pdf}{Input Output Reference} document.~ OutputFileMeters is a similar file to contain meter (only) output.~ Meter values also may appear in the OutputFileStandard file. Only values that change during the simulation should be output to these files.~ They are automaticallly included by the SetupOutputVariable calls.
diff --git a/doc/module-developer/src/output/how-do-i-output-my-variables.tex b/doc/module-developer/src/output/how-do-i-output-my-variables.tex
new file mode 100644
index 00000000000..12d7dd9e7ef
--- /dev/null
+++ b/doc/module-developer/src/output/how-do-i-output-my-variables.tex
@@ -0,0 +1,68 @@
+\section{How Do I Output My Variables?}\label{how-do-i-output-my-variables}
+
+Module developers are responsible for ``setting'' up the variables that will appear in the OutputFileStandard.
+
+To do this is very simple.~ All you need to do is place a simple call to \emph{SetupOutputVariable} into your module for each variable to be available for reporting.~ This call should be done only once for each Variable/KeyedValue pair (see below).~ For HVAC and Plant components, this call is usually at the end of the ``GetInput'' subroutine. See the example module for an illustration of this. Other calls in the simulation routines will invoke the EnergyPlus \emph{OutputProcessor} automatically at the proper time to have the data appear in the OutputFileStandard.
+
+For you the call is:
+
+Call SetupOutputVariable(VariableName,ActualVariable,~ \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ IndexTypeKey, VariableTypeKey,KeyedValue,ReportFreq \&
+
+~~~~~~~~~~~~~~~~~~~~~~~~ ResourceTypeKey,EndUseKey,GroupKey)
+
+Interface statements allow for the same call to be used for either real or integer ``ActualVariable'' variables.~ A few examples from EnergyPlus and then we will define the arguments:
+
+CALL SetupOutputVariable(`Site Outdoor Drybulb Temperature {[}C{]}', \&
+
+~~~~~~~ OutDryBulbTemp,`Zone',`Average',`Environment')
+
+CALL SetupOutputVariable(`Zone Mean Air Temperature {[}C{]}', \&
+
+~~~~~~~ ZnRpt(Loop)\%MeanAirTemp,`Zone', `State',Zone(Loop)\%Name)
+
+CALL SetupOutputVariable(`Fan Coil Heating Energy {[}J{]}', \&
+
+~~~~~~~ FanCoil(FanCoilNum)\%HeatEnergy,`System',~~ \&
+
+~~~~~ ~`Sum',FanCoil(FanCoilNum)\%Name)
+
+CALL SetupOutputVariable(`Humidifier Electric Energy {[}J{]}',
+
+~~~~~~~ Humidifier(HumNum)\%ElecUseEnergy,`System',`Sum', \&
+
+~~~~~~~ Humidifier(HumNum)\%Name, ResourceTypeKey = `ELECTRICITY',\&
+
+~~~~~~~ EndUseKey = `HUMIDIFIER', GroupKey = `System')
+
+% table 4
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{SetupOutputVariable Arguments \label{table:setupoutputvariable-arguments}} \tabularnewline
+\toprule 
+SetupOutput Variable Arguments & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{SetupOutputVariable Arguments} \tabularnewline
+\toprule 
+SetupOutput Variable Arguments & Description \tabularnewline
+\midrule
+\endhead
+
+VariableName & String name of variable, units should be included in [].~ If no units, use [] \tabularnewline
+ActualVariable & This should be the actual variable that will store the value.~ The OutputProcessor sets up a pointer to this variable, so it will need to be a SAVEd variable if in a local routine.~ As noted in examples, can be a simple variable or part of an array/derived type. \tabularnewline
+IndexTypeKey & When this variable has its proper value.~ ‘Zone’ is used for variables that will have value on the global timestep (alias “HeatBalance�).~ ‘HVAC’ is used for variables that will have values calculated on the variable system timesteps (alias “System�, “Plant�) \tabularnewline
+VariableTypeKey & Two kinds of variables are produced.~ ‘State’ or ‘Average’ are values that are instantaneous at the timestep (zone air temperature, outdoor weather conditions).~ ‘NonState’ or ‘Sum’ are values which need to be summed for a period (energy). \tabularnewline
+KeyedValue & Every variable to be reported needs to have an associated keyed value. ~Zone Air Temperature is available for each Zone, thus the keyed value is the Zone Name. \tabularnewline
+ReportFreq & This optional argument should only be used during debugging of your module but it is provided for the developers so that these variables would always show up in the OutputFile.~ (All other variables must be requested by the user). \tabularnewline
+ResourceTypeKey & Meter Resource Type; an optional argument used for including the variable in a meter. The meter resource type can be 'Electricity', ‘Gas’, ‘Coal’, ‘FuelOil\#1’, ‘FuelOil\#2’, ‘Propane’, ‘Water’, or ‘EnergyTransfer’. \tabularnewline
+EndUseKey & Meter End Use Key; an optional argument used when the variable is included in a meter. The end use keys can be: 'InteriorLights’, 'ExteriorLights', 'Heating', ‘Cooling’, 'DHW', 'Cogeneration', 'ExteriorEquipment', 'ZoneSource', 'PurchasedHotWater', 'PurchasedChilledWater', 'Fans', 'HeatingCoils', 'CoolingCoils', 'Pumps', 'Chillers', 'Boilers', 'Baseboard', 'HeatRejection', 'Humidifier', 'HeatRecovery' or ‘Refrigeration’. \tabularnewline
+EndUseSubKey & Meter End Use Subcategory Key; an optional argument to further divide a particular End Use.~ This key is user-defined in the input object and can be any string, e.g., 'Task Lights', 'Exit Lights', 'Landscape Lights', 'Computers', or 'Fax Machines'. \tabularnewline
+GroupKey & Meter Super Group Key; an optional argument used when the variable is included in a meter. The group key denotes whether the variable belongs to the building, system, or plant.The choices are: 'Building', 'HVAC' or 'Plant'. \tabularnewline
+\bottomrule
+\end{longtable}
+
+As described in the \emph{Input Output Reference}, not all variables may be available in any particular simulation.~ Only those variables that will have values generated will be available for reporting.~ In the IDF, you can include a ``Output:VariableDictionary,regular;'' command that will produce the eplusout.rdd file containing all the variables with their IndexTypeKeys.~ This list can be used to tailor the requests for values in the OutputFileStandard.
+
+This variable dictionary is separated into two pieces: regular reporting variables and meter variables.~ It can also be sorted by name (ascending).
diff --git a/doc/module-developer/src/output/output-variable-dos-and-don-ts.tex b/doc/module-developer/src/output/output-variable-dos-and-don-ts.tex
new file mode 100644
index 00000000000..987632a4151
--- /dev/null
+++ b/doc/module-developer/src/output/output-variable-dos-and-don-ts.tex
@@ -0,0 +1,298 @@
+\section{Output Variable Dos and Don'ts}\label{output-variable-dos-and-donts}
+
+For general output variables there aren't many rules. For meter output variables there are quite a few. Here are some tips to keep you out of trouble.
+
+\subsection{What Variables Should I Output?}\label{what-variables-should-i-output}
+
+The choice of variables to output is really up to the developer. Since variables don't appear on the output file unless requested by the user in the IDF input file, it is better to ``SetUp'' too many rather than too few. For an HVAC component one should generally output the heating and cooling outputs of the component both in terms of energy and power. Energy is always output in Joules, power in Watts. If there is humidification or dehumidification both total and sensible cooling should be reported. Any electricity or fuel consumed by a component should be reported out, again both in terms of energy (Joules) and power (Watts). For HVAC components in most cases reporting inlet and outlet temperatures and humidities is unnecessary since these quantities can be obtained from the system node outputs.
+
+\subsection{Output Variable Naming Conventions}\label{output-variable-naming-conventions}
+
+The names for output variables need to be selected carefully to maintain a high level of consistency and clarity. Well-chosen names help users quickly understand the meaning of a specific output.
+
+The following general guidelines are to be followed when choosing names for new output variables:
+
+\begin{itemize}
+\item
+  Output variable names shall be written in title case where every major word is capitalized (exceptions: ``a'', ``the'', ``for'', etc.) with spaces separating words.
+\item
+  Output variable names shall be written using natural language terminology but should be relatively concise. The language is American English.
+\item
+  Although they should be avoided where practical, acronyms (and symbols) are acceptable where their use is commonplace and contributes to conciseness in identifying a complex engineering concept. Examples of acceptable acronyms for output variable names are listed in the table below.
+\item
+  Abbreviations should not be used and the words spelled out completely (except for Units).
+\item
+  Where practical, reuse existing names for output variables across different models for similar components.~ For example, a new model for a zone baseboard heater should reuse the existing names for output variables already in use for other baseboard models rather than use new names that distinguish the kind of baseboard model that the output is associated with.~ The user-defined name of the component should allow the user to know the association without the basic name of the output variable reflecting that association.~ This has the advantage of reducing the total number of output variable names and making it simpler for users.
+\item
+  Engineering terminology should generally be consistent with that used in ASHRAE handbooks and literature (American Society of Heating, Refrigeration and~ Air-Conditioning Engineers, Inc., Atlanta, CA, USA)
+\item
+  Output variable names shall have no punctuation or special characters. The names are expected to contain many adjectives adjacent to each other and no hyphens or commas are needed to clarify.
+\item
+  Output variable names shall always be less than 100 characters long.
+\end{itemize}
+
+An output variable name should be constructed from up to six separate name elements.~ The following diagram shows the elements and the order that they are to be used in the name.~ The first three are each somewhat optional and are used as needed to identify the type of engineering model, object, or device being reported on.~ The last three are nearly always needed. Units are always needed (as described below.
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image003.jpg}
+\caption{Output Variable Classification Elements \protect \label{fig:output-variable-classification-elements}}
+\end{figure}
+
+\textbf{Model Classification}. This name element is used to identify the specific type of modeling being conducted.~ When used, it will form the first part of the name. This name element is often not needed, such as when the output is for a more or less usual aspect of buildings and HVAC system models.~ This is typically used to identify outputs that are associated with an alternative, usually more advanced, model, such as AirflowNetwork (AFN) or Conduction Finite Difference (CondFD).~ Although modeling domains such as Building, HVAC, or Internal Loads are usually obvious and not needed here, this classification can be useful for non-obvious sub-domains such as Environmental Impact, Refrigeration, or Daylighting.
+
+\textbf{Spatial Classification}. This name element is used to identify spatial or topological location of the thing being reported on.~ It is generally used to identify which part of the building or system is being referred to by the output.~ For parts of the building, classifications such as ``Zone'' and ``Surface'' are the most common.~ For a model such as Refrigeration this classification may identify specific parts of the system, such as ``Secondary Loop.''~ There is often no spatial or topological aspect needed and in that case this name element can be omitted.
+
+\textbf{Type of Component}. This name element is used to identify the type of device or phenomena being modeled and reported on.~ For most component models this should be a simple generic term for the type of device and attempt to reuse established names for similar devices or models.~ In cases where the Model and Spatial Classifications are sufficient, this element can be omitted.
+
+\textbf{Specific Nature.} This name element is used to identify the nature of what is being reported for the device or phenomena being modeled. This is where the most low-level and specific detail is applied to describe the output variable.~ This name element is nearly always needed.
+
+\textbf{Dimensional Nature.} This name element is used to identify the nature of the physical dimensions of the quantity being reported in words.~ This name element is nearly always needed. This name element is the final part of the name so that names end with terms that reflect the nature of the value being reported. However, the name element should not be the actual units.~ For example, an output that has units of degrees Celsius, the final word in the name should be ``Temperature.''~ Or an output for air flow that has units of kg/s, the final words in the name should be ``Mass Flow Rate.''~ When reporting on electricity use in Watts, the term ``Power'' is used; however most other uses of Watts use the term ``Rate.''
+
+\textbf{Units}. This name element is used to identify the units of the value being reported.~ ~Units of output variables are strictly SI, as used in EnergyPlus.~ Units are concatenated on the end of the name with square brackets and separated by a space and.~ Dimensionless quantities shall use empty brackets ``{[} {]}.''~ The preferred set of units is listed at the top of the Energy+.idd file. Units are always abbreviated.
+
+In some situations, a model may lend itself to generating a series of related output variables that depend on input.~ For example a surface heat transfer model may have results for numerous individual nodes or cells across the thickness of the surfaces.~ The number of nodes in the model will vary at runtime depending on the Construction.~ When this is the case, the standard approach used in EnergyPlus is to produce a series of output variables by enumerating the output variable name (rather than the key value) to generate a specific name for each instance.~ The generated name element for each instance in the series is appended to the end of the name (but before the Units element) and should end in a number. For example, the third node in a stratified tank model is called ``Chilled Water Thermal Storage Temperature Node 3 {[}C{]}.''~ This is done to facilitate wildcarding when postprocessing output.
+
+For Version 8.0, a comprehensive effort was made to rename output variables to follow the guidelines and scheme described above.~ As of Version 8.0 the existing output variables demonstrate the pattern and should serve as good examples to follow for future output variables. The following table lists a few examples of terms, but these are not meant to be comprehensive or restrictive.~ It is expected that new models may have valid reasons to introduce new terms and units. Developers should examine RDD output files for comprehensive lists of example output variable names.
+
+% table 5
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Output Variable Classifications \label{table:output-variable-classifications}} \tabularnewline
+\toprule 
+Model Classification & Spatial Classification & Type of Component & Dimensional Nature \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Output Variable Classifications} \tabularnewline
+\toprule 
+Model Classification & Spatial Classification & Type of Component & Dimensional Nature \tabularnewline
+\midrule
+\endhead
+
+AFN & Zone & Inside Face & Rate \tabularnewline
+Refrigeration & Surface & Outside Face & Rate per Area \tabularnewline
+Room Air & Linkage & Air Terminal & Energy \tabularnewline
+HAMT & Interior & Boiler & Temperature \tabularnewline
+CondFD & Exterior & Chiller & Mass Flow Rate \tabularnewline
+EMPD & Site & Cooling Coil & COP \tabularnewline
+Plant & Supply Side & Infiltration & Power (electric) \tabularnewline
+Environmental Impact & Air System & Unit Heater & Level \tabularnewline
+HVAC & Facility & Generator & Fraction \tabularnewline
+Setpoint Manager & Node & Baseboard & Status \tabularnewline
+\bottomrule
+\end{longtable}
+
+~The following table lists acronyms and symbols used in output variable names.
+
+Table 6. Output Variable Example Abbreviations
+
+Acronym
+
+Definition
+
+AC
+
+Alternating Current
+
+AFN
+
+AirflowNetwork
+
+Ar
+
+Argon
+
+ASHRAE
+
+American Society of Heating, Refrigeration, and Air-Conditioning Engineers, Inc.
+
+BSDF
+
+Bidirectional Scattering Distribution Function
+
+CEN
+
+European Committee for Standardization (Comite Europeen de Normalisation)
+
+CH4
+
+Methane
+
+CO
+
+Carbon Monoxide
+
+CO2
+
+Carbon Dioxide
+
+CondFD
+
+Conduction Finite Difference
+
+COP
+
+Coefficient of Performance
+
+DC
+
+Direct Current
+
+DX
+
+Direct Expansion
+
+EIR
+
+Energy Input Ratio
+
+EMPD
+
+Effective Moisture Penetration Depth
+
+H20
+
+Water
+
+HAMT
+
+Heat and Moisture Transfer
+
+Hg
+
+Mercury
+
+HHV
+
+Higher Heating Value
+
+HVAC
+
+Heating Ventilation and Air Conditioning
+
+KSU
+
+Kansas State University
+
+LHV
+
+Lower Heating Value
+
+N2
+
+Nitrogen
+
+N2O
+
+Nitrous Oxide
+
+NH3
+
+Ammonia
+
+NMVOC
+
+Non-Methane Volatile Organic Compounds
+
+NOx
+
+Nitrogen Oxides
+
+O2
+
+Oxygen
+
+Pb
+
+Lead
+
+PM
+
+Particulate Matter
+
+PM10
+
+Particulate Matter of 10 microns or less in size
+
+PM2.5
+
+Particulate Matter of 2.5 microns or less in size
+
+PMV
+
+Predicted Mean Vote
+
+PPD
+
+Percent People Dissatisfied
+
+PV
+
+Photovoltaic
+
+PVT
+
+Photovoltaic-Thermal
+
+SO2
+
+Sulfur Dioxide
+
+VAV
+
+Variable Air Volume
+
+VRF
+
+Variable Refrigerant Flow
+
+WAHP
+
+Water to Air Heat Pump
+
+\subsection{What are Meters?}\label{what-are-meters}
+
+In EnergyPlus meters are an additional output reporting capability. A meter is a way of grouping similar output variables. Meters are output variables just like ordinary output variables except that they sum or average a collection of ordinary output variables. In EnergyPlus the meter variables serve two purposes.
+
+\begin{itemize}
+\item
+  Providing output of fuel and electricity consumption by end use categories and at the system plant, building and facility level.
+\item
+  Providing a way of summing heating or cooling outputs for a category of components. The resource type EnergyTransfer is used for this purpose. An example would be reporting out the sum of the heating energy from all the heating coils in a system.
+\end{itemize}
+
+\subsection{How Do I Create A Meter?}\label{how-do-i-create-a-meter}
+
+Meter output variables are created at the same time and in the same manner as ordinary output variables. SetupOutputVariable is called but the optional arguments ResourceTypeKey, EndUseKey, and GroupKey must be used in addition to the usual arguments. For example, in the electric steam humidifier module
+
+CALL SetupOutputVariable(`Humidifier Electric Energy {[}J{]}', \&
+
+~ Humidifier(HumNum)\%ElecUseEnergy, `System',`Sum', \&
+
+~ Humidifier(HumNum)\%Name)
+
+creates an output variable labeled `Humidifier Electric Energy {[}J{]}' with the value of Humidifier(HumNum)\%ElecUseEnergy.
+
+CALL SetupOutputVariable(`Humidifier Electric Energy {[}J{]}', \&
+
+~ Humidifier(HumNum)\%ElecUseEnergy, `System',`Sum', \&
+
+~ Humidifier(HumNum)\%Name, \& ~ ResourceTypeKey = `ELECTRICITY',EndUseKey = `HUMIDIFIER', \&
+
+~ GroupKey = `System')
+
+Creates the same output variable but in addition creates a meter output variable Humidifier:Electricity {[}J{]}. This variable will contain the sum of all the electricity consumption of the humidifiers in the system. In addition, this electrical consumption will be added into the meter variables Electricity:HVAC {[}J{]} and Electricity:Facility {[}J{]}.
+
+\subsection{Rules for Meter Variables}\label{rules-for-meter-variables}
+
+There are a number of rules developers must follow in order to account for all electricity and fuel consumption as well as to prevent consumables from being double counted.
+
+t~Electricity and fuel meters must always be defined at the simple component level. Some EnergyPlus components are compound components: they are built up from simple components. Examples are fan coils (composed of heating coils, cooling coils, and fans), terminal units etc. Some example simple components are heating and cooling coils, fans, humidifiers etc. Electricity and fuel consumption should always be metered at the simple component level and never at the compound component level. This prevents double counting of the fuel or energy consumption.
+
+t~A variable should be metered once only. This means a variable can be assigned to only one resource type and to only one end use category.
+
+t~Energy Transfer should be metered in the same way as fuel or electricity use. Energy Transfer meters should only be defined for simple components and should be assigned the same end use category as the fuel or electricity consumption.
+
+t~All fuel and electricity consumption must be put in some (one) meter.
+
+t~Use Energy Transfer judiciously; if in doubt, leave it out.
diff --git a/doc/module-developer/src/quick-procedure-outline-for-making-code.tex b/doc/module-developer/src/quick-procedure-outline-for-making-code.tex
new file mode 100644
index 00000000000..b941c4498c5
--- /dev/null
+++ b/doc/module-developer/src/quick-procedure-outline-for-making-code.tex
@@ -0,0 +1,39 @@
+\chapter{Quick Procedure Outline For Making Code Changes to EnergyPlus}\label{quick-procedure-outline-for-making-code-changes-to-energyplus}
+
+Some of the steps in this section are primarily applicable to developers who are part of the ``EnergyPlus Team''.~ However, these steps should also be followed as you develop a module or other piece to submit to the EnergyPlus Team for inclusion in an EnergyPlus release.
+
+1.~~~Write a New Feature Proposal (often called NFP) for discussion at a bi-weekly conference call.~ Based on that discussion, update the NFP. Out of team developers: use the NFP format to help formulate your submission documentation to the EnergyPlus Team. \textbf{\emph{The NFP format is shown in Appendix F. The sections of the NFP format are shown in}} \textbf{\emph{Table~\ref{table:sections-of-a-new-feature-proposal}. Sections of a New Feature Proposal.}}
+
+2.~~~Get the relevant files for your development. Team developers can check out files from StarTeam.
+
+a.~~~Energy+.idd and Featurechanges.csv are in the `Release' Folder. This folder also contains the ``Rules'' spreadsheet and ``Report Variables'' files.
+
+b.~~~ExampleFiles.xls, ExampleFilesDoc.txt, and baseline or relevant IDF files from `Test Files - Utilities\textbackslash{}InternalTests\textbackslash{}InputFiles`
+
+c.~~~F90 files from the `SourceCode' folder.
+
+d.~~~Documents (InputOutputReference.doc, EngineeringReference.doc, OutputDetailsAndExamples.doc, etc.) from the `External Documentation\textbackslash{}Documentation Sources' folder.
+
+3.~~~Following proper procedures (\emph{e.g., Object naming conventions are specified earlier in this document}) make your object changes to the Energy+.idd and relevant IDF files.~ If your IDD modifications make changes for existing objects, you must determine if you need to add to the ``Rules'' spreadsheet so that the transition program can be made for existing IDF files.~ Likewise, if you change existing report variable names, you must update the ``Report Variables'' file. Note that the ExampleFiles.xls has some guidance on the contents of new test suite files. Create or change existing IDF files for your feature.
+
+4.~~~Make code changes to F90 files for subroutines, GetInput, Sim, Report or create your own module following the Programming Standards and Programming Templates.~ Programming Templates are available in Appendix D.~ Programming Standards is a separate document.
+
+5.~~~Compile and run in debug mode to track errors.
+
+6.~~~Test making sample runs; review summary and time step reports to identify issues. Test many features of your module even if you are not including all in the Test Suite IDF file. Go back to Step 4 as necessary. Note some of the issues in the ``Important Rules for Developers''.
+
+7.~~~When complete, run full test suite to make sure there are no crashes or unexpected changes in other files.
+
+8.~~~Run Reverse DD for your featured files -- making sure the results \emph{exactly} match.
+
+9.~~~Update relevant portions of documents: InputOutputReference.doc, EngineeringReference.doc, OutputDetailsAndExamples.doc, etc.~ Only excerpted portions of the document should be sent forward for review and final inclusion in the whole document. Depending on the changes, it may be better to ``track changes'' in the document or give instructions for inclusion in the whole document. Send these documents up the review chain as appropriate.~ \textbf{\emph{Appendix C also has some information about formatting documents.}}
+
+10.~Procedure on checking in files changes from time to time.~ Currently, all source code files are kept locked and your code may go through another reivew before you are allowed to check in.~ \textbf{\emph{Follow procedures in Appendix B as well about submitting your feature -- many parts are repeated in this section.}}
+
+11.~Check in modified or new files. If changes have been made to the original checked out file, you must carefully merge your changes into the file -- this also may necessitate you repeating your test runs. Usually, your featurechanges modification will be very simple and be the last line in that file.
+
+12.~Send email to the team notifying them of the new feature/changed feature/defect fix and what files were changed/added/etc.
+
+13.~Incorporate any feedback after checkin.
+
+14.~Use \textbf{\emph{Appendix G}} to submit information, if applicable, about your feature.
diff --git a/doc/module-developer/src/running-testing-energyplus-for-developers.tex b/doc/module-developer/src/running-testing-energyplus-for-developers.tex
new file mode 100644
index 00000000000..076ba1dc181
--- /dev/null
+++ b/doc/module-developer/src/running-testing-energyplus-for-developers.tex
@@ -0,0 +1,32 @@
+\chapter{Running/Testing EnergyPlus -- for Developers}\label{runningtesting-energyplus-for-developers}
+
+Any item mentioned in this section is available at no charge to collaborative or other developers -- the documentation, however, may be rudimentary and use of the procedures require some knowledge of command line (Windows) or Linux scripts.
+
+EnergyPlus is rigorously tested during each release cycle and prior to each release.~ Details on some of the test suites that have been used can be seen at:
+
+http://www.eere.energy.gov/buildings/energyplus/testing.html
+
+Equally important is the testing done by each developer during feature development or changes.~ For example, on the core development team, developers are charged with executing the entire test suite (≥230 files) for their checkins.~ In addition, one of the core development team does run the entire test suite with each checkin and compares those results to previous results.~ Unexpected changes, and certainly crashes, should NOT occur.
+
+Since most modules being developed are aimed at the HVAC or plant features, there is a standard 5-zone template geometry that can be used.~ This should form the basis of any new additions.~ The old 3-zone model should not be used.~ Of course, you may develop your own model.
+
+Developers are also charged with making sure their input file runs an entire weather year, has minimal errors (including max simulation errors) and results compare \emph{exactly} when design days (preferably winter-summer vs summer-winter) are reversed in consecutive runs (also known as ReverseDD).~ To assist in ReverseDD testing, each input file \emph{should} have a ``Run Control'' object as well as (at least) two design days (winter-summer / summer-winter as the first two).
+
+Input files should report Zone Air temperatures (Zone Mean Air Temperature or Zone/Sys Air Temperature) as well as meters such as electricity and gas (if applicable).~ Of course, reporting features being implemented should be done as well.~ These variables will help identify files that have proper ``ReverseDD'' requirements (failures usually indicate some initialization problems).~ Developers should try to minimize output file size -- if you are running a full annual simulation (as required by your feature), you should \emph{NOT} report variables at the timestep level.
+
+To compare results, we have a python script (Mathdiff) that is run on the .csv files.~ It will report (by default) differences \textless{} = .001 or \textless{} = .5\% as ``within range'' and outside those limits as ``differences''.~ If they are exactly the same (from the .csv precision limits), they will be reported as such.
+
+Developers in the core development team use several methods for running the entire test suite.
+
+\begin{itemize}
+\item
+  One method uses a list of input file names along with an indication of the proper weather file.~ A program reads this file and produces several batch files which help with not only running the file but comparing them to previous results, building the ``composite error'' (the .err files from each file run), and other utility features.~ (The same file can be used in Linux testing)
+\item
+  Another method uses a batch file with options that will allow running old vs.~new exes as well as somewhat automating the reverse dd testing.
+\item
+  Still another method uses a simple batch procedure to ``run'' all files in a folder.
+\item
+  Finally, EP-Launch and ``groups'' can be used.
+\end{itemize}
+
+To facilitate testing, Environment Variables ``values'' have been implemented in EnergyPlus and/or script files.~ To use, one uses the ``Set'' command and the value as indicated.~ Environment variable value testing is inherent in F2003 compliant compilers; for others we have written a set of routines that can either be modified or used directly.
diff --git a/doc/module-developer/src/running-testing-energyplus-for-developers/air-loop-simulation-environment-variables.tex b/doc/module-developer/src/running-testing-energyplus-for-developers/air-loop-simulation-environment-variables.tex
new file mode 100644
index 00000000000..e1f3c05db0d
--- /dev/null
+++ b/doc/module-developer/src/running-testing-energyplus-for-developers/air-loop-simulation-environment-variables.tex
@@ -0,0 +1,21 @@
+\section{Air Loop Simulation Environment Variables}\label{air-loop-simulation-environment-variables}
+
+To facilitate comparing the runtime performance of various solution techniques for the air loop simulation a mechanism to track runtime statistics has been implemented in EnergyPlus. To facilitate debugging the air loop simulation a tracing mechanism operating either at the air loop-level or at the controller-level has been implemented in EnergyPlus.~ To use, one uses the ``Set'' command and the value as indicated.
+
+\subsubsection{TRACK\_AIRLOOP: Runtime performance tracker for air loop simulation}\label{trackux5fairloop-runtime-performance-tracker-for-air-loop-simulation}
+
+Setting to ``yes'' will cause EnergyPlus to track the performance of the air loop simulation at runtime and dump the results in a file named ``statistics.HVACControllers.csv'' upon ending the simulation.~ (Uses logical variable \textbf{TrackAirLoopEnvFlag} in module DataSystemVariables).
+
+Set TRACK\_AIRLOOP = yes
+
+\subsubsection{TRACE\_AIRLOOP: Air loop simulation tracer}\label{traceux5fairloop-air-loop-simulation-tracer}
+
+Setting to ``yes'' will cause EnergyPlus to write to a trace file named ``controller.\textless{}Air Loop Name\textgreater{}.csv'' the converged solutions of all controllers defined on each air loop, at each HVAC iteration.~ (Uses logical variable \textbf{TraceAirLoopEnvFlag} in module DataSystemVariables).
+
+Set TRACE\_AIRLOOP = yes
+
+\subsubsection{TRACE\_HVACCONTROLLER: Individual HVAC controller tracer}\label{traceux5fhvaccontroller-individual-hvac-controller-tracer}
+
+Setting to ``yes'' will cause EnergyPlus to write to a trace file named ``controller.\textless{}Controller Name\textgreater{}.csv'' a detailed description of each controller iteration at each HVAC iteration.~ (Uses logical variable \textbf{TraceControllerEnvFlag} in module DataSystemVariables).
+
+Set TRACE\_HVACCONTROLLER = yes
diff --git a/doc/module-developer/src/running-testing-energyplus-for-developers/environment-variables-to-assist-running.tex b/doc/module-developer/src/running-testing-energyplus-for-developers/environment-variables-to-assist-running.tex
new file mode 100644
index 00000000000..a9f100a68c4
--- /dev/null
+++ b/doc/module-developer/src/running-testing-energyplus-for-developers/environment-variables-to-assist-running.tex
@@ -0,0 +1,183 @@
+\section{Environment Variables to Assist Running}\label{environment-variables-to-assist-running}
+
+Some environment variables can be used with single or several idf file(s) to keep IDF files pristine while allowing developers or others trying to determine a problem or run a group of files. Many of these have counterparts in Output:Diagnostics objects (some may not be documented). Likewise there may be some ``sections'' that will produce certain outputs not generally documented.
+
+\subsubsection{DDOnly: Design Days Only}\label{ddonly-design-days-only}
+
+Setting to ``yes'' will cause EnergyPlus to set Run Control option (regardless of whether there is a Run Control object in the input file) for Do the Design Day Simulation to ``yes'' and Do the Weather File Simulation to ``no''.~ (Uses logical variable \textbf{DDOnly} in module DataSystemVariables). There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set DDOnly = yes
+\end{lstlisting}
+
+\subsubsection{FullAnnualRun: Full Annual simulation}\label{fullannualrun-full-annual-simulation}
+
+Setting to ``yes'' will cause EnergyPlus to set Run Control option (regardless of whether there is a Run Control object in the input file) for Do the Weather File Simulation to ``yes''. Scripts should use a weather file when this environment variable is set.~ (Uses logical variable \textbf{FullAnnualRun} in module DataSystemVariables). There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set FullAnnualRun = yes
+\end{lstlisting}
+
+And appropriate changes to script files
+
+\subsubsection{NoWeatherFile: Do not use weatherfile even if indicated}\label{noweatherfile-do-not-use-weatherfile-even-if-indicated}
+
+Setting to ``yes'' doesn't cause EnergyPlus to do anything but can be used in the scripts to not copy a weather file even when indicated. There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set NoWeatherFile = yes
+\end{lstlisting}
+
+And appropriate changes to script files
+
+\subsubsection{ReverseDD: Reverse Design Days during run}\label{reversedd-reverse-design-days-during-run}
+
+Setting to ``yes'' causes the first two design days requested in the input file to be reversed during EnergyPlus execution.~ (Uses logical variable \textbf{ReverseDD} in module DataSystemVariables).~ For proper comparisons to original order, a program such as \textbf{ReverseDDInCSV} or \textbf{ReverseDDInESO} must be run or hand edited. There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set ReverseDD = yes
+\end{lstlisting}
+
+And appropriate changes to script files
+
+\subsubsection{MinReportFrequency: Set minimum reporting frequency for outputs}\label{minreportfrequency-set-minimum-reporting-frequency-for-outputs}
+
+Some developers persist in reporting at the timestep or detailed level even if their runs are full annual runs. This is really burdensome on developers that try to run the full test suite for checking changes. The MinReportFrequency environment variable allows EnergyPlus to report at a higher/less frequent level that still allows for changes to be checked (though differences may require more frequent reporting to track down). EnergyPlus reads this environment variable and sets reporting frequency appropriately. There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set MinReportFrequency = daily
+\end{lstlisting}
+
+The standard frequencies accepted by EnergyPlus must be used: detail, timestep, hourly, daily, monthly, runperiod, environment, annual. In addition, if this environment variable is used, the following will show in the .eio file:
+
+! \textless{}Minimum Reporting Frequency (overriding input value)\textgreater{}, Value, Input Value
+
+~Minimum Reporting Frequency,~ !Daily {[}Value,Min,Hour,Minute,Max,Hour,Minute{]},DAILY
+
+\subsubsection{ReportDuringWarmup: Cause reporting during warmup}\label{reportduringwarmup-cause-reporting-during-warmup}
+
+Setting to ``yes'' causes reporting (Output:Variable, Output:Meter) to be reporting during the warmup days at the start of each environment. (Uses logical variable \textbf{ReportDuringWarmup} in module DataSystemVariables).~ The Output:Diagnostics, ReportDuringWarmup; is equivalent.
+
+\begin{lstlisting}
+Set ReportDuringWarmup = yes
+\end{lstlisting}
+
+\subsubsection{REPORTDURINGHVACSIZINGSIMULATION: Cause SQLite reporting during HVAC Sizing Simulations}\label{reportduringhvacsizingsimulation-cause-sqlite-reporting-during-hvac-sizing-simulations}
+
+Setting to ``yes'' causes output to be sent to SQLite database file during HVAC Sizing Simulations. (Uses Boolean variable ReportDuringHVACSizingSimulation in DataSystemVariables). The Output:Diagnostics, ReportDuringHVAVSizingSimulation; is equivalent.
+
+\begin{lstlisting}
+Set REPORTDURINGHVACSIZINGSIMULATIN = YES
+\end{lstlisting}
+
+\subsubsection{DisplayAllWarnings: turn on all extra warnings}\label{displayallwarnings-turn-on-all-extra-warnings}
+
+Setting to ``yes'' causes turning on the warnings: DisplayAllWarnings, DisplayExtraWarnings, DisplayUnusedSchedules, DisplayUnusedObjects. DisplayUnusedObjects also displays unused fluids (that is, fluids that are not directly retrieved by the simulation). The Output:Diagnostics, DisplayAllWarnings; is equivalent.
+
+\begin{lstlisting}
+Set DisplayAllWarnings = yes
+\end{lstlisting}
+
+\subsubsection{DisplayExtraWarnings: turn on~ extra warnings}\label{displayextrawarnings-turn-on-extra-warnings}
+
+Setting to ``yes'' causes turning on DispalyExtraWarnings. The Output:Diagnostics, DisplayExtraWarnings; is equivalent.
+
+\begin{lstlisting}
+Set DisplayExtraWarnings = yes
+\end{lstlisting}
+
+\subsubsection{DisplayUnusedObjects: turn on display of unused objects and fluids}\label{displayunusedobjects-turn-on-display-of-unused-objects-and-fluids}
+
+Setting to ``yes'' causes the orphan objects and fluids that are in the input file but not used to be displayed at the end of the simulation. The Output:Diagnostics, DisplayUnusedObjects; is equivalent.
+
+\begin{lstlisting}
+Set DisplayUnusedObjects = yes
+\end{lstlisting}
+
+\subsubsection{DisplayUnusedSchedules: turn on display of unused schedules}\label{displayunusedschedules-turn-on-display-of-unused-schedules}
+
+Setting to ``yes'' causes the schedules that are in the input file but not used to be displayed at the end of the simulation. The Output:Diagnostics, DisplayUnusedSchedules; is equivalent.
+
+\begin{lstlisting}
+Set DisplayUnusedSchedules = yes
+\end{lstlisting}
+
+\subsubsection{DisplayZoneAirHeatBalanceOffBalance: turn on this development output}\label{displayzoneairheatbalanceoffbalance-turn-on-this-development-output}
+
+Setting to ``yes'' causes the program to calculate and display the Zone Air Heat Balance ``out of balance'' warnings. The Output:Diagnostics, DisplayZoneAirHeatBalanceOffBalance; is equivalent.
+
+\begin{lstlisting}
+Set DisplayZoneAirHeatBalanceOffBalance = yes
+\end{lstlisting}
+
+\subsubsection{IgnoreSolarRadiation: turn off using Solar in simulation}\label{ignoresolarradiation-turn-off-using-solar-in-simulation}
+
+Setting to ``yes'' causes the program to ignore all solar values during simulation.~ One might use this when a new set of weather files are produced but you are unsure of their impacts. It also speeds the program as no shading calculations are done. The Output:Diagnostics, IgnoreSolarRadiation; is equivalent.
+
+\begin{lstlisting}
+Set IgnoreSolarRadiation = yes
+\end{lstlisting}
+
+\subsubsection{DisplayAdvancedReportVariables: turn on access to advance report variables}\label{displayadvancedreportvariables-turn-on-access-to-advance-report-variables}
+
+Setting to ``yes'' causes the program to be able to access the ``advanced report variable'' set in the program.The Output:Diagnostics, DisplayAdvancedReportVariables; is equivalent.
+
+\begin{lstlisting}
+Set DisplayAdvancedReportVariables = yes
+\end{lstlisting}
+
+\subsubsection{SortIDD: turn on (or off) the sorting of IDD objects}\label{sortidd-turn-on-or-off-the-sorting-of-idd-objects}
+
+Setting to ``yes'' (internal default) causes the program to use sorted lists (a speed up mechanism) in searching for existant objects during IDF processing. There is really no reason to turn it off. There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set SortIDD = yes
+\end{lstlisting}
+
+\subsubsection{DeveloperFlag: turn on (or off) some different outputs for the developer}\label{developerflag-turn-on-or-off-some-different-outputs-for-the-developer}
+
+Setting to ``yes'' (internal default is ``no'') causes the program to display some different information that could be useful to developers. In particular, this will cause the Warmup Convergence output to show the last day for each zone, each timestep. There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set DeveloperFlag = yes
+\end{lstlisting}
+
+\subsubsection{IgnoreBeamRadiation: turn on (or off) the beam radiation}\label{ignorebeamradiation-turn-on-or-off-the-beam-radiation}
+
+Setting to ``yes'' causes the program to ignore beam radiation in solar calculations. Of limited use, but may be useful for some simulation developments or isolating problems. There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set IgnoreBeamRadiation = yes
+\end{lstlisting}
+
+\subsubsection{IgnoreDiffuseRadiation: turn on (or off) the diffuse radiation}\label{ignorediffuseradiation-turn-on-or-off-the-diffuse-radiation}
+
+Setting to ``yes'' causes the program to ignore diffuse radiation in solar calculations. Of limited use, but may be useful for some simulation developments or isolating problems. There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set IgnoreDiffuseRadiation = yes
+\end{lstlisting}
+
+\subsubsection{SutherlandHodgman: turn on (or off) the polygon clipping algorithm}\label{sutherlandhodgman-turn-on-or-off-the-polygon-clipping-algorithm}
+
+Setting to ``yes'' (internal default) causes the program to use the SutherlandHodgman polygon clipping algorithm. You might use this if you wanted to run a bunch of files with the legacy clipping algorithm (convex Weiler Atherton). There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set SutherlandHodgman = yes
+\end{lstlisting}
+
+\subsubsection{MinimalShadowing: turn on (or off) the use of Minimal Shadowing}\label{minimalshadowing-turn-on-or-off-the-use-of-minimal-shadowing}
+
+Setting to ``yes'' causes the program to use Minimal Shadowing (a speed up mechanism) in calculations. This could be useful when large files are being run to search for non-shadowing related problems. There is no Output:Diagnostics equivalent.
+
+\begin{lstlisting}
+Set MinimalShadowing = yes
+\end{lstlisting}
+
+\subsubsection{DisplayInputInAudit: turn on (or off) to show the input file in the audit file}\label{displayinputinaudit-turn-on-or-off-to-show-the-input-file-in-the-audit-file}
+
+Setting to ``yes'' causes the audit file to include a line-by-line echoing of the input file which may be useful for debugging purposes. For versions 8.2 and earlier, the default behavior was to include the line-by-line echoing of the input file into the audit file but it was changed to not do this by default as a way to speed up the input processing portion of executing EnergyPlus. When not set to ``yes'', the audit file contains a reference on using the DisplayInputInAudit environment variable to see the line-by-line echoing of the input file.
+
+\subsubsection{Caution: Environment Variables}\label{caution-environment-variables}
+
+Some combinations will cause fatal errors from EnergyPlus -- \textbf{DDOnly} and \textbf{FullAnnualRun}, for example.~ \textbf{FullAnnualRun} and \textbf{NoWeatherFile} won't cause fatal errors from EnergyPlus but probably should from the script files.~ We welcome any suggestions for future environment variables.
diff --git a/doc/output-details-and-examples/CMakeLists.txt b/doc/output-details-and-examples/CMakeLists.txt
new file mode 100644
index 00000000000..a2e2c9af52d
--- /dev/null
+++ b/doc/output-details-and-examples/CMakeLists.txt
@@ -0,0 +1,67 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/output-details-and-examples.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-details-and-examples.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/introduction.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/output-file-list.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-audit.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-bnd.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-dbg.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-dxf.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-edd.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-eio.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusssz-lt-ext-gt.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/epluszsz-lt-ext-gt.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-lt-ext-gt.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusmtr-lt-ext-gt.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusmap-lt-ext-gt.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-dfs.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusscreen-csv.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplustbl-lt-ext-gt.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/readvars-rvaudit.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-svg.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-sci.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/eplusout-wrl.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/output-files/delight-output-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/example-input-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/data-sets.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/data-sets/simple-list-data-sets.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/src/data-sets/macro-data-sets.tex
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/../title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image001.jpg
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image002.jpg
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image017.png
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image018.jpg
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image019.png
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image020.png
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image021.png
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image022.jpg
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image023.jpg
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image024.jpg
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image025.jpg
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image026.jpg
+  ${CMAKE_SOURCE_DIR}/doc/output-details-and-examples/media/image027.jpg
+) 
+
+SET( SOURCE_FILENAME "output-details-and-examples" )
+SET( OUTPUT_FILENAME "OutputDetailsAndExamples" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/src/docs/OutputDetailsAndExamples/media/ep.gif b/doc/output-details-and-examples/media/ep.gif
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diff --git a/doc/src/docs/OutputDetailsAndExamples/media/image023.jpg b/doc/output-details-and-examples/media/image023.jpg
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diff --git a/doc/src/docs/OutputDetailsAndExamples/media/image024.jpg b/doc/output-details-and-examples/media/image024.jpg
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rename from doc/src/docs/OutputDetailsAndExamples/media/image024.jpg
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diff --git a/doc/src/docs/OutputDetailsAndExamples/media/image025.jpg b/doc/output-details-and-examples/media/image025.jpg
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diff --git a/doc/src/docs/OutputDetailsAndExamples/media/image026.jpg b/doc/output-details-and-examples/media/image026.jpg
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diff --git a/doc/src/docs/OutputDetailsAndExamples/media/image027.jpg b/doc/output-details-and-examples/media/image027.jpg
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diff --git a/doc/output-details-and-examples/output-details-and-examples.tex b/doc/output-details-and-examples/output-details-and-examples.tex
new file mode 100644
index 00000000000..37b6e68dae2
--- /dev/null
+++ b/doc/output-details-and-examples/output-details-and-examples.tex
@@ -0,0 +1,72 @@
+\input{../header}
+
+\title{Output Details and Examples}
+
+\hypersetup{unicode=true,
+            pdftitle={Output Details and Examples},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/output-details-and-examples}
+
+\input{src/introduction}
+
+\input{src/output-files}
+
+\input{src/output-files/output-file-list}
+
+\input{src/output-files/eplusout-audit}
+
+\input{src/output-files/eplusout-bnd}
+
+\input{src/output-files/eplusout-dbg}
+
+\input{src/output-files/eplusout-dxf}
+
+\input{src/output-files/eplusout-edd}
+
+\input{src/output-files/eplusout-eio}
+
+\input{src/output-files/eplusssz-lt-ext-gt}
+
+\input{src/output-files/epluszsz-lt-ext-gt}
+
+\input{src/output-files/eplusout-lt-ext-gt}
+
+\input{src/output-files/eplusmtr-lt-ext-gt}
+
+\input{src/output-files/eplusmap-lt-ext-gt}
+
+\input{src/output-files/eplusout-dfs}
+
+\input{src/output-files/eplusscreen-csv}
+
+\input{src/output-files/eplustbl-lt-ext-gt}
+
+\input{src/output-files/readvars-rvaudit}
+
+\input{src/output-files/eplusout-svg}
+
+\input{src/output-files/eplusout-sci}
+
+\input{src/output-files/eplusout-wrl}
+
+\input{src/output-files/delight-output-files}
+
+\input{src/example-input-files}
+
+\input{src/data-sets}
+
+\input{src/data-sets/simple-list-data-sets}
+
+\input{src/data-sets/macro-data-sets}
+
+\end{document}
diff --git a/doc/output-details-and-examples/src/data-sets.tex b/doc/output-details-and-examples/src/data-sets.tex
new file mode 100644
index 00000000000..2f5b0bf9eea
--- /dev/null
+++ b/doc/output-details-and-examples/src/data-sets.tex
@@ -0,0 +1,3 @@
+\chapter{Data Sets}\label{data-sets}
+
+Data sets are the EnergyPlus answer to ``libraries''. Data sets come in two flavors -- a simple list and a ``macroized'' list. Macroized lists are files that could have the elements extracted using a simple macro name.
diff --git a/doc/output-details-and-examples/src/data-sets/macro-data-sets.tex b/doc/output-details-and-examples/src/data-sets/macro-data-sets.tex
new file mode 100644
index 00000000000..fc340b5eb1a
--- /dev/null
+++ b/doc/output-details-and-examples/src/data-sets/macro-data-sets.tex
@@ -0,0 +1,19 @@
+\section{Macro Data Sets}\label{macro-data-sets}
+
+\subsection{Locations-DesignDays.xls}\label{locations-designdays.xls}
+
+Strictly speaking, the locations-designdays.xls file is not a macro enabled input file. Rather, it is the ``pointer'' to other files and can be searched by city name, country, etc. All the Design Conditions from the ASHRAE Handbook of Fundamentals (2005) have been encoded into Design Day definitions and are stored on the EnergyPlus web site by WMO Region (similarly to how the weather data is stored). The spreadsheet contains a ``readme'' page as well as cities, countries, and links to the proper web pages.
+
+\subsection{SandiaPVData.idf}\label{sandiapvdata.idf}
+
+Use these PV statements for implementing PV modules in an EnergyPlus input file when using the Sandia model.
+
+\subsection{SolarCollectors.idf}\label{solarcollectors.idf}
+
+Use these SOLAR COLLECTOR PARAMETERS objects for implementing solar collector modules in an EnergyPlus input file.
+
+Data has been reproduced with permission from: ``Directory of SRCC Certified Solar Collector Ratings'' Copyright (c) 2004 by the Solar Rating and Certification Corporation. For more information, contact: Solar Rating and Certification Corporation, c/o FSEC, 1679 Clearlake Road, Cocoa, FL 32922-5703 USA~ Tel: (321) 638-1537~ Fax: (321) 638-1010~ ,~~ www.solar-rating.org
+
+\subsection{UtilityTariffObjects.imf}\label{utilitytariffobjects.imf}
+
+Use the large collections of input objects to model the costs of energy supplied by utility companies. This file is ready for use in macro processing but the input objects can readily be copied out of the macro file and used in a regular input file. The data were assembled by NREL researcher Brent Griffith and represent a best effort at putting together a comprehensive set of utility tariffs for commercial buildings for the USA as of Spring 2005. Use the data at your own risk and note that utility tariffs need to be continually updated to reflect current conditions.
diff --git a/doc/output-details-and-examples/src/data-sets/simple-list-data-sets.tex b/doc/output-details-and-examples/src/data-sets/simple-list-data-sets.tex
new file mode 100644
index 00000000000..8ee93c81613
--- /dev/null
+++ b/doc/output-details-and-examples/src/data-sets/simple-list-data-sets.tex
@@ -0,0 +1,1383 @@
+\section{Simple List Data Sets}\label{simple-list-data-sets}
+
+\subsection{AirCooledChillers.idf}\label{aircooledchillers.idf}
+
+This dataset includes performance curves for air cooled electric EIR chiller (object type: Chiller:Electric:EIR). Knowing the type of chiller that you want to simulate, you can find it and the associated performance curves in the dataset file. A brief synopsis of AirCooledChiller.idf is shown below:
+
+\begin{lstlisting}
+
+! AirCooledChillers.idf
+  !
+  ! This dataset includes performance curves for object type Chiller:Electric:EIR
+  !
+  ! Summary Table for Electric EIR Chiller reference data sets.
+  ! Chillers are listed in order of reference capacity. Reference capacity and COP do not necessarily
+  ! indicate rated capacity and COP at standard rating conditions (e.g. ARI Standard 550/590).
+  !
+  ! Performance curves developed from information collected from manufacturer's catalog data
+  ! The nomenclature used for the chiller is as follows:
+  ! ElectricEIRChiller - Manufacturer's Name - Model - Reference Capacity in kW - Reference COP
+  !
+  !                                                      Compressor   Reference    Reference
+  ! Chiller Name                                            Type       Capacity      COP
+  !                                                                    kW (tons)
+  ! ElectricEIRChiller McQuay AGZ010BS 34.5kW/2.67COP      Scroll     34.5 (9.8)      2.67
+  ! ElectricEIRChiller McQuay AGZ013BS 47.1kW/2.67COP      Scroll     47.1 (13.4)     2.67
+  ! ElectricEIRChiller York YCAL0019EE 54.2kW/2.9COP       Scroll     54.2 (15.4)     2.9
+  ! ElectricEIRChiller McQuay AGZ017BS 54.5kW/2.67COP      Scroll     54.5 (15.5)     2.67
+\end{lstlisting}
+
+\subsection{ASHRAE\_2005\_HOF\_Materials.idf}\label{ashraeux5f2005ux5fhofux5fmaterials.idf}
+
+This reference data set contains content from two chapters in the ASHRAE 2005 Handbook of Fundamentals, Chapter 30 - the Cooling and Heating Loads calculations chapter has both materials with thermal properties and constructions for Light, Medium, and Heavy buildings. Chapter 25 contains details thermal properties of many materials -- no constructions are created from that data.
+
+The following materials and constructions are created from ASHRAE Handbook of Fundamentals, 2005, Chapter 30, Table 19 and Table 22. These are representative of materials and constructions used in Cooling and Heating Load Calculations.
+
+\subsection{Boilers.idf}\label{boilers.idf}
+
+This dataset includes performance curves for non-electric boilers. Reference: Condensing Technology, Technical Series, Viessmann, 9446 803 - 1 GB Nov. 2004.
+
+\subsection{California\_Title\_24-2008.idf}\label{californiaux5ftitleux5f24-2008.idf}
+
+This dataset includes occupancy data and non-residential schedules for California Title 24-2008 compliance calculations when lighting plans are submitted for the Entire Building or when lighting compliance is not performed. Data is based on Table N2-5 of the 2008 Non-residential ACM Manual.
+
+\subsection{Chillers.idf}\label{chillers.idf}
+
+This dataset includes object types for specific (by manufacturer and type) Chiller:Electric:EIR and Chiller: Electric:ReformulatedEIR and associated performance curves.
+
+Knowing the type of chiller that you want to simulate, you can find it and the associated performance curves in the dataset file. By example, here is part of the comments in the Chiller.idf file:
+
+\begin{lstlisting}
+
+! Summary Table for Electric EIR Chiller reference data sets (Ref. CoolTools project).
+  ! Chillers are listed in order of compressor type and reference capacity (model calibration
+  ! point). Reference capacity and COP do not necessarily indicate rated capacity and COP at
+  ! standard rating conditions (e.g. ARI Standard 550/590).
+  !
+  ! Performance curves developed from information collected over a 10-year period from 1991 to 2001.
+  !
+  !                                                      Compressor   Reference  Reference Unloading
+  ! Chiller Name                                            Type       Capacity    COP     Mechanism
+  !                                                                    kW (tons)
+  !-------------------------------------------------------------------------------------------------
+  ! ElectricEIRChiller McQuay WSC 471kW/5.89COP/Vanes    Centrifugal   471 (134)   5.89   Inlet Vanes
+  ! ElectricEIRChiller York YT 563kW/10.61COP/Vanes      Centrifugal   563 (160)   10.61  Inlet Vanes
+  ! ElectricEIRChiller McQuay PEH 703kW/7.03COP/Vanes    Centrifugal   703 (200)   7.03   Inlet Vanes
+  ! ElectricEIRChiller Carrier 23XL 724kW/6.04COP/Vanes  Centrifugal   724 (206)   6.04   Inlet Vanes
+\end{lstlisting}
+
+\subsection{CompositeWallConstructions.idf}\label{compositewallconstructions.idf}
+
+The Reference Data Set CompositeWallConstructions.idf contains constructions and associated materials for a set of \textbf{composite} walls. These are walls---such as stud walls---that have complicated heat-flow paths so that the conduction is two- or three-dimensional.
+
+An example entry in this data set--for an insulated 2''x4'' steel-stud wall--looks like:
+
+\begin{lstlisting}
+
+CONSTRUCTION,Composite 2x4 Steel Stud R11,
+  ! ASHRAE 1145-RP Wall Assembly 10
+  ! 2"x4" steel studs at 24" on center with between-stud R11 fibreglass insulation.
+  ! Studs are 3.5", 16 gauge, 15 flange.
+  ! Layers are 1/2" wood siding, 1/2" plywood, 2x4 steel studs and R11 insulation, 1/2" gypsum board.
+  ! Area-average R-Value = 8.796 ft2-F-h/Btu (1.548 m2-K/W).
+  ! Total wall thickness = 5.00in (0.127m)
+  ! Material layer names follow:
+    Composite 2x4 Steel Stud R11 \#3,
+    Composite 2x4 Steel Stud R11 \#2,
+    Composite 2x4 Steel Stud R11 \#1;
+  MATERIAL,Composite 2x4 Steel Stud R11 \#1,
+    Smooth,  !- Roughness
+    0.013,   !- Thickness (m)
+    0.720,   !- Conductivity (W/m-K)
+    640.0,   !- Density (kg/m3)
+    1048,    !- Specific Heat (J/kg-K)
+    0.9,     !- Absorptance:Thermal
+    0.7,     !- Absorptance:Solar
+    0.7;     !- Absorptance:Visible
+  MATERIAL,Composite 2x4 Steel Stud R11 \#2,
+    Smooth,  !- Roughness
+    0.089,   !- Thickness (m)
+    0.060,   !- Conductivity (W/m-K)
+    118.223, !- Density (kg/m3)
+    1048,    !- Specific Heat (J/kg-K)
+    0.9,     !- Absorptance:Thermal
+    0.7,     !- Absorptance:Solar
+    0.7;     !- Absorptance:Visible
+  MATERIAL,Composite 2x4 Steel Stud R11 \#3,
+    Smooth,  !- Roughness
+    0.025,   !- Thickness (m)
+    0.452,   !- Conductivity (W/m-K)
+    413.782, !- Density (kg/m3)
+    1048,    !- Specific Heat (J/kg-K)
+    0.9,     !- Absorptance:Thermal
+    0.7,     !- Absorptance:Solar
+    0.7;     !- Absorptance:Visible
+\end{lstlisting}
+
+The materials here are \textbf{not} real materials but are ``equivalent'' materials obtained from finite-difference modeling. The thickness, conductivity, density and specific heat values of the material layers for the different constructions have been taken from the ASHRAE report ``Modeling Two- and Three-Dimensional Heat Transfer through Composite Wall and Roof Assemblies in Hourly Energy Simulation Programs (1145-TRP),'' by Enermodal Engineering Limited, Oak Ridge National Laboratory, and the Polish Academy of Sciences, January 2001. EnergyPlus will calculate conduction transfer functions using these materials. The heat transfer based on these conduction transfer functions will then be very close to what would be calculated with a two- or three-dimensional heat transfer calculation.
+
+For stud walls, using these composite constructions will give more accurate heat flow than you would get by manually dividing the wall into a stud section and a non-stud section.
+
+If your wall's exterior or interior roughness or thermal, solar or visible absorptances are different from those in the data set, you can make the appropriate changes to the first material (the outside layer) or the third material (the inside layer). \textbf{None of the other values should be changed.}
+
+Following is a summary of the constructions in the composite wall data set:
+
+\begin{lstlisting}
+
+CONSTRUCTION,Composite 2x4 Wood Stud R11,
+  ! ASHRAE 1145-RP Wall Assembly 1
+  ! 2"x4" wood studs at 24" on center with between-stud R11 fibreglass insulation.
+  ! Layers are 1/2" wood siding, 1/2" plywood, 2x4 wood studs and R11 insulation, 1/2" gypsum board.
+  ! Area-average R-Value = 11.391 ft2-F-h/Btu (2.005 m2-K/W).
+
+  CONSTRUCTION,Composite 2x6 Wood Stud R19,
+  ! ASHRAE 1145-RP Wall Assembly 2
+  ! 2"x6" wood studs at 24" on center with between-stud R19 fibreglass insulation.
+  ! Layers are 1/2" wood siding, 1/2" plywood, 2x6 wood studs and R19 insulation, 1/2" gypsum board.
+  ! Area-average R-Value = 17.487 ft2-F-h/Btu (3.078 m2-K/W).
+
+  CONSTRUCTION,Composite Insulated Concrete Form Wall With Steel Ties,
+  ! ASHRAE 1145-RP Wall Assembly 7
+  ! Wall system is made of two rigid insulation sides held together with wire mesh.
+  ! The two sides come together to create the formwork for the concrete.
+  ! Layers are 3/4" concrete stucco, outer polystyrene shell, concrete core, inner polystyrene shell.
+  ! Area-average R-Value = 11.230 ft2-F-h/Btu (1.977 m2-K/W).
+
+  CONSTRUCTION,Composite Concrete/Foam/Concrete With Steel Connectors,
+  ! ASHRAE 1145-RP Wall Assembly 8
+  ! Wall system is made of two 3" concrete slabs separated by 2" rigid insulation.
+  ! The slab connectors are steel ties with a 0.15"x0.15" cross section.
+  ! Layers are 3" concrete, 2" polystyrene, 3" concrete.
+  ! Area-average R-Value = 7.659 ft2-F-h/Btu (1.348 m2-K/W).
+
+  CONSTRUCTION,Composite Concrete/Foam/Concrete With Plastic Connectors,
+  ! ASHRAE 1145-RP Wall Assembly 9
+  ! Wall system is made of two 3" concrete slabs separated by 2" rigid insulation.
+  ! The slab connectors are plasic ties with a 0.25"x0.25" cross section.
+  ! Layers are 3" concrete, 2" polystyrene, 3" concrete.
+  ! Area-average R-Value = 10.582 ft2-F-h/Btu (1.862 m2-K/W).
+
+  CONSTRUCTION,Composite 2x4 Steel Stud R11,
+  ! ASHRAE 1145-RP Wall Assembly 10
+  ! 2"x4" steel studs at 24" on center with between-stud R11 fibreglass insulation.
+  ! Studs are 3.5", 16 gauge, 15 flange.
+  ! Layers are 1/2" wood siding, 1/2" plywood, 2x4 steel studs and R11 insulation, 1/2" gypsum board.
+  ! Area-average R-Value = 8.796 ft2-F-h/Btu (1.548 m2-K/W).
+
+  CONSTRUCTION,Composite Brick Foam 2x4 Steel Stud R11,
+  ! ASHRAE 1145-RP Wall Assembly 15
+  ! Brick veneer, polystyrene, 2"x4" steel studs at 24" on center with
+  !  between-stud R11 fibreglass insulation.
+  ! Studs are 3.5", 16 gauge, 15 flange.
+  ! Layers are 3.25" brick,1" polystyrene insulation, 1/2" plywood, 2x4 steel studs and R11 insulation,
+  !  1/2" gypsum board.
+  ! Area-average R-Value = 12.792 ft2-F-h/Btu (2.251 m2-K/W).
+
+  CONSTRUCTION,Composite 2x6 Steel Stud R19,
+  ! ASHRAE 1145-RP Wall Assembly 16
+  ! 2"x6" steel studs at 24" on center with between-stud R19 fibreglass insulation.
+  ! Studs are 5.5", 16 gauge, 15 flange.
+  ! Layers are 1/2" wood siding, 1/2" plywood, 2x6 steel studs and R19 insulation, 1/2" gypsum board.
+  ! Area-average R-Value = 12.792 ft2-F-h/Btu (1.991 m2-K/W).
+
+  CONSTRUCTION,Composite Foam 2x6 Steel Stud R19,
+  ! ASHRAE 1145-RP Wall Assembly 17
+  ! Polystyrene, 2"x6" steel studs at 24" on center with between-stud R19 fibreglass insulation.
+  ! Studs are 5.5", 16 gauge, 15 flange.
+  ! Layers are 3/4" concrete stucco,1" polystyrene insulation, 1/2" plywood, 2x6 steel studs and R19 insulation,
+  !  1/2" gypsum board.
+  ! Area-average R-Value = 15.157 ft2-F-h/Btu (2.668 m2-K/W).
+
+  CONSTRUCTION,Composite Brick Foam 2x6 Steel Stud R19,
+  ! ASHRAE 1145-RP Wall Assembly 18
+  ! Brick veneer, polystyrene, 2"x6" steel studs at 24" on center with
+  !  between-stud R19 fibreglass insulation.
+  ! Studs are 5.5", 16 gauge, 15 flange.
+  ! Layers are 3.25" brick,1" polystyrene insulation, 1/2" plywood, 2x6 steel studs and R19 insulation,
+  !  1/2" gypsum board.
+  ! Area-average R-Value = 15.465 ft2-F-h/Btu (2.722 m2-K/W).
+
+  CONSTRUCTION,Composite 2-Core Filled Concrete Block Uninsulated,
+  ! ASHRAE 1145-RP Wall Assembly 19
+  ! Wall system is made of 12" 2-core concrete blocks without insulation.
+  ! The core area is filled with rebar and poured concrete.
+  ! Area-average R-Value = 1.326 ft2-F-h/Btu (0.239 m2-K/W).
+
+  CONSTRUCTION,Composite 2-Core Filled Concrete Block Insulated,
+  ! ASHRAE 1145-RP Wall Assembly 20
+  ! Wall system is made of 12" 2-core concrete blocks with 1.875"-thick
+  !  foam inserts in the block cores.
+  ! The remaining core area is filled with poured concrete.
+  ! Area-average R-Value = 2.291 ft2-F-h/Btu (0.403 m2-K/W).
+\end{lstlisting}
+
+\subsection{DXCoolingCoil.idf}\label{dxcoolingcoil.idf}
+
+This dataset includes performance curves for the object types Coil:Cooling:DX:SingleSpeed and Coil:Cooling:DX:TwoStageWithHumidityControlMode. This data set is developed by using catalog data published by different manufacturers which are listed in the file.
+
+Here is a synopsis of the DXCoolingCoil.idf:
+
+\begin{lstlisting}
+
+! DXCoolingCoil.idf
+  !
+  ! This dataset includes performance curves for the object types Coil:Cooling:DX:SingleSpeed and
+  ! Coil:Cooling:DX:TwoStageWithHumidityControlMode
+  !
+  ! Reference capacity at standard rating conditions (ARI 95F OAT, 67F EWBT and air flow rate
+  ! around 400 cfm/Ton).
+  !
+  ! In the objects Coil:Cooling:DX:SingleSpeed and Coil:Cooling:DX:TwoStageWithHumidityControlMode
+  ! below, input fields 'Availability Schedule Name', 'Air Inlet Node Name' and 'Air Outlet Node
+  ! Name' need to be defined by the user.
+  !
+  !------------------------------------------------------------------------------------------------!                             Compressor  Nominal    Reference      Reference   Refrig  Expansion
+  !                                                                                         Valve
+  ! Name                           Type     Capacity   Capacity          COP       Type      Type
+  !                                         (tons)     kW (tons)
+  !------------------------------------------------------------------------------------------------! Carrier Centurion 50PG06      Scroll      5        18.28(5.2)        4.15     R-410A    TXV
+  ! Carrier Centurion 50PG12      Scroll      10       36.79(10.47)      4.05     R-410A    TXV
+  ! Carrier Centurion 50PG24      Scroll      20       73.81(21)         3.95     R-410A    TXV
+
+    Coil:Cooling:DX:SingleSpeed,
+      Carrier Centurion 50PG06,     !- Name
+      CoolingCoilAvailSched,        !- Availability Schedule Name
+      18276.96,                     !- Rated Total Cooling Capacity {W}
+      0.74,                         !- Rated Sensible Heat Ratio
+      4.15,                         !- Rated COP
+      0.944,                        !- Rated Air Flow Rate {m3/s}
+      ,                             !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
+      DXCoilAirInletNode,           !- Air Inlet Node Name
+      DXCoilAirOutletNode,          !- Air Outlet Node Name
+      CarrierCenturion50PG06CapFT,  !- Total Cooling Capacity Function of Temperature Curve Name
+      CarrierCenturion50PG06CapFFF, !- Total Cooling Capacity Function of Flow Fraction Curve Name
+      CarrierCenturion50PG06EIRFT,       !- Energy Input Ratio Function of Temperature Curve Name
+      CarrierCenturion50PG06EIRFFF,      !- Energy Input Ratio Function of Flow Fraction Curve Name
+      Carrier Centurion 50PG06 PLFFPLR;  !- Part Load Fraction Correlation Curve Name
+
+  ! Curve set (5 Curves):
+
+  ! Cooling Capacity Function of Temperature Curve
+  ! x = Entering Wet-bulb Temp and y = Outdoor Dry-bulb Temp
+
+    Curve:Biquadratic,
+      CarrierCenturion50PG06CapFT,  !- Name
+      0.9953455,               !- Coefficient1 Constant
+      -0.0118418,              !- Coefficient2 x
+      0.0012277,               !- Coefficient3 x**2
+      0.0030246,               !- Coefficient4 y
+      -0.0000702,              !- Coefficient5 y**2
+      -0.0003685,              !- Coefficient6 x*y
+      12.22,                   !- Minimum Value of x
+      26.67,                   !- Maximum Value of x
+      15.56,                   !- Minimum Value of y
+      51.67,                   !- Maximum Value of y
+      ,                        !- Minimum Curve Output
+      ,                        !- Maximum Curve Output
+      Temperature,             !- Input Unit Type for X
+      Temperature,             !- Input Unit Type for Y
+      Dimensionless;           !- Output Unit Type
+
+  ! EIR Function of Temperature Curve
+  ! x = Entering Wet-bulb Temp and y = Outdoor Dry-bulb Temp
+
+    Curve:Biquadratic,
+      CarrierCenturion50PG06EIRFT,  !- Name
+      0.3802131,               !- Coefficient1 Constant
+      0.0199468,               !- Coefficient2 x
+      -0.0006682,              !- Coefficient3 x**2
+      0.0058933,               !- Coefficient4 y
+      0.0004646,               !- Coefficient5 y**2
+      -0.0004072,              !- Coefficient6 x*y
+      12.22,                   !- Minimum Value of x
+      26.67,                   !- Maximum Value of x
+      15.56,                   !- Minimum Value of y
+      51.67,                   !- Maximum Value of y
+      ,                        !- Minimum Curve Output
+      ,                        !- Maximum Curve Output
+      Temperature,             !- Input Unit Type for X
+      Temperature,             !- Input Unit Type for Y
+      Dimensionless;           !- Output Unit Type
+
+  ! Cooling Capacity Function of Flow Fraction Curve
+  ! x = Flow Fraction
+
+    Curve:Quadratic,
+      CarrierCenturion50PG06CapFFF,  !- Name
+      0.7705358,               !- Coefficient1 Constant
+      0.2848007,               !- Coefficient2 x
+      -0.0580891,              !- Coefficient3 x**2
+      0.75,                    !- Minimum Value of x
+      1.25;                    !- Maximum Value of x
+
+  ! EIR Function of Flow Fraction Curve
+  ! x = Flow Fraction
+
+    Curve:Quadratic,
+      CarrierCenturion50PG06EIRFFF,   !- Name
+      1.3439758,               !- Coefficient1 Constant
+      -0.5111244,              !- Coefficient2 x
+      0.1732549,               !- Coefficient3 x**2
+      0.75,                    !- Minimum Value of x
+      1.25;                    !- Maximum Value of x
+
+  ! Part Load Fraction Function of Part Load Ratio Curve
+  ! x = Part Load Ratio
+
+    Curve:Quadratic,
+      CarrierCenturion50PG06PLFFPLR,   !- Name
+      0.85,                    !- Coefficient1 Constant
+      0.15,                    !- Coefficient2 x
+      0.0,                     !- Coefficient3 x**2
+      0.0,                     !- Minimum Value of x
+      1.0;                     !- Maximum Value of x
+\end{lstlisting}
+
+\subsection{ElectricGenerators.idf}\label{electricgenerators.idf}
+
+This dataset includes inputs for the GENERATOR:MICROTURBINE object and associated performance curves. The performance curves were developed from manufacturer data collected in Summer 2007.
+
+Includes data for generators: Capstone C65, Elliott TA100,~ Ingersoll Rand MT70, Ingersoll Rand MT250.
+
+Further documentation is contained in the dataset file.
+
+\subsection{Electricity USA Environmental Impact Factors.idf}\label{electricity-usa-environmental-impact-factors.idf}
+
+United States 1999 national average electricity emissions factors based on eGRID, 1605, AirData. United States Water Emission Fuel Factors are the combined thermoelectric and hydroelectric weighted averages from:
+
+Torcellini, Paul; Long, Nicholas; Judkoff, Ron; ``Consumptive Water Use for U.S. Power Production'';NREL Report No. TP-550-33905. Golden, CO; 2003; http://www.nrel.gov/docs/fy04osti/33905.pdf;
+
+or
+
+Torcellini, Paul; Long, Nicholas; Judkoff, Ron; ``Consumptive Water Use for U.S. Power Production''; ASHRAE Transactions 2003, Vol 110, Part 1. Atlanta, GA; January 2004;
+
+\subsection{ElectronicEnthalpyEconomizerCurves.idf}\label{electronicenthalpyeconomizercurves.idf}
+
+These curves approximate the electronic (variable) enthalpy curves used to simulate humidity biased economizer control. This control scheme adjusts the upper outdoor air humidity ratio based on outdoor air dry-bulb temperature as shown in the figure below. California Title 24 ACM 2005 lists the optional economizer control strategies. One of these control strategies is referred to as variable enthalpy control curve A. This control strategy is also cited in ASHRAE Standard 90.1-2004, using the term ``electronic enthalpy''. Electronic enthalpy curves A-D are included in this dataset.
+
+\begin{figure}[hbtp] % fig 12
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image027.jpg}
+\caption{Psychrometric Chart Illustration of the Electronic (Variable) Enthalpy Economizer Limit Example Curve Objects \protect \label{fig:psychrometric-chart-illustration-of}}
+\end{figure}
+
+For the curves provided, curve A has the highest limit and curve D has the lowest limit. These curve objects represent a single-point electronic enthalpy control curve with the curve object's minimum value of x (temperature) crossing the psychrometric chart's saturation line and the curve object's maximum value of x crossing the psychrometric chart's dry-bulb temperature axis. The curve object's minimum (maximum) value of x should be just low (high) enough to ensure that the curve crosses the psychrometric chart's saturation line (temperature axis). The curves are evaluated at an outdoor dry-bulb temperature to provide a maximum operating outdoor humidity ratio for economizer operation. If the outdoor humidity ratio is greater than this maximum value, economizer operation is terminated. These curves may be used with other economizer limits to create multi-point economizer control (Temperature Limit, Temperature Low Limit, Enthalpy Limit, and Dewpoint Temperature Limit).
+
+\subsubsection{Form of the Electronic Enthalpy Curve Equation:}\label{form-of-the-electronic-enthalpy-curve-equation}
+
+The electronic enthalpy curve equation represents a unique curve and is a function of both temperature and relative humidity. The equation is set equal to a constant which provides a unique temperature for each relative humidity entered into the equation. Each control curve has a unique constant as shown in the table below. Other constants may be used to develop specialized electronic enthalpy curves.
+
+\begin{equation}
+K = 45.672192 - 1.1559942 \cdot T - 0.144599 \cdot RH
+\end{equation}
+
+where:
+
+\begin{itemize}
+\tightlist
+\item
+  K~ = Constant value to represent specific curve
+\item
+  T~ = Outdoor Dry-Bulb Temperature (C)
+\item
+  RH = Outdoor Relative Humidity (\%)
+\end{itemize}
+
+NOTE:~ modifying the RH multiplier (-0.144599) tends to ``wag'' the curvature at the upper relative humidities. Decreasing the multiplier ``wags'' the upper portion of the curve downward, increasing ``wags'' it upwards. Modifying the constant (K) moves the intersection of the curve with the Dry-Bulb Temperature ~axis. Increasing the constant moves the intersection to the left as shown in the figure, decreasing moves to the right. The minimum and/or maximum x boundaries in the curve objects may have to be adjusted when modifying the equation.
+
+% table 43
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{3.0in}}
+\caption{Electronic Enthalpy Curve Constants and approximate control point at 50\% RH \label{table:electronic-enthalpy-curve-constants}} \tabularnewline
+\toprule 
+Control Curve & Curve Constant K & Approximate Control Point at 50\% RH (ºC) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Electronic Enthalpy Curve Constants and approximate control point at 50\% RH} \tabularnewline
+\toprule 
+Control Curve & Curve Constant K & Approximate Control Point at 50\% RH (ºC) \tabularnewline
+\midrule
+\endhead
+
+A & 12 & 22.9 \tabularnewline
+B & 14 & 21.1 \tabularnewline
+C & 16 & 19.4 \tabularnewline
+D & 18 & 17.7 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Example Curve A:}\label{example-curve-a}
+
+The method described here was used to create each of the four ``cubic'' curve objects provided in the electronic enthalpy economizer control data set.
+
+\textbf{Step 1:} Substitute the curve constant K for curve A (12) into the electronic enthalpy curve equation and solve for temperature. Then identify the outdoor air dry-bulb temperatures at known values of relative humidity (e.g., columns 1 and 2 in the table below). Psychrometric routines are helpful for this step.
+
+\begin{equation}
+\text{Temperature} = \frac{12 - 45.672192 + 0.144599 \cdot \text{RelativeHumidity}}{-1.1559942}
+\end{equation}
+
+\textbf{Step 2:} Identify humidity ratio at each point (e.g.~column 3 in the following table). Psychrometric routines are helpful for this step.
+
+\begin{longtable}[c]{@{}l@{}}
+\toprule 
+Glycols \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Glycols \tabularnewline
+\midrule
+\endhead
+
+EthyleneGlycol \tabularnewline
+PropyleneGlycol \tabularnewline
+Water \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{~}
+
+\textbf{Step 3:} Use multiple linear regression to solve one of the following equations:
+
+\emph{Quadratic~ Curve}: Humidity Ratio = A0 + A1*Temperature + A2*Temperature\(^{2}\)
+
+\emph{Cubic~ Curve}: Humidity Ratio = A0 + A1*Temperature + A2*Temperature\(^{2}\) + A3*Temperature\(^{3}\)
+
+\textbf{Step 4:} Use the coefficients calculated in the multiple linear regression to create a cubic (or quadratic) curve object.
+
+\subsection{Exhaust Fired Chiller.idf}\label{exhaust-fired-chiller.idf}
+
+This dataset includes the curves for exhaust fired absorption chiller.
+
+1)~~~Cooling Capacity Function of Temperature Curve
+
+2)~~~Thermal Energy Input to Cooling Output Ratio Function of Temperature Curve
+
+3)~~~Thermal Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve
+
+\subsection{Fossil Fuel Environmental Impact Factors.idf}\label{fossil-fuel-environmental-impact-factors.idf}
+
+Impact factors for environmental reporting. References for each fuel are given in the dataset.
+
+\subsection{FluidPropertiesRefData.idf}\label{fluidpropertiesrefdata.idf}
+
+This data set includes fluid properties reference data. Fluid properties for R404a, R407a, R410a, R505a, R744, were developed using the NIST Standard Reference Database 23, NIST Reference Thermodynamic and Transport Properties -- REFPROP, April 2007 Version 8.0, National Institute of Standards and Technology, 2007. The other refrigerants were developed using older versions of the NIST Standard Reference Database. The entire data set includes:
+
+\begin{longtable}[c]{@{}l@{}}
+\toprule 
+Glycols \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Glycols \tabularnewline
+\midrule
+\endhead
+
+EthyleneGlycol \tabularnewline
+PropyleneGlycol \tabularnewline
+Water \tabularnewline
+\bottomrule
+\end{longtable}
+
+To use the data, copy the appropriate data for the refrigerant you desire into your input file.
+
+\subsection{GlycolPropertiesRefData.idf}\label{glycolpropertiesrefdata.idf}
+
+This data set includes fluid properties (glycol) reference data. Reference for the data is the ASHRAE Handbook of Fundamentals. Included are:
+
+\begin{longtable}[c]{@{}l@{}}
+\toprule 
+Glycols \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Glycols \tabularnewline
+\midrule
+\endhead
+
+EthyleneGlycol \tabularnewline
+PropyleneGlycol \tabularnewline
+Water \tabularnewline
+\bottomrule
+\end{longtable}
+
+To use the data, copy the appropriate data for the glycol you desire into your input file.
+
+\subsection{GHLERefData.idf}\label{ghlerefdata.idf}
+
+This file contains sample input for the ground loop heat exchanger model. The response of the borehole/ground is found from the `G-function' that is~ defined in the input as series of `n' pairs of values (LNTTSn, GNFCn). It is important to note that the G-functions have to be calculated for specific GHE configurations and borehole resitance, length and borehole/ length ratio. That is, the parameters for the units vary with each design. The data in this file are intended as examples/samples and may not represent actual designs.
+
+The sample data has been calculated for a number of configurations:
+
+\begin{itemize}
+\tightlist
+\item
+  1 x 2 boreholes
+\item
+  4 x 4 boreholes
+\item
+  8 x 8 boreholes
+\end{itemize}
+
+Data is given for both `standard' grout (k = 0.744 W/m.K) and `thermally enhanced' grout (k = 1.471 W/m.K). The flow rate per borehole is .1514 kg/s. The pipe given is 0.75in. Dia. SDR11 HDPE. The fluid is water. The borehole/length ratio is 0.06~ (76.2m/4.572m {[}300ft/15ft{]})
+
+\subsection{MoistureMaterials.idf}\label{moisturematerials.idf}
+
+This data set includes the special moisture materials that can be used with the Moisture Penetration Depth Conduction Transfer Function (EMPD) and Combined Heat and Moisture Finite Element (HAMT) calculation procedures.
+
+\subsection{PerfCurves.idf}\label{perfcurves.idf}
+
+This file contains performance curves for various EnergyPlus equipment objects.
+
+\begin{itemize}
+\item
+  Variable speed DX cooling:~ These curves are appropriate for small DX cooling units with variable speed compressors. These curves would be referenced by the EnergyPlus object Coil:Cooling:DX:TwoSpeed. See the example input file 5ZoneAutoDXVAV for an example of their use.
+\item
+  Variable Speed Cooling Tower: These model coefficient objects are appropriate for use with the variable speed cooling tower object and represent the coefficients used in the YorkCalc and CoolTools empirical models. These model coefficient objects would be referenced by the EnergyPlus object Cooling Tower:Variable Speed. See the example input file CoolingTower\_VariableSpeed.idf for an example of where these curves could be used (these model coefficient objects are not specifically used in this idf but could be used by the Cooling Tower:Variable Speed object). Additional information on variable speed cooling tower model coefficients can be found in the Input Output Reference and Engineering Reference documents.
+\item
+  Note that performance curves for the Electric EIR chiller and the Electric Reformulated EIR chiller are contained in the Chillers.idf dataset.
+\end{itemize}
+
+\subsection{PrecipitationSchedulesUSA.idf}\label{precipitationschedulesusa.idf}
+
+This file contains schedules (for an entire year) of precipitation for use with the SitePrecipitation object. Use these schedules for adding rain water to the simulation. The values are in meters per hour and are scaled to match the average monthly precipitation. They also coincide with the EPW rain/snow flags from the original source files.
+
+\subsection{RefrigerationCasesDataSet.idf}\label{refrigerationcasesdataset.idf}
+
+All the refrigerated cases included in this database are listed in the following list. Comments before each refrigeration:case object include the manufacturer's model number and assumptions about the fan, lights, defrost etc. The user must ensure that the case names used in the idf file are UNIQUE and must supply the correct zone name.~ The user must also supply any required correction curves or schedules. The defrost and drip-down schedule names included here indicate the frequency and duration required. The user must ensure that schedules are provided that meet these needs and that are diversified so that all the cases don't start their defrost cycles at the same time. Please see the example cases for supermarkets to see how these case objects are included with the rest of a supermarket refrigeration system.
+
+\begin{itemize}
+\item
+  Multi-Deck Dairy/Deli Merchandiser with Synergy-E
+\item
+  Multi-Deck Rear Dairy/Deli Merchandiser with Synergy-E
+\item
+  Multi-Deck Deli back
+\item
+  Single Deck Club Case Merchandiser
+\item
+  Single Deck Club Case Merchandiser
+\item
+  Single Deck Club Merchandiser
+\item
+  Single Deck Club Case Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
+\item
+  Multi-Deck Dairy/Deli Merchandiser with Synergy-E
+\item
+  Multi Deck Frozen Food Merchandiser
+\item
+  Multi Deck Frozen Food Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  International Style Service Deli/Meat/Seafood Merchandiser
+\item
+  International Style Flat Glass Service Deli/Meat/Seafood Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
+\item
+  Multi-Deck Deli/Meat End Cap Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
+\item
+  Multi-Deck Dairy/Deli/Produce/Meat Merchandiser with Synergy-E
+\item
+  Multi-Deck Dairy/Deli/Produce/Meat Merchandiser with Synergy-E
+\item
+  Multi-Deck Produce/Dairy/Deli/Meat Merchandiser
+\item
+  Multi-Deck Deli/Meat End Cap Merchandiser
+\item
+  Multi-Deck Bulk Produce End Cap Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Produce Merchandiser
+\item
+  Wide Island Multi-Deck Produce Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Multi-Deck Dairy/Deli/Produce Merchandiser
+\item
+  Multi-Deck Dairy/Deli/Produce Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Wide Island Multi-Deck Deli/Meat Merchandiser
+\item
+  Multi-Deck Dairy/Deli/Produce Merchandiser
+\item
+  Multi-Deck Dairy/Deli/Produce Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Multi-Deck Merchandiser with Synergy-E
+\item
+  Multi-Deck Merchandiser with Synergy-E
+\item
+  Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  High Multi-Deck Merchandiser with Synergy-E
+\item
+  High Multi-Deck Merchandiser with Synergy-E
+\item
+  High Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  High Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  High Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Multi-Deck Read Load Merchandiser with Synergy-E
+\item
+  Multi-Deck Rear Load Dairy Merchandiser
+\item
+  Multi-Deck Rear Load Dairy Merchandiser
+\item
+  High Multi-Deck Rear Load Dairy Merchandiser
+\item
+  High Multi-Deck Rear Load Dairy Merchandiser
+\item
+  Multi Deck Merchandiser with Synergy-E
+\item
+  Multi-Deck Deli/Meat Merchandiser
+\item
+  High Multi-Deck~ Merchandiser with Synergy-E
+\item
+  Multi-Deck Rear Load Deli/Meat Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Multi-Deck Frozen Food Merchandiser
+\item
+  Multi-Deck Frozen Food Merchandiser
+\item
+  Multi-Deck Dairy/Deli/Produce Merchandiser with Synergy E
+\item
+  Multi-Deck Dairy/Deli/Produce Merchandiser with Synergy E
+\item
+  Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Full Service Bakery Merchandiser
+\item
+  Full Service Flat Glass Bakery Merchandiser
+\item
+  Self Service Bakery/Deli Merchandiser
+\item
+  Self Service Bakery/Deli Merchandiser
+\item
+  Self Service Bakery/Deli Merchandiser
+\item
+  Self Service Deli/Cheese Merchandiser
+\item
+  Self Service Deli/Cheese Merchandiser
+\item
+  Single Deck Deli/Meat End Cap Merchandiser
+\item
+  Single Deck Buck Produce End Cap Merchandiser
+\item
+  American Style Vertical Glass Service Deli/Meat/Seafood Gravity Coil Merchandiser
+\item
+  Multi-Deck Deli/Meat Merchandiser
+\item
+  Multi-Deck Deli/Meat Merchandiser
+\item
+  Multi-Deck Merchandiser with Synergy-E
+\item
+  Multi-Deck Merchandiser with Synergy-E
+\item
+  High Multi-Deck Deli/Meat Merchandiser
+\item
+  High Multi-Deck Deli/Meat Merchandiser
+\item
+  Multi-Deck Produce Merchandiser
+\item
+  Multi-Deck Produce Merchandiser
+\item
+  High Multi-Deck Merchandiser with Synergy-E
+\item
+  High Multi-Deck Merchandiser with Synergy-E
+\item
+  High Multi-Deck Merchandiser with Synergy-E
+\item
+  High Multi-Deck Merchandiser with Synergy-E
+\item
+  Wide Island Deli/Meat Merchandiser
+\item
+  Wide Island Deli/Meat Merchandiser
+\item
+  Wide Island Deli/Meat Merchandiser
+\item
+  Wide Island Deli/Meat Merchandiser
+\item
+  Wide Island Deli/Meat Merchandiser
+\item
+  Wide Island Deli/Meat Merchandiser
+\item
+  Wide Island Bulk Produce Merchandiser
+\item
+  Wide Island Bulk Produce Merchandiser
+\item
+  Wide Island Bulk Produce Merchandiser
+\item
+  Island Frozen Food Merchandiser
+\item
+  Island Frozen Food Merchandiser
+\item
+  Flat Glass Service Deli Merchandiser
+\item
+  Flat Glass Service Deli Gravity Coil Merchandiser
+\item
+  Single-Deck Deli/Meat/Seafood Merchandiser with Synergy -E
+\item
+  Single-Deck Deli/Meat/Seafood Merchandiser
+\item
+  Single-Deck Deli/Meat/Seafood Merchandiser
+\item
+  Single Deck Frozen Meat Merchandiser
+\item
+  Single Deck Frozen Food/Ice Cream Merchandiser
+\item
+  Single Deck Frozen Food/Ice Cream Merchandiser
+\item
+  Narrow Mulit Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
+\item
+  Narrow Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
+\item
+  Narrow Multi Deck Deli Meat End Cap Merchandiser
+\item
+  Narrow Multi Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
+\item
+  Narrow Multi-Deck Deli/Meat End Cap Merchandiser
+\item
+  Narrow Multi Deck Bulk Produce End Cap Merchandiser
+\item
+  Narrow Island Multi Deck Deli/Meat Merchandiser
+\item
+  Narrow Island Multi Deck Deli/Meat Merchandiser
+\item
+  Narrow Multi Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
+\item
+  Multi-Deck Self Service Hot Foods Merchandiser
+\item
+  Narrow Multi Deck Produce/Dairy/Deli Merchandiser
+\item
+  Narrow Multi Deck Produce/Dairy/Deli Merchandiser
+\item
+  Narrow Multi Deck Produce/Dairy/Deli Merchandiser
+\item
+  High Narrow Multi-Deck Merchandiser with Synergy-E
+\item
+  High Narrow Multi-Deck Merchandiser with Synergy-E
+\item
+  High Narrow Multi-Deck Produce/Dairy Merchandiser
+\item
+  High Narrow Multi-Deck Produce/Dairy Merchandiser
+\item
+  Narrow Multi-Deck Deli End Cap Merchandiser
+\item
+  Narrow Multi-Deck Produce Merchandiser
+\item
+  Narrow Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Narrow Single Deck Frozen Meat End Cap Merchandiser
+\item
+  Narrow Multi-Deck Deli/Meat Merchandiser
+\item
+  Narrow Multi-Deck Deli/Meat Merchandiser
+\item
+  High Narrow Multi-Deck Deli/Meat Merchandiser
+\item
+  High Narrow Multi-Deck Deli/Meat Merchandiser
+\item
+  Narrow Multi-Deck Produce Merchandiser
+\item
+  Narrow Multi-Deck Produce Merchandiser
+\item
+  High Narrow Multi-Deck Produce Merchandiser
+\item
+  High Narrow Multi-Deck Produce Merchandiser
+\item
+  Narrow Island Deli/Meat Merchandiser double Wraparound end
+\item
+  Narrow Island Deli/Meat Merchandiser double Wraparound end
+\item
+  Narrow Island Bulk Produce Merchandiser
+\item
+  Narrow Island Bulk Produce Merchandiser
+\item
+  Narrow Island Bulk Produce Merchandiser
+\item
+  Narrow Island Frozen Food/Ice Cream Merchandiser
+\item
+  Narrow Island Frozen Food/Ice Cream Merchandiser
+\item
+  Narrow Island Frozen Food/Ice Cream Merchandiser
+\item
+  Narrow Island Frozen Food Merchandiser
+\item
+  Narrow Single Deck Frozen Meat Merchandiser
+\item
+  Multi Deck Dairy Merchandiser
+\item
+  Narrow Multi Deck Deli Merchandiser
+\item
+  Multi Deck Utility Merchandiser
+\item
+  Narrow Single Deck Produce Merchandiser
+\item
+  Narrow Glass Door Reach In Beverage Merchandiser
+\item
+  Narrow Glass Door Reach In Beverage Merchandiser
+\item
+  High Narrow Glass Door Reach-in Beverage Merchandiser
+\item
+  High Narrow Glass Door Reach-in Beverage Merchandiser
+\item
+  Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser: Frozen food
+\item
+  Narrow Glass Door Reach in~ Back-toBack Frozen Food/Ice Cream Merchandiser: Ice Cream
+\item
+  High Narrow Glass Door Reach-in Back-to-Back Frozen Food/Ice Cream: Frozen food
+\item
+  High Narrow Glass Door Reach-in Back-to-Back Frozen Food/Ice Cream: Ice cream
+\item
+  Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser: Frozen food
+\item
+  Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser: Ice Cream
+\item
+  High Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser
+\item
+  High Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser
+\item
+  High Narrow Glass Door Reach in Back to back Frozen Food/Ice Cream Merchandiser
+\item
+  Narrow Multi-Deck Produce/Dairy/Deli/Meat Merchandiser
+\item
+  Narrow Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
+\item
+  Narrow Multi-Deck Dome Deli Merchandiser
+\item
+  Narrow Single-Deck Frozen Food/Ice Cream Merchandiser
+\item
+  Narrow Single-Deck Frozen Food/Ice Cream Merchandiser
+\item
+  Narrow Single-Deck Frozen Food/Ice Cream Merchandiser
+\item
+  Single Deck Produce Merchandiser
+\item
+  Single Deck Produce Merchandiser
+\item
+  Single Deck Produce Merchandiser
+\item
+  Single Deck Produce Merchandiser
+\item
+  Glass Door Reach-in Beverage Merchandiser
+\item
+  Glass Door Reach-in Beverage Merchandiser
+\item
+  High Glass Door Reach-in Beverage Merchandiser
+\item
+  High Glass Door Reach-in Beverage Merchandiser
+\item
+  Glass Door Reach-in Rear Load Beverage Merchandiser
+\item
+  Roll in Rear Load Merchandiser with Synergy-E
+\item
+  Roll in Rear Load Dairy Merchandiser
+\item
+  Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
+\item
+  Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
+\item
+  Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
+\item
+  Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
+\item
+  Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
+\item
+  Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
+\item
+  High Glass Door Reach-in Frozen Food/Ice Cream Merchandiser
+\item
+  High Glass Door Reach-in Frozen Food/Ice Cream Merchandiser
+\item
+  American Style Curved Glass Service Deli Merchandiser
+\item
+  American Style Curved Glass Service Deli/Meat/Seafood Gravity Merchandiser
+\item
+  American Style Curved Glass Service Deli/Meat/Seafood Gravity Merchandiser
+\item
+  American Style Glass Service Deli Merchandiser
+\item
+  American Style Glass Service Deli Merchandiser
+\item
+  American Style Flat Glass Service Deli/Meat/Seafood Gravity Coil Merchandiser
+\item
+  International Style Service Deli/Seafood Merchandiser
+\item
+  International Style Flat Glass Service Deli/Meat/Seafood Merchandiser
+\item
+  International Style Single Deck Deli Seafood Merchandiser
+\item
+  American Style Vertical Glass Service Deli Merchandiser
+\item
+  American Style Flat Glass Service Frozen Food Merchandiser
+\item
+  Multi-Deck Produce/Dairy/Meat/Seafood Merchandiser
+\item
+  Wide Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Wide Multi-Deck Produce/Dairy/Deli Merchandiser
+\item
+  Wide Island End Cap Frozen Food/Ice Cream Merchandiser
+\item
+  Wide Island End Cap Frozen Food/Ice Cream Merchandiser
+\item
+  Wide Island End Cap Frozen Food/Ice Cream Merchandiser
+\item
+  Wide High Multi-Deck Produce Merchandiser
+\item
+  Wide High Multi-Deck Produce Merchandiser
+\item
+  Wide Island Frozen Food/Ice Cream Merchandiser
+\item
+  Wide Island Frozen Food/Ice Cream Merchandiser
+\item
+  Wide Island Frozen Food/Ice Cream Merchandiser
+\item
+  Wide Single Deck Produce Merchandiser
+\item
+  Wide Single Deck Produce Merchandiser
+\item
+  Wide Single Deck Produce Merchandiser
+\item
+  Wide Single Deck Produce Merchandiser
+\item
+  Wide International Style Service Deli/Seafood Merchandiser
+\item
+  Wide International Style Single Deck Deli/Seafood Merchandiser
+\item
+  Single Deck Frozen Food Merchandiser
+\item
+  Single Deck Frozen Food Merchandiser
+\item
+  Wide Single Deck Frozen Food Merchandiser
+\item
+  Full Service Flat Glass Deli Merchandiser
+\item
+  Multi-Deck Curved Glass Dome Deli/Meat/Seafood Merchandiser
+\item
+  Multi-Deck Curved Glass Dome Deli/Meat/Seafood Merchandiser
+\item
+  Glass Door Reach-in Beverage Merchandiser
+\item
+  Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser: Frozen food
+\item
+  Narrow Glass Door Reach in~ Back-toBack Frozen Food/Ice Cream Merchandiser: Ice Cream
+\item
+  High Glass Door Reach-in Frozen Food/Ice Cream Merchandiser
+\item
+  High Glass Door Reach-in Frozen Food/Ice Cream Merchandiser
+\item
+  Single Deck Wood Clad Merchandiser for Medium Temp Application
+\item
+  Single Deck Wood Clad Merchandiser for Medium Temp Application
+\item
+  55'' Tall Convertible With Extended Canopy. Medium Temperature Merchandiser
+\item
+  C2LGE MultiDeck 3 display levels
+\item
+  Convertible Island End. Low Profile Multi-Deck
+\item
+  Unitized Convertible Island. Low Profile Multi-Deck
+\item
+  Convertible Island. Low Profile Multi-Deck
+\item
+  Unitized Convertible Island. Low Profile Multi-Deck
+\item
+  Unitized Convertible Island. Low Profile Multi-Deck
+\item
+  Unitized Convertible Island. Low Profile Multi-Deck
+\item
+  Unitized Convertible Island. Low Profile Multi-Deck
+\item
+  Convertible Island. Low Profile Multi-Deck
+\item
+  Self-Serve Three-Level Display With Extended Canopy
+\item
+  Self-Serve Four-Level Display With Extended Canopy
+\item
+  Self-Serve Four-Level Display With Extended Canopy
+\item
+  ED1 Impact Service Merchandiser with curved hinged glass 1 display level
+\item
+  ED1 Impact Service Merchandiser with curved hinged glass 1 display level
+\item
+  EDS1 Impact self service glass 1 display level
+\item
+  E1 Self Service Single Deck Display for Deli Cheese and Salads
+\item
+  E1S Self Service Single Deck Display for Deli Cheese and Salads
+\item
+  E2 Self-Serve Multi-Deck Display For Deli Cheese Pizza Floral Fresh Juice
+\item
+  E2 Self-Serve Multi-Deck Display For Deli Cheese Pizza Floral Fresh Juice
+\item
+  E2S Self-Serve Three Level Display For Deli Cheese Pizza
+\item
+  E2S Self-Serve Three Level Display For Deli Cheese Pizza
+\item
+  E2S Self-Serve Three Level Display For Deli Cheese Pizza
+\item
+  E2S Self-Serve Three Level Display For Deli Cheese Pizza
+\item
+  E3 Self-Serve Multi-Deck Display For Deli Cheese Pizza Floral Fresh Juice
+\item
+  Self Serve Multi-Deck Display Merchandiser
+\item
+  Self Serve Multi-Deck Display Merchandiser
+\item
+  ES1 Single-Deck Curved Glass Service Case with 1 display level
+\item
+  ES1S Single-Deck Straight glass Service Case with one display level
+\item
+  ESBD Curved glass case for deli with blower coil and one display level with optional shelves
+\item
+  ESBDHV High Volume Curved Glass Blower Coil Service Case for Deli with 3 display levels
+\item
+  ESBDS Straight glass service case for deli with blower coil and one display level with optional 2 shelves
+\item
+  ESGM Curved Glass Gravity Coil Service Case for Meat and Seafood
+\item
+  ESGMS Straight Glass Gravity Coil Service Case for Meat and Seafood
+\item
+  ESGMVS Vertical hinged glass service case for Deli with Gravity Coil\_single display level
+\item
+  ESGS Curved Glass Gravity Coil Service Case for Meat and Seafood
+\item
+  ESGSS Straight Glass Gravity Coil Service Case for Meat and Seafood
+\item
+  ESBDVS Straight hinged glass service case for Deli with Blower Coil\_1 display level with optional shelves
+\item
+  B1X BulkSinlge Decked Extended Depth Glass Front
+\item
+  B3XC Bulk Multi-Deck Convertible Merchandiser
+\item
+  B3XC Bulk Multi-Deck Convertible Merchandiser
+\item
+  B4-XE Four-Deck High Volume Bulk Convertible Merchandiser
+\item
+  C2X Low-Profile Multi-Deck Convertible Merchandiser
+\item
+  C2X Low-Profile Multi-Deck Convertible Merchandiser
+\item
+  C2X Low-Profile Multi-Deck Convertible Merchandiser
+\item
+  C2X Low-Profile Multi-Deck Convertible Merchandiser
+\item
+  C2X Low-Profile Multi-Deck Convertible Merchandiser
+\item
+  C2X Low-Profile Multi-Deck Convertible Merchandiser
+\item
+  C2X Low-Profile Multi-Deck Convertible Merchandiser
+\item
+  C2X Low-Profile Multi-Deck Convertible Merchandiser
+\item
+  C2X Low-Profile Multi-Deck Convertible Merchandiser
+\item
+  C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
+\item
+  C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
+\item
+  C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
+\item
+  C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
+\item
+  C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
+\item
+  C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
+\item
+  C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
+\item
+  C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
+\item
+  C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
+\item
+  C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
+\item
+  C3X Multi-Deck Convertible Merchandiser with four display levels
+\item
+  C3X Multi-Deck Convertible Merchandiser with four display levels
+\item
+  C4X Multi-Deck Convertible Merchandiser
+\item
+  C4X Multi-Deck Convertible Merchandiser
+\item
+  C4X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C5X Multi-Deck Convertible Merchandiser
+\item
+  C6X High Capacity Multi-Deck Convertible Merchandiser
+\item
+  C6X High Capacity Multi-Deck Convertible Merchandiser
+\item
+  C6X High Capacity Multi-Deck Convertible Merchandiser
+\item
+  C6X High Capacity Multi-Deck Convertible Merchandiser
+\item
+  C6X High Capacity Multi-Deck Convertible Merchandiser
+\item
+  C6X High Capacity Multi-Deck Convertible Merchandiser
+\item
+  C6X High Capacity Multi-Deck Convertible Merchandiser
+\item
+  C6X High Capacity Multi-Deck Convertible Merchandiser
+\item
+  C6XLRE High Capacity Multi-Deck Convertible Merchandiser with Rear Load-In for Dairy and Deli
+\item
+  D5X-ULEP Ultra Low Front Multi-Deck Dairy/Deli Merchandiser
+\item
+  D5X-E Multi-Deck Dairy/Deli Merchandiser
+\item
+  D5X-EP Multi-Deck Dairy/Deli Merchandiser
+\item
+  D5X-EP Multi-Deck Dairy/Deli Merchandiser
+\item
+  D5X-HE Multi-Deck Dairy/Deli Merchandiser
+\item
+  D5X Multi-Deck Dairy/Deli Merchandiser
+\item
+  D5X-LE Multi-Deck Dairy/Deli Merchandiser
+\item
+  D5X-LEP Multi-Deck Dairy/Deli Merchandiser
+\item
+  D5X-LEP Multi-Deck Dairy/Deli Merchandiser
+\item
+  D5XLRE Multi-Deck Dairy/Deli Merchandiser With Rear Sliding Doors and low front
+\item
+  D5XRRI Rear Roll-IN Dairy Merchandiser
+\item
+  D5XRRIS Rear Roll-IN Dairy Merchandiser
+\item
+  D6NX Narrow Footprint Extra Tall Multi-Deck Dairy/Deli Merchandiser
+\item
+  D6NX Narrow Footprint Extra Tall Multi-Deck Dairy/Deli Merchandiser
+\item
+  D6NX Narrow Footprint Extra Tall Multi-Deck Dairy/Deli Merchandiser
+\item
+  D6NX Narrow Footprint Extra Tall Multi-Deck Dairy/Deli Merchandiser
+\item
+  D6X-ULEP Ultra Low Front Dairy Merchandiser
+\item
+  F Single Deck Wall Model Merchandiser~ with solid front for Frozen Food
+\item
+  F Single Deck Wall Model Merchandiser~ with solid front for Ice Cream
+\item
+  F Single Deck Wall Model Merchandiser~ with solid front for Medium Temp Products
+\item
+  FI Intermediate Island Merchandiser with solid walls for Frozen Food
+\item
+  F2XLG Low Temperature Multi-Deck Merchandiser for Frozen Seafood and Meat
+\item
+  F6 Low Temperature Multi-Deck Open Merchandiser
+\item
+  F6L Low Temperature Multi-Deck Open Merchandiser
+\item
+  FG Single Deck Wall Model Merchandiser with glass front for Frozen Food
+\item
+  FG Single Deck Wall Model Merchandiser r with glass front for Ice Cream
+\item
+  FG Single Deck Wall Model Merchandiser r with glass front for Medium Temp Products
+\item
+  FIG Intermediate Island Merchandiser with glass walls for Frozen Food
+\item
+  FL5NX Excel Multi-Deck Narrow Footprint Floral Merchandiser
+\item
+  FN Narrow Island display with solid walls for Frozen Food
+\item
+  FN Narrow Island display with solid walls for Ice Cream
+\item
+  FN Narrow Island display with solid walls for medium temperature
+\item
+  FNG Narrow Glass Sided Island Merchandiser for Frozen
+\item
+  FNG Narrow Glass Sided Island Merchandiser for Ice Cream
+\item
+  FNG Narrow Glass Sided Island Merchandiser for Medium Temperature
+\item
+  FW Wide Island Display with Solid Walls for Frozen Food
+\item
+  FW Wide Island Display with Solid Walls for Ice Cream
+\item
+  FW Wide Island Display with Solid Walls for Medium Temperature;
+\end{itemize}
+
+\subsection{RefrigerationCompressorCurves.idf}\label{refrigerationcompressorcurves.idf}
+
+This dataset includes object types for specific (by manufacturer and type) Refrigeration:Compressor and associated performance curves. Knowing the nominal refrigerating capacity, power, and refrigerant for the compressor(s) that you want to simulate, you can find it and the associated performance curves in the dataset file. By example, here is part of the RefrigerationCompressorCurves.idf file:
+
+! Capacity Curve for Carlyle\_R-22\_Low\_06CC016,~~ !nominal MBtu/h = 18561.0
+
+! Results in Watts, Inputs:~ Sat Suction Temp (C), Sat Discharge Temp (C)
+
+\begin{lstlisting}
+
+Curve:Bicubic,
+      06CC016_R-22_Low_qcurv,  !- Name
+      2.350e+004,              !- Coefficient1 Constant
+      816.7,                   !- Coefficient2 x
+      10.70,                   !- Coefficient3 x**2
+      -28.24,                  !- Coefficient4 y
+      0.1131,                  !- Coefficient5 y**2
+      -0.4553,                 !- Coefficient6 x*y
+      0.05604,                 !- Coefficient7 x**3
+      -0.004120,               !- Coefficient8 y**3
+      -0.006728,               !- Coefficient9 x**2*y
+      0.006782,                !- Coefficient10 x*y**2
+      -40.0,                   !- Minimum Value of x
+      -17.8,                   !- Maximum Value of x
+      10.0,                    !- Minimum Value of y
+      48.9;                    !- Maximum Value of y
+
+  ! Power Curve for Carlyle_R-22_Low_06CC016,   !nominal kW = 3.1
+  ! Results in Watts, Inputs:  Sat Suction Temp (C), Sat Discharge Temp (C)
+  Curve:Bicubic,
+      06CC016_R-22_Low_pwrcurv,!- Name
+      4018.,                   !- Coefficient1 Constant
+      95.00,                   !- Coefficient2 x
+      1.507,                   !- Coefficient3 x**2
+      5.705,                   !- Coefficient4 y
+      1.247,                   !- Coefficient5 y**2
+      -1.381,                  !- Coefficient6 x*y
+      0.01277,                 !- Coefficient7 x**3
+      -0.007518,               !- Coefficient8 y**3
+      -0.02424,                !- Coefficient9 x**2*y
+      0.02917,                 !- Coefficient10 x*y**2
+      -40.0,                   !- Minimum Value of x
+      -17.8,                   !- Maximum Value of x
+      10.0,                    !- Minimum Value of y
+      48.9;                    !- Maximum Value of y
+
+  !Detailed Compressor: Carlyle_R-22_Low_06CC016,   !nominal MBtu/h = 18561.0, !nominal kW = 3.1
+  Refrigeration:Compressor,
+      Carlyle_R-22_Low_06CC016,!- Name
+      06CC016_R-22_Low_pwrcurv,!- Refrigeration Compressor Power Curve Name
+      06CC016_R-22_Low_qcurv,  !- Refrigeration Compressor Capacity Curve Name
+      ,                        !- Rated Superheat {deltaC}
+      18.3,                    !- Compressor Rated Suction Temperature {C}
+      4.4,                     !- Rated Liquid Temperature {C}
+      ;                        !- Compressor Rated Subcooling {C}
+\end{lstlisting}
+
+\subsection{RooftopPackagedHeatPump.idf}\label{rooftoppackagedheatpump.idf}
+
+This dataset includes performance curves for the object types Coil:Cooling:DX:SingleSpeed, Coil:Cooling:DX:TwoStageWithHumidityControlMode and Coil:Heating:DX:SingleSpeed required to model rooftop packaged heat pumps in EnergyPlus. Manufacturer's data used to develop the data set is also listed in the file. The part of RooftopPackagedHeatPump.idf is shown below.
+
+\subsection{SandiaPVData.idf}\label{sandiapvdata.idf-000}
+
+Use these PV statements for implementing PV modules in an EnergyPlus input file when using the Sandia model.
+
+\subsection{Schedules.idf}\label{schedules.idf}
+
+This data set contains the schedule information for various common (e.g.~Office Occupancy) scheduling instances. Derived from the Schedules Library issued with the BLAST program. Includes the building types schedules from ASHRAE 90.1-1989, Section 13. Schedules are listed alphabetically, with general schedules first, followed by the ten 90.1 building type schedules.
+
+\subsection{SolarCollectors.idf}\label{solarcollectors.idf-000}
+
+Use these SOLAR COLLECTOR PARAMETERS objects for implementing solar collector modules in an EnergyPlus input file.
+
+Data has been reproduced with permission from: ``Directory of SRCC Certified Solar Collector Ratings''~ Copyright (c) 2004 by the Solar Rating and Certification Corporation. For more information, contact: Solar Rating and Certification Corporation, c/o FSEC, 1679 Clearlake Road, Cocoa, FL 32922-5703 USA~ Tel: (321) 638-1537~ Fax: (321) 638-1010~ ,~~ www.solar-rating.org
+
+\subsection{StandardReports.idf}\label{standardreports.idf}
+
+This file contains the Report Table:Monthly command for some commonly used/desired monthly reports.
+
+\subsection{SurfaceColorSchemes.idf}\label{surfacecolorschemes.idf}
+
+This file offers examples for using custom color schemes for DXF output.
+
+\subsection{USHolidays-DST.idf}\label{usholidays-dst.idf}
+
+This is the set of US national holidays as well as daylight saving period defaults.
+
+\subsection{Window5DataFile.dat}\label{window5datafile.dat}
+
+This is an example data file from the Window5 program that can be used with EnergyPlus windows.
+
+\subsection{WindowBlindMaterials.idf}\label{windowblindmaterials.idf}
+
+This is a data set of Window Blind materials.
+
+\subsection{WindowConstructs.idf}\label{windowconstructs.idf}
+
+This is a data set of Window constructions. It does not include the required pieces of the Window construction (glass materials, gas materials).
+
+\subsection{WindowGasMaterials.idf}\label{windowgasmaterials.idf}
+
+This is a data set of Window Gas materials.
+
+\subsection{WindowGlassMaterials.idf}\label{windowglassmaterials.idf}
+
+This is a data set of Window Glass materials.
+
+\subsection{WindowShadeMaterials.idf}\label{windowshadematerials.idf}
+
+This is a data set of Window Shade materials.
+
+\subsection{WindowScreenMaterials.idf}\label{windowscreenmaterials.idf}
+
+This is a data set of Window Screen materials.
diff --git a/doc/output-details-and-examples/src/example-input-files.tex b/doc/output-details-and-examples/src/example-input-files.tex
new file mode 100644
index 00000000000..3d913e1a904
--- /dev/null
+++ b/doc/output-details-and-examples/src/example-input-files.tex
@@ -0,0 +1,119 @@
+\chapter{Example Input Files}\label{example-input-files}
+
+The EnergyPlus install includes a sample of example input files. For the most part, the developers create these files to illustrate and test a specific feature in EnergyPlus. Then, we pass them along to you for illustrative purposes. The install contains two spreadsheet files related to the example files:
+
+\begin{itemize}
+\item
+  \textbf{ExampleFiles.xls} - lists all the files available -- whether through the install or through an external site.
+\item
+  \textbf{ExampleFiles-ObjectLink.xls} - illustrates the first 3 occurances in the example files of an object.
+\end{itemize}
+
+Following convention, each example file should have at the top a set of comments that tell what the purpose of the file is and the key features.
+
+For example, the file titled ``5ZoneAirCooled.idf'' has:
+
+\begin{lstlisting}
+
+! 5ZoneAirCooled.idf
+  ! Basic file description:  1 story building divided into 4 exterior and one interior conditioned zones and return plenum.
+  !
+  ! Highlights:              Electric chiller with air cooled condenser; autosized preheating and precooling water coils in the
+  !                          outside air stream controlled to preheat and precool setpoints.
+  !
+  ! Simulation Location/Run: CHICAGO_IL_USA TMY2-94846, 2 design days, 2 run periods,
+  !                          Run Control executes the run periods using the weather file
+  !
+  ! Location:                Chicago, IL
+  !
+  ! Design Days:             CHICAGO_IL_USA Annual Heating 99% Design Conditions DB, MaxDB = -17.3°C
+  !                          CHICAGO_IL_USA Annual Cooling 1% Design Conditions, MaxDB =   31.5°C MCWB =   23.0°C
+  !
+  ! Run Period (Weather File): Winter 1/14, Summer 7/7, CHICAGO_IL_USA TMY2-94846
+  !
+  ! Run Control:             Zone and System sizing with weather file run control (no design days run)
+  !
+  ! Building: Single floor rectangular building 100 ft x 50 ft. 5 zones - 4 exterior, 1 interior, zone height 8 feet.
+  !           Exterior zone depth is 12 feet. There is a 2 foot high return plenum: the overall building height is
+  !           10 feet. There are windows on all 4 facades; the south and north facades have glass doors.
+  !           The south facing glass is shaded by overhangs. The walls are woodshingle over plywood, R11 insulation,
+  !           and gypboard. The roof is a gravel built up roof with R-3 mineral board insulation and plywood sheathing.
+  !           The windows are of various single and double pane construction with 3mm and 6mm glass and either 6mm or
+  !           13mm argon or air gap. The window to wall ratio is approxomately 0.29.
+  !           The south wall and door have overhangs.
+  !
+  !           The building is oriented 30 degrees east of north.
+  !
+
+
+  ! Floor Area:        463.6 m2 (5000 ft2)
+  ! Number of Stories: 1
+  !
+  ! Zone Description Details:
+  !
+  !      (0,15.2,0)                      (30.5,15.2,0)
+  !           _____   ________                ____
+  !         |\     ***        ****************   /|
+  !         | \                                 / |
+  !         |  \                 (26.8,11.6,0) /  |
+  !         *   \_____________________________/   *
+  !         *    |(3.7,11.6,0)               |    *
+  !         *    |                           |    *
+  !         *    |                           |    *
+  !         *    |               (26.8,3.7,0)|    *
+  !         *    |___________________________|    *
+  !         *   / (3.7,3.7,0)                 \   *
+  !         |  /                               \  |
+  !         | /                                 \ |
+  !         |/___******************___***________\|
+  !          |       Overhang        |   |
+  !          |_______________________|   |   window/door = *
+  !                                  |___|
+  !
+  !      (0,0,0)                            (30.5,0,0)
+  !
+  ! Internal gains description:     lighting is 1.5 watts/ft2, office equip is 1.0 watts/ft2. There is 1 occupant
+  !                                 per 100 ft2 of floor area. The infiltration is 0.25 air changes per hour.
+  !
+  ! Interzone Surfaces:             6 interzone surfaces (see diagram)
+  ! Internal Mass:                  None
+  ! People:                         50
+  ! Lights:                         7500 W
+  ! Windows:                        4 ea.: 1) Double pane clear, 3mm glass, 13mm air gap
+  !                                        2) Double pane clear, 3mm glass, 13mm argon gap
+  !                                        3) Double pane clear, 6mm glass, 6mm air gap
+  !                                        4) Double pane lowE,  6mm lowE glass outside, 6mm air gap, 6mm clear glass
+  !
+  ! Doors:                          2 ea.:    Single pane grey,  3mm glass
+  !
+  ! Detached Shading:               None
+  ! Daylight:                       None
+  ! Natural Ventilation:            None
+  ! Compact Schedules:              Yes
+  !
+  ! HVAC:                           Standard VAV system with outside air, hot water reheat coils,
+  !                                 central chilled water cooling coil. Central Plant is single hot water
+  !                                 boiler, electric compression chiller with air cooled condenser.
+  !                                 All equipment is autosized. HW and ChW coils are used in the outside air
+  !                                 stream to precondition the outside air.
+  !
+  ! Zonal Equipment:                AirTerminal:SingleDuct:VAV:Reheat
+  ! Central Air Handling Equipment: Yes
+  ! System Equipment Autosize:      Yes
+  ! Purchased Cooling:              None
+  ! Purchased Heating:              None
+  ! Coils:                          Coil:Cooling:Water, Coil:Heating:Water
+  ! Pumps:                          Pump:VariableSpeed
+  ! Boilers:                        Boiler:HotWater
+  ! Chillers:                       Chiller:Electric
+  !
+  ! Results:
+  ! Standard Reports:               None
+  ! Timestep or Hourly Variables:   Hourly
+  ! Time bins Report:               None
+  ! HTML Report:                    None
+  ! Environmental Emissions:        None
+  ! Utility Tariffs:                None
+\end{lstlisting}
+
+In addition to the idf files, usually an .rvi and perhaps a .mvi of the same file set is included. As discussed previously, the .rvi is used with the ReadVarsESO post-processing program and the .eso file to create a .csv file which can be read easily into Excelâ„¢. Like the .rvi, the .mvi file can be used with the .mtr file to create a similar version for ``metered'' outputs.
diff --git a/doc/output-details-and-examples/src/introduction.tex b/doc/output-details-and-examples/src/introduction.tex
new file mode 100644
index 00000000000..846d3aee484
--- /dev/null
+++ b/doc/output-details-and-examples/src/introduction.tex
@@ -0,0 +1,5 @@
+\chapter{Introduction}\label{introduction}
+
+This document is intended to give an in-depth look at the various output files produced by EnergyPlus. Some of these may be referenced in various other parts of the documentation but are presented here with more details.
+
+The scripts that assist in running EnergyPlus will usually rename the standard names used in the program. The two scripts that are distributed with EnergyPlus are: \textbf{EPL-Run.bat} (which is used by the EP-Launch program) and \textbf{RunEPlus.bat}~ (which can be used from the command line). The RunEPlus batch file can also be used to string together several runs such as usually termed ``batch processing''. In renaming the files created by the program or its post-processing program(s), usually the file extension will be retained. The following table will illustrate the native EnergyPlus file name, a description of its contents and the EP-Launch ``version'' of the file. In this table, \textless{}filename\textgreater{} refers to the source/original file name (without extension) selected. Files are presented in alphabetic order. For output purposes, the most important files to understand are the eplusout.eso, eplusout.mtr and eplusout.err files. The first two are manipulated with the ReadVarsESO post processing program. The latter will contain any critical errors that were encountered during the run.
diff --git a/doc/output-details-and-examples/src/output-details-and-examples.tex b/doc/output-details-and-examples/src/output-details-and-examples.tex
new file mode 100644
index 00000000000..63f37402bb8
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-details-and-examples.tex
@@ -0,0 +1 @@
+\input{../title}
diff --git a/doc/output-details-and-examples/src/output-files.tex b/doc/output-details-and-examples/src/output-files.tex
new file mode 100644
index 00000000000..c21c45511e0
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files.tex
@@ -0,0 +1 @@
+\chapter{Output Files}\label{output-files}
diff --git a/doc/output-details-and-examples/src/output-files/delight-output-files.tex b/doc/output-details-and-examples/src/output-files/delight-output-files.tex
new file mode 100644
index 00000000000..79c880959c0
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/delight-output-files.tex
@@ -0,0 +1,37 @@
+\section{Delight output files}\label{delight-output-files}
+
+\subsection{eplusout.delightin}\label{eplusout.delightin}
+
+Following completion of an EnergyPlus run that includes Daylighting:DElight objects, an ASCII text file created during the run is given a file name that consists of the project name appended with DElight.in (e.g., MyProjectDElight.in).
+
+This text file is a formatted DElight input file that was created from the EnergyPlus input data relevant to a DElight simulation. This file can be manually reviewed to determine the exact data that were transformed from EnergyPlus into DElight input.
+
+\subsection{eplusout.delightout}\label{eplusout.delightout}
+
+Following completion of an EnergyPlus run that includes Daylighting:DElight objects, an ASCII text file created during the run is given a file name that consists of the project name appended with DElight.out (e.g., MyProjectDElight.out).
+
+This text file is a formatted DElight output file that was generated by the DElight simulation engine following the pre-processing daylight factors calculation. This file can be manually reviewed to see the results of these calculations. The file contains an echo of DElight input data, as well as the results of intermediate calculations such as geometrical transformations, surface gridding, and daylight factors, including the following.
+
+\textbf{Surface Data}
+
+\begin{itemize}
+\item
+  Vertex coordinates in the Building coordinate system. Search for the string ``BldgSystem\_Surface\_Vertices'' within the output file.
+\item
+  Exterior face luminance values under overcast skies, and for each sun position under clear skies. Search for the string ``Surface Exterior Luminance'' within the output file.
+\item
+  Common data for radiosity nodal patches for each surface including Area and Number of Nodes. Search for the string ``Surface\_Node\_Area'' within the output file.
+\item
+  Individual data for radiosity nodal patches for each node on each surface including: building coordinate system coordinates; direct and total luminance values under overcast skies, and for each sun position under clear skies. Search for the string ``BldgSystem\_Node\_Coordinates'' within the output file.
+\end{itemize}
+
+\textbf{Reference Point Data}
+
+\begin{itemize}
+\item
+  Illuminance values from the daylighting factors preprocessor for overcast skies, and for each sun position under clear skies.
+\item
+  Daylight Factor values from the daylighting factors preprocessor for overcast skies, and for each sun position under clear skies.
+\item
+  NOTE: The Monthly Average data for Daylight Illuminances and Electric Lighting Reduction will all be zero since these data are not calculated as part of the pre-processing done by the point at which this output file is generated for EnergyPlus.
+\end{itemize}
diff --git a/doc/output-details-and-examples/src/output-files/eplusmap-lt-ext-gt.tex b/doc/output-details-and-examples/src/output-files/eplusmap-lt-ext-gt.tex
new file mode 100644
index 00000000000..cd8480a729e
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusmap-lt-ext-gt.tex
@@ -0,0 +1,44 @@
+\section{eplusmap.\textless{}ext\textgreater{}}\label{eplusmap.ext}
+
+The eplusmap.csv (or txt or tab extension) is a file that is generated by the Output:IlluminanceMap object. These are calculated for the Daylighting:Controls daylighting option. By default, this is a comma delimited text file (csv) that can be imported into a spreadsheet program. For example, the input for the Output:IlluminanceMap object shown below:
+
+\begin{lstlisting}
+Output:IlluminanceMap,
+    Daylit Map,              !- Map Name
+    Daylit Zone,             !- Zone Name
+    0.8,                     !- Z height {m}
+    0.1,                     !- X minimum coordinate {m}
+    4.9,                     !- X maximum coordinate {m}
+    10,                      !- Number of X grid points
+    0.1,                     !- Y minimum coordinate {m}
+    9.9,                     !- Y maximum coordinate {m}
+    10;                      !- Number of Y grid points
+\end{lstlisting}
+
+generates the following output in csv format when viewed with Microsoft Excel.~ \textbf{Note that if the point is outside the zone a ``*'' will be shown.}
+
+\begin{figure}[hbtp] % fig 7
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image019.png}
+\caption{Spreadsheet view of Daylight Map output \protect \label{fig:spreadsheet-view-of-daylight-map-output}}
+\end{figure}
+
+Each cell reports the illuminance (in lux) at the location specified by the (X;Y) coordinates in the column and row headers. These are XY pairs separated by a semi-colon for ease in importing into the spreadsheet. The Z coordinate of the map is shown in the title (the illuminance map is set in a plane). The date and time are indicated in the upper left cell of the map. One map is reported for every hour of the simulation.
+
+The illuminance values are organized to allow the user to rapidly plot a visualization of the data using Microsoft Excel's standard ``3-D Column'' graph. A 3-D graph is shown below for the data in a single day similar to the earlier example.
+
+\begin{figure}[hbtp] % fig 8
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image020.png}
+\caption{3D Graph of Illuminance Map \protect \label{fig:3d-graph-of-illuminance-map}}
+\end{figure}
+
+The following figure illustrates a similar map for the tubular daylighting device example file that is included with the installation.
+
+\begin{figure}[hbtp] % fig 9
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image021.png}
+\caption{A 3D illuminance map for the tubular daylighting device file \protect \label{fig:a-3d-illuminance-map-for-the-tubular}}
+\end{figure}
+
+Individual 3-D graphs can be generated for each hour of a given day and collected to generate a sequence of graphs representing the progression of daylighting conditions over the course of the day. Using additional software tools (not provided with EnergyPlus) the user can do further post-processing to link screenshots of the graphs into an animated sequence.
diff --git a/doc/output-details-and-examples/src/output-files/eplusmtr-lt-ext-gt.tex b/doc/output-details-and-examples/src/output-files/eplusmtr-lt-ext-gt.tex
new file mode 100644
index 00000000000..91c316db1bd
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusmtr-lt-ext-gt.tex
@@ -0,0 +1,3 @@
+\section{eplusmtr.\textless{}ext\textgreater{}}\label{eplusmtr.ext}
+
+The eplusmtr.csv (or txt or tab extension) is a file that can be produced by post-processing on the eplusout.mtr file. EnergyPlus distributes a post-processing program (ReadVarsESO -- see next section) with the installation.
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-audit.tex b/doc/output-details-and-examples/src/output-files/eplusout-audit.tex
new file mode 100644
index 00000000000..af695b6aef0
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-audit.tex
@@ -0,0 +1,53 @@
+\section{eplusout.audit}\label{eplusout.audit}
+
+This file is simply the echo of the inputs to the EnergyPlus program -- the Energy+.idd (data dictionary) and in.idf (\textless{}filename\textgreater{}.idf -- the input data file). Every attempt has been made to not require this file to be saved -- errors are interpreted as much as possible and encapsulated onto the eplusout.err file. Any errors in the data dictionary processing should be accomplished during development -- users should never see errors there. Thus, this file is not ``saved'' after processing by the standard script file. Occasionally, you may wish to view this file because of something obscure.
+
+An excerpt of the file follows. Lines in green are notes produced from EnergyPlus (some of these are more useful to developers than users). Lines in red are lines with error messages shown to illustrate context. The other lines are echoes from inputs (with line numbers).
+
+In all the examples, the actual version of the EnergyPlus exe would appear. In the examples these will be shown as: \textless{}version\textgreater{}.
+
+\begin{lstlisting}
+  Processing Data Dictionary (Energy+.idd) File -- Start
+     1 !IDD_Version <version>
+     2 ! **************************************************************************
+     3 !
+<reduced for brevity>
+ 13000 \key DETAILS
+ 13001 \key Vertices
+ 13002 \key DetailsWithVertices
+  Processing Data Dictionary (Energy+.idd) File -- Complete
+  Maximum number of Alpha Args= 4500
+  Maximum number of Numeric Args= 1800
+  Number of Object Definitions= 473
+  Number of Section Definitions= 2
+  Processing Input Data File (in.idf) -- Start
+    1 ! Basic file description: Basic illustration of using Purchased Air as a system
+    2 ! Run: 2 design days.
+    3 ! 2 annual run periods, 2 summer days and 3 winter days.
+<reduced for brevity>
+   63 RunPeriod, ! 3 day winter simuluation
+   64 1, 1, ! Start Month ,Day
+   65 1, 3; ! End Month ,Day
+  ** Warning ** Object=RUNPERIOD, entered with less than minimum number of fields.
+  ** ~~~ ** Attempting fill to minimum.
+   66 MATERIAL:Regular,A1 - 1 IN STUCCO, !- Material Name
+<reduced for brevity>
+  784 End Simulation Data;
+  Processing Input Data File (in.idf) -- Complete
+  Number of IDF "Lines"= 359
+  Maximum number of Alpha IDF Args= 29
+  Maximum number of Numeric IDF Args= 20
+ Getting object=VERSION
+ Getting object=TIMESTEP
+ Getting object=SIMULATIONCONTROL
+ Getting object=SIZING:PARAMETERS
+ Getting object=SIZING:ZONE
+ Getting object=SIZING:SYSTEM
+ Getting object=SIZING:PLANT
+<etc>
+MaxRVariable= 5000
+MaxIVariable= 100
+NumEnergyMeters= 108
+NumVarMeterArrays= 106
+\end{lstlisting}
+
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-bnd.tex b/doc/output-details-and-examples/src/output-files/eplusout-bnd.tex
new file mode 100644
index 00000000000..01dea9efe12
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-bnd.tex
@@ -0,0 +1,179 @@
+\section{eplusout.bnd}\label{eplusout.bnd}
+
+The ``branch node details'' (bnd) file is intended to give enough information that one could (with a chosen software) diagram the nodes and components of the HVAC system. It may or may not achieve that objective. Of more use may be its illustration of node connection/branch errors that aren't detected by the software. This file has the details to support any ``node connection'' errors that will be noted in the eplusout.err file. Branch validation is shown in this file. Branches are checked to assure that each output node of the branch element is an input node to the next branch element. Cross-branch checking is not done directly within the program though the details will illustrate some problems of that nature.
+
+Supply and Return Air Paths are also checked and feedback about each item are shown.
+
+As is standard with many EnergyPlus output files, this file is CSV (comma-delimited) such that it can be read by spreadsheet programs for further manipulation by the user.
+
+An example will illustrate. Notes about the reporting are highlighted in green.
+
+Program Version,EnergyPlus, \textless{}version\textgreater{}
+
+! This file shows details about the branches, nodes, and other
+
+! elements of the flow connections.
+
+! This file is intended for use in ``debugging'' potential problems
+
+! that may also be detected by the program, but may be more easily
+
+! identified by ``eye''.
+
+! This file is also intended to support software which draws a
+
+! schematic diagram of the HVAC system.
+
+! = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+
+! \#Nodes,\textless{}Number of Unique Nodes\textgreater{}
+
+~\#Nodes,11
+
+\textbf{List of all nodes follows. \# references may be an indication of faulty node spec (or not)}
+
+! \textless{}Node\textgreater{},\textless{}NodeNumber\textgreater{},\textless{}Node Name\textgreater{},\textless{}Node Fluid Type\textgreater{},\textless{}\# Times Node Referenced After Definition\textgreater{}
+
+~Node,1,SUPPLY INLET NODE,Air,3
+
+~Node,2,FAN INLET NODE,Air,4
+
+\textless{}reduced for brevity\textgreater{}
+
+Node,10,ZONE EQUIPMENT OUTLET NODE,Air,2
+
+~Node,11,RELIEF AIR OUTLET NODE,Air,1
+
+! = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+
+! Suspicious nodes have 0 references. It is normal for some nodes, however.
+
+! Suspicious nodes have 0 references.~ It is normal for some nodes, however.
+
+! Listing nodes with 0 references (culled from previous list):
+
+! \textless{}Suspicious Node\textgreater{},\textless{}NodeNumber\textgreater{},\textless{}Node Name\textgreater{},\textless{}Node Fluid Type\textgreater{},\textless{}\# Times Node Referenced After Definition\textgreater{}
+
+~Suspicious Node,7,MAIN ZONE NODE,Air,0
+
+\textbf{List of branches follow.}
+
+! \textless{}\#Branch Lists\textgreater{},\textless{}Number of Branch Lists\textgreater{}
+
+~\#Branch Lists,1
+
+! \textless{}Branch List\textgreater{},\textless{}Branch List Count\textgreater{},\textless{}Branch List Name\textgreater{},\textless{}Loop Name\textgreater{},\textless{}Loop Type\textgreater{},\textless{}Number of Branches\textgreater{}
+
+! \textless{}Branch\textgreater{},\textless{}Branch Count\textgreater{},\textless{}Branch Name\textgreater{},\textless{}Loop Name\textgreater{},\textless{}Loop Type\textgreater{},\textless{}Branch Inlet Node Name\textgreater{},\textless{}Branch Outlet Node Name\textgreater{}
+
+~Branch List,1,AIR LOOP BRANCHES,EVAP COOLER SYSTEM,Air,1
+
+~~ Branch,1,AIR LOOP MAIN BRANCH,EVAP COOLER SYSTEM,Air,SUPPLY INLET NODE,SUPPLY OUTLET NODE
+
+! = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+
+! \textless{}\#Supply Air Paths\textgreater{},\textless{}Number of Supply Air Paths\textgreater{}
+
+! \textless{}\#Supply Air Paths\textgreater{},\textless{}Number of Supply Air Paths\textgreater{}
+
+~\#Supply Air Paths,1
+
+! \textless{}Supply Air Path\textgreater{},\textless{}Supply Air Path Count\textgreater{},\textless{}Supply Air Path Name\textgreater{},\textless{}AirLoopHVAC Name\textgreater{}
+
+! \textless{}\#Components on Supply Air Path\textgreater{},\textless{}Number of Components\textgreater{}
+
+! \textless{}Supply Air Path Component\textgreater{},\textless{}Component Count\textgreater{},\textless{}Component Type\textgreater{},\textless{}Component Name\textgreater{},\textless{}AirLoopHVAC Name\textgreater{}
+
+! \textless{}\#Outlet Nodes on Supply Air Path Component\textgreater{},\textless{}Number of Nodes\textgreater{}
+
+! \textless{}Supply Air Path Component Nodes\textgreater{},\textless{}Node Count\textgreater{},\textless{}Component Type\textgreater{},\textless{}Component Name\textgreater{},\textless{}Inlet Node Name\textgreater{},\textless{}Outlet Node Name\textgreater{},\textless{}AirLoopHVAC Name\textgreater{}
+
+~Supply Air Path,1,ZONE SUPPLY AIR PATH,EVAP COOLER SYSTEM
+
+~~ \#Components on Supply Air Path,1
+
+~~ Supply Air Path Component,1,AIRLOOPHVAC:ZONESPLITTER,ZONE SUPPLY AIR SPLITTER,EVAP COOLER SYSTEM
+
+~~~~ \#Outlet Nodes on Supply Air Path Component,1
+
+~~~~ Supply Air Path Component Nodes,1,AIRLOOPHVAC:ZONESPLITTER,ZONE SUPPLY AIR SPLITTER,ZONE EQUIPMENT INLET NODE,MAIN ZONE INLET NODE,EVAP COOLER SYSTEM
+
+! \textless{}\#Nodes on Supply Air Path\textgreater{},\textless{}Number of Nodes\textgreater{}
+
+! \textless{}Supply Air Path Node\textgreater{},\textless{}Node Type\textgreater{},\textless{}Node Count\textgreater{},\textless{}Node Name\textgreater{},\textless{}AirLoopHVAC Name\textgreater{}
+
+\#Nodes on Supply Air Path,2
+
+~~ Supply Air Path Node,Inlet Node,1,ZONE EQUIPMENT INLET NODE,EVAP COOLER SYSTEM
+
+~~ Supply Air Path Node,Outlet Node,2,MAIN ZONE INLET NODE,EVAP COOLER SYSTEM
+
+! = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+
+! \textless{}\#Return Air Paths\textgreater{},\textless{}Number of Return Air Paths\textgreater{}
+
+! \textless{}\#Return Air Paths\textgreater{},\textless{}Number of Return Air Paths\textgreater{}
+
+~\#Return Air Paths,1
+
+! \textless{}Return Air Path\textgreater{},\textless{}Return Air Path Count\textgreater{},\textless{}Return Air Path Name\textgreater{},\textless{}AirLoopHVAC Name\textgreater{}
+
+! \textless{}\#Components on Return Air Path\textgreater{},\textless{}Number of Components\textgreater{}
+
+! \textless{}Return Air Path Component\textgreater{},\textless{}Component Count\textgreater{},\textless{}Component Type\textgreater{},\textless{}Component Name\textgreater{},\textless{}AirLoopHVAC Name\textgreater{}
+
+! \textless{}\#Inlet Nodes on Return Air Path Component\textgreater{},\textless{}Number of Nodes\textgreater{}
+
+! \textless{}Return Air Path Component Nodes\textgreater{},\textless{}Node Count\textgreater{},\textless{}Component Type\textgreater{},\textless{}Component Name\textgreater{},\textless{}Inlet Node Name\textgreater{},\textless{}Outlet Node Name\textgreater{},\textless{}AirLoopHVAC Name\textgreater{}
+
+~Return Air Path,1,ZONE RETURN AIR PATH,EVAP COOLER SYSTEM
+
+~~ \#Components on Return Air Path,1
+
+~~ Return Air Path Component,1,AIRLOOPHVAC:ZONEMIXER,ZONE RETURN AIR MIXER,EVAP COOLER SYSTEM
+
+~~~~ \#Inlet Nodes on Return Air Path Component,1
+
+~~~~ Return Air Path Component Nodes,1,AIRLOOPHVAC:ZONEMIXER,ZONE RETURN AIR MIXER,MAIN ZONE OUTLET NODE,ZONE EQUIPMENT OUTLET NODE,EVAP COOLER SYSTEM
+
+! \textless{}\#Nodes on Return Air Path\textgreater{},\textless{}Number of Nodes\textgreater{}
+
+! \textless{}Return Air Path Node\textgreater{},\textless{}Node Type\textgreater{},\textless{}Node Count\textgreater{},\textless{}Node Name\textgreater{},\textless{}AirLoopHVAC Name\textgreater{}
+
+~~ \#Nodes on Return Air Path,2
+
+~~ Return Air Path Node,Outlet Node,1,ZONE EQUIPMENT OUTLET NODE,EVAP COOLER SYSTEM
+
+~~ Return Air Path Node,Inlet Node,2,MAIN ZONE OUTLET NODE,EVAP COOLER SYSTEM
+
+! = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+
+! \#Outside Air Nodes,\textless{}Number of Outside Air Nodes\textgreater{}
+
+! \#Outdoor Air Nodes,\textless{}Number of Outdoor Air Nodes\textgreater{}
+
+~\#Outdoor Air Nodes,1
+
+! \textless{}Outdoor Air Node\textgreater{},\textless{}NodeNumber\textgreater{},\textless{}Node Name\textgreater{}
+
+~Outdoor Air Node,5,OUTSIDE AIR INLET NODE
+
+! = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+
+\textbf{Component sets. Very important for node connection error detection.}
+
+! \textless{}\#Component Sets\textgreater{},\textless{}Number of Component Sets\textgreater{}
+
+~\#Component Sets,4
+
+! \textless{}Component Set\textgreater{},\textless{}Component Set Count\textgreater{},\textless{}Parent Object Type\textgreater{},\textless{}Parent Object Name\textgreater{},\textless{}Component Type\textgreater{},\textless{}Component Name\textgreater{},\textless{}Inlet Node ID\textgreater{},\textless{}Outlet Node ID\textgreater{},\textless{}Description\textgreater{}
+
+~Component Set,1,BRANCH,AIR LOOP MAIN BRANCH,AIRLOOPHVAC:OUTDOORAIRSYSTEM,OUTSIDE AIR SYSTEM,SUPPLY INLET NODE,FAN INLET NODE,Air Nodes
+
+~Component Set,2,BRANCH,AIR LOOP MAIN BRANCH,FAN:CONSTANTVOLUME,SUPPLY FAN,FAN INLET NODE,EVAP COOLER INLET NODE,Air Nodes
+
+~Component Set,3,BRANCH,AIR LOOP MAIN BRANCH,EVAPORATIVECOOLER:DIRECT:CELDEKPAD,EVAPORATIVE COOLER,EVAP COOLER INLET NODE,SUPPLY OUTLET NODE,Evap Air Nodes
+
+~Component Set,4,AIRLOOPHVAC:OUTDOORAIRSYSTEM,OUTSIDE AIR SYSTEM,OUTDOORAIR:MIXER,OUTSIDE AIR MIXING BOX,OUTSIDE AIR INLET NODE,FAN INLET NODE,Air Nodes
+
+\textbf{Similar details for Plant Loops, Condenser Loops, Controlled Zones, etc.}
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-dbg.tex b/doc/output-details-and-examples/src/output-files/eplusout-dbg.tex
new file mode 100644
index 00000000000..b707e86317d
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-dbg.tex
@@ -0,0 +1,37 @@
+\section{eplusout.dbg}\label{eplusout.dbg}
+
+Developers use this file during debugging and can be ``turned on'' by the DEBUG OUTPUT object in the input file. The only reason a user might specify this flag would be to send a file to the support group.
+
+\textbf{Output:DebuggingData, 1, 0;~~~ ! standard debug output, during simulation days}
+
+The standard debug output appears like this:
+
+Day of Sim~~~~ Hour of Day~~~ Time
+
+~~~~~~~~~~ 1~~~~~~~~~~ 1~ 0.166666666666667
+
+node \#~~ Temp~~~~~ MassMinAv~ MassMaxAv TempSP~~ MassFlow~~ MassMin~~~ MassMax~~~ MassSP~~~~~ Press~~~~~~~ Enthal~~~~ HumRat~~~ Fluid Type
+
+~~ 1~~~ -12.500~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~ 100344.00~~~~ -9363.63~~~ 0.00129~ Air
+
+~~ 2~~~ -12.500~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~ 100344.00~~~~ -9363.63~~~ 0.00129~ Air
+
+~~ 3~~~ -12.500~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~ 100344.00~~~~ -9363.63~~~ 0.00129~ Air
+
+~~ 4~~~ -12.500~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~ 100344.00~~~~ -9363.63~~~ 0.00129~ Air
+
+~~ 5~~~~ 50.000~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.0320~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~ 100344.00~~~~ 60617.55~~~ 0.00400~ Air
+
+~~ 6~~~~ 50.000~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.0326~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~ 100344.00~~~~ 60617.55~~~ 0.00400~ Air
+
+~~ 7~~~~ 50.000~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.1636~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~ 100344.00~~~~ 60617.55~~~ 0.00400~ Air
+
+~~ 8~~~~ 50.000~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.1648~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~ 100344.00~~~~ 60617.55~~~ 0.00400~ Air
+
+~~ 9~~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~~~~ 0.00~~~~~~~~ 0.00~~~ 0.00000~ blank
+
+~ 10~~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~~~~ 0.00~~~~~~~~ 0.00~~~ 0.00000~ blank
+
+~ 11~~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~~~~ 0.00~~~~~~~~ 0.00~~~ 0.00000~ blank
+
+~ 12~~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~ 0.0000~~~~~~~ 0.00~~~~~~~~ 0.00~~~ 0.00000~ blank
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-dfs.tex b/doc/output-details-and-examples/src/output-files/eplusout-dfs.tex
new file mode 100644
index 00000000000..e2b1ee2664c
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-dfs.tex
@@ -0,0 +1,99 @@
+\section{eplusout.dfs}\label{eplusout.dfs}
+
+The daylight factors report contains the pre-calculated hourly daylight factors for the four CIE sky types (clear, clear turbid, intermediate, and overcast sky) and two daylight reference points for each exterior window of a daylight zone. The file is CSV formatted -- ready for spreadsheet viewing. The input for requesting the report is simple:
+
+The following shows an excerpt the daylight factors for a window without shade:
+
+This file contains daylight factors for all exterior windows of daylight zones.
+
+If only one reference point the last 4 columns in the data will be zero.
+
+MonthAndDay,Zone Name,Window Name,Window State
+
+Hour,Daylight Factor for Clear Sky at Reference point 1,Daylight Factor for Clear Turbid Sky at Reference point 1,Daylight Factor for Intermediate Sky at Reference point 1,Daylight Factor for Overcast Sky at Reference point 1,Daylight Factor for Clear Sky at Reference point 2,Daylight Factor for Clear Turbid Sky at Reference point 2,Daylight Factor for Intermediate Sky at Reference point 2,Daylight Factor for Overcast Sky at Reference point 2
+
+01/21,PERIMETER\_BOT\_ZN\_1,PERIMETER\_BOT\_ZN\_1\_WALL\_SOUTH\_WINDOW,Base Window
+
+1,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+2,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+3,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+4,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+5,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+6,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+7,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+8,5.08810E-002,5.78633E-002,2.59271E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
+
+9,5.85018E-002,6.68126E-002,3.02054E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
+
+10,6.26710E-002,7.12830E-002,3.37475E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
+
+11,6.35876E-002,7.17181E-002,3.59982E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
+
+12,6.23746E-002,6.98139E-002,3.66365E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
+
+13,6.39669E-002,7.21972E-002,3.61684E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
+
+14,6.25455E-002,7.10272E-002,3.39911E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
+
+15,5.85994E-002,6.67866E-002,3.05581E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
+
+16,5.17581E-002,5.89493E-002,2.63461E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
+
+17,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+18,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+19,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+20,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+21,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+22,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+23,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+24,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
+
+The first line describes the data in the eplusout.dfs file. The second line describes the header of the daily row:
+
+\begin{longtable}[c]{p{0.66in}p{0.66in}p{0.66in}p{0.66in}p{0.66in}p{0.66in}p{0.66in}p{0.66in}p{0.66in}}
+\toprule 
+Hour & Daylight factor for clear sky at reference point 1 & Daylight factor for clear turbid sky at reference point 1 & Daylight factor for intermediate sky at reference point 1 & Daylight factor for overcast sky at reference point 1 & Daylight factor for clear sky at reference point 2 & Daylight factor for clear turbid sky at reference point 2 & Daylight factor for intermediate sky at reference point 2 & Daylight factor for overcast sky at reference point 2 \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Hour & Daylight factor for clear sky at reference point 1 & Daylight factor for clear turbid sky at reference point 1 & Daylight factor for intermediate sky at reference point 1 & Daylight factor for overcast sky at reference point 1 & Daylight factor for clear sky at reference point 2 & Daylight factor for clear turbid sky at reference point 2 & Daylight factor for intermediate sky at reference point 2 & Daylight factor for overcast sky at reference point 2 \tabularnewline
+\midrule
+\endhead
+
+10 & 0.06239 & 0.07088 & 0.03377 & 0.01427 & 0.0 & 0.0 & 0.0 & 0.0 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The Window State column has three possible outputs -- Base Window indicating windows without shades; a numeric value, from 0.0 to 180.0 for every 10.0 step, indicating the slat angle (in degrees) of the blind shading the window; blink indicating windows in shaded state by shades, screens, and blinds with fixed slat angle.
+
+The third line describes the hourly daylight factors. Note that the last 4 columns are 0.0 because there is only one daylight reference point.:
+
+\begin{longtable}[c]{p{0.66in}p{0.66in}p{0.66in}p{0.66in}p{0.66in}p{0.66in}p{0.66in}p{0.66in}p{0.66in}}
+\toprule 
+Hour & Daylight factor for clear sky at reference point 1 & Daylight factor for clear turbid sky at reference point 1 & Daylight factor for intermediate sky at reference point 1 & Daylight factor for overcast sky at reference point 1 & Daylight factor for clear sky at reference point 2 & Daylight factor for clear turbid sky at reference point 2 & Daylight factor for intermediate sky at reference point 2 & Daylight factor for overcast sky at reference point 2 \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Hour & Daylight factor for clear sky at reference point 1 & Daylight factor for clear turbid sky at reference point 1 & Daylight factor for intermediate sky at reference point 1 & Daylight factor for overcast sky at reference point 1 & Daylight factor for clear sky at reference point 2 & Daylight factor for clear turbid sky at reference point 2 & Daylight factor for intermediate sky at reference point 2 & Daylight factor for overcast sky at reference point 2 \tabularnewline
+\midrule
+\endhead
+
+10 & 0.06239 & 0.07088 & 0.03377 & 0.01427 & 0.0 & 0.0 & 0.0 & 0.0 \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-dxf.tex b/doc/output-details-and-examples/src/output-files/eplusout-dxf.tex
new file mode 100644
index 00000000000..92f6e7a0f75
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-dxf.tex
@@ -0,0 +1,105 @@
+\section{eplusout.dxf}\label{eplusout.dxf}
+
+The DXF output report file is formatted according to the ``Data Exchange Format'' standard rules for representing CADD type coordinates. The file can be used in several inexpensive, shareware or freeware viewers. Quickview Plus â„¢ can display DXF files as shown in Figure~\ref{fig:quick-view-plus-version-of-dxf-file} below. A free program originally from Autocadâ„¢, Voloview Expressâ„¢, can display solid model rendering as shown in Figure~\ref{fig:voloview-3d-solid-view}. Other viewers are available from Microstationâ„¢, Visioâ„¢ and other shareware or freeware vendors.
+
+This file is generated when the following line is included in the IDF.
+
+\textbf{Output:Surfaces:Drawing, DXF;}
+
+You can ask it to triangulate surfaces with \textgreater{}4 sides:
+
+\textbf{Output:Surfaces:Drawing, DXF, Triangulate3dface;}
+
+In addition to the building shape (including detached shading elements), the DXF view includes a ``true north'' arrow (at ground level) and the name from the BUILDING object.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image001.jpg}
+\caption{Quick View Plus version of DXF file \protect \label{fig:quick-view-plus-version-of-dxf-file}}
+\end{figure}
+
+Even in the Quick View version, you can see that the different building elements have different colors. These are the ``original'' colors used in EnergyPlus. The current default color scheme is shown in the following figure of the solid model.
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image002.jpg}
+\caption{Voloview 3D Solid view \protect \label{fig:voloview-3d-solid-view}}
+\end{figure}
+
+The DXF file of itself is an ASCII file, with a specific structure as specified in the standard. An excerpt of the file is shown below:
+
+\begin{lstlisting}
+SECTION
+  2
+ENTITIES
+  0
+TEXT
+  8
+1
+  6
+CONTINUOUS
+ 62
+  3
+ 10
+      -11.00000
+ 20
+        3.00000
+ 30
+        0.10000
+ 40
+ .25
+  1
+True North
+ 41
+ 0.0
+  7
+MONOTXT
+210
+0.0
+220
+0.0
+230
+1.0
+  0
+\end{lstlisting}
+
+\begin{lstlisting}
+3DFACE
+  8
+1
+ 62
+  3
+ 10
+      -10.00000
+ 20
+        3.00000
+ 30
+        0.10000
+ 11
+      -10.00000
+ 21
+        3.00000
+ 31
+        0.00000
+ 12
+      -10.00000
+ 22
+        0.00000
+ 32
+        0.00000
+ 13
+      -10.00000
+ 23
+        0.00000
+ 33
+        0.10000
+  0
+ENDSEC
+  0
+EOF
+999
+DXF created from EnergyPlus
+999
+\end{lstlisting}
+
+Program Version,EnergyPlus, \textless{}version\textgreater{}
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-edd.tex b/doc/output-details-and-examples/src/output-files/eplusout-edd.tex
new file mode 100644
index 00000000000..7e0ddbda117
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-edd.tex
@@ -0,0 +1,51 @@
+\section{eplusout.edd}\label{eplusout.edd}
+
+This file is invoked by including an Output:EnergyManagementSystem input object. The EDD file contains three different types of information related to the Energy Management System (EMS) including: (1) listing of available actuators, (2) listing of available internal variables, and (3) a record of the execution of user's programs for the EnergyPlus Runtime Language (Erl).
+
+The EMS feature in EnergyPlus uses ``Actuators'' to do control operations. The actuators available in a given model depend on the non-EMS-related content of the input file. Similar to how EnergyPlus reports the available output variables to the RDD file, a list of available actuators can be written to the EDD file. There are three settings in the Output:EnergyManagementSystem input object that control how actuators are listed. Selecting ``None'' directs the program to not list the available actuators. Selecting ``NotByUniqueKeyNames'' directs the program to provide a concise listing of the available actuators that does not include their enumeration by unique name. Selecting ``Verbose'' directs the program to provide a complete listing of the available actuators including the unique identifying names. An example listing of actuators using the~ ``NotByUniqueKeyNames''~ option follows.
+
+! \textless{}EnergyManagementSystem:Actuator Available\textgreater{}, *, Component Type, 'Control Type, Units
+
+EnergyManagementSystem:Actuator Available, *,Schedule:Compact,Schedule Value,{[} {]}
+
+EnergyManagementSystem:Actuator Available, *,People,Number of People,{[}each{]}
+
+EnergyManagementSystem:Actuator Available, *,Lights,Electric Power Level,{[}W{]}
+
+EnergyManagementSystem:Actuator Available, *,ElectricEquipment,Electric Power Level,{[}W{]}
+
+EnergyManagementSystem:Actuator Available, *,Window Shading Control,Control Status,{[}ShadeStatus{]}
+
+EnergyManagementSystem:Actuator Available, *,Zone Temperature Control,Heating Setpoint,{[}C{]}
+
+EnergyManagementSystem:Actuator Available, *,Zone Temperature Control,Cooling Setpoint,{[}C{]}
+
+EnergyManagementSystem:Actuator Available, *,Surface,Interior Surface Convection Heat Transfer Coefficient,{[}W/m2-K{]}
+
+EnergyManagementSystem:Actuator Available, *,Surface,Exterior Surface Convection Heat Transfer Coefficient,{[}W/m2-K{]}
+
+EnergyManagementSystem:Actuator Available, *,Ideal Loads Air System,Air Mass Flow Rate,{[}kg/s{]}
+
+The EMS feature in EnergyPlus uses ``Internal Variables'' to obtain input data for use in scaling the results of control calculations. The internal variables available in a give model depend on the non-EMS-related content of the input file. Similar to how EnergyPlus reports the available output variables to the RDD file, a list of available internal variables can be written to the EDD file. There are three settings in the Output:EnergyManagementSystem input object that control how internal variables are listed. Selecting ``None'' directs the program to not list the available internal variables. Selecting ``NotByUniqueKeyNames'' directs the program to provide a concise listing of the available internal variables that does not include their enumeration by unique name. Selecting ``Verbose'' directs the program to provide a complete listing of the available internal variables including the unique identifying names. An example listing of actuators using the~ ``NotByUniqueKeyNames''~ option follows.
+
+! \textless{}EnergyManagementSystem:InternalVariable Available\textgreater{}, *, Internal Data Type
+
+EnergyManagementSystem:InternalVariable Available, *,People Count Design Level,{[}each{]}
+
+EnergyManagementSystem:InternalVariable Available, *,Lighting Power Design Level,{[}W{]}
+
+EnergyManagementSystem:InternalVariable Available, *,Plug and Process Power Design Level,{[}W{]}
+
+EnergyManagementSystem:InternalVariable Available, *,Zone List Multiplier,{[} {]}
+
+EnergyManagementSystem:InternalVariable Available, *,Zone Floor Area,{[}m2{]}
+
+EnergyManagementSystem:InternalVariable Available, *,Zone Air Volume,{[}m3{]}
+
+EnergyManagementSystem:InternalVariable Available, *,Zone Multiplier,{[} {]}
+
+EnergyManagementSystem:InternalVariable Available, *,Zone List Multiplier,{[} {]}
+
+The EMS uses the EnergyPlus Runtime Language, or Erl, to do custom controlling. When Erl programs are being developed, the EDD becomes a primary source of information for debugging. When a line of Erl code is executed, the program can output records called ``line traces'' that are useful for debugging because they show the outcome of each line of code. There are three settings in the Output:EnergyManagementSystem input object that control how line traces are reported. Selecting ``None'' directs the program to not write out any line traces. Selecting ``ErrorsOnly'' directs the program to only write line traces when computation errors are encountered (such as divide by zero). Selecting ``Verbose'' directs the program to write out line traces for each and every line of Erl program code that is executed.
+
+It is very important to be careful with the EDD file. The Verbose option should be used with care because a full line-by-line trace of Erl program execution for an annual run can easily create an enormous computer file that is too large for most computer systems. ~It is possible for EnergyPlus to generate an EDD file that cannot be opened in traditional text editors.
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-eio.tex b/doc/output-details-and-examples/src/output-files/eplusout-eio.tex
new file mode 100644
index 00000000000..f5000786ec0
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-eio.tex
@@ -0,0 +1,7977 @@
+\section{eplusout.eio}\label{eplusout.eio}
+
+This file contains some standard and some optional ``reports''. It is intended to be a somewhat intelligent report of input conditions when they don't fit well in other places or when they aren't substantial enough for their own ``file''. (e.g. \textbf{eplusout.bnd})~ Contents of the file are somewhat documented in various places in the \href{file:///E:/Docs4PDFs/InputOutputReference.pdf}{Input Output Reference document} -- as results of objects. This file or portions of it can be easily imported into spreadsheet programs and more analysis done there. Contents of this file include construction details, location information, ``environment'' information, number of ``warmup'' days required in each environment.
+
+The form of the file is a data dictionary line followed by the data. In this case, the data dictionary line precedes the first ``data'' line though there may be several defining ``dictionary lines''. Each dictionary line will show the field as \textless{}field name\textgreater{} followed by other fields that will be in the data lines. Data will be displayed similarly. Each field of dictionary or data will be separated from the next by a comma ``,'' -- and produce a comma delimited file. However, the lines for data will not be contiguous -- some follow a stream of consciousness of the EnergyPlus execution.
+
+This section is subdivided into grouped sections by type.
+
+Note that the lines in the eplusout.eio file can be extremely long (current limit is 500 characters).
+
+\subsection{Simulation Parameters}\label{simulation-parameters}
+
+! \textless{}Version\textgreater{}, Version ID
+
+~Version, \textless{}version\textgreater{}
+
+! \textless{}Timesteps per Hour\textgreater{}, \#TimeSteps, Minutes per TimeStep
+
+~Timesteps Per Hour,~ 4, 15
+
+! \textless{}Run Control\textgreater{}, Do Zone Sizing, Do System Sizing, Do Plant Sizing, Do Design Days, Do Weather Simulation
+
+~Run Control, Yes, Yes, No, No, Yes
+
+! \textless{}GroundTemperatures\textgreater{}, Months From Jan to Dec \{Deg C\}
+
+~GroundTemperatures,~ 20.03,~ 20.03,~ 20.13,~ 20.30,~ 20.43,~ 20.52,~ 20.62,~ 20.77,~ 20.78,~ 20.55,~ 20.44,~ 20.20
+
+! \textless{}GroundTemperatures:Surface\textgreater{}, Months From Jan to Dec \{Deg C\}
+
+~GroundTemperatures:Surface,~ 18.00,~ 18.00,~ 18.00,~ 18.00,~ 18.00,~ 18.00,~ 18.00,~ 18.00,~ 18.00,~ 18.00,~ 18.00,~ 18.00
+
+! \textless{}GroundTemperatures:Deep\textgreater{}, Months From Jan to Dec \{Deg C\}
+
+~GroundTemperatures:Deep,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00
+
+! \textless{}GroundReflectances\textgreater{}, Months From Jan to Dec \{dimensionless\}
+
+~GroundReflectances,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20
+
+! \textless{}Snow Ground Reflectance Modifiers\textgreater{}, Normal, Daylighting \{dimensionless\}
+
+~Snow Ground Reflectance Modifiers,~~ 1.000,~~ 1.000
+
+! \textless{}Snow GroundReflectances\textgreater{}, Months From Jan to Dec \{dimensionless\}
+
+~Snow GroundReflectances,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20
+
+! \textless{}Snow GroundReflectances For Daylighting\textgreater{}, Months From Jan to Dec \{dimensionless\}
+
+~Snow GroundReflectances For Daylighting,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20
+
+! \textless{}Location\textgreater{}, Location Name, Latitude \{N+/S- Deg\}, Longitude \{E+/W- Deg\},~ Time Zone Number \{GMT+/-\}, Elevation \{m\},~ Standard Pressure at Elevation \{Pa\}
+
+Location,CHICAGO IL USA TMY2-94846 WMO\# = 725300,41.78,-87.75,-6.00,190.00,99063.
+
+! \textless{}Building Information\textgreater{}, Building Name,North Axis \{deg\},Terrain,~ Loads Convergence Tolerance Value,Temperature Convergence Tolerance Value,~ Solar Distribution,Maximum Number of Warmup Days,Minimum Number of Warmup Days
+
+~Building, BUILDING,~ 30.000,City,~~ 0.04000,~~ 0.40000,FullExterior,25,6
+
+! Inside Convection Algorithm, Value \{Simple \textbar{} Detailed \textbar{} CeilingDiffuser\}
+
+Inside Convection Algorithm,Simple
+
+! Outside Convection Algorithm, Value \{Simple \textbar{} Detailed\}
+
+Outside Convection Algorithm,Simple
+
+! Solution Algorithm, Value \{CTF \textbar{} EMPD \textbar{} CONDFD \textbar{} HAMT\}
+
+Solution Algorithm, CTF
+
+! Sky Radiance Distribution, Value \{Anisotropic\}
+
+Sky Radiance Distribution,Anisotropic
+
+! \textless{}Environment:Site Atmospheric Variation\textgreater{},Wind Speed Profile Exponent \{\},Wind Speed Profile Boundary Layer Thickness \{m\},Air Temperature Gradient Coefficient \{K/m\}
+
+Environment:Site Atmospheric Variation,0.330,460.000,6.500000E-003
+
+! \textless{} Input Surface Geometry Information\textgreater{},Starting Corner,Vertex Input Direction,Coordinate System
+
+~SurfaceGeometry,UpperLeftCorner,CounterClockwise,RelativeCoordinateSystem
+
+! \textless{}Program Control Information:Threads/Parallel Sims\textgreater{}, Threading Supported,Maximum Number of Threads, Env Set Threads (OMP\_NUM\_THREADS), EP Env Set Threads (EP\_OMP\_NUM\_THREADS). IDF Set Threads, Number of Threads Used (Interior Radiant Exchange), Number NominalSurface, Number Parallel Sims
+
+Program Control:Threads/Parallel Sims, Yes,2, Not Set, Not Set, Not Set, 2, 60, N/A
+
+The simulation parameters output is the simplest form of reporting in the \textbf{eplusout.eio} file. Each of the ``header'' records (lines starting with an ``!'') are followed immediately by the one and only data line. By and large, these data lines are all merely echoes of the entries in the IDF (or defaulted for blank fields). For most of these descriptions, you can look at the object fields (of same name) in the \href{file:///E:/Docs4PDFs/InputOutputReference.pdf}{Input Output Reference} document.
+
+\subsection{Version}\label{version}
+
+! \textless{}Version\textgreater{}, Version ID
+
+~Version, \textless{}version\textgreater{}
+
+This is the version of the IDF as entered in the IDF file. If it does not match the current EnergyPlus Version, a warning will be issued and show in the \textbf{eplusout.err} file.
+
+\subsection{Timestep}\label{timestep}
+
+! \textless{}Timesteps per Hour\textgreater{}, \#TimeSteps, Minutes per TimeStep
+
+~Timesteps Per Hour,~ 4, 15
+
+This is the number of timesteps in hour as entered in the IDF file as well as showing how many minutes will encompass each timestep (i.e.~4 timesteps in hour = 15 minutes per timestep).
+
+\subsection{SimulationControl}\label{simulationcontrol}
+
+! \textless{}Run Control\textgreater{}, Do Zone Sizing, Do System Sizing, Do Plant Sizing, Do Design Days, Do Weather Simulation, Do HVAC Sizing Simulation
+
+~Run Control, Yes, Yes, Yes, No, Yes, No
+
+This shows how the sizing and running (design days vs.~weather file) will be accomplished. Design days are required for sizing but do not necessarily need to be ``run'' after sizing has completed. Thus, the user can choose to do sizing, not do a ``normal'' calculation with the design day definitions but then go ahead and run the full simulation year. Some advanced sizing methods require also running HVAC Sizing Simulations.
+
+\subsection{Building}\label{building}
+
+! \textless{}Building Information\textgreater{}, Building Name,North Axis \{deg\},Terrain,~ Loads Convergence Tolerance Value,Temperature Convergence Tolerance Value,~ Solar Distribution,Maximum Number of Warmup Days
+
+~Building Information, BUILDING,~ 30.000,City,~~ 0.04000,~~ 0.40000,FullExterior,25
+
+This shows the values put in for the Building Object in the IDF.
+
+\subsection{Inside Convection Algorithm}\label{inside-convection-algorithm}
+
+! \textless{}Inside Convection Algorithm\textgreater{}, Value \{Simple \textbar{} Detailed \textbar{} CeilingDiffuser\}
+
+Inside Convection Algorithm,Simple
+
+This shows the global inside (interior) convection algorithm selected by the IDF value. This may be overridden by zone entries or even surface entries.
+
+\subsection{Outside Convection Algorithm}\label{outside-convection-algorithm}
+
+! \textless{}Outside Convection Algorithm\textgreater{}, Value \{Simple \textbar{} Detailed ! TARP ! MoWitt ! DOE-2 ! BLAST\}
+
+Outside Convection Algorithm,Simple
+
+This shows the global outside (exterior) convection algorithm selected by the IDF value. This may be overridden by zone entries or even surface entries.
+
+\subsection{Solution Algorithm}\label{solution-algorithm}
+
+! \textless{}Solution Algorithm\textgreater{}, Value \{CTF \textbar{} EMPD \textbar{} CONDFD \textbar{} HAMT\},Inside Surface Max Temperature Limit\{C\}
+
+Solution Algorithm, CTF,200
+
+This shows the solution algorithm approach selected by the IDF value and Inside Surface Max Temperature override or default value.
+
+\subsection{Sky Radiance Distribution}\label{sky-radiance-distribution}
+
+! \textless{}Sky Radiance Distribution\textgreater{}, Value \{Anisotropic\}
+
+Sky Radiance Distribution,Anisotropic
+
+This shows the solution algorithm approach used in the simulation. As this value cannot be changed by the user, it is shown for information only.
+
+\subsection{Site Atmospheric Variation}\label{site-atmospheric-variation}
+
+! \textless{}Environment:Site Atmospheric Variation\textgreater{},Wind Speed Profile Exponent \{\},Wind Speed Profile Boundary Layer Thickness \{m\},Air Temperature Gradient Coefficient \{K/m\}
+
+Environment:Site Atmospheric Variation,0.330,460.000,6.500000E-003
+
+This shows actual values used for Site Atmospheric Variations.
+
+\subsection{Shadowing/Sun Position Calculations}\label{shadowingsun-position-calculations}
+
+! \textless{}Shadowing/Sun Position Calculations\textgreater{} {[}Annual Simulations{]}, Calculation Method, Value \{days\}, Allowable Number Figures in Shadow Overlap \{\}, Polygon Clipping Algorithm, Sky Diffuse Modeling Algorithm
+
+Shadowing/Sun Position Calculations, AverageOverDaysInFrequency, 20, 15000, SutherlandHodgman, SimpleSkyDiffuseModeling
+
+This shows how many days between the re-calculation of solar position during a weather file simulation. While a smaller number of days will lead to a more accurate solar position estimation (solar position is important in shadowing as well as determining how much solar enters the space), it also increases the calculation time necessarily to complete the simulation. The default, re-calculating every 20 days, gives a good compromise. The allowable number of figures in a shadow overlap can be increased if necessary for the model. There are two calculation methods available: AverageOverDaysInFrequency (default) and DetailedTimestepIntegration.
+
+\subsection{AirflowNetwork Model:Control}\label{airflownetwork-modelcontrol}
+
+! \textless{}AirflowNetwork Model:Control\textgreater{}, No Multizone or Distribution/Multizone with Distribution/Multizone without Distribution/Multizone with Distribution only during Fan Operation
+
+AirflowNetwork Model:Control,MultizoneWithoutDistribution
+
+This shows the AirflowNetwork Model:Control selected by the IDF value in the object AirflowNetwork:SimulationControl.
+
+\subsection{AirflowNetwork Model:Wind Direction}\label{airflownetwork-modelwind-direction}
+
+! \textless{}AirflowNetwork Model:Wind Direction\textgreater{}, Wind Direction \#1 to n (degree)
+
+AirflowNetwork Model:Wind Direction, 0.0,30.0,60.0,90.0,120.0,150.0,180.0,210.0,240.0,270.0,300.0,330.0
+
+\subsubsection{Field: \textless{}AirflowNetwork Model:Wind Direction\textgreater{}}\label{field-airflownetwork-modelwind-direction}
+
+This field contains the field name ``AirflowNetwork Model:Wind Direction''.
+
+\subsubsection{Field: Wind Direction \#1 to n}\label{field-wind-direction-1-to-n}
+
+These values are the wind directions corresponding to the first through the Nth wind pressure coefficient value. If Wind Pressure Coefficient Type = Input in the AirflowNetwork:SimulationControl object, the wind directions described here are the inputs specified in the AirflowNetwork:MultiZone:WindPressureCoefficientArray object,. If Wind Pressure Coefficient Type = SurfaceAverageCalculation in the AirflowNetwork:SimulationControl object, the wind directions are also described here and are fixed at 30 degree increments.
+
+\subsection{AirflowNetwork Model:Wind Pressure Coefficients}\label{airflownetwork-modelwind-pressure-coefficients}
+
+! \textless{}AirflowNetwork Model:Wind Pressure Coefficients\textgreater{}, Name, Wind Pressure Coefficients \#1 to n (dimensionless)
+
+AirflowNetwork Model:Wind Pressure Coefficients, NFACADE\_WPCVALUE, 0.60,0.48,4.00E-002,-0.56,-0.56,-0.42,-0.37,-0.42,-0.56,-0.56,4.00E-002,0.48
+
+AirflowNetwork Model:Wind Pressure Coefficients, EFACADE\_WPCVALUE, -0.56,4.00E-002,0.48,0.60,0.48,4.00E-002,-0.56,-0.56,-0.42,-0.37,-0.42,-0.56
+
+AirflowNetwork Model:Wind Pressure Coefficients, SFACADE\_WPCVALUE, -0.37,-0.42,-0.56,-0.56,4.00E-002,0.48,0.60,0.48,4.00E-002,-0.56,-0.56,-0.42
+
+AirflowNetwork Model:Wind Pressure Coefficients, WFACADE\_WPCVALUE, -0.56,-0.56,-0.42,-0.37,-0.42,-0.56,-0.56,4.00E-002,0.48,0.60,0.48,4.00E-002
+
+\subsubsection{Field:~ \textless{} AirflowNetwork Model: Wind Pressure Coefficients\textgreater{}}\label{field-airflownetwork-model-wind-pressure-coefficients}
+
+This field contains the constant ``AirflowNetwork Model: Wind Pressure Coefficients'' for each line.
+
+\subsubsection{Field: Name}\label{field-name}
+
+This is the WindPressureCoefficientValues object name entered from the IDF.
+
+\subsubsection{Field: Wind Pressure Coefficients \#1 to n}\label{field-wind-pressure-coefficients-1-to-n}
+
+These values are the wind pressure coefficient for the building façade. These wind pressure coefficient values correspond to the first through Nth wind directions reported above for \textless{}AirflowNetwork Model:Wind Direction\textgreater{}. If Wind Pressure Coefficient Type = INPUT in the AirflowNetwork:SimulationControl object, the wind pressure coefficients described here are the inputs specified in the AirflowNetwork:MultiZone:Wind Pressure Coefficient Values object,. If Wind Pressure Coefficient Type = SurfaceAverageCalculation in the AirflowNetwork:SimulationControl object, the wind pressure coefficients are calculated internally and also described here.
+
+\subsection{Zone Volume Capacitance Multiplier}\label{zone-volume-capacitance-multiplier}
+
+! \textless{}Zone Volume Capacitance Multiplier\textgreater{}, Sensible Heat Capacity Multiplier, Moisture Capacity Multiplier, Carbon Dioxide Capacity Multiplier, Generic Contaminant Capacity Multiplier
+
+Zone Volume Capacitance Multiplier,~~ 1.000, 1.000, 1.000, 1.000
+
+This shows the zone volume capacitance multipliers selected by the IDF value or defaulted. The object for this item is ZoneCapacitanceMultiplier:ResearchSpecial.
+
+\subsubsection{Field: Sensible Heat Capacity Multiplier}\label{field-sensible-heat-capacity-multiplier}
+
+Value used to alter the effective heat capacitance of the zone air volume.
+
+\subsubsection{Field: Moisture Capacity Multiplier}\label{field-moisture-capacity-multiplier}
+
+Value used to alter the effective moisture capacitance of the zone air volume.
+
+\subsubsection{Field: Carbon Dioxide Capacity Multiplier}\label{field-carbon-dioxide-capacity-multiplier}
+
+Value used to alter the effective carbon dioxide capacitance of the zone air volume.
+
+\subsubsection{Field: Generic Contaminant Capacity Multiplier}\label{field-generic-contaminant-capacity-multiplier}
+
+Value used to alter the effective generic contaminant capacitance of the zone air volume.
+
+\subsubsection{Surface Geometry}\label{surface-geometry}
+
+! \textless{}SurfaceGeometry\textgreater{},Starting Corner,Vertex Input Direction,Coordinate System,Daylight Reference Point Coordinate System,Rectangular (Simple) Surface Coordinate System
+
+Surface Geometry, UpperLeftCorner, Counterclockwise, RelativeCoordinateSystem, RelativeCoordinateSystem, RelativeToZoneOrigin
+
+This shows the expected order of the vertices for each surface. The object for this item is GlobalGeometryRules.
+
+\subsubsection{Field: Starting Corner}\label{field-starting-corner}
+
+Value used to designate which corner the surface(s) start with.
+
+\subsubsection{Field: Vertex Input Direction}\label{field-vertex-input-direction}
+
+Value whether the coordinates for the surface are entered clockwise or counter-clockwise.
+
+\subsubsection{Field: Coordinate System}\label{field-coordinate-system}
+
+Value whether the coordinate system is World/Absolute or Relative.
+
+\subsubsection{Field: Daylight Reference Point Coordinate System}\label{field-daylight-reference-point-coordinate-system}
+
+If daylighting is used, this describes the coordinate system for entering daylight reference points.
+
+\subsubsection{Field: Rectangular (Simple) Surface Coordinate System}\label{field-rectangular-simple-surface-coordinate-system}
+
+For simple surfaces (Wall, Window, Door, and so forth) the coordinate system that is used to describe their starting point.
+
+\subsection{Program Control}\label{program-control}
+
+! \textless{}Program Control Information:Threads/Parallel Sims\textgreater{}, Threading Supported,Maximum Number of Threads, Env Set Threads (OMP\_NUM\_THREADS), EP Env Set Threads (EP\_OMP\_NUM\_THREADS). IDF Set Threads, Number of Threads Used (Interior Radiant Exchange), Number Nominal Surfaces, Number Parallel Sims
+
+Program Control:Threads/Parallel Sims, Yes,2, Not Set, Not Set, Not Set, 2, 60, N/A
+
+More examples:
+
+Program Control:Threads/Parallel Sims, Yes,2, Not Set, Not Set, Not Set, 1, 6, N/A
+
+Program Control:Threads/Parallel Sims, Yes,2, Not Set, Not Set, 1, 1, 46, N/A
+
+This describes the threading that may be active for the simulation. The ProgramControl object is used for this output. As described in that object, only the Interior Radiant Exchange calculation has been exposed to use threading, goal being to speed up calculations but may not always be the most beneficial.
+
+\subsubsection{Field: Threading Supported}\label{field-threading-supported}
+
+The compile of the program has to support threading (OpenMP for now). If it is compiled thus, this field will be \textbf{Yes}.~ Otherwise it will be \textbf{No}.
+
+\subsubsection{Field: Maximum Number of Threads}\label{field-maximum-number-of-threads}
+
+Regardless of whether the compile has supported threading, the system is queried for the number of threads possible -- that number is entered in this field.
+
+\subsubsection{Field: Env Set Threads (OMP\_NUM\_THREADS)}\label{field-env-set-threads-ompux5fnumux5fthreads}
+
+The Environment Variable OMP\_NUM\_THREADS can be manually inserted to set the number of system threads to be used. This would be reported here if set.~ If not set, \textbf{Not Set} will be shown. This is a system variable, but suggest that you use the following environment variable if you want to manually control the number of threads.
+
+\subsubsection{Field: EP Env Set Threads (EP\_OMP\_NUM\_THREADS)}\label{field-ep-env-set-threads-epux5fompux5fnumux5fthreads}
+
+The Environment Variable EP\_OMP\_NUM\_THREADS can be manually inserted to set the number of system threads to be used. This would be reported here if set.~ If not set, \textbf{Not Set} will be shown.
+
+\subsubsection{Field: IDF Set Threads}\label{field-idf-set-threads}
+
+If you use the ProgramControl object in your IDF, you can again manually control the number of threads to be used. This would be reported here if set.~ If not set, \textbf{Not Set} will be shown.
+
+\subsubsection{Field: Number of Threads Used (Interior Radiant Exchange)}\label{field-number-of-threads-used-interior-radiant-exchange}
+
+This is the number of threads that was actually used in the Interior Radiant Exchange routines (which calculates the interior surface temperatures).
+
+\subsubsection{Field: Number Nominal Surfaces}\label{field-number-nominal-surfaces}
+
+This is the number of ``nominal'' surfaces (based on surface objects) that a quick calculation from the program has found. If the number of surfaces is not greater than 30, then the number of threads to be used will be set by the program to 1.
+
+\subsubsection{Field: Number Parallel Sims}\label{field-number-parallel-sims}
+
+This is the number of windowed/parallel simulations being run simultaneously as set by EP-Launch or other scripts distributed with the EnergyPlus program. Third party distributions may also set this item.
+
+\subsection{Climate Group Outputs}\label{climate-group-outputs}
+
+Climate related variables appear in two places for EnergyPlus outputs. Certain objects that are invariant throughout a simulation period have lines appear in the eplusout.eio file:
+
+! \textless{}Environment:Weather Station\textgreater{},Wind Sensor Height Above Ground \{m\},Wind Speed Profile Exponent \{\},Wind Speed Profile Boundary Layer Thickness \{m\},Air Temperature Sensor Height Above Ground \{m\},Wind Speed Modifier Coefficient {[}Internal{]},Temperature Modifier Coefficient {[}Internal{]}
+
+Environment:Weather Station,10.000,0.140,270.000,1.500,1.586,9.750E-003
+
+! \textless{}Environment:Site Atmospheric Variation\textgreater{},Wind Speed Profile Exponent \{\},Wind Speed Profile Boundary Layer Thickness \{m\},Air Temperature Gradient Coefficient \{K/m\}
+
+Environment:Site Atmospheric Variation,~~ 0.220, 370.000, 0.006500
+
+! \textless{}Location\textgreater{}, Location Name, Latitude, Longitude, Time Zone Number, Elevation \{m\}
+
+~Location, DENVER COLORADO,~~ 39.75, -104.87,~~ -7.00,~~~~~ 1610.26
+
+In addition for each ``environment'' simulated, information about the environment is shown:
+
+! \textless{}Environment\textgreater{},Environment Name,Environment Type, Start Date, End Date, Start DayOfWeek, Duration \{\#days\}, Source:Start DayOfWeek,~ Use Daylight Savings, Use Holidays, Apply Weekend Holiday Rule
+
+! \textless{}Environment:Special Days\textgreater{}, Special Day Name, Special Day Type, Source, Start Date, Duration \{\#days\}
+
+! \textless{}Environment:Daylight Saving\textgreater{}, Daylight Saving Indicator, Source, Start Date, End Date
+
+! \textless{}Environment:Design\_Day\_Misc\textgreater{},DayOfYear,ASHRAE A Coeff,ASHRAE B Coeff,ASHRAE C Coeff,Solar Constant-Annual Variation,Eq of Time \{minutes\}, Solar Declination Angle \{deg\}, Solar Model
+
+! \textless{}Environment:WarmupDays\textgreater{}, NumberofWarmupDays
+
+For example, a DesignDay:
+
+Environment,PHOENIX ARIZONA WINTER,DesignDay, 1/21, 1/21,MONDAY,~ 1,N/A,N/A,N/A,N/A
+
+Environment:Daylight Saving,No,DesignDay
+
+Environment:Design\_Day\_Misc, 21,1228.9,0.1414,5.7310E-002,1.0,-11.14,-20.0
+
+A Design RunPeriod:
+
+Environment,EXTREME SUMMER WEATHER PERIOD FOR DESIGN,User Selected WeatherFile Typical/Extreme Period (Design) = Summer Extreme,07/13,07/19,SummerDesignDay,~ 7,Use RunPeriod Specified Day,No ,No ,No ,No ,No
+
+Environment:Daylight Saving,No,RunPeriod Object
+
+Environment:WarmupDays,~ 3
+
+Or a RunPeriod (Name listed in the RunPeriod output is dependent on user input for the RunPeriod object -- when a blank is input, the name of the weather file location is used):
+
+Environment,CHICAGO IL TMY2-94846 WMO\# = 725300,WeatherRunPeriod, 1/ 1,12/31,SUNDAY,365,UseWeatherFile,Yes,Yes,No
+
+Environment:Daylight Saving,No,
+
+Environment:Special Days,NEW YEARS DAY,Holiday,WeatherFile, 1/ 1,~ 1
+
+Environment:Special Days,MEMORIAL DAY,Holiday,WeatherFile, 5/31,~ 1
+
+Environment:Special Days,INDEPENDENCE DAY,Holiday,WeatherFile, 7/ 5,~ 1
+
+Environment:Special Days,LABOR DAY,Holiday,WeatherFile, 9/ 6,~ 1
+
+Environment:Special Days,THANKSGIVING,Holiday,WeatherFile,11/25,~ 1
+
+Environment:Special Days,CHRISTMAS,Holiday,WeatherFile,12/25,~ 1
+
+Environment:WarmupDays,~ 4
+
+Note that in this display, using ``weekend rule'' and specific date holidays, the actual observed dates are shown in the output display -- in the example above, Independence Day (July 4) is actually observed on July 5.
+
+\subsection{Climate Group -- Simple Outputs}\label{climate-group-simple-outputs}
+
+Some of the climate outputs are a ``simple'' group. The ``header'' line is followed immediately by the data line.
+
+\subsection{Location}\label{location}
+
+This output represents the location data used for the simulation. Note that if a runperiod is used, the IDF ``Location'' is ignored and the location from the weather file is used instead.
+
+\subsubsection{Field: \textless{}Location\textgreater{}}\label{field-location}
+
+This data field will contain the constant ``Location''.
+
+\subsubsection{Field: Location Name}\label{field-location-name}
+
+This is the name given to the location whether from the IDF or the weather file.
+
+\subsubsection{Field: Latitude}\label{field-latitude}
+
+This is the latitude of the site, expressed decimally. Convention uses positive (+) values for North of the Equator and negative (-) values for South of the Equator. For example, S 30° 15' is expressed as --30.25.
+
+\subsubsection{Field: Longitude}\label{field-longitude}
+
+This is the longitude of the site, expressed decimally. Convention uses positive (+) values for East of the Greenwich meridian and negative (-) values for West of the Greenwich meridian. For example, E 130° 45' is expressed as +130.75.
+
+\subsubsection{Field: Time Zone Number}\label{field-time-zone-number}
+
+This is the time zone of the site, expressed decimally. Convention uses positive (+) values for GMT+ (Longitude East of the Greenwich meridian) and negative (-) values for GMT- (Longitude West of the Greenwich meridian). For example, the time zone for Central US time is --6. The time zone for parts of Newfoundland is --3.5 (-3 hours, 30 minutes from GMT).
+
+\subsubsection{Field: Elevation \{m\}}\label{field-elevation-m}
+
+This is the elevation of the site. Units are m.
+
+\subsection{Weather Station}\label{weather-station}
+
+\subsubsection{Field: Wind Sensor Height Above Ground \{m\}}\label{field-wind-sensor-height-above-ground-m}
+
+This is the wind sensor height above ground for weather data measurements.
+
+\subsubsection{Field: Wind Speed Profile Exponent}\label{field-wind-speed-profile-exponent}
+
+The wind speed profile exponent for the terrain surrounding the weather station.
+
+\subsubsection{Field: Wind Speed Profile Boundary Layer Thickness \{m\}}\label{field-wind-speed-profile-boundary-layer-thickness-m}
+
+The wind speed profile boundary layer thickness {[}m{]} for the terrain surrounding the weather station.
+
+\subsubsection{Field: Air Temperature Sensor Height Above Ground \{m\}}\label{field-air-temperature-sensor-height-above-ground-m}
+
+The height {[}m{]} above ground for the air temperature sensor.
+
+\subsubsection{Field: Wind Speed Modifier Coefficient {[}Internal{]}}\label{field-wind-speed-modifier-coefficient-internal}
+
+This field is intended to provide a slight help for the user to determine the calculations that will be used to calculate the Wind Speed at a specific height at the site.
+
+The full calculation for Local Wind Speed is:
+
+\begin{equation}
+\text{LocalWindSpeed} = \text{WindSpeed}_{met} \left( \frac{\text{WindBoundaryLayerThickness}_{met}}{\text{AirSensorHeight}_{met}} \right)^{\text{WindExponent}_{met}} \left(\frac{\text{HeightAboveGround}_{site/component}}{\text{WindBoundaryLayerThickness}_{site}}\right)^{\text{SiteWindExponent}}
+\end{equation}
+
+The Wind Speed Modifier Coefficient {[}Internal{]} simplifies the equation to:
+
+\begin{equation}
+\text{LocalWindSpeed} = \text{WindSpeed}_{met} \left( \text{WindSpeedModifier} \right) \left(\frac{\text{HeightAboveGround}_{site/component}}{\text{WindBoundaryLayerThickness}_{site}}\right)^{\text{SiteWindExponent}}
+\end{equation}
+
+Where the Wind Speed Modifier encapsulates:
+
+\begin{equation}
+\text{WindSpeedModifier} = \left( \frac{\text{WindBoundaryLayerThickness}_{met}}{\text{AirSensorHeight}_{met}} \right)^{\text{WindExponent}_{met}}
+\end{equation}
+
+Where
+
+\begin{itemize}
+\tightlist
+\item
+  met = meteorological station
+\item
+  site = location of the building
+\end{itemize}
+
+\subsubsection{Field:Temperature Modifier Coefficient {[}Internal{]}}\label{fieldtemperature-modifier-coefficient-internal}
+
+This field is intended to provide a slight help for the user to determine the calculations that will be used to calculate the air (dry-bulb) or wet-bulb temperature at a specific height at the site.
+
+The site temperature modifier coefficient (TMC) is defined as:
+
+\begin{equation}
+TMC = frac{ \text{AtmosphericTemperatureGradient} \cdot \text{EarthRadius} \cdot \text{TemperatureSensorHeight}_{met} }
+                  { \text{EarthRadius} + \text{TemperatureSensorHeight}_{met} }
+\end{equation}
+
+Then, the temperature at a height above ground is calculated as:
+
+\begin{equation}
+\text{ActualTemperature} = \text{Temperature}_{met} + TMC - 
+    frac{ \text{TemperatureGradient}_{site} * \text{EarthRadius} * \text{Height}_{site/component} }
+        { \text{EarthRadius} + \text{Height}_{site/component} }
+\end{equation}
+
+Where
+
+\begin{itemize}
+\tightlist
+\item
+  met = meteorological station
+\item
+  site = location of the building
+\end{itemize}
+
+\subsection{Site Atmospheric Variation}\label{site-atmospheric-variation-1}
+
+\subsubsection{Field: Wind Speed Profile Exponent}\label{field-wind-speed-profile-exponent-1}
+
+The wind speed profile exponent for the terrain surrounding the site.
+
+\subsubsection{Field: Wind Speed Profile Boundary Layer Thickness \{m\}}\label{field-wind-speed-profile-boundary-layer-thickness-m-1}
+
+The wind speed profile boundary layer thickness {[}m{]} for the terrain surrounding the site.
+
+\subsubsection{Field: Air Temperature Gradient Coefficient \{K/m\}}\label{field-air-temperature-gradient-coefficient-km}
+
+The air temperature gradient coefficient {[}K/m{]} is a research option that allows the user to control the variation in outdoor air temperature as a function of height above ground. The real physical value is 0.0065 K/m.
+
+\subsection{Ground Temperatures and Ground Reflectances}\label{ground-temperatures-and-ground-reflectances}
+
+! \textless{}Site:GroundTemperature:BuildingSurface\textgreater{}, Months From Jan to Dec \{Deg C\}
+
+~Site:GroundTemperature:BuildingSurface,~ 20.03,~ 20.03,~ 20.13,~ 20.30,~ 20.43,~ 20.52,~ 20.62,~ 20.77,~ 20.78,~ 20.55,~ 20.44,~ 20.20
+
+! \textless{}Site:GroundTemperature:FCfactorMethod\textgreater{}, Months From Jan to Dec \{Deg C\}
+
+~Site:GroundTemperature:FCfactorMethod,~ -1.89,~ -3.06,~ -0.99,~~ 2.23,~ 10.68,~ 17.20,~ 21.60,~ 22.94,~ 20.66,~ 15.60,~~ 8.83,~~ 2.56
+
+! \textless{}Site:GroundTemperature:Shallow\textgreater{}, Months From Jan to Dec \{Deg C\}
+
+~Site:GroundTemperature:Shallow,~ 13.00,~ 13.00,~ 13.00,~ 13.00,~ 13.00,~ 13.00,~ 13.00,~ 13.00,~ 13.00,~ 13.00,~ 13.00,~ 13.00
+
+! \textless{}Site:GroundTemperature:Deep\textgreater{}, Months From Jan to Dec \{Deg C\}
+
+~Site:GroundTemperature:Deep,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00,~ 16.00
+
+! \textless{}Site:GroundReflectance\textgreater{}, Months From Jan to Dec \{dimensionless\}
+
+~Site:GroundReflectance,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20
+
+! \textless{}Site:GroundReflectance:SnowModifier\textgreater{}, Normal, Daylighting \{dimensionless\}
+
+~Site:GroundReflectance:SnowModifier,~~ 1.000,~~ 1.000
+
+! \textless{}Site:GroundReflectance:Snow\textgreater{}, Months From Jan to Dec \{dimensionless\}
+
+~Site:GroundReflectance:Snow,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20
+
+! \textless{}Site:GroundReflectance:Snow:Daylighting\textgreater{}, Months From Jan to Dec \{dimensionless\}
+
+~Site:GroundReflectance:Snow:Daylighting,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20,~ 0.20
+
+\subsection{Ground Temperatures}\label{ground-temperatures}
+
+\subsubsection{Field: \textless{}GroundTemperatures\textgreater{}}\label{field-groundtemperatures}
+
+This data field will contain the constant ``GroundTemperatures''.
+
+\subsubsection{Field Set (1-12) -- Monthly Ground Temperatures}\label{field-set-1-12-monthly-ground-temperatures}
+
+There will be a set of 12 numbers -- the ground temperatures by month: January, February, March, April, May, June, July, August, September, October, November, December. Units are C.
+
+\subsection{Ground Reflectance}\label{ground-reflectance}
+
+\subsubsection{Field: \textless{}GroundReflectances\textgreater{}}\label{field-groundreflectances}
+
+This data field will contain the constant ``GroundReflectances''.
+
+\subsubsection{Field Set (1-12) -- Monthly Ground Reflectances}\label{field-set-1-12-monthly-ground-reflectances}
+
+There will be a set of 12 numbers -- the ground reflectances by month: January, February, March, April, May, June, July, August, September, October, November, December.
+
+\subsection{Snow Ground Reflectance Modifiers}\label{snow-ground-reflectance-modifiers}
+
+It is generally accepted that snow resident on the ground increases the basic ground reflectance. EnergyPlus allows the user control over the snow ground reflectance for both ``normal ground reflected solar'' calculations (see above) and snow ground reflected solar modified for daylighting. This is the display of the user entered or defaulted values.
+
+\subsubsection{Field: \textless{}Snow Ground Reflectance~ Modifiers\textgreater{}}\label{field-snow-ground-reflectance-modifiers}
+
+This data field will contain the constant ``Snow Ground Reflectance Modifiers''.
+
+\subsubsection{Field: Normal}\label{field-normal}
+
+This field is the value between 0.0 and 1.0 which is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values).
+
+\begin{equation}
+\text{GroundReflectance}_{used} = \text{GroundReflectance} \cdot \text{Modifier}_{snow}
+\end{equation}
+
+\subsubsection{Field: Daylighting}\label{field-daylighting}
+
+This field is the value between 0.0 and 1.0 which is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values).
+
+\begin{equation}
+\text{DaylightingGroundReflectance}_{used} = \text{GroundReflectance} \cdot \text{Modifier}_{snow}
+\end{equation}
+
+\subsection{Snow Ground Reflectance}\label{snow-ground-reflectance}
+
+This data is the result of using the Snow Ground Reflectance modifier and the basic Ground Reflectance value.
+
+\subsubsection{Field: \textless{}GroundReflectances\textgreater{}}\label{field-groundreflectances-1}
+
+This data field will contain the constant ``Snow GroundReflectances''.
+
+\subsubsection{Field Set (1-12) -- Monthly Snow Ground Reflectances}\label{field-set-1-12-monthly-snow-ground-reflectances}
+
+There will be a set of 12 numbers -- the snow ground reflectances by month: January, February, March, April, May, June, July, August, September, October, November, December.
+
+\subsection{Snow Ground Reflectance for Daylighting}\label{snow-ground-reflectance-for-daylighting}
+
+This data is the result of using the Snow Ground Reflectance for Daylighting modifier and the basic Ground Reflectance value.
+
+\subsubsection{Field: \textless{} Snow GroundReflectances For Daylighting\textgreater{}}\label{field-snow-groundreflectances-for-daylighting}
+
+This data field will contain the constant ``Snow GroundReflectances For Daylighting''.
+
+\subsubsection{Field Set (1-12) -- Monthly Snow Ground Reflectances for Daylighting}\label{field-set-1-12-monthly-snow-ground-reflectances-for-daylighting}
+
+There will be a set of 12 numbers -- the ground reflectances by month: January, February, March, April, May, June, July, August, September, October, November, December.
+
+\subsection{Climate Group -- Not so Simple Outputs}\label{climate-group-not-so-simple-outputs}
+
+For each ``environment'' simulated, a set of outputs is produced. The header group is only produced once. (The Design Day Misc header is produced only when there is a design day.)
+
+! \textless{}Environment\textgreater{},Environment Name,Environment Type, Start Date, End Date, Start DayOfWeek, Duration \{\#days\}, Source:Start DayOfWeek,~ Use Daylight Saving, Use Holidays, Apply Weekend Holiday Rule
+
+! \textless{}Environment:Special Days\textgreater{}, Special Day Name, Special Day Type, Source, Start Date, Duration \{\#days\}
+
+! \textless{}Environment:Daylight Saving\textgreater{}, Daylight Saving Indicator, Source, Start Date, End Date
+
+! \textless{}Environment:Design\_Day\_Misc\textgreater{},DayOfYear,ASHRAE A Coeff,ASHRAE B Coeff,ASHRAE C Coeff,Solar Constant-Annual Variation,Eq of Time \{minutes\}, Solar Declination Angle \{deg\}
+
+! \textless{}Environment:WarmupDays\textgreater{}, NumberofWarmupDays
+
+\subsection{Environment Line}\label{environment-line}
+
+Each ``environment'' (i.e.~each design day, each run period) will have this line shown.
+
+\subsubsection{Field: \textless{}Environment\textgreater{}}\label{field-environment}
+
+This field will have the constant ``Environment'' in each data line.
+
+\subsubsection{Field:Environment Name}\label{fieldenvironment-name}
+
+This field will have the ``name'' of the environment. For example, the design day name (``DENVER COLORADO SUMMER'') or the weather file location name (``BOULDER CO TMY2-94018 WMO\# = 724699'').
+
+\subsubsection{Field:Environment Type}\label{fieldenvironment-type}
+
+This will be ``DesignDay'' for design day simulations and ``WeatherRunPeriod'' for weather file run periods.
+
+\subsubsection{Field: Start Date}\label{field-start-date}
+
+This will have the month/day that is the starting date for the simulation period. (7/21, for example).
+
+\subsubsection{Field: End Date}\label{field-end-date}
+
+This will have the month/day that is the ending date for the simulation period. Note that Design Days are only one day and the end date will be the same as the start date.
+
+\subsubsection{Field: Start DayOfWeek}\label{field-start-dayofweek}
+
+For weather periods, this will be the designated starting day of week. For design days, it will be the day type listed for the design day object (e.g.~SummerDesignDay or Monday).
+
+\subsubsection{Field: Duration \{\#days\}}\label{field-duration-days}
+
+Number of days in the simulation period will be displayed in this field. Design days are only 1 day.
+
+\subsubsection{Field: Source:Start DayOfWeek}\label{field-sourcestart-dayofweek}
+
+This field will list the ``source'' of the Start Day of Week listed earlier. This could be the RunPeriod command from the input file or the Weather File if the UseWeatherFile option was chosen in the RunPeriod command. For design days, this will be ``N/A''.
+
+\subsubsection{Field: Use Daylight Saving}\label{field-use-daylight-saving}
+
+This field reflects the value of the Use Daylight Saving field of the RunPeriod object. For design days, this will be ``N/A''.
+
+\subsubsection{Field: Use Holidays}\label{field-use-holidays}
+
+This field reflects the value of the Use Holidays field of the RunPeriod object. For design days, this will be ``N/A''.
+
+\subsubsection{Field: Apply Weekend Holiday Rule}\label{field-apply-weekend-holiday-rule}
+
+For design days, this will show ``N/A''. For weather periods, this will show ``Yes'' if the Apply Weekend Holiday Rule is in effect or ``No'' if it isn't.
+
+\subsection{Design Day Misc Line}\label{design-day-misc-line}
+
+This line is shown for each design day simulated. It is not shown for sizing runs that do not subsequently use the design day as a simulation period.
+
+\subsubsection{Field: \textless{}Design Day Misc\textgreater{}}\label{field-design-day-misc}
+
+This is a constant that will display ``Environment:Design\_Day\_Misc''.
+
+\subsubsection{Field:DayOfYear}\label{fielddayofyear}
+
+This is the Julian day of year for the design day (i.e.~Jan 1 is 1, Jan 31 is 31).
+
+\subsubsection{Field:ASHRAE A Coeff}\label{fieldashrae-a-coeff}
+
+Reference ASHRAE HOF 30 -- this is the A Coefficient in Wh/m\(^{2}\) calculated from EnergyPlus.
+
+\subsubsection{Field:ASHRAE B Coeff}\label{fieldashrae-b-coeff}
+
+Likewise, this is the ASHRAE B Coefficient (dimensionless).
+
+\subsubsection{Field:ASHRAE C Coeff}\label{fieldashrae-c-coeff}
+
+This is the ASHRAE C Coefficient (dimensionless).
+
+\subsubsection{Field:Solar Constant-Annual Variation}\label{fieldsolar-constant-annual-variation}
+
+This is the calculated solar constant using the given location and day of year.
+
+\subsubsection{Field:Eq of Time \{minutes\}}\label{fieldeq-of-time-minutes}
+
+This is the calculated equation of time (minutes) using the given location and day of year.
+
+\subsubsection{Field: Solar Declination Angle \{deg\}}\label{field-solar-declination-angle-deg}
+
+This is the solar declination angle for the day of year, degrees.
+
+\subsection{Special Day Line}\label{special-day-line}
+
+\subsubsection{Field: \textless{}Environment:Special Days\textgreater{}}\label{field-environmentspecial-days}
+
+This is a constant that will display ``Environment:SpecialDays''.
+
+\subsubsection{Field: Special Day Name}\label{field-special-day-name}
+
+This is the user designated name for the special day.
+
+\subsubsection{Field: Special Day Type}\label{field-special-day-type}
+
+This shows the type for the special day (e.g.~Holiday).
+
+\subsubsection{Field: Source}\label{field-source}
+
+This will display ``InputFile'' if it was specified in the IDF or ``WeatherFile'' if it came from the weather file designation.
+
+\subsubsection{Field: Start Date}\label{field-start-date-1}
+
+This shows the starting date as month/day (e.g.~7/4).
+
+\subsubsection{Field: Duration \{\#days\}}\label{field-duration-days-1}
+
+This shows how many days the special day period continues. Usually, holidays are only 1 day duration.
+
+\subsection{Daylight Saving Line}\label{daylight-saving-line}
+
+\subsubsection{Field: \textless{}Environment:Daylight Saving\textgreater{}}\label{field-environmentdaylight-saving}
+
+This is a constant that will display ``Environment:DaylightSaving''.
+
+\subsubsection{Field: Daylight Saving Indicator}\label{field-daylight-saving-indicator}
+
+This will be Yes if daylight saving is to be observed for this simulation period and No if it is not observed.
+
+\subsubsection{Field: Source}\label{field-source-1}
+
+This will show the source of this invocation (or non-invocation). Inputfile if DaylightSavingPeriod was entered (weather files only), WeatherFile if used in the Weather file and selected in the Run Period object and designday if that was the source.
+
+\subsubsection{Field: Start Date}\label{field-start-date-2}
+
+If the indicator field is Yes, then this field will be displayed and the month/day (e.g.~4/1) that starts the daylight saving period observance will be shown.
+
+\subsubsection{Field: End Date}\label{field-end-date-1}
+
+If the indicator field is Yes, then this field will be displayed and the month/day (e.g.~10/29) that ends the daylight saving period observance will be shown.
+
+\subsection{Zone Outputs}\label{zone-outputs}
+
+\subsection{Zone Summary}\label{zone-summary}
+
+An overall zone summary is shown:
+
+! \textless{}Zone Summary\textgreater{}, Number of Zones, Number of Surfaces, Number of SubSurfaces
+
+~Zone Summary,19,158,12
+
+As indicated:
+
+\subsubsection{Field: \textless{}Zone Summary\textgreater{}}\label{field-zone-summary}
+
+This field contains the constant ``Zone Summary''.
+
+\subsubsection{Field: Number of Zones}\label{field-number-of-zones}
+
+This field will contain the number of zones in the simulation.
+
+\subsubsection{Field: Number of Surfaces}\label{field-number-of-surfaces}
+
+This field will contain the total number of surfaces in the simulation.
+
+\subsubsection{Field: Number of SubSurfaces}\label{field-number-of-subsurfaces}
+
+This field will contain the total number of subsurfaces in the simulation.
+
+\subsection{Zone Information}\label{zone-information}
+
+Each zone is summarized in a simple set of statements as shown below:
+
+! \textless{}Zone Information\textgreater{},Zone Name,North Axis \{deg\},Origin X-Coordinate \{m\},Origin Y-Coordinate \{m\},Origin Z-Coordinate \{m\},Centroid X-Coordinate \{m\},Centroid Y-Coordinate \{m\},Centroid Z-Coordinate \{m\},Type,Zone Multiplier,Zone List Multiplier,Minimum X \{m\},Maximum X \{m\},Minimum Y \{m\},Maximum Y \{m\},Minimum Z \{m\},Maximum Z \{m\},Ceiling Height \{m\},Volume \{m3\},Zone Inside Convection Algorithm \{Simple-Detailed-CeilingDiffuser-TrombeWall\},Zone Outside Convection Algorithm \{Simple-Detailed-Tarp-MoWitt-DOE-2-BLAST\}, Floor Area \{m2\},Exterior Gross Wall Area \{m2\},Exterior Net Wall Area \{m2\},Exterior Window Area \{m2\}, Number of Surfaces, Number of SubSurfaces, Number of Shading SubSurfaces,~ Part of Total Building Area
+
+~Zone Information, PSI FOYER,0.0,0.00,0.00,0.00,8.56,-1.80,2.27,1,1,1,0.00,16.34,-9.51,4.88,0.00,6.10,3.81,368.12,Detailed,DOE-2,96.62,70.61,70.61,106.84,6,1,0,Yes
+
+~Zone Information, DORM ROOMS AND COMMON AREAS,0.0,0.00,6.10,0.00,18.35,11.26,3.05,1,1,1,3.57,31.70,-4.75,25.36,0.00,6.10,6.10,2723.33,Detailed,DOE-2,445.93,312.15,267.56,52.59,10,22,0,Yes
+
+~Zone Information, LEFT FORK,-36.9,0.00,31.70,0.00,22.07,31.46,3.05,1,1,1,19.02,25.12,25.36,37.55,0.00,6.10,6.10,453.07,Detailed,DOE-2,74.32,185.81,135.64,50.17,6,10,0,Yes
+
+~Zone Information, MIDDLE FORK,0.0,4.88,35.36,0.00,31.21,28.41,3.05,1,1,1,25.12,37.31,21.70,35.11,0.00,6.10,6.10,453.07,Detailed,DOE-2,74.32,185.81,155.71,30.10,6,1,0,Yes
+
+~Zone Information, RIGHT FORK,36.9,10.97,35.36,0.00,36.70,20.48,3.05,1,1,1,29.99,43.40,15.85,25.12,0.00,6.10,6.10,453.07,Detailed,DOE-2,74.32,185.81,135.64,50.17,6,10,0,Yes
+
+\subsubsection{Field:~ \textless{}Zone Information\textgreater{}}\label{field-zone-information}
+
+This field contains the constant ``Zone Information'' for each line.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name}
+
+This is the Zone Name entered from the IDF.
+
+\subsubsection{Field: North Axis \{deg\}}\label{field-north-axis-deg}
+
+This is the North Axis entered from the IDF. Note that this is used primarily in the positioning of the building when ``relative'' coordinates are used -- however, the Daylighting:Detailed object also uses this. Units are degrees, clockwise from North.
+
+\subsubsection{Fields: X Origin \{m\}, Y Origin \{m\}, Z Origin \{m\}}\label{fields-x-origin-m-y-origin-m-z-origin-m}
+
+This is the origin vertex \{X,Y,Z\} entered from the IDF. Note that this is used primarily in the positioning of the building when ``relative'' coordinates are used -- however, the Daylighting:Detailed object also uses this. Units are m.
+
+\subsubsection{Field: TypeField: Multiplier}\label{field-typefield-multiplier}
+
+This is the multiplier (must be integral) entered from the IDF.
+
+\subsubsection{Field: Ceiling Height \{m\}}\label{field-ceiling-height-m}
+
+This is the ceiling height entered, if any, in the IDF. Ceiling height is also heuristically calculated from the surfaces in the zone -- however, not all surfaces need to be entered and sometimes the user would rather enter the ceiling height for the zone. If no ceiling height was entered (i.e.~the default of 0), this field will be the calculated value. A minor warning message will be issued if the calculated value is significantly different than the entered value. Units are m.
+
+\subsubsection{Field: Volume \{m3\}}\label{field-volume-m3}
+
+Like the ceiling height, this user can also enter this value in the IDF. Volume is also heuristically calculated using the ceiling height (entered or calculated) as well as the calculated floor area (see later field). If entered here, this value will be used rather than the calculated value. A minor warning message will be issued if the calculated value is significantly different than the entered value. Units are m\(^{3}\).
+
+\subsubsection{Field: Zone Inside Convection Algorithm \{Simple-Detailed-CeilingDiffuser-TrombeWall\}}\label{field-zone-inside-convection-algorithm-simple-detailed-ceilingdiffuser-trombewall}
+
+The interior convection algorithm shown earlier (entire building) can be overridden for each zone by an entry in the individual Zone object. This field will show which method is operational for the zone.
+
+\subsubsection{Field:~ Floor Area \{m2\}}\label{field-floor-area-m2}
+
+This field is calculated from the floor surfaces entered for the zone. Units are m\(^{2}\).
+
+\subsubsection{Field: Exterior Gross Wall Area \{m2\}}\label{field-exterior-gross-wall-area-m2}
+
+This field is calculated from the exterior wall surfaces entered for the zone. Units are m\(^{2}\).
+
+\subsubsection{Field: Exterior Net Wall Area \{m2\}}\label{field-exterior-net-wall-area-m2}
+
+This field is calculated from the exterior wall surfaces entered for the zone. Any sub-surface area is subtracted from the gross area to determine the net area. Units are m\(^{2}\).
+
+\subsubsection{Field: Exterior Window Area \{m2\}}\label{field-exterior-window-area-m2}
+
+This field is calculated from the exterior window surfaces entered for the zone. Units are m\(^{2}\).
+
+\subsubsection{Field: Number of Surfaces}\label{field-number-of-surfaces-1}
+
+This field is a count of the number of base surfaces in the zone.
+
+\subsubsection{Field: Number of SubSurfaces}\label{field-number-of-subsurfaces-1}
+
+This field is a count of the number of subsurfaces (windows, doors, glass doors and the list) in the zone.
+
+\subsubsection{Field: Number of Shading SubSurfaces}\label{field-number-of-shading-subsurfaces}
+
+This field is a count of the number of shading surfaces (overhangs, fins) for the zone.
+
+\subsubsection{Field: Part of Total Building Area}\label{field-part-of-total-building-area}
+
+This field displays ``Yes'' when the zone is to be considered part of the total building floor area or ``No'' when it's not to be considered. This consideration has no impact on simulation but on reporting. Namely, when the value is ``no'', the zone is not part of the Total Floor Area as shown in the Annual Building Utility Performance Summary tables. In addition, when ``No'' is specified, the area is excluded from both the conditioned floor area and the total floor area in the Building Area sub table and the Normalized Metrics sub tables.
+
+\subsection{Internal Gains Outputs}\label{internal-gains-outputs}
+
+\subsection{Zone Internal Gains}\label{zone-internal-gains}
+
+Nominal Zone Internal Gains (people, lights, electric equipment, etc.) are summarized:
+
+! \textless{}Zone Internal Gains/Equipment Information - Nominal\textgreater{},Zone Name, Floor Area \{m2\},\# Occupants,Area per Occupant \{m2/person\},Occupant per Area \{person/m2\},Interior Lighting \{W/m2\},Electric Load \{W/m2\},Gas Load \{W/m2\},Other Load \{W/m2\},Hot Water Eq \{W/m2\},Steam Equipment \{W/m2\},Sum Loads per Area \{W/m2\},Outdoor Controlled Baseboard Heat
+
+~Zone Internal Gains, PLENUM-1,463.60,0.0,N/A,0.000,0.000,0.000,0.000,0.000,0.000,0.000,0.000,No
+
+~Zone Internal Gains, SPACE1-1,99.16,11.0,9.015,0.111,15.974,10.649,0.000,0.000,0.000,0.000,26.624,No
+
+~Zone Internal Gains, SPACE2-1,42.74,5.0,8.547,0.117,16.006,10.670,0.000,0.000,0.000,0.000,26.676,No
+
+~Zone Internal Gains, SPACE3-1,96.48,11.0,8.771,0.114,16.418,10.945,0.000,0.000,0.000,0.000,27.363,No
+
+~Zone Internal Gains, SPACE4-1,42.74,5.0,8.547,0.117,16.006,10.670,0.000,0.000,0.000,0.000,26.676,No
+
+~Zone Internal Gains, SPACE5-1,182.49,20.0,9.125,0.110,16.242,10.828,0.000,0.000,0.000,0.000,27.070,No
+
+\subsubsection{Field:~ \textless{}Zone Internal Gains/Equipment Information - Nominal\textgreater{}}\label{field-zone-internal-gainsequipment-information---nominal}
+
+This field contains the constant ``Zone Internal Gains'' for each line.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-1}
+
+This is the Zone Name entered from the IDF.
+
+\subsubsection{Field: Floor Area \{m2\}}\label{field-floor-area-m2-1}
+
+This is the floor area for the zone.
+
+\subsubsection{Field: \# Occupants}\label{field-occupants}
+
+This is the nominal number of occupants (from the PEOPLE statements).
+
+\subsubsection{Field: Area per Occupant \{m2/person\}}\label{field-area-per-occupant-m2person}
+
+This is the Zone Floor Area per occupant (person).
+
+\subsubsection{Field: Occupant per Area \{person/m2\}}\label{field-occupant-per-area-personm2}
+
+This is the number of occupants per area.
+
+\subsubsection{Field: Interior Lighting \{W/m2\}}\label{field-interior-lighting-wm2}
+
+This is the lighting (Lights) per floor area.
+
+\subsubsection{Field: Electric Load \{W/m2\}}\label{field-electric-load-wm2}
+
+This is the electric equipment load (\textbf{Electric Equipment}) per floor area.
+
+\subsubsection{Field: Gas Load \{W/m2\}}\label{field-gas-load-wm2}
+
+This is the gas equipment load (\textbf{Gas Equipment}) per floor area.
+
+\subsubsection{Field: Other Load \{W/m2}\label{field-other-load-wm2}
+
+This is the other equipment load (\textbf{Other Equipment}) per floor area.
+
+\subsubsection{Field: Hot Water Eq \{W/m2\}}\label{field-hot-water-eq-wm2}
+
+This is the hot water equipment load (\textbf{Hot Water Equipment}) per floor area.
+
+\subsubsection{Field: Steam Equipment \{W/m2\}}\label{field-steam-equipment-wm2}
+
+This is the steam equipment load (\textbf{Steam Equipment}) per floor area.
+
+\subsubsection{Field: Sum Loads per Area \{W/m2\}}\label{field-sum-loads-per-area-wm2}
+
+This is the nominal sum of loads per area (equipment). This metric can be useful for incorrect (too much) loads in a zone.
+
+\subsubsection{Field: Outdoor Controlled Baseboard Heat}\label{field-outdoor-controlled-baseboard-heat}
+
+This field is ``yes'' if there is outdoor controlled baseboard heat in a Zone.
+
+\subsection{People Gains}\label{people-gains}
+
+! \textless{}People Internal Gains - Nominal\textgreater{},Name,Schedule Name,Zone Name,Zone Floor Area \{m2\},\# Zone Occupants,Number of People \{\},People/Floor Area \{person/m2\},Floor Area per person \{m2/person\},Fraction Radiant,Fraction Convected,Sensible Fraction Calculation,Activity level,ASHRAE 55 Warnings,Carbon Dioxide Generation Rate,Nominal Minimum Number of People,Nominal Maximum Number of People
+
+People Internal Gains,~ SPACE1-1 PEOPLE 1, OCCUPY-1, SPACE1-1, 99.16, 11.0, 11.0, 0.111, 9.015, 0.300, 0.700, AutoCalculate, ACTSCHD, No, 3.8200E-008, 0, 11
+
+~People Internal Gains,~ SPACE2-1 PEOPLE 1, OCCUPY-1, SPACE2-1, 42.74, 5.0, 5.0, 0.117, 8.547, 0.300, 0.700, AutoCalculate, ACTSCHD, No, 3.8200E-008, 0, 5
+
+~People Internal Gains,~ SPACE3-1 PEOPLE 1, OCCUPY-1, SPACE3-1, 96.48, 11.0, 11.0, 0.114, 8.771, 0.300, 0.700, AutoCalculate, ACTSCHD, No, 3.8200E-008, 0, 11
+
+~People Internal Gains,~ SPACE4-1 PEOPLE 1, OCCUPY-1, SPACE4-1, 42.74, 5.0, 5.0, 0.117, 8.547, 0.300, 0.700, AutoCalculate, ACTSCHD, No, 3.8200E-008, 0, 5
+
+~People Internal Gains,~ SPACE5-1 PEOPLE 1, OCCUPY-1, SPACE5-1, 182.49, 20.0, 20.0, 0.110, 9.125, 0.300, 0.700, AutoCalculate, ACTSCHD, No, 3.8200E-008, 0, 20
+
+\subsubsection{Field: \textless{}People Internal Gains - Nominal\textgreater{}}\label{field-people-internal-gains---nominal}
+
+This field contains the constant ``People Internal Gains'' for each line.
+
+\subsubsection{Field: Name}\label{field-name-1}
+
+This field contains the name of the People statement from the IDF file.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name}
+
+This is the schedule of occupancy fraction -- the fraction is applied to the number of occupants for the statement. Limits are {[}0,1{]}.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-2}
+
+This is the name of the Zone for the people/occupants.
+
+\subsubsection{Field: Zone Floor Area \{m2\}}\label{field-zone-floor-area-m2}
+
+This is the floor area (m2) of the zone.
+
+\subsubsection{Field: \# Zone Occupants}\label{field-zone-occupants}
+
+This is the total number of occupants for the zone.
+
+\subsubsection{Field: Number of People}\label{field-number-of-people}
+
+This is the specific number of people for this statement (nominal).
+
+\subsubsection{Field: People/Floor Area \{person/m2\}}\label{field-peoplefloor-area-personm2}
+
+This value represents the number of people density (this statement) per area (zone floor area).
+
+\subsubsection{Field: Floor Area per person \{m2/person\}}\label{field-floor-area-per-person-m2person}
+
+This is the floor area per person (this statement)
+
+\subsubsection{Field: Fraction Radiant}\label{field-fraction-radiant}
+
+This is the fraction radiant for each person (this statement).
+
+\subsubsection{Field: Fraction Convected}\label{field-fraction-convected}
+
+This is the fraction convected for each person (this statement).
+
+\subsubsection{Field: Sensible Fraction Calculation}\label{field-sensible-fraction-calculation}
+
+This field will show ``Autocalculate'' if the default calculation for sensible fraction of load is to be used. Or a specific value can be entered. If so, that value will be displayed.
+
+\subsubsection{Field: Activity level}\label{field-activity-level}
+
+This field will show the activity level schedule name.
+
+\subsubsection{Field: ASHRAE 55 Warnings}\label{field-ashrae-55-warnings}
+
+If this field shows ``yes'', then ASHRAE 55 comfort warnings are enabled. If ``no'', then no ASHRAE 55 comfort warnings are calculated or issued.
+
+\textbf{The following fields are shown only when one of the Comfort calculations (Fanger, KSU, Pierce) is used.}
+
+\subsubsection{Field: MRT Calculation Type}\label{field-mrt-calculation-type}
+
+This field's value will be one of the valid MRT calculation types (Zone Averaged, Surface Weighted, Angle Factor).
+
+\subsubsection{Field: Work Efficiency}\label{field-work-efficiency}
+
+This field will be the work efficiency schedule name for this people statement.
+
+\subsubsection{Field: Clothing}\label{field-clothing}
+
+This field will be the clothing schedule name for this people statement.
+
+\subsubsection{Field: Air Velocity}\label{field-air-velocity}
+
+This field will be the air velocity schedule name for this people statement.
+
+\subsubsection{Field: Fanger Calculation}\label{field-fanger-calculation}
+
+This field will be ``yes'' if Fanger calculations are enabled for this people statement; otherwise it will be ``no''.
+
+\subsubsection{Field: Pierce Calculation}\label{field-pierce-calculation}
+
+This field will be ``yes'' if Pierce calculations are enabled for this people statement; otherwise it will be ``no''.
+
+\subsubsection{Field: KSU Calculation}\label{field-ksu-calculation}
+
+This field will be ``yes'' if KSU calculations are enabled for this people statement; otherwise it will be ``no''.
+
+\subsubsection{Field: Carbon Dioxide Generation Rate}\label{field-carbon-dioxide-generation-rate}
+
+This numeric input field specifies carbon dioxide generation rate per person with units of m3/s-W. The total carbon dioxide generation rate from this object is:
+
+Number of People * People Schedule * People Activity * Carbon Dioxide Generation Rate. The default value is 3.82E-8 m3/s-W (obtained from ASHRAE Standard 62.1-2007 value at 0.0084 cfm/met/person over the general adult population). The maximum value can be 10 times the default value.
+
+\subsubsection{Field: Nominal Minimum Number of People}\label{field-nominal-minimum-number-of-people}
+
+This numeric field is the calculated minimum number of people based on the number of people field * the minimum value (annual) for the people schedule. It may be useful in diagnosing errors that occur during simulation.
+
+\subsubsection{Field: Nominal Maximum Number of People}\label{field-nominal-maximum-number-of-people}
+
+This numeric field is the calculated maximum number of people based on the number of people field * the maxnimum value (annual) for the people schedule. It may be useful in diagnosing errors that occur during simulation.
+
+\subsection{Lights Gains}\label{lights-gains}
+
+! \textless{}Lights Internal Gains - Nominal\textgreater{}, Name, Schedule Name, Zone Name, Zone Floor Area \{m2\}, \# Zone Occupants, Lighting Level \{W\}, Lights/Floor Area \{W/m2\}, Lights per person \{W/person\}, Fraction Return Air, Fraction Radiant, Fraction Short Wave, Fraction Convected, Fraction Replaceable, End-Use Category, Nominal Minimum Lighting Level \{W\}, Nominal Maximum Lighting Level \{W\}
+
+Lights Internal Gains,~ SPACE1-1 LIGHTS 1, LIGHTS-1, SPACE1-1, 99.16, 11.0, 1584.000, 15.974, 144.000, 0.200, 0.590, 0.200, 1.000E-002, 0.000, GeneralLights, 79.200, 1584.000
+
+~Lights Internal Gains,~ SPACE2-1 LIGHTS 1, LIGHTS-1, SPACE2-1, 42.74, 5.0, 684.000, 16.006, 136.800, 0.200, 0.590, 0.200, 1.000E-002, 0.000, GeneralLights, 34.200, 684.000
+
+~Lights Internal Gains,~ SPACE3-1 LIGHTS 1, LIGHTS-1, SPACE3-1, 96.48, 11.0, 1584.000, 16.418, 144.000, 0.200, 0.590, 0.200, 1.000E-002, 0.000, GeneralLights, 79.200, 1584.000
+
+~Lights Internal Gains,~ SPACE4-1 LIGHTS 1, LIGHTS-1, SPACE4-1, 42.74, 5.0, 684.000, 16.006, 136.800, 0.200, 0.590, 0.200, 1.000E-002, 0.000, GeneralLights, 34.200, 684.000
+
+~Lights Internal Gains,~ SPACE5-1 LIGHTS 1, LIGHTS-1, SPACE5-1, 182.49, 20.0, 2964.000, 16.242, 148.200, 0.200, 0.590, 0.200, 1.000E-002, 0.000, GeneralLights, 148.200, 2964.000
+
+\subsubsection{Field: \textless{}Lights Internal Gains - Nominal\textgreater{}}\label{field-lights-internal-gains---nominal}
+
+This field contains the constant ``Lights Internal Gains'' for each line.
+
+\subsubsection{Field: Name}\label{field-name-2}
+
+This field contains the name of the Lights statement from the IDF file.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name-1}
+
+This is the schedule of lights fraction -- the fraction is applied to the nominal lighting level for the statement. Limits are {[}0,1{]}.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-3}
+
+This is the name of the Zone for the lights.
+
+\subsubsection{Field: Zone Floor Area \{m2\}}\label{field-zone-floor-area-m2-1}
+
+This is the floor area (m2) of the zone.
+
+\subsubsection{Field: \# Zone Occupants}\label{field-zone-occupants-1}
+
+This is the total number of occupants for the zone.
+
+\subsubsection{Field: Lighting Level \{W\}}\label{field-lighting-level-w}
+
+This is the nominal lighting level (this statement) in Watts.
+
+\subsubsection{Field: Lights/Floor Area \{W/m2\}}\label{field-lightsfloor-area-wm2}
+
+This is the watts per floor area (this statement)
+
+\subsubsection{Field: Lights per person \{W/person\}}\label{field-lights-per-person-wperson}
+
+This is the watts per person that this statement represents.
+
+\subsubsection{Field: Fraction Return Air}\label{field-fraction-return-air}
+
+This is the fraction return air for this statement.
+
+\subsubsection{Field: Fraction Radiant}\label{field-fraction-radiant-1}
+
+This is the fraction radiant for this lighting level.
+
+\subsubsection{Field: Fraction Short Wave}\label{field-fraction-short-wave}
+
+This is the fraction short wave for this lighting level.
+
+\subsubsection{Field: Fraction Convected}\label{field-fraction-convected-1}
+
+This is the fraction convected for this lighting level.
+
+\subsubsection{Field: Fraction Replaceable}\label{field-fraction-replaceable}
+
+This is the fraction replaceable for this lighting level. For daylighting calculations, this value should either be 0 (no dimming control) or 1 (full dimming control).
+
+\subsubsection{Field: End-Use Category}\label{field-end-use-category}
+
+This field shows the end-use category for this lights statement. Usage can be reported by end-use category.
+
+\subsubsection{Field: Nominal Minimum Lighting Level \{W\}}\label{field-nominal-minimum-lighting-level-w}
+
+This numeric field is the calculated minimum amount of lighting in Watts based on the calculated lighting level (above) * the minimum value (annual) for the lights schedule. It may be useful in diagnosing errors that occur during simulation.
+
+\subsubsection{Field: Nominal Maximum Lighting Level \{W\}}\label{field-nominal-maximum-lighting-level-w}
+
+This numeric field is the calculated maximum amount of lighting in Watts based on the calculated lighting level (above) * the maximum value (annual) for the lights schedule. It may be useful in diagnosing errors that occur during simulation.
+
+\subsection{Equipment (Electric, Gas, Steam, Hot Water) Gains}\label{equipment-electric-gas-steam-hot-water-gains}
+
+These equipments are all reported similarly. Electric Equipment is used in the example below:
+
+! \textless{}ElectricEquipment Internal Gains - Nominal\textgreater{}, Name, Schedule Name, Zone Name, Zone Floor Area \{m2\}, \# Zone Occupants, Equipment Level \{W\}, Equipment/Floor Area \{W/m2\}, Equipment per person \{W/person\}, Fraction Latent, Fraction Radiant, Fraction Lost, Fraction Convected, End-Use SubCategory, Nominal Minimum Equipment Level \{W\}, Nominal Maximum Equipment Level \{W\}
+
+ElectricEquipment Internal Gains,~ SPACE1-1 ELECEQ 1, EQUIP-1, SPACE1-1, 99.16, 11.0, 1056.000, 10.649, 96.000, 0.000, 0.300, 0.000, 0.700, General, 21.120, 950.400
+
+~ElectricEquipment Internal Gains,~ SPACE2-1 ELECEQ 1, EQUIP-1, SPACE2-1, 42.74, 5.0, 456.000, 10.670, 91.200, 0.000, 0.300, 0.000, 0.700, General, 9.120, 410.400
+
+~ElectricEquipment Internal Gains,~ SPACE3-1 ELECEQ 1, EQUIP-1, SPACE3-1, 96.48, 11.0, 1056.000, 10.945, 96.000, 0.000, 0.300, 0.000, 0.700, General, 21.120, 950.400
+
+~ElectricEquipment Internal Gains,~ SPACE4-1 ELECEQ 1, EQUIP-1, SPACE4-1, 42.74, 5.0, 456.000, 10.670, 91.200, 0.000, 0.300, 0.000, 0.700, General, 9.120, 410.400
+
+~ElectricEquipment Internal Gains,~ SPACE5-1 ELECEQ 1, EQUIP-1, SPACE5-1, 182.49, 20.0, 1976.000, 10.828, 98.800, 0.000, 0.300, 0.000, 0.700, General, 39.520, 1778.400
+
+\subsubsection{Field: \textless{}{[}Specific{]} Equipment Internal Gains - Nominal\textgreater{}}\label{field-specific-equipment-internal-gains---nominal}
+
+This field will contain the type of equipment internal gain in each line (i.e.~Electric Equipment Internal Gains, Gas Equipment Internal Gains, \ldots{}).
+
+\subsubsection{Field: Name}\label{field-name-3}
+
+This field contains the name of the equipment statement from the IDF file.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name-2}
+
+This is the schedule of equipment fraction -- the fraction is applied to the nominal equipment level for the statement. Limits are {[}0,1{]}.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-4}
+
+This is the name of the Zone for the equipment.
+
+\subsubsection{Field: Zone Floor Area \{m2\}}\label{field-zone-floor-area-m2-2}
+
+This is the floor area (m2) of the zone.
+
+\subsubsection{Field: \# Zone Occupants}\label{field-zone-occupants-2}
+
+This is the total number of occupants for the zone.
+
+\subsubsection{Field: Equipment Level \{W\}}\label{field-equipment-level-w}
+
+This is the nominal equipment level (in Watts) for the statement.
+
+\subsubsection{Field: Equipment/Floor Area \{W/m2\}}\label{field-equipmentfloor-area-wm2}
+
+This is the watts per floor area (this statement)
+
+\subsubsection{Field: Equipment per person \{W/person\}}\label{field-equipment-per-person-wperson}
+
+This is the watts per person that this statement represents.
+
+\subsubsection{Field: Fraction Latent}\label{field-fraction-latent}
+
+This is the fraction latent for this equipment.
+
+\subsubsection{Field: Fraction Radiant}\label{field-fraction-radiant-2}
+
+This is the fraction radiant for this equipment.
+
+\subsubsection{Field: Fraction Lost}\label{field-fraction-lost}
+
+This is the fraction lost (not attributed to the zone) for this equipment.
+
+\subsubsection{Field: Fraction Convected}\label{field-fraction-convected-2}
+
+This is the fraction convected for this equipment.
+
+\subsubsection{Field: End-Use SubCategory}\label{field-end-use-subcategory}
+
+This field shows the end-use category for this statement. Usage can be reported by end-use category.
+
+\subsubsection{Field: Nominal Minimum Equipment Level \{W\}}\label{field-nominal-minimum-equipment-level-w}
+
+This numeric field is the calculated minimum amount of the equipment in Watts based on the calculated design level (above) * the minimum value (annual) for the equipment schedule. It may be useful in diagnosing errors that occur during simulation.
+
+\subsubsection{Field: Nominal Maximum Equipment Level \{W\}}\label{field-nominal-maximum-equipment-level-w}
+
+This numeric field is the calculated maximum amount of the equipment in Watts based on the calculated design level (above) * the maximum value (annual) for the equipment schedule. It may be useful in diagnosing errors that occur during simulation.
+
+\subsection{Other Equipment Gains}\label{other-equipment-gains}
+
+Other equipment report is shown below (does not have an end-use category -- is not attached to any normal meter):
+
+! \textless{}OtherEquipment Internal Gains - Nominal\textgreater{}, Name, Schedule Name, Zone Name, Zone Floor Area \{m2\}, \# Zone Occupants, Equipment Level \{W\}, Equipment/Floor Area \{W/m2\}, Equipment per person \{W/person\}, Fraction Latent, Fraction Radiant, Fraction Lost, Fraction Convected, Nominal Minimum Equipment Level \{W\}, Nominal Maximum Equipment Level \{W\}
+
+OtherEquipment Internal Gains,~ TEST 352A, ALWAYSON, ZONE ONE, 232.26, 0.0, 352.000, 1.516, N/A, 0.000, 0.000, 0.000, 1.000, 352.000, 352.000
+
+~OtherEquipment Internal Gains,~ TEST 352 MINUS, ALWAYSON, ZONE ONE, 232.26, 0.0, -352.000, -1.516, N/A, 0.000, 0.000, 0.000, 1.000, -352.000, -352.000
+
+\subsubsection{Field: \textless{}Other Equipment Internal Gains - Nominal\textgreater{}}\label{field-other-equipment-internal-gains---nominal}
+
+This field contains the constant ``OtherEquipment Internal Gains'' for each line.
+
+\subsubsection{Field: Name}\label{field-name-4}
+
+This field contains the name of the equipment statement from the IDF file.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name-3}
+
+This is the schedule of equipment fraction -- the fraction is applied to the nominal equipment level for the statement. Limits are {[}0,1{]}.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-5}
+
+This is the name of the Zone for the equipment.
+
+\subsubsection{Field: Zone Floor Area \{m2\}}\label{field-zone-floor-area-m2-3}
+
+This is the floor area (m2) of the zone.
+
+\subsubsection{Field: \# Zone Occupants}\label{field-zone-occupants-3}
+
+This is the total number of occupants for the zone.
+
+\subsubsection{Field: Equipment Level \{W\}}\label{field-equipment-level-w-1}
+
+This is the nominal equipment level (in Watts) for the statement.
+
+\subsubsection{Field: Equipment/Floor Area \{W/m2\}}\label{field-equipmentfloor-area-wm2-1}
+
+This is the watts per floor area (this statement)
+
+\subsubsection{Field: Equipment per person \{W/person\}}\label{field-equipment-per-person-wperson-1}
+
+This is the watts per person that this statement represents.
+
+\subsubsection{Field: Fraction Latent}\label{field-fraction-latent-1}
+
+This is the fraction latent for this equipment.
+
+\subsubsection{Field: Fraction Radiant}\label{field-fraction-radiant-3}
+
+This is the fraction radiant for this equipment.
+
+\subsubsection{Field: Fraction Lost}\label{field-fraction-lost-1}
+
+This is the fraction lost (not attributed to the zone) for this equipment.
+
+\subsubsection{Field: Fraction Convected}\label{field-fraction-convected-3}
+
+This is the fraction convected for this equipment.
+
+\subsubsection{Field: Nominal Minimum Equipment Level \{W\}}\label{field-nominal-minimum-equipment-level-w-1}
+
+This numeric field is the calculated minimum amount of the equipment in Watts based on the calculated design level (above) * the minimum value (annual) for the equipment schedule. It may be useful in diagnosing errors that occur during simulation.
+
+\subsubsection{Field: Nominal Maximum Equipment Level \{W\}}\label{field-nominal-maximum-equipment-level-w-1}
+
+This numeric field is the calculated maximum amount of the equipment in Watts based on the calculated design level (above) * the maximum value (annual) for the equipment schedule. It may be useful in diagnosing errors that occur during simulation.
+
+\subsection{Outdoor Controlled Baseboard Heat}\label{outdoor-controlled-baseboard-heat}
+
+! \textless{}Outdoor Controlled Baseboard Heat Internal Gains - Nominal\textgreater{},Name,Schedule Name,Zone Name,Zone Floor Area \{m2\},\# Zone Occupants,Capacity at Low Temperature \{W\},Low Temperature \{C\},Capacity at High Temperature \{W\},High Temperature \{C\},Fraction Radiant,Fraction Convected,End-Use Subcategory
+
+~Outdoor Controlled Baseboard Heat Internal Gains, SPACE4-1 BBHEAT 1,EQUIP-1,SPACE4-1,42.74,5.0,1500.000,0.000,500.000,10.000,0.500,0.500,Baseboard Heat
+
+\subsubsection{Field: \textless{}Outdoor Controlled Baseboard Heat Internal Gains - Nominal\textgreater{}}\label{field-outdoor-controlled-baseboard-heat-internal-gains---nominal}
+
+This field contains the constant ``Outdoor Controlled Baseboard Heat Internal Gains'' for each line.
+
+\subsubsection{Field: Name}\label{field-name-5}
+
+This field contains the name of the baseboard heat statement from the IDF file.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name-4}
+
+This is the schedule of equipment fraction -- the fraction is applied to the nominal equipment level for the statement. Limits are {[}0,1{]}.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-6}
+
+This is the name of the Zone for the equipment.
+
+\subsubsection{Field: Zone Floor Area \{m2\}}\label{field-zone-floor-area-m2-4}
+
+This is the floor area (m2) of the zone.
+
+\subsubsection{Field: \# Zone Occupants}\label{field-zone-occupants-4}
+
+This is the total number of occupants for the zone.
+
+\subsubsection{Field: Capacity at Low Temperature \{W\}}\label{field-capacity-at-low-temperature-w}
+
+This is the capacity (in Watts) of the equipment at low outdoor temperature.
+
+\subsubsection{Field: Low Temperature \{C\}}\label{field-low-temperature-c}
+
+This is the low outdoor temperature (dry-bulb) for the capacity in the previous field. If the outdoor dry-bulb temperature (degrees Celsius) is at or below the low temperature, thebaseboard heater operates at the low temperature capacity.
+
+\subsubsection{Field: Capacity at High Temperature \{W\}}\label{field-capacity-at-high-temperature-w}
+
+This is the capacity (in Watts) of the equipment at high outdoor temperature.
+
+\subsubsection{Field: High Temperature \{C\}}\label{field-high-temperature-c}
+
+This is the high outdoor temperature (dry-bulb) for the capacity in the previous field. If the outdoor dry-bulb temperature (degrees Celsius) is exceeds the high temperature, thebaseboard heater turns off.
+
+\subsubsection{Field: Fraction Radiant}\label{field-fraction-radiant-4}
+
+This is the fraction radiant for this equipment.
+
+\subsubsection{Field: Fraction Convected}\label{field-fraction-convected-4}
+
+This is the fraction convected for this equipment.
+
+\subsubsection{Field: EndUse Subcategory}\label{field-enduse-subcategory}
+
+This field shows the enduse category for this statement. Usage can be reported by enduse category.
+
+\subsection{Simple Airflow Outputs}\label{simple-airflow-outputs}
+
+\subsection{Infiltration, Ventilation, Mixing, Cross Mixing Statistics}\label{infiltration-ventilation-mixing-cross-mixing-statistics}
+
+Infiltration, Ventilation, Mixing, Cross Mixing are only specified when the Airflow Model is ``Simple'' (no Airflow Network).
+
+\subsection{Infiltration}\label{infiltration}
+
+! \textless{}Infiltration Airflow Stats - Nominal\textgreater{},Name,Schedule Name,Zone Name, Zone Floor Area \{m2\}, \# Zone Occupants,Design Volume Flow Rate \{m3/s\},Volume Flow Rate/Floor Area \{m3/s/m2\},Volume Flow Rate/Exterior Surface Area \{m3/s/m2\},ACH - Air Changes per Hour,Equation A - Constant Term Coefficient \{\},Equation B - Temperature Term Coefficient \{1/C\},Equation C - Velocity Term Coefficient \{s/m\}, Equation D - Velocity Squared Term Coefficient \{s2/m2\}
+
+ZoneInfiltration Airflow Stats, SPACE1-1 INFIL 1,INFIL-SCH,SPACE1-1,99.16,11.0,3.200E-002,3.227E-004,4.372E-004,0.482,0.000,0.000,0.224,0.000
+
+~ZoneInfiltration Airflow Stats, SPACE2-1 INFIL 1,INFIL-SCH,SPACE2-1,42.74,5.0,1.400E-002,3.276E-004,3.838E-004,0.488,0.000,0.000,0.224,0.000
+
+~ZoneInfiltration Airflow Stats, SPACE3-1 INFIL 1,INFIL-SCH,SPACE3-1,96.48,11.0,3.200E-002,3.317E-004,4.372E-004,0.482,0.000,0.000,0.224,0.000
+
+~ZoneInfiltration Airflow Stats, SPACE4-1 INFIL 1,INFIL-SCH,SPACE4-1,42.74,5.0,1.400E-002,3.276E-004,3.838E-004,0.488,0.000,0.000,0.224,0.000
+
+~ZoneInfiltration Airflow Stats, SPACE5-1 INFIL 1,INFIL-SCH,SPACE5-1,182.49,20.0,6.200E-002,3.397E-004,N/A,0.499,0.000,0.000,0.224,0.000
+
+\subsubsection{Field: \textless{}Infiltration Airflow Stats - Nominal\textgreater{}}\label{field-infiltration-airflow-stats---nominal}
+
+This field contains the constant ``Infiltration Airflow Stats'' for each line.
+
+\subsubsection{Field: Name}\label{field-name-6}
+
+This field contains the name of the infiltration statement from the IDF file.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name-5}
+
+This is the schedule of use fraction -- the fraction is applied to the nominal volume flow rate for the statement. Limits are {[}0,1{]}.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-7}
+
+This is the name of the Zone for the infiltration.
+
+\subsubsection{Field: Zone Floor Area \{m2\}}\label{field-zone-floor-area-m2-5}
+
+This is the floor area (m2) of the zone.
+
+\subsubsection{Field: \# Zone Occupants}\label{field-zone-occupants-5}
+
+This is the total number of occupants for the zone.
+
+\subsubsection{Field: Design Volume Flow Rate \{m3/s\}}\label{field-design-volume-flow-rate-m3s}
+
+This is the nominal flow rate for the infiltration in m3/s.
+
+\subsubsection{Field: Volume Flow Rate/Floor Area \{m3/s/m2\}}\label{field-volume-flow-ratefloor-area-m3sm2}
+
+This field is the volume flow rate density per floor area (flow rate per floor area) for infiltration.
+
+\subsubsection{Field: Volume Flow Rate/Exterior Surface Area \{m3/s/m2\}}\label{field-volume-flow-rateexterior-surface-area-m3sm2}
+
+This field is the volume flow rate density per exterior surface area (flow rate per exterior area) for infiltration.
+
+\subsubsection{Field: ACH - Air Changes per Hour}\label{field-ach---air-changes-per-hour}
+
+This field is the air changes per hour for the given infiltration rate.
+
+\subsubsection{Field: Equation A - Constant Term Coefficient}\label{field-equation-a---constant-term-coefficient}
+
+Actual infiltration amount is an equation based value:
+
+\begin{equation}
+\text{Infiltration} = I_{design} F_{schedule} \left[ A + B \left| T_{zone}-T_{odb} \right| + C\left(\text{WindSpeed}\right) + D\left(\text{WindSpeed}^2\right)  \right]
+\end{equation}
+
+This field value is the A coefficient in the above equation.
+
+\subsubsection{Field: Equation B - Temperature Term Coefficient \{1/C\}}\label{field-equation-b---temperature-term-coefficient-1c}
+
+This field value is the B coefficient in the above equation.
+
+\subsubsection{Field: Equation C - Velocity Term Coefficient \{s/m\}}\label{field-equation-c---velocity-term-coefficient-sm}
+
+This field value is the C coefficient in the above equation.
+
+\subsubsection{Field:~ Equation D - Velocity Squared Term Coefficient \{s2/m2\}}\label{field-equation-d---velocity-squared-term-coefficient-s2m2}
+
+This field value is the D coefficient in the above equation.
+
+\subsection{Ventilation}\label{ventilation}
+
+! \textless{}Ventilation Airflow Stats - Nominal\textgreater{},Name,Schedule Name,Zone Name, Zone Floor Area \{m2\}, \# Zone Occupants,Design Volume Flow Rate \{m3/s\},Volume Flow Rate/Floor Area \{m3/s/m2\},Volume Flow Rate/person Area \{m3/s/person\},ACH - Air Changes per Hour,Fan Type \{Exhaust;Intake;Natural/None\},Fan Pressure Rise \{?\},Fan Efficiency \{\},Equation A - Constant Term Coefficient \{\},Equation B - Temperature Term Coefficient \{1/C\},Equation C - Velocity Term Coefficient \{s/m\}, Equation D - Velocity Squared Term Coefficient \{s2/m2\},Minimum Indoor Temperature/Schedule,Maximum Indoor Temperature/Schedule,Delta Temperature/Schedule,Minimum Outdoor Temperature/Schedule,Maximum Outdoor Temperature/Schedule,Maximum WindSpeed
+
+~Ventilation Airflow Stats, SPACE1-1 VENTL 1,NIGHTVENTSCHED,SPACE1-1,99.16,11.0,5.295E-002,5.340E-004,4.814E-003,0.797,Intake,67.000,0.7,1.000,0.000,0.000,0.000,MININDOORTEMP,MAXINDOORTEMP,DELTATEMP,MINOUTDOORTEMP,MAXOUTDOORTEMP,40.00
+
+~Ventilation Airflow Stats, SPACE1-1 VENTL 2,NIGHTVENTSCHED,SPACE1-1,99.16,11.0,5.295E-002,5.340E-004,4.814E-003,0.797,Intake,67.000,0.7,1.000,0.000,0.000,0.000,MININDOORTEMP,MAXINDOORTEMP,DELTATEMP,MINOUTDOORTEMP,MAXOUTDOORTEMP,40.00
+
+~Ventilation Airflow Stats, SPACE2-1 VENTL 1,NIGHTVENTSCHED,SPACE2-1,42.74,5.0,7.030E-002,1.645E-003,1.406E-002,2.450,Intake,67.000,0.7,1.000,0.000,0.000,0.000,18.00,100.00,2.00,-100.00,100.00,40.00
+
+Ventilation Airflow Stats, RESISTIVE ZONE VENTL 1,INF-SCHED,RESISTIVE ZONE,37.16,3.0,2.000E-002,5.382E-004,6.667E-003,0.636,Natural,0.000,1.0,0.606,2.020E-002,5.980E-004,0.000,18.00,100.00,1.00,-100.00,100.00,40.00
+
+~Ventilation Airflow Stats, EAST ZONE VENTL 1,INF-SCHED,EAST ZONE,37.16,3.0,2.000E-002,5.382E-004,6.667E-003,0.636,Natural,0.000,1.0,0.606,2.020E-002,5.980E-004,0.000,18.00,100.00,1.00,-100.00,100.00,40.00
+
+~Ventilation Airflow Stats, NORTH ZONE VENTL 1,INF-SCHED,NORTH ZONE,55.74,4.0,2.000E-002,3.588E-004,5.000E-003,0.424,Natural,0.000,1.0,0.606,2.020E-002,5.980E-004,0.000,18.00,100.00,1.00,-100.00,100.00,40.00
+
+\subsubsection{Field: \textless{}Ventilation Airflow Stats - Nominal\textgreater{}}\label{field-ventilation-airflow-stats---nominal}
+
+This field contains the constant ``Ventilation Airflow Stats'' for each line.
+
+\subsubsection{Field: Name}\label{field-name-7}
+
+This field contains the name of the ventilation statement from the IDF file.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name-6}
+
+This is the schedule of use fraction -- the fraction is applied to the nominal volume flow rate for the statement. Limits are {[}0,1{]}.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-8}
+
+This is the name of the Zone for the ventilation.
+
+\subsubsection{Field: Zone Floor Area \{m2\}}\label{field-zone-floor-area-m2-6}
+
+This is the floor area (m2) of the zone.
+
+\subsubsection{Field: \# Zone Occupants}\label{field-zone-occupants-6}
+
+This is the total number of occupants for the zone.
+
+\subsubsection{Field: Design Volume Flow Rate \{m3/s\}}\label{field-design-volume-flow-rate-m3s-1}
+
+This is the nominal flow rate for the ventilation in m3/s.
+
+\subsubsection{Field: Volume Flow Rate/Floor Area \{m3/s/m2\}}\label{field-volume-flow-ratefloor-area-m3sm2-1}
+
+This field is the volume flow rate density per floor area (flow rate per floor area) for ventilation.
+
+\subsubsection{Field: Volume Flow Rate/person Area \{m3/s/person\}}\label{field-volume-flow-rateperson-area-m3sperson}
+
+This field is the volume flow rate density per person (flow rate per person) for ventilation.
+
+\subsubsection{Field: ACH - Air Changes per Hour}\label{field-ach---air-changes-per-hour-1}
+
+This field is the air changes per hour for the given ventilation rate.
+
+\subsubsection{Field: Fan Type \{Exhaust;Intake;Natural\}}\label{field-fan-type-exhaustintakenatural}
+
+This field shows the entered value for the type of ventilation {[}NATURAL, EXHAUST, or INTAKE{]}. Natural ventilation is the air movement/exchange a result of openings in the building façade and does not consume any fan energy. For either EXHAUST or INTAKE, values for fan pressure and efficiency define the fan electric consumption. For NATURAL and EXHAUST ventilation, the conditions of the air entering the space are assumed to be equivalent to outdoor air conditions. For INTAKE ventilation, an appropriate amount of fan heat is added to the air stream.
+
+\subsubsection{Field: Fan Pressure Rise \{Pa\}}\label{field-fan-pressure-rise-pa}
+
+Operational when Fan Type is INTAKE or EXHAUST, this is the pressure rise experienced across the fan in Pascals (N/m\(^{2}\)). This is a function of the fan and plays a role in determining the amount of energy consumed by the fan.
+
+\subsubsection{Field: Fan Efficiency}\label{field-fan-efficiency}
+
+Operational when Fan Type is INTAKE or EXHAUST, this is the total fan efficiency (a decimal number between 0.0 and 1.0). This is a function of the fan and plays a role in determining the amount of energy consumed by the fan.
+
+\subsubsection{Field: Equation A - Constant Term Coefficient}\label{field-equation-a---constant-term-coefficient-1}
+
+Actual ventilation amount is an equation based value:
+
+\begin{equation}
+\text{Ventilation} = V_{design} F_{schedule} \left[ A + B \left| T_{zone}-T_{odb} \right| + C\left(\text{WindSpeed}\right) + D\left(\text{WindSpeed}^2\right)  \right]
+\end{equation}
+
+This field value is the A coefficient in the above equation.
+
+\subsubsection{Field: Equation B - Temperature Term Coefficient \{1/C\}}\label{field-equation-b---temperature-term-coefficient-1c-1}
+
+This field value is the B coefficient in the above equation.
+
+\subsubsection{Field: Equation C - Velocity Term Coefficient \{s/m\}}\label{field-equation-c---velocity-term-coefficient-sm-1}
+
+This field value is the C coefficient in the above equation.
+
+\subsubsection{Field:~ Equation D - Velocity Squared Term Coefficient \{s2/m2\}}\label{field-equation-d---velocity-squared-term-coefficient-s2m2-1}
+
+This field value is the D coefficient in the above equation.
+
+\subsubsection{Field: Minimum Indoor Temperature\{C\}/Schedule}\label{field-minimum-indoor-temperaturecschedule}
+
+This is the indoor temperature (in Celsius) below which ventilation is shutoff. As the values can also be entered as a schedule, the schedule name may be listed here rather than a temperature.
+
+\subsubsection{Field: Maximum Indoor Temperature\{C\}/Schedule}\label{field-maximum-indoor-temperaturecschedule}
+
+This is the indoor temperature (in Celsius) above which ventilation is shutoff. As the values can also be entered as a schedule, the schedule name may be listed here rather than a temperature.
+
+\subsubsection{Field: Delta Temperature\{C\}/Schedule}\label{field-delta-temperaturecschedule}
+
+This is the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which ventilation is shutoff. As the values can also be entered as a schedule, the schedule name may be listed here rather than a temperature.
+
+\subsubsection{Field: Minimum Outdoor Temperature\{C\}/Schedule}\label{field-minimum-outdoor-temperaturecschedule}
+
+This is the outdoor temperature (in Celsius) below which ventilation is shut off. As the values can also be entered as a schedule, the schedule name may be listed here rather than a temperature.
+
+\subsubsection{Field: Maximum Outdoor Temperature\{C\}/Schedule}\label{field-maximum-outdoor-temperaturecschedule}
+
+This is the outdoor temperature (in Celsius) above which ventilation is shut off. As the values can also be entered as a schedule, the schedule name may be listed here rather than a temperature.
+
+\subsubsection{Field: Maximum WindSpeed\{m/s\}}\label{field-maximum-windspeedms}
+
+This is the wind speed (m/s) above which ventilation is shut off.
+
+\subsection{Mixing}\label{mixing}
+
+! \textless{}Mixing Airflow Stats - Nominal\textgreater{},Name,Schedule Name,Zone Name, Zone Floor Area \{m2\}, \# Zone Occupants,Design Volume Flow Rate \{m3/s\},Volume Flow Rate/Floor Area \{m3/s/m2\},Volume Flow Rate/person Area \{m3/s/person\},ACH - Air Changes per Hour,From/Source Zone,Delta Temperature \{C\}
+
+~Mixing Airflow Stats, RESISTIVE ZONE MIXNG 1,ZONE MIXING,RESISTIVE ZONE,37.16,3.0,5.000E-002,1.345E-003,1.667E-002,1.589,EAST ZONE,0.00
+
+\subsubsection{Field: \textless{}Mixing Airflow Stats - Nominal\textgreater{}}\label{field-mixing-airflow-stats---nominal}
+
+This field contains the constant ``Mixing Airflow Stats'' for each line.
+
+\subsubsection{Field: Name}\label{field-name-8}
+
+This field contains the name of the mixing statement from the IDF file.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name-7}
+
+This is the schedule of use fraction -- the fraction is applied to the nominal volume flow rate for the statement. Limits are {[}0,1{]}.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-9}
+
+This is the name of the Zone for the mixing.
+
+\subsubsection{Field: Zone Floor Area \{m2\}}\label{field-zone-floor-area-m2-7}
+
+This is the floor area (m2) of the zone.
+
+\subsubsection{Field: \# Zone Occupants}\label{field-zone-occupants-7}
+
+This is the total number of occupants for the zone.
+
+\subsubsection{Field: Design Volume Flow Rate \{m3/s\}}\label{field-design-volume-flow-rate-m3s-2}
+
+This is the nominal flow rate for the mixing in m3/s.
+
+\subsubsection{Field: Volume Flow Rate/Floor Area \{m3/s/m2\}}\label{field-volume-flow-ratefloor-area-m3sm2-2}
+
+This field is the volume flow rate density per floor area (flow rate per floor area) for mixing.
+
+\subsubsection{Field: Volume Flow Rate/person Area \{m3/s/person\}}\label{field-volume-flow-rateperson-area-m3sperson-1}
+
+This field is the volume flow rate density per person (flow rate per person) for mixing.
+
+\subsubsection{Field: ACH - Air Changes per Hour}\label{field-ach---air-changes-per-hour-2}
+
+This field is the air changes per hour for the given mixing rate.
+
+\subsubsection{Field: From/Source Zone}\label{field-fromsource-zone}
+
+This is the source zone for the mixing rate.
+
+\subsubsection{Field: Delta Temperature \{C\}}\label{field-delta-temperature-c}
+
+This number controls when mixing air from the source zone is sent to the receiving zone. This parameter is a temperature \{units Celsius\}. If this field is positive, the temperature of the zone from which the air is being drawn (source zone) must be ``Delta Temperature'' warmer than the receiving zone air or else no mixing occurs. If this field is negative, the temperature of the source zone must be ``Delta Temperature'' cooler than the receiving zone air or else no mixing occurs. If this parameter is zero, mixing occurs regardless of the relative zone temperatures.
+
+\subsection{Cross Mixing}\label{cross-mixing}
+
+! \textless{}CrossMixing Airflow Stats - Nominal\textgreater{},Name,Schedule Name,Zone Name, Zone Floor Area \{m2\}, \# Zone Occupants,Design Volume Flow Rate \{m3/s\},Volume Flow Rate/Floor Area \{m3/s/m2\},Volume Flow Rate/person Area \{m3/s/person\},ACH - Air Changes per Hour,From/Source Zone,Delta Temperature \{C\}
+
+~CrossMixing Airflow Stats, EAST ZONE XMIXNG 1,ZONE MIXING,EAST ZONE,37.16,3.0,0.100,2.691E-003,3.333E-002,3.178,NORTH ZONE,1.00
+
+~CrossMixing Airflow Stats, NORTH ZONE XMIXNG 1,ZONE MIXING,NORTH ZONE,55.74,4.0,0.100,1.794E-003,2.500E-002,2.119,EAST ZONE,1.00
+
+\subsubsection{Field: \textless{}CrossMixing Airflow Stats - Nominal\textgreater{}}\label{field-crossmixing-airflow-stats---nominal}
+
+This field contains the constant ``CrossMixing Airflow Stats'' for each line.
+
+\subsubsection{Field: Name}\label{field-name-9}
+
+This field contains the name of the mixing statement from the IDF file.
+
+\subsubsection{Field: Schedule Name}\label{field-schedule-name-8}
+
+This is the schedule of use fraction -- the fraction is applied to the nominal volume flow rate for the statement. Limits are {[}0,1{]}.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-10}
+
+This is the name of the Zone for the mixing.
+
+\subsubsection{Field: Zone Floor Area \{m2\}}\label{field-zone-floor-area-m2-8}
+
+This is the floor area (m2) of the zone.
+
+\subsubsection{Field: \# Zone Occupants}\label{field-zone-occupants-8}
+
+This is the total number of occupants for the zone.
+
+\subsubsection{Field: Design Volume Flow Rate \{m3/s\}}\label{field-design-volume-flow-rate-m3s-3}
+
+This is the nominal flow rate for the mixing in m3/s.
+
+\subsubsection{Field: Volume Flow Rate/Floor Area \{m3/s/m2\}}\label{field-volume-flow-ratefloor-area-m3sm2-3}
+
+This field is the volume flow rate density per floor area (flow rate per floor area) for mixing.
+
+\subsubsection{Field: Volume Flow Rate/person Area \{m3/s/person\}}\label{field-volume-flow-rateperson-area-m3sperson-2}
+
+This field is the volume flow rate density per person (flow rate per person) for mixing.
+
+\subsubsection{Field: ACH - Air Changes per Hour}\label{field-ach---air-changes-per-hour-3}
+
+This field is the air changes per hour for the given mixing rate.
+
+\subsubsection{Field: From/Source Zone}\label{field-fromsource-zone-1}
+
+This is the source zone for the mixing -- air is exchanged equally between the two zones.
+
+\subsubsection{Field: Delta Temperature \{C\}}\label{field-delta-temperature-c-1}
+
+This number controls when mixing air from the source zone is sent to the receiving zone. This parameter is a temperature \{units Celsius\}. If this field is positive, the temperature of the zone from which air is being drawn (``source zone'') must be ``Delta Temperature'' warmer than the zone air or no mixing occurs. If this field is zero, mixing occurs regardless of the relative air temperatures. Negative values for ``Delta Temperature'' are not permitted.
+
+\subsection{RefrigerationDoor Mixing}\label{refrigerationdoor-mixing}
+
+! \textless{}RefrigerationDoorMixing~ Airflow Stats - Nominal\textgreater{}, Name, Zone 1 Name, Zone 2 Name, Door Opening Schedule Name, Door Height \{m\},Door Area \{m2\},Door Protection Type
+
+~RefrigerationDoorMixing Airflow Stats, FREEZER1\_SUBFREEZER1, FREEZER\_1, SUBFREEZER, FREEZER1DOORSCHEDA, 1.800, 2.300, StripCurtain
+
+~RefrigerationDoorMixing Airflow Stats, FREEZER5\_COOLER2, COOLER\_2, FREEZER\_5, FREEZER5DOORSCHEDA, 1.800, 2.300, AirCurtain
+
+\subsubsection{Field: \textless{}RefrigerationDoorMixing Airflow Stats - Nominal\textgreater{}}\label{field-refrigerationdoormixing-airflow-stats---nominal}
+
+This field contains the constant ``RefrigerationDoor Airflow Stats'' for each line.
+
+\subsubsection{Field: Name}\label{field-name-10}
+
+This field contains the name of the mixing statement from the IDF file.
+
+\subsubsection{Field: Zone 1 Name}\label{field-zone-1-name}
+
+This is the name of one of the two Zones for the mixing.
+
+\subsubsection{Field: Zone 2 Name}\label{field-zone-2-name}
+
+This is the name of the other Zone for the mixing.
+
+\subsubsection{Field: Door Opening Schedule Name}\label{field-door-opening-schedule-name}
+
+This is the schedule of use fraction -- the fraction is applied to the nominal volume flow rate for the statement. Limits are {[}0,1{]}.
+
+\subsubsection{Field: Door Height \{m\}}\label{field-door-height-m}
+
+This is the nominal flow rate for the mixing in m3/s.
+
+\subsubsection{Field: Door Area \{m2\}}\label{field-door-area-m2}
+
+This is the floor area (m2) of the zone.
+
+\subsubsection{Field: Door Protection Type}\label{field-door-protection-type}
+
+This is one of three keywords, None, StripCurtain, or AirCurtain.
+
+\subsection{Shading Summary}\label{shading-summary}
+
+Similar to the Zone Summary, the Shading Summary:
+
+! \textless{}Shading Summary\textgreater{}, Number of Fixed Detached Shades, Number of Building Detached Shades, Number of Attached Shades
+
+~Shading Summary,0,6,14
+
+\subsubsection{Field: \textless{}Shading Summary\textgreater{}}\label{field-shading-summary}
+
+This field contains the constant ``Shading Summary''.
+
+\subsubsection{Field: Number of Fixed Detached Shades}\label{field-number-of-fixed-detached-shades}
+
+This field contains the number of fixed detached shades (e.g.~Shading:Site or Shading:Site:Detailed) in the simulation.
+
+\subsubsection{Field: Number of Building Detached Shades}\label{field-number-of-building-detached-shades}
+
+This field contains the number of building relative detached shades (e.g.~Shading:Building or Shading:Building:Detailed) in the simulation.
+
+\subsubsection{Field: Number of Attached Shades}\label{field-number-of-attached-shades}
+
+This field contains the number of building attached shading surfaces (e.g.~Overhang, Shading:Zone:Detailed, etc.) in the simulation.
+
+\subsection{Surface Details Report}\label{surface-details-report}
+
+A good example of this is the surface details report(s) (\textbf{Output:Surfaces:List, Details;} \textbf{Output:Surfaces:List, Vertices; Output:Surfaces:List, DetailsWithVertices;}). Excerpt from the file:
+
+\textbf{Line 1:}! \textless{}Zone/Shading Surfaces\textgreater{}\textbf{,}\textless{}Zone Name\textgreater{}/\#Shading Surfaces,\# Surfaces, Vertices are shown starting at Upper-Left-Corner = \textgreater{} Counter-Clockwise = \textgreater{} World Coordinates
+
+\textbf{Line 2:}! \textless{}HeatTransfer/Shading/Frame/Divider\_Surface\textgreater{},Surface Name,Surface Class, Base Surface,Construction,Nominal U (w/o film coefs),Nominal U (with film coefs),Area (Net), Area (Gross), Area (Sunlit Calc), Aimuth, Tilt, \textasciitilde{}Width, \textasciitilde{}Height, Reveal, \textless{}ExtBoundCondition\textgreater{}, \textless{}ExtConvCoeffCalc\textgreater{}, \textless{}IntConvCoeffCalc\textgreater{},\textless{}SunExposure\textgreater{},\textless{}WindExposure\textgreater{},ViewFactorToGround,ViewFactorToSky,ViewFactorToGround-IR,ViewFactorToSky-IR,\#Sides, \{Vertex 1\},,, \{Vertex 2\},,, \{Vertex 3\},,, \{Vertex 4\}, ,,\{etc\}
+
+\textbf{Line 3:} ! \textless{}Units\textgreater{},,,,,\{W/m2-K\},\{W/m2-K\},\{m2\},\{m2\},\{m2\},\{deg\},\{deg\},\{m\},\{m\},\{m\},,,,,,,,,,X \{m\},Y \{m\},Z \{m\},X \{m\},Y \{m\},Z \{m\},X \{m\},Y \{m\},Z \{m\},X \{m\},Y \{m\},Z \{m\}
+
+\textbf{Ex Line 1:} Shading\_Surfaces,Number of Shading Surfaces,~~ 10
+
+\textbf{Ex Line 2:} Shading\_Surface,WEST SIDE BUSHES,Detached Shading:Building,,,,, 180.0, 180.0, 180.0, 90.0, 90.0, 60.00, 3.00,,,,,,,,,,, 4, -5.00, 0.00, 3.00, -5.00, 0.00, 0.00, -5.00, 60.00, 0.00, -5.00, 60.00, 3.00
+
+\textbf{Ex Line 2:} Shading\_Surface,EAST SIDE TREE1,Detached Shading:Building,,,,, 500.0, 500.0, 500.0, 270.0, 90.0, 20.00, 50.99,,,,,,,,,,, 3, 70.00, 30.00, 50.00, 70.00, 40.00, 0.00, 70.00, 20.00, 0.00
+
+\textbf{Ex Line 2:} Shading\_Surface,EAST SIDE TREE2,Detached Shading:Building,,,,, 500.0, 500.0, 500.0, 0.0, 90.0, 20.00, 50.99,,,,,,,,,,, 3, 70.00, 30.00, 50.00, 80.00, 30.00, 0.00, 60.00, 30.00, 0.00
+
+\textbf{Ex Line 1:} Zone\_Surfaces,HEARTLAND AREA,~~ 35
+
+\textbf{Ex Line 2:} HeatTransfer\_Surface,ZN001:WALL001,Wall,,EXTERIOR,0.644, 0.588, 136.0, 200.0, 136.0, 180.0, 90.0, 20.0, 10.0, 0.00,ExternalEnvironment,ASHRAEDetailed,ASHRAEDetailed,SunExposed,WindExposed, 0.50, 0.50, 0.67,~ 0.33, 4, 20.00, 10.00, 10.00, 20.00, 10.00, 0.00, 40.00, 10.00, 0.00, 40.00, 10.00, 10.00
+
+\textbf{Ex Line 2:} HeatTransfer\_Surface,ZN001:WALL001:WIN001,Window,ZN001:WALL001,SINGLE PANE HW WINDOW,N/A,6.121, 64.00000, 64.00000, 64.00000,180.0, 90.0, 8.00, 8.00, 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed,~ 0.50,~ 0.50,~ 0.71,~ 0.29, 4, 26.00, 10.00, 8.10, 26.00, 10.00, 0.10, 34.00, 10.00, 0.10, 34.00, 10.00, 8.10
+
+\textbf{Ex Line 2:} HeatTransfer\_Surface,ZN001:WALL002,Wall,,EXTERIOR,0.644,0.588, 155.0, 200.0, 155.0, 90.0, 90.0, 20.00, 10.00, 0.00,ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed, 0.50,~ 0.50,~ 0.73,~ 0.27, 4, 50.00, 20.00, 10.00, 50.00, 20.00, 0.00, 50.00, 40.00, 0.00, 50.00, 40.00, 10.00
+
+\textbf{Ex Line 2:} HeatTransfer\_Surface,ZN001:WALL002:WIN001,Window,ZN001:WALL002,SINGLE PANE HW WINDOW,N/A,6.121, 15.0, 15.0, 15.0, 90.0, 90.0, 3.00, 5.00,~ 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed,~ 0.50,~ 0.50,~ 0.76,~ 0.24, 4, 50.00, 22.20, 7.30, 50.00, 22.20, 2.30, 50.00, 25.20, 2.30, 50.00, 25.20, 7.30
+
+\textbf{Ex Line 2:} HeatTransfer\_Surface,ZN001:WALL002:WIN002,Window,ZN001:WALL002,SINGLE PANE HW WINDOW, N/A, 6.121, 15.00, 15.00, 15.00, 90.00, 90.00, 3.00, 5.00, 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed, 0.50, 0.50, 0.71, 0.29, 4, 50.00, 28.50, 7.30, 50.00, 28.50, 2.30, 50.00, 31.50, 2.30, 50.00, 31.50, 7.30
+
+\textbf{Ex Line 2:} HeatTransfer\_Surface, ZN001:WALL002:WIN003, Window, ZN001:WALL002, SINGLE PANE HW WINDOW, N/A, 6.121, 15.00, 15.00, 15.00, 90.00, 90.00, 3.00, 5.00, 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed, 0.50, 0.50, 0.77, 0.23, 4, 50.00, 35.30, 7.30, 50.00, 35.30, 2.30, 50.00, 38.30, 2.30, 50.00, 38.30, 7.30
+
+\textless{}reduced for brevity\textgreater{}
+
+\textbf{Ex Line 1:} Zone\_Surfaces,MAINE WING,~~ 12
+
+\textbf{Ex Line 2:} HeatTransfer\_Surface, ZN005:WALL001, Wall, , EXTERIOR, 0.644, 0.588, 100.00, 100.00, 100.00, 180.00, 90.00, 10.00, 10.00, 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed, 0.50, 0.50, 0.74, 0.26, 4, 50.00, 40.00, 10.00, 50.00, 40.00, 0.00, 60.00, 40.00, 0.00, 60.00, 40.00, 10.00
+
+\textbf{Ex Line 2:} HeatTransfer\_Surface, ZN005:FLR001, Floor, , SLAB FLOOR, 17.040, 3.314, 400.00, 400.00, 400.00, 90.00, 180.00, 20.00, 20.00, 0.00, Ground, N/A-Ground, ASHRAEDetailed, NoSun, NoWind, 1.00, 0.00, 1.00, 0.00, 4, 60.00, 40.00, 0.00, 40.00, 40.00, 0.00, 40.00, 60.00, 0.00, 60.00, 60.00, 0.00
+
+\textbf{Ex Line 2:} HeatTransfer\_Surface, ZN005:ROOF001, Roof, , ROOF31, 0.790, 0.688, 400.00, 400.00, 400.00, 180.00, 0.00, 20.00, 20.00, 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed, 0.00, 1.00, 2.41E-002, 0.98, 4, 40.00, 60.00, 10.00, 40.00, 40.00, 10.00, 60.00, 40.00, 10.00, 60.00, 60.00, 10.00
+
+\subsubsection{Description of the Detailed Surfaces Report(s)}\label{description-of-the-detailed-surfaces-reports}
+
+The preceding excerpt includes the surface details \emph{and} vertices. You can also obtain the report with \emph{just} the details or \emph{just} the vertices.
+
+\textbf{Line 1:}! \textless{}Zone/Shading Surfaces\textgreater{}\textbf{,}\textless{}Zone Name\textgreater{}/\#Shading Surfaces,\# Surfaces, Vertices are shown starting at Upper-Left-Corner = \textgreater{} Counter-Clockwise = \textgreater{} World Coordinates
+
+When a line is shown with the comment character (!) in the first position, it signifies a informational ``header'' record for the report. In addition, ``Line 1'' is also a header for the subsequent ``real'' surface lines.
+
+\subsubsection{Field: \textless{}Zone/Shading Surfaces\textgreater{}}\label{field-zoneshading-surfaces}
+
+This field is a dual purpose field. For beginning of the Shading Surfaces, it will show ``Shading\_Surfaces''. At each Zone, it will show ``Zone\_Surfaces''.
+
+\subsubsection{Field: \textless{}Zone Name\textgreater{}/\#Shading Surfaces}\label{field-zone-nameshading-surfaces}
+
+This field is a dual purpose field. It will either show the Zone Name of the subsequent surfaces or the ``Number of Shading Surfaces'' for the entire building.
+
+\subsubsection{Field: \# Surfaces}\label{field-surfaces}
+
+This field, then, specifies the number of surfaces of the type (zone or shading) that will follow.
+
+The example lines illustrate:
+
+Shading\_Surfaces,Number of Shading Surfaces,~~ 10
+
+Zone\_Surfaces,HEARTLAND AREA,~~ 35
+
+Zone\_Surfaces,MAINE WING,~~ 12
+
+\textbf{Line 2:}! \textless{}HeatTransfer/Shading/Frame/Divider\_Surface\textgreater{}, Surface Name, Surface Class, Base Surface, Construction, Nominal U (w/o film coefs), Nominal U (with film coefs), Area (Net), Area (Gross), Area (Sunlit Calc), Azimuth, Tilt, \textasciitilde{}Width, \textasciitilde{}Height, Reveal, \textless{}ExtBoundCondition\textgreater{}, \textless{}ExtConvCoeffCalc\textgreater{}, \textless{}IntConvCoeffCalc\textgreater{}, \textless{}SunExposure\textgreater{}, \textless{}WindExposure\textgreater{}, ViewFactorToGround, ViewFactorToSky, ViewFactorToGround-IR, ViewFactorToSky-IR, \#Sides, \{Vertex 1\},,, \{Vertex 2\},,, \{Vertex 3\},,, \{Vertex 4\}, ,,\{etc\}
+
+\textbf{Line 3:} ! \textless{}Units\textgreater{},,,,,\{W/m2-K\},\{W/m2-K\},\{m2\},\{m2\},\{m2\},\{deg\},\{deg\},\{m\},\{m\},\{m\},,,,,,,,,,X \{m\},Y \{m\},Z \{m\},X \{m\},Y \{m\},Z \{m\},X \{m\},Y \{m\},Z \{m\},X \{m\},Y \{m\},Z \{m\}
+
+Line 2 shows the full detail of each surface record with Line 3 used for illustrating the units of individual fields (as appropriate).
+
+The first four fields (\textless{}HeatTransfer/ShadingSurface\textgreater{},Surface Name, Surface Class, Base Surface) are included in all the Surface reports (Details, Vertices, Details with Vertices).
+
+\subsubsection{Field: \textless{}HeatTransfer/Shading/Frame/Divider\_Surface\textgreater{}}\label{field-heattransfershadingframedividerux5fsurface}
+
+For shading surfaces, this will be a constant ``Shading\_Surface''. For heat transfer surfaces, this will be a constant ``HeatTransfer\_Surface''. For Frame and Divider Surfaces, it will be a constant ``Frame/Divider\_Surface'' with the proper type showing in the Surface Class.
+
+\subsubsection{Field: Surface Name}\label{field-surface-name}
+
+This field will contain the actual surface name as entered in the IDF.
+
+\subsubsection{Field: Surface Class}\label{field-surface-class}
+
+This field contains the surface class (e.g.~Window, Door, Wall, Roof) as entered in the IDF.
+
+\subsubsection{Field: Base Surface}\label{field-base-surface}
+
+This field contains the base surface name if this surface is a sub-surface (i.e.~Window, Door).
+
+\subsubsection{Fields in Details and Details with Vertices report.}\label{fields-in-details-and-details-with-vertices-report.}
+
+\subsubsection{Field: Construction}\label{field-construction}
+
+This field will contain the name of the construction used for the surface. (Will be empty for shading surfaces).
+
+\subsubsection{Field: Nominal U (w/o film coefs)}\label{field-nominal-u-wo-film-coefs}
+
+A nominal thermal conductance for the surface is calculated for the surface. It does not include interior or exterior film coefficients as this is calculated during the simulation and is dependent on several factors that may change during the simulation time period. Units for this field are W/m\(^{2}\)-K.
+
+For windows, no value is reported because the film coefficients cannot be removed from the U-value.
+
+\subsubsection{Field: Nominal U (with film coefs)}\label{field-nominal-u-with-film-coefs}
+
+A nominal thermal conductance for the surface is calculated for the surface, including film coefficients. Units for this field are W/m\(^{2}\)-K.
+
+For opaque surfaces, interior and exterior film coefficients are added to the surface construction based on the prescribed R-values for interior and exterior film coefficients as found in ASHRAE 90.1-2004, Appendix A, and shown below:~ The SI values are the exact values used inside EnergyPlus.
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+NOTE:~ The resulting ``Nominal U with film coefs'' is only for comparison purposes with the ASHRAE 90.1 requirements. Actual film coefficients are calculated during the simulation and are dependent on several factors that may change during the simulation time period.
+
+For windows, the ``Nominal U with film coefs'' is calculated using the following assumptions from the WINDOW 5 program (also NFRC winter conditions):
+
+\begin{itemize}
+\item
+  Indoor air temperature = 21 C (69.8 F)
+\item
+  Outdoor air temperature = -18 C (-.4 F)
+\item
+  Exterior film coefficient = ~ 26 W/m\(^{2}\) (4.58 ft\(^{2}\)-F-hr/BTU)
+\item
+  Interior film coefficient = Calculated by EnergyPlus convection algorithm
+\item
+  No incident solar beam radiation
+\end{itemize}
+
+\subsubsection{Field: Area (Net)}\label{field-area-net}
+
+When surfaces are entered, the gross area of the surface is calculated from the vertices (except for Internal Mass where it is entered directly). As net area is needed in the calculations, any sub-surfaces to the primary surface are subtracted from the original gross area. This field will show the final ``net'' area for the surface. For example, walls with windows will have the multiplier (of the window) * window area subtracted from the gross amount. Likewise, any divider area (including multipliers) for the window will be subtracted. Units for this field are m\(^{2}\).
+
+\subsubsection{Field: Area (Gross)}\label{field-area-gross}
+
+This field shows the gross area of the surface. Units for this field are m\(^{2}\).
+
+\subsubsection{Field: Area (Sunlit Calc)}\label{field-area-sunlit-calc}
+
+This field shows the net area for the purposes of sunlit/shading calculations. For these, only 1 unit of a multiplied window/door is subtracted from the gross area of a wall that the window/door is on. This net area includes the \emph{frame area} (if any) for the windows on the wall. For windows, this value includes the divider area of the window. Thus for both frames and dividers, there will be a * in this field -- since the areas are included in the wall/window areas. Units for this field are m\(^{2}\).
+
+\subsubsection{Field: Azimuth}\label{field-azimuth}
+
+Using the specified vertices for the surface (and order of entry), EnergyPlus can determine the outward facing normal angle for the surface. That angle is displayed in this field. Units for this field are degrees.
+
+\subsubsection{Field: Tilt}\label{field-tilt}
+
+Using the specified vertices for the surface (and order of entry), EnergyPlus can determine the tilt of the surface with respect to ``horizontal''. That angle is displayed in this field. Units for this field are degrees.
+
+\subsubsection{Field: \textasciitilde{}Width}\label{field-width}
+
+This field (approximate width of the surface) is calculated and filled by EnergyPlus from the entered vertices. Some parts of EnergyPlus use a width and height rather than the more detailed vertex/area calculations. Units for this field are m.
+
+\subsubsection{Field: \textasciitilde{}Height}\label{field-height}
+
+This field (approximate height of the surface) is calculated and filled by EnergyPlus from the entered vertices. Some parts of EnergyPlus use a width and height rather than the more detailed vertex/area calculations. Units for this field are m.
+
+\subsubsection{Field: Reveal}\label{field-reveal}
+
+This field is calculated for sub-surfaces with respect to their base surfaces using the entered vertices, plane of the two surfaces, and distance between the planes. Reveal may be important in shading of windows, in particular. Units for this field are m.
+
+\subsubsection{Field: \textless{}ExtBoundCondition\textgreater{}}\label{field-extboundcondition}
+
+This field shows the exterior boundary condition for the surface. If this is a surface that is ``external'' the values will be \textbf{ExternalEnvironment} or \textbf{Ground}. If this surface is an interzone surface, this value will be the surface name in the ``other'' zone. If this surface is an internal surface, this value will be the same as the surface name. If this is a special surface with ``Other Side Coefficients'', the value will be the OtherSideCoefficient name (see description of OtherSideCoefficient reporting later in this document). If this is a special surface with ``Other Side Condition Model'', the value will be the OtherSideConditionModel name.
+
+\subsubsection{Field: \textless{}ExtConvCoeffCalc\textgreater{}}\label{field-extconvcoeffcalc}
+
+The value for this field will be a descriptor of the External Convection Coefficient calculation. If this surface uses Other Side Coefficients, this field will display \textbf{N/A-OSC}. If this surface uses Other Side Condition Model, this field will display \textbf{N/A-OSCM}. Ground surfaces will display \textbf{N/A-Ground}. If this is an interior or inter-zone surface, it will display \textbf{Other/Same Surface Int Conv}. If a schedule is used, it will display \textbf{User Supplied Schedule.} If a constant value is supplied by the user, it will display \textbf{User Supplied Value}. The standard values may also be displayed here (e.g. \textbf{ASHRAEDetailed}).
+
+\subsubsection{Field: \textless{}IntConvCoeffCalc\textgreater{}}\label{field-intconvcoeffcalc}
+
+The value for this field will be a descriptor of the Internal Convection Coefficient calculation. If a schedule is used, it will display \textbf{User Supplied Schedule.} If a constant value is supplied by the user, it will display \textbf{User Supplied Value}. The standard values may also be displayed here (e.g. \textbf{ASHRAEDetailed}).
+
+\subsubsection{Field: \textless{}SunExposure\textgreater{}}\label{field-sunexposure}
+
+The value for this field will be \textbf{SunExposed} or \textbf{NoSun}. Internal surfaces should have NoSun exposure.
+
+\subsubsection{Field: \textless{}WindExposure\textgreater{}}\label{field-windexposure}
+
+The value for this field will be \textbf{WindExposed} or \textbf{NoWind}. Internal surfaces should have NoWind exposure.
+
+\subsubsection{Field: ViewFactorToGround}\label{field-viewfactortoground}
+
+This value has been entered as part of the surface description. View factor to ground is described in the Input Output Reference document during the Surface:HeatTransfer description.
+
+\subsubsection{Field: ViewFactorToSky}\label{field-viewfactortosky}
+
+This value is calculated by EnergyPlus based on surface tilt and shadowing surfaces.
+
+\subsubsection{Field: ViewFactorToGround-IR}\label{field-viewfactortoground-ir}
+
+This value is calculated by EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground IR view factor.
+
+\subsubsection{Field: ViewFactorToSky-IR}\label{field-viewfactortosky-ir}
+
+This value is calculated by EnergyPlus based on surface tilt and shadowing surfaces.
+
+\subsubsection{Field: \#Sides}\label{field-sides}
+
+This value is the number of sides / vertices the surface has.
+
+\subsubsection{Fields in Vertices Reports}\label{fields-in-vertices-reports}
+
+\subsubsection{Field Set: Vertex x {[}X \{m\}, Y \{m\}, Z \{m\}{]}}\label{field-set-vertex-x-x-m-y-m-z-m}
+
+For each side of the surface, the vertices are shown in three separate fields (comma separated) in the EnergyPlus ``standard'' coordinate order (Upper Left Corner first, Counter-Clockwise, World Coordinates). Units for each vertex is m.
+
+\subsection{Calculating with Surface Details Report}\label{calculating-with-surface-details-report}
+
+It is reasonably easy to import this data into a spreadsheet and then calculate glazing area percentage based on wall facing direction:
+
+\begin{figure}[hbtp] % fig 3
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image012.png}
+\caption{Surface Details with Window/Wall \% calculated \protect \label{fig:surface-details-with-windowwall-calculated}}
+\end{figure}
+
+\subsection{Surface Convection Parameters}\label{surface-convection-parameters}
+
+When detailed surface reports are requested, extra information on the surfaces related to how convection coefficients are calculated are also output to the EIO file.~ The first block of data relates to overall geometry parameters assigned to each surface and has the following header
+
+! \textless{}Surface Convection Parameters\textgreater{}, Surface Name, Outside Model Assignment , Outside Area {[}m2{]}, Outside Perimeter {[}m{]}, Outside Height {[}m{]}, Inside Model Assignment, Inside Height {[}cm{]}, Inside Perimeter Envelope {[}m{]}, Inside Hydraulic Diameter {[}m{]}, Window Wall Ratio {[} {]},Window Location {[} {]}, Near Radiant {[}T/F{]}, Has Active HVAC {[}T/F{]}
+
+With example data record.
+
+Surface Convection Parameters,PERIMETER\_ZN\_1\_WALL\_SOUTH,0,84.45,61.48,3.05,0,3.05,27.69,6.94,0.24,0, F, F
+
+\subsubsection{Field: Outside Model Assignment}\label{field-outside-model-assignment}
+
+This is an integer code for the type of model assigned to the outside face, if a specific model has been assigned. Surface(SurfLoop)\%ExtConvCoeff
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Field: Outside Area}\label{field-outside-area}
+
+This is the area used for convection calculations for the outside face.~ It is intended to be a model of the area of the larger group of surfaces that this surfaces is a part of. {[}m\(^{2}\){]}
+
+\subsubsection{Field Outside Perimeter}\label{field-outside-perimeter}
+
+This is the length of edge used for convection calculations for the outside face.~ It is intended to be a model of the perimeter for a larger group of surfaces that surface is a part of.~ {[}m{]}
+
+\subsubsection{Field: Outside Height}\label{field-outside-height}
+
+This is the height scale used for convection calculations for the outside face.~ It is intended to be a model of the overall height of a larger group of surfaces that this surface is a part of. {[}m{]}
+
+\subsubsection{Field: Inside Model Assignment}\label{field-inside-model-assignment}
+
+~This is an integer code for the type of model assigned to the inside face, if a specific model has been assigned. Surface(SurfLoop)\%IntConvCoeff
+
+\subsubsection{Field: Inside Height}\label{field-inside-height}
+
+This is the height scale used for convection calculations for the inside face.~ It is intended to be for the entire zone. {[}m{]}
+
+\subsubsection{Field: Inside Perimeter Envelope}\label{field-inside-perimeter-envelope}
+
+This is the length scale for the zone for the amount of exterior envelope with glazing.~ It is the length of wall that has glazed exterior.{[}m{]}
+
+\subsubsection{Field: Inside Hydraulic Diameter}\label{field-inside-hydraulic-diameter}
+
+This is the length scale for horizontal surfaces in the zone.~~ It is calculated using 4 * area/ perimeter and is used for natural convection on the floor or ceiling. {[}m{]}
+
+\subsubsection{Field: Window to Wall Ratio}\label{field-window-to-wall-ratio}
+
+This is the ratio of exterior window area to exterior wall area.~ It is for the zone. {[}non dimensional{]}
+
+\subsubsection{Field: Window Location}\label{field-window-location}
+
+This is an integer code for relative window positioning.~ It is used for some inside face correlations.
+
+\subsubsection{Field: Near Radiant}\label{field-near-radiant}
+
+This is a true or false flag indicating if this surfaces is near a radiant HVAC unit. If ``T'' then surface is is modeled as near a radiant HVAC device.~ If~ ``F'' then surface is normal.
+
+\subsubsection{Field: Has Active HVAC}\label{field-has-active-hvac}
+
+This is a true or false flag indicating if this surface has active HVAC elements inside it.~ If ``T'' then surface is modeled has having HVAC pipes or element inside it making it active for heating or cooling.~ If~ ``F'' then surface is normal.
+
+\subsection{OtherSideCoefficient Outputs}\label{othersidecoefficient-outputs}
+
+For the most part, the output for the Other Side Coefficients represents the input as entered. The header record for the Other Side Coefficients output is shown below:
+
+\textbf{Line 1:} ! Other Side Coefficients,Name,Combined convective/radiative film coefficient,User selected Constant Temperature,Coefficient modifying the constant temperature term,Coefficient modifying the external dry bulb temperature term,Coefficient modifying the ground temperature term,Coefficient modifying the wind speed term \{s/m\},Coefficient modifying the zone air temperature term,Constant Temperature Schedule Name
+
+\subsubsection{Field: Other Side Coefficients}\label{field-other-side-coefficients}
+
+This field will be filled with the text \textbf{OtherSideCoefficients}.
+
+The report describes the actions for the following equation:
+
+The coefficients listed above are used in the following equation:
+
+\begin{equation}
+T = C_2 T_{zone} + C_3 T_{oadb} + C_4 C_5 + C_6 T_{grnd} + C_7 W_{spd} T_{oadb}
+\end{equation}
+
+where:
+
+\begin{itemize}
+\tightlist
+\item
+  T = Outdoor air Temperature when Combined convective/radiative film Coeff \textgreater{} 0
+\item
+  T = Exterior Surface Temperatre when Combined convective/radiative film Coeff \textless{} = 0
+\item
+  Tzone~ = Temperature of the zone being simulated (°C)
+\item
+  Toadb~ = Dry-bulb temperature of the outdoor air (°C)
+\item
+  Tgrnd~ = Temperature of the ground (°C)
+\item
+  Wspd~ = Outdoor wind speed (m/sec)
+\end{itemize}
+
+\subsubsection{Field: Name}\label{field-name-11}
+
+This is the unique name entered for the OtherSideCoefficient. Note that the surface it applies to will have this name in the \textless{}ExtBoundCondition\textgreater{} field.
+
+\subsubsection{Field: Combined convective/radiative film coefficient}\label{field-combined-convectiveradiative-film-coefficient}
+
+This field is a trigger value. When entered as \textgreater{}0, it is used as the combined convective/radiative film coefficient. The other fields in the OtherSideCoefficient object are used then as well: the remaining fields are used first to calculate the outdoor air temperature for the surface and then to calculate the outside surface temperature based on the outdoor air temperature and the film coefficient. If this field contains \textbf{N/A}, then the remaining fields are used to calculate the surface temperature (not the outdoor air temperature).
+
+\subsubsection{Field: User selected Constant Temperature}\label{field-user-selected-constant-temperature}
+
+This field is a temperature that remains a constant part of the calculation either of the surface or outdoor air temperature. When the schedule option is used, this field will show \textbf{N/A}. The parameter in the equation for this or the schedule value is \textbf{\emph{C5}}.
+
+\subsubsection{Field: Coefficient modifying the constant temperature term}\label{field-coefficient-modifying-the-constant-temperature-term}
+
+This field is multiplied to the previous field when a simple number is entered. This parameter is shown as \textbf{\emph{C4}} in the equation. This parameter is dimensionless. The value of this parameter should be 1.0 if a schedule is used to set \textbf{\emph{C5}}.
+
+\subsubsection{Field: Coefficient modifying the external dry bulb temperature term}\label{field-coefficient-modifying-the-external-dry-bulb-temperature-term}
+
+This field defines a constant coefficient that is applied to the outdoor air dry-bulb temperature. This parameter is shown as \textbf{\emph{C3}} in the equation. This parameter is dimensionless.
+
+\subsubsection{Field: Coefficient modifying the ground temperature term}\label{field-coefficient-modifying-the-ground-temperature-term}
+
+This field defines a constant coefficient that is applied to the ground temperature. This parameter is shown as \textbf{\emph{C6}} in the equation. This parameter is dimensionless.
+
+\subsubsection{Field: Coefficient modifying the wind speed term \{s/m\}}\label{field-coefficient-modifying-the-wind-speed-term-sm}
+
+This field defines a constant coefficient that is applied to the product of the outdoor air dry-bulb temperature and the wind speed. This parameter is shown as \textbf{\emph{C7}} in the equation. This parameter has dimensions of inverse velocity or s/m.
+
+\subsubsection{Field: Coefficient modifying the zone air temperature term}\label{field-coefficient-modifying-the-zone-air-temperature-term}
+
+This field defines a constant coefficient that is applied to the temperature of the zone to which this surface belongs. This parameter is shown as \textbf{\emph{C2}} in the equation. This parameter is dimensionless.
+
+\subsubsection{Field: Constant Temperature Schedule Name}\label{field-constant-temperature-schedule-name}
+
+This field is used to supply a schedule name. That schedule supplies the ``constant'' temperature value \textbf{\emph{C5}}. Note that the value of the \textbf{\emph{C4}} field should normally be 1.0 if a schedule is used for \textbf{\emph{C5}}. If this field contains a value, then constant temperature field will be \textbf{N/A} in this report.
+
+\subsection{Construction Element Outputs}\label{construction-element-outputs}
+
+An optional report (contained in \textbf{eplusout.eio}) gives calculated elements for the materials and constructions used in the input. One report is specific to opaque constructions (note that nominal thermal conductance is calculated).
+
+The report is invoked by including the following in the IDF:
+
+\textbf{Output:Constructions,Constructions;}
+
+\textbf{Line 1:}! \textless{}Construction\textgreater{},Construction Name,\#Layers,\#CTFs,Time Step \{hours\},ThermalConductance \{w/m2-K\},OuterThermalAbsorptance,InnerThermalAbsorptance,OuterSolarAbsorptance,InnerSolarAbsorptance,Roughness
+
+\textbf{Line 2:}! \textless{}Material\textgreater{},Material Name,Thickness \{m\},Conductivity \{w/m-K\},Density \{kg/m3\},Specific Heat \{J/kg-K\},ThermalResistance \{m2-K/w\}
+
+\textbf{Line 3:}! \textless{}Material:Air\textgreater{},Material Name,ThermalResistance \{m2-K/w\}
+
+\textbf{Line 4:}! \textless{}CTF\textgreater{},Time,Outside,Cross,Inside,Flux (except final one)
+
+\textbf{Ex Line 1:} Construction,EXTWALL09, 4,10, 0.250,2.545~~~ ,~~ 0.900,~~ 0.900,~~ 0.930,~~ 0.920,Rough
+
+\textbf{Ex Line 2:} Material,A2 - 4 IN DENSE FACE BRICK,~ 0.1015, 1.245, 2082.400, 920.480,~ 0.8151E-01
+
+\textbf{Ex Line 2:} Material:Air,B1 - AIRSPACE RESISTANCE,~ 0.1604
+
+\textbf{Ex Line 2:} Material,C3 - 4 IN HW CONCRETE BLOCK,~ 0.1015, 0.813,~ 977.126,~ 836.800,~ 0.1249
+
+\textbf{Ex Line 2:} Material,E1 - 3 / 4 IN PLASTER OR GYP BOARD,0.0191,0.726, 1601.846,~ 836.800,~ 0.2622E-01
+
+\textbf{Ex Line 3:} CTF,~ 10,~~~~~ 0.13890138E-11,~~~~~ 0.95367648E-14,~~~~~ 0.62566281E-10,~~~~ -0.39500133E-14
+
+\textbf{Ex Line 3:} CTF,~~ 9,~~~~ -0.32803336E-08,~~~~~ 0.29933755E-10,~~~~ -0.60855613E-07,~~~~~ 0.10196216E-10
+
+\textbf{Ex Line 3:} CTF,~~ 8,~~~~~ 0.23798948E-05,~~~~~ 0.21201413E-07,~~~~~ 0.21649376E-04,~~~~ -0.88463084E-08
+
+\textbf{Ex Line 3:} CTF,~~ 7,~~~~ -0.58681847E-03,~~~~~ 0.38118098E-05,~~~~ -0.26539198E-02,~~~~~ 0.25879187E-05
+
+\textbf{Ex Line 3:} CTF,~~ 6,~~~~~ 0.46201324E-01,~~~~~ 0.18871269E-03,~~~~~ 0.12095720~~~ ,~~~~ -0.26290432E-03
+
+\textbf{Ex Line 3:} CTF,~~ 5,~~~~~ -1.2828328~~~ ,~~~~~ 0.27337395E-02,~~~~~ -2.1646103~~~ ,~~~~~ 0.91268499E-02
+
+\textbf{Ex Line 3:} CTF,~~ 4,~~~~~~ 13.603723~~~ ,~~~~~ 0.11920108E-01,~~~~~~ 17.065325~~~ ,~~~~ -0.12663354
+
+\textbf{Ex Line 3:} CTF,~~ 3,~~~~~ -62.546625~~~ ,~~~~~ 0.15112689E-01,~~~~~ -64.276824~~~ ,~~~~~ 0.73877389
+
+\textbf{Ex Line 3:} CTF,~~ 2,~~~~~~ 133.27916~~~ ,~~~~~ 0.47414487E-02,~~~~~~ 120.00640~~~ ,~~~~~ -1.9706501
+
+\textbf{Ex Line 3:} CTF,~~ 1,~~~~~ -130.02410~~ ~,~~~~~ 0.22383019E-03,~~~~~ -106.88260~~~ ,~~~~~~ 2.3359193
+
+\textbf{Ex Line 3:} CTF,~~ 0,~~~~~~ 46.959981~~~ ,~~~~~ 0.53137072E-06,~~~~~~ 36.168919~~~
+
+\subsection{Opaque Constructions}\label{opaque-constructions}
+
+\subsubsection{Description of the Opaque Construction Report}\label{description-of-the-opaque-construction-report}
+
+The Opaque Construction report has 3 parts for each construction.
+
+Part 1 is the construction name along with some derived values for the entire construction (i.e.~Thermal Conductance) as well as noting other details about the surface (\# CTFs, \#~ Layers).
+
+Part 2 shows the material layers for the construction. This is essentially just an echo of the entered properties of the materials from the IDF.
+
+Part 3 shows the CTFs as calculated for the Construction. CTFs are described more completely in the Engineering Reference document.
+
+\subsubsection{Fields in Part 1 -- Opaque Construction Report}\label{fields-in-part-1-opaque-construction-report}
+
+\subsubsection{Field: \textless{}Construction\textgreater{}}\label{field-construction-1}
+
+This will be filled with the constant ``Construction'' for each Construction line.
+
+\subsubsection{Field: Construction Name}\label{field-construction-name}
+
+This is the name of the construction as entered in the IDF.
+
+\subsubsection{Field: \#Layers}\label{field-layers}
+
+This is the number of material layers inferred from the construction entry in the IDF. Material layers are listed ``outside'' to ``inside'' of the construction. This, of course, depends on the placement of the surface in the building -- the ``outside'' of an internal surface is the layer that is closest to whatever the surface touches whereas the ``inside'' of an internal surface is the layer that shows in the surface's ``zone''. The outside of an external surface is the layer that faces the outside environment and, again, the inside is the layer that shows in the zone.
+
+\subsubsection{Field: \#CTFs}\label{field-ctfs}
+
+This is the calculated number of CTFs (Conduction Transfer Functions). The conduction transfer functions are temperature and flux coefficients that characterize the thermal properties of the wall.
+
+\subsubsection{Field: Time Step}\label{field-time-step}
+
+The ``timestep'' in the construction line is the timestep at which the CTFs are valid. Because CTFs for certain constructions might not be stable at the user specified timestep (might be too ``heavy'' from a thermal mass standpoint), this may be different from the zone timestep (specified in ``TimeStep in Hour''). In all cases though, this will be greater than or equal to the zone timestep. If the timestep for the construction is greater than the zone timestep, E+ will use interpolated histories to solve for the surface heat balances for this surface (see discussion on interpolated histories in the \href{file:///E:/Docs4PDFs/EngineeringDoc.pdf}{Engineering Reference} document).
+
+\subsubsection{Field: Thermal Conductance}\label{field-thermal-conductance}
+
+This is the nominal thermal conductance of the construction calculated without film coefficients. Units are w/m\(^{2}\)-K.
+
+\subsubsection{Field: Outer Thermal Absorptance}\label{field-outer-thermal-absorptance}
+
+This will be the thermal absorptance of the outer material layer.
+
+\subsubsection{Field: Inner Thermal Absorptance}\label{field-inner-thermal-absorptance}
+
+This will be the thermal absorptance of the inner material layer.
+
+\subsubsection{Field: Outer Solar Absorptance}\label{field-outer-solar-absorptance}
+
+This will be the solar absorptance of the outer material layer.
+
+\subsubsection{Field: Inner Solar Absorptance}\label{field-inner-solar-absorptance}
+
+This will be the solar absorptance of the inner material layer.
+
+\subsubsection{Field: Roughness}\label{field-roughness}
+
+The construction takes on the roughness from the outer material layer. Roughness is used in several parts of external environment calculations.
+
+\subsubsection{Fields in Part 2 -- Opaque Construction Report}\label{fields-in-part-2-opaque-construction-report}
+
+\textbf{Line 2:} ! \textless{}Material\textgreater{},Material Name,Thickness \{m\},Conductivity \{w/m-K\},Density \{kg/m3\},Specific Heat \{J/kg-K\},ThermalResistance \{m2-K/w\}
+
+In this version of part 2, the full material properties are entered by the user and displayed in the report.
+
+\subsubsection{Field: \textless{}Material\textgreater{}}\label{field-material}
+
+This will be filled with the constant ``Material'' for each material layer line.
+
+\subsubsection{Field: Material Name}\label{field-material-name}
+
+This is the name of the material as entered in the IDF.
+
+\subsubsection{Field: Thickness}\label{field-thickness}
+
+This is the entered thickness of the material. Units are m.
+
+\subsubsection{Field: Conductivity}\label{field-conductivity}
+
+For Material:Regular materials, this will be the entered conductivity in w/m-K. For Material:Regular-R materials, this will be shown as 0.0.
+
+\subsubsection{Field: Density}\label{field-density}
+
+For Material:Regular materials, this will be the entered density in kg/m\(^{3}\). For Material:Regular-R materials, this will be shown as 0.0.
+
+\subsubsection{Field: Specific Heat}\label{field-specific-heat}
+
+For Material:Regular materials, this will be the entered specific heat in J/kg-K. For Material:Regular-R materials, this will be shown as 0.0.
+
+\subsubsection{Field: Thermal Resistance}\label{field-thermal-resistance}
+
+For Material:Regular-R materials, this is the entered thermal resistance in m\(^{2}\)-K/w. For Material:Regular materials, this is the calculated thermal resistance based on the other properties.
+
+\textbf{Line 3:} ! \textless{}Material:Air\textgreater{},Material Name,ThermalResistance \{m2-K/w\}
+
+In this version of part 2, only the thermal resistance of the air layer is entered by the user and displayed in the report.
+
+\subsubsection{Field: \textless{}Material:Air\textgreater{}}\label{field-materialair}
+
+This will be filled with the constant ``Material:Air'' for each material layer line.
+
+\subsubsection{Field: Material Name}\label{field-material-name-1}
+
+This is the name of the material as entered in the IDF.
+
+\subsubsection{Field: Thermal Resistance}\label{field-thermal-resistance-1}
+
+This is the entered thermal resistance in m\(^{2}\)-K/w.
+
+\subsubsection{Fields in Part 3 -- Opaque Construction Report}\label{fields-in-part-3-opaque-construction-report}
+
+\textbf{Line 4:} ! \textless{}CTF\textgreater{},Time,Outside,Cross,Inside,Flux (except final one)
+
+In part 3, the CTF calculations are shown. It is necessary to use the conduction transfer functions labeled ``Inside'' and ``Cross'' to calculate the heat flux at the inside surface and the conduction transfer functions labeled ``Outside'' and ``Cross'' to calculate the heat flux at the outside surface. Inside and outside coefficients will be identical for symmetric walls.
+
+Conduction through constructions such as walls, roofs, floors, etc. is generally characterized as one-dimensional and transient within EnergyPlus. The solution to this partial differential equation results in ``conduction transfer functions'' or CTFs. In a CTF equation, the current heat transfer flux due to conduction through a construction is a function of the current temperature at either face of the surface as well as the history of temperatures at either face and the history of conductive fluxes at this face. CTFs are a simplification of response factors which are based solely on temperature histories and require an ``infinite'' history. The inclusion of heat flux history terms reduces the overall number of terms in the equation for conductive flux significantly, resulting in a more efficient solution.
+
+For each unique combination of materials, there are a unique set of CTFs. While there are other procedures to determine the CTFs for a particular construction, EnergyPlus uses a state-space method (see conduction transfer function documentation) to obtain the CTF coefficients. These coefficients are calculated once at the beginning of the simulation and are constant for a particular construction. The CTF equation itself is a linear equation with these constant coefficients.
+
+Conduction heat transfer flux at the outside face of a particular surface is a function of the construction of the surface (which leads to the CTF coefficients), the current and previous temperatures at both the inside and outside face of the surface, and the previous conduction heat transfer fluxes at the outside surface. The CTF coefficients that would be used in this equation would be the ``Outside'' (multiplied by the temperature history at the outside face) terms, the ``Cross'' (multiplied by the temperature history at the inside face) terms, and the ``Flux'' (multiplied by the flux history at the outside face) terms. Solving for the conductive flux at the inside surface would require the use of the ``Inside'' (multiplied by the temperature history at the inside face) terms, the ``Cross'' (multiplied by the temperature history at the outside face) terms, and the ``Flux'' (multiplied by the flux history at the inside face) terms. A textual example is given below for illustration purposes:
+
+Current Outside Conductive Flux = (Outside Term 0) * (Current Outside Face Temperature)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ +(Outside Term 1) * (Previous Outside Face Temperature)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ +(Outside Term 2) * (Outside Face Temperature 2 Time Steps Ago)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ +(Outside Term 3) * (Outside Face Temperature 3 Time Steps Ago)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ + \ldots{}
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ +(Cross Term 0) * (Current Inside Face Temperature)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ +(Cross Term 1) * (Previous Inside Face Temperature)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ +(Cross Term 2) * (Inside Face Temperature 2 Time Steps Ago)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ +(Cross Term 3) * (Inside Face Temperature 3 Time Steps Ago)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ + \ldots{}
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ +(Flux Term 1) * (Previous Outside Face Flux)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ +(Flux Term 2) * (Outside Face Flux 2 Time Steps Ago)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ +(Flux Term 3) * (Outside Face Flux 3 Time Steps Ago)
+
+~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ + \ldots{}
+
+The number of terms is based on the CTF coefficient calculation routine and is related to the amount of thermal mass contained within a particular construction. Actual signs (positive or negative) of various terms in the preceding equation will vary based on their definition and use within the equation. Those interested in more details on the use and calculation of CTFs are encouraged to read the Engineering Documentation.
+
+\subsubsection{Field: \textless{}CTF\textgreater{}}\label{field-ctf}
+
+This will be filled with the constant ``CTF'' for each CTF coefficient line.
+
+\subsubsection{Field: Time}\label{field-time}
+
+This field ``time'' refers to the history term to which the coefficients are applied. The last line is the ``zero'' term that gets applied to the current values of temperatures. The line with a ``1'' refers to the temperatures and fluxes from the previous timestep--previous as in time minus one timestep. Timestep, in this case, is defined by the construction timestep (see description on ``Fields in Part 1 -- Opaque Construction Report'') \emph{not} the zone timestep. Lines with other values are for previous timesteps at t-n(timestep). These are the terms that are used to model conduction through a construction.
+
+\subsubsection{Field: Outside}\label{field-outside}
+
+\subsubsection{Field: Cross}\label{field-cross}
+
+\subsubsection{Field: Inside}\label{field-inside}
+
+\subsubsection{Field: Flux (except final one)}\label{field-flux-except-final-one}
+
+\subsection{Window Constructions}\label{window-constructions}
+
+\subsubsection{Description of the Windows Construction Report}\label{description-of-the-windows-construction-report}
+
+A separate report is available for windows (note that both nominal conductance and Solar Heat Gain Coefficient are calculated for windows). Like the opaque construction, the window construction report has multiple parts -- in this case, 2.
+
+\textbf{Line 1:} ! \textless{}WindowConstruction\textgreater{},Construction Name,\#Layers,Roughness,Conductance \{W/m2-K\},SHGC,SolarTransmittanceNormalIncid,VisibleTransmittanceNormalIncid
+
+\textbf{Line 2:} ! \textless{}WindowMaterial:Glazing\textgreater{}, Material Name, Optical Data Type, Spectral Data Set Name, Thickness \{m\}, Solar Transmittance,Front Solar Reflectance, Back Solar Reflectance, Visible Transmittance, Front Visible Reflectance,Back Visible Reflectance,Infrared Transmittance, Front Thermal Emissivity, Back Thermal Emissivity,Conductivity \{W/m-K\},Dirt Factor,Solar Diffusing
+
+\textbf{Line 3:} ! \textless{}WindowMaterial:Gas\textgreater{},Material Name,GasType,Thickness \{m\}
+
+\textbf{Line 4:} ! \textless{}WindowMaterial:Shade\textgreater{},Material Name,Thickness \{m\},Conductivity \{W/m-K\},ThermalAbsorptance,Transmittance,VisibleTransmittance,ShadeReflectance
+
+\textbf{Line 5:} ! \textless{}WindowMaterial:Screen\textgreater{},Material Name,Thickness \{m\},Conductivity \{W/m-K\},ThermalAbsorptance,Transmittance,Reflectance,VisibleReflectance,DiffuseReflectance,DiffuseVisibleReflectance,ScreenMaterialDiameterToSpacingRatio,ScreenToGlassDistance \{m\}
+
+\textbf{Line 6:} ! \textless{}WindowMaterial:Blind\textgreater{},Material Name,SlatWidth \{m\},SlatSeparation \{m\},SlatThickness \{m\},SlatAngle \{deg\},SlatBeamSolarTransmittance,SlatBeamSolarFrontReflectance,BlindToGlassDistance \{m\}
+
+WindowConstruction,DOUBLE PANE WITH SCREEN,~~ 4,MediumRough,~~ 2.514,~~ 0.555,~~ 0.511,~~ 0.589
+
+~WindowMaterial:Screen,BRIGHT ALUMINUM SCREEN 1, 0.00025,~ 2.210E+02,~ 0.272,~ 0.697,~ 0.166,~ 0.166,~ 0.195,~ 0.195,~ 0.165,~ 0.025
+
+~WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,SpectralAverage,,~ 0.00300,~ 0.83700,~ 0.07500,~ 0.07500,~ 0.89800,~ 0.08100,~ 0.08100,~ 0.00000,~ 0.84000,~ 0.84000,~ 0.90000,~ 1.00000,No
+
+~WindowMaterial:Gas,WINAIRB1 - AIRSPACE RESISTANCE,Air,~ 1.300E-02,
+
+~WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,SpectralAverage,,~ 0.00300,~ 0.83700,~ 0.07500,~ 0.07500,~ 0.89800,~ 0.08100,~ 0.08100,~ 0.00000,~ 0.84000,~ 0.84000,~ 0.90000,~ 1.00000,No
+
+WindowConstruction,DOUBLE PANE WITH SHADE,~~ 4,VerySmooth,~~ 2.716,~~ 0.482,~~ 0.039,~~ 0.050
+
+~WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,SpectralAverage,,~ 0.00300,~ 0.83700,~ 0.07500,~ 0.07500,~ 0.89800,~ 0.08100,~ 0.08100,~ 0.00000,~ 0.84000,~ 0.84000,~ 0.90000,~ 1.00000,No
+
+~WindowMaterial:Gas,WINAIRB1 - AIRSPACE RESISTANCE,Air,~ 1.300E-02,
+
+~WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,SpectralAverage,,~ 0.00300,~ 0.83700,~ 0.07500,~ 0.07500,~ 0.89800,~ 0.08100,~ 0.08100,~ 0.00000,~ 0.84000,~ 0.84000,~ 0.90000,~ 1.00000,No
+
+~WindowMaterial:Shade,SHADE ROLL - LIGHT OPAQUE,~ 0.003,~ 1.000E-01,~ 0.900,~ 0.050,~ 0.050,~ 0.500
+
+WindowConstruction,DOUBLE PANE WITH BLIND,~~ 4,VerySmooth,~~ 2.761,~~ 0.714,~~ 0.395,~~ 0.456
+
+~WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,~ 0.003,~ 0.900,~ 0.837,~ 0.898,~ 0.840,~ 0.840,~ 0.075,~ 0.075,~ 0.081,~ 0.081,~ 1.000,NO
+
+~WindowMaterial:Gas,WINAIRB1 - AIRSPACE RESISTANCE,Air,~ 1.300E-02,
+
+~WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,~ 0.003,~ 0.900,~ 0.837,~ 0.898,~ 0.840,~ 0.840,~ 0.075,~ 0.075,~ 0.081,~ 0.081,~ 1.000,NO
+
+~WindowMaterial:Blind,INTERIOR BLIND, 0.0010, 0.0022, 0.0010,~ 0.000,~ 0.000,~ 0.200,~ 0.025
+
+\subsubsection{Fields in Part 1 -- Window Construction Report}\label{fields-in-part-1-window-construction-report}
+
+\textbf{Line 1:} ! \textless{}WindowConstruction\textgreater{},Construction Name,\#Layers,Roughness,Conductance \{W/m2-K\},SHGC,SolarTransmittanceNormalIncid,VisibleTransmittanceNormalIncid
+
+\subsubsection{Field: \textless{}WindowConstruction\textgreater{}}\label{field-windowconstruction}
+
+This will be filled with the constant ``Construction'' for each Window Construction line.
+
+\subsubsection{Field: Construction Name}\label{field-construction-name-1}
+
+This is the name of the window as entered in the IDF.
+
+\subsubsection{Field: \#Layers}\label{field-layers-1}
+
+This is the number of material layers inferred from the windows construction entry in the IDF. Material layers are listed ``outside'' to ``inside'' of the construction. This, of course, depends on the placement of the surface in the building -- the ``outside'' of an internal surface is the layer that is closest to whatever the surface touches whereas the ``inside'' of an internal surface is the layer that shows in the surface's ``zone''. The outside of an external surface is the layer that faces the outside environment and, again, the inside is the layer that shows in the zone.
+
+\subsubsection{Field: Roughness}\label{field-roughness-1}
+
+The window construction takes on the roughness from the outer material layer. Roughness is used in several parts of external environment calculations.
+
+\subsubsection{Field: Conductance}\label{field-conductance}
+
+This is the center-of-glass conductance of the construction calculated with film coefficients, for winter conditions (indoor air temperature = 21C (69.8F), outdoor air temperature = -18C (-.4F), windspeed = 5.5 m/s (12.3 mph), no solar radiation). Units are W/m\(^{2}\)-K.
+
+\subsubsection{Field: SHGC}\label{field-shgc}
+
+This is the center-of-glass Solar Heat Gain Coefficient for summer conditions (indoor air temperature = 24C (75.2F), outdoor air temperature = 32C (89.6F), windspeed = 2.8 m/s (6.2 mph), 783 W/m2 (248 Btu/h-ft2) incident beam solar radiation normal to glazing.
+
+The following transmittance and reflectance values are for the window glazing (plus shade, screen or blind, if present in the construction). For exterior windows, ``front'' means the side of the window facing the exterior environment and ``back'' means the side facing the zone. For interior windows, ``front'' means the side to window facing the zone and ``back'' means the side facing the adjacent zone.
+
+\subsubsection{Field: Solar Transmittance at Normal Incidence (SolarTransmittanceNormalIncid)}\label{field-solar-transmittance-at-normal-incidence-solartransmittancenormalincid}
+
+Transmittance at normal incidence averaged over the solar spectrum.
+
+\subsubsection{Field: Visible Transmittance at Normal Incidence (VisibleTransmittanceNormalIncid)}\label{field-visible-transmittance-at-normal-incidence-visibletransmittancenormalincid}
+
+Transmittance normal incidence averaged over the solar spectrum and weighted by the response of the human eye.
+
+\subsubsection{Fields in Part 2 -- Window Construction Report}\label{fields-in-part-2-window-construction-report}
+
+Part 2 of the Window Construction Report encompasses several ``lines''.
+
+\textbf{Line 2:} ! \textless{}WindowMaterial:Glazing\textgreater{}, Material Name, Optical Data Type, Spectral Data Set Name, Thickness \{m\}, Solar Transmittance,Front Solar Reflectance, Back Solar Reflectance, Visible Transmittance, Front Visible Reflectance,Back Visible Reflectance,Infrared Transmittance, Front Thermal Emissivity, Back Thermal Emissivity,Conductivity \{W/m-K\},Dirt Factor,Solar Diffusing
+
+\textbf{Line 3:} ! \textless{}WindowMaterial:Gas\textgreater{},Material Name,GasType,Thickness \{m\}
+
+\textbf{Line 4:} ! \textless{}WindowMaterial:Shade\textgreater{},Material Name,Thickness \{m\},Conductivity \{W/m-K\},ThermalAbsorptance,Transmittance,VisibleTransmittance,ShadeReflectance
+
+\textbf{Line 5:} ! \textless{}WindowMaterial:Screen\textgreater{},Material Name,Thickness \{m\},Conductivity \{W/m-K\},ThermalAbsorptance,Transmittance,Reflectance,VisibleReflectance,DiffuseReflectance,DiffuseVisibleReflectance,ScreenMaterialDiameterToSpacingRatio,ScreenToGlassDistance \{m\}
+
+\textbf{Line 6:} ! \textless{}WindowMaterial:Blind\textgreater{},Material Name,SlatWidth \{m\},SlatSeparation \{m\},SlatThickness \{m\},SlatAngle \{deg\},SlatBeamSolarTransmittance,SlatBeamSolarFrontReflectance,BlindToGlassDistance \{m\}
+
+\subsection{\texorpdfstring{Material\textbf{:}WindowGlass}{Material:WindowGlass}}\label{materialwindowglass}
+
+\subsubsection{Field:~ \textless{}Material:WindowGlass\textgreater{}}\label{field-materialwindowglass}
+
+This will be filled with the constant ``Material:WindowGlass'' for each material of this type in the construction.
+
+\subsubsection{Field: Material Name}\label{field-material-name-2}
+
+Name of the glass layer.
+
+\subsubsection{Field: Thickness \{m\}}\label{field-thickness-m}
+
+Thickness of the glass layer.
+
+\subsubsection{Field: Conductivity \{w/m-K\}}\label{field-conductivity-wm-k}
+
+Conductivity of the glass layer.
+
+\subsubsection{Field: SolarTransmittance}\label{field-solartransmittance}
+
+Transmittance of the glass layer at normal incidence averaged over the solar spectrum.
+
+\subsubsection{Field: VisibleTransmittance}\label{field-visibletransmittance}
+
+Transmittance normal incidence of the glass layer averaged over the solar spectrum and weighted by the response of the human eye.
+
+\subsubsection{Field: ThermalFrontAbsorptance}\label{field-thermalfrontabsorptance}
+
+Thermal emissivity of the front face of the glass layer.
+
+\subsubsection{Field: ThermalBackAbsorptance}\label{field-thermalbackabsorptance}
+
+Thermal emissivity of the back face of the glass layer.
+
+\subsubsection{Field: SolarFrontReflectance}\label{field-solarfrontreflectance}
+
+Reflectance of the front face of the glass layer at normal incidence averaged over the solar spectrum.
+
+\subsubsection{Field: SolarBackReflectance}\label{field-solarbackreflectance}
+
+Reflectance of the back face of the glass layer at normal incidence averaged over the solar spectrum.
+
+\subsubsection{Field: VisibleFrontReflectance}\label{field-visiblefrontreflectance}
+
+Reflectance of the front face of the glass layer at normal incidence averaged over the solar spectrum.
+
+\subsubsection{Field: VisibleBackReflectance}\label{field-visiblebackreflectance}
+
+Reflectance of the back face of the glass layer at normal incidence averaged over the solar spectrum.
+
+\subsubsection{Field: GlassTransDirtFactor}\label{field-glasstransdirtfactor}
+
+Glass transmittance dirt factor (1.0 is clear, no dirt factor).
+
+\subsubsection{Field: SolarDiffusing}\label{field-solardiffusing}
+
+Solar Diffusing value -- Yes if solar diffusing glass, No if not.
+
+\subsubsection{Material:WindowGas}\label{materialwindowgas}
+
+\subsubsection{Field:~ \textless{}Material:WindowGas\textgreater{}}\label{field-materialwindowgas}
+
+This will be filled with the constant ``Material:WindowGas'' for each material of this type in the construction.
+
+\subsubsection{Field: Material Name}\label{field-material-name-3}
+
+Name of the gas layer.
+
+\subsubsection{Field: GasType}\label{field-gastype}
+
+Type of the gas layer. Possibilities are Air, Argon, Krypton,~ Xenon, and Custom.
+
+\subsubsection{Field: Thickness \{m\}}\label{field-thickness-m-1}
+
+Thickness of the gas layer.
+
+\subsubsection{Material:WindowShade}\label{materialwindowshade}
+
+\subsubsection{Field:~ \textless{}Material:WindowShade\textgreater{}}\label{field-materialwindowshade}
+
+This will be filled with the constant ``Material:WindowShade'' for each material of this type in the construction.
+
+\subsubsection{Field: Material Name}\label{field-material-name-4}
+
+Name of the window shade layer.
+
+\subsubsection{Field: Thickness \{m\}}\label{field-thickness-m-2}
+
+Thickness of the window shade layer.
+
+\subsubsection{Field: Conductivity \{w/m-K\}}\label{field-conductivity-wm-k-1}
+
+Thermal conductivity of the window shade layer.
+
+\subsubsection{Field: ThermalAbsorptance}\label{field-thermalabsorptance}
+
+Emissivity of the window shade layer (assumed same for front and back faces).
+
+\subsubsection{Field: SolarTransmittance}\label{field-solartransmittance-1}
+
+Transmittance of the window shade layer averaged over the solar spectrum. Assumed same for beam solar radiation and diffuse solar radiation. Transmittance of beam solar radiation is assumed to be independent of angle of incidence.
+
+\subsubsection{Field: VisibleTransmittance}\label{field-visibletransmittance-1}
+
+Transmittance of the window shade layer averaged over the solar spectrum and weighted by the response of the human eye. Assumed same for beam visible radiation and diffuse visible radiation. Transmittance of beam visible radiation is assumed to be independent of angle of incidence.
+
+\subsubsection{Field: ShadeReflectance}\label{field-shadereflectance}
+
+Reflectance of the window shade layer averaged over the solar spectrum. Assumed same for beam solar radiation and diffuse solar radiation. Reflectance of beam solar radiation is assumed to be independent of angle of incidence. Reflectance is assumed to be the same for the front and back faces of the shade layer.
+
+\subsection{Material:WindowBlind}\label{materialwindowblind}
+
+This will be filled with the constant ``Material:WindowBlind'' for each material of this type in the construction.
+
+\subsubsection{Field: \textless{}Material:WindowBlind\textgreater{}}\label{field-materialwindowblind}
+
+\subsubsection{Field: Material Name}\label{field-material-name-5}
+
+Name of the blind layer.
+
+\subsubsection{Field: SlatWidth \{m\}}\label{field-slatwidth-m}
+
+Width of the slats in the blind.
+
+\subsubsection{Field: SlatSeparation \{m\}}\label{field-slatseparation-m}
+
+Distance between the centerline of adjacent slats.
+
+\subsubsection{Field: SlatThickness \{m\}}\label{field-slatthickness-m}
+
+Distance between front and back faces of a slat.
+
+\subsubsection{Field: SlatAngle \{deg\}}\label{field-slatangle-deg}
+
+This is the angle between the glazing outward normal and the slat outward normal, where the outward normal points away from the front face of the slat.
+
+\subsubsection{Field: SlatBeamSolarTransmittance}\label{field-slatbeamsolartransmittance}
+
+The beam solar transmittance of the slat at normal incidence. Any transmitted beam radiation is assumed to be 100\% diffuse (i.e., slats are translucent). Transmittance is assumed to have the same value at other angles of incidence.
+
+\subsubsection{Field: SlatBeamSolarFrontReflectance}\label{field-slatbeamsolarfrontreflectance}
+
+The beam solar reflectance at normal incidence on the front side of the slat. Assumed to have the same value at other angles of incidence (matte finish).
+
+\subsubsection{Field: BlindToGlassDistance \{m\}}\label{field-blindtoglassdistance-m}
+
+Distance from the mid-plane of the blind to the adjacent glass (m).
+
+\subsubsection{Material:WindowScreen}\label{materialwindowscreen}
+
+\subsubsection{Field:~ \textless{}Material:WindowScreen\textgreater{}}\label{field-materialwindowscreen}
+
+This will be filled with the constant ``Material:WindowScreen'' for each material of this type in the construction.
+
+\subsubsection{Field: Material Name}\label{field-material-name-6}
+
+Name of the window screen layer.
+
+\subsubsection{Field: Thickness \{m\}}\label{field-thickness-m-3}
+
+Thickness of the window screen layer (screen material diameter).
+
+\subsubsection{Field: Conductivity \{w/m-K\}}\label{field-conductivity-wm-k-2}
+
+Thermal conductivity of the window screen layer. This is the effective value for the overall screen ``assembly'' including open spaces between the screen material.
+
+\subsubsection{Field: ThermalAbsorptance}\label{field-thermalabsorptance-1}
+
+Emissivity of the window screen layer (assumed same for front and back faces). This is the effective value for the overall screen ``assembly'' including open spaces between the screen material.
+
+\subsubsection{Field: Transmittance}\label{field-transmittance}
+
+Beam transmittance of the window screen layer including any inward reflections from the material surface if specified (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method). This is the effective value for the overall screen ``assembly'' including open spaces between the screen material. The value reported here is for direct normal incidence.
+
+\subsubsection{Field: Reflectance}\label{field-reflectance}
+
+Solar reflectance (beam-to-diffuse) of the window screen layer accounting for inward-reflected beam solar radiation as specified (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method). This is the effective value for the overall screen ``assembly'' including open spaces between the screen material averaged over the solar spectrum. The value reported here is for direct normal incidence.
+
+\subsubsection{Field: VisibleReflectance}\label{field-visiblereflectance}
+
+Visible reflectance (beam-to-diffuse) of the window screen layer accounting for inward-reflected beam solar radiation as specified (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method). This is the effective value for the overall screen ``assembly'' including open spaces between the screen material averaged over the solar spectrum and weighted by the response of the human eye. The value reported here is for direct normal incidence.
+
+\subsubsection{Field: DiffuseReflectance}\label{field-diffusereflectance}
+
+Solar reflectance (diffuse-to-diffuse) of the window screen layer accounting for inward-reflected beam solar radiation as specified (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method). Reflectance of diffuse solar radiation is considered constant and applies to both the front and back surfaces of the screen. Diffuse reflectance is calculated by the model as an average value by integrating the screen's solar reflectance (beam-to-diffuse) over a quarter hemisphere of incident radiation.
+
+\subsubsection{Field: DiffuseVisibleReflectance}\label{field-diffusevisiblereflectance}
+
+Visible reflectance (diffuse-to-diffuse) of the window screen layer accounting for inward-reflected beam solar radiation as specified (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method). Visible reflectance of diffuse solar radiation is considered constant and applies to both the front and back surfaces of the screen. Diffuse visible reflectance is calculated by the model as an average value by integrating the screen's visible beam reflectance (beam-to-diffuse) over a quarter hemisphere of incident radiation.
+
+\subsubsection{Field: ScreenMaterialDiameterToSpacingRatio}\label{field-screenmaterialdiametertospacingratio}
+
+The aspect ratio of the screen material. The aspect ratio is calculated as the ratio of the screen material diameter to screen material spacing.
+
+\subsubsection{Field: ScreenToGlassDistance \{m\}}\label{field-screentoglassdistance-m}
+
+Distance from the mid-plane of the screen to the adjacent glass (m).
+
+\subsection{ThermoChromic Windows}\label{thermochromic-windows}
+
+Windows with Thermochromic constructions are reported similarly to other window constructions. First, you see the window as entered in the IDF:
+
+WindowConstruction,TCWINDOW,~~ 5,VerySmooth,~~ 1.666,~~ 0.429,~~ 0.242,~~ 0.520
+
+~WindowMaterial:Glazing,CLEAR3PPG,Spectral,CLEAR3PPGSP,~ 0.00328,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.84000,~ 0.84000,~ 1.00000,~ 1.00000,No
+
+~WindowMaterial:Gas,AIR 3MM,Air,~ 3.000E-03,
+
+~WindowMaterial:Glazing,WO18RT25,Spectral,WO18RT25SP,~ 0.00750,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.84000,~ 0.84000,~ 0.60000,~ 1.00000,No
+
+~WindowMaterial:Gas,AIR 8MM,Air,~ 8.000E-03,
+
+~WindowMaterial:Glazing,SB60CLEAR3PPG,Spectral,SB60CLEAR3PPGSP,~ 0.00328,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.03500,~ 0.84000,~ 1.00000,~ 1.00000,No
+
+Then, there will be a list of window constructions reported with each one corresponding to a particular temperature of the thermochromic glazing layer. For example, the following excerpt shows a list of window constructions for the thermochromic window TCWINDOW at different temperature of the thermochromic layer - TCWINDOW\_TC\_25 at 25°C, TCWINDOW\_TC\_27 at 27°C, and TCWINDOW\_TC\_29 at 29°C. Detailed properties of the thermochromic glazing layer are also listed for each temperature - WO18RT25 \textbf{at} 25°C, WO18RT27 \textbf{at} 27°C, and WO18RT29 \textbf{at} 29°C.
+
+WindowConstruction,TCWINDOW\_TC\_25,~~ 5,VerySmooth,~~ 1.666,~~ 0.429,~~ 0.242,~~ 0.520
+
+~WindowMaterial:Glazing,CLEAR3PPG,Spectral,CLEAR3PPGSP,~ 0.00328,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.84000,~ 0.84000,~ 1.00000,~ 1.00000,No
+
+~WindowMaterial:Gas,AIR 3MM,Air,~ 3.000E-03,
+
+~WindowMaterial:Glazing,WO18RT25,Spectral,WO18RT25SP,~ 0.00750,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.84000,~ 0.84000,~ 0.60000,~ 1.00000,No
+
+~WindowMaterial:Gas,AIR 8MM,Air,~ 8.000E-03,
+
+~WindowMaterial:Glazing,SB60CLEAR3PPG,Spectral,SB60CLEAR3PPGSP,~ 0.00328,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.03500,~ 0.84000,~ 1.00000,~ 1.00000,No
+
+~WindowConstruction,TCWINDOW\_TC\_27,~~ 5,VerySmooth,~~ 1.666,~~ 0.424,~~ 0.236,~~ 0.504
+
+~WindowMaterial:Glazing,CLEAR3PPG,Spectral,CLEAR3PPGSP,~ 0.00328,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.84000,~ 0.84000,~ 1.00000,~ 1.00000,No
+
+~WindowMaterial:Gas,AIR 3MM,Air,~ 3.000E-03,
+
+~WindowMaterial:Glazing,WO18RT27,Spectral,WO18RT27SP,~ 0.00750,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.84000,~ 0.84000,~ 0.60000,~ 1.00000,No
+
+~WindowMaterial:Gas,AIR 8MM,Air,~ 8.000E-03,
+
+~WindowMaterial:Glazing,SB60CLEAR3PPG,Spectral,SB60CLEAR3PPGSP,~ 0.00328,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.03500,~ 0.84000,~ 1.00000,~ 1.00000,No
+
+~WindowConstruction,TCWINDOW\_TC\_29,~~ 5,VerySmooth,~~ 1.666,~~ 0.419,~~ 0.230,~~ 0.490
+
+~WindowMaterial:Glazing,CLEAR3PPG,Spectral,CLEAR3PPGSP,~ 0.00328,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.84000,~ 0.84000,~ 1.00000,~ 1.00000,No
+
+~WindowMaterial:Gas,AIR 3MM,Air,~ 3.000E-03,
+
+~WindowMaterial:Glazing,WO18RT29,Spectral,WO18RT29SP,~ 0.00750,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.84000,~ 0.84000,~ 0.60000,~ 1.00000,No
+
+~WindowMaterial:Gas,AIR 8MM,Air,~ 8.000E-03,
+
+~WindowMaterial:Glazing,SB60CLEAR3PPG,Spectral,SB60CLEAR3PPGSP,~ 0.00328,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.00000,~ 0.03500,~ 0.84000,~ 1.00000,~ 1.00000,No
+
+\subsection{Complex Fenestration}\label{complex-fenestration}
+
+Complex fenestration is reported in a similar manner as other windows.~ The first line is the header, followed by details about each fenestration object (window).
+
+~! \textless{}WindowConstruction:Complex\textgreater{},Construction Name,Index,\#Layers,U-factor \{W/m2-K\},SHGC
+
+~WindowConstruction:Complex,CFS\_GLZ\_813,6,4,0.544,9.104E-002
+
+~WindowConstruction:Complex,CFS\_GLZ\_2015,7,3,1.777,9.205E-002
+
+~WindowConstruction:Complex,CFS\_GLZ\_2046,8,3,2.418,9.273E-002
+
+~WindowConstruction:Complex,CFS\_GLZ\_2001,9,3,1.989,9.253E-002
+
+\subsubsection{Field: Construction Name}\label{field-construction-name-2}
+
+Name of the complex fenestration construction.
+
+\subsubsection{Field: Index}\label{field-index}
+
+Index number in construction data.
+
+\subsubsection{Field: \#Layers}\label{field-layers-2}
+
+Number of solid layers in the complex fenestration construction.~ This number accounts for glass and shading layers.
+
+\subsubsection{Field: U-factor}\label{field-u-factor}
+
+Complex fenestration U-factor according to ASHRAE winter conditions.
+
+\subsubsection{Field: SHGC}\label{field-shgc-1}
+
+Complex fenestration solar heat gain coefficient according to ASHRAE summer conditions.
+
+\subsection{HAMT Cell Data}\label{hamt-cell-data}
+
+This gives the surface name,the construction name, the origins and cell numbers of the cells used within the HAMT solutions algorithm. The cell numbering starts from the external surface to the internal surface.
+
+! \textless{}HAMT origins\textgreater{}, Surface Name, Construction Name, Cell origins (m)
+
+! \textless{}HAMT cells\textgreater{}, Surface Name, Construction Name, Cell Numbers
+
+HAMT origins,SOUTH WALL,EXTERIOR WALL, 0.0000000, 0.0005729,
+
+0.0026459, 0.0060000, 0.0093541, 0.0114271, 0.0128076, 0.0159588,
+
+0.0219528, 0.0302028, 0.0399012, 0.0500988, 0.0597972, 0.0680472,
+
+0.0740412, 0.0771924, 0.0785729, 0.0806459, 0.0840000, 0.0873541,
+
+0.0894271, 0.0900000
+
+HAMT cells, SOUTH WALL,EXTERIOR
+
+WALL,~~ 1,~~ 2,~~ 3,~~ 4,~~ 5,~~ 6,~~ 7,~~ 8,~~ 9,~ 10,~ 11,~ 12,
+
+13,~ 14,~ 15,~ 16,~ 17,~ 18,~ 19,~ 20,~ 21,~ 22
+
+\subsubsection{Field: Surface Name}\label{field-surface-name-1}
+
+Name of the Surface.
+
+\subsubsection{Field: Construction Name}\label{field-construction-name-3}
+
+Name of the construction.
+
+\subsubsection{Field: Cell origins}\label{field-cell-origins}
+
+Origins of the Cells.
+
+\subsubsection{Field: Cell Numbers}\label{field-cell-numbers}
+
+Numbers for the Cells.
+
+\subsection{Sizing Information}\label{sizing-information}
+
+The sizing information in the .eio file reflects the inputs and results for the zone, system and plant (component). Actual fields/details included depend on the ``autosize'' inputs.
+
+\subsubsection{Timesteps in Zone Design Calculation}\label{timesteps-in-zone-design-calculation}
+
+\textbf{! \textless{}Load Timesteps in Zone Design Calculation Averaging Window\textgreater{}, Value}
+
+~Load Timesteps in Zone Design Calculation Averaging Window,~~~ 1
+
+\subsubsection{Field: Load Timesteps in Zone Design Calculation Averaging Window}\label{field-load-timesteps-in-zone-design-calculation-averaging-window}
+
+The number of load timesteps in the zone design flow sequence averaging window. The default is 1, in which case the calculated zone design flow rates are averaged over the load timestep.
+
+The zone design air flow rate calculation is performed assuming a potentially infinite supply of heating or cooling air at a fixed temperature. Thus, the calculated design air flow rate will always be able to meet any load or change in load no matter how large or abrupt. In reality air flow rates are limited by duct sizes and fan capacities. The idealized zone design flow calculation may result in unrealistically large flow rates, especially if the user is performing the sizing calculations using thermostat schedules with night setup or setback. The calculated zone design flow rates are always averaged over the load timestep. The user may want to perform a broader average to mitigate the effect of thermostat setup and setback and prevent the warm up or cool down flow rates from dominating the design flow rate calculation. Specifying the width of the averaging window allows the user to do this.
+
+For example, if the load calculation timestep is 15 minutes and the user specifies the \emph{timesteps in averaging window}to be 4, the zone design air flows will be averaged over a time period of 1 hour. Specifying 8 would result in averaging over a 2 hour period.
+
+\subsubsection{Sizing Factor Information}\label{sizing-factor-information}
+
+\textbf{! \textless{}Sizing Factor Information\textgreater{}, Sizing Factor ID, Value}
+
+Sizing Factor Information, Global,~~ 1.3000
+
+~Sizing Factor Information, Zone SPACE1-1,~~ 1.3000
+
+~Sizing Factor Information, Zone SPACE2-1,~~ 1.3000
+
+~Sizing Factor Information, Zone SPACE3-1,~~ 1.3000
+
+~Sizing Factor Information, Zone SPACE4-1,~~ 1.3000
+
+~Sizing Factor Information, Zone SPACE5-1,~~ 1.3000
+
+\subsubsection{Field: Sizing Factor ID}\label{field-sizing-factor-id}
+
+Sizing factors can be entered in two places: Sizing Parameters, Zone Sizing. If entered in the Sizing Parameters statement, the Sizing Factor ID is ``Global'' (applied to all if not specified). If entered in the Zone Sizing statement, the Zone and Zone Name designation are shown.
+
+This sizing factor ratio is applied at the zone level to all of the zone heating and cooling loads and air flow rates. These new loads and air flow rates are then used to calculate the system level flow rates and capacities and are used in all of the component sizing calculations.
+
+\subsubsection{Field: Value}\label{field-value}
+
+This is the sizing factor ratio to be applied as described previously.
+
+\subsection{Zone Sizing Information}\label{zone-sizing-information}
+
+! \textless{}Zone Sizing Information\textgreater{}, Zone Name, Load Type, Calc Des Load \{W\}, User Des Load \{W\}, Calc Des Air Flow Rate \{m3/s\}, User Des Air Flow Rate \{m3/s\}, Design Day Name, Date/Time of Peak, Temperature at Peak \{C\}, Humidity Ratio at Peak \{kgWater/kgAir\}, Floor Area \{m2\}, \# Occupants, Calc Outdoor Air Flow Rate \{m3/s\}
+
+~Zone Sizing Information, SPACE1-1, Cooling, 2502.43786, 3253.16922, 0.21023, 0.27329, CHICAGO ANN CLG 1\% CONDNS DB = \textgreater{}MWB, 7/21 16:00:00, 30.85800, 1.45947E-002, 99.16000, 11.00000, 0.10384
+
+~Zone Sizing Information, SPACE1-1, Heating, 2606.90880, 3388.98144, 7.56806E-002, 0.10384, CHICAGO ANN HTG 99\% CONDNS DB, 1/21 23:45:00, -17.30000, 8.38927E-004, 99.16000, 11.00000, 0.10384
+
+~Zone Sizing Information, SPACE2-1, Cooling, 2038.79983, 2650.43978, 0.17125, 0.22263, CHICAGO ANN CLG 1\% CONDNS DB = \textgreater{}MWB, 7/21 10:15:00, 27.83525, 1.45947E-002, 42.73500, 5.00000, 4.72000E-002
+
+~Zone Sizing Information, SPACE2-1, Heating, 1149.09174, 1493.81926, 3.33591E-002, 4.72000E-002, CHICAGO ANN HTG 99\% CONDNS DB, 1/21 24:00:00, -17.30000, 8.38927E-004, 42.73500, 5.00000, 4.72000E-002
+
+~Zone Sizing Information, SPACE3-1, Cooling, 2318.10750, 3013.53976, 0.19473, 0.25315, CHICAGO ANN CLG 1\% CONDNS DB = \textgreater{}MWB, 7/21 15:00:00, 31.50000, 1.45947E-002, 96.48000, 11.00000, 0.10384
+
+~Zone Sizing Information, SPACE3-1, Heating, 2589.95436, 3366.94067, 7.51884E-002, 0.10384, CHICAGO ANN HTG 99\% CONDNS DB, 1/21 23:30:00, -17.30000, 8.38927E-004, 96.48000, 11.00000, 0.10384
+
+~Zone Sizing Information, SPACE4-1, Cooling, 2325.33534, 3022.93594, 0.19534, 0.25394, CHICAGO ANN CLG 1\% CONDNS DB = \textgreater{}MWB, 7/21 17:30:00, 29.46700, 1.45947E-002, 42.73500, 5.00000, 4.72000E-002
+
+~Zone Sizing Information, SPACE4-1, Heating, 1143.87745, 1487.04068, 3.32077E-002, 4.72000E-002, CHICAGO ANN HTG 99\% CONDNS DB, 1/21 23:30:00, -17.30000, 8.38927E-004, 42.73500, 5.00000, 4.72000E-002
+
+~Zone Sizing Information, SPACE5-1, Cooling, 2589.39474, 3366.21317, 0.21753, 0.28279, CHICAGO ANN CLG 1\% CONDNS DB = \textgreater{}MWB, 7/21 15:00:00, 31.50000, 1.45947E-002, 182.49000, 20.00000, 0.18880
+
+~Zone Sizing Information, SPACE5-1, Heating, 1706.17191, 2218.02348, 4.95314E-002, 0.18880, CHICAGO ANN HTG 99\% CONDNS DB, 1/21 23:45:00, -17.30000, 8.38927E-004, 182.49000, 20.00000, 0.18880
+
+\subsubsection{Field: \textless{}Zone Sizing Information\textgreater{}}\label{field-zone-sizing-information}
+
+This field just contains ``Zone Sizing Information''.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-11}
+
+This field contains the Zone Name.
+
+\subsubsection{Field: Load Type}\label{field-load-type}
+
+This field specifies which kind of load is being sized -- Heating or Cooling.
+
+\subsubsection{Field: Calc Des Load \{W\}}\label{field-calc-des-load-w}
+
+The unaltered zone load resulting from the zone sizing calculations, using the design weather and schedules specified in the input.
+
+\subsubsection{Field: User Des Load \{W\}}\label{field-user-des-load-w}
+
+User Des Load is the load after user specified adjustments and is the load actually used for sizing components. Following the calculations (as in the previous field) various adjustments can be made based on user input - the most obvious is a sizing factor; but it could also be something like cooling min air flow per zone area or just a user input design flow rate.
+
+\subsubsection{Field: Calc Des Air Flow Rate \{m3/s\}}\label{field-calc-des-air-flow-rate-m3s}
+
+This is the calculated design air flow rate in m3/s. The calculated design air flow rate is the ``non-adjusted'' air flow rate. It is the air flow rate sufficient to meet the zone loads from the design day simulation.
+
+\subsubsection{Field: User Des Air Flow Rate \{m3/s\}}\label{field-user-des-air-flow-rate-m3s}
+
+User Des Air Flow Rate is the flow rate after user specified adjustments and is the flow rate actually used for sizing components. Following the calculations (as in the previous field) various adjustments can be made based on user input - the most obvious is a sizing factor; but it could also be something like cooling min air flow per zone area or just a user input design flow rate.
+
+\subsubsection{Field: Design Day Name}\label{field-design-day-name}
+
+This is the name of the design day or design run period that triggered the sizing calculations.
+
+\subsubsection{Field: Date/Time of Peak}\label{field-datetime-of-peak}
+
+This is the date and time of the peak load (used for the sizing calculations).
+
+\subsubsection{Field: Temperature at Peak \{C\}}\label{field-temperature-at-peak-c}
+
+This is the temperature (outdoor dry-bulb) at the time of the peak load.
+
+\subsubsection{Field: Humidity Ratio at Peak \{kgWater/kgAir\}}\label{field-humidity-ratio-at-peak-kgwaterkgair}
+
+This is the humidity ratio (outdoor) at the time of the peak load.
+
+\subsubsection{Field: Floor Area \{m2\}}\label{field-floor-area-m2-2}
+
+This is the floor area of the zone.
+
+\subsubsection{Field: \# Occupants}\label{field-occupants-1}
+
+This is the number of occupants in the zone.
+
+\subsubsection{Field: Calc Outdoor air Flow Rate \{m3/s\}}\label{field-calc-outdoor-air-flow-rate-m3s}
+
+This is the calculated outdoor air flow rate.
+
+\subsection{System Sizing Information}\label{system-sizing-information}
+
+\textbf{! \textless{}System Sizing Information\textgreater{}, System Name, Field Description, Value}
+
+~System Sizing Information, VAV SYS 1, Calculated Cooling Design Air Flow Rate {[}m3/s{]}, 1.05725
+
+~System Sizing Information, VAV SYS 1, User Cooling Design Air Flow Rate {[}m3/s{]}, 1.05725
+
+~System Sizing Information, VAV SYS 1, Calculated Heating Design Air Flow Rate {[}m3/s{]}, 0.43343
+
+~System Sizing Information, VAV SYS 1, User Heating Design Air Flow Rate {[}m3/s{]}, 0.43343
+
+\subsubsection{Field: \textless{}System Sizing Information\textgreater{}}\label{field-system-sizing-information}
+
+This field just contains ``System Sizing Information''.
+
+\subsubsection{Field: System Name}\label{field-system-name}
+
+This field contains the system (Air Loop) name.
+
+\subsubsection{Field: Field Description}\label{field-field-description}
+
+This contains the field description and units.
+
+\subsubsection{Field: Value}\label{field-value-1}
+
+This contains the value of the field.
+
+\textbf{\emph{Note:}} ``Calculated'' values are the unaltered result of the system sizing calculations, using the design day weather and schedules given in the input. ``User'' values are the calculated values altered by various user inputs in Sizing:Zone and Sizing:System. For instance, sizing factors will alter the calculated values. Another example would be using the \emph{flow/system} method to specify a system design flow rate.
+
+\subsection{Plant Coincident Sizing Algorithm}\label{plant-coincident-sizing-algorithm}
+
+A special report is issued to the eio file that provides details for the Coincident sizing option. Coincident plant sizing adjustments using HVAC Sizing Simulations run a sizing algorithm at the end of each Sizing Pass. The following report provides details on the calculations and observations from monitoring the previous Sizing Pass.
+
+\begin{lstlisting}
+! <Plant Coincident Sizing Algorithm>,Plant Loop Name,Sizing Pass {#},Measured Mass Flow{kg/s},Measured Demand {W},Demand Calculated Mass Flow{kg/s},Sizes Changed {Yes/No},Previous Volume Flow Rate {m3/s},New Volume Flow Rate {m3/s},Demand Check Applied {Yes/No},Sizing Factor {},Normalized Change {},Specific Heat{J/kg-K},Density {kg/m3}
+Plant Coincident Sizing Algorithm,HOT WATER LOOP,1,0.1062471,11942.67,0.2586269,Yes,7.324432E-004,2.586533E-004,Yes,1.0000,0.646862,4197.9300,999.8980
+Plant Coincident Sizing Algorithm,CHILLED WATER LOOP,1,1.1222815,17614.26,0.6290764,Yes,1.197307E-003,1.122396E-003,No,1.0000,6.256652E-002,4197.9300,999.8980
+\end{lstlisting}
+
+\subsubsection{Field: }\label{field}
+
+This field simply contains the words ``Plant Sizing Coincident Flow Algorithm.''
+
+\subsubsection{Field: Plant Loop Name}\label{field-plant-loop-name}
+
+This field shows the name of the plant loop being analyzed.
+
+\subsubsection{Field: Sizing Pass}\label{field-sizing-pass}
+
+This field shows which sizing pass has just completed prior to running the sizing algorithm. Each Sizing Pass is an iteration of a set of HVAC Sizing Simulations.
+
+\subsubsection{Field: Measured Mass Flow \{kg/s\}}\label{field-measured-mass-flow-kgs}
+
+This is the maximum coincident mass flow rate, in kg/s, found at the supply side inlet system node. This was recorded by a data logging system tracking node mass flow rate over all the sizing periods. It will include any zone timestep averaging.
+
+\subsubsection{Field: Measured Demand \{W\}}\label{field-measured-demand-w}
+
+This is the maximum loop coincident demand, in W, on the supply side. This was recorded by a data logging system tracking the report value for loop demand over all the sizing periods. It will include and zone timestep averaging.
+
+\subsubsection{Field: Demand Calculated Mass Flow \{kg/s\}}\label{field-demand-calculated-mass-flow-kgs}
+
+This is the flow rate, in kg/s, that was calculated from measured demand, the temperature difference in the plant sizing object, and the fluid specific heat.
+
+\subsubsection{Field: Sizes Changed \{Yes/No\}}\label{field-sizes-changed-yesno}
+
+This field indicates if the sizing algorithm resulted in a change of size. If the flows did not change significantly, the sizes might not change.
+
+\subsubsection{Field: Previous Volume Flow Rate \{m3/s\}}\label{field-previous-volume-flow-rate-m3s}
+
+This field is the prior size of the plant loop, in m3/s. This is the size before the adjustment if the size changes.
+
+\subsubsection{Field: New Volume Flow Rate \{m3/s\}}\label{field-new-volume-flow-rate-m3s}
+
+This field is the result of the sizing algorithm, in m3/s. If the size changes, this is the new value used for the plant loop maximum volume flow rate.
+
+\subsubsection{Field: Demand Check Applied \{Yes/No\}}\label{field-demand-check-applied-yesno}
+
+This field indicates if the algorithm produced a new mass flow rate from the measured demand or not. If this field is ``No,'' then the algorithm used coincident mass flow. If this field is ``Yes,'' then the mass flow derived from demand was larger than the measured mass flow and the demand drove the result.
+
+\subsubsection{Field: Sizing Factor}\label{field-sizing-factor}
+
+This field is the value of the sizing factor applied to the measured or calculated coincident flows.
+
+\subsubsection{Field: Normalized Change}\label{field-normalized-change}
+
+This field is the normalized change used to determine if the new flow size is significantly different from the previous.
+
+\subsubsection{Field: Specific Heat \{J/kg-K \}}\label{field-specific-heat-jkg-k}
+
+This is the fluid specific heat, in J/kg-K, used in the calculation of mass flow from the maximum coincident demand.
+
+\subsubsection{Field: Density \{kg/m3\}}\label{field-density-kgm3}
+
+This is the fluid density , in kg/m3, used in the calculation of volume flow rate from the mass flow rate.
+
+\subsection{Component Sizing Information}\label{component-sizing-information}
+
+Component sizing is applicable to all manners of autosized components and equipments (coils, boilers, chillers, towers, humidifiers, namely -- whatever can be autosized)
+
+\textbf{! \textless{}Component Sizing Information\textgreater{}, Component Type, Component Name, Input Field Description, Value}
+
+Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE1-1 VAV REHEAT, Maximum Air Flow Rate {[}m3/s{]}, 0.22672
+
+~Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE1-1 VAV REHEAT, Maximum Reheat Water Flow Rate {[}m3/s{]}, 5.87104E-005
+
+~Component Sizing Information, Coil:Heating:Water, SPACE1-1 ZONE COIL, Maximum Water Flow Rate {[}m3/s{]}, 5.87104E-005
+
+~Component Sizing Information, Coil:Heating:Water, SPACE1-1 ZONE COIL, Design Coil Load {[}W{]}, 2699.50304
+
+~Component Sizing Information, Coil:Heating:Water, SPACE1-1 ZONE COIL, U-Factor Times Area Value {[}W/K{]}, 66.15122
+
+~Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE2-1 VAV REHEAT, Maximum Air Flow Rate {[}m3/s{]}, 0.17666
+
+~Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE2-1 VAV REHEAT, Maximum Reheat Water Flow Rate {[}m3/s{]}, 4.57480E-005
+
+~Component Sizing Information, Coil:Heating:Water, SPACE2-1 ZONE COIL, Maximum Water Flow Rate {[}m3/s{]}, 4.57480E-005
+
+~Component Sizing Information, Coil:Heating:Water, SPACE2-1 ZONE COIL, Design Coil Load {[}W{]}, 2103.49527
+
+~Component Sizing Information, Coil:Heating:Water, SPACE2-1 ZONE COIL, U-Factor Times Area Value {[}W/K{]}, 51.54607
+
+~Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE3-1 VAV REHEAT, Maximum Air Flow Rate {[}m3/s{]}, 0.20944
+
+~Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE3-1 VAV REHEAT, Maximum Reheat Water Flow Rate {[}m3/s{]}, 5.42362E-005
+
+~Component Sizing Information, Coil:Heating:Water, SPACE3-1 ZONE COIL, Maximum Water Flow Rate {[}m3/s{]}, 5.42362E-005
+
+~Component Sizing Information, Coil:Heating:Water, SPACE3-1 ZONE COIL, Design Coil Load {[}W{]}, 2493.78307
+
+~Component Sizing Information, Coil:Heating:Water, SPACE3-1 ZONE COIL, U-Factor Times Area Value {[}W/K{]}, 61.11006
+
+~Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE4-1 VAV REHEAT, Maximum Air Flow Rate {[}m3/s{]}, 0.22257
+
+~Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE4-1 VAV REHEAT, Maximum Reheat Water Flow Rate {[}m3/s{]}, 5.76351E-005
+
+~Component Sizing Information, Coil:Heating:Water, SPACE4-1 ZONE COIL, Maximum Water Flow Rate {[}m3/s{]}, 5.76351E-005
+
+~Component Sizing Information, Coil:Heating:Water, SPACE4-1 ZONE COIL, Design Coil Load {[}W{]}, 2650.06093
+
+~Component Sizing Information, Coil:Heating:Water, SPACE4-1 ZONE COIL, U-Factor Times Area Value {[}W/K{]}, 64.93964
+
+~Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE5-1 VAV REHEAT, Maximum Air Flow Rate {[}m3/s{]}, 0.22187
+
+~Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE5-1 VAV REHEAT, Maximum Reheat Water Flow Rate {[}m3/s{]}, 5.74541E-005
+
+~Component Sizing Information, Coil:Heating:Water, SPACE5-1 ZONE COIL, Maximum Water Flow Rate {[}m3/s{]}, 5.74541E-005
+
+~Component Sizing Information, Coil:Heating:Water, SPACE5-1 ZONE COIL, Design Coil Load {[}W{]}, 2641.74210
+
+~Component Sizing Information, Coil:Heating:Water, SPACE5-1 ZONE COIL, U-Factor Times Area Value {[}W/K{]}, 64.73579
+
+~Component Sizing Information, Branch, VAV SYS 1 MAIN BRANCH, Maximum Flow Rate {[}m3/s{]}, 1.05725
+
+~Component Sizing Information, AirLoopHVAC, VAV SYS 1, Design Supply Air Flow Rate {[}m3/s{]}, 1.05725
+
+~Component Sizing Information, Controller:OutdoorAir, OA CONTROLLER 1, Maximum Outdoor Air Flow Rate {[}m3/s{]}, 1.05725
+
+~Component Sizing Information, Controller:OutdoorAir, OA CONTROLLER 1, Minimum Outdoor Air Flow Rate {[}m3/s{]}, 0.26412
+
+~Component Sizing Information, Coil:Heating:Water, OA HEATING COIL 1, Maximum Water Flow Rate {[}m3/s{]}, 1.48158E-004
+
+~Component Sizing Information, Coil:Heating:Water, OA HEATING COIL 1, Design Coil Load {[}W{]}, 6812.28921
+
+~Component Sizing Information, Coil:Heating:Water, OA HEATING COIL 1, U-Factor Times Area Value {[}W/K{]}, 84.72044
+
+~Component Sizing Information, Coil:Cooling:Water, OA COOLING COIL 1, Design Water Flow Rate {[}m3/s{]}, 1.14523E-003
+
+~Component Sizing Information, Coil:Cooling:Water, OA COOLING COIL 1, Design Air Flow Rate {[}m3/s{]}, 0.26412
+
+~Component Sizing Information, Coil:Cooling:Water, OA COOLING COIL 1, Design Inlet Air Temperature {[}C{]}, 30.01375
+
+Component Sizing Information, Coil:Cooling:Water, OA COOLING COIL 1, Design Outlet Air Humidity Ratio, 8.00000E-003
+
+Component Sizing Information, Coil:Cooling:Water, MAIN COOLING COIL 1, Design Inlet Air Humidity Ratio, 9.33031E-003
+
+~Component Sizing Information, Coil:Cooling:Water, MAIN COOLING COIL 1, Design Outlet Air Humidity Ratio, 8.00000E-003
+
+Component Sizing Information, Coil:Cooling:DX:TwoStageWithHumidityControlMode, ACDXCOIL 2:ACDXCOIL 2 STANDARD MODE-STAGE 1, Rated Air Flow Rate {[}m3/s{]}, 2.04925
+
+~Component Sizing Information, Coil:Heating:Water, MAIN HEATING COIL 1, Maximum Water Flow Rate {[}m3/s{]}, 7.51969E-005
+
+~Component Sizing Information, Coil:Heating:Water, MAIN HEATING COIL 1, Design Coil Load {[}W{]}, 3457.55329
+
+~Component Sizing Information, Coil:Heating:Water, MAIN HEATING COIL 1, U-Factor Times Area Value {[}W/K{]}, 55.78870
+
+~Component Sizing Information, Fan:VariableVolume, SUPPLY FAN 1, Maximum Flow Rate {[}m3/s{]}, 1.05725
+
+~Component Sizing Information, Fan:VariableVolume, SUPPLY FAN 1, Minimum Flow Rate {[}m3/s{]}, 0.35326
+
+~Component Sizing Information, Controller:WaterCoil, OA CC CONTROLLER 1, Maximum Actuated Flow {[}m3/s{]}, 1.14523E-003
+
+~Component Sizing Information, Controller:WaterCoil, OA HC CONTROLLER 1, Maximum Actuated Flow {[}m3/s{]}, 1.48158E-004
+
+~Component Sizing Information, Controller:WaterCoil, CENTRAL COOLING COIL CONTROLLER 1, Maximum Actuated Flow {[}m3/s{]}, 9.16309E-004
+
+~Component Sizing Information, Controller:WaterCoil, CENTRAL HEATING COIL CONTROLLER 1, Maximum Actuated Flow {[}m3/s{]}, 7.51969E-005
+
+~Component Sizing Information, PlantLoop, HOT WATER LOOP, Maximum Loop Flow Rate {[}m3/s{]}, 4.97138E-004
+
+~Component Sizing Information, PlantLoop, HOT WATER LOOP, Plant Loop Volume {[}m3{]}, 0.55928
+
+~Component Sizing Information, PlantLoop, CHILLED WATER LOOP, Maximum Loop Flow Rate {[}m3/s{]}, 2.06154E-003
+
+~Component Sizing Information, PlantLoop, CHILLED WATER LOOP, Plant Loop Volume {[}m3{]}, 2.31923
+
+~Component Sizing Information, Chiller:Electric, CENTRAL CHILLER, Nominal Capacity {[}W{]}, 34468.93699
+
+~Component Sizing Information, Chiller:Electric, CENTRAL CHILLER, Design Chilled Water Flow Rate {[}m3/s{]}, 2.06154E-003
+
+~Component Sizing Information, Boiler:HotWater, CENTRAL BOILER, Nominal Capacity {[}W{]}, 22858.42690
+
+~Component Sizing Information, Boiler:HotWater, CENTRAL BOILER, Design Water Flow Rate {[}m3/s{]}, 4.97138E-004
+
+~Component Sizing Information, Pump:VariableSpeed, HW CIRC PUMP, Rated Flow Rate {[}m3/s{]}, 4.97138E-004
+
+~Component Sizing Information, Pump:VariableSpeed, HW CIRC PUMP, Rated Power Consumption {[}W{]}, 127.01247
+
+~Component Sizing Information, Pump:VariableSpeed, CW CIRC PUMP, Rated Flow Rate {[}m3/s{]}, 2.06154E-003
+
+~Component Sizing Information, Pump:VariableSpeed, CW CIRC PUMP, Rated Power Consumption {[}W{]}, 526.69672
+
+~Component Sizing Information, Humidifier:Steam:Electric, HUMIDIFIER 1, Rated Power {[}W{]}, 9826.56303
+
+Component Sizing Information, Humidifier:Steam:Gas, MAIN GAS HUMIDIFIER, Design Size Nominal Capacity Volume {[}m3/s{]}, 1.05405E-002
+
+Component Sizing Information, Humidifier:Steam:Gas, MAIN GAS HUMIDIFIER, Design Size Rated Power {[}W{]}, 103710.42776
+
+\subsubsection{Field: \textless{}Component Sizing Information\textgreater{}}\label{field-component-sizing-information}
+
+This field simply contains the words ``Component Sizing''.
+
+\subsubsection{Field: ~Component Type}\label{field-component-type}
+
+This field shows the component type (e.g.~Pump:Variable Speed, Plant Loop, Fan:Simple:VariableVolume) being sized.
+
+\subsubsection{Field: ~Component Name}\label{field-component-name}
+
+This field shows the name of the component.
+
+\subsubsection{Field: ~Input Field Description}\label{field-input-field-description}
+
+This field shows the field description/variable with units. When using HVAC Sizing Simulation for advanced sizing methods, there are two versions of the report for each component that might be affected. With HVAC Sizing Simulation, there is a first size value reported, which is the result of the Ideal Loads Sizing Simulation, and there is the final value after all the Sizing Passes have completed. This input field description will have ``Initial'' prepended to the description to indicate that this is the first size, the same report without ``Initial'' is the final size. Note that with HVAC Sizing Simulation, these reports will occur much later in the simulation and hence appear further down in the .eio file.
+
+\subsubsection{Field: ~Value}\label{field-value-2}
+
+This field shows the value of the sized component.
+
+\subsection{Heating/Cooling Coil Capacity Information}\label{heatingcooling-coil-capacity-information}
+
+Water heating coils appear:
+
+! \textless{}Water Heating Coil Capacity Information\textgreater{},Component Type,Name,Nominal Total Capacity \{W\}
+
+Water Heating Coil Capacity Information,Coil:Heating:Water,BASEMENT VAV BOX REHEAT COIL,66543.21
+
+\subsubsection{Field: \textless{}Water Heating Coil Capacity Information\textgreater{}}\label{field-water-heating-coil-capacity-information}
+
+This field simply contains the words ``Water Heating Coil Capacity Information''.
+
+\subsubsection{Field: Component Type}\label{field-component-type-1}
+
+This field contains the component type (e.g.~Coil:Heating:Water).
+
+\subsubsection{Field: Component Name}\label{field-component-name-1}
+
+This field contains the user supplied name for the coil.
+
+\subsubsection{Field: Nominal Total Capacity \{W\}}\label{field-nominal-total-capacity-w}
+
+This field contains the nominal heating capacity of the coil in Watts. The capacity is calculated using the rated inlet conditions: inlet air dry bulb temperature = 16.6C, inlet relative humidity = 50\%, inlet hot water temperature = 82.2C.
+
+! \textless{}Water Cooling Coil Capacity Information\textgreater{},Component Type, Name, Nominal Total Capacity \{W\},Nominal Sensible Capacity \{W\},Nominal Latent Capacity \{W\},Nominal Sensible Heat Ratio, Nominal Coil UA Value \{W/C\}, Nominal Coil Surface Area \{m2\}
+
+Water Cooling Coil Capacity Information, Coil:Cooling:Water, MAIN COOLING COIL 1,37219.64,24969.42,12250.22,0.67,4202.30,42.62
+
+\subsubsection{Field: \textless{}Water Cooling Coil Capacity Information\textgreater{}}\label{field-water-cooling-coil-capacity-information}
+
+This field simply contains the words ``Water Cooling Coil Capacity Information''.
+
+\subsubsection{Field: Component Type}\label{field-component-type-2}
+
+This field contains the component type (e.g.~Coil:Cooling:Water).
+
+\subsubsection{Field: Component Name}\label{field-component-name-2}
+
+This field contains the user supplied name for the coil.
+
+\subsubsection{Field: Nominal Total Capacity \{W\}}\label{field-nominal-total-capacity-w-1}
+
+This field contains the nominal cooling capacity of the coil in Watts.
+
+\subsubsection{Field: Nominal Sensible Capacity \{W\}}\label{field-nominal-sensible-capacity-w}
+
+This field contains the nominal sensible cooling capacity of the coil in Watts.
+
+\subsubsection{Field: Nominal Latent Capacity \{W\}}\label{field-nominal-latent-capacity-w}
+
+This field contains the nominal latent cooling capacity of the coil in Watts.
+
+\subsubsection{Field: Nominal Sensible Heat Ratio Capacity \{W\}}\label{field-nominal-sensible-heat-ratio-capacity-w}
+
+This field contains the nominal sensible heat ratio (SHR) capacity of the coil in Watts.
+
+\subsubsection{Field: Nominal UA Value \{W/C\}}\label{field-nominal-ua-value-wc}
+
+This field contains the nominal cooling coil UA value in Watts per deg C.
+
+\subsubsection{\texorpdfstring{Field: Nominal Surface Area \{m\(^{2}\)\}}{Field: Nominal Surface Area \{m\^{}\{2\}\}}}\label{field-nominal-surface-area-m2}
+
+This field contains the nominal cooling coil surface area in square meter.
+
+\textbf{\emph{Note:}} values labeled ``Nominal'' are calculated using the rated inlet conditions: inlet air dry bulb temperature = 26.67C, inlet air wet bulb temperature = 19.44C, inlet chilled water temperature = 6.67C.
+
+\subsection{Refrigerated Case and WalkIn Output}\label{refrigerated-case-and-walkin-output}
+
+Refrigeration related variables appear in the eio file according to the refrigeration models selected. The total possible header records would show:
+
+! \textless{}\#Refrigeration Compressor Racks\textgreater{},Number of Refrigeration Compressor Racks
+
+! \textless{}Refrigeration Compressor Rack\textgreater{},Compressor Rack Name, \# Refrigerated Cases Connected,\# WalkIn Coolers Connected, Heat Rejection Location, Condenser Type, COP
+
+! \textless{}\#Detailed Refrigeration Systems\textgreater{},Number of Detailed Refrigeration Systems
+
+! \textless{}Detailed Refrigeration System\textgreater{},Refrigeration System Name,Refrigerant Used, \# Refrigerated Cases Connected, \# WalkInCoolers Connected, \#Air Chillers Connected, \# Secondary Loops Served, \# Cascade Condensers Served, \# Mechanical Subcoolers Served, \# Compressors Connected, \# Compression Stages, Intercooler Type, Intercooler Effectiveness, \# Subcoolers Connected, Minimum Condensing Temperature (C)
+
+!~ \textless{}\#Detailed Transcritical Refrigeration Systems\textgreater{},Number of Detailed Transcritical Refrigeration Systems
+
+!~ \textless{}Detailed Transcritical Refrigeration System\textgreater{},Transcritical Refrigeration System Name, Refrigerant Used, \# Medium Temperature Refrigerated Cases Connected, \# Low Temperature Refrigerated Cases Connected, \# Medium Temperature WalkInCoolers Connected, \# Low Temperature WalkInCoolers Connected, \# High Pressure Compressors Connected, \# Low Pressure Compressors Connected, Minimum Condensing Temperature (C)
+
+! \textless{}\#Secondary Refrigeration Systems\textgreater{},Number of Secondary Refrigeration Systems
+
+! \textless{}Secondary Refrigeration System: Fluid Always Liquid\textgreater{}, Secondary Number, Secondary Name, \# Refrigerated Cases Connected, \# WalkIn Coolers Connected, Fluid Name, Capacity (W),Evap Temperature in Secondary Evaporator (C), Approach Temperature Difference (DeltaC), Temperature Range (DeltaC), TotalPumpPower (W)
+
+! \textless{}Secondary Refrigeration System: Liquid Overfeed\textgreater{}, Secondary Number, Secondary Name, \# Refrigerated Cases Connected, \# WalkIn Coolers Connected, Fluid Name, Capacity (W),Evap Temperature in Secondary Evaporator (C), Approach Temperature Difference (DeltaC), Circulating Rate, TotalPumpPower (W)
+
+!~ \textless{}Refrigeration Case\textgreater{},Refrigeration Case Number, Refrigeration Case Name,Zone Name,Zone Node \#,Zone Node Name,Capacity (W/m),LHR,Temperature (C),Length (m),Fan (W/m),Installed Lighting (W/m),Anti-Sweat (W/m),Defrost (W/m)
+
+!~ \textless{}Refrigeration Walk In Cooler\textgreater{}, Walk In Number, Walk In Name,Capacity (W),Temperature (C),Coil Fan (W), Circulating Fan (W), Lighting (W),Heaters (W),Defrost (W), \# Zones
+
+!~~~~~ \textless{}Walk-In Surfaces Facing Zone\textgreater{}, ZoneName, Wall/Ceiling Area (m2), UValue (W/m2-C), AreaStockDoors (m2), HeightStockDoors, UValueStockDoors (W/m2-C), AreaGlassDoors (m2), HeightGlassDoors (m),~ UValueGlassDoors (W/m2-C)
+
+!~ \textless{}Refrigeration Compressor\textgreater{},Compressor Number,Compressor Name,Nominal Capacity (W)
+
+!~ \textless{}Refrigeration Condenser:Air-Cooled\textgreater{},Condenser Number,Condenser Name,Rated Condensing Temperature (C),Rated Capacity (W), Rated Fan Power (W)
+
+!~ \textless{}Refrigeration Condenser:Evaporative-Cooled\textgreater{},Condenser Number,Condenser Name,Rated Capacity (W), Rated Fan Power (W)
+
+!~ \textless{}Refrigeration Condenser:Water-Cooled\textgreater{},Condenser Number,Condenser Name,Rated Condensing Temperature (C),Rated Capacity (W), Rated Water Inlet Temperature (C), Rated Water Flow Rate (m3/s)
+
+!~ \textless{}Refrigeration Condenser:Cascade\textgreater{}, Condenser Number, Condenser Name, Condensing Temperature Control Type, Rated Condensing Temperature (C), Capacity (W), Approach Temperature Difference (DeltaC)
+
+!~ \textless{}Refrigeration GasCooler:Air-Cooled\textgreater{},Gas Cooler Number, Gas Cooler Name, Rated Outlet Pressure (Pa), Rated Outlet Temperature (C), Rated Approach Temperature (C), Rated Capacity (W), Rated Fan Power (W)
+
+!~ \textless{}Secondary Load\textgreater{}, Secondary System Served Name, Secondary Number
+
+!~ \textless{}Cascade Load\textgreater{}, System Name Connected, Condenser Number, Condenser Name
+
+!~ \textless{}Mechanical Subcooler Load\textgreater{}, Subcooler Number, Subcooler Name
+
+!~ \textless{}Refrigeration Mechanical Subcooler\textgreater{}, Subcooler Number, Subcooler Name, Name of System Providing Cooling, Design Outlet Temperature (C)
+
+!~ \textless{}Refrigeration Liquid Suction Subcooler\textgreater{}, Subcooler Number, Subcooler Name, Design Subcooling (DeltaC),Design liquid inlet temperature (C), Design vapor inlet temperature (C)
+
+For example, a supermarket refrigeration system including models for a compressor rack and four detailed systems that include refrigerated cases, walk-ins, subcoolers, air-, water-, and evaporative-cooled condensers, and a secondary loop would show the following data lines following the header lines :
+
+\#Refrigeration Compressor Racks: 1
+
+~Refrigeration Compressor Rack,RACKA,4,0,Outdoors,Air-Cooled,~ 2.500
+
+~~ Refrigeration Case,1,DELI\_CASE:1\_ MULTIDECKDAIRYANDDELICASE,DELI,76,DELI AIR NODE,~ 1442.2,~~ 0.30,~~~ 2.2,~~~ 3.0,~~ 87.6,~~ 38.7,~~ 65.6,~~~ 0.0
+
+~~ Refrigeration Case,3,SALES\_CASE:1\_MEATDISPLAYCASE,SALES,78,SALES AIR NODE,~ 1442.2,~~ 0.10,~~~ 2.2,~~ 33.6,~~ 87.6,~~ 38.7,~~ 65.6,~ 443.0
+
+~~ Refrigeration Case,4,SALES\_CASE:2\_ MULTIDECKDIARYANDDELICASE,SALES,78,SALES AIR NODE,~ 1442.2,~~ 0.30,~~~ 2.2,~~ 49.2,~~ 41.0,~~ 60.0,~~~ 0.0,~~~ 0.0
+
+~~ Refrigeration Case,10,PRODUCE\_CASE:1\_ MULTIDECKDIARYANDDELICASE,PRODUCE,80,PRODUCE AIR NODE,~ 1442.2,~~ 0.30,~~~ 2.2,~~ 30.0,~~ 41.0,~~ 60.0,~~~ 0.0,~~~ 0.0
+
+\#Detailed Refrigeration Systems,4
+
+~Detailed Refrigeration System,MEDIUMTEMPSYSTEM,R22,3,0,0,0,1,3,0,~~~ 25.0
+
+~~ Refrigeration Case,2,FISHDISPLAYCASE,SALESFLOOR,9,SALESFLOOR NODE,~~ 288.4,~~ 0.10,~~~ 1.1,~~ 15.0,~~~ 0.0,~~ 41.6,~~~ 0.0,~~~ 0.0
+
+~~ Refrigeration Case,5,MEATDISPLAYCASE,SALESFLOOR,9,SALESFLOOR NODE,~~ 456.6,~~ 0.10,~~ -4.4,~~ 26.0,~~ 47.2,~~ 86.8,~~ 13.2,~ 585.8
+
+~~ Refrigeration Case,6,MULTIDECKDAIRYANDDELICASE,SALESFLOOR,9,SALESFLOOR NODE,~ 1890.0,~~ 0.30,~~ -1.1,~~ 12.0,~~ 78.7,~ 307.3,~~~ 0.0,~~~ 0.0
+
+~~ Mechanical Subcooler Load, 2,SampleMSC
+
+~~ Refrigeration Compressor,1,MEDTEMP001CARLYLE\_R-22\_MED\_06DR820,~~~~~~~~~~ 15535.
+
+~~ Refrigeration Compressor,2,MEDTEMP002CARLYLE\_R-22\_MED\_06DR820,~~~~~~~~~~ 15535.
+
+~~ Refrigeration Compressor,3,MEDTEMP003CARLYLE\_R-22\_MED\_06DR820,~~~~~~~~~~ 15535.
+
+~~ Refrigeration Condenser:Air-Cooled,1,MEDIUMTEMPCONDENSER~ ,~~~~~~~~ 51.7,~~~~~ 52563.5,~~~~~~ 4000.0
+
+Detailed Refrigeration System,LOWTEMPSYSTEM,R22,3,0,0,0,0,3,1,0,0.80,2,~~~ 25.0
+
+~~ Refrigeration Case,7,OPENWELLICECREAMDISPLAYCASE,SALESFLOOR,9,SALESFLOOR NODE,~~ 441.6,~~ 0.08,~ -34.4,~~ 14.6,~~ 28.7,~~ 42.7,~~ 70.0,~~ 76.5
+
+~~ Refrigeration Case,8,GLASSDOORFROZENFOOD,SALESFLOOR,9,SALESFLOOR NODE,~~ 615.8,~~ 0.13,~ -23.3,~~ 11.7,~~ 57.9,~~ 99.8,~ 218.7, 1106.5
+
+~~ Refrigeration Case,9,WALKINFREEZER,BACKROOM,11,BACKROOM NODE,~ 1098.0,~~ 0.10,~~ -2.2,~~~ 4.3,~ 172.2,~~ 28.1,~~~ 0.0, 1291.7
+
+~~ Refrigeration Compressor,4,LOWTEMP001CARLYLE\_R-22\_LOW\_06CC665,~~~~~~~~~~ 15952.
+
+~~ Refrigeration Compressor,5,LOWTEMP002CARLYLE\_R-22\_LOW\_06DR718,~~~~~~~~~~~ 2940.
+
+~~ Refrigeration Compressor,6,LOWTEMP003CARLYLE\_R-22\_LOW\_06DR718,~~~~~~~~~~~ 2940.
+
+~~ Refrigeration Condenser:Air-Cooled,2,LOWTEMPCONDENSER~ ,~~~~~~~~ 51.7,~~~~~ 34875.5,~~~~~~ 2600.0
+
+~~ Refrigeration Mechanical Subcooler,2,SAMPLEMSC,MEDIUMTEMPSYSTEM,~~~ 10.0
+
+~~ Refrigeration Liquid Suction Subcooler,1,SAMPLELSHX,~~~~ 6.0,~~~ 16.0,~~~~ 0.0
+
+~Detailed Refrigeration System,MEDIUMTEMPSYSTEM2,R22,0,0,1,0,0,3,1,0,0.80,0,~~~ 25.0
+
+~~Secondary Load,SECONDARY,1
+
+~~ Refrigeration Compressor,7,MEDTEMP004CARLYLE\_R-22\_MED\_06DR820,~~~~~~~~~~ 15535.
+
+~~ Refrigeration Compressor,8,MEDTEMP005CARLYLE\_R-22\_MED\_06DR820,~~~~~~~~~~ 15535.
+
+~~ Refrigeration Compressor,9,MEDTEMP006CARLYLE\_R-22\_MED\_06DR820,~~~~~~~~~~ 15535.
+
+~~ Refrigeration Condenser:Evaporative-Cooled,1,MEDIUMTEMPEVAPCOOLEDCONDENSER1~ ,~~~~~ 64800.0,~~~~~~~ 746.0
+
+~Detailed Refrigeration System,LOWTEMPSYSTEM2,R22,4,1,0,0,0,3,1,0,0.80,0,~~~ 25.0
+
+~~ Refrigeration Case,11,OPENWELLICECREAMDISPLAYCASE2,SALESFLOOR,9,SALESFLOOR NODE,~~ 441.6,~~ 0.08,~ -34.4,~~ 14.6,~~ 28.7,~~ 42.7,~~ 70.0,~~ 76.5
+
+~~ Refrigeration Case,12,GLASSDOORFROZENFOODA,SALESFLOOR,9,SALESFLOOR NODE,~~ 615.8,~~ 0.13,~ -23.3,~~~ 4.0,~~ 57.9,~~ 99.8,~ 218.7, 1106.5
+
+~~ Refrigeration Case,13,GLASSDOORFROZENFOODB,SALESFLOOR,9,SALESFLOOR NODE,~~ 615.8,~~ 0.13,~ -23.3,~~~ 4.0,~~ 57.9,~~ 99.8,~ 218.7, 1106.5
+
+~~ Refrigeration Case,14,GLASSDOORFROZENFOODC,SALESFLOOR,9,SALESFLOOR NODE,~~ 615.8,~~ 0.13,~ -23.3,~~~ 4.0,~~ 57.9,~~ 99.8,~ 218.7, 1106.5
+
+~~ Refrigeration Walk In Cooler,~ 1,~ WALKINFREEZER2,~~ 4690.0,~~~~ -2.2,~~~ 735.0,~~~~~ 0.0,~~~ 120.0,~~~~~ 0.0,~~ 5512.0,~~~~~ 0.0,~~ 1
+
+~~~~~~ Walk-In Surfaces Facing Zone,BACKROOM,~~~~ 43.4,~~ 0.2350 ,~~~ 2.00,~~~~ 2.00,~~ 0.3785 ,~~~ 1.00,~~~~ 2.00,~~ 1.2050
+
+~~ Refrigeration Compressor,10,LOWTEMP004CARLYLE\_R-22\_LOW\_06CC665,~~~~~~~~~~ 15952.
+
+~~ Refrigeration Compressor,11,LOWTEMP005CARLYLE\_R-22\_LOW\_06DR718,~~~~~~~~~~~ 2940.
+
+~~ Refrigeration Compressor,12,LOWTEMP006CARLYLE\_R-22\_LOW\_06DR718,~~~~~~~~~~~ 2940.
+
+~~ Refrigeration Condenser:Water-Cooled,2,LOWTEMPCONDENSERWATER~ ,~~~~~~~~ 29.4,~~~~~ 58000.0,~~~~~~~~~ 0.0,~~~~~~~~~ 0.0
+
+\#Secondary Refrigeration Systems,1
+
+~Secondary Refrigeration System: Fluid Always Liquid,1,SECONDARY,3,0,PROGLY30PERCENT, 35000.0, -12.60,~~~ 2.7,~~~ 4.0,~ 725.0,
+
+~ Refrigeration Case,15,FISHDISPLAYCASE2,SALESFLOOR,9,SALESFLOOR NODE,~~ 288.4,~~ 0.10,~~~ 1.1,~~ 15.0,~~~ 0.0,~~ 41.6,~~~ 0.0,~~~ 0.0
+
+~ Refrigeration Case,16,MEATDISPLAYCASE2,SALESFLOOR,9,SALESFLOOR NODE,~~ 456.6,~~ 0.10,~~ -4.4,~~ 26.0,~~ 47.2,~~ 86.8,~~ 13.2,~ 585.8
+
+~ Refrigeration Case,17,MULTIDECKDAIRYANDDELICASE2,SALESFLOOR,9,SALESFLOOR NODE,~ 1890.0,~~ 0.30,~~ -1.1,~~ 12.0,~~ 78.7,~ 307.3,~~~ 0.0,~~~ 0.0
+
+For a supermarket system including a model for a cascade condenser arrangement, the eio would show:
+
+Detailed Refrigeration System,CASCADELOWTEMPSYSTEM,R22,4,1,0,0,0,3,1,0,0.80,0,~~~ -4.0
+
+~~ Refrigeration Case,5,OPENWELLICECREAMDISPLAYCASE,SALESFLOOR,10,SALESFLOOR NODE,~~ 441.6,~~ 0.08,~ -34.4,~~ 14.6,~~ 28.7,~~ 42.7,~~ 70.0,~~ 76.5
+
+~~ Refrigeration Case,6,GLASSDOORFROZENFOODA,SALESFLOOR,10,SALESFLOOR NODE,~~ 615.8,~~ 0.13,~ -23.3,~~~ 4.0,~~ 57.9,~~ 99.8,~ 218.7, 1106.5
+
+~~ Refrigeration Case,7,GLASSDOORFROZENFOODB,SALESFLOOR,10,SALESFLOOR NODE,~~ 615.8,~~ 0.13,~ -23.3,~~~ 4.0,~~ 57.9,~~ 99.8,~ 218.7, 1106.5
+
+~~ Refrigeration Case,8,GLASSDOORFROZENFOODC,SALESFLOOR,10,SALESFLOOR NODE,~~ 615.8,~~ 0.13,~ -23.3,~~~ 4.0,~~ 57.9,~~ 99.8,~ 218.7, 1106.5
+
+~~ Refrigeration Walk In Cooler,~ 1,~ WALKINFREEZER,~~ 4690.0,~~~~ -2.2,~~~ 735.0,~~~~~ 0.0,~~~ 120.0,~~~~~ 0.0,~~ 5512.0,~~~~~ 0.0,~~ 1
+
+~~~~~~ Walk-In Surfaces Facing Zone,BACKROOM,~~~~ 43.4,~~ 0.2350 ,~~~ 2.00,~~~~ 2.00,~~ 0.3785 ,~~~ 2.00,~~~~ 2.00,~~ 1.2050
+
+~~ Refrigeration Compressor,4,LOWTEMP001CARLYLE\_R-22\_LOW\_06CC665,~~~~~~~~~~ 16680.
+
+~~ Refrigeration Compressor,5,LOWTEMP002CARLYLE\_R-22\_LOW\_06DR718,~~~~~~~~~~~ 5523.
+
+~~ Refrigeration Compressor,6,LOWTEMP003CARLYLE\_R-22\_LOW\_06DR718,~~~~~~~~~~~ 5523.
+
+~~ Refrigeration Condenser:Cascade,4,CASCADECONDENSER1,Fixed~ ,~~~~~~~~ -4.0,~~~~~ 20000.0,~~~~~~~~~ 3.0
+
+~Detailed Refrigeration System,CASCADEHIGHTEMPSYSTEM,R22,0,0,0,1,0,4,1,0,0.80,0,~~~ 25.0
+
+~~ Cascade Load,CASCADELOWTEMPSYSTEM,4,CASCADECONDENSER1
+
+~~ Refrigeration Compressor,7,MEDTEMP005CARLYLE\_R-22\_MED\_06DR820,~~~~~~~~~~ 17190.
+
+~~ Refrigeration Compressor,8,MEDTEMP006CARLYLE\_R-22\_MED\_06DR820,~~~~~~~~~~ 17190.
+
+~~ Refrigeration Compressor,9,MEDTEMP007CARLYLE\_R-22\_MED\_06DR820,~~~~~~~~~~ 17190.
+
+~~ Refrigeration Compressor,10,MEDTEMP008CARLYLE\_R-22\_MED\_06DR820,~~~~~~~~~~ 17190.
+
+~~ Refrigeration Condenser:Air-Cooled,3,CASCADETOPSYSTEMCONDENSER~ ,~~~~~~~~ 51.7,~~~~~ 52563.5,~~~~~~ 4000.0
+
+The refrigeration output in the \textbf{eplusout.eio} file shows the number of refrigeration compressor racks, detailed refrigeration systems, detailed transcritical refrigeration systems, and secondary refrigeration systems found in the input data file (IDF). Additional information is shown for each compressor rack and the refrigerated case(s) and walk-in(s) connected to each compressor rack. For the detailed systems, additional information is shown for each refrigerated case(s), walk-in(s), cascade loads, secondary loads, mechanical subcooler loads, compressors, condenser, and mechanical and liquid suction heat exchanger subcoolers connected to the system. For the detailed transcritical refrigeration systems, additional information is shown for each refrigerated case(s), walk-in(s), compressor and gas cooler connected to the system. For secondary refrigeration systems, additional information is shown for each refrigerated case(s) and walk-in(s) connected to the system. For walk-ins, additional information is shown for each zone exchanging energy with that walk-in.
+
+The refrigeration ``header'' records (lines starting with an ``!'') precede all the data lines. The data lines are grouped, showing the number of refrigeration compressor racks specified in the input data file followed by lines that reflect the information for each refrigeration compressor rack followed by the information for each refrigerated case and walk-in connected to this rack. The number of detailed systems is followed by a group of data lines describing the input values for the detailed refrigeration systems and similarly for the secondary refrigeration systems.
+
+This output reflects information for the specified refrigeration equipment along with entries from the IDF (or default data for blank fields). The data are preceded by a description (i.e. \#Refrigeration Compressor Racks, Refrigeration Compressor Rack, Refrigerated Case, \#Orphaned Refrigerated Cases, and Orphaned Refrigerated Case) followed by the information associated with each description.
+
+A final set of ``header'' records and descriptions are output only when a refrigeration object is found in the IDF but is not connected to a refrigeration compressor rack or refrigeration system object (i.e., orphaned).
+
+The following fields define each description and associated information.
+
+\subsubsection{Header Record: \#Refrigeration Compressor Racks}\label{header-record-refrigeration-compressor-racks}
+
+This field simply says ``\#Refrigeration Compressor Racks'' .
+
+\subsubsection{Field: Number ofRefrigeration Compressor Racks}\label{field-number-ofrefrigeration-compressor-racks}
+
+The total number of refrigeration compressor racks simulated. This is the number of Refrigeration:CompressorRack objects found in the IDF.
+
+\subsubsection{Header Record: Refrigeration Compressor Rack}\label{header-record-refrigeration-compressor-rack}
+
+\subsubsection{Field: Compressor Rack Name}\label{field-compressor-rack-name}
+
+The name of the compressor rack simulated. Echoes the field Name in object Refrigeration:CompressorRack from the IDF.
+
+\subsubsection{Field: \# Refrigerated Cases Connected}\label{field-refrigerated-cases-connected}
+
+The total number of refrigerated cases connected to the compressor rack.
+
+\subsubsection{Field: \# WalkInCoolers Connected}\label{field-walkincoolers-connected}
+
+The total number of refrigeration walk-ins connected to the compressor rack.
+
+\subsubsection{Field: Heat Rejection Location}\label{field-heat-rejection-location}
+
+The location of the compressor rack's air-cooled condenser. Echoes the field Heat Rejection Location in object Refrigeration:CompressorRack from the IDF.
+
+\subsubsection{Field: COP}\label{field-cop}
+
+The Coefficient of Performance (W/W) of the compressor rack. Echoes the field Design Compressor Rack COP in object Refrigeration:CompressorRack from the IDF.
+
+\subsubsection{Header Record: Refrigeration Case}\label{header-record-refrigeration-case}
+
+\subsubsection{Field: Refrigeration Case Number}\label{field-refrigeration-case-number}
+
+The number of the refrigerated case, assigned sequentially according to the order in which these objects are defined in the IDF.
+
+\subsubsection{Field: Refrigeration~ Case Name}\label{field-refrigeration-case-name}
+
+The name of the refrigerated case simulated. Echoes the field Name in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-12}
+
+The name of the zone where the refrigerated case is located. Echoes the field Zone Name in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field: Zone Node \#}\label{field-zone-node}
+
+The number of the zone node (connection to the air loop) where the refrigerated case is located. This is the number of the zone node as found in the \textbf{eplusout.bnd} file.
+
+\subsubsection{Field: Zone Node Name}\label{field-zone-node-name}
+
+The name of the zone node where the refrigerated case is located. The refrigerated case will impact the air heat balance in this zone.
+
+\subsubsection{Field: Capacity}\label{field-capacity}
+
+The total cooling capacity (W/m) of the refrigerated case. Echoes the field Rated Total Cooling Capacity per Unit Length in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field: LHR}\label{field-lhr}
+
+The design latent heat ratio (latent capacity divided by total cooling capacity) of the refrigerated case. Echoes the field Rated LHR in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field: Temperature \{C\}}\label{field-temperature-c}
+
+The average temperature (C) of the air and products within the refrigerated case. Echoes the field Case Operating Temperature in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field: Length \{m\}}\label{field-length-m}
+
+The length (m) of the refrigerated case. Echoes the field Case Length in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field: Fan \{W/m\}}\label{field-fan-wm}
+
+The total operating fan power (W/m) in the refrigerated case. Echoes the field Operating Case Fan Power per Unit Length in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field:Installed Lighting \{W/m\}}\label{fieldinstalled-lighting-wm}
+
+The total installed lighting power (W/m) in the refrigerated case. Echoes the field Installed Case Lighting Power per Unit Length in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field: Anti-Sweat \{W/m\}}\label{field-anti-sweat-wm}
+
+The electric anti-sweat heater power (W/m) in the refrigerated case. Echoes the field Case Anti-Sweat Heater Power per Unit Length in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field: Defrost \{W/m\}}\label{field-defrost-wm}
+
+The defrost power (W/m) in the refrigerated case. Echoes the field Case Defrost Power per Unit Length in object Refrigeration:Case from the IDF.
+
+\subsubsection{Header Record: Refrigeration Walk In Cooler}\label{header-record-refrigeration-walk-in-cooler}
+
+\subsubsection{Field: Walk In Number}\label{field-walk-in-number}
+
+The number of the refrigerated walk-in, assigned sequentially according to the order in which these objects are defined in the IDF.
+
+\subsubsection{Field: Walk In Name}\label{field-walk-in-name}
+
+The name of the refrigerated walk-in simulated. Echoes the field Name in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: Capacity}\label{field-capacity-1}
+
+The total cooling capacity (W) of the walk-in. Echoes the field Rated Coil Cooling Capacity in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: Temperature \{C\}}\label{field-temperature-c-1}
+
+The average temperature (C) of the air and products within the refrigerated case. Echoes the field Operating Temperature in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: Coil Fan \{W\}}\label{field-coil-fan-w}
+
+The coil fan power (W) in the walk-in . Echoes the field Cooling Coil Fan Power in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: Circulation Fan \{W\}}\label{field-circulation-fan-w}
+
+The circulation fan power (W) in the walk-in. Echoes the field Circulation Fan Power in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: Lighting \{W\}}\label{field-lighting-w}
+
+The total lighting power (W) in the walk-in. Echoes the field Total Lighting Power in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: Heaters \{W\}}\label{field-heaters-w}
+
+The total electric heater power (W) in the walk-in. Echoes the field Total Heating Power in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: Defrost \{W\}}\label{field-defrost-w}
+
+The defrost power (W) in the walk-in. Echoes the field Defrost Power in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: \# Zones}\label{field-zones}
+
+The number of zones that exchange energy with the walk-in. Counted according to the number of records in the Refrigeration:WalkIn object in the IDF..
+
+\subsubsection{Header Record: Walk-In Surfaces Facing Zone}\label{header-record-walk-in-surfaces-facing-zone}
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-13}
+
+The name of a zone adjacent to the walk-in. Echoes the field Zone Name in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: Wall/Ceiling Area \{m2\}}\label{field-wallceiling-area-m2}
+
+The insulated surface area facing this zone adjacent to the walk-in. Echoes the field Total Insulated Surface Area Facing this Zone in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: UValue \{W/m2-C{]}\}}\label{field-uvalue-wm2-c}
+
+The thermal conductance of the insulated surface area facing this zone adjacent to the walk-in. Echoes the field Insulated Surface UValue Facing this Zone in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: AreaStockDoors \{m2\}}\label{field-areastockdoors-m2}
+
+The total surface area of stock doors facing this zone adjacent to the walk-in. Echoes the field Area of Stocking Doors Facing this Zone in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: HeightStockDoors \{m\}}\label{field-heightstockdoors-m}
+
+The height of stock doors facing this zone adjacent to the walk-in. Echoes the field Height of Stocking Doors Facing this Zone in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: UValueStockDoors \{W/m2-C{]}\}}\label{field-uvaluestockdoors-wm2-c}
+
+The thermal conductance of the stock doors facing this zone adjacent to the walk-in. Echoes the field Stocking Door U Value Facing this Zone in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: AreaGlassDoors \{m2\}}\label{field-areaglassdoors-m2}
+
+The total surface area of glass doors facing this zone adjacent to the walk-in. Echoes the field Area of Glass Reach In Doors Facing this Zone in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: HeightGlassDoors \{m\}}\label{field-heightglassdoors-m}
+
+The height of glass doors facing this zone adjacent to the walk-in. Echoes the field Height of Glass Doors Facing this Zone in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Field: UValueGlassDoors \{W/m2-C{]}\}}\label{field-uvalueglassdoors-wm2-c}
+
+The thermal conductance of the glass doors facing this zone adjacent to the walk-in. Echoes the field Glass Reach In Door U Value Facing this Zone in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Header Record: \#Detailed Refrigeration Systems}\label{header-record-detailed-refrigeration-systems}
+
+\subsubsection{Field: Number of Detailed Refrigeration Systems}\label{field-number-of-detailed-refrigeration-systems}
+
+The total number of detailed refrigeration systems found in the IDF.
+
+\subsubsection{Header Record:~ Detailed Refrigeration System}\label{header-record-detailed-refrigeration-system}
+
+\subsubsection{Field: Refrigeration System Name}\label{field-refrigeration-system-name}
+
+The name of the Refrigeration System simulated. Echoes the field Name in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: Refrigerant Used}\label{field-refrigerant-used}
+
+The name of the refrigerant used in the system. Echoes the field Working Fluid ID in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: \# Refrigerated Cases Connected}\label{field-refrigerated-cases-connected-1}
+
+The total number of refrigerated cases connected to the refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: \# WalkInCoolers~ Connected}\label{field-walkincoolers-connected-1}
+
+The total number of walk-ins connected to the refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: \# Secondary Loops Served}\label{field-secondary-loops-served}
+
+The total number of secondary loops connected to the refrigeration system. These are assigned to the refrigeration system through the field Refrigeration Transfer Load or TransferLoad List Name in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: \# Cascade Condensers Served}\label{field-cascade-condensers-served}
+
+The total number of cascade condensers cooled by the refrigeration system. These are assigned to the refrigeration system through the field Refrigeration Transfer Load or TransferLoad List Name in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: \# Mechanical Subcoolers Served}\label{field-mechanical-subcoolers-served}
+
+The total number of mechanical subcoolers cooled by the refrigeration system. These are assigned to the refrigeration system through the field Capacity-Providing System in object Refrigeration:Subcooler from the IDF.
+
+\subsubsection{Field: \# Compressors Connected}\label{field-compressors-connected}
+
+The total number of compressors connected to the refrigeration system. These are assigned to the refrigeration system through the field Compressor Name or CompressorList Name in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: \# Compression Stages}\label{field-compression-stages}
+
+The number of compressor stages for the refrigeration system. The value is either ``1'' for single-stage compression systems or ``2'' for two-stage compression systems.
+
+\subsubsection{Field: Intercooler Type}\label{field-intercooler-type}
+
+The intercooler type (either ``1'' for Flash Intercooler or ``2'' for Shell-and-Coil Intercooler) for two-stage compression systems.~ A value of ``0'' indicates no intercooler (single-stage compression systems only).
+
+\subsubsection{Field: Intercooler Effectiveness}\label{field-intercooler-effectiveness}
+
+The intercooler effectiveness for the shell-and-coil intercooler.
+
+\subsubsection{Field: \# Subcoolers Connected}\label{field-subcoolers-connected}
+
+The total number of subcoolers, both liquid suction and mechanical, that provide cooling to the refrigeration system. These are assigned to the refrigeration system through the fields Mechanical Subcooler Name and Liquid Suction Heat Exchanger Subcooler Name in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: Minimum Condensing Temperature (C)}\label{field-minimum-condensing-temperature-c}
+
+The minimum condensing temperature allowed for the refrigeration system. Echoes the field Minimum Condensing Temperature in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Header Record: \#Detailed Transcritical Refrigeration Systems}\label{header-record-detailed-transcritical-refrigeration-systems}
+
+\subsubsection{Field: Number of Detailed Transcritical Refrigeration Systems}\label{field-number-of-detailed-transcritical-refrigeration-systems}
+
+The total number of detailed transcritical CO\(_{2}\) refrigeration systems found in the IDF.
+
+\subsubsection{Header Record:~ Detailed Transcritical Refrigeration System}\label{header-record-detailed-transcritical-refrigeration-system}
+
+\subsubsection{Field: Transcritical Refrigeration System Name}\label{field-transcritical-refrigeration-system-name}
+
+The name of the Transcritical Refrigeration System simulated. Echoes the field Name in object Refrigeration:TranscriticalSystem from the IDF.
+
+\subsubsection{Field: Refrigerant Used}\label{field-refrigerant-used-1}
+
+The name of the refrigerant used in the transcritical refrigeration system. Echoes the field Working Fluid ID in object Refrigeration:TranscriticalSystem from the IDF.
+
+\subsubsection{Field: \# Medium Temperature Refrigerated Cases Connected}\label{field-medium-temperature-refrigerated-cases-connected}
+
+The total number of medium temperature refrigerated cases connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:TranscriticalSystem from the IDF.
+
+\subsubsection{Field: \# Low Temperature Refrigerated Cases Connected}\label{field-low-temperature-refrigerated-cases-connected}
+
+The total number of low temperature refrigerated cases connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:TranscriticalSystem from the IDF.
+
+\subsubsection{Field: \# Medium Temperature WalkInCoolers~ Connected}\label{field-medium-temperature-walkincoolers-connected}
+
+The total number of medium temperature walk-ins connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:TranscriticalSystem from the IDF.
+
+\subsubsection{Field: \# Low Temperature WalkInCoolers~ Connected}\label{field-low-temperature-walkincoolers-connected}
+
+The total number of low temperature walk-ins connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:TranscriticalSystem from the IDF.
+
+\subsubsection{Field: \# High Pressure Compressors Connected}\label{field-high-pressure-compressors-connected}
+
+The total number of high pressure compressors connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Compressor Name or CompressorList Name in object Refrigeration:TranscriticalSystem from the IDF.
+
+\subsubsection{Field: \# Low Pressure Compressors Connected}\label{field-low-pressure-compressors-connected}
+
+The total number of low pressure compressors connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Compressor Name or CompressorList Name in object Refrigeration:TranscriticalSystem from the IDF.
+
+\subsubsection{Field: Minimum Condensing Temperature (C)}\label{field-minimum-condensing-temperature-c-1}
+
+The minimum condensing temperature allowed during subcritical operation for the transcritical refrigeration system. Echoes the field Minimum Condensing Temperature in object Refrigeration:GasCooler:AirCooled from the IDF.
+
+\subsubsection{Header Record: Cascade Load}\label{header-record-cascade-load}
+
+\subsubsection{Field: System Name Connected}\label{field-system-name-connected}
+
+The name of another detailed system that rejects heat to a cascade condenser cooled by this detailed system. These are assigned to the refrigeration system, via the name of the cascade condenser, through the field Refrigeration Transfer Load or TransferLoad List Name in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: Condenser Number}\label{field-condenser-number}
+
+The number of the cascade condenser cooled by this detailed system, assigned sequentially according to the order in which these objects are defined in the IDF.
+
+\subsubsection{Field: Condenser Name}\label{field-condenser-name}
+
+The name of a cascade condenser cooled by this detailed system. These are assigned to the refrigeration system, via the name of the cascade condenser, through the field Refrigeration Transfer Load or TransferLoad List Name in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Condenser:Cascade
+
+\subsubsection{Header Record: Secondary Load}\label{header-record-secondary-load}
+
+\subsubsection{Field: Secondary System Served Name}\label{field-secondary-system-served-name}
+
+The name of the secondary system cooled by this detailed system. These are assigned to the refrigeration system through the field Refrigeration Transfer Load or TransferLoad List Name in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:SecondarySystem.
+
+\subsubsection{Field: Secondary Number}\label{field-secondary-number}
+
+The number of the secondary system cooled by this detailed system, assigned sequentially according to the order in which these objects are defined in the IDF.
+
+\subsubsection{Header Record: Mechanical Subcooler Load}\label{header-record-mechanical-subcooler-load}
+
+\subsubsection{Field: Subcooler Number}\label{field-subcooler-number}
+
+The number of the mechanical subcooler cooled by this detailed system, assigned sequentially according to the order in which these objects are defined in the IDF.
+
+\subsubsection{Field: Subcooler Name}\label{field-subcooler-name}
+
+The name of the secondary system cooled by this detailed system. These are assigned to the refrigeration system through the field Capacity-Providing System in object Refrigeration:Subcooler from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Subcooler.
+
+\subsubsection{Header Record:~ Refrigeration Compressor}\label{header-record-refrigeration-compressor}
+
+\subsubsection{Field: Compressor Number}\label{field-compressor-number}
+
+The number of the refrigeration compressor, assigned sequentially according to the order in which these objects are defined in the IDF.
+
+\subsubsection{Field: Compressor Name}\label{field-compressor-name}
+
+The name of the compressor simulated. Echoes the field Name of Compressor in object List:Refrigeration:Compressors from the IDF.
+
+\subsubsection{Field: Nominal Capacity, W}\label{field-nominal-capacity-w}
+
+The nominal capacity of the compressor based on the capacity curve (identified by the field Unique Name of Capacity Curve in the object Refrigeration:Compressor in the IDF) evaluated at the lowest design evaporating temperature of all the cases attached to the system and at the design condensing temperature of the condenser attached to the system.
+
+\subsubsection{Header Record:~ Refrigeration Condenser, Air-Cooled}\label{header-record-refrigeration-condenser-air-cooled}
+
+\subsubsection{Field: Condenser~ Number}\label{field-condenser-number-1}
+
+The number of the refrigeration condenser, assigned sequentially according to the order in which all the Refrigeration:Condenser:*~ objects are defined in the IDF.
+
+\subsubsection{Field: Condenser Name}\label{field-condenser-name-1}
+
+The name of the condenser simulated. Echoes the field Name of Condenser for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Condenser:Aircooled.
+
+\subsubsection{Field: Rated Condensing Temperature, C}\label{field-rated-condensing-temperature-c}
+
+The rated condensing temperature of the condenser, set by standard ARI 460 for air-cooled condensers.
+
+\subsubsection{Field: Rated Capacity, W}\label{field-rated-capacity-w}
+
+The rated capacity of the condenser. This value is taken from the capacity curve (identified by the field Name of Condenser Heat of Rejection Curve, Linear, in the object Refrigeration:Condenser:AirCooled in the IDF) evaluated at the temperature difference specified in standard ARI 460.
+
+\subsubsection{Field: Rated Fan Power, W}\label{field-rated-fan-power-w}
+
+The rated fan power of the condenser. Echoes the field Rated Fan Power in object Refrigeration:Condenser:AirCooled from the IDF.
+
+\subsubsection{Header Record:~ Refrigeration Condenser, Water-Cooled}\label{header-record-refrigeration-condenser-water-cooled}
+
+\subsubsection{Field: Condenser~ Number}\label{field-condenser-number-2}
+
+The number of the refrigeration condenser, assigned sequentially according to the order in which all the Refrigeration: Condenser:* objects are defined in the IDF.
+
+\subsubsection{Field: Condenser Name}\label{field-condenser-name-2}
+
+The name of the condenser simulated. Echoes the field Name of Condenser for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Condenser:WaterCooled.
+
+\subsubsection{Field: Rated Condensing Temperature, C}\label{field-rated-condensing-temperature-c-1}
+
+The rated condensing temperature of the condenser, echos the field Rated Condensing Temperature in the object Refrigeration:Condenser:WaterCooled.
+
+\subsubsection{Field: Rated Capacity, W}\label{field-rated-capacity-w-1}
+
+The rated capacity of the condenser. Echos the field Rated Total Heat Rejection Effect in the object Refrigeration:Condenser:WaterCooled in the IDF.
+
+\subsubsection{Field: Rated Water Inlet Temperature, C}\label{field-rated-water-inlet-temperature-c}
+
+The rated water inlet temperature of the condenser. Echos the field Rated Water Inlet Temperature in the object Refrigeration:Condenser:WaterCooled in the IDF.
+
+\subsubsection{Field: Rated Water Flow Rate, m3/s}\label{field-rated-water-flow-rate-m3s}
+
+The rated water flow rate of the condenser. Echos the field Water Design Flow Rate in the object Refrigeration:Condenser:WaterCooled in the IDF.
+
+\subsubsection{Header Record:~ Refrigeration Condenser, Evaporative-Cooled}\label{header-record-refrigeration-condenser-evaporative-cooled}
+
+\subsubsection{Field: Condenser~ Number}\label{field-condenser-number-3}
+
+The number of the refrigeration condenser, assigned sequentially according to the order in which all the Refrigeration: Condenser:* objects are defined in the IDF.
+
+\subsubsection{Field: Condenser Name}\label{field-condenser-name-3}
+
+The name of the condenser simulated. Echoes the field Name of Condenser for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Condenser: EvaporativeCooled.
+
+\subsubsection{Field: Rated Capacity, W}\label{field-rated-capacity-w-2}
+
+The rated capacity of the condenser. Echos the field Rated Total Heat Rejection Effect in the object Refrigeration:Condenser:EvaporativeCooled in the IDF.
+
+\subsubsection{Field: Rated Fan Power, W}\label{field-rated-fan-power-w-1}
+
+The rated fan power of the condenser. Echoes the field Rated Fan Power in object~ Refrigeration:Condenser: EvaporativeCooled in the IDF.
+
+\subsubsection{Header Record:~ Refrigeration Condenser, Cascade}\label{header-record-refrigeration-condenser-cascade}
+
+\subsubsection{Field: Condenser~ Number}\label{field-condenser-number-4}
+
+The number of the refrigeration condenser, assigned sequentially according to the order in which all the Refrigeration: Condenser *~ objects are defined in the IDF.
+
+\subsubsection{Field: Condenser Name}\label{field-condenser-name-4}
+
+The name of the condenser simulated. Echoes the field Name of Condenser for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Condenser:Cascade.
+
+\subsubsection{Field: Condensing Temperature Control Type,}\label{field-condensing-temperature-control-type}
+
+Echoes the field Condensing Temperature Control Type in object Refrigeration:Condenser:Cascade.
+
+\subsubsection{Field: Rated Condensing Temperature, C}\label{field-rated-condensing-temperature-c-2}
+
+The rated condensing temperature of the condenser, echoes the field Rated Condensing Temperature in object Refrigeration:Condenser:Cascade.
+
+\subsubsection{Field: Rated Capacity, W}\label{field-rated-capacity-w-3}
+
+The rated capacity of the condenser, echoes the field Rated Effective Total Heat Rejection Rate in object Refrigeration:Condenser:Cascade.
+
+\subsubsection{Field: Approach Temperature Difference, DeltaC}\label{field-approach-temperature-difference-deltac}
+
+The approach temperature difference of the condenser, echoes the field Rated Approach Temperature Difference in object Refrigeration:Condenser:Cascade from the IDF.
+
+\subsubsection{Header Record:~ Refrigeration GasCooler:Air-Cooled}\label{header-record-refrigeration-gascoolerair-cooled}
+
+\subsubsection{Field: Gas Cooler Number}\label{field-gas-cooler-number}
+
+The number of the refrigeration gas cooler, assigned sequentially according to the order in which all the Refrigeration:GasCooler objects are defined in the IDF.
+
+\subsubsection{Field: Gas Cooler Name}\label{field-gas-cooler-name}
+
+The name of the gas cooler simulated. Echoes the field Refrigeration Gas Cooler Name in object Refrigeration:TranscriticalSystem from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:GasCooler:Aircooled.
+
+\subsubsection{Field: Rated Outlet Pressure, Pa}\label{field-rated-outlet-pressure-pa}
+
+The rated gas cooler pressure corresponding to the rated capacity.
+
+\subsubsection{Field: Rated Outlet Temperature, C}\label{field-rated-outlet-temperature-c}
+
+The rated gas cooler outlet temperature corresponding to the rated capacity.
+
+\subsubsection{Field: Rated Approach Temperature, C}\label{field-rated-approach-temperature-c}
+
+The rated gas cooler approach temperature corresponding to the rated capacity.
+
+\subsubsection{Field: Rated Capacity, W}\label{field-rated-capacity-w-4}
+
+The rated capacity of the gas cooler. This value is taken from the capacity curve (identified by the field Rated Total Heat Rejection Rate Curve Name, in the object Refrigeration:GasCoooler:AirCooled in the IDF) evaluated at the rated approach temperature.
+
+\subsubsection{Field: Rated Fan Power, W}\label{field-rated-fan-power-w-2}
+
+The rated fan power of the gas cooler. Echoes the field Rated Fan Power in object Refrigeration:GasCooler:AirCooled from the IDF.
+
+\subsubsection{Header Record: Refrigeration~ Mechanical Subcooler}\label{header-record-refrigeration-mechanical-subcooler}
+
+\subsubsection{Field: Subcooler Number}\label{field-subcooler-number-1}
+
+The number of the mechanical subcooler, assigned sequentially according to the order in which all the Refrigeration:Subcooler~ objects are defined in the IDF.
+
+\subsubsection{Field: Subcooler Name}\label{field-subcooler-name-1}
+
+The name of the subcooler simulated. Echoes the field Mechanical Subcooler Name for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Subcooler.
+
+\subsubsection{Field: Name of System Providing Cooling}\label{field-name-of-system-providing-cooling}
+
+The name of the detailed system that absorbs heat from the subcooler. These are assigned to the subcooer through the field Capacity-Providing System in object Refrigeration:Subcooler from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:System.
+
+\subsubsection{Field: Design Outlet Temperature, C}\label{field-design-outlet-temperature-c}
+
+The controlled outlet temperature of the subcooler, echoes the field Outlet Control Temperature in object Refrigeration: Subcooler.
+
+\subsubsection{Header Record:~ Refrigeration Liquid Suction Subcooler}\label{header-record-refrigeration-liquid-suction-subcooler}
+
+\subsubsection{Field: Subcooler Number}\label{field-subcooler-number-2}
+
+The number of the liquid suction subcooler, assigned sequentially according to the order in which all the Refrigeration:Subcooler~ objects are defined in the IDF.
+
+\subsubsection{Field: Subcooler Name}\label{field-subcooler-name-2}
+
+The name of the subcooler simulated. Echoes the field Liquid Suction Heat Exchanger Subcooler Name for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Subcooler.
+
+\subsubsection{Field: Design Subcooling, deltaC}\label{field-design-subcooling-deltac}
+
+The design change in temperature of the warm fluid within the liquid suction subcooler, echoes the field Liquid Suction Design Subcooling Temperature in object Refrigeration: Subcooler.
+
+\subsubsection{Field: Design liquid inlet temperature, C}\label{field-design-liquid-inlet-temperature-c}
+
+The design warm liquid inlet temperature of the liquid suction subcooler, echoes the field Design Liquid Inlet Temperature in object Refrigeration: Subcooler.
+
+\subsubsection{Field: Design vapor inlet temperature, C}\label{field-design-vapor-inlet-temperature-c}
+
+The design cold vapor inlet temperature of the liquid suction subcooler, echoes the field Design Vapor Inlet Temperature in object Refrigeration: Subcooler.
+
+\subsubsection{Header Record: \# Secondary Refrigeration Systems}\label{header-record-secondary-refrigeration-systems}
+
+\subsubsection{Field: Number of Secondary Refrigeration Systems}\label{field-number-of-secondary-refrigeration-systems}
+
+The total number of secondary refrigeration systems found in the IDF.
+
+\subsubsection{Header Record:~ Secondary Refrigeration System: Fluid Always Liquid}\label{header-record-secondary-refrigeration-system-fluid-always-liquid}
+
+\subsubsection{Field: Secondary Number}\label{field-secondary-number-1}
+
+The number of the secondary refrigeration system, assigned sequentially according to the order in which all the Refrigeration:SecondarySystem~ objects are defined in the IDF.
+
+\subsubsection{Field: Secondary Name}\label{field-secondary-name}
+
+The name of the secondary refrigeration system simulated. Echoes the field Name in object Refrigeration:SecondarySystem from the IDF.
+
+\subsubsection{Field: \# Refrigerated Cases Connected}\label{field-refrigerated-cases-connected-2}
+
+The total number of refrigerated cases connected to the secondary refrigeration system. These are assigned to the secondary refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:SecondarySystem from the IDF.
+
+\subsubsection{Field: \# WalkInCoolers~ Connected}\label{field-walkincoolers-connected-2}
+
+The total number of walk-ins connected to the secondary refrigeration system. These are assigned to the secondary refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: Fluid Name}\label{field-fluid-name}
+
+The name of the circulating fluid used in the system. Echoes the field Circulating Fluid Name in object Refrigeration:SecondarySystem from the IDF.
+
+\subsubsection{Field: Capacity, W}\label{field-capacity-w}
+
+The rated capacity of the evaporator, echoes the field Evaporator Design Capacity In Watts in object Refrigeration:SecondarySystem.
+
+\subsubsection{Field: Evap Temperature in Secondary Evaporator, C}\label{field-evap-temperature-in-secondary-evaporator-c}
+
+The rated evaporating temperature of the heat exchanger, echoes the field Design Evaporating Temperature in object Refrigeration:SecondarySystem.
+
+\subsubsection{Field: Approach Temperature Difference, DeltaC}\label{field-approach-temperature-difference-deltac-1}
+
+The approach temperature difference of the heat exchanger, echoes the field Design Approach Temperature Difference in object Refrigeration:SecondarySystem from the IDF.
+
+\subsubsection{Field: Temperature Range, DeltaC}\label{field-temperature-range-deltac}
+
+The temperature range of the heat exchanger, echoes the field Design Range Temperature Difference in object Refrigeration:SecondarySystem from the IDF.
+
+\subsubsection{Field: TotalPumpPower, W}\label{field-totalpumppower-w}
+
+The rated total pump power of the secondary loop, echoes the field Design Total Pump Power in object Refrigeration:SecondarySystem.
+
+\subsubsection{Header Record:~ Secondary Refrigeration System: Liquid Overfeed}\label{header-record-secondary-refrigeration-system-liquid-overfeed}
+
+\subsubsection{Field: Secondary Number}\label{field-secondary-number-2}
+
+The number of the secondary refrigeration system, assigned sequentially according to the order in which all the Refrigeration:SecondarySystem~ objects are defined in the IDF.
+
+\subsubsection{Field: Secondary Name}\label{field-secondary-name-1}
+
+The name of the secondary refrigeration system simulated. Echoes the field Name in object Refrigeration:SecondarySystem from the IDF.
+
+\subsubsection{Field: \# Refrigerated Cases Connected}\label{field-refrigerated-cases-connected-3}
+
+The total number of refrigerated cases connected to the secondary refrigeration system. These are assigned to the secondary refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:SecondarySystem from the IDF.
+
+\subsubsection{Field: \# WalkInCoolers~ Connected}\label{field-walkincoolers-connected-3}
+
+The total number of walk-ins connected to the secondary refrigeration system. These are assigned to the secondary refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:System from the IDF.
+
+\subsubsection{Field: Fluid Name}\label{field-fluid-name-1}
+
+The name of the circulating fluid used in the system. Echoes the field Circulating Fluid Name in object Refrigeration:SecondarySystem from the IDF.
+
+\subsubsection{Field: Capacity, W}\label{field-capacity-w-1}
+
+The rated capacity of the evaporator, echoes the field Evaporator Design Capacity In Watts in object Refrigeration:SecondarySystem.
+
+\subsubsection{Field: Evap Temperature in Secondary Evaporator, C}\label{field-evap-temperature-in-secondary-evaporator-c-1}
+
+The rated evaporating temperature of the heat exchanger, echoes the field Design Evaporating Temperature in object Refrigeration:SecondarySystem.
+
+\subsubsection{Field: Approach Temperature Difference, DeltaC}\label{field-approach-temperature-difference-deltac-2}
+
+The approach temperature difference of the heat exchanger, echoes the field Design Approach Temperature Difference in object Refrigeration:SecondarySystem from the IDF.
+
+\subsubsection{Field: Circulating Rate}\label{field-circulating-rate}
+
+The ratio of the mass flow rate of refrigerant at the pump to the mass flow rate of refrigerant vapor leaving the refrigeration load(s), echoes the field PhaseChange Circulating Rate in object Refrigeration:SecondarySystem from the IDF.
+
+\subsubsection{Field: TotalPumpPower, W}\label{field-totalpumppower-w-1}
+
+The rated total pump power of the secondary loop, echoes the field Design Total Pump Power in object Refrigeration:SecondarySystem.
+
+\subsubsection{Header Record: \#Orphaned Refrigerated Cases}\label{header-record-orphaned-refrigerated-cases}
+
+\subsubsection{Field: Number of Orphaned Refrigerated Cases}\label{field-number-of-orphaned-refrigerated-cases}
+
+The total number of orphaned refrigerated cases found in the IDF.
+
+\subsubsection{Field: Message}\label{field-message}
+
+A message stating ``NOTE: These cases were not simulated\ldots{}''.
+
+\subsubsection{Header Record: Orphaned Refrigerated Case}\label{header-record-orphaned-refrigerated-case}
+
+\subsubsection{Field: Refrigerated Case Number}\label{field-refrigerated-case-number}
+
+The number of the orphaned refrigerated case found in the IDF. The refrigerated case numbers are assigned sequentially according to the order in which these objects are defined in the IDF.
+
+\subsubsection{Field: Refrigerated Case Name}\label{field-refrigerated-case-name}
+
+The name of the orphaned refrigerated case which is \textbf{not} connected to a compressor rack or detailed refrigeration system. Echoes the field Name in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-14}
+
+The name of the zone where the refrigerated case is located. Echoes the field Zone Name in object Refrigeration:Case from the IDF.
+
+\subsubsection{Field: Zone Node \#}\label{field-zone-node-1}
+
+The number of the zone node (connection to the air loop) where the refrigerated case is located. This is the number of the zone node as found in the \textbf{eplusout.bnd} file.
+
+\subsubsection{Field: Zone Node Name}\label{field-zone-node-name-1}
+
+The name of the zone node where the orphaned refrigerated case is located. This orphaned refrigerated case will \textbf{not} impact the air heat balance in this zone.
+
+\subsubsection{Header Record: \#Orphaned Walk Ins}\label{header-record-orphaned-walk-ins}
+
+\subsubsection{Field: Number of OrphanedWalk Ins}\label{field-number-of-orphanedwalk-ins}
+
+The total number of orphaned Walk Ins found in the IDF.
+
+\subsubsection{Field: Message}\label{field-message-1}
+
+A message stating ``NOTE: These Walk Ins were not simulated\ldots{}''.
+
+\subsubsection{Header Record: Orphaned Walk In}\label{header-record-orphaned-walk-in}
+
+\subsubsection{Field:Walk In Number}\label{fieldwalk-in-number}
+
+The number of the orphaned Walk In found in the IDF. The Walk In numbers are assigned sequentially according to the order in which these objects are defined in the IDF.
+
+\subsubsection{Field: Walk In Name}\label{field-walk-in-name-1}
+
+The name of the orphaned Walk In which is \textbf{not} connected to a compressor rack or refrigeration system. Echoes the field Name in object Refrigeration:WalkIn from the IDF.
+
+\subsubsection{Header Record: \#Orphaned Refrigeration Compressors}\label{header-record-orphaned-refrigeration-compressors}
+
+\subsubsection{Field: Number of Orphaned Refrigeration Compressors}\label{field-number-of-orphaned-refrigeration-compressors}
+
+The total number of orphaned Refrigeration Compressors found in the IDF.
+
+\subsubsection{Field: Message}\label{field-message-2}
+
+A message stating ``NOTE: These Compressors were not simulated\ldots{}''.
+
+\subsubsection{Header Record: Orphaned Refrigeration Compressor}\label{header-record-orphaned-refrigeration-compressor}
+
+\subsubsection{Field:Compressor ~Number}\label{fieldcompressor-number}
+
+The number of the orphaned Compressor found in the IDF. The Compressor numbers are assigned sequentially according to the order in which these objects are defined in the IDF.
+
+\subsubsection{Field: Compressor Name}\label{field-compressor-name-1}
+
+The name of the orphaned Compressor which is \textbf{not} connected to a detailed refrigeration system. Echoes the field Name in object Refrigeration:Compressor from the IDF.
+
+\subsubsection{Header Record: \#Orphaned Refrigeration Secondary Loops}\label{header-record-orphaned-refrigeration-secondary-loops}
+
+\subsubsection{Field: Number of Orphaned Secondary Loops}\label{field-number-of-orphaned-secondary-loops}
+
+The total number of orphaned Secondary Loops found in the IDF.
+
+\subsubsection{Field: Message}\label{field-message-3}
+
+A message stating ``NOTE: These Secondary Loops were not simulated\ldots{}''.
+
+\subsubsection{Header Record: Orphaned Refrigeration Secondary Loop}\label{header-record-orphaned-refrigeration-secondary-loop}
+
+\subsubsection{Field:Secondary ~Number}\label{fieldsecondary-number}
+
+The number of the orphaned Secondary System found in the IDF. The Secondary System numbers are assigned sequentially according to the order in which these objects are defined in the IDF.
+
+\subsubsection{Field: Secondary Name}\label{field-secondary-name-2}
+
+The name of the orphaned Secondary which is not connected to a detailed refrigeration system. Echoes the field Name in object Refrigeration:SecondarySystem from the IDF.
+
+\subsection{View Factor Info}\label{view-factor-info}
+
+A semi-debugging, informational report on View Factors for each zone/surface is available when you add \textbf{Output:Diagnostics,DisplayAdvancedVariables;} to your input file.
+
+After EnergyPlus receives the geometry information for the building, it calculates the view factors and grey interchange information for each zone and surface. These are used to calculate the interior radiant exchange between surfaces. The first set is called the approximate view factors; then, a deeper evaluation of the zone's geometry and surfaces is performed to see if corrections need to be applied. Three sets of values are provided for the user's information.
+
+! \textless{}Surface View Factor Check Values\textgreater{},ZoneName,Original Check Value,Calculated Fixed Check Value,Final Check Value
+
+Surface View Factor Check Values,ZONE ONE,8.881784E-016,8.637788E-004,8.881784E-016
+
+\subsubsection{Field: Zone Name}\label{field-zone-name-15}
+
+This is the zone name for the values.
+
+\subsubsection{Field: Original Check Value}\label{field-original-check-value}
+
+Original check value as submitted to the ``Test and Check'' routine. This value represents the Sum of the N (number of surfaces) by N matrix -- the Number of Surfaces. Ideally, it should be very close to zero. The original check value could come from either the User inputting the view factors for the zone or the approximate view factor calculation in EnergyPlus.
+
+\subsubsection{Field: Calculated Fixed Check Value}\label{field-calculated-fixed-check-value}
+
+This is the value of the view factor matrix (i.e.~SUM(NXNmatrix -- N) after the fix routine has applied them.
+
+\subsubsection{Field: Final Check Value}\label{field-final-check-value}
+
+This value should match one of the previous values and indicate whether the original matrix or the modfied/fixed matrix will be used in the calculations.
+
+\subsection{View Factor Details}\label{view-factor-details}
+
+View factors for zones (surfaces) can be entered into the input file (object: ZoneProperty:UserViewFactors) if desired. Or they can be reported from the input file. The following describes the reporting of these view factors. You can report the surface view factor information by using:
+
+Output:Surfaces:List,ViewFactorInfo;
+
+This triggers EnergyPlus to produce a special output section in the file eplusout.eio. This file, which is csv format, can be opened in Excel, and will show detailed information about the surfaces in all the zones.
+
+In order to get user view factors ready for inclusion in an input file, several steps much be taken. \emph{First, because EnergyPlus has a data structure for zones that only is defined at initialization, it is necessary to use EnergyPlus to determine the surface numbers (i,j) before a UserViewFactors object can be constructed.} (This is a known defect -- a new object is being defined that will make this unnecessary). THIS STILL NEEDS TO BE REVISED BASE ON IF WE GO FOR NEW INPUT OR NOT.
+
+! \textless{}Surface View Factor and Grey Interchange Information\textgreater{}
+
+! \textless{}View Factor - Zone Information\textgreater{},Zone Name,Number of Surfaces
+
+! \textless{}View Factor - Surface Information\textgreater{},Surface Name,Surface Class,Area \{m2\},Azimuth,Tilt,Thermal Emissivity,\#Sides,Vertices
+
+! \textless{}View Factor / Grey Interchange Type\textgreater{},Surface Name(s)
+
+! \textless{}View Factor\textgreater{},Surface Name,Surface Class,Row Sum,View Factors for each Surface
+
+Surface View Factor - Zone Information,ZONE ONE,6
+
+Surface View Factor - Surface Information, ZN001:WALL001,Wall,69.6773,180.0000,90.0000,0.9000,4, 0.0000,0.0000,4.5720,0.0000,0.0000,0.0000,15.2400,0.0000,0.0000,15.2400,0.0000,4.5720,
+
+Surface View Factor - Surface Information,ZN001:WALL002,Wall,69.6773,90.0000,90.0000,0.9000,4, 15.2400,0.0000,4.5720,15.2400,0.0000,0.0000,15.2400,15.2400,0.0000,15.2400,15.2400,4.5720,
+
+Surface View Factor - Surface Information,ZN001:WALL003,Wall,69.6773,0.0000,90.0000,0.9000,4, 15.2400,15.2400,4.5720,15.2400,15.2400,0.0000,0.0000,15.2400,0.0000,0.0000,15.2400,4.5720,
+
+Surface View Factor - Surface Information,ZN001:WALL004,Wall,69.6773,270.0000,90.0000,0.9000,4, 0.0000,15.2400,4.5720,0.0000,15.2400,0.0000,0.0000,0.0000,0.0000,0.0000,0.0000,4.5720,
+
+Surface View Factor - Surface Information,ZN001:FLR001,Floor,232.2576,90.0000,180.0000,0.9000,4, 15.2400,0.0000,0.0000,0.0000,0.0000,0.0000,0.0000,15.2400,0.0000,15.2400,15.2400,0.0000,
+
+Surface View Factor - Surface Information,ZN001:ROOF001,Roof,232.2576,180.0000,0.0000,0.9000,4, 0.0000,15.2400,4.5720,0.0000,0.0000,4.5720,15.2400,0.0000,4.5720,15.2400,15.2400,4.5720,
+
+Approximate or User Input ViewFactors,To Surface,Surface Class,RowSum,ZN001:WALL001,ZN001:WALL002,ZN001:WALL003,ZN001:WALL004,ZN001:FLR001,ZN001:ROOF001,
+
+View Factor,ZN001:WALL001,Wall,1.0000,0.0000,0.1034,0.1034,0.1034,0.3448,0.3448,
+
+View Factor,ZN001:WALL002,Wall,1.0000,0.1034,0.0000,0.1034,0.1034,0.3448,0.3448,
+
+View Factor,ZN001:WALL003,Wall,1.0000,0.1034,0.1034,0.0000,0.1034,0.3448,0.3448,
+
+View Factor,ZN001:WALL004,Wall,1.0000,0.1034,0.1034,0.1034,0.0000,0.3448,0.3448,
+
+View Factor,ZN001:FLR001,Floor,1.0000,0.1364,0.1364,0.1364,0.1364,0.0000,0.4545,
+
+View Factor,ZN001:ROOF001,Roof,1.0000,0.1364,0.1364,0.1364,0.1364,0.4545,0.0000,
+
+Final ViewFactors,To Surface,Surface Class,RowSum,ZN001:WALL001,ZN001:WALL002,ZN001:WALL003,ZN001:WALL004,ZN001:FLR001,ZN001:ROOF001,
+
+View Factor,ZN001:WALL001,Wall,1.0000,0.0000,0.1034,0.1034,0.1034,0.3448,0.3448,
+
+View Factor,ZN001:WALL002,Wall,1.0000,0.1034,0.0000,0.1034,0.1034,0.3448,0.3448,
+
+View Factor,ZN001:WALL003,Wall,1.0000,0.1034,0.1034,0.0000,0.1034,0.3448,0.3448,
+
+View Factor,ZN001:WALL004,Wall,1.0000,0.1034,0.1034,0.1034,0.0000,0.3448,0.3448,
+
+View Factor,ZN001:FLR001,Floor,1.0000,0.1364,0.1364,0.1364,0.1364,0.0000,0.4545,
+
+View Factor,ZN001:ROOF001,Roof,1.0000,0.1364,0.1364,0.1364,0.1364,0.4545,0.0000,
+
+Script F Factors,X Surface,ZN001:WALL001,ZN001:WALL002,ZN001:WALL003,ZN001:WALL004,ZN001:FLR001,ZN001:ROOF001,
+
+Script F Factor,ZN001:WALL001,1.1191E-002,9.4126E-002,9.4126E-002,9.4126E-002,0.3032,0.3032,
+
+Script F Factor,ZN001:WALL002,9.4126E-002,1.1191E-002,9.4126E-002,9.4126E-002,0.3032,0.3032,
+
+Script F Factor,ZN001:WALL003,9.4126E-002,9.4126E-002,1.1191E-002,9.4126E-002,0.3032,0.3032,
+
+Script F Factor,ZN001:WALL004,9.4126E-002,9.4126E-002,9.4126E-002,1.1191E-002,0.3032,0.3032,
+
+Script F Factor,ZN001:FLR001,0.1199,0.1199,0.1199,0.1199,3.4097E-002,0.3863,
+
+Script F Factor,ZN001:ROOF001,0.1199,0.1199,0.1199,0.1199,0.3863,3.4097E-002,
+
+\subsubsection{Surface View Factor -- Zone Information}\label{surface-view-factor-zone-information}
+
+This line provides the zone name and the number of surfaces (heat transfer) in the zone. This information may be redundant with other reports in the eio file. It is included here to assist users who wish to use the auxiliary view factor program to generate view factors.
+
+\subsubsection{Surface View Factor -- Surface Information}\label{surface-view-factor-surface-information}
+
+These lines provide the surface information for each surface in the zone. This includes the name, class, area, azimuth (outward facing normal angle), the tilt angle, the thermal emissivity, the number of sides to the surface and the vertices.~ Again, this information may be redundant with other reports in the eio file. It is included here to assist users who wish to use the auxiliary view factor program to generate view factors.
+
+\subsubsection{Approximate or User Input View Factors}\label{approximate-or-user-input-view-factors}
+
+This section/lines provide the original view factors after either user input or approximate calculation. Surface name and class information are given again as well as each row sum (these should sum to 1, ideally) and then the view factors to other surfaces shown in columnar order.
+
+\subsubsection{Final View Factors}\label{final-view-factors}
+
+This section/lines shows view factors after they have been corrected for reciprocity and completeness. Correction may be necessary to make sure any two surfaces exchange radiation reciprocally, that is, the radiation leaving one surface directed at another surface is the same as the amount of radiation arriving at the other surface, and that the sum of all the radiant energy exchanges in the zone is zero. If the user input view factors are perfect in these characteristics, the correction will not change them. The displayed lines show what view factors will be used during the simulation.
+
+\subsubsection{Script F Factors}\label{script-f-factors}
+
+Finally, grey interchange coefficients are presented. These are the coefficients that are used to calculate the radiant energy exchange between the surfaces in the zone. They are calculated to include reflection from intervening surfaces in the zone.
+
+\subsection{DX Coil Outputs}\label{dx-coil-outputs}
+
+\subsection{DX Cooling Coil Outputs}\label{dx-cooling-coil-outputs}
+
+Outputs are provided for air-cooled, single-speed direct expansion (DX) cooling coils as follows:
+
+\begin{lstlisting}
+! <DX Cooling Coil Standard Rating Information>, Component Type, Component Name, Standard Rating (Net) Cooling Capacity {W}, Standard Rated Net COP {W/W}, EER {Btu/W-h}, SEER {Btu/W-h}, IEER {Btu/W-h}
+\end{lstlisting}
+
+~ DX Cooling Coil Standard Rating Information, Coil:Cooling:DX:SingleSpeed, PSZ-AC\_1:1\_COOLC DXCOIL, 29299.3, 3.04, 10.38, 10.47, 10.67
+
+\begin{lstlisting}
+DX Cooling Coil Standard Rating Information, Coil:Cooling:DX:SingleSpeed, PSZ-AC\_2:2\_COOLC DXCOIL, 17427.1, 3.21, 10.95, 11.04, 11.20
+\end{lstlisting}
+
+\subsubsection{Field: Component Type}\label{field-component-type-3}
+
+This is the component type, currently Coil:Cooling:DX:SingleSpeed is the only valid type.
+
+\subsubsection{Field: Component Name}\label{field-component-name-3}
+
+The name of the DX cooling coil from the input data file (IDF).
+
+\subsubsection{Field: Standard Rating (Net) Cooling Capacity \{W\}}\label{field-standard-rating-net-cooling-capacity-w}
+
+The standard rating (net) cooling capacity for this DX cooling coil. Units are Watts. See the EnergyPlus Engineering Reference (Single Speed DX Cooling Coil, Standard Ratings) for details on how this value is calculated.
+
+\subsubsection{Field: Standard Rated Net COP \{W/W\}}\label{field-standard-rated-net-cop-ww}
+
+The standard rated net COP or energy efficiency ratio (\emph{EER}) at standard rating conditions for the DX cooling coil in SI units of W/W. See the EnergyPlus Engineering Reference (Single Speed DX Cooling Coil, Standard Ratings) for details on how this value is calculated.
+
+\subsubsection{Field: EER \{Btu/W-h\}}\label{field-eer-btuw-h}
+
+The energy efficiency ratio (\emph{EER}) at standard rating conditions for the DX cooling coil in IP units of Btu/W-hr. See the EnergyPlus Engineering Reference (Single Speed DX Cooling Coil, Standard Ratings) for details on how this value is calculated.
+
+\subsubsection{Field: SEER \{Btu/W-h\}}\label{field-seer-btuw-h}
+
+The seasonal energy efficiency ratio (SEER) for the DX cooling coil in IP units of Btu/W-hr. See the EnergyPlus Engineering Reference (Single Speed DX Cooling Coil, Standard Ratings) for details on how this value is calculated.
+
+\subsubsection{Field: IEER \{Btu/W-h\}}\label{field-ieer-btuw-h}
+
+The integrated energy efficiency ratio (\emph{IEER}) for the DX cooling coil in IP units of Btu/W-hr. See the EnergyPlus Engineering Reference (Single Speed DX Cooling Coil, Standard Ratings) for details on how this value is calculated.
+
+\subsection{DX Cooling Coil Outputs for ASHRAE 127 Standard Ratings}\label{dx-cooling-coil-outputs-for-ashrae-127-standard-ratings}
+
+\subsubsection{Field: Component Type}\label{field-component-type-4}
+
+This is the component type, currently Coil:Cooling:DX:SingleSpeed is the only valid type.
+
+\subsubsection{Field: Component Name}\label{field-component-name-4}
+
+The name of the DX cooling coil from the input data file (IDF).
+
+\subsubsection{Field: Class}\label{field-class}
+
+The application classification classes of the DX cooling coil. There are four application classification classes per ASHRAE standard 127: Class I, Class II, Class III, and Class IV. The standard ratings are reported for each the four classification classes and test conditions.
+
+\subsubsection{Field: Rated Net Cooling Capacity at Test A \{W\}}\label{field-rated-net-cooling-capacity-at-test-a-w}
+
+Rated net cooling capacity for this DX cooling coil at Test condition A per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The net cooling capacity is reported for class I, II, II and IV test conditions.
+
+\subsubsection{Field: Rated Total Electric Power Test A \{W\}}\label{field-rated-total-electric-power-test-a-w}
+
+Rated total electric power input of the unit at Test condition A per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The total electric power includes the supply fan power as well. The total electric power input is reported for class I, II, III and IV test conditions.
+
+\subsubsection{Field: Rated Net Cooling Capacity at Test B \{W\}}\label{field-rated-net-cooling-capacity-at-test-b-w}
+
+Rated net cooling capacity of this unit at Test condition B per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The net cooling capacity is reported for class I, II, II and IV test conditions.
+
+\subsubsection{Field: Rated Total Electric Power Test B \{W\}}\label{field-rated-total-electric-power-test-b-w}
+
+Rated total electric power input of the unit at Test condition B per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The total electric power includes the supply fan power as well. The total electric power input is reported for class I, II, III and IV test conditions.
+
+\subsubsection{Field: Rated Net Cooling Capacity at Test C \{W\}}\label{field-rated-net-cooling-capacity-at-test-c-w}
+
+Rated net cooling capacity of this unit at Test condition C per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The net cooling capacity is reported for class I, II, II and IV test conditions.
+
+\subsubsection{Field: Rated Total Electric Power Test C \{W\}}\label{field-rated-total-electric-power-test-c-w}
+
+Rated total electric power input of the unit at Test condition C per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The total electric power includes the supply fan power as well. The total electric power input is reported for class I, II, III and IV test conditions.
+
+\subsubsection{Field: Rated Net Cooling Capacity at Test D \{W\}}\label{field-rated-net-cooling-capacity-at-test-d-w}
+
+Rated net cooling capacity of unit at Test condition D per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The net cooling capacity is reported for class I, II, II and IV test conditions.
+
+\subsubsection{Field: Rated Total Electric Power Test D \{W\}}\label{field-rated-total-electric-power-test-d-w}
+
+Rated total electric power input of the unit at Test condition D per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The total electric power includes the supply fan power as well. The total electric power input is reported for class I, II, III and IV test conditions.
+
+\begin{lstlisting}
+! <DX Cooling Coil ASHRAE 127 Standard Ratings Information>, Component Type, Component Name, Standard 127 Classification, Rated Net Cooling Capacity Test A {W}, Rated Total Electric Power Test A {W}, Rated Net Cooling Capacity Test B {W}, Rated Total Electric Power Test B {W}, Rated Net Cooling Capacity Test C {W}, Rated Total Electric Power Test C {W}, Rated Net Cooling Capacity Test D {W}, Rated Total Electric Power Test D {W} 
+ DX Cooling Coil ASHRAE 127 Standard Ratings Information, Coil:Cooling:DX:SingleSpeed, MAIN COOLING COIL 1, Class 1, 126953.8, 35918.5, 135678.7, 30852.7, 141523.1, 24400.1, 141727.0, 13951.0
+ DX Cooling Coil ASHRAE 127 Standard Ratings Information, Coil:Cooling:DX:SingleSpeed, MAIN COOLING COIL 1, Class 2, 133377.6, 37330.3, 140336.0, 31647.7, 141727.0, 24424.7, 141727.0, 13951.0
+ DX Cooling Coil ASHRAE 127 Standard Ratings Information, Coil:Cooling:DX:SingleSpeed, MAIN COOLING COIL 1, Class 3, 139488.4, 38673.3, 141354.0, 31821.4, 141727.0, 24424.7, 141727.0, 13951.0
+ DX Cooling Coil ASHRAE 127 Standard Ratings Information, Coil:Cooling:DX:SingleSpeed, MAIN COOLING COIL 1, Class 4, 145024.0, 39889.8, 141727.0, 31885.1, 141727.0, 24424.7, 141727.0, 13951.0
+\end{lstlisting}
+
+\subsection{DX Heating Coil Outputs}\label{dx-heating-coil-outputs}
+
+Outputs are provided for single-speed direct expansion (DX) heating coils as follows:
+
+\begin{lstlisting}
+! <DX Heating Coil Standard Rating Information>, Component Type, Component Name, High Temperature Heating Standard (Net) Rating Capacity {W}, Low Temperature Heating Standard (Net) Rating Capacity {W}, HSPF {Btu/W-h, Region Number
+DX Heating Coil Standard Rating Information, Coil:Heating:DX:SingleSpeed, PSZ-AC\_1:1\_HEATC DXCOIL, 10476.1, 5833.2, 6.10, 4
+\end{lstlisting}
+
+\subsubsection{Field: Component Type}\label{field-component-type-5}
+
+This is the component type, currently Coil:Heating:DX:SingleSpeed is the only valid type.
+
+\subsubsection{Field: Component Name}\label{field-component-name-5}
+
+The name of the DX heating coil from the input data file (IDF).
+
+\subsubsection{Field: High Temperature Heating Standard (Net) Rating Capacity \{W\}}\label{field-high-temperature-heating-standard-net-rating-capacity-w}
+
+The standard rating (net) heating capacity for this DX heating coil at high temperature. Units are Watts. See the EnergyPlus Engineering Reference (Single Speed DX Heating Coil, Standard Ratings) for details on how this value is calculated.
+
+\subsubsection{Field: Low Temperature Heating Standard (Net) Rating Capacity \{W\}}\label{field-low-temperature-heating-standard-net-rating-capacity-w}
+
+The standard rating (net) heating capacity for this DX heating coil at low temperature. Units are Watts. See the EnergyPlus Engineering Reference (Single Speed DX Heating Coil, Standard Ratings) for details on how this value is calculated.
+
+\subsubsection{Field: HSPF \{Btu/W-h\}}\label{field-hspf-btuw-h}
+
+The heating seasonal performance factor (\emph{HSPF}) for the DX heating coil in IP units of Btu/W-h. See the EnergyPlus Engineering Reference (Single Speed DX Heating Coil, Standard Ratings) for details on how this value is calculated.
+
+\subsubsection{Field: Region Number}\label{field-region-number}
+
+The standard region number for which above ratings are calculated (from the input data file).
+
+\subsection{Chiller Outputs}\label{chiller-outputs}
+
+Outputs are provided for Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR objects as follows:
+
+\begin{lstlisting}
+! <Chiller Standard Rating Information>, Component Type, Component Name, IPLV in SI Units {W/W}, IPLV in IP Units {Btu/W-h}
+Chiller Standard Rating Information, Chiller:Electric:EIR, Big Chiller 1, 4.5, 15.4
+Chiller Standard Rating Information, Chiller:Electric:ReformulatedEIR, Big Chiller 2, 4.8, 16.4
+\end{lstlisting}
+
+\subsubsection{Field: Component Type}\label{field-component-type-6}
+
+This is the component type, Chiller:Electric:EIR and/or Chiller:Electric:ReformulatedEIR.
+
+\subsubsection{Field: Component Name}\label{field-component-name-6}
+
+The name of the Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR objects from the input data file (IDF).
+
+\subsubsection{Field: IPLV in SI Units \{W/W\}}\label{field-iplv-in-si-units-ww}
+
+The integrated part load value (\emph{IPLV}) for the Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR in SI units of W/W. See the EnergyPlus Engineering Reference (Electric Chiller Model Based on Condenser Entering Temperature, Standard Ratings) for details on how this value is calculated.
+
+\subsubsection{Field: IPLV in IP Units \{Btu/W-h\}}\label{field-iplv-in-ip-units-btuw-h}
+
+The integrated part load value (\emph{IPLV}) for the Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR in IP units of Btu/W-hr. See the EnergyPlus Engineering Reference (Electric Chiller Model Based on Condenser Entering Temperature, Standard Ratings) for details on how this value is calculated.
+
+\subsection{Lookup Table Outputs}\label{lookup-table-outputs}
+
+\textbf{The following fields are shown only when the diagnostics flag is set to DisplayExtraWarnings (ref. Output:Diagnotstics, DisplayAdvancedReportVariables).}
+
+Outputs are provided for lookup tables in two forms. The first being the outputs related to the creation of a performance curve. When the Interpolation Method for table objects is set to EvaluateCurveToLimits, a performance curve object is created. The coefficients of the performance curve are calculated and a curve object is written for review. The regression statistics are also included. This performance curve may be used in subsequent simulations or saved in a library file for future use.
+
+\begin{lstlisting}
+! <CREATING NEW CURVE OBJECT>
+CREATING NEW CURVE OBJECT
+! Input as Table:OneIndependentVariable "HPACCOOLCAPFFF"
+! RSquared       = 1.0000000000
+! Standard Error = 0.0000000000
+! Sample Size    = 3
+Curve:Quadratic,
+FromTable_HPACCOOLCAPFFF,  !- Name
+  0.8000000000,  !- Coefficient1 Constant
+  0.2000000000,  !- Coefficient2 x
+  -3.1086244690E-015,  !- Coefficient3 x**2
+  0.0000000000,  !- Minimum Value of x
+  1.5000000000,  !- Maximum Value of x
+  0.8000000000,  !- Minimum Curve Output
+  1.5000000000;  !- Maximum Curve Output
+END CREATING NEW CURVE OBJECT
+``
+\end{lstlisting}
+
+\begin{lstlisting}
+A second output form is provided to echo the reading of tabular data. The tabular data is echoed for each multi-variable lookup table object (ref. Table:MultiVariableLookup). The data is echoed using an increasing order sort format regardless of the format specified by the user. In addition, the tabular data is echoed when the data is included in the table object, or when read from an external file. This output form is provided as a verification step when reading tabular data. The normalization point is not included in the raw data varification.
+\end{lstlisting}
+
+! READING LOOKUP TABLE DATA ! Reading tabular data for Table:MultiVariableLookup ``HPACCOOLCAPFFF2'' ~ 1~~ 3 ~ 0.000000000000000E+000~~ 1.00000000000000~~~~~~~ 1.50000000000000 ~ 0.800000000000000~~~~~~~ 1.00000000000000~~~~~~~ 1.10000000000000 END READING LOOKUP TABLE DATA
+
+\begin{lstlisting}
+### Warmup Days Line
+\end{lstlisting}
+
+\begin{lstlisting}
+As described elsewhere, EnergyPlus simulates the first day of each simulation period until it reaches “convergence�. This data line will show how many warm up days were required to reach that state.
+\end{lstlisting}
+
+\begin{lstlisting}
+! <Environment:WarmupDays>, NumberofWarmupDays
+\end{lstlisting}
+
+\begin{lstlisting}
+Environment:WarmupDays,  6
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: <Environment:WarmupDays>
+\end{lstlisting}
+
+\begin{lstlisting}
+This is a constant that will display “Environment:WarmupDays�.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: NumberofWarmupDays
+\end{lstlisting}
+
+\begin{lstlisting}
+This field will show the number of days required to reach the convergence state for the simulation.
+\end{lstlisting}
+
+\begin{lstlisting}
+### Warmup Convergence Outputs
+\end{lstlisting}
+
+\begin{lstlisting}
+Warmup is performed for each environment being simulated. When a file passes convergence, no warnings are shown.  However, when it doesn’t a warning appears in the eplusout.err file, for example:
+\end{lstlisting}
+
+\begin{lstlisting}
+CheckWarmupConvergence: Loads Initialization, Zone = "BACKROOM" did not converge after 25 warmup days.
+\end{lstlisting}
+
+\begin{lstlisting}
+See Warmup Convergence Information in .eio file for details
+\end{lstlisting}
+
+\begin{lstlisting}
+...Environment(RunPeriod) = "Phoenix Sky Harbor Intl Ap AZ USA TMY3 WMO\# = 722780"
+\end{lstlisting}
+
+\begin{lstlisting}
+..Max Temp Comparison = 8.46E-005 vs Temperature Convergence Tolerance = 0.40 - Pass Convergence
+\end{lstlisting}
+
+\begin{lstlisting}
+..Min Temp Comparison = 7.05E-002 vs Temperature Convergence Tolerance = 0.40 - Pass Convergence
+\end{lstlisting}
+
+\begin{lstlisting}
+..Max Heat Load Comparison = 9.8513E-002 vs Loads Convergence Tolerance = 4.00E-002 - Fail Convergence
+\end{lstlisting}
+
+\begin{lstlisting}
+..Max Cool Load Comparison = 8.2481E-003 vs Loads Convergence Tolerance = 4.00E-002 - Pass Convergence
+\end{lstlisting}
+
+\begin{lstlisting}
+### Warmup Convergence Information
+\end{lstlisting}
+
+\begin{lstlisting}
+Warmup convergence information reflects the warmup days calculations and whether or not the zone has reached “convergence�. Warmup calculations are done for each environment (e.g. each sizing period simulated, each run period simulated). Reference the building parameters on Minimum and Maximum Number of Warmup Days as well as Loads and Temperature convergence Tolerance. The file contains two possible flavors of warmup information: summary and detailed.
+\end{lstlisting}
+
+\begin{lstlisting}
+### Summary Warmup Convergence Information
+\end{lstlisting}
+
+\begin{lstlisting}
+Summary (warmup convergance information is not reported during sizing and only at the end of the calculations). The below information is included after each warmup period.
+\end{lstlisting}
+
+\begin{lstlisting}
+! <Warmup Convergence Information>,Zone Name,Environment Type/Name,Average Warmup Temperature Difference {deltaC},Std Dev Warmup Temperature Difference {deltaC},Max Temperature Pass/Fail Convergence,Min Temperature Pass/Fail Convergence,Average Warmup Load Difference {W},Std Dev Warmup Load Difference {W},Heating Load Pass/Fail Convergence,Cooling Load Pass/Fail Convergence
+\end{lstlisting}
+
+\begin{lstlisting}
+Warmup Convergence Information,PLENUM-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\# = 725300,0.1459548118,7.6866834879E-002,Pass,Pass,6.4148162842E-002,0.1344412193,Pass,Pass
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information,SPACE1-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\# = 725300,0.1205887641,0.2962564087,Pass,Pass,0.6840608138,3.7598304674,Pass,Pass
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information,SPACE2-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\# = 725300,0.1494584750,0.4540146507,Pass,Pass,0.7552649309,3.0925096445,Pass,Pass
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information,SPACE3-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\# = 725300,0.1150550710,0.2873890950,Pass,Pass,7.0443709912,61.6558566585,Pass,Pass
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information,SPACE4-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\# = 725300,0.1153798692,0.4838241280,Pass,Pass,2.4744275587,18.1154149427,Pass,Pass
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information,SPACE5-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\# = 725300,0.1208173250,0.2114200039,Pass,Pass,0.4984428726,2.8997025264,Pass,Pass
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Zone Name
+\end{lstlisting}
+
+\begin{lstlisting}
+This field will show the name of individual zone.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Environment Type/Name
+\end{lstlisting}
+
+\begin{lstlisting}
+Type of environment being run (SizingPeriod, RunPeriod) as well as it’s “name�.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Average Warmup Temperature Difference {deltaC}
+\end{lstlisting}
+
+\begin{lstlisting}
+This field displays the average mean air temperature difference of the zone over the warmup days.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Std Dev Warmup Temperature Difference {deltaC}
+\end{lstlisting}
+
+\begin{lstlisting}
+This field displays the standard deviation of mean air temperature difference of the zone over the warmup days.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Max Temperature Pass/Fail Convergence
+\end{lstlisting}
+
+\begin{lstlisting}
+This field indicates **Pass** or **Fail** for the maximum temperature difference criteria.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Min Temperature Pass/Fail Convergence
+\end{lstlisting}
+
+\begin{lstlisting}
+This field indicates **Pass** or **Fail** for the minimum temperature difference criteria.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Average Warmup Load Difference {W}
+\end{lstlisting}
+
+\begin{lstlisting}
+This field displays the average load difference of the zone over the warmup days.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Std Dev Warmup Load Difference {W}
+\end{lstlisting}
+
+\begin{lstlisting}
+This field displays the standard deviation load difference of the zone over the warmup days.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Heating Load Pass/Fail Convergence
+\end{lstlisting}
+
+\begin{lstlisting}
+This field indicates **Pass** or **Fail** for the heating load criteria.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Cooling Load Pass/Fail Convergence
+\end{lstlisting}
+
+\begin{lstlisting}
+This field indicates **Pass** or **Fail** for the cooling load criteria.
+\end{lstlisting}
+
+\begin{lstlisting}
+### Detailed Warmup Convergence Information
+\end{lstlisting}
+
+\begin{lstlisting}
+Detailed warmup convergence information is reported if you add an Output:Diagnostics, ReportDetailedWarmupConvergence; object statement to the input file. It does not include the current environment name or type as it is displayed immediately after the environment details.
+\end{lstlisting}
+
+\begin{lstlisting}
+! <Warmup Convergence Information>, Zone Name,Time Step,Hour of Day, Warmup Temperature Difference {deltaC}, Warmup Load Difference {W}
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information, PLENUM-1,1,1,7.2649997289E-005,0.3830511891
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information, SPACE1-1,1,1,1.9871863274E-004,1.6099213169E-002
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information, SPACE2-1,1,1,4.2767539998E-003,3.1481614518
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information, SPACE3-1,1,1,1.2388614949E-003,5.9934952313
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information, SPACE4-1,1,1,2.7512443391E-003,3.9192729035
+\end{lstlisting}
+
+\begin{lstlisting}
+ Warmup Convergence Information, SPACE5-1,1,1,1.7415692658E-003,5.3879887714
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Zone Name
+\end{lstlisting}
+
+\begin{lstlisting}
+This field will show the name of individual zone.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Time Step
+\end{lstlisting}
+
+\begin{lstlisting}
+This field will show the value of time step.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Hour of Day
+\end{lstlisting}
+
+\begin{lstlisting}
+This field will show the value of hour of the day.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Warmup Temperature Difference
+\end{lstlisting}
+
+\begin{lstlisting}
+This field will provide a mean air temperature comparison between the second to last and the last warmup day for the simulation.  In other words, it will provide a DT between, for example, 9:10AM on the second to last warmup day and 9:10AM on the last warmup day. The value will be on a zone-by-zone basis for each time step in the simulation.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Field: Warmup Load Difference
+\end{lstlisting}
+
+\begin{lstlisting}
+This field is similar to the previous field except that it displays the heating or cooling load of the zone in question.
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.end
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+This is a simple one line synopsis of the simulation. Successful or Not Successful, including number of errors/warnings:
+\end{lstlisting}
+
+\begin{lstlisting}
+EnergyPlus Completed Successfully-- 8 Warning; 0 Severe Errors
+\end{lstlisting}
+
+\begin{lstlisting}
+If no file is produced, it is really *not* successful and EnergyPlus has probably crashed during the run. This file and its contents are intended for interfaces that will put friendly front-ends onto EnergyPlus. This file is also used by the EP-Launch program so that it can determine if the run was successful or not – if not, the user should review the eplusout.err file. (Actually, the eplusout.err file should always be reviewed but often is ignored in haste to view the results.)
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.epmidf
+---------------
+\end{lstlisting}
+
+\begin{lstlisting}
+If you use an EPMacro file (usual extension is .imf) as your basis for input, then this file is the “idf� that the EPMacro program produces.
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.epmdet
+---------------
+\end{lstlisting}
+
+\begin{lstlisting}
+If you use an EPMacro file (usual extension is .imf) as your basis for input, then this file is the details of the EPMacro run (including any error messages).
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.err
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+This file is *very important* to every simulation run. All of the warnings, errors, etc that occur during the run will show up in this file. They may show up in other files as well. The first line of the error file is also significant:
+\end{lstlisting}
+
+\begin{lstlisting}
+Program Version,EnergyPlus, <version>,IDD\_Version <version>
+\end{lstlisting}
+
+\begin{lstlisting}
+This shows not only the current version of the program but the “version� of the Energy+.idd file that was used.
+\end{lstlisting}
+
+\begin{lstlisting}
+Table 3. EnergyPlus Errors
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+The previous table illustrates the three levels of errors that occur in the eplusout.err file. Several other message lines may be shown as well. For example:
+\end{lstlisting}
+
+\begin{lstlisting}
+\*\* Warning \*\* World Coordinate System selected.  Any non-zero Building/Zone North Axes or non-zero Zone Origins are ignored.
+\end{lstlisting}
+
+\begin{lstlisting}
+\*\*   ~~~   \*\* These may be used in daylighting reference point coordinate calculations  but not in normal geometry inputs.
+\end{lstlisting}
+
+\begin{lstlisting}
+The line that includes the “~~~� is a “continue� error line. It continues from the previous line to help describe the context of the error.
+\end{lstlisting}
+
+\begin{lstlisting}
+Some common errors, their consequences, and what to do about them follows:
+\end{lstlisting}
+
+\begin{lstlisting}
+\*\* Severe  \*\* IP: Possible incorrect IDD File
+\end{lstlisting}
+
+\begin{lstlisting}
+\*\* Severe  \*\* IP: Possible Invalid Numerics
+\end{lstlisting}
+
+\begin{lstlisting}
+\*\*  Fatal  \*\* IP: Errors occurred on processing IDF file. Preceding condition(s) cause termination.
+\end{lstlisting}
+
+\begin{lstlisting}
+The previous errors cause program termination. The most likely cause is that you have an “old� IDF and have not converted it to work with the current version of the program. In this case, you will likely has some other hints such as alphas in numeric fields or too many fields in an object. Energyplus also has built in range checking:
+\end{lstlisting}
+
+\begin{lstlisting}
+\*\* Severe  \*\* Out of range value Numeric Field\#7 (Sky Clearness), value = 100.00000, range = {> = 0.0 and < = 1.2}, in SIZINGPERIOD:DESIGNDAY = CHICAGO ANN CLG .4% CONDNS WB = >MDB
+\end{lstlisting}
+
+\begin{lstlisting}
+If these occur during the initial processing of the IDF, you will see a termination clause:
+\end{lstlisting}
+
+\begin{lstlisting}
+\*\* Severe  \*\* IP: Out of "range" values found in input
+\end{lstlisting}
+
+\begin{lstlisting}
+\*\* Severe  \*\* IP: Out of "range" values and/or blank required fields found in input
+\end{lstlisting}
+
+\begin{lstlisting}
+\*\*  Fatal  \*\* IP: Errors occurred on processing IDF file. Preceding condition(s) cause termination.
+\end{lstlisting}
+
+\begin{lstlisting}
+The error message should supply you with enough information to find the line with the error. More details on error message formatting and some standard error messages are described in the Tips & Tricks document.
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.eso
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+The standard output file from EnergyPlus. It includes all the applicable variables selected with the “Output:Variable� commands as well as those with the “Output:Meter� commands. All levels of frequency of reporting are included intermingled as occurs in the running of the program. The form of the file is a data dictionary, followed by the data.
+\end{lstlisting}
+
+\begin{lstlisting}
+In this case, the dictionary portion of the file comes first followed by an “end of data dictionary line� and then the data makes up the rest of the file.
+\end{lstlisting}
+
+\begin{lstlisting}
+Thus, the basic structure of the standard output file is:
+\end{lstlisting}
+
+\begin{lstlisting}
+Data Dictionary Information
+\end{lstlisting}
+
+\begin{lstlisting}
+End of Data Dictionary
+\end{lstlisting}
+
+\begin{lstlisting}
+Data
+\end{lstlisting}
+
+\begin{lstlisting}
+…
+\end{lstlisting}
+
+\begin{lstlisting}
+Data
+\end{lstlisting}
+
+\begin{lstlisting}
+End of Data
+\end{lstlisting}
+
+\begin{lstlisting}
+As with the IDF structure, there are rules associated with the interpretation of the standard output data dictionary. These rules are summarized as follows:
+\end{lstlisting}
+
+\begin{lstlisting}
+- The first item on each line is an integer which represents the “report code�. This “report code� will be listed in the data section where it will also be the first item on each line, identifying the data. Only 2 lines in the output file will not have an integer as the first item (“End of Data Dictionary� and “End of Data� lines).
+\end{lstlisting}
+
+\begin{lstlisting}
+- The second item on each line is also an integer. This integer corresponds to the number of items left on the dictionary line. Each string consists of a variable name and units in square brackets. Square brackets are required for all strings. If there are no units associated with a particular variable, then there are no characters between the brackets.
+\end{lstlisting}
+
+\begin{lstlisting}
+Six standard items appear at the start of every EnergyPlus Standard Output File Data Dictionary:
+\end{lstlisting}
+
+\begin{lstlisting}
+Program Version,EnergyPlus <version number indicated>
+\end{lstlisting}
+
+\begin{lstlisting}
+  1,5,Environment Title[],Latitude[deg],Longitude[deg],Time Zone[],Elevation[m]
+\end{lstlisting}
+
+\begin{lstlisting}
+  2,6,Day of Simulation[],Month[],Day of Month[],DST Indicator[1 = yes 0 = no],Hour[],StartMinute[],EndMinute[],DayType
+\end{lstlisting}
+
+\begin{lstlisting}
+  3,3,Cumulative Day of Simulation[],Month[],Day of Month[],DST Indicator[1 = yes 0 = no],DayType  ! When Daily Report Variables Requested
+\end{lstlisting}
+
+\begin{lstlisting}
+  4,2,Cumulative Days of Simulation[],Month[]  ! When Monthly Report Variables Requested
+\end{lstlisting}
+
+\begin{lstlisting}
+  5,1,Cumulative Days of Simulation[] ! When Run Period Report Variables Requested
+\end{lstlisting}
+
+\begin{lstlisting}
+Item 0 is the program version statement.
+\end{lstlisting}
+
+\begin{lstlisting}
+Item 1 is produced at the beginning of each new “environment� (design day, run period).
+\end{lstlisting}
+
+\begin{lstlisting}
+Item 2 is produced prior to any variable reported at the timestep or hourly intervals. Hourly intervals will be shown with a start minute of 0.0 and an end minute of 60.0. Timestep intervals will show the appropriate start and end minutes.
+\end{lstlisting}
+
+\begin{lstlisting}
+Item 3 is produced prior to any variable reported at the daily interval.
+\end{lstlisting}
+
+\begin{lstlisting}
+Item 4 is produced prior to any variable reported at the monthly interval.
+\end{lstlisting}
+
+\begin{lstlisting}
+Item 5 is produced prior to any variable reported at the end of the “environment�.
+\end{lstlisting}
+
+\begin{lstlisting}
+Following these five standard lines will be the variables requested for reporting from the input file (ref. Report Variable). For example:
+\end{lstlisting}
+
+\begin{lstlisting}
+6,2,Environment,Site Outdoor Air Drybulb Temperature [C] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+21,2,ZONE ONE,Zone Mean Air Temperature [C] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+22,2,ZONE ONE,Zone Total Latent Gain [J] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+26,2,ZONE ONE,Zone Lights Electric Energy [J] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+This example illustrates the non-consecutive nature of the “report codes�. Internally, EnergyPlus counts each variable that *could* be reported. This is the assigned “report code�. However, the user may not request each possible variable for reporting. Note that, currently, the requested reporting frequency is shown as a comment (!) line in the standard output file.
+\end{lstlisting}
+
+\begin{lstlisting}
+The data is produced when the actual simulation is performed (after the warmup days unless the Output:Diagnostics requesting ReportDuringWarmup is used). Data output is simpler in format than the data dictionary lines. From the dictionary above:
+\end{lstlisting}
+
+\begin{lstlisting}
+     1,DENVER COLORADO WINTER,  39.75,-104.87,  -7.00,1610.26
+\end{lstlisting}
+
+\begin{lstlisting}
+     2,  1, 1,21, 0, 1, 0.00,60.00,Monday
+\end{lstlisting}
+
+\begin{lstlisting}
+6,-17.22222
+\end{lstlisting}
+
+\begin{lstlisting}
+21,-17.22219
+\end{lstlisting}
+
+\begin{lstlisting}
+22,0.0000000E+00
+\end{lstlisting}
+
+\begin{lstlisting}
+26,0.0000000E+00
+\end{lstlisting}
+
+\begin{lstlisting}
+     2,  1, 1,21, 0, 2, 0.00,60.00,Monday
+\end{lstlisting}
+
+\begin{lstlisting}
+6,-17.22222
+\end{lstlisting}
+
+\begin{lstlisting}
+21,-17.22219
+\end{lstlisting}
+
+\begin{lstlisting}
+22,0.0000000E+00
+\end{lstlisting}
+
+\begin{lstlisting}
+26,0.0000000E+00
+\end{lstlisting}
+
+\begin{lstlisting}
+     2,  1, 1,21, 0, 3, 0.00,60.00,Monday
+\end{lstlisting}
+
+\begin{lstlisting}
+6,-17.22222
+\end{lstlisting}
+
+\begin{lstlisting}
+21,-17.22219
+\end{lstlisting}
+
+\begin{lstlisting}
+22,0.0000000E+00
+\end{lstlisting}
+
+\begin{lstlisting}
+26,0.0000000E+00
+\end{lstlisting}
+
+\begin{lstlisting}
+…
+\end{lstlisting}
+
+\begin{lstlisting}
+This output file can be easily turned into a form that is read into commonly used spreadsheet programs where it can be further analyzed, graphed, etc.
+\end{lstlisting}
+
+\begin{lstlisting}
+![](media/image014.png)
+\end{lstlisting}
+
+\begin{lstlisting}
+Figure 4. Example Chart from Standard Output File
+\end{lstlisting}
+
+\begin{lstlisting}
+Program Version,EnergyPlus, <version>
+\end{lstlisting}
+
+\begin{lstlisting}
+     1,5,Environment Title[],Latitude[deg],Longitude[deg],Time Zone[],Elevation[m]
+\end{lstlisting}
+
+\begin{lstlisting}
+     2,6,Day of Simulation[],Month[],Day of Month[],DST Indicator[1 = yes 0 = no],Hour[],StartMinute[],EndMinute[],DayType
+\end{lstlisting}
+
+\begin{lstlisting}
+     3,3,Cumulative Day of Simulation[],Month[],Day of Month[],DST Indicator[1 = yes 0 = no],DayType  ! When Daily Report Variables Requested
+\end{lstlisting}
+
+\begin{lstlisting}
+     4,2,Cumulative Days of Simulation[],Month[]  ! When Monthly Report Variables Requested
+\end{lstlisting}
+
+\begin{lstlisting}
+     5,1,Cumulative Days of Simulation[] ! When Run Period Report Variables Requested
+\end{lstlisting}
+
+\begin{lstlisting}
+6,2,Environment, Site Outdoor Air Drybulb Temperature [C] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+429,2,RESISTIVE ZONE, Zone Air System Sensible Heating Energy [J] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+450,2,RESISTIVE ZONE, Zone Air System Sensible Cooling Energy [J] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+458,2,RESISTIVE ZONE, Zone Air Temperature [C] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+463,2,EAST ZONE, Zone Air System Sensible Heating Energy [J] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+469,2,EAST ZONE, Zone Air System Sensible Cooling Energy [J] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+472,2,EAST ZONE, Zone Air Temperature [C] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+477,2,NORTH ZONE, Zone Air System Sensible Heating Energy [J] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+483,2,NORTH ZONE, Zone Air System Sensible Cooling Energy [J] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+486,2,NORTH ZONE, Zone Air Temperature [C] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+491,2,SimHVAC, HVAC System Solver Iteration Count !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+521,2,SimAir, Air System Simulation Maximum Iteration Count !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+<reduced for brevity>
+\end{lstlisting}
+
+\begin{lstlisting}
+End of Data Dictionary
+\end{lstlisting}
+
+\begin{lstlisting}
+  1,CHANUTE AFB ILLINOIS SUMMER,  40.30, -88.13,  -6.00, 229.51
+\end{lstlisting}
+
+\begin{lstlisting}
+  2,   1, 7,21, 0, 1, 0.00,60.00,Monday
+\end{lstlisting}
+
+\begin{lstlisting}
+6,21.2884261500000
+\end{lstlisting}
+
+\begin{lstlisting}
+429,0.000000000000000E+000
+\end{lstlisting}
+
+\begin{lstlisting}
+450,0.000000000000000E+000
+\end{lstlisting}
+
+\begin{lstlisting}
+458,31.1054947436037
+\end{lstlisting}
+
+\begin{lstlisting}
+463,0.000000000000000E+000
+\end{lstlisting}
+
+\begin{lstlisting}
+469,0.000000000000000E+000
+\end{lstlisting}
+
+\begin{lstlisting}
+472,31.2222148107451
+\end{lstlisting}
+
+\begin{lstlisting}
+477,0.000000000000000E+000
+\end{lstlisting}
+
+\begin{lstlisting}
+483,0.000000000000000E+000
+\end{lstlisting}
+
+\begin{lstlisting}
+486,31.5855358697037
+\end{lstlisting}
+
+\begin{lstlisting}
+Each report variable (ref: eplusout.rdd) is assigned an identification number, as in the line:
+\end{lstlisting}
+
+\begin{lstlisting}
+486,2,NORTH ZONE,Zone Air Temperature [C] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+**\#486** is the id number of the Zone/Sys Air Temperature value for the North Zone.
+\end{lstlisting}
+
+\begin{lstlisting}
+**2** – is the number of parameters on the line
+\end{lstlisting}
+
+\begin{lstlisting}
+**North Zone** – the identifying “key name� for the line
+\end{lstlisting}
+
+\begin{lstlisting}
+**Zone Air Temperature [C]** – the actual report variable name along with units [C]
+\end{lstlisting}
+
+\begin{lstlisting}
+**! Hourly** – the ! is the standard comment character, information following this character reminds the user how frequently this data will appear in the following.
+\end{lstlisting}
+
+\begin{lstlisting}
+As another example:
+\end{lstlisting}
+
+\begin{lstlisting}
+Each **Output:Variable** object causes a specific number assignment for outputs. For example, you could request separate reporting for the outside temperature:
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*, Site Outdoor Air Drybulb Temperature,timestep;
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*, Site Outdoor Air Drybulb Temperature,hourly;
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*, Site Outdoor Air Drybulb Temperature,monthly;
+\end{lstlisting}
+
+\begin{lstlisting}
+And the following would appear in the standard output file:
+\end{lstlisting}
+
+\begin{lstlisting}
+6,2,Environment,Site Outdoor Air Drybulb Temperature [C] !TimeStep
+\end{lstlisting}
+
+\begin{lstlisting}
+7,2,Environment,Site Outdoor Air Drybulb Temperature [C] !Hourly
+\end{lstlisting}
+
+\begin{lstlisting}
+8,2,Environment,Site Outdoor Air Drybulb Temperature [C] !Monthly [Value,Min,Day,Hour,Minute,Max,Day,Hour,Minute]
+\end{lstlisting}
+
+\begin{lstlisting}
+Item \# 6 will be listed following the TimeStep timestamp for each timestep. Item \#7 will be listed following an hourly timestamp. And item \#8 will be listed following a monthly timestamp and has additional fields (because it is an “average� variable) that show the minimum and maximum values with identifying times for those minimum and maximum. An excerpt will illustrate:
+\end{lstlisting}
+
+\begin{lstlisting}
+     2,  1, 7,21, 0, 1, 0.00,15.00,Monday** – timestep timestamp**
+\end{lstlisting}
+
+\begin{lstlisting}
+6,17.08889
+\end{lstlisting}
+
+\begin{lstlisting}
+48,21.39851
+\end{lstlisting}
+
+\begin{lstlisting}
+49,0.0000000E+00
+\end{lstlisting}
+
+\begin{lstlisting}
+53,0.0000000E+00
+\end{lstlisting}
+
+\begin{lstlisting}
+60,21.87214
+\end{lstlisting}
+
+\begin{lstlisting}
+     2,  1, 7,21, 0, 1, 0.00,60.00,Monday** – hourly timestamp**
+\end{lstlisting}
+
+\begin{lstlisting}
+7,16.75555
+\end{lstlisting}
+
+\begin{lstlisting}
+     4,  1, 7** – monthly timestamp**
+\end{lstlisting}
+
+\begin{lstlisting}
+8,22.77037,15.00000,21, 4,60,32.77778,21,14,60
+\end{lstlisting}
+
+\begin{lstlisting}
+To interpret, the first value (\#6) is 17.09 C, \#7 is 16.76 C (average for the hour), and \#8 is 22.77 C, the average for the month with the low (minimum) of 15 C occurring on 7/21 4:60 (or 5:00) and the high (maximum) occurring on 7/21 14:60 (or 15:00).
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.log
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+When EnergyPlus is running, it is usually running from a “command� window (unless inside another interface program) and some items may appear in the command window. These messages are preserved in the “log� output file. For example:
+\end{lstlisting}
+
+~EnergyPlus Starting ~EnergyPlus, Version ~Processing Data Dictionary ~Processing Input File ~Warming up ~Initializing Response Factors ~Calculating CTFs for ``ROOF-1'', Construction \#1 ~Calculating CTFs for ``WALL-1'', Construction \#2 ~Calculating CTFs for ``FLOOR-SLAB-1'', Construction \#6 ~Calculating CTFs for ``INT-WALL-1'', Construction \#7 ~Initializing Window Optical Properties ~Initializing Solar Calculations ~Initializing HVAC ~Warming up ~Warming up ~Performing Zone Sizing Simulation ~Warming up ~Warming up ~Performing Zone Sizing Simulation ~Calculating System sizing ~Calculating System sizing ~Initializing New Environment Parameters ~Warming up \{1\} ~Warming up \{2\} ~Warming up \{3\} ~Starting Simulation at 01/01 for CHICAGO IL USA TMY2-94846 WMO\# = 725300 ~Updating Shadowing Calculations, Start Date = 01/21 ~Continuing Simulation at 01/21 for CHICAGO IL USA TMY2-94846 WMO\# = 725300 ~Updating Shadowing Calculations, Start Date = 02/10 ~Continuing Simulation at 02/10 for CHICAGO IL USA TMY2-94846 WMO\# = 725300 ~Updating Shadowing Calculations, Start Date = 03/02 ~Continuing Simulation at 03/02 for CHICAGO IL USA TMY2-94846 WMO\# = 725300 ~Updating Shadowing Calculations, Start Date = 03/22 ~Continuing Simulation at 03/22 for CHICAGO IL USA TMY2-94846 WMO\# = 725300 Updating Shadowing Calculations, Start Date = 12/07 ~Continuing Simulation at 12/07 for CHICAGO IL USA TMY2-94846 WMO\# = 725300 ~Updating Shadowing Calculations, Start Date = 12/27 ~Continuing Simulation at 12/27 for CHICAGO IL USA TMY2-94846 WMO\# = 725300 ~EnergyPlus Run Time = 00hr 00min 46.00sec ReadVarsESO program starting. ReadVars Run Time = 00hr 00min~ 1.11sec ReadVarsESO program completed successfully. ReadVarsESO program starting. ReadVars Run Time = 00hr 00min~ 0.00sec ReadVarsESO program completed successfully. ~ Started HVAC Diagram ~ Complete
+
+\begin{lstlisting}
+eplusout.mtd
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+This file contains the “meter details� for the run. This shows what report variables are on which meters and vice versa – which meters contain what report variables.
+\end{lstlisting}
+
+\begin{lstlisting}
+The meter details file consists of two parts:
+\end{lstlisting}
+
+\begin{lstlisting}
+- For report variables that are on meters, it shows all the meters that the report variable is on.  In the following example, “Meters for “ <report variable \#>, <report variable name> is shown and then the meters that accumulate the value of that variable as a “meter�.
+\end{lstlisting}
+
+\begin{lstlisting}
+ Meters for 1240,SPACE1-1:Lights-Electric Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = Electricity:Facility [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = Electricity:Building [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = Electricity:Zone:SPACE1-1 [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = InteriorLights:Electricity [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = InteriorLights:Electricity:Zone:SPACE1-1 [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+ Meters for 1460,SPACE1-1:Zone Air System Sensible Heating Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = EnergyTransfer:Facility [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = EnergyTransfer:Building [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = EnergyTransfer:Zone:SPACE1-1 [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = Heating:EnergyTransfer [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+ Meters for 1557,SPACE1-1 ZONE COIL:Heating Coil Heating Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = EnergyTransfer:Facility [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = EnergyTransfer:HVAC [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = HeatingCoils:EnergyTransfer [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+- For each meter, the report variables that make up that meter are shown. In the following example, “For Meter = � <name of meter>, “contents are:� and then each variable that occurs on that “meter� are shown.
+\end{lstlisting}
+
+\begin{lstlisting}
+For Meter = Electricity:Facility [J], contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE1-1 LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE2-1 LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE3-1 LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE4-1 LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE5-1 LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE1-1 ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE2-1 ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE3-1 ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE4-1 ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE5-1 ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SUPPLY FAN 1:Fan Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  CENTRAL CHILLER:Chiller Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  HW CIRC PUMP:Pump Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  CW CIRC PUMP:Pump Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+ For Meter = Electricity:Building [J], contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE1-1 LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE2-1 LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE3-1 LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE4-1 LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE5-1 LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE1-1 ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE2-1 ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE3-1 ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE4-1 ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE5-1 ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+ For Meter = Electricity:Zone:SPACE1-1 [J], contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE1-1 LIGHTS:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE1-1 ELECEQ:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+ For Meter = InteriorLights:Electricity [J], contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE1-1 LIGHTS:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE2-1 LIGHTS:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE3-1 LIGHTS:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE4-1 LIGHTS:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE5-1 LIGHTS:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+For Meter = Gas:Facility [J], contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  CENTRAL BOILER:Boiler Gas Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+ For Meter = Gas:Plant [J], contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  CENTRAL BOILER:Boiler Gas Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+ For Meter = Heating:Gas [J], contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  CENTRAL BOILER:Boiler Gas Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+ For Meter = Electricity:Plant [J], contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  CENTRAL CHILLER:Chiller Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  HW CIRC PUMP:Pump Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  CW CIRC PUMP:Pump Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+ For Meter = Cooling:Electricity [J], contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  CENTRAL CHILLER:Chiller Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+ For Meter = Cooling:EnergyTransfer [J], contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  PLENUM-1:Zone Air System Sensible Cooling Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE1-1:Zone Air System Sensible Cooling Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE2-1:Zone Air System Sensible Cooling Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE3-1:Zone Air System Sensible Cooling Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE4-1:Zone Air System Sensible Cooling Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SPACE5-1:Zone Air System Sensible Cooling Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+As further illustration, an abbreviated example shows:
+\end{lstlisting}
+
+\begin{lstlisting}
+Meters for 6,EAST ZONE LIGHTS 1:Lights Electric Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = Electricity:Facility [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = Electricity:Building [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = Electricity:Zone:EAST ZONE [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = InteriorLights:Electricity [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = InteriorLights:Electricity:Zone:EAST ZONE [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+  OnMeter = GeneralLights:InteriorLights:Electricity [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+For Meter = Electricity:Facility [J], ResourceType = Electricity, contents are:
+\end{lstlisting}
+
+\begin{lstlisting}
+  EAST ZONE LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  NORTH ZONE LIGHTS 1:Lights Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  WEST ZONE ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  EAST ZONE ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  NORTH ZONE ELECEQ 1:Electric Equipment Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  SUPPLY FAN 1:Fan Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  LITTLE CHILLER:Chiller Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  BIG CHILLER:Chiller Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  BIG TOWER:Cooling Tower Fan Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  CIRC PUMP:Pump Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  COND CIRC PUMP:Pump Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+  HW CIRC PUMP:Pump Electric Energy
+\end{lstlisting}
+
+\begin{lstlisting}
+This shows the meters on which the Zone: Lights Electric Energy appear as well as the contents of the Electricity:Facility meter.
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.mtr
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+This is the equivalent file to the eplusout.eso file but contains only the Report Meter requests. The format and style of the file is identical to the eplusout.eso file.
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.rdd
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+This file (from the **Output:VariableDictionary,regular;** and **Output:VariableDictionary,IDF;** commands) shows all the report variables along with their “availability� for the current input file. Each simulation *may have* different output variables though some are constant (for example the environmental/outdoor variables! A user must first run the simulation (at least semi-successfully) before the available output variables are known. This output file is available in two flavors: regular (listed as they are in the Input Output Reference) and IDF (ready to be copied and pasted into your Input File). Once this file is generated, the IDF editor can use them for Output:Variable keys. You can also ask for the outputs to be sorted by name.
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:VariableDictionary,regular,Name;
+\end{lstlisting}
+
+\begin{lstlisting}
+“**Zone**� variables are calculated and can be reported after each Zone/Heat Balance timestep (ref: TimeSteps in Hour command). “**HVAC**� variables are calculated and can be reported with each variable HVAC timestep. “Average� variables will be averaged over the time interval being reported whereas “sum� variables are summed over that time interval.
+\end{lstlisting}
+
+\begin{lstlisting}
+There are two mitigating factors for this output variable list. One is the “Advanced Report Variables� and the other is the “Create Minimal Surface Variables�.
+\end{lstlisting}
+
+\begin{lstlisting}
+### Normal Output Variables – regular format
+\end{lstlisting}
+
+\begin{lstlisting}
+A typical rdd file might be:
+\end{lstlisting}
+
+\begin{lstlisting}
+Program Version,EnergyPlus, <version>, <date/time of run>,IDD\_Version <IDD Version>
+\end{lstlisting}
+
+\begin{lstlisting}
+Var Type (reported timestep),Var Report Type,Variable Name [Units]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Outdoor Air Drybulb Temperature [C]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Outdoor Air Dewpoint Temperature [C]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Outdoor Air Wetbulb Temperature [C]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Outdoor Air Humidity Ratio [kgWater/kgAir]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Outdoor Air Relative Humidity [%]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Outdoor Air Barometric Pressure [Pa]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Wind Speed [m/s]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Wind Direction [deg]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Sky Temperature [C]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Diffuse Solar Radiation Rate per Area [W/m2]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Direct Solar Radiation Rate per Area [W/m2]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Ground Reflected Solar Radiation Rate per Area [W/m2]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Site Ground Temperature [C]
+\end{lstlisting}
+
+\begin{lstlisting}
+<reduced>
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Surface Window Transmitted Solar Radiation Rate[W]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Surface Window Transmitted Beam Solar Radiation Rate[W]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Surface Window Transmitted Diffuse Solar Radiation Rate[W]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Zone Windows Total Heat Gain Rate[W]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Zone Windows Total Heat Loss Rate[W]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Surface Window Gap Convective Heat Transfer Rate[W]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Surface Window Shading Device Absorbed Solar Radiation Rate[W]
+\end{lstlisting}
+
+\begin{lstlisting}
+<reduced>
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Temperature [C]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Mass Flow Rate[kg/s]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Humidity Ratio[]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Setpoint Temperature[C]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Setpoint Temperature Hi[C]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Setpoint Temperature Lo[C]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Setpoint Humidity Ratio[kgWater/kgDryAir]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Setpoint Minimum Humidity Ratio[kgWater/kgDryAir]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Setpoint Maximum Humidity Ratio[kgWater/kgDryAir]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Current Density Volume Flow Rate[m3/s]HVAC,Average,System Node Enthalpy[J/kg]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,System Node Wetbulb Temperature[C]
+\end{lstlisting}
+
+\begin{lstlisting}
+<reduced>
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum, Zone Mechanical Ventilation No Load Heat Removal Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum,Zone Mechanical Ventilation Cooling Load Increase Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum, Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum,Zone Mechanical Ventilation Cooling Load Decrease Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum,Zone Mechanical Ventilation No Load Heat Addition [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum,Zone Mechanical Ventilation Heating Load Increase Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum, Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy[J]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum,Zone Mechanical Ventilation Heating Load Decrease Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,Zone Mechanical Ventilation Mass Flow Rate [kg/s]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average, Zone Mechanical Ventilation Standard Density Volume Flow Rate [m3/s]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum,Zone Mechanical Ventilation Standard Density Volume [m3]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum,Zone Mechanical Ventilation Mass [kg]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Average,Zone Mechanical Ventilation Air Changes per Hour [ach]
+\end{lstlisting}
+
+\begin{lstlisting}
+### Normal Output Variables – regular format – sorted by name
+\end{lstlisting}
+
+\begin{lstlisting}
+The same variables but now sorted alphabetically by name.
+\end{lstlisting}
+
+\begin{lstlisting}
+Program Version,EnergyPlus, <version>, <date/time of run>,IDD\_Version <IDD Version>
+\end{lstlisting}
+
+\begin{lstlisting}
+Var Type (reported time step),Var Report Type,Variable Name [Units]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum,Air System Solver Iteration Count []
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum,Environmental Impact Total CH4 Emissions Carbon Equivalent Mass [kg]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum,Environmental Impact Total CO2 Emissions Carbon Equivalent Mass [kg]
+\end{lstlisting}
+
+\begin{lstlisting}
+HVAC,Sum, Environmental Impact Total N2O Emissions Carbon Equivalent Mass [kg]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Sum,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Sum,Surface Inside Face Interior Windows Incident Beam Solar Radiation Energy [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate [W]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate [W]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate per Area [W/m2]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Average, Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate per Area [W/m2]
+\end{lstlisting}
+
+\begin{lstlisting}
+### Normal Output Variables – IDF format
+\end{lstlisting}
+
+\begin{lstlisting}
+A brief excerpt of the IDF format is shown below. These can be copied and pasted directly into an IDF or used from the IDF Editor.
+\end{lstlisting}
+
+\begin{lstlisting}
+! Program Version, <version>, <date/time of run>,IDD\_Version <IDD version>
+\end{lstlisting}
+
+\begin{lstlisting}
+! Output:Variable Objects (applicable to this run)
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*,Site Outdoor Air Drybulb Temperature,hourly; !- Zone Average [C]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*,Site Outdoor Air Dewpoint Temperature,hourly; !- Zone Average [C]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*,Site Outdoor Air Wetbulb Temperature,hourly; !- Zone Average [C]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*,Site Outdoor Air Humidity Ratio,hourly; !- Zone Average [kgWater/kgDryAir]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*,Site Outdoor Air Relative Humidity,hourly; !- Zone Average [%]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*,Site Outdoor Air Barometric Pressure,hourly; !- Zone Average [Pa]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*,Site Wind Speed,hourly; !- Zone Average [m/s]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Variable,\*,Site Wind Direction,hourly; !- Zone Average [deg]
+\end{lstlisting}
+
+\begin{lstlisting}
+### Advanced Output Variables
+\end{lstlisting}
+
+\begin{lstlisting}
+The DisplayAdvancedReportVariables key to the Output:Diagnostics object adds a number of variables that may need special handling or understanding of the users. Search on the Input Output Reference document for DisplayAdvancedReportVariables for more details.
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.mdd
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+This file (from the **Output:VariableDictionary,regular;** and **Output:VariableDictionary,IDF;** commands) shows all the report meters along with their “availability� for the current input file. A user must first run the simulation (at least semi-successfully) before the available output meters are known. This output file is available in two flavors: **regular** (listed as they are in the Input Output Reference) and **IDF** (ready to be copied and pasted into your Input File). Once this file is generated, the IDF editor can use them for Output:Meter and Output:CumulativeMeter keys.
+\end{lstlisting}
+
+\begin{lstlisting}
+Note that meters are always accumulated to the Zone timestep. They are always “summed� variables.
+\end{lstlisting}
+
+\begin{lstlisting}
+### Meter Variables – regular format
+\end{lstlisting}
+
+\begin{lstlisting}
+Program Version,EnergyPlus <version>, <date time of run>,IDD\_Version <IDD Version>
+\end{lstlisting}
+
+\begin{lstlisting}
+Var Type (reported timestep),Var Report Type,Variable Name [Units]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,Electricity:Facility [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,Electricity:Building [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,Electricity:Zone:SOUTHZONE\_1STFLOOR [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,InteriorLights:Electricity [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,InteriorLights:Electricity:Zone:SOUTHZONE\_1STFLOOR [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,GeneralLights:InteriorLights:Electricity [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+<reduced>
+\end{lstlisting}
+
+\begin{lstlisting}
+Note that custom meters also appear on this file:
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,MYGENERALLIGHTS [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,MYBUILDINGELECTRIC [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,MYBUILDINGOTHER [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+### Meter Variables – regular format – sorted by name
+\end{lstlisting}
+
+\begin{lstlisting}
+The meter variable file can also be sorted by name. If the rdd is sorted by name, then the meter mdd file will be as well.
+\end{lstlisting}
+
+\begin{lstlisting}
+Program Version,EnergyPlus <version>, <date time of run>,IDD\_Version <IDD Version>
+\end{lstlisting}
+
+\begin{lstlisting}
+Var Type (reported time step),Var Report Type,Variable Name [Units]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,Carbon Equivalent:Facility [kg]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,CarbonEquivalentEmissions:Carbon Equivalent [kg]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,Cogeneration:ElectricityNet [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,Cogeneration:ElectricityPurchased [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Zone,Meter,Cogeneration:ElectricitySurplusSold [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+<snip>
+\end{lstlisting}
+
+\begin{lstlisting}
+### Meter Variables – IDF format
+\end{lstlisting}
+
+\begin{lstlisting}
+This report produces the variable names in a form that are ready to be merged into an input file. By design, hourly reporting is selected – replace this with your desired frequency. An example of the results:
+\end{lstlisting}
+
+\begin{lstlisting}
+! Program Version, <version>, <date/time of run>, IDD\_Version <IDD version>
+\end{lstlisting}
+
+\begin{lstlisting}
+! Output:Meter Objects (applicable to this run)
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,DistrictHeating:Facility,hourly; !- [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter:Cumulative,DistrictHeating:Facility,hourly; !- [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,DistrictHeating:HVAC,hourly; !- [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter:Cumulative,DistrictHeating:HVAC,hourly; !- [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,Heating:DistrictHeating,hourly; !- [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter:Cumulative,Heating:DistrictHeating,hourly; !- [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,DistrictCooling:Facility,hourly; !- [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter:Cumulative,DistrictCooling:Facility,hourly; !- [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,DistrictCooling:HVAC,hourly; !- [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter:Cumulative,DistrictCooling:HVAC,hourly; !- [J]
+\end{lstlisting}
+
+\begin{lstlisting}
+### Meter Naming Convention
+\end{lstlisting}
+
+\begin{lstlisting}
+To repeat some of the detail described in the Input Output Reference document:
+\end{lstlisting}
+
+\begin{lstlisting}
+Meter names are of three forms:
+\end{lstlisting}
+
+\begin{lstlisting}
+- <ResourceType>:<name>
+\end{lstlisting}
+
+\begin{lstlisting}
+Or
+\end{lstlisting}
+
+\begin{lstlisting}
+- <EndUseType>:<ResourceType>:<name>
+\end{lstlisting}
+
+\begin{lstlisting}
+Or
+\end{lstlisting}
+
+\begin{lstlisting}
+- <EndUseSubcategory>:<EndUseType>:<ResourceType>:<name>.
+\end{lstlisting}
+
+\begin{lstlisting}
+The user requests reporting by either specifying the full name above (without Units) or a “wildcard� representation of that name (to obtain all meters of a type). For example, entering “Electricity:\*� for the meter name will report on all the Electricity: meters (Electricity:Facility, Electricity:Building, Electricity:Zone:Resistive Zone, Electricity:Zone:East Zone, Electricity:North Zone in the example above). Both the resource types and end-use types are set within the program by the developers. End-use subcategories are user-defined and are an input field for certain objects.
+\end{lstlisting}
+
+\begin{lstlisting}
+To summarize the previous paragraph, you could use:
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,Electricity:\*;
+\end{lstlisting}
+
+\begin{lstlisting}
+To get the same outputs as if you had entered:
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,Electricity:Facility;
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,Electricity:Building;
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,Electricity:Zone:South Zone;
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,Electricity:Zone:East Zone;
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Meter,Electricity:North Zone;
+\end{lstlisting}
+
+\begin{lstlisting}
+From a three zone file that had no HVAC electricity (i.e., had only electric equipment or lighting equipment in an uncontrolled three zone building).
+\end{lstlisting}
+
+\begin{lstlisting}
+Current resource types are shown in the table below:
+\end{lstlisting}
+
+\begin{lstlisting}
+Table 4. Table of Metered Resource  Types
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+The end use types are shown in the following table (note that certain end use types apply only to the EnergyTransfer resource):
+\end{lstlisting}
+
+\begin{lstlisting}
+The end use types are shown in the following table:
+\end{lstlisting}
+
+\begin{lstlisting}
+Table 5. End Use Category Types
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Specific meter types are then used for grouping the fuel type meters:
+\end{lstlisting}
+
+\begin{lstlisting}
+Table 6. Overall Meter Types
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Facility meters contain all the energy of a fuel type. Building meters contain the sum of each zone’s energy. System meters contain the energy from the system components. Plant meters contain the energy from the plant equipments.
+\end{lstlisting}
+
+\begin{lstlisting}
+Thus, the following relationships should be observed:
+\end{lstlisting}
+
+\begin{lstlisting}
+$$\text{Facility} = \sum\left(\text{Building} + \text{System} + \text{Plant} + \text{Exterior}\right)$$ 
+\end{lstlisting}
+
+\begin{lstlisting}
+$$\text{Building} = \sum_{i}^{\#Zones} \text{Zone}$$ 
+\end{lstlisting}
+
+\begin{lstlisting}
+Custom Meters, (review Input Output Reference, objects: **Meter:Custom** and **Meter:CustomDecrement**) for further requirements, are reported in the same way as pre-defined meters.
+\end{lstlisting}
+
+\begin{lstlisting}
+For example, one might put the Building Infiltration Heat Loss & Heat Gain on a set of custom meters:
+\end{lstlisting}
+
+~ Meter:Custom, ~~~ Building Infiltration Heat Loss,~ !- Name ~~~ Generic,~~~~~~~~~~~~ !- Fuel Type ~~~ *,~~~~~~~~~~~~~~~~~~~~~~ !- Key Name 1 ~~~ Zone Infiltration Total Heat Loss Energy;~ !- Output Variable Name 1
+
+~ Meter:Custom, ~~ ~Building Infiltration Heat Gain,~ !- Name ~~~ Generic,~~~~~~~~~~~~ !- Fuel Type ~~~ *,~~~~~~~~~~~~~~~~~~~~~~ !- Key Name 1 ~~~ Zone Infiltration Total Heat Gain Energy;~ !- Output Variable Name 1
+
+\begin{lstlisting}
+One can then report these values the same way one reports other standard meters.
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.shd
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+This file contains details of the shadow casting, back and receiving surfaces for the building. The [Engineering Reference](file:///E:\Docs4PDFs\EngineeringReference.pdf) explains the shadowing calculations in more detail; this report file merely shows the level of interactions that the calculations will use. The report shows the Solar Distribution algorithm (in the example Full Interior and Exterior) and then proceeds to illustrate which surfaces shade (possibly) which other surfaces.
+\end{lstlisting}
+
+\begin{lstlisting}
+Note, a casting surface -- a shadow casting surface or general casting surface (so called in the file) -- is one that casts a shadow on other surfaces. A receiving surface - a shadow receiving surface -- is one that receives shadows from other surfaces (i.e. casting surfaces). A back surface -- an inside surface -- is one that may be partially sunlit/receive solar transmission for interior solar distribution.
+\end{lstlisting}
+
+\begin{lstlisting}
+An example follows:
+\end{lstlisting}
+
+\begin{lstlisting}
+Shadowing Combinations
+\end{lstlisting}
+
+\begin{lstlisting}
+..Solar Distribution = FullInteriorAndExterior
+\end{lstlisting}
+
+\begin{lstlisting}
+  = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = ZN001:WALL001 is used as Receiving Surface in calculations.
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of general casting surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of back surfaces =            5
+\end{lstlisting}
+
+\begin{lstlisting}
+ ...Surface = ZN001:WALL002
+\end{lstlisting}
+
+\begin{lstlisting}
+ ...Surface = ZN001:WALL003
+\end{lstlisting}
+
+\begin{lstlisting}
+ ...Surface = ZN001:WALL004
+\end{lstlisting}
+
+\begin{lstlisting}
+ ...Surface = ZN001:FLR001
+\end{lstlisting}
+
+\begin{lstlisting}
+ ...Surface = ZN001:ROOF001
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of receiving sub surfaces =            1
+\end{lstlisting}
+
+\begin{lstlisting}
+ ....Surface = ZN001:WALL001:WIN001
+\end{lstlisting}
+
+\begin{lstlisting}
+  = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = ZN001:WALL001:WIN001 is not used as Receiving Surface in calculations.
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of general casting surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of back surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of receiving sub surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+  = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = ZN001:WALL002 is used as Receiving Surface in calculations.
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of general casting surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of back surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of receiving sub surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+  = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = ZN001:WALL003 is not used as Receiving Surface in calculations.
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of general casting surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of back surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of receiving sub surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+  = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = ZN001:WALL004 is not used as Receiving Surface in calculations.
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of general casting surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of back surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of receiving sub surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+  = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = ZN001:FLR001 is not used as Receiving Surface in calculations.
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of general casting surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of back surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of receiving sub surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+  = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = = =
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = ZN001:ROOF001 is used as Receiving Surface in calculations.
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of general casting surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of back surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+ Number of receiving sub surfaces =            0
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.sln
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+The following shows an excerpt of “lines� report (**eplusout.sln**) for a single surface. It gives the surface name and then the coordinates in the “standard� EnergyPlus fashion (that is, UpperLeftCorner first and proceeding around, in this case, the four vertices in the surface.
+\end{lstlisting}
+
+\begin{lstlisting}
+SPACE1-1:MAIN SOUTH OVERHANG
+\end{lstlisting}
+
+\begin{lstlisting}
+     -0.65,     -1.13,      2.20,      0.00,      0.00,      2.20
+\end{lstlisting}
+
+\begin{lstlisting}
+      0.00,      0.00,      2.20,     17.15,     -9.90,      2.20
+\end{lstlisting}
+
+\begin{lstlisting}
+     17.15,     -9.90,      2.20,     16.50,    -11.03,      2.20
+\end{lstlisting}
+
+\begin{lstlisting}
+     16.50,    -11.03,      2.20,     -0.65,     -1.13,      2.20
+\end{lstlisting}
+
+\begin{lstlisting}
+The following shows an excerpt of “lines, IDF� report (**eplusout.sln**) for a single surface. It gives the coordinates in the “standard� EnergyPlus fashion (that is, UpperLeftCorner first and proceeding around, in this case, the four vertices in the surface. Note that this is NOT a complete description of the surface but enough to change your IDF file, if you want to.
+\end{lstlisting}
+
+\begin{lstlisting}
+Building North Axis = 0
+\end{lstlisting}
+
+\begin{lstlisting}
+GlobalGeometryRules,UpperLeftCorner,CounterClockwise,WorldCoordinates;
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = SHADING, Name = ROOMSOUTH SURF6-VFIN1-6
+\end{lstlisting}
+
+\begin{lstlisting}
+  4,  !- Number of (X,Y,Z) groups in this surface
+\end{lstlisting}
+
+\begin{lstlisting}
+      -23.34,    -14.85,      2.41,  !- X,Y,Z = = > Vertex 1
+\end{lstlisting}
+
+\begin{lstlisting}
+      -23.34,    -14.76,      2.49,  !- X,Y,Z = = > Vertex 2
+\end{lstlisting}
+
+\begin{lstlisting}
+      -18.13,    -14.76,      2.49,  !- X,Y,Z = = > Vertex 3
+\end{lstlisting}
+
+\begin{lstlisting}
+      -18.13,    -14.85,      2.41;  !- X,Y,Z = = > Vertex 4
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = WALL, Name = ROOMNORTH SURF3-1
+\end{lstlisting}
+
+\begin{lstlisting}
+  4,  !- Number of (X,Y,Z) groups in this surface
+\end{lstlisting}
+
+\begin{lstlisting}
+      -15.94,     -5.34,      3.00,  !- X,Y,Z = = > Vertex 1
+\end{lstlisting}
+
+\begin{lstlisting}
+      -15.94,     -5.34,      0.00,  !- X,Y,Z = = > Vertex 2
+\end{lstlisting}
+
+\begin{lstlisting}
+      -18.91,     -5.34,      0.00,  !- X,Y,Z = = > Vertex 3
+\end{lstlisting}
+
+\begin{lstlisting}
+      -18.91,     -5.34,      3.00;  !- X,Y,Z = = > Vertex 4
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = WALL, Name = ROOMNORTH SURF4-1
+\end{lstlisting}
+
+\begin{lstlisting}
+  4,  !- Number of (X,Y,Z) groups in this surface
+\end{lstlisting}
+
+\begin{lstlisting}
+      -18.91,     -5.34,      3.00,  !- X,Y,Z = = > Vertex 1
+\end{lstlisting}
+
+\begin{lstlisting}
+      -18.91,     -5.34,      0.00,  !- X,Y,Z = = > Vertex 2
+\end{lstlisting}
+
+\begin{lstlisting}
+      -22.65,     -5.34,      0.00,  !- X,Y,Z = = > Vertex 3
+\end{lstlisting}
+
+\begin{lstlisting}
+      -22.65,     -5.34,      3.00;  !- X,Y,Z = = > Vertex 4
+\end{lstlisting}
+
+\begin{lstlisting}
+ Surface = WINDOW, Name = ROOMNORTH SURF5-1-NOSHADE
+\end{lstlisting}
+
+\begin{lstlisting}
+  4,  !- Number of (X,Y,Z) groups in this surface
+\end{lstlisting}
+
+\begin{lstlisting}
+      -19.02,     -5.34,      2.59,  !- X,Y,Z = = > Vertex 1
+\end{lstlisting}
+
+\begin{lstlisting}
+      -19.02,     -5.34,      0.41,  !- X,Y,Z = = > Vertex 2
+\end{lstlisting}
+
+\begin{lstlisting}
+      -22.54,     -5.34,      0.41,  !- X,Y,Z = = > Vertex 3
+\end{lstlisting}
+
+\begin{lstlisting}
+      -22.54,     -5.34,      2.59;  !- X,Y,Z = = > Vertex 4
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.sql
+------------
+\end{lstlisting}
+
+\begin{lstlisting}
+eplusout.sql is an optional output format for EnergyPlus. The eplusout.sql output file is a sqlite3 database file (see http://www.sqlite.org) and includes all of the data found in EnergyPlus’ eplustbl.\* files, eplusout.eso and eplusout.mtr output files (i.e., EnergyPlus’ standard variable and meter output files) plus a number of reports that are found in the eplusout.eio output file.
+\end{lstlisting}
+
+\begin{lstlisting}
+A discussion of the individual data tables is presented below followed by a discussion about how to access data within the SQL file.
+\end{lstlisting}
+
+\begin{lstlisting}
+### List of Available SQLite Tables
+\end{lstlisting}
+
+\begin{lstlisting}
+This initial release of the SQL database output option includes a variety of data in the following tables:
+\end{lstlisting}
+
+\begin{lstlisting}
+- ComponentSizes Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- ConstructionLayers Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- Constructions Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- Materials Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- NominalBaseboardHeaters Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- NominalElectricEquipment Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- NominalGasEquipment Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- NominalHotWaterEquipment Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- NominalInfiltration Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- NominalLighting Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- NominalOtherEquipment Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- NominalPeople Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- NominalSteamEquipment Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- NominalVentilation Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- ReportData Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- ReportDataDictionary Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- ReportExtendedData Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- RoomAirModels Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- Schedules Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- Surfaces Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- SystemSizes Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- Time Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- ZoneGroups Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- Zones Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- ZoneLists Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- ZoneSizes Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- ZoneInfoLists Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- [Simulations](#_Simulations_Table_1)Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- [EnvironmentPeriods](#_EnvironmentPeriods_Table)Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- TabularData Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- [Strings](#_Strings_Table)Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- [StringTypes](#_StringTypes_Table)Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- [TabularDataWithStrings](#_TabularDataWithStrings_Table)Table
+\end{lstlisting}
+
+\begin{lstlisting}
+- Errors Table
+\end{lstlisting}
+
+\begin{lstlisting}
+A short discussion of contents of each of the above SQL tables is given in the sections that follow.
+\end{lstlisting}
+
+\begin{lstlisting}
+### Report Data
+\end{lstlisting}
+
+\begin{lstlisting}
+Data in the following four tables are also found in EnergyPlus’ standard output file (i.e., eplusout.eso – see that section for more information) or in EnergyPlus' eplusout.mtr (i.e. meter) output file. As with the standard output file, the “Report Variable� and “Report Meter� commands control the data in these tables.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### ReportDataDictionary Table
+\end{lstlisting}
+
+\begin{lstlisting}
+The ReportDataDictionary table provides the equivalent of the dictionary portion of the ESO file (i.e., the first section of the .eso file) or eplusout.mtr. Please see the Report Variable section of the Input-Output Reference for more information.  Like in the eplusout.mtr file (see the eplusout.mtr section), only data requested by "Report Meter" commands will set isMeter to 1 or True.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+#### ReportData Table
+\end{lstlisting}
+
+\begin{lstlisting}
+The ReportData table contains the report or meter variable data (e.g., the hourly, daily, and monthly report variable data). Please see the Report Variable section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+#### ReportExtendedData Table
+\end{lstlisting}
+
+\begin{lstlisting}
+The ReportExtendedData table contains additional data (e.g., monthly maximums and minimums) that is available for certain report or meter variables.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+#### Time Table
+\end{lstlisting}
+
+\begin{lstlisting}
+The Time table provides the time information for both the “report variable� and “report meter� variables (the ReportData table).
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+### One time (EIO) File Data
+\end{lstlisting}
+
+\begin{lstlisting}
+Data in the tables below can also be found in EnergyPlus input output file (i.e., in the eplusout.eio output file).
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Zones Table
+\end{lstlisting}
+
+\begin{lstlisting}
+The Zones table provides a variety of information about the zones specified within EnergyPlus. One of its most common uses is to provide zone name and area information for the other tables within the SQL database (e.g., use the ZoneIndex to look up the ZoneName).
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Zone object in the Group-Thermal Zone Description/Geometry section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### NominalPeople Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the NominalPeople SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the People object in the Group-Internal Gains section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### NominalLighting Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the NominalLighting SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the LIGHTS object in the Group-Internal Gains section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### NominalElectricEquipment Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the NominalElectricEquipment SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Electric Equipment object in the Group-Internal Gains section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### NominalGasEquipment Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the NominalGasEquipment SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Gas Equipment object in the Group-Internal Gains section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### NominalSteamEquipment Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the NominalSteamEquipment SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Steam Equipment object in the Group-Internal Gains section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### NominalHotWaterEquipment Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the NominalHotWaterEquipment SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Hot Water Equipment object in the Group-Internal Gains section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### NominalOtherEquipment Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the NominalOtherEquipment SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Other Equipment object in the Group-Internal Gains section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### NominalBaseboardHeaters Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the NominalBaseboardHeaters SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Baseboard Heat object in the Group-Internal Gains section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### NominalInfiltration Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the NominalInfiltration SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Infiltration object in the Group-Airflow section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### NominalVentilation Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the NominalVentilation SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Ventilation object in the Group-Airflow section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Surfaces Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the Surfaces SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Surface(s) object in the Group-Thermal Zone Description/Geometry section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Constructions Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the Constructions SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Construction object in the Group-Surface Construction Elements section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### ConstructionLayers Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the ConstructionLayers SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Construction object in the Group-Surface Construction Elements section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Materials Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the Materials SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Materials object in the Group-Surface Construction Elements section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### RoomAirModels Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the RoomAirModels SQL table is shown below. Please see the Group-RoomAir Models section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+#### ComponentSizes Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the ComponentSizes SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Sizing object in the Group-Design Objects section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### SystemSizes Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the SystemSizes SQL table is shown below. Please see the System Sizing object in the Group-Design Objects section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+#### ZoneSizes Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the ZoneSizes SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Zone Sizing object in the Group-Design Objects section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### ZoneGroups Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the ZoneGroups SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Zone Group object in the Group-Thermal Zone Description/Geometry section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### ZoneLists Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the ZoneLists SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Zone List object in the Group-Thermal Zone Description/Geometry section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### ZoneInfoZoneLists Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the ZoneInfoZoneLists SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+This is a join table to represent the many-to-many relationship of zones and zone lists.  ZoneListIndex and ZoneIndex together are the Primary Key for this table.
+\end{lstlisting}
+
+\begin{lstlisting}
+### Miscellaneous Tables
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Schedules Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the Schedules SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+Please see the Group-Schedules section of the Input-Output Reference for more information.
+\end{lstlisting}
+
+\begin{lstlisting}
+#### Simulations Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the Simulations SQL table is shown below.  Currently there will only be one record in the table, because the SQLite database is relevant to only one simulation.  In the future this might change if multiple simulations are aggregated into a larger database.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+#### EnvironmentPeriods Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the EnvironmentPeriods SQL table is shown below.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+#### TabularData Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the TabularData SQL table is shown below.   The TabularData table is only output when the “SimpleAndTabular� choice is made in the Output:SQLite object.  The TabularData table contains all of the tabular report information that is typically output to one of the formats controlled by the OutputControl:Table:Style object.  This is a generic way of dumping all of the existing tabular reports to the SQLite database.  This table has many references to the companion Strings table.  The Strings table simply associates strings to an integer value for space efficiency of the database.  Tabular data is easier to query from the TabularDataWithStrings table, which is implemented as a database view that joins this table with the Strings table.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+#### Strings Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the Strings SQL table is shown below. The Strings table is only output when the “SimpleAndTabular� choice is made in the Output:SQLite object.  The Strings table simply associates strings with integers to save space in the database.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+#### StringTypes Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the StringTypes SQL table is shown below. The StringTypes table is only output when the “SimpleAndTabular� choice is made in the Output:SQLite object.
+\end{lstlisting}
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{lstlisting}
+#### TabularDataWithStrings Table
+\end{lstlisting}
+
+\begin{lstlisting}
+An overview of the TabularDataWithStrings SQL table is shown below.  This table is implemented as a view of other tables and is not actually a table in the database.  This view is similar to the TabularData table except text strings are directly available in place of foreign keys to the Strings table.   The TabularDataWithStrings view is only created when the “SimpleAndTabular� choice is made in the Output:SQLite object.
+\end{lstlisting}
+
+\begin{lstlisting}
+An example of a SQL query to get a table out of the AnnualBuildingUtilityPerformanceSummary report is the following.
+\end{lstlisting}
+
+select * FROM TabularDataWithStrings WHERE ReportName = `AnnualBuildingUtilityPerformanceSummary' and TableName = `Site and Source Energy'; ````
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{Errors Table}\label{errors-table}
+
+The Errors SQL table reports errors and warnings for the simulation.~ The content of this table includes most of the content of the error file.~ However, it does not contain purely informational messages (e.g.~not warnings or errors) and some of the error summary statistics which may be readily computed. Users should be aware that errors experienced while processing input cause EnergyPlus to exit before the SQLite output database has been initialized.~ This is because the Output:SQLite object must be parsed from the input to request the database.~ Therefore, failures in input processing are indicated by the absence of a SQLite output file.~ The regular error or audit files must be used to identify the erroneous input objects in this case.~ Because each error or warning message is expected to be unique these messages are stored directly in the Errors table and not in the Strings table.
+
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{2.99in}}
+\caption{Table 42. SQL Errors Table Contents \label{table:table-42.-sql-errors-table-contents}} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Table 42. SQL Errors Table Contents} \tabularnewline
+\toprule 
+Field Name & Field Type & Description \tabularnewline
+\midrule
+\endhead
+
+ErrorIndex & INTEGER PRIMARY KEY & The index of the error or warning message. \tabularnewline
+SimulationIndex & INTEGER FOREIGN KEY & The simulation the error or warning pertains to. \tabularnewline
+ErrorType & INTEGER & Type of error or warning 0=Warning, 1=Severe, 2=Fatal. \tabularnewline
+ErrorMessage & TEXT & The text of the error message. \tabularnewline
+Count & INTEGER & Number of times that the error was repeated.~ This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated. \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{How to Access the SQLite Data}\label{how-to-access-the-sqlite-data}
+
+The SQL database can be accessed in a number of ways, including via the command line, through ODBC, or through as SQLite's API interface. SQLite uses the industry standard SQL 92 language.
+
+\subsubsection{Command Line}\label{command-line}
+
+One of the simplest ways to access the data in the SQL database is by way of the SQL command line tool (i.e., sqlite3). A brief description of how to use sqlite3 for each computing platform is given below.
+
+\subsubsection{Windows XP and Windows Vista}\label{windows-xp-and-windows-vista}
+
+While Windows does not ship with sqlite3 installed, the sqlite3 binary can be downloaded from the SQLite webpage (www.sqlite.org/download.html). After downloading the precompiled binary, install it in the EnergyPlus directory.
+
+Once the sqlite3 executable is installed, access the program from the command line by typing ``sqlite3'' at the DOS prompt.
+
+\subsubsection{Linux}\label{linux}
+
+The sqlite3 command line tool comes preinstalled on a number of more recent Linux releases. To see if sqlite3 is available (and which version is installed), type ``sqlite3 --version'' from the command line. If sqlite3 is not installed, the sqlite3 binary, as well as source code, can be downloaded from the SQLite webpage (http://www.sqlite.org/download.html) and installed in the directory of your choice.
+
+\subsubsection{Macintosh OS X}\label{macintosh-os-x}
+
+The sqlite3 program comes standard on MacOS X 10.5. From the command line, type ``sqlite3 --version'' to see which version of sqlite3 is installed.~ In order to access the database created by EnergyPlus, version 3 or later is required.
+
+\subsubsection{Accessing the Data from the Command Line}\label{accessing-the-data-from-the-command-line}
+
+Once it has been confirmed that SQLite3 is installed on your machine, the SQL database can be accessed by typing:
+
+\begin{lstlisting}
+sqlite3 <database name>
+\end{lstlisting}
+
+at the command line, where \textless{}database name \textgreater{} is the name of the SQL database (e.g., sqlite3 eplusout.sql).
+
+The sqlite.org \href{http://www.sqlite.org/sqlite.html}{website} gives examples of how sqlite3 can be used to access and output data in various formats.
+
+\subsubsection{ODBC}\label{odbc}
+
+ODBC allows access to the SQL database from a variety of programs, including Microsoft Excel, Microsoft Access, and FileMaker. How to install and use ODBC drivers is outside the scope of this document, and more information can be found at the following websites:
+
+Macintosh ODBC drivers:
+
+http://www.actualtechnologies.com/
+
+Windows and Linux ODBC information and drivers:
+
+http://www.sqlite.org/cvstrac/wiki?p = SqliteOdbc
+
+http://www.ch-werner.de/sqliteodbc/
+
+\subsubsection{API}\label{api}
+
+Sqlite3 includes a rich C++ API (detailed on the SQLite website \href{http://www.sqlite.org/cintro.html}{www.sqlite.org/cintro.html}), and wrappers for the API interface are available in a variety of programming languages, including Fortran, TCL, and Ruby (see \href{http://www.sqlite.org/cvstrac/wiki?p\%20=\%20SqliteWrappers}{www.sqlite.org/cvstrac/wiki?p = SqliteWrappers} for more information).
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-lt-ext-gt.tex b/doc/output-details-and-examples/src/output-files/eplusout-lt-ext-gt.tex
new file mode 100644
index 00000000000..6fdad768ac4
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-lt-ext-gt.tex
@@ -0,0 +1,3 @@
+\section{eplusout.\textless{}ext\textgreater{}}\label{eplusout.ext}
+
+The eplusout.csv (or txt or tab extension) is a file that can be produced by post-processing on the eplusout.eso file. EnergyPlus distributes a post-processing program (ReadVarsESO -- see next section) with the installation.
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-sci.tex b/doc/output-details-and-examples/src/output-files/eplusout-sci.tex
new file mode 100644
index 00000000000..eec553eb0b2
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-sci.tex
@@ -0,0 +1,29 @@
+\section{eplusout.sci}\label{eplusout.sci}
+
+This is the surface cost information report. This report file is obtained by including the following in the input file:
+
+\textbf{Output:Surfaces:List, CostInfo;}
+
+The intent is to make available a separate file that lists the unique surfaces and their construction types for potential use in external calculations that need to estimate the cost of construction. Note that such cost estimating can now also be performed internal to EnergyPlus using Cost Estimate objects. The listing can also be used to check that the input for surfaces is producing the expected areas (although the DXF is probably more useful for such checking).
+
+The output file contains a list of the unique surfaces and their net and gross areas. The area information is calculated by EnergyPlus from the vertices entered for individual surfaces. The net area is the area remaining after the areas of subsurfaces are subtracted. The file contains six columns of comma-separate-data as shown in the following table:
+
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\toprule 
+Column & Description \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+Column & Description \tabularnewline
+\midrule
+\endhead
+
+1 & Integer counter for surfaces. The surfaces are listed in the order that they are stored internally in EnergyPlus. Note that in this report, the algorithms sort out and exclude duplicate surfaces that are entered for the interior partitions between adjacent thermal zones. Therefore the list is usually not consecutive. \tabularnewline
+2 & The name of the surface entered by the user \tabularnewline
+3 & The name of the construction for the surface entered by the user \tabularnewline
+4 & The type of the surface (e.g. wall, roof, floor, window …) \tabularnewline
+5 & The net area of the surface in m \tabularnewline
+6 & The gross area of the surface in m \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-svg.tex b/doc/output-details-and-examples/src/output-files/eplusout-svg.tex
new file mode 100644
index 00000000000..603e6892c16
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-svg.tex
@@ -0,0 +1,123 @@
+\section{eplusout.svg}\label{eplusout.svg}
+
+This is a Scalable Vector Graphics (SVG) file that shows a diagram of the HVAC system from the inputs of the simulation. The diagram is generated for most HVAC systems but a few valid HVAC configurations cannot be displayed correctly. The SVG file is generated by the HVAC Diagram utility that is included with EnergyPlus and is run automatically when using EP-Launch.
+
+The SVG format is a graphics format that includes a descriptions of lines, boxes, text, etc. set in a two dimensional perspective. To learn more about the SVG format see:
+
+http://www.w3.org/Graphics/SVG/
+
+Several viewers are available so that you can view these files including plug-ins for Internet Explorer by Adobe and Corel. The Adobe SVG plug in can be found at:
+
+http://www.adobe.com/svg/viewer/install/
+
+But many different viewers are available and links are shown at:
+
+http://www.svgi.org/
+
+An example of a diagram generated by HVAC Diagram is shown
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image023.jpg}
+\caption{}
+\end{figure}
+
+A close up of one part of this diagram is shown below
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image024.jpg}
+\caption{}
+\end{figure}
+
+The SVG file format is an XML based format so it is text based. The diagram shown above is shown below in text (reduced).
+
+\textless{}?xml version = ``1.0'' standalone = ``no''?\textgreater{}
+
+\textless{}!DOCTYPE svg\textgreater{}
+
+\textless{}svg width = ``250mm'' height = ``200mm'' viewBox = ``0 0~~ 3200~~~ 1500'' xmlns:ev = ``http://www.w3.org/2001/xml-events'' xmlns:xlink = ``http://www.w3.org/1999/xlink'' xmlns = ``http://www.w3.org/2000/svg'' preserveAspectRatio = ``xMidYMid meet'' zoomAndPan = ``magnify''\textgreater{}
+
+\textless{}g font-family = ``Verdana'' font-size = ``8''\textgreater{}
+
+~ \textless{}line x1 = ``~ 2400'' y1 = ``~~ 470'' x2 = ``~ 2100'' y2 = ``~~~ 30'' style = ``stroke:linen ;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 2400'' y1 = ``~~ 510'' x2 = ``~ 2100'' y2 = ``~~~ 70'' style = ``stroke:linen ;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 2400'' y1 = ``~~ 550'' x2 = ``~ 2100'' y2 = ``~~ 110'' style = ``stroke:linen ;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 2400'' y1 = ``~~ 590'' x2 = ``~ 2100'' y2 = ``~~ 150'' style = ``stroke:linen ;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 2400'' y1 = ``~~ 630'' x2 = ``~ 2100'' y2 = ``~~ 190'' style = ``stroke:linen ;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 2400'' y1 = ``~~ 670'' x2 = ``~~ 900'' y2 = ``~~~ 30'' style = ``stroke:linen ;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 2050'' y1 = ``~~ 830'' x2 = ``~~ 600'' y2 = ``~~~ 30'' style = ``stroke:linen ;''/\textgreater{}
+
+~ \textless{}line x1 = ``~~ 300'' y1 = ``~~~ 30'' x2 = ``~~ 550'' y2 = ``~~ 950'' style = ``stroke:linen ;''/\textgreater{}
+
+~ \textless{}line x1 = ``~~ 800'' y1 = ``~~ 790'' x2 = ``~ 2050'' y2 = ``~~ 310'' style = ``stroke:linen ;''/\textgreater{}
+
+~ \textless{}rect x = ``~~ 200'' y = ``~~ 940'' width = ``~~ 200'' height = ``~~~ 20'' style = ``fill:snow; stroke: Black;''/\textgreater{}~~~ ~1
+
+~ \textless{}text x = ``~~ 202'' y = ``~~ 953'' startOffset = ``0''\textgreater{}OUTSIDE AIR INLET NODE LIST\textless{}/text\textgreater{}
+
+~ \textless{}rect x = ``~ 2300'' y = ``~~~ 20'' width = ``~~ 200'' height = ``~~~ 20'' style = ``fill:chartreuse; stroke: Black;''/\textgreater{}~~~~ 2
+
+~ \textless{}text x = ``~ 2302'' y = ``~~~ 33'' startOffset = ``0''\textgreater{}ZN1\_S\_SPACE\_1\textless{}/text\textgreater{}
+
+~ \textless{}rect x = ``~ 1400'' y = ``~~~ 20'' width = ``~~ 200'' height = ``~~~ 20'' style = ``fill:wheat; stroke: Black;''/\textgreater{}~~~~ 7
+
+~ \textless{}text x = ``~ 1402'' y = ``~~~ 33'' startOffset = ``0''\textgreater{}VAV SYS 1 ZONE SPLITTER\textless{}/text\textgreater{}
+
+~ \textless{}rect x = ``~ 1700'' y = ``~~~ 20'' width = ``~~ 200'' height = ``~~~ 20'' style = ``fill:wheat; stroke: Black;''/\textgreater{}~~~~ 8
+
+~ \textless{}text x = ``~ 1702'' y = ``~~~ 33'' startOffset = ``0''\textgreater{}ZN1\_S\_SPACE\_1 VAV REHEAT\textless{}/text\textgreater{}
+
+\textless{}reduced\textgreater{}
+
+~ \textless{}line x1 = ``~ 1600'' y1 = ``~~~ 30'' x2 = ``~ 1700'' y2 = ``~~~ 30'' style = ``stroke: Black;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 1600'' y1 = ``~~~ 30'' x2 = ``~ 1700'' y2 = ``~~~ 70'' style = ``stroke: Black;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 1600'' y1 = ``~~~ 30'' x2 = ``~ 1700'' y2 = ``~~ 110'' style = ``stroke: Black;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 1600'' y1 = ``~~~ 30'' x2 = ``~ 1700'' y2 = ``~~ 150'' style = ``stroke: Black;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 1600'' y1 = ``~~~ 30'' x2 = ``~ 1700'' y2 = ``~~ 190'' style = ``stroke: Black;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 1900'' y1 = ``~~~ 30'' x2 = ``~ 2000'' y2 = ``~~~ 30'' style = ``stroke: Black;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 1900'' y1 = ``~~~ 70'' x2 = ``~ 2000'' y2 = ``~~~ 70'' style = ``stroke: Black;''/\textgreater{}
+
+~ \textless{}line x1 = ``~ 1900'' y1 = ``~~ 110'' x2 = ``~ 2000'' y2 = ``~~ 110'' style = ``stroke: Black;''/\textgreater{}
+
+\textless{}reduced\textgreater{}
+
+~ \textless{}text x = ``~~ 200'' y = ``~ 1000'' startOffset = ``0''\textgreater{}Unused Non-Parent Objects:\textless{}/text\textgreater{}
+
+~ \textless{}text x = ``~~ 220'' y = ``~ 1020'' startOffset = ``0''\textgreater{}VAV SYS 1 SUPPLY AIR TEMP MANAGER\textless{}/text\textgreater{}
+
+~ \textless{}text x = ``~~ 220'' y = ``~ 1040'' startOffset = ``0''\textgreater{}VAV SYS 1 HEATING COIL AIR TEMP MANAGER\textless{}/text\textgreater{}
+
+~ \textless{}text x = ``~~ 220'' y = ``~ 1060'' startOffset = ``0''\textgreater{}CHILLER PLANT CHW TEMP MANAGER\textless{}/text\textgreater{}
+
+~ \textless{}text x = ``~~ 220'' y = ``~ 1080'' startOffset = ``0''\textgreater{}BOILER PLANT HW TEMP MANAGER\textless{}/text\textgreater{}
+
+~ \textless{}text x = ``~~ 220'' y = ``~ 1100'' startOffset = ``0''\textgreater{}VAV SYS 1 COOLING COIL AIR TEMP MANAGER\textless{}/text\textgreater{}
+
+~ \textless{}text x = ``~~ 220'' y = ``~ 1120'' startOffset = ``0''\textgreater{}VAV SYS 1 MIXED AIR TEMP MANAGER\textless{}/text\textgreater{}
+
+~ \textless{}text x = ``~~ 220'' y = ``~ 1140'' startOffset = ``0''\textgreater{}VAV SYS 1 COOLING COIL CONTROLLER\textless{}/text\textgreater{}
+
+~ \textless{}text x = ``~~ 220'' y = ``~ 1160'' startOffset = ``0''\textgreater{}VAV SYS 1 HEATING COIL CONTROLLER\textless{}/text\textgreater{}
+
+~ \textless{}text x = ``~~ 220'' y = ``~ 1180'' startOffset = ``0''\textgreater{}VAV SYS 1 OA CONTROLLER\textless{}/text\textgreater{}
+
+~ \textless{}text x = ``~~ 200'' y = ``~ 1220'' startOffset = ``0''\textgreater{}
+
+The following are not supported:~ objects related to controls, DIRECT AIR, or~ PURCHASED AIR\textless{}/text\textgreater{}
+
+\textless{}/g\textgreater{}
+
+\textless{}/svg\textgreater{}
diff --git a/doc/output-details-and-examples/src/output-files/eplusout-wrl.tex b/doc/output-details-and-examples/src/output-files/eplusout-wrl.tex
new file mode 100644
index 00000000000..4fbd8f074aa
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusout-wrl.tex
@@ -0,0 +1,101 @@
+\section{eplusout.wrl}\label{eplusout.wrl}
+
+The VRML output report file is formatted according to the ``Virtual Reality Modeling Language'' standard rules for representing building type surfaces. The file can be used in several inexpensive, shareware or freeware viewers. There are a variety of stand alone and viewers integrated within browsers. A good list of viewers can be found at:
+
+http://cic.nist.gov/vrml/vbdetect.html
+
+This site detects what, if any, VRML plugin is installed in your browser as well as gives a list of active ones with links to their sites.
+
+This file is generated when the following line is included in the IDF.
+
+\textbf{Output:Surfaces:Drawing, VRML;}
+
+In addition, like the DXF output, you can ask it to triangulate (algorithm within EnergyPlus) surfaces with \textgreater{}4 sides:
+
+\textbf{Output:Surfaces:Drawing, VRML, Triangulate 3dface;}
+
+Most viewers will illustrate a solid model by default:
+
+\begin{figure}[hbtp] % fig 10
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image025.jpg}
+\caption{VRML output - solid model \protect \label{fig:vrml-output-solid-model}}
+\end{figure}
+
+With some/many viewers, you can also see a wireframe model; some will even fill this model. Also, viewers can triangulate any surface that isn't labeled as ``convex'' by the software writing the file (i.e.~EnergyPlus). However, this triangulation may not be correct so you may wish to do it from within EnergyPlus as illustrated above.
+
+A wireframe model of the same building as above is:
+
+\begin{figure}[hbtp] % fig 11
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image026.jpg}
+\caption{VRML output - wireframe model \protect \label{fig:vrml-output-wireframe-model}}
+\end{figure}
+
+The actual file produced is a text file. EnergyPlus adds some comments, such as the list of zone names and surface names before each coordinate specification. The line/solid colors are set as Floor, Wall, etc. so the file is somewhat readable.
+
+\begin{lstlisting}
+#VRML V2.0 utf8
+WorldInfo {
+   title "Building - Building"
+   info ["EnergyPlus Program Version EnergyPlus <version>, 9/14/2006 1:31 PM"]
+}
+# Zone Names
+# Zone = 1:PLENUM-1
+# Zone = 2:SPACE1-1
+# Zone = 3:SPACE2-1
+# Zone = 4:SPACE3-1
+# Zone = 5:SPACE4-1
+# Zone = 6:SPACE5-1
+Shape {
+appearance DEF FLOOR Appearance {
+material Material { diffuseColor 0.502 0.502 0.502 }
+}
+}
+\end{lstlisting}
+
+\begin{lstlisting}
+# PLENUM-1:WALL-1PF
+Shape {
+appearance USE WALL
+geometry IndexedFaceSet {
+solid TRUE
+coord DEF Surf5 Coordinate {
+point [
+        0.00000         0.00000         3.00000,
+        0.00000         0.00000         2.40000,
+       26.41377       -15.25000         2.40000,
+       26.41377       -15.25000         3.00000,
+]
+}
+coordIndex [
+ 0 1 2 3 -1
+]
+ccw TRUE
+solid TRUE
+}
+}
+\end{lstlisting}
+
+\begin{lstlisting}
+# PLENUM-1:WALL-1PR
+Shape {
+appearance USE WALL
+geometry IndexedFaceSet {
+solid TRUE
+coord DEF Surf6 Coordinate {
+point [
+       26.41377       -15.25000         3.00000,
+       26.41377       -15.25000         2.40000,
+       34.01377        -2.08641         2.40000,
+       34.01377        -2.08641         3.00000,
+]
+}
+coordIndex [
+ 0 1 2 3 -1
+]
+ccw TRUE
+solid TRUE
+}
+}
+\end{lstlisting}
diff --git a/doc/output-details-and-examples/src/output-files/eplusscreen-csv.tex b/doc/output-details-and-examples/src/output-files/eplusscreen-csv.tex
new file mode 100644
index 00000000000..47d42ca2cb3
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusscreen-csv.tex
@@ -0,0 +1,9 @@
+\section{eplusscreen.csv}\label{eplusscreen.csv}
+
+Results of the window screen transmittance map. This file can be used to create a 3-D Column chart for graphically viewing the direct beam and reflected beam transmittance at various relative azimuth and relative altitude angles. The ``relative'' angles in this file are the incident solar angles with respect to the outward surface normal. The figures below are example 3-D charts generated using the data provided in this output file.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image022.jpg}
+\caption{TransmittancePlotExample}
+\end{figure}
diff --git a/doc/output-details-and-examples/src/output-files/eplusssz-lt-ext-gt.tex b/doc/output-details-and-examples/src/output-files/eplusssz-lt-ext-gt.tex
new file mode 100644
index 00000000000..acabe410ad0
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplusssz-lt-ext-gt.tex
@@ -0,0 +1,91 @@
+\section{eplusssz.\textless{}ext\textgreater{}}\label{eplusssz.ext}
+
+This file is the result of the system sizing calculation. As usual, the file can be read into a spreadsheet for easy viewing. System Sizing (see Sizing:System object) performs a special calculation that, to oversimplify, sums up the results of the zone sizing calculation and saves the results in the system sizing arrays for reporting on component size requirements.
+
+An excerpt of the file:
+
+Time,:Des Heat Mass Flow {[}kg/s{]},:Des Cool Mass Flow {[}kg/s{]},:Des Heat Cap {[}W{]},:Des Sens Cool Cap {[}W{]},
+
+00:15:00,1.063942E+00,0.000000E+00,5.944201E+03,0.000000E+00,
+
+00:30:00,1.063942E+00,0.000000E+00,5.944201E+03,0.000000E+00,
+
+00:45:00,1.063942E+00,0.000000E+00,5.944201E+03,0.000000E+00,
+
+01:00:00,1.063942E+00,0.000000E+00,5.944201E+03,0.000000E+00,
+
+01:15:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+01:30:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+01:45:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+02:00:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+02:15:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+02:30:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+02:45:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+03:00:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+03:15:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+03:30:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+03:45:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+04:00:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+04:15:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+04:30:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+04:45:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+05:00:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+05:15:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
+
+05:30:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00, = = = reduced for brevity = = =
+
+Coinc Peak~~ ,1.063943E+00,1.378986E+00,5.944199E+03,2.165922E+04,
+
+NonCoinc Peak,1.063943E+00,1.553319E+00,5.944199E+03,2.165922E+04,
+
+\subsubsection{Field: Time}\label{field-time}
+
+Calculation time -- this will show the time steps used by the simulation and by the sizing calculation.
+
+\subsubsection{Field: Des Heat Mass Flow {[}kg/s{]}}\label{field-des-heat-mass-flow-kgs}
+
+Calculated design heating mass flow rate.
+
+\subsubsection{Field: Des Cool Mass Flow {[}kg/s{]}}\label{field-des-cool-mass-flow-kgs}
+
+Calculated design cooling mass flow rate.
+
+\subsubsection{Field: Des Heat Cap {[}W{]}}\label{field-des-heat-cap-w}
+
+Calculated design heating capacity.
+
+\subsubsection{Field: Des Sens Cool Cap {[}W{]}}\label{field-des-sens-cool-cap-w}
+
+Calculated design sensible cooling capacity.
+
+\subsubsection{Line: Coinc Peak}\label{line-coinc-peak}
+
+The values in this line only apply to the Mass Flow Rates. The coincident peak cooling mass flow rate is the maximum of the sum of the zone peak cooling mass flow rates occurring at each time step. The coincident peak heating mass flow rate is the maximum of the sum of the zone peak heating mass flow rates occurring at each time step.
+
+\subsubsection{Line: NonCoinc Peak}\label{line-noncoinc-peak}
+
+The values in this line only apply to the Mass Flow Rates. The noncoincident peak cooling mass flow rate is the sum of the zone peak cooling mass flow rates, no matter what time of day the individual zone peaks occurred. The noncoincident peak heating mass flow rate is the sum of the zone peak heating mass flow rates, no matter what time of day the individual zone peaks occurred.
+
+Or as depicted graphically:
+
+\begin{figure}[hbtp] % fig 5
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image017.png}
+\caption{System Size depiction from eplusout.ssz \protect \label{fig:system-size-depiction-from-eplusout.ssz}}
+\end{figure}
diff --git a/doc/output-details-and-examples/src/output-files/eplustbl-lt-ext-gt.tex b/doc/output-details-and-examples/src/output-files/eplustbl-lt-ext-gt.tex
new file mode 100644
index 00000000000..a3857b9186f
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/eplustbl-lt-ext-gt.tex
@@ -0,0 +1,3640 @@
+\section{eplustbl.\textless{}ext\textgreater{}}\label{eplustbl.ext}
+
+The eplustbl file contains the tabular output results that are created when using the following objects:
+
+\begin{itemize}
+\item
+  Output:Table:SummaryReports
+\item
+  Output:Table:TimeBins
+\item
+  Output:Table:Monthly
+\item
+  UtilityCost:Tariff
+\item
+  ComponentCost:Line Item
+\end{itemize}
+
+The format and the extension for the file depends on the setting of the ColumnSeparator field of the Output:Table:Style object. The choices of HTML, tab, fixed, comma, and XML result in eplustbl.htm, eplustbl.tab, eplustbl.txt, eplustbl.csv, eplustbl.xml respectively. The HTML version of the report also includes a table of contents that allows easier navigation through the file.
+
+By default the energy units reported in all of the eplustbl files are in Joules (J) but the UnitConversion field of the Output:Table:Style object allows for the values to be reported in MJ, GJ or in kWh. In addition, the Output:Table:Style object can specify for the tables to be in IP units for all fields.
+
+\subsection{Output:Table:SummaryReports}\label{outputtablesummaryreports}
+
+Several predefined reports are available from the Output:Table:SummaryReports object including the following. (spaces are inserted in names for readability; keys are included in the Input Data Dictionary or by just removing the spaces):
+
+\begin{itemize}
+\tightlist
+\item
+  All Summary
+\end{itemize}
+
+Lists all following applicable tables with ``Summary'' in the name.
+
+\begin{itemize}
+\tightlist
+\item
+  All Monthly
+\end{itemize}
+
+Lists all following applicable tables with ``Monthly'' in the name.
+
+\begin{itemize}
+\tightlist
+\item
+  All Summary And Monthly
+\end{itemize}
+
+Lists all following applicable tables with both ``Summary'' and ``Monthly'' in the name. This does not include the Zone Component Load Summary report.
+
+\begin{itemize}
+\tightlist
+\item
+  All Summary and Sizing Period
+\end{itemize}
+
+Lists the All Summary tables as well as the Zone Component Load report (currently the only Sizing Period report). Please note that the Zone Component Load report does increase the run time because it repeats sizing periods.
+
+\begin{itemize}
+\tightlist
+\item
+  All Summary Monthly and Sizing Period
+\end{itemize}
+
+Lists the All Summary tables, the Monthly tables as well as the Zone Component Load report (currently the only Sizing Period report). Please note that the Zone Component Load report does increase the run time because it repeats sizing periods.
+
+\begin{itemize}
+\item
+  Annual Building Utility Performance Summary
+\item
+  Input Verification and Results Summary
+\item
+  Demand End Use Components Summary
+\item
+  Source Energy End Use Components Summary
+\item
+  Climatic Data Summary
+\item
+  Equipment Summary
+\item
+  Envelope Summary
+\item
+  Surface Shadowing Summary
+\item
+  Shading Summary
+\item
+  Lighting Summary
+\item
+  HVAC Sizing Summary
+\item
+  System Summary
+\item
+  Component Sizing Summary
+\item
+  Outdoor Air Summary
+\item
+  Object Count Summary
+\item
+  Component Cost Economics Summary
+\item
+  Energy Meters
+\item
+  Sensible Heat Gain Summary
+\item
+  Standard 62.1 Summary
+\item
+  Zone Component Load Summary
+\item
+  Zone Cooling Summary Monthly
+\item
+  Zone Heating Summary Monthly
+\item
+  Zone Electric Summary Monthly
+\item
+  Space Gains Monthly
+\item
+  Peak Space Gains Monthly
+\item
+  Space Gain Components At Cooling Peak Monthly
+\item
+  Energy Consumption Electricity Natural Gas Monthly
+\item
+  Energy Consumption Electricity Generated Propane Monthly
+\item
+  Energy Consumption Diesel FuelOil Monthly
+\item
+  Energy Consumption District Heating Cooling Monthly
+\item
+  Energy Consumption Coal Gasoline Monthly
+\item
+  End Use Energy Consumption Electricity Monthly
+\item
+  End Use Energy Consumption NaturalGas Monthly
+\item
+  End Use Energy Consumption Diesel Monthly
+\item
+  End Use Energy Consumption FuelOil Monthly
+\item
+  End Use Energy Consumption Coal Monthly
+\item
+  End Use Energy Consumption Propane Monthly
+\item
+  End Use Energy Consumption Gasoline Monthly
+\item
+  Peak Energy End Use Electricity Part1 Monthly
+\item
+  Peak Energy End Use Electricity Part2 Monthly
+\item
+  Electric Components Of Peak Demand Monthly
+\item
+  Peak Energy End Use NaturalGas Monthly
+\item
+  Peak Energy End Use Diesel Monthly
+\item
+  Peak Energy End Use FuelOil Monthly
+\item
+  Peak Energy End Use Coal Monthly
+\item
+  Peak Energy End Use Propane Monthly
+\item
+  Peak Energy End Use Gasoline Monthly
+\item
+  Setpoints Not Met With Temperatures Monthly
+\item
+  Comfort Report Simple55 Monthly
+\item
+  Unglazed Transpired Solar Collector Summary Monthly
+\item
+  Occupant Comfort Data Summary Monthly
+\item
+  Chiller Report Monthly
+\item
+  Tower Report Monthly
+\item
+  Boiler Report Monthly
+\item
+  DX Report Monthly
+\item
+  Window Report Monthly
+\item
+  Window Energy Report Monthly
+\item
+  Window Zone Summary Monthly
+\item
+  Window Energy Zone Summary Monthly
+\item
+  Average Outdoor Conditions Monthly
+\item
+  Outdoor Conditions Maximum DryBulb Monthly
+\item
+  Outdoor Conditions Minimum DryBulb Monthly
+\item
+  Outdoor Conditions Maximum WetBulb Monthly
+\item
+  Outdoor Conditions Maximum DewPoint Monthly
+\item
+  Outdoor Ground Conditions Monthly
+\item
+  WindowAC Report Monthly
+\item
+  Water Heater Report Monthly
+\item
+  Generator Report Monthly
+\item
+  Daylighting Report Monthly
+\item
+  Coil Report Monthly
+\item
+  PlantLoop Demand Report Monthly
+\item
+  Fan Report Monthly
+\item
+  Pump Report Monthly
+\item
+  CondLoop Demand Report Monthly
+\item
+  Zone Temperature Oscillation Report Monthly
+\item
+  AirLoop System Energy And Water Use Monthly
+\item
+  AirLoop System Component Loads Monthly
+\item
+  AirLoop System Component Energy Use Monthly
+\item
+  Mechanical Ventilation Loads Monthly
+\end{itemize}
+
+Each of these reports is made up of several sub-tables of information. Examples of some of the tables are shown below. To enable all of the reports the single All Summary may be specified.
+
+\subsection{Annual Building Utility Performance Summary}\label{annual-building-utility-performance-summary}
+
+The Annual Building Utility Performance Summary report provides an overview of energy consumption in the building for different end uses. The following is an example this report (some columns may be truncated due to page size). The key used to obtain this report is AnnualBuildingUtilityPerformanceSummary.
+
+In the \emph{Comfort and Setpoint Not Met Summary} sub-table, facility hours represents the total number of hours that any single zone did not meet the comfort or setpoint criteria. It is not weighted by number of zones or number of occupants.
+
+The values in the \emph{End Uses} sub-table are from report meters. To determine which components are attached to each end-use meter, consult the meter details output file (*.mtd).
+
+Report: Annual Building Utility Performance Summary
+
+For: Entire Facility
+
+Timestamp: 2009-02-10 12:39:35
+
+Values gathered over 8760.00 hours
+
+Site and Source Energy
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Source to Site Energy Converstion Factors
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Building Area
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+End Uses
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\emph{Note: Natural gas appears to be the principal heating source based on energy usage.}
+
+End Uses By Subcategory
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Normalized Metrics
+
+Utility Use Per Conditioned Floor Area
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Utility Use Per Total Floor Area
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Electric Loads Satisfied
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+On-Site Thermal Sources
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Water Source Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Comfort and Setpoint Not Met Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Note 1: An asterisk (*) indicates that the feature is not yet implemented.
+
+\subsection{Input Verification and Results Summary}\label{input-verification-and-results-summary}
+
+The Input Verification and Results Summary report provides a summary of some of the most common input assumptions that are not included in any of the other predefined reports. Directly following is an example of the report. The key used to obtain this report is InputVerificationandResultsSummary.
+
+Report: Input Verification and Results Summary
+
+For: Entire Facility
+
+Timestamp: 2009-02-10 12:39:35
+
+General
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+ENVELOPE
+
+Window-Wall Ratio
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Skylight-Roof Ratio
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+PERFORMANCE
+
+Zone Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Demand End Use Components Summary}\label{demand-end-use-components-summary}
+
+The Demand End Use Components Summary report shows the demand breakdown by component end use at the time that the peak demand for each source of energy is set. The time of the peak demand is shown in the first row. The contributions of each end use at the time of the peak demand of the energy source is shown in this report. The key used to obtain this report is DemandEndUseComponentsSummary.
+
+Report: Demand End Use Components Summary
+
+For: Entire Facility
+
+Timestamp: 2009-02-10 12:39:35
+
+End Uses
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+End Uses By Subcategory
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Source Energy End Use Components Summary}\label{source-energy-end-use-components-summary}
+
+The Source Energy End Use Components Summary report produces a report that includes three tables. These tables display source energy by fuel type that is calculated based on site to source energy factors specified by the user in the EnvironmentalImpactFactors and FuelFactors objects. The last two tables display the source energy in terms of area normalized metrics. Directly following is an example of the three tables. The key used to obtain this report is SourceEnergyEndUseComponentsSummary.
+
+Report: \textbf{Source Energy End Use Components Summary}
+
+For: \textbf{Entire Facility}
+
+Timestamp: \textbf{2011-10-07 20:53:43}
+
+\textbf{Values gathered over 8760.00 hours}
+
+\textbf{Source Energy End Use Components Summary}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{Normalized Metrics}
+
+\textbf{Source Energy End Use Components Per Conditioned Floor Area}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{Source Energy End Use Components Per Total Floor Area}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Equipment Summary}\label{equipment-summary}
+
+The Equipment Summary report provides a summary of the HVAC related equipment in the building. The central chiller example shows the most common type of chillers, boilers and towers used in EnergyPlus. The remaining subtables cover DX coils, fans and water heating equipment. Not every type of HVAC equipment is represented in this report. Directly following is an example of the report. The key used to obtain this report is EquipmentSummary.
+
+Report: Equipment Summary
+
+For: Entire Facility
+
+Timestamp: 2009-02-10 12:39:35
+
+Central Plant
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Cooling Coils
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Heating Coils
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Fans
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Pumps
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Service Water Heating
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Envelope Summary}\label{envelope-summary}
+
+The Envelope Summary report provides a summary of the elements of the envelope of the building. The first table describes the exterior opaque elements and the second table describes the fenestration elements. Reflectance is defined as one minus the thermal absorptance. Directly following is an example of the report. The key used to obtain this report is EnvelopeSummary.
+
+Report: Envelope Summary
+
+For: Entire Facility
+
+Timestamp: 2009-02-10 12:39:35
+
+Opaque Exterior
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Fenestration
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Surface Shadowing Summary}\label{surface-shadowing-summary}
+
+The Surface Shadowing Summary report summarizes how the surfaces may cast shadows on other surfaces. Directly following is an example of the report. The key used to obtain this report is SurfaceShadowingSummary.
+
+Report: Surface Shadowing Summary
+
+For: Entire Facility
+
+Timestamp: 2007-10-17 08:54:27
+
+Surfaces (Walls, Roofs, etc) that may be Shadowed by Other Surfaces
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Subsurfaces (Windows and Doors) that may be Shadowed by Surfaces
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Shading Summary}\label{shading-summary-000}
+
+The Shading Summary report shows how much of each window is sunlit at different times of the year and also includes a summary of the window controls. Directly following is an example of the report. The key used to obtain this report is ShadingSummary.
+
+Report: Shading Summary
+
+For: Entire Facility
+
+Timestamp: 2007-10-17 08:54:27
+
+Sunlit Fraction
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Window Control
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Lighting Summary}\label{lighting-summary}
+
+The Lighting Summary report provides a description of the interior and exterior lighting systems being simulated. It also provides a summary of daylighting controls. The Interior Lighting table has three columns that are explained below:
+
+Scheduled Hours/Week {[}hr{]} - In the schedule shown, this represents the average weekly sum of hourly values. It is based on a full year even if the simulation is only performed for part of the year. It is not affected by daylighting.
+
+Hours/Week \textgreater{} 1\% {[}hr{]} -- This represents the average hours per week that are above 1\% of the design value.
+
+Full Load Hours/Week {[}hr{]} -- This is based on consumption and hours that the consumption occurred. It is dependent on the run period used. When simulating only a portion of the year, the value depends on which days of the year (the number of weekdays versus weekend days, for example) are simulated. It also indicates the impact of daylighting control. Directly following is an example of the report. The key used to obtain this report is LightingSummary.
+
+Report: Lighting Summary
+
+For: Entire Facility
+
+Timestamp: 2012-09-05 12:10:52
+
+Interior Lighting
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Daylighting
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Exterior Lighting
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{HVAC Sizing Summary}\label{hvac-sizing-summary}
+
+The HVAC Sizing Summary report provides information on the zone cooling and heating sizing and the peak load conditions as well as information about the system air flow sizing. The Design Load is the zone sensible load only and it does not include any system effects or ventilation loads. The user specified design load and airflow and the values calculated by the program are shown in the report along with the time of the peak load and the temperature and humidity ratio at the time of the peak during the sizing periods. This information is generated for both the Zone Sensible Cooling and Zone Sensible Heating tables.
+
+Also included is the System Design Air Flow Rates which includes the calculated cooling air flow rate, the user specified air flow rate for cooling, the calculated heating air flow rate, and the user specified air flow rate for heating.
+
+\emph{Note:} values listed as ``calculated'' are the unaltered result of the zone or system sizing calculations, using the design sizing period weather and schedules specified in the input. Values listed as ``user specified'' are either the calculated values modified by global or zone sizing factors or values specified with the \emph{flow/zone} or \emph{flow/system} design air flow method.
+
+Directly following is an example of the report.
+
+The key used to obtain this report is HVACSizingSummary.
+
+Report: \textbf{HVAC Sizing Summary}
+
+For: \textbf{Entire Facility}
+
+** Timestamp: **2011-09-23 15:09:34
+
+\textbf{Zone Sensible Cooling}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{Zone Sensible Heating}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{System Design Air Flow Rates}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{Plant Loop Coincident Design Fluid Flow Rate Adjustments}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{System Summary}\label{system-summary}
+
+The System Summary report provides information about some of the primary components in the system including the economizer and demand controlled ventilation. In addition, this report describes when the zone conditions are not comfortable or when set points are not met.
+
+In the \emph{Time Not Comfortable Based on Simple ASHRAE 55-2004} and Time Setpoint Not Met sub-tables, The reported time represents the total number of hours that a given zone did not meet the comfort or setpoint criteria. For the Facility row, this is the total numbers of hours that one or more zones were out of range. The values are not weighted by number of zones or number of occupants.
+
+Directly following is an example of the report. The key used to obtain this report is SystemSummary.
+
+Report: System Summary
+
+For: Entire Facility
+
+Timestamp: 2007-10-17 08:54:27
+
+Economizer
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Demand Controlled Ventilation using VENTILATION:MECHANICAL
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Time Not Comfortable Based on Simple ASHRAE 55-2004
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Time Setpoint Not Met
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Component Sizing Summary}\label{component-sizing-summary}
+
+The Component Sizing Summary report includes details on many of the HVAC components in the simulation. For each of the components, one or more parameters are shown. Directly following is an example of the report. The key used to obtain this report is ComponentSizingSummary.
+
+Report: Component Sizing Summary
+
+For: Entire Facility
+
+Timestamp: 2007-10-17 08:54:27
+
+SINGLE DUCT:VAV:REHEAT
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+COIL:Water:SimpleHeating
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+BRANCH
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+AIR PRIMARY LOOP
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+CONTROLLER:OUTSIDE AIR
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+COIL:Water:Cooling
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+FAN:SIMPLE:VARIABLEVOLUME
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+CONTROLLER:SIMPLE
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+PLANT LOOP
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+BOILER:SIMPLE
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+CHILLER:ELECTRIC
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+PUMP:VARIABLE SPEED
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Outdoor Air Summary}\label{outdoor-air-summary}
+
+The Outdoor Air Summary provides information for each zone on the average and minimum ventilation provided.
+
+The reports described so far in this section are displayed when specified in the Output:Table:Predefined object. They are either on or off and are not customizable. The next few types of tabular reports are customizable. You can specify the report variables being used in each one.
+
+Directly following is an example of the report. The key used to obtain this report is OutdoorAirSummary.
+
+Report: Outdoor Air Summary
+
+For: Entire Facility
+
+Timestamp: 2007-10-17 08:54:27
+
+Average Outside Air During Occupied Hours
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Minimum Outside Air During Occupied Hours
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Climatic Data Summary}\label{climatic-data-summary}
+
+The Climatic Data Summary provides some statistics from the .STAT file concerning the selected weather. The Stat file must be available (it is included with all the weather files on the EnergyPlus website) for the report to be fully produced. Directly following is an example of the report. The key used to obtain this report is ClimaticDataSummary.
+
+Report: Climatic Data Summary
+
+For: Entire Facility
+
+Timestamp: 2009-02-10 13:27:45
+
+SizingPeriod:DesignDay
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Weather Statistics File
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Object Count Summary}\label{object-count-summary}
+
+The object count summary report provides the count on the number of specific objects in the file. Directly following is an example of the report. The key used to obtain this report is ObjectCountSummary.
+
+Report: Object Count Summary
+
+For: Entire Facility
+
+Timestamp: 2009-02-10 12:39:35
+
+Surfaces by Class
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+HVAC
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Component Cost Economics Summary}\label{component-cost-economics-summary}
+
+The Component Cost Economics Summary provides the construction cost estimate summary for the project. The costs are broken into eight catagories and the reference building costs are provided as a comparison. A second table is also produced that provides line item details with one line for every line item object. Directly following is an example of this report.
+
+Report: Component Cost Economics Summary
+
+For: Entire Facility
+
+Timestamp: 2016-01-12 15:47:39
+
+Construction Cost Estimate Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Cost Line Item Details
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{LEED Summary}\label{leed-summary}
+
+The LEED Summary report provides many of the simulation results required for certification of Energy and Atmosphere Credit 1 Optimized Energy Performance according to the LEED Green Building Rating Systemâ„¢. The report can be produced by specifying LEEDSummary in Output:Table:SummaryReports which is also part of the AllSummary option. Directly following is an example of this report.
+
+Report: LEED Summary
+
+For: Entire Facility
+
+Timestamp: 2013-03-01 15:24:37
+
+Sec1.1A-General Information
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+EAp2-1. Space Usage Type
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+EAp2-2. Advisory Messages
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+EAp2-3. Energy Type Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+EAp2-4/5. Performance Rating Method Compliance
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+EAp2-6. Energy Use Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+EAp2-7. Energy Cost Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Process energy cost based on ratio of process to total energy.
+
+L-1. Renewable Energy Source Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+EAp2-17a. Energy Use Intensity - Electricity
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+EAp2-17b. Energy Use Intensity - Natural Gas
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+EAp2-17c. Energy Use Intensity - Other
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+EAp2-18. End Use Percentage
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Energy Meters}\label{energy-meters}
+
+This report provides the details on all the energy meters generated by the simulation. Directly following is an example of the report. The key used to obtain this report is EnergyMeters.
+
+Report: Energy Meters
+
+For: Entire Facility
+
+Timestamp: 2012-05-01 17:07:24
+
+Annual and Peak Values - Electricity
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Annual and Peak Values - Gas
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Annual and Peak Values - Cooling
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Annual and Peak Values - Water
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Annual and Peak Values - Other by Weight/Mass
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Annual and Peak Values - Other Volumetric
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Annual and Peak Values - Other Liquid/Gas
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Annual and Peak Values - Other
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Sensible Heat Gain Summary}\label{sensible-heat-gain-summary}
+
+This report is more fully described in the Input Output Reference but represents the major heat gain components for each zone as well as the HVAC loads satisfied. Directly following is an example of the report. The key used to obtain this report is SensibleHeatGainSummary.
+
+Report: Sensible Heat Gain Summary
+
+For: Entire Facility
+
+Timestamp: 2011-09-09 08:02:03
+
+Annual Building Sensible Heat Gain Components
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Peak Cooling Sensible Heat Gain Components
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Peak Heating Sensible Heat Gain Components
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Standard 62.1 Summary}\label{standard-62.1-summary}
+
+This report is more fully described in the Input Output Reference. The Standard 62.1 Summary produces a report that is consistent with many of the outputs needed when doing calculations consistent with ASHRAE Standard 62.1-2010. The report is generated when sizing calculations are specified. The abbreviations used in the report are consistent with the abbreviations used in Appendix A4 of the Standard. Directly following is an example of the report. The key used to obtain this report is Standard62.1Summary.
+
+Report: Standard 62.1 Summary
+
+For: Entire Facility
+
+Timestamp: 2012-04-20 12:00:57
+
+System Ventilation Requirements for Cooling
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+System Ventilation Requirements for Heating
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Zone Ventilation Parameters
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+System Ventilation Parameters
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Zone Ventilation Calculations for Cooling Design
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+System Ventilation Calculations for Cooling Design
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Zone Ventilation Calculations for Heating Design
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+System Ventilation Calculations for Heating Design
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Zone Component Loads Summary}\label{zone-component-loads-summary}
+
+The Zone Component Loads Summary provides an estimate of the heating and cooling peak loads for each zone broken down into various components. This report may help determine which components of the load have the largest impact for the heating and cooling peak design conditions. When specified, the Zone Component Loads Summary report is created for each zone that is conditioned. The Sensible-Delayed column of the summary is only an estimate based on a procedure described in the Engineering Reference documentation. An intermediate calculation in this procedure is the decay curves that are shown in the the EIO file when Output:Surfaces:List is set to show DecayCurvesFromZoneComponentLoads. The difference between the peak design sensible load and the estimated instant + delayed sensible load (as shown in the \emph{Peak Conditions} subtable) is an indication of how consistent the overall total estimate may be to the computed total peak loads for the zone. When the report is called the zone sizing calculations are repeated twice so this may result in longer simulation times.~ The key used to obtain this report is ZoneComponentLoadSummary.
+
+Report: ZoneComponentLoadSummary
+
+For: SPACE1-1
+
+Timestamp: 2012-09-21 15:48:46
+
+Estimated Cooling Peak Load Components
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Cooling Peak Conditions
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Estimated Heating Peak Load Components
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Heating Peak Conditions
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Output:Table:TimeBins}\label{outputtabletimebins}
+
+A TimeBins report shows a grid of the number of hours that specific report variable spend in a range of values. The first table is broken into two parts. The first part is monthly and the second part is for each hour of the day. The columns show the range of values. A second table is provided to show some statistics on the report variable for the entire year including the maximum and minimum. These statistics are helpful in setting the field values for the interval in the Output Table:TimeBins object. Due to this, it is often necessary to run two simulations to fully utilize the TimeBins report with the first run used to find the minimum and maximum of the variable, these values are then used in the TimeBins object and the second run a better table of binned results are displayed.
+
+Report: PURCHASEDCOOLING:FACILITY J per second
+
+For: Meter
+
+Timestamp: 2006-08-30 07:48:55
+
+Values in table are in hours.
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Statistics
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Output:Table:Monthly}\label{outputtablemonthly}
+
+Monthly reports are not predefined. Instead each column is defined when using the Output:Table:Monthly object. In that object each column is defined by a variable and how it should be aggregated. The StandardReports.idf file is located in DataSets directory where EnergyPlus is installed and contains a large number of examples of how to use Output:Table:Monthly to get summaries of the performance of different components in the building model. These examples include:
+
+\begin{itemize}
+\item
+  Zone Cooling Summary
+\item
+  Zone Heating Summary
+\item
+  Zone Electric Summary
+\item
+  Space Gains
+\item
+  Peak Space Gains
+\item
+  Space Gain Components at Cooling Peak
+\item
+  Energy Consumption - Electricity \& Natural Gas
+\item
+  Energy Consumption - Electricity Generated \& Propane
+\item
+  Energy Consumption - Diesel \& Fuel Oil
+\item
+  Energy Consumption~ - Purchased Heating \& Cooling
+\item
+  Energy Consumption - Coal \& Gasoline
+\item
+  End-Use Energy Consumption - Electricity
+\item
+  End-Use Energy Consumption - Natural Gas
+\item
+  End-Use Energy Consumption - Diesel
+\item
+  End-Use Energy Consumption - Fuel Oil
+\item
+  End-Use Energy Consumption - Coal
+\item
+  End-Use Energy Consumption - Propane
+\item
+  End-Use Energy Consumption - Gasoline
+\item
+  Peak Energy End-Use - Electricity Part 1
+\item
+  Peak Energy End-Use - Electricity Part 2
+\item
+  Electric Components of Peak Demand
+\item
+  Peak Energy End-Use - Natural Gas
+\item
+  Peak Energy End-Use - Diesel
+\item
+  Peak Energy End-Use - Fuel Oil
+\item
+  Peak Energy End-Use - Coal
+\item
+  Peak Energy End-Use - Propane
+\item
+  Peak Energy End-Use - Gasoline
+\item
+  Setpoints Not Met With Temperatures
+\item
+  Comfort Report - Simple 55
+\item
+  Unglazed Transpired Solar Collector Summary
+\item
+  Occupant Comfort Data Summary
+\item
+  Chiller Report
+\item
+  Tower Report
+\item
+  Boiler Report
+\item
+  DX Report
+\item
+  Window Report
+\item
+  Window Energy Report
+\item
+  Window Zone Summary
+\item
+  Average Outdoor Conditions
+\item
+  Outdoor Conditions Maximum Drybulb
+\item
+  Outdoor Conditions Minimum Drybulb
+\item
+  Outdoor Conditions Maximum Wetbulb
+\item
+  Outdoor Conditions Maximum Dewpoint
+\item
+  Outdoor Ground Conditions
+\item
+  Window AC Report
+\item
+  Water Heater Report
+\item
+  Generator Report
+\item
+  Daylighting Report
+\item
+  Coil Report
+\item
+  Plant Loop Demand Report
+\item
+  Fan Report
+\item
+  Pump Report
+\item
+  Cond Loop Demand Report
+\item
+  Zone Temperature Oscillation Report
+\item
+  Air Loop System Energy and Water Use
+\item
+  Air Loop System Component Loads
+\item
+  Air Loop System Component Energy Use
+\item
+  Mechanical Ventilation Loads
+\end{itemize}
+
+An example of the Zone Cooling Summary monthly report is shown below.
+
+Report: ZONE COOLING SUMMARY
+
+For: SPACE2-1
+
+Timestamp: 2006-08-29 07:21:57
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{UtilityCost:Tariff}\label{utilitycosttariff}
+
+The use of UtilityCost:Tariff objects automatically generates two reports related to the calculation of annual utility costs. The first report is a summary across multiple tariffs and is called the Economics Results Summary report and is shown directly below. After that example is an example of the Tariff report which is created for each of the UtilityCost:Tariff Objects defined in the IDF file~ (some columns may be truncated due to page size).
+
+Report: Economics Results Summary Report
+
+For: Entire Facility
+
+Timestamp: 2006-08-29 07:21:57
+
+Annual Cost
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Tariff Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+The following is an example of the Tariff report which is created for each of the UtilityCost:Tariff objects defined in the file.
+
+Report: Tariff Report
+
+For: EXAMPLEA
+
+Timestamp: 2006-08-29 07:21:57
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Categories
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Charges
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Ratchets
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Qualifies
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Native Variables
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Other Variables
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Computation - Automatic FLATENERGYCHARGE FROM TotalEnergy EnergyCharges SUM FLATENERGYCHARGE Basis SUM EnergyCharges DemandCharges ServiceCharges Subtotal SUM Basis Adjustment Surcharge Total SUM Subtotal Taxes
+
+\subsection{Construction Cost Estimate Summary}\label{construction-cost-estimate-summary}
+
+The Construction Cost Estimate Summary report shows the details of a simplified cost estimate of the building along with a comparison with reference building costs entered by the user. An example of the Construction Cost Estimate Summary report is shown below.
+
+Construction Cost Estimate Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Cost Line Item Details
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Line No. & Item Name & Quantity. & Units & \textbackslash\$ per Qty. & SubTotal \textbackslash\$ \tabularnewline
+\midrule
+\endhead
+
+-- & 1 & EXTERIOR WALLS & 627.57 & m2 & 168.64 & 105832.65 \tabularnewline
+-- & 2 & INTERIOR WALLS & 854.18 & m2 & 31.16 & 26616.23 \tabularnewline
+-- & 3 & ROOF & 1857.96 & m2 & 104.69 & 194509.64 \tabularnewline
+-- & 4 & GROUND FLR SLAB & 1857.96 & m2 & 56.06 & 104157.14 \tabularnewline
+-- & 5 & ACOUSTICAL DROP CEILINGS & 1857.96 & m2 & 23.79 & 44200.83 \tabularnewline
+-- & 6 & QUAD HIGH SHGC SUPERWINDOWS & 226.22 & m2 & 687.84 & 155604.96 \tabularnewline
+-- & 7 & QUAD LOW SHGC SUPERWINDOWS & 42.68 & m2 & 687.84 & 29359.55 \tabularnewline
+-- & 8 & CENTRAL CHILLER & 153.48 & kW (tot cool cap.) & 340.00 & 52183.09 \tabularnewline
+-- & 9 & CONTINUOUS AIR BARRIER & 1.00 & Ea. & 8500.00 & 8500.00 \tabularnewline
+Line Item SubTotal & -- & -- & -- & -- & -- & 720964.07 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{XML Tabular Output}\label{xml-tabular-output}
+
+The tables discussed in this section can also be output in an XML format that may be easier for some other programs to extract specific results. An excerpt of the XML file format is shown below. This report presents the same output results as the other tabular report formats but using XML tags.
+
+\textless{}?xml version = ``1.0''?\textgreater{}
+
+\textless{}EnergyPlusTabularReports\textgreater{}
+
+~ \textless{}BuildingName\textgreater{}NONE\textless{}/BuildingName\textgreater{}
+
+~ \textless{}EnvironmentName\textgreater{}Chicago Ohare Intl Ap IL USA TMY3 WMO\# = 725300\textless{}/EnvironmentName\textgreater{}
+
+~ \textless{}WeatherFileLocationTitle\textgreater{}Chicago Ohare Intl Ap IL USA TMY3 WMO\# = 725300\textless{}/WeatherFileLocationTitle\textgreater{}
+
+~ \textless{}ProgramVersion\textgreater{}EnergyPlus, Version 8.0, YMD = 2013.02.18 15:50\textless{}/ProgramVersion\textgreater{}
+
+~ \textless{}SimulationTimestamp\textgreater{}
+
+~~~ \textless{}Date\textgreater{}
+
+~~~~~ 2013-02-18
+
+~~~ \textless{}/Date\textgreater{}
+
+~~~ \textless{}Time\textgreater{}
+
+~~~~~ 15:50:33
+
+~~~ \textless{}/Time\textgreater{}
+
+~ \textless{}/SimulationTimestamp\textgreater{}
+
+\textless{}AnnualBuildingUtilityPerformanceSummary\textgreater{}
+
+~ \textless{}for\textgreater{}Entire Facility\textless{}/for\textgreater{}
+
+~ \textless{}SiteAndSourceEnergy\textgreater{}
+
+~~~ \textless{}name\textgreater{}TotalSiteEnergy\textless{}/name\textgreater{}
+
+~~~ \textless{}TotalEnergy units = ``kBtu''\textgreater{}200671.97\textless{}/TotalEnergy\textgreater{}
+
+~~~ \textless{}EnergyPerTotalBuildingArea units = ``kBtu/ft2''\textgreater{}143.32\textless{}/EnergyPerTotalBuildingArea\textgreater{}
+
+~~~ \textless{}EnergyPerConditionedBuildingArea units = ``kBtu/ft2''\textgreater{}143.32\textless{}/EnergyPerConditionedBuildingArea\textgreater{}
+
+~ \textless{}/SiteAndSourceEnergy\textgreater{}
+
+~ \textless{}SiteAndSourceEnergy\textgreater{}
+
+~~~ \textless{}name\textgreater{}NetSiteEnergy\textless{}/name\textgreater{}
+
+~~~ \textless{}TotalEnergy units = ``kBtu''\textgreater{}200671.97\textless{}/TotalEnergy\textgreater{}
+
+~~~ \textless{}EnergyPerTotalBuildingArea units = ``kBtu/ft2''\textgreater{}143.32\textless{}/EnergyPerTotalBuildingArea\textgreater{}
+
+~~~ \textless{}EnergyPerConditionedBuildingArea units = ``kBtu/ft2''\textgreater{}143.32\textless{}/EnergyPerConditionedBuildingArea\textgreater{}
+
+~ \textless{}/SiteAndSourceEnergy\textgreater{}
+
+~ \textless{}SiteAndSourceEnergy\textgreater{}
+
+~~~ \textless{}name\textgreater{}TotalSourceEnergy\textless{}/name\textgreater{}
+
+~~~ \textless{}TotalEnergy units = ``kBtu''\textgreater{}442504.19\textless{}/TotalEnergy\textgreater{}
+
+~~~ \textless{}EnergyPerTotalBuildingArea units = ``kBtu/ft2''\textgreater{}316.04\textless{}/EnergyPerTotalBuildingArea\textgreater{}
+
+~~~ \textless{}EnergyPerConditionedBuildingArea units = ``kBtu/ft2''\textgreater{}316.04\textless{}/EnergyPerConditionedBuildingArea\textgreater{}
+
+~ \textless{}/SiteAndSourceEnergy\textgreater{}
+
+~ \textless{}SiteAndSourceEnergy\textgreater{}
+
+~~~ \textless{}name\textgreater{}NetSourceEnergy\textless{}/name\textgreater{}
+
+~~~ \textless{}TotalEnergy units = ``kBtu''\textgreater{}397810.98\textless{}/TotalEnergy\textgreater{}
+
+~~~ \textless{}EnergyPerTotalBuildingArea units = ``kBtu/ft2''\textgreater{}284.12\textless{}/EnergyPerTotalBuildingArea\textgreater{}
+
+~~~ \textless{}EnergyPerConditionedBuildingArea units = ``kBtu/ft2''\textgreater{}284.12\textless{}/EnergyPerConditionedBuildingArea\textgreater{}
+
+~ \textless{}/SiteAndSourceEnergy\textgreater{}
+
+\emph{An actual file will be much longer than this example but follows this format.}
diff --git a/doc/output-details-and-examples/src/output-files/epluszsz-lt-ext-gt.tex b/doc/output-details-and-examples/src/output-files/epluszsz-lt-ext-gt.tex
new file mode 100644
index 00000000000..36dc53e40f0
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/epluszsz-lt-ext-gt.tex
@@ -0,0 +1,90 @@
+\section{epluszsz.\textless{}ext\textgreater{}}\label{epluszsz.ext}
+
+This file is a result of the zone sizing calculation. Zone Sizing (see Sizing:Zone object) performs a special calculation, using a theoretical ideal zonal system, and determines the zone design heating and cooling flow rates and loads, saving the results in the zone sizing arrays. The file has a similar format to the eplusssz.\textless{}ext\textgreater{} file.
+
+An excerpt (this is a direct copy of the CSV data, so you can copy it to a spreadsheet to view it easier):
+
+Time,SPACE1-1:CHICAGO\_IL\_USA ANNUAL HEATING 99\% DESIGN CONDITIONS DB:Des Heat Load {[}W{]},SPACE1-1:CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB:Des Sens Cool Load {[}W{]},SPACE1-1:CHICAGO\_IL\_USA ANNUAL HEATING 99\% DESIGN CONDITIONS DB:Des Heat Mass Flow {[}kg/s{]},SPACE1-1:CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB:Des Cool Mass Flow {[}kg/s{]},SPACE2-1:CHICAGO\_IL\_USA ANNUAL HEATING 99\% DESIGN CONDITIONS DB:Des Heat Load {[}W{]},SPACE2-1:CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB:Des Sens Cool Load {[}W{]},SPACE2-1:CHICAGO\_IL\_USA ANNUAL HEATING 99\% DESIGN CONDITIONS DB:Des Heat Mass Flow {[}kg/s{]},SPACE2-1:CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB:Des Cool Mass Flow {[}kg/s{]},SPACE3-1:CHICAGO\_IL\_USA ANNUAL HEATING 99\% DESIGN CONDITIONS DB:Des Heat Load {[}W{]},SPACE3-1:CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB:Des Sens Cool Load {[}W{]},SPACE3-1:CHICAGO\_IL\_USA ANNUAL HEATING 99\% DESIGN CONDITIONS DB:Des Heat Mass Flow {[}kg/s{]},SPACE3-1:CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB:Des Cool Mass Flow {[}kg/s{]},SPACE4-1:CHICAGO\_IL\_USA ANNUAL HEATING 99\% DESIGN CONDITIONS DB:Des Heat Load {[}W{]},SPACE4-1:CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB:Des Sens Cool Load {[}W{]},SPACE4-1:CHICAGO\_IL\_USA ANNUAL HEATING 99\% DESIGN CONDITIONS DB:Des Heat Mass Flow {[}kg/s{]},SPACE4-1:CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB:Des Cool Mass Flow {[}kg/s{]},SPACE5-1:CHICAGO\_IL\_USA ANNUAL HEATING 99\% DESIGN CONDITIONS DB:Des Heat Load {[}W{]},SPACE5-1:CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB:Des Sens Cool Load {[}W{]},SPACE5-1:CHICAGO\_IL\_USA ANNUAL HEATING 99\% DESIGN CONDITIONS DB:Des Heat Mass Flow {[}kg/s{]},SPACE5-1:CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB:Des Cool Mass Flow {[}kg/s{]}
+
+00:15:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+00:30:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+00:45:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+01:00:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+01:15:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+01:30:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+01:45:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+02:00:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+02:15:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+02:30:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+02:45:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
+
+= = = reduced for brevity = = =
+
+Peak,3.860764E+03,2.647331E+03,1.371872E-01,2.618408E-01,1.625149E+03,2.234379E+03,5.774764E-02,2.209833E-01,3.753069E+03,2.506339E+03,1.333603E-01,2.478849E-01,1.625149E+03,2.464720E+03,5.774764E-02,2.437670E-01,2.981568E+03,2.628694E+03,1.059457E-01,2.599981E-01
+
+Peak Vol Flow (m3/s),,,1.166672E-01,2.226756E-01,,,4.910995E-02,1.879294E-01,,,1.134128E-01,2.108072E-01,,,4.910995E-02,2.073052E-01,,,9.009871E-02,2.211085E-01
+
+The columns are:
+
+\subsubsection{Field: Time}\label{field-time-000}
+
+Calculation time -- this will show the time steps used by the simulation and by the sizing calculation.
+
+\subsubsection{Sizing Calculation Fields}\label{sizing-calculation-fields}
+
+Each of the Zone Sizing output fields has the Zone Name, the Environment Name for the peak prepended to the item that has been calculated.~ The four fields calculated are:
+
+\begin{itemize}
+\item
+  Des Heat Load
+\item
+  Des Sens Cool Load
+\item
+  Des Heat Mass Flow
+\item
+  Des Cool Mass Flow
+\end{itemize}
+
+These are repeated for the number of zones in the sizing calculation.
+
+\subsubsection{Field:~ Des Heat Load {[}W{]}}\label{field-des-heat-load-w}
+
+This is the calculated design/required heating load at the time step.
+
+\subsubsection{Field:~ Des Sens Cool Load {[}W{]}}\label{field-des-sens-cool-load-w}
+
+This is the calculated design/required cooling load at the time step.
+
+\subsubsection{Field:~ Des Heat Mass Flow {[}kg/s{]}}\label{field-des-heat-mass-flow-kgs-000}
+
+This is the calculated design/required heating mass flow rate at the time step.
+
+\subsubsection{Field: Des Cool Mass Flow {[}kg/s{]}}\label{field-des-cool-mass-flow-kgs-000}
+
+This is the calculated design/required cooling mass flow rate at the time step.
+
+\subsubsection{Line: Peak}\label{line-peak}
+
+This indicates the peak calculation (load or mass flow) over the 24 hour condensed sizing period.
+
+\subsubsection{Line: Peak Vol Flow {[}m3/s{]}}\label{line-peak-vol-flow-m3s}
+
+For the mass flow rates, this indicates the peak volume flow calculation (m3/s) over the 24 hour condensed sizing period.
+
+Or as depicted in a chart:
+
+\begin{figure}[hbtp] % fig 6
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image018.jpg}
+\caption{Zone Sizing from epluszsz.csv \protect \label{fig:zone-sizing-from-epluszsz.csv}}
+\end{figure}
diff --git a/doc/output-details-and-examples/src/output-files/output-file-list.tex b/doc/output-details-and-examples/src/output-files/output-file-list.tex
new file mode 100644
index 00000000000..c82d6af4d9d
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/output-file-list.tex
@@ -0,0 +1,74 @@
+\section{Output File List}\label{output-file-list}
+
+Following are the native file names that are output from EnergyPlus; native -- directly out of EnergyPlus. Usually you will not see these file names as batch files and interfaces will change them to be \textless{}file name\textgreater{}.\textless{}ext\textgreater{} or in some instances \textless{}file name\textgreater{}\textless{}qualifier\textgreater{}.\textless{}ext\textgreater{}. Usually the extension is the important piece and is described in the following table.
+
+% table 1
+\begin{longtable}[c]{p{1.5in}p{3.0in}p{1.5in}}
+\caption{EnergyPlus Basic Output  Files \label{table:energyplus-basic-output-files}} \tabularnewline
+\toprule 
+Output File Name & Description & EP-Launch File Name \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{EnergyPlus Basic Output  Files} \tabularnewline
+\toprule 
+Output File Name & Description & EP-Launch File Name \tabularnewline
+\midrule
+\endhead
+
+eplusout.audit & Echo of input, includes both IDD echo and IDF echo – may have errors shown in context with IDD or IDF statements & < filename > .audit (without echoing IDD unless errors in IDD). \tabularnewline
+eplusout.bnd & This file contains details about the nodes and branches. Useful in determining if all your nodes are connected correctly. May be used to diagram the network/ nodes of the HVAC system. & < filename > .bnd \tabularnewline
+eplusout.dbg & From Debug Output object – may be useful to support to help track down problems & < filename > .dbg \tabularnewline
+eplusout.dxf & DXF (from Output:Surfaces:Drawing,DXF;) & < filename > .dxf \tabularnewline
+eplusout.edd & Descriptive output from the EMS portion & < filename > .edd \tabularnewline
+eplusout.eio & Contains several standard and optional “report� elements. CSV format – may be read directly into spreadsheet program for better formatting. & < filename > .eio \tabularnewline
+eplusout.end & A one line summary of success or failure (useful for Interface programs) & Not saved in the standard EPL-Run script file. \tabularnewline
+eplusout.epmidf & Output from EPMacro program – contains the idf created from the input imf file & < filename > .epmidf \tabularnewline
+eplusout.epmdet & Output from EPMacro program – the audit/details of the EPMacro processing & < filename > .epmdet \tabularnewline
+eplusout.err & Error file – contains very important information from running the program. & < filename > .err \tabularnewline
+eplusout.eso & Standard Output File (contains results from both Output:Variable and Output:Meter objects). & < filename > .eso \tabularnewline
+eplusout.log & Log of items that appear in the command file output from the run. & < filename > .log \tabularnewline
+eplusout.mdd & Meter names that are applicable for reporting in the current simulation. & < filename > .mdd \tabularnewline
+eplusout.mtd & Meter details report – what variables are on what meters and vice versa. This shows the meters on which the Zone: Lights Electric Energy appear as well as the contents of the Electricity:Facility meter. & < filename > .mtd \tabularnewline
+eplusout.mtr & Similar to .eso but only has Output:Meter outputs. & < filename > .mtr \tabularnewline
+eplusout.rdd & Variable names that are applicable for reporting in the current simulation. & < filename > .rdd \tabularnewline
+eplusout.shd & Surface shadowing combinations report & < filename > .shd \tabularnewline
+eplusout.sln & Similar to DXF output but less structured. Results of Output:Reports,Surface, Lines object. & < filename > .sln \tabularnewline
+eplusout.sql & Mirrors the data in the .eso and .mtr files but is in SQLite format (for viewing with SQLite tools). & < filename > .sql \tabularnewline
+eplusssz. < ext > & Results from the Sizing:System object. This file is “spreadsheet� ready. Different extensions (csv, tab, and txt) denote different “separators� in the file. & < filename > Ssz. < ext > \tabularnewline
+epluszsz. < ext > & Results from the Sizing:Zone object. This file is “spreadsheet� ready. Different extensions (csv, tab, and txt) denote different “separators� in the file. & < filename > Zsz. < ext > \tabularnewline
+eplusmap. < ext > & Daylighting intensity “map� output. Different extensions (csv, tab, and txt) denote different “separators� in the file. & < filename > Map. < ext > \tabularnewline
+eplusout.dfs & This file contains the hourly pre-calculated daylight factors for exterior windows of a daylight zone. & < filename > DFS.csv \tabularnewline
+eplusscreen.csv & Window screen transmittance (direct and reflected) “map� output. & < filename > Screen.csv \tabularnewline
+eplustbl. < ext > & Results of tabular and economics requests. Different extensions (csv, tab, and txt) denote different “separators� in the file. & < filename > Table. < ext > \tabularnewline
+eplusout.svg & Results from the HVAC-Diagram application. SVG is a Scalable Vector Graphics file for which several viewers can be found. & < filename > .svg \tabularnewline
+eplusout.sci & File of cost information & < filename > .sci \tabularnewline
+eplusout.delightin & File produced during DElight simulations – descriptive of EnergyPlus inputs into DElight inputs. & < filename > delight.in \tabularnewline
+eplusout.delightout & File produced during DElight simulations – basic results from DElight simulation. & < filename > delight.out \tabularnewline
+eplusout.wrl & VRML output from (Output:Reports, Surfaces, VRML) & < filename > .wrl \tabularnewline
+\bottomrule
+\end{longtable}
+
+In addition to the basic output files from EnergyPlus there are three standard ``hybrid'' output files. These are called ``hybrid'' because they are a result of post-processing after EnergyPlus has completed. Note that if there is an error during processing, these will not normally be ``complete''.
+
+% table 2
+\begin{longtable}[c]{p{1.5in}p{3.0in}p{1.5in}}
+\caption{"Hybrid" EnergyPlus Output Files \label{table:hybrid-energyplus-output-files}} \tabularnewline
+\toprule 
+Output File Name & Description & EP-Launch File Name \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{"Hybrid" EnergyPlus Output Files} \tabularnewline
+\toprule 
+Output File Name & Description & EP-Launch File Name \tabularnewline
+\midrule
+\endhead
+
+eplusout. < ext >  ~ & “spreadsheet� ready file that contains either all the report variables requested (default: up to limit of 255) from the input file or specific ones specified by the user. Different extensions (csv, tab, and txt denote different “separators� in the file. & < filename > .csv or  < filename > .tab or  < filename > .txt \tabularnewline
+eplusmtr. < ext >  ~ & “spreadsheet� ready file that contains either all the report meter requests (default: up to 255) from the input file or specific ones specified by the user. Different extensions (csv, tab, and txt denote different “separators� in the file. & < filename > Meter.csv or  < filename > Meter.tab or  < filename > Meter.txt \tabularnewline
+readvars.rvaudit & Results of any “ReadVarsESO� execution in the current batch run. & < filename > .rvaudit \tabularnewline
+\bottomrule
+\end{longtable}
+
+Now, each file will be described in more detail with some examples of use.
diff --git a/doc/output-details-and-examples/src/output-files/readvars-rvaudit.tex b/doc/output-details-and-examples/src/output-files/readvars-rvaudit.tex
new file mode 100644
index 00000000000..e01c873827a
--- /dev/null
+++ b/doc/output-details-and-examples/src/output-files/readvars-rvaudit.tex
@@ -0,0 +1,77 @@
+\section{readvars.rvaudit}\label{readvars.rvaudit}
+
+This file is available from standard EnergyPlus runs (batch file, EP-Launch, etc) where the included utility ``ReadVarsESO'' is used to create .csv or other delimited files. It shows what steps were taken during the read vars run(s) -- in standard EnergyPlus runs there are two: one for the .eso file and one for the .mtr file. Contents might be:
+
+Mon 04/02/2007 19:34:17.09 ReadVars
+
+~ReadVarsESO
+
+~processing:eplusout.inp
+
+~input file:eplusout.eso
+
+~output file:eplusout.csv
+
+~found/finding:
+
+~~~~ 1 Outdoor Dry Bulb
+
+~~~~ 6 Zone/Sys Air Temperature
+
+~~~~ 6 Zone/Sys Sensible Cooling Rate
+
+~~~~ 6 Zone/Sys Sensible Heating Rate
+
+~~~~ 6 Total Water Heating Coil Rate
+
+~~~~ 1 Total Water Cooling Coil Rate
+
+~~~~ 1 Sensible Water Cooling Coil Rate
+
+~~~~ 2 Plant Loop Cooling Demand
+
+~~~~ 2 Plant Loop Heating Demand
+
+~~~~ 1 Boiler Gas Consumption Rate
+
+~~~~ 1 Boiler Heating Output Rate
+
+~~~~ 1 Chiller Electric Power
+
+~~~~ 1 Chiller Evap Heat Trans Rate
+
+~~~~ 1 Chiller Evap Water Inlet Temp
+
+~~~~ 1 Chiller Evap Water Outlet Temp
+
+~~~~ 1 Chiller Evap Water Mass Flow Rate
+
+~~~~ 1 Chiller Cond Heat Trans Rate
+
+~~~~ 0 Chiller Cond Water Inlet Temp
+
+~~~~ 0 Chiller Cond Water Outlet Temp
+
+~~~~ 0 Chiller Cond Water Mass Flow Rate
+
+~~~~ 2 Pump Mass Flow Rate
+
+~~~~ 2 Pump Outlet Temp
+
+~ReadVars Run Time = 00hr 00min~ 1.78sec
+
+~ReadVarsESO program completed successfully.
+
+~ReadVarsESO
+
+~processing:test.mvi
+
+~input file:eplusout.mtr
+
+~output file:eplusmtr.csv
+
+~getting all vars from:eplusout.mtr
+
+~ReadVars Run Time = 00hr 00min~ 0.00sec
+
+~ReadVarsESO program completed successfully.
diff --git a/doc/plant-application-guide/CMakeLists.txt b/doc/plant-application-guide/CMakeLists.txt
new file mode 100644
index 00000000000..25c16816633
--- /dev/null
+++ b/doc/plant-application-guide/CMakeLists.txt
@@ -0,0 +1,175 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/plant-application-guide.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/title.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/introduction.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/introduction/organization.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/scope.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/energyplus-nomenclature.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/generating-an-energyplus-line-diagram.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/generating-an-energyplus-line-diagram/example-for-energyplus-line-diagram.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/inputting-the-system-into-the-idf-file.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops/chilled-water-loop.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops/condenser-loop.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-02-thermal-energy-storage.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-02-thermal-energy-storage/primary-cooling-loop-coolsysprimary-chiller.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-02-thermal-energy-storage/condenser-loop-condenser-loop-cooling-tower.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-02-thermal-energy-storage/heating-loop-heatsys1-boiler.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/primary-chilled-water-loop-chiller-s.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/secondary-chilled-water-loop-plate-heat.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/primary-secondary-pumping.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/condenser-loop-cooling-tower.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/src/references.tex
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/../title.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image001.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image002.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image003.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image004.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image005.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image006.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image007.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image008.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image009.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image010.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image011.png
+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image012.png
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+  ${CMAKE_SOURCE_DIR}/doc/plant-application-guide/media/image127.png
+) 
+
+SET( SOURCE_FILENAME "plant-application-guide" )
+SET( OUTPUT_FILENAME "PlantApplicationGuide" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
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similarity index 100%
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similarity index 100%
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similarity index 100%
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similarity index 100%
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similarity index 100%
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image008.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image009.png
rename to doc/plant-application-guide/media/image009.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image010.png
rename to doc/plant-application-guide/media/image010.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image011.png
rename to doc/plant-application-guide/media/image011.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image012.png
rename to doc/plant-application-guide/media/image012.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image013.png b/doc/plant-application-guide/media/image013.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image013.png
rename to doc/plant-application-guide/media/image013.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image014.png
rename to doc/plant-application-guide/media/image014.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image015.png b/doc/plant-application-guide/media/image015.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image015.png
rename to doc/plant-application-guide/media/image015.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image016.png b/doc/plant-application-guide/media/image016.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image016.png
rename to doc/plant-application-guide/media/image016.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image017.png b/doc/plant-application-guide/media/image017.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image017.png
rename to doc/plant-application-guide/media/image017.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image018.png b/doc/plant-application-guide/media/image018.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image018.png
rename to doc/plant-application-guide/media/image018.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image019.png b/doc/plant-application-guide/media/image019.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image019.png
rename to doc/plant-application-guide/media/image019.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image020.png b/doc/plant-application-guide/media/image020.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image020.png
rename to doc/plant-application-guide/media/image020.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image021.png b/doc/plant-application-guide/media/image021.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image021.png
rename to doc/plant-application-guide/media/image021.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image022.png b/doc/plant-application-guide/media/image022.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image022.png
rename to doc/plant-application-guide/media/image022.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image023.png b/doc/plant-application-guide/media/image023.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image023.png
rename to doc/plant-application-guide/media/image023.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image024.png
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similarity index 100%
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image026.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image027.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image028.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image029.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image030.png
rename to doc/plant-application-guide/media/image030.png
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similarity index 100%
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similarity index 100%
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similarity index 100%
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similarity index 100%
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image035.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image036.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image037.png
rename to doc/plant-application-guide/media/image037.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image038.png
rename to doc/plant-application-guide/media/image038.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image039.png
rename to doc/plant-application-guide/media/image039.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image040.png
rename to doc/plant-application-guide/media/image040.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image041.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image042.png
rename to doc/plant-application-guide/media/image042.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image043.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image044.png
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diff --git a/doc/src/docs/PlantApplicationGuide/media/image045.png b/doc/plant-application-guide/media/image045.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image045.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image046.png
rename to doc/plant-application-guide/media/image046.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image047.png
rename to doc/plant-application-guide/media/image047.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image048.png
rename to doc/plant-application-guide/media/image048.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image049.png b/doc/plant-application-guide/media/image049.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image049.png
rename to doc/plant-application-guide/media/image049.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image050.png b/doc/plant-application-guide/media/image050.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image050.png
rename to doc/plant-application-guide/media/image050.png
diff --git a/doc/src/docs/PlantApplicationGuide/media/image051.png b/doc/plant-application-guide/media/image051.png
similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image051.png
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similarity index 100%
rename from doc/src/docs/PlantApplicationGuide/media/image052.png
rename to doc/plant-application-guide/media/image052.png
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diff --git a/doc/plant-application-guide/plant-application-guide.tex b/doc/plant-application-guide/plant-application-guide.tex
new file mode 100644
index 00000000000..4080f3938b9
--- /dev/null
+++ b/doc/plant-application-guide/plant-application-guide.tex
@@ -0,0 +1,60 @@
+\input{../header}
+
+\title{Plant Application Guide}
+
+\hypersetup{unicode=true,
+            pdftitle={Plant Application Guide},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/title}
+
+\input{src/introduction}
+
+\input{src/introduction/organization}
+
+\input{src/scope}
+
+\input{src/energyplus-nomenclature}
+
+\input{src/generating-an-energyplus-line-diagram}
+
+\input{src/generating-an-energyplus-line-diagram/example-for-energyplus-line-diagram}
+
+\input{src/inputting-the-system-into-the-idf-file}
+
+\input{src/example-01-chiller-and-condenser-loops}
+
+\input{src/example-01-chiller-and-condenser-loops/chilled-water-loop}
+
+\input{src/example-01-chiller-and-condenser-loops/condenser-loop}
+
+\input{src/example-02-thermal-energy-storage}
+
+\input{src/example-02-thermal-energy-storage/primary-cooling-loop-coolsysprimary-chiller}
+
+\input{src/example-02-thermal-energy-storage/condenser-loop-condenser-loop-cooling-tower}
+
+\input{src/example-02-thermal-energy-storage/heating-loop-heatsys1-boiler}
+
+\input{src/example-system-3-primary-secondary-pumping}
+
+\input{src/example-system-3-primary-secondary-pumping/primary-chilled-water-loop-chiller-s}
+
+\input{src/example-system-3-primary-secondary-pumping/secondary-chilled-water-loop-plate-heat}
+
+\input{src/example-system-3-primary-secondary-pumping/primary-secondary-pumping}
+
+\input{src/example-system-3-primary-secondary-pumping/condenser-loop-cooling-tower}
+
+\input{src/references}
+
+\end{document}
diff --git a/doc/plant-application-guide/src/energyplus-nomenclature.tex b/doc/plant-application-guide/src/energyplus-nomenclature.tex
new file mode 100644
index 00000000000..a56024d9832
--- /dev/null
+++ b/doc/plant-application-guide/src/energyplus-nomenclature.tex
@@ -0,0 +1,36 @@
+\chapter{EnergyPlus Nomenclature}\label{energyplus-nomenclature}
+
+The following is a list of terms that are used in this guide. A simple description of each of the terms is provided. More detailed descriptions can be obtained from the EnergyPlus Input Output Reference. Some keywords are provided to assist with the search for these terms in the Input Output Reference guide.
+
+\begin{itemize}
+\item
+  \textbf{Loops} -- Loops are high-level construction objects in EnergyPlus. Loops are paths through which the working fluid is circulated in order to satisfy a cooling or heating load. An HVAC system may consist of a zone, plant loop, and a condenser loop. Loops are constructed by using branches. (Keywords: \emph{PlantLoop})\emph{.} Note: Although EnergyPlus has separate object classes for \emph{CondenserLoops} and \emph{PlantLoops,} the difference between them is very trivial; therefore all the condenser loops in this guide will be modeled by a \emph{PlantLoop} object.
+\item
+  \textbf{Supply side half-loop} -- This is the half loop that contains components (such as Boilers and chillers) which treat the working fluid to supply a working fluid state to the demand components.
+\item
+  \textbf{Demand side half-loop} -- This is the half loop that contains components (such as cooling coils and heating coils which use the working fluid to satisfy a load.
+\item
+  \textbf{Branches} -- Branches are mid-level construction objects in EnergyPlus. Branches are the segments used to construct the loops. They are constructed by using nodes and a series of components. Every branch must have at least one component. Branches will be denoted by using blue colored lines in the EnergyPlus schematics. (Keyword: \emph{Branch})\emph{.}
+\item
+  \textbf{Branchlists} -- Branchlists list all the branches on one side of a loop. (Keyword: \emph{Branchlist})\emph{.}
+\item
+  \textbf{Bypass Branch} -- A bypass branch is used to bypass the core operating components, it ensures that when the operating components are not required, the working fluid can be circulated through the bypass pipe instead of component. Note: Only one bypass per half loop is required.
+\item
+  \textbf{Connectors} -- Connectors are mid-level loop construction objects that are used to connect the various branches in the loops. There are two kinds of connectors: splitter which split the flow into two or more branches, and mixers which mix the flow from two or more branches. A connector pair consists of a splitter and a mixer. A maximum of one connector pair is allowed on each half loop. Connectors will be denoted by using green colored lines in the EnergyPlus schematics used in this guide. (Keywords: \emph{Connector:Mixer, Connector:Splitter})\emph{.}
+\item
+  \textbf{Connectorlists} -- Connectorlists list all the connectors on one side of a loop. (Keyword: \emph{Connectorlist})\emph{.}
+\item
+  \textbf{Components} -- Components are the low-level construction objects in EnergyPlus. Physical objects that are present in the loop are generally called components. Components such as a chiller, cooling tower, and a circulation pump can be considered as the operating/active components. Pipes and ducts can be considered as passive or supporting components. (Keywords: \emph{Chiller:Electric, Pipe:Adiabatic, and many others})\emph{.}
+\item
+  \textbf{Nodes} -- Nodes define the starting and ending points of components and branches.
+\item
+  \textbf{Nodelists} -- Nodelists can be used to list a set of nodes in the loop. These nodelists can then be used for a variety of purposes. For example, a setpoint can be assigned to multiple nodes by referring to a particular nodelist. (Keyword: \emph{Nodelist})\emph{.}
+\item
+  \textbf{Set-point} -- Setpoints are control conditions imposed on node(s) that are monitored by the \emph{SetpointManager} to control the system. (Keyword: \emph{SetpointManager:Scheduled, and others}).
+\item
+  \textbf{Plant equipment operation scheme} -- This object details the mechanism required to control the operation of the plant loop, as well as the availability of the plant equipment under various conditions. (Keyword: \emph{PlantEquipmentOperation:CoolingLoad, and others}).
+\item
+  \textbf{Schedule} -- Schedules allow the user to influence the scheduling of many operational parameters in the loop. For example, a schedule can determine the time period of a simulation, or instruct the load profile object of a plant to import data from a certain external file, among other actions. (Keywords: \emph{Schedule:Compact, Schedule:file})\emph{.}
+\item
+  \textbf{Load Profile} -- A load profile object is used to simulate a demand profile. This object can be used when the load profile of a building is already known. (Keyword: \emph{LoadProfile:Plant}). Note: This object does not allow feedback from the plant conditions to the air system or the zones. However, this object is a great tool for plant-only development and debugging.
+\end{itemize}
diff --git a/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops.tex b/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops.tex
new file mode 100644
index 00000000000..30d8aad7d8c
--- /dev/null
+++ b/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops.tex
@@ -0,0 +1,26 @@
+\chapter{Example System 1: Chiller and Condenser Loops}\label{example-system-1-chiller-and-condenser-loops}
+
+A simple cooling system will be used as an example to demonstrate the process of inputting a system into the input file. The input file for this example can be found under the name: PlantApplicationsGuide\_Example1.idf.
+
+This particular system consists of two unique sub-systems/loops. It contains the \emph{PlantLoop} with the chiller and the load profile, and another \emph{PlantLoop} with the cooling tower. A schedule containing previously obtained simulation loads is used to simulate the demand load profile for this loop (Note: In a more general scenario a cooling coil placed in a building zone would provide the load profile). Flow diagrams along with some keywords from the input file will be used to record to steps that are required to properly input the system into EnergyPlus. The simple line diagram for this system is provided in Figure~\ref{fig:simple-cooling-system-line-diagram}. The complete EnergyPlus schematic for the system is provided in Figure~\ref{fig:energyplus-line-diagram}.
+
+\begin{figure}[hbtp] % fig 12
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image012.png}
+\caption{Simple cooling system line diagram \protect \label{fig:simple-cooling-system-line-diagram}}
+\end{figure}
+
+
+\begin{figure}[hbtp] % fig 13
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image013.png}
+\caption{EnergyPlus line diagram for the simple cooling system \protect \label{fig:energyplus-line-diagram}}
+\end{figure}
+
+The cooling system consists of a chilled water loop which is defined by the \emph{PlantLoop} object, and a condenser loop which is also defined by the \emph{PlantLoop} object. Identification of these loops in the system is critical for the process of modeling the system in the input file the flowchart for loop identification is provided in Figure~\ref{fig:flowchart-for-loop-identification}.
+
+\begin{figure}[hbtp] % fig 14
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image014.png}
+\caption{Flowchart for loop identification \protect \label{fig:flowchart-for-loop-identification}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops/chilled-water-loop.tex b/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops/chilled-water-loop.tex
new file mode 100644
index 00000000000..0be90e7ec2f
--- /dev/null
+++ b/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops/chilled-water-loop.tex
@@ -0,0 +1,119 @@
+\section{Chilled water (CW) loop}\label{chilled-water-cw-loop}
+
+The chilled water loop is constructed by using a \emph{PlantLoop} object\emph{.} This loop uses a water-cooled electric chiller to supply chilled water to the demand side of this loop. As mentioned above, the cooling coil is replaced by a load profile object that contains the demand load profile. The chiller is operated by using set points, plant equipment operation schemes and schedules. Refer to Figure~\ref{fig:simple-line-diagram-for-the-chilled-water} for a simple diagram of the Chilled Water Loop.
+
+\begin{figure}[hbtp] % fig 15
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image015.png}
+\caption{Simple line diagram for the chilled water loop \protect \label{fig:simple-line-diagram-for-the-chilled-water}}
+\end{figure}
+
+\subsection{Flowcharts for the CW Loop Input Process}\label{flowcharts-for-the-cw-loop-input-process}
+
+This series of flow charts serve as a process guide for identifying and inputting the chilled water loop and its components into the input file. Refer to Figure~\ref{fig:energyplus-line-diagram-for-the-chilled-water} for an EnergyPlus schematic of the Chilled Water Loop.
+
+\begin{figure}[hbtp] % fig 16
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image016.png}
+\caption{EnergyPlus line diagram for the chilled water loop \protect \label{fig:energyplus-line-diagram-for-the-chilled-water}}
+\end{figure}
+
+The ``PlantLoop'' object is entered into the input file, with water as the working fluid. The supply side of the chilled water loop is then input into the system followed by the demand side. A flow chart for separating the half loops in the loop is provided in Figure~\ref{fig:simple-flowchart-for-separation-of-half-loops}.
+
+\begin{figure}[hbtp] % fig 17
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image017.png}
+\caption{Simple flowchart for separation of half loops in the chilled water loop \protect \label{fig:simple-flowchart-for-separation-of-half-loops}}
+\end{figure}
+
+\subsubsection{CW Loop Supply Side Loop Construction}\label{cw-loop-supply-side-loop-construction}
+
+The main components in the supply side of the chilled water loop are the circulation pump for the chilled water and the electric chiller that supplies the chilled water. The set-point is set to the outlet node of this half of the loop; the temperature at this node is controlled to regulate the operation of the chiller. This side of the loop has eight nodes, four components and four branches, while it is not required to define individual node positions in the loop, the components and branches have to be defined with an inlet and an outlet node. Connectors are the objects that connect the branches together and complete the loop. Therefore, the branches and the connectors will set the positions of the nodes in the loop. The EnergyPlus line diagram for the Chilled Water Loop supply side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-supply-side}. The flowchart for supply side branches and components is provided in Figure~\ref{fig:flowchart-for-chilled-water-loop-supply-side-and}. The flowchart for the supply side connectors is provided in Figure~\ref{fig:flowchart-for-chilled-water-loop-supply-side-connectors}.
+
+\begin{figure}[hbtp] % fig 18
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image018.png}
+\caption{EnergyPlus line diagram for the supply side of the chilled water loop \protect \label{fig:energyplus-line-diagram-for-the-supply-side}}
+\end{figure}
+
+\begin{figure}[htbp] % fig 19
+\centering
+\includegraphics{media/image019.png}
+\caption{Flowchart for chilled water loop supply side branches and components \protect \label{fig:flowchart-for-chilled-water-loop-supply-side-and}}
+\end{figure}
+
+\begin{figure}[htbp] % fig 20
+\centering
+\includegraphics{media/image020.png}
+\caption{Flowchart for chilled water loop supply side connectors \protect \label{fig:flowchart-for-chilled-water-loop-supply-side-connectors}}
+\end{figure}
+
+\subsubsection{CW Loop Demand Side Loop Construction}\label{cw-loop-demand-side-loop-construction}
+
+The demand side of the loop is entered next. The main component in this side of the loop is the cooling load profile(instead of the cooling coil). This load profile is input by using a Schedule:Compact object which indicates the hourly cooling loads for the annual run period. In a more general scenario a cooling coil would take the place of the load profile and the cooling load will be simulated from the data obtained in the building system energy simulation. Apart from the load profile, the structure of the loop is very similar to the structure of the supply side. This side of the loop also has eight nodes, four components, and four branches. An EnergyPlus schematic for the demand side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-demand-side}. The flowchart for demand side branch definition is provided in Figure~\ref{fig:flowchart-for-chilled-water-loop-demand-side-and}. The flowchart for the demand side connectors is provided in Figure~\ref{fig:flowchart-for-chilled-water-loop-demand-side-connectors}.
+
+\begin{figure}[htbp] % fig 21
+\centering
+\includegraphics{media/image021.png}
+\caption{EnergyPlus line diagram for the demand side of the chilled water loop \protect \label{fig:energyplus-line-diagram-for-the-demand-side}}
+\end{figure}
+
+\begin{figure}[htbp] % fig 22
+\centering
+\includegraphics{media/image022.png}
+\caption{Flowchart for chilled water loop demand side branches and components \protect \label{fig:flowchart-for-chilled-water-loop-demand-side-and}}
+\end{figure}
+
+\begin{figure}[htbp] % fig 23
+\centering
+\includegraphics{media/image023.png}
+\caption{Flowchart for chilled water loop demand side connectors \protect \label{fig:flowchart-for-chilled-water-loop-demand-side-connectors}}
+\end{figure}
+
+As shown in the flowchart above, the load profile is attached to the chilled water loop at its designated position (the LoadProfile:Plant object can be used just like any other component) on the demand side of the loop.
+
+\subsection{Flowcharts for CW Loop Controls}\label{flowcharts-for-cw-loop-controls}
+
+The chilled water loop is operated by using set-points, plant equipment operation schemes and schedules.
+
+\subsubsection{Chilled Water Loop Schedules}\label{chilled-water-loop-schedules}
+
+The chilled water loop uses two different schedules to operate properly. The \emph{Chiller AlwaysOnSchedule} is a compact schedule that keeps the chiller ON at all times of the day for a whole year. This compact schedule uses a discrete \emph{ScheduleTypeLimit} (\emph{CW Loop On/Off)} which defines that the value of On is 1 and that of Off is 0. This plant loop also uses another compact schedule named \emph{CW Loop Temp Schedule} to set the temperature at the chilled water loop outlet node. This schedule uses a schedule type limit named \emph{CW Loop Any Number}. The flowchart for chilled water loop schedule definition is provided in Figure~\ref{fig:flowchart-for-chilled-water-loop-schedules}.
+
+\emph{~}
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image024.png}
+\caption{Flowchart for chilled water loop schedules \protect \label{fig:flowchart-for-chilled-water-loop-schedules}}
+\end{figure}
+
+\subsubsection{Chilled Water Loop Plant Equipment Operation Schemes}\label{chilled-water-loop-plant-equipment-operation-schemes}
+
+The \emph{PlantEquipmentOperationschemes} object uses the \emph{Chiller AlwaysOnSchedule} and the \emph{CW Loop Cooling Load} objects to set the range of the demand load for which the chiller can be operated during the simulation period. Operation schemes are especially useful and crucial when using multiple active components. For example, the performance of multiple chillers can be optimized by carefully managing the load ranges on each of the chillers. A flowchart detailing the chilled water loop plant equipment operation schemes is provided in Figure~\ref{fig:flowchart-for-chilled-water-loop-plant-equipment}.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image025.png}
+\caption{Flowchart for chilled water loop plant equipment operation schemes \protect \label{fig:flowchart-for-chilled-water-loop-plant-equipment}}
+\end{figure}
+
+\subsubsection{Chilled Water Loop Setpoints}\label{chilled-water-loop-setpoints}
+
+The \emph{Chilled Water Loop Setpoint Manager} uses the \emph{CW Loop Temp Schedule} to set a temperature control point at the \emph{CW Supply Outlet Node}. This setpoint allows the program to control the temperature at the node by operating the components in the chilled water loop. ~Since, setpoint managers are high-level control objects, their usefulness is realized in much more complex systems, where multiple nodes have to be monitored in order to operate the system properly. A flowchart for chilled water loop setpoints is provided in Figure~\ref{fig:flowchart-for-chilled-water-loop-setpoints}.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image026.png}
+\caption{Flowchart for chilled water Loop setpoints \protect \label{fig:flowchart-for-chilled-water-loop-setpoints}}
+\end{figure}
+
+\subsubsection{Chilled Water Loop Sizing}\label{chilled-water-loop-sizing}
+
+The chilled water loop is sized such a way that the design loop exit temperature is 7 degrees Celsius, and the loop design temperature difference is 5 degrees Celsius. A flowchart for the chilled water loop sizing is provided in Figure~\ref{fig:flowchart-for-chilled-water-loop-sizing}. Note: Since the Load Profile object does not demand any feedback from the \emph{PlantLoop} object, the chilled water loop does not necessarily need to be sized (This object is commented out in the example file). The sizing shown here is just an example of how the object class can be used in EnergyPlus.
+
+\begin{figure}[htbp]
+\centering
+\includegraphics{media/image027.png}
+\caption{Flowchart for chilled water loop sizing \protect \label{fig:flowchart-for-chilled-water-loop-sizing}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops/condenser-loop.tex b/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops/condenser-loop.tex
new file mode 100644
index 00000000000..28170478f94
--- /dev/null
+++ b/doc/plant-application-guide/src/example-01-chiller-and-condenser-loops/condenser-loop.tex
@@ -0,0 +1,121 @@
+\section{Condenser Loop}\label{condenser-loop}
+
+The condenser loop uses a cooling tower to supply cooling water to the water-cooled electric chiller in the chilled water loop. Hence, the supply side of this loop consists of the cooling tower and the demand side consists of the electric chiller. The schedules for this loop are almost identical to the ones applied on the CW loop. They dictate that the cooling tower also works around the year. The plant equipment schemes specify the cooling capacity/load of the cooling tower. The operation of the cooling tower is managed by monitoring the outdoor air wet bulb (air cooled condenser) temperature at the location of the simulation. The structure of this loop is very similar to that of the chilled water loop, the only difference being the main components in the loop. A simple line diagram of the condenser loop is provided in Figure~\ref{fig:simple-line-diagram-for-the-condenser-loop-002}.
+
+\begin{figure}[hbtp] % fig 28
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image028.png}
+\caption{Simple line diagram for the condenser loop \protect \label{fig:simple-line-diagram-for-the-condenser-loop-002}}
+\end{figure}
+
+\subsection{Flowcharts for the Condenser Loop Input Process}\label{flowcharts-for-the-condenser-loop-input-process-001}
+
+As discussed in Section 1 the supply side and the demand side of the loop are modeled separately by following the process provided in the flow chart. The flow charts for this loop are provided below.
+
+A \emph{PlantLoop} object is used to model the condenser loop with the chiller and the cooling tower as its main components. The working fluid is water. This loop is also sized such that the loop exit temperature is set to 20 degrees Celsius and the loop design temperature difference is 5 degrees Celsius. The chiller serves as the bridge between the chilled water loop and the condenser loop. This is achieved by managing the nodal connections on the chiller, hence the chiller appears on two branches in the system (supply branch of the CW loop, and the demand branch of the condenser loop). The EnergyPlus line diagram for the condenser loop is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-condenser-002}. A simple flow chart for the separation of the half loops is provided in Figure~\ref{fig:simple-flowchart-for-separation-of-half-loops-001}.
+
+\begin{figure}[hbtp] % fig 29
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image029.png}
+\caption{EnergyPlus line diagram for the condenser loop \protect \label{fig:energyplus-line-diagram-for-the-condenser-002}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 30
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image030.png}
+\caption{Simple flowchart for separation of half loops in the condenser loop \protect \label{fig:simple-flowchart-for-separation-of-half-loops-001}}
+\end{figure}
+
+\subsubsection{Condenser Loop Supply Side Construction}\label{condenser-loop-supply-side-construction-001}
+
+The main components in the supply side of the condenser loop are the condenser circulation pump and the cooling tower. The temperature set-point is set at the outlet node, where the outdoor air wet bulb temperature is monitored to regulate the operation of the cooling tower. The outdoor air conditions are obtained from the weather information file during the simulation. This side of the loop has eight nodes and four branches. An EnergyPlus diagram for the condenser loop supply side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-supply-side-003}. The flowchart for supply side branch definition is provided in Figure~\ref{fig:flowchart-for-condenser-supply-side-branches}. The flowchart for the supply side connectors is provided in Figure~\ref{fig:condenser-loop-supply-side-connectors}.
+
+\begin{figure}[hbtp] % fig 31
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image031.png}
+\caption{EnergyPlus line diagram for the supply side of the condenser loop \protect \label{fig:energyplus-line-diagram-for-the-supply-side-003}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 32
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image032.png}
+\caption{Flowchart for condenser supply side branches and components \protect \label{fig:flowchart-for-condenser-supply-side-branches}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 33
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image033.png}
+\caption{Condenser loop supply side connectors \protect \label{fig:condenser-loop-supply-side-connectors}}
+\end{figure}
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+\subsubsection{Condenser Loop Demand Side Construction}\label{condenser-loop-demand-side-construction-001}
+
+The central component of the demand side is the chiller. The flowchart for the construction of the demand side is also provided below. The schedules for this side do not need to be specified, because the schedules that apply to the chiller also apply to this side of the condenser loop. This side of the loop also contains eight nodes and four branches. An EnergyPlus schematic for the demand side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-demand-side}. The flowchart for demand side branch definition is provided in Figure~\ref{fig:condenser-loop-demand-side-construction}. The flowchart for the demand side connectors is provided in Figure~\ref{fig:condenser-loop-demand-side-schedules}.
+
+\begin{figure}[hbtp] % fig 34
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image034.png}
+\caption{EnergyPlus line diagram for the demand side of the condenser loop \protect \label{fig:energyplus-line-diagram-for-the-demand-side}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 35
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image035.png}
+\caption{Condenser loop demand side construction \protect \label{fig:condenser-loop-demand-side-construction}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 36
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image036.png}
+\caption{Condenser loop demand side schedules, equipment schemes and setpoints \protect \label{fig:condenser-loop-demand-side-schedules}}
+\end{figure}
+
+\subsection{Flowcharts for Condenser Loop Controls}\label{flowcharts-for-condenser-loop-controls-001}
+
+The cooling tower is also scheduled similar to the chiller because both of these units have to work together in order to satisfy the cooling load. The operation of the cooling tower is determined by using a set point at the condenser supply exit node. This set point monitors the temperature at this node as well as the outdoor air wet bulb temperature to operate the cooling tower. The flowchart for the schedules, plant equipment schemes, and the set points are also provided below.
+
+\subsubsection{Condenser Loop Schedules}\label{condenser-loop-schedules-001}
+
+The \emph{Tower AlwaysOnSchedule} is a compact schedule that keeps the tower ON at all times of the day for a whole year, this compact schedule uses a discrete \emph{scheduletypelimit} (\emph{Tower On/Off)} which defines that the value of On is 1 and that of Off is 0. A flowchart for condenser loop schedules is provided in Figure~\ref{fig:condenser-loop-schedules}.
+
+\emph{~}
+
+\begin{figure}[hbtp] % fig 37
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image037.png}
+\caption{Condenser loop schedules \protect \label{fig:condenser-loop-schedules}}
+\end{figure}
+
+\subsubsection{Condenser Loop Plant Equipment Operation Schemes}\label{condenser-loop-plant-equipment-operation-schemes-001}
+
+The plant equipment operation schemes for the condenser loop are very similar to those of the chilled water loop. The \emph{PlantEquipmentOperationschemes} object uses the \emph{Tower AlwaysOnSchedule} and the \emph{Tower Load} objects to set the range of the demand loads for which the cooling tower is operated during the simulation period. A flowchart for the condenser loop plant equipment operation schemes is provided in Figure~\ref{fig:condenser-loop-plant-equipment-operation}.
+
+\begin{figure}[hbtp] % fig 38
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image038.png}
+\caption{Condenser loop plant equipment operation schemes \protect \label{fig:condenser-loop-plant-equipment-operation}}
+\end{figure}
+
+\subsubsection{Condenser Loop Setpoints}\label{condenser-loop-setpoints-001}
+
+The \emph{Condensercontrol setpointmanager} places a temperature setpoint at the \emph{Condenser Supply Outlet Node.} The temperature at this point is controlled with respect to the outdoor air wet bulb temperature at that point in the simulation. The outdoor air wet bulb temperature is obtained from the weather data at the location of the simulation. A flowchart for the condenser loop setpoint is provided in Figure~\ref{fig:condenser-loop-setpoints}.
+
+\begin{figure}[hbtp] % fig 39
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image039.png}
+\caption{Condenser loop setpoints \protect \label{fig:condenser-loop-setpoints}}
+\end{figure}
+
+\subsubsection{Condenser Loop Sizing}\label{condenser-loop-sizing-000}
+
+The condenser loop is sized such that the loop exit temperature is 20 degrees Celsius and the loop temperature difference is 5 degrees Celsius. A flowchart for condenser loop sizing is provided in Figure~\ref{fig:condenser-loop-sizing}.
+
+\begin{figure}[hbtp] % fig 40
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image040.png}
+\caption{Condenser loop sizing \protect \label{fig:condenser-loop-sizing}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/example-02-thermal-energy-storage.tex b/doc/plant-application-guide/src/example-02-thermal-energy-storage.tex
new file mode 100644
index 00000000000..5ecbb23d7c3
--- /dev/null
+++ b/doc/plant-application-guide/src/example-02-thermal-energy-storage.tex
@@ -0,0 +1,41 @@
+\chapter{Example System 2: Thermal Energy Storage}\label{example-system-2-thermal-energy-storage}
+
+This system will detail the process required to model a Plant Loop coupled with Thermal Energy Storage (TES) in EnergyPlus. The input file for this example can be found under the name: PlantApplicationsGuide\_Example2.idf.
+
+The TES tank will be charged by using a chiller loop, which will in turn be cooled by a condenser loop. The schedules for this system are setup such that the TES tank will be charged by the chiller during the night and then the stored chilled water is used to satisfy the building cooling load during the day. The TES tank used in this system is a stratified tank. This system also includes one heating loop which satisfies the heating load. The cooling and heating system operate in conjunction with an air loop that is spread across a total of five zones. The air loop modeling will not be discussed in this guide. This system consists of a total of three separate plant loops, the cooling side is comprised of two loops and the heating side contains one loop. A simple line diagram for the cooling system is provided in Figure~\ref{fig:simple-line-diagram-for-cooling-system}. The EnergyPlus line diagram for the cooling loop is provided in Figure~\ref{fig:energyplus-line-diagram-for-cooling-system}. A simple line diagram for the heating loop is provided in Figure~\ref{fig:simple-line-diagram-for-heating-loop}, whereas its EnergyPlus line diagram is provided in Figure~\ref{fig:energyplus-line-diagram-for-heating-loop}.
+
+\begin{figure}[htbp] % fig 41
+\centering
+\includegraphics{media/image041.png}
+\caption{Simple line diagram for cooling system \protect \label{fig:simple-line-diagram-for-cooling-system}}
+\end{figure}
+
+\begin{figure}[htbp] % fig 42
+\centering
+\includegraphics{media/image042.png}
+\caption{Simple line diagram for heating loop \protect \label{fig:simple-line-diagram-for-heating-loop}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 43
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image043.png}
+\caption{EnergyPlus line diagram for cooling system \protect \label{fig:energyplus-line-diagram-for-cooling-system}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 44
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image044.png}
+\caption{EnergyPlus line diagram for heating loop \protect \label{fig:energyplus-line-diagram-for-heating-loop}}
+\end{figure}
+
+SHWSys1
+
+The cooling side of the system will be modeled first. The primary cooling loop (named ``CoolSysPrimary'' in the input file) uses the chiller as the supply side component to charge the TES tank. The chilled water that is stored in the TES tank is then supplied to the cooling coil. A cooling tower that operates on the supply side of the condenser loop (named ``Condenser Loop'') supplies the cooling water to the chiller that is used in the primary cooling loop. These two loops serve as the cooling system for this building. This system will be modeled first with emphasis placed on the primary cooling loop. In particular the schedules used for the charging and discharging the TES tank play a crucial role in the efficient operation of the system.
+
+The building also has one heating loop. The heating loop (named ``HeatSys 1'') uses a boiler to provide hot water to five heating coils that are located in the five zones. This heating loop also supplies hot water to the reheat coil. A flow chart for loop identification is provided in Figure~\ref{fig:flowchart-for-loop-identification-001}.
+
+\begin{figure}[hbtp] % fig 45
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image045.png}
+\caption{Flowchart for loop identification \protect \label{fig:flowchart-for-loop-identification-001}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/example-02-thermal-energy-storage/condenser-loop-condenser-loop-cooling-tower.tex b/doc/plant-application-guide/src/example-02-thermal-energy-storage/condenser-loop-condenser-loop-cooling-tower.tex
new file mode 100644
index 00000000000..19a555aa8c1
--- /dev/null
+++ b/doc/plant-application-guide/src/example-02-thermal-energy-storage/condenser-loop-condenser-loop-cooling-tower.tex
@@ -0,0 +1,113 @@
+\section{\texorpdfstring{Condenser Loop (\emph{Condenser Loop}) - Cooling Tower}{Condenser Loop (Condenser Loop) - Cooling Tower}}\label{condenser-loop-condenser-loop---cooling-tower}
+
+The Condenser Loop is constructed by using a \emph{PlantLoop} object. It uses a cooling tower (modeled by using a \emph{CoolingTower:SingleSpeed} object class) and a constant speed pump (modeled by using a \emph{Pump:ConstantSpeed)} to supply cooling water to the electric chiller (modeled by using a \emph{Chiller:Electric} object). Therefore, the supply side of the loop contains the Cooling Tower and the demand side contains the electric chiller. The loop is operated by using plant equipment operation schemes, and schedules. ~Refer to Figure~\ref{fig:simple-line-diagram-for-the-condenser-loop} for a simple diagram of the Condenser Loop.
+
+\begin{figure}[hbtp] % fig 61
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image061.png}
+\caption{Simple line diagram for the condenser loop \protect \label{fig:simple-line-diagram-for-the-condenser-loop}}
+\end{figure}
+
+\subsection{Flowcharts for the Condenser Loop Input Process}\label{flowcharts-for-the-condenser-loop-input-process}
+
+This series of flowcharts serve as a guide for identifying and inputting the Condenser Loop and its components into the input file. The EnergyPlus line diagram for this loop is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-condenser}. A simple flowchart for the separation of the half loops is provided in Figure~\ref{fig:simple-flow-chart-for-separation-on-half}.
+
+\begin{figure}[hbtp] % fig 62
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image062.png}
+\caption{EnergyPlus line diagram for the condenser loop \protect \label{fig:energyplus-line-diagram-for-the-condenser}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 63
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image063.png}
+\caption{Simple flow chart for separation on half loops in the condenser loop \protect \label{fig:simple-flow-chart-for-separation-on-half}}
+\end{figure}
+
+\subsubsection{Condenser Loop Supply Side Construction}\label{condenser-loop-supply-side-construction}
+
+The main components on the supply side half loop for the Condenser Loop are the Cooling Tower that supplies the cooling water and the constant speed pump that circulates the cooling water through the loop. This half loop supplies cooling water to the electric chiller on the demand side half loop. The supply side half loop contains four components, four branches, eight nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the Condenser loop supply side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-supply-side-001}. The flowchart for supply side branches and components is provided in Figure~\ref{fig:flowchart-for-condenser-loop-supply-side-branches-and}. The flowchart for supply side connectors is provided in Figure~\ref{fig:flowchart-for-condenser-loop-supply-side-connectors}.
+
+\begin{figure}[hbtp] % fig 64
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image064.png}
+\caption{EnergyPlus line diagram for the supply side of the condenser loop \protect \label{fig:energyplus-line-diagram-for-the-supply-side-001}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 65
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image065.png}
+\caption{Flowchart for condenser loop supply side branches and components \protect \label{fig:flowchart-for-condenser-loop-supply-side-branches-and}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 66
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image066.png}
+\caption{Flowchart for condenser loop supply side connectors \protect \label{fig:flowchart-for-condenser-loop-supply-side-connectors}}
+\end{figure}
+
+\subsubsection{Condenser Loop Demand Side Construction}\label{condenser-loop-demand-side-construction}
+
+The main component on the demand side half loop is the Chiller that uses the cooling water supplied by the cooling tower. The chiller in turn is used to supply chilled water in the Primary Cooling loop. ~This side of the loop also has eight nodes, four components, four branches and one splitter-mixer pair. An EnergyPlus schematic for the demand side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-demand-side-001}. The flowchart for demand side branch definition is provided in Figure~\ref{fig:flowchart-for-condenser-loop-demand-side-branches-and}. The flowchart for the demand side connectors is provided in Figure~\ref{fig:flowchart-for-condenser-loop-demand-side-connectors}.
+
+\begin{figure}[hbtp] % fig 67
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image067.png}
+\caption{EnergyPlus line diagram for the demand side of the condenser loop \protect \label{fig:energyplus-line-diagram-for-the-demand-side-001}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 68
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image068.png}
+\caption{Flowchart for condenser loop demand side branches and components \protect \label{fig:flowchart-for-condenser-loop-demand-side-branches-and}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 69
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image069.png}
+\caption{Flowchart for condenser loop demand side connectors \protect \label{fig:flowchart-for-condenser-loop-demand-side-connectors}}
+\end{figure}
+
+\subsection{Flowcharts for Condenser Loop Controls}\label{flowcharts-for-condenser-loop-controls}
+
+The Condenser Loop is operated by using set-points, plant equipment operation schemes and schedules.
+
+\subsubsection{Condenser Loop Schedules}\label{condenser-loop-schedules}
+
+The flowchart for condenser loop schedule definition is provided in Figure~\ref{fig:flowchart-for-condenser-loop-schedules}. The Condenser loop uses one schedule to operate properly. \emph{PlantOnSchedule} is a compact schedule that keeps the Cooling Tower On at all times of the day, this compact schedule uses a discrete \emph{ScheduleTypeLimit} (\emph{On/Off)} which defines that the value of On is 1 and that of Off is 0.
+
+\begin{figure}[hbtp] % fig 70
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image070.png}
+\caption{Flowchart for condenser loop schedules \protect \label{fig:flowchart-for-condenser-loop-schedules}}
+\end{figure}
+
+\subsubsection{Condenser Loop Plant Equipment Operation Schemes}\label{condenser-loop-plant-equipment-operation-schemes}
+
+The \emph{PlantEquipmentOperationschemes} object uses the \emph{PlantOnSchedule} and the \emph{Condenser Loop Operation Scheme} objects to set the range of demand loads for which the cooling tower is operated during the simulation period. A flowchart detailing the Condenser Loop plant equipment operation schemes is provided in Figure~\ref{fig:flowchart-for-condenser-loop-plant-equipment-operation}.
+
+\begin{figure}[hbtp] % fig 71
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image071.png}
+\caption{Flowchart for condenser loop plant equipment operation schemes \protect \label{fig:flowchart-for-condenser-loop-plant-equipment-operation}}
+\end{figure}
+
+\subsubsection{Condenser Loop Setpoints}\label{condenser-loop-setpoints}
+
+The \emph{MyCondenserControl} setpointmanager places a temperature setpoint at the \emph{Condenser Supply Outlet Node.} The temperature at this point is controlled with respect to the outdoor air wet bulb temperature at that point in the simulation. The outdoor air wet bulb temperature is obtained from the weather data at the location of the simulation. The minimum setpoint temperature is 5 degrees Celsius and the maximum setpoint temperature is 80 degrees Celsius. A flowchart for Secondary Cooling loop setpoints is provided in Figure~\ref{fig:flowchart-for-condenser-loop-setpoints}.
+
+\begin{figure}[hbtp] % fig 72
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image072.png}
+\caption{Flowchart for condenser loop setpoints \protect \label{fig:flowchart-for-condenser-loop-setpoints}}
+\end{figure}
+
+\subsubsection{Condenser Loop Sizing}\label{condenser-loop-sizing}
+
+The Condenser loop is sized such a way that the design loop exit temperature is 29.4 degrees Celsius, and the loop design temperature difference is 5.6 degrees Celsius. A flowchart for the chilled water loop sizing is provided in Figure~\ref{fig:flowchart-for-condenser-loop-sizing}.
+
+\begin{figure}[hbtp] % fig 73
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image073.png}
+\caption{Flowchart for condenser loop sizing \protect \label{fig:flowchart-for-condenser-loop-sizing}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/example-02-thermal-energy-storage/heating-loop-heatsys1-boiler.tex b/doc/plant-application-guide/src/example-02-thermal-energy-storage/heating-loop-heatsys1-boiler.tex
new file mode 100644
index 00000000000..cdbb3b4e1d2
--- /dev/null
+++ b/doc/plant-application-guide/src/example-02-thermal-energy-storage/heating-loop-heatsys1-boiler.tex
@@ -0,0 +1,113 @@
+\section{\texorpdfstring{Heating Loop (\emph{HeatSys1}) - Boiler}{Heating Loop (HeatSys1) - Boiler}}\label{heating-loop-heatsys1---boiler}
+
+The Heating loop is constructed by using a \emph{PlantLoop} object. It uses an electric boiler to (modeled by using a \emph{Boiler:HotWater} object class) to supply hot water to the five heating coils placed in the five zones of the building (modeled by using a \emph{Coil:Heating:Water} object class). Therefore, the supply side of the loop contains the hot water boiler and the demand side contains a total of six heating coils. The loop is operated by using plant equipment operation schemes, and schedules. ~Refer to Figure~\ref{fig:simple-line-diagram-for-the-heating-loop} for a simple diagram of the Condenser Loop.
+
+\begin{figure}[hbtp] % fig 74
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image074.png}
+\caption{Simple line diagram for the heating loop \protect \label{fig:simple-line-diagram-for-the-heating-loop}}
+\end{figure}
+
+\subsection{Flowcharts for the Heating Loop Input Process}\label{flowcharts-for-the-heating-loop-input-process}
+
+This series of flowcharts serve as a guide for identifying and inputting the Heating loop and its components into the input file. The EnergyPlus line diagram for this loop is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-heating-loop}. A simple flowchart for the separation of the half loops is provided in Figure~\ref{fig:simple-flow-chart-for-separation-on-half-002}.
+
+\begin{figure}[hbtp] % fig 75
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image075.png}
+\caption{EnergyPlus line diagram for the heating loop \protect \label{fig:energyplus-line-diagram-for-the-heating-loop}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 76
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image076.png}
+\caption{Simple flow chart for separation on half loops in the heating loop \protect \label{fig:simple-flow-chart-for-separation-on-half-002}}
+\end{figure}
+
+\subsubsection{Heating Loop Supply Side Construction}\label{heating-loop-supply-side-construction}
+
+The main components on the supply side half loop for the Heating Loop are the hot water boiler that generates hot water and the variable speed pump that circulates the hot water through the loop. This half loop supplies hot water to five heating coils on the demand side half loop. The supply side half loop contains four components, four branches, eight nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the Primary Cooling loop supply side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-supply-side-004}. The flowchart for supply side branches and components is provided in Figure~\ref{fig:flowchart-for-heating-loop-supply-side-branches-and}. The flowchart for supply side connectors is provided in Figure~\ref{fig:flowchart-for-heating-loop-supply-side-connectors}.
+
+\begin{figure}[hbtp] % fig 77
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image077.png}
+\caption{EnergyPlus line diagram for the supply side of the heating loop \protect \label{fig:energyplus-line-diagram-for-the-supply-side-004}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 78
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image078.png}
+\caption{Flowchart for heating loop supply side branches and components \protect \label{fig:flowchart-for-heating-loop-supply-side-branches-and}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 79
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image079.png}
+\caption{Flowchart for heating loop supply side connectors \protect \label{fig:flowchart-for-heating-loop-supply-side-connectors}}
+\end{figure}
+
+\subsubsection{Heating Loop Demand Side Construction}\label{heating-loop-demand-side-construction}
+
+The demand side half loop contains five heating coils that heat the air in the different zones of the building by using the hot water that is supplied by the hot water boiler. This side of the loop also has sixteen nodes, eight components, eight branches, and one splitter-mixer pair. An EnergyPlus schematic for the demand side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-demand-side-004}. The flowchart for demand side branch definition is provided in Figure~\ref{fig:flowchart-for-heating-loop-demand-side-branches-and}. The flowchart for the demand side connectors is provided in Figure~\ref{fig:flowchart-for-heating-loop-demand-side-connectors}.
+
+\begin{figure}[hbtp] % fig 80
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image080.png}
+\caption{EnergyPlus line diagram for the demand side of the heating loop \protect \label{fig:energyplus-line-diagram-for-the-demand-side-004}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 81
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image081.png}
+\caption{Flowchart for heating loop demand side branches and components \protect \label{fig:flowchart-for-heating-loop-demand-side-branches-and}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 82
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image082.png}
+\caption{Flowchart for heating loop demand side connectors \protect \label{fig:flowchart-for-heating-loop-demand-side-connectors}}
+\end{figure}
+
+\subsection{Flowcharts for Heating Loop Controls}\label{flowcharts-for-heating-loop-controls}
+
+The Heating Loop is operated by using set-points, plant equipment operation schemes and schedules.
+
+\subsubsection{Heating Loop Schedules}\label{heating-loop-schedules}
+
+The flowchart for Primary Heating loop schedule definition is provided in Figure~\ref{fig:flowchart-for-heating-loop-schedules}. The Heating Loop uses three different schedules to operate properly. \emph{PlantOnSchedule} is a compact schedule that uses a discrete \emph{ScheduleTypeLimit} (\emph{On/Off)} which defines that the value of ON is 1 and that of Off is 0. This plant loop also uses another compact schedule named \emph{HW Loop Temp Schedule} to declare that the temperature at the heating loop outlet and the boiler outlet to be 82 degrees Celsius. This schedule uses a schedule type limit named \emph{Temperature,} which defines the loop upper and lower temperature limits. The compact schedule \emph{ALWAYS\_ON} dictates that the boiler and the cooling coils are On at all times of the day. This schedule uses the \emph{ScheduleTypeLimit (Fraction)} to set the fractional flow rate of the components to 1.
+
+\begin{figure}[hbtp] % fig 83
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image083.png}
+\caption{Flowchart for heating loop schedules \protect \label{fig:flowchart-for-heating-loop-schedules}}
+\end{figure}
+
+\subsubsection{Heating Loop Plant Equipment Operation Schemes}\label{heating-loop-plant-equipment-operation-schemes}
+
+The \emph{PlantEquipmentOperationschemes} object uses the \emph{PlantOnSchedule} and the \emph{HeatSys1 Operation Scheme} objects to set the range of the demand loads for which the boiler is operated during the simulation period. Operation schemes are especially useful and crucial when using multiple active components but it is required to enter set up a plant equipment operation scheme for every \emph{PlantLoop} that is used in a system. A flowchart detailing the heating loop plant equipment operation scheme is provided in Figure~\ref{fig:flowchart-for-heating-loop-plant-equipment-operation}.
+
+\begin{figure}[hbtp] % fig 84
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image084.png}
+\caption{Flowchart for heating loop plant equipment operation schemes \protect \label{fig:flowchart-for-heating-loop-plant-equipment-operation}}
+\end{figure}
+
+\subsubsection{Heating Loop Setpoints}\label{heating-loop-setpoints}
+
+The \emph{HeatSys1 Loop Setpoint Manager} uses the \emph{HW Loop Temp Schedule} to set a temperature control point at the \emph{HeatSys1 Supply Outlet Node}. This setpoint allows the program to control the temperature (set to 82 degrees Celsius) at the node by operating the components in the Heating loop. The Heating Loop also uses another schedule (\emph{HeatSys1 Boiler Setpoint Manager)} to set the temperature of the boiler outlet to 82 degrees Celsius. If the \emph{HeatSys1 Boiler Setpoint Manager} is not entered the program assumes the overall loop setpoint for the boiler outlet node. Since, setpoint managers are high-level control objects, their usefulness is realized in much more complex systems, where multiple nodes have to be monitored in order to operate the system properly. A flowchart for heating loop setpoints is provided in Figure~\ref{fig:flowchart-for-heating-loop-setpoints}.
+
+\begin{figure}[hbtp] % fig 85
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image085.png}
+\caption{Flowchart for heating loop setpoints \protect \label{fig:flowchart-for-heating-loop-setpoints}}
+\end{figure}
+
+\subsubsection{Heating Loop Sizing}\label{heating-loop-sizing}
+
+The Heating Loop is sized such a way that the design loop exit temperature is 82.0 degrees Celsius, and the loop design temperature difference is 11.0 degrees Celsius. A flowchart for the chilled water loop sizing is provided in Figure~\ref{fig:flowchart-for-heating-loop-sizing}.
+
+\begin{figure}[hbtp] % fig 86
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image086.png}
+\caption{Flowchart for heating loop sizing \protect \label{fig:flowchart-for-heating-loop-sizing}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/example-02-thermal-energy-storage/primary-cooling-loop-coolsysprimary-chiller.tex b/doc/plant-application-guide/src/example-02-thermal-energy-storage/primary-cooling-loop-coolsysprimary-chiller.tex
new file mode 100644
index 00000000000..26a9db464f7
--- /dev/null
+++ b/doc/plant-application-guide/src/example-02-thermal-energy-storage/primary-cooling-loop-coolsysprimary-chiller.tex
@@ -0,0 +1,131 @@
+\section{\texorpdfstring{Primary Cooling Loop (\emph{CoolSysPrimary}) - Chiller}{Primary Cooling Loop (CoolSysPrimary) - Chiller}}\label{primary-cooling-loop-coolsysprimary---chiller}
+
+The primary cooling system is constructed by using a \emph{PlantLoop} object. It uses an electric chiller that generates chilled water which is used to charge the TES tank at night. The chilled water stored in the TES tank is later used during the peak hours to satisfy the demand loads. Therefore, the supply side of the loop contains the electric chiller and the charge side of the TES tank. The demand side loop contains the cooling coil. The loop is operated by using plant equipment operation schemes, and schedules. Refer to Figure~\ref{fig:simple-line-diagram-for-the-primary-cooling} for a simple diagram of the Primary Cooling Loop.
+
+\begin{figure}[hbtp] % fig 46
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image046.png}
+\caption{Simple line diagram for the primary cooling system \protect \label{fig:simple-line-diagram-for-the-primary-cooling}}
+\end{figure}
+
+\subsection{Flowcharts for the Primary Cooling Loop Input Process}\label{flowcharts-for-the-primary-cooling-loop-input-process}
+
+This series of flowcharts serve as a guide for identifying and inputting the CoolSysPrimary loop and its components into the input file. The working fluid in this loop is water. The important area for this loop is its controls. The EnergyPlus line diagram for this loop is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-primary-001}. A simple flowchart for the separation of the half loops is provided in Figure~\ref{fig:simple-flowchart-for-the-separation-of-half-001}.
+
+\begin{figure}[hbtp] % fig 47
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image047.png}
+\caption{EnergyPlus line diagram for the primary cooling system \protect \label{fig:energyplus-line-diagram-for-the-primary-001}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 48
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image048.png}
+\caption{Simple flowchart for the separation of half-loops in the primary cooling system \protect \label{fig:simple-flowchart-for-the-separation-of-half-001}}
+\end{figure}
+
+\subsubsection{CoolSysPrimary Supply Side Loop Construction}\label{coolsysprimary-supply-side-loop-construction}
+
+The main components on the supply side half loop for the primary cooling system are the electric chiller that supplies the chilled water, the variable speed pump that circulates the chilled water through the loop, and the TES tank that stores the supplied chilled water. This half loop supplies chilled water to the cooling coil which is placed on the demand side half loop. The supply side half loop contains five components, four branches, nine nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the primary cooling loop supply side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-supply-side-006}. The flowchart for supply side branches and components is provided in Figure~\ref{fig:flowchart-for-primary-cooling-loop-supply-side-branches}. The flowchart for supply side connectors is provided in Figure~\ref{fig:flowchart-for-primary-cooling-loop-supply-side-connectors}.
+
+\begin{figure}[hbtp] % fig 49
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image049.png}
+\caption{EnergyPlus line diagram for the supply side of the primary cooling loop \protect \label{fig:energyplus-line-diagram-for-the-supply-side-006}}
+\end{figure}
+
+\begin{figure}[htbp] % fig 50
+\centering
+\includegraphics{media/image050.png}
+\caption{Flowchart for primary cooling loop supply side branches and components \protect \label{fig:flowchart-for-primary-cooling-loop-supply-side-branches}}
+\end{figure}
+
+\begin{figure}[htbp] % fig 51
+\centering
+\includegraphics{media/image051.png}
+\caption{Flowchart for primary cooling loop supply side connectors \protect \label{fig:flowchart-for-primary-cooling-loop-supply-side-connectors}}
+\end{figure}
+
+\subsubsection{CoolSysPrimary Demand Side Loop Construction}\label{coolsysprimary-demand-side-loop-construction}
+
+The main component on the demand side half loop is the cooling coil which cools the air in the building by using the chilled water that is supplied by the supply side half loop. This side of the loop has eight nodes, four components, four branches, and one splitter mixer pair. An EnergyPlus line diagram for the demand side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-demand-side-006}. The flowchart for demand side branch definition is provided in Figure~\ref{fig:flowchart-for-primary-cooling-loop-demand-side-branches}. The flowchart for the demand side connectors is provided in Figure~\ref{fig:flowchart-for-primary-cooling-loop-demand-side-connectors}.
+
+\begin{figure}[htbp] % fig 52
+\centering
+\includegraphics{media/image052.png}
+\caption{EnergyPlus line diagram for the demand side of the primary cooling loop \protect \label{fig:energyplus-line-diagram-for-the-demand-side-006}}
+\end{figure}
+
+\begin{figure}[htbp] % fig 53
+\centering
+\includegraphics{media/image053.png}
+\caption{Flowchart for primary cooling loop demand side branches and components \protect \label{fig:flowchart-for-primary-cooling-loop-demand-side-branches}}
+\end{figure}
+
+\begin{figure}[htbp] % fig 54
+\centering
+\includegraphics{media/image054.png}
+\caption{Flowchart for primary cooling loop demand side connectors \protect \label{fig:flowchart-for-primary-cooling-loop-demand-side-connectors}}
+\end{figure}
+
+\subsection{Flowcharts for Primary Cooling Loop Controls}\label{flowcharts-for-primary-cooling-loop-controls}
+
+The Primary Cooling loop is operated by using set-points, plant equipment operation schemes and schedules. The TES tank charging schedule is one of the most important schedules in this system.
+
+\subsubsection{CoolSysPrimary Schedules}\label{coolsysprimary-schedules}
+
+The flowchart for Primary Cooling loop schedule definition is provided in Figure 56. The Primary Cooling loop uses five different schedules to operate properly.~ The \emph{PlantOnSchedule} is a compact schedule that keeps the chiller and the TES tank ON at all times of the day, this compact schedule uses a discrete \emph{ScheduleTypeLimit} (\emph{On/Off)} which defines that the value of On is 1 and that of Off is 0. This plant loop also uses another compact schedule named \emph{CW Primary Loop Temp Schedule} declare that the temperature of the chilled water loop outlet flow is 6.7 degrees Celsius at all times. This schedule is used by the setpoint manager (\emph{CoolSysPrimary Loop Setpoint Manager)}. This schedule uses a schedule type limit named \emph{Temperature,} which defines the upper and lower loop temperature limits
+
+The compact schedule \emph{ALWAYS\_ON} dictates that the use/discharge side of the TES tank is On at all times of the day. This schedule uses the \emph{ScheduleTypeLimit (Fraction)} to set the fractional flow rate of the use side. This schedule is used to define the use side availability of the TES tank. The compact schedule \emph{CW Tank Temp Schedule} is input in the TES tank object class to define the limits of the temperature for the chilled water storage tank outlet. This schedule uses the \emph{ScheduleTypeLimit (Temperature)} to define that the temperature at that outlet should be 7.5 degrees Celsius at all times of the day.
+
+The \emph{TES Charge Schedule} is a very important schedule for the functioning of the CoolSysPrimary Loop the schedule from the input file is provided in Figure~\ref{fig:tes-charge-schedule}. The schedule shows that, the on/off \emph{ScheduleTypeLimit} is used to determine if the TES schedule is On or off for a certain period of time. A value of 1.0 means On and a value of 0 means Off. For example, it can be observed from the figure that, for the weekdays the TES tank is charged until 10:00AM, then it is operated during the day from 10:00 AM to 5:00 PM and then it is charged until midnight. The schedule for the other days is also shown in the figure.
+
+\begin{figure}[hbtp] % fig 55
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image055.png}
+\caption{TES Charge Schedule \protect \label{fig:tes-charge-schedule}}
+\end{figure}
+
+\begin{figure}[htbp] % fig 56
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image056.png}
+\caption{Flowchart for primary cooling loop schedules \protect \label{fig:flowchart-for-primary-cooling-loop-schedules}}
+\end{figure}
+
+\subsubsection{CoolSysPrimary Plant Equipment Operation Schemes}\label{coolsysprimary-plant-equipment-operation-schemes}
+
+This loop has two plant equipment operation schemes, one for the chiller and one for the TES tank. The \emph{PlantEquipmentOperationschemes} object uses the \emph{PlantOnSchedule} and the \emph{CoolSysPrimary Operation Scheme} objects to set the range of demand loads for which the chiller is operated during the simulation period. Operation schemes are especially useful and crucial when using multiple active components. For example, the performance of multiple chillers can be optimized by carefully managing the load ranges on each of the chillers. It should be noted that it is required to enter a plant equipment operation scheme for every plant loop in the system. A flowchart detailing the chilled water loop plant equipment operation schemes is provided in Figure~\ref{fig:flowchart-for-chiller-plant-equipment-operation}.
+
+\begin{figure}[htbp] % fig 57
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image057.png}
+\caption{Flowchart for Chiller plant equipment operation schemes \protect \label{fig:flowchart-for-chiller-plant-equipment-operation}}
+\end{figure}
+
+The TES tank operation is modeled here. The \emph{PlantEquipmentOperationschemes} object uses the \emph{PlantOnSchedule} and the \emph{TES Operation Scheme} objects to set the range of the demand loads for which the TES tank is operated during the simulation period. A flowchart detailing the Secondary Cooling Loop plant equipment operation schemes is provided in Figure~\ref{fig:flowchart-for-thermal-energy-storage-plant-equipment-operation}.
+
+\begin{figure}[htbp] % fig 58
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image058.png}
+\caption{Flowchart for Thermal Energy Storage plant equipment operation schemes \protect \label{fig:flowchart-for-thermal-energy-storage-plant-equipment-operation}}
+\end{figure}
+
+\subsubsection{CoolSysPrimary Setpoints}\label{coolsysprimary-setpoints}
+
+The \emph{CoolSysPrimary Loop Setpoint Manager} uses the \emph{CoolSysPrimary Loop Temp Schedule} to set a temperature control point at the \emph{CoolSysPrimary Supply Outlet Node}. This setpoint allows the program to control the temperature at the node by operating the components in the Primary Cooling loop. ~A flowchart for Secondary Cooling loop setpoints is provided in Figure~\ref{fig:flowchart-for-primary-cooling-loop-setpoints}.
+
+\begin{figure}[htbp] % fig 59
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image059.png}
+\caption{Flowchart for primary cooling loop setpoints \protect \label{fig:flowchart-for-primary-cooling-loop-setpoints}}
+\end{figure}
+
+\subsubsection{CoolSysPrimary Sizing}\label{coolsysprimary-sizing}
+
+The chilled water loop is sized such a way that the design loop exit temperature is 6.7 degrees Celsius, and the loop design temperature difference is 5 degrees Celsius. A flowchart for the Secondary Cooling loop sizing is provided in Figure~\ref{fig:flowchart-for-primary-cooling-loop-sizing}.
+
+\begin{figure}[htbp] % fig 60
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image060.png}
+\caption{Flowchart for primary cooling loop sizing \protect \label{fig:flowchart-for-primary-cooling-loop-sizing}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping.tex b/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping.tex
new file mode 100644
index 00000000000..17771b6502c
--- /dev/null
+++ b/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping.tex
@@ -0,0 +1,31 @@
+\chapter{Example System 3: Primary/Secondary Pumping}\label{example-system-3-primarysecondary-pumping}
+
+This example will discuss the basics of primary/secondary pumping systems and some of the controls that are used in managing such systems. The input file for this example can be found under the name: PlantApplicationsGuide\_Example3.idf.
+
+Although it is common for these systems to have a common pipe setup to allow for flow imbalance as shown in Figure~\ref{fig:example-of-a-common-pipe-setup} and even though there is a provision in EnergyPlus to model common pipes, this example will not discuss them. In the future, the common pipe is expected to be obsolesced, and therefore using a heat exchanger and two separate loops is recommended for future primary/secondary pumping arrangements.
+
+\begin{figure}[hbtp] % fig 87
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image087.png}
+\caption{Example of a common pipe setup \protect \label{fig:example-of-a-common-pipe-setup}}
+\end{figure}
+
+This system services a three zone building by using, two chillers and purchased cooling on the primary chilled water loop to satisfy the demand loads. The chilled water from the supply side of the primary chilled water loop is passes through a plate heat exchanger which serves as the supply side for the secondary chilled water loop. The cooling coil is placed on the demand side of the secondary loop. The primary loop uses a constant speed pump to circulate the working fluid (water). The secondary loop uses a variable speed pump to manipulate the flow of the fluid such that the cooling coil demand is satisfied. The above mentioned pumps are considered as a primary/secondary pumping pair.
+
+Therefore there are four different loops in the system. The cooling loops in the system will be modeled first. The primary cooling loop (`Primary Chilled Water Loop') which contains a small chiller, a big chiller and a purchased cooling object on the supply side half loop for supplying chilled water to a fluid to fluid plate heat exchanger on the demand side. The secondary cooling loop (`Secondary Chilled Water Loop') contains the fluid to fluid plate heat exchanger on the supply side half loop and a cooling coil on the demand side. The condenser loop (`Condenser Loop') which uses a cooling tower to supply cold water to the chillers on the demand side is modeled next. The heating loop (`Heating Loop') uses purchased heating to serve the demand loads of three reheat coils places in each of the zones of the buildings, this loop will not be discussed in this application guide because it does not relate to the primary/secondary pumping setup in any way.
+
+The plant equipment operation scheme for the primary chilled water loop and the primary/secondary pumping setup are the most important features of this system.
+
+The simple line diagram for the system is shown in Figure~\ref{fig:energyplus-line-diagram-for-the-cooling}. The EnergyPlus line diagram is shown in Figure~\ref{fig:energyplus-line-diagram-for-the-cooling}.
+
+\begin{figure}[hbtp] % fig 88
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image088.png}
+\caption{Simple line diagram for the cooling system \protect \label{fig:simple-line-diagram-for-the-cooling-system}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 89
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image089.png}
+\caption{EnergyPlus line diagram for the cooling system \protect \label{fig:energyplus-line-diagram-for-the-cooling}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/condenser-loop-cooling-tower.tex b/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/condenser-loop-cooling-tower.tex
new file mode 100644
index 00000000000..e15fd10b6e1
--- /dev/null
+++ b/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/condenser-loop-cooling-tower.tex
@@ -0,0 +1,103 @@
+\section{Condenser Loop - Cooling Tower}\label{condenser-loop---cooling-tower}
+
+The Condenser Loop is constructed by using a \emph{PlantLoop} object. It uses a cooling tower (modeled by using a \emph{CoolingTower:SingleSpeed} object class) and a variable speed pump (modeled by using a \emph{Pump:VariableSpeed)} to supply cooling water to the chillers in the primary cooling loop. Therefore, the supply side of the loop contains the Cooling Tower and the demand side contains the chillers. The loop is operated by using plant equipment operation schemes, and schedules. ~Refer to Figure~\ref{fig:simple-line-diagram-for-the-condenser-loop-001} for a simple diagram of the Condenser Loop.
+
+\begin{figure}[hbtp] % fig 116
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image116.png}
+\caption{Simple line diagram for the condenser loop \protect \label{fig:simple-line-diagram-for-the-condenser-loop-001}}
+\end{figure}
+
+\subsection{Flowcharts for the Condenser Loop Input Process}\label{flowcharts-for-the-condenser-loop-input-process-000}
+
+This series of flowcharts serve as a guide for identifying and inputting the Condenser Loop and its components into the input file. The EnergyPlus line diagram for this loop is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-condenser-001}. A simple flowchart for the separation of the half loops is provided in Figure~\ref{fig:simple-flow-chart-for-separation-on-half-001}.
+
+\begin{figure}[hbtp] % fig 117
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image117.png}
+\caption{EnergyPlus line diagram for the condenser loop \protect \label{fig:energyplus-line-diagram-for-the-condenser-001}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 118
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image118.png}
+\caption{Simple flow chart for separation on half loops in the condenser loop \protect \label{fig:simple-flow-chart-for-separation-on-half-001}}
+\end{figure}
+
+\subsubsection{Condenser Loop Supply Side Construction}\label{condenser-loop-supply-side-construction-000}
+
+The main components on the supply side half loop for the Condenser Loop are the Cooling Tower that supplies the cooling water and the variable speed pump that circulates the cooling water through the loop. This half loop supplies cooling water to the chillers on the demand side half loop. The supply side half loop contains four components, four branches, eight nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the Condenser loop supply side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-supply-side-002}. The flowchart for supply side branches and components is provided in Figure~\ref{fig:flowchart-for-condenser-loop-supply-side-002}. The flowchart for supply side connectors is provided in Figure~\ref{fig:flowchart-for-condenser-loop-supply-side-connectors-002}.
+
+\begin{figure}[hbtp] % fig 119
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image119.png}
+\caption{EnergyPlus line diagram for the supply side of the Condenser Loop \protect \label{fig:energyplus-line-diagram-for-the-supply-side-002}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 120
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image120.png}
+\caption{Flowchart for Condenser Loop supply side branches and components \protect \label{fig:flowchart-for-condenser-loop-supply-side-002}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 121
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image121.png}
+\caption{Flowchart for Condenser Loop supply side connectors \protect \label{fig:flowchart-for-condenser-loop-supply-side-connectors-002}}
+\end{figure}
+
+\subsubsection{Condenser Loop Demand Side Construction}\label{condenser-loop-demand-side-construction-000}
+
+The main components on the demand side half loop are the small constant COP chiller and the bigger electric chiller that use the cooling water supplied by the cooling tower. The chillers are in turn used to supply chilled water in the Primary Cooling loop. ~This side of the loop also has ten nodes, five components, five branches and one splitter-mixer pair. An EnergyPlus schematic for the demand side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-demand-side-002}. The flowchart for demand side branch definition is provided in Figure~\ref{fig:flowchart-for-condenser-loop-demand-side-002}. The flowchart for the demand side connectors is provided in Figure~\ref{fig:flowchart-for-condenser-loop-demand-side-connectors-002}.
+
+\begin{figure}[hbtp] % fig 122
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image122.png}
+\caption{EnergyPlus line diagram for the demand side of the Condenser Loop \protect \label{fig:energyplus-line-diagram-for-the-demand-side-002}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 123
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image123.png}
+\caption{Flowchart for Condenser Loop demand side branches and components \protect \label{fig:flowchart-for-condenser-loop-demand-side-002}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 124
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image124.png}
+\caption{Flowchart for Condenser Loop demand side connectors \protect \label{fig:flowchart-for-condenser-loop-demand-side-connectors-002}}
+\end{figure}
+
+\subsection{Flowcharts for Condenser Loop Controls}\label{flowcharts-for-condenser-loop-controls-000}
+
+The Condenser loop is operated by using set-points, plant equipment operation schemes and schedules.
+
+\subsubsection{Condenser Loop Schedules}\label{condenser-loop-schedules-000}
+
+The flowchart for condenser loop schedule definition is provided in Figure~\ref{fig:flowchart-for-condenser-loop-schedules-002}. The Condenser loop uses one schedule to operate properly. \emph{ON} is a compact schedule that keeps the Cooling Tower On at all times of the day, this compact schedule uses a continuous \emph{ScheduleTypeLimit} (\emph{Fraction)} which defines that the value of On is 1 and that of Off is 0.
+
+\begin{figure}[hbtp] % fig 125
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image125.png}
+\caption{Flowchart for condenser loop schedules \protect \label{fig:flowchart-for-condenser-loop-schedules-002}}
+\end{figure}
+
+\subsubsection{Condenser Loop Plant Equipment Operation Schemes}\label{condenser-loop-plant-equipment-operation-schemes-000}
+
+The \emph{PlantEquipmentOperationschemes} object uses the \emph{ON} schedule and the \emph{Tower Operation} objects to set the range of demand loads for which the cooling tower is operated during the simulation period. A flowchart detailing the Condenser Loop plant equipment operation schemes is provided in Figure~\ref{fig:flowchart-for-condenser-loop-plant-equipment-operation-002}.
+
+\begin{figure}[hbtp] % fig 126
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image126.png}
+\caption{Flowchart for Condenser Loop plant equipment operation schemes \protect \label{fig:flowchart-for-condenser-loop-plant-equipment-operation-002}}
+\end{figure}
+
+\subsubsection{Condenser Loop Setpoints}\label{condenser-loop-setpoints-000}
+
+The \emph{MyCondenserControl} setpoint manager places a temperature setpoint at the \emph{Condenser Supply Outlet Node.} The temperature at this point is controlled with respect to the outdoor air wet bulb temperature at that point in the simulation. The outdoor air wet bulb temperature is obtained from the weather data at the location of the simulation. A flowchart for Secondary Cooling loop setpoints is provided in Figure~\ref{fig:flowchart-for-condenser-loop-setpoints-002}.
+
+\begin{figure}[hbtp] % fig 127
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image127.png}
+\caption{Flowchart for Condenser Loop setpoints \protect \label{fig:flowchart-for-condenser-loop-setpoints-002}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/primary-chilled-water-loop-chiller-s.tex b/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/primary-chilled-water-loop-chiller-s.tex
new file mode 100644
index 00000000000..4b7702edb4b
--- /dev/null
+++ b/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/primary-chilled-water-loop-chiller-s.tex
@@ -0,0 +1,109 @@
+\section{Primary Chilled Water Loop -- Chiller(s) and purchased cooling}\label{primary-chilled-water-loop-chillers-and-purchased-cooling}
+
+The Secondary Cooling system is constructed by using a \emph{PlantLoop} object. It uses two chillers (a small constant COP chiller and a bigger electric chiller) and purchased district cooling. Therefore, the supply side of the loop contains the chillers and the purchased cooling, and the demand side contains one side of the plate heat exchanger. The loop is operated by using plant equipment operation schemes and schedules. Refer to Figure~\ref{fig:simple-line-diagram-for-the-primary-chilled} for a simple diagram of the Primary Cooling Loop.
+
+\begin{figure}[hbtp] % fig 90
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image090.png}
+\caption{Simple line diagram for the primary chilled water loop \protect \label{fig:simple-line-diagram-for-the-primary-chilled}}
+\end{figure}
+
+\subsection{Flowcharts for the Primary Chilled Water Loop Input Process}\label{flowcharts-for-the-primary-chilled-water-loop-input-process}
+
+This series of flowcharts serve as a guide for identifying and inputting the Primary Chilled Water loop and its components into the input file. The working fluid in this loop is water. The EnergyPlus line diagram for this loop is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-primary}. A simple flowchart for the separation of the half loops is provided in Figure~\ref{fig:simple-flowchart-for-the-separation-of-half}.
+
+\begin{figure}[hbtp] % fig 91
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image091.png}
+\caption{EnergyPlus line diagram for the primary chilled water loop \protect \label{fig:energyplus-line-diagram-for-the-primary}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 92
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image092.png}
+\caption{Simple flowchart for the separation of half-loops in the primary chilled water loop \protect \label{fig:simple-flowchart-for-the-separation-of-half}}
+\end{figure}
+
+\subsubsection{Primary Cooling System Supply Side Loop Construction}\label{primary-cooling-system-supply-side-loop-construction}
+
+The main components on the supply side half loop for the primary chilled water loop are two chillers and district cooling object that supply chilled water and the constant speed pump that circulates the chilled water through the loop. This pump (`CW Primary Circ Pump') is the primary pump in the primary/secondary pumping setup. This half loop supplies chilled water to the plate heat exchanger which is placed on the demand side half loop. The supply side half loop contains six components, six branches, twelve nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the Primary Cooling loop supply side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-supply-side-005}. The flowchart for supply side branches and components is provided in Figure~\ref{fig:flowchart-for-primary-cooling-loop-supply-side-branches-and-components}. The flowchart for supply side connectors is provided in Figure~\ref{fig:flowchart-for-primary-cooling-loop-supply-side-connectors}.
+
+\begin{figure}[hbtp] % fig 93
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image093.png}
+\caption{EnergyPlus line diagram for the supply side of the primary chilled water loop \protect \label{fig:energyplus-line-diagram-for-the-supply-side-005}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 94
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image094.png}
+\caption{Flowchart for Primary Cooling Loop supply side branches and components \protect \label{fig:flowchart-for-primary-cooling-loop-supply-side-branches-and-components}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 95
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image095.png}
+\caption{Flowchart for Primary Cooling Loop supply side branches and components \protect \label{fig:flowchart-for-primary-cooling-loop-supply-side-connectors}}
+\end{figure}
+
+\subsubsection{Primary Cooling Loop Demand Side Loop Construction}\label{primary-cooling-loop-demand-side-loop-construction}
+
+The main component on the demand side half loop is the plate heat exchanger that facilitates the exchange of heat between the fluids of the primary and secondary chilled water loop. The plate heat exchanger will not be discussed in this loop. Instead the object will be discussed in the supply side half loop of the secondary chilled water loop. This side of the loop also has eight nodes, four components, four branches, and one splitter mixer pair. An EnergyPlus schematic for the demand side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-demand-side-005}. The flowchart for demand side branch definition is provided in Figure~\ref{fig:flowchart-for-primary-chilled-water-loop-demand-side-branches-and-components}. The flowchart for the demand side connectors is provided in Figure~\ref{fig:flowchart-for-primary-chilled-water-loop-demand-side-connectors}.
+
+\begin{figure}[hbtp] % fig 96
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image096.png}
+\caption{EnergyPlus line diagram for the demand side of the primary chilled water loop \protect \label{fig:energyplus-line-diagram-for-the-demand-side-005}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 97
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image097.png}
+\caption{Flowchart for primary chilled water loop demand side branches and components \protect \label{fig:flowchart-for-primary-chilled-water-loop-demand-side-branches-and-components}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 98
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image098.png}
+\caption{Flowchart for primary chilled water loop demand side connectors \protect \label{fig:flowchart-for-primary-chilled-water-loop-demand-side-connectors}}
+\end{figure}
+
+\subsection{Flowcharts for Primary Chilled Water Loop Controls}\label{flowcharts-for-primary-chilled-water-loop-controls}
+
+The Primary Cooling loop is operated by using set-points, plant equipment operation schemes and schedules. The plant equipment scheme for the on peak and off peak operation of the chillers is very important
+
+\subsubsection{Primary Chilled Water Loop Schedules}\label{primary-chilled-water-loop-schedules}
+
+The Primary Cooling loop uses three different schedules to operate properly. \emph{On Peak} is a compact schedule that defines the on peak hours (9 AM to 6 PM). The \emph{Off Peak} is a compact schedule that defines the off peak hours (6 PM to 9 AM). This plant loop also uses another compact schedule named \emph{CW Loop Temp Schedule} declare that the temperature of the chilled water loop outlet flow is 6.7 degrees Celsius at all times. This schedule is used by the setpoint manager (\emph{Primary CW Loop Setpoint Manager)}. This schedule uses a schedule type limit named \emph{Temperature,} which defines the loop upper and lower temperature limits. The flowchart for Primary Cooling loop schedule definition is provided in Figure~\ref{fig:flowchart-for-primary-chilled-water-loop-schedules}.
+
+\begin{figure}[hbtp] % fig 99
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image099.png}
+\caption{Flowchart for primary chilled water loop schedules \protect \label{fig:flowchart-for-primary-chilled-water-loop-schedules}}
+\end{figure}
+
+\subsubsection{Primary Chilled Water Loop Plant Equipment Operation Schemes}\label{primary-chilled-water-loop-plant-equipment-operation-schemes}
+
+There are two important operation schemes in the primary chilled water loop. The \emph{CW Loop Operation} plant equipment operation scheme used two schedules (\emph{On Peak} and \emph{off Peak}) to control the supply components in the primary cooling loop. \emph{Peak Operation} is set up such that different components or combinations of components are operated for different values of cooling load during the peak hours (9AM to 6PM everyday) of the simulation period. Up to 25,000 W of cooling load, the small constant COP chiller is operated, for 25,000-245,000 W the big electric chiller and purchased cooling are used and for 245,000-500,000 W purchased cooling is used. This setup serves to increase the efficiency of the system. \emph{Off Peak Operation} is set up such that both the chillers are operated during the off peak hours (6 PM to 9 AM). Flowcharts detailing the chilled water loop plant equipment operation schemes are provided in Figure~\ref{fig:flowchart-for-on-peak-operation-of} and Figure~\ref{fig:flowchart-for-off-peak-plant-operation-of}.
+
+\begin{figure}[hbtp] % fig 100
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image100.png}
+\caption{Flowchart for on peak operation of the primary chilled water loop \protect \label{fig:flowchart-for-on-peak-operation-of}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 101
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image101.png}
+\caption{Flowchart for off peak plant operation of the primary chilled water loop \protect \label{fig:flowchart-for-off-peak-plant-operation-of}}
+\end{figure}
+
+\subsubsection{Primary Chilled Water Loop Setpoints}\label{primary-chilled-water-loop-setpoints}
+
+The \emph{Primary CW Loop Setpoint Manager} uses the \emph{CW Loop Temp Schedule} to set a temperature control point at the \emph{CW Primary Supply Outlet Node}. This setpoint allows the program to control the temperature at the node by operating the components in the Primary Cooling loop. ~Since, setpoint managers are high-level control objects, their usefulness is realized in much more complex systems, where multiple nodes have to be monitored in order to operate the system properly. A flowchart for Secondary Cooling loop setpoints is provided in Figure~\ref{fig:flowchart-for-primary-cooling-loop-setpoints}.
+
+\begin{figure}[hbtp] % fig 102
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image102.png}
+\caption{Flowchart for Primary Cooling Loop setpoints \protect \label{fig:flowchart-for-primary-cooling-loop-setpoints}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/primary-secondary-pumping.tex b/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/primary-secondary-pumping.tex
new file mode 100644
index 00000000000..c9715c11689
--- /dev/null
+++ b/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/primary-secondary-pumping.tex
@@ -0,0 +1,3 @@
+\section{Primary/Secondary Pumping}\label{primarysecondary-pumping}
+
+As mentioned in sections \emph{Primary Cooling System Supply Side Loop Construction} and \emph{Secondary Chilled Water Loop Supply Side Loop Construction}, the CW primary Circ Pump and the CW Sec Circ Pump function as the primary/secondary (respectively) pumping system. The primary pump is a constant speed pump that circulates chilled water at a constant flow rate through one side the plate heat exchanger in the primary chilled water loop. The secondary pump is a variable speed pump that circulates chilled water at a variable flow rate through the other side of the plate heat exchanger depending on the demand load.
diff --git a/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/secondary-chilled-water-loop-plate-heat.tex b/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/secondary-chilled-water-loop-plate-heat.tex
new file mode 100644
index 00000000000..9146a160340
--- /dev/null
+++ b/doc/plant-application-guide/src/example-system-3-primary-secondary-pumping/secondary-chilled-water-loop-plate-heat.tex
@@ -0,0 +1,113 @@
+\section{Secondary Chilled Water Loop -- Plate Heat Exchanger}\label{secondary-chilled-water-loop-plate-heat-exchanger}
+
+The Secondary Cooling system is constructed by using a \emph{PlantLoop} object, the working fluid in this loop is water. It uses one side of a plate heat exchanger (modeled using a \emph{HeatExchanger:FluidToFluid} object) to supply chilled water to a cooling coil (modeled by using a \emph{Coil:Cooling:DetailedGeometry} object). Therefore, the supply side of the loop contains the heat exchanger and the demand side contains the cooling coil. The loop is operated by using plant equipment operation schemes, and schedules. ~Refer to Figure~\ref{fig:simple-line-diagram-for-the-secondary-chilled} for a simple diagram of the secondary chilled water loop.
+
+\begin{figure}[hbtp] % fig 103
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image103.png}
+\caption{Simple line diagram for the secondary chilled water loop \protect \label{fig:simple-line-diagram-for-the-secondary-chilled}}
+\end{figure}
+
+\subsection{Flowcharts for the Secondary Chilled Water Loop Input Process}\label{flowcharts-for-the-secondary-chilled-water-loop-input-process}
+
+This series of flowcharts serve as a guide for identifying and inputting the secondary chilled water loop and its components into the input file. The EnergyPlus line diagram for this loop is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-secondary}. A simple flowchart for the separation of the half loops is provided in Figure~\ref{fig:simple-flow-chart-for-separation-on-half-003}.
+
+\begin{figure}[hbtp] % fig 104
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image104.png}
+\caption{EnergyPlus line diagram for the secondary chilled water loop \protect \label{fig:energyplus-line-diagram-for-the-secondary}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 105
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image105.png}
+\caption{Simple flow chart for separation on half loops in the secondary chilled water loop \protect \label{fig:simple-flow-chart-for-separation-on-half-003}}
+\end{figure}
+
+\subsubsection{Secondary Chilled Water Loop Supply Side Loop Construction}\label{secondary-chilled-water-loop-supply-side-loop-construction}
+
+The main components on the supply side half loop for the Secondary Cooling System are the plate heat exchanger that supplies the chilled water and the variable speed pump that circulates the chilled water through the loop. The variable speed pump (named `CW Sec Circ Pump') is the secondary pump in the primary/secondary pumping setup. This half loop supplies chilled water to a cooling coil on the demand side half loop. The supply side half loop contains four components, four branches, eight nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the secondary chilled water loop supply side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-supply-side-007}. The flowchart for supply side branches and components is provided in Figure~\ref{fig:flowchart-for-secondary-chilled-water-loop-supply-side-007}. The flowchart for supply side connectors is provided in Figure~\ref{fig:flowchart-for-secondary-chilled-water-loop-supply-side-connectors}.
+
+\begin{figure}[hbtp] % fig 106
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image106.png}
+\caption{EnergyPlus line diagram for the supply side of the secondary chilled water loop \protect \label{fig:energyplus-line-diagram-for-the-supply-side-007}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 107
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image107.png}
+\caption{Flowchart for secondary chilled water loop supply side branches and components \protect \label{fig:flowchart-for-secondary-chilled-water-loop-supply-side-007}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 108
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image108.png}
+\caption{Flowchart for secondary chilled water loop supply side connectors \protect \label{fig:flowchart-for-secondary-chilled-water-loop-supply-side-connectors}}
+\end{figure}
+
+\subsubsection{Secondary Chilled Water Loop Demand Side Loop Construction}\label{secondary-chilled-water-loop-demand-side-loop-construction}
+
+The main component on the demand side half loop is the Cooling Coil that cools the air in the building by using the chilled water that is supplied by the plate heat exchanger. This side of the loop also has eight nodes, four components, four branches, and one splitter-mixer pair. An EnergyPlus schematic for the demand side is provided in Figure~\ref{fig:energyplus-line-diagram-for-the-demand-side-007}. The flowchart for demand side branch definition is provided in Figure~\ref{fig:flowchart-for-secondary-chilled-water-loop-demand-side-007}. The flowchart for the demand side connectors is provided in Figure~\ref{fig:flowchart-for-secondary-chilled-water-loop-demand-side-connectors}.
+
+\begin{figure}[hbtp] % fig 109
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image109.png}
+\caption{EnergyPlus line diagram for the demand side of the secondary chilled water loop \protect \label{fig:energyplus-line-diagram-for-the-demand-side-007}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 110
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image110.png}
+\caption{Flowchart for secondary chilled water loop demand side branches and components \protect \label{fig:flowchart-for-secondary-chilled-water-loop-demand-side-007}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 111
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image111.png}
+\caption{Flowchart for secondary chilled water loop demand side connectors \protect \label{fig:flowchart-for-secondary-chilled-water-loop-demand-side-connectors}}
+\end{figure}
+
+\subsection{Flowcharts for secondary chilled water loop Controls}\label{flowcharts-for-secondary-chilled-water-loop-controls}
+
+The secondary chilled water loop is operated by using set-points, plant equipment operation schemes and schedules.
+
+\subsubsection{Secondary Chilled Water Loop Schedules}\label{secondary-chilled-water-loop-schedules}
+
+The flowchart for Primary Cooling loop schedule definition is provided in Figure~\ref{fig:flowchart-for-secondary-chilled-water-loop-schedules}. The Secondary Cooling loop uses two different schedules to operate properly. \emph{ON} is a compact schedule that keeps the plate heat exchanger running at all times of the day, this compact schedule uses a continuous \emph{ScheduleTypeLimit} (\emph{Fraction)} which defines that the value of On is 1 and that of Off is 0. This plant loop also uses another compact schedule named \emph{CW Sec Loop Temp Schedule} declares that the outlet temperature of the Secondary Cooling loop should be 6.67 degrees Celsius at any time; this schedule is used by the setpoint manager (\emph{CW Sec Loop Setpoint Manager)}. This schedule uses a schedule type limit named \emph{Temperature,} which defines the loop upper and lower temperature limits.
+
+\begin{figure}[hbtp] % fig 112
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image112.png}
+\caption{Flowchart for secondary chilled water loop schedules \protect \label{fig:flowchart-for-secondary-chilled-water-loop-schedules}}
+\end{figure}
+
+\subsubsection{Secondary Chilled Water Loop Plant Equipment Operation Schemes}\label{secondary-chilled-water-loop-plant-equipment-operation-schemes}
+
+The \emph{PlantEquipmentOperationschemes} object uses the \emph{ON} schedule and the \emph{CW Sec Operation Scheme} objects to set the range of the demand loads for which the heat exchanger is operated during the simulation period. A flowchart detailing the secondary chilled water loop plant equipment operation schemes is provided in Figure~\ref{fig:flowchart-for-secondary-chilled-water-loop-plant-equipment-operation}.
+
+\begin{figure}[hbtp] % fig 113
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image113.png}
+\caption{Flowchart for secondary chilled water loop plant equipment operation schemes \protect \label{fig:flowchart-for-secondary-chilled-water-loop-plant-equipment-operation}}
+\end{figure}
+
+\subsubsection{Secondary Chilled Water Loop Setpoints}\label{secondary-chilled-water-loop-setpoints}
+
+The \emph{CW Sec Loop Setpoint Manager} uses the \emph{CW Sec Loop Temp Schedule} to set a temperature control point at the \emph{CW Sec Supply Outlet Node}. This setpoint allows the program to control the temperature at the node by operating the components in the Secondary Cooling loop. A flowchart for Secondary Cooling loop setpoints is provided in Figure~\ref{fig:flowchart-for-secondary-chilled-water-loop-setpoints}.
+
+\begin{figure}[hbtp] % fig 114
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image114.png}
+\caption{Flowchart for secondary chilled water loop setpoints \protect \label{fig:flowchart-for-secondary-chilled-water-loop-setpoints}}
+\end{figure}
+
+\subsubsection{Secondary Chilled Water Loop Sizing}\label{secondary-chilled-water-loop-sizing}
+
+The secondary chilled water loop is sized such a way that the design loop exit temperature is 6.67 degrees Celsius, and the loop design temperature difference is 5 degrees Celsius. A flowchart for the chilled water loop sizing is provided in Figure~\ref{fig:flowchart-for-secondary-chilled-water-loop-sizing}.
+
+\begin{figure}[hbtp] % fig 115
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image115.png}
+\caption{Flowchart for secondary chilled water loop sizing \protect \label{fig:flowchart-for-secondary-chilled-water-loop-sizing}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/generating-an-energyplus-line-diagram.tex b/doc/plant-application-guide/src/generating-an-energyplus-line-diagram.tex
new file mode 100644
index 00000000000..12e271f5a90
--- /dev/null
+++ b/doc/plant-application-guide/src/generating-an-energyplus-line-diagram.tex
@@ -0,0 +1,27 @@
+\chapter{Generating an EnergyPlus Line Diagram}\label{generating-an-energyplus-line-diagram}
+
+The following list of steps will outline the process for converting an engineering line diagram into an EnergyPlus line diagram. Throughout the process, the components in the systems should be identified and named properly. It is easier to input the system if a list of components and their names is available.
+
+1.~~~~\textbf{Obtain an engineering line diagram for the system.}
+
+2.~~~~\textbf{Identify all the loops in the system.} Some systems may be very complex, but an effort should be made to separate the system into its constituent plant loops. A system may have multiple plant loops. Therefore, proper documentation of the loops and their components should be a priority.
+
+3.~~~~\textbf{Identify the demand side and supply side of the individual loops.} EnergyPlus expects the demand side loop and supply side loop to be entered separately. Some examples of simple plant loops are: a hot water heater (supply component) connected to a heating coil (demand component), a chiller (supply component) connected to a cooling coil (demand component) or a cooling tower (supply component) connected to a water cooled chiller (demand component). These loops may have multiple supply components and multiple demand components. A chiller may also be a supply or demand component depending on the loop.
+
+4.~~~~\textbf{Identify the components in the system.} All the operating/active components, such as chillers, pumps, cooling towers, thermal energy storage tanks, heating and cooling coils, and other components should be identified and named properly. It should be noted that even though EnergyPlus has objects for modeling valves, they are not often used. Instead the flow through a component is regulated by using schedules, plant equipment operation schemes and set points. Passive components such as inlet and outlet pipes for each side of the loop should also be identified, as they will help in modeling the loop connectors.
+
+5.~~~~\textbf{Identify all the nodes in the system.} Nodes are necessary to connect the different components in the system. Nodes define the starting and ending points of branches as well as intermediate nodes on multi-component branches. A good method to pin-point nodes on the line diagram would be to put a node on either side of an active or passive component. Note: If the outlet of one component does not feed into a splitter or a mixer, then the outlet node will be the same as the inlet node of the downstream component.
+
+6.~~~~\textbf{Identify all the branches in the loops.} A good way to define a branch would be to include at least one of the components in the branch. Branches can accommodate multiple components in series, but parallel components should be modeled on separate branches. Operating/active components (except pumps) should be bypassed by adding a bypass branch parallel to the branch containing the active component. Multiple bypass branches in parallel can be replaced by a single bypass branch.
+
+7.~~~~\textbf{Identify the position of the connectors in the system.} Connectors are an integral part of the system and are important in constructing the loop. There are two types of connectors, splitters and mixers. Splitters can distribute the flow from a single branch into multiple parallel branches. Mixers can combine the flow from multiple branches into a single branch. As mentioned above, most systems have multiple supply and demand side components, so splitters and mixers play a crucial role in distributing and recombining the flow of the working fluid through all the components.
+
+8.~~~~\textbf{Generate an EnergyPlus diagram} of the whole system as well as the individual loops by using the information gathered from the preceding steps.
+
+A flowchart for this process is provided in Figure~\ref{fig:flowchart-for-energyplus-line-diagram} .
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image002.png}
+\caption{Flowchart for EnergyPlus line diagram generation \protect \label{fig:flowchart-for-energyplus-line-diagram}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/generating-an-energyplus-line-diagram/example-for-energyplus-line-diagram.tex b/doc/plant-application-guide/src/generating-an-energyplus-line-diagram/example-for-energyplus-line-diagram.tex
new file mode 100644
index 00000000000..78d8da62141
--- /dev/null
+++ b/doc/plant-application-guide/src/generating-an-energyplus-line-diagram/example-for-energyplus-line-diagram.tex
@@ -0,0 +1,69 @@
+\section{Example for EnergyPlus Line Diagram Generation}\label{example-for-energyplus-line-diagram-generation}
+
+A series of figures are provided below to detail the process for generating an EnergyPlus line diagram.
+
+1.~~~~\textbf{Obtain a simple engineering line diagram for the system.} This system is a simple cooling system that employs a primary/secondary pumping setup with a one-way common pipe to circulate chilled water through a building. Figure~\ref{fig:simple-line-diagram-for-the-example-system} shows the simple line diagram for the system.
+
+\begin{figure}[hbtp] % fig 3
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image003.png}
+\caption{Simple line diagram for the example system, (recreated from Reed and Davis 2007) \protect \label{fig:simple-line-diagram-for-the-example-system}}
+\end{figure}
+
+2.~~~~\textbf{Identify all the loops in the system.} This system contains only one plant loop. Loop name: Cooling Loop.
+
+\textbf{3.~~~~Identify the demand side and supply side of the loop.} ~The half loops are depicted in Figure~\ref{fig:breakdown-of-a-loop-into-its-constituent-half}.
+
+\begin{figure}[hbtp] % fig 4
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image004.png}
+\caption{Breakdown of a loop into its constituent half-loops \protect \label{fig:breakdown-of-a-loop-into-its-constituent-half}}
+\end{figure}
+
+4.~~~~\textbf{Identify the components in the system.} While identifying the main components in the loop, it should be noted that this loop has a primary/secondary pumping setup, and that there is a common pipe that allows for flow imbalance. (Note: The \emph{PlantLoop} object in EnergyPlus has a provision for the input of a common pipe. The user only has to specify the existence of a common pipe in the loop, and the program calculates its position in the loop). The primary pump is shown below is shown in Figure~\ref{fig:a-component-in-the-loop}.
+
+\begin{figure}[hbtp] % fig 5
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image005.png}
+\caption{A component in the loop \protect \label{fig:a-component-in-the-loop}}
+\end{figure}
+
+5.~~~~\textbf{Identify all the nodes in the system.} As mentioned above, placing a node on each side of a component is a good way to pinpoint all the nodes in the system. This process should be repeated for every component in the loop. Figure~\ref{fig:node-placement-on-components} shows the placement of all the nodes on Individual components, while Figure~\ref{fig:nodes-in-the-system} shows all the nodes in the system.
+
+\begin{figure}[hbtp] % fig 6
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image006.png}
+\caption{Node placement on components \protect \label{fig:node-placement-on-components}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 7
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image007.png}
+\caption{Nodes in the system \protect \label{fig:nodes-in-the-system}}
+\end{figure}
+
+Note: No nodes were placed on the common pipe, but its existence should be specified in the \emph{PlantLoop} object.
+
+6.~~~~\textbf{Identify all the branches in the system.} Remember to add the bypass branches to the operating components (except the pumps). Branches have to start and end with nodes, and should contain at least one component. The branches are denoted by the blue lines in Figure~\ref{fig:branch-definition}.
+
+\begin{figure}[hbtp] % fig 8
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image008.png}
+\caption{Branch definition \protect \label{fig:branch-definition}}
+\end{figure}
+
+7.~~~~\textbf{Identify the position of the connectors in the system.} The \emph{PlantLoop} accepts only one splitter-mixer pair per half loop. The connectors are defined by using branches; a splitter can have one inlet branch and any number of outlet branches whereas a mixer can have any number of inlet branches and one outlet branch. All the connectors in the loop are denoted by the green lines in Figure~\ref{fig:splitters-and-mixers-in-the-loop}.
+
+\begin{figure}[hbtp] % fig 9
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image009.png}
+\caption{Splitters and mixers in the loop \protect \label{fig:splitters-and-mixers-in-the-loop}}
+\end{figure}
+
+8.~~~~An EnergyPlus diagram can be generated by using all the identified components. The complete schematic is shown in Figure~\ref{fig:complete-energyplus-line-diagram}.
+
+\begin{figure}[hbtp] % fig 10
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image010.png}
+\caption{Complete EnergyPlus line diagram \protect \label{fig:complete-energyplus-line-diagram}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/inputting-the-system-into-the-idf-file.tex b/doc/plant-application-guide/src/inputting-the-system-into-the-idf-file.tex
new file mode 100644
index 00000000000..7c6b350c6ee
--- /dev/null
+++ b/doc/plant-application-guide/src/inputting-the-system-into-the-idf-file.tex
@@ -0,0 +1,9 @@
+\chapter{Inputting the system into the IDF file}\label{inputting-the-system-into-the-idf-file}
+
+Since, it is not possible to input schematics into the input file, it is important to add descriptive comments to all of the entries to ensure that all the components in the system have been accounted for. Such documentation will also make debugging easier. It should be noted that all of the syntax for the inputs is documented in the Input-Output reference guide. A flowchart for the basic input process is provided in Figure~\ref{fig:flowchart-for-input-process}.
+
+\begin{figure}[hbtp] % fig 11
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image011.png}
+\caption{Flowchart for input process \protect \label{fig:flowchart-for-input-process}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/introduction.tex b/doc/plant-application-guide/src/introduction.tex
new file mode 100644
index 00000000000..62fee9042e3
--- /dev/null
+++ b/doc/plant-application-guide/src/introduction.tex
@@ -0,0 +1,5 @@
+\chapter{Introduction}\label{introduction}
+
+This document provides an in-depth look at plant modeling in EnergyPlus. Plant refers to the subset of HVAC that involves hydronic equipment for heating, cooling, and service water heating (or domestic hot water).
+
+This guide serves as an aid to help model plant systems in EnergyPlus simulations. It is intended to augment the Input Output Reference, which describes the syntax and the details of individual input objects. This guide will discuss how the different objects can be used to construct a plant loop that can service a building load.
diff --git a/doc/plant-application-guide/src/introduction/organization.tex b/doc/plant-application-guide/src/introduction/organization.tex
new file mode 100644
index 00000000000..cfe0e9db1cb
--- /dev/null
+++ b/doc/plant-application-guide/src/introduction/organization.tex
@@ -0,0 +1,7 @@
+\section{Organization}\label{organization}
+
+This document begins with some general information to introduce users to the syntax used in EnergyPlus as well as this guide. Then some basic conversion methods needed to take a real system and format it to simplify the input process are provided. The bulk of this Application Guide is devoted to modeling example systems. The example systems are intended to demonstrate the input process for various types of plant systems, such as systems that use thermal energy storage tanks and those that have a primary/secondary pumping configurations.
+
+The example systems are defined by breaking the system into its constituent loops. The loops are then separated into supply and demand sides. These half-loops are then defined by branches, connectors, and components. The controls for each loop are set after the loop has been completed. Figures and flowcharts are used to display the definition process. The flow charts should be read from top to bottom and each branched level should be read from left to right.
+
+The Object Class Names and Object Names used in the flow charts match those used in the input file provided for the example. One thing that is not specified in the flow charts or figures is the node names used. The various object class names and object names used in the examples refer to the entries in the example input files.
diff --git a/doc/plant-application-guide/src/references.tex b/doc/plant-application-guide/src/references.tex
new file mode 100644
index 00000000000..9517389f05a
--- /dev/null
+++ b/doc/plant-application-guide/src/references.tex
@@ -0,0 +1,5 @@
+\chapter{References}\label{references}
+
+Reed, M. A., Davis, C. 2007, ``Chilled Water Plant Savings at No Cost.'' \emph{ASHRAE Journal} 49(7), 38-44.
+
+Hyman, L. B., Little, D. 2004, ``Overcoming Low Delta T, Negative Delta P At Large University Campus.'' \emph{ASHRAE Journal} 46(2), 28-34.
diff --git a/doc/plant-application-guide/src/scope.tex b/doc/plant-application-guide/src/scope.tex
new file mode 100644
index 00000000000..2b7b9ecb365
--- /dev/null
+++ b/doc/plant-application-guide/src/scope.tex
@@ -0,0 +1,9 @@
+\chapter{Scope}\label{scope}
+
+The scope of modeling plant loops in EnergyPlus is limited depending on the application. For example, there is no provision to model nested loops, and multiple splitter-mixer pairs in a single loop which are often used in large scale systems. Thus, it has to be realized that modeling large scale district loops may be challenging in EnergyPlus. One way to model such systems is to make some assumptions to condense some arrangements of components that cannot be modeled in EnergyPlus. This approach may not work because the arrangements could be very important to the system. Figure~\ref{fig:central-plant-chilled-water-schematic-for} shows a central plant chilled water system for the University of California, Riverside (Hyman and Little, 2004). This system contains a total of eight splitter-mixer pairs, four on the supply side, and four on the demand side. We could make some assumptions to simplify the system. For example we can use a single chiller instead of the array of five chillers, this could work if we size and control the chiller properly, but the concept of scheduling the different chillers to operate at different times of the day to improve efficiency will be lost. Hence, it should be noted that while simplifications can provide a general overview of how the system will operate, they may defeat the original purpose of the complex design. Therefore, this guide will only discuss building plant systems which are less complicated.
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image001.png}
+\caption{Central plant chilled water schematic for the University of California, Riverside (recreated from Hyman and Little, 2004) \protect \label{fig:central-plant-chilled-water-schematic-for}}
+\end{figure}
diff --git a/doc/plant-application-guide/src/title.tex b/doc/plant-application-guide/src/title.tex
new file mode 100644
index 00000000000..63f37402bb8
--- /dev/null
+++ b/doc/plant-application-guide/src/title.tex
@@ -0,0 +1 @@
+\input{../title}
diff --git a/doc/src/CMakeLists.txt b/doc/src/CMakeLists.txt
deleted file mode 100644
index 559195962c0..00000000000
--- a/doc/src/CMakeLists.txt
+++ /dev/null
@@ -1,202 +0,0 @@
-
-if(MSVC)
-  find_program(WKHTMLTOPDF_EXECUTABLE 
-    wkhtmltopdf
-    PATHS "C:/Program Files/wkhtmltopdf/bin" "C:/Program Files (x86)/wkhtmltopdf/bin")
-else()
-  find_program(WKHTMLTOPDF_EXECUTABLE 
-    wkhtmltopdf
-    )
-endif()
-
-# wkhtmltopdf
-execute_process(COMMAND ${WKHTMLTOPDF_EXECUTABLE} -V 
-  OUTPUT_VARIABLE wkhtmltopdfversionout)
-
-string(REGEX MATCH "([0-9]+\\.?)+" WKHTMLTOPDF_VER "${wkhtmltopdfversionout}")
-string(FIND "${wkhtmltopdfversionout}" "with patched qt" WKHTMLTOPDF_PATCHEDQT )
-
-
-if (WKHTMLTOPDF_VER VERSION_LESS "0.12.2.1")
-  message(FATAL_ERROR "wkhtmltopdf version 0.12.2.1 or greater required")
-endif()
-
-if (WKHTMLTOPDF_PATCHEDQT LESS "0")
-  message(FATAL_ERROR "wkhtmltopdf with special patchedqt build required")
-endif()
-
-# pandoc
-
-find_program(PANDOC_EXECUTABLE pandoc)
-
-file(MAKE_DIRECTORY ${CMAKE_CURRENT_BINARY_DIR}/Products)
-
-execute_process(COMMAND ${PANDOC_EXECUTABLE} -v 
-  OUTPUT_VARIABLE pandocversionout)
-
-string(REGEX MATCH "([0-9]+\\.?)+" PANDOC_VER "${pandocversionout}")
-
-if (PANDOC_VER VERSION_LESS "1.13.2")
-  message(FATAL_ERROR "pandoc version 1.13.2 or greater required")
-endif()
-
-
-
-Function(AddSplitMarkdownInput docName fileName offset)
-  set(input_name ${CMAKE_CURRENT_SOURCE_DIR}/docs/${docName}/${fileName})
-  set(output_name ${CMAKE_BINARY_DIR}/docs/${docName}/${fileName}.html)
-  set(${docName}_Inputs ${${docName}_Inputs} ${output_name} PARENT_SCOPE)
-
-  file(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/docs/${docName})
-
-  add_custom_command(OUTPUT ${output_name}
-    COMMAND ${PANDOC_EXECUTABLE} ${input_name} -o ${output_name} -f markdown_github -s -t html -N -H ${CMAKE_CURRENT_SOURCE_DIR}/docs/header.html --number-offset=${offset} --email-obfuscation=none
-    DEPENDS ${input_name} ${CMAKE_CURRENT_SOURCE_DIR}/docs/header.html
-    )
-EndFunction()
-
-Function(AddSplitPDF docName zoom )
-  set(output_name ${CMAKE_BINARY_DIR}/built_pdfs/${docName}.pdf)
-  file(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/built_pdfs)
-
-  set(shrinking_options --disable-smart-shrinking --zoom ${zoom})
-
-  add_custom_command(OUTPUT ${output_name}
-    COMMAND ${CMAKE_COMMAND} -E copy_directory ${CMAKE_CURRENT_SOURCE_DIR}/docs/${docName}/media ${CMAKE_BINARY_DIR}/docs/${docName}/media
-    COMMAND ${WKHTMLTOPDF_EXECUTABLE}  --window-status "MATHJAXDONE" --outline --outline-depth 3  ${shrinking_options} --page-size Letter --load-error-handling abort --load-media-error-handling abort --minimum-font-size 3 --footer-center [page] --no-stop-slow-scripts   toc --xsl-style-sheet ${CMAKE_CURRENT_SOURCE_DIR}/docs/toc.xsl  ${${docName}_Inputs} ${output_name} 
-    DEPENDS ${${docName}_Inputs} ${CMAKE_CURRENT_SOURCE_DIR}/docs/toc.xsl
-    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/docs/${docName}
-    )
-
-  add_custom_target(${docName}_pdf ALL
-    DEPENDS ${output_name}
-    )
-
-  INSTALL(FILES "${output_name}" DESTINATION "./Documentation")
-EndFunction()
-
-
-
-Function(AddMarkdownInput docName tag offset)
-  set(output_name ${CMAKE_BINARY_DIR}/docs/${docName}/${docName}${tag}.html)
-
-  set(input_names "")
-
-  foreach(input_name ${ARGN})
-    list(APPEND input_names ${CMAKE_CURRENT_SOURCE_DIR}/docs/${docName}/${input_name})
-  endforeach()
-
-  file(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/docs/${docName})
-
-  add_custom_command(OUTPUT ${output_name}
-    COMMAND ${PANDOC_EXECUTABLE} ${input_names} --number-offset ${offset}  -o ${output_name} -f markdown_github -s -t html -N -H ${CMAKE_CURRENT_SOURCE_DIR}/docs/header.html  --email-obfuscation=none
-    DEPENDS ${input_names} ${CMAKE_CURRENT_SOURCE_DIR}/docs/header.html
-    )
-EndFunction()
-
-
-Function(AddPDF docName tag)
-
-  set(output_name ${CMAKE_BINARY_DIR}/built_pdfs/${docName}${tag}.pdf)
-  file(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/built_pdfs)
-
-  add_custom_command(OUTPUT ${output_name}
-    COMMAND ${CMAKE_COMMAND} -E copy_directory ${CMAKE_CURRENT_SOURCE_DIR}/docs/${docName}/media ${CMAKE_BINARY_DIR}/docs/${docName}/media
-    COMMAND ${WKHTMLTOPDF_EXECUTABLE} -q --window-status "MATHJAXDONE" --outline --outline-depth 3  --enable-smart-shrinking --page-size Letter --load-error-handling abort --load-media-error-handling abort --minimum-font-size 3 --footer-center [page] --no-stop-slow-scripts  toc --xsl-style-sheet ${CMAKE_CURRENT_SOURCE_DIR}/docs/toc.xsl  ${CMAKE_BINARY_DIR}/docs/${docName}/${docName}${tag}.html ${output_name} 
-    DEPENDS ${CMAKE_BINARY_DIR}/docs/${docName}/${docName}${tag}.html ${CMAKE_CURRENT_SOURCE_DIR}/docs/toc.xsl
-    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/docs/${docName}
-    )
-
-  add_custom_target(${docName}${tag}_pdf ALL
-    DEPENDS ${output_name}
-    )
-
-  if (PACKAGE_BUILT_DOCS)
-    INSTALL(FILES "${output_name}" DESTINATION "./Documentation")
-  endif()
-
-EndFunction()
-
-AddMarkdownInput(Acknowledgements "" 0 Acknowledgements.md)
-AddPDF(Acknowledgements "")
-
-AddMarkdownInput(AuxiliaryPrograms "" 0 AuxiliaryPrograms.md)
-AddPDF(AuxiliaryPrograms "")
-
-AddMarkdownInput(EMS_Application_Guide "" 0 EMS_Application_Guide.md)
-AddPDF(EMS_Application_Guide "")
-
-
-if (BUILD_MONOLITHIC_ENGINEERINGREFERENCE)
-  AddSplitMarkdownInput(EngineeringReference 01-Overview.md 0)
-  AddSplitMarkdownInput(EngineeringReference 02-IntegratedSolution.md 1)
-  AddSplitMarkdownInput(EngineeringReference 03-SurfaceHeatBalance.md 2)
-  AddSplitMarkdownInput(EngineeringReference 04-AdvancedSurface.md 3)
-  AddSplitMarkdownInput(EngineeringReference 05-Climate.md 4)
-  AddSplitMarkdownInput(EngineeringReference 06-SolarRadiation.md 5)
-  AddSplitMarkdownInput(EngineeringReference 07-Daylighting.md 6)
-  AddSplitMarkdownInput(EngineeringReference 08-AirHeatBalance.md 7)
-  AddSplitMarkdownInput(EngineeringReference 09-BuildingSystemSimulation.md 8)
-  AddSplitMarkdownInput(EngineeringReference 10-Sizing.md 9)
-  AddSplitMarkdownInput(EngineeringReference OperationalFaults.md 10)
-  AddSplitMarkdownInput(EngineeringReference 11-DemandLimiting.md 11)
-  AddSplitMarkdownInput(EngineeringReference 12-AlternativeModeling.md 12)
-  AddSplitMarkdownInput(EngineeringReference 13-EncyclopaedicRefs.md 13)
-  AddSplitMarkdownInput(EngineeringReference 13a-EncyclopaedicRefs.md 14)
-  AddSplitMarkdownInput(EngineeringReference 13b-EncyclopaedicRefs.md 15)
-  AddSplitMarkdownInput(EngineeringReference 13c-EncyclopaedicRefs.md 16)
-  AddSplitMarkdownInput(EngineeringReference 13d-EncyclopaedicRefs.md 17)
-  AddSplitMarkdownInput(EngineeringReference 13e-EncyclopaedicRefs.md 18)
-  AddSplitMarkdownInput(EngineeringReference 13f-EncyclopaedicRefs.md 19)
-  AddSplitMarkdownInput(EngineeringReference 14-OnSiteGeneration.md 20)
-  AddSplitMarkdownInput(EngineeringReference 15-PerformanceCurves.md 21)
-  AddSplitMarkdownInput(EngineeringReference 16-Economics.md 22)
-  AddSplitMarkdownInput(EngineeringReference 17-SpecialModulesReporting.md 23)
-  AddSplitPDF(EngineeringReference .61)
-else()
-  # Note: put part2 first because it takes the longest to build, so we don't want things waiting on it
-  AddMarkdownInput(EngineeringReference "-part2" 6 07-Daylighting.md 08-AirHeatBalance.md 09-BuildingSystemSimulation.md 10-Sizing.md OperationalFaults.md 11-DemandLimiting.md 12-AlternativeModeling.md)
-  AddPDF(EngineeringReference "-part2")
-
-  AddMarkdownInput(EngineeringReference "-part1" 0 01-Overview.md 02-IntegratedSolution.md 03-SurfaceHeatBalance.md 04-AdvancedSurface.md 05-Climate.md 06-SolarRadiation.md )
-  AddPDF(EngineeringReference "-part1")
-
-  AddMarkdownInput(EngineeringReference "-part3" 13 13a-EncyclopaedicRefs.md 13b-EncyclopaedicRefs.md)
-  AddPDF(EngineeringReference "-part3")
-
-  AddMarkdownInput(EngineeringReference "-part4" 16 13c-EncyclopaedicRefs.md 13d-EncyclopaedicRefs.md)
-  AddPDF(EngineeringReference "-part4")
-
-  AddMarkdownInput(EngineeringReference "-part5" 17 13e-EncyclopaedicRefs.md 13f-EncyclopaedicRefs.md 14-OnSiteGeneration.md 15-PerformanceCurves.md 16-Economics.md 17-SpecialModulesReporting.md)
-  AddPDF(EngineeringReference "-part5")
-endif()
-
-AddMarkdownInput(ExternalInterfaces_Application_Guide "" 0 ExternalInterfaces_Application_Guide.md)
-AddPDF(ExternalInterfaces_Application_Guide "")
-
-AddMarkdownInput(GettingStarted "" 0 GettingStarted.md)
-AddPDF(GettingStarted "")
-
-AddMarkdownInput(InputOutputReference "" 0 01a-InputOutputReference.md 01b-InputOutputReference.md 01c-InputOutputReference.md 01d-InputOutputReference.md 02-HVACTemplates.md 03-Economics.md 04-Parametrics.md 05-InputForOutput.md 06-StandardOutputReports.md 07-WeatherData.md 08-RunningEnergyPlus.md 09-Appendix.md)
-AddPDF(InputOutputReference "")
-
-AddMarkdownInput(InterfaceDeveloper "" 0 InterfaceDeveloper.md)
-AddPDF(InterfaceDeveloper "")
-
-AddMarkdownInput(ModuleDeveloper "" 0 ModuleDeveloper.md)
-AddPDF(ModuleDeveloper "")
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-AddMarkdownInput(OutputDetailsAndExamples "" 0 OutputDetailsAndExamples.md)
-AddPDF(OutputDetailsAndExamples "")
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-AddMarkdownInput(PlantApplicationGuide "" 0 PlantApplicationGuide.md)
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-AddMarkdownInput(Tips_and_Tricks_Using_EnergyPlus "" 0 Tips_and_Tricks_Using_EnergyPlus.md)
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-AddMarkdownInput(Using_EnergyPlus_for_Compliance "" 0 Using_EnergyPlus_for_Compliance.md)
-AddPDF(Using_EnergyPlus_for_Compliance "")
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-
-
diff --git a/doc/src/bootstrap_nrel_html/base.html b/doc/src/bootstrap_nrel_html/base.html
deleted file mode 100644
index 1bf4a3640af..00000000000
--- a/doc/src/bootstrap_nrel_html/base.html
+++ /dev/null
@@ -1,93 +0,0 @@
-<!DOCTYPE html>
-<html lang="en">
-  <head>
-    <title>{{ page_title }}</title>
-    <meta http-equiv="X-UA-Compatible" content="IE=edge">
-    <meta charset="utf-8">
-    <meta name="viewport" content="width=device-width, initial-scale=1.0">
-    {% if page_description %}<meta name="description" content="{{ page_description }}">{% endif %}
-    {% if site_author %}<meta name="author" content="{{ site_author }}">{% endif %}
-    {% if canonical_url %}<link rel="canonical" href="{{ canonical_url }}">{% endif %}
-    {% if favicon %}<link rel="shortcut icon" href="{{ favicon }}">
-    {% else %}<link rel="shortcut icon" href="{{ base_url }}/img/favicon.ico">{% endif %}
-    <link href="{{ base_url }}/css/bootstrap-3.3.4.min.css" rel="stylesheet">
-    <link href="{{ base_url }}/css/font-awesome-4.3.0.min.css" rel="stylesheet">
-    <link href="{{ base_url }}/css/prettify-1.0.css" rel="stylesheet">
-    <link href="{{ base_url }}/css/base.css" rel="stylesheet">
-    {%- for path in extra_css %}
-    <link href="{{ path }}" rel="stylesheet">
-    {%- endfor %}
-    <!-- HTML5 shim and Respond.js IE8 support of HTML5 elements and media queries -->
-    <!--[if lt IE 9]>
-      <script src="https://oss.maxcdn.com/libs/html5shiv/3.7.0/html5shiv.js"></script>
-      <script src="https://oss.maxcdn.com/libs/respond.js/1.3.0/respond.min.js"></script>
-    <![endif]-->
-    <link href="http://netdna.bootstrapcdn.com/font-awesome/4.0.3/css/font-awesome.css" rel="stylesheet">
-    <script src="http://ajax.googleapis.com/ajax/libs/jquery/1.11.0/jquery.min.js"></script>
-  </head>
-  <body>
-    {% include "nav.html" %}
-    <div class="container">
-      <div class="row">
-        <div class="col-md-3">
-          {% include "toc.html" %}
-        </div>
-        <div class="col-md-9" role="main">
-          <script>
-           (function() {
-            var cx = '007045650438215436378:sghdz0ne6rg';
-            var gcse = document.createElement('script');
-            gcse.type = 'text/javascript';
-            gcse.async = true;
-            gcse.src = (document.location.protocol == 'https:' ? 'https:' : 'http:') +
-                '//www.google.com/cse/cse.js?cx=' + cx;
-            var s = document.getElementsByTagName('script')[0];
-            s.parentNode.insertBefore(gcse, s);
-           })();
-          </script>
-          <gcse:search></gcse:search>
-          {% include "content.html" %}
-          {% include "footer.html" %}
-        </div>
-      </div>
-    </div>
-    {% if include_search %}{% include "search.html" %}{% endif %}
-
-    <script src="{{ base_url }}/js/jquery-2.1.3.min.js"></script>
-    <script src="{{ base_url }}/js/bootstrap-3.3.4.min.js"></script>
-    <script src="{{ base_url }}/js/bootstrap-hover-dropdown-2.1.3.min.js"></script>
-    <script src="{{ base_url }}/js/prettify-1.0.min.js"></script>
-    <script src="{{ base_url }}/js/base.js"></script>
-    {%- for path in extra_javascript %}
-    <script src="{{ path }}"></script>
-    {%- endfor %}
-    <script type="text/x-mathjax-config">
-      MathJax.Hub.Config({
-        extensions: ["tex2jax.js"],
-        jax: ["input/TeX", "output/HTML-CSS"],
-        TeX: { equationNumbers: {autoNumber: "all"}},
-        showMathMenu: true,
-        showMathMenuMSIE: false,
-        "HTML-CSS": {
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-        tex2jax: {inlineMath: [['$','$'], ['\\(','\\)']]}
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-          id = $el.attr('id');
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-          if (id) {
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diff --git a/doc/src/bootstrap_nrel_html/content.html b/doc/src/bootstrap_nrel_html/content.html
deleted file mode 100644
index cddd07099f2..00000000000
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-{{ content }}
diff --git a/doc/src/bootstrap_nrel_html/css/base.css b/doc/src/bootstrap_nrel_html/css/base.css
deleted file mode 100644
index d6908a90d30..00000000000
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+++ /dev/null
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-body {
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-.footer {
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-/*
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diff --git a/doc/src/bootstrap_nrel_html/css/bootstrap-3.3.4.min.css b/doc/src/bootstrap_nrel_html/css/bootstrap-3.3.4.min.css
deleted file mode 100644
index cd1c616ad86..00000000000
--- a/doc/src/bootstrap_nrel_html/css/bootstrap-3.3.4.min.css
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-/*!
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diff --git a/doc/src/bootstrap_nrel_html/js/bootstrap-hover-dropdown-2.1.3.min.js b/doc/src/bootstrap_nrel_html/js/bootstrap-hover-dropdown-2.1.3.min.js
deleted file mode 100644
index 5a2adf8fa6b..00000000000
--- a/doc/src/bootstrap_nrel_html/js/bootstrap-hover-dropdown-2.1.3.min.js
+++ /dev/null
@@ -1,12 +0,0 @@
-/**
- * @preserve
- * Project: Bootstrap Hover Dropdown
- * Author: Cameron Spear
- * Version: v2.1.3
- * Contributors: Mattia Larentis
- * Dependencies: Bootstrap's Dropdown plugin, jQuery
- * Description: A simple plugin to enable Bootstrap dropdowns to active on hover and provide a nice user experience.
- * License: MIT
- * Homepage: http://cameronspear.com/blog/bootstrap-dropdown-on-hover-plugin/
- */
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\ No newline at end of file
diff --git a/doc/src/bootstrap_nrel_html/js/jquery-2.1.3.min.js b/doc/src/bootstrap_nrel_html/js/jquery-2.1.3.min.js
deleted file mode 100644
index 25714ed29ab..00000000000
--- a/doc/src/bootstrap_nrel_html/js/jquery-2.1.3.min.js
+++ /dev/null
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diff --git a/doc/src/bootstrap_nrel_html/nav.html b/doc/src/bootstrap_nrel_html/nav.html
deleted file mode 100644
index ce0b905094a..00000000000
--- a/doc/src/bootstrap_nrel_html/nav.html
+++ /dev/null
@@ -1,47 +0,0 @@
-<div class="container">
-  <nav class="navbar navbar-default navbar-fixed-top" role="navigation">
-    <div class="container">
-      <div class="navbar-header">
-        <button type="button" class="navbar-toggle collapsed" data-toggle="collapse" data-target=".navbar-collapse">
-          <span class="sr-only">Toggle navigation</span>
-          <span class="icon-bar"></span>
-          <span class="icon-bar"></span>
-          <span class="icon-bar"></span>
-        </button>
-        <a class="navbar-brand" href="{{ homepage_url }}"><img alt="" src="{{ base_url }}/img/EP_32x32.png"> {{ site_name }}</a>
-      </div>
-      <div class="navbar-collapse collapse">
-        <!-- Main navigation -->
-        <ul class="nav navbar-nav">
-        {% for nav_item in nav %}
-          {% if nav_item.children %}
-          <li class="dropdown{% if nav_item.active %} active{% endif %}">
-            <a href="#" class="dropdown-toggle" data-hover="dropdown" data-toggle="dropdown">{{ nav_item.title }} <span class="caret"></span></a>
-            <ul class="dropdown-menu" role="menu">
-            {% for nav_item in nav_item.children %}
-              <li{% if nav_item.active %} class="active"{% endif %}>
-                <a href="{{ nav_item.url }}">{{ nav_item.title }}</a>
-              </li>
-            {% endfor %}
-            </ul>
-          </li>
-          {% else %}
-          <li{% if nav_item.active %} class="active"{% endif %}>
-            <a href="{{ nav_item.url }}">{{ nav_item.title }}</a>
-          </li>
-          {% endif %}
-        {% endfor %}
-        </ul>
-
-        <!-- Search, Navigation and Repo links -->
-        <ul class="nav navbar-nav navbar-right">
-        {% if include_search %}
-          <li>
-            <a href="#searchModal" data-toggle="modal"><i class="fa fa-search"></i> Search</a>
-          </li>
-        {% endif %}
-        </ul>
-      </div>
-    </div>
-  </nav>
-</div>
diff --git a/doc/src/bootstrap_nrel_html/toc.html b/doc/src/bootstrap_nrel_html/toc.html
deleted file mode 100644
index 93b00b1d1a1..00000000000
--- a/doc/src/bootstrap_nrel_html/toc.html
+++ /dev/null
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-<div class="bs-docs-sidebar hidden-print affix well" role="complementary">
-  <ul class="nav">
-  {% for toc_item in toc %}
-    <li class="main{% if toc_item.active %} active{% endif %}"><a href="{{ toc_item.url }}">{{ toc_item.title }}</a>
-      <ul class="nav">
-        {% for toc_item in toc_item.children %}
-        <li><a href="{{ toc_item.url }}">{{ toc_item.title }}</a></li>
-        {% endfor %}
-      </ul>
-    </li>
-  {% endfor %}
-  </ul>
-  <div class="home-btn">
-    <a class="btn btn-default" role="button" href="https://github.com/NREL/EnergyPlus">Back to EnergyPlus</a>
-  </div>
-</div>
diff --git a/doc/src/bootstrap_nrel_htmlpdf/base.html b/doc/src/bootstrap_nrel_htmlpdf/base.html
deleted file mode 100644
index 5ab3662e5c8..00000000000
--- a/doc/src/bootstrap_nrel_htmlpdf/base.html
+++ /dev/null
@@ -1,75 +0,0 @@
-<!DOCTYPE html>
-<html lang="en">
-  <head>
-    <title>{{ page_title }}</title>
-    <meta http-equiv="X-UA-Compatible" content="IE=edge">
-    <meta charset="utf-8">
-    <meta name="viewport" content="width=device-width, initial-scale=1.0">
-    {% if page_description %}<meta name="description" content="{{ page_description }}">{% endif %}
-    {% if site_author %}<meta name="author" content="{{ site_author }}">{% endif %}
-    {% if canonical_url %}<link rel="canonical" href="{{ canonical_url }}">{% endif %}
-    {% if favicon %}<link rel="shortcut icon" href="{{ favicon }}">
-    {% else %}<link rel="shortcut icon" href="{{ base_url }}/img/favicon.ico">{% endif %}
-    <link href="{{ base_url }}/css/bootstrap-3.3.4.min.css" rel="stylesheet">
-    <link href="{{ base_url }}/css/font-awesome-4.3.0.min.css" rel="stylesheet">
-    <link href="{{ base_url }}/css/base.css" rel="stylesheet">
-    {%- for path in extra_css %}
-    <link href="{{ path }}" rel="stylesheet">
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-    <!--[if lt IE 9]>
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-    <script src="http://ajax.googleapis.com/ajax/libs/jquery/1.11.0/jquery.min.js"></script>
-    <script type="text/javascript" src="{{ base_url }}/js/generated_toc.js"></script> <!--: http://www.kryogenix.org/code/browser/generated-toc/ -->
-  </head>
-  <body>
-    <div class="container">
-      <div class="row">
-        <div class="col-md-9" role="main">
-          {% include "content.html" %}
-          {% include "footer.html" %}
-        </div>
-      </div>
-    </div>
-    {% if include_search %}{% include "search.html" %}{% endif %}
-
-    <script src="{{ base_url }}/js/jquery-2.1.3.min.js"></script>
-    <script src="{{ base_url }}/js/bootstrap-3.3.4.min.js"></script>
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-    <script src="{{ path }}"></script>
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-      MathJax.Hub.Config({
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-  </body>
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diff --git a/doc/src/bootstrap_nrel_htmlpdf/content.html b/doc/src/bootstrap_nrel_htmlpdf/content.html
deleted file mode 100644
index cddd07099f2..00000000000
--- a/doc/src/bootstrap_nrel_htmlpdf/content.html
+++ /dev/null
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-{{ content }}
diff --git a/doc/src/bootstrap_nrel_htmlpdf/css/base.css b/doc/src/bootstrap_nrel_htmlpdf/css/base.css
deleted file mode 100644
index 2382656ef77..00000000000
--- a/doc/src/bootstrap_nrel_htmlpdf/css/base.css
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-.container p img {
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-.container iframe {
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-a.navbar-brand > img {
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-/*
- * Side navigation
- *
- * Scrollspy and affixed enhanced navigation to highlight sections and secondary
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-
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-.bs-docs-sidebar.affix {
-    margin-left: 15px;
-    position: static;
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-.bs-docs-sidebar.well {
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-.bs-docs-sidebar {
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-/* Show and affix the side nav when space allows it */
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-    /* Widen the fixed sidebar */
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diff --git a/doc/src/bootstrap_nrel_htmlpdf/css/bootstrap-3.3.4.min.css b/doc/src/bootstrap_nrel_htmlpdf/css/bootstrap-3.3.4.min.css
deleted file mode 100644
index 1f06dd27fd6..00000000000
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a.attr("data-original-title"))&&a.attr("data-original-title",a.attr("title")||"").attr("title","")},c.prototype.hasContent=function(){return this.getTitle()},c.prototype.getPosition=function(b){b=b||this.$element;var c=b[0],d="BODY"==c.tagName,e=c.getBoundingClientRect();null==e.width&&(e=a.extend({},e,{width:e.right-e.left,height:e.bottom-e.top}));var f=d?{top:0,left:0}:b.offset(),g={scroll:d?document.documentElement.scrollTop||document.body.scrollTop:b.scrollTop()},h=d?{width:a(window).width(),height:a(window).height()}:null;return a.extend({},e,g,h,f)},c.prototype.getCalculatedOffset=function(a,b,c,d){return"bottom"==a?{top:b.top+b.height,left:b.left+b.width/2-c/2}:"top"==a?{top:b.top-d,left:b.left+b.width/2-c/2}:"left"==a?{top:b.top+b.height/2-d/2,left:b.left-c}:{top:b.top+b.height/2-d/2,left:b.left+b.width}},c.prototype.getViewportAdjustedDelta=function(a,b,c,d){var e={top:0,left:0};if(!this.$viewport)return e;var 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c=this;b&&(c=a(b.currentTarget).data("bs."+this.type),c||(c=new this.constructor(b.currentTarget,this.getDelegateOptions()),a(b.currentTarget).data("bs."+this.type,c))),c.tip().hasClass("in")?c.leave(c):c.enter(c)},c.prototype.destroy=function(){var a=this;clearTimeout(this.timeout),this.hide(function(){a.$element.off("."+a.type).removeData("bs."+a.type)})};var d=a.fn.tooltip;a.fn.tooltip=b,a.fn.tooltip.Constructor=c,a.fn.tooltip.noConflict=function(){return a.fn.tooltip=d,this}}(jQuery),+function(a){"use strict";function b(b){return this.each(function(){var d=a(this),e=d.data("bs.popover"),f="object"==typeof b&&b;(e||!/destroy|hide/.test(b))&&(e||d.data("bs.popover",e=new c(this,f)),"string"==typeof b&&e[b]())})}var c=function(a,b){this.init("popover",a,b)};if(!a.fn.tooltip)throw new Error("Popover requires tooltip.js");c.VERSION="3.3.4",c.DEFAULTS=a.extend({},a.fn.tooltip.Constructor.DEFAULTS,{placement:"right",trigger:"click",content:"",template:'<div class="popover" 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d=a.fn.popover;a.fn.popover=b,a.fn.popover.Constructor=c,a.fn.popover.noConflict=function(){return a.fn.popover=d,this}}(jQuery),+function(a){"use strict";function b(c,d){this.$body=a(document.body),this.$scrollElement=a(a(c).is(document.body)?window:c),this.options=a.extend({},b.DEFAULTS,d),this.selector=(this.options.target||"")+" .nav li > a",this.offsets=[],this.targets=[],this.activeTarget=null,this.scrollHeight=0,this.$scrollElement.on("scroll.bs.scrollspy",a.proxy(this.process,this)),this.refresh(),this.process()}function c(c){return this.each(function(){var d=a(this),e=d.data("bs.scrollspy"),f="object"==typeof c&&c;e||d.data("bs.scrollspy",e=new b(this,f)),"string"==typeof c&&e[c]()})}b.VERSION="3.3.4",b.DEFAULTS={offset:10},b.prototype.getScrollHeight=function(){return this.$scrollElement[0].scrollHeight||Math.max(this.$body[0].scrollHeight,document.documentElement.scrollHeight)},b.prototype.refresh=function(){var 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-var e=c.find(".active:last a"),f=a.Event("hide.bs.tab",{relatedTarget:b[0]}),g=a.Event("show.bs.tab",{relatedTarget:e[0]});if(e.trigger(f),b.trigger(g),!g.isDefaultPrevented()&&!f.isDefaultPrevented()){var h=a(d);this.activate(b.closest("li"),c),this.activate(h,h.parent(),function(){e.trigger({type:"hidden.bs.tab",relatedTarget:b[0]}),b.trigger({type:"shown.bs.tab",relatedTarget:e[0]})})}}},c.prototype.activate=function(b,d,e){function f(){g.removeClass("active").find("> .dropdown-menu > .active").removeClass("active").end().find('[data-toggle="tab"]').attr("aria-expanded",!1),b.addClass("active").find('[data-toggle="tab"]').attr("aria-expanded",!0),h?(b[0].offsetWidth,b.addClass("in")):b.removeClass("fade"),b.parent(".dropdown-menu").length&&b.closest("li.dropdown").addClass("active").end().find('[data-toggle="tab"]').attr("aria-expanded",!0),e&&e()}var g=d.find("> .active"),h=e&&a.support.transition&&(g.length&&g.hasClass("fade")||!!d.find("> .fade").length);g.length&&h?g.one("bsTransitionEnd",f).emulateTransitionEnd(c.TRANSITION_DURATION):f(),g.removeClass("in")};var d=a.fn.tab;a.fn.tab=b,a.fn.tab.Constructor=c,a.fn.tab.noConflict=function(){return a.fn.tab=d,this};var e=function(c){c.preventDefault(),b.call(a(this),"show")};a(document).on("click.bs.tab.data-api",'[data-toggle="tab"]',e).on("click.bs.tab.data-api",'[data-toggle="pill"]',e)}(jQuery),+function(a){"use strict";function b(b){return this.each(function(){var d=a(this),e=d.data("bs.affix"),f="object"==typeof b&&b;e||d.data("bs.affix",e=new c(this,f)),"string"==typeof b&&e[b]()})}var c=function(b,d){this.options=a.extend({},c.DEFAULTS,d),this.$target=a(this.options.target).on("scroll.bs.affix.data-api",a.proxy(this.checkPosition,this)).on("click.bs.affix.data-api",a.proxy(this.checkPositionWithEventLoop,this)),this.$element=a(b),this.affixed=null,this.unpin=null,this.pinnedOffset=null,this.checkPosition()};c.VERSION="3.3.4",c.RESET="affix affix-top affix-bottom",c.DEFAULTS={offset:0,target:window},c.prototype.getState=function(a,b,c,d){var e=this.$target.scrollTop(),f=this.$element.offset(),g=this.$target.height();if(null!=c&&"top"==this.affixed)return c>e?"top":!1;if("bottom"==this.affixed)return null!=c?e+this.unpin<=f.top?!1:"bottom":a-d>=e+g?!1:"bottom";var h=null==this.affixed,i=h?e:f.top,j=h?g:b;return null!=c&&c>=e?"top":null!=d&&i+j>=a-d?"bottom":!1},c.prototype.getPinnedOffset=function(){if(this.pinnedOffset)return this.pinnedOffset;this.$element.removeClass(c.RESET).addClass("affix");var a=this.$target.scrollTop(),b=this.$element.offset();return this.pinnedOffset=b.top-a},c.prototype.checkPositionWithEventLoop=function(){setTimeout(a.proxy(this.checkPosition,this),1)},c.prototype.checkPosition=function(){if(this.$element.is(":visible")){var b=this.$element.height(),d=this.options.offset,e=d.top,f=d.bottom,g=a(document.body).height();"object"!=typeof d&&(f=e=d),"function"==typeof e&&(e=d.top(this.$element)),"function"==typeof f&&(f=d.bottom(this.$element));var h=this.getState(g,b,e,f);if(this.affixed!=h){null!=this.unpin&&this.$element.css("top","");var i="affix"+(h?"-"+h:""),j=a.Event(i+".bs.affix");if(this.$element.trigger(j),j.isDefaultPrevented())return;this.affixed=h,this.unpin="bottom"==h?this.getPinnedOffset():null,this.$element.removeClass(c.RESET).addClass(i).trigger(i.replace("affix","affixed")+".bs.affix")}"bottom"==h&&this.$element.offset({top:g-b-f})}};var d=a.fn.affix;a.fn.affix=b,a.fn.affix.Constructor=c,a.fn.affix.noConflict=function(){return a.fn.affix=d,this},a(window).on("load",function(){a('[data-spy="affix"]').each(function(){var c=a(this),d=c.data();d.offset=d.offset||{},null!=d.offsetBottom&&(d.offset.bottom=d.offsetBottom),null!=d.offsetTop&&(d.offset.top=d.offsetTop),b.call(c,d)})})}(jQuery);
\ No newline at end of file
diff --git a/doc/src/bootstrap_nrel_htmlpdf/js/bootstrap-hover-dropdown-2.1.3.min.js b/doc/src/bootstrap_nrel_htmlpdf/js/bootstrap-hover-dropdown-2.1.3.min.js
deleted file mode 100644
index 5a2adf8fa6b..00000000000
--- a/doc/src/bootstrap_nrel_htmlpdf/js/bootstrap-hover-dropdown-2.1.3.min.js
+++ /dev/null
@@ -1,12 +0,0 @@
-/**
- * @preserve
- * Project: Bootstrap Hover Dropdown
- * Author: Cameron Spear
- * Version: v2.1.3
- * Contributors: Mattia Larentis
- * Dependencies: Bootstrap's Dropdown plugin, jQuery
- * Description: A simple plugin to enable Bootstrap dropdowns to active on hover and provide a nice user experience.
- * License: MIT
- * Homepage: http://cameronspear.com/blog/bootstrap-dropdown-on-hover-plugin/
- */
-!function(e,n){var o=e();e.fn.dropdownHover=function(t){return"ontouchstart"in document?this:(o=o.add(this.parent()),this.each(function(){function r(){n.clearTimeout(a),n.clearTimeout(i),i=n.setTimeout(function(){o.find(":focus").blur(),f.instantlyCloseOthers===!0&&o.removeClass("open"),n.clearTimeout(i),d.attr("aria-expanded","true"),s.addClass("open"),d.trigger(l)},f.hoverDelay)}var a,i,d=e(this),s=d.parent(),u={delay:500,hoverDelay:0,instantlyCloseOthers:!0},h={delay:e(this).data("delay"),hoverDelay:e(this).data("hover-delay"),instantlyCloseOthers:e(this).data("close-others")},l="show.bs.dropdown",c="hide.bs.dropdown",f=e.extend(!0,{},u,t,h);s.hover(function(e){return s.hasClass("open")||d.is(e.target)?void r(e):!0},function(){n.clearTimeout(i),a=n.setTimeout(function(){d.attr("aria-expanded","false"),s.removeClass("open"),d.trigger(c)},f.delay)}),d.hover(function(e){return s.hasClass("open")||s.is(e.target)?void r(e):!0}),s.find(".dropdown-submenu").each(function(){var o,t=e(this);t.hover(function(){n.clearTimeout(o),t.children(".dropdown-menu").show(),t.siblings().children(".dropdown-menu").hide()},function(){var e=t.children(".dropdown-menu");o=n.setTimeout(function(){e.hide()},f.delay)})})}))},e(document).ready(function(){e('[data-hover="dropdown"]').dropdownHover()})}(jQuery,window);
\ No newline at end of file
diff --git a/doc/src/bootstrap_nrel_htmlpdf/js/generated_toc.js b/doc/src/bootstrap_nrel_htmlpdf/js/generated_toc.js
deleted file mode 100644
index 5d5c17153dd..00000000000
--- a/doc/src/bootstrap_nrel_htmlpdf/js/generated_toc.js
+++ /dev/null
@@ -1,315 +0,0 @@
-/** Generated TOC
-    Stuart Langridge, July 2007
-    
-    Generate a table of contents, based on headings in the page.
-    
-    To place the TOC on the page, add
-    
-    <div id="generated-toc"></div>
-    
-    to the page where you want the TOC to appear. If this element
-    is not present, the TOC will not appear.
-    
-    The TOC defaults to displaying all headings that are contained within
-    the same element as it itself is contained in (or all headings on the
-    page if you did not provide a generated-toc container). To override this,
-    provide a "highest heading" value by adding class="generate_from_h3"
-    (or h2, h4, etc) to the container. (If unspecified, this will display all
-    headings, as if class="generate_from_h1" was specified.)
-    
-    The TOC defaults to operating only on headings contained within the same
-    element as it itself, i.e., in a page like this:
-    
-    <div>
-      <div>
-        <div id="generated-toc"></div>
-        <h1>foo</h1>
-        <h2>bar</h2>
-      </div>
-      <h1>quux</h1>
-    </div>
-    
-    The "quux" heading will not appear in the TOC. To override this,
-    add class="generate_for_page" to the container, which will process
-    all headings on the page wheresoever they may be.
-
-*/
-
-generated_toc = {
-  generate: function() {
-    // Identify our TOC element, and what it applies to
-    generate_from = '0';
-    generate_for = 'unset';
-    tocparent = document.getElementById('generated-toc');
-    if (tocparent) {
-      // there is a div class="generated-toc" in the document
-      // dictating where the TOC should appear
-      classes = tocparent.className.split(/\s+/);
-      for (var i=0; i<classes.length; i++) {
-        // if it specifies which heading level to generate from,
-        // or what level to generate for, save these specifications
-        if (classes[i].match(/^generate_from_h[1-6]$/)) {
-          generate_from = classes[i].substr(classes[i].length-1,1);
-        } else if (classes[i].match(/^generate_for_[a-z]+$/)) {
-          generate_for = classes[i].match(/^generate_for_([a-z])+$/)[1];
-        }
-      }
-    } else {
-      // They didn't specify a TOC element; exit
-      return;
-    }
-    
-    // set top_node to be the element in the document under which
-    // we'll be analysing headings
-    if (generate_for == 'page') {
-      top_node = document.getElementsByTagName('body');
-    } else {
-      // i.e., explicitly set to "parent", left blank (so "unset"),
-      // or some invalid value
-      top_node = tocparent.parentNode;
-    }
-    
-    // If there isn't a specified header level to generate from, work
-    // out what the first header level inside top_node is
-    // and make that the specified header level
-    if (generate_from == 0) {
-      first_header_found = generated_toc.findFirstHeader(top_node);
-      if (!first_header_found) {
-        // there were no headers at all inside top_node!
-        return;
-      } else {
-        generate_from = first_header_found.toLowerCase().substr(1);
-      }
-    }
-    
-    // add all levels of heading we're paying attention to to the
-    // headings_to_treat dictionary, ready to be filled in later
-    headings_to_treat = {"h3":''};
-    for (var i=2; i>= parseInt(generate_from); i--) {
-      headings_to_treat["h" + i] = '';
-    }
-    
-    // get headings. We can't say 
-    // getElementsByTagName("h1" or "h2" or "h3"), etc, so get all
-    // elements and filter them ourselves
-    // need to use .all here because IE doesn't support gEBTN('*')
-    nodes = top_node.all ? top_node.all : top_node.getElementsByTagName('*');
-    
-    // put all the headings we care about in headings
-    headings = [];
-    for (var i=0; i<nodes.length;i++) {
-      if (nodes[i].nodeName.toLowerCase() in headings_to_treat) {
-        // if heading has class no-TOC, skip it
-        if ((' ' + nodes[i].className + ' ').indexOf('no-TOC') != -1) {
-          continue;
-        }
-        headings.push(nodes[i]);
-      }
-    }
-    
-    // make the basic elements of the TOC itself, ready to fill into
-    
-    // first, check if there's a cookie defined to save the state as open
-    status = generated_toc.readCookie("generated_toc_display");
-    if (status && status == "open") {
-      display_initially = "block";
-      toggle_initially = "Table of contents";
-    } else {
-      display_initially = "none";
-      toggle_initially = "Show table of contents";
-    }
-
-    cur_head_lvl = "h" + generate_from;
-    cur_list_el = document.createElement('ul');
-    cur_list_el.style.display = "block"; //display_initially;
-    p = document.createElement('p');
-    span = document.createElement('span');
-    span.className = 'hidden';
-    a = document.createElement('a');
-    a.href = '#aftertoc';
-    a.appendChild(document.createTextNode('skip table of contents'));
-    span.appendChild(a);
-    p.appendChild(span);
-    tocparent.appendChild(p);
-    p = document.createElement('p');
-    p.id = 'toggle-container'; 
-    a = document.createElement('a');
-    a.id = 'generated_toc_d_toggle';
-    a.appendChild(document.createTextNode("Table of contents")); //toggle_initially));
-    p.appendChild(a);
-    a.onclick = generated_toc.wrapOpenClose(a,cur_list_el);
-    a.href = '#';
-    tocparent.appendChild(p);
-    tocparent.appendChild(cur_list_el);
-    
-    // now walk through our saved heading nodes
-    for (var i=0; i<headings.length; i++) {
-      this_head_el = headings[i];
-      this_head_lvl = headings[i].nodeName.toLowerCase();
-      if (!this_head_el.id) {
-        // if heading doesn't have an ID, give it one
-        this_head_el.id = 'heading_toc_j_' + i;
-        this_head_el.setAttribute('tabindex','-1');
-      }
-      
-      while(this_head_lvl > cur_head_lvl) {
-        // this heading is at a lower level than the last one;
-        // create additional nested lists to put it at the right level
-
-        // get the *last* LI in the current list, and add our new UL to it
-        var last_listitem_el = null;
-        for (var j=0; j<cur_list_el.childNodes.length; j++) {
-          if (cur_list_el.childNodes[j].nodeName.toLowerCase() == 'li') {
-            last_listitem_el = cur_list_el.childNodes[j];
-          }
-        }
-        if (!last_listitem_el) {
-          // there aren't any LIs, so create a new one to add the UL to
-          last_listitem_el = document.createElement('li');
-        }
-        new_list_el = document.createElement('ul');
-        last_listitem_el.appendChild(new_list_el);
-        cur_list_el.appendChild(last_listitem_el);
-        cur_list_el = new_list_el;
-        cur_head_lvl = 'h' + (parseInt(cur_head_lvl.substr(1,1)) + 1);
-      }
-      
-      while (this_head_lvl < cur_head_lvl) {
-        // this heading is at a higher level than the last one;
-        // go back up the TOC to put it at the right level
-        cur_list_el = cur_list_el.parentNode.parentNode;
-        cur_head_lvl = 'h' + (parseInt(cur_head_lvl.substr(1,1)) - 1);
-      }
-      
-      // create a link to this heading, and add it to the TOC
-      li = document.createElement('li');
-      a = document.createElement('a');
-      a.href = '#' + this_head_el.id;
-      a.appendChild(document.createTextNode(generated_toc.innerText(this_head_el)));
-      li.appendChild(a);
-      cur_list_el.appendChild(li);
-    }
-    
-    // add an aftertoc paragraph as destination for the skip-toc link
-    p = document.createElement('p');
-    p.id = 'aftertoc';
-    tocparent.appendChild(p);
-    
-    // go through the TOC and find all LIs that are "empty", i.e., contain
-    // only ULs and no links, and give them class="missing"
-    var alllis = tocparent.getElementsByTagName("li");
-    for (var i=0; i<alllis.length; i++) {
-      var foundlink = false;
-      for (var j=0; j<alllis[i].childNodes.length; j++) {
-        if (alllis[i].childNodes[j].nodeName.toLowerCase() == 'a') {
-          foundlink = true;
-        }
-      }
-      if (!foundlink) {
-        alllis[i].className = "missing";
-      } else {
-        alllis[i].className = "notmissing";
-      }
-    }
-    
-  },
-  
-  wrapOpenClose: function(a, cur_list_el) {
-    // we return a function here so that it acts as a closure;
-    // in essence the inner function, which is the event handler
-    // for clicking on the toggle-toc link, remembers the a and cur_list_el
-    // elements as they are when they're passed in to it.
-    // This is an explicit function rather than an anonymous function
-    // defined where it's called so it's easier to understand.
-    return function(e) {
-      d = cur_list_el.style.display;
-      a.firstChild.nodeValue = (d == 'block' ? 'Show' : '') + ' Table of contents';
-      a.className = (d == 'block' ? 'toggle-closed' : 'toggle-open'); 
-      cur_list_el.style.display = d == 'block' ? 'none' : 'block';
-      // set a cookie to "open" or "closed" to save the state of the TOC
-      if (cur_list_el.style.display == "block") {
-        generated_toc.createCookie("generated_toc_display","open",21);
-      } else {
-        generated_toc.createCookie("generated_toc_display","closed",21);
-      }
-      if (window.event) {
-        window.event.returnValue = false;
-        window.event.cancelBubble = true;
-      } else {
-        e.preventDefault();
-        e.stopPropagation();
-      }
-    }
-  },
-  
-  /* cookie handling: http://www.quirksmode.org/js/cookies.html */
-  createCookie: function(name,value,days) {
-    if (days) {
-      var date = new Date();
-      date.setTime(date.getTime()+(days*24*60*60*1000));
-      var expires = "; expires="+date.toGMTString();
-    }
-    else var expires = "";
-    document.cookie = name+"="+value+expires+"; path=/";
-  },
-
-  readCookie: function(name) {
-    var nameEQ = name + "=";
-    var ca = document.cookie.split(';');
-    for(var i=0;i < ca.length;i++) {
-      var c = ca[i];
-      while (c.charAt(0)==' ') c = c.substring(1,c.length);
-      if (c.indexOf(nameEQ) == 0) 
-        return c.substring(nameEQ.length,c.length);
-    }
-    return null;
-  },
-
-  eraseCookie: function(name) {
-    createCookie(name,"",-1);
-  },  
-  
-  innerText: function(el) {
-    return (typeof(el.innerText) != 'undefined') ? el.innerText :
-          (typeof(el.textContent) != 'undefined') ? el.textContent :
-          el.innerHTML.replace(/<[^>]+>/g, '');
-  },
-  
-  findFirstHeader: function(node) {
-    // a recursive function which returns the first header it finds inside
-    // node, or null if there are no functions inside node.
-    var nn = node.nodeName.toLowerCase();
-    if (nn.match(/^h[1-6]$/)) {
-      // this node is itself a header; return our name
-      return nn;
-    } else {
-      for (var i=0; i<node.childNodes.length; i++) {
-        var subvalue = generated_toc.findFirstHeader(node.childNodes[i]);
-        // if one of the subnodes finds a header, abort the loop and return it
-        if (subvalue) return subvalue;
-      }
-      // no headers in this node at all
-      return null;
-    }
-  },
-
-  init: function() {
-    // quit if this function has already been called
-    if (arguments.callee.done) return;
-
-    // flag this function so we don't do the same thing twice
-    arguments.callee.done = true;
-
-    generated_toc.generate();
-  }
-};
-
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-document.addEventListener("DOMContentLoaded",i,false); } else if(e){     (
-function(){var t=document.createElement('doc:rdy');try{t.doScroll('left');
-i();t=null;}catch(e){st(arguments.callee,0);}})();}else{window.onload=i;}})(generated_toc.init);
-
-
diff --git a/doc/src/bootstrap_nrel_htmlpdf/js/jquery-2.1.3.min.js b/doc/src/bootstrap_nrel_htmlpdf/js/jquery-2.1.3.min.js
deleted file mode 100644
index 25714ed29ab..00000000000
--- a/doc/src/bootstrap_nrel_htmlpdf/js/jquery-2.1.3.min.js
+++ /dev/null
@@ -1,4 +0,0 @@
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diff --git a/doc/src/bootstrap_nrel_htmlpdf/nav.html b/doc/src/bootstrap_nrel_htmlpdf/nav.html
deleted file mode 100644
index ce0b905094a..00000000000
--- a/doc/src/bootstrap_nrel_htmlpdf/nav.html
+++ /dev/null
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-  <nav class="navbar navbar-default navbar-fixed-top" role="navigation">
-    <div class="container">
-      <div class="navbar-header">
-        <button type="button" class="navbar-toggle collapsed" data-toggle="collapse" data-target=".navbar-collapse">
-          <span class="sr-only">Toggle navigation</span>
-          <span class="icon-bar"></span>
-          <span class="icon-bar"></span>
-          <span class="icon-bar"></span>
-        </button>
-        <a class="navbar-brand" href="{{ homepage_url }}"><img alt="" src="{{ base_url }}/img/EP_32x32.png"> {{ site_name }}</a>
-      </div>
-      <div class="navbar-collapse collapse">
-        <!-- Main navigation -->
-        <ul class="nav navbar-nav">
-        {% for nav_item in nav %}
-          {% if nav_item.children %}
-          <li class="dropdown{% if nav_item.active %} active{% endif %}">
-            <a href="#" class="dropdown-toggle" data-hover="dropdown" data-toggle="dropdown">{{ nav_item.title }} <span class="caret"></span></a>
-            <ul class="dropdown-menu" role="menu">
-            {% for nav_item in nav_item.children %}
-              <li{% if nav_item.active %} class="active"{% endif %}>
-                <a href="{{ nav_item.url }}">{{ nav_item.title }}</a>
-              </li>
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-          </li>
-          {% else %}
-          <li{% if nav_item.active %} class="active"{% endif %}>
-            <a href="{{ nav_item.url }}">{{ nav_item.title }}</a>
-          </li>
-          {% endif %}
-        {% endfor %}
-        </ul>
-
-        <!-- Search, Navigation and Repo links -->
-        <ul class="nav navbar-nav navbar-right">
-        {% if include_search %}
-          <li>
-            <a href="#searchModal" data-toggle="modal"><i class="fa fa-search"></i> Search</a>
-          </li>
-        {% endif %}
-        </ul>
-      </div>
-    </div>
-  </nav>
-</div>
diff --git a/doc/src/bootstrap_nrel_htmlpdf/toc.html b/doc/src/bootstrap_nrel_htmlpdf/toc.html
deleted file mode 100644
index 93b00b1d1a1..00000000000
--- a/doc/src/bootstrap_nrel_htmlpdf/toc.html
+++ /dev/null
@@ -1,16 +0,0 @@
-<div class="bs-docs-sidebar hidden-print affix well" role="complementary">
-  <ul class="nav">
-  {% for toc_item in toc %}
-    <li class="main{% if toc_item.active %} active{% endif %}"><a href="{{ toc_item.url }}">{{ toc_item.title }}</a>
-      <ul class="nav">
-        {% for toc_item in toc_item.children %}
-        <li><a href="{{ toc_item.url }}">{{ toc_item.title }}</a></li>
-        {% endfor %}
-      </ul>
-    </li>
-  {% endfor %}
-  </ul>
-  <div class="home-btn">
-    <a class="btn btn-default" role="button" href="https://github.com/NREL/EnergyPlus">Back to EnergyPlus</a>
-  </div>
-</div>
diff --git a/doc/src/docs/Acknowledgements/Acknowledgements.md b/doc/src/docs/Acknowledgements/Acknowledgements.md
deleted file mode 100644
index 00c54663d4d..00000000000
--- a/doc/src/docs/Acknowledgements/Acknowledgements.md
+++ /dev/null
@@ -1,277 +0,0 @@
-(EnergyPlus Documentation, v8.4.0)
-
-Notices and Acknowledgments 
-===========================
-
-Copyright Notice
-----------------
-
-Copyright (c) 1996-2015 The Board of Trustees of the University of Illinois and The Regents of the University of California through Ernest Orlando Lawrence Berkeley National Laboratory. All rights reserved.
-
-Portions of the EnergyPlusâ„¢ software package have been developed and copyrighted by other individuals, companies and institutions. These portions have been incorporated into the EnergyPlus software package under license.
-
-**In addition to the primary authorship of the LBNL Simulation Research Group (**[**http://simulationresearch.lbl.gov/**](http://simulationresearch.lbl.gov/)**) and the UIUC Building Systems Laboratory, the following have contributed to EnergyPlus Versions (includes all minor revisions):**
-
-Portions of the EnergyPlus weather processor were developed by US Department of Energy, Office of Building Technologies.
-
-Portions of the input processing, output processing, weather processor, BLAST Translator were developed by US Army Corps of Engineers, Construction Engineering Research Laboratories, 2902 Newmark Drive, Champaign IL  61821. [http://www.erdc.usace.army.mil/Locations/ConstructionEngineeringResearchLaboratory.aspx](http://www.erdc.usace.army.mil/Locations/ConstructionEngineeringResearchLaboratory.aspx)
-
-Portions of this software package were developed for Ernest Orlando Lawrence Berkeley National Laboratory and Florida Solar Energy Center by Linda Lawrie of DHL Consulting.
-
-Portions of this software package were developed for Ernest Orlando Lawrence Berkeley National Laboratory and Florida Solar Energy Center by C.O. Pedersen Associates.
-
-Portions of the EnergyPlus utility software (EP-Launch, IDFEditor, DOE2Translator, HVAC-Diagram, ExpandObjects, CSVProc, ParametricPreprocessor, AppGPostProcess, EP-Compare, and convertESOMTR) were developed by GARD Analytics, Inc. 115 S. Wilke Road, Suite 105, Arlington Heights, IL, USA, &lt;info@gard.com&gt;, [www.gard.com](http://www.gard.com/). GARD Analytics performed independent verification and validation testing of the software after developing the testing strategy and plan. GARD Analytics was also responsible for gas absorption chiller, desiccant dehumidifier, ice storage (simple), table reports, economics and life cycle costing.
-
-Portions of flow resolver, chiller models (absorption, electric, const cop, engine-driven, gas-turbine), generator models (diesel electric, gas turbine), furnace models, heat recovery loop, plant loop, plant condenser loop, air-change dependent inside film coefficients were developed by Oklahoma State University, 110 Engineering North, Stillwater, OK 74078.
-
-Portions of EnergyPlus related to the models for EMPD moisture calculations, DX coils, furnace/unitary systems, air-to-air heat pumps, changeover-bypass VAV systems, packaged terminal heat pumps, cooling towers, AirflowNetwork, refrigerated cases, reformulated and electric EIR chillers, desuperheater air and water heating coils, heat pump water heaters, desiccant and generic air-to-air heat exchangers, window screens, and thermal comfort controls were developed by University of Central Florida, Florida Solar Energy Center (FSEC), 1679 Clearlake Road, Cocoa, FL  32922, [www.fsec.ucf.edu/](http://www.fsec.ucf.edu/).
-
-Portions of the refrigeration model and the exhaust-fired absorption chiller model were developed by Oak Ridge National Laboratory, Bethel Valley Road, Oak Ridge, Tennessee 37831.
-
-Portions of EnergyPlus were developed by the National Renewable Energy Laboratory (NREL), 1617 Cole Blvd, Golden, CO 80401.
-
-Portions of EnergyPlus related to transformer losses model, autosizing calculations, life cycle costing and chemical battery storage model were developed by Pacific Northwest National Laboratory (PNNL), P.O. Box 999, Richland, WA 99352.
-
-EnergyPlus v1.0.1, v1.0.2, v1.0.3, v1.1, v1.1.1 (Wintel platform) included a link to TRNSYS (The Transient Energy System Simulation Tool) for photovoltaic calculations developed by Thermal Energy System Specialists, 2916 Marketplace Drive, Suite 104, Madison, WI 53719; Tel: (608) 274-2577. EnergyPlus v1.2 and later includes Photovoltaic calculations implemented in EnergyPlus by Thermal Energy System Specialists. This model was originally developed by Oystein Ulleberg, Institute for Energy Technology, Norway -- based on the Duffie and Beckman equivalent one-diode model.
-
-Portions of this software package that convert certain stand-alone heat transfer models for slab-on-grade and basement foundations were developed by William Bahnfleth, Cynthia Cogil, and Edward Clements, Department of Architectural Engineering, Pennsylvania State University, 224 Engineering Unit A, University Park, Pennsylvania 16802-1416, (814) 863-2076.
-
-The concept and initial implementation for the EnergyPlus COM/DLL version (Wintel platform) was made possible through cooperation with DesignBuilder Software, Ltd, Andy Tindale – an EnergyPlus collaborative developer.
-
-The thickness, conductivity, density and specific heat values of the material layers for the constructions in the Composite Wall Construction reference data set have been taken from the ASHRAE report “Modeling Two- and Three-Dimensional Heat Transfer through Composite Wall and Roof Assemblies in Hourly Energy Simulation Programs (1145-TRP),� by Enermodal Engineering Limited, Oak Ridge National Laboratory, and the Polish Academy of Sciences, January 2001.
-
-EnergyPlus v1.2 and later versions contains DELight2, a simulation engine for daylighting and electric lighting system analysis developed at Ernest Orlando Lawrence Berkeley National Laboratory.
-
-EnergyPlus v1.2.2 through v3.1 contained links to SPARK, a simulation engine for detailed system modeling developed at Ernest Orlando Lawrence Berkeley National Laboratory in conjunction with Ayres Sowell Associates, Inc.
-
-The airflow calculation portion of the EnergyPlus AirflowNetwork model was based on AIRNET written by George Walton of the National Institute for Standards and Technology (NIST), 100 Bureau Drive, Gaithersburg, MD 20899. The EnergyPlus AirflowNetwork model also includes portions of stack effect and detailed large opening from an early version of COMIS (Conjunction Of Multizone Infiltration Specialists) developed by a multinational, multi-institutional effort under the auspices of the International Energy Agency's Buildings and Community Systems Agreement working group focusing on multizone air flow modeling (Annex 23) and now administered by the Swiss Federal Laboratories for Materials Testing and Research (EMPA), Division 175, Überlandstrasse 129, CH-8600 Dübendorf, Switzerland.
-
-The EnergyPlus model for displacement ventilation and cross-ventilation (version v1.2 and later) was developed by Guilherme Carrilho da Graça (Department of Mechanical and Aerospace Engineering, University of California, San Diego and NaturalWorks) and Paul Linden (Department of Mechanical and Aerospace Engineering, University of California, San Diego).
-
-The EnergyPlus models for UFAD served zones were developed by Anna Liu and Paul Linden at the Department of Mechanical and Aerospace Engineering, University of California, San Diego.
-
-ASHRAE research project 1254-RP supported the development of the following features first added in EnergyPlus v1.2.2: DXSystem:AirLoop enhancements (valid as OA system equipment, new humidity control options); New set point managers: SET POINT MANAGER:SINGLE ZONE HEATING, SET POINT MANAGER:SINGLE ZONE COOLING, and SET POINT MANAGER:OUTSIDE AIR PRETREAT; New 2-stage DX coil with enhanced dehumidification option (COIL:DX:MultiMode:CoolingEmpirical); Additional DESICCANT DEHUMIDIFIER:SOLID setpoint control option;  American Society of Heating Refrigerating and Air-Conditioning Engineers, Inc., 1791 Tullie Circle, N.E., Atlanta, GA 30329. [www.ashrae.org/](http://www.ashrae.org/). Work performed by GARD Analytics, Inc., 115 S. Wilke Road, Suite 105, Arlington Heights, IL, USA, &lt;info@gard.com&gt;, [www.gard.com/](http://www.gard.com/), November 2004. These items were renamed in V3.0 to SetpointManager:SingleZone:Heating, SetpointManager:SingleZone:Cooling, SetpointManager:OutdoorAirPretreat, Coil:Cooling:DX:TwoStageWithHumidityControlMode, Dehumidifier:Desiccant:NoFans, respectively.
-
-The Ecoroof (Green Roof) model, first introduced in EnergyPlus v2.0, was developed at Portland State University, by David Sailor and his students. It is based on the FASST vegetation models developed by Frankenstein and Koenig for the US Army Corps of Engineers.
-
-The HAMT (Heat And Moisture Transfer) model, first introduced in EnergyPlus v3.0.0 was developed by Phillip Biddulph, Complex Built Environment Systems, The Bartlett School of Graduate Studies, University College London, Gower Street, London WC1E 6BT, United Kingdom. [http://www.cbes.ucl.ac.uk/](http://www.cbes.ucl.ac.uk/).
-
-The SQLite output module, first introduced in EnergyPlus v3.0.0, was developed by Gregory B. Stark, P.E., Building Synergies, LLC, 1860 Washington Street, Suite 208, Denver, Colorado 80203, United States.
-
-Refrigeration compressor performance data and refrigeration practices were provided by CDH Energy, Cazenovia, NY 12035.
-
-The external interface was developed by Michael Wetter and Philip Haves (Lawrence Berkeley National Laboratory) and by Rui Zhang (Carnegie Mellon University). An earlier upgrade to a development version of EnergyPlus 3.0 was implemented by Charles Corbin, Anthony Florita, Gregor Henze and Peter May-Ostendorp (University of Colorado at Boulder).
-
-Various suggestions for time reduction, improved documentation and other items have been incorporated from Autodesk, Inc., Bentley Systems, and others.
-
-Particular recognition goes to Noel Keen (LBNL Computational Research Division) and Geof Sawaya (Oak Ridge National Laboratory fellow) who have done extensive profiling and creation of time reduction features that have gone into the code.
-
-Second Law modified the WaterToAirHeatPump:EquationFit module to include the variable “WaterCyclingMode�. This variable determines whether the heat pump water flow is constant, whether it cycles with the compressor, or whether it is constant when the heat pump is active. WaterFlowMode is set by the HVAC wrapper object; either ZoneHVAC:WaterToAirHeatPump or AirLoopHVAC:UnitaryHeatPump:WaterToAir. Second Law, Burlington, VT, Karen Walkerman.
-
-**NOTICE:** The U.S. Government is granted for itself and others acting on its behalf a paid-up, nonexclusive, irrevocable, worldwide license in this data to reproduce, prepare derivative works, and perform publicly and display publicly. Beginning five (5) years after permission to assert copyright is granted, subject to two possible five year renewals, the U.S. Government is granted for itself and others acting on its behalf a paid-up, non-exclusive, irrevocable worldwide license in this data to reproduce, prepare derivative works, distribute copies to the public, perform publicly and display publicly, and to permit others to do so.
-
-**TRADEMARKS:** EnergyPlus is a trademark of the US Department of Energy.
-
-Other Software included or referenced directly
-----------------------------------------------
-
-The following notices apply to those EnergyPlus distributions which include the interface to BCVTB or Functional Mock-up Units.
-
-### ZLIB DATA COMPRESSION LIBRARY
-
-zlib 1.2.5 is a general purpose data compression library.  All the code is thread safe.  The data format used by the zlib library is described by RFCs (Request for Comments) 1950 to 1952 in the files http://www.ietf.org/rfc/rfc1950.txt (zlib format), rfc1951.txt (deflate format) and rfc1952.txt (gzip format).
-
-All functions of the compression library are documented in the file zlib.h (volunteer to write man pages welcome, contact zlib@gzip.org).  A usage example of the library is given in the file example.c which also tests that the library is working correctly.  Another example is given in the file minigzip.c.  The compression library itself is composed of all source files except example.c and minigzip.c.
-
-To compile all files and run the test program, follow the instructions given at the top of Makefile.in.  In short "./configure; make test", and if that goes well, "make install" should work for most flavors of Unix.  For Windows, use one of the special makefiles in win32/ or contrib/vstudio/ .  For VMS, use make\_vms.com.  Questions about zlib should be sent to &lt;zlib@gzip.org&gt;, or to Gilles Vollant &lt;info@winimage.com&gt; for the Windows DLL version.  The zlib home page is http://zlib.net/ .  Before reporting a problem, please check this site to verify that you have the latest version of zlib; otherwise get the latest version and check whether the problem still exists or not.
-
-PLEASE read the zlib FAQ &gt;http://zlib.net/zlib_faq.html&lt; before asking for help.
-
-Mark Nelson &lt;markn@ieee.org&gt; wrote an article about zlib for the Jan.  1997 issue of Dr.  Dobb's Journal; a copy of the article is available at &lt;http://marknelson.us/1997/01/01/zlib-engine/&gt; .
-
-The changes made in version 1.2.5 are documented in the file ChangeLog.
-
-Unsupported third party contributions are provided in directory contrib/ .
-
-zlib is available in Java using the java.util.zip package, documented at &lt;http://java.sun.com/developer/technicalArticles/Programming/compression/&gt; .
-
-A Perl interface to zlib written by Paul Marquess &lt;pmqs@cpan.org&gt; is available at CPAN (Comprehensive Perl Archive Network) sites, including &lt;http://search.cpan.org/~pmqs/IO-Compress-Zlib/&gt; .
-
-A Python interface to zlib written by A.M. Kuchling &lt;amk@amk.ca&gt; is available in Python 1.5 and later versions, see &lt;http://www.python.org/doc/lib/module-zlib.html&gt;.
-
-zlib is built into tcl: &lt;http://wiki.tcl.tk/4610&gt; .
-
-An experimental package to read and write files in .zip format, written on top of zlib by Gilles Vollant &lt;info@winimage.com&gt;, is available in the contrib/minizip directory of zlib.
-
-Notes for some targets:
-
-- For Windows DLL versions, please see win32/DLL\_FAQ.txt
-
-- For 64-bit Irix, deflate.c must be compiled without any optimization. With -O, one libpng test fails. The test works in 32 bit mode (with the -n32   compiler flag). The compiler bug has been reported to SGI.
-
-- zlib doesn't work with gcc 2.6.3 on a DEC 3000/300LX under OSF/1 2.1 it works when compiled with cc.
-
-- On Digital Unix 4.0D (formely OSF/1) on AlphaServer, the cc option -std1 is necessary to get gzprintf working correctly. This is done by configure.
-
-- zlib doesn't work on HP-UX 9.05 with some versions of /bin/cc. It works with other compilers. Use "make test" to check your compiler.
-
-- gzdopen is not supported on RISCOS or BEOS.
-
-- For PalmOs, see &lt;http://palmzlib.sourceforge.net/&gt;
-
-Acknowledgments:
-
-  The deflate format used by zlib was defined by Phil Katz.  The deflate and zlib specifications were written by L.  Peter Deutsch.  Thanks to all the people who reported problems and suggested various improvements in zlib; they are too numerous to cite here.
-
-Copyright notice:
-
- (C) 1995-2010 Jean-loup Gailly and Mark Adler
-
-This software is provided 'as-is', without any express or implied warranty.  In no event will the authors be held liable for any damages arising from the use of this software.
-
-Permission is granted to anyone to use this software for any purpose, including commercial applications, and to alter it and redistribute it freely, subject to the following restrictions:
-
-1. The origin of this software must not be misrepresented; you must not claim that you wrote the original software. If you use this software in a product, an acknowledgment in the product documentation would be appreciated but is not required.
-
-2. Altered source versions must be plainly marked as such, and must not be misrepresented as being the original software.
-
-3. This notice may not be removed or altered from any source distribution.
-
-  Jean-loup Gailly        Mark Adler
-
-  jloup@gzip.org          madler@alumni.caltech.edu
-
- 
-
-If you use the zlib library in a product, we would appreciate \*not\* receiving lengthy legal documents to sign.  The sources are provided for free but without warranty of any kind.  The library has been entirely written by Jean-loup Gailly and Mark Adler; it does not include third-party code.
-
-If you redistribute modified sources, we would appreciate that you include in the file ChangeLog history information documenting your changes.  Please read the FAQ for more information on the distribution of modified source versions.
-
-### ExPat Copying Notice
-
-Copyright (c) 1998, 1999, 2000 Thai Open Source Software Center Ltd
-
-Permission is hereby granted, free of charge, to any person obtaining a copy of this software and associated documentation files (the "Software"), to deal in the Software without restriction, including without limitation the rights to use, copy, modify, merge, publish, distribute, sublicense, and/or sell copies of the Software, and to permit persons to whom the Software is furnished to do so, subject to the following conditions:
-
-The above copyright notice and this permission notice shall be included in all copies or substantial portions of the Software.
-
-THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY, FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT. IN NO EVENT SHALL THE AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING FROM, OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER DEALINGS IN THE SOFTWARE.
-
-### FMU SDK license
-
-Copyright (c) 2008-2011, QTronic GmbH. All rights reserved.
-
-The FmuSdk is licensed by the copyright holder under the BSD License (&lt;http://www.opensource.org/licenses/bsd-license.html&gt;): Redistribution and use in source and binary forms, with or without modification, are permitted provided that the following conditions are met:
-
-- Redistributions of source code must retain the above copyright notice, this list of conditions and the following disclaimer.
-
-- Redistributions in binary form must reproduce the above copyright notice, this list of conditions and the following disclaimer in the documentation and/or other materials provided with the distribution.
-
-THIS SOFTWARE IS PROVIDED BY QTRONIC GMBH "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL QTRONIC GMBH BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
-
-### Minizip Notice
-
-Condition of use and distribution are the same than zlib :
-
-This software is provided 'as-is', without any express or implied warranty.  In no event will the authors be held liable for any damages arising from the use of this software.
-
-Permission is granted to anyone to use this software for any purpose, including commercial applications, and to alter it and redistribute it freely, subject to the following restrictions:
-
-1. The origin of this software must not be misrepresented; you must not claim that you wrote the original software. If you use this software in a product, an acknowledgment in the product documentation would be appreciated but is not required.
-
-2. Altered source versions must be plainly marked as such, and must not be misrepresented as being the original software.
-
-3. This notice may not be removed or altered from any source distribution.
-
-### MODELISAR Notice
-
-Copyright (c) 2008-2010, MODELISAR consortium. All rights reserved.
-
-This file is licensed by the copyright holders under the BSD License (&lt;http://www.opensource.org/licenses/bsd-license.html&gt;):
-
-----------------------------------------------------------------------------
-
-Redistribution and use in source and binary forms, with or withoutmodification, are permitted provided that the following conditions are met:
-
-- Redistributions of source code must retain the above copyright notice, this list of conditions and the following disclaimer.
-
-- Redistributions in binary form must reproduce the above copyright notice, this list of conditions and the following disclaimer in the documentation and/or other materials provided with the distribution.
-
-- Neither the name of the copyright holders nor the names of its contributors may be used to endorse or promote products derived from this software without specific prior written permission.
-
-THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
-
-### Functional Mock-up Unit for Co-Simulation Import Notice
-
-Functional Mock-up Unit for Co-Simulation Import in EnergyPlus Copyright (c) 2012, The Regents of the University of California, through Lawrence Berkeley National Laboratory (subject to receipt of any required approvals from the U.S. Dept. of Energy). All rights reserved.
-
-If you have questions about your rights to use or distribute this software, please contact Berkeley Lab's Technology Transfer Department at &lt;TTD@lbl.gov&gt;.
-
-NOTICE.  This software was developed under partial funding from the U.S. Department of Energy.  As such, the U.S. Government has been granted for itself and others acting on its behalf a paid-up, nonexclusive, irrevocable, worldwide license in the Software to reproduce, prepare derivative works, and perform publicly and display publicly.  Beginning five (5) years after the date permission to assert copyright is obtained from the U.S. Department of Energy, and subject to any subsequent five (5) year renewals, the U.S. Government is granted for itself and others acting on its behalf a paid-up, nonexclusive, irrevocable, worldwide license in the Software to reproduce, prepare derivative works, distribute copies to the public, perform publicly and display publicly, and to permit others to do so.
-
-Modified BSD License agreement
-
-Functional Mock-up Unit for Co-Simulation Import in EnergyPlus Copyright (c) 2012, The Regents of the University of California, through Lawrence Berkeley National Laboratory (subject to receipt of any required approvals from the U.S. Dept. of Energy).  All rights reserved.
-
-Redistribution and use in source and binary forms, with or without modification, are permitted provided that the following conditions are met:
-
-Redistributions of source code must retain the above copyright notice, this list of conditions and the following disclaimer.
-
-Redistributions in binary form must reproduce the above copyright notice, this list of conditions and the following disclaimer in the documentation and/or other materials provided with the distribution.
-
-Neither the name of the University of California, Lawrence Berkeley National Laboratory, U.S. Dept. of Energy nor the names of its contributors may be used to endorse or promote products derived from this software without specific prior written permission.
-
-THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT OWNER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
-
-You are under no obligation whatsoever to provide any bug fixes, patches, or upgrades to the features, functionality or performance of the source code ("Enhancements") to anyone; however, if you choose to make your Enhancements available either publicly, or directly to Lawrence Berkeley National Laboratory, without imposing a separate written license agreement for such Enhancements, then you hereby grant the following license: a non-exclusive, royalty-free perpetual license to install, use, modify, prepare derivative works, incorporate into other computer software, distribute, and sublicense such enhancements or derivative works thereof, in binary and source code form.
-
-### Functional Mock-up Unit Export of EnergyPlus Notice
-
-Functional Mock-up Unit Export of EnergyPlus (c)2013, The Regents of the University of California, through Lawrence Berkeley National Laboratory (subject to receipt of any required approvals from the U.S. Department of Energy). All rights reserved.
-
-If you have questions about your rights to use or distribute this software, please contact Berkeley Lab's Technology Transfer Department at &lt;TTD@lbl.gov&gt;.referring to "Functional Mock-up Unit Export of EnergyPlus (LBNL Ref 2013-088)".
-
-NOTICE: This software was produced by The Regents of the University of California under Contract No. DE-AC02-05CH11231 with the Department of Energy.
-
-For 5 years from November 1, 2012, the Government is granted for itself and others acting on its behalf a nonexclusive, paid-up, irrevocable worldwide license in this data to reproduce, prepare derivative works, and perform publicly and display publicly, by or on behalf of the Government. There is provision for the possible extension of the term of this license.
-
-Subsequent to that period or any extension granted, the Government is granted for itself and others acting on its behalf a nonexclusive, paid-up, irrevocable worldwide license in this data to reproduce, prepare derivative works, distribute copies to the public, perform publicly and display publicly, and to permit others to do so. The specific term of the license can be identified by inquiry made to Lawrence Berkeley National Laboratory or DOE. Neither the United States nor the United States Department of Energy, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any data, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights.
-
-Copyright (c) 2013, The Regents of the University of California, Department of Energy contract-operators of the Lawrence Berkeley National Laboratory.
-
-All rights reserved.
-
-1. Redistribution and use in source and binary forms, with or without modification, are permitted provided that the following conditions are met:
-
-(1) Redistributions of source code must retain the copyright notice, this list of conditions and the following disclaimer.
-
-(2) Redistributions in binary form must reproduce the copyright notice, this list of conditions and the following disclaimer in the documentation and/or other materials provided with the distribution.
-
-(3) Neither the name of the University of California, Lawrence Berkeley National Laboratory, U.S. Dept. of Energy nor the names of its contributors may be used to endorse or promote products derived from this software without specific prior written permission.
-
-2. THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS"
-
-AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT OWNER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
-
-3. You are under no obligation whatsoever to provide any bug fixes, patches, or upgrades to the features, functionality or performance of the source code ("Enhancements") to anyone; however, if you choose to make your Enhancements available either publicly, or directly to Lawrence Berkeley National Laboratory, without imposing a separate written license agreement for such Enhancements, then you hereby grant the following license: a non-exclusive, royalty-free perpetual license to install, use, modify, prepare derivative works, incorporate into other computer software, distribute, and sublicense such enhancements or derivative works thereof, in binary and source code form.
-
-NOTE: This license corresponds to the "revised BSD" or "3-clause BSD"
-
-License and includes the following modification: Paragraph 3. has been added.
-
-Other Acknowledgments
----------------------
-
-This work was supported by the Assistant Secretary for Energy Efficiency and Renewable Energy, Office of Building Technologies of the US Department of Energy – under the guidance of Dru Crawley from inception through March 2010.
-
-Additional support was provided by the Gas Technology Institute and the California Energy Commission.
-
-The ice thermal storage module development was supported by the U.S. Department of Energy Office of Electricity Delivery and Energy Reliability.
-
-The HAMT (Heat And Moisture Transfer) model was supported by the Engineering and Physical Sciences Research Council (EPSRC), the UK government agency for funding research and training in engineering and the physical sciences.
-
-The SQLite output module was funded by Building Synergies, LLC and was made possible by inclusion of software code from the SQLite project (&lt;http://www.sqlite.org/&gt;).
-
- 
-
-
diff --git a/doc/src/docs/AuxiliaryPrograms/AuxiliaryPrograms.md b/doc/src/docs/AuxiliaryPrograms/AuxiliaryPrograms.md
deleted file mode 100644
index 5975ea0dc09..00000000000
--- a/doc/src/docs/AuxiliaryPrograms/AuxiliaryPrograms.md
+++ /dev/null
@@ -1,11482 +0,0 @@
-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Auxiliary EnergyPlus Programs</h1>
-<h2>Extra programs for EnergyPlus</h2>
-<br/>
-<p><i>(Extra! Extra! Read all about it!)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-Auxiliary Programs Introduction
-===============================
-
-This document will describe several of the "auxiliary programs" of the EnergyPlus system in more detail. Some of these programs are only available or only distributed for certain platforms. Typically, the programs are available on the Windows platform. Within the descriptions, other platforms will be noted as applicable. These programs include:
-
-**Weather Converter Program** (aka "Weather")
-
-**Ground Heat Transfer in EnergyPlus** - Procedure for Ground Temperature creation
-
-**View Factor Calculation Program** - Auxiliary program used to calculate View Factors which can be used with EnergyPlus
-
-**Using Older Version Input Files - Transition** - to convert input files from one version to another upon release of a new version
-
-**EPDraw** - Create DXF files from your input files
-
-**Input Macros** - Use a macro language to increase efficiency in creating EnergyPlus input files.  Unfortunately, IDF files containing macros cannot be read in the IDF Editor.
-
-**HVAC Diagram** - Use a post processing program to diagram your HVAC inputs.
-
-**CoeffConv/CoeffCheck** - Convert DOE-2 temperature dependent curves (Fahrenheit) to EnergyPlus temperature curves (Centigrade/Celsius)
-
-**ExpandObjects** - Some technical details of the Expand Objects program which preprocessed HVACTemplate:\* and GroundHeatTransfer:\* objects for use inside EnergyPlus.
-
-**CSVproc** - Get simple statistics from CSV output files.
-
-**convertESOMTR** - convert your outputs to Inch-Pound (default) or other custom unit conversions.
-
-**CalcSoilSurfTemp Program** - calculate soil surface parameters used in the Earth Tube simulation
-
-**HVAC Performance Curve Fit Tool**- generates HVAC performance curves in EnergyPlus IDF format
-
-**Parametric Spreadsheets** - Parametric spreadsheets are available to help illustrate or calculate some parameters/coefficients.
-
-**ParametricPreprocessor** **-** Special objects can be inserted in IDF files and generate a series of IDF files from a single source IDF file that contains parametric objects and expressions. Unlike using the macro language, these input files are capable of being read in the IDF Editor.
-
-**AppGPostProcess - Appendix G PostProcessing program** - The ASHRAE 90.1 Appendix G postprocessing program takes simulation outputs and processes them to help meet Appendix G requirements..
-
-**BLASTTranslator** - The BLAST translator can take BLAST (Building Loads Analysis and System Thermodynamics) input files and make them ready for running in EnergyPlus.
-
-**DOE2Translator** - The DOE-2 translator can take DOE-2 program input files and make them ready for running in EnergyPlus.
-
-**Running Console Applications** - this section describes how to run console applications that are part of EnergyPlus and how you might modify these to your specific needs. Instructions for running individual programs are included in their descriptions.
-
-**Technical Details of Running EnergyPlus** - this section gives full instructions on both EP-Launch and the IDF-Editor as well as some more details on running EnergyPlus manually.
-
-**EP-Compare** - A utility to graphically compare tabular results from multiple simulation files.
-
-Weather Converter Program
-=========================
-
-The Weather Converter program is stored in the EnergyPlus folder area under "PreProcess" and subsequently in the "WeatherConverter" folder.
-
-To perform annual/run period simulations in EnergyPlus, one needs weather data. Most weather data is still issued in an hour by hour (hourly) format though as you will see, EnergyPlus and its weather converter can accept data that has a finer resolution on the data (such as every 10 or 15 minutes).
-
-The special weather format (EPW) used in EnergyPlus is a simple, ascii format as is common in the rest of the inputs for EnergyPlus.
-
-Background
-----------
-
-All building simulation programs employ some means of representing local climatic conditions relative to the building models. For example, Radiance (Ward 1996) needs a description of sky conditions and illuminance values to calculate solar distribution through a window and within a space. Three of the widely used energy simulation programs in the UK and US, ESP-r (ESRU 1999), BLAST (UI 1998), and DOE-2 (Winkelmann et al. 1993) also use weather conditions to simulate the response of a building. But even after 30 years of significant development advances in simulation capabilities, these programs use the same climate representations as in the past-a simple set of hourly temperature, humidity, wind speed and direction, and atmospheric pressure and solar radiation or cloud cover data. These data are often 'typical' data derived from hourly observations at a specific location by the national weather service or meteorological office. Examples of these typical data include TMY2 (NREL 1995) and WYEC2 (ASHRAE 1997) in the United States and Canada and TRY (CEC 1985) in Europe. The TMY2 and WYEC2 typical weather years contain more solar radiation and illumination data than older formats such as TMY (NCDC 1983), WYEC (ASHRAE 1985), and TRY (NCDC 1981) in the U.S. Crawley (1998) demonstrated that the methods used to select data for the US TMY2 and European TRY data sets better fits the long-term climate patterns.
-
-Radiation and illumination data are becoming increasingly necessary in simulation programs. Anyone who has ever attempted to measure daylight factors will be familiar with the fluctuations in lighting levels under partly cloudy conditions. The expansion and contraction of lightweight building components also shares sensitivity to rapid fluctuations in solar radiation. Single-sided ventilation is dependant on wind pressure fluctuations and pedestrians in many cities are acquainted with the disarming tendency of the wind to guest and change direction. It is increasingly the case that design questions touch on such issues.
-
-In a research context, the advent of tools such as LabVIEW (National Instruments Corporation 1999) have made it possible for increasing numbers of researchers to acquire and process test-cell data. The increasing use of building energy management systems (BEMS) has also provided high frequency information from which simulation could be used as a predictive tool for future control strategies. Other issues of control, particularly of advanced daylighting control require sub-hourly illumination data to ensure that possible control regimes are tested under realistic conditions. Janak (1997) observed that the differences between 5 minute and hourly illumination data could result in prediction variations approaching 40%.
-
-Thus far, projects that mix empirical and simulation-based work have had to store and access such data via temporal database facilities (ESRU 1999). As the number of high quality datasets increases so does the need to encapsulate such information in a form that can be broadly distributed. The simulation community must also consider the uncertainty in high frequency performance predictions that are based on boundary conditions that have been sampled at one or two magnitudes less temporal resolution.
-
-The simulation community must also consider practitioner demands and issues of quality assurance. Someone who is not a native of Copenhagen may not know that there are three or four recognizable patterns of winter weather that should be included in detailed assessments. A data set that lacks documentation or is dependent on separately held lists of assumptions can be effectively useless.
-
-In the absence of data within the weather data format, the simulation programs must calculate these data often with older calculation methods. As the simulation programs have become more capable, data at hourly resolution is no longer enough-interpolating between hourly observations does not accurately represent weather conditions that change much more frequently such as illumination.
-
-We have developed a generalized weather data format for use by energy simulation programs has been developed and adopted by both ESP-r (in the UK) and EnergyPlus (in the US). Anticipating the need for data at time steps less than one hour, the format includes a minute field to facilitate the use of sub hourly data. The data include basic location identifiers such as location name, data source, latitude, longitude, time zone, elevation, peak design conditions, holidays, daylight saving period, typical and extreme periods, ground temperatures, period(s) covered by the data and space for descriptive comments. The time step data include dry bulb and dew point temperature, relative humidity, station pressure, solar radiation (global, extraterrestrial, horizontal infrared, direct, and diffuse), illuminance, wind direction and speed, sky cover, and current weather.
-
-Weather Format for Simulation Programs
---------------------------------------
-
-For these reasons, we developed a generalized weather data format for use with two major simulation programs-ESP-r and EnergyPlus (Crawley et al. 1999). All the data are in SI units. The format is simple, text-based with comma-separated data. It is based on the data available within the TMY2 weather format but has been rearranged to facilitate visual inspection of the data. The TMY2 data are a strict, position-specific format-filling missing data with nines and zero values with zeroes. The new weather data format contains commas to facilitate data reading and analysis with spreadsheet programs. By eliminating redundant 'fill' values, the size of each file is only slightly larger than the original TMY2 format. Details about the TMY2 format can be found in the TMY2 User's manual (see references at the end of this section).
-
-The traditional distribution of data source and uncertainty flags within the raw data fields carries with it not only the need for many field separators, it obfuscates the relationships between non-numerical data. In a set of minute data, which could easily require hundreds of thousands of records, the space penalty is considerable. In the E/E file format, all data source and uncertainty fields have been clumped together as a single field immediately following the day and time stamp. For applications where uncertainty is not an issue such data can be easily ignored. When it is important, a single text field is conceptually and computationally easy to parse.
-
-Another difference between the EnergyPlus/ESP-r (E/E) format and TMY2 is the addition of two new data fields-minute and infrared sky. The minute field facilitates use of data observed at intervals of less than one hour such as measured data from a research study of energy efficiency for a particular building. This will allow easier and more accurate calibration of a simulation model to measured data than possible in the past. The infrared sky field allows the programs to calculate the effective sky temperature for re-radiation during nighttime.
-
-The last difference is that a full year of data (such as 8760 hours) is not required-subsets of years are acceptable. Which periods are covered by the data is described in the files.  Periods of typical weather patterns based on analysis of the data are also included within the format. A side-by-side comparison of data included in the E/E weather format with data previously used by ESP-r, DOE-2, and BLAST is shown in Table 1.  A deficiency noted within ESP-r for example is the lack of correcting air volumes for elevation change-many of the users of ESP-r are in relatively low elevations. For DOE-2 and BLAST, neither program used illumination data in daylighting calculations or infrared sky temperatures-it was always recalculated at time of use.
-
-By including the uncertainty and data source information found in TMY2, users now can evaluate the potential impact of weather variability on the performance of the building.
-
-McDonald and Strachan (1998) are introducing uncertainty analysis into ESP-r.
-
-We use the EnergyPlus data dictionary format to describe the E/E weather data set. (See the end of this document). Each line in the format is preceded by a keyword such as LOCATION, DESIGN CONDITIONS, followed by a list of variables beginning either with A or N and a number. A stands for alphanumeric; N for numeric. The number following A/N is the sequence of that number in the keyword list. Commas separate data. (Refer to the IDD Conventions document in "[Input Output Reference](InputOutputReference.pdf)" for further explanation of the format). The header information consists of eight lines (keywords):  LOCATION, DESIGN CONDITIONS, TYPICAL/EXTREME PERIODS, GROUND TEMPERATURES, HOLIDAYS/DAYLIGHT SAVINGS, COMMENTS 1, COMMENTS 2, and DATA PERIODS. This is followed by the time step data.
-
-The first eight lines or header within each E/E weather file define basic location information such as longitude, latitude, time zone, elevation, annual design conditions, monthly average ground temperatures, typical and extreme periods, holidays/daylight saving periods, and data periods included. There is also space for users to document any special features or information about the file such as sources of data.
-
-Weather Data Availability
--------------------------
-
-Typically, acquisition of weather data has been a user's burden. Though this will remain the case in many instances for EnergyPlus users, the EnergyPlus team has been successful in making a wealth of US, Canadian and International data available to our users. To summarize, the weather data for 2092 locations is available at the EnergyPlus web site: [www.energyplus.gov](http://www.energyplus.gov)
-
-The details are shown in Table 18. Summary of Downloadable Weather Data by Type.   This data has been selected with the energy simulation user in mind. All the data (as well as the statistical reports - described later in this document) are downloadable for individual locations.
-
-Table 1. Comparison of E/E with ESP-r/DOE-2/BLAST Weather Data Formats
-
-<table class="table table-striped">
-  <tr>
-    <th>Data Element</th>
-    <th>DOE-2</th>
-    <th>BLAST</th>
-    <th>ESP-r</th>
-    <th>E/E</th>
-  </tr>
-  <tr>
-    <td>Location (name, latitude, longitude, elevation, time zone)</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Data source</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Commentary</td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Design conditions</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Typical/extreme periods</td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Data periods</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Holiday/Daylight Saving</td>
-    <td></td>
-    <td>X</td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Solar Angles/Equation of Time Hours</td>
-    <td></td>
-    <td>X</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Degree Days</td>
-    <td></td>
-    <td>X</td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Year</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Month</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Day</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Hour</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Minute</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Data source and uncertainty flags</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Dry bulb temperature</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Wet bulb temperature</td>
-    <td>X</td>
-    <td>X</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Dew point temperature</td>
-    <td>X</td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Atmospheric station pressure</td>
-    <td>X</td>
-    <td>X</td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Humidity ratio</td>
-    <td>X</td>
-    <td>X</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Relative humidity</td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Enthalpy</td>
-    <td>X</td>
-    <td></td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Density</td>
-    <td>X</td>
-    <td></td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Wind Speed</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Wind Direction</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Infrared Sky Temperature</td>
-    <td></td>
-    <td>X</td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Solar Radiation (global, normal, diffuse)</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Illuminance (global, normal, diffuse)</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Sky cover (cloud amount)</td>
-    <td>X</td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Opaque sky cover</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Visibility</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Ceiling height</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Clearness (monthly)</td>
-    <td>X</td>
-    <td></td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>"Undisturbed" Ground temperatures (monthly)</td>
-    <td>X</td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Present weather observation and codes (rain, snow)</td>
-    <td></td>
-    <td>X</td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Precipitable water</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Aerosol optical depth</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Snow depth</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Days since last snowfall</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Albedo</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Liquid Precipitation Depth</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Liquid Precipitation Quantity</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>X</td>
-  </tr>
-</table>
-
-Using the Weather Converter
----------------------------
-
-We developed a utility for the E/E format to read standard weather service file types such as SAMSON and newer 'typical year' weather files such as TMY2, WYEC2, and IWEC. The utility also reads ESP-r (CLM format), DOE-2 (fmt format), BLAST (Ascii format) files and other files.
-
-The utility translates and extends typical weather data into the E/E format. The processor makes the calculations necessary for supplying data (when data is missing) and calculates the Horizontal Infrared Radiation Intensity values-not typically currently an observed value reported by the meteorological offices through the world. The utility also prepares an statistical summary of the weather data set as part of the processing. An additional "output format" from the utility is a comma-delimited file that can easily be imported into a spreadsheet program such as Excelâ„¢ for further user perusal, charting and/or editing.
-
-The utility consists of two parts: a user interface that executes on standard Wintel systems and a DLL that does the work of the processing. The DLL interface is described in a later section for those developers who might wish to access it directly.
-
-The user front end is a simple to use program with standard graphical user interface menus. It is executed from the Start Menu programs using the specific folder where the EnergyPlus program was installed. (e.g., Start Menu -&gt; EnergyPlus &lt;version&gt; -&gt; WeatherConverter). For convenience, it automatically opens with the "convert" option.
-
-EP-Launch can also be used to run the weather utility program.  Weather is one of the options on the Utilities tab in EP-Launch. See the section on EP-Launch in this document for more information on how to use EP-Launch with the weather utility program.
-
-![](media/image001.jpg)
-
-Figure 1. Main menu screen of the Weather Converter Utility
-
-
-
-### File Menu
-
-The file menu has four options:
-
-#### Fix Out of Range Data
-
-This is a toggle option that once selected is saved in the registry with other options (for example, screen size) for the program. As shown in the IDD type description of the Weather Data, there are minimum and maximum values for several of the fields. The weather converter program can ignore these (and just report them) or it can try to fix them with appropriate values. If the option is "checked", then the processor will try to fix the data; if it is blank, the processor will not fix the data though it will report any out of range data that it finds.
-
-#### Select Delta DB Trigger
-
-Depending on the quality control and accuracy of the weather data collection, time period (usually hour to hour) changes in some data values may make the data suspect for that time period. This selection brings up the screen shown below and will allow the user some control over the actual value reporting. Note that this data is not "fixed", merely reported by the program in the audit output file.
-
-![](media/image002.jpg)
-
-Figure 2. Delta DB Trigger Selection
-
-Though only one "trigger" value is selected from this screen, consecutive values of dry-bulb temperature, dew-point temperature and wind speed are reported using appropriate calculated values. Both dew-point and wind speed use a calculated value based on mean of their values over the entire data period and standard deviation from that mean, heuristically derived.
-
-An excerpt from the audit file is illustrative:
-
-Average Delta DB Change=  0.78°C ; Std Dev=  0.83°C
-
- Average Delta DP Change=  0.68°C ; Std Dev=  0.78°C
-
- Average Delta Relative Humidity Change=  4.02% ; Std Dev=  4.22%
-
- Average Delta Wind Speed Change=  0.91m/s ; Std Dev=  0.88m/s
-
- Hourly Dry Bulb temperature change trigger = minimum of  12.13°C  and  10.°C
-
-     12.13°C = calculated trigger based on mean change in dry-bulb temperature and standard deviation shown above
-
-     10.°C = trigger set by user
-
-Here the calculated DB trigger would be 12.13°C, but the user chosen trigger is 10°C. Changes &gt;= 10°C will be reported.
-
-- Delta DB/DP Range Triggered for Apr 30
-
-- Change in DB= 11.60°C, Hour=14
-
-Such detail allows the user to hand edit the incoming data, if desired.
-
-#### Delete File
-
-You may use this menu option to browse your computer and delete files.
-
-#### Input Folder =&gt; Output Folder
-
-Choosing this option (a check will show and will carry over from one use to the next) sets the output folder for saving files to be the same as the input folder where the original files are located.
-
-#### Exit
-
-This choice exits the program.
-
-### Converting Data
-
-This screen is automatically shown when you start the program - it will allow you to select raw data for processing, change the default type (based on file extension), select the kind of conversion you want, select where and what name to store for the processed data, and process the data. An "almost" completed screen shows:
-
-![](media/image003.jpg)
-
-Figure 3. Convert Data Screen selections
-
-
-
-The screen is navigated by choosing the following buttons on the left portion of the screen. Interpretation from the program is shown in the status boxes on the right portion of the screen.
-
-#### Select File to Convert
-
-Selecting this command button brings up a common dialog interface that allows you to select a file for conversion from a specific set of default file extensions. These are shown in the following table. Note that you can (mostly) override the default file extension by the use of a simple DEF file and change the input file type.
-
-Table 2. Input File Extensions with implied Data types
-
-<table class="table table-striped">
-  <tr>
-    <th>File Extension</th>
-    <th>Implicit Data File Type</th>
-  </tr>
-  <tr>
-    <td>LST</td>
-    <td>Processing List of Files</td>
-  </tr>
-  <tr>
-    <td>&lt;any&gt; or CST</td>
-    <td>Custom - must have "def" file as specified below</td>
-  </tr>
-  <tr>
-    <td>EPW</td>
-    <td>EnergyPlus E/E</td>
-  </tr>
-  <tr>
-    <td>CSV</td>
-    <td>Comma Delimited File (EPW Format) Note: special EnergyPlus CSV format. For other CSV files use the DEF file and describe the format.</td>
-  </tr>
-  <tr>
-    <td>TM2</td>
-    <td>TMY2</td>
-  </tr>
-  <tr>
-    <td>TMY</td>
-    <td>TMY</td>
-  </tr>
-  <tr>
-    <td>IWC</td>
-    <td>IWEC</td>
-  </tr>
-  <tr>
-    <td>WY2</td>
-    <td>WYEC2</td>
-  </tr>
-  <tr>
-    <td>DAT</td>
-    <td>SAMSON</td>
-  </tr>
-  <tr>
-    <td>FMT</td>
-    <td>DOE-2 Formatted File</td>
-  </tr>
-  <tr>
-    <td>CLM</td>
-    <td>ESP-r Climate Formatted File</td>
-  </tr>
-  <tr>
-    <td>ASC</td>
-    <td>BLAST ASCII</td>
-  </tr>
-  <tr>
-    <td>SWE</td>
-    <td>SWERA</td>
-  </tr>
-  <tr>
-    <td>WEA</td>
-    <td>Ecotect WEA file</td>
-  </tr>
-</table>
-
-Of course, the "all files" (\*.\*) may be used as well. If the file selected is not one of the above types, you will be cautioned to use the "override default type" button to select the correct type before proceeding. Most of the data file types are described in other publications and won't be described in detail here.
-
-Note on the input CSV format:  It is the EPW CSV format. The CSV format must mirror the output CSV format very closely. The processor expects a Location header record and the headers for the data fields as a minimum (as well as the data that supports those header fields). If you have a differently formatted file, possible comma delimited, investigate the "custom" format option.
-
-The LST data type allows you to specify a list of files to be "batch processed". The format of this file is very simple (however, the default extensions from the preceding table **must** be used **or** you must include a "def" file - see below for details).
-
-Each line of the LST file can have a columnar structure as shown in the following table or can have the input file separated from the output file with a TAB character.
-
-
-
-Table 3. LST File Structure
-
-<table class="table table-striped">
-<tr>
-<th>Columns</th>
-<th>Contents</th>
-</tr>
-<tr>
-<td>1-45</td>
-<td>Name of Input File to be Processed</td>
-</tr>
-<tr>
-<td>46-105 (or follow the first name with a {TAB})</td>
-<td>Output File with:
-EPW - same as output type "EPW"
-CSV - same as output type "CSV"
-Both - same as output type "both"
-Rpt - same as output type "rpt"</td>
-</tr>
-<tr>
-<td>106-end (or follow the second name with a {TAB})</td>
-<td>URL for KML output</td>
-</tr>
-</table>
-
-#### Definitions File
-
-An auxiliary file, the Definitions File (extension .def) can be used to specify additional or replacement characteristics for the incoming data. This file is fully described in the section "Definitions File & Custom File Processing" later in this document.
-
-#### Override Default Type
-
-This button is used as described above to select the correct data type for a file that might have one of the standard "default" extensions but may, in fact, be a data file of an entirely different type. For example, the BLAST ASCII files as they exist on the BLAST CD have extensions of .dat - our default type for the SAMSON data. You must select the proper data type for your data or the processor probably won't work anywhere near what you expect.
-
-#### Select Output Format
-
-You may select from four options of output format:
-
-- EPW Format  -- both an epw file and a statistical report file are produced
-
-- CSV Format - both a csv file and a statistical report file are produced
-
-- Both EPW and CSV - epw, csv, and statistical report files are produced
-
-- Rpt only - only a statistical report file is produced (output extension is "stat")
-
-Note that the CSV file is very similar to the EPW format file but is ready to be imported into a spreadsheet program such as Excelâ„¢ and has some additional "header" records in front of each EPW style header record
-
-#### Save File As…
-
-This button allows you to select the location to save your file set from the output format selection. The utility automatically places a "data type" extension on the file name to show its original data file type.
-
-Note on Save As…  Since you select the "save as" file name from a dialog, the processor DOES NOT warn you of overwriting previous files of the same name. In addition, if you have previously saved several types (e.g. EPW and CSV) but this time only save the RPT - it DOES NOT create new of the others nor does it delete the previous ones.
-
-#### Convert File
-
-Pressing this button causes the processing of the data to proceed. If you choose a ".lst" input format, you will see messages as each once is completed and/or has errors. If you choose a single data file, you will see a similar message box once the processing is done (or has terminated due to errors).
-
-### Help
-
-No online help is available. This brings up an "about" box for the program.
-
-Definitions File & Custom File Processing
------------------------------------------
-
-### Description of "Def" input file
-
-Some of the data formats have inherent omissions (e.g. TMY does not have location data, BLAST ASCII does not have elevations). In order to overcome this limitation and to provide further flexibility, a definitions file (extension must be .def) is implemented. By naming this with the same "file name" as your input file (in the same folder), the weather converter will read the format and use that data, as appropriate, in the file conversions. The .def file uses Fortran "Namelist" input fields as shown in the example below. For flexibility, you can also define a "presets.def" file (such as when you have a list of files to process and the format or some portion is all the same between the group of files. The two def files (one named the same as the file name for the raw data and one named presets.def) will both be processed. Conflicts between the two will be shown in the .audit file. The set of namelist groups is:
-
-- &location - Location data
-
-- &miscdata - Comments to be applied to "COMMENT2" in the EPW file and "Source Data"
-
-- &wthdata -  weather data specifications including file type, custom formats
-
-- &datacontrol - user specified control over "missing" data (Custom format only)
-
-**Note that the "Def" formats are entirely different from the usual IDF formats of EnergyPlus.  No commas separate fields.  No semicolon terminates the entry.**
-
-    &location
-    City='Hong Kong'
-    StateProv=' '
-    Country='CHN'
-    InLat=22.75
-    InLong=115
-    InTime=8
-    InElev=0
-    InWMO=450040
-    /
-    
-    &miscdata
-    Comments1='This file was given to us by....'
-    SourceData='Original xyz data'
-    /
-
-The "slash" (/) character terminating each block is very important - omissions results in incorrect reading of data.
-
-Definitions File Details are shown in the following table. You may leave out a field if you wish - the program will use whatever default is applicable (or usable) from the data format. All data formats accept this additional file. Only Custom format currently uses the &datacontrol element. And only Custom format input type uses the Data Elements, Format and Conversion factors from the &wthdata element.
-
-Note that strings in the "def" should be enclosed in single quotes if there is more than one word in the string - if only one word, quotes do not need to be used.
-
-Table 4. Definitions File &location description
-
-<table class="table table-striped">
-<tr>
-<th>&amp;location Field Description</th>
-<th>Field Name</th>
-<th>Type</th>
-</tr>
-<tr>
-<td>Name of City</td>
-<td>City</td>
-<td>String</td>
-</tr>
-<tr>
-<td>State or Province</td>
-<td>StateProv</td>
-<td>String</td>
-</tr>
-<tr>
-<td>Country Code</td>
-<td>Country</td>
-<td>String (3 characters)</td>
-</tr>
-<tr>
-<td>Latitude (N+/S-)</td>
-<td>InLat</td>
-<td>Numeric</td>
-</tr>
-<tr>
-<td>Longitude (W-/E+)</td>
-<td>InLong</td>
-<td>Numeric</td>
-</tr>
-<tr>
-<td>Time Zone (GMT +/-)</td>
-<td>InTime</td>
-<td>Numeric</td>
-</tr>
-<tr>
-<td>Elevation (meters)</td>
-<td>InElev</td>
-<td>Numeric</td>
-</tr>
-<tr>
-<td>WMO #</td>
-<td>InWMO</td>
-<td>Numeric or String (6 characters)</td>
-</tr>
-</table>
-
-### Expected Formats for &location
-
-#### Fields: City, StateProv, Country
-
-These fields are string variables. If Country is *not* included, an attempt to use the State/Prov entry may be used to determine country. Otherwise, these fields are not validated and are used to create part of the "location" header record in the EPW file. City can be up to 30 characters in length; StateProv up to 15 characters; Country up to 10 characters (standard 3 character abbreviation preferred).
-
-#### Fields: InLat, InLong
-
-These fields are decimal equivalent for Latitude and Longitude. The convention is North Latitude is positive; South is negative. Likewise, East Longitude is positive; West Longitude is negative. That is, if your latitude is N 30° 15' (North 30 degrees, 15 minutes) then your input is +30.25.
-
-#### Field: InTime
-
-This field is the decimal equivalent for the Time Zone value. The convention is GMT +/-. That is, if your time zone is "behind" GMT time by 6 hours, your input would be -6.
-
-#### Field: InElev
-
-This field is the location elevation in meters. Range can be from -300 to 6096. (These are the values from EnergyPlus - there is no validation of these in the weather converter.)
-
-#### Field: InWMO
-
-This field is the WMO (World Meterological Organization) number for the location. Though not validated per se, if found in the "design conditions" auxiliary files, the Design Day information can be generated.
-
-Table 5. Definitions File - &miscdata description
-
-<table class="table table-striped">
-<tr>
-<th>&amp;mischata Field Description</th>
-<th>Field Name</th>
-<th>Type</th>
-</tr>
-<tr>
-<td>String for Comments 1 header</td>
-<td>Comments1</td>
-<td>String</td>
-</tr>
-<tr>
-<td>String for Comments 2 header</td>
-<td>Comments2</td>
-<td>String</td>
-</tr>
-<tr>
-<td>String for Source Data in Location header</td>
-<td>SourceData</td>
-<td>String</td>
-</tr>
-<tr>
-<td>URL for output</td>
-<td>OutputURL</td>
-<td>String</td>
-</tr>
-</table>
-
-### Expected Formats for &miscdata
-
-#### Fields: Comments1, Comments2
-
-These are strings. After concatenation, they become part of the comment header lines in the EPW headers. Up to 150 characters each is allowed.
-
-#### Field: SourceData
-
-This string is applied to the "Source Data" field in the Location Header. Up to 60 characters is allowed.
-
-#### Field: OutputURL
-
-When a list of files is being processed, one of the outputs that results from the processing is a KML (Keyhole Markup Language) file that can be used with Google Earth to pinpoint the locations of the weather site. This field can be used to set this URL for later output. The list file format also includes a URL as its third (optional) parameter. If included, this input would overwrite other URL designations.
-
-Table 6. Definitions file - &wthdata description
-
-<table class="table table-striped">
-  <tr>
-    <th>&amp;wthdata Field Description</th>
-    <th>Field Name</th>
-    <th>Type</th>
-  </tr>
-  <tr>
-    <td>Input File Type</td>
-    <td>InputFileType</td>
-    <td>String</td>
-  </tr>
-  <tr>
-    <td>Number of records per hour</td>
-    <td>NumInHour</td>
-    <td>Integer</td>
-  </tr>
-  <tr>
-    <td>Data Element Names</td>
-    <td>DataElements</td>
-    <td>Strings</td>
-  </tr>
-  <tr>
-    <td>Data Units</td>
-    <td>DataUnits</td>
-    <td>Strings</td>
-  </tr>
-  <tr>
-    <td>Multiplicative Conversion Factors for Data</td>
-    <td>DataConversionFactors</td>
-    <td>Numeric</td>
-  </tr>
-  <tr>
-    <td>Special Missing Values</td>
-    <td>DataMissingValues</td>
-    <td>Numeric</td>
-  </tr>
-  <tr>
-    <td>Format for input</td>
-    <td>InFormat</td>
-    <td>Format String or "delimited"</td>
-  </tr>
-  <tr>
-    <td>Delimiter Character</td>
-    <td>DelimiterChar</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Decimal Delimiter Character</td>
-    <td>DecimalSymbolChar</td>
-    <td>String</td>
-  </tr>
-  <tr>
-    <td>Date Separator</td>
-    <td>DateSeparator</td>
-    <td>String (single character)</td>
-  </tr>
-</table>
-
-### Expected Formats for &wthdata
-
-#### Field: InputFileType
-
-You can always use this field and def file to "override" the default input format type that depends on the extension of your file (see Table 2. Input File Extensions with implied Data types). A complete set of valid values for Input File types is shown in the following table. Data Files are described more fully in the section Source Weather Data Formats that occurs later in this document.
-
-Table 7. Input File Type Values
-
-<table class="table table-striped">
-<tr>
-<th>Value</th>
-<th>File Type Description</th>
-</tr>
-<tr>
-<td>Tmy or ,tm2</td>
-<td>TMY2 Data File</td>
-</tr>
-<tr>
-<td>Iwec or iwc</td>
-<td>IWEC Data File</td>
-</tr>
-<tr>
-<td>Samson or dat</td>
-<td>SAMSON Data File</td>
-</tr>
-<tr>
-<td>wyec2 or wy2</td>
-<td>WYEC2 Data File</td>
-</tr>
-<tr>
-<td>Fmt or txt</td>
-<td>DOE-2 FMT File</td>
-</tr>
-<tr>
-<td>Clm or esp-r</td>
-<td>ESP-r Formatted (CLM) data file</td>
-</tr>
-<tr>
-<td>Blast or asc</td>
-<td>BLAST ASCII Data File</td>
-</tr>
-<tr>
-<td>Tmy</td>
-<td>TMY Data File</td>
-</tr>
-<tr>
-<td>Epw</td>
-<td>EPW Data File</td>
-</tr>
-<tr>
-<td>Csv</td>
-<td>EPW - CSV Data File</td>
-</tr>
-<tr>
-<td>Wea</td>
-<td>Ecotect wea Data File</td>
-</tr>
-<tr>
-<td>Swera or swe</td>
-<td>SWERA Data File</td>
-</tr>
-<tr>
-<td>Custom or User</td>
-<td>Custom Data File</td>
-</tr>
-</table>
-
-#### Field: NumInHour
-
-This field can be used to specify multi-interval (per hour) files. Without this field, the only formats that can have multiple intervals per hour are the EPW and CSV file formats - using the header record DataPeriods value for that field.
-
-#### Fields below only used in "Custom" format processing
-
-#### Field: DataElements
-
-For custom files, you will need to indicate which data elements are in which positions of the raw data file. The fields must come from a standardized list of names see following tables that include internal names (short and long - as shown in Table 8) as well as the EnergyPlus CSV format names (short and long - shown in Table 9) plus some further elements that can be specified when the standard data elements are not part of the raw data (as shown in Table 10). "Ignore" is used to skip a raw data field that is not applicable to the weather converter formats. Note that variables listed in the following table (in italics) are allowed for flexibility - i.e. wetbulb temperature can be used to determine relative humidity and/or dewpoint temperature. The following three tables illustrate the names for data elements.
-
-Table 8. Internal Data Element Names (directly applicable to EPW)
-
-<table class="table table-striped">
-  <tr>
-    <th>Short Name</th>
-    <th>Long Name</th>
-    <th>Default EPW Units</th>
-    <th>Used by EnergyPlus</th>
-  </tr>
-  <tr>
-    <td>year</td>
-    <td>Year</td>
-    <td>-</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>month</td>
-    <td>Month</td>
-    <td>-</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>day</td>
-    <td>Day</td>
-    <td>-</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>hour</td>
-    <td>hour</td>
-    <td>-</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>minute</td>
-    <td>minute</td>
-    <td>-</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>datasource</td>
-    <td>datasource</td>
-    <td>-</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>drybulb</td>
-    <td>dry_bulb_temperature</td>
-    <td>C</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>dewpoint</td>
-    <td>dew_point_temperature</td>
-    <td>C</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>relhum</td>
-    <td>relative_humidity</td>
-    <td>%</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>atmos_pressure</td>
-    <td>atmospheric_pressure</td>
-    <td>Pa</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>exthorrad</td>
-    <td>extraterrestrial_horizontal_radiation</td>
-    <td>Wh/m2</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>extdirrad</td>
-    <td>extraterrestrial_direct_normal_radiation</td>
-    <td>Wh/m2</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>horirsky</td>
-    <td>horizontal_infrared_radiation_intensity_from_sky</td>
-    <td>Wh/m2</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>glohorrad</td>
-    <td>global_horizontal_radiation</td>
-    <td>Wh/m2</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>dirnorrad</td>
-    <td>direct_normal_radiation</td>
-    <td>Wh/m2</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>difhorrad</td>
-    <td>diffuse_horizontal_radiation</td>
-    <td>Wh/m2</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>glohorillum</td>
-    <td>global_horizontal_illuminance</td>
-    <td>lux</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>dirnorillum</td>
-    <td>direct_normal_illuminance</td>
-    <td>lux</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>difhorillum</td>
-    <td>diffuse_horizontal_illuminance</td>
-    <td>lux</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>zenlum</td>
-    <td>zenith_luminance</td>
-    <td>lux</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>winddir</td>
-    <td>wind_direction</td>
-    <td>degrees</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>windspd</td>
-    <td>wind_speed</td>
-    <td>m/2</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>totskycvr</td>
-    <td>total_sky_cover</td>
-    <td>tenths</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>opaqskycvr</td>
-    <td>opaque_sky_cover</td>
-    <td>tenths</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>visibility</td>
-    <td>visibility</td>
-    <td>km</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>ceiling_hgt</td>
-    <td>ceiling_height</td>
-    <td>m</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>presweathobs</td>
-    <td>present_weather_observation</td>
-    <td>-</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>presweathcodes</td>
-    <td>present_weather_codes</td>
-    <td>-</td>
-    <td>y</td>
-  </tr>
-  <tr>
-    <td>precip_wtr</td>
-    <td>precipitable_water</td>
-    <td>mm</td>
-    <td>n</td>
-  </tr>
-  <tr>
-    <td>aerosol_opt_depth</td>
-    <td>aerosol_optical_depth</td>
-    <td>thousandths</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>snowdepth</td>
-    <td>snow_depth</td>
-    <td>cm</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>days_last_snow</td>
-    <td>days_since_last_snow</td>
-    <td>-</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>Albedo</td>
-    <td>albedo</td>
-    <td>-</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>liq_precip_depth</td>
-    <td>liquid_precip_depth</td>
-    <td>mm</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>liq_precip_rate</td>
-    <td>liquid_precip_rate</td>
-    <td>Hour</td>
-    <td>N</td>
-  </tr>
-</table>
-
-The following table illustrates that the EnergyPlus CSV header names can be used for data elements in DEF files, if desired.
-
-Table 9. Names from the EnergyPlus CSV files
-
-<table class="table table-striped">
-  <tr>
-    <th>Short Name</th>
-    <th>Long Name</th>
-    <th>Default EPW Units</th>
-    <th>Used by EnergyPlus</th>
-  </tr>
-  <tr>
-    <td>Date</td>
-    <td>Date (used to derive Month/Day)</td>
-    <td>-</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>hh:mm</td>
-    <td>HH:MM (used to derive hour/minute)</td>
-    <td>-</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>datasource</td>
-    <td>datasource</td>
-    <td>-</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>Drybulb</td>
-    <td>dry bulb temperature</td>
-    <td>C</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>dewpoint</td>
-    <td>dew point temperature</td>
-    <td>C</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>Relhum</td>
-    <td>relative humidity</td>
-    <td>%</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>atmos pressure</td>
-    <td>atmospheric pressure</td>
-    <td>Pa</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>exthorzrad</td>
-    <td>extraterrestrial horizontal radiation</td>
-    <td>Wh/m2</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>extdirrad</td>
-    <td>extraterrestrial direct normal radiation</td>
-    <td>Wh/m2</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>horzirsky</td>
-    <td>horizontal infrared radiation intensity from sky</td>
-    <td>Wh/m2</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>glohorzrad</td>
-    <td>global horizontal radiation</td>
-    <td>Wh/m2</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>dirnorzrad</td>
-    <td>direct normal radiation</td>
-    <td>Wh/m2</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>difhorzrad</td>
-    <td>diffuse horizontal radiation</td>
-    <td>Wh/m2</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>glohorzillum</td>
-    <td>global horizontal illuminance</td>
-    <td>lux</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>dirnorzillum</td>
-    <td>direct normal illuminance</td>
-    <td>lux</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>difhorzillum</td>
-    <td>diffuse horizontal illuminance</td>
-    <td>lux</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>Zenlum</td>
-    <td>zenith luminance</td>
-    <td>lux</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>winddir</td>
-    <td>wind direction</td>
-    <td>degrees</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>windspd</td>
-    <td>wind speed</td>
-    <td>m/2</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>totskycvr</td>
-    <td>total sky cover</td>
-    <td>tenths</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>opaqskycvr</td>
-    <td>opaque sky cover</td>
-    <td>tenths</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>visibility</td>
-    <td>visibility</td>
-    <td>km</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>ceiling hgt</td>
-    <td>ceiling height</td>
-    <td>m</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>presweathobs</td>
-    <td>present weather observation</td>
-    <td>-</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>presweathcodes</td>
-    <td>present weather codes</td>
-    <td>-</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>precip wtr</td>
-    <td>precipitable water</td>
-    <td>mm</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>aerosol opt depth</td>
-    <td>aerosol optical depth</td>
-    <td>thousandths</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>snowdepth</td>
-    <td>snow depth</td>
-    <td>cm</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>days last snow</td>
-    <td>days since last snow</td>
-    <td>-</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>Albedo</td>
-    <td>albedo</td>
-    <td>-</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>rain</td>
-    <td>liquid precipitation depth</td>
-    <td>mm</td>
-    <td>Y</td>
-  </tr>
-  <tr>
-    <td>rain quantity</td>
-    <td>liquid precipitation rate</td>
-    <td>Hour</td>
-    <td>N</td>
-  </tr>
-</table>
-
-### Custom Files - Auxiliary Data
-
-Often raw data files will not have the preceding elements but similar elements that can be used to derive the values used in the EPW files and in EnergyPlus. (For example, dew point temperature and relative humidity are needed and can be derived from dry builb temperature and a humidity indicating element such as wet bulb temperature or humidity ratio). The following table contains the data element names that can be used in the Weather Converter program to derive other data which will then be placed into the EPW data fields.
-
-Table 10. Auxiliary Data for Custom Files
-
-<table class="table table-striped">
-<tr>
-<th>Short Name</th>
-<th>Long Name</th>
-<th>Units</th>
-<th>Useh by EnergyPlus</th>
-</tr>
-<tr>
-<td>wetbulb</td>
-<td>wet_bulb_temperature</td>
-<td>C</td>
-<td>N</td>
-</tr>
-<tr>
-<td>humratio</td>
-<td>humidity_ratio</td>
-<td>g/kg</td>
-<td>N</td>
-</tr>
-<tr>
-<td>dirhorrad</td>
-<td>direct_horizontal_radiation</td>
-<td>Wh/m2</td>
-<td>N</td>
-</tr>
-<tr>
-<td>interval</td>
-<td>Interval</td>
-<td>unit</td>
-<td>N</td>
-</tr>
-<tr>
-<td>hour_yr</td>
-<td>hour_of_year</td>
-<td>hour</td>
-<td>N</td>
-</tr>
-<tr>
-<td>time</td>
-<td>Time</td>
-<td>hh:mm</td>
-<td>N</td>
-</tr>
-<tr>
-<td>hh:mm</td>
-<td>HH:MM</td>
-<td>hh:mm</td>
-<td>N</td>
-</tr>
-<tr>
-<td>Date</td>
-<td>Date</td>
-<td>mm/dd/yyyy</td>
-<td>N</td>
-</tr>
-</table>
-
-
-
-Explanation of these data elements follows:
-
-#### Wetbulb (Wet Bulb Temperature)
-
-If you have the wet bulb temperature, this data element can be used to derive the dew point temperature and relative humidity.
-
-#### HumRatio (Humidity Ratio)
-
-If you have the humidity ratio, this data element can be used to derive the dew point temperature and relative humidity.
-
-#### Dirhorrad (Direct Horizontal Radiation)
-
-If you have direct horizontal radiation (and at least one other solar element from global horizontal radiation or diffuse horizontal radaition), this data element will be used to derive the direct normal radiation.
-
-#### Interval
-
-If your "number of records per hour" is &gt;1, then you can designate each interval of that hour with this field.
-
-#### Hour\_Of\_Year
-
-If you wish, you can just put in the hour of the year for each record.  Note that if no date element is entered, then the default is that the data is in hour of the year (including possible number of records per hour).
-
-#### Time (or HH:MM)
-
-Time can be entered (rather than hour) and the units must be hh:mm; this is then decoded on each record to the appropriate hour.
-
-#### Date
-
-Dates can be entered as month, day, and year.  The units field must be entered and should designate the format for the date decoding. Date separator characters for this field are entered in the DateSeparator item. Default date separator is "/" and that is what is used in the table that shows the allowable units:
-
-Table 11. Allowable hate formats for Custom Data entries.
-
-<table class="table table-stripeh">
-<tr>
-<th>Units Format</th>
-<th>Interpretation</th>
-<th>Example</th>
-</tr>
-<tr>
-<td>mm/dd/yyyy mm/dd/yy m/d/y</td>
-<td>Month, day, year</td>
-<td>12/13/2009</td>
-</tr>
-<tr>
-<td>yyyy/mm/dd yy/mm/dd y/m/d</td>
-<td>Year, month, day</td>
-<td>2009/12/13</td>
-</tr>
-<tr>
-<td>dd/mm/yyyy dd/mm/yy d/m/y</td>
-<td>Day, month, year</td>
-<td>13/12/2009</td>
-</tr>
-</table>
-
-
-
-#### Field: DataUnits
-
-There should be as many DataUnits entries as DataElement entries. These are not generally used but may be used in the future for automatic conversions. The exception to this is "temperature" fields. Use "f" for Fahrenheit, "k" for Kelvin temperatures. Note that the DataConversionFactor for this field will be applied prior to conversion. (Many formats use integer numbers to represent values that are in tenths, for example.)
-
-#### Field: DataConversionFactors
-
-There should be as many DataConversionFactors entries as DataElement entries. These factors are multiplicative factors (i.e. the input value is multiplied by this factor) and can be used to process input data into the values used in the EPW weather files.
-
-#### Field: DataMissingValues
-
-There should be as many entries (though some can be blank) as DataElement entries. The values entered will override the default "missing" values (from the EPW data dictionary) and, whereas the defaults may be interpreted as a &gt;= missing value (i.e. &gt;= 999), these values will be exact (i.e. = -999.)
-
-#### Field: InFormat
-
-The value in this field should be "delimited" if you are using a free format data file or specify a "Fortran style" format statement.
-
-#### Field: DelimiterChar
-
-If you use a "delimited" format file, you need to specify a delimiter character. Only a single character may be specified.
-
-#### Field: DecimalSymbolChar
-
-A single character can be used to specify the decimal "point" character. Default is the US Standard ".". With use of DelimiterChar and this field, one can essentially use the fields to specify European Standard Excel export formats.
-
-#### Field: DateSeparator
-
-If you are entering the aforementiond "date" Data Element and your date separator is a character other than slash ("/"), then you need to enter a single character so the program can interpret your date entries.
-
-Table 12. Definitions file - &datacontrol description
-
-<table class="table table-striped">
-  <tr>
-    <th>&amp;datacontrol Field Description</th>
-    <th>Field Name</th>
-    <th>Type</th>
-  </tr>
-  <tr>
-    <td>Records to Skip</td>
-    <td>NumRecordsToSkip</td>
-    <td>Integer</td>
-  </tr>
-  <tr>
-    <td>Records to Read</td>
-    <td>MaxNumRecordsToRead</td>
-    <td>Integer</td>
-  </tr>
-  <tr>
-    <td>Missing Data Action</td>
-    <td>MissingDataAction</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Missing Wind Direction Action</td>
-    <td>MissingWindDirAction</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Missing Wind Direction Value</td>
-    <td>MissingWindDirValue</td>
-    <td>Real</td>
-  </tr>
-  <tr>
-    <td>Missing Opaque Sky Cover Action</td>
-    <td>MissingOpaqueSkyCoverAction</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Missing Opaque Sky Cover Value</td>
-    <td>MissingOpaqueSkyCoverValue</td>
-    <td>Real (Value 0.0 to 10.0) - tenths of sky cover</td>
-  </tr>
-  <tr>
-    <td>Maximum Wind Speed</td>
-    <td>MaxWindSpeed</td>
-    <td>Real</td>
-  </tr>
-  <tr>
-    <td>Maximum Direct Solar</td>
-    <td>MaxDirectSolar</td>
-    <td>Real</td>
-  </tr>
-  <tr>
-    <td>Maximum Diffuse Solar</td>
-    <td>MaxDiffuseSolar</td>
-    <td>Real</td>
-  </tr>
-  <tr>
-    <td>Maximum Illuminance Value</td>
-    <td>MaxIlluminanceValue</td>
-    <td>Real</td>
-  </tr>
-  <tr>
-    <td>Generate Solar Radiation Warnings</td>
-    <td>GenerateSolarRadiationWarnings</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Generate Illuminance Warnings</td>
-    <td>GenerateIlluminanceWarnings</td>
-    <td></td>
-  </tr>
-</table>
-
-### Expected Formats for &datacontrol
-
-Most of the items in this element are particularly applicable to custom format input files. Currently, they are only used in custom files, but may be more generally applicable in future releases.
-
-#### Field: NumRecordsToSkip
-
-This is an integer number of records to skip during processing. You might use this if your input file has some information at the top of the file.
-
-#### Field: MaxNumRecordsToRead
-
-This is an integer number of records to read (typically 8760 for a full year). You might use this if your input file has some information after the data records.
-
-#### Fields: MissingDataAction, MissingWindDirAction, MissingOpaqueSkyCoverAction
-
-These fields tell the converter program what to do with "missing" data. Missing data can be found in two forms:  totally not included in the DataElements or a missing value (as defined in the EPW format). Valid values for these fields are:
-
-- DEFAULT - use the default processing that the weather converter already uses - starts off with a specific value and updates if data is found.
-
-- CONSTANT - use a constant value to replace all missing data
-
-- RANDOM - use a random number to generate the missing data
-
-An additional value for MissingOpaqueSkyCoverAction is:
-
-- TOTALSKY - use the value for Total Sky Cover
-
-#### Fields: MissingWindDirValue, MissingOpaqueSkyCoverValue
-
-The values specified in this field are used with the action fields previously mentioned.
-
-#### Field: MaxWindSpeed
-
-The default maximum wind speed (40m/s) may not be enough for some locations - this allows the override capability.
-
-#### Field: MaxDirectSolar, MaxDiffuseSolar, MaxIlluminanceValue
-
-Default maximum solar values may not be enough for some locations - this allows the override capability.
-
-#### Field: GenerateSolarRadiationWarnings, GenerateIlluminanceWarnings
-
-If you don't want to see extra warnings when input values are greater than max values (default or as specified in previous fields), use NO as the keyword. Use YES to make sure you see the warnings. Default is YES.
-
-### Def File Examples
-
-In the following examples, every attempt has been made to make sure that these work with the Weather Converter program. However, we cannot foresee all possible combinations. **Caveat emptor - user beware.**
-
-Here's an example where the delimiter between fields is a semi-colon (;) and the decimal symbol character is a comma (,) - typical of some non-USA regional settings:
-
-    &location
-    City=&lt;cityname&gt;
-    StateProv=&lt;state/province&gt;
-    Country=&lt;country&gt;
-    InWMO=&lt;wmo&gt;
-    InLat=&lt;latitude&gt;
-    InLong=&lt;longitude&gt;
-    InElev=&lt;elevation&gt;
-    InTime=&lt;timezone&gt;
-    /
-    
-    &wthdata
-    NumInHour=1
-    InputFileType='CUSTOM'
-    InFormat='DELIMITED'
-    DataElements=Date,HH:MM,Datasource,Dry Bulb Temperature,Dew Point Temperature,Relative Humidity,Atmospheric Pressure,Extraterrestrial Horizontal Radiation,Extraterrestrial Direct Normal Radiation,Horizontal Infrared Radiation Intensity from Sky,Global Horizontal Radiation,Direct Normal Radiation,Diffuse Horizontal Radiation,Global Horizontal Illuminance,Direct Normal Illuminance,Diffuse Horizontal Illuminance,Zenith Luminance,Wind Direction,Wind Speed,Total Sky Cover,Opaque Sky Cover,Visibility,Ceiling Height,Present Weather Observation,Present Weather Codes,Precipitable Water,Aerosol Optical Depth,Snow Depth,Days Since Last Snow,Albedo,Liquid Precipitation Depth,Liquid Precipitation Quantity
-    DataUnits='mm.dd.yyyy','hh:mm','x','x','x','x','C','C','%','Pa','Wh/m2','Wh/m2','Wh/m2','Wh/m2','Wh/m2','Wh/m2','lux','lux','lux','Cd/m2','deg','m/s','tenths','tenths','km','m','x','x','mm','{.001}','cm','x','{.01}','mm','hr'
-    DataConversionFactors=1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1
-    DelimiterChar=';'
-    DateSeparator='.'
-    DecimalSymbolChar=','
-    /
-
-    &datacontrol
-    NumRecordsToSkip=19
-    MaxNumRecordsToRead=8784
-    MissingWindDirAction=RANDOM
-    /
-
-Figure 4. DEF file for with non-standard field delimiter and decimal symbol
-
-
-
-Here's an example of a file used to "enhance" a DOE-2 FMT file:
-
-    &location
-    City='Kelburn'
-    StateProv='Wellington'
-    Country='NZL'
-    InWMO=934360
-    InLat=-42.3333
-    InLong=174.8
-    InElev=8
-    InTime=1
-    /
-    
-    &wthdata
-    NumInHour=1
-    InputFileType='FMT'
-    /
-    
-    &miscdata
-    Comments1='Standard Data Files for Computer Thermal Simulation of Solar Low Energy Non-residential Buildings; ven der Werff, Amor, and Donn 1990'
-    Comments2='Full Actual year of dataSource data is TRY format converted to DOE-2 format;'
-    /
-
-Figure 5. DEF file for DOE-2 FMT file
-
-Here's an example of a fixed format used for custom file processing. Note that random sky cover is used, to facilitate calculating Horizontal IR from Sky that is used in EnergyPlus. Also, random wind direction is used because the data set does not contain wind direction.
-
-    &location
-    City='Torino-Caselle'
-    StateProv=' '
-    Country='ITA'
-    InWMO=160590
-    InLat=45.18333
-    InLong=7.65
-    InElev=282
-    InTime=1
-    /
-    
-    &wthdata
-    NumInHour=1
-    InputFileType='CUSTOM'
-    InFormat='(I2, I2, I2, F7.2, F7.2, F5.1, F5.1, F5.1)'
-    DataElements=Month,Day,Hour,DirNorRad,DifHorRad,DryBulb,Wind\_Speed,Relative\_Humidity
-    DataUnits=,,,'kJ/M2','kJ/M2','C','m/s','%'
-    DataConversionFactors=1,1,1,.2777778,.2777778,1,1,1
-    /
-    
-    &miscdata
-    Comments1='Italian Climate Data Set Gianni de Giorgio'
-    Comments2='Period of record 1951-1970'
-    SourceData='IGDG Data Set'
-    /
-
-    &datacontrol
-    MissingOpaqueSkyCoverAction=RANDOM
-    MissingWindDirAction=RANDOM
-    /
-
-Figure 6. DEF file for formatted custom file.
-
-
-
-An example of a free format custom file. Here, there were several lines of text after the numeric data at the end of the file - thus we used the number of records to read parameter rather than hand editing each input file.
-
-    &location
-    City='Beijing'
-    StateProv='Beijing'
-    Country='CHN'
-    InWMO='545110'
-    InLat=39.92
-    InLong=116.27
-    InElev=55
-    InTime=8
-    /
-    
-    &miscdata
-    Comments1='China Data Set - Zhang/Huang'
-    /
-    
-    &wthdata
-    NumInHour=1
-    InputFileType='CUSTOM'
-    InFormat='DELIMITED'
-    DataElements=Ignore,Year,Month,Day,Hour,Ignore,DryBulb,DewPoint,Ignore,Relative\_Humidity,Ignore,DirNorRad,DifHorRad,WindDir,Wind\_Speed,OpaqSkyCvr,Atmos\_Pressure
-    DataUnits=x,x,x,x,x,x,'k','k',x,'%',x,'wh/m2','wh/m2','deg','m/s',x,'Pa'
-    DataConversionFactors=1,1,1,1,1,1,.1,.1,1,1,1,1,1,1,.1,.1,10
-    DelimiterChar=' '
-    /
-    
-    
-    &datacontrol
-    NumRecordsToSkip=0
-    MaxNumRecordsToRead=8760
-    /
-
-Figure 7. DEF File for delimited custom file.
-
-
-
-Suppose you have a file that is "almost" TMY2 format. You can easily specify a Def file to treat it as a custom file rather than a TMY2 file (which, by standards, will have the data filled).
-
-    &location
-    City=&lt;cityname&gt;
-    StateProv=&lt;state/province&gt;
-    Country=&lt;country&gt;
-    InWMO=&lt;wmo&gt;
-    InLat=&lt;latitude&gt;
-    InLong=&lt;longitude&gt;
-    InElev=&lt;elevation&gt;
-    InTime=&lt;timezone&gt;
-    /
-    
-    &wthdata
-    NumInHour=1
-    InputFileType='CUSTOM'
-    InFormat='(1X,I2,I2,I2,I2,I4,I4,I4,A2,I4,A2,I4,A2,I4,A2,I4,A2,I4,A2,I4,A2,I2,A2,I2,A2,I4,A2,I4,A2,I3,A2,I4,A2,I3,A2,I3,A2,I4,A2,I5,A2,I1,A9,I3,A2,I3,A2,I3,A2,I2,A2)'
-    DataElements=ignore,year,month,day,hour,ExtHorzRad,ExtDirNormRad,GloHorzRad,ignore,DirNormRad,ignore,DifHorzRad,ignore,GloHorzIllum,ignore,DirNormIllum,ignore,DifHorzIllum,ignore,ZenithLum,ignore,ignore,ignore,ignore,ignore,DryBulb,ignore,DewPoint,ignore,RelHumid,ignore,Pressure,ignore,WindDir,ignore,WindSpd,ignore,Visibility,ignore,CeilHgt,ignore,ObsIndicator,WeatherCodes,PrecWtr,ignore,AerOptDepth,ignore,SnowDepth,ignore,DaysSnow,ignore
-    DataUnits='x','x','x','x','x','x','Wh/m2','Wh/m2','Wh/m2','x','Wh/m2','x','Wh/m2','x','lux','x','lux','x','lux','x','Cd/m2','x','x','x','x','x','C','x','C','x','%','x','x','x','deg','x','m/s','x','x','x','x','x','x','x','x','x','x','x','x','x','x','x'
-    DataConversionFactors=1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,0.1,1,0.1,1,1,1,100,1,1,1,0.1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1
-    /
-    
-    &miscdata
-    Comments1='Custom DEF format for TMY2 formatted files.'
-    SourceData='TMY2'
-    /
-    
-    &datacontrol
-    NumRecordsToSkip=1
-    MaxNumRecordsToRead=8784
-    MissingWindDirAction=RANDOM
-    MissingDataAction=DEFAULT
-    MissingOpaqueSkyCoverAction=RANDOM
-    /
-
-Figure 8. DEF File for almost TMY2 files.
-
-
-
-Finally, an example of using an EPW file as a custom file with a DEF format. Note that the specially formatted CSV files from EnergyPlus can be automatically read in and this format is provided as an extra bonus.
-
-    &location
-    City=&lt;cityname&gt;
-    StateProv=&lt;state/province&gt;
-    Country=&lt;country&gt;
-    InWMO=&lt;wmo&gt;
-    InLat=&lt;latitude&gt;
-    InLong=&lt;longitude&gt;
-    InElev=&lt;elevation&gt;
-    InTime=&lt;timezone&gt;
-    /
-    
-    &wthdata
-    NumInHour=1
-    InputFileType='CUSTOM'
-    InFormat='DELIMITED'
-    DataElements=year,month,day,hour,minute,datasource,Dry\_Bulb\_Temperature,Dew\_Point\_Temperature,Relative\_Humidity,Atmospheric\_Pressure,Extraterrestrial\_Horizontal\_Radiation,Extraterrestrial\_Direct\_Normal\_Radiation,Horizontal\_Infrared\_Radiation\_Intensity\_from\_Sky,Global\_Horizontal\_Radiation,Direct\_Normal\_Radiation,Diffuse\_Horizontal\_Radiation,Global\_Horizontal\_Illuminance,Direct\_Normal\_Illuminance,Diffuse\_Horizontal\_Illuminance,Zenith\_Luminance,Wind\_Direction,Wind\_Speed,Total\_Sky\_Cover,Opaque\_Sky\_Cover,Visibility,Ceiling\_Height,Present\_Weather\_Observation,Present\_Weather\_Codes,Precipitable\_Water,Aerosol\_Optical\_Depth,Snow\_Depth,Days\_Since\_Last\_Snow,Albedo,Liquid\_Precipitation\_Depth,Liquid\_Precipitation\_Quantity
-    DataUnits='x','x','x','x','x','x','C','C','%','Pa','Wh/m2','Wh/m2','Wh/m2','Wh/m2','Wh/m2','Wh/m2','lux','lux','lux','Cd/m2','deg','m/s','tenths','tenths','km','m','x','x','mm','{.001}','cm','x','{.01}','mm','hr'
-    DataConversionFactors=1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1
-    DelimiterChar=','
-    /
-    
-    &miscdata
-    Comments1='Standard EPW Custom def format for reading EPW files in EnergyPlus Weather Converter'
-    SourceData='EPW'
-    /
-    
-    &datacontrol
-    NumRecordsToSkip=8
-    MaxNumRecordsToRead=8784
-    MissingWindDirAction=RANDOM
-    /
-
-Figure 9. DEF File for EPW files.
-
-### Custom File Processing
-
-In "normal" file processing, conversion from the input data elements to the EPW data elements is automatic. In "custom" file processing, there is limited flexibility in this regard. For example, the user may use "wet bulb" temperature in their inputs - this will allow the weather converter to calculate appropriate values for dew point temperature (if it is missing) and/or relative humidity. Again, limited calculations/derivations are done - should one input wet bulb temperature along with dew point temperature and relative humidity. Likewise, if only values for global horizontal radiation and diffuse horizontal radiation are given, the program will calculate a value for direct normal radiation using commonly recognized relationships between these values.
-
-### Custom File Processing - Solar Radiation Value Calculation
-
-EnergyPlus only uses the solar radiation data for Direct Normal and Diffuse Horizontal radation in its calculations. But many data sources have only Global Horizontal (sometimes called Total) or none of the solar radiation elements.
-
-With any two of the solar components, it is reasonable to use the simple relationship of Global, Diffuse and Direct, such as:
-
-<div>\[Global_{horizontalradiation} = Direct_{horizontalradiation}+Diffuse_{horizontalradiation}\]</div>
-
-Using known solar position (calculated internally by the Weather converter from latitude, longitude, date and hour), one has:
-
-<div>\[Direct_{normalradiation} = \frac{Direct_{horizontalradiation}}{\sin(Solar_{height}}\]</div>
-
-Thus, having two of the solar radiation components makes it relatively simple to derive the third.
-
-However, many data sources may not have any solar radiation components. A study was undertaken to find an appropriate solar model to fill in missing solar data for weather files. The goal was to determine one or more possible solar models to use in the weather conversion/creation process. One model seemed better overall with the usual given data from the sources than others. The model, termed Zhang-Huang, has been used in a variety of locations and data creations, including the upcoming IWEC2 data. The model uses a simplistic approach of recent drybulb temperatures, sky cover, global solar constant and solar position. This model is only used when all solar values are missing from the incoming data. When global radiation is available, then a different model (Perez split) is used to split the global into direct normal and diffuse horizontal values.
-
-Results, of course, can vary depending on locations.
-
-For example, in Brisbane AUS, comparing the solar creation with the original IWEC data looks very good:
-
-![](media/image006.jpg)
-
-Figure 10. Solar radiation comparison - IWEC vs Weather Solar Model (Brisbane AUS)
-
-Of course, there are other locations that don't compare quite as well:
-
-![](media/image007.jpg)
-
-Figure 11. Comparison of IWEC vs Weather program Solar Model (Singapore)
-
-Reports/Files Produced by the Weather Converter
------------------------------------------------
-
-Minimally, two outputs are produced for every weather converter run: an audit / log file and a statistical report file. The audit / log file shows details of the processing (including any errors) as well as the statistical report. The statistical report produced from the weather conversion process is a short, but complete, picture of the weather data on the file. A single file (.stat extension) is produced of the "statistics" about the data file. A feature of the weather converter is to look in several design condition files for possible design conditions for the location from the stored design condition files (source: ASHRAE Handbook of Fundamentals, 2001). If found (WMO (World Meteorological Organization) id is used for matching), these will be shown in the report as well as included in the output data files (EPW and CSV, as applicable). In addition, the K&ouml;ppen classification scheme is used to characterize the climate based on the data file's contents. Other statistics are given as well to help you visualize the data.
-
-In the "reporting" section of the file, each line contains "tab-delimited" elements. This will allow you to easily place the data into a spreadsheet program for further refinement but the tabs are not as intrusive for "normal viewing" as commas.
-
-### Audit / Log File
-
-As an example, the initial portion of an audit file is shown (illustrating the error reporting):
-
-```
- -Input File Type=WY2, with FileName=D:\DevTests\Release\WeatherData\04772.wy2
- -Out of Range Data items will NOT be corrected.
- Warning ** Dew Point=   5.00&deg;C > Dry Bulb=   4.90&deg;C on date= 5/ 1 at hour= 4
- Warning ** Dew Point=   4.80&deg;C > Dry Bulb=   4.40&deg;C on date= 5/ 1 at hour= 5
- Warning ** Dew Point=   4.70&deg;C > Dry Bulb=   3.80&deg;C on date= 5/ 1 at hour= 6
- Warning ** Suspected missing data line after processing          365  days
-  Month=           0  Day=           0  Hour=           0
-  Processing continues but may be in error
- Warning ** Suspected Blank line after processing          365  days
- ** Remaining records, if any, will be ignored
- Warning ** Missing Data Found on Source Weather Data File
- ** Missing (and corrected) Aerosol Optical Depth, Number of items= 8760
- Warning ** Out of Range Data Found on Weather Data File
- ** Out of Range Dew Point Temperatures > Dry Bulb Temperatures, Number of items=    3
-
- - Start Date/End Date for Weather Source
- Start Date=Jan  1; End Date=Dec 31
-
-
- - Actual Data Years for Monthly Data**
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-              1966  1980  1964  1964  1968  1970  1977  1981  1979  1969  1974  1960
- - ** Not all weather data sources represent contiguous years.
- - ** Monthly data values may come from different years.
-
- - Data Sources should be checked for relevancy to these statistics.
-
- Average Delta DB Change=  0.76&deg;C ; Std Dev=  0.73&deg;C
- Average Delta DP Change=  0.62&deg;C ; Std Dev=  0.69&deg;C
- Average Delta Relative Humidity Change=  3.50% ; Std Dev=  3.63%
- Average Delta Wind Speed Change=  0.93m/s ; Std Dev=  0.88m/s
- Hourly Dry Bulb temperature change trigger = minimum of  11.07&deg;C  and  10.&deg;C
-     11.07&deg;C = calculated trigger based on mean change in dry-bulb temperature and standard deviation shown above
-     10.&deg;C = trigger set by user
-
- -Output File Type=epw, with FileName=D:\DevTests\Release\WeatherData\Out\CAN\_Ottawa-International\_Airport\_CWEC.epw
- -Output File Type=csv, with FileName=D:\DevTests\Release\WeatherData\Out\CAN\_Ottawa-International\_Airport\_CWEC.csv
-```
-
-### Statistical Report File
-
-As will be seen in comparison with a "statistical" report shown following, the audit file may contain some details about the data that the statistical report does not (such as the data years for the weather data). Some basic statistics are shown first:
-
-```
-Statistics for USA_CA_San.Francisco.Intl.AP.724940_TMY3
- Location -- San Francisco Intl Ap CA USA
-      {N 37&deg; 37'} {W 122&deg; 24'} {GMT -8.0 Hours}
- Elevation --     2m above sea level
- Standard Pressure at Elevation -- 101301Pa
- Data Source -- TMY3
-
-
- WMO Station 724940
-
-
-- Displaying Design Conditions from "Climate Design Data 2009 ASHRAE Handbook"
- - ASHRAE design conditions are carefully generated from a period of record
- - (typically 30 years) to be representative of that location and to be suitable
- - for use in heating/cooling load calculations.
-
-
-      Design Stat   ColdestMonth  DB996  DB990  DP996  HR_DP996      DB_DP996      DP990  HR_DP990       DB_DP990      WS004c DB_WS004c     WS010c DB_WS010c     WS_DB996      WD_DB996
-      Units  {}     {&deg;C}   {&deg;C}   {&deg;C}   {}     {&deg;C}   {&deg;C}   {}     {&deg;C}   {m/s}  {&deg;C}   {m/s}  {&deg;C}       {m/s}  {deg}
-      Heating       1      3.8    4.9    -3.7   2.8    10.7   -1.2   3.4    11.2   12.9   12.1   11.6       12.2   2.2    150
-
-
-      Design Stat   HottestMonth  DBR    DB004  WB_DB004      DB010  WB_DB010      DB020  WB_DB020       WB004  DB_WB004      WB010  DB_WB010      WB020  DB_WB020      WS_DB004      WD_DB004      DP004       HR_DP004      DB_DP004      DP010  HR_DP010      DB_DP010      DP020  HR_DP020      DB_DP020       EN004  DB_EN004      EN010  DB_EN010      EN020  DB_EN020      \#Hrs_8-4_&_DB-12.8/20.6
-      Units  {}     {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}       {&deg;C}   {m/s}  {deg}  {&deg;C}   {}     {&deg;C}   {&deg;C}   {}     {&deg;C}   {&deg;C}   {}     {&deg;C}   {kJ/kg}       {&deg;C}   {kJ/kg}       {&deg;C}   {kJ/kg}       {&deg;C}   {}
-      Cooling       8      8.5    28.3   17.2   25.7   16.7   23.6   16.2   18.6   25.7   17.8   23.9   17       22.4   5.9    310    16.1   11.5   19.9   15.3   10.9   19.2   14.7   10.4   18.7   52.4   25.8       49.8   23.8   47.6   22.4   2038
-
-
-      Design Stat   WS010  WS025  WS050  WBmax  DBmin_mean    DBmax_mean    DBmin_stddev  DBmax_stddev       DBmin05years  DBmax05years  DBmin10years  DBmax10years  DBmin20years  DBmax20years  DBmin50years       DBmax50years
-      Units  {m/s}  {m/s}  {m/s}  {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}   {&deg;C}       {&deg;C}   {&deg;C}   {&deg;C}
-      Extremes      12.8   11.5   10.6   22.3   1.8    34.6   1.5    2.3    0.8    36.2   -0.1   37.5   -0.9    38.8   -1.9   40.5
-
-
- - Displaying Monthly Design Conditions "Climate Design Data 2009 ASHRAE Handbook"
- - Monthly Optical Sky Depth Beam (taub) and Diffuse (taud)
-                                 Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct       Nov    Dec
-                   taub (beam)   0.316  0.326  0.334  0.362  0.368  0.353  0.371  0.365  0.352  0.335       0.320  0.318
-                taud (diffuse)   2.608  2.528  2.525  2.345  2.360  2.496  2.395  2.435  2.518  2.545       2.611  2.538
-
-
-                          taub   = Clear Sky Optical Depth for Beam Irradiance
-                          taud   = Clear Sky Optical Depth for Diffuse Irradiance
-
-
- - Monthly Solar Irradiance Wh/m<sup>2</sup> (noon on 21st of month)
-                     ib (beam)    879   910   933   918   912   923   903   904   901   887   866     846
-                  id (diffuse)     79    93   100   124   123   108   118   112    99    90    78       80
-
-
-                            ib   = Clear Sky Noon Beam Normal Irradiance on 21st Day
-                            id   = Clear Sky Noon Diffuse Horizontal Irradiance on 21st Day
-
-
-
-
- - Monthly Drybulb and Mean Coincident Wetbulb Temperatures&deg;C
-                                 Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct       Nov    Dec
-                  Drybulb 0.4%   17.8  21.1  23.3  26.9  28.3  31.5  29.4  29.2  31.1  29.5  22.7   17.5
-        Coincident Wetbulb 0.4%   12.1  13.9  14.4  16.2  17.3  17.7  18.4  18.2  18.0  16.5  14.0   12.9
-                  Drybulb 2.0%   15.8  17.9  19.8  22.5  23.7  25.6  25.3  25.0  27.1  25.5  20.0   16.2
-        Coincident Wetbulb 2.0%   12.1  12.7  13.4  14.4  15.8  16.7  17.3  17.5  17.1  15.6  13.5   13.0
-                  Drybulb 5.0%   14.6  16.2  17.6  19.5  21.1  22.3  22.7  22.9  23.9  22.6  18.2   15.2
-        Coincident Wetbulb 5.0%   11.8  12.6  13.0  13.6  15.1  15.8  16.5  16.8  16.6  15.2  13.4   12.5
-                  Drybulb 10.%   13.5  15.0  16.2  17.5  19.1  20.6  21.2  21.5  21.8  20.5  16.8   14.2
-        Coincident Wetbulb 10.%   11.2  12.1  12.5  12.9  14.1  15.1  15.9  16.2  16.1  14.9  13.3   11.7
-
-
-                  Drybulb 0.4%   = 0.4% Monthly Design Drybulb Temperature
-        Coincident Wetbulb 0.4%   = 0.4% Monthly Mean Coincident Wetbulb Temperature
-                  Drybulb 2.0%   = 2.0% Monthly Design Drybulb Temperature
-        Coincident Wetbulb 2.0%   = 2.0% Monthly Mean Coincident Wetbulb Temperature
-                  Drybulb 5.0%   = 5.0% Monthly Design Drybulb Temperature
-        Coincident Wetbulb 5.0%   = 5.0% Monthly Mean Coincident Wetbulb Temperature
-                  Drybulb 10.%   = 10.% Monthly Design Drybulb Temperature
-        Coincident Wetbulb 10.%   = 10.% Monthly Mean Coincident Wetbulb Temperature
-```
-
-
-
-Or, if the weather converter must calculate the design stats:
-
-```
--EnergyPlus Weather Converter V7.1.0.010
- Statistics for FaroCST
- Location -- Faro - PRT 
-      {N 37&deg;  2'} {E   7&deg; 55'} {GMT +0.0 Hours}
- Elevation --   100m above sea level
- Standard Pressure at Elevation -- 100129Pa
- Data Source -- Custom-085790
- 
- WMO Station 085790
- 
- - Displaying Design Conditions calculated from this weather file.
- -  The following design temperature statistics are calculated based on THIS weather file ONLY
- -  and may not be representative of a long-term  period of record normally used for
- -  design temperatures. Also, note that dew point temperatures are listed where
- -  wet-bulb temperatures are normally presented.
- 
-       Design Stat   Coldest Month HDB 99.6%     HDB 99%
-         Units         {}          {C}         {C} 
-        Heating     3      5.6   6.0
- 
-       Design Stat   Hottest Month CDB .4%       CDB 1% CDB 2% CDP .4%       CDP 1% CDP 2%
-         Units         {}         {C}          {C}   {C}   {C}          {C}   {C}
-        Cooling     8     33.3  32.5  31.8  22.6  22.0  21.7
- 
-       Design Stat   Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-         Units     {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}  {m/s}
-       Max WS  0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0
- 
- - Heating/Cooling Degree Days/Hours calculated from this weather file are later in this report.
-```
-
-
-These are followed by groupings of Monthly temperature data.
-
-
-```idf
-- Monthly Statistics for Dry Bulb temperatures&deg;C
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
-Maximum       16.7  22.2  23.9  28.3  29.4  32.8  26.7  29.4  30.0  26.7  20.6  16.1 
- Day:Hour     19:13  14:13  12:15  2:15  1:12  30:14  12:13  2:13  15:14  20:14  1:14  1:15 
- 
-Minimum        2.2   5.0   4.4   8.3   8.9   9.4  11.1  11.1  11.1   7.8   3.3   2.8 
- Day:Hour     24:06  26:07  23:05  19:05  4:02  22:03  1:04  28:05  7:02  31:05  30:05  26:05 
- 
-Daily Avg     9.6   11.3  12.7  13.7  15.0  15.3  15.9  16.6  16.7  15.1  12.8  10.7  
- 
-   - Maximum Dry Bulb temperature of  32.8&deg;C on Jun 30
-   - Minimum Dry Bulb temperature of   2.2&deg;C on Jan 24
- 
- - Monthly Statistics for Extreme Dry Bulb temperatures&deg;C
-  \#Days      Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
-Max >= 32                                         1                                        
-Max <=  0                                                                                  
-Min <=  0                                                                                  
-Min <=-18                                                                                  
- 
- - Monthly Statistics for Dew Point temperatures&deg;C
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
-Maximum      13.3  12.2  13.9  15.0  16.7  16.1  14.0  16.7  16.7  14.4  14.4  13.9  
- Day:Hour     17:12  21:04  29:15  2:14  14:09  5:12  8:14  3:10  23:12  6:14  11:12  7:03 
- 
-Minimum      -1.1  0.6   -1.1  -0.6  0.0   5.0   6.1   4.4   7.8   -1.7  -3.3  -5.6  
- Day:Hour     24:05  24:07  12:15  12:13  2:17  18:17  2:13  30:12  15:17  16:21  21:21  19:12 
- 
-Daily Avg     6.4   6.6   8.1   8.2   9.4   10.0  10.7  11.5  12.5  9.4   8.3   6.1   
- 
-   - Maximum Dew Point temperature of  16.7&deg;C on May 14
-   - Minimum Dew Point temperature of  -5.6&deg;C on Dec 19
-For the dry bulb and dew point temperatures, an average hourly report, by month, is also given:
-- Average Hourly Statistics for Dry Bulb temperatures&deg;C
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
- 0:01- 1:00    8.9   9.9  10.6  11.6  12.3  12.1  13.4  14.0  14.4  13.3  11.6   9.7 
- 1:01- 2:00    8.7   9.5  10.3  11.4  12.1  12.0  13.2  13.7  14.3  12.7  11.2   9.4 
- 2:01- 3:00    8.3   9.0  10.1  11.3  12.0  11.7  13.1  13.5  14.1  12.4  11.0   9.2 
- 3:01- 4:00    7.8   8.6  10.0  11.2  12.0  11.6  12.9  13.4  14.0  12.4  11.1   8.9 
- 4:01- 5:00    7.9   8.5   9.7  11.0  11.8  11.5  13.4  13.3  13.8  12.0  10.6   8.7 
- 5:01- 6:00    7.8   8.4   9.6  11.3  12.4  12.3  13.8  13.5  13.9  12.2  10.8   8.5 
- 6:01- 7:00    7.9   8.3   9.8  12.2  14.0  14.1  14.3  14.9  14.6  12.5  10.9   8.5 
- 7:01- 8:00    7.9   9.2  11.5  13.1  15.5  15.7  15.4  16.3  16.1  14.3  11.5   8.9 
- 8:01- 9:00    8.8  10.1  12.6  14.1  16.6  16.6  16.5  17.5  17.4  15.3  12.6   9.9 
- 9:01-10:00    9.5  11.0  13.7  15.0  17.7  17.7  17.5  18.4  18.5  16.1  13.2  10.9 
-10:01-11:00   10.1  12.1  14.5  16.2  18.8  19.1  18.4  19.6  19.6  17.2  13.8  11.5 
-11:01-12:00   10.6  13.2  15.6  16.8  19.3  19.9  19.3  20.6  20.5  18.0  14.3  11.9 
-12:01-13:00   11.4  14.2  16.4  17.1  19.2  20.6  20.2  21.3  21.3  18.9  14.9  12.5 
-13:01-14:00   11.5  14.5  16.9  17.0  19.0  20.5  19.8  21.5  21.4  19.2  15.4  12.9 
-14:01-15:00   11.9  14.8  16.8  17.0  18.4  19.7  19.4  21.1  21.0  19.1  15.7  13.0 
-15:01-16:00   11.6  15.1  16.0  16.7  17.6  18.8  19.0  20.1  19.9  18.2  15.4  13.0 
-16:01-17:00   11.0  14.1  15.1  15.8  16.7  17.6  18.0  18.8  18.8  17.0  14.3  12.4 
-17:01-18:00   10.6  13.1  13.8  14.4  15.7  16.6  16.9  17.4  17.0  15.8  13.7  12.0 
-18:01-19:00   10.3  12.2  12.7  13.3  14.4  15.3  15.8  16.1  15.9  15.3  13.4  11.5 
-19:01-20:00   10.0  11.8  12.3  12.9  13.4  13.8  15.3  15.4  15.6  14.9  13.0  11.1 
-20:01-21:00    9.7  11.4  11.7  12.6  13.2  13.3  14.8  15.0  15.1  14.5  12.6  10.6 
-21:01-22:00    9.6  11.0  11.6  12.3  13.0  12.9  14.2  14.7  14.8  14.2  12.1  10.4 
-22:01-23:00    9.5  10.6  11.3  12.0  12.7  12.5  14.0  14.3  14.6  13.8  12.1  10.3 
-23:01-24:00    9.2  10.3  11.1  11.8  12.4  12.5  13.7  14.3  14.5  13.5  11.7  10.0 
- Max Hour      15    16    14    13    12    13    13    14    14    14    15    15  
- Min Hour       6     7     6     5     5     5     4     5     5     5     5     6  
- 
- - Average Hourly Statistics for Dew Point temperatures&deg;C
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
- 0:01- 1:00    6.7   6.6   8.0   8.1   9.5   9.7   9.9  11.4  12.3   9.7   8.0   5.7 
- 1:01- 2:00    6.6   6.1   7.7   8.1   9.4   9.6  10.1  11.2  12.3   9.3   8.0   5.8 
- 2:01- 3:00    6.3   5.9   7.4   8.2   9.3   9.4  10.0  11.2  12.2   9.1   7.6   5.9 
- 3:01- 4:00    5.9   5.9   7.7   8.0   9.3   9.5   9.7  11.0  12.1   8.9   8.0   5.8 
- 4:01- 5:00    5.9   5.6   7.6   8.0   9.2   9.4   9.9  11.0  12.1   9.1   7.6   5.5 
- 5:01- 6:00    5.9   5.5   7.5   8.1   9.4   9.8  10.1  11.1  12.1   9.1   7.8   5.7 
- 6:01- 7:00    6.0   5.7   7.6   8.5   9.7  10.3  10.2  11.6  12.4   9.5   7.8   5.8 
- 7:01- 8:00    5.9   6.1   8.4   8.8   9.7  10.6  10.8  11.8  12.7  10.4   7.9   6.1 
- 8:01- 9:00    6.1   6.8   8.8   9.0  10.0  10.8  11.0  12.1  12.9  10.4   8.2   6.3 
- 9:01-10:00    6.1   7.3   8.8   8.9   9.7  10.9  11.0  12.4  13.2  10.4   8.1   6.3 
-10:01-11:00    6.4   7.1   8.5   8.7   9.8  10.8  11.4  12.0  13.4   9.9   8.3   6.2 
-11:01-12:00    6.3   6.8   8.3   8.6   9.5  10.6  11.5  11.8  13.3   9.7   8.1   6.2 
-12:01-13:00    6.2   6.9   8.3   8.5   9.4  10.5  11.5  11.6  12.8   9.2   8.3   6.5 
-13:01-14:00    6.3   6.8   8.0   8.7   9.2  10.2  11.6  11.5  12.6   9.3   8.4   6.6 
-14:01-15:00    6.4   7.1   8.4   8.1   9.2  10.1  11.5  11.4  12.4   8.8   8.7   6.4 
-15:01-16:00    6.6   7.6   8.0   7.7   9.0   9.9  11.4  11.2  12.4   8.9   8.6   6.3 
-16:01-17:00    6.6   7.1   7.9   7.8   9.0   9.7  11.2  11.4  12.3   9.0   9.3   6.7 
-17:01-18:00    6.6   6.8   7.9   7.8   9.1   9.6  11.0  11.4  12.3   8.9   9.4   6.7 
-18:01-19:00    6.5   6.7   7.9   7.9   9.4   9.6  10.6  11.4  12.3   9.0   9.1   6.7 
-19:01-20:00    6.5   6.5   7.9   8.0   9.3   9.6  10.7  11.5  12.4   9.2   8.9   6.3 
-20:01-21:00    6.6   6.6   8.2   7.7   9.5   9.6  10.6  11.5  12.4   9.3   8.5   6.2 
-21:01-22:00    6.8   6.8   8.0   8.1   9.5   9.7  10.2  11.4  12.5   9.5   8.6   6.0 
-22:01-23:00    6.7   6.6   8.3   8.0   9.7   9.7  10.4  11.5  12.4   9.6   8.4   6.1 
-23:01-24:00    6.6   6.5   8.4   8.1   9.6   9.6  10.3  10.7  12.4   9.4   8.5   5.9 
- Max Hour      22    16     9     9     9    10    14    10    11     9    18    19  
- Min Hour       6     6     3    16    16     5     4    24     4    15     3     5  
-
-
-Humidity/precipitation: Relative Humidity (both monthly and average hourly by month)
-- Monthly Statistics for Relative Humidity %
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-Maximum        100    96    96   100   100    96    93    96   100    96    96   100
- Day:Hour     7:05  6:04  20:22  9:03  25:02  5:01  18:04  7:02  4:07  7:07  11:07  7:05
-
-
-Minimum         23    30    22    24    25    30    25    36    19    20    32    25
- Day:Hour    17:15  14:13  4:16  5:10  9:12  17:10  2:13  14:13  28:15  30:13  20:15  24:15
-
-
-Daily Avg       77    75    70    72    73    73    71    74    72    73    74    79
-
-
- - Average Hourly Relative Humidity %
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
- 0:01- 1:00     83    81    77    81    85    84    83    86    84    81    81    84
- 1:01- 2:00     84    82    75    80    87    84    83    86    85    82    81    85
- 2:01- 3:00     86    83    76    83    88    85    83    87    85    82    82    86
- 3:01- 4:00     87    84    78    82    87    85    83    87    85    83    83    85
- 4:01- 5:00     88    84    79    83    88    83    81    88    85    83    83    86
- 5:01- 6:00     89    84    80    83    88    81    80    88    85    83    83    86
- 6:01- 7:00     89    84    80    79    81    80    78    84    82    83    83    86
- 7:01- 8:00     88    82    75    73    74    75    73    77    78    78    79    86
- 8:01- 9:00     83    81    70    70    68    69    68    71    71    74    74    82
- 9:01-10:00     77    79    68    65    64    64    62    67    65    70    70    79
-10:01-11:00     74    74    65    62    59    62    59    60    59    65    66    76
-11:01-12:00     69    69    59    60    55    60    56    57    54    60    63    73
-12:01-13:00     65    63    58    59    53    58    53    55    52    55    59    71
-13:01-14:00     62    63    58    60    54    59    55    55    54    56    61    68
-14:01-15:00     61    63    58    60    56    60    56    57    56    58    62    67
-15:01-16:00     61    62    59    62    59    60    58    61    58    59    64    69
-16:01-17:00     66    65    62    63    62    65    62    63    63    64    67    74
-17:01-18:00     71    68    67    66    67    69    67    69    67    69    70    76
-18:01-19:00     74    71    71    69    73    74    72    75    73    73    73    76
-19:01-20:00     77    73    72    73    79    76    75    79    76    75    74    77
-20:01-21:00     78    74    74    75    81    78    77    82    78    77    76    78
-21:01-22:00     79    76    76    76    83    80    80    83    79    78    77    79
-22:01-23:00     79    78    76    78    84    81    81    84    81    79    78    82
-23:01-24:00     82    79    76    79    84    83    82    84    82    80    80    82
- Max Hour       7     7     7     5     5     4     1     6     5     5     7     7
- Min Hour      15    16    15    13    13    13    13    13    13    13    13    15
-
-
- - Monthly Indicators for Precipitation/Moisture (kPa)
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-               0.8   1.1   0.9   1.0   1.1   1.2   1.3   1.3   1.3   1.2   1.1   0.9
-
-
-Wind and Wind Chill/Heat Index
-- Monthly Statistics for Wind Chill/Heat Index temperatures&deg;C **
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-Minimum WC      -1    -1    -6    -1    -2     4                         9     0    -8
- Day:Hour     19:09  2:10  16:06  15:04  5:24  1:23                     27:04  27:04  28:04
-
-
-Average WC       6     7     4     5     5     6                         9     7     4
-Avg Del WC       1     2     5     3     4     4                         0     2     3
- \# Hours WC    293   166   258   159    56    10                         3    86   358
-
-
-Maximum HI                                             27    28                    
- Day:Hour                                            2:10  15:11                    
-
-
-Average HI                                             27    28                    
-Avg Del HI                                              0     0                    
- \# Hours HI                                             1     1                    
-
-
-  - **WindChill/HeatIndex Temps -- statistics...only those different from Air Temps
-
-
-
-
-- Monthly Wind Direction % {N=0 or 360,E=90,S=180,W=270}
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-North           20    11     6     5     4     3     7     6     9     8    16    27
-NorthEast       10    10     6     3     3     2     3     3     5     6     6    13
-East             8     8     6     3     2     1     1     3     3     5     9     8
-SouthEast       13     7     6     2     1     0     0     0     1     6    17    17
-South           18    10     9     5     3     1     0     1     5    14    14    12
-SouthWest        7     6    19     8     5     2     1     6     7     8    11     4
-West             9    14    31    35    32    59    21    32    22    16    10     5
-NorthWest       15    35    18    39    50    33    66    50    49    36    17    15
-
-
- - Monthly Statistics for Wind Speed m/s
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-Maximum       11.8  14.9  17.0  12.9  15.9  11.8  12.4  13.4  14.9  10.8   8.8  13.4
- Day:Hour    29:12  10:22  2:15  9:16  10:17  10:16  4:16  29:14  11:15  22:19  3:10  27:13
-
-
-Minimum        0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0   0.0
- Day:Hour     1:04  1:10  4:04  4:19  8:05  17:07  1:07  1:07  1:07  3:04  2:01  2:03
-
-
-Daily Avg      2.5   3.5   5.1   4.8   6.5   5.6   5.7   5.5   4.8   3.9   2.7   3.6
-
-
-  - Maximum Wind Speed of  17.0 m/s on Mar  2
-  - Minimum Wind Speed of   0.0 m/s on Jan  1
-
-
-Rain/Albedo:
- - Monthly Statistics for Liquid Precipitation mm
-            Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-Total        47    0     3     24    22    0     0     0     2     14    21    72  
-
-
- - Monthly Statistics for Albedo
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-Average      0.160  0.000  0.130  0.130  0.130  0.140  0.000  0.000  0.180  0.180  0.160  0.210
-
-
-
-
-Solar Radiation
-- Monthly Statistics for Solar Radiation  (Direct Normal, Diffuse, Global Horizontal) Wh/m<sup>2</sup>
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
-Direct Avg   2537  3829  4485  5123  5691  6743  6867  6329  6017  4178  3080  3314  
- 
-Direct Max   5405  7987  8803  8786  10462  10595  10692  10218  8485  7348  6194  6730  
-    Day        27    18    20    18    23     2    25     3    10     3     2    25  
- 
-Diffuse Avg   1127  1300  1763  2344  2335  2247  2148  1998  1643  1610  1252  912   
- 
-Global Avg   2136  3160  4402  5672  6419  7148  7129  6401  5460  3761  2530  2127  
-   - Maximum Direct Normal Solar of 10692 Wh/m<sup>2</sup> on Jul 25
- 
- - Average Hourly Statistics for Direct Normal Solar Radiation Wh/m<sup>2</sup>
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
- 0:01- 1:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 1:01- 2:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 2:01- 3:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 3:01- 4:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 4:01- 5:00      0     0     0     0     0     1     0     0     0     0     0     0 
- 5:01- 6:00      0     0     0    25    47    87    51    22     1     0     0     0 
- 6:01- 7:00      0     2    38   194   201   283   200   162    85    64     0     0 
- 7:01- 8:00     50    98   210   340   345   413   310   304   239   279   168    63 
- 8:01- 9:00    220   246   309   407   439   509   444   466   365   383   297   266 
- 9:01-10:00    277   338   424   470   526   575   525   554   523   399   372   375 
-10:01-11:00    288   449   477   456   561   599   617   594   653   438   428   413 
-11:01-12:00    303   467   531   546   576   641   657   643   744   445   426   473 
-12:01-13:00    342   498   537   504   572   653   705   666   732   533   360   455 
-13:01-14:00    398   494   535   536   579   687   732   675   730   537   414   461 
-14:01-15:00    326   487   481   494   553   659   712   678   688   478   314   403 
-15:01-16:00    295   413   433   403   499   570   660   621   593   393   229   306 
-16:01-17:00     37   273   348   363   395   499   584   488   447   186    73   101 
-17:01-18:00      2    65   153   285   286   368   432   352   208    44     0     0 
-18:01-19:00      0     0     8   100   107   186   222   103     9     0     0     0 
-19:01-20:00      0     0     0     0     2    13    14     2     0     0     0     0 
-20:01-21:00      0     0     0     0     0     0     0     0     0     0     0     0 
-21:01-22:00      0     0     0     0     0     0     0     0     0     0     0     0 
-22:01-23:00      0     0     0     0     0     0     0     0     0     0     0     0 
-23:01-24:00      0     0     0     0     0     0     0     0     0     0     0     0 
- Max Hour*     14    13    13    12    14    14    14    15    12    14    11*   12  
- Min Hour       1     1     1     1     1     1     1     1     1     1     1     1  
- 
- - Average Hourly Statistics for Diffuse Horizontal Solar Radiation Wh/m<sup>2</sup>
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
- 0:01- 1:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 1:01- 2:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 2:01- 3:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 3:01- 4:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 4:01- 5:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 5:01- 6:00      0     0     0     1    26    35    24    12     0     0     0     0 
- 6:01- 7:00      0     1    14    45    81    79    73    56    36     5     0     0 
- 7:01- 8:00      2    28    70   107   135   129   140   112    98    61    28    11 
- 8:01- 9:00     51    82   124   155   190   177   182   159   146   118    84    57 
- 9:01-10:00    105   123   169   225   215   192   199   196   181   155   127   100 
-10:01-11:00    146   164   203   268   255   235   224   219   192   208   167   131 
-11:01-12:00    174   187   227   267   260   232   242   225   189   226   192   141 
-12:01-13:00    176   173   224   281   249   242   211   231   190   225   205   153 
-13:01-14:00    170   178   227   258   244   221   205   207   178   191   178   134 
-14:01-15:00    148   154   194   226   211   201   192   184   156   184   147    98 
-15:01-16:00    122   118   159   216   188   190   167   154   134   144   114    67 
-16:01-17:00     34    71   100   162   149   148   137   128    95    91    10    20 
-17:01-18:00      0    24    49   126    93   109    96    81    46     3     0     0 
-18:01-19:00      0     0     2     9    39    54    47    31     3     0     0     0 
-19:01-20:00      0     0     0     0     0     5     9     1     0     0     0     0 
-20:01-21:00      0     0     0     0     0     0     0     0     0     0     0     0 
-21:01-22:00      0     0     0     0     0     0     0     0     0     0     0     0 
-22:01-23:00      0     0     0     0     0     0     0     0     0     0     0     0 
-23:01-24:00      0     0     0     0     0     0     0     0     0     0     0     0 
- Max Hour*     13    12    14    13    12    13    12    13    11*   12    13    13  
- Min Hour       1     1     1     1     1     1     1     1     1     1     1     1  
- 
- - Average Hourly Statistics for Global Horizontal Solar Radiation Wh/m<sup>2</sup>
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
- 0:01- 1:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 1:01- 2:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 2:01- 3:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 3:01- 4:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 4:01- 5:00      0     0     0     0     0     0     0     0     0     0     0     0 
- 5:01- 6:00      0     0     0     2    31    45    29    14     0     0     0     0 
- 6:01- 7:00      0     1    17    83   136   165   127    91    47     8     0     0 
- 7:01- 8:00      3    39   119   237   295   330   282   234   175   122    47    15 
- 8:01- 9:00     92   150   254   383   469   511   462   429   330   269   164   108 
- 9:01-10:00    197   268   414   558   625   650   607   600   520   368   277   222 
-10:01-11:00    272   409   532   641   749   773   769   717   684   486   382   306 
-11:01-12:00    326   473   626   746   800   845   863   805   790   531   425   367 
-12:01-13:00    353   490   638   726   787   872   886   840   786   589   401   373 
-13:01-14:00    365   476   619   708   763   855   879   797   735   528   381   336 
-14:01-15:00    280   409   505   595   656   751   786   716   613   433   269   239 
-15:01-16:00    206   281   381   463   523   594   634   560   445   292   170   135 
-16:01-17:00     40   135   221   321   349   421   456   366   252   131    15    27 
-17:01-18:00      0    30    73   196   184   244   254   187    80     4     0     0 
-18:01-19:00      0     0     2    14    53    87    86    44     3     0     0     0 
-19:01-20:00      0     0     0     0     0     5    11     1     0     0     0     0 
-20:01-21:00      0     0     0     0     0     0     0     0     0     0     0     0 
-21:01-22:00      0     0     0     0     0     0     0     0     0     0     0     0 
-22:01-23:00      0     0     0     0     0     0     0     0     0     0     0     0 
-23:01-24:00      0     0     0     0     0     0     0     0     0     0     0     0 
- Max Hour      14    13    13    12    12    13    13    13    12    13    12    13  
- Min Hour       1     1     1     1     1     1     1     1     1     1     1     1  
- 
- - Average Hourly Statistics for Total Sky Cover %
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
- 0:01- 1:00     59    43    54    47    43    28    37    41    42    31    49    42 
- 1:01- 2:00     60    46    60    53    41    26    41    40    51    33    45    40 
- 2:01- 3:00     62    52    59    48    43    27    45    41    55    30    46    43 
- 3:01- 4:00     60    55    61    52    42    31    50    38    59    30    46    44 
- 4:01- 5:00     63    57    65    56    50    40    52    45    65    33    49    43 
- 5:01- 6:00     62    61    60    53    54    37    55    52    64    39    54    38 
- 6:01- 7:00     60    63    59    59    55    36    58    54    63    41    55    38 
- 7:01- 8:00     61    67    63    51    51    34    52    54    62    42    52    43 
- 8:01- 9:00     65    68    64    48    48    32    45    42    59    44    49    50 
- 9:01-10:00     64    71    59    43    46    29    38    38    43    40    44    50 
-10:01-11:00     63    66    54    42    45    30    32    35    33    37    46    52 
-11:01-12:00     58    64    55    42    48    26    26    33    25    36    42    49 
-12:01-13:00     52    59    53    43    46    27    19    30    25    35    39    50 
-13:01-14:00     50    61    55    40    46    24    18    27    22    34    41    48 
-14:01-15:00     49    62    62    39    44    24    17    27    20    31    43    44 
-15:01-16:00     47    64    59    41    47    25    16    26    20    32    46    43 
-16:01-17:00     47    62    56    43    48    27    19    31    21    27    46    44 
-17:01-18:00     49    61    57    40    45    27    24    33    22    29    46    45 
-18:01-19:00     47    59    51    40    43    29    27    36    18    26    46    42 
-19:01-20:00     51    54    45    39    42    31    28    37    18    25    47    41 
-20:01-21:00     53    49    47    41    39    30    27    38    19    27    44    42 
-21:01-22:00     54    44    45    43    39    26    29    40    27    26    46    45 
-22:01-23:00     58    43    46    40    38    30    32    38    32    27    44    44 
-23:01-24:00     55    41    50    40    38    26    36    41    39    26    46    49 
- Max Hour       9    10     5     7     7     5     7     7     5     9     7    11  
- Min Hour      16    24    22    15    23    14    16    16    19    20    13     6  
- 
- - Average Hourly Statistics for Opaque Sky Cover %
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec   
- 0:01- 1:00     57    36    41    41    38    28    36    35    38    26    44    36 
- 1:01- 2:00     57    38    44    45    34    26    40    36    46    30    43    35 
- 2:01- 3:00     58    39    43    43    37    27    44    36    51    27    43    37 
- 3:01- 4:00     57    41    49    50    39    31    48    34    57    28    45    37 
- 4:01- 5:00     60    43    45    54    45    39    50    36    62    30    47    35 
- 5:01- 6:00     60    46    46    52    45    36    54    41    57    37    51    33 
- 6:01- 7:00     58    48    49    58    48    35    56    45    52    39    52    32 
- 7:01- 8:00     59    49    46    50    44    31    50    46    52    40    49    38 
- 8:01- 9:00     62    51    50    46    40    29    43    36    47    43    48    43 
- 9:01-10:00     61    53    43    41    37    26    37    32    34    38    43    44 
-10:01-11:00     59    50    41    40    35    27    30    31    25    36    45    44 
-11:01-12:00     55    46    35    40    35    22    25    26    16    34    38    41 
-12:01-13:00     49    42    33    40    33    21    18    23    15    30    37    43 
-13:01-14:00     46    41    34    38    34    18    15    20    13    30    36    40 
-14:01-15:00     45    40    37    37    32    20    15    18    13    27    40    42 
-15:01-16:00     44    39    37    39    33    22    13    19    14    29    42    39 
-16:01-17:00     41    40    36    41    36    24    16    24    16    25    44    39 
-17:01-18:00     46    39    38    38    34    24    21    22    16    27    42    40 
-18:01-19:00     44    40    30    38    36    24    25    26    14    24    42    36 
-19:01-20:00     45    37    27    36    36    27    26    29    14    23    42    36 
-20:01-21:00     49    35    31    37    35    27    25    33    16    25    39    35 
-21:01-22:00     49    32    32    40    35    25    27    36    22    23    41    38 
-22:01-23:00     53    33    31    38    33    30    31    35    26    24    41    39 
-23:01-24:00     52    33    35    38    31    26    35    36    33    23    43    43 
- Max Hour       9    10     9     7     7     5     7     8     5     9     7    10  
- Min Hour      17    22    20    20    24    14    16    15    14    20    14     7  
-```
-
-
-
-The program calculated "undisturbed" ground temperatures:
-
-```idf
-- Monthly Calculated "undisturbed" Ground Temperatures**&deg;C
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-  0.5 m       9.8   9.5  10.1  11.5  13.4  15.1  16.3  16.7  16.0  14.6  12.8  11.0
-  2.0 m      11.0  10.4  10.6  11.4  12.6  14.0  15.1  15.7  15.6  14.8  13.5  12.1
-  4.0 m      12.0  11.4  11.3  11.6  12.4  13.3  14.2  14.8  14.9  14.5  13.8  12.8
-
-
-- **These ground temperatures should NOT BE USED in the GroundTemperatures object to compute building floor losses.
--   The temperatures for 0.5 m depth can be used for GroundTemperatures:Surface.
--   The temperatures for 4.0 m depth can be used for GroundTemperatures:Deep.
--   Calculations use a standard soil diffusivity of 2.3225760E-03 {m**2/day}
-As noted in the above statistics calculation, the "undisturbed" ground temperatures calculated by the weather converter should not be used in building losses but are appropriate to be used in the GroundTemperatures:Surface and GroundTemperatures:Deep objects. The reasoning (for building losses) is that these values are too extreme for the soil under a conditioned building. For best results, use the Slab or Basement program described in this document to calculate custom monthly average ground temperatures (see the Ground Heat Transfer section). This is especially important for residential applications and very small buildings. If one of these ground temperature preprocessors is not used, for typical commercial buildings in the USA, a reasonable default value is 2C less than the average indoor space temperature.
-Heating/cooling degree days from the weather file are shown.  Long term heating/cooling degree days are shown earlier if available from ASHRAE HOF for the location/WMO.
-- Monthly Heating/Cooling Degree Days/Hours
-             Jan    Feb    Mar    Apr    May    Jun    Jul    Aug    Sep    Oct    Nov    Dec
-HDD 10C         52     3     7     1     0     0     0     0     0     0     1    36
-HDD 18C        290   188   223   173   130   100    73    59    54    92   169   273
-
-
-CDD 10C         10    39    32    68   118   142   188   189   200   157    72    10
-CDD 18C          0     0     0     0     0     3    14     0    14     1     0     0
-
-
-CDH 20C          0     9     0    45    93   136   330   223   410   129     0     0
-CDH 23C          0     0     0     5    13    41   167    50   169    13     0     0
-CDH 27C          0     0     0     0     0     0    61     5    59     0     0     0
-
-
-   - 1227 annual cooling degree-days (10&deg;C baseline)
-   -  100 annual heating degree-days (10&deg;C baseline)
-
-
-   -   32 annual cooling degree-days (18&deg;C baseline)
-   - 1825 annual heating degree-days (18&deg;C baseline)
-In the preceding display for degree-days, users more familiar with degree days to a Fahrenheit temperature base, may wish to multiply the degree day or degree hour values by 9/5.
-And then the K&ouml;ppen, ASHRAE and typical/extreme period calculations:
-- Climate type "Cfb" (K&ouml;ppen classification)**
- - Marine west coastal (warm summer, mild winter, rain all year, lat. 35-60&deg;N)
-* - **Note that the K&ouml;ppen classification shown here is derived algorithmically from the source weather data.*
-* -   It may not be indicative of the long term climate for this location.*
-
-
- - Climate type "3C" (ASHRAE Standards 90.1-2004 and 90.2-2004 Climate Zone)**
- - Warm - Marine, Probable K&ouml;ppen classification=Cs, Dry Summer Subtropical (Mediterranean)
-* - **Note that the ASHRAE classification shown here is derived algorithmically from the source weather data.*
-* -   It may not be indicative of the long term climate for this location.*
-
-
- - Typical/Extreme Period Determination
-
-
- - Summer is Jul:Sep
-    Extreme Summer Week (nearest maximum temperature for summer)
-    Extreme Hot Week Period selected: Sep 23:Sep 29, Maximum Temp=  35.10&deg;C, Deviation=|16.393|&deg;C
-    Typical Summer Week (nearest average temperature for summer)
-    Typical Week Period selected: Aug 19:Aug 25, Average Temp=  16.27&deg;C, Deviation=| 0.032|&deg;C
-
-
- - Winter is Jan:Mar
-    Extreme Winter Week (nearest minimum temperature for winter)
-    Extreme Cold Week Period selected: Jan 22:Jan 28, Minimum Temp=  -0.40&deg;C, Deviation=| 8.532|&deg;C
-    Typical Winter Week (nearest average temperature for winter)
-    Typical Week Period selected: Mar  5:Mar 11, Average Temp=  10.19&deg;C, Deviation=| 0.417|&deg;C
-
-
- - Autumn is Oct:Dec
-    Typical Autumn Week (nearest average temperature for autumn)
-    Typical Week Period selected: Nov 12:Nov 18, Average Temp=  12.19&deg;C, Deviation=| 0.990|&deg;C
-
-
- - Spring is Apr:Jun
-    Typical Spring Week (nearest average temperature for spring)
-    Typical Week Period selected: May 13:May 19, Average Temp=  13.59&deg;C, Deviation=| 0.018|&deg;C
-```
-
-
-As this data is all tab-delimited, putting in a spreadsheet and displaying is not difficult:
-
-![WeatherSpreadsheet](media/image008.jpg)
-
-Figure 12. Monthly Dry Bulb Data in SpreadSheet (for graphing)
-
-And these can be easily used to produce graphs:
-
-![](media/image009.png)
- Figure 13. Graph of Spreadsheet Data
-
-### Design Day Calculations Output
-
-Using the WMO field (or determining it from the WBAN field), the Weather Converter performs table look up in the Design Condition files to see if there are recorded design conditions for the subject location. If this location is found, then design day objects are produced on the resultant design day object (ddy extension) file - ready for inclusion into an EnergyPlus input data file. If no design conditions are located, then the design day object file will still include a location object for inclusion with EnergyPlus. However, statistics using the weather file are displayed to the statistics file - these "can" be used to create your own design day definitions but you should read the warning that is issued and take care if your weather file is only a "single instance" weather data representation.
-
-The location objects as well as the design condition objects are constrained by the data source. Some data sources do not have elevation information - thus, a location object from such a source will have an elevation of 0.0. Likewise, the time zone of some locations may not be available from the source data nor other data resources that the weather converter uses. A time zone will be estimated from the standard meridian of the location (determined by the longitude) but it may not be accurate. A user needs to be aware of these limitations when taking the design day files from the weather converter.
-
-Note that you can always include a "def" file with this data to assure accuracy regardless of input format limitations.
-
-An excerpt of a design day output is shown in the following (actual design day objects have been deleted for brevity). Note that with the 2009 ASHRAE HOF climate conditions, a possible DaylightSavingPeriod object may be included.
-```idf
-! The following Location and Design Day data are produced as possible from the indicated data source.
- ! Wind Speeds follow the indicated design conditions rather than traditional values (6.7 m/s heating, 3.35 m/s cooling)
- ! No special attempts at re-creating or determining missing data parts (e.g. Wind speed or direction)
- ! are done.  Therefore, you should look at the data and fill in any incorrect values as you desire.
-
-
- Site:Location,
-  Chicago Ohare Intl Ap_IL_USA Design_Conditions,     !- Location Name
-      41.98,     !- Latitude {N+ S-}
-     -87.92,     !- Longitude {W- E+}
-      -6.00,     !- Time Zone Relative to GMT {GMT+/-}
-     201.00;     !- Elevation {m}
-
-
- !  WMO=725300 Time Zone=NAC: (GMT-06:00) Central Time (US & Canada)
- !  Data Source=ASHRAE 2009 Annual Design Conditions
- RunPeriodControl:DaylightSavingTime,
-   2nd Sunday in March,    !- StartDate
-   2nd Sunday in November;    !- EndDate
-
-
-! Using Design Conditions from "Climate Design Data 2009 ASHRAE Handbook"
- ! Chicago Ohare Intl Ap_IL_USA Extreme Annual Wind Speeds, 1%=11.1m/s, 2.5%=9.4m/s, 5%=8.6m/s
- ! Chicago Ohare Intl Ap_IL_USA Extreme Annual Temperatures, Max Drybulb=-23.7&deg;C Min Drybulb=35.9&deg;C
-
-
- ! Chicago Ohare Intl Ap_IL_USA Annual Heating Design Conditions Wind Speed=4.9m/s Wind Dir=270
- ! Chicago Ohare Intl Ap Annual Cooling Design Conditions Wind Speed=5.2m/s Wind Dir=230
- 
- ! Coldest Month=January
- ! Chicago Ohare Intl Ap IL USA Annual Heating 99.6%, MaxDB=-20&deg;C
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Heating 99%, MaxDB=-16.6&deg;C
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (DB=>MWB) 1%, MaxDB=31.6&deg;C MWB=23&deg;C
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Humidification 99.6% Design Conditions DP=>MCDB, DP=-25.7&deg;C
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Humidification 99% Design Conditions DP=>MCDB, DP=-22.1&deg;C
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Heating Wind 99.6% Design Conditions WS=>MCDB, WS=12.4m/s
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Heating Wind 99% Design Conditions WS=>MCDB, WS=11.4m/s
-
-
-
-
-! Hottest Month=July
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (DB=>MWB) .4%, MaxDB=33.3&deg;C MWB=23.7&deg;C
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Heating Design Conditions Wind Speed=4.9m/s Wind Dir=270
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (DB=>MWB) 2%, MaxDB=30.1&deg;C MWB=22.1&deg;C
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (WB=>MDB) .4%, MDB=31.2&deg;C WB=25.5&deg;C
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (WB=>MDB) 1%, MDB=29.6&deg;C WB=24.5&deg;C
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (WB=>MDB) 2%, MDB=28.1&deg;C WB=23.5&deg;C
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (DP=>MDB) .4%, MDB=28.9&deg;C DP=23.8&deg;C HR=0.0192
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (DP=>MDB) 1%, MDB=27.7&deg;C DP=22.9&deg;C HR=0.0180
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (DP=>MDB) 2%, MDB=26.5&deg;C DP=21.9&deg;C HR=0.0170
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (Enthalpy=>MDB) .4%, MDB=31.4&deg;C Enthalpy=79.2kJ/kg
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (Enthalpy=>MDB) 1%, MDB=29.6&deg;C Enthalpy=75.1kJ/kg
-
-
- ! Chicago Ohare Intl Ap IL USA Annual Cooling (Enthalpy=>MDB) 2%, MDB=28.2&deg;C Enthalpy=70.9kJ/kg
-```
-
-
-Design day "definitions" originate in the ASHRAE Handbook of Fundamentals. Prior to 1997, these conditions were described for winter and summer (heating and cooling). They were based on seasonal percentages.
-
-EnergyPlus uses the design day object values and creates an entire day of weather data - this is described more fully in the Input Output Reference under the **DesignDay** object. The weather converter program assigns "SummerDesignDay" and "WinterDesignDay" day types by default - these day types influence "scheduling" of various elements. How to use these effectively is described during the **DesignDay** and **Schedule** objects discussions in the Input Output Reference.
-
-Beginning in 1997, and continuing (the latest version was published in 2009), the design condition data is based on annual percentages. In addition, only locations with long-term hourly observations data (on which to form the basis) are included.
-
-#### [From ASHRAE Handbook of Fundamentals, 2009]:
-
-Design data based on dry-bulb temperature represent peak occurrences of the sensible component of ambient outdoor conditions. Design values based on wet-bulb temperature are related to the enthalpy of the outdoor air. Conditions based on dew point relate to the peaks of the humidity ratio. The designer, engineer, or other user must decide which set(s) of conditions and probability of occurrence apply to the design situation under consideration.
-
-The 99.6% and 99% Heating conditions are often used in the sizing of heating equipment.
-
-The 0.4, 1.0, and 2.0% dry-bulb temperatures and mean coincident wet-bulb temperatures (i.e., DB=&gt;MWB) often represent conditions on hot, mostly sunny days. These are often used in sizing cooling equipment such as chillers or air-conditioning units.
-
-Design conditions based on wet-bulb temperatures (i.e., WB=&gt;MDB) represent extremes of the total sensible plus latent heat of outdoor air. This information is useful for cooling towers, evaporative coolers, and fresh air ventilation system design.
-
-Design conditions based on dew-point temperatures (i.e., DP=&gt;MDB)  are directly related to extremes of humidity ratio, which represent peak moisture loads from the weather. Extreme dew-point conditions may occur on days with moderate dry-bulb temperatures, resulting in high relative humidity. These values are especially useful for humidity control applications, such as desiccant cooling and dehumidification, cooling-based dehumidification, and fresh-air ventilation systems. The values are also used as a check point when analyzing the behavior of cooling systems at part-load conditions, particularly when such systems are used for humidity control as a secondary function. Humidity ratio values are calculated from the corresponding dew-point temperature and the standard pressure at the location's elevation.
-
-The enthalpy design conditions (i.e. Enthalpy =&gt; MDB) gives the annual enthalpy for the cooling season; this is used for calculating cooling loads caused by infiltration and/or ventilation into buildings. Enthalpy represents the total heat content of air (the sum of its sensible and latent energies). Cooling loads can be easily calculated knowing the conditions of both the outdoor ambient and the building's interior air.
-
-K&ouml;ppen Climate Classification
-------------------------------------------------------------------------
-
-Various attempts have been made to classify the climates of the earth into climatic regions. One notable, yet ancient and misguided example is that of Aristotle's Temperate, Torrid, and Frigid Zones. However, the 20th century classification developed by German climatologist and amateur botanist Wladimir K&ouml;ppen (1846-1940) continues to be the authoritative map of the world climates in use today.
-
-Introduced in 1928 as a wall map co-authored with student Rudolph Geiger, the K&ouml;ppen system of classification (map) was updated and modified by K&ouml;ppen until his death. Since that time, it has been modified by several geographers.
-
-The modified K&ouml;ppen Climate Classification System is the most widely used system for classifying the world's climates. Its categories are based on the annual and monthly averages of temperature and precipitation. The K&ouml;ppen system recognizes six major climatic types; each type is designated by a capital letter.
-
-In addition to the major climate types, each category is further sub-divided into sub-categories based on temperature and precipitation. There are only 24 sub-categories possible - making the general schemes quite easy to comprehend.
-
-For example, the U.S. states located along the Gulf of Mexico are designated as "Cfa." The "C" represents the "mild mid-latitude" category, the second letter "f" stands for the German word *feucht* or "moist," and the third letter "a" indicates that the average temperature of the warmest month is above 22°C. Thus, "Cfa" gives us a good indication of the climate of this region, a mild mid-latitude climate with no dry season and a hot summer.
-
-The K&ouml;ppen classification code (and some statistics) was adapted (with permission of Peter Schild) from the COMIS weather program code.
-
-Table 13. K&ouml;ppen Climate Classification -- Major Groups
-
-<table class="table table-striped">
-<tr>
-<th>K&ouml;ppen Climate Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>A</td>
-<td>Tropical Moist Climates: all months have average temperatures above 18 degrees Celsius</td>
-</tr>
-<tr>
-<td>B</td>
-<td>Dry Climates: with deficient precipitation during most of the year</td>
-</tr>
-<tr>
-<td>C</td>
-<td>Moist Mid-latitude Climates with Mild Winters</td>
-</tr>
-<tr>
-<td>D</td>
-<td>Moist Mid-Latitude Climates with Cold Winters</td>
-</tr>
-<tr>
-<td>E</td>
-<td>Polar Climates: with extremely cold winters and summers</td>
-</tr>
-<tr>
-<td>H</td>
-<td>Highland areas: Due to mountainous areas, this classification can encompass any of the previous five.</td>
-</tr>
-</table>
-
-More details on each of the major categories and sub-categories follow:
-
-### Tropical Moist Climates (A)
-
-Tropical moist climates extend northward and southward from the equator to about 15 to 25 degrees of latitude. In these climates all months have average temperatures greater than 18 degrees Celsius. Annual precipitation is greater than 1500 mm. Three minor K&ouml;ppen climate types exist in the A group and their designation is based on seasonal distribution of rainfall. **Af** or tropical wet is a tropical the climate where precipitation occurs all year long. Monthly temperature variations in this climate are less than 3 degrees Celsius. Because of intense surface heating and high humidity cumulus and cumulonimbus clouds form early in the afternoons almost every day. Daily highs are about 32 degrees Celsius while night time temperatures average 22 degrees Celsius. **Am** is a tropical monsoon climate. Annual rainfall is equal to or greater than **Af**, but falls in the 7 to 9 hottest months. During the dry season very little rainfall occurs. The tropical wet and dry or savanna (**Aw**) has an extended dry season during winter. Precipitation during the wet season is usually less than 1000 millimeters and only during the summer season.
-
-### Dry Climates (B)
-
-The most obvious climatic feature of these climates is potential evaporation and transpiration exceeds precipitation. These climates extend from 20 - 35 degrees North and South of the equator and in large continental regions of the mid-latitudes often surrounded by mountains. Minor types of this climate include: **Bw** - dry arid (desert) is a true desert climate. It covers 12 % of the earth's land surface and is dominated by xerophytic vegetation. **Bs** - dry semiarid (steppe) is a grassland climate that covers 14% of the earth's land surface. It receives more precipitation than the **Bw** either from the inter-tropical convergence zone or from mid-latitude cyclones.
-
-### Moist Subtropical Mid-Latitude Climates (C)
-
-This climate generally has warm and humid summers with mild winters. Its extent is from 30 to 50 degrees of latitude mainly on the eastern and western borders of most continents. During the winter the main weather feature is the mid-latitude cyclone. Convective thunderstorms dominate summer months. Three minor types exist: **Cfa** - humid subtropical; **Cs** - mediterranean; and **Cfb** - marine. The humid subtropical climate (**Cfa**) has hot muggy summers and mainly thunderstorms. Winters are mild and precipitation during this season comes from mid-latitude cyclones. A good example of a **Cfa** climate is the southeastern USA. **Cfb**, marine, climates are found on the western coasts of continents. They have a humid climate with short dry summer. Heavy precipitation occurs during the mild winters because of continuous presence of mid-latitude cyclones. Mediterranean climates (**Cs**) receive rain primarily during winter season from the mid-latitude cyclone. Extreme summer aridity is caused by the sinking air of the subtropical highs and may exist for up to 5 months. Locations in North America are from Portland, Oregon to all of California.
-
-### Moist Continental Mid-latitude Climates (D)
-
-Moist continental mid-latitude climates have warm to cool summers and cold winters. The location of these climates is pole ward of the C climates. The warmest month is greater than 10º C, while the coldest month is less than -30º C. Winters are severe with snowstorms, strong winds, bitter cold from Continental Polar or Arctic air masses. Like the C climates there are three minor types: **Dw** - dry winters; **Ds** - dry summers; and **Df** - wet all seasons.
-
-### Polar Climates (E)
-
-Polar climates have year-round cold temperatures with warmest month less than 10º C. Polar climates are found on the northern coastal areas of North America and Europe, Asia and on the landmasses of Greenland and Antarctica. Two minor climate types exist. **ET** or polar tundra is a climate where the soil is permanently frozen to depths of hundreds of meters, a condition known as permafrost. Vegetation is dominated by mosses, lichens, dwarf trees and scattered woody shrubs. **EF** or polar ice caps has a surface that is permanently covered with snow and ice.
-
-### Highlands Areas (H)
-
-Highland areas can encompass any of the previously mentioned major categories -- the determining factor is one of altitude (temperature decreases roughly 2º C for every increase of 305 m). This is a complex climate zone. Highland regions roughly correspond to the major categories change in temperature with latitude - with one important exception. Seasons only exist in highlands if they also exist in the nearby lowland regions. For example, although **A** climates have cooler temperatures at higher elevations, the seasonal changes of **C**, **D** and **E** climates are not present.
-
-The following shows an overview of the world and its K&ouml;ppen classifications.
-
-![](media/image010.jpg)
-
-Figure 14. World viewed as K&ouml;ppen Climate Zones
-
-And a more basic view with monthly dry bulb temperature and dew point temperatures for these zones (Northern Hemisphere).
-
-![](media/image011.png)
-
-Figure 15. Monthly Dry Bulb Temperatures in K&ouml;ppen Climates (Northern Hemisphere)
-
-
-
-![](media/image012.png)
-
-Figure 16. Monthly Dew Point in K&ouml;ppen Climates (Northern Hemisphere)
-
-
-
-ASHRAE Climate Classification
-------------------------------------------------------------------------
-
-For the ASHRAE 90.1 and 90.2 standards (2004), a climate zone classification scheme was introduced, similar to the K&ouml;ppen classification. The methodology is described in two ASHRAE Transactions papers - Briggs - 2002.
-
-EnergyPlus Weather File (EPW) Data Dictionary
-----------------------------------------------------------
-
-The "data dictionary" for EnergyPlus Weather Data is shown below. Note that semi-colons do NOT terminate lines in the EnergyPlus Weather Data. It helps if you have familiarity with the IDD conventions please view them in the Input Output Reference document. Briefly, we have similar "\\" conventions that are important for reading the following tables:
-
-\\minimum, \\minimum&gt; - values for this field must be either &gt;= or &gt; than the following number
-
-\\maximum, \\maximum&lt; - values for this field must be either &lt;= or &lt; than the following number
-
-\\missing - if values in this field are &gt;= the following number, it is considered "missing" and missing data rules will apply
-
-\\default - blank fields will receive the following as "default" values
-
-\\units - expected units for the field. Standard EnergyPlus units are shown in the Input Output Reference Document.
-
-Note that in the header records where "date" is used, the interpretation is shown in the following table.
-
-Table 14. Weather File Date Field Interpretation
-
-<table class="table table-striped">
-<tr>
-<th>Field Contents</th>
-<th>Interpretation</th>
-<th>Header Applicability</th>
-</tr>
-<tr>
-<td>&lt;number&gt;</td>
-<td>Julian Day of Year</td>
-<td>All date fields</td>
-</tr>
-<tr>
-<td>&lt;number&gt; / &lt;number&gt;</td>
-<td>Month / Day</td>
-<td>All date fields</td>
-</tr>
-<tr>
-<td>&lt;number&gt; / &lt;number&gt; / &lt;number&gt;</td>
-<td>Month / Day / Year</td>
-<td>DataPeriod only - special multiple year file - ref: RunPeriod:CustomRange object in IDF / Input Output Reference document</td>
-</tr>
-<tr>
-<td>&lt;number&gt; Month</td>
-<td>Day and Month</td>
-<td>All date fields</td>
-</tr>
-<tr>
-<td>Month &lt;number&gt;</td>
-<td>Day and Month</td>
-<td>All date fields</td>
-</tr>
-<tr>
-<td>&lt;number&gt; Weekday in Month</td>
-<td>Numbered weekday of month</td>
-<td>Holiday, DaylightSavingPeriod</td>
-</tr>
-<tr>
-<td>Last Weekday In Month</td>
-<td>Last weekday of month</td>
-<td>Holiday, DaylightSavingPeriod</td>
-</tr>
-</table>
-
-In the table, Month can be one of (January, February, March, April, May, June, July, August, September, October, November, December). Abbreviations of the first three characters are also valid.
-
-In the table, Weekday can be one of (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday). Abbreviations of the first three characters are also valid.
-
-```idd
-!ESP(r)/EnergyPlus Weather Format
-!April 2002
-\memo Dates in the EPW file can be several formats:
-\memo <number>/<number>  (month/day)
-\memo <number> Month
-\memo Month <number>
-\memo <number> (taken to be Julian day of year)
-\memo Months are January, February, March, April, May,
-\memo            June, July, August, September, October, November, December
-\memo Months can be the first 3 letters of the month
-```
-
-```idd
-LOCATION,
-   A1, \field city
-   \type alpha
-   A2, \field State Province Region
-   \type alpha
-   A3, \field Country
-   \type alpha
-   A4, \field Source
-   \type alpha
-   N1, \field WMO
-    \note usually a 6 digit field. Used as alpha in EnergyPlus
-    \type alpha
-   N2 , \field Latitude
-       \units deg
-       \minimum -90.0
-       \maximum +90.0
-       \default 0.0
-       \note + is North, - is South, degree minutes represented in decimal (i.e. 30 minutes is .5)
-       \type real
-   N3 , \field Longitude
-       \units deg
-       \minimum -180.0
-       \maximum +180.0
-       \default 0.0
-       \note - is West, + is East, degree minutes represented in decimal (i.e. 30 minutes is .5)
-       \type real
-   N4 , \field TimeZone
-       \units hr - not on standard units list???
-       \minimum -12.0
-       \maximum +12.0
-       \default 0.0
-       \note  Time relative to GMT.
-       \type real
-   N5 ; \field Elevation
-       \units m
-       \minimum -1000.0
-       \maximum< +9999.9
-       \default 0.0
-       \type real
-```
-
-The Location header record duplicates the information required for the Location Object. When only a Run Period object is used (i.e. a weather file), then the Location Object Is not needed. When a Run Period and Design Day objects are entered, then the Location on the weather file (as described previously) is used and overrides any Location Object entry.
-
-```idd
-DESIGN CONDITIONS,
-     N1, \field Number of Design Conditions
-     A1, \field Design Condition Source
-         \note current sources are ASHRAE HOF 2009 US Design Conditions, Canadian Design Conditions
-         \note and World Design Conditions
-     A2, \field Design Condition Type (HEATING)
-       \note fields here will be dependent on the source, they are shown in a header/data format 
-       \note in both the .rpt and .csv files that are produced by the WeatherConverter program
-     ...
-     An, \field Design Condition Type (COOLING)
-       \note same as note on Heating Design Conditions
-```
-
-The Design Conditions header record encapsulates matching (using WMO\# -- World Meteorological Organization Station Number) design conditions for a weather file location. Currently only those design conditions contained in the ASHRAE Handbook of Fundamentals 2009 are contained in the weather files. These conditions can be used as desired. In addition, Design Day definition files have been created of all World, Canada, and United States Design Conditions. These files are available in the DataSet folder of the EnergyPlus installation.
-
-```idd
-TYPICAL/EXTREME PERIODS,
-     N1, \field Number of Typical/Extreme Periods
-     A1, \field Typical/Extreme Period 1 Name
-     A2, \field Typical/Extreme Period 1 Type
-     A3, \field Period 1 Start Day
-     A4, \field Period 1 End Day
-     \note repeat (A1-A3) until number of typical periods
- -- etc to # of periods entered
-```
-
-Using a heuristic method, the weather converter can determine typical and extreme weather periods for full year weather files. These will then be shown on the Typical/Extreme Periods header record. These are also reported in the statistical report output from the Weather Converter.
-
-```idd
-GROUND TEMPERATURES,
-       N1, Number of Ground Temperature Depths
-       N2, \field Ground Temperature Depth 1
-         \units m
-       N3, \field Depth 1 Soil Conductivity
-         \units W/m-K,
-       N4, \field Depth 1 Soil Density
-         \units kg/m3
-       N5, \field Depth 1 Soil Specific Heat
-         \units J/kg-K,
-       N6, \field Depth 1 January Average Ground Temperature
-        \units C
-       N7, \field Depth 1 February Average Ground Temperature
-        \units C
-       N8, \field Depth 1 March Average Ground Temperature
-        \units C
-       N9, \field Depth 1 April Average Ground Temperature
-        \units C
-       N10, \field Depth 1 May Average Ground Temperature
-        \units C
-       N11, \field Depth 1 June Average Ground Temperature
-        \units C
-       N12, \field Depth 1 July Average Ground Temperature
-        \units C
-       N13, \field Depth 1 August Average Ground Temperature
-        \units C
-       N14, \field Depth 1 September Average Ground Temperature
-        \units C
-       N15, \field Depth 1 October Average Ground Temperature
-        \units C
-       N16, \field Depth 1 November Average Ground Temperature
-        \units C
-       N17, \field Depth 1 December Average Ground Temperature
-        \units C
-      \note repeat above (N2-N17) to number of ground temp depths indicated
--- etc to # of depths entered
-```
-
-The weather converter program can use a full year weather data file to calculate "undisturbed" ground temperatures based on temperatures. Since an important part of soil heat transfer includes soil properties such as conductivity, density and specific heat AND these cannot be calculated from simple weather observations, this header record is provided primarilyfor user information. However, with the FC construction option, these are automatically selected (.5 depth) for use if the user does not include values in the Site:GroundTemperature:FcfactorMethod object.
-
-As noted in the statistics report, the "undisturbed" ground temperatures calculated by the weather converter should not be used in building losses but are appropriate to be used in the GroundTemperatures:Surface and GroundTemperatures:Deep objects. The reasoning (for building losses) is that these values are too extreme for the soil under a conditioned building. For best results, use the Slab or Basement program described in this document to calculate custom monthly average ground temperatures (see the Ground Heat Transfer section). This is especially important for residential applications and very small buildings. If one of these ground temperature preprocessors is not used, for typical commercial buildings in the USA, a reasonable default value is 2C less than the average indoor space temperature.
-
-```idd
-HOLIDAYS/DAYLIGHT SAVING,
-     A1, \field LeapYear Observed
-      \type choice
-      \key Yes
-      \key No
-      \note Yes if Leap Year will be observed for this file
-      \note No if Leap Year days (29 Feb) should be ignored in this file
-     A2, \field Daylight Saving Start Day
-     A3, \field Daylight Saving End Day
-     N1, \field Number of Holidays (essentially unlimited)
-     A4, \field Holiday 1 Name
-     A5, \field Holiday 1 Day
-     \note repeat above two fields until Number of Holidays is reached
--- etc to # of Holidays entered
-```
-
-The Holidays / Daylight Saving header record details the start and end dates of Daylight Saving Time and other special days such as might be recorded for the weather file. These can be used by keying "Yes" for appropriate fields in the Run Period Object.
-
-Note: EnergyPlus processed weather files available on the EnergyPlus web site:  have neither special days specified nor daylight saving period.
-
-For example, using a RunPeriod:
-
-```idf
-RunPeriod,
-    1,                       !- Begin Month
-    1,                       !- Begin Day Of Month
-    12,                      !- End Month
-    31,                      !- End Day Of Month
-    Wednesday,               !- Day Of Week For Start Day
-    Yes,                     !- Use WeatherFile Holidays/Special Days
-    No,                      !- Use WeatherFile DaylightSavingPeriod
-    Yes,                     !- Apply Weekend Holiday Rule
-    Yes,                     !- Use WeatherFile Rain Indicators
-    Yes;                     !- Use WeatherFile Snow Indicators
-```
-
-Will use any holidays specified in the Holidays / Daylight Saving header record of the weather file but will not use the Daylight Saving Period that is specified there (if any). In addition, the user can specify Special Day Periods via the Special Day Period object and/or Daylight Saving Period via the Daylight Saving Period object to additionally specify these items.
-
-```idd
-COMMENTS 1, A1 \field Comments_1
-COMMENTS 2, A1 \field Comments_2
-```
-
-The Comment header records may provide additional information about the weather data source or other information which may not fit in other header record formats.
-
-```idd
-DATA PERIODS,
-     N1, \field Number of Data Periods
-     N2, \field Number of Records per hour
-     A1, \field Data Period 1 Name/Description
-     A2, \field Data Period 1 Start Day of Week
-       \type choice
-       \key  Sunday
-       \key  Monday
-       \key  Tuesday
-       \key  Wednesday
-       \key  Thursday
-       \key  Friday
-       \key  Saturday
-     A3, \field Data Period 1 Start Day
-     A4, \field Data Period 1 End Day
-     \note repeat above to number of data periods
--- etc to # of periods entered
-```
-
-A weather file may contain several "data periods" though this is not required (and, in fact, may be detrimental). In addition, a weather file may contain multiple records per hour BUT these must match the Number of Time Steps In Hour for the simulation. Multiple interval data files can be valued when you want to be sure of the weather values for each time step (rather than relying on "interpolated" weather data). A weather file may also contain several consecutive years of weather data. EnergyPlus will automatically process the extra years when the Number of Years field is used in the RunPeriod object. Sorry - there is no way to jump into a year in the middle of the EPW file.
-
-
-
-Note that a Run Period object may not cross Data Period boundary lines.
-
-For those interested in creating their own weather data in the CSV or EPW formats or reading the .csv and .epw files that are produced by the Weather Converter program, the fields are shown in the following "IDD" description. Items shown in bold are used directly in the EnergyPlus program.
-
-```idd
-! Actual data does not have a descriptor
-     N1, \field Year
-     N2, \field Month
-     N3, \field Day
-     N4, \field Hour
-     N5, \field Minute
-     A1, \field Data Source and Uncertainty Flags
-     \note Initial day of weather file is checked by EnergyPlus for validity (as shown below)
-     \note Each field is checked for "missing" as shown below. Reasonable values, calculated
-     \note values or the last "good" value is substituted.
-     N6, \field Dry Bulb Temperature
-        \units C
-        \minimum> -70
-        \maximum< 70
-        \missing 99.9
-     N7, \field Dew Point Temperature
-        \units C
-        \minimum> -70
-        \maximum< 70
-        \missing 99.9
-     N8, \field Relative Humidity
-         \missing 999.
-         \minimum 0
-         \maximum 110
-     N9, \field Atmospheric Station Pressure
-        \units Pa
-        \missing 999999.
-        \minimum> 31000
-        \maximum< 120000
-     N10, \field Extraterrestrial Horizontal Radiation
-        \units Wh/m2
-        \missing 9999.
-        \minimum 0
-     N11, \field Extraterrestrial Direct Normal Radiation
-        \units Wh/m2
-        \missing 9999.
-        \minimum 0
-     N12, \field Horizontal Infrared Radiation Intensity
-        \units Wh/m2
-        \missing 9999.
-        \minimum 0
-     N13, \field Global Horizontal Radiation
-        \units Wh/m2
-        \missing 9999.
-        \minimum 0
-     N14, \field Direct Normal Radiation
-        \units Wh/m2
-        \missing 9999.
-        \minimum 0
-     N15, \field Diffuse Horizontal Radiation
-        \units Wh/m2
-        \missing 9999.
-        \minimum 0
-     N16, \field Global Horizontal Illuminance
-        \units lux
-        \missing 999999.
-        \note will be missing if >= 999900
-        \minimum 0
-     N17, \field Direct Normal Illuminance
-        \units lux
-        \missing 999999.
-        \note will be missing if >= 999900
-        \minimum 0
-     N18, \field Diffuse Horizontal Illuminance
-        \units lux
-        \missing 999999.
-        \note will be missing if >= 999900
-        \minimum 0
-     N19, \field Zenith Luminance
-        \units Cd/m2
-        \missing 9999.
-        \note will be missing if >= 9999
-        \minimum 0
-     N20, \field Wind Direction
-        \units degrees
-        \missing 999.
-        \minimum 0
-        \maximum 360
-     N21, \field Wind Speed
-        \units m/s
-        \missing 999.
-        \minimum 0
-        \maximum 40
-     N22, \field Total Sky Cover
-        \missing 99
-        \minimum 0
-        \maximum 10
-     N23, \field Opaque Sky Cover (used if Horizontal IR Intensity missing)
-        \missing 99
-        \minimum 0
-        \maximum 10
-     N24, \field Visibility
-        \units km
-        \missing 9999
-     N25, \field Ceiling Height
-        \units m
-        \missing 99999
-     N26, \field Present Weather Observation
-     N27, \field Present Weather Codes
-     N28, \field Precipitable Water
-        \units mm
-        \missing 999
-     N29, \field Aerosol Optical Depth
-        \units thousandths
-        \missing .999
-     N30, \field Snow Depth
-        \units cm
-        \missing 999
-     N31, \field Days Since Last Snowfall
-        \missing 99
-     N32, \field Albedo
-        \missing 999
-     N33, \field Liquid Precipitation Depth
-          \units mm
-        \missing 999
-     N34; \field Liquid Precipitation Quantity
-          \units hr
-        \missing 99
-```
-
-### Data Field Descriptions
-
-Descriptions of the fields are taken from the IWEC manual - as descriptive of what should be contained in the data fields.
-
-#### Field: Year
-
-This is the Year of the data. Not really used in EnergyPlus. Used in the Weather Converter program for display in audit file.
-
-#### Field: Month
-
-This is the month (1-12) for the data. Cannot be missing.
-
-#### Field: Day
-
-This is the day (dependent on month) for the data. Cannot be missing.
-
-#### Field: Hour
-
-This is the hour of the data. (1 - 24). Hour 1 is 00:01 to 01:00. Cannot be missing.
-
-#### Field: Minute
-
-This is the minute field. (1..60)
-
-#### Field: Data Source and Uncertainty Flags
-
-The data source and uncertainty flags from various formats (usually shown with each field) are consolidated in the E/E+ EPW format. More is shown about Data Source and Uncertainty in Data Sources/Uncertainty section later in this document.
-
-#### Field: Dry Bulb Temperature
-
-This is the dry bulb temperature in C at the time indicated. Note that this is a full numeric field (i.e. 23.6) and not an integer representation with tenths. Valid values range from -70&deg;C to 70&deg;C. Missing value for this field is 99.9.
-
-#### Field: Dew Point Temperature
-
-This is the dew point temperature in C at the time indicated. Note that this is a full numeric field (i.e. 23.6) and not an integer representation with tenths. Valid values range from -70&deg;C to 70&deg;C. Missing value for this field is 99.9.
-
-#### Field: Relative Humidity
-
-This is the Relative Humidity in percent at the time indicated. Valid values range from 0% to 110%. Missing value for this field is 999.
-
-#### Field: Atmospheric Station Pressure
-
-This is the station pressure in Pa at the time indicated. Valid values range from 31,000 to 120,000. (These values were chosen from the standard barometric pressure for all elevations of the World). Missing value for this field is 999999.
-
-#### Field: Extraterrestrial Horizontal Radiation
-
-This is the Extraterrestrial Horizontal Radiation in Wh/m2. It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 9999.
-
-#### Field: Extraterrestrial Direct Normal Radiation
-
-This is the Extraterrestrial Direct Normal Radiation in Wh/m2. (Amount of solar radiation in Wh/m2 received on a surface normal to the rays of the sun at the top of the atmosphere during the number of minutes preceding the time indicated). It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 9999.
-
-#### Field: Horizontal Infrared Radiation Intensity
-
-This is the Horizontal Infrared Radiation Intensity in Wh/m2. If it is missing, it is calculated from the Opaque Sky Cover field as shown in the following explanation. It should have a minimum value of 0; missing value for this field is 9999.
-
-<div>\[Horizontal_{IR} = \epsilon\sigma T^4_{drybulb}\]</div>
-
-where
-
-* <span>\(Horizontal_{IR}\)</span> is the horizontal IR intensity {W/m<sup>2</sup>}
-* <span>\(\epsilon\)</span> is the sky emissivity
-* <span>\(\sigma\)</span> is the Stefan-Boltzmann constant = 5.6697e-8 W/m<sup>2</sup>-K<sup>4</sup>
-* <span>\(T_{drybulb}\)</span> is the drybulb temperature {K}
-
-The sky emissivity is given by
-
-<div>\[ \epsilon = \left( 0.787 +0.764 \ln\left(\frac{T_{dewpoint}}{273}\right)\right)\left( 1 + 0.0224N + 0.0035N^2 + 0.00028N^3 \right)\]</div>
-
-where
-
-* <span>\(T_{dewpoint}\)</span> is the dewpoint temperature {K}
-* <span>\(N\)</span> is the opaque sky cover {tenths}
-
-Example: Clear sky (<span>\(N=0\)</span>), <span>\(T_{drybulb} = 273+20=293 K\)</span>, <span>\(T_{dewpoint} = 273+10=283 K\)</span>:
-
-<span>\(\epsilon = 0.787 + 0.764*0.036 = 0.815\)</span>
-
-<span>\(Horizontal_{IR} = 0.815*5.6697e-8*(293^4) = 340.6 W/m^2\)</span>
-
-References (Walton, 1983) (Clark, Allen, 1978) for these calculations are contained in the references section at the end of this list of fields.
-
-#### Field: Global Horizontal Radiation
-
-This is the Global Horizontal Radiation in Wh/m2. (Total amount of direct and diffuse solar radiation in Wh/m2 received on a horizontal surface during the number of minutes preceding the time indicated.) It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 9999.
-
-#### Field: Direct Normal Radiation
-
-This is the Direct Normal Radiation in Wh/m2. (Amount of solar radiation in Wh/m2 received directly from the solar disk on a surface perpendicular to the sun's rays, during the number of minutes preceding the time indicated.)  If the field is missing (<span>\(\ge 9999\)</span>) or invalid (<span>\(<0\)</span>), it is set to 0. Counts of such missing values are totaled and presented at the end of the runperiod.
-
-#### Field: Diffuse Horizontal Radiation
-
-This is the Diffuse Horizontal Radiation in Wh/m2. (Amount of solar radiation in Wh/m2 received from the sky (excluding the solar disk) on a horizontal surface during the number of minutes preceding the time indicated.) If the field is missing (<span>\(\ge 9999\)</span>) or invalid (<span>\(<0\)</span>), it is set to 0. Counts of such missing values are totaled and presented at the end of the runperiod.
-
-#### Field: Global Horizontal Illuminance
-
-This is the Global Horizontal Illuminance in lux. (Average total amount of direct and diffuse illuminance in hundreds of lux received on a horizontal surface during the number of minutes preceding the time indicated.) It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 999999 and will be considered missing if greater than or equal to 999900.
-
-#### Field: Direct Normal Illuminance
-
-This is the Direct Normal Illuminance in lux. (Average amount of illuminance in hundreds of lux received directly from the solar disk on a surface perpendicular to the sun's rays, during the number of minutes preceding the time indicated.)  It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 999999 and will be considered missing if greater than or equal to 999900.
-
-#### Field: Diffuse Horizontal Illuminance
-
-This is the Diffuse Horizontal Illuminance in lux. (Average amount of illuminance in hundreds of lux received from the sky (excluding the solar disk) on a horizontal surface during the number of minutes preceding the time indicated.)  It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 999999 and will be considered missing if greater than or equal to 999900.
-
-#### Field: Zenith Luminance
-
-This is the Zenith Illuminance in Cd/m2. (Average amount of luminance at the sky's zenith in tens of Cd/m2 during the number of minutes preceding the time indicated.) It is not currently used in EnergyPlus calculations. It should have a minimum value of 0; missing value for this field is 9999.
-
-#### Field: Wind Direction
-
-This is the Wind Direction in degrees where the convention is that North=0.0, East=90.0, South=180.0, West=270.0. (Wind direction in degrees at the time indicated. If calm, direction equals zero.) Values can range from 0 to 360. Missing value is 999.
-
-#### Field: Wind Speed
-
-This is the wind speed in m/sec. (Wind speed at time indicated.) Values can range from 0 to 40. Missing value is 999.
-
-#### Field: Total Sky Cover
-
-This is the value for total sky cover (tenths of coverage). (i.e. 1 is 1/10 covered. 10 is total coverage). (Amount of sky dome in tenths covered by clouds or obscuring phenomena at the hour indicated at the time indicated.) Minimum value is 0; maximum value is 10; missing value is 99.
-
-#### Field: Opaque Sky Cover
-
-This is the value for opaque sky cover (tenths of coverage). (i.e. 1 is 1/10 covered. 10 is total coverage). (Amount of sky dome in tenths covered by clouds or obscuring phenomena that prevent observing the sky or higher cloud layers at the time indicated.)  This is not used unless the field for Horizontal Infrared Radiation Intensity is missing and then it is used to calculate Horizontal Infrared Radiation Intensity. Minimum value is 0; maximum value is 10; missing value is 99.
-
-#### Field: Visibility
-
-This is the value for visibility in km. (Horizontal visibility at the time indicated.)  It is not currently used in EnergyPlus calculations. Missing value is 9999.
-
-#### Field: Ceiling Height
-
-This is the value for ceiling height in m. (77777 is unlimited ceiling height. 88888 is cirroform ceiling.) It is not currently used in EnergyPlus calculations. Missing value is 99999.
-
-#### Field: Present Weather Observation
-
-If the value of the field is 0, then the observed weather codes are taken from the following field. If the value of the field is 9, then "missing" weather is assumed. Since the primary use of these fields (Present Weather Observation and Present Weather Codes) is for rain/wet surfaces, a missing observation field or a missing weather code implies no rain.
-
-Table 15. Present Weather Observation Values
-
-<table class="table table-striped">
-<tr>
-<th>Element</th>
-<th>Values</th>
-<th>Definition</th>
-</tr>
-<tr>
-<td>Observation Indicator</td>
-<td>0 or 9</td>
-<td>0 = Weather observation made; 9 = Weather observation not made, or missing</td>
-</tr>
-</table>
-
-
-
-#### Field: Present Weather Codes
-
-The present weather codes field is assumed to follow the TMY2 conventions for this field. Note that though this field may be represented as numeric (e.g. in the CSV format), it is really a text field of 9 single digits. This convention along with values for each "column" (left to right) is presented in Table 16. Note that some formats (e.g. TMY) does not follow this convention - as much as possible, the present weather codes are converted to this convention during WeatherConverter processing. Also note that the most important fields are those representing liquid precipitation - where the surfaces of the building would be wet. EnergyPlus uses "Snow Depth" to determine if snow is on the ground.
-
-Table 16. Weather Codes Field Interpretation
-<table class="table table-striped">
-  <tr>
-    <th>Column - Poisition in Field</th>
-    <th>Element Description</th>
-    <th>Possible Values</th>
-    <th>Definition</th>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td>Occurrence ofThunderstorm,Tornado, orSquall</td>
-    <td>0 - 2, 4, 6- 9</td>
-    <td>
-    0 = Thunderstorm-lightning and thunder. Wind gusts less than 25.7 m/s, and hail, if any, less than 1.9 cm diameter <BR>
-    1 = Heavy or severe thunderstorm-frequent intense lightning and thunder. Wind gusts greater than 25.7 m/s and hail, if any, 1.9 cm or greater diameter <BR>
-    2 = Report of tornado or waterspout <BR>
-    4 = Moderate squall-sudden increase of windspeed by at least 8.2 m/s, reaching 11.3 m/s or more and lasting for at least 1 minute <BR>
-    6 = Water spout (beginning January 1984) <BR>
-    7 = Funnel cloud (beginning January 1984) <BR>
-    8 = Tornado (beginning January 1984) <BR>
-    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9
-    </td>
-  </tr>
-  <tr>
-    <td>2</td>
-    <td>Occurrence ofRain, RainShowers, orFreezing Rain</td>
-    <td>0 - 9</td>
-    <td>
-    0 = Light rain <BR>
-    1 = Moderate rain <BR>
-    2 = Heavy rain <BR>
-    3 = Light rain showers <BR>
-    4 = Moderate rain showers <BR>
-    5 = Heavy rain showers <BR>
-    6 = Light freezing rain <BR>
-    7 = Moderate freezing rain <BR>
-    8 = Heavy freezing rain <BR>
-    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9  <BR>
-    Notes: <BR>
-    Light = up to 0.25 cm per hour  <BR>
-    Moderate = 0.28to 0.76 cm per hour  <BR>
-    Heavy = greater than 0.76cm per hour <BR>
-    </td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>Occurrence ofRain Squalls,Drizzle, orFreezing Drizzle</td>
-    <td>0, 1, 3-9</td>
-    <td>
-    0 = Light rain squalls <BR>
-    1 = Moderate rain squalls <BR>
-    3 = Light drizzle <BR>
-    4 = Moderate drizzle <BR>
-    5 = Heavy drizzle <BR>
-    6 = Light freezing drizzle <BR>
-    7 = Moderate freezing drizzle <BR>
-    8 = Heavy freezing drizzle <BR>
-    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9 <BR>
-    Notes: When drizzle or freezing drizzle occurswith other weather phenomena: Light = up to0.025 cm per hour Moderate = 0.025 to 0.051cm per hour Heavy = greater than 0.051 cmper hour When drizzle or freezing drizzle occurs alone:  <BR>
-    Light = visibility 1 km or greater  <BR>
-    Moderate =visibility between 0.5 and 1 km  <BR>
-    Heavy =visibility 0.5 km or less <BR>
-    </td>
-  </tr>
-  <tr>
-    <td>4</td>
-    <td>Occurrence ofSnow, SnowPellets, or IceCrystals</td>
-    <td>0 - 9</td>
-    <td>
-    0 = Light snow <BR>
-    1 = Moderate snow <BR>
-    2 = Heavy snow <BR>
-    3 = Light snow pellets <BR>
-    4 = Moderate snow pellets <BR>
-    5 = Heavy snow pellets <BR>
-    6 = Light ice crystals <BR>
-    7 = Moderate ice crystals <BR>
-    8 = Heavy ice crystals <BR>
-    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9  <BR>
-    Notes:Beginning in April 1963, any occurrence of icecrystals is recorded as a 7. <BR>
-    </td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>Occurrence ofSnow Showers,Snow Squalls, orSnow Grains</td>
-    <td>0 - 7, 9</td>
-    <td>
-    0 = Light snow <BR>
-    1 = Moderate snow showers <BR>
-    2 = Heavy snow showers <BR>
-    3 = Light snow squall <BR>
-    4 = Moderate snow squall <BR>
-    5 = Heavy snow squall <BR>
-    6 = Light snow grains <BR>
-    7 = Moderate snow grains <BR>
-    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9 <BR>
-    </td>
-  </tr>
-  <tr>
-    <td>6</td>
-    <td>Occurrence ofSleet, SleetShowers, or Hail</td>
-    <td>0 - 2, 4, 9</td>
-    <td>
-    0 = Light ice pellet showers <BR>
-    1 = Moderate ice pellet showers <BR>
-    2 = Heavy ice pellet showers <BR>
-    4 = Hail <BR>
-    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9 <BR>
-    Notes: Prior to April 1970, ice pellets werecoded as sleet. Beginning in April 1970, sleetand small hail were redefined as ice pellets andare coded as 0, 1, or 2.
-    </td>
-  </tr>
-  <tr>
-    <td>7</td>
-    <td>Occurrence ofFog, BlowingDust, or Blowing Sand</td>
-    <td>0 - 9</td>
-    <td>
-    0 = Fog <BR>
-    1 = Ice fog <BR>
-    2 = Ground fog <BR>
-    3 = Blowing dust <BR>
-    4 = Blowing sand <BR>
-    5 = Heavy fog <BR>
-    6 = Glaze (beginning 1984) <BR>
-    7 = Heavy ice fog (beginning 1984) <BR>
-    8 = Heavy ground fog (beginning 1984) <BR>
-    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9 <BR>
-    Notes:These values recorded only when visibility isless than 11 km.
-    </td>
-  </tr>
-  <tr>
-    <td>8</td>
-    <td>Occurrence ofSmoke, Haze,Smoke andHaze, BlowingSnow, BlowingSpray, or Dust</td>
-    <td>0 - 7, 9</td>
-    <td>
-    0 = Smoke <BR>
-    1 = Haze <BR>
-    2 = Smoke and haze <BR>
-    3 = Dust <BR>
-    4 = Blowing snow <BR>
-    5 = Blowing spray <BR>
-    6 = Dust storm (beginning 1984) <BR>
-    7 = Volcanic ash <BR>
-    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9 <BR>
-    Notes: These values recorded only when visibility is less than 11 km.
-    </td>
-  </tr>
-  <tr>
-    <td>9</td>
-    <td>Occurrence ofIce Pellets</td>
-    <td>0 - 2, 9</td>
-    <td>
-    0 = Light ice pellets <BR>
-    1 = Moderate ice pellets <BR>
-    2 = Heavy ice pellets <BR>
-    9 = None if Observation Indicator element equals 0, or else unknown or missing if Observation Indicator element equals 9
-    </td>
-  </tr>
-</table>
-
-
-For example, a Present Weather Observation (previous field) of 0 and a Present Weather Codes field of 929999999 notes that there is heavy rain for this data period (usually hourly but depends on the number of intervals per hour field in the "Data Periods" record).
-
-#### Field: Precipitable Water
-
-This is the value for Precipitable Water in mm. (This is not rain - rain is inferred from the PresWeathObs field but a better result is from the Liquid Precipitation Depth field)). It is not currently used in EnergyPlus calculations (primarily due to the unreliability of the reporting of this value). Missing value is 999.
-
-#### Field: Aerosol Optical Depth
-
-This is the value for Aerosol Optical Depth in thousandths. It is not currently used in EnergyPlus calculations. Missing value is .999.
-
-#### Field: Snow Depth
-
-This is the value for Snow Depth in cm. This field is used to tell when snow is on the ground and, thus, the ground reflectance may change. Missing value is 999.
-
-#### Field: Days Since Last Snowfall
-
-This is the value for Days Since Last Snowfall. It is not currently used in EnergyPlus calculations. Missing value is 99.
-
-#### Field: Albedo
-
-The ratio (unitless) of reflected solar irradiance to global horizontal irradiance. It is not currently used in EnergyPlus.
-
-#### Field: Liquid Precipitation Depth
-
-The amount of liquid precipitation (mm) observed at the indicated time for the period indicated in the liquid precipitation quantity field. If this value is not missing, then it is used and overrides the "precipitation" flag as rainfall.  Conversely, if the precipitation flag shows rain and this field is missing or zero, it is set to 1.5 (mm).
-
-#### Field: Liquid Precipitation Quantity
-
-The period of accumulation (hr) for the liquid precipitation depth field. It is not currently used in EnergyPlus.
-
-### References
-
-Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards, p. 21.
-
-Clark, G. and C. Allen, "The Estimation of Atmospheric Radiation for Clear and Cloudy Skies," Proceedings 2nd National Passive Solar Conference (AS/ISES), 1978, pp. 675-678.
-
-EPW CSV Format (In/Out)
------------------------
-
-EPW CSV Format to the Weather Converter is a special CSV format which echoes the format of the EPW file.  For the "header" records in the CSV file, they are basically the same as the header records for the EPW file (see above). However, in the CSV file, each header is shown and then the data. Partial year files will not have all of these headers "filled" in. Also see Figure 17. EnergyPlus EPW CSV file (spreadsheet view) and Figure 18. EnergyPlus EPW CSV Data Records (spreadsheet view) for snapshot pictures of the EnergyPlus EPW CSV file as shown in a spreadsheet.
-
-### Location Header/Data (CSV)
-
-Location Title,Latitude {N+/S-},Longitude {E+/W-},TimeZone {+/- GMT},Elevation {m}
-
-LOCATION\_SYDNEY\_\_AUS\_IWEC Data\_947670,-33.95,151.18,10.0,3.0
-
-LOCATION + the city, state/province, country and WMO fields from the EPW file are concatenated to form the "Location Title". The latitude, longitude, time zone and elevation fields are numeric.
-
-### Design Conditions Header/Data (CSV)
-
-If there are design conditions, then the format is as follows:
-
-Number of Design Conditions,Title of Design Condition,Design Stat,HDB 99.6%,HDB 99%,X WS 1%,X WS 2.5%,X WS 5%,CM WS .4%,CM MDB .4%,CM WS 1%,CM MDB 1%,MWS 99.6%,PWD 99.6%,MWS .4%,PWD .4%,X MnDB Max,X MnDB Min,X StdDB Max,X StdDB Min,Design Stat,CDB .4%,C MWB .4%,CDB 1%,C MWB 1%,CDB 2%,C MWB 2%,E WB .4%,E MDB .4%,E WB 1%,E MDB 1%,E WB 2%,E MDB 2%,DP .4%,HR .4%,MDB .4%,DP 1%,HR 1%,MDB 1%,DP 2%,HR 2%,MDB 2%,DB Range
-
-,,Units,{°C},{°C},{m/s},{m/s},{m/s},{m/s},{°C},{m/s},{°C},{m/s},{Degree},{m/s},{Degree},{°C},{°C},{°C},{°C},Units,{°C},{°C},{°C},{°C},{°C},{°C},{°C},{°C},{°C},{°C},{°C},{°C},{°C},{g/kg},{°C},{°C},{g/kg},{°C},{°C},{g/kg},{°C},{°C}
-
-1,World Climate Design Data 2001 ASHRAE Handbook,HEATING,5.8,6.8,11.3,9.9,8.8,11.1,14.2,9.1,13.4,1.1,320,5.3,300,39.3,3.1,2.9,1.9,COOLING,32.2,20,29.5,19.7,27.9,20.1,23,28,22.3,26.2,21.7,25.3,21.7,16.4,24.8,21.1,15.8,24.3,20.6,15.3,23.9,6.7
-
-However, if there are no design conditions, then the format looks like:
-
-Number of Design Conditions,Title of Design Condition,
-
-0
-
-Theoretically, there can be more than one design condition included.
-
-### Typical/Extreme Periods Header/Data (CSV)
-
-The results from the typical / extreme period heuristic calculation are shown.
-
-Number of Typical/Extreme Periods,Period Name,Period Type,Period Start Day,Period End Day,&lt;repeat to \# periods&gt;
-
-6,Summer - Week Nearest Max Temperature For Period,Extreme,1/ 4,1/10,Summer - Week Nearest Average Temperature For Period,Typical,11/29,12/ 5,Winter - Week Nearest Min Temperature For Period,Extreme,7/ 3,7/ 9,Winter - Week Nearest Average Temperature For Period,Typical,6/ 5,6/11,Autumn - Week Nearest Average Temperature For Period,Typical,3/22,3/28,Spring - Week Nearest Average Temperature For Period,Typical,8/ 1,8/ 7
-
-### Ground Temperatures Header/Data (CSV)
-
-The results from the ground temperature heuristic calculation are shown, typically for 3 depths. Users may also fill in the blank fields (soil conductivity, soil density, soil specific heat) with known values and/or perform their own calculations and depths and supply those. These should be considered "undisturbed" ground temperatures - temperatures of soil that have not been disturbed by construction. They are not considered appropriate for calculations of building losses.
-
-The program uses a heuristic, time lagged calculation based on dry bulb temperature and location. References on the topic are found in Kusuda (see references).
-
-Number of Ground Temperature Depths,Ground Temperature Depth {m},Soil Conductivity {W/m-K},Soil Density {kg/m3},Soil Specific Heat {J/kg-K},Jan {C},Feb{C},Mar {C},Apr {C},May {C},Jun {C},Jul {C},Aug {C},Sep {C},Oct {C},Nov {C},Dec {C},&lt;repeat to Number of temperature depths&gt;
-
-3,.5,,,,20.69,22.30,22.69,22.26,19.95,17.43,15.09,13.43,12.99,13.86,15.84,18.29,2,,,,19.18,20.71,21.41,21.40,20.16,18.43,16.58,15.03,14.25,14.45,15.59,17.28,4,,,,18.18,19.38,20.10,20.30,19.82,18.80,17.56,16.35,15.56,15.39,15.89,16.89
-
-### Holiday/Daylight Saving Header/Data (CSV)
-
-If these data are entered, the weather converter will process them. Default weather processing contains no holidays or daylight saving period. Of course, these can also be specified in your input data file for EnergyPlus and do not need to be embedded in the weather file.
-
-Leap Year Observed?,Daylight Saving Start Date,Daylight Saving End Date,Number of Holidays,Holiday Name,Holiday Date,&lt;repeat for \# Holidays&gt;
-
-No,0,0,0
-
-### Comment 1 Header/Data (CSV)
-
-Some original data files fill the comment 1 header and some do not. Typically, it will display at least a "station" number and potentially more information.
-
-Comment Line \#1
-
-"IWEC- WMO\#947670 - South-west Pacific -- Original Source Data (c) 2001 American Society of Heating, Refrigerating and Air-Conditioning Engineers (ASHRAE), Inc., Atlanta, GA, USA. www.ashrae.org  All rights reserved as noted in the License Agreement and Additional Conditions. DISCLAIMER OF WARRANTIES: The data is provided 'as is' without warranty of any kind, either expressed or implied. The entire risk as to the quality and performance of the data is with you. In no event will ASHRAE or its contractors be liable to you for any damages, including without limitation any lost profits, lost savings, or other incidental or consequential damages arising out of the use or inability to use this data."
-
-### Comment 2 Header/Data (CSV)
-
-Comment Line \#2
-
- -- Ground temps produced with a standard soil diffusivity of 2.3225760E-03 {m\*\*2/day}
-
-### Data Period Header/Data (CSV)
-
-Number of Data Periods [DP],Number of Intervals per Hour,DP Name/Description,DP Start Day of Week,DP Start Day, DP End Day,&lt;repeat to \# Data Periods&gt;
-
-1,1,Data,Sunday, 1/ 1,12/31
-
-### Data Records (CSV)
-
-The field "names" for each item are shown. First, the "short" names:
-
-Date,HH:MM,Datasource,DryBulb {C},DewPoint {C},RelHum {%},Atmos Pressure {Pa},ExtHorzRad {Wh/m2},ExtDirRad {Wh/m2},HorzIRSky {Wh/m2},GloHorzRad {Wh/m2},DirNormRad {Wh/m2},DifHorzRad {Wh/m2},GloHorzIllum {lux},DirNormIllum {lux},DifHorzIllum {lux},ZenLum {Cd/m2},WindDir {deg},WindSpd {m/s},TotSkyCvr {.1},OpaqSkyCvr {.1},Visibility {km},Ceiling Hgt {m},PresWeathObs,PresWeathCodes,Precip Wtr {mm},Aerosol Opt Depth {.001},SnowDepth {cm},Days Last Snow,Albedo {.01},Rain {mm},Rain Quantity {hr}
-
-Then, the longer names:
-
-Date,HH:MM,Datasource,Dry Bulb Temperature {C},Dew Point Temperature {C},Relative Humidity {%},Atmospheric Pressure {Pa},Extraterrestrial Horizontal Radiation {Wh/m2},Extraterrestrial Direct Normal Radiation {Wh/m2},Horizontal Infrared Radiation Intensity from Sky {Wh/m2},Global Horizontal Radiation {Wh/m2},Direct Normal Radiation {Wh/m2},Diffuse Horizontal Radiation {Wh/m2},Global Horizontal Illuminance {lux},Direct Normal Illuminance {lux},Diffuse Horizontal Illuminance {lux},Zenith Luminance {Cd/m2},Wind Direction {deg},Wind Speed {m/s},Total Sky Cover {.1},Opaque Sky Cover {.1},Visibility {km},Ceiling Height {m},Present Weather Observation,Present Weather Codes,Precipitable Water {mm},Aerosol Optical Depth {.001},Snow Depth {cm},Days Since Last Snow,Albedo {.01},Liquid Precipitation Depth {mm},Liquid Precipitation Quantity {hr}
-
-As noted previously, these headers and data are in the identical order to the items in the EPW records. Then the data is shown:
-
-1983/1/1,01:00,C9C9C9C9\*0?9?9?9?9?9?9?9\*0C8C8C8C8\*0\*0E8\*0\*0,26.2,19.2,65,101100,0,1415,412,0,0,0,0,0,0,0,180,6.5,9,7,23.3,77777,9,'999999999,0,0.2300,0,88
-
-The Date and Time fields need a bit of description. The Date field (e.g. 1983/1/1) uses your standard system date for formatting. In the EPW file, these are three separate fields (year, month, and day in this example). The time field combines the hours and minutes into one field (hh:mm). This makes it easier for graphing with spreadsheet programs but a bit harder if you use the CSV format as input.
-
-Each data item field obeys the same "missing" and other content rules as shown above in the EnergyPlus Weather File (EPW) Data Dictionary.
-
-![](media/image015.png)
-
-Figure 17. EnergyPlus EPW CSV file (spreadsheet view)
-
-The figure above shows how the EnergyPlus EPW CSV file (initial header records) looks when opened in a spreadsheet.  Each header record is shown in bold with data following the headers..
-
-![](media/image016.png)
-
-Figure 18. EnergyPlus EPW CSV Data Records (spreadsheet view)
-
-The above figure shows how the data periods header record and the individual data records look when opened in a spread sheet. Again, the headers are shown in bold.  Note that there are two header records for the data records - one with short names - one with longer more descriptive names.
-
-Missing Weather File Data
--------------------------
-
-The following data contains "missing" descriptors; a new concept not introduced previously in our IDD conventions. In this case, it will be processed as though those values are "missing" in the weather conversions. This may not always be desirable though the weather processor will fill in "missing" value with something "appropriate". Eventually, these missing values will be available through the weather processor. Until then, the following are used for initial missing conditions. When a valid value is encountered from weather data, however, it will become the new "missing" replacement value:
-
-Table 17. Missing weather replacement values
-
-<table class="table table-striped">
-<tr>
-<th>Data item</th>
-<th>Supplied Value</th>
-<th>Units</th>
-</tr>
-<tr>
-<td>Dry Bulb Temperature</td>
-<td>6</td>
-<td>C</td>
-</tr>
-<tr>
-<td>Dew Point Temperature</td>
-<td>3</td>
-<td>C</td>
-</tr>
-<tr>
-<td>Relative Humidity</td>
-<td>50</td>
-<td>%</td>
-</tr>
-<tr>
-<td>Atmospheric Pressure</td>
-<td>Standard** Barometric Pressure (altitude based)</td>
-<td>Pa</td>
-</tr>
-<tr>
-<td>Wind Speed</td>
-<td>2.5</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>Wind Direction</td>
-<td>180</td>
-<td>Deg</td>
-</tr>
-<tr>
-<td>Total Sky Cover</td>
-<td>5</td>
-<td>(tenths)</td>
-</tr>
-<tr>
-<td>Opaque Sky Cover</td>
-<td>5</td>
-<td>(tenths)</td>
-</tr>
-<tr>
-<td>Visibility</td>
-<td>777.7</td>
-<td>Km</td>
-</tr>
-<tr>
-<td>Ceiling Height</td>
-<td>77777</td>
-<td>m</td>
-</tr>
-<tr>
-<td>Precipitable Water</td>
-<td>0</td>
-<td>Mm</td>
-</tr>
-<tr>
-<td>Aerosol Optical Depth</td>
-<td>0</td>
-<td>Broadband turbidity</td>
-</tr>
-<tr>
-<td>Snow Depth</td>
-<td>0</td>
-<td>Cm</td>
-</tr>
-<tr>
-<td>Days Since Last Snow</td>
-<td>88</td>
-<td>Days</td>
-</tr>
-<tr>
-<td>Radiation Values (Direct/Diffuse)</td>
-<td>0.0</td>
-<td>Wh/m2</td>
-</tr>
-<tr>
-<td>Illuminance Values</td>
-<td>0.0</td>
-<td>lux (or CD/m2)</td>
-</tr>
-</table>
-
-\*\*Standard Barometric pressure based on location elevation is taken from ASHRAE 2001 Handbook of Fundamentals, pages 6.1 & 6.2.
-
-Source Weather Data Formats
----------------------------
-
-Source weather data for building energy simulation programs can be broken into two major classes: *historical data* and *typical weather years*. Historical data is just "real" data: usually measured (but sometimes modeled) data from a particular location for a given period of record. Typical years are ersatz years assembled to match the long term data from a particular location using a particular statistical measure. Typical data may also be "real" data but may not be a contiguous year - the data may be comprised of months from multiple years.
-
-The primary source for historical weather data is the U.S. National Climatic Data Center (NCDC) in Asheville, NC: http://www.ncdc.noaa.gov/. NCDC can provide hourly historical data for thousands of locations around the world. This data may not always be complete; data items or periods of record may be missing.
-
-### Data Set vs. Data Format
-
-In this document as well in many others, you will read about a certain "data set" and you will also read about data in a "certain" format - e.g., the TMY2 data set and the TMY2 data format. Simply stated, a data set refers to a set of data files developed around a set of procedures for selection and usually with a specific purpose for use. A data format is merely the identification of data elements in a data file. In the TMY2 example, the TMY2 data set was developed as described below and the format of the data is usually called a TMY2 format.
-
-Any data *could* be put into a TMY2 format, but it wouldn't necessarily be selected using the same procedures as the TMY2 data set.
-
-### SAMSON Data Set/Format
-
-A highly reliable source of historical data for U.S. locations is the Solar and Meteorological Surface Observational Network (SAMSON) data set assembled by the National Renewable Energy Laboratory (NREL) in Golden, CO: http://www.nrel.gov/. The SAMSON data set contains a 30 year (1961 to 1990) period of record for 239 locations and are available from the NCDC.
-
-SAMSON also describes a file format. Though no data from the SAMSON data set are available for download in EPW format, the weather conversion utility can read and process this file format.
-
-### TMY2 Data Set/Format
-
-The TMY2 are data sets of hourly values of solar radiation and meteorological elements for a 1-year period. Their intended use is for computer simulations of solar energy conversion systems and building systems to facilitate performance comparisons of different system types, configurations, and locations in the United States and its territories. Because they represent typical rather than extreme conditions, they are not suited for designing systems to meet the worst-case conditions occurring at a location. The data are available from the National Renewable Energy Laboratory for download or on CD.
-
-TMY3 files have somewhat replaced TMY2 files but all TMY2 files are available for download from the website.
-
-### Solar and Wind Energy Resource Assessment (SWERA) Format
-
-The Solar and Wind Energy Resource Assessment (SWERA) project, funded by the United Nations Environment Program, is developing high quality information on solar and wind energy resources in 14 developing countries. Currently typical year hourly data are available for 156 locations in Belize, Brazil, China, Cuba, El Salvador, Ethiopia, Ghana, Guatemala, Honduras, Kenya, Maldives, Nicaragua, and Sri Lanka. The data are available from the SWERA project web site. http://swera.unep.net/;
-
-The SWERA format is very similar to the TMY2 format except:  WMO stations are used (6 character) in the header and 4 digit years have been adopted in the data lines.
-
-### WYEC2 Data Set/Format
-
-Culminating in the early 1980s, ASHRAE published their "Weather Year for Energy Calculations" (WYEC) hourly weather files for 51 US and Canadian locations. These files were intended to support the then growing interest in computer simulation of energy use in buildings. In the late 1980s, a major revision was initiated - this included the addition of 26 Typical Meteorological Year (TMY) hourly weather files to the original WYEC data set and a number of improvements.
-
-The work of revising and improving the WYEC data base was performed by at the National Renewable Energy Laboratory (NREL) as part of the Solar Radiation Resource Assessment Program (SRRAP), during the period 1989 through 1993. Richard Perez, at the State University of New York at Albany -- Atmospheric Sciences Research Center provided a substantial contribution to this work. The resulting set of 77 revised and corrected hourly weather files are referred to as WYEC Version 2 or "WYEC2" data set.
-
-The WYEC2 format is used as the format for several other data sets. The WYEC2 data set, however, was not made available for download though, of course, those files can be read if desired with the EnergyPlus Weather Converter utility.
-
-### Canadian Weather for Energy Calculations (CWEC)
-
-Produced by Numerical Logics in collaboration with Environment Canada and the National Research Council of Canada, the CWEC were derived using a methodology similar to the TMY2 and TMY. CWEC hourly files represent weather conditions that result in approximately average heating and cooling loads in buildings. The National Energy Code of Canada requires the use of a CWEC file representative of a location when the performance path and customized design calculations are chosen as the means of building energy consumption compliance. The CWEC follow the ASHRAE WYEC2 format and were derived from the Canadian Energy and Engineering Data Sets (CWEEDS) of hourly weather information for Canada from the 1953-1995 period of record.
-
-The 80 CWEC files contain hourly weather observations representing an artificial one-year period specifically designed for building energy calculations. All 80 locations in the CWEC data set are available for download in EnergyPlus weather format.
-
-### International Weather for Energy Calculations (IWEC)
-
-The IWEC are the result of ASHRAE Research Project 1015 conducted by Numerical Logics and Bodycote Materials Testing Canada for ASHRAE Technical Committee 4.2 Weather Information. The IWEC data files are 'typical' weather files suitable for use with building energy simulation programs for 227 locations outside the USA and Canada.
-
-The files are derived from up to 18 years of DATSAV3 hourly weather data originally archived at the U S National Climatic Data Center. The weather data is supplemented by solar radiation estimated on an hourly basis from earth-sun geometry and hourly weather elements, particularly cloud amount information. The IWEC CD-ROM is available from ASHRAE.
-
-The Department of Energy has licensed the IWEC data from ASHRAE. Our license with ASHRAE allows us to: "Distribute versions of the individual IWEC files in converted format suitable for EnergyPlus (EPW). Make the EnergyPlus versions of the IWEC files available to users at no cost via this EnergyPlus web site."  All 227 locations in the IWEC data set are available for download in EnergyPlus weather format.
-
-The IWEC source data is © 2001 American Society of Heating, Refrigerating and Air-Conditioning Engineers (ASHRAE), Inc., Atlanta, GA, USA. http://www.ashrae.org/ All rights reserved as noted in the License Agreement and Additional Conditions.
-
-IWEC also describes a data format, very similar to the TMY2 data format.
-
-### Typical Meteorological Year (TMY)
-
-Data for 230 locations in the USA plus four locations in Cuba, Marshall Islands, Palau, and Puerto Rico, derived from a 1948-1980 period of record. Many of the locations in the TMY data set were subsequently updated by the TMY2.
-
-Similar to the TMY2, the TMY are data sets of hourly values of solar radiation and meteorological elements for a 1-year period. Their intended use is for computer simulations of solar energy conversion systems and building systems to facilitate performance comparisons of different system types, configurations, and locations in the United States and its territories. Because they represent typical rather than extreme conditions, they are not suited for designing systems to meet the worst-case conditions occurring at a location. The data are available for purchase from the National Climatic Data Center.
-
-All TMY locations are available for download in EnergyPlus weather format.
-
-TMY also describes a data format.
-
-### California Climate Zones 2 (CTZ2)
-
-Updated weather data for 16 California climate zones for use to demonstrate compliance with Title 24 with approved building energy simulation programs. All 16 CTZ2 weather files are available for download in EnergyPlus weather format. The original source data is available from the California Energy Commission. These source data files are described using the WYEC2 format.
-
-### Solar and Wind Energy Resource Assessment (SWERA)
-
-The Solar and Wind Energy Resource Assessment (SWERA) project, funded by the United Nations Environment Program, is developing high quality information on solar and wind energy resources in 13 developing countries. Currently typical year hourly data are available for 48 locations in Belize, Cuba, El Salvador, Guatemala, Honduras, Maldives, Nicaragua, and Sri Lanka. The data are available from the SWERA project web site. SWERA plans to release new data for Brazil, Ethiopia, Ghana, Kenya, and Nepal over the coming few months. These source data files are described using the SWERA format.
-
-### Spanish Weather for Energy Calculations (SWEC)
-
-Originally developed for use with Calener, a new program for building energy labelling in Spain, these weather files cover all 52 Spanish provincial capitals. Calener was developed by the Grupo de Termotecnia of the Escuela Superior de Ingeneiros in Seville for the Spanish Government. The weather files were synthetically generated using Climed (Portuguese software developed by Ricardo Aguiar) from mean monthly data coming from the Spanish Meteorological National Institute. These weather files were converted from the DOE-2 binary to EnergyPlus format and include constant wind speeds of 6.7 m/s.
-
-For more information on these weather files, contact: Profesor Luis Pérez-Lombard ([lpl@tmt.us.es](file:///E:\Docs4PDFs\lpl@tmt.us.es)) Escuela Superior de Ingenieros
-
-### Italian Climatic data collection "Gianni De Giorgio" (IGDG)
-
-Developed for use in simulating renewable energy technologies, this set of 66 weather files is based on a 1951-1970 period of record. The data were created by Professor Livio Mazzarella, Politecnico di Milano, and is named in honor of Gianni de Giorgio.
-
-### Chinese Typical Year Weather (CTYW)
-
-Developed for use in simulating building heating and air conditioning loads and energy use, and for calculating renewable energy utilization, this set of 57 weather files is based on a 1982-1997 period of record with data obtained from the U. S. National Climatic Data Center. The data were created by Prof. ZHANG Qingyuan of Tsukuba University Japan, in collaboration with Joe Huang of Lawrence Berkeley National Laboratory. The original typical year weather files are contained in: Zhang Qingyuan and Joe Huang. 2004. Chinese Typical Year Weather Data for Architectural Use (in Chinese). ISBN 7-111-14810-X. Beijing: China Machine Press. Available from: China Machine Press; No. 22 Baiwanzhuang Dajie; Beijing, CHINA 100037.
-
-The CTYW files are no longer available for download from the web site.
-
-### INETI Synthetic data for Portugal
-
-Two weather files for Portugal developed by Ricardo Aguiar of Instituto Nacional de Engenharia, Tecnologia e Inovação (INETI). Synthetic data set based on spatially interpolation of public climatic data published by Instituto de Meteorologia 1951-80 combined with INETI owned data and other freely available data sources. INETI has granted DOE permission to distribute versions of the individual INETI files in converted format suitable for EnergyPlus (EPW) and make those files available to users at no cost via this EnergyPlus web site.
-
-The INETI synthetic data are © 2005 Instituto Nacional de Engenharia, Tecnologia e Inovação, Lisboa, Portugal. http://www.ineti.pt
-
-### ISHRAE India Weather Data Files (ISHRAE)
-
-Developed for use in simulating building heating and air conditioning loads and energy use, and for calculating renewable energy utilization, this set of 58 weather files was developed by the Indian Society of Heating, Refrigerating, and Air-Conditioning Engineers (ISHRAE). The source data are Copyright 2005 ISHRAE. ISHRAE has made these data available to DOE under license for use at no cost to the EnergyPlus user community.
-
-### City University of Hong Kong (CUHK) Data Set
-
-CityUHK-45007 -- WMO\#450070   Typical year file Hong Kong originally in IWEC format spreadsheet jointly developed by Dr TT Chow and ALS Chan of the City University of Hong Kong supported by a CERG grant from the Research Grants Council of the Hong Kong Special Administrative Region of China. Solar radiation measured from observatory station at 22.32N  114.17'E  65m above mean sea level.
-
-### Chinese Standard Weather Data (CSWD)
-
-Developed for use in simulating building heating and air conditioning loads and energy use, and for calculating renewable energy utilization, this set of 270 typical hourly data weather files. These data were developed by Dr. Jiang Yi, Department of Building Science and Technology at Tsinghua University and China Meteorological Bureau. The source data include annual design data, typical year data,  and extreme years for maximum enthalpy, and maximum and minimum temperature and solar radiation.
-
-China Meteorological Bureau, Climate Information Center, Climate Data Office and Tsinghua University, Department of Building Science and Technology. 2005. China Standard Weather Data for Analyzing Building Thermal Conditions, April 2005. Beijing: China Building Industry Publishing House, ISBN 7-112-07273-3 (13228). http://www.china-building.com.cn.
-
-### Kuwait Weather Data from Kuwait Institute for Scientific Research (KISR)
-
-Two weather files for Kuwait based on measured meteorological data for Kuwait International Airport and KISR's coastal weather station. Provided by KISR in spreadsheet format.
-
-### Egyptian Weather for Energy Calculations (EWEC)
-
-Developed for standards development and energy simulation by Joe Huang from data provided by National Climatic Data Center for periods of record from 12 to 21 years, all ending in 2003. Joe Huang and Associates, Moraga, California, USA.
-
-### Israel weather data (MSI)
-
-Weather data for Israel locations developed by Faculty of Civil and Environmental Engineering, Technion - Israel Institute of Technology, Haifa, Israel, from data provided by the Israel Meteorological Service.
-
-### Representative Meteorological Year (RMY) Australia Climatic Data
-
-RMY Australia Representative Meteorological Year Climate Files Developed for the Australia Greenhouse Office for use in complying with Building Code of Australia. These data are licensed through ACADS BSG Ltd for use by EnergyPlus users. For use in any other formats, users must contact ACADS BSG Ltd for licensing information.
-
-The RMY data are © 2006 Commonwealth of Australia, Department of the Environment and Water Resources, Australia Greenhouse Office, Canberra, ACT, Australia. [www.greenhouse.gov.au/buildings/code.html](https://web.archive.org/web/20070608213812/http://www.greenhouse.gov.au/buildings/code.html) (URL has since been removed, so replaced with a link on The Internet Archive from 2007.)  All intellectual property rights reserved.
-
-### Iranian Typical Meteorological Year (ITMY)
-
-Typical year weather files have been created for Tehran from weather data for 1992 through 2003 published by the Islamic Republic of Iran Meteorological Organization (IRIMO) for Tehran Mehrabad. Developed for standards development and energy simulation by Joe Huang, White Box Technologies.
-
-### New Zealand National Institute of Water & Atmospheric Research Ltd (NIWA)
-
-The New Zealand Energy Efficiency and Conservation Authority (EECA) has developed a Home Energy Rating Scheme (HERS) for New Zealand households based on software simulation of energy loss and demand. The software requires hourly data to represent the different climates zones around New Zealand, especially for larger population centres. These climate data consist of hourly records for an artificial year created from twelve representative months.
-
-Liley, J Ben, Hisako Shiona, James Sturman, David S Wratt. 2007. Typical Meteorological Years for the New Zealand Home Energy Rating Scheme. Prepared for the Energy Efficiency and Conservation Authority. NIWA Client Report: LAU2007- 02-JBL. NIWA, Omakau, New Zealand.
-
-### Chartered Institution of Building Services Engineers (CIBSE)
-
-The CIBSE, in association with the (UK) Met Office has produced 'Test Reference Years' and 'Design Summer Years' for 14 UK locations for use with building energy simulation software. The data sets are available in various formats, including EnergyPlus/ESP-r. These data are NOT available on the EnergyPlus web site. For further details, see:
-
-[www.cibse.org/index.cfm?go=publications.view&PubID=332&S1=y&L1=0&L2=0](file:///E:\Docs4PDFs\www.cibse.org\index.cfm%3fgo=publications.view&PubID=332&S1=y&L1=0&L2=0)
-
-### Meteonorm Data
-
-Meteonorm software can be used when there is no measured data near the location for the simulation. Meteonorm extrapolates hourly data from statistical data for a location. Where statistical data aren't available, Meteonorm interpolates from other nearby sites. Generally a statistical approach is a last resort -- weather files generated from statistics will not demonstrate the normal hour-to-hour and day-to-day variability seen in measured data. Meteonorm version 6 will directly write EPW files.
-
-### Other Formats
-
-The data sets and formats described above are some of the newest formats available for use with building simulation programs. Source data comes in various formats. Typically the files are ASCII, but the data items, units, item location, and record length vary from format to format. NCDC can provide historical data in a variety of formats: TD-3280, TD-3510, TD-9950 (DATSAV2), TD-9956 (DATSAV3) and TD-1440 (CD144). The EnergyPlus weather processor cannot process any of the types directly.
-
-Table 18. Summary of Downloadable Weather Data by Type
-<table class="table table-striped">
-  <tr>
-    <th rowspan="3">Source</th>
-    <th colspan="8" align="center">WMO Region</th>
-    <th></th>
-  </tr>
-  <tr>
-    <td colspan="3">North and Central America</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>USA</td>
-    <td>Canada</td>
-    <td>Central America</td>
-    <td>Africa</td>
-    <td>Asia</td>
-    <td>South America</td>
-    <td>Southwest Pacific</td>
-    <td>Europe</td>
-    <td>Total</td>
-  </tr>
-  <tr>
-    <td>ETMY</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>11</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>11</td>
-  </tr>
-  <tr>
-    <td>IGDG</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>66</td>
-    <td>66</td>
-  </tr>
-  <tr>
-    <td>IMGW</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>61</td>
-    <td>61</td>
-  </tr>
-  <tr>
-    <td>INETI</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>2</td>
-    <td>2</td>
-  </tr>
-  <tr>
-    <td>ISHRAE</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>58</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>58</td>
-  </tr>
-  <tr>
-    <td>ITMY</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>1</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>1</td>
-  </tr>
-  <tr>
-    <td>IWEC</td>
-    <td></td>
-    <td></td>
-    <td>5</td>
-    <td>12</td>
-    <td>49</td>
-    <td>19</td>
-    <td>20</td>
-    <td>122</td>
-    <td>227</td>
-  </tr>
-  <tr>
-    <td>KISR</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>2</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>2</td>
-  </tr>
-  <tr>
-    <td>Los Alamos TMY2</td>
-    <td>1</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>1</td>
-  </tr>
-  <tr>
-    <td>MSI</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>4</td>
-    <td>4</td>
-  </tr>
-  <tr>
-    <td>NIWA</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>16</td>
-    <td></td>
-    <td>16</td>
-  </tr>
-  <tr>
-    <td>RMY</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>80</td>
-    <td></td>
-    <td>80</td>
-  </tr>
-  <tr>
-    <td>SWEC</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>2</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>50</td>
-    <td>52</td>
-  </tr>
-  <tr>
-    <td>SWERA</td>
-    <td></td>
-    <td></td>
-    <td>37</td>
-    <td>33</td>
-    <td>66</td>
-    <td>20</td>
-    <td></td>
-    <td></td>
-    <td>156</td>
-  </tr>
-  <tr>
-    <td>TMY</td>
-    <td>229</td>
-    <td></td>
-    <td>1</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>4</td>
-    <td></td>
-    <td>234</td>
-  </tr>
-  <tr>
-    <td>TMY2</td>
-    <td>235</td>
-    <td></td>
-    <td>1</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>1</td>
-    <td></td>
-    <td>237</td>
-  </tr>
-  <tr>
-    <td>TMY3</td>
-    <td>1011</td>
-    <td></td>
-    <td>7</td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td>2</td>
-    <td></td>
-    <td>1020</td>
-  </tr>
-  <tr>
-    <td>Totals</td>
-    <td>1476</td>
-    <td>0</td>
-    <td>51</td>
-    <td>58</td>
-    <td>176</td>
-    <td>39</td>
-    <td>123</td>
-    <td>305</td>
-    <td></td>
-  </tr>
-</table>
-
-One other format worth mentioning is TRY. TRY is "test reference year" data that did not include solar radiation data. "Test Reference Year" is a term that usually denotes selection of a specific year of "real" data based on some statistical procedure. The original TRY data (TD-9706) was based on an ASHRAE procedure to select the data from a "period of record". "The principle of the selection is to eliminate years in the period of record containing months with extremely high or low mean temperatures until only one year remains."  The weather conversion utility cannot process data in "TRY" format. However, many organizations develop data for reference year data (e.g. European TRY, Moisture Reference Data).
-
-### Custom Format
-
-Using a "definitions" file (see Description of "Def" input file), the weather converter can process a wide range of data formats. In the table above, both the GDG and CTYW weather data was processed by a custom format approach.
-
-### Solar Data
-
-Source weather data files may or may not contain solar data. All of the files that can be processed by the EnergyPlus Weather conversion utility contain solar data. The weather processor will transfer this data to the EPW weather file and the EnergyPlus simulation program will use it.
-
-Historical weather data files in CD144 format do not contain solar data nor is such data generally available for a specific location and time period. In this case, ersatz solar data must be generated from cloud cover and other data using sky models and regression formulas. Currently, neither the Weather Conversion utility nor the EnergyPlus program synthesizes this data.  However, the weather conversion utility can use any two of the commonly recorded data (i.e. two of Global Horizontal Radiation, Horizontal Diffuse Radiation and Direct Normal (or Direct Horizontal) Radiation to calculate the EnergyPlus primary solar data of Direct Normal and Horizontal Diffuse Radiation values).
-
-Data Sources/Uncertainty
-------------------------
-
-More recent weather data source files have introduced the concept of data sources and uncertainty flags for many of the fields. The EnergyPlus weather format faithfully reproduces these fields as appropriate for the input source data types. By and large, most of the data sources and uncertainties have used the TMY2 established fields and values (See following table). As noted earlier, to enhance readability and reduce obfuscation, the EnergyPlus format for the data source and uncertainty flags collates them into one large field. Each data element still has its data source and uncertainty: it is positionally embodied depending on its place in the EPW data record.
-
-Table 19. Key to Data Source and Uncertainty Flags
-
-<table class="table table-striped">
-<tr>
-<th>Data Flag</th>
-<th>Flag Values</th>
-</tr>
-<tr>
-<td>Dry Bulb Temperature Data Source</td>
-<td>A-F</td>
-</tr>
-<tr>
-<td>Dry Bulb Temperature Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Dew Point Temperature Data Source</td>
-<td>A-F</td>
-</tr>
-<tr>
-<td>Dew Point Temperature Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Relative Humidity Data Source</td>
-<td>A-F</td>
-</tr>
-<tr>
-<td>Relative Humidity Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Atmospheric Station Pressure Data Source</td>
-<td>A-F</td>
-</tr>
-<tr>
-<td>Atmospheric Station Pressure Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Horizontal Infrared Radiation Data Source</td>
-<td>A-H, ?</td>
-</tr>
-<tr>
-<td>Horizontal Infrared Radiation Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Global Horizontal Radiation Data Source</td>
-<td>A-H, ?</td>
-</tr>
-<tr>
-<td>Global Horizontal Radiation Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Direct Normal Radiation Data Source</td>
-<td>A-H, ?</td>
-</tr>
-<tr>
-<td>Direct Normal Radiation Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Diffuse Horizontal Radiation Data Source</td>
-<td>A-H, ?</td>
-</tr>
-<tr>
-<td>Diffuse Horizontal Radiation Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Global Horizontal Illuminance Data Source</td>
-<td>I, ?</td>
-</tr>
-<tr>
-<td>Global Horizontal Illuminance Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Direct Normal Illuminance Data Source</td>
-<td>I, ?</td>
-</tr>
-<tr>
-<td>Direct Normal Illuminance Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Diffuse Horizontal Illuminance Data Source</td>
-<td>I, ?</td>
-</tr>
-<tr>
-<td>Diffuse Horizontal Illuminance Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Zenith Luminance Data Source</td>
-<td>I, ?</td>
-</tr>
-<tr>
-<td>Zenith Luminance Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Wind Direction Data Source</td>
-<td>A-F</td>
-</tr>
-<tr>
-<td>Wind Direction Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Wind Speed Data Source</td>
-<td>A-F</td>
-</tr>
-<tr>
-<td>Wind Speed Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Total Sky Cover Data Source</td>
-<td>A-F</td>
-</tr>
-<tr>
-<td>Total Sky Cover Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Opaque Sky Cover Data Source</td>
-<td>A-F</td>
-</tr>
-<tr>
-<td>Opaque Sky Cover Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Visibility Data Source</td>
-<td>A-F, ?</td>
-</tr>
-<tr>
-<td>Visibility Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Ceiling Height Data Source</td>
-<td>A-F, ?</td>
-</tr>
-<tr>
-<td>Ceiling Height Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Precipitable Water Data Source</td>
-<td>A-F</td>
-</tr>
-<tr>
-<td>Precipitable Water Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Broadband Aerosol Optical Depth Data Source</td>
-<td>A-F</td>
-</tr>
-<tr>
-<td>Broadband Aerosol Optical Depth Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Snow Depth Data Source</td>
-<td>A-F, ?</td>
-</tr>
-<tr>
-<td>Snow Cover Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-<tr>
-<td>Days Since Last Snowfall Data Source</td>
-<td>A-F, ?</td>
-</tr>
-<tr>
-<td>Days Since Last Snowfall Data Uncertainty</td>
-<td>0-9</td>
-</tr>
-</table>
-
-
-
-The definition of the solar radiation source flags and solar radiation uncertainty flags are shown in the following two tables:
-
-Table 20. Solar Radiation and Illuminance Data Source Flag Codes
-
-<table class="table table-striped">
-<tr>
-<th>Flag Code</th>
-<th>Definition</th>
-</tr>
-<tr>
-<td>A</td>
-<td>Post-1976 measured solar radiation data as received from NCDC or other sources</td>
-</tr>
-<tr>
-<td>B</td>
-<td>Same as &quot;A&quot; except the global horizontal data underwent a calibration correction</td>
-</tr>
-<tr>
-<td>C</td>
-<td>Pre-1976 measured global horizontal data (direct and diffuse were not measured before 1976), adjusted from solar to local time, usually with a calibration correction</td>
-</tr>
-<tr>
-<td>D</td>
-<td>Data derived from the other two elements of solar radiation using the relationship, global = diffuse + direct ´ cosine (zenith)</td>
-</tr>
-<tr>
-<td>E</td>
-<td>Modeled solar radiation data using inputs of observed sky cover (cloud amount) and aerosol optical depths derived from direct normal data collected at the same location</td>
-</tr>
-<tr>
-<td>F</td>
-<td>Modeled solar radiation data using interpolated sky cover and aerosol optical depths derived from direct normal data collected at the same location</td>
-</tr>
-<tr>
-<td>G</td>
-<td>Modeled solar radiation data using observed sky cover and aerosol optical depths estimated from geographical relationships</td>
-</tr>
-<tr>
-<td>H</td>
-<td>Modeled solar radiation data using interpolated sky cover and estimated aerosol optical depths</td>
-</tr>
-<tr>
-<td>I</td>
-<td>Modeled illuminance or luminance data derived from measured or modeled solar radiation data</td>
-</tr>
-<tr>
-<td>?</td>
-<td>Source does not fit any of the above categories. Used for nighttime values and missing data</td>
-</tr>
-</table>
-
-
-
-Table 21. Solar Radiation and Illuminance Data Uncertainty Flag Codes
-
-<table class="table table-striped">
-<tr>
-<th>Flag</th>
-<th>Uncertainty Range (%)</th>
-</tr>
-<tr>
-<td>1</td>
-<td>Not used</td>
-</tr>
-<tr>
-<td>2</td>
-<td>2 - 4</td>
-</tr>
-<tr>
-<td>3</td>
-<td>4 - 6</td>
-</tr>
-<tr>
-<td>4</td>
-<td>6 - 9</td>
-</tr>
-<tr>
-<td>5</td>
-<td>9 - 13</td>
-</tr>
-<tr>
-<td>6</td>
-<td>13 - 18</td>
-</tr>
-<tr>
-<td>7</td>
-<td>18 - 25</td>
-</tr>
-<tr>
-<td>8</td>
-<td>25 - 35</td>
-</tr>
-<tr>
-<td>9</td>
-<td>35 - 50</td>
-</tr>
-<tr>
-<td>0</td>
-<td>Not applicable</td>
-</tr>
-</table>
-
-Finally, the Meteorological data source and uncertainty flag/codes are shown in the following two tables:
-
-Table 22. Meteorological Data Source Flag Codes
-
-<table class="table table-striped">
-<tr>
-<th>Flag</th>
-<th>Definition</th>
-</tr>
-<tr>
-<td>A</td>
-<td>Data as received from NCDC, converted to SI units</td>
-</tr>
-<tr>
-<td>B</td>
-<td>Linearly interpolated</td>
-</tr>
-<tr>
-<td>C</td>
-<td>Non-linearly interpolated to fill data gaps from 6 to 47 hours in length</td>
-</tr>
-<tr>
-<td>D</td>
-<td>Not used</td>
-</tr>
-<tr>
-<td>E</td>
-<td>Modeled or estimated, except: precipitable water, calculated from radiosonde data; dew point temperature calculated from dry bulb temperature and relative humidity; and relative humidity calculated from dry bulb temperature and dew point temperature</td>
-</tr>
-<tr>
-<td>F</td>
-<td>Precipitable water, calculated from surface vapor pressure; aerosol optical depth, estimated from geographic correlation</td>
-</tr>
-<tr>
-<td>?</td>
-<td>Source does not fit any of the above. Used mostly for missing data</td>
-</tr>
-</table>
-
-
-
-Table 23. Meteorological Uncertainty Flag Codes
-
-<table class="table table-striped">
-<tr>
-<th>Flag</th>
-<th>Definition</th>
-</tr>
-<tr>
-<td>1- 6</td>
-<td>Not used</td>
-</tr>
-<tr>
-<td>7</td>
-<td>Uncertainty consistent with NWS practices and the instrument or observation used to obtain the data</td>
-</tr>
-<tr>
-<td>8</td>
-<td>Greater uncertainty than 7 because values were interpolated or estimated</td>
-</tr>
-<tr>
-<td>9</td>
-<td>Greater uncertainty than 8 or unknown.</td>
-</tr>
-<tr>
-<td>0</td>
-<td>Not definable.</td>
-</tr>
-</table>
-
-
-
-Advanced use - accessing weather conversion capabilities
---------------------------------------------------------
-
-### Interface to the EPlusWth.dll
-
-To provide information for outside developers/interfaces that might want to use the basic weather processing utility from within their interface, the EPlusWth.dll was developed. It is actually used by the weather converter utility. In addition to the basic interface calls, six important files are also used by this library. These are placed in the WeatherConverter folder during install of EnergyPlus.
-
-### Files used by EPlusWth.dll
-
-Each of the files is in a general comma-delimited format. Thus, they can be easily viewed by importing into a spreadsheet program such as Excelâ„¢. The files are used to support information lacking in the source data files and/or supply additional information used during the conversion process. In each case (with one exception), there will be a single or set of "header" records describing each column of the file and then the data values of the file will follow on subsequent records. Each of the files is described briefly in the next few sections.
-
-#### Abbreviations.csv
-
-This file does not have a header record, but it consists of 3 columns. It is used for data files that might have 2-character abbreviations for US States or Canadian provinces and provides a translation to the full name and 3-character country code. Likewise, it can use the full name of these items to obtain the 2-character abbreviation or 3-character country code.
-
-#### WBANLocations.csv
-
-In many older data sets, the station identifier for the weather data uses the WBAN (Weather Bureau Army-Navy) designation system. This has largely been superseded by the WMO (World Meteorological Organization) designation for station collection site identifiers. This file provides a translation between the two identifier systems. In addition, this file contains latitude, longitude, time zone and elevation information for the sites.
-
-#### Cal Climate Zone Lat Long data.csv
-
-Note that this file has spaces in the name. The California c limate zone data source files do not have standard station identifiers. Rather they use a climate zone designator from 1-16. This file is used to obtain the latitude, longitude, time zone and elevation data for these climate zones. The WYEC2 "File Source Code" (field 2, column 6 of each data record) is used to determine that the file is a California compliance type file.
-
-#### ASHRAE\_2009\_Yearly\_DesignConditions.csv
-
-The three files for design conditions have roughly the same format. These are the values from the ASHRAE Handbook of Fundamentals, 2009, Chapter 14, Appendix. The WMO station identifier is used to determine the design condition values that apply to a source data file and, thus, are included in the DESIGN CONDITION header record on the EPW file produced as part of the conversion. This information is also included in the statistical report file (STAT) produced from the weather converter utility. In addition, these are used to supply the information for the design day object (DDY) file creation.
-
-### Public calls to EPlusWth.dll
-
-Several points of the library are made available for use with external programs. In each case the parameters passed will be described along with the Visual Basicâ„¢ (VB6) code that is used to declare them as well as Fortran 90 style "Interface" statements to the same calls. The library is placed in the same folder with the weather converter utility - you may need to copy it to your program's folder if you choose to add external calls from your program to it.
-
-#### SetupPWInternalDataPath
-
-This call designates the "path" to the files listed above. This is the location where the ProcessWeather call will expect to find the files. Having this incorrectly specified is not fatal, but will probably cause confusion.
-
-VB declaration statement:
-
-Private Declare Sub SetupPWInternalDataPath Lib "EPlusWth" (ByVal strPath As String, ByVal InPathLen As Long)
-
-And a call from a VB program:
-
-
-```basic
-Call SetupPWInternalDataPath(AppPath, Len(AppPath))
-```
-
-
-Likewise for Fortran 90/95:
-
-
-```fortran
-  INTERFACE
-    SUBROUTINE SetupPWInternalDataPath (Path)
-    CHARACTER(len=\*), INTENT(IN) :: Path    ! Path where data files reside
-    END SUBROUTINE
-  END INTERFACE
-```
-
-And then calling it from Fortran:
-
-
-```fortran
-Character(len=255) DataPath
-CALL SetupPWInternalDataPath(trim(DataPath))
-```
-
-#### SetFixOutOfRangeData
-
-As shown earlier (file menu option in the weather converter utility), there is an option to "fix" out of range data or not. By default, this is turned off (does not fix data). Again a character convention ("yes" for fixing; "no" for not fixing) is used. Case of the actual string is ignored.
-
-VB Declaration statement:
-
-Private Declare Sub SetFixOutOfRangeData Lib "EPlusWth" (ByVal strValue As String, ByVal strValueLen As Long)
-
-And calling it from VB:
-
-```basic
-    Global FixOutOfRangeData As String
-    FixOutOfRangeData = "Yes"
-    Call SetFixOutOfRangeData(FixOutOfRangeData, Len(FixOutOfRangeData))
-```
-
-For Fortran 90/95:
-
-```fortran
-  INTERFACE
-    SUBROUTINE SetFixOutOfRangeData (YesNo)
-    CHARACTER(len=\*),INTENT(IN) :: YesNo    ! 'yes' to set fixing option;
-                                            ! 'no' to not
-    END SUBROUTINE
-  END INTERFACE
-```
-
-And then calling it:
-
-```fortran
-CALL SetFixOutOfRangeData('no')
-```
-
-#### SetDefaultChgLimit
-
-This call sets the value for the DB trigger shown earlier. Both values passed in are strings and are specific to the dialog shown earlier:
-
-Table 24. Trigger Limit Call Values
-<table class="table table-striped">
-  <tr>
-    <th>Trigger <BR> Limit</th>
-    <th>Result</th>
-    <th>Ignore <BR> Calc <BR> Trigger</th>
-    <th>Result</th>
-  </tr>
-  <tr>
-    <td>0</td>
-    <td>use only calculated trigger</td>
-    <td>0</td>
-    <td>Uses Calculated Trigger</td>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td>use 5&deg;C</td>
-    <td>1</td>
-    <td>Ignores calculated trigger</td>
-  </tr>
-  <tr>
-    <td>2</td>
-    <td>use 10&deg;C</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>use 15&deg;C</td>
-    <td></td>
-    <td></td>
-  </tr>
-</table>
-
-
-You can also choose to ignore the calculated trigger entirely. If you do not "ignore" the calculated trigger, then the trigger is the minimum of the calculated and your trigger limit selection.
-
-VB Declaration Statement:
-
-```basic
-Private Declare Sub SetDefaultChgLimit Lib "EPlusWth" (ByVal strValue As String, ByVal strValueLen As Long, ByVal strValue As String, ByVal strValueLen As Long)
-```
-
-And a call from VB:
-
-```basic
-    Call SetDefaultChgLimit(TriggerLimit, Len(TriggerLimit), IgnoreCalcTrigger, Len(IgnoreCalcTrigger))
-```
-
-#### ProcessWeather
-
-The "meat" of the processing is done by this routine. It gets passed the input file name (source data), the input file type, output file name, and output file type. As an output it can provide a notice that the processing was successful or not.
-
-VB Declaration Statement:
-
-```basic
-Private Declare Sub ProcessWeather Lib "EPlusWth" (ByVal strInType As String, ByVal InTypeLen As Long, ByVal strOutType As String, ByVal OutTypeLen As Long, ByVal strInFileName As String, ByVal InFileNameLen As Long, ByVal strOutFileName As String, ByVal OutFileNameLen As Long, ErrorFlag As Boolean, Optional ByVal strOutFileURL As String, Optional ByVal OutFileURLlen As Long)
-```
-
-Calling it from VB:
-
-```basic
-Call ProcessWeather(InputFileDataType, Len(InputFileDataType),
-      OutputFileDataType, Len(OutputFileDataType),
-      InputFileName, Len(InputFileName),
-      OutputFileName, Len(OutputFileName),
-      ErrorFlag)
-```
-
-Valid values for the Input File Data Type are shown in the following table:
-
-Table 25. Valid Input File Types for "ProcessWeather" call
-
-<table class="table table-striped">
-<tr>
-<th>Input File Type</th>
-<th>Source Data file Format Type</th>
-</tr>
-<tr>
-<td>TMY2 or TM2</td>
-<td>TMY2 data file</td>
-</tr>
-<tr>
-<td>IWEC or IWC</td>
-<td>IWEC data file</td>
-</tr>
-<tr>
-<td>SAMSON or DAT</td>
-<td>SAMSON data file</td>
-</tr>
-<tr>
-<td>WYEC2 or WY2</td>
-<td>WYEC2 data file</td>
-</tr>
-<tr>
-<td>FMT or TXT</td>
-<td>DOE-2 Formatted data file</td>
-</tr>
-<tr>
-<td>CLM or ESP-r</td>
-<td>ESP-r formatted data file</td>
-</tr>
-<tr>
-<td>BLAST or ASC</td>
-<td>BLAST ASCII formatted data file</td>
-</tr>
-<tr>
-<td>EPW</td>
-<td>EnergyPlus EPW file</td>
-</tr>
-<tr>
-<td>CSV</td>
-<td>EnergyPlus CSV file</td>
-</tr>
-<tr>
-<td>TMY</td>
-<td>TMY data files</td>
-</tr>
-<tr>
-<td>WEA</td>
-<td>Eco-Tect WEA files</td>
-</tr>
-<tr>
-<td>SWERA or SWE</td>
-<td>SWERA data files</td>
-</tr>
-<tr>
-<td>&lt;any&gt;</td>
-<td>Custom - must have "def" file</td>
-</tr>
-</table>
-
-Valid values for the Output File Type(s) are shown in the following table:
-
-Table 26. Valid Output File Types for the "ProcessWeather" call
-
-<table class="table table-striped">
-<tr>
-<th>Output File Type</th>
-<th>File(s) produced</th>
-</tr>
-<tr>
-<td>EPW</td>
-<td>EPW and RPT files</td>
-</tr>
-<tr>
-<td>CSV</td>
-<td>CSV and RPT files</td>
-</tr>
-<tr>
-<td>BOTH</td>
-<td>EPW, CSV and RPT files</td>
-</tr>
-<tr>
-<td>RPT</td>
-<td>RPT file</td>
-</tr>
-</table>
-
-For Input and Output file names, the complete paths should be included.
-
-ErrorFlag will be returned as "true" if an error occurs during processing or "false" if the process is successful.
-
-Fortran 90/95 Declaration:
-
-```fortran
-INTERFACE
-  SUBROUTINE ProcessWeather(InType,OutType,InFileName,OutFileName,ErrFlag)
-    CHARACTER(len=\*), INTENT(IN) :: InType       ! InputFile Type
-    CHARACTER(len=\*), INTENT(IN) :: OutType      ! OutputFile Type
-    CHARACTER(len=\*), INTENT(IN) :: InFileName   ! InputFile Name (Full path)
-    CHARACTER(len=\*), INTENT(IN) :: OutFileName  ! OutputFileName (Full path)
-    LOGICAL(Byte2), INTENT(OUT)  :: ErrFlag      ! If errors are found,
-                                                 ! set to true and put
-                                                 ! description put in file.
-  END SUBROUTINE
-END INTERFACE
-```
-
-And calling it from Fortran:
-
-```fortran
-call processweather(trim(intype),trim(outtype),    &
-                    trim(infilename),trim(outfilename),errflag)
-```
-
-
-Note that the file where error messages will be placed is the RPT file. If the value of the output file path is incorrect, you may need to search for this file by using the RPT extension.
-
-References
-----------
-
-ASHRAE. 1985. *Weather Year for Energy Calculations*. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 1997. *WYEC2 Weather Year for Energy Calculations 2, Toolkit and Data*, Atlanta: ASHRAE.
-
-ASHRAE. 2001. *International Weather for Energy Calculations (IWEC Weather Files) Users Manual and CD-ROM*, Atlanta: ASHRAE
-
-ASHRAE. 2004. *ANSI/ASHRAE Standard 90.2-2004*, "Energy-Efficient Design of Low-Rise Residential Buildings," September 2004. Atlanta: American Society of Heating, Refrigerating, and Air-conditioning Engineers.
-
-ASHRAE. 2004. *ANSI/ASHRAE/IESNA Standard 90.1-2004*, "Energy-Efficient Design of Buildings Except Low-Rise Residential," September 2004. Atlanta: American Society of Heating, Refrigerating, and Air-conditioning Engineers.
-
-ASHRAE, 2009. Handbook of Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-conditioning Engineers.
-
-Briggs, Robert S., Robert G. Lucas, and Z. Todd Taylor. 2002. "Climate Classification for Building Energy Codes and Standards: Part 1 - Development Process" in *ASHRAE Transactions 2002*, 109, Pt 1. Atlanta:  ASHRAE.
-
-Briggs, Robert S., Robert G. Lucas, and Z. Todd Taylor. 2002. "Climate Classification for Building Energy Codes and Standards: Part 2 - Zone Definitions, Maps and Comparisons" in *ASHRAE Transactions*, 109, Pt 1. Atlanta:  ASHRAE.
-
-Buhl, W.F. 1998. DOE-2 Weather Processor, DOE2.1E Documentation Update, Berkeley: Lawrence Berkeley National Laboratory.
-
-COMIS Weather Program, http://www.byggforsk.no/hybvent/COMISweather.htm
-
-China Meteorological Bureau, Climate Information Center, Climate Data Office and Tsinghua University, Department of Building Science and Technology. 2005. China Standard Weather Data for Analyzing Building Thermal Conditions, April 2005. Beijing: China Building Industry Publishing House, ISBN 7-112-07273-3 (13228). http://www.china-building.com.cn.
-
-Commission of the European Community. 1985. *Test Reference Years,* Weather data sets for computer simulations of solar energy systems and energy consumption in buildings, CEC, DG XII. Brussels, Belgium: Commission of the European Community.
-
-Crawley, Drury B., Linda K. Lawrie, Curtis O. Pedersen, Richard J. Liesen, Daniel E. Fisher, Richard K. Strand, Russell D. Taylor, Frederick C. Winkelmann, W.F. Buhl, A. Ender Erdem, and Y. Joe Huang. 1999. "EnergyPlus, A New-Generation Building Energy Simulation Program," in *Proceedings of Building Simulation '99*, Kyoto, Japan. IBPSA.
-
-Crawley, Drury B. 1998. "Which Weather Data Should You Use for Energy Simulations of Commercial Buildings?," *ASHRAE Transactions*, pp. 498-515, Vol. 104, Pt. 2. Atlanta:  ASHRAE.
-http://energyplus.gov/pdfs/bibliography/whichweatherdatashouldyouuseforenergysimulations.pdf
-
-Crawley, Drury B., Jon Hand, and Linda K. Lawrie, 1999. "Improving the Weather Information Available to Simulation Programs", in *Proceedings of Building Simulation '99*, Kyoto, Japan. September 1999. IBPSA.
-
-Energy Simulation Research Unit. 1999.  http://www.strath.ac.uk/Departments/ESRU
-
-Janak, M. 1997. "Coupling Building Energy and Lighting Simulation," in *Proceedings of Building Simulation 97*, September 1997, Volume II pp 313-319, Prague, Czech Republic, IBPSA.
-
-K&ouml;ppen, W. 1931. Grundriss der Klimakunde. Berlin: Walter de Gruyter & Co.
-
-Kusuda, T., "Earth Temperatures Beneath Five Different Surfaces", Institute for Applied Technology, NBS Report 10-373, 1971, NBS, Washington DC 20234.
-
-Kusuda, T., Least Squares Technique for the Analysis of Periodic Temperature of the Earth's Surface Region, NBS Journal of Research, Vol. 71C, Jan-Mar. 1967, pp 43-50.
-
-National Instruments Corporation. 1999. *LabVIEW User Manual*. Austin, Texas:  National Instruments Corporation.
-
-McDonald, Iain, and Paul Strachan. 1998. "Practical Application of Uncertainty Analysis" in *Proceedings of EPIC 98: Second International Conference on Energy Performance and Indoor Climate in Buildings*, Lyon, France, 19-21 November 1998.
-
-National Climatic Data Center (NCDC). 1976. *Test Reference Year (TRY)*, Tape Reference Manual, TD-9706, September 1976. Asheville, North Carolina: National Climatic Data Center, U.S. Department of Commerce.
-
-NCDC. 1981. *Typical Meteorological Year User's Manual, TD-9734, Hourly Solar Radiation -- Surface Meteorological Observations*, May 1981. Asheville, North Carolina: National Climatic Data Center, U.S. Department of Commerce.
-
-NCDC. 1981. *Meteorological Observations*, May 1981. Asheville, North Carolina: National Climatic Data Center, U.S. Department of Commerce.
-
-NCDC. 1993. *Solar and Meteorological Surface Observation Network, 1961-1990, Version 1.0*, September 1993. Asheville, North Carolina: National Climatic Data Center, U.S. Department of Commerce.
-
-National Renewable Energy Laboratory (NREL). 1995. *User's Manual for TMY2s (Typical Meteorological Years)*, NREL/SP-463-7668, and *TMY2s, Typical Meteorological Years Derived from the 1961-1990 National Solar Radiation Data Base*, June 1995, CD-ROM. Golden, Colorado: National Renewable Energy Laboratory.
-
-http://rredc.nrel.gov/solar/pubs/tmy2/
-
-Numerical Logics. 1999. Canadian Weather for Energy Calculations, Users Manual and CD-ROM. Downsview, Ontario: Environment Canada.
-
-Oliver, John E. 1991. "The History, Status and Future of Climatic Classification," in Physical Geography 1991, Vol 12, No. 3, pp. 231-251.
-
-Perez R, Ineichen P, Maxwell E, Seals R and Zelenka. A 1992. Dynamic Global-to-Direct Irradiance Conversion Models. *ASHRAE Transactions-Research Series*,354-369.
-
-Perez R, Ineichen P, Seals R, Michalsky J and Stewart R. 1990. Modeling daylight.availability and irradiance components from direct and global irradiance. *Solar.Energy*44, 271-289.
-
-University of Illinois. 1998. *BLAST User's Guide.* Building Systems Laboratory, University of Illinois. Urbana, Illinois:  University of Illinois, Department of Industrial and Mechanical Engineering.
-
-Ward. G. 1996. *Radiance.* Berkeley:  Lawrence Berkeley National Laboratory.
-
-Winkelmann, F.C., W.F. Buhl, B. Birdsall, A. E. Erdem, and K. Ellington. 1994. *DOE-2.1E Supplement*, DE-940-11218. Lawrence Berkeley Laboratory, Berkeley, California. Springfield, Virginia: NTIS.
-
-Zhang, Q. Y., Y. J. Huang. 2002. "Development of Typical Year Weather Files for Chinese Locations", in ASHRAE Transactions, Volume 108, Part 2.
-
-Web Resources
--------------
-
-Building Energy Tools Directory, a directory of information on 340+ energy tools from around the world.
-
-http://www.energytoolsdirectory.gov/
-
-Energy Systems Research Unit, University of Strathclyde, authors of ESP-r, up-to-date information on ESP-r and other energy systems research and software development.
-
-http://www.strath.ac.uk/Departments/ESRU
-
-EnergyPlus, up-to-date information on the current status of EnergyPlus and working with the team, and documentation such as input data structure, output data structure, and licensing opportunities. Additional weather files may be posted here as well.
-
-http://www.energyplus.gov
-
-Description of the SWERA project. http://swera.unep.net/swera/
-
-Weather Analytics ([www.wxaglobal.com](http://www.wxaglobal.com)) - Site specific weather files in EnergyPlus format based on the latest 30 years of hourly data are now available from the private sector company Weather Analytics for any official weather station or over 600,000 35-km grid tiles across the globe. These files are built by integrating hourly weather station observations and the new NOAA reanalysis data sets.  Both Typical Meteorological Year (TMY) files and individual, Actual Meteorological Year (AMY) files are available as well as files constructed from the previous 12 months.
-
-Meteonorm ([www.meteonorm.com](http://www.meteonorm.com)) - Files for specific locations can be purchased in EnergyPlus format from Meteonorm company. Meteonorm extrapolates hourly data from statistical data for a location. Where statistical data aren't available, Meteonorm interpolates from other nearby sites. Generally a statistical approach is a last resort--weather files generated from statistics will not demonstrate the normal hour-to-hour and day-to-day variability seen in measured data.
-
-Ground Heat Transfer in EnergyPlus
-==================================
-
-Caution
--------
-
-For ground-contact surfaces in EnergyPlus, it is important to specify appropriate ground temperatures. Do not use the "undisturbed" ground temperatures from the weather data. These values are too extreme for the soil under a conditioned building. For best results, use the Slab or Basement program described in this section to calculate custom monthly average ground temperatures. This is especially important for residential applications and very small buildings. If one of these ground temperature preprocessors is not used, for typical commercial buildings in the USA, a reasonable default value is 2C less than the average indoor space temperature.
-
-Introduction
-------------
-
-There are two difficulties behind linking ground heat transfer calculations to EnergyPlus. One is the fact that the conduction calculations in EnergyPlus (and in DOE-2 and BLAST previously) are one-dimensional and the ground heat transfer calculations are two or three-dimensional. This causes severe modeling problems irrespective of the methods being used for the ground heat transfer calculation. The other difficulty is the markedly different time scales involved in the processes. Basically, the zone model is on an hour scale and the ground heat transfer is on a monthly time scale. The basic heat balance based zone model of EnergyPlus has to be considered as the foundation for building energy simulation at the present time and for some time in the future. Thus, it is necessary to be able to relate ground heat transfer calculations to that model.
-
-The heat balance zone model considers a single room or thermal zone in a building and performs a heat balance on it. A fundamental modeling assumption is that the faces of the enclosure are isothermal planes. A ground heat transfer calculation usually considers an entire building and the earth that surrounds it, resulting in non-isothermal face planes where there is ground contact. While it is not impossible to imagine multi-zone, whole building models that include the surrounding earth and non-isothermal building surfaces, such models will not be practical for some time in the future, and their usefulness even then is not clear.
-
-The EnergyPlus development team addressed the problem and decided that the most reasonable first step would be to partially decouple the ground heat transfer calculation from the thermal zone calculation. The most important parameter for the zone calculation is the outside face temperature of the building surface that is in contact with the ground. Thus this becomes a reasonable "separation plane" for the two calculations. It was further decided that the current usage of monthly average ground temperature was reasonable for this separation plane temperature as well, since the time scales of the building heat transfer processes are so much shorter than those of the ground heat transfer processes.
-
-Using the separation plane premise, the 3D ground heat transfer programs for slabs developed by Bahnfleth (1989, 1990) were modified by Clements (2004) to produce outside face temperatures. EnergyPlus permits separate monthly average inside temperatures as input. The program produces outside face temperatures for the core area and the perimeter area of the slab. It is described in the section "Use of the Ground Temperatures with Slabs" below.
-
-A 3D basement program also is included with EnergyPlus. This is described below in Using Ground Temperatures with Basements. It uses the same principle as the slab procedure; it determines the outside face (surface) temperature of the walls and floor of a basement in contact with the ground.
-
-It should be noted that either for slabs or basements the ground heat transfer is usually small unless the building is very small or has some special characteristics.
-
-Multiple Ground Temperatures shows how the OtherSideCoefficients object of EnergyPlus can be used to supply multiple ground temperatures.
-
-Use of the Ground Temperatures with Slabs
------------------------------------------
-
-The Slab program produces temperature profiles for the outside surface at the core and at the perimeter of the slab. It also produces the average based on the perimeter and core areas used in the calculation. This allows the user to apply the Slab temperatures one of two ways in EnergyPlus:
-
-*Option 1 - Core and Perimeter Temperatures*:  The EnergyPlus OtherSideCoefficients object can be used to provide two sets of twelve monthly average ground temperature values. In this way, both the perimeter and the core values from the Slab program can be used in the succeeding EnergyPlus run. This method assumes that the floor slab will be described using at least two different heat transfer surfaces. The use of OtherSideCoefficients to provide additional ground contact surfaces is described in detail in the "Multiple Ground Temperatures" section below.
-
-*Option 2 - Average Temperatures: * Use the monthly average temperatures produced by the Slab program in the EnergyPlus GroundTemperatures object. This will provide an average ground temperature at the outside face of any heat transfer surface whose OutsideFaceEnvironment field is set to "ground".
-
-EnergyPlus accepts twelve separate monthly average inside temperatures. In addition, it is possible to add an hourly sinusoidal variation of the inside temperature with a 24 hour period sine function. This was included to show the effect of something such as night setback on the face temperature. Generally, the effect is quite small.
-
-First the results for a monthly specified constant average inside temperature. The location is Minneapolis, and the slab is insulated.
-
-```
-Monthly Slab Outside Face Temperatures, C
-Perimeter Area: 304.00  Core Area: 1296.00
-Month   Average   Perimeter    Core      Inside
-1      17.67     16.11      18.03       18.0
-2      17.45     15.92      17.81       18.0
-3      17.43     16.07      17.74       18.0
-4      19.00     17.82      19.27       20.0
-5      19.24     18.23      19.48       20.0
-6      19.31     18.42      19.52       20.0
-7      20.92     20.14      21.11       22.0
-8      21.17     20.44      21.35       22.0
-9      21.22     20.45      21.40       22.0
-10      21.21     20.26      21.44       22.0
-11      19.62     18.54      19.88       20.0
-12      19.35     17.99      19.67       20.0
-```
-
-The resulting heat flux is shown below. The inside heat transfer coefficient and slab thermal properties are specified in the input file. For this example the total thermal resistance from the inside air to the slab bottom surface was 0.27 (m<sup>2</sup> C)/W. This value is controlled by the user with the inside heat transfer coefficient and slab thermal properties values in the slab program input file.
-
-
-<table class="table table-striped">
-<tr>
-<th>Month</th>
-<th>Average</th>
-<th>Perimeter</th>
-<th>Core</th>
-<th>Inside</th>
-<th>Perimeter Heat Flux W/m<sup>2</sup></th>
-<th>Average Heat Flux W/m<sup>2</sup></th>
-</tr>
-<tr>
-<td>1</td>
-<td>17.67</td>
-<td>16.11</td>
-<td>18.03</td>
-<td>18</td>
-<td>7.00</td>
-<td>1.22</td>
-</tr>
-<tr>
-<td>2</td>
-<td>17.45</td>
-<td>15.92</td>
-<td>17.81</td>
-<td>18</td>
-<td>7.70</td>
-<td>2.04</td>
-</tr>
-<tr>
-<td>3</td>
-<td>17.43</td>
-<td>16.07</td>
-<td>17.74</td>
-<td>18</td>
-<td>7.15</td>
-<td>2.11</td>
-</tr>
-<tr>
-<td>4</td>
-<td>19</td>
-<td>17.82</td>
-<td>19.27</td>
-<td>20</td>
-<td>8.07</td>
-<td>3.70</td>
-</tr>
-<tr>
-<td>5</td>
-<td>19.24</td>
-<td>18.23</td>
-<td>19.48</td>
-<td>20</td>
-<td>6.56</td>
-<td>2.81</td>
-</tr>
-<tr>
-<td>6</td>
-<td>19.31</td>
-<td>18.42</td>
-<td>19.52</td>
-<td>20</td>
-<td>5.85</td>
-<td>2.56</td>
-</tr>
-<tr>
-<td>7</td>
-<td>20.92</td>
-<td>20.14</td>
-<td>21.11</td>
-<td>22</td>
-<td>6.89</td>
-<td>4.00</td>
-</tr>
-<tr>
-<td>8</td>
-<td>21.17</td>
-<td>20.44</td>
-<td>21.35</td>
-<td>22</td>
-<td>5.78</td>
-<td>3.07</td>
-</tr>
-<tr>
-<td>9</td>
-<td>21.22</td>
-<td>20.45</td>
-<td>21.4</td>
-<td>22</td>
-<td>5.74</td>
-<td>2.89</td>
-</tr>
-<tr>
-<td>10</td>
-<td>21.21</td>
-<td>20.26</td>
-<td>21.44</td>
-<td>22</td>
-<td>6.44</td>
-<td>2.93</td>
-</tr>
-<tr>
-<td>11</td>
-<td>19.62</td>
-<td>18.54</td>
-<td>19.88</td>
-<td>20</td>
-<td>5.41</td>
-<td>1.41</td>
-</tr>
-<tr>
-<td>12</td>
-<td>19.35</td>
-<td>17.99</td>
-<td>19.67</td>
-<td>20</td>
-<td>7.44</td>
-<td>2.41</td>
-</tr>
-</table>
-
-Then for the same conditions, the results with a 2 degree C amplitude 24-hour sine wave variation. Notice that the inside temperatures are the same since they are monthly averages and the daily variation oscillates about the mean. The core and perimeter slab temperatures are affected slightly.
-
-```
-Monthly Slab Outside Face Temperatures, C
-Perimeter Area: 304.00  Core Area: 1296.00
-Month   Average   Perimeter    Core      Inside
-1      17.51     16.03      17.86       18.0
-2      17.29     15.85      17.63       18.0
-3      17.27     16.00      17.57       18.0
-4      18.87     17.77      19.13       20.0
-5      19.11     18.16      19.34       20.0
-6      19.17     18.34      19.37       20.0
-7      20.81     20.07      20.98       22.0
-8      21.05     20.36      21.21       22.0
-9      21.09     20.38      21.26       22.0
-10      21.08     20.19      21.29       22.0
-11      19.47     18.45      19.71       20.0
-12      19.20     17.92      19.51       20.0
-```
-
-
-An example of a 24-hour inside temperature profile for this case is shown below. The sine wave amplitude was 2 C.
-
-```
-Day       Hour   Perim Out Ts    Core Out Ts    Inside Temp
-1           1   17.30827       19.15832       18.51749
-1           2   17.29503       19.15274       18.99974
-1           3   17.30236       19.16732       19.41389
-1           4   17.32258       19.19376       19.73175
-1           5   17.34834       19.22526       19.93166
-1           6   17.37288       19.25529       20.00000
-1           7   17.39023       19.27798       19.93212
-1           8   17.39544       19.28838       19.73265
-1           9   17.38485       19.28117       19.41517
-1          10   17.35602       19.24733       19.00130
-1          11   17.30590       19.18686       18.51924
-1          12   17.23507       19.10210       18.00180
-1          13   17.14650       18.99703       17.48425
-1          14   17.04291       18.87713       17.00183
-1          15   16.92873       18.74895       16.58738
-1          16   16.81076       18.61963       16.26915
-1          17   16.69609       18.49656       16.06881
-1          18   16.59243       18.38671       16.00000
-1          19   16.50669       18.29626       16.06741
-1          20   16.44276       18.23010       16.26645
-1          21   16.40369       18.19161       16.58356
-1          22   16.38873       18.18218       16.99714
-1          23   16.39435       18.19834       17.47902
-1          24   16.41942       18.23298       17.99639
-```
-
-A plot of the daily profiles is shown below. Note that the inside temperature change of 4 C produces only a small change in the slab lower face temperature.
-
-![FigGrndXFer](media/image017.jpg)
-
-Figure 19. Daily Temperature Profiles (Slab)
-
-The resulting heat fluxes are shown below.  They can be compared with the fluxes shown above for the constant inside temperature run. The changes resulting from a fairly large 4 C daily temperature variation are probably not significant.
-
-
-
-<table class="table table-striped">
-<tr>
-<th>Month</th>
-<th>Average</th>
-<th>Perimeter</th>
-<th>Core</th>
-<th>Inside</th>
-<th>Perimeter Heat Flux W/m<sup>2</sup></th>
-<th>Average Heat Flux W/m<sup>2</sup></th>
-</tr>
-<tr>
-<td>1</td>
-<td>17.51</td>
-<td>16.03</td>
-<td>17.86</td>
-<td>18</td>
-<td>7.30</td>
-<td>1.81</td>
-</tr>
-<tr>
-<td>2</td>
-<td>17.29</td>
-<td>15.85</td>
-<td>17.63</td>
-<td>18</td>
-<td>7.96</td>
-<td>2.63</td>
-</tr>
-<tr>
-<td>3</td>
-<td>17.27</td>
-<td>16</td>
-<td>17.57</td>
-<td>18</td>
-<td>7.41</td>
-<td>2.70</td>
-</tr>
-<tr>
-<td>4</td>
-<td>18.87</td>
-<td>17.77</td>
-<td>19.13</td>
-<td>20</td>
-<td>8.26</td>
-<td>4.19</td>
-</tr>
-<tr>
-<td>5</td>
-<td>19.11</td>
-<td>18.16</td>
-<td>19.34</td>
-<td>20</td>
-<td>6.81</td>
-<td>3.30</td>
-</tr>
-<tr>
-<td>6</td>
-<td>19.17</td>
-<td>18.34</td>
-<td>19.37</td>
-<td>20</td>
-<td>6.15</td>
-<td>3.07</td>
-</tr>
-<tr>
-<td>7</td>
-<td>20.81</td>
-<td>20.07</td>
-<td>20.98</td>
-<td>22</td>
-<td>7.15</td>
-<td>4.41</td>
-</tr>
-<tr>
-<td>8</td>
-<td>21.05</td>
-<td>20.36</td>
-<td>21.21</td>
-<td>22</td>
-<td>6.07</td>
-<td>3.52</td>
-</tr>
-<tr>
-<td>9</td>
-<td>21.09</td>
-<td>20.38</td>
-<td>21.26</td>
-<td>22</td>
-<td>6.00</td>
-<td>3.37</td>
-</tr>
-<tr>
-<td>10</td>
-<td>21.08</td>
-<td>20.19</td>
-<td>21.29</td>
-<td>22</td>
-<td>6.70</td>
-<td>3.41</td>
-</tr>
-<tr>
-<td>11</td>
-<td>19.47</td>
-<td>18.45</td>
-<td>19.71</td>
-<td>20</td>
-<td>5.74</td>
-<td>1.96</td>
-</tr>
-<tr>
-<td>12</td>
-<td>19.2</td>
-<td>17.92</td>
-<td>19.51</td>
-<td>20</td>
-<td>7.70</td>
-<td>2.96</td>
-</tr>
-</table>
-
-
-
-Slab configuration Drawing
---------------------------
-
-The slab configuration used in the slab model is a "slab in grade" model. That is, the slab top surface is assumed level with the outside earth surface. If a "slab on grade" configuration, having the bottom surface of the slab level with the outside earth surface is desired, the best approximation is to use the horizontal insulation configuration. The edge of the slab will have a small thermal resistance due to the two dimensional path through the earth, but the effect is small. In any case, uninsulated slab edges are certainly not recommended in cold climates.
-
-![](media/image018.jpg)
-
-Figure 20. Slab-in-grade illustration
-
-Running the Slab Program
-------------------------
-
-EP-Launch can be used to run the Slab program using two different methods.
-
-If the Slab objects (see Description of the Objects in the E+SlabGHT.IDD) are located in the standard EnergyPlus IDF input file than the Single Input File and Group of Input File tabs of EP-Launch can be used and the Slab preprocessor will be called automatically during the simulation process. In this case the Slab objects should all appear with the object name starting with "**GroundHeatTransfer:Slab:**" This option also requires a **GroundHeatTransfer:Control** object in the EnergyPlus idf file (see Input Output Reference).
-
-If the Slab objects are located in a separate file, they should be run using the Slab option on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the Slab program.
-
-You can also run the slab program as a console application.  To execute it, we have provided the batch file:
-
-RunSlab
-
-Steps for running the program
-
-1)   Open a DOS command prompt window (Start à Programs à Accessories à Command Prompt)
-
-2)   Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
-
-C:
-
-CD \\&lt;rootfolder&gt;\&lt;/span>
-
-3)   Change to the specific folder for the console application:
-
-CD PreProcess\\GrndTempCalc
-
-4)   Run the program (for example use the example included with the install):
-
-RunSlab SlabExample USA\_IL\_Chicago-OHare\_TMY2
-
-In the following section, some description of modifying the batch file and details on files that the slab program uses are given.
-
-Technical Details on Files for Ground Heat Transfer with Slabs
---------------------------------------------------------------
-
-The slab program used to calculate the results is included with the EnergyPlus distribution. It requires an input file named GHTin.idf in input data file format. The needed corresponding idd file is SlabGHT.idd. An EnergyPlus weather file for the location is also needed. A batch file, RunSlab, is placed in the same folder with the program and sample files. To use it (Command mode or DOS mode), one may modify several important lines:
-
-```
-:Instructions:
-:  Complete the following path and program names.
-:  path names must have a following \\ or errors will happen
- set program\_path=
- set program\_name=Slab.exe
- set input\_path=
- set output\_path=
- set weather\_path=C:\\EnergyPlus\\WeatherData\\
-```
-
-and then in command mode issue the run command:
-
-```
-RunSlab myinput Chicago
-```
-
-Where you would have myinput.idf in "input\_path" and Chicago would be the name of the .epw file in the "weather\_path".
-
-You should set up the command mode so that it does not automatically close the window at the end of program termination if you want to see the commands as they run and know for sure that no errors occurred.
-
-Slab Program Output Files
--------------------------
-
-The following output files are created by the Slab program and saved in the output file path specified in the RunSlab.bat file:
-
-
-
-\*\_slab.ger - Error file. Input errors are reported here.
-
-\*\_slab.out - Summary of inputs, location data, and grid coordinates
-
-\*\_slab.gtp - Monthly ground temperatures and EnergyPlus idf objects
-
-
-
-### EnergyPlus idf Objects from Slab Program
-
-If the objects are placed in the normal EnergyPlus input IDF file using the "GroundHeatTransfer:Slab:" prefix, then the values resulting from the Slab preprocessor will be automatically included in the simulation at run time. The surfaces can reference these values using Outside Boundary Conditions of:
-
-* GroundSlabPreprocessorAverage
-
-* GroundSlabPreprocessorCore
-
-* GroundSlabPreprocessorPerimeter
-
-The objects that support this include:
-
-* BuildingSurface:Detailed
-
-* Wall:Detailed
-
-* RoofCeiling:Detailed
-
-* Floor:Detailed
-
-The slab program is capable of supplying the EnergyPlus idf objects needed to use the slab program outputs directly by copying the objects into the EnergyPlus idf file. The file containing these objects has the extension gtp, and an example is shown below. It contains the output temperatures and heat fluxes, and in addition it contains an OtherSideCoefficient object example as mentioned above, and three compact schedule objects that can be used to describe the average, core and perimeter temperatures directly in EnergyPlus. The Name in the compact schedule corresponds to the GroundTemperatureScheduleName in the OtherSideCoefficient object.
-
-================================================
-
- CHECK CONVERGENCE MESSAGE AT END OF THIS FILE!
-
- ================================================
-
-```
-   Monthly Slab Outside Face Temperatures, C and Heat Fluxes(loss), W/(m^2)
- Perimeter Area: 304.00  Core Area: 1296.00
-       Month   TAverage   TPerimeter    TCore      TInside AverageFlux PerimeterFlux CoreFlux
-          1      17.74     16.41        18.05       18.00       0.88        5.39       -0.17
-          2      17.49     16.15        17.81       18.00       1.73        6.29        0.66
-          3      17.45     16.23        17.74       18.00       1.86        6.02        0.88
-          4      18.96     17.86        19.22       20.00       3.51        7.24        2.64
-          5      19.22     18.22        19.45       20.00       2.66        6.04        1.86
-          6      19.28     18.38        19.49       20.00       2.44        5.48        1.73
-          7      20.83     19.98        21.03       22.00       3.96        6.87        3.28
-          8      21.12     20.39        21.29       22.00       2.98        5.47        2.40
-          9      21.18     20.46        21.35       22.00       2.76        5.22        2.19
-         10      21.17     20.23        21.39       22.00       2.82        6.02        2.08
-         11      19.64     18.63        19.88       20.00       1.22        4.63        0.42
-         12      19.36     18.14        19.65       20.00       2.16        6.30        1.19
-
-! OTHER SIDE COEFFICIENT OBJECT EXAMPLE FOR IDF FILE
- SurfaceProperty:OtherSideCoefficients,
- ExampleOSC,                !- OtherSideCoeff Name \*\*\*CHANGE THIS!\*\*\*
- 0,                         !- Combined convective/radiative film coefficient
- 1,                         !- N2,User selected Constant Temperature {C}
- 1,                         !- Coefficient modifying the user selected constant temperature
- 0,                         !- Coefficient modifying the external dry bulb temperature
- 0,                         !- Coefficient modifying the ground temperature
- 0,                         !- Coefficient modifying the wind speed term (s/m)
- 0,                         !- Coefficient modifying the zone air temperature
-                            !  part of the equation
- GroundTempCompactSchedName; !- Name of Schedule for values of const
-                            ! temperature. Schedule values replace N2.
-                            !  \*\*\*REPLACE WITH CORRECT NAME\*\*\*
-
-
-Schedule:Compact,
-MonthlyAveSurfaceTemp, !Name
-Temperature ,            !- ScheduleType
-Through:   1/31,
-For:AllDays,
-Until:24:00,
- 17.74    ,
-Through:   2/28,
-For:AllDays,
-Until:24:00,
- 17.49    ,
-Through:   3/31,
-For:AllDays,
-Until:24:00,
- 17.45    ,
-Through:   4/30,
-For:AllDays,
-Until:24:00,
- 18.96    ,
-Through:   5/31,
-For:AllDays,
-Until:24:00,
- 19.22    ,
-Through:   6/30,
-For:AllDays,
-Until:24:00,
- 19.28    ,
-Through:   7/31,
-For:AllDays,
-Until:24:00,
- 20.83    ,
-Through:   8/31,
-For:AllDays,
-Until:24:00,
- 21.12    ,
-Through:   9/30,
-For:AllDays,
-Until:24:00,
- 21.18    ,
-Through:  10/31,
-For:AllDays,
-Until:24:00,
- 21.17    ,
-Through:  11/30,
-For:AllDays,
-Until:24:00,
- 19.64    ,
-Through:  12/31,
-For:AllDays,
-Until:24:00,
- 19.36    ;
-
-<reduced for brevity> - compact schedules for MonthlyPerimeterTemp and MonthlyCoreTemp are included.
-
-  Convergence has been gained.
-```
-
-Description of the Objects in the E+SlabGHT.IDD
------------------------------------------------
-
-These objects also appear in the main Energy+.IDD file with the prefix "GroundHeatTransfer:Slab:"
-
-### Materials or GroundHeatTransfer:Slab:Materials Object
-
-The materials object gives an overall description of the ground heat transfer model.
-
-#### Field: NMAT: Number of Materials
-
-This field specifies the number of different materials that will be used in the model. Typically only a ground material and a slab material are used.
-
-#### Field: Albedo: Surface Albedo: NoSnow
-
-#### Field: Albedo: Surface Albedo: Snow
-
-Two fields specify the albedo value of the surface: first for no snow coverage days; second for days with snow coverage. The albedo is the solar reflectivity of the surface, and can vary from 0.05 for blacktop to 0.95 for fresh snow. Typical values for North America reported by Bahnfleth range from 0.16 to 0.4.
-
-#### Field EPSLW: Surface Emissivity: NoSnow
-
-#### Field EPSLW: Surface Emissivity: Snow
-
-This field specifies the long wavelength (thermal) emissivity of the ground surface. It is primarily important for nighttime radiation to the sky, and a value of 0.95 for both snow and no snow is reasonable.
-
-#### Field: Z0 Surface Roughness: NoSnow
-
-#### Field: Z0 Surface Roughness: Snow
-
-These two fields specify a surface roughness that is used in the determination of the convection heat transfer coefficient between the ground surface and the air. This roughness is based on boundary layer considerations, and specifies the height at which an experimentally measured velocity profile goes to zero. The units are centimeters, not meters. Typical values are 0.75 cm for no snow, and 0.05 cm for snow.
-
-#### Field: HIN: Indoor Hconv: Downward Flow
-
-#### Field: HIN: Indoor Hconv: Upward Flow
-
-These fields specify the combined convective and radiative heat transfer coefficient between the slab top inside surface and the room air for the cases where heat is flowing downward, and upward. The program toggles between the two if the direction of the heat flux changes. Typical values can be found in the ASHRAE Handbook of Fundamentals, but should be about 6 W/(m<sup>2</sup>-K) for downward heat flow and 9 W/(m<sup>2</sup>-K) for upward heat flow.
-
-The Materials object in the IDD is shown below.
-
-```idf
-Materials,
- N1, \field NMAT: Number of materials
-  \note typical 2
- N2, \field ALBEDO: Surface Albedo: No Snow
-  \note typical value= 0-1
- N3, \field ALBEDO: Surface Albedo: Snow
-  \note typical value= 0-1
- N4, \field EPSLW: Surface Emissivity: No Snow
-  \note typical value= 0.9
- N5, \field EPSLW: Surface Emissivity: Snow
-  \note typical value= 0.9
- N6, \field Z0: Surface Roughness: No Snow
-  \note typical value= 0-10 cm
- N7, \field Z0: Surface Roughness: Snow
-  \note typical value= 0-10
- N8, \field HIN: Indoor HConv: Downward Flow
-  \note typical value= 4-10
-  \units W/m2-K
- N9; \field HIN: Indoor HConv: Upward
-  \note typical value= 4-10
-  \units W/m2-K
-```
-
-
-### MatlProps or GroundHeatTransfer:Slab:MatlProps Object
-
-This object contains the material properties that describe the materials used in the model. The fields are quite self explanatory and consist of the following:
-
-#### Field: RHO: Slab Material Density
-
-#### Field: RHO: Soil Density
-
-These two fields specify the density of the slab material and the soil in SI units of kg/m<sup>3</sup>
-
-#### Field: CP: Slab CP
-
-#### Field: CP: Soil CP
-
-These two fields specify the specific heat of the slab and soil in SI units of J/(kg-K).
-
-#### Field: TCON: Slab K
-
-#### Field: TCON: Soil K
-
-These two fields specify the thermal conductivity of the slab and soil in W/(m<sup>2</sup>-K)
-
-The IDD object is shown below:
-
-```
-MatlProps,
-        N1, \field RHO: Slab Material density
-            \note typical value= 2300.0
-            \units kg/m3
-        N2, \field RHO: Soil Density
-            \note typical value= 1200.0
-            \units kg/m3
-        N3, \field CP: Slab CP
-            \note typical value=650.0
-            \units J/kg-K
-        N4, \field CP: Soil CP
-            \note typical value= 1200.0
-            \units J/kg-K
-        N5, \field TCON: Slab k
-            \note typical value= .9
-            \units W/m2-K
-        N6; \field TCON: Soil k
-            \note typical value= 1.0
-            \units W/m2-K
-```
-
-### BoundConds or GroundHeatTransfer:Slab:BoundConds Object
-
-This object supplies some of the boundary conditions used in the simulation.
-
-#### Field: EVTR: Is surface evapotranspiration modeled
-
-This field specifies whether or not to use the evapotransporation model. Evapotransportation comprises all of the processes at the ground surface the involve exchanges of latent heat. The inclusion of evapotransporation in the calculation has the greatest effect in warm dry climates, primarily on the ground surface temperature. This field can be used to turn the evapotransporation off and on to check sensitivity to it.
-
-#### Field: FIXBC: is the lower boundary at a fixed temperature
-
-This field permits using a fixed temperature at the lower surface of the model instead of a zero heat flux condition. This change normally has a very small effect on the results. If the flag is set to use a specified temperature, the program calculates an undisturbed temperature profile and used the value at the model depth. The model depth is set by the program using the domain size from the EquivAutoGrid object below.
-
-#### Field: TDEEPin
-
-The fixed lower level temperature as described in the FIXBC field.
-
-#### Field: USPHflag: Is the ground surface h specified by the user?
-
-This field flags the use of a user specified heat transfer coefficient on the ground surface. This condition is used primarily for testing. For normal runs (USPHflag is FALSE), the program calculates the heat transfer coefficient using the weather conditions.
-
-#### Field: USERH: User specified ground surface heat transfer coeff
-
-This field supplies the value of the heat transfer coefficient if USPHflag is TRUE. W/(m<sup>2</sup>-K)
-
-The BoundConds object is shown below:
-
-```
-BoundConds,
-        A1, \field EVTR: Is surface evapotranspiration modeled
-            \type choice
-            \key TRUE
-            \key FALSE
-        A2, \field FIXBC: is the lower boundary at a fixed temperature
-            \type choice
-            \key TRUE
-            \key FALSE
-            \note FALSE selects the zero flux lower boundary condition
-        N1, \field TDEEPin,
-            \note User input lower boundary temperature if FIXBC is TRUE
-            \units C
-            \note Blank for FIXBC FALSE or
-            \note to use the calculated 1-D deep ground temperature.
-        A3, \field USRHflag: Is the ground surface h specified by the user?
-            \type choice
-            \key TRUE
-            \key FALSE
-        N2; \field USERH: User specified ground surface heat transfer coeff
-            \units W/(m2-K)
-            \note Used only if USRHflag is TRUE
-```
-
-### BldgProps or GroundHeatTransfer:Slab:BldgProps Object
-
-This object provides information about the building and its operating conditions.
-
-#### Field: IYRS Number of years to iterate
-
-This field specifies the number of years to iterate. This means that the simulation comes to an either an annual steady periodic condition by converging to a tolerance (see ConvTol field) or it runs for this number of years. A ten year maximum is usually sufficient. It is important to note that the ground heat transfer behavior will change during the first several years of operating a ground contact structure. It takes several years to change from the undisturbed profile to the disturbed profile under a building.
-
-#### Field: Shape Slab shape
-
-Use only the value 0 here. Only a rectangular shape is implemented.
-
-#### Field: HBLDG: Building Height
-
-This field supplies the building height. This is used to calculate the building shadowing on the ground. Height is in meters.
-
-#### Field: TIN1 - TIN12 &lt;month&gt; Indoor Average temperature set point
-
-The next twelve fields specify the average indoor building set point temperatures for each month of the year. These fields are useful for simulating a building that is not temperature controlled for some of the year. In such a case, the average indoor set point temperatures can be obtained by first running the model in EnergyPlus with an insulated floor boundary condition, and then using the resulting monthly average zone temperatures in these fields.
-
-#### Field: TINAmp: Daily Indoor sine wave variation amplitude
-
-This field permits imposing a daily sinusoidal variation in the indoor setpoint temperature to simulate the effect of a setback profile. The value specified will be the amplitude of the sine wave.
-
-#### Field: ConvTol: Convergence Tolerance
-
-This final field specifies the convergence tolerance used to control the iteration. When the temperature change of all nodes is less than the convergence value, iteration ceases.
-
-The entire BldgProps Object is shown below.
-
-```
-BldgProps,
-      N1, \field IYRS: Number of years to iterate
-          \note typical value= 10
-      N2, \field Shape: Slab shape
-          \note only value= 0
-      N3, \field HBLDG: Building height
-          \note typical value= 0-20
-          \units m
-      N4, \field TIN1: January Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N5, \field TIN2: February Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N6, \field TIN3: March Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N7, \field TIN4: April Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N8, \field TIN5: May Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N9, \field TIN6: June Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N10, \field TIN7: July Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N11, \field TIN8: August Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N12, \field TIN9: September Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N13, \field TIN10: October Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N14, \field TIN11: NovemberIndoor Average temperature set point
-          \note typical value=22
-          \units C
-      N15, \field TIN12: December Indoor Average temperature set point
-          \note typical value=22
-          \units C
-      N16, \field TINAmp: Daily Indoor sine wave variation amplitude
-           \note typical value: 0
-           \units C
-      N17; \field ConvTol: Convergence Tolerance
-           \note typical value= 0.1
-```
-
-### Insulation or GroundHeatTransfer:Slab:Insulation  Object
-
-This object supplies the information about insulation used around the slab. There are two possible configurations: under the slab or vertical insulation around the slab.
-
-#### Field RINS: R value of under slab insulation
-
-This field provides the thermal resistance value of the under slab insulation. It should be zero if the vertical insulation configuration is selected. Units are m<sup>2</sup> K/W.
-
-#### Field DINS: Width of strip of under slab insulation
-
-This specifies the width of the perimeter strip of insulation under the slab in meters. Again a zero value should be used for the vertical insulation configuration. Units are m.
-
-#### Field RVINS: R value of vertical insulation
-
-This field specifies the thermal resistance of the vertical insulation. It should be zero if the under slab insulation configuration is in effect. Units are m<sup>2</sup> K/W.
-
-#### Field ZVINS: Depth of vertical insulation
-
-This field specifies the depth of the vertical insulation into the ground in meters. Note that it starts at the slab upper surface and extends into the ground. Only .2 .4 .6 .8 1.0 1.5 2.0 2.5  or 3.0 m should be used. Units are m.
-
-#### Field IVINS: Flag: Is there vertical insulation?
-
-This final field specifies that vertical the vertical insulation configuration is being used. The value of 1 specifies yes and 0 specifies no.
-
-The Insulation object is shown below.
-
-```
-Insulation,
-        N1, \field RINS: R value of under slab insulation
-            \note typical value= 0-2.0
-            \units m2-K/W
-        N2, \field DINS: Width of strip of under slab insulation
-            \note typical value= 0-2.0
-            \units m
-        N3, \field RVINS: R value of vertical insulation
-            \note typical value= 0-3.0
-            \units m2-K/W
-        N4, \field ZVINS: Depth of vertical insulation
-            \note only use values= .2 .4 .6 .8 1.0 1.5 2.0 2.5 3.0
-            \units m
-        N5; \field IVINS: Flag: Is there vertical insulation
-            \note values: 1=yes 0=no
-```
-
-### EquivalentSlab or GroundHeatTransfer:Slab:EquivalentSlab Object
-
-This object provides the basic information for running a model that uses the area over perimeter ratio of the slab to determine the size of an equivalent rectangular slab.
-
-#### Field APRatio: The area to perimeter ratio for this slab
-
-This field specifies the area over perimeter ratio of the slab in meters.
-
-#### Field SLABDEPTH: Thickness of slab on grade
-
-This field specifies the thickness of the slab in meters. Note that the slab top surface is level with the ground surface, so this is the depth into the ground. The slab depth has a significant effect on the temperature calculation, and it is also important for the auto-grid process. The finite difference grids are set in such a way that they use the slab thickness to determine the vertical grid spacing. Because of this, autogridding will fail if the slab thickness is specified larger than 0.25 meters. The program also is set up so that the slab is a single finite difference cell in the vertical direction. Thus, if the slab thickness is set too large, the accuracy of the calculation may be suspect. The results with three different slab thicknesses are shown below.
-
-All other inputs for the runs were the same. It is clear that the slab thickness has a significant effect because of the horizontal component of conduction in both directions in the slab.
-
-#### Field CLEARANCE: Distance from edge of slab to domain edge
-
-This field specifies the distance from the slab to the edge of the area that will be modeled with the grid system. It is the basic size dimension that is used to set the horizontal extent of the domain. The units are meters, and 15 meters is a reasonable value.
-
-#### Field ZCLEARANCE: Distance from bottom of slab to domain bottom
-
-This field specifies the vertical distance from the slab to the bottom edge of the area that will be modeled with the grid system. It is the basic size dimension that is used to set vertical extent of the domain. The units are meters, and 15 meters is a reasonable value.
-
-The object is shown below.
-
-```
-EquivalentSlab,
-\memo Using an equivalent slab allows non-rectangular shapes to be modeled accurately
-        N1, \field APRatio: The area to perimeter ratio for this slab
-            \units m
-        N2, \field SLABDEPTH: Thickness of slab on grade
-            \note typical value= 0.1
-            \units m
-        N3, \field CLEARANCE: Distance from edge of slab to domain edge
-            \note typical value= 15.0
-            \units m
-        N4; \field ZCLEARANCE: Distance from bottom of slab to domain bottom
-            \note typical value= 15.0
-            \units m
-```
-
-![GHTSlabs](media/image019.jpg)
-
-Figure 21. Graph of Slab Outside Temperature vs Slab Thickness
-
-**The EquivSlab object and the EquivAutoGrid Objects that follow have been replaced by the EquivalentSlab object above.  They are included in the idd so that old idf files can still be read.**
-
-### EquivSlab Object - Obsolete
-
-This object provides the basic information for running a model that uses the area over perimeter ratio of the slab to determine the size of an equivalent rectangular slab.
-
-#### Field APRatio: The area to perimeter ratio for this slab
-
-This field specifies the area over perimeter ratio of the slab in meters.
-
-#### Field: EquivSizing
-
-This field value should be TRUE. This means that the program will determine the dimensions of the equivalent slab that satisfactorily models the A/P ratio.
-
-The object is shown below.
-
-```
-EquivSlab,
-\memo Using an equivalent slab allows non-rectangular shapes to be modeled accurately
-\memo The simulation default should be EquivSizing=True
-        N1, \field APRatio: The area to perimeter ratio for this slab
-            \units m
-        A1; \field EquivSizing:
-            \note Flag: Will the dimensions of an equivalent slab
-            \note be calculated (TRUE) or will the dimensions be input directly? (FALSE)
-            \note It is recommended that EnergyPlus users use TRUE.
-```
-
-### EquivAutoGrid Object - Obsolete
-
-This object provides the information needed by the program to automatically generate the calculation grid when the slab is described as an equivalent slab. It is necessary for EnergyPlus users because equivalent slab is the appropriate option.
-
-#### Field SLABDEPTH: Thickness of slab on grade
-
-This field specifies the thickness of the slab in meters. Note that the slab top surface is level with the ground surface, so this is the depth into the ground. The slab depth has a significant effect on the temperature calculation, and it is also important for the auto-grid process. The finite difference grids are set in such a way that they use the slab thickness to determine the vertical grid spacing. Because of this, autogridding will fail if the slab thickness is specified larger than 0.25 meters. The program also is set up so that the slab is a single finite difference cell in the vertical direction. Thus, if the slab thickness is set too large, the accuracy of the calculation may be suspect. The results with three different slab thicknesses are shown below.
-
-All other inputs for the runs were the same. It is clear that the slab thickness has a significant effect because of the horizontal component of conduction in both directions in the slab.
-
-#### Field CLEARANCE: Distance from edge of slab to domain edge
-
-This field specifies the distance from the slab to the edge of the area that will be modeled with the grid system. It is the basic size dimension that is used to set both the horizontal and vertical extent of the domain. The units are meters, and 15 meters is a reasonable value.
-
-The EquivAutoGrid object is shown below.
-
-```
-EquivAutoGrid, \memo  EquivAutoGrid only necessary when EquivSizing is true
-               \memo  EnergyPlus users normally use this option.
-        N1, \field SLABDEPTH: Thickness of slab on grade
-            \note typical value= 0.1
-            \units m
-        N2; \field CLEARANCE: Distance from edge of slab to domain edge
-            \note typical value= 15.0
-            \units m
-```
-
-### Additional Objects
-
-There are five additional objects in the IDD that can be used under very special situations by researchers who want to generate special calculation grids. They are normally not useful to EnergyPlus users. They will be shown as IDD sections only. They do not need to be in the IDF.
-
-```
-AutoGrid,   \memo AutoGrid only necessary when EquivSizing is false
-            \memo  Not normally needed by EnergyPlus users.
-        N1, \field SLABX: X dimension of the building slab
-            \note typical values= 0-60.0
-            \units m
-        N2, \field SLABY: Y dimension of the building slab
-            \note typical values= 0-60.0
-            \units m
-        N3, \field SLABDEPTH: Thickness of slab on grade
-            \note typical value= .1
-            \units m
-        N4; \field CLEARANCE: Distance from edge of slab to domain edge
-            \note typical value= 15.0
-            \units m
-
-ManualGrid, \memo Manual Grid only necessary using manual gridding (not recommended)
-            \memo   Used only in special cases.
-        N1, \field NX: Number of cells in the X direction
-            \note typical values= 15
-        N2, \field NY: Number of cells in the Y direction
-            \note typical values= 15
-        N3, \field NZ: Number of cells in the Z direction
-            \note typical values= 15
-        N4, \field IBOX: X direction cell indicator of slab edge
-            \note typical values= 1-10
-        N5; \field JBOX: Y direction cell indicator of slab edge
-            \note typical values= 1-10
-
-XFACE,  \memo This is only needed when using manual gridding (not recommended)
-        \memo XFACE: X Direction cell face coordinates: m
-  N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
-  N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26, N27, N28, N29,
-  N30, N31, N32, N33, N34, N35, N36, N37, N38, N39, N40;
-
-YFACE,  \memo This is only needed when using manual gridding (not recommended)
-        \memo YFACE: Y Direction cell face coordinates: m,
-  N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
-  N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26, N27, N28, N29,
-  N30, N31, N32, N33, N34, N35, N36, N37, N38, N39, N40;
-
-ZFACE,  \memo This is only needed when usuing manual gridding (not recommended)
-        \memo ZFACE: Z Direction cell face coordinates: m
-        N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
-        N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25;
-```
-
-### Sample IDF File - Slab Program
-
-A sample IDF file is shown below.
-
-```idf
-
-!-Generator IDFEditor 1.12
-!-NOTE: All comments with '!-' are ignored by the IDFEditor and are generated automatically.
-!-      Use '!' comments if they need to be retained when using the IDFEditor.
-
-!-   ===========  ALL OBJECTS IN CLASS: MATERIALS ===========
-
-Materials,
- 2,           !- NMAT: Number of materials
- 0.158,       !- ALBEDO: Surface Albedo: No Snow
- 0.379,       !- ALBEDO: Surface Albedo: Snow
- 0.9,         !- EPSLW: Surface Emissivity: No Snow
- 0.9,         !- EPSLW: Surface Emissivity: Snow
- 0.75,        !- Z0: Surface Roughness: No Snow
- 0.03,        !- Z0: Surface Roughness: Snow
- 6.13,        !- HIN: Indoor HConv: Downward Flow {W/m2-K}
- 9.26;        !- HIN: Indoor HConv: Upward {W/m2-K}
-
-!-   ===========  ALL OBJECTS IN CLASS: MATLPROPS ===========
-
-MatlProps,
- 2300,        !- RHO: Slab Material density {kg/m3}
- 1200,        !- RHO: Soil Density {kg/m3}
- 653,         !- CP: Slab CP {J/kg-K}
- 1200,        !- CP: Soil CP {J/kg-K}
- 0.93,        !- TCON: Slab k {W/m-K}
- 1;           !- TCON: Soil k {W/m-K}
-
-!-   ===========  ALL OBJECTS IN CLASS: BOUNDCONDS ===========
-
-BoundConds,
- TRUE,        !- EVTR: Is surface evapotranspiration modeled
- TRUE,        !- FIXBC: is the lower boundary at a fixed temperature
- FALSE;       !- OLDTG: is there an old ground temperature file
-
-!-   ===========  ALL OBJECTS IN CLASS: BLDGPROPS ===========
-
-BldgProps,
- 10,          !- IYRS: Number of years to iterate
- 0,           !- Shape: Slab shape
- 4,           !- HBLDG: Building height {m}
- 18,          !- TIN1: January Indoor Average temperature set point {C}
- 18,          !- TIN2: February Indoor Average temperature set point {C}
- 18,          !- TIN3: March Indoor Average temperature set point {C}
- 20,          !- TIN4: April Indoor Average temperature set point {C}
- 20,          !- TIN5: May Indoor Average temperature set point {C}
- 20,          !- TIN6: June Indoor Average temperature set point {C}
- 22,          !- TIN7: July Indoor Average temperature set point {C}
- 22,          !- TIN8: August Indoor Average temperature set point {C}
- 22,          !- TIN9: September Indoor Average temperature set point {C}
- 22,          !- TIN10: October Indoor Average temperature set point {C}
- 20,          !- TIN11: NovemberIndoor Average temperature set point {C}
- 20,          !- TIN12: December Indoor Average temperature set point {C}
- 0,           !- TINAmp: Daily sine wave variation amplitude {C}
- 0.10;        !- ConvTol: Convergence Tolerance
-
-!-   ===========  ALL OBJECTS IN CLASS: INSULATION ===========
-
-Insulation,
- 0.,          !- RINS: R value of under slab insulation {m2-K/W}
- 0.,          !- DINS: Width of strip of under slab insulation {m}
- 2.0,         !- RVINS: R value of vertical insulation {m2-K/W}
- 2.0,         !- ZVINS: Depth of vertical insulation {m}
- 1;           !- IVINS: Flag: Is there vertical insulation
-
-!-   ===========  ALL OBJECTS IN CLASS: EQUIVSLAB ===========
-
-EquivalentSlab,
- 10,          !- APRatio: The area to perimeter ratio for this slab {m}
- 0.1,         !- SLABDEPTH: Thickness of slab on grade {m}
- 15,          !- CLEARANCE: Distance from edge of slab to domain edge {m}
- 10;          !-ZCLEARANCE: Distance from bottom of slab to domain bottom
-```
-
-
-Using Ground Temperatures with Basements
-----------------------------------------
-
-The basement routine is used to calculate the face (surface) temperatures on the outside of the basement wall or the floor slab. This is the plane between the outside insulation and the basement wall. The insulation thermal resistance can range from zero (no insulation) to any reasonable value. The units are K/(W/m<sup>2</sup>). The program will simulate two conditions: full insulation from grade to the footing or half insulation that extends halfway down from grade to footing. The temperature on this plane is used with the OtherSideCoefficients object in EnergyPlus to supply the outside face temperature of the walls or slab.
-
-![GHTfigx](media/image020.jpg)
-
-Figure 22. Basement Configuration
-
-
-
-The output from the program is a csv file, named MonthlyResults.csv, as shown below.
-
-![GHTfigx](media/image021.jpg)
-
-Figure 23. Output from Basement program
-
-Column B gives the basement zone temperature. This can vary month by month as will be explained later. Column C is the monthly average wall outside face temperature, as shown in the diagram above. Column D is the corresponding average monthly average inside wall face temperature. Columns E and F contain the same information for the basement floor slab. Columns G-J contain the same information for the upper half and the lower half of the basement walls.
-
-Columns K through N contain the monthly average heat flux for the floor, the walls, the upper half of the walls and the lower half of the walls. The flux is reported in units of W/m<sup>2</sup>.
-
-The program also produces an output file named EPObjects.TXT. This file contains the necessary idf objects to make it easy to include the wall outside surface temperatures in an EnergyPlus input file. Idf objects for all of the temperatures in the output file shown above are included. These objects are explained in detail in the section Using the Interface Surface Temperature Results in EnergyPlus.
-
-Running the Basement Program
-----------------------------
-
-EP-Launch can be used to run the Basement program.
-
-If the Basement Objects (see The Basement idd below) are located in the standard EnergyPlus IDF input file than the Single Input File and Group of Input File tabs of EP-Launch can be used and the Basement preprocessor will be called automatically during the simulation process. In this case the Basement objects should all appear with the object name starting with "**GroundHeatTransfer:Basement:**" This option also requires a **GroundHeatTransfer:Control** object in the EnergyPlus idf file (see Input Output Reference).
-
-If the Basement objects are located in a separate file, they should be run using the Basement option on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the Basement program.
-
-You can also run the Basement program as a console application. To execute it, we have provided the batch file:
-
-RunBasement
-
-Steps for running the program
-
-1)   Open a DOS command prompt window (Start -&gt; Programs -&gt; Accessories -&gt; Command Prompt)
-
-2)   Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
-
-C:
-
-CD \\&lt;rootfolder&gt;\&lt;/span>
-
-3)   Change to the specific folder for the console application:
-
-CD PreProcess\\GrndTempCalc
-
-4)   Run the program (for example use the example included with the install):
-
-RunBasement BasementExample USA\_IL\_Chicago-OHare\_TMY2
-
-In the following section, some description of modifying the batch file and details on files that the basement program uses are given.
-
-Technical Details on Files for Ground Heat Transfer with Basements
-------------------------------------------------------------------
-
-The basement program used to calculate the results is included with the EnergyPlus distribution. It requires an input file named BasementGHTin.idf in input data file format. The needed corresponding idd file is BasementGHT.idd. An EnergyPlus weather file for the location is also needed. A batch file, RunBasement, is placed in the same folder with the program and sample files. To use it (Command mode or DOS mode), one may modify several important lines:
-
-```
-:Instructions:
-:  Complete the following path and program names.
-:  path names must have a following \\ or errors will happen
- set program\_path=
- set program\_name=Basement.exe
- set input\_path=
- set output\_path=
- set weather\_path=C:\\EnergyPlus\\WeatherData\\
-```
-
-and then in command mode issue the run command:
-
-```
-RunBasement myinput Chicago
-```
-
-Where you would have myinput.idf in "input\_path" and Chicago would be the name of the .epw file in the "weather\_path".
-
-You should set up the command mode so that it does not automatically close the window at the end of program termination if you want to see the commands as they run and know for sure that no errors occurred.
-
-Basement Program Output Files
------------------------------
-
-The following output files are created by the Basement program and saved in the output file path specified in the RunBasement.bat file:
-
-
-
-\*.audit - Audit file. Input errors are reported here as well as other information about the progress of the program..
-
-\*.out - Summary of inputs, location data, and grid coordinates
-
-\*.csv - Monthly temperatures and fluxes for each surface.
-
-\*.idf - the EPObjects.txt file - ready to be included in an EnergyPlus input file (idf)
-
-The Basement idd
-----------------
-
-The basement idd objects and fields are shown below. These objects also appear in the main Energy+.IDD file with the prefix "GroundHeatTransfer:Basement:"
-
-```
-! Basement foundation heat transfer module Input Data Dictionary file
-! Created:    August 18, 2000
-! Written by: Edward Clements
-! Modified for EnergyPlus Auxiliary Application by C. O. Pedersen 10/04
-! Description format: FORTRAN var.: description, units, typ. values
-
-SimParameters,
-      N1,\field F: Multiplier for the ADI solution:
-         \note 0<F<1.0,
-         \note typically 0.1 (0.5 for high k soil]
-      N2; \field IYRS: Maximum number of yearly iterations:
-         \note typically 15-30]
-
-MatlProps,
-     N1, \field NMAT: Number of materials in this domain
-         \maximum 6
-     N2, \field Density for Foundation Wall
-         \note typical value 2243
-         \units kg/m3
-     N3, \field density for Floor Slab
-         \note typical value 2243
-         \units kg/m3
-     N4, \field density for Ceiling
-         \note typical value 311
-         \units kg/m3
-     N5, \field density for Soil
-         \note typical value 1500
-         \units kg/m3
-     N6, \field density for Gravel
-         \note typical value 2000
-         \units kg/m3
-     N7, \field density for Wood
-         \note typical value 449
-         \units kg/m3
-     N8,  \field Specific heat for foundation wall
-          \note typical value 880
-          \units J/kg-K
-     N9,  \field Specific heat for floor slab
-          \note typical value 880
-          \units J/kg-K
-     N10, \field Specific heat for ceiling
-          \note typical value 1530
-          \units J/kg-K
-     N11, \field Specific heat for soil
-          \note typical value 840
-          \units J/kg-K
-     N12, \field Specific heat for gravel
-          \note typical value 720
-          \units J/kg-K
-     N13, \field Specific heat for wood
-          \note typical value 1530
-          \units J/kg-K
-     N14, \field Thermal conductivity for foundation wall
-          \note typical value 1.4
-          \units W/m-K
-     N15, \field Thermal conductivity for floor slab
-          \note typical value 1.4
-          \units W/m-K
-     N16, \field Thermal conductivity for ceiling
-          \note typical value 0.09
-          \units W/m-K
-     N17,  \field thermal conductivity for soil
-          \note typical value 1.1
-          \units W/m-K
-     N18, \field thermal conductivity for gravel
-          \note typical value 1.9
-          \units W/m-K
-     N19; \field thermal conductivity for wood
-          \note typical value 0.12
-          \units W/m-K
-
-
-Insulation,
-     N1, \field REXT: R Value of any exterior insulation, K/(W/m2)]
-         \units m2-K/W
-     A1; \field INSFULL: Flag: Is the wall fully insulated?
-         \note  True for full insulation
-         \note  False for insulation half way down side wall from grade line
-
-SurfaceProps,
-     N1, \field ALBEDO: Surface albedo for No snow conditions
-         \note typical value 0.16
-     N2, \field ALBEDO: Surface albedo for snow conditions
-         \note typical value 0.40
-     N3, \field EPSLN: Surface emissivity No Snow
-         \note typical value 0.94
-     N4, \field EPSLN: Surface emissivity  with Snow
-         \note typical value 0.86
-     N5, \field VEGHT: Surface roughness No snow conditions,cm
-         \note typical value 6.0
-         \units cm
-     N6, \field VEGHT: Surface roughness Snow conditions, cm, ]
-         \note typical value 0.25
-         \units cm
-     A1; \field PET: Flag, Potential evapotranspiration on? T/F]
-         \note  Typically, PET is True
-
-BldgData,
-     N1, \field DWALL: Wall thickness,
-         \note typical value .2]
-         \units m
-     N2, \field DSLAB: Floor slab thickness,
-         \units m
-         \maximum 0.25
-     N3, \field DGRAVXY: Width of gravel pit beside basement wall
-         \units  m
-     N4, \field DGRAVZN: Gravel depth extending above the floor slab
-         \units m
-     N5; \field DGRAVZP: Gravel depth below the floor slab,
-         \units m
-         \note typical value 0.1
-
-Interior,
-   A1, \field COND: Flag: Is the basement conditioned?
-       \note TRUE or FALSE
-       \note for EnergyPlus this should be TRUE
-   N1, \field HIN: Downward convection only heat transfer coefficient
-       \units W/m2-K
-   N2, \field HIN: Upward convection only heat transfer coefficient
-       \units W/m2-K
-   N3, \field HIN: Horizontal convection only heat transfer coefficient
-       \units W/m2-K
-   N4, \field HIN: Downward combined (convection and radiation) heat transfer coefficient
-       \units W/m2-K
-   N5, \field HIN: Upward combined (convection and radiation) heat transfer coefficient
-       \units W/m2-K
-   N6; \field HIN: Horizontal combined (convection and radiation) heat transfer coefficient
-       \units W/m2-K
-
-ComBldg,
-\memo ComBldg contains the monthly average temperatures (C) and possibility of daily variation amplitude
-   N1,  \field January average temperature
-        \units C
-   N2,  \field February average temperature
-        \units C
-   N3,  \field March average temperature
-        \units C
-   N4,  \field April average temperature
-        \units C
-   N5,  \field May average temperature
-        \units C
-   N6,  \field June average temperature
-        \units C
-   N7,  \field July average temperature
-        \units C
-   N8,  \field August average temperature
-        \units C
-   N9,  \field September average temperature
-        \units C
-   N10, \field October average temperature
-        \units C
-   N11, \field November average temperature
-        \units C
-   N12, \field December average temperature
-        \units C
-   N13; \field Daily variation sine wave amplitude
-        \units C
-        \note (Normally zero, just for checking)
-
-EquivSlab,  !  Supplies the EquivSizing Flag
-    ! Using an equivalent slab allows non-rectangular shapes to be
-    !    modeled accurately.
-    ! The simulation default should be EquivSizing=True
-   N1, \field APRatio: The area to perimeter ratio for this slab
-       \ units m
-   A1; \field EquivSizing: Flag
-         \note Will the dimensions of an equivalent slab be calculated (TRUE)
-         \note or will the dimensions be input directly? (FALSE)]
-         \note Only advanced special simulations should use FALSE.
-
-EquivAutoGrid,
-     \memo EquivAutoGrid necessary when EquivSizing=TRUE, TRUE is is the normal case.
-       N1, \field CLEARANCE: Distance from outside of wall to edge of 3-D ground domain
-         \units m
-         \note typical value 15m
-       N2, \field SlabDepth: Thickness of the floor slab
-         \units m
-         \note typical value 0.1m
-       N3; \field BaseDepth: Depth of the basement wall below grade
-         \units m
-
-!
-! ******** The following input objects are required only for special cases.
-!
-
-AutoGrid,   ! NOTE: AutoGrid only necessary when EquivSizing is false
-! If the modelled building is not a rectangle or square, Equivalent
-! sizing MUST be used to get accurate results
-       N1, \field CLEARANCE: Distance from outside of wall to edge, 15m]
-       N2, \field SLABX: X dimension of the building slab, 0-60.0 m]
-       N3, \field SLABY: Y dimension of the building slab, 0-60.0 m]
-       N4, \field ConcAGHeight: Height of the fndn wall above grade, m]
-       N5, \field SlabDepth: Thickness of the floor slab, m, 0.1]
-       N6; \field BaseDepth: Depth of the basement wall below grade, m]
-
-ManualGrid, ! NOTE: Manual Grid only necessary using manual gridding
-!  (not recommended)
-       N1, \field NX: Number of cells in the X direction: 20]
-       N2, \field NY: Number of cells in the Y direction: 20]
-       N3, \field NZAG: Number of cells in the Z direction
-!              above grade: 4 Always]
-       N4, \field NZBG: Number of cells in Z dir. below grade: 10-35]
-       N5, \field IBASE: X direction cell indicator of slab edge: 5-20]
-       N6, \field JBASE: Y direction cell indicator of slab edge: 5-20]
-       N7; \field KBASE: Z direction cell indicator
-!              of the top of the floor slab: 5-20]
-
-XFACE,       ! NOTE: This is only needed when using manual gridding
-!  (not recommended)
-!       [XFACE: X Direction cell face coordinates: m]
-       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
-       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
-       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
-       N39, N40, N41, N42, N43, N44;
-
-YFACE,  !NOTE: This is only needed when using manual gridding
-!  (not recommended)
-!       [YFACE: Y Direction cell face coordinates: m],
-       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
-       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
-       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
-       N39, N40, N41, N42, N43, N44;
-
-ZFACE,  !NOTE: This is only needed when using manual gridding
-!  (not recommended)
-!       [ZFACE: Z Direction cell face coordinates: m]
-       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
-       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
-       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
-      N39, N40;
-```
-
-Description of the Objects in the BasementGHT.idd
--------------------------------------------------
-
-These objects also appear in the main Energy+.IDD file with the prefix "GroundHeatTransfer:Basement:"
-
-### SimParameters or GroundHeatTransfer:Basement:SimParameters Object
-
-#### Field:  F: Multiplier for the ADI solution:
-
-This field specifies an alternating direction iteration scheme multiplier. It should normally be set to 0.1. It can be increased if the soil conductivity is high.
-
-#### Field: IYRS: Maximum number of yearly iterations:
-
-This specifies the maximum number of years the simulation will be allowed to run. If convergence is reached, the simulation will not run this long. It can be used to stop simulation before quasi steady convergence state is reached.
-
-### MatlProps or GroundHeatTransfer:Basement:MatlProps Object
-
-#### Field: NMAT: Number of materials in this domain
-
-This field specifies the number of materials whose properties are going to be specified. The order of the materials is not adjustable so six materials need to be specified. For the EnergyPlus basement application, only the foundation wall, floor slab, soil, and gravel are used.
-
-#### Field: Density for Foundation Wall
-
-This field is the density (kg/m3) of the foundation wall. Typical value is 2243.
-
-#### Field: Density for Floor Slab
-
-This field is the density (kg/m3) of the floor slab. Typical value is 2243.
-
-#### Field: Density for Ceiling
-
-This field is the density (kg/m3) of the ceiling. Typical value is 311.
-
-#### Field: Density for Soil
-
-This field is the density (kg/m3) of soil. Typical value is 1500.
-
-#### Field: Density for Gravel
-
-This field is the density (kg/m3) of gravel. Typical value is 2000.
-
-#### Field: Density for Wood
-
-This field is the density (kg/m3) of wood. Typical value is 449.
-
-#### Field: Specific Heat for Foundation Wall
-
-This field is the specific heat (J/kg-K) of the foundation wall. Typical value is 880.
-
-#### Field: Specific Heat for Floor Slab
-
-This field is the specific heat (J/kg-K) of the floor slab. Typical value is 880.
-
-#### Field: Specific Heat for Ceiling
-
-This field is the specific heat (J/kg-K) of the ceiling. Typical value is 1530.
-
-#### Field: Specific Heat for Soil
-
-This field is the specific heat (J/kg-K) of soil. Typical value is 840.
-
-#### Field: Specific Heat for Gravel
-
-This field is the specific heat (J/kg-K) of gravel. Typical value is 720.
-
-#### Field: Specific Heat for Wood
-
-This field is the specific heat (J/kg-K) of wood. Typical value is 1530.
-
-#### Field: Thermal Conductivity for Foundation Wall
-
-This field is the thermal conductivity (W/m-K) of the foundation wall. Typical value is 1.4.
-
-#### Field: Thermal Conductivity for Floor Slab
-
-This field is the thermal conductivity (W/m-K) of the floor slab. Typical value is 1.4.
-
-#### Field: Thermal Conductivity for Ceiling
-
-This field is the thermal conductivity (W/m-K) of the ceiling. Typical value is 0.09.
-
-#### Field: Thermal Conductivity for Soil
-
-This field is the thermal conductivity (W/m-K) of soil. Typical value is 1.1.
-
-#### Field: Thermal Conductivity for Gravel
-
-This field is the thermal conductivity (W/m-K) of gravel. Typical value is 1.9.
-
-#### Field: Thermal Conductivity for Wood
-
-This field is the thermal conductivity (W/m-K) of wood. Typical value is 0.12.
-
-### Insulation or GroundHeatTransfer:Basement:Insulation Object
-
-This object describes the insulation.
-
-#### Field: REXT: R Value of any exterior insulation
-
-This field is the R value (m2-K/W) of any exterior insulation.
-
-#### Field: INSFULL: Flag: Is the wall fully insulated?
-
-This field uses "true" for fully insulated walls and "false" for insulation half way down the side wall from the grade line.
-
-### SurfaceProps or GroundHeatTransfer:Basement:SurfaceProps Object
-
-The first six fields in this object specify the parameters used in the surface heat transfer boundary condition determination. They are specified for no snow and snow covered conditions.
-
-#### Field: ALBEDO: Surface albedo for No snow conditions
-
-This field specifies the surface solar albedo for no snow conditions. Solar albedo is more commonly available than the solar absorptivity. The total solar energy absorbed by a horizontal surface is (1-albedo)\*(Total solar). Typical value for this field is 0.16.
-
-#### Field: ALBEDO: Surface albedo for snow conditions
-
-This field specifies the surface solar albedo for snow covered conditions. Solar albedo is more commonly available than the solar absorptivity. The total solar energy absorbed by a horizontal surface is (1-albedo)\*(Total solar). Typical value for this field is 0.40.
-
-#### Field: EPSLN: Surface emissivity No Snow
-
-This field specifies the long wavelength or thermal radiation emissivity for the ground surface under no snow conditions. Typical value is 0.94.
-
-#### Field: EPSLN: Surface emissivity with Snow
-
-This field specifies the long wavelength or thermal radiation emissivity for the ground surface under snow covered conditions. Typical value is 0.86.
-
-#### Field: VEGHT: Surface roughness No snow conditions
-
-This field specifies the surface roughness or vegetation height (cm) that is used in determining the convective heat transfer coefficient on the surface under no snow conditions. Typical value is 6.0.
-
-#### Field: VEGHT: Surface roughness snow conditions
-
-This field specifies the surface roughness or vegetation height (cm) that is used in determining the convective heat transfer coefficient on the surface under snow covered conditions. Typical value is 0.25.
-
-#### Field: PET: Flag, Potential evapotranspiration on?
-
-This field is a flag that invokes the evapotranspiration calculation at the surface. This covers all forms of latent heat transfer from the surface. It normally should be included. The user enters "true" for "yes" and "false" for no.
-
-### BldgData or GroundHeatTransfer:Basement:BldgData Object
-
-This object specifies the major configuration parameters for the basement. The 3-D grid used in the simulation has the capability of including a gravel "fill" around the basement. Thus several dimensions must be specified. All units are in meters.
-
-#### Field: DWALL: Wall thickness
-
-This field specifies the basement wall thickness (m). Typical value is 0.2.
-
-#### Field: DSLAB: Floor Slab thickness
-
-This field specifies the thickness of the floor slab (m). Typical value is 0.25.
-
-#### Field: DGRAVXY: Width of gravel pit beside basement wall
-
-This field specifies the width of the gravel "fill" bed beside the basement wall (m).
-
-#### Field: DGRAVZN: Gravel depth extending above the floor slab
-
-This field specifies the depth of the gravel fill above the floor slab (m).
-
-#### Field: DGRAVZP: Gravel depth below the floor slab
-
-This field specifies the depth of the gravel fill below the floor slab (m).
-
-### Interior or GroundHeatTransfer:Basement:Interior Object
-
-This object provides the information needed to simulate the boundary conditions inside the basement.
-
-#### Field: COND: Flag: Is the basement conditioned?
-
-This flag indicates that the basement temperature is controlled. For EnergyPlus runs, this should be TRUE.
-
-#### Field: HIN: Downward convection only heat transfer coefficient
-
-This field specifies the convection only heat transfer coefficient for floors (downward heat flux - W/m2-K).
-
-#### Field: HIN: Upward convection only heat transfer coefficient
-
-This field specifies the convection only heat transfer coefficient for floors (upward heat flux - W/m2-K).
-
-#### Field: HIN: Horizontal convection only heat transfer coefficient
-
-This field specifies the convection only heat transfer coefficient for walls (horizontal heat flux - W/m2-K).
-
-#### Field: HIN: Downward combined (convection and radiation) heat transfer coefficient
-
-This field specifies the combined thermal radiation and convection heat transfer coefficient for floors (downward heat flux - W/m2-K).
-
-#### Field: HIN: Upward combined (convection and radiation) heat transfer coefficient
-
-This field specifies the combined thermal radiation and convection heat transfer coefficient for floors (upward heat flux - W/m2-K).
-
-#### Field: HIN: Horizontal combined (convection and radiation) heat transfer coefficient
-
-This field specifies the combined thermal radiation and convection heat transfer coefficient for walls (horizontal heat flux - W/m2-K).
-
-### ComBldg or GroundHeatTransfer:Basement:ComBldg Object
-
-This object specifies the 12 monthly average basement temperatures (air temperature). The last field allows a daily sine wave variation to be placed on the inside temperature. During testing, it was found that entering values for the daily sine wave amplitude had very little effect on the results.
-
-#### Field: January average temperature
-
-This field is the average air temperature (C) for the basement for January.
-
-#### Field: February average temperature
-
-This field is the average air temperature (C) for the basement for February.
-
-#### Field: March average temperature
-
-This field is the average air temperature (C) for the basement for March.
-
-#### Field: April average temperature
-
-This field is the average air temperature (C) for the basement for April.
-
-#### Field: May average temperature
-
-This field is the average air temperature (C) for the basement for May.
-
-#### Field: June average temperature
-
-This field is the average air temperature (C) for the basement for June.
-
-#### Field: July average temperature
-
-This field is the average air temperature (C) for the basement for July.
-
-#### Field: August average temperature
-
-This field is the average air temperature (C) for the basement for August.
-
-#### Field: September average temperature
-
-This field is the average air temperature (C) for the basement for September.
-
-#### Field: October average temperature
-
-This field is the average air temperature (C) for the basement for October.
-
-#### Field: November average temperature
-
-This field is the average air temperature (C) for the basement for November.
-
-#### Field: December average temperature
-
-This field is the average air temperature (C) for the basement for December.
-
-#### Field: Daily variation sine wave amplitude
-
-This field is the amplitude (variation) for a daily sine wave variation to be placed on the inside temperature. This has been shown to have little effect on results so zero can be used safely.
-
-### EquivSlab or GroundHeatTransfer:Basement:EquivSlab Object
-
-This object provides the information needed to do the simulation as an equivalent square geometry by utilizing the area to perimeter ratio. This procedure was shown to be accurate by Cogil (1998).
-
-#### Field: APRatio: The area to perimeter ratio for this slab
-
-This field specifies the Area to Perimeter (A/P) ratio for the slab.
-
-#### Field: EquivSizing: Flag
-
-This field should always be TRUE unless the user wants to specifically look at the differences between the long wall and the short wall on a rectangular configuration.
-
-### EquivAutoGrid or GroundHeatTransfer:Basement:EquivAutoGrid Object
-
-This is a necessary object when the EquivSizing Flag in the EquivSlab object is TRUE. This object provides the information needed to set up the three dimensional conduction grid surrounding the basement.
-
-#### Field: CLEARANCE: Distance from outside of wall to edge of 3-D ground domain
-
-This field specifies the distance to the outside of the field from the basement wall. It has been determined that 15 meters is quite satisfactory.
-
-#### Field: SlabDepth: Thickness of the floor slab
-
-This field specifies the thickness of the slab in meters. Note that the slab top surface is level with the ground surface, so this is the depth into the ground. The slab depth has a significant effect on the temperature calculation, and it is also important for the auto-grid process. The finite difference grids are set in such a way that they use the slab thickness to determine the vertical grid spacing. Because of this, autogridding will fail if the slab thickness is specified larger than 0.25 meters. The program also is set up so that the slab is a single finite difference cell in the vertical direction. Thus, if the slab thickness is set too large, the accuracy of the calculation may be suspect. Typical value is 0.1.
-
-#### Field: BaseDepth: Depth of the basement wall below grade
-
-This field specifies the depth of the basement wall below grade level (m). This is the height of the wall above the footing.
-
-Field N2 specifies the height of the basement wall above the grade level. This should be zero for EnergyPlus runs since if an above grade segment is to be simulated, it should be done with EnergyPlus not with the basement program.
-
-Field N3 specifies the floor slab thickness.
-
-Field N4 specifies the depth of the basement wall below grade level.  This is the height of the wall above the footing.
-
-### Sample idf File - Basement
-
-```idf
-! Minneapolis Test Cases
-SimParameters,
- 0.1,     ! [F: Multiplier for the ADI solution: 0&lt;F&lt;1.0,
- !         typically 0.1 (0.5 for high k
- 1;       ! [IYRS: Maximum number of iterations: typically 25-30
-
-MatlProps,
- 6, ! [NMAT: Number of materials in this domain, UP TO 6]
- 2242.6, 2242.6, 311.66, 1500.0, 2000.0, 448.5,! [RHO(1-6): Matl density
- !(Fndn wall, Floor Slab, Ceiling,Soil, Gravel, Wood), kg/m3, ]
- 880.0, 880.0, 1513.0, 840.0, 720.0, 1630.0,!       [CP(1-6): Specific Heat: J/kg-K,
- 1.402, 1.402, 0.093, 0.5, 1.9, 0.119;  !       [TCON(1-6): Conductivity: W/m-K
-
-Insulation,
- 5.0, ! [REXT: R Value of any exterior insulation, K/(W/m2)]
- TRUE; ! [INSFULL: Flag: Is the wall fully insulated? TRUE/FALSE]
-
-SurfaceProps,
- .16, .40, ! [ALBEDO: Surface albedo array, .16 .40]
- .94, .86, ! [EPSLN: Surface emissivity No Snow/ Snow .94 .86]
- 6.0, 0.25, ! [VEGHT: Surface roughness NS/S, cm, 6.0, 0.25]
- TRUE;! [PET: Flag, Potential evapotranspiration on? T/F]
- !                Typically, PET is True
-
-BldgData,
- .2, ! [DWALL: Wall thickness, m, .2]
- .1, ! [DSLAB: Floor slab thickness, m, 0.1]
- .3, ! [DGRAVXY: Width of gravel pit beside footing, m, 0.3]
- .2, ! [DGRAVZN: Gravel depth above the floor slab, m, 0.2]
- .1;! [DGRAVZP: Gravel depth below the floor slab, m, 0.1]
-
-Interior,
- TRUE, ! [COND: Flag: Is the basement conditioned? TRUE/FALSE]
- ! [HIN: Indoor convective heat transfer coefficients, W/m2-K
- !       Convection Only: 1)Q Downward 2)Q Upward 3)Q Horizontal
- !       Conv and Radiation: 4)Q Downward 5)Q Upward 6)Q Horizontal]
- 0.92, !Q Downward Convection Only
- 4.04,!Q Upward Convection Only
- 3.08,!Q HorizontalConvection Only
- 6.13, !Q Downward Conv and Radiation
- 9.26, !Q Upward Conv and Radiation
- 8.29;!Q Horizontal Conv and Radiation
-
-EquivSlab,
- 15.0, ! [APRatio: The area to perimeter ratio for this slab: m]
- TRUE;! [EquivSizing: Flag: Will the dimensions of an equivalent
- !             slab be calculated (TRUE) or will the dimensions be
- !              input directly? (FALSE)]
- !             Only advanced special simulations should use FALSE.
-
-EquivAutoGrid,   ! NOTE: EquivAutoGrid necessary when EquivSizing=TRUE
- !                This is the normal case.
- ! If the modelled building is not a rectangle or square, Equivalent
- ! sizing MUST be used to get accurate results
- 15, ! [CLEARANCE: Distance from outside of wall to edge, 15m]
- .1,  ! [SlabDepth: Thickness of the floor slab, m, 0.1]
- 2.4; ! [BaseDepth: Depth of the basement wall below grade, m]
-
-ComBldg, !  Commercial building
- 20.,  !  Jan Ave basement temp
- 20.,  !  Feb Ave basement temp
- 20.,  !  Mar Ave basement temp
- 20.,  !  Apr Ave basement temp
- 20.,  !  May Ave basement temp
- 20.,  !  Jun Ave basement temp
- 20.,  !  Jul Ave basement temp
- 20.,  !  Aug Ave basement temp
- 20.,  !  Sep Ave basement temp
- 20.,  !  Oct Ave basement temp
- 20.,  !  Nov Ave basement temp
- 20.,  !  Dec Ave basement temp
- 0.0;  !  Daily variation Sine Wave amplitude
-```
-
-### Additional Objects
-
-There are five additional objects in the IDD that can be used under very special situations by researchers who want to generate special calculation grids. They are normally not useful to EnergyPlus users. They will be shown as IDD sections only. They do not need to be in the IDF.
-
-```
-AutoGrid,
-\memo AutoGrid only necessary when EquivSizing is false
-\memo If the modelled building is not a rectangle or square, Equivalent
-\memo sizing MUST be used to get accurate results
-       N1, \field CLEARANCE: Distance from outside of wall to edge, 15m]
-       N2, \field SLABX: X dimension of the building slab, 0-60.0 m]
-       N3, \field SLABY: Y dimension of the building slab, 0-60.0 m]
-       N4, \field ConcAGHeight: Height of the fndn wall above grade, m]
-       N5, \field SlabDepth: Thickness of the floor slab, m, 0.1]
-       N6; \field BaseDepth: Depth of the basement wall below grade, m]
-
-ManualGrid,
-\memo Manual Grid only necessary using manual gridding (not recommended)
-       N1, \field NX: Number of cells in the X direction: 20]
-       N2, \field NY: Number of cells in the Y direction: 20]
-       N3, \field NZAG: Number of cells in the Z direction. above grade: 4 Always]
-       N4, \field NZBG: Number of cells in Z direction. below grade: 10-35]
-       N5, \field IBASE: X direction cell indicator of slab edge: 5-20]
-       N6, \field JBASE: Y direction cell indicator of slab edge: 5-20]
-       N7; \field KBASE: Z direction cell indicator of the top of the floor slab: 5-20]
-
-XFACE,
-\memo This is only needed when using manual gridding (not recommended)
-\memo XFACE: X Direction cell face coordinates: m
-       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
-       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
-       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
-       N39, N40, N41, N42, N43, N44;
-
-YFACE,
-\memo This is only needed when using manual gridding (not recommended)
-\memo YFACE: Y Direction cell face coordinates: m
-       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
-       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
-       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
-       N39, N40, N41, N42, N43, N44;
-
-ZFACE,
-\memo This is only needed when using manual gridding (not recommended)
-\memo ZFACE: Z Direction cell face coordinates: m
-       N1, N2, N3, N4, N5, N6, N7, N8, N9, N10, N11, N12, N13, N14,
-       N15, N16, N17, N18, N19, N20, N21, N22, N23, N24, N25, N26,
-       N27, N28, N29, N30, N31, N32, N33, N34, N35, N36, N37, N38,
-       N39, N40;
-```
-
-Using the Interface Surface Temperature Results in EnergyPlus
--------------------------------------------------------------
-
-If the objects are placed in the normal EnergyPlus input IDF file using the "GroundHeatTransfer:Basement:" prefix, then the values resulting from the Basement preprocessor will be automatically included in the simulation at run time. The surfaces can reference these values using Outside Boundary Conditions of:
-
-* GroundBasementPreprocessorAverageWall
-
-* GroundBasementPreprocessorAverageFloor
-
-* GroundBasementPreprocessorUpperWall
-
-* GroundBasementPreprocessorLowerWall
-
-The objects that support this include:
-
-* BuildingSurface:Detailed
-
-* Wall:Detailed
-
-* RoofCeiling:Detailed
-
-* Floor:Detailed
-
-The monthly results from the basement program are used with the SurfaceProperty:OtherSideCoefficients object in EnergyPlus. The idd corresponding to that object is shown below. The two applicable fields are N2 and A2. N2 should have the value 1.0. It will be modified by a schedule that is named in A2, and that temperature will be used on the outside of the surface specified as having the OtherSideCoeffcients named in A1.
-
-```idf
-SurfaceProperty:OtherSideCoefficients,
-  \memo This object sets the other side conditions for a surface in a variety of ways.
-  \min-fields 8
- A1, \field Name
-  \required-field
-  \reference OSCNames
-  \reference OutFaceEnvNames
- N1, \field Combined Convective/Radiative Film Coefficient
-  \required-field
-  \type real
-  \note if>0, this field becomes the exterior convective/radiative film coefficient
-  \note and the other fields are used to calculate the outdoor air temperature
-  \note then exterior surface temperature based on outdoor air and specified coefficient
-  \note if<=0, then remaining fields calculate the outside surface temperature
-  \note following fields are used in the equation:
-  \note SurfTemp=N7*TempZone + N4*OutdoorDry-bulb + N2*N3 + GroundTemp*N5 + WindSpeed*N6*OutdoorDry-bulb
- N2, \field Constant Temperature
-  \units C
-  \type real
-  \default 0
-  \note This parameter will be overwritten by the values from the Constant Temperature Schedule Name (below) if one is present
- N3, \field Constant Temperature Coefficient
-  \note This coefficient is used even with a Schedule.  It should normally be 1.0 in that case
-  \default 1
- N4, \field External Dry-Bulb Temperature Coefficient
-  \type real
-  \default 0
- N5, \field Ground Temperature Coefficient
-  \type real
-  \default 0
- N6, \field Wind Speed Coefficient
-  \type real
-  \default 0
- N7, \field Zone Air Temperature Coefficient
-  \type real
-  \default 0
- A2; \field Constant Temperature Schedule Name
-  \note Name of schedule for values of constant temperature.
-  \note Schedule values replace any value specified in the field Constant Temperature.
-  \type object-list
-  \object-list ScheduleNames
-```
-
-
-A sample idf for this object is shown below.
-
-```idf
-SurfaceProperty:OtherSideCoefficients, OSCCoef:Zn005:Wall003, !- OSC Name
- !  Example input for second ground temperature
- 0.0000000E+00,    !- OSC SurfFilmCoef
- 0.000000    ,    !- OSC Temp
- 1.000000    ,    !- OSC Temp Coef
- 0.000000    ,    !- OSC dry-bulb
- 0.000000    ,    !- OSC GrndTemp
- 0.000000    ,    !- OSC WindSpdCoeff
- 0.000000    ,    !- OSC ZoneAirTemp
- GroundTempSched;  !  Name of schedule defining additional ground temperature.
-```
-
-
-The OSC object can be repeated for as many outside temperatures as needed. A more detailed explanation of how to use this object is contained in the next section, and an example object is output by the program in the file EPObjects.txt.
-
-### Multiple Ground Temperatures
-
-These three objects show how the OtherSideCoefficients object can be used to provide extra ground temperatures for surfaces exposed to different ground temperatures.
-
-Here is the surface description. Note that the OutsideFaceEnvironment is specified as OtherSideCoeff.
-
-```idf
-BuildingSurface:Detailed,
-    OSCTest:South Wall,      !- User Supplied Surface Name
-    Wall,                    !- Surface Type
-    Exterior,                !- Construction Name of the Surface
-    OSCTest,                 !- Zone
-    OtherSideCoefficients,   !- Outside Boundary Condition
-    ExampleOSC,              !- Outside Boundary Condition Object
-    NoSun  ,                 !- Sun Exposure
-    NoWind  ,                !- Wind Exposure
-    0.5,                     !- View Factor to Ground
-    4,                       !- Number of Vertices
-    0,0,0,                   !- Vertex 1 X,Y,Z-coordinates {m}
-    6.096,0,0,               !- Vertex 2 X,Y,Z-coordinates {m}
-    6.096,0,4.572,           !- Vertex 3 X,Y,Z-coordinates {m}
-    0,0,4.572;               !- Vertex 4 X,Y,Z-coordinates {m}
-```
-
-The OtherSideCoefficients object has to supply the basic form of the environment. Note that the name corresponds to thee name in the Surface object. This object also supplies the name of a schedule that will provide the monthly ground temperature values.
-
-```idf
-SurfaceProperty:OtherSideCoefficients,
-  ExampleOSC,              !- OtherSideCoeff Name
-  0,                       !- Combined convective/radiative film coefficient
-  1,                       !- User selected Constant Temperature {C}
-  1,                       !- Coefficient modifying the user selected constant temperature
-  0,                       !- Coefficient modifying the external dry bulb temperature
-  0,                       !- Coefficient modifying the ground temperature
-  0,                       !- Coefficient modifying the wind speed term (s/m)
-  0,                       !- Coefficient modifying the zone air temperature part of the equation
-  GroundTempCompactSched;  !- Schedule Name for values of "const" temperature. Schedule values replace N2.
-```
-
-The schedule named in the last field of the OtherSideCoefficients object must be supplied. In compact schedule format it would appear as shown below. Again, objects for each of the surface temperatures are produced by the program and output in the file EPObjects.txt.
-
-```idf
-Schedule:Compact,
-    GroundTempCompactSched,  !- Name
-    Temperature ,            !- ScheduleType
-    Through: 1/31,           !- Complex Field \#1
-    For:AllDays,             !- Complex Field \#2
-    Until: 24:00,            !- Complex Field \#3
-    16,                      !- Complex Field \#4
-    Through: 2/28,           !- Complex Field \#5
-    For:AllDays,             !- Complex Field \#6
-    Until: 24:00,            !- Complex Field \#7
-    17,                      !- Complex Field \#8
-    Through: 3/31,           !- Complex Field \#9
-    For:AllDays,             !- Complex Field \#10
-    Until: 24:00,            !- Complex Field \#11
-    18,                      !- Complex Field \#12
-    Through: 4/30,           !- Complex Field \#13
-    For:AllDays,             !- Complex Field \#14
-    Until: 24:00,            !- Complex Field \#15
-    19,                      !- Complex Field \#16
-    Through: 5/31,           !- Complex Field \#17
-    For:AllDays,             !- Complex Field \#18
-    Until: 24:00,            !- Complex Field \#19
-    20,                      !- Complex Field \#20
-    Through: 6/30,           !- Complex Field \#21
-    For:AllDays,             !- Complex Field \#22
-    Until: 24:00,            !- Complex Field \#23
-    20,                      !- Complex Field \#24
-    Through: 7/31,           !- Complex Field \#25
-    For:AllDays,             !- Complex Field \#26
-    Until: 24:00,            !- Complex Field \#27
-    20,                      !- Complex Field \#28
-    Through: 8/31,           !- Complex Field \#29
-    For:AllDays,             !- Complex Field \#30
-    Until: 24:00,            !- Complex Field \#31
-    19,                      !- Complex Field \#32
-    Through: 9/30,           !- Complex Field \#33
-    For:AllDays,             !- Complex Field \#34
-    Until: 24:00,            !- Complex Field \#35
-    18,                      !- Complex Field \#36
-    Through: 10/31,          !- Complex Field \#37
-    For:AllDays,             !- Complex Field \#38
-    Until: 24:00,            !- Complex Field \#39
-    17,                      !- Complex Field \#40
-    Through: 11/30,          !- Complex Field \#41
-    For:AllDays,             !- Complex Field \#42
-    Until: 24:00,            !- Complex Field \#43
-    16,                      !- Complex Field \#44
-    Through: 12/31,          !- Complex Field \#45
-    For:AllDays,             !- Complex Field \#46
-    Until: 24:00,            !- Complex Field \#47
-    16;                      !- Complex Field \#48
-```
-
-References
-----------
-
-Bahnfleth, W.P. 1989. *Three Dimensional Modeling of Heat Transfer from Slab Floors*, Ph.D. dissertation, also published as USACERL TM E-89/11, University of Illinois.
-
-Bahnfleth, W.P. and C.O. Pedersen. 1990. A Three Dimensional Numerical Study of Slab-on-Grade Heat Transfer. *ASHRAE Transactions* Pt. 2, 96:61-72.
-
-Clements, Edward. 2004. *Three Dimensional Foundation Heat Transfer Modules for Whole-Building Energy Analysis*, MS Thesis, Pennsylvania State University.
-
-Cogil, Cynthia A. 1998. Modeling of Basement Heat Transfer and Parametric Study of Basement Insulation for Low Energy Housing. MS Thesis of Architectural Engineering, Pennsylvania State University.
-
-View Factor Calculation Program
-===============================
-
-EnergyPlus has the capability of accepting user defined view factors for special research situations. This option is not recommended for general use because the normal approximate view factor determination within EnergyPlus accounts for such practical things as thermal mass (furniture), and realistic exchange limits. However, when a user desires to supply view factors, this auxiliary program can be used to calculate them for a variety of configurations. The program is named View3D, and was developed at NIST (1). This document will describe how to use the program.
-
-Associated Files
-----------------
-
-Three files come with the auxiliary view factor package. They are:
-
-- View3D.exe
-
-- ViewFactorInterface.xls
-
-- View3D32.doc
-
-The first is the executable program that calculates the view factors. The second is an excel interface that will set up the input files and execute View3D.exe. The third file is the documentation file from NIST that contains some explanation of the program.
-
-Using the View Factor Interface program
----------------------------------------
-
-The interface program has two main sheets. One, named ZoneSheet, uses surface areas, tilts and facing directions to develop the input for View3D. The other one, named VerticesZoneSheet, uses the surface vertices to develop the input for View3D. The sheets are shown in Figure 24 and Figure 25.
-
-![ViewFactorInterfaceSheet](media/image022.png)
-
-Figure 24. View Factor Interface ZoneSheet
-
-
-
-
-
-![VerticesZoneSheetPic](media/image023.png)
-
-Figure 25. View Factor Interface VerticesZoneSheet
-
-Either sheet can be used to generate an input file for the View3D program. An example of that file is shown below.
-
-```
-T Test case from Excel interface
-C encl=  1  list=  2  eps=  0.0001  maxu=  8  maxo=  8  mino=  0  emit=  0
-F  3
-V  1  50  0  0
-V  2  0  0  0
-V  3  0  0  8
-V  4  50  0  8
-S  1  1  2  3  4   0  0   .999  SouthWall
-! =========================
-V  5  50  60  0
-V  6  50.00025  0  0
-V  7  50.00026  0  8
-V  8  50.00001  60  8
-S  2  5  6  7  8   0  0   .999  EastWall
-! =========================
-V  9  0  60  0
-V  10  50  60.00014  0
-V  11  50  60.00015  8
-V  12  0  60.00001  8
-S  3  9  10  11  12   0  0   .999  NorthWall
-! =========================
-V  13  0  0  0
-V  14  0  60  0
-V  15  0  60  8
-V  16  0  0  8
-S  4  13  14  15  16   0  0   .999  WestWall
-! =========================
-V  17  0  0  0
-V  18  50  1.377901E-04  0
-V  19  49.99984  60.00014  0
-V  20 -1.653482E-04  60  0
-S  5  17  18  19  20   0  0   .999  Floor
-! =========================
-V  21  0  60  8
-V  22  50  60.00014  8
-V  23  50.00016  1.373291E-04  8.000166
-V  24  1.653482E-04  0  8.000166
-S  6  21  22  23  24   0  0   .999  Roof
-! =========================
-End Of Data
-```
-
-Notice the title from row 6 on the interface appears at the top of the input file, and the control line information in rows 7 and 8 appear below the title line in a line with the character C at the left end. The explanation of the control parameters from the program document states:
-
-
-(C c)  The control line includes the following parameters (in order): name = value
-
-eps = 1.0e-4
-
-integration convergence criterion for both adaptive integration and view obstruction. This is not an exact measure of the accuracy of the computed view factors, but smaller values will usually lead to more precise values. The convergence criteria should not be less than about 1.0e-6 because many of the intermediate calculations are accurate only to single (32-bit) precision.
-
-maxU = 8
-
-maximum recursions used in computing the unobstructed view factors.
-
-maxO = 8
-
-maximum recursions used in computing the obstructed view factors. Limiting the maximum number of recursions limits the total execution time of the program but may prevent reaching the specified convergence.
-
-minO = 0
-
-minimum recursions: used in computing the obstructed view factors. This can help in cases where an obstruction occurs very near the view between the edges of two surfaces. The normal adaptive integration may miss the obstruction. Increasing this value from its normal value of 0 to 1 or 2 may catch the obstruction. This is probably not necessary except when very accurate view factors are desired. It can add considerably to execution time.
-
-row = 0
-
-selected row for computing view factors (0 = all rows)
-
-col = 0
-
-selected column for computing view factors (0 = all columns)
-
-encl = 0
-
-1 indicates that the surfaces form an enclosure; 0 indicates that they do not. This data is used to adjust the view factors of an enclosure to guarantee conservation of energy.
-
-emit = 0
-
-1 indicates that diffuse reflectance effects will be included in the computed view factors; 0 indicates they will not, i.e., surfaces will be considered 'black'.
-
-out = 0
-
-view factor output file format - 1 = …gence criterion for the numerical integration used to compute view factors between surfaces that have view obstructing surfaces between them.
-
-list = 0
-
-computational summary written to the VIEW3D.LOG file; 0 gives minimal information; 1 gives slightly more; 2 prints all the view factors; 3 causes dumping of some intermediate values.
-
-
-
-The values of the parameters shown on the interface sheets are reasonable defaults, and they should need to be adjusted only rarely.
-
-In the upper right corner of either sheet is a button that causes two files to be generated and View3D to be executed. The two files generated are the input file that uses the name from cell D13 with the extension vs3, and a file with the same name and an extension dxf. VoloView can be used with this file to generate a wire frame drawing of the zone being analyzed.
-
-Two paths are needed for executing the program. The directory path where the vs3 and dxf files will be placed is specified in cell D11. This directory can be selected using the Browse button in cell B11. The path to the View3D.exe program is specified by cell D15. This directory can be selected with the Browse button in cell B15.
-
-If you are using the ZoneSheet, the zone surfaces are described in the region from row 17 to row 27. Each column supplies the details for one surface. Additional surface columns can be added by copying and pasting a desired starting column to the right of column H. If either the surface height or base surface length is zero, the gross area cell will be zero and column is ignored. The facing direction of the surface is the direction an inward normal to the surface would point. So, the south wall of a zone faces north or 0 degrees. Note that this is different from EnergyPlus where the facing direction of a surface is based on the outward normal. The facing direction becomes just slightly more difficult with horizontal surfaces like floors and ceilings. The key to determining their facing direction is to visualize them being rotated slightly into the zone around their base surface axis. In the example, both ceiling and floor are chosen to face south. The tilt of a surface is relative to a horizontal upward facing (in the conventional sense) surface such as a floor. A ceiling or flat roof it tilted 180 degrees. Vertical surfaces have a tilt of 90 degrees.
-
-The remaining information needed to describe the surfaces is the coordinates of the lower left hand corner of the surface when viewed from inside the zone. This is where the visualization of a slight rotation of the floor and roof becomes helpful. Consider the roof surface on the sheet. Its base side lies along the east west axis since it faces south. With a slight inward rotation, it is clear that the lower left hand corner is the northwest corner of the roof. This corner has coordinates of 0, 60, and 8.
-
-If the VerticesZoneSheet is being used, the description of the surfaces consists only of the vertices. For this program, the vertices are specified in a counter clockwise rotation order if looking at the surface from the inside, and in a clockwise rotation order if looking from the outside.
-
-The vs3 file produced is shown previously and the dxf file generates the wire frame drawing shown in Figure 26.
-
-![ExampleDXFpicture](media/image024.png)
-
-Figure 26. DXF Format of Example Zone
-
-The input file and the output files produced by View3D are read into the interface spreadsheet, and appear on new worksheets.
-
-Figure 27 shows the lower corner of the interface sheet with the additional sheet tabs.
-
-![](media/image025.png)
-
-Figure 27. Files brought into the Interface Workbook
-
-The results file is named with the name in cell D13 with an extension of out. This file is shown below.
-
-```
-View3D 3.2 0 1 0 6
-400 480 400 480 3000 3000
-0.000000 0.078244 0.029324 0.078217 0.407109 0.407106
-0.065204 0.000000 0.065204 0.044282 0.412652 0.412659
-0.029324 0.078245 0.000000 0.078217 0.407110 0.407105
-0.065181 0.044282 0.065181 0.000000 0.412679 0.412677
-0.054281 0.066024 0.054281 0.066029 0.000000 0.759385
-0.054281 0.066025 0.054281 0.066028 0.759385 0.000000
-0.999 0.999 0.999 0.999 0.999 0.999
-```
-
-Excel macro capabilities are used by the interface to convert the text to columns and add the surface names and other headings. The modified results are placed on the Results worksheet as shown in Figure 28.
-
-![resultsWorksheet](media/image026.png)
-
-Figure 28. View Factors with Surface Names Inserted
-
-The results file information is used to generate a UserViewFactor object for EnergyPlus. This object is located in the first column of a new worksheet named UserVFObject. This column can simply be copied and inserted into the EnergyPlus idf file.
-
-If the results sheet does not appear, or the program terminates, the sheet named View3Dlog or the output file by the same name should be consulted. It contains a complete history of the execution. Any problem with the input file or the calculations should show up there.
-
-The extra sheets generated by the VBA macros will be deleted if the program is called with the run button while they are present. The user will be queried to make sure the sheets should be deleted.   During the succeeding run, new sheets will be created.
-
-Additional Information
-----------------------
-
-The interface and this document do not describe all of the features of the View3D program. Additional information can be found in the NIST document View3D32.pdf that accompanies the distribution. For example, if an obstruction wall is desired, it can be placed using the interface, but then the "C" at the left end of the row describing that surface in the input file should be changed to "O". The program can then be rerun with the new input file. If View3D.exe is double clicked, it will ask for the names of the input file and the output file.
-
-An additional point should be emphasized. The program will not calculate view factors for walls containing windows. That is all surfaces must be convex. Therefore,  a wall containing a subsurface must be described as four sections surrounding the subsurface. They can be combined using the "comb" column as described in the View3D document. However, this in not necessary if the user is willing to work with a few additional surfaces.
-
-
-
-Using Older Version Input Files - Transition
-============================================
-
-The transition program(s) are console programs that assist users in converting input files from prior release versions to the current (or interim). Sometimes many changes are made to the input file syntax; sometimes very few but the Transition program(s) can do the fastest job of making the conversions. An ObjectStatus spreadsheet is also included for those who want the details of each object's change.
-
-IDF Version Updater
--------------------
-
-The transition programs have been written as console applications similar to EnergyPlus. However, that may not be the easiest for users who want to transition several versions or several files at one time. Thus the IDF Version Updater GUI application was created.
-
-The IDF Version Updater lives in the folder with the multiple transition programs -- see Figure 29. Note that this application is also available from the EP-Launch Utilities tab (utility: IDFVersionUpdater). If you need to convert files from older than V6.0, the transition program set will need to be downloaded before use.  Once "IDF Version Updater" is selected from the Utilities pulldown list, click on the "Run IDF Version Updater" box and the single window shown below appears:
-
-
-
-![](media/image027.jpg)
-
-Figure 29.  Transition GUI screen
-
-Using the program is quite simple. As the window indicates, you press "Choose File to Update" to select a file or list of files (see IDF Version Converter / Transition File Lists) to convert. If doing multiple transitions using a transition file list you also press the "Choose File to Update, a browse window will appear at the bottom of which is a pulldown list for the "Files of Type".  Select the "Text File With List of EnergyPlus Files (\*.lst)" (see the section IDF Version Converter / Transition File Lists for format of this .lst file) option.  Once a file is found, its version is checked and appears as the "Current Version". By default, the latest "New Version" will be selected by the program - you can override this by choosing a different file version as the end version. The "Update File" button will then be able to be selected and the conversion will be done. The audit from the multiple transitions will be able to be viewed once the process is complete. If you are doing multiple transitions (e.g., from V2.2 to V6), you can select the check box "Create Intermediate Files" and after each transition, a file for the resultant version will be created and labeled &lt;filename&gt;)\_Vx.idf (where x is an abbreviated version number).
-
-The converted file becomes the new &lt;file&gt;.idf and the original file is saved in the original folder as &lt;file&gt;\_original.idf. To delete the original file instead of saving it, check the "Delete Original Files" checkbox.
-
-Table 27. IDF Version Updater Output Files and Descriptions.
-
-<table class="table table-striped">
-<tr>
-<th>Transition Output File Name</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>&lt;filename&gt;_Transition.audit</td>
-<td>This is the contents of what you would see on the screen if you sat and watched the transition process during a console run. If you convert multiple versions, all the messages are shown in this file.</td>
-</tr>
-<tr>
-<td>&lt;filename&gt;.idf</td>
-<td>Converted results to the latest version or version selected.</td>
-</tr>
-<tr>
-<td>&lt;filename&gt;_Vxxx.idf</td>
-<td>If you don't select "create intermediate versions", this will only be the original version. Otherwise will have each version.</td>
-</tr>
-</table>
-
-Transition Console Program Details
-----------------------------------
-
-For those who are interested, this is the detailed description of the Transition console applications including the current one. There are methods to use the program set from the command line; those details are not included in this document but available from EnergyPlus Support group.
-
-TransitionVA-B-C-to-VD-E-F.exe is the transition program that converts files from version "A-B-C" to "D-E-F", and is distributed in the "D-E-F" installer package. It uses several important files that are included in the "EnergyPlus" installation folder, in the PreProcess/IDFVersionUpdator subdirectory.
-
-Table 28. Transition files for current release
-
-<table class="table table-striped">
-<tr>
-<th>File Name</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>TransitionVA-B-C-to-VD-E-F.exe</td>
-<td>The executable program</td>
-</tr>
-<tr>
-<td>VA-B-C-Energy+.idd</td>
-<td>Base, starting, version Energy+.idd file</td>
-</tr>
-<tr>
-<td>VD-E-F-Energy+.idd</td>
-<td>Target, new idd file; Identical to Energy+.idd when distributed</td>
-</tr>
-<tr>
-<td>Report Variables A-B-C to D-E-F.csv</td>
-<td>Report variable name changes</td>
-</tr>
-</table>
-
- Another file "RulesA-B-C-to-D-E-F.xls" is not used directly by the program but contains the "rules" for translating objects from version A-B-C release to the D-E-F release. The ObjectStatus file can also be viewed - it will show if deleted objects are automatically transitioned to the new input file versions.
-
-There are several methods to executing the transition program - these methods give you the most flexibility in changing files from one version to the next. The easiest transition is through the EP-Launch program which can detect if the input file about to be run is of the same version as the IDD or not and suggest transitioning. You can also manually transition from the file menu in EP-Launch. (To have this feature, you must also have the files from the preceding table in the same folder as EP-Launch - which is usually the folder that also has the EnergyPlus.exe program).
-
-There are two command line methods to execute the transition version (from the Command Prompt). One is to simply use the file name you want transitioned (including .rvi or .mvi file names) or you can use a file name with a .lst extension and simply enter file names to be done in a text file. When you execute the transition program in this fashion, you will get the "typical" program defaults of a "full" transition, field names will be shown at each field with units, and any blank fields will be left blank rather than filled in with the current defaults.
-
-IDF Version Converter / Transition File Lists
----------------------------------------------
-
-Both the console program and the IDF-Version Updater (see) can use a text file of file names to perform the transitions. The file is a very simple list of file names:
-
-```
-FileName1
-FileName2
-```
-
-But you must include the path name in the file if it is not in the same folder as the transition set of programs:
-
-```
-C:\Myfiles\abc.idf
-C:\My Working Files\abcdef.idf
-D:\OtherFiles\xxxxxyyyyy.idf
-Etc
-```
-
-Note that the files need not be in the same folder. And, if you use the IDF Version Updater app, they need not all be the same version! If you use the straight batch files form the CMD line, all files in this list must be the same starting version and you will need to select that version when you run the batch file. List files have the implicit transition options seen in the following section.
-
-Converting imf files
---------------------
-
-The transition/conversion programs can "automatically" transition imf (ep-macro) files. One note of caution: if your macro file contains \#if statements in the form:
-
-```idf
-PEOPLE,
-    ZONE ONE,                !- Zone Name
-**\#\#if \#[DoSizing[] EQSU Y]**
-    \#[FAREA[] / OCCDENPEAK[]],        !- Number of People
-  **\#\#else**
-    \#[FAREA[] / OCCDENAVG[]],         !- Number of People
-**\#\#endif   **
-    OCCSCHED[],       !- Number of People SCHEDULE Name (real--fraction)
-    0.5000000,        !- Fraction Radiant
-    Activity Sch;     !- Activity level SCHEDULE Name (units W/person, real)
-```
-
-They should look like this:
-
-```idf
-**\#\#if \#[DoSizing[] EQSU Y]**
-PEOPLE,
-    ZONE ONE,                !- Zone Name
-    \#[FAREA[] / OCCDENPEAK[]],       !- Number of People
-    OCCSCHED[],       !-   Number of People SCHEDULE Name (real--fraction)
-    0.5000000,        !- Fraction Radiant
-    Activity Sch;     !- Activity level SCHEDULE Name (units W/person, real)
-  **\#\#else**
-PEOPLE,
-    ZONE ONE,                !- Zone Name
-    \#[FAREA[] / OCCDENAVG[]],        !- Number of People
-    OCCSCHED[],       !- Number of People SCHEDULE Name (real--fraction)
-    0.5000000,        !- Fraction Radiant
-    Activity Sch;     !- Activity level SCHEDULE Name (units W/person, real)
-**\#\#endif   **
-```
-
-EPDrawGUI
-=========
-
-The EPDrawGUI program is a simple utility that can be used to generate a dxf file from an input file without running EnergyPlus. It is a simple cross platform application is stored in the Preprocess subfolder of the EnergyPlus folder upon installation. A companion DLL (EPlusDrw.dll) is also needed in the same folder. And its library folders are required in a subfolder (EPDrawGUI Libs).
-
-![](media/image028.png)
-
-Figure 30. EPDrawGUI Main Screen
-
-Help is offered on the Main Tab and on the Options Tab when you place the mouse, without clicking, over the buttons, check boxes, and option boxes. In addition, the program copyright information is displayed when the mouse is over the Version number text in the lower left corner.
-
-Main Tab
---------
-
-The Main Tab, shown in Figure 30, contains the "Create DXF from IDF" button which is the button to use to create a DXF file from an IDF file, the main function of the EPDrawGUI program. This is the primary button that you will need to use. When pressed, you select an IDF file that you want to use as the basis for a drawing.  If the "Show DXF File After Created" check box is check, when the "Create DXF from IDF" button is pressed, the drawing will be viewed immediately after the DXF file is created. Normally, the viewer for DXF files is automatically found but if the program cannot find a drawing viewer program, you can select one manually on the Options Tab.
-
-
-
-![](media/image029.png)
-
-Figure 31. EPDrawGUI Options Tab
-
-Option Tab
-----------
-
-The Option Tab, shown in Figure 31, contains an additional option to control some complex drawings as well as ways to select the DXF file viewer and view DXF files.
-
-The "View DXF File" button is used to select a previously created DXF file and view it with the DXF file viewer. The DXF viewer is usually found automatically but if this function does not work, you may want to select the DXF file viewer manually using the Select DXF Viewer button.
-
-The "Select DXF Viewer" button allows you to manually select the program used to display DXF files. Normally, it is not necessary to use this function since the DXF file viewer program is automatically detected but if the wrong file viewer is automatically detected or no file viewer is detected, this button can be used to select the viewer program.
-
-For IDF files that contain surfaces with more than four sides, the options under "Polygons with 5+ Sides" can affect the way the drawing is shown. Polygons with &gt;4 sides do not display with the DXF 3DFACE command used for surfaces of 3 and 4 sides which subsequently will display very nicely as a "solid" in many DXF viewers.
-
-Thus there are four options which the user may choose to display &gt;4 sided polygons.
-
-- Attempt Triangulation
-
-This option attempts simple triangulation for the polygon (&gt;4 sides) surfaces.  This triangulation will show in the wireframe views but will appear as a solid face in 3D views. This triangulation is only for drawing purposes and does not affect the simulations in any way. The triangle algorithm is not perfect and warnings do result when the software cannot triangulate a surface. If unable to triangulate simply, a warning error is generated to the .EPDerr file.
-
-- Thick Polyline
-
-With this option, the &gt;4 sided polygon appears as a thicker line in all views of the building model. This option creates a 'thick' line at the border of the polygon (&gt;4 sides) surfaces. It will look like a hole in the drawing with a thicker edge. This thick border shows in wireframe as well as 3D views and can be confusing, due to overlap with other surfaces.
-
-- Regular Polyline
-
-With this option, the &gt;4 sided polygon appears as a wire frame line in all views of the building model. This option creates a 'regular' polyline for all polygon (&gt;4 sides) surfaces. It will look like a hole in the drawing.  Also, it will look the same in both wireframe and 3D views.
-
-- Wireframe
-
-This option creates a wireframe drawing (all lines) for all surfaces.  All surfaces will appear as lines in both wireframe and 3D views.
-
-Note that the EPDrawGUI program only processes building and shading surfaces. It does not process daylighting reference points though the similar option in the EnergyPlus program (Report, Surfaces, DXF;) does show the daylighting reference points (but not illuminance map points) in the DXF view.
-
-Input Macros
-============
-
-Introduction
-------------
-
-The Input Macros feature increases the flexibility of the EnergyPlus input files. This feature is intended for advanced users who are already familiar with EnergyPlus IDF files and need to prepare input manually. The basic capabilities are:
-
-- Incorporating external files containing pieces of IDF into the main EnergyPlus input stream.
-
-- Selectively accepting or skipping portions of the input.
-
-- Defining a block of input with parameters and later referencing this block.
-
-- Performing arithmetic and logical operations on the input.
-
-- Input macro debugging and listing control.
-
-These capabilities are invoked in the EP-MACRO program by using macro commands. Macro commands are preceded by \#\# to distinguish them from regular EnergyPlus input commands. After execution by the EP-MACRO processor, macro commands produce regular lines of EnergyPlus input that are shown in the resultant IDF file (**out.idf**) and, subsequently, in the EnergyPlus echo print (**audit.out**). Following are descriptions of the macro commands associated with the above capabilities. A detailed example of input macros is given at the end of this section; you should review it before reading the macro command descriptions.
-
-Running the EP-Macro program
-----------------------------
-
-The EP-Macro program is run automatically from the batch files (RunEPlus or EPL-Run from EP-Launch). Skip this small section if you are using either the RunEPlus batch file or EP-Launch. If you wish to run it by hand, it is found in the main folder of the EnergyPlus install (bin folder in the Linux install). Note that in EP-Launch and other script files for use with EP-Macro the convention is to name the file &lt;filename&gt;.imf (input macro file). If you name it &lt;filename&gt;.idf (input data file), the scripts will most likely think it is a "normal" EnergyPlus input file and ignore using EP-Macro on it - giving you a less than desireable result.
-
-Table 29. Files used in EP-Macro program
-
-<table class="table table-striped">
-<tr>
-<th>File Name</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>in.imf</td>
-<td>Input file containing the macro commands</td>
-</tr>
-<tr>
-<td>audit.out</td>
-<td>audit of the EPMacro run</td>
-</tr>
-<tr>
-<td>out.idf</td>
-<td>Output file that can be run with EnergyPlus</td>
-</tr>
-</table>
-
-The EP-Macro program is a Console Application, so to run by hand you would need to open a command prompt in the Main EnergyPlus install folder. Then, you would need to copy your input file containing the macro commands from its folder to this folder with the name "in.imf". The installed name of the EP-Macro program is "epmacro.exe". After execution, you can save the out.idf in an appropriate folder or rename it to in.idf in order to execute EnergyPlus. You can view the audit.out file for any errors that might have occurred during EP-Macro processing.
-
-
-
-Incorporating External Files
-----------------------------
-
-**\#\#include** {includefilename}
-
-This command puts all of the lines in an external file into the EnergyPlus input stream starting right after the command line. The name of the file that is included is the concatenation of {prefixpathname}, entered using  **\#\#fileprefix** , and {includefilename}. The lines in the external file will be listed in the resultant IDF file. When all the lines in the external file have been read in, input reverts back to the original input file at the line following the  **\#\#include**  command.
-
-**\#\#fileprefix**  {prefixpathname}
-
-specifies a pathname that will be prefixed to the filename given in an  **\#\#include** command. The **\#\#fileprefix**  command allows commonly-used include files to be kept in a directory other than the directory in which the current input file resides.
-
-Example: on a PC, the combination
-
-**\#\#fileprefix**  C:\\EnergyPlus\\Library
-
-**\#\#include**  SCHEDULES.IDF
-
-will include into the EnergyPlus input stream the file whose full name is
-
-C:\\EnergyPlus\\Library\\SCHEDULES.IDF
-
-**\#\#includesilent**  {includefilename}
-
-This command is identical to  **\#\#include**, except that the lines in the included file will not be listed in the EP-MACRO echo.
-
-**\#\#nosilent**
-
-Overrides the listing suppression of  **\#\#includesilent**. Used for debugging purposes only. After  **\#\#nosilent** , all following  **\#\#includesilent**  commands are treated as  **\#\#include** commands. 
-
-Example:   Assume the following files contain the indicated lines:
-
-<table class="table table-striped">
-<tr>
-<th>Main input file:</th>
-<th>External file:</th>
-</tr>
-<tr>
-<td>input1.inp</td>
-<td>file2.inp</td>
-</tr>
-<tr>
-<td>line 1a</td>
-<td>line 2a</td>
-</tr>
-<tr>
-<td>##include  file2.inp</td>
-<td>line 2b</td>
-</tr>
-<tr>
-<td>line 1b</td>
-<td>line 2c</td>
-</tr>
-<tr>
-<td>line 1c</td>
-<td> </td>
-</tr>
-</table>
-
-The end result of processing **\#\#include** input1.inp will be:
-
-    line 1a     (from input1.inp)
-
-    line 2a     (from file2.inp)
-
-    line 2b    (from file2.inp)
-
-    line 2c     (from file2.inp)
-
-    line 1b    (from input1.inp)
-
-    line 1c     (from input1.inp)
-
-External files can also contain  **\#\#include** commands, as shown in the following example:
-
-<table class="table table-striped">
-<tr>
-<th>Main input file:</th>
-<th>First external file:</th>
-<th>Seconh external file:</th>
-</tr>
-<tr>
-<td>input1.inp</td>
-<td>file2.inp</td>
-<td>file3.inp</td>
-</tr>
-<tr>
-<td>line 1a</td>
-<td>line 2a</td>
-<td>line 3a</td>
-</tr>
-<tr>
-<td>##include  file2.inp</td>
-<td>line 2b</td>
-<td>line 3b</td>
-</tr>
-<tr>
-<td>line 1b</td>
-<td>##include file3.inp</td>
-<td>line 3c</td>
-</tr>
-<tr>
-<td>line 1c</td>
-<td>line 2c</td>
-<td>line 3d</td>
-</tr>
-</table>
-
-The end result of processing **\#\#include** input1.tmp will be:
-
-    line 1a     (from input1.inp)
-
-    line 2a     (from file2.inp)
-
-    line 2b    (from file2.inp)
-
-    line 3a     (from file3.inp)
-
-    line 3b    (from file3.inp)
-
-    line 3c     (from file3.inp)
-
-    line 3d    (from file3.inp)
-
-    line 2c     (from file2.inp)
-
-    line 1b    (from input1.inp)
-
-    line 1c     (from input1.inp)
-
-Note:  Up to nine  **\#\#include** commands can be nested. However, there should be no recursion. This is an example of a recursion:
-
-file1.inp contains   **\#\#include**   file2.inp
-
-file2.inp contains   **\#\#include**   file1.inp
-
-Selectively Accepting or Skipping Lines of Input
-------------------------------------------------
-
-The  **\#\#if**  series of commands is used to selectively accept or skip lines of input according to the following sequence:
-
-
-```idf
-**##if ** {condition1}
-  line1a
-  line1b
-...
-
-**##elseif ** {condition2}
-  line2a
-  line2b
-...
-
-**##elseif ** {condition3**}**
-  line3a
-  line3b
-...
-
-**##else**
-  line N a
-  line N b
-...
-
-**##endif**
-
-Then the lines that will be included into the EnergyPlus input stream are:
-
-```idf
-If {condition 1} is TRUE,
-  line1a
-  line1b
-...
-
-otherwise
-
-If {condition 2} is TRUE,
-  line2a
-  line2b
-...
-
-otherwise
-
-If {condition 3} is TRUE,
-  line3a
-  line3b
-...
-
-otherwise
-
-If {condition 1}, {condition 2}, {condition 3} are all FALSE.
-  line N a
-  line N b
-...
-```
-
-There are six different  **\#\#if...** commands:
-
-Command
-
-
-
-Result
-
-**\#\#ifdef**
-
-{macro name}
-
-:  if macro name defined, include following lines
-
-**\#\#ifndef**
-
-{macro name}
-
-:  if macro name NOT defined, include following lines
-
-**\#\#if**
-
-{condition}
-
-:  if condition is TRUE, include following lines
-
-**\#\#elseif**
-
-{condition}
-
-:  if condition is TRUE, and previous conditions are FALSE, include
-
-   following lines
-
-**\#\#else**
-
-
-
-:  if all previous conditions are FALSE, include following lines
-
-**\#\#endif**
-
-
-
-:  indicates the end of the if block
-
-Notes:
-
-{macro name} is explained in section *Defining Blocks of Input*, below.
-
-{condition} is 0 or BLANK meaning FALSE, and any other character meaning TRUE.
-
-**\#\#ifdef**  and  **\#\#ifndef**  do not have corresponding  **\#\#elseif**  commands, but they do have
-
-       corresponding  **\#\#else**  and  **\#\#endif**  commands.
-
-
-
-Defining Blocks of Input
-------------------------
-
-The  **\#\#def** command allows a block of input text to be defined and given a name. The block of text can then be inserted anywhere in the EnergyPlus input stream by simply referencing the name of the block. (This process is called macro expansion.)  The block can have parameters (also called arguments) that can be given different values each time the block is referenced.
-
-The syntax of the  **\#\#def** command is as follows:
-
-```
-        unique name
-           |         zero or more arguments   macro text
-           |            |                     |
-           |            |                     |
-    ##def  macro-name [ arg1 arg2,arg3 ...]   text line 1
-  |_     |           | |    |_   |   _|     |
-    |    |           | |      |  |  |       |
-    |    |           | |      |  |  |       
-zero    one       zero_|     space(s)       one
-or      or        or         or comma       or
-more    more      more                      more
-spaces  spaces    spaces                    spaces
-```
-
-Example:    Define a schedule macro with name "All\_Const":
-
-```
-**##def** All_Const[x]
-**       ** Fraction, WeekON, 1,1, 12,31;
-    WEEKSCHEDULE, WeekON,
-        DayON,DayON,DayON,
-        DayON,DayON,DayON,
-        DayON,DayON,DayON,
-        DayON,DayON,DayON;
-    DAYSCHEDULE, DayON, Fraction,
-        x,x,x,x,x,x,x,x,x,x,x,x,
-        x,x,x,x,x,x,x,x,x,x,x,x ;
-**##enddef**
-```
-
-Then, in the EnergyPlus input stream (file in.imf), when we write :
-
-```idf
-SCHEDULE, Constant At 0.8, All_Const[0.8]
-```
-
-the result (file out.idf) is equivalent to:
-
-```
-SCHEDULE, Constant At 0.8,
-        Fraction, WeekON, 1,1, 12,31;
-    WEEKSCHEDULE, WeekON,
-        DayON,DayON,DayON,
-        DayON,DayON,DayON,
-        DayON,DayON,DayON,
-        DayON,DayON,DayON;
-    DAYSCHEDULE, DayON, Fraction,
-        0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,
-        0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8,0.8 ;
-```
-
-Macro definitions may have one or more arguments; the maximum number of arguments is 32. When a macro with arguments is referenced, its arguments must be given values. When a macro has no arguments, the brackets are still required both for macro definition and reference.
-
-Caution: Square brackets [  ] have been used in some versions of EnergyPlus inputs as comment/units fields. These will be expanded if left in the IDF and sent to EPMacro.
-
-Macro names must be unique (except see **\#\#set1** below); i.e., when a macro name is defined it cannot be defined again. Macro names are limited to 40 characters.
-
-To summarize, commands you use to define macros are the following:
-
-**\#\#def**   macro-name  [**arg1**,..,**arg*n*** ]  macro-text
-
-Defines a macro with the name macro-name  and arguments "arg1" through "arg*n*". "Macro-text" is one or more lines of text. If there are no arguments, the syntax is **\#\#def** macro-name macro-text.
-
-**\#\#enddef**
-
-Indicates the end of the macro definition initiated by **\#\#def.**
-
-**\#\#def1**    macro-name  [**arg1**,..,**arg*n*** ]  macro-text
-
-This is the same as  **\#\#def** but there is only one line of text so that the terminating command  **\#\#enddef** is not required.
-
-**\#\#set1**    macro-name   macro-text
-
-Like  **\#\#def1**  but has no arguments and macro-text is evaluated before storing. "Macro-text is evaluated" means that if macro-text contains other macros, these macros will be expanded, and the expanded text becomes the macro-text defined by  **\#\#set1**.
-
-Example:
-
-                    **\#\#def1**   xx  123
-                    **\#\#set1**   yy  xx[]
-
-is equivalent to:   **\#\#set1**   yy  123
-
-**\#\#set1**  can also be used to redefine macro-name.
-
-**\#\#set1**   x   0
-  .
-  .
-  .
-
-**\#\#set1**   x    **\#eval**[ x[]+1 ]
-
-
-
-(see Arithmetic Operations for description of the **\#eval** macro.)
-
-### Arithmetic Operations
-
-The built-in macro called  **\#eval[ ] ** can be used to perform arithmetic, literal, and logical operations. It can be abbreviated to **\# [ ].**
-
-\#eval[ X OP Y  ]  or  \#[ X OP Y ]
-
-gives the result  X OP Y. The allowed values for X, OP, and Y, and the corresponding result, are shown in the following table.
-
-<table class="table table-striped">
-  <tr>
-    <th>X*</th>
-    <th>OP **</th>
-    <th>Y</th>
-    <th>Result</th>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>+ (plus)</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>- (minus)</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>* (times)</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>/ (divided by)</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>min</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>max</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>mod</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>** (power)</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>SIN</td>
-    <td>OF</td>
-    <td>number (degrees)</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>COS</td>
-    <td>OF</td>
-    <td>number (degrees)</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>TAN</td>
-    <td>OF</td>
-    <td>number (degrees)</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>SQRT</td>
-    <td>OF</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>ABS</td>
-    <td>OF</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>ASIN</td>
-    <td>OF</td>
-    <td>number</td>
-    <td>number (degrees)</td>
-  </tr>
-  <tr>
-    <td>ACOS</td>
-    <td>OF</td>
-    <td>number</td>
-    <td>number (degrees)</td>
-  </tr>
-  <tr>
-    <td>ATAN</td>
-    <td>OF</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>INT</td>
-    <td>OF</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>LOG10</td>
-    <td>OF</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>LOG</td>
-    <td>OF</td>
-    <td>number</td>
-    <td>number</td>
-  </tr>
-  <tr>
-    <td>literal1</td>
-    <td>// (concatenate)</td>
-    <td>literal2</td>
-    <td>literal "literal1literal2"</td>
-  </tr>
-  <tr>
-    <td>literal1</td>
-    <td>/// (concatenate)</td>
-    <td>literal2</td>
-    <td>literal "literal1 literal2"</td>
-  </tr>
-  <tr>
-    <td>literal</td>
-    <td>EQS (=)</td>
-    <td>literal</td>
-    <td>logical (true or false) case sensitive</td>
-  </tr>
-  <tr>
-    <td>literal</td>
-    <td>NES (&ne;)</td>
-    <td>literal</td>
-    <td>logical (true or false) case sensitive</td>
-  </tr>
-  <tr>
-    <td>literal</td>
-    <td>EQSU (=)</td>
-    <td>literal</td>
-    <td>logical (true or false) not case sensitive</td>
-  </tr>
-  <tr>
-    <td>literal</td>
-    <td>NESU (&ne;)</td>
-    <td>literal</td>
-    <td>logical (true or false) not case sensitive</td>
-  </tr>
-  <tr>
-    <td>logical</td>
-    <td>AND</td>
-    <td>logical</td>
-    <td>logical (true or false)</td>
-  </tr>
-  <tr>
-    <td>logical</td>
-    <td>OR</td>
-    <td>logical</td>
-    <td>logical (true or false)</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>NOT</td>
-    <td>logical</td>
-    <td>logical (true or false)</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>EQ (=)</td>
-    <td>number</td>
-    <td>logical (true or false)</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>NE (&ne;)</td>
-    <td>number</td>
-    <td>logical (true or false)</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>GT (&gt;)</td>
-    <td>number</td>
-    <td>logical (true or false)</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>GE (&ge;)</td>
-    <td>number</td>
-    <td>logical (true or false)</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>LT (&lt;)</td>
-    <td>number</td>
-    <td>logical (true or false)</td>
-  </tr>
-  <tr>
-    <td>number</td>
-    <td>LE (&le;)</td>
-    <td>number</td>
-    <td>logical (true or false)</td>
-  </tr>
-  <tr>
-    <td colspan="4">* Upper or lower case is allowed for SIN, COS, etc.</td>
-  </tr>
-  <tr>
-    <td colspan="4">** Upper or lower case is allowed for OF, EQS, etc.</td>
-  </tr>
-</table>
-
-Example
-
-**\#eval[**  1 + 2  **]**     when expanded becomes 3.
-
-**\#eval[** 1 +  **\#eval**[2 \* 3] **]**  when expanded becomes 7.
-
-Example
-
-**\#\#set1** city[] Washington
-
-  DesignDay, \#[ city[ ] /// SUMMER ], ! Design Day Name
-
-gives
-
-     DesignDay, "Washington SUMMER", ! Design Day Name
-
-The following example illustrates the use of **\#eval**  inside  **\#if**  commands:
-
-**\#\#if**  **\#[** city[ ] EQS  Chicago **]**
-
-**\#\#if**  **\#[\#[** city[ ] EQS  Chicago ] and **\#[** occup[ ] NES low **]** **]**
-
-Notes:
-
-1.   For logical values:
-
-False = 0 or BLANK,
-
-True = any other character
-
-2.   A literal must be enclosed inside a pair of double quotes if it contains BLANKs or reserved characters like [ ]  ( )  ,
-
-E.g., "abc \*def"
-
-Otherwise, the quotes around the literals are optional.
-
-3.   Literal concatenation operators // and /// produce quoted literals.
-
-E.g.,  \#  [ large  ///  office ]   gives  "large office"
-
-4.   Literals are case sensitive. For example, "Chicago", "CHICAGO" and "chicago" are distinct.
-
-5.   EQS and NES are case sensitive string comparisons. EQSU and NESU are case insensitive string comparisons.
-
-6.   Literals are limited to 40 characters.
-
-Macro Debugging and Listing Control
------------------------------------
-
-**\#\#list**
-
-Turn on listing; echo of input lines on the OUTPUT file is enabled. This is the default condition.
-
-**\#\#nolist**
-
-Turn off listing; echo of input lines on the output file is disabled.
-
-**\#\#show**
-
-Start printing expanded line on output file. After this command, if a macro expansion was done, the expanded line is printed on the output file. In this way you can see the end result of macro expansions, which is the input as seen by the EnergyPlus Input processor.
-
-**\#\#noshow**
-
-Stop printing expanded line on output file. This is the default condition.
-
-**\#\#showdetail**
-
-Start printing each macro expansion. After this command, every time a macro expansion is done the result of the expansion is printed. This can produce lots of output.
-
-**\#\#noshowdetail**
-
-Stop printing each macro expansion. This is the default condition.
-
-\#\#expandcomment
-
-Comment fields may contain macro expansion directions. Following this command, the macros will be expanded in comments.
-
-For example, you might have:
-
-\#\#set1 Location = "Colorado Springs, CO"
-
-! Simulation run for Location[]
-
-If \#\#expandcomment preceded the set1 command, then the output would look like:
-
-! Simulation run for Colorado Springs, CO
-
-\#\#noexpandcomment
-
-This does not expand macros in comment fields. This is the default condition.
-
-**\#\#traceback**
-
-Give full traceback when printing an error message. After this command, if there is a EP-MACRO error, a full traceback of the macro expansions in progress is printed. This is the default condition.
-
-**\#\#notraceback**
-
-Don't give full traceback when printing an error message.
-
-**\#\#write**
-
-Start writing expanded text into file 22. This is similar to  **\#\#show** except that the expanded lines are written into file 22. Therefore, file 22 will contain only the text that will be seen by the EnergyPlus processor. This file is used only for debugging purposes. It allows you to see what the macro-processed input file looks like.
-
-**\#\#nowrite**
-
-Stop writing expanded text into file 22. This is the default condition.
-
-**\#\#symboltable**
-
-Prints table of current macro names. All of the macro names that are defined will be printed.
-
-**\#\#clear**
-
-Clear all macro definitions. All the macro names defined up to this point will be deleted.
-
-**\#\#reserve**   TEXT  *k*    NAMES  *l*    STACK  *m*
-
-Allocates memory.
-
-Reserves    *k*          words of space in AA array for macro definition storage.
-
-Reserves    *l*           positions in macro definition names table.
-
-Reserves    *m*         words of stack space.
-
-If used, the  **\#\#reserve**  command must precede  all other macro commands in the EP-MACRO input. This command should be used only if one or more of the following error messages is received:
-
-"Need more memory for storing macro definitions"
-
-Use  "**\#\#reserve** TEXT nnnnnn" command to get more memory. Current value of  *nnnnnn*  is: \_ \_ \_
-
-"Macro table capacity exceeded"
-
-Use "**\#\#reserve** NAMES nnnnnn" command to get more memory. Current value of  *nnnnnn*  is: \_ \_ \_
-
-"Macro stack overflow"
-
-Use "**\#\#reserve** STACK nnnnnn" command to get more memory. Current value of  *nnnnnn*  is: \_ \_ \_
-
-**\#\#! &lt;comment&gt;**
-
-Allows you to enter comment lines inside a macro. **&lt;comment&gt; ** is printed in the EP-MACRO echo but is not acted on by the macro processor.
-
-*Example:*
-
-This example shows the use of the  **\#\#set**, **\#\#include**, **\#\#eval** and **\#\#if** commands. Let an external file called cities.idf contain the following text:
-
-
-
-** \#\#if \#**[ city[ ] **EQS** CHICAGO ]
-
-  Location,Chicago IL,  !- Location Name
-
-   41.880,  !- Latitude
-
-   -87.63,  !- Longitude
-
-   -6.0,    !- Time Zone
-
-   2.;      !- Elevation {m}
-
-**\#\#elseif \#**[ city[ ] **EQS** WASHINGTON ]
-
-  Location,Washington DC,  !- Location Name
-
-   38.9,   !- Latitude
-
-   -77.0,  !- Longitude
-
-   -5.0,   !- Time Zone
-
-   15.;    !- Elevation {m}
-
-**\#\#else**
-
-** ** ERROR --- City Undefined
-
-**\#\#endif**
-
-
-
-Then the EnergyPlus input
-
-**\#\#set1** city[ ] CHICAGO
-
-**\#\#include** cities.idf
-
-will be converted, after macro processing, to:
-
-Location,Chicago IL,  !- Location Name
-
-   41.880,  !- Latitude
-
-   -87.63,  !- Longitude
-
-   -6.0,    !- Time Zone
-
-   2.;      !- Elevation {m}
-
-Listing Format
---------------
-
-The format of listing from EP-MACRO gives information about the status of the input macros, as shown in the following:
-
-```
- 1. 1.1  * 123 * ...... EnergyPlus input line
- -  - -  ------- ----------------------------------
- |  | |     |     echo of EnergyPlus input line
- |  | |     |
- |  | |    line number ( if the current line is being skipped
- |  | |                  by " ##if... " etc, this is indicated
- |  | |                  by printing "- 123 -" instead of
- |  | |                  "* 123 *" in the line number field;
- |  | |                  if the current line is part of a
- |  | |                  macro command, it is indicated by
- |  | |                  printing "# 123 #" )
- |  | |
- |  | macro expansion nesting level
- |  |
- |"##if" nesting level
- |
- "##include" nesting level
-```
-
-HVAC Diagram
-============
-
-Introduction
-------------
-
-The HVAC-Diagram program is a simple utility that can be used to generate a svg file based on the bnd file generated by EnergyPlus. It is a stored in the primary EnergyPlus\\PostProcessor folder upon installation.
-
-It creates a series of diagrams for the layout of the HVAC system components. The SVG file can be viewed with a number of internet browser plug-ins such as produced by Adobe that can be downloaded at [www.adobe.com/svg](http://www.adobe.com/svg). To get help within the Adobe viewer, right click anywhere on the drawing.
-
-Each diagram should be read from left to right, which is the direction of the flow of the fluid through the components.
-
-The HVAC-Diagram program is automatically called when using EP-Launch but can also be included in other batch files. To view the drawing in EP-Launch, click on the drawing button. You can zoom in on this drawing and with the "copy" command, paste a zoomed in portion as a bitmap in your document.
-
-![](media/image030.jpg)
-
-Figure 32. HVAC Diagram -- SVG Drawing
-
-
-
-Objects that are recognized by the HVAC diagram are shown in Table 30 (sorted by Object Name) and Table 31 (sorted by color).
-
-
-
-Table 30. HVAC Diagram Object Names (primary sort) Colors
-
-<table class="table table-striped">
-<tr>
-<th>Object Name</th>
-<th>Color</th>
-</tr>
-<tr>
-<td>AirLoopHVAC:ReturnPlenum</td>
-<td>lightgreen</td>
-</tr>
-<tr>
-<td>AirLoopHVAC:SupplyPlenum</td>
-<td>lightgreen</td>
-</tr>
-<tr>
-<td>AirLoopHVAC:ZoneMixer</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>AirLoopHVAC:ZoneSplitter</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>AirTerminal:DualDuct:ConstantVolume</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>AirTerminal:DualDuct:VAV</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>AirTerminal:SingleDuct:Uncontrolled</td>
-<td>none</td>
-</tr>
-<tr>
-<td>AirTerminal:SingleDuct:VAV:NoReheat</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>AirTerminal:SingleDuct:VAV:Reheat</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>Boiler:HotWater</td>
-<td>indianred</td>
-</tr>
-<tr>
-<td>Chiller:Absorption</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>Chiller:CombustionTurbine</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>Chiller:ConstantCOP</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>Chiller:Electric</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>Chiller:EngineDriven</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>ChillerHeater:Absorption:DirectFired</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:DX:MultiSpeed</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:DX:SingleSpeed</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:Water</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:Water:DetailedGeometry</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:WaterToAirHeatPump:EquationFit</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:WaterToAirHeatPump:ParameterEstimation</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Heating:DX:SingleSpeed</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Heating:Electric</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>Coil:Heating:Gas</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>Coil:Heating:Water</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>Coil:Heating:WaterToAirHeatPump:EquationFit</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>Coil:Heating:WaterToAirHeatPump:ParameterEstimation</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>Connector:Mixer</td>
-<td>lightgreen</td>
-</tr>
-<tr>
-<td>Connector:Splitter</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>Controller:OutdoorAir</td>
-<td>none</td>
-</tr>
-<tr>
-<td>Controller:WaterCoil</td>
-<td>none</td>
-</tr>
-<tr>
-<td>CoolingTower:SingleSpeed</td>
-<td>pink</td>
-</tr>
-<tr>
-<td>Dehumidifier:Desiccant:NoFans</td>
-<td>tan</td>
-</tr>
-<tr>
-<td>DistrictCooling</td>
-<td>none</td>
-</tr>
-<tr>
-<td>DistrictHeating</td>
-<td>none</td>
-</tr>
-<tr>
-<td>EvaporativeCooler:Direct:CelDekPad</td>
-<td>aliceblue</td>
-</tr>
-<tr>
-<td>EvaporativeCooler:Indirect:CelDekPad</td>
-<td>aliceblue</td>
-</tr>
-<tr>
-<td>EvaporativeCooler:Indirect:ResearchSpecial</td>
-<td>aliceblue</td>
-</tr>
-<tr>
-<td>Fan:ConstantVolume</td>
-<td>silver</td>
-</tr>
-<tr>
-<td>Fan:OnOff</td>
-<td>silver</td>
-</tr>
-<tr>
-<td>Fan:VariableVolume</td>
-<td>silver</td>
-</tr>
-<tr>
-<td>Fan:ZoneExhaust</td>
-<td>silver</td>
-</tr>
-<tr>
-<td>Generator:CombustionTurbine</td>
-<td>orange</td>
-</tr>
-<tr>
-<td>Generator:InternalCombustionEngine</td>
-<td>orange</td>
-</tr>
-<tr>
-<td>GroundHeatExchanger:Pond</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>GroundHeatExchanger:Surface</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>GroundHeatExchanger:Vertical</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>HeatExchanger:AirToAir:FlatPlate</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>HeatExchanger:AirToAir:SensibleAndLatent</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>HeatExchanger:Hydronic</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>HeatPump:WaterToWater:EquationFit:Cooling</td>
-<td>lightslategray</td>
-</tr>
-<tr>
-<td>HeatPump:WaterToWater:EquationFit:Heating</td>
-<td>lightslategray</td>
-</tr>
-<tr>
-<td>HeatPump:WaterToWater:ParameterEstimation:Cooling</td>
-<td>lightslategray</td>
-</tr>
-<tr>
-<td>HeatPump:WaterToWater:ParameterEstimation:Heating</td>
-<td>lightslategray</td>
-</tr>
-<tr>
-<td>Humidifier:Steam:Electric</td>
-<td>lavender</td>
-</tr>
-<tr>
-<td>LoadProfile:Plant</td>
-<td>none</td>
-</tr>
-<tr>
-<td>OutdoorAir:Mixer</td>
-<td>lawngreen</td>
-</tr>
-<tr>
-<td>OutdoorAir:NodeList</td>
-<td>none</td>
-</tr>
-<tr>
-<td>Pipe:Adiabatic</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>PlantLoopConnection</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>Pump:ConstantSpeed</td>
-<td>springgreen</td>
-</tr>
-<tr>
-<td>Pump:VariableSpeed</td>
-<td>springgreen</td>
-</tr>
-<tr>
-<td>SolarCollector:FlatPlate:Water</td>
-<td>yellow</td>
-</tr>
-<tr>
-<td>WaterHeater:Mixed</td>
-<td>orange</td>
-</tr>
-<tr>
-<td>WaterHeater:Stratified</td>
-<td>orange</td>
-</tr>
-<tr>
-<td>ZoneHVAC:Baseboard:Convective:Water</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>ZoneHVAC:EnergyRecoveryVentilator:Controller</td>
-<td>none</td>
-</tr>
-<tr>
-<td>ZoneHVAC:EquipmentConnections</td>
-<td>chartreuse</td>
-</tr>
-<tr>
-<td>ZoneHVAC:IdealLoadsAirSystem</td>
-<td>none</td>
-</tr>
-<tr>
-<td>ZoneHVAC:LowTemperatureRadiant:ConstantFlow</td>
-<td>orangered</td>
-</tr>
-<tr>
-<td>ZoneHVAC:LowTemperatureRadiant:VariableFlow</td>
-<td>orangered</td>
-</tr>
-<tr>
-<td>ZoneHVAC:UnitVentilator</td>
-<td>sandybrown</td>
-</tr>
-</table>
-
-
-
-Table 31. HVAC Diagram Object Names and Color (primary sort)
-
-<table class="table table-striped">
-<tr>
-<th>Object Name</th>
-<th>Color</th>
-</tr>
-<tr>
-<td>EvaporativeCooler:Direct:CelDekPad</td>
-<td>aliceblue</td>
-</tr>
-<tr>
-<td>EvaporativeCooler:Indirect:CelDekPad</td>
-<td>aliceblue</td>
-</tr>
-<tr>
-<td>EvaporativeCooler:Indirect:ResearchSpecial</td>
-<td>aliceblue</td>
-</tr>
-<tr>
-<td>ZoneHVAC:EquipmentConnections</td>
-<td>chartreuse</td>
-</tr>
-<tr>
-<td>Boiler:HotWater</td>
-<td>indianred</td>
-</tr>
-<tr>
-<td>Humidifier:Steam:Electric</td>
-<td>lavender</td>
-</tr>
-<tr>
-<td>OutdoorAir:Mixer</td>
-<td>lawngreen</td>
-</tr>
-<tr>
-<td>AirLoopHVAC:ReturnPlenum</td>
-<td>lightgreen</td>
-</tr>
-<tr>
-<td>AirLoopHVAC:SupplyPlenum</td>
-<td>lightgreen</td>
-</tr>
-<tr>
-<td>Connector:Mixer</td>
-<td>lightgreen</td>
-</tr>
-<tr>
-<td>HeatPump:WaterToWater:EquationFit:Cooling</td>
-<td>lightslategray</td>
-</tr>
-<tr>
-<td>HeatPump:WaterToWater:EquationFit:Heating</td>
-<td>lightslategray</td>
-</tr>
-<tr>
-<td>HeatPump:WaterToWater:ParameterEstimation:Cooling</td>
-<td>lightslategray</td>
-</tr>
-<tr>
-<td>HeatPump:WaterToWater:ParameterEstimation:Heating</td>
-<td>lightslategray</td>
-</tr>
-<tr>
-<td>AirTerminal:SingleDuct:Uncontrolled</td>
-<td>none</td>
-</tr>
-<tr>
-<td>Controller:OutdoorAir</td>
-<td>none</td>
-</tr>
-<tr>
-<td>Controller:WaterCoil</td>
-<td>none</td>
-</tr>
-<tr>
-<td>DistrictCooling</td>
-<td>none</td>
-</tr>
-<tr>
-<td>DistrictHeating</td>
-<td>none</td>
-</tr>
-<tr>
-<td>LoadProfile:Plant</td>
-<td>none</td>
-</tr>
-<tr>
-<td>OutdoorAir:NodeList</td>
-<td>none</td>
-</tr>
-<tr>
-<td>ZoneHVAC:EnergyRecoveryVentilator:Controller</td>
-<td>none</td>
-</tr>
-<tr>
-<td>ZoneHVAC:IdealLoadsAirSystem</td>
-<td>none</td>
-</tr>
-<tr>
-<td>Generator:CombustionTurbine</td>
-<td>orange</td>
-</tr>
-<tr>
-<td>Generator:InternalCombustionEngine</td>
-<td>orange</td>
-</tr>
-<tr>
-<td>WaterHeater:Mixed</td>
-<td>orange</td>
-</tr>
-<tr>
-<td>WaterHeater:Stratified</td>
-<td>orange</td>
-</tr>
-<tr>
-<td>ZoneHVAC:LowTemperatureRadiant:ConstantFlow</td>
-<td>orangered</td>
-</tr>
-<tr>
-<td>ZoneHVAC:LowTemperatureRadiant:VariableFlow</td>
-<td>orangered</td>
-</tr>
-<tr>
-<td>GroundHeatExchanger:Pond</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>GroundHeatExchanger:Surface</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>GroundHeatExchanger:Vertical</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>HeatExchanger:AirToAir:FlatPlate</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>HeatExchanger:AirToAir:SensibleAndLatent</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>HeatExchanger:Hydronic</td>
-<td>paleturquoise</td>
-</tr>
-<tr>
-<td>CoolingTower:SingleSpeed</td>
-<td>pink</td>
-</tr>
-<tr>
-<td>Chiller:Absorption</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>Chiller:CombustionTurbine</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>Chiller:ConstantCOP</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>Chiller:Electric</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>Chiller:EngineDriven</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>ChillerHeater:Absorption:DirectFired</td>
-<td>powderblue</td>
-</tr>
-<tr>
-<td>Coil:Heating:Electric</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>Coil:Heating:Gas</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>Coil:Heating:Water</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>Coil:Heating:WaterToAirHeatPump:EquationFit</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>Coil:Heating:WaterToAirHeatPump:ParameterEstimation</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>ZoneHVAC:Baseboard:Convective:Water</td>
-<td>salmon</td>
-</tr>
-<tr>
-<td>ZoneHVAC:UnitVentilator</td>
-<td>sandybrown</td>
-</tr>
-<tr>
-<td>Fan:ConstantVolume</td>
-<td>silver</td>
-</tr>
-<tr>
-<td>Fan:OnOff</td>
-<td>silver</td>
-</tr>
-<tr>
-<td>Fan:VariableVolume</td>
-<td>silver</td>
-</tr>
-<tr>
-<td>Fan:ZoneExhaust</td>
-<td>silver</td>
-</tr>
-<tr>
-<td>Coil:Cooling:DX:MultiSpeed</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:DX:SingleSpeed</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:Water</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:Water:DetailedGeometry</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:WaterToAirHeatPump:EquationFit</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Cooling:WaterToAirHeatPump:ParameterEstimation</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Coil:Heating:DX:SingleSpeed</td>
-<td>skyblue</td>
-</tr>
-<tr>
-<td>Pump:ConstantSpeed</td>
-<td>springgreen</td>
-</tr>
-<tr>
-<td>Pump:VariableSpeed</td>
-<td>springgreen</td>
-</tr>
-<tr>
-<td>Dehumidifier:Desiccant:NoFans</td>
-<td>tan</td>
-</tr>
-<tr>
-<td>AirLoopHVAC:ZoneMixer</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>AirLoopHVAC:ZoneSplitter</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>AirTerminal:DualDuct:ConstantVolume</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>AirTerminal:DualDuct:VAV</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>AirTerminal:SingleDuct:VAV:NoReheat</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>AirTerminal:SingleDuct:VAV:Reheat</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>Connector:Splitter</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>Pipe:Adiabatic</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>PlantLoopConnection</td>
-<td>wheat</td>
-</tr>
-<tr>
-<td>SolarCollector:FlatPlate:Water</td>
-<td>yellow</td>
-</tr>
-</table>
-
-CoeffConv/CoeffCheck
-====================
-
-These two programs are stored in the PreProcess folder of your EnergyPlus installation under a folder CoeffConv.
-
-CoeffConv
----------
-
-CoeffConv is a program to convert DOE-2 temperature dependent curves in Fahrenheit to EnergyPlus curves in Centigrade. The program converts the DOE-2 coefficients of a biquadratic curve to the equivalent EnergyPlus biquadratic curve coefficients.
-
-EP-Launch can be used to run the CoeffConv program. CoeffConv is one of the options on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the CoeffConv program. When using EP-Launch to run CoeffConv the input file must have the file extension .coi and will create an output file with the file extension .coo.
-
-You can also run the CoeffConv program as a console application. The input file then must be from file CoeffConvInput.txt (status=OLD). There are 6 lines of ascii input.
-
-For example:
-
-```
-VarSpeedCoolCapFt
--0.29382,0.0222213,0.00006988,0.0040928,-0.00000226,-0.00013774
-55.,75.
-75.,115.
-67.0,95.0
-5.0
-```
-
-* The 1st line is the user selected name of the curve.
-* The 2nd line contains the 6 biquadratic curve coefficients, comma separated. These are the Doe-2 coefficients.
-* The 3rd line contains the min and max values of the 1st independent variable, comma separated, deg F.
-* The 4th line contains the min and max values of the 2nd independent variable, comma separated, deg F.
-* The 5th line contains the rated values of the 1st & 2nd independent variables, comma separated, deg F.
-* The 6th line contains the delta T for the output performance maps.
-
-All the input lines should start in column 1.
-
-The above sequence can be repeated up to 100 times.
-
-The output file is CoeffConvOutput.txt (status=NEW) (that means you need to delete any existing CoeffConvOutput.txt).
-
-The output file will contain the EnergyPlus idf input for the curve, as well as any error messages;
-
-Also, the DOE-2 and EnergyPlus curve values at the rating point (where the value should be 1.0) and performance maps for the curves - both DOE-2 and EnergyPlus.
-
-There is an example input file and an example output file installed with the program.
-
-CoeffCheck
-----------
-
-CoeffCheck is a program to print out a performance map given a bi-quadratic performance curve.
-
-EP-Launch can be used to run the CoeffCheck program. CoeffCheck is one of the options on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the CoeffCheck program. When using EP-Launch to run CoeffCheck the input file must have the file extension .cci and will create an output file with the file extension .cco.
-
-You can also run the CoeffCheck program as a console application. The input file then must be from file CoeffCheckInput.txt (status=OLD). There are 6 lines of ascii input.
-
-For example:
-
-```
-VarSpeedCoolCapFt
-0.476428E+00,0.401147E-01,0.226411E-03,-0.827136E-03,-0.732240E-05,-0.446278E-03
-12.777778,23.888889
-23.888889,46.111111
-19.444444,35.0
-2.777778
-```
-
-* The 1st line is the user selected name of the curve.
-* The 2nd line contains the 6 biquadratic curve coefficients, comma separated.
-* The 3rd line contains the min and max values of the 1st independent variable, comma separated
-* The 4th line contains the min and max values of the 2nd independent variable, comma separated
-* The 5th line contains the rated values of the 1st & 2nd independent variables, comma separated
-* The 6th line contains the delta T for the output performance map
-
-The output file is CoeffCheckOutput.txt (status=NEW).
-
-There is an example input file and an example output file installed with the program.
-
-Running the CoeffConv or CoeffCheck programs
---------------------------------------------
-
-EP-Launch can be used to run both the CoeffConv and CoeffCheck programs.  CoeffConv and CoeffCheck are two of the options on the Utilities tab in EP-Launch.  See the EP-Launch section in this document for more information on how to use EP-Launch with the CoeffConv and CoeffCheck programs.
-
-You can also run both programs as console applications and, because they are small, they are automatically installed with EnergyPlus. You will need to open a command window using the following steps:
-
-1)   Open a DOS command prompt window (Start -&gt; Programs -&gt; Accessories -&gt; Command Prompt)
-
-2)   Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
-
-C:
-
-CD \\&lt;rootfolder&gt;\&lt;/span>
-
-3)   Change to the specific folder for the coefficient conversion applications:
-
-CD PreProcess\\CoeffConv
-
-4)   Run the program:
-
-After creating your files as shown above, enter either CoeffConv or CoeffCheck as desired. The folder also contains a "readme.txt" file which you can peruse.
-
-ExpandObjects
-=============
-
-Introduction
-------------
-
-The ExpandObjects program uses HVACTemplate objects in the IDF file to "expand" them into full fledged objects for EnergyPlus.  Read more details of the systems and the individual fields in the HVACTemplate objects in the Input Output Reference document.
-
-ExpandObjects also processes GroundHeatTransfer objects, sends an input file to the Slab and Basement preprocessors, and replaces ground heat transfer boundary condition fields in building surface objects. Read more details of the ground heat transfer processing in the Input Output Reference.
-
-Technically speaking, the ExpandObjects program is a preprocessor that is currently used with the HVACTemplate objects. The preprocessor reads an **idf** file and generates an expanded.idf file (usually with the extension .**expidf**). The original idf file contains objects that will be read by the preprocessor and those that are ignored by the preprocessor. The objects read can be either commented out or left as is. The objects created by the preprocessor in the expanded.idf file should require no further preprocessing. The preprocessor does not read the EnergyPlus Data Dictionary file (Energy+.IDD) and does limited validation. Most of the object values that are created are "passed" through from input objects. This allows EnergyPlus to provide most of the validation. If errors are found, error messages are passed to the EnergyPlus program using the Output:Preprocessor object. These errors will be shown in the usual EnergyPlus error file. When used with EP-Launch, the expanded.idf file is renamed to the original file name with the extension **expidf**.
-
-HVAC Template Objects Processed
--------------------------------
-
-The HVACTemplate objects that are currently read by the ExpandObjects preprocessor are:
-
-- HVACTemplate:Thermostat
-
-- HVACTemplate:Zone:IdealLoadsAirSystem
-
-- HVACTemplate:Zone:FanCoil
-
-- HVACTemplate:Zone:PTAC
-
-- HVACTemplate:Zone:PTHP
-
-- HVACTemplate:Zone:Unitary
-
-- HVACTemplate:Zone:VAV
-
-- HVACTemplate:Zone:VAV:FanPowered
-
-- HVACTemplate:Zone:WatertoAirHeatPump
-
-- HVACTemplate:System:Unitary
-
-- HVACTemplate:System:UnitaryHeatPump:AirToAir
-
-- HVACTemplate:System:VAV
-
-- HVACTemplate:System:PackagedVAV
-
-- HVACTemplate:System:DedicatedOutdoorAir
-
-- HVACTemplate:Plant:ChilledWaterLoop
-
-- HVACTemplate:Plant:Chiller
-
-- HVACTemplate:Plant:Chiller:ObjectReference
-
-- HVACTemplate:Plant:Tower
-
-- HVACTemplate:Plant:Tower:ObjectReference
-
-- HVACTemplate:Plant:HotWaterLoop
-
-- HVACTemplate:Plant:Boiler
-
-- HVACTemplate:Plant:Boiler:ObjectReference
-
-Ground Heat Transfer Objects Processed
---------------------------------------
-
-The GroundHeatTransfer objects that are currently read by the ExpandObjects preprocessor are:
-
-- GroundHeatTransfer:Control
-
-- GroundHeatTransfer:Slab:Materials
-
-- GroundHeatTransfer:Slab:MatlProps
-
-- GroundHeatTransfer:Slab:BoundConds
-
-- GroundHeatTransfer:Slab:BldgProps
-
-- GroundHeatTransfer:Slab:Insulation
-
-- GroundHeatTransfer:Slab:EquivalentSlab
-
-- GroundHeatTransfer:Slab:AutoGrid
-
-- GroundHeatTransfer:Slab:ManualGrid
-
-- GroundHeatTransfer:Slab:XFACE
-
-- GroundHeatTransfer:Slab:YFACE
-
-- GroundHeatTransfer:Slab:ZFACE
-
-- GroundHeatTransfer:Basement:SimParameters
-
-- GroundHeatTransfer:Basement:MatlProps
-
-- GroundHeatTransfer:Basement:Insulation
-
-- GroundHeatTransfer:Basement:SurfaceProps
-
-- GroundHeatTransfer:Basement:BldgData
-
-- GroundHeatTransfer:Basement:Interior
-
-- GroundHeatTransfer:Basement:ComBldg
-
-- GroundHeatTransfer:Basement:EquivSlab
-
-- GroundHeatTransfer:Basement:EquivAutoGrid
-
-- GroundHeatTransfer:Basement:AutoGrid
-
-- GroundHeatTransfer:Basement:ManualGrid
-
-- GroundHeatTransfer:Basement:XFACE
-
-- GroundHeatTransfer:Basement:YFACE
-
-- GroundHeatTransfer:Basement:ZFACEHVACTemplate:Thermostat
-
-Building Surface Objects Processed
-----------------------------------
-
-The building surface objects that are currently modified by the ExpandObjects preprocessor are:
-
-- BuildingSurface:Detailed
-
-- Wall:Detailed
-
-- RoofCeiling:Detailed
-
-- Floor:Detailed
-
-- Site:GroundTemperature:BuildingSurface
-
-CSVproc
-=======
-
-This simple post processing utility may be useful when doing parametric analyses. It takes a CSV (comma separated values file) and performs some simple statistics. It is a very small application with no interface. It is typically executed from the command line.
-
-1)   Open a DOS command prompt window (Start à Programs à Accessories à Command Prompt)
-
-2)   Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
-
-C:
-
-CD \\&lt;root folder&gt;\&lt;/span>
-
-3)   Change to the specific folder for the coefficient conversion applications:
-
-CD PostProcess
-
-4)   Run the program:
-
-CSVproc &lt;filename&gt;
-
-Where &lt;filename&gt; is the name of a CSV file, including extension. There is a simple readme.txt file in the folder. The program performs some simple statistics on each column and creates a new file with the same name without extension and -PROC.CSV added to the name.
-
-The statistics performed on each column are:
-
-* SUM
-
-* MAX
-
-* MIN
-
-* AVERAGE
-
-* COUNT
-
-* COUNTIF &gt; 0
-
-* COUNTIF &gt; 5
-
-* COUNTIF &gt; 10
-
-* COUNTIF &gt; 15
-
-* COUNTIF &gt; 20
-
-* COUNTIF &gt; 25
-
-* COUNTIF &gt; 30
-
-* COUNTIF &gt; 35
-
-* COUNTIF &gt; 40
-
-* COUNTIF &gt; 45
-
-* COUNTIF &gt; 50
-
-* COUNTIF &gt; 55
-
-* COUNTIF &gt; 60
-
-* COUNTIF &gt; 65
-
-* COUNTIF &gt; 70
-
-* COUNTIF &gt; 75
-
-* COUNTIF &gt; 80
-
-* COUNTIF &gt; 85
-
-* COUNTIF &gt; 90
-
-* COUNTIF &gt; 95
-
-* COUNTIF &gt; 100
-
-* COUNTIF = 1
-
-* COUNTIF &lt; 19.9
-
-* COUNTIF &gt; 24.0
-
-Obviously, not all statistics are relevant for every output report variable. The average is based on the sum divided by the number of non-blank rows. The average is not based on the length of time for that timestep. Due to this, CSVproc is best suited for an hourly output file.
-
-Source code is available upon request from jglazer@gard.com.
-
-convertESOMTR
-=============
-
-This simple post processing utility will convert the raw data "ESO" and "MTR" files to IP (Inch-Pound) units before later processing into CSV files. EP-Launch has an option to automatically convert to IP units that invokes convertESOMTR, see VIEW - Options - Miscellaneous dialog box. The ReadVarsESO program will take these converted files and make them into normal CSV files but will have IP units. The RunEPlus batch file does not include this option but could be edited to perform the same functions if desired.
-
-Technically speaking, the convertESOMTR program uses the "convert.txt" file which contains the conversion factors. It creates files "ip.eso" and "ip.mtr" as appropriate. The batch examples then renames the old eplusout.eso to eplusout.esoold, old eplusout.mtr to eplusout.mtrold and the ip files to the default eplusout.eso, eplusout.mtr.
-
-The convert.txt file contains the conversion factors using three different commands.
-
-conv,&lt;si-unit&gt;,&lt;ip-unit&gt;,&lt;multiplier&gt;,&lt;offset&gt;
-
-wild,&lt;match-string&gt;,&lt;si-unit&gt;,&lt;ip-unit&gt;
-
-vari,&lt;variable-name-no-units&gt;,&lt;si-unit&gt;,&lt;ip-unit&gt;
-
-If a specific variable needs to be converted, the 'vari' line may be used to convert the units on that specific variable only. To convert a class of variables that contains a specific string of characters in the names of the variables, the 'wild' line may be used. The 'conv' lines are the lines that actually create the conversion factors.  If no 'vari' or 'wild' match a variable, then it is converted used the first 'conv' line that matches. The default convert.txt file contains some conversions for Inch-Pound units but any set of units may be used by editing the convert.txt file. Note that the convert.txt file uses the standard EnergyPlus comment character (!).
-
-A snippet of the convert.txt file:
-
-```
-! Power
-!------------------------------
-!    (1 kW / 1000 W)
-conv,W,kW,0.001,0
-!    (1 Btuh/ 0.2928751 W) * (1 kBtuh/1000 Btuh)
-conv,W,kBtuh,3.41442E-03,0
-```
-
-CalcSoilSurfTemp Program
-========================
-
-The CalcSoilSurfTemp program calculates three important parameters for the simulation of the earth tube:
-
-- the annual average soil surface temperature
-
-- the amplitude of soil surface temperature
-
-- the phase constant of soil surface temperature
-
-Since soil temperature is one of the most significant factors affecting the overall performance of earth tube system, soil temperature around the earth tube should be accurately predicted.
-
-Before the soil temperature around earth tube can be calculated during the running period of earth tube model in EnergyPlus, the ground surface temperature straight above earth tube should be predicted. Using CalcSoilSurfTemp program, these parameters are predicted by considering the convective heat transfer between the air and ground, solar radiation absorption by the ground, long-wave radiation emitted from the soil, and latent heat loss due to the moisture evaporation at the ground surface.
-
-Running the Program
--------------------
-
-EP-Launch can be used to run the CalcSoilSurfTemp program. CalcSoilSurfTemp is one of the options on the Utilities tab in EP-Launch. See the EP-Launch section in this document for more information on how to use EP-Launch with the CalcSoilSurfTemp program.
-
-You can also run the CalcSoilSurfTemp program as a console application with a batch file RunCalcSoilSurfTemp. The argument to the batch file is the name of the weather file to be used. Steps to running this program follow:
-
-1)   Open a DOS command prompt window (Start à Programs à Accessories à Command Prompt)
-
-2)   Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
-
-C:
-
-CD \\&lt;root folder&gt;\&lt;/span>
-
-3)   Change to the calculate surface soil temperature folder:
-
-CD PreProcess\\CalcSoilSurfTemp
-
-4)   Run the program:
-
-runcalcsoilsurftemp USA\_IL\_Chicago-OHare\_TMY2
-
-When installed, the batch file automatically points the path for weather data to the installed weather data path. If you save your weather files in a different location, you will need to modify the batch file or create your own with your own folder paths.
-
-Note that the program is interactive (expects user responses) from the command line. These inputs are described in the following section.
-
-Program Inputs
---------------
-
-In order to use the CalcSoilSurfTemp program, a weather data file is used. The entire year of weather data is used to calculate parameters of the soil surface temperature.
-
-The CalcSoilSurfTemp program is simple and requires only two input fields: soil condition and soil surface condition. First, the user will see the four following options in the screen for the selection of the soil condition:
-
-1. HEAVY AND SATURATED
-
-2. HEAVY AND DAMP
-
-3. HEAVY AND DRY
-
-4. LIGHT AND DRY
-
-Among them, the user should select the number corresponding to the particular soil condition. This determines the thermal diffusivity and thermal conductivity of the surrounding soil.
-
-After the selection of soil condition, the user should also select the number corresponding to the condition of the ground surface above the earth tube from the eight following options:
-
-1. BARE AND WET
-
-2. BARE AND MOIST
-
-3. BARE AND ARID
-
-4. BARE AND DRY
-
-5. COVERED AND WET
-
-6. COVERED AND MOIST
-
-7. COVERED AND ARID
-
-8. COVERED AND DRY
-
-This determines the absorption coefficient and the fraction of evaporation rate of the ground surface.
-
-Note that both soil condition and soil surface condition are the average of the year -  not a particular time period within the year.
-
-From this information and an analysis of the weather data, the CalcSoilSurfTemp program calculates the annual average soil surface temperature, the amplitude of soil surface temperature, and the phase constant of soil surface temperature. The user must then add these parameters as input parameter into earth tube model in EnergyPlus.
-
-Program Outputs
----------------
-
-As noted earlier, there are three output parameters and they are automatically saved in the CalcSoilSurfTemp.out file. The basic concept and description of three output parameters are as follows.
-
-**Annual Average Soil Surface Temperature**
-
-This is the annual average value of soil surface temperature.
-
-**Amplitude of Soil Surface Temperature**
-
-This is the difference between the maximum and minimum soil surface temperature of the whole year divided by two.
-
-**Phase Constant of Soil Surface Temperature**
-
-This is the time elapsed from the beginning of the year at which the soil surface temperature reaches the minimum value in the year.
-
-These values are placed in the ZoneEarthTube object numeric fields (12, 13, 14) of similar names. The ZoneEarthTube IDD definition with these fields highlighted is included:
-
-```idf
-ZoneEarthtube,
-  \min-fields 22
-  \memo  Earth Tube is specified as a design level which is modified by a Schedule fraction, temperature difference and wind speed:
-  \memo  Earthtube=Edesign * Fschedule * (A + B*|(Tzone-Todb)| + C*WindSpd + D * WindSpd**2)
- A1, \field Zone Name
-  \required-field
-  \type object-list
-  \object-list ZoneNames
- A2, \field Schedule Name
-  \required-field
-  \type object-list
-  \object-list ScheduleNames
- N1, \field Design Flow Rate
-  \required-field
-  \units m3/s
-  \note  "Edesign" in Equation
-  \type real
-  \minimum 0
- N2, \field Minimum Zone Temperature when Cooling
-  \required-field
-  \note this is the indoor temperature below which the earth tube is shut off
-  \units C
-  \type real
-  \minimum -100
-  \maximum 100
- N3, \field Maximum Zone Temperature when Heating
-  \required-field
-  \note this is the indoor temperature above which the earth tube is shut off
-  \units C
-  \type real
-  \minimum -100
-  \maximum 100
- N4, \field Delta Temperature
-  \required-field
-  \note This is the temperature difference between indoor and outdoor below which the earth tube is shut off
-  \units deltaC
-  \type real
-  \minimum 0
- A3, \field Earthtube Type
-  \required-field
-  \type choice
-  \key Natural
-  \key Intake
-  \key Exhaust
-  \default Natural
- N5, \field Fan Pressure Rise
-  \required-field
-  \note pressure rise across the fan
-  \type real
-  \units Pa
-  \minimum 0
-  \default 0
- N6, \field Fan Total Efficiency
-  \required-field
-  \type real
-  \minimum> 0
-  \default 1
- N7, \field Pipe Radius
-  \required-field
-  \units m
-  \type real
-  \minimum> 0
-  \default 1
- N8, \field Pipe Thickness
-  \required-field
-  \units m
-  \type real
-  \minimum> 0
-  \default 0.2
- N9, \field Pipe Length
-  \required-field
-  \units m
-  \type real
-  \minimum> 0
-  \default 15
- N10, \field Pipe Thermal Conductivity
-  \required-field
-  \units W/m-K
-  \type real
-  \minimum> 0
-  \default 200
- N11, \field Pipe Depth Under Ground Surface
-  \required-field
-  \units m
-  \type real
-  \minimum> 0
-  \default 3
- A4, \field Soil Condition
-  \required-field
-  \type choice
-  \key HeavyAndSaturated
-  \key HeavyAndDamp
-  \key HeavyAndDry
-  \key LightAndDry
-  \default HeavyAndDamp
- N12, \field Average Soil Surface Temperature
-  \required-field
-  \units C
-  \type real
-  \default 0
- N13, \field Amplitude of Soil Surface Temperature
-  \required-field
-  \units C
-  \type real
-  \minimum 0
-  \default 0
- N14, \field Phase Constant of Soil Surface Temperature
-  \required-field
-  \units days
-  \type real
-  \minimum 0
-  \default 0
- N15, \field Constant Term Flow Coefficient
-  \required-field
-  \note  "A" in Equation
-  \type real
-  \default 1
- N16, \field Temperature Term Flow Coefficient
-  \required-field
-  \note  "B" in Equation
-  \type real
-  \default 0
- N17, \field Velocity Term Flow Coefficient
-  \required-field
-  \note  "C" in Equation
-  \type real
-  \default 0
- N18; \field Velocity Squared Term Flow Coefficient
-  \required-field
-  \note  "D" in Equation
-  \type real
-  \default 0
-```
-
-HVAC Performance Curve Fit Tool
-===============================
-
-Introduction
-------------
-
-This auxiliary tool generates HVAC performance curves in EnergyPlus curve object format.  For each set of performance data entered, Capacity and EIR performance curves are generated, and these curves are generated either as a function of temperature(s) or flow fraction.  The Capacity and EIR of Cooling DX Coils as a function of temperatures require only Biquadratic curve whereas Capacity and EIR of Heating DX Coils may use Biquadratic, Cubic and Quadratic curves. The selection of either of these curves is dependent on availability of performance data. The Capacity and EIR as a function of flow fraction allows either Cubic or Quadratic curve type. The curve types allowed are:
-
-Biquadratic: <span>\(\text{CurveValue} = a_0 + a_1 X + a_2 X^2 + a_3 Y + a_4 Y^2 + a_5 XY \)</span>
-
-Cubic: <span>\(\text{CurveValue} = a_0 + a_1 X + a_2 X^2 + a_3 X^3 \)</span>
-
-Quadratic: <span>\(\text{CurveValue} = a_0 + a_1 X + a_2 X^2 \)</span>
-
-These performance curves as a function of temperatures are generated for a given set of input data at a given speed. The curves as a function of flow fraction are generated at the rated temperature conditions.  The rated test condition is the AHRI standard test condition (AHRI 2003;2007; 2008).  The AHRI standard test condition may vary by the equipment type.   For multiple speeds or multiple stage DX Coils, different curve sets can be generated by entering a different set of data for each speed or stage at a time.  The tool automatically populates the labels for each data inputs variable when users select the Coil Type, Independent Variables, Curve Type, and Units. The curve fit tool interface in Figure 1 shows labels selected to generate capacity and EIR biquadratic curves as function of temperatures for DX cooling coil.
-
-![](media/image034.jpg)
-
-Figure 33. Curve Fit Tool Input Interface
-
-The tool can be used for Coil:Cooing:DX:SingleSpeed, Coil:Heating:DX:SingleSpeed, Coil:Cooing:DX:TwoSpeed (high and low speed) , CoilPerformance:DX:Cooling (each stage), and any HVAC equipment that use Biquadratic, Cubic or Quadratic curves. To add this flexibility generic input data labels can be populated by selecting "Other" for DX Coil Type input field, located in Cell B3 in Figure 33.
-
-Inputs
-------
-
-First step in curve generation is to select appropriate parameters from the dropdown menu.  These inputs define the DX Coil Type, Curve Type, Independent Variable and the Units type. The choices available for each input parameters are described in table-1. Once these input parameters are selected the tool read in the values and automatically populates labels for each of the independent and dependent variables. The labels guide users to enter the data for each variable in the corresponding worksheet input range.   Two sets of input data are required for curve generation: Rated, and Performance Data.
-
-Table-1 Input parameters description
-
-<table class="table table-striped">
-<tr>
-<th>Input Parameter</th>
-<th>Description of Inputs</th>
-</tr>
-<tr>
-<td>DX Coil Type</td>
-<td>Cooling: applicable for DX cooling coil single speed
-Heating: applicable for DX heating coil single speed
-Other: applicable for any equipment that use the three curve types</td>
-</tr>
-<tr>
-<td>Independent Variables</td>
-<td>Temperature
-Flow</td>
-</tr>
-<tr>
-<td>Curve Types</td>
-<td>Biquadratic: Capacity and EIR as a function of temperature
-Cubic: Capacity and EIR as a function of flow fraction or temperature
-Quadratic: capacity and EIR as a function of flow fraction</td>
-</tr>
-<tr>
-<td>Units</td>
-<td>IP: Temperature in °F, Capacity in kBtu/h, Power in kW, and Flow in CFM
-SI: Temperature in °C, Capacity in kW, Power in kW, and Flow in m<sup>3</sup>/s</td>
-</tr>
-<tr>
-<td>Curve Object Name</td>
-<td>This input is optional.  This string is appended to the default curve object name, or if left blank the default curve object name will be displayed. A curve object is named is created by concatenation as follows:
-<span>\(
-=
-\left\{
- \begin{array}{c}
-  \text{User Specified} \\
-  \text{Curve Object Name}
- \end{array}
-\right\} + 
-\text{"DXCoilType"} + 
-\left\{
- \begin{array}{c}
-  \text{CAPFTemp} \\ 
-  \text{CAPFFF} \\
-  \text{EIRFTemp} \\
-  \text{EIRFFF}
- \end{array}
-\right\}
-\)</span></td>
-</tr>
-</table>
-
-Rated Data
-----------
-
-The rated data is used to normalize the performance data set. The rated test conditions depend on the equipment type.  For DX cooling coil the rated test temperatures are 67°F (19.4°C) indoor coil entering wet bulb, 80°F (26.7°C) indoor coil entering dry bulb and 95°F (35.0°C) outdoor coil entering dry bulb air temperatures per ANSI/AHRI Std. 210/240 (AHRI 2008).  If the rated test temperatures are different from the values populated by the tool, then the user may enter the applicable values manually.  The rated data can be one of the performance data points depending on the speed or stage. The rated data set is entered in the Cells range "B11:E11" of the INPUT tab as shown in Figure 1.
-
-Performance Data
-----------------
-
-The performance data set entered depends on the type of independent variables selected.  To generate performance curves (e.g. DX Coils) as a function of temperatures require the capacity and power data at various combinations of indoor and outdoor coil entering air temperatures at a rated supply air flow rate. And performance curves (e.g. DX Coil) as function of flow fraction require  capacity and power data at various supply air flow rates and rated indoor and outdoor coil entering air (or water) temperatures. The performance data set may include the rated data as one of the data points. The performance data set is entered starting from row 15 and down for each of the variables as shown in Figure 33.
-
-The total cooling and heating capacities must be the gross values, i.e., not corrected for the supply fan heating effect.  Also the input power has to exclude the supply air fan power, but includes other miscellaneous power inputs (e.g. control panel power).   If manufacturers provide the total power, then the supply fan power must be deducted from the former.  If the capacity and power data are normalized values, then enter 1.0 for rated gross capacity and power in the ***Rated Data*** input Cells range (B11:E11 in the INPUT tab). Two samples of performance and rated data set are included in the "**INSTRUCTION**" tab.
-
-Outputs
--------
-
-The generated curves are post-processed to make sure that the curve value is 1.0 at the rated condition.  The post processing is applied only if the curve value at the rated condition deviates by a value less than or equal to 0.025 and the performance data set contains the rated data set as one the data points. The coefficients of these curves are displayed on the "OUTPUT" tab as shown in Figure 2.
-
-![](media/image036.jpg)
-
-Figure 34. Curve Fit Tool Output Interface
-
-Besides the curve coefficients, the goodness of curve fit indicator statistical parameters *R<sup>2</sup>* is also reported.  The *R<sup>2</sup>* is the ratio of the sum of the squared deviations of the curve fit values from the mean to the sum of the squared deviations of the original data from the mean.  R squared values closer to 1.0 are good.  The tool has an option to save the curve objects to an output file by running another macro (SaveCurveObjToTextFile).  The option output files and the directory path are specified in the OUPUT tab in cells C2 and C3, respectively, as shown in Figure 34. If the output file name and path are left blank, then default names, "EplusCurveObjects.IDF" and the local directory where the tool is located are used.  The local directory where the tool is located must not have write restriction.
-
-Sample EnergyPlus curve objects output file generated using this auxiliary tool.
-
-```idf
-Curve:Biquadratic,
- HeatPumpCoolingCAPFTemp,      !- Name
- 1.4248528695,                !- Coefficient1 Constant
- -0.0554469607,                !- Coefficient2 x
- 0.0027506982,                !- Coefficient3 x**2
- -0.0017453896,                !- Coefficient4 y
- -0.0000081,                   !- Coefficient5 y**2
- -0.0004638975,                !- Coefficient6 x*y
- 13.8888888889,                !- Minimum Value of x
- 22.2222222222,                !- Maximum Value of x
- 29.4444444444,                !- Minimum Value of y
- 46.1111111111,                !- Maximum Value of y
- 0.7875,                       !- Minimum Curve Output
- 1.1725,                       !- Maximum Curve Output
- Temperature,                  !- Input Unit Type for X
- Temperature,                  !- Input Unit Type for Y
- Dimensionless;                !- Output Unit Type
-
-Curve:Biquadratic,
- HeatPump1CoolingEIRFTemp,     !- Name
- 0.1566419771,                 !- Coefficient1 Constant
- 0.0522807347,                 !- Coefficient2 x
- -0.0017986792,                !- Coefficient3 x**2
- 0.009523995,                  !- Coefficient4 y
- 0.0002405903,                 !- Coefficient5 y**2
- -0.0001781171,                !- Coefficient6 x*y
- 13.8888888889,                !- Minimum Value of x
- 22.2222222222,                !- Maximum Value of x
- 29.4444444444,                !- Minimum Value of y
- 46.1111111111,                !- Maximum Value of y
- 0.8216,                       !- Minimum Curve Output
- 1.3703,                       !- Maximum Curve Output
- Temperature,                  !- Input Unit Type for X
- Temperature,                  !- Input Unit Type for Y
- Dimensionless;                !- Output Unit Type
-```
-
-
-Error Message
--------------
-
-Reports progress of the curve object generation calculation starting from reading input data to error massage output file "errorCurveObjects.txt".  This error message file provides information whether the tool run successfully or not.  Also points to the step where problem occurred.
-
-Notes
------
-
-This tool has been tested on Ubuntu 11 using Libre Office and MS Office Macintosh 2011 machines.  But the button for running the macro may not be imported properly on Ubuntu hence users may have to run the tool manually by selecting "**ManageCurveFit**" and "**SaveCurveObjToTextFile**" subroutine from the macro list.
-
-References
-----------
-
-AHRI 2008. ANSI/AHRI Standard 210/240: 2008 Standard for Performance Rating of Unitary Air-Conditioning & Air-Source Heat Pump Equipment. Arlington, VA: Air-Conditioning, Heating, and Refrigeration Institute.
-
-AHRI 2007. ANSI/AHRI Standard 340/360: 2007 Standard for Performance Rating of Commercial and Industrial Unitary Air-Conditioning and Heat Pump Equipment. Arlington, VA: Air-Conditioning, Heating, and Refrigeration Institute.
-
-AHRI 2003. ANSI/AHRI Standard 550/590: 2003 Standard for Performance Rating Of Water -Chilling Packages Using The Vapor Compression Cycle. Arlington, VA: Air-Conditioning, Heating, and Refrigeration Institute.
-
-
-
-Parametric Spreadsheets
-=======================
-
-Several spreadsheet applications are included in the Preprocess\\ParametricSpreadsheets folder.  These include spreadsheets (Excelâ„¢) for the Water Source heat pumps and Water to Air heat pumps.
-
-Water-to-Water Heat Pump Parameter / Coefficient Generator (Cooling and Heating Mode)
--------------------------------------------------------------------------------------
-
-This document gives brief instructions on generating the parameters/ coefficients for the water-to-water heat pump models in cooling and heating mode. The Excelâ„¢ spreadsheets (WaterWater\_PE\_Cooling.xls and WaterWater\_PE\_Heating.xls) are used. Since the spreadsheet functions are very similar for both cooling and heating modes, only one instruction document is supplied. The spreadsheet generates:
-
-- parameters for the parameter estimation based model.
-
-- coefficients for the curve-fit model.
-
-The following theses have detailed information about the curve-fit model and parameter estimation based model:
-
-Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at [www.hvac.okstate.edu](http://www.hvac.okstate.edu))
-
-Shenoy,Arun. 2004. Simulation, Modeling and Analysis of Water to Air Heat Pump. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at [www.hvac.okstate.edu](http://www.hvac.okstate.edu))
-
-Tang,C.C. 2004. Modeling Packaged Heat Pumps in a Quasi-Steady State Energy Simulation Program. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at [www.hvac.okstate.edu](http://www.hvac.okstate.edu))
-
-### Step 1: Catalog Data Input
-
-Data points are obtained from the heat pump manufacturer data. Minimum data points for the parameter estimation based model are 32 data points according to Jin (2002). The curve-fit model performance is not affected by the number of data points and a minimum of 5 data points is required since the governing equations require 6 coefficients. The data points must have varying inlet conditions (e.g. water flow rates, inlet water temperatures, etc.) that covers the entire range of the heat pump operating conditions. Correction tables provided by the manufacturer should be used to extend the catalog data range in order to have a good set of parameters/coefficients.
-
-- Using the heat pump performance data, enter the values to Table 1 in worksheet "CATALOG DATA". The values can be in SI or IP units.
-
-- Click on Button 1 based on the units used.
-
-For IP units:
-
-![](media/image037.png)
-
-For SI units:
-
-![](media/image038.png)
-
-- The program will convert the values to the desired units and display them on Table 2 in worksheet "INPUT".
-
-- The button shown below is used clearing Table 1 (worksheet "CATALOG DATA"), and Table 2 (worksheet "INPUT"). It is advisable to clear the tables before generating parameters/coefficients for a new heat pump model.
-
-![](media/image039.png)
-
-After Table 2 is created, the parameters/coefficients are then calculated as follows:
-
-- Worksheet "ParamEstimator" is used for generating the parameters for the parameter estimation based model using Nelder Mead Simplex. Refer to the steps in the Parameter Estimation Procedure.
-
-- Worksheet "CoeffCalculator" is used for calculate the coefficients for the curve-fit model using the generalized least square method. Refer to the steps in the Curve Fit Model procedure.
-
-### Parameter Estimation Procedure
-
-#### Step 2a: Generating First Set of Parameters (PE-Based Model)
-
-- Using Table 2, the program can generate parameters. The user must fill all the cells colored light blue in worksheet "ParamEstimator".
-
-- **Accuracy:** Start with a low accuracy for faster convergence, recommended value of 0.001.
-
-- **Compressor Type:** Only reciprocating compressor is currently available in EnergyPlus. One might be able to generate parameters for heat pump model with different compressor types but this might result in unrealistic parameters.
-
-- **Refrigerant:** Contact the manufacturer on the refrigerant used to generate the catalog data and select from the list of refrigerants. Usually the refrigerant used is R22. .
-
-- **Which Initial Guess?:**  The user may choose a set of initial guesses(1-5) that will be used by the optimization routine in generating the parameters. Start with 1, which is the set of initial guess 1 at column B.
-
-- **Initial Guess:** Initial guess for all the parameters. For Initial Guess 1, enter a value of 1 for all the parameters except for the loss factor (less than 1.0). The loss factor should be less than 1.0 because the efficiency of the compressor should be less than 100%. Adjust the values in Initial Guess 1 if the program happens to crash and try again.
-
--  Now click on Button 2 shown below to generate the parameters.
-
-![](media/image040.png)
-
-It will take some time to generate the parameters depending on the number of data points. The parameters generated will be displayed at Parameters 1.
-
-- Look at the error analysis of Error 1 which gives the user a summary of the errors for Qload, Qsource and Power. An average error of 5-8% is achievable for all the values.
-
-- The errors for all the individual catalog data points are displayed in worksheet "RESULT".
-
-#### Step 2b: Improving the Set of Parameters (PE-Based Model)
-
-- After the initial set of parameters has been generated, the user can increase the accuracy of the parameters by using parameters generated as the initial guess for the second simulation and increasing the accuracy of the program.
-
-- Copy and Paste Parameters 1 to Initial Guess 2.
-
-- Change the initial guess indicator (**Which Initial Guess?:)** from 1 to 2.
-
-- Increase the accuracy by twice. For example, set accuracy to 0.000001.
-
-- Now click on Button 2 shown below to generate the second set of parameters.
-
-![](media/image041.png)
-
-The simulation time would most likely be less but it depends on the accuracy value as well. And the parameters generated will be displayed at Parameter 2.
-
-- Compare Error 2 to Error 1, the error values should be less which means that the parameters are getting better and more accurate.
-
-- Repeat the steps in 2a and 2b until a desired set of error values is achieved or the errors stop decreasing
-
-#### Step 3: Generating EnergyPlus Input Parameters
-
-- Click on the Button 3 shown below to convert and arrange the parameters generated to fit EnergyPlus Input File (IDF) which will be listed from cell B52:B59 for cooling mode and B46:B54 for heating mode.
-
-![](media/image042.png)
-
-- The button shown below in worksheet "ParamEstimator" is used for clearing Initial Guess (2-5), Parameters(1-5), Error(1-5), EnergyPlus Input parameters and Result(1-5) in worksheet "RESULT".
-
-![](media/image043.png)
-
-### End Parameter Estimation Procedure
-
-### Curve Fit Model Procedure
-
-#### Step 2: Generating the coefficients (Curve-Fit Model)
-
-- Using Table 2, the program is ready to generate the coefficients. User is required to fill all the cells colored light blue in worksheet "CoeffCalculator".
-
-- **RatedLoadVolFlowRate:** Rated load side volumetric flow rate (m<sup>3</sup>/s) which corresponds to the highest load side heat transfer rate listed in the catalog data.
-
-- **RatedSourceVolFlowRate:** Rated source side volumetric flow rate (m<sup>3</sup>/s) which corresponds to the highest load side heat transfer rate listed in the catalog data.
-
-- **RatedQload:** Rated load side heat transfer rate (W) which is the highest load side heat transfer rate listed in the catalog data.
-
-- **RatedPower:** Rated power consumption (W) which corresponds to the highest load side heat transfer rate listed in the catalog data.
-
-- Now click on Button 2 shown below to calculate the coefficients.
-
-![](media/image044.png)
-
-- The coefficients for the corresponding curves are listed at cell B12:C16. Error analysis of model is listed at cell B19:B27.
-
-- The errors for all the individual catalog data points are displayed in worksheet "RESULT".
-
-- The button shown below in worksheet "CoeffCalculator" is used for clearing the coefficients, the error analysis and the outputs in worksheet "RESULT".
-
-![](media/image045.png)
-
-### End Curve Fit Model Procedure
-
-Water-to-Air Heat Pump Parameter / Coefficient Generator (Cooling)
-------------------------------------------------------------------
-
-This document gives brief instructions on generating the parameters or coefficients for the water-to-air heat pump models in cooling mode. The Excelâ„¢ spreadsheets (WaterAir\_PE\_Cooling.xls) are used. The spreadsheet generates:
-
-- parameters for the parameter estimation based model.
-
-- coefficients for the curve-fit model.
-
-The following theses have detailed information about the curve-fit model and parameter estimation based model:
-
-Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at [www.hvac.okstate.edu](http://www.hvac.okstate.edu))
-
-Shenoy,Arun. 2004. Simulation, Modeling and Analysis of Water to Air Heat Pump. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at [www.hvac.okstate.edu](http://www.hvac.okstate.edu))
-
-Tang,C.C. 2004. Modeling Packaged Heat Pumps in a Quasi-Steady State Energy Simulation Program. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at [www.hvac.okstate.edu](http://www.hvac.okstate.edu))
-
-### Step 1: Catalog Data Input
-
-Data points are obtained from the heat pump manufacturer data. Minimum data points for the parameter estimation based model are 32 data points according to Jin (2002). The curve-fit model performance is not affected by the number of data points and a minimum of 6 data points is required since the sensible cooling capacity requires 6 coefficients. The data points must have varying inlet conditions (e.g. air flow rates, inlet water temperatures, and etc.) that covers the entire range of the heat pump operating conditions. Correction tables provided by the manufacturer should be used to extend the catalog data range in order to have a good set of parameters/coefficients.
-
-- Using the heat pump performance data, enter the values to Table 1 in worksheet "CATALOG DATA". The values can be in SI or IP units.
-
-- Click on Button 1 based on the units used.
-
-For IP units:
-
-![](media/image046.png)
-
-For SI units:
-
-![](media/image047.png)
-
-- The program will convert the values to the desired units and display them on Table 2 in worksheet "INPUT".  Then the program will discard bad catalog points by calculating the relative humidity of the exiting air at the load side (relative humidity should be less or equal to 1). Table 3 in worksheet "INPUT" shows the input catalog data that will be used by the parameter/coefficient generator program.
-
-- The button shown below is used clearing Table 1 (worksheet "CATALOG DATA"), Table 2, and Table 3 (worksheet "INPUT"). It is advisable to clear the tables before generating parameters/coefficients for a new heat pump model.
-
-![](media/image048.png)
-
-After Table 3 is created, the parameters/coefficients are then calculated as follows:
-
-- Worksheet "ParamEstimator" is used for generating the parameters for the parameter estimation based model using Nelder Mead Simplex. Refer to the steps in the Parameter Estimation Procedure.
-
-- Worksheet "CoeffCalculator" is used for calculate the coefficients for the curve-fit model using the generalized least square method. Refer to the steps in the Curve Fit Model procedure.
-
-### Parameter Estimation Procedure
-
-#### Step 2a: Generating First Set of Parameters (PE-Based Model)
-
-- Using contents of Table 3, the program can generate parameters. The user must fill all the cells colored light blue in worksheet "ParamEstimator".
-
-- **Accuracy:** Start with a low accuracy for faster convergence, recommended value of 0.001.
-
-- **Compressor Type:** User is allowed to select from 3 types of compressors: scroll, rotary or reciprocating. Contact the manufacturer to make sure that the compressor selected is correct. Wrong type of compressor selected would lead to the program crashing or inaccurate parameters.
-
-- **Refrigerant:** Contact the manufacturer on the refrigerant used to generate the catalog data and select from the list of refrigerants. Usually the refrigerant used is R22. .
-
-- **Which Initial Guess?:**  The user may choose a set of initial guesses(1-5) that will be used by the optimization routine in generating the parameters. Start with 1, which is the set of initial guesses 1 at column B.
-
-- **Initial Guess:** Initial guess for all the parameters. For Initial Guess 1, enter a value of 1 for all the parameters except for the loss factor (less than 1.0). The loss factor should be less than 1.0 because the efficiency of the compressor should be less than 100%. Adjust the values in Initial Guess 1 if the program happens to crash and try again.
-
--  Now click on Button 2 shown below to generate the parameters.
-
-![](media/image049.png)
-
-It will take some time to generate the parameters depending on the number of data points. The parameters generated will be displayed at Parameters 1.
-
-- Look at the error analysis of Error 1, which gives the user a summary of the errors for Qtotal, Qsensible, Qsource and Power. An average error of 5-8% is achievable for all the values.
-
-- The errors for all the individual catalog data points are displayed in worksheet "RESULT".
-
-#### Step 2b: Improving the Set of Parameters (PE-Based Model)
-
-- After the initial set of parameters has been generated, the user can increase the accuracy of the parameters by using parameters generated as the initial guess for the second simulation and increasing the accuracy of the program.
-
-- Copy and Paste Parameters 1 to Initial Guess 2.
-
-- Change the initial guess indicator **(Which Initial Guess?)** from 1 to 2.
-
-- Increase the accuracy by twice. For example, set accuracy to 0.000001.
-
-- Now click on Button 2 shown below to generate the second set of parameters.
-
-![](media/image041.png)
-
-The simulation time would most likely be less but it depends on the accuracy value as well. The parameters generated will be displayed at Parameter 2.
-
-- Compare Error 2 to Error 1, the error values should be less which means that the parameters are getting better and more accurate.
-
-- Repeat the steps in 2a and 2b until a desired set of error values is achieved or the errors stop decreasing
-
-#### Step 3: Generating EnergyPlus Input Parameters
-
-- Click on the Button 3 shown below to convert and arrange the parameters generated to fit EnergyPlus Input File (IDF), which will be listed from cell B52:B61.
-
-![](media/image050.png)
-
-- The button shown below in worksheet "ParamEstimator" is used for clearing Initial Guess (2-5), Parameters(1-5), Error(1-5), EnergyPlus Input parameters and Result(1-5) in worksheet "RESULT".
-
-![](media/image051.png)
-
-### End Parameter Estimation Procedure
-
-### Curve Fit Model Procedure
-
-#### Step 2: Generating the coefficients (Curve-Fit Model)
-
-- Using the contents of Table 3, the program can generate the coefficients. The user must fill all the cells colored light blue in worksheet "CoeffCalculator".
-
-- **RatedAirVolFlowRate:** Rated volumetric air flow rate (m<sup>3</sup>/s) which corresponds to the highest total cooling capacity listed in the catalog data.
-
-- **RatedWaterVolFlowRate:** Rated volumetric water flow rate (m<sup>3</sup>/s) which corresponds to the highest total cooling capacity listed in the catalog data.
-
-- **RatedTotalCap:** Rated total cooling capacity (W) which is the highest total cooling capacity listed in the catalog data.
-
-- **RatedSensCap:** Rated sensible cooling capacity (W) which corresponds to the highest total cooling capacity listed in the catalog data.
-
-- **RatedPower:** Rated power consumption (W) which corresponds to the highest total cooling capacity listed in the catalog data.
-
-- Now click on Button 2 shown below to calculate the coefficients.
-
-![](media/image052.png)
-
-- The coefficients for the corresponding curves are listed at cell B12:D17. Error analysis of model are listed at cell B19:B30.
-
-- The errors for all the individual catalog data points are displayed in worksheet "RESULT".
-
-- The button shown below in worksheet "CoeffCalculator" is used for clearing the coefficients, the error analysis and the outputs in worksheet "RESULT".
-
-![](media/image053.png)
-
-### End Curve Fit Model Procedure
-
-Water-to-Air Heat Pump Parameter / Coefficient Generator (Heating Mode)
------------------------------------------------------------------------
-
-This document gives brief instructions on generating the parameters/ coefficients for the water-to-air heat pump models in heating mode. The Excelâ„¢ spreadsheets (WaterAir\_PE\_Heating.xls) are used. The spreadsheet generates:
-
-- parameters for the parameter estimation based model.
-
-- coefficients for the curve-fit model.
-
-The following theses have detailed information about the curve-fit model and parameter estimation based model:
-
-Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at [www.hvac.okstate.edu](http://www.hvac.okstate.edu))
-
-Shenoy,Arun. 2004. Simulation, Modeling and Analysis of Water to Air Heat Pump. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at [www.hvac.okstate.edu](http://www.hvac.okstate.edu))
-
-Tang,C.C. 2004. Modeling Packaged Heat Pumps in a Quasi-Steady State Energy Simulation Program. M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable at [www.hvac.okstate.edu](http://www.hvac.okstate.edu))
-
-### Step 1: Catalog Data Input
-
-Data points are obtained from the heat pump manufacturer data. Minimum data points for the parameter estimation based model are 32 data points according to Jin (2002). The curve-fit model performance is not affected by the number of data points and a minimum of 5 data points is required since the governing equations require 5 coefficients. The data points must have varying inlet conditions (e.g. air flow rates, inlet water temperatures, and etc.) that covers the entire range of the heat pump operating conditions. Correction tables provided by the manufacturer should be used to extend the catalog data range in order to have a good set of parameters/coefficients.
-
-- Using the heat pump performance data, enter the values to Table 1 in worksheet "CATALOG DATA". The values can be in SI or IP units.
-
-- Click on Button 1 based on the units used.
-
-For IP units:
-
-![](media/image054.png)
-
-For SI units:
-
-![](media/image055.png)
-
-- The program will convert the values to the desired units and display them on Table 2 in worksheet "INPUT" which will be used by the parameter/coefficient generator program.
-
-- The button shown below is used for clearing Table 1 (worksheet "CATALOG DATA") and Table 2 (worksheet "INPUT"). It is advisable to clear the tables before generating parameters/coefficients for a new heat pump model.
-
-![](media/image056.png)
-
-After Table 2 is created, the parameters/coefficients are then calculated as follows:
-
-- Worksheet "ParamEstimator" is used for generating the parameters for the parameter estimation based model using Nelder Mead Simplex. Refer to the steps in the Parameter Estimation Procedure.
-
-- Worksheet "CoeffCalculator" is used for calculate the coefficients for the curve-fit model using the generalized least square method. Refer to the steps in the Curve Fit Model procedure.
-
-### Parameter Estimation Procedure
-
-#### Step 2a: Generating First Set of Parameters (PE-Based Model)
-
-- Using Table 2, the program can generate parameters. The user must fill all the cells colored light blue in worksheet "ParamEstimator".
-
-- **Accuracy:** Start with a low accuracy for faster convergence, recommended value of 0.001.
-
-- **Compressor Type:** User is allowed to select from 3 types of compressors: scroll, rotary or reciprocating. Contact the manufacturer to make sure that the compressor selected is correct. Wrong type of compressor selected would lead to the program crashing or inaccurate parameters.
-
-- **Refrigerant:** Contact the manufacturer on the refrigerant used to generate the catalog data and select from the list of refrigerants. Usually the refrigerant used is R22. .
-
-- **Source Side Fluid:** Select the type of fluid used for the source side. 0: Water, 1: Antifreeze Mixture. Note that the number of parameters will change depending on the type of fluid. Antifreeze mixture requires one additional parameter.
-
-- **Which Initial Guess?:**  The user may choose a set of initial guesses(1-5) that will be used by the optimization routine in generating the parameters. Start with 1, which is the set of initial guesses 1 at column B.
-
-- **Initial Guess:** Initial guess for all the parameters. For Initial Guess 1, enter a value of 1 for all the parameters except for the loss factor (less than 1.0). The loss factor should be less than 1.0 because the efficiency of the compressor should be less than 100%. Adjust the values in Initial Guess 1 if the program happens to crash and try again.
-
--  Now click on Button 2 shown below to generate the parameters.
-
-![](media/image057.png)
-
-It will take some time to generate the parameters depending on the number of data points. The parameters generated will be displayed at Parameters 1.
-
-- Look at the error analysis of Error 1, which gives the user a summary of the errors for Heating Capacity, Heating Absorption and Power. An average error of 5-8% is achievable for all the values.
-
-- The errors for all the individual catalog data points are displayed in worksheet "RESULT".
-
-#### Step 2b: Improving the Set of Parameters (PE-Based Model)
-
-- After the initial set of parameters has been generated, the user can increase the accuracy of the parameters by using parameters generated as the initial guess for the second simulation and increasing the accuracy of the program.
-
-- Copy and Paste Parameters 1 to Initial Guess 2.
-
-- Change the initial guess indicator **(Which Initial Guess?)** from 1 to 2.
-
-- Increase the accuracy by twice. For example, set accuracy to 0.000001.
-
-- Now click on Button 2 shown below to generate the second set of parameters.
-
-![](media/image041.png)
-
-The simulation time would most likely be less but it depends on the accuracy value as well. And the parameters generated will be displayed at Parameter 2.
-
-- Compare Error 2 to Error 1, the error values should be less, which means that the parameters are getting better and more accurate.
-
-- Repeat the steps in 2a and 2b until a desired set of error values is achieved or the errors stop decreasing
-
-#### Step 3: Generating EnergyPlus Input Parameters
-
-- Click on the Button 3 shown below to convert and arrange the parameters generated to fit EnergyPlus Input File (IDF), which will be listed from cell B46:B54.
-
-![](media/image058.png)
-
-- The button shown below in worksheet "ParamEstimator" is used for clearing Initial Guess (2-5), Parameters(1-5), Error(1-5), EnergyPlus Input parameters and Result(1-5) in worksheet "RESULT".
-
-![](media/image059.png)
-
-### End Parameter Estimation Procedure
-
-### Curve Fit Model Procedure
-
-#### Step 2: Generating the coefficients (Curve-Fit Model)
-
-- Using Table 2, the program can generate the coefficients. The user must fill all the cells colored light blue in Worksheet "CoeffCalculator".
-
-- **RatedAirVolFlowRate:** Rated volumetric air flow rate (m<sup>3</sup>/s) which corresponds to the highest heating capacity listed in the catalog data.
-
-- **RatedWaterVolFlowRate:** Rated volumetric water flow rate (m<sup>3</sup>/s) which corresponds to the highest heating capacity listed in the catalog data.
-
-- **RatedTotalCap:** Rated heating capacity (W) which is the highest heating capacity listed in the catalog data.
-
-- **RatedPower:** Rated power consumption (W) which corresponds to the highest heating capacity listed in the catalog data.
-
-- Now click on Button 2 shown below to calculate the coefficients.
-
-![](media/image060.png)
-
-- The coefficients for the corresponding curves are listed at cell B12:C16. Error analysis of model are listed at cell B19:B27.
-
-- The errors for all the individual catalog data points are displayed in worksheet "RESULT".
-
-- The button shown below in worksheet "CoeffCalculator" is used for clearing the coefficients, the error analysis and the outputs in worksheet "RESULT".
-
-![](media/image059.png)
-
-### End Curve Fit Model Procedure
-
-G-Function Spreadsheet
-----------------------
-
-The spreadsheet (g-function\_library.xls) has comparison plots for different configurations/grouts for the Ground Heat Exchanger:Vertical. A user can see how the boreholes interact with each other in different configurations. It has the actual screen shot (GLHEPro) showing the conditions/inputs used to obtain the data. GLHEPro is not included with EnergyPlus and it or something similar should be used to generate similar values. Some of the values used in getting g-functions are not used in the EnergyPlus Ground loop model, but the spreadsheet screen shot gives an idea of what the inputs were in obtaining the g-functions.
-
-The reference data set GLHERefData.idf contains sets of parameters for the Ground Heat Exchangers:
-
-"This file contains sample input for the ground loop heat exchanger model. The response of the borehole/ground is found from the 'G-function' that is defined in the input as series of 'n' pairs of values (LNTTSn, GNFCn). It is important to note that the G-functions have to be calculated for specific GHE configurations and borehole resitance, length and borehole/ length ratio. That is, the parameters for the units vary with each design. The data in this file are intended as examples/samples and may not represent actual designs.
-
-The sample data has been calculated for a number of configurations:
-
-- 1 x 2 boreholes
-
-- 4 x 4 boreholes
-
-- 8 x 8 boreholes
-
-Data is given for both 'standard' grout (k=0.744 W/m.K) and 'thermally enhanced' grout (k= 1.471 W/m.K). The flow rate per borehole is .1514 kg/s. The pipe given is 0.75in. Dia. SDR11 HDPE. The fluid is water. The borehole/length ratio is 0.06 (76.2m/4.572m [300ft/15ft])
-
-ParametricPreprocessor
-======================
-
-The parametric preprocessor used to create a series of resulting IDF files from a single source IDF file that contains parametric objects and expressions. The parametric objects in EnergyPlus are interpreted by the ParametricPreprocessor and are:
-
-* Parametric:SetValueForRun
-* Parametric:Logic
-* Parametric:RunControl
-* Parametric:FileNameSuffix
-
-The ParametricPreprocessor reads the source IDF file and removes the Parametric objects shown above, processes these objects and any embedded expressions and produces a series of resulting IDF files, one for each "run" described by the objects.
-
-An intermediate file called parametric.int is used that contains references to all embedded expressions that will need to be substituted into the file.
-
-An error file called parametric.err is also produced to help debug problems with the objects.
-
-The Parametric objects are described in detail in the InputOutputReference document.
-
-ParametricPreprocessor can be called at the command line with the name of the source file as the only argument.
-
-The ParametricPreprocessor is used in the batch files that come with EnergyPlus and is used by EP-Launch automatically.
-
-AppGPostProcess - Appendix G PostProcessing program
-===================================================
-
-The baseline for Standard 90.1 Appendix G requires simulating the baseline building in four cardinal directions and comparing the average of those simulation results with the proposed building simulation results.  The AppGPostProcess utility helps perform the averaging needed. The utility takes the four HTML files generated by EnergyPlus and creates an average HTML file. In addition, the AppGPostProcess utility takes the four CSV files (based on ESO files) and creates an average CSV file as well as averaging the meter CSV files (based on the MTR files).  The source files must have specific names for this utility to work:
-
-fileNameRoot-G000.csv
-
-fileNameRoot-G090.csv
-
-fileNameRoot-G180.csv
-
-fileNameRoot-G270.csv
-
-fileNameRoot-G000Meter.csv
-
-fileNameRoot-G090Meter.csv
-
-fileNameRoot-G180Meter.csv
-
-fileNameRoot-G270Meter.csv
-
-fileNameRoot-G000Table.html
-
-fileNameRoot-G090Table.html
-
-fileNameRoot-G180Table.html
-
-fileNameRoot-G270Table.html
-
-Where "fileNameRoot" can be the characters typically used to name files without extension. A single command line argument is passed to the AppGPostProcess utility which is the name of one of the HTML files. The remaining file names will be used based on any of the HTML files selected.
-
-The utility creates the files
-
-fileNameRoot-GAVG.csv
-
-fileNameRoot-GAVGMeter.csv
-
-fileNameRoot-GAVGTable.html
-
-The numeric values in the output files are the average results from the four corresponding source files. In the HTML file, if not all the four files contain a numeric value, then the four values are displayed instead. The source files must have identical structure for AppGPostProcess to work. For CSV files, the same number of rows and the same number of columns are needed each file. This means that monthly or hourly values should be included in the CSV file, and not TimeStep values. For HTML files, the same reports should be included in each and the IDF files should be identical.
-
-The intention is that the four baseline IDF files would be identical except for the use of the Compliance:Building object and only the value of the field "Building Rotation for Appendix G" would change.
-
-EP-Launch can be used to run both the AppGPostProcess program by using the Utilities tab in EP-Launch.  See the EP-Launch section in this document for more information on how to use EP-Launch.
-
-
-
-BLASTTranslator
-===============
-
-The BLAST Translator will produce an IDF file from an existing BLAST Input File (usually called &lt;something&gt;.bin. For anyone that is unfamiliar, BLAST stands for the Building Loads Analysis and Systems Thermodynamics computer program.  Documentation is included here though the BLAST Translator is no longer included with the EnergyPlus Installation - it is available as a special download for those who need it.
-
-A special batch file (**RunXLate.bat**) can be used to run the translation program. Similar to running EnergyPlus (see above), you run this batch file:
-
-RunXLate &lt;blastinputfile&gt;
-
-Where &lt;blastinputfile&gt; is the part of the file name without extension. The program produces a .idf file of the same name.
-
-The BLASTTranslator uses an "Energy+.ini" file for some parameters. For example:
-
-```
-[program]
-dir=
-ver=
-surf=group
-
-[weather]
-dir=
-```
-
-The above BLASTTranslator ini file sets the "version" of EnergyPlus to the current version and has the "surf" parameter set to "group". This BLASTTranslator run will produce an EnergyPlus input file for the current release version format and will name surfaces by Zone and Class (e.g. ZN001:Wall001). The alternative "Consecutive" will number surfaces in sequence.
-
-DOE2Translator
-==============
-
-The DOE2Translator program creates an EnergyPlus input file from a DOE-2.1E input file. The translation is not intended to be complete but simply an aid to help you move your library of DOE-2.1E input files into EnergyPlus. You should look over the resulting EnergyPlus input file, review the documentation of EnergyPlus, and make any necessary edits to the translated file. Documentation is included here though the BLAST Translator is no longer included with the EnergyPlus Installation - it is available as a special download for those who need it.
-
-To use the DOE2Translator program, at the DOS prompt (or the command prompt for Windows NT/2000 systems), go to the directory that the DOE2Translator is located. That directory is likely to be:
-
-  c:\\EnergyPlus\\PreProcess\\DOE2Translator
-
-In this directory there should be several files:
-
-  DOE2Translator.exe   - the program
-
-  D2E\_macr.txt         - a support file that contains the header of the translated file
-
-  D2comkey.dat         - a support file that contains a list of DOE-2 keywords
-
-  Samp4n.inp         -  sample DOE-2.1E input file
-
-  Samp4n.imf         - the EnergyPlus macro input file resulting from the sample
-
-To use the DOE2Translator simply type
-
-  DOE2Translator  &lt;file&gt;
-
-Where you substitute the file you want to translate for &lt;file&gt; without a file extension. The ".inp" file extension is assumed. For example, if you want to translate one of the sample DOE-2.1E input files you would type:
-
-  DOE2Translator  samp1b
-
-The &lt;file&gt; can also have a full path, but it should not have an extension. If you have spaces in your path name, enclose the whole thing in ".
-
-Several files get created when you run the DOE2Translator program. In the same directory as the DOE-2.1E input file, a new file with the same name and the file extension of ".imf" contains the EnergyPlus translation.
-
-This is an EnergyPlus macro file and the macro processor EPMacro needs to be used. The DOE2Tranlator uses many macros so using EPMacro is essensial. EP-Launch automatically runs EP-Macro when an ".imf" file is selected. In the translated file, comments shown with a tilde "~" are messages from the DOE2Translator program that may be helpful in understanding the limits of the translation.
-
-The D2EP.log file contains a detailed log of the translation process. The D2E\_TEMP.txt file contains an intermediate version of the log file. Both of these files are created in the same directory as the DOE2Translator program and can usually be deleted.
-
-Since DOE-2.1e and EnergyPlus share a common macro language, many macro features are passed to the EnergyPlus file unchanged, including \#\#set1, \#\#if, \#\#def and other macro commands. References to macro variables (i.e., "var[]") and expressions (i.e., " \#[x[] + 1]") are usually passed through to the resulting EneryPlus IMF unless the DOE2Translator needs to understand that field during the translation process. The DOE2Translator does not evaluate macro expressions and if it needs to understand a field value and a macro is present instead will use a default value for the field instead. Most fields do not need to be understood by the translator and are directly passed through to the IMF file unchanged.
-
-Files that are included with the \#\#include are not translated automatically and would each need to be run through the DOE2Translator. If the included file does not have the INP extension it would need to be changed prior to the translation. In addition, the user would need to edit the \#\#include commands to use the IMF extension instead of the INP extension.
-
-In this version of the DOE2Translator program, translation is limited to the following DOE-2 commands, which represent the majority of the building envelope and internal gains:
-
-```
-    SPACE (except SHAPE=BOX)
-    SPACE-CONDITIONS
-    DAY-SCHEDULE (except use of HOURS and VALUES keywords)
-    WEEK-SCHEDULE (except use of DAYS and DAY-SCHEDULE keywords)
-    SCHEDULE (except use of WEEK-SCHEDULE keyword)
-    MATERIAL
-    LAYERS
-    CONSTRUCTION
-    EXTERIOR-WALL, ROOF (except polygon)
-    INTERIOR-WALL
-    FIXED-SHADE
-    WINDOW
-    DOOR
-    RUN-PERIOD
-    DESIGN-DAY
-    LIKE
-    SET-DEFAULT
-```
-
-Running Console Applications
-============================
-
-Several of the auxiliary programs included with EnergyPlus are Console Applications. This designation means that they are executed from the "command window" (Windows OS) or terminal window (Linux OS). We will include generic instructions for the Windows OS use of these applications in this section. Each program will also include specifics for the Windows OS in the individual program documentation.
-
-As installed, the batch files that accompany console applications will be set so that file extensions are not included for input parameters, paths to installed data (such as weather data) will be set automatically, and these paths can be modified by the user as desired. (Instructions included a bit later in this section).
-
-Generally, the steps for executing a console application is:
-
-1)   Open a DOS command prompt window (Start à Programs à Accessories à Command Prompt)
-
-2)   Change to the directory where EnergyPlus is installed (modify the commands below if you did not install EnergyPlus in the default install path):
-
-C:
-
-CD \\&lt;root folder&gt;\&lt;/span>
-
-3)   Change to the specific folder for the console application:
-
-CD &lt;folder&gt;
-
-4)   Run the program:
-
-&lt;batchfile&gt; &lt;input parameters&gt;
-
-Modifying the batch file
-------------------------
-
-Generally, the batch files set several environment variables that govern the execution of the specific program.
-
-Table 32. Environment Variables used in Batch Files
-<table class="table table-striped">
-  <tr>
-    <th>Environment Variable Name</th>
-    <th>Description</th>
-  </tr>
-  <tr>
-    <td>Program Path</td>
-    <td>Specific or relative program path</td>
-  </tr>
-  <tr>
-    <td>Program Name</td>
-    <td>Name of program</td>
-  </tr>
-  <tr>
-    <td>Input_Path</td>
-    <td>Input Path Specification</td>
-  </tr>
-  <tr>
-    <td>Output_Path</td>
-    <td>Output Path Specification</td>
-  </tr>
-  <tr>
-    <td>Weather_Path</td>
-    <td>Weather Data Path Specification</td>
-  </tr>
-</table>
-
-Or, as seen in the batch file text:
-
-```
-:Instructions:
-:  Complete the following path and program names.
-:  path names must have a following \ or errors will happen
- set program_path=
- set program_name=<specific program name will be here>
- set input_path=
- set output_path=
- set weather_path=..\..\WeatherData\
-```
-
-As the instructions in the batch file show, the path character must terminate the path specification or errors can occur. The "weather\_path" specification shows an example of using a "relative" path specification. Depending on the program, this specification, of course, might change.
-
-```
-set weather_path=..\..\WeatherData\
-```
-
-What the specification says is that above (..) and above again (..) and then "WeatherData" is where the weather data files are located. This kind of relative path would be true for most "Preprocess" programs in the installed folders. The following illustrates the folder tree:
-
-```
-<Root Folder> (this is usually EnergyPlusV<version>)
-      Preprocess
-                  Specific Program Folders
-      WeatherData
-```
-
-Thus, the user can simply put the name of the weather data file onto the batch file run and it will look for that file in the installed WeatherData folder.
-
-Technical Details of Running EnergyPlus
-=======================================
-
-This section will contain the details of running EnergyPlus - more (and some duplicated) information on EP-Launch (basic discussion included in the Getting Started manual) and "by hand" - describing the batch files that are included with the install. The first parts of this section deal with using EnergyPlus on a Wintel/Windows OS system. Though similar commands can be used on other OS - such as Linux, they will not be exactly the same commands (usually).
-
-EP-Launch Program
------------------
-
-EP-Launch is an optional component of the EnergyPlus Windows installation (it is not available for Linux and Mac platforms). For users that want a simple way of selecting files and running EnergyPlus, EP-Launch provides this and more. In addition, EP-Launch can help open a text editor for the input and output files, open a spreadsheet for the postprocessor results files, a web browser for the tabular results file, and start up a viewer for the selected drawing file.
-
-![](media/image101.png)
-
-Figure 35. EP-Launch Screen
-
-
-
-### Start EP-Launch
-
-EP-Launch is located in the main directory/folder for EnergyPlus. In addition, it is available on the shortcut menu for EnergyPlus.  By double clicking on the EP-Launch icon you get the screen shown above (Figure 35) for running a single input file. The EP-Launch program simply starts other programs and allows you to avoid having to use the DOS command line prompt to run EnergyPlus. More help is provided for the program under the "Help" menu.
-
-### Selecting Input and Weather Files
-
-The input file and weather files can be selected on the Single  Input File tab from the two pull down lists which show recently used files or you can press the "Browse…" buttons to locate an input or weather file that you have created yourself. If this is your first time using EP-Launch, the pull down lists will show some files from the ExampleFiles subdirectory. These are not the only examples, use browse to open other example files from the ExampleFiles subdirectory or other EnergyPlus input files.
-
-### Running a Single Input File
-
-On the Single Input File tab, after you select the weather and input files simply push the "Simulate…" button to start the EnergyPlus building energy simulation engine. At this point a black DOS window should pop up on your screen and show the progress of your simulation. The simulation is complete when the black DOS box closes. The EnergyPlus program black DOS window will show scrolling text as the simulation procedure progresses. If you would like to see these messages more slowly you have two options:
-
-1)   Press the "Control-S" key combination to try to stop the progress and any key to continue.
-
-2)   Under the "View" menu on the EP-Launch program, select "Options" then "Command Window" then check "Pause During Simulation" and this will pause the process immediately after EnergyPlus executes. To continue after the pause, press any key.
-
-If the file contains Parametric objects, the single input file may cause multiple simulations to be performed. If multiple simulations are performed, the output files will be listed on the History tab and will be named with either the file suffixes defined in the input file or with a serial number.
-
-Multiple single input file and group simulations can be started at the same time. On a computer with multiple-processors or multiple-cores, this will enable the simulations to complete more quickly than starting one after another.
-
-### Looking at the Results
-
-After you have run a simulation and the black DOS window closes, EnergyPlus has completed, and a status message is displayed (see figure below):
-
-![](media/image102.png)
-
-Figure 36. EP-Launch Finish Status.
-
-This status gives you a quick overview of whether there were warning (**should look at**), severe (**should probably fix**) or fatal (**must fix**) errors in the run as well as the time it took for the simulation to complete.  After pressing "OK" from this box, selecting "ERR/EIO/BND Output Files Only" from the "View" menu will display the ERR, EIO, and BND files - useful when errors may have occurred. Alternatively, pressing the F2 function key will display the same three files.
-
-Another way to open files easily is by using the View Results buttons as shown in 29. Two different panels of buttons can be used under View Results, one shown by using the "All" tab on the left edge and by using the "Sets" tab on the left edge. The "All" tab shows all the various files by file extension that can be viewed individually. Files available for view  based on the current input file name, are "enabled" (extension names clearly readable).
-
-![](media/image103.png)
-
-Figure 37. EP-Launch with the Sets tab of View Results
-
-The figure above shows the same main screen of EP-Launch but with the "Sets" tab selected on the left edge of the View Results section. The buttons on this tab can open many files at the same time and are a shortcut to opening the files that may be commonly used. The Text Output Files, Drawing Files, and Spreadsheets buttons cause several different results files to open at once based on the currently selected Input File. The HTML file opens just the tabular results file if that file was produced (see *OutputControl:Table:Style*). The buttons labeled as Set 1 to Set 8 allow you to select which sets of files you want to open. Press the "Define" button in order to define the files to view.
-
-![](media/image104.png)
-
-Figure 38. Define Files to View
-
-When the "Define" button is pressed on the Sets tab of the View Results section of the main screen, the dialog box in the figure above is shown. This allows the files extensions to be selected that would be opened for each of the Set 1 to Set 8 buttons. One or many files can be selected for each of the Set buttons. This allows you to define exactly which files you want opened.
-
-The content of each file extension is listed below.  The contents (along with examples) are discussed in the [Output Details](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf) document.
-
-By pressing the "Text Output Files" button, a text editor will open each of the text output files. Up to 29 files will open, if they exist. Selecting "Single File" from the 'View'  menu displays a menu of all available output files from which any file can be opened individually. Each file may also be opened with an associated function key. The output files and function key shortcuts are listed below:
-
-1.    Variable - tabulated results in comma, tab or space delimited format (generated by the ReadVarsESO postprocessor) (F4)
-
-2.    ESO - raw report variable output (F5),
-
-3.    RDD - list of output variables available from the run (F6).
-
-4.    MDD - list of output meters available from the run (Shift-Ctrl-F3)
-
-5.    EIO - additional EnergyPlus results (F7),
-
-6.    ERR - list of errors and warnings (F8),
-
-7.    BND - HVAC system node and component connection details (F9),
-
-8.    MTR - raw report meter output (F11),
-
-9.    MTD - list of meter component variables (F12)
-
-10. METER File - tabulated meter report in comma, tab or space delimited format (generated by the ReadVarsESO postprocessor) (Ctrl-F4)
-
-11. ZSZ - zone sizing details in comma, tab or space delimited format (Ctrl+F5)
-
-12. SSZ - system sizing details in comma, tab or space delimited format (Ctrl+F6)
-
-13. AUDIT - input file echo with input processor errors and warnings (Ctrl+F8)
-
-14. SLN - output from "report, surfaces, lines" (Ctrl+F9)
-
-15. DBG - output from the debug command (Ctrl+F11)
-
-16. SHD - output related to shading (Ctrl+F12)
-
-17. SVG - HVAC Diagram (Shift+ F4)
-
-18. EPMIDF - clean idf file after EP-Macro processing (Shift+F5)
-
-19. EPMDET - EP-Macro detailed output with errors and warnings (Shift+F6)
-
-20. MAP - daylighting illuminance map (Shift+F7)
-
-21. TABLE - tabulated report of bin and monthly data in comma, tab or space delimited or HTML format  (Shift+F8)
-
-22. VMRL - drawing file in VRML (Virtual Reality Markup Language) format (Shift F+F11)
-
-23. DXF - drawing file in AutoCAD DXF format (Shift+F12)
-
-24. Delight IN - DElight input generated from EnergyPlus processed input (Shift+Ctrl+F4)
-
-25. Delight OUT - Detailed DElight output (Shift+Ctrl+F5)
-
-26. Delight ELDMP - DElight reference point illuminance per time step (Shift+Ctrl+F6)
-
-27. Delight DFDMP - DElight warning and error messages (Shift+Ctrl+F7)
-
-28. EXPIDF - Expanded IDF when using HVACTemplate objects (Shift+Ctrl+F8)
-
-29. Group Error - combined error files for a group run. (Shift+Ctrl+F9)
-
-30. VCpErr - Transition program error file (Shift+Ctrl+F11)
-
-31. Screen (Shift+Ctrl+f12)
-
-32. Proc CSV - Simple statistiscs generated from CSVProc (also see Create Statistics File option under View-Options).
-
-33. EDD - Energy Management System details.
-
-Clicking on the "Drawing File" button will open the generated DXF file if an appropriate viewer has been configured (see *Selecting Viewers and Editors* below). The DXF file is a CAD format that displays the physical shape of the building being modeled in three dimensions. The "Drawing File" button also opens the HVAC diagram generated with the HVAC-Diagram utility (see Auxiliary Programs).
-
-Clicking on the "Spreadsheets" buttons will open any generated CSV files if an appropriate viewer has been configured (see *Selecting Viewers and Editors* below).
-
-### Viewing the Drawing File without Running a Simulation
-
-The "Drawing" button (or the View menu Drawing File option) will automatically run EPDrawGUI if the DXF file does not exist or it is older than the input file. This allows the building geometry to be viewed without running a full simulation. For more information about EPDrawGUI, see the EPDrawGUI section in this document.
-
-### Editing the Input Files
-
-The input file, called IDF file that is selected from the top pull-down list, can be edited by pressing one of two buttons in the "Input File" area. The "Edit - Text Editor" button will start a text editor and the "Edit - IDF Editor" will start the separate program called the IDF Editor. Remember to save any changes you make in either editor before returning to EP-Launch to run the simulations again.
-
-### File Menu
-
-The File menu can be used for selecting input and weather files just like the "Browse…" buttons (see the *Selecting Input and Weather Files* section above)
-
-If you are upgrading from the previous version of EnergyPlus you can use the "File", "Transition" menu option to upgrade your EnergyPlus input files (IDF and IMF) to the most recent version (see the section Using Older Version Input Files - Transition for more information about the Transition program). This EP-Launch option only works for upgrading input files one version.
-
-### Edit Menu
-
-No cutting or pasting is used in this program so the edit menu shows options that duplicate the functions of the "Edit - Text Editor" and "Edit - IDF Editor" buttons. In addition, the weather file and the postprocessor command file (rvi) may be opened in the text editor.
-
-### View Menu
-
-The View menu (see Figure 39) duplicates the options in the "View Results" area of the main screen (see the *Looking at the Results* section above) and allows opening of selected output files. You can also open the folders that contain the active input and weather files. Opening a single file is under a submenu and is very similar to the Quick Open Panel for Single Simulation described above. Selecting "HTML File" from the "View" menu will open any user created files saved in the format: &lt;filename&gt;table.html (see *OutputControl:Table:Style*).
-
-![](media/image105.png)
-
-Figure 39. EP-Launch View Menu
-
-![](media/image106.png)
-
-Figure 40. EP-Launch Options Screen.
-
-The "View" menu also accesses the "Options" menu item shown in Figure 40 that is used to control many of the optional features of EP-Launch. These optional features are described below:
-
-#### Command Window Options
-
-**Pause During Simulation (Unless Minimized)** - Stops the progress of the EnergyPlus run at different points. This does not stop the simulation itself but pauses before or after important events as files are copied or utility programs are run. It is usually used only for diagnosing problems with the EPL-RUN batch file. The feature is also described in the *Running a Single Input File* section above.
-
-**Minimize Single Simulation Command Window** - For a single input file, minimizes the Command Window that EP-Launch uses to run EnergyPlus. The command window will appear only in the Windows taskbar and the command window will not be visible. You can restore the command window be clicking on the taskbar item labeled "EnergyPlus Process". This option should be used with caution since you will not see any indication of the simulation being complete other than the "EnergyPlus Process" taskbar item will disappear.
-
-**Minimum Group Simulation Command Window** - For a group of input files, minimizes the Command Window that EP-Launch uses to run EnergyPlus. This is a good option when working on something else on your computer at the same time as the group of simulations is running since the command window normally becomes the front window each time a new simulation starts. This option prevents the command window coming to the front for each simulation. The command window will appear only in the Windows taskbar and the command window will not be visible. You can restore the command window be clicking on the taskbar item labeled "EnergyPlus Process". This option should be used with caution since you will not see any indication of the simulation being complete other than the "EnergyPlus Process" taskbar item will not be present.
-
-**Number of Simultaneous Processes** - Select the maximum number of simulations that should be able to be run at the same time. For a computer with multiple processors or multiple cores, this will allow better utilization of the computers power. The value selected should correspond to the number of processors/cores but higher or lower number can be used as well.
-
-**Disable Multi-Threading** - Check this box if you wish to disable the built in multi-threading capabilities of EnergyPlus. Portions of EnergyPlus have been programmed to use more than one processor, or CPU core, at the same time during a single simulation. This multithreading may not be desirable when running more than one simulation at a time on the same computer (because it can actually run more slowly). When this check box is checked multi-threading is turned off. The check box sets the **EP\_OMP\_NUM\_THREADS** environmental variable to 1. The multi-threading capability of EnergyPlus can also be controlled using the **ProgramControl** object field called Number of Threads Allowed. That field takes precedence over the setting of the checkbox. Also note that when multiple simulations are started from EP-Launch, this automatically disables multithreading by setting the EP\_OMP\_NUM\_THREADS environmental variable to 1 whether this box is checked or not. The ProgramControl object is described in the Input Output Reference document.
-
-#### Interface Options
-
-**Extra Wide Window** - Select this option to make the main EP-Launch window wider. This is useful when files are used with very long file path names.
-
-**Alternative layout** - Changes the layout of the EP-Launch window to an alternative arrangement of buttons.
-
-#### Miscellaneous Options
-
-**Tab Delimited Open with Spreadsheet** - Selecting "Single File" and then "Main Results File" from the "View" menu or pressing the F4 function key will open TAB files with the default spreadsheet application rather than the text editor. Comma-separated variable (CSV) is the default setting for viewing tabulated results set in the RVI file. If the user changes the setting for viewing tabulated results to TAB or TXT format, selecting "Single File" and then "Main Results File" from the "View" menu or pressing the F4 function key will open the files in the default text editor.  TAB files, when selected, will also be opened by the text editor when the "Text Output Files" button is pressed after a successful run.
-
-**Allow More Than 250 Columns** - Tabulated data that exceeds 250 columns, the MS Excel maximum, will be truncated to that limit unless "Allow &gt;250 Columns" is selected. Excel versions prior to 2007 were limited to 255 columns in a sheet; later versions allow unlimited number of columns. This limitation may not be true for other spreadsheet programs.
-
-**Check VERSION Prior to Simulation** - Automatically check the VERSION object in the selected EnergyPlus input file prior to simulation and if it is an older version than the current version will run the Transition program to update the file.
-
-**Convert ESO/MTR to IP Units** - Runs the convertESOMTR utility program (see AuxiliaryPrograms documentation for more information). This utility will convert the ESO and MTR files into Inch-Pound units. The CSV file created from these files will also be in Inch-Pound units.
-
-**Create Statistics File** - Runs the CSVProc utility program (see the AuxiliaryPrograms documentation for more information) and creates the -Proc.csv file. This file contains some simple statistics on each variable in the normal CSV file.
-
-**Create Batch File to Run EnergyPlus** - Traditionally EP-Launch has created a batch file in order to execute EnergyPlus with the various options chosen. This can cause problems with some operating systems, such as Windows Vista, when set to a higher security setting.  This option can be unchecked and a batch file is not created when running EnergyPlus instead parameters are passed to an existing batch file.
-
-**Run ParametricPreprocessor** - When this option is checked, if Parametric objects are present in the file, the ParametricPreprocessor will be run prior to the first simulation and if multiple simulations are needed they will all be executed. See the Auxiliary Programs documentation for details.
-
-**Check for Updates to EnergyPlus** - When this option is checked, EP-Launch will check every seven days if an update to EnergyPlus or any of the files distributed with EnergyPlus are available to download. If they are available a message will be shown upon start up.  You can also manually check by going to HELP .. CHECK FOR UPDATES.
-
-#### Text Editor Options
-
-EP-Launch will start a text editor when editing a IDF file or when viewing many of the results files.  The text editor that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the text editor of your choice. The Auto Find button will automatically find the program that is associated with the TXT file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a text editor is available immediately. The most common text editor is NOTEPAD.EXE and is built into Windows but many other text editors are also available.
-
-#### Drawing Viewer Options
-
-The default drawing viewer is the application associated with DXF files. This can be changed to your favorite drawing program by using the Select button then locating the executable file for your favorite drawing software capable of reading a DXF file. The Auto Find button will automatically find the program that is associated with the DXF file extension and use that program. A variety of programs (free of charge) can render DXF files for viewing.  The [Output Details](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf) document lists some of these programs as well as displaying what a DXF rendered file looks like on the screen.
-
-#### VRML Viewer Options
-
-EP-Launch will start a VRML Viewer when a building drawing is created using the Report, Surfaces, VRML option in your IDF file.  The VRML Viewer that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the VRML Viewer of your choice. The Auto Find button will automatically find the program that is associated with the WRL file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a VRML Viewer is available immediately. Many other VRML Viewers are available.
-
-#### Spreadsheet Options
-
-EP-Launch will start a spreadsheet program when viewing many of the results files.  The spreadsheet that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the spreadsheet program of your choice. The Auto Find button will automatically find the program that is associated with the CSV file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a spreadsheet program is available immediately.
-
-#### Diagramming Options
-
-EP-Launch will start a diagramming program to view SVG files from HVAC Diagram.  The diagramming program that will be used is shown but can be changed by either pressing the Select button, the Auto Find button, the Use Firefox button or the Use Opera button. The Select button allows you to find the diagramming program of your choice but make sure it is capable of opening SVG files. The Auto Find button will automatically find the program that is associated with the SVG file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a spreadsheet program is available immediately.  Since both Firefox and Opera web browsers can view SVG files, those buttons will select those respective browsers if available.
-
-#### HTML Browser Options
-
-EP-Launch will start a HTML browser program when viewing the tabular results file when HTML is chosen in OutputControl:Table:Style.  The HTML browser that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the HTML browser of your choice. The Auto Find button will automatically find the program that is associated with the HTML file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a HTML browser is available immediately.
-
-#### ESO Viewer Options
-
-By default, ESO files are opened with a text editor. ESO files are the raw output file containing results from EnergyPlus for Report Variable objects. They are often processed into CSV files to make it easier to view them. At least one utility program has been developed to view ESO files directly (see the EnergyPlus.gov web site under "Interfaces & Other Tools", "Third-party EnergyPlus Tools).  The Auto Find and Select buttons work the same way as other viewer selectors. If no special ESO viewer is selected the box will be shown as empty. It can also be emptied by using the Clear button.
-
-#### PDF Viewer Options
-
-EP-Launch will start a PDF viewer program when opening the EnergyPlus documentation under the Help menu.  The PDF Viewer that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the PDF Viewer of your choice. The Auto Find button will automatically find the program that is associated with the PDF file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a PDF Viewer is available immediately.
-
-#### File Association Options
-
-When installing EnergyPlus, you are given an option if you want IDF, IMF, and EPG files associated with EP-Launch. This allows double clicking on files with those extensions and having EP-Launch start automatically with those files. If during the install that option is not selected or if you have changed the program that opens IDF, IMF and EPG files and want to change it back to EP-Launch, the button for this option will do that.
-
-#### Reset Options
-
-Two reset options are available here.
-
-The **Auto Find All File Viewers** button will autofind all the file viewers in one step. This is equivalent to pressing the Auto Find button for each viewer program.
-
-The **Reset All Options and Exit** button will clear all options and restore the default values used when first invoking EP-Launch for the first time. This also clears the list of recently used IDF and weather files.  This option will exit EP-Launch and you will have to start EP-Launch again.
-
-### Help Menu
-
-The Help menu can be used to open the EnergyPlus documentation files and the EP-Launch help file. In addition, you can check for updates to the EnergyPlus program and other files in the EnergyPlus distribution.
-
-### Recently Used Files
-
-The recently used input, weather and group file pull down lists can hold a maximum of twenty items. These lists, like the viewers selected, are saved between times you use the EP-Launch program.
-
-### Running Groups of Input Files
-
-If you are running EnergyPlus on one file or even just a few different files, the easiest way to do this is on the Single Simulation tab. If you are performing an analysis of a building which requires running EnergyPlus for a larger number of times, you may want to consider the Group of Input Files tab, shown below. You may also want to set the Number of Simultaneous Processes option under View Options Command Window so that the simulations are completed as fast as your computer will allow.
-
-
-
-![](media/image107.png)
-
-Figure 41. EP-Launch Group of Input Files Tab.
-
-This tab lets you manage EPG, EnergyPlus Group files which contain a list of simulations that need to be performed. The EPG file is simply a text file that contains on each line the input file and weather file names to be used for a simulation along with how the output files should be named and a counter.
-
-You do not need to manually create EPG files, instead press the New Group button on the Group of Input Files Tab and a step-by-step "wizard" will help to create a new EPG, EnergyPlus Group file. The first step of the wizard is to selected the EnergyPlus input files that should be simulated as part of the group:
-
-![](media/image108.png)
-
-Figure 42. EP-Launch Step 1 of New Group Wizard.
-
-Use the boxes next to each file to select the files to be simulated. The path to files shown may be changed using the "path" button. Once the files in a certain directory are selected the "next" button should be pressed. If additional files are desired in different directories, you will get a chance to add them to the EnergyPlus group file in a later step.
-
-Select one or several weather files using the second step of the wizard, shown below:
-
-![](media/image109.png)
-
-Figure 43. EP-Launch Step 2 of New Group Wizard.
-
-The next step is to review the simulations selected. Each combination of weather file and input file is initially shown. Each simulation is displayed as a single row. You may select a row and delete the simulation at this point. In addition, if additional simulations are desired, the "Add more simulations button" brings you back to the first step of the wizard to add more file.
-
-![](media/image110.png)
-
-Figure 44. EP-Launch Step 3 of New Group Wizard.
-
-The next step of the wizard allows you to decide exactly where you want the output files located and what they should be named. For most people just trying to group their simulations and wanting the output files in the same directory as the input files, just select "Original Input File Locations".
-
-![](media/image111.png)
-
-Figure 45. EP-Launch Step 4 of New Group Wizard.
-
-More advanced users may choose to define their locations for the output files using symbols that define the name of the directory and file name using:
-
-%I = input file name
-
-%G = group file name
-
-%W =  weather file name
-
-%N = repeat number for IMF files
-
-%J = input file path
-
-%H = group file path
-
-%X = weather file path
-
-Each of these symbols may be used in the location field and substitutions will be made for each when defining the output file location.
-
-For macro files (they have an extension IMF instead of IDF) used in a parametric analysis, the macro file may be run repeatedly up to 999 times. Each time they are simulated a new COUNTER.INC file is created which sets a macro parameter. The COUNTER.INC file should be included using the \#\#include statement in the macro file.
-
-Finally, you can save the EPG, EnergyPlus Group, file wherever you would like.
-
-To run the simulations press the "Simulate Group" button on the Group of Input Files tab. To prevent a specific simulation from being performed, edit the file and use a comment character (an exclamation point) to comment out the line.
-
-When the group of input file simulations is running, the title bar of EP-Launch will show the progress.
-
-### History of Simulations Performed
-
-The History tab allows you to see what files were associated with a particular simulation that was performed. The list shows the date and time of the simulation along with the input and weather file names.
-
-![](media/image112.png)
-
-Figure 46. EP-Launch History Tab.
-
-
-
-You can expand the level of detail by clicking on the plus signs or double clicking on the entry. The detail shown includes the names of all the input and output files associated with that simulation along with the message summary of the warnings and errors generated. It is possible that a file may be shown that no longer exists.
-
-The View Files button will display the selected file using a spreadsheet, text editor, DXF file viewer, SVG file viewer, or HTML web browser. When groups of simulations are performed using the Group of Input File tab and User Defined Locations are used for the output files, the history view is the only way to access those files using EP-Launch.
-
-The history tab displays the HISTORY.CSV file that is located in the same directory as EP-Launch. If EP-Launch seems to be starting slowly, it is possible that the history file has grown very large. It may be deleted or renamed and a new history file will be automatically created during the next simulation. The HISTORY.CSV file may also be opened in a spreadsheet program.
-
-### Utilities Tab
-
-The utilities tab shown in the following figure allows several utility programs that come with EnergyPlus to be used directly. More information on each utility is also available in the AuxiliaryPrograms documentation.
-
-![](media/image113.png)
-
-Figure 47. EP-Launch Utilities Tab.
-
-For each utility, input files can be selected by using the Browse Button. The input file can be opened using a text editor and, for certain utilities, the IDF Editor. If a weather file is needed for a utility it can also be selected. For other utilities, no weather file is needed and that portion of the screen is not shown. The appropriate output files can be opened by the "Open" button near the bottom of the screen. To run the utility, use the "Run" button in the lower left corner of the screen above the "Exit" button.
-
-In addition, for each utility, a brief description of the function of the utility is shown in the about box but much more information is available in the AuxiliaryPrograms documentation.
-
-### Caveats
-
-Remember to save changes made in the editor before you run another simulation.
-
-The simulation cannot write new results to open files which are locked by another application.
-
-You will need to close the spreadsheet program that views the resulting CSV files prior to another simulation and you may need to close the text editor windows also (depending on your editor).
-
-The EPL-RUN.BAT batch file is used to run EnergyPlus from the EP-Launch program. It can be edited with care if other postprocessors or preprocessors are to be used.
-
-### When things go wrong
-
-Though EnergyPlus has had several releases (including beta releases prior to initial release), there still may be problems when input files meet with EnergyPlus. If you are using EP-Launch when this happens, you will see a window appear as in the figure below (Figure 48). Follow the instructions listed on the screen.
-
-![](media/image114.png)
-
-Figure 48. EnergyPlus crash within EP-Launch.
-
-### Bugs
-
-The EP-Launch program has been through several "releases" but there is still a chance you will find bugs. Please report them to the energyplus-support@gard.com address so that we can fix them prior to the release.
-
-If the pull-down lists ever are shown as blank the "reset" button may be used. This unlabeled button is very small in the lower left-hand corner of the main screen. It removes the items shown in the recently used file list and causes the program to forget the selected viewers and text editors; and exits the program. When you start EP-Launch again, you will need to make these selections (viewers and text editors) again.
-
-EP-Launch Lite
---------------
-
-EP-Launch Lite is a small application included with the EnergyPlus Macintosh installation. It is a small GUI application that provides a simple way to run EnergyPlus models. Its purpose is similar to EP-Launch but it is a much simpler application with fewer features.
-
-EnergyPlus File Extensions
---------------------------
-
-This section will present a list (perhaps not complete) of EnergyPlus file extensions and what they mean. This will help you after the EP-Launch program finishes.
-
-### Input Files
-
-The following files are input to the EnergyPlus program.
-
-#### IDD
-
-The *input data dictionary* (IDD) is an ascii (text) file containing a list of all possible EnergyPlus objects and a specification of the data each object requires. This file is analogous to the DOE-2 keyword file. The *Guide for Interface Developers* contains a full description of the input data dictionary.
-
-#### idf
-
-The *input data file* (IDF) is an ascii file containing the data describing the building and HVAC system to be simulated. Many example files are installed as part of the EnergyPlus installation. Additionally, a spreadsheet file "ExampleFiles.xls"  contains columnar descriptions of each file's features.
-
-#### imf
-
-The *input macro file* (IMF) is an ascii file containing the data describing the building and HVAC system to be simulated and will have some contents of "macro" commands. The Auxiliary programs document describes use of the macro commands and the program that processes them - EP-Macro.   Many example files are installed as part of the EnergyPlus installation.
-
-#### ini
-
-This is the EnergyPlus initialization file. It is an optional ascii input file that allows the user to specify the path for the directory containing Energy+.idd. This file, using the actual directories of the install, will be created during the install. Unless you change where the EnergyPlus.exe file resides, you will not need to change this file.
-
-#### epw
-
-The *EnergyPlus weather* file is an ascii file containing the hourly or sub-hourly weather data needed by the simulation program. The data format is described in detail in the Auxiliary Programs Document. It is also described succinctly in the Input Output Reference document.
-
-### Output Files
-
-More information (and more up-to-date) about output files is shown in the [Output Details and Examples](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf) Document.
-
-#### err
-
-A text file containing the error messages issued by EnergyPlus. **This is the first output that should be examined after a simulation.**Error messages may be issued by EnergyPlus during its input phase or during the simulation. There are three levels of error severity: *fatal*, *severe*, and *warning* as well as simple *"message"* lines. A fatal error causes the program to terminate immediately. The following table illustrates the necessary actions.
-
-Table 33. Error Message Levels - Required Actions
-
-<table class="table table-striped">
-<tr>
-<th>Error Level</th>
-<th>Action</th>
-</tr>
-<tr>
-<td>Information</td>
-<td>Informative, usually a follow-on to one of the others. No action required.</td>
-</tr>
-<tr>
-<td>Warning</td>
-<td>Take note. Fix as applicable.</td>
-</tr>
-<tr>
-<td>Severe</td>
-<td>Should Fix</td>
-</tr>
-<tr>
-<td>Fatal</td>
-<td>Program will abort</td>
-</tr>
-</table>
-
-
-An example of an error message due to an input syntax error is:
-
-```
-** Severe  ** Did not find " DessignDay" in list of Objects
-   **  Fatal  ** Errors occurred on processing IDF file -
-       probable incorrect IDD file. View "audit.out" for details.
-   ************* EnergyPlus Terminated--Error(s) Detected.
-```
-
-#### audit
-
-This is an text file which echoes the IDD and IDF files, flagging syntax errors in either file. Note that both *err* and *audit* will show most of the error messages caused by input syntax errors; however only *err* will show errors issued during the actual simulation. The *audit* can be used when you need to see the context of the error message to fully ascertain the cause. The *audit* file also contains potentially extra information that may be useful from the input scan.
-
-#### eso
-
-The *EnergyPlus Standard Output* (ESO) is a text file containing the time varying simulation output. The format of the file is discussed in the *Guide for Interface Developers* and the *InputOutputReference*. The contents of the file are controlled by *Output:Variable* commands in the IDF file. Although the ESO is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
-
-#### mtr
-
-The *EnergyPlus Meter Output* (MTR) is a text file containing the time varying simulation output. The format of the file is similar to the ESO file. As described in the Getting Started document, meters are a powerful reporting tool in EnergyPlus. Values are grouped onto logical meters and can be viewed the same way that the ESO variables are used. The contents of the file are controlled by *Output:Meter* commands in the IDF file. Although the MTR is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
-
-#### mtd
-
-This file contains all the details (i.e., which report variables are on a meter and, conversely, what meters contain) about meters.
-
-#### eio
-
-The *EnergyPlus Invariant Output* (EIO) is a text file containing output that does not vary with time. For instance, location information (latitude, longitude, time zone, altitude) appears on this file.
-
-#### rdd
-
-#### mdd
-
-The *Report (variable) Data Dictionary* (RDD) is a text file listing those variables available for reporting (on the ESO) for this particular simulation. Which variables are available for output depends on the actual simulation problem described in the IDF. The *Report (meter) Data Dictionary* (MDD) is a text file listing those variables available for reporting (on the MTR) for this particular simulation. Which meters are available for output depends on the actual simulation problem described in the IDF. A simulation with no chiller would not permit the output of any chiller report variables. The user may need to examine the RDD or MDD to find out which report variables are available in a particular simulation. The RDD and MDD are written only if the following is included in the IDF file.
-
-```
-Output:VariableDictionary, Regular;
-```
-
-A variant produces the same files in a IDF "ready" format.
-
-```
-Output:VariableDictionary, IDF;
-```
-
-#### dbg
-
-This is a text file containing *debug* output for use by EnergyPlus developers. Generally developers will add debug print statements wherever in the code that that they wish. There is a "standard" debug output that prints out conditions at all the HVAC nodes. This output is triggered by placing
-
-```
-Output:DebuggingData,1;
-```
-
-in the IDF file. If Output:DebuggingData, 0 is entered, you will get an empty eplusout.dbg file.
-
-#### dxf
-
-This is a file in AutoCad DXF format showing all the surfaces defined in the IDF file. It provides a means of viewing the building geometry. The DXF file from EnergyPlus highlights different building elements (shading, walls, subsurfaces) in differing colors. A number of programs can read and display DXF files. Output of this file is triggered by
-
-```
-Output:Reports, Surfaces, DXF;
-```
-
-in the IDF.
-
-#### sln
-
-A text file containing the coordinates of the vertices of the surfaces in the IDF.
-
-Output of this file is triggered by
-
-Output:Reports, Surfaces, Lines;
-
-in the IDF.
-
-### Postprocessing Program/Files
-
-A postprocessing program *ReadVarsESO.exe* is available that will read an ESO or MTR file and produce a file that can be read by Excelâ„¢. It can use an input file or not. In batch mode it is run by the little batch file *RunReadESO.bat*:  Further information on this program is provided in the [Input Output Reference](file:///E:\Docs4PDFs\InputOutputReference.pdf) under a section heading called "Using ReadVarsESO".
-
-RunEPlus batch file
--------------------
-
-It is simple to run EnergyPlus: open a DOS or CMD box in the EnergyPlus directory and use the RunEPlus.bat procedure file. The procedure file takes two arguments - the input file name (containing the building description) and the weather file name:
-
-RunEPlus &lt;input\_file\_name&gt; &lt;weather\_file\_name&gt;
-
-Though it's possible to supply arguments to the batch file with embedded blanks, it's better practice not to. More extensive information about the intricacies of EnergyPlus execution is given in the next parts of this section.
-
-As installed, the RunEPlus is ready to run the sample files that are included. If you wish to create and run other files, you may wish to modify the batch file to your own preferences. See "RunEPlus details" later in this document for parts of the batch file that you will need to modify.
-
-Running EnergyPlus by Hand
---------------------------
-
-EnergyPlus runs as a console application with optional command line arguments. The arguments may be listed by typing `energyplus --help` (on any operating system) and `man energyplus` (on Unix-based operating systems, Mac OS X and Linux). For more information about the command line interface, see https://github.com/NREL/EnergyPlus/blob/develop/doc/running-energyplus-from-command-line.md. The remainder of this section describes running EnergyPlus in legacy mode (i.e. no command-line arguments) on Windows OS.
-
-To run the program bring up the command prompt and "cd" to the directory containing the executable. Assume that the executable is called *EnergyPlus.exe*. In the same directory EnergyPlus expects *in.idf*, the input data file; *Energy+.idd*, the data dictionary file; *in.epw*, the weather file (needed only if there is a RunPeriod in the input); and optionally *Energy+.ini*, the initialization file. Typing "EnergyPlus" (and hitting the *Enter* key) will execute the program. EnergyPlus will write messages to the command window as it runs. A simulation with two design days and one run period looks like:
-
-```
- EnergyPlus Starting
- EnergyPlus, Version 1.3
- Warming up
- Initializing Response Factors
- Calculating CTFs for "EXTWALL80", Construction \#1
- Calculating CTFs for "PARTITION06", Construction \#2
- Calculating CTFs for "FLOOR SLAB 8 IN", Construction \#3
- Calculating CTFs for "ROOF34", Construction \#4
- Initializing Window Optical Properties
- Initializing Solar Calculations
- Initializing HVAC
- Warming up
- Warming up
- Warming up
- Performing Zone Sizing Simulation
- Warming up
- Warming up
- Warming up
- Performing Zone Sizing Simulation
- Initializing New Environment Parameters
- Warming up {1}
- Warming up {2}
- Warming up {3}
- Warming up {4}
- Starting Simulation at 01/14 for CHICAGO IL UNITED STATES TMY2 94846 WMO#=725340
- Initializing New Environment Parameters
- Warming up {1}
- Warming up {2}
- Warming up {3}
- Warming up {4}
- Starting Simulation at 07/07 for CHICAGO IL UNITED STATES TMY2 94846 WMO#=725340
- EnergyPlus Run Time=00hr 00min  7.31sec
-```
-
-When execution is finished, *eplusout.err* and *eplusout.audit* will always appear. If the program terminated with an input error, these may be the only output files. If the program runs normally, *eplusout.eio* will appear. Depending on what was requested in the input, the other output files described above will also be written.
-
-RunEPlus details
-----------------
-
-A procedure (batch) file is the normal way to run a console application. The *installed* procedure file **RunEPlus.bat** can be used to execute EnergyPlus and deal with all the file handling and postprocessing. It can accommodate running the EPMacro program if you name your files appropriately. And it can use ExpandObjects to expand the special "HVACTemplate" objects into "normal" IDF objects.
-
-The "set" statements near the beginning of the procedure file can be customized for each local system. Thus "program\_path" should be set to the directory path where the program executable resides on your local computer, "program\_name" should be set to the name of the EnergyPlus executable file, "input\_path" should be set to the directory path containing the input (IDF) file, and so forth. Each of the path environment variables must have "\\" as the final character or things won't run correctly. As mentioned before, the batch file is executed by typing:
-
-
-
-RunEPlus &lt;input\_filename&gt; &lt;weather\_filename&gt;
-
-
-
-where &lt;input\_filename&gt; is the name of the IDF file, without the file extension, and &lt;weather\_filename&gt; is the name of the weather file, without the file extension.The &lt;input\_filename&gt; can also be a complete path to the file (without extension) and it will work.
-
- In addition, RunEPlus can be called from a different directory and the temporary files will be created in the directory it is called from. This enables multiple RunEPlus.bat to be used with multiple processors or a multiple-core processor without the temporary files of one set of simulations interfering with another. Each call to RunEPlus.bat should be from different directories.
-
-Instructions appear at the top of the batch file:
-
-```
-:Instructions:
-:  Complete the following path and program names.
-:  path names must have a following \ or errors will happen
-:  does not have the capability to run input macro files (yet)
-:   %program_path% contains the path to the executable as well as IDD and is
-:                  the root directory
-:   %program_name% contains the name of the executable (normally EnergyPlus.exe)
-:   %input_path%   contains the path to the input file (passed in as first argument)
-:   %output_path%  contains the path where the result files should be stored
-:   %post_proc%    contains the path to the post processing program (ReadVarsESO)
-:   %weather_path% contains the path to the weather files (used with optional argument 2)
-:   %pausing%      contains Y if pause should occur between major portions of
-:                  batch file (mostly commented out)
-:   %maxcol%       contains "250" if limited to 250 columns otherwise contains
-:                  "nolimit" if unlimited (used when calling readVarsESO)
-
- echo ===== %0 (Run EnergyPlus) %1 %2 ===== Start =====
- set program_path=
- set program_name=EnergyPlus.exe
- set input_path=ExampleFiles\
- set output_path=Test\
- set post_proc=PostProcess\
- set weather_path=WeatherData\
- set pausing=N
- set maxcol=250
-
-:  This batch file will perform the following steps:
-:
-:   1. Clean up directory by deleting old working files from prior run
-:   2. Clean up target directory
-:   3. Copy %1.idf (input) into In.idf
-:   4. Copy %2 (weather) into In.epw
-:   5. Execute EnergyPlus
-:   6. If available Copy %1.rvi (post processor commands) into Eplusout.inp
-:   7. Execute ReadVarsESO.exe (the Post Processing Program)
-:   8. If available Copy %1.mvi (post processor commands) into test.mvi
-:       or create appropriate input to get meter output from eplusout.mtr
-:   9. Execute ReadVarsESO.exe (the Post Processing Program) for meter output
-:  10. Copy Eplusout.* to %1.*
-:  11. Clean up working directory.
-```
-
-RunDirMulti Batch File
-----------------------
-
-The RunDirMulti.bat batch file runs all the IDF files in the directory that it is located in. The batch file is used to run EnergyPlus simulations using the RunEPlus.bat for all the files in the current directory across multiple separate processor cores.  It has  two parameters, the weather file name to use for simulations and the number of processors.
-
-RunDirMulti &lt;weather file&gt; (opt) &lt;number processor cores&gt; (opt)
-
-The RunDirMulti batch file loops through the files located in the current directory and puts RunEPlus calls to each file into as many temporary batch files as processor cores and then starts each of the batch files. No load balancing between the cores is achieved using this method. The RunDirMulti.bat file should be located in a directory that contains the IDF files. Editing of the file may be necessary to match the directory that EnergyPlus is installed in.
-
-Since the batch file starts up other batch files in different CMD windows, the only way to know that the simulations are all complete is when all of the other CMD windows are closed. Those windows are named "Batch Simulation&lt;n&gt;" where n is 1 to the number of processor cores you selected to use.
-
-
-
-EnergyPlus Files
-----------------
-
-### Input Files
-
-The following files are input to the EnergyPlus program.
-
-#### Energy+.idd
-
-The *input data dictionary* (IDD) is an ascii (text) file containing a list of all possible EnergyPlus objects and a specification of the data each object requires. This file is analogous to the DOE-2 keyword file. The *Guide for Interface Developers* contains a full description of the input data dictionary.
-
-#### in.idf
-
-The *input data file* (IDF) is an ascii file containing the data describing the building and HVAC system to be simulated. The *Guide for Interface Developers* shows examples of IDF input. Many example files are installed as part of the EnergyPlus installation.
-
-#### in.imf
-
-The *input macro file* (IMF) is an ascii file that is formatted for the EP-Macro program.  Output from the EP-Macro program will be the standard in.idf format.  IMF files are not directly read by EnergyPlus.
-
-#### Energy+.ini
-
-This is the EnergyPlus initialization file. It is an optional ascii input file that allows the user to specify the path for the directory containing Energy+.idd. This file, using the actual directories of the install, will be created during the install. An example is:
-
-```
-[program]
-dir=C:\EnergyPlus
-
-[weather]
-dir=
-
-[BasementGHT]
-dir=PreProcess\GrndTempCalc
-
-[SlabGHT]
-dir= PreProcess\GrndTempCalc
-```
-
-Under [program], dir should indicate the folder where EnergyPlus is installed (e.g. C:\\Program Files\\EnergyPlusV2-0-0 or C:\\EnergyPlusV2-0-0).  This is automatically generated during the install and may be the "shortened form" of these folder names. The "weather" portion of the initialization file is unused for normal EnergyPlus. [BasementGHT] and [SlabGHT] are used by the EP-Launch program when the Utilities tab is used to execute the Basement and Slab programs, respectively.
-
-#### in.epw
-
-The *EnergyPlus weather* file is an ascii file containing the hourly or sub-hourly weather data needed by the simulation program. The data format is described in this document in the section: EnergyPlus Weather File (EPW) Data Dictionary.
-
-### Output Files
-
-More information (and more up-to-date) about output files is shown in the [Output Details and Examples](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf) Document.
-
-#### eplusout.err
-
-A text file containing the error messages issued by EnergyPlus. This is the first output that should be examined after a simulation. Error messages are issued by EnergyPlus during its input phase or during the simulation. There are three levels of error severity: *fatal*, *severe*, and *warning* as well as simple *"message"* lines. A fatal error causes the program to terminate immediately. The following table illustrates the necessary actions.
-
-Table 34. Error Message Levels - Required Actions
-
-<table class="table table-striped">
-<tr>
-<th>Error Level</th>
-<th>Action</th>
-</tr>
-<tr>
-<td>"Information"</td>
-<td>Informative, usually a follow-on to one of the others. No action required.</td>
-</tr>
-<tr>
-<td>Warning</td>
-<td>Take note. Fix as applicable.</td>
-</tr>
-<tr>
-<td>Severe</td>
-<td>Should Fix</td>
-</tr>
-<tr>
-<td>Fatal</td>
-<td>Program will abort</td>
-</tr>
-</table>
-
-
-
-An example of an error message due to an input syntax error is:
-
-```
-** Severe  ** Did not find " DessignDay" in list of Objects
-   **  Fatal  ** Errors occurred on processing IDF file -
-       probable incorrect IDD file. View "audit.out" for details.
-   ************* EnergyPlus Terminated--Error(s) Detected.
-```
-
-#### eplusout.audit
-
-This is an text file which echoes the IDD and IDF files, flagging syntax errors in either file. Note that both *eplusout.err* and *eplusout.audit* will show the error messages caused by input syntax errors; however only *eplusout.err* will show errors issued during the actual simulation. *eplusout.audit* can be used when you need to see the context of the error message to fully ascertain the cause.
-
-#### eplusout.eso
-
-The *EnergyPlus Standard Output* (ESO) is a text file containing the time varying simulation output. The format of the file is discussed in the *Guide for Interface Developers* and the *InputOutputReference*. The contents of the file are controlled by *Report Variable* commands in the IDF file. Although the ESO is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
-
-#### eplusout.mtr
-
-The *EnergyPlus Meter Output* (MTR) is a text file containing the time varying simulation output. The format of the file is similar to the ESO file. Meters are a powerful reporting tool in EnergyPlus. Values are grouped onto logical meters and can be viewed the same way that the ESO variables are used. The contents of the file are controlled by *Report Meter* commands in the IDF file. Although the MTR is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
-
-#### eplusout.eio
-
-The *EnergyPlus Invariant Output* (EIO) is a text file containing output that does not vary with time. For instance, location information (latitude, longitude, time zone, altitude) appears on this file.
-
-#### eplusout.rdd
-
-The *Report (variable) Data Dictionary* (RDD) is a text file listing those variables available for reporting (on the ESO or MTR) for this particular simulation. Which variables are available for output on the ESO or MTR depends on the actual simulation problem described in the IDF. A simulation with no chiller would not permit the output of any chiller report variables. The user may need to examine the RDD to find out which report variables are available in a particular simulation. The RDD is written only if
-
-```
-Output:VariableDictionary, <either Regular or IDF>;
-```
-
-appears in the input (IDF) file.
-
-#### eplusout.dbg
-
-This is a text file containing *debug* output for use by EnergyPlus developers. Generally developers will add debug print statements wherever in the code that that they wish. There is a "standard" debug output that prints out conditions at all the HVAC nodes. This output is triggered by placing
-
-DEBUG OUTPUT,1;
-
-in the IDF file. If DEBUG OUTPUT, 0 is entered, you will get an empty eplusout.dbg file.
-
-#### eplusout.dxf
-
-This is a file in AutoCad DXF format showing all the surfaces defined in the IDF file. It provides a means of viewing the building geometry. The DXF file from EnergyPlus highlights different building elements (shading, walls, subsurfaces) in differing colors. A number of programs can read and display DXF files. One that works well is Volo View Express, available free from the Autodesk web site. Output of this file is triggered by
-
-Report, Surfaces, DXF;
-
-in the IDF.
-
-#### eplusout.sln
-
-A text file containing the coordinates of the vertices of the surfaces in the IDF.
-
-Output of this file is triggered by
-
-Report, Surfaces, Lines;
-
-in the IDF.
-
-### Postprocessing Program/Files
-
-A postprocessing program *ReadVarsESO.exe* is available that will read an ESO or MTR file and produce a file that can be read by Excelâ„¢. It can use an input file or not. In batch mode it is run by the little batch file *RunReadESO.bat*:  Further information on this program is provided in the [Input Output Reference](file:///E:\Docs4PDFs\InputOutputReference.pdf) as well as the [Output Details and Examples](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf) documents.
-
-You can also used the CSVProc and convertESOMTR described earlier in this document as part of your post processing strategy.
-
-
-
-Creating Input Files
-====================
-
-EnergyPlus has several options for the user to create input files. One of the goals of EnergyPlus was to make a simple, readable input file for the program. More of this background and explanation is contained in the Interface Developer's Guide. Understanding the Input Data Dictionary (IDD) is the key to reading the input file. We have set some conventions for commenting the IDD so that the units, minimum, maximum, and other information. This changes some of the information that is shown in the Interface Developer's guide. The Energy+.idd (delivered with the install program) contains the most current information. In addition to the four methods for creating inputs described below, several other items are described that may assist you in getting the results you want from EnergyPlus in a timely manner.
-
-Four methods (with the installed program) are available to create input files:
-
-1)    IDFEditor - this is a very simple, "intelligent" editor that reads the IDD and IDFs and allows creation/revision of IDF files. It can be run from a shortcut in the main EnergyPlus directory (created as part of the install) or directly from EP-Launch.
-
-2)    BLAST Translator - if you already have BLAST and/or BLAST input files, this program will produce the bulk of a translation to EnergyPlus for you. It generates a complete IDF file but does not include specifics for Systems or Plants. (It does include the System and Plant schedules that were in the BLAST deck). Many of the sample files included with the install started out as BLAST input files.
-
-3)    DOE-2 Translator - if you already have  DOE-2.1e input files, this program will produce the bulk of a translation to EnergyPlus for you. It generates a IMF (input macro file) that must be run through the EnergyPlus Macro (EPMacro) program before it can be used by EnergyPlus.
-
-4)    Hand editing - for simple changes to an existing file (such as one of the sample files), you can hand edit a file using your knowledge of the IDD, comments in the IDF file, and a text editor such as NOTEPADâ„¢ (Wordpadâ„¢ for large files). For creating HVAC simulations - the HVACtemplate objects provide a quick way to start at HVAC simulation.
-
-IDD Conventions
----------------
-
-The following is a basic description of the structure of the IDD (it's actually taken directly from the IDD file). As noted within, ! signifies a comment character as does the \\. \\ has also been adopted as a convention for including more specific comments about each field in an object. These have been used with success in the IDFEditor and it is hoped the flexibility will provide other interface developers with useful information.
-
-```
-! Object Description
-! ------------------
-! To define an object (a record with data), develop a key word that is unique
-! Each data item to the object can be A (Alphanumeric string) or N (numeric)
-! Number each A and N.  This will show how the data items will be put into the
-! arrays that are passed to the Input Processor "Get" (GetObjectItem) routines.
-! All alpha fields are limited to 100 characters.  Numeric fields should be
-! valid numerics (can include such as 1.0E+05) and are placed into double
-! precision variables.
-!
-! NOTE: Even though a field may be optional, a comma representing that field
-!   must be included (unless it is the last field in the object).  Since the
-!   entire input is "field-oriented" and not "keyword-oriented", the EnergyPlus
-!   Input Processor must have some representation (even if blank) for each
-!   field.
-!
-! Object Documentation
-! --------------------
-! In addition, the following special comments appear one per line and
-! most are followed by a value.  Comments may apply to a field or the object
-! or a group of objects.
-!
-! Field-level comments:
-!
-!  \field           Name of field
-!                     (should be succinct and readable, blanks are encouraged)
-!
-!  \note            Note describing the field and its valid values
-!
-!  \required-field  To flag fields which may not be left blank
-!                     (this comment has no "value")
-!
-!  \begin-extensible  Marks the first field at which the object accepts an extensible
-!                   field set.  A fixed number of fields from this marker define the
-!                   extensible field set, see the object code \extensible for
-!                   more information.
-!
-!  \units           Units (must be from EnergyPlus standard units list)
-!                   EnergyPlus units are standard SI units
-!
-!  \ip-units        IP-Units (for use by input processors with IP units)
-!                   This is only used if the default conversion is not
-!                   appropriate.
-!
-!  \unitsBasedOnField  For fields that may have multiple possible units, indicates
-!                   the field in the object that can be used to determine
-!                   the units. The field reference is in the A2 form.
-!
-!  \minimum         Minimum that includes the following value
-!
-!  \minimum>        Minimum that must be > than the following value
-!
-!  \maximum         Maximum that includes the following value
-!
-!  \maximum<        Maximum that must be < than the following value
-!
-!  \default         Default for the field (if N/A then omit entire line)
-!
-!  \deprecated      This field is not really used and will be deleted from the object.
-!                   The information is gotten internally within the program.
-!
-!  \autosizable     Flag to indicate that this field can be used with the Auto
-!                   Sizing routines to produce calculated results for the
-!                   field.  If a value follows this, then that will be used
-!                   when the "Autosize" feature is flagged.  To trigger
-!                   autosizing for a field, enter Autosize as the field's
-!                   value.  Only applicable to numeric fields.
-!
-! \autocalculatable Flag to indicate that this field can be automatically
-!                   calculated. To trigger auto calculation for a field, enter
-!                   Autocalculate as the field's value.  Only applicable to
-!                   numeric fields.
-!
-!  \type            Type of data for the field -
-!                     integer
-!                     real
-!                     alpha       (arbitrary string),
-!                     choice      (alpha with specific list of choices, see
-!                                 \key)
-!                     object-list (link to a list of objects defined elsewhere,
-!                                  see \object-list and \reference)
-!                     node        (name used in connecting HVAC components)
-!
-!  \retaincase      Retains the alphabetic case for alpha type fields
-!
-!  \key             Possible value for "\type choice" (blanks are significant)
-!                     use multiple \key lines to indicate all valid choices
-!
-!  \object-list     Name of a list of user-provided object names that are valid
-!                     entries for this field (used with "\reference")
-!                     see Zone and BuildingSurface:Detailed objects below for
-!                     examples.
-!                  ** Note that a field may have multiple \object-list commands.
-!
-!  \reference       Name of a list of names to which this object belongs
-!                     used with "\type object-list" and with "\object-list"
-!                     see Zone and BuildingSurface:Detailed objects below for
-!                     examples:
-!
-!                        Zone,
-!                          A1 , \field Name
-!                               \type alpha
-!                               \reference ZoneNames
-!
-!                        BuildingSurface:Detailed,
-!                          A4 , \field Zone Name
-!                               \note Zone the surface is a part of
-!                               \type object-list
-!                               \object-list ZoneNames
-!
-!             For each zone, the field "Name" may be referenced
-!             by other objects, such as BuildingSurface:Detailed, so it is
-!             commented with "\reference ZoneNames"
-!             Fields that reference a zone name, such as BuildingSurface:Detailed's
-!             "Zone Name", are commented as
-!             "\type object-list" and "\object-list ZoneNames"
-!             ** Note that a field may have multiple \reference commands.
-!             ** This is useful if the object belongs to a small specific
-!             object-list as well as a larger more general object-list.
-!
-! Object-level comments:
-!
-!  \memo            Memo describing the object
-!
-!  \unique-object   To flag objects which should appear only once in an idf
-!                     (this comment has no "value")
-!
-!  \required-object To flag objects which are required in every idf
-!                     (this comment has no "value")
-!
-!  \min-fields      Minimum number of fields that should be included in the
-!                   object.  If appropriate, the Input Processor will fill
-!                   any missing fields with defaults (for numeric fields).
-!                   It will also supply that number of fields to the "get"
-!                   routines using blanks for alpha fields (note -- blanks
-!                   may not be allowable for some alpha fields).
-!
-!  \obsolete        This object has been replaced though is kept (and is read)
-!                   in the current version.  Please refer to documentation as
-!                   to the dispersal of the object.  If this object is
-!                   encountered in an IDF, the InputProcessor will post an
-!                   appropriate message to the error file.
-!                   usage:  \obsolete New=>[New object name]
-!
-!  \extensible:<#>  This object is dynamically extensible -- meaning, if you
-!           change the IDD appropriately (if the object has a simple list
-!           structure -- just add items to the list arguments (i.e. BRANCH
-!           LIST). These will be automatically redimensioned and used during
-!           the simulation. <#> should be entered by the developer to signify
-!           how many of the last fields are needed to be extended (and EnergyPlus
-!           will attempt to auto-extend the object).  The first field of the first
-!           instance of the extensible field set is marked with \begin-extensible.
-!
-!  \begin-extensible See previous item, marks beginning of extensible fields in
-!                   an object.
-!
-!  \format          The object should have a special format when saved in
-!                   the IDF Editor with the special format option enabled.
-!                   The options include SingleLine, Vertices, CompactSchedule,
-!                   FluidProperties, ViewFactors, and Spectral.
-!                   The SingleLine option puts all the fields for the object
-!                   on a single line. The Vertices option is used in objects
-!                   that use X, Y and Z fields to format those three fields
-!                   on a single line.
-!                   The CompactSchedule formats that specific object.
-!                   The FluidProperty option formats long lists of fluid
-!                   properties to ten values per line.
-!                   The ViewFactor option formats three fields related to
-!                   view factors per line.
-!                   The Spectral option formats the four fields related to
-!                   window glass spectral data per line.
-!
-!   \reference-class-name Adds the name of the class to the reference list
-!                   similar to \reference.
-!
-! Group-level comments:
-!
-!  \group          Name for a group of related objects
-!
-!
-! Notes on comments
-! -----------------
-!
-! 1.  If a particular comment is not applicable (such as units, or default)
-! then simply omit the comment rather than indicating N/A.
-!
-! 2.  Memos and notes should be brief (recommend 5 lines or less per block).
-! More extensive explanations are expected to be in the user documentation
-!
-! Default IP conversions (no \ip-units necessary)
-!     m                      =>   ft                  3.281
-!     W                      =>   Btu/h               3.412
-!     m3/s                   =>   ft3/min             2118.6438
-!     C                      =>   F                   1.8 (plus 32)
-!     kg/J                   =>   lb/Btu              2325.83774250441
-!     Pa                     =>   psi                 0.0001450377
-!     W/m-K                  =>   Btu-in/h-ft2-F      6.93481276005548
-!     W/K                    =>   Btu/h-F             1.8987
-!     deltaC                 =>   deltaF              1.8
-!     m2                     =>   ft2                 10.764961
-!     K                      =>   R                   1.8
-!     1/K                    =>   1/R                 0.555555556
-!     (kg/s)/W               =>   (lbm/sec)/(Btu/hr)  0.646078115385742
-!     J/kg                   =>   Btu/lb              0.00042986 (plus 7.686)
-!     kg-H2O/kg-air          =>   lb-H2O/lb-air       1
-!     kJ/kg                  =>   Btu/lb              0.429925
-!     lux                    =>   foot-candles        0.092902267
-!     kg/m3                  =>   lb/ft3              0.062428
-!     kg/s                   =>   lb/s                2.2046
-!     kg/s-m                 =>   lb/s-ft             0.67194
-!     m3                     =>   ft3                 35.319837041
-!     m3                     =>   gal                 264.172
-!     W/m2-K                 =>   Btu/h-ft2-F         0.176110194261872
-!     1/m                    =>   1/ft                0.304785126485827
-!     J/kg-K                 =>   Btu/lb-F            0.000239005736137667
-!     J/m3-K                 =>   Btu/ft3-F           1.49237004739337E-05
-!     m/s                    =>   ft/min              196.86
-!     m/s                    =>   miles/hr            2.2369
-!     m2-K/W                 =>   ft2-F-hr/Btu        5.678263
-!     W/m2                   =>   Btu/h-ft2           0.316957210776545
-!     A/K                    =>   A/F                 0.555555555555556
-!     g/kg                   =>   grains/lb           7.00000
-!     g/m-s                  =>   lb/ft-s             0.000671968949659
-!     g/m-s-K                =>   lb/ft-s-F           0.000373574867724868
-!     J/K                    =>   Btu/F               0.000526917584820558
-!     J/kg-K2                =>   Btu/lb-F2           0.000132889924714692
-!     J/m3                   =>   Btu/ft3             2.68096514745308E-05
-!     kg/kg-K                =>   lb/lb-F             0.555555555555556
-!     kPa                    =>   psi                 0.145038
-!     kPa                    =>   inHg                0.29523
-!     m2/s                   =>   ft2/s               10.764961
-!     m3/kg                  =>   ft3/lb              16.018
-!     m3/m3                  =>   ft3/ft3             1
-!     N-s/m2                 =>   lbf-s/ft2           0.0208857913669065
-!     V/K                    =>   V/F                 0.555555555555556
-!     W/m-K2                 =>   Btu/h-F2-ft         0.321418310071648
-!     m3/s-m                 =>   ft3/min-ft          645.89
-!     J/m2-K                 =>   Btu/ft2-F           4.89224766847393E-05
-!     cycles/hr              =>   cycles/hr           1
-!     kg/kg                  =>   lb/lb               1
-!     J/J                    =>   Btu/Btu             1
-!     g/GJ                   =>   lb/MWh              0.00793664091373665
-!     L/GJ                   =>   gal/kWh             0.000951022349025202
-!     m3/GJ                  =>   ft3/MWh             127.13292
-!     m3/s-m2                =>   ft3/min-ft2         196.85
-!     m3/s-person            =>   ft3/min-person      2118.6438
-!     W/m2-K2                =>   Btu/h-ft2-F2        0.097826
-!     g/MJ                   =>   lb/MWh              7.93664091373665
-!     L/MJ                   =>   gal/kWh             0.951022349025202
-!     m3/MJ                  =>   ft3/kWh             127.13292
-!     W/W                    =>   Btuh/Btuh           1
-!     $/m2                   =>   $/ft2               0.0928939733269818
-!     $                      =>   $                   1
-!     $/kW                   =>   $/(kBtuh/h)         0.293083235638921
-!     $/m3                   =>   $/ft3               0.0283127014102352
-!     years                  =>   years               1
-!     $/(W/K)                =>   $/(Btu/h-F)         0.52667614683731
-!     $/(m3/s)               =>   $/(ft3/min)         0.000472000059660808
-!     W/m                    =>   Btu/h-ft            1.04072
-!     K/m                    =>   F/ft                0.54861322767449
-!     W/s                    =>   W/s                 1
-!     kmol                   =>   kmol                1
-!     J                      =>   Wh                  0.000277777777777778
-!     GJ                     =>   ton-hrs             78.9889415481832
-!     kg/m2                  =>   lb/ft2              0.204794053596664
-!     kg                     =>   lb                  2.2046
-!     percent/K              =>   percent/F           0.555555555555556
-!     kg/s2                  =>   lb/s2               2.2046
-!     g/mol                  =>   lb/mol              0.0022046
-!     deltaJ/kg              =>   deltaBtu/lb         0.0004299
-!     person/m2              =>   person/ft2          0.0928939733269818
-!     m2/person              =>   ft2/person          10.764961
-!     W/person               =>   Btu/h-person        3.412
-!     m3/person              =>   ft3/person          35.319837041
-!     m3/hr-person           =>   ft3/hr-person       35.319837041
-!     m3/m2                  =>   ft3/ft2             3.281
-!     m3/hr-m2               =>   ft3/hr-ft2          3.281
-!     m3/hr                  =>   ft3/hr              35.319837041
-!     s/m                    =>   s/ft                0.304785126485827
-!     m2/m                   =>   ft2/ft              3.281
-!     L/day                  =>   pint/day            2.11337629827348
-!     L/kWh                  =>   pint/kWh            2.11337629827348
-!     kg/Pa-s-m2             =>   lb/psi-s-ft2        1412.00523459398
-!     m/hr                   =>   ft/hr               3.281
-!     Mode                   =>   Mode                1
-!     Control                =>   Control             1
-!     Availability           =>   Availability        1
-!     rev/min                =>   rev/min             1
-!     W/(m3/s)               =>   W/(ft3/min)         0.0004719475
-!     VA                     =>   VA                  1
-!     N-m                    =>   lbf-in              8.85074900525547
-!     m3/s-W                 =>   ft3-h/min-Btu       621.099127332943
-!     cm2                    =>   inch2               0.15500031000062
-!     kg/m                   =>   lb/ft               0.67196893069637
-!     m/yr                   =>   inch/yr             39.37
-!
-! Other conversions supported (needs the \ip-units code)
-!
-!     m                      =>   in                  39.37
-!     W                      =>   W                   1
-!     m3/s                   =>   gal/min             15852
-!     m3/s                   =>   lbH2O/hr            7936289.998
-!     Pa                     =>   inHg                0.00029613
-!     Pa                     =>   inH2O               0.00401463
-!     Pa                     =>   ftH2O               0.00033455
-!     W/person               =>   W/person            1
-!     W/m2                   =>   W/m2                1
-!     W/m2                   =>   W/ft2               0.0928939733269818
-!     W/m-K                  =>   Btu/h-ft-F          0.577796066000163
-!
-! Units fields that are not translated
-!     deg
-!     hr
-!     A
-!     dimensionless
-!     V
-!     ohms
-!     A/V
-!     eV
-!     percent
-!     s
-!     W/m2 or deg C
-!     W/m2, W or deg C
-!     minutes
-!     1/hr
-! **************************************************************************
-```
-
-IDFEditor
----------
-
-IDF Editor is an optional component of the EnergyPlus installation. For users who want a simple way of creating or editing EnergyPlus input data files (IDF), IDF Editor provides this service.  The IDF Editor does not check inputs for validity, although some numeric fields are highlighted if out of range and some text fields are highlighted if they contain an invalid reference. For instructions and rules that must be followed when creating an IDF file the user should refer to the [*Input/Output Reference*](../../EnergyPlusFromStarTeam/EnergyPlusFromStarTeam/Documentation/sources/InputOutputReference.pdf) document.
-
-![](media/image115.png)
-
-Figure 49. IDF Editor Screen.
-
-### Start IDF Editor
-
-IDF Editor should be located in the EnergyPlus\\PreProcessor\\IDFEditor directory where you installed EnergyPlus. By double clicking on the IDF Editor icon you will get a screen similar to the one shown above. IDF Editor works in conjunction with the current EnergyPlus Input Data Directory (IDD) file that resides in the directory where EnergyPlus is installed. Another way to start the IDF Editor is from EP-Launch. Multiple IDF files can be opened at once.
-
-### Creating or Selecting an Input Data File
-
-Creating a new input data file or selecting an existing input data file can be accomplished either through use of the File menu on the menu bar at the top of the screen or through use of the New File icon button or Open File icon button on the tool bar.
-
-### Class List and Objects
-
-The classes that can be used to make up an IDF file have been organized into groups as shown in the 'Class List' portion of the screen. A class is made up of a group of objects. Select a class from the list by clicking on and highlighting the class. The field to the left of the selected class in the 'Class List' will either contain [------] to indicate that this class has no objects in the IDF file or it will contain a number like [0003] to indicate the number of times the object currently appears in the IDF file. For example, for the BuildingSurface:Detailed class selected in the screen above under the Thermal Zone Description/Geometry group, there are 40 objects in the IDF file. The details for these 40 objects or any new object that is defined are displayed in columns within the grid. Each object is made up of fields and can be used to further define the object. Any units attached to each field are shown in the second column. You may need to scroll down the 'field' list or maximize the application to see all of the fields. Likewise, you may need to scroll to the right of the main grid to see other objects.
-
-Options under the view menu can change how you use the Class List. To display only classes that contain objects select the "show classes with objects only" option on the "View" menu. You can also toggle this feature on and off with CTRL+L. If the file is empty and has no objects, this toggle does not impact the display.
-
-The "Show Quick Select Dropdowns" view menu option adds two new input fields to the main screen. The input fields can be used to go quickly to different classes in the main list of classes. By typing in the top input field, the group that starts with those letters are displayed. After selecting one and pressing the tab button, classes in that group are shown and by typing the first few letters, you can easily select a specific class. Pressing tab again displays that class and it objects. This method allows for quick selection of classes if you remember the group name and class name.
-
-### Changing Values
-
-By clicking and highlighting a value within an object, several things happen:
-
-1)   Any user comments from the IDF file will be displayed in the 'Comments from IDF' portion of the screen
-
-2)   Any notes contained in the IDD for this input field will be displayed in the 'Explanation of Keyword' portion of the screen
-
-3)   The value can be edited. Depending on the field, a drop down list may display the default value, maximum and minimum, or other keywords that can be used with the field.
-
-4)   Numeric fields that can be autosized will include "autosize" as a selection in the drop down list.
-
-5)   Some numeric fields have a maximum and/or minimum value specified in the IDD. If the value entered is outside this range, the cell will be highlighted in pale orange.
-
-6)   For values that are names of nodes, a new dialog box titled "Edit or Select Node Name" can be shown when the small button is pressed that is on the right side in each node name cell as described in the next section.
-
-### Edit or Select Node Names Dialog
-
-The following dialog box is displayed when the small button is pressed that is on the right side of cells used for node names. Double clicking on cells containing node names can also make the dialog box appear.
-
-![](media/image116.png)
-
-Figure 50. Edit or Select Node Name Dialog Box
-
-To enter a new node name, type it in the "Node Name" field near the top of the dialog. To select a name of a node that is already being used in the file, choose a node name from the list shown on the left of the dialog box and labeled "Other Node Names." When a node name is selected from the list on the left side of the dialog box, the box near the bottom left shown as "Where Selected Other Node Name Appears in File" will display the name of the class, name of the object and name of the field for each other location in the file that node name is currently be used.
-
-The Other Node Names list on the left side of the dialog box may contain a very long list of node names depending on the complexity of the HVAC system. To help with this, four options are available just above the list titled All, Recent, Containing, and Class or Field. The All option shows all node names used in the file while the other options are used to narrow the list down to only certain node names. The Recent option shows only node names that have recently been edited. The Containing option shows a list on the right side of the dialog box called "Filter by Contents" which shows all of the various words used as part of node names. These words can be selected and the Other Node Names list will only show node names that contain those words. By selecting words from this list, the list of Other Node Names can be shortened very quickly. The last option, Class or Field, shows a hierarchical list on the right side titled Filter by Object or Field containing the list of classes and fields that can have node names. By selecting an object or a field, the Other Node Names list on the right shows only node names that are present in the selected object or field. This is another way of quickly shortening the list of Other Node Names so that the appropriate node name can be selected.
-
-Finally, the Containing Text field just above the OK button can be typed in. Whatever you type limits the Other Node Names list to just those characters. The more typed, the shorter the list becomes. This is another method of quickly finding the node name used in other parts of the file. The Containing Text field is usually used with the All option but can be used with the other display options as well.
-
-### Working with Objects
-
-To delete an object, first click on any value for the object and then click on the "Del Obj" button. To add a new object, click on the "New Obj" button and a new object column with fields set to blanks, zeros, or default values will be added to the far right of the grid. The "Dup Obj" button is similar to "New Obj", but copies the values of the fields of the currently selected object. Copying and pasting an object or groups of objects is also possible using the "Copy Obj" and "Paste Obj" buttons.  These allow objects to be copied between files are also good for copying from files in the DataSets subdirectory. (Also see the Edit menu to perform these functions.)
-
-### File Menu
-
-The File menu can be used for creating or selecting input files just like the buttons on the IDF Editor screen (see the *Creating or Selecting an Input File* section above). In addition, the File menu is used to save a file or exit the IDF Editor. More than one file can be opened at a time.
-
-The "File", "Save Options" screen is shown below.
-
-
-
- ![](media/image117.png)
-
-Figure 51. IDF Editor Save Options Screen.
-
-The save options allow the order of the objects in the file to be sorted by type of object or to keep the original order of the objects (for an existing file). The placement of new objects when the original order is specified can be either at the top or bottom of the file.
-
-In addition, the Save Options also allow certain objects to be written to the file using a specific format that some users prefer.
-
-The settings for the save options are kept for each file saved from the IDF Editor.
-
-The "Set as Default" option allows you to keep the save options intact for files that have not been saved yet with a version of IDF Editor that has this capability.
-
-The Help that is available from the Save Options screen is reproduced below:
-
-* The save options are related to the layout of the IDF file after it is saved. These options are not important if you never edit the IDF file with a text editor.
-
-* The sorted order of saving objects is the traditional way the IDF Editor sorts objects within files. Each type of object is presented in groups in the order they appear in the Energy+.IDD. The other options preserve the original order of the objects from the file but each object will be still be reformatted. By preserving the order, the objects are not rearranged so you can group them using a text editor and they will stay in that order. New objects are placed either near the top of the file or near the bottom of the file so that they can be easily found when using a text editor.
-
-* You can also choose to specially format some objects. This affects how individual fields in objects are arranged when saved. Selecting this option will format the following objects on a single line: Report, Report Meter, Report Variable, Version, Timestep in Hour, Inside Convection Algorithm, Outside Convection Algorithm, Solution Algorithm, Shadowing Calculations, Ground Reflectances, and GroundTemperatures:Deep. In addition, Schedule:Compact objects will be formatted to have two field for some lines. With this option, objects with geometric vertices are formatted to have the X, Y, and Z values on the same line. Those objects include: Surface:HeatTransfer, Surface:HeatTransfer:Sub, Surface:Shading:Detached:Fixed, Surface:Shading:Detached:Building and Surface:Shading:Attached.
-
-* These options are saved for each file. If a file has not been saved with IDF Editor yet, the default is used  but if a file does not specify the default values for these can also be set by using the set as default option. The saved file keeps these options by using the !-option line with SortedOrder, OriginalOrderTop, OriginalOrderBottom, and UseSpecialFormat."
-
-* Full line comments which begin with "!" are preserved by IDF Editor and become associated with the object immediately followin the comment line(s).
-
-* Endline comments which begin with "!" are preserved by IDF Editor and are placed immediately before the object they are found in.
-
-* Endline comment which being with "!-" are automatic comments which IDF Editor will overwrite with the field name and units. User-provided text which follows "!-" will be lost. User comments should be added above the pertinent object using "!" to begin the line.
-
-Also on the File menu is the Open DataSet menu and submenu. This allows you to open any input file that appears in the DataSet subdirectory and copy objects from them into another file. This is required because EnergyPlus does not read the DataSet files, it is up to you to include objects from them.
-
-### Edit Menu
-
-The Edit Menu offers options to create a new object, duplicate an object, and delete an object as well as finding and searching. The object options are the same operations as can be accomplished by using the 'New Obj', 'Dup Obj' and 'Del Obj' buttons (see the *Working with Objects* section above). In addition, the "Next Row after Enter" option can be toggled. When this option is on, the selection moves down one row after pressing Enter. The copy and paste object commands allow a single object to be copied within a file or between files. The pasted object appears as the last object in the class. This capability makes it easier to utilize the data in the DataSets directory.
-
-The Find Class menu item brings up the following dialog box used to search through the Class List:
-
-![](media/image118.png)
-
-Figure 52. Find Class Dialog Box
-
-The Find Class dialog can be used to find class names quickly and can be activated by the CTRL-F keyboard combination. The Find Previous Class (CTRL-T) and Find Next Class (CTRL-G) can continue the searching process for the next and previous times that the searched text is found in the Class List. If you find this option useful you may also want to try the Show Quick Select Dropdowns option under the View menu which also speeds up searching through the Class List.
-
-The Search and Replace menu item or CTRL-H activates the following dialog box:
-
-![](media/image119.png)
-
-Figure 53. Search and Replace Diaglog Box
-
-The Search and Replace dialog box can be used to find and change each instance of text being searched with some replacement text. The Search and Replace dialog is used to search and replace values of fields rather than classes like the Find Class dialog. To use the Search and Replace dialog, enter the text being searched in the Find What field and press the Find button.  After the Find button is pressed, the list shows the places in the file that the text appears. For each time the text is found, the entire field value is shown followed by the class name, name of the object, and the name of the field in parentheses.  Each item in the list can be selected using the check box to the left. The All and None buttons will select all or none of the items found. After the locations are selected that need to be replaced, you should enter the text in the Replace With field. When the Replace Selected button is pressed the value in each of locations that were checked will be replaced with the Replace with text.
-
-The dialog will usually open with the Find What field filled with the value of the currently selected cell. If the current cell has just been changed, the Find What and the Replace With fields will contain the before and after values of the change in the current cell. This makes it easy to change other instances in the file to be consistent with the changes just made. If renaming objects, the recommended approach is to rename the object and select the cell again and open the Search and Replace dialog. This will show other places in the file that use that object name that also may need to be changed.
-
-### View Menu
-
-The View menu offers options for units and column widths. The Narrow/Medium/Wide Column options set the standard column width for items in the object grid. Individual columns can also be resized by dragging the column separator. The displayed value is rounded and/or expressed in scientific notation to fit within the column width.
-
-1)   EnergyPlus input files are always in SI units. However, selecting "Inch-Pound" (IP) units in the View menu displays and edits values in IP units in the IDF editor. The IP unit will be displayed in the units column of the object grid. Some SI units convert to multiple IP units. For example, W becomes Btu/hr for heating and cooling capacity but remains as W for lighting and electrical equipment.
-
-2)   All conversion factors used in the IDF editor are documented in a block of comments near the top of the Energy+.IDD file.
-
-3)   Schedules, fluid properties and curves now support IP unit conversions. For curves, the minimum and maximum values are converted but the coefficients are not.
-
-To display only classes that contain objects select the "show classes with objects only" option on the "View" menu. You can also toggle this feature on and off with CTRL+L. If the file is empty and has no objects, this toggle does not impact the display.
-
-The "Show Quick Select Dropdowns" option, which can also be turned on and off with CTRL-Q, displays two dropdown lists above the class list that can be quickly used to select classes. The first list displays the possible groups. Once those are selected, the second list contains only the classes within that group. This option may be used to quickly access classes while avoiding scrolling through the long class list. In addition these pull down menus may be used with the keyboard to select groups and class names based on the first few letters of the names.
-
-The figure below shows the "Layout Options" also accessible under the View menu.
-
-![](media/image120.png)
-
-Figure 54. IDF Editor Layout Options Screen.
-
-This option allows for different arrangements of the layout for the main screen of the IDF Editor. Select one of the four layouts available.
-
-The "Show Quick Select Dropdowns" view menu option adds two new input fields to the main screen. The input fields can be used to go quickly to different classes in the main list of classes.
-
-The "Validity Check" function has replaced and expanded upon the old "Check Out-of-Range" function. It can also be started by using CTRL-R. The "Validity Check" function performs three kinds of validity checks and displays the results as shown in the dialog box below:
-
-![](media/image121.png)
-
-Figure 55. Validity Check Dialog Box
-
-The list displays the values and locations for objects with values that are either above the maximum or below the minimum values. This allows you to check your input for out-of-range values prior to running EnergyPlus.  It also displays fields that contain invalid references. An invalid reference is when a name is used that should be the name of object but no object exists that uses that name. For example, if a Construction object references a layer named IN20 but no Material (or Material:NoMass, etc.) object is named IN20. When viewing the class that contains invalid references, those references are shown with a different background color similar to numbers that are out of range. The "Validity Check" dialog also shows when an entry for a field is not one of the possible lists of choices. The Goto button allows you to jump directly to the selected identified problems. The Perform Validity Check When Saving File can be turned on and off and automatically performs the check whenever the file is saved.
-
-### Help Menu
-
-The Help menu offers options to open the EnergyPlus documentation files.
-
-### Caveats
-
-Remember to save any changes made before you create or edit another input file.
-
-No "Run EnergyPlus" button is available. Save your IDF file and use EP-Launch to execute an EnergyPlus run.
-
-You cannot edit comments in the 'Comments from IDF' section of the screen.
-
-The use of point "." or comma "," as the decimal symbol is controlled by the windows system settings. This setting is found in the Control Panel, Regional Options, Number tab, Decimal Symbol field. IDF Editor will use the current decimal symbol to signify the start of the fractional portion of the number and will ignore other symbols. The idf file is always written using point "." as the decimal symbol.
-
-### Bugs
-
-Please report any bugs to the helpdesk (email to energyplus-support@gard.com) so that we can fix them prior to the next release.
-
-Manipulating Output Files
-=========================
-
-EP-Compare
-----------
-
-The EP-Compare program is intended to be used to compare the tabular results of several simulations including the ABUPS summary report. To generate tabular reports in EnergyPlus use the Output:Table:SummaryReports object and make sure the OutputControl:Table:Style includes HTML output. EP-Compare displays bar graphs and monthly line graphs for most of the tabular reports. It can be used in Windows, Linux and Macintosh systems. The main screen is shown below:
-
-![](media/image122.png)
-
-Figure 56. EP-Compare Main Screen
-
-The main screen shows both the graph being displayed at the bottom and allows the user to select a graph from a list at the top. The list of graphs is based on each table name and subtable name and then has a list of graphs supported including stacked bars, simple bar, 100% stacked bars, side-by-side bars, and monthly line graphs. The program window can be resized.
-
-The first time the program is started no graphs are shown because no files have been selected. To select files use the "Manage Files" button. This brings up the Manage Files dialog box shown below:
-
-![](media/image123.png)
-
-Figure 57. EP-Compare Dialog box
-
-This dialog lets you add and remove files from the list of files. The files selected should be HTML or HTM files that are produced by EnergyPlus when using the Output:Table:SummaryReports object with OutputControl:Table:Style set to produce HTML files. It is best to compare files that have similar reports otherwise missing values will be shown as zeros.The dialog also provides a button to add entire directories of files but that adding too many files makes the graphs difficult to understand. To change the order that files appear in the graph, the files can be dragged up and down the list of files in the Manage Files dialog. The dialog box window can be resized to view longer files names if necessary.
-
-When EP-Compare is started again, the files last selected are shown in the graph if they are still available.
-
-The Copy button allows the current graph (as it is sized in the window) to be copied to another application such as Microsoft Word or PowerPoint. To paste a copied image to those programs use the Paste Special option and select one of the bitmap formats.
-
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-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Application Guide for EMS</h1>
-<h2>Energy Management System User Guide</h2>
-<br/>
-<p><i>(a.k.a. The Book of Erl)</i></p>
-<br/>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-
-Introduction
-============
-
-This document provides an in-depth look at the Energy Management System (EMS) feature in EnergyPlus and provides a way to develop custom control and modeling routines for EnergyPlus models. EMS is an advanced feature of EnergyPlus and is not for beginners. You will need to write your own custom computer programs and have a thorough understanding of how you want your models to behave. If you are intimidated by the idea of writing computer programs to adjust the fine details of how an EnergyPlus model runs, be aware that EMS is not for all (or even most) users. However, if you relish the idea of being able to write small computer programs that override some annoying behavior, you may find that writing Erl programs can solve many problems faced by energy modelers. EMS is a complicated feature  and this application guide augments the Input/Output Reference by providing an overall discussion of how to use EMS.
-
-EMS provides high-level, supervisory control to override selected aspects of EnergyPlus modeling. A small programming language called EnergyPlus Runtime Language (Erl) is used to describe the control algorithms. EnergyPlus interprets and executes your Erl program as the model is being run. This guide serves as a programming manual for Erl and attempts to show you how to customize your EnergyPlus simulations.
-
-Background
-----------
-
-We used the operations manual for a common commercial brand of EMS to guide the initial formulation of Erl. The circa 2000 EMS language from a major manufacturer is a good example because it uses a full-featured EMS language and does not rely on a graphical user interface.
-
-Organization
-------------
-
-We first describe Erl, then discuss its rules and features, including syntax for writing statements, variables, expressions, and built-in functions. We then discuss sensors, actuators, and calling points for the EMS. Then we describe a set of examples applications for EMS. The last section provides information about debugging Erl programs.
-
-EnergyPlus Runtime Language
-===========================
-
-Erl is the simplified programming language used to define the EMS control and modeling programs. This section describes the rules and syntax for using Erl to write programs.
-
-Statement Keywords
-------------------
-
-Every programming language has instructions or commands that tell the processor what to do. Erl supports a few types of program statements. Each line of an Erl program begins with a statement keyword. The syntax for each line depends on the keyword that starts that line. Only those listed in Table 1 are allowed.
-
-<table class="table table-striped">
-<tr>
- <th>Keyword</th>
- <th>Syntax</th>
- <th>Statement Description</th>
-</tr>
-<tr>
- <td>RUN</td>
- <td>RUN &lt;program name&gt;</td>
- <td>Calls another Erl program or subroutine. Returns to the calling point when completed. Recursive calling is allowed.</td>
-</tr>
-<tr>
- <td>RETURN</td>
- <td>RETURN,</td>
- <td>Prematurely exits a subroutine or program and returns control to the caller.</td>
-</tr>
-<tr>
- <td>SET</td>
- <td>SET &lt;variable&gt; = &lt;expression&gt;,</td>
- <td>Assigns the right-hand side to the left-hand side. If <variable> has not been used before, it is dynamically declared (with local scope). **Note: &lt;variables&gt; should NOT start with numerics.**</td>
-</tr>
-<tr>
- <td>IF</td>
- <td>IF &lt;expression&gt;,</td>
- <td>Begins an “IF block.� Conditional decision. If &lt;expression&gt; evaluates to anything other than zero, the block of statements after the IF is executed.</td>
-</tr>
-<tr>
- <td>ELSEIF</td>
- <td>ELSEIF &lt;expression&gt;</td>
- <td>Conditional decision that follows a regular IF block of instructions. If &lt;expression&gt; evaluates to anything other than zero, the block of instructions after the ELSEIF is executed.</td>
-</tr>
-<tr>
- <td>ELSE</td>
- <td>ELSE,</td>
- <td>Conditional decision. Associated with an IF statement, the block of statements after the ELSE is executed if &lt;expression&gt; evaluates to zero for preceding IF and ELSEIF statements.</td>
-</tr>
-<tr>
- <td>ENDIF</td>
- <td>ENDIF,</td>
- <td>Terminates IF block (required).</td>
-</tr>
-<tr>
- <td>WHILE</td>
- <td>WHILE &lt;expression&gt;</td>
- <td>Begins a “WHILE block.�  Conditional decision.  If &lt;expression&gt; evaluates to anything other than zero, the block of statements after the WHILE is repeatedly executed.</td>
-</tr>
-<tr>
- <td>ENDWHILE</td>
- <td>ENDWHILE,</td>
- <td>Terminates WHILE block (required).</td>
-</tr>
-</table>
-
-### Rules for IF blocks:
-
-- IF blocks can be nested, but only up to five deep.
-
-- ELSE is optional. If omitted, the IF block is terminated by ENDIF.
-
-IF-ELSEIF-ELSE-ENDIF blocks are allowed. If there are many ELSEIF statements, the first in the list that evaluates to true (1.0) is applied and the execution jumps to the ENDIF for that IF block. If no IF or ELSEIF is true, the ELSE condition (if any) is applied. A single IF block currently has a limit of 199 ELSEIF statements plus one ELSE statement.
-
-### Rules for WHILE blocks:
-
-- WHILE blocks cannot be nested.
-
-- A WHILE block must be terminated by an ENDWHILE
-
-- The block is repeated until the expression following the WHILE statement evaluates to 0.0 (false).
-
-- Once the WHILE loop is entered, there is a maximum limit on the number of times the loop can be repeated. The limit is set at one million repetitions to protect against the possibility of an Erl program entering an infinite loop if the WHILE loop’s expression is malformed so as to never evaluate to 0.0 (false).
-
-Erl programs are entered into the input data file (IDF) using the input objects called EnergyManagementSystem:Program and EnergyManagementSystem:Subroutine. These objects use individual fields to store the statements for an Erl program. As with most EnergyPlus objects, each field is separated by a comma and typically given a separate line of text for readability. In this case, each field can be considered a separate line of Erl program code. Every input field (line of code) must conform to the following rules:
-
-- Every input field contains only one statement.
-
-- Every field begins with a statement keyword that identifies what that particular line of code is doing.
-
-- The syntax for each statement depends on the keyword.
-
-- All field content (keywords, variable names, etc.) is case insensitive.
-
-- A comma (or semicolon if it is the last field) marks the end of every statement.
-
-- The maximum length for a field is 100 characters. If you enter a longer field, it will be truncated to the first 100 characters. This can have subtle effects if the remaining portion forms a viable expression.
-
-- The “!� character is for comments.
-
-REMEMBER, every line needs to end in a comma or, if it is the last in the program, a semicolon.
-
-Variables
----------
-
-Variables are important to any programming language. All Erl variables, except trend variables, are treated the same way in Erl and can be used interchangeably with any instruction.
-
-The rules for selecting names of EMS variables are:
-
-- No spaces are allowed in user-defined variable names.
-
-- Underscore (“\_�) is the only special character allowed in variable names.
-
-- Variable names are **not** case sensitive.
-
-- Names of variables with global scope must be unique.
-
-- Variables cannot be declared with the same name as a built-in variable.
-
-- Variables can be alpha numeric strings but should NOT start with a numeric.
-
-The rules for using EMS variables are:
-
-- All numeric variables are treated as floating point numbers. You use the underlying Fortran language features to handle these as double precision real numbers.
-
-- You can use the SET statement to reassign sensor variables and built-in variables.
-
-- Actuator variables use SET to perform control actions.
-
-EMS variables can have either local or global scope. Global scope means that the variables can be used across Erl programs and always refer to the same instance of a particular variable. Global variables must have unique names. Local scope means that variables can be used only within a given Erl program.
-
-Erl programs have eight types of variables:
-
-- Sensor. Each EnergyManagementSystem:Sensor input object declares a user-defined variable and maps it to a variable elsewhere in EnergyPlus (via output variables). Variables so declared have global scope and are used to *get* time-varying input data from elsewhere in the EnergyPlus model.
-
-- Actuator. Each EnergyManagementSystem:Actuator input object declares a user-defined Erl variable and maps it to a variable elsewhere in EnergyPlus. Variables so declared have global scope and are used to *set* control results elsewhere in the EnergyPlus model.
-
-- Local. Local variables do not need to be explicitly declared. These undeclared variables will be automatically registered as EMS variables with local scope. This allows you to create new variables “on the fly.�  Local variables can be used for temporary storage of intermediate results.
-
-- Global. EnergyManagementSystem:GlobalVariable input objects are used to declare variables with a user-defined name and global scope. Global variables can be used to store intermediate results that span across Erl programs. Because the Erl compiler does not support functions or argument passing, global variables have an important role in using subroutines. These variables are global only within Erl and not with respect to code elsewhere in EnergyPlus.
-
-- Built-in. The EMS system automatically declares a set of built-in variables with predefined names. These variables have global scope. The built-in variables are always created and cannot be eliminated.
-
-- Internal. Each EnergyManagementSystem:InternalVariable input object declares a user-defined Erl variable and maps it to a variable elsewhere in EnergyPlus. Variables so declared have global scope and are used to *get* static input data from elsewhere in EnergyPlus.
-
-- Trend. Each EnergyManagementSystem:TrendVariable input object declares a user-defined Erl trend variable and maps it to a global Erl variable for logging. Trend variables are used to store the history of Erl variables. Trend variables differ from other Erl variables in that they can be put to use only through the built-in trend functions (see Table 6).
-
-- Index. Each EnergyManagementSystem:CurveOrTableIndexVariable and/or EnergyManagementSystem:ConstructionIndexVariable declares a user defined Erl variable and maps it to a specific item in the IDF of indicated type.
-
-Built-in variables, internal variables, and sensor variables are primarily used to *get* information about the state of the simulation. However, because all variables are treated alike, built-in variables and sensor variables can also be overwritten by the SET instruction. (This applies within the EMS only; the variables in the rest of EnergyPlus program will not be overwritten.)  This allows you to reassign constants such as “on� and “off� as well as the values of the other built-in variables and sensor variables. There is really no problem with this, as long as you know what you are doing. One possible application is to reset a sensor variable that references the outdoor drybulb temperature so it contains the temperature in degrees Fahrenheit instead of Celsius. Regardless of reassignment, sensor variables and the dynamic built-in variables (e.g., date and time) will be cleared and updated with the latest values from EnergyPlus at the next timestep. Resetting a sensor variable does not have a retroactive effect on the report variable to which it is mapped.
-
-The actuator variable is the counterpart of the sensor variable. Sensor variables are used to *get* the state of building systems; actuator variables are used to *set* the state of building systems. When used with actuator variables, the SET instruction performs control actions on the object to which it maps.
-
-### Built-In Variables
-
-A set of built-in variables provides date, time, and weather information that is not available via standard report variables, as well as several handy constant variables such as “true,� “false,� “on,� and “off.� Several variables provide access to the time and date information during the course of a simulation.  The CurrentTime, Hour and Minute variables represent the point in time at end of the timestep currently being simulated. EnergyPlus primarily operates in standard time and these clock values are not adjusted for daylight savings time.  The built-in variable DaylightSavings time is available for use with the daylight savings time adjustment feature (see RunPeriodControl:DaylightSavingTime). The duration of simulation timesteps are available in the variables ZoneTimeStep and SystemTimeStep.  The status of whether or not the simulation is currently during the initial warmup days is available in the variable WarmupFlag.
-
-Table 2 lists the built-in variables that are always available for use in Erl programs.
-
-Table 2. Built-In Unique Variables for Erl
-
-<table class="table table-striped">
-<tr>
-<th>Variable Name</th>
-<th>Value</th>
-</tr>
-<tr>
-<td>Year</td>
-<td>1900–2100</td>
-</tr>
-<tr>
-<td>Month</td>
-<td>1–12</td>
-</tr>
-<tr>
-<td>DayOfMonth</td>
-<td>1–31</td>
-</tr>
-<tr>
-<td>DayOfWeek</td>
-<td>1–7 (1 = Sun, 2 = Mon, …)</td>
-</tr>
-<tr>
-<td>DayOfYear</td>
-<td>1–365</td>
-</tr>
-<tr>
-<td>Holiday</td>
-<td>0 if not. 1.0, 2.0, etc., for each type of holiday in model</td>
-</tr>
-<tr>
-<td>DaylightSavings</td>
-<td>0 or 1, 0 if not daylight savings time, 1 if daylight savings time</td>
-</tr>
-<tr>
-<td>CurrentTime</td>
-<td>0.0-24.0, (fractional hours)</td>
-</tr>
-<tr>
-<td>Hour</td>
-<td>0–23 (whole hours only)</td>
-</tr>
-<tr>
-<td>Minute</td>
-<td>1.0–60.0 (fractional minutes)</td>
-</tr>
-<tr>
-<td>True</td>
-<td>1.0</td>
-</tr>
-<tr>
-<td>False</td>
-<td>0.0</td>
-</tr>
-<tr>
-<td>On</td>
-<td>1.0</td>
-</tr>
-<tr>
-<td>Off</td>
-<td>0.0</td>
-</tr>
-<tr>
-<td>PI</td>
-<td>3.14159265358979</td>
-</tr>
-<tr>
-<td>SunIsUp</td>
-<td>0 (= no) or 1 (= yes)</td>
-</tr>
-<tr>
-<td>IsRaining</td>
-<td>0 (= no) or 1 (= yes)</td>
-</tr>
-<tr>
-<td>ZoneTimeStep</td>
-<td>Durating of the zone timestep in hours</td>
-</tr>
-<tr>
-<td>SystemTimeStep</td>
-<td>Current duration of the system timestep in hours</td>
-</tr>
-<tr>
-<td>CurrentEnvironment</td>
-<td>Integer index for the current environment period (sizing periods and run periods accumulate throughout the run)</td>
-</tr>
-<tr>
-<td>Null</td>
-<td>Special structure that stops an actuator from overriding control</td>
-</tr>
-<tr>
-<td>ActualDateAndTime</td>
-<td>A simple sum of the values of the date/time function. Could be used in random seeding.</td>
-</tr>
-<tr>
-<td>ActualTime</td>
-<td>A simple sum of the values of the time part of the date/time function. Could be used in random seeding.</td>
-</tr>
-<tr>
-<td>WarmupFlag</td>
-<td>0 (= not during warmup) or 1 (= during warmup)</tr>
-</table>
-
-### Trend Variables
-
-Trend variables are used to log data over time. They hold the history of Erl variables from previous zone timesteps. You create trend variables with an EnergyManagementSystem:TrendVariable input object,  each of which declares a user-defined Erl trend variable and maps it to a global Erl variable for logging.
-
-Trend variables are also used to store the history of Erl variables. The trend input includes the number of timesteps that are to be logged. The logging of data is first-in-first-out, meaning that the oldest data are pushed out the back of the log to make room for the most recent data. The zone timestep is used as the (constant) increment of time between different elements in the log and this value, in fractional hours, is available in the ZoneTimeStep built-in variable.
-
-Trend variables differ from other Erl variables in that they can be used only through the built-in trend functions (see Table 6). Trend functions provide a number of ways to analyze trend data and extract data from the log. There are functions to obtain the maximum, minimum, average, and sum of logged data. There is a function to obtain the rate of change in the data. All the trend functions include an argument for a log index. This index tells the function how far back in time to go when evaluating.
-
-Expressions
------------
-
-An expression is a sequence of variables and/or constants linked together by operators. An expression is always evaluated to a single value.
-
-The rules for expressions are:
-
-- An expression is a sequence of variables and/or constants linked by operators.
-
-- Expressions always evaluate to a single value.
-
-- Comparison operators evaluate to 1.0 for “true� or 0.0 for “false.�
-
-- Compound expressions are allowed and can be organized with parentheses.
-
-The operators shown in Table 3 are available for use in Erl programs.
-
-Table 3. Operators for Erl
-
-<table class="table table-striped">
-<tr>
-<th>Operator Symbol</th>
-<th>Description</th>
-<th>Evaluation Order</th>
-<th>Example</th>
-</tr>
-<tr>
-<td>( )</td>
-<td>Parentheses</td>
-<td>left-to-right</td>
-<td>SET z = 23/(3 + 2)</td>
-</tr>
-<tr>
-<td>+</td>
-<td>Addition</td>
-<td>right-to-left</td>
-<td>SET a = 4 + 5</td>
-</tr>
-<tr>
-<td>-</td>
-<td>Subtraction</td>
-<td>right-to-left</td>
-<td>SET b = a - 3</td>
-</tr>
-<tr>
-<td>*</td>
-<td>Multiplication</td>
-<td>right-to-left</td>
-<td>SET c = a * b</td>
-</tr>
-<tr>
-<td>/</td>
-<td>Division</td>
-<td>left-to-right</td>
-<td>SET d = b/a</td>
-</tr>
-<tr>
-<td>^</td>
-<td>Raise to a power</td>
-<td>left-to-right</td>
-<td>SET e = c ^ 0.5</td>
-</tr>
-<tr>
-<td>==</td>
-<td>Equality comparison</td>
-<td>left-to-right</td>
-<td>IF a == b</td>
-</tr>
-<tr>
-<td>&lt;&gt; </td>
-<td>Inequality comparison</td>
-<td>left-to-right</td>
-<td>IF c &lt;&gt; d</td>
-</tr>
-<tr>
-<td>&gt; </td>
-<td>Greater than comparison</td>
-<td>left-to-right</td>
-<td>IF a &gt; e</td>
-</tr>
-<tr>
-<td>&gt;=</td>
-<td>Greater than or equal to comparison</td>
-<td>left-to-right</td>
-<td>IF a &gt;= 6</td>
-</tr>
-<tr>
-<td>&lt; </td>
-<td>Less than comparison</td>
-<td>left-to-right</td>
-<td>IF b &lt; 2</td>
-</tr>
-<tr>
-<td>&lt;=</td>
-<td>Less than or equal to comparison</td>
-<td>left-to-right</td>
-<td>IF b &lt;= f</td>
-</tr>
-<tr>
-<td>&amp;&amp;</td>
-<td>Logical AND</td>
-<td>right-to-left</td>
-<td>IF c &amp;&amp; d</td>
-</tr>
-<tr>
-<td>||</td>
-<td>Logical OR</td>
-<td>right-to-left</td>
-<td>IF c || d</td>
-</tr>
-</table>
-
-
-
-Because expressions can be evaluated to a single value, they can be used in SET and IF statements. That means both of the following instructions are allowed:
-
-```
-SET a = c < d
-IF a - 1
-```
-
-In the case of the SET example, the value of “a� is set to 1 if “c� is less than “d�; otherwise, it is set to 0. For the IF example, the IF block of instructions are executed if a – 1 is greater than zero.
-
-Compound expressions allow multiple operators to be sequenced or nested. For example:
-
-```
-a + b \* 7 / 4.5
-(a \* 3 + 4) ^ 2
-(a > b) && (c < d)
-```
-
-For complicated expressions, it helps to make heavy use of parentheses in your equations.  By using parentheses with proper algebraic evaluation in mind to group terms, you can help the Erl parser.  The language processor is simplistic compared to a full-blown programming language and sometimes has problems applying the rules of algebra.  It is safer to err on the side of extra parentheses and to inspect the results of complex expressions in the EDD output.
-
-Built-In Functions
-------------------
-
-Several useful, built-in functions are available for use in Erl programs. You cannot configure these; they are internal to the language processor inside EnergyPlus. They provide access to a subset of general service routines that are useful inside the main EnergyPlus program or are intrinsic functions available in the underlying Fortran language. The “@� character is used to signal to the language processor that the following character string defines a built-in function that is used to assign a result to an Erl variable. The characters appended to the “@� operator must be one of the predefined names listed in Table 4, Table 5, Table 6, or Table 7. The syntax of the function call will vary depending on the arguments required by the function, but the general structure is:
-
-SET &lt;variable&gt; = @&lt;function name&gt;  &lt;argument1&gt;  &lt;argument2&gt;   …   &lt;argumentN&gt;
-
-Where “argument� can be either an Erl variable or a numeric constant.
-
-For example, the following two statements can be used to set the value of an Erl variable called mySupplyRH to have percent relative humidity.
-
-SET mySupplyRH = @RhFnTdbWPb mySupplyDryblub mySupplyHumRat mySupplyPress
-
-SET mySupplyRH = mySupplyRH \* 100
-
-### Built-in Math Functions
-
-Table 4 lists the built-in functions for common mathematical functions. The numerical model for these functions is provided by the underlying Fortran language and the compiler.
-
-Table 4. Built-in Math Functions for Erl
-
-<table class="table table-striped">
-<tr>
-<th>Function Name</th>
-<th>Description</th>
-<th>Number of Arguments</th>
-</tr>
-<tr>
-<td>@Round</td>
-<td>Decreases precision of real number argument to nearest whole number, remains a real number.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@Mod</td>
-<td>Returns remainder after dividing the first argument by the second.</td>
-<td>2</td>
-</tr>
-<tr>
-<td>@Sin</td>
-<td>Sine, returns sine of angle given in radians.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@Cos</td>
-<td>Cosine, returns cosine of angle given in radians.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@ArcSin</td>
-<td>Arcsine, returns angle in radians from sine of angle.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@ArcCos</td>
-<td>ArcCosine, returns angle in radians from cosine of angle.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@DegToRad</td>
-<td>Degrees to radians, returns radians from degrees.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@RadToDeg</td>
-<td>Radians to degrees, returns degrees from radians.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@Exp</td>
-<td>Exponential, e<sup>x</sup>, returns result.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@Ln</td>
-<td>Natural log, log<sub>e</sub>(x), returns result.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@Max</td>
-<td>Maximum, returns largest value of two arguments.</td>
-<td>2</td>
-</tr>
-<tr>
-<td>@Min</td>
-<td>Minimum, returns smallest value of two arguments.</td>
-<td>2</td>
-</tr>
-<tr>
-<td>@Abs</td>
-<td>Absolute value, returns positive magnitude of argument.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@RandomUniform</td>
-<td>Pseudo-Random Number Generator, returns random number with uniform probability distribution across the range of values passed as the arguments, inclusive. Argument 1 is the lower limit. Argument 2 is the upper limit.</td>
-<td>2</td>
-</tr>
-<tr>
-<td>@RandomNormal</td>
-<td>Pseudo-Random Number Generator, returns random number with normal (Gaussian) probability distribution as a function of the mean, standard deviation, and limits. Argument 1 is the mean. Argument 2 is the standard deviation. Argument 3 is the lower limit. Argument 4 is the upper limit.</td>
-<td>4</td>
-</tr>
-<tr>
-<td>@SeedRandom</td>
-<td>Random Seed, controls the seed used in the random number generator for calls to @RandomUniform and @RandomNormal.  Use is optional and provided for repeatable series of random numbers. The argument is rounded to the nearest whole number and then used to set the size and values of the seed for the number generator. </td>
-<td>1</td>
-</tr>
-</table>
-
-
-
-### Built-In Simulation Management Functions
-
-Table 5. Built-in EnergyPlus Simulation Management Functions for Erl
-
-<table class="table table-striped">
-<tr>
-<th>Function Name</th>
-<th>Description</th>
-<th>Number of Arguments</th>
-</tr>
-<tr>
-<td>@FatalHaltEp</td>
-<td>Throws fatal error with time of occurrence and stops execution of current model. Argument passes a number that can be used as an error code.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@SevereWarnEp</td>
-<td>Throws severe error with time of occurrence and continues execution. Argument passes a number that can be used as an error code.</td>
-<td>1</td>
-</tr>
-<tr>
-<td>@WarnEp</td>
-<td>Throws warning error and continues execution. Argument passes a number that can be used as an error code.</td>
-<td>1</td>
-</tr>
-</table>
-
-### Built-in Trend Variable Functions
-
-For control algorithms, you often need to be able put a sensor reading into some historical context. The trend variables are provided in Erl as a way to log the time history of data to use in control decisions. To use the trend variables in Erl programs, their values must be extracted and placed into normal Erl variables. Setting up an Erl variable as a trend variable requires an EnergyManagementSystem:TrendVariable input object. The access functions listed in Table 6 are used to obtain data from a trend variable during the execution of an Erl program. These functions act on trend variables and return values into the user’s Erl variables for subsequent use in calculations. Each trend function takes the name of the trend variable and an index that identifies how far back in time the function should be applied. Trend variable names are also Erl variables but with special pointers to another data structure with the time series data storage. The trend logs have a first-in, first-out storage array where only the most recent data are retained. Each element in the history corresponds to the result for that value over a zone timestep. The time difference between trend log items is the zone timestep in hours, so that the slope returned by @TrendDirection is in per-hour units.
-
-Table 6. Built-in Functions for Trend Variables in Erl
-
-<table class="table table-striped">
-<tr>
-<th>Function Name</th>
-<th>Description</th>
-<th>Number of Arguments</th>
-</tr>
-<tr>
-<td>@TrendValue</td>
-<td>Returns history value for a particular number of timesteps into the past. Dereferences data stored in trend into another Erl variable. Takes trend variable name and the specific timestep into the past to return.</td>
-<td>2</td>
-</tr>
-<tr>
-<td>@TrendAverage</td>
-<td>Returns historical average (mean) for values in trend variable. Takes trend variable name and number of steps into the past to analyze</td>
-<td>2</td>
-</tr>
-<tr>
-<td>@TrendMax</td>
-<td>Returns historical maximum for values in trend variable. Takes trend variable name and number of steps into the past to analyze.</td>
-<td>2</td>
-</tr>
-<tr>
-<td>@TrendMin</td>
-<td>Returns historical minimum for values in trend variable within the index. Takes trend variable name and number of steps into the past to analyze.</td>
-<td>2</td>
-</tr>
-<tr>
-<td>@TrendDirection</td>
-<td>Returns slope of a linear least squares fit of trend data within the index. Positive if trend is increasing, negative if decreasing. Takes trend variable name and number of steps into the past to analyze.</td>
-<td>2</td>
-</tr>
-<tr>
-<td>@TrendSum</td>
-<td>Returns sum of elements stored in trend. Takes trend variable name and number of steps into the past to analyze.</td>
-<td>2</td>
-</tr>
-</table>
-
-The trend functions all take as their second argument an array index. This number should be considered an integer for locating an array position. (It will be rounded down to the nearest integer using Fortran’s FLOOR intrinsic.)  This index argument tells the trend functions how far back in time they should reach into the history log when they evaluate the function call. This enables you to compare long- and short-range trends.
-
-### Built-in Psychrometric Functions
-
-Building modeling often involves calculations related to moist air. A comprehensive set of built-in functions is available for psychrometric calculations. Table 7 lists the functions available for use in Erl programs that are related to moist air properties and some physical properties related to water. More discussion of the psychrometric functions is provided in the section “Pyschrometric services� in the Module Developer Guide.
-
-Table 7. Built-in Psychrometric Functions for Erl
-
-<table class="table table-striped">
-  <tr>
-    <th>Function Name</th>
-    <th>Arguments</th>
-    <th>Description</th>
-    <th>Units</th>
-  </tr>
-  <tr>
-    <td rowspan="4">@RhoAirFnPbTdbW</td>
-    <td>Result</td>
-    <td>Density of moist air</td>
-    <td>kg/m&lt;sup&gt;3&lt;/sup&gt;</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 3</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@CpAirFnWTdb</td>
-    <td>Result</td>
-    <td>Heat capacity of moist air</td>
-    <td>J/kg-&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@HfgAirFnWTdb`</td>
-    <td>Result</td>
-    <td>Heat of vaporization for vapor</td>
-    <td>J/kg</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@HgAirFnWTdb</td>
-    <td>Result</td>
-    <td>Enthalpy of the gas</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td rowspan="4">@TdpFnTdbTwbPb</td>
-    <td>Result</td>
-    <td>Dew-point temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Wetbulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 3</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@TdpFnWPb</td>
-    <td>Result</td>
-    <td>Dew-point temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@HFnTdbW</td>
-    <td>Result</td>
-    <td>Enthalpy of moist air</td>
-    <td>J/kg</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td rowspan="4">@HFnTdbRhPb</td>
-    <td>Result</td>
-    <td>Enthalpy of moist air</td>
-    <td>J/kg</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Relative humidity</td>
-    <td>Fraction (0.0 .. 1)</td>
-  </tr>
-  <tr>
-    <td>Input 3</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@TdbFnHW</td>
-    <td>Result</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Enthalpy of moist air</td>
-    <td>J/kg</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@RhovFnTdbRh</td>
-    <td>Result</td>
-    <td>Vapor density in air</td>
-    <td>kg/m&lt;sup&gt;3&lt;/sup&gt;</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Relative humidity</td>
-    <td>Fraction (0.0 .. 1)</td>
-  </tr>
-  <tr>
-    <td rowspan="4">@RhovFnTdbWPb</td>
-    <td>Result</td>
-    <td>Vapor density in air</td>
-    <td>kg/m&lt;sup&gt;3&lt;/sup&gt;</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 3</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@RhFnTdbRhov</td>
-    <td>Result</td>
-    <td>Relative humidity</td>
-    <td>Fraction (0.0 .. 1)</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Vapor density in air</td>
-    <td>kg/m&lt;sup&gt;3&lt;/sup&gt;</td>
-  </tr>
-  <tr>
-    <td rowspan="4">@RhFnTdbWPb</td>
-    <td>Result</td>
-    <td>Relative humidity</td>
-    <td>Fraction (0.0 .. 1)</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 3</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="4">@TwbFnTdbWPb</td>
-    <td>Result</td>
-    <td>Wetbulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 3</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="4">@VFnTdbWPb</td>
-    <td>Result</td>
-    <td>Specific volume</td>
-    <td>m&lt;sup&gt;3&lt;/sup&gt;/kg</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 3</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@WFnTdpPb</td>
-    <td>Result</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Dew-point temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@WFnTdbH</td>
-    <td>Result</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Enthalpy of moist air</td>
-    <td>J/kg</td>
-  </tr>
-  <tr>
-    <td rowspan="4">@WFnTdbTwbPb</td>
-    <td>Result</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Wetbulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 3</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="4">@WFnTdbRhPb</td>
-    <td>Result</td>
-    <td>Humidity ratio</td>
-    <td>kgWater/kgDryAir</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Relative humidity</td>
-    <td>Fraction (0.0 .. 1)</td>
-  </tr>
-  <tr>
-    <td>Input 3</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="2">@PsatFnTemp</td>
-    <td>Result</td>
-    <td>Saturation pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Drybulb temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td rowspan="3">@TsatFnHPb</td>
-    <td>Result</td>
-    <td>Saturation temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Enthalpy of moist air</td>
-    <td>J/kg</td>
-  </tr>
-  <tr>
-    <td>Input 2</td>
-    <td>Barometric pressure</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td rowspan="2">@CpCW</td>
-    <td>Result</td>
-    <td>Heat capacity of water</td>
-    <td>J/kg</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td rowspan="2">@CpHW</td>
-    <td>Result</td>
-    <td>Heat capacity of water</td>
-    <td>J/kg</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-  <tr>
-    <td rowspan="2">@RhoH2O</td>
-    <td>Result</td>
-    <td>Density of water</td>
-    <td>kg/m&lt;sup&gt;3&lt;/sup&gt;</td>
-  </tr>
-  <tr>
-    <td>Input 1</td>
-    <td>Temperature</td>
-    <td>&amp;deg;C</td>
-  </tr>
-</table>
-
-
-### Built-in Curve and Table Functions
-
-EnergyPlus has a number of different generic curve and table input objects that are used to describe the performance characteristics for various component models.  Table 8 describes a built-in function called @CurveValue that is available for reusing those curve and table input objects in your Erl programs.  Although the Erl language could be used to replicate the functionality, reusing those input objects can have advantages because the input may have already been developed for use in traditional component models or the limiting and interpolation methods are helpful.  The @CurveValue function expects six arguments, although usually only a subset of them will be used depending on the number of independent variables involved with the curve or table.  Because Erl does not support passing optional arguments, dummy variables do need to be included in the function call for all unused independent variables.  For example, the Curve:Biquadratric object has only x and y independent variables, so input arguments 4, 5, and 6 will not be used when @CurveValue is evaluated:
-
-      Set MyCurveResult = @CurveValue myCurveIndex X1 Y1 dummy dummy dummy;
-
-The first input argument is always an Erl variable that has been declared using an EnergyManagementSystem:CurveOrTableIndexVariable input object.  This variable identifies the location of a specific curve or table in the program’s internal data structures.  It is important that you do not inadvertently reassign the value held in this variable because it is only filled once at the beginning of the simulation.
-
-
-
-Table 8. Built-in Function for Accessing Curves and Tables
-
-<table class="table table-striped">
-<tr>
- <th>Function Name</th>
- <th>Arguments</th>
- <th>Description</th>
- <th>Notes</th>
-</tr>
-<tr>
- <td rowspan="7">@CurveValue</td>
- <td>Result</td>
- <td>Result from evaluating the curve or table as a function of the input arguments</td>
- <td></td>
-</tr>
-<tr>
- <td>Input 1</td>
- <td>Index variable that "points" to a specific curve or table object defined elsewhere in the IDF.</td>
- <td>This variable needs to be declared and filled using an EnergyManagementSystem:CurveOrTableIndexVariable object.</td>
-</tr>
-<tr>
- <td>Input 2</td>
- <td>First independent variable</td>
- <td>Typically the "X" input value, always used</td>
-</tr>
-<tr>
- <td>Input 3</td>
- <td>Second independent variable</td>
- <td>Typically the "Y" value, only used if curve/table has two or more independent variables</td>
-</tr>
-<tr>
- <td>Input 4</td>
- <td>Third independent variable</td>
- <td>Typically the "Z" value, only used if curve/table has three or more independent variables.</td>
-</tr>
-<tr>
- <td>Input 5</td>
- <td>Fourth independent variable</td>
- <td>Only used if table has four or more independent variables</td>
-</tr>
-<tr>
- <td>Input 6</td>
- <td>Fifth independent variable</td>
- <td>Only used if table has five independent variables</td>
-</tr>
-</table>
-
-Internal Variables
-==================
-
-Internal variables form a category of built-in data accessible for EMS. They are internal in that they access information about the input file from inside EnergyPlus. You should already have access to the information contained in these because they depend on other content in the IDF. However, it would be inconvenient to always have to coordinate changes between Erl programs and the rest of the IDF. Internal variables simplify the process of keeping an Erl program in sync with other changes to the model. These differ from the built-in variables in that they may or may not be created in every simulation and have user-defined names that distinguish among different instances of the same type of data. The internal variables differ from sensors in that they are usually static values that do not change over time. The constants might vary from run to run but never within a single run period. Internal variables are read only.
-
-Internal variables are automatically made available whenever an input file includes basic EMS input objects and the model they are associated with is included in the input file. To use an internal variable in an Erl program, you must declare it with an EnergyManagementSystem:InternalVariable input object. This object assigns a specified Erl variable name to contain the value in an internal EnergyPlus data structure. The EDD file lists the specific internal variable types, their unique identifying names, and the units. The rest of this section provides information about specific internal variables.
-
-Zone Geometry
--------------
-
-The internal variables called “Zone Air Volume� and “Zone Floor Area� provide basic geometric information about each zone. EnergyPlus calculates these from the geometry in the IDF, or you may input the zone air volume in the zone input object. These internal variables in Erl programming should be useful during a parametric study where the shape of the building is being varied, as for a massing study. For example, you could use the zone floor area to normalize Erl calculations with a per-unit area. Or you could use the zone air volume to convert between air flows in m<sup>3</sup>/s to air changes per hour (ACH).
-
-The internal variables called “Zone Multiplier� and “Zone List Multiplier� indicate the multipliers assigned to zones.  These can be useful for customizing sizing calculations.
-
-Internal Gains
---------------
-
-A number of internal variables describe design levels for the various types of internal gains.
-
-### People Count Design Level
-
-The internal variable “People Count Design Level� provides information about the maximum number of people associated with each people input object. The units are number of people. This is the value entered in, or resulting from intermediate calculations using, the inputs in the People object. This variable is useful for scaling the values assigned to the “Number of People� control in the “People� EMS actuator.
-
-### Lighting Power Design Level
-
-The internal variable “Lighting Power Design Level� provides information about the maximum lighting electrical power level associated with each Lights input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the lights object. This variable is useful for scaling the values assigned to the “Electric Power Level control in the “Lights� EMS actuator.
-
-### Plug and Process Power Design Level
-
-The internal variable “Plug and Process Power Design Level� provides information about the maximum electrical equipment power level associated with each ElectricEquipment input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the ElectricEquipment object. This variable is useful for scaling the values assigned to the “Electric Power Level� control in the “ElectricEquipment� EMS actuator.
-
-### Gas Process Power Design Level
-
-The internal variable “Gas Process Power Design Level� provides information about the maximum gas equipment power level associated with each GasEquipment input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the GasEquipment object. This variable is useful for scaling the values assigned to the “Gas Power Level� control in the “GasEquipment� EMS actuator.
-
-### Process District Heat Design Level
-
-The internal variable “Process District Heat Design Level� provides information about the maximum district heating power level associated with each HotWaterEquipment input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the HotWaterEquipment object. This variable is useful for scaling the values assigned to the “District Heating Power Level� control in the “HotWaterEquipment� EMS actuator.
-
-### Process Steam District Heat Design Level
-
-The internal variable “Process Steam District Heat Design Level� provides information about the maximum district heating power level associated with each SteamEquipment input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the SteamEquipment object. This variable is useful for scaling the values assigned to the “District Heating Power Level� control in the “SteamEquipment� EMS actuator.
-
-### Other Equipment Design Level
-
-The internal variable “Other Equipment Design Level� provides information about the maximum power level associated with each OtherEquipment input object. The units are Watts. This is the value entered in, or resulting from intermediate calculations using, the inputs in the OtherEquipment object. This variable is useful for scaling the values assigned to the “Power Level� control in the “OtherEquipment� EMS actuator.
-
-### Simple Zone Baseboard Capacity
-
-The internal variables called “Simple Zone Baseboard Capacity At Low Temperature� and “Simple Zone Baseboard Capacity At High Temperature� provide information about the power levels associated with each ZoneBaseboard:OutdoorTemperatureControlled object. These value are inputs to that object. The variables are useful for scaling the values assigned to the “Power Level� control in the “ZoneBaseboard:OutdoorTemperatureControlled� EMS actuator.
-
-HVAC Systems
-------------
-
-### AirTerminal:SingleDuct:Uncontrolled
-
-An internal variable called “AirTerminal:SingleDuct:Uncontrolled Maximum Mass Flow Rate� provides information about the design flow rate for direct air terminals. The units are kg/s. This is the mass flow rate (for dry air at standard conditions) at the volume flow rate entered in the field Maximum Air Flow Rate (m<sup>3</sup>/s) in the AirTerminal:SingleDuct:Uncontrolled input object. This internal variable is useful for scaling the flow rates assigned to the “Mass Flow Rate� control in the “AirTerminal:SingleDuct:Uncontrolled� EMS actuator.
-
-### Fan Nominal Ratings
-
-#### Fan Maximum Mass Flow Rate
-
-The input variable “Fan Maximum Mass Flow Rate� provides information about the maximum flow rate for a fan. The units are kg/s. This is the mass flow rate (for dry air at standard conditions) associated with the volume flow rate entered into the Maximum Air Flow Rate (m<sup>3</sup>/s) in the various fan input objects. This internal variable is useful for scaling the flow rates assigned to the “Fan Air Mass Flow Rate� control in the “Fan� EMS actuator.
-
-#### Fan Nominal Pressure Rise
-
-The input variable “Fan Nominal Pressure Rise� provides information about the static pressure rise experienced by a fan. The units are Pascals. This is the value entered into the field called Pressure Rise in the various fan input objects. This internal variable is useful for scaling the pressures assigned to the “Fan Pressure Rise� control in the “Fan� EMS actuator.
-
-#### Fan Nominal Total Efficiency
-
-The input variable “Fan Nominal Total Efficiency� provides information about the nominal efficiency of each fan. The value is dimensionless and expressed as a fraction. This is the value entered into the field called Fan Efficiency in the various fan input objects. This internal variable is useful for scaling the value assigned to “Fan Total Efficiency� control in the “Fan� EMS actuator.
-
-### Unitary HVAC Nominal Ratings
-
-#### Unitary HVAC Design Heating Capacity
-
-The internal variable called “Unitary HVAC Design Heating Capacity� provides information about the nominal heating capacity of unitary or furnace HVAC equipment. The units are Watts. The source of these data will vary depending on the type of heating coil. This internal variable is useful for scaling the value assigned to “Sensible Load Request� control in the “Unitary HVAC� EMS actuator.
-
-#### Unitary HVAC Design Cooling Capacity
-
-The internal variable called “Unitary HVAC Design Cooling Capacity� provides information about the nominal cooling capacity of unitary or furnace HVAC equipment. The units are Watts. The source of these data will vary depending on the type of cooling coil. This internal variable is useful for scaling the value assigned to “Sensible Load Request� control in the “Unitary HVAC� EMS actuator.
-
-### Outdoor Air Mixer Nominal Ratings
-
-#### Outdoor Air Controller Maximum Mass Flow Rate
-
-The internal variable called “Outdoor Air Controller Maximum Mass Flow Rate� provides information about the maximum outdoor air rate for each outdoor air system. The units are kg/s. The sources of these data are inputs in the Controller:OutdoorAir input object. This internal variable is useful for scaling the value assigned to the “Air Mass Flow Rate� control in the “Outdoor Air Controller� EMS actuator.
-
-#### Outdoor Air Controller Minimum Mass Flow Rate
-
-The internal variable called “Outdoor Air Controller Minimum Mass Flow Rate� provides information about the minimum outdoor air rate for each outdoor air system. The units are kg/s. The sources of these data are inputs in the Controller:OutdoorAir input object. This internal variable is useful for scaling the value assigned to the “Air Mass Flow Rate� control in the “Outdoor Air Controller� EMS actuator.
-
-### Pump Nominal Ratings
-
-The internal variable called “Pump Maximum Mass Flow Rate� provides information about the size of the pump. The units are kg/s. This is the mass flow rate associated with the volume flow rate entered into the Rated Flow Rate (m<sup>3</sup>/s) in the various pump input objects. This internal variable is useful for scaling the flow rates assigned to the “Pump Mass Flow Rate� control in the “Pump� EMS actuator.
-
-### Unitary Systems
-
-#### Unitary System Control Zone Mass Flow Fraction
-
-The internal variable called “Unitary System Control Zone Mass Flow Fraction� is used to adjust the zone load such that the total load met by the HVAC system, when distributed to the conditioned zones, will meet the controlling zones load. The controlling zone is the zone with the thermostat. See the AirloopHVAC:UnitarySystem input field named "Controlling Zone or Thermostat Location."
-
-### Low Temperature Radiant Hydronic
-
-#### Constant Flow Low Temp Radiant Design Water Mass Flow Rate
-
-The internal variable called “Constant Flow Low Temp Radiant Design Water Mass Flow Rate� provides information about the design water flow rate for radiant systems defined using a ZoneHVAC:LowTemperatureRadiant:ConstantFlow input object. The units are m<sup>3</sup>/s. This internal variable is useful for scaling the flow rates assigned to the “Water Mass Flow Rate� control in the “Constant Flow Low Temp Radiant� EMS actuator.
-
-#### Hydronic Low Temp Radiant Design Water Mass Flow Rate for Heating
-
-The internal variable called “Hydronic Low Temp Radiant Design Water Mass Flow Rate for Heating� provides information about the heating design water flow rate for radiant systems defined using a ZoneHVAC:LowTemperatureRadiant:VariableFlow input object. The units are m<sup>3</sup>/s. This internal variable is useful for scaling the flow rates assigned to the “Water Mass Flow Rate� control in the “Hydronic Low Temp Radiant� EMS actuator.
-
-#### Hydronic Low Temp Radiant Design Water Mass Flow Rate for Cooling
-
-The internal variable called “Hydronic Low Temp Radiant Design Water Mass Flow Rate for Heating� provides information about the cooling design water flow rate for radiant systems defined using a ZoneHVAC:LowTemperatureRadiant:VariableFlow input object. The units are m<sup>3</sup>/s. This internal variable is useful for scaling the flow rates assigned to the “Water Mass Flow Rate� control in the “Hydronic Low Temp Radiant� EMS actuator.
-
-### Boiler Nominal Ratings
-
-#### Boiler Nominal Capacity
-
-The internal variable called “Boiler Nominal Capacity� provides information about the nominal heating capacity of boiler equipment. The units are Watts. 
-
-### Chiller Nominal Ratings
-
-#### Chiller Nominal Capacity
-
-The internal variable called “Chiller Nominal Capacity� provides information about the nominal cooling capacity of chiller equipment. The units are Watts. 
-
-
-On-Site Electricity Production
-------------------------------
-
-### Generator Nominal Ratings
-
-The internal variables called “Generator Nominal Maximum Power� and “Generator Nominal Thermal To Electric Power� provide information about the nominal capacity of a generator to produce electricity and heat. The values made available here are those listed in the associated ElectricLoadCenter:Generators input object. The power is expressed in Watts.
-
-The thermal-to-electric ratio describes how the nominal thermal output compares to the nominal electrical output and is useful for characterizing combined heat and power (CHP) units.
-
-### Electrical Storage
-
-The internal variables called Electrical Storage Simple Maximum Capacity and  Electrical Storage Battery Maximum Capacity provide information about the capacity of electrical storage devices. Electrical Storage Simple Maximum Capacity is the value of the field called Maximum Storage Capacity in the ElectricLoadCenter:Storage:Simple input object, the units are in Joules.  Electrical Storage Battery Maximum Capacityâ is the value of the field called Maximum Module Capacity in the ElectricLoadCenter:Storage:Battery input object, the units are in amp-hours for just one battery module.
-
-Sizing
-------
-
-Several internal variables relate to sizing calculations. Although the primary intent for the EMS is to enable custom controls for operation, using internal variables is a prime example of extending the power of user-defined calculations to control certain aspects of sizing calculations.
-
-### Sizing:Zone
-
-A series of internal variables is available related to zone sizing:
-
-- Final Zone Design Heating Air Mass Flow Rate (kg/s)
-
-- Intermediate Zone Design Heating Air Mass Flow Rate (kg/s)
-
-- Final Zone Design Cooling Air Mass Flow Rate (kg/s)
-
-- Intermediate Zone Design Cooling Air Mass Flow Rate (kg/s)
-
-- Final Zone Design Heating Load (W)
-
-- Intermediate Zone Design Heating Load (W)
-
-- Final Zone Design Cooling Load (W)
-
-- Intermediate Zone Design Cooling Load (W)
-
-- Final Zone Design Heating Air Density (kg/m<sup>3</sup>)
-
-- Intermediate Zone Design Heating Air Density (kg/m<sup>3</sup>)
-
-- Final Zone Design Cooling Air Density (kg/m<sup>3</sup>)
-
-- Intermediate Zone Design Cooling Air Density (kg/m<sup>3</sup>)
-
-- Final Zone Design Heating Volume Flow (m3/s)
-
-- Intermediate Zone Design Heating Volume Flow (m3/s)
-
-- Final Zone Design Cooling Volume Flow (m3/s)
-
-- Intermediate Zone Design Cooling Volume Flow (m3/s)
-
-- Zone Outdoor Air Design Volume Flow Rate (m<sup>3</sup>/s)
-
-### Sizing:System
-
-A series of internal variables is available related to air system sizing:
-
-- Intermediate Air System Main Supply Volume Flow Rate (m<sup>3</sup>/s)
-
-- Intermediate Air System Coincident Peak Cooling Mass Flow Rate (kg/s)
-
-- Intermediate Air System Coincident Peak Heating Mass Flow Rate (kg/s)
-
-- Intermediate Air System Noncoincident Peak Cooling Mass Flow Rate (kg/s)
-
-- Intermediate Air System Noncoincident Peak Heating Mass Flow Rate (kg/s)
-
-- Intermediate Air System Heating Volume Flow Rate (m<sup>3</sup>/s)
-
-- Intermediate Air System Cooling Volume Flow Rate (m<sup>3</sup>/s)
-
-- Air System Cooling Design Sensible Capacity (W)
-
-- Air System Heating Design Sensible Capacity (W)
-
-- Air System Preheating Design Sensible Capacity (W)
-
-- Air System Outdoor Air Design Volume Flow Rate (m<sup>3</sup>/s)
-
-- Air System Cooling Design Mixed Air Temperature (C)
-
-- Air System Cooling Design Mixed Air Humidity Ratio (kgWater/kgDryAir)
-
-- Air System Cooling Design Return Air Temperature (C)
-
-- Air System Cooling Design Return Air Humidity Ratio (kgWater/kgDryAir)
-
-- Air System Cooling Design Outdoor Air Temperature (C)
-
-- Air System Cooling Design Outdoor Air Humidity Ratio (kgWater/kgDryAir)
-
-- Air System Heating Design Mixed Air Temperature (C)
-
-- Air System Heating Design Mixed Air Humidity Ratio (kgWater/kgDryAir)
-
-- Air System Heating Design Return Air Temperature (C)
-
-- Air System Heating Design Return Air Humidity Ratio (kgWater/kgDryAir)
-
-- Air System Heating Design Outdoor Air Temperature (C)
-
-- Air System Heating Design Outdoor Air Humidity Ratio (kgWater/kgDryAir)
-
-### Sizing:Plant
-
-An internal variable is available for plant system sizing.
-
-- Plant Design Volume Flow Rate (m<sup>3</sup>/s)
-
-EMS Sensors
-===========
-
-This section provides more information about EMS sensors.
-
-The input object EnergyManagementSystem:Sensor is simple but quite powerful. It reuses the normal EnergyPlus output variables to provide a general way of obtaining a wide variety of input data with minimal complications.
-
-One odd result of the approach taken for EMS sensors is that information about the available sensors is derived from what are usually the outputs of EnergyPlus. The RDD file is an important resource for EMS users. The RDD file is an output from running EnergyPlus and is called “eplusout.rdd� (but you may rename it to &lt;your-filename&gt;.rdd with a run manager such as EP-Launch). This output file is often needed to develop EMS input, so you may need to do an initial run of the model with traditional controls to obtain an RDD file. The contents of an RDD file will vary depending on the type of model. Once you have experience and familiarity with the outputs expected from a model, you should not need to prerun models, as you will be able to foresee the available output. The RDD file from a similar model with the same types of components and systems can also be used as a guide for what will be available in a specific model.
-
-Variable Types
---------------
-
-Various types of output variables in EnergyPlus can be used as sensors in the EMS. It is important to understand some distinctions.
-
-- Reported variables have two update frequencies: **zone** and **system**. Zone variables are updated for each zone timestep. System variables are updated for each system timestep.
-
-- Reported variables have two types of content: **averaged** and **summed**. Averaged variables are state variables such as temperature and mass flow rate. Summed variables are quantities of energy such as electricity use.
-
-Schedules
----------
-
-The EnergyManagementSystem:Sensor object can also provide scheduled data for use in Erl programs. Because schedule values are available as outputs that use the “Schedule Value� output, they can also be mapped as sensors. You can use any of the various types of schedule input objects to define a schedule. The schedule does not need to be used elsewhere in the model. The value of the schedule is then mapped to an EMS variable with the Schedule Value report variable. When used with the Schedule:File input object, the sensor object can import time series data into the EMS from an external file. One application might be to test a proposed EMS algorithm with real experimental data.
-
-
-
-EMS Actuators
-=============
-
-This section provides details about EMS actuators, the conduits by which Erl programs control EnergyPlus simulations. They *actuate* selected features inside EnergyPlus. Rather than add a new set of controls and component models that have EMS awareness, they generally override established features.
-
-Internal to EnergyPlus are two separate lists of actuators:  those that are available for use, and those that are being used in the EMS. While implementing the EMS, developers have added code to control points to make them available for use in EMS. The actuators available in a given model depend on the non-EMS-related content of the input file. Similar to how EnergyPlus reports the available output variables to the RDD file, a list of available actuators is written to the EDD file (depending on the settings in Output:EnergyManagementSystem). Note that the EDD file is ONLY produced if you have set up EMS / Erl programs. To use an actuator in EMS, you need to enter an EnergyManagementSystem:Actuator input object. The EDD file contains information needed for this input object; however, it is not available until after the output has been generated from a previous run. If you do not see a particular actuator in the EDD output file, it is not available in EMS for that particular model. There is no way to create a new actuator (except by modifying EnergyPlus source code); you can only customize the behavior of current actuators. If you need an actuator that you suspect could be provided by the program but is not available, you can use the regular system(s) for user support to request it be added to the program. New actuators are added to the program from time to time so the availability of actuators will grow with each new release.
-
-Actuators override things inside EnergyPlus whenever the actuator’s Erl variable is set to a value other than “Null.�  Null is a special built-in variable used to deactivate an actuator. Once an actuator starts overriding, it will continue to do so until the actuator’s Erl variable is set to Null. You should set the actuators to Null whenever you want the EMS to revert to normal operation.
-
-The rest of this section provides details about specific actuators.
-
-HVAC Systems
-------------
-
-### System Node Setpoints
-
-A series of actuators is available for all the setpoints that can be placed on system nodes. System nodes are used to define air and plant loops, and a natural application of EMS is to control the setpoints at these nodes. The node actuators are all called “System Node Setpoint.�  There are nine control types:
-
-- Temperature Setpoint, (°C)
-
-- Temperature Minimum Setpoint (°C)
-
-- Temperature Maximum Setpoint (°C)
-
-- Humidity Ratio Setpoint (kgWater/kgDryAir)
-
-- Humidity Ratio Minimum Setpoint (kgWater/kgDryAir)
-
-- Humidity Ratio Maximum Setpoint (kgWater/kgDryAir)
-
-- Mass Flow Rate Setpoint (kg/s)
-
-- Mass Flow Rate Minimum Setpoint (kg/s)
-
-- Mass Flow Rate Maximum Setpoint (units kg/s)
-
-Using these actuators is natural with an EMS. Typically, the controller would place the setpoint on the outlet node. Then the component’s low-level controller should operate to meet the leaving setpoint. Setting the setpoints on nodes should be a common application for the EMS.
-
-Although all nine possible setpoints are available as EMS actuators, it does not follow that EnergyPlus can use all of them. Most components can use only one or two setpoints. If a component cannot control to meet the setpoints on a node, the actuator will do nothing.
-
-### Zone HVAC Control
-
-Several actuators relate to HVAC zone controls for temperature, humidity, and comfort.
-
-- Two actuators called “Zone Temperature Control� are available with the control types of “Heating Setpoint� and “Cooling Setpoint.�  These enable you to directly override the zone-by-zone heating and cooling setpoints. The units are in degrees Celsius. The unique identifier is the zone name.
-
-- Two actuators called “Zone Humidity Control� are available with the control types “Relative Humidity Humidifying Setpoint� and “Relative Humidity Dehumidifying Setpoint.�  These enable you to directly override the zone-by-zone humidity control setpoints. The units are in percent relative humidity. The unique identifier is the zone name.
-
-- Two actuators called “Zone Comfort Control� are available with the control types “Heating Setpoint� and “Cooling Setpoint.�  These enable you to directly override the zone-by-zone comfort control setpoints. The units are predicted mean vote (PMV). The unique identifier is the zone name.
-
-### Plant Supervisory Control
-
-Several levels of actuators are available for on/off supervisory control of Plant systems.
-
-- Each plant (and condenser) loop has an actuator called “Plant Loop Overall� available with the control type “On/Off Supervisory.�  Setting the value of this actuator to 1.0 directs the overall plant to loop to run normally based on other controls. Setting the value of this actuator to 0.0 directs the overall plant loop to shut down regardless of what other controls indicate.
-
-- Each plant (and condenser) loop has actuators called “Supply Side Half Loop� and “Demand Side Half Loop� that are available with the control type “On/Off Supervisory.�  Setting the value of this actuator to 1.0 directs the plant’s loop side to run normally based on other controls. Setting the value of this actuator to 0.0 directs the plant’s loop side to shut down regardless of what other controls indicate.
-
-- Each plant (and condenser) loop has a series of actuators called “Supply Side Branch� and “Demand Side Branch� that are available with the control type “On/Off Supervisory.�  These are available for each individual branch in a loop. Setting the value of this actuator to 1.0 directs the plant’s branch to run normally based on other controls. Setting the value of this actuator to 0.0 directs the plant’s branch to shut down regardless of what other controls indicate.
-
-- Each plant (and condenser) loop has a series of actuators called “Plant Component \*� that are available with the control type “On/Off Supervisory.�  These are available for each individual component on a loop. Setting the value of this actuator to 1.0 directs the component to run normally based on other controls. Setting the value of this actuator to 0.0 directs the component to shut down regardless of what other controls indicate.
-
-### Outdoor Air System Node Conditions
-
-Actuators called “Outdoor Air System Node� are available with control types called “Drybulb Temperature� and “Wetbulb Temperature.�  The units are degrees Celsius. These actuators are available for all system nodes that are listed in either an OutdoorAir:Node or OutdoorAir:NodeList input object. You should probably set both the drybulb and wetbulb temperatures to ensure a full description of the moist air conditions.
-
-The air system and many component models require you to specify a node as an outdoor air node to obtain values for the outdoor conditions. For example, outdoor air nodes are used at the inlet to an outdoor air mixer or at the inlet of the heat rejection side of a component model. Typically this is the weather data value for outdoor conditions. But local variations in microclimate may shift the local outdoor air temperature to differ slightly from the weather data. (Currently the only local variation model for this effect in EnergyPlus varies the outdoor air conditions as a function of height.)  If you want to experiment with other models for local variations in outdoor air conditions, this EMS actuator allows you to override the outdoor temperature at a particular system node with any model that can be implemented in an Erl program. For example (although better models for the changes in conditions may need be developed), this actuator could be used to examine the energy impacts of warmer outdoor air temperatures experienced by a rooftop packaged HVAC system sitting on a black roof or the cooler conditions experienced by a unit that is located on the shaded side of a building.  Another example is to make use of a separate model, outside of EnergyPlus, for some unique type of component (such as a labyrinth or earth-tube) that preconditions outdoor air; the results of that model could be fed into the air system model in EnergyPlus using these actuators.
-
-### AirLoopHVAC Availability Status
-
-This actuator is available in all models with central, or primary, air systems that are entered with the object “AirLoopHVAC.�  Various availability managers use the air loop’s availability status to override control of the central air system fan. The fan may be scheduled to be unavailable during certain times to shut down the system when it is not needed. However, there may be times when the air system should be started to protect from freezing, for example. This actuator can force an air system to start up or shut down.
-
-The control is actuated by setting values for the availability status. The settings are numeric, but represent discrete states the status can take. The following settings are valid:
-
-- 0.0 (= NoAction). This tells the air system to do whatever it would usually do without any special override status.
-
-- 1.0 (= ForceOff). This overrides the air system to shut down when it would normally want to run.
-
-- 2.0 (= CycleOn). This overrides the air system to start up when it would normally be off.
-
-- 3.0 (= CycleOnZoneFansOnly). This overrides only the zone fans (not the central fans) if they would normally be off.
-
-### Ideal Loads Air System
-
-An actuator called “Ideal Loads Air System� is available with control types called “Air Mass Flow Rate� (supply air), “Outdoor Air Mass Flow Rate,� “Air Temperature,� and “Air Humidity Ratio.�  These are available in models that use the ideal loads air system, formerly known as purchased air. The units are kg/s for mass flow rate, C for temperature and kgWater/kgDryAir for humidity ratio. The unique identifier is the user-defined name of the ZoneHVAC:IdealLoadsAirSystem input object.
-
-For Air Temperature and Air Humidity Ratio, the overrides are absolute. They are applied after all other limits have been checked. For mass flow rate, the overrides are not absolute, in that the model has additional internal controls that may not always be overridden. The internal controls will still apply the capacity and flow rate limits if defined in the input object. The EMS override affects the flow rate only if the air system is on. If the air system is “off,� the mass flow is zero regardless of the actuator setting. The internal model controls will turn off the air system if the zone is in the dead band or if it is scheduled “off� by availability managers. This behavior allows you to use the internal controls to determine when the air should cycle on, as for a constant volume system that cycles to achieve control. If both the Air Mass Flow Rate and Outdoor Air Mass Flow Rate are overridden, the Outdoor Air Mass Flow Rate will not be allowed to be greater than the override value for Air Mass Flow Rate.
-
-### Fan
-
-Actuators called “Fan� are available with the control types “Fan Air Mass Flow Rate,� “Fan Pressure Rise,� and “Fan Total Efficiency.�  These provide direct control over the fan operation in an air system. The EMS program can override the flow rate by using kg/s. It can override the total pressure rise at the fan by using Pascals. And it can override the fan efficiency on a scale from 0.0 to 1.0. The unique identifier is the name of the fan in the Fan input objects.
-
-An actuator is also available for overriding the autosize value for the fan’s design air flow rate.  This actuator is called “Fan� and the control type is “'Fan Autosized Air Flow Rate� with units in m<sup>3</sup>/s. It is only useful from the calling point named AfterComponentInputReadIn.
-
-### DX Cooling Coils
-
-Actuators are available for overriding the autosize values related to the size of single speed DX coils.  Actuators called “Coil:Cooling:DX:SingleSpeed� are available with control types “Autosized Rated Air Flow Rate� (in m3/s), “Autosized Rated Sensible Heat Ratio� (in W/W), and “Autosized Rated Total Cooling Capacity� (in W).  These are only useful from the calling point named AfterComponentInputReadIn.
-
-### Unitary Equipment
-
-Actuators called “Unitary HVAC� are available with the control types “Sensible Load Request� and “Moisture Load Request.�  These control the operation of unitary equipment. Normally these systems operate to meet zone loads, but these actuators allow you to override the controls of unitary systems. The units are in Watts. The unique identifier is the name of the unitary equipment in the input objects.
-
-Actuators are available for overriding the autosize values related to supply air flow rates some unitary HVAC equipment.  These actuators allow selectively altering the outcome of sizing routines and are used from the calling point named AfterComponentInputReadIn.  The units are m<sup>3</sup>/s.
-
-- An actuator called “AirLoopHVAC:Unitary:Furnace:HeatOnly� is available with control type “Autosized Supply Air Flow Rate.�
-
-- An actuator called “AirLoopHVAC:UnitaryHeatOnly� is available with control type “Autosized Supply Air Flow Rate.�
-
-- Actuators called “AirLoopHVAC:Unitary:Furnace:HeatCool� and “AirLoopHVAC:UnitaryHeatCool�are available with control types “Autosized Supply Air Flow Rate,�  “Autosized Supply Air Flow Rate During Cooling Operation,� “Autosized Supply Air Flow Rate During Heating Operation,� and “Autosized Supply Air Flow Rate During No Heating or Cooling Operation.�
-
-- An actuator called “AirLoopHVAC:UnitaryHeatPump:AirToAir� is available with control type “Autosized Supply Air Flow Rate.�
-
-- An actuator called “AirLoopHVAC:UnitaryHeatPump:WaterToAir� is available with control type “Autosized Supply Air Flow Rate.�
-
-### AirTerminal:SingleDuct:Uncontrolled
-
-An actuator called “AirTerminal:SingleDuct:Uncontrolled� is available with a control type called “Mass Flow Rate.�  This actuator is available in models that use the direct air terminal. The units are kg/s. This actuator is used to control the flow rate. Normally, the flow rate of direct air terminals is fixed by the input or sizing results, but this actuator provides a way to override the flow with Erl programs.
-
-### Outdoor Air Controller
-
-An actuator called “Outdoor Air Controller� is available with the control type called “Air Mass Flow Rate.�  This provides override control over the rate of outdoor air. The units are kg/s. The unique identifier is the name of the Controller:OutdoorAir input object.
-
-### Plant Load Profile
-
-Actuators called “Plant Load Profile� are available with the control types called “Mass Flow Rate� (in kg/s) and “Power� (in W). The unique identifier is the name of the LoadProfile:Plant input object. These actuators provide override control over the loads placed on a plant system by a plant load profile.
-
-### Pump
-
-An actuator called “Pump� is available with the control type “Pump Mass Flow Rate� (in kg/s). This allows you to override the flow rate produced by a pump. The unique identifier is the name of Pump Input object.
-
-### Window Air Conditioner
-
-An actuator called “Window Air Conditioner� is available with a control type called “Part Load Ratio.�  This is nondimensional and takes numbers between 0.0 and 1.0. The unique identifier is the name of the ZoneHVAC:WindowAirConditioner input object.
-
-### Low Temperature Radiant Hydronic
-
-Actuators called “Hydronic Low Temp Radiant� and “Constant Flow Low Temp Radiant� are available with the control type “Water Mass Flow Rate� (in kg/s). This allows you to override the flow of water through hydronic radiant systems. The unique identifier is the name of either the ZoneHVAC:LowTemperatureRadiant:VariableFlow or ZoneHVAC:LowTemperature  
- Radiant:ConstantFlow input objects.
-
-### Variable Refrigerant Flow Heat Pump Air Conditioner
-
-An actuator called “Variable Refrigerant Flow Heat Pump� is available with a control type called “Operating Mode.�  This is nondimensional and takes numbers between 0.0 and 2.0 where 0.0 means the system is off, 1.0 means the system is in cooling mode, and 2.0 means the system is in heating mode. The unique identifier is the name of the AirConditioner:VariableRefrigerantFlow input object.
-
-### Variable Refrigerant Flow Terminal Unit
-
-An actuator called “Variable Refrigerant Flow Terminal Unit� is available with a control type called “Part Load Ratio.�  This is nondimensional and takes numbers between 0.0 and 1.0. The unique identifier is the name of the ZoneHVAC:TerminalUnit:VariableRefrigerantFlow input object. This control over rides the part-load ratio of the terminal unit and can be applied only when the cooling or heating minimum and maximum outdoor temperature limits of the condenser (i.e., the AirConditioner:VariableRefrigerantFlow object) are not exceeded.
-
-Thermal Envelope
-----------------
-
-### Window Shading Control
-
-This actuator is available in models that also have the WindowProperty:ShadingControl input objects. The user-defined name for the WindowProperty:ShadingControl is not used to identify unique window shading controls; rather, the window name is used to identify the actuator. This is because there could be multiple windows, all with shades, each of which is governed by a single WindowProperty:ShadingControl input object. The EMS actuator can override the control actions for each window separately.
-
-The control is actuated by setting values for the control status. The settings are numeric but represent discrete states the control can take. The appropriate values depend on the type and position of the shading device. There are three basic types of shading devices:  switchable glazings, shades, and blinds. (Shades are described with WindowMaterial:Shade input objects. Blinds are described with WindowMaterial:Blind input objects.)  Shades and blinds can be situated in the exterior, between the glass, or in the interior.
-
-The following settings are valid and must be used:
-
-- –1.0:     No shading device.
-
-- 0.0:       Shading device is off (applies to shades and blinds).
-
-- 1.0:       Interior shade is on.
-
-- 2.0:       Glazing is switched to a darker state (switchable glazings only).
-
-- 3.0:       Exterior shade is on.
-
-- 6.0:       Interior blind is on.
-
-- 7.0:       Exterior blind is on.
-
-- 8.0:       Between-glass shade is on.
-
-- 9.0:       Between-glass blind is on.
-
-### Slat Angle
-
-If the shading device is a blind, there is also a control type called “Slat Angle.�  This angle control is a continuous numeric value from 0.0 to 180.0. The angle is defined as between the glazing system’s outward normal and the slat’s outward normal (see the diagram in the input output reference under WindowMaterial:Blind).
-
-### Surface Convection Heat Transfer Coefficient
-
-Two actuators called “Surface� are available with the control types of “Interior Surface Convection Heat Transfer Coefficient� and “Exterior Surface Convection Heat Transfer Coefficient.�  These provide direct control over the convection coefficient. The units are W/m<sup>2</sup>-K. The unique identifier is the surface name.
-
-This actuator controls the heat transfer modeling. Changes in air distribution systems can affect the interior surface convection coefficients. A sheltered exterior surface may have a lower surface heat transfer coefficient. This actuator provides a method of applying new models for convection coefficients.
-
-### Material Surface Properties
-
-Three actuators are available for controlling the surface properties material related to absorptance. Those material layers used in a Construction object that lie at the outside and the inside of the assembly determine the surface properties of a heat transfer surface.  Actuators called “Material� are available with the control types “Surface Property Solar Absorptance,� “Surface Property Thermal Absorptance,� and “Surface Property Visible Absorptance.�  These are dimensionless parameters between 0.0 and 1.0.  These actuators are useful for modeling switchable coatings such as thermochromic paints.
-
-### Surface Construction State
-
-An actuator is available for controlling the construction assigned to a surface that can be useful for modeling dynamic technologies for thermal envelopes.  These actuators are called “Surface� and have a control type “Construction State.�  This actuator is used in conjunction with the input object called EnergyManagementSystem:ConstructionIndexVariable.  Each Construction object defined in an input file has an index that points to where the data for that construction are stored in the program’s internal data structures.  The EnergyManagementSystem:ConstructionIndexVariable input object is used to create and fill a global Erl variable with the value that points to the specific construction named in the object. The Erl variable is what you assign to the construction state actuator’s variable to override the construction assigned to a particular surface.  When the actuator is set to Null, the surface reverts to the Construction originally referenced by the surface in the input file.
-
-Using the surface construction state actuator brings with it a high degree of risk when it comes to modeling thermal heat capacity and transient heat transfer in opaque surfaces.  If this actuator is used inappropriately, for example to assign different constructions, to a single surface, that have radically different heat storage capacities, then the heat transfer modeling results may not be physically accurate.  When a construction state is overridden using this actuator, the thermal history data that evolved while using the previous construction are reused for the new construction. When this actuator is used, the program attempts to detect if incompatible constructions are being assigned. In some cases it issues a warning and allows the assignments to proceed, in others it warns and doesn’t allow the assignment to proceed.  If the original construction assigned to a surface has internal source/sink (defined using Construction:InternalSource) then any assignments to the surface must also be internal source constructions.  If using the heat transfer algorithm called ConductionFiniteDifference, then the constructions must have the same number of finite difference nodes or the assignment is not allowed.  The construction state actuator cannot be used in conjunction with the heat transfer algorithms called ConductionFiniteDifferenceSimplified or CombinedHeatAndMoistureFiniteElement.
-
-### Surface Boundary Conditions
-
-Four actuators, called “Other Side Boundary Conditions,� are available for controlling the convection and radiation boundary conditions for surfaces that use “OtherSideConditionsModel.�  Each instance of a SurfaceProperty:OtherSideConditionsModel object will make available these actuators with the following four control types:
-
-- “Convection Bulk Air Temperature.�  This is the temperature of the ambient air exposed to the surface, in degrees C.  This is the temperature used for surface convection heat transfer boundary conditions on the outdoor, outside-face, other side of the surface.
-
-- “Convection Heat Transfer Coefficient.�  This is the heat transfer coefficient, in W/(m-K) used for surface convection boundary conditions on the outdoor, outside-face, or other side of the surface.
-
-- “Radiation Effective Temperature.�  This is the effective temperature of the environment surrounding the surface, in degrees C.  This is the temperature used for surface thermal radiation heat transfer boundary conditions on the outdoor, outside-face, other side of the surface.
-
-- “Radiation Linear Heat Transfer Coefficient.�  This is the linearized heat transfer coefficient, in W/(m-K), used for surface thermal radiation boundary conditions on the outdoor, outside-face, or other side of the surface.
-
-When using these actuators, values should be set for all four types.  This boundary condition has no solar, only convection and radiation.
-
-Air Movement
-------------
-
-### Zone Infiltration
-
-An actuator called “Zone Infiltration� is available with a control type called “Air Exchange Flow Rate� (m<sup>3</sup>/s). This provides override control over the zone-by-zone infiltration rate. The unique identifier is the name of the ZoneInfiltration object.
-
-### Zone Ventilation
-
-An actuator called “Zone Ventilation� is available with a control type called “Air Exchange Flow Rate� (m<sup>3</sup>/s). This provides override control over the zone-by-zone ventilation rate. This simple ventilation model is provided by the input object ZoneVentilation. The unique identifier is the name of the ZoneVentilation object.
-
-### Zone Mixing
-
-An actuator called “ZoneMixing� is available with a control type called “Air Exchange Flow Rate� (m<sup>3</sup>/s). This provides override control over the zone-to-zone mixing rate. This simple air movement model is provided by the input object ZoneMixing. The unique identifier is the name of the ZoneMixing object.
-
-### Zone Cross Mixing
-
-An actuator called “ZoneCrossMixing� is available with a control type called “Air Exchange Flow Rate� (m<sup>3</sup>/s). This provides override control over the interzonal mixing rate. This is the simple air movement model provided by the input object ZoneCrossMixing. The unique identifier is the name of the ZoneCrossMixing object.
-
-### Airflow Network Openings
-
-An actuator called “AirFlow Network Window/Door Opening� is available with a control type called “Venting Opening Factor.�  It is available in models that have operable openings in the Airflow Network model and that are entered by using either AirflowNetwork:MultiZone:Component:DetailedOpening or AirflowNetwork:MultiZone:Component:SimpleOpening input objects. This control allows you to use EMS to vary the size of the opening during the airflow model calculations, such as for natural and hybrid ventilation.
-
-The unique identifier is the name of the window or door, not the name of the associated airflow network input objects. The actuator control involves setting the value of the opening factor between 0.0 and 1.0.
-
-Internal Gains and Exterior Lights
-----------------------------------
-
-### People
-
-An actuator called “People� is available with a control type called “Number of People.�  This allows you to dictate the number of people in a zone. The units are persons. The unique identifier is the name of the people input object. Because you cannot really control people, this is an example the EMS in EnergyPlus departing from the real world of building EMS.
-
-### Lights
-
-An actuator called “Lights� is available with a control type called “Electric Power Level� (in W)  This allows you to set the lighting power associated with each Lights input object. The unique identifier is the name of the Lights input object.
-
-### Electric Equipment
-
-An actuator called “ElectricEquipment� is available with a control type called “Electric Power Level� (in W). This allows you to set the power associated with each ElectricEquipment input object. The unique identifier is the name of the ElectricEquipment input object.
-
-### Gas Equipment
-
-An actuator called “GasEquipment� is available with a control type called “Gas Power Level� (in W). This allows you to set the power associated with each GasEquipment input object.  The unique identifier is the name of the GasEquipment input object.
-
-### Hot Water Equipment
-
-An actuator called “HotWaterEquipment� is available with a control type called “District Heating Power Level� (in W). This allows you to set the power associated with each HotWaterEquipment input object. The unique identifier is the name of the HotWaterEquipment input object.
-
-### Steam Equipment
-
-An actuator called “SteamEquipment� is available with a control type called “District Heating Power Level� (in W). This allows you to set the power associated with each SteamEquipment input object. The unique identifier is the name of the SteamEquipment input object.
-
-### Other Equipment
-
-An actuator called “OtherEquipment� is available with a control type called “Power Level� (in W). This allows you to set the power associated with each OtherEquipment input object. The unique identifier is the name of the OtherEquipment input object.
-
-Other equipment offers a way to adjust the zone air energy balance without consuming any energy resources.
-
-### Baseboard
-
-An actuator called “ZoneBaseboard:OutdoorTemperatureControlled� is available with a control type called “Power Level� (in W). The unique identifier is the name of the ZoneBaseboard:OutdoorTemperatureControlled input object.
-
-### Exterior Lights
-
-An actuator called "ExteriorLights" is available with a control type called "Electric Power" (in W). The unique identifier is the name of the Exterior:Lights input object.
-
-On-Site Electricity Production
-------------------------------
-
-### Generator Dispatch
-
-An actuator called “On-Site Generator Control� is available with a control type called “Requested Power.� This actuator is available in models that have on-site electrical generators. The units are Watts. This control allows you to use the EMS to override how requests for power generation are dispatched.
-
-The unique identifier is the name of each generator. The Erl programs should set the actuator value with Watts. Depending on the type and limitations of the generator being modeled, the power production may not exactly meet what is requested.
-
-### Electrical Storage
-
-Actuators called “Electrical Storage� are available with control types called “Power Draw Rate� and “Power Charge Rate� (in W). These are available in models that have ElectricLoadCenter:Storage:Simple input objects. These controls allow you to use the EMS to override the rate of charging or drawing from storage.
-
-The unique identifiers are the names of the storage objects. For a given timestep, the electrical storage device can only charge or draw. If the EMS tries to override charge and draw during the same timestep, the program will find the larger of the two and apply the difference in that direction.
-
-Refrigeration
--------------
-
-### Condenser Operation
-
-An actuator called “Refrigeration:System� is available with a control type called “Minimum Condensing Temperature.�  This actuator is available in models that use the Refrigeration:System object.  This actuator allows the user to override the usually constant value that is input into the field called Minimum Condensing Temperature in the Refrigeration:System object.  This allows operating the condenser using custom control algorithms.
-
-General
--------
-
-### Schedules
-
-A series of actuators is available for overriding schedule values. The following actuators are available with the control type called “Schedule Value�:  Schedule:Year, Schedule:Compact, Schedule:File, and Schedule:Constant. The units are not known by the schedule and are determined by the model that references the schedule. The unique identifier is the name of schedule.
-
-If you try to use a particular schedule as input to calculations that modify that schedule, you will be in a circular situation with unexpected results. The modified schedule will lose the original information (unless the actuator is set to Null) and the modifications will be reapplied on top of previous modifications. When this situation arises, use a copy of the original schedule as input to the Erl program so you have the original schedule values.
-
-### Curves
-
-An advanced actuator called “Curve� with a control type called “Curve Result� is available whenever any generic curve objects are used. This allows you to override the results generated by these curves. The units are not known by the actuator and depend on how the curve is being used by the component model that calls it.
-
-This actuator must be used with caution. The EMS does not necessarily have access to the independent variables used by the models when the curves are evaluated during normal evaluation, so in most situations you will probably need to examine EnergyPlus source code to use this actuator correctly.
-
-### Weather Data
-
-A series of actuators are available for overriding the values of weather data that are normally derived from the .epw weather file.  These provide the ability to alter weather data and were originally requested for use with ExternalInterface for using measured data.  The following can be overridden: outdoor drybulb, outdoor dewpoint, outdoor relative humidity, diffuse solar, direct solar, wind speed, and wind direction.
-
-Sizing
-------
-
-### Sizing:Zone
-
-A series of actuators called “Sizing:Zone� is available. These offer a way to override the results of zone sizing calculations. The unique identifier for each is the name of the Zone Input object. The following control types are available:
-
-- Zone Design Heating Air Mass Flow Rate (kg/s)
-
-- Zone Design Cooling Air Mass Flow Rate (kg/s)
-
-- Zone Design Heating Load (W)
-
-- Zone Design Cooling Load (W)
-
-- Zone Design Heating Vol Flow (m<sup>3</sup>/s)
-
-- Zone Design Cooling Vol Flow (m<sup>3</sup>/s)
-
-### System Sizing
-
-A series of actuators called “Sizing:System� is available. These offer a way to override the results of air system sizing calculations. The unique identifier is the name of the AirLoopHVAC input object. The following control types are available:
-
-- Main Supply Volume Flow Rate (m<sup>3</sup>/s)
-
-- Main Supply Coincident Peak Cooling Mass Flow Rate (kg/s)
-
-- Main Supply Coincident Peak Heating Mass Flow Rate (kg/s)
-
-- Main Supply Noncoincident Peak Cooling Mass Flow Rate (kg/s)
-
-- Main Supply Noncoincident Peak Heating Mass Flow Rate (kg/s)
-
-- Main Heating Volume Flow Rate (m<sup>3</sup>/s)
-
-- Main Cooling Volume Flow Rate (m<sup>3</sup>/s)
-
-EMS Calling Points
-==================
-
-This section provides an overview of EnergyPlus’s program flow and describes the various places where you can use the EMS to initiate calls for custom controlling. The input object EnergyManagementSystem:ProgramCallingManager requires the user describe the timing for when the Erl programs are run. These *EMS Calling Points* correspond to places inside the EnergyPlus program where and when the EMS can be called to do something. The EMS offers a wide range of calling points. This section attempts to explain what you need to know about the EnergyPlus program flow so you can better understand which calling point to use for a particular application. Because the EMS needs to interact with the rest of the EnergyPlus computer program, you need a fairly high level of understanding of the inner workings of EnergyPlus. Finding the right point to insert your Erl override is a challenge. This is a complicated computer program. Using an interpreted language to override its calculations is no simple thing and should not be taken lightly.
-
-The best calling point will depend on the type of actuator being controlled and the intent of the override activity. Unfortunately, there is no easy way to explain the inner workings of a model as large as EnergyPlus, so this section includes only a brief overview. We attempt to provide useful recommendations for the types of control that are best suited for particular calling points. But for the full details you will need to refer to the EnergyPlus source code, which you can obtain with a developer license.
-
-This section starts with a series of three figures and then discusses them and the 14 calling points. Figure 1 shows the overall flow of an EnergyPlus model with some EMS calling points. Figure 2 shows the sequence for a single timestep with the remaining EMS calling points. Figure 3 is similar but shows the calling points for shortened system timesteps. These diagram the flow of procedures during a run from top to bottom.
-
-![EMSCallingPointDiagOverall](media/image003.jpg)
-
-Figure 1. Overall Program Flow and EMS Calling Points
-
-
-
-![EMSCallingPointDiagTimestep](media/image004.jpg)
-
-Figure 2. Timestep Sequence with EMS Calling Points
-
-
-
-
-
-![EMSCallingPointDiagSystemTimestep](media/image005.jpg)
-
-Figure 3. System Timestep Sequence with EMS Calling Points
-
-When EnergyPlus runs a model, it first does various sizing and setup activities and then models the environment periods you ask for; e.g., design days and run periods. The built-in variable called CurrentEnvironment indentifies which of these is being simulated and any given time. Figure 1 diagrams the overall program flow starting at the top and listing certain key steps in outline form. EnergyPlus models contain a lot of input, and the internal processes to acquire and process that input take some time to complete. Before the model starts doing final calculations, it may have to do various sizing calculations and automatically design the size of components. It will also go through special setup periods that model a truncated set of timesteps for each environment period. In the diagram, this initial phase is not finished until just before the design periods begin. Two EMS calling points that occur only once in a given run, EndOfZoneSizing and EndOfSystemSizing, can be triggered during this initial setup phase. During the phase called “Setup Simulation,� the various timestep-based calling points diagrammed in Figure 2 will also be called.
-
-Another thing that happens during the setup phase described above is that individual HVAC component models access their input data and do various setup calculations in preparation for the rest of the simulation.   An EMS calling point (added for Version 7) called “AfterComponentInputReadIn� is available for selected HVAC components that allows triggering Erl programs at a point just after the component’s input data have been read in but before the component’s sizing routines have executed.  This calling point is intended to be used with various actuators that are setup to override the autosize values that result from sizing.
-
-To model environment periods, EnergyPlus runs through a serious of timesteps. Figure 2 diagrams the program flow for a single timestep where the timestep for the system modeling is equal to that for the zone load modeling. The *system* timestep can be shorter than the *zone* timestep. The usual process of modeling a timestep is to first calculate the zone loads during the “Predictor,� then model the response of the HVAC systems, and then calculate the resulting zone conditions during the “Corrector.�  Within the HVAC system modeling, some system iterations are used to iteratively solve a system of systems. Figure 3 is a slightly modified version Figure 2 that diagrams the situation when the timestep of the system calculations has been reduced to half the length of the zone timestep.
-
-Begin New Environment
----------------------
-
-The calling point referred to with the keyword “BeginNewEnvironment� occurs once near the beginning of each environment period. Environment periods include sizing periods, design days, and run periods. This calling point will not be useful for control actions, but is useful for initializing variables and calculations that do not need to be repeated during each timestep. Once a value is set, Erl variables remember the value during the course of a simulation. Considerable repetition can be avoided by designing Erl programs to use this calling point for initializations and calculations that are needed only once. It is not called during individual timesteps.
-
-After New Environment Warmup Is Complete
-----------------------------------------
-
-The calling point referred to with the keyword “AfterNewEnvironmentWarmUpIsComplete� occurs once near at the beginning of each environment period but after any warmup days are complete. This is similar to the previous calling point. Warmup days are used to condition the transient aspects of the model before proceeding with the first day. This will not be useful for control actions, but would be useful for reinitializing Erl programs with fresh values after the warmup days have finished running and the model is about to start the final timestep calculations for a particular environment period.
-
-Begin Timestep Before Predictor
--------------------------------
-
-The calling point called “BeginTimestepBeforePredictor� occurs near the beginning of each timestep but before the predictor executes. “Predictor� refers to the step in EnergyPlus modeling when the zone loads are calculated. This calling point is useful for controlling components that affect the thermal loads the HVAC systems will then attempt to meet. Programs called from this point might actuate the building envelope or internal gains based on current weather or on the results from the previous timestep. Demand management routines might use this calling point to reduce lighting or process loads, change thermostat settings, operate window shades, etc.
-
-After Predictor Before HVAC Managers
-------------------------------------
-
-The calling point called “AfterPredictorBeforeHVACManagers� occurs after predictor and before the traditional HVAC managers are called. It occurs at each timestep just after the predictor executes but before SetpointManager and AvailabilityManager models are called. It is useful for a variety of control actions. However, if there are conflicts, the EMS control actions could be overwritten by other SetpointManager or AvailabilityManager actions.
-
-After Predictor After HVAC Managers
------------------------------------
-
-The calling point called “AfterPredictorAfterHVACManagers� occurs after the predictor and after the traditional HVAC managers have been called. It occurs at each timestep after the predictor executes and after the SetpointManager and AvailabilityManager models are called. It is useful for a variety of control actions. However, if there are conflicts, SetpointManager or AvailabilityManager actions may be overwritten by EMS control actions.
-
-Inside HVAC System Iteration Loop
----------------------------------
-
-The calling point called “InsideHVACSystemIterationLoop� occurs before HVAC systems are modeled. Within a timestep, EnergyPlus loops over the HVAC model to solve a system of systems. It recurs after each HVAC system iteration within each timestep and can be used for a variety of control actions that affect system operation. Being within the iteration loop can increase the accuracy of control modeling when the inputs to the controls are also changing interactively. The disadvantage is extra computational expense.
-
-End of Zone Timestep Before Reporting
--------------------------------------
-
-The calling point called “EndOfZoneTimestepBeforeZoneReporting� occurs near the end of a zone timestep but before output variable reporting is finalized. It is useful for custom output variables that use the ZoneTimestep reporting frequency.
-
-End of Zone Timestep After Reporting
-------------------------------------
-
-The calling point called “EndOfZoneTimestepAfterZoneReporting� occurs at the end of a zone timestep after output variable reporting is finalized. It is useful for preparing calculations that will go into effect the next timestep. Its capabilities are similar to BeginTimestepBeforePredictor, except that input data for current time, date, and weather data align with different timesteps.
-
-End of System Timestep Before HVAC Reporting
---------------------------------------------
-
-The calling point called “EndOfSystemTimestepBeforeHVACReporting� occurs near the end of a system timestep but before output variable reporting is finalized. It is useful for custom output variables that use the SystemTimestep reporting frequency.
-
-End of System Timestep After HVAC Reporting
--------------------------------------------
-
-The calling point called “EndOfSystemTimestepAfterHVACReporting� occurs at the end of a system timestep after output variable reporting is finalized.
-
-End of Zone Sizing
-------------------
-
-The calling point called “EndOfZoneSizing� is used to alter the results of zone sizing calculations. It executes only once per simulation during the early stages and only if the model includes zone sizing calculations. It is not useful for control applications.
-
-End of System Sizing
---------------------
-
-The calling point called “EndOfSystemSizing� is used to alter the results of air system sizing calculations. It executes only once per simulation and is not useful for control applications.
-
-After Component Model Input has Been Read In
---------------------------------------------
-
-The calling point called “AfterComponentInputReadIn� is used to alter the results of individual autosize fields.  It executes whenever one of the selected components has finished reading in its input data.  Those, and only those, component models that have some type of actuator with an “Autosized� control type will also have this calling point.  This same calling point identifier is used for different HVAC components so programs executed from this point will be repeated.  Currently this calling point exists in three different places:  (1) after DX coil input, (2) after fan input, and (3) after unitary system input.
-
-User Defined Component Model
-----------------------------
-
-The calling point called “UserDefinedComponentModel� is used with Erl programs that are associated with user defined component models.  This calling point is executed whenever a user-defined component model is called to simulate.  The user defined component models track which program calling managers are associated with the specific component and only those calling managers are executed when this calling point is triggered. This calling point is only used with calling managers referenced by the following input objects: PlantComponent:UserDefined, Coil:UserDefined, ZoneHVAC:ForcedAir:UserDefined, or AirTerminal:SingleDuct:UserDefined.
-
-User-Defined Component Models
-=============================
-
-This section provides an overview of how you can use EMS to create your own custom models for HVAC and plant equipment.  EMS can be used not only for controls and overriding the behavior of existing models, but also to implement entirely new component models of your own formulation.  Such user-defined component models are implemented by writing Erl programs, setting up internal variables, sensors, actuators and output variables that work in conjunction with a set of special input objects in the group called “User Defined HVAC and Plant Component Models.�
-
-This system provides a means of modeling new types of equipment that do not yet have models implemented in EnergyPlus.  The capability to add new custom models should have a wide variety of creative applications such as evaluating the annual energy performance implications of new types of equipment and providing a mechanism for including “exceptional calculation methods� in your EnergyPlus models.
-
-This section first introduces common characteristics of the user-defined component models and then goes into more detail on each of available component modeling shells that are used to connect user-defined models and algorithms to the rest of EnergyPlus’ HVAC and plant simulations.
-
-Common Characteristics
-----------------------
-
-In general, each of the user-defined components will:
-
-- Setup new EMS internal variables for the state conditions entering the component at each inlet node being used.  Internal variables serve a similar role as Sensors in terms of obtaining input data.  The difference is that they are updated just before the component model programs execute and therefore do not suffer the timestep lag issues that can be associated with sensors tied to output variables.  Whereas most EMS internal variables are constants, those intended for use with user-defined components are filled each time the component is simulated and vary over time with the most current data available.
-
-- Setup new EMS actuators for the state conditions at each outlet node being used.  These actuators are not optional and must be used.  For each air or plant connection with an active outlet node, the associated actuators must be used and filled with valid values in order for the component model to be properly coupled to the rest of EnergyPlus.  Some of the components will also set the results at their inlet node, for example to request a mass flow rate.
-
-- Trigger one or more specific program calling manager(s) to execute EMS programs that are called to initialize, register, and size the component model.
-
-- Trigger one or more specific program calling manager(s) to execute EMS programs that are called to actually model the component when it is called to be simulated.
-
-The various user-defined components have some similar input fields.  Once the user gains familiarity with one of the components, many of the concepts will carry over to the other user-defined components.  The separate objects are primarily for the purpose of distinguishing how user-defined components need to vary in order to fit with the rest of EnergyPlus.
-
-
-
-Zone Forced Air Unit
---------------------
-
-The input object called ZoneHVAC:ForcedAir:UserDefined provides a shell for creating custom models of a device that serves as a single-zone HVAC unit that operates by circulating air in and out of the zone.  This device is analogous to those component models in the Group -- Zone Forced Air Units, such as ZoneHVAC:PackagedTerminalAirConditioner or ZoneHVAC:WaterToAirHeatPump.
-
-In addition to the primary air connection that connects to the zone, there are options for additional connections to a second air stream (e.g. for outdoor ventilation or heat source or sink), up to three separate plant loop connections (e.g. hot water, chilled water, heat rejection), a water supply tank, a water collection tank, and a separate zone for skin losses.
-
-The zone unit is associated with a thermal zone (by the ZoneHVAC:EquipmentConnections and ZoneHVAC:EquipmentList objects).  In EnergyPlus, when there are controlled thermal zones with thermostat (and humidistat) controls, the central routines predict the loads that zone equipment need to meet in order to maintain control of the zone conditions.  When there are multiple types of equipment serving a zone, they are sequenced to meet heating or cooling loads in a particular order.  Rather than the total predicted load, the second or third devices need to know the load that remains after the earlier-sequenced devices have already operated on the zone.  The following internal variables are useful inputs for controlling zone equipment in your models:
-
-- An internal variable called “Remaining Sensible Load to Heating Setpoint� provides the current value for the sensible load, in [W], that remains for this device that if delivered will allow the zone to reach the heating setpoint under current conditions.
-
-- An internal variable called “Remaining Sensible Load to Cooling Setpoint� provides the current value for the sensible load, in [W], that remains for this device that if delivered will allow the zone to reach the cooling setpoint under current conditions.
-
-- An internal variable called “Remaining Latent Load to Humidifying Setpoint� provides the current value for the latent load, in [kg/s], that remains for this device that if delivered will allow the zone to reach the humidification setpoint under current conditions.
-
-- An internal variable called “Remaining Latent Load to Dehumidifying Setpoint� provides the current value for the latent load, in [kg/s], that remains for this device that if delivered will allow the zone to reach the dehumidification setpoint under current conditions.
-
-
-
-### Primary Air Connection
-
-The primary air connection includes both an inlet and an outlet that are required to be used when using this component.  This is called the primary air connection because it is how the zone unit is connected to the zone.  The inlet to the custom zone unit is a node that is also an exhaust outlet from the zone.  The following EMS internal variables are made available for this inlet node and should be useful inputs to your own custom models:
-
-- An internal variable called “Inlet Temperature for Primary Air Connection,� provides the current value for the drybulb air temperature at the component’s inlet node, in [C].
-
-- An internal variable called “Inlet Humidity Ratio for Primary Air Connection,� provides the current value for the moist air humidity ratio at the component’s inlet node, in [kgWater/kgDryAir]
-
-- An internal variable called “Inlet Density for Primary Air Connection,� provides the current value for the density of moist air at the component’s main inlet node, in [kg/m<sup>3</sup>].
-
-- An internal variable called “Inlet Specific Heat for Primary Air Connection,� provides the current value for the specific heat of moist air at the component’s main inlet node, in [J/kg-C].
-
-The inlet node also has an actuator associated with it so that the rate of air flow leaving the thermal zone and entering the unit can be passed to the rest of EnergyPlus.
-
-- An actuator called “Primary Air Connection,� with the control type “Inlet Mass Flow Rate,� in [kg/s], needs to be used.  This will set the flow rate of air leaving the zone through the zone exhaust air node.
-
-The primary outlet for the custom zone unit is a node that is also an inlet to the zone.  The following EMS actuators are created for this outlet node and must be used to pass results from the custom model to the rest of EnergyPlus:
-
-- An actuator called “Primary Air Connection,� with the control type “Outlet Temperature,� in [C], needs to be used.  This will set the drybulb temperature of the air leaving the zone unit and entering the zone through the zone air inlet node.
-
-- An actuator called “Primary Air Connection,� with the control type “Outlet Humidity Ratio,� in [kgWater/kgDryAir], needs to be used.  This will set the humidity ratio of the air leaving the zone unit and entering the zone through the zone air inlet node.
-
-- An actuator called “Primary Air Connection,� with the control type “Outlet Mass Flow Rate,� in [kg/s], needs to be used.  This will set the flow rate of air leaving the zone unit and entering the zone through the zone air inlet node.
-
-It is not required that the primary air connections inlet and outlet mass flow rates be identical.  However, if there is an imbalance, then the model should use the secondary air connection to balance air mass flows.
-
-### Secondary Air Connection
-
-The secondary air connection provides options for an added inlet node, or outlet node, or both depending on the user’s needs.  This separate air stream can be used for outdoor air ventilation or as a source or sink for energy.  The secondary air inlet node will often be defined to be an outdoor air node (ref. OutdoorAir:Node) but that is not required.  The secondary air outlet node can be used as relief exhaust when the unit is providing outdoor air ventilation.  If the secondary air outlet is not really connected to anything else and just releases air to the outdoors, then it isn’t necessary that moist air properties be set using actuators because they will not impact anything else in the model.
-
-If the secondary air connection inlet node is used, then the following internal variables and actuator are made available:
-
-- An internal variable called “Inlet Temperature for Secondary Air Connection,� provides the current value for the drybulb air temperature at the secondary inlet node, in [C].
-
-- An internal variable called “Inlet Humidity Ratio for Secondary Air Connection,� provides the current value for the moist air humidity ratio at the secondary inlet node, in [kgWater/kgDryAir]
-
-- An internal variable called “Inlet Density for Secondary Air Connection,� provides the current value for the density of moist air at the secondary inlet node, in [kg/m<sup>3</sup>].
-
-- An internal variable called “Inlet Specific Heat for Secondary Air Connection,� provides the current value for the specific heat of moist air at the secondary inlet node, in [J/kg-C].
-
-- An actuator called “Secondary Air Connection,� with the control type “Inlet Mass Flow Rate,� in [kg/s], needs to be used.  This will set the flow rate of air entering the zone unit through the secondary air connection inlet.
-
-If the secondary air connection outlet node is used, then the following actuators are created:
-
-- An actuator called “Secondary Air Connection,� with the control type “Outlet Temperature,� in [C], needs to be used.  This will set the drybulb temperature of the air leaving the zone unit through the secondary air outlet node.
-
-- An actuator called “Secondary Air Connection,� with the control type “Outlet Humidity Ratio,� in [kgWater/kgDryAir], needs to be used.  This will set the humidity ratio of the air leaving the zone unit through the secondary air outlet node.
-
-- An actuator called “Secondary Air Connection,� with the control type “Outlet Mass Flow Rate,� in [kg/s], needs to be used.  This will set the flow rate of air leaving the zone unit through the secondary air outlet node.
-
-### Plant Connections
-
-The user defined zone unit can also be connected to up to three different plants to provide hydronic-based cooling, heating, and/or heat source or rejection.
-
-Although the zone unit actively conditions the zone, from the point of view of plant they are demand components.  These plant connections are always “demand� in the sense that the zone unit will place loads onto the plant loops serving it and are not configured to be able to meet plant loads in the way that supply equipment could (loading mode is always DemandsLoad).  These plant connections are always of the type that when flow is requested, the loop will be operated to try and meet the flow request and if not already running, these flow requests can turn on the loop (loop flow request mode is always NeedsFlowAndTurnsLoopOn).
-
-For plant loops, both the inlet and outlet nodes need to be used for each loop connection.  The ZoneHVAC:ForcedAir:UserDefined object appears directly on the Branch object used to describe the plant.  The central plant routines require that each plant component be properly initialized and registered. Special actuators are provided for these initializations and they should be filled with values by the Erl programs that are called by the program calling manager assigned to the zone unit for model setup and sizing.  The following three actuators are created for each of “*N*� plant loops and must be used to properly register the plant connection:
-
-- An actuator called “Plant Connection *N*� with the control type “Minimum Mass Flow Rate,� in [kg/s], should be used.  This will set the so-called hardware limit for component’s minimum mass flow rate when operating.  (If not used, then the limit will be set to zero which may be okay for many if not most models.)
-
-- An actuator called “Plant Connection *N*� with the control type “Maximum Mass Flow Rate,� in [kg/s], needs to be used.  This will set the so-called hardware limit for the component’s maximum mass flow rate when operating.
-
-- An actuator called “Plant Connection *N*� with the control type “Design Volume Flow Rate,� in [m<sup>3</sup>/s], needs to be used.  This will register the size of the component for use in sizing the plant loop and supply equipment that will need to meet the loads.
-
-For each plant loop connection that is used, the following internal variables are available for inputs to the custom component model:
-
-- An internal variable called “Inlet Temperature for Plant Connection *N*� provides the current value for the temperature of the fluid entering the component, in [C].
-
-- An internal variable called “Inlet Mass Flow Rate for Plant Connection *N*� provides the current value for the mass flow rate of the fluid entering the component, in [kg/s].
-
-- An internal variable called “Inlet Density for Plant Connection *N*� provides the current value for the density of the fluid entering the component, in [kg/m<sup>3</sup>].  This density is sensitive to the fluid type (e.g. if using glycol in the plant loop) and fluid temperature at the inlet.
-
-- An internal variable called “Inlet Specific Heat for Plant Connection *N*� provides the current value for the specific heat of the fluid entering the component, in [J/kg-C]. This specific heat is sensitive to the fluid type (e.g. if using glycol in the plant loop) and fluid temperature at the inlet.
-
-For each plant loop connection that is used, the following EMS actuators are created and must be used to pass results from the custom model to the rest of EnergyPlus:
-
-- An actuator called “Plant Connection *N*� with the control type “Outlet Temperature,� in [C], needs to be used.  This is the temperature of the fluid leaving the zone unit through that particular plant connection.
-
-- An actuator called “Plant Connection N� with the control type “Mass Flow Rate,� in kg/s, needs to be used. This actuator registers the component model’s request for plant fluid flow.  The actual mass flow rate through the component may be different than requested if the overall loop situation is such that not enough flow is available to meet all the various requests.  In general, this actuator is used to lodge a request for flow, but the more accurate flow rate will be the internal variable called “Inlet Mass Flow Rate for Plant Connection *N.*�
-
-### Water Use
-
-The user defined zone unit can be connected to the water use models in EnergyPlus that allow modeling on-site storage.  If a supply inlet water storage tank is used, then an actuator called “Water System� with the control type “Supplied Volume Flow Rate,� in m<sup>3</sup>/s, needs to be used.  This sets up the zone unit as a demand component for that storage tank.  If a collection outlet water storage tank is used, then an actuator called “Water System� with the control type “Collected Volume Flow Rate,� in m<sup>3</sup>/s, needs to be used.
-
-### Ambient Zone
-
-The user defined zone unit can be connected to an ambient zone and provide internal gains to that zone.  The zone can be different than the one that unit is connected to via the primary air connection if desired.  This is for “skin losses� that the unit might have that result from inefficiencies and other non-ideal behavior.  When an ambient zone is specified, the following actuators are created that can be used for different types of internal gains to the named zone:
-
-- An actuator called “Component Zone Internal Gain� with the control type “Sensible Heat Gain Rate,� in [W], is available.  This can be used for purely convective sensible heat gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Return Air Heat Gain Rate,� in [W], is available.  This can be used for purely convective sensible heat gains (or losses) to the return air duct for a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Thermal Radiation Heat Gain Rate,� in [W], is available.  This can be used for thermal radiation gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Latent Heat Gain Rate,’ in [W], is available.  This can be used for latent moisture gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Return Air Latent Heat Gain Rate,� in [W], is available.  This can be used for latent moisture gains (or losses) to a the return air duct for a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Carbon Dioxide Gain Rate,� in [m<sup>3</sup>/s], is available.  This can be used for carbon dioxide gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Gaseous Contaminant Gain Rate,� in [m<sup>3</sup>/s], is available.  This can be used for generic gaseous air pollutant gains (or losses) to a zone.
-
-Air Terminal Unit
------------------
-
-The input object called AirTerminal:SingleDuct:UserDefined provides a shell for creating custom models for an air terminal that connects a multi-zone air handler to a thermal zone.  This device is analogous to the single-duct terminal units in the Group – Air Distribution Equipment, such as AirTerminal:SingleDuct:VAV:Reheat or AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction.
-
-In addition to the primary air connection that connects from the air loop to the zone, there are options for additional connections to a second air stream (e.g. for outdoor ventilation or heat source or sink), up to two separate plant loop connections (e.g. hot water and chilled water), a water supply tank, a water collection tank, and a separate zone for skin losses.
-
-The air terminal unit is a associated with a thermal zone (by the ZoneHVAC:EquipmentConnections, ZoneHVAC:EquipmentList, and ZoneHVAC:AirDistributionUnit objects).  In EnergyPlus, when there are controlled thermal zones with thermostat (and humidistat) controls, the central routines predict the loads that zone equipment need to meet in order to maintain control of the zone conditions.  When there are multiple types of equipment serving a zone, they are sequenced to meet heating or cooling loads in a particular order.  Rather than the total predicted load, the second or third devices need to know the load that remains after the earlier-sequenced devices have already operated on the zone.  The following internal variables are useful inputs for controlling zone equipment in your models:
-
-- An internal variable called “Remaining Sensible Load to Heating Setpoint� provides the current value for the sensible load, in [W], that remains for this device that if delivered will allow the zone to reach the heating setpoint under current conditions.
-
-- An internal variable called “Remaining Sensible Load to Cooling Setpoint� provides the current value for the sensible load, in [W], that remains for this device that if delivered will allow the zone to reach the cooling setpoint under current conditions.
-
-- An internal variable called “Remaining Latent Load to Humidifying Setpoint� provides the current value for the latent load, in [kg/s], that remains for this device that if delivered will allow the zone to reach the humidification setpoint under current conditions.
-
-- An internal variable called “Remaining Latent Load to Dehumidifying Setpoint� provides the current value for the latent load, in [kg/s], that remains for this device that if delivered will allow the zone to reach the dehumidification setpoint under current conditions.
-
-### Primary Air Connection
-
-The primary air connection includes both an inlet and an outlet that are required to be used when using this component.  This called the primary air connection because it is how the terminal unit is connected from the air handle to the zone.  The inlet to the custom air terminal unit is a node that is also the outlet from an AirLoopHVAC:ZoneSplitter object.  The following EMS internal variables are made available for this inlet node and should be useful inputs to your own custom models:
-
-- An internal variable called “Inlet Temperature for Primary Air Connection,� provides the current value for the drybulb air temperature at the component’s inlet node, in [C].
-
-- An internal variable called “Inlet Humidity Ratio for Primary Air Connection,� provides the current value for the moist air humidity ratio at the component’s inlet node, in [kgWater/kgDryAir]
-
-- An internal variable called “Inlet Density for Primary Air Connection,� provides the current value for the density of moist air at the component’s main inlet node, in [kg/m<sup>3</sup>].
-
-- An internal variable called “Inlet Specific Heat for Primary Air Connection,� provides the current value for the specific heat of moist air at the component’s main inlet node, in [J/kg-C].
-
-The inlet node also has an actuator associated with it so that the rate of air flow leaving the thermal zone and entering the unit can be passed to the rest of EnergyPlus.
-
-- An actuator called “Primary Air Connection,� with the control type “Inlet Mass Flow Rate,� in [kg/s], needs to be used.  This will set the flow rate of air leaving the zone splitter and entering the air terminal unit.
-
-The primary outlet for the custom air terminal unit is a node that is also an inlet to the zone.  The following EMS actuators are created for this outlet node and must be used to pass results from the custom model to the rest of EnergyPlus:
-
-- An actuator called “Primary Air Connection,� with the control type “Outlet Temperature,� in [C], needs to be used.  This will set the drybulb temperature of the air leaving the air terminal unit and entering the zone through the zone air inlet node.
-
-- An actuator called “Primary Air Connection,� with the control type “Outlet Humidity Ratio,� in [kgWater/kgDryAir], needs to be used.  This will set the humidity ratio of the air leaving the air terminal unit and entering the zone through the zone air inlet node.
-
-- An actuator called “Primary Air Connection,� with the control type “Outlet Mass Flow Rate,� in [kg/s], needs to be used.  This will set the flow rate of air leaving the air terminal unit and entering the zone through the zone air inlet node.
-
-It is not required that the primary air connections inlet and outlet mass flow rates be identical.  However, if there is an imbalance, then the model should use the secondary air connection to balance air mass flows.
-
-### Secondary Air Connection
-
-The secondary air connection provides options for an added inlet node, or outlet node, or both depending on the user’s needs.  This separate air stream can be used for outdoor air ventilation or as a source or sink for energy.  The secondary air inlet node will often be defined to be an outdoor air node (ref. OutdoorAir:Node) but that is not required.  The secondary air outlet node can be used as relief exhaust when the unit is providing outdoor air ventilation.  If the secondary air outlet is not really connected to anything else and just releases air to the outdoors, then it isn’t necessary that moist air properties be set using actuators because they will not impact anything else in the model.
-
-If the secondary air connection inlet node is used, then the following internal variables and actuator are made available:
-
-- An internal variable called “Inlet Temperature for Secondary Air Connection,� provides the current value for the drybulb air temperature at the secondary inlet node, in [C].
-
-- An internal variable called “Inlet Humidity Ratio for Secondary Air Connection,� provides the current value for the moist air humidity ratio at the secondary inlet node, in [kgWater/kgDryAir]
-
-- An internal variable called “Inlet Density for Secondary Air Connection,� provides the current value for the density of moist air at the secondary inlet node, in [kg/m<sup>3</sup>].
-
-- An internal variable called “Inlet Specific Heat for Secondary Air Connection,� provides the current value for the specific heat of moist air at the secondary inlet node, in [J/kg-C].
-
-- An actuator called “Secondary Air Connection,� with the control type “Inlet Mass Flow Rate,� in [kg/s], needs to be used.  This will set the flow rate of air entering the air terminal unit through the secondary air connection inlet.
-
-If the secondary air connection outlet node is used, then the following actuators are created:
-
-- An actuator called “Secondary Air Connection,� with the control type “Outlet Temperature,� in [C], needs to be used.  This will set the drybulb temperature of the air leaving the air terminal unit through the secondary air outlet node.
-
-- An actuator called “Secondary Air Connection,� with the control type “Outlet Humidity Ratio,� in [kgWater/kgDryAir], needs to be used.  This will set the humidity ratio of the air leaving the air terminal unit through the secondary air outlet node.
-
-- An actuator called “Secondary Air Connection,� with the control type “Outlet Mass Flow Rate,� in [kg/s], needs to be used.  This will set the flow rate of air leaving the air terminal unit through the secondary air outlet node.
-
-### Plant Connections
-
-The user defined air terminal unit can also be connected to up to two different plants to provide hydronic-based cooling, heating, or heat source or rejection.
-
-Although the air terminal unit actively conditions the zone, from the point of view of plant they are demand components.  These plant connections are always “demand� in the sense that the air terminal unit will place loads onto the plant loops serving it and are not configured to be able to meet plant loads in the way that supply equipment could (loading mode is always DemandsLoad).  These plant connections are always of the type that when flow is requested, the loop will be operated to try and meet the flow request and if not already running, these flow requests can turn on the loop (loop flow request mode is always NeedsFlowAndTurnsLoopOn).
-
-For plant loops, both the inlet and outlet nodes need to be used for each loop connection.  The AirTerminal:SingleDuct:UserDefined object appears directly on the Branch object used to describe the plant.  The central plant routines require that each plant component be properly initialized and registered. Special actuators are provided for these initializations and they should be filled with values by the Erl programs that are called by the program calling manager assigned to the air terminal unit for model setup and sizing.  The following three actuators are created for each of “*N*� plant loops and must be used to properly register the plant connection:
-
-- An actuator called “Plant Connection *N*� with the control type “Minimum Mass Flow Rate,� in [kg/s], should be used.  This will set the so-called hardware limit for component’s minimum mass flow rate when operating.  (If not used, then the limit will be set to zero which may be okay for many if not most models.)
-
-- An actuator called “Plant Connection *N*� with the control type “Maximum Mass Flow Rate,� in [kg/s], needs to be used.  This will set the so-called hardware limit for the component’s maximum mass flow rate when operating.
-
-- An actuator called “Plant Connection *N*� with the control type “Design Volume Flow Rate,� in [m<sup>3</sup>/s], needs to be used.  This will register the size of the component for use in sizing the plant loop and supply equipment that will need to meet the loads.
-
-For each plant loop connection that is used, the following internal variables are available for inputs to the custom component model:
-
-- An internal variable called “Inlet Temperature for Plant Connection *N*� provides the current value for the temperature of the fluid entering the component, in [C].
-
-- An internal variable called “Inlet Mass Flow Rate for Plant Connection *N*� provides the current value for the mass flow rate of the fluid entering the component, in [kg/s].
-
-- An internal variable called “Inlet Density for Plant Connection *N*� provides the current value for the density of the fluid entering the component, in [kg/m<sup>3</sup>].  This density is sensitive to the fluid type (e.g. if using glycol in the plant loop) and fluid temperature at the inlet.
-
-- An internal variable called “Inlet Specific Heat for Plant Connection *N*� provides the current value for the specific heat of the fluid entering the component, in [J/kg-C]. This specific heat is sensitive to the fluid type (e.g. if using glycol in the plant loop) and fluid temperature at the inlet.
-
-For each plant loop connection that is used, the following EMS actuators are created and must be used to pass results from the custom model to the rest of EnergyPlus:
-
-- An actuator called “Plant Connection *N*� with the control type “Outlet Temperature,� in [C], needs to be used.  This is the temperature of the fluid leaving the air terminal unit through that particular plant connection.
-
-- An actuator called “Plant Connection *N*� with the control type “Mass Flow Rate,� in kg/s, needs to be used. This actuator registers the component model’s request for plant fluid flow.  The actual mass flow rate through the component may be different than requested if the overall loop situation is such that not enough flow is available to meet all the various requests.  In general, this actuator is used to lodge a request for flow, but the more accurate flow rate will be the internal variable called “Inlet Mass Flow Rate for Plant Connection *N.*�
-
-### Water Use
-
-The user defined air terminal unit can be connected to the water use models in EnergyPlus that allow modeling on-site storage.  If a supply inlet water storage tank is used, then an actuator called “Water System� with the control type “Supplied Volume Flow Rate,� in m<sup>3</sup>/s, needs to be used.  This sets up the air terminal unit as a demand component for that storage tank.  If a collection outlet water storage tank is used, then an actuator called “Water System� with the control type “Collected Volume Flow Rate,� in m<sup>3</sup>/s, needs to be used.
-
-### Ambient Zone
-
-The user defined air terminal unit can be connected to an ambient zone and provide internal gains to that zone.  The zone can be different than the one that unit is connected to via the primary air connection if desired.  This is for “skin losses� that the unit might have that result from inefficiencies and other non-ideal behavior.  When an ambient zone is specified, the following actuators are created that can be used for different types of internal gains to the named zone:
-
-- An actuator called “Component Zone Internal Gain� with the control type “Sensible Heat Gain Rate,� in [W], is available.  This can be used for purely convective sensible heat gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Return Air Heat Gain Rate,� in [W], is available.  This can be used for purely convective sensible heat gains (or losses) to the return air duct for a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Thermal Radiation Heat Gain Rate,� in [W], is available.  This can be used for thermal radiation gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Latent Heat Gain Rate,’ in [W], is available.  This can be used for latent moisture gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Return Air Latent Heat Gain Rate,� in [W], is available.  This can be used for latent moisture gains (or losses) to a the return air duct for a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Carbon Dioxide Gain Rate,� in [m<sup>3</sup>/s], is available.  This can be used for carbon dioxide gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Gaseous Contaminant Gain Rate,� in [m<sup>3</sup>/s], is available.  This can be used for generic gaseous air pollutant gains (or losses) to a zone.
-
-
-
-Air Coil
---------
-
-The input object called Coil:UserDefined provides a shell for creating custom models for a coil that processes air as part of an air handler.  This device is analogous to coils models such as Coil:Cooling:Water, Coil:Heating:Water, and Coil:Cooling:DX:SingleSpeed, but can also be used for heat-exchanger-like devices such as HeatExchanger:AirToAir:SensibleAndLatent or EvaporativeCooler:Indirect:WetCoil.
-
-The user defined coil model can use one or two air connections, one optional plant connection, a water supply tank, a water collection tank, and a separate zone for skin losses.
-
-### Air Connections
-
-Each of the two air connections that are available include both an inlet and an outlet node that are required for each air connection that is used.  The Coil:UserDefined object appears directly on a Branch object used to define the supply side of an air handler, or in the AirLoopHVAC:OutdoorAirSystem:EquipmentList object used to define outdoor air systems.  The following EMS internal variables are made available for each inlet node and should be useful inputs to your own custom models:
-
-- An internal variable called “Inlet Temperature for Air Connection *N*,� provides the current value for the drybulb air temperature at the component’s inlet node, in [C].
-
-- An internal variable called “Inlet Humidity Ratio for Air Connection *N*,� provides the current value for the moist air humidity ratio at the component’s inlet node, in [kgWater/kgDryAir]
-
-- An internal variable called “Inlet Density for Air Connection *N*,� provides the current value for the density of moist air at the component’s main inlet node, in [kg/m<sup>3</sup>].
-
-- An internal variable called “Inlet Specific Heat for Air Connection *N*,� provides the current value for the specific heat of moist air at the component’s main inlet node, in [J/kg-C].
-
-The following EMS actuators are created for each outlet node and must be used to pass results from the custom model to the rest of EnergyPlus:
-
-- An actuator called “Air Connection *N*,� with the control type “Outlet Temperature,� in [C], needs to be used.  This will set the drybulb temperature of the air leaving the coil.
-
-- An actuator called “Air Connection *N*,� with the control type “Outlet Humidity Ratio,� in [kgWater/kgDryAir], needs to be used.  This will set the humidity ratio of the air leaving the coil.
-
-- An actuator called “Air Connection *N*,� with the control type “Outlet Mass Flow Rate,� in [kg/s], needs to be used.  This will set the flow rate of air leaving the coil.
-
-### Plant Connections
-
-The user defined coil can also be connected to one plant loop to provide hydronic-based cooling, heating, or heat source or rejection.
-
-Although the coil actively conditions the air stream passing through it, from the point of view of plant it is a demand component.  This plant connection is always “demand� in the sense that the coil will place loads onto the plant loop serving it and is not configured to be able to meet plant loads in the way that supply equipment could (loading mode is always DemandsLoad).  This plant connection is always of the type that when flow is requested, the loop will be operated to try and meet the flow request and if not already running, these flow requests can turn on the loop (loop flow request mode is always NeedsFlowAndTurnsLoopOn).
-
-Both the inlet and outlet nodes need to be used is a loop is connected.  The Coil:UserDefined object appears directly on the Branch object used to describe the plant.  The central plant routines require that each plant component be properly initialized and registered. Special actuators are provided for these initializations and they should be filled with values by the Erl programs that are called by the program calling manager assigned to the coil for model setup and sizing.  The following three actuators are created for the plant loop and must be used to properly register the plant connection:
-
-- An actuator called “Plant Connection� with the control type “Minimum Mass Flow Rate,� in [kg/s], should be used.  This will set the so-called hardware limit for component’s minimum mass flow rate when operating.  (If not used, then the limit will be set to zero which may be okay for many if not most models.)
-
-- An actuator called “Plant Connection� with the control type “Maximum Mass Flow Rate,� in [kg/s], needs to be used.  This will set the so-called hardware limit for the component’s maximum mass flow rate when operating.
-
-- An actuator called “Plant Connection� with the control type “Design Volume Flow Rate,� in [m<sup>3</sup>/s], needs to be used.  This will register the size of the component for use in sizing the plant loop and supply equipment that will need to meet the loads.
-
-When the plant loop connection is used, the following internal variables are available for inputs to the custom component model:
-
-- An internal variable called “Inlet Temperature for Plant Connection� provides the current value for the temperature of the fluid entering the component, in [C].
-
-- An internal variable called “Inlet Mass Flow Rate for Plant Connection� provides the current value for the mass flow rate of the fluid entering the component, in [kg/s].
-
-- An internal variable called “Inlet Density for Plant Connection� provides the current value for the density of the fluid entering the component, in [kg/m<sup>3</sup>].  This density is sensitive to the fluid type (e.g. if using glycol in the plant loop) and fluid temperature at the inlet.
-
-- An internal variable called “Inlet Specific Heat for Plant Connection� provides the current value for the specific heat of the fluid entering the component, in [J/kg-C]. This specific heat is sensitive to the fluid type (e.g. if using glycol in the plant loop) and fluid temperature at the inlet.
-
-When the plant loop connection is used, the following EMS actuators are created and must be used to pass results from the custom model to the rest of EnergyPlus:
-
-- An actuator called “Plant Connection� with the control type “Outlet Temperature,� in [C], needs to be used.  This is the temperature of the fluid leaving the coil.
-
-- An actuator called “Plant Connection� with the control type “Mass Flow Rate,� in kg/s, needs to be used. This actuator registers the component model’s request for plant fluid flow.  The actual mass flow rate through the component may be different than requested if the overall loop situation is such that not enough flow is available to meet all the various requests.  In general, this actuator is used to lodge a request for flow, but the more accurate flow rate will be the internal variable called “Inlet Mass Flow Rate for Plant Connection*.*�
-
-### Water Use
-
-The user defined coil can be connected to the water use models in EnergyPlus that allow modeling on-site storage.  If a supply inlet water storage tank is used, then an actuator called “Water System� with the control type “Supplied Volume Flow Rate,� in m<sup>3</sup>/s, needs to be used.  This sets up the coil as a demand component for that storage tank.  If a collection outlet water storage tank is used, then an actuator called “Water System� with the control type “Collected Volume Flow Rate,� in m<sup>3</sup>/s, needs to be used.
-
-### Ambient Zone
-
-The user defined coil can be connected to an ambient zone and provide internal gains to that zone.  This is for “skin losses� that the coil might have that result from inefficiencies and other non-ideal behavior.  When an ambient zone is specified, the following actuators are created that can be used for different types of internal gains to the named zone:
-
-- An actuator called “Component Zone Internal Gain� with the control type “Sensible Heat Gain Rate,� in [W], is available.  This can be used for purely convective sensible heat gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Return Air Heat Gain Rate,� in [W], is available.  This can be used for purely convective sensible heat gains (or losses) to the return air duct for a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Thermal Radiation Heat Gain Rate,� in [W], is available.  This can be used for thermal radiation gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Latent Heat Gain Rate,’ in [W], is available.  This can be used for latent moisture gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Return Air Latent Heat Gain Rate,� in [W], is available.  This can be used for latent moisture gains (or losses) to a the return air duct for a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Carbon Dioxide Gain Rate,� in [m<sup>3</sup>/s], is available.  This can be used for carbon dioxide gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Gaseous Contaminant Gain Rate,� in [m<sup>3</sup>/s], is available.  This can be used for generic gaseous air pollutant gains (or losses) to a zone.
-
-
-
-Plant Component
----------------
-
-The input object called PlantComponent:UserDefined provides a shell for creating custom models of a device that is part of the plant models used for hydronic-type systems.  This object can be used for primary heating or cooling devices, such as boilers or chillers.
-
-Although the other user-defined component models can also connect to plant, they are always simple “demand� components (from the point of view of plant modeling) and their calls to simulate are led by the air side portions of the program’s calling tree.  The plant-centric component here however, is called to simulate along with other plant components (in flow order) by plant’s central routines.
-
-The user defined plant component can use up to four different plant loop connections, one optional air connection, a water supply tank, a water collection tank, and an ambient zone for skin losses.
-
-### Plant Connections
-
-The user defined plant component can be connected to up to four different plant loops.
-
-For plant loops, both the inlet and outlet nodes need to be used for each loop connection.  The PlantComponent:UserDefined object appears directly on the Branch object used to describe the plant.  The central plant routines require that each plant component be properly initialized and registered. Special actuators are provided for these initializations and they should be filled with values by the Erl programs that are called by the program calling manager assigned to that particular loop connection for model setup and sizing.  The following six actuators are created for each of “*N*� plant loops and must be used to properly register the plant connection:
-
-- An actuator called “Plant Connection *N*� with the control type “Minimum Mass Flow Rate,� in [kg/s], should be used.  This will set the so-called hardware limit for component’s minimum mass flow rate when operating.  (If not used, then the limit will be set to zero which may be okay for many if not most models.)
-
-- An actuator called “Plant Connection *N*� with the control type “Maximum Mass Flow Rate,� in [kg/s], needs to be used.  This will set the so-called hardware limit for the component’s maximum mass flow rate when operating.
-
-- An actuator called “Plant Connection *N*� with the control type “Design Volume Flow Rate,� in [m<sup>3</sup>/s], needs to be used.  This will register the size of the component for use in sizing the plant loop and supply equipment that will need to meet the loads.
-
-- An actuator called “Plant Connection *N*� with the control type “Minimum Loading Capacity,� in [W], needs to be used if the device is to be used as a supply component with load-based operation schemes.
-
-- An actuator called “Plant connection *N*� with the control type “Maximum Loading Capacity,� in [W], needs to be used if the device is to be used as a supply component with load-based operation schemes.
-
-- An actuator called “Plant Connection *N*� with the control type “Optimal Loading Capacity,� in [W], needs to be used if the device is to be used as a supply component with load-based operation schemes.
-
-For each plant loop connection that is used, the following internal variables are available for inputs to the custom component model:
-
-- An internal variable called “Inlet Temperature for Plant Connection *N*� provides the current value for the temperature of the fluid entering the component, in [C].
-
-- An internal variable called “Inlet Mass Flow Rate for Plant Connection *N*� provides the current value for the mass flow rate of the fluid entering the component, in [kg/s].
-
-- An internal variable called “Inlet Density for Plant Connection *N*� provides the current value for the density of the fluid entering the component, in [kg/m<sup>3</sup>].  This density is sensitive to the fluid type (e.g. if using glycol in the plant loop) and fluid temperature at the inlet.
-
-- An internal variable called “Inlet Specific Heat for Plant Connection *N*� provides the current value for the specific heat of the fluid entering the component, in [J/kg-C]. This specific heat is sensitive to the fluid type (e.g. if using glycol in the plant loop) and fluid temperature at the inlet.
-
-- An internal variable called “Load Request for Plant Connection N� provides the current value for the desired operating capacity, in [W].  This is the input for how the model is being asked to meet the loads on the supply side.  This is the result of the central routines for operation schemes and should be useful for controlling a plant model.  (This internal variable is not made available when this plant connection’s loading mode is set to DemandsLoad.)
-
-For each plant loop connection that is used, the following EMS actuators are created and must be used to pass results from the custom model to the rest of EnergyPlus:
-
-- An actuator called “Plant Connection *N*� with the control type “Outlet Temperature,� in [C], needs to be used.  This is the temperature of the fluid leaving the air terminal unit through that particular plant connection.
-
-- An actuator called “Plant Connection *N*� with the control type “Mass Flow Rate,� in kg/s, needs to be used. This actuator registers the component model’s request for plant fluid flow.  The actual mass flow rate through the component may be different than requested if the overall loop situation is such that not enough flow is available to meet all the various requests.  In general, this actuator is used to lodge a request for flow, but the more accurate flow rate will be the internal variable called “Inlet Mass Flow Rate for Plant Connection *N.*�
-
-For each plant loop connection that is used, there is input required to specify the nature of the connection with respect to loads.  One of the following choices must be selected depending on the purpose of the component model.
-
-- DemandsLoad. This type of loading is used for plant connections that place a load on the loop.  Connections that use this loading scheme are not set up to meet loads and interact with the operation schemes.  For example, this loading mode is appropriate for the condenser side of a chiller.
-
-- MeetsLoadWithPassiveCapacity.  This type of loading is used for plant connections where the component has some capacity to meet loads but it is not really of the type that could be controlled.  For example, a ground heat exchanger is passive because while it can provide some level of heat rejection or source, the amount will vary with current conditions and cannot usually be explicitly controlled.
-
-- MeetsLoadWithNominalCapacity.  This type of loading is used for plant connections where the component has controllable capacity to meet loads and no outlet temperature restrictions.
-
-- MeetsLoadWithNominalCapacityLowOutLimit.  This type of loading is used for plant connections where the component has controllable capacity to meet loads but with a lower limit on the fluid temperature at the outlet node.  For example, this can be used for a chiller evaporator connection when the chiller is prevented from producing chilled water below a certain temperature limit.  When this type of loading is selected, an actuator is created to allow setting the low temperature limit for use by the load dispatch routines.  The actuator is called “Plant Connection *N*� with the control type “Low Outlet Temperature Limit,� in [C], and needs to be used.
-
-- MeetsLoadWithNominalCapacityHiOutLimit.  This type of loading is used for plant connections where the component has controllable capacity to meet loads but with an upper limit on the fluid temperature at the outlet node.  For example, this can be used for a boiler connection when the boiler is prevented from producing hot water above a certain temperature limit.  When this type of loading is selected, an actuator is created to allow setting the high temperature limit for use by the load dispatch routines.  The actuator is called “Plant Connection *N*� with the control type “High Outlet Temperature Limit,� in [C], and needs to be used.
-
-For each plant loop connection, there is input required for the nature of the flow requests made by the component with respect to determining the overall flow for the loop.  Mass flow request are also important for resolving the flow rates in parallel branches, but the mode here is related to the problem of determining the overall flow rate for the loop, not the flow down one particular branch.  The overall loop flow rate is a function of all the flow requests made by the different devices on the loop and different types of devices have different implications for the overall loop rate.  One of the following three choices must be made depending on the nature of the plant component.
-
-- NeedsFlowIfLoopOn.  Devices with this flow request mode will contribute to the overall loop flow rate but will not initiate flow themselves.  Other devices on the plant loop (of type NeedsFlowAndTurnsLoopOn ) need to make flow requests to get the loop flowing at all, but once it is flowing, this device can affect the overall loop flow rate.  For example, a chiller may have a lower limit on the allowable chilled water flow rate through its evaporator and if that lower limit is higher than the current request for chilled water by the cooling coils, then the overall loop flow will be that needed by the chiller rather than the coils.
-
-- NeedsFlowAndTurnsLoopOn.  Devices with this flow request mode will contribute to the overall loop flow rate and initiate flow themselves.  This mode is used for demand component such as coils.  Devices with this mode will initiate loops to turn on and start moving fluid.
-
-- ReceivesWhateverFlowAvailable.  Devices with this flow request mode will not contribute to the overall loop flow rate and do not initiate flow themselves.  These are essentially passive devices that take whatever flow is sent to them, such as a ground heat exchanger.
-
-Separate program calling managers are available for each plant loop connection.  The user defined plant component is called to simulate by the central plant routines (whereas the other user defined components are called by the central HVAC routines).  The calls to simulate are made for each connection and you may want or need to perform different model calculations depending on which plant loop connection is being simulated at the time.  There is an Erl program calling manager for initialization, setup, and sizing that needs to be used *for each plant connection* and is only called during the early plant loop initialization phase.  There is also an Erl program calling manager for the model calculations to perform for each plant connection.
-
-### Air Connection
-
-An air connection is available that includes both an inlet and an outlet node.  This can be used for air source or heat rejections. The following EMS internal variables are made available for the inlet node, if it is used, and should be useful inputs to your own custom models:
-
-- An internal variable called “Inlet Temperature for Air Connection,� provides the current value for the drybulb air temperature at the component’s inlet node, in [C].
-
-- An internal variable called “Inlet Mass Flow Rate for Air Connection,� provides the current value for the mass flow rate of air at the component’s inlet node, in [kg/s].
-
-- An internal variable called “Inlet Humidity Ratio for Air Connection,� provides the current value for the moist air humidity ratio at the component’s inlet node, in [kgWater/kgDryAir]
-
-- An internal variable called “Inlet Density for Air Connection,� provides the current value for the density of moist air at the component’s main inlet node, in [kg/m<sup>3</sup>].
-
-- An internal variable called “Inlet Specific Heat for Air Connection,� provides the current value for the specific heat of moist air at the component’s main inlet node, in [J/kg-C].
-
-The following EMS actuators are created for the outlet air node, if it is used, and must be used to pass results from the custom model to the rest of EnergyPlus:
-
-- An actuator called “Air Connection,� with the control type “Outlet Temperature,� in [C], needs to be used.  This will set the drybulb temperature of the air leaving the component.
-
-- An actuator called “Air Connection,� with the control type “Outlet Humidity Ratio,� in [kgWater/kgDryAir], needs to be used.  This will set the humidity ratio of the air leaving the component.
-
-- An actuator called “Air Connection,� with the control type “Outlet Mass Flow Rate,� in [kg/s], needs to be used.  This will set the flow rate of air leaving the component.
-
-### Water Use
-
-The user defined plant component can be connected to the water use models in EnergyPlus that allow modeling on-site storage.  If a supply inlet water storage tank is used, then an actuator called “Water System� with the control type “Supplied Volume Flow Rate,� in m<sup>3</sup>/s, needs to be used.  This sets up the plant component as a demand component for that storage tank.  If a collection outlet water storage tank is used, then an actuator called “Water System� with the control type “Collected Volume Flow Rate,� in m<sup>3</sup>/s, needs to be used.
-
-### Ambient Zone
-
-The user defined plant component can be connected to an ambient zone and provide internal gains to that zone.  This is for “skin losses� that the component might have that result from inefficiencies and other non-ideal behavior.  When an ambient zone is specified, the following actuators are created that can be used for different types of internal gains to the named zone:
-
-- An actuator called “Component Zone Internal Gain� with the control type “Sensible Heat Gain Rate,� in [W], is available.  This can be used for purely convective sensible heat gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Return Air Heat Gain Rate,� in [W], is available.  This can be used for purely convective sensible heat gains (or losses) to the return air duct for a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Thermal Radiation Heat Gain Rate,� in [W], is available.  This can be used for thermal radiation gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Latent Heat Gain Rate,’ in [W], is available.  This can be used for latent moisture gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Return Air Latent Heat Gain Rate,� in [W], is available.  This can be used for latent moisture gains (or losses) to a the return air duct for a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Carbon Dioxide Gain Rate,� in [m<sup>3</sup>/s], is available.  This can be used for carbon dioxide gains (or losses) to a zone.
-
-- An actuator called “Component Zone Internal Gain� with the control type “Gaseous Contaminant Gain Rate,� in [m<sup>3</sup>/s], is available.  This can be used for generic gaseous air pollutant gains (or losses) to a zone.
-
-
-
-EMS Examples
-============
-
-This section provides examples that demonstrate how to use the EMS. Each example provides a problem statement, discusses how to approach a solution using EMS, and provides example EMS input objects. For each example a complete input data file is provided with the EnergyPlus release (you can find this in the ExampleFiles\\ directory).
-
-A range of example applications is presented here. Each is presented in isolation for simplicity, but a much more comprehensive approach to EMS programs is also possible.
-
-Example 1. Whole-Building Average Zone Air Temperature
-------------------------------------------------------
-
-### Problem Statement
-
-Although EnergyPlus can report an enormous number of output variables, you may want a custom report variable such as one for the average temperature in the building. Only zone-by-zone indoor air temperatures are available. Because it is nearly always important to check that models are properly controlling zone air conditions, you may need to examine air temperature results from your models. Compared to scanning across the many zones in a large building, you could save time when checking a model if you have a single value for a whole-building average temperature. Of course, you could calculate such a value after a run by postprocessing, but redoing this for every run is cumbersome and time consuming. Therefore, it would be more convenient to automatically calculate such a value inside the program and output it in the usual manner. For example, if we take the Small Office Reference Building (RefBldgSmallOfficeNew2004\_Chicago.idf), is there a way to create a custom report variable that provides a weighted average for the indoor temperature of all the occupied zones in a model?
-
-### EMS Design Discussion
-
-This is a fairly simple example in that the EMS controls nothing. There are no actuators.
-
-The example file has six zones, but one is an attic that we do not care about. Therefore, the main inputs, or EMS sensors, will be the zone air temperatures for the five occupied zones. We will use EnergyManagementSystem:Sensor objects to obtain the values for the air temperatures by mapping to the output variable called “Zone Mean Air Temperature.�
-
-A model for average temperature can be constructed by using the zone air volumes as weights so larger zones have more influence than smaller zones on the resulting average. The model equation we will implement in EMS for our new report variable is
-
-<div>$$T_{average} = \frac{\sum\left(T_{zone}\text{Vol}_{zone}\right)}{\sum\left(\text{Vol}_{zone}\right)}$$</div>
-
-The example file specifies the zone volume in its zone objects so we have the data needed for the weighting factors from elsewhere in the IDF. However, a study could vary the geometry such that the volumes differ from one simulation to another. Zone Air Volume is available as internal data, so we will use EnergyManagementSystem:InternalVariable input objects to assign these weighting factors into global Erl variables. If we did not know beforehand that Zone Air Volume was an available internal variable, we would have had to prerun the model with some EMS-related objects and the appropriate level of reporting selected in an Output:EnergyManagementSystem object, and then studied the EDD output file. Note that the EDD file is only produced if you have EMS/Erl programs in your input file.
-
-The custom output variable will be defined by using an EnergyManagementSystem:OutputVariable input object. This requires the Erl variable to be global, so we need to declare a variable. Let’s call it AverageBuildingTemp, to be global using an EnergyManagementSystem:GlobalVariable object so we have a way to connect the result calculated in the Erl program to the custom output.
-
-There are two main considerations when selecting an EMS calling point:
-
-- The call should be toward the end of the zone timestep so the zone air temperature calculations are finalized.
-
-- The call should be before reporting updates so our new value is available before the reporting is finalized.
-
-We therefore choose the EMS calling point with the key of “EndOfZoneTimestepBeforeReporting.�
-
-### EMS Input Objects
-
-A set of input objects to solve this problem appears below and is included in the example file called “EMSCustomOutputVariable.idf.�
-
-```idf
-EnergyManagementSystem:Sensor,
-   T1, !Name
-   Perimeter_ZN_1 ,! Output:Variable or Output:Meter Index Key Name
-   Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
-
-
- EnergyManagementSystem:Sensor,
-   T2, !Name
-   Perimeter_ZN_2 , ! Output:Variable or Output:Meter Index Key Name
-   Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
-
-
- EnergyManagementSystem:Sensor,
-   T3, !Name
-   Perimeter_ZN_3 , ! Output:Variable or Output:Meter Index Key Name
-   Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
-
-
- EnergyManagementSystem:Sensor,
-   T4, !Name
-   Perimeter_ZN_4, ! Output:Variable or Output:Meter Index Key Name
-   Zone Mean Air Temperature ;! Output:Variable or Output:Meter Name
-
-
- EnergyManagementSystem:Sensor,
-   T5, !Name
-   Core_ZN , ! Output:Variable or Output:Meter Index Key Name
-   Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
-
-
- EnergyManagementSystem:ProgramCallingManager,
-   Average Building Temperature , ! Name
-   EndOfZoneTimestepBeforeZoneReporting , ! EnergyPlus Model Calling Point
-   AverageZoneTemps ; ! Program Name 1
-
-
- EnergyManagementSystem:GlobalVariable,
-   AverageBuildingTemp;
-
-
- EnergyManagementSystem:OutputVariable,
-   Weighted Average Building Zone Air Temperature [C], ! Name
-   AverageBuildingTemp, ! EMS Variable Name
-   Averaged, ! Type of Data in Variable
-   ZoneTimeStep ; ! Update Frequency
-
-
- EnergyManagementSystem:InternalVariable,
-   Zn1vol,
-   Perimeter_ZN_1,
-   Zone Air Volume;
-
-
- EnergyManagementSystem:InternalVariable,
-   Zn2vol,
-   Perimeter_ZN_2,
-   Zone Air Volume;
-
-
- EnergyManagementSystem:InternalVariable,
-   Zn3vol,
-   Perimeter_ZN_3,
-   Zone Air Volume;
-
-
- EnergyManagementSystem:InternalVariable,
-   Zn4vol,
-   Perimeter_ZN_4,
-   Zone Air Volume;
-
-
- EnergyManagementSystem:InternalVariable,
-   Zn5vol,
-   Core_ZN ,
-   Zone Air Volume;
-
-
- EnergyManagementSystem:Program,
-   AverageZoneTemps , ! Name
-   SET SumNumerator = T1*Zn1vol + T2*Zn2vol + T3*Zn3vol + T4*Zn4vol + T5*Zn5vol,
-   SET SumDenominator = Zn1vol + Zn2vol + Zn3vol + Zn4vol + Zn5vol,
-   SET AverageBuildingTemp = SumNumerator / SumDenominator;
-
-
- Output:EnergyManagementSystem,
-   Verbose,
-   Verbose,
-   Verbose;
-
-
- Output:Variable,
-   *,                       !- Key Value
-   Weighted Average Building Zone Air Temperature,  !- Variable Name
-   timestep;                  !- Reporting Frequency
-```
-
-
-Example 2. Traditional Setpoint and Availability Managers
----------------------------------------------------------
-
-### Problem Statement
-
-The traditional way of modeling supervisory control of HVAC systems in EnergyPlus is to use SetpointManagers and AvailabilityManagers. To gain experience with EMS, we should ask, Is there a way to take a model such as the Large Office Reference Building (RefBldgLargeOfficeNew2004\_Chicago.idf) and replicate the traditional HVAC managers by using only the EMS?
-
-### EMS Design Discussion
-
-A review of the example file shows that three types of traditional HVAC managers are being used:  scheduled setpoints, mixed air setpoints, and night cycle availability. We will discuss these separately.
-
-The input object SetpointManager:Scheduled functions by placing a setpoint value on a specified node based on the value in a schedule. Therefore, our EMS program will do the same. First we will need to access the schedule. In this example, a schedule called Seasonal-Reset-Supply-Air-Temp-Sch contains the temperature values desired for the air system’s supply deck. We use an EnergyManagementSystem:Sensor object based on the output variable called “Schedule Value� to fill schedule values into an Erl variable called Seasonal\_Reset\_SAT\_Sched. Once we have the sensor and actuator setup, putting the setpoint on the node involves a single line of Erl code, “SET VAV\_1\_SAT\_setpoint = Seasonal\_Reset\_SAT\_Sched.�
-
-The input object SetpointManager:Mixed air functions by placing a setpoint value on a specified node based on the value of the setpoint at another node and the temperature rise across the fan. The temperature rise is found by taking the temperature at the fan outlet node and subtracting the temperature at the fan inlet node. The EMS needs two additional sensors to obtain these temperatures, which are set up by using a pair EnergyManagementSystem:Sensor objects. The example file has three mixed air setpoint managers that place setpoints on the outlet of the outdoor air mixer, the outlet of the cooling coil, and the outlet of the heating coil. Therefore, we need three actuators to place setpoints at these three nodes, which are set up using three EnergyManagementSystem:Actuator objects. Each mixed air setpoint calculation is a simple single-line of program code such as “SET VAV\_1\_CoolC\_Setpoint = Seasonal\_Reset\_SAT\_Sched - (T\_VAV1FanOut - T\_VAV1FanIn).�
-
-The input object AvailabilityManager:NightCycle functions by monitoring zone temperature and starting up the air system (if needed) to keep the building within the thermostat range. The sensors here are the zone air temperatures, which are set up by using EnergyManagementSystem:Sensor objects in the same way as for Example 1. We will need one zone temperature sensor for each zone that is served by the air system so we can emulate the “CycleOnAny� model being used. The other sensors we need are the desired zone temperatures used by the thermostat. We access these temperatures directly from the schedules (HTGSETP\_SCH and CLGSETP\_SCH in the example) by using EnergyManagementSystem:Sensor objects. To control the air system’s operation status, we use an EnergyManagementSystem:Actuator object that is assigned to an “AirLoopHVAC� component type using the control variable called “Availability Status.�  EnergyPlus recognizes four availability states that control the behavior of the air system. Inside EnergyPlus these are integers, but EMS has only real-valued variables, so we will use the following whole numbers:
-
-- NoAction = 0.0
-
-- ForceOff = 1.0
-
-- CycleOn = 2.0
-
-- CycleOnZoneFansOnly = 3.0.
-
-The traditional AvailabilityManager:NightCycle object operates by turning on the system for a prescribed amount of time (1800 seconds in the example file), and then turning it off for the same amount of time. You should be able to model this starting and stopping in EMS by using Trend variables to record the history of the actions. However, this cycling is not necessarily how real buildings are operated, and for this example we do not try to precisely emulate the traditional EnergyPlus night cycle manager. Rather, we use a simpler temperature-based control to start and stop the air system for the night cycle. The algorithm first assumes an offset tolerance of 0.83°C and calculates limits for when heating should turn on and off and when cooling should turn on and off. It then finds the maximum and minimum zone temperatures for all the zones attached to the air system. These use the @Max and @Min built-in functions, which take on two operators at a time. Then a series of logic statements is used to compare temperatures and decide what the availability status of the air system should be.
-
-### EMS Input Objects
-
-EMS examples are provided for the three types of traditional HVAC managers. The full set to run with no traditional managers is provided in the example file “EMSReplaceTraditionalManagers\_LargeOffice.idf.�
-
-Example input objects that replicate a scheduled setpoint manager using EMS follow.
-
-```idf
-EnergyManagementSystem:Sensor,
-   Seasonal_Reset_SAT_Sched, !Name
-   Seasonal-Reset-Supply-Air-Temp-Sch , ! Output:Variable Index Key Name
-   Schedule Value;   ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Actuator,
-   VAV_1_SAT_setpoint,                ! Name
-   VAV_1 Supply Equipment Outlet Node,      ! Component Name
-   System Node Setpoint,              ! Component Type
-   Temperature Setpoint;              ! Control Variable
-
-
-EnergyManagementSystem:Program,
-   VAV_1_SchedSetpoint , ! Name
-   SET VAV_1_SAT_setpoint = Seasonal_Reset_SAT_Sched;
-
-
-Example input objects that replicate a mixed air setpoint manager using EMS follow.
-EnergyManagementSystem:Sensor,
-   T_VAV1FanIn, !Name
-   VAV_1_HeatC-VAV_1_FanNode , ! Output:Variable Key Name
-   System Node Temperature; ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Sensor,
-   T_VAV1FanOut, !Name
-   VAV_1 Supply Equipment Outlet Node, ! Output:Variable Index Key Name
-   System Node Temperature ; ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Actuator,
-   VAV_1_CoolC_Setpoint,            ! Name
-   VAV_1_CoolC-VAV_1_HeatCNode ,    ! Component Name
-   System Node Setpoint,            ! Component Type
-   Temperature Setpoint;            ! Control Variable
-
-
-EnergyManagementSystem:Actuator,
-   VAV_1_HeatC_Setpoint,                            ! Name
-   VAV_1_HeatC-VAV_1_FanNode ,                  ! Component Name
-   System Node Setpoint,                          ! Component Type
-   Temperature Setpoint;            ! Control Variable
-
-
-EnergyManagementSystem:Actuator,
-   VAV_1_OA_Setpoint,                            ! Name
-   VAV_1_OA-VAV_1_CoolCNode ,                  ! Component Name
-   System Node Setpoint,                          ! Component Type
-   Temperature Setpoint;            ! Control Variable
-
-
-
-
-EnergyManagementSystem:Program,
-   VAV1MixedAirManagers , ! Name
-   SET VAV_1_CoolC_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV1FanOut - T_VAV1FanIn),
-   SET VAV_1_HeatC_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV1FanOut - T_VAV1FanIn),
-   SET VAV_1_OA_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV1FanOut - T_VAV1FanIn);
-
-
-Example input objects for a night cycle availability manager follow.
-EnergyManagementSystem:Actuator,
-  VAV_1_NightCycleStatus,   ! Name
-  VAV_1,                    ! Component Name
-  AirLoopHVAC,              ! Component Type
-  Availability Status;      ! Control Variable
-
-
-
-
-EnergyManagementSystem:Sensor,
-  heating_setpoint,                  ! Name
-  HTGSETP_SCH ,         ! Output:Variable or Output:Meter Index Key Name
-  Schedule Value ; ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Sensor,
-  cooling_setpoint,                  ! Name
-  CLGSETP_SCH ,         ! Output:Variable or Output:Meter Index Key Name
-  Schedule Value ; ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Sensor,
-  TzoneVAV1_1,                  ! Name
-  Core_bottom ,         ! Output:Variable or Output:Meter Index Key Name
-  Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Sensor,
-  TzoneVAV1_2,                  ! Name
-  Perimeter_bot_ZN_3 ,         ! Output:Variable Key Name
-  Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Sensor,
-  TzoneVAV1_3,                  ! Name
-  Perimeter_bot_ZN_2 ,         ! Output:Variable Key Name
-  Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Sensor,
-  TzoneVAV1_4,                  ! Name
-  Perimeter_bot_ZN_1 ,         ! Output:Variable Key Name
-  Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Sensor,
-  TzoneVAV1_5,                  ! Name
-  Perimeter_bot_ZN_4 ,         ! Output:Variable Key Name
-  Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Program,
-   VAV_1_NightCycleMGR , ! Name
-   SET Toffset = 0.8333  ,  ! 1.5F
-   SET NoAction = 0.0 ,
-   SET ForceOff = 1.0 ,
-   SET CycleOn = 2.0 ,
-   SET CycleOnZoneFansOnly = 3.0 ,
-   SET VAV1_heating_TurnOn  = heating_setpoint - Toffset ,
-   SET VAV1_heating_TurnOff = heating_setpoint + Toffset ,
-   SET VAV1_cooling_TurnOn  = cooling_setpoint + Toffset ,
-   SET VAV1_cooling_TurnOff = cooling_setpoint - Toffset ,
-   ! find max and min for "cycleOnAny" operation
-   SET Tmin = @MIN TzoneVAV1_1 TzoneVAV1_2  ,
-   SET Tmin = @MIN Tmin        TzoneVAV1_3  ,
-   SET Tmin = @MIN Tmin        TzoneVAV1_4  ,
-   SET Tmin = @MIN Tmin        TzoneVAV1_5  ,
-   SET Tmax = @MAX TzoneVAV1_1 TzoneVAV1_2  ,
-   SET Tmax = @MAX Tmax        TzoneVAV1_3  ,
-   SET Tmax = @MAX Tmax        TzoneVAV1_4  ,
-   SET Tmax = @MAX Tmax        TzoneVAV1_5  ,
-   IF Tmin < VAV1_heating_TurnOn ,
-     SET VAV_1_NightCycleStatus = CycleOn,
-     RETURN,  ! need to exit early or cooling check could also trigger
-   ELSEIF Tmin &gt; VAV1_heating_TurnOff,
-     SET VAV_1_NightCycleStatus = NoAction,
-   ENDIF,
-   IF Tmax &gt; VAV1_cooling_TurnOn,
-     SET VAV_1_NightCycleStatus = CycleOn,
-   ELSEIF Tmax < VAV1_cooling_TurnOff,
-     SET VAV_1_NightCycleStatus = NoAction   ,
-   ENDIF;
-```
-
-
-
-
-Example 3. Hygro-thermal Window Opening Control for Airflow Network
--------------------------------------------------------------------
-
-### Problem Statement
-
-A user of EnergyPlus version 3.1 posted the following question on the Yahoo! list (circa spring 2009):
-
-I am currently trying to model a simple ventilation system based on an
-
-exhaust fan and outdoor air variable aperture paths that open according to
-
-the indoor relative humidity.
-
-As I didn't find any object to directly do this, I am trying to use an
-
-AirflowNetwork: MultiZone: Component: DetailedOpening object and its
-
-AirflowNetwork: multizone: Surface object to model the variable aperture. But
-
-the Ventilation Control Mode of the surface object can only be done via
-
-Temperature or Enthalpy controls (or other not interesting for my purpose),
-
-and not via humidity.
-
-So my questions are:
-
-1- is it possible to make the surface object variable according to the
-
-relative humidity? (maybe adapting the program?)
-
-2- or is there an other way to make it?
-
-Because the traditional EnergyPlus controls for window openings do not support humidity-based controls (or did not as of Version 3.1), the correct response to Question \#1 was “No.�  But with the EMS, we can now answer Question \#2 as “Yes.�  How can we take the example file called HybridVentilationControl.idf and implement humidity-based control for a detailed opening in the airflow network model?
-
-### EMS Design Discussion
-
-The main EMS sensor will be the zone air humidity, so we use an EnergyManagementSystem:Sensor object that maps to the output variable called System Node Relative Humidity for the zone’s air node. This zone has the detailed opening.
-
-The EMS will actuate the opening in an airflow network that is defined by the input object AirflowNetwork:MultiZone:Component:DetailedOpening. The program will setup the actuator for this internally, but we need to use an EnergyManagementSystem:Actuator object to declare that we want to use the actuator and provide the variable name we want for the Erl programs.
-
-Because we do not know the exactly what the user had in mind, for this example we assume that the desired behavior for the opening area is that the opening should vary linearly with room air relative humidity. When the humidity increases, we want the opening to be larger. When the humidity decreases, we want the opening to be smaller. For relative humidity below 25% we close the opening. At 60% or higher relative humidity, the opening should be completely open. We formulate a model equation for opening factor as
-
-<div>$$
-  F_{open} = \begin{array}{ll}
-    0.0 & RH &lt; 25\% \\
-    \frac{RH-25}{60-25} & 25\% \leq RH \leq 60\% \\
-    1.0 & RH > 60\%  
-  \end{array}
-$$</div>
-
-### EMS Input Objects
-
-EMS-related input objects to solve this problem are listed below and are included in the example file called “EMSAirflowNetworkOpeningControlByHumidity.idf.�
-
-```idf
-EnergyManagementSystem:Sensor,
-  ZoneRH , ! Name
-  Zone 1 Node, ! Output:Variable or Output:Meter Index Key Name
-  System Node Relative Humidity; ! Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Actuator,
-  MyOpenFactor,                            ! Name
-  Zn001:Wall001:Win001,                  ! Component Name
-  AirFlow Network Window/Door Opening, ! Component Type
-  Venting Opening Factor;    ! Control Type
-
-
-EnergyManagementSystem:ProgramCallingManager,
-  RH Controlled Open Factor ,    ! Name
-  BeginTimestepBeforePredictor , ! EnergyPlus Model Calling Point
-  RH_OpeningController ;         ! Program Name 1
-
-
-EnergyManagementSystem:Program,
-  RH_OpeningController ,     ! Name
-  IF ZoneRH < 25,
-    SET MyOpenFactor = 0.0 ,
-  ELSEIF ZoneRH &gt; 60,
-    SET MyOpenFactor = 1.0 ,
-  ELSE,
-    SET MyOpenFactor = (ZoneRH - 25) / (60 - 25),
-  ENDIF;
-
-
-Output:EnergyManagementSystem,
-  Verbose,
-  Verbose,
-  Verbose;
-```
-
-
-
-
-Example 4. Halt Program Based on Constraint
--------------------------------------------
-
-### Problem Statement
-
-Heavy users of EnergyPlus explore the enormous parameter space associated with building design options. Computational requirements often limit what can be accomplished in a given study. For optimizations and other parametric studies, there is usually a tension between having a very detailed model that is comfortably accurate, and a simpler model that executes faster.
-
-For most studies many trial simulations are discarded because they violate some constraint. To save computation time, you might consider “fatal–out� simulations where early calculations show that some predetermined constraints will not be met in the final result. Many studies could save considerable computing resources by prematurely quitting models rather than always letting each simulation run to completion. All types of constraints such as poor comfort, excessive system iterations, and high energy costs could be used to kill a run. You should ask, Is there a way to use the EMS to expedite my optimal searches by stopping models prematurely if they fail some test?
-
-### EMS Design Discussion
-
-As an example, let us assume that the criterion for early exit is that the model fails to be sufficiently comfortable. We will start with the Small Hotel Reference Building example file (RefBldgSmallHotelNew2004\_Chicago.idf). Short periods of discomfort are tolerated, but if the space is uncomfortable over time, we want to abandon the simulation and save computational expense. A simulation can be stopped from within an Erl program by calling the built-in function “@FatalHaltEp.�  The EMS system has only numeric data types, so we cannot generate text for the error message. Therefore, we choose a particular real-numbered value to use as an error code that provides some detail on which constraint caused early termination. In this example, we choose the value “1002.50� to indicate an average PMV exceeds 2.5 and the value “9001.30� indicates the average PMV less than 1.3. We will formulate the constraint by using the result of the Fanger comfort model for PMV for the building’s core zone named “Core\_ZN.�  If the occupants will be too cold, we will call @FatalHaltEp with the error code 9001.30. If the occupants will be too warm during a summer design day, we will fatal out with the error code 1002.50. (These values were chosen arbitrarily to demonstrate EMS; PMV of 1.3 is not necessarily a problem.)
-
-To monitor PMV, we will use a trend variable, which we create by using the EnergyManagementSystem:TrendVariable input object. A trend variable is a log of historical values for Erl variables. A trend log is an array that goes farther and farther back in time. For this example, we assume the constraint is to monitor the average PMV for the previous 2-hour period. The example file has 6 timesteps per hour, so each trend point is 10 minutes and a 2-hour average needs 12 timesteps. So the field Number of Timesteps to be Logged must be 12 or larger. To access the values stored in a trend variable, the built-in functions provided for accessing trends must be used. The @TrendAverage function called with an index of 12 will return the 2-hour running average. To monitor this result of running average PMV, we set up custom output variable using an EnergyManagementSystem:OutputVariable input object.
-
-### EMS Input Objects
-
-The EMS input objects for this example follow and are contained in the example file called “EMSTestMAthAndKill.idf.�
-
-```idf
- EnergyManagementSystem:ProgramCallingManager,
-   Average Building Temperature , ! Name
-   EndOfZoneTimestepBeforeZoneReporting , ! EnergyPlus Model Calling Point
-   updateMy_averagePMV; ! Program Name 1
-
- EnergyManagementSystem:Sensor,
-   PMV5, !Name
-   Core_ZN , ! Output:Variable or Output:Meter Index Key Name
-   Zone Thermal Comfort Fanger Model PMV ; ! Output:Variable Name
-
- EnergyManagementSystem:TrendVariable,
-   PMVtrendLog1,
-   PMV5,
-   300;
-
- EnergyManagementSystem:GlobalVariable,
-   PMVrunningAvg;
-
- EnergyManagementSystem:OutputVariable,
-   Running Two Hour Average PMV [PMVunits], ! Name
-   PMVrunningAvg, ! EMS Variable Name
-   Averaged, ! Type of Data in Variable
-   ZoneTimeStep ; ! Update Frequency
-
- EnergyManagementSystem:Program,
-   UpdateMy_averagePMV,
-   Set PMVrunningAvg = @TrendAverage PMVtrendLog1 12, ! two hour running average.
-   RUN Kill_Run_if_Uncomfortable;
-
- EnergyManagementSystem:Subroutine,
-   Kill_Run_if_Uncomfortable,
-   IF PMVrunningAvg &gt; 2.5,
-     SET tmpError = @FatalHaltEp 1002.50, ! error code "1002.50" for comfort avg over 2.5
-   ENDIF,
-   IF PMVrunningAvg < 0.0 - 1.3,
-     SET tmpError = @FatalHaltEp 9001.30, ! error code "9001.30" for comfort avg under - 1.3
-   ENDIF;
-```
-
-
-Example 5. Computed Schedule
-----------------------------
-
-### Problem Statement
-
-Many models have schedule inputs that could be used to control the object, but creating the schedules it is too cumbersome. We need to ask, Can we use the EMS to dynamically calculate a schedule?
-
-### EMS Design Discussion
-
-As an example, we will take the model from example 1 and use the EMS to replicate the heating and cooling zone temperature setpoint schedules. The input object Schedule:Constant has been set up to be available as an actuator. We then add EnergyManagementSystem:Actuator objects that set these actuators up as Erl variables.
-
-To devise an Erl program to compute the schedule, we need to use the built-in variables that describe time and day. The built-in variable Hour will provide information about the time of day; DayOfWeek will provide information about whether it is the weekend or a weekday.
-
-### EMS Input Objects
-
-Example EMS input for computing a schedule for heating and cooling setpoints follows and are contained in the example file called “EMSCustomSchedule.idf.�
-
-```idf
-Schedule:Constant,
-    CLGSETP_SCH,
-    Temperature,
-    24.0;
-
-  EnergyManagementSystem:Actuator,
-    myCLGSETP_SCH_Override,
-    CLGSETP_SCH,Schedule:Constant,Schedule Value;
-
-  EnergyManagementSystem:ProgramCallingManager,
-    My Setpoint Schedule Calculator Example,
-    BeginTimestepBeforePredictor,
-    MyComputedCoolingSetpointProg,
-    MyComputedHeatingSetpointProg;
-
-  EnergyManagementSystem:Program,
-    MyComputedCoolingSetpointProg,
-    IF (DayOfWeek == 1),
-      Set myCLGSETP_SCH_Override = 30.0  ,
-    ELSEIF (Holiday == 3.0) && (DayOfMonth == 21) && (Month == 1),  !winter design day
-      Set myCLGSETP_SCH_Override = 30.0 ,
-    ELSEIF HOUR < 6       ,
-      Set myCLGSETP_SCH_Override = 30.0  ,
-    ELSEIF (Hour &gt;= 6) && (Hour < 22)  && (DayOfWeek &gt;=2) && (DayOfWeek <=6) ,
-      Set myCLGSETP_SCH_Override = 24.0  ,
-    ELSEIF (Hour &gt;= 6) && (hour < 18) && (DayOfWeek == 7)
-      Set myCLGSETP_SCH_Override = 24.0  ,
-    ELSEIF (Hour &gt;= 6) && (hour &gt;= 18) && (DayOfWeek == 7)
-      Set myCLGSETP_SCH_Override = 30.0  ,
-    ELSEIF (Hour &gt;= 22)                   ,
-      Set myCLGSETP_SCH_Override = 30.0  ,
-    ENDIF;
-
-  Schedule:Constant,
-    HTGSETP_SCH,
-    Temperature,
-    21.0;
-
-  EnergyManagementSystem:Actuator,
-    myHTGSETP_SCH,
-    HTGSETP_SCH,Schedule:Constant,Schedule Value;
-
-  EnergyManagementSystem:Program,
-   MyComputedHeatingSetpointProg,
-   Set locHour = Hour, ! echo out for debug
-   Set locDay = DayOfWeek, ! echo out for debug
-   Set locHol = Holiday,  ! echo out for debug
-   IF (DayOfWeek == 1),
-     Set myHTGSETP_SCH = 15.6  ,
-   ELSEIF (Holiday == 3.0) && (DayOfYear == 21),  !winter design day
-     Set myHTGSETP_SCH = 21.0 ,
-   ELSEIF HOUR < 5       ,        
-     Set myHTGSETP_SCH = 15.6  ,
-   ELSEIF (Hour >= 5) && (Hour < 19)  && (DayOfWeek &gt;=2) && (DayOfWeek <=6) ,
-     Set myHTGSETP_SCH = 21.0  ,
-   ELSEIF (Hour >= 6) && (hour < 17) && (DayOfWeek == 7),
-     Set myHTGSETP_SCH = 21.0  ,
-   ELSEIF (Hour >= 6) && (hour <= 17) && (DayOfWeek == 7) ,
-     Set myHTGSETP_SCH = 15.6   ,
-   ELSEIF (Hour >= 19)          ,
-     Set myHTGSETP_SCH = 15.6   ,
-   ENDIF;
-```
-
-
-
-
-Example 6. Window Shade Control
--------------------------------
-
-### Problem Statement
-
-EnergyPlus offers a wide range of control options in the WindowProperty:ShadingControl object, but it is easy to imagine custom schemes for controlling shades or blinds that are not available. We need to ask, Can we use the EMS to override the shading controls?
-
-### EMS Design Discussion
-
-We will take the example file PurchAirWindowBlind.idf and use EMS to add a new control scheme. This file has an interior blind that can be either “on� or “off.�  The control scheme has three parts:
-
-- Deploy the blind whenever too much direct sun would enter the zone and cause discomfort for the occupants.
-
-- Deploy the blind whenever there is a significant cooling load.
-
-- Leave the blind open whenever the first two constraints have not triggered.
-
-We assume that a model for the direct sun control is based on incidence angle, where the angle is defined as zero for normal incidence relative to the plane of the window. When the direct solar incidence angle is less than 45 degrees, we want to draw the blind. EnergyPlus has a report variable called “Surface Ext Solar Beam Cosine Of Incidence Angle,� for which we will use a sensor in our EnergyManagementSystem:Sensor input object. This sensor is a cosine value that we turn into an angle value with the built-in function @ArcCos. Then we will use the built-in function @RadToDeg to convert from radians to degrees. This new window/solar incidence angle in degree may be an interesting report variable, so we use an EnergyManagementSystem:OutputVariable input object to create custom output.
-
-Because the transmitted solar is a problem only when there is a cooling load, we also trigger the blind based on the current data for cooling. The report variable called “Zone/Sys Sensible Cooling Rate� is used in an EMS sensor to obtain an Erl variable with the most recent data about zone cooling load required to meet setpoint. When this value is positive, we know the zone cannot make good use of passive solar heating, so we close the blind.
-
-The EMS actuator will override the operation of a WindowProperty:ShadingControl input object. Related to this, the EDD file shows
-
-! &lt;EnergyManagementSystem:Actuator Available&gt;, Component Unique Name, Component Type,  Control Type
-
-EnergyManagementSystem:Actuator Available,ZN001:WALL001:WIN001,Window Shading Control,Control Status
-
-Although the user-defined name for the WindowProperty:ShadingControl is “INCIDENT SOLAR ON BLIND,� the component unique name of the actuator that is available is called “ZN001:WALL001:WIN001.�  There could be multiple windows, all with shades, and each is governed by a single WindowProperty:ShadingControl input object. The EMS actuator could override each window separately. The Control Type is called “Control Status,� and requires you to set the status to one of a set of possible control flags. For this case, with only an interior shade, there are two states for the actuator to take. The first shows the shade is “off,� and corresponds to a value of 0.0. The second shows the interior shade is “on,� and corresponds to a value of 6.0.
-
-### EMS Input Objects
-
-The EMS input objects for this example follow and are contained in the example file called “EMSWindowShadeControl.idf.�
-
-```idf
-Output:EnergyManagementSystem,
-   Verbose,
-   Verbose,
-   Verbose;
-
-
- EnergyManagementSystem:Sensor,
-   Solar_Beam_Incident_Cos, !Name
-   Zn001:Wall001:Win001,! Output:Variable or Output:Meter Index Key Name
-   Surface Outside Face Beam Solar Incident Angle Cosine Value; ! Var Name
-
-
- Output:Variable, Zn001:Wall001:Win001,
-    Surface Outside Face Beam Solar Incident Angle Cosine Value, Timestep;
-
-
- EnergyManagementSystem:Sensor,
-   Zone_Sensible_Cool_Rate, !Name
-   RESISTIVE ZONE,! Output:Variable or Output:Meter Index Key Name
-   Zone Air System Sensible Cooling Rate; ! Var Name
-
-
- Output:Variable, RESISTIVE ZONE,
-    Zone Air System Sensible Cooling Rate, Timestep;
-
-
-EnergyManagementSystem:ProgramCallingManager,
-  Window Shading Device EMS Controller,    ! Name
-  BeginTimestepBeforePredictor , ! EnergyPlus Model Calling Point
-  Set_Shade_Control_State ;         ! Program Name 1
-
-
-EnergyManagementSystem:Actuator,
-  Zn001_Wall001_Win001_Shading_Deploy_Status,   ! Name
-  Zn001:Wall001:Win001,    ! Component Name  Surface name with shade controls
-  Window Shade Control, ! Component Type
-  Control Status;    ! Control Type
-
-
-
-
-EnergyManagementSystem:Program,
-  Set_Shade_Control_State,     ! Name
-  !
-  Set IncidentAngleRad = @ArcCos Solar_Beam_Incident_Cos,
-  Set IncidentAngle   = @RadToDeg IncidentAngleRad,
-  !
-  IF IncidentAngle < 45 , ! Block intense direct sun
-   Set Zn001_Wall001_Win001_Shading_Deploy_Status = Shade_Status_Interior_Blind_On,
-  ELSEIF Zone_Sensible_Cool_Rate &gt; 20, ! block to reduce cooling loads
-   Set Zn001_Wall001_Win001_Shading_Deploy_Status = Shade_Status_Interior_Blind_On,
-  Else,
-   Set Zn001_Wall001_Win001_Shading_Deploy_Status = Shade_Status_Off ,
-  ENDIF ;
-
-
-
-
-EnergyManagementSystem:OutputVariable,
-   Erl Shading Control Status, ! Name
-   Zn001_Wall001_Win001_Shading_Deploy_Status, ! EMS Variable Name
-   Averaged, ! Type of Data in Variable
-   ZoneTimeStep ; ! Update Frequency
-
-
-EnergyManagementSystem:OutputVariable,
-   Erl Zn001:Wall001:Win001 Incident Angle, ! Name
-   IncidentAngle, ! EMS Variable Name
-   Averaged, ! Type of Data in Variable
-   ZoneTimeStep ; ! Update Frequency
-
-
- EnergyManagementSystem:GlobalVariable,  IncidentAngle;
-
-
-Output:Variable,
-  *,
-  Erl Shading Control Status,
-  Timestep;
-
-
-Output:Variable,
-  *,
-  Erl Zn001:Wall001:Win001 Incident Angle,
-  Timestep;
-
-
-
-
-
-
-EnergyManagementSystem:ProgramCallingManager,
-  Init Window Shading Device Control Constants,    ! Name
-  BeginNewEnvironment , ! EnergyPlus Model Calling Point
-  InitializeShadeControlFlags ;         ! Program Name 1
-
-
- EnergyManagementSystem:GlobalVariable,    Shade_Status_None;
- EnergyManagementSystem:GlobalVariable,    Shade_Status_Off ;
- EnergyManagementSystem:GlobalVariable,    Shade_Status_Interior_Shade_On;
- EnergyManagementSystem:GlobalVariable,    Shade_Status_Switchable_Dark;
- EnergyManagementSystem:GlobalVariable,    Shade_Status_Exterior_Shade_On;
- EnergyManagementSystem:GlobalVariable,    Shade_Status_Interior_Blind_On;
- EnergyManagementSystem:GlobalVariable,    Shade_Status_Exterior_Blind_On;
- EnergyManagementSystem:GlobalVariable,    Shade_Status_Between_Glass_Shade_On;
- EnergyManagementSystem:GlobalVariable,    Shade_Status_Between_Glass_Blind_On;
-
-
-
-
- EnergyManagementSystem:Program,
-    InitializeShadeControlFlags,
-          ! these are control flag values used inside EnergyPlus for window shades
-          ! EMS control of window shading devices involves setting the control values for shading control actuators with
-          !  one of these values. The variable names can be used or replaced, it is the whole number values that trigger
-          !  changes in the modeling.
-          !  Shades and Blinds are either fully on or fully off, partial positions require multiple windows.
-          ! the window shading control flag values follow
-          !  -1: if window has no shading device
-    Set Shade_Status_None = 0.0 - 1.0,  ! this is how to write a negative number Erl does not have unary "minus,"  only binary subtraction
-          !   0: if shading device is off
-    Set Shade_Status_Off = 0.0,
-          !   1: if interior shade is on
-    Set Shade_Status_Interior_Shade_On = 1.0,
-          !   2: if glazing is switched to darker state
-    Set Shade_Status_Switchable_Dark = 2.0,
-          !   3: if exterior shade is on
-    Set Shade_Status_Exterior_Shade_On = 3.0,
-          !   6: if interior blind is on
-    Set Shade_Status_Interior_Blind_On = 6.0,
-          !   7: if exterior blind is on
-    Set Shade_Status_Exterior_Blind_On = 6.0,
-          !   8: if between-glass shade is on
-    Set Shade_Status_Between_Glass_Shade_On = 8.0,
-          !   9: if between-glass blind is on
-    Set Shade_Status_Between_Glass_Blind_On = 9.0;
-          !  10: window has interior shade that is off but may be triggered on later
-          !       to control daylight glare
-          !  20: window has switchable glazing that is unswitched but may be switched later
-          !       to control daylight glare or daylight illuminance
-          !  30: window has exterior shade that is off but may be triggered on later
-          !       to control daylaight glare or daylight illuminance
-          !  60: window has interior blind that is off but may be triggered on later
-          !       to control daylaight glare or daylight illuminance
-          !  70: window has exterior blind that is off but may be triggered on later
-          !       to control daylaight glare or daylight illuminance
-          !  80: window has between-glass shade that is off but may be triggered on later
-          !       to control daylaight glare or daylight illuminance
-          !  90: window has between-glass blind that is off but may be triggered on later
-          !       to control daylaight glare or daylight illuminance
-          ! A "shading device" may be an exterior, interior or between-glass shade or blind,
-          ! or the lower-transmitting (dark) state of switchable glazing (e.g., electrochromic).
-          ! In all cases, the unshaded condition is represented
-          ! by the construction given by window's Surface()%Construction and
-          ! the shaded condition is represented by the construction given by
-          ! the window's Surface()%ShadedConstruction
-```
-
-
-
-
-Example 7. Constant Volume Purchased Air System
------------------------------------------------
-
-### Problem Statement
-
-The simplest way to add HVAC control to an EnergyPlus thermal zone is to use the ZoneHVAC:IdealLoadsAirSystem. This was called *purchased air* in older versions. The ideal loads air system is intended for load calculations. You provide input for the supply air conditions of drybulb and humidity ratio, but the flow rate cannot be controlled. The model operates by varying the flow rate to exactly meet the desired setpoints. However, you may want to experiment with various designs in a slightly different way in which, given a prescribed supply air situation, then adjust the design to maximize the thermal comfort. It would be interesting to use the simple-to-input purchased air model to examine how a zone responds to a system, rather than how the system responds to a zone. We should ask, Can we use the EMS to prescribe the supply air flow rates for a purchased air model?
-
-### EMS Design Discussion
-
-For this example we begin with the input file from Example 6 (primarily because it already has purchased air). We examine the typical mass flow rates the air system provides to have some data to judge what an appropriate constant flow rate might be. A cursory review of the data indicates that cooling flow rates of 0.3 kg/s are chosen for two zones and 0.4 kg/s is chosen for the third. Heating flow rates of 0.1 and 0.15 kg/s are also chosen.
-
-We want the model to respond differently for heating and cooling. We define two operating states and create global variables to hold that state for each zone. The first state is when the zone calls for heating; we will assign a value of 1.0. The second is when the zone calls for cooling; we assign 2.0.
-
-To sense the state we will use EMS sensors associated with the output variable called “Zone/Sys Sensible Load Predicted.�  We will set up one of these for each zone and use it as input data. If this value is less than zero, the zone is in the cooling state. If it is greater than zero, the zone is in the heating state. This predicted load is calculated during the predictor part of the model, so we choose the EMS calling point called “AfterPredictorAfterHVACManagers.�
-
-An EMS actuator is available for the ideal loads air system that overrides the air mass flow rate (kg/s) delivered by the system when it is on. The override is not absolute in that the model will still apply the limits defined in the input object and overrides only if the system is “on.�  The internal logic will turn off the air system if the zone is in the thermostat dead band or scheduled “off� by availability managers. This “off� state is modeled inside the ideal loads air system so it does not need to be calculated in Erl. This control leads to a constant volume system that cycles in an attempt to control the zone conditions. In practice, it can achieve relatively good control when loads do not exceed the available capacity.
-
-### EMS Input Objects
-
-A set of EMS input objects for a constant volume purchased air system serving three zones follows are contained in the example file called “EMSConstantVolumePurchAir.idf.�
-
-```idf
-EnergyManagementSystem:ProgramCallingManager,
-  Constant Volume Purchased Air Example,    ! Name
-  AfterPredictorAfterHVACManagers , ! EnergyPlus Model Calling Point
-  Determine_Purch_Air_State,         ! Program Name 1
-  Set_Purch_Air;
-
-
-EnergyManagementSystem:Program,
-  Determine_Purch_Air_State,     ! Name
-  ! State representation:  1.0 is heating, 2.0 is cooling
-  IF (Sensible_Load_Zone_1 <= 0.0) ,
-    SET Zone_1_State = 2.0,
-  ELSEIF (Sensible_Load_Zone_1 &gt; 0.0) ,
-    SET Zone_1_State = 1.0,
-  ENDIF,
-  IF (Sensible_Load_Zone_2 <= 0.0) ,
-    SET Zone_2_State = 2.0,
-  ELSEIF (Sensible_Load_Zone_2 &gt; 0.0) ,
-    SET Zone_2_State = 1.0,
-  ENDIF,
-  IF (Sensible_Load_Zone_3 <= 0.0) ,
-    SET Zone_3_State = 2.0,
-  ELSEIF (Sensible_Load_Zone_3 &gt; 0.0) ,
-    SET Zone_3_State = 1.0,
-  ENDIF;
-
-
-
-
- EnergyManagementSystem:Program,
-  Set_Purch_Air,
-  IF (    Zone_1_State == 2.0),
-    SET ZONE_1_AIR_Mdot = 0.3,
-  ELSEIF (Zone_1_State == 1.0),
-    SET ZONE_1_AIR_Mdot = 0.1,
-  ENDIF,
-  IF (    Zone_2_State == 2.0),
-    SET ZONE_2_AIR_Mdot = 0.3,
-  ELSEIF (Zone_2_State == 1.0),
-    SET ZONE_2_AIR_Mdot = 0.1,
-  ENDIF,
-  IF (    Zone_3_State == 2.0),
-    SET ZONE_3_AIR_Mdot = 0.4,
-  ELSEIF (Zone_3_State == 1.0),
-    SET ZONE_3_AIR_Mdot = 0.15,
-  ENDIF;
-
-
-
-
- EnergyManagementSystem:GlobalVariable,  Zone_1_State;
- EnergyManagementSystem:GlobalVariable,  Zone_2_State;
- EnergyManagementSystem:GlobalVariable,  Zone_3_State;
-
-
- EnergyManagementSystem:Actuator,  ZONE_1_AIR_Mdot,
-  ZONE1AIR,Ideal Loads Air System,Air Mass Flow Rate;
- EnergyManagementSystem:Actuator, ZONE_2_AIR_Mdot,
-  ZONE2AIR,Ideal Loads Air System,Air Mass Flow Rate;
- EnergyManagementSystem:Actuator, ZONE_3_AIR_Mdot,
-  ZONE3AIR,Ideal Loads Air System,Air Mass Flow Rate;
-
-
- EnergyManagementSystem:Sensor,
-  Sensible_Load_Zone_1, !Name
-  RESISTIVE ZONE,! Output:Variable or Output:Meter Index Key Name
-  Zone Predicted Sensible Load to Setpoint Heat Transfer Rate; ! Var Name
-
-
- EnergyManagementSystem:Sensor,
-  Sensible_Load_Zone_2, !Name
-  EAST ZONE,! Output:Variable or Output:Meter Index Key Name
-  Zone Predicted Sensible Load to Setpoint Heat Transfer Rate; ! Var Name
-
-
- EnergyManagementSystem:Sensor,
-  Sensible_Load_Zone_3, !Name
-  NORTH ZONE,! Output:Variable or Output:Meter Index Key Name
-  Zone Predicted Sensible Load to Setpoint Heat Transfer Rate; ! Var Name
-```
-
-
-
-
-Example 8. System Sizing with Discrete Package Sizes
-----------------------------------------------------
-
-### Problem Statement
-
-One tension often arises with modeling when options being evaluated have an indirect effect on air system size. In normal autosizing, the changes in sizes are continuous, but in real systems, equipment sizes tend to be discrete. If we start with the Strip Mall Reference Building model (RefBldgStripMallNew2004\_Chicago.idf), we should ask, Could we use the EMS custom calculations to intervene and make the final system sizing results follow the discrete sizes available for a particular product line of equipment?
-
-### EMS Design Discussion
-
-Examining the vendor’s literature for one line of commercial packaged single-zone HVAC air systems shows that the nominal product sizes include 1200 cfm, 1600 cfm, 2000 cfm, 2400 cfm, 3000 cfm, 3400, cfm, and 4000 cfm. The literature also classifies units by tonnage of cooling capacity; however, in EnergyPlus modeling it is simpler to classify by air flow rate rather than by cooling capacity (because the direct expansion models have a tight range for allowable cooling capacity per air flow rate and size themselves off the flow rate). We construct the following simple model to select the next higher air flow rate product that uses the volume flow determined during the usual autosizing calculations, <span>\(\dot{V}_{size}\)</span>, and threshold values taken from the nominal product sizes (in m<sup>3</sup>/s):
-
-<table class="table table-striped">
-  <tr>
-    <th>Thresholh</th>
-    <th>Selection</th>
-  </tr>
-  <tr>
-    <td><span>\(0 &lt; \dot{V}_{size} \leq 0.566 \)</span></td>
-    <td><span>\(\dot{V}= 0.566\)</span></td>
-  </tr>
-  <tr>
-    <td><span>\(0.566 &lt; \dot{V}_{size} \leq 0.755 \)</span></td>
-    <td><span>\(\dot{V}= 0.755\)</span></td>
-  </tr>
-  <tr>
-    <td><span>\(0.755 &lt; \dot{V}_{size} \leq 0.944 \)</span></td>
-    <td><span>\(\dot{V}= 0.944\)</span></td>
-  </tr>
-  <tr>
-    <td><span>\(0.944 &lt; \dot{V}_{size} \leq 1.133 \)</span></td>
-    <td><span>\(\dot{V}= 1.133\)</span></td>
-  </tr>
-  <tr>
-    <td><span>\(1.133 &lt; \dot{V}_{size} \leq 1.416 \)</span></td>
-    <td><span>\(\dot{V}= 1.416\)</span></td>
-  </tr>
-  <tr>
-    <td><span>\(1.416 &lt; \dot{V}_{size} \leq 1.604 \)</span></td>
-    <td><span>\(\dot{V}= 1.604\)</span></td>
-  </tr>
-  <tr>
-    <td><span>\(1.604 &lt; \dot{V}_{size} \leq 1.888 \)</span></td>
-    <td><span>\(\dot{V}= 1.888\)</span></td>
-  </tr>
-</table>
-
-The system sizing calculations determine a value for the volume flow rate. To obtain this result for use in an Erl program, we use an EnergyManagementSystem:InternalVariable input object to set up a variable for the data called “Intermediate Air System Main Supply Volume Flow Rate.�  We can then use this value in our algorithm to find a discrete system size.
-
-Once we have the new system size, we need to set up an actuator to apply the new size. For this we use an EnergyManagementSystem:Actuator input object to establish control over “Sizing:System� type of component using the “Main Supply Volume Flow Rate� control type.
-
-The EMS calling point for controlling air system sizing is called “EndOfSystemSizing.�  So we enter this into the program calling manager.
-
-For this example, we modify the example file called “RefBldgStripMallNew2004\_Chicago.idf.�  This file has 10 separate packaged units, so rather than repeat the algorithm several times, we use a subroutine so the same Erl code can be reused for each air system. The subroutine has two arguments that we will declare as global variables:  the input for continuous size and the output for the discrete size.
-
-### EMS Input Objects
-
-A set of input objects for EMS control for discrete resizing of 10 air systems follows and is included in the example file called “EMSDiscreteAirSystemSizes.idf.�
-
-```idf
-Output:EnergyManagementSystem,
-  Verbose,
-  Verbose,
-  Verbose;
-
-
-EnergyManagementSystem:ProgramCallingManager,
-  Apply Discrete Package Sizes to Air System Sizing , ! Name
-  EndOfSystemSizing ,    ! EnergyPlus Model Calling Point
-  Resize_PSZ_To_Match_Product_Availability;         ! Program Name 1
-
-
-
-
-EnergyManagementSystem:Program,
-  Resize_PSZ_To_Match_Product_Availability , ! Name
-  SET argMainVdot = PSZ_1_CalcMainSupVdot,
-  RUN Select_Discrete_Nominal_Air_Flow,
-  SET PSZ_1_MainSupVdotSet = argDiscreteMainVdot,
-  SET argMainVdot = PSZ_2_CalcMainSupVdot,
-  RUN Select_Discrete_Nominal_Air_Flow,
-  SET PSZ_2_MainSupVdotSet = argDiscreteMainVdot,
-  SET argMainVdot = PSZ_3_CalcMainSupVdot,
-  RUN Select_Discrete_Nominal_Air_Flow,
-  SET PSZ_3_MainSupVdotSet = argDiscreteMainVdot,
-  SET argMainVdot = PSZ_4_CalcMainSupVdot,
-  RUN Select_Discrete_Nominal_Air_Flow,
-  SET PSZ_4_MainSupVdotSet = argDiscreteMainVdot,
-  SET argMainVdot = PSZ_5_CalcMainSupVdot,
-  RUN Select_Discrete_Nominal_Air_Flow,
-  SET PSZ_5_MainSupVdotSet = argDiscreteMainVdot,
-  SET argMainVdot = PSZ_6_CalcMainSupVdot,
-  RUN Select_Discrete_Nominal_Air_Flow,
-  SET PSZ_6_MainSupVdotSet = argDiscreteMainVdot,
-  SET argMainVdot = PSZ_7_CalcMainSupVdot,
-  RUN Select_Discrete_Nominal_Air_Flow,
-  SET PSZ_7_MainSupVdotSet = argDiscreteMainVdot,
-  SET argMainVdot = PSZ_8_CalcMainSupVdot,
-  RUN Select_Discrete_Nominal_Air_Flow,
-  SET PSZ_8_MainSupVdotSet = argDiscreteMainVdot,
-  SET argMainVdot = PSZ_9_CalcMainSupVdot,
-  RUN Select_Discrete_Nominal_Air_Flow,
-  SET PSZ_9_MainSupVdotSet = argDiscreteMainVdot,
-  SET argMainVdot = PSZ_10_CalcMainSupVdot,
-  RUN Select_Discrete_Nominal_Air_Flow,
-  SET PSZ_10_MainSupVdotSet = argDiscreteMainVdot;
-
-
-EnergyManagementSystem:Subroutine,
-  Select_Discrete_Nominal_Air_Flow,
-  ! argMainVdot          Input
-  ! argDiscreteMainVdot         Output
-  IF (argMainVdot <= 0.56628) , ! 1200 cfm
-    SET argDiscreteMainVdot = 0.56628 ,
-  ELSEIF (argMainVdot &gt; 0.56628) && (argMainVdot <= 0.75504) , ! 1600 CFM
-    SET argDiscreteMainVdot = 0.75504 ,
-  ELSEIF (argMainVdot &gt; 0.75504) && (argMainVdot <= 0.9438 ) , ! 2000 CFM
-    SET argDiscreteMainVdot = 0.9438 ,
-  ELSEIF (argMainVdot &gt; 0.9438) && (argMainVdot <= 1.13256 ) , ! 2400 CFM
-    SET argDiscreteMainVdot = 1.13256 ,
-  ELSEIF (argMainVdot &gt; 1.13256) && (argMainVdot <= 1.4157 ) , ! 3000 CFM
-    SET argDiscreteMainVdot = 1.4157 ,
-  ELSEIF (argMainVdot &gt; 1.4157) && (argMainVdot <= 1.60446 ) , ! 3400 CFM
-    SET argDiscreteMainVdot = 1.60446 ,
-  ELSEIF (argMainVdot &gt; 1.60446) && (argMainVdot <= 1.8879 ) , ! 4000 CFM
-    SET argDiscreteMainVdot = 1.8879 ,
-  ELSEIF (argMainVdot &gt; 1.8879), ! too high
-    set dummy = @SevereWarnEP 666.0,
-  ENDIF;
-
-
-EnergyManagementSystem:GlobalVariable, argDiscreteMainVdot;
-EnergyManagementSystem:GlobalVariable, argMainVdot;
-
-
-EnergyManagementSystem:InternalVariable,
-   PSZ_1_CalcMainSupVdot,
-   PSZ-AC_1:1 ,
-   Intermediate Air System Main Supply Volume Flow Rate;
-
-
-EnergyManagementSystem:Actuator,
-   PSZ_1_MainSupVdotSet,                            ! Name
-   PSZ-AC_1:1  ,                  ! Component Name
-   Sizing:System, ! Component Type
-   Main Supply Volume Flow Rate;    ! Control Type
-
-
-
-
-EnergyManagementSystem:InternalVariable,
-   PSZ_2_CalcMainSupVdot,
-   PSZ-AC_2:2 ,
-   Intermediate Air System Main Supply Volume Flow Rate;
-
-
-EnergyManagementSystem:Actuator,
-   PSZ_2_MainSupVdotSet,                            ! Name
-   PSZ-AC_2:2  ,                  ! Component Name
-   Sizing:System, ! Component Type
-   Main Supply Volume Flow Rate;    ! Control Type
-
-
-EnergyManagementSystem:InternalVariable,
-   PSZ_3_CalcMainSupVdot,
-   PSZ-AC_3:3 ,
-   Intermediate Air System Main Supply Volume Flow Rate;
-
-
-EnergyManagementSystem:Actuator,
-   PSZ_3_MainSupVdotSet,                            ! Name
-   PSZ-AC_3:3  ,                  ! Component Name
-   Sizing:System, ! Component Type
-   Main Supply Volume Flow Rate;    ! Control Type
-
-
-EnergyManagementSystem:InternalVariable,
-   PSZ_4_CalcMainSupVdot,
-   PSZ-AC_4:4 ,
-   Intermediate Air System Main Supply Volume Flow Rate;
-
-
-EnergyManagementSystem:Actuator,
-   PSZ_4_MainSupVdotSet,                            ! Name
-   PSZ-AC_4:4  ,                  ! Component Name
-   Sizing:System, ! Component Type
-   Main Supply Volume Flow Rate;    ! Control Type
-
-
-EnergyManagementSystem:InternalVariable,
-   PSZ_5_CalcMainSupVdot,
-   PSZ-AC_5:5 ,
-   Intermediate Air System Main Supply Volume Flow Rate;
-
-
-EnergyManagementSystem:Actuator,
-   PSZ_5_MainSupVdotSet,                            ! Name
-   PSZ-AC_5:5  ,                  ! Component Name
-   Sizing:System, ! Component Type
-   Main Supply Volume Flow Rate;    ! Control Type
-
-
-EnergyManagementSystem:InternalVariable,
-   PSZ_6_CalcMainSupVdot,
-   PSZ-AC_6:6 ,
-   Intermediate Air System Main Supply Volume Flow Rate;
-
-
-EnergyManagementSystem:Actuator,
-   PSZ_6_MainSupVdotSet,                            ! Name
-   PSZ-AC_6:6  ,                  ! Component Name
-   Sizing:System, ! Component Type
-   Main Supply Volume Flow Rate;    ! Control Type
-
-
-EnergyManagementSystem:InternalVariable,
-   PSZ_7_CalcMainSupVdot,
-   PSZ-AC_7:7 ,
-   Intermediate Air System Main Supply Volume Flow Rate;
-
-
-EnergyManagementSystem:Actuator,
-   PSZ_7_MainSupVdotSet,                            ! Name
-   PSZ-AC_7:7  ,                  ! Component Name
-   Sizing:System, ! Component Type
-   Main Supply Volume Flow Rate;    ! Control Type
-
-
-EnergyManagementSystem:InternalVariable,
-   PSZ_8_CalcMainSupVdot,
-   PSZ-AC_8:8 ,
-   Intermediate Air System Main Supply Volume Flow Rate;
-
-
-EnergyManagementSystem:Actuator,
-   PSZ_8_MainSupVdotSet,                            ! Name
-   PSZ-AC_8:8  ,                  ! Component Name
-   Sizing:System, ! Component Type
-   Main Supply Volume Flow Rate;    ! Control Type
-
-
-EnergyManagementSystem:InternalVariable,
-   PSZ_9_CalcMainSupVdot,
-   PSZ-AC_9:9 ,
-   Intermediate Air System Main Supply Volume Flow Rate;
-
-
-EnergyManagementSystem:Actuator,
-   PSZ_9_MainSupVdotSet,                            ! Name
-   PSZ-AC_9:9  ,                  ! Component Name
-   Sizing:System, ! Component Type
-   Main Supply Volume Flow Rate;    ! Control Type
-
-
-EnergyManagementSystem:InternalVariable,
-   PSZ_10_CalcMainSupVdot,
-   PSZ-AC_10:10 ,
-   Intermediate Air System Main Supply Volume Flow Rate;
-
-
-EnergyManagementSystem:Actuator,
-   PSZ_10_MainSupVdotSet,                            ! Name
-   PSZ-AC_10:10  ,                  ! Component Name
-   Sizing:System, ! Component Type
-   Main Supply Volume Flow Rate;    ! Control Type
-```
-
-
-Example 9. Demand Management
-----------------------------
-
-### Problem Statement
-
-Demand management refers to controlling a building to reduce the peak electrical power draws or otherwise improve the load profile from the perspective of the electric utility. Managing electricity demand is an important application for EMS. We should ask, Can we take the model from example 2 and use the EMS to add demand management?
-
-### EMS Design Discussion
-
-Example 2 is a model of a large office building, but unfortunately the utility tariff is not a demand-based rate. Therefore, we change to a different set of utility rate input objects so the model has demand charges.
-
-For this example, we assume that demand is managed by turning down the lights and increasing the cooling setpoint. The EMS calling point chosen is “BeginTimestepBeforePredictor� because it allows you to change the lighting power levels and temperature setpoints before you predict the zone loads.
-
-To manage the demand, we first need to develop some targets based on some a priori idea of what level of demand should be considered “high.�  Therefore, we first run the model without demand management and note the simulation results for demand. There are many ways to obtain the demand results, but one method is to obtain them from the tabular report for Tariffs called “Native Variables.�  In that report, the row called PeakDemand is the demand used to calculate demand charges and is listed in kW. We will use these values to construct a target level of demand for each month by taking these results and multiplying by 0.85 in an effort to reduce demand by 15%. For example, the demand for January was 1,154.01 kW, so we make our target level to be 0.85 \* 1154.01 = 980.91 kW and the demand for August was 1,555.20 kW, so the target is 0.85 \* 1555.20 = 1,321.92 kW.
-
-To develop our Erl program, we separate the overall task into two parts:
-
-1)   Determine the current state of demand management control.
-
-2)   Set the controls based on that control state.
-
-We then divide the Erl programs into two main programs and give them descriptive names:  “Determine\_Current\_Demand\_Manage\_State�;  “Dispatch\_Demand\_Changes\_By\_State.�
-
-The Erl program to determine the control state determines the current status for the demand management controls. You can record and manage the control state by setting the value of a global variable called “argDmndMngrState.�  For this example, we develop four control states that represent four levels of demand management:
-
-- Level 1 is assigned a value of 0.0 and represents no override to implement changes to demand-related controls.
-
-- Level 2 is assigned a value of 1.0 and represents moderately aggressive overrides for demand-related controls.
-
-- Level 3 is assigned a value of 2.0 and represents more aggressive override.
-
-- Level 4 is assigned a value of 3.0 and represents the most aggressive overrides.
-
-We develop an algorithm for choosing the control state by assuming it should be a function of how close the current power level is to the target power level, the current direction for changes in power use, and the recent history of control state. The current demand is obtained by using a sensor that is based on the “Total Electric Demand� output variable. This current demand is compared to the target demand levels discussed as well as a “level 1� demand level that is set to be 90% of the target. If the current demand is higher than the level 1 demand but lower than the target, the state will tend to be at level 1. If the current demand is higher than the target, the current state will be either level 2 or level 3 depending on the trend direction. However, we do not want the response to be too quick because it leads to too much bouncing between control states. Therefore, we also introduce some numerical damping with the behavior that once a control state is selected it should be selected for at least two timesteps before dropping down to a lower level. This damping is modeled with the help of a trend variable that records the control state over time so we can retrieve what the control state was during the past two timesteps.
-
-Once the control state is determined, the Erl programs will use EMS actuators to override controls based on the state. The following table summarizes the control adjustments used in our example for each control state.
-
-Table 9. Example 9 Demand Management Adjustments by Control State
-
-<table class="table table-striped">
-<tr>
-<th>Control State</th>
-<th>Lighting Power Ahjustment Factor</th>
-<th>Cooling Thermostat Offset</th>
-</tr>
-<tr>
-<td>0</td>
-<td>None</td>
-<td>none</td>
-</tr>
-<tr>
-<td>1</td>
-<td>0.9</td>
-<td>+ 0.8ºC</td>
-</tr>
-<tr>
-<td>2</td>
-<td>0.8</td>
-<td>+ 1.5ºC</td>
-</tr>
-<tr>
-<td>3</td>
-<td>0.7</td>
-<td>+ 2.0ºC</td>
-</tr>
-</table>
-
-
-
-For control state level 0, the actuators are all set to Null so they stop overriding controls and return the model to normal operation.
-
-To alter the lighting power density with EMS, you could use either a direct method that employs a Lights actuator or an indirect method that modifies the lighting schedule. For this example we use the direct method with EnergyManagementSystem:Actuator input objects that enable you to override the Electric Power Level for each zone’s lights. We also set up internal variables to obtain the Lighting Power Design Level for each Lights object.  Finally, we set up an EMS sensor to obtain the lighting schedule value to use in Erl programs. If the demand management control state is 1, 2, or 3, we use the following model to determine a new lighting power level:
-
-Power = (Adjustment Factor) × (Lighting Power Design Level) × (Schedule Value)
-
-There are also two ways to alter the cooling setpoint with EMS. To dynamically alter the cooling setpoints, we modify the schedule rather than directly actuating Zone Temperature Control actuators. Changing the schedule allows one actuator to override all the zones; the more direct approach would require actuators for each zone. (This can be used to advantage if different zones are to be managed differently.)  The algorithm applies an offset depending on the control state. In the input file, the schedule for cooling setpoints is called CLGSETP\_SCH, so we set up an actuator for this Schedule Value. Because the algorithm is a simple offset from the original schedule, we need to keep track of the values in the original schedule. We cannot use the same schedule as an input to the algorithm because once an actuator overrides the schedule value it will corrupt the original schedule. This would be an example of a circular reference problem. Therefore, we make a copy of the cooling setpoint schedule, naming it CLGSETP\_SCH\_Copy, and use the copy in a EnergyManagementSystem:Sensor object to obtain the current scheduled value for the setpoint. When we override the CLGSETP\_SCH schedule, it will not corrupt the values from the CLGSTEP\_SCH\_Copy schedule used as input.
-
-### EMS Input Objects
-
-The main input objects that implement this example of demand management are listed below and are included in the example file called “EMSDemandManager\_LargeOffice.idf.�  The results indicate that demand management controls could reduce electricity costs by around $40,000 or 10%.
-
-```idf
-EnergyManagementSystem:ProgramCallingManager,
-  Demand Manager Demonstration,
-  BeginTimestepBeforePredictor,
-  Determine_Current_Demand_Manage_State,
-  Dispatch_Demand_Controls_By_State;
-
-
-EnergyManagementSystem:Program,
-  Determine_Current_Demand_Manage_State,
-  Set localDemand = CurntFacilityElectDemand / 1000.0 ,
-  Set CurrntTrend = @TrendDirection FacilityElectTrend 4,
-  IF (Month == 1) ,
-    Set argTargetDemand = 0.85 * 1154.01,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ELSEIF (Month == 2),
-    Set argTargetDemand = 0.85 * 1150.85 ,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ELSEIF (Month == 3),
-    Set argTargetDemand = 0.85 * 1313.56 ,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ELSEIF (Month == 4),
-    Set argTargetDemand = 0.85 * 1364.28,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ELSEIF (Month == 5),
-    Set argTargetDemand = 0.85 * 1506.29  ,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ELSEIF (Month == 6),
-    Set argTargetDemand = 0.85 * 1516.93  ,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-
-
-  ELSEIF (Month == 7),
-    Set argTargetDemand = 0.85 * 1545.20  ,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ELSEIF (Month == 8),
-    Set argTargetDemand = 0.85 * 1555.20  ,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ELSEIF (Month == 9),
-    Set argTargetDemand = 0.85 * 1491.38  ,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ELSEIF (Month == 10),
-    Set argTargetDemand = 0.85 * 1402.86  ,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ELSEIF (Month == 11),
-    Set argTargetDemand = 0.85 * 1418.69  ,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ELSEIF (Month == 12),
-    Set argTargetDemand = 0.85 * 1440.48  ,
-    Set argCrntDmnd = localDemand,
-    Set argTrendDirection = CurrntTrend,
-  ENDIF,
-  Run Find_Demand_State;
-
-
-
-
-EnergyManagementSystem:Subroutine,
-  Find_Demand_State,
-  !  argTargetDemand       Input kW level target
-  !  argCrntDmnd           Input  kW level current
-  !  argTrendDirection            Input   J/hour
-  !  argDmndMngrState     Output  value code, 0.0 = no management,
-  !                        1.0 = level 1 demand management
-  !                     2.0 = level 2 demand management
-  !                     3.0 = level 3 demand management
-  Set DmndStateX1 = @TrendValue Demand_Mgr_State_Trend 1,
-  Set DmndStateX2 = @TrendValue Demand_Mgr_State_Trend 2,
-  Set Level1Demand = 0.9 * argTargetDemand,
-  Set argCrntDmnd = argCrntDmnd,
-  Set argTargetDemand = argTargetDemand,
-  SET argDmndMngrState = DmndStateX1, ! initialize to last state then model changes
-  IF (argCrntDmnd &gt; Level1Demand) && (argCrntDmnd <argTargetDemand) && (argTrendDirection &gt; 0.0),
-
-
-    IF DmndStateX1 <= 1.0,
-      SET argDmndMngrState = 1.0,
-    ELSEIF (DmndStateX1 == 2.0) && (DmndStateX2 < 2.0),
-      SET argDmndMngrState = 2.0,  ! go at least two timesteps at 2.0
-    ELSEIF (DmndStateX1 == 3.0) && (DmndStateX2 == 3.0),
-      SET argDmndMngrState = 2.0,
-    ELSEIF (DmndStateX1 == 3.0) && (DmndStateX2 == 2.0),
-      SET argDmndMngrState = 3.0,  ! go at least two timesteps at 3.0
-    ENDIF,
-
-
-  ELSEIF (argCrntDmnd &gt; argTargetDemand) && (argTrendDirection < 0.0),
-    IF DmndStateX1 <= 2.0,
-      SET argDmndMngrState = 2.0,
-    ELSEIF (DmndStateX1 == 3.0) && (DmndStateX2 == 2.0) , ! go at least two timesteps at 3.0
-      SET argDmndMngrState = 3.0,
-    ELSEIF (DmndStateX1 == 3.0) && (DmndStateX2 == 3.0),
-      SET argDmndMngrState = 2.0,
-    ENDIF,
-
-
-  ELSEIF (argCrntDmnd &gt; argTargetDemand) && (argTrendDirection &gt;= 0.0),
-    Set argDmndMngrState = 3.0,
-  ENDIF;
-
-
-
-
-EnergyManagementSystem:Program,
-  Dispatch_Demand_Controls_By_State,
-  IF     (argDmndMngrState == 0.0),
-    RUN Unset_Demand_Controls,
-  ELSEIF (argDmndMngrState == 1.0),
-    RUN Set_Demand_Level1_Controls,
-  ELSEIF (argDmndMngrState == 2.0),
-    Run Set_Demand_Level2_Controls,
-  ELSEIF (argDmndMngrState == 3.0),
-    Run Set_Demand_Level3_Controls,
-  ENDIF;
-
-
-
-
-EnergyManagementSystem:Subroutine,
-  Unset_Demand_Controls,
-  SET Set_Cooling_Setpoint_Sched    = Null,
-  SET Set_Basement_Lights           = Null,
-  SET Set_Core_bottom_Lights        = Null,
-  SET Set_Core_mid_Lights           = Null,
-  SET Set_Core_top_Lights           = Null,
-  SET Set_Perimeter_bot_ZN_3_Lights = Null,
-  SET Set_Perimeter_bot_ZN_2_Lights = Null,
-  SET Set_Perimeter_bot_ZN_1_Lights = Null,
-  SET Set_Perimeter_bot_ZN_4_Lights = Null,
-  SET Set_Perimeter_mid_ZN_3_Lights = Null,
-  SET Set_Perimeter_mid_ZN_2_Lights = Null,
-  SET Set_Perimeter_mid_ZN_1_Lights = Null,
-  SET Set_Perimeter_mid_ZN_4_Lights = Null,
-  SET Set_Perimeter_top_ZN_3_Lights = Null,
-  SET Set_Perimeter_top_ZN_2_Lights = Null,
-  SET Set_Perimeter_top_ZN_1_Lights = Null,
-  SET Set_Perimeter_top_ZN_4_Lights = Null;
-
-
-EnergyManagementSystem:Subroutine,
-  Set_Demand_Level1_Controls,
-  ! set lighting power to 90% of what it would otherwise be
-  SET Set_Cooling_Setpoint_Sched    = Cooling_Setpoint_Sched + 0.8, ! add 0.8 deg C to cooling setpoint
-  SET Set_Basement_Lights           = 0.90 * Basement_Lights * BLDG_LIGHT_SCH,
-  SET Set_Core_bottom_Lights        = 0.90 * Core_bottom_Lights * BLDG_LIGHT_SCH,
-  SET Set_Core_mid_Lights           = 0.90 * Core_mid_Lights * BLDG_LIGHT_SCH,
-  SET Set_Core_top_Lights           = 0.90 * Core_top_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_3_Lights = 0.90 * Perimeter_bot_ZN_3_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_2_Lights = 0.90 * Perimeter_bot_ZN_2_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_1_Lights = 0.90 * Perimeter_bot_ZN_1_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_4_Lights = 0.90 * Perimeter_bot_ZN_4_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_3_Lights = 0.90 * Perimeter_mid_ZN_3_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_2_Lights = 0.90 * Perimeter_mid_ZN_2_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_1_Lights = 0.90 * Perimeter_mid_ZN_1_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_4_Lights = 0.90 * Perimeter_mid_ZN_4_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_3_Lights = 0.90 * Perimeter_top_ZN_3_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_2_Lights = 0.90 * Perimeter_top_ZN_2_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_1_Lights = 0.90 * Perimeter_top_ZN_1_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_4_Lights = 0.90 * Perimeter_top_ZN_4_Lights * BLDG_LIGHT_SCH;
-
-
-EnergyManagementSystem:Subroutine,
-  Set_Demand_Level2_Controls,
-  ! set lighting power to 80% of what it would otherwise be
-  SET Set_Cooling_Setpoint_Sched    = Cooling_Setpoint_Sched + 1.5, ! add 1.5 deg C to cooling setpoint
-  SET Set_Basement_Lights           = 0.80 * Basement_Lights * BLDG_LIGHT_SCH,
-  SET Set_Core_bottom_Lights        = 0.80 * Core_bottom_Lights * BLDG_LIGHT_SCH,
-  SET Set_Core_mid_Lights           = 0.80 * Core_mid_Lights * BLDG_LIGHT_SCH,
-  SET Set_Core_top_Lights           = 0.80 * Core_top_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_3_Lights = 0.80 * Perimeter_bot_ZN_3_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_2_Lights = 0.80 * Perimeter_bot_ZN_2_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_1_Lights = 0.80 * Perimeter_bot_ZN_1_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_4_Lights = 0.80 * Perimeter_bot_ZN_4_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_3_Lights = 0.80 * Perimeter_mid_ZN_3_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_2_Lights = 0.80 * Perimeter_mid_ZN_2_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_1_Lights = 0.80 * Perimeter_mid_ZN_1_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_4_Lights = 0.80 * Perimeter_mid_ZN_4_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_3_Lights = 0.80 * Perimeter_top_ZN_3_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_2_Lights = 0.80 * Perimeter_top_ZN_2_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_1_Lights = 0.80 * Perimeter_top_ZN_1_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_4_Lights = 0.80 * Perimeter_top_ZN_4_Lights * BLDG_LIGHT_SCH;
-
-
-
-
-EnergyManagementSystem:Subroutine,
-  Set_Demand_Level3_Controls,
-  ! set lighting power to 70% of what it would otherwise be
-  SET Set_Cooling_Setpoint_Sched    = Cooling_Setpoint_Sched + 2.0, ! add 2.0 deg C to cooling setpoint
-  SET Set_Basement_Lights           = 0.70 * Basement_Lights * BLDG_LIGHT_SCH,
-  SET Set_Core_bottom_Lights        = 0.70 * Core_bottom_Lights * BLDG_LIGHT_SCH,
-  SET Set_Core_mid_Lights           = 0.70 * Core_mid_Lights * BLDG_LIGHT_SCH,
-  SET Set_Core_top_Lights           = 0.70 * Core_top_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_3_Lights = 0.70 * Perimeter_bot_ZN_3_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_2_Lights = 0.70 * Perimeter_bot_ZN_2_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_1_Lights = 0.70 * Perimeter_bot_ZN_1_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_bot_ZN_4_Lights = 0.70 * Perimeter_bot_ZN_4_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_3_Lights = 0.70 * Perimeter_mid_ZN_3_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_2_Lights = 0.70 * Perimeter_mid_ZN_2_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_1_Lights = 0.70 * Perimeter_mid_ZN_1_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_mid_ZN_4_Lights = 0.70 * Perimeter_mid_ZN_4_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_3_Lights = 0.70 * Perimeter_top_ZN_3_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_2_Lights = 0.70 * Perimeter_top_ZN_2_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_1_Lights = 0.70 * Perimeter_top_ZN_1_Lights * BLDG_LIGHT_SCH,
-  SET Set_Perimeter_top_ZN_4_Lights = 0.70 * Perimeter_top_ZN_4_Lights * BLDG_LIGHT_SCH;
-
-
-
-
-
-
-EnergyManagementSystem:GlobalVariable,argTargetDemand;
-EnergyManagementSystem:GlobalVariable,argCrntDmnd;
-EnergyManagementSystem:GlobalVariable,argTrendDirection;
-EnergyManagementSystem:GlobalVariable,argDmndMngrState;
-
-
-EnergyManagementSystem:Sensor,
-  BLDG_LIGHT_SCH, !- Name
-  BLDG_LIGHT_SCH, !- Output:Variable or Output:Meter Index Key Name
-  Schedule Value; !- Output:Variable or Output:Meter Name
-
-
-
-
-EnergyManagementSystem:Sensor,
-  CurntFacilityElectDemand,  !- Name
-  Whole Building,        !- Output:Variable or Output:Meter Index Key Name
-  Facility Total Electric Demand Power; !- Output:Variable Name
-
-
-
-
-EnergyManagementSystem:TrendVariable,
-  Demand_Mgr_State_Trend , !- Name
-  argDmndMngrState, !- EMS Variable Name
-  48 ; !- Number of Timesteps to be Logged
-
-
-EnergyManagementSystem:TrendVariable,
-  FacilityElectTrend , !- Name
-  CurntFacilityElectDemand, !- EMS Variable Name
-  144 ; !- Number of Timesteps to be Logged
-
-
-EnergyManagementSystem:Sensor,
-  Cooling_Setpoint_Sched,  !- Name
-  CLGSETP_SCH_Copy,        !- Output:Variable or Output:Meter Index Key Name
-  Schedule Value; !- Output:Variable or Output:Meter Name
-
-
-EnergyManagementSystem:Actuator,
-  Set_Cooling_Setpoint_Sched,  !- Name
-  CLGSETP_SCH ,     !- Actuated Component Unique Name
-  Schedule:Compact,   !- Actuated Component Type
-  Schedule Value    ; !- Actuated Component Control Type
-
-
-EnergyManagementSystem:OutputVariable,
-  Erl Cooling Setpoint [C],    !- Name
-  Set_Cooling_Setpoint_Sched,  !- EMS Variable Name
-  Averaged   ,                 !- Type of Data in Variable
-  ZoneTimestep;                !- Update Frequency
-
-
-
-
-Output:Variable,
-  *,
-  Erl Cooling Setpoint,
-  Timestep;
-
-
-EnergyManagementSystem:Actuator,
-  Set_Basement_Lights,  !- Name
-  Basement_Lights ,     !- Actuated Component Unique Name
-  Lights,               !- Actuated Component Type
-  Electric Power Level; !- Actuated Component Control Type
-
-
-EnergyManagementSystem:InternalVariable,
-  Basement_Lights , !- Name
-  Basement_Lights , !- Internal Data Index Key Name
-  Lighting Power Design Level ; !- Internal Data Type
-
-
-EnergyManagementSystem:Actuator,
-  Set_Core_bottom_Lights, !- Name
-  Core_bottom_Lights ,  !- Actuated Component Unique Name
-  Lights,               !- Actuated Component Type
-  Electric Power Level; !- Actuated Component Control Type
-EnergyManagementSystem:InternalVariable,
-  Core_bottom_Lights , !- Name
-  Core_bottom_Lights , !- Internal Data Index Key Name
-  Lighting Power Design Level ; !- Internal Data Type
-
-
-<< Snipped remaining Lights Sensors and Actuators >>
-```
-
-
-
-
-Example 10. Plant Loop Override Control
----------------------------------------
-
-### Problem Statement
-
-A common occurrence in EnergyPlus central plant simulations is for a component to be designed well, but during the course of an annual simulation, it is operated outside of its allowable region.  This is due to the governing control strategies (operating schemes).  These operation schemes may not have the intelligence to say, turn off a cooling tower when the outdoor temperature is too low.
-
-Within the EnergyPlus example files, the cooling tower offers warnings stating that the tower temperature is going below a low temperature limit.  We should ask, can we use a simple EMS addition to an input file to override the loop and turn off the cooling tower to avoid these situations and therefore the warnings?
-
-### EMS Design Discussion
-
-For this example, we will start with the example file that is packaged with EnergyPlus called EcoRoofOrlando.idf.  This is one example of an input file where a cooling tower throws warnings due to operating at too low of a temperature.  Although the input file has many aspects related to zone and HVAC, we will only be interested in the loop containing the tower, which is a *CondenserLoop* named *Chiller Plant Condenser Loop.* The loop has a minimum loop temperature of 5 degrees Celsius, as specified by the *CondenserLoop* object.
-
-In order to avoid these warnings and properly shut off the tower, EMS will be used to check the outdoor temperature and shut down the whole loop.  Special care must be taken when manipulating plant and condenser loops with EMS.  The most robust way found is to both disable the loop equipment and also override (turn off) the loop.  Skipping either of these can cause mismatches where either components are still expecting flow but the pump is not running, or the pump is trying to force flow through components which are disabled.  Either of these cases can cause unstable conditions and possibly fatal flow errors.
-
-The outdoor air temperature must be checked in order to determine what the EMS needs to do at a particular point in the simulation.  This is handled by use of an EMS sensor monitoring the Outdoor Dry Bulb standard E+ output variable.
-
-To manage the loop and pump, actuators are employed on both.  The pump actuator is a mass flow rate override.  This can be used to set the flow to zero, effectively shutting off the pump.  The loop actuator is an on/off supervisory control, which allows you to “shut the entire loop down.�  This actuator will not actually shut the loop down, it effectively empties the equipment availability list, so that there is no equipment available to reject/absorb load on the supply side.  If you use this actuator alone to “shut down the loop,� you may find that the pump is still flowing fluid around the loop, but the equipment will not be running.
-
-The EMS calling point chosen is “*InsideHVACSystemIterationLoop,*� so that the operation will be updated every time the plant loops are simulated.
-
-The Erl program is quite simple for this case.  If the outdoor dry bulb temperature goes below a certain value, the loop and pump actuators are set to zero.  If the outdoor temperature is equal to or above this value, the actuators are set to *Null*, relinquishing control back to the regular operation schemes.  In modifying this specific input file it was found that the outdoor dry bulb temperature which removed these warnings was six degrees Celsius.  We also create a custom output variable called “EMS Condenser Flow Override On� to easily record when the overrides have occurred.
-
-### EMS Input Objects
-
-The main input objects that implement this example of plant loop control are listed below and are included in the example file called “EMSPlantLoopOverrideControl.idf.�  The addition of the EMS objects properly shuts down the loop as the outdoor temperature go below the transition value, and the simulation error file shows no warnings for the tower outlet temperature.
-
-```idf
-  EnergyManagementSystem:Sensor,
-    OutdoorTemp,         !- Name
-    Environment,         !- Output:Variable Index Key Name
-    Site Outdoor Air Drybulb Temperature;    !- Output:Variable Name
-
-
-  EnergyManagementSystem:Actuator,
-    Actuator_Loop,       !- Name
-    Chiller Plant Condenser Loop, !- Actuated Component Unique Name
-    Plant Loop Overall,  !- Actuated Component Type
-    On/Off Supervisory;  !- Actuated Component Control Type
-
-
-  EnergyManagementSystem:Actuator,
-    PumpFlowOverride,    !- Name
-    Chiller Plant Cnd Circ Pump,  !- Actuated Component Unique Name
-    Pump,                !- Actuated Component Type
-    Pump Mass Flow Rate; !- Actuated Component Control Type
-
-
-  EnergyManagementSystem:GlobalVariable,
-    PumpFlowOverrideReport;
-
-
-  EnergyManagementSystem:OutputVariable,
-    EMS Condenser Flow Override On [On/Off], !- Name
-    PumpFlowOverrideReport,    !- EMS Variable Name
-    Averaged,            !- Type of Data in Variable
-    SystemTimeStep;      !- Update Frequency
-
-
-
-
-
-
-  EnergyManagementSystem:ProgramCallingManager,
-    Condenser OnOff Management,
-    InsideHVACSystemIterationLoop,
-    TowerControl;
-
-
-  EnergyManagementSystem:Program,
-    TowerControl,
-    IF (OutdoorTemp < 6.0),
-      SET Actuator_Loop = 0.0,
-      SET PumpFlowOverride = 0.0,
-      SET PumpFlowOverrideReport = 1.0,
-    ELSE,
-      SET Actuator_Loop = Null,
-      SET PumpFlowOverride = Null,
-      SET PumpFlowOverrideReport = 0.0,
-    ENDIF;
-
-
-  Output:Variable,
-    *,
-    EMS Condenser Flow Override On,
-    Hourly;
-```
-
-
-Example 11. Performance Curve Result Override
----------------------------------------------
-
-### Problem Statement
-
-The output of EnergyPlus performance curves (or tables) can be modified as necessary to simulate hardware or controls that cannot be accurately realized using a single performance curve. This example describes a method for modifying the capacity of a DX cooling coil via the DX coil objects Total Cooling Capacity Function of Temperature performance curve object.
-
-A particular manufacturer controls the DX cooling coil such that the capacity of the coil changes at 31°C outdoor air dry-bulb temperature. The following EMS program logic will calculate alternate inputs for cooling coil capacity and over-write the existing performance curve results.
-
-### EMS Design Discussion
-
-For this example, we will start with the equation for cooling capacity of the DX coil object (ref. Coil:Cooling:DX:SingleSpeed). From the engineering reference, the equation used to calculate the cooling capacity is:
-
-<div>$$
-\text{TotCapTempModFac} = a + b \left( T_{wb,i} \right) + c \left( T_{wb,i} \right) + d \left( T_{c,i} \right) + e \left( T_{c,i} \right) + f \left( T_{wb,i} \right)\left( T_{c,i} \right)
-$$</div>
-
-The first term (Twb,i) refers to the cooling coil inlet air wet-bulb temperature and the second (Tc,i) refers to the outdoor condenser inlet air dry-bulb temperature. Using the EMS, a new total capacity as a function of temperature value will be calculated and used during the simulation. The Energyplus input objects for the cooling coil capacity curve, the associated outdoor air mixer object, and the original cooling capacity performance curve are shown here.
-
-```idf
-  Coil:Cooling:DX:SingleSpeed,
-    Zone1PTHPDXCoolCoil,     !- Name
-    CoolingCoilAvailSched,   !- Availability Schedule Name
-    8750.0,                  !- Rated Total Cooling Capacity {W}
-    0.75,                    !- Rated Sensible Heat Ratio
-    3.0,                     !- Rated COP
-    0.5,                     !- Rated Air Flow Rate {m3/s}
-    ,          !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
-    Zone1PTHPFanOutletNode,  !- Air Inlet Node Name
-    Zone1PTHPDXCoolCoilOutletNode,  !- Air Outlet Node Name
-    HPACCoolCapFT,    !- Total Cooling Capacity f(Temperature) Curve Name
-    HPACCoolCapFFF,   !- Total Cooling Capacity f(Flow Fraction) Curve Name
-    HPACEIRFT,        !- Energy Input Ratio f(Temperature) Curve Name
-    HPACEIRFFF,       !- Energy Input Ratio f(Flow Fraction) Curve Name
-    HPACPLFFPLR;      !- Part Load Fraction Correlation Curve Name
-
-
-  OutdoorAir:Mixer,
-    Zone1PTHPOAMixer,        !- Name
-    Zone1PTHPOAMixerOutletNode,  !- Mixed Air Node Name
-    Zone1PTHPOAInNode,       !- Outdoor Air Stream Node Name
-    Zone1PTHPExhNode,        !- Relief Air Stream Node Name
-    Zone1PTHPAirInletNode;   !- Return Air Stream Node Name
-
-
-  Curve:Biquadratic,
-    HPACCoolCapFT,           !- Name
-    0.942587793,             !- Coefficient1 Constant
-    0.009543347,             !- Coefficient2 x
-    0.000683770,             !- Coefficient3 x**2
-    -0.011042676,            !- Coefficient4 y
-    0.000005249,             !- Coefficient5 y**2
-    -0.000009720,            !- Coefficient6 x*y
-```
-
-
-
-
-Note that the Total Cooling Capacity Function of Temperature Curve Name is HPACCoolCapFT and the inlet air node for this cooling coil is Zone1PTHPFanOutletNode. From the mixer object, the outdoor air node name is Zone1PTHPOAInNode. The existing cooling capacity performance curve name is HPACCoolCapFT. These node or object names will be used in the EMS program to point to the node or object as required.
-
-### EMS Input Objects
-
-The main input objects that implement this example for over-riding a performance curve result are listed below. Note that the node wet-bulb temperature at the inlet node of the cooling coil is calculated both using the node wet-bulb temperature and the psychrometric function to calculate a wet-bulb temperature from dry-bulb temperature and humidity ratio. The node wet-bulb temperature EMS sensor is left in this example for the sole purpose of showing how to access this node variable in a direct and indirect manner.
-
-Referring to the cooling capacity equation above, a new equation must be developed to represent this same performance aspect of the cooling coil. Since, in this example, the cooling capacity changes at 31°C, one of the coefficients is modified and used in the IF block to modify the cooling capacity above and below this outdoor air temperature limit. Note also that the coefficients used in the EMS program are all positive values and the negative sign is accounted for the CurveInput equation. Also, the value of C2 was changed to a negative value to represent the change in performance at 31°C. To calculate the new performance curve results, EMS sensors are placed at the cooling coil air inlet node to capture air dry-bulb temperature and humidity ratio, and at the outdoor air mixer outdoor air node inlet to capture outdoor air dry-bulb temperature and pressure. The curve input equation is identical to the equation shown above except that 1) the equation coefficients are all positive and any negative coefficients are accounted for in the equation itself, and 2) alternate coefficients (actually only C2a in this example) are used for the second equation. The results of this example show a marked difference in the cooling capacity above 31°C.
-
-
-
-```idf
-  EnergyManagementSystem:ProgramCallingManager,
-    EMSBasedCurveManager,  !- Name
-    AfterPredictorBeforeHVACManagers,  !- EnergyPlus Model Calling Point
-    CurveOverwriteMGR;     !- Program Name 1
-
-
-  EnergyManagementSystem:Program,
-    CurveOverwriteMGR,
-    SET TTmp = CoilInletDBT,
-    SET WTmp = CoilInletW,
-    SET PTmp = Pressure,
-    SET MyWB = @TwbFnTdbWPb TTmp WTmp PTmp,
-    SET IVOne = CoilInletWBT,
-    SET IVOne = MyWB,
-    SET IVTwo = OAT,
-    SET IVThree = IVOne*IVTwo,
-    SET C1 = 0.942567793,
-    SET C2 = 0.009543347,
-    SET C2a = 0.009543347, !-  -0.009543347
-    SET C3 = 0.00068377,
-    SET C4 = 0.011042676, !-  -0.011042676
-    SET C5 = 0.000005249,
-    SET C6 = 0.000009720, !-  -0.000009720
-    IF OAT < 31.0,
-      SET CurveInput = C1 + (C2*IVOne) + (C3*IVOne*IVone) - (C4*IVTwo) + (C5*IVTwo*IVTwo) - (C6*IVThree),
-    ELSE,
-      SET CurveInput = C1 - (C2a*IVOne) + (C3*IVOne*IVone) - (C4*IVTwo) + (C5*IVTwo*IVTwo) - (C6*IVThree),
-    ENDIF,
-    SET CurveOverwrite = CurveInput;
-
-
-
-
-  EnergyManagementSystem:Actuator,
-    CurveOverwrite,    !- Name
-    HPACCOOLCAPFT,     !- Actuated Component Unique Name
-    Curve,             !- Actuated Component Type
-    Curve Result;      !- Actuated Component Control Type
-
-
-  EnergyManagementSystem:Sensor,
-    ActualCurve,           !- Name
-    HPACCOOLCAPFT,     !- Output:Variable or Output:Meter Index Key Name
-    Performance Curve Output Value;  !- Output:Variable or Output:Meter Name
-
-
-  EnergyManagementSystem:Sensor,
-    CoilInletWBT,          !- Name
-    Zone1PTHPFanOutletNode, !- Output:Variable or Output:Meter Index Key Name
-    System Node Wetbulb Temperature; !- Output:Variable or Output:Meter Name
-
-
-  EnergyManagementSystem:Sensor,
-    Pressure,          !- Name
-    Zone1PTHPOAInNode,     !- Output:Variable or Output:Meter Index Key Name
-    System Node Pressure ;  !- Output:Variable or Output:Meter Name
-
-
-  EnergyManagementSystem:Sensor,
-    CoilInletDBT,          !- Name
-    Zone1PTHPFanOutletNode, !- Output:Variable or Output:Meter Index Key Name
-    System Node Temperature;  !- Output:Variable or Output:Meter Name
-
-
-  EnergyManagementSystem:Sensor,
-    CoilInletW,          !- Name
-    Zone1PTHPFanOutletNode, !- Output:Variable or Output:Meter Index Key Name
-    System Node Humidity Ratio;  !- Output:Variable or Output:Meter Name
-
-
-  EnergyManagementSystem:Sensor,
-    OAT,          !- Name
-    Zone1PTHPOAInNode,     !- Output:Variable or Output:Meter Index Key Name
-    System Node Temperature;  !- Output:Variable or Output:Meter Name
-
-
-  EnergyManagementSystem:OutputVariable,
-    ERLCurveValue, ! Name
-    ActualCurve,   ! EMS Variable Name
-    Averaged,      ! Type of Data in Variable
-    ZoneTimeStep ; ! Update Frequency
-
-
-  EnergyManagementSystem:OutputVariable,
-    NewCurveValue, ! Name
-    CurveInput,    ! EMS Variable Name
-    Averaged,      ! Type of Data in Variable
-    ZoneTimeStep ; ! Update Frequency
-
-
-  Output:EnergyManagementSystem,
-    Verbose,       !- Actuator Availability Dictionary Reporting
-    Verbose,       !- Internal Variable Availability Dictionary Reporting
-    Verbose;       !- EMS Runtime Language Debug Output Level
-
-
-  Output:Variable,
-    *,
-    ERLCurveValue,
-    Hourly;
-
-
- Output:Variable, HPACCOOLCAPFT,
-     Performance Curve Output Value,Hourly;
- Output:Variable, HPACCOOLCAPFT,
-     Performance Curve Input Variable 1 Value,Hourly;
- Output:Variable, HPACCOOLCAPFT,
-     Performance Curve Input Variable 2 Value,Hourly;
- Output:Variable, Zone1PTHPFanOutletNode,
-     System Node Wetbulb Temperature, Hourly;
-```
-
-
-
-
-
-
-![](media/image011.jpg)
-
-Figure 4. Results of Performance Curve Override
-
-Example 12. Variable Refrigerant Flow System Override
------------------------------------------------------
-
-### Problem Statement
-
-The variable refrigerant flow heat pump air conditioner has several available thermostat control options. These operation control schemes may not provide the type of control desired. How can we use a simple EMS addition to an input file that can override the specified thermostat control logic and set an alternate mode of operation?
-
-### EMS Design Discussion
-
-Depending on the type of thermostat control logic, the EnergyPlus program will review the loads in each zone, the number of zones in cooling or heating, the deviation from set point temperature, etc. to determine the mode of operation for the heat pump condenser. Alternate control logic may be developed to more accurately reflect the operation of a specific manufacturers product, or investigate other control techniques. This control logic may be added to an input file and used as the operating control logic of the heat pump.
-
-This simple example shows how to use EMS actuators to SET the operating mode and cause a specific terminal unit to operate at a specified part-load ratio (PLR). When setting the terminal unit PLR, the terminal unit will turn on only if the condenser is allowed to operate according to the minimum and maximum outdoor temperature limits.
-
-### EMS Input Objects
-
-The main input objects that implement this example are the variable refrigerant flow actuators that control the VRF system and specific terminal unit. Note that the terminal unit PLR can be controlled without controlling the mode of the VRF condenser, however, the specific terminal unit will operate in whatever mode the existing operation control scheme chooses. This example program simply “sets� the operating mode and PLR, other more complex control algorithms can be developed by the user as needed.
-
-
-
-```idf
-  Output:EnergyManagementSystem,
-    Verbose,                 !- Actuator Availability Dictionary Reporting
-    Verbose,                 !- Internal Variable Availability Dictionary Reporting
-    Verbose;                 !- EMS Runtime Language Debug Output Level
-
-
-  EnergyManagementSystem:ProgramCallingManager,
-    VRF OnOff Management,     !- Name
-    InsideHVACSystemIterationLoop,  !- EnergyPlus Model Calling Point
-    VRFControl;               !- Program Name 1
-
-
-  EnergyManagementSystem:Program,
-    VRFControl,               !- Name
-    SET VRF_Actuator_OnOff = VRF_Status_Heating, !- Program Line 2
-    SET VRF_TerminalUnit1_PLR = 0.5;
-
-
-  EnergyManagementSystem:Actuator,
-    VRF_Actuator_OnOff,       !- Name
-    VRF Heat Pump,            !- Actuated Component Unique Name
-    Variable Refrigerant Flow Heat Pump,      !- Actuated Component Type
-    Operating Mode;           !- Actuated Component Control Type
-
-
-  EnergyManagementSystem:Actuator,
-    VRF_TerminalUnit1_PLR,    !- Name
-    TU1,                      !- Actuated Component Unique Name
-    Variable Refrigerant Flow Terminal Unit,  !- Actuated Component Type
-    Part Load Ratio;          !- Actuated Component Control Type
-
-
-  EnergyManagementSystem:OutputVariable,
-    Erl VRF Control Status,   !- Name
-    VRF_Actuator_OnOff,       !- EMS Variable Name
-    Averaged,                 !- Type of Data in Variable
-    SystemTimeStep;           !- Update Frequency
-
-
-  Output:Variable,*,Erl VRF Control Status, detailed;
-  Output:Variable,*,VRF Heat Pump Operating Mode, detailed;
-  Output:Variable,*,Cooling Coil Runtime Fraction, detailed;
-  Output:Variable,*,Heating Coil Runtime Fraction, detailed;
-
-
-  EnergyManagementSystem:ProgramCallingManager,
-    Init VRF Control Mode Constants,  !- Name
-    BeginNewEnvironment,           !- EnergyPlus Model Calling Point
-    InitializeVRFControlModes;     !- Program Name 1
-
-
-  EnergyManagementSystem:Program,
-    InitializeVRFControlModes,     !- Name
-    Set VRF_Status_Off = 0.0,      !- Program Line 1
-    Set VRF_Status_Cooling = 1.0,  !- Program Line 2
-    Set VRF_Status_Heating = 2.0;  !- Program Line 3
-
-
-  EnergyManagementSystem:GlobalVariable,
-    VRF_Status_Off,                !- Erl Variable 1 Name
-    VRF_Status_Cooling,            !- Erl Variable 2 Name
-    VRF_Status_Heating;            !- Erl Variable 3 Name
-```
-
-
-Example 13. Surface Construction Actuator for Thermochromic Window
-------------------------------------------------------------------
-
-### Problem Statement
-
-There are a variety of novel new technologies for dynamic thermal envelopes that are the subject of research and development. Can we use EMS to investigate dynamic envelope technologies?
-
-### EMS Design Discussion
-
-As an example, we will show how to use the EMS to replicate a thermochromic window.  EnergyPlus already has a dedicated model for thermochromic windows (see the input object WindowMaterial:GlazingGroup:Thermochromic) that is demonstrated in the example file called ThermochromicWindow.idf.  For this EMS example we will start with that file, remove the WindowMaterial:GlazingGroup:Thermochromic and emulate the thermochromic window using the EMS actuator called “Surface� with the control type “Construction State.�
-
-The first step is to create the individual Construction objects that will represent the individual states.  The original thermochromic example file already includes a series of WindowMaterial:Glazing input objects that correspond to the properties of the thermochromic glazing at different temperatures.  These glazing layers are then used in a series of Construction objects that represent the entire glazing system description at each temperature “state.�  Separate EnergyManagementSystem:ConstructionIndexVariable objects are then added for each Construction to setup Erl variables that point to each construction.
-
-The control algorithm is very simple.  The temperature of the glazing is used in a long IF-ELSEIF-ELSE-ENDIF block to select the appropriate construction to assign the surface.  In this case the native thermochromic model has an important advantage in that the dedicated model can access the temperature of the middle pane in a triple glazed window whereas the EMS model can only access the temperature of the outside pane or the inside pane.  Here we use the temperature of the outside face of the surface because it is closer to the temperature of the middle pane (which can be much higher when in direct sun).
-
-### EMS Input Objects
-
-The main input objects that implement this example of EMS-based thermochromic glazing system are listed below.  The surface called “Perimeter\_ZN\_1\_wall\_south\_Window\_1� is the one being actuated by EMS and we can observe the outcomes of the override by reporting the output variable called Surface Construction Index.  See the example file called EMSThermochromicWindow.idf.
-
-
-
-```idf
-  Construction,
-    TCwindow_25,                !- Name
-    Clear3PPG,               !- Outside Layer
-    AIR 3MM,                 !- Layer 2
-    WO18RT25,              !- Layer 3
-    AIR 8MM,                 !- Layer 4
-    SB60Clear3PPG;           !- Layer 5
-
-
-  EnergyManagementSystem:ConstructionIndexVariable,
-    TCwindow_25,
-    TCwindow_25;
-
-
-  Construction,
-    TCwindow_27,                !- Name
-    Clear3PPG,               !- Outside Layer
-    AIR 3MM,                 !- Layer 2
-    WO18RT27,              !- Layer 3
-    AIR 8MM,                 !- Layer 4
-    SB60Clear3PPG;           !- Layer 5
-
-
-  EnergyManagementSystem:ConstructionIndexVariable,
-    TCwindow_27,
-    TCwindow_27;
-
-
- <<SNIPPED states between 27C and 80C>>
-
-
-  Construction,
-    TCwindow_80,                !- Name
-    Clear3PPG,               !- Outside Layer
-    AIR 3MM,                 !- Layer 2
-    WO18RT80,              !- Layer 3
-    AIR 8MM,                 !- Layer 4
-    SB60Clear3PPG;           !- Layer 5
-
-
-  EnergyManagementSystem:ConstructionIndexVariable,
-    TCwindow_80,
-    TCwindow_80;
-
-
-  Construction,
-    TCwindow_85,                !- Name
-    Clear3PPG,               !- Outside Layer
-    AIR 3MM,                 !- Layer 2
-    WO18RT85,              !- Layer 3
-    AIR 8MM,                 !- Layer 4
-    SB60Clear3PPG;           !- Layer 5
-
-
-  EnergyManagementSystem:ConstructionIndexVariable,
-    TCwindow_85,
-    TCwindow_85;
-
-
-  EnergyManagementSystem:Sensor,
-    Win1_Tout,
-    Perimeter_ZN_1_wall_south_Window_1,
-    Surface Outside Face Temperature;
-
-
-  EnergyManagementSystem:Actuator,
-    Win1_Construct,
-    Perimeter_ZN_1_wall_south_Window_1,
-    Surface,
-    Construction State;
-
-
-  EnergyManagementSystem:ProgramCallingManager,
-    My thermochromic window emulator,
-    BeginTimestepBeforePredictor,
-    ZN_1_wall_south_Window_1_Control;
-
-
-  EnergyManagementSystem:Program,
-    ZN_1_wall_south_Window_1_Control,
-    IF Win1_Tout <= 26.0 ,
-      Set Win1_Construct = TCwindow_25,
-    ELSEIF Win1_Tout <= 28.0 ,
-      SEt Win1_Construct = TCwindow_27,
-    ELSEIF Win1_Tout <= 30.0 ,
-      SET Win1_Construct = TCwindow_29,
-    ELSEIF Win1_Tout <= 32.0 ,
-      SET Win1_Construct = TCwindow_31,
-    ELSEIF Win1_Tout <= 34.0 ,
-      SET Win1_Construct = TCwindow_33,
-    ELSEIF Win1_Tout <= 36.0 ,
-      SET Win1_Construct = TCwindow_35,
-    ELSEIF Win1_Tout <= 38.0 ,
-      SET Win1_Construct = TCwindow_37,
-    ELSEIF Win1_Tout <= 40.0 ,
-      SET Win1_Construct = TCwindow_39,
-    ELSEIF Win1_Tout <= 42.0 ,
-      SET Win1_Construct = TCwindow_41,
-    ELSEIF Win1_Tout <= 44.0 ,
-      SET Win1_Construct = TCwindow_43,
-    ELSEIF Win1_Tout <= 47.5 ,
-      SET Win1_Construct = TCwindow_45,
-    ELSEIF Win1_Tout <= 52.5 ,
-      SET Win1_Construct = TCwindow_50,
-    ELSEIF Win1_Tout <= 57.5 ,
-      SET Win1_Construct = TCwindow_55,
-    ELSEIF Win1_Tout <= 62.5 ,
-      SET Win1_Construct = TCwindow_60,
-    ELSEIF Win1_Tout <= 67.5 ,
-      SET Win1_Construct = TCwindow_65,
-    ELSEIF Win1_Tout <= 72.5 ,
-      SET Win1_Construct = TCwindow_70,
-    ELSEIF Win1_Tout <= 77.5 ,
-      SET Win1_Construct = TCwindow_75,
-    ELSEIF Win1_Tout <= 82.5 ,
-      SET Win1_Construct = TCwindow_80,
-    ELSE ,
-      SET Win1_Construct = TCwindow_85,
-    ENDIF;
-
-
-Output:Variable, Perimeter_ZN_1_wall_south_Window_1, Surface Construction Index, timestep;
-```
-
-
-
-
-Debugging EMS Programs
-======================
-
-This section discusses approaches to debugging Erl programs. As you develop your own programs, you will need to identify and correct coding problems. The task of debugging an Erl program is challenging. Compared to most programming, with integrated development environments and sophisticated debugging interfaces, the Erl programmer has only rudimentary tools available for debugging. If you have some type of developer license and EnergyPlus source code, you could debug Erl programs inside a full-featured debugging environment (such as IVF integrated into VS9). But this is only for extremely advanced users and developers implementing EMS related code inside EnergyPlus. Most users’ EMS should have little need to deal with compilers and development environments, because enough information is produced by EnergyPlus when it runs their Erl programs. This section examines output related to EMS in an effort to help you debug your Erl programs.
-
-ERR File
---------
-
-A key output file to review is the ERR file (eplusout.err), the one with the “.err� file extension. This is the common error file for all of EnergyPlus, and many EMS-related errors will appear there. The file might contain critical problems that arose while the Erl programs were being read in and processed. Although the EDD file will likely be the focus of most debugging, remember the ERR file. Also, sometimes no EDD file is produced from a run. This occurs when problems are captured early during input processing and the program fatals out before an Erl program is run. Depending on the run manager you use to execute EnergyPlus, the EDD file may be from a previous run, so check the file creation times for ERR and EDD.
-
-An especially important error revealed in the ERR file is truncation from too long input. Each program line in Erl is limited to 100 characters. (It becomes useful to keep variable names shorter in Erl because the line length limit can be onerous.)  If there are more than 100 characters, the program truncates the line to the first 100. This will often throw a severe error that halts because the truncated line is not a valid statement. But an unlucky truncation may form a viable line of code and the program will run. Truncation of any Erl program line is surely a bad thing, so it is important to check the ERR file.
-
-EDD File
---------
-
-If the Erl programs are processed and start running, the EDD becomes a primary source of information for debugging. The EDD file is the output file associated only with the EMS. When a line of Erl code is executed, and full trace is selected, the program will output records that are useful for debugging.
-
-It is very important to be careful with the EDD file. There are options to control how verbose the EDD file becomes with modes such as only the errors or a full trace. The full trace option should be used with care because a full line-by-line trace of EMS program execution for an annual run can easily create an enormous file that is too large for most computer systems.
-
-Line Trace
-----------
-
-You can use the EDD file to examine the execution of every line of code. If you request a verbose level of debugging output in the Output:EnergyManagementSystem input object, the EDD file will contain a series of text records that trace the execution of each line of Erl code. Traces contain the name of the program, the program line number, the text of the line, the result returned by executing the line (if any), and a timestamp that indicates when it was executed during the environment period. Note that the EDD file is only produced if you have EMS/Erl programs in your input file.
-
-An example of a single trace follows. This is one record, or single line of text from one of the traces in an EDD file.
-
-```
-VAV1MIXEDAIRMANAGERS,Line 1,SET VAV_1_COOLC_SETPOINT = SEASONAL_RESET_SAT_SCHED - ( T_VAV1FANOUT - T_VAV1FANIN),13.0000000000000, During Warmup, Occurrence info=CHICAGO IL USA TMY2-94846 WMO\#=725300, 01/01 18:30 - 18:45
-```
-
-Each block of text is separated by comma, so the trace information could be read into a spreadsheet and formatted to columns using comma separation.
-
-“VAV1MIXEDAIRMANAGERS� is the name of a user-defined Erl Program.
-
-“Line 1� indicates that this trace is from the first line of the Erl program called VAV1MIXEDAIRMANAGERS.
-
-The next block of text, “SET VAV\_1\_COOLC\_SETPOINT = SEASONAL\_RESET\_SAT\_SCHED - ( T\_VAV1FANOUT - T\_VAV1FANIN)� is the Erl program statement contained at Line 1 in the Erl program called VAV1MIXEDAIRMANAGERS.
-
-The value “13.0000000000000� is the result of this particular SET statement. The value of 13.0 has been assigned to the variable called VAV\_1\_COOLC\_SETPOINT.
-
-The next block of text “During Warmup� indicates that the line was executed while the simulation was in a warm up phase. (Warmup happens during the beginning of each environment period to precondition the model’s transients with the conditions of the first day.)
-
-The next block of text “Occurrence info=CHICAGO IL USA TMY2-94846 WMO\#=725300� indicates the environment period being simulated. This is a weather-file-based RunPeriod for Chicago using TMY2 data source associated with weather station number 725300.
-
-The last block of text “01/01 18:30 - 18:45� is the date and time of day for the simulation timestep when the Erl program line was executed.
-
-
-
-Debugging Strategies
---------------------
-
-This section attempts to provide some debugging tips.
-
-There is no debugging environment, so the main way to obtain information is to use verbose mode and trace each line.
-
-Say, for example, we are trying to debug the following line:
-
-```
- ELSEIF (Hour >= 5) && (Hour < 19)  && (DayOfWeek >=2) && (DayOfWeek <=6) ,
-```
-
-The line trace, shown next, shows only the result of the logical condition, i.e., 0.0 (highlighted) if overall it is false or 1.0 if overall it is true.
-
-```
-MYCOMPUTEDHEATINGSETPOINTPROG,Line 10,ELSEIF (HOUR >= 5) && (HOUR < 19)  && (DAYOFWEEK >=2) && (DAYOFWEEK <=6),0.0, Occurrence info=CHICAGO IL USA TMY2-94846 WMO\#=725300, 09/23 10:20 - 10:30
-```
-
-To debug what is going on with the individual terms in the logical expression, we can add some otherwise useless statements so line traces contain an echo of the current values of the HOUR and DAYOFWEEK built-in variables. So if we add the following lines before the start of the IF block,
-
-```
-    Set locHour = Hour, ! echo out for debug
-    Set locDay = DayOfWeek, ! echo out for debug
-```
-
-We will see the values that Hour and DayOfWeek contain in the debug output. The local variables Erl variables locHour and locDay do not need to be used for anything, but by adding these Erl statements we can glean debugging insights.
-
-The line of Erl code is switched to all uppercase on input, so the line trace differs from the input file in that all characters are capitalized. If the input file was developed using a CamelCase convention, it may be much more difficult to read in the line trace output. Thus, the underscore character “\_� may be a more useful convention for inputting Erl code because it will be more readable in the debugging traces.
-
-
diff --git a/doc/src/docs/EngineeringReference/01-Overview.md b/doc/src/docs/EngineeringReference/01-Overview.md
deleted file mode 100644
index 36169098007..00000000000
--- a/doc/src/docs/EngineeringReference/01-Overview.md
+++ /dev/null
@@ -1,148 +0,0 @@
-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Engineering Reference</h1>
-<h2>The Reference to EnergyPlus Calculations</h2>
-<br/>
-<p><i>(in case you want or need to know)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-
-Overview
-========
-
-Document Overview
------------------
-
-This document is organized to give you the best possible look into the EnergyPlus calculations. First, the concepts of modeling in EnergyPlus are presented. These include descriptions of the zone heat balance process, air loop/plant loop processes as well as other important processes for the building simulation.
-
-Discussions during the modeling process may reference specific “object names� as found in the Input/Output Reference document.
-
-The remainder of the document focuses on individual models.
-
-General Modeling Overview
--------------------------
-
-The EnergyPlus program is a collection of many program modules that work together to calculate the energy required for heating and cooling a building using a variety of systems and energy sources. It does this by simulating the building and associated energy systems when they are exposed to different environmental and operating conditions. The core of the simulation is a model of the building that is based on fundamental heat balance principles. Since it is relatively meaningless to state: “based on fundamental heat balance principles�, the model will be described in greater detail in later sections of this document in concert with the FORTRAN code which is used to describe the model. It turns out that the model itself is relatively simple compared with the data organization and control that is needed to simulate the great many combinations of system types, primary energy plant arrangements, schedules, and environments. The next section shows this overall organization in schematic form. Later sections will expand on the details within the blocks of the schematic.
-
-![](media/image1.png)
-
-Figure 1. EnergyPlus Program Schematic
-
-Simulation Manager
-------------------
-
-The simulation manager of EnergyPlus is contained in a single module. The main subroutine is shown below. Flow within the entire program is managed using a series of flags. These paired flags, in order (from the highest to the lowest) are:
-
-Table 1. Simulation Flags
-
-<table class="table table-striped">
-<tr>
-<td>BeginSimulationFlag</td>
-<td>EndSimulationFlag</td>
-</tr>
-<tr>
-<td>BeginEnvironmentFlag</td>
-<td>EndEnvironmentFlag(one to many days)</td>
-</tr>
-<tr>
-<td>BeginDayFlag</td>
-<td>EndDayFlag</td>
-</tr>
-<tr>
-<td>BeginHourFlag</td>
-<td>EndHourFlag</td>
-</tr>
-<tr>
-<td>BeginTimeStepFlag</td>
-<td>EndTimeStepFlag</td>
-</tr>
-</table>
-
-There is also a **WarmupFlag** to signal that the program is in warmup state. The operation of these flags can be seen in the following subroutine. The advantage of using the flag system is that any subroutine throughout the code can determine the exact state of the simulation by checking the status of the flags.
-
-````
-SUBROUTINE ManageSimulation     ! Main driver routine for this module
-BeginSimFlag = .TRUE.
-  EndSimFlag = .FALSE.
-  CALL OpenOutputFiles
-  CALL GetProjectData
-  CALL GetEnvironmentInfo                 ! Get the number and type of Environments
-  DO Envrn = 1, NumOfEnvrn        ! Begin environment loop ...
-    BeginEnvrnFlag = .TRUE.
-    EndEnvrnFlag   = .FALSE.
-    WarmupFlag     = .TRUE.
-    DayOfSim       =  0
-    DO WHILE ((DayOfSim.LT.NumOfDayInEnvrn).OR.(WarmupFlag))  ! Begin day loop ...
-      DayOfSim     = DayOfSim + 1
-      BeginDayFlag = .TRUE.
-      EndDayFlag   = .FALSE.
-      DO HourOfDay = 1, 24      ! Begin hour loop ...
-        BeginHourFlag = .TRUE.
-        EndHourFlag   = .FALSE.
-          DO TimeStep = 1, NumOfTimeStepInHour  ! Begin time step (TINC) loop ...
-          BeginTimeStepFlag = .TRUE.
-          EndTimeStepFlag   = .FALSE.
-          ! Set the End\_\_Flag variables to true if necessary. Note that each flag builds on
-          ! the previous level. EndDayFlag cannot be .true. unless EndHourFlag is also .true., etc.
-          ! Note that the EndEnvrnFlag and the EndSimFlag cannot be set during warmup.
-          ! Note also that BeginTimeStepFlag, EndTimeStepFlag, and the
-          ! SubTimeStepFlags can/will be set/reset in the HVAC Manager.
-          IF ((TimeStep.EQ.NumOfTimeStepInHour)) THEN
-            EndHourFlag = .TRUE.
-            IF (HourOfDay.EQ.24) THEN
-              EndDayFlag = .TRUE.
-              IF ((.NOT.WarmupFlag).AND.(DayOfSim.EQ.NumOfDayInEnvrn)) THEN
-                EndEnvrnFlag = .TRUE.
-                IF (Envrn.EQ.NumOfEnvrn) THEN
-                  EndSimFlag = .TRUE.
-                END IF
-              END IF
-            END IF
-          END IF
-          CALL ManageWeather
-          CALL ManageHeatBalance
-          BeginHourFlag  = .FALSE.
-          BeginDayFlag   = .FALSE.
-          BeginEnvrnFlag = .FALSE.
-          BeginSimFlag   = .FALSE.
-        END DO                              ! ... End time step (TINC) loop.
-      END DO                    ! ... End hour loop.
-    END DO                      ! ... End day loop.
-  END DO                        ! ... End environment loop.
-  CALL CloseOutputFiles
-  RETURN
-END SUBROUTINE ManageSimulation
-````
-
-Warmup Convergence
-------------------
-
-At the beginning of each new environment (design day or runperiod) zone and surface temperatures are initialized to 23C, and zone humidity ratios are initialized to the outdoor humidity ratio. The first day of the environment is repeated until the loads/temperature convergence tolerance values specified in the Building object are satisfied or until it reaches “maximum number of warmup days�.
-
-Since everything in EnergyPlus is based on the foundation of the loads simulation, it stands to reason that any inaccuracies in the loads calculation will result in inaccuracies of similar or larger magnitude in the HVAC calculations. In the presumably limited cases where convergence was not truly achieved before the actual simulation began, it is unknown how much error would be introduced into the results. While simulations that last longer (annual vs. design day) will hopefully have any initial condition problems balanced by the shear number of days in the simulation, shorter simulations—particularly those used for sizing—could result in relatively large errors. The simulation results could be unreliable and inaccurate when steady periodic conditions are not achieved. Therefore, it is important to properly determine when there is enough temperature and flux history terms to start an EnergyPlus simulation since this has a potential economic and energy impact on buildings that use EnergyPlus in design.
-
-EnergyPlus determines warmup convergence in the following manner as shown in the Figure 2 below. The process of the convergence checks begins by tracking four parameters such including the maximum zone air temperature, the minimum zone air temperature, the maximum heating load, and the maximum cooling load for individual zone. It is note that these convergence checks are only in effective in simulations with at least one zone since the criteria is solely based on the maximum and minimum values obtained from an individual zone. Differences in these parameters between two consecutive days are then compared with the convergence tolerance values at the end of the day during the warmup period. For example, the maximum and minimum air temperature and the percentage difference of zone load for each zone at 9:00AM during the second to last warmup is compared to the values at 9:00AM last warmup day as follows:
-
-<div>$${T_{\max ,prev}} - {T_{\max }} &lt; {T_{tol}}$$</div>
-
-<div>$${T_{\min ,prev}} - {T_{\min }} &lt; {T_{tol}}$$</div>
-
-<div>$$\frac{{{q_h} - {q_{h,prev}}}}{{{q_h}}} &lt; {q_{tol}}$$</div>
-
-<div>$$\frac{{{q_c} - {q_{c,prev}}}}{{{q_c}}} &lt; {q_{tol}}$$</div>
-
-where Tmax,prev is the maximum zone temperature of previous day, Tmax is the maximum zone temperature of current day, Ttol is the value of temperature tolerance, qh,prev is the maximum heating load of previous day, qh, is the maximum heating load of current day, qtol is the value of load tolerance, qc,prev is the maximum cooling load of previous day, and qc, is the maximum cooling load of current day.
-
-Note that a minimum load of 100W is used to establish a fraction for the maximum loads when they are less than the minimum. This is done to avoid a false negative indication for the percentage load difference that may appear when zonal loads are very small. The convergence checks are repeated until passed for all zones. EnergyPlus assumes that the warmup period has been reached steady-periodic when these four parameters are within tolerance. Finally, temperature and load differences between the last two warmup days for individual zone at each time step in the last warmup day are reported so that users can easily track whether or not the warmup period has converged. The input parameters and output related to the warmup period are discussed in the Input-Output Reference.
-
-![](media/image6.png)
-
-Figure 2. Flows of Warmup Convergence Checks
-
diff --git a/doc/src/docs/EngineeringReference/02-IntegratedSolution.md b/doc/src/docs/EngineeringReference/02-IntegratedSolution.md
deleted file mode 100644
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--- a/doc/src/docs/EngineeringReference/02-IntegratedSolution.md
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-Integrated Solution Manager
-===========================
-
-EnergyPlus is an integrated simulation. This means that all three of the major parts, building, system, and plant, must be solved simultaneously. In programs with sequential simulation, such as BLAST or DOE-2, the building zones, air handling systems, and central plant equipment are simulated sequentially with no feedback from one to the other. The sequential solution begins with a zone heat balance that updates the zone conditions and determines the heating/cooling loads at all time steps. This information is fed to the air handling simulation to determine the system response; but that response does not affect zone conditions. Similarly, the system information is passed to the plant simulation without feedback. This simulation technique works well when the system response is a well-defined function of the air temperature of the conditioned space. For a cooling situation, a typical supply and demand situation is shown schematically in the Figure 3. Here, the operating point is at the intersection of the supply and demand curves.
-
-![](media/image7.png)
-
-Figure 3. Sequential Simulation Supply/Demand Relationship.
-
-However, in most situations the system capacity is dependent on outside conditions and/or other parameters of the conditioned space. The simple supply and demand situation above becomes a more complex relationship and the system curve is not fixed. The solution should move up and down the demand curve. This doesn’t happen in sequential simulation methods and the lack of feedback from the system to the building can lead to nonphysical results. For example, if the system provides too much cooling to a conditioned space the excess is reported by the program as "overcooling". Other categories of unmatched loads exist and are similarly reported by the program. While this kind of reporting enables the affected system or plant components to be properly sized, the system designer would, in most cases, prefer to see the actual change in zone temperature. The same mismatches can occur between the system and plant simulations when they are simulated sequentially.
-
-To obtain a simulation that is physically realistic, the elements have to be linked in a simultaneous solution scheme. The entire integrated program can be represented as a series of functional elements connected by fluid loops as shown in Figure “Schematic of Simultaneous Solution Scheme�. In EnergyPlus all the elements are integrated and controlled by the Integrated Solution Manager. The loops are divided into supply and demand sides, and the solution scheme generally relies on successive substitution iteration to reconcile supply and demand using the Gauss-Seidell philosophy of continuous updating.
-
-![](media/image8.png)
-
-Figure 4. Schematic of Simultaneous Solution Scheme
-
-In the sections which follow, the various individual functions of the integrated solution will be described.
-
-Basis for the Zone and Air System Integration
----------------------------------------------
-
-The basis for the zone and air system integration is to formulate energy and moisture balances for the zone air and solve the resulting ordinary differential equations using a predictor-corrector approach. The formulation of the solution scheme starts with a heat balance on the zone air.
-
-<div>$${C_z}\frac{{d{T_z}}}{{dt}} = \sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}\left( {{T_{zi}} - {T_z}} \right)\, + {\dot m_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right) + {\dot Q_{sys}}$$</div>
-
-where:
-
-<span>$\sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}} $</span> = sum of the convective internal loads
-
-<span>$\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right)$</span> = convective heat transfer from the zone surfaces
-
-<span>${\dot m_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right)$</span> = heat transfer due to infiltration of outside air
-
-<span>$\sum_{i=1}^{N_{zones}} \dot m_i C_p\left( T_{zi} - {T_z} \right)$</span> = heat transfer due to interzone air mixing
-
-<span>${\dot Q_{sys}}$</span> = air systems output
-
-<span>${C_z}\frac{{d{T_z}}}{{dt}} = $</span>energy stored in zone air
-
-C<sub>z</sub> = �<sub>air</sub>C<sub>p</sub>C<sub>T</sub>
-
-�<sub>air</sub> = zone air density
-
-C<sub>p</sub> = zone air specific heat
-
-C<sub>T</sub> = sensible heat capacity multiplier (Detailed description is provided below)
-
-If the air capacitance is neglected, the steady-state system output must be:
-
-<div>$$ - {\dot Q_{sys}} = \sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}\left( {{T_{zi}} - {T_z}} \right)\, + {\dot m_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right)$$</div>
-
-Air systems provide hot or cold air to the zones to meet heating or cooling loads. The system energy provided to the zone, Qsys, can thus be formulated from the difference between the supply air enthalpy and the enthalpy of the air leaving the zone as in Equation :
-
-<div>$${\dot Q_{sys}} = {\dot m_{sys}}{C_p}\left( {{T_{\sup }} - {T_z}} \right)$$</div>
-
-This equation assumes that the zone supply air mass flow rate is exactly equal to the sum of the air flow rates leaving the zone through the system return air plenum and being exhausted directly from the zone. Both air streams exit the zone at the zone mean air temperature. The result of substituting Equation for Qsys in the heat balance Equation is shown in Equation :
-
-<div>$$
-  \begin{array}{ll}
-    {C_z}\frac{{d{T_z}}}{{dt}} &= \sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}\left( {{T_{zi}} - {T_z}} \right) \\
-                               &+ {{\dot m}_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right) + {{\dot m}_{sys}}{C_p}\left( {{T_{\sup }} - {T_z}} \right)
-  \end{array}
-$$</div>
-
-The sum of zone loads and air system output now equals the change in energy stored in the zone. Typically, the capacitance Cz would be that of the zone air only. However, thermal masses assumed to be in equilibrium with the zone air could be included in this term.
-
-EnergyPlus provides three different solution algorithms to solve the zone air energy and moisture balance equations. These are defined in the Algorithm field in the ZoneAirHeatBalanceAlgorithm object: 3rdOrderBackwardDifference, EulerMethod and AnalyticalSolution. The first two methods to solve Equation use the finite difference approximation while the third uses an analytical solution. A short description is given below.
-
-In order to calculate the derivative term with respect to time, a finite difference approximation may be used, such as:
-
-<div>$$\frac{{dT}}{{dt}} = {\left( {\delta t} \right)^{ - 1}}\left( {{T_z}^t - {T_z}^{t - \delta t}} \right) + {\rm O}\left( {\delta t} \right)$$</div>
-
-The use of numerical integration in a long time simulation is a cause for some concern due to the potential build-up of truncation error over many time steps. In this case, the finite difference approximation is of low order that further aggravates the problem. However, the cyclic nature of building energy simulations should cause truncation errors to cancel over each daily cycle so that no net accumulation of error occurs, even over many days of simulation (Walton, 1990). The Euler formula, Equation , was employed in Equation to replace the derivative term. All the terms containing the zone mean air temperature were then grouped on the left hand side of the equation.  Since the remaining terms are not known at the current time, they were lagged by one time step and collected on the right hand side. This manipulation resulted in Equation , the formula for updating the zone mean air temperature:
-
-<div>$$\begin{array}{l}{C_z}\frac{{T_z^t - T_z^{t - \delta t}}}{{dt}} + T_z^t\left( {\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}{C_p}} \right) = \\\sum\limits_{i = 1}^{{N_{sl}}} {\dot Q_i^t}  + {{\dot m}_{sys}}{C_p}T_{{\rm{supply}}}^t + {\left( {\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}} + {{\dot m}_{\inf }}{C_p}{T_\infty }} \right)^{t - \delta t}}\end{array}$$</div>
-
-One final rearrangement was to move the lagged temperature in the derivative approximation to the right side of the equation. The explicit appearance of the zone air temperature was thus eliminated from one side of the equation. An energy balance equation that includes the effects of zone capacitance was then obtained by dividing both sides by the coefficient of Tz:
-
-<div>$$T_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {\dot Q_i^t}  + {{\dot m}_{sys}}{C_p}T_{{\rm{supply}}}^t + {{\left( {{C_z}\frac{{T_z^{}}}{{\delta t}} + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}} + {{\dot m}_{\inf }}{C_p}{T_\infty }} \right)}^{t - \delta t}}}}{{\frac{{{C_z}}}{{\delta t}} + \left( {\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}{C_p}} \right)}}$$</div>
-
-Equation could be used to estimate zone air temperatures, and is defined as the EulerMethod, one of the three solution algorithms provided in the ZoneAirHeatBalanceAlgorithm object. However, it can severely limit the time step size under some conditions. To improve on this, higher order expressions for the first derivative, with corresponding higher-order truncation errors, were developed. The goal of this approach was to allow for the use of larger time steps in the simulation than would be possible using the first order Euler form, without experiencing instabilities. Approximations from second through fifth order were tried as reported by Taylor, et al. (1990) with the conclusion that the third order finite difference approximation, shown below, gave the best results:
-
-<div>$${\left. {\frac{{d{T_z}}}{{dt}}} \right|_t} \approx {\left( {\delta t} \right)^{ - 1}}\left( {\frac{{11}}{6}T_z^t - 3T_z^{t - \delta t} + \frac{3}{2}T_z^{t - 2\delta t} - \frac{1}{3}T_z^{t - 3\delta t}} \right) + O\left( {\delta {t^3}} \right)$$</div>
-
-When this form for the derivative is used, equation changes to:
-
-<div>$$\begin{array}{l}{C_z}{\left( {\delta t} \right)^{ - 1}}\left( {\frac{{11}}{6}T_z^t - 3T_z^{t - \delta t} + \frac{3}{2}T_z^{t - 2\delta t} - \frac{1}{3}T_z^{t - 3\delta t}} \right) = \sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}\left( {{T_{zi}} - {T_z}} \right)\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + {{\dot m}_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right) + {{\dot m}_{sys}}{C_p}\left( {{T_{\sup }} - {T_z}} \right)\end{array}$$</div>
-
-and the zone temperature update equation becomes:
-
-<div>$$T_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}}\, + {{\dot m}_{\inf }}{C_p}{T_\infty } + {{\dot m}_{sys}}{C_p}{T_{{\rm{supply}}}} - \left( {\frac{{{C_z}}}{{\delta t}}} \right)\left( { - 3T_z^{t - \delta t} + \frac{3}{2}T_z^{t - 2\delta t} - \frac{1}{3}T_z^{t - 3\delta t}} \right)}}{{\left( {\frac{{11}}{6}} \right)\frac{{{C_z}}}{{\delta t}} + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} A + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}C}}$$</div>
-
-This is the form historically used in EnergyPlus and is the current default referred to as 3rdOrderBackwardDifference in the ZoneAirHeatBalanceAlgorithm object. This algorithm requires zone air temperatures at three previous time steps and uses constant temperature coefficients. The assumption is that three previous time steps lengths are the same.
-
-The AnalyticalSolution algorithm is an integration approach. While the 3<sup>rd</sup> order finite difference approximation provides stability without requiring a prohibitively small time step, the method still has truncation errors and requires a fixed time step length for the previous three simulation time steps. Therefore, different time step lengths for the previous three simulation time steps may make the temperature coefficients invalid.
-
-The AnalyticalSolution algorithm provides a possible way to obtain solutions without truncation errors and independent of time step length. In addition, the algorithm only requires the zone air temperature for one previous time step, instead of three previous time steps as required by the 3rdOrderBackwardDifference algorithm. The integrated (analytical) solution for Eq. (4) may be expressed as follows:
-
-<div>$$\begin{array}{l}T_z^t = \left( {T_z^{t - \delta t} - \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}} + {{\dot m}_{\inf }}{C_p}{T_\infty } + {{\dot m}_{sys}}{C_p}{T_{\sup }}}}{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}{C_p}}}} \right)\\\;\;\;\;\;\;\;*\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}{C_p}}}{{{C_z}}}\delta t} \right)\\\;\;\;\;\;\;\; + \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}} + {{\dot m}_{\inf }}{C_p}{T_\infty } + {{\dot m}_{sys}}{C_p}{T_{\sup }}}}{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {{\dot m}_{\inf }}{C_p} + {{\dot m}_{sys}}{C_p}}}\end{array}$$</div>
-
-Since the load on the zone drives the entire process, that load is used as a starting point to give a demand to the air system. Then a simulation of the air system provides the actual supply capability and the zone temperature is adjusted if necessary. This process in EnergyPlus is referred to as a Predictor/Corrector process. It is summarized below.
-
-Code Reference: the **ZoneTempPredictorCorrector** module performs the calculations.
-
-### Zone Sensible Heat Capacity Multiplier
-
-If the Zone Sensible Heat Capacity Multiplier = 1.0, this represents just the sensible heat capacitance of the air volume in the specified zone. If the value is not defined, it is set to 1.0. This multiplier can be greater than 1.0 if the zone air sensible heat capacity needs to be increased for stability of the simulation. This multiplier increases the capacitance of the air volume by increasing the zone volume that is used in the zone predictor-corrector algorithm in the simulation. This can be done for numerical reasons, such as to increase the stability by decreasing the zone air temperature deviations at the time step level. Or it can be increased to try and account for the additional capacitance in the air loop not specified in the zone, i.e. dampers, diffusers, duct work, etc., to see the effect on the dynamics of the simulation. See the Input/Output Reference for additional information (Object: ZoneCapacitanceMultiplier:ResearchSpecial).
-
-In the source code below we see how the ZoneVolCapMultpSens increases the zone volume used for the air ratio at the time step in the air system. This multiplier is constant throughout the simulation.
-
-````
-    AIRRAT(ZoneNum) = Zone(ZoneNum)%Volume\***ZoneVolCapMultpSens**\* &
-               PsyRhoAirFnPbTdbW(OutBaroPress,MAT(ZoneNum),ZoneAirHumRat(ZoneNum))\* &
-               PsyCpAirFnWTdb(ZoneAirHumRat(ZoneNum),MAT(ZoneNum))/(TimeStepSys\*SecInHour)
-````
-
-
-Summary of Predictor-Corrector Procedure
-----------------------------------------
-
-The predictor-corrector scheme can be summarized as follows:
-
- - Using equation , an estimate is made of the air system energy required to balance the equation with the zone air temperature equal to the setpoint temperature.
- - With that quantity as a demand, the air system is simulated to determine its actual supply capability at the time of the simulation. This will include a plant simulation if necessary.
- - The actual air system capability is used in equation to calculate the resulting zone temperature.
-
-Air System Control
-------------------
-
-Previously, the formulation of a new heat balance equation with an unsteady zone capacitance term was discussed Equation . In this equation the updated zone temperature was calculated by removing its explicit dependence from the right hand side and lagging, by one time step, the unknown terms on that side. However, the right hand side still contains implicit dependencies on the zone temperature through the air system control logic; the need for heating or cooling in the zones, is based on zone temperature. In real buildings the control system consists of one or more sensing units in the zone, such as a wall thermostat that samples the air temperature and sends signals to a control unit. The controller looks at the difference between the actual zone temperature and the desired temperature to ascertain if heating or cooling is required and then sends appropriate signals to the air system components to drive the zone temperature closer to the desired value.
-
-Although many control systems use only the zone air temperature to control the air system, most modern energy management systems consider many other variables, such as outside environment conditions. Simulating such controllers would seem to be relatively straightforward in a simulation especially since some of the more complex control problems, such as managing duct pressures and flow rates, are not always modeled. However, real controllers have an advantage because they can sample zone conditions, and thus update air system response, on a time scale much shorter than any characteristic time of the air system or zone. Thus the feedback between zone and air system usually results in steady or, at worst, slowly oscillating zone conditions and air system operation unless the air system is grossly oversized. On the other hand, the numerical model is only able to sample zone conditions at discrete time intervals. In the interest of minimizing computation time, these intervals need to be as long as possible. Frequently, they are of the order of, or longer than, the characteristic times of the air system and zones, except in the case of small air system capacity in relation to zone capacitance. This situation has the potential for unstable feedback between the zone and air system, resulting in an oscillatory or diverging solution.
-
-Prior to implementing the new heat balance method (3rdOrderBackwardDifference) in IBLAST, several air system control strategies were considered. The primary objective was selection of a control method that would be numerically stable over a reasonable range of conditions, realistic from the standpoint of looking and operating like an actual air system controller, and flexible enough to be applied to all current and projected systems. The method actually implemented in IBLAST, and later EnergyPlus, took advantage of the computational model's "knowledge" of how much energy enters or leaves the zone as a function of zone air temperature i.e., the zone load. The real controller, on the other hand, does not have this information. The net zone load is given by Equation :
-
-<div>$${\dot Q_{load}} = \sum\limits_{i = 1}^{{N_{sl}}} {\dot Q_i^{}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}\left( {{T_{si}} - {T_z}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}\left( {{T_{zi}} - {T_z}} \right) + {\dot m_{\inf }}{C_p}\left( {{T_\infty } - {T_z}} \right)$$</div>
-
-This is Equation without the term due to the air system. In addition, Tz is now the *desired* zone temperature as defined by the control system setpoints that must be specified for each zone. An assumption was made that if the air system has sufficient capacity (based on the desired zone air temperature) to meet the zone conditioning requirements (i.e. Qsys=Qload) at the desired zone air temperature then those requirements will be met. On the other hand, if the air system cannot provide enough conditioning to the zone to maintain the desired temperature, then the air system provides its maximum output to the zone and the zone air temperature is allowed to "float."  Equation was used to calculate the air system output required to maintain the desired zone air temperature; the actual zone temperature update was accomplished using Equation . This method was called *predictive system energy balance*. It has many characteristics of a predictor-corrector method since the air system response is first approximated based on a predicted zone temperature and then the actual change in zone temperature is determined from that air system response. The predictive air system energy balance method required that the system controls on air mass flow rate, supply air temperature, etc., be formulated as a function of the zone air temperature. However, this was not a serious drawback. The first example considered was a single zone draw through air system. Typically, such systems have a cooling coil and heating coil in series, and constant air volume flow rate. Single zone draw through systems run at maximum capacity when turned on; so the only way to regulate net air system output and keep the zone air temperature within the desired range is to turn the air system on and off. A simplified schematic of this system type is shown in Figure 5. Simplified Single Zone Draw Through Air System.
-
-![](media/image31.svg.png)
-
-Figure 5. Simplified Single Zone Draw Through Air System
-
-The amount of heating or cooling provided by the air system in relation to the desired zone air temperature is given by:
-
-<div>$${\dot Q_{sys}} = {\dot m_{sys}}{C_p}\eta \left( {{T_{\sup }} - {T_{z,\,desired}}} \right)$$</div>
-
-where h is the fraction of the time step that the air system is turned on and varies between 0 and 1. The supply air temperature is also implicitly limited by the effectiveness of the coils and the operating parameters of the central plant components. These interactions are discussed later.
-
-A far more complex, though again simplified, air system is the variable air volume (VAV) system, shown in Figure 6. Simplified Variable Volume Air System. In VAV systems, the supply air temperature, as well as the supply air volume, are continuous functions of zone air temperature. As shown in Figure 7. Idealized Variable Volume System Operation., when the zone air temperature is between Tcl and Tcu, cooling is required and the air system varies the supply air flow rate while maintaining a constant supply air temperature. When the zone air temperature is between Thl and Thu, heating is required and air is supplied at a constant minimum flow rate while the supply air temperature is varied.
-
-![](media/image33.svg.png)
-
-Figure 6. Simplified Variable Volume Air System.
-
-The next figure (Idealized variable volume system operation) shows idealized behavior of a VAV system; in practice, the air flow rate and temperature are not exact linear functions of zone air temperature.
-
-![](media/image34.svg.png)
-
-Figure 7. Idealized Variable Volume System Operation.
-
-As long as a VAV system has sufficient capacity, the zone air temperatures can be expected to vary within the limits defining the range of operation of the air damper, when cooling, or the throttling range of the reheat coil, when the air system is heating. This means that the desired zone air temperature, used to predict the air system response, is variable and must be calculated in order to determine the air system output. For the purposes of this calculation, the following definitions were found useful:
-
-<div>$${\dot Q_0} = \sum\limits_{i = 1}^{{N_{sl}}} {{{\dot Q}_i}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{T_{zi}} + {\dot m_{\inf }}{C_p}{T_\infty }$$</div>
-
-<div>$${\dot Q_{slope}} = \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p} + {\dot m_{\inf }}{C_p}$$</div>
-
-Equations and are derived, respectively, from the numerator and denominator of Equation but with the system related terms omitted. Also excluded from these expressions are the effects of zone capacitance.
-
-When a zone requires cooling, the VAV system is designed to provide air to that zone at a constant supply air temperature. The amount of cooling is matched to the load by dampers in the supply air duct that vary the air volume flow rate of being supplied to the zone. Assuming that the volume flow rate varies linearly with zone air temperature, the volume flow rate of supply air normalized to the maximum flow rate, or supply air fraction, is given by:
-
-<div>$${\eta_c} = {\eta_{c,\,\min }} + \left( {1 - {\eta_{c,\,\min }}} \right)\left( {\frac{{{T_z} - {T_{c,\,lower}}}}{{{T_{c,\,upper}} - {T_{c,\,lower}}}}} \right);\,{\eta_{c,\,\min }} \le {\eta_c} \le 1.0$$</div>
-
-Normally, the minimum supply air fraction hc,min must be greater than zero to ensure a supply of fresh air sufficient to eliminate contaminants from the zone.
-
-Conversely, when heating is required in a zone, the VAV system becomes a constant volume flow rate system with a variable supply air temperature. The dampers are set to provide air to the zone at the minimum supply air fraction. Throttling the hot water supply to the reheat coil, which effectively alters the coil’s heating capacity, modulates the supply air temperature. Again, assuming the heat energy output varies linearly with zone air temperature and normalizing with respect to the maximum coil output gives the following result:
-
-<div>$${\eta_h} = \left( {\frac{{{T_{h,\,upper}} - {T_z}}}{{{T_{h,\,upper}} - {T_{h,\,lower}}}}} \right);\,0 \le {\eta_h} \le 1.0$$</div>
-
-Observe that when hh is equal to zero, the zone is supplied with air at the cooling coil outlet temperature at the minimum air fraction. Because the control strategies of the VAV system are different whether the air system is heating or cooling, two equations are necessary to describe the air system output in terms of hh and hc. These expressions are as shown in Equations and :
-
-<div>$${\dot Q_{sys,h}} = {\eta_h}{\dot Q_{h/c,\,\max }} + {C_p}\rho {\dot V_{\min }}\left( {{T_{c/c}} - {T_{z,pred,heat}}} \right)$$</div>
-
-<div>$${\dot Q_{sys,c}} = {C_p}\rho \left( {{\eta_c}{{\dot V}_{\max }}} \right)\left( {{T_{c/c}} - {T_{z,pred,cool}}} \right)$$</div>
-
-Equation is valid for zone air temperatures below Th,upper, while Equation is valid for all temperatures above this value. Equating the system output to the zone load, as given by Equation , the definitions of hc and hh were then used to develop expressions for the predicted zone air temperature in the cases of heating and cooling:
-
-<div>$${T_{z,pred,heat}} = \frac{{{{\dot Q}_{h/c,\max }}{T_{h,upper}}}}{{{T_{h,upper}} - {T_{h,lower}}}} + {\dot Q_0} + \frac{{{C_p}\rho {{\dot V}_{\min }}{T_{c/c}}}}{{\frac{{{{\dot Q}_{h/c,\max }}}}{{{T_{h,upper}} - {T_{h,lower}}}} + {C_p}\rho {{\dot V}_{\min }} + {{\dot Q}_{slope}}}}$$</div>
-
-<div>$${T_{z,pred,cool}} = \frac{{{B_1} + \sqrt {B_1^2 + {B_2}} }}{2}$$</div>
-
-where,
-
-<div>$${B_1} = {T_{c/c}} + {T_{c,lower}} - \frac{{{\eta_{c,\min }} - {C_2}}}{{{C_1}}}$$</div>
-
-<div>$${B_2} = 4\left( {\frac{{{C_3}}}{{{C_1}}} + {T_{c/c}}\left( {\frac{{{\eta_{c,\min }}}}{{{C_1}}} - {T_{c,lower}}} \right)} \right)$$</div>
-
-and,
-
-<div>$${C_1} = \frac{{1 - {\eta_{c,\min }}}}{{{T_{c,upper}} - {T_{c,lower}}}}$$</div>
-
-<div>$${C_2} = \frac{{{{\dot Q}_{slope}}}}{{{C_p}\rho {{\dot V}_{\max }}}}$$</div>
-
-<div>$${C_3} = \frac{{{{\dot Q}_0}}}{{{C_p}\rho {{\dot V}_{\max }}}}$$</div>
-
-Once the predicted zone air temperature has been calculated from Equations and , the air system response may be determined. When a zone requires cooling the system supply air temperature is constant at the cooling coil outlet temperature and the volume flow rate is given by:
-
-<div>$${\dot V_{\sup ply}} = {\eta_c}{\dot V_{\max }}$$</div>
-
-where the supply air fraction hc is computed from Equation . When heating is required by the zone, the air system provides air at the minimum volume flow rate and at a temperature given by:
-
-<div>$${T_{\sup ply}} = {T_{c/c}} + \frac{{{\eta_h}{{\dot Q}_{h/c,\max }}}}{{{C_p}\rho {{\dot V}_{\min }}}}$$</div>
-
-The reheat coil capacity fraction hh is determined by using Equation . Once Equation or , has been used, the supply air flow rate and temperature are known. These values are then used in Equation to calculate the updated zone air temperature. The equations describing VAV system operation may be solved without iteration if the cooling coil outlet temperature is constant, i.e. if the coil has infinite capacity, and if the reheat coil capacity varies linearly with zone air temperature. This is not the case, either in practice or in simulations, when realistic coil models are used. Therefore, an iteration scheme was developed that solved these equations simultaneously with the coil performance models.
-
-Moisture Predictor-Corrector
-----------------------------
-
-The transient air mass balance equation for the change in the zone humidity ratio = sum of internal scheduled latent loads + infiltration + system + multizone airflows + convection to the zone surfaces may be expressed as follows:
-
-<div>$$\begin{array}{l}{\rho_{air}}{V_z}{C_W}\frac{{d{W_z}}}{{dt}} = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}\left( {{W_{surf{s_i}}} - W_z^t} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{W_{zi}} - W_z^t} \right)\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; + {{\dot m}_{\inf }}\left( {{W_\infty } - W_z^t} \right) + {{\dot m}_{sys}}\left( {{W_{\sup }} - W_z^t} \right)\end{array}$$</div>
-
-where
-
-C<sub>W</sub> = humidity capacity multiplier (See the InputOutput Reference for additional information on the object ZoneCapacitanceMultiplier:ResearchSpecial)
-
-In the same manner as described above for zone air temperature (ref. Basis for the Zone and Air System Integration), the solution algorithms provided in the ZoneAirHeatBalanceAlgorithm object are also applied to zone air moisture calculations.
-
-In order to calculate the derivative term with respect to time, the first order backward finite difference method, defined as the EulerMethod in the ZoneAirHeatBalanceAlgorithm object, may be used:
-
- <div>$$\frac{{dW}}{{dt}} = {\left( {\delta t} \right)^{ - 1}}(W_z^t - W_z^{t - \delta t}) + O(\delta t)$$</div>
-
-The zone air humidity ratio update at the current time step using the EulerMethod may be expressed as follows:
-
-<div>$$\begin{array}{l}{\rho_{air}}V{C_W}{\left( {\delta t} \right)^{ - 1}}\left( {W_z^t - W_z^{t - \delta t}} \right) = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}\left( {{W_{surf{s_i}}} - W_z^t} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{W_{zi}} - W_z^t} \right)\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; + {{\dot m}_{\inf }}\left( {{W_\infty } - W_z^t} \right) + {{\dot m}_{sys}}\left( {{W_{\sup }} - W_z^t} \right)\end{array}$$</div>
-
-To preserve the stability of the calculation of the zone humidity ratio, the third order differential approximation, derived by a Taylor Series and used in the calculation of the next time step’s zone air temperature, is also applied to the zone air humidity ratio calculations. This algorithm is the default choice and is defined as 3rdOrderBackwardDifference in the ZoneAirHeatBalanceAlgorithm object.
-
-The third order derivative derived from a Taylor Series expansion is defined as:
-
-<div>$${\left. {\frac{{d{W_z}}}{{dt}}} \right|_t} \approx \frac{{\left( {{\textstyle{{11} \over 6}}W_z^t - 3W_z^{t - \delta t} + {\textstyle{3 \over 2}}W_z^{t - 2\delta t} - {\textstyle{1 \over 3}}W_z^{t - 3\delta t}} \right)}}{{\delta t}} + O\left( {\delta {t^3}} \right)$$</div>.
-
-The coefficients of the approximated derivative are very close to the coefficients of the analogous Adams-Bashforth algorithm. Then the approximated derivative is substituted into the mass balance and the terms with the humidity ratio at past time steps are all put on the right hand side of the equation. This third order derivative zone humidity ratio update increases the number of previous time steps that are used in calculating the new zone humidity ratio, and decreases the dependence on the most recent. The higher order derivative approximations have the potential to allow the use of larger time steps by smoothing transitions through sudden changes in zone operating conditions.
-
-<div>$$\begin{array}{l}\frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\left( {\frac{{11}}{6}} \right)W_z^t + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}W_z^t + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} W_z^t + {{\dot m}_{\inf }}W_z^t + {{\dot m}_{sys}}W_z^t = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}}\\\;\;\;\;\;\;\;\;\;\; + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {{\dot m}_{\inf }}{W_\infty } + {{\dot m}_{sys}}{W_{\sup }} - \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\left( { - 3W_z^{t - \delta t} + \frac{3}{2}W_z^{t - 2\delta t} - \frac{1}{2}W_z^{t - 3\delta t}} \right)\end{array}$$</div>
-
-This gives us the basic air mass balance equation that will be solved two different ways, one way for the predict step and one way for the correct step.
-
-Since the third choice of solution algorithms uses an integration approach, defined as AnalyticalSolution in the ZoneAirHeatBalanceAlgorithm object, it does not require any approximations and has no truncation errors. The solutions in both prediction and correction are provided below in detail.
-
-### Moisture Prediction
-
-For the moisture prediction case the equation is solved for the anticipated system response as shown below.
-
-<div>$$
-  \begin{array}{l}
-    \rm{PredictedSystemLoad} = \dot{m}_{sys}*\left(W_z^t - W_{sup}\right) \\
-    \rm{MassFlow * HumRat} = \frac{kg_{air}}{sec}\frac{kg_{water}}{kg_{air}} = \frac{kg_{water}}{sec}
-  \end{array}
-$$</div>
-
-Since the program provides three solution algorithms, the moisture prediction from each solution algorithm is given below.
-
-#### EulerMethod
-
-For this solution algorithm, the air mass balance for the predicted air system load or response is:
-
-<div>$$\begin{array}{l}{\rm{PredictedSystemLoad}}\;[k{g_{Water}}/\sec ] = {\rho_{air}}{V_z}{C_W}{\left( {\delta t} \right)^{ - 1}}\left( {W_{{\rm{setpoint}}}^t - W_z^{t - \delta t}} \right)\\\;\;\;\; - \left[ {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}\left( {{W_{surf{s_i}}} - W_{{\rm{setpoint}}}^t} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{W_{zi}} - W_{{\rm{setpoint}}}^t} \right) + {{\dot m}_{\inf }}\left( {{W_\infty } - W_{{\rm{setpoint}}}^t} \right)} \right]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\end{array}$$</div>
-
-#### ThirdOrderBackwardDifference
-
-For this solution algorithm, the air mass balance for the predicted system load or response is given below:
-
-<div>$$\begin{array}{l}{\rm{PredictedSystemLoad}}\;[k{g_{Water}}/\sec ] = \left( {\frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\left( {\frac{{11}}{6}} \right) + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }}} \right)W_z^t - \\\;\;\;\left[ {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {{\dot m}_{\inf }}{W_\infty } + \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\left( {3W_z^{t - \delta t} - \frac{3}{2}W_z^{t - 2\delta t} + \frac{1}{3}W_z^{t - 3\delta t}} \right)} \right]\;\;\end{array}$$</div>
-
-Then, using the following substitutions, the air mass balance equation becomes:
-
-<div>$$A = \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {\dot m_{\inf }}$$</div>
-
-<div>$$B = \;\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {\dot m_{\inf }}{W_\infty }\;$$</div>
-
-<div>$$C = \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\;$$</div>
-
-<div>$$\begin{array}{l}{\rm{PredictedSystemLoad}}\;[k{g_{Water}}/\sec ] = \left[ {\frac{{11}}{6}*C + A} \right]\;*{W_{SetPo{\mathop{\rm int}} }} - \\\;\;\;\;\;\;\;\;\;\left[ {B + C*\left( {3W_z^{t - \delta t} - \frac{3}{2}W_z^{t - 2\delta t} + \frac{1}{3}W_z^{t - 3\delta t}} \right)} \right]\end{array}$$</div>
-
-#### AnalyticalSolution
-
-For this solution algorithm, the air mass balance for the predicted air system load or response is given below:
-
-<div>$$\begin{array}{l}{\rm{PredictedSystemLoad}}\;[k{g_{Water}}/\sec ] = \left[ {\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}}\; + {{\dot m}_{\inf }}} \right]*\\\;\;\;\left[ {W_{{\rm{setpoint}}}^t - W_z^{t - \delta t}*\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}}\; + {{\dot m}_{\inf }}}}{{{\rho_{air}}{V_z}{C_W}}}\delta t} \right)} \right]*\\\;\;\;{\left[ {1 - \exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }}}}{{{\rho_{air}}{V_z}{C_W}}}\delta t} \right)} \right]^{ - 1}} - \\\;\;\;\left( {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}} \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}}\; + {{\dot m}_{\inf }}{W_\infty }} \right)\end{array}$$</div>
-
-At the prediction point in the simulation, the system air mass flows are not known; therefore, the system response is approximated. The predicted air system moisture load is then used in the system simulation to achieve the best results possible. The system simulation components that have moisture control will try to meet this predicted moisture load. For example, humidifiers will look for positive moisture loads and add moisture at the specified rate to achieve the relative humidity setpoint. Likewise, dehumidification processes will try to remove moisture at the specified negative predicted moisture load to meet the relative humidity setpoint.
-
-After the system simulation is completed the actual response from the air system is used in the moisture correction of step, which is shown next.
-
-### Moisture Correction
-
-For the correct step the expanded air mass balance equation is solved for the final zone humidity ratio at the current time step. When the air system is operating, the mass flow for the system outlet includes the infiltration mass flow rate, therefore the infiltration mass flow rate is not included as a separate term in the air mass balance equation. But when the air system is off, the infiltration mass flow in is then exhausted out of the zone directly.
-
-In the same manner as described above for predicting the moisture load to be met by the air system, the zone air moisture correction calculation will be described individually for the three solution algorithms.
-
-#### EulerMethod
-
-<div>$$W_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {{\dot m}_{\inf }}{W_\infty } + {{\dot m}_{sys}}{W_{\sup }} + {\rho_{air}}{V_z}{C_W}\frac{{W_z^{t - \delta t}}}{{\delta t}}}}{{\frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}} + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}{\rho_{ai{r_z}}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}$$</div>
-
-#### ThirdOrderBackwardDifference
-
-<div>$$W_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {{\dot m}_{\inf }}{W_\infty } + {{\dot m}_{sys}}{W_{\sup }} + \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}(3W_z^{t - \delta t} - \frac{3}{2}W_z^{t - 2\delta t} + \frac{1}{3}W_z^{t - 3\delta t})}}{{\frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\left( {\frac{{11}}{6}} \right) + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}{\rho_{ai{r_z}}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}$$</div>
-
-Using the same A, B, and C parameters from the prediction step modified with actual zone mass flows with the air system ON and OFF result in:
-
-
-
-**If** (ZoneSupplyAirMassFlowRate &gt; 0.0) **Then**
-
-<div>$$A = \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {\dot m_{\inf }} + {\dot m_{sys}}$$</div>
-
-<div>$$B = \;\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {\dot m_{\inf }}{W_\infty }\; + {\dot m_{sys}}{W_{\sup }}$$</div>
-
-<div>$$C = \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\;$$</div>
-
-**Else If** (ZoneSupplyAirMassFlowRate &lt;= 0.0) **Then**
-
-<div>$$A = \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {\dot m_{\inf }} + {\dot m_{Exhaust}}$$</div>
-
-<div>$$B = \;\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}} + {\dot m_{\inf }}{W_\infty }\; + {\dot m_{Exhaust}}{W_\infty }$$</div>
-
-<div>$$C = \frac{{{\rho_{air}}{V_z}{C_W}}}{{\delta t}}\;$$</div>
-
-**End If**
-
-Inserting in the parameters A, B and C above in the air mass balance equation, it simplifies to:
-
-<div>$$W_z^t = \left[ {\frac{{B + C * \left( {3W_z^{t - \delta t} - {\textstyle{3 \over 2}}W_z^{t - 2\delta t} + {\textstyle{1 \over 3}}W_z^{t - 3\delta t}} \right)}}{{\left( {{\textstyle{{11} \over 6}}} \right) * C + A}}} \right]$$</div>
-
-#### AnalyticalSolution
-
-<div>$$\begin{array}{l}W_z^t = \left[ \begin{array}{l}W_z^{t - \delta t} - \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}}\; + {{\dot m}_{\inf }}{W_\infty } + {{\dot m}_{sys}}{W_{\sup }}}}{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}\\\end{array} \right]*\\\;\;\;\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}{{{\rho_{air}}{V_z}{C_W}}}\delta t} \right) + \\\;\;\;\frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}}{W_{surf{s_i}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {W_{zi}}\; + {{\dot m}_{\inf }}{W_\infty } + {{\dot m}_{sys}}{W_{\sup }}}}{{\sum\limits_{i = 1}^{{N_{surfaces}}} {{A_i}{h_{mi}}} {\rho_{ai{r_z}}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}\end{array}$$</div>
-
-The above solutions are implemented in the Correct Zone Air Humidity Ratio step in EnergyPlus. This moisture update equation is used for the Conduction Transfer Function (CTF) heat balance algorithm, in addition to the effective moisture penetration depth (EMPD) with conduction transfer function heat balance algorithm. The equations are identical except that the convection to the zone surfaces is non-zero for the moisture penetration depth case. This moisture update allows both methods to be updated in the same way, with the only difference being the additional moisture capacitance of the zone surfaces for the Effective Moisture Penetration Depth (EMPD) solution approach.
-
-When the HAMT (Combined Heat And Moisture Finite Element) defined in the HeatBalanceAlgorithm object is applied, the moisture update equations are also the same as the equations used in the effective moisture penetration depth (EMPD) with conduction transfer function solution algorithm.
-
-Carbon Dioxide Predictor-Corrector
-----------------------------------
-
-The transient air mass balance equation for the change in zone air carbon dioxide concentration may be expressed as follows:
-
-<div>$${\rho_{air}}{V_z}{C_{CO2}}\frac{{dC_z^t}}{{dt}} = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{zi}} - C_z^t} \right)\; + {\dot m_{\inf }}\left( {{C_\infty } - C_z^t} \right) + {\dot m_{sys}}\left( {{C_{\sup }} - C_z^t} \right)$$</div>
-
-where:
-
-<span>$\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}} $</span> = sum of scheduled internal carbon dioxide loads. The zone air density is used to convert the volumetric rate of carbon dioxide generation from user input into mass generation rate [kg/s].The coefficient of 10<sup>6</sup> is used to make the units of carbon dioxide as ppm.
-
-<span>$\sum_{i=1}^{N_{zones}} \dot m_i \left( C_{zi} - C_z^t \right) $</span> = carbon dioxide transfer due to interzone air mixing [ppm-kg/s]
-
-<span>${C_{zi}}$</span> = carbon dioxide concentration in the zone air being transferred into this zone [ppm]
-
-<span>${\dot m_{\inf }}\left( {{C_\infty } - C_z^t} \right)$</span> = carbon dioxide transfer due to infiltration and ventilation of outdoor air [ppm-kg/s]
-
-<span>${C_\infty }$</span> = carbon dioxide concentration in outdoor air [ppm]
-
-<span>${\dot m_{sys}}\left( {{C_{\sup }} - C_z^t} \right)$</span> = carbon dioxide transfer due to system supply [ppm-kg/s]
-
-<span>${C_{\sup }}$</span> = carbon dioxide concentration in the system supply airstream [ppm]
-
-<span>${\dot m_{sys}}$</span> = air system supply mass flow rate [kg/s]
-
-<span>${\rho_{air}}{V_z}\frac{{dC_z^t}}{{dt}}$</span>= carbon dioxide storage term in zone air [kg/s]
-
-<span>$C_z^t$</span> = zone air carbon dioxide concentration at the current time step [ppm]
-
-<span>${\rho_{air}}$</span>= zone air density [kg/m<sup>3</sup>]
-
-<span>${V_z}$</span>= zone volume [m<sup>3</sup>]
-
-C<sub>CO2</sub> = carbon dioxide capacity multiplier [dimensionless] (See the InputOutput Reference for additional information on the object ZoneCapacitanceMultiplier:ResearchSpecial)
-
-In the same manner as described above for zone air temperature (ref. Basis for the Zone and Air System Integration), the solution algorithms provided in the ZoneAirHeatBalanceAlgorithm object are also applied to the zone air carbon dioxide calculations.
-
-In order to calculate the derivative term with respect to time, the first order backward finite difference method, defined as the EulerMethod in the ZoneAirHeatBalanceAlgorithm object, may be used:
-
-<div>$$\frac{{dC_z^t}}{{dt}} = {\left( {\delta t} \right)^{ - 1}}(C_z^t - C_z^{t - \delta t}) + O(\delta t)$$</div>
-
-The zone air carbon dioxide concentration update at the current time step using the EulerMethod may be expressed as follows:
-
-<div>$${\rho_{air}}{V_Z}{C_{CO2}}{\left( {\delta t} \right)^{ - 1}}\left( {C_z^t - C_z^{t - \delta t}} \right) = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}} *{10^6} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{zi}} - C_z^t} \right) + {\dot m_{\inf }}\left( {{C_\infty } - C_z^t} \right) + {\dot m_{sys}}\left( {{C_{\sup }} - C_z^t} \right)$$</div>
-
-To preserve the stability of the calculation of the zone carbon dioxide concentration, the third order differential approximation, derived by a Taylor Series and used in the calculation of the next time step’s zone air temperature, is also applied to the zone air carbon dioxide calculations. This algorithm is the default choice and is defined as ThirdOrderBackwardDifference in the ZoneAirHeatBalanceAlgorithm object.
-
-The third order derivative derived from a Taylor Series expansion is defined as:
-
-<div>$$\frac{{dC_z^t}}{{dt}} \approx \frac{{\frac{{11}}{6}C_z^t - 3C_z^{t - \delta t} + \frac{3}{2}C_z^{t - 2\delta t} - \frac{1}{3}C_z^{t - 3\delta t}}}{{\delta t}} + O(\delta {t^3})$$</div>
-
-The coefficients of the approximated derivative are very close to the coefficients of the analogous Adams-Bashforth algorithm. Then the approximated derivative is substituted into the mass balance and the terms with the carbon dioxide concentration at past time steps are all put on the right-hand side of the equation. This third order derivative zone carbon dioxide update increases the number of previous time steps that are used in calculating the new zone carbon dioxide concentration, and decreases the dependence on the most recent. The higher order derivative approximations have the potential to allow the use of larger time steps by smoothing transitions through sudden changes in zone operating conditions.
-
-<div>$$\begin{array}{l}\frac{{{\rho_{air}}{V_z}{C_{CO2}}}}{{\delta t}}\left( {\frac{{11}}{6}} \right)C_z^t + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} C_z^t + {{\dot m}_{\inf }}C_z^t + {{\dot m}_{sys}}C_z^t = \sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}} *{10^6}\\\;\;\;\;\;\;\; + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}} + {{\dot m}_{\inf }}{C_\infty } + {{\dot m}_{sys}}{C_{\sup }} - \frac{{{\rho_{air}}{V_z}{C_{CO2}}}}{{\delta t}}( - 3C_z^{t - \delta t} + \frac{3}{2}C_z^{t - 2\delta t} - \frac{1}{3}C_z^{t - 3\delta t})\end{array}$$</div>
-
-This gives us the basic air mass balance equation that will be solved two different ways, one way for the predict step and one way for the correct step.
-
-Since the third choice of solution algorithms uses an integration approach, defined as AnalyticalSolution in the ZoneAirHeatBalanceAlgorithm object, it does not require any approximations and has no truncation errors. The solutions in both prediction and correction are provided below in detail.
-
-### Carbon Dioxide Prediction
-
-For the carbon dioxide concentration prediction case, the equation is solved for the anticipated system response as shown below.
-
-<div>$${\rm{PredictedSystemLoad}} = {\dot m_{sys}}\left( {{C_{\sup }} - C_z^t} \right)$$</div>
-
-Since the program provides three solution algorithms, the carbon dioxide prediction from each solution algorithm is given below.
-
-#### EulerMethod
-
-For this solution algorithm, the air mass balance for the predicted air system load or response is:
-
-<div>$$\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = {\rho_{air}}{V_Z}{C_{CO2}}{\left( {\delta t} \right)^{ - 1}}\left( {C_{{\rm{setpoint}}}^t - C_z^{t - \delta t}} \right)\\\;\;\;\; - \left[ {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}} *{{10}^6} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{zi}} - C_{{\rm{setpoint}}}^t} \right) + {{\dot m}_{\inf }}\left( {{C_\infty } - C_{{\rm{setpoint}}}^t} \right)} \right]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\end{array}$$</div>
-
-#### ThirdOrderBackwardDifference
-
-For this solution algorithm, the air mass balance for the predicted system load or response is given below:
-
-<div>$$\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = \left[ {\frac{{{\rho_{air}}{V_z}{C_{CO2}}}}{{\delta t}}\left( {\frac{{11}}{6}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }}} \right]*C_{{\rm{setpoint}}}^t\\\;\;\;\; - \left[ {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}} + {{\dot m}_{\inf }}{C_\infty } + \frac{{{\rho_{air}}{V_z}{C_{CO2}}}}{{\delta t}}\left( {3C_z^{t - \delta t} - \frac{3}{2}C_z^{t - 2\delta t} + \frac{1}{3}C_z^{t - 3\delta t}} \right)} \right]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\end{array}$$</div>
-
-#### AnalyticalSolution
-
-For this solution algorithm, the air mass balance for the predicted air system load or response is given below:
-
-<div>$$\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = \left[ {\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }}} \right]*\;\left[ {C_{{\rm{setpoint}}}^t - C_z^{t - \delta t}*\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }}}}{{{\rho_{air}}{V_Z}{C_{CO2}}}}\delta t} \right)} \right]*\\\;\;\;{\left[ {1 - \exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }}}}{{{\rho_{air}}{V_Z}{C_{CO2}}}}\delta t} \right)} \right]^{ - 1}} - \;\left( {\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}}\; + {{\dot m}_{\inf }}{C_\infty }} \right)\end{array}$$</div>
-
-At the prediction point in the simulation, the system air mass flows are not known; therefore, the system response is approximated. The predicted air system carbon dioxide load is then used in the system simulation to achieve the best results possible. If a central HVAC system provides the outdoor flow rate from a Controller:MechanicalVentilation object, the outdoor airflow rate may be approximated as:
-
-<div>$${\rm{PredictedSystemLoad}} = {\dot m_{sys}}\left( {{C_{\sup }} - C_z^t} \right) \approx {\dot m_{OA,z}}\left( {{C_\infty } - C_{{\rm{setpoint}}}^t} \right)$$</div>
-
-where:
-
-<span>${\dot m_{OA,z}}$</span>= supply outdoor airflow rate into the controlled zone [kg/s]
-
-The above approximation is based on the assumption that the carbon dioxide concentration at the outdoor air (OA) mixer inlet is equal to the zone air outlet concentration level, and the carbon dioxide level at the zone supply air inlet is equal to the level at the outlet node of the OA mixer.
-
-After the system simulation is completed the actual response from the air system is used in the carbon dioxide correction step, which is shown next.
-
-### Carbon Dioxide Correction
-
-For the correct step the expanded air mass balance equation is solved for the final zone carbon dioxide concentration at the current time step. In the same manner as described above for predicting the carbon dioxide load to be met by the air system, the zone air carbon dioxide correction calculation will be described individually for the three solution algorithms.
-
-
-
-#### EulerMethod
-
-<div>$$C_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}} + {{\dot m}_{\inf }}{C_\infty } + {{\dot m}_{sys}}{C_{\sup }} + {\rho_{air}}{V_Z}{C_{CO2}}\frac{{C_z^{t - \delta t}}}{{\delta t}}}}{{\frac{{{\rho_{air}}{V_Z}{C_{CO2}}}}{{\delta t}} + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}$$</div>
-
-#### ThirdOrderBackwardDifference
-
-<div>$$C_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}} + {{\dot m}_{\inf }}{C_\infty } + {{\dot m}_{sys}}{C_{\sup }} + \frac{{{\rho_{air}}{V_Z}{C_{CO2}}}}{{\delta t}}(3C_z^{t - \delta t} - \frac{3}{2}C_z^{t - 2\delta t} + \frac{1}{3}C_z^{t - 3\delta t})}}{{\frac{{{\rho_{air}}{V_Z}{C_{CO2}}}}{{\delta t}}\left( {\frac{{11}}{6}} \right) + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}$$</div>
-
-#### AnalyticalSolution
-
-<div>$$\begin{array}{l}C_z^t = \left[ {C_z^{t - \delta t} - \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}}\; + {{\dot m}_{\inf }}{C_\infty } + {{\dot m}_{sys}}{C_{sys}}}}{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}} \right]*\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}{{{\rho_{air}}{V_Z}{C_{CO2}}}}\delta t} \right) + \\\;\;\;\frac{{\sum\limits_{i = 1}^{{N_{sl}}} {k{g_{mas{s_{sched\;load}}}}*{{10}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{zi}}\; + {{\dot m}_{\inf }}{C_\infty } + {{\dot m}_{sys}}{C_{sys}}}}{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}}}}\end{array}$$</div>
-
-The above solutions are implemented in the Correct Zone Air Carbon Dioxide step in the Zone Contaminant Predictor Corrector module of EnergyPlus.
-
-Generic Contaminant Predictor-Corrector
----------------------------------------
-
-The transient air mass balance equation for the change in zone air generic contaminant concentration may be expressed as follows:
-
-<div>$$\begin{array}{l}{\rho_{air}}{V_z}{M_{for}}\frac{{dC_{f,z}^t}}{{dt}} = \sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6} - } {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}{C_{f,z}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{f,z,i}} - C_{f,z}^t} \right)\; + {{\dot m}_{\inf }}\left( {{C_{f,\infty }} - C_{f,z}^t} \right)\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; + {{\dot m}_{sys}}\left( {{C_{f,\sup }} - C_{f,z}^t} \right) + \sum\limits_j {{h_j}\rho {A_j}(\frac{{{C_{s,j}}}}{{{k_j}}} - {C_{f,z}})}  + {S_f}(C_{f,z}^{t - \delta t})\end{array}$$</div>
-
-where:
-
-<span>$\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}} $</span>=  Sum of internal generic contaminant loads from sources in a zone or interior surfaces.
-
-The zone air density is used to convert the volumetric rate of generic contaminant generation from user input into mass generation rate [kg/s].The coefficient of 10<sup>6</sup> is used to make the units of generic contaminant as ppm.
-
-<span>${\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}{C_{f,z}}} $</span>= Sum of removal rate from sinks in a zone or interior surfaces [ppm-kg/s]
-
-<span>$\sum_{i=1}^{N_{zones}} \dot m_i \left( C_{f,z,i} - C_{f,z}^t \right)$</span> = Generic contaminant transfer due to interzone air mixing [ppm-kg/s]
-
-<span>${C_{f,z,i}}$</span> = Generic contaminant concentration in the zone air being transferred into this zone [ppm]
-
-<span>${\dot m_{\inf }}\left( {{C_{f,\infty }} - C_{f,z}^t} \right)$</span>   = Generic contaminant transfer due to infiltration and ventilation of outdoor air [ppm-kg/s]
-
-<span>${C_{f,\infty }}$</span> = Generic contaminant concentration in outdoor air [ppm]
-
-<span>${\dot m_{sys}}\left( {{C_{f,\sup }} - C_{f,z}^t} \right)$</span> = Generic contaminant transfer due to system supply [ppm-kg/s]
-
-<span>${C_{f,\sup }}$</span> = Generic contaminant concentration in the system supply airstream [ppm]
-
-<span>${\dot m_{sys}}$</span> = Air system supply mass flow rate [kg/s]
-
-<span>${\rho_{air}}{V_z}\frac{{dC_{f,z}^t}}{{dt}}$</span>= Generic contaminant storage term in zone air [ppm-kg/s]
-
-<span>$C_{f,z}^t$</span> = Zone air generic contaminant concentration at the current time step [ppm]
-
-<span>${\rho_{air}}$</span>= Zone air density [kg/m<sup>3</sup>]
-
-<span>${V_z}$</span>= Zone volume [m<sup>3</sup>]
-
-<span>$\sum\limits_j {{h_j}\rho {A_j}(\frac{{{C_{s,j}}}}{{{k_j}}} - {C_{f,z}})} $</span>       = Generic contaminant transport through diffusion between interior surfaces and zone air
-
-<span>${S_f}(C_{f,z}^{t - \delta t})$</span>= Generic contaminant generation or removal rate as a function of zone air generic contaminant level at the previous time step
-
-Mfor = Generic contaminant capacity multiplier [dimensionless] (See the InputOutput Reference for additional information on the object ZoneCapacitanceMultiplier:ResearchSpecial)
-
-In the same manner as described above for zone air temperature (ref. Basis for the Zone and Air System Integration), the solution algorithms provided in the ZoneAirHeatBalanceAlgorithm object are also applied to the zone air carbon dioxide calculations.
-
-In order to calculate the derivative term with respect to time, the first order backward finite difference method, defined as the EulerMethod in the ZoneAirHeatBalanceAlgorithm object, may be used:
-
-<div>$$\frac{{dC_{f,z}^t}}{{dt}} = {\left( {\delta t} \right)^{ - 1}}(C_{f,z}^t - C_{f,z}^{t - \delta t}) + O(\delta t)$$</div>
-
-The zone air generic contaminant concentration update at the current time step using the EulerMethod may be expressed as follows:
-
-<div>$$\begin{array}{l}{\rho_{air}}{V_z}{M_{for}}{\left( {\delta t} \right)^{ - 1}}\left( {C_{f,z}^t - C_{f,z}^{t - \delta t}} \right) = \sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6} - } {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}{C_{f,z}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{f,z,i}} - C_{f,z}^t} \right)\;\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; + {{\dot m}_{\inf }}\left( {{C_{f,\infty }} - C_{f,z}^t} \right) + {{\dot m}_{sys}}\left( {{C_{f,\sup }} - C_{f,z}^t} \right) + \sum\limits_j {{h_j}\rho {A_j}(\frac{{{C_{s,j}}}}{{{k_j}}} - {C_{f,z}})}  + {S_f}\end{array}$$</div>
-
-To preserve the stability of the calculation of the zone generic contaminant concentration, the third order differential approximation, derived by a Taylor Series and used in the calculation of the next time step’s zone air temperature, is also applied to the zone air carbon dioxide calculations. This algorithm is the default choice and is defined as ThirdOrderBackwardDifference in the ZoneAirHeatBalanceAlgorithm object.
-
-The third order derivative resulting from a Taylor Series expansion is defined as:
-
-<div>$$\frac{{dC_{f,z}^t}}{{dt}} \approx \frac{{\frac{{11}}{6}C_{f,z}^t - 3C_{f,z}^{t - \delta t} + \frac{3}{2}C_{f,z}^{t - 2\delta t} - \frac{1}{3}C_{f,z}^{t - 3\delta t}}}{{\delta t}} + O(\delta {t^3})$$</div>
-
-The coefficients of the approximated derivative are very close to the coefficients of the analogous Adams-Bashforth algorithm. Then the approximated derivative is substituted into the mass balance, and the terms with the carbon dioxide concentration at past time steps are all put on the right-hand side of the equation. This third order derivative zone carbon dioxide update increases the number of previous time steps that are used in calculating the new zone generic contaminant concentration and decreases the dependence on the most recent. The higher order derivative approximations have the potential to allow the use of larger time steps by smoothing transitions through sudden changes in zone operating conditions.
-
-<div>$$\begin{array}{l}\frac{{{\rho_{air}}{V_z}{M_{for}}}}{{\delta t}}\left( {\frac{{11}}{6}} \right)C_{f,z}^t + {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}C_{f,z}^t}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} C_{f,z}^t + {{\dot m}_{\inf }}C_{f,z}^t + {{\dot m}_{sys}}C_{f,z}^t + \sum\limits_j {{h_j}\rho {A_j}C_{f,z}^t} \\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; = \sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{f,z,i}} + {{\dot m}_{\inf }}{C_{f,\infty }} + {{\dot m}_{sys}}{C_{f,\sup }} + \sum\limits_j {{h_j}\rho {A_j}\frac{{{C_{s,j}}}}{{{k_j}}}}  + {S_f}\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; - \frac{{{\rho_{air}}{V_z}{M_{for}}}}{{\delta t}}\left( { - 3C_{f,z}^{t - \delta t} + \frac{3}{2}C_{f,z}^{t - 2\delta t} - \frac{1}{3}C_{f,z}^{t - 3\delta t}} \right)\end{array}$$</div>
-
-This gives us the basic air mass balance equation that will be solved in two different ways, one way for the predict step and one way for the correct step.
-
-Since the third choice of solution algorithms uses an integration approach, defined as AnalyticalSolution in the ZoneAirHeatBalanceAlgorithm object, it does not require any approximations and has no truncation errors. The solutions in both prediction and correction are provided below in detail.
-
-### Generic Contaminant Prediction
-
-For the generic contaminant concentration prediction case, the equation is solved for the anticipated system response as shown below.
-
-<div>$${\rm{PredictedSystemLoad}} = {\dot m_{sys}}\left( {{C_{f,\sup }} - C_{f,z}^t} \right)$$</div>
-
-Since the program provides three solution algorithms, the generic contaminant prediction from each solution algorithm is given below.
-
-#### EulerMethod
-
-For this solution algorithm, the air mass balance for the predicted air system load or response is:
-
-<div>$$\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = {\rho_{air}}{V_z}{M_{for}}{\left( {\delta t} \right)^{ - 1}}\left( {{C_{{\rm{setpoint}}}} - C_{f,z}^{t - \delta t}} \right)\\\;\;\;\;\;\;\; - \left[ {\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6} - } {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}{C_{{\rm{setpoint}}}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \left( {{C_{f,z,i}} - {C_{{\rm{setpoint}}}}} \right) + {S_f}} \right]\\\;\;\;\;\;\; - \left[ {{{\dot m}_{\inf }}\left( {{C_{f,\infty }} - {C_{{\rm{setpoint}}}}} \right) + \sum\limits_j {{h_j}\rho {A_j}(\frac{{{C_{s,j}}}}{{{k_j}}} - {C_{{\rm{setpoint}}}})} } \right]\;\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\end{array}$$</div>
-
-#### ThirdOrderBackwardDifference
-
-For this solution algorithm, the air mass balance for the predicted system load or response is given below:
-
-<div>$$\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = \frac{{{\rho_{air}}{V_z}{M_{for}}}}{{\delta t}}\left( {\frac{{11}}{6}} \right){C_{{\rm{setpoint}}}} - \left[ {{\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}{C_{{\rm{setpoint}}}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{{\rm{setpoint}}}} + {{\dot m}_{\inf }}{C_{{\rm{setpoint}}}}} \right]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; - \left[ {\sum\limits_j {{h_j}\rho {A_j}{C_{{\rm{setpoint}}}}}  + \sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{f,z,i}} + {{\dot m}_{\inf }}{C_{f,\infty }} + \sum\limits_j {{h_j}\rho {A_j}\frac{{{C_{s,j}}}}{{{k_j}}} + {S_f}} } \right]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; + \frac{{{\rho_{air}}{V_z}{M_{for}}}}{{\delta t}}\left( { - 3C_{f,z}^{t - \delta t} + \frac{3}{2}C_{f,z}^{t - 2\delta t} - \frac{1}{3}C_{f,z}^{t - 3\delta t}} \right)\end{array}$$</div>
-
-#### AnalyticalSolution
-
-For this solution algorithm, the air mass balance for the predicted air system load or response is given below:
-
-<div>$$\begin{array}{l}{\rm{PredictedSystemLoad}}\;[kg/\sec ] = \left[ {\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } } \right]*\\\;\;\;\;\;\;\;\;\;\;\;\left[ {C_{{\rm{setpoint}}}^t - C_z^{t - \delta t}*\exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } }}{{{\rho_{air}}{V_Z}{M_{FOR}}}}\delta t} \right)} \right]*\\\;\;\;\;\;\;\;\;\;\;\;{\left[ {1 - \exp \left( { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } }}{{{\rho_{air}}{V_Z}{M_{FOR}}}}\delta t} \right)} \right]^{ - 1}} - \\\;\;\;\;\;\;\;\;\;\;\;\left( {\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{f,z,i}}\; + {{\dot m}_{\inf }}{C_{f,\infty }} + \sum\limits_j {{h_j}\rho {A_j}} \frac{{{C_{s,j}}}}{{{k_j}}} + {S_f}} \right)\end{array}$$</div>
-
-At the prediction point in the simulation, the system air mass flows are not known; therefore, the system response is approximated. The predicted air system generic contaminant load is then used in the system simulation to achieve the best results possible. If a central HVAC system provides the outdoor flow rate from a Controller:MechanicalVentilation object, the outdoor airflow rate may be approximated as:
-
-<div>$${\rm{PredictedSystemLoad}} = {\dot m_{sys}}\left( {{C_{f,\sup }} - C_{f,z}^t} \right) \approx {\dot m_{OA,z}}\left( {{C_{f,\infty }} - C_{{\rm{setpoint}}}^t} \right)$$</div>
-
-where:
-
-<span>${\dot m_{OA,z}}$</span>= Supply outdoor airflow rate into the controlled zone [kg/s]
-
-The above approximation is based on the assumption that the generic contaminant concentration at the outdoor air (OA) mixer inlet is equal to the zone air outlet concentration level, and the generic contaminant level at the zone supply air inlet is equal to the level at the outlet node of the OA mixer.
-
-After the system simulation is completed, the actual response from the air system is used in the generic contaminant correction step, which is shown next.
-
-### Generic Contaminant Correction
-
-For the correct step, the expanded air mass balance equation is solved for the final zone generic contaminant concentration at the current time step. In the same manner as described above for predicting the carbon dioxide load to be met by the air system, the zone air carbon dioxide correction calculation will be described individually for the three solution algorithms.
-
-#### EulerMethod
-
-<div>$$\begin{array}{l}C_{f,z}^t = \frac{{\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}{C_{f,z,i}}}  + {{\dot m}_{\inf }}{C_{f,\infty }} + {{\dot m}_{sys}}{C_{f,\sup }} + \sum\limits_j {{h_j}\rho {A_j}\frac{{{C_{s,j}}}}{{{k_j}}} + {\rho_{air}}{V_Z}{M_{FOR}}\frac{{C_{f,z}^{t - \delta t}}}{{\delta t}} + {S_f}} }}{{{\rho_{air}}{V_z}{M_{for}}{{\left( {\delta t} \right)}^{ - 1}} + {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}} + \sum\limits_j {{h_j}\rho {A_j}} }}\\\end{array}$$</div>
-
-#### ThirdOrderBackwardDifference
-
-<div>$$\begin{array}{l}C_{f,z}^t = \frac{\begin{array}{l}\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}{C_{f,z,i}}}  + {{\dot m}_{\inf }}{C_{f,\infty }} + {{\dot m}_{sys}}{C_{f,\sup }}\\ + \sum\limits_j {{h_j}\rho {A_j}\frac{{{C_{s,j}}}}{{{k_j}}} + \frac{{{\rho_{air}}{V_Z}{M_{FOR}}}}{{\delta t}}(3C_{f,z}^{t - \delta t} - \frac{3}{2}C_{f,z}^{t - 2\delta t} + \frac{1}{3}C_{f,z}^{t - 3\delta t}) + {S_f}} \end{array}}{{{\rho_{air}}{V_z}{M_{for}}{{\left( {\delta t} \right)}^{ - 1}}\left( {\frac{{11}}{6}} \right) + {\rho_{air}}\sum\limits_i^{N{\rm{sink}}} {{R_{f,i}}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}} + \sum\limits_j {{h_j}\rho {A_j}} }}\\\end{array}$$</div>
-
-#### AnalyticalSolution
-
-<div>$$\begin{array}{l}C_{f,z}^t = \left[ {C_{f,z}^{t - \delta t} - \frac{{\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{f,z,i}}\; + {{\dot m}_{\inf }}{C_{f,\infty }} + {{\dot m}_{sys}}{C_{f,sys}} + \sum\limits_j {{h_j}\rho {A_j}} \frac{{{C_{s,j}}}}{{{k_j}}}}}{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} \; + {{\dot m}_{\inf }} + {{\dot m}_{sys}} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } }}} \right]*\\\;\;\;\;\;\;\;\;\;\exp \left[ { - \frac{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } }}{{{\rho_{air}}{V_Z}{M_{FOR}}}}\delta t} \right] + \\\;\;\;\;\;\;\;\;\frac{{\sum\limits_{i = 1}^{{N_{source}}} {{\rho_{air}}{G_{f,i}}*{{1.0}^6}}  + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_{f,z,i}}\; + {{\dot m}_{\inf }}{C_{f,\infty }} + {{\dot m}_{sys}}{C_{f,sys}} + \sum\limits_j {{h_j}\rho {A_j}} \frac{{{C_{s,j}}}}{{{k_j}}} + {S_f}}}{{\sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}}  + {{\dot m}_{\inf }} + {{\dot m}_{sys}} + {\rho_{air}}\sum\limits_i^{{N_{{\rm{sink}}}}} {{R_{f,i}} + \sum\limits_j {{h_j}\rho {A_j}} } }}\end{array}$$</div>
-
-The above solutions are implemented in the Correct Zone Air Generic Contaminant step in the Zone Contaminant Predictor Corrector module of EnergyPlus.
-
-Zone Air Mass Flow Conservation
--------------------------------
-
-####Overiew
-The zone air mass flow conservation object, ZoneAirMassFlowConservation, activates zone air mass flow balance calculations.  This feature is available only for controlled zones (ZoneVAC:EquipmentConnections) which also have either a zone mixing or infiltration object.  The user may specify that zone mixing, infiltration, or both can be overridden to balance the zone air mass flows. The following rules apply:
-
- - If there are no zone mixing flows to adjacent zones, then the zone air mass flow is balanced by setting the Zone Mixing objects mass flow rate to zero. 
- - If there are no zone exhaust fans defined and there are no zone mixing objects specified, then a zone in an air loop is always balanced.  
- - Infiltration mass flow is included in the zone air mass flow balance depending upon one of three options:  none (all infiltration is assumed to be self-balanced), all zones, or only zones that serve as a source zone for zone mixing objects. 
- - The base infiltration mass flow rate (calculated based on user inputs) may be controlled one of two ways for zone air mass flow balance purposes: adjust the base infiltration up or down as needed to balance the zone air mass flow, or assume the base infiltration rate is self-balanced and add infiltration if needed to balance the zone air mass flow.
- - Optional user inputs can override the default return air flow rate.
-
-The zone air mass flow conservation equation always includes: supply air flow rates, return air flow rates, and zone exhaust fan flow rates. Zone mixing and infiltration object flow rates may be included depending upon the selected options. A particular zone can be a source zone, receiving zone, or both depending on the number of ZoneMixing objects specified for that zone. 
-
-#### Return Air Flow Rate Calculations
-The return air flow rate is calculated one of two ways.  
-
-The default calculation is:
-
-<div>$${\dot m_{R}} = ReturnFlowSchedule*MAX\left( {0.0,\,{{\dot m}_S} + {{\dot m}_{XR}} - {{\dot m}_{EX}} - {{\dot m}_{XS}}} \right)$$</div>
-
-If one or more Zone Return Air Flow Rate Basis Nodes are specified in the ZoneHVAC:EquipmentConnections object, then the base return flow rate is:
-
-<div>$${\dot m_{R}} = ReturnFlowSchedule*\sum\nolimits_j {{{\dot m}_{BasisNode,j}}} $$</div>
-
-
-where,
-
-<span>${\dot m_{R}}$</span>   =    zone return air mass flow rate, (kg/s)
-
-<span>${\dot m_{Basis Node,j}}$</span>   =    zone return air flow basis node mass flow rate, (kg/s)
-
-<span>${\dot m_{EX}}$</span>  =    zone exhaust air mass flow rate from exhaust fans, (kg/s)
-
-<span>${\dot m_{XR}}$</span>  =    zone mixing mass flow rate as a receiving zone, (kg/s)
-
-<span>${\dot m_{XS}}$</span>  =    zone mixing mass flow rate as a source zone, (kg/s)
-
-<span>${\dot m_S}$</span>   =    zone supply air mass flow rate, (kg/s)
-
-ReturnFlowSchedule = optional Zone Return Air Flow Rate Fraction Schedule value
-
-#### Zone Mixing Flow Rate Calculations
-
-Figure 8 illustrates the zone mass flow components for an air loop system providing conditioned air to the two zones connected with a zone mixing object. Since Zone 1 is a source zone only, infiltration object is defined for zone 1 only.  The zone mixing object air flow rate depends on the user specified values and the zone air mass flow balance requirements.  When required the zone mixing object flow rate is adjusted from the user specified value for balancing purpose.
-
-
-
-![](media/image134.svg.png)
-
-
-
-Figure 8. Illustration of zone air mass flow balance components
-
-
-
-An individual zone may be a source zone for multiple receiving zones, and the same source zone may receive mixing flows from multiple adjacent zones in an air loop.  The source and receiving mass flow rates of ZoneMixing objects are calculated from user defined mixing flow rates at the first HVAC iteration for each time step and adjusted in subsequent iterations to balance the zone air mass flow. The source zone mixing mass flow rate is calculated by tracking the mass flow rates of ZoneMixing objects connected to a zone and is given by:
-
-
-
-<div>$${\dot m_{XS}} = \sum\nolimits_j {{{\dot m}_{XS,j}}} $$</div>
-
-
-
-Determine the zone return air mass flow rate as shown above, then adjust the zone mixing mass flow rates based on the current zone return air mass flow rate:
-
-
-
-<div>$${\dot m_{XR,\,new}} = {\dot m_R} + {\dot m_{EX}} + {\dot m_{XS}} - {\dot m_S}$$</div>
-
-
-
-This updated receiving zone mixing air mass flow rate is distributed to the mixing objects connected to the current zone proportional to user specified design flow rate. A single zone may be connected to more than one adjacent zone using multiple ZoneMixing objects.  Thus, the mixing flow rate of each contributing mixing objects defined in the current zone is updated as follows:
-
-
-
-<div>$${\dot m_{XR,\,new,j}} = \left( {{{\dot m}_{XR,jDesign}}/{{\dot m}_{XR,Design}}} \right) \cdot {\dot m_{XR,\,new}}$$</div>
-
-
-####Infiltration Flow Rate Adjustments
-
-There are three options for the treatement of infiltration in the zone air mass balance: None, AddInfiltrationFlow, and AdjustInfiltrationFlow. There are also two options to specify which zones are included in the infiltration adjustments: AllZones or MixingSourceZonesOnly.
-
-If a zone is excluded from infiltration adjustments, then the base infiltration rate specified by the Infiltration:* object(s) in the zone is assumed to be self-balanced, and infiltration is not included in the mass flow calculations for that zone.
-
-If a zone is included in the infiltration adjustment, the infiltration air mass flow rate required to balance the zone is determined as follows:
-
-<div>$${\dot m_{Inf-required}} = MAX\left( {0.0,\,{{\dot m}_{XS}} + {{\dot m}_{EX}} + {{\dot m}_{R}} - {{\dot m}_S}} \right)$$</div>
-
-This infiltration air mass flow rate calculated is either added to the base infiltration air flow, which is calculated from user inputs, or overrides the base infiltration air flow depending on user choice. For AddInfiltrationFlow, the zoneinfiltration flow rate is:
-
-<div>$${\dot m_{Inf}} = {\dot m_{Inf-base}} + {\dot m_{Inf-required}} $$</div>
-
-For AdjustInfiltrationFlow, the zone infiltration flow rate is:
-
-<div>$${\dot m_{Inf}} = {\dot m_{Inf-required}} $$</div>
-
-where,
-
-<span>${\dot m_{Inf}}$</span>   =    zone infiltration  mass flow rate, (kg/s)
-
-<span>${\dot m_{Inf-base}}$</span>   =    base zone infiltration  mass flow rate calculated from Infiltration:\* objects, (kg/s)
-
-<span>${\dot m_{Inf-required}}$</span>   =    required zone infiltration mass flow rate to balance the zone, (kg/s)
-
-There is an additional constraint to the return air mass flow rate calculation.  The sum of the return air mass flow rates of zones in air loop must satisfy the air loop return air mass flow balance.  The above four sets of equations are iterated for each zone in an air loop until the convergence criterion is satisfied or until the maximum iteration limit is exceeded.
-
-The mass conservation calculations are performed in routine CalcZoneMassBalance in the ZoneEquipmentManager module. The latest ZoneMixing and Infiltration object flow rates are communicated back to the zone air heat balance terms. This is done by re-simulating the simple flow objects as zone equipment during each HVAC iteration.  This requires calling the routine CalcAirFlowSimple in SimZoneEquipment routine as zone equipment. Both of these routines are also in the ZoneEquipmentManager module.
-
-
-
-*Zone Mass Conservation Convergence*
-
-The zone mass conservation calculation convergence criterion is based on the absolute difference of the zone mixing objects mass flow rates between successive iteration.  If the difference is above tolerance limits of 0.00001 then the HVAC Air loop is simulated again.
-
-
-
-
-
-Summary of Time Marching Solution
----------------------------------
-
-EnergyPlus models building performance over time spans of days to years using a time marching method based on *timesteps*. This section provides more information on issues related to timestep formulation.
-
-### Summary of Timestep Model Formulation
-
-An EnergyPlus simulation covers a certain period of time, such as a day or a year, that is broken down into a series of discrete bins of time that are referred to as *timesteps*. The program marches through time by recalculating model equations at each timestep. The figure below diagrams some of these basic concepts.
-
-![TimeStepDataDefn](media/image141.png)
-
-Figure 9. Diagram of TimeStep Formulation
-
-Most models in EnergyPlus are quasi-steady energy balance equations used to predict the conditions present during each timestep. Various input data and boundary conditions for the models are time-varying and a “staircase� approach is used where such values are determined for a particular timestep and then essentially held constant over the entire timestep. Predictions for state variables, such as temperature, are averages over the timestep. Predictions for summed variables, such as energy use, are simple totals over the timestep.
-
-EnergyPlus produces time-series results for selected output variables at selected frequencies. The time values associated with the time-series data, or timestamps, are output for the end of the timestep, but the values of the variables are for the entire bin of time prior to the timestamp. When data are reported at coarser frequencies such as hourly, then the results are averages or simple totals for all the timesteps that are contained within the larger bin of time.
-
-To simplify solutions that would otherwise need to be simultaneous, models sometimes use data that are “lagged� which means that the values used in the calculations for the current timestep are actually results from the previous timestep. Many models just use the most current results available and so may use lagged data for a first iteration, but then use current data that are not lagged for subsequent iterations.
-
-### Zone Update Method
-
-A zone is not necessarily a single room but is usually defined as a region of the building or a collection of rooms subject to the same type of thermal control and having similar internal load profiles that, subsequently, can be grouped together. Zones can interact with each other thermally through adjacent surfaces and by intermixing of zone air. In EnergyPlus, the conditions in each zone are updated by Equation , which uses previously calculated values of the zone conditions. This means that EnergyPlus does not have to iterate to find a self-consistent solution of the updated zone conditions. However, because heat transfer through each zone's surfaces and interzone mixing of air still occur, the new space temperatures must be computed at the same simulation time and on the same time step in all zones, even though conditions in one zone may be changing much more rapidly than conditions in the other zones. We have previously documented the method used to update the zone temperature at each time step. This method, called the predictor corrector method, has proved to be satisfactory over a wide range of conditions.
-
-### Variable Timestep
-
-The need for a variable timestep in EnergyPlus was identified during development of its predecessor IBLAST. Prior to the integration of the central plant simulation in IBLAST, a time step Dt for the zone temperature update of 0.25 hours (15 minutes) was found to give stable results without a large increase in computation time. The first step in integrating plant was to implement the detailed coil models and coil control strategies without actually adding the plant models themselves. This meant that the user had to specify the coil water inlet temperature and the maximum coil inlet water flow rate to run the simulation. The real life analogy would be a chiller of very large, though not infinite, capacity. The coil capacity was controlled by adjusting the water flow rate, but the effect of the plant on the chilled water temperature was eliminated. After implementation of this step, experience with the program showed that updating the zone temperatures on a fixed time step frequently resulted in instabilities unless a very short time step was used. However, as the time step got shorter the time required to execute the program got prohibitively high.
-
-Clearly, an adaptive time step was required. This would shorten the time step to maintain stability of the zone air energy balance calculation when zone conditions were changing rapidly and expand it to speed computation when zone conditions were relatively unchanging. But, the adaptive time step could not be applied easily to the surface heat transfer calculations, even using interpolation methods to determine new temperature and flux histories. The problem of updating the zone temperature was resolved by using a two-time-step approach in which the zone air temperature is updated using an adaptive time step that ensures stability. In this two time level scheme, the contributions to the zone loads from the surfaces, and user specified internal loads are updated at the default or user specified time step that is constant. This is often referred to as the “zone� time step. The contributions to the zone loads from HVAC system response, infiltration, and air mixing are updated at a second variable time step, referred to as the “system� time step. The system time step is limited to between one minute and the zone time step. The lower limit of the system time step can be increased to larger than one minute by the user with a System Convergence Limits object (which may be useful to decrease simulation run times at the expense of some accuracy).
-
-The program’s decision to adapt the time step is made by first using the usual zone time step and executing the full predictor-corrector calculations to find resulting zone temperatures. The maximum temperature change experienced by any zone in the model is determined. If this maximum zone temperature change is more than a preset limit of 0.3°C, then the simulation switches to using the shorter system time step. The number of system time steps (within a particular zone time step) is modeled from the results for the maximum zone temperature change (just obtained from the corrector) by assuming that temperature change is linear.  The number of system time steps indicated by the temperatures is:
-
-<div>$$\left( {\frac{{Maximum{\kern 1pt} \;Zone\;Temperature\;Change}}{{Maximum\;Zone\;Temperature\;Difference\;\{ .3C\} }}} \right) + 1.0$$</div>
-
-The limit for the number of system time steps is:
-
-<div>$$\left( {\frac{{Zone\;Time\;Step}}{{Minimum\;System\;Time\;Step}}} \right)$$</div>
-
-EnergyPlus takes the smallest of these two, truncates them to a whole number and calculates a system time step as:
-
-<div>$$System\;Time\;Step = \left( {\frac{{Zone\;Time\;Step}}{{Number\;of\;System\;Time\;Steps}}} \right)$$</div>
-
-The same length of time is used for all the system time steps within a particular zone time step, but the system time step length can vary between different zone time steps. Report variables that use the “detailed� frequency show results at the system time step time scale.
-
-This approach can be justified because the internal loads and surface temperatures vary on a different and longer time scale than the system response and the zone air temperature.
-
-When the simulation down-steps from using the zone time step to the system time step, linear interpolation is used to generate zone condition history terms:
-
-<div>$$
- \begin{array}{l}
-  T_z^{t-\delta t} \\
-  T_z^{t-2\delta t} \\
-  T_z^{t-3\delta t}
- \end{array}
-$$</div>
-
-for the system time steps using the history data for the zone time step. If two consecutive zone time steps both down-step to have the same number of system time steps, then the system time step history is preserved and used directly rather than being interpolated from zone time step history. The zone temperature update is made for each system time step using the same equation as for the zone time step except that the zone temperature history and time difference (delta-t) terms are for the system time step instead of for the zone time step.
-
-### Simultaneous Solution of Plant/System Water Loop
-
-Simultaneous solution of the system and plant operating parameters required that the temperature of the water entering the coils must be the same as the temperature leaving the chillers or boilers. In addition, the temperature of the return water from the coils must be equal to the chiller or boiler entering water temperature. In practice so long as the plant is not out of capacity the leaving water temperature from chillers and boilers is constant and equal to the design value. No iteration was required to match system and plant boundary conditions. However, if either the chiller or boiler plant was overloaded then the temperature of the water leaving the plant was not equal to the design value and the maximum output of the plant could change because of the off-design conditions. An iterative scheme using the secant method to predict successive updates to the plant leaving water conditions was therefore employed to solve for the water loop conditions with the plant operating at its maximum capacity. The simulation of the system and plant loops is described in greater detail in the later sections.
-
-### References
-
-Ceylan, H. T., and G. E. Myers. 1980. Long-time Solutions to Heat Conduction Transients with Time-Dependent Inputs. ASME Journal of Heat Transfer, Volume 102, No. 1, pp. 115-120.
-
-Hittle, D. C. 1979. Calculating Building Heating and Cooling Loads Using the Frequency Response of Multilayered Slabs, Ph.D. Thesis, University of Illinois, Urbana, IL.
-
-Hittle, D. C., and R. Bishop. 1983. An Improved Root-Finding Procedure for Use in Calculating Transient Heat Flow Through Multilayered Slabs. International Journal of Heat and Mass Transfer, Vol. 26, No. 11, pp. 1685-1693.
-
-Ouyang, K., and F. Haghighat. 1991. A Procedure for Calculating Thermal Response Factors of Multi-layered Walls--State Space Method. Building and Environment, Vol. 26, No. 2, pp. 173-177.
-
-Seem, J. E. 1987. Modeling of Heat Transfer in Buildings, Ph.D. Thesis, University of Wisconsin, Madison, WI.
-
-Strand, R. K. 1995. Heat Source Transfer Functions and Their Application to Low Temperature Radiant Heating Systems, Ph.D. Thesis, University of Illinois, Urbana, IL.
-
-Taylor, R. D., C.O. Pedersen, L.K. Lawrie. 1990. *Simultaneous Simulation of Buildings and Mechanical Systems in Heat Balance Based Energy Analysis Programs*, Proceedings of the 3rd International Conference on System Simulation in Buildings, Liege, Belgium, December 3-5, 1990.
-
-Taylor, R.D., C.O. Pedersen, D.E. Fisher, R. J. Liesen, L.K. Lawrie. 1991. Impact of Simultaneous Simulation of Buildings and Mechanical Systems in Heat Balance Based Energy Analysis Programs on System Response and Control, Conference Proceedings IBPSA Building Simulation '91, Nice, France, August 20-22, 1991.
-
-
-
diff --git a/doc/src/docs/EngineeringReference/03-SurfaceHeatBalance.md b/doc/src/docs/EngineeringReference/03-SurfaceHeatBalance.md
deleted file mode 100644
index 55476d3e9f6..00000000000
--- a/doc/src/docs/EngineeringReference/03-SurfaceHeatBalance.md
+++ /dev/null
@@ -1,4181 +0,0 @@
-Surface Heat Balance Manager / Processes
-========================================
-
-Conduction Through The Walls
-----------------------------
-
-### Conduction Transfer Function Module
-
-The most basic time series solution is the response factor equation which relates the flux at one surface of an element to an infinite series of temperature histories at both sides as shown by Equation :
-
-<div>$${q''_{ko}}(t) = \sum\limits_{j = 0}^\infty  {{X_j}} {T_{o,t - j\delta }} - \sum\limits_{j = 0}^\infty  {{Y_j}} {T_{i,t - j\delta }}$$</div>
-
-where q� is heat flux, T is temperature, i signifies the inside of the building element, o signifies the outside of the building element, t represents the current time step, and X and Y are the response factors.
-
-While in most cases the terms in the series decay fairly rapidly, the infinite number of terms needed for an exact response factor solution makes it less than desirable.  Fortunately, the similarity of higher order terms can be used to replace them with flux history terms.  The new solution contains elements that are called conduction transfer functions (CTFs).  The basic form of a conduction transfer function solution is shown by the following equation:
-
-<div>$${q''_{ki}}(t) =  - {Z_o}{T_{i,t}} - \sum\limits_{j = 1}^{nz} {{Z_j}} {T_{i,t - j\delta }} + {Y_o}{T_{o,t}} + \sum\limits_{j = 1}^{nz} {{Y_j}} {T_{o,t - j\delta }} + \sum\limits_{j = 1}^{nq} {{\Phi_j}{{q''}_{ki,t - j\delta }}} $$</div>
-
-for the inside heat flux, and
-
-<div>$${q''_{ko}}(t) =  - {Y_o}{T_{i,t}} - \sum\limits_{j = 1}^{nz} {{Y_j}} {T_{i,t - j\delta }} + {X_o}{T_{o,t}} + \sum\limits_{j = 1}^{nz} {{X_j}} {T_{o,t - j\delta }} + \sum\limits_{j = 1}^{nq} {{\Phi_j}{{q''}_{ko,t - j\delta }}} $$</div>
-
-for the outside heat flux (q²=q/A)
-
-where:
-
-X*<sub>j</sub>*  = Outside CTF coefficient, j= 0,1,...nz.
-
-Y*<sub>j</sub>* = Cross CTF coefficient, j= 0,1,...nz.
-
-Z*<sub>j</sub>* = Inside CTF coefficient, j= 0,1,...nz.
-
-F*<sub>j</sub>* = Flux CTF coefficient, j = 1,2,...nq.
-
-T*<sub>i</sub>* = Inside face temperature
-
-T*<sub>o</sub>* = Outside face temperature
-
-<span>\({q''_{ko}}\)</span> = Conduction heat flux on outside face
-
-<span>\(q''\)</span> = Conduction heat flux on inside face
-
-The subscript following the comma indicates the time period for the quantity in terms of the time step d.  Note that the first terms in the series (those with subscript 0) have been separated from the rest in order to facilitate solving for the current temperature in the solution scheme.  These equations state that the heat flux at either face of the surface of any generic building element is linearly related to the current and some of the previous temperatures at both the interior and exterior surface as well as some of the previous flux values at the interior surface.
-
-The final CTF solution form reveals why it is so elegant and powerful.  With a single, relatively simple, linear equation with constant coefficients, the conduction heat transfer through an element can be calculated.  The coefficients (CTFs) in the equation are constants that only need to be determined once for each construction type.  The only storage of data required are the CTFs themselves and a limited number of temperature and flux terms.  The formulation is valid for any surface type and does not require the calculation or storage of element interior temperatures.
-
-### Calculation of Conduction Transfer Functions
-
-The basic method used in EnergyPlus for CTF calculations is known as the state space method (Ceylan and Myers 1980; Seem 1987; Ouyang and Haghighat 1991).  Another common, older method used Laplace transformations to reach the solution;  the Laplace method was  used in BLAST (Hittle, 1979; Hittle & Bishop, 1983).  The basic state space system is defined by the following linear matrix equations:
-
-<div>$$\frac{{d\left[ {\bf{x}} \right]}}{{dt}} = \left[ {\bf{A}} \right]\left[ {\bf{x}} \right] + \left[ {\bf{B}} \right]\left[ {\bf{u}} \right]$$</div>
-
-<div>$$\left[ {\bf{y}} \right] = \left[ {\bf{C}} \right]\left[ {\bf{x}} \right] + \left[ {\bf{D}} \right]\left[ {\bf{u}} \right]$$</div>
-
-where x is a vector of state variables, u is a vector of inputs, y is the output vector, t is time, and A, B, C, and D are coefficient matrices.  Through the use of matrix algebra, the vector of state variables (x) can be eliminated from the system of equations, and the output vector (y) can be related directly to the input vector (u) and time histories of the input and output vectors.
-
-This formulation can be used to solve the transient heat conduction equation by enforcing a finite difference grid over the various layers in the building element being analyzed.  In this case, the state variables are the nodal temperatures, the environmental temperatures (interior and exterior) are the inputs, and the resulting heat fluxes at both surfaces are the outputs.  Thus, the state space representation with finite difference variables would take the following form:
-
-<div>$$
-  \frac{d\left[\begin{array}{c}T_1 \\ \vdots \\ T_n\end{array}\right]}{dt} = \left[\bf{A}\right]\left[\begin{array}{c}T_1 \\ \vdots \\ T_n\end{array}\right]+\left[\bf{B}\right]\left[\begin{array}{c}T_i \\ T_o\end{array}\right]
-$$</div>
-
-<div>$$
-  \left[\begin{array}{c}{q''}_i \\ {q''}_o\end{array}\right] = \left[\bf{C}\right]\left[\begin{array}{c}T_1 \\ \vdots \\ T_n\end{array}\right]+\left[\bf{D}\right]\left[\begin{array}{c}T_i \\ T_o\end{array}\right]
-$$</div>
-
-where T1, T2, ..., Tn-1, Tn are the finite difference nodal temperatures, n is the number of nodes, Ti and To are the interior and exterior environmental temperatures, and q"i and q"o are the heat fluxes (desired output).
-
-Seem (1987) shows that for a simple one layer slab with two interior nodes as in Figure 7 and convection at both sides the resulting finite difference equations are given by:
-
-<div>$$C\frac{{d{T_1}}}{{dt}} = hA\left( {{T_o} - {T_1}} \right) + \frac{{{T_2} - {T_1}}}{R}$$</div>
-
-<div>$$C\frac{{d{T_2}}}{{dt}} = hA\left( {{T_i} - {T_2}} \right) + \frac{{{T_1} - {T_2}}}{R}$$</div>
-
-<div>$$q{``_i} = h\left( {{T_i} - {T_2}} \right)$$</div>
-
-<div>$$q{``_o} = h\left( {{T_1} - {T_o}} \right)$$</div>
-
-where:
-
-<span>\(R = \frac{\ell }{{kA}}\)</span>,
-
-<span>\(C = \frac{{\rho {c_p}\ell A}}{2}\)</span>, and
-
-A is the area of the surface exposed to the environmental temperatures.
-
-In matrix format:
-
-<div>$$
-  \left[\begin{array}{c}\frac{dT_1}{dt} \\ \frac{dT_2}{dt}\end{array}\right] = 
-     \left[\begin{array}{cc}-\frac{1}{RC}-\frac{hA}{C} & \frac{1}{RC} \\ \frac{1}{RC} & -\frac{1}{RC}-\frac{hA}{C}\end{array}\right]\left[\begin{array}{c}T_1 \\ T_2\end{array}\right] + 
-     \left[\begin{array}{cc}\frac{hA}{C} & 0 \\ 0 & \frac{hA}{C}\end{array}\right]\left[\begin{array}{c}T_o \\ T_i\end{array}\right]
-$$</div>
-
-<div>$$
-  \left[\begin{array}{c}{q''}_o \\ {q''}_i\end{array}\right] = 
-    \left[\begin{array}{cc}0 & -h \\ h & 0\end{array}\right] \left[\begin{array}{c}T_1 \\ T_2\end{array}\right] +
-    \left[\begin{array}{cc}0 & h \\ -h & 0\end{array}\right] \left[\begin{array}{c}T_o \\ T_i\end{array}\right]
-$$</div>
-
-![](media/image168.svg.png)
-
-Figure 10.  Two Node State Space Example.
-
-The important aspect of the state space technique is that through the use of matrix algebra the state space variables (nodal temperatures) can be eliminated to arrive at a matrix equation that gives the outputs (heat fluxes) as a function of the inputs (environmental temperatures) only.  This eliminates the need to solve for roots in the Laplace domain.  In addition, the resulting matrix form has more physical meaning than complex functions required by the Laplace transform method.
-
-The accuracy of the state space method of calculating CTFs has been addressed in the literature.  Ceylan and Myers (1980) compared the response predicted by the state space method to various other solution techniques including an analytical solution.  Their results showed that for an adequate number of nodes the state space method computed a heat flux at the surface of a simple one layer slab within 1% of the analytical solution.  Ouyang and Haghighat (1991) made a direct comparison between the Laplace and state space methods.  For a wall composed of insulation between two layers of concrete, they found almost no difference in the response factors calculated by each method.
-
-Seem (1987) summarizes the steps required to obtain the CTF coefficients from the A, B, C, and D matrices.  While more time consuming than calculating CTFs using the Laplace Transform method, the matrix algebra (including the calculation of an inverse and exponential matrix for A) is easier to follow than root find algorithms.  Another difference between the Laplace and State Space methods is the number of coefficients required for a solution.  In general, the State Space method requires more coefficients.  In addition, the number of temperature and flux history terms is identical (nz=nq).  Note that as with the Laplace method that the actual number of terms will vary from construction to construction.
-
-Two distinct advantages of the State Space method over the Laplace method that are of interest when applying a CTF solution for conduction through a building element are the ability to obtain CTFs for much shorter time steps and the ability to obtain 2- and 3-D conduction transfer functions.  While not implemented in the Toolkit, both Seem (1987) and Strand (1995) have demonstrated the effectiveness of the State Space method in handling these situations that can have important applications in buildings.
-
-### Conduction Transfer Function (CTF) Calculations in EnergyPlus
-
-Conduction transfer functions are an efficient method to compute surface heat fluxes because they eliminate the need to know temperatures and fluxes within the surface.  However, conduction transfer function series become progressively more unstable as the time step decreases.  This became a problem as investigations into short time step computational methods for the zone/system interactions progressed because, eventually, this instability caused the entire simulation to diverge.  This phenomenon was most apparent for thermally massive constructions with long characteristic times and, correspondingly, requiring a large number of terms in the CTF series. This indicates that the problem is related to round-off and truncation error and is in no way an indictment of the CTF method itself.  Methods that develop CTF series from finite difference approximations to the heat conduction equation (Meyers, 1980; Seem, 1987) were considered to address this problem.  Seem's method did give better accuracy and stability at short time steps than the current BLAST technique but, the method still had difficulty computing stable CTF series for time steps of less than 1/4 hour for the heaviest constructions in the BLAST library.
-
-The zone heat gains consist of specified internal heat gains, air exchange between zones, air exchange with the outside environment, and convective heat transfer from the zone surfaces.  Of these, the surface convection load requires the most complicated calculations because a detailed energy balance is required at the inside and outside surface of each wall, floor, and roof.  In addition, the transient heat conduction in the material between the surfaces must be solved.  This solution gives the inside and outside temperatures and heat fluxes that must be known in order to calculate the convection component to the zone load for each zone surface.  BLAST uses a conduction transfer function CTF method attributed to Hittle (1980) to solve the transient conduction problem for each surface.  The method results in a time series of weighting factors that, when multiplied by previous values of the surface temperatures and fluxes and the current inside and outside surface temperatures, gives the current inside and outside heat flux.  The method is easily applied to multilayered constructions for which analytical solutions are unavailable.  In addition, determining the series of CTF coefficients is a one-time calculation, making the method much faster than finite difference calculations.
-
-A problem with CTF methods is that the series time step is fixed; that is, a CTF series computed for a one hour time step takes information at t-1 hours, t-2 hours, etc. and computes conditions at the current time t.  As time advances the oldest term in the input series is dropped and the data moved back one time step to allow the newest value to be added to the series.  For convenience, the time step used to determine the CTF series should be the same as the time step used to update the zone mean air temperature in the zone energy balance.  But, as the time step used to calculate the CTF series gets shorter, the number of terms in the series grows.  Eventually, with enough terms, the series becomes unstable due to truncation and round-off error.  Heavy constructions, such as slab-on-grade floors (12" heavyweight concrete over 18" dirt), have accuracy and stability problems at time steps as large as 0.5 hours when modeled by Hittle's CTF method.  In an attempt to overcome this problem, Hittle's method was replaced by Seem's method (1987) in IBLAST.  This resulted in some improvement in stability at shorter time steps, but not enough to allow IBLAST to run at a 0.1 hour time step without restricting the types of surfaces that could be used.
-
-Even though CTF methods require that values of the surface temperatures and fluxes be stored for only a few specific times before the current time, the temperature and flux histories are, actually, continuous functions between those discrete points.  However, there is no way to calculate information at these intermediate times once a series has been initialized.  The terms in the temperature and flux histories are out of phase with these points.  However, they can be calculated by shifting the phase of the temperature and flux histories by only a fraction of a time step.  This procedure would allow a CTF series computed for a time step Dt, to be used to compute information at times t+Dt/2, t+Dt/3, t+Dt/4, or any other arbitrary fraction of the time step, so long as the surface temperatures and flux values were still Dt apart.  Several ways of doing this are described below.
-
-The method shown in the Figure 11 maintains two sets of histories out of phase with each other.  The figure shows how this would work for two sets of histories out of phase by one half of a time step.  More sets of temperature and flux histories could be used, allowing the simulation time step to take on values: 1/3, 1/4, 1/5, etc., of the minimum time step allowed for the CTF calculations.  The time step between inputs to the CTF series would be the smallest convenient interval at which the CTF series is stable.  This scenario is illustrated in this figure for two separate sets of temperature and flux histories.  Cycling through each history, in order, allowed calculations of the zone energy balance to be performed with updated surface information at a shorter time step than one CTF history series would otherwise allow.  This method required no interpolation between the series once each set of histories was initialized.  However, if the smallest time step for a stable CTF series was large compared to the zone temperature update time step, significant memory was required to store all the sets of histories.
-
-![](media/image169.svg.png)
-
-Figure 11. Multiple, staggered time history scheme
-
-Another method is shown in Figure 12. Sequential interpolation of new histories that uses successive interpolations to determine the next set of temperature and flux histories.  The current history is interpolated directly from the previous history set using the required time phase shift between the two.  This method required permanent storage for only one set of temperature and flux histories at a time, but smoothed out temperature and flux data as more interpolations were performed.  As a result, at concurrent simulation times current values of history terms were different form previous "in phase" history terms.  This was unacceptable from, a physical point of view, because it allowed current information to change data from a previous time.
-
-![](media/image170.svg.png)
-
-Figure 12. Sequential interpolation of new histories
-
-A final method, shown in Figure 13. Master history with interpolation, was something of a hybrid of the previous two methods.  One "master" history set was maintained and updated for all time; this solved the problem of current events propagating information backwards in time.  When surface fluxes needed to be calculated at times out of phase with this master history a new, temporary history was interpolated from the master values.  This method proved to be the best of the three options described because it eliminated propagation of information backwards in time and only required concurrent storage of two sets of temperature and flux histories. This method was subsequently incorporated into the IBLAST program in conjunction with Seem's procedure for calculating the coefficients of the CTF series.
-
-![](media/image171.svg.png)
-
-Figure 13. Master history with interpolation
-
-### Conduction Transfer Function (CTF) Calculations Special Case: R-Value Only Layers
-
-Most users will elect to enter materials with four parameters that are of interest for calculating conduction transfer functions: thickness, conductivity, density, and specific heat.  For these materials, EnergyPlus will divide each material layer within a construction into between 6 and 18 nodes for the application of the state-space method.  For multi-layered constructions, nodes are also placed at the interface between two layers.  These interface nodes consist of half a node of the first layer and half a node of the second layer.
-
-In some cases, either due to a lack of information or a desire to simplify input, a user may choose to enter a material layer as a “no mass� or “R-Value only� material.  This assumption essentially says that these layers add nothing to the thermal mass of the overall construction and only add to the overall resistance or R-Value of the construction as a whole.  While this is not recommended, it is allowed and in some cases is not a poor assumption for extremely lightweight materials such as some types of insulation.
-
-In the past, when a user enters such a “no mass� material into EnergyPlus, internally the properties of this layer are converted to approximate the properties of air (density, specific heat, and conductivity) with the thickness adjusted to maintain the user’s desired R-Value.  This allowed such layers to be handled internally in the same way as other layers without any additional changes to the code.  This solution was deemed accurate enough as air has very little thermal mass and it made the coding of the state space method simpler.
-
-It is possible to account for layers that have no thermal mass in the state space solution without resorting to the assignment of fictitious material properties.  The EnergyPlus internal equations for assigning values to portions of the A, B, C, and D matrices as shown in the previous subsections have been altered to account for the potential presence of R-Value only (or no mass) layers without resorting to assigning these materials the properties of air.  This is handled by assuming that the “no mass� layer is a single node layer.  As nodes are defined that the interface between material layers, the “no mass� layer is essentially two “half nodes� that are shared with the surrounding layers.  This allows the surrounding material layers to provide thermal capacitance for each of the nodes at the material interfaces.
-
-In EnergyPlus, there are two possible cases for the existence of “no mass� layers: either between two other solid, thermally massive layers (multiple “no mass� layers next to each other are simply combined in this approach) or at the inner or outer most layers of a construction.  There are potential issues with having a resistance-only layer at either the inner or outer most layers of a construction.  A little or no mass layer there could receive intense thermal radiation from internal sources or the sun causing the temperature at the inner or outer surface to achieve very high levels.  This is undesirable from a simulation standpoint as there are limits to temperature levels in EnergyPlus that could be exceeded causing the simulation to terminate and is likely unrealistic from a real-world perspective.  Thus, for such potentially problematic calculational scenarios, EnergyPlus will continue to convert a “no mass� layer at either the inner or outer most layer of a construction into a thermal mass layer using the properties of air as has been done in the past.
-
-The case where a resistance-only layer is defined anywhere except the inner or outer layer of a construction is handled by treating the “no mass� layer as a single node layer.  This will result in a node at each interface as in the standard material layer cases.  When a “no mass� material is present, the R-Value only layer will not add any thermal capacitance to the nodes at the interfaces at either side of the material.  It will simply add resistance between the two nodes.
-
-![](media/image172.png)
-
-Figure 14. Illustration of no-mass layer between two mass layers
-
-From the EnergyPlus code, the A matrix (AMat) is assigned with values at the interface using the following equations (taken from the actual code):
-
-````
-cap = ( rho(Layer)\*cp(Layer)\*dx(Layer) + rho(Layer+1)\*cp(Layer+1)\*dx(Layer+1) ) \* 0.5D0
-AMat(Node,Node-1) = rk(Layer)/dx(Layer)/cap           ! Assign matrix values for the current node
-AMat(Node,Node)   = -1.0D0 \* ( rk(Layer)/dx(Layer)+rk(Layer+1)/dx(Layer+1) ) / cap
-AMat(Node,Node+1) = rk(Layer+1)/dx(Layer+1)/cap       ! node.
-````
-
-Note that these equations do not change.  For “no mass� layers, the density (rho) and the specific heat (cp) variables will be assigned zero values.  In addition, the thickness (dx) will be equated with the user-defined R-Value and conductivity (rk) will be assigned a value of unity.  In addition, the number of nodes for the “no mass� layer will be set to 1.
-
-This handles resistive layers correctly without resorting to assigning the properties of air to the “no mass� layer.  The only potential problem with this is if two resistive layers are placed next to each other.  In that case, the interface between the two resistive layers would have no mass (variable “cap� would equal zero) and a divide by zero would result.  To avoid this, adjacent “no mass� layers are combined internally so that the user does not have to do this and also to avoid any divide by zero errors.
-
-While from a results standpoint, the difference in output between assigning air properties for specific heat, density, etc. and handling the no mass materials explicitly is negligible, handling the no mass layers properly does provide better code efficiency from a calculation speed standpoint.
-
-### References
-
-Ceylan, H. T., and G. E. Myers. 1980. Long-time Solutions to Heat Conduction Transients with Time-Dependent Inputs. ASME Journal of Heat Transfer, Volume 102, No. 1, pp. 115-120.
-
-Hittle, D. C. 1979. Calculating Building Heating and Cooling Loads Using the Frequency Response of Multilayered Slabs, Ph.D. Thesis, University of Illinois, Urbana, IL.
-
-Hittle, D. C., and R. Bishop. 1983. An Improved Root-Finding Procedure for Use in Calculating Transient Heat Flow Through Multilayered Slabs. International Journal of Heat and Mass Transfer, Vol. 26, No. 11, pp. 1685-1693.
-
-Ouyang, K., and F. Haghighat. 1991. A Procedure for Calculating Thermal Response Factors of Multi-layered Walls--State Space Method. Building and Environment, Vol. 26, No. 2, pp. 173-177.
-
-Seem, J. E. 1987. Modeling of Heat Transfer in Buildings, Ph.D. Thesis, University of Wisconsin, Madison, WI.
-
-Strand, R. K. 1995. Heat Source Transfer Functions and Their Application to Low Temperature Radiant Heating Systems, Ph.D. Thesis, University of Illinois, Urbana, IL.
-
-Taylor, R. D., C.O. Pedersen, D.E. Fisher, R. J. Liesen, L.K. Lawrie. 1990. *Simultaneous Simulation of Buildings and Mechanical Systems in Heat Balance Based Energy Analysis Programs*, Proceedings of the 3rd International Conference on System Simulation in Buildings, Liege, Belgium, December 3-5, 1990.
-
-Taylor, R.D., C.O. Pedersen, D.E. Fisher, R. J. Liesen, L.K. Lawrie. 1991. Impact of Simultaneous Simulation of Buildings and Mechanical Systems in Heat Balance Based Energy Analysis Programs on System Response and Control, Conference Proceedings IBPSA Building Simulation '91, Nice, France, August 20-22, 1991.
-
-Conduction Finite Difference Solution Algorithm
------------------------------------------------
-
-### Basic Finite Difference Solution Approach
-
-EnergyPlus models follow fundamental heat balance principles very closely in almost all aspects of the program. However, the simulation of building surface constructions has relied on a conduction transfer function (CTF) transformation carried over from BLAST. This has all the usual restrictions of a transformation-based solution: constant properties, fixed values of some parameters, and do not produce results for the interior of the surface. As the energy analysis field moves toward simulating more advanced constructions, such as phase change materials (PCM), it becomes necessary to step back from transformations to more fundamental forms. Accordingly, a conduction finite difference (CondFD) solution algorithm has been incorporated into EnergyPlus. This does not replace the CTF solution algorithm, but complements it for cases where the user needs to simulate phase change materials or variable thermal conductivity. It is also possible to use the finite difference algorithm for zone time steps as short as one minute.
-
-EnergyPlus includes two different options for the specific scheme or formulation used for the finite difference model.  The first scheme is referred to as Crank-Nicholson and was the formulation used in EnergyPlus prior to version 7.  As of version 7 a second scheme was added and is referred to as fully implicit.  The selection between the two can be made by the user with the HeatBalanceSettings:ConductionFiniteDifference input object.  Once selected, the same scheme is used throughout the simulation.  Although the two different schemes differ in their fundamental heat transfer equations, they share nearly all the same supporting models for material properties, data storage, solution schemes, and spatial discretization algorithms.
-
-The Crank-Nicholson scheme is semi-implicit and based on an Adams-Moulton solution approach. It is considered second-order in time.  The algorithm uses an implicit finite difference scheme coupled with an enthalpy-temperature function to account for phase change energy accurately. The implicit formulation for an internal node is shown in the equation below.
-
-<div>$$
-  C_p \rho \Delta x \frac{T_i^{j+1}-T_i^j}{\Delta t} = 
-     \frac{1}{2}\left(k_W\frac{T_{i+1}^{j+1}-T_{i}^{j+1}}{\Delta x} +
-                      k_E\frac{T_{i-1}^{j+1}-T_{i}^{j+1}}{\Delta x} + 
-                      k_W\frac{T_{i+1}^{j}-T_{i}^{j}}{\Delta x} +
-                      k_E\frac{T_{i-1}^{j}-T_{i}^{j}}{\Delta x}\right)
-$$</div>
-
-Where:
-
-T <sub>=</sub> node temperature
-
-Subscripts:
-
-i = node being modeled
-
-i+1 = adjacent node to interior of construction
-
-i-1 = adjacent node to exterior of construction
-
-j+1 = new time step
-
-j = previous time step
-
-Dt = calculation time step
-
-Dx = finite difference layer thickness (always less than construction layer thickness)
-
-C<sub>p</sub> = specific heat of material
-
-k<sub>w</sub> = thermal conductivity for interface between i node and i+1 node
-
-k<sub>E</sub> = thermal conductivity for interface between i node and i-1 node
-
-r  = density of material
-
-Then, this equation is accompanied by a second equation that relates enthalpy and temperature.
-
-<div>$${h_i} = HTF\left( {{T_i}} \right)$$</div>
-
-where HTF is an enthalpy-temperature function that uses user input data.
-
-The fully implicit scheme is also based on an Adams-Moulton solution approach. It is considered first order in time.  The model equation for this scheme is show in the following equation.
-
-<div>$${C_p}\rho {\rm{\Delta x}}\frac{{T_i^{j + 1} - T_i^j}}{{{\rm{\Delta }}t}} = \left( {{k_W}\frac{{\left( {T_{i + 1}^{j + 1} - T_i^{j + 1}} \right)}}{{{\rm{\Delta x}}}} + {k_E}\frac{{\left( {T_{i - 1}^{j + 1} - T_i^{j + 1}} \right)}}{{{\rm{\Delta x}}}}} \right)$$</div>
-
-For both schemes, EnergyPlus uses the following four types of nodes, as shown in the figure below (1) interior surface nodes, (2) interior nodes, (3) material interface nodes and (4) external surface nodes. The grid for each material is established by specifying a half node for each edge of a material and equal size nodes for the rest of the material. Equations such as are formed for all nodes in a construction. The formulation of all node types is basically the same.
-
-![Description: C:\Griffith\AnalysisTools\CondFDpaper\Figures\Figures\Figure2.tif](media/image176.png)
-
-Figure 15. Node depiction for Conduction Finite Difference Model
-
-In the CondFD model, surface discretization depends on the thermal diffusivity of the material (α) and time step (Δt) selected, as shown in the equation below. The default value of 3 for the space discretization constant, *C*, is basically the inverse of the Fourier Number:
-
-<div>$$
-Fo = \frac{\alpha \Delta t}{\Delta x^2}
-$$</div>
-
-and is based on the stability requirement for the explicit mode that requires values higher than 2, or a Fourier number lower than 0.5. However, CondFD uses implicit schemes that do not have the same stability requirements as the explicit mode. Thus, the default 3 was originally set rather arbitrary.  As of version 7, the value of this constant can be controlled by the user with the input field called Space Discretization Constant in the HeatBalanceSettings:ConductionFiniteDifference input object.   The discretization method allows CondFD to assign different node spacing or grid size to different material layers in a wall or roof, as building walls and roofs typically consist of several layers of different materials having different thermal properties.
-
-<div>$${\rm{\Delta x}} = \sqrt {{\rm{C\alpha \Delta t}}} $$</div>
-
-The actual integer number of nodes for each layer is then calculated by rounding off the result from dividing the length of the material layer by the result of the equation above. After this, Δx is recalculated by dividing the length of the material by the number of nodes. A full node is equal to two half nodes. Lower values for the Space Discretization Constant yield more nodes, with higher values yield fewer nodes.
-
-Because the solution is implicit, a Gauss-Seidell iteration scheme is used to update to the new node temperatures in the construction and under-relaxation is used for increased stability.  The Gauss-Seidell iteration loop is the inner-most solver and is called for each surface.  It is limited to 30 iterations but will exit early when the sum of all the node temperatures changes between the last call and the current call, normalized by the sum of the temperature values, is below  0.000001C. This convergence criteria is typically met after 3 iterations, except when PCMs are simulated as it takes an average of 2-3 more iterations when PCM are changing phase. If the number if iterations needed to met convergence criteria start to increase, an automatic internal relaxation factor stabilities the solution and in most cases keep the number of iterations less than 10.
-
-EnergyPlus also uses a separate, outer iteration loop across all the different inside surface heat balances so that internal long-wave radiation exchange can be properly solved.  For CTF formulations, this iteration is controlled by a maximum allowable temperature difference of 0.002C for inside face surface temperatures from one iteration to the next (or a limit of 100 iterations). CondFD uses the same default value for allowable temperature difference as CTF. However, this parameter was found to often need to be smaller for stability and so the inside surface heat balance manager uses a separate allowable maximum temperature difference when modeling CondFD.  The user can control the value of the relaxation factor by using the input field called  Inside Face Surface Temperature Convergence Criteria in the HeatBalanceSettings:ConductionFiniteDifference input object. In addition, if the program detects that there is instability by watching for excessive numbers of iterations in this outer loop and may decrease the relaxation factor. Users can also output the number of iterations inside of CondFD loop for each surface and the outer internal heat balance loop for each zone with “CondFD Inner Solver Loop Iterations� and “Heat Balance Inside Surfaces Calculation Iterations� respectively.
-
-<div>$${T_{i,new}} = {T_{i,old}} + \left( {{T_{i,new}} - {T_{i,old}}} \right)*Relax$$</div>
-
-Because of the iteration scheme used for CondFD,  the node enthalpies get updated each iteration, and then they are used to develop a variable Cp if a phase change material is being simulated. This is done by including a third equation for Cp.
-
-<div>$$Cp = \frac{{{h_{i,new}} - {h_{i,old}}}}{{{T_{i,new}} - {T_{i,old}}}}$$</div>
-
-The iteration scheme assures that the correct enthalpy, and therefore the correct Cp is used in each time step, and the enthalpy of the material is accounted for accurately. Of course, if the material is regular, the user input constant Cp is used.
-
-The algorithm also has a provision for including a temperature coefficient to modify the thermal conductivity. The thermal conductivity is obtained from:
-
-<div>$$k = {k_o} + {k_1}\left( {{T_i} - 20} \right)$$</div>
-
-where:
-
-k<sub>o</sub> is the 20°C value of thermal conductivity (normal idf  input)
-
-k<sub>1</sub> is the change in conductivity per degree temperature difference from 20°C
-
-As of Version 7, the CondFD implementation was changed to evaluate the thermal conductivity at the interface between nodes, as shown below. In this case, EnergyPlus uses a linear interpolation between nodal points.
-
-<div>$${C_p}\rho {\rm{\Delta x}}\frac{{T_i^{j + 1} - T_i^j}}{{{\rm{\Delta }}t}} = \frac{1}{2}\left[ {\left( {{k_W}\frac{{\left( {T_{i + 1}^{j + 1} - T_i^{j + 1}} \right)}}{{{\rm{\Delta x}}}} + {k_E}\frac{{\left( {T_{i - 1}^{j + 1} - T_i^{j + 1}} \right)}}{{{\rm{\Delta x}}}}} \right) + \left( {{k_W}\frac{{\left( {T_{i + 1}^j - T_i^j} \right)}}{{{\rm{\Delta x}}}} + {k_E}\frac{{\left( {T_{i - 1}^j - T_i^j} \right)}}{{{\rm{\Delta x}}}}} \right)} \right]$$</div>
-
-Where,
-
-<div>$${k_W} = \frac{{\left( {k_{i + 1}^{j + 1} + k_i^{j + 1}} \right)}}{2}$$</div>
-
-<div>$${{\rm{k}}_{\rm{E}}} = \frac{{\left( {{\rm{k}}_{{\rm{i}} - 1}^{{\rm{j}} + 1} + {\rm{k}}_{\rm{i}}^{{\rm{j}} + 1}} \right)}}{2}$$</div>
-
-These additional property information values are put into the input file as explained in the Input/Output Reference Document, but it consists simply of a value for k1 and set of enthalpy temperature pairs that describe the enthalpy of the phase change material in straight line segments with respect to temperature.
-
-A graph showing the effect of a large PCM on the outside surface of a zone is shown below. The phase change temperature was 30°C, and the flat temperature response during the phase change is obvious. This example was run with a zone time step of one minute to show that such small time steps can be done with the finite difference solution technique. It is more efficient to set the zone time step shorter than those used for the CTF solution algorithm. It should be set to 20 time steps per hour or greater, and can range up to 60. The finite difference algorithm actually works better with shorter zone time steps. The computation time has a minimum at a zone time step around two minutes (30 time steps/hr), and increases for shorter or longer zone time steps.
-
-![Description: Phase Change Graph OutsidePCM](media/image185.png)
-
-Figure 16. Effects of Large PCM on Outside Zone Surface
-
-### Finite Difference Node Arrangement in Surfaces
-
-The Conduction Finite Difference algorithm determines the number of nodes in each layer of the surface based on the Fourier stability criteria.  The node thicknesses are normally selected so that the time step is near the explicit solution limit in spite of the fact that the solution is implicit. For very thin, high conductivity layers, a minimum of two nodes is used.  This means two half thickness nodes with the node temperatures representing the inner and outer faces of the layer. All thicker layers also have two half thickness nodes at their inner and outer faces. These nodes produce layer interface temperatures.
-
-The ConductionFiniteDifferenceSimplified capability was removed as of Version 7.2.
-
-### Conduction Finite Difference Variable Thermal Conductivity
-
-The Conduction Finite Difference algorithm has also been given the capability to use an expanded thermal conductivity function. This function, explained in the input/output document, is similar to the temperature enthalpy function. It consists of pairs of temperature and thermal conductivity values that form a linear segmented function. It is established with the MaterialProperty:VariableThermalConductivity object.
-
-### Conduction Finite Difference Source Sink Layers
-
-The Conduction Finite Difference algorithm can also invoke the source/sink layer capability by using the **Construction:InternalSource** object.
-
-### Conduction Finite Difference Heat Flux Outputs
-
-The Conduction Finite Difference algorithm can output the heat flux at each node and the heat capacitance of each half-node.  During the CondFD solution iterations, the heat capacitance of each half node (CondFD Surface Heat Capacitance Node < n  >) is stored:
-
-<div>$${HeatCap_{i} = Cp_{i}*\Delta x_{i}*\rho_{i}/2}$$</div>
-
-For nodes which are at the inside or outside face of the surface, there is only one half-node.
-
-After the CondFD node temperatures have been solved for a given timestep, the heat fluxes (CondFD Surface Heat Flux Node < i > ) are calculated beginning with the inside face of the surface.
-
-<div>$${QDreport_{N} = Q_{inside}}$$</div>
- 
-for the remaining nodes
-
-<div>$${QDreport_{i} = QDreport_{i+1}+HeatCap1_{i+1}* \frac{\left(T_{i+1,new}-T_{i+1,old}\right)}{\Delta t}-QSource_{i}+HeatCap2_{i}* \frac{\left(T_{i,new}-T_{i,old}\right)}{\Delta t}}$$</div>
-
-Where:
-
-HeatCap1<sub>i</sub> = heat capacitance associated with a given outer half-node
-HeatCap2<sub>i</sub> = heat capacitance associated with a given inner half-node
-QDreport<sub>i</sub> = CondFD Surface Heat Flux Node < i >
-QSource<sub>i</sub> = internal source heat flux at node i
-Q<sub>inside</sub> = Surface Inside Face Conduction Heat Transfer Rate per Area [W/m<sup>2</sup>]
-
-N = total number of nodes in a surface including the surface inside face node.
-Note that the variable *TotNodes* used in the source code is actually N-1. The surface inside face node is referenced as *TotNodes+1*.
-
-### References
-
-Pedersen C.O., Enthalpy Formulation of conduction heat transfer problems involving latent heat, Simulation, Vol 18, No. 2, February 1972
-
-Versteeg, H. and Malalasekra, W. 1996. An introduction to computational fluid dynamic: the finite volume method approach. Prentice Hall.
-
-[Tabares-Velasco, P.C. and Griffith, B. 2012. Diagnostic Test Cases for Verifying Surface Heat Transfer Algorithms and Boundary Conditions in Building Energy Simulation Programs, Journal of Building Performance Simulation, doi:10.1080/19401493.2011.595501](../../../Documents%20and%20Settings/ptabares/My%20Documents/Paulo/CV/Tabares%20Velasco%20CV%20UPDATED2.doc)
-
-Tabares-Velasco, P.C., Christensen, C. and Bianchi, M. 2012. Verification and Validation of EnergyPlus Phase Change Material Model for Opaque Wall Assemblies, Building and Environment 54: 186-196.
-
-Combined Heat and Moisture Transfer (HAMT) Model
-------------------------------------------------
-
-### Overview
-
-The combined heat and moisture transfer finite (HAMT) solution algorithm is a completely coupled, one-dimensional, finite element, heat and moisture transfer model simulating the movement and storage of heat and moisture in surfaces simultaneously from and to both the internal and external environments. As well as simulating the effects of moisture buffering, HAMT is also be able to provide temperature and moisture profiles through composite building walls, and help to identify surfaces with high surface humidity.
-
-### HAMT Nomenclature
-
-Dependencies on moisture content are indicated by a superscript <sup>w</sup>, on heat by a superscript <sup>h</sup> and vapor pressure by a superscript <sup>v</sup>.
-
-Table 2. Combined Heat and Moisture Transfer Model Nomenclature
-
-<table class="table table-striped">
-<tr>
-<th>Symbol</th>
-<th>Units</th>
-<th>Meaning</th>
-</tr>
-<tr>
-<td>T</td>
-<td>°C</td>
-<td>Temperature</td>
-</tr>
-<tr>
-<td>RH,φ</td>
-<td>%, fraction</td>
-<td>Relative humidity</td>
-</tr>
-<tr>
-<td>W</td>
-<td>kg/m<sup>3</sup></td>
-<td>Moisture Content</td>
-</tr>
-<tr>
-<td><span>\({\raise0.7ex\hbox{${\partial H}$} \!\mathord{\left/ {\vphantom {{\partial H} {\partial T}}}\right.}\!\lower0.7ex\hbox{${\partial T}$}}\)</span></td>
-<td>J/m<sup>3</sup>C</td>
-<td>Moisture dependent heat storage capacity</td>
-</tr>
-<tr>
-<td><span>\({\raise0.7ex\hbox{${\partial w}$} \!\mathord{\left/ {\vphantom {{\partial w} {\partial \phi }}}\right.}\!\lower0.7ex\hbox{${\partial \phi }$}}\)</span></td>
-<td>kg/m<sup>3</sup></td>
-<td>Moisture dependent moisture storage capacity</td>
-</tr>
-<tr>
-<td><span>\({k^w}\)</span></td>
-<td>W/mC</td>
-<td>Moisture dependent thermal conductivity</td>
-</tr>
-<tr>
-<td><span>\({h_v}\)</span></td>
-<td>J/kg</td>
-<td>Evaporation enthalpy of water (= 2, 489, 000J/kg)</td>
-</tr>
-<tr>
-<td><span>\(\delta \)</span></td>
-<td>kg/msPa</td>
-<td>Vapor diffusion coefficient in air</td>
-</tr>
-<tr>
-<td><span>\(\mu \)</span></td>
-<td>-</td>
-<td>Moisture dependent vapor diffusion resistance factor</td>
-</tr>
-<tr>
-<td>P</td>
-<td>Pa</td>
-<td>Vapor pressure</td>
-</tr>
-<tr>
-<td>p<sub>ambient</sub></td>
-<td>Pa</td>
-<td>Ambient air pressure</td>
-</tr>
-<tr>
-<td>C</td>
-<td>J/kgC</td>
-<td>Specific heat capacity of dry material</td>
-</tr>
-<tr>
-<td>c<sup>w</sup></td>
-<td>J/KgC</td>
-<td>Specific heat capacity of water (=4,180J/kg<sup>o</sup>C@ 20<sup>o</sup>C)</td>
-</tr>
-<tr>
-<td><span>\(\rho \)</span></td>
-<td>kg/m<sup>3</sup></td>
-<td>Material Density</td>
-</tr>
-<tr>
-<td><span>\({\rho ^w}\)</span></td>
-<td>kg/m<sup>3</sup></td>
-<td>Density of water (= 1000kg/m3)</td>
-</tr>
-<tr>
-<td><span>\({D^w}\)</span></td>
-<td>m<sup>2</sup>/s</td>
-<td>Liquid Transport Coefficient</td>
-</tr>
-<tr>
-<td>A</td>
-<td>m<sup>2</sup></td>
-<td>Contact Surface area</td>
-</tr>
-<tr>
-<td><span>\(\Delta {V_i}\)</span></td>
-<td>m<sup>3</sup></td>
-<td>Cell Volume</td>
-</tr>
-<tr>
-<td><span>\(t\)</span></td>
-<td>s</td>
-<td>Time</td>
-</tr>
-<tr>
-<td><span>\(\Delta \tau \)</span></td>
-<td>s</td>
-<td>Time step between calculations</td>
-</tr>
-<tr>
-<td>x</td>
-<td>m</td>
-<td>Distance between cell centres</td>
-</tr>
-<tr>
-<td><span>\(C_i^h\)</span></td>
-<td>J/C</td>
-<td>Heat Capacitance of cell i</td>
-</tr>
-<tr>
-<td><span>\(C_i^w\)</span></td>
-<td>kg</td>
-<td>Moisture Capacitance of cell i</td>
-</tr>
-<tr>
-<td><span>\(R_{ij}^h\)</span></td>
-<td>C/W</td>
-<td>Heat Resistance between cells i and j</td>
-</tr>
-<tr>
-<td><span>\(R_{ij}^v\)</span></td>
-<td>sPa/kg</td>
-<td>Vapor Resistance between cells i and j</td>
-</tr>
-<tr>
-<td><sup><span>\(R_{ij}^w\)</span></sup></td>
-<td>s/kg</td>
-<td>Liquid Moisture Resistance between cells i and j</td>
-</tr>
-<tr>
-<td><sup><span>\(q_i^v\)</span></sup></td>
-<td>W</td>
-<td>Heat due to Vaporisation</td>
-</tr>
-<tr>
-<td><sup><span>\(q_i^{adds}\)</span></sup></td>
-<td>W</td>
-<td>Heat from additional Sources</td>
-</tr>
-<tr>
-<td>P</td>
-<td>m3/m3</td>
-<td>Material Porosity</td>
-</tr>
-<tr>
-<td>p(as a superscript)</td>
-<td>s</td>
-<td>Present Time Step</td>
-</tr>
-<tr>
-<td>i,j</td>
-<td>-</td>
-<td>Cell indices</td>
-</tr>
-
-</table>
-
-### HAMT Model Description
-
-Equations and are derived from heat and moisture balance equations and are taken from [Künzel, H.M. (1995)]. They describe a theoretical model for the transfer of heat and moisture through a material.
-
-<div>$$\frac{{\partial H}}{{\partial T}}\frac{{\partial T}}{{\partial \tau }} = \frac{\partial }{{\partial x}}\left( {{k^w}\frac{{\partial T}}{{\partial x}}} \right) + {h_v}\frac{\partial }{{\partial x}}\left( {\frac{\delta }{\mu }\frac{{\partial T}}{{\partial x}}} \right)$$</div>
-
-The three terms in equation describe the storage, transport and generation of heat respectively.
-
-<div>$$\frac{{\partial w}}{{\partial \phi }}\frac{{\partial \phi }}{{\partial \tau }} = \frac{\partial }{{\partial x}}\left( {{D^w}\frac{{\partial w}}{{\partial \phi }}\frac{{\partial \phi }}{{\partial x}}} \right) + \frac{\partial }{{\partial x}}\left( {\frac{\delta }{\mu }\frac{{\partial T}}{{\partial x}}} \right)$$</div>
-
-The three terms in equation describe the storage of moisture, the transport of liquid moisture and the transport of vapor respectively. The equation to calculate the vapor diffusion coefficient in air (<span>\(\delta \)</span>) used in the third term of both equations, is also taken from Künzel,
-
-<div>$$\delta  = \frac{{\left( {2 \times {{10}^{ - 7}} \times {{\left( {T + 273.15} \right)}^{0.81}}} \right)}}{{{P_{ambient}}}}$$</div>
-
-The heat storage capacity (<span>\(\frac{\partial H}{\partial T}\)</span>) depends on the moisture content w of the material by the following equation.
-
-<div>$$\frac{{\partial H}}{{\partial T}} = \left( {c\rho  + {c^w}w} \right)$$</div>
-
-The moisture content of the material w and the vapor diffusion resistance factor μ depend on the relative humidity inside the material. The parameters <span>\(\frac{\partial w}{\partial \phi}\)</span>, <span>\({k^w}\)</span> and <span>\({D^w}\)</span>are also moisture dependent parameters.
-
-The following sections describe how the above equations are used within the HAMT model.
-
-#### Surfaces, Material Layers and Cells
-
-“Surfaces� are made of a number of layers of potentially any combination of materials. Each surface is split into its constituent materials and is then split up further into cells through its depth. HAMT will generate no more than 10 cells per material with widths that are thinner near the boundaries of each material where most changes are expected and detail is needed.
-
-#### Heat Transfer
-
-Equation 1 can be re-written and used to describe the heat storage and transfer through the i<sup>th</sup> cell in a surface.
-
-<div>$$\left( {{c_i}{\rho_i} + {c^w}{w_i}} \right)\Delta {V_i}\frac{{T_i^{p + 1} - T_i^p}}{{\Delta \tau }} = \sum\limits_j {k_{ij}^w{A_{ij}}\frac{{T_j^{p + 1} - T_i^{p + 1}}}{{{x_{ij}}}}}  + \sum\limits_j {{h_v}\frac{{{\delta_{ij}}}}{{{\mu_{ij}}}}{A_{ij}}\frac{{p_j^{p + 1} - p_i^{p + 1}}}{{{x_{ij}}}}} $$</div>
-
-In the one dimensional case there are only two adjacent cells each labelled j. The heat generated due to vaporisation<span>\(q_i^v\)</span> can be calculated separately.
-
-<div>$$q_i^v = \sum\limits_j {{h_v}\frac{{{\delta_{ij}}}}{{{\mu_{ij}}}}{A_{ij}}\frac{{p_j^{p + 1} - p_i^{p + 1}}}{{{x_{ij}}}}} $$</div>
-
-Rearranging equation and including other sources of heat (<span>\(q_i^{adds}\)</span>) such as radiation from other surfaces in the calculation gives the temperature in a cell in the next time step as,
-
-<div>$$T_i^{p + 1} = \frac{{\sum\nolimits_j {\frac{{T_j^{p + 1}}}{{R_{ij}^h}}}  + q_i^v + q_i^{adds} + C_i^h\frac{{T_i^p}}{{\Delta \tau }}}}{{\frac{{C_i^h}}{{\Delta \tau }} + \sum\nolimits_j {\frac{1}{{R_{ij}^h}}} }}$$</div>
-
-where<span>\(C_i^h = \left( {{c_i}{\rho_i} + {c^w}{w_i}} \right)\Delta {V_i}\)</span> is thermal heat capacitance of cell i and <span>\(R_{ij}^h = \frac{x_{ij}}{k_{ij}A_{ij}}\)</span> is the thermal resistance between cells i and j.
-
-This equation can be solved using the Gauss-Seidel iteration technique. The i<sup>th</sup> cell temperature is calculated whilst the j<sup>th</sup> cell temperatures are kept as up to date as possible. The iteration is stopped when the maximum difference between two consecutive calculations in all cells is less than a threshold of 0.002°C.
-
-#### Moisture Content w
-
-The moisture content (w) of a cell is needed for the calculation of the heat transfer through the cell as it affects the thermal resistance and heat capacitance. The moisture content of cells is calculated from the relative humidity (RH) of the material. The relationship between w and the RH for each material is known as the sorption isotherm and measured data points are entered into EnergyPlus as a series of coordinates. HAMT interpolates between the measurements to obtain the moisture content of a material for any RH value. The sorption isotherm input is via the MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm object and is described in the Input Output Reference document.
-
-#### Porosity P
-
-The porosity of a material (P) is an input variable and defined as the maximum fraction, by volume, of a material that can be taken up with moisture. It is used to calculate the maximum point on the sorption isotherm curve.  The porosity is entered for each material via the MaterialProperty:HeatAndMoistureTransfer:Settings object, as described in the Input Output Reference document.
-
-#### Moisture Dependant Thermal Conductivity k<sup>w</sup>
-
-The thermal conductivity (k<sup>w</sup>) of the cell is determined by interpolating between data points of thermal conductivity versus the moisture content of the material, entered into EnergyPlus via the MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity object. The moisture content is determined via the sorption isotherm which gives the moisture content as a function of Relative Humidity.
-
-#### Moisture Dependant Moisture Diffusion Coefficient μ
-
-This is used in the third term of equation to describe the heat transfer due to vapor movement. It is determined by interpolating between data points of moisture diffusion coefficient versus the moisture content of the material, entered into EnergyPlus via the MaterialProperty:HeatAndMoistureTransfer:Diffusion object. A simple linear interpolation is used to obtain the conductivity between measured points.
-
-#### Moisture Transfer
-
-Moisture, as well as heat, is transported through materials as either liquid (w) or vapor (p). There are two different potentials that control the movement though the material. Liquid transfer is driven by differences in relative humidity whereas vapor transfer is driven by differences in vapor pressure. Materials also have a capacity to store moisture. Equation can be re-written for a discrete cell in a continuous material.
-
-<div>$$\frac{{dw}}{{d{\phi_i}}}\Delta {V_i}\frac{{\phi_i^{p + 1} - \phi_i^p}}{{\Delta \tau }} = \sum\limits_j {{k_{ij}}{A_{ij}}\frac{{\phi_j^{p + 1} - \phi_i^{p + 1}}}{{{x_{ij}}}}}  + \sum\limits_j {\frac{{{\delta_{ij}}}}{{{\mu_{ij}}}}{A_{ij}}\frac{{p_j^{p + 1} - p_i^{p + 1}}}{{{x_{ij}}}}} $$</div>
-
-Equation can be rearranged to provide the relative humidity of the i<sup>th</sup> cell in the next time step.
-
-<div>$$\phi_i^{p + 1} = \frac{{\sum\nolimits_j {\frac{{\phi_j^{p + 1}}}{{R_{ij}^w}}}  + \sum\nolimits_j {\frac{{p_i^{p + 1}}}{{R_{ij}^v}}}  + C_i^w\frac{{\phi_i^p}}{{\Delta \tau }}}}{{\frac{{C_i^w}}{{\Delta \tau }} + \sum\nolimits_j {\frac{1}{{R_{ij}^w}} + \sum\nolimits_j {\frac{{p_i^{sat}}}{{R_{ij}^v}}} } }}$$</div>
-
-where <span>\(C_i^w = \frac{dw}{d\phi_{i}}\Delta {V_i}\)</span> is the "Moisture Capacitance" of cell i,
-
-<div>$$R_{ij}^w = \frac{{{x_{ij}}}}{{{A_{ij}}D_{ij}^w\frac{{dw}}{{d\phi }}}}$$</div>
-
-is the moisture resistance between cells i and j and <span>\(R_{ij}^v = \frac{\mu_{ij}x_{ij}}{A_{ij}\delta_{ij}}\)</span> is the vapor resistance between cells i and j.
-
-Equation can be used together with the heat equation in an alternate step by step fashion to calculate the new temperature and relative humidity profiles for each cell for the next time step.
-
-#### Liquid Transport Coefficient D<sup>w</sup>
-
-The Moisture Dependant Liquid Transport Coefficient is entered as a series of moisture density and liquid transport coefficient data points. There are two different coefficients, one for suction, where the surface is wet due to rain, and one for redistribution where the surface is no longer wet. If the weather file has a rain flag it is used to switch between these two types of coefficient. HAMT-SUCTION and HAMT-REDISTRIBUTION.
-
-#### Moisture Dependent Moisture Capacity <span>\(\frac{\partial w}{\partial \phi}\)</span>
-
-This is simply the gradient of moisture sorption isotherm at the RH of the material.
-
-#### Convective Heat Transfer
-
-The internal and external heat transfer coefficients are used to calculate the thermal resistance of the boundary layer between the zone air and the surface of the surface. They are either supplied by the user via the advanced surface concepts object “SurfaceProperty:ConvectionCoefficients� or, if these are not provided, dynamic values are calculated.
-
-#### Convective Vapor Transfer
-
-The internal and external vapor transfer coefficients are used to calculate the resistance to vapour transfer of the boundary layer between the zone air and the surface of the surface. They are also either supplied by the user via the advanced surface concept object SurfaceProperties:VaporCoefficients. If these are not provided then dynamic values are calculated based on the convective heat transfer coefficients.
-
-#### Initial Moisture Content
-
-At the start of an EnergyPlus simulation “warm up� days are used to ensure that the temperatures of surfaces come to equilibrium with the environment before the simulation starts proper. Moisture content within some building fabrics can take a very long time to come to equilibrium with its environment and it is therefore necessary to set initial or typical values of moisture content for each material to be used at the start of the simulation. These initial values are entered for each material via the MaterialProperty:HeatAndMoistureTransfer:Settings object as described in the Input Output Reference document.
-
-#### Using the Model
-
-As an illustration of the use of the Heat and Moisture Transfer (HAMT) model, the material properties for a small sample of six generic materials have been provided in the EnergyPlus Reference DataSets (MoistureMaterials.idf). The properties were synthesised from the Annex 24 database [Kumar Kumaran, M. (1996)], supplemented, when required, by data from the database of the WUFI model [WUFI (1999)] and are therefore not related to any unique, measured material. Users should consult material property catalogues and other primary sources when the properties of a specific material are required.
-
-Moisture and heat from the surfaces are used by EnergyPlus to calculate the room air temperature and moisture content. EnergyPlus with HAMT works best with as short a time step as possible. However the optimum time step which gives a good prediction for a short computing time will very much depend on the nature of the weather and type of building. Buildings with frequent and large changes in internal and external temperature will need a small time step, maybe even 60 steps per hour. Slowly evolving temperatures and relative humidity’s will not require such a short time step and 20, or even 6, steps per hour may be sufficient.
-
-### References
-
-Künzel, H.M. (1995) Simultaneous Heat and Moisture Transport in Building Components. One- and two-dimensional calculation using simple parameters. IRB Verlag 1995
-
-Holman, J.P. (2002) Heat Transfer, Ninth Edition. McGraw-Hill
-
-Winterton, R.H.S. (1997) Heat Transfer. (Oxford Chemistry Primers; 50) Oxford University Press
-
-Kumar Kumaran, M. (1996) IEA ANNEX 24, Final Report, Volume 3
-
-WUFI (1999) version 2.2 Simultaneous Heat and Moisture Transport in Building components. Fraunhofer IBP, Holzkirchen, Germany
-
-Effective Moisture Penetration Depth (EMPD) Model
----------------------------------------------------------------------------
-
-### Overview
-
-Moisture has little effect on heating system performance, but a profound effect on the performance of air conditioning systems.  In order to accurately describe building performance during periods when cooling is needed, it is very important to know the moisture conditions of the building.  If one assumes that all building moisture is contained in the room air, then one ignores the fact that the materials that bound the room (e.g. wall surfaces, furnishings, linens, etc.) store and release moisture.  Thus, to assume that the only moisture that effects cooling system performance is contained in the room air is a false, and it can lead to significant error in the prediction of room moisture conditions and cooling system loads.
-
-The EMPD (Effective Moisture Penetration Depth) model is a simplified, lumped approach to simulate surface moisture adsorption and desorption.
-
-### EMPD Model Description
-
-The EMPD concept assumes that a thin layer (δ<sub>M</sub>) close to the wall surface behaves dynamically and exchanges moisture with the air domain when exposed to cyclic air moisture pulses.  For short periods where the cyclic integral of the total moisture adsorption and desorption is near zero (i.e. there is no net moisture storage), the EMPD concept has been shown to be a reasonable approximation of reality (Kerestecioglu et al, 1989).  In other words, the following constraint must be met:
-
-<div>$$\int_{{\tau_1}}^{{\tau_2}} {\frac{{dU}}{{d\tau }}} d\tau  = 0$$</div>
-
-where, τ<sub>2</sub>-τ<sub>1</sub> denotes the finite time interval over which the equation holds.  The EMPD model assumes no spatial distribution of moisture content across the thickness (L) of the solid; rather, a thin layer (δ<sub>M</sub>) of uniform moisture content (U) is assumed to represent the total moisture content of the solid. This may be mathematically stated as:
-
-<div>$$\int_0^L {U(x)dx = U{\delta_M}} $$</div>
-
-For most building materials, the equilibrium moisture sorption isotherm can be defined by the following general equation (Kerestecioglu et al. 1988):
-
-<div>$$U = a{\varphi ^b} + c{\varphi ^d}$$</div>
-
-where
-
-<div>$$\varphi  \approx \frac{{{W^*}}}{{{W_{sat}}^*}}$$</div>
-
-and
-
-<div>$${W_{sat}}^* = \frac{1}{{{R_v}{\rho_a}{T^*}}}\exp \left( {23.7093 - \frac{{4111}}{{{T^*} - 35.45}}} \right)$$</div>
-
- Given that U=U(W<sup>\*</sup>,T<sup>\*</sup>), the moisture content may be differentiated with respect to time in the following manner:
-
-<div>$$\frac{{du}}{{d\tau }} = \frac{{\partial U}}{{\partial {W^*}}}\frac{{d{W^*}}}{{d\tau }} + \frac{{\partial U}}{{\partial {T^*}}}\frac{{d{T^*}}}{{d\tau }} = {A_T}\frac{{d{W^*}}}{{d\tau }} - {B_\rho }\frac{{d{T^*}}}{{d\tau }}$$</div>
-
-where A<sub>T</sub> and B<sub>�</sub> are the isothermal moisture capacity and thermo-gradient coefficient, respectively.  From Eqs. , and , they can be expressed as:
-
-<div>$${A_T} = \frac{{ab{\varphi ^b} + cd{\varphi ^d}}}{{{W^*}}}$$</div>
-
-and
-
-<div>$${B_\rho } =  - \left[ {\frac{1}{{{T^*}}} - \frac{{4111}}{{{{({T^*} - 35.45)}^2}}}} \right]*(ab{\varphi ^b} + cd{\varphi ^d})$$</div>
-
-The lumped mass transfer equation for the i-th solid domain may be written as
-
-<div>$${(A{\rho_b}{\delta_M})_i}\frac{{d{U_i}}}{{d\tau }} = {h_{M,i}}{A_i}({W_r} - {W_i}^*)$$</div>
-
-Using Eqs. , , and , one obtains the final equation needed for closure moisture transfer at internal surface.
-
-<div>$${({A_i}{\rho_b}{\delta_M}{A_T})_i}\frac{{d{W_i}^*}}{{d\tau }} = {h_{M,i}}{A_i}({W_r} - {W_i}^*) + {(A{\rho_b}{\delta_M}{B_\rho })_i}\frac{{d{T_i}^*}}{{d\tau }}$$</div>
-
-The energy equation for the envelope contains the surface temperature and is given by the conduction equation
-
-<div>$$\rho {C_p}\frac{{dT}}{{d\tau }} = \nabla  \cdot (k\nabla T)$$</div>
-
-with the boundary conditions at interior surface
-
-<div>$$ - k\nabla T =  - {q_T}`` + {h_T}({T^*} - {T_r}) + \lambda {h_M}({W^*} - {W_r})$$</div>
-
-A more detailed account of the numerical solution procedure can be found in Kerestecioglu et al. (1988).
-
-### EMPD Value Determination
-
-An effective moisture penetration depth may be determined from either experimental or detailed simulation data by using actual surface areas and moisture vapor diffusivity.  An empirical function derived from the detailed simulation may be used to determine the EMPD value (Kerestecioglu et al, 1989):
-
-<div>$${\delta_M} = 12.567024 - 12.21373*\exp \left( { - 267.0211*{D_v}^{0.7}*{\xi ^{ - 0.7}}} \right)$$</div>
-
-where
-
-<div>$$\xi  = \left| {\frac{{\Delta \varphi }}{{\Delta \tau }}} \right|$$</div>
-
-Figure 17 gives the EMPD values to be used for various vapor diffusivities evaluated at different ambient excitations.
-
-![](media/image241.svg.png)
-
-Figure 17. Limit of Effective Penetration Depth Values for Various Vapor Diffusivities at Different Ambient Excitations.
-
-### EMPD Nomenclature
-
-A                = Area [m<sup>2</sup>]
-
-A<sub>T</sub>               = Isothermal moisture capacity [m<sup>3</sup>/kg]
-
-B<sub>�</sub>               = Thermo-gradient coefficient [kg/kg-K]
-
-C<sub>p</sub>               = Specific heat [J/kg.K]
-
-h<sub>M</sub>               = Convective mass transfer coeff. [kg/m<sup>2</sup>-s]
-
-h<sub>T</sub>               = Convective heat transfer coeff. [W/m<sup>2</sup>-K]
-
-k                = Thermal conductivity [W/m-K]
-
-L                = Length [m]
-
-q"<sub>T</sub>              = Imposed heat flux [W/m<sup>2</sup>]
-
-R<sub>v</sub>               = Ideal gas constant [461.52 J/kg-K]
-
-T                = Temperature [K]
-
-U                = Moisture content [kg/kg]
-
-W               = Humidity ratio [kg/kg]
-
-#### Greek letters
-
-δ<sub>M</sub>              = Effective penetration depth for moisture equation [m]
-
-λ                = Heat of vaporization [J/kg]
-
-�                = Density [kg/m<sup>3</sup>]
-
-τ                 = Time [s]
-
-φ                = Relative humidity [0 to 1]
-
-ξ                 = Ambient moisture excitation rate [1/h]
-
-
-
-#### Subscripts and superscripts
-
-a                = Air
-
-b                = Bulk
-
-\*                 = Surface
-
-i                 = i-th surface
-
-### References
-
-Kerestecioglu, A., Swami, M., Dabir, R., Razzaq, N., and Fairey, P., 1988, "Theoretical and Computational Investigation of Algorithms for Simultaneous Heat and Moisture Transport in Buildings," FSEC-CR-191-88, Florida Solar Energy Center, Cape Canaveral, FL.
-
-Kerestecioglu, A., M. Swami and A. Kamel, 1989, "Theoretical and Computational Investigation of Simultaneous Heat and Moisture Transfer in Buildings: Effective Penetration Depth Theory."  ASHRAE Winter Meeting, Atlanta, GA.
-
-Kerestecioglu, A., M. V. Swami, P. Brahma, L. Gu, P. Fairey, and S. Chandra, 1989, “FSEC 1.1 User’s Manual,� Florida Solar Energy Center, Cape Canaveral, FL
-
-Outside Surface Heat Balance
-----------------------------
-
-![](media/image242.png)
-
-Figure 18. Outside Heat Balance Control Volume Diagram
-
-The heat balance on the outside face is:
-
-<div>$${q''_{\alpha sol}} + {q''_{LWR}} + {q''_{conv}} - {q''_{ko}} = 0$$</div>
-
-where:
-
-<sub><span>\({q''_{\alpha sol}}\)</span> </sub>= Absorbed direct and diffuse solar (short wavelength) radiation heat flux.
-
-<sub><span>\({q''_{LWR}}\)</span> </sub>= Net long wavelength (thermal) radiation flux exchange with the air and surroundings.
-
-<sub><span>\({q''_{conv}}\)</span> </sub>= Convective flux exchange with outside air.
-
-<sub><span>\({q''_{ko}}\)</span> </sub> = Conduction heat flux (q/A) into the wall.
-
-All terms are positive for net flux to the face except the conduction term, which is traditionally taken to be positive in the direction from outside to inside of the wall.  Simplified procedures generally combine the first three terms by using the concept of a *sol-air temperature*.  Each of these heat balance components is introduced briefly below.
-
-### External Shortwave Radiation
-
-<sub><span>\({q''_{\alpha sol}}\)</span> </sub> is calculated using procedures presented later in this manual and includes both direct and diffuse incident solar radiation absorbed by the surface face.  This is influenced by location, surface facing angle and tilt, surface face material properties, weather conditions, etc.
-
-### External Longwave Radiation
-
-<span>\({q''_{LWR}}\)</span> is a standard radiation exchange formulation between the surface, the sky, and the ground.  The radiation heat flux is calculated from the surface absorptivity, surface temperature, sky and ground temperatures, and sky and ground view factors.
-
-The longwave radiation heat exchange between surfaces is dependent on surface temperatures, spatial relationships between surfaces and surroundings, and material properties of the surfaces. The relevant material properties of the surface, emissivity e and absorptivity a, are complex functions of temperature, angle, and wavelength for each participating surface. However, it is generally agreed that reasonable assumptions for building loads calculations are (Chapman 1984; Lienhard 1981):
-
-·        each surface emits or reflects diffusely and is gray and opaque (a = e, t = 0, r = 1- e)
-
-·        each surface is at a uniform temperature
-
-·        energy flux leaving a surface is evenly distributed across the surface,
-
-·        the medium within the enclosure is non-participating.
-
-These assumptions are frequently used in all but the most critical engineering applications.
-
-
-
-Table 3. Nomenclature List of Variables.
-
-<table class="table table-striped">
-<tr>
-<th>Mathematical variable</th>
-<th>Description</th>
-<th>Units</th>
-<td>Range</td>
-</tr>
-<tr>
-<td>q&quot;<sub>LWR</sub></td>
-<td>Exterior surface longwave radiation flux</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>r</sub></td>
-<td>Linearized radiative heat transfer  coefficient to air temperature</td>
-<td>W/(m<sup>2</sup> K)</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sub>surf</sub></td>
-<td>Surface Outside face temperatures</td>
-<td>K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sub>air</sub></td>
-<td>Outside air temperature</td>
-<td>K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sub>gnd</sub>
- </td>
-<td>Environmental ground surface temperature</td>
-<td>K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sub>sky</sub></td>
-<td>Sky Effective temperature</td>
-<td>K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>F<sub>gnd</sub></td>
-<td>view factor of wall surface to ground surface</td>
-<td>-</td>
-<td>0~1</td>
-</tr>
-<tr>
-<td>F<sub>sky</sub></td>
-<td>View factor of wall surface to sky</td>
-<td>-</td>
-<td>0~1</td>
-</tr>
-<tr>
-<td>F<sub>air</sub></td>
-<td>View factor of wall surface to air</td>
-<td>-</td>
-<td>0~1</td>
-</tr>
-<tr>
-<td>e</td>
-<td>Surface long-wave emissivity</td>
-<td>-</td>
-<td>0~1</td>
-</tr>
-<tr>
-<td>s</td>
-<td>Stefan-Boltzmann constant</td>
-<td>W/m<sup>2</sup>-K<sup>4</sup></td>
-<td>0.0000000567</td>
-</tr>
-
-</table>
-
-Consider an enclosure consisting of building exterior surface, surrounding ground surface, and sky.  Using the assumptions above, we can determine the longwave radiative heat flux at the building exterior surface (Walton 1983; McClellan and Pedersen 1997).  The total longwave radiative heat flux is the sum of components due to radiation exchange with the ground, sky, and air.
-
-<div>$$q_{LWR}^`` = {q''_{gnd}} + {q''_{sky}} + {q''_{air}}$$</div>
-
-Applying the Stefan-Boltzmann Law to each component yields:
-
-<div>$$q_{_{LWR}}^`` = \varepsilon \sigma {F_{gnd}}(T_{gnd}^4 - T_{surf}^4) + \varepsilon \sigma {F_{sky}}(T_{sky}^4 - T_{surf}^4) + \varepsilon \sigma {F_{air}}(T_{air}^4 - T_{surf}^4)$$</div>
-
-where
-
-e=long-wave emittance of the surface
-
-s=Stefan-Boltzmann constant
-
-F<sub>gnd</sub> = view factor of wall surface to ground surface temperature
-
-F<sub>sky</sub> = view factor of wall surface to sky temperature
-
-F<sub>air</sub> =view factor of wall surface to air temperature
-
-T<sub>surf</sub> = outside surface temperature
-
-T<sub>gnd</sub> = ground surface temperature
-
-T<sub>sky</sub> = sky temperature
-
-T<sub>air</sub> = air temperature
-
-Linearized radiative heat transfer coefficients are introduced to render the above equation more compatible with the heat balance formulation,
-
-<div>$$q_{_{LWR}}^`` = {h_{r,gnd}}({T_{gnd}} - {T_{surf}}) + {h_{r,sky}}({T_{sky}} - {T_{surf}}) + {h_{r,air}}({T_{air}} - {T_{surf}})$$</div>
-
-where
-
-<div>$${h_{r,gnd}} = \frac{{\varepsilon \sigma {F_{gnd}}(T_{surf}^4 - T_{gnd}^4)}}{{{T_{surf}} - {T_{gnd}}}}$$</div>
-
-<div>$${h_{r,sky}} = \frac{{\varepsilon \sigma {F_{sky}}(T_{surf}^4 - T_{sky}^4)}}{{{T_{surf}} - {T_{sky}}}}$$</div>
-
-<div>$${h_{r,air}} = \frac{{\varepsilon \sigma {F_{air}}(T_{surf}^4 - T_{air}^4)}}{{{T_{surf}} - {T_{air}}}}$$</div>
-
-The longwave view factors to ground and sky are calculated with the following expressions (Walton 1983):
-
-<div>$${F_{ground}} = 0.5(1 - \cos \phi )$$</div>
-
-<div>$${F_{sky}} = 0.5(1 + \cos \phi )$$</div>
-
-where *f* is the tilt angle of the surface.  The view factor to the sky is further split between sky and air radiation by:
-
-<div>$$\beta  = \sqrt {0.5\left( {1 + \cos \phi } \right)} $$</div>
-
-The ground surface temperature is assumed to be the same as the air temperature.  The final forms of the radiative heat transfer coefficients are shown here.
-
-<div>$${h_{r,gnd}} = \frac{{\varepsilon \sigma {F_{gnd}}(T_{surf}^4 - T_{air}^4)}}{{{T_{surf}} - {T_{air}}}}$$</div>
-
-<div>$${h_{r,sky}} = \frac{{\varepsilon \sigma {F_{sky}}\beta (T_{surf}^4 - T_{sky}^4)}}{{{T_{surf}} - {T_{sky}}}}$$</div>
-
-<div>$${h_{r,air}} = \frac{{\varepsilon \sigma {F_{sky}}\left( {1 - \beta } \right)(T_{surf}^4 - T_{air}^4)}}{{{T_{surf}} - {T_{air}}}}$$</div>
-
-### References
-
-ASHRAE. 1993. 1993 ASHRAE Handbook – Fundamentals. Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
-
-Chapman, A. J. 1984. Heat Transfer, 4<sup>th</sup> Edition, New York: Macmillan Publishing Company.
-
-Lienhard, J. H. 1981. A Heat Transfer Textbook, Englewood Cliffs, N.J.: Prentice-Hall, Inc.
-
-McClellan, T. M., and C. O. Pedersen. 1997. Investigation of Outside Heat Balance Models for Use in a Heat Balance Cooling Load Calculation. ASHRAE Transactions, Vol. 103, Part 2, pp. 469-484.
-
-Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards.
-
-### Atmospheric Variation
-
-All buildings are located in the troposphere, the lowest layer of the atmosphere.  The troposphere extends from sea level to an altitude of 11 km.  Throughout the troposphere, air temperature decreases almost linearly with altitude at a rate of approximately 1°C per 150 m.  Barometric pressure decreases more slowly.  Wind speed, on the other hand, increases with altitude.
-
-Because the atmosphere changes with altitude (defined as *height above ground* in this case), tall buildings can experience significant differences in local atmospheric properties between the ground floor and the top floor.  Buildings interact with the atmosphere through convective heat transfer between the outdoor air and the exterior surfaces of the building envelope, and through the exchange of air between the outside and inside of the building via infiltration and ventilation.
-
-Impetus for using this modeling is illustrated in the next table.  Using a 70 story (284 meters) building as an example, the atmospheric variables are significant.
-
-Table 4.  Atmospheric Variables at Two Different Altitudes above Ground Level
-
-<table class="table table-striped">
-<tr>
-<th>Variable</th>
-<th>1.5 Meters</th>
-<th>284 meters</th>
-<th>Absolute Diff</th>
-<th>Percent Diff</th>
-</tr>
-<tr>
-<td>Air Temperature</td>
-<td>15°C</td>
-<td>13.15°C</td>
-<td>1.85°C</td>
-<td>12.3%</td>
-</tr>
-<tr>
-<td>Barometric Pressure</td>
-<td>101,325 Pa</td>
-<td>97,960 Pa</td>
-<td>3,365 Pa</td>
-<td>3.3%</td>
-</tr>
-<tr>
-<td>Wind Speed</td>
-<td>2.46 m/s</td>
-<td>7.75 m/s</td>
-<td>5.29 m/s</td>
-<td>215%</td>
-</tr>
-
-</table>
-
-Comparing the annual energy usage between 60 discretely modeled floors of a building, it turns out that the effect due to wind speed change is dominant over the first ten floors.  But at floor 25, surprisingly, the effect due to air temperature has caught up and is about equal to the effect of wind speed.  Above floor 25 the effect due to air temperature is now dominant.  Clearly it is desirable to model air temperature variation with altitude for high-rise buildings.
-
-To accommodate atmospheric variation EnergyPlus automatically calculates the local outdoor air temperature and wind speed separately for each zone and surface that is exposed to the outdoor environment.  The zone centroid or surface centroid are used to determine the height above ground.  Only local outdoor air temperature and wind speed are currently calculated because they are important factors for the exterior convection calculation for surfaces (see Exterior Convection below) and can also be factors in the zone infiltration and ventilation calculations.  Variation in barometric pressure, however, is considered when using the Airflow Network objects.
-
-#### Local Outdoor Air Temperature Calculation
-
-Variation in outdoor air temperature is calculated using the U.S. Standard Atmosphere (1976).  According to this model, the relationship between air temperature and altitude in a given layer of the atmosphere is:
-
-<div>$${T_z} = {T_b} + L\left( {{H_z} - {H_b}} \right)$$</div>
-
-where
-
-*T<sub>z</sub>* = air temperature at altitude *z*
-
-*T<sub>b</sub>* = air temperature at the base of the layer, i.e., ground level for the troposphere
-
-*L* = air temperature gradient, equal to –0.0065 K/m in the troposphere
-
-*H<sub>b</sub>* = offset equal to zero for the troposphere
-
-*H<sub>z</sub>* = geopotential altitude.
-
-The variable *H<sub>z</sub>* is defined by:
-
-<div>$${H_z} = \frac{{Ez}}{{\left( {E + z} \right)}}$$</div>
-
-where
-
-*E* = 6,356 km, the radius of the Earth
-
-*z* = altitude.
-
-For the purpose of modeling buildings in the troposphere, altitude *z* refers to the height above ground level, not the height above sea level.  The height above ground is calculated as the height of the centroid, or area-weighted center point, for each zone and surface.
-
-The air temperature at ground level, *T<sub>b</sub>*, is derived from the weather file air temperature by inverting the equation above:
-
-<div>$${T_b} = {T_{z,met}} - L\left( {\frac{{E{z_{met}}}}{{E + {z_{met}}}} - {H_b}} \right)$$</div>
-
-where
-
-*T<sub>z,met</sub>* = weather file air temperature (measured at the meteorological station)
-
-*z<sub>met</sub>* = height above ground of the air temperature sensor at the meteorological station.
-
-The default value for *z<sub>met</sub>* for air temperature measurement is 1.5 m above ground.  This value can be overridden by using the Site:WeatherStation object.
-
-#### Local Wind Speed Calculation
-
-Chapter 16 of the Handbook of Fundamentals (ASHRAE 2005).  The wind speed measured at a meteorological station is extrapolated to other altitudes with the equation:
-
-<div>$${V_z} = {V_{met}}{\left( {\frac{{{\delta_{met}}}}{{{z_{met}}}}} \right)^{{\alpha_{met}}}}{\left( {\frac{z}{\delta }} \right)^\alpha }$$</div>
-
-where
-
-*z* = altitude, height above ground
-
-*V<sub>z</sub>* = wind speed at altitude *z*
-
-*a* = wind speed profile exponent at the site
-
-*d* = wind speed profile boundary layer thickness at the site
-
-*z<sub>met</sub>* = height above ground of the wind speed sensor at the meteorological station
-
-*V<sub>met</sub>* = wind speed measured at the meteorological station
-
-*a<sub>met</sub>* = wind speed profile exponent at the meteorological station
-
-*d<sub>met</sub>* = wind speed profile boundary layer thickness at the meteorological station.
-
-The wind speed profile coefficients *a*, *d*, *a<sub>met</sub>*, and *d<sub>met</sub>*, are variables that depend on the roughness characteristics of the surrounding terrain.  Typical values for *a* and d are shown in the following table:
-
-
-
-Table 5. Wind Speed Profile Coefficients (ASHRAE Fundamentals 2005).
-
-<table class="table table-striped">
-<tr>
-<th>Terrain Description</th>
-<th>Exponent,a</th>
-<th>Boundary Layer Thickness,d (m)</th>
-</tr>
-<tr>
-<td>Flat, open country</td>
-<td>0.14</td>
-<td>270</td>
-</tr>
-<tr>
-<td>Rough, wooded country</td>
-<td>0.22</td>
-<td>370</td>
-</tr>
-<tr>
-<td>Towns and cities</td>
-<td>0.33</td>
-<td>460</td>
-</tr>
-<tr>
-<td>Ocean</td>
-<td>0.10</td>
-<td>210</td>
-</tr>
-<tr>
-<td>Urban, industrial, forest</td>
-<td>0.22</td>
-<td>370</td>
-</tr>
-
-</table>
-
-
-
-The terrain types above map to the options in the *Terrain* field of the Building object.  The *Terrain* field can be overridden with specific values for *a* and d by using the Site:HeightVariation object.
-
-The default value for *z<sub>met</sub>* for wind speed measurement is 10 m above ground.  The default values for *a<sub>met</sub>* and *d<sub>met</sub>* are 0.14 and 270 m, respectively, because most meteorological stations are located in an open field.  These values can be overridden by using the Site:WeatherStation object.
-
-### Outdoor/Exterior Convection
-
-Heat transfer from surface convection is modeled using the classical formulation:
-
-<div>$${Q_c} = {h_{c,ext}}A\left( {{T_{surf}} - {T_{air}}} \right)$$</div>
-
-where
-
-*Q<sub>c</sub>* = rate of exterior convective heat transfer
-
-*h<sub>c,ext</sub>* = exterior convection coefficient
-
-*A* = surface area
-
-*T<sub>surf</sub>* = surface temperature
-
-*T<sub>air</sub>* = outdoor air temperature
-
-Substantial research has gone into the formulation of models for estimating the exterior convection coefficient. Since the 1930's there have been many different methods published for calculating this coefficient, with much disparity between them (Cole and Sturrock 1977; Yazdanian and Klems 1994).  More recently Palyvos (2008) surveyed correlations cataloging some 91 different correlations into four categories based on functional form of the model equation.  EnergyPlus therefore offers a wide selection of different methods for determining values for *h<sub>c,ext</sub>*. The selection of model equations for *h<sub>c,ext</sub>* can be made at two different levels. The first is the set of options available in the input object SurfaceConvectionAlgorithm:Outside that provides a way of broadly selecting which model equations are applied throughout the model.  The input objects SurfaceProperty:ConvectionCoefficients and SurfaceProperty:ConvectionCoefficients:MultipleSurface also provide ways of selecting which model equations or values are applied for specific surfaces.  These basic options are identified by the key used for input and include:
-
-* SimpleCombined
-
-* TARP
-
-* MoWiTT
-
-* DOE-2
-
-* AdaptiveConvectionAlgorithm
-
-Note that when the outside environment indicates that it is raining, the exterior surfaces (exposed to wind) are assumed to be wet.  The convection coefficient is set to a very high number (1000) and the outside temperature used for the surface will be the wet-bulb temperature.  (If you choose to report this variable, you will see 1000 as its value.)
-
-When the AdaptiveConvectionAlgorithm is used, there is a second, deeper level of control available for selecting among a larger variety of *h<sub>c,ext</sub>* equations and also defining custom equations using curve or table objects.  These options are described in this section.
-
-In addition to the correlation choices described below, it is also possible to override the convection coefficients on the outside of any surface by other means:
-
-* Use the SurfaceProperty:ConvectionCoefficients object in the input file to set the convection coefficient value on either side of any surface.
-
-* Use the SurfaceProperty:OtherSideCoefficients object in the input file to set heat transfer coefficients and temperatures on surfaces.
-
-* Use the EnergyManagementSystem Actuators that are available for overriding h<sub>c</sub> values.
-
-These options can also use schedules to control values over time. Specific details are given in the Input Output Reference document.
-
-#### Simple Combined
-
-The simple algorithm uses surface roughness and local surface windspeed to calculate the exterior heat transfer coefficient (key:SimpleCombined).  The basic equation used is:
-
-<div>$$h = D + E{V_z} + F{V_z}^2$$</div>
-
-where
-
-*h* = heat transfer coefficient
-
-*V<sub>z</sub>* = local wind speed calculated at the height above ground of the surface centroid
-
-D, E, F = material roughness coefficients
-
-The roughness correlation is taken from Figure 1, Page 22.4, ASHRAE Handbook of Fundamentals (ASHRAE 1989).  The roughness coefficients are shown in the following table:
-
-Table 6.  Roughness Coefficients D, E, and F.
-
-<table class="table table-striped">
-<tr>
-<th>Roughness Index</th>
-<th>D</th>
-<th>E</th>
-<th>F</th>
-<th>Example Material</th>
-</tr>
-<tr>
-<td>1 (Very Rough)</td>
-<td>11.58</td>
-<td>5.894</td>
-<td>0.0</td>
-<td>Stucco</td>
-</tr>
-<tr>
-<td>2 (Rough)</td>
-<td>12.49</td>
-<td>4.065</td>
-<td>0.028</td>
-<td>Brick</td>
-</tr>
-<tr>
-<td>3 (Medium Rough)</td>
-<td>10.79</td>
-<td>4.192</td>
-<td>0.0</td>
-<td>Concrete</td>
-</tr>
-<tr>
-<td>4 (Medium Smooth)</td>
-<td>8.23</td>
-<td>4.0</td>
-<td>-0.057</td>
-<td>Clear pine</td>
-</tr>
-<tr>
-<td>5 (Smooth)</td>
-<td>10.22</td>
-<td>3.1</td>
-<td>0.0</td>
-<td>Smooth Plaster</td>
-</tr>
-<tr>
-<td>6 (Very Smooth)</td>
-<td>8.23</td>
-<td>3.33</td>
-<td>-0.036</td>
-<td>Glass</td>
-</tr>
-
-</table>
-
-Note that the simple correlation yields a combined convection and radiation heat transfer coefficient.  Radiation to sky, ground, and air is included in the exterior convection coefficient for this algorithm.
-
-All other algorithms yield a *convection only* heat transfer coefficient.  Radiation to sky, ground, and air is calculated automatically by the program.
-
-#### TARP ALGORITHM
-
-TARP, or Thermal Analysis Research Program, is an important predecessor of EnergyPlus (Walton 1983).  Walton developed a comprehensive model for exterior convection by blending correlations from ASHRAE and flat plate experiments by Sparrow et. al. In older versions of EnergyPlus, prior to version 6, the “TARP� model was called “Detailed.�  The model was reimplemented in version 6 to use Area and Perimeter values for the group of surfaces that make up a facade or roof, rather than the single surface being modeled.
-
-Table 7. Nomenclature List of Variables.
-
-<table class="table table-striped">
-<tr>
-<th>Variable</th>
-<th>Description</th>
-<th>Units</th>
-<th>Range</th>
-</tr>
-<tr>
-<td>A</td>
-<td>Surface area of the surface</td>
-<td>m<sup>2</sup></td>
-<td>/= 0</td>
-</tr>
-<tr>
-<td>h<sub>c</sub></td>
-<td>Surface exterior convective heat transfer coefficient</td>
-<td>W/(m<sup>2</sup>K)</td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>f</sub></td>
-<td>Forced convective heat transfer coefficient</td>
-<td>W/(m<sup>2</sup>K)</td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>n</sub></td>
-<td>Natural convective heat transfer coefficient</td>
-<td>W/(m<sup>2</sup>K)</td>
-<td>-</td>
-</tr>
-<tr>
-<td>P</td>
-<td>Perimeter of surface</td>
-<td>m</td>
-<td>-</td>
-</tr>
-<tr>
-<td>R<sub>f</sub></td>
-<td>Surface roughness multiplier</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sub>air</sub></td>
-<td>Local outdoor air temperature calculated at the height above ground of the surface centroid</td>
-<td>°C</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sub>so</sub></td>
-<td>Outside surface temperature</td>
-<td>°C</td>
-<td>-</td>
-</tr>
-<tr>
-<td>DT</td>
-<td>Temperature difference between the surface and air,</td>
-<td>°C</td>
-<td>-</td>
-</tr>
-<tr>
-<td>V<sub>z</sub></td>
-<td>Local wind speed calculated at the height above ground of the surface centroid</td>
-<td>m/s</td>
-<td>-</td>
-</tr>
-<tr>
-<td>W<sub>f</sub></td>
-<td>Wind direction modifier</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>f</td>
-<td>Angle between the ground outward normal and the surface outward normal</td>
-<td>degree</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Roughness Index</td>
-<td>Surface roughness index (6=very smooth, 5=smooth, 4=medium smooth, 3=medium rough, 2=rough, 1=very rough)</td>
-<td>-</td>
-<td>1~6</td>
-</tr>
-
-</table>
-
-
-
-The Detailed, BLAST, and TARP convection models are very similar.  In all three models, convection is split into forced and natural components (Walton 1981).  The total convection coefficient is the sum of these components.
-
-<div>$${h_c} = {h_f} + {h_n}$$</div>
-
-The forced convection component is based on a correlation by Sparrow, Ramsey, and Mass (1979):
-
-<div>$${h_f} = 2.537{W_f}{R_f}{\left( {\frac{{P{V_z}}}{A}} \right)^{1/2}}$$</div>
-
-where
-
-W<sub>f</sub>  =  1.0 for windward surfaces
-
-or
-
-W<sub>f</sub>  = 0.5 for leeward surfaces
-
-Leeward is defined as greater than 100 degrees from normal incidence (Walton 1981).
-
-The surface roughness multiplier Rf is based on the ASHRAE graph of surface conductance (ASHRAE 1981) and may be obtained from the following table:
-
-Table 8.  Surface Roughness Multipliers (Walton 1981).
-
-<table class="table table-striped">
-<tr>
-<th>Roughness Index</th>
-<th>Rf</th>
-<th>Example Material</th>
-</tr>
-<tr>
-<td>1 (Very Rough)</td>
-<td>2.17</td>
-<td>Stucco</td>
-</tr>
-<tr>
-<td>2 (Rough)</td>
-<td>1.67</td>
-<td>Brick</td>
-</tr>
-<tr>
-<td>3 (Medium Rough)</td>
-<td>1.52</td>
-<td>Concrete</td>
-</tr>
-<tr>
-<td>4 (Medium Smooth)</td>
-<td>1.13</td>
-<td>Clear pine</td>
-</tr>
-<tr>
-<td>5 (Smooth)</td>
-<td>1.11</td>
-<td>Smooth Plaster</td>
-</tr>
-<tr>
-<td>6 (Very Smooth)</td>
-<td>1.00</td>
-<td>Glass</td>
-</tr>
-
-</table>
-
-The natural convection component *h<sub>n</sub>* is calculated in the same way as the interior "Detailed" model.  The detailed natural convection model correlates the convective heat transfer coefficient to the surface orientation and the difference between the surface and zone air temperatures (where DT = Air Temperature - Surface Temperature).  The algorithm is taken directly from Walton (1983).  Walton derived his algorithm from the ASHRAE Handbook (2001), Table 5 on p. 3.12, which gives equations for natural convection heat transfer coefficients in the turbulent range for large, vertical plates and for large, horizontal plates facing upward when heated (or downward when cooled).   A note in the text also gives an approximation for large, horizontal plates facing downward when heated (or upward when cooled) recommending that it should be half of the facing upward value.  Walton adds a curve fit as a function of the cosine of the tilt angle to provide intermediate values between vertical and horizontal.  The curve fit values at the extremes match the ASHRAE values very well.
-
-For no temperature difference OR a vertical surface the following correlation is used:
-
-<div>$$h = 1.31{\left| {\Delta T} \right|^{\frac{1}{3}}}$$</div>
-
-For (DT &lt; 0.0 AND an upward facing surface)  OR  (DT &gt; 0.0 AND an downward facing surface) an enhanced convection correlation is used:
-
-<div>$$h = \frac{{9.482{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{7.283 - \left| {\cos \Sigma } \right|}}$$</div>
-
-where S is the surface tilt angle.
-
-For (DT &gt; 0.0 AND an upward facing surface)  OR  (DT &lt; 0.0 AND an downward facing surface) a reduced convection correlation is used:
-
-<div>$$h = \frac{{1.810{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{1.382 + \left| {\cos \Sigma } \right|}}$$</div>
-
-where S is the surface tilt angle.
-
-#### MoWiTT Algorithm
-
-Table 9.  Nomenclature List of Variables.
-
-<table class="table table-striped">
-<tr>
-<th>Variable</th>
-<th>Description</th>
-<th>Units</th>
-<th>Range</th>
-</tr>
-<tr>
-<td>A</td>
-<td>Constant</td>
-<td>W/(m<sup>2</sup>K(m/s)<sup>b</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>B</td>
-<td>Constant</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>C<sub>t</sub></td>
-<td>Turbulent natural convection constant</td>
-<td>W/(m<sup>2</sup>K<sup>4/3</sup>)</td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>c</sub></td>
-<td>Surface exterior convective heat transfer coefficient</td>
-<td>W/(m<sup>2</sup>K)</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sub>so</sub></td>
-<td>Outside surface temperature</td>
-<td>°C/K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>DT</td>
-<td>Temperature difference between the surface and air</td>
-<td>°C/K</td>
-<td>-</td>
-</tr>
-
-</table>
-
-
-
-The MoWiTT model is based on measurements taken at the Mobile Window Thermal Test (MoWiTT) facility (Yazdanian and Klems 1994).  The correlation applies to very smooth, vertical surfaces (e.g. window glass) in low-rise buildings and has the form:
-
-<div>$${h_c} = \sqrt {{{\left[ {{C_t}{{\left( {\Delta T} \right)}^{\frac{1}{3}}}} \right]}^2} + {{\left[ {aV_z^b} \right]}^2}} $$</div>
-
-Constants a, b and turbulent natural convection constant C<sub>t</sub> are given in Table 10.  The original MoWiTT model has been modified for use in EnergyPlus so that it is sensitive to the local suface’s wind speed which varies with the height above ground.  The original MoWiTT model was formulated for use with the air velocity at the location of the weather station.  As of Version 7.2, EnergyPlus uses the “a� model coefficients derived by Booten et al. (2012) rather than the original values from Yazdanian and Klems (1994).
-
-NOTE:  The MoWiTT algorithm may not be appropriate for rough surfaces, high-rise surfaces, or surfaces that employ movable insulation.
-
-Table 10. MoWiTT Coefficients (Yazdanian and Klems 1994, Booten et al. 2012)
-
-<table class="table table-striped">
-<tr>
-<th>Wind Direction</th>
-<th>Ct</th>
-<th>a</th>
-<th>b</th>
-</tr>
-<tr>
-<td>(Units)</td>
-<td>W/m<sup>2</sup>K<sup>4/3</sup></td>
-<td>W/m<sup>2</sup>K(m/s)<sup>b</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>Windward</td>
-<td>0.84</td>
-<td>3.26</td>
-<td>0.89</td>
-</tr>
-<tr>
-<td>Leeward</td>
-<td>0.84</td>
-<td>3.55</td>
-<td>0.617</td>
-</tr>
-
-</table>
-
-
-
-#### DOE-2 Model
-
-Table 11.  Nomenclature List of Variables.
-
-<table class="table table-striped">
-<tr>
-<th>Variable</th>
-<th>Description</th>
-<th>Units</th>
-<th>Range</th>
-</tr>
-<tr>
-<td>a</td>
-<td>Constant</td>
-<td>W/(m<sup>2</sup>K(m/s)<sup>b</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>b</td>
-<td>Constant</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>c</sub></td>
-<td>Surface exterior convective heat transfer coefficient</td>
-<td>W/(m<sup>2</sup>K)</td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>c,glass</sub></td>
-<td>Convective heat transfer coefficient for very smooth surfaces (glass)</td>
-<td>W/(m<sup>2</sup>K)</td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>n</sub></td>
-<td>Natural convective heat transfer coefficient</td>
-<td>W/(m<sup>2</sup>K)</td>
-<td>-</td>
-</tr>
-<tr>
-<td>R<sub>f</sub></td>
-<td>Surface roughness multiplier</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sub>so</sub></td>
-<td>Outside surface temperature</td>
-<td>°C/K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>DT</td>
-<td>Temperature difference between the surface and air,</td>
-<td>°C/K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>f</td>
-<td>Angle between the ground outward normal and the surface outward normal</td>
-<td>radian</td>
-<td>-</td>
-</tr>
-
-</table>
-
-##### 
-
-The DOE-2 convection model is a combination of the MoWiTT and BLAST Detailed convection models (LBL 1994). The convection coefficient for very smooth surfaces (e.g. glass) is calculated as:
-
-<div>$${h_{c,glass}} = \sqrt {h_n^2 + {{\left[ {aV_z^b} \right]}^2}} $$</div>
-
-h<sub>n</sub> is calculated using Equation or Equation .  Constants a and b are given in Table 10.
-
-For less smooth surfaces, the convection coefficient is modified according to the equation
-
-<div>$${h_c} = {h_n} + {R_f}({h_{c,glass}} - {h_n})$$</div>
-
-where R<sub>f</sub> is the roughness multiplier given by Table 8.
-
-#### Adaptive Convection Algorithm
-
-This algorithm has a structure that allows for finer control over the models used for particular surfaces.  The algorithm for the outside face was developed for EnergyPlus but it borrows concepts and its name from the research done by Beausoleil-Morrison (2000, 2002) for convection at the inside face (see the description below for interior convection).
-
-The adaptive convection algorithm implemented in EnergyPlus for the outside face is much simpler than that for the inside face. The surface classification system has a total of 4 different categories for surfaces that depend on current wind direction and heat flow directions.  However it is more complex in that the *h<sub>c</sub>* equation is split into two parts and there are separate model equation selections for forced convection, *h<sub>f</sub>*, and natural convection, *h<sub>n</sub>*. The following table summarizes the categories and the default assignments for *h<sub>c</sub>* equations. The individual *h<sub>c</sub>* equations are documented below.
-
-Table 12. Adaptive Convection Algorithm Details
-
-<table class="table table-striped">
-<tr>
-<th>#</th>
-<th>Surface Classifi-cation</th>
-<th>Heat Flow Direction</th>
-<th>Wind Direct-ion</th>
-<th>h<sub>f</sub>  Models</th>
-<th>h<sub>n</sub> Models</th>
-</tr>
-<tr>
-<td>1</td>
-<td>Roof Stable</td>
-<td>Down</td>
-<td>Any</td>
-<td>TARPWindward MoWiTTWindward DOE2Windward NusseltJurges BlockenWindward EmmelRoof ClearRoof</td>
-<td>WaltonStableHorizontalOrTilt AlamdariStableHorizontal</td>
-</tr>
-<tr>
-<td>2</td>
-<td>Roof Unstable</td>
-<td>Up</td>
-<td>Any</td>
-<td>TARPWindward MoWiTTWindward DOE2Windward NusseltJurges BlockenWindward EmmelRoof ClearRoof</td>
-<td>WaltonUnstableHorizontalOrTilt AlamdariUnstableHorizontal</td>
-</tr>
-<tr>
-<td>3</td>
-<td>Vertical Wall Windward</td>
-<td>Any</td>
-<td>Windward</td>
-<td>TARPWindward DOE2Windward MoWiTTWindward NusseltJurges McAdams Mitchell BlockenWindward EmmelVertical</td>
-<td>ASHRAEVerticalWall AlamdariHammondVerticalWall FohannoPolidoriVerticalWall ISO15099Windows</td>
-</tr>
-<tr>
-<td>4</td>
-<td>Vertical Wall Leeward</td>
-<td>Any</td>
-<td>Leeward</td>
-<td>TARPLeeward MoWiTTLeeward DOE2Leeward EmmelVertical NusseltJurges McAdams Mitchell</td>
-<td>ASHRAEVerticalWall AlamdariHammondVerticalWall FohannoPolidoriVerticalWall ISO15099Windows</td>
-</tr>
-
-</table>
-
-
-
-##### Outside Face Surface Classification
-
-During an initial setup phase, all the heat transfer surfaces in the input file are analyzed in groups to determine appropriate values for geometry scales used in many of the convection correlations.  Eight separate groups are assembled for nominally vertical exterior surfaces for eight bins of azimuth: north, northeast, east, southeast, south, southwest, west, northwest.  Surfaces with the same range of azimuth are grouped together and analyzed for overall geometry parameters.  A ninth group is assembled for nominally horizontal exterior surfaces for a roof bin that is also analyzed for geometry.  These geometry routines find bounds and limits of all the surfaces in the group and then model geometric parameters from these limits.
-
-##### Sparrow Windward
-
-As discussed above for the TARP algorithm, a Sparrow et al. (1979) conducted flat plate measurements and develop the following correlation for finite-size flat plates oriented to windward.
-
-<div>$${h_f} = 2.53{R_f}{\left( {\frac{{P{V_z}}}{A}} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 2}}\right.}\!\lower0.7ex\hbox{$2$}}}}$$</div>
-
-##### Sparrow Leeward
-
-Sparrow et al. (1979) conducted flat plate measurements and develop the following correlation for finite-size flat plates oriented to leeward.
-
-<div>$${h_f} = \frac{{2.53}}{2}{R_f}{\left( {\frac{{P{V_z}}}{A}} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 2}}\right.}\!\lower0.7ex\hbox{$2$}}}}$$</div>
-
-##### MoWITT Windward
-
-As discussed above, Yazdanian and Klems (1994) used outdoor laboratory measurements to develop the following correlation for smooth surfaces oriented to windward. Booten et al. (2012) developed revised coefficients for use with local surface wind speeds.
-
-<div>$${h_c} = \sqrt {{{\left[ {0.84{{\left| {\Delta T} \right|}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}}} \right]}^2} + {{\left[ {2.38{\kern 1pt} {\kern 1pt} V_z^{0.89}} \right]}^2}} $$</div>
-
-This model equation is for the total film coefficient and includes the natural convection portion. Therefore it should not be used in conjunction with a second natural convection model equation.
-
-##### MoWITT Leeward
-
-Yazdanian and Klems (1994) used outdoor laboratory measurements to develop the following correlation for smooth surfaces oriented to leeward. Booten et al. (2012) developed revised coefficients for use with local surface wind speeds.
-
-<div>$${h_c} = \sqrt {{{\left[ {0.84{{\left| {\Delta T} \right|}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}}} \right]}^2} + {{\left[ {2.86{\kern 1pt} {\kern 1pt} V_z^{0.617}} \right]}^2}} $$</div>
-
-This model equation is for the total film coefficient and includes the natural convection portion. Therefore it should not be used in conjunction with a second natural convection model equation.
-
-##### Blocken
-
-Blocken et al. (2009) developed a set of correlations for windward facing outdoor surfaces using numerical methods (key: BlockenWindward).
-
-<div>$$
-  \begin{array}{lcl}
-    h_f = 4.6V^{0.89}_{10m} & : & \theta \leq 11.25 \\
-    h_f = 5.0V^{0.80}_{10m} & : & 11.25 &lt; \theta \leq 33.75 \\
-    h_f = 4.6V^{0.84}_{10m} & : & 33.75 &lt; \theta \leq 56.25 \\
-    h_f = 4.5V^{0.81}_{10m} & : & 56.25 &lt; \theta \leq 100.0
-  \end{array}
-$$</div>
-
-Where *V<sub>10m</sub>* is the air velocity at the location of the weather station and θ is the angle of incidence between the wind and the surface in degrees.  This model is only applicable to windward surfaces and lacks a natural convection component and therefore cannot be used on its own but only within the adaptive convection algorithm for the outside face.
-
-##### Clear
-
-Clear et al. (2003) developed correlations from measurements for horizontal roofs on two commercial buildings. In EnergyPlus the implementation uses the model for natural convection plus turbulent forced convection (eq. 8A in the reference) and applies it to the center point of each surface section that makes up the roof.
-
-<div>$${h_c} = \eta \frac{k}{{{L_n}}}0.15Ra_{{L_n}}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}} + \frac{k}{x}{R_f}0.0296{\mathop{\rm Re}\nolimits}_x^{{\raise0.7ex\hbox{$4$} \!\mathord{\left/ {\vphantom {4 5}}\right.}\!\lower0.7ex\hbox{$5$}}}{\Pr ^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}}$$</div>
-
-Where
-
-* *x* is the distance to the surface centroid from where the wind begins to intersect the roof. In EnergyPlus this is currently simplified to half the square root of the roof surface.
-
-* <span>\({L_n} = \frac{{Area}}{{Perimeter}}\)</span> of overall roof
-
-* <span>\(k\)</span> is the thermal conductivity of air
-
-* <span>\(\eta  = \frac{ln\left(1+\frac{Gr_{L,x}}{Re_x^2}\right)} {1+ln\left(1+\frac{Gr_{L,x}}{Re_x^2}\right)} is the weighting factor for natural convection (suppressed at high forced convection rates)
-
-* <span>\(R{a_{{L_n}}} = G{r_{{L_n}}}\Pr \)</span> is the Rayleigh number
-
-* <span>\(G{r_{{L_n}}} = \frac{{g{\rho ^2}{L_n}^3\Delta T}}{{{T_f}{\mu ^2}}}\)</span>is the Grashof number
-
-* <span>\({{\mathop{\rm Re}\nolimits}_x} = \frac{{{V_z}\rho x}}{\mu }\)</span>is the Reynolds number at x
-
-* Pr is the Prandtl number
-
-This model only claims to be applicable to horizontal roof surfaces so it may not be applicable to tilted roofs. It combines natural and forced convection and therefore should not be used in conjunction with yet another natural convection model.
-
-##### Emmel
-
-Emmel et al. (2007) developed a set of correlations for outdoor surfaces using numerical methods.  The following equations are for vertical surfaces (key: EmmelVertical):
-
-<div>$$
-  \begin{array}{lcl}
-    h_f = 5.15V^{0.81}_{10m} & : & \theta \leq 22.5 \\
-    h_f = 3.34V^{0.84}_{10m} & : & 22.5 &lt; \theta \leq 67.5 \\
-    h_f = 4.78V^{0.71}_{10m} & : & 67.5 &lt; \theta \leq 112.5 \\
-    h_f = 4.05V^{0.77}_{10m} & : & 112.5 &lt; \theta \leq 157.5 \\
-    h_f = 3.54V^{0.76}_{10m} & : & 157.5 &lt; \theta \leq 180.0
-  \end{array}
-$$</div>
-
-Where *V<sub>10m</sub>* is the air velocity at the location of the weather station and θ is the angle of incidence between the wind and the surface in degrees.  The following equations are used for horizontal (roof) surfaces (key: EmmelRoof):
-
-<div>$$
-  \begin{array}{lcl}
-    h_f = 5.11V^{0.78}_{10m} & : & \theta \leq 22.5 \\
-    h_f = 4.60V^{0.79}_{10m} & : & 22.5 &lt; \theta \leq 67.5 \\
-    h_f = 3.67V^{0.85}_{10m} & : & 67.5 &lt; \theta \leq 90
-  \end{array}
-$$</div>
-
-Where θ is the angle of incidence between the wind and the longest edge of the roof surface in degrees.
-
-This model is for all wind directions but lacks a natural convection component.  The model was developed for simple, rectangular low-rise buildings.  It is available only within the adaptive convection algorithm for the outside face
-
-##### Nusselt Jurges
-
-Perhaps the oldest equation for wind-driven convection was developed by Nusselt and Jurges (1922).  Palyvos (2008) casts their model in simplified form in SI units as:
-
-<div>$${h_c} = 5.8 + 3.94\;{V_z}$$</div>
-
-Where *V<sub>z</sub>* is the wind velocity in m/s, in EnergyPlus that velocity is adjusted for height above ground using the z axis coordinate of the surface’s centroid and the site wind model.  This model can be applied to all surfaces and the relatively large constant is assumed to represent the natural convection portion of a total convection coefficient.  The model is not sensitive to wind direction nor surface roughness.
-
-##### McAdams
-
-A venerable equation for wind-driven convection was developed by McAdams (1954) which Palyvos (2008) casts in SI units as:
-
-<div>$${h_c} = 5.7 + 3.8\;{V_z}$$</div>
-
-Where *V<sub>z</sub>* is the wind velocity in m/s that has been adjusted for height above ground using the z axis coordinate of the surface’s centroid.  This model can be applied to all surfaces and the relatively large constant is assumed to represent the natural convection portion of a total convection coefficient.  The model is not sensitive to wind direction nor surface roughness.
-
-##### Mitchell
-
-A useful geometric scale based on building volume is used in an equation developed by Mitchell (1976).  The wind-driven convection equation is cast by Palyvos as:
-
-<div>$${h_f} = \frac{{8.6\;V_z^{0.6}}}{{{L^{0.4}}}}$$</div>
-
-Where *V<sub>z</sub>* is the wind velocity in m/s that has been adjusted for height above ground using the z axis coordinate of the surface’s centroid and *L* is the cube root of the building’s total volume. EnergyPlus interprets this as the sum of the volume of all the zones in the input file.
-
-### Exterior/External Conduction
-
-The conduction term, <span>\({q''_{ko}}\)</span><sub>,</sub> can in theory be calculated using a wide variety of heat conduction formulations. Typically in EnergyPlus, the Conduction Transfer Function (CTF) method is used. The available models are described in this section: Conduction Through The Walls.
-
-### References
-
-ASHRAE. 1981. 1981 ASHRAE Handbook – Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 1989. 1989 ASHRAE Handbook – Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 1993. 1993 ASHRAE Handbook – Fundamentals, Chapter 3, Heat Transfer, I-P & S-I Editions, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2001. 2001 ASHRAE Handbook – Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2005. 2005 ASHRAE Handbook – Fundamentals, Chapter 16, Air Flow Around Buildings, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
-
-Booten, C., N. Kruis, and C. Christensen. 2012. Identifying and Resolving Issues in EnergyPlus and DOE-2 Window Heat Transfer Calculations. National Renewable Energy Laboratory. NREL/TP-5500-55787. Golden, CO.
-
-Cole, R. J., and N. S. Sturrock. 1977. The Convective Heat Exchange at the External Surface of Buildings. Building and Environment, Vol. 12, p. 207.
-
-Ellis, P.G., and P.A. Torcellini. 2005. "Simulating Tall Buildings Using EnergyPlus", Proceedings of the Ninth International IBPSA Conference, Building Simulation 2005, Montreal, Canada, August 15-18, 2005.
-
-Lawrence Berkeley Laboratory (LBL). 1994. DOE2.1E-053 source code.
-
-Sparrow, E. M., J. W. Ramsey, and E. A. Mass. 1979. Effect of Finite Width on Heat Transfer and Fluid Flow about an Inclined Rectangular Plate. Journal of Heat Transfer, Vol. 101, p. 204.
-
-U.S. Standard Atmosphere. 1976. U.S. Government Printing Office, Washington, D.C.
-
-Walton, G. N. 1981. Passive Solar Extension of the Building Loads Analysis and System Thermodynamics (BLAST) Program, Technical Report, United States Army Construction Engineering Research Laboratory, Champaign, IL.
-
-Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards.
-
-Yazdanian, M. and J. H. Klems. 1994. Measurement of the Exterior Convective Film Coefficient for Windows in Low-Rise Buildings. ASHRAE Transactions, Vol. 100, Part 1, p. 1087.
-
-Inside Heat Balance
--------------------
-
-The heart of the heat balance method is the internal heat balance involving the inside faces of the zone surfaces.  This heat balance is generally modeled with four coupled heat transfer components: 1) conduction through the building element, 2) convection to the air, 3) short wave radiation absorption and reflectance and 4) longwave radiant interchange.  The incident short wave radiation is from the solar radiation entering the zone through windows and emittance from internal sources such as lights.  The longwave radiation interchange includes the absorption and emittance of low temperature radiation sources, such as all other zone surfaces, equipment, and people.
-
-The heat balance on the inside face can be written as follows:
-
-<div>$${q''_{LWX}} + {q''_{SW}} + {q''_{LWS}} + {q''_{ki}} + {q''_{sol}} + {q''_{conv}} = 0$$</div>
-
-where:
-
-<span>\({q''_{LWX}}\)</span>= Net longwave radiant exchange flux between zone surfaces.
-
-<span>\({q''_{SW}}\)</span> = Net short wave radiation flux to surface from lights.
-
-<span>\({q''_{LWS}}\)</span>= Longwave radiation flux from equipment in zone.
-
-<span>\({q''_{ki}}\)</span> = Conduction flux through the wall.
-
-<span>\({q''_{sol}}\)</span> = Transmitted solar radiation flux absorbed at surface.
-
-<span>\({q''_{conv}}\)</span> = Convective heat flux to zone air.
-
-Each of these heat balance components is introduced briefly below.
-
-![](media/image301.png)
-
-Figure 19.  Inside Heat Balance Control Volume Diagram
-
-### Internal Long-Wave Radiation Exchange
-
-#### LW Radiation Exchange Among Zone Surfaces
-
-There are two limiting cases for internal LW radiation exchange that are easily modeled:
-
-nThe zone air is completely transparent to LW radiation.
-
-nThe zone air completely absorbs LW radiation from the surfaces within the zone.
-
-The limiting case of completely absorbing air has been used for load calculations and also in some energy analysis calculations.  This model is attractive because it can be formulated simply using a combined radiation and convection heat transfer coefficient from each surface to the zone air.  However, it oversimplifies the zone surface exchange problem, and as a result, the heat balance formulation in EnergyPlus treats air as completely transparent.  This means that it does not participate in the LW radiation exchange among the surfaces in the zone. The model, which considers room air to be completely transparent, is reasonable physically because of the low water vapor concentrations and the short mean path lengths.  It also permits separating the radiant and convective parts of the heat transfer at the surface, which is an important attribute of the heat balance method.
-
-EnergyPlus uses a grey interchange model for the longwave radiation among zone surfaces.  This model is based on the “ScriptF� concept developed by Hottel (Hottel and Sarofim, Radiative Transfer, Chapter 3, McGraw Hill, 1967).  This procedure relies on a matrix of exchange coefficients between pairs of surfaces that include all exchange paths between the surfaces.  In other words all reflections, absorptions and re-emissions  from other surfaces in the enclosure are included in the exchange coefficient, which is called ScriptF.  The major assumptions are that all surface radiation properties are grey and all radiation is diffuse.  Both assumptions are reasonable for building zone interchange.
-
- The ScriptF coefficients are developed by starting with the traditional direct radiation view factors.  In the case of building rooms and zones, there are several complicating factors in finding the direct view factors-–the main one being that the location of surfaces such as thermal mass representing furniture and partitions are not known.  The other limitation is that the exact calculation of direct view factors is computationally very intensive even if the positions of all surfaces are known. Accordingly, EnergyPlus uses a procedure to approximate the direct view factors.  The procedure has two steps:
-
-1)   Determine the total area of other surfaces “seen� by a surface.
-
-2)   Approximate the direct view factor from surface 1 to surface 2 as the ratio of the area of surface 2 to the total area “seen� by surface 1.
-
-The determination of the “seen� area has several constraints:
-
-·        No surface sees itself.
-
-·        All surfaces see thermal mass surfaces.
-
-·        No surface facing within 10 degrees of another surface is seen by the other surface.
-
-·        All surfaces see roofs, floors and ceilings (subject to the preceding facing direction constraint).
-
-Because the approximate view factors may not satisfy the basic requirements of reciprocity (two surfaces should exchange equal amounts of heat in each direction), and completeness (every surface should have a direct view factor sum of 1.0), EnergyPlus does a view factor fix operation before they are used in the ScriptF determination.  Normally both of the requirements are satisfied, but in some special situations they are not, and special rules are applied.
-
-·        If a user includes less than four surfaces in a zone, only reciprocity is enforced.
-
-·        If the area of one surface in a zone is greater than the sum of the areas of all other surfaces, reciprocity only is enforced, but sometimes, for very large surfaces, that enforcement becomes impossible, and the view factors are modified so that only the large surface is seen by very small surfaces.
-
-Warning messages are produced for both of these cases, and the results should be examined very carefully to ascertain that they are reasonable.   The suggested action for the second case (the extra-large surface) is to divide the large surface into several smaller surfaces; then the enclosure will be treated as normal.
-
-Once the ScriptF coefficients are determined, the longwave radiant exchange is calculated for each surface using:
-
-<div>$${q_{i,j}} = {A_i}{F_{i,j}}\left( {T_i^4 - T_j^4} \right)$$</div>
-
-where ***F***<sub>i,j</sub> is the ScriptF between surfaces i and j.
-
-#### Thermal Mass and Furniture
-
-Furniture in a zone has the effect of increasing the amount of surface area that can participate in the radiation and convection heat exchanges.  It also adds participating thermal mass to the zone.  These two changes both affect the response to temperature changes in the zone and also affect the heat extraction characteristics.
-
-The proper modeling of furniture is an area that needs further research, but the heat balance formulation allows the effect to be modeled in a realistic manner by including the furniture surface area and thermal mass in the heat exchange process.
-
-#### LW Radiation From Internal Sources
-
-The traditional model for this source is to define a radiative/convective split for the heat introduced into a zone from equipment.  The radiative part is then distributed over the surfaces within the zone in some prescribed manner.  This, of course, is not a completely realistic model, and it departs from the heat balance principles. However, it is virtually impossible to treat this source in any more detail since the alternative would require knowledge of the placement and surface temperatures of all equipment.
-
-### Internal Short-Wave Radiation
-
-#### SW Radiation from Lights
-
-The short wavelength radiation from lights is distributed over the surfaces in the zone in some prescribed manner.
-
-#### Transmitted Solar
-
-Transmitted solar radiation is also distributed over the surfaces in the zone in a prescribed manner.  It would be possible to calculate the actual position of beam solar radiation, but that would involve partial surface irradiation, which is inconsistent with the rest of the zone model that assumes uniform conditions over an entire surface.  The current procedures incorporate a set of prescribed distributions.  Since the heat balance approach can deal with any distribution function, it is possible to change the distribution function if it seems appropriate.
-
-#### Convection to Zone Air
-
-The convection flux is calculated using the heat transfer coefficients as follows:
-
-<span>\({q''_{conv}} = {h_c}({T_s} - {T_a})\)</span>                                                                                      (89)
-
-The inside convection coefficients (*h<sub>c</sub>*) can be calculated using one of many different models.  Currently the implementation uses coefficients based on correlations for natural, mixed, and forced convection.
-
-### Interior Conduction
-
-This contribution to the inside surface heat balance is the wall conduction term, <span>\({q''_{ki}}\)</span> shown in Equation (30).  This represents the heat transfer to the inside face of the building element. Again, a CTF formulation is used to determine this heat flux.
-
-### Interior Convection
-
-There are many different modeling options available in EnergyPlus for inside convection coefficients, *h<sub>c</sub>*.  There are four different settings to direct how EnergyPlus managers select *h<sub>c</sub>* models during a simulation.  There are numerous individual model equations for *h<sub>c</sub>* in EnergyPlus to cover different situations that arise from surface orientations, room airflow conditions, and heat flow direction.  Additionally, in many cases multiple researchers have developed competing models for the same situations that differ and there is no way to declare one is better than another.  An overall default for the simulation is selected in the “SurfaceConvectionAlgorithm:Inside� object and can be overridden by selecting a different option in a zone description.  These models are explained in the following sections. In addition to the correlation choices described below, it is also possible to override the convection coefficients on the inside of any surface by using the “SurfaceProperty:ConvectionCoefficients� object in the input file to set the convection coefficient value on the inside of any surface. The values can be specified directly or with schedules. Specific details are given in the Input Output Reference document.
-
-#### Adaptive Convection Algorithm
-
-Beausoleil-Morrison (2000, 2002) developed a methodology for dynamically managing the selection of *h<sub>c</sub>* equations called *adaptive convection algorithm*.  The algorithm is used to select among the available *h<sub>c</sub>* equations for the one that is most appropriate for a given surface at a given time.  As Beausoleil-Morrison notes, the adaptive convection algorithm is intended to be expanded and altered to reflect different classification schemes and/or new *h<sub>c</sub>* equations.  The implementation in EnergyPlus has been modified from the original in the following ways:
-
-* An input mechanism is provided (see the SurfaceConvectionAlgorithm:Inside:AdapativeModelSelections object) so that the user can customize the specific selections of *h<sub>c</sub>* equations that are applied for different flow regimes and surface orientations.  The changes apply in a general way to the entire model (but can be overridden by setting surface properties).
-
-* To avoid requiring additional user input on the position of ZoneHVAC-type equipment within a zone, there is no distinction between zones that have convective zone heater equipment located underneath the windows and those that have convective heaters located away from the windows.  This applies to the air flow regime associated with convective zone heaters.  Using Beausoleil-Morrison’s terminology, regimes B1 and B2 are combined into just one B regime.
-
-* To avoid requiring additional user input on the position of ZoneHVAC-type equipment within a zone, there is no distinction between surfaces that are directly blown on the fan and those that are away from the fan for the air flow regime associated with mechanical circulation from a zone fan (ZoneHVAC type equipment).
-
-* The correlation for horizontal free jet developed by Fisher (1995) is not used.  Ceiling diffuser models are used for all mechanical circulation from central air system.  This decision was made for two reasons: (1) to avoid requiring additional user input on the position of, and momentum generated by, air terminal units, and (2) because Fisher (1995) found that the Coanda effect is so significant that in practice a free horizontal jet is difficult to maintain and mechanical-driven room airflows generally attach to surfaces and tend to match the flow regime of a ceiling diffuser much more often than a free jet.
-
-* EnergyPlus supports arbitrary geometry so surfaces can be tilted with respect to vertical or horizontal.  Beausoleil-Morrison’s adaptive convection algorithm was originally structured to use *h<sub>c</sub>* equations that have no functional dependence on surface tilt angle.  However, tilted surfaces do perform differently than vertical or horizontal surface when buoyancy forces are significant.  Therefore, the EnergyPlus implementation expands the structure of the algorithm to include additional categories for tilted surfaces.  The *h<sub>c</sub>* equations developed by Walton (1983) are selected as the defaults for tilted surfaces because they have a functional dependence on tilt angle.
-
-* Fohanno and Polidari (2006) produced a new *h<sub>c</sub>* equation for vertical walls inside buildings with a simple buoyancy flow regime.  They used a theoretical approach based on integral formalism and uniform heat flux (rather than uniform temperature) that covers both laminar and turbulent flow situations.  In EnergyPlus, this model is selected as the default in place of the model by Alamdari and Hammond (1983) for vertical walls.
-
-* Karadag (2009) produced a new *h<sub>c</sub>* equation for ceiling surfaces that are actively chilled.  He used computation fluid dynamics and various sized rooms and temperature conditions.  In EnergyPlus, this model is selected as the default for surfaces that have active, in-ceiling cooling (in place of the model by Alamdari and Hammond (1983) for unstable ceilings).
-
-* International Standard Organization (ISO) completed Standard 15099-2003 which includes *h<sub>c</sub>* equations for the inside face of windows.  EnergyPlus strives to adhere to formal modeling Standards where possible.  Therefore the implementation includes a larger structure for the adaptive algorithm that includes additional categories for windows in all flow regimes and ISO 15099-2003 models are used as the default for windows in natural convection flow regimes.  The ISO 15099 model applies to various tilt angles.
-
-* Goldstein and Novosalec (2010) produced new *h<sub>c</sub>* equations for forced air situations with ceiling slot diffusers along perimeters with significant glazing fractions.  They used experiments with full-sized test room.  These new equations are selected as the default for windows, ceilings and floors when there is an active central air system.
-
-* Interior mass surfaces are assigned the *h<sub>c</sub>* equation that would apply (stable or unstable) to a horizontal, upward facing surface for each flow regime.
-
-* The algorithm switches between forced, mixed, and natural flow regimes by calculating the Richardson number, Ri = Gr/Re^2, for the zone.  Large values of Ri indicate buoyancy dominates, while small values indicate forced flows dominate. To distinguish between opposing Zone unit type equipment (with fans) are assumed to force air up walls, and central air type equipment (with diffusers) are assumed to force air down walls.
-
-The adaptive convection algorithm implemented in EnergyPlus for the inside face has a total of 45 different categories for surfaces and 29 different options for *h<sub>c</sub>* equation selections.  The following table summarizes the categories and the default assignments for *h<sub>c</sub>* equations.  The individual *h<sub>c</sub>* equations are documented below.
-
-<table class="table table-striped">
-  <caption>Table 13. Inside Convection Categories and Assignments</caption>
-  <tr>
-    <th>#</th>
-    <th>Zone Air Flow Regime</th>
-    <th>IB-M's #</th>
-    <th>Surface orientation and heat flow direction</th>
-    <th>Keywords for Applicable Model Equation Sources</th>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td rowspan="10">Simple Buoyancy</td>
-    <td rowspan="10">A3</td>
-    <td rowspan="3">Vertical Walls</td>
-    <td>FohannoPolidoriVerticalWall *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>AlamdariHammondVerticalWall</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>ASHRAEVerticalWall</td>
-  </tr>
-  <tr>
-    <td>2</td>
-    <td rowspan="2">Stable Horizontal</td>
-    <td>AlamdariHammondStableHorizontal *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonStableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td rowspan="2">Unstable Horizontal</td>
-    <td>AlamdariHammondUnstableHorizontal *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonUnstableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>4</td>
-    <td>Stable Tilted</td>
-    <td>WaltonStableHorizontalOrTilt *</td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>Unstable Tilted</td>
-    <td>WaltonUnstableHorizontalOrTilt *</td>
-  </tr>
-  <tr>
-    <td>6</td>
-    <td>Windows</td>
-    <td>ISO15099Windows *</td>
-  </tr>
-  <tr>
-    <td>7</td>
-    <td rowspan="17">In-floor Heating or In-ceiling Cooling</td>
-    <td rowspan="17">A1</td>
-    <td rowspan="4">Vertical Walls</td>
-    <td>KhalifaEq3WallAwayFromHeat *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>FohannoPolidoriVerticalWall</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>AlamdariHammondVerticalWall</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>ASHRAEVerticalWall</td>
-  </tr>
-  <tr>
-    <td>8</td>
-    <td rowspan="2">Stable Horizontal</td>
-    <td>AlamdariHammondStableHorizontal *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonStableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>9</td>
-    <td rowspan="3">Unstable Horizontal</td>
-    <td>KhalifaEq4CeilingAwayFromHeat *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>AlamdariHammondUnstableHorizontal</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonUnstableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>10</td>
-    <td rowspan="3">Heated Floor</td>
-    <td>AwbiHattonHeatedFloor *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonUnstableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>AlamdariHammondUnstableHorizontal</td>
-  </tr>
-  <tr>
-    <td>11</td>
-    <td rowspan="2">Chilled Ceiling</td>
-    <td>KaradagChilledCeiling *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonUnstableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>12</td>
-    <td>Stable Tilted</td>
-    <td>WaltonStableHorizontalOrTilt *</td>
-  </tr>
-  <tr>
-    <td>13</td>
-    <td>Unstable Tilted</td>
-    <td>WaltonUnstableHorizontalOrTilt *</td>
-  </tr>
-  <tr>
-    <td>14</td>
-    <td>Windows</td>
-    <td>ISO15099Windows *</td>
-  </tr>
-  <tr>
-    <td>15</td>
-    <td rowspan="12">Wall Panel Heating</td>
-    <td rowspan="12">A2</td>
-    <td rowspan="3">Vertical Walls (non-heated)</td>
-    <td>KhalifaEq6NonHeatedWalls *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>FohannoPolidoriVerticalWall</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>ASHRAEVerticalWall</td>
-  </tr>
-  <tr>
-    <td>16</td>
-    <td>Heated Wall</td>
-    <td>AwbiHattonHeatedWall *</td>
-  </tr>
-  <tr>
-    <td>17</td>
-    <td rowspan="2">Stable Horizontal</td>
-    <td>AlamdariHammondStableHorizontal *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonStableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>18</td>
-    <td rowspan="3">Unstable Horizontal</td>
-    <td>KhalifaEq7Ceiling *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>AlamdariHammondUnstableHorizontal</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonUnstableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>19</td>
-    <td>Stable Tilted</td>
-    <td>WaltonStableHorizontalOrTilt *</td>
-  </tr>
-  <tr>
-    <td>20</td>
-    <td>Unstable Tilted</td>
-    <td>WaltonUnstableHorizontalOrTilt *</td>
-  </tr>
-  <tr>
-    <td>21</td>
-    <td>Windows</td>
-    <td>ISO15099Windows *</td>
-  </tr>
-  <tr>
-    <td>22</td>
-    <td rowspan="14">Convective Zone Heater</td>
-    <td rowspan="14">B</td>
-    <td rowspan="5">Vertical Walls not near heater</td>
-    <td>FohannoPolidoriVerticalWall *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>KhalifaEq6NonHeatedWalls</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>KhalifaEq3WallAwayFromHeat</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>AlamdariHammondVerticalWall</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>ASHRAEVerticalWall</td>
-  </tr>
-  <tr>
-    <td>23</td>
-    <td>Vertical Walls near heater</td>
-    <td>KhalifaEq5WallNearHeat *</td>
-  </tr>
-  <tr>
-    <td>24</td>
-    <td rowspan="2">Stable Horizontal</td>
-    <td>AlamdariHammondStableHorizontal *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonStableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>25</td>
-    <td rowspan="3">Unstable Horizontal</td>
-    <td>KhalifaEq7Ceiling *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>KhalifaEq4CeilingAwayFromHeat</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonUnstableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>26</td>
-    <td>Stable Tilted</td>
-    <td>WaltonStableHorizontalOrTilt *</td>
-  </tr>
-  <tr>
-    <td>27</td>
-    <td>Unstable Tilted</td>
-    <td>WaltonUnstableHorizontalOrTilt *</td>
-  </tr>
-  <tr>
-    <td>28</td>
-    <td>Windows</td>
-    <td>ISO15099Windows *</td>
-  </tr>
-  <tr>
-    <td>29</td>
-    <td rowspan="7">Mechanical Central Air Diffuser</td>
-    <td rowspan="7">C</td>
-    <td rowspan="2">Walls</td>
-    <td>GoldsteinNovoselacCeilingDiffuserWalls *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>FisherPedersenCeilingDiffuserWalls</td>
-  </tr>
-  <tr>
-    <td>30</td>
-    <td>Ceiling</td>
-    <td>FisherPedersenCeilingDiffuserCeiling *</td>
-  </tr>
-  <tr>
-    <td>31</td>
-    <td rowspan="2">Floor</td>
-    <td>GoldsteinNovoselacCeilingDiffuserFloor *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>FisherPedersenCeilingDiffuserFloor</td>
-  </tr>
-  <tr>
-    <td>32</td>
-    <td rowspan="2">Windows</td>
-    <td>GoldsteinNovoselacCeilingDiffuserWindow *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>ISO15099Windows</td>
-  </tr>
-  <tr>
-    <td>33</td>
-    <td rowspan="9">Mechanical Zone Fan Circulation</td>
-    <td rowspan="9">D</td>
-    <td>Walls</td>
-    <td>KhalifaEq3WallAwayFromHeat *</td>
-  </tr>
-  <tr>
-    <td>34</td>
-    <td rowspan="2">Stable Horizontal</td>
-    <td>AlamdariHammondStableHorizontal *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonStableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>35</td>
-    <td rowspan="2">Unstable Horizontal</td>
-    <td>KhalifaEq4CeilingAwayFromHeat *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>WaltonUnstableHorizontalOrTilt</td>
-  </tr>
-  <tr>
-    <td>36</td>
-    <td>Stable Tilted</td>
-    <td>WaltonStableHorizontalOrTilt *</td>
-  </tr>
-  <tr>
-    <td>37</td>
-    <td>Unstable Tilted</td>
-    <td>WaltonUnstableHorizontalOrTilt *</td>
-  </tr>
-  <tr>
-    <td>38</td>
-    <td rowspan="2">Windows</td>
-    <td>GoldsteinNovoselacCeilingDiffuserWindow *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>ISO15099Windows</td>
-  </tr>
-  <tr>
-    <td>39</td>
-    <td rowspan="8">Mixed</td>
-    <td rowspan="8">E</td>
-    <td>Assisting Flow Walls</td>
-    <td>BeausoleilMorrisonMixedAssistedWall *</td>
-  </tr>
-  <tr>
-    <td>40</td>
-    <td>Opposing Flow Walls</td>
-    <td>BeausoleilMorrisonMixedOpposingWall *</td>
-  </tr>
-  <tr>
-    <td>41</td>
-    <td>Stable Floor</td>
-    <td>BeausoleilMorrisonMixedStableFloor *</td>
-  </tr>
-  <tr>
-    <td>42</td>
-    <td>Unstable Floor</td>
-    <td>BeausoleilMorrisonMixedUnstableFloor *</td>
-  </tr>
-  <tr>
-    <td>43</td>
-    <td>Stable Ceiling</td>
-    <td>BeausoleilMorrisonMixedStableCeiling *</td>
-  </tr>
-  <tr>
-    <td>44</td>
-    <td>Unstable Ceiling</td>
-    <td>BeausoleilMorrisonMixedUnstableCeiling *</td>
-  </tr>
-  <tr>
-    <td>45</td>
-    <td rowspan="2">Windows</td>
-    <td>GoldsteinNovoselacCeilingDiffuserWindow *</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>ISO15099Windows</td>
-  </tr>
-</table>
-
-\*Indicates the default selection for *h<sub>c</sub>* model equation.
-
-#### Inside Face Surface Classification
-
-The adaptive convection algorithm is based on classifying surfaces by flow regime and orientation so that the correct *h<sub>c</sub>* equation can be chosen at a particular point in time during the simulation.  The classification depends on user input with some aspects processed only once at the beginning and others during each timestep.  There are also various parameters or inputs to the *h<sub>c</sub>* equations that need static or dynamic processing.
-
-For each surface, it and the zone it is attached to are processed for the following static characteristics.
-
-* Characteristic height for convection is taken as the zone height.
-
-* Surfaces listed as receiving heat from Zone HVAC equipment with radiative models are considered “near� the heater.
-
-* Zones are examined for low temperature radiant systems.  The surfaces that contain the active elements are examined and the zone characterized to know if it has in-floor heating, in-ceiling cooling, or in-wall heating.
-
-* A hydraulic diameter is calculated for horizontal surfaces for the entire zone.
-
-and calculating various parameters needed by *h<sub>c</sub>* equations.  Selecting flow regime is done in the following manner.  For each surface, we examine the zone on the inside face for the following:
-
-* HVAC system type
-
-* HVAC operating status
-
-* HVAC system ACH
-
-The surfaces are evaluated to determine:
-
-* Surface classification: Floor, wall, roof, window, types
-
-* Tilt angle
-
-* Convective stability (sign of ΔT)
-
-The individual *h<sub>c</sub>* model equations and their respective references are listed in next by the keyword used to identify them.
-
-#### ASHRAE Vertical Wall
-
-Walton adopted the following equation for natural convection from ASHRAE .
-
-<div>$$h = 1.31{\left| {\Delta T} \right|^{\frac{1}{3}}}$$</div>
-
-This is usually bound at a minimum of .1 in EnergyPlus. This is a component of the TARP overall algorithm described below.
-
-#### Walton Unstable Horizontal Or Tilt
-
-Walton (11983) developed the following equation by fitting curves from various sources.
-
-<div>$$h = \frac{{9.482{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{7.283 - \left| {\cos \Sigma } \right|}}$$</div>
-
-Unstable refers to the direction of heat flow and the associated buoyancy relative to the surfaces. Unstable is when the natural tendency is to enhance flow in the sense that rising warmer air, or falling cooler air, is free to move away from the surface. This is usually bound at a minimum of .1 in EnergyPlus. This is a component of the TARP overall algorithm described below.
-
-#### Walton Stable Horizontal Or Tilt
-
-Walton (11983) developed the following equation by fitting curves from various sources.
-
-<div>$$h = \frac{{1.810{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{1.382 + \left| {\cos \Sigma } \right|}}$$</div>
-
-Stable refers to the direction of heat flow and the associated buoyancy relative to the surfaces. Stable is when the natural tendency is to retard flow in the sense that rising warmer air, or falling cooler air, is driven against the surface. This is usually bound at a minimum of .1 in EnergyPlus. This is a component of the TARP overall algorithm described below.
-
-#### Fisher Pedersen Ceiling Diffuser Walls
-
-Fisher and Pedersen 1997) developed the following equation from laboratory chamber measurements.
-
-<div>$$h = 1.208 + 1.012 * AC{H^{0.604}}$$</div>
-
-This is a component of the CeilingDiffuser overall algorithm described below.
-
-#### Fisher Pedersen Ceiling Diffuser Ceiling
-
-Fisher and Pedersen (1997) developed the following equation from laboratory chamber measurements.
-
-<div>$$h = 2.234 + 4.099 * AC{H^{0.503}}$$</div>
-
-This is a component of the CeilingDiffuser overall algorithm described below.
-
-#### Fisher Pedersen Ceiling Diffuser Floor
-
-Fisher and Pedersen 1997) developed the following equation from laboratory chamber measurements.
-
-<div>$$h = 3.873 + 0.082 * AC{H^{0.98}}$$</div>
-
-This is a component of the CeilingDiffuser overall algorithm described below.
-
-#### Alamdari Hammond Stable Horizontal
-
-Alamdari and Hammond (1983) developed the following correlation for horizontal surfaces in stable thermal situation.
-
-<div>$$h = 0.6{\left( {\frac{{\left| {\Delta T} \right|}}{{D_h^2}}} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{$5$}}}}$$</div>
-
-where,
-
-<span>\({D_h} = \frac{{4A}}{P}\)</span>, hydraulic diameter of horizontal surface, *A* is area (m<sup>2</sup>) and *P* is the perimeter (m) of the entire zone.
-
-#### Alamdari Hammond Unstable Horizontal
-
-Alamdari and Hammond (1983) developed the following correlation for horizontal surfaces in a buoyant thermal situation.
-
-<div>$$h = {\left\{ {{{\left[ {1.4{{\left( {\frac{{\left| {\Delta T} \right|}}{{{D_h}}}} \right)}^{^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{$4$}}}}}} \right]}^6} + {{\left[ {1.63{{\left| {\Delta T} \right|}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}}} \right]}^6}} \right\}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 6}}\right.}\!\lower0.7ex\hbox{$6$}}}}$$</div>
-
-#### Alamdari Hammond Vertical Wall
-
-Alamdari and Hammond (1983) developed the following correlation for vertical surfaces.
-
-<div>$$h = {\left\{ {{{\left[ {1.5{{\left( {\frac{{\left| {\Delta T} \right|}}{H}} \right)}^{^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{$4$}}}}}} \right]}^6} + {{\left[ {1.23{{\left| {\Delta T} \right|}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}}} \right]}^6}} \right\}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 6}}\right.}\!\lower0.7ex\hbox{$6$}}}}$$</div>
-
-where,
-
-      *H* is the characteristic height for the surface.  In EnergyPlus this is the zone’s ceiling height (which could be larger than the height of an individual surface when wall are subdivided into more than one surface).
-
-#### Khalifa Eq3 Wall Away From Heat
-
-Khalifa (1989) conducted experiments with test chambers and developed correlations for certain types of surfaces.  One of them, identified as “Equation 3� in original reference, is for convectively heated zones and applies to the inside surfaces of walls away from the heat source:
-
-<div>$$h = 2.07{\left| {\Delta T} \right|^{0.23}}$$</div>
-
-#### Khalifa Eq4 Ceiling Away From Heat
-
-Khalifa (1989) conducted experiments with test chambers and developed correlations for certain types of surfaces.  One of them, identified as “Equation 4� in original reference, is for convectively heated zones and applies to the inside surfaces of ceilings away from the heat source:
-
-<div>$$h = 2.72{\left| {\Delta T} \right|^{0.13}}$$</div>
-
-#### Khalifa Eq5 Wall Near Heat
-
-Khalifa (1989) conducted experiments with test chambers and developed correlations for certain types of surfaces.  One of them, identified as “Equation 5� in original reference, is for convectively heated zones and applies to the inside surfaces of walls near the heat source:
-
-<div>$$h = 1.98{\left| {\Delta T} \right|^{0.32}}$$</div>
-
-#### Khalifa Eq6 Non Heated Walls
-
-Khalifa (1989) conducted experiments with test chambers and developed correlations for certain types of surfaces.  One of them, identified as “Equation 6� in original reference, is for heated zones and applies to the inside surfaces of walls that are not heated:
-
-<div>$$h = 2.30{\left| {\Delta T} \right|^{0.24}}$$</div>
-
-#### Khalifa Eq7 Ceiling
-
-Khalifa (1989) conducted experiments with test chambers and developed correlations for certain types of surfaces.  One of them, identified as “Equation 7� in original reference, is for heated zones and applies to the inside surfaces of ceilings:
-
-<div>$$h = 3.10{\left| {\Delta T} \right|^{0.17}}$$</div>
-
-#### Awbi Hatton Heated Floor
-
-Awbi and Hatton (1999) conducted laboratory measurements using environmental chambers and developed the following correlation for floor surfaces that are being actively heated.
-
-<div>$$h = \frac{{2.175{{\left| {\Delta T} \right|}^{0.308}}}}{{D_h^{0.076}}}$$</div>
-
-where,
-
-<span>\({D_h} = \frac{{4A}}{P}\)</span> , hydraulic diameter of horizontal surface, *A* is area (m<sup>2</sup>) and *P* is the perimeter (m) of the entire zone (all of the adjacent floor surfaces if more than one in the zone).
-
-#### Awbi Hatton Heated Wall
-
-Awbi and Hatton (1999) developed the following correlation for wall surfaces that are being actively heated.
-
-<div>$$h = \frac{{1.823{{\left| {\Delta T} \right|}^{0.293}}}}{{D_h^{0.076}}}$$</div>
-
-where,
-
-<span>\({D_h} = \frac{{4A}}{P}\)</span> , hydraulic diameter of wall surface, *A* is area (m<sup>2</sup>) and *P* is the perimeter (m) of the entire wall (all of the adjacent wall surfaces if more than one along the wall).
-
-#### Beausoleil Morrison Mixed Assisted Wall
-
-Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for walls where the flow driving forces from mechanical forces are augmented by the driving forces from buoyancy.
-
-<div>
-$$
-h = \left( 
-\left\{
-\left[1.5\left(\frac{\left|\Delta T\right|}{H}\right)^{1/4}\right]^6 +
-\left[1.23\left|\Delta T\right|^2\right]^{1/6}
-\right\}^{1/2} + 
-\left\{
-\left[\frac{T_{surf}-T_{SAT}}{\left|\Delta T\right|}\right]
-\left[-0.199+0.190\cdot ACH^{0.8}\right]
-\right\}^3
-\right)^{1/3}
-$$
-</div>
-
-where,
-
-      *T<sub>SAT</sub>* is the supply air temperature at the diffuser.
-
-Here the reference temperature is the zone air temperature rather than the diffuser supply air temperature.
-
-#### Beausoleil Morrison Mixed Opposing Wall
-
-Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for walls where the flow driving forces from mechanical forces are opposed by the driving forces from buoyancy.
-
-<div>
-$$
-h = \max \left\{
-\begin{array}{l}
-\left(\left\{\left[1.5\left(\frac{\left|\Delta T\right|}{H}\right)^{1/4}\right]^6+\left[1.23\left|\Delta T\right|^2\right]^{1/6}\right\}^{1/2}-\left\{\left[\frac{T_{surf}-T_{SAT}}{\left|\Delta T\right|}\right]\cdot\left[-0.199+0.190\cdot ACH^{0.8}\right]\right\}^3\right)^{1/3} \\
-0.8\cdot \left\{\left[1.5\left(\frac{\left|\Delta T\right|}{H}\right)^{1/4}\right]^6+\left[1.23\left|\Delta T\right|^2\right]\right\}^{1/6} \\
-0.8\cdot \left\{\left[\frac{T_{surf}-T_{SAT}}{\left|\Delta T\right|}\right]\cdot\left[-0.199+0.190\cdot ACH^{0.8}\right]\right\}
-\end{array}
-\right.
-$$
-</div>
-
-#### Beausoleil Morrison Mixed Stable Floor
-
-Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for floors where the flow driving forces include both mechanical forces and thermally stable buoyancy.
-
-<div>$$h = {\left( {{{\left\{ {0.6 \cdot {{\left( {\frac{{\left| {\Delta T} \right|}}{{{D_H}}}} \right)}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{$5$}}}}} \right\}}^3} + {{\left\{ {\left[ {\frac{{{T_{surf}} - {T_{SAT}}}}{{\left| {\Delta T} \right|}}} \right]\cdot\left[ {0.159 + 0.116AC{H^{0.8}}} \right]} \right\}}^3}} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}}$$</div>
-
-#### Beausoleil Morrison Mixed Unstable Floor
-
-Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for floors where the flow driving forces include both mechanical forces and thermally unstable buoyancy.
-
-<div>$$h = {\left( {{{\left\{ {{{\left[ {1.4{{\left( {\frac{{\left| {\Delta T} \right|}}{{{D_h}}}} \right)}^{^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{$4$}}}}}} \right]}^6} + {{\left[ {1.63{{\left| {\Delta T} \right|}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}}} \right]}^6}} \right\}}^{{\raise0.7ex\hbox{$3$} \!\mathord{\left/ {\vphantom {3 6}}\right.}\!\lower0.7ex\hbox{$6$}}}} + {{\left\{ {\left[ {\frac{{{T_{surf}} - {T_{SAT}}}}{{\left| {\Delta T} \right|}}} \right]\cdot\left[ {0.159 + 0.116AC{H^{0.8}}} \right]} \right\}}^3}} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}}$$</div>
-
-#### Beausoleil Morrison Mixed Stable Ceiling
-
-Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for ceilings where the flow driving forces include both mechanical forces and thermally Stable buoyancy.
-
-<div>$$h = {\left( {{{\left\{ {0.6 \cdot {{\left( {\frac{{\left| {\Delta T} \right|}}{{{D_H}}}} \right)}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{$5$}}}}} \right\}}^3} + {{\left\{ {\left[ {\frac{{{T_{surf}} - {T_{SAT}}}}{{\left| {\Delta T} \right|}}} \right]\cdot\left[ { - 0.166 + 0.484AC{H^{0.8}}} \right]} \right\}}^3}} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}}$$</div>
-
-#### Beausoleil Morrison Mixed Unstable Ceiling
-
-Beausoleil-Morrison (2000) used blending techniques to combine correlations originally developed by Alamdari and Hammond (1983) and Fisher and Pedersen (1997) to create the following correlation is for ceilings where the flow driving forces include both mechanical forces and thermally unstable buoyancy.
-
-<div>
- $$
-  h = \left(
-   \left(
-    \left[
-     1.4 \left(
-      \frac{
-       \left|
-        \Delta T
-       \right|
-      }{
-       D_h
-      }
-     \right)^{1/4}
-    \right]^6 +
-    \left[
-     1.63 \left|\Delta T\right|^{1/3}
-    \right]^6
-   \right)^{3/6} +
-   \left(
-    \left[
-     \frac{
-      T_{surf}-T_{SAT}
-     }{
-      \left|\Delta T\right|
-     }
-    \right]
-    \cdot
-    \left[
-     -0.166 + 0.484 \cdot ACH^{0.8}
-    \right]
-   \right)^3
-  \right)^{1/3}
- $$
-</div>
-
-#### Fohanno Polidori Vertical Wall
-
-Fohanno and Polidori (2006) developed the following equation for *h<sub>c</sub>* for vertical walls under simple buoyancy flow conditions.
-
-<div>$$h = \left\{ \begin{array}{l}1.332{\left( {\frac{{\left| {\Delta T} \right|}}{H}} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{$4$}}}}\quad ,\quad Ra_H^* \le 6.3 \times {10^9}\\1.235{e^{\left( {0.0467H} \right)}}{\left| {\Delta T} \right|^{0.316}}\quad ,\quad Ra_H^* > 6.3 \times {10^9}\end{array} \right.$$</div>
-
-where,
-
-<div>$$Ra_H^* = \frac{{g{\beta_f}{{q''}_c}{H^4}}}{{{k_f}\nu_f^2}}{\Pr_f}$$</div>
-
-#### Karadag Chilled Ceiling
-
-Karadag (2009) used numerical methods to develop the following equation for *h<sub>c</sub>* for chilled-ceiling surfaces.
-
-<div>$$h = 3.1{\left| {\Delta T} \right|^{0.22}}$$</div>
-
-#### ISO 15099 Windows
-
-ISO Standard 15099-2003 includes the equations for *h<sub>c</sub>* for room-side of windows and surfaces with any tilt angle and heat flow direction.  The ISO 15099 correlation is for still room air angle and is determined in terms of the Nusselt number, <span>\(Nu\)</span>, where
-
-<div>$${h_i} = Nu\left( {\frac{\lambda }{H}} \right)$$</div>
-
-where,
-
-<span>\(\lambda \)</span> is the thermal conductivity of air, and
-
-<span>\(H\)</span> is the height of the window.
-
-The Rayleigh number based on height, <span>\(R{a_H}\)</span>, is calculated using,
-
-<div>$$R{a_H} = \frac{{{\rho ^2}{H^3}g\,{c_p}\left| {{T_{surf,i}} - {T_{air}}} \right|}}{{{T_{m,f}}\mu \lambda }}$$</div>
-
-where,
-
-<span>\(\rho \)</span> is the density of air
-
-<span>\(g\)</span> is the acceleration due to gravity,
-
-<span>\({c_p}\)</span> is the specific heat of air,
-
-<span>\(\mu \)</span> is the dynamic viscosity of air, and
-
-<span>\({T_{m,f}}\)</span> is the mean film temperature in Kelvin given by,
-
-<div>$${T_{m,f}} = {T_{air}} + \frac{1}{4}\left( {{T_{surf,i}} - {T_{air}}} \right)$$</div>
-
-There are four cases for the Nusselt correlation that vary by the tilt angle in degrees, <span>\(\gamma \)</span>, and are based on heating conditions.  For cooling conditions (where <span>\({T_{surf,i}} > {T_{air}}\)</span>) the tilt angle is complemented so that <span>\(\gamma  = 180 - \gamma \)</span>
-
-Case A. <span>\({0^\circ } \le \gamma  &lt; 15^\circ \)</span>
-
-<div>$$Nu = 0.13Ra_H^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}$$</div>
-
-Case B. <span>\(15^\circ  \le \gamma  \le 90^\circ \)</span>
-
-<div>$$R{a_{cv}} = 2.5 \times {10^5}{\left( {\frac{{{e^{0.72\gamma }}}}{{\sin \lambda }}} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{$5$}}}}$$</div>
-
-<div>$$Nu = 0.56{\left( {R{a_H}\sin \gamma } \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{$4$}}}};\;for\;R{a_H} \le R{a_{CV}}$$</div>
-
-<div>$$Nu = 0.13\left( {Ra_H^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}} - Ra_{CV}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}} \right) + 0.56{\left( {R{a_{CV}}\sin \gamma } \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{$4$}}}};\;R{a_H} > R{a_{CV}}$$</div>
-
-Case C. <span>\(90^\circ  &lt; \gamma  \le 179^\circ \)</span>
-
-<div>$$Nu = 0.56{\left( {R{a_H}\sin \gamma } \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{$4$}}}};\;{10^5} \le R{a_H}\sin \gamma  &lt; {10^{11}}$$</div>
-
-Case D. <span>\(179^\circ  &lt; \gamma  \le 180^\circ \)</span>
-
-<div>$$Nu = 0.58Ra_H^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{$5$}}};\;R{a_H} \le {10^{11}}$$</div>
-
-The material properties are evaluated at the mean film temperature.  Standard EnergyPlus psychrometric functions are used for <span>\(\rho \)</span> and <span>\({c_p}\)</span>.  Thermal conductivity is calculated using,
-
-<span>\(\lambda  = 2.873 \times {10^{ - 3}} + 7.76 \times {10^{ - 8}}{T_{m,f}}\)</span>.
-
-Kinematic viscosity is calculated using,
-
-<span>\(\mu  = 3.723 \times {10^{ - 6}} + 4.94 \times {10^{ - 8}}{T_{m,f}}\)</span>.
-
-This correlation depends on the surface temperature of the room-side glazing surface and is therefore included inside the window heat balance iteration loop.
-
-#### Goldstein Novoselac Ceiling Diffuser Window
-
-Goldstein and Novoselac (2010) used laboratory chamber measurements to develop convection correlations for perimeter zones with highly glazed spaces served by overhead slot-diffuser-based air systems. The following are for bare windows in such spaces.
-
-For WWR&lt;50% with window in upper part of wall:
-
-<div>$$h = 0.117{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}$$</div>
-
-For WWR&lt;50% with window in lower part of wall
-
-<div>$$h = 0.093{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}$$</div>
-
-For WWR &gt; 50%
-
-<div>$$h = 0.103{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}$$</div>
-
-Where,
-
- WWR is the window to wall ratio.
-
- *L* is the length of exterior wall with glazing in the zone.
-
- <span>\(\dot V\)</span>is the air system flow rate in m<sup>3</sup>/s.
-
-#### Goldstein Novoselac Ceiling Diffuser Walls
-
-Goldstein and Novoselac (2010) used laboratory chamber measurements to develop convection correlations for perimeter zones with highly glazed spaces served by overhead slot-diffuser-based air systems. The following are for exterior walls in such spaces.
-
-For walls located below a window
-
-<div>$$h = 0.063{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}$$</div>
-
-For walls located above a window
-
-<div>$$h = 0.093{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}$$</div>
-
-#### Goldstein Novoselac Ceiling Diffuser Floor
-
-Goldstein and Novoselac (2010) used laboratory chamber measurements to develop convection correlations for perimeter zones with highly glazed spaces served by overhead slot-diffuser-based air systems. The following is for floors in such spaces.
-
-<div>$$h = 0.048{\left( {\frac{{\dot V}}{L}} \right)^{0.8}}$$</div>
-
-Separate from the above model structure, there are also other comprehensive algorithm structures which are described below.
-
-#### TARP Algorithm
-
-The comprehensive natural convection model, accessed using the keyword “TARP,� correlates the convective heat transfer coefficient to the surface orientation and the difference between the surface and zone air temperatures (where DT = Surface Temperature - Air Temperature).  The algorithm is taken directly from Walton (1983).  Walton derived his algorithm from ASHRAE literature which can now be found for example in the ASHRAE Handbook (HoF 2001), Table 5 on p. 3.12, which gives equations for natural convection heat transfer coefficients in the turbulent range for large, vertical plates and for large, horizontal plates facing upward when heated (or downward when cooled).   A note in the text also gives an approximation for large, horizontal plates facing downward when heated (or upward when cooled) recommending that it should be half of the facing upward value.  Walton adds a curve fit as a function of the cosine of the tilt angle to provide intermediate values between vertical and horizontal.  The curve fit values at the extremes match the ASHRAE values very well.
-
-For no temperature difference OR a vertical surface the following correlation is used:
-
-<span>\(h = 1.31{\left| {\Delta T} \right|^{\frac{1}{3}}}\)</span>                                                                                             (90)
-
-For (DT &lt; 0.0 AND an upward facing surface)  OR  (DT &gt; 0.0 AND an downward facing surface) an enhanced convection correlation is used:
-
-<span>\(h = \frac{{9.482{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{7.283 - \left| {\cos \Sigma } \right|}}\)</span>                                                                                     (91)
-
-where S is the surface tilt angle.
-
-For (DT &gt; 0.0 AND an upward facing surface)  OR  (DT &lt; 0.0 AND an downward facing surface) a reduced convection correlation is used:
-
-<span>\(h = \frac{{1.810{{\left| {\Delta T} \right|}^{\frac{1}{3}}}}}{{1.382 + \left| {\cos \Sigma } \right|}}\)</span>                                                                                     (92)
-
-where S is the surface tilt angle.
-
-#### Simple Natural Convection Algorithm
-
-The simple convection model uses constant coefficients for different heat transfer configurations, using the same criteria as the detailed model to determine reduced and enhanced convection.  The coefficients are also taken directly from Walton (1983).  Walton derived his coefficients from the surface conductances for e=0.90 found in the ASHRAE Handbook (1985) in Table 1 on p. 23.2.  The radiative heat transfer component was estimated at 1.02 \* 0.9 = 0.918 BTU/h-ft2-F and then subtracted off.  Finally the coefficients were converted to SI units to yield the values below.
-
-For a vertical surface:
-
-<div>$${\rm{h  =  3}}{\rm{.076}}$$</div>
-
-For a horizontal surface with reduced convection:
-
-<div>$${\rm{h  =  0}}{\rm{.948}}$$</div>
-
-For a horizontal surface with enhanced  convection:
-
-<div>$${\rm{h  =  4}}{\rm{.040}}$$</div>
-
-For a tilted surface with reduced convection:
-
-<div>$${\rm{h  =  2}}{\rm{.281}}$$</div>
-
-For a tilted surface with enhanced convection:
-
-<div>$${\rm{h  =  3}}{\rm{.870}}$$</div>
-
-#### Ceiling Diffuser Algorithm
-
-The ceiling diffuser algorithm is based on empirical correlations developed by Fisher and Pedersen (1997).  The correlation was reformulated to use the room outlet temperature as the reference temperature.  The correlations are shown below.
-
-For Floors:
-
-<span>\(h = 3.873 + 0.082 * AC{H^{0.98}}\)</span>                                                                      (93)
-
-The correlation for floors is illustrated in the following figure:
-
-![](media/image378.png)
-
-Figure 1017.  Ceiling Diffuser Correlation for Floors
-
-For ceilings:
-
-<span>\(h = 2.234 + 4.099 * AC{H^{0.503}}\)</span>                                                                     (94)
-
-The correlation for ceilings is illustrated in the following figure:
-
-![](media/image380.png)
-
-Figure 1018.  Ceiling Diffuser Correlation for Ceilings
-
-For Walls:
-
-<span>\(h = 1.208 + 1.012 * AC{H^{0.604}}\)</span>                                                                      (95)
-
-The correlation for walls is illustrated in the following figure:
-
-![](media/image382.png)
-
-Figure 1019.  Ceiling Diffuser Correlation for Walls
-
-#### Trombe Wall Algorithm
-
-The Trombe wall algorithm is used to model convection in a "Trombe wall zone", i.e. the air space between the storage wall surface and the exterior glazing.  (See the later sections on Passive and Active Trombe Walls below for more information about Trombe walls.)  The algorithm is identical to the convection model (based on ISO 15099) used in Window5 for convection between glazing layers in multi-pane window systems.  The use of the algorithm for modeling an unvented Trombe wall has been validated against experimental data by Ellis (2003).
-
-This algorithm gives the convection coefficients for air in a narrow vertical cavity that is sealed and not ventilated.  This applies both to the air gap in between panes of a window or to the air gap between the Trombe wall glazing and the inner surface (often a selective surface).  These convection coefficients are really the only difference between a normal zone and a Trombe zone.  The rest of the zone heat balance is the same, e.g., transmitted solar, long-wave radiation between surfaces, etc.
-
-For a vertical cavity, the correlation from ISO 15099 is:
-
-<span>\({\rm{NU1 = 0}}{\rm{.0673838 R}}{{\rm{a}}^{{\textstyle{{\rm{1}} \over {\rm{3}}}}}}\)</span>                                                        for 5E4 &lt; Ra &lt; 1E6
-
-<span>\({\rm{NU1 = 0}}{\rm{.028154 R}}{{\rm{a}}^{{\rm{0}}{\rm{.4134}}}}\)</span>                                                     for 1E4 &lt; Ra &lt; 5E4
-
-<span>\({\rm{NU1 = 1 + 1}}{\rm{.7596678E - 10 R}}{{\rm{a}}^{{\rm{2}}{\rm{.2984755}}}}\)</span>                                           for Ra &lt;= 1E4
-
-<div>$${\rm{NU2}} = 0.242{\left( {{\raise0.7ex\hbox{${{\rm{Ra}}}$} \!\mathord{\left/ {\vphantom {{{\rm{Ra}}} {\rm{A}}}}\right.}\!\lower0.7ex\hbox{${\rm{A}}$}}} \right)^{0.272}}$$</div>
-
-<div>$${\rm{NU = MAX(NU1,NU2)}}$$</div>
-
-where
-
-Nu = Nusselt number
-
-Ra = Rayleigh number
-
-A = aspect ratio of cavity
-
-This is then used in EnergyPlus as follows:
-
-Net convection coefficient from glazing to wall is:
-
-<div>$${h_{net}} = {\rm{k}}\left( {{\raise0.7ex\hbox{${{\rm{NU}}}$} \!\mathord{\left/ {\vphantom {{{\rm{NU}}} {\rm{L}}}}\right.}\!\lower0.7ex\hbox{${\rm{L}}$}}} \right)$$</div>
-
-where
-
-k = conductivity of air
-
-L = air gap thickness
-
-Convection coefficient applied to each wall separately and actually used in the zone heat balance is:
-
-<div>$${h_c} = 2{h_{net}}$$</div>
-
-#### References
-
-Alamdari, F. and G.P. Hammond. 1983. Improved data correlations for buoyancy-driven convection in rooms.  Building Services Engineering Research & Technology. Vol. 4, No. 3.
-
-ASHRAE. 1985. 1985 ASHRAE Handbook – Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2001. 2001 ASHRAE Handbook – Fundamentals, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
-
-Awbi, H.B. and A. Hatton. 1999. Natural convection from heated room surfaces. Energy and Buildings 30 (1999) 233-244.
-
-Beausoleil-Morrison, I. 2000. The adaptive coupling of heat and air flow modeling within dynamic whole-building simulations. PhD. Thesis. University of Strathclyde, Glasgow, UK.
-
-Ellis, Peter G. 2003. Development and Validation of the Unvented Trombe Wall Model in EnergyPlus. Master's Thesis, University of Illinois at Urbana-Champaign.
-
-Fisher, D.E. and C.O. Pedersen. 1997. "Convective Heat Transfer in Building Energy and Thermal Load Calculations", ASHRAE Transactions, Vol. 103, Pt. 2.
-
-Fohanno, S., and G. Polidori. 2006. Modelling of natural convective heat transfer at an internal surface. Energy and Buildings 38 (2006) 548 - 553
-
-Goldstein, K. and A. Novoselac. 2010. Convective Heat Transfer in Rooms With Ceiling Slot Diffusers (RP-1416). *HVAC&R Research Journal* TBD
-
-Karadag, R. 2009. New approach relevant to total heat transfer coefficient including the effect of radiation and convection at the ceiling in a cooled ceiling room. Applied Thermal Engineering 29 (2009) 1561-1565
-
-Khalifa AJN. 1989. Heat transfer processes in buildings. Ph.D. Thesis, University of Wales College of Cardiff, Cardiff, UK.
-
-ISO. 2003. ISO 15099:2003. Thermal performance of windows, doors, and shading devices – Detailed calculations. International Organization for Standardization.
-
-Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards (now NIST). This is documentation for “TARP.�
-
-Adiabatic Boundary Conditions
------------------------------
-
-Adiabatic boundary conditions are applied to two surface types in EnergyPlus:
-
-1)   Surfaces with adiabatic outside boundary conditions
-
-2)   Internal Mass objects
-
-For both surface types, EnergyPlus will apply the same boundary conditions to each side of the construction so that there is no temperature difference across the surface. In this case, all heat transfer into the surface is a result of the dynamic response of the construction to varying inside boundary conditions. The surface will store and release heat only at the inside face of the surface (it is assumed that the outside face is not within the zone). If both faces are within the zone, this situation can be modeled either by creating another adiabatic or internal mass surface with the reverse construction, or, for symmetric constructions, simply doubling the area of the surface.
-
-Infrared Radiation Transfer Material
-------------------------------------
-
-One of the important technical features of EnergyPlus is that the fundamental zone model includes infrared (IR) radiation exchange among all surfaces within the zone. A zone can consist of a single room or multiple rooms having similar thermal characteristics. The other fundamental characteristic of a zone in EnergyPlus is that the air within the zone is modeled with the assumption that it is well-stirred, so it is characterized by a single uniform air temperature. Normally, this corresponds to the desired physical state of the air within a zone. Practically, this is accomplished with the mixing caused by the air distribution system or even with the addition of ceiling fans. However, there are situations where the well-stirred model condition does not fit the physical conditions within a space (e.g., large atria spaces, displacement ventilation systems, and under floor air distribution systems). In these cases, the air temperature varies spatially within the zone, but the surfaces in the regions that have different air temperatures still exchange IR radiation with the other surfaces in the zone, even those in regions having a different air temperature.
-
-Historically, several approaches have been taken to model such situations. They all involve unrealistically modifying the convective heat transfer characteristics within a single zone to produce reasonable total heat transfer for the zone while maintaining the zone IR radiation in its basic form. The IRT model takes a different, more fundamental approach. The space is divided into subzones, each having the basic well-stirred air model, but surfaces in these subzones are able to exchange IR radiation with other surfaces throughout the original space. Any convective air exchange between subzones is handled using the existing flexible capabilities within EnergyPlus. In other words, the subzones are standard EnergyPlus zones but they have been given the capability of allowing IR radiation to be exchanged with surfaces in adjacent zones.
-
-The IR radiation exchange is accomplished by introducing special IR Transparent (IRT) surfaces to link adjacent zones. These surfaces transmit the IR radiation incident on them to the surfaces in adjacent zone. The special surfaces have no thermal resistance, and they also have zero convective heat transfer coefficients on both sides. Consider a stratified atrium as an example. The atrium would be divided into stacked vertical zones, with each zone having the special IRT surface between it and the next lower zone. All physical surfaces in the two zones exchange radiation with the IRT surface, but it does not impede the transfer of radiation from one zone to the other. On each side it interacts as a black body surface and any radiation incident on it is absorbed. Since it has no other heat transfer mechanisms, it comes to equilibrium with zero net radiation transfer.
-
-Schematic diagrams of the application of the IRT surfaces are shown in Figure 20 and Figure 21. The first figure shows it applied between two stacked zones that could be part of an atrium. All radiation incident on the IRT in the lower and upper zone is completely absorbed by the surface. It is prevented from participating in the zone air heat balance by fixing the heat transfer coefficients on either side at zero.
-
-![IRTFig1](media/image390.png)
-
-Figure 20. Schematic View of Stacked Zones
-
-The same arrangement can be used for simulating a underfloor air distribution system (UFAD). The two zones represent the lower occupied (mixed) zone and the upper stratified zone. Since the upper zone is being modeled as a mixed EnergyPlus zone, it is not precisely the stratified zone concept. However, if a user has concern about having the entire upper part of the space at a single average temperature, the space could be modeled with two stacked upper zones. In that case the stratified temperature profile would be established by the relative size of the mixing from the convective plumes. The user would have to supply those estimates from external knowledge of the behavior of UFAD systems and plumes.
-
-![IRTFig2](media/image391.png)
-
-Figure 21. Schematic Model of a UFAD Zone
-
-### Radiation Exchange Basics
-
-The behavior of the IRT surface can be analyzed by considering three parallel black plates infinite in extent, as shown in Figure 22. The outside plates are held at two different temperatures, and the intermediate plate assumes an equilibrium temperature when the net heat flux goes to zero. All plates have black body surface characteristics.
-
-![IRTFig3](media/image392.png)
-
-Figure 22. Radiation Exchange Model
-
-The radiant exchange between surface 1 and 2 is:
-
-<div>$${q_{1 - 2}} = \sigma A\left( {T_1^4 - T_2^4} \right)$$</div>
-
-The exchange between surfaces 2 and 3 is:
-
-<div>$${q_{2 - 3}} = \sigma A\left( {T_2^4 - T_3^4} \right)$$</div>
-
-Equating heat fluxes and eliminating T<sub>2</sub> gives:
-
-<div>$${q_{1 - 3}} = \frac{\sigma }{2}A\left( {T_1^4 - T_3^4} \right)$$</div>
-
-where:
-
-q is the heat flux in W/m<sup>2</sup>
-
-σ is the Stephan Boltzman constant
-
-A is the plate area in m<sup>2</sup>, and
-
-T is the temperature in K.
-
-Equation shows that the presence of a black body surface between a source and a sink reduces the heat flux by a factor of two. The same result occurs when the IRT surface is between two zones in EnergyPlus. In that case the adjacent zones behave as black body cavities at some equivalent temperature. In order to account for this reduction, the IRT area must be doubled. This can be done without any difficulty in the EnergyPlus radiant exchange routine because the radiation view factors are determined by an approximate procedure that is based on the areas of the surfaces. Thus, doubling the surface area of the IRT surface results in the correct transfer of radiation through the IRT surface. The doubling will occur automatically in the program as described in the Input Output Reference document.
-
-It should be noted that, because of the black body behavior of the IRT surface, any visible or solar short wavelength radiation incident on the surface will be absorbed and included with the long wavelength (IR) exchange with the adjacent zone. No energy will be lost, but zones with IRT surfaces should not be used in any lighting analyses.
-
-### Radiation Transfer Surface Details
-
-#### Specifying an Infrared Transparent (IRT) surface
-
-The Infrared Transparent (IRT) surface is similar to a resistance-only surface. The idd object for this type of surface is shown below. The fields indicate that the surface will actually participate in the transfer of visible and solar radiation by doing a wavelength transformation and making all short wavelength radiation that is incident on the surface into long wavelength radiation and having it participate in the long wavelength radiant exchange. The Material:InfraredTransparent object requires only a name. All other parameters are set internally.
-
-The Infrared Transparent surface should not participate in a convective/conductive exchange between the zones it separates. In order to minimize this effect, the SurfaceProperty:ConvectionCoefficients object must be used. Outside and Inside values for the surface’s convection coefficients should be on the order of .1.  Further examples are given in the Input Output Reference document.
-
-### Behavior Checks
-
-The behavior of multi zones separated with infrared transparent surfaces can be checked with a simple comparison. Begin with a single zone model as shown below. This model has a south-facing window, and four walls exposed to wind and sun, and a roof exposed to wind and sun.
-
-![SingleZoneDrawing](media/image396.png)
-
-Figure 23. Single Zone Model
-
-The single zone model will be compared with a stacked three zone model that has zones separated by interzone infrared transparent surfaces. This model is shown below.
-
-![ThreeZone-bldgAreaSE-2](media/image397.png)
-
-Figure 24. Stacked Three Zone Model
-
-The two upper zones have south facing windows whose total area is the same as the area of the single window in the single zone model. The top and the sides are again exposed to sun and wind. The separating surfaces are modeled as IRT surfaces. All zones in both models are controlled at the same setpoint temperature using purchased air.
-
-The sensible heating results are shown below. The results show the sum of the sensible cooling load for the three stacked zones and the single zone. It is clear that the IRT surfaces are very effective in transmitting infrared radiation between the zones. Some small differences, such as those shown, will occur because of the conversion from short wavelength solar to infrared through the special IRT dividing surfaces.
-
-
-
-![Comparison of single and three stacked zones](media/image398.png)
-
-Figure 25. Comparison of Single and Three Stacked Zones
-
-Transparent Insulation Material (TIM)
--------------------------------------
-
-### Introduction
-
-The input object “SurfaceControl:MovableInsulation� allows modeling Transparent Insulation Materials (TIM) that were originally designed for use in solar collector systems, where there was a need to increase the insulation in the solar collector without dramatically reducing solar energy transmittance.  Transparent Insulation provides both these properties, insulation from heat loss and transmittance of solar energy.  The combination of these properties is achieved, because Transparent Insulation is a transmitter of short wave radiation but a barrier to longwave radiation.  Therefore short wave solar radiation passes through the Transparent Insulation and longwave heat radiation is insulated by the transparent insulation. Incident solar energy falling on the transparent insulation is reflected and re-reflected within the material and eventually falls on the absorber.  In addition, transparent insulation materials also have increase thermal resistance due to conduction in comparison to standard glass.
-
-Transparent Insulation is now used in the housing industry as a passive solar feature. It is attached to the walls of houses for insulation and solar energy gains are transmitted to the house during the right ambient conditions. The walls of the house act as a thermal mass, absorbing the sunlight at the surface and converting it into heat which is slowly transmitted to the inside of the house.
-
-### Comparison of Opaque and Transparent Insulation
-
-A qualitative comparison between the performance of Transparent Insulation and opaque insulation is shown diagrammatically in the figure below. The upper half of the figure represents approximate heat transfer through the wall cross-section for both transparent and opaque insulation cases.  The lower half of this figure shows representative temperature variations through the wall cross-sections for different solar conditions.
-
-![](media/image399.png)
-
-Figure 26.  Energy Flows of Opaquely and Transparently Insulated Walls (Wood and Jesch 1993).
-
-While both types of insulation reduce energy losses from the building via conduction through the building surfaces, transparent insulation allows solar radiation to penetrate deeper into the surface construction.  This increases the construction internal temperature and can result in heat being conducted into the building under the proper weather conditions.  This can be seen in the lower half of the above figure during a sunny day.  The temperature plot shows a maximum between the transparent insulation and the rest of the surface construction.  As a result, the temperature gradient results in heat transfer from this point into the interior space, causing a heating effect on the zone.  Thus, the advantage of transparent insulation is that, like opaque insulation, it reduces winter heat transfer losses during low or no solar conditions and has the possibility of providing heating during sunny winter days.  It should be noted that this same effect in summer could be detrimental to the cooling loads of a building since the introduction of solar radiation closer to the space will increase the solar heating within the zone.  Most systems counteract this with a shading device or with sophisticated transparent insulation systems.
-
-### Types of Transparent Insulation Materials
-
-Transparent insulation can be classified into four general categories:
-
-Absorber Parallel Covers
-
-Cavity Structures
-
-Absorber Vertical Covers
-
-Quasi-Homogeneous Structures
-
-Cross-sections of each of these types is shown in the figure below.  The arrows in these diagrams indicate solar rays and the path these rays trace as they are transmitted through the transparent insulation layer.  The most advantageous set-up (see absorber-parallel below) would send most of the rays downward towards the interior of the building while minimizing the rays that are reflected back to the exterior environment.
-
-![](media/image400.png)
-
-Figure 27.  Geometrical Categories of Classification for Transparent Insulation Material (Wood and Jesch 1993).
-
-### TIM- Basic Mathematical Model
-
-![](media/image401.png)
-
-Figure 28.  Cross Section of TIM and wall, showing energy flow
-
-Mathematical model to calculate amount of energy absorbed at the surface of moveable insulation (TIM) and at the Outside surface of the Wall.
-
-<div>$$QSM = {\alpha_{TIM}}\cdot Incident\;Solar$$</div>
-
-The total solar gain on any exterior surface is a combination of the absorption of direct and diffuse solar radiation given by
-
-***<span>\(Incident\;Solar = ({I_b}\cdot \cos \theta \cdot \frac{{{S_s}}}{S} + {I_s}\cdot {F_{ss}} + {I_g}\cdot {F_{sg}})\)</span>                                      ***
-
-Where,
-
-a<sub>       </sub> = solar absorptance of the surface
-
-<span>\(\theta \)</span>   = angle of incidence of the sun’s rays
-
-S<sub>       </sub> = area of the surface
-
-S<sub>s     </sub> = sunlit area of the surface
-
-I<sub>b        </sub> = intensity of the beam (direct) radiation
-
-I<sub>s        </sub> = intensity of the sky diffuse radiation
-
-I<sub>g       </sub> = intensity of the beam (direct) radiation
-
-F<sub>ss   </sub> = angle factor between the surface and the sky
-
-F<sub>sg   </sub> = angle factor between the surface and the ground
-
-Now,
-
-<div>$${\alpha_{wall}} + {\rho_{wall}} = 1$$</div>
-
-The model for TIM is simplified in that it assumes that absorption of solar radiation takes place at the inside and outside of the TIM only, not throughout the material.  In addition, the model assumes that the solar radiation absorbed during the first pass through the TIM affects the outside surface of the TIM while the solar radiation reflected at the outer wall surface that gets absorbed during the back reflection will affect the inside TIM surface (which is also the outside surface of the wall).  Thus, the heat absorbed at the outside of the TIM is as shown in Equation .
-
-The heat absorbed at the inside of the TIM/outside of the wall includes two components.  The first component is the amount of solar that is transmitted through the TIM and absorbed at the inside of the wall.  This is characterized by the following equation:
-
-<div>$$First\,pass\,solar\,absorbed\,by\,wall = \left( {{\tau_{TIM}}\cdot Incident\,Solar} \right)\cdot \left( {{\alpha_{wall}}} \right)$$</div>
-
-The amount of solar absorbed by the TIM and aggregated at the inside surface of the TIM (outside wall surface) is:
-
-<div>$$Amount\,of\,back\,reflection\,absorbed\,by\,TIM = \left( {{\tau_{TIM}}\cdot Incident\,Solar} \right)\cdot \left( {1 - {\alpha_{wall}}} \right)\cdot {\alpha_{TIM}}$$</div>
-
-The heat absorbed at the interface between the wall and the TIM includes both of these components.  Thus, QSO is equal to:
-
-<div>$$QSO = \left( {{\tau_{TIM}}\cdot Incident\,Solar} \right)\cdot \left\{ {{\alpha_{wall}} + \left( {1 - {\alpha_{wall}}} \right)\cdot \alpha {}_{TIM}} \right\}$$</div>
-
-Substituting the definition for QSM into this equation and rearranging results in:
-
-<div>$$QSO = \left\{ {\frac{{{\tau_{TIM}}\cdot QSM}}{{{\alpha_{TIM}}}}} \right\}\cdot \left\{ {{\alpha_{wall}} + \left( {1 - {\alpha_{wall}}} \right)\cdot {\alpha_{TIM}}} \right\}$$</div>
-
-<div>$$QSO = \left( {{\tau_{TIM}}\cdot QSM} \right)\cdot \left\{ {\left( {\frac{{{\alpha_{wall}}}}{{{\alpha_{TIM}}}}} \right) + \left( {1 - {\alpha_{wall}}} \right)} \right\}$$</div>
-
-Where,
-
-*QSM*           = Short wave radiant flux absorbed at surface of Movable Insulation
-
-*QSO*           = Short wave radiant flux absorbed at surface of Wall.
-
-a<sub>TIM                        </sub> = Absorptance of TIM
-
-t<sub>TIM                         </sub> = Transmittance of TIM.
-
-a<sub>WALL                     </sub> = Absorptance of Wall.
-
-r <sub>WALL                   </sub> = Reflectance of Wall surface
-
-Following is the FORTRAN Code used in the HeatBalanceSurfaceManager module, to determine the short wave radiation absorbed on outside of movable insulation and the short wave radiation absorbed on outside of opaque surface of the wall.
-
-IF (Surface(SurfNum)%MaterialMovInsulExt.GT.0)                                     &
-
-    CALL EvalOutsideMovableInsulation(SurfNum,HMovInsul,RoughIndexMovInsul,AbsExt)
-
-    IF (HMovInsul &gt; 0) THEN    ! Movable outside insulation in place
-
-      QRadSWOutMvIns(SurfNum) = QRadSWOutAbs(SurfNum)\*AbsExt          &
-
-                       /Material(Construct(ConstrNum)%LayerPoint(1))%AbsorpSolar
-
-!  For Transparent Insulation
-
-      QRadSWOutAbs(SurfNum) = Material(Surface(SurfNum)%MaterialMovInsulExt)%Trans  &
-
-             \*QRadSWOutMvIns(SurfNum)\*                              &
-
-                 (  (Material(Construct(ConstrNum)%LayerPoint(1))%AbsorpSolar/AbsExt)   &
-
-                        +(1-Material(Construct(ConstrNum)%LayerPoint(1))%AbsorpSolar)  )
-
-### Sample Test Run Cases: – Comparison
-
-A series of test cases were run in EnergyPlus to test the TIM model.  The building was a very simple box with walls facing north, south, east, and west, all of which are exterior walls.  Transparent Insulation Material has been applied to the south wall (except as noted in the table below).  The program was run for this fictional 1 zone building located in Chanute AFB IL, for two design days, (21<sup>st</sup> June and 21<sup>st</sup> January).  The main purpose of these runs was to verify that the transparent insulation model was predicting results that were reasonable using a simple test case.  The winter design day was also modified in some runs to have a clearness of 1.0 so that the effect that solar radiation during winter-time conditions could be studied.
-
-The Transparent Insulation material is conceived by applying a SurfaceControl:MoveableInsulation on the exterior.  In the test cases, the TIM had the following thermal properties:
-
-    0.05, ! Thickness {m}
-
-    0.90,  ! Solar transmittance at normal incidence
-
-    0.031,  ! Solar reflectance at normal incidence: front side
-
-    0.031,  ! Solar reflectance at normal incidence: back side
-
-    0.90,  ! Visible transmittance at normal incidence
-
-    0.05,  ! Visible reflectance at normal incidence: front side
-
-    0.05,  ! Visible reflectance at normal incidence: back side
-
-    0.0,   ! IR transmittance at normal incidence
-
-    0.84,  ! IR emissivity: front side
-
-    0.84,  ! IR emissivity: back side
-
-    0.04;   ! Conductivity {W/m-K}
-
-The Wall Construction is defined as an EXTWALL80 composed of 1� Stucco, 4� Common Brick and ¾� Plaster or Gypboard.
-
-The following two tables shows data for two series of runs.  The first “summer table� illustrates the execution of a summer design day.  The second “winter table� shows winter conditions with clearness=0 (the typical default for a winter design day) and clearness=1 (to illustrate solar radiation with other winter conditions).  Test cases included no movable insulation, moveable opaque insulation, and TIM on the exterior (south wall unless otherwise noted).  Savings reported are heating and cooling loads for the design days only.  The results showed that the TIM model was performing reasonably well and was producing results that were within expectations.
-
-
-
-
-
-Table 14.  TIM with Summer Conditions
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Conductivity</th>
-<th>Thick-ness.</th>
-<th>Sensible</th>
-<th>Energy Saved</th>
-</tr>
-<tr>
-<td>EXTWALL80 Construction</td>
-<td> </td>
-<td> </td>
-<td>Cooling Energy</td>
-<td> </td>
-</tr>
-<tr>
-<td> </td>
-<td>[W/m-K]</td>
-<td>[m]</td>
-<td>[J]</td>
-<td>[J]</td>
-</tr>
-<tr>
-<td>Normal case
-Without any Insulation</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>3.37E+08</td>
-<td>0.00E+00</td>
-</tr>
-<tr>
-<td>With Dense Insulation Present</td>
-<td>0.040</td>
-<td>0.025</td>
-<td>3.17E+08</td>
-<td>2.05E+07</td>
-</tr>
-<tr>
-<td>With Dense Insulation Present</td>
-<td>0.040</td>
-<td>0.050</td>
-<td>3.09E+08</td>
-<td>2.84E+07</td>
-</tr>
-<tr>
-<td>With Dense Insulation Present</td>
-<td>0.040</td>
-<td>0.100</td>
-<td>3.02E+08</td>
-<td>3.53E+07</td>
-</tr>
-<tr>
-<td>With TIM Present</td>
-<td>0.040</td>
-<td>0.025</td>
-<td>4.27E+08</td>
-<td>-9.01E+07</td>
-</tr>
-<tr>
-<td>With TIM Present</td>
-<td>0.040</td>
-<td>0.050</td>
-<td>4.63E+08</td>
-<td>-1.26E+08</td>
-</tr>
-<tr>
-<td>With TIM Present</td>
-<td>0.040</td>
-<td>0.100</td>
-<td>4.89E+08</td>
-<td>-1.52E+08</td>
-</tr>
-<tr>
-<td>With TIM Present -R value =
-( 0.05m,0.04W/m-K)</td>
-<td>0.035</td>
-<td>0.044</td>
-<td>4.63E+08</td>
-<td>-1.26E+08</td>
-</tr>
-<tr>
-<td>With TIM Present
-(EAST WALL)</td>
-<td>0.040</td>
-<td>0.050</td>
-<td>5.49E+08</td>
-<td>-2.12E+08</td>
-</tr>
-<tr>
-<td>With TIM Present
-(NORTH WALL)</td>
-<td>0.040</td>
-<td>0.050</td>
-<td>3.63E+08</td>
-<td>-2.57E+07</td>
-</tr>
-<tr>
-<td>With TIM Present
-(WEST WALL)</td>
-<td>0.040</td>
-<td>0.050</td>
-<td>5.64E+08</td>
-<td>-2.27E+08</td>
-</tr>
-
-</table>
-
-
-
-Table 15. TIM with Winter Conditions
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Conduc-tivity</th>
-<th>Thick-ness.</th>
-<th>Sensible</th>
-<th>Energy Saved</th>
-<th>Sensible</th>
-<th> Energy Saved</th>
-</tr>
-<tr>
-<td>EXTWALL80 Construction</td>
-<td> </td>
-<td> </td>
-<td>Heating Energy</td>
-<td>Winter Clear-ness=0</td>
-<td>Heating Energy</td>
-<td>Winter Clear-ness=1</td>
-</tr>
-<tr>
-<td> </td>
-<td>[W/m-K]</td>
-<td>[m]</td>
-<td>[J]</td>
-<td>[J]</td>
-<td>[J]</td>
-<td>[J]</td>
-</tr>
-<tr>
-<td>Normal case
-Without any Insulation</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>1.47E+09</td>
-<td>0.00E+00</td>
-<td>1.05E+09</td>
-<td>0.00E+00</td>
-</tr>
-<tr>
-<td>With Dense Insulation Present</td>
-<td>0.040</td>
-<td>0.025</td>
-<td>1.30E+09</td>
-<td>1.70E+08</td>
-<td>9.76E+08</td>
-<td>7.40E+07</td>
-</tr>
-<tr>
-<td>With Dense Insulation Present</td>
-<td>0.040</td>
-<td>0.050</td>
-<td>1.26E+09</td>
-<td>2.10E+08</td>
-<td>9.73E+08</td>
-<td>7.70E+07</td>
-</tr>
-<tr>
-<td>With Dense Insulation Present</td>
-<td>0.040</td>
-<td>0.100</td>
-<td>1.22E+09</td>
-<td>2.50E+08</td>
-<td>9.74E+08</td>
-<td>7.60E+07</td>
-</tr>
-<tr>
-<td>With TIM Present</td>
-<td>0.040</td>
-<td>0.025</td>
-<td>1.30E+09</td>
-<td>1.70E+08</td>
-<td>5.66E+08</td>
-<td>4.84E+08</td>
-</tr>
-<tr>
-<td>With TIM Present</td>
-<td>0.040</td>
-<td>0.050</td>
-<td>1.26E+09</td>
-<td>2.10E+08</td>
-<td>4.41E+08</td>
-<td>6.09E+08</td>
-</tr>
-<tr>
-<td>With TIM Present</td>
-<td>0.040</td>
-<td>0.100</td>
-<td>1.22E+09</td>
-<td>2.50E+08</td>
-<td>3.57E+08</td>
-<td>6.93E+08</td>
-</tr>
-<tr>
-<td>With TIM Present -R value =
-( 0.05m,0.04W/m-K)</td>
-<td>0.035</td>
-<td>0.044</td>
-<td>1.26E+09</td>
-<td>2.10E+08</td>
-<td>4.40E+08</td>
-<td>6.10E+08</td>
-</tr>
-<tr>
-<td>With TIM Present
-(EAST WALL)</td>
-<td>0.040</td>
-<td>0.050</td>
-<td>1.26E+09</td>
-<td>2.10E+08</td>
-<td>7.36E+08</td>
-<td>3.14E+08</td>
-</tr>
-<tr>
-<td>With TIM Present
-(NORTH WALL)</td>
-<td>0.040</td>
-<td>0.050</td>
-<td>1.24E+09</td>
-<td>2.30E+08</td>
-<td>8.31E+08</td>
-<td>2.19E+08</td>
-</tr>
-<tr>
-<td>With TIM Present
-(WEST WALL)</td>
-<td>0.040</td>
-<td>0.050</td>
-<td>1.24E+09</td>
-<td>2.30E+08</td>
-<td>7.07E+08</td>
-<td>3.43E+08</td>
-</tr>
-
-</table>
-
-
-
-### References
-
-P.O. Braun, A. Goetzberger, J. Schmid, and W.Stahl. Transparent Insulation of Building Facades- Steps from Research to Commercial applications, Fraunhofer Institute for Solar Energy Systems, Oltmannsstrasse 22, D-7800 Freiburg, Germany.
-
-Thermotropic materials and Systems for Overheating Protection.
-
-Robert Hausner. Arbeitsgemeinschaft Erneuerbare energie, Transparent Insulation- Areas of Application, Society for Renewable Energy.
-
-Werner J.Platzer. Transparent Insulation materials: a review, Fraunhofer Institute for Solar Energy Systems, Oltmannsstr. 5, D-79100 Freiburg, Germany.
-
-Volker Wittwer. The use of Transparent Insulation Materials and Optical Switching Layers in Window Systems, Fraunhofer Institute for Solar Energy Systems, Oltmannsstr. 5, D-79100 Freiburg, Germany.
-
-M. Wood and L.F. Jesch. 1993. Transparent insulation technology: a technical note, Ambient Press Limited.
-
-Façade Modules with back-ventilated Transparent Insulation- Research and Development toward Series Application.
-
-Two 0-Energy Houses,
-
-Advanced Building Technologies – Transparent Insulation Materials ( TIM ).
-
-Transparent Insulation,
-
-G. Verbeeck, H. Hens. Transparent Insulation: an alternative solution for summer discomfort. Die neue Transparenz: Warmedamm-Verbund- system StoTherm Solar.
-
-E.Lindauer, H.Leonhardt. Brauchwasservorerwarmmung mit transparent gedammten Bauteilen ( Hybridsystem ), Fraunhofer- Institut fur Bauphysik.
-
-Surface Heat Balance With Moveable Insulation
----------------------------------------------
-
-### Basic Heat Balance Cases
-
-A heat balance must exist at the outside surface-air interface. The incoming conductive, convective, and radiative fluxes must sum up to zero:
-
-<div>$$Conductive + Convective + Radiative = 0$$</div>
-
-In contrast to the internal surface heat balance that treats all surfaces simultaneously, the external thermal balance for each surface is performed independent of all other surfaces. This implies that there is no direct interaction between the individual surfaces.
-
-TARP includes four possible representations for the basic outside surface heat balance. The first two depend on which of the optimal surface conductance algorithms the user selects. The simple outside surface conductance that includes both the convective and thermal interchange between the surface and the environment in a single coefficient, is represented by the thermal network in Figure 29. Equation can also be expressed as:
-
-<div>$$\left[ {{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {{\rm{Y}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{I}}_t} - {{\rm{X}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{O}}_{\rm{t}}}} \right]{\rm{ + }}\left[ {{\rm{HO}}\cdot \left( {{{\rm{T}}_{\rm{a}}} - {\rm{T}}{{\rm{O}}_t}} \right)} \right]{\rm{  + QSO  =  0}}$$</div>
-
-This can be solved for the outside surface temperature.
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{\rm{t}}}{\rm{ + HO}}\cdot {{\rm{T}}_{\rm{a}}}}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HO}}}}} \right]{\rm{  }}$$</div>
-
-The detailed outside surface conductance model considers convection and radiant interchange with the sky and with the ground as separate factors. Its use in the outside thermal balance is shown in Figure 30.In this case, equation can be expanded to give
-
-<div>$$\left[ {{\rm{KO}}{{\rm{P}}_{\rm{t}}}{\rm{ + }}{{\rm{Y}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{I}}_{\rm{t}}}{\rm{ - }}{{\rm{X}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{O}}_{\rm{t}}}} \right]{\rm{ + }}\left[ {{\rm{HA}}\cdot \left( {{{\rm{T}}_{\rm{a}}}{\rm{ - T}}{{\rm{O}}_{\rm{t}}}} \right){\rm{ + HS}}\cdot \left( {{{\rm{T}}_{\rm{s}}}{\rm{ - T}}{{\rm{O}}_{\rm{t}}}} \right){\rm{ + HG}}\cdot \left( {{{\rm{T}}_{\rm{g}}}{\rm{ - T}}{{\rm{O}}_{\rm{t}}}} \right)} \right]{\rm{  + QSO  =  0  }}$$</div>
-
-This can be solved for the outside surface temperature:
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{\rm{t}}}{\rm{ + HA}}\cdot {{\rm{T}}_{\rm{a}}}{\rm{ + HS}}\cdot {{\rm{T}}_{\rm{s}}}{\rm{ + HG}}\cdot {{\rm{T}}_{\rm{g}}}}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HA + HS + HG}}}}} \right]{\rm{  }}$$</div>
-
-The third and fourth representations occur when the outside surface has been covered with movable insulation. The insulation has a conductance of UM. The thermal network in Figure 31 represents this case.The insulation must be mass-less because it is not generally possible to perform a correct thermal balance at the juncture of two surfaces each modeled by CTF.
-
-The equation for the thermal balance between the surface and the insulation is
-
-<div>$$\left[ {{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {{\rm{Y}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{I}}_t} - {{\rm{X}}_{\rm{0}}}\cdot {\rm{T}}{{\rm{O}}_{\rm{t}}} + {\rm{UM}}\cdot \left( {{\rm{TM - T}}{{\rm{O}}_{\rm{t}}}} \right)} \right]{\rm{ + QSO  =  0}}$$</div>
-
-Which can be rewritten to solve for TO :
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{\rm{t}}}{\rm{ + UM}}\cdot {\rm{TM}}}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + UM}}}}} \right]{\rm{  }}$$</div>
-
-Depending on whether or not the detailed or simple algorithm for surface conductance is being used, there are two expressions for TM, the outside temperature of the insulation. For the simple conductance:
-
-<div>$${\rm{TM}} = \left[ {\frac{{{\rm{QSM + UM}}\cdot {\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ + HO}}\cdot {{\rm{T}}_{\rm{a}}}}}{{{\rm{UM + HO}}}}} \right]$$</div>
-
-For the detailed conductance:
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{QSM}} + {\rm{UM}}\cdot {\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ + HA}}\cdot {{\rm{T}}_{\rm{a}}}{\rm{ + HS}}\cdot {{\rm{T}}_{\rm{s}}}{\rm{ + HG}}\cdot {{\rm{T}}_{\rm{g}}}}}{{{\rm{UM + HA + HS + HG}}}}} \right]{\rm{  }}$$</div>
-
-In this case the values of HA, HS and HG must be found by using an estimated value of TM in place of TO.
-
-
-
-![](media/image420.png)
-
-Figure 29.  Thermal Network for Simple Outside Surface Coefficient
-
-![](media/image421.png)
-
-Figure 30.  Thermal Network for Detailed Outside Surface Coefficient
-
-![](media/image422.png)
-
-Figure 31.  Thermal Network for Outside Moveable Insulation
-
-### Heat Balance Cases
-
-TO<sub>t</sub> and TI<sub>t  </sub> are related through the Y<sub>0</sub> CTF<sub>. </sub> However TI<sub>t  </sub> is also unknown. While it is possible to combine the outside and the inside surface heat balances to compute TO<sub>t</sub> and TI<sub>t  </sub> simultaneously, TARP uses a simpler procedure where TO<sub>t </sub> is based on a previous value of TI. When Y<sub>0</sub> is small, as occurs in well insulated or very massive surfaces, TI<sub>t  </sub> can be replaced by TI<sub>t\\ -1  </sub> (which is known for the previous hour’s heat balance) without significantly effecting the value of TO<sub>t\\ . </sub> When Y<sub>0</sub> is large, TO and TI can so strongly be coupled that separate outside and inside heat balances do not work because the environment and zone temperatures have negligible influence on the heat balances. The TARP uses the inside surface heat balance to couple TO<sub>t  </sub> with TZ and TR. These two temperatures are less strongly influenced by TO and allow a reasonable heat balance. On the first heat balance iteration, TZ and TR are the values at time t-1. The user may optionally require that TO<sub>t </sub> be recomputed with every iteration of TI<sub>t \\ .</sub>  In this case TZ and TR have values from the previous iteration and a true simultaneous solution is achieved. In most conventional constructions, recomputing TO<sub>t</sub> does not significantly change the computed zone loads and temperatures. The inside surface heat balance is given by
-
-<div>$${\rm{T}}{{\rm{I}}_{\rm{t}}} = \left[ {\frac{{KI{P_t} + QSI + HC\cdot TZ + HR\cdot TR + {Y_0}\cdot TO}}{{{Z_0} + HC + HR}}} \right]$$</div>
-
-The surface heat balances can be combined in eight ways according to conditions for calculations of the outside surface temperature
-
-<div>$${F_1} = \left[ {\frac{{{Y_0}}}{{{Z_0} + HI + HR}}} \right]$$</div>
-
-<div>$${F_2} = \left[ {\frac{{UM}}{{UM + HO}}} \right]$$</div>
-
-<div>$${F_3} = \left[ {\frac{{UM}}{{UM + HA + HS + HG}}} \right]$$</div>
-
-#### Case1: Y<sub>0</sub>  small, simple conductance, no movable insulation:
-
-From Equation
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{{\rm{t - 1}}}}{\rm{ + HO}}\cdot {{\rm{T}}_{\rm{a}}}}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HO}}}}} \right]{\rm{  }}$$</div>
-
-#### Case2: Y<sub>0</sub> not small, simple conductance, no movable insulation:
-
-From Equations and
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {\rm{HO}}\cdot {{\rm{T}}_{\rm{a}}} + {{\rm{F}}_1}\cdot \left( {{\rm{KI}}{{\rm{P}}_{\rm{t}}}{\rm{ + QSI + HI}}\cdot {\rm{TZ + HR}}\cdot {\rm{TR}}} \right)}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HO - }}{{\rm{F}}_{\rm{1}}}\cdot {{\rm{Y}}_0}}}} \right]{\rm{  }}$$</div>
-
-#### Case3: Y<sub>0</sub>  small, detailed conductance, no movable insulation:
-
-From Equation
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{{\rm{t - 1}}}}{\rm{ + HA}}\cdot {{\rm{T}}_{\rm{a}}} + {\rm{HS}}\cdot {{\rm{T}}_{\rm{s}}} + {\rm{HG}}\cdot {{\rm{T}}_{\rm{g}}}}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HA + HS + HG}}}}} \right]{\rm{  }}$$</div>
-
-#### Case4: Y<sub>0</sub> not small, detailed conductance, no movable insulation:
-
-From Equations and
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {\rm{HA}}\cdot {{\rm{T}}_{\rm{a}}} + {\rm{HS}}\cdot {{\rm{T}}_{\rm{s}}} + {\rm{HG}}\cdot {{\rm{T}}_{\rm{g}}} + {{\rm{F}}_{\rm{1}}}\cdot \left( {{\rm{KI}}{{\rm{P}}_{\rm{t}}}{\rm{ + QSI + HI}}\cdot {\rm{TZ + HR}}\cdot {\rm{TR}}} \right)}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + HA + HS + HG - }}{{\rm{F}}_1}\cdot {{\rm{Y}}_0}}}} \right]{\rm{  }}$$</div>
-
-#### Case5: Y<sub>0</sub>  small, simple conductance, with movable insulation:
-
-From Equations and
-<span>\(
-  TO_t = \left[ \frac{ KOP_t + QSO + HA \cdot T_a + HS \cdot T_s + HG \cdot T_g + F_1 \cdot \left( KIP_t QS1 + HI \cdot TZ + HR \cdot TR \right) } { X_0 + HA + HS + HG - F_1 \cdot Y_0 } \right]
-\)</span>
-
-#### Case6: Y<sub>0</sub> not small, simple conductance, with movable insulation:
-
-From Equations , and
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{F}}_2}\cdot \left( {{\rm{QSM + HO}}\cdot {{\rm{T}}_{\rm{a}}}} \right) + {{\rm{F}}_1}\cdot \left( {{\rm{KI}}{{\rm{P}}_{\rm{t}}}{\rm{ + QSI + HI}}\cdot {\rm{TZ + HR}}\cdot {\rm{TR}}} \right)}}{{{{\rm{X}}_{\rm{0}}} + {\rm{UM - }}{{\rm{F}}_{\rm{2}}}\cdot {\rm{UM - }}{{\rm{F}}_{\rm{1}}}\cdot {{\rm{Y}}_{\rm{0}}}}}} \right]{\rm{  }}$$</div>
-
-#### Case7: Y<sub>0</sub>  small, detailed conductance, with movable insulation:
-
-From Equations and
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{Y}}_0}\cdot {\rm{T}}{{\rm{I}}_{{\rm{t - 1}}}}{\rm{ + }}{{\rm{F}}_{\rm{3}}}\left( {{\rm{QSM + HA}}\cdot {{\rm{T}}_{\rm{a}}}{\rm{ + HS}}\cdot {{\rm{T}}_{\rm{s}}}{\rm{ + HG}}\cdot {{\rm{T}}_{\rm{g}}}} \right)}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + UM - }}{{\rm{F}}_{\rm{3}}}\cdot {\rm{UM}}}}} \right]{\rm{  }}$$</div>
-
-#### Case8: Y<sub>0</sub> not small, detailed conductance, with movable insulation:
-
-From Equations , and
-
-<div>$${\rm{T}}{{\rm{O}}_{\rm{t}}}{\rm{ = }}\left[ {\frac{{{\rm{KO}}{{\rm{P}}_{\rm{t}}} + {\rm{QSO}} + {{\rm{F}}_1}\cdot \left( {{\rm{KI}}{{\rm{P}}_{\rm{t}}}{\rm{ + QSI + HI}}\cdot {\rm{TZ + HR}}\cdot {\rm{TR}}} \right){\rm{ + }}{{\rm{F}}_{\rm{3}}}\left( {{\rm{QSM + HA}}\cdot {{\rm{T}}_{\rm{a}}}{\rm{ + HS}}\cdot {{\rm{T}}_{\rm{s}}}{\rm{ + HG}}\cdot {{\rm{T}}_{\rm{g}}}} \right)}}{{{{\rm{X}}_{\rm{0}}}{\rm{ + UM - }}{{\rm{F}}_{\rm{3}}}\cdot {\rm{UM - }}{{\rm{F}}_{\rm{1}}}\cdot {{\rm{Y}}_{\rm{0}}}}}} \right]{\rm{  }}$$</div>
-
-### Fortran Algorithm Examples
-
-#### Case5: Y<sub>0</sub>  small, simple conductance, with movable insulation:
-
-From Equation
-
-! Outside heat balance case: Movable insulation, slow conduction, simple convection
-
- F2 = DBLE(HmovInsul) / ( DBLE(HmovInsul) + DBLE(HExtSurf(SurfNum)) )
-
- TH(SurfNum,1,1) = (-CTFConstOutPart(SurfNum)  &
-
-                    +DBLE(QRadSWOutAbs(SurfNum) )  &
-
-           +Construct(ConstrNum)%CTFCross(0)\*TempSurfIn(SurfNum)  &
-
-           +F2\* ( DBLE(QRadSWOutMvIns(SurfNum))                   &
-
-           + DBLE(HExtSurf(SurfNum))\* DBLE(TempExt) )   )         &
-
-           /( Construct(ConstrNum)%CTFOutside(0) + DBLE(HmovInsul) &
-
-          - F2\* DBLE(HMovInsul))
-
-#### Case6: Y<sub>0</sub> not small, simple conductance, with movable insulation:
-
-From Equation
-
-! Outside heat balance case: Movable insulation, quick conduction, simple convection
-
-F2 = DBLE(HmovInsul) / ( DBLE(HmovInsul) + DBLE(HExtSurf(SurfNum)) )
-
-TH(SurfNum,1,1) = (-CTFConstOutPart(SurfNum)             &
-
-+ DBLE(QRadSWOutAbs(SurfNum))                            &
-
-+F2\*( DBLE(QRadSWOutMvIns(SurfNum))                      &
-
-+DBLE(HExtSurf(SurfNum))\* DBLE(TempExt)  )               &
-
-+F1\*( CTFConstInPart(SurfNum)                            &
-
-+ DBLE(QRadSWInAbs(SurfNum))                             &
-
-+ DBLE(QRadThermInAbs(SurfNum))                          &
-
-+ DBLE(HConvIn(SurfNum))\*MAT(ZoneNum)                    &
-
-+ DBLE(NetLWRadToSurf(SurfNum))  ) )                     &
-
-/( Construct(ConstrNum)%CTFOutside(0) + DBLE(HmovInsul)  &
-
--F2\* DBLE(HMovInsul )- F1\*Construct(ConstrNum)%CTFCross(0) )
-
-#### Case7: Y<sub>0</sub>  small, detailed conductance, with movable insulation:
-
-From Equation
-
-! Outside heat balance case: Movable insulation, slow conduction, detailed convection
-
-F2 = DBLE(HMovInsul)/ ( DBLE(HMovInsul) + DBLE(HExtSurf(SurfNum)) &
-
-           +DBLE(HSky) + DBLE(HGround) )
-
-TH(SurfNum,1,1) = (-CTFConstOutPart(SurfNum)                      &
-
-+DBLE(QRadSWOutAbs(SurfNum))                                      &
-
-+Construct(ConstrNum)%CTFCross(0)\*TempSurfIn(SurfNum)             &
-
-+F2\*( DBLE(QRadSWOutMvIns(SurfNum))                               &
-
-+DBLE(HExtSurf(SurfNum))\*DBLE(TempExt)                            &
-
-+DBLE(HSky)\*DBLE(SkyTemp)                                         &
-
-+DBLE(HGround)\*DBLE(OutDryBulbTemp) ) )                           &
-
-/( Construct(ConstrNum)%CTFOutside(0)                             &
-
-+DBLE(HMovInsul) - F2\*DBLE(HMovInsul) )
-
-#### Case8: Y<sub>0</sub> not small, detailed conductance, with movable insulation:
-
-From Equation
-
-! Outside heat balance case: Movable insulation, quick conduction, detailed convection
-
-F2 = DBLE(HMovInsul)/ ( DBLE(HMovInsul) + DBLE(HExtSurf(SurfNum)) &
-
-           +DBLE(HSky) + DBLE(HGround) )
-
-TH(SurfNum,1,1) = (-CTFConstOutPart(SurfNum)                      &
-
-+DBLE(QRadSWOutAbs(SurfNum))                                      &
-
-+F1\*( CTFConstInPart(SurfNum)                                     &
-
-+DBLE(QRadSWInAbs(SurfNum))                                       &
-
-+DBLE(QRadThermInAbs(SurfNum))                                    &
-
-+DBLE(HConvIn(SurfNum))\*MAT(ZoneNum)                              &
-
-+DBLE(NetLWRadToSurf(SurfNum)) )                                  &
-
-+F2\*( DBLE(QRadSWOutMvIns(SurfNum))                               &
-
-+DBLE(HExtSurf(SurfNum))\*DBLE(TempExt)                            &
-
-+DBLE(HSky)\*DBLE(SkyTemp)                                         &
-
-+DBLE(HGround)\*DBLE(OutDryBulbTemp) )                             &
-
-/( Construct(ConstrNum)%CTFOutside(0)                             &
-
-+DBLE(HMovInsul) - F2\*DBLE(HMovInsul)                             &
-
--F1\*Construct(ConstrNum)%CTFCross(0)   )
-
-
-
-### Fortran Variable Descriptions
-
-Table 16.  Fortran Variables and Descriptions
-
-<table class="table table-striped">
-<tr>
-<th>FORTRAN Variable</th>
-<th>Description</th>
-<th>Tarp Variable</th>
-<th>Units</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>TH(SurfNum,1,1)</td>
-<td>Temperature History(SurfNum,Hist Term,In/Out), where: Hist Term (1 = Current Time, 2-MaxCTFTerms = previous times), In/Out (1 = Outside, 2 = Inside)</td>
-<td>TO<sub>t</sub></td>
-<td>C</td>
-<td>Temperature of outside of surface I at time t</td>
-</tr>
-<tr>
-<td>Construct(ConstrNum)%CTFCross(0)</td>
-<td>Cross or Y term of the CTF equation</td>
-<td>Y0</td>
-<td>W/m<sup>2</sup>K</td>
-<td>Cross CTF term</td>
-</tr>
-<tr>
-<td>Construct(ConstrNum)%CTFInside(0)</td>
-<td>Inside or Z terms of the CTF equation</td>
-<td>Z0</td>
-<td>W/m<sup>2</sup>K</td>
-<td>Inside CTF term</td>
-</tr>
-<tr>
-<td>Construct(ConstrNum)%CTFOutside(0)</td>
-<td>Outside or X terms of the CTF equation</td>
-<td>X0</td>
-<td>W/m<sup>2</sup>K</td>
-<td>Outside CTF term</td>
-</tr>
-<tr>
-<td>CTFConstInPart(SurfNum)</td>
-<td>Constant inside portion of the CTF calculation</td>
-<td>KIP<sub>t</sub></td>
-<td>W/m<sup>2</sup></td>
-<td>Portion of inward conductive flux based on previous temperature and flux history terms</td>
-</tr>
-<tr>
-<td>CTFConstOutPart(SurfNum)</td>
-<td>Constant Outside portion of the CTF calculation</td>
-<td>KOP<sub>t</sub></td>
-<td>W/m<sup>2</sup></td>
-<td>Portion of outward conductive flux based on previous temperature and flux history terms</td>
-</tr>
-<tr>
-<td>F1, F2, F3</td>
-<td>Intermediate calculation variables</td>
-<td>F1, F2, F3</td>
-<td> </td>
-<td>Radiation interchange factor between surfaces</td>
-</tr>
-<tr>
-<td>GroundTemp</td>
-<td>Ground surface temperature</td>
-<td>T<sub>g</sub></td>
-<td>C</td>
-<td>Temperature of ground at the surface exposed to the outside environment</td>
-</tr>
-<tr>
-<td>HConvIn(SurfNum)</td>
-<td>Inside convection coefficient</td>
-<td>HI</td>
-<td>W/m<sup>2</sup>K</td>
-<td>Inside convection coefficient</td>
-</tr>
-<tr>
-<td>HExtSurf(SurfNum)</td>
-<td>Outside Convection Coefficient</td>
-<td>HO, HA</td>
-<td>W/m<sup>2</sup>K</td>
-<td>Overall outside surface conductance</td>
-</tr>
-<tr>
-<td>HGround</td>
-<td>Radiant exchange (linearized) coefficient</td>
-<td>HG</td>
-<td>W/m<sup>2</sup>K</td>
-<td>Radiative conductance (outside surface to ground temperature</td>
-</tr>
-<tr>
-<td>HmovInsul</td>
-<td>Conductance or &quot;h&quot; value of movable insulation</td>
-<td>UM</td>
-<td>W/m<sup>2</sup>K</td>
-<td>Conductance of Movable insulation</td>
-</tr>
-<tr>
-<td>HSky</td>
-<td>Radiant exchange (linearized) coefficient</td>
-<td>HS</td>
-<td>W/m<sup>2</sup>K</td>
-<td>Radiative conductance (outside surface to sky radiant temperature</td>
-</tr>
-<tr>
-<td>MAT(ZoneNum)</td>
-<td>Zone temperature</td>
-<td>TZ</td>
-<td>C</td>
-<td>Temperature of zone air</td>
-</tr>
-<tr>
-<td>NetLWRadToSurf(SurfNum)</td>
-<td>Net interior longwave radiation to a surface from other surfaces</td>
-<td>HR*TR</td>
-<td>W/m<sup>2</sup></td>
-<td>Net surface to surface radiant exchange</td>
-</tr>
-<tr>
-<td>QRadSWInAbs(SurfNum)</td>
-<td>Short-wave radiation absorbed on inside of opaque surface</td>
-<td>QSI</td>
-<td>W/m<sup>2</sup></td>
-<td>Short wave radiant flux absorbed at inside of surface</td>
-</tr>
-<tr>
-<td>QRadSWOutAbs(SurfNum)</td>
-<td>Short wave radiation absorbed on outside opaque surface</td>
-<td>QSO</td>
-<td>W/m<sup>2</sup></td>
-<td>Short wave radiant flux absorbed at outside of surface</td>
-</tr>
-<tr>
-<td>QRadSWOutMvIns(SurfNum)</td>
-<td>Short wave radiation absorbed on outside of movable insulation</td>
-<td>QSM</td>
-<td>W/m<sup>2</sup></td>
-<td>Short wave radiant flux absorbed at surface of movable insulation</td>
-</tr>
-<tr>
-<td>QRadThermInAbs(SurfNum)</td>
-<td>Thermal Radiation absorbed on inside surfaces</td>
-<td> </td>
-<td>W/m<sup>2</sup></td>
-<td>Longwave radiant flux from internal gains</td>
-</tr>
-<tr>
-<td>SkyTemp</td>
-<td>Sky temperature</td>
-<td>T<sub>s</sub></td>
-<td>C</td>
-<td>Sky temp</td>
-</tr>
-<tr>
-<td>TempExt</td>
-<td>Exterior surface temperature or exterior air temperature</td>
-<td>TM, T<sub>a</sub></td>
-<td>C</td>
-<td>Temperature of external surface of movable insulation or outside ambient air temperature</td>
-</tr>
-<tr>
-<td>TempSurfIn(SurfNum)</td>
-<td>Temperature of inside surface for each heat transfer surface</td>
-<td>TI<sub>t-1</sub></td>
-<td>C</td>
-<td>Temperature of inside of surface I at time t-1</td>
-</tr>
-
-</table>
-
-
-
-### References
-
-Walton, G.N. 1983. “The Thermal Analysis Research Program Reference Manual Program (TARP)�, National Bureau of Standards (now National Institute of Standards and Technology).
-
-Ground Heat Transfer Calculations using C and F Factor Constructions
---------------------------------------------------------------------
-
-Building energy code and standards like ASHRAE 90.1, 90.2 and California Title 24 require the underground wall constructions and slabs-on-grade or underground floors not to exceed certain maximum values of C-factor and F-factor, which do not specify detailed layer-by-layer materials for the constructions. If using the normal approach (layer by layer) of ground constructions with EnergyPlus, users would need to create a pseudo wall or floor construction to match the thermal performance such as thermal mass effect and U-factor, and rely on the EnergyPlus Basement and Slabs tools to generate the monthly ground temperatures.
-
-A simplified approach is introduced to create equivalent constructions and model the ground heat transfer through underground walls and ground floors for the building energy code compliance calculations. The approach is to create constructions based on the user defined C or F factor with two layers: one concrete layer (0.15 m thick) with thermal mass, and one fictitious insulation layer with no thermal mass.
-
-Three objects are used in the C and F factor calculations:
-
-* Construction:CfactorUndergroundWall
-
-* Construction:FfactorGroundFloor
-
-* Site:GroundTemperature:FCfactorMethod
-
-Site:GroundTemperature:FCfactorMethod is used only by the underground walls or slabs-on-grade or underground floors defined with C-factor (Construction:CfactorUndergroundWall) and F-factor (Construction:FfactorGroundFloor) method for code compliance calculations where detailed construction layers are unknown. Only one such ground temperature object can be included. The monthly ground temperatures for this object are close to the monthly outside air temperatures delayed by three months. If user does not input this object in the IDF file, it will be defaulted to the 0.5m set of monthly ground temperatures from the weather file if they are available.
-
-Detailed description of the three objects is in the Input Output Reference document. The following section describes how the equivalent material layers are created based on the C-factor and F-factor.
-
-#### Slab-on-grade and Underground Floors Defined with F-factors
-
-The steady state heat transfer through the floor is calculated as,
-
-Q = Area \* U<sub>eff</sub> \* (T<sub>air,out</sub> – T<sub>air,in</sub>) = (T<sub>air,out</sub> – T<sub>air,in</sub>) \* (P<sub>exp</sub> \* F-factor)
-
-Where,
-
-Q is the steady state heat transfer through the floor in Watt
-
-Area is the area of the floor in m<sup>2</sup>
-
-U<sub>eff</sub> is the effective heat transfer coefficient including the floor construction, the soil, and the thermal resistance of the interior and exterior air films.
-
-T<sub>air,in</sub> is the indoor air temperature in °C
-
-T<sub>air,out</sub> is the outside air temperature in °C
-
-P<sub>exp</sub> is the exposed perimeter of the floor in m
-
-F-Factor is the heat transfer through the floor, induced by a unit temperature difference between the outside and inside air temperature, on the per linear length of the exposed perimeter of the floor. The unit is W/m·K.
-
-Therefore,
-
-U<sub>eff</sub> = (P<sub>exp</sub> \* F-factor) / Area
-
-1 / U<sub>eff</sub> = R<sub>eff</sub> + R<sub>film,in</sub> + R<sub>film,\\ out</sub>
-
-R<sub>eff</sub> = Area / (P<sub>exp</sub> \* F-factor) - R<sub>film,in</sub> - R<sub>film,\\ out</sub>
-
-Where,
-
-R<sub>eff</sub> is the effective thermal resistance in m<sup>2</sup>·K/W, including the soil and the floor construction
-
-R<sub>film,in</sub> and R<sub>film,\\ out</sub> are the air film resistance of the inside and outside surfaces, respectively.
-
-The outside air film resistance R<sub>film,\\ out</sub> = 0.03 m<sup>2</sup>·K/W. The inside air film resistance R<sub>film,in</sub> = 0.125 m<sup>2</sup>·K/W, which is the average of the 0.14 m<sup>2</sup>·K/W for heat flow up and 0.11 m<sup>2</sup>·K/W for heat flow down.
-
-Approximate the thermal mass of the floor construction with a 6-inch (0.15 m) heavy concrete, and use a fictitious insulation layer with no thermal mass to match the thermal resistance of the construction.
-
-We have,
-
-R<sub>fic</sub> = R<sub>eff</sub> – R<sub>con</sub>
-
-Where,
-
-R<sub>fic</sub> is the thermal resistance of the fictitious insulation layer in m<sup>2</sup>·K/W.
-
-R<sub>con</sub> is the thermal resistance of the concrete layer in m<sup>2</sup>·K/W.
-
-Properties of the concrete layer are:
-
-Thickness = 0.15 m
-
-Conductivity = 1.95 W/m·K
-
-Density = 2240 kg/m<sup>3</sup>
-
-Specific heat = 900 J/kg·K
-
-R<sub>con</sub> = 0.15/1.95 = 0.077 m<sup>2</sup>·K/W
-
-Finally,
-
-R<sub>fic</sub> = R<sub>eff</sub> – 0.077
-
-![FCDrawing](media/image435.png)
-
-Figure 32. Schematic for Slab on Grade - Two Spaces
-
-For slabs-on-grade as shown in the figure above, the exposed perimeter is (2A + C) for the Dining area, and (2B + C) for the Kitchen area. For underground floors with no exposed perimeter, the R<sub>eff</sub> can be assumed a big value such as 1000 hr·ft<sup>2</sup>·°F/Btu (177 m<sup>2</sup>·K/W).
-
-***Underground Walls Defined with C-Factors***
-
-The steady state heat transfer through the underground wall is calculated as,
-
-Q = Area \* U<sub>eff</sub> \* (T<sub>air,out</sub> – T<sub>air,in</sub>)
-
-1 / U<sub>eff</sub> = R<sub>eff</sub> + R<sub>film,out</sub> + R<sub>film,in</sub>
-
-Where,
-
-Q is the heat transfer through the wall in Watt
-
-Area is the area of the wall in m2
-
-U<sub>eff</sub> is the effective heat transfer coefficient including the floor construction, the soil, and the thermal resistance of the interior and exterior air films.
-
-R<sub>eff</sub> is the effective thermal resistance in m<sup>2</sup>·K/W, including the soil and the wall construction
-
-R<sub>film,in</sub> and R<sub>film,\\ out</sub> are the air film resistance of the inside and outside surfaces, respectively.
-
-C-factor is the time rate of steady-state heat flow through unit area of the construction, induced by a unit temperature difference between the body surfaces. The C-Factor unit is W/m<sup>2</sup>·K. The C-factor does not include soil or air films.
-
-R<sub>eff</sub> = 1/C-factor + R<sub>soil</sub> <sub> </sub>
-
-R<sub>soil</sub> is the effective R-value of the soil. Reference values from Table C6.10.1 of the SI version of the ASHRAE Standard 90.1-2010 are as follows:
-
-Table 17. Effective R-Value of Soil for Below-Grade Walls
-
-![](media/image436.png)
-
-A fairly good linear regression (R<sup>2</sup> = 0.9967) for the above data is,
-
-R<sub>soil</sub> = 0.0607 + 0.3479 \* Depth
-
-Approximate the thermal mass of the wall construction with a 6-inch (0.15 m) heavy concrete, and use a fictitious insulation layer with no thermal mass to match the thermal resistance of the construction. Then we have the thermal resistance of the insulation layer,
-
-R<sub>fic</sub> = R<sub>eff</sub> – R<sub>con</sub>
-
-Where,
-
-R<sub>fic</sub> is the thermal resistance of the fictitious insulation layer
-
-R<sub>con</sub> is the thermal resistance of the concrete layer in m<sup>2</sup>·K/W.
-
-Properties of the concrete layer are:
-
-Thickness = 0.15 m
-
-Conductivity = 1.95 W/m·K
-
-Density = 2240 kg/m<sup>3</sup>
-
-Specific heat = 900 J/kg·K
-
-R<sub>con</sub> = 0.15/1.95 = 0.077 m<sup>2</sup>·K/W
-
-Ground Heat Transfer Calculations using Site:GroundDomain:Slab
---------------------------------------------------------------
-
-In order to simulate heat transfer with horizontal building surfaces in contact with the ground, a general finite difference ground model has been implemented. The model simulates heat transfer with the horizontal building surfaces through the ground domain. The domain can simulate heat transfer for slab-in-grade or slab-on-grade scenarios. In all scenarios, the ground domain must interact with the zone through an OthersideConditionsModel as the horizontal surface’s outside boundary condition.
-
-#### Approach
-
-This model is generalized to be able to handle a number of different slab and insulation configurations.  It uses an implicit finite difference formulation to solve for the ground temperatures. As a result the simulation is stable for all timesteps and grid sizes, but an iteration loop must be employed to converge the temperatures in the domain for each domain timestep.
-
-Multiple horizontal surfaces can be coupled to each ground domain object. The model determines which surfaces are coupled to the ground domain and creates a surface of equivalent surface area within the ground domain as a representation of the horizontal surfaces coupled to the ground domain. This surface then interacts with the ground providing updated other side conditions model temperatures to the coupled surfaces for use in their surface heat balance calculations.
-
-#### Boudary Conditions
-
-At the interface surface, the average surface conduction heat flux from all surfaces connected to the ground domain is imposed as a GroundDomain boundary condition at the Surface/GroundDomain interface cells. Far-field temperatures are applied as boundary temperature at the GroundDomain sides and lower surface. The ground temperature profile at the domain sides and lower surface are taken from Kusuda & Achenbach 1965. The correlation requires annual ground surface temperature data.
-
-Ground surface cells are treated as a heat balance, where long and short wave radiation, conduction, and convection are considered. Evapotranspiration is also considered. The evapotranspiration rate is calculated as a moisture loss by using the Allen et al. (2005) model, and translated into a heat loss by multiplication with the density and latent heat of evaporation of water. The evapotranspiration rate is dependent on the type of vegetation at the surface; the user can vary the surface vegetation from anywhere between a concrete surface and a fairly tall grass (about 7�).
-
-Once the ground model has run, the updated cells with zone surface boundary conditions will update the OtherSideConditionsModel temperatures which are the used at the next timestep in the surface heat balance calculations.
-
-#### Simulation Methodology
-
-The ground domain is updated at each zone timestep, or hourly as specified by the user. For situations when the ground domain is updated at each timestep, the domain is simulated by applying the surface heat flux boundary conditions from the previous timestep and calculating a new OthersideConditionsModeltemperature. At this point, the surface heat balance algorithms can then take the new outside surface temperatures to update their surface heat fluxes. For situations when the user has elected to have the domain update on an hourly basis, the surface heat balance for each coupled surface is aggregated and passed to the domain as an average surface heat flux from the previous hour, which will then update the outside surface temperatures for the surface heat balance’s next iteration.
-
-Both in-grade and on-grade scenarios are simulated with the GroundDomain object. The key difference being that for in-grade situations, the slab and horizontal insulation are simulated by the ground domain, whereas for the on-grade situations the slab and horizontal insulation must be included in the floor construction object. All possible insulation/slab configurations are seen in Table 18.
-
-Table 18. Possible insulation/slab configurations for Site:GroundDomain model.
-
-<table class="table table-striped">
-<tr>
-<th>Situations</th>
-<th>Vert. Ins.</th>
-<th>Horiz Ins. (Full)</th>
-<th>Horiz Ins. (Perim)</th>
-</tr>
-<tr>
-<td rowspan="6">In-Grade</td>
-<td>1</td>
-<td>X</td>
-<td></td>
-<td></td>
-</tr>
-<tr>
-<td>2</td>
-<td>X</td>
-<td>X</td>
-<td></td>
-</tr>
-<tr>
-<td>3</td>
-<td>X</td>
-<td></td>
-<td>X</td>
-</tr>
-<tr>
-<td>4</td>
-<td></td>
-<td></td>
-<td></td>
-</tr>
-<tr>
-<td>5</td>
-<td></td>
-<td>X</td>
-<td></td>
-</tr>
-<tr>
-<td>6</td>
-<td></td>
-<td></td>
-<td>X</td>
-</tr>
-<tr>
-<td rowspan="4">On-Grade</td>
-<td>7</td>
-<td>X</td>
-<td></td>
-<td></td>
-</tr>
-<tr>
-<td>8*</td>
-<td>X</td>
-<td>X</td>
-<td></td>
-</tr>
-<tr>
-<td>9</td>
-<td></td>
-<td></td>
-<td></td>
-</tr>
-<tr>
-<td>10*</td>
-<td></td>
-<td>X</td>
-<td></td>
-</tr>
-</table>
-\* Horizontal insulation must be included in the floor construction
-
-For the slab-in-grade scenarios, a thin surface layer must be included in the floor construction. This can be a very thin layer of the slab or other floor covering materials above the slab. This provides a zone boundary condition for the GroundDomain while still allowing 3-dimensional heat transfer effects to occur within the slab.
-
-#### References
-
-Kusuda, T. & Achenbach, P. 1965. Earth Temperature and Thermal Diffusivity at Selected Stations in the United States, ASHRAE Transactions 71(1): 61–75.
-
-Allen, R.G., Walter, I.A., Elliott, R.L., Howell, T.A., Itenfisu, D., Jensen, M.E., Snyder, R.L. 2005. The ASCE Standardized Reference Evapotranspiration Equation. Reston, VA: American Society of Civil Engineers.
-
-Ground Heat Transfer Calculations using Site:GroundDomain:Basement
-------------------------------------------------------------------
-
-Basement heat transfer calculations are performed by the same model used by Site:GroundDomain:Slab to simulate zone-ground coupled surfaces. To simulate basements, the previous model is extended to situations where surfaces are below ground.
-
-#### Approach
-
-This model is generalized to be able to handle several basement surface and insulation configurations. An implicit finite difference formulation is used to solve for the ground temperatures. As a result the simulation is stable for all timesteps and grid sizes, but an iteration loop must be employed to converge the temperatures in the domain for each domain timestep.
-
-Multiple basement zones can be coupled to each basement domain object. The model determines which floor surfaces are coupled to the basement domain and creates a floor surface of equivalent surface area within the basement domain as a representation of the horizontal surfaces coupled to the domain. The user defined aspect ratio, which is the ratio of basement width to length, along with the total surface area of all surfaces connected to this basement floor will define the size and shape of the basement ground domain.
-
-Vertical basement depth below the ground surface of the domain is user specified. For situations when the ground surface is lower than the first above ground level a separate surface should be employed to bridge the space between the ground domain, and the first above-ground level.
-
-Basement wall and floor surfaces are created normally using the BuildingSurface:Detailed objects, with the outside boundary condition being the OtherSideConditionsModel used for the walls and floor of the basement domain. The interface between the basement walls and floors occurs at the outside surface of the walls and floor. Outside underground insulation is simulated by the ground domain, and therefore should not be included in the basement wall and floor construction objects.
-
-#### Boundary Conditions
-
-At the zone interface surfaces, the average surface conduction heat flux from all surfaces connected to the ground domain is imposed as a boundary condition at the Surface/Domain interface cells. Far-field temperatures are applied as boundary temperature at the domain sides and lower surface. The ground temperature profile at the domain sides and lower surface are taken from Kusuda & Achenbach 1965. The correlation requires annual ground surface temperature data. Ground surface temperature data can be determined by using the CalcSoilSurfTemp preprocessor; or, if the user has average monthly ground surface temperature data available, they can use the Site:GroundTemperature:Shallow object to provide the model monthly ground surface temperatures. From that, the model can then determine the ground temperature model parameters for the Kusuda & Achenbach (1965) ground temperature model.
-
-Ground surface cells are treated as a heat balance, where long and short wave radiation, conduction, and convection are considered. Evapotranspiration is also considered. The evapotranspiration rate is calculated as a moisture loss by using the Allen et al. (2005) model, and translated into a heat loss by multiplication with the density and latent heat of evaporation of water. The evapotranspiration rate is dependent on the type of vegetation at the surface; the user can vary the surface vegetation from anywhere between a concrete surface and a fairly tall grass (about 7�). The model can be sensitive to variations in this parameter, especially in hot dry climates.
-
-Once the basement model has run, the updated cells with zone surface boundary conditions will update the OtherSideConditionsModel temperatures which are then used at the next timestep in the surface heat balance calculations.
-
-#### Simulation Methodology
-
-The ground domain is updated at each zone timestep, or hourly as specified by the user. For situations when the ground domain is updated at each timestep, the domain is simulated by applying the surface heat flux boundary conditions from the previous timestep and calculating a new OthersideConditionsModel temperature. At this point, the surface heat balance algorithms can then take the new outside surface temperatures to update their surface heat fluxes. For situations when the user has elected to have the domain update on an hourly basis, the surface heat flux for each coupled surface is aggregated and passed to the domain as an average surface heat flux from the previous hour, which will then update the outside surface temperatures for the surface heat balance’s next iteration.
-
-The basement floor and walls are simulated by standard surface heat balance models within EnergyPlus (CTF, finite difference). The horizontal and vertical insulation are simulated by the ground domain finite difference solver. This is shown in the [Figure](#BasementGHTFigure1) below where the dotted red line defines the OtherSideConditionsModel interface separating the two solution domains. This methodology applies to the basement floor and walls.
-
-![](media/image8000.png)
-
-Figure: Example surface construction. <a name="BasementGHTFigure1"></a>
-
-References
-
-Kusuda, T. & Achenbach, P. 1965. ‘Earth Temperature and Thermal Diffusivity at Selected Stations in the United States’, ASHRAE Transactions 71(1): 61–75.
-
-Allen, R.G., Walter, I.A., Elliott, R.L., Howell, T.A., Itenfisu, D., Jensen, M.E., Snyder, R.L. 2005. The ASCE standardized reference evapotranspiration equation. Reston, VA: American Society of Civil Engineers.
-
-
-Undisturbed Ground Temperature Model: Finite Difference
--------------------------------------------------------
-
-#### Approach
-This model uses a 1D implicit finite difference heat transfer model to determine the steady-periodic annual ground temperature. The model, which uses a daily timestep, is run through an annual simulation using the user provided weather file to determine daily averages for global horizontal radiation, air temperature, relative humidity, and wind speed. Once the steady-periodic ground temperature has been determined, the temperatures are cached for use later in the simulation. The basis for the model was taken from Xing, 2014, however, the numerical methods were adapted from those described in Lee, 2013; the latter uses an implicit numerically stable finite difference method, whereas the former utilized an explicit, conditionally stable method.
-
-Surface heat balance boundary conditions are similar what is described in Herb et al., 2008. Evapotranspiration is considered as described by Allen et al., 1998. Soil freezing given the assumed stagnant soil moisture content is also considered.
-
-#### Limitations
-The model does not consider the effects of vegitative canopy layers, snow cover, ground water flow, ground moisture transport, or surface runoff. 
-
-#### References
-
-Allen, R.G., L.S. Pereira, D. Raes, M. Smith. 1998. *Crop Evapotranspiration - Guidelines for Computing Crop Water Requirements.* Food and Agriculture Organization of the United Nations.
-
-Herb, W.R., B. Janke, O. Mohseni, & H.G. Stefan. 2008. 'Ground Surface Temperature Simulation for Different Land Covers.' Journal of Hydrology, 356: pp 327-343.
-
-Lee, E.S. 2013. An Improved Hydronic Loop System Solution Algorithm with a Zone-Coupled Horizontal Ground Heat Exchanger Model for Whole Building Energy Simulation. Ph.D. Diss. Oklahoma State University, Stillwater, OK.
-
-Xing, L. 2014. Estimations of Undisturbed Ground Temperatures using Numerical and Analytical Modeling. Ph.D. Diss. Oklahoma State University, Stillwater, OK.
-
-
-Undisturbed Ground Temperature Model: Kusuda-Achenbach
-------------------------------------------------------
-
-#### Approach
-The model uses the correlation developed by Kusuda & Achenbach, 1965 which is shown below. The average soil surface temperature, amplitude of the soil surface temperature, and day of minimum surface temperature are all required inputs. These can be determined by using the CalcSoilSurfTemp preprocessor. They can also automatically be generated by leaving the parameters blank and including a Site:GroundTemperature:Shallow object in the input file.
-
-<div>$$T(z,t)=\bar{T}_{s} - \Delta\bar{T}_{s} \cdot e^{-z \cdot \sqrt{\frac{\pi}{\alpha\tau}}} \cdot cos\left( \frac{2\pi t}{\alpha t} - \theta \right)$$</div>
-
-Where:
-<div>$$T(z,t)$$</div> is the undisturbed ground temperature as a function of time and depth
-<div>$$\bar{T}_{s}$$</div> is the average annual soil surface temperature, in deg C
-<div>$$\Delta\bar{T}_{s}$$</div> is the amplitude of the soil temperature change throughout the year, in deg C
-<div>$$\theta$$</div> is the phase shift, or day of minimum surface temperature
-<div>$$\alpha$$</div> is the themal diffusivity of the ground
-<div>$$\tau$$</div> is time constant, 365.
-
-#### References
-
-Kusuda, T. and P.R. Achenbach. 1965. 'Earth Temperatures and Thermal Diffusivity at Selected Stations in the United States.' *ASHRAE Transactions*. 71(1): 61-74.
-
-
-Undisturbed Ground Temperature Model: Xing
-------------------------------------------
-
-#### Approach
-This model uses the correlation developed by Xing, 2014 to predict undisturbed ground temperature. The correlation parameters for 4000+ international locations can be found in Xing, 2014. The parameters were first determined by creating and validating a finite difference numerical model which used local weather data for boundary conditions. From the numerical model, the correlation parameters were determined to provide for this simplified design model. 
-
-<div>$$ T(z,t)=\bar{T}_{s} - \sum_{n=1}^{2} \Delta\bar{T}_{s,n} \cdot e^{-z \cdot \sqrt{\frac{n\pi}{\alpha\tau}}} \cdot cos\left[ \frac{2 \pi n}{\tau} \left(t - \theta_{n} \right) - z \sqrt{\frac{n \pi}{\alpha \tau}} \right]$$</div>
-
-<div>$$T(z,t)$$</div> is the undisturbed ground temperature as a function of time and depth
-<div>$$\bar{T}_{s}$$</div> is the average annual soil surface temperature, in deg C
-<div>$$\Delta\bar{T}_{s,n}$$</div> is the n-th amplitude of the soil temperature change throughout the year, in deg C
-<div>$$\theta_{n}$$</div> is the n-th phase shift, or day of minimum surface temperature
-<div>$$\alpha$$</div> is the themal diffusivity of the ground
-<div>$$\tau$$</div> is time constant, 365.
-
-#### References
-
-Xing, L. 2014. Estimations of Undisturbed Ground Temperatures using Numerical and Analytical Modeling. Ph.D. Diss. Oklahoma State University, Stillwater, OK.
\ No newline at end of file
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-Advanced Surface Concepts
-=========================
-
-Exterior Naturally Vented  Cavity
----------------------------------
-
-The input object “SurfaceProperty:ExteriorNaturalVentedCavity� allows modeling a special case for the outside boundary conditions of heat transfer surfaces with a multi-skin exterior that is opaque.  From the thermal envelope’s point of view, the presence of a vented cavity on the outside of the surface modifies the conditions experienced by the underlying heat transfer surfaces.  This exterior cavity acts as a radiation and convection baffle situated between the exterior environment and the outside face of the underlying heat transfer surface.  The actual outer surface is referred to as the “baffle�.  The modeling here assumes that the heat capacity in the outer baffle can be neglected since it is much lower than the underlying mass surface.  This object is used with the BuildingSurface:Detailed object where the heat transfer surfaces are referred to as the underlying surfaces.  The constructions and materials for the heat transfer surfaces should reflect the construction of just the underlying surface.  The SurfaceProperty:ExteriorNaturalVentedCavity object is used to describe the detached layer, or baffle, and the characteristics of the cavity and openings for natural ventilation.  This model uses the SurfaceProperty:OtherSideConditionsModel object to pass boundary conditions to the heat transfer modeling for the underlying surfaces.
-
-### Baffle Heat Balance
-
-The baffle is assumed to be sufficiently thin and high-conductivity so that it can be modeled using a single temperature (for both sides and along its area).  This temperature <span>\({T_{s,baff}}\)</span>is determined by formulating a heat balance on a control volume that just encapsulates the baffle surface.  The baffle is assumed to completely cover the underlying surface such that it is opaque to shortwave and longwave radiation.  This assumption means that even though the baffle will have some open area for ventilation, no solar energy passes through these openings. The heat balance is diagrammed in the following figure.
-
-![](media/image438.png)
-
-Figure 33.  Baffle Surface Heat Balance
-
-The heat balance on the baffle surface’s control volume is:
-
-<div>$${q''_{\alpha sol}} + {q''_{LWR,Env}} + {q''_{conv,Env}} + {q''_{LWR,cav}} + {q''_{conv,cav}} + {q''_{source}} = 0$$</div>
-
-where:
-
-<sub><span>\({q''_{\alpha sol}}\)</span> </sub>is absorbed direct and diffuse solar (short wavelength) radiation heat flux.
-
-<span>\({q''_{LWR,Env}}\)</span> is net long wavelength (thermal) radiation flux exchange with the air and surroundings.
-
-<sub><span>\({q''_{conv,Env}}\)</span> </sub>= surface convection flux exchange with outside air.
-
-<sub><span>\({q''_{LWR,cav}}\)</span> </sub>is net long wavelength (thermal) radiation flux exchange with the outside face of the underlying surface(s).
-
-<sub><span>\({q''_{conv,cav}}\)</span> </sub>= surface convection flux exchange with cavity air.
-
-<span>\({q''_{source}}\)</span> is a source/sink term that accounts for energy exported out of the control volume when the baffle is a hybrid device such as a photovoltaic panel.
-
-All terms are positive for net flux to the baffle.  Each of these heat balance components is introduced briefly below.
-
-#### External SW Radiation
-
-<sub><span>\({q''_{\alpha sol}}\)</span> </sub> is calculated using procedures presented elsewhere in this manual and includes both direct and diffuse incident solar radiation absorbed by the surface face.  This is influenced by location, surface facing angle and tilt, shading surfaces, surface face material properties, weather conditions, etc.  The baffle blocks all shortwave radiation from reaching the underlying surface.
-
-#### External LW Radiation
-
-<span>\({q''_{LWR,Env}}\)</span> is a standard radiation exchange formulation between the surface, the sky, the ground, and the atmosphere.  The radiation heat flux is calculated from the surface absorptivity, surface temperature, sky, air, and ground temperatures, and sky and ground view factors.  Radiation is modeled using linearized coefficients.  The baffle blocks all longwave radiation.
-
-#### External Convection
-
-<span>\(q''_{conv,env}\)</span> is modeled using the classical formulation: <span>\(q''_{conv} = h_{co}(T_{air} - T_{o})\)</span> where h<sub>co</sub>, is the convection coefficient.  The h<sub>co</sub> is treated in the same way as an outside face with ExteriorEnvironment conditions.  In addition, when it is raining outside, we assume the baffle gets wet and model the enhanced surface heat transfer using a large value for <span>\({h_{co}}\)</span>.
-
-#### Cavity LW Radiation
-
-<span>\({q''_{LWR,cav}}\)</span>is a standard radiation exchange formulation between the baffle surface and the underlying heat transfer surface located across the cavity.  Radiation is modeled using linearized coefficients.
-
-#### Cavity Convection
-
-<span>\(q''_{conv,cav}\)</span> is modeled using the classical formulation: <span>\(q''_{conv} = h_{cp}(T_{air} - T_{o))\)</span>  where h<sub>cp</sub>, is the convection coefficient.  The value for h<sub>cp</sub> is obtained from correlations used for window gaps from ISO (2003) standard 15099.
-
-Substituting models into (113) and solving for <span>\({T_{s,baff}}\)</span> yields the following equation:
-
-<div>$${T_{s,baff}} = \frac{{\left( {{I_s}\alpha  + {h_{co}}{T_{amb}} + {h_{r,atm}}{T_{amb}} + {h_{r,sky}}{T_{sky}} + {h_{r,gnd}}{T_{amb}} + {h_{r,cav}}{T_{so}} + {h_{c,cav}}{T_{a,cav}} + {{q''}_{source}}} \right)}}{{\left( {{h_{co}} + {h_{r,air}} + {h_{r,sky}} + {h_{r,gnd}} + {h_{r,cav}} + {h_{c,cav}}} \right)}}$$</div>
-
-where,
-
-<span>\({I_s}\)</span> is the incident solar radiation of all types [W/m<sup>2</sup>],
-
-<span>\(\alpha \)</span> is the solar absorptivity of the baffle [dimensionless],
-
-<span>\({h_{r,atm}}\)</span>is the linearized radiation coefficient for the surrounding atmosphere [W/m<sup>2</sup>·K],
-
-<span>\({T_{amb}}\)</span> is the outdoor drybulb from the weather data, also assumed for ground surface [ºC],
-
-<span>\({h_{r,sky}}\)</span> is the linearized radiation coefficient for the sky [W/m<sup>2</sup>·K],
-
-<span>\({T_{sky}}\)</span> is the effective sky temperature [ºC],
-
-<span>\({h_{r,gnd}}\)</span> is the linearized radiation coefficient for the ground [W/m<sup>2</sup>·K],
-
-<span>\({h_{r,cav}}\)</span> is the linearized radiation coefficient for the underlying surface [W/m<sup>2</sup>·K],
-
-<span>\({T_{so}}\)</span> is the temperature of the outside face of the underlying heat transfer surface [ºC],
-
-<span>\({h_{co}}\)</span> is the convection coefficient for the outdoor environment [W/m<sup>2</sup>·K],
-
-<span>\({h_{c,cav}}\)</span> is the convection coefficient for the surfaces facing the plenum [W/m<sup>2</sup>·K], and
-
-<span>\({T_{a,cav}}\)</span> is the drybulb temperature for air in the cavity [ºC].
-
-### Cavity Heat Balance
-
-The *cavity* is the volume of air located between the baffle and the underlying heat transfer surface.  The cavity air is modeled as well-mixed.  The uniform temperature of the cavity air, <span>\({T_{a,cav}}\)</span>, is determined by formulating a heat balance on a control volume of air as diagrammed below.
-
-![](media/image469.png)
-
-Figure 34.  Cavity Air Heat Balance
-
-
-
-The heat balance on the cavity air control volume is:
-
-<div>$${\dot Q_{vent}} + {\dot Q_{co}} + {\dot Q_{c,baff}} = 0$$</div>
-
-where,
-
-<span>\({\dot Q_{vent}}\)</span> is the net rate of energy added from natural ventilation – where outdoor ambient air exchanges with the cavity air.
-
-<sub><span>\({\dot Q_{co}}\)</span> </sub> is the net rate of energy added by surface convection heat transfer with the underlying surface.
-
-<span>\({\dot Q_{c,baff}}\)</span>is the net rate of energy added by surface convection heat transfer with the collector.
-
-And substituting into yields the following equation:
-
-<div>$${T_{a,cav}} = \frac{{\left( {{h_{c,cav}}A\,{T_{so}} + {{\dot m}_{vent}}{c_p}{T_{amb}} + {h_{c,cav}}A\,{T_{s,baff}}} \right)}}{{\left( {{h_{c,cav}}A + {{\dot m}_{vent}}{c_p} + {h_{c,cav}}A} \right)}}$$</div>
-
-where,
-
-<span>\({\dot m_{vent}}\)</span> is the air mass flow from natural forces [kg/s]
-
-Modeling natural ventilation air exchanges in a general way is challenging.  Simplistic engineering models are used to model <span>\({\dot m_{vent}}\)</span> resulting from natural buoyancy and wind forces.  Reasoning that the configuration is similar to single-side natural ventilation, we elect to use correlations for natural ventilation presented as equations (29) and (30) in Chapter 26. of ASHRAE HOF (2001).
-
-<div>$${\dot m_{vent}} = \rho \,{{\rm{\rlap{--} \dot V}}_{{\rm{tot}}}}$$</div>
-
-where,
-
-<span>\(\rho \)</span> is the density of air [kg/m<sup>3</sup>], and
-
-<span>\(\dot{V}_{tot} = \dot{V}_{wind} + \dot{V}_{thermal} \)</span> is the total volumetric flow rate of air ventilating in and out of the cavity.
-
-<div>$$\dot{V}_{wind} = C_{v}A_{in}U_{\infty}$$</div>
-
-<div>$$
-  \dot{V}_{thermal} = \left\{
-    \begin{array}{cl}
-      C_{D}A_{in}\sqrt{2g\Delta H_{NPL}\left(T_{a,cav}-T_{amb}\right)/T_{a,cov}} & \; \left(T_{a,cav}>T_{amb}\right) \\
-      C_{D}A_{in}\sqrt{2g\Delta H_{NPL}\left(T_{amb}-T_{a,cav}\right)/T_{amb}} & \; \left(T_{a,cav} \lt T_{amb}\,\text{and baffle is vertical}\right) 
-    \end{array}
-  \right.
-$$</div>
-
-<span>\({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}} = {C_D}{A_{in}}\sqrt {2g\Delta {H_{NPL}}\left( {{T_{a,cav}} - {T_{amb}}} \right)/{T_{a,cav}}} \)</span>  (if <span>\({T_{a,cav}} > {T_{amb}}\)</span>)
-
-<span>\({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}} = {C_D}{A_{in}}\sqrt {2g\Delta {H_{NPL}}\left( {{T_{amb}} - {T_{a,cav}}} \right)/{T_{amb}}} \)</span>  (if <span>\({T_{amb}} > {T_{a,cav}}\)</span> and baffle is vertical)
-
-<span>\({C_v}\)</span> is the effectiveness of the openings that depends on opening geometry and the orientation with respect to the wind.  ASHRAE HoF (2001) indicates values ranging from 0.25 to 0.6.  This value is available for user input.
-
-<span>\({C_D}\)</span> is the discharge coefficient for the opening and depends on opening geometry.  This value is available for user input.
-
-Mass continuity arguments lead to modeling the area of the openings as one half of the total area of the openings, so we have:
-
-<div>$${A_{in}} = \frac{{A\,}}{2}$$</div>
-
-<span>\(g\)</span> is the gravitational constant taken as 9.81 [m/s<sup>2</sup>].
-
-<span>\(\Delta {H_{NPL}}\)</span> is the height from midpoint of lower opening to the Neutral Pressure Level.  This is value is available for user input.
-
-If the cavity is horizontal and <span>\({T_{amb}} > {T_{a,cav}}\)</span> then <span>\({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}}{\rm{  =  0}}\)</span> because this is a stable situation.
-
-### Underlying Heat Transfer Surface
-
-The exterior baffle and cavity are applied to the outside of a heat transfer surface.  This surface is modeled using the usual EnergyPlus methods for handling heat capacity and transients – typically the CTF method.  These native EnergyPlus heat balance routines are used to calculate <span>\({T_{so}}\)</span>.  The exterior baffle and cavity system is coupled to the underlying surface using the SurfaceProperty:OtherSideConditionsModel mechanism.  The exterior naturally vented cavity model provides values for <span>\({h_{r,cav}}\)</span>,<span>\({T_{s,baff}}\)</span>, <span>\({h_{c,cav}}\)</span>, and <span>\({T_{a,cav}}\)</span> for use with the heat balance model calculations for the outside face of the underlying surface (described elsewhere in this manual).
-
-### Solar and Shading Calculations
-
-The exterior vented cavity model uses standard EnergyPlus surfaces in order to take advantage of the detailed solar and shading calculations.  Solar radiation incident on the surface includes beam and diffuse radiation, as well as radiation reflected from the ground and adjacent surfaces.  Shading of the collector by other surfaces, such as nearby buildings or trees, is also taken into account.
-
-### Local Wind Speed Calculations
-
-The outdoor wind speed affects terms used in modeling.  The wind speed in the weather file is assumed to be measured at a meteorological station located in an open field at a height of 10 m.  To adjust for different terrain at the building site and differences in the height of building surfaces, the local wind speed is calculated for each surface.
-
-The wind speed is modified from the measured meteorological wind speed by the equation (ASHRAE 2001):
-
-<div>$${U_\infty } = {V_{met}}{\left( {\frac{{{\delta_{met}}}}{{{z_{met}}}}} \right)^{{a_{met}}}}{\left( {\frac{z}{\delta }} \right)^a}$$</div>
-
-where z is the height of the centroid of the system, z<sub>met</sub> is the height of the standard meteorological wind speed measurement, and a and d are terrain-dependent coefficients.  d is the boundary layer thickness for the given terrain type.  The values of a and d are shown in the following tables:
-
-Table 19. Terrain-Dependent Coefficients (ASHRAE 2001).
-
-<table class="table table-striped">
-<tr>
-<th>Terrain</th>
-<th>Description</th>
-<th>Exponent, a</th>
-<th>Layer Thickness,d (m)</th>
-</tr>
-<tr>
-<td>1</td>
-<td>Flat, open country</td>
-<td>0.14</td>
-<td>270</td>
-</tr>
-<tr>
-<td>2</td>
-<td>Rough, wooded country</td>
-<td>0.22</td>
-<td>370</td>
-</tr>
-<tr>
-<td>3</td>
-<td>Towns and cities</td>
-<td>0.33</td>
-<td>460</td>
-</tr>
-<tr>
-<td>4</td>
-<td>Ocean</td>
-<td>0.10</td>
-<td>210</td>
-</tr>
-<tr>
-<td>5</td>
-<td>Urban, industrial, forest</td>
-<td>0.22</td>
-<td>370</td>
-</tr>
-
-</table>
-
-The exterior vented cavity can be defined such that it has multiple underlying heat transfer surfaces.  The centroid heights for each surface are area-weighted to determine the average height for use in the local wind calculation.
-
-### Convection Coefficients
-
-Exterior cavity modeling requires calculating up to three different coefficients for surface convection heat transfer.  These coefficients are defined in the classic way by:
-
-<div>$${h_c} = \frac{{{T_{air}} - {T_{surf}}}}{{{{q''}_{conv}}}}$$</div>
-
-First, <span>\({h_{co}}\)</span> is the convection coefficient for the baffle surface facing the outdoors.  It is modeled in exactly the same way as elsewhere in EnergyPlus and will depend on the user setting for Outside Convection Algorithm – Outside Surface Heat Balance entry elsewhere in this document.
-
-Second, <span>\({h_{c,cav}}\)</span> is the convection coefficient for baffle surfaces facing the cavity.  This coefficient is applied to both the baffle and the underlying surface.  The convection coefficient is modeled in the same way used in EnergyPlus to model air gaps in windows.  These correlations vary by Rayleigh number and surface tilt and are based on the work of various research including Hollands et. al., Elsherbiny et. al., Wright, and Arnold.  The formulations are documented in ISO (2003) standard 15099.  The routines were adapted from Subroutine NusseltNumber in WindowManager.f90 (by F. Winkelmann), which itself was derived from Window5 subroutine “nusselt�.
-
-### Radiation Coefficients
-
-Exterior vented cavity modeling requires calculating up to four different linearized coefficients for radiation heat transfer.  Whereas radiation calculations usually use temperature raised to the fourth power, this greatly complicates solving heat balance equations for a single temperature.  Linearized radiation coefficients have the same units and are used in the same manner as surface convection coefficients and introduce very little error for the temperature levels involved.
-
-The radiation coefficient, <span>\({h_{r,cav}}\)</span>, is used to model thermal radiation between the collector surface and the outside face of the underlying heat transfer surface.  We assume a view factor of unity.  It is calculated using:
-
-<div>$${h_{r,cav}} = {\sigma_{SB}}{e_{baff}}{e_{so}}\frac{{\left( {T_{s,baff}^4 - T_{so}^4} \right)}}{{\left( {{T_{s,baff}} - {T_{so}}} \right)}}$$</div>
-
-where,
-
-all temperatures are converted to Kelvin,
-
-<span>\({\sigma_{SB}}\)</span> is the Stefan-Boltzmann constant,
-
-<span>\({e_{baff}}\)</span> is the longwave thermal emittance of the baffle, and
-
-<span>\({e_{so}}\)</span> is the longwave thermal emittance of the underlying heat transfer surface.
-
-The three other coefficients, <span>\({h_{r,atm}}\)</span>, <span>\({h_{r,sky}}\)</span>, and <span>\({h_{r,gnd}}\)</span> are used elsewhere in EnergyPlus for the outside face surface heat balance and are calculated in the same manner as equation .  [This is accomplished by calling subroutine InitExteriorConvectionCoeffs in the file HeatBalanceConvectionCoeffs.f90. ]
-
-### References
-
-ASHRAE HOF 2001.  2001 ASHRAE Fundamentals Handbook.  American Society of Heating Refrigeration and Air-Conditioning Engineers. Altanta GA.
-
-ISO. 2003. ISO 15099:2003. Thermal performance of windows, doors, and shading devices – Detailed calculations. International Organization for Standardization.
-
-Green Roof Model (EcoRoof)
-----------------------------------------------------
-
-### Overview
-
-The input object Material:RoofVegetation provides a model for green roofs (aka ecoroofs or vegetated roofs) that are becoming increasingly common for both new and retrofit buildings. There is widespread recognition and a growing literature of measured data that suggest green roofs can reduce building energy consumption. Currently, however, there are few design tools available to assist developers and architects in assessing the likely magnitude of energy savings associated with various implementation options (e.g., soil type/depth, irrigation options, plant type). As a result there is a significant need for a quantitative and physically-based building energy simulation tool that represents the effects of green roof constructions. Such a tool would facilitate more rapid spread of green roof technologies and make it possible to account for green roof benefits in state energy codes and related energy efficiency standards such as LEED.
-
-In response to the need for green roof design tools a computational model of the heat transfer processes involved on a vegetated roof has been developed. This model accounts for:
-
-* long wave and short wave radiative exchange within the plant canopy,
-
-* plant canopy effects on convective heat transfer,
-
-* evapotranspiration from the soil and plants, and
-
-* heat conduction (and storage) in the soil layer
-
-The ability to track moisture-dependent thermal properties is not implemented yet due to stability issues in the CTF scheme, but is under development for use with the finite difference solution scheme made available in EnergyPlus starting in version 2.
-
-As implemented in EnergyPlus the green roof module allows the user to specify “ecoroof� as the outer layer of a rooftop construction using a “Material:RoofVegetation� object. The user can then specify various aspects of the green roof construction including growing media depth, thermal properties, plant canopy density, plant height, stomatal conductance (ability to transpire moisture), and soil moisture conditions (including irrigation).
-
-The model formulation includes the following:
-
-* simplified moisture balance that allows precipitation, irrigation, and moisture transport between two soil layers (top and root zone).
-
-* soil and plant canopy energy balance based on the Army Corps of Engineers’ FASST vegetation models (Frankenstein and Koenig), drawing heavily from BATS (Dickenson et al.) and SiB (Sellers et al.).
-
-* soil surface (T<sub>g</sub>) and foliage (T<sub>f</sub>) temperature equations are solved simultaneously each time step, inverting the CTF to extract heat flux information for the energy balance calculation.
-
-The detailed energy balance analysis and resulting equations, being rather complicated, are summarized here. The interested reader is referred to the FASST documentation cited herein for the complete development. The end result is a set of two simultaneous equations for temperature—one for the soil surface and the other for the foliage.
-
-### Green Roof Model Description
-
-As with a traditional roof, the energy balance of an green roof is dominated by radiative forcing from the sun. This solar radiation is balanced by sensible (convection) and latent (evaporative) heat flux from soil and plant surfaces combined with conduction of heat into the soil substrate. This energy balance is illustrated in Figure 35. The variables introduced in this figure are defined in the equations that follow.
-
-![Fig1EcoRoof](media/image509.png)
-
-Figure 35.  The Energy Balance for a Green Roof.
-
-The energy budget analysis follows the Fast All Season Soil Strength (FASST) model developed by Frankenstein and Koenig for the US Army Corps of Engineers. FASST was developed, in part, to determine the ability of soils to support manned and unmanned vehicles and personnel movement. In order to accomplish this, however, FASST tracks the energy and moisture balance (including ice and snow) within a vegetated soil. It is a one-dimensional model that draws heavily from other plant canopy models including BATS (Dickinson et al.) and SiB (Sellers et al.). We have implemented FASST here with only a few modifications to adapt it for use with a relatively thin soil layer. The sign convention used assumes all heat fluxes are positive when energy is absorbed into the layer.
-
-In the following discussion this energy budget is divided into a budget for the foliage layer (F<sub>f</sub>) and a budget for the ground surface (F<sub>g</sub>­). The various parameterizations for latent and sensible heat flux are described in some detail and then the equation set is reduced to the simultaneous solution of two equations involving the temperatures of the foliage and ground surface.
-
-#### Energy budget in the foliage layer
-
-The foliage energy balance is given by:
-
-<div>$${F_f} = {\sigma_f}\left[ {{I_S}^ \downarrow (1 - {\alpha_f}) + {\varepsilon_f}{I_{ir}}^ \downarrow  - {\varepsilon_f}\sigma {T_f}^4} \right] + \frac{{{\sigma_f}{\varepsilon_g}{\varepsilon_f}\sigma }}{{{\varepsilon_1}}}\left( {{T_g}^4 - {T_f}^4} \right) + {H_f} + {L_f}$$</div>
-
-Where sigma_f is calculated as a function of Leaf-Area-Index (LAI):
-
-<div> $$ \sigma_f = 0.9 - 0.7 \exp{-0.75 LAI } $$ </div>
-
-In addition to convective and sensible heat transfer this equation accounts for both the short and longwave radiation absorbed by the vegetation, including the effects of multiple reflections. The sensible and latent heat flux terms (H<sub>f</sub> and L<sub>f­</sub>) are somewhat complicated and therefore discussed in some detail below.
-
-##### Sensible heat flux in the foliage layer
-
-The sensible heat transfer between the leaf surface and near-canopy air (H<sub>f</sub>) is influenced by the temperature difference between them, wind speed, and Leaf Area Index (LAI). The Leaf Area Index is the dimensionless ratio of the projected leaf area for a unit ground area (Oke). In contrast fractional vegetative cover (s<sub>f</sub>) is the ratio of shaded ground surface to total ground surface area. The sensible heat flux is given by:
-
-<div>$${H_f} = (1.1*LAI{\rho_{af}}{C_{p,a}}{C_f}{W_{af}})*({T_{af}} - {T_f})$$</div>
-
-In this equation the constant 1.1 accounts for heat transfer from the stems, twigs and limbs (Deardorff). The properties of air near the foliage are modeled using the average from the foliage and instrument conditions:
-
-<div>$${\rho_{af}} = 0.5({\rho_a} + {\rho_f})$$</div>
-
-where r<sub>a</sub> is the density of air at the instrument height  and r<sub>f</sub> is the density of air at the leaf temperature. The air temperature within the foliage is estimated by:
-
-<div>$${T_{af}} = (1 - {\sigma_f})({T_a}) + {\sigma_f}\left( {0.3{T_a} + 0.6{T_f} + 0.1{T_g}} \right)$$</div>
-
-*where, T<sub>a</sub>* is the air temperature at the instrument height in Kelvin *T<sub>f</sub>*, is leaf temperature in Kelvin and *T<sub>g</sub>*, is the ground surface temperature in Kelvin. The foliage wind speed is estimated as:
-
-<div>$${W_{af}} = 0.83{\sigma_f}W\sqrt {C_{hn}^f}  + (1 - {\sigma_f})W$$</div>
-
-Here *W* is the larger of 2.0 m/s or the actual wind speed above the canopy (Hughes et al.) and C<sup>f</sup><sub>hn</sub> is the transfer coefficient at near-neutral atmospheric stability conditions:
-
-<div>$$C_{hn}^f = {K_v}^2 \cdot {\left( {\ln \left( {\frac{{{Z_a} - {Z_d}}}{{Z_o^f}}} \right)} \right)^{ - 2}}$$</div>
-
-where *K<sub>v</sub>,* is von Karmen’s constant (0.4), Z<sub>a</sub> is the instrument height, Z<sub>d</sub> is the zero displacement height in meters (height above soil within which the wind speed is effectively zero), and Z<sup>f</sup><sub>o</sub> is the foliage roughness length scale (m). The formulations for zero displacement height, roughness length are based on Balick et al.:
-
-<div>$${Z_d} = 0.701Z_{_f}^{0.979}$$</div>
-
-<div>$${Z_o} = 0.131Z_{_f}^{0.997}$$</div>
-
-Finally, the bulk transfer coefficient as defined by Deardorff is given by:
-
-<div>$${C_f} = 0.01*\left( {1 + \frac{{0.3(m/s)}}{{{W_{af}}(m/s)}}} \right)$$</div>
-
-##### Latent heat flux in the foliage layer
-
-The process of water loss through plant respiration is known as transpiration. It is controlled by the closing and opening of stomata - the intercellular openings between to epidermal (guard) cells (Gates). The resistance to the diffusion of water vapor from these spaces into the atmosphere is called stomatal resistance. It depends on factors such as light intensity, soil moisture content and vapor pressure difference between inside leaf and the outside atmosphere. It is measured in units of s/m and is formulated as:
-
-<div>$${r_s} = \frac{{{r_{s,\min }}}}{{LAI}} \cdot {f_1} \cdot {f_2} \cdot {f_3}$$</div>
-
-Here, r<sub>s,min</sub> is the minimum stomatal resistance. The actual stomatal resistance at any time is proportional to this minimum resistance and inversely proportional to LAI. The stomatal resistance is further modified by fractional multiplying factors that relate to incoming solar radiation and atmospheric moisture. As found in Frankenstein and Koenig the inverses of the multiplying factors f<sub>1</sub>, f<sub>2</sub>, and f<sub>3</sub> are given by:
-
-<div>
- $$
-  \begin{array}{l}
-   \frac{1}{f_1} = \min \left[ 1,\frac{{0.004*{I_s}^ \downarrow  + 0.005}}{{0.81*(0.004*{I_s}^ \downarrow  + 1)}} \right] \\
-   \frac{1}{f_2} = \left\{ 
-     \begin{array}{cl}
-       0                                                                 & \text{when} \; \theta_r \gt \overline \theta \\
-       \frac{ \overline \theta   - \theta_r }{ \theta_{max} - \theta_r } & \text{when} \; \theta_r \le \overline \theta \le \theta_{max}
-     \end{array} \right. \\
-   \frac{1}{f_3} = \exp \left[ - {g_d}({e_{f,sat}} - {e_a} \right]
-  \end{array}
- $$
-</div>
-
-Here, Q<sub>r</sub>, is the residual moisture content (defined as the amount of moisture in soil when plants begin to wilt), Q<sub>max</sub> is the maximum moisture content (defined as the maximum amount of moisture a particular type of soil can hold and above which run off occurs), and <span>\(\overline \Theta  \)</span> is the average soil moisture in the root zone. The residual moisture content is typically around 0.01 m<sup>3</sup>/m<sup>3</sup> (Frankenstein and Koenig). The maximum moisture content depends upon the soil, but generally varies from 0.3 to 0.6 m<sup>3</sup>/m<sup>3</sup> (Guymon et al.). In the expression for f<sub>3</sub>, g<sub>d</sub> is a plant specific characteristic that is only non-zero for trees, e<sub>f,sat</sub> is the saturated vapor pressure at the leaf temperature, and e<sub>a</sub> is the air vapor pressure.
-
-Resistance to moisture exchange offered by the boundary layer formed on the leaf surface is known as aerodynamic resistance. It is measured in units of (s/m) and is influenced by wind speed, surface roughness and stability of the atmosphere (Oke). It is formulated as:
-
-<div>$${r_a} = \frac{1}{{{c_f}{W_{af}}}}$$</div>
-
-The combined effect of aerodynamic and stomatal resistances to vapor diffusion is integrated into a foliage surface wetness factor:
-
-<div>$$r'' = \frac{{{r_a}}}{{{r_a} + {r_s}}}$$</div>
-
-This surface wetness factor is simply a ratio of the aerodynamic resistance to the total resistance. When the aerodynamic resistance is small the wetness factor approaches zero (leaf surfaces remain dry as surface moisture is readily evaporated). As the aerodynamic resistance increases in importance relative to stomatal resistance the wetness factor approaches 1.0 (moisture readily travels to the leaf surfaces, but is not easily evaporated).
-
-The latent heat flux is then given by:
-
-<div>$${L_f} = {l_f} * LAI{\rho_{af}}{C_f}{W_{af}}{r^``}\left( {{q_{af}} - {q_{f,sat}}} \right)$$</div>
-
-Here *l<sub>f</sub>* , is the latent heat of vaporization (J/kg), q<sub>f,sat</sub> is the saturation mixing ratio at the leaf surface temperature, and q<sub>af</sub> is the mixing ratio of the air within the canopy. As developed in Frankenstein and Koenig the mixing ratio within the canopy can be determined from:
-
-<div>$${q_{af}} = \left[ {\frac{{\left( {1 - {\sigma_f}} \right){q_a} + {\sigma_f}\left( {0.3{q_a} + 0.6{q_{f,sat}}{r^``} + 0.1{q_{f,sat}}{M_g}} \right)}}{{1 - {\sigma_f}\left[ {0.6\left( {1 - {r^``}} \right) + 0.1\left( {1 - {M_g}} \right)} \right]}}} \right]$$</div>
-
-where the factor *M<sub>g</sub>*  (ranging from 0 to 1) is the ratio of volumetric moisture content to the porosity of the soil (Koenig). The latent heat of vaporization (*l<sub>f</sub>*) is the amount of energy required to convert a unit mass of water to vapor. It is measured in units of J/kg and is inversely proportional to the temperature. From Henderson-Sellers it is estimated as:
-
-<div>$${l_f} = 1.91846*{10^6}{\left[ {\frac{{{T_f}}}{{{T_f} - 33.91}}} \right]^2}$$</div>
-
-#### Soil Energy budget
-
-The energy budget at the soil surface is mainly influenced by the soil thermal properties, the amount of foliage coverage (s<sub>f</sub>) and the amount of moisture in the soil. If the soil surface is densely covered the diurnal range of surface temperature is small. In the soil energy budget the heat released or gained due to phase changes of soil water, precipitation heat flux and heat flux due to vertical transport of water in the soil are ignored. Future refinements to this model will incorporate these phenomena. The sign convention followed here is the same as above (heat flux into the soil is positive). The overall energy balance at the soil surface (as given in Frankenstein and Koenig) is:
-
-<div>$${F_g} = (1 - {\sigma_f})\left[ {I_s^ \downarrow (1 - {\alpha_g}) + {\varepsilon_g}I_{ir}^ \downarrow  - {\varepsilon_g}T_g^4} \right] - \frac{{{\sigma_f}{\varepsilon_g}{\varepsilon_f}\sigma }}{{{\varepsilon_1}}}\left( {T_g^4 - T_f^4} \right) + {H_g} + {L_g} + K*\frac{{\partial {T_g}}}{{\partial z}}$$</div>
-
-As with the energy equation for the foliage this equation represents sensible heat flux (H<sub>g</sub>), latent heat flux (L<sub>g</sub>) and the multiple reflections associated with long and short wave radiation. The final term on the right side gives the conduction of heat into the soil substrate.
-
-##### Sensible heat flux in the soil layer
-
-Sensible heat flux between the soil surface and air in its vicinity is dependent on the temperature difference between them and the wind speed within the canopy. It is given as
-
-<div>$${H_g} = {\rho_{ag}}{C_{p,a}}C_h^g{W_{af}}({T_{af}} - {T_g})$$</div>
-
-where <span>\(C_h^g\)</span> is the bulk transfer coefficient and r<sub>ag</sub> is the density of air near the soil surface (kg/m<sup>3</sup>) given by:
-
-<div>$${p_{ag}} = \frac{{{p_a} + {p_g}}}{2}$$</div>
-
-Here r<sub>g</sub> is the density of air at the ground surface temperature
-
-The bulk transfer coefficient is given as the linear combination of bulk transfer coefficient near ground (C<sup>f</sup><sub>hn</sub>) and near foliage-atmosphere interface (C<sup>g</sup><sub>hn</sub>) multiplied by the stability factor (G<sub>h</sub>) and is formulated as:
-
-<div>$$C_h^g = {\Gamma_k}\left[ {\left( {1 - {\sigma_f}} \right)C_{hn}^g + {\sigma_f}C_{hn}^f} \right]$$</div>
-
-The ground and foliage bulk transfer coefficients, in turn, are given by:
-
-<div>$$C_{hn}^g = r_{ch}^{ - 1}{\left[ {\frac{{{K_v}}}{{\ln \left( {{\raise0.7ex\hbox{${{Z_a}}$} \!\mathord{\left/ {\vphantom {{{Z_a}} {Z_o^g}}}\right.}\!\lower0.7ex\hbox{${Z_o^g}$}}} \right)}}} \right]^2}$$</div>
-
-And
-
-<div>$$C_{hn}^f = {\left[ {\frac{{{K_v}}}{{\ln \left( {{\raise0.7ex\hbox{${{Z_a} - {Z_d}}$} \!\mathord{\left/ {\vphantom {{{Z_a} - {Z_d}} {Z_o^f}}}\right.}\!\lower0.7ex\hbox{${Z_o^f}$}}} \right)}}} \right]^2}$$</div>
-
-where<span>\(Z_o^g\)</span> and <span>\(Z_o^f\)</span> are the ground and foliage roughness lengths,  r<sub>ch</sub> is turbulent Schmidt number (0.63), and K<sub>v</sub> is the von Karman constant (0.4).
-
-The condition of the atmosphere (G<sub>h</sub>) is determined as stable or unstable based on the sign of the bulk Richardson number:
-
-<div>$${R_{ib}} = \frac{{2g{Z_a}\left( {{T_{af}} - {T_g}} \right)}}{{\left( {{T_{af}} + {T_g}} \right)W_{af}^2}}$$</div>
-
-The atmospheric stability factor is then given by Businger and Lumley and Panofsky as:
-
-<div>$$
-  \Gamma_h = \left\{ 
-    \begin{array}{cl}
-      \frac{1.0}{\left( 1.0 - 16.0 R_{ib} \right)^{0.5}} & \text{for} \; R_{ib} \lt 0 \\
-      \frac{1.0}{\left( 1.0 - 5.0  R_{ib} \right)      } & \text{for} \; R_{ib} \gt 0
-    \end{array}
-  \right.
-$$</div>
-
-##### Latent heat flux in the soil layer
-
-Removal of water vapor from the soil surface depends on the difference between the mixing ratio of the soil surface and air and the wind speed within the canopy. The resulting latent heat flux is then given by:
-
-<div>$${L_R} = C_e^g{l_g}{W_{af}}{\rho_{ag}}\left( {{q_{af}} - {q_g}} \right)$$</div>
-
-Here<span>\(C_e^g\)</span>is the bulk transfer coefficient, l<sub>g</sub> is the latent heat of vaporization at the ground surface temperature, q<sub>af</sub> is the mixing ratio at the foliage-atmosphere interface, and q<sub>f</sub> is the mixing ratio at the ground surface, given by:
-
-<div>$${q_g} = {M_g}{q_{g,sat}} + \left( {1 - {M_g}} \right){q_{af}}$$</div>
-
-The bulk transfer coefficient for latent heat exchange is analogous to that for sensible heat exchange and is given by:
-
-<div>$$C_e^g = {\Gamma_e}\left[ {\left( {1 - {\sigma_f}} \right)C_{en}^g + {\sigma_f}C_{hn}^f} \right]$$</div>
-
-where <span>\(C_{en}^g\)</span> is the near ground bulk transfer coefficient for Latent heat flux and G<sub>e</sub> is the latent heat exchange stability correction factor (assumed to be the same as G<sub>h</sub>).
-
-### Linearization
-
-In order to solve the foliage and soil heat budget equations, the 4<sup>th</sup> <sup> </sup>order terms T<sub>f</sub><sup>4</sup> and T<sub>g</sub><sup>4</sup>  and mixing ratio terms q<sub>g,sat</sub> and q<sub>f,sat</sub> <sub> </sub>are linearized as given by Deardorff:
-
-<div>$${\left[ {T_f^{\left( {n + 1} \right)}} \right]^4} = {\left[ {T_f^n} \right]^4} + 4{\left[ {T_f^n} \right]^3}\left[ {T_f^{n + 1} - T_f^n} \right]$$</div>
-
-<div>$${\left[ {T_g^{\left( {n + 1} \right)}} \right]^4} = {\left[ {T_g^n} \right]^4} + 4{\left[ {T_g^n} \right]^3}\left[ {T_g^{n + 1} - T_g^n} \right]$$</div>
-
-Here T<sub>f</sub><sup>n+1</sup> and T<sub>g</sub><sup>n+1</sup> are the current time step leaf and ground surface temperatures in Kelvin. T<sub>f</sub><sup>n</sup> and T<sub>g</sub><sup>n</sup> are the corresponding temperatures at the previous time step.
-
-The saturation mixing ratio at the ground and leaf surface temperatures are given as:
-
-<div>$${q_{g,sat}}\left( {T_g^{n + 1}} \right) = {q_{sat}}\left( {T_g^n} \right) + {\left( {\frac{{\partial {q_{sat}}}}{{\partial T}}} \right)_{T_g^n}} * \left( {T_g^{n + 1} - T_g^n} \right)$$</div>
-
-<div>$${q_{f,sat}}\left( {T_f^{n + 1}} \right) = {q_{sat}}\left( {T_f^n} \right) + {\left( {\frac{{\partial {q_{sat}}}}{{\partial T}}} \right)_{T_f^n}} * \left( {T_f^{n + 1} - T_f^n} \right)$$</div>
-
-where q<sub>sat</sub>(T<sub>g</sub><sup>n</sup>) is the saturation mixing ratio at the previous time step and is formulated as given in Garratt:
-
-<div>$${q_{sat}}\left( {T_g^n} \right) = \frac{{0.622{e^ * }\left( {T_g^n} \right)}}{{P - {e^ * }\left( {T_g^n} \right)}}$$</div>
-
-Here the saturation vapor pressure e\* (Pa) is evaluated at the ground temperature from the previous time step (T<sub>g</sub><sup>n</sup>) as:
-
-<div>$${e^*} = 611.2\exp \left[ {17.67\left( {\frac{{T_g^n - 273.15}}{{T_g^n - 29.65}}} \right)} \right]$$</div>
-
-The derivative of saturation mixing ratio at the previous time step is given by:
-
-<div>$$\frac{{d{q^ * }}}{{dT_g^n}} = \left[ {\frac{{0.622 * P}}{{{{\left( {P - 0.378 * {e^ * }} \right)}^2}}}} \right]\left( {\frac{{d{e^ * }}}{{dT_g^n}}} \right)$$</div>
-
-Here, the derivative of the saturation vapor pressure can be calculated from the Clausius-Clapeyron equation:
-
-<div>$$\frac{{d{e^ * }}}{{dT_g^n}} = \frac{{{l_g} * {e^ * }\left( {T_g^n} \right)}}{{\left( {{R_v} * {{\left( {T_g^n} \right)}^2}} \right)}}$$</div>
-
-Where R<sub>v</sub> is the gas constant for water vapor and l<sub>g</sub> is the latent heat of vaporization at the soil surface temperature.
-
-The corresponding saturation mixing ratio relations for the leaf surfaces can be obtained by replacing T<sub>g</sub> with T<sub>f</sub> in the above relations.
-
-### Final Equations
-
-After linearization the final equations are of the form:
-
-<div>$$C_1^f + C_2^f{T_g} + C_3^f{T_f} = 0$$</div>
-
-<div>$$C_1^g + C_2^g{T_g} + C_3^g{T_f} = 0$$</div>
-
-The coefficients in these equations result from the direct combination of the equations from the above development. The interested reader is directed to the papers by Frankenstein and Koenig for the complete and somewhat complicated expressions.
-
-This final set of equations is then solved simultaneously to obtain T*<sub>g</sub>* and T*<sub>f</sub>* . One key difference in our implementation of the FASST algorithm is that the conduction terms in the equations for <span>\(C_1^g\)</span>and <span>\(C_2^g\)</span> are solved by inverting the Conduction Transfer Functions (CTF) within the EnergyPlus solution scheme.
-
-### Green Roof Nomenclature
-
-C<sub>1</sub>, C<sub>2</sub>, C<sub>3</sub>    =          coefficients in linearized temperature equations
-
-*C<sub>e</sub><sup>g</sup>              =         * latent heat flux bulk transfer coefficient at ground layer
-
-*C<sub>f</sub>              * =          bulk heat transfer coefficient
-
-C<sub>h</sub><sup>g</sup>              =          sensible heat flux bulk transfer coefficient at ground layer
-
-C<sub>hn</sub><sup>f</sup>             =          near-neutral transfer coefficient at foliage layer
-
-C<sub>hn</sub><sup>g</sup> =          near-neutral transfer coefficient at ground layer
-
-C<sub>p,a</sub>             =          specific heat of air at constant pressure (1005.6 J/kg k)
-
-e<sup>\*</sup>                =          saturation vapor pressure (Pa)
-
-f<sub>1</sub>                =          multiplying factor for radiation effect on stomatal resistance
-
-f<sub>2</sub>                =          multiplying factor for moisture effect on stomatal resistance
-
-f<sub>3</sub>                =          additional multiplying factor for stomatal resistance
-
-F<sub>f</sub>                =          net heat flux to foliage layer (W/m<sup>2</sup>)
-
-F<sub>g</sub>               =          net heat flux to ground surface (W/m<sup>2</sup>)
-
-g<sub>d</sub>               =          plant specific characteristic related to stomatal resistance
-
-H *<sub>f</sub>*               =          foliage sensible heat flux (W/m<sup>2</sup>)
-
-H<sub>g</sub>               =          ground sensible heat flux (W/m<sup>2</sup>)
-
-<span>\(I_s^ \downarrow \)</span>             =          total incoming short wave radiation (W/m<sup>2</sup>)
-
-<span>\(I_{i\gamma }^ \downarrow \)</span>             =          total incoming longwave radiation (W/m<sup>2</sup>)
-
-K<sub>v</sub>               =          von Karmen constant (0.4)
-
-l<sub>f</sub>                 =          latent heat of vaporization at foliage temperature (J/kg)
-
-l<sub>g</sub>                =          latent heat of vaporization at ground temperature (J/kg)
-
-L*<sub>f</sub>*                =          foliage latent heat flux (W/m<sup>2</sup>)
-
-L<sub>g</sub>               =          ground latent heat flux (W/m<sup>2</sup>)
-
-*LAI*             =          leaf area index (m<sup>2</sup>/m<sup>2</sup>)
-
-M<sub>g</sub>              =          moisture saturation factor
-
-q<sub>a</sub>               =          mixing ratio for air
-
-q<sub>af</sub>               =          mixing ratio for air within foliage canopy
-
-q<sub>f,sat</sub>             =          saturation mixing ratio at foliage temperature
-
-q<sub>g,sat</sub>            =          saturation mixing ratio at ground temperature
-
-r<sub>a</sub>                =          aerodynamic resistance to transpiration (s/m)
-
-r<sub>s</sub>                =          foliage leaf stomatal resistance (s/m)
-
-r<sub>s,min</sub>            =          minimal leaf stomatal resistance (s/m)
-
-r�                =          surface wetness factor
-
-R<sub>ib</sub>              =          bulk Richardson number
-
-R<sub>v</sub>               =          gas constant for water vapor (461.53 J/kgK)
-
-*T<sub>a     \\                        </sub>* =          the air temperature at the instrument height (Kelvin)
-
-T<sub>af     </sub>             =          air temperature with in the canopy (Kelvin)
-
-T*<sub>f</sub>*               =          leaf temperature (Kelvin)
-
-T<sub>g</sub>                =          ground surface temperature (Kelvin)
-
-W               =          wind speed above canopy (m/s)
-
-W<sub>af</sub>              =          wind speed with in the canopy (m/s)
-
-z                 =          height or depth (m)
-
-Z<sub>a</sub>               =          instrument height (m)
-
-Z<sub>d</sub>               =          displacement height (m)
-
-Z<sub>o</sub><sup>f</sup>               =          foliage roughness length scale (m)
-
-#### Greek letters
-
-a<sub>f</sub>                =          albedo (short wave reflectivity) of the canopy
-
-a<sub>g</sub>               =          albedo (short wave reflectivity) of ground surface
-
-<sub><span>\({\varepsilon_1}\)</span></sub>              =          <sub><span>\({\varepsilon_g} + {\varepsilon_f} - {\varepsilon_f}{\varepsilon_g}\)</span></sub>
-
-<sub><span>\({\varepsilon_f}\)</span>  </sub>             =          emissivity of canopy
-
-<sub><span>\({\varepsilon_g}\)</span>  </sub>             =          emissivity of the ground surface
-
-G<sub>h</sub>                    =             stability factor
-
-r<sub>a</sub>               =          density of air at instrument height (kg/m<sup>3</sup>)
-
-r<sub>f</sub>                =          density of air at foliage temperature (kg/m<sup>3</sup>)
-
-r<sub>af</sub>               =          density of air at foliage temperature (kg/m<sup>3</sup>)
-
-r<sub>ag</sub>              =          density of air at ground surface temperature (kg/m<sup>3</sup>)
-
-<span>\(\sigma \)</span>              =          the Stefan-Boltzmann constant (5.699\*10<sup>-8</sup> W/m<sup>2</sup> ºK<sup>4</sup>)
-
-<span>\({\sigma_f}\)</span>                        =          fractional vegetation coverage
-
-#### Subscripts and superscripts
-
-a                =          air
-
-af               =          air within the foliage layer
-
-e                =          latent heat flux term
-
-f                 =          foliage surface
-
-g                =          ground surface
-
-h                =          sensible heat flux term
-
-n                =          current time step
-
-n+1             =          future time step
-
-ir                =          infrared (or long-wave)
-
-sat              =          saturation value
-
-S                =          short-wave
-
-### References
-
-ASHRAE. 2005. 2005 ASHRAE Handbook – Fundamentals. Chapter 16, Air flow Around Buildings, Atlanta: American Society of Heating Refrigerating and Air-Conditioning Engineers, Inc.
-
-Balick, L. R., R. K. Scoggins, and L. E. Link. 1981. Inclusion of a simple vegetation layer in terrain temperature models for thermal IR signature prediction. IEEE Geoscience and Remote Sensing GE-19(3), pp.143-152.
-
-Businger, J. A. 1966. In ‘Arctic Heat Budget and Atmospheric Circulation’, Symposium Proceedings, pp. 305-332. The Rand Corporation.
-
-Deardorff, J.W. 1978. “Efficient Prediction of ground surface temperature and moisture with inclusion of a layer of vegetation�, Journal Geophysical Research, pp. 1889-1902.
-
-Dickinson, R.E., A. Henderson-Sellers, P.J. Kennedy, and M.F. Wilson. 1986. Biosphere-Atmosphere Transfer Scheme (BATS) for the NCAR community climate model. NCAR Technical Note, TN-275+STR.
-
-ECMWF. 2002. European Centre for Medium-Range Weather Forecasts, Integrated Forecast System. Documentation, CY25R1 (Operational implementation 9 April 2002). .
-
-Frankenstein, S., and G. Koenig. 2004.FASST Vegetation Models. U. S. Army Engineer Research and Development Center, Cold regions Research and Engineering Laboratory, ERDC/CRREL Technical Report TR-04-25.
-
-Frankenstein, S., and G. Koenig. 2004.Fast All-season Soil Strength (FASST). U.S. Army Engineer Research and Development Center, Cold regions Research and Engineering Laboratory, ERDC/CRREL Special Report SR-04-1.
-
-Garratt, J.R. 1992. The Atmospheric Boundary Layer, Cambridge university press.
-
-Gates, D.M. 1980. Biophysical Ecology. New York: Springer-Verlag
-
-Guymon, G.L., R.L. Berg, and T.V. Hromadka. 1993. Mathematical Model of Frost Heave and Thaw Settlement in Pavements. U.S. Army Cold Regions Research and Engineering Laboratory, CRREL Report 93-2.
-
-Henderson-Sellers, B. 1984. “A New Formula for Latent Heat of Vaporization of water as function of temperature�, Quarterly Journal Royal Meteorological Society, 10 pp. 1186-1190.
-
-Hughes, P.A., T.J.L. McComb, A.B. Rimmer, and K.E. Turver. 1993. “A mathematical model for the prediction of temperature of man-made and natural surfaces�, International Journal of Remote Sensing 14 (7), pp. 1383-1412.
-
-Koenig, G.G. 1994. Smart Weapons Operability Enhancement (SWOE) Joint Test and Evaluation (JT and E) Program: Final Report. Dr. James P. Welch, Joint Test Director, SWOE JT and E, SWOE Report 94-10, Annex D.
-
-Lumley, J. L. and Panofsky, H. A. 1964. ‘The structure of Atmospheric Turbulence’. Interscience Monographs and Texts in Physics and Astronomy, Vol. XII. Wiley, New York.
-
-Oke, T.R. 1987. Boundary Layer Climates, University Press, Cambridge
-
-Sellers, P.J., Y. Mintz, Y.C. Sud, and A. Dalcher. 1986. A simple biosphere model (SiB) for use within general circulation models. Journal of Atmospheric Science, 43 (6), pp. 505-532.
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-
-Climate, Sky and Solar/Shading Calculations
-===========================================
-
-Climate Calculations
---------------------
-
-The location of the facility under analysis is critical for the determination of energy consumption, heating/cooling loads, daylighting potential, and a host of other calculations. In EnergyPlus, both external (i.e, weather files supplied from others) and internal (i.e., solar position, design day temperature/humidity/solar profiles) data is used during simulations.
-
-The “Site:Location� input object includes parameters (Latitude, Longitude, Elevation, Timezone) that allow EnergyPlus to calculate the solar position (using Latitude, Longitude and Timezone) for any day of the year as well as supply the standard barometric pressure (using elevation). Solar position modeling is discussed in more detail in both the Sky Radiance and Shading Calculation sections that directly follow this section.
-
-Weather files have hourly or sub-hourly data for each of the critical elements needed during the calculations (i.e., Dry-Bulb Temperature, Dew-Point Temperature, Relative Humidity, Barometric Pressure, Direct Normal Radiation, Diffuse Horizontal Radiation, Total & Opaque Sky Cover, Wind Direction, Wind Speed) as well as some auxiliary data such as Rain or Snow that assist in certain calculational aspects. Weather file excerpts such as might be used in sizing calculations also have this breadth of data. The input object “SizingPeriod:DesignDay� describes design days (meant to mimic ASHRAE design conditions but in a whole day profile) using certain characteristics for the day and then EnergyPlus supplies the remaining portions to complete outdoor conditions needed for program execution. SizingPeriod:DesignDay are perhaps the best objects for sizing equipment as the ASHRAE specified design conditions can be input AND weather files may or may not have the conditions necessary to size equipment properly.
-
-Two other objects, however, can be used at times: SizingPeriod:WeatherFileDays and SizingPeriod:WeatherFileConditionType.  With the first of these, one specifies a set of weather file days similar to a RunPeriod (but will be used for the Sizing calculations). In the second, the extreme or typical conditions that are calculated for the weather file during processing can be used by name.  Of course, either of these can be used as a measure of usage over small periods.
-
-The ASHRAE Handbook of Fundamentals describes their criteria in creating design condition synopses. “Design data based on dry-bulb temperature represent peak occurrences of the sensible component of ambient outdoor conditions. Design values based on wet-bulb temperature are related to the enthalpy of the outdoor air. Conditions based on dewpoint relate to the peaks of the humidity ratio. The designer, engineer, or other user must decide which set(s) of conditions and probability of occurrence apply to the design situation under consideration.�
-
-### EnergyPlus Design Day Temperature Calculations
-
-In EnergyPlus, the typical design day input includes a “high� and a “low� dry-bulb temperature for the day. As these two temperatures are insufficient to represent a full 24 hour period, the program uses a “range multiplier� profile to represent the full day’s temperatures:
-
-![](media/image563.svg.png)
-
-Figure 36. Default Daily Temperature Range Profile
-
-The multipliers are taken from the ASHRAE 2009 HOF, Table # 6, p. 14.11.. More explicitly, EnergyPlus creates an air temperature for each timestep by using the entered maximum dry-bulb temperature in conjunction with the entered daily range and the above multiplier values. The actual equation used is shown below:
-
-<div>$${T_{current}} = {T_{Max}} - {T_{range}}\cdot {T_{Multiplier}}$$</div>
-
-where
-
-T<sub>current</sub>= Air temperature of current Hour of Day
-
-T<sub>Max</sub>= User supplied Max Dry-bulb Temperature
-
-T<sub>range</sub>= User supplied Daily Temperature Range
-
-T<sub>Multiplier</sub>= Range multiplier as shown on the above graph
-
-The range multiplier values represent typical conditions of diurnal temperatures (i.e. the low temperature for the day occurring about 5:00 AM and the maximum temperature for the day occurring about 3:00 PM.  Note that EnergyPlus does not shift the profile based on the time of solar noon as is optionally allowed by ASHRAE procedures.
-
-ASHRAE research indicates that dry-bulb and wet-bulb temperatures typically follow the same profile, so EnergyPlus can use the default daily temperature profile to generate humidity conditions based on maximum and range of wet-bulb temperature.
-
-Since this default temperature profile may not be applicable to all locations, the user can give a different profile as part of the design day definition.
-
-### Sky Radiation Modeling
-
-EnergyPlus calculates the Horizontal Infrared Radiation Intensity in Wh/m<sup>2,</sup> if it is missing on the weather file or for design days, from the Opaque Sky Cover field as shown in the following explanation.
-
-<div>$$Horizontal\_IR = Sk{y_{emissivity}}\cdot Sigma\cdot Temperature_{drybulb}^4$$</div>
-
-where
-
-Horizontal\_IR = horizontal IR intensity {W/m<sup>2</sup>}
-
-Sky<sub>emissivity</sub> = sky emissivity
-
-Sigma = Stefan-Boltzmann constant = 5.6697e-8 {W/m<sup>2</sup>-K<sup>4</sup>}
-
-Temperature<sub>drybulb</sub> = drybulb temperature {K}
-
-The sky emissivity is given by
-
-<div>$$Sk{y_{emissivity}} = \left( {.787 + .764\cdot \ln \left( {\frac{{Temperatur{e_{dewpoint}}}}{{273.}}} \right)} \right)\cdot \left( {1. + .0224N - .0035{N^2} + .00028{N^3}} \right)$$</div>
-
-where
-
-Temperature<sub>dewpoint</sub> = dewpoint temperature {K}
-
-N = opaque sky cover {tenths}
-
-Example: Clear sky (N=0), Temperature<sub>drybulb</sub> = 273+20=293 K, Temperature<sub>dewpoint</sub> = 273+10=283 K:
-
-Sky<sub>emissivity</sub> = 0.787 + 0.764\*0.036 = 0.815
-
-Horizontal\_IR = 0.815\*5.6697e-8\*(293\*\*4) = 340.6 W/m<sup>2</sup>
-
-References for these calculations are contained in the references section at the end of this list of fields. (Walton, 1983) (Clark and Allen, 1978).
-
-### EnergyPlus Sky Temperature Calculation
-
-The default calculation for sky temperature is:
-
-<div>$$Sk{y_{Temperature}} = {\left( {\frac{{Horizontal\_IR}}{{Sigma}}} \right)^{.25}} - Temperatur{e_{Kelvin}}$$</div>
-
-Where
-
-Sky<sub>Temperature</sub> = Sky radiative temperature {C}
-
-Horiizontal\_IR = Horizontal Infrared Radiation Intensity as described in the previous section {Wh/m<sup>2</sup>}
-
-Temperature<sub>Kelvin</sub> = Temperature conversion from Kelvin to C, i.e. 273.15
-
-The Sky Temperature can also be set by the user from several options using the **WeatherProperty:SkyTemperature** object.
-
-### EnergyPlus Design Day Solar Radiation Calculations
-
-Similarly, calculating solar irradiance (solar modeling) is one of the important effects to be accomplished. Several solar models exist with varying complexity.
-
-#### ASHRAE Clear Sky Solar Model
-
-The default model used is the ASHRAE Clear Sky model. The ASHRAE clear sky model described in ASHRAE HOF 2005 Chapter 31 can be used to estimate hourly clear-day solar radiation for any month of the year in U.S. or similar temperate climates in the northern hemisphere. EnergyPlus calculations extend the clear sky application to both northern and southern hemispheres.  Note that the Clear Sky model has been updated in the ASHRAE HOF 2009 (see ASHRAE Revised Clear Sky Model below).
-
-At the earth’s surface on a clear day, direct normal irradiation is represented by
-
-<div>$$Direct\;Normal\;Irradiation = \frac{A}{{exp\left( {{\raise0.7ex\hbox{$B$} \!\mathord{\left/ {\vphantom {B {\sin \beta }}}\right.}\!\lower0.7ex\hbox{${\sin \beta }$}}} \right)}}$$</div>
-
-where
-
-*A* = apparent solar irradiation at air mass m = 0 (Table 20)
-
-B = atmospheric extinction coefficient Table 20)
-
-Values of A and B vary during the year because of seasonal changes in the dust and water vapor content of the atmosphere and because of the changing earth-sun distance. Equation does not give the maximum value of direct normal irradiation that can occur in each month but yields values that are representative of conditions on cloudless days for a relatively dry and clear atmosphere. For very clear atmospheres, direct normal irradiation can be 15% higher than indicated by Equation , using values of A and B in Table 20 below.
-
-Table 20. Extraterrestrial Solar Irradiance and Related Data
- Note: Data are for 21st day of each month during the base year of 1964.
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>I<sub>o</sub> {W/m<sup>2</sup>}</th>
-<th>Equation of Time {minutes}</th>
-<th>Declination {degrees}</th>
-<th>A {W/m<sup>2</sup>}</th>
-<th>B {}</th>
-<th>C {}</th>
-</tr>
-<tr>
-<td>Jan</td>
-<td>1416</td>
-<td>-11.2</td>
-<td>-20.0</td>
-<td>1202</td>
-<td>0.141</td>
-<td>0.103</td>
-</tr>
-<tr>
-<td>Feb</td>
-<td>1401</td>
-<td>-13.9</td>
-<td>-10.8</td>
-<td>1187</td>
-<td>0.142</td>
-<td>0.104</td>
-</tr>
-<tr>
-<td>Mar</td>
-<td>1381</td>
-<td>-7.5</td>
-<td>0.0</td>
-<td>1164</td>
-<td>0.149</td>
-<td>0.109</td>
-</tr>
-<tr>
-<td>Apr</td>
-<td>1356</td>
-<td>1.1</td>
-<td>11.6</td>
-<td>1130</td>
-<td>0.164</td>
-<td>0.120</td>
-</tr>
-<tr>
-<td>May</td>
-<td>1336</td>
-<td>3.3</td>
-<td>20.0</td>
-<td>1106</td>
-<td>0.177</td>
-<td>0.130</td>
-</tr>
-<tr>
-<td>Jun</td>
-<td>1336</td>
-<td>-1.4</td>
-<td>23.45</td>
-<td>1092</td>
-<td>0.185</td>
-<td>0.137</td>
-</tr>
-<tr>
-<td>Jul</td>
-<td>1336</td>
-<td>-6.2</td>
-<td>20.6</td>
-<td>1093</td>
-<td>0.186</td>
-<td>0.138</td>
-</tr>
-<tr>
-<td>Aug</td>
-<td>1338</td>
-<td>-2.4</td>
-<td>12.3</td>
-<td>1107</td>
-<td>0.182</td>
-<td>0.134</td>
-</tr>
-<tr>
-<td>Sep</td>
-<td>1359</td>
-<td>7.5</td>
-<td>0.0</td>
-<td>1136</td>
-<td>0.165</td>
-<td>0.121</td>
-</tr>
-<tr>
-<td>Oct</td>
-<td>1380</td>
-<td>15.4</td>
-<td>-10.5</td>
-<td>1166</td>
-<td>0.152</td>
-<td>0.111</td>
-</tr>
-<tr>
-<td>Nov</td>
-<td>1405</td>
-<td>13.8</td>
-<td>-19.8</td>
-<td>1190</td>
-<td>0.144</td>
-<td>0.106</td>
-</tr>
-<tr>
-<td>Dec</td>
-<td>1417</td>
-<td>1.6</td>
-<td>-23.45</td>
-<td>1204</td>
-<td>0.141</td>
-<td>0.103</td>
-</tr>
-
-</table>
-
-For locations where clear, dry skies predominate (e.g., at high elevations) or, conversely, where hazy and humid conditions are frequent, values found by using Equation and Table 20 should be multiplied by the clearness numbers in Threlkeld and Jordan (1958), reproduced as Figure # 5 in Chapter 33 of the 2007 ASHRAE Handbook—HVAC Applications.
-
-The Clear Sky model usually over estimates the amount of solar radiation available to the building.
-
-#### ASHRAE Revised Clear Sky Model (“Tau Model�)
-
-The ASHRAE 2009 HOF introduced a revised clear sky model based on location-specific optical depths for direct and diffuse radiation.  These values are tabulated by month for all 5564 locations in the ASHRAE design data that accompanies the 2009 HOF.
-
-The model requires air mass, m, calculated as follows --
-
-<div>$$m = {1 \mathord{\left/ {\vphantom {1 {\left[ {\sin \beta  + 0.50572 \cdot {{\left( {6.07995 + \beta } \right)}^{ - 1.6364}}} \right]}}} \right. } {\left[ {\sin \beta  + 0.50572 \cdot {{\left( {6.07995 + \beta } \right)}^{ - 1.6364}}} \right]}}$$</div>
-
-where <span>\(\beta \)</span> = solar altitude, degrees.
-
-Direct and diffuse irradiance are determined with the following relationships,
-
-<div>$${E_b} = {E_o} \cdot \exp \left[ { - {\tau_b} \cdot {m^{ab}}} \right]$$</div>
-
-<div>$${E_d} = {E_o} \cdot \exp \left[ { - {\tau_d} \cdot {m^{ad}}} \right]$$</div>
-
-where:
-
-<span>\({E_b}\)</span> = beam normal irradiance, W/m<sup>2</sup>
-
-<span>\({E_d}\)</span> = diffuse horizontal irradiance,
-
-<span>\({E_o}\)</span> = extraterrestrial normal irradiance,
-
-*<span>\(m\)</span>* = air mass
-
-t<sub>b</sub> and t<sub>d</sub> = beam and diffuse optical depths (from ASHRAE climatic design data)
-
-<span>\(ab\)</span> and <span>\(ad\)</span> = beam and diffuse air mass exponents (see below)
-
-Values of t<sub>b</sub> and t<sub>d</sub> are location-specific and vary during the year. They embody the dependence of clear sky solar radiation upon local conditions, such as elevation, precipitable water content, and aerosols.
-
-The air mass exponents <span>\(ab\)</span> and <span>\(ad\)</span> were correlated to t<sub>b</sub> and t<sub>d</sub> through the following empirical relationships:
-
-<div>$$ab = 1.219 - 0.043 \cdot {\tau_b} - 0.151 \cdot {\tau_d} - 0.204 \cdot {\tau_b} \cdot {\tau_d}$$</div>
-
-<div>$$ad = 0.202 + 0.852 \cdot {\tau_b} - 0.007 \cdot {\tau_d} - 0.357 \cdot {\tau_b} \cdot {\tau_d}$$</div>
-
-Studies done as part of ASHRAE research projects show that the revised tau model produces more physically plausible irradiance values than does the traditional clear sky model.  In particular, diffuse irradiance values are more realistic.
-
-#### Zhang-Huang Solar Model
-
-The Zhang-Huang solar model was developed for initial use in modeling typical meteorological years for China weather sites. This model seems to be good for other locations as well. Using total cloud cover, dry-bulb temperature, relative humidity, and wind speed as the independent variables, the total (global horizontal) solar radiation is estimated by:
-
-<div>$$I = \frac{{\left[ {{I_0}\cdot \sin (h)\cdot \left( {{c_0} + {c_1}\cdot CC + {c_2}\cdot C{C^2} + {c_3}\left( {{T_n} - {T_{n - 3}}} \right) + {c_4}\cdot \varphi  + {c_5}\cdot {V_w}} \right) + d} \right]}}{k}$$</div>
-
-Where
-
-I = estimated hourly solar radiation, W/m<sup>2</sup>
-
-I<sub>0</sub>= global solar constant, 1355 W/m<sup>2</sup>
-
-h=solar altitude angle, i.e, the angle between the horizontal and the line to the sun
-
-CC = cloud cover
-
-<span>\(\varphi \)</span> = relative humidity, %
-
-<span>\({T_n},{T_{n - 3}}\)</span> = dry-bulb temperature at hours n (current) and n-3, respectively
-
-<span>\({V_w}\)</span> = Wind speed, m/s
-
-<span>\({c_0},{c_1},{c_2},{c_3},{c_4},{c_5},d,k\)</span> = regression coefficients
-
-The constants were determined by analysis from measured data and are as follows:
-
-c<sub>0</sub> = .5598, c<sub>1</sub> = .4982, c<sub>2</sub> = -.6762, c<sub>3</sub> = .02842, c<sub>4</sub> = -.00317, c<sub>5</sub> = .014,
- d = -17.853, k = .843.
-
-This is the same model used to estimate the global solar radiation value (when it is absent from the source data) in the Weather Converter. References given in the reference section (Watanabe, Urano, Hayashi, 1983) (Zhang, Huang, 2002).
-
-### Perez Direct/Diffuse Splitting Model
-
-Splitting from global calculated (EnergyPlus) or entered values (WeatherConverter) into direct normal and diffuse horizontal components are done using the Perez direct/diffuse split. References shown in the reference section (Perez et al, 1992) (Perez et al, 1990)
-
-### Weather File Solar Interpolation
-
-The solar values on the weather file are average values over the hour. For interpolation of hourly weather data (i.e., when the specified timestep is greater than 1), the average value is assumed to be the value at the midpoint of the hour.  The reported values in the output are totals for each reporting period. So, hourly reported values will not match the original values in the weather file, but the total solar for a day should agree. Reference (Ellis, Liesen, Pedersen, 2003)
-
-### References
-
-Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards, p. 21.
-
-Clark, G. and C. Allen, "The Estimation of Atmospheric Radiation for Clear and Cloudy Skies," Proceedings 2nd National Passive Solar Conference (AS/ISES), 1978, pp. 675-678.
-
-Watanabe, T., Urano, Y., and Hayashi, T. 1983. "Procedures for Separating Direct and Diffuse Insolation on a Horizontal Surface and Prediction of Insolation on Tilted Surfaces" (in Japanese), Transactions, No. 330, Architectural Institute of Japan, Tokyo, Japan.
-
-Zhang, Q.Y. and Huang, Y.J. 2002. Development of typical year weather files for Chinese locations, LBNL-51436, ASHRAE Transactions, Vol. 108, Part 2.
-
-Perez R., Ineichen P., Maxwell E., Seals, R. and Zelenka, A. 1992. Dynamic Global-to-Direct Irradiance Conversion Models. ASHRAE Transactions-Research Series,354-369.
-
-Perez, R., Ineichen, P., Seals, R., Michalsky, J. and Stewart, R. 1990. Modeling daylight availability and irradiance components from direct and global irradiance. Solar Energy 44, 271-289.
-
-Ellis, P.G., Liesen, R.J. and Pedersen, C.O. 2003. “Energyplus Experimental Data Validation Work: Development and Validation of the Unvented Trombe Wall Model and Other Heat Balance Components�, CERL Final Report DACA42-01-D-0004, Task 3.
-
-Design Week Specification
--------------------------
-
-A design week (or longer) may be specified in EnergyPlus by selecting a RunPeriod of one week.  One-week custom weather files may be constructed if extreme design week conditions are desired or one can use the specific dates from the EPW weather files that designate the extreme conditions on the weather file.  The design week simulation requires that the simulation reach a ‘steady-periodic’ state for the one week time period.  This is achieved manually by increasing the ‘number of years of simulation’ until the weekly profile does not change from one year to the next.  The ‘steady-periodic’ output for the last week of the simulation represents the design week simulation results.
-
-Using the SizingPeriod:WeatherFileDays object, one could size equipment from a longer period.
-
-Sky Radiance Model
-------------------
-
-In EnergyPlus the calculation of diffuse solar radiation from the sky incident on an exterior surface takes into account the anisotropic radiance distribution of the sky. For this distribution, the diffuse sky irradiance on a surface is given by
-
-<div>$$AnisoSkyMultiplie{r_{surface}}\cdot DiffuseSolarIrradiance$$</div>
-
-Where
-
-Diffuse Solar Irradiance is the diffuse solar irradiance from the sky on the ground.
-
-surface is the surface being analyzed.
-
-AnisoSkyMultiplier is determined by surface orientation and sky radiance distribution, and accounts for the effects of shading of sky diffuse radiation by shadowing surfaces such as overhangs. It does not account for *reflection* of sky diffuse radiation from shadowing surfaces.
-
-The sky radiance distribution is based on an empirical model based on radiance measurements of real skies, as described in Perez et al., 1990. In this model the radiance of the sky is determined by three distributions that are superimposed (see Figure 37)
-
-(1) An isotropic distribution that covers the entire sky dome;
-
-(2) A circumsolar brightening centered at the position of the sun;
-
-(3) A horizon brightening.
-
-![](media/image589.png)
-
-Figure 37. Schematic view of sky showing solar radiance distribution as a superposition of three components: dome with isotropic radiance, circumsolar brightening represented as a point source at the sun, and horizon brightening represented as a line source at the horizon.
-
-The proportions of these distributions depend on the sky condition, which is characterized by two quantities, *clearness factor* and *brightness factor*, defined below, which are determined from sun position and solar quantities from the weather file.
-
-The *circumsolar brightening* is assumed to be concentrated at a point source at the center of the sun although this region actually begins at the periphery of the solar disk and falls off in intensity with increasing angular distance from the periphery.
-
-The *horizon brightening* is assumed to be a linear source at the horizon and to be independent of azimuth. In actuality, for clear skies, the horizon brightening is highest at the horizon and decreases in intensity away from the horizon. For overcast skies the horizon brightening has a negative value since for such skies the sky radiance increases rather than decreases away from the horizon.
-
-Table 21.  Variables in Anisotropic Sky Model and Shadowing of Sky Diffuse Radiation
-
-<table class="table table-striped">
- <tr>
-  <th>Mathematical variable</th>
-  <th>Description</th>
-  <th>Units</th>
-  <th>FORTRAN variable</th>
- </tr>
- <tr>
-  <td>I<sub>sky</sub></td>
-  <td>Solar irradiance on surface from sky</td>
-  <td>W/m<sup>2</sup></td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>I<sub>horizon</sub></td>
-  <td>Solar irradiance on surface from sky horizon</td>
-  <td>W/m<sup>2</sup></td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>I<sub>dome</sub></td>
-  <td>Solar irradiance on surface from sky dome</td>
-  <td>W/m<sup>2</sup></td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>I<sub>circumsolar</sub></td>
-  <td>Solar irradiance on surface from circumsolar region</td>
-  <td>W/m<sup>2</sup></td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>I<sub>h</sub></td>
-  <td>Horizontal solar irradiance</td>
-  <td>W/m<sup>2</sup></td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>S</td>
-  <td>Surface tilt</td>
-  <td>radians</td>
-  <td>Surface(SurfNum)%Tilt\*DegToRadians</td>
- </tr>
- <tr>
-  <td>a, b</td>
-  <td>intermediate variables</td>
-  <td>-</td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>F<sub>1</sub>, F<sub>2</sub></td>
-  <td>Circumsolar and horizon brightening coefficients</td>
-  <td>-</td>
-  <td>F1, F2</td>
- </tr>
- <tr>
-  <td>α</td>
-  <td>Incidence angle of sun on surface</td>
-  <td>radians</td>
-  <td>IncAng</td>
- </tr>
- <tr>
-  <td>Z</td>
-  <td>Solar zenith angle</td>
-  <td>radians</td>
-  <td>ZenithAng</td>
- </tr>
- <tr>
-  <td><div>$\Delta$</div></td>
-  <td>Sky brightness factor</td>
-  <td>-</td>
-  <td>Delta</td>
- </tr>
- <tr>
-  <td>ε</td>
-  <td>Sky clearness factor</td>
-  <td>-</td>
-  <td>Epsilon</td>
- </tr>
- <tr>
-  <td>m</td>
-  <td>relative optical air mass</td>
-  <td>-</td>
-  <td>AirMass</td>
- </tr>
- <tr>
-  <td>I<sub>O</sub></td>
-  <td>Extraterrestrial solar irradiance</td>
-  <td>W/m<sup>2</sup></td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>I</td>
-  <td>Direct normal solar irradiance</td>
-  <td>W/m<sup>2</sup></td>
-  <td>Material%Thickness</td>
- </tr>
- <tr>
-  <td>κ</td>
-  <td>constant = 1.041 for Z in radians</td>
-  <td>radians<sup>-3</sup></td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>F<sub>ij</sub></td>
-  <td>Brightening coefficient factors</td>
-  <td>-</td>
-  <td>F11R, F12R, etc.</td>
- </tr>
- <tr>
-  <td>R<sub>circumsolar</sub></td>
-  <td>Shadowing factor for circumsolar radiation</td>
-  <td>-</td>
-  <td>SunLitFrac</td>
- </tr>
- <tr>
-  <td>R<sub>dome</sub></td>
-  <td>Shadowing factor for sky dome radiation</td>
-  <td>-</td>
-  <td>DifShdgRatioIsoSky</td>
- </tr>
- <tr>
-  <td>R<sub>horizon</sub></td>
-  <td>Shadowing factor for horizon radiation</td>
-  <td>-</td>
-  <td>DifShdgRatioHoriz</td>
- </tr>
- <tr>
-  <td>E</td>
-  <td>Sky radiance</td>
-  <td>W/m<sup>2</sup></td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>*θ*</td>
-  <td>Azimuth angle of point in sky</td>
-  <td>radians</td>
-  <td>Theta</td>
- </tr>
- <tr>
-  <td>φ</td>
-  <td>Altitude angle of point in sky</td>
-  <td>radians</td>
-  <td>Phi</td>
- </tr>
- <tr>
-  <td>I<sub>i</sub></td>
-  <td>Irradiance on surface from a horizon element</td>
-  <td>W/m<sup>2</sup></td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>I<sub>ij</sub></td>
-  <td>Irradiance on surface from a sky dome element</td>
-  <td>W/m<sup>2</sup></td>
-  <td>-</td>
- </tr>
- <tr>
-  <td>SF</td>
-  <td>Sunlit fraction</td>
-  <td>-</td>
-  <td>FracIlluminated</td>
- </tr>
- <tr>
-  <td>I’</td>
-  <td>Sky solar irradiance on surface with shadowing</td>
-  <td>W/m<sup>2</sup></td>
-  <td>-</td>
- </tr>
-</table>
-
-### Sky Diffuse Solar Radiation on a Tilted Surface
-
-The following calculations are done in subroutine AnisoSkyViewFactors in the SolarShading module.
-
-In the absence of shadowing, the sky formulation described above gives the following expression for sky diffuse irradiance, *I<sub>sky</sub>*, on a tilted surface:
-
-<div>$${I_{sky}} = {I_{horizon}} + {I_{dome}} + {I_{circumsolar}}$$</div>
-
-where
-
-<div>$$
-  \begin{array}{rcl}
-    I_{horizon} &= \rm{irradiance on surface from sky horizon} &= I_h F_2\sin S \\
-    I_{dome}    &= \rm{irradiance on surface from sky dome}    &= I_h (1 - F_1)(1 + \cos S)/2 \\
-    I_{circumsolar} &= \rm{irradiance on surface from circumsolar region} &= I_h F_1 a/b
-  \end{array}
-$$</div>
-
-AnisoSkyMult is then *I<sub>sky</sub>* /DifSolarRad.
-
-In the above equations:
-
-I<sub>h</sub> = horizontal solar irradiance (W/m<sup>2</sup>)
-
-*S* = surface tilt (radians)
-
-*a* = max(0,cos*α*)
-
-*b* = max(0.087, cos*Z*)
-
-*F<sub>1</sub>* = circumsolar brightening coefficient
-
-*F<sub>2</sub>* = horizon brightening coefficient
-
-where
-
-*α* = incidence angle of sun on the surface (radians)
-
-*Z* = solar zenith angle (radians).
-
-The brightening coefficients are a function of sky conditions; they are given by
-
-<div>$$
-  \begin{array}{rl}
-    F_1 &= F_{11}(\varepsilon ) + F_{12}(\varepsilon )\Delta  + F_{13}(\varepsilon )Z  \\
-    F_2 &= F_{21}(\varepsilon ) + F_{22}(\varepsilon )\Delta  + F_{23}(\varepsilon )Z
-  \end{array}
-$$</div>
-
-Here the sky brightness factor is
-
-<div>$$\Delta  = {I_h}m/{I_o}$$</div>
-
-where
-
-*m* = relative optical air mass
-
-*I<sub>o</sub>* = extraterrestrial irradiance (taken to have an average annual value of 1353 W/m<sup>2</sup>);
-
-and the sky *clearness factor* is
-
-<div>$$\varepsilon  = \frac{{({I_h} + I)/{I_h} + \kappa {Z^3}}}{{1 + \kappa {Z^3}}}$$</div>
-
-where
-
-I = direct normal solar irradiance
-
-κ = 1.041 for Z in radians
-
-The factors *F<sub>ij</sub>*  are shown in the following table. The F<sub>ij</sub> values in this table were provided by R. Perez, private communication, 5/21/99. These values have higher precision than those listed in Table # 6 of Perez et al., 1990.
-
-Table 22.  F<sub>ij</sub> Factors as a Function of Sky Clearness Range.
-
-<table class="table table-striped">
-<tr>
-<th>ε  Range</th>
-<th>1.000-1.065</th>
-<th>1.065-1.230</th>
-<th>1.230-1.500</th>
-<th>1.500-1.950</th>
-<th>1.950-2.800</th>
-<th>2.800-4.500</th>
-<th>4.500-6.200</th>
-<th>&gt; 6.200</th>
-</tr>
-<tr>
-<td>F<sub>11</sub></td>
-<td>-0.0083117</td>
-<td>0.1299457</td>
-<td>0.3296958</td>
-<td>0.5682053</td>
-<td>0.8730280</td>
-<td>1.1326077</td>
-<td>1.0601591</td>
-<td>0.6777470</td>
-</tr>
-<tr>
-<td>F<sub>12</sub></td>
-<td>0.5877285</td>
-<td>0.6825954</td>
-<td>0.4868735</td>
-<td>0.1874525</td>
-<td>-0.3920403</td>
-<td>-1.2367284</td>
-<td>-1.5999137</td>
-<td>-0.3272588</td>
-</tr>
-<tr>
-<td>F<sub>13</sub></td>
-<td>-0.0620636</td>
-<td>-0.1513752</td>
-<td>-0.2210958</td>
-<td>-0.2951290</td>
-<td>-0.3616149</td>
-<td>-0.4118494</td>
-<td>-0.3589221</td>
-<td>-0.2504286</td>
-</tr>
-<tr>
-<td>F<sub>21</sub></td>
-<td>-0.0596012</td>
-<td>-0.0189325</td>
-<td>0.0554140</td>
-<td>0.1088631</td>
-<td>0.2255647</td>
-<td>0.2877813</td>
-<td>0.2642124</td>
-<td>0.1561313</td>
-</tr>
-<tr>
-<td>F<sub>22</sub></td>
-<td>0.0721249</td>
-<td>0.0659650</td>
-<td>-0.0639588</td>
-<td>-0.1519229</td>
-<td>-0.4620442</td>
-<td>-0.8230357</td>
-<td>-1.1272340</td>
-<td>-1.3765031</td>
-</tr>
-<tr>
-<td>F<sub>23</sub></td>
-<td>-0.0220216</td>
-<td>-0.0288748</td>
-<td>-0.0260542</td>
-<td>-0.0139754</td>
-<td>0.0012448</td>
-<td>0.0558651</td>
-<td>0.1310694</td>
-<td>0.2506212</td>
-</tr>
-
-</table>
-
-### Shadowing of Sky Diffuse Solar Radiation
-
-Sky diffuse solar shadowing on an exterior surface is calculated as follows in subroutine SkyDifSolarShading in the SolarShading module. The sky is assumed to be a superposition of the three Perez sky comp1onents described above.
-
-For the horizon source the following ratio is calculated by dividing the horizon line into 24 intervals of equal length:
-
-<div>$${R_{horiz}} = \frac{{{\rm{Irradiance from horizon with obstructions}}}}{{{\rm{Irradiance from horizon without obstructions}}}} = \frac{{\sum\limits_{i = 1}^{24} {{I_i}S{F_i}} }}{{\sum\limits_{i = 1}^{24} {{I_i}} }}$$</div>
-
-where* I<sub>i</sub>*is the unobstructed irradiance on the surface from the* i*<sup>th</sup> interval, *SF<sub>i</sub>* is the sunlit fraction from radiation coming from the *i*<sup>th</sup> interval, and the sums are over intervals whose center lies in front of the surface. *SF<sub>i</sub>* is calculated using the beam solar shadowing method as though the sun were located at the *i*<sup>th</sup> horizon point. Here
-
-<div>$${I_i} = E({\theta_i})d\theta \cos {\alpha_i}$$</div>
-
-where
-
-*E* (*θ<sub>i</sub>*) = radiance of horizon band (independent of θ)
-
-*dθ* = 2π/24 = azimuthal extent of horizon interval (radians)
-
-*θ<sub>i</sub>* = 0<sup>O</sup>, 15<sup>O</sup>, … , 345<sup>O</sup>
-
-α<sub>i</sub> = incidence angle on surface of radiation from *θ<sub>i</sub>*
-
-The corresponding ratio for the isotropic sky dome is given by
-
-<div>$${R_{dome}} = \frac{{{\rm{Irradiance from dome with obstructions}}}}{{{\rm{Irradiance from dome without obstructions}}}} = \frac{{\sum\limits_{i = 1}^{24} {\sum\limits_{j = 1}^6 {{I_{ij}}S{F_{ij}}} } }}{{\sum\limits_{i = 1}^{24} {\sum\limits_{j = 1}^6 {{I_{ij}}} } }}$$</div>
-
-where (*i,j*) is a grid of 144 points (6 in altitude by 24 in azimuth) covering the sky dome, *I<sub>ij</sub>* is the unobstructed irradiance on the surface from the sky element at the *ij*<sup>th</sup> point, *SF<sub>ij</sub>* is the sunlit fraction for radiation coming from the *ij*<sup>th</sup> element, and the sum is over points lying in front of the surface. Here
-
-<div>$${I_{ij}} = E({\theta_i},{\phi_j})\cos {\phi_j}d\theta d\phi \cos {\alpha_{ij}}$$</div>
-
-where
-
-*E* (*θ<sub>i</sub>*,*φ<sub>j</sub>*) = sky radiance (independent of θ and φ for isotropic dome)
-
-*dθ* = 2π/24 = azimuthal extent of sky element (radians)
-
-*dφ* = (π/2)/6 = altitude extent of sky element (radians)
-
-*θ<sub>i</sub>* = 0<sup>O</sup>, 15<sup>O</sup>, … , 345<sup>O</sup>
-
-*φ<sub>j</sub>*= 7.5<sup>O</sup>, 22.5<sup>O</sup>, … , 82.5<sup>O</sup>
-
-α<sub>ij</sub> = incidence angle on surface of radiation from (*θ<sub>i</sub>*,*φ<sub>j</sub>*)
-
-Because the circumsolar region is assumed to be concentrated at the solar disk, the circumsolar ratio is
-
-<div>$${R_{circumsolar}} = \frac{{{\rm{Irradiance from circumsolar region with obstructions}}}}{{{\rm{Irradiance from circumsolar without obstructions}}}} = S{F_{sun}}$$</div>
-
-where *SF<sub>sun</sub>* is the beam sunlit fraction. The total sky diffuse irradiance on the surface with shadowing is then
-
-<div>$${I'_{sky}} = {R_{horizon}}{I_{horizon}} + {R_{dome}}{I_{dome}} + {R_{circumsolar}}{I_{circumsolar}}$$</div>
-
-*R<sub>horizon</sub>* and *R<sub>dome</sub>* are calculated once for each surface since they are independent of sun position.
-
-With shadowing we then have:
-
-AnisoSkyMult = *I’<sub>sky</sub>* /DifSolarRad.
-
-### Shadowing of Sky Long-Wave Radiation
-
-EnergyPlus calculates the sky long-wave radiation incident on exterior surfaces assuming that the sky long-wave radiance distribution is isotropic. If obstructions such as overhangs are present the sky long-wave incident on a surface is multiplied by the isotropic shading factor, *R<sub>dome</sub>*, described above. The long-wave radiation from these obstructions is added to the long-wave radiation from the ground; in this calculation both obstructions and ground are assumed to be at the outside air temperature and to have an emissivity of 0.9.
-
-Shading Module
---------------
-
-### Shading and Sunlit Area Calculations
-
-When assessing heat gains in buildings due to solar radiation, it is necessary to know how much of each part of the building is shaded and how much is in direct sunlight. As an example, the figure below shows a flat roofed, L-shaped structure with a window in each of the visible sides. The sun is to the right so that walls 1 and 3 and windows a and c are completely shaded, and wall 4 and window d are completely sunlit. Wall 2 and window b are partially shaded. The sunlit area of each surface changes as the position of the sun changes during the day. The purpose of the EnergyPlus shadow algorithm is to compute these **sunlit areas**.  Predecessors to the EnergyPlus shadowing concepts include the BLAST and TARP shadowing algorithms.
-
-The shadow algorithm is based on coordinate transformation methods similar to Groth and Lokmanhekim and the shadow overlap method of Walton.
-
-Using the **ShadowCalculation** object, you can set how often the shadowing calculations are performed. Having them calculated each day is obviously the most accurate but may also be the most time consuming.  Using a greater length of time (number of days) before calculating again can yield speedier results.  For lengths of time greater than one day, the solar position values (e.g. equation of time, sun position angles) are averaged over that time period for the shadowing calculations.
-
-![](media/image601.png)
-
-Figure 38.  Overall Shadowing Scheme Depiction
-
-### Solar Position
-
-Current solar position is described in terms of three direction cosines that are convenient for determining the angle of incidence of the sun’s rays on a building surface.  The following procedure is used to determine the direction cosines.  The values of the solar declination angle, d, and the equation of time, e, are based on *Astronomical Algorithms*, Meeus.  Solar declination is a function of local/site latitude.
-
-The fractional year is calculated, in radians:
-
-<div>$$\gamma  = \frac{{2\pi }}{{366}}(day\_of\_year)$$</div>
-
-From this fractional year, the equation of time and solar declination angle are calculated.  For each time step (time value = fractional hour), the hour angle is calculated from:
-
-<div>$$HourAngle = \left( {15\cdot \left( {12 - \left( {TimeValue + EquationOfTime} \right)} \right) + \left( {TimeZoneMeridian - Longitude} \right)} \right)$$</div>
-
-TimeZoneMeridian is the standard meridian for the location’s time zone {GMT +/-}.
-
-Solar HourAngle (*H*) gives the apparent solar time for the current time period (degrees); HourAngle is positive before noon, negative after noon.  It is common astronomical practice to express the hour angle in hours, minutes and seconds of time rather than in degrees.  You can convert the hour angle displayed from EnergyPlus to time by dividing by 15.  (Note that 1 hour is equivalent to 15 degrees; 360° of the Earth’s rotation takes place every 24 hours.)  The relationship of angles in degrees to time is shown in the following table:
-
-Table 23.  Relationship of Angles (degrees) to Time
-
-<table class="table table-striped">
-<tr>
-<th>Unit of Angle</th>
-<th>Equivalent time</th>
-</tr>
-<tr>
-<td>1 radian</td>
-<td>3.819719 hours</td>
-</tr>
-<tr>
-<td>1 degree</td>
-<td>4 minutes</td>
-</tr>
-<tr>
-<td>1 arcmin</td>
-<td>4 seconds</td>
-</tr>
-<tr>
-<td>1 arcsec</td>
-<td>0.066667 seconds</td>
-</tr>
-
-</table>
-
-The Solar Altitude Angle (b) is the angle of the sun above the horizontal (degrees).  The Solar Azimuth Angle (f) is measured from the North (clockwise) and is expressed in degrees.  This is shown more clearly in the following figure.
-
-![](media/image604.png)
-
-Figure 39.  Solar Position Illustration
-
-### Surface Geometry
-
-Shadow calculations first require that the building surfaces be described geometrically. Surfaces are described by the coordinates of their vertices in a three dimensional Cartesian coordinate system. This Right-hand coordinate system has the X-axis pointing east, the Y-axis pointing north, and the Z-axis pointing up (see figure below). The azimuth angle (y) of a surface is the angle from the north axis to the projection onto the X-Y plane of a normal to the surface (clockwise positive). The surface tilt angle (f) is the angle between the Z-axis and the normal to the surface. The vertices are recorded in counter-clockwise sequence (as the surface is viewed from outside its zone).
-
-During surface entry, surfaces are checked for convex or non-convex shape. If non-convex and inappropriate (used as a receiving surface) then a severe error is produced telling the user that shadowing calculations may be inaccurate.
-
-Similarly collinear points (or as noted below, points within 1 mm distance) are removed unless removing would make an illegal surface (less than 3 points). But degenerate collinear surfaces *should* be removed – they make the shadowing routines do extra work which takes extra time.
-
-Collinear – points that essentially form a “line� rather than a surface shape.
-
-Resolution of 1mm or less – near collinear points.
-
-Note that the resolution on surfaces/shadowing is 1 mm – using resolution beyond that will result in truncation of the shadowing.
-
-![](media/image605.png)
-
-Figure 40.  EnergyPlus Coordinate System
-
-The GlobalGeometryRules object specifies to EnergyPlus how the surface vertices will be presented in the input file.  Of pertinent interest here is that the user may specify the vertices in either “relative� or “world� coordinates.  Regardless of input specifications, when vertices are reported, they are reported in world coordinates, starting at the upper-left-corner (4-sided surface) and are listed counter-clockwise.
-
-#### Relative Coordinate Transformation
-
-When vertices are specified in “relative� coordinates, there can be a “building� north axis as well as a “zone� north axis.  The building north axis/coordinate system is a rotation of y<sub>b</sub> degrees from the global/world coordinate system.  The global coordinates of zone origins are related to the building relative coordinates by:
-
-<div>$${X_{zo}} = {X_{br}}\cdot \cos {\psi_b} - {Y_{br}}\cdot \sin {\psi_b}$$</div>
-
-<div>$${Y_{zo}} = {Y_{br}}\cdot \sin {\psi_b} - {Y_{br}}\cdot \cos {\psi_b}$$</div>
-
-<div>$${Z_{zo}} = {Z_{br}}$$</div>
-
-Where
-
-zo – represents Zone Origin
-
-br – represents the Zone Origin as input (relative to building origin)
-
-The zone may also be rotated y<sub>z</sub> degrees relative to the building coordinates. Origins of zone surfaces are then given relative to the zone coordinate system. The global coordinates of the surface origins are calculated by:
-
-<div>$${X_{so}} = {X_{zo}} + {X_{zr}}\cdot \cos {\psi_z} - {Y_{zr}}\cdot \sin {\psi_z}$$</div>
-
-<div>$${Y_{so}} = {Y_{zo}} + {X_{zr}}\cdot \sin {\psi_z} - {Y_{zr}}\cdot \cos {\psi_z}$$</div>
-
-<div>$${X_{so}} = {X_{zo}} + {X_{zr}}\cdot \cos {\psi_z} - {Y_{zr}}\cdot \sin {\psi_z}$$</div>
-
-A surface azimuth angle relative to the zone coordinate system (y<sub>s</sub>) is converted to a global azimuth by:
-
-<div>$$\psi  = {\psi_s} + {\psi_z} + {\psi_b}$$</div>
-
-The surface tilt angle (f) is not changed by these rotations about the Z-axis.
-
-The coordinates of the surface vertices are given in a coordinate system in the plane of the surface relative to the second vertex as shown for surfaces in Figure 40. The X-axis of the surface coordinate system is a horizontal line through the second vertex. The global coordinates of the surface vertices are given by:
-
-<div>$$X = {X_{so}} + {X_{sr}}\cdot \cos \psi  - {Y_{sr}}\cdot \sin \psi \cdot \cos \phi $$</div>
-
-<div>$$Y = {Y_{so}} + {X_{sr}}\cdot \sin \psi  - {Y_{sr}}\cdot \cos \psi \cdot \cos \phi $$</div>
-
-<div>$$Z = {Z_{so}} + {Y_{sr}}\cdot \sin \phi $$</div>
-
-#### World Coordinates è Relative Coordinates
-
-Vertices in the global coordinate system can be transformed to the coordinate system relative to a given surface by
-
-<div>$${X'} = X - {X_{so}}$$</div>
-
-<div>$${Y'} = Y - {Y_{so}}$$</div>
-
-<div>$${Z'} = Z - {Z_{so}}$$</div>
-
-<div>$${X_{sr}} =  - {X'}\cdot \cos \psi  + {Y'}\cdot \sin \psi $$</div>
-
-<div>$${Y_{sr}} =  - {X'}\cdot \sin \psi \cdot \cos \phi  + {Y'}\cdot \cos \psi \cdot \cos \phi  + {Z'}\cdot \sin \phi $$</div>
-
-<div>$${Z_{sr}} =  - {X'}\cdot \sin \psi \cdot \sin \phi  + {Y'}\cdot \cos \psi \cdot \sin \phi  + {Z'}\cdot \cos \phi $$</div>
-
-### Shadow Projection
-
-All architectural forms are represented by plane polygons. This can give good accuracy even for curved surfaces: a sphere can be approximated by the 20 nodes of an icosahedron with only 3 percent error in the shadow area cast by the sphere. Consider how a solid object, which is composed of a set of enclosing plane polygons, casts a shadow. Figure 41 shows a box shaped structure on a horizontal surface. The structure consists of a top (surface 1) and four vertical surfaces (2 and 3 visible to the observer and 4 and 5 not visible). The sun is positioned behind and to the right of the structure and a shadow is cast onto the horizontal surface (the ground).
-
-Surfaces 1, 4, and 5 are in sunlight; 2 and 3 are in shade. It is possible to think of the structure's shadow as the combination of shadows cast by surfaces 1, 2, 3, 4 and 5 or by 1, 4 and 5, or by surfaces 2 and 3.  This last combination of shadow casting surfaces is the simplest. In the EnergyPlus shadow algorithm every surface is considered to be one of the surfaces that enclose a solid, and only those surfaces that are not sunlit at a given hour are considered shadowing surfaces.
-
-![](media/image622.png)
-
-Figure 41.  Basic shadowing concept structure
-
-The expressions in equation are the direction cosines of the surface:
-
-<div>$$C{W_1} = \sin \psi \cdot \cos \phi $$</div>
-
-<div>$$C{W_2} = \cos \psi \cdot \sin \phi $$</div>
-
-<div>$$C{W_3} = \cos \phi $$</div>
-
-The cosine of the angle of incidence of the sun's rays on the surface are given by the dot product of surface and sun direction cosines.
-
-<div>$$\cos \theta  = C{S_1}\cdot C{W_1} + C{S_2}\cdot C{W_2} + C{S_3}\cdot C{W_3}$$</div>
-
-If <span>\(\cos \theta \)</span> is less than zero, the sun is behind the surface.
-
-A shadow is projected from the vertices of the shadowing polygon (SP) along the direction of the sun's rays to the plane of the shadow receiving polygon (RP).  If any vertices of the SP are below the plane of the RP (z &lt; 0), a false shadow is cast as in Figure 42.  The "submerged" portion of the SP must be clipped off before projection.
-
-![](media/image628.png)
-
-Figure 42.  Illustration of Shadow Clipping
-
-This is done by finding, through linear interpolation, the points on the perimeter of the SP, which intersect the plane of the RP. These points become new vertices of the SP, which together with the other positive vertices define a clipped SP that casts only a real shadow.
-
-A vertex located at (x, y, z) relative to the RP coordinate system casts a shadow to a point in the plane of the RP given by
-
-<div>$${x'} = x - \frac{{z\cdot a}}{{\cos \theta }}$$</div>
-
-<div>$${y'} = y - \frac{{z\cdot b}}{{\cos \theta }}$$</div>
-
-where
-
-<div>$$a = \sin \psi \cdot C{S_1} - \cos \psi \cdot C{S_2}$$</div>
-
-and
-
-<div>$$b =  - \cos \psi \cdot \cos \phi \cdot C{S_1} - \sin \psi \cdot \cos \phi \cdot C{S_2} + \sin \phi \cdot C{S_3}$$</div>
-
-More explicitly, a casting surface – a shadow casting surface or general casting surface – is one that casts a shadow on other surfaces. A receiving surface – a shadow receiving surface – is one that receives shadows from other surfaces (i.e. casting surfaces). A back surface – an inside surface – is one that may be partially sunlit/receive solar transmission for interior solar distribution.
-
-### Homogeneous Coordinates
-
-Two-dimensional homogeneous coordinate techniques are used to determine the vertices of shadow overlaps. In homogeneous coordinates, points and lines are represented by a single form that allows simple vector operations between those forms [Newman-Sproul].  A point (X, Y) is represented by a three element vector (x, y, w) where x = w\*X, y = w\*Y, and w is any real number except zero. A line is also represented by a three element vector (a, b, c). The directed line (a, b, c) from point (x<sub>1</sub>, y<sub>1</sub>, w<sub>1</sub>) to point (x<sub>2</sub>, y<sub>2</sub>, w<sub>2</sub>) is given by:
-
-<div>$$(a,b,c) = ({x_1},{y_1},{z_1}) \otimes ({x_2},{y_2},{z_2})$$</div>
-
-The sequence in the cross product is a convention to determine sign. The condition that a point (x, y, w) lie on a line (a, b, c) is that
-
-<div>$$(a,b,c) \bullet (x,y,w) = 0$$</div>
-
-The point is normalized by dividing by w. Then if
-
-<div>$$(a,b,c) \bullet (x/w,y/w,1) > 0$$</div>
-
-the point is to the left of the line.  If it is less than zero, the point is to the right of the line. The intercept (x, y, w) of line (a<sub>1</sub>, b<sub>1</sub>, c<sub>1</sub>) and line (a<sub>2</sub>, b<sub>2</sub>, c<sub>2</sub>) is given by:
-
-<div>$$(x,y,w) = ({a_1},{b_1},{c_1}) \otimes ({a_2},{b_2},{c_2})$$</div>
-
-Note that the use of homogeneous coordinates as outlined above provides a consistent method and notation for defining points and lines, for determining intercepts, and for determining whether a point lies to the left, to the right, or on a line.  Normalization provides the means for transforming to and from homogeneous notation and Cartesian coordinates.  Thus, if (X, Y) is a Cartesian coordinate pair, its homogeneous coordinates are (X, Y, 1).  Similarly, the homogeneous coordinates (x, y, w) can be transformed to the Cartesian point with coordinates (x/w, y/w).
-
-### Polygon Clipping Algorithms
-
-Two methods for polygon clipping (treating of overlapping shadows) are currently in use in EnergyPlus.
-
-* Convex Weiler - Atherton
-
-* Sutherland – Hodgman
-
-The original EnergyPlus method for polygon clipping is a special version of the Weiler-Atherton model (Weiler, Atherton, 1977). It was developed to be sufficiently general to clip concave polygons with holes. The implementation in the current version of EnergyPlus, however, does not support concave shadowing surfaces or holes. The relative computational complexity is preserved – the algorithm is carried out in four steps. For example, if A and B are polygons (see Figure 43).
-
-1)   A call to INCLOS determines which vertices of X lie within Y.
-
-2)   A second call determines which vertices of Y lie within X.
-
-3)   If neither polygon is contained completely within the other, INTCPT is called to collect points of intersection between X and Y.
-
-4)   Since the points are usually gathered out of order, they must then be oriented.
-
-The Sutherland-Hodgman algorithm (Sutherland, Hodgman, 1974) is less complex compared to the Weiler-Atherton method and is well-suited to clipping convex polygons. In actuality, only convex shading surfaces are currently supported by EnergyPlus. Let X be a polygon called the “subject polygon� (SP) and Y be a polygon called the “clipping polygon� (CP). The method performs the computation by iterating over the edges of the CP and removing points from the SP that fall in the clipping plane, i.e. points that fall to the left of the edge of the CP. Intersections between the clip edge and the edges of the SP are added appropriately, and points falling outside of the clipping plane, i.e. to the right of the edge of the CP, are added the output polygon as well. This resultant polygon is stored and the process is repeated for the rest of the clip edges in CP. The process is analogous to cutting off pieces of the SP one-by-one with respect to each edge of the CP. The result is ordered and identical to the polygon produced by the Weiler-Atherton method.
-
-### Overlapping Shadows
-
-After transforming the shadows onto the plane of the receiving surface, the basic job of the shadow algorithm is to determine the area of the overlap between the polygons representing the shadows and the polygon representing the receiving surface. Concave surfaces are supported only for exterior wall heat transfer surfaces, when using SutherlandHodgman option. Concave shading devices are not supported by the this option. Neither concave shading devices nor concave exterior wall heat transfer surfaces are supported by the ConvexWeilerAtherton clipping routine.
-
-When only convex shading devices are considered, this provides a great simplification. The overlap between two convex polygons (i.e. projections of shading devices via the direction of the sun) is another convex polygon. Coordinate and projection transformations of a convex polygon produce another convex polygon. Any non-convex polygon can be constructed as the union of convex ones.
-
-For ConvexWeilerAtherton, there is considerable simplification if only convex (no interior angle &gt; 180 ) polygons are considered. The overlap between two convex polygons is another convex polygon. Coordinate and projection transformations of a convex polygon produce another convex polygon. Any non-convex polygon can be constructed as a sum of convex ones.
-
-The vertices that define the overlap between two convex polygons, A and B, consist of:
-
-* the vertices of A enclosed by B
-
-* the vertices of B enclosed by A
-
-* and the intercepts of the sides of A with the sides of B
-
-In Figure 43, point a is the result of rule 1, point c is the result of rule 2, and points b and d result from rule 3. The overlap of A and B is the polygon a-b-c-d. Figure 44 shows an overlap where all of the vertices of B are enclosed by A.  Figure 45 shows an overlap defined only by the intercepts of A and B. Figure 46 shows a more complex overlap.
-
-![](media/image637.png)
-
-Figure 43.  Point a – Vertex of A Enclosed by B
-
-Coordinate transformation retains the order of the vertices of a polygon, while a projection reverses the order. The sequence of vertices of the receiving polygons should be reversed so it and all shadow polygons will have the same sequence.
-
-![](media/image638.png)
-
-Figure 44.  Surface A Totally Overlaps Surface B.
-
-A point is enclosed by a clockwise, convex polygon if the point lies to the right of all sides (or does not lie to the left of any side) of the polygon.  The intercept of two sides may not lie beyond the ends of either side. These are "line segments" rather than "lines". It is possible to tell if line segments A and B intercept within their end points by noting that the ends of A must lie on both sides of B, and the ends of B must lie on both sides of A. This should be done before the intercept is calculated.
-
-![](media/image639.png)
-
-Figure 45.  Figure Formed from Intercept Overlaps Between A and B
-
-Once the vertices are determined, they must be sorted into clockwise order for the area to be computed.  Given a closed, planar polygon of n sequential vertices (x<sub>1</sub>, y<sub>1</sub>), (x<sub>2</sub>, y<sub>2</sub>) …, (x<sub>n</sub>, y<sub>n</sub>), its **area** is given:
-
-<div>$$Area = {\textstyle{1 \over 2}}\sum\limits_{i = 1}^n {({x_i}{y_{i + 1}} - {x_{i + 1}}{y_i})} $$</div>
-
-where (x<sub>n+1</sub>,y<sub>n+1</sub>)= (x<sub>1</sub>, y<sub>1</sub>)
-
-The area is positive if the vertices are counter-clockwise and negative if they are clockwise.
-
-![](media/image641.png)
-
-Figure 46.  Complex Overlapping Condition
-
-If two shadows overlap the receiving surface, they may also overlap each other as in Figure 47. The vertices of this overlap can be computed.  The areas of all overlaps can be computed.  The total sunlit area can be expressed as the sum of all polygon areas given a proper sign on each of the areas.
-
-
-
-The following convention was adopted:
-
-Table 24.  Surface / Area Characteristic / Convention
-
-<table class="table table-striped">
-<tr>
-<th>Surface Characteristic</th>
-<th>Area Convention</th>
-</tr>
-<tr>
-<td>receiving surface</td>
-<td>positive (A)</td>
-</tr>
-<tr>
-<td>overlap between shadow and receiving</td>
-<td>negative (B &amp; C)</td>
-</tr>
-<tr>
-<td>overlap between two shadows</td>
-<td>positive (D)</td>
-</tr>
-
-</table>
-
-and so on through multiple overlaps where the sign of the overlap area is the product of the signs of the overlapping areas.
-
-![](media/image642.png)
-
-Figure 47.  Multiple Shadow Overlaps
-
-Partially transparent shadowing surfaces can also be modeled by giving a transparency (t)to every shadowing polygon. Let tof the receiving polygon be one. Then the tof every overlap of polygons i and jis the product of t<sub>i</sub>and t<sub>j</sub>The shaded area is then computed by summing A<sub>i</sub>·(1 - t<sub>i</sub>) for all overlap polygons.
-
-It is easy to determine the sunlit area of a window once all the shadow and overlap vertices on the wall have been computed. Consider wall 2 of Figure 38. First, the wall is considered a simple rectangle and the window on it is ignored. The shadow overlapping is performed and the sunlit portion of the gross wall area is computed. Then the window rectangle is overlapped with the shadow to determine its sunlit area. The sunlit area of the window is subtracted from the gross wall sunlit area to determine the net wall sunlit area. During this calculation it is not necessary to recompute the shadows, because they were precisely determined on the wall.
-
-When the SutherlandHodgman option is selected, the overlap is computed using the Sutherland-Hodgman algorithm for polygon clipping when. Let X be a polygon called the “subject polygon� (SP) and Y be a polygon called the “clipping polygon� (CP). The method performs the computation by iterating over the edges of the CP and removing points from the SP that fall in the clipping plane, i.e. points that fall to the left of the edge of the CP. If it is to the left of any edge, it the point does not overlap with the CP. Intersections between the clip edge and the edges of the SP are added appropriately, and points falling outside of the clipping plane, i.e. to the right of the edge of the CP, are added the output polygon as well. This resultant polygon is stored and the process is repeated for the rest of the clip edges in CP. The process is analogous to cutting off pieces of the SP one-by-one with respect to each edge of the CP. Note that the SP may be concave, but the CP may not. This means that the exterior wall surfaces may be concave, while shading devices may not be concave.
-
-### Solar Gains
-
-The total solar gain on any exterior surface is a combination of the absorption of direct and diffuse solar radiation given by
-
-<div>$${Q_{so}} = \alpha \cdot \left( {{I_b}\cdot \cos \theta \cdot \frac{{{S_s}}}{S} + {I_s}\cdot {F_{ss}} + {I_g}\cdot {F_{sg}}} \right)$$</div>
-
-where
-
-a =solar absorptance of the surface
-
-A =angle of incidence of the sun's rays
-
-S =area of the surface
-
-S<sub>s</sub> = sunlit area
-
-I<sub>b</sub> =intensity of beam (direct) radiation
-
-I<sub>s</sub> =intensity of sky diffuse radiation
-
-I<sub>g</sub> =intensity of ground reflected diffuse radiation
-
-F<sub>ss</sub> = angle factor between the surface and the sky
-
-F<sub>sg</sub> = angle factor between the surface and the ground
-
-For the surface of a building located on a featureless plain
-
-<div>$${F_{ss}} = \frac{{1 + \cos \phi }}{2}$$</div>
-
-and
-
-<div>$${F_{sg}} = \frac{{1 - \cos \phi }}{2}$$</div>
-
-If the surface is shaded the program modifies *F<sub>ss</sub>*by a correction factor that takes into account the radiance distribution of the sky (see “Shadowing of Sky Diffuse Solar Radiation�).
-
-Shading of ground diffuse solar radiation is not calculated by the program. It is up to the user to estimate the effect of this shading and modify the input value of *F<sub>sg</sub>*accordingly.
-
-### Solar Distribution
-
-As discussed in the Input Output Reference (Object: Building), the field Solar Distribution, in the “Building� input object, determines how EnergyPlus will treat beam solar radiation entering a zone through exterior windows.  There are five choices: **MinimalShadowing**, **FullExterior**, **FullInteriorAndExterior, FullExteriorWithReflections**, and **FullInteriorAndExteriorWithReflections**.
-
-#### MinimalShadowing
-
-In this case, there is no exterior shadowing except from window and door reveals. All beam solar radiation entering the zone is assumed to fall on the floor, where it is absorbed according to the floor's solar absorptance. Any reflected by the floor is added to the transmitted diffuse radiation, which is assumed to be uniformly distributed on all interior surfaces. If no floor is present in the zone, the incident beam solar radiation is absorbed on all interior surfaces according to their absorptances. The zone heat balance is then applied at each surface and on the zone's air with the absorbed radiation being treated as a flux on the surface.
-
-#### FullExterior
-
-In this case, shadow patterns on exterior surfaces caused by detached shading, wings, overhangs, and exterior surfaces of all zones are computed. As for MinimalShadowing, shadowing by window and door reveals is also calculated. Beam solar radiation entering the zone is treated as for MinimalShadowing.
-
-#### FullExteriorWithReflections
-
-This case is the same interior distribution as the preceding option but uses exterior reflections as well (see the section Solar Radiation Reflected from Exterior Surfaces for further explanation).
-
-#### FullInteriorAndExterior
-
-This is the same as FullExterior except that instead of assuming all transmitted beam solar falls on the floor the program calculates the amount of beam radiation falling on each surface in the zone, including floor, walls and windows, by projecting the sun's rays through the exterior windows, taking into account the effect of exterior shadowing surfaces and window shading devices.
-
-If this option is used, you should be sure that the surfaces of the zone totally enclose a space. This can be determined by viewing the **eplusout.dxf** file with a program like AutoDesk’s Volo View Express. You should also be sure that the zone is **convex**. Examples of convex and non-convex zones are shown in Figure 48. The most common non-convex zone is an L-shaped zone. (A formal definition of convex is that any straight line passing through the zone intercepts at most two surfaces.)  If the zone’s surfaces do not enclose a space or if the zone is not convex you should use Solar Distribution = **FullExterior** instead of **FullInteriorAndExterior**.
-
-If you use **FullInteriorAndExterior** the program will calculate how much beam radiation falling on an interior window is absorbed by the window, how much is reflected back into the zone, and how much is transmitted into the adjacent zone. (Interior windows are assumed to have no shading device).
-
-If you use **FullInteriorAndExterior** the program will also calculate how much beam radiation falling on the inside of an exterior window (from other windows in the zone) is absorbed by the window, how much is reflected back into the zone, and how much is transmitted to the outside. In this calculation the effect of an interior or exterior shading device, if present, is accounted for.
-
-#### FulInteriorAndlExteriorWithReflections
-
-This case is the same interior distribution as the preceding option but uses exterior reflections as well (see Solar Radiation Reflected from Exterior Surfaces for further explanation).
-
-
-
-![](media/image646.png)
-
-Figure 48. Illustration of Convex and Non-convex Zones
-
-### Details of the Interior Solar Distribution Calculation
-
-EnergyPlus calculates the distribution of short-wave radiation in the interior of each thermal zone. This radiation consists of beam solar radiation, diffuse solar radiation, and short-wave radiation from electric lights. The program determines the amount of this radiation that is (1) absorbed on the inside face of opaque surfaces, (2) absorbed in the glass and shading device layers of the zone’s exterior and interior windows, (3) transmitted through the zone’s interior windows to adjacent zones, and (4) transmitted back out of the exterior windows. The effects of movable shading devices on the exterior windows are taken into account; *the program does not allow shading devices on interior windows*. Most of this calculation is done in subroutine CalcInteriorSolarDistribution in the SolarShading module.
-
-#### Initial Distribution of Diffuse Solar Transmitted through Exterior and Interior Windows
-
-Diffuse solar (from sky and ground sources) transmitted through exterior windows is first distributed to the interior heat transfer surfaces in the zone containing the exterior windows. This initial distribution apportions the transmitted diffuse solar to interior surfaces using the approximate view factors described above in “LW Radiation Exchange Among Zone Surfaces.� The amount of this initially distributed diffuse solar absorbed by each interior surface, and each window material layer, is calculated and later added to the “short-wave radiation absorbed� values described below. The amount of this initially distributed diffuse solar that is reflected is accumulated for each zone and redistributed uniformly as part of the QD calculation described below. The amount of this initially distributed diffuse solar that is transmitted by interior windows to adjacent zones is initially distributed to the interior heat transfer surfaces in the adjacent zone in the same manner as just described.
-
-This new treatment of diffuse solar is intended to more accurately account for the initial absorption, transmittance, and reflection of short-wave radiation prior to the uniform distribution described below.
-
-#### Interior Solar Radiation Absorbed by Opaque Surfaces
-
-The short-wave radiation absorbed on the inside face of an opaque surface (floor, wall or ceiling) is given by
-
-<div>$$
-  QRadSWInAbs(SurfNum) = QS(ZoneNum)*AbsIntSurf(SurfNum) + AISurf(SurfNum)*BeamSolarRad [W/m2]
-$$</div>
-
-where
-
-*SurfNum*= surface number
-
-*ZoneNum =*number of zone that surface belongs to
-
-*QS(ZoneNum)*= short-wave diffuse irradiance in the zone [W/m<sup>2</sup>]
-
-*AbsIntSurf(SurfNum)*= inside solar absorptance of the surface
-
-*AISurf(SurfNum)* = inside beam solar irradiance factor for the surface [-]
-
-*BeamSolarRad* = outside beam normal solar irradiance [W/m<sup>2</sup>]
-
-##### Interior Diffuse Radiation
-
-*QS* is assumed to be uniformly distributed throughout the zone. It is calculated as follows. Let *Q<sub>sw</sub>* be the total diffuse short-wave radiation entering the zone or originating in the zone. Since *Q<sub>sw</sub>* is ultimately absorbed or transmitted by zone heat transfer surfaces, summing over these surfaces gives the following energy balance equation:
-
-<div>$$\sum\limits_{i = 1}^{{N_{surf}}} {QS(ZoneNum)*{\alpha_i}{A_i} = {Q_{SW}}(ZoneNum)} $$</div>
-
-where
-
-*i* = zone surface number counter
-
-*N<sub>surf</sub>*= number of heat transfer surfaces in zone
-
-*A<sub>i</sub>* = surface area [m<sup>2</sup>]
-
-<span>\({\alpha_i}\)</span>= inside solar absorptance for an opaque surface, or, for a window, = back diffuse transmittance plus back diffuse system absorptance of glass layers and shading device layers (if present)
-
-Solving this equation for *QS* gives:
-
-<div>$$QS(ZoneNum) = \frac{{{Q_{SW}}(ZoneNum)}}{{\sum\limits_{i = 1}^{{N_{surf}}} {AbsInsSur{f_i}{A_i}} }} = {Q_{SW}}(ZoneNum)*VMULT(ZoneNum)$$</div>
-
-where
-
-<div>$$VMULT(ZoneNum) = \frac{1}{{\sum\limits_{i = 1}^{{N_{surf}}} {AbsIntSur{f_i}*{A_i}} }}{\rm{    [}}{{\rm{m}}^{{\rm{ - 2}}}}]$$</div>
-
-*Q<sub>sw</sub>* is given by
-
-<div>$$
-  Q{S_{SW}} = QD(ZoneNum) + ZoneIntGain(ZoneNum)\% QLTSW + ZoneIntGain(ZoneNum)\% T\_QLTSW [W]
-$$</div>
-
-where
-
-*ZoneIntGain(ZoneNum)%QLTSW* = short-wave radiation into zone from general (overhead) electric lighting [W]
-
-*ZoneIntGain(*ZoneNum*)%T\_QLTSW* = short-wave radiation into zone from task electric lighting [W]
-
-*QD(ZoneNum)* = diffuse solar radiation entering or originating in zone [W]
-
-*QD(ZoneNum)* is given by:
-
-<div>$$QD(ZoneNum) = DBZone(ZoneNum)*BeamSolarRad + InitialDifSolDistReflectedW(ZoneNum)$$</div>
-
-where
-
-*BeamSolarRad* is the outside beam normal solar irradiance [W/m<sup>2</sup>]
-
-*DBZone(ZoneNum)* is the diffuse solar radiation originating from beam solar that passes through the exterior windows in the zone and reflects diffusely from inside zone surfaces plus beam solar entering the zone as diffuse radiation from windows with shading devices or diffusing glass (all divided by BeamSolarRad)   [m<sup>2</sup>]
-
-*InitialDifSolDistReflectedW(ZoneNum)* is the diffuse solar radiation originating from sky and sun related diffuse solar transmitted through the zone’s exterior or interior windows into the zone, and reflected diffusely from inside zone surfaces.
-
-*DBZone(ZoneNum)* is calculated as:
-
-<div>$$DBZone(ZoneNum) = BTOTZone - BABSZone{\rm{    [}}{{\rm{m}}^{\rm{2}}}]$$</div>
-
-where
-
-*BTOTZone* = total beam solar incident on the zone’s exterior windows that is transmitted as beam or diffuse.[[1]](#_ftn1)
-
-*BABSZone=* total beam solar absorbed inside the zone.
-
-*BTOTZone* is given by:
-
-<div>$$BTOTZone = \sum\limits_{i = 1}^{{N_{extwin}}} {TBmAl{l_i}*SunlitFrac{t_i}*CosIn{c_i}*Are{a_i}*InOutprojSLFracMul{t_i}} $$</div>
-
-*+ Diffuse entering zone from beam reflected by window inside reveal surfaces[**[2]**](#_ftn2)*
-
-*+ Diffuse transmitted by windows from beam reflected by outside reveal surfaces*
-
-*–  Beam absorbed by window inside reveal surfaces*
-
-Here,
-
-*TBmAll* = beam-to-beam plus beam-to-diffuse transmittance of window
-
-*SunlitFract* = fraction of window irradiated by sun
-
-*CosInc* = cosine of solar incidence angle on window
-
-*Area* = glazed area of window [m<sup>2</sup>]
-
-*InOutProjSLFracMult* = shadowing factor due to inside and outside projections of window frame and/or divider (= 1.0 if there is no frame or divider).
-
-*BABSZone* is given by the following sum (see Figure 49):
-
-*BABSZone* =  *Beam absorbed by opaque inside surfaces[**[3]**](#_ftn3)*
-
-*                        + Beam transmitted through the zone’s interior windows +*
-
-*                        + Beam transmitted back out of the zone’s exterior windows +*
-
-*                        + Beam absorbed by the zone’s exterior and interior windows +*
-
-*                        + Beam absorbed by inside daylighting shelves*
-
-![](media/image656.png)
-
-Figure 49. Vertical section through a two-zone building showing where transmitted beam solar falls. Some of the beam solar from exterior window EW is absorbed by the floor, D, interior wall, B, and interior window, IW. Some is transmitted by IW to the adjacent zone, Z2. Aoverlap is the irradiated area of a surface projected back onto the plane of EW. Beam reflected by D, B and IW contributes to the interior short-wave radiation flux in Z1.
-
-If zone *ZoneNum* shares interior windows with other zones, *QS(ZoneNum)* is modified to take into account short-wave radiation received from the other zones through these windows:
-
-<div>$$
-  \begin{array}{rl}
-   QS(ZoneNum) &= QS(ZoneNum) \\
-               &+ \sum_{otherZones}\text{FractDifShortZtoZ(OtherZoneNum,ZoneNum)} \\
-               &* [QD(OtherZoneNum) + ZoneIntGain(OtherZoneNum)\% QLTSW + ZoneIntGain(OtherZoneNum)\% T\_QLTSW]
-  \end{array}
-$$</div>
-
-where
-
-*FractDifShortZtoZ(OtherZoneNum,ZoneNum)* = “diffuse solar exchange factor� = fraction of short-wave radiation in *OtherZoneNum* that is transmitted to *ZoneNum*. This factor is calculated in subroutine ComputeDifSolExcZonesWIZWindows taking into account multiple reflection between zones. For example, for two zones means that some of the radiation transmitted from Zone1 to Zone2 is reflected back to Zone1, and some of this is in turn reflected back to Zone2, etc.
-
-##### Interior Beam Radiation
-
-The inside beam solar irradiance factor[[4]](#_ftn4) in is given by:
-
-
-
-<span>\(AISurf(SurfNum) = \frac{{AbsIntSurf(SurfNum)}}{{A(SurfNum)}}\sum\limits_{i = 1}^{{N_{extwin}}} {TB{m_i}*Aoverla{p_i}(SurfNum)*CosIn{c_i}} \)</span>where
-
-*i* = exterior window number
-
-*N<sub>extwin</sub>=* number of exterior windows in zone
-
-*CosInc<sub>i</sub>* = cosine of angle of incidence of beam on exterior window *i*
-
-*TBm<sub>i</sub>* = beam-to-beam transmittance of exterior window* i*at *CosInc<sub>i</sub>* [[5]](#_ftn5)
-
-*Aoverlap<sub>i</sub>(SurfNum)* = beam solar irradiated area of surface *SurfNum* projected back onto the plane of exterior window* i* (the *Aoverlap*’s for an exterior window sum up to the glazed area of the window). These overlap areas (Figure 49) are determined with the EnergyPlus shadowing routines by considering a zone’s exterior window as a “sending� surface and the inside faces of the zone’s other surfaces as “receiving� surfaces (see “Shading Module�). The overlap areas for a particular exterior window depend on the sun position, the geometry of the window, the geometry of the interior surfaces, and the location of the window with respect to the interior surfaces.
-
-*AbsIntSurf(SurfNum)*= inside face solar absorptance of surface *SurfNum*
-
-*A(SurfNum)* = area of surface *SurfNum* [m<sup>2</sup>]
-
-#### Interior Solar Radiation Absorbed by Windows
-
-The interior short-wave radiation absorbed by layer *l* (glass, shade or blind) of a window is equal to:
-
-
-
-<span>\(\begin{array}{l}QS(ZoneNum)*\alpha_{l,back}^{dif}(SurfNum) + \\BeamSolarRad*\frac{{\alpha_{l,back}^{beam}(SurfNum)}}{{A(SurfNum)}}\sum\limits_{i = 1}^{{N_{extwin}}} {TB{m_i}*Aoverla{p_i}(SurfNum)} *CosIn{c_i}{\rm{  [W/}}{{\rm{m}}^{\rm{2}}}]\end{array}\)</span>where
-
-<span>\(\alpha_{l,back}^{dif}\)</span>= the system diffuse solar absorptance of layer* l* for irradiance from the back side
-
-<span>\(\alpha_{l,back}^{beam}\)</span>= the system beam solar absorptance of layer* l* for irradiance from the back side
-
-*A(SurfNum)*= glazing area [m<sup>2</sup>]
-
-Note that as of Version 2.1, the initially distributed diffuse solar absorbed by each surface (as described above under “Initial Distribution of Diffuse Solar Transmitted through Exterior and Interior Windows�) is added to this uniformly distributed short-wave radiation.
-
-#### Interior Solar Radiation Transmitted by Interior Windows
-
-##### Interior Diffuse Radiation Transmitted by Interior Windows
-
-The interior diffuse short-wave radiation transmitted by an interior window to the adjacent zone is given by
-
-<div>$$QS(ZoneNum)*{\tau ^{dif}}(SurfNum)*A(SurfNum){\rm{    [W]}}$$</div>
-
-where
-
-<span>\({\tau ^{dif}}(SurfNum)\)</span>= diffuse transmittance of the interior window
-
-##### Interior Beam Radiation Transmitted by Interior Windows
-
-The interior beam solar radiation transmitted by an interior window to the adjacent zone is
-
-<div>$$BeamSolarRad*{\tau ^{beam}}(SurfNum)\sum\limits_{i = 1}^{{N_{extwin}}} {TB{m_i}*Aoverla{p_i}(SurfNum)*CosIn{c_i}{\rm{    [W}}]} $$</div>
-
-where <span>\({\tau ^{beam}}(SurfNum)\)</span>is the beam-to-beam transmittance of the interior window at the angle of incidence of beam solar from the exterior window on the interior window. The program does not track where this radiation falls in the adjacent zone: it is counted as diffuse radiation in that zone. Therefore,
-
-<div>$$QS(ZoneNum) \to QS(ZoneNum) + [{\rm{beam solar from adjacent zones]}}*VMULT(ZoneNum)$$</div>
-
-### Ground Reflectances
-
-Ground reflectance values (Ref Object: Site:GroundReflectance) are used to calculate the ground reflected solar amount.  This fractional amount (entered monthly) is used in the following equation:
-
-<div>$${\rm{GroundReflectedSolar = (BeamSolar}} \bullet {\rm{COS(SunZenithAngle) + DiffuseSolar)}} \bullet {\rm{GroundReflectance}}$$</div>
-
-Of course, the Ground Reflected Solar is never allowed to be negative.  The Snow Ground Reflectance Modifier can further modify the ground reflectance when snow is on the ground.  If the user enters 0.0 for each month, no ground reflected solar is used.
-
-### Ground Reflectances (Snow)
-
-When snow is on the ground, ground reflectances may change.  (Ref Object: Site:GroundReflectance:SnowModifier).  This object allows the user to specify two values, Ground Reflected Solar Modifier and Daylighting Ground Reflected Solar Modifier.
-
-Ground Reflected Solar Modifier is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values). Values can range from 0.0 to 1.0.
-
-<div>$${\rm{GroundReflectanc}}{{\rm{e}}_{{\rm{used}}}} = {\rm{GroundReflectance}} \bullet SolarModifie{r_{Snow}}$$</div>
-
-Daylighting Ground Reflected Solar Modifier is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values). Values can range from 0.0 to 1.0.
-
-<div>$${\rm{DaylightingGroundReflectanc}}{{\rm{e}}_{{\rm{used}}}} = {\rm{GroundReflectance}} \bullet DaylightingModifie{r_{Snow}}$$</div>
-
-### References
-
-ASHRAE. 2005. Handbook of Fundamentals, Chapter 31, Atlanta: ASHRAE.
-
-ASHRAE. 2007. HVAC Applications, Chapter 33, Atlanta, ASHRAE.
-
-Zhang, Qingyuan, Joe Huang, and Siwei Lang. 2002. "Development of Typical Year Weather Data for Chinese Locations", American Society of Heating Refrigeration and Air-Conditioning Engineers, ASHRAE Transactions, Vol 108, Part 2.
-
-Threlkeld, J.L. and R.C. Jordan. 1958. Direct solar radiation available on clear days. ASHRAE Transactions 64:45.
-
-Groth, C. C., and Lokmanhekim, M. 1969. "Shadow ‑ A New Technique for the Calculation of Shadow Shapes and Areas by Digital Computer," Second Hawaii International Conference on System Sciences, Honolulu, HI, January 22‑24, 1969.
-
-Walton, G.N. 1983. “The Thermal Analysis Research Program Reference Manual Program (TARP)�, National Bureau of Standards (now National Institute of Standards and Technology).
-
-Walton, G. N. 1978. "The Application of Homogeneous Coordinates to Shadowing Calculations", American Society of Heating Refrigeration and Air-Conditioning Engineers, ASHRAE Transactions, Vol 84, Part I.
-
-Meeus, Jean. 2000. Astronomical Algorithms, Willmann-Bell.
-
-Newman, M. W., and Sproul, R. F. 1973. Principles of Interactive Computer Graphics, McGraw‑Hill.
-
-Polygon area derived from Green’s Theorem.  Graphic Gems repository.
-
-Weiler, Kevin, Atherton, Peter. “Hidden Surface Removal Using Polygon Area Sorting.� Program of Computer Graphics, Cornell University. Ithaca, NY: 1977.
-
-Sutherland, I.E., and Hodgman, G.W. 1974. “Reentrant Polygon Clipping�, Communication of Association for Computing Machinery (CACM), vol. 17, pp. 32-42.
-
-Maillot,Patrick-Gilles.** “**A New, Fast Method For 2D Polygon Clipping: Analysis and Software Implementation.� Sun Microsystems, inc. Mountain View, CA: 1992.
-
-Wisstein, Eric W. “Convex Polygon� From Mathworld- A Wolfram Web Resource.
-
diff --git a/doc/src/docs/EngineeringReference/06-SolarRadiation.md b/doc/src/docs/EngineeringReference/06-SolarRadiation.md
deleted file mode 100644
index 87116823792..00000000000
--- a/doc/src/docs/EngineeringReference/06-SolarRadiation.md
+++ /dev/null
@@ -1,258 +0,0 @@
-Solar Radiation Reflected from Exterior Surfaces
-================================================
-
-EnergyPlus has an option to calculate beam and sky solar radiation that is reflected from exterior surfaces and then strikes the building. This calculation occurs if “withReflections� is used on the SolarDistribution option in the Building object. For zones with detailed daylighting, these reflections are also considered in the daylight illuminance calculations.[[6]](#_ftn6)
-
-The reflecting surfaces fall into three categories:
-
-* **Shadowing surfaces**. These are surfaces like overhangs or neighboring buildings entered with objects Shading:Site:Detailed, Shading:Building:Detailed, or Shading:Zone:Detailed Examples are shown in Figure 50.
-
-These surfaces can have diffuse and/or specular (beam-to-beam)  reflectance values that are specified with the ShadingProperty:Reflectance object.
-
-* **Exterior building surfaces**. In this case one section of the building reflects solar radiation onto another section (and vice-versa). See Figure 51.
-
-Opaque building surfaces (walls, for example) are assumed to be diffusely reflecting. Windows and glass doors are assumed to be specularly reflecting. The reflectance values for opaque surfaces are calculated by the program from the Solar Absorptance and Visible Absorptance values of the outer material layer of the surface’s construction. The reflectance values for windows and glass doors are calculated by the program from the reflectance properties of the individual glass layers that make up surface’s construction assuming no shading device is present and taking into account inter-reflections among the layers.
-
-* **The ground surface**. Beam solar and sky solar reflection from the ground is calculated even if “withReflections� is not used (the default). But in this case the ground plane is considered unobstructed, i.e., the shadowing of the ground by the building itself or by obstructions such as neighboring buildings is ignored. This shadowing is taken into account only if “WithReflections� is used in the Solar Distribution field (in “Building� input object) (Figure 52). In this case the user-input value of ground view factor is not used.
-
-![](media/image670.png)
-
-Figure 50.   Examples of solar reflection from shadowing surfaces in the Shading series of input objects. Solid arrows are beam solar radiation; dashed arrows are diffuse solar radiation. (a) Diffuse reflection of beam solar radiation from the top of an overhang. (b) Diffuse reflection of sky solar radiation from the top of an overhang. (c) Beam-to-beam (specular) reflection from the façade of an adjacent highly-glazed building represented by a vertical shadowing surface.
-
-![](media/image671.png)
-
-Figure 51.   Solar reflection from building surfaces onto other building surfaces. In this example beam solar reflects from a vertical section of the building onto a roof section. The reflection from the window is specular. The reflection from the wall is diffuse.
-
-![](media/image672.png)
-
-Figure 52. Shadowing by the building itself affects beam solar reflection from the ground.  Beam-to-diffuse reflection from the ground onto the building occurs only for sunlit areas, A and C, not for shaded area, B. Shadowing by the building also affects sky solar reflection from ground (not shown).
-
-Diffuse Reflection of Beam Solar and Sky Solar Radiation
---------------------------------------------------------
-
-A ray-tracing method is used to calculate beam solar and sky solar radiation that is diffusely reflected onto each of a building’s exterior surfaces (walls, roofs, windows and doors), called here “receiving surfaces.� The calculation begins by generating a set of rays proceeding into the outward hemisphere at each receiving point on a receiving surface. Then it determinines whether each ray hits the sky, ground or an obstruction. The radiance at the hit point from reflection of incident beam or sky solar is determined and the contribution of this radiance to the receiving surface is calculated, added to the contribution from other hit points, and averaged over the receiving points. Separate calculations are done for beam-to-diffuse and sky solar reflection from all obstructions and beam-to-diffuse and sky solar reflection from the ground. (For beam-to-beam reflection see “Beam Solar Radiation Specularly Reflected from Obstructions,� below.)
-
-### *Receiving points*
-
-An *N*-sided surface is assigned *N* receiving points with the following coordinates, expressed in terms of the surface vertex coordinates:
-
-<div>$${P_{ij}} = \sum\limits_{k = 1}^N {{a_{ki}}{v_{kj}},{\rm{  }}i = 1,3;{\rm{  }}j = 1,3} $$</div>
-
-where
-
-*P<sub>ij</sub> = j<sup>th</sup>* coordinate of the* i<sup>th</sup>* receiving point
-
-*v<sub>kj</sub>* =* j<sup>th</sup>* coordinate of the *k<sup>th</sup>* surface vertex
-
-If *N* = 3:  *a<sub>kj</sub>* = 3/5 if *k*= *i*;  = 1/5 otherwise
-
-If *N* &gt; 3:  *a<sub>kj</sub>* = <span>\(\frac{{N + 1}}{{2N}}\)</span> if *k*= *i*;  = <span>\(\frac{1}{{2N}}\)</span> otherwise
-
-For example, for a vertical 3m by 5m rectangle with vertices (0,0,3), (0,0,0), (5,0,0) and (5,0,3), this expression gives receiving points at (1.25,0,2.25), (1.25,0,0.75), (3.75,0,0.75) and (3.75,0,2.25), as shown in Figure 53.
-
-
-
-![](media/image676.png)
-
-Figure 53. Vertical rectangular exterior heat transfer surface showing location of receiving points for calculating incident solar radiation reflected from obstructions.
-
-### *Rays*
-
-A total of 90 rays are sent out into the exterior hemisphere surrounding each receiving point. An upgoing ray may hit an obstruction or the sky. A downgoing ray may hit an obstruction or the ground. See Figure 54.
-
-In subroutine InitSolReflRecSurf, the following is determined for each ray, *i,*:
-
-1.    Unit vector in direction of ray
-
-2.    Cosine of angle between ray and plane of receiving surface (<span>\(\cos {\alpha_i}\)</span>)
-
-3.    Element of solid angle associated with ray (<span>\(d{\Omega_i}\)</span>)
-
-4.    If the ray hits one or more obstructions, the coordinates of the hit point on the obstruction nearest the receiving point
-
-5.    For the surface containing the hit point: the surface number, the solar reflectance (<span>\({\rho_{obs,i}}\)</span>if an obstruction), and the surface unit vector at the hit point pointing into the hemisphere containing the receiving point
-
-6.    If the ray is downgoing and hits the ground, the coordinates of the ground hit point
-
-7.    Distance from receiving point to hit point
-
-
-
-![](media/image680.png)
-
-Figure 54.  Two-dimensional schematic showing rays going outward from a point on a receiving surface. Rays 1-6 hit the ground, rays 7-11 hit an obstruction, and rays 12-15 hit the sky.
-
-### Sky Solar Radiation Diffusely Reflected from Obstructions
-
-The factor for reflection of sky radiation from obstructions onto a receiving surface is calculated in subroutine CalcSkySolDiffuseReflFactors. It is given by:
-
-<div>$$\begin{array}{l}{\rm{ReflFacSkySolObs(RecSurfNum)}} = \\\frac{1}{{{N_{rec}}}}\sum\limits_1^{{N_{rec}}} {\sum\limits_{i = 1}^{{N_{ray}}} {Hi{t_{obs,i}}ViewFacSk{y_{obs,i}}DifShdgRatioIsoSk{y_{obs,i}}{\rho_{obs,i}}\cos {\alpha_i}/\pi } } \end{array}$$</div>
-
-where
-
-RecSurfNum is the receiving surface number,
-
-<span>\({N_{rec}}\)</span>is the number of receiving points,
-
-<span>\({N_{ray}}\)</span>is the number of rays,
-
-“*obs,i*� denotes the obstruction hit by ray *i*,
-
-*Hit<sub>obs,i</sub>* = 1 if ray* i* hits an obstruction, = 0 otherwise,
-
-*ViewFacSky<sub>obs,i</sub>*= unobstructed sky view factor of the obstruction = <span>\((1 + \cos til{t_{obs}})/2\)</span>,
-
-*DifShdgRatioIsoSky<sub>obs,i</sub>*= (obstructed sky irradiance on obstruction)/(unobstructed sky irradiance on obstruction)
-
-In this equation the product*ViewFacSky\*DifShdgRatioIsoSky*is the sky irradiance at the hit point divided by the horizontal sky irradiance taking into account shadowing of sky diffuse radiation on the obstruction by other obstructions, and assuming that the radiance of the sky is uniform. Note that we ignore secondary reflections here and in the following sections. In the present case this means that the irradiance at the hit point due to reflection of sky radiation from the ground or from other obstructions is not considered.
-
-The above reflection factor is used in the timestep calculation to find the irradiance on a receiving surface due to sky radiation reflected from obstructions:
-
-QRadSWOutIncSkyDiffReflObs(RecSurfNum) =
- DifSolarRad \* ReflFacSkySolObs(RecSurfNum)  (W/m<sup>2</sup>)
-
-where*DifSolarRad* is the horizontal sky irradiance on an unobstructed horizontal plane (W/m<sup>2</sup>).
-
-### Sky Solar Radiation Diffusely Reflected from the Ground
-
-If a downgoing ray from a receiving point hits the ground (for example, rays 1-6 in Figure 54), the program calculates the radiance at the ground hit point due to sky diffuse solar reaching that point. To do this, rays are sent upward from the ground hit point and it is determined which of these rays are unobstructed and so go to the sky (for example, rays 6-10 in Figure 55). For this calculation it is assumed that the radiance of the sky is uniform.
-
-
-
-![](media/image685.png)
-
-Figure 55.  Two-dimensional schematic showing rays going upward from a ground hit point.
-
-The factor for reflection of sky radiation from the ground onto a receiving surface is calculated in subroutine CalcSkySolDiffuseReflFactors. It is given by:
-
-<div>$$\begin{array}{l}{\rm{ReflFacSkySolGnd(RecSurfNum)}} = \\\frac{1}{{{N_{rec}}}}\sum\limits_1^{{N_{rec}}} {\sum\limits_{i = 1}^{{N_{ray}}} {\left[ {(Hi{t_{gnd,i}}d{\Omega_i}\cos {\alpha_i}/\pi )\sum\limits_{j(i)}^{{N_{ray}}} {Hi{t_{sky,j(i)}}\cos {\alpha_{j(i)}}d{\Omega_{j(i)}}/\pi } } \right]} } \end{array}$$</div>
-
-
-
-where
-
-*<span>\(j(i)\)</span> * denotes an upgoing ray from the ground point hit by ray *i*from the receiving point,
-
-*Hit<sub>sky,j(i)</sub>* = 1 if ray* j(i*) hits the sky, = 0 otherwise,
-
-<span>\({\alpha_{j(i)}}\)</span>is the angle of incidence of ray <span>\(j(i)\)</span>with respect to the ground plane,
-
-<span>\(d{\Omega_{j(i)}}\)</span>is the solid angle element associated with ray <span>\(j(i)\)</span>.
-
-This factor is used in the timestep calculation to find the irradiance on a receiving surface due to sky radiation reflected from the ground:
-
-QRadSWOutIncSkyDiffReflGnd(RecSurfNum) =
- DifSolarRad \* <span>\({\rho_{gnd}}\)</span>\* ReflFacSkySolGnd(RecSurfNum)  (W/m<sup>2</sup>)
-
-where <span>\({\rho_{gnd}}\)</span>is the solar reflectance of the ground, which is assumed to be uniform over the ground plane but may vary monthly (because of snow cover, for example).
-
-### Beam Solar Radiation Diffusely Reflected from Obstructions
-
-This calculation is similar to that for sky solar reflected from obstructions. However, to find the radiance at a hit point on an obstruction a line is drawn from the hit point to center of the sun. From this line it is determined (1) if there is an obstruction between the hit point and the sun, in which case it is assumed that no beam solar reaches the hit point; and (2) if beam solar does reach the hit point, what the the solar angle of incidence at that point is.
-
-The calculation is done for the hourly sun positions on each of the design days. It is also done for hourly sun positions on selected days during the weather file run period (the same days for which the shadowing calculations are done).
-
-The factor for diffuse reflection of beam solar radiation from obstructions onto a receiving surface is calculated in subroutine CalcBeamSolDiffuseReflFactors. It is given by:
-
-<div>$${\rm{ReflFacBmToDiffSolObs(RecSurfNum,IHr)}} = \frac{1}{{{N_{rec}}}}\sum\limits_1^{{N_{rec}}} {\sum\limits_{i = 1}^{{N_{ray}}} {Hi{t_{obs,i}}Hi{t_{obs,i,sun}}d{\Omega_i}\cos {\alpha_i}{\rho_{obs,i}}\cos {\alpha_{sun,obs,i}}} } $$</div>
-
-where
-
-* IHr* = hour number
-
-<span>\(Hi{t_{obs,i}}\)</span>= 1 if ray *i* from the receiving point hits an obstruction, = 0 otherwise,
-
-<span>\(Hi{t_{obs,i,sun}}\)</span>= 1 if the line from ray *i*’s hit point to the sun is unobstructed, = 0 otherwise,
-
-<span>\({\alpha_{sun,obs,i}}\)</span> is the angle of incidence of the sun on the obstruction.
-
-This factor is used in the timestep calculation to find the diffuse irradiance on a receiving surface due to beam solar diffusely reflected from obstructions:
-
-QRadSWOutIncBmToDiffReflObs(RecSurfNum) = BeamSolarRad \*
- (WeightNow \* ReflFacBmToDiffSolObs(RecSurfNum,HourOfDay) +
- WeightPreviousHour \* ReflFacBmToDiffSolObs(RecSurfNum,PreviousHour))
-
-
-where *BeamSolarRad* is the timestep value of beam normal solar intensity (W/m2), and *WeightNow* and *WeightPreviousHour* are time-averaging factors.
-
-### Beam Solar Radiation Diffusely Reflected from the Ground
-
-This calculation is the same as that for beam solar diffusely reflected from obstructions except that only rays from a receiving point that hit the ground are considered. The factor for diffuse reflection of beam solar from the ground onto a receiving surface is calculated in subroutine CalcBeamSolDiffuseReflFactors. It is given by:
-
-<div>$${\rm{ReflFacBmToDiffSolGnd(RecSurfNum,IHr)}} = \frac{1}{{{N_{rec}}}}\sum\limits_1^{{N_{rec}}} {\sum\limits_{i = 1}^{{N_{ray}}} {Hi{t_{gnd,i}}Hi{t_{gnd,i,sun}}d{\Omega_i}\cos {\alpha_{gnd,i}}\cos {\alpha_{sun,gnd}}} } $$</div>
-
-where
-
-<span>\(Hi{t_{gnd,i}}\)</span>= 1 if ray *i* hits the ground, = 0 otherwise,
-
-<span>\(Hi{t_{gnd,i,sun}}\)</span>= 1 if the line from ray *i*’s hit point ot the sun is unobstructed, = 0 otherwise,
-
-<span>\({\alpha_{sun,gnd}}\)</span>= angle of incidence of sun on ground (= solar zenith angle).
-
-This factor is used in the timestep calculation to find the diffuse irradiance on a receiving surface due to beam solar diffusely reflected from the ground:
-
-QRadSWOutIncBmToDiffReflGnd(RecSurfNum) = BeamSolarRad \* <span>\({\rho_{gnd}}\)</span>\*
- (WeightNow \* ReflFacBmToDiffSolGnd(RecSurfNum,HourOfDay) +
- WeightPreviousHour \* ReflFacBmToDiffSolGnd(RecSurfNum,PreviousHour))
-
-
-
-### Beam Solar Radiation Specularly Reflected from Obstructions
-
-Figure 56 shows schematically how specular (beam-to-beam) reflection from an obstruction is calculated. [[7]](#_ftn7)
-
-![](media/image703.png)
-
-Figure 56.  Two-dimensional schematic showing specular reflection from an obstruction such as the glazed façade of a neighboring building. The receiving point receives specularly reflected beam solar radiation if (1) DB passes through specularly reflecting surface EF, (2) CD does not hit any obstructions (such as RS), and (3) AC does not hit any obstructions (such as PQ).
-
-The calculation procedure is as follows:
-
-1.    Select receiving point D on receiving surface JK.
-
-2.    Select specularly reflecting surface EF.
-
-3.    Find the mirror image, B, of the sun with respect to the plane of EF and construct ray DB.
-
-4.    Check if DB passes through EF; if yes, find intersection point C and construct ray CD.
-
-5.    Check if CD is obstructed.
-
-6.    If no, construct ray AC and check if it is obstructed.
-
-7.    If no, find reflected beam irradiance (W/m<sup>2</sup>) at D:
-
-<div>$$I_{D,refl}^{bm} = BeamSolarRad*{\rho_{spec}}({\alpha_C})\cos {\alpha_D}$$</div>
-
-where
-
-<span>\({\alpha_C}\)</span>= angle of incidence of beam solar at point C of the obstruction,
-
-<span>\({\rho_{spec}}({\alpha_C})\)</span>= reflectance of obstruction as a function of the angle of incidence,
-
-<span>\({\alpha_D}\)</span>= angle of incidence of ray CD on JK.
-
-The factor for specular reflection of beam solar from obstruction onto a receiving surface is calculated in subroutine CalcBeamSolSpecularReflFactors. It is given by:
-
-<div>$${\rm{ReflFacBmToBmSolObs(RecSurfNum,IHr) }} = \sum\limits_{\scriptstyle specularly\atop{\scriptstyle reflecting\atop\scriptstyle surfaces}} {} \left[ {\frac{1}{{{N_{rec}}}}\sum\limits_1^{{N_{rec}}} {{f_{C,glazed}}{\rho_{spec}}({\alpha_C})\cos {\alpha_D}} } \right]$$</div>
-
-The program assumes that specular reflection from a surface is due to glazing. If the reflecting surface is a window belonging to the building itself (as in Figure 51), then <span>\({f_{C,glazed}}\)</span>is the fraction of the window that is glazed (which is 1.0 unless the window has dividers).
-
-If the surface is a shading surface (that represents, for example, the glazed façade of a neigboring building) the surface reflection information is entered with the Shading Surface Reflectance object. This object contains values for:
-
-1.    Diffuse solar reflectance of the unglazed part of the shading surface
-
-2.    Diffuse visible reflectance of the unglazed part of the shading surface
-
-3.    Fraction of shading surface that is glazed
-
-4.    Name of glazing construction
-
-In this case <span>\({f_{C,glazed}}\)</span> is “Fraction of shading surface that is glazed� and <span>\({\rho_{spec}}({\alpha_C})\)</span>is the front reflectance of the indicated glazing construction as a function of beam solar incidence angle.
-
-The above specular reflection factor is used in the timestep calculation to find the beam irradiance on a receiving surface due to beam-beam reflection from obstructions:
-
-QRadSWOutIncBmToBmReflObsRecSurfNum) = BeamSolarRad \*
- (WeightNow \* ReflFacBmToBmSolObs(RecSurfNum,HourOfDay) +
- WeightPreviousHour \* ReflFacBmToBmSolObs(RecSurfNum,PreviousHour))
-
-
diff --git a/doc/src/docs/EngineeringReference/07-Daylighting.md b/doc/src/docs/EngineeringReference/07-Daylighting.md
deleted file mode 100644
index eb7723d3f6a..00000000000
--- a/doc/src/docs/EngineeringReference/07-Daylighting.md
+++ /dev/null
@@ -1,7425 +0,0 @@
-
-Daylighting and Window Calculations
-===================================
-
-Daylighting Calculations
-------------------------
-
-The EnergyPlus daylighting model, in conjunction with the thermal analysis, determines the energy impact of daylighting strategies based on analysis of daylight availability, site conditions, window management in response to solar gain and glare, and various lighting control strategies.
-
-The daylighting calculation has three main steps:
-
-1.    *Daylight factors*, which are ratios of interior illuminance or luminance to exterior horizontal illuminance, are calculated and stored. The user specifies the coordinates of one or two reference points in each daylit zone. EnergyPlus then integrates over the area of each exterior window in the zone to obtain the contribution of direct light from the window to the illuminance at the reference points, and the contribution of light that reflects from the walls, floor and ceiling before reaching the reference points. Window luminance and window background luminance, which are used to determine glare, are also calculated. Taken into account are such factors as sky luminance distribution, window size and orientation, glazing transmittance, inside surface reflectances, sun control devices such as movable window shades, and external obstructions. Dividing daylight illuminance or luminance by exterior illuminance yields daylight factors. These factors are calculated for the hourly sun positions on sun-paths for representative days of the run period. To avoid the spikes of daylight and glare factors calculated during some sunrise and/or sunset hours when exterior horizontal illuminance is very low, the daylight and glare factors for those hours are reset to 0.
-
-2.    A daylighting calculation is performed each heat-balance time step when the sun is up. In this calculation the illuminance at the reference points in each zone is found by interpolating the stored daylight factors using the current time step’s sun position and sky condition, then multiplying by the exterior horizontal illuminance. If glare control has been specified, the program will automatically deploy window shading, if available, to decrease glare below a specified comfort level. A similar option uses window shades to automatically control solar gain.
-
-3.    The electric lighting control system is simulated to determine the lighting energy needed to make up the difference between the daylighting illuminance level and the design illuminance. Finally, the zone lighting electric reduction factor is passed to the thermal calculation, which uses this factor to reduce the heat gain from lights.
-
-The EnergyPlus daylighting calculation is derived from the daylighting calculation in DOE-2.1E, which is described in [Winkelmann, 1983] and [Winkelmann and Selkowitz, 1985]. There are two major differences between the two implementations: (1) In EnergyPlus daylight factors are calculated for four different sky types—clear, clear turbid, intermediate, and overcast; in DOE-2 only two sky types are used—clear and overcast. (2) In EnergyPlus the clear-sky daylight factors are calculated for hourly sun-path sun positions several times a year whereas in DOE-2 these daylight factors are calculated for a set of 20 sun positions that span the annual range of sun positions for a given geographical location.
-
-Daylight Factor Calculation
----------------------------
-
-Table 25.  Variables in Daylighting Calculations
-
-<table class="table table-striped">
-  <tr>
-    <th>Mathematical Variable</th>
-    <th>Description</th>
-    <th>Units</th>
-    <th>Internal Variable</th>
-  </tr>
-  <tr>
-    <td>E<sub>h,sky</sub></td>
-    <td>Exterior horizontal illuminance due to light from the sky</td>
-    <td>lux</td>
-    <td>GILSK</td>
-  </tr>
-  <tr>
-    <td>E<sub>h,sun</sub></td>
-    <td>Exterior horizontal illuminance due to light from the sun</td>
-    <td>lux</td>
-    <td>GILSU</td>
-  </tr>
-  <tr>
-    <td>d<sub>sky</sub>,d<sub>sun</sub></td>
-    <td>Interior illuminance factor due</td>
-    <td>-</td>
-    <td>DFACSK,DFACSU</td>
-  </tr>
-  <tr>
-    <td>w<sub>sky</sub>,w<sub>sun</sub></td>
-    <td>Window luminance factor due to sky, sun related light</td>
-    <td>cd/lm</td>
-    <td>SFACSK, SFACSU</td>
-  </tr>
-  <tr>
-    <td>b<sub>sky</sub>,b<sub>sun</sub></td>
-    <td>Window background luminance factor due to sky, sun related light</td>
-    <td>cd/lm</td>
-    <td>BFACSK, BFACSU</td>
-  </tr>
-  <tr>
-    <td>N Number of exterior windows</td>
-    <td>Number of exterior windows in a zone</td>
-    <td>-</td>
-    <td>NWD</td>
-  </tr>
-  <tr>
-    <td>θ<sub>sky</sub>,φ<sub>sky</sub></td>
-    <td>Azimuth and altitude angles of a point in the sky</td>
-    <td>radians</td>
-    <td>THSKY, PHSKY</td>
-  </tr>
-  <tr>
-    <td>ψ<sub>cs</sub></td>
-    <td>Clear sky luminance distribution</td>
-    <td>cd/m2</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>ψ<sub>ts</sub></td>
-    <td>Clear turbid sky luminance distribution</td>
-    <td>cd/m2</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>ψ<sub>os</sub></td>
-    <td>Intermediate sky luminance distribution</td>
-    <td>cd/m2</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>ψ<sub>os</sub></td>
-    <td>Overcast sky luminance distribution</td>
-    <td>cd/m2</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>φ<sub>sun</sub></td>
-    <td>Altitude angle of the sun</td>
-    <td>radians or degrees</td>
-    <td>PHSUN</td>
-  </tr>
-  <tr>
-    <td>γ</td>
-    <td>Angle between point in the sky and the sun; or angle between vertical and ray from reference point to window element</td>
-    <td>radians</td>
-    <td>G</td>
-  </tr>
-  <tr>
-    <td>L<sub>z</sub></td>
-    <td>Sky zenith luminance</td>
-    <td>cd/m2</td>
-    <td>ZENL</td>
-  </tr>
-  <tr>
-    <td>Mathematical Variable</td>
-    <td>Optical air mass of the atmosphere</td>
-    <td>m</td>
-    <td>AM</td>
-  </tr>
-  <tr>
-    <td>h</td>
-    <td>Building altitude</td>
-    <td>m</td>
-    <td>ELEVATION</td>
-  </tr>
-  <tr>
-    <td>E<sub>h,k</sub></td>
-    <td>Exterior horizontal illuminance for sky type k</td>
-    <td>lux</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>N<sub>θ</sub>,N<sub>φ</sub></td>
-    <td>Number of azimuth, altitude steps for sky integration</td>
-    <td></td>
-    <td>NTH, NPH</td>
-  </tr>
-  <tr>
-    <td><span>\(\vec{R}_{ref}\)</span></td>
-    <td>Vector from zone origin to reference point</td>
-    <td>m</td>
-    <td>RREF</td>
-  </tr>
-  <tr>
-    <td><span>\(\vec{R}_{win}\)</span></td>
-    <td>Vector from zone origin to window element</td>
-    <td>m</td>
-    <td>RWIN</td>
-  </tr>
-  <tr>
-    <td>dΩ</td>
-    <td>Solid angle subtended by window element</td>
-    <td>steradians</td>
-    <td>DOMEGA</td>
-  </tr>
-  <tr>
-    <td>L<sub>w</sub></td>
-    <td>Luminance of a window element as seen from reference point</td>
-    <td>cd/m2</td>
-    <td>WLUMSK, WLUMSU</td>
-  </tr>
-  <tr>
-    <td>L<sub>w,shade</sub></td>
-    <td>Luminance of window element with shade in place</td>
-    <td>cd/m2</td>
-    <td>WLUMSK, WLUMSU</td>
-  </tr>
-  <tr>
-    <td>dE<sub>h</sub></td>
-    <td>Horizontal illuminance at reference point from window element</td>
-    <td>lux</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>dx, dy</td>
-    <td>Size of window element</td>
-    <td>m</td>
-    <td>DWX, DWY</td>
-  </tr>
-  <tr>
-    <td>D</td>
-    <td>Distance from reference point to window element</td>
-    <td>m</td>
-    <td>DIS</td>
-  </tr>
-  <tr>
-    <td>B</td>
-    <td>Angle between window element's outward normal and rat from reference point to window element</td>
-    <td>radians</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td><span>\(\hat{R}_{ref}\)</span></td>
-    <td>Unit vector from reference point to window element</td>
-    <td>-</td>
-    <td>RAY</td>
-  </tr>
-  <tr>
-    <td><span>\(\hat{W}_{n}\)</span></td>
-    <td>Unit vector normal to window element, pointing away from zone</td>
-    <td>-</td>
-    <td>WNORM</td>
-  </tr>
-  <tr>
-    <td><span>\(\hat{W}_{21}\)</span></td>
-    <td>Unit vector along window y-axis</td>
-    <td>-</td>
-    <td>W21</td>
-  </tr>
-  <tr>
-    <td><span>\(\hat{W}_{23}\)</span></td>
-    <td>Unit vector along window x-axis</td>
-    <td>-</td>
-    <td>W23</td>
-  </tr>
-  <tr>
-    <td>Ï„<sub>vis</sub></td>
-    <td>Glass visible transmittance</td>
-    <td>-</td>
-    <td>TVISB</td>
-  </tr>
-  <tr>
-    <td>L</td>
-    <td>Luminance of sky or obstruction</td>
-    <td>cd/m2</td>
-    <td>ELUM, -</td>
-  </tr>
-  <tr>
-    <td>Φ<sub>FW</sub></td>
-    <td>Downgoing luminous flux from a window</td>
-    <td>lm</td>
-    <td>FLFW –</td>
-  </tr>
-  <tr>
-    <td>Φ<sub>CW</sub></td>
-    <td>Upgoing luminous flux from a window</td>
-    <td>lm</td>
-    <td>FLCW –</td>
-  </tr>
-  <tr>
-    <td>F<sub>1</sub></td>
-    <td>First-reflected flux</td>
-    <td>lm</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>�<sub>FW</sub></td>
-    <td>Area-weighted reflectance of floor and upper part of walls</td>
-    <td>-</td>
-    <td>SurfaceWindow%RhoFloorWall</td>
-  </tr>
-  <tr>
-    <td>�<sub>CW</sub></td>
-    <td>Area-weighted reflectance of ceiling and upper part of walls</td>
-    <td>-</td>
-    <td>SurfaceWindow%RhoCeilingWall</td>
-  </tr>
-  <tr>
-    <td>E<sub>r</sub></td>
-    <td>Average internally-reflected illuminance</td>
-    <td>lux</td>
-    <td>EINTSK, EINTSU</td>
-  </tr>
-  <tr>
-    <td>A</td>
-    <td>Total inside surface area of a zone</td>
-    <td>m2</td>
-    <td>ATOT</td>
-  </tr>
-  <tr>
-    <td>�</td>
-    <td>Area-weighted average reflectance of zone interior surfaces</td>
-    <td>-</td>
-    <td>ZoneDaylight%AveVisDiffREflect</td>
-  </tr>
-  <tr>
-    <td>θ, φ</td>
-    <td>Azimuth and altitude angle of a sky or ground element</td>
-    <td>radians</td>
-    <td>TH, PH</td>
-  </tr>
-  <tr>
-    <td>L(θ, φ)</td>
-    <td>Luminance of sky or ground element at (θ, φ)</td>
-    <td>cd/m2</td>
-    <td>HitPointLum--</td>
-  </tr>
-  <tr>
-    <td>A<sub>w</sub></td>
-    <td>Area of glazed part of window</td>
-    <td>m2</td>
-    <td>Surface%Area</td>
-  </tr>
-  <tr>
-    <td>β</td>
-    <td>Angle of incidence, at center of window, of light from a sky or ground element</td>
-    <td>radians</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>T(β)</td>
-    <td>Glazing visible transmittance at incidence angle β</td>
-    <td></td>
-    <td>TVISBR</td>
-  </tr>
-  <tr>
-    <td>dΦ<sub>inc</sub></td>
-    <td>Luminous flux incident on window from sky or ground element</td>
-    <td>lm</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>dΦ</td>
-    <td>Luminous flux from sky or ground element transmitted through window</td>
-    <td>lm</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>dΦ<sub>FW|, dΦ<sub>CW</sub></td>
-    <td>Luminous flux from sky or ground element transmitted through window and going downward, upward</td>
-    <td>lm</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>{min</sub>, θ{max</sub></td>
-    <td>Azimuth angle integration limits</td>
-    <td>radians</td>
-    <td>THMIN, THMAX</td>
-  </tr>
-  <tr>
-    <td>φ<sub>w</sub></td>
-    <td>Window normal altitude angle</td>
-    <td>radians</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>Φ<sub>sh</sub>,Φ<sub>unsh</sub></td>
-    <td>Transmitted flux through window and shade, without shade</td>
-    <td>lm</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>Φ<sub>CW,sh</sub>,Φ<sub>FW,sh</sub></td>
-    <td>Upgoing and downgoing portions of transmitted flux through window with shade</td>
-    <td>lm</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>Φ<sub>CW,unsh</sub>,Φ<sub>FW,unsh</sub></td>
-    <td>Upgoing and downgoing portions of transmitted flux through window without shade</td>
-    <td>lm</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>f</td>
-    <td>Fraction of hemisphere seen by the inside of window that lies above the window midplane</td>
-    <td>-</td>
-    <td>SurfaceWindow%Fraction UpGoing</td>
-  </tr>
-  <tr>
-    <td>Φ<sub>inc</sub></td>
-    <td>Flux incident on glazing from direct sun</td>
-    <td>lm</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>f<sub>sunlit</sub></td>
-    <td>Fraction of glazing that is sunlit</td>
-    <td>-</td>
-    <td>SunLitFrac</td>
-  </tr>
-  <tr>
-    <td>Φ</td>
-    <td>Transmitted flux from direct sun</td>
-    <td>-</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>L<sub>sh</sub></td>
-    <td>Luminance of window with shade</td>
-    <td>cd/m2</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>L<sub>b</sub></td>
-    <td>Window background luminance</td>
-    <td>cd/m2</td>
-    <td>BLUM</td>
-  </tr>
-  <tr>
-    <td>G</td>
-    <td>Discomfort glare constant</td>
-    <td>-</td>
-    <td>GTOT</td>
-  </tr>
-  <tr>
-    <td>G<sub>i</sub></td>
-    <td>Discomfort glare constant from window I</td>
-    <td>-</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>ω</td>
-    <td>Solid angle subtended by window with respect to reference point</td>
-    <td>steradians</td>
-    <td>SolidAngAtRefPt</td>
-  </tr>
-  <tr>
-    <td>Ω</td>
-    <td>Solid angle subtended by window with respect to reference point, modified to take direction of occupant view into account</td>
-    <td>steradians</td>
-    <td>SolidAngAtRefPtWtd</td>
-  </tr>
-  <tr>
-    <td>N<sub>x</sub>,N<sub>y</sub></td>
-    <td>Number of elements in x and y direction that window is divided into for glare calculation</td>
-    <td>-</td>
-    <td>NWX, NWY</td>
-  </tr>
-  <tr>
-    <td>p(x<sub>R</sub>,y<sub>R</sub>)</td>
-    <td>Position factor for horizontal and vertical displacement ratios x_{R} and y_{R}</td>
-    <td>-</td>
-    <td>DayltgGlarePositionFactor</td>
-  </tr>
-  <tr>
-    <td>p<sub>H</sub></td>
-    <td>Hopkinson position factor</td>
-    <td>-</td>
-    <td>DayltgGlarePositionFactor</td>
-  </tr>
-  <tr>
-    <td>L<sub>b</sub></td>
-    <td>Window background luminance</td>
-    <td>cd/m2</td>
-    <td>BLUM</td>
-  </tr>
-  <tr>
-    <td>E<sub>b</sub></td>
-    <td>Illuminance on window background</td>
-    <td>lm</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>E<sub>r</sub></td>
-    <td>Total internally-reflected component of daylight illuminance</td>
-    <td>lm</td>
-    <td>-</td>
-  </tr>
-  <tr>
-    <td>E<sub>s</sub></td>
-    <td>Illuminance setpoint</td>
-    <td>lm</td>
-    <td>IllumSetPoint</td>
-  </tr>
-  <tr>
-    <td>G<sub>i</sub></td>
-    <td>Glare Index</td>
-    <td>-</td>
-    <td>GLINDX</td>
-  </tr>
-</table>
-
-### Overview
-
-There are three types of daylight factors: interior illuminance factors, window luminance factors, and window background luminance factors. To calculate these factors the following steps are carried out for each hourly sun position on the sun paths for the design days and for representative days[[8]](#_ftn8) during the simulation run period:
-
-1.    Calculate exterior horizontal daylight illuminance from sky and sun for standard (CIE) clear and overcast skies.
-
-2.    Calculate interior illuminance, window luminance and window background luminance for each window/reference-point combination, for bare and for shaded window conditions (if a shading device has been specified), for overcast sky and for standard clear sky.
-
-3.    Divide by exterior horizontal illuminance to obtain daylight factors.
-
-### Interior Illuminance Components
-
-To calculate daylight factors, daylight incident on a window is separated into two components: (1) light that originates from the *sky* and reaches the window directly or by reflection from exterior surfaces; and (2) light that originates from the *sun* and reaches the window directly or by reflection from exterior surfaces. Light from the window reaches the workplane directly or via reflection from the interior surfaces of the room.
-
-For fixed sun position, sky condition (clear or overcast) and room geometry, the sky-related interior daylight will be proportional to the exterior horizontal illuminance, *E<sub>h,sky</sub>*, due to light from the sky. Similarly, the sun-related interior daylight will be proportional to the exterior horizontal solar illuminance, *E<sub>h,sun</sub>*.
-
-### Daylight Factors
-
-The following daylight factors are calculated:
-
-<div>$${d_{sky}} = \frac{{{\rm{Illuminance at reference point due to sky - related light}}}}{{{E_{h,sky}}}}$$</div>
-
-<div>$${d_{sun}} = \frac{{{\rm{Illuminance at reference point due to sun - related light}}}}{{{E_{h,sun}}}}$$</div>
-
-<div>$${w_{sky}} = \frac{{{\rm{Average window luminance due to sky - related light}}}}{{{E_{h,sky}}}}$$</div>
-
-<div>$${w_{sun}} = \frac{{{\rm{Average window luminance due to sun - related light}}}}{{{E_{h,sun}}}}$$</div>
-
-<div>$${b_{sky}} = \frac{{{\rm{Window background luminance due to sky - related light}}}}{{{E_{h,sky}}}}$$</div>
-
-<div>$${b_{sun}} = \frac{{{\rm{Window background luminance due to sun - related light}}}}{{{E_{h,sun}}}}$$</div>
-
-For a daylit zone with *N* windows these six daylight factors are calculated for each of the following combinations of reference point, window, sky-condition/sun-position and shading device:
-
-<div>$$
-  \left[
-    \begin{array}{c}
-      Ref pt 1 \\
-      Ref pt 2
-    \end{array}
-  \right]
-  \left[
-    \begin{array}{c}
-      Window 1 \\
-      Window 2 \\
-      ... \\
-      Window N
-    \end{array}
-  \right]
-  \left[
-    \begin{array}{c}
-      Clear sky, first sun-up hour \\
-      Clear/turbid sky, first sun-up hour \\
-      Intermediate sky, first sun-up hour \\
-      Overcast sky, first sun-up hour \\
-      ...
-      Clear sky, last sun-up hour \\
-      Clear/turbid sky, last sun-up hour \\
-      Intermediate sky, last sun-up hour \\
-      Overcase sky, last sun-up hour
-    \end{array}
-   \right]
-   \left[
-     \begin{array}{c}
-       Unshaded window \\
-       Shaded window \\
-       (if shade assigned)
-     \end{array}
-   \right]
-$$</div>
-
-### Sky Luminance Distributions
-
-The luminance distribution of the sky is represented as a superposition of four standard CIE skies using the approach described in (Perez et al. 1990). The standard skies are as follows.
-
-#### Clear Sky
-
-The clear sky luminance distribution has the form (Kittler, 1965; CIE, 1973)
-
-<div>$${\psi_{cs}}({\theta_{sky}},{\phi_{sky}}) = {L_z}\frac{{(0.91 + 10{e^{ - 3\gamma }} + 0.45{{\cos }^2}\gamma )(1 - {e^{ - 0.32{\rm{cosec}}{\phi_{sky}}}})}}{{0.27385(0.91 + 10{e^{ - 3(\frac{\pi }{2} - {\phi_{sun}})}} + 0.45{{\sin }^2}{\phi_{sun}})}}$$</div>
-
-Here, *L<sub>z</sub>* is the zenith luminance (i.e., the luminance of the sky at a point directly overhead). In the calculation of daylight factors, which are ratios of interior and exterior illumination quantities that are both proportional to *L<sub>z</sub>*, the zenith luminance cancels out. For this reason we will use *L<sub>z</sub>* = 1.0 for all sky luminance distributions.
-
-The various angles, which are defined in the building coordinate system, are shown in Figure 48. The angle,* γ*, between sun and sky element is given by
-
-<div>$$\gamma  = {\cos ^{ - 1}}\left[ {\sin {\phi_{sky}}\sin {\phi_{sun}} + \cos {\phi_{sky}}\cos {\phi_{sun}}\cos ({\theta_{sky}} - {\theta_{sun}})} \right]$$</div>
-
-The general characteristics of the clear-sky luminance distribution are a large peak near the sun; a minimum at a point on the other side of  the zenith from the sun, in the vertical plane containing the sun; and an increase in luminance as the horizon is approached.
-
-#### Clear Turbid Sky
-
-The clear turbid sky luminance distribution has the form [Matsuura, 1987]
-
-<div>$${\psi_{ts}}({\theta_{sky}},{\phi_{sky}}) = {L_z}\frac{{(0.856 + 16{e^{ - 3\gamma }} + 0.3{{\cos }^2}\gamma )(1 - {e^{ - 0.32{\rm{cosec}}{\phi_{sky}}}})}}{{0.27385(0.856 + 10{e^{ - 3(\frac{\pi }{2} - {\phi_{sun}})}} + 0.3{{\sin }^2}{\phi_{sun}})}}$$</div>
-
-#### Intermediate Sky
-
-The intermediate sky luminance distribution has the form [Matsuura, 1987]
-
-<div>$${\psi_{is}}\left( {{\theta_{sky}},{\phi_{sky}}} \right) = {L_z}{Z_1}{Z_2}/({Z_3}{Z_4})$$</div>
-
-where
-
-<span>\({Z_1} = \left[ {1.35(\sin (3.59{\phi_{sky}} - 0.009) + 2.31)\sin (2.6{\phi_{sun}} + 0.316) + {\phi_{sky}} + 4.799} \right]/2.326\)</span><span>\({Z_2} = \exp \left[ { - 0.563\gamma \{ ({\phi_{sun}} - 0.008)({\phi_{sky}} + 1.059) + 0.812\} } \right]\)</span>
-
-<div>$${Z_3} = 0.99224\sin (2.6{\phi_{sun}} + 0.316) + 2.73852$$</div>
-
-<div>$${Z_4} = \exp \left[ { - 0.563({\textstyle{\pi  \over 2}} - {\phi_{sun}})\{ 2.6298({\phi_{sun}} - 0.008) + 0.812\} } \right]$$</div>
-
-
-
-![ClearSkyAngles](media/image733.png)
-
-Figure 57.  Angles appearing in the expression for the clear-sky luminance distribution.
-
-#### Overcast Sky
-
-The overcast sky luminance distribution has the form [Moon & Spencer, 1942]
-
-<div>$${\psi_{os}}({\phi_{sky}}) = {L_z}\frac{{1 + 2\sin {\phi_{sky}}}}{3}$$</div>
-
-Unlike the clear sky case, the overcast sky distribution does not depend on the solar azimuth or the sky azimuth. Note that at fixed solar altitude the zenith (<span>\({\phi_{sky}} = \pi /2\)</span>) is three times brighter than the horizon (<span>\({\phi_{sky}} = 0\)</span>).
-
-### Direct Normal Solar Illuminance
-
-For purposes of calculating daylight factors associated with beam solar illuminance, the direct normal solar illuminance is taken to be 1.0 W/m<sup>2</sup>. The actual direct normal solar illuminance, determined from direct normal solar irradiance from the weather file and empirically-determined luminious efficacy, is used in the time-step calculation.
-
-### Exterior Horizontal Illuminance
-
-The illuminance on an unobstructed horizontal plane due to diffuse radiation from the sky is calculated for each of the four sky types by integrating over the appropriate sky luminance distribution:
-
-<div>$${E_{h,k}} = \int\limits_0^{2\pi } {\int\limits_0^{\pi /2} {{\psi_k}({\theta_{sky}},{\phi_{sky}})\sin {\phi_{sky}}\cos {\phi_{sky}}d{\theta_{sky}}} } d{\phi_{sky}}$$</div>
-
-where* k* = *cs*, *ts*, *is* or *os*. The integral is evaluated as a double summation:
-
-<div>$${E_{h,k}} = \sum\limits_{i = 1}^{{N_\theta }} {\sum\limits_{j = 1}^{{N_\phi }} {{\psi_k}\left( {{\theta_{sky}}(i),{\phi_{sky}}(j)} \right)} } \sin {\phi_{sky}}(j)\cos {\phi_{sky}}(j)\Delta {\theta_{sky}}\Delta {\phi_{sky}}$$</div>
-
-where
-
-<div>$$
-  \begin{array}{l}
-    \theta_{sky}(i) = (i - 1/2) \Delta \theta_{sky} \\
-    \phi_{sky}(j) = (j - 1/2) \Delta \phi_{sky} \\
-    \Delta \theta_{sky} = 2 \pi / N_{\theta} \\
-    \Delta \phi_{sky} = \pi / 2N_{\phi} 
-  \end{array}
-$$</div>
-
-<span>\({N_\theta } = 18\)</span> and <span>\({N_\phi } = 8\)</span> were found to give a <span>\(\pm 1\% \)</span>accuracy in the calculation of <span>\({E_h}_{,k}\)</span>.
-
-### Direct Component of Interior Daylight Illuminance
-
-The direct daylight illuminance at a reference point from a particular window is determined by dividing the window into an x-y grid and finding the flux reaching the reference point from each grid element. The geometry involved is shown in Figure 58. The horizontal illuminance at the reference point, <span>\({\vec R_{ref}}\)</span>, due to a window element is
-
-<div>$$d{E_h} = {L_w}d\Omega \cos \gamma $$</div>
-
-where *L<sub>w</sub>* is the luminance of the window element as seen from the reference point.
-
-The subtended solid angle is approximated by
-
-<div>$$d\Omega  = \frac{{dxdy}}{{{D^2}}}\cos B$$</div>
-
-where
-
-<div>$$D = \left| {{{\bar R}_{win}} - {{\bar R}_{ref}}} \right|$$</div>
-
-*CosB* is found from
-
-<div>$$\cos B = {\hat R_{ray}} \cdot {\hat W_n}$$</div>
-
-where
-
-<div>$${\vec R_{ray}} = ({\vec R_{win}} - {\vec R_{ref}})/D$$</div>
-
-<div>$${\hat W_n} = {\rm{ window outward normal }} = {\hat W_{21}} \times {\hat W_{23}} = \frac{{{{\vec W}_1} - {{\vec W}_2}}}{{\left| {{{\vec W}_1} - {{\vec W}_2}} \right|}} \times \frac{{{{\vec W}_3} - {{\vec W}_2}}}{{\left| {{{\vec W}_3} - {{\vec W}_2}} \right|}}$$</div>
-
-Equation becomes exact as <span>\(dx/D{\rm{ and }}dy/D \to 0\)</span>and is accurate to better than about 1% for <span>\(dx \le D/4{\rm{ and }}dy \le D/4\)</span>.
-
-The net illuminance from the window is obtained by summing the contributions from all the window elements:
-
-<div>$${E_h} = \sum\limits_{\scriptstyle window\atop\scriptstyle elements} {{L_w}d\Omega \cos \gamma } $$</div>
-
-In performing the summation, window elements that lie below the workplane (<span>\(\cos \gamma  &lt; 0\)</span>) are omitted since light from these elements cannot reach the workplane directly.
-
-![GeomDirComp](media/image755.png)
-
-Figure 58.  Geometry for calculation of direct component of daylight illuminance at a reference point. Vectors R<sub>ref</sub>, W<sub>1</sub>, W<sub>2</sub>, W<sub>3</sub> and R<sub>win</sub> are in the building coordinate system.
-
-#### Unshaded Window
-
-For the unshaded window case, the luminance of the window element is found by projecting the ray from reference point to window element and determining whether it intersects the sky or an exterior obstruction such as an overhang. If *L* is the corresponding luminance of the sky or obstruction, the window luminance is
-
-<div>$${L_w} = L{\tau_{vis}}$$</div>
-
-where <span>\({\tau_{vis}}\)</span>is the visible transmittance of the glass for incidence angle *B*.
-
-Exterior obstructions are generally opaque (like fins, overhangs, neighboring buildings, and the building’s own wall and roof surfaces) but can be transmitting (like a tree or translucent awning). Exterior obstructions are assumed to be non-reflecting. If *L<sub>sky</sub>* is the sky luminance and *t<sub>obs</sub>* is the transmittance of the obstruction (assumed independent of incidence angle), then *L* =* L<sub>sky</sub>t<sub>obs</sub>*. Interior obstructions are assumed to be opaque (*t<sub>obs</sub>* = 0).
-
-#### Shaded Window
-
-For the window-plus-shade case the shade is assumed to be a perfect diffuser, i.e., the luminance of the shade is independent of angle of emission of light, position on shade, and angle of incidence of solar radiation falling on the shade. Closely-woven drapery fabric and translucent roller shades are closer to being perfect diffusers than Venetian blinds or other slatted devices, which usually have non-uniform luminance characteristics.
-
-The calculation of the window luminance with the shade in place, *L<sub>w,sh</sub>*, is described in [Winkelmann, 1983]. The illuminance contribution at the reference point from a shaded window element is then given by Eq. (152) with <span>\({L_w} = {L_{w,sh}}\)</span>.
-
-### Internally-Reflected Component of Interior Daylight Illuminance
-
-Daylight reaching a reference point after reflection from interior surfaces is calculated using the *split-flux* method [Hopkinson et al., 1954], [Lynes, 1968]. In this method the daylight transmitted by the window is split into two parts—a downward-going flux, <span>\({\Phi_{FW}}\)</span>(lumens), which falls on the floor and portions of the walls below the imaginary horizontal plane passing through the center of the window (*window midplane*), and an upward-going flux, <span>\({\Phi_{CW}}\)</span>, that strikes the ceiling and portions of the walls above the window midplane. A fraction of these fluxes is absorbed by the room surfaces. The remainder, the first-reflected flux, *F<sub>1</sub>*, is approximated by
-
-<div>$${F_1} = {\Phi_{FW}}{\rho_{FW}} + {\Phi_{CW}}{\rho_{CW}}$$</div>
-
-where *�<sub>FW</sub>* is the area-weighted average reflectance of the floor and those parts of the walls below the window midplane, and *�<sub>CW</sub>* is the area-weighted average reflectance of the ceiling and those parts of the walls above the window midplane.
-
-To find the final average internally-reflected illuminance, *E<sub>r</sub>*, on the room surfaces (which in this method is uniform throughout the room) a flux balance is used. The total reflected flux absorbed by the room surfaces (or lost through the windows) is *AE<sub>r</sub>(1-�)*, where *A* is the total inside surface area of the floor, walls, ceiling and windows in the room, and *�* is the area-weighted average reflectance of the room surfaces, including windows. From conservation of energy
-
-<div>$$A{E_r}(1 - \rho ) = {F_1}$$</div>
-
-or
-
-<div>$${E_r} = \frac{{{\Phi_{FW}}{\rho_{FW}} + {\Phi_{CW}}{\rho_{CW}}}}{{A(1 - \rho )}}$$</div>
-
-This procedure assumes that the room behaves like an integrating sphere with perfectly diffusing interior surfaces and with no internal obstructions. It therefore works best for rooms that are close to cubical in shape, have matte surfaces (which is usually the case), and have no internal partitions. Deviations from these conditions, such as would be the case for rooms whose depth measured from the window-wall is more than three times greater than ceiling height, can lead to substantial inaccuracies in the split-flux calculation.
-
-### Transmitted Flux from Sky and Ground
-
-The luminous flux incident on the center of the window from a luminous element of sky or ground at angular position <span>\((\theta ,\phi )\)</span>, of luminance <span>\(L(\theta ,\phi )\)</span>, and subtending a solid angle <span>\(\cos \phi d\theta d\phi \)</span> is
-
-<div>$$d{\Phi_{inc}} = {A_w}L(\theta ,\phi )\cos \beta \cos \phi d\theta d\phi $$</div>
-
-The transmitted flux is
-
-<div>$$d\Phi  = d{\Phi_{inc}}T(\beta )$$</div>
-
-where *T(β)* is the window transmittance for light at incidence angle *β*. This transmittance depends on whether or not the window has a shade.
-
-For an unshaded window the total downgoing transmitted flux is obtained by integrating over the part of the exterior hemisphere seen by the window that lies above the window midplane. This gives
-
-<div>$${\Phi_{FW,unshaded}} = {A_w}\int\limits_{{\theta_{\min }}}^{{\theta_{\max }}} {\int\limits_0^{\pi /2} {L(\theta ,\phi )T(\beta )\cos \beta \cos \phi d\theta d\phi } } $$</div>
-
-The upgoing flux is obtained similarly by integrating over the part of the exterior hemisphere that lies below the window midplane:
-
-<div>$${\Phi_{CW,unshaded}} = {A_w}\int\limits_{{\theta_{\min }}}^{{\theta_{\max }}} {\int\limits_{\pi /2 - {\phi_w}}^0 {L(\theta ,\phi )T(\beta )\cos \beta \cos \phi d\theta d\phi } } $$</div>
-
-where <span>\({\phi_w}\)</span>is the angle the window outward normal makes with the horizontal plane.
-
-For a window with a diffusing shade the total transmitted flux is
-
-<div>$${\Phi_{sh}} = {A_w}\int\limits_{{\theta_{\min }}}^{{\theta_{\max }}} {\int\limits_{\pi /2 - {\phi_w}}^{\pi /2} {L(\theta ,\phi )T(\beta )\cos \beta \cos \phi d\theta d\phi } } $$</div>
-
-The downgoing and upgoing portions of this flux are
-
-<div>$$
-  \begin{array}{l}
-    \Phi_{FW,sh} = \Phi (1 - f) \\
-    \Phi_{CW,sh} = \Phi f
-  \end{array}
-$$</div>
-
-where *f*, the fraction of the hemisphere seen by the inside of the window that lies above the window midplane, is given by
-
-<div>$$f = 0.5 - {\phi_w}/\pi $$</div>
-
-For a vertical window (<span>\({\phi_w} = 0\)</span>) the up- and down-going transmitted fluxes are equal:
-
-<span>\({\Phi_{FW,sh}} = {\Phi_{CW,sh}} = \Phi /2\)</span>.
-
-For a horizontal skylight (<span>\({\phi_w} = \pi /2\)</span>):
-
-<div>$${\Phi_{FW,sh}} = \Phi ,{\Phi_{CW,sh}} = 0$$</div>
-
-The limits of integration of *θ* in Equations (153), (154) and (155) depend on <span>\(\phi \)</span>. From [Figure # 12 - Winkelmann, 1983] we have
-
-<div>$$\sin \alpha  = \sin (A - \pi /2) = \frac{{\sin \phi \tan {\phi_w}}}{{\cos \phi }}$$</div>
-
-which gives
-
-<div>$$A = {\cos ^{ - 1}}(\tan \phi \tan {\phi_w})$$</div>
-
-Thus
-
-<div>$$
-  \begin{array}{l}
-    \theta_{min} &=  - \left| \cos^{-1}(-\tan\phi\tan\phi_w) \right| \\
-    \theta_{max} &= \left| \cos^{-1}(-\tan\phi\tan\phi_w) \right| 
-  \end{array}
-$$</div>
-
-### Transmitted Flux from Direct Sun
-
-The flux incident on the window from direct sun is
-
-<div>$${\Phi_{inc}} = {A_w}{E_{DN}}\cos \beta {f_{sunlit}}$$</div>
-
-The transmitted flux is
-
-<div>$$\Phi  = T(\beta ){\Phi_{inc}}$$</div>
-
-where T is the net transmittance of the window glazing (plus shade, if present).
-
-For an unshaded window all of the transmitted flux is downward since the sun always lies above the window midplane. Therefore
-
-<div>$$
-  \begin{array}{l}
-    \Phi_{FW,unsh} = \Phi \\
-    \Phi_{CW,unsh} = 0
-  \end{array}
-$$</div>
-
-For a window with a diffusing shade
-
-<div>$$
-  \begin{array}{l}
-    \Phi_{FW,sh} = \Phi (1 - f) \\
-    \Phi_{CW,sh} = \Phi f
-  \end{array}
-$$</div>
-
-### Luminance of Shaded Window
-
-The luminance of a shaded window is determined at the same time that the transmitted flux is calculated. It is given by
-
-<div>$${L_{sh}} = \frac{1}{\pi }\int\limits_{{\theta_{\min }}}^{{\theta_{\max }}} {\int\limits_{\pi /2 - {\phi_w}}^{\pi /2} {L(\theta ,\phi )T(\beta )\cos \beta \cos \phi d\theta d\phi } } $$</div>
-
-### Daylight Discomfort Glare
-
-The discomfort glare at a reference point due to luminance contrast between a window and the interior surfaces surrounding the window is given by [Hopkinson, 1970] and [Hopkinson, 1972]:
-
-<div>$$G = \frac{{L_w^{1.6}{\Omega ^{0.8}}}}{{{L_b} + 0.07{\omega ^{0.5}}{L_w}}}$$</div>
-
-where
-
-*G* = discomfort glare constant
-
-*L<sub>w</sub>* = average luminance of the window as seen from the reference point
-
-*Ω* = solid angle subtended by window, modified to take direction of occupant view into account
-
-*L<sub>b</sub>* = luminance of the background area surrounding the window
-
-By dividing the window into *N<sub>x</sub>* by *N<sub>y</sub>* rectangular elements, as is done for calculating the direct component of interior illuminance, we have
-
-<div>$${L_w} = \frac{{\sum\limits_{j = 1}^{{N_y}} {\sum\limits_{i = 1}^{{N_x}} {{L_w}(i,j)} } }}{{{N_x}{N_y}}}$$</div>
-
-where *L<sub>w</sub>(i,j)* is the luminance of element* (i,j)* as seen from the reference point.
-
-Similarly,
-
-<div>$$\omega  = \sum\limits_{j = 1}^{{N_y}} {\sum\limits_{i = 1}^{{N_x}} {d\omega (i,j)} } $$</div>
-
-where *dω(i,j)* is the solid angle subtended by element* (i,j)*with respect to the reference point.
-
-The modified solid angle is
-
- <span>\(\Omega  = \sum\limits_{j = 1}^{{N_y}} {\sum\limits_{i = 1}^{{N_x}} {d\omega (i,j)} } p({x_R},{y_R})\)</span>
-
-where p is a “position factor� [Petherbridge & Longmore, 1954] that accounts for the decrease in visual excitation as the luminous element moves away from the line of sight. This factor depends on the horizontal and vertical displacement ratios, *x<sub>R</sub>* and *y<sub>R</sub>* (Figure 59),  given by
-
-<div>$$
-  \begin{array}{rl}
-    x_R(i,j) &= \frac{\sqrt{A^2-(YD)^2}}{RR} \\
-    y_R(i,j) &= \left|YD/RR\right|
-  \end{array}
-$$</div>
-
-where
-
-<div>$$
-  \begin{array}{rl}
-    RR &= D (\hat{R}_{ray}\cdot\hat{v}_{view}) \\
-    A^2 &= D^2 - (RR)^2 \\
-    YD = R_{win}(3) - R_{ref}(3)
-  \end{array}
-$$</div>
-
-![GeomGlare](media/image794.png)
-
-Figure 59.  Geometry for calculation of displacement ratios used in the glare formula.
-
-The factor *p* can be obtained from graphs given in [Petherbridge & Longmore, 1954] or it can be calculated from tabulated values of *p<sub>H</sub>*, the Hopkinson position factor [Hopkinson, 1966], since <span>\(p = p_H^{1.25}\)</span>. The values resulting from the latter approach are given in Table 26. Interpolation of this table is used in EnergyPlus to evaluate *p* at intermediate values of *x<sub>R</sub>* and *y<sub>R</sub>*.
-
-Table 26.  Position factor for glare calculation
-
-<table class="table table-striped">
- <tr>
-  <th colspan="2" rowspan="2"></th>
-  <th colspan="8">X<sub>R</sub>: Horizontal Displacement Factor</th>
- </tr>
- <tr>
-  <th>0.0</th>
-  <th>0.5</th>
-  <th>1.0</th>
-  <th>1.5</th>
-  <th>2.0</th>
-  <th>2.5</th>
-  <th>3.0</th>
-  <th>&gt;3.0</th>
- </tr>
- <tr>
-  <th rowspan="6">y<sub>R</sub>: Vertical Displacement Factor</th>
-  <th>0</th>
-  <td>1.00</td>
-  <td>0.492</td>
-  <td>0.226</td>
-  <td>0.128</td>
-  <td>0.081</td>
-  <td>0.061</td>
-  <td>0.057</td>
-  <td>0</td>
- </tr>
- <tr>
-  <th>0.5</th>
-  <td>0.123</td>
-  <td>0.119</td>
-  <td>0.065</td>
-  <td>0.043</td>
-  <td>0.029</td>
-  <td>0.026</td>
-  <td>0.023</td>
-  <td>0</td>
- </tr>
- <tr>
-  <th>1.0</th>
-  <td>0.019</td>
-  <td>0.026</td>
-  <td>0.019</td>
-  <td>0.016</td>
-  <td>0.014</td>
-  <td>0.011</td>
-  <td>0.011</td>
-  <td>0</td>
- </tr>
- <tr>
-  <th>1.5</th>
-  <td>0.008</td>
-  <td>0.008</td>
-  <td>0.008</td>
-  <td>0.008</td>
-  <td>0.008</td>
-  <td>0.006</td>
-  <td>0.006</td>
-  <td>0</td>
- </tr>
- <tr>
-  <th>2.0</th>
-  <td>0</td>
-  <td>0</td>
-  <td>0.003</td>
-  <td>0.003</td>
-  <td>0.003</td>
-  <td>0.003</td>
-  <td>0.003</td>
-  <td>0</td>
- </tr>
- <tr>
-  <th>&gt;2.0</th>
-  <td>0</td>
-  <td>0</td>
-  <td>0</td>
-  <td>0</td>
-  <td>0</td>
-  <td>0</td>
-  <td>0</td>
-  <td>0</td>
- </tr>
- <tr>
-  <th>1.5</th>
-  <td>0.008</td>
-  <td>0.008</td>
-  <td>0.008</td>
-  <td>0.008</td>
-  <td>0.008</td>
-  <td>0.006</td>
-  <td>0.006</td>
-  <td>0</td>
- </tr>
-</table>
-
-The background luminance is
-
-<div>$${L_b} = {E_b}{\rho_b}$$</div>
-
-where *�<sub>b</sub>* is approximated by the average interior surface reflectance of the entire room and
-
-<div>$${E_b} = \max ({E_r},{E_s})$$</div>
-
-where *E<sub>r</sub>*is the total internally-reflected component of daylight illuminance produced by all the windows in the room and *E<sub>s</sub>* is the illuminance setpoint at the reference point at which glare is being calculated. A precise calculation of *E<sub>b</sub>* is not required since the glare index (see next section) is logarithmic. A factor of two variation in *E<sub>b</sub>* generally produces a change of only 0.5 to 1.0 in the glare index.
-
-#### Glare Index
-
-The net daylight glare at a reference point due to all of the windows in a room is expressed in terms of a *glare index* given by
-
-<div>$${G_I} = 10{\log_{10}}\sum\limits_{i = 1}^{\scriptstyle{\rm{number of}}\atop\scriptstyle{\rm{windows}}} {{{\rm{G}}_{\rm{i}}}} $$</div>
-
-where *G<sub>i</sub>* is the glare constant at the reference point due to the *i<sup>th</sup>* window
-
-Time-Step Daylighting Calculation
----------------------------------
-
-### Overview
-
-A daylighting calculation is performed each time step that the sun is up for each zone that has one or two daylighting reference points specified. The exterior horizontal illuminance from the sun and sky is determined from solar irradiance data from the weather file. The interior illuminance at each reference point is found for each window by interpolating the daylight illuminance factors for the current sun position, then, for sky-related interior illuminance, multiplying by the exterior horizontal illuminance from the appropriate sky types that time step, and, for sun-related interior illuminance, multiplying by the exterior horizontal solar illuminance that time step. By summation, the net illuminance and glare due to all of the windows in a zone are found. If glare control has been specified window shading (by movable shading devices or switchable glazing) is deployed to reduce glare. Finally the illuminance at each reference point for the final window and shade configuration is used by the lighting control system simulation to determine the electric lighting power required to meet the illuminance setpoint at each reference point.
-
-Table 27.  Variables in Time-Step Calculations
-
-<table class="table table-striped">
-<tr>
-<th>Mathematical variable</th>
-<th>Description</th>
-<th>Units</th>
-<th>FORTRAN variable</th>
-</tr>
-<tr>
-<td>S<sub>norm,dir</sub></td>
-<td>Direct normal solar irradiance</td>
-<td>W/m<sup>2</sup></td>
-<td>BeamSolarRad</td>
-</tr>
-<tr>
-<td>S<sub>h,dif</sub></td>
-<td>Exterior diffuse horizontal solar irradiance</td>
-<td>W/m<sup>2</sup></td>
-<td>SDIFH, DifSolarRad</td>
-</tr>
-<tr>
-<td>S<sub>h,dir</sub></td>
-<td>Exterior direct horizontal solar irradiance</td>
-<td>W/m<sup>2</sup></td>
-<td>SDIRH</td>
-</tr>
-<tr>
-<td>Z</td>
-<td>Solar zenith angle</td>
-<td>radians</td>
-<td>Zeta</td>
-</tr>
-<tr>
-<td>m</td>
-<td>Relative optical air mass</td>
-<td>-</td>
-<td>AirMass</td>
-</tr>
-<tr>
-<td>Δ</td>
-<td>Sky brightness</td>
-<td>-</td>
-<td>SkyBrightness</td>
-</tr>
-<tr>
-<td>ε</td>
-<td>Sky clearness</td>
-<td>-</td>
-<td>SkyClearness</td>
-</tr>
-<tr>
-<td>k, k’</td>
-<td>Sky type index</td>
-<td>-</td>
-<td>ISky</td>
-</tr>
-<tr>
-<td>s<sub>k,k’</sub></td>
-<td>Interpolation factor for skies k and k’</td>
-<td>-</td>
-<td>SkyWeight</td>
-</tr>
-<tr>
-<td>ψ<sub>k,k’</sub></td>
-<td>Sky luminance distribution formed from linear interpolation of skies k and k’</td>
-<td>cd/m<sup>2</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>f<sub>k</sub></td>
-<td>Fraction of sky that is type k</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>E<sub>h,k</sub></td>
-<td>Horizontal illuminance from sky type k</td>
-<td>cd/m<sup>2</sup></td>
-<td>HorIllSky</td>
-</tr>
-<tr>
-<td>E<sub>h,sky</sub></td>
-<td>Exterior horizontal illuminance from sky</td>
-<td>lux</td>
-<td>HISKF</td>
-</tr>
-<tr>
-<td>E<sub>h,sun</sub></td>
-<td>Exterior horizontal illuminance from sun</td>
-<td>lux</td>
-<td>HISUNF</td>
-</tr>
-<tr>
-<td>η<sub>dif</sub>, η<sub>dir</sub></td>
-<td>Luminous efficacy of diffuse and direct solar radiation</td>
-<td>lm/W</td>
-<td>DiffLumEff, DirLumEff</td>
-</tr>
-<tr>
-<td>I<sub>win</sub></td>
-<td>Interior illuminance from a window</td>
-<td>lux</td>
-<td>DaylIllum</td>
-</tr>
-<tr>
-<td>S<sub>win</sub></td>
-<td>Window luminance</td>
-<td>cd/m<sup>2</sup></td>
-<td>SourceLumFromWinAtRefPt</td>
-</tr>
-<tr>
-<td>B<sub>win</sub></td>
-<td>Window background luminance</td>
-<td>cd/m<sup>2</sup></td>
-<td>BACLUM</td>
-</tr>
-<tr>
-<td>d<sub>sun</sub>, d<sub>sky,k</sub></td>
-<td>Interior illuminance factor for sun, for sky of type k</td>
-<td>-</td>
-<td>DaylIllFacSun, DFSUHR, DaylIllFacSky, DFSUHR</td>
-</tr>
-<tr>
-<td>w<sub>sun</sub>, w<sub>sky,k</sub></td>
-<td>Window luminance factor for sun, for sky of type k</td>
-<td>-</td>
-<td>DaylSourceFacSun, SFSUHR, DaylSourceFacSky, SFSKHR</td>
-</tr>
-<tr>
-<td>b<sub>sun</sub>, b<sub>sky,k</sub></td>
-<td>Window background luminance factor for sun, for sky of type k</td>
-<td>-</td>
-<td>DaylBackFacSun, BFSUHR, DaylBackFacSky, BFSKHR</td>
-</tr>
-<tr>
-<td>w<sub>j</sub></td>
-<td>Weighting factor for time step interpolation</td>
-<td>-</td>
-<td>WeightNow</td>
-</tr>
-<tr>
-<td>i<sub>L</sub></td>
-<td>Reference point index</td>
-<td>-</td>
-<td>IL</td>
-</tr>
-<tr>
-<td>i<sub>S</sub></td>
-<td>Window shade index</td>
-<td>-</td>
-<td>IS</td>
-</tr>
-<tr>
-<td>I<sub>tot</sub></td>
-<td>Total daylight illuminance at reference point</td>
-<td>lux</td>
-<td>DaylIllum</td>
-</tr>
-<tr>
-<td>B<sub>tot</sub>, B</td>
-<td>Total window background luminance</td>
-<td>cd/m<sup>2</sup></td>
-<td>BLUM</td>
-</tr>
-<tr>
-<td>I<sub>set</sub></td>
-<td>Illuminance setpoint</td>
-<td>lux</td>
-<td>ZoneDaylight%IllumSetPoint</td>
-</tr>
-<tr>
-<td>f<sub>L</sub></td>
-<td>Fractional electric lighting output</td>
-<td>-</td>
-<td>FL</td>
-</tr>
-<tr>
-<td>f<sub>P</sub></td>
-<td>Fractional electric lighting input power</td>
-<td>-</td>
-<td>FP</td>
-</tr>
-<tr>
-<td>N<sub>L</sub></td>
-<td>Number of steps in a stepped control system</td>
-<td>-</td>
-<td>LightControlSteps</td>
-</tr>
-<tr>
-<td>M<sub>P</sub></td>
-<td>Lighting power multiplier</td>
-<td>-</td>
-<td>ZonePowerReductionFactor</td>
-</tr>
-
-</table>
-
-
-
-### Time-Step Sky Luminance
-
-The sky luminance distribution, *ψ*, for a particular time step is expressed as a linear interpolation of two of the four standard skies — *ψ<sub>cs</sub>*, *ψ<sub>ts</sub>* , *ψ<sub>is</sub>* and *ψ<sub>os</sub>* — described above under “Sky Luminance Distributions.� The two sky types that are interpolated depend on the value of the sky clearness. The interpolation factors are a function of sky clearness and sky brightness (Perez et al., 1990). Sky clearness is given by
-
-<div>$$\varepsilon  = \frac{{\frac{{{S_{h,dif}} + {S_{norm,dir}}}}{{{S_{h,dif}}}} + \kappa {Z^3}}}{{1 + \kappa {Z^3}}}$$</div>
-
-where *S<sub>h,dif</sub>* is the diffuse horizontal solar irradiance, *S<sub>norm,dir</sub>*is the direct normal solar irradiance, *Z* is the solar zenith angle and *κ* is a constant equal to 1.041 for *Z* in radians.
-
-Sky brightness is given by
-
-<div>$$\Delta  = {S_{h,dif}}m/S_{norm,dir}^{ext}$$</div>
-
-where *m* is the relative optical air mass and <span>\(S_{norm,dir}^{ext}\)</span>is the extraterrestrial direct normal solar irradiance.
-
-If *ε* ≤ 1.2
-
-<div>$${\psi_{is,os}} = {s_{is,os}}{\psi_{is}} + (1 - {s_{is,os}}){\psi_{os}}$$</div>
-
-where *ψ<sub>is</sub>* is the intermediate sky luminance distribution, *ψ<sub>os</sub>* is the overcast sky luminance distribution, and
-
-<div>$${s_{is,os}} = \min \{ 1,\max [0,(\varepsilon  - 1)/0.2,(\Delta  - 0.05)/0.4]\} $$</div>
-
-If 1.2&lt;*ε* ≤ 3
-
-<div>$${\psi_{ts,is}} = {s_{ts,is}}{\psi_{ts}} + (1 - {s_{ts,is}}){\psi_{is}}$$</div>
-
-where *ψ<sub>ts</sub>* is the clear turbid sky luminance distribution and
-
-<div>$${s_{ts,is}} = (\varepsilon  - 1.2)/1.8$$</div>
-
-If *ε* &gt; 3
-
-<div>$${\psi_{cs,ts}} = {s_{cs,ts}}{\psi_{cs}} + (1 - {s_{cs,ts}}){\psi_{ts}}$$</div>
-
-where *ψ<sub>cs</sub>* is the clear sky luminance distribution and
-
-<div>$${s_{cs,ts}} = \min [1,(\varepsilon  - 3)/3]$$</div>
-
-### Interior Illuminance
-
-For each time step the interior illuminance, *I<sub>win</sub>*, from a window is calculated as follows by multiplying daylight factors and exterior illuminance.
-
-First, the sun- and sky-related daylight illuminance factors for the time step are determined by interpolation of the hourly factors:
-
-<div>$${\bar d_{sun}}({i_L},{i_S}) = {w_j}{d_{sun}}({i_L},{i_S},{i_h}) + (1 - {w_j}){d_{sun}}({i_L},{i_S},{i_h} + 1)$$</div>
-
-<div>$${\bar d_{sky,k}}({i_L},{i_S}) = {w_j}{d_{sky,k}}({i_L},{i_S},{i_h}) + (1 - {w_j}){d_{sky,k}}({i_L},{i_S},{i_h} + 1)$$</div>
-
-where *i<sub>L</sub>* is the reference point index (1 or 2), *i<sub>S</sub>* is the window shade index (1 for unshaded window, 2 for shaded window),* i<sub>h</sub>* is the hour number, and *k* is the sky type index. For the* j*th time step in an hour, the time-step interpolation weight is given by
-
-<div>$${w_j} = 1 - \min [1,j/{N_t}]$$</div>
-
-where *N<sub>t</sub>* is the number of  time steps per hour.
-
-The interior illuminance from a window is calculated as
-
-<div>$${I_{win}}({i_L},{i_S}) = {\bar d_{sun}}{E_{h,sun}} + [{\bar d_{sky,k}}({i_L},{i_S}){f_k} + {\bar d_{sky,k'}}({i_L},{i_S}){f_{k'}}]{E_{h,sky}}$$</div>
-
-where *E<sub>h,sun</sub>* and *E<sub>h,sky</sub>* are the exterior horizontal illuminance from the sun and sky, respectively, and *f<sub>k</sub>* and *f<sub>k’</sub>* are the fraction of the exterior horizontal illuminance from the sky that is due to sky type *k* and *k’*, respectively.
-
-The horizontal illuminance from sun and sky are given by
-
-<div>$$
-  \begin{array}{rl}
-    E_{h,sun} &= \eta_{dir} S_{norm,dir} \cos Z \\
-    E_{h,sky} &= \eta_{dif} S_{h,dif}
-  \end{array}
-$$</div>
-
-where *Z* is the solar zenith angle,  *η<sub>dif</sub>* is the luminous efficacy (in lumens/Watt) of diffuse solar radiation from the sky and *η<sub>dir</sub>* is the luminous efficacy of direct radiation from the sun. The efficacies are calculated from direct and global solar irradiance using a method described in (Perez et al, 1990).
-
-The fractions *f<sub>k</sub>* and *f<sub>k’</sub>* are given by
-
-<div>$$
-  \begin{array}{rl}
-    f_k    &= \frac{ s_{k,k'} E_{h,k} } { s_{k,k'} E_{h,k} + (1 - s_{k,k'})E_{h,k'}} \\
-    f_{k'} &= \frac{ (1 - s_{k,k'} ) E_{h,k'} } { s_{k,k'} E_{h,k} + (1 - s_{k,k'} ) E_{h,k'}}
-  \end{array}
-$$</div>
-
-where *E<sub>h,k</sub>* and *E<sub>h,k’</sub>* are the horizontal illuminances from skies *k* and *k’*, respectively (see “Exterior Horizontal Luminance,� above), and *s<sub>k,k’</sub>* is the interpolation factor for skies *k*and *k’*(see “Time-Step Sky Luminance,� above).  For example, if  *ε* &gt; 3, *k*= *cs* (clear sky), *k’* = *ts* (clear turbid sky) and
-
- <span>\(s_{k,k'} = s_{cs,ts} = \min [1,(\varepsilon  - 3)/3]\)</span>
-
-Similarly, the window source luminance, *S<sub>win</sub>*, and window background luminance, *B<sub>win</sub>*, for a window are calculated from
-
-<div>$${S_{win}}({i_L},{i_S}) = {\bar w_{sun}}{E_{h,sun}} + [{\bar w_{sky,k}}({i_L},{i_S}){f_k} + {\bar w_{sky,k'}}({i_L},{i_S}){f_{k'}}]{E_{h,sky}}$$</div>
-
-<div>$${B_{win}}({i_L},{i_S}) = {\bar b_{sun}}{E_{h,sun}} + [{\bar b_{sky,k}}({i_L},{i_S}){f_k} + {\bar b_{sky,k'}}({i_L},{i_S}){f_{k'}}]{E_{h,sky}}$$</div>
-
-The total illuminance at a reference point from all of the exterior windows in a zone is
-
-<div>$${I_{tot}}({i_L}) = \sum\limits_{\scriptstyle{\rm{windows}}\atop\scriptstyle{\rm{in zone}}} {{I_{win}}({i_s},{i_L})} $$</div>
-
-where* i<sub>S</sub>* = 1 if the window is unshaded and *i<sub>S</sub>* = 2 if the window is shaded that time step. (Before the illuminance calculation is done the window shading control will have been simulated to determine whether or not the window is shaded.)
-
-Similarly, the total background luminance is calculated:
-
-<div>$${B_{tot}}({i_L}) = \sum\limits_{\scriptstyle{\rm{windows}}\atop\scriptstyle{\rm{in zone}}} {{B_{win}}({i_s},{i_L})} $$</div>
-
-### Glare Index
-
-The net glare index at each reference point is calculated as
-
-<div>$${G_I}({i_L}) = 10{\log_{10}}\sum\limits_{\scriptstyle{\rm{windows}}\atop\scriptstyle{\rm{in zone}}} {\frac{{{S_{win}}{{({i_L},{i_S})}^{1.6}}\Omega {{({i_L})}^{0.8}}}}{{B({i_L}) + 0.07\omega {{({i_L})}^{0.5}}{S_{win}}({i_L},{i_S})}}} $$</div>
-
-where
-
-<div>$$B\left( {{i_L}} \right) = max\left( {{B_{win}}\left( {{i_L}} \right),{\rho_b}{I_{set}}\left( {{i_L}} \right)} \right)$$</div>
-
-In the last relationship, the background luminance is approximated as the larger of the background luminance from daylight and the average background luminance that would be produced by the electric lighting at full power if the illuminance on the room surfaces were equal to the setpoint illuminance. In a more detailed calculation, where the luminance of each room surface is separately determined, *B(i<sub>L</sub>)* would be better approximated as an area-weighted luminance of the surfaces surrounding a window, taking into account the luminance contribution from the electric lights.
-
-#### Glare Control Logic
-
-If glare control has been specified and the glare index at either reference point exceeds a user-specified maximum value, *G<sub>I,max</sub>*, then the windows in the zone are shaded one by one in attempt to bring the glare at both points below *G<sub>I,max</sub>*. (Each time a window is shaded the glare and illuminance at each reference point is recalculated.) The following logic is used:
-
-5)   If there is only one reference point, shade a window if it is unshaded and shading it decreases the glare, even if it does not decrease the glare below *G<sub>I,max</sub>*. Note that if a window  has already been shaded, say to control solar gain, it will be left in the shaded state.
-
-6)   If there are two reference points, then:
-
-  * If glare is too high at both points, shade the window if it decreases glare at both points.
-
-  * If glare is too high only at the first point, shade the window if the glare at the first point decreases, and the glare at the second point stays below *G<sub>I,max</sub>*.
-
-  * If glare is too high only at the second point, shade the window if the glare at the second point decreases, and the glare at the first point stays below *G<sub>I,max</sub>*.
-
-7)   Shades are closed in the order of window input until glare at both points is below *G<sub>I,max</sub>*, or until there are no more windows left to shade.
-
-### Lighting Control System Simulation
-
-Once the final daylight illuminance value at each reference point has been determined, the electric lighting control is simulated. The fractional electric lighting output, *f<sub>L</sub>*, required to meet the setpoint at reference point *i<sub>L</sub>* is given by
-
-<div>$${f_L}({i_L}) = {\rm{max}}\left[ {0,\frac{{{I_{set}}({i_L}) - {I_{tot}}({i_L})}}{{{I_{set}}({i_L})}}} \right]$$</div>
-
-Here, *I<sub>set</sub>* is the illuminance setpoint and *I<sub>tot</sub>* is the daylight illuminance at the reference point. This relationship assumes that the electric lights at full power produce an illuminance equal to *I<sub>set</sub>* at the reference point.
-
-The fractional electric lighting input power, *f<sub>P</sub>*, corresponding to *f<sub>L</sub>* is then calculated. The relationship between *f<sub>P</sub>* and *f<sub>L</sub>* depends on the lighting control type.
-
-#### Continuous Dimming Control
-
-For a continuously-dimmable control system, it is assumed that *f<sub>P</sub>* is constant and equal to *f<sub>P,min</sub>*for *f<sub>L</sub>&lt;f<sub>L,min</sub>* and that f<sub>P</sub> increases linearly from *f<sub>P,min</sub>* to 1.0 as *f<sub>L</sub>* increases from *f<sub>L,min</sub>* to 1.0 (Figure 60). This gives
-
-<div>$${f_P} = \left\{ \begin{array}{l}{f_{P,\min }} & {\rm{for }}{f_L} &lt; {f_{L,\min }}\\\frac{{{f_L} + (1 - {f_L}){f_{P,\min }} - {f_{L,\min }}}}{{1 - {f_{L,\min }}}}\end{array} \right.{\rm{   for }}{f_{L,\min }} \le {f_L} \le 1$$</div>
-
-![](media/image823.png)
-
-Figure 60.  Control action for a continuous dimming system.
-
-#### Continuous/Off Dimming Control
-
-A “continuous/off� dimming system has the same behavior as a continuous dimming system except that the lights switch off for *f<sub>L</sub> &lt; f<sub>L,min</sub>* rather than staying at *f<sub>P,min</sub>*.
-
-#### Stepped Control
-
-For a stepped control system, *f<sub>P</sub>* takes on discrete values depending on the range of *f<sub>L</sub>*and the number of steps, *N<sub>L</sub>*<sub> </sub> (Figure 61). This gives
-
-<div>$${f_P} = \left\{ \begin{array}{l}0, & {\rm{if }}{f_L} = 0\\\frac{{{\mathop{\rm int}} ({N_L}{f_L}) + 1}}{{{N_L}}}, & {\rm{for }}0 &lt; {f_L} &lt; 1\\1, & {\rm{if }}{f_L} = 1\end{array} \right.$$</div>
-
-If a lighting control probability,* p<sub>L</sub>*, is specified,* f<sub>P</sub>* is set one level higher a fraction of the time equal to *1-p<sub>L</sub>*. Specifically, if* f<sub>P</sub>* &lt;1,* f<sub>P</sub>*à* f<sub>P</sub>*+ 1/*N<sub>L</sub>* if a random number between 0 and 1 exceeds *p<sub>L</sub>*. This can be used to simulate the uncertainty associated with manual switching of lights.
-
-![](media/image825.png)
-
-Figure 61.  Stepped lighting control with three steps.
-
-#### Lighting Power Reduction
-
-Using the value of *f<sub>P</sub>*at each reference point and the fraction *f<sub>Z</sub>* of the zone controlled by the reference point, the net lighting power multiplier, *M<sub>P</sub>*, for the entire zone is calculated; this value multiplies the lighting power output without daylighting.
-
-<div>$${M_P} = \sum\limits_{{i_L} = 1}^2 {{f_P}({i_L})} {f_Z}({i_L}) + \left( {1 - \sum\limits_{{i_L} = 1}^2 {} {f_Z}({i_L})} \right)$$</div>
-
-In this expression, the term to the right in the parentheses corresponds to the fraction of the zone not controlled by either reference point. For this fraction the electric lighting is unaffected and the power multiplier is 1.0.
-
-### References
-
-CIE Technical Committee 4.2. 1973. Standardization of the Luminance Distribution on Clear Skies. CIE Pub. No. 22, Commission Internationale d’Eclairage, Paris.
-
-Hopkinson, R.G., J. Longmore and P. Petherbridge. 1954. An Empirical Formula for the Computation of the Indirect Component of Daylight Factors. Trans. Illum. Eng. Soc. (London) 19, 201.
-
-Hopkinson, R.G., P. Petherbridge and J. Longmore. 1966. Daylighting. Heinnemann, London, p. 322.
-
-Hopkinson, R.G. 1970. Glare from Windows. Construction Research and Development Journal 2, 98.
-
-Hopkinson, R.G. 1972. Glare from Daylighting in Buildings. Applied Ergonomics 3, 206.
-
-Kittler, R. 1965. Standardization of Outdoor Conditions for the Calculation of the Daylight Factor with Clear Skies. Proc. CIE Inter-Session Meeting on Sunlight, Newcastle-Upon-Tyne.
-
-Lynes, J.A. 1968. Principles of Natural Lighting. Applied Science Publishers, Ltd., London, p. 129.
-
-Matsuura, K. 1987. Luminance Distributions of Various Reference Skies. CIE Technical Report of TC 3-09.
-
-Moon, P. and D. Spencer. 1942. Illumination from a Nonuniform Sky. Illuminating Engineering 37, 707-726.
-
-
-
-------------------------------------------------------------------------
-
-[[1]](#_ftnref1) For beam incident on an exterior window we have the following: For transparent glass with no shade or blind there is only beam-to-beam transmission. For diffusing glass, or if a window shade is in place, there is only beam-to-diffuse transmission. If a window blind is in place there is beam-to-diffuse transmission, and, depending on slat angle, solar profile angle, etc., there can also be beam-to-beam transmission.
-
-[[2]](#_ftnref2) See “Beam Solar Reflection from Window Reveal Surfaces.�
-
-[[3]](#_ftnref3) If Solar Distribution = FullInteriorAndExterior in the Building object, the program calculates where beam solar from exterior windows falls inside the zone. Otherwise, all beam solar is assumed to fall on the floor.
-
-[[4]](#_ftnref4) For the purposes of the surface heat balance calculation, any beam solar radiation absorbed by a surface is assumed to be uniformly distributed over the surface even though in reality it is likely to be concentrated in one or more discrete patches on the surface.
-
-[[5]](#_ftnref5) *TBm<sub>i</sub>*<sub></sub>is zero if the window has diffusing glass or a shade. *TBm<sub>i</sub>* can be &gt; 0 if a blind is present and the slat angle, solar profile angle, etc., are such that some beam passes between the slats.
-
-[[6]](#_ftnref6) A different method from that described here is used for calculating reflections from daylighting shelves (see “Daylighting Shelves�).
-
-[[7]](#_ftnref7) The ground surface is assumed to be diffusely reflecting so there is no specular reflection from the ground. The program could be improved by adding a ground surface specular component, which could be important for snow-cover conditions.
-
-[[8]](#_ftnref8) The sun positions for which the daylight factors are calculated are the same as those for which the solar shadowing calculations are done.
-
-
-
-Perez, R., P. Ineichen, R. Seals, J. Michalsky and R. Stewart. 1990. Modeling Daylight Availability and Irradiance Components from Direct and Global Irradiance. Solar Energy 44, 271-289.
-
-Petherbridge, P. and J. Longmore. 1954. Solid Angles Applied to Visual Comfort Problems. Light and Lighting 47,173.
-
-Winkelmann, F.C.  1983. Daylighting Calculation in DOE-2*.* Lawrence Berkeley Laboratory report no. LBL-11353, January 1983.
-
-Winkelmann, F.C. and S. Selkowitz. 1985. Daylighting Simulation in the DOE-2 Building Energy Analysis Program*.* Energy and Buildings 8, 271-286.
-
-DElight Daylighting Calculations
---------------------------------
-
-The Daylighting:DELight series of input objects provide an alternative daylighting model.  The DElight method of analyzing daylighting applies to both simple apertures (i.e., windows and skylights) and complex fenestration systems that include geometrically complicated shading (e.g., roof monitors) and/or optically complicated glazings (e.g., prismatic or holographic glass).  The DElight daylighting calculation methods are derived from the daylighting calculations in DOE-2.1E (as are the models accessed with Daylighting:Controls input object), and Superlite, with several key modifications.  The engineering documentation included here focuses on the details of these differences from methods documented elsewhere.  For the details of the heritage calculations, refer to the section in this documentation entitled “Daylighting Calculations� and to [Winkelmann, 1983], [Winkelmann and Selkowitz, 1985], and  [Modest, 1982].
-
-For each point in time, DElight calculates the interior daylighting illuminance at user specified reference points and then determines how much the electric lighting can be reduced while still achieving a combined daylighting and electric lighting illuminance target.  The daylight illuminance level in a zone depends on many factors, including exterior light sources; location, size, and visible light transmittance of simple and complex fenestration systems; reflectance of interior surfaces; and location of reference points. The subsequent reduction of electric lighting depends on daylight illuminance level, design illuminance setpoint, fraction of zone controlled by reference point, and type of lighting control.
-
-The DElight daylighting calculation has three main steps:
-
-1.    *Daylight Factor Calculation:*  Daylight factors, which are ratios of interior illuminance to exterior horizontal illuminance, are pre-calculated and stored for later use. The user spcifies the coordinates of one or more reference points in each daylit zone. DElight first calculates the contribution of light transmitted through all simple and complex fenestration systems in the zone to the illuminance at each reference point, and to the luminance at subdivided nodal patches of interior surfaces, for a given exterior luminous environment (including sky, sun, and exterior reflecting surfaces).  The effect of inter-reflection of this initial light between interior reflecting surfaces is then calculated, resulting in a final total illuminance at each reference point.  This total illuminace is then divided by the exterior horizontal illuminance for the given exterior environment to give a daylight factor.  Daylight factors are calculated for each reference point, for a set of sun positions and sky conditions that are representative of the building location.
-
-2.    *Time-Step Interior Daylighting Calculation*:  A daylighting calculation is performed for each heat-balance time step when the sun is up. In this calculation the illuminance at the reference points in each zone is found by interpolating the stored daylight factors using the current time step sun position and sky condition, then multiplying by the exterior horizontal illuminance.
-
-3.    *Electric Lighting Control Calculation*:  The electric lighting control system is simulated to determine the proportion of lighting energy needed to make up the difference between the daylighting illuminance level at the given time step, and the design illuminance level. Finally, the zone lighting electric reduction factor is passed to the thermal calculation, which uses this factor to reduce the heat gain from lights.
-
-### DElight Daylight Factor Calculation Differences from EnergyPlus Detailed Methods
-
-* *Initial Interior Illuminance/Luminance Calculation:*  DElight calculates the total initial contribution of light transmitted through all simple fenestration systems (i.e., windows and skylights) in the zone to the illuminance at each reference point, and to the luminance at each gridded nodal patch of interior surfaces.  This differs from the models behind the “Daylighting:Controls� object (henceforth referred to as “EnergyPlus Detailed�) in two ways. The first is that EnergyPlus Detailed calculates initial illuminace values at reference points for each pair of reference point and aperture (window/skylight) in the zone, whereas DElight calculates the total contribution from all apertures to each reference point.  The second difference from EnergyPlus Detailed is that the initial luminance of interior surface nodal patches is calculated to support the inter-reflection calculation described below.  This calculation uses the same formula as EnergyPlus Detailed modified for arbitrarily oriented surfaces (i.e., non-horizontal), and to calculate luminance rather than illuminance.  Note however, DElight does not account for interior surface obstructions (e.g., partitions) in this initial interior illuminance/luminance distribution.  The EnergyPlus Detailed method does account for interior surface obstruction of initial illuminance distribution on reference points.
-
-* *Reference Points:*  DElight allows up to 100 reference points to be arbitrarily positioned with a daylighting zone.  At this time all reference points are assumed to be oriented on a horizontal virtual surface “facing� toward the zenith and “seeing� the hemisphere above the horizontal plane.
-
-* *Complex Fenestration System Calculation:*  DElight calculates the contribution to the initial interior illuminance at each reference point, and to the luminance at each gridded nodal patch of interior surfaces, of the light transmitted by complex fenestration systems (CFS).  The analysis of a CFS within DElight is based on the characterization of the system using bi-directional transmittance distribution functions (BTDF), which must be either pre-calculated (e.g., using ray-tracing techniques) or pre-measured, prior to analysis by DElight.  A BTDF is a set of data for a given CFS, which gives the ratios of incident to transmitted light for a range of incoming and outgoing directions.  As illustrated in Figure 62, a BTDF can be thought of as collapsing a CFS to a “black box� that is represented geometrically as a flat two-dimensional light-transmitting surface that will be treated as an aperture surface in the daylit zone description. For each incoming direction across the exterior hemisphere of the CFS, varying portions of that light are transmitted at multiple outgoing directions across the interior hemisphere of the CFS.  The two-dimensional CFS “surface� and directional hemispheres are “abstract� in that they may not literally correspond to actual CFS component geometric details.
-
-![](media/image827.png)
-
-Figure 62.  Bi-Directional Transmittance Data.
-
-The pre-calculated or pre-measured BTDF for a CFS is independent of its final position and orientation within a building.  Once a specific instance of a CFS aperture has been positioned within a building, the incident light from all exterior sources across the CFS exterior hemisphere can be integrated over all incident directions for each relevant transmitted direction to determine the light transmitted by the CFS surface in that direction. The light transmitted by the CFS aperture is then distributed to surfaces in the zone according to its non-uniform directionality.  The algorithms for this BTDF treatment of CFS in DElight are still under development, and are subject to change in the future.
-
-* *Inter-reflected Interior Illuminance/Luminance Calculation:*  The effect of inter-reflection of the initial interior illuminance/luminance between interior reflecting surfaces is calculated using a radiosity method derived from Superlite [Modest, 1982].  This method subdivides each reflecting surface in the zone into nodal patches and uses view factors between all nodal patch pairs in an iterative calculation of the total contribution of reflected light within the zone.  This method replaces the split-flux method used in EnergyPlus Detailed, resulting in a more accurate calculation of the varied distribution of inter-reflected light throughout the zone.  The ability to input up to 100 reference points supports a more complete assessment of this distribution.  Also, the radiosity method explicitly accounts for interior obstructions between pairs of nodal patches.  The split-flux method used in the EnergyPlus Detailed approach only implicitly accounts for interior surfaces by including their reflectance and surface area in the zone average surface reflectance calculations.
-
-### DElight Time-Step Interior Daylighting Calculation Differences from EnergyPlus Detailed Methods
-
-* *Interior Illuminance Calculation:*  As discussed above, DElight only calculates daylight factors for the total contribution from all windows/skylights and CFS to each defined reference point.  Thus DElight does not support dynamic control of fenestration shading during the subsequent time-step calculations, as does EnergyPlus Detailed.
-
-* *Visual Quality:*  DElight does not currently calculate a measure of visual quality such as glare due to daylighting.  DElight does calculate luminance on nodal patches of all interior, reflecting surfaces.  A variety of visual quality metrics could be calculated from these data in future implementations.
-
-* *Electric Lighting Control Calculation:*  Up to 100 reference points can be defined within a DElight daylighting zone.  One or more of these reference points must be included in the control of the electric lighting system in the zone.  Each reference point input includes the fraction of the zone controlled by that point.  Values of 0.0 are valid, which allows the definition of reference points for which interior illuminance levels are calculated, but which do not control the electric lighting.  Any non-zero fraction is thus the equivalent of a relative weighting given to that reference point’s influence on the overall electric lighting control.  The sum of all fractions for defined reference points must less than or equal to 1.0 for this relative weighting to make physical sense.  If the sum is less than 1.0, the remaining fraction is assumed to have no lighting control.
-
-### References
-
-Modest, M. 1982. A General Model for the Calculation of Daylighting in Interior Spaces, Energy and Buildings 5, 66-79, and Lawrence Berkeley Laboratory report no. LBL-12599A.
-
-Winkelmann, F.C. 1983. Daylighting Calculation in DOE-2*.* Lawrence Berkeley Laboratory report no. LBL-11353, January 1983.
-
-Winkelmann, F.C. and S. Selkowitz. 1985. Daylighting Simulation in the DOE-2 Building Energy Analysis Program*.* Energy and Buildings 8, 271-286.
-
-
-
-Complex Fenestration Daylighting Calculations
----------------------------------------------
-
-The complex fenestration systems (CFS) daylighting calculation method results in the same Daylighting Factor style output as the it is described in Daylighting Calculations chapter.
-
-Transmitted solar radiation reaches the daylighting sensor in two different ways. The first is an indirect path when solar radiation is reflected from surfaces and uniformly distributed into the space. The second is a direct path when the sensor is directly illuminated by the fenestration system.
-
-For the indirect path, the method performs a one-bounce calculation to determine the diffuse illumination for the zone. For a certain sky condition, including the sun position, the method will calculate which surfaces are illuminated from each of the BSDF directions, taking into account the reflectance of the surfaces. This indirect illumination is calculated from both direct sunlight hitting a window with or without a shading device and diffuse illumination calculated from diffuse light coming into the zone from the sky or the ground. This transmitted light strikes the zone interior surfaces and creates a diffuse component. The CFS daylighting method determines the contribution of each sky patch to the illumination of the zone surfaces based on the BSDF transmittances and then luminance is calculated based on the surface reflection.
-
-For the direct path, the window is subdivided using existing subdivision procedures. From the center of each subdivided element, the angle is calculated to the reference point. The illuminance is calculated based on the BSDF data for the outgoing direction that corresponds to that angle and the incident illumination from sky, ground and sun.
-
-### Internal Average Reflected Illuminance From Window
-
-To calculate internal average reflected illumiance from the window it is necessary to calculate transmitted flux at the window.  Observing an infinitesimal window element, illuminance can originate from the sky or sun, and in both cases the ray can reach the window directly or after reflecting from the ground.  Based on this, the calculation of luminance at the window is divided into three parts:
-
-* Sky-related illuminance and luminous flux
-
-* Sun-related illuminance and luminous flux, excluding entering beam
-
-* Sun-related illuminance and luminous flux, due to entering beam
-
-where total illuminance will be calculated as a superposition of these three parts.
-
-For any case, illuminace at a window element can be calculated by using the following general approach:
-
-<div>$$dE{W_{at\_window}} = Lu{m_{el}}({\theta_{el}},{\phi_{el}}) \cdot cos({\beta_{el}}) \cdot \cos ({\phi_{el}}) \cdot d{\theta_{el}} \cdot d{\phi_{el}}$$</div>
-
-where <span>\(dE{W_{at\_window}}\)</span> is the illuminance at a window element, <span>\(Lu{m_{el}}({\theta_{el}},{\phi_{el}})\)</span> represents the function of horizontal luminance from the exterior element in the direction <span>\(({\theta_{el}},{\phi_{el}})\)</span>, <span>\({\beta_{el}}\)</span> represents the angle at which the ray hits the surface of the window and <span>\(({\theta_{el}},{\phi_{el}})\)</span> represents the exterior element azimuth and altitude relative to the window (see Figure 63).
-
-![](media/image834.png)
-
-Figure 63: Exterior Luminance Element
-
-This will produce luminous flux at the interior side of the window:
-
-<div>$$d\phi {W_{inside}} = dE{W_{at\_window}} \cdot \tau ({\beta_{el}}) \cdot dA$$</div>
-
-where <span>\(dE{W_{at\_window}}\)</span> is given by equation , <span>\(\tau ({\beta_{el}})\)</span> is the window transmittance at the incoming angle <span>\({\beta_{el}}\)</span> and <span>\(dA\)</span> is infinitesimal window element surface area.
-
-Integrating luminous flux given by equation over entire window area will give luminous flux on the interior side of the window.
-
-To calculate the interan average reflected illumiance from the window, a simillar approch will be used as described in the chapter “Internally-Reflected Component of Interior Daylight Illuminance�, which gives the flux balance equation:
-
-<div>$$A \cdot {E_r} \cdot (1 - \rho ) = {F_1}$$</div>
-
-where <span>\({F_1}\)</span>represents first reflected flux which in the case of non-CFS is calculated by using the split-flux method.  In the case of CFS, first the reflected flux can be calculated more precisely by using light patches area.  Since each CFS is described by a BSDF, it is possible to calculate the light patches for each outgoing direction (see Figure 64).
-
-![](media/image842.png)
-
-Figure 64: Complex Fenestration System Light Patches
-
-Considering the total flux passing through the window at the outgoing direction “k�, the first reflect flux (<span>\({F_{1,k}}\)</span>) can be calculated as:
-
-<div>$${F_{1,k}} = {\phi_k} \cdot \frac{{\sum\limits_{a = 1}^N {({A_{overlap,k,a}} \cdot {\rho_{vis,k,a}})} }}{{\sum\limits_{a = 1}^N {{A_{overlap,k,a}}} }}$$</div>
-
-where <span>\({\phi_k}\)</span> is the total flux entering the zone at the BSDF outgoing direction “k� and is calculated by integrating equation over the entire window area for a given outgoing direction “k�, N is the number of interior surfaces hit by the BSDF outgoing direction “k� (see Figure 64), <span>\({A_{overlap,k,a}}\)</span> is the surface (patch) area which the window from the BSDF outgoing direction “k� makes at surface “a� and <span>\({\rho_{vis,k,a}}\)</span> is the visible reflectance from surface “a�.
-
-Summing all the outgoing directions will result in total first reflected flux:
-
-<div>$${F_1} = \sum\limits_{k = 1}^{{N_{out}}} {{F_{1,k}}} $$</div>
-
-### Luminance from Exterior Elements
-
-The case of CFS luminance from exterior elements can be calculated by using BSDF incoming directions defined for a given CFS.  Applying equation for a certain incoming BSDF direction will give:
-
-<div>$$\Delta E{W_{el,i}} = Lum({\theta_i},{\psi_i}) \cdot \cos ({\beta_i}) \cdot \cos ({\phi_i}) \cdot \Delta {\theta_i} \cdot \Delta {\psi_i}$$</div>
-
-This equation can be translated in the BSDF coordinate system where instead of standard azimuth and altitude angles, the equation will be transformed into the BSDF coordinate system.  In that case, equation becomes:
-
-<div>$$\Delta E{W_{el,i}} = Lum({\theta_i},{\psi_i}) \cdot {\Lambda_i}$$</div>
-
-where <span>\({\Lambda_i}\)</span>represents the lambda value for the incoming direction “i�.
-
-### Luminous Flux and Direct Illuminance at Interior Side of the Window
-
-In the case of CFS it is of interest to calculate fluxes for each outgoing BSDF direction.  For a given amount of illuminance at an incoming direction “i�, flux into direction “o� will be calculated as:
-
-<div>$$\Delta \phi {W_{i,o}} = \Delta E{W_{el}} \cdot {T_{dir - dir,i,o}}$$</div>
-
-where <span>\({T_{dir - dir,i,o}}\)</span> is the direct-direct transmittance for given incoming and outgoing directions (“i� and “o�).
-
-![](media/image854.png)
-
-Figure 65: Complex Fenestration System Flux Transition - Single Incoming Direction to Single Outgoing Direction
-
-Total flux from the window at the outgoing direction “o� can be calculated by summing over all the incoming directions:
-
-<div>$$\Delta \phi {W_o} = \sum\limits_{i = 1}^{{N_{inc}}} {(\Delta E{W_{el,i}} \cdot {T_{dir - dir,i,o}})} $$</div>
-
-where <span>\({N_{inc}}\)</span> is the number of BSDF incident directions.
-
-Flux transmitted in the outgoing direction “o�, calculated by equation , can be used for any given distribution of an exterior luminous element.  Knowing the intensity of the luminous flux, the direct illuminance at a certain point is calculated as:
-
-<div>$$E{D_o} = \Delta {\Omega_{el}} \cdot \sin ({\phi_{el}}) \cdot \Delta \phi {W_o}$$</div>
-
-where <span>\(E{D_o}\)</span> is the direct illuminance at the BSDF outgoing direction “o�, <span>\(\Delta {\Omega_{el}}\)</span> is the spatial angle of the element viewed from a certain reference point and <span>\({\phi_{el}}\)</span> is the altitude of the window element viewed from the reference point.
-
-### Handling Exterior Obstructions
-
-Exterior obstructions are handled for two different cases.  The first case is to handle obstructions between the luminous element (sky/ground/sun) and the CFS window element. In that case, the direct illuminance at the window element is modified for the product of all the obstruction transmittances between the luminous and window elements, and equation is modified as:
-
-<div>$$\Delta E{W_{el,i}} = Lum({\theta_i},{\psi_i}) \cdot {\Lambda_i} \cdot \prod\limits_{p = 1}^{{N_o}} {{\tau_{obs,p}}} $$</div>
-
-where <span>\({N_o}\)</span>  is the number of exterior obstructions and <span>\({\tau_{obs,p}}\)</span> is the visible transmittance of obstruction “p�.
-
-The second case is to handle all obstructions between the luminous elements and the ground element.  The luminance from the ground element is calculated as:
-
-<div>$$Lu{m_{gnd}} = \frac{{{E_h}}}{\pi } \cdot {\rho_{gnd}}$$</div>
-
-where <span>\({E_h}\)</span> is the horizontal illuminance and <span>\({\rho_{gnd}}\)</span> is the ground reflectance.  Horizontal illuminance is obtained by the integration over sky/sun elements and it is of interest to examine if all elements are visible from a certain ground point.  The integration examines if the ray between the sky and the ground element is hitting an obstruction.  It does not take into account whether or not the obstruction is transparent, it simply counts the number of hits.  The sky obstruction multiplier is calculated as:
-
-<div>$$SOM = \frac{{NumberOfUnobstructedRays}}{{NumberOfRays}}$$</div>
-
-and in case the incoming element is from the ground, the illuminance at the window element (equation ) will be additionally modified from the sky obstruction multiplier:
-
-<div>$$\Delta E{W_{el,i}} = Lum({\theta_i},{\psi_i}) \cdot {\Lambda_i} \cdot SOM \cdot \prod\limits_{p = 1}^{{N_o}} {{\tau_{obs,p}}} $$</div>
-
-Daylighting Devices
--------------------
-
-Daylighting devices are used to improve daylighting in a zone.  Besides their contribution to illuminance, daylighting devices also have a thermal impact on the zone heat balance.  As a result the simulation of daylighting devices is tightly integrated into both the daylighting model and the zone heat balance.
-
-There are two types of daylighting device in EnergyPlus:  tubular daylighting devices and daylighting shelves.
-
-### Tubular Daylighting Devices
-
-The input object DaylightingDevice:Tubular provides a special model for fenestration components known as Tubular Daylighting Devices (TDDs), also known as tubular skylights or light pipes.  TDDs are constructed of three components: a dome, a pipe, and a diffuser.
-
-![TubeDevices](media/image869.png)
-
-Figure 66.  Tubular Daylighting Devices
-
-The dome is typically a hemisphere made of clear plastic.  It allows daylight into the pipe while keeping exterior weather out.  The pipe is assumed to be a smooth cylinder with a highly reflective inside surface.  The surface is usually either bare polished metal or a special reflective sheet adhered to the inside.  The pipe channels the daylight from the dome to the diffuser via multiple internal reflections.  The diffuser is typically a flat frosted plastic cover.  The diffuser evenly distributes the daylight to the zone.  The dome/diffuser area and pipe area must be approximately equal (within 2%) for running the simulation successfully.
-
-In EnergyPlus the TDD model includes three different, but related, phenomena:
-
-* Daylighting
-
-* Solar gains
-
-* Conductive/convective gains
-
-Solar gains and conductive/convective gains are simulated by the zone heat balance.  Daylighting is simulated independently.
-
-For both daylighting and heat balance simulations, the dome and diffuser are treated as special window surfaces to take advantage of many of the standard daylighting and heat transfer routines.  Together the dome and diffuser become "receiver" and "transmitter", i.e. radiation entering the dome ends up exiting the diffuser.
-
-![](media/image870.png)
-
-Figure 67.  Dome and Diffuser Surfaces
-
-The pipe is simulated by a separate code module.  While several different measures for characterizing TDD performance are in use (Zhang 2002; Harrison 1998), the total transmittance of the TDD is most compatible with the EnergyPlus daylighting and heat balance code.  Calculation of the transmittance of the pipe and the TDD for different types of radiation is fundamental to all phenomena covered by the model.
-
-#### Pipe Beam Transmittance
-
-The transmittance of beam radiation is derived from the integration of the transmittance of many discrete rays.  The transmittance of a discrete ray through a pipe is dependent on the reflectivity of the inside pipe surface, the aspect ratio of the pipe, the incident angle of the ray, and the point of entry into the pipe.
-
-![](media/image871.png)
-
-Figure 68.  Discrete Ray in a Pipe
-
-For an opaque surface, the reflectivity is:
-
-<div>$$\rho  = 1 - \alpha $$</div>
-
-where a = surface absorptivity.  Visible (i.e. daylighting) and solar absorptivities give visible and solar reflectivities, respectively.  Measured reflectivities for commercial TDDs range from 0.90 to 0.99.  Although the actual surface reflectivity is slightly dependent on the incident angle, the model assumes a constant reflectivity for all angles.
-
-The full analytical expression for the transmittance of a beam of light in a highly reflective pipe has been developed by Swift and Smith and verified by experiment (1994).  By integrating over all rays incident on the pipe entrance, they find the transmittance of a beam of collimated radiation to be:
-
-<div>$$\tau  = \frac{4}{\pi }\int_{s = 0}^1 {\frac{{{s^2}}}{{\sqrt {1 - {s^2}} }}} {\rho ^{INT\left[ {a\tan \theta /s} \right]}}\left( {1 - \left( {1 - \rho } \right)\left( {a\tan \theta /s - INT\left[ {a\tan \theta /s} \right]} \right)} \right)ds$$</div>
-
-where
-
-a = L/D, the aspect ratio of the TDD
-
-r = surface reflectivity
-
-q = incident angle
-
-s = entry point
-
-This integral does not have an analytical solution and must be calculated numerically.  It was found that a large number of points (100,000) were necessary to achieve an acceptable accuracy.  Since the integration is time consuming and the transmittance of the pipe must be utilized many times at every time step, values are calculated over a range of incident angles and stored in a table.  The tabulated values are interpolated to rapidly give the transmittance at any incident angle.  A polynomial fit was also considered but it was found that interpolation gave superior results.
-
-In the graph below, interpolated values from EnergyPlus are compared to the results of ray tracing simulations performed at the Florida Solar Energy Center for an incident angle of 30 degrees (McCluney 2003).
-
-
-
-![](media/image874.png)
-
-Figure 69.  Pipe Transmittance Comparison.
-
-During initialization of each unique TDD, the program integrates and tabulates values for the visible and solar transmittance of the pipe.  The results are subsequently used in the daylighting simulation and heat balance simulation respectively.
-
-The effect of bends in the pipe on beam transmittance is not included in this model.  Recent research (Zhang 2002) has suggested that a 30 degree bend has a 20% loss in transmitted light.  If the effect of bends must be simulated, it can be approximated by the user by appropriately decreasing the transmittance of the diffuser material.
-
-
-
-#### TDD Beam Transmittance
-
-The beam transmittance of the TDD takes into account the dome and diffuser transmittances in addition to the pipe transmittance.
-
-<div>$${\tau_{TDD}}(\theta ) = {\tau_{dome}}(\theta ){\tau_{pipe}}(\theta ){\tau_{diffuser}}$$</div>
-
-where
-
-t<sub>dome</sub>(q) = beam transmittance of the dome glazing at the incident angle
-
-t<sub>pipe</sub>(q) = beam transmittance of the pipe at the incident angle, as described above
-
-t<sub>diffuser</sub> = diffuse transmittance of the diffuser glazing
-
-The dome transmittance is calculated for a flat window.  The model does not take into account refraction due to the curvature of the dome surface.
-
-Diffuse transmittance is always assumed for the diffuser because multiple internal reflections in the pipe scatter the beam with a diffusing effect.  Although the light exiting the pipe is not isotropic, it can be approximated as diffuse.  The use of a frosted diffuser on the TDD, however, ensures that the light delivered to the zone is very close to isotropic diffuse.
-
-The calculation of TDD diffuse transmittance is considerably more complex and is handled differently in the daylighting simulation and the heat balance simulation.  The details are discussed in the following sections.
-
-#### Daylighting
-
-The daylighting simulation of the TDD treats the diffuser surface as a regular window illuminated from the outside by sun, sky, and ground.  However, the TDD model replaces the window glazing transmittance with the appropriate TDD transmittance and converts all transmitted light to diffuse.
-
-The illuminance due to the direct beam of the sun is found using the TDD beam transmittance t<sub>TDD</sub>(q) as described above.  The incident angle q is relative to the dome surface.
-
-The illuminance due to sky radiation and ground reflected radiation is calculated with the normal daylighting model integration over the sky and ground within the viewable hemisphere of the dome.  The transmittance of each sky or ground  element is also found using the TDD beam transmittance at the incident angle of the sky or ground element relative to the dome.
-
-Light from the diffuser is converted to diffuse inside the zone in the same way as an interior shade.
-
-#### Solar Gains
-
-Solar radiation incident on a window is calculated separately as sun, sky, and ground radiation.  A different transmittance must be applied for each type of radiation.
-
-For beam radiation the TDD beam transmittance t<sub>TDD</sub>(q) for the solar spectrum is used as described above.  For sky and ground radiation a diffuse transmittance for the TDD must be developed.
-
-The transmittance of diffuse radiation can be defined as the total transmitted flux divided by the total incident flux.
-
-<div>$${\tau_{diff}} = \frac{{\sum {{I_{trans}}} }}{{\sum {{I_{inc}}} }}$$</div>
-
-Swift and Smith (1994) suggest a weighted integral of the beam transmittance over the hemisphere for an arbitrary angular distribution:
-
-<div>$${\tau_{diff}} = \frac{{\int_{\theta  = 0}^{\pi /2} {\tau (\theta )P(\theta )} \sin \theta d\theta }}{{\int_{\theta  = 0}^{\pi /2} {P(\theta )} \sin \theta d\theta }}$$</div>
-
-where
-
-P(q) = angular distribution function
-
-For isotropic diffuse radiation P(q) is the cosine of the incident angle q.
-
-<div>$${\tau_{diff,iso}} = \frac{{\int_{\theta  = 0}^{\pi /2} {\tau (\theta )\cos \theta } \sin \theta d\theta }}{{\int_{\theta  = 0}^{\pi /2} {\cos \theta } \sin \theta d\theta }}$$</div>
-
-For a given pipe or TDD, t<sub>diff,iso</sub> is a constant.  The program calculates t<sub>diff,iso</sub> once during initialization using a numerical integration.
-
-The diffuse isotropic transmittance is useful, but not sufficient, for determining the transmittance of sky radiation.  As described in the *Sky Radiance Model* section, sky radiation has an anisotropic distribution modeled as the superposition of three simple distributions: a diffuse isotropic background, a circumsolar brightening near the sun, and a horizon brightening.  While the daylighting model is capable of calculating the luminance of any position in the sky, the solar code only calculates the ultimate irradiance on a surface.  For this reason it is not possible to integrate over an angular distribution function for sky radiance.  Instead the three sky distributions must be handled piecewise.
-
-<div>$${\tau_{diff,aniso}} = \frac{{\sum {{I_{trans,aniso}}} }}{{\sum {{I_{inc,aniso}}} }} = \frac{{{I_{trans,iso}} + {I_{trans,circumsolar}} + {I_{trans,horiz}}}}{{{I_{inc,iso}} + {I_{inc,circumsolar}} + {I_{inc,horiz}}}}$$</div>
-
-Substituting in the appropriate transmittances:
-
-<div>$${\tau_{diff,aniso}} = \frac{{{\tau_{diff,iso}}{I_{inc,iso}} + \tau (\theta ){I_{inc,circumsolar}} + {\tau_{diff,horiz}}{I_{inc,horiz}}}}{{{I_{inc,iso}} + {I_{inc,circumsolar}} + {I_{inc,horiz}}}}$$</div>
-
-where
-
-t<sub>diff,iso</sub> = diffuse isotropic transmittance
-
-t(q) = beam transmittance at incident angle q of sun
-
-t<sub>diff,horiz</sub> = diffuse transmittance of the horizon, derived below
-
-It is important to note that transmittances above are for the total TDD.  The transmittance of the dome and diffuser must be included to account for their angular dependences as well.
-
-The beam transmittance is used as an approximation for all circumsolar radiation.
-
-The diffuse horizon transmittance is found by integrating the beam transmittance over the arc of the horizon.
-
-<div>$${\tau_{diff,horiz}} = \frac{{\sum {{I_{trans,horiz}}} }}{{\sum {{I_{inc,horiz}}} }} = \frac{{\int_{\theta  =  - \pi /2}^{\pi /2} {\tau (\theta )\cos \theta d\theta } }}{{\int_{\theta  =  - \pi /2}^{\pi /2} {\cos \theta d\theta } }}$$</div>
-
-Since the radiance of the horizon is isotropic, and therefore constant across the entire horizon, the actual value of the radiance cancels out.  The result is a constant that is calculated once during initialization.
-
-Ground radiation is assumed to be isotropic diffuse.  The transmittance of ground radiation is the diffuse isotropic transmittance.
-
-<div>$${\tau_{diff,gnd}} = {\tau_{diff,iso}}$$</div>
-
-The solar flux transmitted by a TDD due to beam, sky, and ground radiation is calculated as normal for a window but uses the respective transmittances for the TDD.
-
-<div>$${q''_{TDD - trans,beam}} = \left( {{I_{sun}}\cos \theta } \right){f_{sunlit}}{\tau_{TDD}}(\theta )$$</div>
-
-<div>$${q''_{TDD - trans,sky}} = {I_{h,sky}}{f_{skymult}}{\tau_{TDD,diff,aniso}}$$</div>
-
-<div>$${q''_{TDD - trans,gnd}} = \left( {{I_{sun}}\cos \theta  + {I_{h,sky}}} \right){F_{sg}}{\tau_{TDD,diff,iso}}$$</div>
-
-where
-
-I<sub>sun</sub> = solar beam intensity of the sun
-
-I<sub>h,sky</sub> = total horizontal diffuse solar radiation due to the sky
-
-q = incident angle of the beam on the dome
-
-f<sub>sunlit</sub> = sunlit beam fraction of the dome area
-
-f<sub>skymult</sub> = anisotropic sky view multiplier (see AnisoSkyMult)
-
-F<sub>sg</sub> = view from ground to dome
-
-t<sub>TDD</sub>(q) = TDD beam transmittance
-
-t<sub>TDD,diff,aniso</sub> = TDD anisotropic sky transmittance
-
-t<sub>TDD,diff,iso</sub> = TDD isotropic diffuse transmittance
-
-#### Daylighting vs. Solar
-
-The beam transmittance of a TDD is calculated in the same way for both daylighting and solar gains.  If the visible and solar properties (i.e. absorptances in the input file) are the same, the reported TDD beam transmittances are equal.
-
-However, because the daylighting and solar models treat diffuse radiation differently, the TDD diffuse transmittances reported for visible and solar radiation will not necessarily be equal, even though the properties may be the same.
-
-Since the daylighting model calculates the diffuse illuminance using a sky and ground integration of many discrete elements, a visible diffuse transmittance is not required for the TDD daylighting simulation.  For reporting purposes only, the visible diffuse transmittance is estimated concurrent with the sky and ground integration using:
-
-<div>$${\tau_{diff}} = \frac{{\int {{\tau_{TDD}}(\theta )d{\Phi_{inc}}} }}{{\int {d{\Phi_{inc}}} }}$$</div>
-
-#### Conductive/Convective Gains
-
-For conductive and convective heat gain, TDDs are treated as one entity with an effective thermal resistance (i.e. R-value) between the outside and inside surfaces.  The outside face temperature of the dome and the inside face temperature of the diffuser are calculated as usual by the outside and inside heat balances respectively.  The temperatures are then copied to the inside face of the dome and the outside face of the diffuser.  Normal exterior and interior convection and IR radiation exchange occurs for both surfaces.
-
-Although little research has been done on the thermal characteristics of TDDs, one experiment (Harrison 1998) reports an average effective thermal resistance of 0.279 m<sup>2</sup> K/W for a commercial TDD measuring 0.33 m in diameter by 1.83 m in length.  This value, however, reflects a measurement from outdoor air temperature to indoor air temperature.  The model assumes an effective thermal resistance from outside surface temperature to inside surface temperature.
-
-Solar radiation is inevitably absorbed by the TDD before it reaches the zone.  Every reflection in the pipe leaves behind some solar radiation according to the surface absorptance.  Rays incident at a greater angle make more reflections and leave behind more absorbed solar in the pipe wall.
-
-The total absorbed solar radiation in the TDD is the sum of the following gains:
-
-* Inward bound solar absorbed by multiple pipe reflections
-
-* Outward bound solar absorbed by multiple pipe reflections due to:
-
-* Reflection off of diffuser surface (inside of TDD)
-
-* Zone diffuse interior shortwave incident on the diffuser from lights, etc.
-
-* Inward flowing absorbed solar in dome and diffuser glazing
-
-<div>$${Q_{abs,pipe}} = {Q_{abs,in}} + {Q_{abs,out}} + {Q_{abs,glazing}}$$</div>
-
-The inward bound solar absorbed by the pipe is the difference between the solar transmitted by the dome and the solar incident on the diffuser.
-
-<div>$${Q_{abs,in}} = {q''_{trans,dome}}{A_{dome}} - {q''_{inc,diffuser}}{A_{diffuser}}$$</div>
-
-The solar transmitted by the dome q"<sub>trans,dome</sub> is calculated as usual for a window.  The solar incident on the diffuser q"<sub>inc,diffuser</sub> is more complicated because each component must be treated separately.
-
-<div>$${q''_{inc,diffuser}} = {q''_{beam}}\frac{{{\tau_{TDD,beam}}(\theta )}}{{{\tau_{diffuser}}}} + {q''_{sky}}\frac{{{\tau_{TDD,aniso}}(Hour)}}{{{\tau_{diffuser}}}} + {q''_{gnd}}\frac{{{\tau_{TDD,iso}}}}{{{\tau_{diffuser}}}}$$</div>
-
-The outward bound solar absorbed by the pipe is given by:
-
-<div>$${Q_{abs,out}} = \left( {{{q''}_{refl,diffuser}}\frac{{\left( {1 - {\tau_{TDD}}} \right)}}{{{\tau_{diffuser}}}} + {{q''}_{zoneSW}}\left( {1 - {\tau_{TDD}}} \right)} \right){A_{diffuser}}$$</div>
-
-where q"<sub>zoneSW</sub> is the zone interior diffuse shortwave flux from window, lights, and ambient surface reflections, and
-
-<div>$${q''_{refl,diffuser}} = {q''_{inc,diffuser}} - {q''_{abs,diffuser}} - {q''_{trans,diffuser}}$$</div>
-
-The inward flowing portion of solar absorbed in the dome and diffuser glazing is:
-
-<div>$${Q_{abs,glazing}} = \frac{{{{q''}_{abs,dome}}{A_{dome}}}}{2} + \frac{{{{q''}_{abs,diffuser}}{A_{diffuser}}}}{2}$$</div>
-
-All absorbed solar radiation in the TDD is distributed among the transition zones that the pipe passes through between dome and diffuser.  The transition zone heat gain is proportional to the length of the zone.  Any exterior length of pipe also receives a proportional amount of heat, but this is lost to the outside. 
-
-#### References
-
-Harrison, S. J., McCurdy, G. G., Cooke, R. 1998.  "Preliminary Evaluation of the Daylighting and Thermal Performance of Cylindrical Skylights", Proceedings of International Daylight Conference, Ottawa, Canada, pp. 205-212.
-
-McCluney, R. 2003. "Rating of Tubular Daylighting Devices for Visible Transmittance and Solar Heat Gain -- Final Report", FSEC-CR-1385-03, January 15, 2003, Florida Solar Energy Center, 1679 Clearlake Rd., Cocoa, FL 32922.
-
-Swift, P. D., and Smith, G. B. 1995. "Cylindrical Mirror Light Pipes", Solar Energy Materials and Solar Cells 36, pp. 159-168.
-
-Zhang, X., Muneer, T., and Kubie, J. 2002.  "A Design Guide For Performance Assessment of Solar Light-Pipes", Lighting Research & Technology 34, 2, pp. 149-169.
-
-### Daylighting Shelves
-
-The input object DaylightingDevice:Shelf provides a special model for light shelves used to augment daylighting.  Light shelves are constructed from up to three components: a window, an inside shelf, and an outside shelf.  The inside shelf acts to reflect all transmitted light from the upper window onto the ceiling of the zone as diffuse light.  The outside shelf changes the amount of light incident on the window.  All light reflected from the outside shelf also goes onto the zone ceiling.  The inside shelf and outside shelf are both optional.  However, if neither shelf is specifed, the daylighting shelf object has no effect on the simulation.
-
-The window is divided into two window surfaces: an upper window and a lower window.  The upper window interacts with the daylighting shelf but the lower window does not, except to receive shading from the outside shelf.
-
-![](media/image893.png)
-
-Figure 70.  Daylighting Shelf Diagram
-
-Daylighting shelves are simulated separately for daylighting and the zone heat balance.  The general model is similar in both cases, but the details vary.
-
-#### Inside Shelf Daylighting
-
-The inside shelf is modeled in the daylighting simulation by converting all light transmitted by the upper window into diffuse upgoing flux.  It is assumed that no beam or downgoing flux can pass the end of the shelf regardless of the shelf's position or orientation.
-
-In the daylighting simulation this is accomplished by forcing all the transmitted flux to be upgoing:
-
-<div>$${\Phi_{CW}} = \Phi $$</div>
-
-<div>$${\Phi_{FW}} = 0$$</div>
-
-where
-
-F<sub>CW</sub> = upgoing flux
-
-F<sub>FW</sub> = downgoing flux
-
-F = total flux
-
-Since it is assumed that all light falls on the inside shelf, it is implied that the upper window  cannot contribute any direct illuminance (i.e. the upper window cannot be seen from anywhere in the zone).  The remaining light is entirely interreflected sky-related and interreflected sun-related upgoing flux.
-
-#### Inside Shelf Heat Balance
-
-In the heat balance simulation the inside shelf is defined as an interzone heat transfer surface, e.g. partition.  Since the inside shelf external boundary condition is required to refer to itself, the shelf is essentially equivalent to internal mass.  Because the shelf surface has two sides that participate in the zone heat balance, the surface area is doubled by the program during initialization.  Like internal mass, the shelf surface is allowed to interact convectively and radiatively with the zone air and other zone surfaces.
-
-The zone interior solar distribution is modified by the inside shelf.  Regardless of the solar distribution selected in the input file, all beam solar radiation transmitted by the upper window is incident on one side (half the doubled surface area) of the shelf surface.  The beam radiation not absorbed is reflected throughout the zone as diffuse shortwave radiation.  The treatment of sky and ground radiation is unchanged; both are added directly to the zone diffuse shortwave.
-
-The total beam, sky, and ground radiation transmitted by the upper window does not change.
-
-#### Outside Shelf Daylighting
-
-In the daylighting model the luminous flux transmitted by the upper window is determined by integrating over the sky and ground and summing the luminance contribution of each sky or ground element.  The luminance of any intervening exterior or interior surfaces is assumed to be zero.  As a shading surface, the effect of the outside shelf during the integration is to block part of the view of the ground, thereby reducing the window transmitted flux due to diffuse ground luminance.  After the integration is complete, the program calculates the amount of diffuse light that is reflected through the window from the outside shelf and adds it as a lump sum to the upgoing flux transmitted by the window.
-
-The additional shelf upgoing flux is the sum of sun-related and sky-related flux:
-
-<div>$${\Phi_{shelf,CW}} = {\Phi_{shelf,sun}} + {\Phi_{shelf,sky}}$$</div>
-
-where
-
-<div>$${\Phi_{shelf,sun}} = \left( {{E_{sun}}\cos \theta } \right){f_{sunlit}}{\rho_{vis}}{F_{ws}}{\tau_{diff,vis}}$$</div>
-
-<div>$${\Phi_{shelf,sky}} = {E_{h,sky}}{f_{skymult}}{\rho_{vis}}{F_{ws}}{\tau_{diff,vis}}$$</div>
-
-and
-
-E<sub>sun</sub> = exterior illuminance due to light from the sun
-
-E<sub>h,\\ sky</sub> = exterior horizontal illuminance due to light from the sky
-
-q = incident angle of the beam on the shelf
-
-f<sub>sunlit</sub> = sunlit beam fraction of the shelf surface area
-
-f<sub>skymult</sub> = anisotropic sky view multiplier (see AnisoSkyMult)
-
-r<sub>vis</sub> = shelf surface reflectivity in the visible spectrum
-
-F<sub>ws</sub> = view factor from window to shelf
-
-t<sub>diff,\\ vis</sub> = diffuse window transmittance in the visible spectrum
-
-The sunlit beam fraction f<sub>sunlit</sub> and the anisotropic sky view multiplier f<sub>skymult</sub> are borrowed from the heat balance solar calculations.
-
-The sunlit beam fraction f<sub>sunlit</sub> takes into account the effect of shading due to other surfaces.  Although shadows on the shelf surface change the luminance distribution of the shelf, there is no angular dependence because diffuse properties are assumed.  Therefore, the flux is simply proportional to the sunlit fraction.
-
-The anisotropic sky view multiplier f<sub>skymult</sub> takes into account the anisotropic distribution of sky radiation, the shelf view factor to the sky, and shading.  This value is utilized in the heat balance simulation for solar calculations but is not currently available in the daylighting simulation.  A value of 1.0 is assumed until a better model is developed.  For this reason the sky-related flux may be over-predicted for some building and shelf geometries.  However, for clear sky conditions the sun-related flux is dominant and the resulting error is small.
-
-The view factor to the outside shelf, F<sub>ws</sub>, if not specified by the user in the input object, is an exact view factor calculated for adjacent perpendicular rectangles.
-
-
-
-![](media/image899.png)
-
-Figure 71.  Window and Outside Shelf as Adjacent Perpendicular Rectangles.
-
-For this geometry the view factor is given by (Mills 1995):
-
-<div>$${F_{ws}} = \frac{1}{{\pi M}}\left\{ \begin{array}{l}M{\tan ^{ - 1}}\left( {\frac{1}{M}} \right) + N{\tan ^{ - 1}}\left( {\frac{1}{N}} \right) - {\left( {{M^2} + {N^2}} \right)^{1/2}}{\tan ^{ - 1}}\left( {{{\left( {{M^2} + {N^2}} \right)}^{ - 1/2}}} \right)\\ + \frac{1}{4}\ln \left[ {\left( {\frac{{\left( {1 + {M^2}} \right)\left( {1 + {N^2}} \right)}}{{1 + {M^2} + {N^2}}}} \right){{\left( {\frac{{{M^2}\left( {1 + {M^2} + {N^2}} \right)}}{{\left( {1 + {M^2}} \right)\left( {{M^2} + {N^2}} \right)}}} \right)}^{{M^2}}}{{\left( {\frac{{{N^2}\left( {1 + {M^2} + {N^2}} \right)}}{{\left( {1 + {N^2}} \right)\left( {{M^2} + {N^2}} \right)}}} \right)}^{{N^2}}}} \right]\end{array} \right\}$$</div>
-
-where
-
-<div>$$M = H/W$$</div>
-
-<div>$$N = L/W$$</div>
-
-#### Outside Shelf Heat Balance
-
-The heat balance simulation does not do a sky and ground integration.  View factors to sky and ground are used instead.  Consequently, the heat balance calculation for the outside shelf is very similar to the daylighting calculation.  The main difference is that the incident flux on the upper window is calculated first and reported.  The transmitted and absorbed fractions are subsequently determined.
-
-The solar flux incident on the upper window due to the shelf is given by:
-
-<div>$${q''_{shelf - inc}} = {q''_{shelf - inc,sun}} + {q''_{shelf - inc,sky}}$$</div>
-
-where
-
-<div>$${q''_{shelf - inc,sun}} = \left( {{I_{sun}}\cos \theta } \right){f_{sunlit}}{\rho_{sol}}{F_{ws}}$$</div>
-
-<div>$${q''_{shelf - inc,sky}} = {I_{h,sky}}{f_{skymult}}{\rho_{sol}}{F_{ws}}$$</div>
-
-and
-
-I<sub>sun</sub> = solar beam intensity of the sun
-
-I<sub>h,\\ sky</sub> = total horizontal diffuse solar radiation due to the sky
-
-q = incident angle of the beam on the shelf
-
-f<sub>sunlit</sub> = sunlit beam fraction of the surface area
-
-f<sub>skymult</sub> = anisotropic sky view multiplier (see AnisoSkyMult)
-
-r<sub>sol</sub> = shelf surface reflectivity in the solar spectrum
-
-F<sub>ws</sub> = view factor from window to shelf
-
-The view factor F<sub>ws</sub> is the same as described above for daylighting.
-
-The total diffuse incident radiation due to the shelf is internally added to the ground diffuse incident radiation on the window.  For reporting purposes the shelf radiation is included in the *Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area* output variable.
-
-With the incident radiation determined, the remaining window heat balance is calculated normally.  The resulting transmitted diffuse radiation from the sky, ground, and shelf is:
-
-<div>$${q''_{trans}} = \left( {{{q''}_{sky - inc}} + {{q''}_{gnd - inc}} + {{q''}_{shelf - inc}}} \right){\tau_{diff,sol}}$$</div>
-
-where
-
-t<sub>diff,\\ sol</sub> = diffuse window transmittance in the solar spectrum
-
-#### References
-
-Mills, A. F. 1995. Heat and Mass Transfer, p. 499.
-
-### Window Light Well
-
-The input object DaylightingDevice:LightWell provides a model for attenuation of light transmitted by windows and skylights that can result from surrounding interior finish surfaces that form a “light well.�  The light well model simply attenuates the light transmitted by the exterior window.  The model does not redirect light distributions or alter the relative mixture of diffuse and beam transmitted by the window.
-
-The attenuation is characterized by the **well efficiency**, which is the ratio of the amount of light leaving the well to the amount of light entering the well. The well efficiency varies from close to 1.0  to close to zero if there is high attenuation. The well efficiency is used only in the EnergyPlus detailed daylighting calculation, where it multiplies the beam and diffuse light transmitted by the skylight. (The well efficiency is not used in calculating the solar gain through the skylight.)
-
-![](media/image907.png)
-
-Figure 72. Skylight with light well: (a) perspective view, (b) vertical section.
- If the bottom of the light well is a rectangle of side lengths c and d, as shown in (a), then the perimeter of the bottom of the well = 2(c+d) and the area = cd (see description of field names for the Light Well object).
-
-The well efficiency depends on the visible reflectance of well’s side walls and on the well cavity ratio, ***WCR***, which is given by:
-
-<div>$$WCR = \frac{{{\rm{2}}{\rm{.5 x Well Height x Well Perimeter}}}}{{{\rm{Well Area}}}}$$</div>
-
-Well Height, Well Perimeter and Well Area are inputs to the model and are discussed in the figure caption above.
-
-The model in EnergyPlus was implemented by fitting a curve to the data presented as Figure 8-21, “Efficiency factors for various depths of light wells based on well-interreflectance values,� found in the Lighting Handbook (IES 1993).  The figure below reproduces that reference data and shows well efficiency vs. WCR for different side wall reflectances. For use in the EnergyPlus calculation, a fit has been made to this graph that gives the following mathematical expression, where “Reflectance� is the user input value of the well-wall reflectance expressed as a fraction:
-
-<div>$${\rm{Well efficiency}} = {e^{ - WCR*(0.16368 - 0.144678*{\rm{Reflectance}})}}$$</div>
-
-![](media/image910.png)
-
-Figure 73. Graph showing light well efficiency vs. well cavity ratio (WCR) for well-wall visible reflectances of 80% (upper curve), 60% (middle curve) and 40% (lower curve). Based on Fig. 8-21 of the Lighting Handbook: Reference and Application, 8<sup>th</sup> Edition, 1993, Illuminating Engineering Society of North America.
-
-The well efficiency calculated using this curve fit and user inputs is then applied to daylight transmission rates to attenuate daylight as a result of the presence of the light well,
-
-#### References
-
-Lighting Handbook: Reference & Application, 8th Edition, Illuminating Engineering Society of North America, 1993.
-
-Window Calculation Module
--------------------------
-
-This section describes two potential modeling approaches for Windows.  The first (layer by layer) is implemented.  The second, simple approach, reuses the layer-by-layer approach but converts an arbitrary window performance into an equivalent single layer.
-
-The primary Window calculation is a layer-by-layer approach where windows are considered to be composed of the following components, only the first of which, glazing, is required to be present:
-
-* ***Glazing***, which consists of one or more plane/parallel glass layers. If there are two or more glass layers, the layers are separated by gaps filled with air or another gas. The glazing optical and thermal calculations are based on algorithms from the WINDOW 4 and WINDOW 5 programs [Arasteh et al., 1989], [Finlayson et al., 1993].  Glazing layers are described using te input object WindowMaterial:Glazing.
-
-* ***Gap***, layers filled with air or another gas that separate glazing layers.  Gaps are described using the input object WindowMaterial:Gas.
-
-* ***Frame***, which surrounds the glazing on four sides.  Frames are described using the input object WindowProperty:FrameAndDivider.
-
-* ***Divider***, which consists of horizontal and/or vertical elements that divide the glazing into individual lites.
-
-* ***Shading device***, which is a separate layer, such as drapery, roller shade or blind, on the inside or outside of the glazing, whose purpose is to reduce solar gain, reduce heat loss (movable insulation) or control daylight glare.  Shading layers are described using “WindowProperty:ShadingControl� input objects.
-
-In the following, the description of the layer-by-layer glazing algorithms is based on material from Finlayson et al., 1993. The frame and divider thermal model, and the shading device optical and thermal models, are new to EnergyPlus.
-
-A second approch has been developed where windows are modeled in a simplified approach that requires minimal user input that is processed to develop and equivalent layer that then reuses much of the layer-by-model.  This “Simple Window Construction: model is described below.
-
-### Optical Properties of Glazing
-
-The solar radiation transmitted by a system of glass layers and the solar radiation absorbed in each layer depends on the solar transmittance, reflectance and absorptance properties of the individual layers. The absorbed solar radiation enters the glazing heat balance calculation that determines the inside surface temperature and, therefore, the heat gain to the zone from the glazing (see “Window Heat Balance Calculation�). The transmitted solar radiation is absorbed by interior zone surfaces and, therefore, contributes to the zone heat balance. In addition, the visible transmittance of the glazing is an important factor in the calculation of interior daylight illuminance from the glazing.
-
-Table 28.  Variables in Window Calculations
-
-<table class="table table-striped">
-<tr>
-<th>Mathematical variable</th>
-<th>Description</th>
-<th>Units</th>
-<th>FORTRAN variable</th>
-</tr>
-<tr>
-<td>T</td>
-<td>Transmittance</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>R</td>
-<td>Reflectance</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>R<sup>f</sup>, R<sup>b</sup></td>
-<td>Front reflectance, back reflectance</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sub>i,j</sub></td>
-<td>Transmittance through glass layers i to j</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sup>dir</sup><sub>gl</sub></td>
-<td>Direct transmittance of glazing</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>R<sup>f</sup><sub>i,j</sub>, R<sup>b</sup><sub>i,j</sub></td>
-<td>Front reflectance, back reflectance from glass layers i to j</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>R<sup>dir</sup><sub>gl,f</sub>, R<sup>dir</sup><sub>gl,b</sub></td>
-<td>Direct front and back reflectance of glazing</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>A<sup>f</sup><sub>i</sub>, A<sup>b</sup><sub>i</sub></td>
-<td>Front  absorptance, back absorptance of layer i</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>N</td>
-<td>Number of glass layers</td>
-<td>-</td>
-<td>Nlayer</td>
-</tr>
-<tr>
-<td>λ</td>
-<td>Wavelength</td>
-<td>microns</td>
-<td>Wle</td>
-</tr>
-<tr>
-<td>E<sub>s</sub>(λ)</td>
-<td>Solar spectral irradiance function</td>
-<td>W/m<sup>2</sup>-micron</td>
-<td>E</td>
-</tr>
-<tr>
-<td>V(λ)</td>
-<td>Photopic response function of the eye</td>
-<td>-</td>
-<td>y30</td>
-</tr>
-<tr>
-<td>φ</td>
-<td>Angle of incidence (angle between surface normal and direction of incident beam radiation)</td>
-<td>Rad</td>
-<td>Phi</td>
-</tr>
-<tr>
-<td>Ï„</td>
-<td>Transmittivity or transmittance</td>
-<td>-</td>
-<td>tf0</td>
-</tr>
-<tr>
-<td>�</td>
-<td>Reflectivity or reflectance</td>
-<td>-</td>
-<td>rf0, rb0</td>
-</tr>
-<tr>
-<td>α</td>
-<td>Spectral absorption coefficient</td>
-<td>m<sup>-1</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>d</td>
-<td>Glass thickness</td>
-<td>M</td>
-<td>Material%Thickness</td>
-</tr>
-<tr>
-<td>n</td>
-<td>Index of refraction</td>
-<td>-</td>
-<td>ngf, ngb</td>
-</tr>
-<tr>
-<td>κ</td>
-<td>Extinction coefficient</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>β</td>
-<td>Intermediate variable</td>
-<td>-</td>
-<td>betaf, betab</td>
-</tr>
-<tr>
-<td>P, p</td>
-<td>A general property, such as transmittance</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Ï„<sub>sh</sub></td>
-<td>Shade transmittance</td>
-<td>-</td>
-<td>Material%Trans</td>
-</tr>
-<tr>
-<td>�<sub>sh</sub></td>
-<td>Shade reflectance</td>
-<td>-</td>
-<td>Material%ReflectShade</td>
-</tr>
-<tr>
-<td>α<sub>sh</sub></td>
-<td>Shade absorptance</td>
-<td>-</td>
-<td>Material%AbsorpSolar</td>
-</tr>
-<tr>
-<td>τ<sub>bl,</sub>�<sub>bl,</sub>α<sub>bl</sub></td>
-<td>Blind transmittance, reflectance, absorptance</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Q, G, J</td>
-<td>Source, irradiance and radiosity for blind optical properties calculation</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>F<sub>ij</sub></td>
-<td>View factor between segments i and j</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>f<sub>switch</sub></td>
-<td>Switching factor</td>
-<td>-</td>
-<td>SwitchFac</td>
-</tr>
-<tr>
-<td>T</td>
-<td>Transmittance</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>R</td>
-<td>Reflectance</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>R<sup>f</sup>, R<sup>b</sup></td>
-<td>Front reflectance, back reflectance</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>T<sub>i,j</sub></td>
-<td>Transmittance through glass layers i to j</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>R<sup>f</sup><sub>i,j</sub>, R<sup>b</sup><sub>i,j</sub></td>
-<td>Front reflectance, back reflectance from glass layers i to j</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>A<sup>f</sup><sub>i</sub>, A<sup>b</sup><sub>i</sub></td>
-<td>Front  absorptance, back absorptance of layer i</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>N</td>
-<td>Number of glass layers</td>
-<td>-</td>
-<td>Nlayer</td>
-</tr>
-<tr>
-<td>λ</td>
-<td>Wavelength</td>
-<td>microns</td>
-<td>Wle</td>
-</tr>
-<tr>
-<td>E<sub>s</sub>(λ)</td>
-<td>Solar spectral irradiance function</td>
-<td>W/m<sup>2</sup>-micron</td>
-<td>E</td>
-</tr>
-<tr>
-<td>R(λ)</td>
-<td>Photopic response function of the eye</td>
-<td>-</td>
-<td>y30</td>
-</tr>
-<tr>
-<td>φ'</td>
-<td>Relative azimuth angle (angle between screen surface normal and vertical plane through sun, Ref. Figure 87)</td>
-<td>Rad</td>
-<td>SunAzimuthToScreenNormal</td>
-</tr>
-<tr>
-<td>α'</td>
-<td>Relative altitude angle (angle between screen surface horizontal normal plane and direction of incident beam radiation, Ref. Figure 87)</td>
-<td>Rad</td>
-<td>SunAltitudeToScreenNormal</td>
-</tr>
-<tr>
-<td>�<sub>sc</sub></td>
-<td>Beam-to-diffuse solar reflectance of screen material</td>
-<td>-</td>
-<td>Screens%ReflectCylinder</td>
-</tr>
-<tr>
-<td>γ</td>
-<td>Screen material aspect ratio</td>
-<td>-</td>
-<td>Screens%ScreenDiameterTo
-SpacingRatio</td>
-</tr>
-<tr>
-<td>Α</td>
-<td>Spectral absorption coefficient</td>
-<td>m<sup>-1</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>D</td>
-<td>Glass thickness</td>
-<td>M</td>
-<td>Material%Thickness</td>
-</tr>
-<tr>
-<td>N</td>
-<td>Index of refraction</td>
-<td>-</td>
-<td>ngf, ngb</td>
-</tr>
-<tr>
-<td>Κ</td>
-<td>Extinction coefficient</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Î’</td>
-<td>Intermediate variable</td>
-<td>-</td>
-<td>betaf, betab</td>
-</tr>
-<tr>
-<td>P, p</td>
-<td>A general property, such as transmittance</td>
-<td>-</td>
-<td>-</td>
-</tr>
-
-</table>
-
-### Glass Layer Properties
-
-In EnergyPlus, the optical properties of individual glass layers are given by the following quantities at normal incidence as a function of wavelength:
-
-Transmittance, *T*
-
-Front reflectance, *R<sup>f</sup>*
-
-Back reflectance, *R<sup>b</sup>*
-
-Here “front� refers to radiation incident on the side of the glass closest to the outside environment, and “back� refers to radiant incident on the side of the glass closest to the inside environment. For glazing in exterior walls, “front� is therefore the side closest to the outside air and “back� is the side closest to the zone air. For glazing in interior (i.e., interzone) walls, “back� is the side closest to the zone in which the wall is defined in and “front� is the side closest to the adjacent zone.
-
-### Glass Optical Properties Conversion
-
-#### Conversion from Glass Optical Properties Specified as Index of Refraction and Transmittance at Normal Incidence
-
-The optical properties of uncoated glass are sometimes specified by index of refraction, *n*,*
-* and transmittance at normal incidence, *T*.
-
-The following equations show how to convert from this set of values to the transmittance and reflectance values required by Material:WindowGlass. These equations apply only to uncoated glass, and can be used to convert either spectral-average solar properties or spectral-average visible properties (in general, *n* and *T* are different for the solar and visible). Note that since the glass is uncoated, the front and back reflectances are the same and equal to the *R* that is solved for in the following equations.
-
-Given *n* and *T*, find *R*:
-
-<div>$$\begin{array}{l}r = {\left( {\frac{{n - 1}}{{n + 1}}} \right)^2}\\\tau  = \frac{{{{\left[ {{{(1 - r)}^4} + 4{r^2}{T^2}} \right]}^{1/2}} - {{(1 - r)}^2}}}{{2{r^2}T}}\\R = r + \frac{{{{(1 - r)}^2}r{\tau ^2}}}{{1 - {r^2}{\tau ^2}}}\end{array}$$</div>
-
-**Example:**
-
-*T* = 0.86156
-
-*n* = 1.526
-
-<div>$$\begin{array}{l}r = {\left( {\frac{{1.526 - 1}}{{1.526 + 1}}} \right)^2}\\\tau  = 0.93974\\R = 0.07846\end{array}$$</div>
-
-### Simple Window Model
-
-EnergyPlus includes an alternate model that allows users to enter in simplified window performance indices.  This model is accessed through the WindowMaterial:SimpleGlazingSystem input object and converts the simple indices into an equivalent single layer window.  (In addition a special model is used to determine the angular properties of the system – described below).  Once the model generates the properties for the layer, the program reuses the bulk of the layer-by-layer model for subsequent calculations.  The properties of the equivalent layer are determined using the step by step method outlined by Arasteh, Kohler, and Griffith (2009).  The core equations are documented here.  The reference contains additional information.
-
-The simplified window model accepts U and SHGC indices and is useful for several reasons:
-
-1)   Sometimes, the only thing that is known about the window are its U and SHGC;
-
-2)   Codes, standards, and voluntary programs are developed in these terms;
-
-3)   A single-layer calculation is faster than multi-layer calculations.
-
-Note: This use of U and SHGC to describe the thermal properties of windows is only appropriate for specular glazings.
-
-While it is important to include the ability to model windows with only U-value and SHGC, we note that any method to use U and SHGC alone in building simulation software will inherently be approximate.  This is due primarily to the following factors:
-
-* SHGC combines directly transmitted solar radiation and radiation absorbed by the glass which flows inward.  These have different implications for space heating/cooling.  Different windows with the same SHGC often have different ratios of transmitted to absorbed solar radiation.
-
-* SHGC is determined at normal incidence; angular properties of glazings vary with number of layers, tints, coatings.  So products which have the same SHGC, can have different angular properties.
-
-* Window U-factors vary with temperatures.
-
-Thus, for modeling specific windows, we recommend using more detailed data than just the U and SHGC, if at all possible.
-
-The simplified window model determines the properties of an equivalent layer in the following steps.
-
-#### Step 1.  Determine glass-to-glass Resistance.
-
-Window U-values include interior and exterior surface heat transfer coefficients.  The resistance of the bare window product, or glass-to-glass resistance is augmented by these film coefficients so that,
-
-<div>$$\frac{1}{U} = {R_{i,w}} + {R_{o,w}} + {R_{l,w}}$$</div>
-
-Where,
-
-<span>\({R_{i,w}}\)</span> is the resistance of the interior film coefficient under standard winter conditions in units of m<sup>2</sup>·K/W,
-
-<span>\({R_{o,w}}\)</span> is the resistance of the exterior film coefficient under standard winter conditions in units of m<sup>2</sup>·K/W, and
-
-<span>\({R_{l,w}}\)</span> is the resisance of the bare window under winter conditions (without the film coefficients) in units of m<sup>2</sup>·K/W.
-
-The values for <span>\({R_{i,w}}\)</span> and <span>\({R_{o,w}}\)</span> depend on U and are calculated using the following correlations.
-
-<div>$${R_{i,w}} = \frac{1}{{(0.359073\;Ln(U) + 6.949915)}};\quad for\quad U &lt; 5.85$$</div>
-
-<div>$${R_{i,w}} = \frac{1}{{(1.788041\;U - 2.886625)}};\quad for\quad U \ge 5.85$$</div>
-
-<div>$${R_{o,w}} = \frac{1}{{(0.025342\;U + 29.163853)}}$$</div>
-
-So that the glass-to-glass resistance is calculated using,
-
-<span>\({R_{l,w}} = \frac{1}{U} - {R_{i,w}} - {R_{o,w}}\)</span>.
-
-Because the window model in EnergyPlus is for flat geometries, the models are not necessarily applicable to low-performance projecting products, such as skylights with unisulated curbs.  The model cannot support glazing systems with a U higher than 7.0 because the thermal resistance of the film coefficients alone can provide this level of performance and none of the various resistances can be negative.
-
-#### Step 2.  Determine Layer Thickness.
-
-The thickness of the equivalent layer in units of meters is calculated using,
-
-<div>$$Thickness = 0.002\;;\quad for\;{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 {{R_{l,w}}}}}\right.}\!\lower0.7ex\hbox{${{R_{l,w}}}$}} > 7.0$$</div>
-
-<div>$$Thickness = 0.05914 - \left( {\frac{{0.00714}}{{{R_{l,w}}}}} \right);\;{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 {{R_{l,w}}}}}\right.}\!\lower0.7ex\hbox{${{R_{l,w}}}$}} \le 7.0$$</div>
-
-#### Step 3.  Determine Layer Thermal Conductivity
-
-The effective thermal conductivity, <span>\({\lambda_{eff}}\)</span>, of the equivalent layer is calculated using,
-
-<div>$${\lambda_{eff}} = \frac{{Thickness}}{{{R_{l,w}}}}$$</div>
-
-#### Step 4.  Determine Layer Solar Transmittance
-
-The layer’s solar transmittance at normal incidence, <span>\({T_{sol}}\)</span>, is calculated using correlations that are a function of SHGC and U-Factor.
-
-<div>$${T_{sol}} = 0.939998\;SHG{C^2} + 0.20332\;SHGC;\quad U > 4.5;\;SHGC &lt; 0.7206$$</div>
-
-<div>$${T_{sol}} = 1.30415SHGC - 0.30515\;;\quad U > 4.5;\;SHGC \ge 0.7206$$</div>
-
-<div>$${T_{sol}} = 0.41040\;SHGC;\quad U &lt; 3.4;\;SHGC \le 0.15$$</div>
-
-<div>$${T_{sol}} = 0.085775\;SHG{C^2} + 0.963954\;SHGC - 0.084958\;;\;\;U &lt; 3.4;\;SHGC > 0.15$$</div>
-
-And for U-values between 3.4 and 4.5, the value for <span>\({T_{sol}}\)</span> is interpolated using results of the equations for both ranges.
-
-#### Step 5.  Determine Layer Solar Reflectance
-
-The layer’s solar reflectance is calculated by first determining the inward flowing fraction which requires values for the resistance of the inside and outside film coefficients under summer conditions, <span>\({R_{i,s}}\)</span> and <span>\({R_{o,s}}\)</span>respectively.  The correlations are
-
-<span>\({R_{i,s}} = \frac{1}{{\left( {29.436546\;{{\left( {SHGC - {T_{Sol}}} \right)}^3} - 21.943415{{\left( {SHGC - {T_{Sol}}} \right)}^2} + 9.945872\left( {SHGC - {T_{Sol}}} \right) + 7.426151} \right)}};\,U > 4.5\)</span><span>\({R_{i,s}} = \frac{1}{{\left( {199.8208128\;{{\left( {SHGC - {T_{Sol}}} \right)}^3} - 90.639733{{\left( {SHGC - {T_{Sol}}} \right)}^2} + 19.737055\left( {SHGC - {T_{Sol}}} \right) + 6.766575} \right)}};\,U &lt; 3.4\)</span><span>\({R_{o,s}} = \frac{1}{{\left( {2.225824(SHGC - {T_{Sol}}) + 20.57708} \right)}};\;U > 4.5\)</span>
-
-<div>$${R_{o,s}} = \frac{1}{{\left( {5.763355(SHGC - {T_{Sol}}) + 20.541528} \right)}};\;U &lt; 3.4$$</div>
-
-And for U-values between 3.4 and 4.5, the values are interpolated using results from both sets of equations.
-
-The inward flowing fraction, <span>\(Fra{c_{inward}}\)</span>, is then calculated using
-
-<div>$$Fra{c_{inward}} = \frac{{\left( {{R_{o,s}} + 0.5\,{R_{l,w}}} \right)}}{{\left( {{R_{o,s}} + {R_{l,w}} + {R_{i,s}}} \right)}}$$</div>
-
-The the solar reflectances of the front face, <span>\({R_{s,f}}\)</span>, and back face, <span>\({R_{s,b}}\)</span>, are calculated using,
-
-<span>\({R_{s,f}} = {R_{s,b}} = 1 - {T_{Sol}} - \frac{{\left( {SHGC - {T_{Sol}}} \right)}}{{Fra{c_{inward}}}}\)</span>.
-
-The thermal absorptance, or emittance, is take as 0.84 for both the front and back and the longwave transmittance is 0.0.
-
-#### Step 6.  Determine Layer Visible Properties
-
-The user has the option of entering a value for visible transmittance as one of the simple performance indices.  If the user does not enter a value, then the visible properties are the same as the solar properties.  If the user does enter a value then layer’s visible transmittance at normal incidence, <span>\({T_{Vis}}\)</span>,is set to that value.  The visible light reflectance for the back surface is calculated using,
-
-<div>$${R_{Vis,b}} =  - 0.7409\,T_{Vis}^3 + 1.6531\,T_{Vis}^2 - 1.2299\,{T_{Vis}} + 0.4547$$</div>
-
-The visible light reflectance for the front surface is calculated using,
-
-<div>$${R_{Vis,f}} =  - 0.0622\,T_{Vis}^3 + 0.4277\,T_{Vis}^2 - 0.4169\,{T_{Vis}} + 0.2399$$</div>
-
-#### Step 7. Determine Angular Performance
-
-The angular properties of windows are important because during energy modeling, the solar incidence angles are usually fairly high.  Angles of incidence are defined as angles from the normal direction extending out from the window.  The simple glazing system model includes a range of correlations that are selected based on the values for U and SHGC.  These were chosen to match the types of windows likely to have such performance levels.  The matrix of possible combinations of U and SHGC values have been mapped to set of 28 bins shown in the following figure.
-
-
-
- ![AngularCorrelationMAP](media/image947.png)
-
-Figure 74. Diagram of Transmittance and Reflectance Correlations Used based on U and SHGC.
-
-There are ten different correlations, A thru J, for both transmission and reflectance.  The correlations are used in various weighting and interpolation schemes according the figure above.  The correlations are normalized against the performance at normal incidence.  EnergyPlus uses these correlations to store the glazing system’s angular performance at 10 degree increments and interpolates between them during simulations.  The model equations use the cosine of the incidence angle, <span>\(\cos (\varphi )\)</span>, as the independent variable.  The correlations have the form:
-
-<div>$$T\;or\;R = a\cos {(\varphi )^4} + b\cos {(\varphi )^3} + c\cos {(\varphi )^2} + d\cos (\varphi ) + e$$</div>
-
-The coefficient values for a, b, c, d, and e are listed in the following tables for each of the curves.
-
-
-
-![Figure72](media/image950.png)
-
-Figure 75. Normalized Transmittance Correlations for Angular Performance
-
-
-
-![Fiure73](media/image951.png)
-
-Figure 76. Normalized Reflectanct Correlations for Angular Performance
-
-#### Application Issues
-
-EnergyPlus’s normal process of running the detailed layer-by-layer model, with the equivalent layer produced by this model, creates reports (sent to the EIO file) of the overall performance indices and the properties of the equivalent layer. Both of these raise issues that may be confusing.
-
-The simplified window model does not reuse all aspects of the detailed layer-by-layer model, in that the angular solar transmission properties use a different model when the simple window model is in effect. If the user takes the material properties of an equivalent glazing layer from the simple window model and then re-enters them into just the detailed model, then the performance will not be the same because of the angular transmission model will have changed. It is not proper use of the model to re-enter the equivalent layer’s properties and expect the exact level of performance.
-
-There may not be exact agreement between the performance indices echoed out and those input in the model. This is expected with the model and the result of a number of factors. For example, although input is allowed to go up to U-7 W/m<sup>2</sup>∙K, the actual outcome is limited to no higher than about 5.8W/m<sup>2</sup>∙K. This is because the thermal resistance to heat transfer at the surfaces is already enough resistance to provide an upper limit to the conductance of a planar surface. Sometimes there is conflict between the SHGC and the U that are not physical and compromises need to be made. In general, the simple window model is intended to generate a physically-reasonable glazing that approximates the input entered as well as possible. But the model is not always be able to do exactly what is specified when the specifications are not physical.
-
-#### References
-
-Arasteh, D., J.C. Kohler, B. Griffith, Modeling Windows in EnergyPlus with Simple Performance Indices. Lawrence Berkeley National Laboratory. In Draft. Available at
-
-### Glazing System Properties
-
-The optical properties of a glazing system consisting of *N* glass layers separated by nonabsorbing gas layers (Figure 77.  Schematic of transmission, reflection and absorption of solar radiation within a multi-layer glazing system.) are determined by solving the following recursion relations for *T<sub>i,j</sub>*, the transmittance through layers* i* to* j*; *R<sup>f</sup><sub>i,j</sub>* and *R<sup>b</sup><sub>i,j</sub>*, the front and back reflectance, respectively, from layers* i* to* j*; and *A<sub>j</sub>*, the absorption in layer* j*. Here layer 1 is the outermost layer and layer *N* is the innermost layer. These relations account for multiple internal reflections within the glazing system. Each of the variables is a function of wavelength.
-
-<div>$${T_{i,j}} = \frac{{{T_{i,j - 1}}{T_{j,j}}}}{{1 - R_{j,j}^fR_{j - 1,i}^b}}$$</div>
-
-<div>$$R_{i,j}^f = R_{i,j - 1}^f + \frac{{T_{i,j - 1}^2R_{j,j}^f}}{{1 - R_{j,j}^fR_{j - 1,i}^b}}$$</div>
-
-<div>$$R_{j,i}^b = R_{j,j}^b + \frac{{T_{j,j}^2R_{j - 1,i}^b}}{{1 - R_{j - 1,i}^bR_{j,j}^f}}$$</div>
-
-<div>$$A_j^f = \frac{{{T_{1,j - 1}}(1 - {T_{j,j}} - R_{j,j}^f)}}{{1 - R_{j,N}^fR_{j - 1,1}^b}} + \frac{{{T_{1,j}}R_{j + 1,N}^f(1 - {T_{j,j}} - R_{j,j}^b)}}{{1 - R_{j,N}^fR_{j - 1,1}^b}}$$</div>
-
-In Eq. *T<sub>i,j</sub>* = 1 and *R<sub>i,j</sub>* = 0 if* i*&lt;0 or* j*&gt;*N*.
-
-![](media/image956.png)
-
-Figure 77.  Schematic of transmission, reflection and absorption of solar radiation within a multi-layer glazing system.
-
-As an example, for double glazing (*N*=2) these equations reduce to
-
-<div>$${T_{1,2}} = \frac{{{T_{1,1}}{T_{2,2}}}}{{1 - R_{2,2}^fR_{1,1}^b}}$$</div>
-
-<div>$$R_{1,2}^f = R_{1,1}^f + \frac{{T_{1,1}^2R_{2,2}^f}}{{1 - R_{2,2}^fR_{1,1}^b}}$$</div>
-
-<div>$$R_{2,1}^b = R_{2,2}^b + \frac{{T_{2,2}^2R_{1,1}^b}}{{1 - R_{1,1}^bR_{2,2}^f}}$$</div>
-
-<div>$$A_1^f = (1 - {T_{1,1}} - R_{1,1}^f) + \frac{{{T_{1,1}}R_{2,2}^f(1 - {T_{1,1}} - R_{1,1}^b)}}{{1 - R_{2,2}^fR_{1,1}^b}}$$</div>
-
-<div>$$A_2^f = \frac{{{T_{1,1}}(1 - {T_{2,2}} - R_{2,2}^f)}}{{1 - R_{2,2}^fR_{1,1}^b}}$$</div>
-
-If the above transmittance and reflectance properties are input as a function of wavelength, EnergyPlus calculates “spectral average� values of the above glazing system properties by integrating over wavelength:
-
-The spectral-average solar property is
-
-<div>$${P_s} = \frac{{\int {P(\lambda ){E_s}(\lambda )d\lambda } }}{{\int {{E_s}(\lambda )d\lambda } }}$$</div>
-
-The spectral-average visible property is
-
-<div>$${P_v} = \frac{{\int {P(\lambda ){E_s}(\lambda )V(\lambda )d\lambda } }}{{\int {{E_s}(\lambda )V(\lambda )d\lambda } }}$$</div>
-
-where <span>\({E_s}(\lambda )\)</span>is the solar spectral irradiance function and <span>\(V(\lambda )\)</span>is the photopic response function of the eye. The default functions are shown in Table 29 and Table 30. They can be overwritten by user defined solar and/or visible spectrum using the objects Site:SolarAndVisibleSpectrum and Site:SpectrumData. They are expressed as a set of values followed by the corresponding wavelengths for values.
-
-If a glazing layer has optical properties that are roughly constant with wavelength, the wavelength-dependent values of *T<sub>i,i</sub>* , *R<sup>f</sup><sub>i,i</sub>* and *R<sup>b</sup><sub>i,i</sub>* in Eqs. to can be replaced with constant values for that layer.
-
-Table 29. Solar spectral irradiance function.
-
-<table class="table table-striped">
-<tr>
-<td>Air mass 1.5 terrestrial solar global spectral irradiance values (W/m<sup>2</sup>-micron) on a 37<sup>o</sup> tilted surface. Corresponds to wavelengths in following data block. Based on ISO 9845-1 and ASTM E 892; derived from Optics5 data file ISO-9845GlobalNorm.std, 10-14-99.</td>
-</tr>
-<tr>
-<td>                  0.0,   9.5,  42.3, 107.8, 181.0, 246.0, 395.3, 390.1, 435.3, 438.9,
-       483.7, 520.3, 666.2, 712.5, 720.7,1013.1,1158.2,1184.0,1071.9,1302.0,
-      1526.0,1599.6,1581.0,1628.3,1539.2,1548.7,1586.5,1484.9,1572.4,1550.7,
-      1561.5,1501.5,1395.5,1485.3,1434.1,1419.9,1392.3,1130.0,1316.7,1010.3,
-      1043.2,1211.2,1193.9,1175.5, 643.1,1030.7,1131.1,1081.6, 849.2, 785.0,
-       916.4, 959.9, 978.9, 933.2, 748.5, 667.5, 690.3, 403.6, 258.3, 313.6,
-       526.8, 646.4, 746.8, 690.5, 637.5, 412.6, 108.9, 189.1, 132.2, 339.0,
-       460.0, 423.6, 480.5, 413.1, 250.2,  32.5,   1.6,  55.7, 105.1, 105.5,
-       182.1, 262.2, 274.2, 275.0, 244.6, 247.4, 228.7, 244.5, 234.8, 220.5,
-       171.5,  30.7,   2.0,   1.2,  21.2,  91.1,  26.8,  99.5,  60.4,  89.1,
-        82.2,  71.5,  70.2,  62.0,  21.2,  18.5,   3.2</td>
-</tr>
-<tr>
-<td>Wavelengths (microns) corresponding to above data block</td>
-</tr>
-<tr>
-<td>           0.3000,0.3050,0.3100,0.3150,0.3200,0.3250,0.3300,0.3350,0.3400,0.3450,
-      0.3500,0.3600,0.3700,0.3800,0.3900,0.4000,0.4100,0.4200,0.4300,0.4400,
-      0.4500,0.4600,0.4700,0.4800,0.4900,0.5000,0.5100,0.5200,0.5300,0.5400,
-      0.5500,0.5700,0.5900,0.6100,0.6300,0.6500,0.6700,0.6900,0.7100,0.7180,
-      0.7244,0.7400,0.7525,0.7575,0.7625,0.7675,0.7800,0.8000,0.8160,0.8237,
-      0.8315,0.8400,0.8600,0.8800,0.9050,0.9150,0.9250,0.9300,0.9370,0.9480,
-      0.9650,0.9800,0.9935,1.0400,1.0700,1.1000,1.1200,1.1300,1.1370,1.1610,
-      1.1800,1.2000,1.2350,1.2900,1.3200,1.3500,1.3950,1.4425,1.4625,1.4770,
-      1.4970,1.5200,1.5390,1.5580,1.5780,1.5920,1.6100,1.6300,1.6460,1.6780,
-      1.7400,1.8000,1.8600,1.9200,1.9600,1.9850,2.0050,2.0350,2.0650,2.1000,
-      2.1480,2.1980,2.2700,2.3600,2.4500,2.4940,2.5370</td>
-</tr>
-
-</table>
-
-Table 30. Photopic response function.
-
-<table class="table table-striped">
-
-
-
-
-<tr>
-<td>Photopic response function values corresponding to wavelengths in following data block. Based on CIE 1931 observer; ISO/CIE 10527, CIE Standard Calorimetric Observers; derived from Optics5 data file &quot;CIE 1931 Color Match from E308.txt&quot;, which is the same as WINDOW4 file Cie31t.dat.</td>
-</tr>
-<tr>
-<td>      0.0000,0.0001,0.0001,0.0002,0.0004,0.0006,0.0012,0.0022,0.0040,0.0073,
-      0.0116,0.0168,0.0230,0.0298,0.0380,0.0480,0.0600,0.0739,0.0910,0.1126,
-      0.1390,0.1693,0.2080,0.2586,0.3230,0.4073,0.5030,0.6082,0.7100,0.7932,
-      0.8620,0.9149,0.9540,0.9803,0.9950,1.0000,0.9950,0.9786,0.9520,0.9154,
-      0.8700,0.8163,0.7570,0.6949,0.6310,0.5668,0.5030,0.4412,0.3810,0.3210,
-      0.2650,0.2170,0.1750,0.1382,0.1070,0.0816,0.0610,0.0446,0.0320,0.0232,
-      0.0170,0.0119,0.0082,0.0158,0.0041,0.0029,0.0021,0.0015,0.0010,0.0007,
-      0.0005,0.0004,0.0002,0.0002,0.0001,0.0001,0.0001,0.0000,0.0000,0.0000,
-      0.0000 /</td>
-</tr>
-<tr>
-<td>Wavelengths (microns) corresponding to above data block</td>
-</tr>
-<tr>
-<td>      .380,.385,.390,.395,.400,.405,.410,.415,.420,.425,
-      .430,.435,.440,.445,.450,.455,.460,.465,.470,.475,
-      .480,.485,.490,.495,.500,.505,.510,.515,.520,.525,
-      .530,.535,.540,.545,.550,.555,.560,.565,.570,.575,
-      .580,.585,.590,.595,.600,.605,.610,.615,.620,.625,
-      .630,.635,.640,.645,.650,.655,.660,.665,.670,.675,
-      .680,.685,.690,.695,.700,.705,.710,.715,.720,.725,
-      .730,.735,.740,.745,.750,.755,.760,.765,.770,.775,
-      .780</td>
-</tr>
-
-</table>
-
-### Calculation of Angular Properties
-
-Calculation of optical properties is divided into two categories: uncoated glass and coated glass.
-
-#### Angular Properties for Uncoated Glass
-
-The following discussion assumes that optical quantities such as transmissivity, reflectvity, absorptivity, and index of refraction are a function of wavelength, λ. If there are no spectral data the angular dependence is calculated based on the single values for transmittance and reflectance in the visible and solar range. In the visible range an average wavelength of 0.575 microns is used in the calculations. In the solar range an average wavelength of 0.898 microns is used.
-
-The spectral data include the transmittance, *T*, and the reflectance, *R*. For uncoated glass the reflectance is the same for the front and back surfaces. For angle of incidence, <span>\(\phi \)</span>, the transmittance and reflectance are related to the transmissivity, τ,and reflectivity, �, by the following relationships:
-
-<div>$$T(\phi ) = \frac{{\tau {{(\phi )}^2}{e^{ - \alpha d/\cos \phi '}}}}{{1 - \rho {{(\phi )}^2}{e^{ - 2\alpha d/\cos \phi '}}}}$$</div>
-
-<div>$$R(\phi ) = \rho (\phi )\left( {1 + T(\phi ){e^{ - \alpha d/\cos \phi '}}} \right)$$</div>
-
-The spectral reflectivity is calculated from Fresnel’s equation assuming unpolarized incident radiation:
-
-<div>$$\rho (\phi ) = \frac{1}{2}\left( {{{\left( {\frac{{n\cos \phi  - \cos \phi '}}{{n\cos \phi  + \cos \phi '}}} \right)}^2} + {{\left( {\frac{{n\cos \phi ' - \cos \phi }}{{n\cos \phi ' + \cos \phi }}} \right)}^2}} \right)$$</div>
-
-The spectral transmittivity is given by
-
-<div>$$\tau (\phi ) = 1 - \rho (\phi )$$</div>
-
-The spectral absorption coefficient is defined as
-
-<div>$$\alpha  = 4\pi \kappa /\lambda $$</div>
-
-where κ is the dimensionless spectrally-dependent extinction coefficient and λ is the wavelength expressed in the same units as the sample thickness.
-
-Solving Eq. at normal incidence gives
-
-<div>$$n = \frac{{1 + \sqrt {\rho (0)} }}{{1 - \sqrt {\rho (0)} }}$$</div>
-
-Evaluating Eq. at normal incidence gives the following expression for *κ*
-
-<div>$$\kappa  =  - \frac{\lambda }{{4\pi d}}\ln \frac{{R(0) - \rho (0)}}{{\rho (0)T(0)}}$$</div>
-
-Eliminating the exponential in Eqs. and  gives the reflectivity at normal incidence:
-
-<div>$$\rho (0) = \frac{{\beta  - \sqrt {{\beta ^2} - 4(2 - R(0))R(0)} }}{{2(2 - R(0))}}$$</div>
-
-where
-
-<div>$$\beta  = T{(0)^2} - R{(0)^2} + 2R(0) + 1$$</div>
-
-The value for the reflectivity, *�*(0),from Eq. is substituted into Eqs. and . The result from Eq. is used to calculate the absorption coefficient in Eq. . The index of refraction is used to calculate the reflectivity in Eq. which is then used to calculate the transmittivity in Eq. . The reflectivity, transmissivity and absorption coefficient are then substituted into Eqs. and to obtain the angular values of the reflectance and transmittance.
-
-#### Angular Properties for Coated Glass
-
-A regression fit is used to calculate the angular properties of coated glass from properties at normal incidence. If the transmittance of the coated glass is &gt; 0.645, the angular dependence of uncoated clear glass is used. If the transmittance of the coated glass is ≤ 0.645, the angular dependence of uncoated bronze glass is used. The values for the angular functions for the transmittance and reflectance of both clear glass <span>\(({\bar \tau_{clr}},{\bar \rho_{clr}})\)</span> and bronze glass <span>\(({\bar \tau_{bnz}},{\bar \rho_{bnz}})\)</span>are determined from a fourth-order polynomial regression:
-
-<div>$$\bar \tau (\phi ) = {\bar \tau_0} + {\bar \tau_1}\cos (\phi ) + {\bar \tau_2}{\cos ^2}(\phi ) + {\bar \tau_3}{\cos ^3}(\phi ) + {\bar \tau_4}{\cos ^4}(\phi )$$</div>
-
-and
-
-<div>$$\bar \rho (\phi ) = {\bar \rho_0} + {\bar \rho_1}\cos (\phi ) + {\bar \rho_2}{\cos ^2}(\phi ) + {\bar \rho_3}{\cos ^3}(\phi ) + {\bar \rho_4}{\cos ^4}(\phi ) - \bar \tau (\phi )$$</div>
-
-The polynomial coefficients are given in Table 31.
-
-Table 31. Polynomial coefficients used to determine angular properties of coated glass.
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>0</th>
-<th>1</th>
-<th>2</th>
-<th>3</th>
-<th>4</th>
-</tr>
-<tr>
-<td><span>\({\bar \tau_{clr}}\)</span></td>
-<td>-0.0015</td>
-<td>3.355</td>
-<td>-3.840</td>
-<td>1.460</td>
-<td>0.0288</td>
-</tr>
-<tr>
-<td><span>\({\bar \rho_{clr}}\)</span></td>
-<td>0.999</td>
-<td>-0.563</td>
-<td>2.043</td>
-<td>-2.532</td>
-<td>1.054</td>
-</tr>
-<tr>
-<td><span>\({\bar \tau_{bnz}}\)</span></td>
-<td>-0.002</td>
-<td>2.813</td>
-<td>-2.341</td>
-<td>-0.05725</td>
-<td>0.599</td>
-</tr>
-<tr>
-<td><span>\({\bar \rho_{bnz}}\)</span></td>
-<td>0.997</td>
-<td>-1.868</td>
-<td>6.513</td>
-<td>-7.862</td>
-<td>3.225</td>
-</tr>
-
-</table>
-
-These factors are used as follows to calculate the angular transmittance and reflectance:
-
-For *T*(0) &gt; 0.645:
-
-<div>$$T(\phi ) = T(0){\bar \tau_{clr}}(\phi )$$</div>
-
-<div>$$R(\phi ) = R(0)(1 - {\bar \rho_{clr}}(\phi )) + {\bar \rho_{clr}}(\phi )$$</div>
-
-For *T*(0) ≤ 0.645:
-
-<div>$$T(\phi ) = T(0){\bar \tau_{bnz}}(\phi )$$</div>
-
-<div>$$R(\phi ) = R(0)(1 - {\bar \rho_{bnz}}(\phi )) + {\bar \rho_{bnz}}(\phi )$$</div>
-
-#### Angular Properties for Simple Glazing Systems
-
-When the glazing system is modeled using the simplified method, an alternate method is used to determine the angular properties.  The equation for solar transmittance as a function of incidence angle, <span>\(T\left( \phi  \right)\)</span>, is,
-
-<div>$$T\left( \phi  \right) = T\left( {\phi  = 0} \right)\,\cos \left( \phi  \right)\,\,\left( {1 + (0.768 + 0.817\,SHG{C^4})\;{{\sin }^3}\left( \phi  \right)} \right)$$</div>
-
-where,
-
-<span>\(T\left( {\phi  = 0} \right)\)</span> is the normal incidence solar transmittance, <span>\({T_{Sol}}\)</span>.
-
-The equation for solar reflectance as a function of incidence angle,  <span>\(R\left( \phi  \right)\)</span>, is,
-
-<div>$$R\left( \phi  \right) = \frac{{R\left( {\phi  = 0} \right)\left( {{f_1}\left( \phi  \right) + {f_2}\left( \phi  \right)\sqrt {SHGC} } \right)}}{{{R_{fit,o}}}}$$</div>
-
-where,
-
-<div>$${f_1}\left( \phi  \right) = \left( {\left( {\left( {2.403\cos \left( \phi  \right) - 6.192} \right)\cos \left( \phi  \right) + 5.625} \right)\cos \left( \phi  \right) - 2.095} \right)\cos \left( \phi  \right) + 1$$</div>
-
-<div>$${f_2}\left( \phi  \right) = \left( {\left( {\left( { - 1.188\cos \left( \phi  \right) + 2.022} \right)\cos \left( \phi  \right) + 0.137} \right)\cos \left( \phi  \right) - 1.720} \right)\cos \left( \phi  \right)$$</div>
-
-<div>$${R_{fit,o}} = 0.7413 - \left( {0.7396\;\sqrt {SHGC} } \right)$$</div>
-
-### Calculation of Hemispherical Values
-
-The hemispherical value of a property is determined from the following integral:
-
-<div>$${P_{hemispherical}} = 2\int_0^{\frac{\pi }{2}} {P(\phi )\cos (\phi )\sin (\phi )d\phi } $$</div>
-
-The integral is evaluated by Simpson’s rule for property values at angles of incidence from 0 to 90 degrees in 10-degree increments.
-
-### Optical Properties of Window Shading Devices
-
-Shading devices affect the system transmittance and glass layer absorptance for short-wave radiation and for long-wave (thermal) radiation. The effect depends on the shade position (interior, exterior or between-glass), its transmittance, and the amount of inter-reflection between the shading device and the glazing. Also of interest is the amount of radiation absorbed by the shading device.
-
-In EnergyPlus, shading devices are divided into four categories, “shades,� �blinds,� “screens,� and “switchable glazing.� “Shades� are assumed to be perfect diffusers. This means that direct radiation incident on the shade is reflected and transmitted as hemispherically uniform diffuse radiation: there is no direct component of transmitted radiation. It is also assumed that the transmittance, *τ<sub>sh</sub>*, reflectance, *�<sub>sh</sub>*, and absorptance, *α<sub>sh</sub>*, are the same for the front and back of the shade and are independent of angle of incidence. Many types of drapery and pull-down roller devices are close to being perfect diffusers and can be categorized as “shades.�
-
-“Blinds� in EnergyPlus are slat-type devices such as venetian blinds. Unlike shades, the optical properties of blinds are strongly dependent on angle of incidence. Also, depending on slat angle and the profile angle of incident direct radiation, some of the direct radiation may pass between the slats, giving a direct component of transmitted radiation.
-
-“Screens� are debris or insect protection devices made up of metallic or non-metallic materials. Screens may also be used as shading devices for large glazing areas where excessive solar gain is an issue. The EnergyPlus window screen model assumes the screen is composed of intersecting orthogonally-crossed cylinders, with the surface of the cylinders assumed to be diffusely reflecting. Screens may only be used on the exterior surface of a window construction. As with blinds, the optical properties affecting the direct component of transmitted radiation are dependent on the angle of incident direct radiation.
-
-With “Switchable glazing,� shading is achieved making the glazing more absorbing or more reflecting, usually by an electrical or chemical mechanism. An example is electrochromic glazing where the application of an electrical voltage or current causes the glazing to switch from light to dark.
-
-Shades and blinds can be either fixed or moveable. If moveable, they can be deployed according to a schedule or according to a trigger variable, such as solar radiation incident on the window. Screens can be either fixed or moveable according to a schedule.
-
-#### Shades
-
-#### Shade/Glazing System Properties for Short-Wave Radiation
-
-Short-wave radiation includes
-
-1)   Beam solar radiation from the sun and diffuse solar radiation from the sky and ground incident on the outside of the window,
-
-2)   Beam and/or diffuse radiation reflected from exterior obstructions or the building itself,
-
-3)   Solar radiation reflected from the inside zone surfaces and incident as diffuse radiation on the inside of the window,
-
-4)   Beam solar radiation from one exterior window incident on the inside of another window in the same zone, and
-
-5)   Short-wave radiation from electric lights incident as diffuse radiation on the inside of the window.
-
-**Exterior Shade**
-
-For an exterior shade we have the following expressions for the system transmittance, the effective system glass layer absorptance, and the system shade absorptance, taking inter-reflection between shade and glazing into account. Here, “system� refers to the combination of glazing and shade. The system properties are given in terms of the isolated shade properties (i.e., shade properties in the absence of the glazing) and the isolated glazing properties (i.e., glazing properties in the absence of the shade).
-
-<div>$${T_{sys}}(\phi ) = T_{1,N}^{dif}\frac{{{\tau_{sh}}}}{{1 - R_f^{dif}{\rho_{sh}}}}$$</div>
-
-<div>$$T_{sys}^{dif} = T_{1,N}^{dif}\frac{{{\tau_{sh}}}}{{1 - R_f^{dif}{\rho_{sh}}}}$$</div>
-
-<div>$$A_{j,f}^{sys}(\phi ) = A_{j,f}^{dif}\frac{{{\tau_{sh}}}}{{1 - {R_f}{\rho_{sh}}}},\quad j = 1{\rm{to}}N$$</div>
-
-<div>$$A_{j,f}^{dif,sys} = A_{j,f}^{dif}\frac{{{\tau_{sh}}}}{{1 - {R_f}{\rho_{sh}}}},\quad j = 1{\rm{ to }}N$$</div>
-
-<div>$$A_{j,b}^{dif,sys} = A_{j,b}^{dif}\frac{{T_{1,N}^{dif}{\rho_{sh}}}}{{1 - {R_f}{\rho_{sh}}}},\quad j = 1{\rm{ to }}N$$</div>
-
-<div>$$\alpha_{sh}^{sys} = {\alpha_{sh}}\left( {1 + \frac{{{\tau_{sh}}{R_f}}}{{1 - {R_f}{\rho_{sh}}}}} \right)$$</div>
-
-**Interior Shade**
-
-The system properties when an interior shade is in place are the following.
-
-<div>$${T_{sys}}(\phi ) = T_{1,N}^{}(\phi )\frac{{{\tau_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}$$</div>
-
-<div>$$T_{sys}^{dif} = T_{1,N}^{dif}\frac{{{\tau_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}$$</div>
-
-<div>$$A_{j,f}^{sys}(\phi ) = {A_{j,f}}(\phi ) + {T_{1,N}}(\phi )\frac{{{\rho_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}A_{j,b}^{dif},\quad j = 1{\rm{ to }}N$$</div>
-
-<div>$$A_{j,f}^{dif,sys} = A_{j,f}^{dif} + T_{1,N}^{dif}\frac{{{\rho_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}A_{j,b}^{dif},\quad j = 1{\rm{ to }}N$$</div>
-
-<div>$$A_{j,b}^{dif,sys} = \frac{{{\tau_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}A_{j,b}^{dif},{\rm{    }}j = 1{\rm{ to }}N$$</div>
-
-<div>$$\alpha_{sh}^{sys}(\phi ) = T_{1,N}^{}(\phi )\frac{{{\alpha_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}$$</div>
-
-<div>$$\alpha_{sh}^{dif,sys} = T_{1,N}^{dif}\frac{{{\alpha_{sh}}}}{{1 - R_b^{dif}{\rho_{sh}}}}$$</div>
-
-#### Long-Wave Radiation Properties of Window Shades
-
-Long-wave radiation includes
-
-       Thermal radiation from the sky, ground and exterior obstructions incident on the outside of the window,
-
-       Thermal radiation from other room surfaces incident on the inside of the window, and
-
-       Thermal radiation from internal sources, such as equipment and electric lights, incident on the inside of the window.
-
-The program calculates how much long-wave radiation is absorbed by the shade and by the adjacent glass surface. The system emissivity (thermal absorptance) for an interior or exterior shade, taking into account reflection of long-wave radiation between the glass and shade, is given by
-
-<div>$$\varepsilon_{sh}^{lw,sys} = \varepsilon_{sh}^{lw}\left( {1 + \frac{{\tau_{sh}^{lw}\rho_{gl}^{lw}}}{{1 - \rho_{sh}^{lw}\rho_{gl}^{lw}}}} \right)$$</div>
-
-where <span>\(\rho_{gl}^{lw}\)</span>is the long-wave reflectance of the outermost glass surface for an exterior shade or the innermost glass surface for an interior shade, and it is assumed that the long-wave transmittance of the glass is zero.
-
-The innermost (for interior shade) or outermost (for exterior shade) glass surface emissivity when the shade is present is
-
-<div>$$\varepsilon_{gl}^{lw,sys} = \varepsilon_{gl}^{lw}\frac{{\tau_{sh}^{lw}}}{{1 - \rho_{sh}^{lw}\rho_{gl}^{lw}}}$$</div>
-
-#### Switchable Glazing
-
-For switchable glazing, such as electrochromics, the solar and visible optical properties of the glazing can switch from a light state to a dark state. The switching factor, *f<sub>switch</sub>*, determines what state the glazing is in. An optical property, *p*, such as transmittance or glass layer absorptance, for this state is given by
-
-<div>$$p = (1 - {f_{switch}}){p_{light}} + {f_{switch}}{p_{dark}}$$</div>
-
-where
-
-*p<sub>light</sub>*is the property value for the unswitched, or light state, and *p<sub>dark</sub>* is the property value for the fully switched, or dark state.
-
-The value of the switching factor in a particular time step depends on what type of switching control has been specified: “schedule,� “trigger,� or “daylighting.� If “schedule,� *f<sub>switch</sub>* = schedule value, which can be 0 or 1.
-
-### Thermochromic Windows
-
-Thermochromic (TC) materials have active, reversible optical properties that vary with temperature. Thermochromic windows are adaptive window systems for incorporation into building envelopes. Thermochromic windows respond by absorbing sunlight and turning the sunlight energy into heat. As the thermochromic film warms it changes its light transmission level from less absorbing to more absorbing. The more sunlight it absorbs the lower the light level going through it. Figure 78 shows the variations of window properties with the temperature of the thermochromic glazing layer. By using the suns own energy the window adapts based solely on the directness and amount of sunlight. Thermochromic materials will normally reduce optical transparency by absorption and/or reflection, and are specular (maintaining vision).
-
-![](media/image1015.svg.png)
-
-Figure 78. Variations of Window Properties with the Temperature of the Thermochromic Glazing Layer
-
-On cloudy days the window is at full transmission and letting in diffuse daylighting. On sunny days the window maximizes diffuse daylighting and tints based on the angle of the sun relative to the window. For a south facing window (northern hemisphere) the daylight early and late in the day is maximized and the direct sun at mid day is minimized.
-
-The active thermochromic material can be embodied within a laminate layer or a surface film. The overall optical state of the window at a given time is a function primarily of
-
-* thermochromic material properties
-
-* solar energy incident on the window
-
-* construction of the window system that incorporates the thermochromic layer
-
-* environmental conditions (interior, exterior, air temperature, wind, etc).
-
-The tinted film, in combination with a heat reflecting, low-e layer allows the window to reject most of the absorbed radiation thus reducing undesirable heat load in a building. In the absence of direct sunlight the window cools and clears and again allows lower intensity diffuse radiation into a building. TC windows can be designed in several ways (Figure 79), with the most common being a triple pane windows with the TC glass layer in the middle a double pane windows with the TC layer on the inner surface of the outer pane or for sloped glazing a double pane with the laminate layer on the inner pane with a low-e layer toward the interior. The TC glass layer has variable optical properties depending on its temperature, with a lower temperature at which the optical change is initiated, and an upper temperature at which a minimum transmittance is reached. TC windows act as passive solar shading devices without the need for sensors, controls and power supplies but their optical performance is dependent on varying solar and other environmental conditions at the location of the window.
-
-![](media/image1017.png)
-
-Figure 79. Configurations of Thermochromic Windows
-
-EnergyPlus describes a thermochromic window with a Construction object which references a special layer defined with a WindowMaterial:GlazingGroup:Thermochromic object. The WindowMaterial:GlazingGroup:Thermochromic object further references a series of WindowMaterial:Glazing objects corresponding to each specification temperature of the TC layer. During EnergyPlus run time, a series of TC windows corresponding to each specification temperature is created once. At the beginning of a particular time step calculations, the temperature of the TC glass layer from the previous time step is used to look up the most closed specification temperature whose corresponding TC window construction will be used for the current time step calculations. The current time step calculated temperature of the TC glass layer can be different from the previous time step, but no iterations are done in the current time step for the new TC glass layer temperature. This is an approximation that considers the reaction time of the TC glass layer can be close to EnergyPlus simulation time step say 10 to 15 minutes.
-
-#### Blinds
-
-Window blinds in EnergyPlus are defined as a series of equidistant slats that are oriented horizontally or vertically. All of the slats are assumed to have the same optical properties. The overall optical properties of the blind are determined by the slat geometry (width, separation and angle) and the slat optical properties (front-side and back-side transmittance and reflectance). Blind properties for direct radiation are also sensitive to the “profile angle,� which is the angle of incidence in a plane that is perpendicular to the window plane and to the direction of the slats. The blind optical model in EnergyPlus is based on Simmler, Fischer and Winkelmann, 1996; however, that document has numerous typographical errors and should be used with caution.
-
-The following assumptions are made in calculating the blind optical properties:
-
-* The slats are flat.
-
-* The spectral dependence of inter-reflections between slats and glazing is ignored; spectral-average slat optical properties are used.
-
-* The slats are perfect diffusers. They have a perfectly matte finish so that reflection from a slat is isotropic (hemispherically uniform) and independent of angle of incidence, i.e., the reflection has no specular component. This also means that absorption by the slats is hemispherically uniform with no incidence angle dependence. If the transmittance of a slat is non-zero, the transmitted radiation is isotropic and the transmittance is independent of angle of incidence.
-
-* Inter-reflection between the blind and wall elements near the periphery of the blind is ignored.
-
-* If the slats have holes through which support strings pass, the holes and strings are ignored. Any other structures that support or move the slats are ignored.
-
-#### Slat Optical Properties
-
-The slat optical properties used by EnergyPlus are shown in the following table.
-
-Table 32.  Slat Optical Properties
-
-<table class="table table-striped">
-<tr>
-<td><span>\({\tau_{dir,dif}}\)</span>
- </td>
-<td>Direct-to-diffuse transmittance (same for front and back of slat)</td>
-</tr>
-<tr>
-<td><span>\({\tau_{dif,dif}}\)</span>
- </td>
-<td>Diffuse-to-diffuse transmittance (same for front and back of slat)</td>
-</tr>
-<tr>
-<td><span>\(\rho_{dir,dif}^f{\rm{ , }}\rho_{dir,dif}^b\)</span>
- </td>
-<td>Front and back direct-to-diffuse reflectance</td>
-</tr>
-<tr>
-<td><span>\(\rho_{dif,dif}^f{\rm{ , }}\rho_{dif,dif}^b\)</span></td>
-<td>Front and back diffuse-to-diffuse reflectance</td>
-</tr>
-
-</table>
-
-It is assumed that there is no direct-to-direct transmission or reflection, so that <span>\({\tau_{dir,dir}} = 0\)</span>, <span>\(\rho_{dir,dir}^f = 0\)</span>, and <span>\(\rho_{dir,dir}^b = 0\)</span>. It is further assumed that the slats are perfect diffusers, so that <span>\({\tau_{dir,dif}}\)</span>, <span>\(\rho_{dir,dif}^f\)</span>and <span>\(\rho_{dir,dif}^b\)</span>are independent of angle of incidence. Until the EnergyPlus model is improved to take into account the angle-of-incidence dependence of slat transmission and reflection, it is assumed that <span>\({\tau_{dir,dif}}\)</span>= <span>\({\tau_{dif,dif}}\)</span>, <span>\(\rho_{dir,dif}^f\)</span>=<span>\(\rho_{dif,dif}^f\)</span>, and <span>\(\rho_{dir,dif}^b\)</span>=<span>\(\rho_{dif,dif}^b\)</span>.
-
-#### Direct Transmittance of Blind
-
-The direct-to-direct and direct-to-diffuse transmittance of a blind is calculated using the slat geometry shown in Figure 80 (a), which shows the side view of one of the cells of the blind. For the case shown, each slat is divided into two segments, so that the cell is bounded by a total of six segments, denoted by *s<sub>1</sub>* through *s<sub>6</sub>* (note in the following that *s<sub>i</sub>* refers to both segment *i* and the length of segment *i)*.The lengths of *s<sub>1</sub>* and *s<sub>2</sub>* are equal to the slat separation, *h*, which is the distance between adjacent slat faces. *s<sub>3</sub>* and *s<sub>4</sub>* are the segments illuminated by direct radiation. In the case shown in Figure 80 (a) the cell receives radiation by reflection of the direct radiation incident on *s<sub>4</sub>* and, if the slats have non-zero transmittance, by transmission through *s<sub>3</sub>*, which is illuminated from above.
-
-The goal of the blind direct transmission calculation is to determine the direct and diffuse radiation leaving the cell through *s<sub>2</sub>* for unit direct radiation entering the cell through *s<sub>1</sub>*.
-
-![](media/image1034.png)
-
-Figure 80. (a) Side view of a cell formed by adjacent slats showing how the cell is divided into segments, *s<sub>i</sub>*,  for the calculation of direct solar transmittance; (b) side view of a cell showing case where some of the direct solar passes between adjacent slats without touching either of them. In this figure φ<sub>s</sub> is the profile angle and φ<sub>b</sub> is the slat angle.
-
-#### Direct-to-Direct Blind Transmittance
-
-Figure 80 (b) shows the case where some of the direct radiation passes through the cell without hitting the slats. From the geometry in this figure we see that
-
-<div>$$\tau_{bl,f}^{dir,dir} = 1 - \frac{{|w|}}{h},{\rm{       }}|w|{\rm{ }} \le {\rm{ }}h$$</div>
-
-where
-
-<div>$$w = s\frac{{\cos ({\varphi_b} - {\varphi_s})}}{{\cos {\varphi_s}}}$$</div>
-
-Note that we are assuming that the slat thickness is zero. A correction for non-zero slat thickness is described later.
-
-#### Direct-to-Diffuse Blind Transmittance, Reflectance and Absorptance
-
-The direct-to-diffuse and transmittance and reflectance of the blind are calculated using a radiosity method that involves the following three vector quantities:
-
-*J<sub>i</sub>* = the radiosity of segment *s<sub>i</sub>*, i.e., the total radiant flux into the cell from  *s<sub>i</sub>*
-
-*G<sub>i</sub>*= the irradiance on the cell side of *s<sub>i</sub>*
-
-*Q<sub>i</sub>*= the source flux from the cell side of s*<sub>i</sub>*
-
-Based on these definitions we have the following equations that relate *J*, *G* and *Q* for the different segments:
-
-<div>$$
-  \begin{array}{rl}
-   J_1 &= Q_1 \\
-   J_2 &= Q_2 \\
-   J_3 &= Q_3 + \rho_{dif,dif}^b G_3 + \tau_{dif,dif} G_4 \\
-   J_4 &= Q_4 + \tau_{dif,dif} G_3 + \rho_{dif,dif}^f G_4 \\
-   J_5 &= Q_5 + \rho_{dif,dif}^b G_5 + \tau_{dif,dif} G_6 \\
-   J_6 &= Q_6 + \tau_{dif,dif} G_5 + \rho_{dif,dif}^f G_6
-  \end{array}
-$$</div>
-
-In addition we have the following equation relating *G* and* J*:
-
-<div>$${G_i} = \sum\limits_{j = 1}^6 {{J_j}{F_{ji}}{\rm{ ,    }}i = 1,6} $$</div>
-
-where <span>\({F_{ji}}\)</span>is the view factor between <span>\({s_j}\)</span>and <span>\({s_i}\)</span>, i.e., <span>\({F_{ji}}\)</span>is the fraction of radiation leaving <span>\({s_j}\)</span>that is intercepted by <span>\({s_i}\)</span>.
-
-Using <span>\({J_1} = {Q_1} = 0\)</span>and <span>\({J_2} = {Q_2} = 0\)</span> and combining the above equations gives the following equation set relating* J* and* Q*:
-
-<div>$${J_3} - \rho_{dif,dif}^b\sum\limits_{j = 3}^6 {{J_j}{F_{j3}} - {\tau_{dif,dif}}\sum\limits_{j = 3}^6 {{J_j}{F_{j4}} = {Q_3}} } $$</div>
-
-<div>$${J_4} - \tau_{dif,dif}^{}\sum\limits_{j = 3}^6 {{J_j}{F_{j3}} - \rho_{dif,dif}^f\sum\limits_{j = 3}^6 {{J_j}{F_{j4}} = {Q_4}} } $$</div>
-
-<div>$${J_5} - \rho_{dif,dif}^b\sum\limits_{j = 3}^6 {{J_j}{F_{j5}} - {\tau_{dif,dif}}\sum\limits_{j = 3}^6 {{J_j}{F_{j6}} = {Q_5}} } $$</div>
-
-<div>$${J_6} - \tau_{dif,dif}^{}\sum\limits_{j = 3}^6 {{J_j}{F_{j3}} - \rho_{dif,dif}^f\sum\limits_{j = 3}^6 {{J_j}{F_{j6}} = {Q_6}} } $$</div>
-
-This can be written in the form
-
-<div>$$Q' = XJ'$$</div>
-
-where *X* is a 4x4 matrix and
-
-<div>$$
-  J' = \left[ \begin{array}
-   J_3 \\
-   J_4 \\
-   J_5 \\
-   J_6 \end{array} \right]
-$$</div>  
-  
-<div>$$
-  Q' = \left[ \begin{array}
-    Q_3 \\
-    Q_4 \\
-    Q_5 \\
-    Q_6 \end{array} \right]
-$$</div>
-
-We then obtain <span>\(J'\)</span> from
-
-<div>$$J' = {X^{ - 1}}Q'$$</div>
-
-The view factors, <span>\({F_{ij}}\)</span>, are obtained as follows. The cell we are dealing with is a convex polygon with *n* sides. In such a polygon the view factors must satisfy the following constraints:
-
-<div>$$\sum\limits_{j = 1}^n {{F_{ij}} = 1{\rm{,  }}i = 1,n} $$</div>
-
-<div>$${s_i}{F_{ij}} = {s_j}{F_{ji}}{\rm{,  }}i = 1,n{\rm{;  }}j = 1,n$$</div>
-
-<div>$${F_{ii}} = 0{\rm{,  }}i = 1,n$$</div>
-
-These constraints lead to simple equations for the view factors for* n* = 3 and 4. For *n* = 3, we have the following geometry and view factor expression:
-
-![WindowHB\_1](media/image1059.png)
-
-For  *n* = 4  we have:
-
-![WindowHB\_2](media/image1060.png)
-
-Applying these to the slat cell shown in Figure 81 we have the following:
-
-<div>$${F_{12}} = \frac{{{d_1} + {d_2} - 2s}}{{2h}}$$</div>
-
-<div>$${F_{13}} = \frac{{h + {s_3} - {d_3}}}{{2h}}{\rm{ ,  etc}}{\rm{.}}$$</div>
-
-![](media/image1063.png)
-
-Figure 81. Slat cell showing geometry for calculation of view factors between the segments of the cell.
-
-The sources for the direct-to-diffuse transmittance calculation are:
-
-<div>$${Q_1} = {Q_2} = {Q_5} = {Q_6} = 0 \;  (and therefore) {J_1} = {J_2} = 0$$</div>
-
-<div>$$
-  \left. 
-    \begin{array}{l}
-      Q_3 = \tau_{dir,dif} \\
-      Q_4 = \rho_{dir,dif}^f 
-    \end{array} 
-  \right\} 
-  \;
-  \varphi_b \le \varphi_s + \frac{\pi }{2} 
-  \;
-  \rm{ (beam hits front of slats)}
-$$</div>
-
-<div>$$
-  \left.
-    \begin{array}{l}
-      Q_3 = \rho_{dir,dif}^b \\
-      Q_4 = \tau_{dir,dif}
-    \end{array}
-  \right\}
-  \;
-  \varphi_b \gt \varphi_s + \frac{\pi }{2}
-  \;
-  \rm{ (beam hits back of slats)}
-$$</div>
-
-For unit incident direct flux, the front direct-to-diffuse transmittance and reflectance of the blind are:
-
-<div>$$\begin{array}{l}\tau_{bl,f}^{dir,dif} = {G_2}\\\rho_{bl,f}^{dir,dif} = {G_1}\end{array}$$</div>
-
-where
-
-<div>$$
-  \begin{array}{l}
-    G_2 = \sum_{j=3}^6 J_j F_{j2} \\
-    G_1 = \sum_{j=3}^6 J_j F_{j1} 
-  \end{array}
-$$</div>
-
-and <span>\({J_3}\)</span>to <span>\({J_6}\)</span>are given by Eq. .  
-
-The front direct absorptance of the blind is then
-
-<div>$$\alpha_{bl,f}^{dir} = 1 - \tau_{bl,f}^{dir,dif} - \tau_{bl,f}^{dir,dir} - \rho_{bl,f}^{dir,dif}$$</div>
-
-The direct-to-diffuse calculations are performed separately for solar and visible slat properties to get the corresponding solar and visible blind properties.
-
-#### Dependence on Profile Angle
-
-The direct-to-direct and direct-to-diffuse blind properties are calculated for direct radiation profile angles (see Figure 80) ranging from –90<sup>O</sup> to +90<sup>O</sup> in 5<sup>O</sup> increments. (The “profile angle� is the angle of incidence in a plane that is perpendicular to the window *and* perpendicular to the slat direction.) In the time step loop the blind properties for a particular profile angle are obtained by interpolation.
-
-#### Dependence on Slat Angle
-
-All blind properties are calculated for slat angles ranging from –90<sup>O</sup> to +90<sup>O</sup> in 10<sup>O</sup> increments. In the time-step loop the slat angle is determined by the slat-angle control mechanism and then the blind properties at that slat angle are determined by interpolation. Three slat-angle controls are available: (1) slat angle is adjusted to just block beam solar incident on the window; (2) slat angle is determined by a schedule; and (3) slat angle is fixed.
-
-#### Diffuse-to-Diffuse Transmittance and Reflectance of Blind
-
-To calculate the diffuse-to-diffuse properties, assuming uniformly distributed incident diffuse radiation, each slat bounding the cell is divided into two segments of equal length (Figure 82), i.e., <span>\({s_3} = {s_4}\)</span>and <span>\({s_5} = {s_6}\)</span>.  For front-side properties we have a unit source, <span>\({Q_1} = 1\)</span>.  All the other <span>\({Q_i}\)</span>are zero. Using this source value, we apply the methodology described above to obtain *G<sub>2</sub>*and *G<sub>1</sub>*. We then have
-
-<div>$$\begin{array}{l}\tau_{bl,f}^{dif,dif} = {G_2}\\\rho_{bl,f}^{dif,dif} = {G_1}\\\alpha_{bl,f}^{dif} = 1 - \tau_{bl,f}^{dif,dif} - \rho_{bl,f}^{dif,dif}\end{array}$$</div>
-
-The back-side properties are calculated in a similar way by setting *Q<sub>2</sub>* = 1 with the other <span>\({Q_i}\)</span>equal to zero.
-
-The diffuse-to-diffuse calculations are performed separately for solar, visible and IR slat properties to get the corresponding solar, visible and IR blind properties.
-
-![](media/image1078.png)
-
-Figure 82. Slat cell showing arrangement of segments and location of source for calculation of diffuse-to-diffuse optical properties.
-
-#### Blind properties for sky and ground diffuse radiation
-
-For horizontal slats on a vertical window (the most common configuration) the blind diffuse-to-diffuse properties will be sensitve to whether the radiation is incident upward from the ground or downward from the sky (Figure 83). For this reason we also calculate the following solar properties for a blind consisting of horizontal slats in a vertical plane:
-
-<span>\(\tau_{bl,f}^{gnd - dif,dif} = {\rm{ }}\)</span>front transmittance for ground diffuse solar
-
-<span>\(\tau_{bl,f}^{sky - dif,dif} = {\rm{ }}\)</span>front transmittance for sky diffuse solar
-
-<span>\({\rm{ }}\rho_{bl,f}^{gnd - dif,dif} = \)</span>front reflectance for ground diffuse solar
-
-<span>\(\rho_{bl,f}^{sky - dif,dif} = {\rm{ }}\)</span>front reflectance for sky diffuse solar
-
-<span>\(\alpha_{bl,f}^{gnd - dif,dif} = {\rm{ }}\)</span>front absorptance for ground diffuse solar
-
-<span>\(\alpha_{bl,f}^{sky - dif,dif} = {\rm{ }}\)</span>front absorptance for sky diffuse solar
-
-These are obtained by integrating over sky and ground elements, as shown in Figure 83, treating each element as a source of direct radiation of irradiance <span>\(I({\phi_s})\)</span> incident on the blind at profile angle <span>\({\phi_s}\)</span>. This gives:
-
-<div>$$\tau_{bl,f}^{sky - dif,dif} = \frac{{\int\limits_0^{\pi /2} {\left[ {\tau_{bl,f}^{dir,dir}({\phi_s}) + \tau_{bl,f}^{dir,dif}({\phi_s})} \right]{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}{{\int\limits_0^{\pi /2} {{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}$$</div>
-
-<div>$$\rho_{bl,f}^{sky - dif,dif} = \frac{{\int\limits_0^{\pi /2} {\rho_{bl,f}^{dir,dif}{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}{{\int\limits_0^{\pi /2} {{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}$$</div>
-
-<div>$$\alpha_{bl,f}^{sky - dif} = \frac{{\int\limits_0^{\pi /2} {\alpha_{bl,f}^{dir}{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}{{\int\limits_0^{\pi /2} {{I_{sky}}({\phi_s})\cos {\phi_s}d{\phi_s}} }}$$</div>
-
-![](media/image1090.png)
-
-Figure 83.  Side view of horizontal slats in a vertical blind showing geometry for calculating blind transmission, reflection and absorption properties for sky and ground diffuse radiation.
-
-We assume that the sky radiance is uniform. This means that <span>\({I_{sky}}\)</span>is independent of <span>\({\phi_s}\)</span>, giving:
-
-<div>$$\tau_{bl,f}^{sky - dif,dif} = \int\limits_0^{\pi /2} {\left[ {\tau_{bl,f}^{dir,dir} + \tau_{bl,f}^{dir,dif}} \right]\cos {\phi_s}d{\phi_s}} $$</div>
-
-<div>$$\rho_{bl,f}^{sky - dif,dif} = \int\limits_0^{\pi /2} {\rho_{bl,f}^{dir,dif}\cos {\phi_s}d{\phi_s}} $$</div>
-
-<div>$$\alpha_{bl,f}^{sky - dif} = \int\limits_0^{\pi /2} {\alpha_{bl,f}^{dir}\cos {\phi_s}d{\phi_s}} $$</div>
-
-The corresponding ground diffuse quantities are obtained by integrating <span>\({\phi_s}\)</span> from <span>\(- \pi /2\)</span> to 0.
-
-An improvement to this calculation would be to allow the sky radiance distribution to be non-uniform, i.e.,  to depend on sun position and sky conditions, as is done in the detailed daylighting calculation (see “Sky Luminance Distributions� under “Daylight Factor Calculation�).
-
-#### Correction Factor for Slat Thickness
-
-A correction has to be made to the blind transmittance, reflectance and absorptance properties to account for the amount of radiation incident on a blind that is reflected and absorbed by the slat edges (the slats are assumed to be opaque to radiation striking the slat edges). This is illustrated in Figure 84 for the case of direct radiation incident on the blind. The slat cross-section is assumed to be rectangular. The quantity of interest is the fraction, *f<sub>edge</sub>*, of direct radiation incident on the blind that strikes the slat edges. Based on the geometry shown in Figure 84 we see that
-
-<div>$${f_{edge}} = \frac{{t\cos \gamma }}{{\left( {h + \frac{t}{{\cos \xi }}} \right)\cos {\varphi_s}}} = \frac{{t\cos ({\varphi_s} - \xi )}}{{\left( {h + \frac{t}{{\cos \xi }}} \right)\cos {\varphi_s}}} = \frac{{t\sin ({\varphi_b} - {\varphi_s})}}{{\left( {h + \frac{t}{{\sin {\varphi_b}}}} \right)\cos {\varphi_s}}}$$</div>
-
-The edge correction factor for diffuse incident radiation is calculated by averaging this value of *f<sub>edge</sub>* over profile angles, *φ<sub>s</sub>*, from –90<sup>O</sup> to +90<sup>O</sup>.
-
-As an example of how the edge correction factor is applied, the following two equations show how blind front diffuse transmittance and reflectance calculated assuming zero slat thickness are modified by the edge correction factor. It is assumed that the edge transmittance is zero and that the edge reflectance is the same as the slat front reflectance, *�<sub>f</sub>*.
-
-<div>$$\begin{array}{l}\tau_{bl,f}^{dif,dif} \to \tau_{bl,f}^{dif,dif}\left( {1 - {f_{edge}}} \right)\\\rho_{bl,f}^{dif} \to \rho_{bl,f}^{dif}\left( {1 - {f_{edge}}} \right) + {f_{edge}}{\rho_f}\end{array}$$</div>
-
-![](media/image1100.png)
-
-Figure 84. Side view of slats showing geometry for calculation of slat edge correction factor for incident direct radiation.
-
-#### Comparison with ISO 15099 Calculation of Blind Optical Properties
-
-Table 33 compares EnergyPlus and ISO 15099 [2001] calculations of blind optical properties for a variety of profile angles, slat angles and slat optical properties. The ISO 15099 calculation method is similar to that used in EnergyPlus, except that the slats are divided into five equal segments. The ISO 15099 and EnergyPlus results agree to within 12%, except for the solar transmittances for the 10-degree slat angle case. Here the transmittances are small (from 1% to about 5%) but differ by about a factor of up to two between ISO 15099 and EnergyPlus. This indicates that the slats should be divided into more than two segments at small slat angles.
-
-
-
-Table 33. Comparison of blind optical properties calculated with the EnergyPlus and ISO 15099 methods. EnergyPlus values that differ by more than 12% from ISO 15099 values are shown in bold italics.
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="11">Slat Properties</th>
-  </tr>
-  <tr>
-    <td>Separation (m)</td>
-    <td colspan="2">0.012</td>
-    <td colspan="2">0.012</td>
-    <td colspan="2">0.012</td>
-    <td colspan="2">0.012</td>
-    <td colspan="2">0.012</td>
-  </tr>
-  <tr>
-    <td>Width (m)</td>
-    <td colspan="2">0.016</td>
-    <td colspan="2">0.016</td>
-    <td colspan="2">0.016</td>
-    <td colspan="2">0.016</td>
-    <td colspan="2">0.016</td>
-  </tr>
-  <tr>
-    <td>Angle (deg)</td>
-    <td colspan="2">45</td>
-    <td colspan="2">45</td>
-    <td colspan="2">45</td>
-    <td colspan="2">10</td>
-    <td colspan="2">45</td>
-  </tr>
-  <tr>
-    <td>IR transmittance</td>
-    <td colspan="2">0</td>
-    <td colspan="2">0</td>
-    <td colspan="2">0</td>
-    <td colspan="2">0</td>
-    <td colspan="2">0.4</td>
-  </tr>
-  <tr>
-    <td>IR emissivity, front side</td>
-    <td colspan="2">0.9</td>
-    <td colspan="2">0.9</td>
-    <td colspan="2">0.9</td>
-    <td colspan="2">0.9</td>
-    <td colspan="2">0.55</td>
-  </tr>
-  <tr>
-    <td>IR emissivity, back side</td>
-    <td colspan="2">0.9</td>
-    <td colspan="2">0.9</td>
-    <td colspan="2">0.9</td>
-    <td colspan="2">0.9</td>
-    <td colspan="2">0.55</td>
-  </tr>
-  <tr>
-    <td>Solar transmittance</td>
-    <td colspan="2">0</td>
-    <td colspan="2">0</td>
-    <td colspan="2">0</td>
-    <td colspan="2">0</td>
-    <td colspan="2">0.4</td>
-  </tr>
-  <tr>
-    <td>Solar reflectance, front side</td>
-    <td colspan="2">0.7</td>
-    <td colspan="2">0.55</td>
-    <td colspan="2">0.7</td>
-    <td colspan="2">0.7</td>
-    <td colspan="2">0.5</td>
-  </tr>
-  <tr>
-    <td>Solar reflectance, back side</td>
-    <td colspan="2">0.7</td>
-    <td colspan="2">0.55</td>
-    <td colspan="2">0.4</td>
-    <td colspan="2">0.4</td>
-    <td colspan="2">0.5</td>
-  </tr>
-  <tr>
-    <td colspan="11"></td>
-  </tr>
-  <tr>
-    <td>Solar Profile angle (deg)</td>
-    <td>0</td>
-    <td>60</td>
-    <td>0</td>
-    <td>60</td>
-    <td>0</td>
-    <td>60</td>
-    <td>0</td>
-    <td>60</td>
-    <td>0</td>
-    <td>60</td>
-  </tr>
-  <tr>
-    <td colspan="11"></td>
-  </tr>
-  <tr>
-    <td colspan="11">Calculated blind properties (first row = ISO 15099 calculation, second row (in italics) = EnergyPlus calculation)</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Front solar transmittance, direct to Direct</td>
-    <td>0.057</td>
-    <td>0</td>
-    <td>0.057</td>
-    <td>0</td>
-    <td>0.057</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0.057</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>0.057</td>
-    <td>0</td>
-    <td>0.057</td>
-    <td>0</td>
-    <td>0.057</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0.057</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Back solar transmittance, direct to direct</td>
-    <td>0.057</td>
-    <td>0.31</td>
-    <td>0.057</td>
-    <td>0.31</td>
-    <td>0.057</td>
-    <td>0.31</td>
-    <td>0</td>
-    <td>0.088</td>
-    <td>0.057</td>
-    <td>0.31</td>
-  </tr>
-  <tr>
-    <td>0.057</td>
-    <td>0.309</td>
-    <td>0.057</td>
-    <td>0.309</td>
-    <td>0.057</td>
-    <td>0.309</td>
-    <td>0</td>
-    <td>0.087</td>
-    <td>0.057</td>
-    <td>0.309</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Front solar transmittance, direct to diffuse</td>
-    <td>0.141</td>
-    <td>0.073</td>
-    <td>0.09</td>
-    <td>0.047</td>
-    <td>0.096</td>
-    <td>0.051</td>
-    <td>0.012</td>
-    <td>0.005</td>
-    <td>0.373</td>
-    <td>0.277</td>
-  </tr>
-  <tr>
-    <td>0.155</td>
-    <td>0.074</td>
-    <td>0.1</td>
-    <td>0.048</td>
-    <td>0.104</td>
-    <td>0.051</td>
-    <td>0.019</td>
-    <td>0.006</td>
-    <td>0.375</td>
-    <td>0.275</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Back solar transmittance, direct to diffuse</td>
-    <td>0.141</td>
-    <td>0.288</td>
-    <td>0.09</td>
-    <td>0.216</td>
-    <td>0.076</td>
-    <td>0.271</td>
-    <td>0.011</td>
-    <td>0.027</td>
-    <td>0.373</td>
-    <td>0.306</td>
-  </tr>
-  <tr>
-    <td>0.155</td>
-    <td>0.284</td>
-    <td>0.1</td>
-    <td>0.214</td>
-    <td>0.085</td>
-    <td>0.269</td>
-    <td>0.019</td>
-    <td>0.052</td>
-    <td>0.375</td>
-    <td>0.304</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Front solar reflectance, direct to diffuse</td>
-    <td>0.394</td>
-    <td>0.558</td>
-    <td>0.295</td>
-    <td>0.43</td>
-    <td>0.371</td>
-    <td>0.544</td>
-    <td>0.622</td>
-    <td>0.678</td>
-    <td>0.418</td>
-    <td>0.567</td>
-  </tr>
-  <tr>
-    <td>0.389</td>
-    <td>0.558</td>
-    <td>0.293</td>
-    <td>0.431</td>
-    <td>0.368</td>
-    <td>0.546</td>
-    <td>0.636</td>
-    <td>0.679</td>
-    <td>0.416</td>
-    <td>0.568</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Back solar reflectance, direct to diffuse</td>
-    <td>0.394</td>
-    <td>0.103</td>
-    <td>0.295</td>
-    <td>0.066</td>
-    <td>0.216</td>
-    <td>0.07</td>
-    <td>0.356</td>
-    <td>0.273</td>
-    <td>0.418</td>
-    <td>0.273</td>
-  </tr>
-  <tr>
-    <td>0.389</td>
-    <td>0.115</td>
-    <td>0.293</td>
-    <td>0.074</td>
-    <td>0.214</td>
-    <td>0.077</td>
-    <td>0.363</td>
-    <td>0.272</td>
-    <td>0.416</td>
-    <td>0.275</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Front solar transmittance, hemispherical diffuse to diffuse</td>
-    <td>0.332</td>
-    <td></td>
-    <td>0.294</td>
-    <td></td>
-    <td>0.291</td>
-    <td></td>
-    <td>0.038</td>
-    <td></td>
-    <td>0.495</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>0.338</td>
-    <td></td>
-    <td>0.298</td>
-    <td></td>
-    <td>0.295</td>
-    <td></td>
-    <td>0.053</td>
-    <td></td>
-    <td>0.502</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td rowspan="2">Back solar transmittance, hemispherical diffuse to diffuse</td>
-    <td>0.332</td>
-    <td></td>
-    <td>0.294</td>
-    <td></td>
-    <td>0.291</td>
-    <td></td>
-    <td>0.038</td>
-    <td></td>
-    <td>0.495</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>0.338</td>
-    <td></td>
-    <td>0.298</td>
-    <td></td>
-    <td>0.295</td>
-    <td></td>
-    <td>0.053</td>
-    <td></td>
-    <td>0.502</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td rowspan="2">Front hemispherical IR transmittance</td>
-    <td>0.227</td>
-    <td></td>
-    <td>0.227</td>
-    <td></td>
-    <td>0.227</td>
-    <td></td>
-    <td>0.0245</td>
-    <td></td>
-    <td>0.385</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>0.227</td>
-    <td></td>
-    <td>0.227</td>
-    <td></td>
-    <td>0.227</td>
-    <td></td>
-    <td>0.025</td>
-    <td></td>
-    <td>0.387</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td rowspan="2">Back hemispherical IR transmittance</td>
-    <td>0.227</td>
-    <td></td>
-    <td>0.227</td>
-    <td></td>
-    <td>0.227</td>
-    <td></td>
-    <td>0.0245</td>
-    <td></td>
-    <td>0.385</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>0.227</td>
-    <td></td>
-    <td>0.227</td>
-    <td></td>
-    <td>0.227</td>
-    <td></td>
-    <td>0.025</td>
-    <td></td>
-    <td>0.387</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td rowspan="2">Front hemispherical IR emissivity</td>
-    <td>0.729</td>
-    <td></td>
-    <td>0.729</td>
-    <td></td>
-    <td>0.729</td>
-    <td></td>
-    <td>0.89</td>
-    <td></td>
-    <td>0.536</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>0.73</td>
-    <td></td>
-    <td>0.73</td>
-    <td></td>
-    <td>0.73</td>
-    <td></td>
-    <td>0.895</td>
-    <td></td>
-    <td>0.534</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td rowspan="2">Back hemispherical IR emissivity</td>
-    <td>0.729</td>
-    <td></td>
-    <td>0.729</td>
-    <td></td>
-    <td>0.729</td>
-    <td></td>
-    <td>0.89</td>
-    <td></td>
-    <td>0.536</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>0.73</td>
-    <td></td>
-    <td>0.73</td>
-    <td></td>
-    <td>0.73</td>
-    <td></td>
-    <td>0.895</td>
-    <td></td>
-    <td>0.534</td>
-    <td></td>
-  </tr>
-</table>
-
-#### Blind/Glazing System Properties for Short-Wave Radiation
-
-When a blind is in place we have the following expressions for the system transmittance, the system glass layer absorptance, and the system blind absorptance, taking inter-reflection between blind and glazing into account. The system properties, indicated by “sys,� are given in terms of the isolated blind properties (i.e., blind properties in the absence of the glazing)—indicated by “bl� —and the isolated glazing properties (i.e., glazing properties in the absence of the blind)—indicated by “gl.�
-
-#### Interior Blind
-
-The system properties when an interior blind is in place are the following:
-
-<div>$$T_{f,sys}^{dir,all}(\phi ,{\phi_s}) = T_{gl}^{dir}(\phi )\left( {\tau_{bl,f}^{dir,dir}({\phi_s}) + \tau_{bl,f}^{dir,dif}({\phi_s}) + \frac{{\tau_{bl,f}^{dif}\rho_{bl,f}^{dir,dif}({\phi_s})R_{gl,b}^{dif}}}{{1 - \rho_{bl,f}^{dif}R_{gl,b}^{dif}}}} \right)$$</div>
-
-<div>$$A_{gl,j,f}^{dir,sys}(\phi ,{\phi_s}) = A_{gl,j,f}^{dir}(\phi ) + \frac{{T_{gl}^{dir}(\phi )\alpha_{gl,j,b}^{dif}\rho_{bl,f}^{dir}({\phi_s})}}{{1 - \rho_{bl,f}^{dir}({\phi_s})R_{gl,b}^{dif}}}{\rm{,    }}j = 1,N$$</div>
-
-<div>$$\alpha_{bl,f}^{dir,sys}(\phi ,{\phi_s}) = T_{gl}^{dir}(\phi )\left( {\alpha_{bl,f}^{dir}({\phi_s}) + \frac{{\rho_{bl,f}^{dir}({\phi_s})R_{gl,b}^{dif}\alpha_{bl,f}^{dif}}}{{1 - \rho_{bl,f}^{dif}R_{gl,b}^{dif}}}} \right)$$</div>
-
-<div>$$T_{f,sys}^{dif,dif} = \frac{{T_{gl}^{dif}\tau_{bl,f}^{dif,dif}}}{{1 - \rho_{bl,f}^{dif}R_{gl,b}^{dif}}}$$</div>
-
-
-
-<div>$$T_{f,sys}^{sky - dif,dif} = \frac{{T_{gl}^{dif}\tau_{bl,f}^{sky - dif,dif}}}{{1 - \rho_{bl,f}^{sky - dif}R_{gl,b}^{dif}}}$$</div>
-
-<div>$$T_{f,sys}^{gnd - dif,dif} = \frac{{T_{gl}^{dif}\tau_{bl,f}^{gnd - dif,dif}}}{{1 - \rho_{bl,f}^{gnd - dif}R_{gl,b}^{dif}}}$$</div>
-
-<div>$$A_{gl,j,f}^{dif,sys} = A_{gl,j,f}^{dif} + \frac{{T_{gl}^{dif}\rho_{bl,f}^{dif}A_{gl,j,b}^{dif}}}{{1 - \rho_{bl,f}^{dif}R_{gl,b}^{dif}}}{\rm{,    }}j = 1,N$$</div>
-
-<div>$$A_{gl,j,f}^{sky - dif,sys} = A_{gl,j,f}^{dif} + \frac{{T_{gl}^{dif}\rho_{bl,f}^{sky - dif}A_{gl,j,b}^{dif}}}{{1 - \rho_{bl,f}^{sky - dif}R_{gl,b}^{dif}}}{\rm{,    }}j = 1,N$$</div>
-
-<div>$$A_{gl,j,f}^{gnd - dif,sys} = A_{gl,j,f}^{dif} + \frac{{T_{gl}^{dif}\rho_{bl,f}^{gnd - dif}A_{gl,j,b}^{dif}}}{{1 - \rho_{bl,f}^{gnd - dif}R_{gl,b}^{dif}}}{\rm{,    }}j = 1,N$$</div>
-
-<div>$$\alpha_{bl,f}^{dif,sys} = \frac{{T_{gl}^{dif}\alpha_{bl,f}^{dif}}}{{1 - \rho_{bl,f}^{dif}R_{gl,b}^{dif}}}$$</div>
-
-<div>$$\alpha_{bl,f}^{sky - dif,sys} = \frac{{T_{gl}^{dif}\alpha_{bl,f}^{sky - dif}}}{{1 - \rho_{bl,f}^{sky - dif}R_{gl,b}^{dif}}}$$</div>
-
-<div>$$\alpha_{bl,f}^{gnd - dif,sys} = \frac{{T_{gl}^{dif}\alpha_{bl,f}^{gnd - dif}}}{{1 - \rho_{bl,f}^{gnd - dif}R_{gl,b}^{dif}}}$$</div>
-
-#### Exterior Blind
-
-The system properties when an exterior blind is in place are the following:
-
-<div>$$T_{f,sys}^{dir,all}(\phi ,{\phi_s}) = \tau_{bl,f}^{dir,dir}({\phi_s})\left( {T_{gl}^{dir}(\phi ) + \frac{{T_{gl}^{dif}R_{gl,f}^{dir}\rho_{bl,b}^{dir,dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}} \right) + \frac{{\tau_{bl}^{dir,dif}({\phi_s})T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}$$</div>
-
-<div>$$
-  A_{gl,j,f}^{dir,sys}(\phi ,\phi_s) = 
-     \tau_{bl,f}^{dir,dir}(\phi_s) A_{gl,j,f}^{dir}(\phi ) + 
-     \frac{
-       \left(
-         \tau_{bl,f}^{dir,dir}(\phi_s) R_{gl}^{dir}(\phi) \rho_{bl,b}^{dir}(\phi_s)+ \tau_{bl,f}^{dir,dif}(\phi_s)
-       \right) A_{gl,j,f}^{dif}
-     } {
-       1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}
-     },\;j = 1,N
-$$</div>
-
-<div>$$
-  \alpha_{bl,f}^{dir,sys}(\phi ,\phi_s) = 
-     \alpha_{bl,f}^{dir}(\phi_s) + 
-     \alpha_{bl,b}^{dir}(\phi_s) R_{gl,f}^{dir}(\phi) \tau_{bl,f}^{dir,dir}(\phi_s) + 
-     \frac{
-       \alpha_{bl,b}^{dif}R_{gl,f}^{dif}
-     }{
-       1 - \rho_{bl,b}^{dif} R_{gl,f}^{dif}
-     }
-     \left(
-       R_{gl,f}^{dir}(\phi) \tau_{bl,f}^{dir,dir}(\phi_s) \rho_{bl,b}^{dir}(\phi_s) + \tau_{bl,f}^{dir,dif}(\phi_s) 
-     \right)
-$$</div>
-
-<div>$$T_{f,sys}^{dif,dif} = \frac{{\tau_{bl,f}^{dif,dif}T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}$$</div>
-
-<div>$$T_{f,sys}^{sky - dif,dif} = \frac{{\tau_{bl,f}^{sky - dif,dif}T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}$$</div>
-
-<div>$$T_{f,sys}^{gnd - dif,dif} = \frac{{\tau_{bl,f}^{gnd - dif,dif}T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}$$</div>
-
-<div>$$A_{gl,j,f}^{dif,sys} = \frac{{\tau_{bl,f}^{dif,dif}A_{gl,j,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}},{\rm{    }}j = 1,N$$</div>
-
-<div>$$A_{gl,j,f}^{sky - dif,sys} = \frac{{\tau_{bl,f}^{sky - dif,dif}A_{gl,j,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}},{\rm{    }}j = 1,N$$</div>
-
-<div>$$A_{gl,j,f}^{gnd - dif,sys} = \frac{{\tau_{bl,f}^{gnd - dif,dif}A_{gl,j,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}},{\rm{    }}j = 1,N$$</div>
-
-<div>$$\alpha_{bl,f}^{dif,sys} = \alpha_{bl,f}^{dif} + \frac{{\tau_{bl,f}^{dif,dif}R_{gl,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}\alpha_{bl,b}^{dif}$$</div>
-
-<div>$$\alpha_{bl,f}^{sky - dif,sys} = \alpha_{bl,f}^{sky - dif} + \frac{{\tau_{bl,f}^{sky - dif,dif}R_{gl,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}\alpha_{bl,b}^{dif}$$</div>
-
-<div>$$\alpha_{bl,f}^{gnd - dif,sys} = \alpha_{bl,f}^{gnd - dif} + \frac{{\tau_{bl,f}^{gnd - dif,dif}R_{gl,f}^{dif}}}{{1 - R_{gl,f}^{dif}\rho_{bl,b}^{dif}}}\alpha_{bl,b}^{dif}$$</div>
-
-#### Blind/Glazing System Properties for Long-Wave Radiation
-
-The program calculates how much long-wave radiation is absorbed by the blind and by the adjacent glass surface. The effective emissivity (long-wave absorptance) of an interior or exterior blind, taking into account reflection of long-wave radiation between the glass and blind, is given by
-
-<div>$$\varepsilon_{bl}^{lw,eff} = \varepsilon_{bl}^{lw}\left( {1 + \frac{{\tau_{bl}^{lw}\rho_{gl}^{lw}}}{{1 - \rho_{bl}^{lw}\rho_{gl}^{lw}}}} \right)$$</div>
-
-where <span>\(\rho_{gl}^{lw}\)</span>is the long-wave reflectance of the outermost glass surface for an exterior blind or the innermost glass surface for an interior blind, and it is assumed that the long-wave transmittance of the glass is zero.
-
-The effective innermost (for interior blind) or outermost (for exterior blind) glass surface emissivity when the blind is present is
-
-<div>$$\varepsilon_{gl}^{lw,eff} = \varepsilon_{gl}^{lw}\frac{{\tau_{bl}^{lw}}}{{1 - \rho_{bl}^{lw}\rho_{gl}^{lw}}}$$</div>
-
-The effective inside surface emissivity is the sum of the effective blind and effective glass emissivities:
-
-<div>$$\varepsilon_{ins}^{lw,eff} = \varepsilon_{bl}^{lw,eff} + \varepsilon_{gl}^{lw,eff}$$</div>
-
-The effective temperature of the blind/glazing combination that is used to calculate the window’s contribution to the zone’s mean radiant temperature (MRT) is given by
-
-<div>$$T_{}^{eff} = \frac{{\varepsilon_{bl}^{lw,eff}{T_{bl}} + \varepsilon_{gl}^{lw,eff}{T_{gl}}}}{{\varepsilon_{bl}^{lw,eff} + \varepsilon_{gl}^{lw,eff}}}$$</div>
-
-
-
-#### Solar Radiation Transmitted and Absorbed by a Window/Blind System
-
-Let the direct solar incident on the window be
-
-<div>$${I_{dir,inc}} = {f_{sunlit}}{I_{dir,norm}}\cos \phi {\rm{    }}(W/{m^2})$$</div>
-
-where <span>\({f_{sunlit}}\)</span>is the fraction of the window that is sunlit (determined by the shadowing calculations), <span>\({I_{dir,norm}}\)</span>is the direct normal solar irradiance, and <span>\(\phi \)</span> is the angle of incidence.
-
-Let <span>\({I_{sky,inc}}\)</span>be the irradiance on the window due to diffuse solar radiation from the sky (W/m<sup>2</sup>) and let <span>\({I_{gnd,inc}}\)</span>be the irradiance on the window due to diffuse solar radiation from the ground (W/m<sup>2</sup>).
-
-Then we have the following expressions for different classes of transmitted and absorbed solar radiation for the window/blind system (where <span>\({\phi_s}\)</span>is the direct solar profile angle), all in W/m<sup>2</sup>:
-
-*Direct solar entering zone from incident direct solar:*
-
-<div>$${I_{dir,inc}}T_{f,sys}^{dir,dir}(\phi ,{\phi_s})$$</div>
-
-*Diffuse solar entering zone from incident direct solar:*
-
-<div>$${I_{dir,inc}}T_{f,sys}^{dir,dif}(\phi ,{\phi_s})$$</div>
-
-*Direct solar absorbed by blind:*
-
-<div>$${I_{dir,inc}}\alpha_{bl,f}^{dir,sys}(\phi ,{\phi_s})$$</div>
-
-*Direct solar absorbed by glass layers:*
-
-<div>$${I_{dir,inc}}A_{gl,j,f}^{dir,sys}(\phi ,{\phi_s}),{\rm{    }}j = 1,N$$</div>
-
-#### For windows whose blinds have vertical slats:
-
-*Diffuse solar entering zone from incident diffuse solar:*
-
-<div>$$({I_{sky,inc}} + {I_{gnd,inc}})T_{f,sys}^{dif,dif}$$</div>
-
-*Diffuse solar absorbed by blind:*
-
-<div>$$({I_{sky,inc}} + {I_{gnd,inc}})\alpha_{bl,f}^{dif,sys}$$</div>
-
-*Diffuse solar absorbed by glass layers:*
-
-<div>$$({I_{sky,inc}} + {I_{gnd,inc}})A_{gl,j,f}^{dif,sys},{\rm{   }}j = 1,N{\rm{ }}$$</div>
-
-#### For windows of tilt angle <span>\(\gamma \)</span> whose blinds have horizontal slats:
-
-(vertical windows have tilt = 90<sup>O</sup>, horizontal windows have tilt = 0<sup>O</sup>)
-
-*Diffuse solar entering zone from incident diffuse solar:*
-
-**<span>\(T_{f,sys}^{sky - dif,dif}\left[ {\left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{sky,inc}} + \frac{{|\cos \gamma |}}{2}{I_{gnd,inc}}} \right] + T_{f,sys}^{gnd - dif,dif}\left[ {\frac{{|\cos \gamma |}}{2}{I_{sky,inc}} + \left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{gnd,inc}}} \right]\)</span>**
-
-*Diffuse solar absorbed by blind:*
-
-<div>$$\alpha_{bl,f}^{sky - dif,sys}\left[ {\left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{sky,inc}} + \frac{{|\cos \gamma |}}{2}{I_{gnd,inc}}} \right] + \alpha_{bl,f}^{gnd - dif,sys}\left[ {\frac{{|\cos \gamma |}}{2}{I_{sky,inc}} + \left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{gnd,inc}}} \right]$$</div>
-
-*Diffuse solar absorbed by glass layers:*
-
-<div>$$\begin{array}{l}A_{gl,j,f}^{sky - dif,sys}\left[ {\left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{sky,inc}} + \frac{{|\cos \gamma |}}{2}{I_{gnd,inc}}} \right] + \\A_{gl,j,f}^{gnd - dif,sys}\left[ {\frac{{|\cos \gamma |}}{2}{I_{sky,inc}} + \left( {1 - \frac{{|\cos \gamma |}}{2}} \right){I_{gnd,inc}}} \right],{\rm{    }}j = 1,N\end{array}$$</div>
-
-#### Screens
-
-The model for window screens currently allows placement on the exterior surface of a window system (i.e., between glass and interior window screens can not be modeled). The exterior screen is modeled as a planar semi-transparent sheet having specular transmittance that is dependent on the angle of incidence of beam solar radiation. The screen transmittance algorithm includes two components. The first one, *T<sub>beam</sub>* (α’, φ'), accounts for the blockage of the sun’s rays by the screen material. This component accounts for the beam solar radiation passing through the screen openings without hitting the screen material. The second part, *T<sub>scatt</sub>*  (α’, φ'), accounts for the additional flux of transmitted beam solar radiation by diffuse reflectance (scattering) from the screen material. Since the reflected component is small compared with the incident beam and the direction of scattering is highly dependent on incident angle, the component of transmitted beam radiation due to screen material reflectance can be treated in one of three ways based on a user input to the model.
-
-The user may elect not to model the inward reflected beam transmittance due to the uncertainty of the direction of scattering or its low magnitude for low-reflecting screen materials. The user may alternately choose to model the inwardly-reflected transmitted beam as an additive component to the direct beam transmittance in the same solid angle and direction. Finally, the additional flux due to the inward reflection of direct beam radiation may be modeled as hemispherically-diffuse transmittance.
-
-This reflected beam transmittance component depends upon the diffuse (i.e., beam-to-diffuse) reflectance of the screen material, so this reflectance (�<sub>sc</sub>) is a required input to the model. Guidance input values for this diffuse reflectance are provided, to account for screens that are dark, medium, or light colored in appearance, in the likely case that more accurate values for the material reflectance are difficult or time-consuming to obtain. If the diffuse reflectance of the screen material is known, use this value in place of the guidance provided.
-
-The model is based on an orthogonal crossed cylinder geometry in which the screen material’s cylindrical diameter and spacing are known. The model assumes that the screen material diameter and spacing are the same in both directions. Figure 85 shows a rendering of intersecting orthogonal crossed cylinders used as the basis for the EnergyPlus screen model.
-
-![ScreenDiameter\_Spacing](media/image1148.png)
-
-Figure 85. Screen model rendering of intersecting orthogonal crossed cylinders
-
-If the required screen material dimensions are not available from the manufacturer, they may be determined using the following procedure:
-
-* Lay the screen next to a finely-divided scale or ruler. A magnifying glass may be helpful in determining the screen material dimensions. Alternately, a photograph can be taken and the image enlarged.
-
-* Determine the diameter *D* of an individual screen material “cylinder�. Average the diameter values if different in opposing directions.
-
-* Determine the average center-to-center spacing *S* of the screen material or measure from one side of a “cylinder� to the same side of the next �cylinder� and record the spacing *S*. Average the spacing values if different in opposing directions.
-
-* Enter these values as inputs to the exterior window screen model.
-
-The screen material diameter and spacing are then used to determine the screen material aspect ratio for use in the screen model.
-
-<div>$$\gamma  = {D \mathord{\left/ {\vphantom {D S}} \right. } S}$$</div>
-
-where
-
-<span>\(\gamma \)</span>   = Screen material aspect ratio, dimensionless
-
-<span>\(D\)</span>  = Screen material diameter, m
-
-<span>\(S\)</span>  = Screen material spacing, m
-
-
-
-Figure 86 below shows the input requirements for material diameter and spacing and the associated calculation for openness factor, the equivalent to *T<sub>beam</sub>* at direct normal incidence.
-
-![AspectRatio](media/image1153.png)
-
-Figure 86. Physical screen material properties
-
-### Screen Properties and Calculations
-
-#### Screen Beam Transmittance
-
-The first component of the window screen transmittance model is a geometric representation of the open area of the screen material and is dependent on the angle of incident beam radiation. Figure 87 shows a schematic of a South-facing vertical window screen and the solar angles used in EnergyPlus. The window screen model is based on the relative angles of incidence of the sun’s rays with respect the the window screen outward normal. In the figure, the relative solar azimuth and relative solar altitude are represented as φ’ and α’, respectively.
-
-![WindowScreenSchematic](media/image1154.png)
-
-Figure 87. Schematic of a vertical window screen facing due South
-
-Given the diffuse reflectance �<sub>sc</sub> and the screen aspect ratio γ, the model takes the direction of solar incidence, the relative solar altitude angle α’ and the relative solar azimuth angle φ', illustrated in Figure 87, and calculates the direct beam transmittance *T<sub>beam</sub>* (α’, φ') as follows. Since the direct beam transmittance is only a function of the incident angle and the screen material aspect ratio, the following applies to both solar and visible radiation.
-
-<div>$$\alpha '' = {\rm{arctan}}\left( {\tan \alpha '\sec \varphi '} \right)$$</div>
-
-<div>$$\beta  = \frac{\pi }{2} - \varphi '$$</div>
-
-<div>$${T_y} = 1 - \gamma \left[ {\cos \alpha '' + \sin \alpha ''\tan \alpha '{{\left( {1 + {{\cot }^2}\beta } \right)}^{\frac{1}{2}}}} \right]$$</div>
-
-<div>$$\mu  = \arccos \left( {{{\left[ {{{\cos }^2}\alpha '{{\cos }^2}\varphi ' + {{\sin }^2}\alpha '} \right]}^{\frac{1}{2}}}} \right)$$</div>
-
-<div>$$\varepsilon  = \arccos \left( {{\raise0.7ex\hbox{${\left[ {\cos \alpha '\cos \varphi '} \right]}$} \!\mathord{\left/ {\vphantom {{\left[ {\cos \alpha '\cos \varphi '} \right]} {\cos \mu }}}\right.}\!\lower0.7ex\hbox{${\cos \mu }$}}} \right)$$</div>
-
-<div>$$\eta  = \frac{\pi }{2} - \varepsilon $$</div>
-
-<div>$$\mu ' = \arctan \left( {\tan \mu \sec \varepsilon } \right)$$</div>
-
-<div>$${T_x} = 1 - \gamma \left[ {\cos \mu ' + \sin \mu '\tan \mu {{\left( {1 + {{\cot }^2}\eta } \right)}^{\frac{1}{2}}}} \right]$$</div>
-
-<div>$${T_{beam}}\left( {\alpha ',\varphi '} \right) = T_{beam}^{vis}\left( {\alpha ',\varphi '} \right) = {T_x}{T_y}$$</div>
-
-where
-
-<span>\({T_y}\)</span> = vertical component of direct beam transmittance
-
-<span>\({T_x}\)</span> = horizontal component of direct beam transmittance
-
-<span>\({T_{beam}}\)</span> = direct screen transmittance that accounts for beam solar radiation passing through the screen openings without hitting the screen material
-
-<span>\(T_{beam}^{vis}\)</span> = direct visible screen transmittance that accounts for beam solar radiation passing through the screen openings without hitting the screen material
-
-α’   = relative solar altitude angle [radians]
-
-φ'   = relative solar azimuth angle [radians]
-
-<span>\(\gamma \)</span>   = Screen material aspect ratio, dimensionless
-
-<span>\(\alpha '',\beta ,\mu ,\varepsilon ,\eta ,\mu '\)</span> = intermediate variables
-
-This first component of screen direct beam transmittance was developed using geometric principals and was verified using an optical ray tracing software program.
-
-The second component of the window screen transmittance model is an empirical algorithm that accounts for the inward reflection of incident beam radiation off the screen material surface. The calculation procedure for the screen’s transmittance via beam reflection, *T<sub>scatt</sub>* (α’, φ') is as follows:
-
-<div>$$\begin{array}{l}{T_{scattmax}} = 0.0229\,\gamma  + 0.2971\,{\rho_{sc}} - 0.03624\,{\gamma ^2}\, + \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,0.04763\,{\rho_{sc}}^2 - 0.44416\,\gamma \,{\rho_{sc}}\end{array}$$</div>
-
-<div>$$\begin{array}{l}T_{scattmax}^{vis} = 0.0229\,\gamma  + 0.2971\,\rho_{sc}^{vis} - 0.03624\,{\gamma ^2}\, + \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,0.04763{\left( {\rho_{sc}^{vis}} \right)^2} - 0.44416\,\gamma \,\rho_{sc}^{vis}\end{array}$$</div>
-
-<div>$${\delta_{max}} = 89.7 - {{10\gamma } \mathord{\left/ {\vphantom {{10\gamma } {0.16}}} \right. } {0.16}}$$</div>
-
-<div>$$\delta  = {\left( {\alpha_d^{'2} + \varphi_d^{'2}} \right)^{\frac{1}{2}}}$$</div>
-
-<div>$$Pea{k_{ratio}} = {\raise0.7ex\hbox{${1.0}$} \!\mathord{\left/ {\vphantom {{1.0} {\left( {0.2{\rho_{sc}}\left( {1 - \gamma } \right)} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {0.2{\rho_{sc}}\left( {1 - \gamma } \right)} \right)}$}}$$</div>
-
-<div>$$Peak_{ratio}^{vis} = {\raise0.7ex\hbox{${1.0}$} \!\mathord{\left/ {\vphantom {{1.0} {\left( {0.2\rho_{sc}^{vis}\left( {1 - \gamma } \right)} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {0.2\rho_{sc}^{vis}\left( {1 - \gamma } \right)} \right)}$}}$$</div>
-
-<div>$${T_{scatt}}\left( {\alpha ',\varphi '} \right) = 0.2{\rho_{sc}}{T_{scattmax}}\left( {1 - \gamma } \right)\left( {1 + \left( {Pea{k_{ratio}} - 1} \right){e^{\frac{{ - {{\left| {\delta  - {\delta_{max}}} \right|}^{2.0}}}}{{600}}}}} \right)$$</div>
-
-<div>$$T_{scatt}^{vis}\left( {\alpha ',\varphi '} \right) = 0.2\rho_{sc}^{vis}T_{scattmax}^{vis}\left( {1 - \gamma } \right)\left( {1 + \left( {Peak_{ratio}^{vis} - 1} \right){e^{\frac{{ - {{\left| {\delta  - {\delta_{max}}} \right|}^{2.0}}}}{{600}}}}} \right)$$</div>
-
-<div>$$
-  \begin{array}{rl}
-    IF \left( \delta \gt \delta_{max} \right) \; T_{scatt} \left( \alpha ',\varphi ' \right) &= 
-      0.2 \rho_{sc} T_{scattmax} \left( 1 - \gamma \right) \left( 1 + \left( Peak_{ratio} - 1 \right) e^{\frac{- \left| \delta - \delta_{max} \right|^{2.5}}{600}} \right) - 0.2 \rho_{sc} T_{scattmax} \left( 1 - \gamma \right) \left( \max \left( 0.0, \frac{\delta  - \delta_{max}}{90. - {delta_{max}}} \right) \right) \\
-    IF \left( \delta \gt \delta_{max} \right) \; T_{scatt}^{vis} \left( \alpha ',\varphi ' \right) &= 
-      0.2 \rho_{sc}^{vis} T_{scattmax}^{vis} \left( 1 - \gamma \right) \left( 1 + \left( Peak_{ratio}^{vis} - 1 \right) e^{\frac{- \left| \delta - \delta_{max} \right|^{2.5}}{600}} \right) - 0.2 \rho_{sc}^{vis} T_{scattmax}^{vis} \left( 1 - \gamma \right) \left( \max \left( 0.0, \frac{\delta  - \delta_{max}}{90. - {delta_{max}}} \right) \right) \\
-  \end{array}
-$$</div>
-
-where
-
-<span>\({T_{scattmax}}\)</span> = maximum reflected (scattered) beam transmittance
-
-<span>\(T_{scattmax}^{vis}\)</span> = maximum visible reflected (scattered) beam transmittance
-
-<span>\({\delta_{max}},\delta \)</span> = intermediate variables [degrees]
-
-<span>\(\alpha_d'\)</span> = relative solar altitude [degrees]
-
-<span>\(\varphi_d'\)</span> = relative solar azimuth [degrees]
-
-<span>\(Pea{k_{ratio}}\)</span>= Ratio of peak scattered beam transmittance to scattered beam transmittance at direct normal incidence.
-
-<span>\(Peak_{ratio}^{vis}\)</span>= Ratio of peak scattered visible transmittance to scattered visible transmittance at direct normal incidence.
-
-<span>\({\rho_{sc}}\)</span>= diffuse solar reflectance of the screen material
-
-<span>\(\rho_{sc}^{vis}\)</span>= diffuse visible reflectance of the screen material
-
-<span>\({T_{scatt}}\)</span> = beam solar transmittance due to reflectance (scattering)
-
-<span>\(T_{scatt}^{vis}\)</span> = beam visible transmittance due to reflectance (scattering)
-
-The reflected (scattered) transmittance of incident beam radiation is an empirical model derived by curvefitting results from optical ray trace modeling. Ray traces were performed for a range of screen aspect ratios, diffuse screen reflectances, and relative solar azimuth and altitude angles. The surface of the screen cylinders was assumed to be diffusely reflecting, having the optical properties of a Lambertian surface. The transmitted flux due to reflection was determined by a hemispherical detector on the transmitted side of the screen.
-
-These two components of beam solar transmittance are then used to specify the properties for beam-to-beam and beam-to-diffuse transmittance for the screen based on the user selection for Reflected Beam Transmittance Accounting Method in the WindowMaterial:Screen object. The calculations below apply to both the solar and visible beam solar transmittance.
-
-If the user selects DoNotModel, the direct beam transmittance is set to *T<sub>beam</sub>* and the reflected (scattered) portion of the beam solar transmittance is ignored:
-
-<div>$$T_{sc}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right)$$</div>
-
-<div>$$T_{sc}^{dir,dif} = 0.0$$</div>
-
-<div>$$T_{sc,\,vis}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right)$$</div>
-
-<div>$$T_{sc,\,vis}^{dir,dif} = 0.0$$</div>
-
-where
-
-<span>\(T_{sc}^{dir,dir}\)</span> = direct-to-direct beam transmittance of the screen (output report variable Surface Window Screen Beam to Beam Solar Transmittance)
-
-<span>\(T_{sc}^{dir,dif}\)</span>= direct-to-diffuse beam transmittance of the screen (output report variable Surface Window Screen Beam to Diffuse Solar Transmittance)
-
-<span>\(T_{sc,\,vis}^{dir,dir}\)</span> = direct-to-direct visible transmittance of the screen
-
-<span>\(T_{sc,\,vis}^{dir,dif}\)</span>= direct-to-diffuse visible transmittance of the screen
-
-If the user selects Model as Direct Beam, the reflected (scattered) portion of the beam solar transmittance is added to the direct beam transmittance *T<sub>beam</sub>* in the same solid angle and direction of the unattenuated solar beam:
-
-<div>$$T_{sc}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right) + {T_{scatt}}\left( {\alpha ',\varphi '} \right)$$</div>
-
-<div>$$T_{sc}^{dir,dif} = 0.0$$</div>
-
-<div>$$T_{sc,\,vis}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right) + T_{scatt}^{vis}\left( {\alpha ',\varphi '} \right)$$</div>
-
-<div>$$T_{sc,\,vis}^{dir,dif} = 0.0$$</div>
-
-If the user selects Model as Diffuse Beam, the direct beam transmittance is set to *T<sub>beam</sub>* and the reflected (scattered) portion of the beam solar transmittance is modeled as diffuse hemispherical radiation:
-
-<div>$$T_{sc}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right)$$</div>
-
-<div>$$T_{sc}^{dir,dif} = {T_{scatt}}\left( {\alpha ',\varphi '} \right)$$</div>
-
-<div>$$T_{sc,\,vis}^{dir,dir} = {T_{beam}}\left( {\alpha ',\varphi '} \right)$$</div>
-
-<div>$$T_{sc,\,vis}^{dir,dif} = T_{scatt}^{vis}\left( {\alpha ',\varphi '} \right)$$</div>
-
-#### Screen Beam Reflectance
-
-The screen reflectance (overall value for the screen assembly, accounting for the screen material itself and the open spaces between the screen material) is calculated by first subtracting the direct-to-direct screen transmittance from the unit incident beam. This approximates the fraction of incident beam solar radiation striking the screen that is not inwardly transmitted. The result is then multiplied by the screen material diffuse reflectance �<sub>sc</sub>. The inwardly scattered transmittance is then subtracted from this quantity to obtain an approximate value for the screen’s reflectance R<sub>sc</sub> to beam radiation incident as a function of the relative angles of incident radiation. This equation is used for both beam and visible reflectance:
-
-<div>$$R_{SC}^{dir,dif}\left( {\alpha ',\varphi '} \right) = {\rho_{SC}}\left( {1 - T_{SC}^{dir,dir}} \right) - T_{SC}^{dir,dif}$$</div>
-
-<div>$$R_{SC,vis}^{dir,dif}\left( {\alpha ',\varphi '} \right) = \rho_{SC}^{vis}\left( {1 - T_{SC,vis}^{dir,dir}} \right) - T_{SC,vis}^{dir,dif}$$</div>
-
-#### Screen Beam Absorptance
-
-The screen absorptance(overall value for the screen assembly, accounting for the screen material itself and the open spaces between the screen material) is calculated as the quantity of the unit incident flux (1) less the directly-transmitted component *T<sub>dir,dir</sub>* multiplied by the quantity 1 minus the screen material diffuse reflectance.
-
-<div>$$A_{SC}^{dir}\left( {\alpha ',\varphi '} \right) = \left( {1 - T_{SC}^{dir,dir}} \right)\left( {1 - {\rho_{SC}}} \right)$$</div>
-
-#### Screen Diffuse Properties
-
-The transmittance of the screen to half-hemispherical diffuse (sky) radiation is calculated by performing a finite-element-summation, approximately equivalent to an integration over the solid angle of the beam transmittance, assuming uniform radiance. This single-number screen diffuse transmittance is then multiplied by the irradiance incident on the screen from a uniform half-hemisphere of sky- or ground-reflected radiation to determine the level of additional flux transmitted by the screen to the window from the diffuse sky or ground. The sun angles shown in the figure below represent the solar altitude angle (θ) and solar azimuth angle (Ф) in polar coordinates. These angles are used to calculate the average diffuse-to-diffuse properties for screens in the following derivations.
-
-![PolarCoordinates](media/image1210.png)
-
-Figure 88. Sun Angles in Screen Calculations.
-
-The screen transmittance to diffuse radiation *T<sub>dif,dif</sub>* (γ, �<sub>sc</sub>)  is computed as the integrated average of the combined beam transmittance *T<sub>tot</sub>* (γ, �, θ, Ф) over the directions of incidence using spherical coordinates (θ, Ф) in which the z-axis is perpendicular to the plane of the screen. Using a finite element computation, this is:
-
-<div>$${T_{tot}}(\gamma ,{\rho_{sc}},{\theta_j},{\phi_i}) = {T_{beam}}\left( {\alpha ',\varphi '} \right) + {T_{scatt}}\left( {\alpha ',\varphi '} \right)$$</div>
-
-<div>$$T_{sc}^{dif,dif}(\gamma ,{\rho_{sc}}) = \frac{{\sum\limits_{j = 1}^N {\sum\limits_{i = 1}^M {{T_{tot}}(\gamma ,{\rho_{sc}},{\theta_j},{\phi_i})\sin ({\theta_j})\cos ({\theta_j})} } }}{{\sum\limits_{j = 1}^N {\sum\limits_{i = 1}^M {\sin ({\theta_j})\cos ({\theta_j})} } }}$$</div>
-
-where
-
-<span>\(\theta \)</span> = solar altitude angle in polar coordinates [radians]
-
-<span>\(\phi \)</span> = solar azimuth angle in polar coordinates [radians]
-
-<span>\(T_{sc}^{dif,dif}(\gamma ,{\rho_{sc}})\)</span>= diffuse-diffuse transmittance (output report variable Surface Window Screen Diffuse to Diffuse Solar Transmittance)
-
-Similarly, the reflectance of the screen to diffuse radiation is given by
-
-<div>$$R_{sc}^{dif,dif}(\gamma ,{\rho_{sc}}) = \frac{{\sum\limits_{j = 1}^N {\sum\limits_{i = 1}^M {R_{sc}^{dir,dif}(\gamma ,{\rho_{sc}},{\theta_j},{\phi_i})\sin ({\theta_j})\cos ({\theta_j})} } }}{{\sum\limits_{j = 1}^N {\sum\limits_{i = 1}^M {\sin ({\theta_j})\cos ({\theta_j})} } }}$$</div>
-
-There is an assumption in both of these formulas that the brightness of the sky (or ground) diffuse radiation is the same for all directions. For this reason, the solar azimuth angle Ф and solar altitude angle θ have a range of 0 to <span>\({\pi  \mathord{\left/ {\vphantom {\pi  2}} \right. } 2}\)</span> (instead of <span>\({{ - \pi } \mathord{\left/ {\vphantom {{ - \pi } 2}} \right. } 2}\)</span> to <span>\({{ + \pi } \mathord{\left/ {\vphantom {{ + \pi } 2}} \right. } 2}\)</span>) because the screen is assumed to have identical optical properties for radiation incident at the same angles on either side of a vertical or horizontal plane perpendicular to the screen.
-
-Since the screen direct transmittance model is derived with respect to a different coordinate axis labeling, a coordinate transform is needed in order to calculate the diffuse optical properties. In these calculations, for each spherical solar coordinates (θ, Ф) we need the corresponding screen relative solar coordinates (α’, φ') to evaluate the screen transmittance model for that direction.
-
-For each θ and Ф in the summation, the corresponding values for the relative solar altitude α’ and relative solar azimuth φ’ needed to calculate screen transmittance are determined with the following coordinate transform equations:
-
-<div>$$\sin \alpha ' = \sin \theta \cos \phi $$</div>
-
-<div>$$\tan \varphi ' = \tan \theta \sin \phi $$</div>
-
-The absorptance of the screen to diffuse incident radiation is calculated by subtracting the diffuse transmittance and diffuse reflectance from unity as follows:
-
-<div>$$A_{sc}^{dif}(\gamma ,{\rho_{sc}}) = 1 - T_{sc}^{dif,dif}(\gamma ,{\rho_{sc}}) - R_{sc}^{dif,dif}(\gamma ,{\rho_{sc}})$$</div>
-
-#### Screen/Glass System Properties for Short-Wave Radiation
-
-The combined system properties of the screen/glass combination are calculated using the properties of the screen in combination with the bare glass material properties. Interreflections of radiation between the screen and glass surfaces are included. The following infinite series serves as an example for calculating the combined screen/glass system properties. The terms of the series are built up as illustrated in the following figure. The terms shown at the right of the figure represent each term in the infinite series for the combined screen/glass property (beam transmittance in this example).
-
-For the example of beam transmittance, the incident solar beam strikes the screen at the incident angle associated with the current relative azimuth and altitude angle. The incident beam splits into reflected and transmitted components at the screen. The transmitted component is attenuated as it passes through the screen material by the screen’s beam transmittance (<span>\(T_{sc}^{dir,dir}\)</span>, shown as<span>\(T_{sc}^{dir}\)</span> in the figure and equations below) at this incident angle. The reflected (scattered) transmittance of incident solar beam is also shown at this point and will be discussed later in this section. As the attenuated solar beam continues on towards the front glass surface, a portion of the screen-transmitted beam splits at the window surface into transmitted and reflected components. The reflected component reflects off the front surface of the glass material (<span>\(T_{sc}^{dir,dir}R_{gl,f}^{dir}\)</span>) and the transmitted component continues to travel through the glass material and is further attenuated by the glass beam transmittance. Thus the first term of the combined screen/glass solar beam transmittance is shown as <span>\(T_{sc}^{dir,dir}T_{gl}^{dir}\)</span>. Interreflections are accounted for by following the beam as it continues to reflect off the front surface of the glass material and the back surface of the screen material. Continuing on with the glass-reflected beam (<span>\(T_{sc}^{dir,dir}R_{gl,f}^{dir}\)</span>) described above, this beam strikes the back surface of the screen material at the same incident angle as the incident solar beam. This reflected beam is also assumed to be a collimated beam (solid lines) which strikes the back surface of the screen material and reflects as hemispherically-diffuse radiation (dotted lines). The reflective property of the screen material used here is the beam reflectance calculated at the incident solar angle (<span>\(R_{sc}^{dir,dif}\)</span>). A single ray of this diffuse light will be followed through the remaining steps and represents the energy associated with **all** diffuse rays interreflecting between the screen and glass layers. To determine the second term of the combined screen/glass beam transmittance, the diffusely-reflected ray (<span>\(T_{sc}^{dir,dir}R_{gl,f}^{dir}R_{sc}^{dir,dif}\)</span>) passes through and is attenuated by the glass layer. Since this ray originates from diffuse reflection, the attenuation of this ray is accounted for using the diffuse transmittance property of the glass. Thus, the second term is shown as <span>\(T_{sc}^{dir,dir}R_{gl,f}^{dir}R_{sc}^{dir,dif}T_{gl}^{dif}\)</span>. Defining the remaining terms continues in a similar fashion using diffuse properties of both the screen and glass material. Notice that the 3<sup>rd</sup> and 4<sup>th</sup> terms shown below are similar to the 2<sup>nd</sup> term, but additional terms are raised to increasing powers.
-
-![TransmittanceEquation](media/image1231.png)
-
-Figure 89. Screen/Glass System Transmittance Equation Schematic.
-
-The screen/glass system transmittance equation shown in the figure above is repeated here in an alternate format to emphasize the recurring nature of the infinite series. This equation represents the final solar beam transmittance equation for the screen/glass combination. The recurring terms are shown as a summation of a quantity raised to the n power, with n ranging from 0 to infinity. Since the quantity <span>\(R_{gl}^{dif}R_{sc}^{dif,dif}\)</span> is less than 1, the summation <span>\(\sum\limits_{n = 0}^\infty  {{{(R_{gl,f}^{dif}R_{sc}^{dif,dif})}^n}} \)</span>converges and can be expressed as <span>\({\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 {\left( {1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}} \right)}$}}\)</span>. Since the reflected (scattered) transmittance of incident solar beam (<span>\(T_{sc}^{dir,dif}\)</span>) and the diffusely reflecting beam <span>\(T_{sc}^{dir,dir}R_{gl,f}^{dir}R_{sc}^{dir,dif}\)</span> are both assumed to be hemispherically diffuse radiation, the reflected (scattered) transmittance of incident solar beam is added to the infinite series as shown below.
-
-<div>$$\begin{array}{l}T_{sys}^{dir,all}(\alpha ',\varphi ',\phi ) = T_{sc}^{dir,dir}(\alpha ',\varphi ')T_{gl}^{dir}\left( \phi  \right) + (T_{sc}^{dir,dir}(\alpha ',\varphi ')R_{gl,f}^{dir}R_{sc}^{dir,dif}(\alpha ',\varphi ') + T_{sc}^{dir,dif}(\alpha ',\varphi '))T_{gl}^{dif}\sum\limits_{n = 0}^\infty  {{{(R_{gl,f}^{dif}R_{sc}^{dif,dif})}^n}} \\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; - or - \end{array}$$</div>
-
-<div>$$T_{sys}^{dir,all}(\alpha ',\varphi ',\phi ) = T_{sc}^{dir,dir}(\alpha ',\varphi ')T_{gl}^{dir}\left( \phi  \right) + \frac{{(T_{sc}^{dir,dir}(\alpha ',\varphi ')R_{gl,f}^{dir}R_{sc}^{dir,dif}(\alpha ',\varphi ') + T_{sc}^{dir,dif}(\alpha ',\varphi '))T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}}}$$</div>
-
-where
-
-<span>\(T_{sys}^{dir,all}(\alpha ',\varphi ',\phi )\)</span> = screen/glass system beam transmittance (output report variable Surface Window Screen and Glazing System Beam Solar Transmittance)
-
-Properties for beam absorptance of the individual glass layers and screen/glass combination are derived in a similar fashion to the transmittance calculation described above. Diffuse transmittance and absorptance of individual glass layers and the screen/glass combination are also shown here.
-
-<span>\(\begin{array}{l}A_{gl,j,f}^{dir,sys}\left( {\alpha ',\varphi ',\phi } \right) = T_{sc}^{dir,dir}\left( {\alpha ',\varphi '} \right)A_{gl,j,f}^{dir}\left( \phi  \right) + \\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\;\;\;\;\;\;\frac{{\left( {T_{sc}^{dir,dir}\left( {\alpha ',\varphi '} \right)R_{gl}^{dir}\left( \phi  \right)R_{sc}^{dir,dif}\left( {\alpha ',\varphi '} \right) + T_{sc}^{dir,dif}\left( {\alpha ',\varphi '} \right)} \right)A_{gl,j,f}^{dif}}}{{1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}}},\;j = 1,N\end{array}\)</span><span>\(\begin{array}{l}\alpha_{sc}^{dir,sys}\left( {\alpha ',\varphi ',\phi } \right) = A_{sc}^{dir}\left( {\alpha ',\varphi '} \right)\left( {1 + R_{gl,f}^{dir}\left( \phi  \right)T_{sc}^{dir,dir}\left( {\alpha ',\varphi '} \right)} \right) + \\\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\frac{{A_{sc}^{dif}R_{gl,f}^{dif}}}{{1 - R_{sc}^{dif,dif}R_{gl,f}^{dif}}}\left( {R_{gl,f}^{dir}\left( \phi  \right)T_{sc}^{dir,dir}\left( {\alpha ',\varphi '} \right)R_{sc}^{dir,dif}\left( {\alpha ',\varphi '} \right)} \right)\end{array}\)</span>
-
-<div>$$T_{sys}^{dif,dif} = \frac{{T_{sc}^{dif,dif}T_{gl}^{dif}}}{{1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}}}$$</div>
-
-<div>$$A_{gl,j,f}^{dif,sys} = \frac{{T_{sc}^{dif,dif}A_{gl,j,f}^{dif}}}{{1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}}},\;j = 1,N$$</div>
-
-<div>$$\alpha_{sc}^{dif,\,sys} = A_{sc}^{dif}\left( {1 + \frac{{T_{sc}^{dif,dif}R_{gl,f}^{dif}}}{{1 - R_{gl,f}^{dif}R_{sc}^{dif,dif}}}} \right)$$</div>
-
-
-
-where
-
-<span>\(A_{gl,j,f}^{dir,sys}\left( {\alpha ',\varphi ',\phi } \right)\)</span> = glass layer beam absorptance including interreflections with screen material
-
-<span>\(\alpha_{sc}^{dir,sys}\left( {\alpha ',\varphi ',\phi } \right)\)</span> = beam absorptance of screen material including interreflections with glass
-
-<span>\(T_{sys}^{dif,dif}\)</span> = screen/glass system diffuse transmittance (output report variable Surface Window Screen and Glazing System Diffuse Solar Transmittance)
-
-<span>\(A_{gl,j,f}^{dif,sys}\)</span> = glass layer diffuse absorptance including interreflections with screen material
-
-<span>\(\alpha_{sc}^{dif,sys}\)</span> = diffuse absorptance of screen material including interreflections with glass
-
-#### Screen/Glazing System Properties for Long-Wave Radiation
-
-The program calculates how much long-wave radiation is absorbed by the screen and by the adjacent glass surface. The effective long-wave emissivity (equal to the long-wave absorptance on a wavelength-by-wavelength basis or over the same spectral range) of an exterior screen, taking into account reflection of long-wave radiation between the glass and screen, is given by
-
-<div>$$\varepsilon_{sc}^{lw,eff} = \varepsilon_{sc}^{lw}\left( {1 + \frac{{T_{sc}^{dif,dif}\rho_{gl}^{lw}}}{{1 - R_{sc}^{dif,dif}\rho_{gl}^{lw}}}} \right)$$</div>
-
-where <span>\(\rho_{gl}^{lw}\)</span>is the long-wave reflectance of the outermost glass surface facing an exterior screen, and it is assumed that the long-wave transmittance of the glass is zero.
-
-The effective outermost (for exterior screen) glass surface emissivity when the screen is present is
-
-<div>$$\varepsilon_{gl}^{lw,eff} = \varepsilon_{gl}^{lw}\frac{{T_{sc}^{dif,dif}}}{{1 - R_{sc}^{dif,dif}\rho_{gl}^{lw}}}$$</div>
-
-The effective inside surface emissivity is the sum of the effective screen and effective glass emissivities:
-
-<div>$$\varepsilon_{ins}^{lw,eff} = \varepsilon_{sc}^{lw,eff} + \varepsilon_{gl}^{lw,eff}$$</div>
-
-The effective temperature of the screen/glazing combination that is used to calculate the window’s contribution to the zone’s mean radiant temperature (MRT) is given by
-
-<div>$${T^{eff}} = \frac{{\varepsilon_{sc}^{lw,eff}{T_{sc}} + \varepsilon_{gl}^{lw,eff}{T_{gl}}}}{{\varepsilon_{sc}^{lw,eff} + \varepsilon_{gl}^{lw,eff}}}$$</div>
-
-#### Solar Radiation Transmitted and Absorbed by a Window/Screen System
-
-Let the direct solar incident on the window be
-
-<div>$${I_{dir,inc}} = {f_{sunlit}}{I_{dir,norm}}\cos \phi {\rm{    }}(W/{m^2})$$</div>
-
-where <span>\({f_{sunlit}}\)</span>is the fraction of the window that is sunlit (determined by the shadowing calculations), <span>\({I_{dir,norm}}\)</span>is the direct normal solar irradiance, and <span>\(\phi \)</span> is the angle of incidence.
-
-Let <span>\({I_{sky,inc}}\)</span>be the irradiance on the window due to diffuse solar radiation from the sky (W/m<sup>2</sup>) and let <span>\({I_{gnd,inc}}\)</span>be the irradiance on the window due to diffuse solar radiation from the ground (W/m<sup>2</sup>).
-
-Then we have the following expressions for different classes of transmitted and absorbed solar radiation for the window/screen system, all in W/m<sup>2</sup>:
-
-*Direct and diffuse solar entering zone from incident direct solar:*
-
-<div>$${I_{dir,inc}}T_{sys}^{dir,all}\left( {\alpha ',\varphi '} \right)$$</div>
-
-*Direct solar absorbed by screen:*
-
-<div>$${I_{dir,inc}}\alpha_{sc}^{dir,sys}\left( {\alpha ',\varphi '} \right)$$</div>
-
-*Direct solar absorbed by glass layers:*
-
-<div>$${I_{dir,inc}}A_{gl,j,f}^{dir,sys}(\phi ,{\phi_s}),{\rm{    }}j = 1,N$$</div>
-
-*Diffuse solar entering zone from incident diffuse solar:*
-
-<div>$$\left( {{I_{sky,inc}} + {I_{gnd,inc}}} \right)T_{sys}^{dif,dif}$$</div>
-
-*Diffuse solar absorbed by screen:*
-
-<div>$$\left( {Isky,inc + Ignd,inc} \right)\alpha_{sc}^{dif,sys}$$</div>
-
-*Diffuse solar absorbed by glass layers:*
-
-<div>$$({I_{sky,inc}} + {I_{gnd,inc}})A_{gl,j,f}^{dif,sys},{\rm{   }}j = 1,N{\rm{ }}$$</div>
-
-### Complex Fenestration Calculation Module
-
-This section describes detailed method for modeling complex fenestration systems, including shading devices and general fenestration attachments. This detailed method primarily refers to the optical side of modeling complex fenestration systems. Thermal modeling is done according to ISO 15099 standard, which is described in the Window Heat Balance Calculation section with the addition of deflection and vacuum glazing systems modeling and some modifications to shading layer algorithms, which is described in Shading Device Thermal Model section. Optical caclulations in this method are done using Bidirectional Scattering Distribution Function (BSDF) approach.  The concept behind BSDF is based on the definition of descrete set of incident and outgoing angles, which fully describes optical performance of any system, simple or complex, limited only by the resolution of angular discretization.  In this method each layer, as well as the whole system is described by a matrix of incident and outgoing angles.
-
-#### Complex Fenestration Solar-Optical Calculations
-
-##### **Solar radiation calculation outline**
-
-For solar radiation calculations, each of the layers as well as entire glazing system can be represented with the set of Bi-directional Scattering Distribution Functions or BSDF, consisting of Bi-directional Reflectance Distribution Function or BRDF and Bi-directional Transmittance Distribution Function or BTDF.  Each function is a matrix 145 x 145 that describes reflectance or transmittance distribution in the outgoing hemisphere for each incident angle in the incidence hemisphere.  For each function there is forward and back matrix, for a total of 4 145 x 145 matrices.  Depending on the purpose of calculations, description of entire glazing system is divided into solar and visible spectrum, which means that there can be 8 matrices describing visible and complete solar spectrums.  Reflectance and transmittance being non-dimnsional ratios of reflected or transmitted energy over incident energy, in order to get total reflected and transmitted energy it is necessary to supply vector of incident solar energy, which usually consists of direct and diffuse radition.Specifics of calculations of direct and diffuse solar radiationis be described in some detail in oncoming chapters.
-
-###### **Scattering (Non-Specular) Glazing and Shading Devices**
-
-A general scattering fenestration system is characterized by BTDFs and BRDFs, which were described above.  Given an incident direction ***p***<sup>(I)</sup>, and an incident irradiance *E*( ***p***<sup>(I)</sup>), the transmitted radiance in the outgoing direction ***p***<sup>(T)</sup> is
-
-<div>$$S({{\bf{p}}^{{\rm{(T)}}}}) = {\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})dE({{\bf{p}}^{{\rm{(I)}}}})$$</div>
-
-where the function T is the BTDF.  In the absence of a source of effectively plane-parallel incident radiation (such as direct sunlight) d*E(**p***<sup>(I)</sup>*)* is an infinitesimal quantity, and the right side of the equation must be summed over the irradiance from all incident directions to produce the outgoing radiance:
-
-<div>$$S({{\bf{p}}^{{\rm{(T)}}}}) = \int {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})\frac{{dE({{\bf{p}}^{{\rm{(I)}}}})}}{{d\Omega }}d\Omega } $$</div>
-
-A similar equation gives the reflected radiance in the direction ***p***<sup>(R)</sup>:
-
-<div>$$S({{\bf{p}}^{{\rm{(R)}}}}) = \int {{\mathop{\rm R}\nolimits} ({{\bf{p}}^{{\rm{(R)}}}},{{\bf{p}}^{{\rm{(I)}}}})\frac{{dE({{\bf{p}}^{{\rm{(I)}}}})}}{{d\Omega }}d\Omega } $$</div>
-
-We can express the irradiance in terms of the exterior luminance, S, in that direction,
-
-<div>$$dE({{\bf{p}}^{{\rm{(I)}}}})dA = {S^{{\rm{(I)}}}}({{\bf{p}}^{{\rm{(I)}}}})\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}dA$$</div>
-
-![Calc Outl Fig 1](media/image1271.png)
-
-Figure 90. Irradiance geometry
-
-which allows one to express the transmittance of exterior radiation to produce the total outgoing radiance from the fenestration into the room in a particular direction:
-
-<div>$$S({{\bf{p}}^{{\rm{(T)}}}}) = \int\limits_{{\Omega ^{{\rm{(I)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(I)}}}}({{\bf{p}}^{{\rm{(I)}}}})\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} $$</div>
-
-The negative sign is added to account for the fact that ***p***<sup>(I)</sup> and ***n*** have opposite sign for incoming radiation.
-
-The radiance in equation is emitted from the back side of the element of area shown in Figure 90.  Considering a second surface, viewing the back side of the fenestration system, we can use equation to calculate the irradiance on surface 2,
-
-<div>$${E^{{\rm{(2)}}}}({{\bf{p}}^{{\rm{(T)}}}})d{A^{{\rm{(2)}}}} = {S^{{\rm{(T)}}}}({{\bf{p}}^{{\rm{(T)}}}})\left( { - {{\bf{p}}^{{\rm{(T)}}}}\cdot {{\bf{n}}^{{\rm{(2)}}}}} \right)d{\Omega ^{{\rm{(I,2)}}}}d{A^{{\rm{(2)}}}}$$</div>
-
-This expression, however, contains a number of new quantities, such as <span>\(d{\Omega ^{{\rm{(I,2)}}}}\)</span>, the element of solid angle for incoming radiation as seen from surface 2.  We can sort this out by referring to Figure 91 and making some changes and clarifications in notation.
-
-![](media/image1275.png)
-
-Figure 91. Radiation exchange between two surface elements
-
-In this figure we consider that surface 1 is the back side of the fenestration system, and surface 2 is some other surface in the room that receives the transmitted solar radiation through the fenestration system.  We consider infinitesimal elements *dA*<sup>(1)</sup> and *dA*<sup>(2)</sup> of the two surfaces, and define vector surface elements by *d**A*****<sup>(</sup>**<sup>1)</sup>=*dA*<sup>(1)</sup>***n***<sup>(1)</sup> and *d**A*****<sup>(</sup>**<sup>1)</sup>=*dA*<sup>(1)</sup>***n***<sup>(1)</sup>.  The quantity ***r*** in the figure denotes a vector pointing from surface 1 to surface 2, the magnitude of which is the distance *r* between the two surface elements.  This is used to define two unit vectors: <span>\({{\bf{\hat r}}^{{\rm{(1)}}}} = {{\bf{r}} \mathord{\left/ {\vphantom {{\bf{r}} r}} \right. } r}\)</span> is a unit vector pointing from surface element 1 to surface element 2, and <span>\({{\bf{\hat r}}^{{\rm{(2)}}}} =  - {{\bf{r}} \mathord{\left/ {\vphantom {{\bf{r}} r}} \right. } r}\)</span> is a unit vector pointing from surface element 2 back to surface element 1.  The unit vector ***p***<sup>(T)</sup> in equation is in fact <span>\({{\bf{\hat r}}^{{\rm{(1)}}}}\)</span>.  The shaded quadrilaterals in the figure are the projected area elements normal to ***r***.  Since the areas are infinitesimal, all the radiation leaving one surface element and arriving at the other will be in the direction ***r***, so that all radiation will be contained within the parallelepiped defined by the dashed lines (parallel to ***r***) joining the corners of the two surface elements.  It follows that the area *dA*<sup>(2)</sup>  is not independent of *dA*<sup>(1)</sup>.  The figure also shows the solid angle that has been denoted *d*W<sup>(I,2)</sup> above, which is the solid angle subtended by *dA*<sup>(1)</sup> as seen from *dA*<sup>(2)</sup> and is given by
-
-<div>$$d{\Omega ^{{\rm{(I,2)}}}} = \frac{{d{{\bf{A}}^{{\rm{(1)}}}} \cdot {{\bf{r}}^{{\rm{(1)}}}}}}{{{r^2}}}$$</div>
-
-The net power from surface element 1 to surface element 2 is
-
-<div>$${W^{(1 \to 2)}} = \left( {{S^{{\rm{(1)}}}}({{{\bf{\hat r}}}^{{\rm{(1)}}}}) - {S^{{\rm{(2)}}}}({{{\bf{\hat r}}}^{{\rm{(2)}}}})} \right)\frac{{\left( {d{{\bf{A}}^{{\rm{(1)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(1)}}}}} \right)\left( {d{{\bf{A}}^{{\rm{(2)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(2)}}}}} \right)}}{{{r^2}}}$$</div>
-
-where <span>\({S^{{\rm{(1)}}}}({{\bf{\hat r}}^{{\rm{(1)}}}})\)</span> is the radiance leaving surface element 1 in the direction of surface element 2, and vice-versa for <span>\({S^{{\rm{(2)}}}}({{\bf{\hat r}}^{{\rm{(2)}}}})\)</span>.  In this case, the latter is zero and the former is the quantity called *S*<sup>(T)</sup>(***p***<sup>(T)</sup>) above.  Given equation , we can recognize the quantity multiplying the radiance as the solid angle *d*W<sup>(I,2)</sup> times the projected area of surface element 2 perpendicular to ***r***.  But the expression is symmetrical in the two surface elements, so we could also express it as
-
-<div>$${W^{(1 \to 2)}} = {S^{{\rm{(T)}}}}({{\bf{p}}^{{\rm{(T)}}}})\left( {d{{\bf{A}}^{{\rm{(1)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(1)}}}}} \right)d{\Omega ^{{\rm{(T)}}}}$$</div>
-
-where
-
-<div>$$d{\Omega ^{{\rm{(T)}}}} = \frac{{\left( {d{{\bf{A}}^{{\rm{(2)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(2)}}}}} \right)}}{{{r^2}}}$$</div>
-
-The superscript (T) is used here because the solid angle element pertains to the direction ***p***<sup>(T)</sup>.  In the particular case under discussion that restricts attention to those directions for which the outgoing radiation strikes surface element 2.  We can now rewrite equation as
-
-<div>$${E^{{\rm{(2)}}}}({{\bf{p}}^{{\rm{(T)}}}})d{A^{{\rm{(2)}}}} = {S^{{\rm{(T)}}}}({{\bf{p}}^{{\rm{(T)}}}})\left( {{{\bf{n}}^{{\rm{(1)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(1)}}}}} \right)d{\Omega ^{{\rm{(T)}}}}d{A^{{\rm{(1)}}}}$$</div>
-
-and since, as can readily be seen from Figure 91, <span>\(\left( {d{{\bf{A}}^{{\rm{(1)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(1)}}}}} \right) = \left( {d{{\bf{A}}^{{\rm{(2)}}}} \cdot {{{\bf{\hat r}}}^{{\rm{(2)}}}}} \right)\)</span>, this becomes
-
-<div>$${E^{{\rm{(2)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = {S^{{\rm{(T)}}}}({{\bf{p}}^{{\rm{(T)}}}})\left( { - {{\bf{p}}^{{\rm{(T)}}}} \cdot {{\bf{n}}^{{\rm{(2)}}}}} \right)d{\Omega ^{{\rm{(T)}}}}$$</div>
-
-Substituting equation for *S*<sup>(T)</sup>(***p***<sup>(T)</sup>, we obtain a propagation equation for outside radiation passing through the window and arriving at surface element 2:
-
-<div>$$
-    E^{(2)}(\bf{p}^{(T)}) = \int_{\Omega^{(I)}} 
-      \rm T (\bf{p}^{(T)},\bf{p}^{(I)}) 
-      S^{(I)}(\bf{p}^{(I)})(-\bf{p}^{(I)}\cdot\bf{n}^{(I)})
-      d\Omega^{(I)}(-\bf{p}^{(T)}\cdot\bf{n}^{(2)})d\Omega^{(T)}
-$$</div>
-
-or, in terms involving only irradiance,
-
-<div>$${E^{{\rm{(2)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = \int\limits_{{\Omega ^{{\rm{(I)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})E({{\bf{p}}^{{\rm{(I)}}}})d{\Omega ^{{\rm{(I)}}}}} \left( { - {{\bf{p}}^{{\rm{(T)}}}} \cdot {{\bf{n}}^{{\rm{(2)}}}}} \right)d{\Omega ^{{\rm{(T)}}}}$$</div>
-
-Comparing these two equations with equations and , we can see that physically they represent the processes of (a) propagation of radiation outgoing at one surface (initially, the sky “surface�), where it is characterized by radiance, to incidence on a second surface, characterized by irradiance, followed (b) transmittance, which converts incoming radiation traveling in a given direction to outgoing radiation in a different set of directions, characterized again by radiance.  We can make the former of these processes explicit by defining a propagation function.  Considering the first surface element to be located at a position specified by the vector ***x***<sup>(1)</sup> and the second at ***x***<sup>(2)</sup>, then radiation leaving surface 1 in a direction ***p***<sup>(1)</sup> and arriving at surface 2 in a direction ***p***<sup>(2)</sup> produces an irradiance given by
-
-<div>$${E^{(2)}}({{\bf{p}}^{{\rm{(2)}}}}) = \int {L({{\bf{x}}^{{\rm{(2)}}}},{{\bf{p}}^{{\rm{(2)}}}};{{\bf{x}}^{{\rm{(1)}}}},{{\bf{p}}^{{\rm{(1)}}}}){S^{{\rm{(1)}}}}({{\bf{p}}^{{\rm{(1)}}}})} d{\Omega ^{{\rm{(1)}}}}$$</div>
-
-where the propagation function L is defined by
-
-<div>$$L({{\bf{x}}^{{\rm{(2)}}}},{{\bf{p}}^{{\rm{(2)}}}};{{\bf{x}}^{{\rm{(1)}}}},{{\bf{p}}^{{\rm{(1)}}}}) = \left( { - {{\bf{p}}^{{\rm{(2)}}}}\cdot {{\bf{n}}^{{\rm{(2)}}}}} \right)d{\Omega ^{{\rm{(2)}}}}\delta ({{\bf{p}}^{{\rm{(2)}}}},{{\bf{p}}^{{\rm{(1)}}}})\delta ({{\bf{x}}^{{\rm{(2)}}}},{{\bf{x}}^{{\rm{(1)}}}} + {\bf{r}})$$</div>
-
-The spatial dependence is inserted to guarantee that the geometrical relations in Figure 91 are preserved.  The delta functions in direction and spatial vectors are the mathematically standard d-distributions defined so that
-
-<div>$$\int {\delta ({{\bf{p}}^{{\rm{(2)}}}},{{\bf{p}}^{{\rm{(1)}}}})} f({{\bf{p}}^{{\rm{(1)}}}})d{\Omega ^{{\rm{(1)}}}} = f({{\bf{p}}^{{\rm{(2)}}}})$$</div>
-
-<div>$$\int\limits_\Omega  {\delta ({{\bf{p}}^{{\rm{(2)}}}},{{\bf{p}}^{{\rm{(1)}}}})d{\Omega ^{{\rm{(1)}}}}}  = \left\{ {\begin{array}{*{20}{c}}1&{{{\bf{p}}^{{\rm{(2)}}}} \in \Omega }\\0&{{{\bf{p}}^{{\rm{(2)}}}} \notin \Omega }\end{array}} \right.$$</div>
-
-<div>$$\int {\delta ({{\bf{x}}^{{\rm{(2)}}}},{{\bf{x}}^{{\rm{(1)}}}})} f({{\bf{x}}^{{\rm{(1)}}}})d{A^{{\rm{(1)}}}} = f({{\bf{x}}^{{\rm{(2)}}}})$$</div>
-
-<div>$$\int\limits_A {\delta ({{\bf{x}}^{{\rm{(2)}}}},{{\bf{x}}^{{\rm{(1)}}}})d{A^{{\rm{(1)}}}}}  = \left\{ {\begin{array}{*{20}{c}}1&{{{\bf{x}}^{{\rm{(2)}}}} \in A}\\0&{{{\bf{x}}^{{\rm{(2)}}}} \notin A}\end{array}} \right.$$</div>
-
-for an arbitrary function *f*.  [In equations and the integration is assumed to be over all possible values of either direction or position, so that the vectors ***p***<sup>(2)</sup> and ***x***<sup>(2)</sup> are necessarily within the domain of integration.]
-
-###### Physical Caveats
-
-In equations and the functions T and R pertain to the overall glazing system, and are assumed to be averaged over both wavelength and polarization with appropriate weightings.  [EnergyPlus considers wavelength only in that it distinguishes between radiation in the longwave thermal IR region and in the shortwave solar/visible region.  (In considering daylighting, there is a further limitation to the visible region.)  In this discussion we are concerned solely with the shortwave solar/visible region.]  While fenestration properties may depend on both wavelength and polarization, for externally incident radiation this dependence is taken into account in the calculation and averaging of T and R.  However, both the wavelength distribution (within the solar region) and the polarization state of the outgoing radiation will generally be different from that of the incident radiation.  This is not a feature peculiar to non-specular fenestration systems; it is also true of specular ones, and may in fact be more important there.  For most interior surfaces, where the radiation is either absorbed or diffusely reflected (and where both processes are assumed wavelength and polarization independent), this is of no importance, but in the case of either interior windows or the back-reflectance from exterior windows, it could in principle cause errors, unless proper account is taken in specifying T and R for these cases.
-
-###### Discretization: The LBNL Method
-
-A series of 6 papers (Papamichael, Klems et al. 1988; Klems 1994A; Klems 1994B; Klems and Warner 1995; Klems and Kelley 1996; Klems, Warner et al. 1996) formulated the LBNL method of characterizing scattering fenestration systems.  The relevant aspects of that method will be summarized here.  This method has been incorporated into the WINDOW (from LBNL 2012) computer program.
-
-The method begins by approximating the integrals in equations and by finite sums.  It does this by defining a set of finite solid angle elements {<span>\(\Delta {\Omega_i} \)</span>} that covers the relevant solid angle hemisphere (whether incident, transmitted or reflected directions).  Each solid angle element is characterized by a direction ***p****<sub>i</sub>*, and it is assumed that this may be substituted for any direction within the solid angle element.  This set of solid angle elements and corresponding directions is termed a basis.  Note that, since ***p****<sub>i</sub>* is a two-dimensional vector, enumerating the solid angle elements with a single index *i* implicitly includes specifying an ordering of the direction vectors.  Equation then becomes
-
-<div>$$S({{\bf{p}}_j}^{{\rm{(T)}}}) = \sum\limits_i {{\mathop{\rm T}\nolimits} ({{\bf{p}}_j}^{{\rm{(T)}}},{{\bf{p}}_i}^{{\rm{(I)}}}){S^{{\rm{(I)}}}}({{\bf{p}}_i}^{{\rm{(I)}}})\left( { - {{\bf{p}}_i}^{{\rm{(I)}}}\cdot {\bf{n}}} \right)\Delta {\Omega_i}^{{\rm{(I)}}}} $$</div>
-
-and equation becomes
-
-<div>$${E^{(2)}}({{\bf{p}}_j}^{{\rm{(2)}}}) = \sum\limits_i {\int\limits_{\Delta {\Omega_i}} {L({{\bf{x}}^{{\rm{(2)}}}},{{\bf{p}}_j}^{{\rm{(2)}}};{{\bf{x}}^{{\rm{(1)}}}},{{\bf{p}}_i}^{{\rm{(1)}}}){S^{{\rm{(1)}}}}({{\bf{p}}_i}^{{\rm{(1)}}})d{\Omega ^{{\rm{(1)}}}}} } $$</div>
-
-Referring to the definition of the propagation function in equation and properties of the d-distribution in equation , we see that the integrals in the summation will all be zero, except when ***p****<sub>j</sub>*<sup>(2)</sup> is contained in the solid angle element DW*<sub>i</sub>*.  In that case the integration produces ***p****<sub>i</sub>*<sup>(1)</sup>= ***p****<sub>j</sub>*<sup>(2)</sup>.  We can retain the formal summation by utilizing the finite-dimensional form of the d-distribution, known as the Kronicker delta, d*<sub>ij</sub>*:
-
-<div>$${\delta_{ij}} = \left\{ {\begin{array}{*{20}{c}}1&{i = j}\\0&{i \ne j}\end{array}} \right.$$</div>
-
-Then the integral becomes
-
-<div>$$\int\limits_{\Delta {\Omega_i}} {L({{\bf{x}}^{{\rm{(2)}}}},{{\bf{p}}_j}^{{\rm{(2)}}};{{\bf{x}}^{{\rm{(1)}}}},{{\bf{p}}_i}^{{\rm{(1)}}}){S^{{\rm{(1)}}}}({{\bf{p}}_i}^{{\rm{(1)}}})d{\Omega ^{{\rm{(1)}}}}}  = \lambda ( - {{\bf{p}}_j}^{{\rm{(2)}}}){\delta_{ij}} \cdot \delta ({{\bf{x}}^{{\rm{(2)}}}},{{\bf{x}}^{{\rm{(1)}}}} + {\bf{r}})$$</div>
-
-where the function *l* is defined as
-
-<div>$${\lambda ^{{\rm{(s)}}}}({{\bf{p}}_j}) = \left( {{{\bf{p}}_j}\cdot {{\bf{n}}^{{\rm{(s)}}}}} \right)\Delta {\Omega_j}$$</div>
-
-and the superscript (s) refers to the surface.
-
-The LBNL method, which focuses on glazing systems consisting of plane-parallel layers, makes particular assumptions that allow one to ignore the spatial dependence of L.  Since the only effect of the function <span>\(\delta ({{\bf{x}}^{{\rm{(2)}}}},{{\bf{x}}^{{\rm{(1)}}}} + {\bf{r}})\)</span> in equation is to require that if the expression is formally integrated over two separate surface areas, only the parts of the integration that satisfy the geometric constraints will contribute (in effect, the integration is over only one of the surfaces), we will drop the spatial dependence in the present discussion and replace it later when we consider the total energy transfer between different surfaces.
-
-Equations (without the delta distribution in ***x***) and are then considered to define the components of a diagonal matrix,
-
-<div>$$\begin{array}{*{20}{c}}{{\bf{\Lambda }^{{\rm{(s)}}}} = \left( {{\Lambda ^{{\rm{(s)}}}}_{ij}} \right)}&{{\rm{where}}}&{\Lambda_{ij}^{{\rm{(s)}}} = \left( {{{\bf{p}}_j}\cdot {{\bf{n}}^{{\rm{(s)}}}}} \right)\Delta {\Omega_j}{\delta_{ij}}}\end{array}$$</div>
-
-Considering the radiance in the various basis directions to be the components of a vector,
-
-<div>$$
-  \bf{S} = \left( 
-    \begin{array}
-      S_1 \\ ... \\ S_j \\ ...
-    \end{array}
-  \right)
-  \text{where}
-  S_j = S(\bf{p}_j)
-$$</div>
-  
-equation becomes
-
-<div>$$\begin{array}{*{20}{c}}{{S^{{\rm{(T)}}}}_j = \sum\limits_i {{T_{ji}}} \sum\limits_k {{\Lambda_{ik}}} {S_k}}&{{\rm{where}}}&{{T_{ji}} = {\mathop{\rm T}\nolimits} ({{\bf{p}}_j}^{{\rm{(T)}}},{{\bf{p}}_i}^{{\rm{(I)}}})}\end{array}$$</div>
-
-which has the obvious character of a series of matrix multiplications.  (Note that the superscript (T) here means transmitted, not the matrix operation transpose.)  Similarly, the reflectance matrix elements are
-
-<div>$${R_{ij}} = {\mathop{\rm R}\nolimits} ({{\bf{p}}^{{\rm{(R)}}}},{{\bf{p}}^{{\rm{(I)}}}})$$</div>
-
-The method then identifies the infinitesimal directional irradiances in equation with the components of an irradiance vector,
-
-<div>$$
-  E = \left( 
-    \begin{array}
-      E_1 \\ ... \\ E_i \\ ...
-    \end{array}
-  \right)
-  \text{where}
-  E_i = \frac{dE(\bf{p}_j)}{d\Omega}
-$$</div>
-
-and equations - can be rewritten as matrix equations,
-
-<div>$${{\bf{S}}^{{\rm{(T)}}}} = {\bf{T}} \cdot {{\bf{E}}^{{\rm{(I)}}}}$$</div>
-
-<div>$${{\bf{S}}^{{\rm{(R)}}}} = {\bf{R}} \cdot {{\bf{E}}^{{\rm{(I)}}}}$$</div>
-
-<div>$${{\bf{E}}^{{\rm{(I)}}}}{\bf{ = }}{\bf{\Lambda }^{{\rm{(I)}}}} \cdot {{\bf{S}}^{{\rm{(I)}}}}$$</div>
-
-<div>$${{\bf{S}}^{{\rm{(T)}}}}{\bf{ = T}} \cdot {\bf{\Lambda }^{{\rm{(I)}}}} \cdot {{\bf{S}}^{{\rm{(I)}}}}$$</div>
-
-(These are for radiation incident on the front surface of the fenestration; there is a similar set of equations for radiation incident on the back surface and propagating in an opposite sense to that in the above equations.)
-
-In the LBNL method, these equations are used extensively to calculate the overall properties of a fenestration system from those of its component layers.  Here we will assume that the components of the system property matrices are given at input.  These may be from a calculation by WINDOW or determined by some other method.  The quantities needed for each fenestration are:
-
-Table 34: Fenestration properties needed for the calculation
-
-
-
-
-
-
-
-
-
-
-
-Exterior Window
-
-<div>$$T_{ij}^F$$</div>
-
-Front Transmittance  matrix elements
-
-<div>$$R_{ij}^F$$</div>
-
-Back Reflectance matrix elements
-
-<div>$${\mathop{\rm A}\nolimits}_i^{F,n}$$</div>
-
-In-situ absorptance of n<sup>th</sup> layer for front incidence
-
-<div>$${\mathop{\rm A}\nolimits}_i^{B,n}$$</div>
-
-In-situ absorptance of n<sup>th</sup> layer for back incidence
-
-
-
-
-
-
-
-
-
-
-
-Interior Window
-
-<div>$$T_{ij}^F$$</div>
-
-Front Transmittance matrix elements
-
-<div>$$T_{ij}^B$$</div>
-
-Back Transmittance matrx elements
-
-<div>$$R_{ij}^F$$</div>
-
-Front Reflectance matrix elements
-
-<div>$$R_{ij}^B$$</div>
-
-Back Reflectance matrix elements
-
-<div>$${\mathop{\rm A}\nolimits}_i^{F,n}$$</div>
-
-In-situ absorptance of n<sup>th</sup> layer for front incidence
-
-<div>$${\mathop{\rm A}\nolimits}_i^{B,n}$$</div>
-
-In-situ absorptance of n<sup>th</sup> layer for back incidence
-
-
-
-The transmittance and reflectance are overall system properties.  (For daylighting calculations, one also needs the transmittance and reflectance averaged over the visible spectrum only; the quantities indicated in the table pertain to the entire solar spectrum.)  For the optical calculations we do not need to know anything about the individual layers making up the fenestration.  However, the thermal calculation of heat flow through the fenestration requires knowledge of the amount of radiation absorbed in each of the fenestration layers.  As indicated in the table, we therefore need the in-situ layer absorptance for each layer, referenced to the incident surface.  This is denoted <span>\({\mathop{\rm A}\nolimits}_i^{F,n}\)</span> for the fraction of the *i<sup>th</sup>* component of the irradiance incident on the front surface of the fenestration that is absorbed in layer *n*, with a similar quantity, <span>\({\mathop{\rm A}\nolimits}_i^{B,n}\)</span>, for irradiance incident on the back surface.  The term “in-situ layer absorptance� is used because these are not simply the absorptance of the layer, but include the transmittance and interreflection by other layers of the system prior to the absorptance in layer *n*.  The absorptance is a row vector, having possibly a different value for each direction of the incident irradiance, so that for an irradiance *E<sub>i</sub><sup>F</sup>* on the front surface of a fenestration and *E<sub>i</sub><sup>B</sup>* on the back surface, the power *Q<sup>n</sup>* absorbed per unit area in layer *n* would be
-
-<div>$${Q^n} = \sum\limits_i {{\mathop{\rm A}\nolimits}_i^{F,n}E_i^F}  + \sum\limits_j {{\mathop{\rm A}\nolimits}_j^{B,n}E_j^B} $$</div>
-
-(In the vector/matrix language, <span>\({Q^n} = {\bf{A}^{F,n}} \cdot {{\bf{E}}^F} + {\bf{A}^{B,n}} \cdot {{\bf{E}}^B}\)</span>)
-
-###### Bases and Coordinate Systems
-
-The introduction of a basis or multiple bases is a bit more complicated than indicated in the text preceding equation .  There for transmission we need coordinates describing incoming radiation on one surface of the physical layer and outgoing radiation at the second (opposite) surface, while reflection adds the need for coordinates describing outgoing radiation at the first surface.  Back transmittance and reflectance add the requirement for coordinates describing incoming radiation at the second surface.  The usual way of assigning coordinates to radiation involves specifying its line of propagation relative to the local surface normal. This means that there are separate coordinate systems for the first and second surfaces, and that, moreover, the description is different for incoming and outgoing radiation: for incoming radiation one is specifying a unit vector pointing toward the source of the radiation (*i*.*e*., antiparallel to the direction of propagation), while for outgoing radiation one is specifying a unit vector in the direction of propagation of the radiation.  In principle, then, one needs four coordinate systems or bases (for each physical layer), and the process of transmission or reflection involves a discontinuous transition between an input basis and an output basis.
-
-The LBNL method used by WINDOW uses a particular choice of coordinate systems in which incoming radiation at the first surface and outgoing radiation at the second are described by one coordinate system, while the same coordinate system reflected through the layer is used to describe incoming radiation at the second surface and outgoing radiation at the first.  The reason for this choice is that it greatly simplifies the matrix representations: specular transmittance or reflectance is always represented by a diagonal matrix, one can mix matrices representing forward or backward incidence processes, and all of the coordinate systems have propagation matrices with the same representation, so in effect there is one *L* matrix rather than four.
-
-The point of this discussion is that the components of the transmittance and reflectance matrices, and the layer absorptance vectors, depend on the definition of these four bases.  If they were generated by WINDOW, then they assume the particular coordinate system described above.  (If they were produced by some other means, they may be specified in yet some other coordinate system.)  While the LBNL coordinate system gives an intuitive description of outgoing radiation, as a description of incoming radiation it is very unintuitive.  And in any case, the coordinate system is different from that of EnergyPlus.  It will be necessary to translate the matrices and vectors into the correct EnergyPlus coordinate system.
-
-###### Matching the WINDOW6 Calculation to EnergyPlus
-
-It is useful to have some sense of how well the basis normally used in WINDOW calculations matches the requirements of EnergyPlus.  In using a BSDF window, a user would presumably be interested in the directionality of the transmitted radiation; if the size of the solid angle bins in the basis is large compared to the solid angle subtended by the typical surface in a zone, then that directional information will be lost.  On the other hand, if the bins are very small compared to this solid angle, then (since EnergyPlus does not consider the spatial variations within a surface) the directions are being oversampled.  Since the calculation time will be proportional to the number of matrix elements, which is the square of the number of basis directions, oversampling is to be avoided.
-
-Because of the great variety of buildings that may be modeled with EnergyPlus, and because the user has control over the basis for the BSDF properties, it is not possible to answer this question in a definitive way.  Here we consider the effect of the normal WINDOW basis in a typical perimeter office space, 10 ft wide, 15 ft deep and 11 ft high.  It is assumed to have a window 9 ft wide by 6 ft high, with the sill height 3 ft.  The window is placed to have a 4 in inner reveal.
-
-The normal WINDOW “full� basis has 145 output directions.  Figure 92 shows how the window and the solid angle bin project onto the inner surfaces for three of those directions.  In each case the solid angle bin is projected from the window center, and the window edges are projected along the central ray.
-
-In general, the basis appears to be reasonably matched to the calculation, with neither a loss of angular detail nor great oversampling.
-
-![](media/image1326.png)
-
-Figure 92. Transmitted Radiation in Three Directions for a Perimeter Office.  (a) q=0º; (b) q=40º, f=15º; (c) q=70º, f=67.5º.  q and f are the normal spherical angle coordinates in a right-handed coordinate system where y points up and z is normal to the window p
-
-###### Complex Fenestrations in EnergyPlus
-
-Exterior
-
-EnergyPlus models the exterior radiance in two parts, a moving sun radiance <span>\({S^{{\rm{(Sun)}}}}(t)\Delta {\Omega ^{{\rm{(Sun)}}}}\)</span> and a constant-shape direction-dependent sky radiance <span>\({S^{{\rm{(Sky)}}}}({\bf{p}},t)\)</span>.  The intensities of these vary with time.  For the solar radiation there is a single sky radiance model.  For daylight calculations the treatment is similar for exterior luminance, except that there are a number of user-selectable sky luminance models.  Here we will discuss radiance; the treatment of luminance is analogous.
-
-The direct normal solar intensity (at a given time) is
-
-<div>$${I^{{\rm{(D)}}}}(t) = {S^{{\rm{(Sun)}}}}(t)\Delta {\Omega ^{{\rm{(Sun)}}}}$$</div>
-
-and if we let
-
-<div>$${S^{{\rm{(Sky)}}}}({\bf{p}},t) = {I^{{\rm{(Sky)}}}}(t)s({\bf{p}})$$</div>
-
-where the shape function for the sky radiance model, *s*, is defined so that
-
-<div>$$\int\limits_{2\pi } {s({\bf{p}})d\Omega }  = 1$$</div>
-
-then the global solar irradiance on a horizontal surface at a given time is
-
-<div>$${I^{{\rm{(G)}}}}(t) = {I^{{\rm{(Sky)}}}}(t)\left( {1 - \int\limits_{\Delta {\Omega ^{{\rm{(Sun)}}}}} {s({\bf{p}})d\Omega } } \right) + {I^{{\rm{(D)}}}}(t)\cos {\theta ^{{\rm{(Sun)}}}}(t)$$</div>
-
-It must be understood that in equation the integration region 2p means integration over the sky hemisphere, and that *s(**p**)* is zero for upward-going directions.
-
-With the sky radiance shape *s(**p**)* specified in the EnergyPlus code, the angular size of the sun <span>\(\Delta {\Omega ^{{\rm{(Sun)}}}}\)</span> known, and the solar zenith angle <span>\({\theta ^{{\rm{(Sun)}}}}(t)\)</span> calculated in the code, the two hourly input quantities *I*<sup>(D*)*</sup>*(t)* and *I*<sup>(G)</sup>*(t)* determine the exterior radiance for any given hour.
-
-In this context, the transmitted radiance for a complex fenestration system given in equation becomes
-
-<div>$$\begin{array}{c}S({{\bf{p}}^{{\rm{(T)}}}}) = {I^{({\bf{Sky}})}}(t)\int\limits_{{\Omega ^{{\rm{(Sky)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})s({{\bf{p}}^{{\rm{(I)}}}})\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} \\ + \int\limits_{{\Omega ^{{\rm{(Gnd)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(Gnd)}}}}({{\bf{p}}^{{\rm{(I)}}}},t)\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} \\ + H\left( {\Delta {\Omega ^{{\rm{(Sun)}}}}(t) \not\subset {\Omega ^{{\rm{(Sf)}}}}} \right)\int\limits_{\Delta {\Omega ^{{\rm{(Sun)}}}}(t)} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(Sun)}}}}({{\bf{p}}^{{\rm{(I)}}}},t)\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} \\ + \int\limits_{{\Omega ^{{\rm{(Sf)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(Refl)}}}}({{\bf{p}}^{{\rm{(I)}}}},t)\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} \end{array}$$</div>
-
-where the incoming hemisphere viewed by the fenestration has been broken up into four parts.  The viewed sky (excluding the part containing the sun) is <span>\({\Omega ^{{\rm{(Sky)}}}}\)</span>, the viewed ground is <span>\({\Omega ^{{\rm{(Gnd)}}}}\)</span>, the part subtended by the sun is DW<sup>(Sun)</sup>, and the part subtended by one or more exterior surfaces (shading or reflecting objects) is W<sup>(Sf)</sup>.  These solid angles must exclude the exterior surfaces.  The symbol *H* represents a Helmholtz function: Its value is one if its logical argument is true, zero otherwise.  It has been inserted into the equation to account for those times when the sun is behind an exterior object.  Where there are multiple exterior shading or reflecting objects, W<sup>(Sf)</sup> may consist of several regions that may be disjoint or connected, depending on the exterior geometry.  As indicated in the equation, DW<sup>(Sun)</sup> is time-dependent, to account for the sun’s movement; W<sup>(Gnd)</sup> and W<sup>(Sf)</sup>  are fixed, but as written <span>\({\Omega ^{{\rm{(Sky)}}}}\)</span> has a time dependence induced by the exclusion of the solid angle subtended by the sun.  So that we can discuss the parts separately, we break the outgoing radiance down by source:
-
-<div>$$S({{\bf{p}}^{{\rm{(T)}}}}) = {S^{{\rm{(Sky)}}}}({{\bf{p}}^{{\rm{(T)}}}}) + {S^{{\rm{(Gnd)}}}}({{\bf{p}}^{{\rm{(T)}}}}) + {S^{{\rm{(Sun)}}}}({{\bf{p}}^{{\rm{(T)}}}}) + {S^{{\rm{(Sf)}}}}({{\bf{p}}^{{\rm{(T)}}}})$$</div>
-
-By subtracting the radiation from the part of the sky hidden by the sun from <span>\({S^{{\rm{(Sun)}}}}\)</span> and adding it back into *S*<sup>(Sky)</sup> we can remove the time dependence of W<sup>(Sky)</sup>:
-
-<div>$$\begin{array}{c}{S^{{\rm{(Sun)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = H\left( {\Delta {\Omega ^{{\rm{(Sun)}}}}(t) \not\subset {\Omega ^{{\rm{(Sf)}}}}} \right)\\ \times \int\limits_{\Delta {\Omega ^{{\rm{(Sun)}}}}(t)} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})\left[ {{S^{{\rm{(Sun)}}}}({{\bf{p}}^{{\rm{(I)}}}},t) - {I^{({\bf{Sky}})}}(t)s({{\bf{p}}^{{\rm{(I)}}}})} \right]\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} \end{array}$$</div>
-
-<div>$${S^{{\rm{(Sky)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = {I^{({\bf{Sky}})}}(t)\int\limits_{{\Omega ^{{\rm{(Sky)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}})s({{\bf{p}}^{{\rm{(I)}}}})\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} $$</div>
-
-Now in equation the integral is to be evaluated without regard to the sun position, and therefore <span>\({\Omega ^{{\rm{(Sky)}}}}\)</span> is time-independent.
-
-We can further simplify equation by noting that the angular size of the sun is small, and both *s*(***p***<sup>(I)</sup>) and T(***p***<sup>(T)</sup>, ***p***<sup>(I)</sup>) can be considered as constant over the range of directions in DW<sup>(Sun)</sup>.  We can therefore evaluate them at the direction ***p***<sup>(Sun)</sup>(t) of the center of the sun and move them out of the integration, resulting in
-
-<div>$${S^{{\rm{(Sun)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = {\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(Sun)}}}})\left[ {{I^{{\rm{(D)}}}} - {I^{{\rm{(Sky)}}}}s({{\bf{p}}^{{\rm{(Sun)}}}})\Delta {\Omega ^{{\rm{(Sun)}}}}} \right]\cos {\theta ^{{\rm{(Sun)}}}}H\left( {{{\bf{p}}^{{\rm{(Sun)}}}} \not\subset {\Omega ^{{\rm{(Sf)}}}}} \right)$$</div>
-
-In this equation we have dropped the explicit time dependence, but ***p***<sup>(Sun)</sup>, *q*<sup>(Sun)</sup>, *I*<sup>(D)</sup>, and *I*<sup>(Sky)</sup> are time-varying, while DW<sup>(Sun)</sup> is simply the constant angular size of the sun.
-
-We separate the reflected radiance *S*<sup>(Sf)</sup> into separate components for each surface,
-
-<div>$${S^{{\rm{(Sf)}}}} = \sum\limits_n {{S^{{\rm{(Sf, n)}}}}} $$</div>
-
-The individual shading surface reflected radiances are then
-
-<div>$${S^{{\rm{(Sf, n)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = \int\limits_{{\Omega ^{{\rm{(Sf, n)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(Refl, n)}}}}({{\bf{p}}^{{\rm{(I)}}}},t)\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} $$</div>
-
-The solid angle of integration in this expression is subtended by the portion of the exterior reflecting surface *n* viewed by the fenestration; if one surface lies behind another, the hidden part of its surface is removed from the solid angle it subtends.  This is summarized by the requirement
-
-<div>$$\begin{array}{l}{\Omega ^{{\rm{(Sf)}}}} = \bigcup\limits_n {{\Omega ^{{\rm{(Sf, n)}}}}} \\\bigcap\limits_n {{\Omega ^{{\rm{(Sf, n)}}}}}  = 0\end{array}$$</div>
-
-(This requirement will need to be modified to handle the case of transmitting exterior surfaces.)
-
-*S*<sup>(Refl,n)</sup> is time dependent because the incident radiation on the surface depends on the sun position. * *Equation must be evaluated after the exterior surface shading or reflectance calculations, in order to enforce the requirement that
-
-<div>$${\Omega ^{{\rm{(Sky)}}}} \cap {\Omega ^{{\rm{(Sf)}}}} = 0$$</div>
-
-Finally, the transmitted radiance from the ground-reflected exterior radiation is
-
-<div>$${S^{{\rm{(Gnd)}}}}({{\bf{p}}^{{\rm{(T)}}}}) = \int\limits_{{\Omega ^{{\rm{(Gnd)}}}}} {{\mathop{\rm T}\nolimits} ({{\bf{p}}^{{\rm{(T)}}}},{{\bf{p}}^{{\rm{(I)}}}}){S^{{\rm{(Gnd)}}}}({{\bf{p}}^{{\rm{(I)}}}},t)\left( { - {{\bf{p}}^{{\rm{(I)}}}}\cdot {\bf{n}}} \right)d{\Omega ^{{\rm{(I)}}}}} $$</div>
-
-Here, not only is there the requirement that
-
-<div>$${\Omega ^{{\rm{(Gnd)}}}} \cap {\Omega ^{{\rm{(Sf)}}}} = 0$$</div>
-
-but also the incident radiation on the ground may be affected by shading or reflection from exterior surfaces.  Since this is dependent on the sun position, *S*<sup>(Gnd)</sup> is time dependent, as indicated in equation .
-
-Applying the discretization of the previous section and the definitions in equations -, we can rewrite equation as
-
-<div>$${S_j}^{{\rm{(T,Sky)}}} = {I^{({\bf{Sky}})}}(t)\sum\limits_{i \in {\Omega ^{{\rm{(Sky)}}}}} {{T_{ji}}{\Lambda_{ii}}{s_i}} $$</div>
-
-where
-
-<div>$${s_i} = s({{\bf{p}}_i}^{{\rm{(I)}}})$$</div>
-
-is the sky radiance shape factor evaluated at the central direction of the i<sup>th</sup> solid angle bin.  A “T� superscript has been added on the left-hand side of the equation to denote that *S* is the transmitted outgoing radiance (due to incident sky radiation for the fenestration under discussion).  The stipulation <span>\(i \in {\Omega ^{{\rm{(Sky)}}}}\)</span> on the summation means that the sum is to include only those solid angle elements for which the sky is viewed by the fenestration.  This is essentially a shading calculation, in addition to a restriction to downward-going incident directions.  We anticipate the result of this calculation by defining a sky geometric factor:
-
-<div>$$
-  V_i^{(Sky)} = \left\{
-    \begin{array}
-      1                      & \text{all of } \Delta\Omega_i \text{ views sky for all of fenestration} \\
-      \text{viewed fraction} & \text{some of } \Delta\Omega_i \text{, fenestration views sky} \\
-      0                      & \text{none of } \Delta\Omega_i \text{ views sky for any part of fenestration
-$$</div>
-
-Then we can carry out the summation over all downward directions and write
-
-<div>$${S_j}^{{\rm{(T,Sky)}}} = {I^{({\bf{Sky}})}}(t)\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sky)}}}{s_i}} $$</div>
-
-Similarly, equation becomes
-
-<div>$${S_j}^{{\rm{(T, Sf, n)}}} = \sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}{S^{{\rm{(Refl, n)}}}}({{\bf{p}}_i}^{{\rm{(I)}}},t)} $$</div>
-
-where *V<sub>i</sub>*<sup>(Sf,\\ n)</sup> is another geometric view factor, defined analogously to equation , giving the fraction of the solid angle <span>\(\Delta {\Omega_i}\)</span> that views the exterior surface *n*.  Note that
-
-<div>$$V_i^{{\rm{(Sky)}}} + \sum\limits_{\rm{n}} {V_i^{{\rm{(Sf, n)}}}}  = 1$$</div>
-
-The quantity <span>\(S^{(Refl,n)} (\bf{p}_i^{(I)},t)\)</span> is in fact the reflected radiance at a particular location on the n<sup>th</sup> exterior surface—the location where the direction ***p****<sub>i</sub>*<sup>(I)</sup> intersects the surface.  (This statement will become more precise when the spatial dependence dropped from equation is re-inserted.)  This surface is assumed to have either a diffuse reflectance *r*<sup>(n)</sup> or a specular reflectance *r*<sup>(sp,\\ n)</sup>.  (Both properties are possible simultaneously, but EnergyPlus assumes that an exterior surface is either diffusing or specular, but not both.)  The reflectance is assumed uniform over the surface, but the particular location (effectively, the image of the fenestration projected onto surface n) may or may not view the sky, or, at a particular time, the sun.  We denote the incident irradiance of the surface n by <span>\(E_i^n\)</span>.  This irradiance pertains only to the surface n (in the present EnergyPlus calculation) and is independent of the fenestration or its basis.  We attach the subscript i simply as a reminder that (2) the irradiance pertains to the portion of the surface that is viewed by the solid angle element <span>\(\Delta {\Omega_i}\)</span> of the fenestration f (which would become important if the EnergyPlus shading calculations were modified to relax the assumption of uniform incident irradiance on exterior surfaces) and that the irradiance pertains only to those surfaces n that are viewed by the solid angle element i.  For specularly reflecting surfaces, we make the following definitions: First, within the set of basis solid angles <span>\(\Delta {\Omega_i}\)</span>, let s(*t*) identify the one containing the sun direction at time *t*, and let r(*t*) identify the one containing the specular reflection direction of the sun at time *t*.  We then define a contingent direct beam irradiance, which we denote by <span>\(E_{i{\rm{ }}r(t)}^{(D,n)}\)</span>. This irradiance is non-zero only if <span>\(i = r(t)\)</span>this direction is such that i is the specularly reflected direction for the surface n.  If this is the case, then <span>\(E_{i=r(t)}^{(D,n)}\)</span> is the incident direct beam irradiance.  With this definition,
-
-<div>$${S^{{\rm{(Refl, n)}}}}({{\bf{p}}_i}^{{\rm{(I)}}},t) = {\rho ^{{\rm{(sp, n)}}}}E_{i{\rm{ }}r(t)}^{(D,n)} + {\rho ^{{\rm{(n)}}}}E_i^n$$</div>
-
-If we then define normalized irradiance factors *U* by <span>\(E_i^n = U_i^{(Sky,n)}{I^{(Sky)}}(t) + U_{i{\rm{ }}Sun(tsh)}^{(D,n)}{I^{(D)}}(t)\)</span> and <span>\(E_{i{\rm{ }}r(t)}^{(D,n)} = U_{i{\rm{ }}r(t)}^{(D,n)}{I^{(D)}}(t)\)</span>, where <span>\(U_{i{\rm{ }}Sun(tsh)}^{(D,n)}\)</span> denotes the fraction of the beam solar that irradiates the surface for a given sun direction.  It is evaluated during the shading calculation, as indicated by the notation *Sun(tsh)*.  With these definitions we can rewrite the equation as
-
-<div>$$
-  S^{(Refl,n)}(\bf{p}_i^{(I)},t) = 
-  I^{(D)}(t) U_{i r(t)}^{(D,n)} \rho^{(sp,n)} +
-  I^{(D)}(t) U_{i Sun(tsh)}^{(D,n)} \rho^{(n)} +
-  I^{(sky)}(t) U_i^{(Sky,n)} \rho^{(n)}
-$$</div>
-
-and equation becomes, in terms of the incident irradiances,
-
-<div>$${S_j}^{{\rm{(T, Sf, n)}}} = \sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}\left( {{\rho ^{{\rm{(sp, n)}}}}E_{i{\rm{ }}r(t)}^{(D,n)} + {\rho ^{{\rm{(n)}}}}E_i^n} \right)} $$</div>
-
-and in terms of the normalized irradiance factors,
-
-<div>$$\begin{array}{c}{S_j}^{{\rm{(T, Sf, n)}}} = \sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}{I^{{\rm{(D)}}}}(t)U_{i{\rm{ r(}}t{\rm{)}}}^{{\rm{(D,n)}}}{\rho ^{{\rm{(sp, n)}}}}} \\ + \sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}\left[ {{I^{{\rm{(D)}}}}(t)U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}}{\rho ^{{\rm{(n)}}}} + {I^{(Sky)}}(t)U_i^{{\rm{(Sky,n)}}}{\rho ^{{\rm{(n)}}}}} \right]} \end{array}$$</div>
-
-The specularly reflected term can be removed from the sum, since only one value of i can contribute:
-
-<div>$${S_j}^{{\rm{(T, Sf, n)}}} = {T_{j{\rm{ r(}}t{\rm{)}}}}{\Lambda_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}}V_{{\rm{ r(}}t{\rm{)}}}^{{\rm{(Sf, n)}}}E_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}^{{\rm{(D,n)}}}{\rho ^{{\rm{(sp, n)}}}} + {\rho ^{{\rm{(n)}}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}E_i^n} $$</div>
-
-and
-
-<div>$$\begin{array}{c}{S_j}^{{\rm{(T, Sf, n)}}} = {T_{j{\rm{ r(}}t{\rm{)}}}}{\Lambda_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}}V_{{\rm{ r(}}t{\rm{)}}}^{{\rm{(Sf, n)}}}U_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}^{{\rm{(D,n)}}}{I^{(D)}}(t){\rho ^{{\rm{(sp, n)}}}}\\ + {\rho ^{{\rm{(n)}}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}\left( {{I^{{\rm{(D)}}}}(t)U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}} + U_i^{(Sky,n)}{I^{(Sky)}}(t)} \right)} \end{array}$$</div>
-
-which separates specular and diffuse reflectance from the exterior surfaces.
-
-With respect to shading and reflection of exterior radiation into the fenestration, the exterior reveal surfaces can be treated as additional diffusely reflecting exterior surfaces.
-
-Ground radiation is treated in the same way as radiation reflected from interior surfaces, except that one sums only over upward-going incident directions, and the ground is assumed to be diffusely reflecting.  The transmitted radiance from ground reflectance is
-
-<div>$${S_j}^{{\rm{(T, Gnd)}}} = {\rho ^{{\rm{(Gnd)}}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}E_i^{(Gnd)}} $$</div>
-
-In this equation, the symbol <span>\(E_i^{(Gnd)}\)</span> is shorthand for a spatial calculation.  The solid angle region <span>\(\Delta {\Omega_i}\)</span> views (from various points over the fenestration area) some spatial region of the ground.  The symbol <span>\(E_i^{(Gnd)}\)</span> denotes the incident irradiance on the ground over this spatial region.  In the absence of shading, this would be simply <span>\({I^{(G)}} = {I^{(Sky)}} + {I^{(D)}}\cos {\theta_{Sun}}\)</span>; shading requires a more complex calculation.  Currently the EnergyPlus code does a Monte-Carlo calculation: rays are randomly generated from the window, when they strike the ground a calculation is made to determine whether that point receives direct solar radiation and what portion of the sky it views (reflected radiation from surfaces is neglected).  Here we would perform that calculation for each region of the ground i viewed by a basis solid angle element, instead of generating random rays from the window.  We denote the results of that calculation by <span>\(E_i^{(Gnd)} = U_{i{\rm{ }}Sun(tsh)}^{(D,Gnd)}{I^{(D)}}(t) + U_i^{(Sky,Gnd)}{I^{(Sky)}}(t)\)</span>, where the *U*’s are average viewing factors for the sun and sky, calculated as part of the shading calculation (which is indicated by the subscript *tsh*: *Sun(tsh)* is the sun direction as specified by the shading calculation.  This then gives
-
-<div>$${S_j}^{{\rm{(T, Gnd)}}} = {\rho ^{{\rm{(Gnd)}}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}\left( {U_{i{\rm{ }}Sun(tsh)}^{(D,Gnd)}{I^{(D)}}(t) + U_i^{(Sky,Gnd)}{I^{(Sky)}}(t)} \right)} $$</div>
-
-The transmitted radiance from direct beam radiation is
-
-<div>$${S_j}^{{\rm{(T, Sun)}}} = {T_{j{\rm{ s}}(t)}}\cos {\theta ^{{\rm{(Sun)}}}}{I^{{\rm{(D)}}}}(t)V_{i{\rm{ s(}}t{\rm{)}}}^{{\rm{(D)}}}$$</div>
-
-This introduces yet one more geometric view factor: 
-
-<div>$$
-  V_{i s(t)}^(D)}
-$$</div> 
-
-is zero if the sun direction s*(t)* is not *i*; if *i*=s(*t*) it is the fraction of the fenestration area irradiated by the direct sun.  Equation uses the fact that the angular size of the sun is smaller than any basis solid angle element, and that EnergyPlus treats the sun and circumsolar region as a point source [hence the absence of the sky correction in equation ].
-
-At this point we have developed separate expressions for a fenestration’s  transmitted radiance in a particular direction depending on the exterior source of the radiation.  These expressions utilize the discretized BTDF of the fenestration in the form of transmittance matrix elements over an angular basis.  The exterior geometry is re-expressed in the form of geometric view factors in this basis.  In the process, the explicit time dependence of the exterior radiation has been reduced to the time-varying direct and diffuse solar intensities and the solar position.  The time dependence of the solar position, however, consists merely in specifying, for a particular time, which of the basis solid angle elements contains the solar direction.  The entire exterior geometry necessary for the fenestration transmittance calculation can therefore be pre-calculated.
-
-Interior
-
-We begin with the discretized form of equation , in which we also modify the surface notation.  In that equation, the surfaces involved are termed (1) and (2), where radiation is outgoing from surface 1 and incoming to surface 2.  Here radiation is outgoing from the inner surface of the fenestration, so we label that surface (f).  The receiving surface is one of the surfaces of the zone in which the fenestration is located.  We number those surfaces with the index *k*, so the receiving surface is labeled (*k*).  Equation then becomes
-
-<div>$$dW_j^{{\rm{(f}} \to k{\rm{)}}} = {E^{{\rm{(}}k{\rm{)}}}}({{\bf{p}}_j}^{{\rm{(T)}}})d{A^{{\rm{(}}k{\rm{)}}}} = {S_j}^{{\rm{(T)}}} \cdot \left( {{{\bf{n}}^{{\rm{(f)}}}} \cdot {{\bf{p}}_j}^{{\rm{(T)}}}} \right)\Delta {\Omega_j}^{{\rm{(T)}}}d{A^{{\rm{(f)}}}}$$</div>
-
-or, noting that <span>\( \left(\bf{n}^{(f)}\cdot\bf{p}_j^{(T)}\right) \Delta\Omega^{(T)} = \Lambda_{jj}^{(T)} \)</span> (where the superscript T is retained in case the incoming and outgoing bases are defined differently),
-
-<div>$$dW_j^{{\rm{(f}} \to k{\rm{)}}} = {E^{{\rm{(}}k{\rm{)}}}}({{\bf{p}}_j}^{{\rm{(T)}}})d{A^{{\rm{(}}k{\rm{)}}}} = {S_j}^{{\rm{(T)}}}\Lambda_{jj}^{{\rm{(T)}}}d{A^{{\rm{(f)}}}}$$</div>
-
-If we integrate this expression over the fenestration area *A*<sup>(f)</sup> we obtain the total power leaving the fenestration surface in direction *j*; however, all of that power may not reach surface *k*: some may strike the inner window reveal or a different zone surface.  If we define a spatial projection operator by
-
-<div>$${{\bf{x}}^{{\rm{(}}k{\rm{)}}}} = {{\mathop{\rm P}\nolimits} ^{{\rm{(}}k{\rm{)}}}}({\bf{p}}_j^{{\rm{(T)}}},{{\bf{x}}^{{\rm{(f)}}}}) \equiv {{\mathop{\rm P}\nolimits}_j}^{{\rm{(}}k{\rm{)}}}({{\bf{x}}^{{\rm{(f)}}}})$$</div>
-
-where ***x***<sup>(*k*)</sup> is in the plane of surface *k*, and a geometric form factor by
-
-<div>$$F_j^{{\rm{(}}k{\rm{)}}} = \frac{1}{{{A^{{\rm{(f)}}}}}}\int\limits_{{{\mathop{\rm P}\nolimits}_j}^{{\rm{(}}k{\rm{)}}}({{\bf{x}}^{{\rm{(f)}}}}) \in {A^{{\rm{(}}k{\rm{)}}}}} {d{A^{{\rm{(f)}}}}} $$</div>
-
-then
-
-<div>$$dW_j^{{\rm{(f}} \to k{\rm{)}}} = {S_j}^{{\rm{(T)}}}\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}{A^{{\rm{(f)}}}}$$</div>
-
-The total power leaving the fenestration (in any direction) and arriving at surface *k* is then
-
-<div>$$W_j^{{\rm{(f}} \to k{\rm{)}}} = \sum\limits_j {{S_j}^{{\rm{(T)}}}\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}{A^{{\rm{(f)}}}}} $$</div>
-
-Substituting equations , , , , into equation yields a series of expressions for the total power arriving at surface *k* (by transmission through fenestration f) from each of the sources of exterior radiation.  However, the equations for transmitted radiation describe an infinitesimal region, which means that the radiation in a given direction will always come from one source.  When one integrates the transmitted power over the fenestration surface, one encounters the problem that for this direction different parts of the fenestration area may receive radiation from different sources.  Also, for a given outgoing direction, the projection of a receiving surface back onto the fenestration may produce an image that covers only part of the fenestration area, and this image may not be identical with the part of the area that receives incident radiation from a particular source.  The most important origin of this problem is the existence of inner and outer window reveals, as illustrated in Figure 93.
-
-![](media/image1392.png)
-
-Figure 93. Mismatch of irradiated and viewed fenestration areas for different incident and outgoing directions
-
-In this figure, the portion of the fenestration area not viewed by the plane of surface *k* is instead viewed by one or more of the inner window reveals.  Similarly, the portion of the fenestration not irradiated in the figure is in fact irradiated by diffusely reflected radiation from the outer window reveals.  We can account for this by replacing the area *A*<sup>(f)</sup> in equation with the overlap area <span>\(A_{ji}^{{\rm{(f, Src), }}k}\)</span>* *(dark shaded in the figure), where “Src� stands for the source of the incident radiation.  This area is defined by
-
-<div>$$A_{ji}^{\left( {f,Src} \right),k} = \left. {A_i^{\left( {f,Src} \right)}} \right|A_j^{\left( f \right),k}$$</div>
-
-The total power at the interior surface *k* for each source of radiation then becomes
-
-<div>$${W^{{\rm{(Sky), }}k}} = {I^{({\bf{Sky}})}}(t)\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sky)}}}A_{ji}^{{\rm{(f, Sky), }}k}{s_i}} } $$</div>
-
-<div>$$\begin{array}{c}{W^{{\rm{(Sf,n)}},k}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(sp, n)}}}}\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}{T_{j{\rm{ r(}}t{\rm{)}}}}{\Lambda_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}}V_{{\rm{ r(}}t{\rm{)}}}^{{\rm{(Sf, n)}}}A_{j{\rm{ r(}}t{\rm{)}}}^{{\rm{(f, Sf, n), }}k}U_{{\rm{ r(}}t{\rm{) s(}}t{\rm{)}}}^{{\rm{(D,n)}}}} \\ + {I^{(D)}}(t){\rho ^{{\rm{(n)}}}}\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}A_{ji}^{{\rm{(f, Sf, n), }}k}U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}}} } \\ + {I^{(Sky)}}(t){\rho ^{{\rm{(n)}}}}\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}A_{ji}^{{\rm{(f, Sf, n), }}k}U_i^{{\rm{(Sky,n)}}}} } \end{array}$$</div>
-
-<div>$$\begin{array}{c}{W^{{\rm{(Gnd)}},k}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(Gnd)}}}}\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}A_{ji}^{{\rm{(f, Gnd), }}k}U_{i{\rm{ }}Sky(tch)}^{{\rm{(D, Gnd)}}}} } \\ + {I^{({\bf{Sky}})}}(t){\rho ^{{\rm{(Gnd)}}}}\sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}A_{ji}^{{\rm{(f, Gnd), }}k}U_i^{{\rm{( Sky,Gnd)}}}} } \end{array}$$</div>
-
-<div>$${W^{{\rm{(Sun)}},k}} = {I^{{\rm{(D)}}}}(t)\sum\limits_j {F_j^{{\rm{(}}k{\rm{)}}}\Lambda_{jj}^{{\rm{(T)}}}{T_{j{\rm{ s}}(t)}}\cos {\theta_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}}}V_{i{\rm{ s(}}t{\rm{)}}}^{{\rm{(D)}}}A_{j{\rm{ s(}}t{\rm{)}}}^{{\rm{(f, Sun), }}k}} $$</div>
-
-If we define a series of solar irradiation factors, Z, that describe the fraction of the radiation incident on the fenestration due to a given exterior radiation source that is ultimately incident on the interior surface *k*,
-
-<div>$${Z^{{\rm{(Sky), }}k}} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sky)}}}A_{ji}^{{\rm{(f, Sky), }}k}{s_i}} } $$</div>
-
-<div>$${Z_{{\rm{r(}}t{\rm{)}}}}^{{\rm{(sp, Sf, n)}},k} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}{T_{j{\rm{ r(}}t{\rm{)}}}}{\Lambda_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}}V_{{\rm{ r(}}t{\rm{)}}}^{{\rm{(Sf, n)}}}A_{j{\rm{ r(}}t{\rm{)}}}^{{\rm{(f, Sf, n), }}k}U_{{\rm{ r(}}t{\rm{) s(}}t{\rm{)}}}^{{\rm{(D,n)}}}} $$</div>
-
-<div>$${Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun, Sf, n)}},k} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}A_{ji}^{{\rm{(f, Sf, n), }}k}U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}}} } $$</div>
-
-<div>$${Z^{{\rm{(Sky, Sf, n)}},k}} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}down} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}A_{ji}^{{\rm{(f, Sf, n), }}k}U_i^{{\rm{(Sky, n)}}}} } $$</div>
-
-<div>$${Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(D, Gnd)}},k} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}A_{ji}^{{\rm{(f, Gnd), }}k}U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D, Gnd)}}}} } $$</div>
-
-<div>$${Z^{{\rm{(Sky, Gnd)}},k}} = \sum\limits_j {\Lambda_{jj}^{{\rm{(T)}}}F_j^{{\rm{(}}k{\rm{)}}}\sum\limits_{i{\rm{ }}up} {{T_{ji}}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}A_{ji}^{{\rm{(f, Gnd), }}k}U_i^{{\rm{(Sky, Gnd)}}}} } $$</div>
-
-<div>$${Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}},k} = \sum\limits_j {F_j^{{\rm{(}}k{\rm{)}}}\Lambda_{jj}^{{\rm{(T)}}}{T_{j{\rm{ s}}(t)}}\cos {\theta_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}}}V_{i{\rm{ s(}}t{\rm{)}}}^{{\rm{(D)}}}A_{j{\rm{ s(}}t{\rm{)}}}^{{\rm{(f, Sun), }}k}} $$</div>
-
-then equations through become
-
-<div>$${W^{{\rm{(Sky), }}k}} = {I^{({\bf{Sky}})}}(t){Z^{{\rm{(Sky), }}k}}$$</div>
-
-<div>$$\begin{array}{c}{W^{{\rm{(Sf,n)}},k}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(sp, n)}}}}{Z_{{\rm{r(}}t{\rm{)}}}}^{{\rm{(sp, Sf, n)}},k} + {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(n)}}}}{Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun, Sf, n)}},k}\\ + {I^{({\bf{Sky}})}}(t){\rho ^{{\rm{(n)}}}}{Z^{{\rm{(Sky, Sf, n)}},k}}\end{array}$$</div>
-
-<div>$${W^{{\rm{(Gnd)}},k}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(Gnd)}}}}{Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(D, Gnd)}},k} + {I^{({\bf{Sky}})}}(t){\rho ^{{\rm{(Gnd)}}}}{Z^{{\rm{(Sky, Gnd)}},k}}$$</div>
-
-<div>$${W^{{\rm{(Sun)}},k}} = {I^{{\rm{(D)}}}}(t){Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}},k}$$</div>
-
-The notation s(*t*) appearing in a subscript in several of the above equations refers to the basis direction for which the sun direction is contained in the basis solid angle element.  This is of course time dependent.  What is meant here is that at any given time the particular basis element containing the sun is to be picked out.  (If no basis element for the fenestration contains the sun at a given time, then the corresponding view factor—and therefore irradiance or absorption factor—is zero.)  It is therefore necessary to tabulate those quantities with an s(*t*) subscript for all basis directions *s* that could possibly contain the sun direction (and for *r(t)*, all basis directions that could possibly contain the reflected sun angle for the surface n).  This is a set considerably smaller than that of all incoming basis directions.  Figure 94 illustrates this point for direct irradiation of fenestrations in three different orientations in a building at a particular latitude, using the W6 full basis, which has 145 incoming directions.  In the worst case (west-facing) one only needs to consider around 50 of these, with much fewer needed in other orientations.  The specific numbers for a given fenestration will depend on the choice of basis, orientation and latitude.  The basis direction values can of course be interpolated where greater directional resolution is warranted.  In equation the specular direction r(*t*) is uniquely determined by the sun direction s(*t*), so the Z factor does not need an additional index for *s*.
-
-![](media/image1410.png)
-
-Figure 94. Sun Paths and Incident Basis for Three Window Orientations, 38º N. Latitude.  The nodal positions (blue dots) for a W6 full basis are compared with the summer solstice (red curve) and winter solstice (green curve) solar paths.  Solar paths for other days of the year will lie between these two extremes.  (Note: the basis points are to be interpreted as the direction of a vector pointing from the fenestration to the sun.)  (a) South facing.  (b) West facing.  (c) North facing (the winter path is off the figure (i.e., the window is shaded); allowed paths will be outside the red path.
-
-The reason for the definition of the Z factors is that to a great extent they can be precalculated, so that within the hourly calculation only equations - need to be used.  In addition, there are fewer Z factors to be stored than transmittance matrix elements.  The storage determinants for the foregoing calculations are summarized in the following table.
-
-Table 35: Determination of array sizes
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="2">Parameters</th>
-  </tr>
-  <tr>
-    <td>*N<sub>Basis</sub>*</td>
-    <td>Number of elements in the (incoming or outgoing) basis</td>
-  </tr>
-  <tr>
-    <td>*N<sub>Sun</sub>*</td>
-    <td>Number of basis directions that may be sun directions (depends on fenestration orientation</td>
-  </tr>
-  <tr>
-    <td>*<span>\(N_{Sun}^{(Gnd)}\)</span>*</td>
-    <td>Number of sun directions that give significantly different ground irradiation conditions, as seen by fenestration</td>
-  </tr>
-  <tr>
-    <td>*N<sub>Sf</sub>*</td>
-    <td>Number of reflecting surfaces viewable by fenestration (depends on fenestration orientation)</td>
-  </tr>
-  <tr>
-    <td><sup><span>\(N_{Sun}^{{\rm{(Sf, n)}}}\)</span></sup></td>
-    <td>Number of time steps for which surface *n* is sunlit (depends on orientation of surface *n*; determined during shading calculation)</td>
-  </tr>
-  <tr>
-    <td><sup><span>\(N_{Refl}^{{\rm{(Sf, n)}}}\)</span></sup></td>
-    <td>Number of basis directions that may be reflected sun directions from surface *n* (depends on orientation of fenestration and surface *n*).</td>
-  </tr>
-  <tr>
-    <td>*N<sub>IntSurf</sub>*</td>
-    <td>Number of interior surfaces in the zone containing the fenestration</td>
-  </tr>
-  <tr>
-    <td>*N<sub>Layers</sub>*</td>
-    <td>Number of thermal layers in the fenestration system</td>
-  </tr>
-  <tr>
-    <td colspan="2">Arrays</td>
-  </tr>
-  <tr>
-    <td><div>$$\begin{array}{*{20}{c}}{{\mathop{\rm A}\nolimits}_i^{F,l},}&amp;{{\mathop{\rm A}\nolimits}_i^{B,l}}\end{array}$$</div></td>
-    <td>Absorptance vector element; *N<sub>Basis</sub>*</td>
-  </tr>
-  <tr>
-    <td>*T<sub>ij</sub>*</td>
-    <td>Transmittance matrix element; *N<sub>Basis </sub>* X *N<sub>Basis</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$$V_i^{{\rm{(Sky)}}}$$</div></td>
-    <td>Sky viewed fraction; one-dimensional, *N<sub>Basis</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$$V_i^{{\rm{(Sf, n)}}}$$</div></td>
-    <td>Fraction of surface *n* viewed; *N<sub>Basis</sub>* X *N<sub>Sf</sub>*</td>
-  </tr>
-  <tr>
-    <td>*r*<sup>(n)</sup>,*r*<sup>(sp,\\ n)</sup></td>
-    <td>Surface *n* diffuse, specular reflectance; *N<sub>Sf</sub>*  (already stored by E+)</td>
-  </tr>
-  <tr>
-    <td><div>$$U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}}$$</div></td>
-    <td>Fraction of the image of <span>\(\Delta {\Omega_i}\)</span> on surface *n* that views the sun when it is in direction Sun(tsh); *N<sub>Basis</sub>* X *N<sub>Sf</sub>* X <span>\(N_{Sun}^{{\rm{(Sf, n)}}}\)</span></td>
-  </tr>
-  <tr>
-    <td><div>$$V_i^{{\rm{(Gnd)}}}$$</div></td>
-    <td>Fraction of <span>\(\Delta {\Omega_i}\)</span> that views ground; *N<sub>Basis</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$$U_i^{{\rm{(Sky, Gnd)}}}$$</div></td>
-    <td>Fraction of sky radiation received by the image of <span>\(\Delta {\Omega_i}\)</span> on the ground; *N<sub>Basis</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$$U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D, Gnd)}}}$$</div></td>
-    <td>Fraction of direct solar radiation for sun direction Sun(tsh) received by image of <span>\(\Delta {\Omega_i}\)</span> on ground; <span>\(N_{Sim}^{Gnd}\)</span>*<sub> </sub>*X *N<sub>Basis</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$$V_{i{\rm{ s(}}t{\rm{)}}}^{{\rm{(D)}}}$$</div></td>
-    <td>Fraction of fenestration area irradiated by direct solar radiation for direction *i*, given that sun angle is s(*t*); N*<sub>Sun</sub>* X *N<sub>Basis</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$$F_j^{{\rm{(}}k{\rm{)}}}$$</div></td>
-    <td>Fraction of radiation in direction *j* leaving fenestration interior that arrives at surface *k*; *N<sub>Basis</sub>* X *N<sub>IntSurf</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${Z^{{\rm{(Sky), }}k}}$$</div></td>
-    <td>Sky irradiation factor; *N<sub>IntSurf</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${Z_{{\rm{r(}}t{\rm{)}}}}^{{\rm{(sp, Sf, n)}},k}$$</div></td>
-    <td>Exterior surface specular irradiation factor; <span>\(N_{Sun}^{{\rm{(Sf, n)}}}\)</span>X *N<sub>Sf</sub>* X *N<sub>IntSurf</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun, Sf, n)}},k}$$</div></td>
-    <td>Exterior surface direct-diffuse irradiation factor; <span>\(N_{Sun}^{{\rm{(Sf, n)}}}\)</span> X *N<sub>Sf</sub>* X *N<sub>IntSurf</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${Z^{{\rm{(Sky, Sf, n)}},k}}$$</div></td>
-    <td>Exterior surface sky irradiation factor; *N<sub>Sf</sub>* X *N<sub>IntSurf</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(D, Gnd)}},k}$$</div></td>
-    <td>Ground-reflected direct solar irradiaton factor (given sun direction s(*t*)); <span>\(N_{Sun}^{Gnd}\)</span> X *N<sub>IntSurf</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${Z^{{\rm{(Sky, Gnd)}},k}}$$</div></td>
-    <td>Ground-reflected diffuse solar irradiation factor; *N<sub>IntSurf</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${Z_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}},k}$$</div></td>
-    <td>Direct solar irradiation factor; *N<sub>Sun</sub>* X *N<sub>IntSurf</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${K^{{\rm{(Sky), }}l}}$$</div></td>
-    <td>Sky absorption factor; *N<sub>Layers</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${K_{{\rm{r(}}t{\rm{)}}}}^{{\rm{(sp, Sf, n)}},l}$$</div></td>
-    <td>Exterior surface specular absorption factor; *N<sub>Sf</sub>* X <span>\(N_{Refl}^{{\rm{(Sf, n)}}}\)</span> X *N<sub>Layers</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun, Sf, n)}},l}$$</div></td>
-    <td>Exterior surface diffusely reflected direct sun absorption factor; *N<sub>Sf</sub>* X <span>\(N_{Sun}^{{\rm{(Sf, n)}}}\)</span> X *N<sub>Layers</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${K^{{\rm{(Sky, Sf, n)}},l}}$$</div></td>
-    <td>Exterior surface reflected sky radiation absorption factor;</td>
-  </tr>
-  <tr>
-    <td><div>$${K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(D, Gnd)}},l}$$</div></td>
-    <td>Ground-reflected direct solar absorption factor; <span>\(N_{Sun}^{(Gnd)}\)</span>X *N<sub>Layers</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${K^{{\rm{(Sky, Gnd)}},l}}$$</div></td>
-    <td>Ground-reflected sky radiation absorption factor; *N<sub>Layers</sub>*</td>
-  </tr>
-  <tr>
-    <td><div>$${K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}},l}$$</div></td>
-    <td>Direct sunlight absorption factor; *N<sub>Sun</sub>* X *N<sub>Layers</sub>*</td>
-  </tr>
-</table>
-
-###### Absorption
-
-For thermal calculations it is necessary to know the energy absorbed in each layer of the fenestration.  This depends only on the incident geometry, but otherwise is calculated in the same manner as the solar flux incident on interior surfaces.  For a given layer l of a fenestration f, we define a source-referenced absorption factor, K(source),l.  This is the amount of energy absorbed in layer l divided by the relevant solar intensity (which might be beam, diffuse, or reflected beam or diffuse, depending on the source of the radiation).  These absorption factors and the resultant source-specific absorbed solar powers are calculated by the analogs [see equation of equations through :
-
-<div>$${K^{{\rm{(Sky), }}l}} = {A^{{\rm{(f)}}}}\sum\limits_{i{\rm{ }}down} {{\mathop{\rm A}\nolimits}_i^{F,l}{\Lambda_{ii}}V_i^{{\rm{(Sky)}}}{s_i}} $$</div>
-
-<div>$${Q^{{\rm{(Sky), }}l}} = {I^{({\bf{Sky}})}}(t){K^{{\rm{(Sky), }}l}}$$</div>
-
-<div>$${K_{{\rm{r(}}t{\rm{)}}}}^{{\rm{(sp, Sf, n)}},l} = {A^{{\rm{(f)}}}}{\mathop{\rm A}\nolimits}_{r(t)}^{F,l}{\Lambda_{{\rm{ r(}}t{\rm{) r(}}t{\rm{)}}}}V_{{\rm{ r(}}t{\rm{)}}}^{{\rm{(Sf, n)}}}U_{{\rm{ r(}}t{\rm{) s(}}t{\rm{)}}}^{{\rm{(D,n)}}}$$</div>
-
-<div>$${K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun, Sf, n)}},l} = {A^{{\rm{(f)}}}}\sum\limits_{i{\rm{ }}down} {{\mathop{\rm A}\nolimits}_i^{F,l}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D,n)}}}} $$</div>
-
-<div>$${K^{{\rm{(Sky, Sf, n)}},l}} = {A^{{\rm{(f)}}}}\sum\limits_{i{\rm{ }}down} {{\mathop{\rm A}\nolimits}_i^{F,l}{\Lambda_{ii}}V_i^{{\rm{(Sf, n)}}}U_i^{{\rm{(Sky, n)}}}} $$</div>
-
-<div>$$\begin{array}{c}{Q^{{\rm{(Sf,n)}},l}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(sp, n)}}}}{K_{{\rm{r(}}t{\rm{)}}}}^{{\rm{(sp, Sf, n)}},l} + {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(n)}}}}{K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun, Sf, n)}},l}\\ + {I^{({\bf{Sky}})}}(t){\rho ^{{\rm{(n)}}}}{K^{{\rm{(Sky, Sf, n)}},l}}\end{array}$$</div>
-
-<div>$${K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(D, Gnd)}},l} = {A^{{\rm{(f)}}}}\sum\limits_{i{\rm{ }}up} {{\mathop{\rm A}\nolimits}_i^{F,l}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}U_{i{\rm{ }}Sun(tsh)}^{{\rm{(D, Gnd)}}}} $$</div>
-
-<div>$${K^{{\rm{(Sky, Gnd)}},l}} = {A^{{\rm{(f)}}}}\sum\limits_{i{\rm{ }}up} {{\mathop{\rm A}\nolimits}_i^{F,l}{\Lambda_{ii}}V_i^{{\rm{(Gnd)}}}U_i^{{\rm{(Sky, Gnd)}}}} $$</div>
-
-<div>$${Q^{{\rm{(Gnd)}},l}} = {I^{{\rm{(D)}}}}(t){\rho ^{{\rm{(Gnd)}}}}{K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(D, Gnd)}},l} + {I^{({\bf{Sky}})}}(t){\rho ^{{\rm{(Gnd)}}}}{K^{{\rm{(Sky, Gnd)}},l}}$$</div>
-
-<div>$${K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}},l} = {A^{{\rm{(f)}}}}{\mathop{\rm A}\nolimits}_{{\rm{s}}(t)}^{F,l}\cos {\theta_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}}}V_{i{\rm{ s(}}t{\rm{)}}}^{{\rm{(D)}}}$$</div>
-
-<div>$${Q^{{\rm{(Sun)}},l}} = {I^{{\rm{(D)}}}}(t){K_{{\rm{s(}}t{\rm{)}}}}^{{\rm{(Sun)}},l}$$</div>
-
-###### Comment on Bases
-
-Use of the basis in the above discussion has been mostly implicit, but it should nevertheless be clear that the essential feature of the basis is that it is a two-element list (i.e., a 2 X N array): it associates with an incident (i) or outgoing (j) direction index a vector pi (or pj ) that is a unit vector giving the direction of the radiation, the specification of which is two angles in some coordinate system.  The incident and outgoing bases of course must match the matrix elements of the fenestration properties.  These bases will (certainly in the case of WINDOW program; probably in the case of other input sources) have a structure: ordering of the elements, etc.  However, after the initialization of the hourly loop calculation, this structure will be irrelevant:  EnergyPlus will retain only those incoming and outgoing directions that are essential to the calculation with (one would hope, most of) the others combined into irradiation factors.  At this point, the basis will truly be an arbitrary list.  It follows that the specification of the basis in the EnergyPlus input should be determined by (1) the source of fenestration property data, and (2) user convenience.
-
-A related point concerns the specification of a basis for specular glazings, i.e., multiple layers of glass.  These fenestrations are both specular (input direction=output direction) and axially symmetric.  These properties have different effects on the calculation.
-
-The specular property means that one should not be using equation at all to describe the transmittance.  Instead, one should use the equation
-
-<div>$$S({{\bf{p}}^{{\rm{(T)}}}}) = \tau ({{\bf{p}}^{{\rm{(T)}}}}) \cdot E({{\bf{p}}^{{\rm{(T)}}}})$$</div>
-
-This equation is shoehorned into the integral calculation  of  equation through the use of a delta function in the incident direction vector, resulting (after the discretization) in a diagonal matrix for the transmittance (or reflectance).  The outgoing radiance element on the diagonal would be calculated as *T<sub>ii</sub>*L*<sub>ii</sub>*, where multiplication by L*<sub>ii</sub>* substitutes for integration over the basis solid angle element.  For a specular glazing, <span>\(T_{ii} = \tau(\bf{p}_i^{(T)})/\Lambda_{ii} \)</span>, so one recovers the correct transmittance when one does the multiplication.  However, there is still a problem in principle:  For a specular fenestration, the angular spread of the outgoing radiation will be that of the source, which for direct sunlight is very small; the calculation, however, assumes the angular spread of the basis element.  This problem disappears in the geometric approximation to be used in EnergyPlus: by considering only the central direction of each basis element, the outgoing radiation in that direction is essentially assumed to be specular, so the blurring in the discretization is undone.
-
-The axial symmetry of conventional glazings means that the transmittance (or reflectance) depends on only the incident angle, not the azimuthal angle about the normal to the fenestration plane.  So if one specifies the diagonal elements of the matrix, all of the terms with the same incident angles but different azimuthal angles will be the same.  One could alternatively specify only the specular transmittance at each of the incident angle values, provided one also indicated that it was for an axially symmetric fenestration.  Since expanding this set of values to the equivalent diagonal elements is a trivial calculation, how one specifies a specular glazing is completely a question of user convenience.  For example, if one were dealing with the WINDOW full basis, would it be more user-friendly to specify
-
-(1) <span>\(T_{ii} = \tau(\bf{p}_i^{(T)})/\Lambda_{ii}\)</span>, for 145 values, 135 of which are repeats of the previous value
-
-(2) <span>\(\tau ({\theta_i})\)</span> for 9 values of incident angle, *q<sub>i</sub>* ?
-
-###### Interior Solar Radiation Transmitted by Complex Fenestration
-
-Diffuse Solar Radiation Transmitted by Complex Fenestration
-
-Distribution of solar radiation transmitted through exterior window is divided on diffuse and direct part.
-
-Diffuse solar transmitted through exterior complex fenestration and absorbed in interor walls is calculated and treated in same way as described in the section on Initial Distribution of Diffuse Solar Transmitted through Exterior and Interior Windows. Even though that BSDF is given for various directions, for purpose of diffuse solar radiation, transmittance and reflectances of fenestration system is integrated over incoming and outgoing hemisphere.  Because incoming diffuse solar radiation is divided on ground and sky parts, integration of incoming hemisphere is also perfomed over ground and sky part (see equation .
-
-Direct Solar Radiation Transmitted by Complex Fenestration
-
-Direct solar (beam) transmitted through exterior window is using same overlap calculations (see Figure 49) for each outgoing basis direction.  For certain sun position, algorithm calculatates equivalent incoming beam number.  The inside beam solar irradiance is calculated in similar manner as described in the section titled Interior Beam Radiation.
-
-<div>$$
-  AISurf\left(SurfNum\right) = 
-    \frac{AbsIntSurf\left(SurfNum\right)}
-         {A\left(SurfNum\right)} \cdot
-    \sum_{i=1}^{N_{extwin}} \left( 
-       \sum_{j=1}^{N_{out}} 
-          TB{m_{k,j}} \cdot \Lambda_{k,j} \cdot \text{Aoverlap}_{k,j} \left( SurfNum \right)
-       \right) \cdot \text{CosInc}_i
-$$</div>
-
-*i* = exterior window number
-
-*N<sub>extwin</sub>=* number of exterior windows in zone
-
-*N<sub>out</sub>=* Beam number of exterior windows in zone
-
-*CosInc<sub>i</sub>* = cosine of angle of incidence of beam on exterior window *i*
-
-*TBm<sub>k,j</sub>* = beam-to-beam transmittance of exterior window* i*at incidence direction k outgoing direction j
-
-*Λ<sub>k,j</sub>* = lambda value of exterior window* i*at incidence direction k for outgoing direction j
-
-*Aoverlap<sub>k,j</sub>(SurfNum)* = beam solar irradiated area of surface *SurfNum* projected back onto the plane of exterior window* i* for incoming direction k and outgoing direction j (the *Aoverlap*’s for an exterior window sum up to the glazed area of the window)
-
-*AbsIntSurf(SurfNum)*= inside face solar absorptance of surface *SurfNum*
-
-*A(SurfNum)* = area of surface *SurfNum* [m<sup>2</sup>]
-
-Equation is valid as long as surface which is hit by transmitted solar radiation is not another complex fenestration.  In that case, for beam which is transmitted from other exterior window and reaches back surface of this window, angle of incidence needs to be taken into account.
-
-###### Interior Solar Absorbed by Complex Fenestration
-
-Solar radiation absorbed in window layers is coming from three sources: Diffuse radiation from sky and ground, direct radiation from the sun and beam radiation coming from the sun and it is transmitted through other exterior windows.
-
-Diffuse Radiation from Sky and Ground
-
-Energy absorbed in the layers and which originates from diffuse radiation from sky and ground is represented by following equation:
-
-<div>$$
-  \text{QRadSWwinAbs}(Surf, Lay) = 
-  \sum_{i=1}^{N_{layers}} \left(
-    \text{WinSkyFtAbs}(Surf, Lay) \cdot \text{SkySolarInc} + \text{WinSkyGndAbs}(Surf, Lay) \cdot \text{GndSolarInc}
-  \right)
-$$</div>
-  
-where,
-
-*WinSkyFtAbs(Lay)* = front absorptance averaged over sky for layer (Lay) and window belonging to Surf
-
-*WinSkyGndAbs(Lay)* = front absorptance averaged over ground for layer (Lay) and window belonging to Surf
-
-*SkySolarInc =* incident diffuse solar from the sky
-
-*GndSolarInc* = incident diffuse solar from the ground
-
-Direct Radiation from the Sun
-
-Energy absorbed in the layers and which originates from direct solar radiation is given by following equation:
-
-<div>$$
-  \text{QRadSWwinAbs}(SurfNum, Lay) = \text{AWinSurf}(SurfNum, Lay) \cdot \text{BeamSolar}
-$$</div>
-
-where,
-
-*AWinSurf(SurfNum,Lay)* – is time step value of factor for beam absorbed in fenestration glass layers
-
-*BeamSolar* – Current beam normal solar irradiance
-
-Factor for time step value is given by equation:
-
-<div>$$
-  \text{AWinSurf}(SurfNum,Lay) = \text{WinBmFtAbs}(Lay,HourOfDay,TimeStep) \cdot \text{CosInc} \cdot \text{SunLitFract} \cdot \text{OutProjSLFracMult}(HourOfDay)
-$$</div>
-
-where,
-
-*WinBmFtAbs(Lay,HourOfDay,TimeStep)* – is front directional absorptance for given layer and time
-
-*CosInc* – cosine of beam solar incident angle
-
-*SunLitFract* – sunlit fraction without shadowing effects of frame and divider
-
-*OutProjSLFracMult(HourOfDay)* - Multiplier on sunlit fraction due to shadowing of glass by frame and divider outside projections.
-
-Direct Solar Radiation Coming from Sun and it is Transmitted Through Other Windows
-
-Direct solar radiation transmitted through other windows is using solar overlap calculations described in the section on Overlapping Shadows. Overlapping is used to determine amount of energy transferred through the window is hitting certain surface.  That is used to calculate energy absorbed in walls and same approach will be used to calculate energy absorbed in window layers (equation ).  In case when receiving surface is complex fenestration, it is not enought just to apply equation because factor AbsIntSurf is now depending of incoming angle which is defined through front and back directional absorptance matrices.  It would mean that for each outgoing directions of transmitting complex fenestration, algorithm would need to determine what is best matching basis direction of receiving surface.  Best receiving direction is used to determine absorptance factors which will be used in equation .  It is important to understand that for basis definition, each unit vector defining one beam is going towards surface, which would mean that best matching directions from surface to surface will actually have minimal dot product.
-
-<div>$$Bes{t_{in}} = {\rm{min}}\left( {dot\left( {ou{t_p},i{n_1}} \right),dot\left( {ou{t_p},i{n_2}} \right), \ldots ,dot\left( {ou{t_p},i{n_N}} \right)} \right)$$</div>
-
-where,
-
-Best<sub>in</sub> – is best matching receiving direction basis dot product (in<sub>k</sub>)
-
-out<sub>p</sub> – current transmitting complex fenestration direction
-
-in<sub>1</sub>, ..., in<sub>N</sub> – set of receiving complex fenestration basis directions
-
-Result of equation is minimal dot product, which corresponds to best matching direction of receiving surface.  If we mark that direction with index k, then equation becomes:
-
-<div>$$
-  \begin{array}{l}
-    AWinSurf(SurfNum,Lay) = \\
-      \frac{1}{A(SurfNum)} \cdot \\
-      \sum_{i = 1}^{N_{extwin}} (\sum\limits_{j = 1}^{N_{out}} AbsIntSur{f_k}(SurfNum) \cdot TB{m_{k,j}} \cdot \\
-      A_{k,j} \cdot \text{Aoverlap}_{k,j}(SurfNum)) \cdot \text{CosInc}_i
-  \end{array}
-$$</div>
-
-
-
-where,
-
-*AbsIntSurf<sub>k</sub>(SurfNum)* – directional absorptance for the receiving surface for the best matching direction
-
-Everything else is same as described in equation .
-
-#### References
-
-Klems, J. H. 1994A. "A New Method for Predicting the Solar Heat Gain of Complex Fenestration Systems: I. Overview and Derivation of the Matrix Layer Calculation.". ASHRAE Transactions. 100(pt.1): 1073-1086.
-
-Klems, J. H. 1994B. "A New Method for Predicting the Solar Heat Gain of Complex Fenestration Systems: II. Detailed Description of the Matrix Layer Calculation.". ASHRAE Transactions. 100(pt.1): 1073-1086.
-
-Klems, J. H. 1995. "Measurements of Bidirectional Optical Properties of Complex Shading Devices.". ASHRAE Transactions. 101(pt 1; Symposium Paper CH-95-8-1(RP-548)): 791-801.
-
-Klems, J. H. 1996. "A Comparison between Calculated and Measured SHGC for Complex Glazing Systems.". ASHRAE Transactions. 102(Pt. 1; Symposium Paper AT-96-16-1): 931-939.
-
-Klems, J. H. 1996. "Calorimetric Measurements of Inward-Flowing Fraction for Complex Glazing and Shading Systems.". ASHRAE Transactions. 102(Pt. 1; Symposium Paper AT-96-16-3): 947-954.
-
-Papamichael, K. J. 1998. "Determination and Application of Bidirectional Solar-Optical Properties of Fenestration Systems.". Cambridge, MA: 13th National Passive Solar Conference.
-
-Window Heat Balance Calculation
--------------------------------
-
-Table 36.  Fortran Variables used in Window Heat Balance Calculations
-
-<table class="table table-striped">
-<tr>
-<th>Mathematical variable</th>
-<th>Description</th>
-<th>Units</th>
-<th>FORTRAN variable</th>
-</tr>
-<tr>
-<td>N</td>
-<td>Number of glass layers</td>
-<td>-</td>
-<td>nlayer</td>
-</tr>
-<tr>
-<td>σ</td>
-<td>Stefan-Boltzmann constant</td>
-<td> </td>
-<td>sigma</td>
-</tr>
-<tr>
-<td>ε<sub>i</sub></td>
-<td>Emissivity of face i</td>
-<td>-</td>
-<td>emis</td>
-</tr>
-<tr>
-<td>k<sub>i</sub></td>
-<td>Conductance of glass layer i</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>scon</td>
-</tr>
-<tr>
-<td>h<sub>o</sub>, h<sub>i</sub></td>
-<td>Outside, inside air film convective conductance</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>hcout, hcout</td>
-</tr>
-<tr>
-<td>h<sub>j</sub></td>
-<td>Conductance of gap j</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>hgap</td>
-</tr>
-<tr>
-<td>T<sub>o</sub>, T<sub>i</sub></td>
-<td>Outdoor and indoor air temperatures</td>
-<td>K</td>
-<td>tout, tin</td>
-</tr>
-<tr>
-<td>E<sub>o</sub>, E<sub>i</sub></td>
-<td>Exterior, interior long-wave radiation incident on window</td>
-<td>W/m<sup>2</sup></td>
-<td>outir, rmir</td>
-</tr>
-<tr>
-<td>θ<sub>i</sub></td>
-<td>Temperature of face i</td>
-<td>K</td>
-<td>thetas</td>
-</tr>
-<tr>
-<td>S<sub>i</sub></td>
-<td>Radiation (short-wave, and long-wave from zone internal sources) absorbed by face i</td>
-<td>W/m<sup>2</sup></td>
-<td>AbsRadGlassFace</td>
-</tr>
-<tr>
-<td>I<sup>ext</sup><sub>bm</sub></td>
-<td>Exterior beam normal solar irradiance</td>
-<td>W/m<sup>2</sup></td>
-<td>BeamSolarRad</td>
-</tr>
-<tr>
-<td>I<sup>ext</sup><sub>dif</sub></td>
-<td>Exterior diffuse solar irradiance on glazing</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>I<sup>int</sup><sub>sw</sub></td>
-<td>Interior short-wave radiation (from lights and from reflected diffuse solar) incident on glazing from inside</td>
-<td>W/m<sup>2</sup></td>
-<td>QS</td>
-</tr>
-<tr>
-<td>I<sup>int</sup><sub>lw</sub></td>
-<td>Long-wave radiation from lights and equipment incident on glazing from inside</td>
-<td>W/m<sup>2</sup></td>
-<td>QL</td>
-</tr>
-<tr>
-<td>φ</td>
-<td>Angle of incidence</td>
-<td>radians</td>
-<td>-</td>
-</tr>
-<tr>
-<td>A<sup>f</sup><sub>j</sub></td>
-<td>Front beam solar absorptance of glass layer j</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>A<sub>j</sub><sup>f,dif</sup>, A<sub>j</sub><sup>b,dif</sup></td>
-<td>Front and back diffuse solar absorptance of glass layer j</td>
-<td>-</td>
-<td>AbsDiff, AbsDiffBack</td>
-</tr>
-<tr>
-<td>A, B</td>
-<td>Matrices used to solve glazing heat balance equations</td>
-<td>W/m<sup>2</sup>, W/m<sup>2</sup>-K</td>
-<td>Aface, Bface</td>
-</tr>
-<tr>
-<td>h<sub>r,i</sub></td>
-<td>Radiative conductance for face i</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>hr(i)</td>
-</tr>
-<tr>
-<td>Δθ<sub>i</sub></td>
-<td>Difference in temperature of face i between successive iterations</td>
-<td>K</td>
-<td>-</td>
-</tr>
-
-</table>
-
-
-
-### The Glazing Heat Balance Equations
-
-The window glass face temperatures are determined by solving the heat balance equations on each face every time step. For a window with *N* glass layers there are 2*N* faces and therefore 2*N* equations to solve. Figure 95 shows the variables used for double glazing (*N*=2).
-
-![](media/image1470.png)
-
-Figure 95.  Glazing system with two glass layers showing variables used in heat balance equations.
-
-The following assumptions are made in deriving the heat balance equations:
-
-1)    The glass layers are thin enough (a few millimeters) that heat storage in the glass can be neglected; therefore, there are no heat capacity terms in the equations.
-
-2)    The heat flow is perpendicular to the glass faces and is one dimensional. See “Edge of Glass Corrections,� below, for adjustments to the gap conduction in multi-pane glazing to account for 2-D conduction effects across the pane separators at the boundaries of the glazing.
-
-3)    The glass layers are opaque to IR. This is true for most glass products. For thin plastic suspended films this is not a good assumption, so the heat balance equations would have to be modified to handle this case.
-
-4)    The glass faces are isothermal. This is generally a good assumption since glass conductivity is very high.
-
-5)    The short wave radiation absorbed in a glass layer can be apportioned equally to the two faces of the layer.
-
-The four equations for double-glazing are as follows. The equations for single glazing (*N*=1) and for *N*=3 and *N*=4 are analogous and are not shown.
-
-<div>$${E_o}{\varepsilon_1} - {\varepsilon_1}\sigma \theta_1^4 + {k_1}\left( {{\theta_2} - {\theta_1}} \right) + {h_o}\left( {{T_o} - {\theta_1}} \right) + {S_1} = 0$$</div>
-
-<div>$${k_1}\left( {{\theta_1} - {\theta_2}} \right) + {h_1}\left( {{\theta_3} - {\theta_2}} \right) + \sigma \frac{{{\varepsilon_2}{\varepsilon_3}}}{{1 - \left( {1 - {\varepsilon_2}} \right)\left( {1 - {\varepsilon_3}} \right)}}\left( {\theta_3^4 - \theta_2^4} \right) + {S_2} = 0$$</div>
-
-<div>$${h_1}({\theta_2} - {\theta_3}) + {k_2}({\theta_4} - {\theta_3}) + \sigma \frac{{{\varepsilon_2}{\varepsilon_3}}}{{1 - \left( {1 - {\varepsilon_2}} \right)\left( {1 - {\varepsilon_3}} \right)}}\left( {\theta_2^4 - \theta_3^4} \right) + {S_3} = 0$$</div>
-
-<div>$${E_i}{\varepsilon_4} - {\varepsilon_4}\sigma \theta_4^4 + {k_2}\left( {{\theta_3} - {\theta_4}} \right) + {h_i}\left( {{T_i} - {\theta_4}} \right) + {S_4} = 0$$</div>
-
-#### Absorbed Radiation
-
-*S<sub>i</sub>* in Equations to is the radiation (short-wave and long-wave from zone lights and equipment) absorbed on the *i*<sup>th</sup> face. Short-wave radiation (solar and short-wave from lights) is assumed to be absorbed uniformly along a glass layer, so for the purposes of the heat balance calculation it is split equally between the two faces of a layer. Glass layers are assumed to be opaque to IR so that the thermal radiation from lights and equipment is assigned only to the inside (room-side) face of the inside glass layer. For *N* glass layers *S<sub>i</sub>* is given by
-
-<div>$${S_{2j - 1}} = {S_{2j}} = \frac{1}{2}\left( {I_{bm}^{ext}\cos \phi A_j^f(\phi ) + I_{dif}^{ext}A_j^{f,dif} + I_{sw}^{{\mathop{\rm int}} }A_j^{b,dif}} \right),{\rm{     }}j = 1{\rm{ to }}N$$</div>
-
-<div>$${S_{2N}} = {S_{2N}} + {\varepsilon_{2N}}I_{lw}^{{\mathop{\rm int}} }$$</div>
-
-Here
-
-<span>\(I_{bm}^{ext}\)</span>= exterior beam normal solar irradiance
-
-<span>\(I_{dif}^{ext}\)</span>= exterior diffuse solar incident on glazing from outside
-
-<span>\(I_{sw}^{{\mathop{\rm int}} }\)</span>= interior short-wave radiation (from lights and from reflected diffuse solar) incident on glazing from inside
-
-<span>\(I_{lw}^{{\mathop{\rm int}} }\)</span>= long-wave radiation from lights and equipment incident on glazing from inside
-
-<span>\({\varepsilon_{2N}}\)</span>= emissivity (thermal absorptance) of the room-side face of the inside glass layer
-
-### Room-Side Convection
-
-The correlation for room-side convection coefficient, <span>\({h_i}\)</span>, is from ISO 15099 section 8.3.2.2.  (Prior to EnergyPlus version 3.1, the value for <span>\({h_i}\)</span> was modeled using the “Detailed� algorithm for opaque surface heat transfer, e.g. for a vertical surface <span>\({h_i} = 1.31{\left| {\Delta T} \right|^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}}\)</span>; see section Detailed Natural Convection Algorithm).  The ISO 15099 correlation is for still room air and is determined in terms of the Nusselt number, <span>\(Nu\)</span>, where
-
-<div>$${h_i} = Nu\left( {\frac{\lambda }{H}} \right)$$</div>
-
-where,
-
-<span>\(\lambda \)</span> is the thermal conductivity of air, and
-
-<span>\(H\)</span> is the height of the window.
-
-The Rayleigh number based on height, <span>\(R{a_H}\)</span>, is calculated using,
-
-<div>$$R{a_H} = \frac{{{\rho ^2}{H^3}g\,{c_p}\left| {{T_{surf,i}} - {T_{air}}} \right|}}{{{T_{m,f}}\mu \lambda }}$$</div>
-
-where,
-
-<span>\(\rho \)</span> is the density of air
-
-<span>\(g\)</span> is the acceleration due to gravity,
-
-<span>\({c_p}\)</span> is the specific heat of air,
-
-<span>\(\mu \)</span> is the dynamic viscosity of air, and
-
-<span>\({T_{m,f}}\)</span> is the mean film temperature in Kelvin given by,
-
-<div>$${T_{m,f}} = {T_{air}} + \frac{1}{4}\left( {{T_{surf,i}} - {T_{air}}} \right)$$</div>
-
-There are four cases for the Nusselt correlation that vary by the tilt angle in degrees, <span>\(\gamma \)</span>, and are based on heating conditions.  For cooling conditions (where <span>\({T_{surf,i}} > {T_{air}}\)</span>) the tilt angle is complemented so that <span>\(\gamma  = 180 - \gamma \)</span>
-
-Case A. <span>\({0^\circ } \le \gamma  &lt; 15^\circ \)</span>
-
-<div>$$Nu = 0.13Ra_H^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}$$</div>
-
-Case B. <span>\(15^\circ  \le \gamma  \le 90^\circ \)</span>
-
-<div>$$R{a_{cv}} = 2.5 \times {10^5}{\left( {\frac{{{e^{0.72\gamma }}}}{{\sin \lambda }}} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{$5$}}}}$$</div>
-
-<div>$$Nu = 0.56{\left( {R{a_H}\sin \gamma } \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{$4$}}}};\;for\;R{a_H} \le R{a_{CV}}$$</div>
-
-<div>$$Nu = 0.13\left( {Ra_H^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}} - Ra_{CV}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}} \right) + 0.56{\left( {R{a_{CV}}\sin \gamma } \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{$4$}}}};\;R{a_H} > R{a_{CV}}$$</div>
-
-Case C. <span>\(90^\circ  &lt; \gamma  \le 179^\circ \)</span>
-
-<div>$$Nu = 0.56{\left( {R{a_H}\sin \gamma } \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 4}}\right.}\!\lower0.7ex\hbox{$4$}}}};\;{10^5} \le R{a_H}\sin \gamma  &lt; {10^{11}}$$</div>
-
-Case D. <span>\(179^\circ  &lt; \gamma  \le 180^\circ \)</span>
-
-<div>$$Nu = 0.58Ra_H^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 5}}\right.}\!\lower0.7ex\hbox{$5$}}};\;R{a_H} \le {10^{11}}$$</div>
-
-The material properties are evaluated at the mean film temperature.  Standard EnergyPlus pyschrometric functions are used for <span>\(\rho \)</span> and <span>\({c_p}\)</span>.  Thermal conductivity is calculated using,
-
-<span>\(\lambda  = 2.873 \times {10^{ - 3}} + 7.76 \times {10^{ - 5}}{T_{m,f}}\)</span>.
-
-Kinematic viscosity is calculated using,
-
-<span>\(\mu  = 3.723 \times {10^{ - 6}} + 4.94 \times {10^{ - 8}}{T_{m,f}}\)</span>.
-
-This correlation depends on the surface temperature of the room-side glazing surface and is therefore included inside the window heat balance interation loop.
-
-
-
-### Solving the Glazing Heat Balance Equations
-
-The equations are solved as follows:
-
-1)    Linearize the equations by defining <span>\({h_{r,i}} = {\varepsilon_i}\sigma \theta_i^3\)</span>.  For example, Equation becomes
-
-<div>$${E_o}{\varepsilon_1} - {h_{r,1}}{\theta_1} + {k_1}\left( {{\theta_2} - {\theta_1}} \right) + {h_o}\left( {{T_o} - {\theta_1}} \right) + {S_1} = 0$$</div>
-
-2)    Write the equations in the matrix form <span>\(A\theta  = B\)</span>
-
-3)    Use previous time step’s values of <span>\({\theta_i}\)</span>as initial values for the current time step. For the first time step of a design day or run period the initial values are estimated by treating the layers as a simple RC network.
-
-4)    Save the <span>\({\theta_i}\)</span> for use in the next iteration: <span>\({\theta_{prev,i}} = {\theta_i}\)</span>
-
-5)    Using <span>\({\theta_{2N}}\)</span>, reevaluate the room-side face surface convection coefficient <span>\({h_i}\)</span>
-
-6)    Using the <span>\({\theta_i}\)</span> to evaluate the radiative conductances <span>\({h_{r,i}}\)</span>
-
-7)    Find the solution <span>\(\theta  = {A^{ - 1}}B\)</span>by LU decomposition
-
-8)    Perform relaxation on the the new <span>\({\theta_i}\)</span>**:** <span>\({\theta_i} \to \left( {{\theta_i} + {\theta_{prev,i}}} \right)/2\)</span>
-
-9)    Go to step 4
-
-Repeat steps 4 to 9 until the difference, <span>\(\Delta {\theta_i}\)</span>, between values of the <span>\({\theta_i}\)</span> in successive iterations is less than some tolerance value. Currently, the test is
-
-<div>$$\frac{1}{{2N}}\sum\limits_{i = 1}^{2N} {|\Delta {\theta_i}|{\rm{ }} &lt; 0.02K} $$</div>
-
-If this test does not pass after 100 iterations, the tolerance is increased to 0.2K. If the test still fails the program stops and an error message is issued.
-
-The value of the inside face temperature, <span>\({\theta_{2N}}\)</span>, determined in this way participates in the zone heat balance solution (see Outdoor/Exterior Convection) and thermal comfort calculation (see Occupant Thermal Comfort).
-
-### Edge-Of-Glass Effects
-
-Table 37.  Fortran Variables used in Edge of Glass calculations
-
-<table class="table table-striped">
-<tr>
-<th>Mathematical variable</th>
-<th>Description</th>
-<th>Units</th>
-<th>FORTRAN variable</th>
-</tr>
-<tr>
-<td><span>\(\bar h\)</span></td>
-<td>Area-weighted net conductance of glazing including edge-of-glass effects</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>A<sub>cg</sub></td>
-<td>Area of center-of-glass region</td>
-<td>m<sup>2</sup></td>
-<td>CenterGlArea</td>
-</tr>
-<tr>
-<td>A<sub>fe</sub></td>
-<td>Area of frame edge region</td>
-<td>m<sup>2</sup></td>
-<td>FrameEdgeArea</td>
-</tr>
-<tr>
-<td>A<sub>de</sub></td>
-<td>Area of divider edge region</td>
-<td>m<sup>2</sup></td>
-<td>DividerEdgeArea</td>
-</tr>
-<tr>
-<td>A<sub>tot</sub></td>
-<td>Total glazing area</td>
-<td>m<sup>2</sup></td>
-<td>Surface%Area</td>
-</tr>
-<tr>
-<td>h<sub>cg</sub></td>
-<td>Conductance of center-of-glass region (without air films)</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>fe</sub></td>
-<td>Conductance of frame edge region (without air films)</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>de</sub></td>
-<td>Conductance of divider edge region (without air films)</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>ck</sub></td>
-<td>Convective conductance of gap k</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>rk</sub></td>
-<td>Radiative conductance of gap k</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>-</td>
-</tr>
-<tr>
-<td>η</td>
-<td>Area ratio</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>α</td>
-<td>Conductance ratio</td>
-<td>-</td>
-<td>FrEdgeToCenterGlCondRatio, DivEdgeToCenterGlCondRatio</td>
-</tr>
-
-</table>
-
-Because of thermal bridging across the spacer separating the glass layers in multi-pane glazing, the conductance of the glazing near the frame and divider, where the spacers are located, is higher than it is in the center of the glass. The area-weighted net conductance (without inside and outside air films) of the glazing in this case can be written
-
-<div>$$\overline h  = \left( {{A_{cg}}{h_{cg}} + {A_{fe}}{h_{fe}} + {A_{de}}{h_{de}}} \right)/{A_{tot}}$$</div>
-
-where
-
-*h<sub>cg</sub>* = conductance of center-of-glass region (without air films)
-
-*h<sub>fe</sub>* = conductance of frame edge region (without air films)
-
-*h<sub>de</sub>* = conductance of divider edge region (without air films)
-
-*A<sub>cg</sub>*= area of center-of-glass region
-
-*A<sub>fe</sub>*= area of frame edge region
-
-*A<sub>de</sub>*= area of divider edge region
-
-*A<sub>tot</sub>*= total glazing area = <span>\({A_{cg}} + {A_{fe}} + {A_{de}}\)</span>
-
-The different regions are shown in Figure 96:
-
-![](media/image1534.png)
-
-Figure 96:  Different types of glass regions.
-
-Equation can be rewritten as
-
-<div>$$\overline h  = {h_{cg}}\left( {{\eta_{cg}} + {\alpha_{fe}}{\eta_{fe}} + {\alpha_{de}}{\eta_{de}}} \right)$$</div>
-
-where
-
-<div>$${\eta_{cg}} = {A_{cg}}/{A_{tot}}$$</div>
-
-<div>$${\eta_{fe}} = {A_{fe}}/{A_{tot}}$$</div>
-
-<div>$${\eta_{de}} = {A_{de}}/{A_{tot}}$$</div>
-
-<div>$${\alpha_{fe}} = {h_{fe}}/{h_{cg}}$$</div>
-
-<div>$${\alpha_{de}} = {h_{de}}/{h_{cg}}$$</div>
-
-The conductance ratios <span>\({\alpha_{fe}}\)</span> and <span>\({\alpha_{de}}\)</span>are user inputs obtained from Window 5. They depend on the glazing construction as well as the spacer type, gap width, and frame and divider type.
-
-In the EnergyPlus glazing heat balance calculation effective gap convective conductances are used to account for the edge-of-glass effects. These effective conductances are determined as follows for the case with two gaps (triple glazing). The approach for other numbers of gaps is analogous.
-
-Neglecting the very small resistance of the glass layers, the center-of-glass conductance (without inside and outside air films) can be written as
-
-<div>$${h_{cg}} = {\left( {{{\left( {{h_{r,1}} + {h_{c,1}}} \right)}^{ - 1}} + {{\left( {{h_{r,2}} + {h_{c,2}}} \right)}^{ - 1}}} \right)^{ - 1}}$$</div>
-
-where
-
-<span>\({h_{c,k}} = \)</span>convective conductance of the *k<sup>th</sup>* gap
-
-<span>\({h_{r,k}} = \)</span>radiative conductance of the *k<sup>th</sup>* gap
-
-<div>$$ = \frac{1}{2}\sigma \frac{{{\varepsilon_i}{\varepsilon_j}}}{{1 - \left( {1 - {\varepsilon_i}} \right)\left( {1 - {\varepsilon_j}} \right)}}{\left( {{\theta_i} + {\theta_j}} \right)^3}$$</div>
-
-<span>\({\varepsilon_i},{\varepsilon_j} = \)</span>emissivity of the faces bounding the gap
-
-<span>\({\theta_i},{\theta_j} = \)</span>temperature of faces bounding the gap (K)
-
-Equation then becomes
-
-<div>$$\overline h  = \left( {{\eta_{cg}} + {\alpha_{fe}}{\eta_{fe}} + {\alpha_{de}}{\eta_{de}}} \right){\left( {{{\left( {{h_{r,1}} + {h_{c,1}}} \right)}^{ - 1}} + {{\left( {{h_{r,2}} + {h_{c,2}}} \right)}^{ - 1}}} \right)^{ - 1}}$$</div>
-
-We can also write <span>\(\overline h \)</span>in terms of effective convective conductances of the gaps as
-
-<div>$$\overline h  = {\left( {{{\left( {{h_{r,1}} + {{\overline h }_{c,1}}} \right)}^{ - 1}} + {{\left( {{h_{r,2}} + {{\overline h }_{c,2}}} \right)}^{ - 1}}} \right)^{ - 1}}$$</div>
-
-Comparing Eqs. and we obtain
-
-<div>$${h_{r,k}} + {\overline h_{c,k}} = \left( {{\eta_{cg}} + {\alpha_{fe}}{\eta_{fe}} + {\alpha_{de}}{\eta_{de}}} \right)\left( {{h_{r,k}} + {h_{c,k}}} \right)$$</div>
-
-Using <span>\({\eta_{cg}} = 1 - {\eta_{fe}} - {\eta_{de}}\)</span> gives
-
-<div>$${\overline h_{c,k}} = {h_{r,k}}\left( {{\eta_{fe}}\left( {{\alpha_{fe}} - 1} \right) + {\eta_{de}}\left( {{\alpha_{de}} - 1} \right)} \right) + {h_{c,k}}\left( {1 + {\eta_{fe}}\left( {{\alpha_{fe}} - 1} \right) + {\eta_{de}}\left( {{\alpha_{de}} - 1} \right)} \right)$$</div>
-
-This is the expression used by EnergyPlus for the gap convective conductance when a frame or divider is present.
-
-### Apportioning of Absorbed Short-Wave Radiation in Shading Device Layers
-
-If a shading device has a non-zero short-wave transmittance then absorption takes place throughout the shading device layer. The following algorithm is used to apportion the absorbed short-wave radiation to the two faces of the layer. Here *f<sub>1</sub>* is the fraction assigned to the face closest to the incident radiation and *f<sub>2</sub>* is the fraction assigned to the face furthest from the incident radiation.
-
- <span>\({f_1} = 1,{\rm{ }}{f_2} = 0{\rm{   if }}{\tau_{sh}} = 0\)</span>
-
-Otherwise
-
-<div>$$
-  \begin{array}{cl}
-    f_1 = 0,\;f_2 = 0 &\text{if} \alpha_{sh} \le 0.01 \\
-    f_1 = 1,\;f_2 = 0 &\text{if} \alpha_{sh} \gt 0.999 \\
-    \left.
-      \begin{array}{l}
-        f_1 = \frac{1 - e^{0.5 \ln (1 - \alpha_{sh}}} {\alpha_{sh}} \\
-        f_2 = 1 - {f_1}
-      \end{array}
-    \right\} &\text{if} 0.01 lt \alpha_{sh} \le 0.999
-  \end{array}
-$$</div>
-
-### Window  Frame and Divider Calculation
-
-For the zone heat balance calculation the inside surface temperature of the frame and that of the divider are needed. These temperatures are determined by solving the heat balance equations on the inside and outside surfaces of the frame and divider.
-
-Table 38.  Fortran Variables used in Window/Frame and Divider calculations
-
-<table class="table table-striped">
-<tr>
-<th>Mathematical variable</th>
-<th>Description</th>
-<th>Units</th>
-<th>FORTRAN variable</th>
-</tr>
-<tr>
-<td>Q<sub>ExtIR,abs</sub></td>
-<td>IR from the exterior surround absorbed by outside frame surfaces</td>
-<td>W</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Q<sub>IR,emitted</sub></td>
-<td>IR emitted by outside frame surfaces</td>
-<td>W</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Q<sub>conv</sub></td>
-<td>Convection from outside air to outside frame surfaces</td>
-<td>W</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Q<sub>cond</sub></td>
-<td>Conduction through frame from inside frame surfaces to outside frame surfaces</td>
-<td>W</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Q<sub>abs</sub></td>
-<td>Solar radiation plus outside glass IR absorbed by outside of frame</td>
-<td>W</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Q<sup>dif</sup><sub>abs,sol</sub></td>
-<td>Diffuse solar absorbed by outside frame surfaces, per unit frame face area</td>
-<td>W/ m<sup>2</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>Q<sup>bm</sup><sub>abs,sol</sub></td>
-<td>Beam solar absorbed by outside frame surfaces, per unit frame face area</td>
-<td>W/ m<sup>2</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>I<sup>dif</sup><sub>ext</sub></td>
-<td>Diffuse solar incident on window</td>
-<td>W/ m<sup>2</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>I<sup>bm</sup><sub>ext</sub></td>
-<td>Direct normal solar irradiance</td>
-<td>W/ m<sup>2</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>α<sup>fr</sup><sub>sol</sub></td>
-<td>Solar absorptance of frame</td>
-<td>-</td>
-<td>FrameSolAbsorp</td>
-</tr>
-<tr>
-<td>R<sub>gl</sub><sup>f,dif</sup></td>
-<td>Front diffuse solar reflectance of glazing</td>
-<td>-</td>
-<td> </td>
-</tr>
-<tr>
-<td>R<sub>gl</sub><sup>f,bm</sup></td>
-<td>Front beam solar reflectance of glazing</td>
-<td>-</td>
-<td> </td>
-</tr>
-<tr>
-<td>cos(β<sub>face</sub>)</td>
-<td>Cosine of angle of incidence of beam solar on frame outside face</td>
-<td> </td>
-<td>CosIncAng</td>
-</tr>
-<tr>
-<td>Cos(β<sub>h</sub>)</td>
-<td>Cosine of angle of incidence of beam solar on frame projection parallel to window x-axis</td>
-<td>-</td>
-<td>CosIncAngHorProj</td>
-</tr>
-<tr>
-<td>Cos(β<sub>v</sub>)</td>
-<td>Cosine of angle of incidence of beam solar on frame projection parallel to window y-axis</td>
-<td>-</td>
-<td>CosIncAngVertProj</td>
-</tr>
-<tr>
-<td>f<sub>sunlit</sub></td>
-<td>Fraction of window that is sunlit</td>
-<td>-</td>
-<td>SunlitFrac</td>
-</tr>
-<tr>
-<td>A<sub>f</sub></td>
-<td>Area of frame’s outside face (same as area of frame’s inside face)</td>
-<td>m<sup>2</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>A<sub>p1</sub>, A<sub>p2</sub></td>
-<td>Area of frame’s outside and inside projection faces</td>
-<td>m<sup>2</sup></td>
-<td>-</td>
-</tr>
-<tr>
-<td>F<sub>f</sub></td>
-<td>Form factor of frame’s outside or inside face for IR</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>F<sub>p1</sub>, F<sub>p2</sub></td>
-<td>Form factor of frame outside projection for exterior IR; form factor of frame inside projection for interior IR</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>E<sub>o</sub></td>
-<td>Exterior IR incident on window plane</td>
-<td>W/m<sup>2</sup></td>
-<td>outir</td>
-</tr>
-<tr>
-<td>E<sub>i</sub></td>
-<td>Interior IR incident on window plane</td>
-<td>W/m<sup>2</sup></td>
-<td>SurroundIRfromParentZone</td>
-</tr>
-<tr>
-<td>ε<sub>1</sub>, ε<sub>2</sub></td>
-<td>Outside, inside frame surface emissivity</td>
-<td>-</td>
-<td>FrameEmis</td>
-</tr>
-<tr>
-<td>θ<sub>1</sub>, θ<sub>2</sub></td>
-<td>Frame outside, inside surface temperature</td>
-<td>K</td>
-<td>FrameTempSurfOut, FrameTempSurfIn</td>
-</tr>
-<tr>
-<td>T<sub>o</sub>, T<sub>i</sub></td>
-<td>Outdoor and indoor air temperatures</td>
-<td>K</td>
-<td>tout, tin</td>
-</tr>
-<tr>
-<td>h<sub>o,c</sub>, h<sub>i,c</sub></td>
-<td>Frame outside and inside air film convective conductance</td>
-<td>W/m2-K</td>
-<td>HOutConv, HInConv</td>
-</tr>
-<tr>
-<td>k</td>
-<td>Effective inside-surface to outside-surface conductance of frame per unit area of frame projected onto window plane</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>FrameConductance, FrameCon</td>
-</tr>
-<tr>
-<td>S<sub>1</sub></td>
-<td>Q<sub>abs</sub>/A<sub>f</sub></td>
-<td>W/m<sup>2</sup>-K</td>
-<td>FrameQRadOutAbs</td>
-</tr>
-<tr>
-<td>S<sub>2</sub></td>
-<td>Interior short-wave radiation plus interior IR from internal sources absorbed by inside of frame divided by A<sub>f</sub></td>
-<td>W/m<sup>2</sup>-K</td>
-<td>FrameQRadInAbs</td>
-</tr>
-<tr>
-<td>η<sub>1</sub>, η<sub>2</sub></td>
-<td>A<sub>p1</sub>/A<sub>f</sub>, A<sub>p2</sub>/A<sub>f</sub></td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>H</td>
-<td>Height of glazed portion of window</td>
-<td>m</td>
-<td>Surface%Height</td>
-</tr>
-<tr>
-<td>W</td>
-<td>Width of glazed portion of window</td>
-<td>m</td>
-<td>Surface%Width</td>
-</tr>
-<tr>
-<td>w<sub>f</sub>, w<sub>d</sub></td>
-<td>Frame width, divider width</td>
-<td>m</td>
-<td>FrameWidth, DividerWidth</td>
-</tr>
-<tr>
-<td>p<sub>f1</sub>, p<sub>f2</sub></td>
-<td>Frame outside, inside projection</td>
-<td>m</td>
-<td>FrameProjectionOut, FrameProjectionIn</td>
-</tr>
-<tr>
-<td>N<sub>h</sub>, N<sub>v</sub></td>
-<td>Number of horizontal, vertical dividers</td>
-<td>-</td>
-<td>HorDividers, VertDividers</td>
-</tr>
-<tr>
-<td>T<sub>o,r</sub>, T<sub>i,r</sub></td>
-<td>Frame outside, inside radiative temperature</td>
-<td>K</td>
-<td>TOutRadFr, TInRadFr</td>
-</tr>
-<tr>
-<td>h<sub>o,r</sub>, h<sub>i,r</sub></td>
-<td>Frame outside, inside surface radiative conductance</td>
-<td>W/m<sup>2</sup>-K</td>
-<td>HOutRad, HInRad</td>
-</tr>
-<tr>
-<td>A</td>
-<td>Intermediate variable in frame heat balance solution</td>
-<td>K</td>
-<td>Afac</td>
-</tr>
-<tr>
-<td>C</td>
-<td>Intermediate variable in frame heat balance solution</td>
-<td>-</td>
-<td>Efac</td>
-</tr>
-<tr>
-<td>B, D</td>
-<td>Intermediate variables in frame heat balance solution</td>
-<td>-</td>
-<td>Bfac, Dfac</td>
-</tr>
-
-</table>
-
-
-
-#### Frame Temperature Calculation
-
-Figure 97 shows a cross section through a window showing frame and divider. The outside and inside frame and divider surfaces are assumed to be isothermal. The frame and divider profiles are approximated as rectangular since this simplifies calculating heat gains and losses (see “Error Due to Assuming a Rectangular Profile,� below).
-
-
-
-![](media/image1557.png)
-
-Figure 97.  Cross section through a window showing frame and divider (exaggerated horizontally).
-
-** **
-
-#### Frame Outside Surface Heat Balance
-
-The outside surface heat balance equation is
-
-<div>$${Q_{ExtIR,abs}} - {Q_{IR,emitted}} + {Q_{conv}} + {Q_{cond}} + {Q_{abs}} = 0$$</div>
-
-where
-
-<span>\({Q_{ExtIR,abs}}\)</span> = IR from the exterior surround (sky and ground) absorbed by outside frame surfaces
-
-<span>\({Q_{IR,emitted}}\)</span>= IR emitted by outside frame surfaces
-
-<span>\({Q_{conv}}\)</span>= convection from outside air to outside frame surfaces
-
-<span>\({Q_{cond}}\)</span>= conduction through frame from inside frame surfaces to outside frame surfaces
-
-<span>\({Q_{abs}}\)</span>= solar radiation (from sun, sky and ground) plus IR from outside window surface absorbed by outside frame surfaces (see “Calculation of Absorbed Solar Radiation,� below).
-
-The first term can be written as the sum of the exterior IR absorbed by the outside face of the frame and the exterior IR absorbed by the frame’s outside projection surfaces.
-
-<div>$${Q_{ExtIR,abs}} = {\varepsilon_1}{E_o}{A_f}{F_f} + {\varepsilon_1}{E_o}{A_{p1}}{F_{p1}}$$</div>
-
-where *ε<sub>1</sub>* is the outside surface emissivity.
-
-The exterior IR incident on the plane of the window, *E<sub>o</sub>*, is the sum of the IR from the sky, ground and obstructions. For the purposes of the frame heat balance calculation it is assumed to be isotropic. For isotropic incident IR, *F<sub>f</sub>*= 1.0 and *F<sub>p1</sub>* = 0.5, which gives
-
-<div>$${Q_{ExtIR,abs}} = {\varepsilon_1}{E_o}({A_f} + \frac{1}{2}{A_{p1}})$$</div>
-
-The IR emitted by the outside frame surfaces is
-
-<div>$${Q_{ExtIR,emitted}} = {\varepsilon_1}\sigma ({A_f} + {A_{p1}})\theta_1^4$$</div>
-
-The convective heat flow from the outside air to the outside frame surfaces is
-
-<div>$${Q_{conv}} = {h_{o,c}}({A_f} + {A_{p1}})({T_o} - {\theta_1})$$</div>
-
-The conduction through the frame from inside to outside is
-
-<div>$${Q_{cond}} = k{A_f}({\theta_2} - {\theta_1})$$</div>
-
-Note that *A<sub>f</sub>  *is used here since the conductance, *k*, is, by definition, per unit area of frame projected onto the plane of the window.
-
-Adding these expressions for the *Q* terms and dividing by* A<sub>f</sub>* gives
-
-<div>$${E_0}{\varepsilon_1}\left( {1 + \frac{1}{2}{\eta_1}} \right) - {\varepsilon_1}\left( {1 + {\eta_1}} \right)\theta_1^4 + {h_{o,c}}\left( {1 + {\eta_1}} \right)\left( {{T_0} - {\theta_1}} \right) + k\left( {{\theta_2} - {\theta_1}} \right) + {S_1} = 0$$</div>
-
-where *S<sub>1</sub>* = *Q<sub>abs</sub>/A<sub>f</sub>* and
-
-<div>$${\eta_1} = \frac{{{A_{p1}}}}{{{A_f}}} = \left( {\frac{{{p_{f,1}}}}{{{w_f}}}} \right)\frac{{H + W - ({N_h} + {N_v}){w_d}}}{{H + W + 2{w_f}}}$$</div>
-
-We linearize Eq. as follows.
-
-Write the first two terms as
-
-<div>$${\varepsilon_1}(1 + {\eta_1})[{E_o}(1 + \frac{1}{2}{\eta_1})/(1 + {\eta_1}) - \theta_1^4]$$</div>
-
-and define a radiative temperature
-
-<div>$${T_{o,r}} = {[{E_o}(1 + \frac{1}{2}{\eta_1})/(1 + {\eta_1})]^{1/4}}$$</div>
-
-This gives
-
-<div>$${\varepsilon_1}(1 + {\eta_1})[T_{o,r}^4 - \theta_1^4]$$</div>
-
-which, within a few percent, equals
-
-<div>$${\varepsilon_1}(1 + {\eta_1})\frac{{{{({T_{o,r}} + {\theta_1})}^3}}}{2}({T_{o,r}} - {\theta_1})$$</div>
-
-Defining an outside surface radiative conductance as follows
-
-<div>$${h_{o,r}} = {\varepsilon_1}(1 + {\eta_1})\frac{{{{({T_{o,r}} + {\theta_1})}^3}}}{2}$$</div>
-
-then gives
-
-<div>$${h_{o,r}}({T_{o,r}} - {\theta_1})$$</div>
-
-The final outside surface heat balance equation in linearized form is then
-
-<div>$${h_{o,r}}({T_{o,r}} - {\theta_1}) + {h_{o,c}}(1 + {\eta_1})({T_o} - {\theta_1}) + k({\theta_2} - {\theta_1}) + {S_1} = 0$$</div>
-
-#### Frame Inside Surface Heat Balance
-
-A similar approach can be used to obtain the following linearized *inside* surface heat balance equation:
-
-<div>$${h_{i,r}}({T_{i,r}} - {\theta_2}) + {h_{i,c}}(1 + {\eta_2})({T_i} - {\theta_2}) + k({\theta_1} - {\theta_2}) + {S_2} = 0$$</div>
-
-where
-
-<div>$${T_{i,r}} = {[{E_i}(1 + \frac{1}{2}{\eta_2})/(1 + {\eta_2})]^{1/4}}$$</div>
-
-<div>$${\eta_2} = \frac{{{A_{p2}}}}{{{A_f}}} = \left( {\frac{{{p_{f,2}}}}{{{w_f}}}} \right)\frac{{H + W - ({N_h} + {N_v}){w_d}}}{{H + W + 2{w_f}}}$$</div>
-
-and *E<sub>i</sub>* is the interior IR irradiance incident on the plane of the window.
-
-Solving Eqs. and simultaneously gives
-
-<div>$${\theta_2} = \frac{{D + CA}}{{1 - CB}}$$</div>
-
-with
-
-<div>$$A = \frac{{{h_{o,r}}{T_{o,r}} + {h_{o,c}}{T_o} + {S_1}}}{{{h_{o,r}} + k + {h_{o,c}}}}$$</div>
-
-<div>$$B = \frac{k}{{{h_{o,r}} + k + {h_{o,c}}}}$$</div>
-
-<div>$$C = \frac{k}{{{h_{i,r}} + k + {h_{i,c}}}}$$</div>
-
-<div>$$D = \frac{{{h_{i,r}}{T_{i,r}} + {h_{i,c}}{T_i} + {S_2}}}{{{h_{i,r}} + k + {h_{i,c}}}}$$</div>
-
-#### Calculation of Solar Radiation Absorbed by Frame
-
-The frame outside face and outside projections and inside projections absorb beam solar radiation (if sunlight is striking the window) and diffuse solar radiation from the sky and ground. For the outside surfaces of the frame, the absorbed diffuse solar per unit frame face area is
-
-<div>$$Q_{abs,sol}^{dif} = I_{ext}^{dif}{\alpha_{fr,sol}}\left( {{A_f} + {F_{p1}}{A_{p1}}} \right)/{A_f} = I_{ext}^{dif}{\alpha_{fr,sol}}\left( {1 + 0.5\frac{{{A_{p1}}}}{{{A_f}}}} \right)$$</div>
-
-If there is no exterior window shade, * I<sup>dif</sup><sub>ext</sub>* includes the effect of diffuse solar reflecting off of the glazing onto the outside frame projection, i.e.,
-
-<div>$$I_{ext}^{dif} \to I_{ext}^{dif}\left( {1 + R_{gl}^{f,dif}} \right)$$</div>
-
-The beam solar absorbed by the outside face of the frame, per unit frame face area is
-
-<div>$$Q_{abs,sol}^{bm,face} = I_{ext}^{bm}{\alpha_{fr,sol}}\cos {\beta_{face}}{f_{sunlit}}$$</div>
-
-The beam solar absorbed by the frame outside projection parallel to the window x-axis is
-
-<div>$$Q_{abs,sol}^{bm,h} = I_{ext}^{bm}{\alpha_{fr,sol}}\cos {\beta_h}{p_{f1}}\left( {W - {N_v}{w_d}} \right){f_{sunlit}}/{A_f}$$</div>
-
-Here it is assumed that the sunlit fraction, *f<sub>sunlit</sub>*, for the window can be applied to the window frame. Note that at any given time beam solar can strike only one of the two projection surfaces that are parallel to the window x-axis. If there is no exterior window shade, *I<sup>bm</sup><sub>ext</sub>* includes the effect of beam solar reflecting off of the glazing onto the outside frame projection, i.e.,
-
-<div>$$I_{ext}^{bm} \to I_{ext}^{bm}\left( {1 + R_{gl}^{f,bm}} \right)$$</div>
-
-The beam solar absorbed by the frame outside projection parallel to the window y-axis is
-
-<div>$$Q_{abs,sol}^{bm,v} = I_{ext}^{bm}{\alpha_{fr,sol}}\cos {\beta_v}{p_{f1}}\left( {H - {N_h}{w_d}} \right){f_{sunlit}}/{A_f}$$</div>
-
-Using a similar approach, the beam and diffuse solar absorbed by the *inside* frame projections is calculated, taking the transmittance of the glazing into account.
-
-#### Error Due to Assuming a Rectangular Profile
-
-Assuming that the inside and outside frame profile is rectangular introduces an error in the surface heat transfer calculation if the profile is non-rectangular. The percent error in the calculation of convection and emitted IR is approximately 100<span>\(\left| {{L_{profile,rect}} - {L_{profile,actual}}} \right|/{L_{profile,rect}}\)</span>, where *L<sub>profile,rect</sub>* is the profile length for a rectangular profile (*w<sub>f</sub>* +* p<sub>f1</sub>* for outside of frame or *w<sub>f</sub>* + *p<sub>f2</sub>*for inside of frame) and *L<sub>profile,actual</sub>* is the actual profile length. For example, for a circular profile *vs* a square profile the error is about 22%. The error in the calculation of absorbed beam radiation is close to zero since the beam radiation intercepted by the profile is insensitive to the shape of the profile. The error in the absorbed diffuse radiation and absorbed IR depends on details of the shape of the profile. For example, for a circular profile vs. a square profile the error is about 15%.
-
-#### Divider Temperature Calculation
-
-The divider inside and outside surface temperatures are determined by a heat balance calculation that is analogous to the frame heat balance calculation described above.
-
-### Beam Solar Reflection from Window Reveal Surfaces
-
-This section describes how beam solar radiation that is reflected from window reveal surfaces is calculated. Reflection from outside reveal surfaces—which are associated with the setback of the glazing from the outside surface of the window’s parent wall—increases the solar gain through the glazing. Reflection from inside reveal surfaces—which are associated with the setback of the glazing from the inside surface of the window’s parent wall—decreases the solar gain to the zone because some of this radiation is reflected back out of the window.
-
-The amount of beam solar reflected from reveal surfaces depends, among other things, on the extent to which reveal surfaces are shadowed by other reveal surfaces. An example of this shadowing is shown in Figure 98. In this case the sun is positioned such that the top reveal surfaces shadow the left and bottom reveal surfaces. And the right reveal surfaces shadow the bottom reveal surfaces. The result is that the left/outside, bottom/outside, left/inside and bottom/inside reveal surfaces each have sunlit areas. Note that the top and right reveal surfaces are facing away from the sun in this example so their sunlit areas are zero.
-
-![](media/image1593.png)
-
-Figure 98.  Example of shadowing of reveal surfaces by other reveal surfaces.
-
-The size of the shadowed areas, and the size of the corresponding illuminated areas, depends on the following factors:
-
-* The sun position relative to the window
-
-* The height and width of the window
-
-* The depth of the outside and inside reveal surfaces
-
-We will assume that the reveal surfaces are perpendicular to the window plane and that the window is rectangular. Then the above factors determine a unique shadow pattern. From the geometry of the pattern the shadowed areas and corresponding illuminated areas can be determined. This calculation is done in subroutine CalcBeamSolarReflectedFromWinRevealSurface in the SolarShading module. The window reveal input data is specified in the WindowProperty:FrameAndDivider object expect for the depth of the outside reveal, which is determined from the vertex locations of the window and its parent wall.
-
-If an exterior shading device (shade, screen or blind) is in place it is assumed that it blocks beam solar before it reaches outside or inside reveal surfaces. Correspondingly, it is assumed that an interior or between-glass shading device blocks beam solar before it reaches inside reveal surfaces.
-
-Representative shadow patterns are shown in Figure 99 for a window with no shading device, and without and with a frame. The case with a frame has to be considered separately because the frame can cast an additional shadow on the inside reveal surfaces.
-
-The patterns shown apply to both vertical and horizontal reveal surfaces. It is important to keep in mind that, for a window of arbitrary tilt, if the left reveal surfaces are illuminated the right surfaces will not be, and vice versa. And if the bottom reveal surfaces are illuminated the top surfaces will not be, and vice versa. (Of course, for a vertical window, the top reveal surfaces will never be illuminated by beam solar if the reveal surfaces are perpendicular to the glazing, as is being assumed.
-
-For each shadow pattern in Figure 99, equations are given for the shadowed areas <span>\({A_{1,sh}}\)</span> and *<span>\({A_{2,sh}}\)</span>* of the outside and inside reveal surfaces, respectively. The variables in these equations are the following (see also Figure 100):
-
-<span>\({d_1}\)</span>        = depth of outside reveal, measured from the outside plane of the glazing to the edge of the reveal, plus one half of the glazing thickness.
-
-<span>\({d_2}\)</span>        = depth of inside reveal (or, for illumination on bottom reveal surfaces,  inside sill depth), measured from the inside plane of the glazing to the edge of the reveal or the sill, plus one half of the glazing thickness.
-
-<span>\(L\)</span>        = window height for vertical reveal surfaces or window width for horizontal reveal surfaces
-
-<span>\(\alpha \)</span>          = vertical solar profile angle for shadowing on vertical reveal surfaces or horizontal solar profile angle for shadowing on horizontal reveal surfaces.
-
-<span>\({p_1}({p_2})\)</span> = distance from outside (inside) surface of frame to glazing midplane.
-
-<span>\({d_2}^\prime \)</span>      = depth of shadow cast by top reveal on bottom reveal, or by left reveal on right reveal, or by right reveal on left reveal.
-
-<span>\({d_2}^{\prime \prime }\)</span>     = depth of shadow cast by frame.
-
-
-
-For simplicity it is assumed that, for the case without a frame, the shadowed and illuminated areas extend into the glazing region. For this reason, <span>\({d_1}\)</span>and <span>\({d_2}\)</span>are measured from the midplane of the glazing. For the case with a frame, the beam solar absorbed by the surfaces formed by the frame outside and inside projections perpendicular to the glazing is calculated as described in “Window Frame and Divider Calculation: Calculation of Solar Radiation Absorbed by Frame.�
-
-
-
-Figure 99.  Expression for area of shaded regions for different shadow patterns: (a) window without frame, (b) window with frame
-
-![](media/image1605.png)
-
-![](media/image1606.png)
-
-![](media/image1607.png)
-
-Figure 100.  Vertical section through a vertical window with outside and inside reveal showing calculation of the shadows cast by the top reveal onto the inside sill and by the frame onto the inside sill.
-
-The following logic gives expressions for the shadowed areas for all possible shadow patterns. Here:
-
-d1 = <span>\({d_1}\)</span>
-
-d2= <span>\({d_2}\)</span>
-
-P1 = <span>\({p_1}\)</span>
-
-P2= <span>\({p_2}\)</span>
-
-f1= <span>\({d_1} - {p_1}\)</span>
-
-f2= <span>\({d_2} - {p_2}\)</span>
-
-d2prime = <span>\({d_2}^\prime \)</span>
-
-d2prime2= <span>\({d_2}^{\prime \prime }\)</span>
-
-d12 = <span>\({d_1} + {d_2} - {d_2}^\prime \)</span>
-
-TanAlpha = <span>\(\tan \alpha \)</span>
-
-A1sh= <span>\({A_{1,sh}}\)</span>
-
-A2sh= <span>\({A_{2,sh}}\)</span>
-
-L = <span>\(L\)</span>
-
-L1 = average distance to frame of illuminated area of outside reveal (used to calculate view factor to frame).
-
-L2 = average distance to frame of illuminated area of inside reveal (used to calculate view factor to frame).
-
-
-```
- IF(window does not have a frame) THEN
-      IF(d2prime <= d2) THEN
-     IF(d12*TanAlpha <= L) THEN
-       A1sh = 0.5*TanAlpha*d1**2
-       A2sh = d2prime*L + 0.5*TanAlpha*d12**2 - A1sh
-     ELSE  ! d12*TanAlpha > L
-       IF(d1*TanAlpha <= L) THEN
-         A1sh = 0.5*TanAlpha*d1**2
-         A2sh = d2*L - 0.5*TanAlpha*(L/TanAlpha - d1)**2
-       ELSE  ! d1*TanAlpha > L
-         A1sh = d1*L - (0.5/TanAlpha)*L**2
-         A2sh = d2*L
-       END IF
-     END IF
-   ELSE  ! d2prime > d2
-     A2sh = d2*L
-     IF(d2prime &lt; d1+d2) THEN
-       IF(d12*TanAlpha <= L) THEN
-         A1sh = L*(d2prime-d2) + 0.5*TanAlpha*d12**2
-       ELSE  ! d12*TanAlpha > L
-         A1sh = d1*L - 0.5*L**2/TanAlpha
-       END IF
-     ELSE  ! d2prime >= d1+d2
-       A1sh = d1*L
-     END IF
-   END IF
- ELSE  ! Window has a frame
-  f1 = d1-P1
-  f2 = d2-P2
-  d2prime2 = FrameWidth/TanGamma
-  IF(vertical reveal) THEN  ! Vertical reveal
-    IF(InsReveal+0.5*GlazingThickness <= P2) d2 = P2 + 0.001
-  ELSE                      ! Horizontal
-    IF(bottom reveal surfaces may be illuminated) THEN
-      ! Bottom reveal surfaces may be illuminated
-      IF(InsSillDepth+0.5*GlazingThickness<=P2) d2= P2 + 0.001
-    ELSE
-      ! Top reveal surfaces may be illuminated
-      IF(InsReveal+0.5*GlazingThickness <= P2) d2 = P2 + 0.001
-    END IF
-  END IF
-  IF(d2prime <= f2) THEN
-    ! Shadow from opposing reveal does not go beyond inside
-     !  surface of frame
-    IF(d12*TanAlpha <= L) THEN
-      A1sh = 0.5*TanAlpha*f1**2
-      L1   = f1*(f1*TanAlpha/(6*L)+0.5)
-      IF(d2-(d2prime+d2prime2+P2) >= 0.) THEN
-        A2sh = (d2prime+d2prime2)*L + &
-          0.5*TanAlpha*((d1+d2-d2prime)**2-d1+p2+d2prime2)**2)
-        L2   = d2prime2 + 0.5*(d2-(d2prime+d2prime2+P2))
-      ELSE  ! d2-(d2prime+d2prime2+P2) &lt; 0.
-        ! Inside reveal is fully shadowed by frame and/or
-         !opposing reveal
-        A2sh = f2*L
-        L2   = f2
-      END IF
-    ELSE  ! d12*TanAlpha >= L
-      IF((d1+P2)*TanAlpha <= L) THEN
-        A1sh = 0.5*TanAlpha*f1**2
-        L1 = f1*((f1*TanAlpha)/(6*L) + 0.5)
-        IF((d1+P2+d2prime2)*TanAlpha >= L) THEN
-          A2sh = f2*L
-          L2   = f2
-        ELSE  ! (d1+P2+d2prime2)*TanAlpha &lt; L
-          A2sh = f2*L - 0.5*(L-(d1+P2)*TanAlpha)**2/TanAlpha &
-             + d2prime2*(L-(d1+P2+d2prime2/2)*TanAlpha)
-          L2 = d2prime2 + (L/TanAlpha - (d1+P2+d2prime2))/3
-        END IF
-      ELSE  ! (d1+P2)*TanAlpha > L
-        L2 = f2
-        A2sh = f2*L
-        IF(f1*TanAlpha <= L) THEN
-          A1sh = 0.5*TanAlpha*f1**2
-          L1 = f1*((f1*TanAlpha)/(6*L) + 0.5)
-        ELSE  ! f1*TanAlpha > L
-          A1sh = f1*L - 0.5*L**2/TanAlpha
-          L1 = f1-(L/TanAlpha)/3
-        END IF
-      END IF
-    END IF
-  ELSE
-     ! d2prime > f2 -- Shadow from opposing reveal goes beyond
-     ! inside of frame
-    A2sh = f2*L
-    L2 = f2
-    IF(d2prime >= d1+d2) THEN
-      A1sh = 0.0
-      L1   = f1
-    ELSE  ! d2prime &lt; d1+d2
-      IF(d2prime <= d2+P1) THEN
-        IF(f1*TanAlpha <= L) THEN
-          A1sh = 0.5*TanAlpha*f1**2
-          L1 = f1*((f1*TanAlpha)/(6*L) + 0.5)
-        ELSE  ! f1*TanAlpha > L
-          A1sh = f1*L - 0.5*L**2/TanAlpha
-              L1   = f1 - (L/TanAlpha)/3
-            END IF
-          ELSE  ! d2prime > d2+P1
-            IF(d12*TanAlpha <= L) THEN
-              A1sh = L*(d2prime-(d2+P1)) + 0.5*TanAlpha*d12**2
-              L1   = (L*(f1-d12/2)-d12*TanAlpha* &
-                 (f1/2-d12/3))/(L-d12*TanAlpha/2)
-            ELSE  ! d12*TanAlpha > L
-              A1sh = f1*L - 0.5*L**2/TanAlpha
-              L1   = f1 - (L/TanAlpha)/3
-            END IF
-          END IF
-        END IF
-      END IF
-      FracToGlassOuts = 0.5*(1.0 - ATAN(FrameWidth/L1)/PiOvr2)
-      FracToGlassIns  = 0.5*(1.0 - ATAN(FrameWidth/L2)/PiOvr2)
-    END IF  ! End of check if window has frame
-```
-
-
-The beam solar reflected from a sunlit region of area <span>\(A\)</span>is given by
-
-<div>$$R = {I_B}A\cos \beta (1 - a){\rm{ }}$$</div>
-
-where
-
-<span>\(R\)</span>= reflected solar radiation [W]
-
-<span>\({I_B}\)</span>= beam normal irradiance [W/m<sup>2</sup>]
-
-<span>\(A\)</span>= sunlit area [m<sup>2</sup>]
-
-<span>\(\beta \)</span>= beam solar angle of incidence on reveal surface
-
-<span>\(a\)</span>= solar absorptance of reveal surface
-
-All reflected radiation is assumed to be isotropic diffuse. For outside reveal surfaces it is assumed that <span>\(R/2\)</span> goes toward the window and <span>\(R/2\)</span> goes to the exterior environment. Of the portion that goes toward the window a fraction <span>\({F_1}\)</span> goes toward the frame, if present, and <span>\(1 - {F_1}\)</span> goes toward the glazing.
-
-The view factor <span>\({F_1}\)</span> to the frame calculated by assuming that the illuminated area can be considered to be a line source. Then the area-weighted average distance, <span>\({L_1}\)</span>, of the source to the frame is calculated from the shape of the illuminated area (see above psuedo-code). Then <span>\({F_1}\)</span> is related as follows to the average angle subtended by the frame of width <span>\({w_f}\)</span>:
-
-<div>$${F_1} = \frac{{{{\tan }^{ - 1}}({w_f}/{L_1})}}{{\pi /2}}$$</div>
-
-For the portion going towards the frame, <span>\((R/2){F_1}{a_f}\)</span>is absorbed by the frame (where <span>\({a_f}\)</span>is the solar absorptance of the frame) and contributes to the frame heat conduction calculation. The rest, <span>\((R/2){F_1}(1 - {a_f})\)</span>, is assumed to be reflected to the exterior environment.
-
-If the glazing has diffuse transmittance <span>\({\tau_{diff}}\)</span>, diffuse front reflectance <span>\(\rho_{diff}^f\)</span>, and layer front absorptance <span>\(\alpha_{l,diff}^f\)</span>, then, of the portion, <span>\((R/2)(1 - {F_1})\)</span>, that goes toward the glazing, <span>\((R/2)(1 - {F_1}){\tau_{diff}}\)</span>is transmitted to the zone, <span>\((R/2)(1 - {F_1})\alpha_{l,diff}^f\)</span>is absorbed in glass layer <span>\(l\)</span>and contributes to the glazing heat balance calculation, and <span>\((R/2)(1 - {F_1})\rho_{dif{f_{}}}^f\)</span>is reflected to the exterior environment.
-
-The beam solar absorbed by an outside reveal surface is added to the other solar radiation absorbed by the outside of the window’s parent wall.
-
-For inside reveal surfaces it is assumed that <span>\(R/2\)</span> goes towards the window and <span>\(R/2\)</span> goes into the zone. Of the portion that goes toward the window a fraction <span>\((R/2){F_2}\)</span> goes toward the frame, if present, and <span>\((R/2)(1 - {F_2})\)</span>goes toward the glazing (<span>\({F_2}\)</span> is calculated using a method analogous to that used for <span>\({F_1}\)</span>). For the portion going towards the frame, <span>\((R/2){F_2}{a_f}\)</span>is absorbed by the frame and contributes to the frame heat conduction calculation. The rest, <span>\((R/2){F_2}(1 - {a_f})\)</span>, is assumed to be reflected back into the zone.
-
-If the glazing has diffuse back reflectance <span>\(\rho_{diff}^b\)</span>, and layer back absorptance <span>\(\alpha_{l,diff}^b\)</span>, then, of the portion <span>\((R/2)(1 - {F_2})\)</span> that goes toward the glazing, <span>\((R/2)(1 - {F_2}){\tau_{diff}}\)</span>is transmitted back out the glazing, <span>\((R/2)(1 - {F_2})\alpha_{l,diff}^b\)</span>is absorbed in glass layer <span>\(l\)</span>and contributes to the glazing heat balance calculation, and <span>\((R/2)(1 - {F_2})\rho_{dif{f_{}}}^b\)</span>is reflected into the zone.
-
-The beam solar absorbed by an inside reveal surface is added to the other solar radiation absorbed by the inside of the window’s parent wall.
-
-### Shading Device Thermal Model
-
-Shading devices in EnergyPlus can be on the exterior or interior sides of the window or between glass layers. The window shading device thermal model accounts for the thermal interactions between the shading layer (shade, screen or blind) and the adjacent glass, and between the shading layer and the room (for interior shading) or the shading layer and the outside surround (for exterior shading).
-
-An important feature of the shading device thermal model is calculating the natural convection airflow between the shading device and glass. This flow affects the temperature of the shading device and glazing and, for interior shading, is a determinant of the convective heat gain from the shading layer and glazing to the zone air. The airflow model is based on one described in the ISO Standard 15099, “Thermal Performance of Windows, Doors and Shading Devices—Detailed Calculations� [ISO15099, 2001]. (Between-glass forced airflow is also modeled; see “Airflow Windows.�)
-
-The following effects are considered by the shading device thermal model:
-
-* For interior and exterior shading device: Long-wave radiation (IR) from the surround absorbed by shading device, or transmitted by the shading device and absorbed by the adjacent glass. For interior shading the surround consists of the other zone surfaces. For exterior shading the surround is the sky and ground plus exterior shadowing surfaces and exterior building surfaces “seen� by the window.
-
-* Inter-reflection of IR between the shading device and adjacent glass.
-
-* Direct and diffuse solar radiation absorbed by the shading device.
-
-* Inter-reflection of solar radiation between shading layer and glass layers.
-
-* Convection from shading layer and glass to the air in the gap (or, for between-glass shading, gaps) between the shading layer and adjacent glass, and convection from interior shading layer to zone air or from exterior shading layer to outside air.
-
-* Natural convection airflow in the gap (or, for between-glass shading, gaps) between shading layer and adjacent glass induced by buoyancy effects, and the effect of this flow on the shading-to-gap and glass-to-gap convection coefficients.
-
-* For interior shading, convective gain (or loss) to zone air from gap airflow.
-
-In the following it is assumed that the shading device, when in place, covers the glazed part of the window (and dividers, if present) and is parallel to the glazing. For interior and exterior shading devices it is assumed that the shading layer is separated from the glazing by an air gap. A between-glass shading layer is assumed to be centered between two glass layers and separated from the adjacent glass layers by gaps that is filled with the same gas. If the window has a frame, it is assumed that the shading device does *not* cover the frame.
-
-### Heat Balance Equations for Shading Device and Adjacent Glass
-
-If a window shading device is deployed the heat balance equations for the glass surfaces facing the shading layer are modified, and two new equations, one for each face of the shading layer, are added. Figure 101 illustrates the case of double glazing with an interior shading device.
-
-
-
-![](media/image1663.png)
-
-Figure 101. Glazing system with two glass layers and an interior shading layer showing variables used in heat balance equations.
-
-
-
-The heat balance equation for the glass surface facing the gap between glass and shading layer (called in the following, “gap�) is
-
-<div>$$\frac{{{E_i}{\varepsilon_4}{\tau_{sh}}}}{{1 - {\rho_4}{\rho_{sh}}}} + \frac{{\sigma {\varepsilon_4}}}{{1 - {\rho_4}{\rho_{sh}}}}\left[ {\theta_5^4{\varepsilon_{sh}} - \theta_4^4(1 - {\rho_{sh}})} \right] + {k_2}\left( {{\theta_3} - {\theta_4}} \right) + {h_{cv}}\left( {{T_{gap}} - {\theta_4}} \right) + {S_4} = 0$$</div>
-
-where
-
-*Ï„<sub>sh</sub>* = IR diffuse transmittance of shading device
-
-*ε<sub>sh</sub>* = diffuse emissivity of shading device
-
-*�<sub>sh</sub>* = IR diffuse reflectance of shading device ( = 1 - ( *τ<sub>sh</sub>* + *ε<sub>sh</sub>*))
-
-*θ<sub>5</sub>* = temperature of the surface of the shading layer that faces the gap (K).
-
-The term 1 – *�<sub>4</sub> �<sub>sh</sub>* accounts for the inter-reflection of IR radiation between glass and shading layer.
-
-The convective heat transfer from glass layer \#2 to the air in the gap is
-
-<div>$${q_{c,gl}} = {h_{cv}}({\theta_4} - {T_{gap}})$$</div>
-
-where
-
-*T<sub>gap</sub>* = effective mean temperature of the gap air (K).
-
-*h<sub>cv</sub>*= convective heat transfer coefficient from glass or shading layer to gap air (W/m<sup>2</sup>K).
-
-The corresponding heat transfer from shading layer to gap air is
-
-<div>$${q_{c,sh}} = {h_{cv}}({\theta_5} - {T_{gap}})$$</div>
-
-The convective heat transfer coefficient is given by
-
-<div>$${h_{cv}} = 2{h_c} + 4v$$</div>
-
-where
-
-*h<sub>c</sub>*= surface-to-surface heat transfer coefficient for non-vented (closed) cavities (W/m<sup>2</sup>K)
-
-*v* = mean air velocity in the gap (m/s).
-
-The quantities *h<sub>cv</sub>* and *T<sub>gap</sub>* depend on the airflow velocity in the gap, which in turn depends on several factors, including height of shading layer, glass/shading layer separation (gap depth), zone air temperature for interior shading or outside air temperature for exterior shading, and shading layer and glass face temperatures. The calculation of *h<sub>cv</sub>* and *T<sub>gap</sub>* is described in the following sections.
-
-The heat balance equation for the shading layer surface facing the gap is
-
-<div>$$
-  \frac{E_i \tau_{sh} \rho_4 \varepsilon_{sh}} {1 - \rho_4 \rho_{sh}} + 
-  \frac{\sigma \varepsilon_{sh}} {1 - \rho_4 \rho_{sh}} \left[
-    \varepsilon_4 \theta_4^4 - \theta_5^4 (
-      1 - \rho_4( 
-        \varepsilon_{sh} + \rho_{sh}
-      )
-    )
-  \right] + 
-  k_{sh} \left(
-    \theta_6 - \theta_5
-  \right) + 
-  h_{cv} \left(
-    T_{gap} - \theta_5
-  \right) + 
-  S_{sh,1} = 0
-$$</div>
-
-where
-
-*k<sub>sh</sub>* = shading layer conductance (W/m<sup>2</sup>K).
-
-*θ<sub>6</sub>* = temperature of shading layer surface facing the zone air (K).
-
-*S<sub>sh,1</sub>* = solar radiation plus short-wave radiation from lights plus IR radiation from lights and zone equipment absorbed by the gap-side face of the shading layer (W/m<sup>2</sup>K).
-
-The heat balance equation for the shading layer surface facing the zone air is
-
-<div>$${E_i}{\varepsilon_{sh}} - {\varepsilon_{sh}}\sigma \theta_6^4 + {k_{sh}}\left( {{\theta_5} - {\theta_6}} \right) + {h_i}\left( {{T_i} - {\theta_6}} \right) + {S_{sh,2}} = 0$$</div>
-
-where
-
-*S<sub>sh,2</sub>* = solar radiation plus short-wave radiation from lights plus IR radiation from lights and zone equipment absorbed by the zone-side face of the shading layer (W/m<sup>2</sup>K).
-
-### Solving for Gap Airflow and Temperature
-
-For interior and exterior shading devices a pressure-balance equation is used to determine gap air velocity, gap air mean equivalent temperature and gap outlet air temperature given values of zone air temperature (or outside temperature for exterior shading), shading layer face temperatures and gap geometry. The pressure balance equates the buoyancy pressure acting on the gap air to the pressure losses associated with gap airflow between gap inlet and outlet [ISO15099, 2001]. The variables used in the following analysis of the interior shading case are shown in Figure 102.
-
-![](media/image1670.png)
-
-Figure 102.  Vertical section (a) and perspective view (b) of glass layer and interior shading layer showing variables used in the gap airflow analysis. The opening areas *A<sub>bot</sub>*, *A<sub>top</sub>*, *A<sub>l</sub>*, *A<sub>r</sub>* and *A<sub>h</sub>* are shown schematically.
-
-#### Pressure Balance Equation
-
-The pressure balance equation for airflow through the gap is
-
-<div>$$\Delta {p_T} = \Delta {p_B} + \Delta {p_{HP}} + \Delta {p_Z}$$</div>
-
-Here, *Δp<sub>T</sub>*is the driving pressure difference between room air and gap air. It is given by
-
-<div>$$\Delta {p_T} = {\rho_0}{T_0}gH\sin \phi \frac{{\left| {{T_{gap}} - {T_{gap,in}}} \right|}}{{{T_{gap}}{T_{gap,in}}}}$$</div>
-
-where
-
-*�<sub>0</sub>* = density of air at temperature *T<sub>0</sub>* (kg/m<sup>3</sup>)
-
-*T<sub>0</sub>* = reference temperature (283K)
-
-*g* = acceleration due to gravity (m/s<sup>2</sup>)
-
-*H* = height of shading layer (m)
-
-*φ* = tilt angle of window (vertical = 90<sup>o</sup>)
-
-*T<sub>gap</sub>* = effective mean temperature of the gap air (K)
-
-*T<sub>gap,in</sub>* = gap inlet temperature ( = zone air temperature for interior shading) (K)
-
-The *Δp<sub>B</sub>* term is due to the acceleration of air to velocity *v* (Bernoulli’s law). It is given by
-
-<div>$$\Delta {p_B} = \frac{\rho }{2}{v^2}{\rm{    (Pa)}}$$</div>
-
-where  *�*is the gap air density evaluated at *T<sub>gap</sub>* (kg/m<sup>3</sup>).
-
-The *Δp<sub>HP</sub>* term represents the pressure drop due to friction with the shading layer and glass surfaces as the air moves through the gap. Assuming steady laminar flow, it is given by the Hagen-Poiseuille law for flow between parallel plates [Munson et al. 1998]:
-
-<div>$$\Delta {p_{HP}} = 12\mu \frac{H}{{{s^2}}}{v^{}}{\rm{    (Pa)}}$$</div>
-
-where * μ*  is the viscosity of air at temperature *T<sub>gap</sub>* (Pa-s).
-
-The  *Δp<sub>Z</sub>* term is the sum of the pressure drops at the inlet and outlet openings:
-
-<div>$$\Delta {p_Z} = \frac{{\rho {v^2}}}{2}\left( {{Z_{in}} + {Z_{out}}} \right){\rm{    (Pa)}}$$</div>
-
-Here, the inlet pressure drop factor,* Z<sub>in</sub>*, and the outlet pressure drop factor, *Z<sub>out</sub>*, are given by
-
-<div>$$
-  \begin{array}{rl}
-    Z_{in}  &= \left( \frac{A_{gap}}{0.66A_{eq,in}}  - 1 \right)^2 \\
-    Z_{out} &= \left( \frac{A_{gap}}{0.60A_{eq,out}} - 1 \right)^2
-  \end{array}
-$$</div>
-
-<div>$$\begin{array}{l}{Z_{in}} = {\left( {\frac{{{A_{gap}}}}{{0.66{A_{eq,in}}}} - 1} \right)^2}\\\{Z_{out}} = {\left( {\frac{{{A_{gap}}}}{{0.60{A_{eq,out}}}} - 1} \right)^2}\end{array}$$</div>
-
-where
-
-*A<sub>eq,in</sub>* = equivalent inlet opening area (m<sup>2</sup>)
-
-*A<sub>eq,out</sub>* = equivalent outlet opening area (m<sup>2</sup>)
-
-*A<sub>gap</sub>* = cross-sectional area of the gap = *sW*(m<sup>2</sup>)
-
-If  T<sub>gap</sub> &gt; T<sub>gap,in</sub>
-
-<div>$$
-  \begin{array}{rl}
-    A_{eq,in}  &= A_{bot} + \frac{A_{top}}{2(A_{bot}+A_{top}} \left( A_l + A_r + A_h \right) \\
-    A_{eq,out} &= A_{top} + \frac{A_{bot}}{2(A_{bot}+A_{top}} \left( A_l + A_r + A_h \right) 
-  \end{array}
-$$</div>
-
-If  T<sub>gap</sub> ≤ T<sub>gap,in</sub>
-
-<div>$$
-  \begin{array}{rl}
-    A_{eq,in}  &= A_{top} + \frac{A_{bot}}{2(A_{bot}+A_{top}} \left( A_l + A_r + A_h \right) 
-    A_{eq,out} &= A_{bot} + \frac{A_{top}}{2(A_{bot}+A_{top}} \left( A_l + A_r + A_h \right) \\
-  \end{array}
-$$</div>
-
-Here, the area of the openings through which airflow occurs (see Figure 102 and Figure 103) are defined as follows:
-
-A<sub>bot</sub> = area of the bottom opening (m<sup>2</sup>)
-
-A<sub>top</sub> = area of the top opening (m<sup>2</sup>)
-
-A<sub>l</sub> = area of the left-side opening (m<sup>2</sup>)
-
-A<sub>r</sub> = area of the right-side opening (m<sup>2</sup>)
-
-A<sub>h</sub> = air permeability of the shading device expressed as the total area of openings (“holes�) in the shade surface (these openings are assumed to be uniformly distributed over the shade) (m<sup>2</sup>)
-
-Figure 103 shows examples of A<sub>bot</sub>, A<sub>top</sub>, A<sub>l</sub> and A<sub>r</sub> for different shading device configurations.  These areas range from zero to a maximum value equal to the associated shade/screen/blind-to-glass cross-sectional area; i.e., A<sub>bot</sub> and A<sub>top</sub> ≤ sW,  A<sub>l</sub> and A<sub>r</sub> ≤ sH.
-
-![](media/image1679.png)
-
-Figure 103.  Examples of openings for an interior shading layer covering glass of height H and width W. Not to scale. (a) Horizontal section through shading layer with openings on the left and right sides (top view). (b) Vertical section through shading layer with openings at the top and bottom (side view).
-
-Expression for the Gap Air Velocity
-
- Expressing Equation in terms of  v  yields the following quadratic equation:
-
-<div>$$\frac{{\rho {v^2}}}{2}\left( {1 + {Z_{in}} + {Z_{out}}} \right) + \frac{{12\mu H}}{{{s^2}}}v - {\rho_0}{T_0}gH\sin \phi \frac{{\left| {{T_{gap,in}} - {T_{gap}}} \right|}}{{{T_{gap,in}}{T_{gap}}}} = 0$$</div>
-
-Solving this gives
-
-<div>$$v = \frac{{{{\left[ {{{\left( {\frac{{12\mu H}}{{{s^2}}}} \right)}^2} + \frac{{2{\rho ^2}(1 + {Z_{in}} + {Z_{out}}){\rho_0}{T_0}gH\sin \phi \left| {{T_{gap,in}} - {T_{gap}}} \right|}}{{{T_{gap,in}}{T_{gap}}}}} \right]}^{1/2}} - \frac{{12\mu H}}{{{s^2}}}}}{{\rho (1 + {Z_{in}} + {Z_{out}})}}$$</div>
-
-The choice of the root of the quadratic equation is dictated by the requirement that *v* = 0 if *T<sub>gap,in</sub>* = *T<sub>gap</sub>*.
-
-Gap Outlet Temperature and Equivalent Mean Air Temperature
-
-The temperature of air in the gap as a function of distance, *h*, from the gap inlet (Figure 104) is
-
-<div>$${T_{gap}}(h) = {T_{ave}} - ({T_{ave}} - {T_{gap,in}}){e^{ - h/{H_0}}}$$</div>
-
-where
-
-<div>$${T_{ave}} = \frac{{{T_{gl}} + {T_{sh}}}}{2}$$</div>
-
-is the average temperature of the glass and shading layer surfaces facing the gap (K).
-
-*H<sub>0</sub>*= characteristic height (m), given by
-
-<div>$${H_0} = \frac{{\rho {C_p}s}}{{2{h_{cv}}}}v$$</div>
-
-where *C<sub>p</sub>* is the heat capacity of air.
-
-The gap outlet temperature is given by
-
-<div>$${T_{gap,out}} = {T_{ave}} - ({T_{ave}} - {T_{gap,in}}){e^{ - H/{H_0}}}$$</div>
-
-The thermal equivalent mean temperature of the gap air is
-
-<div>$${T_{gap}} = \frac{1}{H}\int\limits_0^H {{T_{gap}}(h)dh = {T_{ave}} - \frac{{{H_0}}}{H}} \left( {{T_{gap,out}} - {T_{gap,in}}} \right)$$</div>
-
-![](media/image1687.png)
-
-Figure 104.  Variation of gap air temperature with distance from the inlet for upward flow.
-
-Solution Sequence for Gap Air Velocity and Outlet Temperature
-
-The routine WinShadeGapFlow is called within the glazing heat balance iterative loop in SolveForWindowTemperatures to determine *v* and *T<sub>gap,out</sub>*. The solution sequence in WinShadeGapFlow is as follows:
-
-At start of iteration, guess *T<sub>gap</sub>* as ((*T<sub>gl</sub>* + *T<sub>sh</sub>*)/2 + *T<sub>gap,in</sub>*)/2. Thereafter use value from previous iteration.
-
-Get still-air conductance, *h<sub>c</sub>*, by calling WindowGasConductance and NusseltNumber.
-
-Get *v* from Equation
-
-Get *h<sub>cv</sub>* from Equation
-
-Get *T<sub>ave</sub>*from Equation
-
-Get *T<sub>gap,out</sub>* from Equation
-
-Get new value of *T<sub>gap</sub>*from Equation
-
-The values of *h<sub>cv</sub>* and *T<sub>gap</sub>* so determined are then used in the window heat balance equations to find new values of the face temperatures of the glass and shading layers. These temperatures are used in turn to get new values of *h<sub>cv</sub>* and *T<sub>gap</sub>* until the whole iterative process converges.
-
-Convective Heat Gain to Zone from Gap Airflow
-
-The heat added (or removed) from the air as it passes through the gap produces a convective gain (or loss) to the zone air given by
-
-<div>$${q_v} = LW\left[ {{h_{cv}}\left( {{T_{gl}} - {T_{gap}}} \right) + {h_{cv}}\left( {{T_{sh}} - {T_{gap}}} \right)} \right] = 2{h_{cv}}LW\left( {{T_{ave}} - {T_{gap}}} \right){\rm{    (W)}}$$</div>
-
-This can also be expressed as
-
-<div>$${q_v} = \dot m{C_p}\left( {{T_{gap,out}} - {T_{gap,in}}} \right){\rm{    (W)}}$$</div>
-
-where the air mass flow rate in the gap is given by
-
-<div>$$\dot m = \rho {A_{gap}}v{\rm{    (kg/s)}}$$</div>
-
-### Heat Balance Equations for Between-Glass Shading Device
-
-In EnergyPlus shading devices are allowed between the two glass panes of double glazing and between the two inner glass panes of triple glazing. Figure 105 shows the case of a between-glass shading device in double glazing.
-
-
-
-![](media/image1691.png)
-
-Figure 105. Glazing system with two glass layers and a between-glass shading device showing variables used in the heat balance equations.
-
-
-
-The heat balance equations for the two glass surfaces facing the shading device are the following.
-
-For face \#2:
-
-<div>$$
-  h_{cv,1} (T_{gap,1}-\theta_2) + k_1 (\theta_1-\theta_2) +
-    \frac{\sigma \epsilon_2}{1-\rho_2 R_1} \left[
-      \frac{\tau_{sh}}{1-\rho_6\rho_3} (
-        \epsilon_3 \theta_3^4 + \epsilon_6\theta_6^4\rho_3
-      )
-      + \epsilon_5\theta_5^4 + \epsilon_2\theta_2^4R_1
-    \right]
-$$</div>
-
-where
-
-<div>$${R_1} = {\rho_5} + \frac{{\tau_{sh}^2{\rho_3}}}{{1 - {\rho_6}{\rho_3}}}$$</div>
-
-<span>\({T_{gap,1}} = \)</span> effective mean air temperature in gap 1 (K)
-
-<span>\({h_{cv,1}} = \)</span> convective heat transfer coefficient from glass or shading layer to gas in gap 1 (W/m<sup>2</sup>K)
-
-For face \#3:
-
-<div>$$
-  h_{cv,2} (T_{gap,2}-\theta_3) + k_2 (\theta_4-\theta_3) +
-    \frac{\sigma \epsilon_3}{1-\rho_3 R_2} \left[
-      \frac{\tau_{sh}}{1-\rho_5\rho_2} (
-        \epsilon_3 \theta_2^4 + \epsilon_5\theta_5^4\rho_2
-      )
-      + \epsilon_6\theta_6^4 + \epsilon_7\theta_3^4R_2
-    \right]
-$$</div>
-
-where
-
-<div>$${R_2} = {\rho_6} + \frac{{\tau_{sh}^2{\rho_2}}}{{1 - {\rho_5}{\rho_2}}}$$</div>
-
-<span>\({T_{gap,2}} = \)</span> effective mean air temperature in gap 2 (K)
-
-<span>\({h_{cv,2}} = \)</span> convective heat transfer coefficient from glass or shading layer to gas in gap 2 (W/m<sup>2</sup>K)
-
-The heat balance equations for the shading layer faces are:
-
-For face \#5:
-
-<div>$$
-  h_{cv,1} (T_{gap,1}-\theta_5) + k_sh (\theta_6-\theta_5) +
-    \frac{\sigma \epsilon_5}{1-\rho_2 R_1} \left[
-      \frac{\tau_{sh}\rho_2}{1-\rho_5\rho_3} (
-        \epsilon_3 \theta_3^4 + \epsilon_6\theta_6^4\rho_3
-      )
-      + \epsilon_2\theta_2^4 + \epsilon_5\theta_5^4\rho_2
-    \right]
-$$</div>
-
-For face \#6:
-
-<div>$$
-  h_{cv,2} (T_{gap,2}-\theta_3) + k_2 (\theta_4-\theta_3) +
-    \frac{\sigma \epsilon_3}{1-\rho_3 R_2} \left[
-      \frac{\tau_{sh}}{1-\rho_5\rho_2} (
-        \epsilon_2 \theta_2^4 + \epsilon_5\theta_5^4\rho_2
-      )
-      + \epsilon_2\theta_2^4 + \epsilon_7\theta_3^4R_2
-    \right]
-$$</div>
-
-The convective heat transfer coefficients are given by
-
-<div>$$\begin{array}{l}{h_{cv,1}} = 2{h_{c,1}} + 4v\\\{h_{cv,2}} = 2{h_{c,2}} + 4v\end{array}$$</div>
-
-where
-
-<span>\({h_{c,1}},{h_{c,2}} = \)</span>     surface-to-surface heat transfer coefficients for gap \#1 and \#2,  respectively,  when these gaps are non-vented (closed).
-
-<span>\(v = \)</span>               air velocity in the gaps (m/s). It is assumed that the gap widths are equal, so that the velocity of flow in the gaps is equal and opposite, i.e., when the airflow is upward in gap \#1 it is downward in gap \#2 and vice-versa.
-
-In analogy to the interior or exterior shading device case, the air velocity is determined by solving the following pressure balance equation:
-
-
-
-<div>$$\Delta {p_{T,1,2}} = \Delta {p_{B,1}} + \Delta {p_{HP,1}} + \Delta {p_{Z,1}} + \Delta {p_{B,2}} + \Delta {p_{HP,2}} + \Delta {p_{Z,2}}$$</div>
-
-where the driving pressure difference between gap \#1 and \#2 is
-
-<div>$$\Delta {p_{T,1,2}} = {\rho_0}{T_0}gH\sin \phi \frac{{\left| {{T_{gap,1}} - {T_{gap,2}}} \right|}}{{{T_{gap,1}}{T_{gap,2}}}}{\rm{      (Pa)}}$$</div>
-
-The pressure drops on the right-hand side of this equation are:
-
-<div>$$\begin{array}{l}\Delta {p_{B,i}} = \frac{{{\rho_{gap,}}_i}}{2}{v^2}\\\Delta {p_{HP,i}} = 12{\mu_{gap,}}_i\frac{H}{{{s^2}}}\\\Delta {p_{Z,i}} = \frac{{{\rho_{gap,}}_i{v^2}}}{2}({Z_{in,i}} + {Z_{out,i}})\end{array}$$</div>
-
-where *i* = gap number (1 or 2).
-
-It can be shown that <span>\({Z_{in,1}} + {Z_{out,1}} = {Z_{in,2}} + {Z_{out,2}}\)</span>. Then, inserting these pressure drop expressions into , we obtain the following expression for the airflow velocity:
-
-<div>$$v = \frac{{{{\left[ {{{\left( {\frac{{12({\mu_{gap,}}_1 + {\mu_{gap,}}_2)H}}{{{s^2}}}} \right)}^2} + 2\Delta {p_{T,1,2}}({\rho_{gap,1}} + {\rho_{gap,2}})(1 + {Z_{in}} + {Z_{out}})} \right]}^{1/2}} - \frac{{12({\mu_{gap,}}_1 + {\mu_{gap,}}_2)H}}{{{s^2}}}}}{{({\rho_{gap,}}_1 + {\rho_{gap,}}_2)(1 + {Z_{in}} + {Z_{out}})}}$$</div>
-
-The choice of the sign of the square root term is dictated by the requirement that <span>\(v = 0\)</span> if <span>\(\Delta {p_{T,1,2}} = 0\)</span>, i.e., <span>\({T_{gap,1}} = {T_{gap,2}}\)</span>.
-
-Given <span>\(v\)</span> we can now calculate <span>\({T_{gap,1}}\)</span>and <span>\({T_{gap,2}}\)</span>, which gives <span>\(\Delta {p_{T,1,2}}\)</span>. The procedure is as follows. We have
-
-<div>$${T_{gap,1,out}} = {T_{ave,1}} - ({T_{ave,1}} - {T_{gap,1,in}}){\xi_1}$$</div>
-
-where <span>\({T_{ave,1}} = ({\theta_2} + {\theta_5})/2\)</span> and <span>\({\xi_1} = {e^{ - \frac{H}{{{H_{0,1}}}}}}\)</span> with <span>\({H_{0,1}} = {\rho_{gap,1}}{C_p}sv/(2{h_{cv,1}})\)</span>. Since <span>\({T_{gap,1,in}} = {T_{gap,2,out}}\)</span> this gives:
-
-  <span>\({T_{gap,1,out}} = {T_{ave,1}} - ({T_{ave,1}} - {T_{gap,2,out}}){\xi_1}\)</span>
-
-Similarly,
-
-<div>$${T_{gap,2,out}} = {T_{ave,2}} - ({T_{ave,2}} - {T_{gap,1,out}}){\xi_2}$$</div>
-
-Solving these simultaneous equations gives:
-
- <span>\(\begin{array}{l}{T_{gap,1,out}} = \frac{{{T_{ave,1}}(1 - {\xi_1}) + {\xi_1}{T_{ave,2}}(1 - {\xi_2})}}{{1 - {\xi_1}{\xi_2}}}\\\\\{T_{gap,2,out}} = \frac{{{T_{ave,2}}(1 - {\xi_2}) + {\xi_2}{T_{ave,1}}(1 - {\xi_1})}}{{1 - {\xi_1}{\xi_2}}}\end{array}\)</span>
-
-Using these in
-
-<div>$${T_{gap,1}} = {T_{ave,1}} - \frac{{{H_{0,1}}}}{H}\left( {{T_{gap,1,out}} - {T_{gap,2,out}}} \right)$$</div>
-
-gives
-
- <span>\({T_{gap,1}} = {T_{ave,1}} - \frac{{{H_{0,1}}}}{H}\xi \left( {{T_{ave,1}} - {T_{ave,2}}} \right)\)</span>
-
-with
-
-<div>$$\xi  = \frac{{(1 - {\xi_1})(1 - {\xi_2})}}{{1 - {\xi_1}{\xi_2}}}$$</div>
-
-Similarly, from
-
-<div>$${T_{gap,2}} = {T_{ave,2}} - \frac{{{H_{0,2}}}}{H}\left( {{T_{gap,2,out}} - {T_{gap,1,out}}} \right)$$</div>
-
-we get
-
-<div>$${T_{gap,2}} = {T_{ave,2}} - \frac{{{H_{0,2}}}}{H}\xi \left( {{T_{ave,2}} - {T_{ave,1}}} \right)$$</div>
-
-The overall solution sequence is as follows.
-
-At start of iteration guess <span>\({T_{gap,1}} = {T_{ave,1}}\)</span> and <span>\({T_{gap,2}} = {T_{ave,2}}\)</span>. Then
-
-1)    Get <span>\({\rho_{gap,1}},{\rho_{gap,2}},{\mu_{gap,1}},{\mu_{gap,2}}\)</span>using <span>\({T_{gap,1}},{T_{gap,2}}\)</span>.
-
-2)    Get still-air conductances <span>\({h_{c,1}},{h_{c,2}}\)</span>by calling WindowGasConductance and NusseltNumber.
-
-3)    Get <span>\(v\)</span> from Equation
-
-4)    Get <span>\({h_{cv,1}},{h_{cv,2}}\)</span>from Equation
-
-5)    Get <span>\({T_{ave,1}},{T_{ave,2}}\)</span>
-
-6)    Get *H<sub>o,1</sub>*, *H<sub>o,2</sub>*, <span>\({\xi_1}\)</span>and <span>\({\xi_2}\)</span>.
-
-7)    Get <span>\({T_{gap,1}}\)</span>,<span>\({T_{gap,2}}\)</span>from Equations and
-
-The values <span>\({h_{cv,1}}{\rm{, }}{h_{cv,2}}{\rm{, }}{T_{gap,1}}\)</span> and <span>\({T_{gap,2}}\)</span>are then used in the face heat balance equations to find new values of the face temperatures <span>\({\theta_2}{\rm{, }}{\theta_3},{\rm{ }}{\theta_5}\)</span>and <span>\({\theta_6}\)</span>. These are used in turn to get new values of <span>\({h_{cv,1}}{\rm{, }}{h_{cv,2}}{\rm{, }}{T_{gap,1}}\)</span> and <span>\({T_{gap,2}}\)</span>until the whole iterative process converges.
-
-### Airflow Windows
-
-In airflow windows forced air flows in the gap between adjacent layers of glass. Such windows are also known as “heat-extract windows� and “climate windows.�
-
-Five configurations of airflow windows are modeled (Figure 106) that depend on the source and destination of forced air. The allowed combinations of Airflow Source and Airflow Destination are:
-
-InsideAir à OutsideAir
-
-InsideAir à InsideAir
-
-InsideAir à ReturnAir
-
-OutsideAir à InsideAir
-
-OutsideAir à OutsideAir
-
-![](media/image1748.png)
-
-Figure 106. Gap airflow configurations for airflow windows. From “Active facades,� Version no. 1, Belgian Building Research Institute, June 2002.
-
-A common application of airflow windows is to reduce the zone cooling load by exhausting indoor air through the window, thereby picking up and rejecting heat from the glazing (Figure 106).
-
-Figure 107 shows the variables used in the heat balance equations for forced airflow in a double-glazed window.
-
-![](media/image1749.png)
-
-Figure 107. Glazing system with forced airflow between two glass layers showing variables used in the heat balance equations.
-
-The heat balance equation for the left-hand glass surface facing the gap in Figure 107 is:
-
-<div>$${k_1}({\theta_1} - {\theta_2}) + {h_{cv}}({T_{gap}} - {\theta_2}) + \sigma \frac{{{\varepsilon_2}{\varepsilon_3}}}{{1 - (1 - {\varepsilon_2})(1 - {\varepsilon_3})}}\left( {\theta_3^4 - \theta_2^4} \right) + {S_2} = 0$$</div>
-
-The corresponding equation for the right-hand glass surface facing the gap is:
-
-<div>$${k_2}({\theta_4} - {\theta_3}) + {h_{cv}}({T_{gap}} - {\theta_3}) + \sigma \frac{{{\varepsilon_2}{\varepsilon_3}}}{{1 - (1 - {\varepsilon_2})(1 - {\varepsilon_3})}}\left( {\theta_2^4 - \theta_3^4} \right) + {S_3} = 0$$</div>
-
-Here,
-
-*T<sub>gap</sub>* = effective mean temperature of the gap air (K)
-
-*h<sub>cv</sub>*= convective heat transfer coefficient from glass to gap air (W/m2K).
-
-The convective heat transfer coefficient is given by
-
-<div>$${h_{cv}} = 2{h_c} + 4v$$</div>
-
-where
-
-*h<sub>c</sub>*= glass-to-glass heat transfer coefficient for non-vented (closed) cavity (W/m<sup>2</sup>K)
-
-*v* = mean air velocity in the gap (m/s).
-
-The air velocity is determined by the gap cross-sectional area in the flow direction and the air flow rate, which is an input value that is constant or can vary according to a user-specified schedule:
-
-<div>$$v = \frac{F}{{{A_{gap}}}}{\rm{      (m/s)}}$$</div>
-
-where
-
-*F* = airflow rate (m<sup>3</sup>/s)
-
-*A<sub>gap</sub>* = gap cross-sectional area in direction of flow (m2)
-
-It is assumed that the airflow is uniform across the width of the window.
-
-The mean temperature of the gap air is given by the following expression, whose derivation follows that for for the case of an interior shading device:
-
-<div>$${T_{gap}} = {T_{ave}} - \frac{H}{{{H_0}}}({T_{gap,out}} - {T_{gap,in}})$$</div>
-
-where
-
-
-
-<div>$${T_{ave}} = \frac{{{\theta_2} + {\theta_3}}}{2}$$</div>
-
-*H*   = glazing height (m)
-
-<div>$${H_0} = \frac{{\rho {C_p}s}}{{2{h_{cv}}}}v$$</div>
-
-*T<sub>gap,in</sub>*<sub> </sub>=  gap air inlet temperature (*T<sub>i</sub>* if the airflow source is indoor air, *T<sub>o</sub>* if the airflow source is outside air) (K)
-
-The outlet air temperature is given by
-
-<div>$${T_{gap,out}} = {T_{ave}} - ({T_{ave}} - {T_{gap,in}}){e^{ - H/{H_0}}}$$</div>
-
-The equations for glass face \#1 and \#4 are the same as those for no airflow in the gap (Equations and ).
-
-The convective heat gain to the zone air due to the gap airflow when the airflow destination is indoor air is
-
-<div>$${q_v} = \dot m({C_{p,out}}{T_{gap,out}} - {C_{p,i}}{T_i}){\rm{      (W)}}$$</div>
-
-where
-
-*C<sub>p,i</sub>*<sub>   </sub> = heat capacity of the indoor air (J/kg-K)
-
-*C<sub>p,out</sub>*= heat capacity of the gap outlet air (J/kg-K)
-
-and where the air mass flow rate in the gap is
-
-<div>$$\dot m = \rho F{\rm{      (kg/s)}}$$</div>
-
-#### Fan Energy
-
-The fan energy used to move air through the gap is very small and is ignored.
-
-#### Airflow Window with Between-Glass Shading Device
-
-Figure 108 shows the case of a double-glazed airflow window with a between glass shading device. The heat balance equations in this case are the same as those for the between-glass shading device with natural convection (Figure 105 and following equations) except that now
-
-<div>$$v = \frac{{F/2}}{{{A_{gap}}}}{\rm{      (m/s)}}$$</div>
-
-where *A<sub>gap</sub>* = *sW* is the cross-sectional area of the gap on either side of the shading device. It is assumed that the shading device is centered between the two panes of glass so that the airflow, *F*, is divided equally between the two gaps.
-
-The convective heat gain to the zone air due to the airflow through the two gaps when the airflow destination is indoor air is
-
-<div>$${q_v} = \dot m({C_{p,ave,out}}{T_{gap,ave,out}} - {C_{p,i}}{T_i}{\rm{)      (W)}}$$</div>
-
-where the average temperature of the two outlet air streams is
-
-<div>$${T_{gap,ave,out}}{\rm{ =  }}({T_{gap,1,out}} + {T_{gap,2,out}})/2$$</div>
-
-and
-
-*C<sub>p,ave,out</sub>*<sub>  </sub> = heat capacity of the outlet air evaluated at *T<sub>gap,ave,out</sub>* (J/kg-K)
-
-
-
-![](media/image1763.png)
-
-Figure 108. Airflow window with between-glass shading device showing variables used in the heat balance equations.
-
-### Evacuated Glazing Unit (EGU)
-
-Evacuated glazing Units (EGU) are an emerging technology, developed as a concept some 20-30 years ago, but only now approaching wide-spread commercialization and adoption.
-
-#### Evacuated glazing unit (EGU): cavity thermal conductance
-
-Thermal Conductance of the space in an evacuated glazing unit (EGU) is the sum of the conductance of the low pressure gas (air) and radiation conductance.
-
-<div>$${C_{gas}} = {C_{COND}} + {C_{RAD}}$$</div>
-
-**Conductance of the low-pressure gas**
-
-Conductance of low pressure gasses is calculated using formula by Corrucini (Corruccini, R. (1959)).
-
-<div>$${C_{COND}} = \alpha  \cdot \left[ {\frac{{\gamma  + 1}}{{\gamma  - 1}}} \right] \cdot {\left[ {\frac{R}{{8 \cdot \pi  \cdot M \cdot T}}} \right]^{\frac{1}{2}}} \cdot P$$</div>
-
-<div>$$B = \alpha  \cdot \left[ {\frac{{\gamma  + 1}}{{\gamma  - 1}}} \right] \cdot {\left[ {\frac{R}{{8 \cdot \pi  \cdot M \cdot T}}} \right]^{\frac{1}{2}}}$$</div>
-
-<div>$${C_{COND}} = B \cdot P$$</div>
-
-Where:
-
-<div>$$\alpha  = \frac{{{\alpha_1}{\alpha_2}}}{{{\alpha_2} + {\alpha_1}\left( {1 - {\alpha_2}} \right)}}$$</div>
-
-a<sub>1</sub>, a<sub>2</sub> = Accommodation coefficients of the gas molecules with the two surfaces.  These values depend on the temperature, surface conditions, etc.  For the present configuration and conditions, it is expected that *a* is approximately 0.5.  If conservative value is needed than value of 1.0 could be used.  With a<sub>1</sub>, a<sub>2</sub> = 0.5, a = 0.333
-
-g     = Specific heat ratio, g<sub>air</sub> = 1.40.
-
-*R*    = Universal gas constant, *R* = 8,314.462175 J/mol·K
-
-*M*   = Molecular Weight, *M*<sub>air</sub> = 28.97 [mol/g]
-
-*T*    = (*T*<sub>1</sub> + *T*<sub>2</sub>)/2 [K]
-
-*P*    = Pressure of the gas [N/m<sup>2</sup>]
-
-From the paper Collins and Robinson (Collins, R., & Robinson, S. (1991)), B is set at approximately 50 for Air, if pressure is given in torr.  Therefore according to Collins and Robinson, for air and approximate conditions of EGU:
-
-*C*<sub>COND</sub> ≈ 50·P
-
-Where P is in torr (i.e., mm Hg).
-
-*Note: Conversion from Pa to torr is accomplished by multiplying value in torr by 133.28.*
-
-Using formula 2 and assuming *T*<sub>1</sub> to be 20 ºC and *T*<sub>2</sub> to be -18 ºC (expected temperatures of glass surfaces in EGU, if one glass surface is low-e and unit is exposed to NFRC standard environmental conditions), and using SI system of units, the B is calculated as 54.4, which is very close to the value of 50, proposed by Collins and Robinson
-
-*C*<sub>COND</sub> ≈ 54.4·P
-
-We will use exact value, calculated by the formula, so values of will be input into the calculations, which enables more flexible model that can account for special treatment of glass surfaces.
-
-#### Radiation conductance
-
-Radiation conductance for the two parallel plates is given by:
-
-<div>$${C_{RAD}} = \frac{1}{{{\varepsilon_1}^{ - 1} + {\varepsilon_2}^{ - 1} - 1}}\sigma \frac{{\left( {{T_1}^4 - {T_2}^4} \right)}}{{{T_1} - {T_2}}}$$</div>
-
-Where:
-
-e<sub>1</sub>    = emissivity of the first facing glass surface, [ - ]
-
-e<sub>2</sub>    = emissivity of the second facing glass surface, [ - ]
-
-s    = Stefan-Boltzmann Constant, 5.67 x 10<sup>-8</sup>, [W/(m<sup>2</sup>·K<sup>4</sup>)]
-
-T<sub>1</sub>   = Temperature of the first facing glass surface, [K]
-
-T<sub>2</sub>   = Temperature of the second facing glass surface. [K]
-
-Assuming glass surface temperatures of 20 ºC and -18 ºC, respectively, the following radiation conductances are obtained for the three different glass emissivities:
-
-Clear Glass (e<sub>1</sub> = e<sub>2</sub> = 0.84): C<sub>RAD</sub> = 3.4 W/m<sup>2</sup>K
-
-Hard Coat Low-e (e<sub>1</sub> or e<sub>2</sub> = 0.15): C<sub>RAD</sub> = 0.68 W/m<sup>2</sup>K
-
-Soft Coat Low-e (e<sub>1</sub> or e<sub>2</sub> = 0.04): C<sub>RAD</sub> = 0.19 W/m<sup>2</sup>K
-
-***Note:*** *C<sub>RAD</sub> of 0.09 is theoretically possible using best low-e technology today (i.e.,* *e<sub>1</sub> or* *e<sub>2</sub> = 0.02).*
-
-***Note:*** *Low-e values above are typical values, which will vary by manufacturer.  Some more recent hard coat low-e values are at or below 0.1.*
-
-It should also be noted that values above are based on the fix set of temperatures, while in reality temperatures will depend on the environmental conditions and surface emissivities (e.g., it cannot be expected that clear glass will have same *T<sub>1</sub>* and *T<sub>2</sub>* as low-e glass).
-
-Equation is precise formulation for two parallel plates at the constant temperature.  Simplified equation under these conditions is given in the form of:
-
-<div>$${C_{RAD}} = 4\sigma \frac{1}{{{\varepsilon_1}^{ - 1} + {\varepsilon_2}^{ - 1} - 1}}{T_m}^3$$</div>
-
-Where:
-
-*T<sub>m</sub>* =           mean temperature, [K]
-
-<div>$${T_m} = \frac{{\left( {{T_1} + {T_2}} \right)}}{2}$$</div>
-
-Calculation of the U-factor
-
-<div>$$U = \frac{1}{{{R_{tot}}}} = \frac{1}{{{R_o} + 2 \cdot {R_{glass}} + {R_{gap}} + {R_i}}}$$</div>
-
-<div>$${R_{gap}} = \frac{1}{{{C_{gap}}}} = \frac{1}{{{C_{COND}} + {C_{RAD}}}}$$</div>
-
-<div>$${R_{glass}} = \frac{{{t_{glass}}}}{{{k_{glass}}}}$$</div>
-
-Where:
-
-*t*<sub>glass</sub> = glass thickness; [m]
-
-*k*<sub>glass</sub> = glass conductivity; *k*<sub>glass</sub> = 1 W/(m·K)
-
-*R*<sub>glass</sub> = 0.003 m<sup>2</sup>K/W (for 3 mm glass pane)
-
-*R*<sub>o</sub> ≈ 0.033 m<sup>2</sup>K/W
-
-*R*<sub>i</sub> ≈ 0.14 m<sup>2</sup>K/W
-
-U-factor of EGU without any pillars (pretending that this is possible) would be calculated using *C*<sub>RAD</sub> only.  From above radiation conductance calculations:
-
-*Clear Glass:            U = 2.64 W/(m<sup>2</sup>·K) [0.464 Btu/(hr·ft<sup>2</sup>·ºF)]*
-
-*Hard Coat Low-e:     U = 0.62 W/(m<sup>2</sup>·K) [0.109 Btu/(hr·ft<sup>2</sup>·ºF)]*
-
-*Soft Coat Low-e:      U = 0.19 W/(m<sup>2</sup>·K) [0.034 Btu/(hr·ft<sup>2</sup>·ºF)]*
-
-Adding conductance of the air at 0.001 torr (*C*<sub>COND</sub> = 0.08 W/(m<sup>2</sup>·K), these values become:
-
-*Clear Glass:            U = 2.66 W/(m<sup>2</sup>·K) [0.468 Btu/(hr·ft<sup>2</sup>·ºF)]*
-
-*Hard Coat Low-e:     U = 0.68 W/(m<sup>2</sup>·K) [0.120 Btu/(hr·ft<sup>2</sup>·ºF)]*
-
-*Soft Coat Low-e:      U = 0.27 W/(m<sup>2</sup>·K) [0.048 Btu/(hr·ft<sup>2</sup>·ºF)]*
-
-In contrast, the U-factor of the same configuration with the air at atmospheric pressure will be (For the space width of 50 mm, C<sub>COND</sub> ≈ 450 W/m<sup>2</sup>K):
-
-*Clear Glass:            U = 5.52 W/(m<sup>2</sup>·K) [0.468 Btu/(hr·ft<sup>2</sup>·ºF)]*
-
-*Hard Coat Low-e:     U = 5.52 W/(m<sup>2</sup>·K) [0.120 Btu/(hr·ft<sup>2</sup>·ºF)]*
-
-*Soft Coat Low-e:      U = 5.52 W/(m<sup>2</sup>·K) [0.048 Btu/(hr·ft<sup>2</sup>·ºF)]*
-
-It is clear that emissivity of the glass surface makes no difference, because of the dominant conductance of the air space.  Also, it is worth noting that the U-factor of such configuration is very close to the U-factor of single glazing.
-
-#### Evacuated glazing unit (EGU): Glass support element thermal conductance
-
-Glass panes in the EGU are separated by an array of small support elements.  Typically, these support elements have a cylindrical shape and are often referred to as “pillars.�  Typical geometry of the pillar is 0.5-1.0 mm diameter and 0.05 mm (50 mm) height.  They are typically spaced 1-2 in. apart in a form of square or staggered matrix.
-
-#### Calculation of the U-factor
-
-The conductance of these elements can be measured or numerically modeled to determine accurate thermal performance.  Approximate method also exists and is based on the combination of modeling and analytical work for the conduction through small cylinders in contact with infinite parallel plates with thickness much larger than cylinder height.
-
-The following formula can be used to determine conductance of the single pillar, *C*<sub>p</sub> (Collins and Fisher-Cripps 1991):
-
-<div>$${C_p} = \frac{{2ka}}{{1 + \frac{{2h}}{{\pi a}}}}$$</div>
-
-Where:
-
-*k*    = conductivity of glass, W/(m·K)
-
-*a*    = radius of the pillar (m)
-
-*h*    = pillar height, m
-
-For the square array of support pillars (Collins and Fischer-Cripps 1991) proposes the following formula for their conductance, *C*<sub>pa</sub>:
-
-<div>$${C_{pa}} = \frac{{2ka}}{{{\lambda ^2}\left( {1 + \frac{{2h}}{{\pi a}}} \right)}}$$</div>
-
-Where:
-
-l    = pillar spacing, m
-
-This formula is approximate and does not include effect of the conductivity of the pillar, but it gives good approximation for common materials used in this technology, since conductivity of the pillar does not play substantial role for non-insulating pillars (where “non-insulating� would mean that conductivity of the pillar is equal or higher than the conductivity of the glass pane.
-
-The U-factor of the EGU with support pillars is then:
-
-<div>$$U = \frac{1}{{{R_{tot}}}} = \frac{1}{{{R_o} + 2 \cdot {R_{glass}} + {R_{gap}} + {R_i}}}$$</div>
-
-Where:
-
-<div>$${R_{gap}} = \frac{1}{{{C_{gap}}}} = \frac{1}{{{C_{COND}} + {C_{RAD}} + {C_{pa}}}}$$</div>
-
-#### References
-
-Collins, R., & Fischer-Cripps, A. 1991. "Design of Support Pillar Arrays in Flat Evacuated Windows.". Aust. J. Phys.
-
-Collins, R., & Robinson, S. 1991. *"Evacuated Glazing".* Solar Energy. Vol. 47, No. 1, pp. 27-38.
-
-Corruccini, R. 1959. "Gaseous Heat Conduction at Low Pressures and Temperatures". Vacuum. Vol. 7-8, pp.19-29.
-
-### Thermal Performance of Deflected Insulated Glazing Unit (IGU)
-
-#### Introduction
-
-Deflection of insulated glazing unit (IGU) can result in thermal performance degradation or improvement due to the reduction or increase of gap space width. Convection of the gas fill is affected by changed gap space and due to modified convection pattern and shorter or longer thermal path at the center of the glazing unit can result in increased or decreased thermal performance. For the most part, U-factor is mostly affected as a direct result of changed thermal performance; however note that solar heat gain through the window (SHGC) can also be affected because of the effect of inward flowing fraction of absorbed solar radiation, which is affected by thermal performance of the IGU.
-
-Deflection in sealed IGU is caused by the difference in gas pressure in IGU gap vs. outdoor/indoor pressure. Indoor and outdoor pressure can be considered equal, since indoor building environment is in pretty good contact with outdoor environment. We will call this pressure an atmospheric pressure, *P<sub>a</sub>*. The differences in pressure between atmospheric and gap pressure is due to several factors, listed here:
-
-1)   Difference in atmospheric pressure between IGU fabrication location and end use location
-
-2)   Difference in temperature during fabrication and actual operating conditions for the glazing. It should be noted that initial temperature can be higher than ambient temperature during fabrication process, due to elevated sealant temperatures, which can raise local temperatures within the IGU.
-
-3)   Unbalanced gas fill leakage through the sealants, resulting in lower gap pressure and inward deflection.
-
-4)   Wind or static load pressure
-
-Effects 1 and 2 will be modeled using equations presented below, while effect 3 does not have credible mathematical model. However, cumulative deflection, resulting from all three effects can be measured in the field and its effect on thermal performance can be modeled by specifying center glazing deflection.
-
-Wind or static load pressure effects on deflection is not included in this model at this time, but will be considered for future versions.
-
-Recognizing that indoor and outdoor air pressure could be different, such as in hot box test environment, future plans for the extension of the model will include option to specify different values for indoor and outdoor pressure. Another future improvement to the model will also include linking certain air gaps with indoor or outdoor environment, meaning that respective pressures in linked spaces will be set to equal.
-
-#### Mathematical Model
-
-Mathematical model described in detail here is based on the research work by Bernier and Bourret (1997) and Timoshenko and Woinowsky-Krieger (1959). Bernier and Bourret (1997) of the Ecole Polytechnique Montréal adopted Timoshenko and Woinowsky-Krieger (1959) model for calculating flat plate deflection subjected to the differential pressure field (static), while their original contribution was to develop correlations for changes in thermal performance, based on IGU deflection at the center of glazing location. In addition to adopting Bernier and Bourret (1997) model here, we have also developed model for calculating change in thermal performance of deflected units when this deflection is measured in the field. Therefore, the mathematical formulation, presented here is divided into two sections; 1) calculation of the deflection and resulting thermal performance caused by pressure and temperature effects and 2) calculation of the thermal performance of the IGU when the deflection is measured.
-
-#### Calculation of the deflection and thermal performance caused by pressure and temperature effects
-
-If coordinate system is set as shown in Figure 109 and Figure 110, it is possible to calculate deflection distribution at each point of pane by using following equation:
-
-![](media/image1779.png)
-
-Figure 109. Deflection Coordinate System - 2D
-
-<div>$${L_{D\left( i \right)}}\left( {x,y} \right) = \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{{\sin \frac{{m\pi x}}{W}\sin \frac{{n\pi y}}{H}}}{{mn{{\left( {{{\left( {\frac{m}{W}} \right)}^2} + {{\left( {\frac{n}{H}} \right)}^2}} \right)}^2}}}$$</div>
-
-Where,
-
-<div>$${D_{\left( i \right)}} = \frac{{E\cdot t_{\left( i \right)}^3}}{{12\cdot \left( {1 - {\nu ^2}} \right)}}$$</div>
-
-Where,
-
-*E* = Young’s modulus (7.2 x 10<sup>10</sup>) [Force per unit Area; SI: Pa, IP: psi]
-
-*t* = thickness of glazing pane [Length; SI: m, IP: in.]
-
-n = poison’s ratio (0.22 for glass) [Non-Dimensional]
-
-
-
-![](media/image1782.png)
-
-Figure 110. Deflection Coordinate System - 3D
-
-Δ*P<sub>i</sub>* = *P<sub>gap(i)</sub>* - *P<sub>gap(i-1)</sub>* (for i-th pane) [Force per unit Area; SI: Pa, IP: psi]
-
-Δ*P<sub>i</sub>* = *P<sub>gap(1)</sub>* - *P<sub>a</sub>* (first pane) [Force per unit Area; SI: Pa, IP: psi]*                  *
-
-Δ*P<sub>i</sub>* = *P<sub>a</sub> - P<sub>gap(n-1)</sub>* (last pane) [Force per unit Area; SI: Pa, IP: psi]
-
-Where,
-
-*P<sub>a</sub> =* atmospheric pressure. [Force per unit Area; SI: Pa, IP: psi]
-
-<div>$${P_{gap\left( i \right)}} = \frac{{{P_{ini}}{V_{ini\left( i \right)}}{T_{gap\left( i \right)}}}}{{{T_{ini}}{V_{gap\left( i \right)}}}}$$</div>
-
-Where,
-
-*P<sub>ini</sub>* = Initial pressure. Applies to all gaps as a single value (input data - measured or otherwise) [Force per unit Area; SI: Pa, IP: psi]
-
-*T<sub>ini</sub>* = Initial temperature. Applies to all gaps as a single value (input data - measured or otherwise) [Degree Temperature; SI: K, IP: R]
-
-*V<sub>ini(i)</sub>* = Initial volume for i-th gap. [Length\*Length\*Length; SI: m<sup>3</sup>, IP: in<sup>3</sup>]
-
-<div>$${V_{ini\left( i \right)}} = {L_i}\cdot W\cdot H$$</div>
-
-Where,
-
-*L<sub>i</sub>* = non-deflected glazing gap width (for i-th gap) [Length; SI: m, IP: in.]
-
-*W* = IGU width [Length; SI: m, IP: in.]
-
-*H* = IGU height [Length; SI: m, IP: in.]
-
-*T<sub>gap(i)</sub>* = temperature of the gap between two glass panes (calculated using center of glazing thermal calculation algorithm, as described in ISO 15099 (ISO 2003). This value is first calculated using non-deflected state and is recalculated after the resulting deflection is calculated. This process is repeated until temperature at next iteration does not differ by more than 0.1 ºC
-
-*V<sub>gap(i)</sub>* = volume of the IGU gap in deflected state [Lentgh\*Length\*Length; SI: m<sup>3</sup>, IP: in<sup>3</sup>]
-
-<div>$${V_{gap\left( i \right)}} = {V_{ini\left( i \right)}} + W\cdot H\cdot \left( {\overline {{L_{D,i}}}  - \overline {{L_{D,i + 1}}} } \right)$$</div>
-
-Where,
-
-<span>\(\overline {{L_{D,i}}} \)</span> is mean deflection value for i-th pane. [Length; SI: m, IP: in.]
-
-Deflection of each pane can be positive or negative and is done solely to establish reference. Current frame of reference is that positive deflection means that pane is deflecting towards left side, while negative deflection means that pane is deflecting towards right side . Whether the deflection is in the direction of reducing the gap width or increasing it, it will be the result of pressure difference, as described in . When pressure in the glazing unit is higher than surrounding environmental pressure, the deflection will be towards increasing gap width (i.e., ballooning), while the opposite situation will result in decreasing gap width (i.e., vacuuming)
-
-![](media/image1787.png)
-
-Figure 111. Deflection Direction Convention
-
-The important part of calculating deflection of the IGU is to determine mean deflection value for each glazing pane. Mean deflection value is used to calculate gap volume in deflected state . Mean deflection of glazing pane can be calculated by integrating :
-
-<div>$$\overline {{L_{D\left( i \right)}}}  = \mathop \smallint \limits_{x = 0}^W \mathop \smallint \limits_{y = 0}^H \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{{\sin \frac{{m\pi x}}{W}\sin \frac{{n\pi y}}{H}}}{{mn{{\left( {{{\left( {\frac{m}{W}} \right)}^2} + {{\left( {\frac{n}{H}} \right)}^2}} \right)}^2}}}$$</div>
-
-Which is identical with the following expression:
-
-<div>$$\overline {{L_{D\left( i \right)}}}  = \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{{\mathop \smallint \nolimits_{x = 0}^W \mathop \smallint \nolimits_{y = 0}^H \sin \frac{{m\pi x}}{W}\sin \frac{{n\pi y}}{H}}}{{mn{{\left( {{{\left( {\frac{m}{W}} \right)}^2} + {{\left( {\frac{n}{H}} \right)}^2}} \right)}^2}}}$$</div>
-
-and because integral of sin(x) is equal with –cos(x), above equation will become:
-
-<div>$$\overline {{L_{D\left( i \right)}}}  = \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{{\left( {1 - cos\left( {m\pi } \right)} \right)\left( {1 - cos\left( {n\pi } \right)} \right)}}{{mn{{\left( {{{\left( {\frac{m}{W}} \right)}^2} + {{\left( {\frac{n}{H}} \right)}^2}} \right)}^2}}}$$</div>
-
-Finally, because <span>\(cos\left( {m\pi } \right)\)</span> and <span>\(cos\left( {n\pi } \right)\)</span> values are always equal to -1 for the given range of m and n, above equation will became:
-
-<div>$$\overline {{L_{D\left( i \right)}}}  = \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{4}{{{m^2}{n^2}{\pi ^2}{{\left( {{{\left( {\frac{m}{W}} \right)}^2} + {{\left( {\frac{n}{H}} \right)}^2}} \right)}^2}}}$$</div>
-
-After calculating mean pane deflection the following equation is used to calculate mean gap width:
-
-<div>$${L_{r\left( i \right)}} = L + \left( {\overline {{L_{D,\left( i \right)}}}  - \overline {{L_{D,\left( {i + 1} \right)}}} } \right)$$</div>
-
-*Where,*
-
-*L<sub>r(i)</sub> = Mean gap “i� width after incorporating glazing deflection. This mean gap width is used to recalculate thermal performance of deflected IGU.*
-
-<span>\(\overline {{L_{D,i}}} \)</span>*** ****= mean glazing deflection for each pane “i�.*
-
-Calculation of the deflection at the center of glazing and mean glazing deflection for each pane is an iterative process, where the initial temperature distribution is calculated for non-deflected state, then deflection is calculated based on this temperature distribution, new temperature distribution is calculated for this deflected state, then temperatures from previous iteration are compared to the current iteration and the process is repeated until the difference is no larger than 0.1 ºC.
-
-At the end of calculations, program will calculate and return maximum deflection value for each pane (i.e., center of glazing deflection). If we label maximum deflection of each pane as *L<sub>D(i),max</sub>*, we can calculate this value by substituting *x*=*W*/2 and *y*=*H*/2 in equation to determine deflection at the center point. Therefore,
-
-<div>$${L_{D\left( i \right),max}} = \frac{{16\cdot \Delta {P_{\left( i \right)}}}}{{{\pi ^6}\cdot {D_{\left( i \right)}}}}\mathop \sum \limits_{m = 1,3,5 \ldots }^\infty  \mathop \sum \limits_{n = 1,3,5 \ldots }^\infty  \frac{{\sin \frac{{m\pi }}{2}\sin \frac{{n\pi }}{2}}}{{mn{{\left( {{{\left( {\frac{m}{2}} \right)}^2} + {{\left( {\frac{n}{2}} \right)}^2}} \right)}^2}}}$$</div>
-
-For glazing systems with more than two glazing layers, meaning multiple gas filled gaps, the deflection will be calculated for each glazing pane assuming that the pressure in a gap is independent from each other and calculated separately, unless spaces are “linked� together (e.g., stretched film middle glazing that has hole for equalizing pressure).
-
-#### Non-Linked Gaps in 3 or more glazing layer system:
-
-The procedure shown above generally applies to the 3 or more layer glazing system, with the exception that neighboring pressures are no longer *P<sub>a</sub>*, but rather could be *P<sub>a</sub>* on one side and *P<sub>gap</sub>* on the other, or have *P<sub>gap</sub>* on both sides, as shown in Figure 111 for gap “*i*�. Center of glazing thermal calculation will determine new temperature distribution, after deflection is calculated for each glazing and will be used to determine new *P<sub>gap</sub>*, as per the procedure above.
-
-#### Linked Gaps in 3 or more glazing layer system:
-
-When one or more gaps are linked together, their pressure is assumed to be identical (e.g., in triple glazing IGU *P<sub>gap,1</sub>* = *P<sub>gap,2</sub>*.)  This pressure is calculated from temperatures of bounding glazing for linked gaps (e.g., for triple glazing IGU, glazing 1 and 3) and using neighboring pressures outside of those bounding glazing (e.g., for triple glazed IGU, *P<sub>a</sub>* on both sides).
-
-*Note: This feature is not implemented in WINDOW 7.1. It is considered for future enhancements to the program.*
-
-#### Gap(s) Linked to Indoor or Outdoor Environment:
-
-If one or more glazing gaps are linked to either indoor or outdoor environment its pressure is fixed to *P<sub>a</sub>*. In combination situations, such as two or more gaps linked together with one of them being linked to indoor or outdoor environment, they will all have fixed pressure of *P<sub>a</sub>*.
-
-#### Calculation of the thermal performance caused by measured deflection
-
-When deflection is measured, it is normally measured at the point of maximum deflection. Maximum deflection occurs at center of the IGU (at *W*/2 and *H*/2).
-
-Measured value is typically gap width at the point of maximum deflection, which we can label *L<sub>G(i)</sub>*. For i-th measured gap the width is equal to:
-
-<div>$${L_{G\left( i \right)}} = {L_{\left( i \right)}} + \left( {{L_{D\left( i \right),max}} - {L_{D\left( {i + 1} \right),max}}} \right)$$</div>
-
-![](media/image1798.png)
-
-Figure 112. Sketch of the non-symetrically Deflected Glazing Panes
-
-If we label ratio of mean deflection and maximum deflection as R<sub>(i)</sub>, then:
-
-<div>$${R_{(i)}} = \frac{{\overline {{L_{D(i)}}} }}{{{L_{D(i)}}_{,\max }}} = \sum\limits_{m = 1,3,5,...}^\infty  {\sum\limits_{n = 1,3,5,...}^\infty  {\frac{4}{{{m^2}{n^2}{\pi ^2}{{\left( {{{(\frac{m}{W})}^2} + {{(\frac{n}{H})}^2}} \right)}^2}}}} } $$</div>
-
-<span>\(\)</span>Important thing to note is that ratios (<span>\({R_{\left( i \right)}}\)</span>) for all gaps in glazing system are equal.
-
-<div>$${R_{\left( 1 \right)}} = {R_{\left( 2 \right)}} =  \ldots  = {R_{\left( i \right)}} =  \ldots  = {R_{\left( {n - 1} \right)}} = R$$</div>
-
-Replacing and into the following equation is obtained:
-
-<div>$${L_{r\left( i \right)}} = {L_{\left( i \right)}} + R\left( {{L_{D\left( i \right),max}} - {L_{D\left( {i + 1} \right),max}}} \right)$$</div>
-
-Combining with we get the following expression for the mean gap width:
-
-<div>$${L_{r\left( i \right)}} = {L_{\left( i \right)}} + R\left( {{L_{G\left( i \right)}} - {L_{\left( i \right)}}} \right)$$</div>
-
-Number of equations given in expression is equal to n-1, where n is number of panes. Therefore, we need one more equation to complete the system of equations that would allow us to solve for all independent variables. To get the last equation we can rewrite in slightly different manner:
-
-<div>$${L_{D\left( i \right),max}} = \frac{{\Delta {P_{\left( i \right)}}}}{{{D_{\left( i \right)}}}}\cdot K$$</div>
-
-Where coefficient K combines all constant terms, while <span>\({D_{\left( i \right)}}\)</span> is given by and <span>\(\Delta {P_{\left( i \right)}}\)</span> is calculated by, and . Summing over all deflections, <span>\({L_{D\left( i \right),max}}\)</span> the following equation is obtained:
-
-<div>$$\mathop \sum \limits_{i = 1}^n \frac{{{D_{\left( i \right)}}}}{K}\cdot {L_{D\left( i \right),max}} = \mathop \sum \limits_{i = 1}^n \Delta {P_{\left( i \right)}} = 0$$</div>
-
-Note that sum of all <span>\(\Delta {P_{\left( i \right)}}\)</span> is equal to zero since outside pressure is equal to inside. Therefore, the remaining equation that completes the set of equations is:
-
-<div>$$\mathop \sum \limits_{i = 1}^n {D_{\left( i \right)}}\cdot {L_{D\left( i \right),max}} = 0$$</div>
-
-#### Solving system of equations
-
-In order to solve system of equations we will present in slightly different manner:
-
-<div>$$0 = {L_{\left( i \right)}} - {L_{G\left( i \right)}} + {L_{D\left( i \right),max}} - {L_{D\left( {i + 1} \right),max}}$$</div>
-
-Which in developed form will look like this:
-
-<div>$$0 = {L_{\left( 1 \right)}} - {L_{G\left( 1 \right)}} + {L_{D\left( 1 \right),max}} - {L_{D\left( 2 \right),max}}$$</div>
-
-<div>$$0 = {L_{\left( 2 \right)}} - {L_{G\left( 2 \right)}} + {L_{D\left( 2 \right),max}} - {L_{D\left( 3 \right),max}}$$</div>
-
-<div>$$0 = {L_{\left( i \right)}} - {L_{G\left( i \right)}} + {L_{D\left( i \right),max}} - {L_{D\left( {i + 1} \right),max}}$$</div>
-
-<div>$$0 = {L_{\left( {n - 1} \right)}} - {L_{G\left( {n - 1} \right)}} + {L_{D\left( {n - 1} \right),max}} - {L_{D\left( n \right),max}}$$</div>
-
-In order to express each <span>\({L_{D\left( i \right),max}}\)</span> as dependence from <span>\({L_{D\left( n \right),max}}\)</span> (deflection of inside/last pane) we will need to make sum from first to last, then from second to last, third to last and so on. This procedure will create following set of equations:
-
-<div>$${L_{D\left( 1 \right),max}} = \mathop \sum \limits_{k = 1}^{k = n - 1} \left( {{L_{G\left( k \right)}} - {L_{\left( k \right)}}} \right) + {L_{D\left( n \right),max}}$$</div>
-
-<div>$${L_{D\left( 2 \right),max}} = \mathop \sum \limits_{k = 2}^{k = n - 1} \left( {{L_{G\left( k \right)}} - {L_{\left( k \right)}}} \right) + {L_{D\left( n \right),max}}$$</div>
-
-<div>$${L_{D\left( i \right),max}} = \mathop \sum \limits_{k = i}^{k = n - 1} \left( {{L_{G\left( k \right)}} - {L_{\left( k \right)}}} \right) + {L_{D\left( n \right),max}}$$</div>
-
-<div>$${L_{D\left( {n - 1} \right),max}} = \mathop \sum \limits_{k = n - 1}^{k = n - 1} \left( {{L_{G\left( k \right)}} - {L_{\left( k \right)}}} \right) + {L_{D\left( n \right),max}}$$</div>
-
-Now replacing this set of equations back to :
-
-<div>$$\mathop \sum \limits_{i = 1}^{n - 1} {D_{\left( i \right)}}\cdot \left( {\mathop \sum \limits_{k = i}^{k = n - 1} \left( {{L_{G\left( k \right)}} - {L_{\left( k \right)}}} \right) + {L_{D\left( n \right),max}}} \right) + {D_{\left( n \right)}}\cdot {L_{D\left( n \right),max}} = 0$$</div>
-
-Which solving by <span>\({L_{D\left( n \right),max}}\)</span> leads to the following equation:
-
-<div>$${L_{D\left( n \right),max}} = \frac{{\mathop \sum \nolimits_{i = 1}^{n - 1} ({D_{\left( i \right)}}\cdot \mathop \sum \nolimits_{k = i}^{k = n - 1} \left( {{L_{\left( k \right)}} - {L_{G\left( k \right)}}} \right))}}{{\mathop \sum \nolimits_{i = 1}^n {D_{\left( i \right)}}}}$$</div>
-
-Calculating <span>\({L_{D\left( n \right),max}}\)</span> value from this equation and substituting it in will enable calculation of the deflection of remaining panes.
-
-#### References
-
-Arasteh, D.K., J.C. Kohler and B.T. Griffith. Draft 2009. Modeling Windows in EnergyPlus with only U, SHGC, and optionally VT. LBNL report.  Full reference to be determined.
-
-Arasteh, D. J. 2009. Modeling Windows in EnergyPlus with only U, SHGC, and optionally VT. Lawrence Berkeley National Laboratory.
-
-Arasteh, D.K., M.S. Reilly and M.D. Rubin. 1989. A versatile procedure for calculating heat transfer through windows. American Society of Heating, Refrigeration and Air-Conditioning Engineers, ASHRAE Transactions, Vol. 95, Pt. 2.
-
-Bernier, M., & Bourret, B. January 1997. "Effects of Glass Plate Curvature on the U-Factor of Sealed Insulated Glazing Units". Atlanta, GA: ASHRAE Transactions. Vol. 103, Pt. 1. American Society for Heating, Refrigerating and Air-Conditioning Engineers.
-
-Collins, R., & Fischer-Cripps, A. 1991. "Design of Support Pillar Arrays in Flat Evacuated Windows.". Aust. J. Phys.
-
-Collins, R., & Robinson, S. 1991. "Evacuated Glazing". Solar Energy. Vol. 47, No. 1, pp. 27-38.
-
-Corruccini, R. (1959). "Gaseous Heat Conduction at Low Pressures and Temperatures". Vacuum. Vol. 7-8, pp.19-29.
-
-Finlayson, E.U., D.K. Arasteh, C. Huizenga, M.D. Rubin and M.S. Reilly. 1993. WINDOW 4.0: documentation of calculation procedures. Lawrence Berkeley National Laboratory report no. LBL-33943.
-
-ISO. 2003. ISO 15099:2003. Thermal performance of windows, doors, and shading devices – Detailed calculations. International Organization for Standardization.
-
-Klems, J. H. 1994A. "A New Method for Predicting the Solar Heat Gain of Complex Fenestration Systems: I. Overview and Derivation of the Matrix Layer Calculation.". ASHRAE Transactions. 100 (pt.1): 1073-1086.
-
-Klems, J. H. 1994B. "A New Method for Predicting the Solar Heat Gain of Complex Fenestration Systems: II. Detailed Description of the Matrix Layer Calculation.". ASHRAE Transactions. 100 (pt.1): 1073-1086.
-
-Klems, J. H. 1995. "Measurements of Bidirectional Optical Properties of Complex Shading Devices.". ASHRAE Transactions. 101 (pt 1; Symposium Paper CH-95-8-1 (RP-548)): 791-801.
-
-Klems, J. H. 1996. "A Comparison between Calculated and Measured SHGC for Complex Glazing Systems.". ASHRAE Transactions. 102 (Pt. 1; Symposium Paper AT-96-16-1): 931-939.
-
-Klems, J. H. 1996. "Calorimetric Measurements of Inward-Flowing Fraction for Complex Glazing and Shading Systems.". ASHRAE Trans. 102(Pt. 1; Symposium Paper AT-96-16-3): 947-954.
-
-Munson, B.R, D.F. Young and T.H. Okiishi. 1998. “Fundamentals of Fluid Mechanics,� Third Edition Update, John Wiley & Sons, Inc.
-
-Papamichael, K. J. 1998. "Determination and Application of Bidirectional Solar-Optical Properties of Fenestration Systems.". Cambridge, MA: 13th National Passive Solar Conference.
-
-Simmler, H., U. Fischer and F. Winkelmann. 1996. Solar-Thermal Window Blind Model for DOE-2. Lawrence Berkeley National Laboratory, Simulation Research Group internal report, (unpublished).
-
-Timoshenko, S., & Kreiger-Woinowsky, S. 1959. "Theory of Plates and Shells" 2nd Edition. McGraw-Hill Company.
-
-### Equivalent Layer Fenestration Model
-
-The section describes the equivalent layer fenestration optical and thermal model. The Equivalent Layer fenestration model can have four types of attachments: drapes, venetian blinds, roller blinds and insect screens. In this model shading layers are assumed to be uniform and can be represented by an equivalent homogenous layer that has spatially-averaged "effective" optical and thermal properties (ASHRAE 1311-RP). Likewise, venetian blinds can be characterized using effective optical and thermal properties. When solar radiation strikes a window surface some fraction of the incident solar radiation passes unobstructed through openings in a shading layer and the remaining fraction is intercepted by the structure of the layer. The intercepted radiation is partly absorbed, partly reflected and partly transmitted. These reflected and transmitted components of the scattered solar radiation are assumed to be uniformly diffuse. Shading layers, because of their openness, generally transmit longwave radiation, and the effective infrared properties of shades account for that. Using effective optical properties and a beam/diffuse split of solar radiation at each layer, the equivalent layer approach can represent multi-layer systems. This representation provides virtually unlimited flexibility to combine different types of shading layers in a fenestration. The equivalent layer window model requires a few set of optical data to characterize a particular layer and this set of data is used to calculate effective layer properties. For instance, the effective solar optical properties of a venetian blind can be calculated as a function of slats optical properties and geometry. Also, it is possible to adjust slat angle at each time step in response to the changing angular position of the sun. Moreover, the model provides control strategies as a function of slat angle that can be changed at each time step as needed. Likewise, effective properties of a pleated drape are calculated as a function of fabric properties and a specified value of fullness. The only input data needed to fully characterize drapery fabrics, roller blinds and insect screens are material openness as area fraction, and the transmittance and reflectance at normal incidence. Shade openness area fraction is the same as the beam-beam transmittance at normal incidence. In multilayer fenestration, each layer is separated by a gap. A gap in equivalent layer model is defined by specifying the fill gas and the gap spacing. Currently five gas types are allowed: Air, Argon, Xenon, Krypton and Custom. The convective heat transfer coefficient in a gap is calculated depending on the spacing, the temperatures of the layers and the fill gas properties. Equivalent-layer concept – offers wide range of multiple glazing and shading layers combination and can simulate multi-layer complex fenestration systems. The effective layer properties of venetian blinds, pleated drapes, roller blinds, and insect screens are calculated from geometric layer models and material properties. A set of empirical correlations for estimating off-normal material properties were developed under ASHRAE research project (ASHRAE 1311-RP).
-
-#### The Equivalent Layer Analysis
-
-The equivalent layer windows system is treated as a series of parallel layers separated by gaps as shown in Figure 113. This multi-layer structure has been used in several computer programs and the underlying theory has been documented (ASHRAE 1311-RP).
-
-![](media/image1827.svg.png)
-
-Figure 113. Multi-layer fenestration analysis structure (ASHRAE 1311-RP)
-
-Equivalent layer fenestration model uses two-step analysis. First, the flux of absorbed solar radiation at each layer, S<sub>i</sub>, caused by the incident radiation flux, I<sub>sol</sub>, is determined using net radiation analysis. Second, an energy balance is applied at each layer, accounting for heat transfer and the known set of absorbed solar radiations S<sub>i</sub> values, in order to solve for the set of layer temperatures, T<sub>i</sub>, and the corresponding heat fluxes. The fenestration model also accounts for the diathermanous shade layers in the longwave radiant exchange. The latter can be significant for shading layers. Glass is considered opaque with respect to longwave radiation.
-
-#### Equivalent Layer Optical Model
-
-The multilayer optical model is based on an algorithm originally developed by Edwards (1977) and extended by Wright and Kotey (2006). The algorithm models the interaction of incident solar radiation with a glazing system composed of any number of parallel, planar, specular glazing layers. The shading layers scatter portion of the incident solar radiation diffusely, and the model tracks the beam and diffuse components of solar radiation as they interact with a multi-layer system of glazing and shading layers. The conceptual arrangement for tracking beam and diffuse solar flux components is illustrated in Figure 114.
-
-![](media/image1828.svg.png)
-
-Analysis yields beam-beam, beam-diffuse and diffuse-diffuse fluxes, providing full detail concerning the quantities of reflected, transmitted and absorbed radiation.
-
-![](media/image1829.svg.png)
-
-Figure 114. Solar analysis of the multi-layer glazing/shading system showing beam and diffuse fluxes (ASHRAE 1311-RP)
-
-The beam and diffuse characterization of solar radiation demands an expanded set of solar optical properties (Wright and Kotey 2006). The quantities of interest for single layer are shown inFigure 115.
-
-Where,
-
-*t*     =          transmittance of a glazing or a shading layer, (-)
-
-*r*    =          reflectance of a glazing or a shading layer, (-)
-
-*e*     =          thermal emissivity of a glazing or a shading layer, (-)
-
-*q*    =          incident angle, (degree)
-
-*f*    =          slat angle, (degree)
-
-*W*    =          profile angle, (degree)
-
-*J*    =          radiosity of a layer surface, (W/m2)
-
-*T*    =          temperature of a layer, (C)
-
-Subscripts
-
-*f*     =          front side of a layer
-
-*b*    =          back side of a layer
-
-*bb*   =          beam-beam optical property. Represents a fraction of the beam radiation incident at a given layer and leaves the layer without being scattered.
-
-*bd*   =          beam-diffuse optical property. Represents a fraction of the beam radiation incident at a given layer and leaves the layer diffusely
-
-*dd*   =          diffuse-diffuse optical property. Represents a diffuse radiation incident at a given layer and leaves the layer as diffuse
-
-*i     =         * layer index, (-)
-
-Superscripts
-
-*m*   =          represents material property (e.g., fabric material)
-
-*str*  =          represents an apparent material structure property of roller blinds
-
-*w*    =          represents an apparent wire property
-
-![](media/image1830.svg.png)
-
-Figure 115. Twelve solar properties assigned at each layer (ASHRAE 1311-RP)
-
-Each glazing or shading layer, in general, require eleven set of solar properties (Wright and Kotey 2006). Only beam-beam properties are needed for common glazing layers. Each shading layer is represented by a few set of component properties and geometries that are converted to the full set of layer optical and thermal properties by equivalent layer models (ASHRAE 1311-RP). The models also make account for off-normal incidence of solar radiation and can calculate the diffuse component from normal incidence values using numerical integration.
-
-#### Equivalent Layer Thermal Model
-
-A surface energy balance is applied at each layer and the resulting set of equation is solved for layer temperatures and heat transfer fluxes. A schematic drawing of the multi-layer illustration and variables designation is shown in Figure 116. The net radiation formulation based on the radiosities, Jf,i and Jb,i the radiant flux leaving the front and back surfaces of the i<sup>th</sup> layer, respectively, is the used as a solution technique. The net radiant heat flux across a gap can be expressed as the difference between the radiosities of the bounding surfaces. The net radiation model analysis yields the layer temperatures and corresponding heat transfer coefficients that are used to determine U-factor and SHGC. The thermal analysis is done in “ASHWAT\_Thermal� routine.
-
-![](media/image1831.svg.png)
-
-Figure 116. Radiosity model used in thermal analysis of the multi-layer glazing/shading system (ASHRAE 1311-RP)
-
-#### Glazing Layer Analysis
-
-The Equivalent-Layer window model allows a wide range of options regarding the selection of glazing layers and gaps combinations. It also allows mixing glazing and shading layers in any sequence. For instance, it allows placing a venetian blind or a roller blind in between glazing layers. Only beam-beam solar properties at normal incidence, infrared transmittance and infrared emissivity are required for common glazing types. Off-normal solar properties at a given sun position are estimated by adjusting the normal incidence values in “ASHWAT\_OffNormalProperties� routine. The model assumes that the ratio between normal and off-normal transmittance is the same for the glazing layer in question and a reference piece of uncoated 6 mm glass with a moderate tint (ASHRAE 1311-RP). A similar procedure is used to convert solar reflectance from normal to off-normal.
-
-#### Gap Layer Analysis
-
-Gaps can be specified as sealed, vented indoors or vented outdoors. The sealed gap is considered as enclosed cavity. Vented gaps is specified for inner and outer most gaps only and when the gas type is AIR. The vented gap model assumes that air flow at the perimeter of the window is not restricted. Any fill gas can be specified by molecular mass and thermo-physical properties of viscosity, specific heat and thermal conductivity. This is done by providing "a", “b� and "c" coefficients of the quadratic equation of the form, p = a + bT + cT<sup>2</sup>, where the T (K) is temperature and p is the property being evaluated. EnergyPlus has builtin-data available for common fill gas components including Air, Argon, Krypton and Xenon. Users specify CUSTOM gas by defining the coefficients as an input.
-
-#### Shade Layer Analysis
-
-Equivalent layer fenestration model has a complete set of solar and longwave models for the four shading layer types: drapes, venetian blinds, roller blinds and insect screens developed under ASHRAE 1311-RP. And semi-empirical models are used to evaluate the off-normal properties of drape, roller blind and insect screen materials. The effective layer properties of venetian blinds and the effect of pleating in drapes are determined using a more fundamental net radiation scheme. The openness fraction, A<sub>o</sub> and beam-beam solar transmittance at normal incidence, *t*<sub>bb</sub> (q=0) really represent a geometric quantity and it has been confirmed that they can be used interchangeably (ASHRAE 1311-RP). Openness is simply the fraction of a material, by area, that is open. In equivalent layer fenestration model, beam-beam transmittance at normal incidence (i.e., openness fraction), beam-diffuse transmittance and reflectance at normal incidence are required to characterize drapery fabric, roller blind and insect screen material. A conventional venetian blind in equivalent layer model can be characterized by specifying the geometry, solar reflectance and transmittance, and emissivity of the slats. The off-normal solar properties of drape, roller blind and insect screen materials were formulated based on measurements (ASHRAE 1311-RP). The longwave properties of the of the drape fabrics, roller blinds and insect screens can be calculated from the material emissivity and openness of the fabric (ASHRE 1311-RP). The optical model development for venetian blinds is presented by Yahoda and Wright (2004 and 2005), and Kotey et al. (2008).
-
-#### Drapes and Curtains
-
-The off-normal optical properties of drapery fabric is determined from user specified optical properties at normal incidence (q=0) using empirical correlations (Kotey et al., 2009a). The input data required to characterize drapery fabric are the beam-beam transmittance of the material at normal incidence *t*<sub>bb</sub> (q=0) = Ao, the beam-diffuse transmittance of the material at normal incidence*t*<sub>bd</sub> (q=0), and the beam-diffuse (total) reflectance of the materialr<sub>bt</sub> (q=0). The off-normal properties are calculated as follows.
-
-Off-normal Transmittance:
-
-<div>$${\rm{\tau }}_{{\rm{bb}}}^{\rm{m}}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bb}}}^{\rm{m}}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}\left( {\rm{\theta }} \right)$$</div>
-
-<div>$${\rm{\tau }}_{{\rm{bt}}}^{\rm{m}}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bt}}}^{\rm{m}}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}\left( {\rm{\theta }} \right)$$</div>
-
-<div>$${\rm{b}} = {\left[ {\; - 0.5 \cdot \ln \;\left( {\;{{\left[ {{\rm{\tau }}_{{\rm{bb}}}^{\rm{m}}{\rm{(\theta }} = {\rm{0)}}\;{\rm{,}}\;\;{\rm{0}}{\rm{.01}}} \right]}^{\;\max }}\;} \right)\;\;,\;\;0.35\;} \right]^{\;\max }}$$</div>
-
-<div>$${\rm{b}} = {\left[ {\; - 0.5 \cdot \ln \;\left( {\;{{\left[ {{\rm{\tau }}_{{\rm{bt}}}^{\rm{m}}{\rm{(\theta }} = {\rm{0)}}\;{\rm{,}}\;\;{\rm{0}}{\rm{.01}}} \right]}^{\;\max }}\;} \right)\;\;,\;\;0.35\;} \right]^{\;\max }}$$</div>
-
-<div>$${\rm{\tau }}_{{\rm{bt}}}^{\rm{m}}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bd}}}^{\rm{m}}\left( {\rm{\theta }} \right) + {\rm{\tau }}_{{\rm{bb}}}^{\rm{m}}\left( {\rm{\theta }} \right)$$</div>
-
-The off-normal reflectance:
-
-<div>$${\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {\rm{\theta }} \right) = {\rm{\rho }}_{{\rm{bd}}}^{\rm{m}}\left( {\rm{\theta }} \right) = {\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right) + \left( {{\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = 9{\rm{0}}^\circ } \right) - {\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right)} \right) \cdot \left( {1 - {\rm{co}}{{\rm{s}}^{{\rm{0}}{\rm{.6}}}}\left( {\rm{\theta }} \right)} \right)$$</div>
-
-<div>$${\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{90}}^\circ } \right) = {\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right) + \left( {{\rm{1}} - {\rm{\rho }}_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right)} \right)\;\left( {\,0.7{{\left( {\;{\rm{\rho }}_{}^{\rm{y}}} \right)}^{\;0.7}}} \right)$$</div>
-
-The apparent yarn reflectance is given by:
-
-<div>$${\rho ^y} = \frac{{\rho_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}{{{\rm{1}} - \tau_{{\rm{bb}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right)}} = \frac{{\rho_{{\rm{bt}}}^{\rm{m}}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}{{{\rm{1}} - {{\rm{A}}_{\rm{o}}}}}$$</div>
-
-The above set of equations for drapery fabrics are used subject to the condition that the solar absorptance of the fabric, at normal incidence, is not less than 1% (ASHRE 1311-RP). The diffuse-diffuse material properties, for Equivalent layer window model, are determined using Rhomberg integration with 32 panels covering the range from q=0 to q=90° (ASHRAE 1311-RP). The subscript “X� stands for either front or back side of the layer.
-
-<div>$$\tau_{{\rm{x,dd}}}^{\rm{m}} = \;\;{\rm{2}}\;\int\limits_{{\rm{\theta }} = {\rm{0}}}^{{\raise0.5ex\hbox{$\scriptstyle {\rm{\pi }}$}\kern-0.1em/\kern-0.15em\lower0.25ex\hbox{$\scriptstyle {\rm{2}}$}}} {\tau_{{\rm{x,bt}}}^{\rm{m}}\left( {\rm{\theta }} \right) \cdot {\rm{cos}}\left( {\rm{\theta }} \right) \cdot {\rm{sin}}\left( {\rm{\theta }} \right)} \;{\rm{d\theta }}$$</div>
-
-<div>$$\rho_{{\rm{x,dd}}}^{\rm{m}} = \;\;{\rm{2}}\;\int\limits_{{\rm{\theta }} = {\rm{0}}}^{{\raise0.5ex\hbox{$\scriptstyle {\rm{\pi }}$}\kern-0.1em/\kern-0.15em\lower0.25ex\hbox{$\scriptstyle {\rm{2}}$}}} {\rho_{{\rm{x,bt}}}^{\rm{m}}\left( {\rm{\theta }} \right) \cdot {\rm{cos}}\left( {\rm{\theta }} \right) \cdot {\rm{sin}}\left( {\rm{\theta }} \right)} \;{\rm{d\theta }}$$</div>
-
-The above set of equations for drapery fabrics apply to the full range of A<sub>o</sub>, fabric transmittance and fabric reflectance including that falls within the bounds of Keyes' (1967) fabric chart plus sheer fabrics (ASHRAE 1311-RP). The longwave thermal emissivity and thermal transmittances of drapery fabric are calculated using the following correlations and fabric openness fraction (Kotey et al. 2008).
-
-<div>$${\varepsilon ^{\rm{m}}} = {\rm{0}}{\rm{.87}} \cdot \left( {{\rm{1 - }}{{\rm{A}}_{\rm{o}}}} \right)$$</div>
-
-<div>$${\tau ^{\rm{m}}} = {\rm{1}} - {\rm{0}}{\rm{.95}} \cdot \left( {{\rm{1}} - {{\rm{A}}_{\rm{o}}}} \right)$$</div>
-
-The optical and thermal properties determined using the above same sets of equations are equally valid for pleated drape shades (Kotey, et. al., 2009a). For pleated drape, the effective beam-beam and beam-diffuse solar properties are determined by tracking both radiation components, for a given incident angle, and interaction with a fabric pleated rectangular geometry shown in Figure 117. The solar optical properties of the two different pleat planes are evaluated on the basis of the local solar incidence angle. Therefore, the effective layer properties are influenced not just by horizontal solar profile angle, W<sub>H</sub>, but also by incidence angle (ASHRAE 1311-RP).
-
-![](media/image1844.svg.png)
-
-Figure 117. Geometry used for Pleated Drape Analysis
-
-The solar diffuse-diffuse and long-wave effective properties of the pleated drape are evaluated using a much simpler net-radiation analysis using conventional shape factors (Kotey, et. al., 2009a). Users can chose and apply the pleated drape model to any fabric and any degree of fullness (ASHRAE 1311-RP).
-
-#### Venetian Blinds
-
-The effective shortwave optical and longwave optical properties of venetian blind layer is estimated using analytical models (Yahoda and Wright 2004, 2005; Kotey et al. 2008). The model requires properties of venetian blind slats and geometry of the slats shown in Figure 1118.
-
-![](media/image1845.svg.png)
-
-Figure 1118. Likewise, the effective longwave properties are obtained for the layer knowing longwave properties of the slats.
-
-![](media/image1846.svg.png)
-
-Figure 118. Geometry and properties used for venetian blind analysis
-
-The model assumes that venetian blind slats reflect and transmit solar radiation diffusely (ASHRAE 1311-RP). The same assumption is made regarding thermal radiation. The input data required to characterize a venetian blind are: front and back side reflectance and transmittance of the slat, geometry and infrared emissivity and transmittance of the slate. The effective optical properties of the venetian blind are determined by tracking beam and diffuse solar radiation through various interactions with slats positioned at a given slat angle. The model uses simple four-surface model if the slats are fully sunlit and a six-surface model if the slats are partially sunlit (ASHRAE 1311-RP). Slats are assumed to be thin and flat but a correction is applied to account for slat curvature effect (Kotey et al. 2008).
-
-#### Roller Blinds
-
-The off-normal properties of roller-blind are determined from solar properties of roller blind fabric measured at normal incidence (q=0) using correlations (Kotey, et. al., 2009b). The off-normal properties for roller blind shades are calculated using the set equations given below:
-
-<div>$${{\rm{\tau }}_{bb}}\left( {\rm{\theta }} \right) = \left\{ \begin{array}{l}{{\rm{\tau }}_{bb}}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}{\kern 1pt} \left( {\frac{{\rm{\theta }}}{{{{\rm{\theta }}_{{\rm{cutoff}}}}}} \cdot \frac{\pi }{2}} \right)\quad \theta  &lt; {\theta_{CutOff}}\\0\quad \quad \quad \theta  \ge {\theta_{CutOff}}\end{array} \right.$$</div>
-
-<div>$${\rm{b}} = {\rm{0}}{\rm{.6}} \cdot {\rm{co}}{{\rm{s}}^{{\rm{0}}{\rm{.3}}}}\left( {{{\rm{A}}_{\rm{o}}} \cdot \frac{{\rm{\pi }}}{{\rm{2}}}} \right)$$</div>
-
-<div>$${{\rm{\theta }}_{{\rm{cutoff}}}} = {\rm{65}}^\circ  + \;\left( {{\rm{90}}^\circ  - {\rm{65}}^\circ } \right) \cdot \left( {{\rm{1}} - {\rm{cos}}\left( {{{\rm{A}}_{\rm{o}}} \cdot \frac{{\rm{\pi }}}{{\rm{2}}}} \right)} \right)$$</div>
-
-<div>$${\rm{\tau }}_{{\rm{bt}}}^{}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bt}}}^{}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}{\kern 1pt} \left( {\rm{\theta }} \right)$$</div>
-
-<div>$$
-  b = \left\{ 
-    \begin{array}{lc}
-      0.133 \cdot \left( \rm{\tau}^{str} + 0.003 \right)^{-0.467} &\text{if} \left( 0 \le \rm{\tau}^{str} \le 0.33 \right) \\
-      0.33 \cdot \left( 1 - \rm{\tau}^{str} \right)               &\text{if} \left( 0.33 &lt; \rm{\tau}^{str} \le 1 \right)
-    \end{array}
-  \right.
-$$</div>
-
-<div>$${\rm{\tau }}_{}^{{\rm{str}}} = \frac{{{\rm{\tau }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right) - {{\rm{\tau }}_{{\rm{bb}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}{{{\rm{1}} - {{\rm{\tau }}_{{\rm{bb}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}$$</div>
-
-<div>$${\rm{\tau bt}}\left( {\rm{\theta }} \right) = {\rm{\tau bd}}\left( {\rm{\theta }} \right) + {\rm{\tau bb}}\left( {\rm{\theta }} \right)$$</div>
-
-The off-normal solar property calculation of roller blind is based on a set of correlations developed from measurement data using samples of commonly used commercially produced roller blind material openness range of 0.0 – 0.14. Thus, these correlations are not applicable for shades with materials openness fraction exceeding 0.20. The mean solar reflectance of a roller blind material was found to be purely diffuse and unaffected by incidence angle and is given by:
-
-<div>$${\rm{\rho }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right) = {\rm{\rho }}_{{\rm{bd}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right) = {\rm{\rho }}_{{\rm{bt}}}^{}\left( {\rm{\theta }} \right) = {\rm{\rho }}_{{\rm{bd}}}^{}\left( {\rm{\theta }} \right)$$</div>
-
-The diffuse-diffuse transmittance and reflectance are obtained by Rhomberg numerical integration. The longwave properties of roller blind material determined using the material property and the openness fraction (Kotey et al. 2008) as shown below:
-
-<div>$${\varepsilon ^{{\rm{rb}}}} = {\rm{0}}{\rm{.91}} \cdot \left( {{\rm{1 - }}{{\rm{A}}_{\rm{o}}}} \right)$$</div>
-
-<div>$${\tau ^{{\rm{rb}}}} = {\rm{1}} - {\rm{0}}{\rm{.95}} \cdot \left( {{\rm{1}} - {{\rm{A}}_{\rm{o}}}} \right)$$</div>
-
-#### Insect Screens
-
-The empirical correlations formulated to obtain the effective off-normal solar and longwave properties of insect screens were based on measurements (Kotey et al. (2009a). Insect screen geometry is shown in Figure 119. The calculation of effective solar properties requires a set of properties measured at normal incidence: *t*<sub>bb</sub> (q=0), *t*<sub>bd</sub> (q=0) and *r*<sub>bt</sub> (q=0).
-
-![](media/image1857.svg.png)
-
-Figure 119. Geometry used for insect screen analysis
-
-Openness can be determined by optical measurement at normal incidence, A<sub>o</sub>=*t*<sub>bb</sub> (q=0), but in the case of insect screens A<sub>o</sub> can reliably be calculated knowing wire diameter (*d*), and wire spacing (*s*) as follows:
-
-<div>$${A_o} = {\left( {1 - {d \mathord{\left/ {\vphantom {d s}} \right. } s}} \right)^2}$$</div>
-
-The incidence angle beyond which direct beam transmission is cut off, *q*<sub>CutOff</sub>, can also be estimated purely from geometry and is given by:
-
-<div>$${\theta_{CutOff}} = co{s^{ - 1}}\left( {{d \mathord{\left/ {\vphantom {d S}} \right. } S}} \right)$$</div>
-
-The off-normal properties are calculated as follows.
-
-<div>$${\tau_{bb}}\left( {\rm{\theta }} \right) = \left\{ \begin{array}{l}{\tau_{bb}}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}\left( {\frac{{\rm{\theta }}}{{{{\rm{\theta }}_{{\rm{cutoff}}}}}} \cdot \frac{\pi }{{\rm{2}}}} \right)\quad {\rm{\theta }} &lt; {{\rm{\theta }}_{{\rm{cutoff}}}}\\0\quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \;\,{\rm{\theta }} \ge {{\rm{\theta }}_{{\rm{cutoff}}}}\end{array} \right.$$</div>
-
-<div>$${\rm{b}} =  - {\rm{0}}{\rm{.45}}\;{\rm{ln}}\;\left( {{\rm{MAX}}\left( {{{\rm{\tau }}_{{\rm{bb}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right){\rm{,}}\;{\rm{0}}{\rm{.01}}} \right)} \right)\; + \;{\rm{0}}{\rm{.1}}$$</div>
-
-<div>$${\rm{\tau }}_{{\rm{bt}}}^{}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bt}}}^{}{\rm{(\theta }} = {\rm{0)}} \cdot {\rm{co}}{{\rm{s}}^{\rm{b}}}\left( {\rm{\theta }} \right)$$</div>
-
-<div>$${\rm{b}} =  - {\rm{0}}{\rm{.65}}\;{\rm{ln}}\;\left( {{\rm{MAX}}\left( {{{\rm{\tau }}_{{\rm{bt}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right){\rm{,}}\;{\rm{0}}{\rm{.01}}} \right)} \right)\; + \;{\rm{0}}{\rm{.1}}$$</div>
-
-<div>$${\rm{\tau }}_{{\rm{bd}}}^{}\left( {\rm{\theta }} \right) = {\rm{\tau }}_{{\rm{bt}}}^{}\left( {\rm{\theta }} \right) - {\rm{\tau }}_{{\rm{bb}}}^{}\left( {\rm{\theta }} \right)$$</div>
-
-<div>$${\rm{\rho }}_{{\rm{bt}}}^{}\left( {\rm{\theta }} \right) = {\rm{\rho }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right) + \left( {{\rm{\rho }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = 9{\rm{0}}^\circ } \right) - {\rm{\rho }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right)} \right) \cdot \left( {1 - {\rm{co}}{{\rm{s}}^{\rm{b}}}\left( {\rm{\theta }} \right)} \right)$$</div>
-
-<div>$${\rm{b}} =  - {\rm{0}}{\rm{.45}}\;{\rm{ln}}\;{\left( {{{\rm{\rho }}^{\rm{w}}}} \right)^{}}$$</div>
-
-<div>$${\rm{\rho }}_{}^{\rm{w}} = \frac{{{\rm{\rho }}_{{\rm{bt}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}{{{\rm{1}} - {\rm{\tau }}_{{\rm{bb}}}^{}\left( {{\rm{\theta }} = {\rm{0}}} \right)}}$$</div>
-
-<div>$${\rho_{{\rm{bt}}}}\left( {{\rm{\theta }} = {\rm{90}}^\circ } \right) = {\rho_{{\rm{bt}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right) + \left( {1 - {\rho_{{\rm{bt}}}}\left( {{\rm{\theta }} = {\rm{0}}} \right)} \right)\;\left( {{\rm{0}}{\rm{.35}}{\rho ^{\rm{w}}}} \right)$$</div>
-
-The diffuse-diffuse material properties are obtained by Rhomberg numerical integration. The longwave properties of insect screen are given by expressions similar those formulated for drapery fabrics, and roller blinds (Kotey et al. 2008) is given by:
-
-<div>$${\varepsilon ^{screen}} = {\varepsilon ^{\rm{w}}} \cdot \left( {{\rm{1  -  }}{{\rm{A}}_{\rm{o}}}} \right)$$</div>
-
-<div>$${\tau ^{{\rm{screen}}}} = {\rm{1 - }}{\tau ^{\rm{w}}} \cdot \left( {{\rm{1  -  }}{{\rm{A}}_{\rm{o}}}} \right)$$</div>
-
-The apparent wire material emissivity can be taken as *e*<sup>w</sup>=0.93 for common insect screens - screens with dark, rough, non-metallic wire surfaces. The corresponding infrared wire material transmittance is *t*<sup>w</sup>=0.98. A lower infrared emissivity can be used for screens constructed with shiny metallic wire. For example, to model stainless-steel wire mesh use *e*<sup>w</sup>=0.32 and *t*<sup>w</sup>=0.81.
-
-#### Integration with Heat Balance Method
-
-The solar model calculations are performed surface by surface following the existing structure of EnergyPlus’s heat balance algorithm. The optical and thermal calculations are performed for each surface at each time step. The thermal model needs to be updated at each time step during the surface heat balance iteration. Thus, window thermal model is invoked during the surface heat balance but only once. This is consistent with the current EnergyPlus’s window model inside surface heat balance iteration scheme. The equivalent layer window thermal model also has internal iteration scheme. The thermal model routine also requires the solar and shortwave radiation flux absorbed by each layer of a fenestration at each time step. The calculation of the absorbed radiation flux is performed using the existing scheme except that the optical properties are calculated by the equivalent layer optical model. The equivalent layer thermal model returns the temperatures and the fluxes at each layer.
-
-#### Equivalent Layer Window Solar Model
-
-The equivalent layer window solar model calculates the transmittance of the window and absorptance of each layer. Separate optical properties calculations are performed for exterior beam and diffuse radiations, and interior diffuse radiation (e.g., lighting and inter-reflected solar gain). The fractions for beam radiations depend on solar incident angle and hence updated for each time step. Diffuse radiation fractions are the same for all time steps unless the shade characteristics are altered; for instance, when the venetian blind slat angle is controlled. Otherwise, the diffuse fractions are constant for a given configuration and time step. The hub of the optical properties calculation routine for Equivalent Layer window model is the routine “ASHWAT\_Solar�. For beam radiation, at each time step, first the normal incidence optical properties are modified for current incident angle. Using the off-normal properties, then the ASHWAT\_Solar routine sets up the coefficient matrix based on the net radiation concept to determine the effective absorptance of each layer and the window transmittance. The total intensity of shortwave radiation absorbed at each layer is determined by multiplying the incident solar radiation, reflected internal solar radiations, and internal shortwave source components by the appropriate absorbed fractions and summing them.
-
-#### Equivalent Layer Window Thermal Model
-
-The equivalent layer thermal model is calculated only once for each time step. But the thermal model has internal iterative solutions scheme. During each time step, the procedure initially assumes that room air and means radiant temperatures are known. The surface heat balance loops through all zone surfaces while invoking the Equivalent Layer thermal model only once for each window surface at the first iteration. The window surfaces temperatures from the first iteration are used to complete the heat balances for the indoor (and implicitly the outdoor) face of each surface iteratively. Once indoor surface temperatures are calculated using the surface heat balance, the zone air temperature can be updated and the loads are predicted. Shaded fenestration in general do not have single inside temperature by virture their long-wave radiation transmittance. The equivalent layer window model accounts for this using effective emissivity of the composite layers derived for each fenestration (ASHRAE 1311-RP) as shown below:
-
-<div>$${\varepsilon ^{eff}} = \sum\limits_{j = 0}^{nl} {\left[ {{\varepsilon_j} \cdot \prod\limits_{k = j{ + 1}}^{nl + {1}} {{\tau_k}} } \right]} $$</div>
-
-where
-
-*e<sup>eff</sup>*   =          composite indoor (room-side) longwave emissivity, (-)
-
-*e<sub>j</sub>    =         * effective emissivity of layer j, (-)
-
-*t<sub>k</sub>    =         * effective infrared transmittance of layer k (*t<sub>nl+1</sub>* = 1)
-
-*nl    =         * number of layers in fenestration system (glazing and shade). Layers are numbered outside to inside (layer 1 is outermost, layer *nl* is innermost).
-
-Each equivalent layer window surafce yields net longwave radiant flux exchanged with the zone surfaces. Net longwave radiation exchange from the window to the zone is recast for a composite surface temperature calculation as follows:
-
-<div>$${T^{eff}} = \sqrt[4]{{\frac{{{Q_{lw}}}}{{\sigma {\varepsilon ^{eff}}}}}} + {T_0}$$</div>
-
-where
-
-*T<sup>eff</sup>*  =          inside surface temperature of the composite layer, °C (°F)
-
-*Q<sub>lw</sub>*  =          infrared radiant gain from zone, W/m2 (Btu/h-ft2)
-
-*s*    =          Stefan-Boltzmann constant, W/m2-K4 (Btu/h-ft2-R4)
-
-*T<sub>0</sub>*   =          Temperature of absolute zero, -273.15 °C (-459.67 °F)
-
-Recalculating effective inside face window temperature may result in extra convection flux. The  “extra� (Other) convective flux is computed; this is the gain in excess of that resulting from the standard surface heat balance model. The net other convection term *QX* calculated below is added to the zone air heat balance (ASHRAE 1311-RP).
-
-<div>$$QX = {Q_{conv}} - hc \cdot ({T^{eff}} - {T_a})$$</div>
-
-Where,
-
-*h<sub>c</sub>   =         * inside convective coefficient of the fenestration, W/m<sup>2</sup>-K (Btu/h-ft<sup>2</sup>-F)
-
-*Q<sub>conv</sub>            =         * total convective heat flux to zone from equivalent layer window thermal model, W/m<sup>2</sup> (Btu/h-ft<sup>2</sup>); includes open-channel gains and impact of inside surface convective coefficient
-
-*T<sub>a</sub>   =         * zone air temperature, °C (°F)
-
-#### References:
-
-Edwards, D.K. 1977. Solar absorption by each element in an absorber-coverglass array, Technical Note, Solar Energy, Vol. 19, pp. 401-402.
-
-Parmelee, G. V., and W. W. Aubele. 1952. The shading of sunlit glass: an analysis of the effect of uniformly spaced flat opaque slats, ASHVE Transactions, Vol. 58, pp. 377-398.
-
-Farber, Erich A.; William A. Smith, C.W. Pennington, John C. Reed. 1963. Theoretical analysis of solar heat gain through insulating glass with inside shading. ASHRAE Transactions, Vol. 69, pp.393-405.
-
-Rheault, S., and E. Bilgen. 1989. Heat transfer analysis in an automated venetian blind system, Journal of Solar Energy, Vol. 111 (Feb.), pp. 89-95.
-
-Pfrommer, P., K. J. Lomas, and C. Kupke. 1996. "Solar Radiation Transport through Slat-Type Blinds: a New Model and its Application for Thermal Simulation of Buildings," Solar Energy, Vol. 57, No. 2, pp. 77-91.
-
-Rosenfeld, J.L.J., W. J. Platzer, H. Van Dijk, and A. Maccari. 2000. "Modelling the Optical and Thermal Properties of Complex Glazing: Overview of Recent Developments", Solar Energy, Vol. 69 Supplement, No. 1-6, pp.1-13.
-
-Yahoda, D. S. and J. L. Wright. 2004. "Methods for Calculating the Effective Longwave Radiative Properties of a Venetian Blind Layer," ASHRAE Transactions, Vol. 110, Pt. 1., pp. 463-473.
-
-Yahoda, D. S. and J. L. Wright. 2005. "Methods for Calculating the Effective Solar-Optical Properties of a Venetian Blind Layer," ASHRAE Transactions, Vol. 111, Pt. 1, pp. 572-586.
-
-Yahoda, D. S. and J. L. Wright. 2004. "Heat Transfer Analysis of a Between-Panes Venetian Blind Using Effective Longwave Radiative Properties," ASHRAE Transactions, Vol. 110, Pt. 1., pp. 455-462.
-
-Huang, N.Y.T., J. L. Wright, M. R. Collins. 2006. "Thermal Resistance of a Window with an Enclosed Venetian Blind: Guarded Heater Plate Measurements," ASHRAE Transactions, Vol. 112, Pt. 2. pp. 13-21.
-
-Wright, J. L. 2008. "Calculating Centre-Glass Performance Indices of Glazing Systems with Shading Devices," ASHRAE Transactions, Vol. 114, Pt. 2.
-
-Wright, J. L., N. Y. T. Huang, and M. R. Collins. 2008. "Thermal Resistance of a Window with an Enclosed Venetian Blind: A Simplified Model," ASHRAE Transactions, Vol. 114, Pt. 1.
-
-Kotey, N. A., J. L. Wright, and M. R. Collins. 2008. “Determining Longwave Radiative Properties of Flat Shading Materials,� 33rd Annual SESCI / 3rd CSBC Conference Proceedings, Fredericton, NB.
-
-Kotey, N.A., Wright, J.L., M. R. Collins. 2009a. "Determination of Angle-Dependent Solar Optical Properties of Roller Blind Materials," drafted for submission to ASHRAE Transactions, Vol. 115, Pt. 1.
-
-Kotey, N.A., Wright, J.L., M. R. Collins. 2009b. "Determination of Angle-Dependent Solar Optical Properties of Drapery Fabrics," in review, ASHRAE Transactions, Vol. 115, Pt. 2.
-
-Wright, John L., Charles S. Barnaby, Michael R. Collins, and Nathan A. Kotey. Improving Cooling Load Calculations for Fenestration with Shading Devices . ASHRAE 1311-RP, Final Report, February 11, 2009.
diff --git a/doc/src/docs/EngineeringReference/08-AirHeatBalance.md b/doc/src/docs/EngineeringReference/08-AirHeatBalance.md
deleted file mode 100644
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+++ /dev/null
@@ -1,391 +0,0 @@
-
-Air Heat Balance Manager / Processes
-====================================
-
-Convection from Surfaces
-------------------------
-
-This contribution is expressed using the convective heat transfer coefficient as follows:
-
-<div>$${q_{conv}} = \sum\limits_{i = 1}^{nsurfaces} {{h_{c,i}}{A_i}\left( {{T_a} - {T_{s,i}}} \right)} $$</div>
-
-The inside heat transfer coefficient is modeled from a choice of correlations.
-
-Convection from Internal Sources
---------------------------------
-
-This component is the companion part of the radiant contribution from internal gains described previously.  It is added directly into the air heat balance. Such a treatment also violates the tenets of the heat balance since the surface temperature of the surfaces producing the internal loads exchange heat with the zone air through normal convective processes.   However, once again, the details required to include this component in the heat balance are generally not available, and its direct inclusion into the air heat balance is a reasonable approach..
-
-Infiltration/Ventilation
-------------------------
-
-### Infiltration
-
-Any outdoor air that enters by way of infiltration is assumed to be immediately mixed with the zone air. The determination of the amount of infiltration air is quite complicated and subject to significant uncertainty. In the most common procedure, the infiltration quantity is converted from a number of air changes per hour (ACH) and included in the zone air heat balance using the outside temperature at the current simulation time step.
-
-EnergyPlus contains three models for infiltration. The first is the “Design Flow Rate� model that was inherited from EnergyPlus’ predecessor programs. It is accessed through the ZoneInfiltration:DesignFlowRate object and is based on environmental conditions modifying a design flow rate.  The second is the “Effective Leakage Area� model based on Sherman and Grimsrud (1980) and accessed using the ZoneInfiltration:EffectiveLeakageArea input object.  The third is the “Flow Coefficient� model based on Walker and Wilson (1998) and accessed using the ZoneInfiltration:FlowCoefficient input object. The model formulations for the Effective Leakage Area and Flow Coefficient models are from the ASHRAE Handbook of Fundamentals (2001 Chapter 26; 2005 Chapter 27) where they are referred to as “Basic� and “Enhanced�, respectively.
-
-### Infiltration Design Flow Rate
-
-Infiltration (Ref Object: ZoneInfiltration:DesignFlowRate) is the unintended flow of air from the outdoor environment directly into a thermal zone. Infiltration is generally caused by the opening and closing of exterior doors, cracks around windows, and even in very small amounts through building elements. In this model, the user defines a design flow rate that can be modified by temperature differences and windspeed. The basic equation (Coblenz and Achenbach 1963) used to calculate infiltration with this model is:
-
-<div>$$Infiltration = \left( {{I_{design}}} \right)\left( {{F_{schedule}}} \right)\left[ {A + B\left| {\left( {{T_{zone}} - {T_{odb}}} \right)} \right| + C\left( {WindSpeed} \right) + D\left( {Windspee{d^2}} \right)} \right]$$</div>
-
-More advanced infiltration calculations are possible using the EnergyPlus AirflowNetwork model for natural infiltration driven by wind when the HVAC system does not operate and/or driven by wind and forced air for times when the HVAC system operates. Exfiltration (the leakage of zone air to the outside) is generally handled better as zone exhaust air in the zone equipment description.
-
-The question of typical values for these coefficients is subject to debate. Ideally, one should do a detailed analysis of the infiltration situation and then determine a custom set of coefficients using methods such as those laid out in Chapter 26 of the ASHRAE Handbook of Fundamentals. The EnergyPlus defaults are 1,0,0,0 which gives a constant volume flow of infiltration under all conditions.
-
-BLAST (one of the EnergyPlus predecessors) used the following values as defaults:  0.606, 0.03636, 0.1177, 0. These coefficients produce a value of 1.0 at 0C deltaT and 3.35 m/s (7.5 mph) windspeed, which corresponds to a typical summer condition. At a winter condition of 40C deltaT and 6 m/s (13.4 mph) windspeed, these coefficients would increase the infiltration rate by a factor of 2.75.
-
-In DOE-2 (the other EnergyPlus predecessor), the air change method defaults are (adjusted to SI units) 0, 0, 0.224 (windspeed), 0. With these coefficients, the summer conditions above would give a factor of 0.75, and the winter conditions would give 1.34. A windspeed of 4.47 m/s (10 mph) gives a factor of 1.0.
-
-The source of the BLAST defaults is noted in the BLAST documentation as:
-
-"Empirical equation and the coefficient default were determined from ASHRAE journal articles and other data on the effects of outdoor weather conditions."
-
-The source of the DOE-2 defaults is based on examining the infiltration relationships described in the ASHRAE Handbook of Fundamentals.
-
-The EnergyPlus example files use all of the above, the BLAST defaults in some (e.g., GeometryTest), the DOE-2 defaults in some (e.g., 5ZoneAirCooled), and the EnergyPlus defaults in some (e.g., LgOffVAVDetCoil).
-
-### Infiltration by Effective Leakage Area
-
-The Effective Leakage Area model is based on Sherman and Grimsrud (1980) and accessed using the ZoneInfiltration:EffectiveLeakageArea input object.  The model formulation used in EnergyPlus is from the ASHRAE Handbook of Fundamentals (2001 Chapter 26; 2005 Chapter 27) where it is referred to as the “Basic� model.
-
-The Effective Leakage Area, or Sherman-Grimsrud, model is:
-
-<div>$$Infiltration = \left( {{F_{Schedule}}} \right)\frac{{{A_L}}}{{1000}}\sqrt {{C_s}\Delta T + {C_w}{{\left( {WindSpeed} \right)}^2}} $$</div>
-
-where,
-
-<span>\({F_{schedule}}\)</span> is a value from a user-defined schedule,
-
-<span>\({A_L}\)</span> is the effective air leakage area in cm<sup>2</sup> that corresponds to a 4 Pa pressure differential,
-
-<span>\({C_s}\)</span> is the coefficient for stack-induced infiltration in (L/s)<sup>2</sup>/(cm<sup>4</sup>·K),
-
-<span>\(\Delta T\)</span> is the absolute temperature difference between zone air and outdoor air,
-
-<span>\({C_w}\)</span> is the coefficient for wind-induced infiltration in (L/s)<sup>2</sup>/(cm<sup>4</sup>·(m/s)<sup>2</sup>), and
-
-<span>\(WindSpeed\)</span> is the local wind speed.
-
-### Infiltration by Flow Coefficient
-
-The Flow Coefficient model is based on Walker and Wilson (1998) and accessed using the ZoneInfiltration:FlowCoefficient input object.  The model formulation used in EnergyPlus is from the ASHRAE Handbook of Fundamentals (2001 Chapter 26; 2005 Chapter 27) where it is referred to as the “Enhanced� or “AIM-2� model.
-
-The Enhanced, or AIM-2, model is:
-
-<div>$$Infiltration = \left( {{F_{Schedule}}} \right)\sqrt {{{\left( {c\,{C_s}\Delta {T^n}} \right)}^2} + {{\left( {c\,{C_w}{{\left( {s * WindSpeed} \right)}^{2n}}} \right)}^2}} $$</div>
-
-where,
-
-<span>\({F_{schedule}}\)</span> is a value from a user-defined schedule,
-
-<span>\(c\)</span> is the flow coefficient in m<sup>3</sup>/(s·Pa<sup>n</sup>),
-
-<span>\({C_s}\)</span> is the coefficient for stack-induced infiltration in (Pa/K)<sup>n</sup>,
-
-<span>\(n\)</span> is the pressure exponent,
-
-<span>\({C_w}\)</span> is the coefficient for wind-induced infiltration in (Pa·s<sup>2</sup>/m<sup>2</sup>)<sup>n</sup>, and
-
-<span>\(s\)</span> is the shelter factor.
-
-#### References:
-
-Coblenz, C. W. and Achenbach, P. R. 1963. Field Measurement of Ten Electrically-Heated Houses. ASHRAE Transactions pp 358-365.
-
-Sherman, M.H. and D.T. Grimsrud. 1980. Infiltration-pressurization correlation: Simplified physical modeling. ASHRAE Transactions 86(2):778
-
-Walker, I.S., and D.J. Wilson. 1998. Field validation of equations for stack and wind driven air infiltration calculations.  International Journal of HVAC&R Research 4(2).
-
-ASHRAE Handbook of Fundamentals. 2005. Chapter 27. (and 2001 Chapter 26).
-
-### Ventilation
-
-EnergyPlus contains two models for ventilation.  The “Design Flow Rate� model, inherited from EnergyPlus’ predecessor programs, is accessed through the ZoneVentilation:DesignFlowRate object and is based on environmental conditions modifying a design flow rate.  The “Wind and Stack with Open Area� model, based on equations defined in Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals, is accessed using the ZoneVentilation:WindandStackOpenArea input object. Since the “Wind and Stack with Open Area� object requires the height difference between the midpoint of the lower opening and the neutral pressure level, which is difficult to estimate, this object should be used with care (e.g., research only).
-
-These two ventilation objects can be used alone or in combination to determine ventilation air for a zone. If multiple ZoneVentilation:\* objects are specified for a zone, then the total zone ventilation flow rate is the sum of the ventilation air flow rates calculated by each ZoneVentilation object.
-
-### Ventilation Design Flow Rate
-
-Ventilation (Ref Object: ZoneVentilation:DesignFlowRate) is the purposeful flow of air from the outdoor environment directly into a thermal zone in order to provide some amount of non-mechanical cooling.  Ventilation as specified by this input syntax is intended to model “simple� ventilation as opposed to the more detailed ventilation investigations that can be performed with the AirflowNetwork model.  Simple ventilation in EnergyPlus can be controlled by a schedule and through the specification of minimum, maximum and delta temperatures. The temperatures can be either single constant values for the entire simulation or schedules which can vary over time. Specific details are given in the Input/Output reference document. As with infiltration, the actual flow rate of ventilation can be modified by the temperature difference between the inside and outside environment and the wind speed. The basic equation used to calculate ventilation using this model is:
-
-<div>$$Ventilation = \left( {{V_{design}}} \right)\left( {{F_{schedule}}} \right)\left\lfloor {A + B\left| {{T_{zone}} - {T_{odb}}} \right| + C\left( {WindSpeed} \right) + D\left( {WindSpee{d^2}} \right)} \right\rfloor $$</div>
-
-More advanced ventilation calculations are possible using the EnergyPlus AirflowNetwork model.
-
-The following description is copied from the Infiltration discussion above. The question of typical values for these coefficients is subject to debate. Ideally, one should do a detailed analysis of the ventilation situation and then determine a custom set of coefficients using methods such as those laid out in Chapter 26 of the ASHRAE Handbook of Fundamentals. The EnergyPlus defaults are 1,0,0,0 which gives a constant volume flow of ventilation under all conditions.
-
-BLAST (one of the EnergyPlus predecessors) used the following values as defaults:  0.606, 0.03636, 0.1177, 0. These coefficients produce a value of 1.0 at 0C deltaT and 3.35 m/s (7.5 mph) windspeed, which corresponds to a typical summer condition. At a winter condition of 40C deltaT and 6 m/s (13.4 mph) windspeed, these coefficients would increase the ventilation rate by a factor of 2.75.
-
-In DOE-2 (the other EnergyPlus predecessor), the air change method defaults are (adjusted to SI units) 0, 0, 0.224 (windspeed), 0. With these coefficients, the summer conditions above would give a factor of 0.75, and the winter conditions would give 1.34. A windspeed of 4.47 m/s (10 mph) gives a factor of 1.0.
-
-The source of the BLAST defaults is noted in the BLAST documentation as:
-
-"Empirical equation and the coefficient default were determined from ASHRAE journal articles and other data on the effects of outdoor weather conditions."
-
-The source of the DOE-2 defaults is based on examining the infiltration relationships described in the ASHRAE Handbook of Fundamentals.
-
-The EnergyPlus example files use all of the above, the BLAST defaults in some (e.g., AirflowNetwork\_Simple\_house), the DOE-2 defaults in some (e.g., VentilationSimpleTest – has all 3), and the EnergyPlus defaults in some (e.g., 5ZoneNightVent2).
-
-### Ventilation by Wind and Stack with Open Area
-
-For this model (Ref Object: ZoneVentilation:WindandStackOpenArea), the ventilation air flow rate is a function of wind speed and thermal stack effect, along with the area of the opening being modeled. This object can be used alone or in combination with ZoneVentilation:DesignFlowRate objects. This model is intended for simplified ventilation calculations as opposed to the more detailed ventilation investigations that can be performed with the AirflowNetwork model. Using the “Wind and Stack with Open Area� model, the natural ventilation flow rate can be controlled by a multiplier fraction schedule applied to the user-defined opening area and through the specification of minimum, maximum and delta temperatures. The temperatures can be either single constant values for the entire simulation or schedules which can vary over time. The equation used to calculate the ventilation rate driven by wind is given by Eq. 37 in Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals:
-
-<div>$${Q_w} = {C_w}{A_{opening}}{F_{schedule}}V$$</div>
-
-where,
-
-*Q<sub>w</sub>*  = Volumetric air flow rate driven by wind [m<sup>3</sup>/s]
-
-*C<sub>w</sub>*  = Opening effectiveness [dimensionless]
-
-*A<sub>opening</sub>*        = Opening area [m<sup>2</sup>]
-
-*F<sub>schedule</sub>* = Open area fraction [user-defined schedule value, dimensionless]
-
-*V*    = Local wind speed [m/s]
-
-If the user specifies “Autocalculate� for the Opening Effectiveness input field, the opening effectiveness is calculated for each simulation time step based on the angle between the actual wind direction and the Effective Angle (a user-defined input) using the following equation:
-
-<div>$${C_w} = 0.55 - \frac{{\left| {EffectiveAngle - WindDirection} \right|}}{{180}}*0.25$$</div>
-
-The difference |EffectiveAngle – WindDirection| should be between 0 and 180 degrees. If the difference |EffectivAngle – WindDirection| is greater than 180, the difference is reset to be minus 180 degrees. This equation is a linear interpolation using the values recommended by the 2009 ASHRAE Handbook of Fundamentals (page 16.13): 0.5 to 0.6 for perpendicular winds and 0.25 to 0.35 for diagonal winds.
-
-The equation used for calculating the ventilation rate due to stack effect is given by Eq. 38 in Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals:
-
-<div>$${Q_s} = {C_D}{A_{opening}}{F_{schedule}}\sqrt {2g\Delta {H_{NPL}}(|{T_{zone}} - {T_{odb}}|/{T_{zone}})} $$</div>
-
-where,
-
-*Q<sub>s</sub>*  = Volumetric air flow rate due to stack effect [m<sup>3</sup>/s]
-
-*C<sub>D</sub>*  = Discharge coefficient for opening [dimensionless]
-
-*A<sub>opening</sub>*        = Opening area [m<sup>2</sup>]
-
-*F<sub>schedule</sub>* = Open area fraction [user-defined schedule value, dimensionless]
-
-*ΔH<sub>NPL</sub>*        = Height from midpoint of lower opening to the neutral pressure level [m].
-
-Estimation of this value is difficult; refer to Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals for guidance.
-
-*T<sub>zone</sub>*            = Zone air dry-bulb temperature [K]
-
-*T<sub>odb</sub>*<sub>                        </sub> = Local outdoor air dry-bulb temperature [K]
-
-The following equation, given by Eq. 39 in Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals, is used to calculate the Discharge Coefficient for Opening when the user sets the value for this input field to “Autocalculate�:
-
-<div>$${C_D} = 0.40 + 0.0045\left| {{T_{zone}} - {T_{odb}}} \right|$$</div>
-
-The total ventilation rate calculated by this model is the quadrature sum of the wind and stack air flow components:
-
-<div>$$Ventilatio{n_{WindAndStack}} = \sqrt {{Q_s}^2 + {Q_w}^2} $$</div>
-
-If desired, a simple summation, instead of quadrature summation, can be realized by inputting two ZoneVentilation:WindAndStackOpenArea objects. One object can be defined with only a wind-driven component by setting C<sub>D</sub>=0, and the other object can have only stack-effect inputs specified and set C<sub>w</sub>=0.
-
-### Zone Air Balance Outdoor Airflow (ZoneAirBalance:OutdoorAir)
-
-ASHRAE 2009 Handbook of Fundamentals specifies that any unbalanced supply or exhaust ventilation air, Q<sub>u,v</sub>, to a zone causes pressurization/depressurization that influences the flow of infiltration air and thus should be combined with natural infiltration, Q<sub>n</sub>, (and, if present, unbalanced duct leakage, Qu,l) in superposition. Balanced ventilation airflow, Q<sub>b,v</sub>, to a zone (such as an ERV or HRV with balanced exhaust and intake air flows) does not interact with infiltration air and is added in whole:
-
-<div>$$Q = \sqrt {{Q_n}^2 + {Q_{u,v}}^2 + ({Q_{u,l}}^2)}  + {Q_{b,v}}$$</div>
-
-where,
-
-*Q*    = Combined outdoor airflow with infiltration, balanced and unbalanced outdoor air flows, and unbalanced duct leakage [m<sup>3</sup>/s]
-
-*Q<sub>n</sub>*   = Natural infiltration airflow [m<sup>3</sup>/s]
-
-*Q<sub>b,v</sub>* = Balanced ventilation airflow, excluding infiltration [m<sup>3</sup>/s]
-
-*Q<sub>u,v</sub>* = Unbalanced ventilation airflow, excluding infiltration [m<sup>3</sup>/s]
-
-*Q<sub>u,l</sub>*  = Unbalanced duct leakage: the difference between supply and return leaks [m<sup>3</sup>/s]
-
-The natural infiltration airflow includes all outdoor airflows from all ZoneInfiltration:\* objects for the same zone.
-
-<div>$${Q_n} = \sum\limits_i {{Q_{Infiltration,i}}} $$</div>
-
-where,
-
-*Q<sub>Infiltration,i</sub>*      = Outdoor airflow rate given in the ith ZoneInfiltration:\* objects for the same zone
-
-The balanced ventilation airflow is the sum of outdoor airflows from all ZoneVentilation: DesignFlowRate objects with Ventilation Type = Balanced:
-
-<div>$${Q_{b,v}} = \sum\limits_i {{Q_{v,Balanced,i}}} $$</div>
-
-where,
-
-*Q<sub>v,Balanced,i</sub>*     = Ventilation rate with “Balanced� ventilation type defined in the ith ZoneVentilation:DesignFlowRate object for the same zone
-
-The unbalanced ventilation airflow is given by the following equation:
-
-<div>$${Q_{u,v}} = {\left[ {{{\left( {\sum\limits_i {{Q_{v,Natural,i}}}  + \sum\limits_i {{Q_{v,Wind,i}}} } \right)}^2} + {{\left( {\sum\limits_i {{Q_{v,Intake,i}}} } \right)}^2} + {{\left( {\sum\limits_i {{Q_{v,Exhaust,i}}} } \right)}^2} + {{\left( {\sum\limits_i {Max\left( {0,\;({Q_{ERV,Exh,i}} - {Q_{ERV,Sup,i}})} \right)} } \right)}^2}} \right]^{0.5}}$$</div>
-
-where
-
-*Q<sub>v,Exhaust,i</sub>*      = Ventilation rate with “Exhaust� type in the ith ZoneVentilation:DesignFlowRate object for the same zone
-
-*Q<sub>v,Intake,i</sub>*        = Ventilation rate with “Intake� type in the ith ZoneVentilation:DesignFlowRate object for the same zone
-
-*Q<sub>v,Natural,i</sub>*       = Ventilation rate with “Natural� type in the ith ZoneVentilation:DesignFlowRate object for the same zone
-
-*Q<sub>v,Wind,v</sub>*        = Ventilation rate in the ith ZoneVentilation:WindandStackOpenArea object for the same zone
-
-*Q<sub>ERV,Sup,i</sub>*       = Supply flow rate given in the ith ZoneHVAC:EnergyRecoveryVentilator object
-
-*Q<sub>ERV,Exh,i</sub>*       = Exhaust flow rate given in the ith ZoneHVAC:EnergyRecoveryVentilator object
-
-For Ventilation Type = Intake in the ZoneVentilation:DesignFlowRate object, an appropriate amount of fan heat will be ignored and the outdoor temperature will be used in the zone air heat balance equation.
-
-This object provides a simple airflow interaction model without having to use the AirflowNetwork capabilities, when the Air Balance Method is specified as Quadrature.
-
-### Reference
-
-ASHRAE. 2009. 2009 ASHRAE Handbook – Fundamentals, Chapter 16, Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
-
-Air Exchange
-------------
-
-Air exchange and interchange between zones is treated as a convective gain. Temperature-difference-controlled or constant air mixing can be specified as a one-way or cross-zone phenomenon modeled using the ZoneMixing or ZoneCrossMixing objects. Air exchange through doorways between refrigerated spaces can be modeled using the ZoneRefrigerationMixing object.
-
-For one-way mixing (using ZoneMixing object(s)), the mixing air flow is only used for the energy and mass balance for the receiving zone. The mass referred in this section includes air, water vapor and CO<sub>2</sub>. The source zone energy and mass balance are not effected, although the user may choose to enter complementary pairs of one-way mixing objects. Multiple mixing flows can be defined for any receiving zone. For cross-zone mixing (using ZoneCrossMixing object(s)), the mixing air flow impacts the mass and energy balances in both the source and receiving zones. No more than one ZoneCrossMixing object can be used for any receiving zone. A separate ZoneCrossMixing object must be used for each of the two zones exchanging air if the mixing flow is bi-directional and based on a temperature difference greater than zero.
-
-For refrigerated space air exchange (using ZoneRefrigerationDoorMixing object(s)), the mixing air flow impacts the mass and energy balances in both the source and receiving zones. A single object accounts for the two-way air flow with the energy and mass exchanges determined by  the air density difference between the two zones.
-
-### Temperature Difference Controlled Air Exchange
-
-The volume of air flow into the receiving zone is specified by the user with a number of control parameters and schedules listed in the Input Output Guide. The user can turn this one-way flow on or off based on the temperature difference between the source and receiving zones, or it may be independent of the temperature difference. The density and specific heat of the air flowing into the receiving zone are determined using the average temperature and average humidity ratio in the source and receiving zones. The humidity ratio of the air flowing into the receiving zone is set equal to the humidity ratio of the source zone. The mass, moisture,and energy terms are then used as described in two previous sections, Basis for the Zone and Air System Integration, and Moisture Predictor-Corrector.
-
-<div>$$
-  \begin{array}{cl}
-    \rho_{Avg} &= f \left( \frac{T_{ReceivingZone} + T_{SourceZone}}{2},\frac{W_{ReceivingZone} + W_{SourceZone}}{2},P_{Barometric} \right) \\
-    c_{P,Avg} &= f \left( \frac{T_{ReceivingZone} + T_{SourceZone}}{2},\frac{W_{ReceivingZone} + W_{SourceZone}}{2}\right) \\
-    \dot m_{MixingFlowToReceivingZone} &= \sum_{AllSourceZones} \rho_{Avg}\dot V_{Air} \\
-    \dot Q_{MixingFlowToReceivingZone} &= \sum_{AllSourceZones} \rho_{Avg}C_{p,Avg}\dot V_{Air}\left(T_{sourceZone}-T_{receivingZone}\right) \\
-    \text{Moisture}_{MixingFlowToReceivingZone} &= \sum_{AllSourceZones} \rho_{Avg} \dot V_{Air} W_{SourceZone}
-  \end{array}
-$$</div>  
-  
-where:
-
-c<sub>P,Avg</sub>                                   = Average specific heat of air within the two zones (J/kg.K)
-
-<span>\({\dot m_{{\rm{MixingFlowToReceivingZone}}}}\)</span>          = Mass of moist air flowing into the receiving zone (kg<sub>air</sub>/s)
-
-Moisture<sub>MixingFlowToReceivingZone</sub>    = Moisture mass flow rate into the receiving zone (kg<sub>H2O</sub>/s)
-
-P<sub>Barometric</sub>                              = Outside barometric pressure (Pa)
-
-�<sub>Avg\\                                                                         </sub> = Average density of air within the two zones (kg/s)
-
-<span>\({\dot Q_{{\rm{MixingFlowToReceivingZone}}}}\)</span>          = Energy added to receiving zone air by mixing mass flow (W)
-
-T<sub>ReceivingZone                                                      </sub> = Temperature in the Receiving Zone (<sup>o</sup>C)
-
-T<sub>SourceZone</sub>                              = Temperature in the Source Zone (<sup>o</sup>C)
-
-<span>\({\dot V_{Air}}\)</span>                                   = Volume rate of air flow defined by the user (m<sup>3</sup>/s)
-
-W<sub>ReceivingZone</sub>              = Humidity Ratio in the Receiving Zone (kg<sub>H2O</sub>/kg<sub>dry\\ air</sub>)
-
-W<sub>SourceZone</sub>                             = Humidity Ratio in the Source Zone (kg<sub>H2O</sub>/kg<sub>dry\\ air</sub>)
-
-For cross-mixing, the mass of moist air exchanged between the two zones is assumed to be equal.  Again, the density and specific heat are based on the average conditions in the two zones. Note that the temperature and humidity ratio differences ensure that when the energy and  moisture terms are used in the Moisture Predictor-Corrector, they correctly reflect a loss or gain in each zone.
-
-<div>$$
-  \begin{array}{cl}
-    \dot{m}_{MixingFlowToReceivingZone} &= \dot{m}_{MixingFlowToSourceZone} = \rho_{Avg}\dot{V}_{Air} \\
-    \dot{Q}_{MixingFlowToSourceZone}    &= \rho_{Avg} C_{p,Avg} \dot{V}_{Air} \left( T_{ReceivingZone}-T_{SourceZone} \right) \\
-    \dot{Q}_{MixingFlowToReceivingZone} &= \rho_{Avg} C_{p,Avg} \dot{V}_{Air} \left( T_{SourceZone} - T_{ReceivingZone} \right) \\
-    \text{Moisture}_{MixingFlowToSourceZone} &= \rho_{Avg} \dot{V}_{Air} W_{ReceivingZone} \\
-    \text{Moisture}_{MixingFlowToReceivingZone} &= \rho_{Avg} \dot{V}_{Air} W_{SourceZone}
-  \end{array}
-$$</div>
-    
-where:
-
-<span>\({\dot m_{{\rm{MixingFlowToSourceZone}}}}\)</span>             = Mass of moist air flowing into the source zone (kg<sub>air</sub>/s)
-
-Moisture<sub>MixingFlowToSourceZone</sub>       = Moisture mass flow rate into the source zone (kg<sub>H2O</sub>/s)
-
-<span>\({\dot Q_{{\rm{MixingFlowToSourceZone}}}}\)</span>             = Sensible energy added to source zone air by mixing mass flow (W)
-
-<span>\({\dot Q_{{\rm{MixingFlowToReceivingZone}}}}\)</span>          = Sensible energy added to receiving zone air by mixing mass flow, W
-
-<span>\(Moistur{e_{{\rm{MixingFlowToSourceZone}}}}\)</span>= Latent load added to source zone air by mixing mass flow (kg<sub>H2O</sub>/s)
-
-<span>\(Moistur{e_{{\rm{MixingFlowToReceivingZone}}}}\)</span>= Latent load added to receiving zone air by mixing mass flow (kg<sub>H2O</sub>/s)
-
-### Density Difference Controlled Air Exchange
-
-When closed refrigerated spaces exchange air with other closed spaces, the air flow is determined by the difference in air density between the two spaces. The fundamental assumption for this case is that the mass of dry air exchanged between the two spaces is the same.(Gosney and Olama,  1975] This assumption applies to situations where the colder of the two spaces is essentially sealed to other air flows, that is, there are no open doors or exhaust air flows. Multiple refrigeration door mixing objects can be used for the zone, but if there are multiple doors open at the same time for any significant amount of time, the model will not give results appropriate for that condition.
-
-The sensible and latent energy loads are modeled according to the guidance specified in (ASHRAE 2006d, ASHRAE 2009, and Gosney and Olama, 1975).  Equal dry air exchange is assumed, that is, the mass of dry air infiltrating into the receiving zone is assumed to equal the mass of dry air infiltrating out of the source zone.
-
-<div>$$
-  \begin{array}{cl}
-    h_{zoneA},\rho_{zoneA} &= f (T_{zoneA},W_{zoneA},P_{Barometric}) \\
-    h_{zoneB},\rho_{zoneB} &= f (T_{zoneB},W_{zoneB},P_{Barometric}) \\
-    \rho_{zoneA} &\gt \rho_{zoneB} \\
-    \dot{Q}_{Mixing} &= \dot{Q}_{FullFlow} \times \text{Schedule}_{DoorOpen} \times F_{Flow} \times (1-F_{Protection}) \\
-    \dot{Q}_{FullFlow} &= B (h_{zoneB}-h_{zoneA}) \\
-    B &= 0.221 A_{door} \rho_{zoneA} F_{Density} \sqrt{ \left(1-\frac{\rho_{zoneB}}{\rho_{zoneA}}\right) g H_{Door} } \\
-    F_{Density} &= \left[ \frac{2}{1+\left(\rho_{zoneA}/\rho_{zoneB}\right)^{1/3}} \right]^{1.5} \\
-    \dot{m}_{DryAirZonesAB} &= \frac{\dot{Q}_{Mixing}}{h_{zoneB}-h_{zoneA}} \\
-    \dot{m}_{MixingFlowZoneBtoA} &= \sum_{AllZoneBs} \dot{m}_{DryAirZonesAB}\left(1+W_{ZoneB}\right) \\
-    \dot{Q}_{MixingFlowZoneBtoA} &= \sum_{AllZoneBs} \dot{m}_{ZoneBtoA} C_{p,ZoneB} \left(T_{zoneB}-T_{zoneA}\right) \\
-    \text{Moisture}_{MixingFlowZoneBtoA} &= \sum_{AllZoneBs} \dot{m}_{ZoneBtoA} \left( W_{zoneB}-W_{zoneA} \right) \\
-    \dot{m}_{MixingFlowZoneAtoB} &= \sum_{AllZoneAs} \dot{m}_{DryAirZonesAB}\left(1+W_{ZoneA}\right) \\
-    \dot{Q}_{MixingFlowZoneAtoB} &= \sum_{AllZoneAs} \dot{m}_{ZoneBtoA} C_{p,ZoneA} \left(T_{zoneA}-T_{zoneB}\right) \\
-    \text{Moisture}_{MixingFlowZoneAtoB} &= \sum_{AllZoneAs} \dot{m}_{ZoneBtoA} \left( W_{zoneA}-W_{zoneB} \right) 
-  \end{array}
-$$</div>
-
-where:
-
-A<sub>door</sub>            =  Area of door between Zones A and B (m<sup>2</sup>)
-
-F<sub>Flow</sub>            =  Doorway flow factor, = 0.8 if ΔT &gt; 11<sup>o</sup>C; =1.1 if ΔT &lt;= 11<sup>o</sup>C
-
-F<sub>Protection</sub>        = Doorway protection factor, = 0 for no protection; =  0.5 for an air curtain; and 0.9 for a strip curtain (dimensionless)
-
-g                =  Gravitational constant (m/s<sup>2</sup>)
-
-h<sub>ZoneA                     </sub> =  enthalpy of the air within Zone A (J/kg)
-
-h<sub>ZoneB                     </sub> =  enthalpy of the air within Zone B (J/kg)
-
-H<sub>door</sub>            =  Height of door between source and receiving zones (m)
-
-Q<sub>FullFlow</sub>        = Sensible and latent refrigeration load (on Zone A) for fully established flow (W)
-
-Q<sub>Mixing</sub>          = Sensible and latent mixing refrigeration load on Zone A for the time step (W)
-
-m<sub>DryAirZoneAB</sub>   = Mass of dry air exchanged between zones A and B (kg<sub>air</sub>/s)
-
-Schedule<sub>DoorOpen</sub>        = Value scheduled by user, fraction of time door open during time step (dimensionless)
-
-W<sub>ZoneA                  </sub> =  Humidity ratio of the air within Zone A (kg<sub>H2O</sub>/kg<sub>air</sub>)
-
-W<sub>ZoneB</sub>          =  Humidity ratio of air within Zone B (kg<sub>H2O</sub>/kg<sub>air</sub>)
-
-Ρ<sub>ZoneA                    </sub> =  Density of air within Zone A (kg/m<sup>3</sup>)
-
-�<sub>ZoneB</sub>           =  Density of air within Zone B (kg/m<sup>3</sup>)
-
-### References
-
-ASHRAE. 2006d. *Refrigeration Handbook*, Chapter 13. Atlanta: American Society of Heating,
-
-Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2009. *Fundamentals Handbook*, Chapter 1. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Gosney, W.B., Olama, G.A.-L. 1975. Heat and Enthalpy Gains through Cold Room Doorways,  Proceedings of the Institute of Refrigeration, vol. 72, pp 31-41
-
-Calculation of Zone Air Temperature
------------------------------------
-
-The zone air heat balance is the primary mechanism for linking the loads calculation to the system simulation.  As such, the zone air temperature becomes the main interface variable.  Its role in the integration process was described previously (“Basis for the Zone and Air System Integration�).
diff --git a/doc/src/docs/EngineeringReference/09-BuildingSystemSimulation.md b/doc/src/docs/EngineeringReference/09-BuildingSystemSimulation.md
deleted file mode 100644
index 188932899ba..00000000000
--- a/doc/src/docs/EngineeringReference/09-BuildingSystemSimulation.md
+++ /dev/null
@@ -1,1409 +0,0 @@
-
-Building System Simulation System Manager / Processes
-=====================================================
-
-EnergyPlus uses a loop based HVAC system formulation.  An example of the dual duct VAV system is shown below.
-
-Air Loops
----------
-
-### Definition of Air Loop
-
-In EnergyPlus an air loop is a central forced air HVAC system. The term “loop� is used because in most cases some air is recirculated so that the air system forms a fluid loop. The air loop is just the “air side� of a full HVAC system.  The input objects related to these air loops begin “AirLoopHVAC.�
-
-For simulation purposes the air loop is divided into 2 parts: the primary air system (representing the supply side of the loop) and the zone equipment (representing the demand side of the loop). The primary air system includes supply and return fans, central heating and cooling coils, outside air economizer, and any other central conditioning equipment and controls. The zone equipment side of the loop contains the air terminal units as well as fan coils, baseboards, window air conditioners, and so forth. Supply and return plenums are also included on the zone equipment side of the loop.
-
-### Simulation Method
-
-Simulating a forced air system and its associated zones can be done in a number of ways. EnergyPlus uses algebraic energy and mass balance equations combined with steady state component models. When the zone air and the air system are modeled with algebraic equations (steady state) then – in cases with recirculated air – there will be one or more algebraic loops. In other words it is not possible to solve the equations directly; instead iterative methods are needed. Typically a humidity ratio and a mass flow rate will be variables involved in the iterative solution.
-
-In EnergyPlus the zone humidity ratios and temperatures are decoupled from the solution of the air system equations. The zone air is assigned heat and moisture storage capacities and the capacity effects are modeled by 1<sup>st</sup> order ordinary differential equations. During each system simulation time step new zone temperatures and humidities are predicted using past values. The zone temperatures and humidities are then held constant during the simulation of the air system (and the plant). Then the zone temperatures and humidity ratios are corrected using results from the system simulation. As a result the usual algebraic loops arising in steady state air system simulations are eliminated from the EnergyPlus system simulation. The zone temperatures, humidity ratios, and heating and cooling demands are known inputs to the system simulation.
-
-The need for iteration can be reintroduced by the need for system control. If system setpoints are fixed, externally determined, or lagged and control is local (sensor located at a component outlet, actuator at a component inlet) then iteration can be confined to the components and the overall air system equations can be solved directly. However these requirements are too restrictive to simulate real systems. System setpoints are held fixed during a system time step. But controller sensors are allowed to be remote from the location of the actuator. Consequently EnergyPlus uses iteration over the entire primary air system in order to converge the system controllers.
-
-### Component Models
-
-EnergyPlus component models are algorithmic with fixed inputs and outputs. They are embodied as Fortran90 subroutines within software modules. For each component several choices of inputs and outputs are possible. There is no one choice that will be most usable and efficient for all system configurations and control schemes. For reasons of consistency and comprehensibility the requirement was imposed that all EnergyPlus models be forward models. That is, the component inputs correspond to the inlet conditions and the outputs to the outlet conditions.  If another choice of inputs and outputs is needed it is obtained by numerical inversion of the forward model.
-
-### Iteration Scheme
-
-The primary air system simulation uses successive substitution starting at the return air inlet node and proceeding in the flow direction to the supply air outlet nodes. The iteration proceeds until an individual actuator-controller has converged (the sensed value matches the setpoint within the specified tolerance). The system controllers are simulated in sequence. During this sequence of iterative solutions the air mass flow rates are held constant. The controllers are converged by the method of interval halving. This method was chosen (rather than for instance Newton-Raphson) for its robustness.
-
-### Determination of Air Mass Flow Rates
-
-In most cases the air mass flow rate of the central air system is set by zone equipment downstream of the primary air system. The air terminal unit components with their built in dampers and controllers respond to the zone heating and cooling loads by setting air flow rates at their inlet nodes. These flow rates are passed back upstream to the primary air system, establishing the flow rates in the primary air system branches. These flow rates are held fixed while the primary air system is simulated.
-
-Air Loop Simulation
--------------------
-
-A complete simulation of each primary air system – zone equipment air loop is done in the following manner.
-
-* If this is the first simulation this system time-step, just call *ManageAirLoops* (simulates the primary air systems) and *ManageZoneEquipment* (simulates the zone equipment sets) once and quit. This initial pass is simulated with full design air flow rates and allows the zone equipment to set the flow rates for each zone that will meet the zone loads.
-
-* Otherwise loop over primary air systems and zone equipment sets until the temperatures, flow rates, enthalpies, humidity ratios etc. agree to within tolerance at each primary air system – zone equipment gap.
-
-```
-DO WHILE ((SimAirLoops .OR. SimZoneEquipment) .AND. (IterAir.LE.MaxAir) )
-  IF (SimAirLoops) THEN
-    CALL ManageAirLoops(FirstHVACIteration,SimAirLoops,SimZoneEquipment)
-    SimPlantDemandLoops = .TRUE
-    SimElecCircuits =.TRUE.
-  END IF
-
-  IF (SimZoneEquipment) THEN
-    CALL ResolveAirLoopFlowLimits(IterAir+1)
-    CALL ManageZoneEquipment(FirstHVACIteration,SimZoneEquipment,SimAirLoops)
-    SimPlantDemandLoops = .TRUE.
-    SimElecCircuits =.TRUE.
-  END IF
-
-  IterAir = IterAir + 1
-
-END DO
-
-CALL ResolveLockoutFlags(SimAirLoops)
-```
-
-
-The logical flags *SimAirLoops* and *SimZoneEquipment* are used to signal whether the primary air systems or the zone equipment sets need to be resimulated. These flags are set by the subroutine *UpdateHVACInterface* which is called  from within *ManageAirLoops* and *ManageZoneEquipment* at the end of each half-loop simulation. *UpdateHVACInterface* (when called from *ManageAirLoops*) passes the values at the outlet nodes of a primary air system on to the inlet nodes of the corresponding zone equipment half-loop and similarly (when called from *ManageZoneEquipment*) passes the values of the outlet nodes of a zone equipment half-loop on to the inlet nodes of its corresponding  primary air system. Each time *UpdateHVACInterface* is called it also checks whether the values at the half-loop outlet nodes are in agreement with the values at the downstream half-loop inlet nodes. If they are not it sets the simulate flag of the downstream half-loop to *true*. The values checked by *UpdateHVACInterface* and their tolerances are as follows.
-
-<table class="table table-striped">
-<tr>
-<th>Quantities</th>
-<th>Tolerances</th>
-</tr>
-<tr>
-<td>specific enthalpy [J/kg}</td>
-<td>10.0</td>
-</tr>
-<tr>
-<td>mass flow rate [kg/s]</td>
-<td>0.01</td>
-</tr>
-<tr>
-<td>humidity ratio [kg H<sub>2</sub>O / kg dry air]</td>
-<td>0.0001</td>
-</tr>
-<tr>
-<td>quality</td>
-<td>0.01</td>
-</tr>
-<tr>
-<td>air pressure [Pa]</td>
-<td>10.0</td>
-</tr>
-<tr>
-<td>temperature [C]</td>
-<td>0.01</td>
-</tr>
-<tr>
-<td>energy [J]</td>
-<td>10.0</td>
-</tr>
-
-</table>
-
-
-
-*ResolveAirLoopFlowLimits* is invoked to deal with zone equipment – primary air system flow mismatches. For instance the zone air terminal units (ATUs) may be asking for more air than the central fan can supply. In this case *ResolveAirLoopFlowLimits* takes the air flow that the fan can supply and apportions it among the ATUs in proportion to their design maximum air flow rates (*ResolveAirLoopFlowLimits* sets the <span>\({\dot m_{\max avail,node}}\)</span> at the entering node of each ATU in the system).
-
-At the end of the air loop simulation *ResolveLockoutFlags* is called. This subroutine checks if any air system component has requested that the economizer be locked out. If such a request has been made and if the economizer is active, *ResolveLockoutFlags* sets *SimAirLoops* to *true* and the *EconoLockout* flag to *true* to ensure that the air loop will be resimulated with the economizer forced off.
-
-Primary Air System Simulation
------------------------------
-
-When the EnergyPlus HVAC simulation manager needs to simulate the primary air system side of the air loop it calls *ManageAirLoops*, the primary air system simulation manager subroutine.
-
-Note that “air loop� is used inconsistently in the program: sometimes it means the full loop consisting of both supply & demand sides – primary air system and zone equipment; sometimes it means just the supply side – the primary air system.
-
-Like the other manager routines in EnergyPlus, *ManageAirLoops* has a very simple structure:
-
-Table 39.  ManageAirLoop Code
-
-
-```
-IF (GetInputFlag) THEN  !First time subroutine has been entered
-      CALL GetAirPathData ! Get air loop descriptions from input file
-      GetInputFlag=.false.
-  END IF
-
-    ! Initialize air loop related parameters
-  CALL InitAirLoops(FirstHVACIteration)
-
-    ! Call the AirLoop Simulation
-  IF (SysSizingCalc) THEN
-    CALL SizeAirLoops
-  ELSE
-    CALL SimAirLoops(FirstHVACIteration,SimZoneEquipment)
-  END IF
-
-  ! No Update
-
-    ! Report information at the Manage Air Loop Level
-  CALL ReportAirLoops
-```
-
-1.  If the user input data has not been input, get the data and store it in the air loop data structures.
-
-2.  Perform air loop initialization calculations:
-
-    a. at the beginning of the simulation (one time initializations);
-
-    b. at the start of each environment (design day or simulation run period);
- 
-    c.  before each air loop simulation.
-
-3. If automatic sizing of the loop flow rates is called for, do it.
-
-4. Otherwise perform a simulation of the air loop.
-
-### Input data
-
-The input data specifying an air loop consists of:
-
-1. the loop configuration;
-
-    a. Splitters, Mixers, and Branches;
-
-    b. Components on the Branches
-
-2. loop control;
-
-    a. Controllers;
-
-    b. System Availability Managers;
-
-3. connection to zone equipment;
-
-4. design flow rate.
-
-These objects and their data are described in the EnergyPlus *Input Output Reference* document. The utility routines used to get and check the data are described in the EnergyPlus *Guide for Module Developers*, section Input Services.
-
-### Initialization Calculations
-
-#### One Time Calculations
-
-##### Zones Served by System
-
-The main one time calculation involves figuring out what zones are served by each air loop. The EnergyPlus input does not explicitly describe which zones receive supply air from a given air loop. Instead that knowledge is embedded implicitly in the overall air loop – zone equipment network description. For sizing calculations it is important to have a data structure that explicitly shows which zones each air loop serves. For instance, the air loop design supply air flow rate is obtained by summing the design heating or cooling air flow rates of the zones connected to the air loop.
-
-For each air loop, the following calculation is performed.
-
-(1)  For each air loop outlet branch, the corresponding zone equipment inlet node is identified.
-
-(2)  This node number is compared to the inlet node of all AirLoopHVAC:SupplyPaths. When a match is found, the AirLoopHVAC:ZoneSplitter for this supply path is identified.
-
-(3)  The outlet nodes of the AirLoopHVAC:ZoneSplitter are compared to the cooling inlet nodes of all the zone ZoneHVAC:AirDistributionUnits. When a match is found this zone is identified as being served by cooling supply air from the air loop.
-
-(4)  Similarly the outlet nodes of the AirLoopHVAC:ZoneSplitter are compared with the heating inlet nodes of all ZoneHVAC:AirDistributionUnits. A match indicates that this zone is served by heating supply air from the air loop.
-
-(5)  The case where there is no AirLoopHVAC:ZoneSplitter for a AirLoopHVAC:SupplyPath must be handled. In this case the program looks for a match between the zone equipment inlet node and an ZoneHVAC:AirDistributionUnit heating or cooling inlet node. When a match is found that zone is identified as being served with heating or cooling supply air from the air loop.
-
-(6)  The list of cooled and heated zones are saved in the air loop data structure AirToZoneNodeInfo.
-
-##### Branch Sizing
-
-If this *not* an air loop sizing calculation, but is the first pass through the HVAC code in a normal simulation, loop over all the branches in all air loops and trigger the branch design air flow auto-sizing calculation. The actual calculation is described in the Sizing section of this document.
-
-#### Begin Environment Initializations
-
-For each air loop, loop over all the branches in the loop. Initialize each branch mass flow rate:
-
-<div>$${\dot m_{br,\max }} = {\rho_{std}} \cdot {\dot V_{br,\max }}$$</div>
-
-<div>$${\dot m_{br,\min }} = {\rho_{std}} \cdot {\dot V_{br,\min }}$$</div>
-
-where <span>\({\rho_{std}}\)</span> is the density of air at 20 degrees C, humidity ratio = 0, standard pressure.
-
-For each branch, loop over all the nodes on the branch and set the node data to the following values:
-
-<div>$${T_{node}} = {20^{\rm{o}}}C$$</div>
-
-<div>$${W_{node}} = {W_{oa}}$$</div>
-
-<div>$${h_{node}} = {\mathop{\rm PsyHFnTdbW}\nolimits} {\rm{(}}20.0,{W_{oa}}{\rm{)}}$$</div>
-
-<div>$${\dot m_{node}} = {\dot m_{br,\max }}$$</div>
-
-<div>$${\dot m_{\max ,node}} = {\dot m_{br,\max }}$$</div>
-
-<div>$${\dot m_{\max avail,node}} = {\dot m_{br,\max }}$$</div>
-
-<div>$${\dot m_{\min ,node}} = 0.0$$</div>
-
-<div>$${\dot m_{setpt,node}} = 0.0$$</div>
-
-<div>$${\dot m_{\min avail,node}} = 0.0$$</div>
-
-<div>$${p_{node}} = {p_{std,baro}}$$</div>
-
-<div>$$Q{u_{node}} = 0.0$$</div>
-
-where <span>\({W_{oa}}\)</span> is the humidity ratio of the outside air; <span>\({\rm{PsyHFnTdbW}}\)</span>is the EnergyPlus psychrometric function for enthalpy *h*, given temperature and humidity ratio; and *Qu* is quality.
-
-#### System Time Step Initializations
-
-For each branch in each air loop, loop over all the nodes on the branch and set <span>\({\dot m_{setpt,node}} = 0.0\)</span>; if it is the start of an HVAC solution sequence set <span>\({\dot m_{\max avail,node}} = {\dot m_{\max ,node}}\)</span>. Then set the mass flow rate setpoints for the air loop nodes.
-
-1)    On each air loop, loop over the outlet branches and find the loop outlet nodes. If it is the start of an HVAC solution sequence, set <span>\({\dot m_{setpt,outletnode}} = {\dot m_{outletbr,\max }}\)</span>. This will insure that during the first pass through the full loop that the mass flow rate will be at the maximum. Otherwise, set <span>\({\dot m_{setpt,outletnode}} = {\dot m_{zone{\rm{ }}eq{\rm{ }}inletnode}}\)</span>. This sets the air loop flow rate to the total zone requirement.
-
-2)    Pass the mass flow rate setpoint upstream to the start of the outlet branches; through the splitter, if one exists; and upstream to the beginning node of the splitter inlet branch.
-
-3)    Sum the total return air mass flow rate and save it in the AirLoopFlow data structure.
-
-4)    For each air loop, loop over the inlet nodes and, at the start of each HVAC solution sequence, set the entering node mass flow rate equal to the primary air system design mass flow rate (subject to it not being larger than the entering node mass flow rate setpoint).
-
-### Central air system simulation
-
-The subroutine *SimAirLoops* does the actual simulation the central air system equipment for all the air loops. The simulation of a full air loop (central equipment plus zone terminal units and equipment) requires the interaction of 2 managers: *ManageAirLoops* and *ManageZoneEquipment*. Thus a single call to *SimAirLoops* results in a simulation of all the central air system equipment, but this is one part of a larger iterative simulation of the full air loops involving the zone equipment as well.
-
-*SimAirLoops* accomplishes its task using a set of nested loops.
-
-* Loop over all of the central air systems (*Air Primary Loops*).
-
-* For each air system, make 1 or 2 simulation passes
-
-* Loop over each controller in the *Air Primary Loop*
-
-* For each controller, repeat the simulation of all the *Air Primary Loop* components until the controller has converged
-
-* Loop over each branch in the *Air Primary Loop*
-
-* On each branch, simulate in sequence each component
-
-During and at the end of each loop some tests are performed.
-
-At the end of the first pass of loop 2, a decision is made on whether a second pass is needed. The first pass has been performed assuming that there is a mass flow balance in the central air system simulation. This is usually the case. A call to *ResolveSysFlow* checks the mass balance and imposes a mass balance if there is not a balance. The lack of a system mass balance requires a resimulation of the central air system: i.e., a second pass in loop 2.
-
-In loop 3 a call to *ManageControllers* simulates controller action and checks for controller convergence. If convergence is achieved loop 3 is exited.
-
-After all the controllers on a loop are converged,  steps 5 & 6 are repeated one more time to ensure all the components on the loop have final values.
-
-At the end of the primary air system simulation a call to *UpdateHVACInterface* passes the primary air system outlet node data to the zone equipment inlet nodes. If the data across the supply side – demand side gap doesn’t match to within a preset tolerance, the flag *SimZoneEquipment* is set to *true* to ensure that the zone equipment side gets resimulated. Finally a flag indicating whether the economizer is active is set. This flag is used at a higher level to decide whether the primary air system needs to be resimulated if an HVAC component is calling for economizer lockout.
-
-Outdoor Air System
-------------------
-
-The AirLoopHVAC:OutdoorAirSystem is a subsystem of the primary air system (object AirLoopHVAC). To the primary air system it appears to be a single component. Within the subsystem are components and controllers very much like the primary air system. The purpose of the outside air system is to simulate the splitting of the return air into relief and recirculated air; mix the recirculated and outside air to obtain the mixed air (all accomplished by the OutdoorAir:Mixer); simulate the components in the outside air stream; control the components and outside air flow rate (economizer control). The outside air system differs from the primary air system in that it is not described in terms of splitters, mixers, and branches. Instead the components are simply listed in simulation order in an AirLoopHVAC:OutdoorAirSystem:EquipmentList input object. The components other than the OutdoorAir:Mixer are assumed to be in the outside air stream. The connectivity is defined by upstream component’s outlet node = downstream component’s inlet node. The OutdoorAir:Mixer should be the first component in the AirLoopHVAC:OutdoorAirSystem:EquipmentList object.
-
-### Simulation
-
-The data for and simulation of the outside air system are contained in the MixedAir module. This includes the data and simulation of the OutdoorAir:Mixer and the Controller:OutdoorAir. The simulation of the outside air system is straightforward.
-
-* All controllers other than Controller:OutdoorAir are moved up to the primary air system level, where they are simulated with the primary air system controllers.
-
-* The Controller:OutdoorAir is simulated.
-
-* The compnents contained in the outside air system are simulated in the order of their input in the AirLoopHVAC:OutdoorAirSystem:EquipmentList.
-
-Outdoor Air Mixer
------------------
-
-The OutdoorAir:Mixer is the fundamental component of the outside air system. There should always be one OutdoorAir:Mixer in an AirLoopHVAC:OutdoorAirSystem. The outside air mixer splits the primary air system (AirLoopHVAC) return air into relief and recirculated air streams. Then it mixes the outside air stream with the recirculated air stream to obtain the mixed air stream. The outdoor air mixer has 2 inlet flow nodes: the return air node and the outside air node. It has 2 outlet flow nodes: the relief air node and the mixed air node.
-
-### Simulation
-
-Given the air mass flow rates and conditions (humidity ratio, specific enthalpy) at the return air node, relief air node, and outside air node, the simulation uses mass and energy balance to calculate the air mass flow rate, humidity ratio, and specific enthalpy at the mixed air node. The mixed air temperature is calculated from the mixed air humidity ratio and specific enthalpy using the EnergyPlus psychrometric routine *PsyTdbFnHW*.
-
-Zone Equipment Simulation
--------------------------
-
-When the EnergyPlus HVAC simulation manager needs to simulate the zone equipment side of the air loop it calls *ManageZoneEquipment*, the zone equipment simulation manager subroutine. Like the other managers, *ManageZoneEquipment* has a very simple structure:
-
-```
-        IF (GetInputFlag) THEN
-          CALL GetZoneEquipment
-          GetInputFlag = .FALSE.
-        END IF
-
-        CALL InitZoneEquipment(FirstHVACIteration)
-
-        IF (ZoneSizingCalc) THEN
-          CALL SizeZoneEquipment
-        ELSE
-          CALL SimZoneEquipment(FirstHVACIteration, SimAir)
-        END IF
-
-        CALL RecordZoneEquipment(SimAir)
-
-        CALL ReportZoneEquipment
-
-        SimZone = .False.
-
-        RETURN
-```
-1. If the user input data has not been input, get the data and store it in the zone equipment data structures
-
-2. Perform zone equipment initialization calculations.
-
-3. If calculation of the design zone air flow rates and loads needs to be done, do it. The results of this calculation are stored in the zone sizing data structures and used by the component automatic sizing algorithms and the central system sizing calculations.
-
-4. Otherwise simulate all of the zone equipment.
-
-5. Transfer the zone equipment outlet node data to the inlet nodes of the primary air systems and check for convergence (done in RecordZoneEquipment by calling UpdateHVACInterface).
-
-### Input data
-
-The input specifying a set of zone equipment consists of:
-
-1. the ZoneHVAC:EquipmentConnections object data;
-
-    a. the zone connection to the air loop – air inlet nodes, exhaust nodes, outlet node, zone node;
-
-    b. the components serving each zone – air terminal units, fan coils etc.;
-
-2. zone supply air path data;
-
-    a. zone splitters and supply plenums;
-
-3. zone return air path data;
-
-    a. zone mixer and return plenums;
-
-### Initialization Calculations
-
-#### One Time Calculations
-
-There are no one time calculations for zone equipment
-
-#### Begin Environment Initializations
-
-For each controlled zone initialize the zone inlet, exhaust and zone nodes to standard conditions. Namely:
-
-<div>$${T_{node}} = {20^{\rm{o}}}C$$</div>
-
-<div>$${W_{node}} = {W_{oa}}$$</div>
-
-<div>$${h_{node}} = {\mathop{\rm PsyHFnTdbW}\nolimits} {\rm{(}}20.0,{W_{oa}}{\rm{)}}$$</div>
-
-<div>$${\dot m_{node}} = 0$$</div>
-
-<div>$$Q{u_{node}} = 1.0$$</div>
-
-<div>$${p_{node}} = {p_{oa}}$$</div>
-
-where *W<sub>oa</sub>* is the humidity of the outside air; <span>\({\rm{PsyHFnTdbW}}\)</span>is the EnergyPlus psychrometric function for enthalpy *h*, given temperature and humidity ratio; *p<sub>oa</sub>* is the pressure of the outside air; and *Qu* is quality.
-
-#### System Time Step Initializations
-
-For each controlled zone, set the exhaust nodes conditions equal to the zone node conditions; except set the exhaust nodes mass flow rate and min and max available mass flow rates to zero.
-
-### Simulation
-
-The subroutine *SimZoneEquipment* does the actual simulation of all the zone equipment. Note that this includes components that are part of the demand side of an air loop as well as components that are independent of any air loop.
-
-For zone equipment components that are part of the demand side of an air loop the simulation sequence is effectively performed in the direction of the air flow. First the supply air plenums and zone splitters are simulated in their input order. Then the air terminal units are simulated followed by the zone return plenums and zone mixer. Each air terminal unit sets its inlet node to the air mass flow rate required to satisfy its zone load. These mass flow rates are then passed back upstream to the air loop demand-side inlet nodes at the end of each zone equipment simulation sequence. These demand-side inlet mass flow rates are then used as mass flow rate setpoints in the air loop supply-side simulation.
-
-If multiple air-conditioning components are attached to a zone, the components are simulated in the order specified by the user assigned priority given in the ZoneHVAC:EquipmentList object.
-
-For each full air loop there should be 1 supply air path for each primary air system outlet (i.e. 1 for single duct systems,  2 for dual duct systems). For each full air loop there should be one return air path. The supply air paths consist of any combination of zone splitters and zone supply air plenums as long as it forms a tree structure with the supply air path inlet node the root and the air terminal unit inlet nodes as the leaves. The return air path configuration is limited to a single mixer; there may be multiple return plenums.
-
-1. Loop over all the supply air paths.
-
-    a. Loop over each component (supply plenum or zone splitter) on the supply air path and simulate each component. The components are simulated in input order.
-
-2. Loop over all the controlled zones.
-
-    a. Set the required system output.
-
-    b. Loop over the components serving the zone in the user prioritized order.
-
-        i. Simulate each component.
-
-        ii. Increment the required system output.
-
-3. Loop over all the supply air paths
-
-    a. Loop over the components on each supply air path in reverse input order. This reverse order simulation passes the air terminal units inlet mass flows back upstream to the return air path inlet node.
-
-    b. Check to see if the supply air path inlet node mass flow rate has changed. If it has set the *SimAir* flag to *true*. This signals the HVAC manager that the supply-side of the air loop needs to be resimulated.
-
-4. Calculate the zone air flow mass balance – the zone inlet and exhaust mass flow rates are summed and the zone node and return air node mass flow rates are determined by a mass balance for each zone.
-
-5. Calculate the conditions at each zone return air node. Here energy not included in the zone energy balance such as light-heat-to-return-air is added to the return nodes of the controlled zones.
-
-6. Loop over all of the return air paths.
-
-    a. Loop over each component (return plenum or zone mixer) on the return air path and simulate each component.
-
-This completes a single simulation sequence of all the zone equipment.
-
-Air Path Components
--------------------
-
-### Overview
-
-The air path from the outlet of an AirLoopHVAC (the supply side of a full air loop / central air system) to the zone air distribution units (terminal units) is specified in a AirLoopHVAC:SupplyPath. The AirLoopHVAC:SupplyPath consists of AirLoopHVAC:ZoneSplitters and AirLoopHVAC:SupplyPlenums hooked together outlets to inlet.
-
-The air path from the zone return nodes to the AirLoopHVAC inlet node is described in a AirLoopHVAC:ReturnPath object. The  AirLoopHVAC:ReturnPath consists of AirLoopHVAC:ZoneMixers and AirLoopHVAC:ReturnPlenums hooked together outlet to inlets.
-
-### Zone Supply Air Path
-
-The AirLoopHVAC:SupplyPaths are simulated just before the zone equipment is simulated and just after the zone equipment is simulated (in module ZoneEquipmentManager, subroutine SimZoneEquipment). In both cases the simulation consists of looping over all the AirLoopHVAC:SupplyPaths and simulating each component (AirLoopHVAC:ZoneSplitter or AirLoopHVAC:SupplyPlenum) in the path. For the “just before� simulation a flag *FirstCall* is set to *True* which tells the zone splitter and zone supply plenum models to do a downstream simulation (pass component inlet conditions to component outlets, except for air mass flow rate). For the “just after� simulation, *FirstCall* = *False*, which tells the components to do an upstream simulation (set the component inlet air mass flow rate to the sum of the component outlet air mass flow rates, do nothing with other properties).
-
-### Zone Splitter
-
-The AirLoopHVAC:ZoneSplitter divides an inlet air stream into multiple outlet streams. Its data and simulation model are encapsulated in the module *SplitterComponent*. There are two simulation modes. If *SimAirLoopSplitter* is called with input parameter *FirstCall* = *True* then the splitter is simulated in downstream mode. The outlet air streams’ humidity ratio, pressure, enthalpy, and temperature are set to the conditions on the inlet air stream.  If *SimAirLoopSplitter* is called with input parameter *FirstCall* = *False*, the splitter is simulated in the upstream mode. In this case the inlet air stream air mass flow rate is set to the sum of the outlet air mass flow rates. The same calculation is done for the maximum available and minimum available air flow rates.
-
-### Zone Supply Plenum
-
-The AirLoopHVAC:SupplyPlenum acts analogously to the AirLoopHVAC:ZoneSplitter. The only difference is that the AirLoopHVAC:SupplyPlenum is associated with a Zone for which it sets the supply air flow rate and from which it gets its outlet air conditions. The AirLoopHVAC:SupplyPlenum divides an inlet air stream into multiple outlet streams. Its data and simulation model are encapsulated in the module *ZonePlenum*. There are two simulation modes. If *SimAirZonePlenum* is called with input parameter *FirstCall* = *True* then the plenum is simulated in downstream mode. The outlet air streams’ humidity ratio, pressure, enthalpy, and temperature are set to the zone conditions.  If *SimAirZonePlenum* is called with input parameter *FirstCall* = *False*, the plenum is simulated in the upstream mode. In this case the inlet air stream air mass flow rate is set to the sum of the outlet air mass flow rates. The same calculation is done for the maximum available and minimum available air flow rates.
-
-### Zone Return Air Path
-
-The AirLoopHVAC:ReturnPaths are simulated after all the zone equipment is simulated (in module ZoneEquipmentManager, subroutine SimZoneEquipment). The simulation is accomplished by a call to *SimReturnAirPath* (in module *ReturnAirPathManager*). The simulation just consists of looping over all the AirLoopHVAC:ReturnPaths and simulating the components (AirLoopHVAC:ZoneMixer or AirLoopHVAC:ReturnPlenum) in each path.
-
-### Zone Mixer
-
-The AirLoopHVAC:ZoneMixer combines multiple inlet air streams into a single outlet air stream. Its data and simulation model are encapsulated in the module *MixerComponent*. The following mass and energy balance equations are used.
-
-<div>$${\dot m_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}} $$</div>
-
-<div>$${\dot m_{air,out}}\cdot {W_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}} \cdot {W_{air,in,i}}$$</div>
-
-<div>$${\dot m_{air,out}}\cdot {h_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}} \cdot {h_{air,in,i}}$$</div>
-
-<div>$${\dot m_{air,out}}\cdot {P_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}} \cdot {P_{air,in,i}}$$</div>
-
-<div>$${T_{air,out}} = PsyTdbFnHW({h_{air,out}},{W_{air,out}})$$</div>
-
-Where <span>\(\dot m\)</span>is air mass flow rate, *W* is humidity ratio, *h* is specific enthalpy, *P* is pressure, and *T* is temperature. *PsyTdbFnHW* is the EnergyPlus psychrometric function for drybulb temperature as a function of enthalpy and humidity ratio. The air mass flow rate calculation is also done for the maximum and minimum available mass flow rates.
-
-### Zone Return Plenum
-
-The AirLoopHVAC:ReturnPlenum acts analogously to the AirLoopHVAC:ZoneMixer. The only difference is that the AirLoopHVAC:ReturnPlenum is associated with a Zone for which it sets the supply air flow rate and from which it gets its outlet air conditions. The AirLoopHVAC:ReturnPlenum combines multiple inlet air streams into a single outlet air stream. Its data and simulation model are encapsulated in the module *ZonePlenum*. The outlet air mass flow rate is obtained from
-
-<div>$${\dot m_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}} $$</div>
-
-The outlet air temperature, enthalpy, humidity ratio and pressure are set to the zone conditions.
-
-In addition to its normal function of acting as an air stream mixer, the return plenum can have 2 types of special connection to upstream air terminal units.
-
-(1) The user can model the effects of duct leakage in VAV single duct systems using the Simplified Duct Leakage Model (see ZoneHVAC:AirDistributionUnit for how to set up this model). After the normal outlet air flow calculation is completed as above, the calculation loops over the air distribution units connected to the zones that feed air to the plenum and adds in to the outlet air mass flow rate the leakage air flow rates from the upstream leaks defined in the ZoneHVAC:AirDistributionUnit inputs. This connection between the leaks and the plenum is not explicit: no extra nodes are defined in the return plenum or in the terminal unit.
-
-(2) The user can model secondary (recirculated) air drawn from the plenum into a fan powered induction unit (AirTerminal:SingleDuct:SeriesPIU:Reheat or AirTerminal:SingleDuct:ParallelPIU:Reheat). In this case the connection is explicit: extra outlet nodes are defined in the return plenum which act as the secondary air inlet nodes for the terminal units. The recirculated air flow rates are set by the terminal units. The outlet return air is then:
-
-<div>$${\dot m_{air,out}} = \sum\limits_{i = 1,n} {{{\dot m}_{air,in,i}}}  - \sum\limits_{j = 1,m}^{} {{{\dot m}_{air,recirc,j}}} $$</div>
-
-Plant Load Profile
-------------------
-
-The LoadProfile:Plant object is used to simulate a scheduled demand profile. This can be useful when the building loads are already known. Demanded load and flow rate are schedules specified in the object definition. The load profile can specify heating and cooling loads. Cooling loads are entered as negative numbers. The actual load met is dependent on the performance of the supply loop components.
-
-The LoadProfile:Plant object must be connected on the demand side of the plant loop. If desired, multiple LoadProfile:Plant objects can be combined in series and/or parallel.
-
-### Calculation Model
-
-The LoadProfile:Plant object calculates the outlet water temperature based on the inlet water temperature from the plant loop and user inputs for the scheduled plant load and the requested flow rate.  The calculation can be expressed with the equation:
-
-<div>$${T_{out}} = {T_{in}} - \frac{{{Q_{load}}}}{{\dot m{c_p}}}$$</div>
-
-where
-
-<span>\({T_{out}}\)</span> = the outlet water temperature
-
-<span>\({T_{in}}\)</span> = the inlet water temperature
-
-<span>\({Q_{load}}\)</span> = the scheduled plant load
-
-<span>\(\dot m\)</span> = the water mass flow rate
-
-<span>\({c_p}\)</span> = the specific heat of water
-
-The user requested flow rate is not always available from the plant loop.  The actual flow rate used in the calculation is the lesser of the user requested value and the plant available value.
-
-Note that the LoadProfile:Plant object can still request and receive flow even if the scheduled plant load is zero.  In this case the outlet temperature will be the same as the inlet temperature.  This allows users to drive the plant loop flow without necessarily affecting the loop temperature.
-
-For reporting purposes the energy consumption of the object is calculated using the equation:
-
-<div>$$E = {Q_{load}}\Delta t$$</div>
-
-where
-
-<span>\(E\)</span> = the energy consumption
-
-<span>\({Q_{load}}\)</span> = the scheduled plant load
-
-<span>\(\Delta t\)</span> = the time step interval
-
-Plant/Condenser Loops
----------------------
-
-### Integration of System and Plant
-
-In order to integrate the air handling system simulation with the zones simulation, methods were developed to model the system air loop and its interactions with the zones due to temperature controls and the relative difference between the zone and supply air temperatures. A similar situation is encountered when integrating the central plant simulation. Typically, the central plant interacts with the systems via a fluid loop between the plant components and heat exchangers, called either heating or cooling coils. In EnergyPlus the performance of the air systems and plant are interdependent because the simulations are combined. The plant outputs must match the system inputs and vice versa. That is, the temperature of the chilled water leaving the plant must equal the temperature of the water entering the coils, and the chilled water flow rate must satisfy mass continuity. In addition, coil controls are usually necessary to ensure that the values of chilled water flow variables entering and leaving the coil remain in a reasonable range. Plants can also interact with each other so that the operation of a chilled water loop and chiller will affect the operation of a condenser water loop.
-
-### Current Primary System Modeling Methodology
-
-There are two main types of loops within the HVAC simulation in EnergyPlus: an air loop and a plant loop. The air loop is assumed to use air as the transport medium as part of an air handling system while the plant loops use a liquid fluid of the user’s choosing (typically water).  Condenser loops are a special case of plant loop that are for heat rejection and are distinguished by slightily different control options and applicable equipment types.  A user may have any number of each type of loop in a particular input file. There are no explicit limits on the number of loops within the program—the user is only limited by computer hardware. Execution speed will naturally vary with the complexity of the input file.
-
-Plant loops are further divided into “half-loops� or “semi-loops� for organizational clarity and simulation logistics (see Figure “Connections between the Main HVAC Simulation Loops and Half-Loops�). These sub-loops, or half-loop sides, are matched pairs that consist of half of a main plant loop. Plant loops are broken into supply and demand sides. The plant demand side half-loop contains equipment that places a load on the primary equipment. This might include coils, baseboards, radiant systems, etc. The load is met by primary equipment such as chillers or boilers on the supply side half-loop. Each supply side half-loop must be connected to a demand side half-loop and vice versa. A similar breakdown is present on condenser loops where the demand side includes the water side of chiller’s condensers while the supply side includes condenser equipment such as cooling towers.
-
-![](media/image1957.svg.png)
-
-Figure 120. Connections between the Main HVAC Simulation Loops and Half-Loops.
-
-The breakdown into two half-loops allows for better handling and control of information and simulation flow throughout the program. Direct connections between the half-loops of the air, plant, and condenser loops are enhanced by components with connections between the various main loop types. For example, coils (heating or cooling) are in reality heat exchangers with an air and a water or refrigerant side. The air side of the coil is handled within the air loop where the control of the device is also maintained. The fluid side of the coil is handled within the plant demand side, which passes the energy requirements of the coil on to the plant supply side. All loops are simulated together by successively modeling each half-loop in a particulary calling order. Overall iterations ensure that the results for the current time step are balanced and updated information has been passed to both sides of the sub-loops as well as across to the other side of air loop connections such as coils.
-
-The plant equipment on a half-loop is described by a set of branches for that half-loop.  Components can be arranged on a branch in series, and branches can be placed in parallel, with some restrictions. Figure “Branch Layout for Individual Plant Half-Loops� provides an overview of the intended branch layout for each plant half-loop. Branches are individual legs within the loop structure. Thus, the segment between point A and point B is defined as a branch, as is the section between points E and F. There may be multiple sections (C1 to D1 through Cn to Dn) in between the splitter and mixer.
-
-Each half-loop may only have one splitter and one mixer. Thus, equipment may be in parallel between the mixer and splitter, however, within any single branch, there can only be components in series and not in parallel. The topology rules for individual half-loops allow a reasonable amount of flexibility without requiring a complicated solver routine to determine the actual flow and temperature conditions. Note that since plant supply and demand are broken up into two separate half-loops, chillers or boilers may be in parallel to each other in the supply side and coils may be in parallel to each other on the demand side. Thus, the restriction of only a single splitter and mixer on a particular half-loop does not unduly limit the allowable configurations. In some cases a single branch can be used to define an entire half-loop, but in general a half-loop should have a splitter and a mixer even if all equipment on the sub-loop is simply in series.
-
-In addition, to avoid the need for overly complex solver routines, there are some restrictions on the placement of pumps within a particular half-loop. There are two general types of pumps, loop pumps and branch pumps. A pump that is the first component on the first branch (between A and B) is termed a “loop pump� while any pump in the parallel section (between Ci and Di) is termed a “branch pump�.   The simplest and most common arrangement is to have one loop pump on the supply side inlet.  In plant demand half-loops pumps can be placed only in the inlet branch. This will allow simulation of primary-secondary systems. For more information on pumps and pump placement rules, see the section on PipingSystem:Underground Simulation Pumps in this document.
-
-![](media/image1958.svg.png)
-
-Figure 121. Branch Layout for Individual Plant Half-Loops
-
-Essentially, each branch is made up of one or more components linked together in series. The branch has system nodes that store properties at a location on the loop (temperature, enthalpy, flow rate, etc.) at the beginning and end of the branch as well as between components. Components on the branch take the conditions of the node at their inlet and use that information as well as overall control information to simulate the component and write the outlet data to the node following the component. This information is then used either by the next component on the branch or establishes the outlet conditions for the branch.
-
-Although the plant model in EnergyPlus is quite flexible, in most cases the topology of the plant system in the model will be somewhat different from the topology of the actual plant system in a building.  EnergyPlus is focused on modeling building energy performance over long periods of time and is not intended as a completely flexible system that can directly model any actual plant system with its full complexity and exact layout.  Given the design of an actual complex plant system, the modeler will typically need to develop a simpler system that conforms to EnergyPlus’s capabilities and strives to capture the issues important for energy consumption modeling.  Just like complex geometry should be simplified into thermal zones for energy models, complex plants should to be simplified into sets of pairs of closed half-loops with the allowed branch topologies.
-
-### Plant Manager
-
-#### Plant Half-Loop Calling Order
-
-Because there can be multiple plant loops in a model that depend on each other, one job of the plant manager is to determine an appropriate calling order for the half-loops.  The intial starting calling order (and the order always used prior to EnergyPlus Version 7) is as follows:
-
-1.    Call all the demand side half-loops of the plant loops (in input object order)
-
-2.    Call all the supply side half-loops of plant loops (in input object order)
-
-3.    Call all the demand side half-loops of condenser loops (in input object order)
-
-4.    Call all the supply side half-loops of the condenser loops (in input object order).
-
-This initial calling order is then revised during a setup phase of program execution when the plant component models are iteratively read in, initialized and sized.  The algorithm is based on information provided by those component models that connect loops together.  The components register that two loop-sides are connected and declare which one places demands on the other.  If a half loop is connected and places demands on anther loop, then the calling order for the independent demanding loop is placed just ahead of the dependent loaded half-loop.  For example a water cooled chiller component model reports that the supply side of the chilled water loop is connected to the demand side of the condenser loop and that the chilled water loop places demands on the condenser loop.  The plant manger algorithm is iterative and repeatedly calls all of the half loops a total of four times.  After this setup phase, the calling order is fixed for the rest of the simulation.
-
-### Plant Flow Resolver
-
-#### Overview of the Plant Flow Resolver Concept
-
-An important aspect of the solution procedure within plant loops is the method used to solve for the fluid flow rates throughout the various half-loops. This involves making the supply side meet a particular load and flow situation based on the simulation of the demand side loops. Load distribution is an issue that must be addressed as well as how flow rates are adjusted and temperatures are updated. These issues are discussed in the next several subsections, and the algorithms described are important to how the plant simulation functions.
-
-In the first step, the plant loop manager calls the appropriate module to simulate (in flow order) all of the components on each branch of the loop except for splitters and mixers. In this step, each component would set the conditions at the outlet node including temperature, flow rate, maximum allowed (design) flow rate, minimum allowed (design) flow rate, maximum available flow rate, and minimum available flow rate. This would be based purely on the component’s own control scheme and thus each component would be free to request as much (or as little) flow as desired.
-
-In the second step, the loop manager would resolve the flow at all nodes and through all branches of the local loop. The components are then simulated with the corrected flows. For this iteration, the flow resolver sets the flow rate through each loop component.
-
-#### Overall Loop Flow Rate
-
-The plant models determine an overall fluid flow rate for each loop based on the dynamic requests and needs of the components on the loop.  The flow resolver examines the requests and needs of each half-loop and chooses an overall flow rate.  As individual plant components are modeled, they register their requests for fluid flow which are stored on the inlet node (variable called MassFlowRateRequest).   These requests for flow are used for two purposes, overall loop flows and resolution of parallel flows inside a splitter/mixer.  For determining the overall loop flow request, the requests by individual components are further qualified into three categories based on the nature of the device.
-
-1.    Need flow and turns loop on
-
-2.    Need flow if loop is already on
-
-3.    Take what ever flow they get.
-
-The loop will only run at all if there are flow requests of type 1.  If there are flow requests of type 2, they will not turn on the loop but may affect the overall flow rate if it is already on because of some non-zero type 1 requests.  Flow requests of type 3 will not affect the overall loop flow rate.  These classifications are hard coded and cannot be altered by the user.
-
-#### Pump Control for Plant and Condenser Loops.
-
-The pump is quite simply the component that drives the flow (also see PipingSystem:Underground Simulation Pumps). . How it reacts depends on several different conditions. In total, there are three different decision variables, two of which are defined by user input. These three deciding factors are whether the pump is constant or variable speed, whether the pump operation is continuous or intermittent, and whether or not there is a request for overall loop flow. After the overall loop flow request has been determined the simulation knows what the loop would like to do.  The next thing it does is simulation all the loop pumps to see what the pumps can actually provide. Then the overall loop flow is bounded by the minimum and maximum that the loop pumps can provide at that time. The operation of a constant speed pump is fairly straightforward. If the user designates a constant speed pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump is constant speed and operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop.
-
-A variable speed pump is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump is operating intermittently, then the pump can shutdown. For any other condition such as the loop having a load and the pump is operating intermittently or the pump is continuously operating (regardless of the loading condition), the pump will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump is running, it will try to meet the flow request for the overall loop.
-
-In many cases, the first estimate of flow requested by the demand side tends to be fairly accurate and the flow rate does not vary in subsequent iterations. However, because there is the possibility that the coils or some other component might request more flow in future iterations during the same time step, the program must not only set flow rates but also maintain a record of the current maximum and minimum flow rate limits. This information is important not only to the pump itself but also to other pieces of equipment which may control their flow rates and thus require knowledge of the limits within which they may work. In general, the decisions on what to set the maximum and minimum flow rates is directly related to the type of pump (constant or variable speed). For constant speed pumps, the maximum and minimum flow rate values are the same and thus if the flow requested does not match this, the other components must either deal with the flow or a bypass branch must be available to handle the excess flow. For variable speed pumps, the maximum and minimum flow rates are set by the user-defined limits.
-
-#### Plant/Condenser Supply Side
-
-Component models, such as boilers, chillers, condensers and cooling towers are simulated on the supply side of the plant and condenser loops. In order to allow specification of realistic configurations, the plant loop managers were designed to support parallel-serial connection of component models on the loop. In addition, loop managers were designed to support both semi-deterministic models (e.g. the parameter estimation models of the ASHRAE Primary Toolkit [Pedersen 2001]) and “demand based� models (e.g. the performance map models of BLAST and DOE2.1E). As a result, the loop manager must be able to simulate models that require the mass flow rate as an input and models that calculate the mass flow rate as an output—sometimes in the context of a single loop configuration.
-
-In order to achieve these design criteria without resorting to a pressure based flow network solver in the HVAC portion of the code, a rules-based “flow resolver� was developed for the EnergyPlus plant manager. The flow resolver is based on the following assumptions and limitations:
-
-* Each loop is only allowed to have a single splitter and a single mixer
-
-* Due to the fact that there can only be one splitter and one mixer on a given loop, it follows logically that there can be at most one bypass on each loop side
-
-* No other components may be in series with a bypass, i.e., a branch that contains a bypass may have no other equipment on that branch
-
-* Equipment may be in parallel only between the splitter and mixer components of a loop
-
-* Equipment may be hooked together in series in each branch of the loop
-
-* Flow rates on individual branches will be controlled using maximum and minimum available flow rate limits
-
-The flow resolver employs a simple predictor-corrector algorithm to enforce mass continuity across the plant loop splitter as shown in the following figure.
-
-![](media/image1959.png)
-
-Figure 122. Plant/Condenser Supply Side Solution Scheme.
-
-As previously discussed, the pump establishes the total loop mass flow rate by setting the flow in the first supply side branch. In the second step, a predictor algorithm calls to simulate each piece of equipment on the loop and they update their mass flow rate requests based on the current flow rates, temperatures and load dispatch requests. The loop manager calls the appropriate module to simulate (in flow order) all of the components on each branch of the loop except for splitters and mixers. In this step, each component sets the conditions at its outlet node including temperature and sets component flows on the inlet node.   Each component and branch is classified for their type of flow control.  Prior to version 7 this was input by the user where branch objects were tagged in the user input file as an ACTIVE, SERIESACTIVE, PASSIVE or BYPASS type of model.  As of version 7 this has been hard coded and the input is no longer used.  An ACTIVE flow control type describes a demand based plant model that calculates mass flow rate as an output. An ACTIVE component when OFF will shut down the whole branch irrespective of the type of other components on the branch. A SERIESACTIVE branch is like an ACTIVE component except that there are more than one ACTIVE components on the branch so that two components requests may be at odds with each other and so it might not shut down the whole branch when the component is OFF. The flow resolution algorithm is same for both ACTIVE and SERIESACTIVE components and in the rest of the document description of one type will fit the other type too. A PASSIVE type describes a semi-deterministic model that is simulated with the mass flow rate as an input. The BYPASS type designates a loop bypass.
-
-The predictor algorithm first establishes the desired flow rate of each branch by searching for ACTIVE components on the branch. The first ACTIVE component in simulation order sets the desired branch flow. Branches with only PASSIVE components require a flow rate between the minimum and maximum allowable branch flow. Branches with a BYPASS component have a branch flow only when all other branches combined cannot handle the entire loop flow.
-
-The loop flow resolver  makes any necessary “corrections� to the requested branch flows in order to enforce overall continuity on the loop. If mass conservation allows all ACTIVE branches to be satisfied, then the remaining flow is divided between the PASSIVE branches and as a last resort, the BYPASS. If there is insufficient flow to meet the branch demand, ACTIVE branch requests are met first in the order that the branches appear in the branch list in the input file.
-
-The flow rate is resolved first for each individual branch. For every branch, the program cycles through each node on the branch and determines what the flow requests and flow limits are. The most restrictive flow constraints are assumed to be valid for the entire branch regardless of component type. Active components are given highest priority for requesting a particular flow rate. If there is more than one active component on a particular branch, then it is assumed that the active component on the branch with the highest flow request dictates the flow request for the entire branch.
-
-Once all of the branches have set their flow rates and constraints, the splitter and mixer must resolve the various flow requests. The mixer and any branch following the mixer is passive. Thus, all of the flow control happens at the splitter. The splitter first attempts to sum the maximum and minimum constraints from all of the active branches coming out of the device and compares those to the constraints that are valid for the branch leading into the splitter. When there is a mismatch between the outlet constraints and the inlet constraints, the simulation will defer to the inlet constraints due to the fact that the pump is in reality controlling flow on the loop. Since the constraints of the pump would be passed across to the demand side from the supply side, an assumption is made that the coils or other demand side components must live within the bounds of the pump.
-
-Once the flow has been resolved at the splitter, the branch flow rates and constraints between the splitter and mixer can be adjusted, if necessary. In some cases, this will be mandatory to maintain a mass balance at the splitter. When the flow rate coming out of the splitter does not match the active branch requests, individual branch flow rates must be adjusted to provide for the extra flow or the “flow deficit�. When there is extra flow, the excess flow is sent through any bypass branch first and then is sent to passive branches in reverse order of their appearance in the splitter outlet list. When all of these branches have been exhausted and there is still excess flow, flow will be increased to the active branches, also in reverse order. The reverse order guarantees that the branch appearing first has the highest priority to receive the flow rate it has requested.
-
-if there is not enough flow to meet all active branch requests (i.e., a “flow deficit�), then the flow rates through the bypass and passive branches are set to zero. The flow rates through the active branches will then be decreased in reverse order until the splitter outlet flow rate matches the available flow at the splitter inlet. For a plant loop flow deficit, the bypass and passive branch flows are also set to zero, and flow rates for each active branch are calculated as follows:
-
-<div>$${\dot m_{br}} = \frac{{{{\dot m}_{br\_request}}}}{{{{\dot m}_{tot\_request}}}}*{\dot m_{tot\_available}}$$</div>
-
-where:
-
-<div>$$
-  \begin{array}{rl}
-    \dot m_{br} &= \rm{ final resolved branch flow rate} \\
-    \dot m_{br\_request} &= \rm{ requested branch flow rate } \\
-    \dot m_{tot\_request} &= \rm{ total loop mass flow rate request} \\
-    \dot m_{tot\_available} &= \rm{ total loop mass flow rate available}
-  \end{array}
-$$</div>
-
-It is also necessary to monitor the flow constraints at the branches and components since once the flow rates are changed, the components must be resimulated by the controlling loop (air loop, zone equipment, or plant supply side). The controllers for these components must know if the constraints have been modified so that the simulation does not toggle between a component requesting a flow that the pump cannot meet and the pump then resetting the flow to what it can provide. Note that once a flow rate for any component has changed that this signals the need to resimulate any sub-loop to which it might have an indirect connection. Currently, this means that if a flow rate on the plant demand side changes, the simulation must recalculate the conditions on both the air loop and zone equipment sub-loops since coils and other equipment could be on either side of the main air loop. Similarly, if the condenser demand side simulation results in a change in flow rate through a chiller condenser, then the plant supply side must be triggered to perform its calculations again. Care has been taken to avoid cases where the various half-loops might simply keep triggering the resimulation of their indirect connections in an infinite loop.
-
-#### Loop Capacitance and Pump Heat
-
-The plant model includes simplified methods of modeling fluid capacitance and the temperature rise because of pumping and friction. The transition from load or energy based plant models to a loop based arrangement makes variables of both the flow rate and the fluid temperature. This means there are more degrees of freedom that must be controlled. The flow resolver concept discussed previously controls the fluid flow rates through the components and maintains an overall mass flow balance through the loop. However, the temperatures still need to be controlled and modeled. A purely iterative procedure can be expected to converge to the appropriate loop temperatures, but the procedure can become slow to converge under conditions where the demand changes rapidly or the supply components may not have enough capacity to meet the system demand. This situation is somewhat analogous to that existing in the link between the zone and the air system. In that case, the convergence and stability of the iterative solution was greatly improved by adding the thermal capacitance of the zone air and other fast responding mass within the zone. Based on that experience, it was decided to add thermal capacitance to the plant loop model to benefit from the added stability. Because the thermal capacitance in the zone/system interaction is relatively small, it was necessary to use a third order numerical solution there. Although the plant loop’s fluid thermal capacitance is relatively high, the fluid flows also have high heat capacity and can change temperatures rapidly a simple first order solution was not found to be satisfactory and an exact analytical solution was needed.
-
-In realistic conditions there is often some delay between changes in supply conditions and corresponding changes at demand side components due to the transport of fluid round the loop having a finite velocity.
-
-The act of pumping fluid around a loop adds heat to the fluid through friction.  The slight warming occurs at the pump and all around the circuit.  The amount of heat is equal to the work done on the fluid by the pump.  This so-called pump heat is a complicating factor in plant simulation because the pump heat alters the load on primary equipment.  A simple method of accounting for pumping heat is needed that doesn’t increase the difficulties of the numerical solution and (as of version 7) in EnergyPlus this accomplished by including the pump heat in the loop capacitance model.
-
-Plant loops include a simple loop capacitance model to simulate these effects based on a well-stirred tank model. Each half-loop has a well-stirred tank located at its inlet as indicated in Figure 123. The temperature of the tank is modeled as a function of the tank mass, inlet fluid flow rate and temperature, and pump heat.  No energy is lost or gained because of storage in the loop capacitance.
-
-
-
-![Loop Capacitance.tif](media/image1962.png)
-
-Figure 123. Loop Capacitance Tank Models
-
-The total plant loop volume is separated into two tanks, on on each half-loop inlet. For normal loops (without common pipes) each tank is one half of the plant loop volume. For common pipe plant loops, the tank on the supply side inlet has three fourths of the volume and the tank on the demand side inlet has one fourth. Each plant loop is assigned a total fluid volume as user input or an autocalculate routine based on the design flow rate. The size of the thermal capacitance affects the speed of recovery from situations where the setpoint was not maintained. The user must estimate a fluid volume based on the size of the pipes in the loop. Note that rough estimates seem to be sufficient. Loop capacitance (m<sup>3</sup>) could be calculated from pipe size data but this is not usually known. If zero capacitance is specified the above formulation reduces to an instantaneous update in demand update temperature and the demand inlet temperature becomes the supply outlet temperature at the previous time step. If a very large capacitance is specified unrealistic time delay may result and there may be poor response to changes in loop setpoint temperature. The loop capacitance ‘autocalculate’ option gives reasonable values and is calculated as follows,
-
-<div>$$Capacity = \frac{{{{\dot m}_s}*{t_{sys}}*3600}}{{0.8\rho }}$$</div>
-
-The tank temperature is modeled by drawing a control volume and energy balance around the tank and solving for the temperature.  The temperature of each tank is recalculated whenever the two half-loops are interfaced together. The tank temperature history is stored at the end of the simulation timestep.  The model equation for tank (and outlet temperature) is formulated as follows:
-
-<div>$${T_{tank,new}} = \frac{{\dot m{c_p}{T_{inlet}} + \frac{{{M_{tank}}{c_p}{T_{tank,old}}}}{{{t_{sys}}3600}} + {{\dot Q}_{pumpheat}}}}{{\mathop {m{c_P} + }\limits^ \frac{{{M_{tank}}{c_p}}}{{{t_{sys}}3600}}}}$$</div>
-
-The tank temperature at the end of the simulation timestep is solved by the analytical approach and expressed as
-
-<div>$$T_{tank}^t = \left( {T_{tank}^{t - \delta t} - \frac{{\dot m{c_p}{T_{inlet}} + {{\dot Q}_{pumpheat}}}}{{\dot m{c_p}}}} \right)\exp \left( { - \frac{{\dot m{c_p}}}{{{M_{tank}}{c_p}}}t} \right) + \frac{{\dot m{c_p}{T_{inlet}} + {{\dot Q}_{pumpheat}}}}{{\dot m{c_p}}}$$</div>
-
-where:
-
-<span>\(T_{tank}^{t - \delta t}\)</span>          = Previous system time-step tank temperature [°C]
-
-<span>\(T_{tank}^t\)</span>           = Current tank and tank outlet temperature [°C]
-
-<span>\(\dot m\)</span>              = Current fluid mass flow rate through the tank [kg/s]
-
-<span>\(\delta t\)</span>             = Duration of system time step [second]
-
-<span>\({c_P}\)</span>             = Heat capacity of fluid [J/kg]
-
-<span>\({M_{tank}}\)</span>         = Mass of the water in the tank [kg]
-
-<span>\({\dot Q_{pumpheat}}\)</span>    = Heat generated by a pump in the tank [W]
-
-When modeling plants using one of the common pipe modes for plant loops, the same tank model is used but the tanks are situated differently and account for extra connections.  For common pipe situation, the tanks are located on the outlet of a half loop with common pipe interactions downstream of the tank.
-
-The average temperature is reported as the tank temperature. The average temperature is defined as the value of an integral function of tank temperature on an interval [*0*,*δt*]
-
-<div>$$\mathop T\limits^ -   = \frac{1}{{\delta t}}\int_0^{\delta t} {T_{tank}^tdt} \;\; = \frac{{{M_{tank}}{c_p}}}{{\dot m{c_p}\delta t}}\left( {T_{tank}^{t - \delta t} - \frac{{\dot m{c_p}{T_{inlet}} + {{\dot Q}_{pumpheat}}}}{{\dot m{c_p}}}} \right)\left( {1 - \exp \left( { - \frac{{\dot m{c_p}}}{{{M_{tank}}{c_p}}}\delta t} \right)} \right) + \frac{{\dot m{c_p}{T_{inlet}} + {{\dot Q}_{pumpheat}}}}{{\dot m{c_p}}}$$</div>
-
-#### Plant Flow Resolver Input
-
-The input specifically related to the flow resolver consists of the plant BranchList and the plant ConnectorList as shown in the Input Output Reference. User defined names link the plant loop to its branches (contained in the BranchList) and define the loop splitters and mixers contained in the ConnectorList. The Connector:Splitter and Connector:Mixer syntax in turn define the relative connection of the branches to each other on the loop.
-
-The Branch definition is input in simulation and connection order for all of the components on the branch. The simulation assumes that the inlet node of the first component listed on the branch is the branch inlet node and the outlet node of the last component listed on the branch is the branch outlet node. Examples of all the input syntax is shown in the Input/Output Reference for the appropriate object.
-
-### Summary of Load Distribution Schemes
-
-Five load distribution schemes are employed in EnergyPlus. The figure below illustrates the plant load distribution algorithm. The total loop demand is calculated and used in the **ManagePlantLoopOperation** routine to determine which equipment is available based on the supervisory control scheme specified by the user. Once all available components have been identified the loop demand is distributed to the available components based on the user specified load distribution scheme.
-
- ![](media/image1974.png)
-
-Figure 124. Load Distribution Scheme
-
-
-
-The OPTIMAL scheme first loads each component to its optimal part load ratio (specified in input). Any remaining loop demand is distributed evenly to all the components. The UNIFORMLOAD scheme first divides the load evenly among all available components. If some components do not have the capacity to meet the uniformly distributed load, the remaining load is divided among the remaining components. The SEQUENTIALLOAD scheme loads each component one at a time to capacity until the loop demand is met. The components are loaded up in the order that they appear in the equipment list specified in input. The UNIFORMPLR scheme loads all equipment uniformly by maintaining uniform part load ratios across all equipment on the equipment list. If the load is below the load required by the plant to operate at the largest component minimum part load ratio, the last item is removed from each equipment list. This process is repeated until the plant can operate above the largest component minimum part load ratio. The SEQUENTIALUNIFORMPLR scheme loads all equipment in the order specified on the equipment list to capacity while operating all operational equipment at uniform part load ratios.
-
-
-
-*Note:* For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
-
-### Summary of Plant Loop Demand Calculation Schemes
-
-There are two plant loop demand calculations schemes in EnergyPlus. There is a **SingleSetPoint** and a **DualSetPointDeadband**; the **SingleSetPoint** is the default if that field is left blank in the PlantLoop object. In the SingleSetPoint scheme the Plant Loop requires that a Setpoint Manager set a single setpoint value that sets Node%TempSetPoint. Examples of this Setpoint Manager would be: the objects SetpointManager:Scheduled, SetpointManager:OutdoorAirReset, etc. For the DualSetPointDeadband scheme the Plant Loop requires that a Setpoint Manager that sets the high and low setpoint values for Node%TempSetPointHi and Node%TempSetPointLo. Examples of this setpoint manager would be: SetpointManager:Scheduled:DualSetpoint. Look in the Input Output Reference for the correct usage of these SetpointManagers.
-
-The Plant Loop Demand Calculation Scheme determines the amount of heating or cooling necessary to bring the temperature of the Plant Loop to its setpoint(s). When this value is determined then the Load Distribution scheme explained in the previous section takes this value and distributes the load to the appropriate equipment. The demand calculation scheme determines how the load is calculated. In the next section is a summary of the 2 algorithms and how they are used.
-
-#### Loop Demand Calculation Scheme SingleSetPoint
-
-The SingleSetPoint scheme for the PlantLoop takes the value that is placed on the Node%TempSetPoint and calculates the heating or cooling load necessary to obtain that setpoint.
-
-        DeltaTemp    = LoopSetPoint - LoopTempIn
-
-        LoopDemand = mdot \* Cp \* DeltaTemp
-
-The sign of the Loop Demand determines if the loop has a cooling or heating load. Then the Load Distribution scheme distributes this calculated load to the appropriate equipment.
-
-#### Loop Demand Calculation Scheme DualSetPointDeadband
-
-The DualSetPointDeadband scheme for the PlantLoop takes the value that is placed on the Node%TempSetPointHi and Node%TempSetPointLo calculates the heating or cooling load necessary to obtain that setpoint; if in the DeadBand then no load is calculated. The pseudo code below shows the basis of the algorithm.
-
-```
-        !Calculate the demand on the loop
-        IF (mdot > 0.0) THEN
-          LoadtoHeatingSetPoint = mdot*Cp*(LoopSetPointLo - LoopTempIn)
-          LoadtoCoolingSetPoint = mdot*Cp*(LoopSetPointHi - LoopTempIn)
-          ! Possible combinations:
-          ! 1  LoadToHeatingSetPoint > 0 & LoadToCoolingSetPoint > 0 -->  Heating required
-          ! 2  LoadToHeatingSetPoint < 0 & LoadToCoolingSetPoint < 0 -->  Cooling Required
-          ! 3  LoadToHeatingSetPoint < 0 & LoadToCoolingSetPoint > 0 -->  Dead Band Operation
-          ! 4  LoadToHeatingSetPoint > 0 & LoadToCoolingSetPoint < 0 -->  Not Feasible
-          IF (LoadToHeatingSetPoint .GT. 0.0 .AND. LoadToCoolingSetPoint .GT. 0.0) THEN
-             LoopDemand = LoadToHeatingSetPoint
-          ELSE IF (LoadToHeatingSetPoint .LT. 0.0 .AND. LoadToCoolingSetPoint .LT. 0.0) THEN
-             LoopDemand = LoadToCoolingSetPoint
-          ELSE IF (LoadToHeatingSetPoint .LT. 0.0 .AND. LoadToCoolingSetPoint .GT. 0.0) THEN
-             LoopDemand = 0.0
-          ELSE
-             CALL ShowSevereError
-          END IF
-        ELSE
-          LoopDemand = 0.0
-        END IF
-
-        IF(ABS(LoopDemand) < LoopDemandTol) LoopDemand = 0.0
-```
-
-
-The sign of the Loop Demand determines if the loop has a cooling or heating load. Then the Load Distribution scheme distributes this calculated load to the appropriate equipment, if there is any.
-
-### Plant and Condenser Equipment Operation Schemes
-
-Plants and condenser loops must have some mechanism for controlling the operation of the loop and which equipment is available under different operating conditions. Once the Loop load is calculated by the return conditions from the demand side and using the loop setpoint, this load needs to be allocated to the supply equipment according to the users input. This is mainly done by the operation schemes.
-
-Each operation scheme must have the type of operation scheme, its identifying name, and the schedule that defines its availability. The first scheme appearing in the list is given the highest priority; the second scheme has second highest priority, etc. In other words, if according to its schedule, the first operation scheme is available, then it is used by the simulation to define how the plant or condenser loop operates. If it is not available, the second operation scheme in the list is checked to see if it is available until the highest priority scheme that is also available is found. See the Input Output Reference for input field details.
-
-### Plant Operation Schemes
-
-See the Input Output Reference for input field details. The options for plant control schemes are:
-
-#### Uncontrolled Loop Operation
-
-The PlantEquipmentOperation:Uncontrolled scheme takes the full capacity of the supply equipment and cools or heats the loop accordingly. An example would be a cooling tower where the cooling tower would cool the condenser loop with all of its available capacity and not be limioted by a capacity range or setpoint. Uncontrolled loop operation simply specifies a group of equipment that runs ‘uncontrolled’. If the loop runs, this equipment will run also, unless turned off by the loop flow resolver to maintain continuity in the fluid loop.
-
-#### Cooling Load Range Based Operation or Heating Load Range Based Operation
-
-PlantEquipmentOperation:CoolingLoad (or PlantEquipmentOperation:HeatingLoad) defines the different ranges and which equipment list is valid for each range. In each trio, there is a lower limit for the load range, an upper limit for the load range, and a name that links to an equipment availability list (PlantEquipmentList). Load range operation is used when the loop load is calculated and then the equipment is selected in the proper range. This allows for the most efficient operation of the plant equipment or for the user to determine the most efficient plant configuration. When the equipment list has been deteremined then the load is allocated to the equipment in a manner selected by the user with “Optimal or Sequential� load distribution scheme. The load range based operation scheme has two statements associated with it: a main statement that defines the ranges that individual priority settings are valid and the lists of equipment that may be used for each range.
-
-### Condenser Operation Schemes
-
-This is very similar to the plant operation schemes, but there are several more options avaible with the CondenserLoop. The condenser operation schemes apply to the equipment on the ‘supply side’ of the condenser loop—pumps, cooling towers, ground coupled heat exchangers, etc. The keywords select the algorithm that will be used to determine which equipment is available for each time step. The ‘*Range Based Operation’* schemes select a user specified set of equipment for each user specified range of a particular simulation variable. ‘*Load* *Range* *Based’*  schemes compare the demand on the condenser supply side with specified load ranges and associated equipment lists. ‘*Outdoor…Range Based’* schemes compare the current value of an environmental parameter with user specified ranges of that parameter. See the Input Output Reference for input field details.
-
-#### Uncontrolled Loop Operation
-
-The PlantEquipmentOperation:Uncontrolled scheme takes the full capacity of the supply equipment and cools or heats the loop accordingly. An example would be a cooling tower where the cooling tower would cool the condenser loop with all of its available capacity and not be limioted by a capacity range or setpoint. Uncontrolled loop operation simply specifies a group of equipment that runs ‘uncontrolled’. If the loop runs, this equipment will run also, unless turned off by the loop flow resolver to maintain continuity in the fluid loop.
-
-#### Cooling Load Range Based Operation or Heating Load Range Based Operation
-
-PlantEquipmentOperation:CoolingLoad (or PlantEquipmentOperation:HeatingLoad) statement defines the different ranges and which equipment list is valid for each range. In each trio, there is a lower limit for the load range, an upper limit for the load range, and a name that links to an equipment availability list (CondenserEquipmentList). Load range operation is used when the loop load is calculated and then the equipment is selected in the proper range. This allows for the most efficient operation of the plant equipment or for the user to determine the most efficient plant configuration. When the equipment list has been deteremined then the load is allocated to the equipment in a manner selected by the user with “Optimal or Sequential� load distribution scheme. The load range based operation scheme has two statements associated with it: a main statement that defines the ranges that individual priority settings are valid and the lists of equipment that may be used for each range.
-
-#### Outdoor Drybulb Range Based Operation, Outdoor Wetbulb Range Based Operation,  Outdoor RHPercent Range Based Operation
-
-The various “PlantEquipmentOperation:Outdoor\*� statements define the different ranges of the various environmental parameters and which equipment list is valid for each range. After the keyword and the identifying name, a series of data trios is expected. In each trio, there is a lower limit for the load range, an upper limit for the load range, and a name that links to an equipment availability list (the “CondenserEquipmentList�).
-
-#### Outdoor Drybulb Temperature Difference Based Operation,. Outdoor Wetbulb Temperature Difference Based Operation
-
-
-
-The various “PlantEquipmentOperation:Outdoor\*Difference� statements control strategies help to control any condenser equipment based on the difference between a reference node temperature and any environmental temperature. For example a cooling tower can be controlled by a strategy, which looks at the difference between the tower inlet temperature and wet-bulb temperature. A difference range is specified for each equipment list.
-
-### Primary-Secondary Loop Systems
-
-The method to simulate a primary-secondary system in EnergyPlus is termed Common Pipe.
-
-#### Common Pipe
-
-Common pipe feature eliminates the need of specifying two different EnergyPlus loops each for Primary and Secondary half loops. Instead the user can set up the system as it is used in real life applications. A common pipe simulation requires that pumps be placed on both Demand (Secondary) and Supply (Primary) sides of the loop. A typical Common Pipe layout as used in EnergyPlus is shown in figure 92. The major assumptions in the common pipe implementation are as follows:
-
-* Pumps are placed on both demand and supply side of the loop.
-
-* Secondary pump flow rate can be less than, equal to or greater than the primary pump flow rate.
-
-* The flow at the inlet node of the half loop is equal to the flow at the outlet node of the half loop.
-
-* The pumps can have different schedules and any loop can be shut off when the other loop is still running.
-
-![CommonPipe](media/image1975.png)
-
-Figure 125. Common Pipe Layout Schematic
-
-Common pipe simulation is done during the interface update call at both Supply-to-Demand and Demand-to-Supply. Appropriate checks are used to make sure that the effect of flow reversal in between iteration is taken care of. Moreover, the common pipe keeps track of the flow rates and temperatures at all the four nodes linked to it; namely, the inlet and outlet nodes of each sub loop. This record will help to decide if loops have converged or not. In situations where the primary component meets the setpoint and the coil controls does not change its flow request, the common pipe converges quickly. The simple description of the control algorithm for common Pipe implementation is as follows:
-
-1. At FirstHVACiteration, the common pipe flow is initialized to zero.
-
-2. Common pipe is simulated at interfaces and thus we will have 2 different flows handle on either side of interface.
-
-3. Loops and corresponding flow rates are assigned inlet or outlet (to common pipe) depending on the interface which calls it. So when common pipe is called from demand to supply interface, the inlet loop is demand side and outlet loop is supply side and vice versa.
-
-4. Inlet flow is compared to outlet flow and the difference is set as the common pipe flow.
-
-5. At each interface the common pipe flow is assigned a direction which can be into the interface (Inlet flow &lt; Outlet flow) or away from interface (Inlet flow &gt; Outlet flow).
-
-6. Outlet temperature is calculated depending on the flow rate and flow direction. When flow is away from interface outlet flow temperature is same as inlet flow temperature. For a common pipe flow into the interface, the outlet flow temperature is calculated as mixed temperature of inlet flow and the common pipe flow.
-
-7. At demand to supply interface, the supply side inlet node temperature and flow rate are updated every iteration. At supply to demand interface, only flow is updated. The temperature is updated only at the end of timestep.
-
-8. Loops iterate till the flow and temperatures at all the 4 concerned nodes do not change.
-
-#### Two-Way Common Pipe
-
-A model referred to as Two-Way Common Pipe is available which provides a way to model Primary-Secondary systems as a single Plant Loop.  In a typical EnergyPlus plant loop simulation, the only half loop inlet/outlet node that is controlled is the supply side outlet node. In some cases this requirement becomes a limitation in analyzing different options. A good example is ice thermal storage application, where during charging phase, the coil setpoint can be different from the ice storage equipment setpoint. With this model, the interface between the two half loops includes two additional flow paths that essentially split a single plant loop into both primary and secondary loop sides.  Though the Two-Way common pipe is designed to be generic some assumptions apply in modeling the component. The assumptions are as follows
-
-* The secondary flow may be less than, equal to, or greater than the primary flow.
-
-* The mass flow rate at the Primary Side Outlet Node is always equal to the mass flow rate at the Primary Side Inlet Node.
-
-* The mass flow rate at the Secondary Side Outlet Node is always equal to the mass flow rate at the Secondary Side Inlet Node.
-
-* Only one additional node, either primary-side inlet or secondary-side inlet, (along with the primary-side/supply-side outlet node) can be controlled. The system of equations that describe the loop interface will be under specified if both the Primary and Secondary Inlet nodes have to be controlled.
-
-Figure 126 shows a schematic of the Two-Way Common Pipe. There are two common pipe legs, shown as broken lines, allow for some recirculation at the half loop level.  The model allows for common pipe flow in either or both directions. The model determines flow rates in the common pipes and temperatures at nodes based on the following:
-
-* Which additional node is being controlled to meet a temperature setpoint? If the primary-side inlet node is controlled, then the flows are controlled to deliver the desired temperature at supply side inlet. If the secondary-side inlet node is controlled then the flows are controlled to deliver the desired temperature at the demand side inlet.
-
-* Is the specified setpoint achievable with current secondary and primary outlet conditions? If the setpoint is not achievable, then the flow in each common pipe leg is reduced to its minimum possible value.
-
-* At the controlled node, with known demand outlet temperature, supply outlet temperature, primary flow rate and secondary flow rate, and energy balance is used to calculate recirculation flows in the common pipes for that particular half loop, so that the desired temperature setpoint is achieved.
-
-* With a known flow in one common pipe leg, the flow on Primary to Secondary (or secondary to primary) is easily obtained by mass balance.
-
-* When the Two Way Common Pipe is controlling conditions at the secondary-side, or demand side, inlet node, then the loop capacitance model usually used for the conditions at the demand inlet is not used as it would interfere with control.
-
-![](media/image1976.svg.png)
-
-Figure 126. Schematic of a Two-Way Common Pipe used in Primary-Secondary System.
-
-### Heat Recovery Loop Systems
-
-Heat Recovery is accomplished by specifying another set of supply and demand loops. Each of the heat recovery components, i.e. engine driven and combustion turbine chillers, and internal combustion and combustion turbine generators is designed to use the existing component/loop/solution structure to facilitate the simulation with the existing demand side manager and the supply side manager. Heat recovery normally contains components that produce heat that can be recovered, and the ability to store or use that heat elsewhere in the system. The component that can store the excess heat and allow it to be used elsewhere in the system or for domestic hot water is the Water Heater:Simple and is defined in the Input/Output Reference.
-
-![](media/image1977.png).
-
-Figure 127. Example of a Heat Recovery Loop Simulation
-
-In the example above there is a chilled water Loop with chilled water supplied by a diesel engine driven chiller. There is a hot water Loop that is being supplied by the water heater: simple. There is also scheduled domestic hot water usage on the water heater which excess demand can be met by a number of user-specified heating sources. Then on the demand side of the heat recovery loop there is the engine driven chiller, internal combustion, and combustion turbine electric generators with specified mass flows to recover the heat. This hot water is pump on the supply side by the heat recovery pump and provides the heat to the water heater to meet the water heater setpoint. This is probably one of the more complex configurations and interactions that would take place in heat recovery, but using the Plant supply and demand side configurations this can be extended to meet most user configurations. The plant water heater can also be used to just meet scheduled domestic hot water use, provide a hot water source for PlantLoop equipment, or provide a hot water storage tank for heat recovery as a single function. Or any combination of the above can be configured. Example files of some of these configurations are provided with the installation.
-
-### Plant Pressure Drop Simulation
-
-As of version 4.0, there is an added feature which allows better calculation of pressure in plant and condenser loops. Without any method, the loops essentially ignore the node pressures. This is suitable for many applications, however may cause inaccuracies in the pump power. This is especially prominent in cases where the loop flow may change drastically over a wide range of configurations, as the pump power is based on a rated power value and rated pump head value. As the loop components turn on and off, the pressure drop will change, and so the pump power should be dynamically updated with these changes.
-
-#### Overall model features:
-
-Calculates loop pressure drop based on pressure drop information which is placed on branches. These are entered in terms of generic curves (linear, quadratic) or pressure drop information (minor loss/friction factor).
-
-Loop pressure drop is used as the new pump head. No information is entered about the pump curve, so it is assumed that the pump will always be able to meet this operating point. Future enhancements will allow the pump to ride a curve based on the given pressure head.
-
-Model does not resolve flow rates on parallel branches to match pressure drop, this is explained further below, but basically it takes the maximum pressure drop from parallel pressure components and applies that to all parallel components.
-
-Model works for the following configurations:
-
-1. Pump Location
-
-2. Loop Pump
-
-3. Branch Pumps
-
-4. Loop Types
-
-5. PlantLoop
-
-6. CondenserLoop
-
-The supply side inlet (before the pump) is always set to standard atmospheric pressure. This allows the node pressures around the loop to stay positive. The actual values of pressure are not all that important, it is the delta pressure that is of interest for our calculations, but this makes the pressure values appear realistic if one plots the pressure around the loop.
-
-The pressure drop is at the branch level, not the component level. If multiple components are found on a single branch, the pressure drop is always applied to the last component on the branch. This is coordinated with the rule that a pump must always be the first component if it is found on a branch.
-
-Calculations use the branch flow rate and the branch entering temperature to calculate properties for the whole branch.
-
-#### Detailed Restrictions:
-
-Pressure drop curves must not be placed on branches which only contain a pump. Pressure curves may be placed on the supply inlet branch with a pump as long as there are other components on that same branch, following the pump.
-
-If using branch pumps, pressure drop curves found on the supply inlet branch will be ignored. Put pressure drop information after pumps.
-
-Currently, pressure drop simulations are not allowed with common pipe (demand pump) simulations. A future version of the pressure drop system will allow this by allowing each pump to handle the pressure drop of the given loop side (demand or supply).
-
-#### Detailed Calculation Steps:
-
-Before the demand side is simulated, the pressure system is initialized. All node pressures are reset, and pressure drop values for branches are re-initialized.
-
-After all components on a branch are simulated, the pressure drop for that branch is calculated. This pressure drop is registered in the pressure drop system to be used in subsequent loop level calculations.
-
-Once the entire loop (demand then supply sides) is simulated, the loop level pressure drop calculations are performed using the following steps:
-
-Beginning at demand side outlet (linked to supply inlet), and working backwards, the node pressure is updated and loop pressure is summed by “adding pressure drops� as they are found around the loop. By working backward, we are able to easily preserve the pump inlet pressure as a realistic value (standard atmospheric pressure).
-
-When a parallel system is encountered, a special operation is performed. Since we are not resolving flows with this version of the pressure simulation, the parallel system is set to use the largest value of pressure drop found on the parallel branches. In this manner, the highest pressure drop component essentially governs the set of parallel branches, and the other components must match the pressure drop in order to achieve their desired flow rate. This is performed by placing “imaginary� valves in the splitter. This allows individual branches to report their own pressure information, while the splitter accounts for the required pressure drop to match the governing branch. This is shown graphically in the figure below.
-
-![SplitterValves](media/image1978.png)
-
-Figure 128: Explanation of valves inherently built into Splitter object
-
-Because the splitter automatically handles the pressure drop required to match the pressures in the parallel system, the mixer will have uniform flow entering from all branches and exiting.
-
-These calculations are performed around the loop and result in a value of pressure drop for the entire loop.
-
-Pump power requires a value of pressure head before it can add heat to the loop, which is done before any components are calculated, and any pressure system calculations are performed. Because of this, the pump power is based on rated head during the first iteration. On subsequent iterations, the pump power is based on the dynamic pressure head calculated by pressure drop information.
-
-If anything drastically changes between one iteration and the next, the loop will be re-simulated, and the latest value of pressure head will be used. By the time the loop is converged, the pressure head between the current and most previous iterations will agree to within simulation tolerance. Thus the pump is using a lagged value of pressure head, but once the loop is converged, the lagged and current values will agree.
-
-#### Pressure Drop Calculations:
-
-There are two types of pressure drop curves that can be entered, each with its own calculation engine:
-
-Generic: A curve of any form (single independent variable) such as linear or quadratic may represent the pressure drop in Pascals as a function of current mass flow rate in kg/s. This is common for regressing component pressure drop such as heat pumps into a quadratic best fit form. The branch pressure drop is then calculated by evaluating this curve with the given branch flow rate.
-
-Pressure Information: This calculation involves two types of pressure drop: frictional effects and minor losses. The governing equation is:
-
-<div>$$\Delta P = \left( {f\frac{L}{D} + K} \right)\frac{{\rho {V^2}}}{2}$$</div>
-
-The user enters value for the minor loss coefficient K to represent all the minor losses on that branch. If the user is entering friction information, the minor loss coefficient may be zero or blank.
-
-The user enters roughness, e, or a fixed value of friction factor to account for frictional losses on the branch, as well as an equivalent length L. If the user enters roughness then the friction factor is calculated from a Moody chart approximation (Haaland, 1983):
-
-<div>$$f = {\left\{ { - 1.8\log \left[ {{{\left( {\frac{{e/D}}{{3.7}}} \right)}^{1.11}} + \frac{{6.9}}{{{\mathop{\rm Re}\nolimits} }}} \right]} \right\}^{ - 2}}$$</div>
-
-If the user enters minor loss information, then the friction factor information can be left out.
-
-The diameter is an equivalent value and is used to calculate relative roughness for friction calculations as well as velocity for any pressure drop calculation.
-
-#### Riding Pump Curves to Determine Loop Operating Point
-
-In addition to being able to provide a means of calculating loop pressure drop, EnergyPlus can also perform a “loop-level� pump-system flow resolution.  The pressure drop components that were described in the previous sections are combined with the input of a dimensionless pump pressure-flow curve and at each iteration, these are utilized in determining a proper operating point for the loop.
-
-Some restrictions do apply to this simulation.  As with the basic pressure drop simulation, common pipes are not valid in the current release.  For this pump curve phase, the simulation is also restricted to “loop pumps� such that pumps should not be used on the parallel branches between a mixer and splitter.
-
-The idea of riding a pump curve, as it is currently implemented, is based on a constant speed pump.  A variable speed pump in EnergyPlus can already effectively vary its flow/pressure characteristics to meet the demand.  Thus, this phase is only implemented for the Pump:ConstantSpeed model.
-
-The model works by approximating the loop with a quadratic pressure drop form, then iterating to find an operating point.  The entire plant loop then iterates to find the operating point that attempts to match the requested flows.  Note that when doing a pressure based pump simulation, the loop will likely not hit setpoint every timestep, while doing the simpler approach (non-pressure) may result in a tighter-controlled simulation.  In deciding this, you must consider the realism of the pressure approach vs. the non-pressure approach which may be more tightly controlled and will have less input requirements.
-
-In the first iteration of the plant, there is not yet enough information to determine a pressure-flow simulation, so flow through the loop is set to the rated flow rate of the pump (irrespective of pump performance curve). For this rated flow rate pressure drop in each branch will be calculated by plant pressure system. So after this first pass through the loop, the pressure system now has a valid system flow-pressure point.  From this point (pressure drop in the branch and rated mass flow rate) a pressure constant for each branch is calculated assuming quadratic relationship between pressure drop and mass flow rate.
-
-<div>$${K_{Branch(i)}} = \Delta {P_{Branch(i)}}/{m_{Rated}}^2$$</div>
-
-If there are parallel branches then equivalent K is calculated from following formula.
-
-<div>$$\frac{1}{{\sqrt {{K_{ParallelEquivalent}}} }} = \sum\limits_{j = 1}^m {\frac{1}{{\sqrt {{K_{Branch(j)}}} }}} $$</div>
-
-From all these ‘K’ values of the branches a corresponding K value for complete loop is calculated. This representative K value for the loop will lock down a system curve for a single iteration.  This K value will change throughout the higher-level plant iterations and simulation time steps.
-
-The Non-dimensional pump curve is entered in following way,
-
-<div>$$\psi  = {C_4} \times {\varphi ^4} + {C_3} \times {\varphi ^3} + {C_2} \times {\varphi ^2} + {C_1} \times \varphi  + {C_0}.$$</div>
-
-C<sub>1-4</sub> are curve coefficients with last mandatory non-zero constant term C<sub>0</sub> (as pump curve will not pass through origin).
-
-The nondimensional variables in the previous equation are defined in terms of the following expressions:
-
-Ψ – Non-dimensional pressure rise:  <span>\(\psi  = \frac{{\Delta P}}{{\rho {N^2}{D^2}}}\)</span>
-
-φ - Non-dimensional flow:  <span>\(\varphi  = \frac{{\dot m}}{{\rho N{D^3}}}\)</span>
-
-The user preprocesses mass flow and pressure values into these nondimensional forms in order to generate the curve fit.  The program then resolves the nondimensional forms into actual values based on the pump speed, diameter, and fluid density.  This gives the proper pressure-flow relationship for the simulation.
-
-#### Pump-System Operating Point Flow Resolver:
-
-The pressure drop components and the pump curve are described in the prior sections.  The routine which actually uses these curves to resolve to an operating point is described here.  This routine is called by the pump model as it is determining what flow it should be using.  The flow resolver reads the non-dimensional pump curve, loop pressure constant (K value) and rated mass flow rate (or mass flow rate from last iteration). The resolver finds the intersection of the two curves by successive substitution with 0.9 as a damping factor. If the flow rate is outside (or if in any iteration move out of) the range for which pump curve-fit is suggested, the resolver will bring the value within range, thus it is important to specify the curve-fit range (in terms of non-dimensional flow rate) for pump curve by the user.  It was observed that simple successive substitution (sometimes) diverges depending on shape of curves and/or location of operating point. Damping factor provides stability to successive substitution and it was observed that it converges for less number of iteration, speeding up the function. The damping factor was set as 0.9 as it showed full stability during testing, although a more optimum value may be available for a particular set of curves.  A future version may have an improved selection algorithm for the damping factor itself.
-
-#### References
-
-Haaland, SE. 1983. "Simple and Explicit Formulas for the Friction Factor in Turbulent Flow". Transactions ASIVIE, Journal of Fluids Engineering 103: pp. 89-90.
-
-Steam Systems and Component Models
-----------------------------------
-
-A steam system uses the vapor phase of water to supply enthalpy or kinetic energy through the piping network.  In case of EnergyPlus, the steam system is designed to provide energy solely for the building heating requirements.  Hot steam from the boiler or steam generator in buildings can be used to heat a conditioned space with suitable heat transfer equipment such as fan-coils units, unit-heaters, radiators and convectors or steam can also heat water through shell and tube heat exchangers, and hot water can be supplied to the terminal units to provide the zone heating requirements.
-
-The advantages that steam system offer over hot water or other heating systems are:
-
-1. Steam flows through the system unaided by external energy source such as pumps; pressure difference moves steam across the system.
-
-2. Steam, because of its low-density, can be used in high-rise buildings where water systems create excessive pressure.
-
-3. Terminal units such as heating coils can be added or removed without making any changes to the system.
-
-4. Steam components can be repaired or replaced by closing the steam supply without the difficulties associated with draining and refilling like in the water systems.
-
-5. Steam is pressure-temperature dependent, therefore the system temperature can be controlled by varying either steam pressure or temperature.
-
-6. Steam can be distributed through out the system without any change in temperature.
-
-In view of the advantages mentioned, the steam systems are suitable for applications where heat is required for process and comfort heating such as in industrial plants, hospitals, restaurants, dry cleaning plants laundries and commercial buildings.  They are also suitable in places where the heating medium has to travel great distances such as in facilities with scattered building locations or where the building height would result in excessive pressure in a water system, or locations where the load changes occur intermittently.  Thus steam system is an essential and necessary development step for EnergyPlus.
-
-From EnergyPlus simulation point of view, the advantage associated with a steam system is that steam can be distributed through out the system without change in temperature.  This means that the boiler outlet temperature can simply be set equal to the heating coil inlet temperature for a steam system.
-
-Another simulation-based advantage associated with the steam system is Steam Quality, which does not change from boiler outlet to coil inlet.  Actual building steam systems are equipped with condensate drains through out the system, these drains remove, almost immediately any condensate that is formed during steam transportation, thereby maintaining the steam quality at constant value of 1.0 through out the high-pressure steam side.
-
-The HVAC steam system implementation includes simulation models for two phase steam equipment like steam boiler, steam to air heating coils, steam pipes and condensate pumps, which can be connected to the generic loop framework.
-
-### Steam Loop Assumptions
-
-To replicate the working of an actual building steam system in a satisfactory manner with simulation, it was necessary to make certain assumptions.  These assumptions help simplify the loop complexity and increase usability.  The effects of the assumptions made are described in detail below.
-
-The following figure describes the Temperature Entropy Ts diagram based on which the steam system operates in EnergyPlus.  The steam side of the loop operates on constant saturation pressure of steam: PSteam, the waterside of the loop operates at atmospheric pressure Patm.
-
-
-
-![SteamSchematic](media/image1986.png)
-
-Figure 129. Schematic of Temperature – Entropy Diagram for Steam loop
-
-It should be noted that the figure is simply a schematic and not a scaled representation of the process on a Mollier Chart.  For the following descriptions, please refer to the schematic figure above.
-
-*  Process 1–2 on the Ts diagram, represents condensation of steam in the coil at constant pressure; this is where the steam gives up latent heat to the zone.
-
-*  Process 2–3 represents the subcooling of condensed steam at higher pressure, this subcooling takes place inside the steam coil, just before the steam trap.  The delta temperature represented by 2-3 is the degree of subcooling in the steam coil, and is a user input to the steam coil.  This subcool generally accounts for 1 to 2 % of the total heat transfer in the steam coil.
-
-*  Process 3–4’ represents the isenthalpic expansion of water from high-pressure steam side to atmospheric pressure across the steam trap.  As steam gives up its latent heat at the steam coil the condensate that forms in the steam coil still exists at higher pressure.  This condensate is discharged to a lower pressure across the steam trap, this condensate contains more heat than necessary to maintain the liquid phase at the lower pressure, this excess heat causes some of the condensate to vaporize or flash to steam at lower pressure at some quality.  The amount of water that flashes to steam can be calculated by the following equation
-
-<div>$$\% Flash\,\,Steam\,\, = \frac{{{h_{4'}} - \,{h_4}}}{{{h_{fg}}}}\,\, \times \,\,\,100$$</div>
-
-Where h4’ is Enthalpy of liquid at steam pressure just before condensate is supposed to leave the coil.  Enthalpy at Point 3 is equal to enthalpy at point 4’, since it is an isenthalpic process, and  hfg is the latent enthalpy of the fluid at atmospheric pressure.
-
-For example, water at 102LC and 120 Kpa flashes to steam at at100LC and atmospheric pressure, with quality equal to 0.003.  This results in loss of some latent capacity of steam and is one of the terms contributing to loop loss in steam system.
-
-*  Process 4’- 4 represents the condensation of the flashed steam, which has exited from steam trap into the condensate drain.  Condensation occurs at atmospheric pressure Patm, there is loss in latent capacity due to this unavoidable process, only condensate can be returned back to the boiler in a steam system.
-
-*  Process 4-5 represents the loop sub cooling at atmospheric pressure; this is the sub cooling of the condensate that takes place during condensate return to the boiler because the return loop is not insulated, loop sub cooling is of the order of 20LC to 30LC.  This is a user-defined input in every steam coil, because the variability in location of steam coils in a building will result in different condensate return temperatures for each of the coils.
-
-*  Process 5-6 represents the temperature and pressure rise in condensate due to pump heat addition.  The pumping process generates heat, which is added to the condensate.  The condensate is pumped back to the boiler at higher pressure.
-
-*  Process 6-2 represents the sensible heat addition by the boiler to the return condensate.
-
-*  Process 2-1 represents the latent enthalpy of steam, added by the boiler to the water to convert it to steam at saturation pressure.
-
-*  Point 3, which is outlet of the coil and Point 5, which is inlet of the pump are specified directly by the user, subsequently the loop losses in EnergyPlus are directly summed up as the enthalpy difference between point 3 and 5, which is calculated by fluid property routines in EnergyPlus.  This helps to maintain flexibility and at the same time helps negate the intermediate points calculation in the system.
-
-Aspects of the steam loop such as quality of steam, steam pressure, and steam generation which play an important role in EnergyPlus simulation are described in following sections.
-
-#### Constant Pressure Steam loop
-
-The steam loop in EnergyPlus is pressure driven and it is assumed to operate at constant pressure on the gaseous-steam part, while the condensate return loop is assumed to operate at atmospheric pressure.  The steam loop essentially operates at saturation pressure corresponding to the steam temperature; the steam boiler serves to maintain the loop temperature.  The boiler model determines the amount of energy required to generate the required amount of steam.
-
-Factors such as friction in pipes, which tend to cause small amount of pressure drop in steam loop are neglected in the model.  It is assumed that the steam pipes are fairly well insulated to prevent heat loss and subsequent condensation of steam in the pipes.  In actual systems small quantities of steam, which condenses due to heat loss during transportation is removed immediately from the system by steam drains.  This helps eliminate water hammer, degradation of steam quality and heat transfer capability.
-
-#### Steam Generation at Saturated Conditions:
-
-Building steam heating systems avoid supplying superheated steam because superheat damages the building HVAC equipment.  Superheated steam is generated only if there is a cogeneration power system in building such as steam turbine, which requires superheated steam.  The purpose of having superheated steam is redundant for building steam heating systems because the amount of energy carried by the same is negligible compared to the latent heat. A simple enthalpy calculation, based on each unit of steam mass flow rate (1 kg/s), has been provided in this section to describe the negligible effect of superheat..
-
-Case 1: Loop Operating at Saturation Conditions (no superheat), calculating enthalpy of saturated steam at boiler outlet temperature.
-
-Boiler Outlet Temperature = 105BC,
-
-<div>$${h_{Case1:NoSuperheat}} = [{h_f}_{{{105}^ \bullet }C}]$$</div>
-
-<div>$${h_{Case1:NoSuperheat}} = \,\,\,\,2684000\,\,\,\,\,\,J$$</div>
-
-Case 2: Loop operating with Superheated steam, calculating enthalpy of superheated steam for 5BC superheat.
-
-Degree of Superheat = 5BC
-
-Boiler Outlet Temperature = 110BC,
-
-<div>$${h_{Case2:Superheat}} = [{h_f}_{{{110}^ \bullet }C}]$$</div>
-
-<div>$${h_{Case2:Superheat}} = \,\,\,2691000\,\,\,\,\,\,\,\,J$$</div>
-
-The energy difference between the superheated state and the saturated state as calculated in the following equation.  A 5BC superheat provides only a 0.2608% increase in heat transfer.  The advantage of this additional increase in heat transfer is negligible, especially when considering the economic aspect of sizing a bigger heat exchanger to accommodate additional superheat transfer.  The detrimental effects of superheated steam on the building HVAC system also come into effect once superheat is used.
-
-<div>$$\Delta {Q_{2 - 1}}\,\,\, = \,\,\,\frac{{2691000\, - 2684000}}{{2684000}}\,\, \times 100\,\,\,\, = \,\,0.2608\,\,\,percent$$</div>
-
-Based on the reasoning above the steam loop in EnergyPlus is designed and implemented to operate at saturated conditions.
-
-#### Steam Quality
-
-The boiler operation is assumed capable to generate steam at quality equal to1.0 every time.  This is a reasonable assumption, since in practice the variability in generated steam quality would only occur if the boiler operation were not properly controlled.
-
-The steam loop is assumed to have perfect transport mechanism.  There is no transportation losses due to friction and heat transfer with surroundings.  This assumption helps maintain the quality of steam through out the system constant value of either 0 or 1.
-
-Steam enters the coils at boiler outlet conditions.  Steam coils are designed with steam traps, which only allow condensed steam to leave the coil; hence the steam always condenses and leaves the coil at quality of 0.0.
-
-With the above simplifying assumption enables the EnergyPlus steam loop to be solved without problems.
-
-#### Steam Traps
-
-Steam traps are essential part of the steam system; they are indirect flow controllers of the loop.  Purpose of steam trap is to allow only condensate out of the coil from higher-pressure steam to lower atmospheric pressure condensate return line.  Points 3-4C, in schematic  Figure 129, represent this process across the steam trap on the Ts diagram.  The expansion process across the steam trap is assumed to be isenthalpic.  There is possibility of flashing of high-pressure condensate across the trap because of pressure drop, resulting in generation of steam at lower pressure, this steam generated at lower pressure subsequently condenses in the return piping, and heat is lost to the atmosphere.  This heat lost is a part of the steam loop losses.
-
-Steam traps are modeled in the EnergyPlus steam coil by assigning the condensate outlet from the coil a quality of 0.0 and sub cooling the condensate at lower pressure.
-
-Although condensate from the steam coil contains valuable heat, attempting to utilize this heat by holding the condensate in the coil reduces the heat transfer area.  It causes operational problems because it retains air, which further reduces heat transfer and non-condensable gases such as carbon dioxide, which cause slow corrosion of the steam coil.  Steam moves rapidly in mains and supply piping so when condensate accumulates to the point where the steam can push a slug of it, serious damage can occur from the resulting water hammer, hence the condensate should be immediately removed from the steam coil.  This is achieved with steam traps.
-
-Hence an ideal steam trap should remove all condensate, air, and non-condensable gases that might be in the system, with little or no loss of steam.
-
-#### Loop Losses
-
-Subcooling of condensate in condensate return piping and flash steam condensing across the steam trap constitute the unavoidable loop losses in the EnergyPlus simulation steam system.  These losses can be inferred from Figure 129 and are summed up by calculating enthalpy difference between points 3 and 5 on the schematic Ts diagram.
-
-Unavoidable losses in the EnergyPlus steam loop occur due to pressure drop across the steam trap, which causes flashing of steam and loss in some percentage of latent heat of steam, process 3-4’ and 4’-4 on the Ts diagram in Figure 129.  The condensate is pumped backed to the boiler through return pipe network, which is not insulated.  Sub cooling of the condensate occurs in the return network, represented by process 4-5 on the Ts diagram in Figure 129.  This loop sub cool contributes to significant percentage of loop losses.
-
-In practical systems the return pipeline to the boiler is not insulated despite the condensate containing some valuable heat, however due to low mass flow rate of steam, this amount is negligible and only recovered if separate heat recovery systems are used by coupling them to the loop.  The condensate is occasionally collected in a receiver and then pumped back to the boiler.  EnergyPlus simulation mimics practical systems by assumed that the return pipeline is not insulated and accounts for this by calculating loop losses.
-
-The loop losses are calculated in the steam coil simulation model rather that the steam pipe simulation, because the condensate sub cool in the return loop is a direct function of the location of the steam coil in the building.  In building energy software like EnergyPlus the user would have a fair idea about location of steam coils rather than the location of condensate return piping.
-
-### Steam To Air Heat Exchanger
-
-#### Description of Model:
-
-The steam to air heat exchanger (Coil:Heating:Steam input object) is the terminal equipment in the steam loop on the demand side that satisfies the heating requirements of the various zones.  The steam-to-air heat exchanger simulation model in EnergyPlus calculates the mass flow rate of steam desired to meet the heating demand.
-
-A heating coil can be used either as a zone coil or a coil in the air loop depending on the user and application.  The steam coil simulation model is designed to take these two locations into consideration.  An air-loop steam heating coil is temperature controlled and the zone coil is zone load controlled.  This relatively simple and straightforward concept of coil control is preferred over the iterative method to determine mass flow rates using various numeric techniques.  The assumptions made in the coil model are described in the section below.
-
-This model accounts for the latent heat transfer and sensible cooling of water; the question of superheat is eliminated because steam is assumed to be saturation conditions.  Steam enters the coil at quality equal to 1.0, at saturation temperature and leaves the coil with desired degree of sub cooling.  The user inputs the desired degree of subcooling, which determines the condensate outlet condition from the coil.
-
-EnergyPlus heat balance methods determine the amount of heating required in the zone to maintain the zone at the desired conditions.  Based on this value of heating load, the zone coil determines the mass flow rate of steam required since the heating coil load is the control variable in a zone coil.  The following equation describes this calculation to determine steam mass flow rate required for the desired heating capacity. The steam latent heat of vaporization, *h*<sub>fg</sub> and the condensate heat capacity, *C*<sub>p,w</sub> are evaluated at the steam coil inlet node temperature and standard barometric pressure of 101325.0 Pa.
-
-<div>$${\dot m_{zc}}\,\,\,\, = \,\,\,\,\,\frac{{{Q_{zc}}}}{{{h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}}}}$$</div>
-
-In case of the air loop-heating coil, the load on the coil is calculated within the coil simulation routine.  The air loop coil is setpoint controlled and heats the air to maintain the air stream at the desired setpoint, the setpoint is a user input, generally in the range of 12B C to 16BC. The following equation describes the air loop coil load.
-
-<div>$${Q_{al}}\,\, = \,\,{\dot m_a}\,\,\, \times \,\,\,\,\,{c_{p,a}}\,\,\, \times \,\,\,\,\,\left[ {{T_{sp}}\,\,\, - \,\,\,{T_a}} \right]$$</div>
-
-The following equation is used to determine the steam mass flow rate required by the air loop coil to meet the heating requirements.
-
-<div>$${\dot m_{al}}\,\,\,\, = \,\,\,\,\,\frac{{{Q_{al}}}}{{{h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}}}}$$</div>
-
-Each of the zone coils and air loop coils are simulated independently and the steam mass flow rates for each is added over every time step of simulation.  This value of total mass flow rate is reported to the boiler, which in turns supplies this required amount of steam.
-
-The control of the steam to air coil is a complex issue.  The loop splitter-splits total steam flow from the boiler and delivers the required amount of steam to each of the coils connected to the loop through the steam pipe network.  In cases where the system is undersized, the coils demand more mass flow rate of steam than the boiler can generate.  The splitter in this case cannot provide all the coils with requested steam mass flow.  Subsequently the coils are starved of steam and the zone temperatures fall.  In some cases the user might schedule off the coil, they should then not operate.  These issues need to be taken care of in the implementation of the steam coil simulation model.  The control algorithm for the steam coil operation under various situations is best explained with the help of pseudo-code using standard IF THEN ELSE blocks.
-
-
-
-\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*PSEUDO CODE SECTION STARTS\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-
-
-#### Steam coil is zone load controlled.
-
-<div>$$IF\,\,\,\,\,(Coil\, = LoadControlled)\,\,\,\,\,\,THEN\,$$</div>
-
-
-
-Check for operational conditions only then continue simulation further.  The operational conditions are the inlet mass flow rates of steam and air to the coil, the user schedule to the coil and heating load on the coil.  The coil is simulated only if these conditions are met.
-
-<div>$$IF\,\,\,\left[ {\,({{\dot m}_s}\,\,\, > \,\,\,0)\,\,.\,\,\,and.\,\,\,({{\dot m}_a} > \,\,\,0)\,\,.and.\,\,(Schedule\,\, = \,\,\,ON)\,.and.\,\,\,({Q_{ZC}}\,\, > \,\,0.0)\,} \right]\,\,\,THEN$$</div>
-
-If the heating demand from the zone-heating coil is greater than coil capacity, then the heating coil is undersized, and the coil can only deliver its maximum heating capacity to the zone.  In this case the heating demand on the coil is set equal to this lower value of maximum heating capacity.  If the above is not true then the simulation ignores this statement and proceeds to the next one.
-
-<div>$$IF\,\,\,\left[ {\,\,\,({Q_{ZC}}\,\, > \,\,{Q_{Z{C_{Max}}}})} \right]\,\,\,\,\,\,THEN\,\,\,\,\,\,\left[ {{Q_{ZC}} = \,\,{Q_{Z{C_{Max}}}}} \right]$$</div>
-
-The following equation calculates the steam mass flow rate required by the coil.  This flow rate is required to meet the heating requirements for the zone.  This value of mass flow is requested from the splitter outlet.
-
-<div>$${\dot m_{zc}}\,\,\,\, = \,\,\,\,\,\frac{{{Q_{zc}}}}{{{h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}}}}$$</div>
-
-If the calculated value of steam mass flow with the previous equation is greater than the maximum inlet steam flow that the splitter can provide to the coil at that time step.  Then the requested coil flow rate is set equal to the inlet steam flow rate.  This is the maximum amount of steam that can be supplied to the coil at this moment.  The coil can provide heating capacity equal to this limited amount of steam.  If the requested flow rate is less that what the splitter can provide then the program ignores the logic of the IF Loop Below
-
-<div>$$IF\,\,({\dot m_{zc}}\,\, > \,\,{\dot m_{in}})\,\,THEN\,\,(\,\,\,{\dot m_{zc}}\,\, = \,\,{\dot m_{in}})$$</div>
-
-Re-Calculating the coil heating capacity with the lower value of steam mass flow rate.
-
-<div>$${Q_{ZC}} = {\dot m_{zc}}\,\, \times \,\,({h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}})$$</div>
-
-<div>$$END\,\,IF$$</div>
-
-The following equations calculate the outlet condensate-water and outlet air temperatures to the zone based on the amount of heating capacity provided by the coil.
-
-      <div>$$T{w_{out}} = \,\,T{s_{in}}\,\, - \,\,\,\Delta {T_{sc}}$$</div>
-
-<div>$$T{a_{out}}\,\,\, = \,\,T{a_{in}}\,\, + \,\,\,\frac{{{Q_{zc}}}}{{\,{{\dot m}_a}\, \times \,\,\,{c_{p,a}}}}$$</div>
-
-<div>$$ELSE$$</div> Else the coil is not running and in this case set outlets to inlets.
-
-<div>$${\dot m_s} = 0\,,\,\,\,{\dot m_a} = 0\,,\,\,\,\,\,\,\,\,\,\,\,\,{Q_{zc}} = 0,\,\,\,\,\,\,\,\,\,\,\,\,T{w_{out}} = T{s_{in\,\,,\,\,\,\,}}\,\,\,\,\,\,T{a_{out}} = T{a_{in}}$$</div>
-
-
-
-<div>$$END\,\,IF$$</div>
-
-
-
-<span>\(END\,\,IF\)</span> End IF for the zone load controlled coil.
-
-
-
-#### Steam coil is temperature controlled.
-
-<div>$$IF\,\,\,\,\,(Coil\, = TemperatureControlled)\,\,\,\,\,\,THEN\,$$</div>
-
-Check for operational conditions and continue simulation further.  The operational conditions are the inlet mass flow rates of steam and air to the coil, the user schedule to the coil and delta temp exists between the setpoint and air inlet temperature.  The coil is simulated only if these conditions are met.
-
-<div>$$IF\,\left[ \begin{array}{l}\,({{\dot m}_s}\,\,\, > \,\,\,0)\,\,.\,and.\,({{\dot m}_a} > \,\,\,0)\,\,.and.\,\,(Schedule\,\, = \,\,\,ON)\,.and.\,\\\,\,({T_{SP}} - T{a_{in}})\,\, > \,\,0.0001)\,\end{array} \right]\,THEN$$</div>
-
-Calculate the heating load on the coil using setpoint and inlet air temperatures.
-
-<div>$${Q_{al}}\,\, = \,\,\,{\dot m_a}\, \times \,\,\,C{p_a}\,\, \times \,\,\,\,[\,\,{T_{sp}}\,\, - \,\,\,{T_a}]$$</div>
-
-The logic loop for temperature-controlled coil begins here.  In case the heating load on the coil is negative, which might occur if the setpoint is below the air inlet temperature, the coil operation needs to be shut off.
-
-<div>$$IF\,\,({Q_{al}}\,\,\, &lt; \,\,\,\,0.0)\,\,\,\,THEN$$</div>
-
-Assigning the inlet to outlet and mass flows to zero shuts off the coil operation.
-
-<div>$${\dot m_s} = 0\,,\,\,\,{\dot m_a} = 0\,,\,\,\,\,\,\,\,\,\,\,\,\,{Q_{al}} = 0,\,\,\,\,\,\,\,\,\,\,\,\,T{w_{out}} = T{s_{in\,\,,\,\,\,\,}}\,\,\,\,\,\,T{a_{out}} = T{a_{in}}$$</div>
-
-If air loop coil load is greater than maximum coil load calculated at maximum steam mass flow rate, in such case the coil is undersized, the coil can only deliver to the air loop its maximum heating capacity.  Setting the air loop coil load equal to maximum load on coil.  If this is not the case then the program ignores this ELSE IF block and proceeds to the next one.
-
-<div>$$ELSE\,\,\,IF\,\,\,\,\left[ {\,\,\,({Q_{al}}\,\, > \,\,{Q_{a{l_{Max}}}})} \right]\,\,\,\,\,\,THEN\,\,\,\,\,\,\left[ {{Q_{al}} = \,\,{Q_{a{l_{Max}}}}} \right]$$</div>
-
-If the heating coil is under sized then it can only provide its maximum heating capacity, in this case the air temperature will be below the setpoint, and is calculated based on this maximum allowed value of heat transfer.  Calculating the air and water outlet temperatures.
-
-<div>$$T{a_{out}}\,\,\, = \,\,T{a_{in}}\,\, + \,\,\,\frac{{{Q_{al}}}}{{\,\,{{\dot m}_a}\, \times \,\,\,{c_{p,a}}}}$$</div>
-
-<div>$$T{w_{out}} = \,\,T{s_{in}}\,\, - \,\,\,\Delta {T_{sc}}$$</div>
-
-Determining the mass flow rate of steam required by the undersized coil.  This value of mass flow is requested from the splitter outlet.
-
-<div>$${\dot m_{al}}\,\,\,\, = \,\,\,\,\,\frac{{{Q_{al}}}}{{{h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}}}}$$</div>
-
-A check is introduced to determine if this requested mass flow rate is greater than what the splitter outlet can provide to the coil at that particular time step of simulation.  In this case the requested value of steam mass flow is greater that what the splitter can provide to that coil, subsequently set the requested coil flow rate equal to the inlet steam flow rate, delivered to the coil by the splitter.  This is the maximum amount of steam that can be supplied to the coil at this moment.  If the requested flow rate is less that what the splitter can provide then the program ignores the logic of the IF Loop.
-
-<div>$$IF\,\,\,({\dot m_{al}}\,\, > \,\,{\dot m_{in}})\,\,THEN\,\,(\,\,\,{\dot m_{al}}\,\, = \,\,{\dot m_{in}})$$</div>
-
-Re-Calculating the coil heating capacity and air outlet temperature with the lower value of steam mass flow rate provided by the splitter.
-
-<div>$${Q_{al}}\,\,\,\, = \,\,\,\,{\dot m_{al}}({h_{fg}} + {c_{p,w}} \times \Delta {T_{sc}})$$</div>
-
-<div>$$T{a_{out}}\,\,\, = \,\,T{a_{in}}\,\, + \,\,\,\frac{{{Q_{al}}}}{{\,\,{{\dot m}_a}\, \times \,\,\,{c_{p,a}}}}$$</div>
-
-<div>$$End\,\,\,IF$$</div>
-
-If the above two IF ELSE block are not true, then the coil is perfectly sized, the splitter can provide the required mass flow rate to the coil, and the setpoint temperature can be maintained as desired.
-
-<div>$$ELSE$$</div>
-
-The ideal case where the coils can meet the required setpoint temperature.  Setting the outlet air temperature to the setpoint, calculating the water outlet temperature and the required steam mass flow rate.
-
-<div>$$T{a_{out}}\,\,\, = \,\,{T_{SP}}$$</div>
-
-<div>$$T{w_{out}} = \,\,T{s_{in}}\,\, - \,\,\,\Delta {T_{sc}}$$</div>
-
-<div>$${Q_{al}}\,\, = \,\,\,{\dot m_a}\, \times \,\,\,{c_{p,a}}\,\, \times \,\,\,\,[\,\,{T_{sp}}\,\, - \,\,\,{T_a}]$$</div>
-
-<span>\(END\,\,IF\)</span>   End IF statement, for the air coil heating loop.
-
-<span>\(END\,\,IF\)</span>         End IF statement for the operating condition loop
-
-<span>\(END\,\,IF\)</span>   End IF statement for the Temperature Setpoint Controlled Coil
-
-The steam coil model encapsulates the above described control logic along with the other necessary simulation code for reading the user inputs and the code for reporting the simulation results.
-
-\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*PSEUDO CODE SECTION ENDS\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-The two main types of coil control discussed above are followed by common simulation code in the coil model.  This code calculates the loop losses occurring due to flashing of steam across the steam trap, isenthalpic expansion occurring across the steam trap due to pressure difference, and loss occurring due to condensate sub cooling returning back to the boiler.  The above-mentioned two processes are explained in Figure 129 as process 3-4’ and 4-5.
-
-The loop loss calculation is included in the steam coil simulation model, because the degree of subcooling in the return piping for the condensate is solely a function of the coil location.  In practical applications a coil, which is further away from boiler would return back condensate at much lower temperatures compared to coil, which is closer to boiler.  Hence for user ease it makes perfect sense to include this input into the coil and calculate the pump inlet conditions in the steam coil simulation model itself.
-
-The loop losses in the EnergyPlus steam system is calculated by determining the enthalpy difference between point 3 and 5.  The simulation code that determines the loop loss is common to both the coil models, this helps determine the condensate pump inlet conditions.
-
-The following equation is used to calculate condensate enthalpy at coil outlet, point 3 in Figure 129.  Point 2 represents condensed steam; enthalpy at this point is calculated directly by EnergyPlus property routines.
-
-<div>$${h_{f3}} = {h_{f2}} - {c_{p,w}} \times \Delta {T_{SC}}$$</div>
-
-Point 4 is at atmospheric pressure, enthalpy at this is calculated directly by EnergyPlus property routines.  It is saturation enthalpy of steam at quality equal to 0.0 and saturation temperature at atmospheric pressure.
-
-Point 5 is inlet to the pump; enthalpy at this point is calculated with the following equation  The delta temperature represents the degree of loop subcooling occurring during condensate return back to the pump.
-
-<div>$${h_{f5}} = {h_{f4}} - {c_{p,w}} \times \Delta {T_{LSC}}$$</div>
-
-Subsequently loop loss for each coil would be enthalpy difference between 3 and 5 and is calculated using the following equation
-
-<div>$$\Delta {Q_{loss}} = {\dot m_s}\,\,\, \times \,\,\,\,({h_{f3}} - {h_{f5}})$$</div>
-
-The total loop loss would be a summation of the individual losses occurring for each of the steam coils, this is the unavoidable loss in current steam system.
-
-A simple schematic describing the coil framework, inlet and outlet conditions to the coil and the flow rate resolution is shown in Figure 130.  Five zone coils and one air loop coil are described in the picture, Qzone is calculated by EnergyPlus heat balance and it is the input to the zone coils, while in air loop coil the Qal is calculated within the simulation model
-
-
-
-![SchematicSteamCoil](media/image2032.png)
-
-Figure 130. Schematic of Steam Coil Connection to the Steam Loop
-
-As depicted in the figure above the steam condenses on entering the coils, sub cools by the specified amount and leaves the heat exchanger as water.  The steam in the heat exchanger at any moment has to condense eventually since steam trap at the outlet to coil permits only water to leave the coil.  Steam traps being an essential part of the loop are modeled by controlling the coil outlet condition at quality equal to 0.0.  Subsequently the amount of heat transferred to air is a direct function of latent heat and the degree of sub cooling desired by the user.
-
-#### Model Assumptions
-
-The steam coils works on two basic assumptions, firstly, it’s assumed that perfect latent heat transfer takes place over every time step, secondly, the user specified degree of subcooling occurs in the coil.  Steam coils always use steam traps- purpose of which is to only let water out of the coil, hence the modeler knows with certainty the outlet dryness faction of steam coil is at quality equal to 0.0, because water leaves coil.  Hence the heat transfer is equal to latent heat of steam, which is independent of UA value of coil when averaged over time step of EnergyPlus simulation.
-
-In practice there is 1% to 2 % sub cooling of the outlet water stream, the user with desired degree of subcool input accounts for this, subsequently UA calculation for the coil model become superfluous and is neglected in the EnergyPlus model.
-
-Ideally for sub-cooling UA would play an important role, however sub cooling in steam coil constitutes negligible amount of heat transfer, hence this model avoids the UA calculation.  This is a very reasonable assumption since sensible heat transfer is barely 1% to 2 % of the total heat transfer in steam coils, simply due to large latent heat capacity of coil. NOTE in his thesis he gives a little example here which is probably not necessary for the Docs.
-
-### Condensate Pump
-
-The steam loop operates at a pressure differential over the gaseous and liquid part of the loop; subsequently a condensate pump is required to pump the condensed steam back to the boiler at the required pressure.  Two main reasons for condensed steam to be returned to the boiler is energy savings in reheating water since the water is at high temperature, secondly the water is treated by chemicals to prevent corrosion in the pipes and equipment.  This is an expensive process and therefore it’s economical to reuse the chemically treated water.
-
-#### Description of Pump Model
-
-The pump model designed in EnergyPlus is a variable speed condensate pump.  Condensation of steam produces water, this takes place at variable rate hence the return water flow rate would be variable but constant when averaged over a time step.  Condensate pumps operate intermittently; the pump will run at its capacity if a load/flow rate is sensed and will shut off if there is no load on the loop.
-
-The condensate pump essentially operates between maximum and minimum flow rates, which are the physical limits of the device.  The pump is designed to meet the flow request made by demand side components, which are the coils in case of steam system.
-
-The main difference between the variable volume pump and the constant volume pump is the Part Load Performance Curve.  The fraction of full load power is determined by the third order equation, which follows:
-
-<div>$${P_{Frac}}\,\, = \,\,{C_1} + \,{C_2} \times PLR\,\, + \,\,\,{C_3} \times PL{R^2}\,\, + \,\,{C_4} \times PL{R^3}$$</div>
-
-In preceding equation, PLR stands for part load ratio while C1 to C4 are pump- part load coefficients.  The following five equations describe the pump operation and calculation of pump output variables such as total power, shaft power and pump heat to fluid etc.
-
-<div>$$\dot V\,\, = \,\,\frac{{\,\dot m\,}}{{{\rho_w}}}$$</div>
-
-Using the previous equation the pump volume flow rate is determined; the user enters the value of the maximum and minimum volume flow rate.
-
-The pump part load ratio is a function of the pump volume flow rate at any instance determined by the loop and the pump nominal volume flow rate, which is a user input.  The following equation calculates the Part Load Ratio (PLR).
-
-<div>$$PLR = \,\frac{{\dot V}}{{{{\dot V}_{nom}}}}$$</div>
-
-The pump power is calculated as described in following equation.  Pump power is a product of fractional full load power and pump nominal power use.  Fractional full load power is calculated in a preceding equation while pump nominal power is a user input to the model.
-
-<div>$$P = {P_{Frac}} \times {P_{Nom}}$$</div>
-
-The shaft power is simply the product of the pump power and motor efficiency, this is required to calculate the heat generated and delivered to the fluid being pumped.  The following equation is used to calculate pump shaft power.
-
-<div>$${P_S}\,\,\, = P\,\,\,\, \times \,\,\,\,{\eta_m}$$</div>
-
-The model assumes that all heat generated and lost ends up in the fluid to the loop, this assumption is necessary since EnergyPlus operates on a closed loop.  The following equation is used to calculate the pump heat to the fluid, which raises the condensate temperature.  The pump motor efficiency is defined by the user input and the fractional motor loss to fluid is the amount of heat generated by the pump motor that is added to the fluid loop (as opposed to being lost to the environment where the pump is located).  FracMotorLossToFluid is also a user input
-
-<div>$${P_H} = {P_S}\,\,\, + \,(\,P\,\, - {P_S}) \times {F_{mf}}$$</div>
-
-The shaft power relates to the increase in head through the pump to the loop operating pressure.  The head lost through the piping network due to frictional heat, represents the heat gain by the fluid throughout the network.  .  For model simplicity, this heat is added along with the heat resulting from the pump motor.  The difference between the pump power and the shaft power is the inefficiency of the pump, or the amount of energy input into the pump that the motor converts to heat rather than mechanical energy.  Some of this heat is added to the fluid being pumped.  These two above-mentioned terms are used in the PumpHeatToFluid equation for calculating P<sub>H</sub> shown above.
-
-A simple energy balance over the pump based on the pump inlet conditions and flow rate is used to calculate the pump outlet temperature.  The condensate outlet temperature from the pump is slightly higher than inlet due to the heat dissipation to the fluid steam during pumping action.  This is calculated in the following equation.  The pump water outlet temperature is the boiler inlet temperature.
-
-<div>$${T_{{w_{out}}}} = {T_{{w_{in}}}}\,\,\, + \,\,\,\,\,\frac{{{P_H}}}{{\,\dot m\,\,\, \times \,\,\,\,{c_{p,w}}}}$$</div>
-
-Pump control is an important part of the steam loop.  Existing control structure from EnergyPlus has been utilized to operate the condensate pump.  The pump is simulated first on the supply side of the loop after the demand side loop has determined what the demand on the loop will be.
-
-A simple schematic describing the flow across the pump is shown in the following figure
-
-![SchmaticCondensatePump](media/image2040.png)
-
-Figure 131.  Schematic of Condensate Pump in Steam Loop
-
-#### Model Assumptions
-
-Due to the fact that a pump is a mechanical device that acts on the fluid it is circulating, it causes the fluid temperature rise.  The EnergyPlus model assumes that all pressure increase caused by the pump will eventually be lost due to friction, and that friction will be added as heat to the fluid.  Although the plant and condenser loops in steam systems are simple pressure-based models, a simplifying assumption has be made in EnergyPlus to assume the heat resulting from the pump itself and from friction throughout the loop is added at the fluid being pumped.  In case of steam, this assumption is easily justified because the volume flow rate of water is very small in the loop.
-
-### Steam Pipe
-
-#### Description of Model
-
-The steam pipe essentially serves as “energy carrier� and transfers the node conditions from one point of the pipe to another.  It’s simply a node inlet to node outlet connection, transferring values from inlet to outlet.  The pipe forms an important part of the framework connecting various equipments from the supply to demand side and inlet and outlets of the equipments.
-
-The steam pipe supports two additional properties, which are pressure and quality, unlike its water counterpart.  Pipe simulation model in EnergyPlus is hardwired to water as a fluid type; this necessitated the development of similar model supporting pressure and quality for the steam system.
-
-#### Model Assumptions
-
-The piping network in the developed steam system is assumed to perfectly distribute steam, return the condensate, and remove air and non-condensable gases.  It is also assumed that the pipes are sized to distribute steam not only at full load but also at partial loads and excess loads that can occur during system warm up.
-
-The steam pipe is perfect and there is no losses occurring in transportation.  This assumption was necessitated since if pipe losses were accounted for, the loss would have to be distributed into the zone, which would be a very complex issue in itself, since in EnergyPlus the pipes are unaware of their locations and simply serve as connectors.
diff --git a/doc/src/docs/EngineeringReference/10-Sizing.md b/doc/src/docs/EngineeringReference/10-Sizing.md
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-
-Loop, Equipment Sizing and other Design Data
-============================================
-
-The importance of correct equipment sizing is often ignored in discussions of building simulation methods. The lack of reliable, efficient and flexible sizing calculations can present a serious barrier to the adoption and acceptance of building simulation programs. This section describes the sizing methodology implemented in EnergyPlus. This method includes:
-
-1.    A zone by zone heat balance load and air-flow calculation for multiple design days;
-
-2.    Significant user control with modest input requirements;
-
-3.    Zone, system and plant level calculations of design heating and cooling capacities and fluid flow rates;
-
-4.    Modular, component-specific sizing algorithms for each HVAC component.
-
-5.    Options for monitoring how the initial sizes operate over multiple design days and then making adjustments and repeating plant level calculations
-
-Sizing Manager
---------------
-
-The sizing calculations in EnergyPlus are managed by a sizing manager contained in the software module *SizingManager*. The main sizing manager routine *ManageSizing* is called from *ManageSimulation* before the annual simulation sequence is invoked. *ManageSizing* performs the following tasks.
-
-*  By calling *GetSizingParams*, *GetZoneSizingInput*, *GetSystemSizingInput* and *GetPlantSizingInput* reads in all the user sizing input contained in objects *Sizing:Parameters*, *Sizing:Zone*, *Sizing:System* and *Sizing:Plant*. These objects and their data are described in the EnergyPlus Input Output Reference, Group Design Objects.
-
-*  Set the *ZoneSizingCalc* flag equal to *true*.
-
-*  Loop over all the sizing periods by each day. **This starts the zone design calculations.**
-
-    * Call *UpdateZoneSizing(BeginDay)* to initialize zone design load and flow rate  sequences.
-
-    * Loop over hours in the day
-
-        * Loop over zone time steps in each hour
-
-            * Call *ManageWeather* to obtain outside conditions for this time-step.
-
-            * Call *ManageHeatBalance* to do a full heat balance calculation for each zone. The call to *ManageHeatBalance* also brings about an HVAC simulation. *ZoneSizingCalc = true* signals the *HVACManager* to ignore the real HVAC system and instead run the ideal zonal system (described below) used to calculate design loads and flow rates. HVACManager also calls *UpdateZoneSizing(DuringDay)* to save the results of the ideal zonal system calculation in the design load and flow rate sequences.
-
-        * Call *UpdateZoneSizing(EndDay)* to calculate peaks and moving averages from the zone design sequences for each design day.
-
-* Call *UpdateZoneSizing(EndZoneSizingCalc)* to calculate for each zone the peak heating & cooling loads and flow rates over all the sizing periods (design days and sizing periods from the weather file, if specified). The corresponding design load and flow rate sequences are saved for use in the system design calculations. **This ends the zone design calculations.**
-
-*  Set the *SysSizingCalc* flag equal to *true*.
-
-* Call *ManageZoneEquipment* and *ManageAirLoops* to read in the zone and central system inputs needed for the system design calculations. The program needs enough information to be able to figure out the overall air loop connectivity.
-
-*  Loop over all the sizing periods by each day. **This starts the system design calculations.**
-
-    * Call *UpdateSysSizing(BeginDay)* to initialize system design load and flow rate  sequences.
-
-    * Loop over hours in the day
-
-        * Loop over zone time steps in each hour
-
-            * Call *ManageWeather* to obtain outside conditions for this time-step.
-
-            * Call *UpdateSysSizing(DuringDay)* to save the results of the system design calculations in the system design load and flow rate sequences.
-
-    * Call *UpdateSysSizing(EndDay)* to calculate peaks and moving averages from the system design sequences for each sizing period.
-
-* Call *UpdateSysSizing(EndSysSizingCalc))* to calculate for each system the peak heating & cooling loads and flow rates over all the sizing periods (design days and sizing periods from the weather file, if specified). The corresponding design load and flow rate sequences are saved for use in the component sizing calculations. **This ends the system design calculations.**
-
-* And this ends the tasks of the Sizing Manager.
-
-HVAC Sizing Simulation Manager
-------------------------------
-
-After the Sizing Manager has completed its initial pass, all the data needed to complete a running model should be available and the program is ready to run the main simulation(s).  However, as of Version 8.3 there is now an option of applying some advanced sizing calculations using what are called HVAC Sizing Simulations.  
-
-With this new sizing method we distinguish between different kinds of simulations and introduce some new terminology.  The Primary Simulations are the main simulations that are the final version of the model to be run.  Prior to Version 8.3, these are just the usual simulations with the final results.  When the program is running the zone heat balance model over the sizing periods for zone sizing (for step 3 in the Sizing Manager description above), we call those Ideal Loads Sizing Simulations.  When the program is running the zone heat balance model over the sizing periods for component loads calculations we call those Ideal Component Loads Simulations. HVAC Sizing Simulations are a kind of simulation, where the program creates copies of sizing periods and runs them as complete EnergyPlus simulations with the most current equipment sizes and full HVAC systems.  The advanced sizing algorithms monitor what occurred during those sizing periods and determines if new size results are needed and signals systems and components to repeat their sizing calculations.  The process can repeat in an iterative manner and a Sizing Pass refers to a set of the HVAC Sizing Simulations for each of the sizing periods (e.g. two design days).  
-
-If the user has selected a sizing option that requires HVAC Sizing Simulations the main ManageSimulation will call ManageHVACSizingSimulation before going on to the main simulations.  
-
-* Instantiate a new HVACSizingSimulationManager object.  
-
-* Call DetermineSizingAnalysesNeeded(). This checks what user input and decides what, if anything, needs to be done for advanced sizing algorithms.   This involves, for example, checking the input in Sizing:Plant object to see if coincident sizing option has been selected.
-
-* Call SetupSizingAnalyses().  This method creates the data logging apparatus needed to monitor operation during HVAC Sizing Simulations.  Individual sizing algorithms include selecting specific variables, such as system node states or load output variables, that will be recorded. 
-
-* Loop over some number of Sizing Passes.  The set of sizing periods, run as HVAC Sizing Simulations, can iterate up to a maximum limit on the number of passes
-
-    * Loop over all the sizing periods by each day.  This runs the HVAC Sizing Simulations which have basically the same set of calls as are used for marching through time and calling of EnergyPlus modeling for the Primary Simulations (in ManageSimulation).
-
-        * Call PostProcessLogs().  This method applies running averages (if desired) and averages system timestep data to fill zone timestep data in the records.
-
-        * Call ProcessCoincidentPlantSizeAdjustments(). This method retrieves data from the logs and calls for the coincident plant sizing algorithm to execute. Set flag if the sizing analyses request another Sizing Pass.  (See the section below on Coincident Plant Sizing.)
-
-        * Call RedoKickOffAndResize(). The methods calls SetupSimulation() and sets flag to signal that system and component level sizing methods need to be called again.  These are fake timesteps used to initialize and are not part of a Simulation.
-
-    * Break out of Sizing Pass loop if size results did not change or the limit on Sizing Passes has been reached.
-
-* Empty HVACSizingSimulationManager object to free memory
-
-Currently the only application for HVAC Sizing Simulations is to improve the sizing of plant loops using the Coincident sizing option.  However this approach may be expanded in the future to extend advanced sizing methods to air-side equipment. 
-
-
-Zone Design Loads and Air Flow Rates
-------------------------------------
-
-### Overview
-
-There is no single best way to establish design HVAC flow rates and size HVAC equipment. Different building designs, climates, and HVAC systems will impose varying constraints on the designer. The method used to size an HVAC system in a hot, moist climate such as Miami will be different than the method used for a building in Albuquerque. The type of building is also relevant - a simple watts per square foot loads estimate could be adequate for a building containing a network server farm while a detailed, dynamic loads simulation would be necessary for a passive solar building. In the end the designer's experience and engineering judgement will play an important role in any sizing calculation.
-
-HVAC equipment sizing begins with the calculation of space heating and cooling loads. A space cooling  (heating) load is defined as the rate at which heat must be removed (added) to a space to maintain a constant temperature. The current industry standard method for calculating space loads is the *heat balance method*  [ASHRAE Fundamentals (2001), page 29.1; Pedersen et al., (1997); Pedersen (2001). Since EnergyPlus is a heat balance based simulation program it is straightforward for the program to use this method for calculating zone loads.
-
-### Zone Design Data Arrays
-
-The zone design data arrays are:
-
-*ZoneSizingInput(i)* stores the input data from the Sizing:Zone objects.
-
-*CalcZoneSizing(i,j)* stores the results of the zone design calculations for all zones and all design days. The index i is for the controlled zones, j for design days.
-
-*CalcFinalZoneSizing(i)* stores the results of the zone design calculations for the peak heating and cooling cases for each zone. The index i is for the controlled zones.
-
-*ZoneSizing(i,j)* corresponds to *CalcZoneSizing* but includes the effect of the user specified sizing factor or user specified zone design flow rate.
-
-*FinalZoneSizing(i)* corresponds to *CalcFinalZoneSizing* but includes the effect of the user specified sizing factor or user specified zone design flow rate.
-
-The data stored in *CalcZoneSizing*, *CalcFinalZoneSizing*, *ZoneSizing* and *FinalZoneSizing* includes the following data items.
-
-
-
-Table 40.  Zone Sizing Data
-
-<table class="table table-striped">
-<tr>
-<th>Name</td>
-<th>Description</td>
-</tr>
-<tr>
-<td>All the data from ZoneSizingInput</td>
-<td> </td>
-</tr>
-<tr>
-<td>DesHeatMassFlow</td>
-<td>the zone design heating air mass flow rate in [kg/s]</td>
-</tr>
-<tr>
-<td>DesCoolMassFlow</td>
-<td>the zone design cooling air mass flow rate in [kg/s]</td>
-</tr>
-<tr>
-<td>DesHeatLoad</td>
-<td>the zone design heating load in [W]</td>
-</tr>
-<tr>
-<td>DesCoolLoad</td>
-<td>the zone design cooling load in [W]</td>
-</tr>
-<tr>
-<td>DesHeatDens</td>
-<td>the zone design heating air density [kg/m<sup>3</sup>]</td>
-</tr>
-<tr>
-<td>DesCoolDens</td>
-<td>the zone design cooling air density [kg/m<sup>3</sup>]</td>
-</tr>
-<tr>
-<td>DesHeatVolFlow</td>
-<td>the zone design heating air volume flow rate [m<sup>3</sup>/s]</td>
-</tr>
-<tr>
-<td>DesCoolVolFlow</td>
-<td>the zone design cooling air volume flow rate [m<sup>3</sup>/s]</td>
-</tr>
-<tr>
-<td>DesHeatCoilInTemp</td>
-<td>zone heating coil design air inlet temperature [C]</td>
-</tr>
-<tr>
-<td>DesCoolCoilInTemp</td>
-<td>zone cooling coil design air inlet temperature [C]</td>
-</tr>
-<tr>
-<td>DesHeatCoilInHumRat</td>
-<td>the zone heating coil design air inlet humidity ratio [kg/kg]</td>
-</tr>
-<tr>
-<td>DesCoolCoilInHumRat</td>
-<td>the zone cooling coil design air inlet humidity ratio [kg/kg]</td>
-</tr>
-<tr>
-<td>HeatMassFlow</td>
-<td>current zone heating air mass flow rate at the HVAC time step [kg/s]</td>
-</tr>
-<tr>
-<td>CoolMassFlow</td>
-<td>current zone cooling air mass flow rate at the HVAC time step [kg/s]</td>
-</tr>
-<tr>
-<td>HeatLoad</td>
-<td>Current zone heating load [W]</td>
-</tr>
-<tr>
-<td>CoolLoad</td>
-<td>Current zone cooling load [W]</td>
-</tr>
-<tr>
-<td>HeatZoneTemp</td>
-<td>Current zone temperature during heating [C]</td>
-</tr>
-<tr>
-<td>HeatZoneRetTemp</td>
-<td>current zone return temperature during heating [C]</td>
-</tr>
-<tr>
-<td>CoolZoneTemp</td>
-<td>Current zone temperature during cooling [C]</td>
-</tr>
-<tr>
-<td>CoolZoneRetTemp</td>
-<td>current zone return temperature during cooling [C]</td>
-</tr>
-<tr>
-<td>HeatZoneHumRat</td>
-<td>Current zone humidity ratio during heating [C]</td>
-</tr>
-<tr>
-<td>CoolZoneHumRat</td>
-<td>Current zone humidity ratio during cooling [C]</td>
-</tr>
-<tr>
-<td>ZoneTempAtHeatPeak</td>
-<td>zone temperature at maximum heating [C]</td>
-</tr>
-<tr>
-<td>ZoneRetTempAtHeatPeak</td>
-<td>zone return temperature at maximum heating [C]</td>
-</tr>
-<tr>
-<td>ZoneTempAtCoolPeak</td>
-<td>zone temperature at maximum cooling [C]</td>
-</tr>
-<tr>
-<td>ZoneRetTempAtCoolPeak</td>
-<td>zone return temperature at maximum cooling [C]</td>
-</tr>
-<tr>
-<td>ZoneHumRatAtHeatPeak</td>
-<td>zone humidity ratio at maximum heating [kg/kg]</td>
-</tr>
-<tr>
-<td>ZoneHumRatAtCoolPeak</td>
-<td>zone humidity ratio at maximum cooling [kg/kg]</td>
-</tr>
-<tr>
-<td>TimeStepNumAtHeatMax</td>
-<td>zone time step number (in the day) at the heating peak</td>
-</tr>
-<tr>
-<td>TimeStepNumAtCoolMax</td>
-<td>zone time step number (in the day) at the cooling peak</td>
-</tr>
-<tr>
-<td>HeatDDNum</td>
-<td>design day index of design day causing heating peak</td>
-</tr>
-<tr>
-<td>CoolDDNum</td>
-<td>design day index of design day causing cooling peak</td>
-</tr>
-<tr>
-<td>MinOA</td>
-<td>design minimum outside air [m3/s]</td>
-</tr>
-<tr>
-<td>HeatFlowSeq(i)</td>
-<td>daily sequence of zone heating air mass flow rates (zone time step) [kg/s]</td>
-</tr>
-<tr>
-<td>CoolFlowSeq(i)</td>
-<td>daily sequence of zone cooling air mass flow rates (zone time step) [kg/s]</td>
-</tr>
-<tr>
-<td>HeatLoadSeq(i)</td>
-<td>daily sequence of zone heating loads (zone time step) [W]</td>
-</tr>
-<tr>
-<td>CoolLoadSeq(i)</td>
-<td>daily sequence of zone cooling loads (zone time step) [W]</td>
-</tr>
-<tr>
-<td>HeatZoneTempSeq(i)</td>
-<td>daily sequence of zone temperatures (heating, zone time step) [C]</td>
-</tr>
-<tr>
-<td>HeatZoneRetTempSeq(i)</td>
-<td>daily sequence of zone return temperatures (heating, zone time step) [C]</td>
-</tr>
-<tr>
-<td>CooltZoneTempSeq(i)</td>
-<td>daily sequence of zone temperatures (cooling, zone time step) [C]</td>
-</tr>
-<tr>
-<td>CoolZoneRetTempSeq(i)</td>
-<td>daily sequence of zone return temperatures (cooling, zone time step) [C]</td>
-</tr>
-<tr>
-<td>HeatZoneHumRatSeq(i)</td>
-<td>daily sequence of zone humidity ratios (heating, zone time step) [kg/kg]</td>
-</tr>
-<tr>
-<td>CoolZoneHumRatSeq(i)</td>
-<td>daily sequence of zone humidity ratios (cooling, zone time step) [kg/kg]</td>
-</tr>
-
-</table>
-
-
-
-### Zone Design Load Calculation
-
-As described in the preceding section, the Sizing Manager initiates the zone design calculation by looping over all of the design days and calling the Heat Balance Manager for each zone time-step in each design day. The Heat Balance manager then causes the HVAC Manager to be called in a manner identical to a normal simulation. The *ZoneSizingCalc* set to *true* signals the HVAC Manager to ignore the actual HVAC system and instead calculate the design zone loads and air flow rates using an ideal zonal system.
-
-In module *HVACManager*, subroutine *ManageHVAC* calls *SimHVAC*. *SimHVAC* checks *ZoneSizingCalc*. If it is *true*, *SimHVAC* calls *ManageZoneEquipment* and returns, rather than simulating the actual system. In turn *ManageZoneEquipment* checks if *ZoneSizingCalc* is *true*; if it is it calls *SizeZoneEquipment* rather than *SimZoneEquipment*.
-
-*SizeZoneEquipment* assumes that each controlled zone is served by an ideal air conditioning unit. This unit supplies heating or cooling air at a fixed, user input temperature and humidity (specified in the Sizing:Zone objects). The units have infinite capacity: the flow rate can be any amount.
-
-Before the ideal zone load is calculated, the function checks whether the user wants to account for the heat gain or loss caused by the ventilation air from a Dedicated Outdoor Air System (DOAS). If the user has selected *Account For Dedicated Outdoor Air = Yes* the function performs an ideal DOAS calculation. The DOAS supply temperature is set according to the user's choice of 1 of 3 possible control strategies: *NeutralSupplyAir*, *NeutralDehumidifiedSupplyAir*, or *ColdSupplyAir*. The different strategies are:
-
-  - *DOAS Control Strategy = NeutralSupplyAir*. The purpose of this strategy is to cool or heat the outdoor air (OA) to keep it between the *T<sub>l</sub>* and *T<sub>h</sub>* setpoints.
-
-  - *DOAS Control Strategy = Neutral Dehumidified Supply Air*. The purpose of this strategy is to cool and dehumidify the outdoor air, then reheat it to a "neutral" temperature so that no sensible load is imposed on the space or AHU unit. The DOAS will with this strategy handle some or all of the latent load. If the outdoor air temperature is greater than *T<sub>l</sub>* the outdoor air is cooled to *T<sub>l</sub>* and reheated to *T<sub>h</sub>*. If the outdoor air temperaure is below *T<sub>l</sub>* it is heated to *T<sub>h</sub>*.
-
-  - *DOAS Control Strategy = ColdSupplyAir*. The purpose of this strategy is to provide cool, dehumidified ventilation air to the zone. In this case the DOAS can handle part of the sensible zone cooling load as well as meet part or all of the latent load. If the outdoor air temperature is below *T<sub>l</sub>* it is heated to *T<sub>h</sub>*. If it is above *T<sub>l</sub>*, it is heated to *T<sub>l</sub>*.
-
-With the DOAS supply temperature set and the air mass flow rate set to the minimum design ventilation flow rate the heat addition rate is just 
-
-<div>$${\dot Q_{doa}} = {c_{p,air}}{\dot m_{vent,min}}({T_{sup}} - {T_z})$$</div>
-
-*UpdateSSystemOutputRequired* is then invoked to adjust the load to be met by the ideal zone system.
-
-The ideal loads calculation steps are as follows.
-
-1)    Loop over all the controlled zones.
-
-2)    If the system is active (zone temperature not in the deadband and zone load greater than 1 watt) the sign of the zone load is used to determine whether heating or cooling is required and *T<sub>in</sub>* and W*<sub>in</sub>* are set to the appropriate values from the Sizing:Zone input. When the SupplyTemperature method is specified in the Sizing:Zone object, *T<sub>in</sub>* is fixed at the cooling or heating supply temperature. When the TemperatureDifference method is selected, *T<sub>in</sub>* is calculated at each time step using the current zone air temperature. The system output *Q<sub>sys</sub>* is simply set equal to the zone demand - it is assumed that the ideal system can always meet the zone load. The air flow rate corresponding to the load is just
-
-<div>$${\dot m_{sys}} = {Q_{sys}}/({C_{p,air}} \cdot ({T_{in}} - {T_z}))$$</div>
-
-If the system is not active, the mass flow rate is set to zero and the system output is left at zero.
-
-3)    The results for each zone are stored in the zone sizing data arrays.
-
-### Updating and Adjusting the Zone Results
-
-The results from *SizeZoneEquipment* are at the system time-step and are for all design days. These results then need to be summed or averaged over the zone time-step, peak values calculated for each design day, a heating & a cooling load sequence chosen for each zone from all the design day results, possible further smoothing of results done, zone coil loads calculated, and user sizing multipliers or user specified design flows taken into account. These tasks are accomplished by the subroutine *UpdateZoneSizing*. It is called at the start of each design day (*CallIndicator = BeginDay*), at the zone time-step (*CallIndicator = DuringDay*), at the end of the design day (*CallIndicator = EndDay*) and at the end of the zone design calculation (*CallIndicator = EndZoneSizingCalc*).
-
-#### BeginDay
-
-The environment (in this case, a design day) name and number are stored in the zone sizing data structures
-
-#### DuringDay
-
-The calculated and stored sequences are summed or averaged over the zone time-step.
-
-#### EndDay
-
-(1)  Smooth the design sequences by applying a moving, fixed-width averaging window to the sequences. The width of the window is user specified in the *Sizing:Parameters* input object. The sequences that are smoothed are:
-
-(a)  *CoolFlowSeq*
-
-(b)  *CoolLoadSeq*
-
-(c)  *HeatFlowSeq*
-
-(d)  *HeatLoadSeq*
-
-(e)  *CoolZoneRetTempSeq*
-
-(f)   *HeatZoneRetTempSeq*
-
-(2)  The peak heating and cooling loads and mass & volume flow rates are extracted from each set of design sequences.
-
-(3)  Using the time of the peak and the design outside air fraction the design zone heating and cooling coil inlet temperatures and humidity ratios are calculated.
-
-(4)  For each zone, looking at the results for all of the design days, the design days that cause the peak heating and peak cooling for that zone are chosen and the corresponding design sequences and peak loads and flow rates are saved in the CalcFinalZoneSizing array. This finishes the calculated - unmodified by the user - portion of the zone design calculation.
-
-#### EndZoneSizingCalc
-
-(1)  Write out onto a comma-separated file the calculated design sequences for each zone: *HeatLoadSeq*, *CoolLoadSeq*, *HeatFlowSeq*, *CoolFlowSeq* and the corresponding peaks and volumetric flow peaks.
-
-(2)  The data in *CalcZoneSizing* and *CalcFinalZoneSizing* is moved to *ZoneSizing* and *FinalZoneSizing*. The user modifications to the calculated sizing will be applied to and stored in *ZoneSizing* and *FinalZoneSizing*.
-
-(3)  The user can modify the calculated zone design results by specifying heating and cooling sizing factors at the global or zone level or by specifying and actual design heating or cooling zone design volumetric flow rate. All of this input is treated as a sizing factor. If the user inputs a cooling design volumetric flow rate for a zone it is divided by the calculated cooling design volumetric flow rate for the zone to give a zone cooling sizing factor. Note that the user can input a zone sizing factor or a zone design flow rate - not both - so there is never a conflict.
-
-(4)  Once the zone heating and cooling sizing factors are established, the design flow and load sequences as well as peak loads and flows are multiplied by the appropriate sizing factor and stored in *ZoneSizing* and *FinalZoneSizing*. This is the data that will be used for sizing zone HVAC equipment and in the system sizing calculation.
-
-(5)  The outside air fractions are recalculated using the new user-modified design flow rates and new design zone coil inlet conditions calculated and stored. At this point the condition that the design flow rates are never allowed to be less than the minimum outside air flow rate is imposed.
-
-If *outside air method* is *flow/zone*, the input *outside air flow per zone* value will be used, even if it is zero or blank. If *outside air method* is *sum*, the sum of the *outside air flow per person* \* *DesignNumberOfPeople* + *outside air flow per area* \* *ZoneArea* will be used. If *outside air method* is *maximum*, the maximum of the *outside air flow per person* \* *DesignNumberOfPeople* and *outside air flow per area* \* *ZoneArea* will be used. If *outside air method* is *flow/person*, *outside air flow per person* will be used to calculate the design minimum outside airflow rate.
-
-If *cooling design air flow method* is *flow/zone*, then *cooling design air flow rate* will be used for the design max cooling air flow rate.  If *cooling design air flow method* is *design day*, then the design day calculation will set the design max cooling air flow rate. If  *cooling design air flow method* is *design day with limit*, then the maximum from *cooling min flow per area* and *cooling min flow* will set a lower limit on the design max cooling air flow rate. In all cases, the maximum from *cooling min flow per area*, *cooling min flow*, and *cooling min flow fraction* will set a minimum zone cooling air flow rate. In all cases the maximum design cooling air flow rate must be &gt;= to the ventilation requirement.
-
-If *heating design air flow method* is *flow/zone*, then *heating design air flow rate* will be used for the design max heating air flow rate.  If *heating design air flow method* is *design day*, then the design day calculation will set the design max heating air flow rate. If *heating design air flow method* is *design day with limit*, then the maximum from *heating max flow per area*, *heating max flow* and *heating max flow fraction* will set an upper limit on the design max heating air flow rate. The design max heating air flow rate must always be &gt;= the ventilation requirement. In each case, the outside airflow will be modified based on zone ventilation effectiveness specified in the zone sizing object.
-
-**This concludes the calculation of the zone design flow rates and loads.**
-
-### Zone HVAC Scalable Sizing
-
-For zone HVAC equipments scalable sizing applies to supply air flow rate and capacity for both cooling and heating.  The scalable sizing method allowed for supply air flow rates include: *FractionOfAutosizedCoolingAirflow*, *FractionOfAutosizedHeatingAirflow*, *FlowPerFloorArea, FlowPerCoolingCapacity*, and *FlowPerHeatingCapacity*.  The supply air flow rate scalable sizing methods are defined as follows:
-
-
-
-***FlowPerFloorArea***: the simulation engine determine the supply air flow rates from the user specified *supply air flow rates per unit floor area* and the zone floor area of the zone served by the zone HVAC equipment.
-
-
-
-***FractionOfAutosizedCoolingAirflow***: the simulation engine determines the supply air flow rates from the user specified *flow fraction* and *autosized cooling design supply air flow rate*.
-
-
-
-***FractionOfAutosizedHeatingAirflow***: the simulation engine determines the supply air flow rates from the user specified *flow fraction* and *autosized heating design supply air flow rate*.
-
-
-
-***FlowPerCoolingCapacity***: he simulation engine determines the supply air flow rates from the user specified *supply air flow per cooling capacity value* and *autosized cooling design capacity*.
-
-
-
-***FlowPerHeatingCapacity***: the simulation engine determines the supply air flow rates from the user specified *supply air flow per heating capacity value* and *autosized heating design capacity*.
-
-
-
-The scalable capacity sizing may be indirectly impacted by the scalable supply air flow rates sizing values. Moreover, the autosized cold water, hot water and steam flow rates in the parent zone HVAC objects and capacity in child components are determined using the scalable sizing method.  Scalable capacity sizing methods allowed for cooling and heating include: *CapacityPerFloorArea, FractionOfAutosizedCoolingCapacity*, *FractionOfAutosizedHeatingCapacity*. The scalable sizing capacity methods are defined as follows:
-
-
-
-**CapacityPerFloorArea**: the simulation engine determines the cooling or heating capacity from user specified capacity per floor area value and the floor area of the zone served by the zone HVAC equipment.
-
-
-
-**FractionOfAutosizedCoolingCapacity**: the simulation engine sizes the cooling capacity from the user specified *capacity fraction* and *autosized cooling design capacity* value.
-
-
-
-**FractionOfAutosizedHeatingCapacity**: the simulation engine sizes the heating capacity from the user specified *capacity fraction* and *autosized heating design capacity* value.
-
-System Design Loads and Air Flow Rates
---------------------------------------
-
-### Overview
-
-The purpose of the system design calculation is to estimate design heating and cooling loads and air flow rates for each air loop in the simulation problem. The calculation sequence for system level design loads and air flow rates resembles the calculation sequence for zone loads and air flow rates. There is an update subroutine *UpdateSysSizing* called at the beginning, during, and end  of a loop in the Sizing Manager over all the design days. The major difference is that this calculation is done at the zone time-step only. There is no idealized component calculation triggered at the system time-step as in the zone calculation. The system design calculation operates at the zone time step using the design environment weather data and the data stored in the zone sizing arrays. The results of the system design calculation are stored in the system sizing arrays described below.
-
-### System Design Data Arrays
-
-The system design data arrays are:
-
-*SysSizInput(i)* stores the input data from the Sizing:System objects.
-
-*SysSizing(i,j)* stores the results of the system design calculations for all systems and all design days. The index i is for air loops, j for design days.
-
-*CalcSysSizing(i*) stores the results of the system design calculations for the peak heating and cooling cases for each air loop. The index i is for the air loops.
-
-*FinalSysSizing(i*) corresponds to *CalcSysSizing* but includes the effect of the user specified sizing factor or user specified system design flow rate.
-
-The data stored in *SysSizing*, *CalcSysSizing* and *FinalSysSizing* includes the following data items.
-
-
-
-Table 41.  System Sizing Data
-
-<table class="table table-striped">
-<tr>
-<th>Name</td>
-<th>Description</td>
-</tr>
-<tr>
-<td>All the data from SysSizInput</td>
-<td> </td>
-</tr>
-<tr>
-<td>CoinCoolMassFlow</td>
-<td>coincident peak cooling mass flow rate [kg/s]</td>
-</tr>
-<tr>
-<td>CoinHeatMassFlow</td>
-<td>coincident peak heating mass flow rate [kg/s]</td>
-</tr>
-<tr>
-<td>NonCoinCoolMassFlow</td>
-<td>noncoincident peak cooling mass flow rate [kg/s]</td>
-</tr>
-<tr>
-<td>NonCoinHeatMassFlow</td>
-<td>noncoincident peak heating mass flow rate [kg/s]</td>
-</tr>
-<tr>
-<td>DesMainVolFlow</td>
-<td>design main supply duct volume flow [m<sup>3</sup>/s]</td>
-</tr>
-<tr>
-<td>DesHeatVolFlow</td>
-<td>design heat supply duct volume flow [m<sup>3</sup>/s]</td>
-</tr>
-<tr>
-<td>DesCoolVolFlow</td>
-<td>design cool supply duct volume flow [m<sup>3</sup>/s]</td>
-</tr>
-<tr>
-<td>SensCoolCap</td>
-<td>design sensible cooling capacity [W]</td>
-</tr>
-<tr>
-<td>TotCoolCap</td>
-<td>design total cooling capacity [W]</td>
-</tr>
-<tr>
-<td>HeatCap</td>
-<td>design heating capacity [W]</td>
-</tr>
-<tr>
-<td>PreheatCap</td>
-<td>design preheat capacity [W]</td>
-</tr>
-<tr>
-<td>MixTempAtCoolPeak</td>
-<td>mixed air temperature at the time of the cooling peak [C]</td>
-</tr>
-<tr>
-<td>MixHumRatAtCoolPeak</td>
-<td>mixed air humidity ratio at the time of the cooling peak [kg water/kg dry air]</td>
-</tr>
-<tr>
-<td>RetTempAtCoolPeak</td>
-<td>return air temperature at the time of the cooling peak [C]</td>
-</tr>
-<tr>
-<td>RetHumRatAtCoolPeak</td>
-<td>return air humidity ratio at the time of the cooling peak [kg water/kg dry air]</td>
-</tr>
-<tr>
-<td>OutTempAtCoolPeak</td>
-<td>outside air temperature at the time of the cooling peak [C]</td>
-</tr>
-<tr>
-<td>OutHumRatAtCoolPeak</td>
-<td>outside air humidity ratio at the time of the cooling peak [kg water/kg dry air]</td>
-</tr>
-<tr>
-<td>HeatMixTemp</td>
-<td>design mixed air temperature for heating [C]</td>
-</tr>
-<tr>
-<td>HeatMixHumRat</td>
-<td>design mixed air humidity ratio for heating [kg water/kg dry air]</td>
-</tr>
-<tr>
-<td>HeatRetTemp</td>
-<td>design return air temperature for heating [C]</td>
-</tr>
-<tr>
-<td>HeatRetHumRat</td>
-<td>design return air humidity ratio for heating [kg water/kg dry air]</td>
-</tr>
-<tr>
-<td>HeatOutTemp</td>
-<td>design outside air temperature for heating [C]</td>
-</tr>
-<tr>
-<td>HeatOutHumRat</td>
-<td>design outside air humidity ratio for heating [kg water/kg dry air]</td>
-</tr>
-<tr>
-<td>HeatFlowSeq(i)</td>
-<td>daily sequence of system heating air mass flow rate (zone time step) [kg/s]</td>
-</tr>
-<tr>
-<td>CoolFlowSeq(i)</td>
-<td>daily sequence of system cooling air mass flow rate (zone time step) [kg/s]</td>
-</tr>
-<tr>
-<td>SumZoneCoolLoadSeq(I)</td>
-<td>daily sequence of zones' summed cooling load (zone time step) [W]</td>
-</tr>
-<tr>
-<td>CoolZoneAvgTempSeq(I)</td>
-<td>daily sequence of zones flow weighted average temperature (zone time step) [W]</td>
-</tr>
-<tr>
-<td>SensCoolCapSeq(I)</td>
-<td>daily sequence of system sensible cooling capacity (zone time step) [W]</td>
-</tr>
-<tr>
-<td>TotCoolCapSeq(I)</td>
-<td>daily sequence of system total cooling capacity (zone time step) [W]</td>
-</tr>
-<tr>
-<td>HeatCapSeq(i)</td>
-<td>daily sequence of system heating capacity (zone time step) [W]</td>
-</tr>
-<tr>
-<td>PreHeatCapSeq(i)</td>
-<td>daily sequence of system preheat capacity (zone time step) [W]</td>
-</tr>
-<tr>
-<td>SysCoolRetTempSeq(i)</td>
-<td>daily sequence of system cooling return temperatures  (zone time step) [C]</td>
-</tr>
-<tr>
-<td>SysCoolRetHumRatSeq(I)</td>
-<td>daily sequence of system cooling return humidity ratios (zone time step) [kg water/kg dry air]</td>
-</tr>
-<tr>
-<td>SysHeatRetTempSeq(i)</td>
-<td>daily sequence of system heating return temperatures  (zone time step) [C]</td>
-</tr>
-<tr>
-<td>SysHeatRetHumRatSeq(I)</td>
-<td>daily sequence of system heating return humidity ratios (zone time step) [kg water/kg dry air]</td>
-</tr>
-<tr>
-<td>SysCoolOutTempSeq</td>
-<td>daily sequence of system cooling outside temperatures (zone time step) [C]</td>
-</tr>
-<tr>
-<td>SysCoolOutHumRatSeq</td>
-<td>daily sequence of system cooling outside humidity ratios (zone time step) [kg water/kg dry air]</td>
-</tr>
-<tr>
-<td>SysHeatOutTempSeq</td>
-<td>daily sequence of system heating outside temperatures (zone time step) [C]</td>
-</tr>
-<tr>
-<td>SysHeatOutHumRatSeq</td>
-<td>daily sequence of system heating outside humidity ratios (zone time step) [kg water/kg dry air]</td>
-</tr>
-</table>
-
-### System Design Flow Rate and Load Summation and Adjustment
-
-There is no system level subroutine corresponding to *SizeZoneEquipment.* Instead the system design loads and flow rates are calculated using the zone level results. The zone design flow rates for the zones served by an air loop are summed to obtain the system level design flow rates. These air flows are mixed with the system level design minimum outside air flow rate to obtain system design coil loads. These activities are all performed within the *UpdateSysSizing* subroutine in the *SimAirServingZones* module. It is called at the start of each design day (*CallIndicator = BeginDay*), at the zone time-step (*CallIndicator = DuringDay*), at the end of the design day (*CallIndicator = EndDay*) and at the end of the zone design calculation (*CallIndicator = EndSysSizingCalc*).
-
-There is a logical flag *SysSizingCalc* corresponding to *ZoneSizingCalc*.  It is used to allow the component routines to distinguish a normal simulation call from a being called during a system sizing calculation.
-
-#### BeginDay
-
-(1)  The environment (in this case, a design day) name is stored in the system sizing data structures.
-
-(2)  Loop over the zones cooled by this air loop:
-
-(a)  *NonCoinCoolMassFlow<sub>sys</sub>*=*DesCoolMassFlow<sub>zone</sub>*
-
-(3)  Loop over the zones heated by this air loop:
-
-(a)  *NonCoinHeatMassFlow<sub>sys</sub>*=*DesHeatMassFlow<sub>zone</sub>*
-
-#### DuringDay
-
-(1)  Loop over the zones cooled by this air loop:
-
-*CoolFlowSeq<sub>sys</sub>(i)* =*CoolFlowSeq <sub>zone</sub>*(i)
-
-*SysCoolRetTemp(i)*=(*CoolZoneRetTempSeq(i) \* CoolFlowSeq<sub>zone</sub>(i)*)*/ CoolFlowSeq<sub>sys</sub>(i)*
-
-*SysCoolRetHumRat(i)*=(*CoolZoneHumRatSeq(i) \* CoolFlowSeq<sub>zone</sub>(i)*)*/ CoolFlowSeq<sub>sys</sub>(i)*
-
-*FracOA=r<sub>air</sub>* \* *DesOutAirVolFlow<sub>sys</sub>*/ *CoolFlowSeq<sub>sys</sub>(i)*
-
-*T<sub>mix</sub>*=*T<sub>outside</sub>* \* *FracOA* + *SysCoolRetTemp(i)*(1 - *FracOA*)
-
-*W<sub>mix</sub>*=*W<sub>outside</sub>* \* *FracOA* + *SysCoolRetHumRat (i)*(1 - *FracOA*)
-
-*SysCoolOutTempSeq(i)*= *T<sub>outside</sub>*
-
-*SysCoolOutHumRatSeq(i)*= *W<sub>outside</sub>*
-
-Get the current (zone time-step) system cooling capacity:
-
-*SysSensCoolCap<sub>cur</sub>*=*C<sub>p,air</sub>* \* *CoolFlowSeq<sub>sys</sub>(i)*  \*( *T<sub>mix</sub>*-*T<sub>sup</sub>*)
-
-*SensCoolCapSeq(I)*= *SysSensCoolCap<sub>cur</sub>*
-
-If *SysSensCoolCap<sub>cur</sub>* is the maximum for the day so far then save *SysSensCoolCap<sub>cur</sub>*  as the design value:
-
-*SensCoolCap(i )<sub>sys</sub>*= *SysSensCoolCap<sub>cur</sub>*
-
-And save the corresponding mixed, return and outside conditions:
-
-*CoolMixTemp<sub>sys</sub>*= *T<sub>mix</sub>*
-
-*CoolMixHumRat<sub>sys</sub>*=*W<sub>mix</sub>*
-
-*CoolRetTemp<sub>sys</sub>*= *SysCoolRetTemp(i)*
-
-*CoolRetHumRat<sub>sys</sub>*= *SysCoolRetHumRat(I)*
-
-*CoolOutTemp<sub>sys</sub>*= *T<sub>outside</sub>*
-
-*CoolOutHumRat<sub>sys</sub>*= *W<sub>outside</sub>*
-
-Here     *r<sub>air</sub>*is the density of dry air at 20C and standard elevation corrected pressure, [kg/m<sup>3]</sup>;
-
-            *FracOA* is the outside air fraction;
-
-*            C<sub>p,air</sub>* is the specific heat of dry air at 20C, [J/kg-K];
-
-*            T<sub>sup</sub>* is the user specified design cooling supply temperature [C];
-
-*            T<sub>mix</sub>* is the current mixed air temperature [C];
-
-*            W<sub>mix</sub>* is the current mixed air humidity ratio [kg water / kg dry air];
-
-            *T<sub>outside</sub>* is the current outside air temperature [C];
-
-*            W<sub>outside</sub>* is the current outside air humidity ratio [kg water / kg dry air].
-
-(2)  Loop over the zones heated by this air loop.
-
-*HeatFlowSeq<sub>sys</sub>(i)* =*HeatFlowSeq <sub>zone</sub>*(i)
-
-*SysHeatRetTemp(i)*=(*HeatZoneRetTempSeq(i) \* HeatFlowSeq<sub>zone</sub>(i)*)*/*
-
-*HeatFlowSeq<sub>sys</sub>(i)*
-
-*SysHeatRetHumRat(i)*=(*HeatZoneHumRatSeq(i) \* HeatFlowSeq<sub>zone</sub>(i)*)*/*
-
-* HeatFlowSeq<sub>sys</sub>(i)*
-
-*FracOA=r<sub>air</sub>* \* *DesOutAirVolFlow<sub>sys</sub>*/ *HeatFlowSeq<sub>sys</sub>(i)*
-
-*T<sub>mix</sub>*=*T<sub>outside</sub>* \* *FracOA* + *SysHeatRetTemp(i)*(1 - *FracOA*)
-
-*W<sub>mix</sub>*=*W<sub>outside</sub>* \* *FracOA* + *SysHeatRetHumRat (i)*(1 - *FracOA*)
-
-*SysHeatOutTempSeq(i)*= *T<sub>outside</sub>*
-
-*SysHeatOutHumRatSeq(i)*= *W<sub>outside</sub>*
-
-Get the current (zone time-step) system heating capacity:
-
-*SysHeatCap<sub>cur</sub>*=*C<sub>p,air</sub>* \* *MinFlowRat<sub>sys</sub>* \**HeatFlowSeq<sub>sys</sub>(i)*  \*( *T<sub>sup</sub>*-*T<sub>mix</sub>*)
-
-*HeatCapSeq(I)*= *SysHeatCap<sub>cur</sub>*
-
-If *SysHeatCap<sub>cur</sub>* is the maximum for the day so far then save *SysHeatCap<sub>cur</sub>*  as the design value:
-
-*HeatCap(i )<sub>sys</sub>*= *SysHeatCap<sub>cur</sub>*
-
-And save the corresponding mixed, return and outside conditions:
-
-*HeatMixTemp<sub>sys</sub>*= *T<sub>mix</sub>*
-
-*HeatMixHumRat<sub>sys</sub>*=*W<sub>mix</sub>*
-
-*HeatRetTemp<sub>sys</sub>*= *SysHeatRetTemp(i)*
-
-*HeatRetHumRat<sub>sys</sub>*= *SysHeatRetHumRat(I)*
-
-*HeatOutTemp<sub>sys</sub>*= *T<sub>outside</sub>*
-
-*HeatOutHumRat<sub>sys</sub>*= *W<sub>outside</sub>*
-
-Here *MinFlowRat<sub>sys</sub>* is the user specified minimum supply flow ratio.
-
-#### EndDay
-
-If the user has specified *coincident* system sizing then:
-
-*DesCoolVolFlow<sub>sys</sub>*=*r<sub>air</sub>* \**CoinCoolMassFlow<sub>sys</sub>*
-
-*DesHeatVolFlow<sub>sys</sub>*=*r<sub>air</sub>* \**CoinHeatMassFlow<sub>sys</sub>*
-
-*DesMainVolFlow<sub>sys</sub>*=**Max**(*DesCoolVolFlow<sub>sys</sub>*, *DesHeatVolFlow<sub>sys</sub>*)
-
-If the user has specified *noncoincident*system sizing then:
-
-*DesCoolVolFlow<sub>sys</sub>*=*r<sub>air</sub>* \**NonCoinCoolMassFlow<sub>sys</sub>*
-
-*DesHeatVolFlow<sub>sys</sub>*=*r<sub>air</sub>* \**NonCoinHeatMassFlow<sub>sys</sub>*
-
-*DesMainVolFlow<sub>sys</sub>*=**Max**(*DesCoolVolFlow<sub>sys</sub>*, *DesHeatVolFlow<sub>sys</sub>*)
-
-Based on the outdoor air method selected, the *DesCoolVolFlow<sub>sys</sub>* and *DesHeatVolFlow<sub>sys</sub>* are modified based on the system ventilation effciency calculated based on the maximum outdoor air fraction.
-
-#### EndSysSizingCalc
-
-At this point all the calculations have been done in *SysSizing(i,j)*: we have results for each design day. Now these results need to be processed to find the heating and cooling design quantities for each system over all the design days.
-
-For coincident sizing the task is quite easy.
-
-(1)  Loop over all of the air loops.
-
-(a)  Loop over all of the design days.
-
-(i)    If the value of *DesCoolVolFlow* in *SysSizing* for the current design day is greater than the value stored in *CalcSysSizing*, then move *DesCoolVolFlow* from *SysSizing* into *CalcSysSizing* along with *CoolDesDay*, *CoinCoolMassFlow*, *SensCoolCap*, *CoolFlowSeq(i)*, *SensCoolCapSeq(i),* *CoolMixTemp*, *CoolRetTemp*, *CoolMixHumRat*, *CoolRetHumRat*, *CoolOutTemp*, *CoolOutHumRat*, *SysCoolRetTempSeq(i)*, *SysCoolRetHumRatSeq(i)*, *SysCoolOutTempSeq(i)* and *SysCoolOutHumRatSeq(i)*.
-
-(ii)   If the value of *DesHeatVolFlow* in *SysSizing* for the current design day is greater than the value stored in *CalcSysSizing*, then move *DesHeatVolFlow* from *SysSizing* into *CalcSysSizing* along with *HeatDesDay*, *CoinHeatMassFlow*, *HeatCap*, *PreHeatCap*, *HeatFlowSeq(i)*, *HeatCapSeq(i),* *PreHeatCapSeq(i), HeatMixTemp*, *HeatRetTemp*, *HeatMixHumRat*, *HeatRetHumRat*, *HeatOutTemp*, *HeatOutHumRat*, *SysHeatRetTempSeq(i)*, *SysHeatRetHumRatSeq(i)*, *SysHeatOutTempSeq(i)* and *SysHeatOutHumRatSeq(i)*.
-
-At the end of each design day loop the peak cooling and the peak heating data will be stored in *CalcSysSizing*. At this point we set *DesMainVolFlow* in *CalcSysSizing* equal to the maximum of *DesCoolVolFlow* and *DesHeatVolFlow.*
-
-For noncoincident sizing the task is harder since we don't have a single time-step during which all the zone peaks occur. So there is no obvious value for outside air temperature at the peak, return air temperature at the peak and so forth. We must return to the zone sizing data and calculate average values for return and outside conditions.
-
-(b)  Loop over all of the zones cooled by this air loop
-
-(i)    In *FinalZoneSizing* replace the value in *DesCoolCoilInTemp* with the user specified *CoolSupTemp<sub>sys</sub>*. Do the same for *DesCoolCoilInHumRat* and *CoolSupHumRat*. This ensures that zone equipment connected to an air loop will use the system design supply air conditions as coil entering conditions.
-
-(ii)   *NonCoinCoolMassFlow<sub>sys</sub>*=*DesCoolMassFlow<sub>zone</sub>*
-
-*SysCoolRetTemp*=(*ZoneRetTempAtCoolPeak \*DesCoolMassFlow<sub>zone</sub>*)
-
-/*NonCoinCoolMassFlow<sub>sys</sub>*
-
-*SysCoolRetHumRat*=(*ZoneHumRatAtCoolPeak \**
-
-*DesCoolMassFlow<sub>zone</sub>*)/*NonCoinCoolMassFlow<sub>sys</sub>*
-
-*SysCoolOutTemp*=(*T<sub>OA,zone\\ peak</sub> \*DesCoolMassFlow<sub>zone</sub>*)/
-
-* NonCoinCoolMassFlow<sub>sys</sub>*
-
-*SysCoolOutHumRat*=(*W<sub>OA,zone\\ peak</sub> \*DesCoolMassFlow<sub>zone</sub>*)/
-
-* NonCoinCoolMassFlow<sub>sys</sub>*
-
-At the end of the zone loop calculate mixed air conditions and the system sensible cooling capacity.
-
-*FracOA=r<sub>air</sub>* \* *DesOutAirVolFlow<sub>sys</sub>*/ *NonCoinCoolMassFlow<sub>sys</sub>*
-
-*T<sub>mix</sub>* =*SysCoolOutTemp* \* *FracOA* + *SysCoolRetTemp* \* (1 - *FracOA*)
-
-*W<sub>mix</sub>* = *SysCoolOutHumRat*  \* *FracOA* + *SysCoolRetHumRat*  \*
-
-(1 - *FracOA*)
-
-*SysSensCoolCap*=*C<sub>p,air</sub>* \* *NonCoinCoolMassFlow*  \*( *T<sub>mix</sub>*-*T<sub>sup</sub>*)
-
-Then (for noncoincident sizing) the variables calculated in section (ii) are moved into the *CalcSysSizing* Array.
-
-(c)  Loop over all of the zones heated by this air loop.
-
-(i)    In *FinalZoneSizing* replace the value in *DesHeatCoilInTemp* with the user specified *HeatSupTemp<sub>sys</sub>*. Do the same for *DesHeatCoilInHumRat* and *HeatSupHumRat*. This ensures that zone equipment connected to an air loop will use the system design supply air conditions as coil entering conditions.
-
-(ii)   *NonCoinHeatMassFlow<sub>sys</sub>*=*DesHeatMassFlow<sub>zone</sub>*
-
-*SysHeatRetTemp*=(*ZoneRetTempAtHeatPeak \*DesHeatMassFlow<sub>zone</sub>*)
-
-/*NonCoinHeatMassFlow<sub>sys</sub>*
-
-*SysHeatRetHumRat*=(*ZoneHumRatAtHeatPeak \**
-
-*DesHeatMassFlow<sub>zone</sub>*)/*NonCoinHeatMassFlow<sub>sys</sub>*
-
-*SysHeatOutTemp*=(*T<sub>OA,zone\\ peak</sub> \*DesHeatMassFlow<sub>zone</sub>*)/
-
-* NonCoinHeatMassFlow<sub>sys</sub>*
-
-*SysHeatOutHumRat*=(*W<sub>OA,zone\\ peak</sub> \*DesHeatMassFlow<sub>zone</sub>*)/
-
-* NonCoinHeatMassFlow<sub>sys</sub>*
-
-At the end of the zone loop calculate mixed air conditions and the system sensible cooling capacity.
-
-*FracOA=r<sub>air</sub>* \* *DesOutAirVolFlow<sub>sys</sub>*/ *NonCoinHeatMassFlow<sub>sys</sub>*
-
-*T<sub>mix</sub>* =*SysHeatOutTemp* \* *FracOA* + *SysHeatRetTemp* \* (1 - *FracOA*)
-
-*W<sub>mix</sub>* = *SysHeatOutHumRat*  \* *FracOA* + *SysHeatRetHumRat*  \*
-
-(1 - *FracOA*)
-
-*SysHeatlCap*=*C<sub>p,air</sub>* \* *NonCoinHeatlMassFlow*  \*( *T<sub>sup</sub>*-*T<sub>mix</sub>*)
-
-Then (for noncoincident sizing) the variables calculated in section (ii) are moved into the *CalcSysSizing* Array.
-
-(2)  We now have the calculated system sizing data. This data needs to be altered to take into account the user input system design flow rates (if any), or the fact that the user may have requested that the system flow rate be sized on the ventilation requirement. Note that user specified sizing ratios have already been applied to the zone sizing data which have been used in out preceding system sizing calculation. Thus the user specified sizing ratios do not have to be explicitly taken into account at the system level.
-
-First we move the calculated system sizing data from *CalcSysSizing* array into the *FinalSysSizing* array. *FinalSysSizing* will contain the user modified system design data when we are all done.
-
-Loop over the air loops.
-
-(i)    As in the zone case, the user specified system design flow rates are turned into sizing ratios by dividing the user input value by the calculated value. The same strategy is employed for sizing on the ventilation requirement: the design ventilation flow rate is divided by the calculated design flow rate value. For each air loop this gives us a *SizRat<sub>cool</sub>* and *SizRat<sub>heat</sub>*.
-
-*CoinCoolMassFlow*= *SizRat<sub>cool</sub>* \* *CoinCoolMassFlow<sub>calc</sub>*
-
-*NonCoinCoolMassFlow*= *SizRat<sub>cool</sub>* \* *NonCoinCoolMassFlow<sub>calc</sub>*
-
-*DesCoolVolFlow*= *SizRat<sub>cool</sub>* \* *DesCoolVolFlow<sub>calc</sub>*
-
-Since the flow rates have been altered the outside air fraction will change. This will alter the design mixed air conditions and lead to an altered value for the cooling capacity. This must be done for the time-step sequence and for the peak value.
-
-(ii)   Loop over the zone timesteps (index=*i*).
-
-*CoolFlowSeq<sub>sys</sub>(i)*= *SizRat<sub>cool</sub>* \* *CoolFlowSeq<sub>sys,calc</sub>(i)*
-
-*FracOA=r<sub>air</sub>* \* *DesOutAirVolFlow<sub>sys</sub>*/ *CoolFlowSeq<sub>sys</sub>(i)*
-
-*T<sub>mix</sub>*= *SysCoolOutTempSeq(i) \*FracOA +*
-
-*SysCoolRetTempSeq(i) \*(*1-FracOA)
-
-*SensCoolCapSeq(i)*= *C<sub>p,air</sub>* \* *CoolFlowSeq<sub>sys</sub>(i)*  \*( *T<sub>mix</sub>*-*T<sub>sup</sub>*)
-
-(iii)  Do the same calculation for peak cooling.
-
-*FracOA=r<sub>air</sub>* \* *DesOutAirVolFlow<sub>sys</sub>*/ *DesCoolVolFlow*
-
-*T<sub>mix</sub>*= *CoolOutTemp<sub>sys</sub> \*FracOA + CoolRetTemp<sub>sys</sub> \*(*1-FracOA)
-
-*W<sub>mix</sub>*= *CoolOutHumRat<sub>sys</sub> \*FracOA + CoolRetHumRat<sub>sys</sub> \**
-
-*(*1-FracOA)
-
-*SensCoolCap<sub>sys</sub>*= *C<sub>p,air</sub>* \* *DesCoolVolFlow<sub>sys</sub>*  \*( *T<sub>mix</sub>*-*T<sub>sup</sub>*)
-
-*T<sub>mix</sub>* and *W<sub>mix</sub>* are saved in *FinalSysSizing* *.*
-
-(iv) Do the same calculation for the heating case.
-
-*CoinHeatMassFlow*= *SizRat<sub>heat</sub>* \* *CoinHeatMassFlow<sub>calc</sub>*
-
-*NonCoinHeatMassFlow*= *SizRat<sub>heat</sub>* \* *NonCoinHeatMassFlow<sub>calc</sub>*
-
-*DesHeatVolFlow*= *SizRat<sub>heat</sub>* \* *DesHeatVolFlow<sub>calc</sub>*
-
-(v)  Loop over the zone timesteps (index=*i*).
-
-*HeatFlowSeq<sub>sys</sub>(i)*= *SizRat<sub>Heat</sub>*  \* *HeatFlowSeq<sub>sys,calc</sub>(i)*
-
-*FracOA=r<sub>air</sub>* \* *DesOutAirVolFlow<sub>sys</sub>*/ *HeatFlowSeq<sub>sys</sub>(i)*
-
-*T<sub>mix</sub>*= *SysHeatOutTempSeq(i) \* FracOA +*
-
-* SysHeatRetTempSeq(i) \** *(*1-FracOA)
-
-*HeatCapSeq(i)*= *C<sub>p,air</sub>* \* *HeatFlowSeq<sub>sys</sub>(i)*  \*(*T<sub>sup</sub>*-*T<sub>mix</sub>*)
-
-(vi) Do the same calculation for peak heating.
-
-*FracOA=r<sub>air</sub>* \* *DesOutAirVolFlow<sub>sys</sub>*/ *DesHeatVolFlow*
-
-*T<sub>mix</sub>*= *HeatOutTemp<sub>sys</sub> \*FracOA + HeatRetTemp<sub>sys</sub> \** *(*1-FracOA)
-
-*W<sub>mix</sub>*= *HeatOutHumRat<sub>sys</sub> \*FracOA + HeatRetHumRat<sub>sys</sub> \**
-
-*(*1-FracOA)
-
-*HeatCap<sub>sys</sub>*= *C<sub>p,air</sub>* \* *DesHeatVolFlow<sub>sys</sub>*  \*( *T<sub>sup</sub>*-*T<sub>mix</sub>*)
-
-*T<sub>mix</sub>* and *W<sub>mix</sub>* are saved in *FinalSysSizing* *.*
-
-(vii)*DesMainVolFlow<sub>sys</sub>*=**MAX**(*DesCoolVolFlow<sub>sys</sub>*,*DesHeatVolFlow<sub>sys</sub>*)
-
-**This concludes the system design calculation.**
-
-** **
-
-**Scalable System HVAC Sizing**
-
-The scalable system sizing applies to system supply air flow rates and sysyem capacity in coolin and heating modes.
-
-
-
-**Scalable System Air Flow Sizing**
-
-The scalable sizing methods for supply air flow rate allowed are  either, *FlowPerFloorArea*, *FractionOfAutosizedCoolingAirflow*, or *FlowPerCoolingCapacity*. The scalable system air flow sizing methods are defined as follows:
-
-
-
-
-
-*FlowPerFloorArea* means the program calculates the cooling supply air volume flow rate from zone floor area served by the airloop and user specified *Flow Per Floor Area* value.
-
-
-
-*FractionOfAutosizedCoolingAirflow* means the program calculates the cooling supply air volume flow rate from user specified fraction and the autosized design cooling supply air volume flow rate value determined by the simulation.
-
-
-
-*FractionOfAutosizedHeatingAirflow* means the program calculates the heating supply air volume flow rate from user specified fraction and the autosized design heating supply air volume flow rate value determined by the simulation.
-
-
-
-*FlowPerCoolingCapacity* means the supply air volume is calculated from user specified flow per cooling capacity and design cooling capacity determined by the simulation.
-
-
-
-*FlowPerHeatingCapacity* means the supply air volume is calculated from user specified flow per heating capacity and design heating capacity determined by the simulation.
-
-
-
-**Scalable System Capacity Sizing**
-
-The scalable sizing methods for system capacity available are: *CapacityPerFloorArea*, *FractionOfAutosizedCoolingCapacity* and *FractionOfAutosizedHeatingCapacity*. The scalable system capacity sizing methods are defined as follows:
-
-
-
-*CapacityPerFloorArea* means the program calculates the design capacity from user specified capacity per floor area and floor area of the zones served by the airloop.
-
-
-
-*FractionOfAutosizedCoolingCapacity* means the program calculates the design cooling capacity from user specified fraction and the auto-sized design cooling capacity.
-
-** **
-
-*FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity.
-
-Plant Loop Sizing
------------------
-
-### Introduction
-
-The program needs to be able to autosize the fluid flow rate in each plant fluid loop. The design plant loop flow rates are set by the sum of the needs of the demanding components on each loop. For chilled water loops these components will be cooling coils. For hot water loops - hot water coils. And for condenser loops - various types of chiller that use condenser water for cooling. Each component that uses water for heating or cooling stores its design water flow rate (in its sizing routine) in the array *CompDesWaterFlow*, labeled by its inlet water supply node number. These individual component design water flow rates are then accessed, summed for each plant loop, and stored in the *PlantSizingData* array. This array also contains the user specified design values for each plant loop.
-
-### Hot and Chilled Water Loop Sizing
-
-#### Maximum Loop Volumetric Flow Rate
-
-The loop maximum volumetric flow rate (m<sup>3</sup>) is just set equal to the value stored in the *PlantSizData* array for this loop.
-
-#### Volume of the plant loop
-
-Since the loop capacitance has a stability requirement of <span>\((\dot V\cdot \Delta tstep/V) \le 1\)</span> the volume is set so that the stability requirement will be 0.8 at the zone time step, which is the largest time step encountered at the max flow rate the loop can reach.
-
-<div>$$Vloop = (\dot Vloop,max\cdot \Delta tstep,zone\cdot 3600)/0.8$$</div>
-
-### Condenser Loop Sizing
-
-#### Maximum Loop Volumetric Flow Rate
-
-The loop maximum volumetric flow rate (m<sup>3</sup>) is just set equal to the value stored in the *PlantSizData* array for this loop.
-
-#### Volume of the plant loop
-
-Since the loop capacitance has a stability requirement of <span>\((\dot V\cdot \Delta tstep/V) \le 1\)</span> the volume is set so that the stability requirement will be 0.8 at the zone time step, which is the largest time step encountered at the max flow rate the loop can reach.
-
-<div>$$Vloop = (\dot Vloop,max\cdot \Delta tstep,zone\cdot 3600)/0.8$$</div>
-
-Coincident Plant Sizing using HVAC Sizing Simulation
-----------------------------------------------------
-
-Coincident plant sizing is an advanced sizing method that uses HVAC Sizing Simulations to determine coincident flows.  This section describes the algorithm used for sizing plant loop flow rate based on the coincidence of flow requests that actually occur when operating the system.  The purpose is to provide a more accurate value for the plant loop design flow rate.  This value is held in PlantSizData( PltSizIndex ).DesVolFlowRate.  For plant, this flow rate is the main independent variable used by component models in their sizing routines (along with the design temperature difference in Sizing:Plant). The code is contained in a PlantCoinicidentAnalysis object, one for each plant loop that is to be sized using the coincident method using HVAC Sizing Simulation.
-
-The analysis will proceed as follows:
-
-1. Find the maximum mass flow rate over all Sizing Periods, along with the coinciding return temperature and load.  Record which sizing period and timestep. This system node used for logging here is the plant loop supply side inlet node. 
-
-2. Find the maximum load, and the coinciding mass flow and return temperature. Record which sizing period and timestep. For a heating or steam plant loop, the load that is logged is associated with the output variable called Plant Supply Side Heating Demand Rate.  For a cooling or condenser plant loop, the load log is as for the output variable called Plant Supply Side Cooling Demand Rate.
-
-3. Calculate a maximum design flow rate from the maximum load, from step 2, and the temperature difference entered in the Plant:Sizing object and the specific heat (at 5 degC) of the plant fluid.  
-
-4. Compare the flow rate from step 1 to the flow rate from step 3 and take the higher.
-
-5. Apply a sizing factor to the flow rate from Step 4, if desired.  The user can select among different options for which sizing factor use.  
-
-6. Compare the flow rate from step 5 to the current value for plant loop flow rate and calculate a normalized change using 
-
-    * <span>\(
-        \rm{Normalized_Change} = \frac{ \left| \rm{NewFlowRate}-\rm{PreviousFlowRate} \right|} \rm{PreviousFlowRate}
-      \)</span>
-
-7. Normalized_Change = <span>\(\frac{\left|\text{NewFlowRate}-\text{PreviousFlowRate}\right|}{\text{PreviousFlowRate}}\)</span>
-    * Compare magnitude of Normalized_Change to a threshold, currently set at 0.005, to determine if it was significant or not.
-    * If change is significant, then alter the size result for that plant loop. Set flags that sizes have changed and sizing calculations need to be called again.  Trigger special setup timesteps with flags set so that all plant system and component level sizes will be recomputed.  Not this will call and resize all of plant so that if one loop has coincident sizing and it places a load on a loop that has noncoincident sizing, the noncoincident loop might still change size because the loop it depends on changed.  Call for another Sizing Pass. 
-    * If change is not significant, then leave the sizes alone and do not trigger resizing. Do not call for another Sizing Pass. 
-
-See OutputDetailsAndExamples documentation for a description of a fairly comprehensive report sent the EIO file called "Plant Coincident Sizing Algorithm" which provides the user details for each execution of the algorithm. There is also a predefined summary table 
-
-The algorithm described above can have powerful impacts on the sizes of plant loops.  It is not uncommon for a hot water plant to size out at around half of what would be determined from the noncoincident sum of the sizes of all the components connected to the loop.  The maximum load aspect of the algorithm is able to increase plant flow rates above the size of the pumps, whereas the flow rate aspect of the algorithm is only able to reduce the flow rates.  It can happen that load spikes cause sizes to increase after the first Sizing Pass, and then the coincident flow rate bring the sizes back down some during subsequent Sizing Passes.  It is worthwhile to explore multiple Sizing Passes, or iterations, because sometimes the algorithm will switch between coincident flow and coincident demand from one Sizing Pass and gradually find a size that just meets conditions.  Be aware that all the controls and and EMS are also      
-
-
-Component Sizing
-----------------
-
-### Introduction
-
-In EnergyPlus each HVAC component sizes itself. Each component module contains a sizing subroutine. When a component is called for the first time in a simulation, it reads in its user specified input data and then calls the sizing subroutine. This routine checks the autosizable input fields for missing data and calculates the data when needed.
-
-A number of high-level variables are used in the sizing subroutines.
-
-*CurDuctType* (in *DataSizing*) contains the information about the current duct type. The types can be *main*, *cooling*, *heating* or *other*.
-
-*CurZoneEqNum* (in *DataSizing*) is the current zone equipment set index and indicates that the component is a piece of zone equipment and should size itself using the zone sizing data arrays.
-
-*CurSysNum* (in *DataSizing*) is the current air loop index and indicates that the component is part of the primary air system and should size itself using the system sizing data arrays.
-
-### Fan Sizing
-
-Fan sizing is done in subroutine *SizeFan*.
-
-#### Max Flow Rate
-
-If the fan is part of the central air system then check the duct type.
-
-For duct type = *main, other* or default, <span>\(\dot{V}_{fan,max} = \text{DesMainVolFlowsys}\)</span>
-
-For duct type=*cooling*, <span>\(\dot{V}_{fan,max} = \text{DesCoolVolFlowsys}\)</span>
-
-For duct type=*heating*, <span>\(\dot{V}_{fan,max} = \text{DesHeatVolFlowsys}\)</span>
-
-If the fan is zone equipment then check whether it is part of a component that only does heating.
-
-For heating only <span>\(\dot{V}_{fan,max} = \text{DesHeatVolFlowzone}\)</span>;
-
-Otherwise <span>\(\dot{V}_{fan,max} = \max\left(\text{DesHeatVolFlowzone},\text{DesCoolVolFlowzone}\right)\)</span>
-
-If the max fan flow rate is less than *SmallAirVolFlow* the max flow rate is set to zero.
-
-### Coil:Cooling:Water
-
-The sizing is done in function *SizeWaterCoil* of module *WaterCoils*
-
-#### Initial Calculations
-
-For central cooling coils, the first step is to determine the design air flow rate, load, and design air entering and exit conditions. The coil design air flow rate is not generally the same as the maximum system air flow rate (used to size the central fans). The cooling coil peak load (either sensible or total) can occur at a different time than the system peak flow rate. Hence the coil air entering conditions can be different than those at the peak system flow rate. Also, the method of controlling the coil's cooling output may also affect coil design flow rate as well as the coil design exit temperature and humidity.
-
-By choosing Type of Load to Size On = _Sensible_ or _Total_ in Sizing:System the user indicates to the program to save the cooling coil air flow rate and system air conditions (mixed, return, outside) at the time of either the system cooling sensible or total load peak. Note that the choice _VentilationRequirement_ uses the time of the sensible peak.
-
-Choosing Central Cooling Capacity Control Method = _VAV_, _Bypass_, _VT_, or _OnOff_ indicates which type of cooling output control the program should assume when calculating the design air flow rate.  The function _GetCoilDesFlowT_ in module _ReportSizingManager_ calculates the air flow rate and exit air temperature for each capacity control method. 
-
-<table class="table table-striped">
-<caption>Cooling coil calculations for different capacity control methods</caption>
-<tr>
- <th>Control Method</th>
- <th>Calculations</th>
-</tr>
-<tr>
- <td>VAV</td>
- <td><span>\(\begin{array}{rl} T_{cc,exit} &= T_{cool,supply} \\ 
-                          \dot{V}_{cc,air} &= \frac{\dot{m}_{cc,air,peak}}{\rho_{air}} \end{array} \)</span></td>
-</tr>
-<tr>
- <td>Bypass</td>
- <td><span>\(\begin{array}{rl} T_{cc,exit} &= T_{cool,supply} \\ 
-                          \dot{V}_{cc,air} &= \dot{V}_{cc,air,max}\cdot\max \left(0, \min \left(1, \frac{T_{mix,at-peak}-T_{sup,avg}}{T_{mix,at-peak}-T_{cc,exit}}\right) \right) \end{array} \)</span></td>
-</tr>
-<tr>
- <td>VT</td>
- <td><span>\(\begin{array}{rl} T_{cc,exit} &= \max\left(T_{cool,supply}, T_{sup,avg}\right) \\ 
-                          \dot{V}_{cc,air} &= \dot{V}_{cc,air,max} \end{array} \)</span></td>
-</tr>
-<tr>
- <td>OnOff</td>
- <td><span>\(\begin{array}{rl} T_{cc,exit} &= T_{cool,supply} \\ 
-                          \dot{V}_{cc,air} &=\dot{V}_{sys,air,max} \end{array} \)</span></td>
-</tr>
-</table>
-
-Where: 
-
-<div>$$ T_{sup,avg} = T_{zones,avg}-\sum_{zones}\frac{\dot{Q}_{sens,at-peak}}{\rho_{air}c_{p,air}\dot{V}_{cool,air,max}}$$</div>
-
-and:
-
-* <span>\(C_{p,air}\)</span>: the specific heat of air (J/kgC)
-
-* <span>\(\dot{m}_{cc,air,peak}\)</span>: the air mass flow rate through the cooling coil at the sensible or total system peak cooling load (m3/s)
-
-* <span>\(\sum_{zones}\dot{Q}_{sens,at-peak}\)</span>: sum of the zone sensible cooling loads at the time of the peak system cooling load
-
-* <span>\(\rho_{air}\)</span>: the density of air (kg/m3)
-
-* <span>\(T_{cc,exit}\)</span>: the design cooling coil exit temperature (c)
-
-* <span>\(T_{cool,supply} \)</span>: the supply air temperature for cooling specified in Sizing:System (C)
-
-* <span>\(T_{mix,at-peak} \)</span>: the mixed air temperature at the time of the system peak cooling load (C)
-
-* <span>\(T_{zones,avg} \)</span>: the average zone temperature at the time of the system peak cooling load (C)
-
-* <span>\(\dot{V}_{cc,air} \)</span>: the design volumetric air flow rate through the cooling coil (m3/s). This is the flow rate at either the sensible or total cooling load peak from the design period calculations. 
-
-* <span>\(\dot{V}_{cool,air,max} \)</span>: the maximum cooling volumetric air flow rate from the design calculations (m3/s). This flow rate occurs at the maximum zone cooling demand.
-
-* <span>\(\dot{V}_{sys,air,max} \)</span>: the maximum volumetric air flow rate from the design calculations (m3/s). This flow rate occurs at either the maximum zone cooling or heating demand.
-
-#### Design Coil Load - System Coils
-
-Design coil load (cooling capacity) is not an input for Coil:Cooling:Water. It is used for calculating the design water flow rate.
-
-The design load is calculated as:
-
-<div>$$ \dot{Q}_{coil,des} = \dot{m}_{a,coil,des}\left(h_{a,coil,des,in}-h_{a,coil,des,out}\right) $$</div>
-
-Where:
-
-* <span>\(h_{a,coil,des,in} \)</span>: is the coil design inlet air enthalpy (J/kg)
-
-* <span>\(h_{a,coil,des,out} \)</span>: is the coil design outlet air enthalpy (J/kg), and 
-
-* <span>\(\dot{m}_{a,coil,des} \)</span>: is the coil design air mass flow rate (kg/s)
-
-The design air mass flow rate depends on the location of the coil.  If the coil is in the outside air stream, the flow rate is set to 
-
-<div>$$\rho_{air}\dot{V}_{a,coil,oa,des}$$</div> where <span>\(\dot{V}_{a,coil.oa,des}\)</span> is the design outside air volumetric flow rate for the system.  Otherwise, it is set to:
-
-<div>$$\rho_{air}\dot{V}_{cc,air}$$</div>
-
-where <span>\(\dot{V}_{cc,air}\)</span> is calculated above in the Initial Calculations section.
-
-To obtain the inlet and outlet enthalpies, we need the inlet and outlet temperatures and humidity ratios. The inlet and outlet conditions depend on whether the coil is in the outside air stream and if it is not, whether or not there is outside air preconditioning.
-
-##### **Coil in outside air stream**:<a name="CoilVsSpacePeakCondition1"></a>
-
-* <span>\(T_{air,in,des}=T_{out,cool,at-peak}\)</span> (the outside air temperature at the design cooling peak)
-  
-* <span>\(T_{air,out,des}=T_{sys,precool}\)</span> (the specified Precool Design Temperature from the System:Sizing object)
-
-* <span>\(W_{air,in,des} = W_{out,cool,at-peak}\)</span> (the outside humidity ratio at the design cooling peak)
-
-* <span>\(W_{air,out,des}=W_{sys,precool}\)</span> (the specified Precool Design Humidity Ratio from the System:Sizing object)
-  
-##### **Coil in main air stream, no preconditioning of outside air** <a name="CoilVsSpacePeakCondition2"></a>
-
-* <span>\(T_{air,in,des}=T_{mix,cool,at-peak}\)</span> (the mixed air temperature at the design cooling peak)
-  
-* <span>\(W_{air,in,des} = W_{mix,cool,at-peak}\)</span> (the mixed humidity ratio at the design cooling peak)
-
-* <span>\(T_{air,out,des}=T_{cc,exit}\)</span> (calculated above in the Initial Calculation section)
-
-* <span>\(W_{air,out,des}=W_{sup,cool}\)</span> (the specified Central Cooling Design Supply Air Humidity Ratio from the Sizing:System object)
-
-##### **Coil in main air stream, outside air preconditioned** <a name="CoilVsSpacePeakCondition3"></a>
-
-The oustide air fraction is calculated as  (where V<sub>cc,air</sub> is calculated as above)
-
-* <span>\(f_{oa}=\frac{\dot V_{air,out,des}}{\dot{V}_{cc,air}}\)</span>
-
-* <span>\(T_{air,in,des}=f_{oa}T_{precool} + \left(1-f_{oa}\right)T_{ret,cool,at-peak}\)</span>(Precool temperature is the specified Precool Design Temperature from System:Sizing Manager; T_ret_cool_at-peak is the return temperature at the system cooling peak load)
-
-* <span>\(W_{air,in,des}=f_{oa}W_{precool} + \left(1-f_{oa}\right)W_{ret,cool,at-peak}\)</span>(Precool humidity ratio is the specified Precool Design Humidity Ratio from System:Sizing Manager; W_ret_cool_at-peak is the return humidity ratio at the system cooling peak load)
-  
-* <span>\(T_{air,out,des}=T_{cc,exit}\)</span> (calculated above in the Initial Calculation section)
-
-* <span>\(W_{air,out,des}=W_{sup,cool}\)</span> (the specified Central Cooling Design Supply Air Humidity Ratio from the Sizing:System object)
-
-With the inlet and outlet conditions established, we can obtain the inlet and outlet enthalpies:
-
-<div>$$ \begin{array}{rl}
-  h_{air,coil,des,in} &= \text{PsyHFnTdbW}\left(T_{air,in,des},W_{air,in,des}\right) \\
-  h_{air,coil,des,out} &= \text{PsyHFnTdbW}\left(T_{air,out,des},W_{air,out,des}\right) \\
-\end{array}$$</div>
-
-Where PsyHFnTdbW is the EnergyPlus function for calculation air specific enthalpy given the air temperature and humidity ratio.  We now have all we need to calculate the design coil capacity, <span>\(\dot{Q}_{coil,des}\)</span>.
-
-#### Design Coil Load - Zone Coils
-
-If the coil is part of an AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction unit or an ZoneHVAC:FourPipeFanCoil, the cooling load (cooling capacity) is passed down from the terminal unit or fan coil sizing calculations. Otherwise the load is defined as:
-
-<div>$$\dot{Q}_{coil,des} = \dot{m}_{a,coil,des}\left(h_{a,coil,des,in}-h_{a,coil,des,out}\right)$$</div>
-
-Where:
-
-* <span>\(h_{a,coil,des,in} \)</span>: is the coil design inlet air enthalpy (J/kg)
-
-* <span>\(h_{a,coil,des,out} \)</span>: is the coil design outlet air enthalpy (J/kg), and 
-
-* <span>\(\dot{m}_{a,coil,des} \)</span>: is the coil design air mass flow rate (kg/s)
-
-The enthalpies are given by:
-
-<div>$$ \begin{array}{lr}
-  h_{air,coil,des,in} &= \text{PsyHFnTdbW}\left(T_{air,in,des},W_{air,in,des}\right) \\
-  h_{air,coil,des,out} &= \text{PsyHFnTdbW}\left(T_{air,out,des},W_{air,out,des}\right) \\
-\end{array}$$</div>
-
-Where the inputs to those functions are the coil inlet design conditions.  For coils in terminal units these are set at the system level to the system design supply air temperature. For zonal units they are set to design return air, mixed air, or outside air as appropriate to the unit. T<sub>air,out,des</sub> is set to the zone cooling design supply air temperature as specified in the _Zone:Sizing_ inputs. W<sub>air,out,des</sub> is set to the zone cooling design supply air humidity ratio as specified in the _Zone:Sizing_ inputs.
-
-#### Design Water Flow Rate (m<sup>3</sup>/s) - System Coils
-
-The design water volumetric flow rate is calculated using:
-
-<div>$$ \dot{V}_{w,coil,des} = \frac{\dot{Q}_{coil,des}}{\rho_w c_{p,w} \Delta T_{w,des}} $$</div>
-
-Where <span>\(\Delta T_{w,des}\)</span> is just the *Loop Design Temperature Difference* user input from *Sizing:Plant* (if the coil is in the outside air stream, 1/2 the *Loop Design Temperature Difference* is used). The design coil load *Load<sub>coil,des</sub>* is calculated from:
-
-#### Design Water Flow Rate (m<sup>3</sup>/s) - Zone Coils
-
-If the coil is part of an AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction unit or an ZoneHVAC:FourPipeFanCoil, the chilled water flow rate is passed down from the terminal unit or fan coil sizing calculations. Otherwise the flow is set to:
-
-<div>$$ \dot{V}_{w,coil,des} = \frac{\dot{Q}_{coil,des}}{\rho_w c_{p,w} \Delta T_{w,des}} $$</div>
-
-Where <span>\(\Delta T_{w,des}\)</span> is just the *Loop Design Temperature Difference* user input from *Sizing:Plant*.
-
-#### Design Air Flow Rate - System Coils
-
-The design air volumetric flow rate for the system cooling coil is set to:
-
-1. the design outside air flow rate if the coil is in the outside air stream;
-
-2. the coil design flow rate from function GetCoilDesFlowT described in section "Initial Calculations";
-
-3. the design flow rate set by the parent component (such as a unitary system) containing the cooling coil.
-
-#### Design Air Flow Rate - Zone Coils
-
-Zone chilled water coils are always part of a zone HVAC component. In almost all cases the design flow rate is passed down from the design flow rate of the parent component. Otherwise if the parent component does cooling only the flow rate for the coil is set to the zone design cooling flow rate. And if the parent component does both cooling and heating, the coil flow rate is set to the maximum of the zone design cooling and heating flow rates.
-
-#### Design Air Inlet Temperature - System Coils
-
-The inlet air temperature depends on whether the coil is in the outside air stream and if it is not, whether or not there is outside air preconditioning.
-
-* Coil in outside air stream: <span>\(T_{air,in,des}=T_{out,cool,at-peak}\)</span> (the outside air temperature set at the design cooling peak).
-
-* Coil in main air stream, no preconditioning of outside air: <span>\(T_{air,in,des}=T_{mix,cool,at-peak}\)</span> (the mixed air temperature at the cooling design peak).
-
-* Coil in main air stream, outside air preconditioned.  The outside air fraction is calculated as <span>\(f_{oa}= \dot V_{air,out,des}/\dot V_{cc,air}\)</span>, where <span>\(\dot V_{cc,air}\)</span> is calculated above.  Then <span>\(T_{air,in,des}=f_{oa}T_{precool}+\left(1-f_{oa}\right)T_{ret,cool,at-peak}\)</span>, where <span>\(T_{precool}\)</span> is the specified *Precool Design Temperature* from *System:Sizing*, and <span>\(T_{ret,cool,at-peak}\)</span> is the return temperature at the system cooling peak load.
-
-#### Design Air Inlet Temperature - Zone Coils
-
-The design inlet temperature depends on whether the coil is in a terminal unit or a zonal unit, and where the coil is positioned within the unit.
-
-1. For the AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction terminal unit the design inlet temperature is set to the zone temperature at the time of the zone cooling peak, since the coil is located in the induced air stream.
-
-2. For fan coil units the design inlet temperature is set to the mixed air temperature: <span>\(T_{air,in,des}=f_{oa}T_{oa,coolpeak} + \left(1-f_{oa}\right)T_{z,coolpeak}\)</span>, where <span>\(f_{oa} = \rho_a \dot V_{z,oa,des} / \dot m_{z,cool,des}\)</span>
-
-3. In all other cases the design inlet temperature is set to the zone design cooling coil inlet temperature which is calculated in the zone sizing simulation and is basically the same calculation as the fan coil unit.
-
-#### Design Air Outlet Temperature - System Coils
-
-The outlet air temperature depends on whether the coil is in the outside air stream.
-
-1. Coil in outside air stream: T<sub>air,out,des</sub> = T<sub>sys,des,precool</sub> (the specified Precool Design Temperature from the Sizing:System object).
-
-2. Coil in main air stream: the design outlet air temperature is set to the temperature calculated in the Initial Calculation section above.
-
-#### Design Air Outlet Temperature - Zone Coils
-
-If the coil is part of an AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction unit, then:
-
-<div>$$
- \begin{array}{rl}
-  \dot{Q}_{coil,des} &= c_{p,air}\rho_{air}\dot{V}_{w,coil,des}\Delta T_{w,des} \\
-  T_1 &= T_{air,in,des} - \dot{Q}_{coil,des} / \left(\rho_{air}c_{p,air}\dot V_{air,coil,des}\right) \\
-  T_2 &= T_{w,out,des} + 2 \\
-  T_{air,out,des} &= \max \left(T_1,T_2\right)
- \end{array}
-$$</div>
-
-For all other cases T<sub>air,out,des</sub> is set to T<sub>z,sup,des</sub> (the zone design supply air temperature as specified in Sizing:Zone).
-
-#### Design Inlet Air Humidity Ratio - System Coils
-
-The design inlet humidity ratio depends on whether the coil is in the outside air stream and if it is not, whether or not there is outside air preconditioning.
-
-* Coil in outside air stream: <span>\(W_{air,in,des}=W_{out,cool,at-peak}\)</span> (the outside air humidity ratio at the design cooling peak).
-
-* Coil in main air stream, no preconditioning of outside air: <span>\(W_{air,in,des}=W_{mix,cool,at-peak}\)</span> (the mixed air humidity ratio at the cooling design peak).
-
-* Coil in main air stream, outside air preconditioned.  The outside air fraction is calculated as <span>\(f_{oa}= \dot V_{air,out,des}/\dot V_{cc,air}\)</span>, where <span>\(\dot V_{cc,air}\)</span> is calculated above.  Then <span>\(W_{air,in,des}=f_{oa}W_{precool}+\left(1-f_{oa}\right)W_{ret,cool,at-peak}\)</span>, where <span>\(W_{precool}\)</span> is the specified *Precool Design Humidity Ratio* from *System:Sizing*, and <span>\(W_{ret,cool,at-peak}\)</span> is the return humidity ratio at the system cooling peak load.
-
-#### Design Air Inlet Humidity Ratio - Zone Coils
-
-The design inlet humidity ratio depends on whether the coil is in a terminal unit or a zonal unit, and where the coil is positioned within the unit.
-
-1. For the AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction terminal unit the design inlet humidity ratio is set to the zone humidity ratio at the time of the zone cooling peak, since the coil is located in the induced air stream.
-
-2. For fan coil units the design inlet humidity ratio is set to the mixed air humidity ratio: <span>\(W_{air,in,des}=f_{oa}W_{oa,coolpeak} + \left(1-f_{oa}\right)W_{z,coolpeak}\)</span>, where <span>\(f_{oa} = \rho_a \dot V_{z,oa,des} / \dot m_{z,cool,des}\)</span>
-
-3. In all other cases the design inlet humidity ratio is set to the zone design cooling coil inlet hunidity ratio which is calculated in the zone sizing simulation and is basically the same calculation as the fan coil unit.
-
-#### Design Outlet Air Humidity Ratio - System Coils
-
-The outlet air humidity ratio depends on whether the coil is in the outside air stream.
-
-* Coil in outside air stream: W<sub>air,out,des</sub> = W<sub>sys,des,precool</sub> (the specified Precool Design Humidity Ratio from the Sizing:System object)
-
-* Coil in main air stream: W<sub>air,out,des</sub> = PsyWFnTdbRhPb(T<sub>air,out,des</sub>,0.9,P<sub>air,std</sub>), where PsyWFnTdbRhPb is the EnergyPlus psychrometric function to calculate humidity ratio from drybulb temperature, relative humidity, and atmospheric pressure. The design outlet humidity ratio is being set to the humidity ratio at 90% relative humidity and design outlet temperature.
-
-#### Design Outlet Air Humidity Ratio - Zone Coils
-
-* If the coil is part of an AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction unit, then:
-    
-    * Get the dewpoint temperature at W<sub>air,in,des</sub>: <span>\(T_{dp,in}=\text{PsyTdpFnWPb}\left(W_{air,in,des},P_{air,std}\right)\)</span>
-    
-    * If T<sub>dp,in</sub> <= T<sub>w,in,des</sub> set W<sub>air,out,des</sub> = W<sub>air,in,des</sub>.  Otherwise set W<sub>air,out,des</sub> = min(PsyWFnTdbRhPb(T<sub>air,out,des</sub>,0.9,P<sub>air,std</sub>),W<sub>air,in,des</sub>)
-    
-#### Design Inlet Water Temperature - System Coils
-
-The Design Inlet Water Temperature is set to the Design Loop Exit Temperature specified in the Sizing:Plant object for the water loop serving this coil.
-
-#### Design Inlet Water Temperature - Zone Coils
-
-The Design Inlet Water Temperature is set to the Design Loop Exit Temperature specified in the Sizing:Plant object for the water loop serving this coil.
-
-### Coil:Cooling:Water:DetailedGeometry Sizing
-
-The sizing is done in subroutine *SizeWaterCoil*
-
-#### Max Water Flow Rate of Coil
-
-The calculation is identical to that done for *Coil:Cooling:Water*.
-
-#### Number of Tubes per Row
-
-<div>$$Ntube/row = {\mathop{\rm Int}\nolimits} ({\rm{13750}}\cdot \dot Vcoil,water,max)$$</div>
-
-*N<sub>tube/row</sub>*=**Max**(*N<sub>tube/row</sub>*,3)
-
-#### Fin Diameter
-
-Depending on the duct type, get the coil design air flow rate.
-
-For duct type = *main, other* or default
-
-<div>$$\dot mair,des = \rho air\cdot DesMainVolFlowsys$$</div>
-
-for duct type=*cooling*
-
-<div>$$\dot mair,des = \rho air\cdot DesCoolVolFlowsys$$</div>
-
-for duct type=*heating*
-
-<div>$$\dot mair,des = \rho air\cdot DesHeatVolFlowsys$$</div>
-
-<div>$$Dfin = 0.335\cdot \dot mair,des$$</div>
-
-#### Minimum Air Flow Area
-
-Depending on the duct type, get the coil design air flow rate.
-
-For duct type = *main, other* or default
-
-<div>$$\dot mair,des = \rho air\cdot DesMainVolFlowsys$$</div>
-
-for duct type=*cooling*
-
-<div>$$\dot mair,des = \rho air\cdot DesCoolVolFlowsys$$</div>
-
-for duct type=*heating*
-
-<div>$$\dot mair,des = \rho air\cdot DesHeatVolFlowsys$$</div>
-
-<div>$$AMinAirFlow = 0.44\cdot \dot mair,des$$</div>
-
-#### Fin Surface Area
-
-Depending on the duct type, get the coil design air flow rate.
-
-For duct type = *main, other* or default
-
-<div>$$\dot mair,des = \rho air\cdot DesMainVolFlowsys$$</div>
-
-for duct type=*cooling*
-
-<div>$$\dot mair,des = \rho air\cdot DesCoolVolFlowsys$$</div>
-
-for duct type=*heating*
-
-<div>$$\dot mair,des = \rho air\cdot DesHeatVolFlowsys$$</div>
-
-<div>$$AFinSurf = 78.5\cdot \dot mair,des$$</div>
-
-#### Total Tube Inside Area
-
-*A<sub>tube,total\\ inside</sub>*=4.4 \**D<sub>tube,inside</sub>* \**N<sub>tube\\ rows</sub>* \**N<sub>tubes/row</sub>*
-
-Where *D<sub>tube,inside</sub>* is the tube inside diameter.
-
-#### Tube Outside Surf Area
-
-*A<sub>tube,outside</sub>*=4.1 \**D<sub>tube,outside</sub>* \**N<sub>tube\\ rows</sub>* \**N<sub>tubes/row</sub>*
-
-Where *D<sub>tube,outside</sub>* is the tube outside diameter.
-
-#### Coil Depth
-
-*Depth<sub>coil</sub>*=*Depth<sub>tube\\ spacing</sub>* \* *N<sub>tube\\ rows</sub>*
-
-### Coil:Cooling:WaterToAirHeatPump:EquationFit Sizing
-
-The sizing is done in subroutine *SizeHVACWaterToAir*
-
-#### Rated Air Flow Rate
-
-The calculation is identical to that done for *Coil:Cooling:Water*.
-
-#### Rated Water Flow Rate
-
-The calculation is identical to that done for *Coil:Cooling:Water*, which is the coil design load divided by the *Loop Design Temperature Difference* user input from *Sizing:Plant.* If there is a companion heating coil, the heating coil design load is used so that both modes will have the same rated water flow rate. For sizing the plant loop serving this coil, only one half of this flow rate is used since both the cooling and heating coil will save a flow rate but only one of these coils will operate at a time.
-
-#### Rated Total Cooling Capacity
-
-The calculation for coil operating temperatures (inlet and outlet) are identical to that done for *Coil:Cooling:Water*. The following calculations are then performed to determine the rated total cooling capacity.
-
-<div>$${T_{WB,ratio}} = {\raise0.7ex\hbox{${\left( {{T_{WB,air,in,des}} + 273.15\,C} \right)}$} \!\mathord{\left/ {\vphantom {{\left( {{T_{WB,air,in,des}} + 273.15\,C} \right)} {283.15\,C}}}\right.}\!\lower0.7ex\hbox{${283.15\,C}$}}$$</div>
-
-<div>$${T_{S,ratio}} = {\raise0.7ex\hbox{${\left( {29.44\,C + 273.15\,C} \right)}$} \!\mathord{\left/ {\vphantom {{\left( {29.44\,C + 273.15\,C} \right)} {283.15\,C}}}\right.}\!\lower0.7ex\hbox{${283.15\,C}$}}$$</div>
-
-where:
-
-<span>\({T_{WB,ratio}} = \)</span>ratio of load-side inlet air wet-bulb temperature in Kelvin to a reference temperature
-
-<span>\({T_{S,ratio}} = \)</span> ratio of source-side inlet water temperature in Kelvin to a reference temperature
-
-TCC1 = user input for Total Cooling Capacity Coefficient 1
-
-TCC2 = user input for Total Cooling Capacity Coefficient 2
-
-TCC3 = user input for Total Cooling Capacity Coefficient 3
-
-TCC4 = user input for Total Cooling Capacity Coefficient 4
-
-TCC5 = user input for Total Cooling Capacity Coefficient 5
-
-<div>$$TotCapTempModFac = \,TCC1 + TCC2\left( {{T_{WB,ratio}}} \right) + TCC3\left( {{T_{S,ratio}}} \right) + TCC4 + TCC5$$</div>
-
-The 4<sup>th</sup> and 5<sup>th</sup> coefficient (TCC4 and TCC5) used in the above equation are multipliers for the load-side and source-side flow ratios, respectively. For sizing, these ratios are assumed to be 1.
-
-The enthalpy of the entering air is then compared with the enthalpy of the exiting air. The calculations for air enthalpy are identical to that done for *Coil:Cooling:Water*. If the entering air enthalpy is less than the exiting air enthalpy, a reference value of 48,000 J/kg is used as the entering air enthalpy. If the TotCapTempModFac calculation above yields 0 as the result, a value of 1 is used in the following calculation. If the design air mass flow rate is determined to be less than a very small flow value (0.001 kg/s) or the capacity calculated here is less than 0, the coil total cooling capacity is set equal to 0.
-
-<div>$$\begin{array}{l}IF({H_{in}}\, > \,{H_{out}})THEN\\\,\,\,\,\,{\mathop Q\limits^\cdot_{coil,des,total}} = {\raise0.7ex\hbox{${{m_{air,des}}\left( {{H_{in}} - {H_{out}}} \right)}$} \!\mathord{\left/ {\vphantom {{{m_{air,des}}\left( {{H_{in}} - {H_{out}}} \right)} {TotCapTempModFac}}}\right.}\!\lower0.7ex\hbox{${TotCapTempModFac}$}}\\ELSE\\\,\,\,\,\,{\mathop Q\limits^\cdot_{coil,des,total}} = {\raise0.7ex\hbox{${{m_{air,des}}\left( {48000 - {H_{out}}} \right)}$} \!\mathord{\left/ {\vphantom {{{m_{air,des}}\left( {48000 - {H_{out}}} \right)} {TotCapTempModFac}}}\right.}\!\lower0.7ex\hbox{${TotCapTempModFac}$}}\\ENDIF\end{array}$$</div>
-
-#### Rated Sensible Cooling Capacity
-
-The calculation for coil operating temperatures (inlet and outlet) are identical to that done for *Coil:Cooling:Water*. The following calculations are then performed to determine the rated sensible cooling capacity.
-
-<div>$${T_{DB,ratio}} = {\raise0.7ex\hbox{${\left( {{T_{DB,air,in,des}} + 273.15\,C} \right)}$} \!\mathord{\left/ {\vphantom {{\left( {{T_{DB,air,in,des}} + 273.15\,C} \right)} {283.15\,C}}}\right.}\!\lower0.7ex\hbox{${283.15\,C}$}}$$</div>
-
-<div>$${T_{S,ratio}} = {\raise0.7ex\hbox{${\left( {29.44\,C + 273.15\,C} \right)}$} \!\mathord{\left/ {\vphantom {{\left( {29.44\,C + 273.15\,C} \right)} {283.15\,C}}}\right.}\!\lower0.7ex\hbox{${283.15\,C}$}}$$</div>
-
-where:
-
-<span>\({T_{DB,ratio}} = \)</span>ratio of load-side inlet air dry-bulb temperature in Kelvin to a reference temperature
-
-SCC1 = user input for Sensible Cooling Capacity Coefficient 1
-
-SCC2 = user input for Sensible Cooling Capacity Coefficient 2
-
-SCC3 = user input for Sensible Cooling Capacity Coefficient 3
-
-SCC4 = user input for Sensible Cooling Capacity Coefficient 4
-
-SCC5 = user input for Sensible Cooling Capacity Coefficient 5
-
-SCC6 = user input for Sensible Cooling Capacity Coefficient 6
-
-<div>$$\begin{array}{l}SensCapTempModFac = \,SCC1 + SCC2\left( {{T_{DB,ratio}}} \right) + SCC3\left( {{T_{WB,ratio}}} \right) + SCC4\left( {{T_{S,ratio}}} \right)\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + SCC5 + SCC6\end{array}$$</div>
-
-The 5<sup>th</sup> and 6<sup>th</sup> coefficient (SCC5 and SCC6) used in the above equation are multipliers for the load-side and source-side flow ratios, respectively. For sizing, these ratios are assumed to be 1.
-
-The dry-bulb temperature of the entering air is then compared with the dry-bulb temperature of the exiting air. The calculations for air dry-bulb temperature are identical to that done for *Coil:Cooling:Water*. If the entering air dry-bulb temperature is less than the exiting air dry-bulb temperature, a reference value of 24 C is used as the entering air dry-bulb temperature. If the SensCapTempModFac calculation above yields 0 as the result, a value of 1 is used in the following calculation. If the design air mass flow rate is determined to be less than a very small flow value (0.001 kg/s) or the capacity calculated here is less than 0, the coil sensible cooling capacity is set equal to 0.
-
-<div>$$\begin{array}{l}IF({T_{DB,in}}\, > \,{T_{DB,out}})THEN\\\,\,\,\,\,{\mathop Q\limits^\cdot_{coil,des,sensible}} = {\raise0.7ex\hbox{${{m_{air,des}}C{p_{air,des}}\left( {{T_{DB,in}} - {T_{DB,out}}} \right)}$} \!\mathord{\left/ {\vphantom {{{m_{air,des}}C{p_{air,des}}\left( {{T_{DB,in}} - {T_{DB,out}}} \right)} {SensCapTempModFac}}}\right.}\!\lower0.7ex\hbox{${SensCapTempModFac}$}}\\ELSE\\\,\,\,\,\,{\mathop Q\limits^\cdot_{coil,des,sensible}} = {\raise0.7ex\hbox{${{m_{air,des}}C{p_{air,des}}\left( {24 - {T_{DB,out}}} \right)}$} \!\mathord{\left/ {\vphantom {{{m_{air,des}}C{p_{air,des}}\left( {24 - {T_{DB,out}}} \right)} {SensCapTempModFac}}}\right.}\!\lower0.7ex\hbox{${SensCapTempModFac}$}}\\ENDIF\end{array}$$</div>
-
-### Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit Sizing
-
-For the cooling coil of VS WSHP, we specify a nominal speed level. During the sizing calculation, the Rated Air Volume Flow Rate, the Rated Water Volume Flow Rate and the Rated Total Cooling Capacity at the Selected Nominal Speed Level are determined in the same way as the *Coil:Cooling:WaterToAirHeatPump:EquationFit* object. The sensible heat transfer rate is not allowed for auto-sizing, instead, it is a function of the rated air and water flow rates, rated total cooling capacity and the Reference Unit SHR at the nominal speed level. The default nominal speed level is the highest speed. However, the model allows the user to select a nominal speed level rather than the highest.
-
-#### Rated Air Flow Rate
-
-The calculation is identical to that done for *Coil:Cooling:WaterToAirHeatPump:EquationFit*.
-
-#### Rated Water Flow Rate
-
-The calculation is identical to that done for *Coil:Cooling:WaterToAirHeatPump:EquationFit* , which is the coil design load divided by the *Loop Design Temperature Difference* user input from *Sizing:Plant.* If there is a companion heating coil, the heating coil design load is used so that both modes will have the same rated water flow rate. For sizing the plant loop serving this coil, only one half of this flow rate is used since both the cooling and heating coil will save a flow rate but only one of these coils will operate at a time.
-
-#### Rated Total Cooling Capacity
-
-The calculation for coil operating temperatures (inlet and outlet) are identical to that done for *Coil:Cooling:WaterToAirHeatPump:EquationFit*. The calculations for air enthalpy are similar to that done for *Coil:Cooling:WaterToAirHeatPump:EquationFit.* The difference is in calculating the total cooling capacity temperature modifier function at the selected nominal speed level, as below:
-
-<div>$$TotCapTempModFra{c_{NominalSpeed}} = {\rm{a}} + {\rm{b*}}W{B_i} + c*WB_i^2 + {\rm{d*EWT}} + e*EW{T^2} + f*W{B_i}*EWT$$</div>
-
-where
-
-WB<sub>i</sub> = wet-bulb temperature of the air entering the heating coil,  degC
-
-EWT = entering water temperature,  degC
-
-a-f = regression curve-fit coefficients.
-
-If the entering air enthalpy is less than the exiting air enthalpy, a reference value of 48,000 J/kg is used as the entering air enthalpy. If the *TotCapTempModFac* calculation above yields 0 as the result, a value of 1 is used in the following calculation. If the rated air mass flow rate is determined to be less than a very small flow value (0.001 kg/s) or the capacity calculated here is less than 0, the coil total cooling capacity is set equal to 0.
-
-*If H<sub>in</sub> &gt; H<sub>out</sub> Then*
-
-<div>$${\dot Q_{coil,rated,total}} = {m_{air,rated}}({H_{in}} - {H_{out}})/TotCapTempModFra{c_{NominalSpeed}}$$</div>
-
-*Else*
-
-<div>$${\dot Q_{coil,rated,total}} = {m_{air,rated}}(48000 - {H_{out}})/TotCapTempModFra{c_{NominalSpeed}}$$</div>
-
-*End If*
-
-### Coil:Heating:WaterToAirHeatPump:EquationFit Sizing
-
-The sizing is done in subroutine *SizeHVACWaterToAir.*
-
-#### Rated Air Flow Rate
-
-The calculation is identical to that done for *Coil:Cooling:Water*.
-
-#### Rated Water Flow Rate
-
-The calculation is identical to that done for *Coil:Cooling:Water* , which is the coil design load divided by the *Loop Design Temperature Difference* user input from *Sizing:Plant.* For sizing the plant loop serving this coil, only one half of this flow rate is used since both the cooling and heating coil will save a flow rate but only one of these coils will operate at a time.
-
-#### Rated Total Heating Capacity
-
-The rated total heating capacity is set equal to the rated total cooling capacity.
-
-### Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit Sizing
-
-For the heating coil of VS WSHP, we specify a nominal speed level. During the sizing calculation, the Rated Air Volume Flow Rate and the Rated Water Volume Flow Rate are determined in the same way as the *Coil:Heating:WaterToAirHeatPump:EquationFit* object. On the other hand, the Rated Heating Capacity at the Selected Nominal Speed Level should be the same as the total cooling capacity of its corresponding cooling coil, which has to be sized first. The default nominal speed level will be the highest speed. However, the model allows the user to select a nominal speed level rather than the highest.
-
-#### Rated Air Flow Rate
-
-The calculation is identical to that done for Coil:Cooling:WaterToAirHeatPump:EquationFit.
-
-#### Rated Water Flow Rate
-
-The calculation is identical to that done for Coil:Cooling:WaterToAirHeatPump:EquationFit, which is the coil design load divided by the *Loop Design Temperature Difference* user input from *Sizing:Plant.* For sizing the plant loop serving this coil, only one half of this flow rate is used since both the cooling and heating coil will save a flow rate but only one of these coils will operate at a time.
-
-#### Rated Total Heating Capacity
-
-The rated total heating capacity is set equal to the rated total cooling capacity.
-
-### Coil:Heating:Water Sizing
-
-The sizing is done in subroutine *SizeWaterCoil*.
-
-#### Max Water Flow Rate of Coil
-
-##### System Coils
-
-With the coil load from the system design data array and the user specified (in a Sizing:Plant object) design hot water temperature fall, calculate the max water flow rate:
-
-<div>$$\dot Vcoil,water,max = HeatCapsys/(Cp,water\cdot \rho water\cdot \Delta Tplt,hw,des)$$</div>
-
-##### Zone Coils
-
-Using the zone design coil inlet and supply air conditions calculate the design coil load.
-
-If the coil is not part of an induction unit then obtain the coil inlet temperature from the zone design data array;
-
-*T<sub>in,air</sub>= DesHeatCoilInTemp<sub>zone</sub>*
-
-If the coil is part of an induction unit take into account the induced air:
-
-*Frac<sub>minflow</sub>*=*MinFlowFrac<sub>zone</sub>*
-
-*T<sub>in,air</sub>*= *DesHeatCoilInTemp<sub>zone</sub>* \* *Frac<sub>minflow</sub>* +
-
-*ZoneTempAtHeatPeak<sub> zone</sub>* \*(1- *Frac<sub>minflow</sub>*)
-
-*T<sub>out,air</sub>=HeatDesTemp<sub>zone</sub>*
-
-W*<sub>out,air</sub>= HeatDesHumRat<sub>zone</sub>*
-
-If the coil is part of a terminal unit the mass flow rate is determined by the volumetric flow rate of the terminal unit:
-
-<div>$$\dot mair,des = \rho air\cdot \dot mair,des,tu$$</div>
-
-Otherwise the design flow is obtained from the zone design data array:
-
-<div>$$\dot mair,des = DesHeatMassFlowzone$$</div>
-
-<div>$$Qcoil,des = cp,air\dot mair,des\cdot (Tout,air - Tin,air)$$</div>
-
-Here *c<sub>p,air</sub>* is calculated at the outlet humidity and the average of the inlet and outlet temperatures.
-
-With the coil load and the user specified (in a Sizing:Plant object) design hot water temperature decrease, calculate the max water flow rate:
-
-<div>$$\dot Vcoil,water,max = Qcoil,des/(Cp,water\cdot \rho water\cdot \Delta Tplt,hw,des)$$</div>
-
-#### UA of the Coil
-
-To obtain the UA of the coil, we specify the model inputs (other than the UA) at design conditions and the design coil load that the coil must meet. Then we numerically invert the coil model to solve for the UA that will enable the coil to meet the design coil load given the specified inputs.
-
-##### System Coils
-
-The design coil load is the system design sensible cooling capacity;
-
-*Q<sub>coil,des</sub>*= *HeatCap<sub>sys</sub>*
-
-The required inputs for the simple coil model are:
-
-*T<sub>in,air</sub>*= *HeatMixTemp<sub>sys</sub>*
-
-*W<sub>in,air</sub>*= *HeatMixHumRat<sub>sys</sub>*
-
-*T<sub>in,water</sub>*= *ExitTemp<sub>plt,hw,des</sub>*
-
-<div>$$\dot min,water = \rho water\cdot \dot Vcoil,water,max$$</div>
-
-Depending on the duct type, get the coil design air flow rate.
-
-For duct type = *main, other* or default
-
-*<span>\(\dot min,air = \rho air\cdot DesMainVolFlowsys\)</span>*
-
-for duct type=*cooling*
-
-*<span>\(\dot min,air = \rho air\cdot DesCoolVolFlowsys\)</span>*
-
-for duct type=*heating*
-
-<div>$$\dot min,air = \rho air\cdot DesHeatVolFlowsys$$</div>
-
-We now have all the data needed to obtain UA. The numerical inversion is carried out by calling subroutine *SolveRegulaFalsi*. This is a general utility routine for finding the zero of a function. In this case it finds the UA that will zero the residual function - the difference between the design coil load and the coil output divided by the design coil load. The residual is calculated in the function *SimpleHeatingCoilUAResidual*.
-
-##### Zone Coils
-
-If the coil is not part of an induction unit then obtain the coil inlet temperature from the zone design data array;
-
-*T<sub>in,air</sub>= DesHeatCoilInTemp<sub>zone</sub>*
-
-If the coil is part of an induction unit take into account the induced air:
-
-*Frac<sub>minflow</sub>*=*MinFlowFrac<sub>zone</sub>*
-
-*T<sub>in,air</sub>*= *DesHeatCoilInTemp<sub>zone</sub>* \* *Frac<sub>minflow</sub>* +
-
-*ZoneTempAtHeatPeak<sub> zone</sub>* \*(1- *Frac<sub>minflow</sub>*)
-
-*W<sub>in,air</sub>*= *DesHeatCoilInHumRat<sub>zone</sub>*
-
-*T<sub>in,water</sub>*= *ExitTemp<sub>plt,hw,des</sub>*
-
-<div>$$\dot min,water = \rho water\cdot \dot Vcoil,water,max$$</div>
-
-*T<sub>out,air</sub>=HeatDesTemp<sub>zone</sub>*
-
-W*<sub>out,air</sub>= HeatDesHumRat<sub>zone</sub>*
-
-If the coil is part of a terminal unit the mass flow rate is determined by the volumetric flow rate of the terminal unit:
-
-<div>$$\dot mair,des = \rho air\cdot \dot mair,des,tu$$</div>
-
-Otherwise the design flow is obtained from the zone design data array:
-
-<div>$$\dot mair,des = DesHeatMassFlowzone$$</div>
-
-<div>$$\dot Qcoil,des = cp,air\cdot \dot mair,des\cdot (Tout,air - Tin,air)$$</div>
-
-Here *c<sub>p,air</sub>* is calculated at the outlet humidity and the average of the inlet and outlet temperatures.
-
-We now have all the data needed to obtain UA. The numerical inversion is carried out by calling subroutine *SolveRegulaFalsi*. This is a general utility routine for finding the zero of a function. In this case it finds the UA that will zero the residual function - the difference between the design coil load and the coil output divided by the design coil load. The residual is calculated in the function *SimpleHeatingCoilUAResidual*.
-
-### Coil:Heating:Steam Sizing
-
-The sizing is done in subroutine *SizeSteamCoil*.
-
-#### Maximum Steam Flow Rate
-
-##### System Coils
-
-The maximum steam volumetric flow rate is calculated using:
-
-<div>$${\dot V_{coil,steam,max}}\,\,\, = \,\,\,\,\,\frac{{Loa{d_{coil,des}}}}{{{\rho_{steam}}\left( {{h_{fg}} + {c_{p,w}}\cdot \Delta {T_{sc}}} \right)}}$$</div>
-
-The steam density (<span>\({\rho_{steam}}\)</span>) is for saturated steam at 100 degC (101325.0 Pa) and *h<sub>fg</sub>* is the latent heat of vaporization of water at 100 degC (101325.0 Pa). *C<sub>p,w</sub>* is the heat capacity of saturated water (condensate) at 100 degC (101325.0 Pa)  and <span>\(\Delta {T_{sc}}\)</span> is the Degree of  Subcooling defined in the Coil:Heating:Steam object input. The design coil load *Load<sub>coil,des</sub>* is calculated from:
-
-<div>$$Loa{d_{coil,des}} = {\dot m_{air,des}}({c_{p,air}})({T_{air,coil,des,out}} - {T_{air,coil,des,in}})$$</div>
-
-The design air mass flow rate depends on the location of the coil (duct type). For duct type =  *main,* the flow rate is set to *r<sub>air</sub>* \**DesMainVolFlow<sub>sys</sub>* \**MinSysAirFlowRatio*. If the coil is in a cooling duct the flow rate is set to *r<sub>air</sub>* \**DesCoolVolFlow<sub>sys</sub>* \**MinSysAirFlowRatio*. If the coil is in a heating duct the flow rate is set to *r<sub>air</sub>* \**DesHeatVolFlow<sub>sys</sub>*. If the coil is in any other kind of duct, the flow rate is set to *r<sub>air</sub>* \**DesMainVolFlow<sub>sys</sub>*.
-
-For sizing, the design outlet air temperature (*T<sub>air,coil,des,out</sub>*) is the Central Heating Design Supply Air Temperature specified in the Sizing:System object.
-
-The design inlet air temperature depends on whether the coil is being sized for 100% outdoor air or minimum outdoor air flow (per 100% Outdoor Air in Heating input field in the Sizing:System object).
-
-1)    Sizing based on 100% Outdoor Air in Heating
-
-*T<sub>air,coil,des,in</sub>* = *HeatOutTemp<sub>sys</sub>* (the outdoor air temperature at the design heating peak)
-
-2)    Sizing based on minimum outdoor air flow. The outdoor air fraction is calculated as *Frac*<sub>oa</sub> = *DesOutAirVolFlow<sub>sys</sub>* / *DesVolFlow*. *DesVolFlow* is <span>\({{{{\mathop m\limits^ \bullet  }_{air,des}}} \mathord{\left/ {\vphantom {{{{\mathop m\limits^ \bullet  }_{air,des}}} {{\rho_{air}}}}} \right. } {{\rho_{air}}}}\)</span>*.*
-
-*T<sub>air,coil,des,in</sub>* =*Frac*<sub>oa</sub>* \* HeatOutTemp<sub>sys</sub>* + (1.- *Frac<sub>oa</sub>*) \**HeatRetTemp<sub>sys</sub>* (see Table 41.  System Sizing Data)
-
-##### Zone Coils
-
-If the coil is part of an *AirTerminal:SingleDuct:\** unit (e.g., *AirTerminal:SingleDuct:ConstantVolume:Reheat, AirTerminal:SingleDuct:VAV:Reheat, AirTerminal:SingleDuct:SeriesPIU:Reheat, etc.)*, the maximum steam flow rate is set equal to the terminal unit's maximum steam flow rate. Otherwise (e.g., the zone-level coil is part of *ZoneHVAC:PackagedTerminalAirConditioner, ZoneHVAC:UnitVentilator, ZoneHVAC:UnitHeater or ZoneHVAC:VentilatedSlab*) the calculation is similar to that at the system level. A design load is calculated:
-
-<div>$$Loa{d_{coil,des}} = {\dot m_{air,des}}({c_{p,air}})({T_{air,coil,des,out}} - {T_{air,coil,des,in}})$$</div>
-
-where:
-
-<span>\({\dot m_{air,des}}\)</span>= *DesHeatMassFlow<sub>zone</sub>* (see Table 40.  Zone Sizing Data)
-
-*T<sub>air,coil,des,in</sub>* = *DesHeatCoilInTemp<sub>zone</sub>* (see Table 40)
-
-*T<sub>air,coil,des,out</sub>* =*HeatDesTemp<sub>zone</sub>* (user input from Sizing:Zone object)
-
-<span>\({c_{p,air}}\)</span> = Specific heat of air (evaluated at the average of inlet and outlet air temperatures, and at the zone heating design supply air humidity ratio *HeatDesHumRat<sub>zone</sub>* [user input from Sizing:Zone object])
-
-<div>$${\dot V_{coil,steam,max}}\,\,\, = \,\,\,\,\,\frac{{Loa{d_{coil,des}}}}{{{\rho_{steam}}\left( {{h_{fg}} + {c_{p,w}}\cdot \Delta {T_{sc}}} \right)}}$$</div>
-
-The terms in the denominator of this equation (*�<sub>steam</sub>*, *h<sub>fg</sub>*, etc.) are evaluated in the same way as described above for steam System Coils.
-
-### Sizing of Gas and Electric Heating Coils
-
-The sizing calculation is done in subroutine *SizeHeatingCoil* in module *HeatingCoils*.
-
-#### Nominal Capacity of the Coil
-
-##### System Coils
-
-The value is obtained from the system design array.
-
-*Cap<sub>nom</sub>*= *HeatCap<sub>sys</sub>*
-
-##### Zone Coils
-
-The capacity is calculated from the design coil inlet and outlet conditions.
-
-If the coil is not part of an induction unit then obtain the coil inlet temperature from the zone design data array;
-
-*T<sub>in,air</sub>= DesHeatCoilInTemp<sub>zone</sub>*
-
-If the coil is part of an induction unit take into account the induced air:
-
-*Frac<sub>minflow</sub>*=*MinFlowFrac<sub>zone</sub>*
-
-*T<sub>in,air</sub>*= *DesHeatCoilInTemp<sub>zone</sub>* \* *Frac<sub>minflow</sub>* +
-
-*ZoneTempAtHeatPeak<sub> zone</sub>* \*(1- *Frac<sub>minflow</sub>*)
-
-*T<sub>out,air</sub>=HeatDesTemp<sub>zone</sub>*
-
-W*<sub>out,air</sub>= HeatDesHumRat<sub>zone</sub>*
-
-*Q<sub>coil,des</sub>*=*C<sub>p,air</sub>* \* *DesHeatMassFlow<sub>zone</sub>* \*(*T<sub>out,air</sub>*-*T<sub>in,air</sub>*)
-
-Here *c<sub>p,air</sub>* is calculated at the outlet humidity and the average of the inlet and outlet temperatures.
-
-### DX Coil Sizing
-
-The sizing calculations are done in subroutine *SizeDXCoil* in module *DXCoils*. This section covers the sizing of the objects
-
-1.    Coil:Cooling:DX:SingleSpeed
-
-2.    Coil:Heating:DX:SingleSpeed
-
-3.    Coil:Cooling:DX:TwoSpeed
-
-#### Rated Air Volume Flow Rate
-
-#### System Coils
-
-The rated air flow rate is obtained from the system design array.
-
-<div>$$\dot Vair,rated = DesMainVolFlowsys$$</div>
-
-#### Zone Coils
-
-The rated air flow rate is the maximum of the heating and cooling design flow rates from the zone design array.
-
-<div>$$\dot Vair,rated = Max(DesCoolVolFlowzone,DesHeatVolFlowzone)$$</div>
-
-#### Rated Total Cooling Capacity
-
-#### System Coils
-
-The rated cooling capacity is obtained by dividing the peak cooling capacity by the *Cooling Capacity Modifier Curve* evaluated at peak mixed wetbulb and outdoor drybulb temperatures.
-
-*T<sub>mix</sub>*= *CoolMixTemp<sub>sys</sub>*
-
-*W<sub>mix</sub>*=*CoolMixHumRat<sub>sys</sub>*
-
-*T<sub>sup</sub>*=*CoolSupTemp<sub>sys</sub>*
-
-*W<sub>sup</sub>*=*CoolSupHumRat<sub>sys</sub>*
-
-*T<sub>outside</sub>*=*CoolOutTemp<sub>sys</sub>*
-
-*r<sub>air</sub>*=*PsyRhoAirFnPbTdbW*(*p<sub>air,std</sub>*, *T<sub>mix</sub>*,*W<sub>mix</sub>*)
-
-*h<sub>mix</sub>*= *PsyHFnTdbW*(*T<sub>mix</sub>*,*W<sub>mix</sub>*)
-
-*h<sub>sup</sub>*= *PsyHFnTdbW*(*T<sub>sup</sub>*,*W<sub>sup</sub>*)
-
-*T<sub>mix,wb</sub>*= *PsyTwbFnTdbWPb*(*T<sub>mix</sub>*,*W<sub>mix</sub>*, *p<sub>air,std</sub>*)
-
-*CapModFac*=*CurveValue*(CCapFTemp,*T<sub>mix,wb</sub>*,*T<sub>outside</sub>*)
-
-<div>$$CCappeak = \rho air\cdot \dot Vair,rated\cdot (hmix - hsup)$$</div>
-
-*CCap<sub>rated</sub>*=*CCap<sub>peak</sub>*/ *CapModFac*
-
-We check that the design volume flow per total capacity is within the prescribed range:
-
-<div>$$FlowCapRatio = \dot Vair,rated/CCaprated$$</div>
-
-If *FlowCapRatio* &lt; *FlowCapRatio<sub>min</sub>*  then
-
-<div>$$CCaprated = \dot Vair,rated/FlowCapRatiomin$$</div>
-
-If *FlowCapRatio* &gt; *FlowCapRatio<sub>max</sub>*  then
-
-<div>$$CCaprated = \dot Vair,rated/FlowCapRatiomax$$</div>
-
-where
-
-*FlowCapRatio<sub>min</sub>* = 0.00004027 m<sup>3</sup>/s per watt (300 cfm/ton)
-
-And
-
-*FlowCapRatio<sub>max</sub>*= 0.00006041 m<sup>3</sup>/s per watt (450 cfm/ton)
-
-The sizing calculation for DX cooling coils for 100% dedicated outdor air system (DOAS) are identical to regular DX cooling coils.  However, they operate operate at different flow to capacity ratio ranges and are within the prescribed range below:
-
-*FlowCapRatio<sub>min</sub>* = 0.00001677 m<sup>3</sup>/s per Watt (125 cfm/ton)
-
-And
-
-*FlowCapRatio<sub>max</sub>*= 0.00003355 m<sup>3</sup>/s per Watt (250 cfm/ton)
-
-
-
-#### Zone Coils
-
-The rated cooling capacity for zone coils is calculated in the same manner as for system coils.
-
-*T<sub>mix</sub>*= *DesCoolCoilInTemp<sub>zone</sub>*
-
-*W<sub>mix</sub>*= *DesCoolCoilInHumRat<sub>zone</sub>*
-
-*T<sub>sup</sub>*= *CoolDesTemp<sub>zone</sub>*
-
-*W<sub>sup</sub>*= *CoolDesHumRat<sub>zone</sub>*
-
-*T<sub>outside</sub>*=*T<sub>outside</sub>,<sub>desday,peak</sub>*
-
-*r<sub>air</sub>*=*PsyRhoAirFnPbTdbW*(*p<sub>air,std</sub>*, *T<sub>mix</sub>*,*W<sub>mix</sub>*)
-
-*h<sub>mix</sub>*= *PsyHFnTdbW*(*T<sub>mix</sub>*,*W<sub>mix</sub>*)
-
-*h<sub>sup</sub>*= *PsyHFnTdbW*(*T<sub>sup</sub>*,*W<sub>sup</sub>*)
-
-*T<sub>mix,wb</sub>*= *PsyTwbFnTdbWPb*(*T<sub>mix</sub>*,*W<sub>mix</sub>*, *p<sub>air,std</sub>*)
-
-*CapModFac*=*CurveValue*(CCapFTemp,*T<sub>mix,wb</sub>*,*T<sub>outside</sub>*)
-
-<div>$$CCappeak = \rho air\cdot \dot Vair,rated\cdot (hmix - hsup)$$</div>
-
-*CCap<sub>rated</sub>*=*CCap<sub>peak</sub>*/ *CapModFac*
-
-We check that the design volume flow per total capacity is within the prescribed range:
-
-<div>$$FlowCapRatio = \dot Vair,rated/CCaprated$$</div>
-
-If *FlowCapRatio* &lt; *FlowCapRatio<sub>min</sub>*  then
-
-<div>$$CCaprated = \dot Vair,rated/FlowCapRatiomin$$</div>
-
-If *FlowCapRatio* &gt; *FlowCapRatio<sub>max</sub>*  then
-
-<div>$$CCaprated = \dot Vair,rated/FlowCapRatiomax$$</div>
-
-where
-
-*FlowCapRatio<sub>min</sub>* = 0.00004027 m<sup>3</sup>/s per watt (300 cfm/ton)
-
-And
-
-*FlowCapRatio<sub>max</sub>*= 0.00006041 m<sup>3</sup>/s per watt (450 cfm/ton)
-
-We check the design flow to the total cooling capacity rato for dedicated zone outdoor unit DX cooling coils to be within the limits prescribed below:
-
-*FlowCapRatio<sub>min</sub>* = 0.00001677 m<sup>3</sup>/s per Watt (125 cfm/ton)
-
-And
-
-*FlowCapRatio<sub>max</sub>*= 0.00003355 m<sup>3</sup>/s per Watt (250 cfm/ton)
-
-#### Rated Total Heating Capacity
-
-For Coil:Heating:DX:SingleSpeed the rated heating capacity is set equal to the cooling capacity.
-
-#### Rated SHR
-
-The rated sensible heat ratio is calculated to be the sensible cooling (from rated inlet conditions to user specified supply conditions) divided by the total cooling (from rated inlet to specified supply).
-
-*T<sub>in,rated</sub>*= 26.6667 <sup>o</sup>C (80 <sup>o</sup>F)
-
-*W<sub>in,rated</sub>*= 0.01125 (corresponds to 80 <sup>o</sup>F drybulb, 67 <sup>o</sup>F wetbulb)
-
-*C<sub>p,air</sub>*= *PsyCpAirFnWTdb*(*W<sub>in,rated</sub>*, *T<sub>in,rated</sub>*)
-
-For system coils
-
-*T<sub>sup</sub>*=*CoolSupTemp<sub>sys</sub>*
-
-*W<sub>sup</sub>*=*CoolSupHumRat<sub>sys</sub>*
-
-For zone coils
-
-*T<sub>sup</sub>*= *CoolDesTemp<sub>zone</sub>*
-
-*W<sub>sup</sub>*= *CoolDesHumRat<sub>zone</sub>*
-
-Then
-
-*h<sub>rated</sub>*= *PsyHFnTdbW*(*T<sub>in,rated</sub>*, *W<sub>in,rated</sub>*)
-
-*h<sub>sup</sub>*= *PsyHFnTdbW*(*T<sub>sup</sub>*, *W<sub>sup</sub>*)
-
-*Dh*<sub>rated,sup</sub>=*h<sub>rated</sub>*-*h<sub>sup</sub>*
-
-*DQs<sub>rated,sup</sub>*=*C<sub>p,air</sub>* \*(*T<sub>in,rated</sub>*-*T<sub>sup</sub>*)
-
-*SHR<sub>rated</sub>*=*DQs<sub>rated,sup</sub>*/*Dh*<sub>rated,sup</sub>
-
-#### Evaporative Condenser Air Volume Flow Rate
-
-The evaporative condenser air volume flow rate (m<sup>3</sup>/s) is set to 0.000114 m<sup>3</sup>/s per watt (850 cfm/ton) times the total rated cooling capacity.
-
-#### Evaporative Condenser Air Volume Flow Rate, Low Speed
-
-The evaporative condenser air volume flow rate, low speed (m<sup>3</sup>/s) is set to 1/3 times 0.000114 m<sup>3</sup>/s per watt (850 cfm/ton) times the total rated cooling capacity.
-
-#### Evaporative Condenser Pump Rated Power Consumption
-
-The evaporative condenser pump rated power consumption is set equal to the total cooling capacity times 0.004266 watts pump power per watt capacity (15 W/ton).
-
-#### Evaporative Condenser Pump Rated Power Consumption, Low Speed
-
-The evaporative condenser pump rated power consumption, low speed, is set equal to 1/3 times the total cooling capacity times 0.004266 watts pump power per watt capacity (15 W/ton).
-
-#### Rated Air Volume Flow Rate, low speed
-
-The rated air volume flow rate, low speed, is set equal to 1/3 times the full rated air volume flow rate.
-
-#### Rated Total Cooling Capacity, Low Speed
-
-The rated total cooling capacity, low speed, is set equal to 1/3 times the full rated total cooling capacity.
-
-#### Rated SHR, low speed
-
-The rated sensible heat ratio, low speed, is set equal to the full speed SHR.
-
-#### Resistive Defrost Heater Capacity
-
-For the heat pump the resistive defrost heat capacity is set equal to the cooling capacity.
-
-### DX MultiSpeed Coil Sizing
-
-The sizing calculations are done in subroutine *SizeDXCoil* in module *DXCoils*. This section covers the sizing of the objects
-
-* Coil:Heating:DX:MultiSpeed
-
-* Coil:Cooling:DX: MultiSpeed
-
-The rated air volume flow rate, rated total cooling capacity, rated heating capacity, rated SHR, evaporative condenser air volume flow rate, evaporative condenser pump rated power consumption at the highest speed are sized in the same ways as DX Coil Sizing.
-
-After the sizes are determined at the highest speed, the sizes in the rest of speeds are assumed to
-
-<div>$$Valu{e_n} = \frac{n}{{NumberOfSpeed}}*Valu{e_{NumberOfSpeed}}$$</div>
-
-where
-
-Value<sub>n</sub>         = Any autosizable variable at Speed n, except SHR
-
-SHR<sub>n</sub> = SHR<sub>NumberOfSpeed</sub>
-
-n    = Speed Index number from 1 to NumberOfSpeed-1
-
-NumberOfSpeed     = The highest speed number
-
-### Coil:Cooling:DX:VariableSpeed Sizing
-
-For the variable-speed DX cooling coil, we specify a nominal speed level. During the sizing calculation, the Rated Total Cooling Capacity at the Selected Nominal Speed Level is determined in the same way as the Coil:Cooling:DX:SingleSpeed object. If the user chooses to autosize the Rated Air Volume Flow Rate, the flow rate, as compared to the Rated Total Cooling Capacity, is sized to have the same ratio as the air volume flow rate to the total cooling capacity at the nominal speed, of the Reference Unit. The sensible heat transfer rate is not allowed for auto-sizing, instead, it is a function of the rated air flow, rated total cooling capacity and the Reference Unit SHR at the nominal speed level. The default nominal speed level is the highest speed. However, the model allows the user to select a nominal speed level rather than the highest.
-
-***Rated Total Cooling Capacity***
-
-The calculation for coil operating temperatures (inlet and outlet) are identical to that done for Coil:Cooling:DX:SingleSpeed. The calculations for air enthalpy are similar to that done for Coil:Cooling:DX:SingleSpeed*.* The difference is in calculating the total cooling capacity temperature modifier function at the selected nominal speed level, as below:
-
-<div>$$TotCapTempModFra{c_{NominalSpeed}} = {\rm{a}} + {\rm{b*}}W{B_i} + c*WB_i^2 + {\rm{d*}}D{B_o} + e*D{B_o}{T^2} + f*W{B_i}*D{B_o}$$</div>
-
-where
-
-WB<sub>i</sub> =wet-bulb temperature of the air entering thecooling coil,  degC
-
-DB<sub>o</sub> =condenser entering air temperature,  degC
-
-a-f = regression curve-fit coefficients.
-
-If the entering air enthalpy is less than the exiting air enthalpy, a reference value of 48,000 J/kg is used as the entering air enthalpy. If the *TotCapTempModFac* calculation above yields 0 as the result, a value of 1 is used in the following calculation. If the rated air mass flow rate is determined to be less than a very small flow value (0.001 kg/s) or the capacity calculated here is less than 0, the coil total cooling capacity is set equal to 0.
-
-*If H<sub>in</sub> &gt; H<sub>out</sub> Then*
-
-<div>$${\dot Q_{coil,rated,total}} = {m_{air,rated}}({H_{in}} - {H_{out}})/TotCapTempModFra{c_{NominalSpeed}}$$</div>
-
-*Else*
-
-<div>$${\dot Q_{coil,rated,total}} = {m_{air,rated}}(48000 - {H_{out}})/TotCapTempModFra{c_{NominalSpeed}}$$</div>
-
-*End If*
-
-The other sizing procedures, e.g. evaporative condenser pump, etc., are the same as Coil:Cooling:DX:SingleSpeed.
-
-### Coil:Heating:DX:VariableSpeed Sizing
-
-For the variable-speed DX heating coil, we specify a nominal speed level. During the sizing calculation, the Rated Heating Capacity at the Selected Nominal Speed Level should be the same as the total cooling capacity of its corresponding cooling coil, which has to be sized first. The default nominal speed level will be the highest speed. However, the model allows the user to select a nominal speed level rather than the highest. If the user chooses to autosize the Rated Air Volume Flow Rate, the flow rate, as compared to the Rated Heating Capacity, is sized to have the same ratio as the air volume flow rate to the heating capacity at the nominal speed, of the Reference Unit. The other sizing procedures are the same as Coil:Heating:DX:SingleSpeed.
-
-### Pump Sizing
-
-The loop pumps' autosizable inputs are design volume flow rate and design power consumption. 
-
-#### Design Volume Flow Rate
-
-This is set equal to the design flow rate for the loop which is obtained from summing the needs of the components on the demand side of the loop.  Each component on the plant loop registers its design flow rate and central routines sum them up. 
-
-#### Design Power Consumption
-
-There are two methods available for calculating the design flow rate. The pump object has a input field to select which method to use.  
-
-The first, and original, method is selected by choosing PowerPerFlowPerPressure.  And the design power is calculated using 
-
-
-<div>$$\dot Q_{nom} = H_{nom} \cdot \dot V_{nom} \cdot ScalingFactor /Eff_{mot}$$</div>
-
-where,
-
-*Eff<sub>mot</sub>* is the motor efficiency, often the default value of 0.9. This is defined as the shaft power output in Watts divided by the electric power in Watts. 
-
-*V<sub>nom</sub>* is the design volume flow rate in m<sup>3</sup>/s.
-
-*ScalingFactor* is an input called Design Shaft Power per Unit Flow Rate per Unit Head, with a default of 1.282051 W/((m<sup>3</sup>/s)-Pa).  (This is the inverse of 0.78 for impeller efficiency that was used prior to version 8.5.)
-
-*H<sub>nom</sub>* the nominal head, or pressure rise across the pump, is an input in Pascals.
-
-
-The second method is selected by choosing PowerPerFlow.  Then the power is calculated more simply and does not use head pressure or motor efficiency  
-
-<div>$$\dot Q_{nom} = \dot V_{nom} \cdot ScalingFactor$$</div>
-
-where 
-
-*ScalingFactor* is an input called Design Electric Power per Unit Flow Rate, with a default of 348701.1 W/(m<sup>3</sup>/s) or 22 W/gpm.  The pump motor efficiency and head are still used to model the pump for its fluid heating.  This method essentially finds a pump impeller and drive efficiency that when combined with the head and motor efficiency results in the desired power consumption per flow rate.  
-
-
-### Electric Chiller Sizing
-
-Generally chillers will need nominal cooling capacity, evaporator flow rate and condenser flow rate. All 3 quantities can be straightforwardly obtained using the user specified loop sizing data and the loop design flow rates.
-
-All chillers on a loop are sized to meet the full loop load. If there are multiple chillers on a loop that call for autosizing, they will all be assigned the same cooling capacity and evaporator flow rate.
-
-#### Nominal Cooling Capacity
-
-<div>$$\dot Qchiller,nom = Cp,w\cdot \rho w\cdot \Delta Tloop,des\cdot \dot Vloop,des$$</div>
-
-where
-
-*C<sub>p,w</sub>* is the specific heat of water at 5 <sup>o</sup>C;
-
-*r<sub>w</sub>* is the density of water at standard conditions (5.05 <sup>o</sup>C);
-
-*DT<sub>loop,des</sub>* is the chilled water loop design temperature rise;
-
-<span>\(\dot Vloop,des\)</span>is the loop design volumetric flow rate.
-
-#### Design Evaporator Volumetric Water Flow Rate
-
-<div>$$\dot Vevap,des = \dot Vloop,des$$</div>
-
-#### Design Condenser Volumetric Water Flow Rate
-
-<div>$$\dot Vcond,des = \dot Qchiller,nom\cdot (1 + 1/COPchiller,nom)/(\Delta Tloop,des\cdot Cp,w\cdot \rho w)$$</div>
-
-where
-
-*C<sub>p,w</sub>* is the specific heat of water at design condenser inlet temperature;
-
-*r<sub>w</sub>* is the density of water at standard conditions (5.05 <sup>o</sup>C);
-
-*DT<sub>loop,des</sub>* is the chilled water loop design temperature rise;
-
-*COP<sub>chiller,nom</sub>* is the chiller nominal COP.
-
-Boiler Sizing
-
-Generally boilers will need nominal heating capacity and rate. Both quantities can be straightforwardly obtained using the user specified loop sizing data and the loop design flow rates.
-
-All boilers on a loop are sized to meet the full loop load. If there are multiple boilers on a loop that call for autosizing, they will all be assigned the same heating capacity and flow rate.
-
-#### Nominal Capacity
-
-<div>$$\dot Qboiler,nom = Cp,w\cdot \rho w\cdot \Delta Tloop,des\cdot \dot Vloop,des$$</div>
-
-where
-
-*C<sub>p,w</sub>* is the specific heat of water at the boiler design outlet temperature;
-
-*r<sub>w</sub>* is the density of water at standard conditions (5.05 <sup>o</sup>C);
-
-*DT<sub>loop,des</sub>* is the hot water loop design temperature decrease;
-
-<span>\(\dot Vloop,des\)</span>is the loop design volumetric flow rate.
-
-#### Design Evaporator Volumetric Water Flow Rate
-
-<div>$$\dot Vdes = \dot Vloop,des$$</div>
-
-### Plant Heat Exchanger Sizing
-
-The sizing of plant heat exchanger component (object: HeatExchanger:FluidToFluid) involves determining design flow rates for both sides, a UA value, and a nominal capacity for reporting.  The component has a sizing factor for fine control and uses the design temperatures defined in the Sizing:Plant object.
-
-The Loop Supply Side design flow rate, <span>\({\dot V_{Sup,des}}\)</span>, is set equal to the design flow rate for that loop, multiplied by the component sizing factor, <span>\({f_{comp}}\)</span>.
-
-<div>$${\dot V_{Sup,des}} = {\dot V_{loop,des}}*{f_{comp}}$$</div>
-
-The Loop Demand Side design flow rate,<span>\({\dot V_{Dmd,des}}\)</span> , is set equal to the Loop Supply Side design flow rate.
-
-<div>$${\dot V_{Dmd,des}} = {\dot V_{Sup,des}}$$</div>
-
-The design heat transfer capacity and UA for the heat exchanger are calculated using the design temperatures for the two plant loops.  The loop design temperature difference for the Loop Supply Side, <span>\(\Delta {T_{SupLoop,Des}}\)</span>, is used to determine a nominal capacity.
-
-<div>$$\dot Q = {\mathop V\limits^._{Sup,des}}\rho {c_p}\Delta {T_{SupLoop,Des}}$$</div>
-
-A loop-to-loop design temperature difference, <span>\(\Delta {T_{LoopToLoop,Des}}\)</span>, is determined depending on the nature of the plant loop connected to the Loop Supply Side.  The Sizing:Plant object includes  classifications for the type of loop that include Heating, Steam, Cooling, or Condenser. For Cooling and Condenser loop types, the loop design temperature difference is added to the design exit temperature for the Loop Supply Side, <span>\({T_{SupLoop,Exit}}\)</span>.  For Heating and Stem loop types, the loop design temperature difference is subtracted from the design exit temperature.  This adjusted supply side temperature is then compared to the design exit temperature for the Loop Demand Side,<span>\({T_{DmdLoop,Exit}}\)</span> .
-
-<span>\(\Delta {T_{LoopToLoop,Des}} = \left( {{T_{SupLoop,Exit}} + \Delta {T_{SupLoop,Des}}} \right) - {T_{DmdLoop,Exit}}\)</span>    (Cooling, Condenser)
-
-<span>\(\Delta {T_{LoopToLoop,Des}} = \left( {{T_{SupLoop,Exit}} - \Delta {T_{SupLoop,Des}}} \right) - {T_{DmdLoop,Exit}}\)</span>    (Heating, Steam)
-
-<div>$$\Delta {T_{LoopToLoop,Des}} = MAX\left( {ABS\left( {\Delta {T_{LoopToLoop,Des}}} \right),2.0} \right)$$</div>
-
-The UA (U-Factor Time Area Value) is determined by assuming that the target capacity can be delivered for the loop-to-loop temperature difference which after substituting and rearranging becomes:
-
-<div>$$UA = \frac{{{{\mathop {V}\limits }_{Sup,des}}\rho {c_p}\Delta {T_{SupLoop,Des}}}}{{\Delta {T_{LoopToLoop,Des}}}}$$</div>
-
-A nominal capacity for the heat exchanger is determined from the design flow rates and UA (regardless of if they were automatically sized or input by the user) and the expected operating temperatures of the two loops.  The loop operating temperatures are obtained from the input in Sizing:Plant object if it is present for that loop.  If no Sizing:Plant is present then the loop's overall setpoint is used (if the loop's load scheme is DualSetpointDeadband then the average of the high and low setpoints is used).  The full heat exchanger model is then calculated for the maximum loop flow rates and expected loop temperatures as inlets to the heat exchanger.  The absolute value for the model result for heat transfer rate is then used as the capacity of the heat exchanger.  This capacity is reported and may be used for controls based on operation scheme.
-
-### Humidifier Sizing
-
-The rated power, or nominal electric power input of an Electric Steam Humidifier (Humidifier:Steam:Electric) is calculated from user specified rated capacity (m<sup>3</sup>/s) and the enthalpy change of the water from a reference temperature (20.0 degC) to saturated steam at 100.0 degC. Autosizing procedure assumes that electrical heating element in the humidifier heat the water from the reference temperature and generate saturated steam at 100 degC, and electric to thermal energy conversion efficiency of 100.0%.
-
-#### Rated Power
-
-<div>$${P_{rated}} = {\dot V_{rated}} \cdot {\rho_w} \cdot \left( {{h_{fg}} + {C_{p,w}} \cdot \Delta {T_w}} \right)$$</div>
-
-where
-
-*C<sub>p,w</sub> is the specific heat of water at average temperature ((100+20)/2 = 60.0* * degC), (J/kgK);*
-
-*r<sub>w</sub> is the density of water at standard conditions (5.05* * degC);*
-
-*DT<sub>w</sub>  is the sensible temperature rise of water (100.0 - 20.0=80.0* * degC);*
-
-*<span>\({\dot V_{rated}}\)</span> is the rated capacity of the humidifier in volumetric flow rate.*
-
-*h<sub>fg</sub> is the latent heat of vaporization of water at 100.0 degC, (J/kg);*
-
-#### Gas Fired Humidifier Sizing
-
-The rated power, or nominal gas use rate of a gas steam humidifier (Humidifier:Steam:Gas) is calculated from user specified rated volumetric capacity (m3/s) and the enthalpy change of the water from a reference temperature of 20.0 degC to a saturated steam at 100.0 degC. Autosizing procedure assumes that gas heater in the humidifier convert the water from the reference temperature and generate saturated steam at 100 degC, using gas to thermal energy conversion rated thermal efficiency. 
-
-Rated Gas Use Rate
-
-The rated or nominal gas use rate is given by:
-
-<div>$$Q_{NG,nom} = \frac{\dot{V}_{cap,nom}\rho_w\left(h_{fg}+c_{p,w}\Delta T_w\right)}{\eta_{rated}}$$</div>
-
-Where, 
-
-- Cp,w: specific heat of water at average temperature ((100+20)/2 = 60.0  degC), (J/kgK);
-
-- rho_w: density of water at standard condition (5.05  degC);
-
-- DeltaTw: sensible temperature rise of water (100.0 - 20.0=80.0  degC);
-
-- V_cap_nom: rated or nominal capacity of the humidifier, (m3/s)
-
-- h_fg: latent heat of vaporization of water at 100.0 degC, (J/kg);
-
-- eta_rated: thermal efficiency at rated condition;
-
-
-#### Rated Capacity
-
-<div>$${\dot m_w} = {\dot m_a}\left( {{\omega_o} - {\omega_i}} \right)$$</div>
-
-where
-
-<span>\({\dot m_w}\)</span>* iswater mass flow rate, kg/s;*
-
-<span>\({\dot m_a}\)</span>* is design air mass flow rate, kg/s;*
-
-*ω<sub>o</sub> is design outlet humidity ratio, kg-water/kg-air; *
-
-*ω<sub>i</sub> is design inlet humidity ratio, kg-water/kg-air.*
-
-
-
-The air mass flow rate and humidity ratios are determined based upon zone design conditions. If the unit is part of zone equipment, then:
-
-
-
-<div>$${\dot m_a} = Max\left( {DesCoolVolFlo{w_{zone}},DesHeatVolFlo{w_{zone}}} \right) \cdot {\rho_a}$$</div>
-
-<div>$${\omega_i} = Min\left( {OutHumRatAtCoolPea{k_{zone}},OutHumRatAtHeatPea{k_{zone}}} \right)$$</div>
-
-      <span>\({\omega_o} = Max\left( {ZoneHumRatAtCoolPea{k_{zone}},ZoneHumRatAtHeatPea{k_{zone}}} \right)\)</span>
-
-
-
-where
-
-*r<sub>a</sub> is the density of air at design conditions, kg/s.*
-
-* *
-
-If the unit is part of the central air system, then check if outdoor air system is present. If outdoor air system is part of the air loop and design outdoor air flow rate is greater than zero, then:
-
-<div>$${\dot m_a} = DesOutAirVolFlo{w_{sys}} \cdot {\rho_a}$$</div>
-
-<div>$${\omega_i} = Min\left( {CoolOutHumRa{t_{sys}},HeatOutHumRa{t_{sys}}} \right)$$</div>
-
-      <span>\({\omega_o} = Max\left( {CoolSupHumRa{t_{sys}},HeatSupHumRa{t_{sys}}} \right)\)</span>
-
-Otherwise, air mass flow rate is determined as follows:
-
-for duct type = *main*
-
-<div>$${\dot m_a} = DesMainAirVolFlo{w_{sys}} \cdot {\rho_a}$$</div>
-
-for duct type = *cooling*
-
-<div>$${\dot m_a} = DesCoolVolFlo{w_{sys}} \cdot {\rho_a}$$</div>
-
-for duct type = *heating*
-
-<div>$${\dot m_a} = DesHeatVolFlo{w_{sys}} \cdot {\rho_a}$$</div>
-
-for duct type = *other*
-
-<span>\({\dot m_a} = DesMainVolFlo{w_{sys}} \cdot {\rho_a}\)</span>,
-
-and the humidity ratios are:
-
-<div>$${\omega_i} = Min\left( {CoolMixHumRa{t_{sys}},HeatMixHumRa{t_{sys}}} \right)$$</div>
-
-      <span>\({\omega_o} = Max\left( {CoolSupHumRa{t_{sys}},HeatSupHumRa{t_{sys}}} \right)\)</span>
-
-### Cooling Tower Sizing
-
-The quantities needed to autosize a cooling tower include the design water flow rate, the nominal fan power and air flow rate, and the tower UA. This data may be need to be given at more than one operating point:, for instance - high speed fan, low speed fan and free convection.
-
-EnergyPlus provides two input choices: the user can input the design water flow rate and tower UA at each operating point or the tower nominal capacity (and let the program calculate the water flow rate and UA). Choice of input method will affect the sizing calculations in ways noted below.
-
-#### Design Water Flow Rate
-
-If *Tower Performance Input Method* = *UFactorTimesAreaAndDesignWaterFlowRate* then
-
-<div>$$\dot Vtower,w,des = \dot Vloop,des$$</div>
-
-If *Tower Performance Input Method* = *NominalCapacity* then
-
-<div>$$\dot Vtower,w,des = 5.382E - 8\cdot \dot Qtower,nom$$</div>
-
-where 5.382 \*10<sup>-08</sup> is m<sup>3</sup>/s per watt corresponds to the rule-of-thumb of sizing the tower flow rate at 3 gallons per minute per ton. For the CoolingTower:VariableSpeed:Merkel model with NominalCapacity input method, the user can input the value used to scale design water flow rate from nominal capacity and the default is 5.382 \*10<sup>-08</sup> m<sup>3</sup>/s/W.
-
-#### Fan Power at Design Air Flow Rate
-
-The nominal fan power is sized to be 0.0105 times the design load.
-
-If *Tower Performance Input Method* = *UFactorTimesAreaAndDesignWaterFlowRate* then
-
-<div>$$\dot Qtower,nom = Cp,w\cdot \rho w\cdot \dot Vtower,w,des\cdot \Delta Tloop,des$$</div>
-
-where
-
-*C<sub>p,w</sub>* is the specific heat of water at the condenser loop design exit temperature;
-
-*r<sub>w</sub>* is the density of water at standard conditions (5.05 <sup>o</sup>C);
-
-*DT<sub>loop,des</sub>* is the condenser water loop design temperature rise;
-
-Finally
-
-<div>$$\dot Qfan,nom = 0.0105\cdot \dot Qtower,nom$$</div>
-
-For the CoolingTower:VariableSpeed:Merkel model, the design fan power is determined using a scaling factor, in units of Watts per Watt, that can be input by the user.  The default value is 0.0105 which is the same as above.
-
-#### Design Air Flow Rate
-
-We assume a fan efficiency of 0.5 and a fan pressure rise of 190 Pascals. Then
-
-<div>$$\dot Vtower,air,des = \dot Qfan,nom\cdot 0.5\cdot \rho air/190$$</div>
-
-where
-
-r<sub>air</sub> is the density of air at standard conditions.
-
-For the CoolingTower:VariableSpeed:Merkel model, the design air flow rate is determined from the nominal capacity using a scaling factor, <span>\({f_{airflow/W}}\)</span>,in units of m<sup>3</sup>/s/W.  The default value is 2.76316\*10<sup>-5</sup>.  When the input field is left blank, the default is used as follows
-
-<div>$${\dot V_{tower,air,des}} = {\dot Q_{tower,nom}} \bullet {f_{airflow/W}} \bullet \frac{{101325}}{{{P_{std,altitude}}}}$$</div>
-
-where, <span>\({P_{std,altitude}}\)</span> is the standard barometric pressure for the location's elevation.
-
-When the input field is filled with a hard value, the pressure scaling is not used
-
-<div>$${\dot V_{tower,air,des}} = {\dot Q_{tower,nom}} \bullet {f_{airflow/W}}$$</div>
-
-#### Tower UA Value at Design Air Flow Rate
-
-To obtain the UA of the tower, we specify the model inputs (other than the UA) at design conditions and the design tower load that the tower must meet. Then we numerically invert the tower model to solve for the UA that will enable the tower to meet the design tower load given the specified inputs.
-
-The design tower load is:
-
-for *Tower Performance Input Method* = *UFactorTimesAreaAndDesignWaterFlowRate*
-
-<div>$$\dot Qtower,des = Cp,w\cdot \rho w\cdot \dot Vtower,w,des\cdot \Delta Tloop,des$$</div>
-
-for *Tower Performance Input Method* = *NominalCapacity*
-
-<span>\(\dot Qtower,des = 1.25\cdot \dot Qtower,nom\)</span>(to allow for compressor heat)
-
-Where, <span>\({f_{des,heat,ratio}}\)</span> is the ratio of actual heat rejection capacity to nominal capacity.  This ratio is available as a user input with a default value of 1.25 (to allow for compressor heat).
-
-Then we assign the inputs needed for the model.
-
-*T<sub>in,air</sub>*=35 <sup>o</sup>C (95 <sup>o</sup>F design air inlet temperature)
-
-*T<sub>in,air,wb</sub>*=25.6 <sup>o</sup>C (78 <sup>o</sup>F design air inlet wetbulb temperature)
-
-*W<sub>in</sub>* is calculated from the entering air drybulb and wetbulb.
-
-The  inlet water mass flow rate is just the design volumetric flow rate times the density of water.
-
-The inlet water temperature is set slightly differently for the 2 input methods. For
-
-*UFactorTimesAreaAndDesignWaterFlowRate*
-
-*T<sub>in,water</sub>*=*T<sub>loop,exit,des</sub>*+*DT<sub>loop,des</sub>*
-
-*NominalCapacity*
-
-*T<sub>in,water</sub>*=35 <sup>o</sup>C (95 <sup>o</sup>F design inlet water temperature).
-
-We now have all the data needed to obtain UA. The numerical inversion is carried out by calling subroutine *SolveRegulaFalsi*. This is a general utility routine for finding the zero of a function. In this case it finds the UA that will zero the residual function - the difference between the design tower load and the tower output divided by the design tower load. The residual is calculated in the function *SimpleTowerUAResidual.*
-
-#### Air Flow Rate at Low Fan Speed
-
-The nominal air flow rate at low fan speed is set to a fraction of the full speed air flow rate. The fraction is available for user input in the field called Low Fan Speed Air Flow Rate Sizing Factor. The default is 0.5.
-
-#### Fan Power at Low Fan Speed
-
-The fan power at low fan speed is set to a fraction of the fan power at full speed.  The fraction is available for user input in the field called Low Fan Speed Fan Power Sizing Factor. The default is 0.16.
-
-#### Tower UA Value at Low Fan Speed
-
-For *Tower Performance Input Method* = *UFactorTimesAreaAndDesignWaterFlowRate* the low speed UA is set to a fraction of the full speed UA.  The fraction is available for user input in the field called Low Fan Speed U-Factor Times Area Sizing Factor. The default is 0.6. For *Tower Performance Input Method* = *NominalCapacity* the low speed UA is calculated in the same manner as the full speed UA using <span>\(\dot Qtower,nom,lowspeed\)</span> instead of <span>\(\dot Qtower,nom\)</span>.
-
-#### Air Flow Rate in Free Convection Regime
-
-The free convection air flow rate is set to a fraction of the full air flow rate. The fraction is available for user input in the field called Free Convection Regime Air Flow Rate Sizing Factor. The default is 0.1.
-
-#### Tower UA Value in Free Convection Regime
-
-For *Tower Performance Input Method* = *UA and Design Water Flow Rate* the low speed UA is set to a fraction of the full speed UA. The fraction is available for user input in the field called Free Convection U-Factor Times Area Value Sizing Factor. The default is 0.1. For *Tower Performance Input Method* = *NominalCapacity* the low speed UA is calculated in the same manner as the full speed UA using <span>\(\dot Qtower,nom,freeconv\)</span> instead of <span>\(\dot Qtower,nom\)</span>.
-
-### Fluid Cooler Sizing
-
-The quantities needed to autosize a fluid cooler include the design water flow rate, the nominal fan power, air flow rate, and the fluid cooler UA. This data may need to be given at more than one operating point:, for instance - high speed fan and low speed fan.
-
-EnergyPlus provides two input choices: the user can input the design water flow rate and fluid cooler UA at each operating point or the fluid cooler nominal capacity and the water flow rate (and let the program calculate UA). Choice of input method will affect the sizing calculations in ways noted below.
-
-#### Design Water Flow Rate
-
-The design water flow rate is sized as follows
-
-<div>$${\dot V_{fluidcooler,w,des}} = {\dot V_{loop,des}}$$</div>
-
-#### Fan Power at Design Air Flow Rate
-
-The nominal fan power is sized to be 0.0105 times the design load.
-
-If *Performance Input Method* = *UFactorTimesAreaAndDesignWaterFlowRate* then
-
-<div>$${\dot Q_{fluidcooler,nom}} = {C_{p,w}} \bullet {\rho_w} \bullet {\dot V_{fluidcooler,w,des}} \bullet \Delta {T_{loop,des}}$$</div>
-
-  where
-
-*  C<sub>p,w</sub>* is the specific heat of water at the condenser loop design exit temperature;
-
-* * *r<sub>w</sub>* is the density of water at standard conditions (5.05 <sup>o</sup>C);
-
-* * *DT<sub>loop,des</sub>* is the condenser water loop design temperature rise;
-
-  Finally
-
-<div>$${\dot Q_{fan,nom}} = 0.0105 \bullet {\dot Q_{fluidcooler,nom}}$$</div>
-
-#### ElseifPerformance Input Method= NominalCapacitythen
-
-      <span>\({\dot Q_{fan,nom}} = 0.0105 \bullet {\dot Q_{fluidcooler,nom}}\)</span>
-
-  Where
-
-      <span>\({\dot Q_{fluidcooler,nom}}\)</span> is provided by the user.
-
-#### Design Air Flow Rate
-
-* For Performance Input Method = UFactorTimesAreaAndDesignWaterFlowRate
-
-  <span>\({\dot Q_{fluidcooler,nom}} = {C_{p,w}} \bullet {\rho_w} \bullet {\dot V_{fluidcooler,w,des}} \bullet \Delta {T_{loop,des}}\)</span>
-
-* For Performance Input Method = NominalCapacity
-
-  <span>\({\dot Q_{fluidcooler,nom}}\)</span> is provided by the user.
-
-  <span>\({\dot V_{fluidcooler,air,des}} = {\dot Q_{fluidcooler,nom}}/({T_{in,water}} - {T_{in,air}})*4\)</span>
-
-Where,
-
-*T<sub>in,water  </sub>* = Design entering water temperature provided by the user
-
-*T<sub>in,air       </sub>* = Design air inlet temperature provided by the user
-
-#### Fluid cooler UA Value at Design Air Flow Rate
-
-To obtain the UA of the fluid cooler, we specify the model inputs (other than the UA) at design conditions and the design fluid cooler load that the fluid cooler must meet. Then we numerically invert the fluid cooler model to solve for the UA that will enable the fluid cooler to meet the design fluid cooler load given the specified inputs.
-
-The design fluid cooler load is:
-
-* For Performance Input Method = UFactorTimesAreaAndDesignWaterFlowRate
-
-  <span>\({\dot Q_{fluidcooler,nom}} = {C_{p,w}} \bullet {\rho_w} \bullet {\dot V_{fluidcooler,w,des}} \bullet \Delta {T_{loop,des}}\)</span>
-
-* For Performance Input Method = NominalCapacity
-
-  <span>\({\dot Q_{fluidcooler,nom}}\)</span> is provided by the user.
-
-Then we assign the inputs needed for the model.
-
-*T<sub>in,air      </sub>* = Design air inlet temperature provided by the user
-
-*T<sub>in,air,wb</sub>* = Design air inlet wetbulb temperature provided by the user
-
-*W<sub>in</sub>* is calculated from the entering air drybulb and wetbulb.
-
-The  inlet water mass flow rate is just the design entering volumetric flow rate times the density of water.
-
-The inlet water temperature is set slightly differently for the 2 input methods. For
-
-* UFactorTimesAreaAndDesignWaterFlowRate
-
-<div>$${T_{in,water}} = {T_{loop,exit,des}} + \Delta {T_{loop,des}}$$</div>
-
-* NominalCapacity
-
-<div>$${T_{in,water}} = Provided\,by\,the\,user$$</div>
-
-We now have all the data needed to obtain UA. The numerical inversion is carried out by calling subroutine *SolveRegulaFalsi*. This is a general utility routine for finding the zero of a function. In this case it finds the UA that will zero the residual function - the difference between the design fluid cooler load and the fluid cooler output divided by the design fluid cooler load. The residual is calculated in the function *SimpleFluidCoolerUAResidual.*
-
-#### Air Flow Rate at Low Fan Speed
-
-The nominal air flow rate at low fan speed is set to a fraction of the full speed air flow rate. The fraction is available for user input in the field called Low Fan Speed Air Flow Rate Sizing Factor. The default is 0.5.
-
-#### Fan Power at Low Fan Speed
-
-The fan power at low fan speed is set to a fraction of the fan power at full speed. The fraction is available for user input in the field called Low Fan Speed Fan Power Sizing Factor. The default is 0.16.
-
-#### Fluid cooler UA Value at Low Fan Speed
-
-For *Performance Input Method* = *UFactorTimesAreaAndDesignWaterFlowRate* the low speed UA is set to a fraction of the full speed UA. .  The fraction is available for user input in the field called Low Fan Speed U-Factor Times Area Sizing Factor. The default is 0.6. For *Performance Input Method* = *NominalCapacity* the low speed UA is calculated in the same manner as the full speed UA using <span>\({\dot Q_{fluidcooler,nom,lowspeed}}\)</span> instead of <span>\({\dot Q_{fluidcooler,nom}}\)</span>.
-
-### Evaporative Fluid cooler Sizing
-
-The quantities needed to autosize an evaporative fluid cooler include the design water flow rate, the nominal fan power, air flow rate, and the fluid cooler UA. This data may need to be given at more than one operating point:, for instance - high speed fan and low speed fan.
-
-EnergyPlus provides three input choices: the user can input the design water flow rate and fluid cooler UA at each operating point (*UFactorTimesAreaAndDesignWaterFlowRate*) or the fluid cooler design capacity and the water flow rate and let the program calculate UA (*UserSpecifiedDesignCapacity*) or only the fluid cooler design capacity and let the program calculate UA and the water flow rate (*StandardDesignCapacity*). Choice of input method will affect the sizing calculations in ways noted below.
-
-#### Design Water Flow Rate
-
-If *Performance Input Method* = *StandardDesignCapacity* then
-
-<div>$${\dot V_{fluidcooler,w,des}} = 5.382E - 8\cdot {\dot Q_{fluidcooler,standarddesign}}$$</div>
-
-Else
-
-<div>$${\dot V_{fluidcooler,w,des}} = {\dot V_{loop,des}}$$</div>
-
-where 5.382 \*10<sup>-08</sup> is m<sup>3</sup>/s per watt corresponds to the rule-of-thumb of sizing the fluid cooler flow rate at 3 gallons per minute per ton.
-
-#### Fan Power at Design Air Flow Rate
-
-The design fan power is sized to be 0.0105 times the design load.
-
-If *Performance Input Method* = *UFactorTimesAreaAndDesignWaterFlowRate* then
-
-<div>$${\dot Q_{fluidcooler,design}} = {C_{p,w}} \bullet {\rho_w} \bullet {\dot V_{fluidcooler,w,des}} \bullet \Delta {T_{loop,des}}$$</div>
-
-where
-
-*C<sub>p,w</sub>* is the specific heat of water at the condenser loop design exit temperature;
-
-*r<sub>w</sub>* is the density of water at standard conditions (5.05 <sup>o</sup>C);
-
-*DT<sub>loop,des</sub>* is the condenser water loop design temperature rise;
-
-Finally
-
-<div>$${\dot Q_{fan,design}} = 0.0105 \bullet {\dot Q_{fluidcooler,design}}$$</div>
-
-#### Else
-
-<div>$${\dot Q_{fan,design}} = 0.0105 \bullet {\dot Q_{fluidcooler,design}}$$</div>
-
-Where
-
-<span>\({\dot Q_{fluidcooler,design}}\)</span>is the design capacity provided by the user for the other two performance input methods
-
-#### Design Air Flow Rate
-
-We assume a fan efficiency of 0.5 and a fan pressure rise of 190 Pascals. Then
-
-<div>$${\dot V_{fluidcooler,air,des}} = {\dot Q_{fan,design}} \bullet 0.5 \bullet {\rho_{air}}/190$$</div>
-
-where
-
-r<sub>air</sub> is the density of air at standard conditions.
-
-#### Fluid cooler UA Value at Design Air Flow Rate
-
-To obtain the UA of the evaporative fluid cooler, we specify the model inputs (other than the UA) at design conditions and the design fluid cooler load that the fluid cooler must meet. Then we numerically invert the fluid cooler model to solve for the UA that will enable the fluid cooler to meet the design fluid cooler load given the specified inputs.
-
-The design fluid cooler load is:
-
-* For Performance Input Method = UFactorTimesAreaAndDesignWaterFlowRate
-
-<div>$${\dot Q_{fluidcooler,design}} = {C_{p,w}} \bullet {\rho_w} \bullet {\dot V_{fluidcooler,w,des}} \bullet \Delta {T_{loop,des}}$$</div>
-
-
-
-* For Performance Input Method = StandardDesignCapacity
-
-<span>\({\dot Q_{fluidcooler,design}} = 1.25 \bullet {\dot Q_{fluidcooler,standarddesign}}\)</span> (to allow for compressor heat)
-
-Then we assign the inputs needed for the model.
-
-*T<sub>in,air      </sub>* = 35 <sup>o</sup>C (95 <sup>o</sup>F design air inlet temperature)
-
-*T<sub>in,air,wb</sub>* = 25.6 <sup>o</sup>C (78 <sup>o</sup>F design air inlet wetbulb temperature)
-
-*W<sub>in</sub>* is calculated from the entering air drybulb and wetbulb.
-
-
-
-* For Performance Input Method = UserSpecifiedDesignCapacity
-
-<div>$${\dot Q_{fluidcooler,design}} = {\dot Q_{fluidcooler,userspecifieddesign}}$$</div>
-
-Where, <span>\({f_{des,heat,ratio}}\)</span> is the ratio of actual heat rejection capacity to nominal capacity.  This ratio is available as a user input with a default value of 1.25 (to allow for compressor heat)
-
-Then we assign the inputs needed for the model.
-
-*T<sub>in,air      </sub>* = Design air inlet temperature provided by the user
-
-*T<sub>in,air,wb</sub>* = Design air inlet wetbulb temperature provided by the user
-
-*W<sub>in</sub>* is calculated from the entering air drybulb and wetbulb.
-
-
-
-The inlet water mass flow rate is just the design entering volumetric flow rate times the density of water.
-
-The inlet water temperature is set slightly differently for the 3 input methods. For
-
-* UFactorTimesAreaAndDesignWaterFlowRate
-
-<div>$${T_{in,water}} = {T_{loop,exit,des}} + \Delta {T_{loop,des}}$$</div>
-
-* StandardDesignCapacity
-
-<div>$${T_{in,water}} = 35^\circ C\;(95^\circ F\,design\,inlet\,water\,temperature)$$</div>
-
-* UserSpecifiedDesignCapacity
-
-<div>$${T_{in,water}} = Provided\,by\,the\,user$$</div>
-
-
-
-We now have all the data needed to obtain UA. The numerical inversion is carried out by calling subroutine *SolveRegulaFalsi*. This is a general utility routine for finding the zero of a function. In this case it finds the UA that will zero the residual function - the difference between the design fluid cooler load and the fluid cooler output divided by the design fluid cooler load. The residual is calculated in the function *SimpleEvapFluidCoolerUAResidual.*
-
-#### Air Flow Rate at Low Fan Speed
-
-The design air flow rate at low fan speed is set to a fraction of the full speed air flow rate. The fraction is available for user input in the field called Low Fan Speed Air Flow Rate Sizing Factor. The default is 0.5.
-
-#### Fan Power at Low Fan Speed
-
-The fan power at low fan speed is set to a fraction of the fan power at full speed. The fraction is available for user input in the field called Low Fan Speed Fan Power Sizing Factor. The default is 0.16.
-
-#### Fluid cooler UA Value at Low Fan Speed
-
-For *Performance Input Method* = *UFactorTimesAreaAndDesignWaterFlowRate* the low speed UA is set to a fraction of the full speed UA. The fraction is available for user input in the field called Low Fan Speed U-Factor Times Area Sizing Factor. The default is 0.6. For *Performance Input Method* = *StandardDesignCapacity* (and similarly for *UserSpecifiedDesignCapacity method*) the low speed UA is calculated in the same manner as the full speed UA using <span>\({\dot Q_{fluidcooler,standarddesign,lowspeed}}\)</span> instead of <span>\({\dot Q_{fluidcooler,standarddesign}}\)</span>.
-
-### Fan Coil Unit Sizing
-
-Fan Coil units are compound components: each unit contains a fan, hot water coil, chilled water coil and outside air mixer. The inputs that may need to be autosized are the nominal unit air flow rate, the maximum hot and chilled water flow rates, and the design outside air flow rate. The data needed for sizing the units is obtained from the zone design arrays and the user specified plant sizing input.
-
-#### Maximum Air Flow Rate
-
-<div>$$\dot Vair,max = Max(DesCoolVolFlowzone,DesHeatVolFlowzone)$$</div>
-
-#### Maximum Outside Air Flow Rate
-
-<div>$$\dot Voutsideair,max = Min(MinOAzone,\dot Vair,max)$$</div>
-
-#### Maximum Hot Water Flow
-
-*T<sub>coil,in</sub>*=*DesHeatCoilInTemp<sub>zone</sub>*
-
-*T<sub>coil,out</sub>*=*HeatDesTemp<sub>zone</sub>*
-
-<sub><span>\(\dot Qcoil,des = cp,air\cdot DesHeatMassFlowzone\cdot (Tout,coil - Tin,coil)\)</span></sub>
-
-<div>$$\dot Vmax,hw = \dot Qcoil,des/(cp,w\cdot \rho w\cdot \Delta Tloop,des)$$</div>
-
-where
-
-*c<sub>p,air</sub>* is evaluated at the average of the inlet & outlet temperatures and the coil outlet humidity ratio.
-
-#### Maximum Cold Water Flow
-
-*T<sub>coil,in</sub>*=*DesColdCoilInTemp<sub>zone</sub>*
-
-*T<sub>coil,out</sub>*=*ColdDesTemp<sub>zone</sub>*
-
-*W<sub>coil,in</sub>*= *DesCoolCoilInHumRat<sub>zone</sub>*
-
-*W<sub>coil,out</sub>*= *CoolDesHumRat<sub>zone</sub>*
-
-*H<sub>coil,in</sub>*= *PsyHFnTdbW*(*T<sub>coil,in</sub>*, *W<sub>coil,in</sub>*)
-
-*H<sub>coil,out</sub>*= *PsyHFnTdbW*(*T<sub>coil,out</sub>*, *W<sub>coil,out</sub>*)
-
-<sub><span>\(\dot Qcoil,des = DesCoolMassFlowzone\cdot (hin,coil - hout,coil)\)</span></sub>
-
-<div>$$\dot Vmax,hw = \dot Qcoil,des/(cp,w\cdot \rho w\cdot \Delta Tloop,des)$$</div>
-
-where
-
-*c<sub>p,air</sub>* is evaluated at the average of the inlet & outlet temperatures and the coil outlet humidity ratio.
-
-### Window Air Conditioner Sizing
-
-Window air conditioners are compound components: each unit contains a fan, a DX coil and an outside air mixer. The inputs that may need to be autosized are the nominal unit air flow rate and the design outside air flow rate. The data needed for sizing the units is obtained from the zone design arrays.
-
-#### Maximum Air Flow Rate
-
-<div>$${\dot V_{air,max}} = DesCoolVolFlo{w_{max}}$$</div>
-
-#### Maximum Outside Air Flow Rate
-
-<div>$$\dot Voutsideair,max = Min(MinOAzone,\dot Vair,max)$$</div>
-
-### Unit Ventilator Sizing
-
-Unit ventilators are compound components: each unit contains an outdoor air mixer, a fan, a heating coil, and a cooling coil. The inputs that may need to be autosized are the maximum supply air flow rate and the maximum/minimum outside air flow rates. The data needed for sizing the units is obtained from the zone design arrays.
-
-#### Maximum Air Flow Rate
-
-If both the cooling and heating coil are present, then:
-
-<div>$${\dot V_{supplyair,max}} = MAX\left( {DesCoolVolFlo{w_{zone}},DesHeatVolFlo{w_{zone}}} \right)$$</div>
-
-If only the heating coil is present, then:
-
-<div>$${\dot V_{supplyair,max}} = DesHeatVolFlo{w_{zone}}$$</div>
-
-If only cooling coil is present, then:
-
-<div>$${\dot V_{supplyair,max}} = DesCoolVolFlo{w_{zone}}$$</div>
-
-If neither heating nor cooling coil is present, then:
-
-<div>$${\dot V_{supplyair,max}} = MinO{A_{zone}}$$</div>
-
-#### Maximum Outside Air Flow Rate
-
-<div>$${\dot V_{outsideair,max}} = {\dot V_{air,max}}$$</div>
-
-#### Minimum Outside Air Flow Rate
-
-<div>$${\dot V_{outsideair,min}} = Min\left( {MinO{A_{zone}},{{\dot V}_{air,max}}} \right)$$</div>
-
-### Packaged Terminal Heat Pump Sizing
-
-Packaged terminal heat pumps are compound components: each unit contains a supply air fan, a DX cooling coil, a DX heating coil, a GAS or ELECTRIC supplemental heating coil, and an outside air mixer. The inputs that may need to be autosized are the supply air and outside air volumetric air flow rates during cooling operation, heating operation, and when no cooling or heating is needed. In addition, the maximum supply air temperature from the supplemental heater can also be automatically selected. The data needed for sizing the units are obtained from the zone design arrays.
-
-#### Supply air volumetric flow rate during cooling operation
-
-<div>$${\mathop V\limits^ \cdot_{SA\,\,,\,cooling}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)$$</div>
-
-#### Supply air volumetric flow rate during heating operation
-
-<div>$${\mathop V\limits^ \cdot_{SA\,\,,\,heating}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)$$</div>
-
-#### Supply air volumetric flow rate when no cooling or heating is needed
-
-<div>$${\mathop V\limits^ \cdot_{SA\,,\,no\,cool\,or\,heat}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)$$</div>
-
-#### Outside air volumetric flow rate during cooling operation
-
-<div>$${\mathop V\limits^ \cdot_{OA\,,\,\,cooling}} = {\rm{MIN}}(MinO{A_{zone}},{\mathop {\,V}\limits^ \cdot_{SA\,,\,\,cooling}})$$</div>
-
-#### Outside air volumetric flow rate during heating operation
-
-<div>$${\mathop V\limits^ \cdot_{OA\,,\,\,heating}} = {\rm{MIN}}(MinO{A_{zone}},{\mathop {\,V}\limits^ \cdot_{SA\,,\,\,heating}})$$</div>
-
-#### Outside air volumetric flow rate when no cooling or heating is needed
-
-<div>$${\mathop V\limits^ \cdot_{OA\,,\,no\,\,cool\,or\,heat}} = {\rm{MIN}}(MinO{A_{zone}},{\mathop {\,V}\limits^ \cdot_{SA\,,\,no\,\,cool\,or\,heat}})$$</div>
-
-#### Maximum supply air temperature from supplemental heater
-
-<div>$${T_{SA,\max }} = HeatDesTem{p_{zone}}$$</div>
-
-### MultiSpeed Heat Pump Sizing
-
-MultiSpeed heat pumps are compound components: each unit contains a supply air fan, a multispeed DX cooling coil, a multispeed DX heating coil, and a GAS or ELECTRIC supplemental heating coil. The inputs that may need to be autosized are the supply air volumetric air flow rates during cooling operation, heating operation, and when no cooling or heating is needed. The data needed for sizing the units are obtained from the controlled zone design arrays.
-
-#### Supply air volumetric flow rate during cooling operation at the highest speed
-
-<div>$${\mathop V\limits^ \cdot_{SA\,\,,\,cooling}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)/ZoneFraction$$</div>
-
-#### Supply air volumetric flow rate during heating operation at the highest speed
-
-<div>$${\mathop V\limits^ \cdot_{SA\,\,,\,heating}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)/ZoneFraction$$</div>
-
-#### Supply air volumetric flow rate when no cooling or heating is needed
-
-<div>$${\mathop V\limits^ \cdot_{SA\,,\,no\,cool\,or\,heat}} = \,\,MAX(DesCoolVolFlowzone,\,DesHeatVolFlowzone)/ZoneFraction$$</div>
-
-where
-
-ZoneFraction           = Fraction of the total volume flow that goes through the controlling zone
-
-#### Supply air volumetric flow rate during cooling operation at Speed n (1 to NumberOfSpeed-1)
-
-<div>$${\mathop V\limits^ \cdot_{SA\,\,,\,cooling,n}} = \frac{n}{{NumberOfSpeed}}{\mathop V\limits^ \cdot_{SA\,\,,\,cooling}}$$</div>
-
-#### Supply air volumetric flow rate during heating operation at Speed n (1 to NumberOfSpeed-1)
-
-<div>$${\mathop V\limits^ \cdot_{SA\,\,,\,heating,n}} = \frac{n}{{NumberOfSpeed}}{\mathop V\limits^ \cdot_{SA\,\,,\,heating}}$$</div>
-
-where
-
-n    = Speed Index number from 1 to NumberOfSpeed-1
-
-NumberOfSpeed     = The highest speed number
-
-### Single Duct Terminal Units
-
-These are all the EnergyPlus components whose names begin with "*AirTerminal:SingleDuct:*" (except for Cooled Beam units). This includes *Uncontrolled, ConstantVolume:Reheat, VAV:NoReheat, VAV:Reheat, VAV:Reheat:VariableSpeedFan, VAV:HeatAndCool:NoReheat, VAV:HeatAndCool:Reheat, SeriesPIU:Reheat, ParallelPIU:Reheat,* and *ConstantVolume:FourPipeInduction*. The inputs that may need to be autosized are the various maximum air flow rates through the unit, minimum air flow rates, and maximum hot water and/or chilled water flow rates if heating or cooling coils are present.
-
-*Note:* all zone design flow rates and loads referenced below may have been altered by system sizing inputs. For instance, if the user specifies a *Cooling Design Air Flow Method = Flow/System*  and specifies a *Cooling Design Air Flow Rate* the zone cooling design values will be altered to match the specified system flow rate.
-
-#### Maximum Air Flow Rate
-
-<div>$${\dot V_{air,\max ,{\rm{terminal}}}} = Max(DesCoolVolFlowzone,DesHeatVolFlowzone)$$</div>
-
-#### Maximum Heating Air Flow Rate
-
-<div>$${\dot V_{air,max,heat,terminal}} = DesHeatVolFlowzone$$</div>
-
-#### Maximum Primary and Secondary Air Flow Rates
-
-For the PIU terminal units, the maximum primary and secondary air flow rates are sized to the same value as the maximum total air flow rate.
-
-#### Minimum Air Flow Rate
-
-Basically minimum air flow rates are sized to the ventilation air requirement. This may be more or less complicated.
-
-For the PIU's, the minimum primary air flow fraction is set to
-
-<span>\(\mathop {MinOA}\nolimits_{zone} /{\dot V_{air,max,primary,terminal}}\)</span>.
-
-For other VAV terminal units
-
-<div>$${\dot V_{air,min,terminal}} = Fra{c_{air,\min }}*DesVolFlowzone$$</div>
-
-where, *Fracair,min*corresponds to the minimum flow fraction of the teminal unit. This value is provided as user input, typically as the field "Zone Minimum Air Flow Fraction." For the VAV terminals that allow scheduling minimum flow fraction (e.g., AirTerminal:SingleDuct:VAV:Reheat), there are two ways that *Fracair,min*can be determined. If a value is entered in the input field Constant Minimum Air Flow Fraction, then it is always used for *Fracair,min*. If the mimimum air flow fraction method is "Schedule" and the Constant Minimum Air Flow Fraction is left blank, then the program uses the average of the minimum and maximum values in the schedule for *Fracair,min*.
-
-#### Fan On Flow Fraction
-
-For the parallel PIU, this is set to the minimum primary air flow fraction.
-
-#### Max Hot  Water Flow
-
-<div>$${T_{coil,in}} = DesHeatCoilInTem{p_{zone}}$$</div>
-
-<div>$${T_{coil,out}} = HeatDesTem{p_{zone}}$$</div>
-
-The coil load and max hot water flow rate are then:
-
-<div>$$ \dot Q_{coil,des} = c_{p,air}\cdot \rho_{air}\cdot \dot V_{air,coil,heating}\cdot (T_{out,coil} - T_{in,coil}) $$</div>
-<div>$$ \dot V_{max,hw} = \dot Q_{coil,des}/(c_{p,w}\cdot \rho_{w}\cdot \Delta T_{loop,des}) $$</div>
-
-where
-
-*c<sub>p,air</sub>* is evaluated at the average of the inlet & outlet temperatures and the coil outlet humidity ratio.
-
-The four-pipe induction unit sizes the heating coil differently: to meet the zone load rather than match the design zone supply temperature. The load on the hot water coil is then the zone load minus whatever the central system does.
-
-<div>$${\dot Q_{coil,des}} = {\dot Q_{zone,des}} - {c_{p,air}}{\rho_{air}}{\dot V_{air,primary,des}}({T_{coil,in}} - {T_{zone,heatpeak}})$$</div>
-
-where
-
-<div>$${T_{coil,in}} = DesHeatCoilInTem{p_{zone}}$$</div>
-
-<div>$${T_{zone,heatpeak}} = ZoneTempAtHeatPea{k_{zone}}$$</div>
-
-<div>$${\dot V_{air,primary,des}} = {\dot V_{air,max,terminal}}/(1 + {R_{induc}})$$</div>
-
-#### Max Chilled Water Flow
-
-The chilled water flow for the four-pipe induction unit is sized analogously to the hot water flow.
-
-### Indirect Evaporative Cooler Sizing
-
-The model for the object called EvaporativeCooler:Indirect:ResearchSpecial has a field for the secondary fan flow rate that can be autosized.
-
-#### Secondary Fan Flow Rate
-
-The secondary fan is not part of an airstream that is directly modeled in EnergyPlus.  Because the primary side air flows can be autosized as part of the air system, it is convenent to also scale the size of the secondary flow.   If the cooler is part of the main loop of a central air system, then the secondary fan flow rate is sized to equal to the main design flow rate.
-
-<div>$$\dot Vfan,max = DesMainVolFlowsys$$</div>
-
-If the cooler is part of the outdoor air path of a central air system, then the secondary fan flow rate is sized to be the maximum of either the design minimum outdoor air flow rate or one-half of the main design flow rate.
-
-<div>$${\dot V_{fan,\max }} = MAX({\rm{DesOutAirVolFlow, 0}}{\rm{.5*DesMainVolFlow)}}$$</div>
-
-### Secondary DX Coils Sizing
-
-The secondary DX coils model does not have a standalone object and it is models as add-on feature to the DX Coils. When the secondary DX coil is added to a primary DX cooling coil, the heat rejected to secondary zone is sensible only and is treated as tnternal gain, hence secondary air flow rate is not required in the model.  Where as when the secondary DX coil is added to a primary DX heating coil, then the heat removed from  secondary zone may have sensible and latent components and is treated as tnternal gain. The sensible/latent component split among other parameters requires secondary coil air flow rate. Hence secondary coil air flow rate sizing is added based on the primary DX cooling coil only.
-
-<div>$$\dot{V}_\rm{SecCoil} = \dot{V}_\rm{PriHeatCoil}\cdot \text{ScalingFactor}$$</div>
-
-where
-
-* <span>\(\dot{V}_\text{SecCoil}\)</span> is the secondary coil design air flow rate (m3/s)
-* <span>\(\dot{V}_\text{SecCoil}\)</span> is the primary heating DX coil design air flow rate (kg/s)
-* <span>\(\text{ScalingFactor}\)</span> is the secondary DX coil air flow rarte scaling factor (-)
-
-### Desiccant Dehumidifier Sizing
-
-The sizing of dehumidifier with no fans is done in subroutine SizeDesiccantDehumidifier.
-
-#### Nominal Process Air Flow Rate
-
-If the unit is part of zone equipment, then:
-
-<div>$${\dot V_p} = Max\left( {DesCoolVolFlo{w_{zone}},DesHeatVolFlo{w_{zone}}} \right)$$</div>
-
-If the unit is part of the central air system, then check if outdoor air system is present. If outdoor air system is part of the air loop and design outdoor air flow rate is greater than zero, then:
-
-<div>$${\dot V_p} = DesOutAirVolFlo{w_{sys}}$$</div>
-
-Otherwise, nominal process air flow rate is determined as follows:
-
-for duct type = *main*
-
-<div>$${\dot V_p} = DesMainVolFlo{w_{sys}}$$</div>
-
-for duct type = *cooling*
-
-<div>$${\dot V_p} = DesCoolVolFlo{w_{sys}}$$</div>
-
-for duct type = *heating*
-
-<div>$${\dot V_p} = DesHeatVolFlo{w_{sys}}$$</div>
-
-for duct type = *other*
-
-<div>$${\dot V_p} = DesMainVolFlo{w_{sys}}$$</div>
-
-### Evaporative Cooler Sizing
-
-The sizing of evaporative cooler objects is done in subroutine SizeEvapCooler.
-
-#### Secondary Fan Flow Rate
-
-<div>$$\dot V = DesMainVolFlo{w_{sys}}$$</div>
-
-Note that it is only applicable to indirect CELdek pad object.
-
-#### Direct Pad Area
-
-As from the continuity equation, the area of direct pad is directly determined by assuming face air velocity of 3m/s as:
-
-<div>$${A_{pad}} = \frac{{DesMainVolFlo{w_{sys}}}}{V}$$</div>
-
-where
-
-* \(A_\rm{pad} is area of direct pad, m<sup>2</sup>
-
-* \(V\) is face air velocity, m/s
-
-#### Direct Pad Depth
-
-The solution of the following regression equation is used, assuming saturation effectiveness of 70% and face air velocity of 3m/s:
-
-<div>$$\epsilon = 0.792714 + 0.958569D - 0.25193V - 1.03215D^2 + 0.0262659V^2 + 0.914869DV - 1.48241VD^2 - 0.018992 D V^3 + 1.13137D^3V + 0.0327622 D^2V^3 - 0.145384D^3 V^2$$</div>
-
-where
-
-* \(D\) is depth of pad, m
-* \(\epsilon\)is saturation effectiveness
-
-### Heat Recovery Sizing
-
-The sizing of heat exchanger objects is done in subroutine SizeHeatRecovery.
-
-#### Nominal Supply Air Flow Rate
-
-If the unit is part of zone equipment, then:
-
-<div>$${\dot V_p} = Max\left( {DesCoolVolFlo{w_{zone}},DesHeatVolFlo{w_{zone}}} \right)$$</div>
-
-If the unit is part of the central air system, then check if outdoor air system is present. If outdoor air system is part of the air loop and design outdoor air flow rate is greater than zero, then:
-
-<div>$${\dot V_p} = DesOutAirVolFlo{w_{sys}}$$</div>
-
-Otherwise, nominal supply air flow rate is determined as follows:
-
-for duct type = *main*
-
-<div>$${\dot V_p} = DesMainVolFlo{w_{sys}}$$</div>
-
-for duct type = *cooling*
-
-<div>$${\dot V_p} = DesCoolVolFlo{w_{sys}}$$</div>
-
-for duct type = *heating*
-
-<div>$${\dot V_p} = DesHeatVolFlo{w_{sys}}$$</div>
-
-for duct type = *other*
-
-<div>$${\dot V_p} = DesMainVolFlo{w_{sys}}$$</div>
-
-#### Nominal Supply Air Flow Rate
-
-It is assumed to be equal to the nominal supply air flow rate.
-
-### Low Temperature Radiant System Sizing
-
-The sizing is done in subroutine *SizeLowTempRadiantSystem*.
-
-#### ZoneHVAC:LowTemperatureRadiant:Electric:
-
-##### Nominal Capacity
-
-<div>$$Cap = DesHeatLoa{d_{zone}} \cdot HeatSizingFactor$$</div>
-
-#### ZoneHVAC:LowTemperatureRadiant:VariableFlow:
-
-##### Maximum Hot Water Flow
-
-<div>$${\dot V_h} = \frac{{DesHeatLoa{d_{zone}} \cdot HeatSizingFactor}}{{\Delta {T_h} \cdot {c_{p,h}} \cdot {\rho_h}}}$$</div>
-
-where
-
-<span>\({\dot V_h}\)</span>* is maximum hot water flow rate, m<sup>3</sup>/s*
-
-*c<sub>p,h</sub> is specific heat of hot water at reference condition (60 degC), J/kgK*
-
-*r<sub>h</sub> is the density of water at reference condition (60 degC), kg/m<sup>3</sup>*
-
-##### Maximum Cool Water Flow
-
-<div>$${\dot V_c} = \frac{{DesCoolLoa{d_{zone}} \cdot CoolSizingFactor}}{{\Delta {T_c} \cdot {c_{p,c}} \cdot {\rho_c}}}$$</div>
-
-<span>\({\dot V_c}\)</span>* is maximum chilled water flow rate, m<sup>3</sup>/s*
-
-*c<sub>p,c</sub> is specific heat of hot water at reference condition (5 degC), J/kgK*
-
-*r<sub>c</sub> is the density of chilled water at reference condition (5 degC), kg/m<sup>3</sup>*
-
-##### Hydronic Tubing Length
-
-<div>$$TubeLength = \frac{{TotalSurfaceArea}}{{TubeSpacing}}$$</div>
-
-Note that tube spacing is assumed to be 0.15m.
-
-#### ZoneHVAC:LowTemperatureRadiant:ConstantFlow:
-
-##### Rated Flow Rate
-
-The object provides both cooling and heating, and also operates in a single operating mode such as cooling-only or heating-only mode. Thus, the rated flow rate is determined, depending upon the operating mode of the unit. If the unit operates in a single operating mode, either design chilled water or hot water flow rate is chosen. The larger of the two is chosen if the unit provides both cooling and heating. The flow rates are determined in the same fashion to the variable flow system above.
-
-##### Hydronic Tubing Length
-
-The length of hydronic tube is determined as described in the variable flow radiant system above.
-
-### Unitary System Sizing
-
-The AirloopHVAC:UnitarySystem object incorporates all coils types and fans as a complete packaged system. The fans and coils are optional allowing virtually any system type to be modeled. Sizing of this object depends on the coils selected. For single coil systems, the associated air flow rate is used as the operating flow rate (i.e., cooling or heating). For systems with both a cooling and heating coil, this methodology still applies except for DX systems (Heat Pumps) where the greater of the cooling or heating air flow rate is used. Heat pumps are defined as systems having both a DX cooling and DX heating coil. The inputs that may need to be autosized are the supply air air volumetric air flow rates during cooling operation, heating operation, and when no cooling or heating is needed. The data needed for sizing the units are obtained from the zone design arrays.
-
-#### Supply Air volumetric flow rate during cooling operation:
-
-<div> $$ \dot V_{SA,cooling} = \text{DesCoolVolFlow}_{zone} / \text{ZoneFraction} $$ </div>
-
-#### Supply Air volumetric flow rate during heating operation:
-
-<div> $$ \dot V_{SA,heating} = \text{DesHeatVolFlow}_{zone} / \text{ZoneFraction} $$ </div>
-
-#### Supply Air volumetric flow rate when DX coils are used as a system:
-
-<div> $$ \dot V_{SA} = \max \left(\text{DesCoolVolFlow}_{zone}, \text{DesHeatVolFlow}_{zone}\right) / \text{ZoneFraction} $$ </div>
-
-where:
-
-* ZoneFraction = Fraction of the total volume flow that goes through the controlling zone
-
-The unitary system object also allows scalable sizing as follows:
-
-Flow Per Floor Area:
-
-<div>$$ \dot V_{SA} = \left(\text{FlowPerFloorArea}\right)\left(\text{TotalFloorArea}\right) $$</div>
-
-Fraction of Autosized Cooling Value:
-
-<div>$$ \dot V_{SA,cooling} = \dot V_{SA,des,cooling}\left(\text{FractionOfCoolingValue}\right) $$</div>
-
-Fraction of Autosized Heating Value:
-
-<div>$$ \dot V_{SA,heating} = \dot V_{SA,des,heating}\left(\text{FractionOfHeatingValue}\right) $$</div>
-
-Flow Per Cooling Capacity
-
-<div>$$ \dot V_{SA,cooling} = \dot Q_{coil,des,cooling}\left(\text{FractionOfCoolingValue}\right) $$</div>
-
-Flow Per Heating Capacity
-
-<div>$$ \dot V_{SA,heating} = \dot Q_{coil,des,heating}\left(\text{FractionOfHeatingValue}\right) $$</div>
-
-#### Maximum Supply Air Temperature
-
-The maximum supply air temperature can also be automatically selected. The value is determined from the Sizing:Zone or Sizing:System object depending on where the object is used in the simulation (i.e., as zone or air loop equipment).
-Maximum supply air temperature
-
-<div>$$T_{SA,max} = \text{HeatDesTemp}_{ZoneOrSystem}$$</div>
-
-Zone Outdoor Air Design Data
-----------------------------
-
-Outdoor air design data may be required for many aspects of a building computer model. Sizing of HVAC equipment, infiltration and ventilation, and specific outdoor air requirements for different zone types are a few examples where required outdoor air quantities may vary. Since there would be a significant chance for data input errors if each individual aspect of the simulation model allowed for independent input of outdoor air design data, this general object is used to define outdoor air design data and this data set may be used throughout the building simulation model.
-
-The design data is provided as a group of inputs that are recognized by designers as standard practice. This information may be used individually or used as a group to calculate summations or maximums of the entered data. These design data include values for:
-
-* Outdoor air per person
-* Outdoor air per zone floor area
-* Outdoor air per zone
-* Outdoor air changes per hour
-
-This design data is entered in an outdoor air design data object and may be referenced by other objects during the simulation. A single specification for outdoor air design data may be used by all other appropriate objects within EnergyPlus, or multiple outdoor air design data objects may be specified and these design data objects may be used as necessary by other objects when outdoor air design quantaties vary for any reason.
-
-### Design Outdoor Air Calculation
-
-The outdoor air design data is entered as a group and referenced through name association to this group of design data (Ref. DesignSpecification:OutdoorAir). The reference name in the following example is "ZoneOAData".
-
-A DesignSpecification:OutdoorAir example:
-
-```idf
-DesignSpecification:OutdoorAir,
-    ZoneOAData,            !- Name
-    Maximum,               !- Outdoor Air Method
-    0.00944,               !- Outdoor Air Flow per Person {m3/s}
-    0.00305;               !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    ,                      !- Outdoor Air Flow per Zone
-    ,                      !- Outdoor Air Flow Air Changes per Hour
-    Min OARequirements Sched; !- Outdoor Air Flow Rate Fraction Schedule Name
-```
-
-
-Given this set of data, the quantity of outdoor air is calculated based on the Outdoor Air Method specified in each outdoor air design data object. In this example, the maximum of the per person and per zone floor area is used to establish the outdoor air quantity.
-
-As previously mentioned, this group of outdoor air design data is reference by other objects used in the simulation. The reference is by the *name* of the outdoor air design data object. Any reference to this name by other objects simply means that the object referencing this data set will use the values specified in this common object. Note that a zone name is not included in the list of data and the calculation of occupancy, zone floor area, or zone volume is implied through this named reference and *the connection to a zone via the referencing object*. For example, if a terminal unit references an outdoor air design data object, the zone served by that terminal unit is used to determine the occupancy, zone floor area, and zone volume in the following calculations.
-
-<div>$$O{A_{people}} = Oc{c_{zone}}\left( {OAFlowperPerson} \right)$$</div>
-
-<div>$$O{A_{floor\,area}} = {A_{zone}}\left( {OAFlowperFloorArea} \right)$$</div>
-
-<div>$$O{A_{zone}} = \left( {OAFlowperZone} \right)$$</div>
-
-<div>$$O{A_{ACH}} = {V_{zone}}\left( {{\raise0.7ex\hbox{${OAFlowAirChangesperHour}$} \!\mathord{\left/ {\vphantom {{OAFlowAirChangesperHour} {3600}}}\right.}\!\lower0.7ex\hbox{${3600}$}}} \right)$$</div>
-
-where:
-
-<span>\(O{A_{people}}\)</span>= outdoor air volume flow rate based on occupancy, [m<sup>3</sup>/s]
-
-<span>\(Oc{c_{zone}}\)</span>= number of occupants in zone, [people]
-
-<span>\(OAFlowperPerson\)</span>= outdoor air volume flow rate per person, [m<sup>3</sup>/s-person]
-
-<span>\(O{A_{floor\;area}}\)</span>= outdoor air volume flow rate based on zone floor area, [m<sup>3</sup>/s]
-
-<span>\({A_{zone}}\)</span>= zone floor area, [m<sup>2</sup>]
-
-<span>\(OAFlowperFloorArea\)</span>= outdoor air volume flow rate per zone floor area, [m<sup>3</sup>/s-m<sup>2</sup>]
-
-<span>\(O{A_{zone}}\)</span>= zone outdoor air volume flow rate, [m<sup>3</sup>/s]
-
-<span>\(OAFlowperZone\)</span>= outdoor air volume flow rate per zone, [m<sup>3</sup>/s]
-
-<span>\(O{A_{ACH}}\)</span>= outdoor air volume flow rate based on air changes per hour, [m<sup>3</sup>/s]
-
-<span>\({V_{zone}}\)</span>= zone volume, [m<sup>3</sup>]
-
-<span>\(OAFlowAirChangesperHour\)</span>= outdoor air volume flow in air changes per hour, [m<sup>3</sup>/s-m<sup>3</sup>]
-
-Given the calculations for each specific type of design data, the method used to calculate the outdoor air design data is then based on a user selected method for this specific outdoor air design data object. The outdoor air methods used to calculate the outdoor air quantity and the associated value for outdoor air volume flow rate are shown here.
-
-Flow/Person =&gt; <span>\(O{A_{people}}\)</span>
-
-Flow/Area =&gt; <span>\(O{A_{floor\,area}}\)</span>
-
-Flow/Zone =&gt; <span>\(O{A_{zone}}\)</span>
-
-AirChanges/Hour =&gt; <span>\(O{A_{ACH}}\)</span>
-
-Sum =&gt; <span>\(O{A_{people}}\, + \,O{A_{floor\,area}}\, + \,O{A_{zone}}\, + \,O{A_{ACH}}\)</span>
-
-Maximum =&gt; <span>\(MAX\left( {O{A_{people}}\,,\,O{A_{floor\,area}}\,,\,O{A_{zone}}\,,\,O{A_{ACH}}} \right)\)</span>
-
-If an Outdoor Air Flow Rate Fraction Schedule Name is specified, the flow rate determined above will be multiplied by the current schedule value.
-
-Examples of objects that reference the outdoor air design data object are:
-
-* AirTerminal:SingleDuct:VAV:NoReheat
-
-* AirTerminal:SingleDuct:VAV:Reheat
-
-### References
-
-ASHRAE Fundamentals 2001. 2001 ASHRAE Fundamentals Handbook. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Pedersen, C.O., D.E. Fisher, and R.J. Liesen. 1997. A heat balance based cooling load calculation procedure. ASHRAE Transactions, Vol. 103(2), pp. 459-468.
-
-Pedersen, C.O. 2001. Toolkit for Building Load Calculations. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
diff --git a/doc/src/docs/EngineeringReference/11-DemandLimiting.md b/doc/src/docs/EngineeringReference/11-DemandLimiting.md
deleted file mode 100644
index a30ec2facbb..00000000000
--- a/doc/src/docs/EngineeringReference/11-DemandLimiting.md
+++ /dev/null
@@ -1,100 +0,0 @@
-
-Demand Limiting
-===============
-
-Demand limiting, or demand management, is a strategy for reducing a building's demand for utilities, e.g., electricity.  Utility companies typically charge a monthly fee for "demand charges" that is based on the peak demand during a certain time period.  Often the peak demand charge is set by one exceptional day that is much higher than the peak demand for an average day during the month.  Therefore, to save utility costs, it is in the interest of building owners to find ways to manage the demand on peak days.  While demand management is generally concerned with the demand for electricity, the future will likely see demand management of other utilities, such as natural gas or water.
-
-Demand limiting controls shut off or reduce the power to non-essential loads in order to reduce the overall building demand.  Some typical controls:
-
-* shut off or dim electric lights, equipment, or HVAC systems
-
-* reset the thermostatic setpoints on HVAC systems
-
-* reduce ventilation load thus electricity demand
-
-* reduce the load of a set of similar components by rotating one or more components "off" for a short time interval
-
-* turn on generators to meet some or all of the building's demand.
-
-The demand limiting controls implemented in EnergyPlus are intended to allow some of the more common demand limiting strategies.  The DemandManagerAssignmentList object is a high level control that makes demand limiting decisions based on a list of possible demand limiting strategies.  Each demand limiting strategy is described in a separate DemandManager object.  Each DemandManager object controls a group of similar load objects of the same type, such as DemandManager:Lights, DemandManager:ElectricEquipment, DemandManager:Thermostats, or DemandManager:Ventilation objects.
-
-### Algorithm
-
-In EnergyPlus the DemandManagerAssignmentList and DemandManager objects are simulated by the Demand Manager module.  The Demand Manager is built into the overall solution method for the program.  For each zone time step, the program executes three major segments of code:
-
-* exterior energy use
-
-* zone heat balance (surface heat balances, internal gains, and air flows)
-
-* HVAC system simulation (air and plant loops)
-
-The exterior energy use segment is completely independent of the zone heat balance and HVAC system simulation.  Exterior energy use handles energy use accounting for exterior lights and exterior equipment that are outside of the building and are not part of the zone heat balance.  The zone heat balance segment includes all of the surface heat balances, internal heat gains, and air flows.  The HVAC system simulation includes air and plant loops with their associated HVAC components.  The behaviour of the HVAC system depends on the results of the zone heat balance.  The HVAC system simulation operates on a variable "system" time step which is automatically shortened if necessary for stability.
-
-The Demand Manager is called after the first pass through the HVAC system simulation, before the system time step is shortened.  After evaluating the DemandManagerAssignmentList object, the Demand Manager decides if demand limiting is required.  If demand limiting is required, the individual DemandManager objects are surveyed to determine which loads can be limited.  Based on the *Demand Manager Priority* selected, the Demand Manager then decides which DemandManager objects should be activated.  In turn, the activated DemandManager objects set the demand limiting hooks on their respective load objects.  Finally, depending on the type of DemandManager objects that were activated, one or more of the major segments of code must be called to be resimulated because the load conditions have changed.  The code segments depend on the type of DemandManager and the relationship of its load objects to the overall solution method.  The table below shows the different DemandManager types and the related code segments that must be resimulated.
-
-
-
-Table 42. Demand Manager Types and Resimulation.
-
-<table class="table table-striped">
-<tr>
-<th>Demand Manager Type</th>
-<th>Resimulate Exterior Energy</th>
-<th>Resimulate Zone Heat Balance</th>
-<th>Resimulate HVAC System</th>
-</tr>
-<tr>
-<td>DemandManager:ExteriorLights</td>
-<td>X</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>DemandManager:Lights</td>
-<td> </td>
-<td>X</td>
-<td>X</td>
-</tr>
-<tr>
-<td>DemandManager:ElectricEquipment</td>
-<td> </td>
-<td>X</td>
-<td>X</td>
-</tr>
-<tr>
-<td>DemandManager:Thermostats</td>
-<td> </td>
-<td> </td>
-<td>X</td>
-</tr>
-<tr>
-<td>DemandManager:Ventilation</td>
-<td> </td>
-<td> </td>
-<td>X</td>
-</tr>
-
-</table>
-
-
-
-All demand limiting controls are disabled during warmup days and sizing runs.
-
-#### Sequential Priority
-
-If the *Demand Manager Priority* field of the DemandManagerAssignmentList object is set to SEQUENTIAL, each DemandManager in the list is activated in sequence from first to last until demand is reduced below the limit or until all managers are activated.  A DemandManager is skipped if it cannot reduce the demand.  Possible reasons that a manager cannot reduce demand include:
-
-* not enough load to limit
-
-* not available because of its *Availability Schedule*
-
-* already activated; load limited during a previous time step.
-
-For each DemandManager in the list that is successfully activated, one or more of the major code segments must be called to be resimulated (see above).  The DemandManagerAssignmentList object is then reevaluated to determine if further demand limiting is required before the next DemandManager is activated.
-
-The implication of sequential priority is that a DemandManagerAssignmentList with many DemandManagers may make many passes through the Demand Manager before all demand limiting decisions are finalized.  Each pass requires an additional resimulation of the current time step.  In some cases this could significantly slow down the overall simulation runtime.  The use of the *Minimum Limit Duration* field can help to ensure that not every DemandManager is being activated at every time step.
-
-#### All Priority
-
-If the *Demand Manager Priority* field of the DemandManagerAssignmentList object is set to ALL, all DemandManagers in the list are activated simultaneously to achieve the maximum demand reduction.  This priority option requires only one final resimulation after all DemandManagers are activated.
-
diff --git a/doc/src/docs/EngineeringReference/12-AlternativeModeling.md b/doc/src/docs/EngineeringReference/12-AlternativeModeling.md
deleted file mode 100644
index 13382f0087d..00000000000
--- a/doc/src/docs/EngineeringReference/12-AlternativeModeling.md
+++ /dev/null
@@ -1,3083 +0,0 @@
-
-Alternative Modeling Processes
-==============================
-
-### RoomAir Models
-
-The group of models described in this section is used to account for non-uniform room air temperatures that may occur within the interior air volume of a zone. These models are accessed using the RoomAirModelType input object. RoomAir modeling was added to EnergyPlus starting with Version 1.2. Although there are many types of analyses (comfort, indoor air quality, etc) that might benefit from localized modeling of how room air varies across space, most of the room air models in EnergyPlus only address the distribution of *temperature* within the zone. This allows surface heat transfer and air system heat balance calculations to be made taking into account natural thermal stratification of air and different types of intentional air distribution designs such as under-floor and side-wall displacement ventilation that purport to extract room air at higher-than-mean temperatures. The exception is the RoomAirflowNetwork model, which integrates the AirflowNetwork model and applies the nodal airflow model within zones. Note that EnergyPlus does **not** have completely general methods of modeling room air that are applicable to every conceivable type of airflow that might occur in a zone. Such models (e.g. RANS-CFD) are too computationally expensive to use with EnergyPlus for the foreseeable future. The models that are available in EnergyPlus offer only limited modeling capabilities for select room airflow configurations. Also note that because the complete mixing model for room air has long been the standard in building energy simulation, there is not currently a consensus on how to best model non-uniform air temperatures in buildings. Therefore, it is up to the user to have a good understanding of when, where, and how to apply the room air models available in EnergyPlus. The rest of this section provides some guidance in the way of examples and further discussion of the models available in EnergyPlus.
-
-EnergyPlus offers the different types of air models listed in the table below along with the input objects associated with the use of that model.
-
-
-
-Table 43. Summary of room air models available in EnergyPlus
-
-<table class="table table-striped">
-<tr>
-<th>Air model name</th>
-<th>Applicability</th>
-<th>Input Objects Required</th>
-</tr>
-<tr>
-<td>Well-Mixed</td>
-<td>All zones</td>
-<td>None, default</td>
-</tr>
-<tr>
-<td>User Defined</td>
-<td>Any zone where the user has prior knowledge of the temperature pattern</td>
-<td>‘RoomAirModelType’, ‘RoomAir:TemperaturePattern:UserDefined’, ‘RoomAir:TemperaturePattern: xx’</td>
-</tr>
-<tr>
-<td>One-Node Displacement Ventilation (Mundt)</td>
-<td>displacement ventilation in typical office-type zones</td>
-<td>‘RoomAirModelType’, ‘RoomAirSettings:OneNodeDisplacementVentilation’, ‘RoomAir:Node’’</td>
-</tr>
-<tr>
-<td>Three-Node Displacement Ventilation (UCSD)</td>
-<td>displacement ventilation</td>
-<td>‘RoomAirModelType’, ‘RoomAirSettings:ThreeNodeDisplacementVentilation’</td>
-</tr>
-<tr>
-<td>Under-Floor Air Distribution Interior Model (UCSD)</td>
-<td>Interior zones served by a UFAD system</td>
-<td>‘RoomAirModelType’, ‘RoomAirSettings:UnderFloorAirDistributionInterior’</td>
-</tr>
-<tr>
-<td>Under-Floor Air Distribution Exterior Model (UCSD)</td>
-<td>Exterior zones served by a UFAD system</td>
-<td>‘RoomAirModelType’, ‘RoomAirSettings:UnderFloorAirDistributionExterior’</td>
-</tr>
-<tr>
-<td>UCSD Cross Ventilation</td>
-<td>cross ventilation</td>
-<td>‘RoomAirModelType’, ‘RoomAirSettings:CrossVentilation’</td>
-</tr>
-<tr>
-<td>RoomAirflowNetwork</td>
-<td>Room air model using AirflowNetwork</td>
-<td>‘RoomAirModelType’, 
-‘RoomAirSettings:AirflowNetwork’
-‘RoomAirflowNetwork:Node’,
-‘RoomAirflowNetwork:Node:AdjacentSurfaceList’,
-‘RoomAirflowNetwork:Node:InternalGains’,
-‘RoomAirflowNetwork:Node:InternalGains’,
-‘AirflowNetwork:IntraZone:Node’,
-‘AirflowNetwork:IntraZone:Linkage’
-</td>
-</tr>
-</table>
-
-The room air models are coupled to the heat balance routines using the framework described by Griffith and Chen (2004).  Their framework was modified to include features needed for a comprehensive program for annual energy modeling rather than one for hourly load calculations.  The formulation is largely shifted from being based on the setpoint temperature to one based on the current mean air temperature.  This is necessary to allow for floating temperatures and dual setpoint control where there may be times that the mean zone temperatures are inside the dead band.  The coupling framework was also extended to allow for exhaust air flows (e.g. bathroom exhaust fans) in addition to air system return flows.
-
-The inside face temperature calculation is modified by rewriting the zone air temperature, *T<sub>a</sub>*, with an additional subscript, *i*, for the surface index (<span>\({T_{{a_j}}} \to {T_{{a_{i,j}}}}\)</span>or <span>\({T_{{a_{}}}} \to {T_{{a_i}}}\)</span>).  The inside face heat balance is solved for its surface temperature using,
-
-<div>$${T_{{s_{i,j}}}} = \frac{{{T_{s{o_{i,j}}}}{Y_{i,o}} + \sum\limits_{k = 1}^{nz} {{T_{s{o_{i,j - k}}}}} {Y_{i,k}} - \sum\limits_{k = 1}^{nz} {{T_{{s_{i,j - k}}}}} {Z_{i,k}} + \sum\limits_{k = 1}^{nq} {{\Phi_{i,k}}{{q''}_{k{i_{i,j - k}}}} + {T_{{a_{i,j}}}}{h_{{c_{i,j}}}} + {{q''}_{LWS}} + {{q''}_{LWX}} + {{q''}_{SW}} + {{q''}_{sol}}} }}{{{Z_{i,o}} + {h_{{c_{i,j}}}}}}$$</div>
-
-where,         *T<sub>s</sub>*         is the inside face temperature
-
-*i*           subscript indicates individual surfaces
-
-      *j*           subscript indicates current time step
-
-      *k*          subscript indicates time history steps
-
-      *T<sub>so</sub>*        is the outside face temperature
-
-      *Y<sub>i</sub>        * are the cross CTF coefficients
-
-      *Z<sub>i                  </sub>* are the inside CTF coefficients
-
-      *Φ<sub>i</sub>*         are the flux CTF coefficients
-
-      <span>\({q''_{ki}}\)</span>       is the conduction heat flux through the surface
-
-      <span>\({h_{{c_i}}}\)</span>       is the surface convection heat transfer coefficient
-
-      *T<sub>a</sub>*         is the near-surface air temperature
-
-      <span>\({q''_{LWS}}\)</span>    is the longwave radiation heat flux from equipment in zone
-
-      <span>\({q''_{LWX}}\)</span>    is the net long wavelength radiation flux exchange between zone surfaces
-
-      <span>\({q''_{SW}}\)</span>     is the net short wavelength radiation flux to surface from lights
-
-      <span>\({q''_{sol}}\)</span>      is the absorbed direct and diffuse solar (short wavelength) radiation
-
-#### References:
-
-Griffith, B. and Q. Chen. 2004. Framework for coupling room air models to heat balance load and energy calculations (RP-1222). International Journal of Heating, Ventilating, Air-conditioning and Refrigerating Research. ASHRAE, Atlanta GA.  Vol 10. No 2. April 2004.
-
-### User Defined RoomAir Temperatures
-
-The input object RoomAir:TemperaturePattern:UserDefined provides a capabity for users to define the sort of air temperature pattern he or she expects in the zone.  With these models, the pattern is generally set beforehand and does not respond to conditions that evolve during the simulation.  (Exception: the pattern available through the RoomAir:TemperaturePattern:TwoGradient object will switch between two different pre-defined vertical gradients depending on the current value of certain temperatures or thermal loads. )
-
-The user-defined patterns obtain the mean air temperature, <span>\({T_{MAT}}\)</span>, from the heat balance domain and then produce modified values for:
-
-      <span>\({T_{ai}}\)</span>       the adjacent air temperature which is then used in the calculation of inside face surface temperature during the heat balance calculations,
-
-      <span>\({T_{leaving}}\)</span>  the temperature of air leaving the zone and entering the air system returns
-
-      <span>\({T_{exhaust}}\)</span>  the temperature of air leaving the zone and entering the exhaust.
-
-      <span>\({T_{stat}}\)</span>     the temperature of air “sensed� at the thermostat (not currently used in air system control because air system flows use load-based control).
-
-The user defined room air models used indirect coupling so that the patterns provide values for, or ways to calculate, how specific temperatures differ from <span>\({T_{MAT}}\)</span>.  The various <span>\(\Delta T\)</span> values determined from the model are applied to <span>\({T_{MAT}}\)</span> as follows:
-
-<div>$${T_{ai}} = \Delta {T_{ai}} + {T_{MAT}}$$</div>
-
-(where “*i’s�* represents each surface in the zone that is affected by the model)
-
-<div>$${T_{leaving}} = \Delta {T_{return}} + {T_{MAT}}$$</div>
-
-<div>$${T_{exhaust}} = \Delta {T_{exhaust}} + {T_{MAT}}$$</div>
-
-<div>$${T_{stat}} = \Delta {T_{stat}} + {T_{MAT}}$$</div>
-
-The patterns defined by the object ‘RoomAir:TemperaturePattern:SurfaceMapping’ are fairly straightforward.  The user directly inputs values for <span>\(\Delta {T_{ai}}\)</span> for each surface.  The pattern “maps� specific surfaces, identified by name, to <span>\(\Delta {T_{ai}}\)</span> values.  This provides completely general control (but in practice may be cumbersome to use).  The other patterns focus on temperature changes in the vertical direction.  Surfaces do not need to be identified, but all the surfaces with the same height will be assigned the same <span>\(\Delta {T_{ai}}\)</span> values.
-
-The patterns defined by the object ‘RoomAir:TemperaturePattern:NondimensonalHeight’ apply a temperature profile based on a non-dimensionalized height, <span>\({\rm Z}\)</span>.  The height of each surface is defined to be the z-coordinate of the surface’s centroid relative to the average z-coordinate of the floor surfaces.  The zone ceiling height is used as the length scale to non-dimensionalize each surface’s height so that,
-
-<div>$${{\rm Z}_i} = ({z_{i,centroid}} - {z_{floorAvg}})/Ceiling\;Height$$</div>
-
-(where “*i’s�* represents each surface in the zone that is affected by the model)
-
-The values for <span>\({Z_i}\)</span> are constrained to be between 0.01 and 0.99 because the value is meant to describe the air layer near the surface (say approximate 0.1 m from the surface) rather than the surface itself.
-
-The user-defined profile is treated as a look up table or piecewise linear model.  The values for <span>\(\Delta {T_{ai}}\)</span> are determined by searching the <span>\({\rm Z}\)</span> values in the user-defined profile and performing linear interpolation on the associated <span>\(\Delta {T_a}\)</span> values.
-
-The patterns defined by the object ‘RoomAir:TemperaturePattern:ConstantGradient’ apply a constant temperature gradient in the vertical direction.  The model assumes that <span>\({T_{MAT}}\)</span> occurs at the mid-plane so that <span>\({{\rm Z}_{{T_{MAT}}}} = 0.5\)</span> (by definition).  The surface <span>\({Z_i}\)</span> values are compared to <span>\({Z_{{T_{MAT}}}}\)</span>and then scaled with zone ceiling height to obtain values for the change in height (in units of meters), <span>\(\Delta z\)</span>.  The user defined gradient, <span>\(grad\)</span>, (units of ºC/m) is then used to determine <span>\(\Delta {T_{ai}}\)</span> values using
-
-<div>$$\Delta {T_{ai}} = \Delta z * grad$$</div>
-
-The patterns defined by the object ‘RoomAir:TemperaturePattern:TwoGradient’ are very similar to the constant gradient pattern above but the value of <span>\(grad\)</span> used at any given time is selected by interpolating between two user-defined values for <span>\(grad\)</span>.  Five options are available, three based on temperatures and two based on thermal loads – see the Input Output Reference.  The user provides upper and lower bounding values.  If the current value of the “sensing� variable lies between the upper and lower bounds, then <span>\(grad\)</span> is determined using linear interpolation.  If the designated value is above the upper bound then the upper value for <span>\(grad\)</span> is used (no extrapolation).  Similarly, if the designated value is below the lower bound, then the lower value for <span>\(grad\)</span> is used.  Note that “upper� and “lower� indicate the temperature and heat rate bounds and that the values for <span>\(grad\)</span> do not have to follow in the same way; the <span>\(grad\)</span> value for the lower bound could be higher than the <span>\(grad\)</span> value for the upper bound (providing a something of a reverse control scheme).  Rather than directly using <span>\(\Delta T\)</span> values from the user, the temperatures for the return air, exhaust and thermostat are determined based on user-entered heights (in units of meters from the floor) and applying the current value for <span>\(grad\)</span>.
-
-### One-Node Displacement Ventilation RoomAir Model
-
-The input object RoomAirSettings:OneNodeDisplacementVentilation provides a simple model for displacement ventilation.  Mundt (1996) points out that a floor air heat balance provides a simple and reasonably accurate method of modeling the temperature near the floor surface. The slope of a linear temperature gradient can then be obtained by adding a second upper air temperature value that comes from the usual overall air system cooling load heat balance.  The figure below diagrams the temperature distribution versus height being calculated by the model.  Mundt’s floor air heat balance is extended to include convection heat gain from equipment and by ventilation or infiltration that may be introduced near the floor in order to maintain all the terms in the air heat balance of the Heat Balance Model.  This yields the following heat balance for a floor air node,
-
-<div>$$\rho \,{c_p}\dot V({T_{AirFloor}} - {T_{Supply}}) = {h_{cFloor}}{A_{Floor}}({T_{Floor}} - {T_{AirFloor}}) + {Q_{ConvSourceFloor}} + {Q_{InfilFloor}}$$</div>
-
-where
-
-*�* is the air density
-
-*c<sub>p</sub>* is the air specific heat at constant pressure
-
-<span>\(\mathop V\limits^\cdot  \)</span>is the air system flow rate
-
-*T<sub>supply</sub>* is the air system’s supply air drybulb temperature
-
-*h<sub>cFloor</sub>*  is the convection heat transfer coefficient for the floor
-
-*A<sub>floor</sub>* is the surface area of the floor
-
-*T<sub>floor</sub>* is the surface temperature of the floor
-
-*Q<sub>convSourceFloor</sub> * is the convection from internal sources near the floor (&lt; 0.2 m)
-
-*Q<sub>InfilFloor</sub>*  is the heat gain (or loss) from infiltration or ventilation near the floor
-
-
-
-“Floor splits� are the fraction of total convective or infiltration loads that are dispersed so as to add heat to the air located near the floor.  The user prescribes values for floor splits as input.  No guidance is known to be available to use in recommending floor splits, but the user could for example account for equipment known to be near the floor, such as tower computer cases, or supplementary ventilation designed to enter along the floor.  The equation above can be solved directly for *T<sub>AirFloor</sub>* and is used in the form of the equation below,
-
-<div>$${T_{AirFloor}} = \frac{{\rho \,{c_p}\dot V{T_{Supply}} + \sum {{h_{cFloor}}{A_{Floor}}{T_{Floor}}}  + {{\dot Q}_{ConvSourceFloor}} + {{\dot Q}_{InfilFloor}}}}{{\rho \,{c_p}\dot V + \sum {{h_{cFloor}}{A_{Floor}}} }}$$</div>
-
-The upper air node temperature is obtained by solving the overall air heat balance for the entire thermal zone for the temperature of the air leaving the zone and going into the air system return, *T<sub>leaving</sub>*.
-
-<div>$${T_{Leaving}} = \frac{{ - {{\dot Q}_{sys}}}}{{p{c_p}\dot V}} + {T_{Supply}}$$</div>
-
-where <span>\({\dot Q_{sys}}\)</span> is the air system heat load with negative values indicating a positive cooling load.  Values for <span>\({\dot Q_{sys}}\)</span> are computed by the load calculation routines and passed to the air model.  The vertical temperature gradient or slope, *dT/dz*, is obtained from,
-
-<div>$$\frac{{dT}}{{dz}} = \frac{{{T_{Leaving}} - {T_{AirFloor}}}}{{{H_{return}}}}$$</div>
-
-where *H<sub>return</sub>* is the distance between the air system return and the floor air node assumed to be 0.1 m from the floor and *z* is the vertical distance.
-
-![](media/image2341.svg.png)
-
-Figure 132.  Height versus temperature schematic for Mundt model
-
-The constant slope allows obtaining temperatures at any vertical location using,
-
-<div>$${T_{{a_i}}} = {T_{leaving}} - \frac{{dT}}{{dz}}({z_{leaving}} - {z_i})$$</div>
-
-So for example the temperatures near the ceiling can easily be determined. Accounting for the location of the thermostat inside the zone (e.g. 1.1 m) is accomplished by returning the temperature for the appropriate height to the appropriate air node used for control. If the walls are subdivided in the vertical direction as shown in the figure above, then the air model can provide individual values for each surface based on the height and slope.  However, no additional heat balances are necessarily made (in the air domain) at these points as all the surface convection is passed to the model in the totaled value for <span>\({\dot Q_{sys}}\)</span>.
-
-#### References
-
-Mundt, E. 1996. The performance of displacement ventilation systems-experimental and theoretical studies, Ph. D. Thesis, Royal Institute of Technology, Stockholm.
-
-### Three-Node Displacement Ventilation RoomAir Model
-
-#### Overview
-
-The input object RoomAirSettings:ThreeNodeDisplacementVentilation provides a simple model for heat transfer and vertical temperature profile prediction in displacement ventilation. The fully-mixed room air approximation that is currently used in most whole building analysis tools is extended to a three node approach, with the purpose of obtaining a first order precision model for vertical temperature profiles in displacement ventilation systems. The use of three nodes allows for greatly improved prediction of thermal comfort and overall building energy performance in low energy cooling strategies that make use of unmixed stratified ventilation flows.
-
-The UCSD Displacement Ventilation Model is one of the non-uniform zone models provided through the Room Air Manager in EnergyPlus. The intent is to provide a selection of useful non-uniform zone air models to enable the evaluation of air-conditioning techniques that use stratified or partially stratified room air. Such techniques include displacement ventilation (DV) and underfloor air distribution (UFAD) systems. The methodology can also include, in principle, natural displacement ventilation and also wind-driven cross-ventilation (CV).
-
-#### Displacement Ventilation
-
-A DV system is a complete contrast to a conventional forced air system. In a conventional system conditioned air is delivered at ceiling level and the intent is to create a fully mixed space with uniform conditions. In a DV system conditioned air is delivered at floor level and low velocity in order to minimize mixing and to establish a vertical temperature gradient. The incoming air “displaces� the air above it which, in turn,  is exhausted through ceiling level vents. In DV a noticeable interface occurs between the occupied zone of the room and a mixed hot layer near the ceiling of the room(Dominique & Guitton, 1997). Maintaining the lower boundary of this warm layer above the occupied zone is one of the many unique challenges of displacement ventilation design. Often DV systems use 100% outside air. The vertical displacement air movement means that convective heat gains introduced near the ceiling will be removed without affecting the occupied region of the room. Also a fraction of the heat gains that occur in the occupied zones rise as plumes into the upper part of the space, thereby reducing the cooling load. Similarly the fresh air will be used more effectively than with a fully mixed system: the fresh air won’t be “wasted� in the upper, unoccupied region of the room. Finally, the vertical temperature gradient means that the average room temperature can be higher for a DV conditioned room than with a conventionally conditioned room: the occupants feel the lower temperature in the lower region of the room and are unaffected by the higher temperature near the ceiling. However, whenever the outside air temperature is above ≈19°C this advantage is mostly lost: the internal loads must be removed from the space independently of the airflow pattern (during the warmer hours buildings tend to be almost closed to the outside, operating in closed loop). The inflow temperature advantage is then only useful for the minimum outside air that must always be provided (in most cases this remaining advantage is negligible).
-
-DV systems have limitations. In order to avoid chilling the occupants the supply air temperature used for DV is considerably higher than that used in conventional forced-air systems. This can lead to problems in removing both sensible and latent loads. Exterior spaces may have conditions that are not conducive to establishing a vertical temperature gradient. DV systems seem to be best suited to interior spaces with only moderate loads.
-
-#### Non-uniform zone models
-
-Several types of models have been proposed as suitable for inclusion in building energy simulation (BES) programs. These models must be simple enough not to impose an undue computational burden on a BES program, yet provide enough predictive capability to produce useful comparisons between conventional and stratified zone operation strategies. ASHRAE RP-1222 (Chen & Griffith 2002) divides the candidate models into two categories: *nodal* and *zonal*. Nodal models describe the zone air as a network of nodes connected by flow paths; each node couples convectively to one or more surfaces. Zonal models are coarse–grained finite volume models. ASHRAE RP-1222 provides a short history (and examples) of each type of model. In terms of nodal models for displacement ventilation we mention the Mundt model (Mundt 1996), since it is implemented in EnergyPlus, and the Rees-Haves model (Rees & Haves 2001) since it is a well developed nodal-type model and is implemented in the RP-1222 toolkit. The Rees-Haves model, while successful in predicting the flow and temperature field for geometries similar to those used in its development, can suffer from lack of flexibility and clarity in the modeling approximations. When dealing with diverse geometries it is not clear that the flow coefficients used in the model are applicable or why they can be used since plumes, the fundamental driving mechanisms of the displacement flow, are not explicitly modeled. This is the main difference between the DV models implemented in theRP-1222 toolkit and the model that is described here.
-
-The UCSD DV model is closer to a nodal model than to a zonal model. However, it is best to classify it in a separate category: plume equation based multi-layer models (Linden *et al*. 1990, Morton *et al*. 1956). These models assume that the dominant mechanism is plume-driven flow from discrete internal sources and that other effects (such as buoyancy driven flow at walls or windows) may be neglected. Alternatively, these heat sources also produce plumes that can be included in the model. The result is a zone divided vertically into two or more well separated regions – each region characterized by a single temperature or temperature profile. This characterization allows the physics of the heat gains and the ventilation flow to be represented in a realistic manner, without the introduction of *ad hoc* assumptions.
-
-#### Model Description
-
-#### Single Plume Two Layer Model
-
-The simplest form of the plume equation based models is the case of a single plume in an adiabatic box with constant supply air flow. For this configuration two layers form in the room: a lower layer with similar density and temperature as the inflow air and a mixed upper layer with the same density / temperature as the outflow air. The main assumption of this model, successfully validated against scaled model experiments (Linden *et al.* 1990), is that the interface between the two layers occurs at the height (h) where the vertical buoyancy driven plume flow rate is the same as the inflow rate. For a point source of buoyancy in a non-stratified environment (a plume) the airflow rate increases with vertical distance from the source according to:
-
-<div>$$\dot V = C\cdot {B^{1/3}}{z^{5/3}}$$</div>
-
-where
-
-<span>\(\dot V\)</span>= plume volume flux [m3/s]
-
-<span>\(B\)</span>= buoyancy flux  [m4/s3]
-
-<span>\(z\)</span>= vertical distance above source [m]
-
-<div>$$C = \frac{6}{5}\alpha {(\frac{9}{{10}}\alpha )^{1/3}}{\pi ^{2/3}}$$</div>
-
-<span>\(\alpha \)</span>= plume entrainment constant; a value of  0.127 is used, suitable for top-hat profiles for density and velocity across the plumes.
-
-For an ideal gas
-
-<div>$$\Delta \rho /\rho  = \Delta {\rm T}/{\rm T}$$</div>
-
-resulting in the following relation between heat input rate and buoyancy flux:
-
-<div>$$B = \frac{{g\dot Q}}{{\rho {C_p}T}}$$</div>
-
-where
-
-<span>\(\rho \)</span>= density of air [kg/m3]
-
-<span>\(T\)</span>= air temperature [K]
-
-<span>\(g\)</span>= acceleration of gravity [m/s2]
-
-<span>\(\dot Q\)</span>= heat input rate [W]
-
-<span>\({C_p}\)</span>=specific heat capacity of air [J/kgK]
-
-Since the plume volume flow rate increases with height with exponent 5/3, for any room inflow rate (F, (m<sup>3</sup>/s)) there will always be a height (h,(m)) where the plume driven flow rate matches the inflow rate. This height is obtained by setting (1.1) equal to F and solving for z=h:
-
-<div>$$h = {F^{3/5}}/({C^{3/5}}{B^{1/5}})$$</div>
-
-Substituting in and introducing air properties at 20 C gives:
-
-<div>$$h = 24.55\cdot {F^{3/5}}/{\dot Q^{1/5}}$$</div>
-
-#### Multiple Plumes and Wall Heat Transfer
-
-Of course, it would be rare for a real world case to consist of a single point-source plume originating on the floor, unaffected by heat gains from walls and windows. For multiple plumes of equal strength a straight-forward extension of the single is possible. N plumes of unequal strength result in the formation of n vertical layers. This case is much more complex but if we are satisfied with a first order precision model the equal strength model can be used by averaging the plume strengths (Carrilho da Graça, 2003). Even in a case where all plumes are of equal strength, nearby plumes may coalesce. Plumes that are less than 0.5 meters apart at their source will coalesce within 2 meters (Kaye & Linden,2004).
-
-As the complexity of the physical systems modeled increases some limitations must be imposed. In particular, the biggest challenge remains the interaction between wall driven boundary layers (positively and negatively buoyant) and displacement flows. For this reason, the model that is developed below is not applicable when:
-
-1.    Downward moving buoyancy driven airflow rate is of the same order of magnitude as plume driven flow (these airflow currents are typically generated on lateral surfaces or in the ceiling whenever these surfaces are much cooler than the room air).
-
-2.    Upward moving wall or floor generated buoyancy flux in the lower layer is of the same order of magnitude as plume driven flow.
-
-Although these limitations are significant it is important to note that even in the presence of dominant convection from the floor surface, a buoyancy, two layer flow can be established whenever the plume buoyancy flux is more than 1/7 of the horizontal flux (Hunt *et al.* 2002). A two layer structure can also originate when the only heat source is a heated portion of the room floor, as long as the heated area does not exceed 15% of the room floor (Holford *et al.* 2002).
-
-For the case of multiple non-coalescing plumes (n), with equal strength, the total vertical airflow for a given height is:
-
-<div>$$\mathop V\limits^\cdot   = Cn{B^{{\raise0.5ex\hbox{$\scriptstyle 1$}\kern-0.1em/\kern-0.15em\lower0.25ex\hbox{$\scriptstyle 3$}}}}{z^{{\raise0.5ex\hbox{$\scriptstyle 5$}\kern-0.1em/\kern-0.15em\lower0.25ex\hbox{$\scriptstyle 3$}}}}$$</div>
-
-resulting in a mixed layer height of:
-
-<div>$$h = \frac{{24.55{F^{{\raise0.5ex\hbox{$\scriptstyle 3$}\kern-0.1em/\kern-0.15em\lower0.25ex\hbox{$\scriptstyle 5$}}}}}}{{{{\left( {{n^3}\dot Q} \right)}^{{\raise0.5ex\hbox{$\scriptstyle 1$}\kern-0.1em/\kern-0.15em\lower0.25ex\hbox{$\scriptstyle 5$}}}}}}$$</div>
-
-#### Implementation
-
-The model predicts three temperatures that characterize the three main levels in the stratification of the room:
-
-1.    a floor level temperature T<sub>floor</sub> to account for the heat transfer from the floor into the supply air
-
-2.    an occupied subzone temperature T<sub>oc</sub> representing the temperature of the occupied region;
-
-3.    an upper level temperature T<sub>mx</sub> representing the temperature of the upper, mixed region and the outflow temperature.
-
-We assume that the model for multiple, equal strength plumes (equations and will be adequate for our calculations. The supply air flow rate <span>\(\dot V\)</span> is obtained by summing all the air flows entering the zone: supply air, infiltration, ventilation, and inter-zone flow. The heat gain <span>\(\dot Q\)</span> is estimated by summing all the convective internal gains located in the occupied subzone – task lights, people, equipment – and dividing this power equally among the n plumes. With these assumptions we can describe the implementation.
-
-The UCSD DV model is controlled by the subroutine *ManageUCSDDVModel* which is called from the *RoomAirModelManager*. The *RoomAirModelManager* selects which zone model will be used for each zone.
-
-The calculation is done in subroutine *CalcUCSDDV*. First we calculate the convective heat gain going into the upper and lower regions.
-
-<div>$$
-  \dot Q_{ocz} = \dot Q_{oc,conv} + \dot Q_{tl,conv} + \dot Q_{eleq,conv} + \dot Q_{gaseq,conv} + \dot Q_{otheq,conv} + \dot Q_{hw,conv} + \dot Q_{stmeq,conv} + \dot Q_{bb,conv}
-$$</div>
-
-<div>$${\dot Q_{mxz}} = {\dot Q_{gl,conv}} + {\dot Q_{ltp}} + {\dot Q_{htrad,conv}}$$</div>
-
-<div>$${\dot Q_{tot,conv}} = {\dot Q_{ocz}} + {\dot Q_{mxz}}$$</div>
-
-Next we sum up the inlet air flows in the form of MCP (mass flow rate times the air specific heat capacity) and MCPT (mass flow rate times C<sub>p</sub> times air temperature).
-
-<div>$$MC{P_{zone}} = MC{P_i} + MC{P_{vent}} + MC{P_{mix}}$$</div>
-
-<div>$$MC{P_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}$$</div>
-
-<div>$$MC{P_{tot}} = MC{P_{zone}} + MC{P_{sys}}$$</div>
-
-<div>$$MCP{T_{zone}} = MCP{T_i} + MCP{T_{vent}} + MCP{T_{mix}}$$</div>
-
-<div>$$MCP{T_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}{T_i}$$</div>
-
-<div>$$MCP{T_{tot}} = MCP{T_{zone}} + MCP{T_{sys}}$$</div>
-
-The number of plumes per occupant <span>\({N_{plumesperpers}}\)</span> is a user input. The total number of plumes in the zone is:
-
-<div>$${N_{plumes}} = {N_{occ}} \cdot {N_{plumesperperson}}$$</div>
-
-The gains fraction <span>\(F{r_{gains}}\)</span>is a user input via a schedule. It is the fraction of the convective gains in the occupied subzone that remain in that subzone. Using this we calculate the total power in the plumes and the power per plume.
-
-<div>$${\dot Q_{plumes}} = (1 - F{r_{gains}}) \cdot {\dot Q_{tot,conv}}$$</div>
-
-<div>$${\dot Q_{perplume}} = {\dot Q_{plumes}}/{N_{plumes}}$$</div>
-
-We now make an initial estimate of the height fraction *Fr<sub>hb</sub>* (height of the boundary layer divided by the total zone height).
-
-<div>$$F{r_{hb}} = \left( {{{24.55} \mathord{\left/ {\vphantom {{24.55} {{H_{ceil}}}}} \right. } {{H_{ceil}}}}} \right){\left( {\frac{{0.000833 \cdot MC{P_{tot}}}}{{{N_{plumes}} \cdot \dot Q_{perplume}^{1/3}}}} \right)^{3/5}}$$</div>
-
-where 0.000833  = <span>\(1/({\rho_{air}} \cdot {c_{p,air}})\)</span>converts <span>\(MC{P_{tot}}\)</span> to a volumetric flow rate. Next we iterate over the following 3 steps.
-
-#### Iterative procedure
-
-1.    Call subroutine *HcUCSDDV* to calculate a convective heat transfer coefficient for each surface in the zone, an effective air temperature for each surface, and HA<sub>mx</sub>, HAT<sub>mx</sub>, HA<sub>oc</sub>, HAT<sub>oc</sub>, HA<sub>fl</sub>, and HAT<sub>fl</sub>. Here HA is <span>\(\sum\limits_{surfaces} {{h_{c,i}}}  \cdot {A_i}\)</span> for a region and HAT is <span>\(\sum\limits_{surfaces} {{h_{c,i}}}  \cdot {A_i} \cdot {T_i}\)</span> for a region. The sum is over all the surfaces bounding the region; <span>\({h_{c,i}}\)</span> is the convective heat transfer coefficient for surface i, <span>\({A_i}\)</span> is the area of surface i,  and <span>\({T_i}\)</span> is the surface temperature of surface i.
-
-2.    Recalculate <span>\(F{r_{hb}}\)</span> using the equation .
-
-3.    Calculate the three subzone temperatures: *T<sub>floor,</sub> T<sub>oc</sub>* and *T<sub>mx</sub>*.
-
-The h<sub>c</sub>’s calculated in step 1 depend on the subzone temperatures and the boundary layer height. In turn the subzone temperatures depend on the HA and HAT’s calculated in step 1. Hence the need for iteration
-
-Next we describe each steps 1 and 3 in more detail.
-
-#### Step 1
-
-Subroutine *HcUCSDDV* is quite straightforward. It loops through all the surfaces in each zone and decides whether the surface is located in the upper, mixed subzone or the lower, occupied subzone, or if the surface is in both subzones. If entirely in one subzone the subzone temperature is stored in the surface effective temperature variable *TempEffBulkAir(SurfNum)* and h<sub>c</sub> for the surface is calculated by a call to subroutine *CalcDetailedHcInForDVModel*. This routine uses the “detailed� natural convection coefficient calculation that depends on surface tilt and <span>\(\Delta {T^{1/3}}\)</span>. This calculation is appropriate for situations with low air velocity.
-
-For surfaces that bound 2 subzones, the subroutine calculates h<sub>c</sub> for each subzone and then averages them, weighting by the amount of surface in each subzone.
-
-During the surface loop, once the h<sub>c</sub> for a surface is calculated, the appropriate subzone HA and HAT sums are incremented. If a surface is in 2 subzones the HA and HAT for each subzone are incremented based on the area of the surface in each subzone.
-
-#### Step 3
-
-The calculation of  subzone temperatures follows the method used in the ***ZoneTempPredictorCorrector*** module and described in the section **Basis for the System and Zone Integration**. Namely a third order finite difference expansion of the temperature time derivative is used in updating the subzone temperatures. Otherwise the subzone temperatures are obtained straightforwardly by solving an energy balance equation for each subzone.
-
-<div>$$
-  T_{fl} = (C_{air,fl} \cdot (3 \cdot T_{ - 1,fl} - (3/2) \cdot T_{ - 2,fl} + (1/3) \cdot T_{ - 3,fl}) + HAT_{fl} + MCPT_{tot})  / ((11/6) \cdot C_{air,fl} + HA_{fl} + MCP_{tot})
-$$</div>
-
-<div>$$
-  \begin{array}{l}
-    T_{oc} = (C_{air,oc} \cdot (3 \cdot T_{ - 1,oc} - (3/2) \cdot T_{ - 2,oc} + (1/3) \cdot T_{ - 3,oc}) + \dot Q_{ocz} \cdot Fr_{gains} + HAT_{oc} + T_{fl} \cdot MCP_{tot}) / (11/6) \cdot C_{air,oc} + HA_{oc} + MCP_{tot})
-    T_{mx} = (C_{air,mx} \cdot (3 \cdot T_{ - 1,mx} - (3/2) \cdot T_{ - 2,mx} + (1/3) \cdot T_{ - 3,mx}) + \dot Q_{ocz} \cdot (1 - Fr_{gains}) + \dot Q_{mxz} + HAT_{mx} + T_{oc} \cdot MCP_{tot}) / ((11/6) \cdot C_{air,mx} + HA_{mx} + MCP_{tot})
-  \end{array}
-$$</div>
-
-Here <span>\({C_{air,fl}}\)</span>, <span>\({C_{air,oc}}\)</span>, and <span>\({C_{air,mx}}\)</span> are the heat capacities of the air volume in each subzone. <span>\({C_{air,mx}}\)</span> is calculated by
-
-<div>$${R_{air,mx}} = {V_{mx}} \cdot (\Delta {z_{mx}}/{z_{ceil}}) \cdot {\rho_{air,mx}} \cdot {c_{p,air,mx}} \cdot Mu{l_{cap}}/(\Delta {t_z} \cdot 3600)$$</div>
-
-<div>$${C_{air,mx}} = {R_{air,mx}} \cdot \Delta {t_z}/\Delta {t_{sys}}$$</div>
-
-The other subzone air heat capacities are calculated in the same manner.
-
-#### Mixed calculation
-
-The above iterative procedure assumed that displacement ventilation was taking place: i.e., conditions were favorable temperature stratification in the zone. Now that this calculation is complete and the subzone temperatures and depths calculated, we check to see if this assumption was justified. If not, zone conditions must be recalculated assuming a well-mixed zone.
-
-If <span>\({T_{mx}} &lt; {T_{oc}}\)</span> or <span>\(MC{P_{tot}} \le 0\)</span> or <span>\({H_{fr}} \cdot {H_{ceil}} &lt; {H_{fl,top}} + \Delta {z_{occ,\min }}\)</span> then the following mixed calculation will replace the displacement ventilation calculation.
-
-**Note:**  <span>\(\Delta {z_{occ,\min }}\)</span> is the minimum thickness of occupied subzone. It is set to 0.2 meters. <span>\({H_{fl,top}}\)</span>is the height of the top of the floor subzone. It is defined to be 0.2 meters; that is, the floor subzone is always 0.2 meters thick and <span>\({T_{fl}}\)</span> is the temperature at 0.1 meter above the floor surface.
-
-The mixed calculation iteratively calculates surface convection coefficients and room temperature just like the displacement ventilation calculation described above. In the mixed case however, only one zone temperature *T<sub>avg</sub>* is calculated. The 3 subzone temperatures are then set equal to *T<sub>avg</sub>*.
-
-First, *Fr<sub>hb</sub>*  is set equal to zero.
-
-Then the code iterates over these steps.
-
-1.    Calculate *T<sub>avg</sub>* using
-
-<div>$$
-  T_{avg} = (C_{air,z} \cdot (3 \cdot T_{ - 1,z} - (3/2) \cdot T_{ - 2,z} + (1/3) \cdot T_{ - 3,z}) + \dot Q_{tot,conv} + HAT_{oc} + HAT_{mx} + HAT_{fl} + MCPT_{tot}) / ((11/6) \cdot C_{air,z} + HA_{oc} + HA_{mx} + HA_{fl} + MCP_{tot})
-$$</div>
-
-<div>$${T_{mx}} = {T_{avg}}$$</div>
-
-<div>$${T_{oc}} = {T_{avg}}$$</div>
-
-<div>$${T_{fl}} = {T_{avg}}$$</div>
-
-2.    Call *HcUCSDDV* to calculate the *h<sub>c</sub>*’s.
-
-3.    Repeat step 1
-
-#### Final calculations
-
-The displacement ventilation calculation finishes by calculating some report variables. Using equation , setting the boundary height to 1.5 meters and solving for the flow, we calculate a minimum flow fraction:
-
-<div>$${\dot V_{\min }} = {(1.5/{\rm{24}}{\rm{.55)}}^{{\rm{5/3}}}} \cdot {N_{plumes}} \cdot \dot Q_{perplume}^{1/3}$$</div>
-
-<div>$$F{r_{\min flow}} = .000833 \cdot MC{P_{tot}}/{\dot V_{\min }}$$</div>
-
-We define heights:
-
-<div>$${H_{trans}} = F{r_{hb}} \cdot {H_{ceil}}$$</div>
-
-<div>$${H_{mxavg}} = ({H_{ceil}} + {H_{trans}})/2$$</div>
-
-<div>$${H_{ocavg}} = ({H_{fltop}} + {H_{trans}})/2$$</div>
-
-<div>$${H_{flavg}} = {H_{fltop}}/2$$</div>
-
-Using the user defined comfort height we calculate the comfort  temperature.
-
-If mixing:
-
-<div>$${T_{comf}} = {T_{avg}}$$</div>
-
-If displacement ventilation:
-
-If *H<sub>comf</sub>* &lt; *H<sub>flavg</sub>*
-
-<div>$${T_{comf}} = {T_{fl}}$$</div>
-
-Else if <span>\({H_{comf}} \ge {H_{flavg}}\)</span> and <span>\({H_{comf}} &lt; {H_{ocavg}}\)</span>
-
-<div>$${T_{comf}} = ({T_{fl}}({H_{ocavg}} - {H_{comf}}) + {T_{mx}}({H_{comf}} - {H_{flavg}})/({H_{ocavg}} - {H_{flavg}})$$</div>
-
-Else if <span>\({H_{comf}} \ge {H_{ocavg}}\)</span> and <span>\({H_{comf}} &lt; {H_{mxavg}}\)</span>
-
-<div>$${T_{comf}} = ({T_{oc}}({H_{mxavg}} - {H_{comf}}) + {T_{mx}}({H_{comf}} - {H_{ocavg}})/({H_{mxavg}} - {H_{ocavg}})$$</div>
-
-Else if <span>\({H_{comf}} \ge {H_{mxavg}}\)</span> and <span>\({H_{comf}} &lt; {H_{ceil}}\)</span>
-
-<div>$${T_{comf}} = {T_{mx}}$$</div>
-
-Using the user defined thermostat height we calculate the temperature at the thermostat.
-
-If mixing:
-
-<div>$${T_{stat}} = {T_{avg}}$$</div>
-
-If displacement ventilation:
-
-If *H<sub>stat</sub>* &lt; *H<sub>flavg</sub>*
-
-<div>$${T_{stat}} = {T_{fl}}$$</div>
-
-Else if <span>\({H_{stat}} \ge {H_{flavg}}\)</span> and <span>\({H_{stat}} &lt; {H_{ocavg}}\)</span>
-
-<div>$${T_{stat}} = ({T_{fl}}({H_{ocavg}} - {H_{stat}}) + {T_{mx}}({H_{stat}} - {H_{flavg}})/({H_{ocavg}} - {H_{flavg}})$$</div>
-
-Else if <span>\({H_{stat}} \ge {H_{ocavg}}\)</span> and <span>\({H_{stat}} &lt; {H_{mxavg}}\)</span>
-
-<div>$${T_{stat}} = ({T_{oc}}({H_{mxavg}} - {H_{stat}}) + {T_{mx}}({H_{stat}} - {H_{ocavg}})/({H_{mxavg}} - {H_{ocavg}})$$</div>
-
-Else if <span>\({H_{stat}} \ge {H_{mxavg}}\)</span> and <span>\({H_{stat}} &lt; {H_{ceil}}\)</span>
-
-<div>$${T_{stat}} = {T_{mx}}$$</div>
-
-The average temperature gradient is:
-
-If <span>\({H_{mxavg}} - {H_{flavg}} > 0.1\)</span>
-
-<div>$$Grad{T_{avg}} = ({T_{mx}} - {T_{fl}})/({H_{mxavg}} - {H_{flavg}})$$</div>
-
-else <div>$$Grad{T_{avg}} =  - 9.999$$</div>
-
-The maximum temperature gradient is:
-
-If  <span>\({H_{ocavg}} - {H_{flavg}} > 0.1\)</span>
-
-<div>$$Grad{T_{\max ,1}} = ({T_{oc}} - {T_{fl}})/({H_{ocavg}} - {H_{flavg}})$$</div>
-
-else <span>\(Grad{T_{\max ,1}} =  - 9.999\)</span>
-
-If  <span>\({H_{mxavg}} - {H_{ocavg}} > 0.1\)</span>
-
-<div>$$Grad{T_{\max ,2}} = ({T_{mx}} - {T_{oc}})/({H_{mxavg}} - {H_{ocavg}})$$</div>
-
-else <span>\(Grad{T_{\max ,2}} =  - 9.999\)</span>
- and
-
-<div>$$Grad{T_{\max }} = \max (Grad{T_{\max ,1}},Grad{T_{\max ,2}})$$</div>
-
-For reporting purposes, if the zone is deemed to be mixed, the displacement ventilation report variables are set to flag values.
-
-If <span>\({T_{mx}} &lt; {T_{oc}}\)</span> or <span>\(MC{P_{tot}} \le 0\)</span> or <span>\({H_{fr}} \cdot {H_{ceil}} &lt; {H_{fl,top}} + \Delta {z_{occ,\min }}\)</span> or <span>\({T_{mx}} - {T_{oc}} &lt; \Delta {T_{Crit{\mathop{\rm Re}\nolimits} p}}\)</span>
-
-<div>$$Grad{T_{avg}} =  - 9.999$$</div>
-
-<div>$$Grad{T_{\max }} =  - 9.999$$</div>
-
-<div>$$F{R_{\min ,flow}} =  - 1.0$$</div>
-
-<div>$${H_{trans}} =  - 9.999$$</div>
-
-Finally, the zone node temperature is set to *T<sub>mx</sub>*.
-
-#### References
-
-Carrilho da Graca, G. 2003. Simplified models for heat transfer in rooms. Ph. D. Thesis, University of California, San Diego.
-
-Chen, Q., and B. Griffith. 2002. Incorporating Nodal Room Air Models into Building Energy Calculation Procedures. ASHRAE RP-1222 Final Report.
-
-Cooper, P. and P.F. Linden. 1996. Natural ventilation of an enclosure containing two buoyancy sources. Journal of Fluid Mechanics, Vol. 311, pp. 153-176.
-
-Dominique, M. and P. Guitton. 1997.  Validation of displacement ventilation simplified models. Proc. of Building Simulation.
-
-Holford, J.M., G.R. Hunt and P.F. Linden. 2002. Competition between heat sources in a ventilated space. Proceedings of RoomVent 2002, pp. 577-580.
-
-Hunt, G.R., J.M. Holford and P.F. Linden. 2002. Characterization of the flow driven by a finite area heat source in a ventilated enclosure. Proceedings of RoomVent 2002, pp.  581-584.
-
-Hunt, G.R. and P.F. Linden.  2001. Steady-state flows in an enclosure ventilated by buoyancy forces assisted by wind. . Journal of Fluid Mechanics, Vol. 426,  pp. 355-386.
-
-Kaye, K.N. and P.F. Linden.  2004. Coalescing axisymmetric turbulent plumes*.* Journal of Fluid Mechanics,  Vol. 502, pp. 41--63.
-
-Linden, P.F., G.F. Lane-Serff and D.A. Smeed. 1990. Emptying filling boxes: the fluid mechanics of natural ventilation. Journal of Fluid Mechanics, Vol. 212, pp. 309-335.
-
-Linden, P.F. and P. Cooper. 1996. Multiple sources of buoyancy in a naturally ventilated enclosure. Journal of Fluid Mechanics, Vol. 311, pp. 177-192.
-
-Morton, B.R., G.I. Taylor andJ.S. Turner. 1956. Turbulent gravitational convection from maintained and instantaneous sources. Proceedings of the Royal Society of London, Vol A234, pp. 1-23.
-
-Mundt, E. 1996. The Performance of Displacement Ventilation Systems – Experimental and Theoretical Studies, Ph. D. Thesis, Bulletin N38, Building Services Engineering KTH, Stockholm.
-
-Rees, S.J., and P. Haves. 2001. A nodal model for displacement ventilation and chilled ceiling systems in office spaces. Building and Environment, Vol. 26, pp. 753-762.
-
-### Under-Floor Air Distribution Interior Zone Model
-
-#### Overview
-
-The input object RoomAirSettings:UnderFloorAirDistributionInterior provides a simple model for heat transfer and nonuniform vertical temperature profile for interior zones of a UFAD system. These zones are expected to be dominated by internal loads, a portion of which (such as occupants and workstations) will act to generate plumes. The plumes act to potentially create room air stratification, depending on the type & number of diffusers, the amount and type of load, and the system flowrate. In order to better model this situation the fully-mixed room air approximation that is currently used in most whole building analysis tools is extended to a two node approach, with the purpose of obtaining a first order precision model for vertical temperature profiles for the interior zones of UFAD systems. The use of 2 nodes allows for greatly improved prediction of thermal comfort and overall building energy performance for the increasingly popular UFAD systems.
-
-TheUCSD UFAD Interior Zone Model is one of the non-uniform zone models provided through the Room Air Manager in EnergyPlus. The intent is to provide a selection of useful non-uniform zone air models to enable the evaluation of air-conditioning techniques that use stratified or partially stratified room air. Such techniques include displacement ventilation (DV) and underfloor air distribution (UFAD) systems. The methodology can also include natural displacement ventilation and also wind-driven cross-ventilation (CV).
-
-#### Underfloor air distribution systems
-
-UFAD systems represent, in terms of room air stratification, an intermediate condition between a well-mixed zone and displacement ventilation. Air is supplied through an underfloor plenum at low pressure through diffusers in the raised floor. The diffusers can be of various types: e.g., swirl, variable-area, displacement, and produce more or less mixing in the zone. UFAD systems are promoted as saving energy due to: higher supply air temperature; low static pressure; cooler conditions in the occupied subzone than in the upper subzone; and sweeping of some portion of the convective load (from ceiling lights, for instance) into the return air without interaction with the occupied region of the zone.
-
-Modeling a UFAD system is quite complex and involves considerably more than just a non-uniform zone model. The zones’ coupling to the supply and return plenums must be modeled accurately (particularly radiative transfer from a warm ceiling to a cool floor and on into the supply plenum by conduction). The supply plenum must be accurately modeled, giving a good estimate of the supply air temperature and conduction heat transfer between supply & return plenums through the slab. The HVAC system must be modeled including return air bypass and various types of fan powered terminal units.
-
-The UCSD UFAD interior zone model is similar to the UCSD DV model. The most obvious difference is that the UFAD model has no separate near-floor subzone. Like the UCSD DV model it is a plume equation based multi-layer model (2 layers in this case). The zone is modeled as being divided into 2 well separated subzones which we denote as “occupied� and “upper�. Each subzone is treated as having a single temperature. The boundary between the 2 subzones moves up & down each time step as a function of zone loads and supply air flow rate. Thus at each HVAC time step, the height of the boundary above the floor must be calculated, portions of surfaces assigned to each subzone, and a separate convective heat balance performed on each subzone.
-
-#### Model Description
-
-The UFAD interior zone model is based upon non-dimensional analysis of the system and using the non-dimensional description to make a comparison between full-scale UCB test chamber data & small-scale UCSD salt tank measurements.
-
-In order to do the non-dimensional comparisons, we need to define two dimensionless parameters. One is <span>\(\Gamma \)</span>, and the other is <span>\(\phi \)</span>. Lin & Linden (Lin & Linden, 2005) showed that in a UFAD system, the buoyancy flux of the heat source <span>\((B)\)</span>and the momentum flux of the cooling jets <span>\((M)\)</span>are the controlling parameters on the stratification. Since <span>\([B] = {L^4}{T^{ - 3}}\)</span>and<span>\([M] = {L^4}{T^{ - 2}}\)</span>, we can have a length scale as <span>\({M^{3/4}}/{B^{1/2}}\)</span>.
-
-*Definition of* *Gfor the single-plume single-diffuser basic model*
-
-We observed, in our small-scale experiments, that the total room height does not affect the interface position, or the height of the occupied zone. In other words, *H* might not be the critical length scale for the stratification. Therefore, we started to use <span>\(\sqrt A \)</span> as the reference length. Then <span>\(\Gamma \)</span>is defined as
-
-<div>$$\Gamma  = \frac{{{M^{3/4}}}}{{{B^{1/2}}{A^{1/2}}}} = \frac{{{{({Q^2}/A)}^{3/4}}}}{{{B^{1/2}}{A^{1/2}}}} = \frac{{{Q^{3/2}}}}{{{A^{5/4}}{B^{1/2}}}}$$</div>
-
-*Definition for multi-diffuser and multi-source cases*
-
-We only considered single-diffuser, single-source cases in above analysis. Suppose there are *n* equal diffusers and *m* equal heat sources in a UFAD room. We shall divide the number of diffusers up into a number of separate heat sources so that each subsection with *n’=n/m* diffusers per heat source will have the same stratification as other subsections. Further, the air flow and the heat load into the subsection *Q’* and *B’* will be<span>\(Q' = Q/m\)</span><span>\(B' = B/m\)</span>respectively, where *Q’* and *B’* are the total air flow and the total heat load for the entire UFAD space. Then the momentum flux each diffuser per heat source carries is<span>\({M_d} = {(\frac{1}{{n'}}Q')^2}/A\)</span>. will be modified as
-
-<div>$$\Gamma  = \frac{{{{(n'{M_d})}^{3/4}}}}{{B{'^{1/2}}\sqrt {n'A} }} = \frac{{Q{'^{3/2}}}}{{{{(n'A)}^{5/4}}B{'^{1/2}}}} = \frac{{{Q^{3/2}}}}{{m{{(n'A)}^{5/4}}{B^{1/2}}}}$$</div>
-
-*Full-scale cases*
-
-Because *B* is the buoyancy flux of the heat sources and *M* is the momentum flux of the cooling jets, in a real full-scale room, we shall consider the total room net heat load (plume heat input, minus the room losses) and the total net flow rate coming from the diffusers (input room air flow, minus the room leakage). Further, if the diffuser is swirl type, the vertical momentum flux should be used.
-
-<div>$$\Gamma  = \frac{{{{(Q\cos \theta )}^{3/2}}}}{{m{{(n'A)}^{5/4}}{{(0.0281W)}^{1/2}}}}$$</div>
-
-where, *Q* is the net flow rate coming out from all diffusers (m<sup>3</sup>/s); *W* is the total net heat load (kW); *A* is the effective area of each diffuser (m<sup>2</sup>); *n’* is the number of diffusers per heat source; *q* is the angle between the diffuser slots and the vertical direction and *m* is the number of heat sources
-
-*Definition of* *F*
-
-In our theoretical model, two-layer stratification forms at steady state, provided that each diffuser carries the same momentum flux, and each heat source has the same heat load. We could define a dimensionless parameter *F*, which indicates the strength of stratification.
-
-*Small-scale cases*
-
-In our salt-water tank experiments, fluid density *r* is measured. Define that
-
-<div>$$\phi  = \frac{{{\rho_u} - {\rho_l}}}{{{\rho_u} - {\rho_o}}}$$</div>
-
-where, *r<sub>u</sub>* and *r<sub>l</sub>* are the fluid density of the upper layer and lower layer, separately; and *r<sub>o</sub>* is the source density at the diffusers.
-
-Therefore, *r<sub>l</sub>* =*r<sub>o</sub>* gives *f*=*1*, which means the largest stratification (displacement ventilation case); *r<sub>l</sub>* =*r<sub>u</sub>* leads to *f*=*0*, in which case there is no stratification (mixed ventilation case).
-
-*Full-scale cases*
-
-Similarly, we can define *f* for full-scale cases by using temperature.
-
-<div>$$\phi  = \frac{{{T_r} - {T_{oz}}}}{{{T_r} - {T_s}}}$$</div>
-
-where *T<sub>r</sub>*, *T<sub>oz</sub>*, and *T<sub>s</sub>* are the return air temperature, the occupied zone temperature and the supply temperature, respectively (K). Again *f=1* occurs in displacement ventilation; while *f=0* happens in mixed ventilation.
-
-*Comparisons between full-scale UCB data and small-scale UCSD data*
-
-![](media/image2469.png)
-
-Figure 133. Data comparisons in the non-dimensional (a) regular G-fplot
-
-![](media/image2470.png)
-
-Figure 134. (b) log-log G-fplot.}
-
-The figures (Figure 133. Data comparisons in the non-dimensional (a) regular G-fplot and Figure 134. (b) log-log G-fplot.} show the comparisons between UCB's data and the UCSD salt tank data in the *G-f* plot. As seen in the figures, the full-scale and small-scale data are on the same trend curve. This provides the evidence that the salt-tank experiments have included most characteristics of a UFAD system. Note that big *G* (&gt;20) of UCB's experiments all have large DDR (from *1.19* to *2.18*). The largest DDR (*2.18*) even gives a negative<span>\(({T_r} - {T_{oz}})/({T_r} - {T_s})\)</span>, which is NOT shown in the figures.)
-
-We could work out the occupied zone temperature by using the least-square fitting line suggested in figure 1(b). Hence the interface height is needed to determine a entire two-layer stratification. Figure 135 shows the dimensionless interface height<span>\((h/\sqrt {n'A} )\)</span>of the UCSD small-scale experiments plotted against *G*. Note that for the experiments with elevated heat source, the interface heights have been modified by<span>\(h' = h - \frac{1}{2}{h_s}\)</span> where *h<sub>s</sub>* is the vertical position of the elevated heat source. All data then are located along a line in Figure 135. Since the salt-tank experiments are concluded to represent important characteristics of a full-scale UFAD room, this figure provides some guidelines for estimate the interface position in a real UFAD room.
-
-![](media/image2474.png)
-
-Figure 135. Non-dimensional interface height of small-scale experiments.
-
-*Formulas for EnergyPlus based on the dimensionless parameter* *G*
-
-If we have input including the supply temperature *T<sub>s</sub>* (K); the number of diffusers *n*; the number of heat sources *m*; the vertical position of the heat sources *h<sub>s</sub>* (m); the heat load *W* (kW); the effective area of a diffuser *A* (m<sup>2</sup>); and the total supply air flow rate *Q* (m<sup>3</sup>/s) then the output will be
-
-<div>$${T_r} = \frac{{0.0281W}}{{Qg}}{T_s} + {T_s}$$</div>
-
-<div>$${T_{oz}} = {T_r} - 1.6{\Gamma ^{ - 0.76}}({T_r} - {T_s})$$</div>
-
-<div>$$h = \sqrt {\frac{n}{m}A} (7.43ln(\Gamma ) - 1.35) + \frac{1}{2}{h_s}$$</div>
-
-where *T<sub>r</sub>* is the return temperature (K); *T<sub>oz</sub>* is the occupied subzone temperature (K); *h* is the interface height (m); and *G* is defined above.
-
-#### Implementation
-
-The implementation closely follows the procedure described in the displacement ventilation zone model. The model predicts two temperatures that characterize the two main levels in the stratification of the room:
-
-1.    an occupied subzone temperature T<sub>oc</sub> representing the temperature of the occupied region;
-
-2.    an upper level temperature T<sub>mx</sub> representing the temperature of the upper, mixed region and the outflow temperature.
-
-
-
-We will use to calculate the interface height and do a heat balance calculation on each subzone. *G* is given by . The supply air flow rate <span>\(\dot V\)</span> is obtained by summing all the air flows entering the zone: supply air, infiltration, ventilation, and inter-zone flow. The heat gain <span>\(\dot Q\)</span> is estimated by summing all the convective internal gains located in the occupied subzone – task lights, people, equipment – and dividing this power equally among the n plumes. With these assumptions we can describe the implementation.
-
-The UCSD UFI model is controlled by the subroutine *ManageUCSDUFModels* which is called from the *RoomAirModelManager*. The *RoomAirModelManager* selects which zone model will be used for each zone.
-
-The calculation is done in subroutine *CalcUCSDUI*. First we calculate the convective heat gain going into the upper and lower regions.
-
-<div>$$
-  \dot Q_{ocz} = \dot Q_{oc,conv} + \dot Q_{tl,conv} + \dot Q_{eleq,conv} + \dot Q_{gaseq,conv} + \dot Q_{otheq,conv} + \dot Q_{hw,conv} + \dot Q_{stmeq,conv} + \dot Q_{bb,conv} + \dot Q_{waterheater,conv} + \dot Q_{fuelcell,conv}
-$$</div>
-
-<div>$${\dot Q_{mxz}} = {\dot Q_{gl,conv}} + {\dot Q_{ltp}} + {\dot Q_{htrad,conv}}$$</div>
-
-<div>$${\dot Q_{tot,conv}} = {\dot Q_{ocz}} + {\dot Q_{mxz}}$$</div>
-
-Next we sum up the inlet air flows in the form of MCP (mass flow rate times the air specific heat capacity) and MCPT (mass flow rate times C<sub>p</sub> times air temperature).
-
-<div>$$MC{P_{zone}} = MC{P_i} + MC{P_{vent}} + MC{P_{mix}}$$</div>
-
-<div>$$MC{P_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}$$</div>
-
-<div>$${\dot m_{systot}} = \sum\limits_{inlets} {{{\dot m}_i}} $$</div>
-
-<div>$$MC{P_{tot}} = MC{P_{zone}} + MC{P_{sys}}$$</div>
-
-<div>$$MCP{T_{zone}} = MCP{T_i} + MCP{T_{vent}} + MCP{T_{mix}}$$</div>
-
-<div>$$MCP{T_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}{T_i}$$</div>
-
-<div>$$MCP{T_{tot}} = MCP{T_{zone}} + MCP{T_{sys}}$$</div>
-
-The number of plumes per occupant <span>\({N_{plumesperpers}}\)</span> is a user input. The total number of plumes in the zone is:
-
-<div>$${N_{plumes}} = {N_{occ}} \cdot {N_{plumesperperson}}$$</div>
-
-Using this we calculate the total power in the plumes and the power per plume.
-
-<div>$${\dot Q_{plumes}} = {\dot Q_{ocz}}$$</div>
-
-<div>$${\dot Q_{perplume}} = {\dot Q_{plumes}}/{N_{plumes}}$$</div>
-
-The number of diffusers per plumes is also a user input. To obtain the number of diffusers in the zone:
-
-<div>$${N_{diffusers}} = {N_{plumes}}\cdot {N_{diffusersperplume}}$$</div>
-
-The area *A<sub>diff</sub>* is also a user input. For swirl diffusers and for displacement diffusers this area is used as input. For the variable area diffusers, though, we calculate the area. We assume 400 ft/min velocity at the diffuser and a design flow rate per diffuser is 150 cfm (.0708 m<sup>3</sup>/s). The design area of the diffuser is 150 ft<sup>3</sup>/min /  400 ft/min = .575 ft<sup>2</sup> = .035 m<sup>2</sup>. Then the variable area each time step is
-
-<div>$${A_{diff}} = {\dot m_{systot}}/(.0708\cdot {N_{diffusers}})$$</div>
-
-We now calculate the height fraction *Fr<sub>hb</sub>* (height of boundary layer divided by the total zone height).
-
-<div>$$\Gamma  = \frac{{{{({{\dot m}_{systot}}\cdot \cos ({\theta_{throw}}))}^{3/2}}}}{{{N_{plumes}}{{({N_{diffusersperplume}}\cdot {A_{diff}})}^{5/4}}{{(0.0281\cdot 0.001\cdot {{\dot Q}_{plumes}})}^{1/2}}}}$$</div>
-
-<div>$$F{r_{hb}} = \frac{{{{({N_{diffusersperplume}}\cdot {A_{diff}})}^{1/2}}(7.43\ln (\Gamma ) - 1.35 + 0.5{H_s})}}{{{H_{ceil}}}}$$</div>
-
-where *q<sub>throw</sub>* is a user input: the angle between the diffuser slots and vertical; and *H<sub>s</sub>* is the source height above the floor (m).
-
-Next we iterate over the following 2 steps.
-
-#### Iterative procedure
-
-1.    Call subroutine *HcUCSDUF* to calculate a convective heat transfer coefficient for each surface in the zone, an effective air temperature for each surface, and HA<sub>mx</sub>, HAT<sub>mx</sub>, HA<sub>oc</sub>, HAT<sub>oc</sub>. Here HA is <span>\(\sum\limits_{surfaces} {{h_{c,i}} \cdot {A_i}} \)</span> for a region and HAT is <span>\(\sum\limits_{surfaces} {{h_{c,i}} \cdot {A_i}}  \cdot {T_i}\)</span> for a region. The sum is over all the surfaces bounding the region; <span>\({{h_{c,i}}}\)</span> is the convective heat transfer coefficient for surface i, <span>\({A_i}\)</span> is the area of surface i,  and <span>\({T_i}\)</span> is the surface temperature of surface i.
-
-2.    Calculate the two subzone temperatures: *T<sub>oc</sub>* and *T<sub>mx</sub>*.
-
-The h<sub>c</sub>’s calculated in step 1 depend on the subzone temperatures. In turn the subzone temperatures depend on the HA and HAT’s calculated in step 1. Hence the need for iteration
-
-Next we describe each steps 1 and 2 in more detail.
-
-#### Step 1
-
-Subroutine *HcUCSDUF* is quite straightforward. It loops through all the surfaces in each zone and decides whether the surface is located in the upper, mixed subzone or the lower, occupied subzone, or if the surface is in both subzones. If entirely in one subzone the subzone temperature is stored in the surface effective temperature variable *TempEffBulkAir(SurfNum)* and h<sub>c</sub> for the surface is calculated by a call to subroutine *CalcDetailedHcInForDVModel*. This routine uses the “detailed� natural convection coefficient calculation that depends on surface tilt and <span>\(\Delta {T^{1/3}}\)</span>. This calculation is appropriate for situations with low air velocity.
-
-For surfaces that bound 2 subzones, the subroutine calculates h<sub>c</sub> for each subzone and then averages them, weighting by the amount of surface in each subzone.
-
-During the surface loop, once the h<sub>c</sub> for a surface is calculated, the appropriate subzone HA and HAT sums are incremented. If a surface is in 2 subzones the HA and HAT for each subzone are incremented based on the area of the surface in each subzone.
-
-#### Step 2
-
-The calculation of  subzone temperatures follows the method used in the ***ZoneTempPredictorCorrector*** module and described in the section **Basis for the System and Zone Integration**. Namely a third order finite difference expansion of the temperature time derivative is used in updating the subzone temperatures. Otherwise the subzone temperatures are obtained straightforwardly by solving an energy balance equation for each subzone.
-
-<div>$$
-  \begin{array}{cl}
-    T_{oc} &= (C_{air,oc} \cdot (3 \cdot T_{ - 1,oc} - (3/2) \cdot T_{ - 2,oc} + (1/3) \cdot T_{ - 3,oc}) + \dot Q_{ocz} \cdot Fr_{gains} + HAT_{oc} + MCPT_{tot}) / ((11/6) \cdot C_{air,oc} + HA_{oc} + MCP_{tot}) \\
-    T_{mx} &= (C_{air,mx} \cdot (3 \cdot T_{ - 1,mx} - (3/2) \cdot T_{ - 2,mx} + (1/3) \cdot T_{ - 3,mx}) + \dot Q_{ocz} \cdot (1 - Fr_{gains}) + \dot Q_{mxz} + HAT_{mx} + T_{oc} \cdot MCP_{tot}) / ((11/6) \cdot C_{air,mx} + HA_{mx} + MCP_{tot})
-  \end{array}
-$$</div>
-
-Here <span>\({C_{air,oc}}\)</span> and <span>\({C_{air,mx}}\)</span> are the heat capacities of the air volume in each subzone. <span>\({C_{air,mx}}\)</span> is calculated by
-
-<div>$${R_{air,mx}} = {V_{mx}} \cdot \left( {\Delta {z_{mx}}/{z_{ceil}}} \right) \cdot {\rho_{air,mx}} \cdot {c_{p,air,mx}} \cdot Mu{l_{cap}}/\left( {\Delta {t_z} \cdot 3600} \right)$$</div>
-
-<div>$${c_{air,mx}} = {R_{air,mx}} \cdot \Delta {t_z}/\Delta {t_{sys}}$$</div>
-
-The gains fraction <span>\(F{r_{gains}}\)</span>is a user input via a schedule. It is the fraction of the convective gains in the occupied subzone that remain in that subzone.
-
-The other subzone air heat capacities are calculated in the same manner.
-
-#### Mixed calculation
-
-The above iterative procedure assumed that the UFAD nonuniform zone model was appropriate: i.e., conditions were favorable temperature stratification in the zone. Now that this calculation is complete and the subzone temperatures and depths calculated, we check to see if this assumption was justified. If not, zone conditions must be recalculated assuming a well-mixed zone.
-
-If <span>\({T_{mx}} &lt; {T_{oc}}\)</span> or <span>\(MC{P_{tot}} \le 0\)</span> or <span>\({H_{fr}} \cdot {H_{ceil}} &lt; \Delta {z_{occ,\min }}\)</span> then the following mixed calculation will replace the UFAD interior zone calculation.
-
-**Note:**  <span>\(\Delta {z_{occ,min}}\)</span> is the minimum thickness of occupied subzone. It is set to 0.2 meters.
-
-The mixed calculation iteratively calculates surface convection coefficients and room temperature just like the displacement ventilation calculation described above. In the mixed case however, only one zone temperature *T<sub>avg</sub>* is calculated. The 3 subzone temperatures are then set equal to *T<sub>avg</sub>*.
-
-First, *Fr<sub>hb</sub>*  is set equal to zero.
-
-Then the code iterates over these steps.
-
-Calculate *T<sub>avg</sub>* using
-
-<div>$$\begin{array}{l}{T_{avg}} = ({C_{air,z}} \cdot (3 \cdot {T_{ - 1,z}} - (3/2) \cdot {T_{ - 2,z}} + (1/3) \cdot {T_{ - 3,z}}) + \\\quad \quad {{\dot Q}_{tot,conv}} + HA{T_{oc}} + HA{T_{mx}}MCP{T_{tot}})/((11/6) \cdot {C_{air,z}} + H{A_{oc}} + H{A_{mx}} + MC{P_{tot}})\end{array}$$</div>
-
-<div>$${T_{mx}} = {T_{avg}}$$</div>
-
-<div>$${T_{oc}} = {T_{avg}}$$</div>
-
-Call *HcUCSDUF* to calculate the *h<sub>c</sub>*’s.
-
-Repeat step 1
-
-#### Final calculations
-
-The UFAD interior zone calculation finishes by calculating some report variables.
-
-We define heights:
-
-<div>$${H_{trans}} = F{r_{hb}} \cdot {H_{ceil}}$$</div>
-
-<div>$${H_{mxavg}} = \left( {{H_{ceil}} + {H_{trans}}} \right)/2$$</div>
-
-<div>$${H_{ocavg}} = {H_{trans}}/2$$</div>
-
-Using the user defined comfort height we calculate the comfort  temperature.
-
-If mixing:
-
-<div>$${T_{comf}} = {T_{avg}}$$</div>
-
-If UFAD:
-
-If  <span>\({H_{comf}} &lt; {H_{ocavg}}\)</span>
-
-<div>$${T_{comf}} = {T_{occ}}$$</div>
-
-Else if <span>\({H_{comf}} \ge {H_{ocavg}}\)</span> and <span>\({H_{comf}} &lt; {H_{mxavg}}\)</span>
-
-<div>$${T_{comf}} = \left( {{T_{oc}}\left( {{H_{mxavg}} - {H_{comf}}} \right) + {T_{mx}}\left( {{H_{comf}} - {H_{ocavg}}} \right)} \right)/\left( {{H_{mxavg}} - {H_{ocavg}}} \right)$$</div>
-
-Else if <span>\({H_{comf}} \ge {H_{mxavg}}\)</span> and <span>\({H_{comf}} &lt; {H_{ceil}}\)</span>
-
-<div>$${T_{comf}} &lt; {T_{mx}}$$</div>
-
-Using the user defined thermostat height we calculate the temperature at the thermostat.
-
-If mixing:
-
-<div>$${T_{stat}} &lt; {T_{avg}}$$</div>
-
-If UFAD:
-
-If<span>\({H_{stat}} &lt; {H_{ocavg}}\)</span>
-
-<div>$${T_{stat}} = {T_{occ}}$$</div>
-
-Else if <span>\({H_{stat}} \ge {H_{ocavg}}\)</span> and <span>\({H_{stat}} &lt; {H_{mxavg}}\)</span>
-
-<div>$${T_{stat}} = \left( {{T_{oc}}\left( {{H_{mxavg}} - {H_{stat}}} \right) + {T_{mx}}\left( {{H_{stat}} - {H_{ocavg}}} \right)} \right)/\left( {{H_{mxavg}} - {H_{ocavg}}} \right)$$</div>
-
-Else if <span>\({H_{stat}} \ge {H_{mxavg}}\)</span> and <span>\({H_{stat}} &lt; {H_{ceil}}\)</span>
-
-<div>$${T_{stat}} = {T_{mx}}$$</div>
-
-The average temperature gradient is:
-
-If <span>\({H_{mxavg}} - {H_{occavg}} > 0.1\)</span>
-
-<div>$$Grad{T_{avg}} = ({T_{mx}} - {T_{occ}})/({H_{mxavg}} - {H_{occavg}})$$</div>
-
-else <span>\(Grad{T_{avg}} = 0.0\)</span>
-
-Finally, the zone node temperature is set to *T<sub>mx</sub>*.
-
-Other variables that are reported out are <span>\(\Gamma \)</span>and <span>\(\phi \)</span>.
-
-<div>$$\phi  = ({T_{mx}} - {T_{occ}})/({T_{mx}} - {T_{sup}})$$</div>
-
-where <span>\({T_{sup}}\)</span>is the zone supply air temperature.
-
-#### References
-
-Lin, Y.J. and P.F. Linden. 2005. A model for an under floor air distribution system. Energy&Building, Vol. 37, pp. 399-409.
-
-### Under-Floor Air Distribution Exterior Zone Model
-
-#### Overview
-
-The input object RoomAirSettings:UnderFloorAirDistributionExterior provides a simple model for heat transfer and a nonuniform vertical temperature profile for exterior zones of a UFAD system. These zones are expected to be dominated by internal loads, a portion of which (such as occupants and workstations) will act to generate plumes, and by window solar and conduction heat gains. The solar radiation penetrating the room is not expected to generate plumes. However, a window plume is likely to be generated in sunny conditions, particularly if an interior blind is deployed. Thus the exterior UFAD zone will have potentially have plumes from people and equipment and plumes arising from the windows. The plumes act to potentially create room air stratification, depending on the type & number of diffusers, the amount and type of load, and the system flowrate. In order to better model this situation the fully-mixed room air approximation that is currently used in most whole building analysis tools is extended to a two node approach, with the purpose of obtaining a first order precision model for vertical temperature profiles for the exterior zones of UFAD systems. The use of 2 nodes allows for greatly improved prediction of thermal comfort and overall building energy performance for the increasingly popular UFAD systems.
-
-TheUCSD UFAD Exterior Zone Model is one of the non-uniform zone models provided through the Room Air Manager in EnergyPlus. The intent is to provide a selection of useful non-uniform zone air models to enable the evaluation of air-conditioning techniques that use stratified or partially stratified room air. Such techniques include displacement ventilation (DV) and underfloor air distribution (UFAD) systems. The methodology can also include natural displacement ventilation and also wind-driven cross-ventilation (CV).
-
-#### Underfloor air distribution systems
-
-UFAD systems represent, in terms of room air stratification, an intermediate condition between a well-mixed zone and displacement ventilation. Air is supplied through an underfloor plenum at low pressure through diffusers in the raised floor. The diffusers can be of various types: e.g., swirl, variable-area, displacement, and produce more or less mixing in the zone. UFAD systems are promoted as saving energy due to: higher supply air temperature; low static pressure; cooler conditions in the occupied subzone than in the upper subzone; and sweeping of some portion of the convective load (from ceiling lights, for instance) into the return air without interaction with the occupied region of the zone.
-
-Modeling a UFAD system is quite complex and involves considerably more than just a non-uniform zone model. The zones’ coupling to the supply and return plenums must be modeled accurately (particularly radiative transfer from a warm ceiling to a cool floor and on into the supply plenum by conduction). The supply plenum must be accurately modeled, giving a good estimate of the supply air temperature and conduction heat transfer between supply & return plenums through the slab. The HVAC system must be modeled including return air bypass and various types of fan powered terminal units.
-
-The UCSD UFAD exterior zone model is similar to the UCSD interior zone model. The most obvious difference is that the exterior UFAD has 2 different types of plume sources: people & equipment and windows. Like the UCSD UFAD interior model it is a plume equation based multi-layer model (2 layers in this case). The zone is modeled as being divided into 2 well separated subzones which we denote as “occupied� and “upper�. Each subzone is treated as having a single temperature. The boundary between the 2 subzones moves up & down each time step as a function of zone loads and supply air flow rate. Thus at each HVAC time step, the height of the boundary above the floor must be calculated, portions of surfaces assigned to each subzone, and a separate convective heat balance performed on each subzone.
-
-#### Model Description
-
-As in the interior zone case, we define 2 dimensionless parameters: <span>\(\Gamma \)</span>and <span>\(\phi \)</span>. The definitions of the 2 parameters are the same as in the previous section (equations , , , , and ). As in the previous case, the experimental data can be plotted versus <span>\(\Gamma \)</span>and lines fitted to the data give the following formulas for occupied subzone temperature and interface height.
-
-<div>$${T_{oz}} = {T_r} - 1.4{\Gamma ^{ - 0.6}}({T_r} - {T_s})$$</div>
-
-<div>$$h = \sqrt {\frac{n}{m}A} (11.03ln(\Gamma ) - 10.73) + \frac{1}{2}{h_s}$$</div>
-
-where *T<sub>oz</sub>* is the occupied subzone temperature (K); *T<sub>r</sub>* is the return temperature (K); *G* is the dimensionless height parameter defined above; *T<sub>s</sub>* is the supply temperature (K); *h* is the interface height (m); *n* is the number of diffusers; *m* is the number of heat sources; *A* is the effective area of a diffuser (m<sup>2</sup>); and *h<sub>s</sub>* is the vertical position of the heat sources (m). The formula for *T<sub>r</sub>* is the same as in the previous section.
-
-#### Implementation
-
-The implementation closely follows the procedure described in the UFAD interior zone model. The model predicts two temperatures that characterize the two main levels in the stratification of the room:
-
-1.    an occupied subzone temperature T<sub>oc</sub> representing the temperature of the occupied region;
-
-2.    an upper level temperature T<sub>mx</sub> representing the temperature of the upper, mixed region and the outflow temperature.
-
-We will use to calculate the interface height and do a heat balance calculation on each subzone. *G* is given by . The supply air flow rate <span>\(\dot V\)</span> is obtained by summing all the air flows entering the zone: supply air, infiltration, ventilation, and inter-zone flow. The heat gain <span>\(\dot Q\)</span> is estimated by summing all the convective internal gains located in the occupied subzone – task lights, people, equipment – and adding to this the convective gain coming from the window surface. With these assumptions we can describe the implementation.
-
-The UCSD UFE model is controlled by the subroutine *ManageUCSDUFModels* which is called from the *RoomAirModelManager*. The *RoomAirModelManager* selects which zone model will be used for each zone.
-
-The calculation is done in subroutine *CalcUCSDUEI*. First we calculate the convective heat gain going into the upper and lower regions.
-
-<div>$$
-  \dot Q_{ocz} = \dot Q_{oc,conv} + \dot Q_{tl,conv} + \dot Q_{eleq,conv} + \dot Q_{gaseq,conv} + \dot Q_{otheq,conv} + \dot Q_{hw,conv} + \dot Q_{stmeq,conv} + \dot Q_{bb,conv} + \dot Q_{waterheater,conv} + \dot Q_{fuelcell,conv}
-$$</div>
-
-<div>$${\dot Q_{mxz}} = {\dot Q_{gl,conv}} + {\dot Q_{ltp}} + {\dot Q_{htrad,conv}}$$</div>
-
-<div>$${\dot Q_{tot,conv}} = {\dot Q_{ocz}} + {\dot Q_{mxz}}$$</div>
-
-Next we sum up the inlet air flows in the form of MCP (mass flow rate times the air specific heat capacity) and MCPT (mass flow rate times C<sub>p</sub> times air temperature).
-
-<div>$$MC{P_{zone}} = MC{P_i} + MC{P_{vent}} + MC{P_{mix}}$$</div>
-
-<div>$$MC{P_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}$$</div>
-
-<div>$${\dot m_{systot}} = \sum\limits_{inlets} {{{\dot m}_i}} $$</div>
-
-<div>$$MC{P_{tot}} = MC{P_{zone}} + MC{P_{sys}}$$</div>
-
-<div>$$MCP{T_{zone}} = MCP{T_i} + MCP{T_{vent}} + MCP{T_{mix}}$$</div>
-
-<div>$$MCP{T_{sys}} = \sum\limits_{inlets} {{{\dot m}_i}} {C_{p,i}}{T_i}$$</div>
-
-<div>$$MCP{T_{tot}} = MCP{T_{zone}} + MCP{T_{sys}}$$</div>
-
-For exterior zone model, we assume one plume: <span>\({N_{plumes}} = 1\)</span>. The number of diffusers in the zone <span>\({N_{diffusers}}\)</span>is a user input.
-
-The area *A<sub>diff</sub>* is also a user input. For swirl diffusers, linear bar grilles, and displacement diffusers this area is used as input. For the variable area diffusers, though, we calculate the area. We assume 400 ft/min velocity at the diffuser and a design flow rate per diffuser is 150 cfm (.0708 m<sup>3</sup>/s). The design area of the diffuser is 150 ft<sup>3</sup>/min /  400 ft/min = .575 ft<sup>2</sup> = .035 m<sup>2</sup>. Then the variable area each time step is
-
-<div>$${A_{diff}} = {\dot m_{systot}}/(.0708\cdot {N_{diffusers}})$$</div>
-
-We now make an initial estimate of the convective gain from the windows.
-
-<div>$${\dot Q_{win,conv}} = \sum\limits_{i = 1,{n_{win}}} {{h_{c,i}}} {A_{win,i}}{T_{winsurf,i}} - {h_{c,i}}{A_{win,i}}{T_{mat}}$$</div>
-
-Then
-
-<div>$${\dot Q_{plumes}} = {\dot Q_{ocz}} + {\dot Q_{win,conv}}$$</div>
-
-We now calculate the height fraction *Fr<sub>hb</sub>* (height of boundary layer divided by the total zone height).
-
-<div>$$\Gamma  = \frac{{{{({{\dot m}_{systot}}\cdot \cos ({\theta_{throw}}))}^{3/2}}}}{{{{({N_{diffusers}}\cdot {A_{diff}})}^{5/4}}{{(0.0281\cdot 0.001\cdot {{\dot Q}_{plumes}})}^{1/2}}}}$$</div>
-
-<div>$$F{r_{hb}} = \frac{{{{({N_{diffusers}}\cdot {A_{diff}})}^{1/2}}(11.03ln(\Gamma ) - 10.73 + 0.5{H_s})}}{{{H_{ceil}}}}$$</div>
-
-where *q<sub>throw</sub>* is a user input: the angle between the diffuser slots and vertical; and *H<sub>s</sub>* is the source height above the floor (m).
-
-Next we iterate over the following 2 steps.
-
-#### Iterative procedure
-
-1.    Call subroutine *HcUCSDUF* to calculate a convective heat transfer coefficient for each surface in the zone, an effective air temperature for each surface, and HA<sub>mx</sub>, HAT<sub>mx</sub>, HA<sub>oc</sub>, HAT<sub>oc</sub>, HA<sub>mx,win</sub>,HAT<sub>mx,win</sub>,HA<sub>oc,win</sub>,and HAT<sub>oc,win</sub>. Here HA is <span>\(\sum\limits_{surfaces} {{h_{c,i}} \cdot {A_i}} \)</span> for a region and HAT is <span>\(\sum\limits_{surfaces} {{h_{c,i}} \cdot {A_i}}  \cdot {T_i}\)</span> for a region. The sum is over all the surfaces bounding the region; <span>\({h_{c,i}}\)</span> is the convective heat transfer coefficient for surface i, <span>\({A_i}\)</span> is the area of surface i,  and <span>\({T_i}\)</span> is the surface temperature of surface i. Variables with the *win* subscript are summed over window surfaces only. Then the convective gain from the window is recalculated:
-
-                              <span>\({\dot Q_{win,conv}} = HA{T_{mx,win}} + HA{T_{oc,win}} - H{A_{mx,win}}{T_{mx}} - H{A_{oc,win}}{T_{oc}}\)</span>
-
-and the power in the plume is recalculated: <span>\({\dot Q_{plumes}} = {\dot Q_{ocz}} + {\dot Q_{win,conv}}\)</span>.
-
-2.    Calculate the two subzone temperatures: *T<sub>oc</sub>* and *T<sub>mx</sub>*.
-
-The h<sub>c</sub>’s calculated in step 1 depend on the subzone temperatures. In turn the subzone temperatures depend on the HA and HAT’s calculated in step 1. Hence the need for iteration
-
-Next we describe each steps 1 and 3 in more detail.
-
-#### Step 1
-
-Subroutine *HcUCSDUF* is quite straightforward. It loops through all the surfaces in each zone and decides whether the surface is located in the upper, mixed subzone or the lower, occupied subzone, or if the surface is in both subzones. If entirely in one subzone the subzone temperature is stored in the surface effective temperature variable *TempEffBulkAir(SurfNum)* and h<sub>c</sub> for the surface is calculated by a call to subroutine *CalcDetailedHcInForDVModel*. This routine uses the “detailed� natural convection coefficient calculation that depends on surface tilt and <span>\(\Delta {T^{1/3}}\)</span>. This calculation is appropriate for situations with low air velocity.
-
-For surfaces that bound 2 subzones, the subroutine calculates h<sub>c</sub> for each subzone and then averages them, weighting by the amount of surface in each subzone.
-
-During the surface loop, once the h<sub>c</sub> for a surface is calculated, the appropriate subzone HA and HAT sums are incremented. If a surface is in 2 subzones the HA and HAT for each subzone are incremented based on the area of the surface in each subzone. The subroutine calculates a separate HA and HAT for the windows for use in calculating the window convective gain.
-
-#### Step 2
-
-The calculation of 
-subzone temperatures follows the method used in the ***ZoneTempPredictorCorrector*** module and described in the section **Basis for the System and Zone Integration**. Namely a third order finite difference expansion of the temperature time derivative is used in updating the subzone temperatures. Otherwise the subzone temperatures are obtained straightforwardly by solving an energy balance equation for each subzone.
-
-<div>$$
- \begin{array}{rl}
-  T_{oc} &= (C_{air,oc} \cdot (3 \cdot T_{ - 1,oc} - (3/2) \cdot T_{ - 2,oc} + (1/3) \cdot T_{ - 3,oc}) + \dot Q_{ocz} \cdot Fr_{gains} + HAT_{oc} + MCPT_{tot})/((11/6) \cdot C_{air,oc} + HA_{oc} + MCP_{tot}) \\
-  T_{mx} &= (C_{air,mx} \cdot (3 \cdot T_{ - 1,mx} - (3/2) \cdot T_{ - 2,mx} + (1/3) \cdot T_{ - 3,mx}) + \dot Q_{ocz} \cdot (1 - Fr_{gains}) + \dot Q_{mxz} + HAT_{mx} + T_{oc} \cdot MCP_{tot})/((11/6) \cdot C_{air,mx} + HA_{mx} + MCP_{tot})
- \end{array}
-$$</div>
-
-Here <span>\({C_{air,oc}}\)</span> and <span>\({C_{air,mx}}\)</span> are the heat capacities of the air volume in each subzone. <span>\({C_{air,mx}}\)</span> is calculated by
-
-<div>$${R_{air,mx}} = {V_{mx}} \cdot \left( {\Delta {z_{mx}}/{z_{ceil}}} \right) \cdot {\rho_{air,mx}} \cdot {c_{p,air,mx}} \cdot Mu{l_{cap}}/\left( {\Delta {t_z} \cdot 3600} \right)$$</div>
-
-<div>$${c_{air,mx}} = {R_{air,mx}} \cdot \Delta {t_z}/\Delta {t_{sys}}$$</div>
-
-The gains fraction <span>\(F{r_{gains}}\)</span> is a user input via a schedule. It is the fraction of the convective gains in the occupied subzone that remain in that subzone.
-
-The other subzone air heat capacities are calculated in the same manner.
-
-#### Mixed calculation
-
-The above iterative procedure assumed that the UFAD zone model was applicable: i.e., conditions were favorable temperature stratification in the zone. Now that this calculation is complete and the subzone temperatures and depths calculated, we check to see if this assumption was justified. If not, zone conditions must be recalculated assuming a well-mixed zone.
-
-If <span>\({T_{mx}} &lt; {T_{oc}}\)</span> or <span>\(MC{P_{tot}} \le 0\)</span> or <span>\({H_{fr}} \cdot {H_{ceil}} &lt; \Delta {z_{occ,\min }}\)</span> then the following mixed calculation will replace the UFAD exterior zone calculation.
-
-**Note:**  <span>\({\Delta_{occ,min}}\)</span> is the minimum thickness of occupied subzone. It is set to 0.2 meters.
-
-The mixed calculation iteratively calculates surface convection coefficients and room temperature just like the displacement ventilation calculation described above. In the mixed case however, only one zone temperature *T<sub>avg</sub>* is calculated. The 2 subzone temperatures are then set equal to *T<sub>avg</sub>*.
-
-First, *Fr<sub>hb</sub>*  is set equal to zero.
-
-Then the code iterates over these steps.
-
-Calculate *T<sub>avg</sub>* using
-
-<div>$$\begin{array}{l}{T_{avg}} = ({C_{air,z}} \cdot (3 \cdot {T_{ - 1,z}} - (3/2) \cdot {T_{ - 2,z}} + (1/3) \cdot {T_{ - 3,z}}) + \\\quad \quad {{\dot Q}_{tot,conv}} + HA{T_{oc}} + HA{T_{mx}}MCP{T_{tot}})/((11/6) \cdot {C_{air,z}} + H{A_{oc}} + H{A_{mx}} + MC{P_{tot}})\end{array}$$</div>
-
-<div>$${T_{mx}} = {T_{avg}}$$</div>
-
-<div>$${T_{oc}} = {T_{avg}}$$</div>
-
-Call *HcUCSDUF* to calculate the *h<sub>c</sub>*’s.
-
-Repeat step 1
-
-#### Final calculations
-
-The UFAD exterior zone calculation finishes by calculating some report variables.
-
-We define heights:
-
-<div>$${H_{trans}} = F{r_{hb}} \cdot {H_{ceil}}$$</div>
-
-<div>$${H_{mxavg}} = \left( {{H_{ceil}} + {H_{trans}}} \right)/2$$</div>
-
-<div>$${H_{ocavg}} = {H_{trans}}/2$$</div>
-
-Using the user defined comfort height we calculate the comfort  temperature.
-
-If mixing:
-
-<div>$${T_{comf}} = {T_{avg}}$$</div>
-
-If UFAD:
-
-If  <span>\({H_{comf}} &lt; {H_{ocavg}}\)</span>
-
-<div>$${T_{comf}} = {T_{occ}}$$</div>
-
-Else if <span>\({H_{comf}} \ge {H_{ocavg}}\)</span> and <span>\({H_{comf}} &lt; {H_{mxavg}}\)</span>
-
-<div>$${T_{comf}} = \left( {{T_{oc}}\left( {{H_{mxavg}} - {H_{comf}}} \right) + {T_{mx}}\left( {{H_{comf}} - {H_{ocavg}}} \right)} \right)/\left( {{H_{mxavg}} - {H_{ocavg}}} \right)$$</div>
-
-Else if <span>\({H_{comf}} \ge {H_{mxavg}}\)</span> and <span>\({H_{comf}} &lt; {H_{ceil}}\)</span>
-
-<div>$${T_{comf}} &lt; {T_{mx}}$$</div>
-
-Using the user defined thermostat height we calculate the temperature at the thermostat.
-
-If mixing:
-
-<div>$${T_{stat}} = {T_{avg}}$$</div>
-
-If UFAD:
-
-If<span>\({H_{stat}} &lt; {H_{ocavg}}\)</span>
-
-<div>$${T_{stat}} = {T_{occ}}$$</div>
-
-Else if <span>\({H_{stat}} \ge {H_{ocavg}}\)</span> and <span>\({H_{stat}} &lt; {H_{mcavg}}\)</span>
-
-<div>$${T_{stat}} = \left( {{T_{oc}}\left( {{H_{mxavg}} - {H_{stat}}} \right) + {T_{mx}}\left( {{H_{stat}} - {H_{ocavg}}} \right)} \right)/\left( {{H_{mxavg}} - {H_{ocavg}}} \right)$$</div>
-
-Else if <span>\({H_{stat}} \ge {H_{mxavg}}\)</span> and <span>\({H_{stat}} &lt; {H_{ceil}}\)</span>
-
-<div>$${T_{stat}} = {T_{mx}}$$</div>
-
-The average temperature gradient is:
-
-If <span>\({H_{mxavg}} - {H_{occavg}} > 0.1\)</span>
-
-<div>$$Grad{T_{avg}} = ({T_{mx}} - {T_{occ}})/({H_{mxavg}} - {H_{occavg}})$$</div>
-
-else <span>\(Grad{T_{avg}} = 0.0\)</span>
-
-Finally, the zone node temperature is set to *T<sub>mx</sub>*.
-
-Other variables that are reported out are <span>\(\Gamma \)</span>and <span>\(\phi \)</span>.
-
-<div>$$\phi  = ({T_{mx}} - {T_{occ}})/({T_{mx}} - {T_{sup}})$$</div>
-
-where <span>\({T_{sup}}\)</span>is the zone supply air temperature.
-
-#### References
-
-Qing Liu. 2006. The Fluid Dynamics of an Underfloor Air Distribution System. A PhD dissertation in Engineering Sciences (Systems Science) at UC San Diego.
-
-### Cross Ventilation Room Air Model
-
-#### Overview
-
-The input object RoomAirSettings:CrossVentilation provides a simple model, developed by UCSD, for heat transfer and vertical temperature profile prediction in cross ventilated rooms. This model was developed using scaling analysis, experimental correlations, computational fluid dynamics, and approximate solutions of the Navier-Stokes equations. The model distinguishes two regions in the room, the main jet region and the recirculations, and predicts characteristic airflow velocities and average air temperatures. The model consists of a set of analytical expressions that clearly display the first order effects of room geometry and inflow characteristics on Cross Ventilation airflow and heat transfer.
-
-#### Cross-Ventilation
-
-The CV model is developed from analysis of the flow structure inside a cross-ventilated room, which naturally divides into distinct jet and recirculation flow regions. The flows are calculated for different room and opening geometries using CFD. Correlations with room and aperture parameters are then deduced for a characteristic temperature and velocity in the jet and recirculation regions.
-
-The SS 2-opening model is developed from analysis of wind tunnel data for pressure and ventilation rates, correlating the flow rate with the pressure difference between the two openings, with contributions from both the mean and unsteady components. The local velocity estimate is also based on wind tunnel data, and gives the velocity as a function of wind angle.
-
-#### Approach
-
-With the widespread availability of air conditioning, natural ventilation became a rare feature in commercial buildings in the US. The recent resurgence of the use of natural ventilation relies on systems whose performance can be predicted and controlled, often working in conjunction with mechanical ventilation and cooling systems in hybrid ventilation configurations. In this contemporary approach natural ventilation deals with thermal and air renewal requirements in the cold and mild season and often plays a limited role in the warm season (due to the need to control indoor velocities and noise levels). Whereas traditional natural ventilation systems often use large openings (1-4m<sup>2</sup>), both recent and expected future examples tend to use smaller openings (0.2-1m<sup>2</sup>), often in multiple opening configurations that allow for efficient heat removal with controlled indoor velocities.
-
-The modeling approach used is based on simplified solutions of the Navier Stokes equations that are integrated into scaling formulae that predict relevant flow quantities (characteristic velocities and temperatures) in distinct regions of the flow. The scaling expressions that will be developed use the principle of flow similarity: for a given room geometry and flow regime (either laminar or turbulent), the flow pattern is constant. In the present case, where the goal is to predict internal velocities using as input the inflow velocity (that can be estimated by the airflow rate predicted by the AirflowNetwork model), the principle can be stated as:
-
-(Velocity in a given position in the room) = (Inflow velocity) × (Constant)
-
-The constant is non-dimensional and depends on the position or room zone where the prediction is being made. For a given geometry the constant can be measured experimentally or inferred from a detailed CFD simulation. It is expected that the constant may depend on non-dimensional room geometry parameters that can be inferred from a careful analysis of the flow. The proposed CV model uses a set of CFD simulations, in conjunction with simplified solutions of the Navier Stokes equations, to obtain the constants and their dependence on room geometry features.
-
-The updated CV model proposed in this document was developed using inlet areas *A*<sub>in</sub> and room cross-section areas *A*<sub>RM</sub> in the following range:
-
-0.5% &lt; *A*<sub>in</sub>/*A*<sub>RM</sub> &lt; 5%
-
-whereas the existing model used
-
-3.2% &lt; *A*<sub>in</sub>/*A*<sub>RM</sub> &lt; 21%
-
-The room lengths for which these models are expected to be applied range between the smallest room size of 4m and the maximum achievable CV room flushing length of 15-18m.
-
-
-
-![](media/image2622.png)
-
-Figure 136. Development of an axisymmetric jet from airflow through a window.
-
-Air flows into the room through an inflow window in the form of an approximately axisymmetric jet, with characteristic diameter *L*=*A*<sub>in</sub><sup>1/2</sup>, that is confined by the room surfaces (see Figure 137). The initial portion of the jet (up to six diameters) is called the potential core and is characterized by shear layer development along the perimeter of the jet. After this phase the jet transitions into a self similar profile whose centerline velocity decays as 1/*x*', where *x*' = *x*/*D* (Awbi, 2003).
-
-For the relevant room length range the geometries used in the two models result in:
-
-      New model:       6 &lt; x' &lt; 60
-
-      Existing model:             2 &lt; x' &lt; 18
-
-The smaller openings used in the new model result in significantly more space for jet development along the room length. In all but the shortest rooms the jet will enter the fully developed stage characterized by a 1/*x*' centerline velocity decay rate. For this reason, the updated model uses the average jet velocity profile as opposed to shear layer momentum transfer.
-
-#### Components of the flow
-
-Figure 136 shows the schematic development of a free axisymmetric jet in an unconfined environment, and Figure 137 depicts the confinement effects. The air entrained by the jet is detrained at the outlet, creating two recirculation zones that do not exist in a free jet.
-
-The recirculation flow is similar to the flow in a lid driven cavity, where here the driving force is the confined jet flow. Turbulent lid driven cavity flows have been shown to have self-similar velocity profiles, as shown in Figure 138.
-
-The model is based on the hypothesis that the flow is composed of:
-
-      A – Lid driven cavity flows (in the recirculation regions).
-
-      B – A confined axisymmetric jet flow.
-
-![](media/image2623.png)
-
-Figure 137. Top view of a cross ventilated room. The air entrained by the jet is detrained at the outlet, typically creating two recirculation zones.
-
-
-
-![](media/image2624.png)
-
-Figure 138. Top view of one half of a cross ventilated room. The flow is approximately composed of a confined jet and two lid driven cavity flows (one on each side).
-
-The goal of the model is to obtain the value and functional form of the constant term shown in the scaling laws for the characteristic average velocities in the two flow regions: jet and recirculation regions.
-
-To estimate the average jet velocity we integrate along the depth of the room (including both the core region and the 1/*x*' velocity decay region) to derive an average maximum jet velocity, *V*<sub>J,m</sub>:∙
-
-<div>$${V_{J,m}} = {U_{in}}\sqrt {{A_{in}}} \left\{ {6 + 6.3\ln \left( {{D^*}/6\sqrt {{A_{in}}} } \right)} \right\}/{D^*}$$</div>
-
-(To allow for wind angle effects the room depth *D* has been replaced by *D*\* - see a later section.) The lid-driven cavity flow profile that characterizes the recirculation region has a maximum velocity that is approximately one half of the driving velocity, which in this case is due to the jet. For this reason we define the separation between the two regions along the virtual surface where the jet reaches 50% of its maximum, centerline, velocity.
-
-The analysis of the flow revealed that the room containment effect leads to higher velocities for cases that combine a large inflow opening with a small room cross-section area. In order to account for this effect we propose to use the following non-dimensional scaling parameter:
-
-<div>$${C_{RM}} = {\left( {{A_{in}}/{A_{RM}}} \right)^{1/2}}$$</div>
-
-The expression used for the scaling of the average jet velocity is then:
-
-<div>$${U_J} = {C_1}{C_{RM}}{V_{J,m}}$$</div>
-
-or
-
-<div>$${U_J} = {C_1}\frac{{{Q_{in}}}}{{\sqrt {{A_{in}}{A_{RM}}} }}\left( {{V_{J,m}}/{U_{in}}} \right)$$</div>
-
-where the constant *C*<sub>1</sub> will be obtained from the results of a set of CFD simulations shown in the next section.
-
-In addition to the jet velocity the characteristic recirculation flow velocity <span>\({U_R}\)</span> is also an interesting parameter that, according to the self-similar flow profile hypothesis shown in Figure 138, should scale with a similar expression to the one shown above for the jet (although with a different correlation constant, *C*<sub>2</sub>). The modeling hypothesis can also be tested by evaluating its capability to predict the maximum recirculation flow rate, which can be predicted by multiplying the average velocity by the room cross-section area:
-
-<div>$${Q_R} = {C_3}\frac{{{Q_{in}}}}{{{C_{RM}}}}\left( {{V_{J,m}}/{U_{in}}} \right)$$</div>
-
-Because of the self-similar velocity profile shape that occurs in the recirculation, the near wall velocity (used to predict forced convection) can be estimated simply by multiplying the characteristic recirculation velocity by two.
-
-The expressions obtained apply in the turbulent regime (because the CFD simulations on which they are based are for that regime). Both velocity correlations presented below have the functional form:
-
-<div>$$V = aX + b$$</div>
-
-where *a* is *C*<sub>1</sub>, *C*<sub>2</sub> or *C*<sub>3</sub>, X is a velocity scale and *b* is a constant that results from the best fit. The model has a lower limit on the value of *X*: if *X* is too small the flow is no longer turbulent. This limit implies that the point *X* = 0 is never achieved, avoiding the unrealistic prediction of *V*(0)=*b*.
-
-In addition to the velocity and airflow rate predictions described above it is also essential to predict the temperature variations in the two zones of the flow. In most cases these variations will be positive due to the internal sensible heat gains. However\`, as a result of room surface heat transfer, in some cases the variations may be negative. Analysis of the CFD simulations that are presented in the next section revealed that approximately all the exhaust air comes from the jet regions. For this reason, the heat gains affect the two regions differently:
-
-
-
-·        Heat gains in the jet region only affect this region (no temperature increase in the recirculation regions)
-
-·        Heat gains in the recirculations affect both jet and recirculation regions (because they must be exhausted by the jets).
-
-In order to predict the temperature increase, heat gains were inserted into the recirculation regions for different room geometries in the set of simulations presented in the next section. The volume containing the heat gains extended over the whole depth of the room, from floor to ceiling, and in the lateral direction from halfway between the window edge and the wall all the way to the wall. Applying energy conservation principles to predict the temperature increase in the jet and recirculation region as a function of the sensible heat gains in each region (the sum of internal gains and internal surface heat transfer) we can obtain the average value of temperature increase in each region:
-
-<div>$$\Delta {T_J} = {C_{T,J}}\frac{{q'{'_{RM}}}}{{\rho {c_p}{Q_{in}}}}$$</div>
-
-<div>$$\Delta {T_R} = {C_{T,R}}\frac{{q'{'_{RM}}}}{{\rho {c_p}{Q_{in}}}}$$</div>
-
-where q’’<sub>RM</sub> is the total internal heat gain for the room, r and *c*<sub>p</sub> are the density and specific heat capacity of air, respectively, and *C*<sub>T,J</sub>, *C*<sub>T,R</sub> are constants.
-
-#### Results
-
-Table 44 lists the cases used to develop the updated CV model, which predicts the output variables defined in Table 45 (see also Figure 139). Figure 140, Figure 141, and Figure 142 show plots of the data derived from the CFD simulations of these test cases, and the lines giving the best fit to the data. Table 46 summarizes the correlation formulae and constants. Finally, Table 47 provides estimates for the error of the correlation in each test case.
-
-![](media/image2634.png)
-
-Figure 139. Jet and recirculation regions in typical vertical cross-section through room (y-z plane). Jet boundary occurs where jet velocity has fallen to 50% of centerline maximum. Remainder of cross-section is treated as recirculation. Volumetric heat sources ar
-
-Table 44. Test cases used to develop correlations
-
-<table class="table table-striped">
-  <tr>
-    <th rowspan="2">Case</th>
-    <th>Opening area</th>
-    <th>Room width</th>
-    <th>Room depth</th>
-    <th>Room height</th>
-  </tr>
-  <tr>
-    <td>A in (m 2 )</td>
-    <td>W (m)</td>
-    <td>D (m)</td>
-    <td>H (m)</td>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td>0.25</td>
-    <td>6</td>
-    <td>9</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>2</td>
-    <td>0.25</td>
-    <td>11</td>
-    <td>9</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>0.5</td>
-    <td>9</td>
-    <td>4.5</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>4</td>
-    <td>0.5</td>
-    <td>9</td>
-    <td>6</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>0.5</td>
-    <td>6</td>
-    <td>9</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>6</td>
-    <td>0.5</td>
-    <td>9</td>
-    <td>9</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>7</td>
-    <td>0.5</td>
-    <td>11</td>
-    <td>9</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>8</td>
-    <td>0.5</td>
-    <td>13.5</td>
-    <td>9</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>9</td>
-    <td>0.5</td>
-    <td>9</td>
-    <td>13.5</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>10</td>
-    <td>0.5</td>
-    <td>9</td>
-    <td>18</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>11</td>
-    <td>0.5</td>
-    <td>13.5</td>
-    <td>18</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>12</td>
-    <td>1</td>
-    <td>9</td>
-    <td>9</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>13</td>
-    <td>1</td>
-    <td>9</td>
-    <td>13.5</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td>14</td>
-    <td>1</td>
-    <td>9</td>
-    <td>18</td>
-    <td>2.3</td>
-  </tr>
-  <tr>
-    <td colspan="5">RANGE (max:min ratio)</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>4</td>
-    <td>2.25</td>
-    <td>4</td>
-    <td>1</td>
-  </tr>
-</table>
-
-Table 45. Definitions of output variables
-
-<table class="table table-striped">
-<tr>
-<th>Output variable</th>
-<th>Symbol</th>
-<th>Units</th>
-<th>Definition</th>
-</tr>
-<tr>
-<td>Jet velocity</td>
-<td><span>\({U_J}\)</span></td>
-<td>m/s</td>
-<td>Volume-averaged jet region velocity. The averaging volume is bounded at each x along the room depth by the line in the y-z plane where the jet velocity drops to 50% of its maximum centerline value.</td>
-</tr>
-<tr>
-<td>Recirculation zone velocity</td>
-<td><span>\({U_R}\)</span></td>
-<td>m/s</td>
-<td>Area-averaged velocity in the y-z plane with maximum flow. The averaging area is the recirculation part of the room cross-section. Typically the plane of maximum flow occurs at x ~ 2D/3 (D/3 before the outlet).</td>
-</tr>
-<tr>
-<td>Recirculation zone flow rate</td>
-<td><span>\({Q_R}\)</span></td>
-<td>m<sup>3</sup>/s</td>
-<td>Total flow rate for the recirculation regions in the plane of maximum flow (see above).</td>
-</tr>
-<tr>
-<td>Jet temperature rise</td>
-<td><span>\(\Delta {T_J}\)</span></td>
-<td>°C</td>
-<td>Volume-averaged temperature variations in the jet region, over the same volume used to define the jet velocity average.</td>
-</tr>
-<tr>
-<td>Recirculation zone temperature rise</td>
-<td><span>\(\Delta {T_R}\)</span></td>
-<td>°C</td>
-<td>Volume-average temperature variations in the recirculation region. The average is calculated over the cuboidal volume placed in each recirculation containing the volumetric sensible heat gains (see main text).</td>
-</tr>
-</table>
-
-See also Figure 139. Note the *x*-coordinate is along the room, the *y*-coordinate is across the room and the *z*-coordinate is vertical.
-
-Table 46. Correlation formulae in the form Y = aX + b
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Y</th>
-<th>X</th>
-<th>a</th>
-<th>b</th>
-<th>R<sup>2</sup></th>
-</tr>
-<tr>
-<td>Jet velocity</td>
-<td><span>\({U_J}/{U_{in}}\)</span></td>
-<td><span>\(\sqrt {{A_{in}}/{A_{RM}}} \cdot \left( {{V_{J,m}}/{U_{in}}} \right)\)</span></td>
-<td>1.6173</td>
-<td>0.1466</td>
-<td>0.8343</td>
-</tr>
-<tr>
-<td>Recirculation zone velocity</td>
-<td><span>\({U_R}/{U_{in}}\)</span></td>
-<td><span>\(\sqrt {{A_{in}}/{A_{RM}}} \cdot \left( {{V_{J,m}}/{U_{in}}} \right)\)</span></td>
-<td>0.8911</td>
-<td>0.0393</td>
-<td>0.6464</td>
-</tr>
-<tr>
-<td>Recirculation zone flow rate</td>
-<td><span>\({Q_R}/{U_{in}}\)</span></td>
-<td><span>\(\sqrt {{A_{in}}{A_{RM}}} \cdot \left( {{V_{J,m}}/{U_{in}}} \right)\)</span></td>
-<td>0.4444</td>
-<td>0.1751</td>
-<td>0.6761</td>
-</tr>
-<tr>
-<td>Jet temperature rise</td>
-<td><span>\(\Delta {T_J}\)</span></td>
-<td><span>\(\frac{{q'{'_{RM}}}}{{\rho {c_p}{Q_{in}}}}\)</span></td>
-<td>0.8254</td>
-<td>0</td>
-<td>n/a</td>
-</tr>
-<tr>
-<td>Recirculation zone temperature rise</td>
-<td><span>\(\Delta {T_R}\)</span></td>
-<td><span>\(\frac{{q'{'_{RM}}}}{{\rho {c_p}{Q_{in}}}}\)</span></td>
-<td>1.2734</td>
-<td>0</td>
-<td>n/a</td>
-</tr>
-
-</table>
-
-Table 47. Accuracy of correlation formulae in predicting test case results
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="5">Cases</th>
-    <th colspan="5">Errors (%)</th>
-  </tr>
-  <tr>
-    <td>ID</td>
-    <td>A (m2)</td>
-    <td>W (m)</td>
-    <td>D (m)</td>
-    <td>H (m)</td>
-    <td>Jet Velocity</td>
-    <td>Recirculation Velocity</td>
-    <td>Recirculation Flow Rate</td>
-    <td>Jet Temperature Rise</td>
-    <td>Recirculation Temperature Rise</td>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td>0.25</td>
-    <td>6</td>
-    <td>9</td>
-    <td>2.3</td>
-    <td>16</td>
-    <td>45</td>
-    <td>60</td>
-    <td>1</td>
-    <td>10</td>
-  </tr>
-  <tr>
-    <td>2</td>
-    <td>0.25</td>
-    <td>11</td>
-    <td>9</td>
-    <td>2.3</td>
-    <td>5</td>
-    <td>43</td>
-    <td>32</td>
-    <td>5</td>
-    <td>7</td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>0.5</td>
-    <td>9</td>
-    <td>4.5</td>
-    <td>2.3</td>
-    <td>2</td>
-    <td>18</td>
-    <td>27</td>
-    <td>15</td>
-    <td>2</td>
-  </tr>
-  <tr>
-    <td>4</td>
-    <td>0.5</td>
-    <td>9</td>
-    <td>6</td>
-    <td>2.3</td>
-    <td>6</td>
-    <td>32</td>
-    <td>28</td>
-    <td>7</td>
-    <td>1</td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>0.5</td>
-    <td>6</td>
-    <td>9</td>
-    <td>2.3</td>
-    <td>7</td>
-    <td>6</td>
-    <td>21</td>
-    <td>7</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>6</td>
-    <td>0.5</td>
-    <td>9</td>
-    <td>9</td>
-    <td>2.3</td>
-    <td>10</td>
-    <td>4</td>
-    <td>6</td>
-    <td>15</td>
-    <td>17</td>
-  </tr>
-  <tr>
-    <td>7</td>
-    <td>0.5</td>
-    <td>11</td>
-    <td>9</td>
-    <td>2.3</td>
-    <td>6</td>
-    <td>7</td>
-    <td>0</td>
-    <td>14</td>
-    <td>20</td>
-  </tr>
-  <tr>
-    <td>8</td>
-    <td>0.5</td>
-    <td>13.5</td>
-    <td>9</td>
-    <td>2.3</td>
-    <td>14</td>
-    <td>9</td>
-    <td>5</td>
-    <td>21</td>
-    <td>2</td>
-  </tr>
-  <tr>
-    <td>9</td>
-    <td>0.5</td>
-    <td>9</td>
-    <td>13.5</td>
-    <td>2.3</td>
-    <td>10</td>
-    <td>11</td>
-    <td>17</td>
-    <td>7</td>
-    <td>8</td>
-  </tr>
-  <tr>
-    <td>10</td>
-    <td>0.5</td>
-    <td>9</td>
-    <td>18</td>
-    <td>2.3</td>
-    <td>10</td>
-    <td>25</td>
-    <td>29</td>
-    <td>8</td>
-    <td>3</td>
-  </tr>
-  <tr>
-    <td>11</td>
-    <td>0.5</td>
-    <td>13.5</td>
-    <td>18</td>
-    <td>2.3</td>
-    <td>8</td>
-    <td>2</td>
-    <td>23</td>
-    <td>9</td>
-    <td>6</td>
-  </tr>
-  <tr>
-    <td>12</td>
-    <td>1</td>
-    <td>9</td>
-    <td>9</td>
-    <td>2.3</td>
-    <td>2</td>
-    <td>5</td>
-    <td>3</td>
-    <td>3</td>
-    <td>4</td>
-  </tr>
-  <tr>
-    <td>13</td>
-    <td>1</td>
-    <td>9</td>
-    <td>13.5</td>
-    <td>2.3</td>
-    <td>8</td>
-    <td>10</td>
-    <td>10</td>
-    <td>3</td>
-    <td>6</td>
-  </tr>
-  <tr>
-    <td>14</td>
-    <td>1</td>
-    <td>9</td>
-    <td>18</td>
-    <td>2.3</td>
-    <td>0</td>
-    <td>18</td>
-    <td>6</td>
-    <td>13</td>
-    <td>2</td>
-  </tr>
-  <tr>
-    <td colspan="5">Average</td>
-    <td>8</td>
-    <td>17</td>
-    <td>19</td>
-    <td>9</td>
-    <td>6</td>
-  </tr>
-</table>
-
-In each case the error is the percentage difference between the given correlation prediction and the test case result obtained from CFD, i.e. 100\*|(correlation prediction – CFD)/CFD|.
-
-
-
-<span>\(\sqrt {{A_{in}}/{A_{RM}}} \left( {{V_{J,m}}/{U_{in}}} \right)\)</span><span>\({U_J}/{U_{in}}\)</span>![](media/image2652.png)
-
-Figure 140. Jet velocity correlation.
-
-
-
-<span>\(\sqrt {{A_{in}}/{A_{RM}}} \left( {{V_{J,m}}/{U_{in}}} \right)\)</span><span>\({U_R}/{U_{in}}\)</span>![](media/image2655.png)
-
-Figure 141. Recirculation region velocity correlation.
-
-
-
-<span>\(\sqrt {{A_{in}}{A_{RM}}} \left( {{V_{J,m}}/{U_{in}}} \right)\)</span><span>\({Q_R}/{U_{in}}\)</span>![](media/image2658.png)
-
-Figure 142. Recirculation region flow rate.
-
-#### Wind angle effects
-
-When the incoming wind is not normal to the façade the jet enters the room at an angle, as shown in Figure 143.
-
-![](media/image2659.png)
-
-Figure 143. Schematic of jet resulting from wind at angle φ to façade.
-
-This oblique geometry has two main effects on the flow and consequent correlation predictions:
-
-The inflow area is reduced, creating a larger inflow velocity for the same flow rate.
-
-The room flow path length is increased, from *D* to *D*\*, resulting in a larger apparent depth.
-
-The first effect increases indoor velocities while the second effect decreases the velocities.
-
-#### Multiple apertures
-
-CFD simulations for rooms with more than one inflow aperture show that the model can be applied to these configurations with minimal adjustments. As a result of increased dissipation in the central recirculation region, where two distinct recirculation flows collide (Figure 144), the airflow velocities are reduced by 5-10%, as shown in the charts in Figure 145.
-
-![](media/image2660.png)
-
-Figure 144. Flow regions for a room with 2 inlets and 2 outlets.
-
-![](media/image2662.png)
-
-Figure 145. Jet velocity and recirculation velocity for the two halves of 3 different 2-inlet rooms, A-C, compared with the corresponding 1-inlet rooms.
-
-***Heat transfer in recirculating flows***
-
-In most cross ventilation flows with recirculations the mixing between recirculation and inflow jet is only partial. Figure 146 shows a schematic representation of the heat transfer process (showing a top view of one half of a symmetrical room). The flow is divided into three distinct streams with connected temperature variations:
-
-The main jet (labeled J in the figure).
-
-The part of the recirculation flow that exchanges heat with the jet (label R).
-
-The wall boundary layer part of the recirculation flow (label W).
-
-![](media/image2663.png)
-
-Figure 146. Top view of the flow structure in case R.
-
-The light gray arrows show flow direction. The dark gray arrows show heat transfer in the shear layer. The recirculation region coordinate system is shown in the figure, with coordinate *r* varying between 0 and *L*.
-
-#### Heat transfer in a shear layer
-
-It is possible to use a formulation with a heat transfer area, a convection heat transfer coefficient and an average shear layer temperature difference to model the heat exchange between jet and recirculation flows:
-
-<span>\({Q_{y = 0}} = {A_{SL}}\,{h_{SL}}\,\Delta {T_{SL}}\)</span>, <span>\({A_{SL}} = L\,\,P\,,\,\,{h_{SL}} = \frac{{\rho \,{C_P}\,F}}{{{C_D}\,\,{A_{IN}}\,\,4\,\sigma \,\sqrt \pi  }}\)</span>
-
-Locally, the heat transfer process is driven by the variable, local, temperature difference:
-
-<div>$$\rho \,{C_P}\,F\,\frac{{\partial \,{T_J}(x)}}{{\partial \,x}} =  - \,\frac{{{A_{SL}}\,{h_{SL}}}}{L}\,\left( {{T_J}(x) - {T_R}(x)} \right) = \frac{{P\,\,\left( {{T_J}(x) - {T_R}(x)} \right)}}{{{C_D}\,{A_{IN}}\,4\,\sigma \,\sqrt \pi  }}$$</div>
-
-#### Predicting air temperature in the recirculation region of the flow
-
-An accurate representation of system behavior must consider both the local heat transfer in the shear layer (varying along the *x* direction, driven by the temperature profiles *T<sub>J</sub>(x)* and *T<sub>R</sub>(x)*) and the heat transfer in the wall boundary layers (with temperature *T<sub>W</sub>(r)*). Both transfers can be modeled using differential equations, resulting in the following system of equations:
-
-<div>$$
-  \begin{array}{rl}
-    \rho C_p F R \frac{\partial T_W \left(r\right)}{\partial r} &= \frac{A_S h_S}{L} \left(T_S - T_W \left(r\right)\right) \\
-    \rho C_p F R \frac{\partial T_R \left(x\right)}{\partial x} &= \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right) \\
-    \rho C_p F \frac{\partial T_J \left(x\right)}{\partial x} &= \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right) 
-  \end{array}
-$$</div>
-
-The relevant boundary conditions are:
-
-<div>$${T_W}({L_{}}) = {T_R}(0)\,,\,{T_W}(0) = {T_R}(L)\,,\,\,{T_J}(0) = {T_{IN}}$$</div>
-
-The first equation in models heat transfer in the wall layer. The second models the temperature variation of the portion of the recirculation flow that is in contact with the jet, it differs from the third equation only in a sign (the temperature variation in *T<sub>R</sub>* is symmetric to the variation in *T<sub>J</sub>*) and the flow rate (*F.R* for the recirculation and *F* for the main jet). The temperature in the recirculation region is given by:
-
-<div>$${T_W}(r) = {T_S} - ({T_S} - {T_{IN}})\,\frac{{{e^{\frac{{{h_S}\,{A_S}}}{{\rho \,{C_P}\,R\,F}}\frac{r}{{{L_{}}}}}}\,({e^{ - \frac{{{A_{SL}}\,{h_{SL}}\,(1 + R)}}{{\rho \,{C_P}\,R\,F}}}} - 1)}}{{{e^{ - \frac{{{A_{SL}}\,{h_{SL}}\,(1 + R)}}{{\rho \,{C_P}\,R\,F}}}} - {e^{\frac{{{h_S}\,{A_S}}}{{\rho \,{C_P}\,R\,F}}}}\,(1 + R) + R}}$$</div>
-
-#### Heat transfer in recirculating flows with internal gains
-
-Whereas surface heat transfer is an important component of room heat transfer, internal gains often dominate the room temperature field. Referring to the previously used subdivision of the room into jet and recirculation regions we can see that gains can occur exclusively in the jet region, exclusively in the recirculation region or in both regions.
-
-#### Heat gains in the jet region
-
-The effect of gains in the jet region on room air temperature distribution is simple to model and, within the first order accuracy goal, can be characterized as follows:
-
-For gains occurring in the jet region (between the inlet and the room outlet) a change in inflow temperature is an adequate, conservative approximation. From energy conservation we conclude that the altered inflow temperature is given by:
-
-<div>$${T_{ING}} = {T_{IN}} + \frac{{{G_J}}}{{\rho {C_P}F}}$$</div>
-
-Gains occurring in the jet region, close to the outlet can be ignored in a first order accuracy model.
-
-Clearly the two approaches described above are only exact when: the gains occur at the inlet and perfectly mix with the inflow jet (for the first case), or whenever the gains occur very close to the outlet (in the second case). In all other situations, the first approach provides a conservative approximation. In the model implementation in EnergyPlus the user will not define the exact location of the heat gains within each region of the flow therefore, heat gains in the jet region, are inserted in two equal parts in two separate points of the jet flow (in the room entrance and before the exit, see points r=0 and r=L<sub>R</sub> in Figure 146).
-
-#### Heat gains in the recirculation region
-
-When heat gains occur in the recirculation region significant heat accumulation occurs due to the limited heat transfer ability of the shear layer. Due to this limited ability, the recirculation is partially isolated from the main jet flow and higher temperatures are generated in this region whenever heat gains are present. The concept of a global heat transfer coefficient is not applicable.
-
-In the case of a flow in a room with adiabatic surfaces and heat gains in the recirculation region the indoor air temperatures can be predicted using the solution to the following system of equations:
-
-<div>$$
-  \begin{array}{rl}
-    \rho C_p F R \left(T_R\left(0\right) - T_R\left(L\right)\right) &= G_R \\
-    \rho C_p F R \frac{\partial T_R \left(x\right)}{\partial x} &= \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right) \\
-    \rho C_p F \frac{\partial T_J \left(x\right)}{\partial x} &= \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right)
-  \end{array}
-$$</div>
-
-This system of equations differs from system F16 in several ways. Because there is no wall heat transfer there is no need to split the recirculation flow in two parts (*R* and *W*). The temperature increase in the recirculation flow is simply defined by the internal gains (first equation in ). The second and third equations in model shear layer heat transfer are similar in the two cases ( and ).
-
-The recirculation flow temperature at *x*=0 is given by:
-
-<div>$${T_R}(0) = {T_{IN}} + \left( {\frac{1}{{{e^{\frac{{{A_{SL}}{h_{SL}}\,(1 + R)}}{{\rho \,{C_P}F\,R}}}} - 1}} + 1} \right)\frac{{{G_R}(1 + R)}}{{\rho \,{C_P}F\,R}}$$</div>
-
-The temperature in the recirculation is inversely proportional to the recirculation flow ratio (*R*) and the shear layer area (measured by the product: *A<sub>SL</sub> h<sub>SL</sub>*). As both of these parameters increase this expression becomes similar to . The recirculation flow temperature at *x=L* is given by:
-
-<div>$${T_R}(L) = {T_R}(0) + \Delta {T_R}$$</div>
-
-The temperature variations in the recirculation flow is given by:
-
-<div>$$\Delta {T_R} = \frac{{{G_R}}}{{\rho \,{C_P}\,F\,R}}$$</div>
-
-#### Combined effects of surface heat transfer and internal gains in the recirculation region
-
-In this case, the following system of equations must be solved:
-
-<div>$$
-  \begin{array}{rl}
-    \rho C_p F R \frac{\partial T_W \left(r\right)}{\partial r} &= -\frac{A_S h_S}{L} \left(T_S - T_W \left(r\right)\right) - \frac{G_R}{L_R} \\
-    \rho C_p F R \frac{\partial T_R \left(x\right)}{\partial x} &= \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right) \\
-    \rho C_p F \frac{\partial T_J \left(x\right)}{\partial x} &= \frac{A_{SL} h_{SL}}{L} \left(T_J\left(x\right) - T_R \left(x\right)\right) 
-  \end{array}
-$$</div>
-
-With the boundary conditions: <span>\({T_W}(L) = {T_R}(0)\,,\,{T_W}(0) = {T_R}(L)\,,\,\,{T_J}(0) = {T_{IN}}\)</span>
-
-For simplicity the heat gains are considered to be evenly distributed along the recirculation path. The temperature variation in the recirculation region is given by:
-
-<div>$${T_W}(r) = {T_S} + \frac{{{G_R}}}{{{A_S}\,{h_S}}} - \frac{{{e^{\frac{{{h_S}\,{A_S}}}{{\rho \,{C_P}\,R\,F}}\frac{r}{{{L_R}}}}}\,({e^{ - \frac{{{A_{SL}}\,{h_{SL}}\,(1 + R)}}{{\rho \,{C_P}\,R\,F}}}} - 1)\,({G_R} + {A_S}\,{h_S}\,({T_S} + {T_{IN}}))}}{{{e^{ - \frac{{{A_{SL}}\,{h_{SL}}\,(1 + R)}}{{\rho \,{C_P}\,R\,F}}}} + R - {e^{\frac{{{h_S}\,{A_S}}}{{\rho \,{C_P}\,R\,F}}}}\,(1 + R)}}$$</div>
-
-
-
-Table 48. List of variables for CV model
-
-<table class="table table-striped">
-<tr>
-<th>Symbol</th>
-<th>Units</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>a</td>
-<td>-</td>
-<td>Slope of correlation line of best fit</td>
-</tr>
-<tr>
-<td>A<sub>in</sub></td>
-<td>m<sup>2</sup></td>
-<td>Inlet area</td>
-</tr>
-<tr>
-<td>A<sub>RM</sub></td>
-<td>m<sup>2</sup></td>
-<td>Room cross-sectional area</td>
-</tr>
-<tr>
-<td>b</td>
-<td>-</td>
-<td>Intercept of correlation line of best fit</td>
-</tr>
-<tr>
-<td>c<sub>p</sub></td>
-<td>J/kg/K</td>
-<td>Specific heat capacity of air</td>
-</tr>
-<tr>
-<td>C<sub>RM</sub></td>
-<td>-</td>
-<td>Confinement scaling factor, (A<sub>in</sub>/A<sub>RM</sub>)<sup>1/2</sup></td>
-</tr>
-<tr>
-<td>C<sub>1</sub></td>
-<td>-</td>
-<td>Correlation constant for jet velocity</td>
-</tr>
-<tr>
-<td>C<sub>2</sub></td>
-<td>-</td>
-<td>Correlation constant for recirculation velocity</td>
-</tr>
-<tr>
-<td>C<sub>3</sub></td>
-<td>-</td>
-<td>Correlation constant for recirculation flow rate</td>
-</tr>
-<tr>
-<td>D</td>
-<td>m</td>
-<td>Room depth, distance between inlet and outlet facades</td>
-</tr>
-<tr>
-<td>D*</td>
-<td>m</td>
-<td>Effective room depth adjusted for wind angle</td>
-</tr>
-<tr>
-<td>H</td>
-<td>m</td>
-<td>Room height</td>
-</tr>
-<tr>
-<td>            <span>\(q'{'_{RM}}\)</span></td>
-<td>W</td>
-<td>Total heat input from internal heat sources</td>
-</tr>
-<tr>
-<td>Q<sub>in</sub></td>
-<td>m<sup>3</sup>/s</td>
-<td>Inlet flow rate, A<sub>in</sub> U<sub>in</sub></td>
-</tr>
-<tr>
-<td>            <span>\({Q_R}\)</span></td>
-<td>m<sup>3</sup>/s</td>
-<td>Maximum recirculation region flow rate</td>
-</tr>
-<tr>
-<td>U<sub>in</sub></td>
-<td>m/s</td>
-<td>Inlet velocity, average over inlet area</td>
-</tr>
-<tr>
-<td>U<sub>m</sub></td>
-<td>m/s</td>
-<td>Maximum centerline velocity of jet</td>
-</tr>
-<tr>
-<td>U<sub>0</sub></td>
-<td>m/s</td>
-<td>Uniform inlet velocity of jet</td>
-</tr>
-<tr>
-<td>            <span>\({U_J}\)</span></td>
-<td>m/s</td>
-<td>Volume-averaged jet velocity</td>
-</tr>
-<tr>
-<td>            <span>\({U_R}\)</span></td>
-<td>m/s</td>
-<td>Average recirculation region velocity over plane of maximum flow</td>
-</tr>
-<tr>
-<td>V</td>
-<td>m/s</td>
-<td>Velocity scale</td>
-</tr>
-<tr>
-<td>V<sub>J,m</sub></td>
-<td>m/s</td>
-<td>Average of U<sub>m</sub> over room depth</td>
-</tr>
-<tr>
-<td>W</td>
-<td>m</td>
-<td>Room width</td>
-</tr>
-<tr>
-<td>x</td>
-<td>m</td>
-<td>Coordinate along room depth, 0 ≤ x ≤ D</td>
-</tr>
-<tr>
-<td>x'</td>
-<td>-</td>
-<td>Non-dimensional x-coordinate, x/D</td>
-</tr>
-<tr>
-<td>X</td>
-<td>m/s</td>
-<td>Velocity correlation parameter</td>
-</tr>
-<tr>
-<td>Y</td>
-<td>m</td>
-<td>Lateral coordinate across room width</td>
-</tr>
-<tr>
-<td>Z</td>
-<td>m</td>
-<td>Vertical coordinate</td>
-</tr>
-<tr>
-<td>            <span>\(\Delta {T_J}\)</span></td>
-<td>°C</td>
-<td>Average jet temperature variation</td>
-</tr>
-<tr>
-<td><span>\(\Delta {T_R}\)</span></td>
-<td>°C</td>
-<td>Average recirculation region temperature variation</td>
-</tr>
-<tr>
-<td>r</td>
-<td>kg/m<sup>3</sup></td>
-<td>Density of air</td>
-</tr>
-<tr>
-<td>φ</td>
-<td>°</td>
-<td>Wind direction relative to façade normal</td>
-</tr>
-
-</table>
-
-#### References
-
-Awbi, H.B. (2003) *Ventilation of Buildings* (2<sup>nd</sup> edition). Routledge, 536pp.
-
-Carrilho da Graca, G. 2003.Simplified models for heat transfer in rooms. Ph. D. Thesis, University of California, San Diego.
-
-Kalema, T., Haapala, T. \`995. Effect of interior heat transfer coefficients on thermal dynamics and energy consumption, Energy and Buildings 22 (2) pp. 101-113.
-
-Aynsley, R.M., Melbourne, W., Vickery, B.J. 1977. Architectural Aerodynamics. Applied Science London.
-
-Baturin, V. V. , Billington, N. S. 1972. Fundamentals of Industrial Ventilation, Franklin Book Company 1972, pp. 174-179.
-
-Neiswanger, L., Johnson, G.A., Carey, V.P. 1987. An experimental study of high Raleigh number mixed convection in a rectangular enclosure with restricted inlet and outlet openings. Transactions of ASME, Vol. 109, 446-453.
-
-Ohba, M., Irie, K., Kurabuchi, T. 2001. Study on airflow characteristics inside and outside a CVmodel, and ventilation flow rate using wind tunnel experiments. Journal of Wind Engineering and Industrial Aerodynamics, in press.
-
-Chandra, S., Kerestecioglu, A.A. 1984. Heat transfer in naturally ventilated rooms data from full-scale measurements, ASHRAE Transactions, Volume 90, part 1b 211-224.
-
-Altmayer, E.F., Gadgil, A.J., Bauman, F.S., Kammerud, R.C. Correlations for convective heat transfer from room surfaces. ASHRAE Transactions, No. 2764.
-
-Spitler, J. D., Pedersen, C.O., Fisher, D.E. 1991. Interior Convective Heat Transfer in Buildings with Large Ventilative Flow Rates. ASHRAE Transactions, Vol. 97, Pt.1, pp. 505-515.
-
-Awbi, H.B. & Hatton, A. 1999. Natural convection from heated room surfaces, Energy and Buildings, 30, 233-244.
-
-Siebers, D. L., Schwind, R. G., Moffat, R. J. 1983. Experimental Mixed Convection Heat Transfer From a Large Vertical Surface in a Horizontal Flow. SAND 83-8225, Sandia National Laboratories, Livermore CA.
-
-Awbi, H.B. & Hatton, A. 2000. Mixed convection from heated room surfaces, Energy and Buildings, 32, 153-166.
-
-Bejan, A. 1994. Convection Heat Transfer 2nd ed, Wiley, USA.
-
-### RoomAirflowNetwork Model
-
-#### Overview
-
-The RoomAirflowNetwork integrates the RoomAir model with the AirflowNetwork model. The model allows multiple Room Air nodes to be associated with AirflowNetwork intra zone nodes. The AirflowNetwork intra zone linkages provide links among the intra zone nodes and users may specify airflow components among these links. The AirflowNetwork model calculates airflows of the links. The incoming airflows are part of the zone heat and moisture balances of intra zone nodes. The model also allows users to specify a node to be connected to surfaces to have convective heat transfer and/or moisture transfer between surfaces and the node, portion of internal gains and supply air and return air fractions from zone equipment and AirLoop terminals.
-
-The input object RoomAirSettings:AirflowNetwork lists multiple RoomAirflowNetwork nodes in a zone. The input object of RoomAirflowNetwork:Node defines a list of connections assigned to a particular RoomAirflowNetwork node so that the connections will be used as components of node heat and moisture balance equations. In addition, the input objects AirflowNetwork:IntraZone:Node and AirflowNetwork:IntraZone:Linkage specify airflow nodes, linkages, and associated flow components, so that the AirflowNetwork model is used to calculate intrazone linkage airflows, which will be a part of loads for the RoomAir node balances.
-
-#### Model description
-
-The model calculates each component of the governing equations first. Then heat and moisture balance equations are solved to get the node temperature and humidity ratio at the current time step.
-
-Governing equations for each RoomAirflowNetwork node are described below:
-
-Energy balance equation
-
-<div>$${F_i}{C_{z,i}}\frac{{d{T_{z,i}}}}{{dt}} = \sum\limits_{j = 1}^{{N_{i,g}}} {{F_{gain,j}{\dot Q}_{i,j}}}  + \sum\limits_{j = 1}^{{N_{i,sur}}} {{h_{i,j}}} {A_j}\left( {{T_{s,j}} - {T_{z,i}}} \right) + \sum\limits_{j = 1}^{{N_{i,AFN}}} {{{\dot m}_{AFN i,j}}} {C_p}\left( {{T_{z,j}} - {T_{z,i}}} \right)\, + \sum\limits_{j = 1}^{{N_{i,HVAC}}} {{{F_{HVAC,j}}{\dot m}_{sup,i,j}}} {C_p}\left( {{T_{sup_j}} - {T_{z,i}}} \right)\ $$</div>
-
-where:
-
-F<sub>i</sub>	= Fraction of zone air volume for the ith node, defined in the Fraction of Zone Air Volume field of the RoomAir:Node:Airflownetwork
-
-C<sub>z,i</sub> 	= Volumetric heat capacity for the ith node: �<sub>air,i</sub>V C<sub>p</sub>C<sub>T</sub> 
-
-�<sub>air,i</sub> = Dry air density at the ith zone node 
-
-C<sub>p</sub> = zone dry air specific heat
-
-C<sub>T</sub> = sensible heat capacity multiplier (Detailed description is provided below)
-
-V	= Zone air volume
-
-T<sub>z,i</sub> 	= Air temperature at the ith zone RoomAir node
-
-N<sub>i,g</sub> 	= The number of internal gains for the ith node, defined in the RoomAir:Node:Airflownetwork:InternalGains object
-
-F<sub>gain,j</sub> 	= Fraction of internal gain from jth internal gain object defined in the RoomAir:Node:Airflownetwork:InternalGains object
-
-${\dot Q}_{i,j}$ 	= The amount of internal sensible gain at the jth internal gain object and ith node.
- 
-${\sum\limits_{j = 1}^{N_{i,g}} F_{gain,j}{\dot Q}_{i,j}}$ = The total amount of internal sensible gains assigned to the ith node
-
-N<sub>i,sur</sub> 	= The number of adjacent surface with convective heat transfer for the ith node, defined in the RoomAir:Node:Airflownetwork:AdjacentSurfaceList object
-
-h<sub>j</sub> 	= Heat transfer coefficient between the jth adjacent surface and ith node
-
-A<sub>j</sub> 	= Area of the jth adjacent surface
-
-T<sub>s,j</sub> 	= Inside temperature at the jth adjacent surface
-
-${\sum\limits_{j = 1}^{N_{i,sur}} h_{j} A_j \left( T_{s,j} - T_{z,i}\right)}$ 	= The total amount of convective gains from adjacent surfaces attached to the ith node
-
-N<sub>i,AFN</sub> 	= The number of RoomAir:Node:Airflownetwork objects connected to the ith node. The links are defined in AirflowNetwork:IntraZone:Linkage objects.
-
-${\dot m}_{AFN,i,j}$ 	= Mass flow rate from the jth node to the ith node. The flow rates are calculated in the AirflowNetwork model. It should be pointed out that the outgoing flows from the ith node will not be used in the present energy and moisture balance calculations, because they are a part of energy and moisture balances.
-
-T<sub>z,j</sub>  	= Air temperature at the jth zone RoomAir node
-
-${\sum\limits_{j = 1}^{N_{i,g}} \dot m_{AFN i,j} {C_p}\left( T_{z,j} - T_{z,i} \right)}$  = The total amount of heat transfer driven by intra zonal flows
-
-N<sub>i,HVAC</sub> 	= The number of RoomAir:Node:Airflownetwork:HVACEquipment objects which provide supply air to the ith node.
-
-F<sub>HVAC,j</sub> 	= Fraction of output or supply air to the ith node from jth HVAC equipment defined in RoomAir:Node:Airflownetwork:HVACEquipment objects
-
-${\dot m}_{sup,i,j}$ 	= The supply mass flow rate from the jth HVAC equipment
-
-T<sub>sup,j</sub>   = Supply air temperature at the jth HVAC equipment
-
-${\sum\limits_{j = 1}^{N_{i,HVAC}} F_{HVAC,j} \dot m_{sup,i,j} \left( T_{sup,j} - T_{z,i}\right)}$  	= The total amount of heat transfer from HVAC equipment to the ith node
-
-Moisture balance equation
-
-<div>$${F_i}{M_{z,i}}\frac{{d{W_{z,i}}}}{{dt}} = \sum\limits_{j = 1}^{{N_{i,g}}} {{F_{gain,j}{\dot Q}_{i,j}}}  + \sum\limits_{j = 1}^{{N_{i,sur}}} {{h_{M,j}}} {A_j}\left( {{W_{s,j}} - {W_{z,i}}} \right) + \sum\limits_{j = 1}^{{N_{i,AFN}}} {{{\dot m}_{AFN i,j}}} \left( {{W_{z,j}} - {W_{z,i}}} \right)\, + \sum\limits_{j = 1}^{{N_{i,HVAC}}} {{{F_{HVAC,j}}{\dot m}_{sup,i,j}}} \left( {{W_{sup_j}} - {W_{z,i}}} \right)\ $$</div>
-
-where:
-
-Fi	= Fraction of zone air volume for the ith node, defined in the Fraction of Zone Air Volume of the RoomAir:Node:Airflownetwork
-
-M<sub>z,i</sub> 	= Mass for the ith node: �<sub>air,i</sub>V<sub>Cp</sub>C<sub>T</sub>
-
-�<sub>air,i</sub> = Dry air density at the ith zone RoomAir node 
-
-V	= Zone air volume 
-
-W<sub>z,i</sub> 	= Air humidity ratio at the ith zone RoomAir node
-
-N<sub>i,g</sub> 	= The number of internal gains for the ith node, defined in the RoomAir:Node:Airflownetwork:InternalGains object
-
-F<sub>gain,j</sub> = Fraction of internal gain from jth internal gain object defined in the RoomAir:Node:Airflownetwork:InternalGains object
-
-${\dot Q}_{i,j}$  	= The amount of internal latent gain at the jth internal gain object and ith node. 
-
-${\sum\limits_{j = 1}^{N_{i,g}} F_{gain,j}{\dot Q}_{i,j}}$  = The total amount of internal latent gains attached to the ith node 
-
-N<sub>i,sur</sub> 	= The number of adjacent surface with convective heat transfer for the ith node, defined in the RoomAir:Node:Airflownetwork:AdjacentSurfaceList object
-
-h<sub>M,j</sub> = Mass transfer coefficient between the jth adjacent surface and ith node
-
-A<sub>j</sub> 	= Area of the jth adjacent surface
-
-W<sub>s,j</sub> 	= Inside humidity ratio at the jth adjacent surface
-
-${\sum\limits_{j = 1}^{N_{i,sur}} h_{M,j} A_j \left( W_{s,j} - W_{z,i}\right)}$ 	= The total amount of convective moisture gains from adjacent surfaces attached to the ith node
-
-N<sub>i,AFN</sub> 	= The number of RoomAir:Node:Airflownetwork objects connected to the ith node. The links are defined in AirflowNetwork:IntraZone:Linkage objects.
-
-${\dot m}_{AFN,i,j}$ 	= Mass flow rate from the jth node to the ith node. The flow rates are calculated in the AirflowNetwork model. It should be pointed out that the outgoing flow from the ith node will not be used in the present calculation, because they are a part of energy balance.
-
-W<sub>z,j</sub>  	= Air humidity ratio at the jth zone RoomAir node
-
-${\sum\limits_{j = 1}^{N_{i,AFN}} \dot m_{AFN,i,j} \left( W_{z,j} - W_{z,i}\right)}$  = The total amount of moisture transfer driven by intra zonal flows
-
-N<sub>i,HVAC</sub> 	= The number of RoomAir:Node:Airflownetwork:HVACEquipment objects which provide supply air to the ith node.
-
-F<sub>HVAC,j</sub> 	= Fraction of output or supply air to the ith node from jth HVAC equipment defined in RoomAir:Node:Airflownetwork:HVACEquipment objects
-
-${\dot m}_{sup,i,j}$  	= The supply mass flow rate from the jth HVAC equipment
-
-W<sub>sup,j</sub>   = Supply air humidity ratio at the jth HVAC equipment
-
-${\sum\limits_{j = 1}^{N_{i,HVAC}} F_{HVAC,j} \dot m_{sup,i,j} \left( W_{sup,j} - W_{z,i}\right)}$ 	= The total amount of moisture transfer from HVAC equipment to the ith node
-
-#### Calculation procedures
-
-The AirflowNetwork model is called first to calculate intrazone linkage air flows based on node temperatures and humidity ratios at the previous time step. The linkage loads are summarized based on each node with all incoming airflow, while any outgoing airflows from the node of the interest are excluded in the node energy and moisture balances. When the RoomAirModelAirflowNetowrk module is called, it summarizes internal gains at each node based on specification provided in the RoomAirflowNetwork:Node:InternalGains object, convective heat transfer from adjacent walls specified in the RoomAirflowNetwork:Node:AdjacentSurfaceList object. These load components are used in the predictor to predict system loads based on thermostat setpoint and supply fraction in the controlled zone node. In the corrector, the supply air conditions defined in the RoomAirflowNetwork:Node:HVACEquipment object are added. After all load components are assembled together, the node energy and moisture balance equations are solved. The node temperature and humidity ratio are calculated at the current time step.
- 
-
-AirflowNetwork Model
---------------------
-
-### Overview
-
-The AirflowNetwork model provides the ability to simulate the performance of an air distribution system, including supply and return leaks, and calculate multizone airflows driven by outdoor wind and forced air during HVAC system operation. The pressure and airflow model described here was developed based on AIRNET (Walton 1989). This detailed model is used to simulate thermal conduction and air leakage losses for constant volume air distribution systems (e.g., in residential or light commercial buildings). The multizone airflow calculations are performed at the HVAC system time step which, among other benefits,.allows for modeling hybrid ventilation systems.
-
-### Model Description
-
-The input object AirflowNetwork:SimulationControl provides access to the airflow network method, which consists of a set of nodes connected by airflow components through linkages. The objects AirflowNetwork:Multizone:Zone,  AirflowNetwork:Multizone:ExternalNode, and AirflowNetwork:Distribution:Node represent airflow nodes. The objects AirflowNetwork:Multizone:Surface and AirflowNetwork:Distribution:Linkage represent airflow linkages. The other objects with a relationship between pressure and airflow represent airflow components.
-
-The AirflowNetwork model consists of three sequential steps:
-
-* Pressure and airflow calculations
-
-* Node temperature and humidity calculations
-
-* Sensible and latent load calculations
-
-The pressure and airflow calculations determine pressure at each node and airflow through each linkage given wind pressures and forced airflows. Based on the airflow calculated for each linkage, the model then calculates node temperatures and humidity ratios given zone air temperatures and zone humidity ratios.  Using these node temperatures and humidity ratios, the sensible and latent loads from duct system conduction and leakage are summed for each zone. The sensible and latent loads obtained in this step are then used in the zone energy balance equations to predict HVAC system loads and to calculate the final zone air temperatures, humidity ratios, and pressures.
-
-The present AirflowNetwork model may only be applied to a single heating and cooling system that uses a single air distribution system (a single AirLoopHVAC object). The model excludes the impact of the air and duct system thermal capacitance. The impact of thermal capacity will be addressed in future upgrades to this model.
-
-### Pressure and Airflow Calculations
-
-The EnergyPlus airflow network consists of a set of nodes linked by airflow components. Therefore, it is a simplified airflow model, compared to detailed models such as those used in computational fluid dynamics (CFD) models. The node variable is pressure and the linkage variable is airflow rate. A brief description is presented below. A detailed description of the airflow network model may be found in the work of Walton (1989), Dols and Walton (2002), and Walton and Dols (2003).
-
-#### Initialization
-
-Newton’s method is used to solve for node air pressures and it requires an initial set of values for the node pressures. There are two initialization methods available. The first is linear initialization and equivalent to Initialization flag = 0. These initial values may be obtained by including in each airflow component a linear approximation relating airflow to pressure drop:
-
-<div>$$\mathop {{m_i}}\limits^ \bullet   = {C_i}\rho \left( {{\raise0.7ex\hbox{${\Delta {P_i}}$} \!\mathord{\left/ {\vphantom {{\Delta {P_i}} \mu }}\right.}\!\lower0.7ex\hbox{$\mu $}}} \right)$$</div>
-
-where
-
-<span>\(\mathop {{m_i}}\limits^ \bullet  \)</span> = Air mass flow rate at i-th linkage [kg/s]
-
-*C<sub>i</sub>*  = Air mass flow coefficient [m<sup>3</sup>]
-
-<span>\(\Delta P\)</span><sub>i                      </sub> = Pressure difference across the i-th linkage [Pa]
-
-*µ   *            = Air viscosity [Pa-s]
-
-This initialization handles stack effects very well and tends to establish the proper direction for the airflows. The linear approximation is provided by the laminar regime.
-
-The second initialization method assumes the initial pressures are zero and uses Newton’s method directly.
-
-#### Convergence criteria
-
-Conservation of air mass flow rate at each linkage provides the convergence criterion. When the sum of mass flow rates in all the linkages approaches zero within the convergence tolerance, the solution has converged. The solution is assumed to have converged when the sum is less than the convergence value, in order to reduce the number of iterations and obtain sufficient accuracy. There are two convergence criteria used in the AirflowNetwork model: Relative airflow convergence tolerance and Absolute airflow convergence tolerance.
-
-Relative airflow tolerance = <span>\(\frac{\left| \sum \dot m_i \right|}{\sum \dot m_i}\)</span>
-
-Absolute airflow tolerance = <span>\(\left| \sum \dot m_i \right|\)</span>
-
-The relative airflow tolerance is equivalent to the ratio of the absolute value of the sum of all network airflows to the sum of the network airflow magnitudes.  The absolute airflow tolerance is the summation of the absolute value of all network airflows. The solution has converged when both of these convergence criteria have been met.
-
-#### Linkage models
-
-A linkage used in the AirflowNetwork model has two nodes, inlet and outlet, and is linked by a component which has a relationship between airflow and pressure.  The pressure difference across each component in a linkage is assumed to be governed by Bernoulli’s equation:
-
-<div>$$\Delta P = \left( {Pn + \frac{{\rho V_n^2}}{2}} \right) - \left( {Pm + \frac{{\rho V_m^2}}{2}} \right) + \rho g\left( {zn - zm} \right)$$</div>
-
- where
-
-*ΔP*            = Total pressure difference between nodes n and m [Pa]
-
-*P<sub>n</sub>, P<sub>m</sub>*        = Entry and exit static pressures [Pa]
-
-*V<sub>n</sub>, V<sub>m</sub>*        = Entry and exit airflow velocities [m/s]
-
-*�   *         = Air density [kg/m<sup>3</sup>]
-
-*g*                = Acceleration due to gravity [9.81 m/s<sup>2</sup>]
-
-*z<sub>n</sub>, z<sub>m</sub>*          = Entry and exit elevations [m]
-
-By rearranging terms and adding wind pressure impacts, the above equation may be rewritten in the format used by the airflow network model:
-
-<div>$$\Delta P = {P_n} - {P_m} + {P_S} + {P_W}$$</div>
-
-where
-
-*P<sub>n</sub>, P<sub>m</sub>* <sub>              </sub> = Total pressures at nodes n and m [Pa]
-
-*P<sub>S</sub>*              = Pressure difference due to density and height differences [Pa]
-
-*P<sub>W </sub>*            = Pressure difference due to wind [Pa]
-
-The Input Output Reference provides the relationship between airflow and pressure for the most of the components (Ref.AirflowNetwork Model). The relationship between airflow and pressure for the AirflowNetwork:Multizone:Component:DetailedOpening, AirflowNetwork:Multizone:Component:SimpleOpening, and AirflowNetwork:Multizone:Component:HorizontalOpening objects are provided in detail in this reference.
-
-![](media/image2691.svg.png)
-
-Figure 147. The general problem of gravitational flow through a vertical opening
-
-The schematic drawing of a possible air flow pattern through a detailed vertical opening (AirflowNetwork:Multizone:Component:DetailedOpening) is shown in Figure 147. The equations used below are extracted from the COMIS Fundamentals manual (1990).
-
-The air density is assumed to be a linear function of height:
-
-<div>$${\rho_i}(z) = {\rho_{0i}} + {b_i}z$$</div>
-
-The pressure difference is assumed to be linear and simulate the effect of turbulence:
-
- <span>\(\Delta {P_t} = {P_{t0}} + {b_t}z\)</span>
-
-The reference pressures on each side are given at the bottom of the opening. By assuming the Bernoulli hypothesis on both sides, the pressure difference can be defined at any level of z as:
-
-<div>$${P_1}(z) - {P_2}(z) = ({P_{01}} - {P_{02}}) - g\left[ {({\rho_{01}}z + {b_1}{z^2}/2) - ({\rho_{02}}z + {b_2}{z^2}/2)} \right] + ({P_{t0}} + {b_t}z)$$</div>
-
-The velocity at any level z is given by
-
-<div>$$v(z) = \sqrt {2\frac{{{P_1}(z) - {P_2}(z)}}{\rho }} $$</div>
-
-The locations of the two possible neutral planes are given by an equilibrium in pressure which leads to a zero velocity point. By assuming the left terms in the equation above to be zero, one may have:
-
-<div>$$g({b_1} - {b_2}){z^2}/2 + \left[ {g({\rho_{01}} - {\rho_{02}}) - {b_t}} \right]z + ( - {P_{01}} + {P_{02}} - {P_{t0}}) = 0$$</div>
-
-This equation above can have two, one, or zero real solutions.  The zero solution represents a one-way flow through the opening and may be expressed in the following equation:
-
-<div>$$\dot m = {C_d}\theta \int\limits_{z = 0}^{z = H} {\rho \nu (z)Wdz} $$</div>
-
-The one real solution represents two-way (bi-directional) flow, which may be written in the following equations.
-
-<div>$${\dot m_{0,z1}} = {C_d}\theta \int\limits_{z = 0}^{z = z1} {\rho \nu (z)Wdz} $$</div>
-
-<div>$${\dot m_{z1,H}} = {C_d}\theta \int\limits_{z = z1}^{z = H} {\rho \nu (z)Wdz} $$</div>
-
-The two real solutions represent three-way flow, which may be written in the following equations.
-
-<div>$${\dot m_{z2,H}} = {C_d}\theta \int\limits_{z = z2}^{z = H} {\rho \nu (z)Wdz} $$</div>
-
-<div>$${\dot m_{z1,z2}} = {C_d}\theta \int\limits_{z = z1}^{z = z2} {\rho \nu (z)Wdz} $$</div>
-
-<div>$${\dot m_{z2,H}} = {C_d}\theta \int\limits_{z = z2}^{z = H} {\rho \nu (z)Wdz} $$</div>
-
-where
-
-*C<sub>d</sub>*  = discharge coefficient [dimensionless]
-
-*θ*    = Area reduction factor [dimensionless]
-
-*W*   = Opening width [m]
-
-The discharge coefficient, opening width, opening height, and start height factor are modulated based on opening factors. A detailed description of opening factor calculations may be found in the Input Output Reference (Ref. AirflowNetwork:Multizone:Zone, AirflowNetwork:Multizone:Surface, and
-
-AirflowNetwork:Multizone:Component:DetailedOpening).
-
-The above calculation procedure is used for a normal rectangular window. For a horizontally pivoted rectangular window, the calculation procedure is slightly different. A schematic drawing of a horizontally-pivoted window is shown in Figure 148.
-
-![PivotedWindow](media/image2703.png)
-
-Figure 148.  Schematic drawing of a horizontally-pivoted window
-
-The opening angle α (0-90°) is linearly proportional to the window opening factor (0-1.0). An opening factor of 1.0 is equal to an opening angle of 90°. The heights in the pivoted area are expressed as:
-
-<div>$$h2 = AxisHeight(1 - \cos (\alpha ))$$</div>
-
-<div>$$h4 = AxisHeight + (WindowHeight - AxisHeight)\cos (\alpha )$$</div>
-
-When z &lt; h2 or z &gt; h4, where z is the distance from the bottom of the window, the integration procedure is the same as the procedure for a normal rectangular window. When h2&lt;z&lt;h4, the window width W in the above equations is modified as:
-
- <span>\({W_{pivot}} = \sqrt {\frac{1}{{\frac{1}{{{W^2}}} + \frac{1}{{{{(2(AxisHeight - z)\tan (\alpha ))}^2}}}}}} \)</span>
-
-The mass flow rate in the pivoted area becomes:
-
-<div>$${\dot m_{pivot}} = {C_d}\theta \int\limits_{z = h2}^{z = h4} {\rho \nu (z){W_{pivot}}dz} $$</div>
-
-It should be pointed out that the discharge coefficient is modulated based on opening factors, while opening width, opening height, and start height factor do not apply for a horizontally-pivoted window. The actual window width and height are used to calculate airflows for a horizontally-pivoted window.
-
-The schematic drawing of air flow patterns through a simple vertical opening (AirflowNetwork:Multizone:Component:SimpleOpening) is shown in Figure 149. The equations used below are available from Walton (1989).
-
-![](media/image2708.svg.png)
-
-Figure 149. Schematic of large opening and associated three flow patterns
-
-The air density for each node is assumed to be constant. The hydrostatic equation is used to relate pressures at various heights for each node:
-
-<div>$$Pn\left( y \right) = {P_{0n}} - {\rho_n}gy$$</div>
-
-<div>$${P_m}(y) = {P_{0m}} - {\rho_m}gy$$</div>
-
-where
-
-*P<sub>0n</sub>, P<sub>0m</sub> = <sub> </sub>*pressure at nodes (zones) n and m at y = 0, the reference elevation of the opening [Pa]
-
-*�<sub>n</sub>, �<sub>m</sub><sub> </sub> =*air densities of zones n and m [kg/m<sup>3</sup>]
-
-*P<sub>n</sub>, P<sub>m</sub> =*reference pressures of zones n and m [Pa]
-
-It is assumed that the velocity of the airflow as a function of height is given by the orifice equation (Brown and Solvason 1962):
-
-<div>$$v(y) = {C_d}\sqrt {2\frac{{{P_n}(y) - {P_m}(y)}}{\rho }} $$</div>
-
- where
-
-*C<sub>d</sub>*<sub>  </sub>= discharge coefficient [dimensionless]
-
-*�*  = density of the air going through the opening [kg/m<sup>3</sup>]
-
-The neutral height, Y, where the velocity of the air is zero, may be calculated in the following equation:
-
-<div>$$Y = \frac{{{P_{on}} - {P_{0m}}}}{{g({\rho_n} - {\rho_m})}}\,\,\,\,\,\,\,\,or\,\,\,\,\,\,\,\frac{{{P_{om}} - {P_{0n}}}}{{g({\rho_m} - {\rho_n})}}$$</div>
-
-When the neutral plane is within the opening (first pattern in Figure 149), two-way (bi-directional) flows occur. The total flow through a large opening is the sum of both flows.
-
-<div>$${\dot m_{0,Y}} = {C_d}\theta \int\limits_{y = 0}^{y = Y} {\rho \nu (y)Wdy} $$</div>
-
-<div>$${\dot m_{Y,H}} = {C_d}\theta \int\limits_{y = Y}^{y = H} {\rho \nu (y)Wdy} $$</div>
-
-When the neutral plane is below or above the large opening (second and third pattern in Figure 149), one-way flow occurs.
-
-<div>$${\dot m_{}} = {C_d}\theta \int\limits_{y = 0}^{y = H} {\rho \nu (y)Wdy} $$</div>
-
-The opening width is modulated based on opening factors. A detailed description of opening factor calculations may be found in the Input Output Reference (Ref. AirflowNetwork:Multizone:Zone, AirflowNetwork:Multizone:Surface, and AirflowNetwork:Multizone:Component:DetailedOpening).
-
-The above two objects are used to simulate airflows across large vertical openings. The simple opening component (AirflowNetwork:Multizone:Component:SimpleOpening) assumes the pressure difference across the opening is a function of height varied from opening bottom to top, so that two-way flow may be obtained if appropriate (Walton 1989). The Detailed Opening component (AirflowNetwork:Multizone:Component:DetailedOpening) assumes both the pressure difference across the opening and air density are a function of height, so that three-way flow may be obtained (COMIS 1990). If these opening models would be used for horizontal openings, the pressure difference across the opening and air density remain constant, so that only one-way flow is possible using the detailed and simple opening components which are meant for vertical or near-vertical openings. In reality, there are two-way flows (air recirculation) across a large horizontal opening caused by buoyancy due to temperature and pressure difference and forced flow driven by air pressure difference only. Therefore, a horizontal opening component (AirflowNetwork:Multizone:Component:HorizontalOpening) is available to simulate airflows across large horizontal openings with the possibility of two-way flow by combining forced and buoyancy airflows together.
-
-The model for horizontal openings consists of forced airflow, buoyancy airflow, purge pressure and sloping plane. The model is mainly from a NIST report presented by Cooper (1989). The sloping plane (Bolmqvist and Sandberg 2004) portion of the model was added to allow for staircase simulations.
-
-For simplicity, a two zone building (upper and lower zones) connected by a large horizontal opening is used to describe the model, as shown in Figure 150. Forced and buoyancy airflows are described separately below.
-
-![AirflowNetwork-4](media/image2716.png)
-
-Figure 150. Air movements across a horizontal opening
-
-Forced airflows
-
-The air mass flow rate is determined by the pressure difference across the opening. The relationship between pressure and airflow is the same as AIRNET for a component (see AirflowNetwork:Multizone:Component:SimpleOpening description above). Since the height of the opening is constant, the forced airflow is unidirectional. A positive value for pressure difference indicates flow direction is from the lower zone to the upper zone across the opening, while a negative value represents flow in the opposite direction. The following description addresses forced air mass flow rates and partial derivatives for three possible scenarios of pressure difference:
-
-P<sub>L</sub> = P<sub>U</sub>
-
-<span>\({\dot m_U}\)</span>= <span>\({\dot m_L}\)</span>= 0
-
-where:
-
-P<sub>L</sub>               = Air pressure in the lower zone [Pa]
-
-P<sub>U</sub>              = Air pressure in the upper zone [Pa]
-
-<span>\({\dot m_U}\)</span>            = Air mass flow rate from the lower zone to the upper zone driven by forced airflow pressure difference [kg/s]
-
-<span>\({\dot m_L}\)</span>            = Air mass flow rate from the upper zone to the lower zone driven by forced airflow pressure difference [kg/s]
-
-1)           P<sub>L</sub> &gt; P<sub>U</sub>
-
-<span>\({\dot m_U}\)</span>= 0
-
-<div>$${\mathop m\limits^ \bullet_L} = {\rho_L}A{C_d}{\left( {\frac{{2\Delta P}}{{{\rho_{ave}}}}} \right)^{0.5}}$$</div>
-
-<div>$$\frac{{{{\mathop {\partial m}\limits^ \bullet  }_L}}}{{\partial {P_L}}} = {\rho_L}A{C_d}{\left( {\frac{1}{{2\Delta P{\rho_{ave}}}}} \right)^{0.5}}$$</div>
-
-where:
-
-�<sub>L</sub>   = Air density in the lower zone [kg/m<sup>3</sup>]
-
-A    = Opening area [m<sup>2</sup>]
-
-C<sub>d     </sub> = Discharge coefficient [Dimensionless]
-
-�<sub>ave</sub> = Average air density between the lower and upper zones [Pa]
-
-ΔP  = Pressure difference P<sub>L</sub> - P<sub>U</sub> [Pa]
-
-2)           P<sub>L</sub> &lt; P<sub>U</sub>
-
-<span>\({\mathop m\limits^ \bullet_{_L}}\)</span>= 0
-
-<div>$${\mathop m\limits^ \bullet_U} =  - {\rho_U}A{C_d}{\left( {\frac{{2\left| {\Delta P} \right|}}{{{\rho_{ave}}}}} \right)^{0.5}}$$</div>
-
-<div>$$\frac{{\partial \mathop {{m_U}}\limits^ \bullet  }}{{\partial {P_L}}} = {\rho_U}A{C_d}{\left( {\frac{1}{{2\left| {\Delta P} \right|{\rho_{ave}}}}} \right)^{0.5}}$$</div>
-
-where**:**
-
-�<sub>U</sub>   = Air density in the upper zone [kg/m<sup>3</sup>]
-
-A    = Opening area [m<sup>2</sup>]
-
-C<sub>d     </sub> = Discharge coefficient [Dimensionless]
-
-�<sub>ave</sub> = Average air density between the lower and upper zones [Pa]
-
-ΔP  = Pressure difference P<sub>L</sub> - P<sub>U</sub> [Pa]
-
-##### Buoyancy airflows
-
-Buoyancy flow only occurs when the air density in the upper zone is greater than the air density in the lower zone. The flow is bi-directional and the amount of upper flow is equal to the lower flow across the opening. The following discussion assumes the air density in the upper zone is greater than the air density in the lower zone. Otherwise, the buoyancy flow rate is equal to zero. It is also assumed that the maximum buoyancy flow occurs when the pressure difference across the opening due to forced airflows is zero. The maximum buoyancy flow may be expressed as a part of Cooper’s model:
-
-<div>$${\mathop m\limits^ \bullet_{buo,\max }} = {\rho_{ave}}*0.055{\left( {\frac{{g\left| {\Delta \rho } \right|D_{_H}^5}}{{{\rho_{ave}}}}} \right)^{0.5}}$$</div>
-
-where:
-
-<span>\({\mathop m\limits^ \bullet_{_{buo,\max }}}\)</span> = Buoyancy mass flow rate at zero forced airflow pressure difference [kg/s]
-
-g    = Gravity acceleration [m/s<sup>2</sup>]
-
-D<sub>H   </sub> = Hydraulic diameter [m]
-
-�<sub>ave</sub> = Average air density between the lower and upper zones [kg/m<sup>3</sup>]
-
-Δ�  = Density difference between the lower and upper zones [kg/m<sup>3</sup>]
-
-##### Combined airflows
-
-When forced and buoyancy flows co-exist, it is possible to have either unidirectional or bi-directional flows. For example, when the upward force due to pressure difference is greater than the buoyancy force (downward), unidirectional flow occurs. Bi-directional flow only occurs when the upward imposed force is less than the buoyancy force. The critical pressure between unidirectional and bi-directional flows is called the purge pressure (Tan and Jaluria 1992). The purge pressure is a function of opening geometry and the buoyancy force (ΔP/(gΔ�D<sub>H</sub>)) and may be expressed as (Cooper 1998):
-
-<div>$$\Delta {P_{Flood}} = \left| {C_{Shape}^2\frac{{g\Delta \rho D_H^5}}{{2{A^2}}}} \right|$$</div>
-
-where:
-
-ΔP<sub>Flood</sub> = Purging pressure [Pa]
-
-g    = Gravity acceleration [m/s<sup>2</sup>]
-
-D<sub>H   </sub> = Hydraulic diameter [m]
-
-A    = Opening area [m<sup>2</sup>]
-
-Δ�  = Density difference between the lower and upper zones [kg/m<sup>3</sup>]
-
-C<sub>Shape</sub> = Shape factor [dimensionless]
-
-<div>$$C_{Shape}^{} = \left\{ \begin{array}{l}0.754\;\;\;{\rm{for}}\;{\rm{a}}\;{\rm{circle}}\;{\rm{opening}}\\0.942(w/D)\;{\rm{for}}\;{\rm{a}}\;{\rm{rectangle}}\;{\rm{opening}}\end{array} \right\}$$</div>
-
-where:
-
-w    = Opening width [m]
-
-D    = Opening depth [m]
-
-As mentioned above, when the air pressure difference between two zones is zero there is the maximum bi-directional flow due to the buoyancy force. When the pressure difference increases from 0 and is less than |ΔP<sub>Flood</sub>|, there is some bi-directional flow across the opening, but less than the maximum flow. If the pressure difference keeps increasing and exceeds |ΔP<sub>Flood</sub>|, there is no bi-directional flow.  Cooper’s model assumes the buoyancy flow varies linearly with pressure difference.
-
-<div>$${\mathop m\limits^ \bullet_{buo}} = \left\{ \begin{array}{l}{\mathop m\limits^ \bullet_{buo,\max }}*\left( {1 - \frac{{\left| {\Delta P} \right|}}{{\left| {\Delta {P_{Flood}}} \right|}}} \right)\;\,\,If\;\Delta \rho  > 0\;and\;\frac{{\left| {\Delta P} \right|}}{{\left| {\Delta {P_{Flood}}} \right|}} &lt; 1\\0\;\,\,\,Otherwise\end{array} \right\}$$</div>
-
-The total air flow across the opening is based on superposition of the forced and buoyancy flows, and may be expressed for three different pressure difference scenarios as follows:
-
-a.                            P<sub>L</sub> = P<sub>U</sub>
-
-<div>$${\mathop m\limits^ \bullet_{_U}} = {\mathop m\limits^ \bullet_{buo}}$$</div>
-
-<div>$${\mathop m\limits^ \bullet_{_L}} = {\mathop m\limits^ \bullet_{buo}}$$</div>
-
-<div>$$\frac{{{{\mathop {\partial m}\limits^ \bullet  }_L}}}{{\partial {P_L}}} = 0$$</div>
-
-b.                           P<sub>L</sub> &gt; P<sub>U</sub>
-
-<div>$${\mathop m\limits^ \bullet_{_U}} = {\mathop m\limits^ \bullet_{buo}}$$</div>
-
-<div>$${\mathop m\limits^ \bullet_L} = {\rho_L}A{C_d}{\left( {\frac{{2\Delta P}}{{{\rho_{ave}}}}} \right)^{0.5}} + {\mathop m\limits^ \bullet_{buo}}$$</div>
-
-<div>$$\frac{{{{\mathop {\partial m}\limits^ \bullet  }_L}}}{{\partial {P_L}}} = {\rho_L}A{C_d}{\left( {\frac{1}{{2\Delta P{\rho_{ave}}}}} \right)^{0.5}} - \frac{{{{\mathop m\limits^ \bullet  }_{buo,\max }}}}{{\left| {\Delta {P_{Flood}}} \right|}}$$</div>
-
-where:
-
-�<sub>L</sub>   = Air density in the lower zone [kg/m<sup>3</sup>]
-
-A    = Opening area [m<sup>2</sup>]
-
-C<sub>d     </sub> = Discharge coefficient [dimensionless]
-
-Ρ<sub>ave</sub> = Average air density between the lower and upper zones [Pa]
-
-ΔP  = Pressure difference P<sub>L</sub> - P<sub>U</sub> [Pa]
-
-c.                            P<sub>L</sub> &lt; P<sub>U</sub>
-
-<div>$${\mathop m\limits^ \bullet_{_L}} = {\mathop m\limits^ \bullet_{buo}}$$</div>
-
-<div>$${\mathop m\limits^ \bullet_U} =  - {\rho_U}A{C_d}{\left( {\frac{{2\left| {\Delta P} \right|}}{{{\rho_{ave}}}}} \right)^{0.5}} + {\mathop m\limits^ \bullet_{buo}}$$</div>
-
-<div>$$\frac{{\partial \mathop {{m_U}}\limits^ \bullet  }}{{\partial {P_L}}} = {\rho_U}A{C_d}{\left( {\frac{1}{{2\left| {\Delta P} \right|{\rho_{ave}}}}} \right)^{0.5}} + \frac{{{{\mathop m\limits^ \bullet  }_{buo,\max }}}}{{\left| {\Delta {P_{Flood}}} \right|}}$$</div>
-
-*Sloping plane*
-
-![](media/image2741.png)
-
-Figure 151. A Staircase is attached to the horizontal opening.
-
-When a staircase is introduced as shown in Figure 151, the effective opening area will be used to replace A (opening area) in the above equations. The effective area may be estimated as (Bolmqvist and Sandberg 2004):
-
-<div>$${A_{eff}} = A\sin \alpha (1 + \cos \alpha )$$</div>
-
-where:
-
-A<sub>eff</sub>  = Effective area of horizontal opening [m<sup>2</sup>]
-
-A    = Area of horizontal opening [m<sup>2</sup>]
-
-α    = Angle between the stair plane and horizontal opening plane [degrees]
-
-Note: the hydraulic diameter calculation is based on the effective opening area, while the opening depth remains the same.
-
-Figure 152 demonstrates possible forced and buoyancy flow rates at different ratios of pressure difference to purging pressure across a horizontal opening when the upper zone air density is greater than the lower zone air density. The pressure difference is the lower zone pressure minus the upper zone pressure. Otherwise, the buoyancy flow is zero. In addition, when the absolute ratio is above 1, the buoyancy flow is also zero. The following table provides a brief description for the legend listed in Figure 152.
-
-Table 49.  Legend Description
-
-<table class="table table-striped">
-<tr>
-<th>Legend</th>
-<th>Description</th>
-* </tr>
-<tr>
-<td>Forced downward</td>
-<td>Forced flow rate from upper to lower at P<sub>L</sub>-P<sub>U</sub> &lt; 0</td>
-</tr>
-<tr>
-<td>Forced upward</td>
-<td>Forced flow rate from lower to upper at P<sub>L</sub>-P<sub>U</sub> &gt; 0</td>
-</tr>
-<tr>
-<td>Buoyancy upward</td>
-<td>Total upward flow rate due to buoyancy only at P<sub>L</sub>-P<sub>U</sub> &lt; 0</td>
-</tr>
-<tr>
-<td>Buoyancy downward</td>
-<td>Total downward flow rate due to buoyancy only at P<sub>L</sub>-P<sub>U</sub> &gt; 0</td>
-</tr>
-<tr>
-<td>Combined downward</td>
-<td>Total downward flow at P<sub>L</sub>-P<sub>U</sub> &lt; 0 (Forced downward + buoyancy upward)</td>
-</tr>
-<tr>
-<td>Combined upward</td>
-<td>Total upward flow at P<sub>L</sub>-P<sub>U</sub> &gt; 0 (Forced upward + buoyancy downward)</td>
-</tr>
-
-</table>
-
-![](media/image2743.svg.png)
-
-Figure 152. Flow rates at different pressure differences
-
-#### Wind pressure calculations
-
-The wind pressure is determined by Bernoulli’s equation, assuming no height change or pressure losses:
-
-<div>$${p_w} = {C_p}\rho \frac{{{V_{ref}}^2}}{2}$$</div>
-
-where:
-
-*p<sub>w  </sub>*            = Wind surface pressure relative to static pressure in undisturbed flow [Pa]
-
-*�*                = Air density [kg/m<sup>3</sup>]
-
-*V<sub>ref</sub>*             = Reference wind speed at local height [m/s]
-
-*C<sub>p</sub>*              = Wind surface pressure coefficient [dimensionless]
-
-*V<sub>ref</sub>* may be expressed as (Ref, Local Wind Speed Calculations):
-
-<div>$${V_{ref}} = {V_{met}}{\left( {\frac{{{\delta_{met}}}}{{{z_{met}}}}} \right)^{{\alpha_{met}}}}{\left( {\frac{z}{\delta }} \right)^\alpha }$$</div>
-
-*C<sub>p</sub>* is a function of location on the building envelope and wind direction. When Wind Pressure Coefficient Type = “INPUT�, the*C<sub>p</sub>* values are explicitly defined in the input for AirflowNetwork:Multizone:Wind Pressure Coefficient Values. When Wind Pressure Coefficient Type = “AVERAGE-SURFACE CALCULATION� and the building shape is rectangular, the program uses the following equations to calculate wind pressure coefficient (*C<sub>p</sub>*) values for different wind directions. For a low rise building, the normalized surface pressure coefficient may be written as (Swami and Chandra 1988):
-
-<div>$${C_{p,n}} = 0.6*\ln \left[ \begin{array}{l}1.248 - 0.703\sin (\alpha /2) - 1.175{\sin ^2}(\alpha ) + 0.131{\sin ^3}(2\alpha G)\\ + \,0.769\cos (\alpha /2) + 0.07{G^2}{\sin ^2}(\alpha /2) + 0.717{\cos ^2}(\alpha /2)\end{array} \right]$$</div>
-
-where
-
-*C<sub>p,n</sub>*            = *C<sub>p</sub>* value at a given angle between wind direction and the outward normal of the surface under consideration [dimensionless]
-
-α                = Angle between wind direction and outward normal of wall under consideration [deg]
-
-*G*               = Natural log of the ratio of the width of the wall under consideration to the width of the adjacent wall [dimensionless]
-
-*n*                = Index of incident angle at 30-degree increments
-
-For walls of a high rise building, a two-dimensional array of surface-averaged wind pressure coefficients is generated based on wind incident angle and side ratio. The wind pressure coefficients are provided in 2001 ASHRAE Fundamentals Handbook, p. 16.5, Fig. 7, “Surface Averaged Wall Pressure Coefficients for Tall Buildings�. The original work was performed by Atkins et al. (1979). The incident angle has an increment of 30 degrees. The side ratio values are 0.25, 1.0, and 4.0. For a given incident angle and building aspect ratio, the program uses linear interpolation to calculate the corresponding wind pressure coefficient *C<sub>p,n</sub>*.
-
-For the roof of a high rise building, a two-dimensional array of surface-averaged wind pressure coefficients is also generated based on wind incident angle and side ratio. The wind pressure coefficients are provided in 2001 ASHRAE Fundamentals Handbook, p. 16.6, Fig. 9, “Surface Averaged Roof Pressure Coefficients for Tall Buildings�. The original work was performed by Holmes (1986). The incident angle has an increment of 30 degrees. The side ratio values are 0.25, 1.0, and 4.0. At a given wind incident angle and building aspect ratio, the program uses linear interpolation to calculate the corresponding wind pressure coefficient *C<sub>p,n</sub>*.
-
-The wind surface pressure at the given incident angle can be calculated by combining the above two equations:
-
-<div>$${p_{w,n}} = {C_{p,n}}\rho \frac{{{V_{ref}}^2}}{2}$$</div>
-
-#### Solution method
-
-Based on the relationship between airflow rate and pressure drop for each component, a system of equations for all components can be assembled together in an n x n square matrix, where n is the number of nodes. Newton’s method is used to iteratively solve for the air pressure at each node. A new estimated vector for all node pressures, {P}\*, is computed from the current estimated vector of node pressures, {P}, by:
-
-<div>$${\left\{ P \right\}^*} = \left\{ P \right\} - \left\{ C \right\}$$</div>
-
-where the correction vector, {C}, is computed by the matrix relationship:
-
-<div>$$\left[ J \right]\left\{ C \right\} = \left\{ B \right\}$$</div>
-
-{B} is a column vector with each component given by:
-
-<div>$${B_n} = \sum\limits_i {\mathop {{m_i}}\limits^ \bullet  } $$</div>
-
-where n is the node number and i indicates all flow paths connecting node n to other nodes, and [J] is the square Jacobian matrix whose elements are given by:
-
-<div>$${J_{n,m}} = \sum\limits_i {\frac{{\partial \mathop m\limits^ \bullet  }}{{\partial {P_m}}}} $$</div>
-
-#### Convergence acceleration
-
-The convergence tolerance is used to check the sum of the mass flow rates by applying mass conservation. The convergence acceleration equation shown below is used to correct the node pressures to more rapidly obtain a solution. By assuming a constant ratio of correction values from one iteration to the next, the following method is applied:
-
-<div>$${P_n}^* = {P_n} - {C_n}/(1 - r)$$</div>
-
-where
-
-*r*     = the ratio of C<sub>n</sub> for the current iteration to its value for the previous iteration [dimensionless]
-
-*C<sub>n</sub>*  = Correction value at the n<sub>th</sub> node [Pa]
-
-*P<sub>n</sub>* <sub>   </sub> = Estimated pressure at the n<sub>th</sub> node [Pa]
-
-*P<sub>n</sub><sup>\*</sup><sub></sub>*<sub>  </sub> = Corrected pressure at the n<sub>th</sub> node used in the next iteration [Pa]
-
-This method is similar to a Steffensen iteration (Conte and de Boor 1972) which is used as a fixed-point iteration method for individual nonlinear equations.
-
-The iteration correction method presented in the above equation gives a variable factor. When the solution is close to convergence, the solution method converges quadratically. By limiting cases where the value of r is less than some value, such as -0.5, the solution will not interfere with the rapid convergence. It has not been proven that the convergence acceleration equation will always lead to convergence, but it can be shown that it will not prevent convergence. Newton’s method converges when the estimated solution values are within some distance, called the radius of convergence, or the correct solution. Applying the convergence acceleration equation when -1 &lt; r &lt;0, will cause a smaller correction than Newton’s method, which therefore, can not force the iterations outside the radius of convergence. When r&lt;-1, the solution diverges in an oscillatory fashion. When r&gt;1, the solution also diverges, but in a nonoscillatory manner. For 0&lt;r&lt;1, the solution is approached from one direction. In all three cases, the convergence acceleration equation applies as long as r is truly constant over several iterations. However, for the last case, this involves a true extrapolation of correction factor which is very sensitive to the accuracy of r. This is most extreme for the case of r=1, which would cause an infinite correction.
-
-### Node Temperature Calculations
-
-A brief description of the air node temperature calculation is given below. A detailed description can be found in the work of Swami et al. (1992). The following equation is used to calculate temperature distribution across a duct element at the given airflow rate and inlet air temperature:
-
-<div>$$\mathop m\limits^ \bullet  {C_p}\frac{{dT}}{{dx}} = UP(T{}_\infty  - T)$$</div>
-
-where
-
-*C<sub>p</sub>*  = Specific heat of airflow [J/kg•K]
-
-<span>\(\mathop m\limits^ \bullet  \)</span>  = Airflow rate [kg/s]
-
-*P*    = Perimeter of a duct element [m]
-
-*T*    = Temperature as a field variable [°C]
-
-<span>\(T{}_\infty \)</span>            = Temperature of air surrounding the duct element [°C]
-
-*U*   = Overall heat transfer coefficient [W/m<sup>2</sup>•K]
-
-<div>$$U = \frac{1}{{\frac{1}{{{h_i}}} + \frac{1}{{{h_o}}} + \sum {\frac{{{t_j}}}{{{k_j}}}} }}$$</div>
-
-*h<sub>i</sub>*         = Inside heat transfer coefficient [W/m<sup>2</sup>•K]
-
-*h<sub>o</sub>*<sub>                 </sub> = Outside heat transfer coefficient [W/m<sup>2</sup>•K]
-
-*t<sub>j</sub>*          = Thickness at j-th layer [m]
-
-*k<sub>j</sub>*          = Thermal conductivity at j-th layer [W/m•K]
-
-
-
-The outlet air temperature at the end of the duct (x=L) is:
-
-<div>$${T_o} = {T_\infty } + ({T_i} - {T_\infty })*\exp \left( { - \frac{{UA}}{{\mathop {m{C_p}}\limits^ \bullet  }}} \right)$$</div>
-
-where
-
-      *T<sub>i</sub>*         = Inlet air temperature [°C]
-
-      *T<sub>o</sub>*         = Outlet air temperature [°C]
-
-      *T<sub>∞</sub>*        = Temperature of air surrounding the duct element [°C]
-
-      *A*          = Surface area (Perimeter \* Length) [m<sup>2</sup>]
-
-
-
-The heat transfer by convection to ambient, *Q*, is:
-
-<div>$$Q = \mathop m\limits^ \bullet  {C_p}({T_\infty } - {T_i})\left[ {1 - \exp \left( { - \frac{{UA}}{{\mathop {m{C_p}}\limits^ \bullet  }}} \right)} \right]$$</div>
-
-The outlet air temperature can be calculated using the above equation at the given inlet air temperature. Since the inlet temperature at one linkage is the outlet temperature for the connected linkage, the outlet air temperatures at all nodes are solved simultaneously. A square linear system assembled by the AirflowNetwork model is expressed below:
-
-<div>$$\{ M\} [T] = [B]$$</div>
-
-where
-
-      {M}       = Airflow matrix
-
-      [T]        = Temperature vector
-
-      [B]        = Given boundary conditions
-
-The zone air temperatures and primary air loop component (fan and coils) outlet conditions are used as prescribed conditions in the AirflowNetwork model. In addition, the temperature difference across zone loop components (terminal units) is held constant during the calculations. For example, thermal zone temperatures calculated during the previous system time step are used as prescribed temperatures when calculating all other node temperatures. The zone air temperature is assumed constant (prescribed) throughout the AirflowNetwork iterative solution. The fan and coil outlet air temperatures, and terminal unit temperature differences are assumed constant within an AirflowNetwork iteration. The sensible heat gains calculated during the AirflowNetwork solution are then used to predict a new zone air temperature.
-
-### Node Humidity Ratio Calculations
-
-A brief description of the air node humidity ratio calculation is given below. A detailed description can found in the work of Swami et al. (1992). The following equation is used to calculate humidity ratio distribution across a duct element at the given airflow rate and inlet air humidity ratio:
-
-<div>$$\mathop m\limits^ \bullet  \frac{{dW}}{{dx}} = {U_m}P(W{}_\infty  - W)$$</div>
-
-where
-
-<span>\(\mathop m\limits^ \bullet  \)</span>             = Airflow rate [kg/s]
-
-*P   *            = Perimeter of a duct element [m]
-
-*W  *            = Humidity ratio [kg/kg]
-
-<span>\(W{}_\infty \)</span>           = Humidity ratio of air surrounding the duct element [kg/kg]
-
-*U<sub>m</sub>*             = Overall moisture transfer coefficient [kg/m<sup>2</sup>•s]
-
-<div>$${U_m} = \frac{1}{{\frac{1}{{{h_{m,i}}}} + \frac{1}{{{h_{m,o}}}} + \sum {\frac{{{t_j}}}{{{D_j}}}} }}$$</div>
-
-*h<sub>m,i</sub>* <sub>                        </sub>             = Inside moisture transfer coefficient [kg/m<sup>2</sup>•s]
-
-*h<sub>m,o               </sub>*<sub>                       </sub> = Outside moisture transfer coefficient [kg/m<sup>2</sup>•s]
-
-*t<sub>j</sub>*                = Thickness at j-th layer [m]
-
-D<sub>j</sub>               = Moisture diffusivity at j-th layer [kg/m•s]
-
-The outlet air humidity ratio at the end of the duct (x=L) is:
-
-<div>$${W_o} = {W_\infty } + ({W_i} - {W_\infty })*\exp \left( { - \frac{{{U_m}A}}{{\mathop m\limits^ \bullet  }}} \right)$$</div>
-
-where
-
-*W<sub>i</sub>*              = Inlet air humidity ratio [kg/kg]
-
-*W<sub>o </sub>*            = Outlet air humidity ratio [kg/kg]
-
-*A*                = Surface area (Perimeter \* Length) [m<sup>2</sup>]
-
-The moisture transfer by convection to ambient, *Q<sub>m</sub>*, is
-
-<div>$${Q_m} = \mathop m\limits^ \bullet  ({W_\infty } - {W_i})\left[ {1 - \exp \left( { - \frac{{{U_m}A}}{{\mathop m\limits^ \bullet  }}} \right)} \right]$$</div>
-
-The outlet air humidity ratio can be calculated using the above equation at the given inlet air humidity ratio. Since the inlet humidity ratio at one linkage is the outlet humidity ratio for the connected linkage, the outlet air humidity ratio at all nodes are solved simultaneously. A square linear system assembled by the AirflowNetwork model is expressed below:
-
-<div>$$\{ {M_m}\} [W] = [{B_m}]$$</div>
-
-where
-
-{M<sub>m</sub>}            = Airflow matrix
-
-[W]             = Humidity ratio vector
-
-[B<sub>m</sub>]                        = Given boundary conditions
-
-The zone air humidity ratios and primary air loop component (fan and coils) outlet conditions are used as prescribed conditions in the AirflowNetwork model. For example, thermal zone humidity ratios calculated during the previous system time step are used as prescribed humidity ratios when calculating all other node humidity ratios. The zone air humidity ratio is assumed constant (prescribed) throughout the AirflowNetwork iterative solution. The coil outlet air humidity ratio is assumed constant within an AirflowNetwork iteration. The latent heat gains calculated during the AirflowNetwork solution are then used to predict a new zone air humidity ratio.
-
-### Sensible and Latent Load Calculations
-
-The zone sensible and latent loads calculated in the AirflowNetwork model consist of multizone, duct conduction and leakage. In addition, the impact of infiltration and mixing is accounted for in this calculation. The multizone load only includes incoming airflows from outside (infiltration) and other adjacent zones (mixing) with and without forced-air fan operation. It is divided into two terms: variable and constant. The constant term is the sum of the mass flow rate multiplied by the specific heat for both infiltration and mixing. The variable term includes the impact of zone and outdoor air temperature. Each of these terms is used in the zone energy balance equation. The sensible load items from the multizone load calculations may be written as follows:
-
-<div>$$MC{P_{airflow}} = \mathop {{m_{\inf }}}\limits^\cdot  {C_p} + \sum {\left( {\mathop {{m_{mix}}}\limits^\cdot  {C_p}} \right)} $$</div>
-
-<div>$$MCP{T_{airflow}} = \mathop {{m_{\inf }}}\limits^\cdot  {C_p}{T_{amb}} + \sum {\left( {\mathop {{m_{mix}}}\limits^\cdot  {C_p}{T_{zone}}} \right)} $$</div>
-
-where
-
-*MCP<sub>airflow</sub>* = Sum of air mass flow rate multiplied by specific heat for infiltration and mixing [W/K]
-
-*MCPT<sub>airflow</sub>* = Sum of air mass flow rate multiplied by specific heat and temperature for infiltration and mixing [W]
-
-<span>\({\mathop m\limits^\cdot_{\inf }}\)</span>           = Incoming air mass flow rate from outdoors [kg/s]
-
-<span>\({\mathop m\limits^\cdot_{mix}}\)</span>          = Incoming air mass flow rate from adjacent zones [kg/s]
-
-*T<sub>amb</sub>*            = Outdoor air dry-bulb temperature [°C]
-
-*T<sub>zone</sub>*           = Adjacent zone air temperature [°C]
-
-The latent load items from multizone load calculations may be written as follows:
-
-<div>$${M_{airflow}} = \mathop {{m_{\inf }}}\limits^\cdot   + \sum {\mathop {{m_{mix}}}\limits^\cdot  } $$</div>
-
-<div>$$M{W_{airflow}} = \mathop {{m_{\inf }}}\limits^\cdot  {W_{amb}} + \sum {\mathop {{m_{mix}}}\limits^\cdot  } {W_{zone}}$$</div>
-
-where
-
-*M<sub>airflow</sub>* = Sum of air mass flow rates for infiltration and mixing [kg/s]
-
-*MW<sub>airflow</sub>* = Sum of air mass flow rate multiplied by humidity ratio for infiltration and mixing [kg/s]
-
-<span>\({\mathop m\limits^\cdot_{\inf }}\)</span>           = Incoming air mass flow rate from outdoors [kg/s]
-
-<span>\({\mathop m\limits^\cdot_{mix}}\)</span>          = Incoming air mass flow rate from adjacent zones [kg/s]
-
-*W<sub>amb</sub>*           = Outdoor air humidity ratio [kg/kg]
-
-*W<sub>zone</sub>*          = Adjacent zone air humidity ratio [kg/kg]
-
-The air distribution system (ADS) loads due to duct conduction and leakage depend on the air distribution system component (e.g., duct) location. The air distribution system sensible and latent loads are calculated for each zone as follows:
-
-<div>$${Q_{ADS,i}} = \sum\limits_j {{Q_{cond(i,j)}} + } \sum\limits_j {{Q_{leak(i,j)}}} $$</div>
-
-<div>$${Q_{ADS,m,i}} = \sum\limits_j {{Q_{cond,m(i,j)}} + } \sum\limits_j {{Q_{leak,m(i,j)}}} $$</div>
-
-where
-
-*Q<sub>ADS,i</sub>*         = Total sensible load in the i-th zone due to ADS losses [W]
-
-*Q<sub>cond(ij)</sub>*       = Duct wall conduction loss at the j-th duct located in the i-th zone [W]
-
-*Q<sub>leak(ij)</sub>*        = Sensible supply leak loss at the j-th linkage located in the i-th zone [W]
-
-*Q<sub>ADS,m,i</sub>*       = Total latent load in the i-th zone due to ADS losses [kg/s]
-
-*Q<sub>cond,m(ij)</sub>*= Duct wall vapor diffusion loss at the j-th duct located in the i-th zone [kg/s]
-
-*Q<sub>leak,m(ij)</sub>* = Latent supply leak loss at the j-th linkage located in the i-th zone [kg/s]
-
-### Impacts of Supply Air Constant Volume Fan Control on Load: Cycling vs. Continuous
-
-The AirflowNetwork model currently allows two types of constant volume fans: Fan:ConstantVolume and Fan:OnOff. The Fan:ConstantVolume object has only one type of supply air fan operation mode: continuous fan, cycling compressor (ContinuousFanWithCyclingCompressor). However, the Fan:OnOff has two types of supply air fan operation modes: cycling fan, cycling compressor (CyclingFanAndCompressor) or continuous fan, cycling compressor (ContinuousFanWithCyclingCompressor). The CyclingFanAndCompressor operation mode is frequently referred to as “AUTO fan�, where the compressor(s) and supply air fan operate in unison to meet the zone heating or cooling load, and cycle off together when the heating or cooling load has been met. The ContinuousFanWithCyclingCompressor operation mode is often referred to as “fan ON�, where the compressor(s) cycle on and off to meet the zone heating or cooling load but the supply air fan operates continuously regardless of compressor operation. The supply air fan operation mode is specified in an HVAC system object based on a given fan operation mode schedule (e.g., AirLoopHVAC:UnitaryHeatCool object).
-
-The determination of the zone sensible and latent loads caused by multizone airflows and forced air distribution system operation is dependent on the supply air fan operation mode (see Sensible and Latent Load Calculations section above). The zone loads calculated by the AirflowNetwork model are added to zone sensible and latent balances in the ZonePredictorCorrector module to calculate zone air temperatures and humidity ratios (see Integration of the AirflowNetwork Model section below). For the case of continuous fan/cycling compressor, the zone loads during forced air distribution system operation are calculated with the system design air mass flow rate without modification, since the system air node conditions (temperature and humidity) reflect the average values for the time step considering the coil/fan on and off periods during the time step.
-
-For the case of cycling fan/cycling compressor, where the forced air distribution system can operate for a portion of the simulation time step, the airflows are determined based on the air distribution system part-load ratio (ratio of the average air mass flow rate for the time step divided by the design air mass flow rate). The **airflows** for the AirflowNetwork:Distribution:Linkage objects are reported during the air distribution system on cycle, since no airflow is assumed during the system off cycle. The **airflows** for the AirflowNetwork:Multizone:Surface objects are weighted by the air distribution system part-load ratio. The **zone loads** are the sum of energy losses during both the air distribution system on and off cycle at each system time step. The energy losses when the air distribution system is on are calculated using the system “on� air flow rate multiplied by the air distribution system run time fraction. The energy losses when the air distribution system is off are obtained from the multizone airflow calculations (without forced air through the air distribution system) and these losses are multiplied by (1.0 - system run time fraction), assuming no airflows through the air distribution system when the fan is off. The formulas used to calculate airflows and zone loads are given below:
-
-Airflow
-
-Airflow = Airflow during ADS on cycle \* ADS Part-load ratio + Airflow during ADS off cycle \* (1.0 – ADS Part-load ratio)
-
-where ADS = Air Distribution System
-
-Zone load
-
-System run time fraction = Maximum run time fraction of coils and fans in the air distribution system
-
-Zone energy losses = Zone energy loss during ADS on cycle \* System run time fraction + Zone energy loss during ADS off cycle \* (1.0 - System run time fraction)
-
-The calculation of loads due to multizone airflow, without forced air distribution system operation, is performed when the HVAC system is first simulated during a simulation time step (FirstHVACIteration = True). The calculation of loads due to air distribution system operation is performed on subsequent iterations within the same simulation time step when the mass flow rate at the supply air fan inlet is greater than 0.0 (and FirstHVACIteration = False).
-
-### Airflow Calculation Procedure using A Supply Variable Air Volume Fan
-
-The AirflowNetwork model currently also allows a variable air volume fan type as Fan:VariableVolume. The allowed terminal type is AirTerminal:SingleDuct:VAV:Reheat only. Other types of terminals will be added later.
-
-In general, the supply fan air flow rate in a VAV central system is determined by a sum of terminal flow rates when the AirflowNetwork model is not applied. When the AirflowNetwork model is applied and the supply air fan flow rate is given, each terminal flow is determined by pressure resistance of each supply air pathway. It is possible that the delivered air flow rate from the pressure resistance at each terminal may be totally different from the desired flow rate determined by terminal units. Therefore, it is not easy to meet both requirements. The following compromised approach, including possible supply and return leaks in an air distribution system, is implemented.
-
-1. Set up terminal airflows in the AirflowNetwork module based on the SimVAV subroutine in the HVACSingleDuctSystem module.
-
-2.    Require AirflowNetwork:Distribution:Component:LeakageRatio objects to define supply leaks, so that the values of the Effective Leakage Ratio field are used to decide the supply fan flow rates. The base of the ratio will be actual supply fan flow rate, instead of the maximum fan flow rate used in the constant volume fan systems.
-
-3.    Assign the supply fan airflow rate based on the sum of all terminal flow rates and all supply leak ratios until it reaches the maximum fan flow rate
-
-<div>$${\dot m_{fan}} = \frac{{\mathop \sum \nolimits_i^n {{\dot m}_{i,terminal}}}}{{1 - \mathop \sum \nolimits_j^k {F_j}}}$$</div>
-
-where
-
-<span>\({\dot m_{fan}}\)</span>          = The supply fan flow rate
-
-<span>\({\dot m_{i,terminal}}\)</span>    = The flow rate at the ith terminal, which is determined in the subroutine SimVAV in the HVACSingleDuctSystem module
-
-n    = Number of terminals
-
-<span>\({F_j}\)</span> = The fraction of the supply fan flow rate at the jth supply leak, given in the AirflowNetwork:Distribution:Component:LeakageRatio objects.
-
-k    = Number of supply leaks
-
-4.    If the calculated supply fan flow rate is above the maximum limit of the supply fan flow rate, and the supply leak ratios remain the same, the supply fan flow rate is set to the maximum limit, and the terminal flow rates are reduced proportionally weighted by a ratio of the maximum supply fan flow rate by input to the calculated supply fan flow rate. Therefore, a sum of all terminal rates and all supply leak rates is equal to the maximum supply fan rate. *** ***
-
-<div>$$R = \frac{{{{\dot m}_{fan,max}}}}{{{{\dot m}_{fan,cal}}}}$$</div>
-
-<div>$${\dot m_{i,terminal,final}} = {\dot m_{i,terminal}}*R$$</div>
-
-where
-
-R    = The ratio of the maximum fan flow rate given in the inputs to the requested fan flow rate based on the above equation
-
-<span>\({\dot m_{fan,max}}\)</span>      = The maximum supply fan flow rate by input
-
-<span>\({\dot m_{fan,cal}}\)</span>       = The calculated supply fan flow rate
-
-<span>\({\dot m_{i,terminal,final}}\)</span>           = The final flow rate at each terminal adjusted by the ratio
-
-### Airflow Calculation Procedure using inputs of Intrazone nodes and linkages 
-
-The inputs of both AirflowNetwork:IntraZone:Node and AirflowNetwork:IntraZone:Linkage objects are treated as normal model nodes and linkages. Therefore, the calculation procedures are the same as above. 
-
-
-### Integration of the AirflowNetwork Model
-
-The loads calculated by the AirflowNetwork model are integrated into the EnergyPlus heat balance equation in a similar manner as described elsewhere in this document in the section “Basis for the Zone and System Integration�. The mass flow rate summations and sensible and latent loads described in the previous section are included in the calculation of zone temperature and humidity ratio.
-
-The revised zone temperature update equation becomes:
-
-<div>$$T_z^t = \frac{{\sum\limits_{i = 1}^{{N_{sl}}} {\mathop {{Q_i}}\limits^ \bullet  }  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i}{T_{si}} + MCPTairflow + {{\mathop m\limits^ \bullet  }_{sys}}{C_p}{T_{{\rm{supply}}}} + QADS,z - \left( {\frac{{{C_z}}}{{\delta t}}} \right)\left( { - 3T_z^{t - \delta t} + \frac{3}{2}T_z^{t - 2\delta t} - \frac{1}{3}T_z^{t - 3\delta t}} \right)}}{{\left( {\frac{{11}}{6}} \right)\frac{{{C_z}}}{{\delta t}} + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} A + MCPairflow + {{\mathop m\limits^ \bullet  }_{sys}}C}}$$</div>
-
-Where MCPT<sub>airflow</sub> is the sum of mass flow rate multiplied by specific heat and temperature for infiltration and mixing, Q<sub>ADS,z</sub> is the added total sensible load in the zone due to Air Distribution System losses, and MCP<sub>airflow</sub> is the sum of mass flow rate multiplied by specific heat for infiltration and mixing as calculated in the AirflowNetwork model described above.
-
-The revised coefficient (B) used in the zone humidity ratio calculation is shown below:
-
-<div>$$B = \sum {k{g_{mas{s_{{\rm{Sched Loads}}}}}}}  + M{W_{airflow}} + {\dot m_{sy{s_{in}}}}{W_{sys}} + \sum\limits_{i = 1}^{surfs} {{A_i}{h_{mi}}{\rho_{ai{r_z}}}{W_{surf{s_i}}}}  + QADS,m,z$$</div>
-
-Where MW<sub>airflow</sub> is the sum of mass flow rate multiplied by humidity ratio for infiltration and mixing and Q<sub>ADS,m,z\\  </sub>is the added total latent (moisture) load in the zone due to Air Distribution System losses from the AirflowNetwork model described above. This coefficient is used in the prediction of moisture as described in the section “Moisture Predictor-Corrector� found elsewhere in this document.
-
-### Model Output
-
-The available outputs from the AirflowNetwork model are described in the EnergyPlus Input Output Reference manual.
-
-### Occupant Ventilation Control
-
-The AirflowNetwork:OccupantVentilationControl object enhances the AirflowNetwork model and provides more practical and advanced controls for window opening and closing operations, based on Marais & Teichmann (2014). This control includes minimum open and closed time control, indoor thermal comfort control, and opening and closing probability controls.
-
-#### Procedures of occupant ventilation control
-
-It should be pointed that the open elapsed time and closed elapsed time are not independent. In other words, when one of the elapsed times value is greater than 0, then other elapsed time value must be equal to 0. The model is either tracking a window as open, in which case the open elapsed time grows, or as closed, in which case the closed elapsed time grows. 
-
-The calculation procedures are presented in the following steps:
-
-Step 1: Open elapsed time check 
-
-The model checks the open elapsed time first. When the open elapsed time is greater than 0 and less than the minimum opening time, a window will remain open. Otherwise, the model goes to Step 2.  
-
-    Open elapsed time > minimum open time
-
-Step 2: Closed elapsed time check 
-
-This step checks the closed elapsed time. When the closed elapsed time is greater than 0 and less than the minimum closed time, a window will remain closed. Otherwise, the model goes to Step 3. 
-
-    Closed elapsed time > minimum closed time
-
-Step 3: Elapsed time only? 
-
-When either the open elapsed time or the closed elapsed time is long enough (greater than the minimum time) and no other checks are needed, the model returns to the other ventilation control defined in the Ventilation Control Mode field in AirflowNetwork:MultiZone:Zone or AirflowNetwork:MultiZone:Surface. If other checks are needed, the following steps will be performed. 
-
-Step 4: Thermal comfort temperature calculation 
-
-The thermal comfort check requires the thermal comfort temperature and the comfort band. The comfort temperature of Tcomf is calculated as a function of the outdoor dry-bulb temperature Tout. The comfort temperature calculation may be based on two curves and a boundary temperature point. 
-
-<div>$$
-  T_{comf} = \left\{ \begin{array}{ll} \rm{Low Temp Curve,} & \min T_{out} &lt; x \leq \rm{Boundary Point} \\ \rm{High Temp Curve,} & \rm{Boundary Point} \leq x &lt; \max T_{out}  \end{array}\right.
-$$</div>
-
-Step 5: Thermal band calculation 
-
-The comfort band is calculated as a function of the design personal dissatisfaction PPD. 
-
-<div>$$\theta = -0.0028 \left(100-\rm{PPD}\right)^2 + 0.3419 \left(100-\rm{PPD}\right) – 6.6275 $$</div>
-
-This equation is valid for PPD 0% to 35%
-
-Step 6: Upper boundary check of thermal comfort 
-
-After calculation of the comfort temperature and band, the thermal comfort check will be performed using the zone air operative temperature Tg. The check consists of upper and lower boundary checks.
-
-The upper boundary check checks window opening status and uses the following logic:
-
-<div>$$T_g > \left(T_{comf} + \theta\right)$$</div>
-
-If the above logic check is true, the opening probability check will be performed. The detailed description is given in the opening probability section. 
-
-If the above logic check is false, no action is needed.
-
-If the opening probability check is true and upper boundary check is satisfied, a window will be opened, regardless of open/closed status at the previous time step. If the opening probability check is false and upper boundary check is satisfied, a window will remain at the status from the previous time step.
-
-<div>$$T_g > \left(T_{comf} + \theta\right) \&\& \rm{OpeningProbability}$$</div>
-
-Step 7: Lower boundary check of thermal comfort 
-
-The lower boundary check will follow the upper boundary check to check the window closing status, using the following logic.
-
-<div>$$T_g &lt; \left(T_{comf} - \theta\right)$$</div>
-
-If the above logic check is true, the closing probability check will be performed. The detailed description is given in the closing probability section. 
-
-If the above logic check is false, no action is needed.
-
-If the closing probability check is true and lower boundary check is satisfied, a window will be closed, regardless of open/closed status at the previous time step. If the closing probability check is false and lower boundary check is satisfied, a window will remain at the status from the previous time step.
-
-<div>$$T_g &lt; \left(T_{comf} - \theta\right) \&\& \rm{ClosingProbability}$$</div>
-
-The output variables from the model are open status, opening probability status, and closing probability status. The detailed description of opening status is given in the Airflow Network Outputs section in the Input Output Reference.
-
-Note: The upper and lower boundary checks are not independent. In other words, when one of boundary check is satisfied, the other check will be dissatisfied.  
- 
-#### Procedures of opening probability control
-
-Opening probability control provides an optional random number check. The control logic of opening probability is described in the following steps.
-
-Step 1: Closed elapsed time check 
-
-This check requires that closed elapsed time is longer than the minimum closing time. 
-
-Closed time > minimum closed time
-
-If the time duration is not long enough, the output is false so that a window remains closed. 
-
-If the time duration is long enough, an occupancy check is performed.
-
-Step 2: Occupancy check 
-
-If a zone is not occupied and the occupancy check is requested, the output is false. If the zone is occupied, the next step is to check the setpoints using zone air temperature at the previous time step as a reference. 
-
-Step 3: Setpoint check 
-
-There are 5 temperature control types. The following types are available:
-
-* No control: Bypass
-
-* Single heating setpoint: If Tzon > setpoint, go to next step. Otherwise, return false.
-
-* Single cooling setpoint: If Tzon &lt; setpoint, go to next step. Otherwise, return false.
-
-* Single heating and cooling setpoint: no action by returning false
-
-* Dual heating and setpoints: If heating setpoint &lt; Tzon &lt; Cooling setpoint, go to next step. Otherwise, return false.
-
-Step 4: Select bypass or opening probability check 
-
-A choice is provided at this stage so that the opening probability check may be performed or bypassed. If bypassed, the output will be true to open a window. If performed, probability will be determined from a schedule. 
-
-Step 5: Perform opening probability check 
-
-The opening probability (OP) value is determined from a schedule.
-
-OP = Schedule value or specific function
-
-If the probability value is greater than a random number, the output is true. 
-
-OP > random number (random number is between 0 and 1)
-
-Otherwise, the result will be false.    
-
-#### Procedures of closing probability control
-
-The control logic of closing probability is described as follows. 
-
-Step 1: Open elapsed time check 
-
-This check requires that open elapsed time is longer than the minimum opening time.
- 
-Open time > minimum open time
-
-If the time duration is not long enough, the output is false and the window remains open. Otherwise, Step 2 will be performed.
-
-Step 2: Select by-pass or closing probability check 
-
-A choice is provided at this step so that the closing probability check may be performed or bypassed. If bypassed, the output will be true to close a window. If performed, the closing probability will be calculated. The closing probability (CP) value is given from a schedule.
-
-CP = Schedule value or specific function
-
-If the closing probability check is performed and the closing probability is greater than a random number, the output is true. 
-
-CP > random number (random number is between 0 and 1)
-
-Otherwise, the result will be false.    
-
-
-### References
-
-Atkins, R. E., J. A. Peterka, and J. E. Cermak. 1979. “Averaged pressure coefficients for rectangular buildings,� Wind Engineering, Proceedings of the Fifth International Conference 7:369-80, Fort Collins, CO. Pergamon Press, NY.
-
-Bolmqvist, C. and M. Sandberg, 2004, “Air Movements through Horizontal Openings in Buildings – A Model Study,� International Journal of Ventilation, Vol. 3, No. 1, pp. 1-9
-
-COMIS Fundamentals. 1990. Edited by Helmut E. Feustel and Alison Rayner-Hooson, LBL-28560, Lawrence Berkeley Laboratory, Berkeley, CA
-
-Conte, S. D. and C de Boor. 1972.Elementary Numerical Analysis: an Algorithmic Approach, McGraw-Hill.
-
-Cooper, L., 1989, “Calculation of the Flow Through a Horizontal Ceiling/Floor Vent,� NISTIR 89-4052, National Institute of Standards and Technology, Gaithersburg, MD
-
-Dols, W. S. & G. N. Walton. 2002. “CONTAMW 2.0 User Manual,� NISTIR 6921, National Institute of Standards and Technology, Gaithersburg , Maryland
-
-Holmes, J. D. 1986. Wind Loads on low-rise buildings: The structural and environmental effects of wind on buildings and structures, Chapter 12, Faculty of Engineering, Monash University, Melbourne, Australia
-
-Marais, J. M. & C. Teichmann, “Window Simulation Methods Required for Manual Window Ventilated Buildings,� Fifth German-Austrian IBPSA Conference, September 22-24, 2014, RWTH Aachen University, Germany 
-
-Swami, M. V. and S. Chandra. 1988. Correlations for pressure distribution on buildings and calculation of natural-ventilation airflow, ASHRAE Transactions 94(1988) (Pt 1), pp. 243-266.
-
-Swami, M. V., L. Gu, & V. Vasanth. 1992. “Integration of Radon and Energy Models for Building,� FSEC-CR-553-92, Florida Solar Energy Center, Cocoa, Florida
-
-Tan, Q. and Y. Jaluria, 1992, “Flow through Horizontal Vents as Related to Compartment Fire Environments,� NIST-GCR-92-607, National Institute of Standards and Technology, Gaithersburg, Maryland
-
-Walton, G. N. 1989. “AIRNET – A Computer Program for Building Airflow Network Modeling,� NISTIR 89-4072, National Institute of Standards and Technology, Gaithersburg, Maryland
-
-Walton, G. N. & W. S. Dols. 2003. “CONTAM 2.1 Supplemental User Guide and Program Documentation,� NISTIR 7049, National Institute of Standards and Technology, Gaithersburg, Maryland
diff --git a/doc/src/docs/EngineeringReference/13-EncyclopaedicRefs.md b/doc/src/docs/EngineeringReference/13-EncyclopaedicRefs.md
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-# Engineering Reference Encyclopedia
-
-The encyclopedic reference of simulation models is a very large document, and so it is split up into multiple pieces.  Here is a quick overview with links to each of the pieces:
-
-* [Volume 1](13a-EncyclopaedicRefs.md)
-    * Air Terminals
-    * Boilers
-    * Chillers
-* [Volume 2](13b-EncyclopaedicRefs.md)
-    * Ice Thermal Storage
-    * Coils
-    * HVAC Controllers
-    * Baseboard Heaters
-* [Volume 3](13c-EncyclopaedicRefs.md)
-    * Cooling Towers
-    * Demand Controlled Ventilation
-    * Evap Coolers
-    * Air System Components
-    * VRF Systems
-    * Heat Exchangers
-    * Humidifiers
-* [Volume 4](13d-EncyclopaedicRefs.md)
-    * Zone Internal Gains
-    * Indoor Swimming Pool
-    * Pipes
-    * Pumps
-    * Ideal Load Air Systems
-    * District Heating and Cooling
-    * Central HP
-    * ChillerHeater
-    * Plant Components
-* [Volume 5](13e-EncyclopaedicRefs.md)
-    * Radiant System Models
-    * Refrigeration
-    * Setpoint Managers
-    * Solar Collectors
-    * System Availability Managers
-* [Volume 6](13f-EncyclopaedicRefs.md)
-    * Thermal Comfort
-    * Trombe Walls
-    * Water Tanks
-    * Water Systems
-    * Zone Controls
-    * Zone Equipment
diff --git a/doc/src/docs/EngineeringReference/13a-EncyclopaedicRefs.md b/doc/src/docs/EngineeringReference/13a-EncyclopaedicRefs.md
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-
-Simulation Models – Encyclopedic Reference
-==========================================
-
-The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of “Heat Balance�, “HVAC�, and “Plant�.  With the integrated solution, these designations signify where the effects of these models have their first impacts.
-
-<!--RemoveStart-->
-Main Sections:
-
-* [Air Terminals](#Terminals)
-* [Boilers](#Boilers)
-* [Chillers](#Chillers)
-<!--RemoveEnd-->
-
-Air System Distribution Terminals <a name="Terminals"></a>
----------------------------------
-
-### Constant Volume Single Duct Uncontrolled Air Terminal
-
-The input object AirTerminal:SingleDuct:Uncontrolled provides a method for directly connecting a central air system to a thermal zone.  Central system air is usually supplied to a zone through a terminal unit such as a single duct VAV reheat box.  Sometimes, however, it is desirable to supply central system air directly to a zone without any zone level control or tempering.  An example would be Furnace or Central DX equipment.  AirTerminal:SingleDuct:Uncontrolled is the input object for a component used to pass supply air directly into a zone without any thermostatic control.  This unit allows the program to know what zone this branch of the air system is attached to and a place to input the maximum air flow rate.  It is typically used with an AirLoopHVAC running as a constant-volume, variable-temperature system.
-
-The AirTerminal:SingleDuct:Uncontrolled object creates the capability of supplying central system air directly to a zone and only contains the zone inlet node.  This node is both the zone inlet node and the outlet node of the AirLoopHVAC:ZoneSplitter.  It can be thought of as a balancing damper in the duct branch going to the zone.  This inlet flow can be controlled by an availability schedule.  This can be thought of as a seasonal shut off of the balancing damper.
-
-For the AirTerminal:SingleDuct:Uncontrolled objects to work correctly, it is important in any systems including them for the sum of the maximum zone air flow rates to be equal to the maximum central system flow rate.  The zone maximum flow rates are specified in the direct air inputs.  The central air system flow rate is specified in the AirLoopHVAC input and also in the air loop branch and central fan inputs.
-
-### Constant Volume Single Duct Reheat Air Terminal
-
-The input object AirTerminal:SingleDuct:ConstantVolume:Reheat provides a model for single duct constant volume systems with reheat that satisfy the cooling load in a zone by changing the inlet air temperature with a reheat coil. The supply air temperature must be low enough to meet the cooling load in the zone having the greatest load. For zones with a smaller cooling load, a reheat coil is used to raise the temperature of the zone inlet air.
-
-This object can be configured with a water, steam, electric or gas reheat coil. Operation is basically the same with all coil types. The coil is controlled to raise the zone supply air temperature (i.e., the Unit Air Outlet Node temperature) to match the zone load.  If the coil is undersized, the zone setpoint temperature will not be maintained.
-
-![ConstVolumeReheat](media/image2788.png)
-
-Figure 153. Schematic of AirTerminal:SingleDuct:ConstantVolume:Reheat Unit
-
-### Variable Air Volume Single Duct Reheat and No Reheat Air Terminals
-
-The VAV Single Duct Reheat and No Reheat terminal units (objects AirTerminal:SingleDuct:VAV:Reheat and AirTerminal:SingleDuct:VAV:NoReheat) provide models for single duct variable-air-volume (VAV) systems that control zone temperature primarily by varying the quantity of supply air rather than by varying the supply air temperature. The supply air temperature must be low enough to meet the cooling load in the zone having the greatest load when the zone terminal device is wide open. For zones with a smaller cooling load, the terminal device damper reduces the flow to match the zone setpoint.. If the lower flow limit on the terminal device is reached and the load is not matched, the inlet air temperature can be moderated if the terminal device has a reheat coil. In that case both the quantity of air and its temperature entering the zone are varied to meet the load. For air terminals using reheat coils, the maximum flow during reheat may be limited. Limiting the maximum flow during reheat occurs only when cooling is required (when any valid air loop cooling coil is active) and the terminal unit must reheat the air. Optional user inputs may also be used to control the amount of outdoor air entering the zone.
-
-
-
-![Damper\_NoHeat](media/image2789.png)
-
-Figure 154. Schematic of AirTerminal:SingleDuct:VAV:NoReheat Unit
-
-
-
-![Damper](media/image2790.png)
-
-Figure 155. Schematic of AirTerminal:SingleDuct:VAV:Reheat Unit
-
-The operation of the dampers and the control are described in the section AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat and AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat**,** which follows. The exception is that the section below describes how the air flow rate is varied for both cooling and heating. For the case of AirTerminal:SingleDuct:VAV:NoReheat and AirTerminal:SingleDuct:VAV:Reheat, air flow only varies during cooling operation and the air flow rate is set at the minimum value (minimum air flow fraction) when zone heating is required.
-
-#### Minimum Outdoor Air Control
-
-The single duct air terminals may also be used to provide a minimum outdoor air quantity. When the air flow rate required to meet the zone load does not provide sufficient outdoor air, the terminal device damper will open to allow sufficient outdoor air to enter the zone. In this case, the terminal damper is controlled based on the air loop’s outdoor air fraction. The outdoor air may be specified as a fixed value per person, per floor area, or per zone. The minimum outdoor air may also be specified as air changes per hour. In addition, these values may be added together to provide a combined minimum outdoor air flow rate or the maximum of each of these values may be used. An outdoor air fraction schedule may also be used to modify the calculation for the minimum amount of outdoor air throughout the simulation (Ref. DesignSpecification:OutdoorAir).
-
-### Variable Air Volume Heating and Cooling Single Duct Reheat and NoReheat Air Terminal
-
-#### Overview
-
-The VAV Heating and Cooling Single Duct Reheat and No Reheat terminal units (objects AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat and AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat provide models for variable-air-volume (VAV) terminal units are widely used in commercial and industrial applications. The VAV terminal units contain actuated dampers that vary the amount of central system air supplied to a zone. These terminal units may also contain a heating coil to trim the supply air temperature when overcooling is possible. The heating coil may also serve as the primary air heating source when the central system contains cooling-only equipment.
-
-The VAV terminal units described here are used primarily with central air handling equipment with cooling and heating capability. The terminal unit dampers modulate in **both** cooling and heating mode to maintain the zone setpoint temperature(s). The central air handling equipment may be either variable air volume or constant volume where a bypass duct is used to shunt excess system air flow back to the inlet of the central air handler as terminal unit dampers modulate to satisfy the zone thermostat (i.e., AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass).
-
-#### Model Description
-
-The no reheat version of the single duct VAV heat and cool terminal unit contains a single virtual damper assembly and requires minimal inputs. The reheat version contains both a virtual damper assembly and an air reheat coil. Multiple reheat coil types are available:
-
-1)   Coil:Heating:Water
-
-2)   Coil:Heating:Electric
-
-3)   Coil:Heating:Gas
-
-4)   Coil:Heating:Steam
-
-Both units are simulated to provide an air flow rate sufficient to satisfy the thermostat request. The air flow rate is a function of the terminal unit’s inlet air temperature and the load sensed by the thermostat. The output of the models are simply the damper position required to satisfy the zone’s thermal load. Other information regarding terminal unit performance may be viewed using node report variables and heating coil report variables.
-
-![Damper\_NoHeat](media/image2791.png)
-
-Figure 156. Schematic of AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat Unit
-
-
-
-![Damper](media/image2792.png)
-
-Figure 157. Schematic of AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat Unit
-
-#### Terminal Unit Inputs
-
-Both terminal unit types share several common input fields. A unique terminal unit name must be entered. A system availability schedule is also defined to allow operational control of the terminal unit. The user must then connect the unit to the air distribution system by defining the unit inlet and outlet node names. Design air flow rates are then specified: maximum total air flow rate (autosizable) and minimum air flow fraction.
-
-The reheat version of this terminal unit requires additional information. The name and type of reheat coil and the damper air outlet node name (same as reheat coil inlet node name). Maximum and minimum water flow rates are entered when a water or steam heating coil is used, as well as a control node name for actuating water-side flow rates and a convergence tolerance for iteration control.
-
-#### Simulation and Control
-
-The simulation begins by determining the air mass flow rate required to satisfy the heating/cooling demand.
-
-<div>$$C{p_{zone}} = PsyCpAirFnWTdb\left( {{\omega_{zone}},{T_{zone}}} \right)$$</div>
-
-<div>$$C{p_{inlet}} = PsyCpAirFnWTdb\left( {{\omega_{inlet}},{T_{inlet}}} \right)$$</div>
-
-<div>$$DeltaCpT = \left( {C{p_{inlet}}} \right)\left( {{T_{inlet}}} \right) - \left( {C{p_{zone}}} \right)\left( {{T_{zone}}} \right)$$</div>
-
-<div>$$\dot m = MIN\left( {{{\dot m}_{max}},\,\,\,MAX\left( {{{\dot m}_{max}}*MinAirFlowFrac\,,\,\,\,{\raise0.7ex\hbox{${{{\dot Q}_{zone}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{zone}}} {DeltaCpT}}}\right.}\!\lower0.7ex\hbox{${DeltaCpT}$}}} \right)\,\,} \right)$$</div>
-
-where
-
-<span>\(C{p_{zone}}\)</span>  = Specific heat of zone air, J/kg-K
-
-<span>\(C{p_{inlet}}\)</span>  = Specific heat of terminal unit inlet air, J/kg-K
-
-<span>\({\omega_{zone}}\)</span>    = Zone air humidity ratio, kg/kg
-
-<span>\({T_{zone}}\)</span>     = Zone air dry-bulb temperature, °C
-
-<span>\({\omega_{inlet}}\)</span>    = Terminal unit inlet air humidity ratio, kg/kg
-
-<span>\({T_{inlet}}\)</span>     = Terminal unit inlet air dry-bulb temperature, °C
-
-<span>\({\dot Q_{zone}}\)</span>    = Zone load, W (positive values denote heating, negative values denote cooling)
-
-<span>\(\dot m\)</span>        = Terminal unit air mass flow rate, kg/s
-
-<span>\(PsyCpAirFnWTdb\)</span>  = Psychrometric function calculating air specific heat given air humidity ratio and dry-bulb temperature
-
-<span>\(MinAirFlowFrac\)</span>    = User-specified zone minimum air flow fraction
-
-<span>\({\dot m_{max}}\)</span>              = Terminal unit maximum air mass flow rate, kg/s
-
-The outdoor air input fields, if entered, are then used to adjust the terminal unit air mass flow rate to ensure the correct amount of outdoor air enters the zone (within the constraints of the terminal unit maximum and minimum flow rate inputs). The amount of outdoor air is calculated per the outdoor air requirements and is adjusted by the fraction of outdoor air entering the air loop outdoor air system.
-
-<div>$$
-  \dot m = \max \left( \dot m, \frac{\dot m_{OA}}{OAFrac} \right)
-$$</div>
-
-where:
-
-<span>\({\mathop m\limits^\cdot_{OA}}\)</span> = zone outdoor air flow rate, kg/s
-
-<span>\(OAFrac\)</span> = fraction of outdoor air entering the air loop outside air system
-
-If the terminal unit is in reheat mode (i.e., the central air loop cooling coil is active, the supply air was overcooled, and the zone thermostat is requesting heating) the maximum air flow rate allowed during reheat mode is adjusted as necessary.
-
-<div>$$\mathop m\limits^\cdot  \, = \,MIN\left( {\mathop m\limits^\cdot  ,\,{{\mathop m\limits^\cdot  }_{reheat}}} \right)$$</div>
-
-where:
-
-<span>\({\mathop m\limits^\cdot_{reheat}}\)</span> = maximum air mass flow rate during reheat, kg/s
-
-The damper position is then calculated as:
-
-<div>$$FRAC_{damper} = \frac{\dot m}{\dot m_{max}} $$</div>
-
-And the amount of outdoor air entering the zone is:
-
-<div>$$\dot V_{OA} = \dot m (OAFrac)$$</div>
-
-where
-
-<span>\(FRAC_{damper}\)</span>  = Output variable ‘Zone Air Terminal VAV Damper Position’, fraction of maximum flow
-
-<span>\({\mathop V\limits^\cdot_{OA}}\)</span> = Output variable “Zone Air Terminal Outdoor Air Volume Flow Rate� entering the zone, m3/s
-
-Simulation of the reheat coil occurs next when applicable. The heating demand required to maintain the thermostat heating setpoint temperature and the heating capacity of air flowing through the terminal unit are used to determine the amount of reheat required.
-
-<div>$${\dot Q_{reheat}} = {\dot Q_{heatSP}} + \dot m C_{p,zone}(T_{inlet}-T_{zone})$$</div>
-
- where
-
-<span>\({\dot Q_{reheat}}\)</span>  = Reheat coil load, W (positive values denote heating)
-
-<span>\({\dot Q_{heatSP}}\)</span> = Load to heating setpoint temperature, W (positive values denote heating)
-
-#### References
-
-No specific references.
-
-### Constant Volume Single Duct Four Pipe Induction Air Terminal
-
-The four pipe induction terminal unit (object name: AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction) is a hybrid air-hydronic unit that supplies both centrally conditioned air and local hydronic heating/cooling to a zone. Centrally conditioned air is supplied to the terminal unit at high pressure and constant flow. The central (primary) air is discharged into the terminal unit through a nozzle, inducing a fixed flow of zone (secondary) through a hydronic heating/cooling coil. The primary and secondary air streams mix and are discharged to the zone. Hot or cold water flow through the coil is varied to meet the zone heating or cooling requirement.
-
-#### Model
-
-The four pipe induction terminal unit is modeled as a compound component consisting of three sub-components: a hot water coil, a chilled water coil and an air mixer. In terms of EnergyPlus objects these are *Coil:Heating:Water*, *Coil:Cooling:Water*, and *AirLoopHVAC:ZoneSplitter*.  The terminal unit is a forward model: its inputs are defined by the state of its inlets: namely its 2 air streams – primary and secondary; and its two water inlets – hot and cold. The outputs of the model are the conditions of the outlet air stream: flow rate, temperature and humidity ratio. The terminal unit data and simulation are encapsulated in the module *HVACSingleDuctInduc*.
-
-#### Inputs and Data
-
-The user describes the terminal unit by inputting the name and type of the heating and cooling coils and the name of the zone mixer. The user must also specify the connectivity of the component by naming the inlet air and water nodes and the air outlet node. Finally maximum and fixed flow rates need to be specified (although these can be autosized): maximum and minimum hot and cold water volumetric flow rates and the total air volumetric flow rate (sum of primary and secondary flow rates). The relative convergence tolerances for the hot and cold water flow rates also need to be input (or allowed to default). Finally the induction ratio needs to be specified: this  is defined as the ratio of the secondary air flow rate to the primary air flow rate. The relationship between the flow rates is:
-
-<div>$${\dot m_{air,tot}} = {\dot m_{air,pri}} + {\dot m_{air,\sec }}$$</div>
-
-<div>$${\dot m_{air,sec}} = {R_{induc}}\cdot {\dot m_{air,pri}}$$</div>
-
-so
-
-<div>$${\dot m_{air,pri}} = {\dot m_{air,tot}}/(1 + {R_{induc}})$$</div>
-
-<div>$${\dot m_{air,sec}} = {\dot m_{air,tot}}\cdot {R_{induc}}/(1 + {R_{induc}})$$</div>
-
-where *R<sub>induc</sub>* is the user-input induction ratio.
-
-All input data for the four pipe induction terminal units is stored in the array *IndUnit*.
-
-#### Calculation
-
-Given the needed inputs, the output is calculated in subroutine *CalcFourPipeIndUnit*. The temperature, humidity ratio and flow rate of the primary and secondary air streams are taken from the inlet air nodes. The inlet hot and chilled water flow rates are passed in as parameters – temperatures are taken from the inlet water nodes. Then
-
-The hot water coil is simulated (Call *SimulateWaterCoilComponents);*
-
-The chilled water coil is simulated (Call *SimulateWaterCoilComponents*);
-
-The two air streams are mixed (Call *SimAirMixer*).
-
-Finally the load met by the terminal unit is calculated and passed back to the calling routine:
-
-<div>$${\dot Q_{out}} = {\dot m_{tot}}\cdot {c_{p,air}}\cdot ({T_{air,out}} - {T_{air,zone}})$$</div>
-
-Note that data is never explicitly passed between the sub-components. This is all handled automatically by the node connections and the data stored on the nodes.
-
-#### Simulation and Control
-
-From the result of the zone simulation we have the heating/cooling demand on the terminal unit 
-<span>\({\dot Q_{z,req}}\)</span>
-. For a given hot and cold water flow *CalcFourPipeIndUnit* will give us the terminal unit heating/cooling output. We need to vary the hot or cold water flow to make the unit output match the demand. To do this we need to numerically invert *CalcFourPipeIndUnit*: given the output, we want one of the inputs – the hot or cold water flow. The numerical inversion is carried out by calling subroutine *SolveRegulaFalsi*. This is a general utility routine for finding the zero of a function (the *residual* function) of a single independent variable. In this case the residual function calculates 
-<span>\(({\dot Q_{z,req}} - {\dot Q_{out}})/{\dot Q_{z,req}}\)</span>
-. *SolveRegulaFalsi* varies either the hot water or cold water mass flow rate to zero the residual.
-
-Decide whether the unit is on or off. The unit is off if: a) it is scheduled off; b) the inlet air mass flow rate is zero; c) the zone thermostat is in the deadband; d) or the zone heating/cooling demand is very small.
-
-If the unit is off, call *CalcFourPipeIndUnit* with the hot and cold water flow rates set to their minimum flows and return.
-
-If the unit is on, check whether active heating or cooling by the hydronic coils is needed. Call *CalcFourPipeIndUnit* with minimum water flows to see what how much cooling (or possibly heating) the unit is doing with primary air only. The output for this case is <span>\({\dot Q_{pri}}\)</span>.
-
-If <span>\({\dot Q_{z,req}} > {\dot Q_{pri}}\)</span> we need active heating. Set the cold water flow rate to the minimum. Check that the terminal unit can meet the load by setting the hot water flow rate to the maximum and calling *CalcFourPipeIndUnit*. If the output is less than the zone demand we are done – all the outputs have been calculated. Otherwise call *SolveRegulaFalsi* to obtain the hot water flow rate that will make the unit output match the zone demand. This ends the unit simulation.
-
-If <span>\({\dot Q_{z,req}} &lt; {\dot Q_{pri}}\)</span>we need active cooling. We set the hot water flow rate to the minimum. We check whether the terminal unit can supply the needed output by setting the cold water flow rate to the maximum and calling *CalcFourPipeIndUnit.* If this maximum cooling output is not able to meet the zone cooling demand we are done. Otherwise call *SolveRegulaFalsi* to obtain the cold water flow rate that will make the unit output match the zone demand. This ends the unit simulation.
-
-Note that the terminal unit output is never explicitly passed to another routine. Instead the output is saved as the outlet conditions on the terminal unit outlet air node. The node data is accessed when the terminal unit output is needed elsewhere in the program (in *SimZoneAirLoopEquipment* for instance).
-
-#### References
-
-No specific references.
-
-### Fan Powered Induction Series and Parallel Single Duct  Reheat Air Terminal
-
-#### Overview
-
-The input objects AirTerminal:SingleDuct:SeriesPIU:Reheat and AirTerminal:SingleDuct:ParallelPIU:Reheat provide models for fan powered induction terminal units that occur in a variety of configurations. EnergyPlus models 2 types: *series* (sometimes called *constant*) and *parallel* (sometimes called *intermittent*). The series unit provides a constant flow of air to the zone (the fan is always on at a constant flow) with a variable proportion of primary and secondary air. The parallel unit has an intermittent fan: the fan is off at maximum cooling and does not switch on until primary air flow is significantly reduced from the maximum. Once on it provides a constant flow of secondary air. Both units induce air from the zone or plenum (secondary air) and mix it with centrally conditioned supply air (primary air). Both units are variable volume: the supply air flow rate is varied to match zone conditioning requirement.
-
-#### Model
-
-Both types of PIU are modeled as compound components. The series unit, in sequence from its inlet, consists of an air mixer, a constant volume fan, and a heating coil. In terms of EnergyPlus objects this is:
-
-1.    AirLoopHVAC:ZoneMixer
-
-2.    Fan:ConstantVolume
-
-3.    Coil:Heating:Water, Coil:Heating:Electric, Coil:Heating:Gas or Coil:Heating:Steam
-
-The parallel unit contains a fan (in the secondary air stream, an air mixer, and a heating coil. In terms of EnergyPlus objects this is:
-
-1.    Fan:ConstantVolume
-
-2.    AirLoopHVAC:ZoneMixer
-
-3.    Coil:Heating:Water, Coil:Heating:Electric, Coil:Heating:Gas or Coil:Heating:Steam
-
-Both units are forward models: their inputs are defined by the state of their inlets: namely the air inlet and the hot water  inlet. The outputs of the models are the conditions of the outlet air stream: flow rate, temperature and humidity ratio. The PIUs data and simulation are encapsulated in the module *PoweredInductionUnits*. The main simulation routine for the units within the module are *CalcSeriesPIU* and *CalcParallelPIU*.
-
-#### Inputs and Data
-
-The user describes the PIU by inputting the names of the mixer, fan and heating coil sub-components plus the type of the heating coil sub-component. The user must connect the unit to the overall HVAC systems by naming various inlet and outlet nodes: the primary air inlet node, the secondary air inlet node, the unit air outlet node, and the hot water inlet node. One internal node name is needed: the coil air inlet node (same as fan outlet mode for series, mixer outlet node for parallel). Design flow rates need to be specified (although these can be autosized): maximum total air flow rate (series), maximum primary air flow rate, minimum primary air flow fraction, maximum secondary air flow rate (parallel), fan-on flow fraction (parallel), and maximum and minimum hot water flow rates. A convergence tolerance needs to be specified for units with hot water coils. There is an on/off availability schedule that need to be set.
-
-All input data for the powered induction terminal units is stored in the array *PIU*.
-
-#### Calculation
-
-The calculation is performed by simulating the sub-components in the order given above. Most of the code is involved with figuring out what the various flow rates should be before simulating the subcomponents. These calculations are described below.
-
-#### Simulation and Control
-
-*Series*
-
-From the result of the zone simulation we have the heating/cooling demand on the terminal unit <span>\({\dot Q_{tot}}\)</span>. The subroutine *CalcSeriesPIU* needs to determine the flow rates that will allow the unit to meet this load. The first step is to determine the on/off state of the unit and determine the air flow rates.
-
-·        If the unit is scheduled off, the primary and secondary flow rates are set to zero.
-
-·        If there is no primary air flow (or less than .001 kg/s), the primary air flow is set to zero and the secondary air flow is set to the constant total air flow input by the user.
-
-·        If the zone temperature is in the deadband or the zone load is less than 1 watt or the zone needs heating, the primary air flow rate is set to the minimum flow rate specified by the input and the secondary air flow rate is set to the difference between the fixed total air flow rate and the primary air flow rate.
-
-·        Otherwise, the zone needs cooling and the unit is active.
-
-§ We determine the fan temperature rise: the secondary air flow is set to the max total air flow, primary air flow to zero, and the mixer and fan are simulated. The fan delta T is the difference between the temperature at the fan’s outlet node and inlet node.
-
-§ We calculate the unit air outlet temperature needed to meet the zone cooling load: <span>\({T_{out}} = C{p_h} + {\dot Q_{z,req}}/({\dot m_{air,tot}}\cdot {c_{p,air,z}})\)</span>
-
-§ The temperature needed at the outlet of the mixer is then: <span>\({T_{mix}} = {T_{out}} - \Delta {T_{fan}}\)</span>
-
-§ We can then set the primary air flow rate.
-
-·        If 
-         <span>\({T_{mix}} \le {T_{in,pri}}\)</span>
-         then 
-         <span>\({\dot m_{pri}} = {\dot m_{pri,max}}\)</span>
-
-·        else if 
-         <span>\({T_{mix}} \ge {T_{in,pri}}\)</span>
-         and 
-         <span>\({T_{mix}} \ge {T_{in,sec}}\)</span>
-         then 
-         <span>\({\dot m_{pri}} = {\dot m_{pri,min}}\)</span>
-
-·        otherwise 
-         <span>\({\dot m_{pri}} = {\dot m_{air,tot}}\cdot ({T_{in,sec}} - {T_{mix}})/({T_{in,sec}} - {T_{in,pri}})\)</span>
-         , subject to the constraints that the flow rate can’t be bigger than the max and min allowed.
-
-The air flow rates are now determined and we can fire the air mixer (Call *SimAir-Mixer*) and fan (Call *SimulateFanComponents*) component simulations. Finally we simulate the heating coil:
-
-·        for a hot water coil, if the coil is off (no flow, deadband, no load) just fire the coil simulation once (Call *SimulateWaterCoilComponents*). Otherwise call *ControlCompOutput*; *ControlCompOutput* is a general component control routine. In this case it calls *SimulateWaterCoilComponents* repeatedly while varying the hot water flow rate and minimizing
-
-<div>$$({c_{p,air}}\cdot {\dot m_{air,tot}}\cdot ({T_{out}} - {T_z}) - {\dot Q_{z,req}})/{\dot Q_{z,req}}$$</div>
-
-to within the heating convergence tolerance.
-
-·        For gas, electric or steam coils, the required coil output is set to <span>\({\dot Q_{coil,req}} = {\dot Q_{z,req}} - {c_{p,air}}\cdot {\dot m_{air,coil}}({T_{air,coil,in}} - {T_z})\)</span>. Then the coil simulation is fired (Call *SimulateHeatingCoilComponent* or *SimulateSteamCoilCompo-nents*).
-
-Finally the unit sensible output is calculated:
-
-<div>$${\dot Q_{sens,out}} = {\rm{PsyHFnTdbW}}({T_{air,out}},{W_z}) - {\rm{PsyHFnTdbW(}}{T_z},{W_z})$$</div>
-
-where *PsyHFnTdb* is the EnergyPlus function giving enthalpy as a function of temperature and humidity ratio.
-
-*Parallel*
-
-From the result of the zone simulation we have the heating/cooling demand on the terminal unit <span>\({\dot Q_{tot}}\)</span>. The subroutine *CalcParallelPIU* needs to determine the flow rates that will allow the unit to meet this load. The first step is to determine the on/off state of the unit and determine the air flow rates.
-
-·        If the unit is scheduled off, the primary and secondary flow rates are set to zero.
-
-·        If there is no primary air flow (or less than .001 kg/s), the primary air flow is set to zero and the secondary air flow is set to the max secondary air flow input by the user.
-
-·        If the zone temperature is in the deadband or the zone load is less than 1 watt or the zone needs heating, the primary air flow rate is set to the minimum flow rate specified by the input and the secondary air flow rate is set to max secondary air flow input by the user.
-
-·        Otherwise, the zone needs cooling and the unit is active.
-
-§ We determine the fan temperature rise: the secondary air flow is set to the max secondary air flow, primary air flow to zero, and the fan and mixer are simulated. The fan delta T is defined as the difference between the temperature at the mixer outlet node and the fan inlet node.
-
-§ Assuming that the fan is off, we calculate the primary air flow needed to meet the cooling demand.
-
-<div>$${\dot m_{pri}} = {\dot Q_{z,req}}/({c_{p,air}}\cdot ({T_{in,pri}} - {T_z}))$$</div>
-
-The flow rate is constrained to be between the min and max primary air flow rates. If this calculated primary flow rate is greater than the fan-on flow rate, the secondary flow rate is set to zero and we are done. Otherwise, the fan is on and we need to recalculate the primary air flow rate.
-
-<div>$${\dot m_{pri}} = ({\dot Q_{z,req}} - {c_{p,air}}\cdot {\dot m_{sec}}\cdot ({T_{in,sec}} + \Delta {T_{fan}} - {T_z}))/({c_{p,air}}\cdot ({T_{in,pri}} - {T_z}))$$</div>
-
-The secondary flow rate is set to the user input fixed flow rate. The primary air flow rate is constrained to be between the min and max primary flow rated.
-
-The air flow rates are now determined and we can fire the fan (Call *SimulateFanComponents*) and air mixer (Call *SimAirMixer*) component simulations. Finally we simulate the heating coil:
-
-·        for a hot water coil, if the coil is off (no flow, deadband, no load) just fire the coil simulation once (Call *SimulateWaterCoilComponents*). Otherwise call *ControlCompOutput*; *ControlCompOutput* is a general component control routine. In this case it calls *SimulateWaterCoilComponents* repeatedly while varying the hot water flow rate and minimizing
-
-<div>$$({c_{p,air}}\cdot {\dot m_{air,tot}}\cdot ({T_{out}} - {T_z}) - {\dot Q_{z,req}})/{\dot Q_{z,req}}$$</div>
-
-to within the heating convergence tolerance.
-
-·        For gas, electric or steam coils, the required coil output is set to <span>\({\dot Q_{coil,req}} = {\dot Q_{z,req}} - {c_{p,air}}\cdot {\dot m_{air,coil}}({T_{air,coil,in}} - {T_z})\)</span>. Then the coil simulation is fired (Call *SimulateHeatingCoilComponent* or *SimulateSteamCoilCompo-nents*).
-
-Finally the unit sensible output is calculated:
-
-<div>$${\dot Q_{sens,out}} = {\rm{PsyHFnTdbW}}({T_{air,out}},{W_z}) - {\rm{PsyHFnTdbW(}}{T_z},{W_z})$$</div>
-
-where *PsyHFnTdb* is the EnergyPlus function giving enthalpy as a function of temperature and humidity ratio.
-
-#### References
-
-No specific references.
-
-### Variable Air Volume Fan Powered Single Duct Air Terminal
-
-#### Overview
-
-The input object AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan provides a model for variable speed (VS) fan VAV terminal unit that is a typical VAV reheat unit with the addition of a variable-speed blower fan to assist in moving supply air from the plenum to the conditioned zone. It is typically used with under-floor air distribution systems (UFAD) where the supply air is sent at low static pressure through an under-floor supply plenum. The fan has two maximum flow rate settings: one for cooling and one for heating. The cooling maximum is usually the actual fan maximum while the heating maximum is a lesser flow rate. The fan is upstream of the heating coil (this is a blow-through unit). The heating coil can be hot-water, electric or gas. Cooling control is obtained by varying the supply air flow rate from the cooling maximum to the minimum flow rate. Heating control is established by varying both the heating coil output (or hot water flow rate for hot water coils) and the supply air flow rate. Note that for this unit the minimum supply air flow rate is the flow rate when the fan is off.
-
-#### Model
-
-The VS fan VAV terminal unit is modeled as a compound component consisting of two sub-components: a fan and a heating coil. In terms of EnergyPlus objects the fan is a *Fan:VariableVolume* object and the heating coil is a *Coil:Heating:Water*, *Coil:Heating:Electric* or a *Coil:Heating:Gas*. The terminal unit is a forward model: its inputs are defined by the state of its inlets: namely its air inlet and its hot water  inlet, if it has a hot water coil. The outputs of the model are the conditions of the outlet air stream: flow rate, temperature and humidity ratio. The terminal unit data and simulation are encapsulated in the module *SingleDuct*. The main simulation routine for the unit within the module is *SimVAVVS*.
-
-#### Inputs and Data
-
-The user describes the terminal unit by inputting the name and type of the heating coil and the name and type of the fan. The user must also specify the connectivity of the component by naming the inlet air node; the air node connecting the fan and heating coil (fan outlet, coil inlet); the unit air outlet node (same as the zone inlet node); and hot water inlet node (if any). Maximum flow rates need to be specified (although these can be autosized): maximum cooling and heating air flow rates and the maximum hot water flow rate (if there is a hot water coil). Minimum flow rates are specified by giving by giving a minimum flow fraction for the air flow and a volumetric flow rate minimum for the hot water. For the units with hot water coils the relative convergence tolerance for the hot water flow rate also needs to be input (or allowed to default).
-
-All input data for the VS fan VAV terminal units is stored in the array *Sys*.
-
-#### Calculation
-
-Given the needed inputs, the output is calculated in subroutine *CalcVAVVS*. The temperature and humidity of the supply air stream are taken from the inlet air node. The inlet air flow rate and the hot water flow rate are passed in as parameters. If the coil is electric or gas the coil heating power is passed instead of the hot water flow rate. Then
-
-The fan is simulated (call *SimulateFanComponents*). If the fan is off the fan outlet conditions are set to the inlet conditions.
-
-The heating coil is simulated (call *SimulateWaterCoilComponents* if the coil is a hot water coil; call *SimulateHeatingCoilComponents* if the coil is gas or electric).
-
-Finally the sensible load met by the terminal unit is calculated and passed back to the calling routine:
-
-<div>$${\dot Q_{out}} = {\dot m_{air}}\cdot {c_{p,air}}\cdot ({T_{air,out}} - {T_{air,zone}})$$</div>
-
-Note that data is never explicitly passed between the sub-components. This is all handled automatically by the node connections and the data stored on the nodes.
-
-#### Simulation and Control
-
-From the result of the zone simulation we have the heating/cooling demand on the terminal unit 
-<span>\({\dot Q_{tot}}\)</span>
-. For the given inlet conditions *CalcVAVVS* will give us the terminal unit heating/cooling output. We need to vary the air or hot water flow rate or the heating coil power (for gas or electric coils) to make the unit output match the demand. To do this we need to numerically invert *CalcVAVVS*: given the output, we want one of the inputs – the air or hot water flow rate or the heating coil power. The numerical inversion is carried out by calling subroutine *SolveRegulaFalsi*. This is a general utility routine for finding the zero of a function (the *residual* function) of a single independent variable. In this case the residual function calculates 
-<span>\(({\dot Q_{tot}} - {\dot Q_{out}})/{\dot Q_{tot}}\)</span>
-. *SolveRegulaFalsi* varies either the air mass flow rate, the hot water mass flow rate or the heating coil power to zero the residual.
-
-The unit is simulated in the following sequence.
-
-Decide whether the unit is on or off. The unit is off if: a) it is scheduled off; b) the inlet air mass flow rate is zero; or c) the zone thermostat is in the deadband
-
-If the unit is off, call *CalcVAVVS* with flow rates set to their minimum flows and return.
-
-If the unit is on, we need to establish the boundaries of 4 conditioning regions: a) active cooling with fan on; b) active heating with fan on; c) active heating with fan off; d) passive cooling with fan off. The heating/cooling demand will fall into one of these regions. Once the correct region is determined, we will know which model input to vary for control and thus how to invert the calculation.
-
-To establish the boundaries of region a) we call *CalcVAVVS* twice: once with the supply air flow rate set to the cooling maximum, once with the cooling air flow rate set to the minimum. In both cases the heating coil output is at the minimum and the fan is on. Call the 2 cooling outputs 
-<span>\({\dot Q_{cool,max,fanon}}\)</span>
-and 
-<span>\({\dot Q_{cool,min,fanon}}\)</span>
-. Remembering that EnergyPlus convention is that cooling loads are negative, then if 
-<span>\({\dot Q_{tot}} &lt; {\dot Q_{cool,max,fanon}}\)</span>
-the terminal unit can not meet the demand. Set the air mass flow rate to the cooling maximum and call *CalcVAVV* again. This concludes the simulation. If  
-<span>\({\dot Q_{cool,max,fanon}} &lt; {\dot Q_{tot}} &lt; {\dot Q_{cool,min,fanon}}\)</span>
-the cooling demand is in the active cooling region. We hold the heating at the minimum, allow the supply air flow to vary between the cooling maximum and the minimum with the fan on, and call *SolveRegulaFalsi* to obtain the supply air flow rate that will produce the unit sensible cooling output that matches the demand. This concludes the simulation.
-
-To establish the boundaries of region b) call *CalcVAVVS* twice: once with the supply air flow rate set to the heating maximum, once with the supply air flow rate set to the minimum. In both calls, if the heating coil is a hot water coil, the hot water flow rate is at the maximum. For electric and gas coils, the heating power is set to the maximum at maximum supply air flow and to zero at the minimum supply air flow. In both calls the fan is set to be on. Call the 2 heating outputs returned from the two calls to *CalcVAVVS* 
-<span>\({\dot Q_{heat,max,fanon}}\)</span>
-and 
-<span>\({\dot Q_{heat,min,fanon}}\)</span>
-. If 
-<span>\({\dot Q_{heat,max,fanon}} &lt; {\dot Q_{tot}}\)</span>
-the terminal unit can not meet the load. Set the air flow rate to the heating maximum and the hot water flow rate or heating coil power to the maximum and call *CalcVAVVS* again. This concludes the simulation for this case. If 
-<span>\({\dot Q_{heat,min,fanon}} &lt; {\dot Q_{tot}} &lt; {\dot Q_{heat,max,fanon}}\)</span>
-the heating demand is in the active heating, fan on region. For a hot water coil we call *SolveRegulaFalsi* with the supply air flow rate as the input that is varied and the hot water flow rate set to the maximum. For electric and gas coils the coil power and the supply air flow rate are both varied together from their minimum to maximum in a call to *SolveRegulaFalsi*.  The call to *SolveRegulaFalsi* concludes the simulation for this case.
-
-This region only applies to terminal units with a hot water coil. To establish the boundaries of region c) the fan is set to off, the supply air flow rate is set to minimum flow and *CalcVAVVS* is called twice: once with the hot water flow at maximum and once with the hot water flow at minimum. Call the two heating outputs 
-<span>\({\dot Q_{heat,max,fanoff}}\)</span> 
-and <span>\({\dot Q_{tot}}\)</span>
-. If 
-<span>\({\dot Q_{tot}}\)</span>
- is between these values, the supply air flow rate is set to its minimum, the fan is set to off, and in the call to *SolveRegulaFalsi* the hot water flow rate is varied to meet the load. This concludes the simulation for this case.
-
-If the cooling demand does not fall into cases a) – c), the unit is assumed to be in the passive cooling state: heating is off or at the minimum, the fan is off, and the minimum supply air flow is delivered to the zone.
-
-Note that the terminal unit output is never explicitly passed to another routine. Instead the output is saved as the outlet conditions on the terminal unit outlet air node. The node data is accessed when the terminal unit output is needed elsewhere in the program (in *SimZoneAirLoopEquipment* for instance).
-
-#### References
-
-No specific references.
-
-### Four Pipe Beam Unit (AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam)
-
-The four pipe beam air terminal units are ceiling-mounted, beam-type units that are provided with primary air from a central system and additional heating or cooling by inducing room air to flow over a hydronic convector.  They are called *four pipe* because the units are connected with two pipes for chilled water supply and return and another two pipes for hot water supply and return.  A simple empirical model is used to enable using input data derived from manufacturer’s catalog data.  
-
-####Model Description
-The model assumes that the total conditioning power, <span>$ {\dot Q_{Tot}} $</span>, is the sum of the conditioning provided by the primary air, <span>$ {\dot Q_{SA}} $</span>, and the conditioning provided by the beam convector, <span>$ {\dot Q_{Beam}} $</span>.
-
-<div>$$ {\dot Q_{Tot}} = {{\dot Q_{SA}} + {\dot Q_{Beam}}} $$</div>
-
-The primary air contribution is easily determined using
-
-<div>$$ {\dot Q_{SA}} = {{\dot m_{SA}}\cdot ({c_{p,SA}} \cdot {T_{SA}} - {c_{p,Z}} \cdot {T_{Z}})} $$</div>
-
-The convector power <span>$ {\dot Q_{Beam}} $</span> is coupled directly to the zone air heat balance (using a source code term called *NonAirSysOutput*) in a way that provides only sensible heat transfer directly to the zone air node.  We therefore assume that the air terminal’s convector is always dry during cooling. Many of the terms used in the performance calculations are normalized by the total length of beam in zones, <span>$ {L} $</span>.
-
-When the unit is operated in cooling mode, the convector power is determined using the rated normalized cooling capacity that is modified by three separate functions.
-
-<div>$$ {\dot Q_{Beam, cool}} = { \dot q_{cool,rated} \cdot f_{ \Delta T_{cool,mod} }() \cdot f_{\dot m_{SA,cool,mod}}() \cdot f_{\dot m_{CW,mod}}() \cdot L }$$</div>
-
-The modification factor <span>$ {f_{ \Delta T_{cool,mod} }() } $</span> describes how the cooling capacity is adjusted to account for the temperature difference between the zone air and the chilled water entering the convector.  This empirical correction factor is intended to account for how heat transfer between the chilled water and induced room air flow depends on the temperature difference, both in terms of surface convection heat transfer and the rate of induced air flow. The function can be described using any of the single-variable curves or a lookup table. The single independent variable is the ratio between the current temperature difference, <span>$ {\Delta T_{air-CW}} $</span>, and the temperature difference used to rate beam performance, <span>$ {\Delta T_{air-CW,rated}} $</span>.
-
-<div>$$ {f_{ \Delta T_{cool,mod} }() }= f_{ \Delta T_{cool,mod} }\left(\frac{\Delta T_{air-CW}}{\Delta T_{air-CW,rated}}\right)  $$</div>
-
-<div>$$ {\Delta T_{air-CW}} = {T_{Z}}-{T_{CW,in}}  $$</div>
-
-The modification factor <span>$ {f_{\dot m_{SA,cool,mod}}()} $</span> describes how the cooling capacity is adjusted to account for the primary air flow rate.  This empirical correction factor is intended to account for how varying primary air flow rates will impact the rate that room air is induced to flow across the convector. The function can be described using any of the single-variable curves or a lookup table. The single independent variable is the ratio between the current normalized primary air flow rate, <span>$ {\dot m_{SA}} $</span>, and the normalized flow rate used to rate beam performance, <span>$ {\dot m_{SA,rated}} $</span>.  Flow rates are normalized by dividing the total length of all the beam units in the zone.  The ratio is calculated using air mass flow rates with the rated flow rate assumed to be for standard temperature and pressure at sea level so that elevation effects appear only in the numerator when the function is evaluated.
-
-<div>$${f_{\dot m_{SA,cool,mod}}()} = f_{\dot m_{SA,cool,mod}}\left(\frac{{\dot m_{SA}}}{{\dot m_{SA,rated}} }\right)  $$</div>
-<div>$${\dot m_{SA}} = \frac{\dot M_{SA}}{L}  $$</div>
-<div>$${\dot m_{SA,rated}} = {\dot v_{SA,rated}} \cdot {\rho_{air,STP}} $$</div>
-
-The modification factor <span>$ f_{\dot m_{CW,mod}}() $</span> describes how the cooling capacity is adjusted to account for the flow rate of chilled water through the convector.  This empirical correction factor is intended to account for how varying chilled water flow rates will impact the velocity of fluid inside the pipes and the corresponding impact on the rate of surface convection heat transfer inside the convector.  The function can be described using any of the single-variable curves or a lookup table.  The single independent variable is the ratio between the current normalized chilled water flow rate, <span>$ {\dot m_{CW}} $</span>, and the normalized chilled water flow rate at the rating point, <span>$ {\dot m_{CW,rated}} $</span>.
- 
-<div>$$ {f_{\dot m_{CW,mod}}()} = f_{\dot m_{CW,mod}}\left(\frac{{\dot m_{CW}}}{{\dot m_{CW,rated}}}\right) $$</div>
-<div>$${\dot m_{CW}} = \frac{\dot M_{CW}}{L}$$</div>
-<div>$${\dot m_{CW,rated}} = {\dot v_{CW,rated}} \cdot {\rho_{CW}}$$</div>
- 
-The model for when the unit is operated in heating mode is very similar. The convector power is determined using the rated normalized heating capacity that is modified by three separate functions.
-
-<div>$${\dot Q_{Beam, heat}} = {\dot q_{heat,rated}}\cdot f_{ \Delta T_{heat,mod} }() \cdot f_{\dot m_{SA,heat,mod}}()\cdot f_{\dot m_{HW,mod}}() \cdot L $$</div>
-
-The modification factor <span>$ f_{ \Delta T_{heat,mod} }() $</span> describes how the heating capacity is adjusted to account for the temperature difference between the hot water and the zone air entering the convector.  Notice that for heating the temperature difference is defined different from cooling operation so that positive difference values are the result.  This empirical correction factor is intended to account for how heat transfer between the hot water and induced room air flow depends on the temperature difference, both in terms of surface convection heat transfer and induced air flow rates. The function can be described using any of the single-variable curves or a lookup table. The single independent variable is the ratio between the current temperature difference, <span>$ \Delta T_{HW-air} $</span>, and the temperature difference used to rate beam performance, <span>$ \Delta T_{HW-air,rated} $</span>.
-
-<div>$${f_{ \Delta T_{heat,mod} }()} = f_{ \Delta T_{heat,mod} }\left(\frac{\Delta T_{HW-air}}{\Delta T_{HW-air,rated}}\right)  $$</div>
-
-<div>$$ {\Delta T_{HW-air}} = {T_{HW,in}} -{T_{Z}} $$</div>
-
-The modification factor <span>$ f_{\dot m_{SA,heat,mod}}() $</span> describes how the heating capacity is adjusted to account for the primary supply air flow rate.  This empirical correction factor is intended to account for how varying primary air flow rates will impact the rate that room air is induced to flow across the convector. The function can be described using any of the single-variable curves or a lookup table. The single independent variable is the same ratio described above for cooling and it is assumed that the unit can be rated using the same primary air flow rate for both heating and cooling operation of the four pipe unit.  Flow rates are normalized by dividing the total length of all the beam units in the zone.  The ratio is calculated using air mass flow rates with the rated flow rate assumed to be for standard temperature and pressure at sea level so that elevation effects appear only in the numerator when the function is evaluated.
-
-<div>$${f_{\dot m_{SA,heat,mod}}()} = f_{\dot m_{SA,heat,mod}}\left(\frac{{\dot m_{SA}}}{{\dot m_{SA,rated}} }\right)  $$</div>
-  
-The modification factor <span>$ f_{\dot m_{HW,mod}}() $</span> describes how the heating capacity is adjusted to account for the flow rate of hot water through the convector.  This empirical correction factor is intended to account for how varying hot water flow rates will impact the velocity of fluid inside the pipes and the corresponding impact on the rate of surface convection heat transfer inside the convector.  The function can be described using any of the single-variable curves or a lookup table.  The single independent variable is the ratio between the current normalized hot water flow rate, <span>$ {\dot m_{HW}} $</span>, and the normalized hot water flow rate at the rating point,
-<span>$ {\dot m_{HW,rated}} $</span>. 
-
-<div>$$ f_{\dot m_{HW,mod}}() = f_{\dot m_{HW,mod}}\left(\frac{{\dot m_{HW}}}{{\dot m_{HW,rated}}}\right) $$</div>
-<div>$${\dot m_{HW}} = \frac{\dot M_{HW}}{L}$$</div>
-<div>$${\dot m_{HW,rated}} = {\dot v_{HW,rated}} \cdot {\rho_{HW}}$$</div>
-
-Where,
-	
-<span>$ {c_{p,SA}} $</span>  Specific heat of primary air entering through the air terminal unit, in J/kg-K.
-	
-<span>$ {c_{p,Z}} $</span>  Specific heat of zone air, in J/kg-K.
-	
-<span>$ {c_{p,CW}} $</span>  Specific heat of zone air, in J/kg-K.
-	
-<span>$ {f_{\dot m_{CW,mod}}()} $</span>  Cooling capacity modification factor function of chilled water flow rate
-	
-<span>$ {f_{ \Delta T_{cool,mod} }()} $</span>  Cooling capacity modification factor function of air-water temperature difference
-	
-<span>$ {f_{\dot m_{SA,cool,mod}}()} $</span>  Cooling capacity modification factor function of primary air flow rate
-	
-<span>$ {f_{\dot m_{HW,mod}}()} $</span>  Heating capacity modification factor function of hot water flow rate
-	
-<span>$ {f_{ \Delta T_{heat,mod} }()} $</span>  Heating capacity modification factor function of water - air temperature difference
-	
-<span>$ {f_{\dot m_{SA,heat,mod}}()} $</span>  Heating capacity modification factor function of primary air flow rate
-	
-<span>$ {L} $</span>  Total length of all beam units serving the zone, in m
-	
-<span>$ {\dot m_{CW}} $</span>  Mass flow rate of chilled water per meter of length, in kg/s-m
-	
-<span>$ {\dot m_{CW,rated}} $</span>  Mass flow rate of chilled water per meter of length at rating point, in kg/s-m
-	
-<span>$ {\dot m_{HW}} $</span>  Mass flow rate of hot water per meter of length, in kg/s-m
-	
-<span>$ {\dot m_{HW,rated}} $</span>  Mass flow rate of hot water per meter of length at rating point, in kg/s-m
-	
-<span>$ {\dot m_{SA}} $</span>  Mass flow rate of primary air per meter of length, in kg/s-m
-	
-<span>$ {\dot m_{SA,rated}} $</span>  Mass flow rate of primary air per meter of length at rating point, kg/s-m
-	
-<span>$ {\dot M_{SA}} $</span>  Mass flow rate of primary air entering the zone through the air terminal unit, in kg/s
-	
-<span>$ {\dot M_{CW}} $</span>  Mass flow rate of chilled water, kg/s
-	
-<span>$ {\dot M_{HW}} $</span>  Mass flow rate of hot water, kg/s
-	
-<span>$ {\dot q_{cool,rated}} $</span>  Rated beam cooling capacity per meter of length, in W/m.
-	 
-<span>$ {\dot q_{heat,rated}} $</span>  Rated beam heating capacity per meter of length, in W/m.
-	
-<span>$ {\dot Q_{Beam}} $</span>  Conditioning power delivered to the zone by the beam convector, in W.
-	
-<span>$ {\dot Q_{SA}} $</span>  Conditioning power delivered to the zone by the primary air mass flow, in W.
-	
-<span>$ {\dot Q_{Tot}} $</span>  Total (net) conditioning power delivered to zone by the air terminal unit, in W.
-	
-<span>$ {\rho_{air,STP}} $</span>  Density of air at standard conditions (sea level), in kg/m<sup>3</sup>
-	
-<span>$ {\rho_{air}} $</span>  Density of air at standard conditions adjusted for elevation), in kg/m<sup>3</sup>
-	
-<span>$ {\rho_{CW}} $</span>  Density of chilled water, in kg/m<sup>3</sup>
-	
-<span>$ {T_{SA}} $</span>  Dryblub temperature of the (central) primary air entering the air terminal unit, in degrees C.
-	
-<span>$ {T_{Z}} $</span>  Dryblub temperature of the zone air, in degrees C.
-	
-<span>$ {T_{CW,in}} $</span>  Temperature of chilled water entering the convector, in degrees C.
-	
-<span>$ {\Delta T_{air-CW}} $</span>  Difference between the zone air temperature and chilled water entering the convector, delta degrees C.
-	
-<span>$ {\Delta T_{HW-air}} $</span>  Difference between the water and zone air temperature entering the convector, delta degrees C.
-	
-<span>$ {\Delta T_{air-CW,rated}} $</span>  Value of <span>$ {\Delta T_{air-CW}} $</span> at rating conditions for cooling performance, delta degrees C.
-	
-<span>$ {\Delta T_{HW-air,rated}} $</span>  Value of <span>$ {\Delta T_{HW-air}} $</span> at rating conditions for heating performance, delta degrees C.
-	
-<span>$ {\dot v_{SA,rated}} $</span>  Volume flow rate of air per meter length at rating point, in m<sup>3</sup>/s-m.
-	
-<span>$ {\dot v_{CW,rated}} $</span>  Volume flow rate of chilled water per meter length at rating point, in m<sup>3</sup>/s-m.
-	
-<span>$ {\dot v_{HW,rated}} $</span>  Volume flow rate of hot water per meter length at rating point, in m<sup>3</sup>/s-m.
-
-The performance capacity model described above is controlled to modulate water flow through the beam's convector using the non-linear numerical solver in EnergyPlus called Solve Regula Falsi.  The predicted zone load to setpoint <span>$ {\dot Q_{Zone, Required}} $</span> is adjusted by <span>$ {\dot Q_{SA}} $</span> to determine the required beam load.
-
-<div>$$ {\dot Q_{Beam, Required}} = {\dot Q_{Zone, Required}} - {\dot Q_{SA}} $$</div>
-
-When <span>$ {\dot Q_{Zone, Required}} $</span> is negative the beams need to provide cooling and when it is positive the beams need to provide heating. The the solver iterates the water flow rate to find a flow rate that will meet the load. 
-
-When cooling, the result for beam capacity (negative for cooling) is used to calculate the leaving temperature of the chilled water using,
-
-<div>$$ {T_{CW,out}} = {T_{CW,in}} - \frac{{\dot Q_{Beam}}}{{\dot m_{CW}} \cdot {c_{p,CW}} } $$</div>
-
-However, to protect from a non-physical result the leaving chilled water temperature is constrained to be no warmer than a 1.0 C approach temperature compared to the zone air or the primary supply air.  If the above result is too warm the leaving temperature and beam cooling capacity are adjusted using the following equations, and a recurring warning is issued to alert the user that there may be a problem with the cooliong performance input data.
-
-<div>$$ {T_{CW,out}} = { max( {T_{SA}} , {T_{Z}}) - 1.0 } $$</div>
-<div>$$ {\dot Q_{Beam}} = {\dot m_{CW}} \cdot {c_{p,CW}} \cdot {( {T_{CW,in}} - {T_{CW,out}}) } $$</div>
-
-Similarly when heating, the result for beam capacity (positive for heating) is used the calculate the leaving temperature of the hot water using, 
-
-<div>$$ {T_{HW,out}} = {T_{HW,in}} - \frac{{\dot Q_{Beam}}}{{\dot m_{HW}} \cdot {c_{p,HW}} } $$</div>
-
-To protect from a non-physical result the leaving hot water temperature is constrained to be no cooler than a 1.0 C approach temperature compared to the zone air or the primary supply air.  If the above result is too cool the leaving temperature and beam heating capacity are adjusted using the following equations, and a recurring warning is issued to alert the user that there may be a problem with the heating performance input data.
-
-<div>$$ {T_{HW,out}} = { min( {T_{SA}} , {T_{Z}}) + 1.0 } $$</div>
-<div>$$ {\dot Q_{Beam}} = {\dot m_{CW}} \cdot {c_{p,CW}} \cdot {( {T_{HW,in}} - {T_{HW,out}}) } $$</div>
-
-####Four Pipe Beam Sizing
-
-The four pipe beam model has four inputs that can be autosized:
-	
-<span>$ {L} $</span>  Total length of all beam units serving the zone, in m
-	
-<span>$ {\dot V_{SA,Des}} $</span>  Design primary supply air volume flow rate, in m<sup>3</sup>/s
-
-<span>$ {\dot V_{CW,Des}} $</span>  Design chilled water volume flow rate, in m<sup>3</sup>/s
-
-<span>$ {\dot V_{HW,Des}} $</span>  Design hot water volume flow rate, in m<sup>3</sup>/s
-
-Because of the way the model is formulated with defaulted inputs for rated, normalized performance data, we can link the four inputs together to ensure an internally consistent set of sizes.  If any one of these four inputs is not autosized (given a fixed value at input) then the other three can be computed using the normalized, rated performance data which are either input or have default values. If the total beam length is input, then the following equations are used
-
-<div>$$ {\dot V_{SA,Des}} = {{\dot v_{SA,rated}} \cdot {L} } $$</div>
-<div>$$ {\dot V_{CW,Des}} = {{\dot v_{CW,rated}} \cdot {L} } $$</div>
-<div>$$ {\dot V_{HW,Des}} = {{\dot v_{HW,rated}} \cdot {L} } $$</div>
-
-If the design primary supply air flow rate is input then the beam length can be determined as follows and then water flow rates evaluated as above.
-
-<div>$$ {L} = {\frac{{\dot V_{SA,Des}}}{{\dot v_{SA,rated}}}  } $$</div>
-
-If the chilled water flow rate is input, then the beam length can be determined as follows and the other values evaluated as above, 
-
-<div>$$ {L} = {\frac{{\dot V_{CW,Des}}}{{\dot v_{CW,rated}}}  } $$</div>
-
-If the hot water flow rate is input, then the beam length can be determined as follows and the other values evaluated as above, 
-
-<div>$$ {L} = {\frac{{\dot V_{HW,Des}}}{{\dot v_{HW,rated}}}  } $$</div>
-
-When all four inputs are autosized, which is the usual case, there is no simple way to anchor the sizes and we need to use the results from the zone and system sizing calculations to determine sizes for the four pipe beam unit. The following design data from the zone and system sizing calculations are used when sizing the four pipe beam:
-
-<span>$ {\dot V_{TU,Z,final,cool} } $</span>  Final zone terminal unit design volume flow rate for cooling, in m<sup>3</sup>/s  
-	
-<span>$ {\dot V_{TU,Z,final,heat} } $</span>  Final zone terminal unit design volume flow rate for heating, in m<sup>3</sup>/s  
-	
-<span>$ {\dot V_{Z,final,OA} } $</span>  Final zone design volume flow rate for minimum outdoor air mechanical ventilation, in m<sup>3</sup>/s.  
-	
-<span>$ {T_{SA,cool,design } } $</span>  Final design zone terminal unit inlet supply air temperature at cooling peak, in degrees C.
-	
-<span>$ {w_{SA,cool,design } } $</span>  Final design zone terminal unit inlet supply air humidity ratio at cooling peak, in kg_H2O/kg_dryair.
-	
-<span>$ {T_{Z,cool,design } } $</span>  Final design zone air temperature at cooling peak, in degrees C.
-	
-<span>$ {w_{Z,cool,design } } $</span>  Final design zone air humidity ratio at cooling peak, in kg_H2O/kg_dryair.
-	
-<span>$ {\dot Q_{Z,cool,design } } $</span>  Final design zone cooling load at cooling peak, in W.
-	
-<span>$ {T_{CW,design}} $</span>  Chilled water plant loop supply side design exit temperature, in degrees C.
-
-<span>$ {T_{SA,heat,design } } $</span>  Final design zone terminal unit inlet supply air temperature at heating peak, in degrees C. 
-	
-<span>$ {w_{SA,heat,design } } $</span>  Final design zone terminal unit inlet supply air humidity ratio at heating peak, in kg_H2O/kg_dryair.
-	
-<span>$ {T_{Z,heat,design } } $</span>  Final design zone air temperature at heating peak, in degrees C.
-	
-<span>$ {w_{Z,heat,design } } $</span>  Final design zone air humidity ratio at heating peak, in kg_H2O/kg_dryair.
-	
-<span>$ {\dot Q_{Z,heat,design } } $</span>  Final design zone heating load at heating peak, in W.
-
-<span>$ {T_{HW,design}} $</span>  Hot water plant loop supply side design exit temperature, in degrees C.
-
-Overhead beam type air terminals induce room air to flow over the convector by the directing primary supply air through special nozzles. Therefore, the cooling and heating capacity of the beam's convector is not separable from the primary flow rate, varying the primary flow rate varies the beam capacity. The design primary flow rate is chosen to be largest value that satisfies three requirements:  (1) the ventilation requirement, (2) the design cooling load (if cooling is present), (3) and the design heating load (if heating is present).
-
-The sizing method here uses the non-linear solver inside EnergyPlus, called Solve Regula Falsi, to arrive at a set of sizes that meet the design load.  The solver is for a single independent variable and although we have four sizes to solve for, we can reduce the problem to finding a suitable design primary supply air flow rate and then the other sizes can be determined from that as shown above. The solver needs as its input a minimum and a maximum "x-value," which here is the primary supply air flow rate, and then it searches for a solution that minimizes a residual.   In general the design primary supply flow rate that meets the load is somewhere between the minimum flow required for ventilation and a maximum flow where the primary supply flow meets all the zone's design load without any help from the beam's convector.  For example if the supply air is cold, as it would be for latent control, and there is a cooling load then there will be a relatively large air flow rate that meets all the load without any cooling from chilled water circulating through the beam.  This larger air flow serves as the upper bound for the solver. 
-
-When sizing for the cooling design load, the following design values are set for use in the model calculations:
-
-<div>$$ {T_{CW,in}} = {T_{CW,design}} $$</div>
-<div>$$ {\dot m_{HW}} = 0.0  $$</div>
-<div>$$ {T_{Z}} = {T_{Z,cool,design } } $$</div>
-<div>$$ {T_{SA}} = {T_{SA,cool,design } } $$</div>
-<div>$$ {c_{p,Z}} = {PsyCpAirFnWTdb ({w_{Z,cool,design } },  {T_{Z,cool,design } }  ) }$$</div>
-<div>$$ {c_{p,SA}} = {PsyCpAirFnWTdb ( {w_{SA,cool,design } },  {T_{SA,cool,design } }   ) }$$</div>
-<div>$$ {\dot Q_{Zone, Required}} = -1.0 \cdot {\dot Q_{Z,cool,design } } $$</div>
-<div>$$ {\dot m_{SA,max limit}} = { \left(\frac{{\dot Q_{Z,cool,design } }}{{c_{p,SA}} \cdot {( {T_{Z,cool,design } } - {T_{SA,cool,design } } )}}  \right) } $$</div>
-or if <span>$ ( {T_{Z,cool,design }} - {T_{SA,cool,design } } ) < 2.0 $</span> then
-<div>$$ {\dot m_{SA,max limit}} = { \left(\frac{{\dot Q_{Z,cool,design } }}{{c_{p,SA}} \cdot 2.0 } \right) } $$</div>
-<div>$$ {\dot m_{SA,min limit}} = min( {\dot V_{Z,final,OA} }, \frac{{\dot m_{SA,max limit}}}{3.0}, max({\dot V_{TU,Z,final,heat} } , {\dot V_{TU,Z,final,cool} }) ) $$</div>
-
-When sizing for the heating design load, the following design values are set for use in the model calculations:
-
-<div>$$ {T_{HW,in}} = {T_{HW,design}} $$</div>
-<div>$$ {\dot m_{CW}} = {0.0}  $$</div>
-<div>$$ {T_{Z}} = {T_{Z,heat,design } } $$</div>
-<div>$$ {T_{SA}} = {T_{SA,heat,design } } $$</div>
-<div>$$ {c_{p,Z}} = {PsyCpAirFnWTdb ({w_{Z,heat,design } },  {T_{Z,heat,design } }  ) }$$</div>
-<div>$$ {c_{p,SA}} = {PsyCpAirFnWTdb ( {w_{SA,heat,design } },  {T_{SA,heat,design } }   ) }$$</div>
-<div>$$ {\dot Q_{Zone, Required}} = {\dot Q_{Z,heat,design } } $$</div>
-<div>$$ {\dot m_{SA,max limit}} = { \left(\frac{{\dot Q_{Z,heat,design } }}{{c_{p,SA}} \cdot ( {T_{SA,heat,design } } - {T_{Z,heat,design }} ) } \right) } $$</div>
-or if <span>$ ( {T_{SA,heat,design } } - {T_{Z,heat,design } }) < 2.0 $</span> then
-<div>$$ {\dot m_{SA,max limit}} = { \left(\frac{{\dot Q_{Z,heat,design } }}{{c_{p,SA}} \cdot 2.0 } \right) }$$</div>
-<div>$$ {\dot m_{SA,min limit}} = {0.0} $$</div>
-
- The trial value for design primary supply air flow rate is used to calculate design values for length, chilled water flow, and hot water flow.
-<div>$$ {\dot V_{SA,Des}} = { \left(\frac{ {\dot m_{SA,trial}} }{{\rho_{air}} } \right) } $$</div>
-<div>$$ {L} = {\frac{{\dot V_{SA,Des}}}{{\dot v_{SA,rated}}}  } $$</div>
-<div>$$ {\dot V_{CW,Des}} = {{\dot v_{CW,rated}} \cdot {L} } $$</div>
-<div>$$ {\dot V_{HW,Des}} = {{\dot v_{HW,rated}} \cdot {L} } $$</div>
-
-The residual is calculated by evaluating the entire model to determine the total capacity for a trial flow rate (and corresponding design length and maximum water flow rates) and comparing it to the design load.
-<div>$$ {residuum} = \left(\frac{ ({\dot Q_{Zone, Required}} - {\dot Q_{Tot}} )}{{\dot Q_{Zone, Required}}}\right) $$</div>
-
-After the solvers have run and the final sizes for the four pipe beam have been determined, there is one more step taken to make further adjustments in the central sizing data structures for sizing air system components.  The usual methods of sizing the main AirLoopHVAC branch and fans are not able account for the methods used to size the four pipe beam. When the Sizing:System object was set to use *VentilationRequirement*, the air handler will be too small.  When the Sizing:System object was set to use *Sensible*, the air handler will be too large.  The system sizing calculations have already been completed at the time the four pipe beam air terminals are sized so we need to make some adjustments.  The final primary supply air flow rate size is compared to the original final zone sizes for the air terminal unit and the air loop sizes adjusted to make up for the difference.  A sizing report item called "AirLoopHVAC Design Supply Air Flow Rate Adjustment [m3/s]" is generated for each four pipe beam that shows the magnitude of the adjustment to data structure values used to size central air systems.  Therefore when autosizing air handlers with four pipe beams, it is expected that the outcomes for air system sizes will not agree with the system sizing reporting because of the differences introduced by this adjustment.  
-
-#### Developing Model Input From Catalog Data
-
-An example is presented showing how manufacturer’s data can be converted into the input data for the proposed model.  The following example is for a Trox active DID632A product with a type “H� nozzle, where the rating point has been chosen based on a 6 foot active length and 140 CFM primary rate with other rating conditions as listed in the catalog data.  The EnergyPlus IDF input for this example is show as the example in the in the Input Output reference description of the four pipe beam. 
-
-![FourPipeBeam/tableData](media/TroxDID632A_Tabledata.png)
-
-Snippet of catalog data for capacity and primary air flow rate dependence (Trox DID632A)
- 
-Choosing a 6 foot beam (with Nozzle type H) at 140 CFM as the rating point, we get 3726 Btu/h = 1092 W, 6 ft = 1.83 m, and 1092/1.83= 597 W/m for normalized beam cooling capacity at rating point.  The associated primary air flow rate of 140 ft<sup>3</sup>/min = 0.066 m^3/s and 0.066/1.83 = 0.036 m<sup>2</sup>/s is the normalized beam primary air flow rate at the rating point.  Note that because the flow rate is normalized by beam length, the units are m<sup>3</sup>/s/m (which reduces to m<sup>2</sup>/s).
-The rating heating capacity is listed as a “net� heating rate but since this is not well defined in the catalog we go ahead and assume that this represents the beam heating rate where the associated cooling provided by the primary air has already been subtracted.  The net heating capacity is 7411 Btu/h = 2172 W.  This value need to be increased by the primary cooling provided by 55 F = 12.7 C air entering a zone at 70 F = 21 C.  The catalog does not completely define the moist air state of the zone nor the primary air so we assume nominal average moist air density of 1.2 kg/m<sup>3</sup> and a specific heat of 1000.0 J/kg-C so that the primary air cooling rate is (21 – 12.7) * 0.066 * 1.2 * 1000 = 660 W.  The beam heating rate is therefore 2172 + 660 = 2832 W.  Then normalizing for beam length 2832/1.83 = 1548 W/m is the rated beam heating capacity.  
-The catalog includes two more data points for capacity at different flow rates, one for 100 ft<sup>3</sup>/min and the other for 180 ft<sup>3</sup>/min.  These are processed in the same way as the rating point data and used to create the modification curves that describe performance as a function of primary air flow rate.  
-
-### Cooled Beam Unit (AirTerminal:SingleDuct:ConstantVolume:CooledBeam)
-
-Cooled beam (frequently called chilled beams) systems are usually hybrid water – air systems. Commonly there is a constant flow, fixed temperature central forced air system for meeting ventilation and latent load requirements.  Sometimes this forced air system’s flow rate is varied according to ventilation demand; and of course its supply air temperature could be reset in various ways. Sensible cooling load is met by the cooled beam units; these are ceiling suspended units with cool water circulating through them. Some types of units are “passive� – they cool by radiation and natural convection. Other types of units are “active� and act as supply air terminal units with the supply air inducing room air over the beam cooling elements. These units cool almost entirely by convection. The DOE-2 model (upon which this model is based) is a convection only model – even the “passive� units are assumed to operate 100% convectively. The cooled beam elements act as an alternative to normal ceiling radiant cooling: they are not coupled to the building mass and they operate more in a convective mode, but they can, like radiant cooling, use fairly warm cooling water.
-
-Heating is accomplished separately from the cooled beam system – usually baseboards are used on the building perimeter to meet heating loads.
-
-#### Model
-
-The chilled beam system is modeled as an EnergyPlus terminal unit. In terms of configuration within the overall HVAC system it will resemble a 4 pipe induction terminal unit. The user describes the system as a typical single duct constant volume system (with outside air mixer, fan, heating and cooling coils) on the air loop side, and with cooled beam terminal units on the zone equipment side.
-
-The model is an empirical model developed at the equipment manufacturer Halton Oy. It consists of the following relationships.
-
-*P<sub>beam</sub>* = *A·K·DT       *                         beam cooling output per unit length W/m
-
-*K=a·DT<sup>n1</sup>·vr<sup>n2</sup>·w<sup>n3</sup>*                            coil heat transfer coefficient W/(m<sup>2</sup>K)
-
-*vr=(q<sub>in</sub>*/a*<sub>0</sub>)·r<sub>air</sub>*                                  room air mass flow rate across coil kg/(m<sup>2</sup>s)
-
-*q<sub>in</sub>=K<sub>1</sub>·DT<sup>n</sup>+K<sub>in</sub>·q<sub>pr</sub>*                             room air volumetric flow rate across coil per
-
-                                                      unit length m<sup>3</sup>/(s-m)
-
-DT is the room air –water temperature difference (average water temperature is used) in degrees C.
-
-w is the water velocity in m/s.
-
-q<sub>pr</sub> is the supply air flow rate per unit length m<sup>3</sup>/(s-m)
-
-The other symbols are the model parameters input by the user (see the IO Ref for descriptions).
-
-#### Inputs and Data
-
-The user describes the unit by inputting the name, referencing an availability schedule, and choosing a type (*active* or *passive*). The user must also specify the connectivity of the component by naming the inlet and outlet air and water nodes. The maximum water and fixed air flow rates need to be specified (although these can be autosized). The design inlet and outlet water temperatures are inputs. Generally the inlet water temperature is quite warm (15C is the default) and the temperature rise is small (design outlet water temperature defaults to 17C). Two key inputs are the number of beams (in the zone) and the beam length. It is generally wise to let these inputs autosize.
-
-The remaining inputs are parameters specific to the product model. Good defaults are supplied and they should not be changed without information from the manufacturer.
-
-#### Sizing
-
-The Cooled Beam sizing calculations generally follow the procedures used for other terminal units (see *Loop Equipment Sizing*). One difference is that the Cooled Beams use the Cooled Beam inputs *Design Inlet Water Temperature* and *Design Outlet Water Temperature* for the chilled water DT rather than the DT from Plant Sizing. There are also two inputs unique to the Cooled Beam units that are autosized and will be described here.
-
-The input *Number of individual beam units in the zone* is autosized by dividing the beam system zone design chilled water flow rate (either input by the user or autosized) by a nominal chilled water beam flow rate: 0.07 kg/s.
-
-The input *Length of an individual beam unit* is autosized by using the model equations to calculate the length. The inputs to the equations are:
-
-1)    the design load per beam. The design load is calculated from the design water mass flow rate and the design water inlet and outlet temperatures. The design load is divided by the number of beams to obtain the design load per beam.
-
-2)    The design air supply air flow per beam – obtained by dividing the design supply air flow by the number of beams.
-
-3)    The design water flow per beam (m<sup>3</sup>/s) – obtained by dividing the design water flow by the number of beams.
-
-4)    The design water velocity – obtained by dividing the design water flow per beam by the cross sectional inside area of a water tube (pD<sup>2</sup>/4, where D is the input *Pipe inside diameter*.
-
-5)    Average air to water *DT = T<sub>z,\\ cool\\ peak</sub>* - *0.5(T<sub>w,des\\ inlet</sub>* *+ T<sub>w,des\\ outlet</sub>)*; where        *T<sub>z,\\ cool\\ peak</sub>* is the zone air temperature at the cooling peak and the *T<sub>w,des</sub>* ‘s are the water design inlet and outlet temperatures.
-
-With these inputs the model equations can be solve directly for beam length for passive cooled beams, and iteratively for active cooled beams.
-
-#### Calculation
-
-The subroutine *CalcCoolBeam*  uses the model equations to calculate the cooling power *P<sub>beams,out</sub>* delivered to the room air and the outlet water temperature given the water flow rate (and the room air temperature and water inlet temperature). Since the model equations are nonlinear they must be solved iteratively. The subroutine does this by varying the outlet water temperature *T<sub>w,out</sub>* and calculating the water-side cooling power
-
-P<sub>w</sub> = q<sub>w,beam</sub>·c<sub>p,w</sub>·(T<sub>w,out</sub>-T<sub>w,in</sub>)
-
-and comparing it to the air-side cooling power
-
-P<sub>air</sub>=K·A·DT·L<sub>beam</sub>
-
-where *q<sub>w,beam</sub>* is the water mass flow rate (kg/s) per beam and *L<sub>beam</sub>* is the length of a beam (m). When *P*<sub>w</sub>  and *P<sub>air</sub>* match to within 0.1 W the subroutine terminates the iteration.
-
-#### Simulation and Control
-
-From the result of the zone simulation we have the heating/cooling demand for the zone equipment. For the cooling demand, we use the load to cooling set point *P<sub>c</sub>*. Part of the demand may be satisfied by the zone supply air:
-
-P<sub>sup</sub>=q<sub>air</sub>·(c<sub>p,air,sys</sub>·T<sub>sys</sub> - c<sub>p,air,z</sub>·T<sub>z</sub>)
-
-The demand on the actual beams is then
-
-P<sub>beams,dem</sub>=P<sub>c</sub> - P<sub>sup</sub>
-
-We want to know the chilled water flow rate that will give a beam cooling output of *P<sub>beams</sub>*. To obtain this we need to numerically invert *CalcCoolBeam*: given its desired output, we want to know the chilled water flow rate. This numerical inversion is carried out by calling the subroutine *SolveRegulaFalsi*. This is a general utility routine for finding the zero of a function (the *residual* function) of a single independent variable. In this case the residual function is basically
-
-(P<sub>beams,out</sub>-P<sub>beams,dem</sub>)/P<sub>beams,out,max</sub>
-
-*SolveRegulaFalsi* varies the cold water mass flow rate to zero the residual. The water inlet and outlet node flow rates are set to the flow rate found by *SolveRegulaFalsi* and the water outlet node temperature is set to the outlet water temperature from *SolveRegulaFalsi*.
-
-#### References
-
-Documentation Package Update \#2 for DOE-2.1E, Version 107, page 3.152 describes the input and the model for the DOE-2 cooled beam model.
-
-### Constant Volume Dual Duct Air Terminal
-
-#### Overview
-
-The input object AirTerminal:DualDuct:ConstantVolume provides a model for dual duct constant-air-volume (DDCAV) systems that are typically used in special applications where precise temperature and humidity control are required and energy efficiency is not of primary concern. Thermal control for each zone is achieved by mixing air from the hot deck with air from the cold deck to achieve a supply air temperature that will exactly meet the zone load and satisfy the zone thermostat demand. Each zone has its own mixing box which is connected directly to the hot and cold decks. The mixing box dampers change the relative amount of hot and cold air that will be delivered (at a constant volumetric flow rate) to the zone.
-
-#### Model Description
-
-The DDCAV model will attempt to meet all of the thermostatic loads of a particular zone by explicitly calculating the hot and cold deck mass flow rates. For the energy and mass balance equations shown below, the zone load, temperatures, specific heats and the design mass flow rate are all known. These equations can then be solved directly for the hot deck and cold deck mass flow rates.
-
-<div>$$\dot Q_{zone} = \dot m_c C_{p,c} T_c + \dot m_h C_{p,h}T_h - \dot m_d C_{p,z} T_z$$</div>
-
-<div>$$\dot m_d = \dot m_c + \dot m_h$$</div>
-
-Where:
-
-<span>\(\dot Q_{zone}\)</span>= Zone load, W (positive=heating, negative=cooling)
-
-<span>\(C{p_z}\)</span>= Specific heat of zone air, J/kg-K
-
-<span>\(C{p_c}\)</span>= Specific heat of cold deck air, J/kg-K
-
-<span>\(C{p_h}\)</span>= Specific heat of hot deck air, J/kg-K
-
-<span>\({T_z}\)</span>= Zone air dry-bulb temperature, °C
-
-<span>\({T_c}\)</span>= Cold deck air dry-bulb temperature, °C
-
-<span>\({T_h}\)</span>= Hot deck air dry-bulb temperature, °C
-
-<span>\({\dot m_d}\)</span>= System design air mass flow rate through both heating or cooling duct, kg/s
-
-<span>\({\dot m_c}\)</span>= Cold deck air mass flow rate, kg/s
-
-<span>\({\dot m_h}\)</span>= Hot deck air mass flow rate, kg/s
-
-#### Simulation and Control
-
-The simulation first calculates the hot deck and cold deck air mass flow rates required to satisfy the heating/cooling demand on the zone. Once the individual flow rates have been calculated based on temperature control, the zone mixed air conditions are calculated assuming adiabatic mixing of the two air streams.
-
-### Variable Air Volume Dual Duct Air Terminal
-
-#### Overview
-
-The input object AirTerminal:DualDuct:VAV provides a model for dual duct variable-air-volume (DDVAV) systems that are typically used in special applications where both temperature and humidity control as well as energy efficiency are of primary concern.  This system combines the advantages of the standard dual duct system for better thermal control with the possibility to reduce fan energy using a variable speed fan. The DDVAV terminal units contain actuated dampers that vary the amount of central system air supplied to a zone from both the hot and cold deck. Optional user inputs may also be used to control the amount of outdoor air entering the zone.
-
-The DDVAV terminal units described here are used primarily with central air handling equipment with cooling and heating capability. The terminal unit dampers modulate the amount of cold air and hot air as well as the overall flow rate to maintain the zone setpoint temperature(s).
-
-#### Model Description
-
-The DDVAV model will attempt to meet all of the thermostatic loads of a particular zone by first sending air through either the heating duct or the cooling duct depending on whether there is a heating or cooling load (respectively).  Flow rate through the opposite duct is kept at zero and flow through the active duct is varied between the minimum air flow rate (minimum zone air fraction multiplied by the maximum flow rate) and the maximum air flow rate.  If the flow rate to meet the load through either the heating or cooling duct results in a flow outside these ranges, then air must be passed through the other duct as well to avoid over- or under-heating or –cooling. This is done using a conservation of energy and mass analysis of the terminal unit as well as the known inlet and necessary outlet condition to meet the thermal needs of the zone.
-
-When there is no load on the zone, the system could either be scheduled off or be in a “no load� condition.  If the system is scheduled off, the model keeps the flow rate at zero for both the heating and cooling duct.  If in a no load condition, the system attempts to throttle back to the minimum possible flow and then find a balance between flow through the heating and cooling duct that will provide no net conditioning to the space.  This means that the enthalpy of air delivered to the space must be equal to the enthalpy of the (average) air in the zone.
-
-#### DDVAV Terminal Unit Inputs
-
-Like other terminal units, the DDVAV terminal unit requires an availability schedule and inlet and outlet node designations.  The DDVAV terminal unit, like the DD terminal unit, has two inlet nodes (one for the heating duct and one for the cooling duct) and one outlet node.
-
-In addition, the DDVAV terminal unit also has a maximum flow rate and a minimum flow fraction like the VAV terminal unit.  This allows the flow to be throttled back when it is possible to provide the proper amount of conditioning with less flow.  The maximum flow rate can be auto-sized, if desired.
-
-#### Minimum Outdoor Air Control
-
-This dual duct air terminal may also be used to provide a minimum outdoor air quantity. When the air flow rate required to meet the zone load does not provide sufficient outdoor air, the terminal device damper will open to allow sufficient outdoor air to enter the zone. In this case, the terminal damper is controlled based on the air loop’s outdoor air fraction. The outdoor air may be specified as a fixed value per person, per floor area, or per zone or as the required minimum air changes per hour. In addition, these values may be added together to provide a combined minimum outdoor air flow rate or the maximum of each of these values may be used. An outdoor air fraction schedule may also be used to modify the calculation for the minimum amount of outdoor air throughout the simulation (Ref. DesignSpecification:OutdoorAir).
-
-#### Simulation and Control
-
-The simulation begins by determining the air mass flow rate required to satisfy the heating/cooling demand using either the heating duct or cooling duct.
-
-<div>$$C{p_{zone}} = \dot m\left( {C{p_{inlet}},{T_{zone}}} \right)$$</div>
-
-<div>$$C{p_{zone}} = PsyCpAirFnWTdb\left( {{T_{zone}},{T_{inlet}}} \right)$$</div>
-
-<div>$$DeltaCpT = \left( {C{p_{inlet}}} \right)\left( {{T_{inlet}}} \right) - \left( {C{p_{zone}}} \right)\left( {{T_{zone}}} \right)$$</div>
-
-<div>$$ \dot m = \min \left( \dot m_{max}, \max \left( \dot m_{max}\cdot MinAirFlowFrac,\frac{\dot Q_{zone}}{DeltaCpT} \right) \right) $$</div>
-
-where
-
-<span>\(C{p_{zone}}\)</span>  = Specific heat of zone air, J/kg-K
-
-<span>\(C{p_{inlet}}\)</span>  = Specific heat of terminal unit inlet air, J/kg-K
-
-<span>\({\omega_{zone}}\)</span>    = Zone air humidity ratio, kg/kg
-
-<span>\({T_{zone}}\)</span>     = Zone air dry-bulb temperature, °C
-
-<span>\({\omega_{inlet}}\)</span>    = Terminal unit inlet air humidity ratio, kg/kg
-
-<span>\({T_{inlet}}\)</span>     = Terminal unit inlet air dry-bulb temperature, °C
-
-<span>\(\dot m\)</span>    = Zone load, W (positive values denote heating, negative values denote cooling)
-
-<span>\(PsyCpAirFnWTdb\)</span>        = Terminal unit air mass flow rate through either heating or cooling duct, kg/s
-
-<span>\(MinAirFlowFrac\)</span>           = Psychrometric function calculating air specific heat given air humidity ratio and dry-bulb temperature
-
-<span>\(MinAirFlowFrac\)</span>    = User-specified zone minimum air flow fraction
-
-<span>\({\dot m_{max}}\)</span>              = Terminal unit maximum air mass flow rate, kg/s
-
-The outdoor air input requirements, if entered, are then used to adjust the terminal unit air mass flow rate to ensure the correct amount of outdoor air enters the zone (within the constraints of the terminal unit maximum and minimum flow rate inputs). The amount of outdoor air is calculated per the outdoor air requirements and is adjusted by the fraction of outdoor air entering the air loop outdoor air system.
-
-<div>$$\mathop m\limits^\cdot   = MAX\left( {\mathop m\limits^\cdot  ,\,{\raise0.7ex\hbox{${\mathop {{m_{OA}}}\limits^\cdot  }$} \!\mathord{\left/ {\vphantom {{\mathop {{m_{OA}}}\limits^\cdot  } {OAFrac}}}\right.}\!\lower0.7ex\hbox{${OAFrac}$}}} \right)$$</div>
-
-where:
-
-<span>\({\mathop m\limits^\cdot_{OA}}\)</span> = zone outdoor air flow rate, kg/s
-
-<span>\(OAFrac\)</span> = fraction of outdoor air entering the air loop outside air system
-
-The damper position is then calculated as:
-
-<div>$$FRA{C_{damper}} = {\raise0.7ex\hbox{${\dot m}$} \!\mathord{\left/ {\vphantom {{\dot m} {{{\dot m}_{max}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{max}}}$}}$$</div>
-
-where
-
-<span>\(FRA{C_{damper}}\)</span>  = Output variable ‘Zone Air Terminal VAV Damper Position’, fraction of maximum flow
-
-If the flow rate was between the maximum flow rate and the minimum flow rate for the terminal unit, then no other calculations are needed.  However, if the flow was reset to either the maximum or minimum flow rate, then flow through the active duct must be balanced by flow through the other duct to achieve the proper conditioning.
-
-#### References
-
-No specific references.  Refer to the ASHRAE Handbook series for general information on different system types as needed.
-
-### Dual Duct Dedicated Outside Air Terminal with VAV Cooling
-
-#### Overview
-
-The input object AirTerminal:DualDuct:VAV:OutdoorAir provides a model for dedicated outside air combined with recirculated air for cooling.  This air terminal has two inlets and one outlet. The outdoor air inlet has one damper that is controlled to meet the air flow requirements for ventilation.  The second inlet is for cool recirculated air and has a second damper that is controlled to meet the zone’s cooling loads.  The two streams are then mixed and inlet to the zone.  This unit is for central air systems (using AirLoopHVAC object).  Because of the limitation in EnergyPlus of allowing only one air terminal per zone, the dual duct approach offers advantages in that it allows modeling dedicated outdoor air systems (DOAS) and central VAV cooling at the same time.  The original motivation for adding this terminal was to model twin-fan, twin-coil systems.
-
-The recirculated cool air duct is actually optional. If no node name is input for the recirculated air inlet node, then only the outdoor air duct is operational and the air terminal behaves as a single duct.  This offers additional capabilities for single duct DOAS in that this terminal can request outdoor air flows that change over time but are not controlled to meet zone loads.
-
-#### Model Description
-
-The model attempts to meet the ventilation requirements and the cooling loads of a particular zone.  If the zone requires heating, ancillary heating equipment is needed as this terminal cannot do any heating.  The model first determines the current required outdoor air flow rate for ventilation and then calculates the flow of cool air needed to reach the cooling setpoint.
-
-The outdoor air rate is controlled by the schedule and specifications contained in a DesignSpecification:OutdoorAir object and can be based on flows per person, per zone, per area, or air changes per hour.  Using the key CurrentOccupancy, the per person rate can be set to operate based on the current occupancy level to model demand controlled ventilation. Using the key DesignOccupancy it can be set to operate based on the design, or maximum, level of occupancy.   The outdoor air inlet side of the terminal is assigned a design maximum flow rate based on the largest flow rates specified by the associated DesignSpecification:OutdoorAir object. This maximum for the outdoor air is used to calculate the damper position and contributes to the overall maximum if that is autosized.
-
-The recirculated cool air flow rate is controlled to meet the zone cooling loads.  The first step is to calculate the impact that the outdoor air flow has on the loads starting with the specific heats.
-
-<div>$${c_{p,zone}} = PsyCpAirFnWTdb\left( {{\omega_{zone}},{T_{zone}}} \right)$$</div>
-
-<div>$${c_{p,OA}} = PsyCpAirFnWTdb\left( {{\omega_{OA}},{T_{OA}}} \right)$$</div>
-
-<div>$${c_{p,RC}} = PsyCpAirFnWTdb\left( {{\omega_{RC}},{T_{RC}}} \right)$$</div>
-
-where,
-
-<span>\({c_{p,zone}} = \)</span> specific heat of zone air being served by the terminal unit, J/kg-K
-
-<span>\({c_{p,OA}} = \)</span> specific heat of outdoor air entering the terminal unit, J/kg-K
-
-<span>\({c_{p,RC}} = \)</span> specific heat of the recirculated (cool) air entering the terminal unit (if present), J/kg-K
-
-<span>\({\omega_{zone}} = \)</span>humidity ratio of the zone air, kg/kg
-
-<span>\({\omega_{OA}} = \)</span>humidity ratio of the outdoor air entering the terminal unit, kg/kg
-
-<span>\({\omega_{RC}} = \)</span>humidity ratio of the recirculated air entering the terminal unit, kg/kg
-
-<span>\({T_{zone}} = \)</span>air drybulb temperature of the zone, ºC
-
-<span>\({T_{OA}} = \)</span>air drybulb temperature of the outdoor air entering the terminal unit, ºC
-
-<span>\({T_{RC}} = \)</span>air drybulb temperature of the recirculated cool air entering the terminal unit, ºC
-
-<span>\(PsyCpAirFnWTdb\)</span> is a psychrometric function for calculating the specific heat of moist air as a function of humidity ratio and drybulb temperature.
-
-The contribution to zone load provided by the outdoor air toward meeting the cooling setpoint, <span>\({\dot Q_{OA}}\)</span> (W), is then calculated using:
-
-<div>$${\dot Q_{OA}} = {\dot m_{OA}}\left( {{c_{p,OA}}{T_{OA}} - {c_{p,zone}}{T_{zonesetpoint}}} \right)$$</div>
-
-where,
-
-<span>\({\dot m_{OA}} = \)</span>is the mass flow rate of outdoor air determined by the outdoor air requirement, kg/s
-
-<span>\({T_{zonesetpoint}} = \)</span>is the zone cooling setpoint drybulb temperature, ºC
-
-This is then used to calculate the load that the recirculated cool air should deliver, <span>\({Q_{RC}}\)</span> (W):
-
-<div>$${\dot Q_{RC}} = {\dot Q_{ToCoolSetpointRemain - }}{\dot Q_{OA}}$$</div>
-
-where,
-
-<span>\({\dot Q_{ToCoolSetpointRemain = }}\)</span> is the remaining load to cooling setpoint as determined by Predictor and including the impacts of any other zone equipment sequenced before this terminal. Then the recirculated cool air mass flow rate, <span>\({\dot m_{RC}}\)</span> (kg/s), is calculated using:
-
-<div>$${\dot m_{RC}} = \frac{{{{\dot Q}_{RC}}}}{{\left( {{c_{p,RC}}{T_{RC}} - {c_{p,zone}}{T_{zone}}} \right)}}$$</div>
-
-The model also includes a form of damping where the last three values for <span>\({\dot m_{RC}}\)</span> are stored and used to detect if the solution is oscillating from one iteration to the next and if it is then the new value is not used but rather the value from the previous iteration is used.  Once the two mass flows are known, the moist air properties of the outlet node are calculated using mass flow weighting.
-
-#### References
-
-Sekhar, S. C., K. W. Tham, et al. (2004). Development of energy-efficient single-coil twin-fan air-conditioning system with zonal ventilation control, Nashville, TX, United states, Amer. Soc. Heating, Ref. Air-Conditoning Eng. Inc.
-
-Boilers <a name="Boilers"></a>
--------
-
-### Simple Hot Water Boiler
-
-The input object Boiler:HotWater provides a simple model for boilers that only requires the user to supply the nominal boiler capacity and thermal efficiency. An efficiency curve can also be used to more accurately represent the performance of non-electric boilers but is not considered a required input. The fuel type is input by the user for energy accounting purposes.
-
-The model is based the following three equations
-
-<div>$$OperatingPartLoadRatio = \frac{{BoilerLoad}}{{BoilerNomCapacity}}$$</div>
-
-<div>$$TheoreticalFuelUse = \frac{{BoilerLoad}}{{NominalThermalEfficiency}}$$</div>
-
-<div>$$FuelUsed = \frac{{TheoreticalFuelUse}}{{BoilerEfficiencyCurveOuput}}$$</div>
-
--or-
-
-<div>$$FuelUsed = \frac{{BoilerLoad}}{{\left( {NominalThermalEfficiency} \right)\left( {BoilerEfficiencyCurveOutput} \right)}}$$</div>
-
-The final equation above includes the impact of the optional boiler efficiency performance curve. To highlight the use of the normalized boiler efficiency curve, the fuel use equation is also shown in an expanded format. The normalized boiler efficiency curve represents the changes in the boiler’s nominal thermal efficiency due to loading and changes in operating temperature. If the optional boiler efficiency curve is not used, the boiler’s nominal thermal efficiency remains constant throughout the simulation (i.e., BoilerEfficiencyCurveOutput = 1).
-
-When a boiler efficiency performance curve is used, any valid curve object with 1 or 2 independent variables may be used. The performance curves are accessed through EnergyPlus’ built-in performance curve equation manager (curve objects). The linear, quadratic, and cubic curve types may be used when boiler efficiency is solely a function of boiler loading, or part-load ratio (PLR). These curve types are used when the boiler operates at the specified setpoint temperature throughout the simulation. Other curve types may be used when the boiler efficiency can be represented by both PLR and boiler operating temperature. Examples of valid single and dual independent variable equations are shown below. For all curve types, PLR is always the x independent variable. When using curve types with 2 independent variables, the boiler water temperature (Twater) is always the y independent variable and can represent either the inlet or outlet temperature depending on user input.
-
-#### Single independent variable:
-
-* <span>\(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right)\)</span> (Linear)
-
-* <span>\(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right) + C3{\left( {PLR} \right)^2}\)</span> (Quadratic)
-
-* <span>\(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right) + C3{\left( {PLR} \right)^2} + C4{(PLR)^3}\)</span> (Cubic)
-
-#### Dual independent variables:
-
-* <span>\(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right) + C3{\left( {PLR} \right)^2} + \left( {C4 + C5\left( {PLR} \right) + C6{{\left( {PLR} \right)}^2}} \right)\left( {Twater} \right)\)</span> (QuadraticLinear)
-
-* <span>\(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right) + C3{\left( {PLR} \right)^2} + C4\left( {Twater} \right) + C5{(Twater)^2} + C6(PLR)(Twater)\)</span> (Biquadratic)
-
-* <span>\(BoilerEfficiencyCurve = C1 + C2\left( {PLR} \right) + C3{\left( {PLR} \right)^2} + C4\left( {Twater} \right) + C5{(Twater)^2} + C6\left( {PLR} \right)\left( {Twater} \right) + C7{(PLR)^3} + C8{(Twater)^3} + C9{\left( {PLR} \right)^2}\left( {Twater} \right) + C10\left( {PLR} \right){(Twater)^2}\)</span> (Bicubic)
-
-When a boiler efficiency curve is used, a constant efficiency boiler may be specified by setting C1 = 1 and all other coefficients to 0. A boiler with an efficiency proportional to part-load ratio or which has a non-linear relationship of efficiency with part-load ratio will typically set the coefficients of a linear, quadratic, or cubic curve to non-zero values. Using other curve types allows a more accurate simulation when boiler efficiency varies as a function of part-load ratio and as the boiler outlet water temperature changes over time due to loading or as changes occur in the water temperature setpoint.
-
-The parasitic electric power is calculated based on the user-defined parasitic electric load and the operating part load ratio calculated above. The model assumes that this parasitic power does not contribute to heating the water.
-
-<div>$${P_{parasitic}} = {P_{load}}\left( {PLR} \right)$$</div>
-
-where:
-
-<span>\({P_{parasitic}}\)</span>= parasitic electric power (W), average for the simulation time step
-
-<span>\({P_{load}}\)</span>    = parasitic electric load specified by the user (W)
-
-### Steam Boiler
-
-#### Description of Model
-
-A steam boiler is the essential part of a building steam heating system and can be described as primary driver of the steam loop.  It is the component that maintains the desired loop temperature.
-
-The emphasis in EnergyPlus was laid on developing a building simulation model for steam boiler with ability to model detailed boiler performance without the cost of exhaustive user inputs to the boiler model.  The Boiler:Steam input object is used on the plant loop supply side of EnergyPlus with the primary purpose of supplying steam to the heating coils, which constitute the demand side of the loop.
-
-The steam boiler is a variable mass flow rate device.  The mass flow rate of steam through the boiler is determined by the heating demand on the loop which in turn is determined by the equipment that is hooked to the demand side of the loop, namely the steam coils and hot water heater.  In short, the steam coil determines the mass flow rate of steam required for heating the zone to its required setpoint, the mixer sums up the total steam demanded by each of the individual coils and reports it to the boiler via the pump.
-
-![SteamBoilerInSteamLoop](media/image2932.png)
-
-Figure 158.  Schematic of Steam Boiler in the Steam loop
-
-
-
-Figure 158 describes the rudimentary loop structure with steam flowing from coils to boiler.  It is essential to mention that it is the coils that determine the mass of steam required and the boiler simply delivers the required mass flow at desired temperature provided it is adequately sized.  The algorithm for determining the mass flow rate is structured on the demand side and the variable flow boiler has no role to play in determining the steam mass flow.
-
-Figure 159 outlines the simple steam boiler model.  Sub cooled water enters the variable flow boiler through the pump, the boiler inputs energy to water stream consuming fuel, boiler losses are accounted via boiler efficiency.  The boiler delivers steam at a quality equal to 1.0 at saturated condition.
-
-The advantage of steam heating systems over hot water is the high latent heat carrying capacity of steam, which reduces the mass flow rate of the fluid required.  The amount of superheated and sub cooled heat transfer in Steam heating systems is negligible, latent heat transfer accounts for almost all of the heat exchange into the zones via steam to air heat exchangers.
-
-![SteamBoilerOperation](media/image2933.png)
-
-Figure 159.  Schematic of Steam Boiler Operation
-
-Boiler Load is a summation of sensible and latent heat addition to the water stream as described with the following equation.  The mass flow rate through the boiler is known, while delta temp is the temperature difference between the boiler inlet and boiler outlet.  Latent heat of steam is calculated at loop operating temperature.
-
-<div>$${Q_B} = \,\dot m\, \times \left[ {({c_{p,w}} \times \Delta T)\,\,\, + \,\,\,{h_{fg}}} \right]$$</div>
-
-Theoretical fuel used is calculated with the following equation.  Boiler efficiency is a user input and accounts for all the losses in the steam boiler.
-
-<div>$${F_t} = \frac{{{Q_B}}}{{{\eta_B}}}$$</div>
-
-The operation part load ratio is calculated with the following equation.  This is later used to calculate the actual fuel consumption, its ratio of boiler load to boiler nominal capacity.
-
-<div>$${O_{PLR}} = \frac{{{Q_B}}}{{{Q_{B,N}}}}$$</div>
-
-The actual fuel consumption by the boiler is calculated as using the following equation, where C1, C2, and C3 are the Part Load Ratio coefficients.
-
-<div>$${F_{}} = \frac{{{F_t}}}{{{C_1}\,\, + \,\,{C_2}\,\, \times \,\,{O_{PLR}}\,\, + \,\,{C_3} \times \,{O_{PLR}}^2\,}}$$</div>
-
-Essentially the boiler model provides a first order approximation of performance for fuel oil, gas, and electric boilers.  Boiler performance is based on theoretical boiler efficiency and a single quadratic fuel use-part load ratio curve represented in the equation above.  This single curve accounts for all combustion inefficiencies and stack losses.
-
-The control algorithm for a steam boiler is an important issue.  The user may want the boiler to be undersized and in such a case it will not be able to meet the demand side steam flow request.  Subsequently the boiler load exceeds the boiler nominal capacity.  The boiler operates at its nominal capacity but is unable to meet the plant heating demand.  Pseudo code from EnergyPlus has been used to describe the control logic used in the steam boiler simulation.
-
-
-
-\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*PSEUDO CODE SECTION STARTS\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-At start of simulation an initial value of steam mass flow rate is calculated.  This is required to start the flow of steam around the loop.
-
-<div>$$If\,\,\,\,(FirstTimeThrough)\,\,\,THEN$$</div>
-
-Calculate the boiler supply steam mass flow rate at start of simulation.
-
-<div>$$\,{\dot m_s}\,\, = \,\,\frac{{{Q_B}}}{{{h_{fg\,\,\, + }}\,\,{c_{p,w}}\,\, \times \Delta {T_{loop}}\,\,}}$$</div>
-
-<div>$$ELSE$$</div>   ! Not first time through
-
-Steam boiler calculations rely heavily on the variable <span>\(\dot m\)</span><sub>b</sub>, boiler mass flow rate.  This variable <span>\(\dot m\)</span><sub>b</sub> is the assigned equal to mass flow at boiler inlet node for preliminary calculations.
-
-<div>$$\,{\dot m_b}\,\,\, = \,\,\,\mathop {\,{{\dot m}_{Inlet\_Node}}}\limits^{} $$</div>
-
-Calculating the boiler delta temperature difference between the inlet and outlet nodes.  This calculation is used to determine various boiler control situation.
-
-<div>$$\Delta {T_{in\_out}}\,\, = \,\,{T_{SP}}\,\, - \,\,{T_{in}}$$</div>
-
-In case the temperature difference calculated with the previous equation equation  is zero then the boiler just needs to supply latent heat to steam, else the boiler performs its normal load calculations by providing both sensible and latent heat to the inlet stream.
-
-<div>$$If\,\,(\Delta {T_{in\_out}}\,\, &lt; \,\,\,\,0\,\,\,)\,\,\,THEN$$</div>
-
-<div>$${Q_B}\,\, = \,\,\,{\dot m_b}\,\,\, \times \,\,{h_{fg}}$$</div>
-
-<div>$$ELSE$$</div>
-
-<div>$${Q_B}\,\, = \,\,\,{\dot m_b}\,\,\, \times \,\,(\,\,\,{h_{fg}} + \,\,{c_{p,w}} \times \Delta {T_{in\_out}}\,\,)$$</div>
-
-<div>$$End\,\,If$$</div>
-
-Sometimes the boiler load Q<sub>B</sub> is greater than the demand side requested load at the current time step, which may occur because the boiler inlet conditions is from previous time step.  There is sudden fall in request of steam mass flow from the demand side.  The boiler now recalculates its new mass flow and adjusts to these new conditions.
-
-<div>$$If\,\,({Q_B}\,\, > \,\,{Q_{HeatingDemand}}\,\,\,)\,\,\,THEN$$</div>
-
-Boiler load is set equal to the new boiler heating demand and steam mass flow rate is recalculated.
-
-<div>$${Q_B}\,\, = \,\,{Q_{HeatingDemand}}$$</div>
-
-<div>$$\,{\dot m_s}\,\,\, = \,\,\frac{{{Q_B}}}{{{h_{fg\,\,\, + }}\,\,{c_{p,w}}\,\, \times \Delta {T_{loop}}\,\,}}$$</div>
-
-<div>$$End\,\,If$$</div>
-
-In case the requested load exceeds the boiler nominal capacity, which is its maximum heating capacity.  In this case the requested steam mass flow is not met and the zone is not heated adequately.  This happens if the boiler is undersized.  The steam mass flow rate is recalculated at nominal capacity.
-
-<div>$$If\,\,({Q_B}\,\, > \,\,{Q_{No\min al\_Capacity}}\,\,\,)\,\,\,THEN$$</div>
-
-Boiler load is set equal to boiler nominal capacity and steam mass flow rate recalculated.
-
-<div>$${Q_B}\,\, = \,\,{Q_{No\min al\_Capacity}}$$</div>
-
-<div>$$\,{\dot m_s}\,\,\, = \,\,\frac{{{Q_B}}}{{{h_{fg\,\,\, + }}\,\,{c_{p,w}}\,\, \times \Delta {T_{loop}}\,\,}}$$</div>
-
-<div>$$End\,\,If$$</div>
-
-<div>$$End\,\,If$$</div>
-
-End If statement for the boiler load control algorithm.  This algorithm determines all possible control conditions that might while simulating a system in EnergyPlus.
-
-
-
-\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*PSEUDO CODE SECTION ENDS\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-If the boiler operating pressure exceeds the maximum allowable boiler pressure, the simulation trips and outputs a warning regarding the same.  This notifies the user about potential system pressure sizing problems.
-
-Integration of the steam boiler simulation model in EnergyPlus required developing number of subroutines, which operate in sequence.  These subroutines are designed to read inputs from the input file, initialize the variables used in the boiler simulation model, simulate the boiler performance, update the node connections, and report the required variables.  In case the user has difficulty with boiler inputs, provisions have been made to auto size the boiler nominal capacity and maximum steam flow rate.  These two values play an important role in sizing the boiler.
-
-#### Model Assumptions
-
-The EnergyPlus boiler model is “simple� in the sense that it requires the user to supply the theoretical boiler efficiency.  The combustion process is not considered in the model.  The model is independent of the fuel type, which is input by the user for energy accounting purposes only.  This is an ideal model for Building Simulation Program such that it utilizes the desired amount of resources in terms of simulation run time, but successfully provides fairly good sizing parameters for an actual boiler.
-
-It is assumed that the steam boiler operates to maintain a desired temperature, the temperature being saturation temperature of steam and corresponding to this saturation temperature there exist a single value of saturation pressure at which the loop operates.  Hence the boiler could either be saturation pressure controlled or temperature controlled.  Since users would have better idea of steam temperatures rather than pressure the boiler inputs are designed for temperature control.
-
-#### Nomenclature for Steam Loop
-
-Table 50.  Steam Loop Nomenclature
-
-<table class="table table-striped">
-<tr>
-<th><span>\({Q_B}\)</span></th>
-<th>Boiler Heat Transfer.  W.</th>
-</tr>
-<tr>
-<td><span>\({Q_{B,N}}\)</span></td>
-<td>Boiler Nominal Capacity.  W.</td>
-</tr>
-<tr>
-<td><span>\(\,{O_{PLR}}\)</span></td>
-<td>Boiler Operating Part Load Ratio. </td>
-</tr>
-<tr>
-<td><span>\(\Delta {T_{sc}}\)</span></td>
-<td>Degree of subcooling in coil. </td>
-</tr>
-<tr>
-<td><span>\(\Delta {T_{in\_out}}\)</span></td>
-<td>Temperature difference across the steam boiler.  ºC.</td>
-</tr>
-<tr>
-<td><span>\({\rho_w}\)</span></td>
-<td>Density of condensate entering the pump.  Kg/m3. </td>
-</tr>
-<tr>
-<td><span>\({Q_{Des}}\)</span></td>
-<td>Design Load on the steam coil.  W.</td>
-</tr>
-<tr>
-<td><span>\({h_{f,\,n}}\)</span></td>
-<td>Enthalpy of fluid at point n on the Ts diagram.  J/kg.</td>
-</tr>
-<tr>
-<td><span>\({P_{Frac}}\)</span></td>
-<td>Fraction of Pump Full Load Power.  W.</td>
-</tr>
-<tr>
-<td><span>\({F_{m,f}}\)</span></td>
-<td>Fractional Motor Power Lost to Fluid.  W.</td>
-</tr>
-<tr>
-<td><span>\({Q_{a,l}}\)</span></td>
-<td>Heating load on the Air Loop Steam Coil.  W.</td>
-</tr>
-<tr>
-<td><span>\({Q_{z,c}}\)</span></td>
-<td>Heating load on the Zone Steam Coil.  W.</td>
-</tr>
-<tr>
-<td><span>\({h_{fg,{T_{Loop}}}}\)</span> </td>
-<td>Latent heat of steam at Loop operating Temperature.  J/kg.</td>
-</tr>
-<tr>
-<td><span>\({h_{fg}}\)</span></td>
-<td>Latent Heat of Steam.  J/kg.</td>
-</tr>
-<tr>
-<td><span>\({Q_{L,H}}\)</span></td>
-<td>Latent Heat Part of the Heating Coil Load.  W.</td>
-</tr>
-<tr>
-<td><span>\(\Delta {Q_{loss}}\)</span></td>
-<td>Loop losses in steam coil.  W.</td>
-</tr>
-<tr>
-<td><span>\(\Delta {T_{loop\,\,}}\)</span></td>
-<td>Loop Temperature Difference.</td>
-</tr>
-<tr>
-<td><span>\({\dot m_a}\)</span></td>
-<td>Mass flow rate for steam coil Kg/s.</td>
-</tr>
-<tr>
-<td><span>\({\dot m_{in}}\)</span></td>
-<td>Mass flow rate of steam entering the steam coil .Kg/s.</td>
-</tr>
-<tr>
-<td><span>\({\dot m_{a,l}}\)</span></td>
-<td>Mass flow rate of steam for Air loop steam coil Kg/s</td>
-</tr>
-<tr>
-<td><span>\({\dot m_{z,c}}\)</span></td>
-<td>Mass flow rate of steam for zone steam coil Kg/s.</td>
-</tr>
-<tr>
-<td><span>\({\dot m_s}\)</span></td>
-<td>Mass flow rate of steam.  Kg/s.</td>
-</tr>
-<tr>
-<td><span>\({\dot m_{loop}}\)</span></td>
-<td>Mass flow rate of steam for the steam loop.  Kg/s.</td>
-</tr>
-<tr>
-<td><span>\(\dot m\)</span></td>
-<td>Mass of condensate entering the pump.  Kg/s.</td>
-</tr>
-<tr>
-<td><span>\({\dot m_{a,\max }}\)</span> </td>
-<td>Maximum allowed mass flow rate of air.  Kg/s</td>
-</tr>
-<tr>
-<td><span>\({\dot m_{S,\max }}\)</span></td>
-<td>Maximum Mass flow rate of steam Kg/s</td>
-</tr>
-<tr>
-<td><span>\({\dot m_{B,Supply}}\)</span></td>
-<td>Maximum steam mass flow rate supplied by boiler.  Kg/s.</td>
-</tr>
-<tr>
-<td><span>\({\dot V_{w,\max }}\,\,\)</span></td>
-<td>Maximum Volume flow rate of condensate in pump.  m<sup>3</sup> /s.</td>
-</tr>
-<tr>
-<td><span>\({\dot V_{w,loop}}\)</span></td>
-<td>Maximum Volume flow rate of condensate in steam loop.  m<sup>3</sup> /s.</td>
-</tr>
-<tr>
-<td><span>\({T_{a,\,\,in,\,\,\min }}\)</span></td>
-<td>Minimum inlet air temperature possible.  ºC.</td>
-</tr>
-<tr>
-<td><span>\({P_n}\,\,\)</span></td>
-<td>Nominal Power Capacity for condensate pump.  W.</td>
-</tr>
-<tr>
-<td><span>\({P_{nom}}\)</span></td>
-<td>Nominal power of the pump.  W.</td>
-</tr>
-<tr>
-<td><span>\({H_n}\)</span></td>
-<td>Nominal Pump Head.  M.</td>
-</tr>
-<tr>
-<td><span>\({\dot V_{nom}}\)</span></td>
-<td>Nominal volume flow rate through the condensate pump.  m<sup>3</sup> /s.</td>
-</tr>
-<tr>
-<td><span>\(PLR\)</span></td>
-<td>Part Load Ratio for condensate pump.</td>
-</tr>
-<tr>
-<td><span>\({\eta_{\rm{p}}}\)</span></td>
-<td>Pump efficiency.</td>
-</tr>
-<tr>
-<td><span>\({\eta_m}\)</span></td>
-<td>Pump Motor Efficiency.</td>
-</tr>
-<tr>
-<td><span>\({P_{}}\)</span></td>
-<td>Pump Power.  W.</td>
-</tr>
-<tr>
-<td><span>\({Q_{S,H}}\)</span></td>
-<td>Sensible Heat Part of the Heating Coil Load.  W.</td>
-</tr>
-<tr>
-<td><span>\({T_{sp}}\)</span></td>
-<td>Setpoint Temperature of the zone.  ºC.</td>
-</tr>
-<tr>
-<td><span>\({T_{a,out,SP}}\)</span></td>
-<td>Setpoint air outlet temperature for the steam coil.  ºC.</td>
-</tr>
-<tr>
-<td><span>\({P_S}\)</span></td>
-<td>Shaft power of the pump.  W.</td>
-</tr>
-<tr>
-<td><span>\(\,\,{c_{p,\,a}}\)</span></td>
-<td>Specific Heat Capacity for Air.  J/Kg K.</td>
-</tr>
-<tr>
-<td><span>\(\,\,{c_{p,\,w}}\)</span></td>
-<td>Specific Heat Capacity for Water.  J/Kg K.</td>
-</tr>
-<tr>
-<td><span>\({\eta_B}\)</span></td>
-<td>Steam Boiler Efficiency.</td>
-</tr>
-<tr>
-<td><span>\(\,Ta,\,i{n_{}}\,\)</span></td>
-<td>Temperature of air entering the coil.  ºC.</td>
-</tr>
-<tr>
-<td><span>\({T_a}\)</span></td>
-<td>Temperature of air entering the steam coil.  ºC.</td>
-</tr>
-<tr>
-<td><span>\(Ta,out\,\,\,\,\,\)</span></td>
-<td>Temperature of air leaving the coil.  ºC.</td>
-</tr>
-<tr>
-<td><span>\(Ts,in\)</span></td>
-<td>Temperature of steam entering the coil.  ºC.</td>
-</tr>
-<tr>
-<td><span>\({F_t}\)</span></td>
-<td>Theoretical Fuel Consumption by the Steam Boiler.  W.</td>
-</tr>
-<tr>
-<td><span>\({\dot m_{coils,R}}\)</span></td>
-<td>Total Mass flow rate requested by all the steam coils.  Kg/s.</td>
-</tr>
-<tr>
-<td><span>\(\dot V\)</span></td>
-<td>Volume of condensate entering the pump.  m<sup>3</sup> /s.</td>
-</tr>
-<tr>
-<td><span>\(Tw,\,out\)</span></td>
-<td>Water outlet temperature from pump.  ºC.</td>
-</tr>
-
-</table>
-
-#### References
-
-ASHRAE Handbook. 1996. HVAC Systems and Equipment, Air Conditioning and Heating Systems.  Chapter 10, Steam Systems.  pp.* * 10.1-10.16. 1996.
-
-*BLAST 3.0 Users Manual*. 1999. Building Systems Laboratory.  Urbana-Champaign: Building Systems Laboratory, Department of Mechanical and Industrial Engineering, University of Illinois.
-
-Chillar, R.J. 2005. “Development and Implementation of a Steam Loop In The Building Energy Simulation Program EnergyPlus,� M.S. Thesis, Department of Mechanical and Industrial Engineering, University of Illinois at Urbana-Champaign.
-
-*TRNSYS 16 User Manual*. 2004. A Transient System Simulation Program. Solar Energy Laboratory, Madison. University of Wisconsin-Madison.
-
-El-Wakil, M. M. 1984. Power Plant Technology, McGraw Hill, New York, pp.   30-72.
-
-Babcock & Wilcox. 1978. Steam-Its Generation and Use, The Babcock & Wilcox Company, New York ,Section I, II, IV, and VII.
-
-S.A. Klein. 2004. Engineering Equation Solver EES. University of Wisconsin Madison.
-
-Chillers <a name="Chillers"></a>
---------
-
-### Absorption Chiller
-
-The input object Chiller:Absorption provides a model for absorption chillers that is an empirical model of a standard absorption refrigeration cycle.  The condenser and evaporator are similar to that of a standard chiller, which are both water-to-water heat exchangers.  The assembly of a generator and absorber provides the compression operation.  Low-pressure vapor from the evaporator is absorbed by the liquid solution in the absorber.  A pump receives low-pressure liquid from the absorber, elevates the pressure of the liquid, and delivers the liquid to the generator.  In the generator, heat from a high temperature source (hot water or steam) drives off the vapor that has been absorbed by the solution.  The liquid solution returns to the absorber through a throttling valve whose purpose is to provide a pressure drop to maintain the pressure difference between the generator and absorber.  The heat supplied to the absorber can be waste heat from a diesel jacket, or the exhaust heat from diesel, gas, and steam turbines.  For more information on absorption chillers, see the Input/Output Reference Document (Object: Chiller:Absorption).
-
-The part-load ratio of the absoprtion chiller’s evaporator is simply the actual cooling effect produced by the chiller divided by the maximum cooling effect available.
-
-<div>$$PLR = {\raise0.7ex\hbox{${{{\dot Q}_{evap}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{evap}}} {{{\dot Q}_{evap,\,\,rated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot Q}_{evap,\,\,rated}}}$}}$$</div>
-
-where
-
-<span>\(PLR\)</span> = part-load ratio of chiller evaporator
-
-<span>\({\dot Q_{evap}}\)</span> = chiller evaporator load [W]
-
-<span>\({\dot Q_{evap,\,rated}}\)</span> = rated chiller evaporator capacity [W]
-
-This absorption chiller model is based on a polynomial fit of absorber performance data.  The Generator Heat Input Part Load Ratio Curve is a quadratic equation that determines the ratio of the generator heat input to the *demand* on the chiller’s evaporator (Q<sub>evap</sub>).
-
-<div>$$GeneratorHeatInputRatio = \frac{{C1}}{{PLR}} + C2 + C3\left( {PLR} \right)$$</div>
-
-The Pump Electric Use Part Load Ratio Curve is a quadratic equation that determines the ratio of the actual absorber pumping power to the nominal pumping power.
-
-<div>$$ElectricInputRatio = C1 + C2 * PLR + C3 * PL{R^2}$$</div>
-
-Thus, the coefficient sets establish the ratio of heat power in-to-cooling effect produced as a function of part load ratio.  The ratio of heat-power-in to cooling-effect-produced is the inverse of the coefficient of performance.
-
-If the operating part-load ratio is greater than the minimum part-load ratio, the chiller will run the entire time step and cycling will not occur (i.e. *CyclingFrac* = 1). If the operating part-load ratio is less than the minimum part-load ratio, the chiller will be on for a fraction of the time step equal to *CyclingFrac*. Steam (or hot water) and pump electrical energy use are also calculated using the chiller part-load cycling fraction.
-
-<div>$$CyclingFrac = MIN\left( {1,\frac{{PLR}}{{PL{R_{min}}}}} \right)$$</div>
-
-<div>$${\dot Q_{generator}} = GeneratorHeatInputRatio\left( {{{\dot Q}_{evap}}} \right)\left( {CyclingFrac} \right)$$</div>
-
-<div>$${\dot Q_{pump}} = ElectricInputRatio\left( {{P_{pump}}} \right)\left( {CyclingFrac} \right)$$</div>
-
-where
-
-<span>\(CyclingFrac\)</span> = chiller part-load cycling fraction
-
-<span>\(PL{R_{min}}\)</span> = chiller minimum part-load ratio
-
-<span>\({\dot Q_{generator}}\)</span> = generator input power [W]
-
-<span>\({\dot Q_{pump}}\)</span> = absorbtion chiller pumping power [W]
-
-The evaporator water mass flow rate is calculated based on the Chiller Flow Mode as follows.
-
-**Constant Flow Chillers:**
-
-**<span>\({\dot m_{evap}} = {\dot m_{evap,max}}\)</span>**
-
-**Variable Flow Chillers:**
-
-<div>$$\Delta {T_{evap}} = {T_{evap,\,in}} - {T_{evap,\,SP}}$$</div>
-
-<div>$${\dot m_{evap}} = {\raise0.7ex\hbox{${{{\dot Q}_{evap}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{evap}}} {{C_{p,\,evap}}\left( {\Delta {T_{evap}}} \right)}}}\right.}\!\lower0.7ex\hbox{${{C_{p,\,evap}}\left( {\Delta {T_{evap}}} \right)}$}}$$</div>
-
-where
-
-<span>\({\dot m_{evap}}\)</span>          = chiller evaporator water mass flow rate (kg/s)
-
-<span>\({\dot m_{evap,\,max}}\)</span>     = chiller design evaporator water mass flow rate (kg/s)
-
-<span>\(\Delta {T_{evap}}\)</span>        = chiller evaporator water temperature difference (ºC)
-
-<span>\({T_{evap,\,in}}\)</span>        = chiller evaporator inlet water temperature (ºC)
-
-<span>\({T_{evap,\,SP}}\)</span>       = chiller evaporator outlet water setpoint temperature (ºC)
-
-<span>\({C_p}\)</span>              = specific heat of water entering evaporator (J/kg•ºC)
-
-The evaporator outlet water temperature is then calculated based on the cooling effect produced and the evaporator entering water temperature.
-
-<div>$${T_{evap,out}} = {T_{evap,in}} + {\raise0.7ex\hbox{${{{\dot Q}_{evap}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{evap}}} {{C_{p,\,evap}}\left( {{{\dot m}_{evap}}} \right)}}}\right.}\!\lower0.7ex\hbox{${{C_{p,\,evap}}\left( {{{\dot m}_{evap}}} \right)}$}}$$</div>
-
-where
-
-<span>\({T_{evap,out}}\)</span> = chiller evaporator outlet water temperature [ºC]
-
-<span>\({T_{evap,in}}\)</span> = chiller evaporator inlet water temperature [ºC]
-
-<span>\({C_{p,\,evap}}\)</span> = specific heat of chiller evaporator inlet water [J/kg/ºC]
-
-<span>\({\dot m_{evap}}\)</span> = chiller evaporator water mass flow rate [kg/s]
-
-The condenser heat transfer and condenser leaving water temperature are also calculated.
-
-<div>$${\dot Q_{cond}} = {\dot Q_{evap}} + {\dot Q_{generator}} + {\dot Q_{pump}}$$</div>
-
-<div>$${T_{cond,out}} = {T_{cond,in}} + {\raise0.7ex\hbox{${{{\dot Q}_{cond}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{cond}}} {{C_{p,\,cond}}\left( {{{\dot m}_{cond}}} \right)}}}\right.}\!\lower0.7ex\hbox{${{C_{p,\,cond}}\left( {{{\dot m}_{cond}}} \right)}$}}$$</div>
-
-where
-
-<span>\({\dot Q_{cond}}\)</span> = chiller condenser heat transfer rate [W]
-
-<span>\({T_{cond,out}}\)</span> = chiller condenser outlet water temperature [ºC]
-
-<span>\({T_{cond,in}}\)</span> = chiller condenser inlet water temperature [ºC]
-
-<span>\({C_{p,\,cond}}\)</span> = specific heat of chiller condenser inlet water [J/kg/ºC]
-
-<span>\({\dot m_{cond}}\)</span> = chiller condenser water mass flow rate [kg/s]
-
-The absorption chiller can model the impact of steam or hot water entering the generator, although the connection of the steam (hot water) nodes to a plant is not actually required. The calculations specific to the generator depend on the type of fluid used and are described here in further detail.
-
-#### Steam Loop Calculations
-
-When a steam loop is used and the inlet and outlet node names are specified (i.e. the nodes are connected to a steam loop), the generator outlet node steam mass flow rate and temperature are calculated based on the generator input power, latent heat of steam, the specific heat of water, and the amount of subcooling in the steam generator. The model assumes dry saturated steam enters the absorption chiller’s generator and exits the generator as a subcooled liquid. The temperature leaving the generator is calculated based on the user entered amount of liquid subcooling in the generator. The effect of subcooling of the liquid (condensate) in the pipe returning to the boiler is not modeled.
-
-<div>$${\dot m_{steam}}\,\,\,\, = \,\,\,\,\,\frac{{{{\dot Q}_{generator}}}}{{{h_{fg}} + {c_{p,\,water}} \times \Delta {T_{sc}}}}$$</div>
-
-<div>$${T_{generator,out}} = {T_{generator,in}} - \Delta {T_{sc}}$$</div>
-
-where
-
-<span>\({\dot m_{steam}}\)</span> = chiller steam mass flow rate [kg/s]
-
-<span>\({h_{fg}}\)</span> = latent heat of steam [J/kg]
-
-<span>\({c_{p,\,water}}\)</span> = specific heat of saturated water in the generator [J/Kg ºK]
-
-<span>\(\Delta {T_{sc}}\)</span> = amount of subcooling in steam generator [ºC]
-
-<span>\({T_{generator,out}}\)</span> = generator steam outlet node temperature [ºC]
-
-<span>\({T_{generator,in}}\)</span> = generator steam inlet node temperature [ºC]
-
-#### Hot Water Loop Calculations
-
-When a hot water loop is used and the inlet and outlet node names are specified (i.e. the nodes are connected to a hot water loop), the generator outlet node temperature is calculated based on the generator input power, mass flow rate of water, and the specific heat of water entering the hot water generator. The calculations are based on the Chiller Flow Mode as follows.
-
-**Constant Flow Chillers:**
-
-<div>$${\dot m_{generator}} = {\dot m_{generator,max}}$$</div>
-
-**Variable Flow Chillers:**
-
-<div>$${\dot m_{generator}} = {\raise0.7ex\hbox{${{{\dot Q}_{generator}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{generator}}} {{C_{p,\,water}}\left( {\Delta {T_{generator}}} \right)}}}\right.}\!\lower0.7ex\hbox{${{C_{p,\,water}}\left( {\Delta {T_{generator}}} \right)}$}}$$</div>
-
-<div>$${T_{generator,out}} = {T_{generator,in}} - \frac{{{{\dot Q}_{generator}}}}{{{{\dot m}_{generator}}\left( {{C_{p\,,\,water}}} \right)}}$$</div>
-
-where
-
-<span>\({\dot m_{generator}}\)</span> = generator hot water mass flow rate [kg/s]
-
-<span>\({\dot m_{generator,\,max}}\)</span>= generator design hot water mass flow rate (kg/s)
-
-<span>\(\Delta {T_{generator}}\)</span>   = generator design hot water temperature difference (ºC)
-
-### Indirect Absorption Chiller
-
-The Chiller:Absorption:Indirect object is an enhanced version of the absorption chiller model found in the Building Loads and System Thermodynamics (BLAST) program. This enhanced model is nearly identical to the existing absorption chiller model (Ref. Chiller:Absorption) with the exceptions that: 1) the enhanced indirect absorption chiller model provides more flexible performance curves and 2) chiller performance now includes the impact of varying evaporator, condenser, and generator temperatures. Since these absorption chiller models are nearly identical (i.e., the performance curves of the enhanced model can be manipulated to produce similar results to the previous model), it is quite probable that the Chiller:Absorption model will be deprecated in a future release of EnergyPlus.
-
-The indirect absorption chiller’s condenser and evaporator are similar to that of a standard chiller, which are both water-to-water heat exchangers. The assembly of a generator and absorber provides the compression operation. A schematic of a single-stage absorption chiller is shown in the figure below. Low-pressure vapor from the evaporator is absorbed by the liquid solution in the absorber. A pump receives low-pressure liquid from the absorber, elevates the pressure of the liquid, and delivers the liquid to the generator. In the generator, heat from a high temperature source (hot water or steam) drives off the vapor that has been absorbed by the solution. The liquid solution returns to the absorber through a throttling valve whose purpose is to provide a pressure drop to maintain the pressure difference between the generator and absorber. The heat supplied to the generator can be either hot water or steam, however, connection to an actual plant loop is not required. For more information on indirect absorption chillers, see the Input/Output Reference Document (Object: Chiller:Absorption:Indirect).
-
-![Schematic\_AbsorptionChiller](media/image3060.png)
-
-Figure 160. Schematic Diagram of a Single-Stage Absorption Chiller
-
-The chiller cooling effect (capacity) will change with a change in condenser water temperature. Similarly, the chiller cooling effect will change as the temperature of the evaporator water changes. The chiller cooling effect will also change with a change in or generator inlet water temperature and only applies when Hot Water is used as the generator heat source. A quadratic or cubic equation is used to modify the rated chiller capacity as a function of both the condenser and generator inlet water temperatures and the evaporator outlet water temperature. If any or all of the capacity correction factor curves are not used, the correction factors are assumed to be 1.
-
-<div>$$CAPF{T_{evaporator}} = a + b\left( {{T_{evaporator}}} \right) + c{\left( {{T_{evaporator}}} \right)^2} + d{\left( {{T_{evaporator}}} \right)^3}$$</div>
-
-<div>$$CAPF{T_{condenser}} = e + f\left( {{T_{condenser}}} \right) + g{\left( {{T_{condenser}}} \right)^2} + h{\left( {{T_{condenser}}} \right)^3}$$</div>
-
-<span>\(CAPF{T_{generator}} = i + j\left( {{T_{generator}}} \right) + k{\left( {{T_{generator}}} \right)^2} + l{\left( {{T_{generator}}} \right)^3}\)</span> (*Hot Water only*)
-
-<div>$${\mathop Q\limits^\cdot_{evap,max}} = {\mathop Q\limits^\cdot_{evap,rated}}\left( {CAPF{T_{evaporator}}} \right)\left( {CAPF{T_{condenser}}} \right)\left( {CAPF{T_{generator}}} \right)$$</div>
-
-where
-
-<span>\(CAPF{T_{evaporator}}\)</span>= Capacity correction (function of evaporator temperature) factor
-
-<span>\(CAPF{T_{condenser}} = \)</span>= Capacity correction (function of condenser temperature) factor
-
-<span>\(CAPF{T_{generator}}\)</span>= Capacity correction (function of generator temperature) factor
-
-<span>\({T_{evaporator}}\)</span> = evaporator outet water temperature [C]
-
-<span>\({T_{condenser}}\)</span> = condenser inlet water temperature [C]
-
-<span>\({T_{generator}}\)</span> = generator inlet water temperature [C]
-
-<span>\({\dot Q_{evap,\,\,max}}\)</span> = maximum chiller capacity [W]
-
-<span>\({\dot Q_{evap,\,\,rated}}\)</span> = rated chiller capacity [W]
-
-The part-load ratio of the indirect absoprtion chiller’s evaporator is simply the actual cooling effect required (load) divided by the maximum cooling effect available.
-
-<div>$$PLR = {\raise0.7ex\hbox{${{{\dot Q}_{evap}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{evap}}} {{{\dot Q}_{evap,\,\,max}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot Q}_{evap,\,\,max}}}$}}$$</div>
-
-where
-
-<span>\(PLR\)</span> = part-load ratio of chiller evaporator
-
-<span>\({\dot Q_{evap}}\)</span> = chiller evaporator operating capacity [W]
-
-The generator’s heat input is also a function of several parameters. The primary input for determining the heat input requirements is the Generator Heat Input function of Part-Load Ratio Curve. The curve is a quadratic or cubic equation that determines the ratio of the generator heat input to the chiller’s maximum capacity (Q<sub>evap,\\ max</sub>) and is solely a function of part-load ratio. Typical generator heat input ratios at full load (i.e., PLR=1) are between 1 and 2. Two additional curves are available to modifiy the heat input requirement based on the generator inlet water temperature and the evaporator outlet water temperature.
-
-<div>$$GeneratorHIR = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2} + d{\left( {PLR} \right)^3}$$</div>
-
-<div>$$GenfCondT = e + f\left( {{T_{generator}}} \right) + g{\left( {{T_{generator}}} \right)^2} + h{\left( {{T_{generator}}} \right)^3}$$</div>
-
-<div>$$GenfEvapT = i + j\left( {{T_{evaporator}}} \right) + k{\left( {{T_{evaporator}}} \right)^2} + l{\left( {{T_{evaporator}}} \right)^3}$$</div>
-
-where
-
-*GeneratorHIR* = ratio of generator heat input to chiller operating capacity
-
-*GenfCondT* = heat input modifier based on generator inlet water temperature
-
-*GenfEvapT* = heat input modifier based on evaporator outlet water temperature
-
-The Pump Electric Use function of Part-Load Ratio Curve is a quadratic or cubic equation that determines the ratio of the actual absorber pumping power to the nominal pumping power.
-
-<div>$$ElectricInputRatio = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2} + d{\left( {PLR} \right)^3}$$</div>
-
-If the chiller operating part-load ratio is greater than the minimum part-load ratio, the chiller will run the entire time step and cycling will not occur (i.e. *CyclingFrac* = 1). If the operating part-load ratio is less than the minimum part-load ratio, the chiller will be on for a fraction of the time step equal to *CyclingFrac*. Generator heat input and pump electrical energy use are also calculated using the chiller part-load cycling fraction.
-
-<div>$$CyclingFrac = MIN\left( {1.\frac{{PLR}}{{PL{R_{min}}}}} \right)$$</div>
-
-<div>$${\dot Q_{generator}} = GeneratorHIR\left( {{{\dot Q}_{evap,\,max}}} \right)\left( {GenfCondT} \right)\left( {GenfEvapT} \right)\left( {CyclingFrac} \right)$$</div>
-
-<div>$${\dot Q_{generator}} = ElectricInputRatio({P_{pump}})(CyclingFrac)$$</div>
-
-where
-
-<span>\(CyclingFrac\)</span> = chiller part-load cycling fraction
-
-<span>\(PL{R_{min}}\)</span> = chiller minimum part-load ratio
-
-<span>\({\dot Q_{generator}}\)</span> = generator heat input [W]
-
-<span>\({\dot Q_{pump}}\)</span> = chiller pumping power [W]
-
-The evaporator water mass flow rate is calculated based on the Chiller Flow Mode as follows.
-
-**Constant Flow Chillers:**
-
-<div>$${\dot m_{evap}} = {\dot m_{evap,max}}$$</div>
-
-**Variable Flow Chillers:**
-
-<div>$$\Delta {T_{evap}} = {T_{evap,\,in}} - {T_{evap,\,SP}}$$</div>
-
-<div>$${\dot m_{evap}} = {\raise0.7ex\hbox{${{{\dot Q}_{evap}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{evap}}} {{C_{p,\,evap}}\left( {\Delta {T_{evap}}} \right)}}}\right.}\!\lower0.7ex\hbox{${{C_{p,\,evap}}\left( {\Delta {T_{evap}}} \right)}$}}$$</div>
-
-where
-
-<span>\({\dot m_{evap}}\)</span>          = chiller evaporator water mass flow rate (kg/s)
-
-<span>\({\dot m_{evap,\,max}}\)</span>     = chiller design evaporator water mass flow rate (kg/s)
-
-<span>\(\Delta {T_{evap}}\)</span>        = chiller evaporator water temperature difference (ºC)
-
-<span>\({T_{evap,\,in}}\)</span>        = chiller evaporator inlet water temperature (ºC)
-
-<span>\({T_{evap,\,SP}}\)</span>       = chiller evaporator outlet water setpoint temperature (ºC)
-
-<span>\({C_{p,\,evap}}\)</span>         = specific heat of water entering evaporator (J/kg ºC)
-
-The evaporator outlet water temperature is then calculated based on the cooling effect produced and the evaporator entering water temperature.
-
-<div>$${T_{evap,out}} = {T_{evap,in}} + {\raise0.7ex\hbox{${{{\dot Q}_{evap}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{evap}}} {{C_{p,\,evap}}\left( {{{\dot m}_{evap}}} \right)}}}\right.}\!\lower0.7ex\hbox{${{C_{p,\,evap}}\left( {{{\dot m}_{evap}}} \right)}$}}$$</div>
-
-where
-
-<span>\({T_{evap,out}}\)</span> = chiller evaporator outlet water temperature [ºC]
-
-<span>\({T_{evap,in}}\)</span> = chiller evaporator inlet water temperature [ºC]
-
-<span>\({C_{p,\,evap}}\)</span> = specific heat of chiller evaporator inlet water [J/kg/ºC]
-
-<span>\({\dot m_{evap}}\)</span> = chiller evaporator water mass flow rate [kg/s]
-
-The condenser heat transfer and condenser leaving water temperature are also calculated.
-
-<div>$${\dot Q_{cond}} = {\dot Q_{evap}} + {\dot Q_{generator}} + {\dot Q_{pump}}$$</div>
-
-<div>$${T_{cond,out}} = {T_{cond,in}} + {\raise0.7ex\hbox{${{{\dot Q}_{cond}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{cond}}} {{C_{p,\,cond}}\left( {{{\dot m}_{cond}}} \right)}}}\right.}\!\lower0.7ex\hbox{${{C_{p,\,cond}}\left( {{{\dot m}_{cond}}} \right)}$}}$$</div>
-
-where
-
-<span>\({\dot Q_{cond}}\)</span> = chiller condenser heat transfer rate [W]
-
-<span>\({T_{cond,out}}\)</span> = chiller condenser outlet water temperature [ºC]
-
-<span>\({T_{cond,in}}\)</span> = chiller condenser inlet water temperature [ºC]
-
-<span>\({C_{p,\,cond}}\)</span> = specific heat of chiller condenser inlet water [J/kg/ºC]
-
-<span>\({\dot m_{cond}}\)</span> = chiller condenser water mass flow rate [kg/s]
-
-The absorption chiller can model the impact of steam or hot water entering the generator, although the connection of the steam (hot water) nodes to a plant is not actually required. The calculations specific to the generator depend on the type of fluid used and are described here in further detail.
-
-#### Steam Loop Calculations
-
-When a steam loop is used and the inlet and outlet node names are specified (i.e. the nodes are connected to a steam loop), the generator outlet node steam mass flow rate and temperature are calculated based on the generator heat input, latent heat of steam, the specific heat of water, and the amount of subcooling in the steam generator. The model assumes dry saturated steam enters the generator and exits the generator as a subcooled liquid. The temperature leaving the generator is calculated based on the user entered amount of liquid subcooling in the generator. The effect of subcooling of the liquid (condensate) in the pipe returning to the boiler is also modeled using the user entered abount of steam condensate loop subcooling.
-
-<div>$${\dot m_{steam}}\,\,\,\, = \,\,\,\,\,\frac{{{{\dot Q}_{generator}}}}{{{h_{fg}} + {c_{p,water}} \times \Delta {T_{sc}}}}$$</div>
-
-<div>$${T_{generator,out}} = {T_{generator,in}} - \Delta {T_{sc}}$$</div>
-
-<div>$${T_{loop,out}} = {T_{generator,out}} - \Delta {T_{sc,\,\,loop}}$$</div>
-
-where
-
-<span>\({\dot m_{steam}}\)</span> = chiller steam mass flow rate [kg/s]
-
-<span>\({h_{fg}}\)</span> = latent heat of steam [J/kg]
-
-<span>\({c_{p,water}}\)</span> = specific heat of water [J/Kg ºC]
-
-<span>\(\Delta {T_{sc}}\)</span> = amount of subcooling in steam generator [ºC]
-
-<span>\(\Delta {T_{sc,\,loop}}\)</span> = amount of condensate subcooling in steam loop [ºC]
-
-<span>\({T_{generator,out}}\)</span> = generator steam outlet node temperature [ºC]
-
-<span>\({T_{generator,in}}\)</span> = generator steam inlet node temperature [ºC]
-
-#### Hot Water Loop Calculations
-
-When a hot water loop is used and the inlet and outlet node names are specified (i.e. the nodes are connected to a hot water loop), the generator outlet node temperature is calculated based on the generator heat input, mass flow rate of water, and the specific heat of water entering the hot water generator. The calculations are based on the Chiller Flow Mode as follows.
-
-**Constant Flow Chillers:**
-
-<div>$${\dot m_{generator}} = {\dot m_{generator,\,max}}$$</div>
-
-**Variable Flow Chillers:**
-
-<div>$${\dot m_{generator}} = {\raise0.7ex\hbox{${{{\dot Q}_{generator}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{generator}}} {{C_{p,\,water}}\left( {\Delta {T_{generator}}} \right)}}}\right.}\!\lower0.7ex\hbox{${{C_{p,\,water}}\left( {\Delta {T_{generator}}} \right)}$}}$$</div>
-
-<div>$${T_{generator,out}} = {T_{generator,in}} - \frac{{{{\dot Q}_{generator}}}}{{{{\dot m}_{generator}}\left( {{C_{p\,,\,water}}} \right)}}$$</div>
-
-where
-
-<span>\({\dot m_{generator}}\)</span> = generator hot water mass flow rate [kg/s]
-
-<span>\({\dot m_{generator,\,max}}\)</span>= generator design hot water mass flow rate (kg/s)
-
-<span>\(\Delta {T_{generator}}\)</span>   = generator design hot water temperature difference (ºC)
-
-### Combustion Turbine Chiller
-
-The input object Chiller:CombustionTurbine provides a chiller model that is the empirical model from the Building Loads and System Thermodynamics (BLAST) program. Fitting catalog data to a third order polynomial equations generates the chiller performance curves.  Three sets of coefficients are required to model the open centrifugal chiller as discussed in the section, titled, ‘Electric Chiller Based on Fluid Temperature Differences’.
-
-The gas turbine-driven chiller is an open centrifugal chiller driven directly by a gas turbine.  The BLAST model of an open centrifugal chiller is modeled as standard vapor compression refrigeration cycle with a centrifugal compressor driven by a shaft power from an engine.  The centrifugal compressor has the incoming fluid entering at the eye of a spinning impeller that throws the fluid by centrifugal force to the periphery of the impeller.  After leaving the compressor, the refrigerant is condensed to liquid in a refrigerant to water condenser.  The heat from the condenser is rejected to a cooling tower, evaporative condenser, or well water condenser depending on which one is selected by the user based on the physical parameters of the plant.  The refrigerant pressure is then dropped through a throttling valve so that fluid can evaporate at a low pressure that provides cooling to the evaporator.  The evaporator can chill water that is pumped to chilled water coils in the building.  For more information, see the Input/Output Reference Document.
-
-This chiller is modeled like the electric chiller with the same numerical curve fits and then some additional curve fits to model the turbine drive.  Shown below are the definitions of the curves that describe this model.
-
-The chiller’s temperature rise coefficient which is defined as the ratio of the required change in condenser water temperature to a given change in chilled water temperature, which maintains the capacity at the nominal value.  This is calculated as the following ratio:
-
-<div>$$\frac{{TCEn{t_{required}} - TCEn{t_{rated}}}}{{TEL{v_{required}} - TEL{v_{rated}}}}$$</div>
-
-Where:
-
-TCEnt<sub>required</sub> = Required entering condenser air or water temperature to maintain rated capacity.
-
-TCEnt<sub>rated</sub> = Rated entering condenser air or water temperature at rated capacity.
-
-TELv<sub>required</sub> = Required leaving evaporator water outlet temperature to maintain rated capacity.
-
-TELv<sub>rated</sub> = Rated leaving evaporator water outlet temperature at rated capacity.
-
-The Capacity Ratio Curve is a quadratic equation that determines the Ratio of Available Capacity to Nominal Capacity.  The defining equation is:
-
-<div>$$AvailToNominalCapacityRatio = {C_1} + {C_2}{\Delta_{temp}} + {C_3}\Delta_{temp}^2$$</div>
-
-Where the Delta Temperature is defined as:
-
-<div>$${\Delta_{{\rm{Temp}}}} = \frac{{{\rm{TempCondIn  -  TempCondInDesign }}}}{{{\rm{TempRiseCoefficient}}}} - ({\rm{TempEvapOut  -  TempEvapOutDesign)}}$$</div>
-
-TempCondIn = Temperature entering the condenser (water or air temperature depending on condenser type).
-
-TempCondInDesign = Temp Design Condenser Inlet from User input above.
-
-TempEvapOut = Temperature leaving the evaporator.
-
-TempEvapOutDesign = Temp Design Evaporator Outlet from User input above.
-
-TempRiseCoefficient = User Input from above.
-
-The following three fields contain the coefficients for the quadratic equation.
-
-The Power Ratio Curve is a quadratic equation that determines the Ratio of Full Load to Power.  The defining equation is:
-
-<div>$$FullLoadtoPowerRatio = {C_1} + {C_2}AvailToNominalCapRatio + {C_3}AvailToNominalCapRati{o^2}$$</div>
-
-The Full Load Ratio Curve is a quadratic equation that determines the fraction of full load power.  The defining equation is:
-
-<div>$$FracFullLoadPower = {C_1} + {C_2}PartLoadRatio + {C_3}PartLoadRati{o^2}$$</div>
-
-The Fuel Input Curve is a polynomial equation that determines the Ratio of Fuel Input to Energy Output.  The equation combines both the Fuel Input Curve Coefficients and the Temperature Based Fuel Input Curve Coefficients.  The defining equation is:
-
-<div>$$FuelEnergyInput = PLoad * (FI{C_1} + FI{C_2}RLoad + FI{C_3}RLoa{d^2}) * (TBFI{C_1} + TBFI{C_2}A{T_{air}} + TBFI{C_3}AT_{air}^2)$$</div>
-
-Where FIC represents the Fuel Input Curve Coefficients, TBFIC represents the Temperature Based Fuel Input Curve Coefficients, Rload is the Ratio of Load to Combustion Turbine Engine Capacity, and AT<sub>air</sub> is the difference between the current ambient and design ambient temperatures.
-
-The Exhaust Flow Curve is a quadratic equation that determines the Ratio of Exhaust Gas Flow Rate to Engine Capacity.  The defining equation is:
-
-*<span>\(ExhaustFlowRate = GTCapacity * ({C_1} + {C_2}A{T_{air}} + {C_3}AT_{air}^2)\)</span> *
-
-Where GTCapacity is the Combustion Turbine Engine Capacity, and AT<sub>air</sub> is the difference between the current ambient and design ambient temperatures.
-
-The Exhaust Gas Temperature Curve is a polynomial equation that determines the Exhaust Gas Temperature.  The equation combines both the Exhaust Gas Temperature Curve Coefficients (Based on the Part Load Ratio) and the (Ambient) Temperature Based Exhaust Gas Temperature Curve Coefficients.  The defining equation is:
-
- <span>\(ExhaustTemperature = ({C_1} + {C_2}RLoad + {C_3}RLoa{d^2}) * (TB{C_1} + TB{C_2}A{T_{air}} + TB{C_3}AT_{air}^2) - 273.15\)</span>
-
-Where C represents the Exhaust Gas Temperature Curve Coefficients, TBC are the Temperature Based Exhaust Gas Temperature Curve Coefficients, RLoad is the Ratio of Load to Combustion Turbine Engine Capacity, and AT<sub>air</sub> is the difference between the actual ambient and design ambient temperatures.
-
-The Recovery Lubricant Heat Curve is a quadratic equation that determines the recovery lube energy.  The defining equation is:
-
-<div>$$RecoveryLubeEnergy = PLoad * ({C_1} + {C_2}RL + {C_3}R{L^2})$$</div>
-
-Where Pload is the engine load and RL is the Ratio of Load to Combustion Turbine Engine Capacity
-
-The UA is an equation that determines the overall heat transfer coefficient for the exhaust gasses with the stack.  The heat transfer coefficient ultimately helps determine the exhaust stack temperature.  The defining equation is:
-
-<div>$$UAToCapacityRatio = {C_1}GasTurbineEngineCapacit{y^{{C_2}}}$$</div>
-
-#### Chiller Basin Heater
-
-This chiller’s basin heater (for evaporatively-cooled condenser type) operates in the same manner as the Engine driven chiller’s basin heater. The calculations for the chiller basin heater are described in detail at the end of the engine driven chiller description (Ref. Engine Driven Chiller).
-
-### ChillerHeater:Absorption:DirectFired
-
-#### Overview
-
-This model (object name ChillerHeater:Absorption:DirectFired) simulates the performance of a direct fired two-stage absorption chiller with optional heating capability. The model is based on the direct fired absorption chiller model (ABSORG-CHLR) in the DOE-2.1 building energy simulation program. The EnergyPlus model contains all of the features of the DOE-2.1 chiller model, plus some additional capabilities.
-
-This model simulates the thermal performance of the chiller and the fuel consumption of the burner(s). This model does not simulate the thermal performance or the power consumption of associated pumps or cooling towers. This auxiliary equipment must be modeled using other EnergyPlus models (e.g. Cooling Tower:Single Speed).
-
-#### Model Description
-
-The chiller model uses user-supplied performance information at design conditions along with five performance curves (curve objects) for cooling capacity and efficiency to determine chiller operation at off-design conditions. Two additional performance curves for heating capacity and efficiency are used when the chiller is operating in a heating only mode or simultaneous cooling and heating mode.
-
-#### Cooling
-
-The following nomenclature is used in the cooling equations:
-
-*AvailCoolCap*         =   available full-load cooling capacity at current conditions [W]
-
-*CEIR*                       =   user input “Electric Input to Cooling Output Ratio�
-
-*CEIRfPLR*               =   electric input to cooling output factor, equal to 1 at full load, user input “Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name�
-
-*CEIRfT*                    =   electric input to cooling output factor, equal to 1 at design conditions, user input “Electric Input to Cooling Output Ratio Function of Temperature Curve Name�
-
-*CFIR*                       =   user input “Fuel Input to Cooling Output Ratio�
-
-*CFIRfPLR*               =   fuel input to cooling output factor, equal to 1 at full load, user input “Fuel Input to Cooling Output Ratio Function of Part Load Ratio Curve Name�
-
-*CFIRfT*                    =   fuel input to cooling output factor, equal to 1 at design conditions, user input “Fuel Input to Cooling Output Ratio Function of Temperature Curve Name�
-
-*CondenserLoad       *=   condenser heat rejection load [W]
-
-*CoolCapfT*              =   cooling capacity factor, equal to 1 at design conditions, user input “Cooling Capacity Function of Temperature Curve Name�
-
-*CoolElectricPower*  =   cooling electricity input [W]
-
-*CoolFuelInput*         =   cooling fuel input [W]
-
-*CoolingLoad*           =   current cooling load on the chiller [W]
-
-*CPLR*                      =   cooling part-load ratio = *CoolingLoad* / *AvailCoolCap*
-
-*HeatingLoad*           =   current heating load on the chiller heater [W]
-
-*HFIR*                       =   user input “Fuel Input to Heating Output Ratio�
-
-*HPLR*                      =   heating part-load ratio = *HeatingLoad* / *AvailHeatCap*
-
-*MinPLR                   *=   user input “Minimum Part Load Ratio�
-
-*NomCoolCap*          =   user input “Nominal Cooling Capacity� [W]
-
-*RunFrac*                  =   fraction of time step which the chiller is running
-
-*T<sub>cond</sub>*                         =   entering or leaving condenser fluid temperature [C]. For a water-cooled condenser this will be the water temperature returning from the condenser loop (e.g., leaving the cooling tower) if the entering condenser fluid temperature option is used. For air- or evap-cooled condensers this will be the entering outdoor air dry-bulb or wet-bulb temperature, respectively, if the entering condenser fluid temperature option is used.
-
-*T<sub>cw,l</sub>*                          =   leaving chilled water temperature [C]
-
-Five performance curves are used in the calculation of cooling capacity and efficiency:
-
-1)    Cooling Capacity Function of Temperature Curve
-
-2)    Fuel Input to Cooling Output Ratio Function of Temperature Curve
-
-3)    Fuel Input to Cooling Output Ratio Function of Part Load Ratio Curve
-
-4)    Electric Input to Cooling Output Ratio Function of Temperature Curve
-
-5)    Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve
-
-The cooling capacity function of temperature (*CoolCapfT*) curve represents the fraction of the cooling capacity of the chiller as it varies by temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser fluid temperature. The output of this curve is multiplied by the nominal cooling capacity to give the full-load cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the design temperatures). The curve should have a value of 1.0 at the design temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-<div>$$CoolCapfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}$$</div>
-
-The available cooling capacity of the chiller is then computed as follows:
-
-<div>$$AvailCoolCap = NomCoolCap \cdot CoolCapfT({T_{cw,l}},{T_{cond}})$$</div>
-
-The fuel input to cooling output ratio function of temperature (*CFIRfT*) curve represents the fraction of the fuel input to the chiller at full load as it varies by temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser fluid temperature. The output of this curve is multiplied by the nominal fuel input to cooling output ratio (*CFIR*) to give the full-load fuel input to cooling capacity ratio at specific temperature operating conditions (i.e., at temperatures different from the design temperatures). The curve should have a value of 1.0 at the design temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-<div>$$CFIRfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}$$</div>
-
-The fuel input to cooling output ratio function of part load ratio (*CFIRfPLR*) curve represents the fraction of the fuel input to the chiller as the load on the chiller varies at a given set of  operating temperatures. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic.
-
-<div>$$CFIRfPLR = a + b \cdot CPLR + c \cdot CPL{R^2}$$</div>
-
-The fraction of the time step during which the chiller heater is operating is computed as a function of the cooling and heating part-load ratios and the user-input minimum part-load ratio:
-
-<div>$$RunFrac = {\mathop{\rm MIN}\nolimits} \left( {1.0,{\mathop{\rm MAX}\nolimits} \left( {HPLR,CPLR} \right)/MinPLR} \right)$$</div>
-
-The cooling fuel input to the chiller is then computed as follows:
-
-<div>$$\begin{array}{l}CoolFuelInput = \\AvailCoolCap \cdot RunFrac \cdot CFIR \cdot CFIRfT({T_{cw,l}},{T_{cond}}) \cdot CFIRfPLR(CPLR)\end{array}$$</div>
-
-The electric input to cooling output ratio as function of temperature (*CEIRfT*) curve represents the fraction of electricity to the chiller at full load as it varies by temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser fluid temperature.
-
-<div>$$CEIRfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}$$</div>
-
-The electric input to cooling output ratio function of part load ratio (*CEIRfPLR*) curve represents the fraction of electricity to the chiller as the load on the chiller varies at a given set of operating temperatures. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic.
-
-<div>$$CEIRfPLR = a + b \cdot CPLR + c \cdot CPL{R^2}$$</div>
-
-The cooling electric input to the chiller is computed as follows:
-
-<div>$$CoolElectricPower = NomCoolCap \cdot RunFrac \cdot CEIR \cdot CEIRfT({T_{cw,l}},{T_{cond}}) \cdot CEIRfPLR(CPLR)$$</div>
-
-All five of these cooling performance curves are accessed through EnergyPlus’ built-in performance curve equation manager (objects Curve:Linear, Curve:Quadratic and Curve:Biquadratic). It is not imperative that the user utilize all coefficients in the performance curve equations if their performance equation has fewer terms (e.g., if the user’s *CFIRfPLR* performance curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero).
-
-The condenser load is computed as follows:
-
-<div>$$CondenserLoad = CoolingLoad + {\raise0.7ex\hbox{${CoolFuelInput}$} \!\mathord{\left/ {\vphantom {{CoolFuelInput} {HFIR}}}\right.}\!\lower0.7ex\hbox{${HFIR}$}} + CoolElectricPower$$</div>
-
-#### Heating
-
-The following nomenclature is used in the heating equations:
-
-*AvailHeatCap*         =   available full-load heating capacity at current conditions [W]
-
-*CPLRh*                    =   cooling part-load ratio for heating curve =
- *CoolingLoad* / *NomCoolCap*
-
-*HeatCapfCPLR*       =   heating capacity factor as a function of cooling part load ratio, equal to 1 at zero cooling load, user input “Heating Capacity Function of Cooling Capacity Curve Name�
-
-*HeatCoolCapRatio *=   user input “Heating to Cooling Capacity Ratio�
-
-*HeatElectricPower*  =   heating electricity input [W]
-
-*HeatFuelInput*         =   heating fuel input [W]
-
-*HeatingLoad*           =   current heating load on the chiller [W]
-
-*HEIR*                       =   user input “Electric Input to Heating Output Ratio�
-
-*HFIR*                       =   user input “Fuel Input to Heating Output Ratio�
-
-*HFIRfHPLR*            =   fuel input to heating output factor, equal to 1 at full load, user input “Fuel Input to Heat Output Ratio During Heating Only Operation Curve Name�
-
-*HPLR*                      =   heating part-load ratio = *HeatingLoad* / *AvailHeatCap*
-
-*MinPLR                   *=   user input “Minimum Part Load Ratio�
-
-*NomCoolCap*          =   user input “Nominal Cooling Capacity� [W]
-
-*RunFrac*                  =   fraction of time step which the chiller is running
-
-*TotalElectricPower *=   total electricity input [W]
-
-*TotalFuelInput        *=   total fuel input [W]
-
-Cooling is the primary purpose of the Direct Fired Absorption Chiller so that function is satisfied first and if energy is available for providing heating that is provided next.
-
-The two performance curves for heating capacity and efficiency are:
-
-1)    Heating Capacity Function of Cooling Capacity Curve
-
-2)    Fuel-Input-to Heat Output Ratio Function
-
-The heating capacity function of cooling capacity curve (*HeatCapfCool*) determines how the heating capacity of the chiller varies with cooling capacity when the chiller is simultaneously heating and cooling. The curve is normalized so an input of 1.0 represents the nominal cooling capacity and an output of 1.0 represents the full heating capacity.  An output of 1.0 should occur when the input is 0.0.
-
-<div>$$HeatCapfCPLR = a + b \cdot CPLRh + c \cdot CPLR{h^2}$$</div>
-
-The available heating capacity is then computed as follows:
-
-<div>$$AvailHeatCap = NomCoolCap \cdot HeatCoolCapRatio \cdot HeatCapfCPLR(CPLRh)$$</div>
-
-The fuel input to heat output ratio curve (*HFIRfHPLR*) function is used to represent the fraction of fuel used as the heating load varies as a function of heating part load ratio. It is normalized so that a value of 1.0 is the full available heating capacity. The curve is usually linear or quadratic and will probably be similar to a boiler curve for most chillers.
-
-<div>$$HFIRfHPLR = a + b \cdot HPLR + c \cdot HPL{R^2}$$</div>
-
-The fuel use rate when heating is computed as follows:
-
-<div>$$HeatFuelInput = AvailHeatCap \cdot HFIR \cdot HFIRfHPLR(HPLR)$$</div>
-
-The fraction of the time step during which the chiller is operating is computed as a function of the cooling and heating part-load ratios and the user-input minimum part-load ratio:
-
-<div>$$RunFrac = {\mathop{\rm MIN}\nolimits} \left( {1.0,{\mathop{\rm MAX}\nolimits} \left( {HPLR,CPLRh} \right)/MinPLR} \right)$$</div>
-
-The heating electric input to the chiller is computed as follows:
-
-<div>$$HeatElectricPower = NomCoolCap \cdot HeatCoolCapRatio \cdot HEIR \cdot RunFrac$$</div>
-
-If the chiller is delivering heating and cooling simultaneously, the parasitic electric load will be double-counted, so the following logic is applied:
-
-```
-IF ( HeatElectricPower <= CoolElectricPower ) THEN
-  HeatElectricPower = 0.0
-ELSE
-  HeatElectricPower = HeatElectricPower - CoolElectricPower
-ENDIF
-```
-
-The total fuel and electric power input to the chiller is computed as shown below:
-
-<div>$$\begin{array}{l}TotalElectricPower = HeatElectricPower + CoolElectricPower\\TotalFuelInput = HeatFuelInput + CoolFuelInput\end{array}$$</div>
-
-### ChillerHeater:Absorption:DoubleEffect
-
-#### Overview
-
-This model (object name ChillerHeater:Absorption:DoubleEffect) simulates the performance of an exhaust  fired two-stage (double effect) absorption chiller with optional heating capability. The model is based on the direct fired absorption chiller model (ABSORG-CHLR) in the DOE-2.1 building energy simulation program. The EnergyPlus model contains all of the features of the DOE-2.1 chiller model, plus some additional capabilities. The model uses the exhaust gas output from Microturbine.
-
-This model simulates the thermal performance of the chiller and the thermal energy input to the chiller. This model does not simulate the thermal performance or the power consumption of associated pumps or cooling towers. This auxiliary equipment must be modeled using other EnergyPlus models (e.g. Cooling Tower:Single Speed).
-
-#### Model Description
-
-The chiller model uses user-supplied performance information at design conditions along with five performance curves (curve objects) for cooling capacity and efficiency to determine chiller operation at off-design conditions. Two additional performance curves for heating capacity and efficiency are used when the chiller is operating in a heating only mode or simultaneous cooling and heating mode.
-
-#### Cooling
-
-The following nomenclature is used in the cooling equations:
-
-*AvailCoolCap*         =   available full-load cooling capacity at current conditions [W]
-
-*CEIR*                       =   user input “Electric Input to Cooling Output Ratio�
-
-*CEIRfPLR*               =   electric input to cooling output factor, equal to 1 at full load, user input “Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name�
-
-*CEIRfT*                    =   electric input to cooling output factor, equal to 1 at design conditions, user input “Electric Input to Cooling Output Ratio Function of Temperature Curve Name�
-
-*TeFIR*                      =   user input “Thermal Energy Input to Cooling Output Ratio�
-
-*TeFIRfPLR*              =   thermal energy input to cooling output factor, equal to 1 at full load, user input “Thermal Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve Name�
-
-*TeFIRfT*                   =   thermal energy input to cooling output factor, equal to 1 at design conditions, user input “Thermal Energy Input to Cooling Output Ratio Function of Temperature Curve Name�
-
-*CondenserLoad       *=   condenser heat rejection load [W]
-
-*CoolCapfT*              =   cooling capacity factor, equal to 1 at design conditions, user input “Cooling Capacity Function of Temperature Curve Name�
-
-*CoolElectricPower*  =   cooling electricity input [W]
-
-*CoolThermalEnergyInput*=          cooling thermal energy input [W]
-
-*CoolingLoad*           =   current cooling load on the chiller [W]
-
-*CPLR*                      =   cooling part-load ratio = *CoolingLoad* / *AvailCoolCap*
-
-*HeatingLoad*           =   current heating load on the chiller heater [W]
-
-*HFIR*                       =   user input “Thermal Energy Input to Heating Output Ratio�
-
-*HPLR*                      =   heating part-load ratio = *HeatingLoad* / *AvailHeatCap*
-
-<span>\({\dot m_{ExhAir}}\)</span>                     =  exhaust air mass flow rate from microturbine (kg/s)
-
-*MinPLR                   *=   user input “Minimum Part Load Ratio�
-
-*NomCoolCap*          =   user input “Nominal Cooling Capacity� [W]
-
-*RunFrac*                  =   fraction of time step which the chiller is running
-
-<span>\({T_{a,o}}\)</span>                            =  exhaust air outlet temperature from microturbine entering the chiller
-
-(<sup>o</sup>C)
-
-<span>\({T_{abs,gen,o}}\)</span>                 =  Temperature of exhaust leaving the chiller (the generator                    component  of the absorption chiller)
-
-*T<sub>cond</sub>*                         =   entering condenser fluid temperature [°C]. For a water-cooled condenser this will be the water temperature returning from the condenser loop (e.g., leaving the cooling tower). For air- or evap-cooled condensers this will be the entering outdoor air dry-bulb or wet-bulb temperature, respectively.
-
-*T<sub>cw,l</sub>*                          =   leaving chilled water temperature [°C]
-
-The selection of entering or leaving condense fluid temperature can be made through the optional field-Temperature Curve Input Variable.
-
-Five performance curves are used in the calculation of cooling capacity and efficiency:
-
-6)    Cooling Capacity Function of Temperature Curve
-
-7)    Thermal Energy Input to Cooling Output Ratio Function of Temperature Curve
-
-8)    Thermal Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve
-
-9)    Electric Input to Cooling Output Ratio Function of Temperature Curve
-
-10) Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve
-
-The cooling capacity function of temperature (*CoolCapfT*) curve represents the fraction of the cooling capacity of the chiller as it varies with temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and the entering condenser fluid temperature. The output of this curve is multiplied by the nominal cooling capacity to give the full-load cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the design temperatures). The curve should have a value of 1.0 at the design temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-<div>$$CoolCapfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}$$</div>
-
-The available cooling capacity of the chiller is then computed as follows:
-
-<div>$$AvailCoolCap = NomCoolCap \cdot CoolCapfT({T_{cw,l}} - {T_{cond}})$$</div>
-
-The thermal energy input to cooling output ratio function of temperature (*TeFIRfT*) curve represents the fraction of the thermal energy input to the chiller at full load as it varies with temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and the entering condenser fluid temperature. The output of this curve is multiplied by the nominal thermal energy input to cooling output ratio (*TeFIR*) to give the full-load thermal energy input to cooling capacity ratio at specific temperature operating conditions (i.e., at temperatures different from the design temperatures). The curve should have a value of 1.0 at the design temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-<div>$$TeFIRfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}$$</div>
-
-The thermal energy input to cooling output ratio function of part load ratio (*TeFIRfPLR*) curve represents the fraction of the thermal energy input to the chiller as the load on the chiller varies at a given set of  operating temperatures. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic.
-
-<div>$$TeFIRfPLR = a + b \cdot CPLR + c \cdot CPL{R^2}$$</div>
-
-The fraction of the time step during which the chiller heater is operating is computed as a function of the cooling and heating part-load ratios and the user-input minimum part-load ratio:
-
-<div>$$RunFrac = MIN(1.0,MAX\left( {HPLR,CPLR} \right)/MinPLR)$$</div>
-
-The cooling thermal energy input to the chiller is then computed as follows:
-
-<div>$$CoolThermalEnergyInput = AvailCoolCap \cdot RunFrac \cdot TeFIR \cdot TeFIRfT\left( {{T_{cw,l}},{T_{cond}}} \right) \cdot TeFIRfPLR(CPLR)$$</div>
-
-To make sure that the exhaust mass flow rate and temperature from microturbine are sufficient to drive the chiller, the heat recovery potential is compared with the cooling thermal energy input to the chiller (CoolThermalEergyInput). The heat recovery potential should be greater than the CoolThermalEnergyInput. Heat recovery potential is calculated as:
-
-<div>$${Q_{Recovery}} = {\dot m_{ExhAir}} \cdot {\rm{}}C{p_{Air}} \cdot {\rm{}}({T_{a,o}} - {T_{Abs,gen,o}})$$</div>
-
-T<sub>abs,gen,o </sub> is the minimum temperature required for the proper operation of the double-effect chiller. It will be defaulted to 176°C.
-
-The electric input to cooling output ratio as function of temperature (*CEIRfT*) curve represents the fraction of electricity to the chiller at full load as it varies with temperature. This a biquadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser fluid temperature.
-
-<div>$$CEIRfT = a + b{T_{cw,l}} + cT_{cw,l}^2 + d{T_{cond}} + eT_{cond}^2 + f{T_{cw,l}}{T_{cond}}$$</div>
-
-The electric input to cooling output ratio function of part load ratio (*CEIRfPLR*) curve represents the fraction of electricity to the chiller as the load on the chiller varies at a given set of operating temperatures. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic.
-
-<div>$$CEIRfPLR = a + b \cdot CPLR + c \cdot CPL{R^2}$$</div>
-
-The cooling electric input to the chiller is computed as follows:
-
-<div>$$CoolElectricPower = NomCoolCap \cdot RunFrac \cdot CEIR \cdot CEIRfT\left( {{T_{cw,l}},{T_{cond}}} \right) \cdot CEIRfPLR(CPLR)$$</div>
-
-All five of these cooling performance curves are accessed through EnergyPlus’ built-in performance curve equation manager (objects Curve:Linear, Curve:Quadratic and Curve:Biquadratic). It is not imperative that the user utilize all coefficients in the performance curve equations if their performance equation has fewer terms (e.g., if the user’s *TeFIRfPLR* performance curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero). A set of curves derived from manufacturer’s data are also provided in the dataset (ExhaustFiredChiller.idf) is provided with E+ installation.
-
-The condenser load is computed as follows:
-
-<div>$$CondenserLoad = CoolingLoad + CoolThermalEnergyInput/HFIR + CoolElectricPower$$</div>
-
-#### Heating
-
-The following nomenclature is used in the heating equations:
-
-
-
-*AvailHeatCap*         =   available full-load heating capacity at current conditions [W]
-
-*CPLRh*                    =   cooling part-load ratio for heating curve =
- *CoolingLoad* / *NomCoolCap*
-
-*HeatCapfCPLR*       =   heating capacity factor as a function of cooling part load ratio, equal to 1 at zero cooling load, user input “Heating Capacity Function of Cooling Capacity Curve Name�
-
-*HeatCoolCapRatio *=   user input “Heating to Cooling Capacity Ratio�
-
-*HeatElectricPower*  =   heating electricity input [W]
-
-*HeatThermalEnergyInput*= heating thermal energy input [W]
-
-*HeatingLoad*           =   current heating load on the chiller [W]
-
-*HEIR*                       =   user input “Electric Input to Heating Output Ratio�
-
-*HFIR*                       =   user input “Thermal Energy Input to Heating Output Ratio�
-
-*HFIRfHPLR*            =   thermal energy input to heating output factor, equal to 1 at full load, user input “Thermal Energy Input to Heat Output Ratio During Heating Only Operation Curve Name�
-
-*HPLR*                      =   heating part-load ratio = *HeatingLoad* / *AvailHeatCap*
-
-*MinPLR                   *=   user input “Minimum Part Load Ratio�
-
-*NomCoolCap*          =   user input “Nominal Cooling Capacity� [W]
-
-*RunFrac*                  =   fraction of time step which the chiller is running
-
-*TotalElectricPower *=   total electricity input [W]
-
-*TotalThermalEnergyInput*=          total thermal energy input [W]
-
-Cooling is the primary purpose of the Exhaust Fired Absorption Chiller so that function is satisfied first and if energy is available for providing heating that is provided next.
-
-The two performance curves for heating capacity and efficiency are:
-
-1)    Heating Capacity Function of Cooling Capacity Curve
-
-2)    Thermal-Energy-Input-to Heat Output Ratio Function
-
-The heating capacity function of cooling capacity curve (*HeatCapfCPLR*) determines how the heating capacity of the chiller varies with cooling capacity when the chiller is simultaneously heating and cooling. The curve is normalized so an input of 1.0 represents the nominal cooling capacity and an output of 1.0 represents the full heating capacity.  An output of 1.0 should occur when the input is 0.0.
-
-<div>$$HeatCapfCPLR = a + b \cdot CPLRh + c \cdot CPLR{h^2}$$</div>
-
-The available heating capacity is then computed as follows:
-
-<div>$$AvailHeatCap = NomCoolCap \cdot HeatCoolCapRatio \cdot HeatCapfCPLR(CPLRh)$$</div>
-
-The thermal energy input to heat output ratio curve (*HFIRfHPLR*) function is used to represent the fraction of thermal energy used as the heating load varies as a function of heating part load ratio. It is normalized so that a value of 1.0 is the full available heating capacity. The curve is usually linear or quadratic and will probably be similar to a boiler curve for most chillers.
-
-<div>$$HFIRfHPLR = a + b \cdot HPLR + c \cdot HPL{R^2}$$</div>
-
-The thermal energy use rate when heating is computed as follows:
-
-<div>$$HeatThermalEnergyInput = AvailHeatCap.HFIR.HFIRfHPLR(HPLR)$$</div>
-
-The fraction of the time step during which the chiller is operating is computed as a function of the cooling and heating part-load ratios and the user-input minimum part-load ratio:
-
-<div>$$RunFrac = MIN(1.0,MAX\left( {HPLR,CPLRh} \right)/MinPLR)$$</div>
-
-The heating electric input to the chiller is computed as follows:
-
-<div>$$HeatElectricPower = NomCoolCap \cdot HeatCoolCapRatio \cdot HEIR.RunFrac$$</div>
-
-If the chiller is delivering heating and cooling simultaneously, the parasitic electric load would be double-counted, so the following logic is applied:
-
-<div>$$\begin{array}{l}IF\left( {HeatElectricPower \le CoolElectricPower} \right)THEN\\\quad HeatElectricPower = 0.0\\ELSE\\\quad HeatElectricPower = HeatElectricPower - CoolElectricPower\\ENDIF\end{array}$$</div>
-
-The total thermal energy and electric power input to the chiller is computed as shown below:
-
-<div>$$TotalElectricPower = HeatElectricPower + CoolElectricPower$$</div>
-
-<div>$$TotalThermalEnergyInput = HeatThermalEnergyInput + CoolThermalEnergyInput$$</div>
-
-#### References
-
-Personal communications with various absorption chiller manufacturers, March 2011.
-
-Absorption Chillers and Heat Pumps, Keith Herold, Reinhard Radermacher and Sanford A. Klein (Mar 18, 1996).
-
-Absorption systems for combined heat and power: The problem of part-load operation, ASHRAE Transactions, 2003, Vol 109, Part1.
-
-### Constant COP Chiller
-
-The input object Chiller:ConstantCOP provides a chiller model that is based on a simple, constant COP simulation of the chiller.  In this case, performance does not vary with chilled water temperature or condenser conditions.  The nominal capacity of the chiller and the COP are user specified along with the connections to the plant and condenser loop and mass flow rates.  *Such a model is useful when the user does not have access to detailed performance data.*
-
-The chiller power is calculated from the load divided by the COP.  This chiller will meet the load as long as it does not exceed the nominal capacity specified by the user.
-
-        QEvaporator = Load
-
-        Power = Load / ConstCOPChiller(ChillNum)%COP
-
-Then the evaporator temperatures are calculated from the load
-
-        EvapDeltaTemp = QEvaporator/EvapMassFlowRate/CPwater
-
-        EvapOutletTemp = Node(EvapInletNode)%Temp - EvapDeltaTemp
-
-The condenser load and temperatures are calculated from the evaporator load and the power to the chiller.
-
-     QCondenser = Power + QEvaporator
-
-
-
-     IF (ConstCOPChiller(ChillNum)%CondenserType == WaterCooled) THEN
-
-       IF (CondMassFlowRate &gt; WaterMassFlowTol) THEN
-
-         CondOutletTemp = QCondenser/CondMassFlowRate/CPCW(CondInletTemp) + CondInletTemp
-
-       ELSE
-
-         CALL ShowSevereError('CalcConstCOPChillerModel: Condenser flow = 0, for CONST COP Chiller='//  &
-
-                              TRIM(ConstCOPChiller(ChillNum)%Name))
-
-         CALL ShowContinueErrorTimeStamp(' ')
-
-         CALL ShowFatalError('Program Terminates due to previous error condition.')
-
-       END IF
-
-    ELSE ! Air Cooled or Evap Cooled
-
-         !  Set condenser outlet temp to condenser inlet temp for Air Cooled or Evap Cooled
-
-         !  since there is no CondMassFlowRate and would divide by zero
-
-      CondOutletTemp = CondInletTemp
-
-    END IF
-
-See the InputOutput Reference for additional information.
-
-#### Chiller Basin Heater
-
-This chiller’s basin heater (for evaporatively-cooled condenser type) operates in the same manner as the Engine driven chiller’s basin heater. The calculations for the chiller basin heater are described in detail at the end of the engine driven chiller description (Ref. Engine Driven Chiller).
-
-### Hot Water Heat Recovery from Chillers
-
-+The electric chillers (e.g., Chiller:Electric, Chiller:EngineDriven, Chiller:CombustionTurbine, Chiller:Electric:EIR, and Chiller:Electric:ReformulatedEIR) all have the option of connecting a third plant loop for heating hot water at the same time the chiller cools the chilled water. The engine and combustion turbine chillers models include curves for heat recovery from oil and or jacket coolers. The other three chillers can model heat recovery where part of its condenser section is connected to a heat recovery loop for what is commonly known as a double bundled chiller, or single condenser with split bundles. The heat recovery chiller is simulated as a standard vapor compression refrigeration cycle with a double bundled condenser. A double bundle condenser involves two separate flow paths through a split condenser. One of these paths is condenser water typically connected to a standard cooling tower; the other path is hot water connected to a heat recovery loop. After leaving the compressor, the refrigerant is condensed to liquid in a refrigerant to water condenser. In a split bundle, the chiller’s internal controls will direct a part of the refrigerant to heat recovery condenser bundle and/or to the tower water condenser bundle depending on the chilled water load, the condenser inlet temperatures and internal chiller controls (and possibly a leaving hot water temperature setpoint). The refrigerant pressure is then dropped through a throttling valve so that fluid can evaporate at a low pressure that provides cooling to the evaporator. Note that the heat recovery side of the chiller is placed on the demand-side of a heat recovery loop which will typically supply a hot water storage tank. Heat recovery is a passive benefit when the chiller is dispatched for cooling. The standard plant controls cannot dispatch the chiller based on a heat recovery requirement.
-
-![](media/image3175.png)
-
-Figure 161.  Diagram of Chiller:Electric with Heat Recovery
-
-The algorithm for the heat recovery portion of the chiller needs to be determined from relatively simple inputs to estimate the amount of the heat that is recovered and then send the rest of the heat to the cooling tower. For the chiller models associated with the object Chiller:Electric,  air- or evaporatively-cooled condensers are allowed to be used with heat recovery and, when used, the condenser specific heat, mass flow rate, and temperatures shown below refer to outdoor air. A condenser air volume flow rate must be specified when using heat recovery with air- or evaporatively-cooled chillers.
-
-The basic energy balance for the condenser section of a heat recovery chiller is
-
-<div>$${\dot Q_{tot}} = {\dot Q_{Evap}} + {\dot Q_{Elec}} = {\dot Q_{Cond}} + {\dot Q_{HR}}$$</div>
-
-In practice, if the entering temperature of the heat recovery hot fluid is too high, the chiller’s internal controls will redirect refrigerant away from the heat recovery bundle.  A user input is available for declaring the inlet high temperature limit, and if it is exceeded, the chiller will shut down heat recovery and request no flow and will not reject any condenser heat to that fluid.
-
-The heat recovery condenser bundle is often physically smaller than the tower water condenser bundle and therefore may have limited heat transfer capacity.  User input for the relative capacity of the heat recovery bundle, <span>\({F_{HR,Cap}}\)</span>, is used to define a maximum rate of heat recovery heat transfer using
-
-<div>$${\dot Q_{HR,Max}} = {F_{HR,Cap}}\left( {{{\dot Q}_{Evap,Ref}} + \frac{{{{\dot Q}_{Evap,Ref}}}}{{CO{P_{Ref}}}}} \right)$$</div>
-
-This capacity factor is also used to autosize the heat recovery design fluid flow rate when it is set to autosize.  The design heat recover flow rate is calculated by multiplying <span>\({F_{HR,Cap}}\)</span> by the condenser tower water design flow rate.  If no capacity factor is input, it is assumed to be 1.0.
-
-A heat recovery chiller may control the temperature of heat recovery fluid leaving the device by modulating the flow of refrigerant to the heat recovery condenser bundle.  There are two different algorithms used depending on if the input has declared a leaving setpoint node.
-
-If no control setpoint node was named, then the model developed by Liesen and Chillar (2004) is used to approximate the relative distribution of refrigerant flow and condenser heat transfer between the bundles.  This model approximates the heat transfer situation by using average temperatures in and out of the condenser section.
-
-<div>$${Q_{Tot}} = ({\dot m_{Heat{\mathop{\rm Re}\nolimits} c}}*C{p_{Heat{\mathop{\rm Re}\nolimits} c}} + {\dot m_{Cond}}*C{p_{Cond}})*({T_{AvgOut}} - {T_{AvgIn}})$$</div>
-
-Then the inlet temperature is flow-weighted to determine lumped inlet and outlet conditions.
-
-<div>$${T_{AvgIn}} = \frac{{({{\dot m}_{Heat{\mathop{\rm Re}\nolimits} c}}*C{p_{Heat{\mathop{\rm Re}\nolimits} c}}*{T_{Heat{\mathop{\rm Re}\nolimits} cIn}} + {{\dot m}_{Cond}}*C{p_{Cond}}*{T_{CondIn}})}}{{({{\dot m}_{Heat{\mathop{\rm Re}\nolimits} c}}*C{p_{Heat{\mathop{\rm Re}\nolimits} c}} + {{\dot m}_{Cond}}*C{p_{Cond}})}}$$</div>
-
-<div>$${T_{AvgOut}} = \frac{{{Q_{Tot}}}}{{({{\dot m}_{Heat{\mathop{\rm Re}\nolimits} c}}*C{p_{Heat{\mathop{\rm Re}\nolimits} c}} + {{\dot m}_{Cond}}*C{p_{Cond}})}} + {T_{AvgIn}}$$</div>
-
-The lumped outlet temperature is then used for an approximate method of determining the heat recovery rate
-
-<div>$${\dot Q_{HR}} = {\dot m_{HR}}{c_p}_{HR}\left( {{T_{Avg,out}} - {T_{HR,in}}} \right)$$</div>
-
-This rate is then limited by the physical size of the heat recovery bundle.
-
-<div>$${\dot Q_{HR}} = Min\left( {{{\dot Q}_{HR}},{{\dot Q}_{HR,max}}} \right)$$</div>
-
-If user input for the leaving temperature setpoint is available, then a second model is used to distribute refrigerant flow and condenser heat transfer between the bundles that attempts to meet the heat recovery load implied by the leaving setpoint.  When setpoint control is used, the desired rate of heat recovery heat transfer is:
-
-<div>$${\dot Q_{HR,Setpoint}} = {\dot m_{HR}}{c_p}_{HR}\left( {{T_{HR,set}} - {T_{HR,in}}} \right)$$</div>
-
-<div>$${\dot Q_{HR,Setpoint}} = Max\left( {{{\dot Q}_{HR,Setpoint}},0.0} \right)$$</div>
-
-Then the heat recovery rate is simply modeled as the lower of the three different heat flow rates:  the desired capacity, the maximum capacity, and the current total heat rejection rate.
-
-<div>$${\dot Q_{HR}} = Min\left( {{{\dot Q}_{HR,Setpoint}},{{\dot Q}_{HR,max}},{{\dot Q}_{Tot}}} \right)$$</div>
-
-For both models, the condenser heat transfer rate is then
-
-<div>$${\dot Q_{Cond}} = {\dot Q_{Tot}} - {\dot Q_{HR}}$$</div>
-
-The outlet temperatures are then calculated using
-
-<div>$${T_{HR,out}} = {T_{HR,in}} + {\raise0.7ex\hbox{${{{\dot Q}_{HR}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{HR}}} {{{\dot m}_{HR}}{c_p}_{HR}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{HR}}{c_p}_{HR}}$}}$$</div>
-
-<div>$${T_{Cond,out}} = {T_{Cond,in}} + {\raise0.7ex\hbox{${{{\dot Q}_{Cond}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{Cond}}} {{{\dot m}_{Cond}}{c_p}_{cond}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{Cond}}{c_p}_{cond}}$}}$$</div>
-
-A heat recovery chiller may need to work harder because the refrigeration system faces a higher lift owing to an elevated effective temperature for heat rejection.  With heat recovery, the condenser temperature used with the chiller’s performance curves is determined using one of the following heat-flow-weighted methods. The first is used for the chiller model for the objects Chiller:Electric, and Chiller:Electric:EIR which use the condensing entering temperature for performance.
-
-<div>$${T_{Cond,in,Avg}} = \frac{{\left( {{{\dot Q}_{HR}}{T_{HR,in}} + {{\dot Q}_{Cond}}{T_{Cond,in}}} \right)}}{{\left( {{{\dot Q}_{HR}} + {{\dot Q}_{Cond}}} \right)}}$$</div>
-
-The second is used for the chiller model for the object Chiller:Electric:ReformulatedEIR which uses the leaving condenser fluid temperature.
-
-<div>$${T_{Cond,out,Avg}} = \frac{{\left( {{{\dot Q}_{HR}}{T_{HR,out}} + {{\dot Q}_{Cond}}{T_{Cond,out}}} \right)}}{{\left( {{{\dot Q}_{HR}} + {{\dot Q}_{Cond}}} \right)}}$$</div>
-
-Both of these are available as an output variable called Chiller Effective Heat Rejection Tempeature, in C.
-
-#### Chiller Basin Heater
-
-This chiller’s basin heater (for evaporatively-cooled condenser type) operates in the same manner as the Engine driven chiller’s basin heater. The calculations for the chiller basin heater are described in detail at the end of the engine driven chiller description (Ref. Engine Driven Chiller).
-
-**Reference**
-
-Leisen and Chillar. 2004. Variable Heat Recovery In Double Bundle Electric Chillers. SimBuild 2004, IBPSA-USA National Conference Boulder, CO, August 4-6, 2004.
-
-### Electric Chiller Model Based on Fluid Temperature Differences
-
-The centrifugal chiller model (object name Chiller:Electric) was originally developed for the BLAST program.  The model is based on a ‘capacity ratio’ curve, which is a quadratic equation that determines the Ratio of Available Capacity to Nominal Capacity. The defining equation is:
-
-<div>$$CapRatio = \frac{{Available Chiller Capacity}}{{Nominal Chiller Capacity}} = {A_1} + {A_2}\Delta {T_{chiller}} + {A_3}\Delta {T_{chiller}}^2$$</div>
-
-Where the Delta Temperature is defined as:
-
-<div>$$\Delta {T_{chiller}} = \frac{{{T_{cond, in}} - {T_{cond,in,design}}}}{{TempRiseRatio}} - \left( {{T_{evap,out}} - {T_{evap,out,design}}} \right)$$</div>
-
-where the temperature rise coefficient is defined as the ratio of the required change in condenser water temperature to a given change in chilled water temperature, which maintains the capacity at the nominal value.  If the chiller is a heat recovery chiller,then the condenser inlet temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers. This is calculated as the following ratio:
-
-<div>$$TempRiseRatio = \frac{{{T_{cond, in,required}} - {T_{cond,in,rated}}}}{{{T_{evap, out,required}} - {T_{evap,out,rated}}}} - \left( {{T_{evap,out}} - {T_{evap,out,design}}} \right)$$</div>
-
-Where:
-
-*T<sub>cond,in,required</sub>* = Required entering condenser air or water temperature to maintain rated capacity (C)
-
-*T<sub>cond,in,rated</sub>* = Rated entering condenser air or water temperature at rated capacity (C)
-
-*T<sub>evap,out,required</sub>* = Required leaving evaporator water outlet temperature to maintain rated capacity (C)
-
-*T<sub>evap,out,rated</sub>* = Rated leaving evaporator water outlet temperature at rated capacity (C)
-
-The Power Ratio Curve is a quadratic equation that determines the Ratio of Full Load to Power.  The defining equation is:
-
-<div>$$PowerRatio = {B_1} + {B_2}PLR + {B_3}PL{R^2}$$</div>
-
-where the part load ratio, PLR is defined as:
-
-<div>$$PLR = \frac{{chiller cooling load}}{{nominal chiller capacity}}$$</div>
-
-The Load Ratio Curve is a quadratic equation that determines the Ratio of Actual Cooling Load to Full Cooling Load.  The defining equation is:
-
-<div>$$LoadRatio = {C_1} + {C_2}CapRatio + {C_3}CapRati{o^2}$$</div>
-
-The evaporator heat transfer rate and the power required by the chiller are then calculated as:
-
-<div>$$Qevap = AvailableChillerCap*PLR$$</div>
-
-<div>$$Power = PowerRatio*LoadRatio*\frac{{AvailableChillerCap}}{{RatedCOP}}$$</div>
-
-### Electric Chiller Model Based on Condenser Entering Temperature
-
-#### Overview
-
-This model (object name Chiller:Electric:EIR) simulates the performance of an electric liquid chiller. The model is based on the compression chiller model (COMREF) in the DOE-2.1 building energy simulation program. The EnergyPlus model contains all of the features of the DOE-2.1 chiller model, plus additional abilities for modeling evaporatively-cooled condensers and heat recovery for water heating.
-
-This model simulates the thermal performance of the chiller and the power consumption of the compressor(s). It also models the power consumption of condenser fans if modeling an air-cooled or evaporatively-cooled condenser. This model does not simulate the thermal performance or the power consumption of associated pumps or cooling towers. This auxiliary equipment must be modeled using other EnergyPlus models (e.g. CoolingTower:SingleSpeed).
-
-#### Model Description
-
-The chiller model uses user-supplied performance information at reference conditions along with three performance curves (curve objects) for cooling capacity and efficiency to determine chiller operation at off-reference conditions. The three performance curves are:
-
-1)    Cooling Capacity Function of Temperature Curve
-
-2)    Energy Input to Cooling Output Ratio Function of Temperature Curve
-
-3)    Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve
-
-·        The cooling capacity function of temperature curve is a biquadratic performance curve with two independent variables: the leaving chilled water temperature and the entering condenser fluid temperature. The output of this curve is multiplied by the reference capacity to give the full-load cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation. If the chiller is a heat recovery chiller,then the condenser inlet temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers.
-
-<span>\(ChillerCapFTemp = a + b\left( {{T_{cw,l}}} \right) + c{\left( {{T_{cw,l}}} \right)^2} + d\left( {{T_{cond,e}}} \right) + e{\left( {{T_{cond,e}}} \right)^2} + f\left( {{T_{cw,l}}} \right)\left( {{T_{cond,e}}} \right)\)</span>where
-
-*ChillerCapFTemp* = cooling capacity factor, equal to 1 at reference conditions
-
-*T<sub>cw,l</sub>*            = leaving chilled water temperature, ˚C
-
-*T<sub>cond,e</sub>*         = entering condenser fluid temperature, ˚C. For a water-cooled condenser this will be the water temperature returning from the condenser loop (e.g., leaving the cooling tower). For air- or evap-cooled condensers this will be the entering outdoor air dry-bulb or wet-bulb temperature, respectively.
-
-·        The energy input to cooling output ratio function of temperature curve is a biquadratic performance curve that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and the entering condenser fluid temperature. The EIR is the inverse of the COP. The output of this curve is multiplied by the reference EIR (inverse of the reference COP) to give the full-load EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-<div>$$ChillerEIRFTemp = a + b\left( {{T_{cw,l}}} \right) + c{\left( {{T_{cw,l}}} \right)^2} + d\left( {{T_{cond,e}}} \right) + e{\left( {{T_{cond,e}}} \right)^2} + f\left( {{T_{cw,l}}} \right)\left( {{T_{cond,e}}} \right)$$</div>
-
-where
-
-*ChillerEIRFTemp* = energy input to cooling output factor, equal to 1 at reference conditions
-
-*T<sub>cw,l</sub>*      = leaving chilled water temperature, ˚C
-
-*T<sub>cond,e</sub>*<sub>     </sub>= entering condenser fluid temperature, ˚C. For a water-cooled condenser this will be the water temperature returning from the condenser loop (e.g., leaving the cooling tower). For air- or evap-cooled condensers this will be the entering outdoor air dry-bulb or wet-bulb temperature, respectively. If the chiller is a heat recovery chiller,then the condenser inlet temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers.
-
-·        The energy input to cooling output ratio function of part-load ratio curve is a quadratic performance curve that parameterizes the variation of the chiller input power ratio as a function of the part-load ratio. The part-load ratio is the actual cooling load divided by the chiller’s available cooling capacity. The output of this curve is multiplied by the reference EIR (inverse of the reference COP) and the Energy Input to Cooling Output Ratio Function of Temperature Curve to give the EIR at the specific temperatures and part-load ratio at which the chiller is operating. This curve should have a value of 1.0 when the part-load ratio equals 1.0. The quadratic curve should be valid for the range of part-load ratios anticipated for the simulation.
-
-<div>$$ChillerEIRFPLR = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2}\, = \,{\raise0.7ex\hbox{${{P_{chiller}}}$} \!\mathord{\left/ {\vphantom {{{P_{chiller}}} {{P_{ref}}\left( {ChillerCapFTemp} \right)\left( {ChillerEIRFTemp} \right)}}}\right.}\!\lower0.7ex\hbox{${{P_{ref}}\left( {ChillerCapFTemp} \right)\left( {ChillerEIRFTemp} \right)}$}}$$</div>
-
-where
-
-*ChillerEIRFPLR* = energy input to cooling output factor, equal to 1 at reference conditions
-
-*PLR* =part-load ratio = (cooling load) / (chiller’s available cooling capacity)
-
-*P<sub>chiller</sub> = chiller power at specific PLR*
-
-*P<sub>ref</sub> = <span>\({\mathop Q\limits^ \bullet_{ref}}\)</span>/COP<sub>ref</sub>*
-
-All three of the performance curves are accessed through EnergyPlus’ built-in performance curve equation manager (curve:quadratic and curve:biquadratic). It is not imperative that the user utilize all coefficients in the performance curve equations if their performance equation has fewer terms (e.g., if the user’s ChillerEIRFPLR performance curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero). Performance curves for more than 160 chillers, including the default DOE-2.1E reciprocating and centrifugal chillers, are provided in the EnergyPlus Reference DataSets (Chillers.idf and AllDataSets.idf).
-
-Note: Chiller:Electric:EIR objects and their associated performance curve objects are developed using performance information for a specific chiller and should normally be used together for an EnergyPlus simulation. Changing the object input values, or swapping performance curves between chillers, should be done with caution.
-
-For any simulation time step, the chiller’s available cooling capacity is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{avail}}\,\, = \,\,{\mathop Q\limits^ \bullet_{ref}}\left( {ChillerCapFTemp} \right)$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{ref}}\)</span>     = chiller capacity at reference conditions (reference temperatures and flow rates defined by the user), W
-
-<span>\(\mathop Q\limits^ \bullet  avail\)</span> = available chiller capacity adjusted for current fluid temperatures, W
-
-The model then calculates the evaporator heat transfer rate required to bring the entering chilled water temperature down to the leaving chilled water setpoint temperature (established using a SetpointManager object and referenced in the PlantLoop object). If this calculated heat transfer rate is greater than the heat transfer rate being requested by the plant equipment operation scheme, then the evaporator heat transfer rate is reset to the requested cooling rate.
-
-The evaporator heat transfer rate is then compared to the available capacity. If the available chiller capacity is sufficient to meet the evaporator heat transfer rate, the leaving chilled water temperature is set equal to the chilled water setpoint temperature. If the requested evaporator heat transfer rate is larger than the available capacity the chilled water leaving the evaporator is allowed to float upward. For this case, the exiting chilled water temperature is calculated based on the water temperature entering the evaporator, the available cooling capacity, and the evaporator mass flow rate as follows:
-
-<div>$${T_{cw,l}} = {T_{cw,e}} - \left( {{\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{avail}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{avail}}} {{{\mathop m\limits^ \bullet  }_{evap}}{C_{p,evap}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop m\limits^ \bullet  }_{evap}}{C_{p,evap}}}$}}} \right)$$</div>
-
-where
-
-*T<sub>cw,l</sub>*            = water temperature leaving the evaporator, ˚C
-
-*T<sub>cw,e</sub>*           = water temperature entering the evaporator, ˚C
-
-<span>\({\mathop m\limits^ \bullet_{evap}}\)</span>         = evaporator mass flow rate, kg/s
-
-*C<sub>p,evap</sub>*         = specific heat of water entering evaporator at *T<sub>cw,e</sub>*, J/kg-˚C
-
-The part-load ratio is then calculated as the ratio of the evaporator heat transfer rate to the available chiller capacity. The part-load ratio is not allowed to be greater than the maximum part-load ratio specified by the user or less than zero as follows:
-
-<div>$$PLR = MAX\left( {0.0,MIN\left( {{\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{evap}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{evap}}} {{{\mathop Q\limits^ \bullet  }_{avail}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{avail}}}$}},\,\,PL{R_{\max }}} \right)} \right)$$</div>
-
-where
-
-*PLR*           = part-load ratio
-
-<span>\({\mathop Q\limits^ \bullet_{evap}}\)</span>         = load to be met by the chiller, W
-
-*PLR<sub>max\\        </sub>*= maximum part-load ratio (specified by the user in the input data file)
-
-
-
-The model assumes that the cooling load is met through chiller unloading down to the minimum unloading ratio. False loading (e.g. hot-gas bypass) is assumed to occur between the minimum unloading ratio and the minimum part load ratio yielding constant electrical power consumption under these conditions. Below the minimum part load ratio, the chiller cycles on and off to meet very small loads and the power consumption during the on cycle is the same as when the chiller is operating at the minimum part load ratio. When the chiller part load ratio is less than the minimum part load ratio, the on-off cycling ratio of the chiller is calculated as follows and is available as an output variable.
-
-<div>$$ChillerCyclingRatio = MIN\left( {{\raise0.7ex\hbox{${PLR}$} \!\mathord{\left/ {\vphantom {{PLR} {PL{R_{\min }}}}}\right.}\!\lower0.7ex\hbox{${PL{R_{\min }}}$}},\,\,1.0} \right)$$</div>
-
-To properly account for chiller electric power consumption when PLR is less than the minimum unloading ratio, the PLR is reset to the greater of the PLR calculated above and the PLR at the minimum unloading ratio. The result is available as the output variable Chiller Part Load Ratio.
-
-<div>$$PLR = MAX(PLR,PL{R_{MinUnloadRatio}})$$</div>
-
-This revised PLR accounts for the “false loading� (e.g., hot gas bypass) that is assumed to occur whenever the PLR (based on cooling load divided by available capacity) is less than the minimum unloading ratio specified. The amount of false loading on the chiller is calculated using this revised PLR and is reported as an output variable as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{falseloading}} = \left( {{{\mathop Q\limits^ \bullet  }_{avail}}} \right)\left( {PLR} \right)\left( {ChillerCyclingRatio} \right) - {\mathop Q\limits^ \bullet_{evap}}$$</div>
-
-The electrical power consumption for the chiller compressor(s) for any simulation time step is then calculated using the following equation:
-
-<span>\({P_{chiller}}\, = \,\,\left( {{{\mathop Q\limits^ \bullet  }_{avail}}\,} \right)\,\left( {\frac{1}{{CO{P_{ref}}}}} \right)\,\left( {ChillerEIRFTemp} \right)\left( {ChillerEIRFPLR} \right)\left( {ChillerCyclingRatio} \right)\)</span>where
-
-*P<sub>chiller</sub>*         = chiller compressor power, W
-
-*COP<sub>ref</sub>*       = reference coefficient of performance, W/W
-
-
-
-Heat rejected by the chiller condenser includes the heat transferred in the evaporator plus a portion or all of the compressor electrical energy consumption. For electric chillers with hermetic compressors, all compressor energy consumption is rejected by the condenser (compressor motor efficiency = *eff<sub>motor</sub>* = 1.0). For chillers with semi-hermetic or open compressors, only a portion of the compressor energy use is rejected by the condenser. The heat transfer rate for the chiller condenser is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{cond}} = \left( {{P_{chiller}} * ef{f_{motor}}} \right) + {\mathop Q\limits^ \bullet_{evap}} + {\mathop Q\limits^ \bullet_{falseloading}}$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{cond}}\)</span>         = condenser heat transfer rate, W
-
-<span>\(ef{f_{motor}}\)</span>       = compressor motor efficiency = fraction of compressor electrical energy consumption rejected as condenser heat
-
-For water-cooled chillers, the water temperature leaving the condenser is then calculated as shown below.
-
-<div>$${T_{cond,l}} = {T_{cond,e}} + {\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{cond}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{cond}}} {\left( {{{\mathop m\limits^ \bullet  }_{cond}} * {C_{p,cond}}} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {{{\mathop m\limits^ \bullet  }_{cond}} * {C_{p,cond}}} \right)}$}}$$</div>
-
-where:
-
-*T<sub>cond,l</sub>*          = water temperature leaving the condenser, ˚C
-
-*T<sub>cond,e</sub>*         = water temperature entering the condenser, ˚C
-
-<span>\({\mathop m\limits^ \bullet_{cond}}\)</span>         = mass flow rate through the condenser, kg/s
-
-<span>\({C_{p,cond}}\)</span>       = specific heat of water entering the condenser at *T<sub>cond,e</sub>*, J/kg-˚C
-
-For air- and evaporatively-cooled condensers, the exiting air temperature is not calculated and is set equal to the entering air or wet-bulb temperature, respectively.
-
-The model then calculates the condenser fan energy for air- and evaporatively-cooled condensers. The amount of condenser fan energy is assumed to be proportional to the chiller cycling ratio and is calculated as follows:
-
-<div>$${P_{cond}}\, = \,{\mathop Q\limits^ \bullet_{ref}}\,\left( {{P_{condfanratio}}} \right)\,\left( {ChillerCyclingRatio} \right)$$</div>
-
-where
-
-*P<sub>cond</sub>*           = chiller condenser fan electric power, W
-
-*P<sub>condfanratio</sub>*   = condenser fan power ratio, W/W
-
-
-
-The final calculations determine the total heat transfer energy for the condenser and evaporator, as well as the total electric energy consumed by the chiller compressor motor(s) and condenser fan(s). The results are available as output variables.
-
-<div>$${Q_{cond}} = {\mathop Q\limits^ \bullet_{cond}}*TimeStepSys*3600$$</div>
-
-<div>$${Q_{evap}} = {\mathop Q\limits^ \bullet_{evap}}\,\,*\,\,TimeStepSys\,\,*\,\,3600$$</div>
-
-<div>$${E_{chiller}} = {P_{chiller}}*\,\,TimeStepSys\,\,*\,\,3600$$</div>
-
-<div>$${E_{cond}} = {P_{cond}}\,\, * \,\,TimeStepSys\,\,*\,\,3600$$</div>
-
-where
-
-*Q<sub>cond</sub>*          = chiller condenser heat transfer energy, J
-
-*Q<sub>evap</sub>*           = chiller evaporator cooling energy, J
-
-*E<sub>chiller</sub>*         = chiller (compressor) electric energy, J
-
-*E<sub>cond</sub>*           = chiller condenser fan electric energy, J
-
-*TimeStepSys* = HVAC system simulation time step, hr
-
-<span>\(3600\)</span>         = conversion factor, sec/hr
-
-#### Electric EIR Chiller with Heat Recovery Option
-
-Heat from the electric EIR chiller condenser may be recovered when a water-cooled condenser is selected for simulation. The heat recovery water flow rate is specified by the user along with the input and output nodes connected to the heat recovery loop. The algorithms are identical to those used for Chiller:Electric. Refer to the section entitled Chillers with Plant Heat Recovery for details.
-
-#### Standard Rating (Integrated Part Load Value)
-
-For the Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR objects in EnergyPlus, the industry standard rating of Integrated Part Load Value (IPLV) is calculated according to ANSI/AHRI Standard 550/590 (2011). This standard rating is not direct input to the model and is calculated using user-entered information for these objects. These standard rating values are provided in the eplusout.eio output file (Ref. Output Details document) and also in the predefined tabular output reports (Output:Table:SummaryReports object, Equipment Summary).
-
-Note: The standard ratings described in this section require that the EIR/Reformulated EIR chiller models be evaluated at specific operating conditions (e.g., specific evaporator outlet temperature (6.67 C) and dry-bulb temperatures for air entering the air-cooled [outdoor] condenser). If the chiller  performance curves can not be evaluated at the required test conditions, then the standard rating value will be determined at user specified curve limit and warning error message is provided. For example, if the curve object (Curve:Biquadratic) for Cooling Capacity Function of Temperature Curve has a minimum value of 21C for dry-bulb temperature entering the air-cooled condenser coil, the IPLV calculation requires that EER<sub>D</sub> be calculated at 13 C – so, this would result in IPLV value calculated at 21C and reported in the output and a warning message in the eplusout.err file.
-
-The IPLV is a single number part-load performance figure of merit for Water-Chilling Packages. The IPLV equations and procedures described below are taken from Appendix D of ANSI/AHRI Std. 550/590, 2011 and provide a consistent method for calculating IPLV. These equations provide representative average part-load efficiency for a single chiller.  For equipment covered by this standard, the *IPLV* is calculated using the following formula:
-
-<div>$$IPLV = (0.01A) + (0.42B) + (0.45C) + (0.12D)$$</div>
-
-where,
-
-<span>\(A\)</span>  =   *EER* or *COP* at 100% capacity at AHRI standard rating conditions
-
-<span>\(B\)</span>  =   *EER* or *COP* at 75% capacity and reduced ambient (see Table 51)
-
-<span>\(C\)</span>  =   *EER* or *COP* at 50% capacity and reduced ambient (see Table 51)
-
-<span>\(D\)</span>  =   *EER* or *COP* at 25% capacity and reduced ambient (see Table 51)
-
-The Coefficient of Performance (*COP*) at the various load capacity points (100%, 75%, 50%, and 25% part-load ratios) are calculated using the procedure outlined below and applicable test conditions specified in Table 51.
-
-EER at desired reduced capacity (75%, 50%, and 25%) is calculated as follows
-
-<div>$$COP = \frac{{\rm{1}}}{{EIR}}$$</div>
-
-<div>$$EIR = EnergyInputRatio = \left( {\frac{{{\rm{Power }}}}{{{\rm{PartLoadRatio * AvailChillerCap}}}}} \right)$$</div>
-
-<div>$$Power = \left( {\frac{{{\rm{AvailChillerCap}}}}{{CO{P_{reference}}}}} \right)(EIRTempModFa{c_{ReducedTemp}})(EIRPLRModFa{c_{ReducedPLR}})$$</div>
-
-<div>$$AvailChillerCap = Capacit{y_{reference}}(CAPTempModFa{c_{ReducedTemp}})$$</div>
-
-<span>\(Capacit{y_{reference}}\)</span>= Reference chiller capacity specified by the user, (W).
-
-<span>\(CO{P_{reference}}\)</span>= Reference coefficient of performance specified by the user, (W/W).
-
-<span>\(EIRTempModFa{c_{ReducedTemp}}\)</span>= User-specified bi-quadratic curve for modifying EIR as a function of leaving chilled water temperature (6.7°C) and entering condenser temperature obtained from Table 51 for reduced capacities, (dimensionless).
-
-<span>\(EIRPLRModFa{c_{ReducedPLR}}\)</span>= User-specified quadratic curve for modifying EIR as a function of part load ratio.
-
-<span>\(CapTempModFa{c_{ReducedTemp}}\)</span>= Capacity (W) of the chiller determined per the ANSI/AHRI Standard 550/590 reduced ambient test conditions as shown in Table 51.
-
-If the equipment cannot be unloaded to the desired reduced capacity (75%, 50%, and 25%) i.e. if the minimum unloading ratio of the chiller is greater than desired reduced capacity, then the model is run at the minimum unloading PLR of the equipment at the condenser entering conditions defined in Table 51 and the efficiency is adjusted for cyclic performance.
-
-<div>$$COP = \frac{{\rm{1}}}{{{C_D} \cdot EIRatMinPLR}}$$</div>
-
- where,
-
-<span>\(EIRatMinPLR\)</span>= EIR of chiller at minimum unloading ratio
-
-<span>\({C_D}\)</span>= degradation coefficient to account for cycling of the compressor for capacity less than the minimum capacity.
-
-Thedegradation coefficient *C<sub>D</sub>* for the desired reduced load points (75%, 50%, or 25%) is determined using the following equation:
-
-<div>$${C_D} = 1.13 - 0.13LF$$</div>
-
-The load factor (*LF*) for the desired reduced load points (75%, 50%, or 25%) calculated from the following equation:
-
-<div>$$LF = \frac{{\left( {\frac{{\% Load}}{{100}}} \right) \cdot Full{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity}}{{Part{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity}}$$</div>
-
-Where,
-
-*<span>\(\left( {\frac{{\% Load}}{{100}}} \right)\)</span>*            =          standard rating part load ratio (*PLR*) points, 75%, 50%, 25%.
-
-<span>\(Full{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity\)</span> =            Full load heating capacity (W) of the air-source heat pump equipment determined from ANSI/AHRI Standard 550/590 and test conditions shown in Table 51 for 100% load.
-
-<span>\(Part{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity\)</span> =           Part load heating capacity (W) of the air-source heat pump units determined from ANSI/AHRI Standard 550/590 at the standard desired reduced ambient test conditions as shown in Table 51  and the minimum part load capacity of the unit.
-
-<div>$$Full{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity = {\dot Q_{total,Reference}}\left( {CapTempModFa{c_{Rated}}} \right)$$</div>
-
-<div>$$Part{\rm{ }}load{\rm{ }}unit{\rm{ }}capacity = MinPLR \cdot {\dot Q_{total,Reference}}\left( {CapTempModFa{c_{ReducedTemp}}} \right)$$</div>
-
-where,
-
-<span>\({\dot Q_{total,Reference}}\)</span> = Reference capacity specified by the user, (W).
-
-<span>\(CapTempModFa{c_{Rated}}\)</span>= User-specified bi-quadratic curve evaluated at full load (100%) test conditions shown in Table 51, (dimensionless).
-
-<span>\(CapTempModFa{c_{ReducedTemp}}\)</span>= Part load capacity (W) of the chiller determined from ANSI/AHRI Standard 550/590 at the standard desired reduced ambient test conditions as shown in Table 51.
-
-<span>\(MinPLR\)</span>= Minimum PLR up to which chiller can be unloaded
-
-Table 51. Standard Rating (Integrated Part Load Value)
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="5">Standard Rating (Integrated Part Load Value)</th>
-  </tr>
-  <tr>
-    <td colspan="5">Source: Table 3, Page 10, ANSI/AHRI Standard 550/590-2011</th>
-  </tr>
-  <tr>
-    <th></th>
-    <td colspan="2">IPLV</th>
-    <td colspan="2">NPLV</th>
-  </tr>
-  <tr>
-    <td>Evaporator (All types)<BR>100 % Load LWT<BR>0% Load LWT<BR>Flow Rate (gpm)<BR>F.F.A</td>
-    <td>2 44.0&deg;F<BR>44.0&deg;F<BR>3 2.4 gpm/ton<BR>0.0001<BR>h- ft 2 -&deg;F/Btu</td>
-    <td>6.7&deg;C<BR>6.7&deg;C<BR>0.043 L/s per<BR>kW<BR>0.000018<BR>m 2 -&deg;C/W</td>
-    <td>2 Selected LWT<BR>Same as 100%<BR>load<BR>3 Selected<BR>gpm/ton<BR>As Specified</td>
-    <td>2 Selected<BR>LWT<BR>Same as 100%<BR>load<BR>3 [L/s per kW]<BR>As Specified</td>
-  </tr>
-  <tr>
-    <td>1 Condenser (Water<BR>Cooled)<BR>100% load EWT<BR>75% load EWT<BR>50% load EWT<BR>25% load EWT<BR>0% load EWT<BR>Flow rate (gpm) [L/s]<BR>F.F.A.</td>
-    <td>2 85.0&deg;F<BR>75.0&deg;F<BR>65.0&deg;F<BR>65.0&deg;F<BR>65.0&deg;F<BR>3 3.0 gpm/ton<BR>0.00025<BR>h- ft 2 -&deg;F/Btu</td>
-    <td>29.4&deg;C<BR>23.9&deg;C<BR>18.3&deg;C<BR>18.3&deg;C<BR>18.3&deg;C<BR>0.054 L/s per<BR>kW<BR>0.000044<BR>m 2 -&deg;C/W</td>
-    <td>2 Selected LWT<BR>4 65.0&deg;F<BR>3 Selected<BR>gpm/ton<BR>As Specified</td>
-    <td>2 Selected LWT<BR>4 18.3&deg;C<BR>3 Selected<BR>L/s per kW<BR>As Specified</td>
-  </tr>
-  <tr>
-    <td>1 Condenser (Air Cooled)<BR>100% load EDB<BR>75% load EDB<BR>50% load EDB<BR>25% load EDB<BR>0% load EDB<BR>F.F.A.</td>
-    <td>95.0&deg;F<BR>80.0&deg;F<BR>65.0&deg;F<BR>55.0&deg;F<BR>55.0&deg;F<BR>0.0 h- ft 2<BR>-&deg;F/Btu</td>
-    <td>35&deg;C<BR>26.7&deg;C<BR>18.3&deg;C<BR>12.8&deg;C<BR>12.8&deg;C<BR>0.0 m 2 -&deg;C/W</td>
-    <td colspan="2">No Rating Requirements</td>
-  </tr>
-  <tr>
-    <td>1 Condenser<BR>(Evaporatively Cooled)<BR>100% load EWB<BR>0% load EWB<BR>F.F.A.</td>
-    <td>75.0&deg;F<BR>50.0&deg;F<BR>0.0 h- ft 2<BR>-&deg;F/Btu</td>
-    <td>23.9&deg;C<BR>10.0&deg;C<BR>0.0 m 2 -&deg;C/W</td>
-    <td colspan="2">No Rating Requirements</td>
-  </tr>
-  <tr>
-    <td>Air-Cooled Without<BR>Condenser<BR>100% load SDT<BR>0% load SDT</td>
-    <td>125.0&deg;F<BR>55.0&deg;F</td>
-    <td>51.7&deg;C<BR>12.8&deg;C</td>
-    <td colspan="2">No Rating Requirements</td>
-  </tr>
-  <tr>
-    <td>Water and Evaporatively-<BR>Cooled Without<BR>Condenser<BR>100% load SDT<BR>0% load SDT</td>
-    <td>105.0&deg;F<BR>65.0&deg;F</td>
-    <td>40.6&deg;C<BR>18.3&deg;C</td>
-    <td colspan="2">No Rating Requirements</td>
-  </tr>
-  <tr>
-    <td colspan="5">1 If the unit Manufacturer’s recommended minimum temperatures are greater than those specified in<BR>Table 3, then those may be used in lieu of the specified temperatures.<BR>2 Correction for Fouling Factor Allowance<BR>3 The flow rates are to be held constant at full load values for all part-load conditions.<BR>4 For part-load entering condenser water temperatures, the temperature should vary linearly from<BR>the selected<BR>EWT at 100% load to 65.0 oF at 50% loads, and fixed at 65.0&deg;F for 50% to 0% loads.<BR>SDT - saturated discharge temperature<BR>LWT - leaving water (liquid) temperature<BR>EWT - entering water (liquid) temperature<BR>EDB - entering air dry-bulb temperature<BR>EWB - entering air wet-bulb temperature<BR>F.F.A. - Fouling Factor Allowance</td>
-  </tr>
-</table>
-
-### Electric Chiller Model Based on Condenser Leaving Temperature
-
-#### Overview
-
-This model (object name Chiller:Electric:ReformulatedEIR) simulates the thermal performance of an electric liquid chiller and the power consumption of its compressor(s). The model, developed by Hydeman et al. (2002) as part of the CoolTools™ project sponsored by Pacific Gas and Electric Company (PG&E), is an empirical model similar to EnergyPlus’ Chiller:Electric:EIR model. The model uses performance information at reference conditions along with three curve fits for cooling capacity and efficiency to determine chiller operation at off-reference conditions. The model has the same capabilities as the Chiller:Electric:EIR model, but can potentially provide significant accuracy improvement over the Chiller:Electric:EIR model for chillers with variable-speed compressor motor drives and/or variable condenser water flow applications.
-
-Chiller performance curves can be generated by fitting manufacturer’s catalog data or measured data. Performance curves developed primarily from manufacturer’s performance data are provided in the EnergyPlus Reference DataSets (Chillers.idf and AllDataSets.idf). This chiller model can be used to predict the performance of various chiller types (e.g., reciprocating, screw, scroll, and centrifugal) with water-cooled condensers. The model does not simulate the thermal performance or the power consumption of associated pumps or cooling towers. This auxiliary equipment must be modeled using other EnergyPlus models (e.g. CoolingTower:SingleSpeed).
-
-The main difference between this model and the Chiller:Electric:EIR model is the condenser fluid temperature used in the associated performance curves: the Chiller:Electric:ReformulatedEIR model uses the LEAVING condenser water temperature while the Chiller:Electric:EIR model uses the ENTERING condenser water temperature. In addition, the Energy Input to Cooling Output Function of Part Load Ratio curve for this reformulated EIR chiller model includes the condenser leaving water temperature as an independent variable in addition to part-load ratio. Since the leaving condenser water temperature is a function of load, chiller performance, and condenser entering water temperature, EnergyPlus must iterate to converge on a solution for each simulation time step.
-
-#### Model Description
-
-The chiller model uses user-supplied performance information at reference conditions along with three performance curves (curve objects) for cooling capacity and efficiency to determine chiller operation at off-reference conditions. The three performance curves are:
-
-1)    Cooling Capacity Function of Temperature Curve
-
-2)    Energy Input to Cooling Output Ratio Function of Temperature Curve
-
-3)    Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve
-
-·        The cooling capacity function of temperature curve is a biquadratic performance curve with two independent variables: the leaving chilled water temperature and the leaving condenser water temperature. The output of this curve is multiplied by the reference capacity to give the full-load cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation (otherwise the program issues warning messages).
-
-<div>$$ChillerCapFTemp = a + b({T_{cw,l}}) + c{({T_{cw,l}})^2} + d({T_{cond,l}}) + e{({T_{cond,l}})^2} + f({T_{cw,l}})({T_{cond,l}})$$</div>
-
-where
-
-*ChillerCapFTemp* = Cooling capacity factor, equal to 1 at reference conditions
-
-*T<sub>cw,l</sub>*            = leaving chilled water temperature, ˚C
-
-*T<sub>cond,l</sub>*<sub>            </sub>= leaving condenser water temperature, ˚C. This will be the water temperature entering the condenser loop (e.g., entering the cooling tower). If the chiller is a heat recovery chiller,then the condenser leaving temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers.
-
-·        The energy input to cooling output ratio function of temperature curve is a biquadratic performance curve that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and the leaving condenser water temperature. The EIR is the inverse of the COP. The output of this curve is multiplied by the reference EIR (inverse of the reference COP) to give the full-load EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified in the input data file by the user. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation (otherwise the program issues warning messages).
-
-<span>\(ChillerEIRFTemp = a + b({T_{cw,l}}) + c{({T_{cw,l}})^2} + d({T_{cond,l}}) + e{({T_{cond,l}})^2} + f({T_{cw,l}})({T_{cond,l}})\)</span>where
-
-*ChillerEIRFTemp* = Energy input to cooling output factor, equal to 1 at reference conditions
-
-*T<sub>cw,l</sub>*      = leaving chilled water temperature, ˚C
-
-*T<sub>cond,l</sub>*<sub>     </sub>= leaving condenser water temperature, ˚C. This will be the water temperature entering the condenser loop (e.g., entering the cooling tower). If the chiller is a heat recovery chiller,then the condenser leaving temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers.
-
-·        The energy input to cooling output ratio function of part-load ratio curve parameterizes the variation of the energy input ratio (EIR). The output of this curve is multiplied by the reference EIR (inverse of the reference COP) and the Energy Input to Cooling Output Ratio Function of Temperature Curve to give the EIR at the specific temperatures and part-load ratio at which the chiller is operating. This curve should have a value of 1.0 at the reference leaving condenser water temperature with part-load ratio equal to 1.0. It is recommended that this performance curve be developed using both full- and part-load performance data. The bicubic curve should be valid for the range of condenser water temperatures and part-load ratios anticipated for the simulation (otherwise the program issues warning messages). Either of the following two types of curves can be used.
-
-The first type is a bicubic performance curve that parameterizes the variation of the chiller input power ratio as a function of the leaving condenser water temperature and the part-load ratio. The part-load ratio is the actual cooling load divided by the chiller’s available cooling capacity.
-
-<div>$$ChillerEIRFPLR = a + b({T_{cond,l}}) + c{({T_{cond,l}})^2} + d(PLR) + e{(PLR)^2} + f({T_{cond,l}})(PLR) + g{(PLR)^3}$$</div>
-
-<div>$$ChillerEIRFPLR = \,{\raise0.7ex\hbox{${{P_{chiller}}}$} \!\mathord{\left/ {\vphantom {{{P_{chiller}}} {{P_{ref}}\left( {ChillerCapFTemp} \right)\left( {ChillerEIRFTemp} \right)}}}\right.}\!\lower0.7ex\hbox{${{P_{ref}}\left( {ChillerCapFTemp} \right)\left( {ChillerEIRFTemp} \right)}$}}$$</div>
-
-where
-
-*ChillerEIRFPLR* = Energy input to cooling output factor, equal to 1 at the reference leaving condenser water temperature and PLR = 1.0
-
-*T<sub>cond,l</sub>*<sub>     </sub>= leaving condenser water temperature, ˚C. This will be the water temperature entering the condenser loop (e.g., entering the cooling tower). If the chiller is a heat recovery chiller,then the condenser leaving temperature is adjusted to account for both fluid streams as described in the section above on heat recovery chillers.
-
-*PLR*      =Part load ratio = (cooling load) / (chiller’s available cooling capacity)
-
-*P<sub>chiller</sub> = chiller power at specific PLR*
-
-*P<sub>ref</sub> = <span>\({\mathop Q\limits^ \bullet_{ref}}\)</span>/COP<sub>ref</sub>*
-
-Note: Although a bicubic curve requires 10 coefficients (ref. Curve:Bicubic), coefficients 7, 9 and 10 are typically not used in the performance curve described here and should be entered as 0 unless sufficient performance data and regression accuracy exist to justify the use of these terms of the bicubic curve.
-
-The second type is a Chiller Part Load Custom Curve that parameterizes the variation of EIR as a function of the normalized dT, normalized Tdev and the PLR.
-
-<div>$$ChillerEIRFPLR = a + b(dT^*) + c(dT^*)^2 + d \cdot PLR + e \cdot PLR^2 + f \cdot (dT^*) \cdot PLR + g \cdot (dT^*)^3  + h \cdot PLR^3 + i \cdot (dT^*)^2 \cdot PLR + j \cdot (dT^*) \cdot PLR^2 + k \cdot (dT^*)^2 \cdot PLR^2 + l \cdot (T_{dev}^*) \cdot PLR^3$$</div>
-
-<div>$$dT^* = dT / dT_{ref}$$</div>
-
-<div>$$T_{dev}^* = T_{dev} / dT_{ref}$$</div>
-
-where
-
-$dT$ = the delta of temperature across the leaving condenser water temperature and leaving evaporator water temperature of a chiller (lift)
-
-$dT^*$ = the normalized fractional lift
-
-$dT_{ref}$ = the lift under the reference condition
-
-PLR = the part load ratio
-
-$T_{dev}$ = the deviation of leaving chilled water temperature from the reference condition
-
-$T_{dev}^*$ = the normalized Tdev term
-
-All three of the performance curves are accessed through EnergyPlus’ built-in performance curve equation manager (curve:biquadratic, curve:bicubic, and Curve:ChillerPartLoadWithLift). Note that the above three performance curves use the leaving condenser water temperature as an independent variable, instead of the entering condenser water temperature used in the performance curves for the Chiller:Electric:EIR model. Since the leaving condenser water temperature is calculated based on the condenser heat transfer rate, which is a function of the load to be met by the chiller, chiller compressor power, and the false loading (detailed calculations are given below), iterative calculations are required to determine the actual (converged) leaving condenser water temperature. The program uses the leaving condenser water temperature from the previous iteration to calculate values for each of the three performance curves described above. After obtaining the condenser heat transfer rate, the leaving condenser water temperature is recalculated. When the difference between the leaving condenser water temperature calculated on successive iterations is less than 0.0001<sup>°</sup>C, the solution is assumed to have converged. Warning messages are issued if the calculated solution for leaving condenser water temperature and/or part-load ratio falls outside the valid range specified for the chiller’s performance curves. If these warnings are issued, the user may choose to extend the range for the performance curves (only if a small extension is required since model extrapolation may produce significant errors) or a different chiller and associated performance curves with extended performance range can be located and used for the simulation.
-
-Note: Chiller:Electric:ReformulatedEIR objects and their associated performance curve objects are developed using performance information for a specific chiller and should almost always be used together for an EnergyPlus simulation. Changing the object input values, or swapping performance curves between chillers, should be done with extreme caution. For example, if the user wishes to model a chiller size that is different from the reference capacity, it is highly recommended that the reference flow rates be scaled proportionately to the change in reference capacity. Although this model can provide more accurate prediction than the Chiller:Electric:EIR model, it requires more performance data to develop the associated performance curves (at least 12 points from full-load performance and 7 points from part-load performance).
-
-Although performance curve data sets for 160 chillers are provided in the EnergyPlus Reference DataSets (Chillers.idf and AllDataSets.idf), they may not meet the requirements for specific applications. One can develop performance curves from performance data using two available techniques (Hydeman and Gillespie 2002). The first technique is called the Least-squares Linear Regression method and is used when sufficient performance data exist to employ standard least-square linear regression techniques. The second technique is called Reference Curve Method and is used when insufficient performance data exist to apply linear regression techniques. A detailed description of both techniques can be found in the reference mentioned above.
-
-For any simulation time step, the chiller’s available cooling capacity is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{avail}}\,\, = \,\,{\mathop Q\limits^ \bullet_{ref}}\left( {ChillerCapFTemp} \right)$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{ref}}\)</span>     = chiller capacity at reference conditions (reference temperatures and flow rates defined by the user), W
-
-<span>\({\mathop Q\limits^ \bullet_{avail}}\)</span> = available chiller capacity adjusted for current water temperatures, W
-
-The model then calculates the evaporator heat transfer rate required to bring the entering chilled water temperature down to the leaving chilled water setpoint temperature (established using a SetpointManager object and referenced in the PlantLoop object). If this calculated heat transfer rate is greater than the heat transfer rate being requested by the plant equipment operation scheme, then the evaporator heat transfer rate is reset to the requested cooling rate.
-
-The evaporator heat transfer rate is then compared to the available capacity. If the available chiller capacity is sufficient to meet the evaporator heat transfer rate, the leaving chilled water temperature is set equal to the chilled water setpoint temperature. If the requested evaporator heat transfer rate is larger than the available capacity the chilled water leaving the evaporator is allowed to float upward. For this case, the exiting chilled water temperature is calculated based on the water temperature entering the evaporator, the available cooling capacity, and the evaporator mass flow rate as follows:
-
-<div>$${T_{cw,l}} = {T_{cw,e}} - \left( {{\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{avail}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{avail}}} {{{\mathop m\limits^ \bullet  }_{evap}}{C_{p,evap}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop m\limits^ \bullet  }_{evap}}{C_{p,evap}}}$}}} \right)$$</div>
-
-where
-
-*T<sub>cw,l</sub>*            = water temperature leaving the evaporator, ˚C
-
-*T<sub>cw,e</sub>*           = water temperature entering the evaporator, ˚C
-
-<span>\({\mathop m\limits^ \bullet_{evap}}\)</span>         = evaporator mass flow rate, kg/s
-
-*C<sub>p,evap</sub>*         = specific heat of water entering evaporator at *T<sub>cw,e</sub>*, J/kg-˚C
-
-The part-load ratio is then calculated as the ratio of the evaporator heat transfer rate to the available chiller capacity. The part-load ratio is not allowed to be greater than the maximum part-load ratio specified by the user or less than zero as follows:
-
-<div>$$PLR = MAX\left( {0.0,MIN\left( {{\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{evap}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{evap}}} {{{\mathop Q\limits^ \bullet  }_{avail}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{avail}}}$}},\,\,PL{R_{\max }}} \right)} \right)$$</div>
-
-where
-
-*PLR*           = part-load ratio
-
-<span>\({\mathop Q\limits^ \bullet_{evap}}\)</span>         = load to be met by the chiller, W
-
-*PLR<sub>max\\        </sub>*= maximum part-load ratio (specified by the user in the input data file)
-
-Note that the maximum part-load ratio (PLR<sub>max</sub>, specified in the Chiller:Electric:ReformulatedEIR object) used in the equation should be less than or equal to the maximum part-load ratio specified in the “Energy Input to Cooling Output Ratio Function of Part-Load Ratio� performance curve object.
-
-The model assumes that the cooling load is met through chiller unloading down to the minimum unloading ratio. False loading (e.g. hot-gas bypass) is assumed to occur between the minimum unloading ratio and the minimum part-load ratio yielding constant electrical power consumption under these conditions. Below the minimum part-load ratio, the chiller cycles on/off to meet very small loads and the power consumption during the on cycle is the same as when the chiller is operating at the minimum part load ratio. When the chiller part-load ratio is less than the minimum part-load ratio, the on-off cycling ratio of the chiller is calculated as follows and is available as an output variable.
-
-<div>$$ChillerCyclingRatio = MIN\left( {{\raise0.7ex\hbox{${PLR}$} \!\mathord{\left/ {\vphantom {{PLR} {PL{R_{\min }}}}}\right.}\!\lower0.7ex\hbox{${PL{R_{\min }}}$}},\,\,1.0} \right)$$</div>
-
-To properly account for chiller electric power consumption when PLR is less than the minimum unloading ratio, the PLR is reset to the greater of the PLR calculated above and the PLR at the minimum unloading ratio. The result is available as the output variable Chiller Part Load Ratio.
-
-<div>$$PLR = MAX(PLR,PL{R_{MinUnloadRatio}})$$</div>
-
-This revised PLR accounts for the “false loading� (e.g., hot-gas bypass) that is assumed to occur whenever the PLR (based on cooling load divided by available capacity) is less than the minimum unloading ratio specified. The amount of false loading on the chiller is calculated using this revised PLR and is reported as an output variable as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{falseloading}} = \left( {{{\mathop Q\limits^ \bullet  }_{avail}}} \right)\left( {PLR} \right)\left( {ChillerCyclingRatio} \right) - {\mathop Q\limits^ \bullet_{evap}}$$</div>
-
-The electrical power consumption for the chiller compressor(s) for any simulation time step is then calculated using the following equation:
-
-<span>\({P_{chiller}}\, = \,\,\left( {{{\mathop Q\limits^ \bullet  }_{avail}}\,} \right)\,\left( {\frac{1}{{CO{P_{ref}}}}} \right)\,\left( {ChillerEIRFTemp} \right)\left( {ChillerEIRFPLR} \right)\left( {ChillerCyclingRatio} \right)\)</span>where
-
-*P<sub>chiller</sub>*         = Chiller compressor power, W
-
-*COP<sub>ref</sub>*       = Reference coefficient of performance, W/W
-
-Heat rejected by the chiller condenser includes the heat transferred in the evaporator plus a portion or all of the compressor electrical energy consumption. For electric chillers with hermetic compressors, all compressor energy consumption is rejected by the condenser (compressor motor efficiency = *eff<sub>motor</sub>* = 1.0). For chillers with semi-hermetic or open compressors, only a portion of the compressor energy use is rejected by the condenser. The heat transfer rate for the chiller condenser is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{cond}} = \left( {{P_{chiller}} * ef{f_{motor}}} \right) + {\mathop Q\limits^ \bullet_{evap}} + {\mathop Q\limits^ \bullet_{falseloading}}$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{cond}}\)</span>         = condenser heat transfer rate, W
-
-<span>\(ef{f_{motor}}\)</span>       = compressor motor efficiency = fraction of compressor electrical energy consumption rejected as condenser heat
-
-The above curve values are calculated based on the leaving condenser water temperature found through iteration. After obtaining the condenser heat transfer rate, the final leaving condenser water temperature is then calculated as:
-
-<div>$${T_{cond,l}} = {T_{cond,e}} + {\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{cond}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{cond}}} {\mathop {\left( {{{\mathop m\limits^ \bullet  }_{cond}}*{C_{p,cond}}} \right)}\limits^{} }}}\right.}\!\lower0.7ex\hbox{${\mathop {\left( {{{\mathop m\limits^ \bullet  }_{cond}}*{C_{p,cond}}} \right)}\limits^{} }$}}$$</div>
-
-where:
-
-*T<sub>cond,l</sub>*          = water temperature leaving the condenser, ˚C
-
-*T<sub>cond,e</sub>*         = water temperature entering the condenser, ˚C
-
-<span>\({\mathop m\limits^ \bullet_{cond}}\)</span>         = mass flow rate through the condenser, kg/s
-
-<span>\({C_{p,cond}}\)</span>       = specific heat of water entering the condenser at *T<sub>cond,e</sub>*, J/kg-˚C
-
-The final calculations determine the total heat transfer energy for the condenser and evaporator, as well as the total electric energy consumed by the chiller compressor motor(s) and condenser fan(s). The results are available as output variables.
-
-<div>$${Q_{cond}} = {\mathop Q\limits^ \bullet_{cond}}*TimeStepSys*3600$$</div>
-
-<div>$${Q_{evap}} = {\mathop Q\limits^ \bullet_{evap}}\,\,*\,\,TimeStepSys\,\,*\,\,3600$$</div>
-
-<div>$${E_{chiller}} = {P_{chiller}}*\,\,TimeStepSys\,\,*\,\,3600$$</div>
-
-<div>$${E_{cond}} = {P_{cond}}\,\, * \,\,TimeStepSys\,\,*\,\,3600$$</div>
-
-where
-
-*Q<sub>cond</sub>*          = chiller condenser heat transfer energy, J
-
-*Q<sub>evap</sub>*           = chiller evaporator cooling energy, J
-
-*E<sub>chiller</sub>*         = chiller (compressor) electric energy, J
-
-*E<sub>cond</sub>*           = chiller condenser fan electric energy, J
-
-*TimeStepSys* = HVAC system simulation time step, hr
-
-<span>\(3600\)</span>         = conversion factor, sec/hr
-
-#### Electric Reformulated EIR Chiller with Heat Recovery Option
-
-Heat from the electric reformulated EIR chiller condenser may be recovered. The heat recovery water flow rate is specified by the user along with the input and output nodes connected to the heat recovery loop. The algorithms are identical to those used for Chiller:Electric and Chiller:Electric:EIR. Refer to the section entitled Chillers with Plant Heat Recovery for details.
-
-#### Standard Rating (Integrated Part Load Value)
-
-Integrated Part Laod Value (IPLV) calculations for Reformulated EIR chiller are similar to what are described above for EIR chillers. The only difference with Reformulated EIR chiller is that it calls an iterative subroutine (SolveRegulaFalsi) to obtain a condenser water outlet temperature which corresponds to condenser inlet temperature at reduced capacity conditions as outlined in Table 51 above. SolveRegulaFalsi is a general utility routine for finding the zero of a function. In this case it finds the condenser inlet temperature that will zero the residual function – the difference between calculated condenser inlet temperature and desired condenser inlet temperature per ANSI/AHRE 550/590, 2011 (table 42 above) divided by desired condenser inlet temperature.
-
-#### References
-
-Hydeman, M., N. Webb, P. Sreedharan, and S. Blanc. 2002. Development and Testing of a Reformulated Regression-Based Electric Chiller Model. ASHRAE Transactions HI-02-18-2.
-
-Hydeman, M. and K.L. Gillespie. 2002. Tools and Techniques to Calibrate Electric Chiller Component Models. ASHRAE Transactions AC-02-9-1.
-
-Hydeman, M., K. Gillespie, and R. Kammerud. 1997. PG&E’s CoolTools project: A toolkit to improve evaluation and operation of chilled water plants. Presented at the Cool$ense National Forum on Integrated Chilled Water Retrofits, Sep. 1997. Berkeley California: Lawrence Berkeley National Laboratory.
-
-### Engine Driven Chiller
-
-The engine driven chiller (Object name: Chiller:EngineDriven) is the empirical model from the Building Loads and System Thermodynamics (BLAST) program. Fitting catalog data to a third order polynomial equations generates the chiller performance curves.  Three sets of coefficients are required to model the open centrifugal chiller as discussed in the section, titled, ‘Electric Chiller Based on Fluid Temperature Differences’. Additional curve fits are required to model the engine.  Because the model inherently involves the lower heating value of the fuel, a reference temperature is also involved in the calculations, which manufacturers present at 25°C.
-
-The engine model was also developed for the BLAST program. It was adapted for use in EnergyPlus. This model is used for both the engine driven generator and the engine driven chiller.  It uses the following set of equations all of which are quadratic fits to the PLR (Part Load Ratio) of the generator.  The coefficients must be derived from manufacturers data.
-
-<div>$$\frac{{chiller\,\,cooling\,\,load}}{{fuel\,\,energy\,\,input}} = \frac{{chiller\,\,cooling\,\,load}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {a_1} + {a_2}PLR + {a_3}PL{R^2}$$</div>
-
-The exhaust gas temp and flow rate are used if a stack heat exchanger is used to recover waste heat from the exhaust.  This temperature is the inlet temperature to the heat exchanger which is modeled in a UA-effectiveness form:
-
-<div>$$\frac{{Total\,Exhaust\,heat}}{{fuel\,energy\,input}} = \frac{{Total\,\,Exhaust\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {d_1} + {d_2}PLR + {d_3}PL{R^2}$$</div>
-
-<div>$$\frac{{Exhaust\,\,Gas\,\,Temp\,\,\left\{ K \right\}}}{{fuel\,\,energy\,\,input}} = \frac{{Exhaust\,\,Gas\,\,Temp\,\,\left\{ K \right\}}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {e_1} + {e_2}PLR + {e_3}PL{R^2}$$</div>
-
-The exhaust flow rate is then calculated as:
-
-<div>$${\dot m_{exhaust}} = \frac{{Total\,\,Exhaust\,\,heat}}{{C{p_{exhaust}} \cdot \left( {{T_{exhaust}} - {T_{reference}}} \right)}}$$</div>
-
-where T<sub>reference</sub> is the reference temperature for the fuel lower heating value, and is given as 25°C in manufacturer’s data, and
-
-<div>$${T_{stack}} = {T_{DesignMinExhaust}} + {\frac{{\left( {{T_{exhaust}} - {T_{DesignMinExhaust}}} \right)}}{{{\rm{exp}}\left( {\frac{{{\rm{UA}}}}{{{{{\rm{\dot m}}}_{{\rm{exhaust}}}}C{p_{exhaust}}}}} \right)}}^2}$$</div>
-
-Finally, heat recovered from the lube oil and the water jacket are accounted for as follows:
-
-<div>$$\frac{{Recoverable\,\,jacket\,\,heat}}{{fuel\,\,energy\,\,input}} = \frac{{Recoverable\,\,jacket\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {b_1} + {b_2}PLR + {b_3}PL{R^2}$$</div>
-
-<div>$$\frac{{Recoverable\,\,lube\,\,oil\,\,heat}}{{fuel\,\,energy\,\,input}} = \frac{{Recoverable\,\,lube\,\,oil\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {c_1} + {c_2}PLR + {c_3}PL{R^2}$$</div>
-
-#### Chiller Basin Heater
-
-Calculations are also made to estimate the electric power input to the basin heater for chillers with evaporatively-cooled condensers. The chillers which calculate basin heater power are Chiller:Electric:EIR, Chiller:Electric, Chiller:ConstantCOP, Chiller:EngineDriven and Chiller:CombustionTurbine.A schedule may be used to disable the basin heater during regular maintenance periods or other time periods (e.g., during summer). If a schedule is not provided, the basin heater is assumed to be available the entire simulation time period. The basin heater operates when it is scheduled on, the outdoor air dry-bulb temperature is below the basin heater setpoint temperature, and the chiller is not active (i.e., chiller is not operating for the simulation time step --- for example, when there is no cooling load to be met by the chiller, *or if there is no water flow through the chiller due to a chiller or pump availability schedule, etc.*). The user is required to enter a basin heater capacity (watts per degree Kelvin) and a heater setpoint temperature (<sup>o</sup>C) if they want to model basin heater electric power.
-
-<div>$$\begin{array}{l}{P_{heater,basin}} = 0.0\\IF\left( {ChillerIsOFF} \right)THEN\\\,\,\,\,\,\,IF\left( {Schedul{e_{heater,basin}}\,is\,Defined} \right)THEN\\\,\,\,\,\,\,\,\,\,\,\,\,IF\left( {CA{P_{heater,basin}}\, > \,0\,.AND.\,Schedul{e_{heater,basin}}\, = \,ON} \right)THEN\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,{P_{heater,basin}} = \,MAX\left( {0.0,CA{P_{heater,basin}}\left( {{T_{setpoint,basin}} - {T_{db,outdoor}}} \right)} \right)\,\,\,\,\,\,\\\,\,\,\,\,\,\,\,\,\,\,ENDIF\\\,\,\,\,\,ELSE\\\,\,\,\,\,\,\,\,\,\,\,IF\left( {CA{P_{heater,basin}}\, > \,0\,} \right)THEN\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,{P_{heater,basin}} = \,MAX\left( {0.0,CA{P_{heater,basin}}\left( {{T_{setpoint,basin}} - {T_{db,outdoor}}} \right)} \right)\,\,\,\,\,\,\\\,\,\,\,\,\,\,\,\,\,\,ENDIF\,\\\,\,\,\,\,ENDIF\\ENDIF\end{array}$$</div>
-
-<div>$${E_{heater,basin}} = \left( {{P_{heater,basin}}} \right)\left( {TimeStepSys} \right)3600$$</div>
-
-where:
-
-<span>\({P_{heater,basin}}\)</span> = Chiller basin heater electric power (W)
-
-<span>\({E_{heater,basin}}\)</span>= Chiller basin heater electric consumption (J)
-
-*T<sub>setpoint,basin</sub>* = Basin heater setpoint temperature, user input (<sup>o</sup>C)
-
-*T<sub>db,outdoor</sub>*    = Outdoor air dry-bulb temperature (<sup>o</sup>C)
-
-*CAP<sub>heater,basin</sub>* = Basin heater capacity, user input (W/K)
-
-*Schedule<sub>heater,basin</sub>* = Basin heater schedule, user input (schedule value &gt; 0 means ON)
-
-*ChillerIsOFF =*Logical variable denoting that the chiller is not operating for the current simulation time step (e.g.,  there is no cooling load to be met by the chiller, or if there is no water flow through the chiller due to a chiller or pump availability schedule, etc.)
-
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-
-<!--RemoveStart-->
-Simulation Models - Encyclopedic Reference
-==========================================
-
-The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of “Heat Balance�, “HVAC�, and “Plant�.  With the integrated solution, these designations signify where the effects of these models have their first impacts.
-
-Main Sections:
-
-* [Ice Thermal Storage](#IceStorage)
-* [Coils](#Coils)
-* [HVAC Controllers](#Controllers)
-* [Baseboard Heaters](#Baseboards)
-<!--RemoveEnd-->
-
-Ice Thermal Storage <a name="IceStorage"></a>
--------------------
-
-### Simple Ice Storage Model
-
-#### Overview
-
-This model (object name ThermalStorage:Ice:Simple) simulates the performance of an ice storage tank. The model is based on an integrated chiller and storage tank model developed for a special optimization project (Henze and Krarti 2002). This implementation removed the integrated chiller and allows the tank to be charged by any chiller configuration in an EnergyPlus plant loop..
-
-This thermal storage model is based on a simple simulation of an ice storage tank with a fixed capacity.  The tank is charged, or frozen, in an ice-on-coil configuration where ice builds up on the outside of the tubes carrying the brine or glycol solution from the chiller.  There are two discharge (melt) options, internal or external.  Internal melt uses the same fluid tubes for charging and discharging.  External melt uses a separate fluid path for discharge such that the outer layers of ice melt first.  The ice storage model includes an implied 3-way valve to control the amount if charge/discharge based on the incoming water temperature and the outlet node setpoint temperature.  The tank is controlled using the PlantEquipmentOperation:ComponentSetpoint plant operation scheme, and requires that a setpoint be placed by a setpoint manager on the ice storage Plant Outlet Node.  The model currently does not calculate any tank losses.
-
-#### Model Description
-
-##### Initialization
-
-The storage tank is assumed to be fully charged (full of ice) at the beginning of each environment.  The tank is then allowed to charge and discharge during the warmup days of the environment.
-
-##### Control
-
-The ice storage module is a passive component and will accept any flow rate placed on the inlet node.  The load on the ice storage tank is determined by the inlet node flow rate, the inlet node temperature, and the outlet node setpoint temperature.  A positive load indicates a request for cooling and the tank discharges if possible.  A negative load indicates a request for charging the tank if possible.  A zero load indicates the tank is dormant in which case all flow bypasses the tank and the outlet node temperature is set to the inlet node temperature.  The model includes an implied 3-way valve which controls the leaving water temperature to the outlet node setpoint temperature if possible.
-
-##### Charging
-
-When charging is requested, the following limits are calculated to determine the actual charging rate:
-
-1)    If the entering water temperature is greater than –1C, the charging rate is zero.
-
-2)    If the entering water temperature is greater than or equal to the outlet setpoint temperature, the charging rate is zero.
-
-3)    If the current fraction of ice stored is 1.0, the tank is fully charge, and the charging rate is zero.
-
-4)    If the requested charging rate times the current system timestep is more than the remaining uncharged storage capacity, the charging rate is limited to that required to completely fill the tank.
-
-5)    The maximum charging rate which the chilled water flow can provide is determined by the entering water temperature and flow rate and an outlet temperature which is the minimum of –1C or the outlet setpoint temperature.
-
-6)    The maximum charging rate which the tank can accept is calculated by the following equations developed in the prior work (Henze and Krarti 2002):
-
-*UAIceCh* = ( 1.3879 - 7.6333\**y* + 26.3423\**y*<sup>2</sup> - 47.6084\**y*<sup>3</sup> + 41.8498\**y*<sup>4</sup> - 14.2948\**y*<sup>5</sup> ) \* *ITSNomCap* / *TimeInterval* / 10.0
-
-where:
-
-*UAIceCh*   = UA rate for charging
-
-*y*                = Current ice fraction stored
-
-*ITSNomCap*          = Nominal storage capacity [GJ]
-
-TimeInterval = 3600 [s]
-
-The smallest charging rate determined by the above rules is selected and the corresponding leaving water temperature is calculated.
-
-##### Discharging
-
-When discharging is requested, the following limits are calculated to determine the actual charging rate:
-
-1)    If the entering water temperature is less than 1C, the discharge rate is zero.
-
-2)    If the entering water temperature is less than or equal to the outlet setpoint temperature, the discharge rate is zero.
-
-3)    If the current fraction of ice stored is 0.0, the tank is fully discharged, and the discharge rate is zero.
-
-4)    If the requested discharge rate times the current system timestep is more than the remaining charged storage capacity, the discharge rate is limited to that required to completely deplete the ice in the tank.
-
-5)    The maximum discharge rate which the chilled water flow can accept is determined by the entering water temperature and flow rate and an outlet temperature which is the maximum of 1C or the outlet setpoint temperature.
-
-6)    The maximum discharge rate which the tank can deliver is calculated by the following equations developed in the prior work (Henze and Krarti 2002):
-
-For ice-on-coil internal melt:
-
-*UAIceDisCh* = ( 1.3879 - 7.6333\**y* + 26.3423\**y*<sup>2</sup> - 47.6084\**y*<sup>3</sup> + 41.8498\**y*<sup>4</sup> - 14.2948\**y*<sup>5</sup> ) \* *ITSNomCap* / *TimeInterval* / 10.0
-
-For ice-on-coil external melt:
-
-*UAIceDisCh* = ( 1.1756 - 5.3689\**y* + 17.3602\**y*<sup>2</sup> - 30.1077\**y*<sup>3</sup> + 25.6387\**y*<sup>4</sup> - 8.5102\**y*<sup>5</sup> ) \* *ITSNomCap* / *TimeInterval* / 10.0
-
-where:
-
-UAIceDisCh            = UA rate for discharging
-
-*y*                = 1 - Current ice fraction stored
-
-*ITSNomCap*          = Nominal storage capacity [GJ]
-
-TimeInterval = 3600 [s]
-
-The smallest discharge rate determined by the above rules is selected and the corresponding leaving water temperature is calculated.
-
-#### References
-
-Henze, Gregor P. and Moncef Krarti. 2002. Predictive Optimal Control of Active and Passive Building Thermal Storage Inventory, Final Report for Phase I:  Analysis, Modeling, and Simulation.  U.S. Department of Energy National Energy Technology Laboratory Cooperative Agreement DE-FC-26-01NT41255, December 2002.
-
-### Detailed Ice Storage Model
-
-The following section describes how the detailed ice storage model works in EnergyPlus (object name ThermalStorage:Ice:Detailed).
-
-#### Charging and Discharging Equation
-
-The actual performance of the ice storage unit depends on the physical geometry, materials, and characteristics of the ice storage unit.  In analyzing performance data trends from ice storage manufacturers, it was determined that the following equation would work well for the discharging process:
-
-<div>$${q^*} = \left[ {C1 + C2\left( {1 - {P_c}} \right) + C3{{\left( {1 - {P_c}} \right)}^2}} \right] + \left[ {C4 + C5\left( {1 - {P_c}} \right) + C6{{\left( {1 - {P_c}} \right)}^2}} \right]\Delta T_{lm}^*$$</div>
-
-or
-
-<div>$${q^*} = \left[ {C1 + C2\left( {{P_d}} \right) + C3{{\left( {{P_d}} \right)}^2}} \right] + \left[ {C4 + C5\left( {{P_d}} \right) + C6{{\left( {{P_d}} \right)}^2}} \right]\Delta T_{lm}^*$$</div>
-
-where:
-
-<div>$${q^*} \equiv \frac{{q\Delta t}}{{{Q_{stor}}}}$$</div>
-
-<div>$$\Delta T_{lm}^* \equiv \frac{{\Delta {T_{lm}}}}{{\Delta {T_{no\min al}}}}$$</div>
-
-<div>$$\Delta {T_{lm}} \equiv \frac{{{T_{brine,in}} - {T_{brine,out}}}}{{\ln \left( {\frac{{{T_{brine,in}} - {T_{brine,freeze}}}}{{{T_{brine,out}} - {T_{brine,freeze}}}}} \right)}}$$</div>
-
-q is the instantaneous heat transfer rate,
-
-Qstor is the total latent storage capacity,
-
-Dt is a time step used in the curve fit (usually one hour),
-
-DT<sub>nominal</sub> is a nominal temperature difference (18°F = 10°C),
-
-T<sub>brine,in</sub> is the tank brine inlet temperature,
-
-T<sub>brine,out</sub> is the tank brine outlet temperature,
-
-T<sub>freeze</sub> is the freezing temperature of water or the latent energy storage material,
-
-P<sub>c</sub> is the fraction charged, and
-
-P<sub>d</sub> is the fraction discharged.
-
-Likewise, the charging process of the ice storage device can be characterized by the following equation that is similar in form to the discharging equation:
-
-<div>$${q^*} = \left[ {C1 + C2\left( {{P_c}} \right) + C3{{\left( {{P_c}} \right)}^2}} \right] + \left[ {C4 + C5\left( {{P_c}} \right) + C6{{\left( {{P_c}} \right)}^2}} \right]\Delta T_{lm}^*$$</div>
-
-Note that the time step might differ from the time step used within the EnergyPlus simulation.  These are actually two separate time steps and are kept separate.
-
-#### Charging Algorithm
-
-During charging, manufacturers have stated that they attempt to charge the unit at the maximum rate until the unit is completely charged.  This, of course, occurs during off-peak electric hours.  Thus, once the setpoint has been scheduled for charging, the unit will charge at the maximum possible rate.  This means that the flow rate through the ice storage device equals the flow to the component (or no bypass).  The only time flow to the ice storage unit would be reduced is at the end of the charge cycle when more ice making capacity is available in a particular time step than is needed to fully charge the tank.  In this case, the flow to the tank would be reduced appropriately to top off the tank storage capacity.  We also have a setpoint goal for the outlet temperature of the ice storage device as defined by the setpoint schedule.
-
-In solving the performance of the ice storage unit, we have effectively two equations (one of which is non-linear) and two unknowns.  The equations are:
-
-<div>$${q^*} = \left[ {C1 + C2\left( {{P_c}} \right) + C3{{\left( {{P_c}} \right)}^2}} \right] + \left[ {C4 + C5\left( {{P_c}} \right) + C6{{\left( {{P_c}} \right)}^2}} \right]\Delta T_{lm}^*$$</div>
-
-from which we can obtain the component load (q) and
-
-<div>$$q = \dot m{C_p}\left( {{T_i} - {T_o}} \right)$$</div>
-
-Both of these equations have q and T<sub>o</sub> as unknowns.  However, since the setpoint temperature is the goal for T<sub>o</sub>, we can use this as an initial guess for T<sub>o</sub>.  Below is an outline of the algorithm:
-
-n Initialize T<sub>o</sub>= T<sub>set</sub>
-
-n Calculate LMTD\*
-
-n Calculate q\* from charging equation for the current percent charged (We will assume that the EnergyPlus time step is sufficiently small so that we do not need to find the average percent charged for the time step.  This was necessary when one hour time steps were used as in BLAST, but EnergyPlus generally uses relatively short time steps.  Since there is already some iteration involved in the solution, we would like to avoid another layer of iteration if at all possible.  One alternative that could be implemented would be to make a second pass with a closer average value based on what happens during the time step.  This would effectively double the execution time for the model and would need to be justified before implementation.)
-
-n Calculate T<sub>o,new</sub> and compare it to T<sub>o</sub>
-
-n Use T<sub>o,new</sub> to calculate a new LMTD\* and iterate until T<sub>o</sub> converges to some acceptable level
-
-Charging would continue in subsequent time steps until the final state of the ice storage unit at the end of a particular time step is fully charged.  If running a chiller would “overcharge� the tank, then the flow to the tank would be reduced (greater than zero bypass flow) while maintaining the same setpoint temperature coming out of the tank (though not necessarily out of the component).
-
-#### Discharging Algorithm
-
-During discharging, we cannot assume that all of the flow is sent through the ice storage unit and thus some of it may be bypassed around it locally.  This ice storage model includes a built-in bypass leg to accommodate this without requiring the user to enter this additional information.  This also allows the bypass leg/valve to be controlled by the ice storage unit.
-
-While we cannot assume that all of the flow is sent through the ice storage unit, we can use that as an initial guess in order to determine the current performance of the ice storage system.  Most of the discharging algorithm then becomes very similar to the charging process.
-
-In solving the performance of the ice storage unit, we have effectively two equations (one of which is non-linear) and two unknowns.  The equations are:
-
-<div>$${q^*} = \left[ {C1 + C2\left( {{P_d}} \right) + C3{{\left( {{P_d}} \right)}^2}} \right] + \left[ {C4 + C5\left( {{P_d}} \right) + C6{{\left( {{P_d}} \right)}^2}} \right]\Delta T_{lm}^*$$</div>
-
-from which we can obtain the component load (q) and
-
-<div>$$q = \dot m{C_p}\left( {{T_i} - {T_o}} \right)$$</div>
-
-Both of these equations have q and T<sub>o</sub> as unknowns.  However, since the setpoint temperature is the goal for T<sub>o</sub>, we can use this as an initial guess for T<sub>o</sub>.  Below is an outline of the algorithm:
-
-n Initialize T<sub>o</sub>= T<sub>set</sub>
-
-n Calculate LMTD\*
-
-n Calculate q\* from charging equation for the current percent charged (we will assume that the EnergyPlus time step is sufficiently small so that we do not need to find the average percent charged for the time step; this was necessary when one hour time steps were used as in BLAST, but EnergyPlus generally uses relatively short time steps)
-
-n Calculate T<sub>o,new</sub> and compare it to T<sub>o</sub>
-
-n Use T<sub>o,new</sub> to calculate a new LMTD\* and iterate until T<sub>o</sub> converges to some acceptable level
-
-n Once T<sub>o</sub> has converged, we need to compare this value again to T<sub>set</sub>.  If T<sub>o</sub> is greater than or equal to T<sub>set</sub>, then we either just met the load (equal) or can’t quite meet it (greater than).  In this case, we simply leave T<sub>o</sub> as is because we cannot meet the setpoint temperature.
-
-n If T<sub>o</sub> is less than T<sub>set</sub>, then we have more capacity available than we need.  In this case, we need to bypass some of the flow.  Since the load on the ice storage device and the outlet temperature are not changing (we are just reducing the flow), we only need to split the flow and do not need to recalculate the action of the ice storage device.  Some systems may be slightly dependent on the actual flow through the device itself.  However, in an actual application, this only means that a slightly different amount will bypass the device.  The overall energy impact will be the same and thus it is not necessary to be concerned about flow rate dependence.
-
-Discharging would continue in subsequent time steps until the final state of the ice storage unit at the end of a particular time step is fully discharged.
-
-#### References
-
-Strand, R.K. 1992. "Indirect Ice Storage System Simulation," M.S. Thesis, Department of Mechanical and Industrial Engineering, University of Illinois at Urbana-Champaign.
-
-Coils <a name="Coils"></a>
------
-
-### Chilled-Water-Based Air Cooling Coil
-
-The input object Coil:Cooling:Water is simpler than the detailed geometry model.  The simple model provides a good prediction of the air and water outlet conditions without requiring the detailed geometric input required for the detailed model.  A greatly simplified schematic of enthalpy and temperature conditions in a counter flow cooling/dehumidifying coil is shown in the schematic Figure 162.  The input required to model the coil includes only a set of thermodynamic design inputs, which require no specific manufacturer's data.  The coil simulation model is essentially a modification of one presented by Elmahdy and Mitalas (1977), TRNSYS, 1990 and Threlkeld, J.L. 1970.  The model calculates the UA values required for a Dry, Wet and Part Wet & Part Dry Coil and iterates between the Dry and Wet Coil to output the fraction wet.  There are two modes of flow operation for this model: Cross Flow, which is widely applicable in HVAC systems and the second being Counter flow mode. The default value in program is set up for Counter Flow.  In addition the coil has two modes of analysis: Simple Analysis and Detailed Analysis. The Simple analysis mode operates the coil as either wet or dry while the detailed mode simulates the coil as part wet part-dry. While the detailed mode provides more accurate results, it is significantly slower than the simple model. The simple mode gives good results for an annual simulation but will not be adequate for a time step performance analysis.
-
-![](media/image3304.svg.png)
-
-Figure 162.  Simplified Schematic of Cooling/Dehumidifying Coil
-
-#### Heat Transfer and Energy Balance
-
-The cooling coil may be completely dry, completely wet with condensation, or it may have wet and dry sections.  The actual condition of the coil surface depends on the humidity and temperature of the air passing over the coil and the coil surface temperature.  The part-dry part-wet case represents the most general scenario for the coil surface conditions.  There are subroutines present in the model for both the dry and wet regions of the coil, and a subroutine that iterates between the dry and wet subroutines to calculate the fraction of the coil surface that is wet.  For each region the heat transfer rate from air to water may be defined by the rate of enthalpy change in the air and in the water.  The rates must balance between each medium for energy to be conserved.
-
-#### Model Description
-
-The Model has two blocks: 1<sup>st</sup> = Design Block with the Design Inputs. This block calculates the Design U-Factor Times Area Value (UA) values required by the model. Using these UA values the model simulates the operating conditions.  The operating block is the one containing the operating conditions, the conditions at which the coil operates. Following is the list of Design and Operating inputs and subsequently the Design and Operating variables used in the model.
-
-Table 52.  Design Inputs (User Inputs)
-
-<table class="table table-striped">
-<tr>
-<th>Input Field</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>DesWaterVolFlowRate:</td>
-<td>Maximum Water Volume Flow Rate</td>
-</tr>
-<tr>
-<td>DesAirVolFlowRate:</td>
-<td>Maximum Air Volume Flow Rate</td>
-</tr>
-<tr>
-<td>DesInletWaterTemp:</td>
-<td>Inlet Water Temperature at Design Condition</td>
-</tr>
-<tr>
-<td>DesInletAirTemp:</td>
-<td>Inlet Air Temperature at Design Condition</td>
-</tr>
-<tr>
-<td>DesOutletAirTemp:</td>
-<td>Outlet Air Temperature at Design Condition</td>
-</tr>
-<tr>
-<td>DesInletAirHumRat:</td>
-<td>Inlet Air Humidity Ratio at Design Conditions</td>
-</tr>
-<tr>
-<td>DesOutletAirHumRat:</td>
-<td>Outlet Air Humidity Ratio at Design Conditions.</td>
-</tr>
-
-</table>
-
-
-
-Table 53.  Operating Conditions (From Nodes -- not user inputs)
-
-<table class="table table-striped">
-<tr>
-<th>Condition Variable</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>InletWaterMassFlowRate:</td>
-<td>Entering Water Mass Flow Rate at operating condition</td>
-</tr>
-<tr>
-<td>InletWaterTemp:</td>
-<td>Inlet Water Temperature at operating condition</td>
-</tr>
-<tr>
-<td>InletAirMassFlowRate:</td>
-<td>Entering Air Mass Flow Rate at operating condition</td>
-</tr>
-<tr>
-<td>InletAirTemp:</td>
-<td>Inlet Air Temperature at operating condition</td>
-</tr>
-<tr>
-<td>InletAirHumRat:</td>
-<td>Entering air humidity ratio at operating conditions</td>
-</tr>
-
-</table>
-
-
-
-#### Intermediate calculated U-Factor Times Area Values: The Crux of the Model
-
-The various U-Factor Times Area values (UA) required by this model are calculated from the above inputs, which are explained later in the document.  The various UA are:
-
-Table 54.  UA Descriptions of Model
-
-<table class="table table-striped">
-<tr>
-<th>UA Variable Name</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>CoilUATotal:</td>
-<td>Overall heat transfer coefficient (W/C)</td>
-</tr>
-<tr>
-<td>CoilUAInternal:</td>
-<td>Overall internal UA (W/C)</td>
-</tr>
-<tr>
-<td>CoilUAExternal:</td>
-<td>Overall external UA (W/C)</td>
-</tr>
-<tr>
-<td>CoilUInternal:</td>
-<td>Internal overall heat transfer coefficient (W/m<sup>2</sup>∙C)</td>
-</tr>
-<tr>
-<td>CoilUWetExternal:</td>
-<td>Wet part external overall heat transfer coefficient (W/m<sup>2</sup>∙C)</td>
-</tr>
-<tr>
-<td>CoilUDryExternal:</td>
-<td>Dry part external overall heat transfer coefficient (W/m<sup>2</sup>∙C)</td>
-</tr>
-
-</table>
-
-The UA values are calculated assuming a wet coil at the design conditions. Following are a few important calculations to understand the working of the model.  The model is basically divided into two blocks: the Design Block and the Operating Block.
-
-The Design Block is a one time calculation. The aim of the Design Block is to calculate the Coil UA for use in the operating Block.
-
-#### Design Block Calculations:
-
-The design block has the code for calculating the six Coil UA values required by the operating block. Reasonable assumptions have been made in the calculations to maintain the simplicity of the model.
-
-Heat transfer in a wet coil model is based on enthalpy rather than temperature to take into account latent effects. While heat transfer rates are commonly expressed as the product of an overall heat transfer coefficient, UA, and a temperature difference, the use of enthalpy-based heat transfer calculations requires an enthalpy-based heat transfer coefficient which we denote as DesUACoilTotalEnth and hence the equation.
-
-Q = DesUACoilTotalEnth \* (H<sub>air,mean</sub> - H<sub>water,mean</sub>). The value of Q is calculated using product of air mass flow rate and difference in inlet and outlet air enthalpies at design conditions.
-
-The relation between the enthalpy-based UA and the temperature-based UA is DesUACoilTotalEnth = CoilUA / C<sub>p</sub>. CoilUA is the conventional heat transfer coefficient and C<sub>p</sub> = specific heat of the air.
-
-We need the following quantities for our design calculations. The *Psy* functions are the EnergyPlus built-in psychrometric functions.
-
-<div>$${\dot m_{air}} = {\rho_{air}}{\dot V_{air}}$$</div>
-
-<div>$${h_{air,in}} = {\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{air,in}},{w_{air,in}})$$</div>
-
-<div>$${h_{air,out}} = {\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{air,out}},wout)$$</div>
-
-<div>$${h_{w,sat,in}} = {\rm{PsyHFnTdbW}}({T_{w,in}},{\rm{PsyWFnTdpPb}}({T_{w,in}},{P_{atm}}))$$</div>
-
-<div>$${\dot Q_{coil}} = {\dot m_{air}}({h_{air,in}} - {h_{air,out}})$$</div>
-
-<div>$${T_{w,out}} = {T_{w,in}} + {\dot Q_{coil}}/({\dot m_{w,\max }}{C_{p,w}})$$</div>
-
-<div>$${h_{w,sat,out}} = {\rm{PsyHFnTdbW}}({T_{w,out}},{\rm{PsyWFnTdpPb}}({T_{w,out}},{P_{atm}}))$$</div>
-
-We now calculate the design coil bypass factor. The bypass factor is not used in subsequent calculations. It is calculated solely to use as check on the reasonableness of the user-input design inlet and outlet conditions. First we make an initial estimate of the apparatus dew point temperature:
-
-<div>$${T_{air,dp,app}} = {\rm{PsyTdpFnWPb}}({w_{air,out}},{P_{atm}})$$</div>
-
-we also need the "slope" of temperature versus humidity ratio on the psych chart between the inlet and outlet air conditions:
-
-<div>$${S_{T,w}} = ({T_{air,in}} - {T_{air,out}})/({w_{air,in}} - {w_{air,out}})$$</div>
-
-We now obtain the actual design apparatus dewpoint temperature by iterating over the following two equations:
-
-<div>$${w_{air,dp,app}} = {\rm{PsyWFnTdpPb}}({T_{air,dp,app}},{P_{atm}})$$</div>
-
-<div>$${T_{air,dp,app}} = {T_{air,in}} - {S_{T,w}}({w_{air,in}} - {w_{air,dp,app}})$$</div>
-
-The apparatus dewpoint enthalpy is then:
-
-<div>$${h_{air,dp,app}} = {\rm{PsyHFnTdbW}}({T_{air,dp,app}},{w_{air,dp,app}})$$</div>
-
-and the coil bypass factor is:
-
-<div>$${F_{coilbypass}} = ({h_{air,out}} - {h_{air,dp,app}})/({h_{air,in}} - {h_{air,dp,app}})$$</div>
-
-If the iterative procedure doesn't converge, or the coil bypass factor is too large (greater than 0.5), or the apparatus dewpoint enthalpy is less than the saturated air enthalpy at the water inlet temperature, the design outlet air conditions are reset to 90% relative humidity at the same outlet enthalpy. The above design calculations are then repeated.
-
-We are now ready to calculate the design coil UA. This will be accomplished by inverting the simple coil calculation routine *CoolingCoil* using the Regula Falsi method. First we make an initial estimate of the coil UA.
-
-<div>$$\Delta {h_{lmd}} = (({h_{air,in}} - {h_{w,sat,out}}) - ({h_{air,out}} - {h_{w,sat,in}}))/log(({h_{air,in}} - {h_{w,sat,out}}) - ({h_{air,out}} - {h_{w,sat,in}}))$$</div>
-
-<div>$$U{A_{coil,enthalpy - based}} = {\dot Q_{coil}}/\Delta {h_{lmd}}$$</div>
-
-<div>$$U{A_{coil,ext}} = {C_{p,air}}U{A_{coil,enthalpy - based}}$$</div>
-
-We set the internal UA to 3.3 times the external UA (as a typical value for a coil). Then the total UA is:
-
-<div>$$U{A_{coil,tot}} = \frac{1}{{(1/U{A_{coil,int}} + 1/U{A_{coil,ext}})}}$$</div>
-
-The next step is to estimate the coil external heat transfer surface area. This is done in the function *EstimateHEXSurfaceArea*:
-
-<div>$$Are{a_{coil,ext}} = {\rm{EstimateHEXSurfaceArea}}$$</div>
-
-using the following assumptions:
-
-* Tube inside diameter = 0.0122 (m)
-
-* Tube side water velocity = 2.0 (m/s)
-
-* Inside to outside coil surface area ratio (Ai/Ao) = 0.07 (-)
-
-* Fins overall efficiency = 0.92 (-)
-
-* Aluminum fins, 12 fins per inch with fins to total outside surface area ratio of 90%.
-
-* Airside combined heat and mass transfer coefficient = 140 (W/m2∙°C)
-
-Interior and exterior U values (really UA's per unit exterior surface area) are calculated by dividing the above UA's by the area. The resulting U<sub>coil,ext</sub> is assumed to be U<sub>coil,ext,wet</sub>; U<sub>coil,ext,dry</sub> is set equal to U<sub>coil,ext,wet</sub>. We now have all the starting values needed for inverting the simple coil model using the chosen Regula Falsi iterative method. Once the iteration is completed, we have coil UA's and U's that yield the design outlet air and water enthalpies given the inlet design conditions and flow rates. Note that the simple coil model can not exactly match the specified design outlet air temperature and humidity ratio. It can only match the design air outlet enthalpy. Generally the simple coil model will yield outlet conditions near the saturation curve if any dehumidification is occuring. Typical outlet relative humidities are around 95%.
-
-#### Variable UA
-
-The above calculations yield coil UA's for the design inlet conditions and air and water flow rates. As the flow rates vary during the time step calculations, the UA's need to be adjusted, since coil UA's are a rather strong function of air and water side flow rates. Each time step the coil UA's are modified using the same formulas as are used in the hot water coil model. Refer to that model for the flow dependences.
-
-#### Operating Block Calculations:
-
-There are two modes of coil analysis in the operating block. They are the Simple analysis mode and the detailed analysis mode. The simple analysis mode assumes the coil to be either all wet or either all dry and execute the model , on the other hand the detailed mode checks for part wet part dry mode of operation and reports surface area wet fraction of coil, however the program execution time in detailed mode is noticeably higher.
-
-The operating block for Detailed Mode Analysis of this coil model is divided into three modes of coil performance. The modes being
-
-n Coil is completely dry: There is no moisture condensation on the coil surface and the coil is a dry coil. This is an extreme condition when the entering air has very low humidity ratio or is dry air.
-
-n Coil is completely wet: The entire coil is wet due to complete condensation on the surface of the coil.
-
-n Part Wet Part Dry Mode: This is the usual/frequent mode of operation of coil, as shown in figure 1, where part of the coil at entry of air is dry and as air cools condensation occurs and part of the coil becomes wet.
-
-The Part Wet Part Dry Mode of operation is essentially a function the Coil Completely Dry and Coil Completely Wet mode. This subroutine iterates between the Dry Coil and the Wet Coil to give outputs, a detailed explanation is given later in the document. The operating block requires 5 inputs, which are mentioned earlier in the document. These inputs are automatically generated from the node connections in Energy Plus. The user does not have to input any information to run this coil model.
-
-The option to identify which mode of operation the coil should perform ie, for a given set of inputs would the coil be Dry, Wet or Part Wet Part Dry, is decided by set of conditions described below.
-
-n **IF** (**Temperature Dewpoint Air &lt; Water Inlet Temperature**) **THEN** the coil is Dry and we call the Subroutine Coil Completely Dry.  In this case outlet temperature of air would be higher than the air dewpoint and hence there would be no condensation.
-
-n **IF** (**Temperature Dewpoint Air &gt; Water Inlet Temperature**) **THEN** the coil is completely wet, call subroutine Coil Completely Wet, it is assumed that moisture condensation occurs over completely surface of the coil. However we go ahead and check for the coil being partially wet with the following condition.
-
-n **IF (AirDewPointTemp &lt; AirInletCoilSurfTemp) THEN,** the coil is Partially Wet because there is possibility that air temperature will go below its dewpoint and moisture will condense on latter part of the cooling coil.
-
-The Operating Block for Simple Mode Analysis is divided into two modes of coil performance, the two modes being
-
-n Coil is completely dry: There is no moisture condensation on the coil surface and the coil is a dry coil.
-
-n Coil is completely wet: The entire coil is wet due to complete condensation on the surface of the coil.
-
-The option to identify which mode of operation the Simple mode analysis should perform ie, for a given set of inputs would the coil be Dry or Wet is decided by set of conditions described below.
-
-n **IF** (**Temperature Dewpoint Air &lt; Water Inlet Temperature**) **THEN** the coil is Dry and we call the Subroutine Coil Completely Dry.  In this case outlet temperature of air would be higher than the air dewpoint and hence there would be no condensation.
-
-n **IF** (**Temperature Dewpoint Air &gt; Water Inlet Temperature**) **THEN** the coil is completely wet, call subroutine Coil Completely Wet, it is assumed that moisture condensation occurs over completely surface of the coil. However we go ahead and check for the coil being partially wet with the following condition.
-
-The above is a simple mode of analysis and the results are very slightly different from the detailed mode of analysis. The algorithms used in Simple mode and the Detailed mode are identically similar. The surface area wet fraction in the coil is reported as 1.0 or 0.0 for wet or dry coil respectively. The program defaults to simple mode of analysis for enabling higher execution speed.
-
-#### Effectiveness Equations:
-
-There are two modes of flow for the coil, Counter Flow mode or the Cross Flow mode, default set up is as cross flow since most air condition applications have cross flow heat exchangers. According to the mode of flow the following NTU - Effectiveness relationships are used to calculate coil effectiveness, which is used later by all the three modes (Dry, Wet, Part Wet) for calculating air outlet conditions and heat transfer.
-
-Following are the relations used for calculating effectiveness equation for the Heat exchangers.
-
-Counter Flow Heat Exchanger: Effectiveness Equation:
-
-<div>$${\eta_{CounterFlow}} = \frac{{(1 - Exp( - NTU \times (1 - Rati{o_{StreamCapacity}})))}}{{1 - Rati{o_{StreamCapacity}} \times Exp( - NTU \times (1 - Rati{o_{StreamCapacity}}))}}$$</div>
-
-In Equation   the variable Ratio\_StreamCapacity is defined as below
-
-<div>$$Rati{o_{StreamCapacity}} = \frac{{MinCapacit{y_{Stream}}}}{{MaxCapacit{y_{Stream}}}}$$</div>
-
-In equation capacity of stream is defined as below in equation
-
-<div>$$(Min,Max)\,\,Capacit{y_{Stream}} = {(MassFlowRate \times Cp)_{air,water}}$$</div>
-
-NTU in equation , is defined as the Number of Transfer Units, it is a function of Coil UA and the Minimum Capacity of Stream. The Coil UA is a variable in this equation and depends on which mode of the coil operation (Dry, Wet, Part Wet) is calling upon equation , i.e., if it is Coil Completely Dry calling upon the effectiveness equation with the value of Dry UA total, which in our case is defined as CoilUA\_total. Equation gives definition for NTU.
-
-<div>$$NTU = \frac{{CoilUA}}{{MinStrea{m_{Capacity}}}}$$</div>
-
-Cross Flow Heat Exchanger: Effectiveness Equation:
-
-<div>$${\eta_{CrossFlow}} = 1 - EXP\left\{ {\frac{{Exp( - NTU \times Rati{o_{StreamCapacity}} \times NT{U^{ - 0.22}}) - 1}}{{Rati{o_{StreamCapacity}} \times NT{U^{ - 0.22}}}}} \right\}$$</div>
-
-The variables in the above equation have already been defined earlier. Depending on the mode of operation of the coil model the cross or the counter flow equations are used to calculate the effectiveness.
-
-#### Coil Outlet Conditions:
-
-Calculating the Outlet Stream Conditions using the effectiveness value from equation   or depending on the mode of flow. The energy difference between the outlet and inlet stream conditions gives the amount of heat transfer that has actually take place. Temperature of air and water at outlet to the coil is given as in following equations
-
-<div>$$TempAi{r_{Out}} = TempAi{r_{inlet}} - {\eta_{cross,counter}} \times \frac{{MaxHeatTransfer}}{{StreamCapacit{y_{Air}}}}$$</div>
-
-<div>$$TempWate{r_{Out}} = TempWate{r_{Inlet}} + {\eta_{Cross,counter}} \times \frac{{MaxHeatTransfer}}{{StreamCapacit{y_{Water}}}}$$</div>
-
-In the above equations and the maximum heat transfer is calculated as shown in the following equation
-
-<div>$$MaxHeatTransfer = MinStrea{m_{Capacity}} \times (TempAi{r_{Inlet}} - TempWate{r_{Inlet}})$$</div>
-
-#### Coil Completely Dry Calculations: (operating block)
-
-Since the coil is dry, the sensible load is equal to total load and the same with the humidity ratios at inlet and outlet, as in equations and .
-
-<div>$$QSensibl{e_{DryCoil}} = QTota{l_{DryCoil}}$$</div>
-
-<div>$$HumRati{o_{Inlet}} = HumRati{o_{Outlet}}$$</div>
-
-Total Heat Transfer in dry coil is as follows:
-
-<div>$${Q_{TotalDryCoil}} = CapacityAir \times (AirTem{p_{In}} - AirTem{p_{Outlet}})$$</div>
-
-The variables in the above equation are calculated earlier in equations and to give the total cooling load on the coil.
-
-#### Coil Completely Wet Calculations: (operating block)
-
-In wet coil we need to account for latent heat transfer, hence calculations are done using enthalpy of air and water instead of stream temperatures Hence we need to define coil UA for the wet coil based on enthalpy of the operating streams and not design streams.
-
-Similar to equations and we calculate the air outlet enthalpy and water outlet enthalpy ie by replacing temperature with enthalpy of the respective streams. The input variable for Coil UA in equation for calculating NTU, in this case it would be enthalpy based and is given as shown in equation
-
-<div>$$CoilU{A_{\,Enthalpy\,Based}} = \frac{1}{{\left( {\frac{{CpSa{t_{Intermediate}}}}{{CoilU{A_{\,Internal}}}} + \frac{{C{p_{Air}}}}{{CoilU{A_{\,External}}}}} \right)}}$$</div>
-
-Total Coil Load in case of Wet Coil is the product of mass flow rate of air and enthalpy difference between the inlet and outlet streams as given in the following equation
-
-<div>$${Q_{Total}} = {\mathop M\limits^ *_{air}} \times (EnthAi{r_{Inlet}} - EnthAi{r_{Outlet}})$$</div>
-
-Once the enthalpy is known the outlet temperatures and outlet humidity ratios of the wet coil are calculated as in equations below.
-
-**IF (TempCondensation &lt; PsyTdpFnWPb(InletAirHumRat ,Patm)) THEN**
-
-<div>$$AirTem{p_{Out}} = AirTem{p_{inlet}} - (AirTem{p_{inlet}} - Condensatio{n_{Temp}}) \times \eta $$</div>
-
-and
-
-**OutletAirHumdityRatio = PsyWFnTdbH(OutletAirTemp,EnthAirOutlet)**
-
-**ELSE**
-
-There is no condensation and hence the inlet and outlet Hum Ratios are equal , and outlet temperature is a function of outlet air enthalpy as below
-
-**OutletAirTemp      =  PsyTdbFnHW (EnthalpyAirOutlet, OutletAirHumRat)**
-
-**and**
-
-**OutletAirHumRat  =  InletAirHumRat**
-
-**ENDIF**
-
-Effectiveness η used in equation is defined in equation and Condensation Temperature is calculated using psychrometric function as in equation .
-
-<div>$$\eta  = 1 - Exp\left\{ { - \frac{{CoilU{A_{\,External}}}}{{Capacitanc{e_{Air}}}}} \right\}$$</div>
-
-<span>\(Condensatio{n_{Temp}} = {\rm{PsyTsatFnHPb(Ent}}{{\rm{h}}_{{\rm{AirCondensateTemp}}}}{\rm{,Patm) }}\)</span>                <span>\(Ent{h_{\,AirCondensateTemp}} = Ent{h_{\,AirInlet}} - \frac{{\left( {Ent{h_{\,AirInlet}} - Ent{h_{\,AirOutlet}}} \right)}}{\eta }\)</span>
-
-Once the air outlet temperature are known, then sensible load is calculated as a product of capacitance of air and temperature difference at inlet and outlet, as in equation
-
-<div>$${Q_{Sensible}} = Capacitanc{e_{Air}} \times \left( {AirTem{p_{Inlet}} - AirTem{p_{Outlet}}} \right)$$</div>
-
-#### Coil Part Wet Part Dry Calculations: (operating block)
-
-The Coil would perform under part wet part dry conditions when Air Dewpoint Temperature is less than Coil surface temperature at inlet to air. In this case part of the coil used value of Dry UA for heat transfer and part the coil used Wet UA value for heat transfer.
-
-This problem is solved utilizing the fact that the Exit conditions from the Dry Part of the Coil would become the inlet conditions to the wet part of the coil (see Figure 162) and the coil model determines by iteration what fraction of the coil is wet and based on that it calculates the areas and subsequently the UA values of that dry and wet part, based on the area of the dry and wet part respectively. Explained below are the steps followed to the estimating the wet dry behavior of the coil.
-
-n Iterate between the Dry Coil and the Wet Coil. First calculate Coil Completely Dry performance by estimating the wet dry interface water temperature using equation and inputting this variable as the water inlet temperature to dry Coil.
-
-<span>\(WetDryInterfac{e_{WaterTemp}} = {\rm{WaterTem}}{{\rm{p}}_{{\rm{Inlet}}}}{\rm{ + Are}}{{\rm{a}}_{{\rm{WetFraction}}}}{\rm{*(WaterTem}}{{\rm{p}}_{{\rm{Outlet}}}}{\rm{ - WaterTem}}{{\rm{p}}_{{\rm{Inlet}}}}{\rm{)}}\)</span>    
-
-The value of Surface Area Wet fraction is estimated initially as follows
-
-<div>$$Are{a_{\,WetFractionEstimate}} = \frac{{AirDewP{t_{\,Temp}} - InletWate{r_{\,Temp}}}}{{OutletWate{r_{\,Temp}} - InletWate{r_{\,Temp}}}}$$</div>
-
-For the above mentioned iteration the value of Coil UA for Wet and Dry part need to be varied according to the new respective area of the wet and dry parts. This estimate of Wet and Dry area is a product of the estimated Surface Area Fraction and total coil external area, which keeps varying as will be explained further in the document.
-
-UA value for Dry part of the Coil is estimated as below.
-
-<div>$$CoilU{A_{Dry\,External}} = \frac{{SurfAre{a_{Dry}}}}{{\frac{1}{{Coil{U_{Dry\,External}}}} + \frac{1}{{Coil{U_{Internal}}}}}}$$</div>
-
-Where Surface Area Dry =(Total Coil Area – Wet Part Area), where the Wet part area is the product of Surface fraction Wet and Total Coil Area.
-
-UA value for the Wet part of the Coil requires Wet UA external and Wet UA Internal, which are calculated as below.
-
-<div>$$WetPartUA{\,_{External}} = Coil{U_{Wet\,External}} \times SurfaceAreaWet$$</div>
-
-<div>$$WetPartUA{\,_{Internal}} = Coil{U_{Internal}} \times SurfaceAreaWet$$</div>
-
-It is essential to remember that the mode of calculation for the coils remains the same as in completely wet and completely dry mode, only the UA values and water, air outlet and inlet values change.
-
-Now Iterate between the Dry Coil and wet Coil with the above respective UA, and usual operating inputs except the variable water inlet temperature for dry Coil is replaced with Wet Dry Interface Water temperature, and in the Wet Coil the Outlet Air Temperature from dry Coil is the inlet air temperature to Wet Coil. The iteration proceeds till the Outlet Water Temperature from Wet Coil equals the Wet Dry Interface Water Temp, which is the input to Dry Coil.
-
-Dry Part Inputs: (changed operating inputs) :Iteration Case 1: Explained In Programming Fashion:
-
-**CALL CoilCompletelyDry (WetDryInterfcWaterTemp, InletAirTemp, DryCoilUA,               &**
-
-**                             OutletWaterTemp, WetDryInterfcAirTemp, WetDryInterfcHumRat,        &**
-
-**DryCoilHeatTranfer).**
-
-Input the calculated values calculated by Dry Coil above into Wet Coil below. The variables have been highlighted in color red and blue.
-
-**CALL**CoilCompletelyWet (InletWaterTemp, **WetDryInterfcAirTemp**, **WetDryInterfcHumRat**
-
-WetPartUAInternal,WetPartUAExternal,                                                  &
-
-**EstimateWetDryInterfcWaterTemp**, OutletAirTemp, OutletAirHumRat,    &
-
-WetCoilTotalHeatTransfer, WetCoilSensibleHeatTransfer,                       &
-
-EstimateSurfAreaWetFraction, WetDryInterfcSurfTemp)
-
-Iterate Between the above two Wet and Dry Coil calls until the two variables in blue ie **WetDryInterfcWaterTemp = EstimateWetDryInterfcWaterTemp.**The key is to have the difference between the variables (WetDryInterfcWaterTemp – OutletWaterTemp) in Dry Coil equal to (InletWaterTemp-EstimatedWetDryInterfcWaterTemp) in Wet Coil. This equality quantized the relative part of coil that is dry and part that is wet on the basis of heat transfer that has occurred.
-
-After the above convergence check for the coil being dry otherwise iterate to calculate surface fraction area wet.
-
-**IF**
-
-<div>$$\left\{ {(AreaFractio{n_{Wet}} \le \,0.0)\,\,and(WetDryInterfac{e_{SurfTemp}} > AirDewPt)} \right\}$$</div>
-
-**THEN CoilCompletelyDry**
-
-If equation is satisfied then Coil is Dry and simply output the value for Dry Coil calculated else the coil is partially wet and then iterate to find the surface fraction area wet. Start with the initially guess value of surface area fraction (equation wet and iterate on the entire loop starting from until the Wet Dry Interface Temperature equals the Air Dewpoint Temperature. The value of Surface Area fraction wet at which the interface air temperature equals is dewpoint is the transition point from wet to dry and gives the % of coil that is dry and % that is wet.
-
-Graphs Showing the Performance of the coil model at optimum operating conditions are shown below. All values of variable used have been normalized.
-
-![](media/image3348.png)
-
-Figure 163.  Air Outlet Temperature Vs Air Mass Flow Rate
-
-
-
-![](media/image3349.png)
-
-Figure 164.  Sensible Load variations Vs Air mass Flow Rate
-
-
-
-![](media/image3350.png)
-
-Figure 165.  Total and Sensible Load variations Vs Air Mass Flow Rate
-
-
-
-![](media/image3351.png)
-
-Figure 166.  Surface Area Fraction Wet Vs Air Mass Flow Rate
-
-#### References
-
-IBPSA BuildSim-2004. 2004. Colarado Boulder: An Improvement of Ashrae Secondary HVAC toolkit Simple Cooling Coil Model for Building Simulation, Rahul J Chillar, Richard J Liesen M&IE ,UIUC.
-
-Stoecker, W.F. &lt;dates unspecified&gt; Design of Thermal Systems,: ME 423 Class Notes , M& IE Dept UIUC.
-
-Brandemeuhl, M. J. 1993. HVAC2 Toolkit: Algorithms and Subroutines for Secondary HVAC Systems Energy Calculations, ASHRAE.
-
-Elmahdy, A.H. and Mitalas, G.P.  1977. "A Simple Model for Cooling and Dehumidifying Coils for Use In Calculating Energy Requirements for Buildings ASHRAE Transactions, Vol.83 Part 2, pp. 103-117.
-
-Threlkeld, J.L.  1970.  Thermal Environmental Engineering, 2nd Edition, Englewood Cliffs: Prentice-Hall,Inc. pp. 254-270.
-
-ASHRAE Secondary HVAC Toolkit TRNSYS.  1990.  A Transient System Simulation Program: Reference Manual. Solar Energy Laboratory, Univ. Wisconsin-Madison, pp. 4.6.8-1 - 4.6.8-12.
-
-Kays, W.M. and A.L. London. 1964. Compact Heat Exchangers, 2nd Edition, New York: McGraw-Hill.
-
-Clark, D.R.. 1985. HVACSIM+ Building Systems and Equipment Simulation Program Reference Manual, Pub. No. NBSIR 84-2996, National Bureau of Standards, U.S. Department of Commerce, January, 1985
-
-Elmahdy, A.H. 1975. Analytical and Experimental Multi-Row Finned-Tube Heat Exchanger Performance During Cooling and Dehumidifying Processes, Ph.D. Thesis, Carleton University, Ottawa, Canada, December, 1975.
-
-Elmahdy, A.H., and Mitalas, G.P. 1977. "A Simple Model for Cooling and Dehumidifying Coils for Use in Calculating Energy Requirements for Buildings," ASHRAE Transactions, Vol.  83, Part 2, pp. 103-117.
-
-### Chilled-Water-Based Detailed Geometry Air Cooling Coil
-
-The input object Coil:Cooling:Water:DetailedGeometry provides a coil model that predicts changes in air and water flow variables across the coil based on the coil geometry. A greatly simplified schematic of enthalpy and temperature conditions in a counterflow cooling/dehumidifying coil is shown in the following schematic figure. In addition, the variables required to model a cooling/dehumidifying coils and their definitions are extensively listed in “Table 55. Coil Geometry and Flow Variables for Coils�. The input required to model the coil includes a complete geometric description that, in most cases, should be derivable from specific manufacturer's data.  The coil simulation model is essentially the one presented by Elmahdy and Mitalas (1977) and implemented in HVACSIM+ (Clark 1985), a modular program also designed for energy analysis of building systems. The model solves the equations for the dry and wet sections of the coil using log mean temperature and log mean enthalpy differences between the liquid and the air streams.  Elmahdy and Mitalas state that crossflow counterflow coils with at four rows or more are approximated well by this model.  This does not constitute a major limitation since cooling and dehumidifying coils typically have more than four rows.
-
-![](media/image3352.svg.png)
-
-Figure 167.  Simplified Schematic of Cooling/Dehumidifying Coil
-
-#### Heat Transfer and Energy Balance
-
-The cooling coil may be completely dry, completely wet with condensation, or it may have wet and dry sections.  The actual condition of the coil surface depends on the humidity and temperature of the air passing over the coil and the coil surface temperature.  The partly wet-partly dry case represents the most general scenario for the coil surface conditions.  The all dry and all wet cases can be considered as limiting solutions of the wet or dry areas respectively going to zero.  In the general case, equations are written for both the dry and wet regions of the coil.  For each region the heat transfer rate from air to water may be defined by the rate of enthalpy change in the air and in the water.  The rates must balance between each medium for energy to be conserved.  Equations through express the energy balance between the water and the air for the case of dry and wet coils respectively.  Equations and represent the heat transfer rate between water and air based on the actual performance of the coil.  The UA parameter can be calculated from the parameters in the following table.
-
-
-
-
-
-Table 55. Coil Geometry and Flow Variables for Coils
-
-<table class="table table-striped">
-<tr>
-<th>A</th>
-<th>area</th>
-<th>LMHD</th>
-<th>log mean enthalpy difference</th>
-</tr>
-<tr>
-<td>A</td>
-<td>air, air side</td>
-<td>LMTD</td>
-<td>log mean temperature difference</td>
-</tr>
-<tr>
-<td>aa, bb</td>
-<td>coeff. in enthalpy approximation</td>
-<td><span>\(\dot m\)</span></td>
-<td>mass flow rate</td>
-</tr>
-<tr>
-<td>C1, C2</td>
-<td>coeff. in air side film coeff.</td>
-<td>mf</td>
-<td>metal and fouling</td>
-</tr>
-<tr>
-<td>Cp</td>
-<td>specific heat</td>
-<td>m</td>
-<td>viscosity</td>
-</tr>
-<tr>
-<td>D</td>
-<td>diameter, effective diameter</td>
-<td>o</td>
-<td>outside (air side)</td>
-</tr>
-<tr>
-<td>Dhdr</td>
-<td>hydraulic diameter on air side</td>
-<td>Pr</td>
-<td>Prandtl number</td>
-</tr>
-<tr>
-<td>D</td>
-<td>dry region</td>
-<td><span>\(\dot Q\)</span></td>
-<td>heat transfer rate</td>
-</tr>
-<tr>
-<td>d</td>
-<td>thickness</td>
-<td>R</td>
-<td>overall thermal resistance</td>
-</tr>
-<tr>
-<td>D</td>
-<td>spacing</td>
-<td>Re</td>
-<td>Reynolds number</td>
-</tr>
-<tr>
-<td>F</td>
-<td>heat transfer film coefficient</td>
-<td>r</td>
-<td>ratio of diameters</td>
-</tr>
-<tr>
-<td>Fai</td>
-<td>variable in fin eff. calculation</td>
-<td>s</td>
-<td>surface, outside of metal</td>
-</tr>
-<tr>
-<td>fin, fins</td>
-<td>air side fin geometry</td>
-<td>St</td>
-<td>Stanton number</td>
-</tr>
-<tr>
-<td>H</td>
-<td>enthalpy</td>
-<td>T</td>
-<td>temperature</td>
-</tr>
-<tr>
-<td>h</td>
-<td>efficiency</td>
-<td>tube</td>
-<td>water tube</td>
-</tr>
-<tr>
-<td>I0()</td>
-<td>mod Bessel fn, 1st kind, ord 0</td>
-<td>UAdry</td>
-<td>dry heat xfer coeff. * dry area</td>
-</tr>
-<tr>
-<td>I1()</td>
-<td>mod Bessel fn, 1st kind, ord 1</td>
-<td>UcAw</td>
-<td>wet heat xfer coeff. * wet area</td>
-</tr>
-<tr>
-<td>K0()</td>
-<td>mod Bessel fn, 2nd kind, ord 0</td>
-<td>ub, ue</td>
-<td>variables in fin eff. calculation</td>
-</tr>
-<tr>
-<td>K1()</td>
-<td>mod Bessel fn, 2nd kind, ord 1</td>
-<td>V</td>
-<td>average velocity</td>
-</tr>
-<tr>
-<td>I</td>
-<td>inside (water side)</td>
-<td>w</td>
-<td>water, water side, or wet region</td>
-</tr>
-<tr>
-<td>K1</td>
-<td>variable in sol'n form of eq.</td>
-<td>wa</td>
-<td>humidity ratio</td>
-</tr>
-<tr>
-<td>K</td>
-<td>thermal conductivity</td>
-<td>Z</td>
-<td>variables in sol'n form of eq.</td>
-</tr>
-<tr>
-<td>L</td>
-<td>length</td>
-<td>1, 2, 3</td>
-<td>positions (see diagram)</td>
-</tr>
-
-</table>
-
-Equations through represent two sets of three equations with 7 unknowns: <span>\({\dot Q_d}\)</span>, Ta,1, Ta,2, Tw,2, Tw,3, <span>\({\dot m_a}\)</span>, <span>\({\dot m_w}\)</span>. However, normally at least four of these variables are specified, for example: inlet water temperature, outlet air temperature, water flow rate, air flow rate, so that the system of equations is effectively closed.
-
-<div>$${\dot Q_d} = {m_a}C{p_a}\left( {{T_{a,1}} - {T_{a,2}}} \right)$$</div>
-
-<div>$${\dot Q_d} = {m_w}C{p_w}\left( {{T_{w,3}} - {T_{w,2}}} \right)$$</div>
-
-<div>$${\dot Q_d} = \left( {U{A_{dry}}} \right)\left( {LMTD} \right)$$</div>
-
-<div>$${\dot Q_w} = {m_a}\left( {{H_{a,2}} - {H_{a,3}}} \right)$$</div>
-
-<div>$${\dot Q_w} = {m_w}C{p_w}\left( {{T_{w,2}} - {T_{w,1}}} \right)$$</div>
-
-<div>$${\dot Q_w} = \left( {{U_c}{A_w}} \right)\left( {LMHD} \right)$$</div>
-
-In order to manipulate these equations, the log mean temperature and enthalpy differences are expanded as shown in Equations and .  Finally, a linear approximation of the enthalpy of saturated air over the range of surface temperature is made using Equation .  Note that in Equation Hw refers to the enthalpy of saturated air at the water temperature.
-
-<div>$$LMTD = \frac{{\left( {{T_{a,1}} - {T_{w,3}}} \right) - \left( {{T_{a,2}} - {T_{w,2}}} \right)}}{{\ln \frac{{{T_{a,1}} - {T_{w,3}}}}{{{T_{a,2}} - {T_{w,2}}}}}}$$</div>
-
-<div>$$LMHD = \frac{{\left( {{H_{a,2}} - {H_{w,2}}} \right) - \left( {{H_{a,3}} - {H_{w,1}}} \right)}}{{\ln \frac{{{H_{a,2}} - {H_{w,2}}}}{{{H_{a,3}} - {H_{w,1}}}}}}$$</div>
-
-<div>$${H_w} = aa + bb {T_w}$$</div>
-
-Equation is derived from the above equations and is used to solve for the coil conditions when all of the inlet conditions are given as input.  Operating in this manner, the coil does not have a controlled outlet air temperature.
-
-<div>$${T_{w,2}} = \frac{{\left( {1 - Z} \right)\left( {{H_{a,1}} - aa - K1 C{p_a} {T_{a,1}}} \right) + Z {T_{w,1}}\left( {bb - \frac{{{m_w}C{p_w}}}{{{m_a}}}} \right)}}{{bb - Z\frac{{{m_w}C{p_w}}}{{{m_a}}} - \left( {1 - Z} \right) K1 C{p_a}}}$$</div>
-
-An alternative solution method is to define the coil leaving air temperature as an input with a variable water flow rate.  In this case Equations and are more convenient.  Equations through define terms that are used to simplify Equations , and .
-
-<div>$${T_{w,2}} = \frac{{\left( {1 - Z} \right)\left( {{H_{a,3}} - aa} \right) + {T_{w,1}}\left( {\frac{{{m_w}C{p_w}}}{{{m_a}}} - bb Z} \right)}}{{\frac{{{m_w}C{p_w}}}{{{m_a}}} - bb}}$$</div>
-
-<div>$${T_{w,2}} = \frac{{\left( {{Z_d} - 1} \right){T_{a1}}C{p_a} + {T_{w,3}}\left( {C{p_a} - {Z_d}\frac{{{m_w}C{p_w}}}{{{m_a}}}} \right)}}{{{Z_d}\left( {C{p_a} - \frac{{{m_w}C{p_w}}}{{{m_a}}}} \right)}}$$</div>
-
-<div>$$Z = exp\left( {{U_c}{A_w}\left( {\frac{1}{{{m_a}}} - \frac{{bb}}{{{m_w}C{p_w}}}} \right)} \right)$$</div>
-
-<div>$$K1 = \frac{{{Z_d} - 1}}{{{Z_d} - \frac{{{m_a}C{p_a}}}{{{m_w}C{p_w}}}}}$$</div>
-
-<div>$${Z_d} = exp\left( {{U_c}{A_{dry}}\left( {\frac{1}{{{m_a}C{p_a}}} - \frac{1}{{{m_w}C{p_w}}}} \right)} \right)$$</div>
-
-#### Underlying Correlations, Properties, and Assumptions
-
-Overall heat transfer coefficients are calculated from the specified coil geometry and by using empirical correlations from fluid mechanics and heat transfer.  For the water side, Equation gives the film heat transfer coefficient in SI units:
-
-<div>$${f_i} = 1.429\left( {1 + 0.0146 {T_w}} \right)V_w^{0.8}D_i^{ - 0.2}$$</div>
-
-This is valid for Reynolds numbers greater than 3100 based on water flow velocity and pipe inside diameter and is given in Elmahdy and Mitalas(1977) as recommended in the standard issued by the Air-Conditioning and Refrigeration Institute (1972) for air-cooling coils.  The definition of overall inside thermal resistance follows directly as shown in Equation.
-
-<div>$${R_i} = \frac{1}{{{f_i}{A_i}}}$$</div>
-
-Equation gives the film coefficient for the air side.  Another form of the same equation is Equation , which is familiar from the data presented in Kays and London (1984).  For coil sections that have a wet surface due to condensation, the air side film coefficient is modified according to Equation .  The correction term, a function of air Reynolds number, is valid for Reynolds numbers between 400 and 1500.  The coefficients in Equation and are calculated by Equations and that are functions of the coil geometry.  Elmahdy (1977)explains the modifier for the wet surface and coefficients for the film coefficient.  Equations through show definitions and values of common parameters and properties.
-
-<div>$${f_o} = {C_1}Re_a^{{C_2}}\frac{{{m_a}}}{{{A_{a\_min\_flow}}}}C{p_a}Pr_a^{{\raise0.5ex\hbox{$\scriptstyle 2$}\kern-0.1em/\kern-0.15em\lower0.25ex\hbox{$\scriptstyle 3$}}}$$</div>
-
-<div>$${C_1}Re_a^{{C_2}} = S{t_a}Pr_a^{{\raise0.5ex\hbox{$\scriptstyle 2$}\kern-0.1em/\kern-0.15em\lower0.25ex\hbox{$\scriptstyle 3$}}}$$</div>
-
-<div>$${f_{o,w}} = {f_o}\left( {1.425 - 5.1 \times {{10}^{ - 4}}R{e_a} + 2.63 \times {{10}^{ - 7}}Re_a^2} \right)$$</div>
-
-<div>$${C_1} = 0.159{\left( {\frac{{{\delta_{fin}}}}{{{D_{hdr}}}}} \right)^{ - 0.065}}{\left( {\frac{{{\delta_{fin}}}}{{{L_{fin}}}}} \right)^{0.141}}$$</div>
-
-<div>$${C_2} =  - 0.323{\left( {\frac{{{\Delta_{fins}}}}{{{L_{fin}}}}} \right)^{0.049}}{\left( {\frac{{{D_{fin}}}}{{{\Delta_{tube\_rows}}}}} \right)^{0.549}}{\left( {\frac{{{\delta_{fin}}}}{{{\Delta_{fins}}}}} \right)^{ - 0.028}}$$</div>
-
-<div>$${D_{hdr}} = \frac{{4{A_{a\_min\_flow}}{\delta_{coil}}}}{{{A_{s\_total}}}}$$</div>
-
-<div>$$R{e_a} = \frac{{4{\delta_{coil}}\left( {1 + {w_a}} \right){m_a}}}{{{A_{s\_total}}{\mu_a}}}$$</div>
-
-<div>$$P{r_a} = 0.733$$</div>
-
-<div>$${\mu_a} = 1.846 \times {10^{ - 5}}$$</div>
-
-The film coefficients above act on the extended surface of the air side, that is the area of the fins and the tubes.  Therefore, the fin efficiency must also be considered in calculating the overall thermal resistance on the outside.  Gardner(1945) gives the derivation of Equation , used as a curve fit to find the fin efficiency as a function of film coefficient.  This equation is based on circular fins of constant thickness.  To model a coil with flat fins, an effective diameter -- that of circular fins with the same fin area -- is used.  Equations through define variables used in Equation .  The overall efficiency of the surface is shown by Equation .  Note that the efficiency is found by the same equations for the wet surface using the wet surface film coefficient.
-
-<div>$${\eta_{fin}} = \frac{{ - 2\rho }}{{fai(1 + \rho )}}\left[ {\frac{{{I_1}({u_b}){K_1}({u_e}) - {K_1}({u_b}){I_1}({u_e})}}{{{I_0}({u_b}){K_1}({u_e}) + {K_0}({u_b}){I_1}({u_e})}}} \right]$$</div>
-
-<div>$$fai = \frac{{({D_{fin}} - {D_{tube}})}}{2}\sqrt {\frac{{2{f_o}}}{{{k_{fin}}{\delta_{fin}}}}} $$</div>
-
-<div>$$\rho  = \frac{{{D_{tube}}}}{{{D_{fin}}}}$$</div>
-
-<div>$${u_e} = \frac{{fai}}{{1 - \rho }}$$</div>
-
-<div>$${u_b} = {u_e}\rho $$</div>
-
-<div>$${\eta_o} = 1 - (1 - {\eta_{fin}})\frac{{{A_{fins}}}}{{{A_{s\_total}}}}$$</div>
-
-The definition of overall outside thermal resistance is given in Equation as a function of fin efficiency and film coefficient.  For a wet coil surface the resistance must be defined differently because the heat transfer equations are based on enthalpy rather than temperature differences, as shown in Equation .
-
-<div>$${R_o} = \frac{1}{{{f_o}{\eta_o}{A_{s,total}}}}$$</div>
-
-<div>$${R_{o,w}} = \frac{{{\raise0.7ex\hbox{${C{p_a}}$} \!\mathord{\left/ {\vphantom {{C{p_a}} {bb}}}\right.}\!\lower0.7ex\hbox{${bb}$}}}}{{{f_{o,w}}{\eta_{o,w}}{A_{s,total}}}}$$</div>
-
-Equation gives the last two overall components of thermal resistance.  They represent the metal tube wall and internal fouling.  The fouling factor, due to deposits of dirt and corrosion of the tube inside surfaces, is assumed to be 5x10-5 m2·K/W.  All components of thermal resistance are added in series to produce the overall heat transfer coefficients shown in Equations and .
-
-<div>$${R_{mf}} = \frac{{{\delta_{tube}}}}{{{k_{tube}}{A_i}}} + \frac{{Fl}}{{{A_i}}}$$</div>
-
-<div>$$U{A_{dry}} = \frac{{{A_{dry}}}}{{{A_{s,total}}}}\left[ {\frac{1}{{{R_i} + {R_{mf}} + {R_o}}}} \right]$$</div>
-
-<div>$${U_c}{A_w} = \frac{{{A_w}}}{{{A_{s,total}}}}\left[ {\frac{{{1 \mathord{\left/ {\vphantom {1 {bb}}} \right. } {bb}}}}{{{R_i} + {R_{mf}} + {R_{o,w}}}}} \right]$$</div>
-
-#### Solution Method of Model
-
-The complicated equations derived above were implemented in a successive substitution solution procedure to calculate the coil performance based on the input parameters.  The MODSIM implementation of a cooling coil, the TYPE12 subroutine, was the motivation for this approach; the method used there has been retained with modifications for the uncontrolled coil model.  Clark (1985) contains notes about the MODSIM routine.
-
-In the general case, the cooling coil is only partially wet.  For an uncontrolled coil, Equation  is used to find the water temperature at the boundary.  Several simple equations in the loop adjust the boundary point until the dry surface temperature at the boundary is equal to the dewpoint of the inlet air.  For the controlled coil, Equations and give two calculations of the boundary temperature, and the water flow rate and boundary position are adjusted until the two equations agree.
-
-Special cases occur when the coil is all wet or all dry.  The coil is solved as if it were all wet before the general case is attempted.  If the wet surface temperatures at the coil inlet and outlet are both below the dewpoint, no further solution is required.  However, to ensure a continuous solution as flow variables are changed, when the surface is all dry or when it is wet with only the dry surface equations yielding a surface temperature below the dewpoint at the water outlet, the general solution is used to calculate the unknowns.  In the solution of the controlled coil the outlet air enthalpy, given some resulting dehumidification, must correspond to the enthalpy at the specified outlet air temperature.
-
-#### Application of Cooling Coil Model to Heating Coils
-
-The implementation of detailed heating coil models in IBLAST was another important aspect of the system/plant integration.  The same kind of loops exist to provide hot water to the heating coils from the boilers as exist to supply the cooling coils with chilled water from the chillers.   Some simplifications can be made, however, since the enthalpy change of the air flowing over a heating coil is entirely sensible.  There is no condensation in a heating coil.  In order to allow heating and cooling coils to be specified using the same geometric parameters, a heating coil simulation was developed from the cooling coil model described above by eliminating the wet surface analysis.
-
-In addition, it was concluded that, since much simpler and less computationally expensive heating coil simulations are possible, an option was provided in IBLAST for a heating coil design using only the UA value of the coil, the product of heat transfer coefficient and coil area.  This model was largely based on the TYPE10 subroutine implemented in MODSIM.  The equations used to model the performance of the TYPE10 heating coil are as follows:
-
-<div>$$
-  \begin{array}{rl} 
-    T_{a,out} &= T_{a,in} + \left( T_{w,in} - T_{ain} \right) \varepsilon \left( \frac{\min \left( C_{p,a} \dot m_a,C_{p,w}\dot m_w \right)} {C_{p,a}\dot m_a} \right) \\
-    T_{w,out} &= T_{w,in} - \left( T_{a,out} - T_{ain} \right) \left( \frac{C_{p,a}\dot m_a}{C_{p,w}\dot m_w} \right)
-  \end{array}
-$$</div>
-
-where the coil effectiveness is given by:
-
-<div>$$\varepsilon  = 1 - \exp \left( {\frac{{\left\{ {\exp \left[ { - \left( {\frac{{\min \left\{ {{C_{p,a}}{{\dot m}_a},{C_{p,w}}{{\dot m}_w}} \right\}}}{{\max \left\{ {{C_{p,a}}{{\dot m}_a},{C_{p,w}}{{\dot m}_w}} \right\}}}} \right){{\left\{ {NTU} \right\}}^{0.78}}} \right] - 1} \right\}}}{{\left( {\frac{{\min \left\{ {{C_{p,a}}{{\dot m}_a},{C_{p,w}}{{\dot m}_w}} \right\}}}{{\max \left\{ {{C_{p,a}}{{\dot m}_a},{C_{p,w}}{{\dot m}_w}} \right\}}}} \right){{\left\{ {NTU} \right\}}^{ - .22}}}}} \right)$$</div>
-
-The parameter NTU is the number of transfer units and is defined as a function of the UA value of the coil as follows:
-
-<div>$${\rm{NTU}} = \frac{{{\rm{UA}}}}{{{\rm{min}}\left( {{{\rm{C}}_{{\rm{p,a}}}}{{{\rm{\dot m}}}_{\rm{a}}}{\rm{,}}{{\rm{C}}_{{\rm{p,w}}}}{{{\rm{\dot m}}}_{\rm{w}}}} \right)}}$$</div>
-
-
-
-### Hot-Water-Based Air Heating Coil
-
-#### Overview
-
-The input object Coil:Heating:Water provides a model that uses an NTU–effectiveness model of a static heat exchanger. The model is an inlet – outlet model: given the inlet conditions and flow rates and the UA, the effectiveness is calculated using the formula for the effectiveness of a cross-flow heat exchanger with both fluid streams unmixed. The effectiveness then allows the calculation of the outlet conditions from the inlet conditions.
-
-The inputs to the model are: (1) the current inlet temperatures and flow rates of the air and water fluid streams and (2) the UA of the coil. Note that the UA is fixed in this model and is not a function of the flow rates.
-
-There are 2 alternative user inputs for the component: the user may input the design water volumetric flow rate and the UA directly; or the user may choose to input the more familiar design heating capacity plus design inlet & outlet temperatures and let the program calculate the design UA. These alternative user inputs are fully described in the EnergyPlus Input Output Reference document.
-
-#### Model Description
-
-The air and water capacitance flows are defined as:
-
-<div>$${\dot C_{air}} = {c_{p,air}}\cdot {\dot m_{air}}$$</div>
-
-<div>$${\dot C_{water}} = {c_{p,water}}\cdot {\dot m_{water}}$$</div>
-
-The minimum and maximum capacity flows are then:
-
-<div>$${\dot C_{\min }} = \min ({\dot C_{air}},{\dot C_{water}})$$</div>
-
-<div>$${\dot C_{\max }} = \max ({\dot C_{air}},{\dot C_{water}})$$</div>
-
-The capacitance flow ratio is defined as:
-
-<div>$$Z = {\dot C_{\min }}/{\dot C_{\max }}$$</div>
-
-The number of transfer units (*NTU*) is:
-
-<div>$$NTU = UA/{\dot C_{\min }}$$</div>
-
-The effectiveness is:
-
-<div>$$\varepsilon  = 1 - \exp (\frac{{{e^{ - NTU \cdot Z \cdot \eta }} - 1}}{{Z \cdot \eta }})$$</div>
-
-Where <span>\(\eta  = NT{U^{ - 0.22}}\)</span>.
-
-The outlet conditions are then:
-
-<div>$${T_{air,out}} = {T_{air,in}} + \varepsilon \cdot {\dot C_{\min }}\cdot ({T_{water,in}} - {T_{air,in}})/{\dot C_{air}}$$</div>
-
-<div>$${T_{water,out}} = {T_{water,in}} - {\dot C_{air}}\cdot ({T_{air,out}} - {T_{air,in}})/{\dot C_{water}}$$</div>
-
-The output of the coil in watts is:
-
-<div>$${\dot Q_{coil}} = {\dot C_{water}}\cdot ({T_{water,in}} - {T_{water,out}})$$</div>
-
-The UA value is recalculated for each timestep.  A nominal UA, *UA<sub>0</sub>*, at the rating point is calculated by the program using the input for rated conditions and a search routine called regula falsi.
-
-User input for the ratio of convective heat transfers at the nominal or rated operating point, “*r*,� is used in the model.  This ratio is defined as
-
-<div>$$r = \frac{{{\eta_f}{{\left( {hA} \right)}_{air}}}}{{{{\left( {hA} \right)}_{water}}}}$$</div>
-
-where,
-
-      <span>\({\eta_f}\)</span> is the fin efficiency, (dimensionless)
-
-      *h* is the surface convection heat transfer coefficient
-
-*      A* is the surface area
-
-The value calculated for *UA<sub>0</sub>* is used with the input for *r* to characterize the convective heat transfer on the water sides at the nominal rating operation point using
-
-<div>$${\left( {{{\left( {hA} \right)}_w}} \right)_0} = U{A_0}\left( {\frac{{r + 1}}{r}} \right)$$</div>
-
-and on the air side at the nominal rating point using
-
-<div>$${\left( {{\eta_f}{{\left( {hA} \right)}_a}} \right)_0} = r{\left( {hA} \right)_{w,0}}$$</div>
-
-Then the following equations are used to calculate a new UA as a function of the flow rates and inlet temperatures at each timestep.
-
-<div>$${x_a} = 1 + 4.769\cdot {10^{ - 3}}\left( {{T_{air,in}} - {T_{air,in,0}}} \right)$$</div>
-
-<div>$${\eta_f}{\left( {hA} \right)_a} = {x_a}{\left( {\frac{{{{\dot m}_a}}}{{{{\dot m}_{a,0}}}}} \right)^{0.8}}{\left( {{\eta_f}{{\left( {hA} \right)}_a}} \right)_0}$$</div>
-
-<div>$${x_w} = 1 + \left( {\frac{{0.014}}{{1 + 0.014{T_{water,in,0}}}}} \right)\;\left( {{T_{water,in}} - {T_{water,in,0}}} \right)$$</div>
-
-<div>$${\left( {hA} \right)_w} = {x_w}{\left( {\frac{{{{\dot m}_w}}}{{{{\dot m}_{w,0}}}}} \right)^{0.85}}{\left( {hA} \right)_{w,0}}$$</div>
-
-<div>$$UA = {\left( {\frac{1}{{{{\left( {hA} \right)}_w}}} + \frac{1}{{{\eta_f}{{\left( {hA} \right)}_a}}}} \right)^{ - 1}}$$</div>
-
-The above formulas are from the following reference, along with further references. The equation for x<sub>w</sub> was modified from that published in Wetter (1999) to correct a small error.
-
-#### References
-
-Wetter, M. 1999. Simulation Model: Finned Water-to-Air Coil Without Condensation. LBNL-42355. This document can be downloaded from .
-
-### Single-Speed Electric DX Air Cooling Coil
-
-#### Overview
-
-This model (object names Coil:Cooling:DX:SingleSpeed and Coil:Cooling:DX:TwoStageWithHumidityControlMode, with CoilPerformance:DX:Cooling) simulates the performance of an air-cooled or evaporative-cooled direct expansion (DX) air conditioner. The model uses performance information at rated conditions along with curve fits for variations in total capacity, energy input ratio and part-load fraction to determine the performance of the unit at part-load conditions (Henderson et al. 1992, ASHRAE 1993). Sensible/latent capacity splits are determined by the rated sensible heat ratio (SHR) and the apparatus dewpoint (ADP)/bypass factor (BF) approach. This approach is analogous to the NTU-effectiveness calculations used for sensible-only heat exchanger calculations, extended to a cooling and dehumidifying coil.
-
-This model simulates the thermal performance of the DX cooling coil and the power consumption of the outdoor condensing unit (compressor, fan, crankcase heater and evap condenser water pump). The total amount of heat rejected by the condenser is also calculated and stored for use by other waste heat recovery models (e.g., Coil:Heating:Desuperheater). The performance of the indoor supply air fan varies widely from system to system depending on control strategy (e.g., constant fan vs. AUTO fan, constant air volume vs. variable air volume, etc.), fan type, fan motor efficiency and pressure losses through the air distribution system. Therefore, this DX system model does not account for the thermal effects or electric power consumption of the indoor supply air fan. EnergyPlus contains separate models for simulating the performance of various indoor fan configurations, and these models can be easily linked with the DX system model described here to simulate the entire DX air conditioner being considered (e.g., see AirLoopHVAC:Unitary:Furnace:HeatCool, AirLoopHVAC:UnitaryHeatCool, ZoneHVAC:WindowAirConditioner or AirLoopHVAC:UnitaryHeatPump:AirToAir).
-
-#### Model Description
-
-The user must input the total cooling capacity, sensible heat ratio (SHR), coefficient of performance (COP) and the volumetric air flow rate across the cooling coil at rated conditions. The capacity, SHR and COP inputs should be “gross� values, excluding any thermal or energy impacts due to the indoor supply air fan. The rated conditions are considered to be air entering the cooling coil at 26.7°C drybulb/19.4°C wetbulb and air entering the outdoor condenser coil at 35°C drybulb/23.9°C wetbulb. The rated volumetric air flow should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of rated total cooling capacity (300 – 450 cfm/ton). The rated volumetric air flow to total cooling capacity ratio for 100% dedicated outdoor air (DOAS) application DX cooling coils should be between 0.00001677 (m3/s)/W (125 cfm/ton) and 0.00003355 (m3/s)/W (250 cfm/ton).
-
-The user must also input five performance curves or performance tables that describe the change in total cooling capacity and efficiency at part-load conditions:
-
-1)    Total cooling capacity modifier curve or table (function of temperature)
-
-2)    Total cooling capacity modifier curve or table (function of flow fraction)
-
-3)    Energy input ratio (EIR) modifier curve or table (function of temperature)
-
-4)    Energy input ratio (EIR) modifier curve or table (function of flow fraction)
-
-5)    Part load fraction correlation curve or table (function of part load ratio)
-
-* The total cooling capacity modifier curve (function of temperature) is a curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the rated total cooling capacity to give the total cooling capacity at the specific entering air temperatures at which the DX coil unit is operating (i.e., at temperatures different from the rating point temperatures).  This curve is typically a biquadratic but any curve or table with two independent variables can be used.
-
-Note: The data used to develop the total cooling capacity modifier curve (function of temperature) should represent performance when the cooling coil is ‘wet’ (i.e., coil providing sensible cooling and at least some dehumidification). Performance data when the cooling coil is ‘dry’ (i.e., not providing any dehumidification) should **not** be included when developing this modifier curve. This model automatically detects and adjusts for ‘dry coil’ conditions (see section “Dry Coil Conditions� below).
-
-<div>$$ \text{TotCapTempModFac} = \text{Func}\left(T_{wb,i},T_c,i\right) $$</div>
-
-where
-
-<span>\({T_{wb,i}}\)</span> = x values = wet-bulb temperature of the air entering the cooling coil, °C
-
-<span>\({T_{c,i}}\)</span> = y values = dry-bulb temperature of the air entering an air-cooled condenser or wet-bulb temperature of the air entering an evaporative-cooled condenser, °C
-
-* The total cooling capacity modifier curve (function of flow fraction) is a curve with one independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the total cooling capacity at the specific temperature and air flow conditions at which the DX unit is operating.  This curve is typically a quadratic but any curve or table with one independent variable can be used.
-
-<div>$$\text{TotCapFlowModFac} = \text{Func}\left(ff\right)$$</div>
-
-where
-
-<div>$$ff = \text{flow fraction} = \left( \frac{\text{Actual air mass flow rate}}{\text{Rated air mass flow rate}} \right) = \text{x value}$$</div>
-
-**Note:**  The actual volumetric air flow rate through the cooling coil for any simulation time step where the DX unit is operating must be between 0.00002684 m<sup>3</sup>/s and .00006713 m<sup>3</sup>/s per watt of rated total cooling capacity (200 - 500 cfm/ton). The simulation will issue a warning message if this air flow range is exceeded.
-
-* The energy input ratio (EIR) modifier curve (function of temperature) is a curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at the specific entering air temperatures at which the DX coil unit is operating (i.e., at temperatures different from the rating point temperatures).  This curve is typically a biquadratic but any curve or table with two independent variables can be used.
-
-Note: The data used to develop the energy input ratio (EIR) modifier curve (function of temperature) should represent performance when the cooling coil is ‘wet’ (i.e., coil providing sensible cooling and at least some dehumidification). Performance data when the cooling coil is ‘dry’ (i.e., not providing any dehumidification) should **not** be included when developing this modifier curve. This model automatically detects and adjusts for ‘dry coil’ conditions (see section “Dry Coil Conditions� below).
-
-<div>$$\text{EIRTempModFac} = \text{Func}\left(T_{wb,i},T_c,i\right)$$</div>
-
-where
-
-<span>\({T_{wb,i}}\)</span> = x values = wet-bulb temperature of the air entering the cooling coil, °C
-
-<span>\({T_{c,i}}\)</span> = y values = dry-bulb temperature of the air entering an air-cooled condenser or wet-bulb temperature of the air entering an evaporative-cooled condenser, °C
-
-* The energy input ratio (EIR) modifier curve (function of flow fraction) is a curve with one independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the DX unit is operating.  This curve is typically a quadratic but any curve or table with one independent variable can be used.
-
-<div>$$\text{EIRFlowModFrac} = \text{Func}\left(ff\right)$$</div>
-
-where
-
-<div>$$ff = \text{flow fraction} = \left( \frac{\text{Actual air mass flow rate}}{\text{Rated air mass flow rate}} \right) = \text{x value}$$</div>
-
-* The part load fraction correlation (function of part load ratio) is a curve with one independent variable being part load ratio (sensible cooling load / steady-state sensible cooling capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the “effective� EIR for a given simulation time step. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.  This curve is typically a linear, quadratic, or cubic but any curve or table with one independent variable can be used.
-
-<div>$$\text{PartLoadFrac} = \text{PLF} = \text{Func}\left(\text{PLR}\right)$$</div>
-
-where
-
-<div>$$\text{PLR} = \text{part load ratio} = \left(\frac{\text{actual sensible cooling load}}{\text{steady-state sensible cooling load}}\right) = \text{x values}$$</div>
-
-The part-load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation time step). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-<div>$$ \begin{array}{rl} \text{PLF} &\geq 0.7 \\ \text{PLF} &\geq \text{PLR} \end{array}$$</div>
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential or small commercial unit) would be:
-
-PLF = 0.85 + 0.15(PLR)
-
-All five part-load curves are accessed through EnergyPlus’ built-in performance curve equation manager (curve: quadratic, curve:cubic and curve:biquadratic). It is not imperative that the user utilize all coefficients shown in equations (449) through (453) if their performance equation has fewer terms (e.g., if the user’s PartLoadFrac performance curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero).
-
-For any simulation time step, the total (gross) cooling capacity of the DX unit is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{total}} = {\mathop Q\limits^ \bullet_{total,rated}}\left( {TotCapTempModFac} \right)\left( {TotCapFlowModFac} \right)$$</div>
-
-In a similar fashion, the electrical power consumed by the DX unit (compressors plus outdoor condenser fans) for any simulation time step is calculated using the following equation:
-
-<div>$$Power = \left( {{{\mathop Q\limits^ \bullet  }_{total}}} \right)\left( {EIR} \right)\left( {RTF} \right)$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{total}}\)</span>= Total cooling capacity, W -- ref. equation (455)
-
-<div>$$EIR = \,Energy\,input\,ratio\, = \,\left( {\frac{1}{{CO{P_{rated}}}}} \right)\left( {EIRTempModFac} \right)\left( {EIRFlowModFac} \right)$$</div>
-
-<span>\(CO{P_{rated}}\)</span> = Coefficient of performance at rated conditions (user input)
-
-<div>$$RTF{\rm{ }} = {\rm{ }}\left( {{\raise0.7ex\hbox{${PLR}$} \!\mathord{\left/ {\vphantom {{PLR} {PartLoadFrac}}}\right.}\!\lower0.7ex\hbox{${PartLoadFrac}$}}} \right)\,\, = \,\,runtime fraction of the cooling coil$$</div>
-
-The total amount of heat rejected by the condenser is then calculated and stored for use by other waste heat recovery models (e.g., Coil:Heating:Desuperheater).
-
-<div>$${\mathop Q\limits^ \bullet_{cond}} = {\mathop Q\limits^ \bullet_{total}}\left( {1 + EIR} \right)$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{cond}}\)</span> = total amount of heat rejected by the condenser (W)
-
-The crankcase heater is assumed to operate when the cooling coil’s compressor is OFF and the outdoor dry-bulb temperature is below the maximum outdoor temperature for crankcase heater operation. The average crankcase heater power for the simulation time step is calculated as follows:
-
-<div>$${P_{crankcase}} = {\mathop Q\limits^ \bullet_{cap,crankcase}}\left( {1 - RTF} \right)$$</div>
-
-where
-
-<span>\({P_{crankcase}}\)</span> = DX cooling coil crankcase heater power, W
-
-<span>\({\mathop Q\limits^ \bullet_{cap,crankcase}}\)</span>= crankcase heater capacity, W
-
-If this cooling coil is used as part of an air-to-air heat pump (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir), the crankcase heater defined for this DX cooling coil is disregarded and the associated output variable is omitted. Instead, the crankcase heater defined for the DX heating coil (Coil:Heating:DX:SingleSpeed) is enabled during the time that the compressor is not running for either heating or cooling. In this instance, RTF in the above equations would be the runtime fraction of the heat pump’s heating coil or cooling coil, whichever is greater.
-
-In addition to calculating the total cooling capacity provided by the DX air conditioner, it is important to properly determine the break down of total cooling capacity into its sensible (temperature) and latent (dehumidification) components. The model computes the sensible/ latent split using the rated SHR and the ADP/BF approach (Carrier et al. 1959). When the DX coil model is initially called during an EnergyPlus simulation, the rated total capacity and rated SHR are used to calculate the coil bypass factor (BF) at rated conditions. The rated total capacity and rated SHR are first used to determine the ratio of change in air humidity ratio to air dry-bulb temperature:
-
-<div>$$SlopeRated = \,\left( {\frac{{{\omega_{in}} - {\omega_{out}}}}{{{T_{db,in}}\, - {T_{db,out}}}}} \right)\mathop {}\limits_{rated} $$</div>
-
-where
-
-*ω<sub>in</sub>* = humidity ratio of the air entering the cooling coil at rated conditions, kg/kg
-
-*ω<sub>out</sub>* = humidity ratio of the air leaving the cooling coil at rated conditions, kg/kg
-
-*T<sub>db,in</sub>* = dry-bulb temperature of the air entering the cooling coil at rated conditions, °C
-
-*T<sub>db,out</sub>* = dry-bulb temperature of the air leaving the cooling coil at rated conditions, °C
-
-Along with the rated entering air conditions, the algorithm then searches along the saturation curve of the psychrometric chart until the slope of the line between the point on the saturation curve and the inlet air conditions matches *SlopeRated*. Once this point, the apparatus dewpoint, is found on the saturation curve the coil bypass factor at rated conditions is calculated as follows:
-
-<div>$$B{F_{rated}} = \,\frac{{{h_{out,rated}}\,\, - \,{h_{ADP}}}}{{{h_{in,rated}}\,\, - \,{h_{ADP}}}}$$</div>
-
-where
-
-*h<sub>out,rated</sub>* <sub> </sub>= enthalpy of the air leaving the cooling coil at rated conditions, J/kg
-
-*h<sub>in,rated</sub>* <sub> </sub>= enthalpy of the air entering the cooling coil at rated conditions, J/kg
-
-*h<sub>ADP</sub>* <sub> </sub>= enthalpy of saturated air at the coil apparatus dewpoint, J/kg
-
-The coil bypass factor is analogous to the “ineffectiveness� (1-ε) of a heat exchanger, and can be described in terms of the number of transfer of unit (NTU).
-
-<div>$$BF = \,{e^{ - NTU}}\, = \,\,{e^{ - \,{{\left( {\frac{{UA}}{{cp}}} \right)} \mathord{\left/ {\vphantom {{\left( {\frac{{UA}}{{cp}}} \right)} {\dot m}}} \right. } {\dot m}}}}\, = \,{e^{ - \,\,{{Ao} \mathord{\left/ {\vphantom {{Ao} {\dot m}}} \right. } {\dot m}}}}$$</div>
-
-For a given coil geometry, the bypass factor is only a function of air mass flow rate. The model calculates the parameter A<sub>o</sub> in equation (460) based on BF<sub>rated</sub> and the rated air mass flow rate. With A<sub>o</sub> known, the coil BF can be determined for non-rated air flow rates.
-
-For each simulation time step when the DX air conditioner operates to meet a cooling load, the total cooling capacity at the actual operating conditions is calculated using equation (455) and the coil bypass factor is calculated based on equation (460). The coil bypass factor is used to calculate the operating sensible heat ratio (SHR) of the cooling coil using equations (461) and (462).
-
-<div>$${h_{ADP}}\,\, = \,{h_{in}}\, - \,\frac{{({{\mathop Q\limits^ \bullet  }_{total}}\,/\dot m)}}{{1 - BF}}$$</div>
-
-<div>$$SHR\,\, = \,Minimum\,\left( {\left( {\frac{{{h_{Tin,wADP}}\, - \,{h_{ADP}}}}{{{h_{in}} - {h_{ADP}}}}} \right),\,\,1} \right)$$</div>
-
-where
-
-<span>\({h_{in}}\)</span>          = enthalpy of the air entering the cooling coil, J/kg
-
-<span>\({h_{ADP}}\)</span>       = enthalpy of air at the apparatus dewpoint condition, J/kg
-
-<span>\({h_{Tin,wADP}}\)</span> = enthalpy of air at the entering coil dry-bulb temperature and humidity ratio at ADP, J/kg
-
-<span>\(\dot m\)</span>            = air mass flow rate, kg/s
-
-With the SHR for the coil at the current operating conditions, the properties of the air leaving the cooling coil are calculated using the following equations:
-
-<div>$${h_{out}}\, = \,{h_{in}} - \,{\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{total}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{total}}} {\dot m}}}\right.}\!\lower0.7ex\hbox{${\dot m}$}}$$</div>
-
-<div>$${h_{Tin,\omega out}}\, = \,{h_{in}} - \,\left( {1 - SHR} \right)\left( {{h_{in}} - {h_{out}}} \right)$$</div>
-
-<div>$${\omega_{out}}\, = \,PsyWFnTdbH({T_{in}},\,\,{h_{Tin,\omega out}})$$</div>
-
-<div>$${T_{db,out}}\, = \,PsyTdbFnHW({h_{out}},\,\,\,{\omega_{out}})$$</div>
-
-where
-
-<span>\({h_{out}}\)</span>         = enthalpy of the air leaving the cooling coil, J/kg
-
-<span>\({h_{Tin,\,\omega out}}\)</span>  = enthalpy of air at the entering coil dry-bulb temperature and leaving air humidity ratio, J/kg
-
-<span>\(\,{\omega_{out}}\)</span>        = leaving air humidity ratio, kg/kg
-
-<span>\(\,{T_{db,out}}\)</span>    = leaving air dry-bulb temperature, °C
-
-*PsyWFnTdbH* = EnergyPlus psychrometric function, returns humidity ratio given dry-bulb temperature and enthalpy
-
-*PsyTdbFnHW* = EnergyPlus psychrometric function, returns dry-bulb temperature given enthalpy and humidity ratio
-
-#### Dry Coil Conditions
-
-If the model determines that the cooling coil is dry (ω<sub>in</sub> &lt; ω<sub>ADP</sub>), then equations (455) and (456) are invalid since they are functions of entering wet-bulb temperature. Under dry-coil conditions, coil performance is a function of dry-bulb temperature rather than wet-bulb temperature. In this case, the model recalculates the performance of the DX cooling unit using the calculation procedure described above but with ω<sub>in\\ =</sub> ω<sub>dry,</sub> where ω<sub>dry</sub> is the inlet air humidity ratio at the coil dry-out point (SHR = 1.0).
-
-#### SHR Calculation Using User Specified SHR Modifier Curves
-
-This alternative SHR calculation method is based on user specified *SHR* modifying curves for temperature and flow fractions.  The modifying curves correct the rated *SHR* value for a given DX cooling coil entering air temperatures and air mass flow fraction.  These *SHR* modifying curves are optional additional curve inputs to the DX cooling coil objects.  These two curves are a biquadratic *SHR* modifier curve for temperature (*SHRFT*), and a quadratic *SHR* correction curve for flow fraction (*SHRFFF*).
-
-·        Biquadratic *SHR* modifier normalized curve for DX cooling coil entering air (outdoor) wet-bulb and dry-bulb temperatures. The coil entering conditions can be outdoor air or pretreated outdoor air.
-
-·        Quadratic SHR modifier curve for flow fraction.
-
-The SHR is given by:
-
-<div>$$SHR = SH{R_{rated}} \cdot SHRFT\left( {{T_{wb,i}},{T_{db,i}}} \right) \cdot SHRFFF\left( {FF} \right)$$</div>
-
-The cooing coil outlet air enthalpy is given by:
-
-<div>$${h_{out}} = {h_{in}} - \frac{{{{\dot Q}_{total}}}}{{\dot m}}$$</div>
-
-The cooling coil outlet air enthalpy at the coil enlet air temperature and coil outlet humidity ratio is given by:
-
-<div>$${h_{{T_{in}}{\omega_{out}}}} = {h_{in}} - \left( {1.0 - SHR} \right)\frac{{{{\dot Q}_{total}}}}{{\dot m}}$$</div>
-
-The DX cooling coil outlet air humidity ratio is calculated from the psychometric function as follows:
-
-<div>$${\omega_{out}} = PsyWFnTdbH\left( {{T_{db,\,i}},{h_{{T_{in}}{\omega_{out}}}}} \right)$$</div>
-
-The DX cooling coils leaving humidity ratio cannot exceed the DX coil entering air humidity ratio. And for dry air condition entering the cooling coil, the above equation may yield unrealistic (in some cases negative values) coil outlet humidity ratio.  In this case the coil outlet air humidity is set a small value as follows:
-
-<div>$${\omega_{out}} = MIN\left( {0.000010,{\omega_{in}}} \right)$$</div>
-
-The DX cooling coil outlet air dry-bulb temperature is determined as follows:
-
-<div>$${T_{db,out}} = PsyTdbFnHW\left( {{h_{out}},{\omega_{out}}} \right)$$</div>
-
-where
-
-<span>\(SHRFT\)</span>  = sensible heat ratio modifier normalized biquadratic curve as a function of coil entering air wet-bulb and dry-bulb temperatures, (-). The DX cooling coil entering air temperature can be the outdoor air condition or pretreated outdoor air when the DX cooling coil is placed after an exhaust heat recovery heat exchangers.
-
-<span>\(SHRFFF\)</span>= sensible heat ratio modifier normalized quadratic curve as a function of air mass flow fraction.  Flow fraction is the ratio of actual to rated mass flow rate of air through the DX cooling coil, (-).
-
-<span>\(SH{R_{rated}}\)</span>  = sensible heat ratio at rated condition, (-).
-
-#### Condenser Options: AirCooled vs. EvaporativelyCooled
-
-As described previously, this model can simulate the performance of air-cooled or evaporative-cooled DX air conditioners. The following paragraphs describe three modeling options.
-
-If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) (equations (449) and (451) above) will utilize the outdoor dry-bulb temperature.
-
-If the user wishes to model an evaporatively-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = EvaporativlyCooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) (equations (449) and (451) above) will utilize the outdoor wet-bulb temperature.
-
-If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = EvaporativelyCooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) will utilize the condenser inlet air temperature as calculated below:
-
-<div>$${T_{c,i}} = \,\left( {{T_{wb,o}}} \right)\,\, + \,\,\left( {1 - EvapCondEffectiveness} \right)\left( {{T_{db,o}}\,\, - {T_{wb,o}}} \right)$$</div>
-
-where
-
-*T<sub>c,i</sub>* = the temperature of the air entering the condenser coil, °C
-
-*T<sub>wb,o</sub>* = the wet-bulb temperature of the outdoor air, °C
-
-*T<sub>db,o</sub>* = the dry-bulb temperature of the outdoor air, °C
-
-In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
-
-If an evaporatively-cooled condenser is modeled, the power requirements for the water pump are calculated as follows:
-
-<div>$${P_{evapcondpump}} = {\mathop Q\limits^ \bullet_{cap,evapcondpump}}\left( {RTF} \right)$$</div>
-
-where
-
-<span>\({P_{evapcondpump}}\)</span> = DX cooling coil evap condenser pump electric power, W
-
-<span>\({\mathop Q\limits^ \bullet_{cap,evapcondpump}}\)</span>= evaporative condenser pump rated power consumption, W
-
-Water consumption for the evaporative-cooled condenser is calculated using the difference in air humidity level across the evaporative media and the condenser air mass flow rate:
-
-<div>$${V_{water}} = \frac{{{{\mathop m\limits^ \bullet  }_{_{air}}}\left( {{\omega_{evapcond,out}} - {\omega_{evapcond,in}}} \right)}}{{{\rho_{water}}}}\left( {RTF} \right)\left( {TimeStepSys} \right)\left( {3600.} \right)\,$$</div>
-
-where
-
-<span>\({V_{water}}\)</span>         = DX cooling coil evap condenser water consumption, m<sup>3</sup>
-
-<span>\({\mathop m\limits^ \bullet_{_{air}}}\)</span>          = evaporative condenser air mass flow rate, kg/s
-
- <span>\({\omega_{evapcond,in}}\)</span>  = humidity ratio of outdoor air entering the evap condenser, kg/kg
-
-<span>\({\omega_{evapcond,out}}\)</span> = humidity ratio of air leaving the evap condenser, kg/kg
-
-<span>\({\rho_{water}}\)</span>         = density of water at the outdoor dry-bulb temperature, kg/m<sup>3</sup>
-
-*TimeStepSys* = HVAC system simulation time step, hr
-
-#### Condenser Inlet Air Temperature
-
-The air temperature entering the outdoor condenser is based on the weather data used during a simulation. This temperature is either taken directly from the weather data, or can be adjusted based on the height of the outdoor condenser. The input for Condenser Air Inlet Node Name can be used to control this optional feature. If this input is left blank, the air temperature entering the condenser is based solely on the weather data. If this input is not blank, then the node name specified must also be listed in an OutdoorAir:Node or OutdoorAir:NodeList object. When the node name is listed in an OutdoorAir:NodeList object, the air temperature entering the condenser is based solely on the weather data. When the node name is listed in an OutdoorAir:Node object, the height of the node determines the air temperature entering the outdoor condenser (see description of Local Outdoor Air Temperature Calculation in the Atmospheric Variation section of this document for further details).
-
-#### Supply Air Fan Control: Cycling vs. Continuous
-
-The DX cooling coil model simulates two specific supply air fan operation modes: cycling fan, cycling compressor or continuous fan, cycling compressor. The first operation mode is frequently referred to as “AUTO fan�, where the compressor(s) and supply air fan operate in unison to meet the zone cooling load, and cycle off together when the cooling load has been met. The second operation mode is often referred to as “fan ON�, where the compressor(s) cycle on and off to meet the zone cooling load but the supply air fan operates continuously regardless of compressor operation.
-
-Since this DX heating coil can only be used in conjunction with a DX cooling coil (i.e. heat pumps), and these coils are used in AC equipment that specifies a fan operation mode schedule (e.g AirLoopHVAC:UnitaryHeatPump:AirToAir), the fan operation mode schedule value determines the fan operation mode for each time step throughout the simulation. A fan operation mode schedule value of 0 specifies AUTO fan mode operation while values other than 0 (a 1 is usually used) specify fan ON operation. The use of a schedule allows the fan operation mode to change based on time-of-day or with changes in season.
-
-The EnergyPlus methodology for determining the impact that HVAC equipment has on an air stream is to calculate the mass flow rate and air properties (e.g., enthalpy, dry-bulb temperature, humidity ratio) exiting the equipment. These exiting conditions are passed along as inlet conditions to the next component model in the air stream. Eventually the flow rate and properties of the air being supplied to the conditioned zone are used in the zone energy balance to determine the resulting zone air temperature and humidity ratio. With this methodology, the determination of the air mass flow rate and air properties for the two different supply air fan operation modes is slightly different.
-
-Cycling Fan Mode:
-
-For the case of cycling fan/cycling compressor when humidity control is not specified, the conditions of the air leaving the cooling coil are the steady-state values calculated using equations (463), (465) and (466) above. However the air mass flow rate passed along to the next component (and eventually to the conditioned zone) is the average air mass flow rate for the system simulation time step (determined by the cooling system; see ZoneHVAC:WindowAirConditioner, AirLoopHVAC:Unitary:Furnace:HeatCool, AirLoopHVAC:UnitaryHeatCool, or AirLoopHVAC:UnitaryHeatPump:AirToAir).
-
-For the case of cycling fan/cyling compressor when humidity control is specified, the conditions of the air leaving the cooling coil are calculated as the average conditions during the fan operating period. When the compressor operates in tandem with the fan (i.e., compressor part-load ratio [PLR] is equal to the fan PLR), the outlet conditions are identical to the calculations described above. When the compressor operates for a shorter duration than the fan (i.e., the compressor PLR is less than the heating/fan PLR), the air properties leaving the cooling coil are calculated as the average conditions during the fan operating period. In this case the calculation of exiting air conditions is analogous to the calculations for continuous fan mode described below except that PLR in the equations represents the ratio of the compressor to the fan operating period. For cycling fan systems, the fan will only operate longer than the compressor, and therefore latent degradation may be modeled (user input), when humidity control is specified, a moisture load exists (i.e., the zone air humidistat senses a moisture load), and a heating load exists where the heating PLR is greater than the cooling PLR.
-
-Continuous Fan Mode:
-
-For the case of continuous fan/cycling compressor, the air mass flow rate is constant. However, the air properties leaving the cooling coil are calculated as the average conditions during the system simulation time step. The model assumes that the exiting air conditions are the steady-state values calculated using equations (463), (465) and (466) above when the compressor(s) operate.  For the remainder of the system simulation time step, it is assumed that the air exiting the DX coil has the same properties as the air entering the coil. For this supply air fan operating strategy, the leaving air properties are calculated as follows:
-
-<div>$${h_{out,ContFanCycComp}}\, = \,{h_{out}}\,\left( {PLR} \right) + \,{h_{in}}\,\,\left( {1 - PLR} \right)$$</div>
-
-<div>$${\omega_{out,ContFanCycComp}}\, = \,{\omega_{out}}\,\left( {PLR} \right) + \,{\omega_{in}}\,\,\left( {1 - PLR} \right)$$</div>
-
-<div>$${T_{db,out,ContFanCycComp}} = \,PsyTdbFnHW({h_{out,\,ContFanCycComp}}\,,\,\,\,\,\,{\omega_{out,ContFanCycComp}})$$</div>
-
-#### Latent Capacity Degradation
-
-The latent (dehumidification) capacity of a direct-expansion (DX) cooling coil is strongly affected by part-load, or cyclic, operation. This is especially true in applications where the supply air fan operates continuously while the cooling coil cycles on and off to meet the cooling load. During constant fan operation, moisture condenses on the cooling coil when the compressor operates, but part or all of the moisture that is held by the coil evaporates back into the airstream when the cooling coil is deactivated (Figure 168). The net effect is that the amount of moisture removed from the air is degraded at part-load conditions as compared to steady-state conditions when the compressor operates continuously (Figure 169).
-
-EnergyPlus is able to model latent capacity degradation based on algorithms developed by Henderson and Rengarajan (1996). The model is applicable to single-stage cooling units, like residential and small commercial air conditioners or heat pumps with less than 19 kW of nominal cooling capacity. The model inputs are described in the EnergyPlus Input/Output Reference for the object Coil:Cooling:DX:SingleSpeed. The model is enabled only if the four numerical inputs are defined (values greater than zero, see IO Reference).
-
-The following discussion applies to both cycling fan and continuous fan operation when the fan operates for a longer period of time than the compressor and air continues to flow over the moisture laden cooling coil after compressor operation has terminated.
-
-![](media/image3484.png)
-
-Figure 168.  Transient Sensible and Latent Capacity of a Cooling Coil Over an Operating Cycle
-
-
-
-![](media/image3485.png)
-
-Figure 169. Field Data Showing the Net Impact of Part-Load Operation on Sensible Heat Ratio
-
-
-
-![](media/image3486.png)
-
-
-
-Figure 170.  Concepts of Moisture Buildup and Evaporation
-
-Figure 170 graphically depicts the latent degradation concepts and defines several key model parameters. After the cooling coil starts to operate, the coil temperature is eventually reduced below the dewpoint temperature of the entering air. Moisture from the air then builds on the surface of the coil until time t<sub>o</sub> has elapsed and the total moisture mass on the coil is M<sub>o</sub>. After this time (t<sub>o</sub>), moisture begins to fall from the coil and all of the latent capacity provided by the coil is “useful� since this condensate is collected and removed from the unit. When the coil cycles off and the supply air fan continues to operate, the initial moisture mass buildup on the coil (M<sub>o</sub>) evaporates back into the supply air stream. If the cooling coil cycles back on before all of the moisture has evaporated, then the time until the first condensate removal (t<sub>o</sub>) is shorter for this cooling cycle since the coil is already partially wetted.
-
-Figure 170 also shows several parameters that are used in the latent degradation model. The ratio of the coil’s moisture holding capacity (M<sub>o</sub>) and the steady-state latent capacity (<span>\({\mathop Q\limits^ \bullet_L}\)</span>) is defined as *t<sub>wet</sub>* : the nominal time for moisture to fall from the coil (ignoring transient effects at startup and starting with a dry coil). The ratio of the initial moisture evaporation rate (<span>\({\mathop Q\limits^ \bullet_e}\)</span>) and the steady-state latent capacity (<span>\({\mathop Q\limits^ \bullet_L}\)</span>) is defined as <span>\(\gamma \)</span>. Both *t<sub>wet</sub>*and <span>\(\gamma \)</span> at the rated air volume flow rate and temperature conditions are required model inputs. Two other model inputs are the Maximum ON/OFF Cycling Rate (cycles per hour, *N<sub>max</sub>*) and the time constant (<span>\(\tau \)</span>, in seconds) for the cooling coil’s latent capacity to reach steady state after startup. The development of the latent degradation model is fully described by Henderson and Rengarajan (1996). The model implemented in EnergyPlus is for their “linear decay� evaporation model.
-
-During the simulation, all of the steady-state calculations described previously in equations (449) through (462) are completed. The latent degradation model then modifies the steady-state sensible heat ratio for the coil as shown below. The value of *t<sub>wet</sub>* at the current air volume flow rate and entering air conditions is first calculated based on the rated value of *t<sub>wet</sub>* entered by the user:
-
-<div>$${t_{wet}} = Minimum\left( {{t_{wet,rated}}\left( {\frac{{{{\mathop Q\limits^ \bullet  }_{latent,rated}}}}{{{{\mathop Q\limits^ \bullet  }_{latent}}}}} \right),\,\,{t_{wet,\max }}} \right)$$</div>
-
-where
-
-*t<sub>wet</sub>*  = nominal time for condensate removal to begin at the current airflow and entering air conditions, starting with a dry coil (sec)
-
-*t<sub>wet,rated</sub>* = nominal time for condensate removal to begin at the coil’s rated airflow and entering air conditions, starting with a dry coil (sec)
-
-<span>\({\mathop Q\limits^ \bullet_{latent,rated}}\)</span>= cooling coil latent capacity at the rated airflow and temperature conditions, W
-
-<span>\({\mathop Q\limits^ \bullet_{latent}}\)</span>= cooling coil latent capacity at the current airflow and temperature conditions, W
-
-*t<sub>wet,max</sub>* = maximum allowed value for *t<sub>wet</sub>* (9999.0 sec)
-
-
-
-Likewise, the value of <span>\(\gamma \)</span>at the current air volume flow rate and entering air conditions is calculated based on the rated value of <span>\(\gamma \)</span>entered by the user:
-
-<div>$$\gamma  = {\gamma_{rated}}\left( {\frac{{{{\mathop Q\limits^ \bullet  }_{latent,rated}}}}{{{{\mathop Q\limits^ \bullet  }_{latent}}}}} \right)\left( {\frac{{{T_{db,i}} - {T_{wb,i}}}}{{{T_{db,rated}} - {T_{wb,rated}}}}} \right)$$</div>
-
-where:
-
-<span>\(\gamma \)</span>         = ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil’s steady-state latent capacity (Watts) at the current air volume flow rate and entering air conditions
-
-<span>\({\gamma_{rated}}\)</span>   = <span>\(\gamma \)</span> at rated air flow and entering air conditions
-
-*T<sub>db,i</sub>*            = dry-bulb temperature of the air entering the cooling coil, °C
-
-*T<sub>wb,i</sub>*           = wet-bulb temperature of the air entering the cooling coil, °C
-
-*T<sub>db,rated</sub>* = dry-bulb temperature of air entering the cooling coil at rated conditions (26.7°C)
-
-*T<sub>wb,rated </sub>*= wet-bulb temperature of air entering the cooing coil at rated conditions (19.4°C)
-
-The cooling coil on and off times are then calculated based on the maximum number of cycles per hour and the calculated run-time fraction for the coil.
-
-<div>$${t_{on}} = \frac{{3600}}{{4{N_{\max }}\left( {1 - X} \right)}}$$</div>
-
-<div>$${t_{off}} = \frac{{3600}}{{4{N_{max}}X}}$$</div>
-
-where
-
-*t<sub>on</sub>*               = duration of cooling coil on-cycle (sec)
-
-*N<sub>max</sub>*            = maximum on/off cycles per hour (cph)
-
-*X*                = cooling coil runtime fraction (-)
-
-*t<sub>off</sub>*              = duration of cooling coil off-cycle (sec)
-
-
-
-For cycling fan systems, the duration of the heating coil on and off cycles are also calculated. When the heating coil operates for a longer duration of time than the cooling coil, latent degradation can also occur. For this case, the off-cycle time (i.e., the amount of time the fan operates longer than the cooling coil) is recalculated and based on the difference between the heating coil on-cycle time and the cooling coil on-cycle time. Ton and Toff for the heating coil are calculated in the same manner as shown above except that the heating run-time fraction is used for the calculations. This model assumes that the cycling rate of the cooling and heating coils are the same. In addition, since the heating coil cycling rate may be different than the cooling coil (based on run-time fractions), the heating coil may also turn on again before the next cooling coil on-cycle. The following equations are used when the heating coil operates for a longer time period than does the cooling coil.
-
-<div>$$ton,heating = \frac{{3600}}{{4Nmax\left( {1 - Xheating} \right)}}$$</div>
-
-<div>$$toff,heating = \frac{{3600}}{{4Nmax\left( {Xheating} \right)}}$$</div>
-
-<div>$$ton,heating = ton,heating + MAX\left( {0,MIN\left( {ton,heating,\left( {\left( {ton + toff} \right) - \left( {ton,heating + toff,heating} \right)} \right)} \right)} \right)$$</div>
-
-<div>$$toff = MIN\left( {toff,ton,heating - ton} \right)$$</div>
-
-where
-
-*t<sub>on,heating</sub>*      = duration of heating coil on-cycle (sec)
-
-*X<sub>,heating</sub>*        = heating coil runtime fraction (-)
-
-*t<sub>off,heating</sub>*      = duration of heating coil off-cycle (sec)
-
-
-
-The equation for calculating the time *t<sub>o</sub>* when moisture first begins to fall from the cooling coil is shown below, and is solved iteratively by EnergyPlus:
-
-<div>$$\mathop t\nolimits_o^{j + 1}  = \gamma {t_{off}} - \left( {\frac{{\mathop \gamma \nolimits^2 }}{{4{t_{wet}}}}} \right)\mathop t\nolimits_{off}^2  - \tau \left( {\mathop e\nolimits^{\frac{{\mathop t\nolimits_o^j }}{\tau }} \,\, - \,\,1} \right)\,\,,\,\,\,\mathop t\nolimits_{off}^{}  \le \,\left( {\frac{{2{t_{wet}}}}{\gamma }} \right)$$</div>
-
-where
-
-<span>\({t_o}\)</span>  = time where condensate removal begins (sec)
-
-<span>\(\tau \)</span>   = latent capacity time constant at start-up (sec)
-
-*j*     = iteration number
-
-The part-load latent heat ratio of the cooling coil is then calculated with <span>\(t_o^{}\)</span>, *t<sub>on</sub>* and <span>\(\tau \)</span>, which is in turn used to calculate the “effective� sensible heat ratio of the cooling including part-load latent degradation effects.
-
-<div>$$\frac{{LHR}}{{LH{R_{ss}}}} = Maximum\left( {\left( {\frac{{{t_{on}} - {t_o}}}{{{t_{on}} + \tau \left( {{e^{\left( {\frac{{ - {t_{on}}}}{\tau }} \right)}}\,\, - \,\,1} \right)}}} \right),0.0} \right)$$</div>
-
-<div>$$SH{R_{eff}} = 1 - \left( {1 - SH{R_{ss}}} \right)\left( {\frac{{LHR}}{{LH{R_{ss}}}}} \right)$$</div>
-
-where
-
-<span>\(LHR\)</span> = part-load latent heat ratio
-
-<span>\(LH{R_{ss}}\)</span> = latent heat ratio at steady-state conditions (<span>\(1 - SH{R_{ss}}\)</span> with <span>\(SH{R_{ss}}\)</span> from eqn. (462))
-
-<span>\(SH{R_{eff}}\)</span> = part-load sensible heat ratio**(<span>\(SH{R_{ss}}\)</span>* ≤<span>\(SH{R_{eff}}\)</span> ≤* 1.0)
-
-<span>\(SH{R_{ss}}\)</span> = steady-state sensible heat ratio (from eqn. (462))
-
-With the “effective� SHR for the coil at the current operating conditions, including the impacts of latent degradation, equations (463) through (466) are then used to calculate the properties of the air leaving the cooling coil when it operates. Finally, equations (467) through (469) are used to calculate the average leaving air conditions (average when the coil is on and off) for the simulation time step.
-
-#### Basin Heater For Single-Speed DX Coil
-
-Calculations are also made to estimate the electric power input to the DX coil basin heater. A schedule may be used to disable the basin heater during regular maintenance periods or other time periods (e.g., during summer). If a schedule is not provided, the basin heater is assumed to be available the entire simulation time period. The basin heater operates when it is scheduled on, the outdoor air dry-bulb temperature is below the basin heater setpoint temperature, and the DX coil is not active. The user is required to enter a basin heater capacity (watts per degree Kelvin) and a heater setpoint temperature (<sup>o</sup>C) if they want to model basin heater electric power.
-
-<div>$$
-  \mathop P\nolimits_{basinheater}  = MAX(0.0,{\rm{ }}\mathop {CAP}\nolimits_{basinheater} (\mathop T\nolimits_{setpoint,basin}  - \mathop T\nolimits_{db,outdoor} )(1 - RTF)) \\ 
-$$</div>
-
-<div>$$
-  \mathop E\nolimits_{basinheater}  = \mathop {(P}\nolimits_{basinheater} )(TimeStepSys)3600
-$$</div>
-
-where:
-
-<span>\(\mathop P\nolimits_{basinheater} \)</span>             = DX coil basin heater electric power (W)
-
-<span>\(\mathop E\nolimits_{basinheater} \)</span>            = DX coil basin heater electric consumption (J)
-
-<span>\(\mathop T\nolimits_{setpoint,basin} \)</span>           = Basin heater setpoint temperature (<sup>o</sup>C)
-
-<span>\(\mathop T\nolimits_{db,outdoor} \)</span>              = Outdoor air dry-bulb temperature (<sup>o</sup>C)
-
-<span>\(\mathop {CAP}\nolimits_{basinheater} \)</span>         = Basin heater capacity (W/K)
-
-<span>\(RTF\)</span>                        = Run time fraction of DX cooling coil
-
-#### Special Calculations for Coil:Cooling:DX:TwoStageWithHumidityControlMode with CoilPerformance:DX:Cooling
-
-The multimode DX coil uses 1 to 4 set of performance specifications which all feed into the main DX coil model as described above. The multimode DX coil may have 1 or 2 capacity stages and may have 1 enhanced dehumidification mode in addition to its "normal" or base mode performance. Any mode may specify that a portion of the total airflow is bypassed.
-
-##### Bypass Operation
-
-When a mode has coil bypass, the non-bypassed air flow fraction is used to model the DX coil performance as described above. Then the bypassed air stream is mixed with the conditioned air stream and these conditions are place on the coil outlet node.
-
-##### Multi-Stage Operation
-
-Multi-stage control is modeled with the DX coil. If 2-stage operation has been specified, stage 1 is assumed to operate first and continue to operate if stage 2 is required. If latent degradation is active, only one of the stages will be degraded. If stage 1 operates for less than the full time step, then latent degradation is applied. If stage 2 operates, then stage 1 is running for the full time step and latent degradation is applied only to the portion of the latent load which is attributed to stage 2 operation.
-
-##### Enhanced Dehumidification Mode
-
-If enhanced dehumidification mode is available, this is controlled by the parent object of the DX coil, such as DXSystem:AirLoop. A dehumidification mode flag is passed to the coil model which is used to select a different set of performance specifications from a CoilPerformance:DX:Cooling input object. Then the simulation of the DX coil proceeds as described above including any bypass or multi-stage operation.
-
-#### Standard Rating of Single-Speed DX Cooling Coils
-
-For small single-speed direct expansion (DX) cooling coils, the industry standard ratings of Standard Rating Cooling Capacity and Seasonal Energy Efficiency Ratio (SEER) are calculated according to ANSI/AHRI Standard 210/240 (AHRI 2008). These ratings apply to unitary air conditioners and air-source unitary heat pumps with air-cooled condensers with standard rating cooling capacities under 19 kW (&lt;65,000 Btu/hr). For larger DX cooling coils, the industry standard ratings of Standard Rating Cooling Capacity, Energy Efficiency Ratio (EER), and Integrated Energy Efficiency Ratio (IEER) are calculated according to ANSI/AHRI Standard 340/360 (AHRI 2007). These ratings apply to unitary air conditioners and air-source unitary heat pumps with standard rating cooling capacities from 19 kW to below 73.2 kW (65,000 Btu/hr to &lt;250,000 Btu/hr).
-
-For the Coil:Cooling:DX:SingleSpeed object in EnergyPlus, these standard ratings are not direct inputs to the model. However, these standard ratings can be calculated using user-entered information for the Coil:Cooling:DX:SingleSpeed object. Since users sometimes lump the performance of several smaller DX cooling units into a single larger cooling coil object for simulation purposes, EnergyPlus outputs the Standard Rating Cooling Capacity, SEER, EER, and IEER regardless of the magnitude of the standard rating cooling capacity of the coil. It is up to the user to determine which standard ratings are applicable to the cooling coil(s) they are modeling. These standard rating values are provided in the eplusout.eio output file (Ref. OutputDetailsAndExamples.pdf) and also in the predefined tabular output reports (Output:Table:SummaryReports object, Equipment Summary). Currently, the standard ratings are only calculated and output for single-speed DX cooling coils with air-cooled condensers. If the single-speed DX coling coil is specified with an evaporatively-cooled condenser, then no standard ratings are output from EnergyPlus at this time.
-
-Note: The standard ratings described in this section require that the DX cooling coil model be evaluated at specific operating conditions (i.e., specific wet-bulb temperatures for air entering the cooling coil and dry-bulb temperatures for air entering the air-cooled [outdoor] condenser). If the cooling coil performance curves can not be evaluated at the required test conditions, then a standard rating value calculated at the curves limit will be output and a warning message will written to eplusout.err. For example, if the curve object (Curve:Biquadratic) for Total Cooling Capacity Function of Temperature Curve has a minimum value of 21C for dry-bulb temperature entering the air-cooled condenser coil, the IEER calculation requires that EER<sub>D</sub> be calculated at 18.3C – so, this would result in IEER calculatd at user specified curve limit as an output and a warning message in the eplusout.err file.
-
-The standard rating cooling capacity (AHRI 2007, AHRI 2008) is calculated as follows:
-
-<div>$$\begin{array}{l}{{\dot Q}_{StandardRating}} = \,\,{{\dot Q}_{Total,Rated}}\left( {TotCapTempModFa{c_{Rated}}} \right)\left( {TotCapFlowModFa{c_{Rated}}} \right)\,\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, - \,\left( {FanPowerPerVolFlowRate \cdot {{\dot V}_{Rated}}} \right)\end{array}$$</div>
-
-where,
-
-<span>\({\dot Q_{StandardRating}}\)</span> = Standard Rating (Net) Cooling Capacity (W)
-
-<span>\({\dot Q_{Total,Rated}}\)</span> = Rated Total (Gross) Cooling Capacity, user input (W)
-
-<span>\(TotCapTempModFa{c_{Rated}}\)</span>= Total Cooling Capacity Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
-
-<span>\(TotCapFlowModFa{c_{Rated}}\)</span>= Total Cooling Capacity Function of Flow Fraction Curve evaluated at a flow fraction of 1.0 (dimensionless)
-
-<span>\(FanPowerPerVolFlowRate\)</span>= Rated Evaporator Fan Power Per Volume Flow Rate, user input ( W/(m<sup>3</sup>/s) )
-
-<span>\({\dot V_{Rated}}\)</span>= Rated Air Volume Flow Rate, user input (m<sup>3</sup>/s)
-
-The Rated Evaporator Fan Power Per Volume Flow rate is a user-entered value, with a default of 773.3 W/(m<sup>3</sup>/s)) if the user leaves this input field blank. The default value is taken from ANSI/AHRI Standards 210/240 and 340/360 where it is defined for systems which do not have a cooling coil fan furnished as part of the system (e.g., a DX cooling coil mounted in the ductwork downstream of a gas furnace where the furnace contains the fan used for air distribution across the gas heating coil and the downstream DX cooling coil). The test conditions in ANSI/AHRI Standards 210/240 and 340/360 vary the external static pressure (i.e., pressure drop associated with ductwork and other devices external to the indoor fan/coil section) seen by the supply air fan based on the standard rating cooling capacity. Note, however, that external static pressure in actual installations is typically much higher. Further details regarding indoor fan power per volume flow rate can be found in Walker and Lutz (2005) and Walker (2007), including differences between Permanent Split Capacitor (PSC) and Brushless Permanent Magnet (BPM) fan motors. Especially at the low external static pressures defined in the ANSI/AHRI Standards, BPM motors (e.g., Electronically Commutated Motors (ECMs)) can draw significantly less power (e.g., 50-75% less) than PSC motors.
-
-The seasonal energy efficiency ratio (SEER) is calculated as follows:
-
-<div>$$SEER = PL{F_{0.5}} \cdot EE{R_{TestB}}$$</div>
-
-<div>$$EE{R_{TestB}} = \frac{{{{\dot Q}_{Total,Net,TestB}}}}{{Powe{r_{Total,TestB}}}}$$</div>
-
-<div>$$\begin{array}{l}{{\dot Q}_{Total,Net,TestB}} = {{\dot Q}_{Total,Rated}}(TotCapTempModFa{c_{TestB}})(TotCapFlowModFa{c_{Rated}})\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, - \,\,\left( {FanPowerPerVolFlowRate \cdot {{\dot V}_{Rated}}} \right)\end{array}$$</div>
-
-<span>\(\begin{array}{l}Powe{r_{Total,TestB}} = \left( {{{\dot Q}_{Total,Rated}}(TotCapTempModFa{c_{TestB}})(TotCapFlowModFa{c_{Rated}})} \right)\, \cdot EI{R_{TestB}}\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + \,\,\left( {FanPowerPerVolFlowRate \cdot {{\dot V}_{Rated}}} \right)\end{array}\)</span><span>\(EI{R_{TestB}} = \left( {\frac{1}{{CO{P_{rated}}}}} \right)(EIRTempModFa{c_{TestB}})(EIRFlowModFa{c_{Rated}})\)</span>
-
-where,
-
-*PLF<sub>0.5</sub>*  =    Part Load Fraction Correlation Curve evaluated at a part load ratio (PLR) of 0.5 (dimensionless)
-
-*EER<sub>TestB</sub>*<sub></sub> = Energy efficiency ratio with 19.44°C wet-bulb temperature air entering the cooling coil, 27.78°C dry-bulb temperature air entering the air-cooled (outdoor) condenser, and rated air volume flow through the cooling coil (W/W)
-
-<span>\({\dot Q_{Total,Net,TestB}}\)</span>= Net total cooling capacity with 19.44°C wet-bulb temperature air entering the cooling coil, 27.78°C dry-bulb temperature air entering the air-cooled (outdoor) condenser, and rated air volume flow through the cooling coil (W)
-
-<span>\(TotCapTempModFa{c_{TestB}}\)</span> = Total Cooling Capacity Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 27.78°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
-
-<span>\(Powe{r_{Total,TestB}}\)</span> = Total electric power (compressors, condenser fans and evaporator fan) with 19.44°C wet-bulb temperature air entering the cooling coil, 27.78°C dry-bulb temperature air entering the air-cooled (outdoor) condenser, and rated air volume flow through the cooling coil (W)
-
-<span>\(CO{P_{rated}}\)</span> = Coefficient of Performance at Rated Conditions, user input (W/W)
-
-<span>\(EIRTempModFa{c_{TestB}}\)</span> = Energy Input Ratio Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 27.78°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
-
-<span>\(EIRFlowModFa{c_{Rated}}\)</span>= Energy Input Ratio Function of Flow Fraction Curve evaluated at a flow fraction of 1.0 (dimensionless).
-
-Energy Efficiency Ratio (EER) is another standard rating (AHRI 2007), and it is defined as the ratio of the total cooling capacity to the total power input at any given set of rating conditions, expressed in W/W (or Btu/W-h). For this class of air-cooled DX cooling coils, EER is calculated at rated test conditions as follows:
-
-<div>$$EE{R_{}} = \frac{{{{\dot Q}_{Standard\,Rating}}}}{{Powe{r_{Total,Rated}}}}$$</div>
-
-<div>$$\begin{array}{l}Powe{r_{Total,Rated}} = \left( {{{\dot Q}_{Total,Rated}}(TotCapTempModFa{c_{Rated}})(TotCapFlowModFa{c_{Rated}})} \right)\, \cdot EI{R_{Rated}}\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + \,\,\left( {FanPowerPerVolFlowRate \cdot {{\dot V}_{Rated}}} \right)\end{array}$$</div>
-
-<div>$$EI{R_{Rated}} = \left( {\frac{1}{{CO{P_{Rated}}}}} \right)(EIRTempModFa{c_{Rated}})(EIRFlowModFa{c_{Rated}})$$</div>
-
-where,
-
-*EER*  = Energy Efficiency Ratio (W/W)
-
-<span>\(Powe{r_{Total,Rated}}\)</span>= Total electric power (compressors, condenser fans and evaporator fan) with 19.44°C wet-bulb temperature air entering the cooling coil, 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser, and air flow rate across the evaporator at the Rated Air Volume Flow Rate (W).
-
-<span>\(TotCapTempModFa{c_{Rated}}\)</span> = Total Cooling Capacity Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
-
-<span>\(EIRTempModFa{c_{Rated}}\)</span> = Energy Input Ratio Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
-
-The Integrated Energy Efficiency Ratio (IEER) is intended to be a measure of merit for the cooling coil’s part-load efficiency. IEER replaced Integrated Part-Load Value (IPLV) as the part-load performance metric in Std. 340/360 as of January 1, 2010. Full details regarding the IEER calculation are available in ANSI/AHRI Std. 340/360 (AHRI 2007). A summary of the IEER calculations made by EnergyPlus for single-speed air-cooled DX cooling coils is provided below:
-
-<div>$$IEER = \,(0.02 \cdot EE{R_A}) + (0.617 \cdot EE{R_B}) + (0.238 \cdot EE{R_C}) + (0.125 \cdot EE{R_D})$$</div>
-
-where,
-
-<span>\(EE{R_A}\)</span> =     *EER* at 100% net capacity at AHRI standard rating conditions (same as EER calculation shown above)
-
-<span>\(EE{R_B}\)</span> =     *EER* at 75% net capacity and reduced outdoor air temperature
-
-<span>\(EE{R_C}\)</span> =     *EER* at 50% net capacity and reduced outdoor air temperature
-
-<span>\(EE{R_D}\)</span>=      *EER* at 25% net capacity and reduced outdoor air temperature
-
-<div>$$EE{R_{B - D}} = \frac{{LF \cdot {{\dot Q}_{Total,Net,PartLoad}}}}{{Powe{r_{Total,{\kern 1pt} PartLoad}}}}$$</div>
-
-<div>$$Powe{r_{Total,{\kern 1pt} PartLoad}} = LF\left( {{C_D} \cdot Powe{r_{CompCondFan,{\kern 1pt} PartLoad}}} \right) + \,\left( {FanPowerPerVolFlowRate \cdot {{\dot V}_{Rated}}} \right)$$</div>
-
-<div>$$\begin{array}{l}Powe{r_{CompCondFan,{\kern 1pt} PartLoad}} = \left( {{{\dot Q}_{Total,Rated}}(TotCapTempModFa{c_{PartLoad}})(TotCapFlowModFa{c_{Rated}})} \right)\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, \cdot EI{R_{PartLoad}}\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\end{array}$$</div>
-
-<div>$$EI{R_{PartLoad}} = \left( {\frac{1}{{CO{P_{Rated}}}}} \right)(EIRTempModFa{c_{PartLoad}})(EIRFlowModFa{c_{Rated}})$$</div>
-
-where,
-
-<span>\({\dot Q_{Total,Net,PartLoad}}\)</span> =     Net total cooling capacity with 19.44°C wet-bulb temperature air entering the cooling coil rated air volume flow through the cooling coil (W). The dry-bulb temperature of air entering the air-cooled condenser varies (B = 27.5°C, C = 20.0°C, D = 18.3°C).
-
-<span>\(Powe{r_{Total,PartLoad}}\)</span> = Total electric power (compressors, condenser fans and evaporator fan) with 19.44°C wet-bulb temperature air entering the cooling coil and air flow rate across the evaporator at the Rated Air Volume Flow Rate (W). The dry-bulb temperature of air entering the air-cooled condenser varies (B = 27.5°C, C = 20.0°C, D = 18.3°C).<span>\(Powe{r_{CompCondFan,{\kern 1pt} PartLoad}}\)</span> = Electric power of the compressor and condenser fan at the various part-load ratios, with 19.44°C wet-bulb temperature air entering the cooling coil and rated supply air volume flow rate (W). The dry-bulb temperature of air entering the air-cooled condenser varies per the part-load ratio (B = 27.5°C, C = 20.0°C, D = 18.3°C).
-
-<span>\(EIRTempModFa{c_{PartLoad}}\)</span> = Energy Input Ratio Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and dry-bulb temperature of air entering the air-cooled condenser corresponding to the reduced part-load ratio (B = 27.5°C, C = 20.0°C, D = 18.3°C) (dimensionless).
-
-<span>\({C_D}\)</span>= degradation coefficient to account for cycling of the compressor = 1.13 – 0.13*LF*.
-
-<span>\(LF\)</span> = fractional “on� time at the desired load point
-
-The load factor (*LF*) is the fractional “on� time for the desired reduced load points (75%, 50%, or 25%) calculated from the following equation:
-
-<div>$$LF = \frac{{\left( {{\raise0.7ex\hbox{${\% Load}$} \!\mathord{\left/ {\vphantom {{\% Load} {100}}}\right.}\!\lower0.7ex\hbox{${100}$}}} \right) \cdot {{\dot Q}_{StandardRating}}}}{{{{\dot Q}_{Total,Net,PartLoad}}}}$$</div>
-
-where,
-
-*<span>\(\% Load\)</span>* = Part-load operating points, i.e., 75% (B), 50% (C), 25% (D)
-
-The calculations for *Q<sub>Total,Net,PartLoad</sub>* and *Power<sub>Total,PartLoad</sub>* are calculated in nearly the same way as *Q<sub>Total,Net,TestB</sub>* and *Power<sub>Total,TestB</sub>* are calculated for SEER (defined above). The only difference is that these cooling capacity and power values, used for calculating EER<sub>B</sub>/EER<sub>C</sub>/EER<sub>D</sub> for IEER, are calculated for a series of dry-bulb temperatures of air entering the air-cooled condenser (B = 27.5°C, C = 20.0°C, D = 18.3°C) and part-load performance degradiation correction is also applied to the condensing unit electric power calculation.
-
-#### ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils
-
-For computer and data processing room unitary air conditioners single-speed direct expansion (DX) cooling coils, the standard ratings net total cooling capacity and total cooling electric power inputs are calculated according to ANSI/AHRI Standard 127 (ASHRAE 2012). These ratings apply to unitary air conditioners with air-cooled. If the single-speed DX cooling coil is specified with an evaporatively-cooled condenser, then no standard ratings are output from EnergyPlus at this time. These standard ratings are not direct inputs to the model. However, these standard ratings can be calculated using user-entered information for the Coil:Cooling:DX:SingleSpeed object.  These standard rating values are provided in the eplusout.eio output file and also in the predefined tabular output reports (Output:Table:SummaryReports object, Equipment Summary). 
-
-**Note**: The standard ratings described in this section require that the DX cooling coil model be evaluated at sixteen different test conditions (i.e., specific wet-bulb temperatures for air entering the cooling coil and dry-bulb temperatures for air entering the air-cooled [outdoor] condenser) for each of the four standard tests and four application classes (ASHRAE – 2012).  The four test conditions: A, B, C and D are provided in the ANSI/ASHRAE Standard 127. And the test conditions are different for each application classes described in the standard.  In total sixteen performance data of net cooling capacity and total electric power inputs are reported.  The total cooling electric power includes the supply fan power.
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="6">Rated Cooling Tests</th>
-  </tr>
-  <tr>
-    <th></th>
-    <th>Application Class</th>
-    <th>A</th>
-    <th>B</th>
-    <th>C</th>
-    <th>D</th>
-  </tr>
-  <tr>
-    <td rowspan="4">Tdb, Indoor</td>
-    <td>Class 1</td>
-    <td>23.9&deg;C(75.0&deg;F)</td>
-    <td>23.9&deg;C(75.0&deg;F)</td>
-    <td>23.9&deg;C(75.0&deg;F)</td>
-    <td>23.9&deg;C(75.0&deg;F)</td>
-  </tr>
-  <tr>
-    <td>Class 2</td>
-    <td>29.4&deg;C(85.0&deg;F)</td>
-    <td>29.4&deg;C(85.0&deg;F)</td>
-    <td>29.4&deg;C(85.0&deg;F)</td>
-    <td>29.4&deg;C(85.0&deg;F)</td>
-  </tr>
-  <tr>
-    <td>Class 3</td>
-    <td>35.0&deg;C(95.0&deg;F)</td>
-    <td>35.0&deg;C(95.0&deg;F)</td>
-    <td>35.0&deg;C(95.0&deg;F)</td>
-    <td>35.0&deg;C(95.0&deg;F)</td>
-  </tr>
-  <tr>
-    <td>Class 4</td>
-    <td>40.5&deg;C(105&deg;F)</td>
-    <td>40.5&deg;C(105&deg;F)</td>
-    <td>40.5&deg;C(105&deg;F)</td>
-    <td>40.5&deg;C(105&deg;F)</td>
-  </tr>
-  <tr>
-    <td colspan="2">Tdp, Indoor</td>
-    <td>35.0&deg;C(95.0&deg;F)</td>
-    <td>26.7&deg;C(80.0&deg;F)</td>
-    <td>18.3&deg;C(65.0&deg;F)</td>
-    <td>4.4&deg;C(40.0&deg;F)</td>
-  </tr>
-  <tr>
-    <td colspan="2">Tdb, Outdoor</td>
-    <td>35.0&deg;C(95.0&deg;F)</td>
-    <td>26.7&deg;C(80.0&deg;F)</td>
-    <td>18.3&deg;C(65.0&deg;F)</td>
-    <td>4.4&deg;C(40.0&deg;F)</td>
-  </tr>
-</table>
-
-The standard rating net total cooling capacity is calculated as follows:
-
-<div>$$ \dot{Q}_{StandardRating} = \dot{Q}_{TotalRated}\left(\text{TotCapTempModFac}_{Rated}\right)\left(\text{TotCapFlowModFac}_{Rated}\right)-\left(\text{FanPowerPerVolFlowRate} \cdot \dot{V}_{Rated}\right) $$</div>
-
-where:
-
-* <span>\(\dot{Q}_{StandardRating} \)</span> = Standard Rating (Net) Cooling Capacity (W)
-
-* <span>\(\dot{Q}_{Total,Rated} \)</span> = Rated Total (Gross) Cooling Capacity, user input (W)
-
-* <span>\(\text{TotCapTempModFac}_{Rated} \)</span> = Total Cooling Capacity Function of Temperature Curve evaluated at wet-bulb temperature of air entering the cooling coil and dry-bulb temperature of air entering the air-cooled (outdoor) condenser (dimensionless)
-
-* <span>\(\text{TotCapFlowModFac}_{Rated} \)</span> = Total Cooling Capacity Function of Flow Fraction Curve evaluated at a flow fraction of 1.0 (dimensionless)
-
-* <span>\(\text{FanPowerPerVolFlowRate} \)</span> = Rated Evaporator Fan Power Per Volume Flow Rate, user input ( W/(m3/s) )
-
-* <span>\(\dot{V}_{Rated} \)</span> = Rated Air Volume Flow Rate, user input (m3/s)
-
-The standard rating net total cooling electric power input is calculated as follows:
-
-<div>$$ \text{Power}_{Total} = \left[\dot{Q}_{Total,Rated}\left(\text{TotCapTempModFac}\right)\left(\text{TotCapFlowModFac}_{Rated}\right)\right]\cdot\text{EIR}+\left(\text{FanPowerPerVolFlowRate}\cdot\dot{V}_{Rated}\right) $$</div>
-
-<div>$$ \frac{\text{EIRTempModFac}\text{EIRFlowModFac_{Rated}}}{COP_{Rated}} $$</div>
-
-where:
-
-* <span>\(EER \)</span> = Energy efficiency ratio at wet-bulb temperature of air entering the cooling coil, dry-bulb temperature of air entering the air-cooled (outdoor) condenser, and rated air volume flow through the cooling coil (W/W)
-
-* <span>\(\text{TotCapTempModFac} \)</span> = Total Cooling Capacity Function of Temperature Curve evaluated at the test condition of wet-bulb temperature of air entering the cooling coil and dry-bulb temperature of air entering the air-cooled (outdoor) condenser (dimensionless)
-
-* <span>\(\text{Power}_{Total} \)</span> = Total electric power (compressors, condenser fans and evaporator fan) at the test conditions of wet-bulb temperature of air entering the cooling coil, and dry-bulb temperature of air entering the air-cooled (outdoor) condenser, and rated air volume flow through the cooling coil (W)
-
-* <span>\(COP_{Rated} \)</span> = Coefficient of Performance at Rated Conditions, user input (W/W)
-
-* <span>\(\text{EIRTempModFac} \)</span> = Energy Input Ratio Function of Temperature Curve evaluated at the test condition of wet-bulb temperature of air entering the cooling coil and dry-bulb temperature of air entering the air-cooled (outdoor) condenser (dimensionless)
-
-* <span>\(\text{EIRFlowModFac}_{Rated} \)</span> = Energy Input Ratio Function of Flow Fraction Curve evaluated at a flow fraction of 1.0 (dimensionless).
-
-Reference:
-
-ASHRAE 2012. ANSI/ASHRAE Standard 127-2012 Method of Testing for Rating Computer and Data Processing Room Unitary Air Conditioners.
-
-#### Basin Heater For Two-Stage DX Coil
-
-Basin heater for the object Coil:Cooling:DX:TwoStageWithHumidityControlMode operates in the same manner as for Coil:Cooling:DX:SingleSpeed. Refer to the “Basin Heater For Single-Speed DX Coil� description above.
-
-If the number of capacity stages is equal to 1 and the CondenserType for that stage is EvapCooled, then the basin heater power is calculated for (1 - RunTimeFractionStage1) of DX coil.
-
-If the number of capacity stages is greater than 1, then
-
-1)   If the CondenserType for stage 1 is EvapCooled, then the basin heater power is calculated for (1 - RunTimeFractionStage1) of DX coil
-
-2)   Elseif the CondenserType for stage 2 is EvapCooled, then the basin heater power is calculated for (1 - RunTimeFractionStage2) of DX coil
-
-#### References
-
-AHRI 2008. ANSI/AHRI Standard 210/240: 2008 Standard for Performance Rating of Unitary Air-Conditioning & Air-Source Heat Pump Equipment.  Arlington, VA:  Air-Conditioning, Heating, and Refrigeration Institute.
-
-AHRI 2007. ANSI/AHRI Standard 340/360: 2007 Standard for Performance Rating of Commercial and Industrial Unitary Air-Conditioning and Heat Pump Equipment.  Arlington, VA:  Air-Conditioning, Heating, and Refrigeration Institute.
-
-ASHRAE. 1993. HVAC2 Toolkit: A Toolkit for Secondary HVAC System Energy Calculation. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Carrier, W.H., R.E. Cherne, W.A. Grant, and W.H. Roberts. 1959. *Modern air conditioning, heating and ventilating*, 3d ed. New York: Pitman Publishing Corporation.
-
-Henderson, H.I. Jr., K. Rengarajan, and D.B. Shirey III. 1992. The impact of comfort control on air conditioner energy use in humid climates. *ASHRAE Transactions* 98(2): 104-113.
-
-Henderson, H.I. Jr. and K. Rengarajan. 1996. A Model to Predict the Latent Capacity of Air Conditioners and Heat Pumps at Part-Load Conditions with Constant Fan Operation. *ASHRAE Transactions* 102(2): 266-274.
-
-Henderson, H. 1998. The impact of part load air conditioner operation on dehumidification performance: Validating a latent capacity degradation model. Presented at ASHRAE’s IAQ & Energy ‘98 conference. New Orleans, LA.  October.
-
-Henderson, H. and D. Shirey. 2003. Understanding the Dehumidification Performance of Air-Conditioning Equipment at Part-Load Conditions. Paper presented at Joint CIBSE/ASHRAE Conference, *Building Sustainability, Value and Profit.* September.  Edinburgh, Scotland.
-
-Walker, I.S. and Lutz, J.D. 2005. Laboratory Evaluation of Residential Furnace Blower Performance. Berekely, CA:  Lawrence Berkeley National Laboratory, Report LBNL 58752.
-
-Walker, I.S. 2007. Comparing Residential Furnace Blowers for Rating and Installed Performance. Berkeley, CA:  Lawrence Berkeley National Laboratory, Environmental Energy Technologies Division Report LBNL 62344.
-
-### Multi-Speed Electric DX Air Cooling Coil
-
-#### Overview
-
-This model (object name Coil:Cooling:DX:MultiSpeed) simulates the performance of an air-to-air direct expansion (DX) cooling system. The main difference compared to the other cooling coil models, such as Coil:Cooling:DX:SingleSpeed, is that this cooling coil allows modeling of two to four discrete compressor speeds. Each speed has a set of corresponding performance information at rated conditions along with curve fits for variations in total capacity, SHR, energy input ratio and part-load fraction to determine the performance of the unit at part-load conditions (DOE 1982).  The full load supply airflow rate is dependent on the speed number and provided by its parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed). The part-load impact on coil energy use is automatically applied to the lowest speed. A choice is provided to determine whether part-load impacts on coil energy use are applied when the coil is operating at speeds greater than speed 1.
-
-This model simulates the thermal performance of the indoor DX cooling coil, and the power consumption of the outdoor unit (multispeed compressor, fans, and crankcase heaters). The performance of the indoor supply air fan varies widely from system to system depending on control strategy (e.g., constant fan vs. AUTO fan), fan type, fan motor efficiency and pressure losses through the air distribution system. Therefore, this DX system model does not account for the thermal effects or electric power consumption of the indoor supply air fan. EnergyPlus contains separate models for simulating the performance of various indoor fan configurations, and these models can be easily linked with the DX system model described here to simulate the entire DX system being considered. For the time being, this coil model can only be called by the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
-
-When the model determines performance at Speed 1 (the lowest speed) or cycling between OFF and Speed 1, its performance is almost the same as the performance for the Coil:Cooling:DX:SingleSpeed model. However, the outlet conditions are calculated slightly differently. Therefore, the Coil:Cooling:DX:SingleSpeed model may be considered as a subset of the model described here. When the multispeed coil model determines performance at higher speeds (above 1), the model linearly interpolates the performance at two consecutive speeds (n-1 and n) as needed to meet the cooling load, with the fraction of time at each speed established by the speed ratio.
-
-When single mode operation is specified at higher speeds (above 1), defined in the UnitarySystemPerformance:Multispeed object, a child object of AirLoopHVAC:UnitarySystem, its performance is almost the same as the performance for the Coil:Cooling:DX:SingleSpeed model at different flow rate and capacity with given speed number. No linear interpolation is performed between two adjacent speeds. The highest speed which does not exceed the sensible load is used for each HVAC timestep. This operation does not apply to speed 1 operation and the case when the sensible load is above the highest sensible capacity.
-
-#### Model Inputs
-
-The model inputs are also very similar to the inputs of the Coil:Cooling:DX:SingleSpeed object. The main difference is that this multispeed model requires a set of fields at each speed, such as rated capacity, rated SHR, rated COP, two capacity modifiers, two energy input ratio modifiers, part-load correction, and latent degradation inputs. The inputs also include waste heat fraction at the rated conditions and modifier as a function of temperature to calculate recoverable waste heat for heat recovery, which are not available in the similar Coil:Cooling:DX:SingleSpeed object
-
-#### Speed 1 Operation
-
-The calculation procedures in this model, including defrost and crankcase heater, are indentical to the Coil:Heating:DX:SingleSpeed object (Ref: Coil:Heating:DX:SingleSpeed) with one exception: outlet node condition calculation when the supply air fan operates continuously (i.e., supply air fan operating mode schedule value is not equal to 0; Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed).
-
-The following procedure provides the detailed description of the exception.
-
-n Total delivered cooling capacity
-
-The total delivered cooling capacity for speed 1 operating at the cycling ratio needed to meet the requested cooling load is:
-
-<div>$${Q_{coil,cycling}} = {\mathop m\limits^\cdot_{Speed1}}*CycRatio*({h_{inlet}} - {h_{outlet,full}})$$</div>
-
-where,
-
-*Q<sub>coil,cyclingl</sub>*      = delivered total cooling capacity for Speed 1 operating at a specific cycling ratio [W]
-
-<span>\({\mathop m\limits^\cdot_{Speed\,\,1}}\)</span>      = air mass flow rate through cooling coil at Speed 1 as set by the parent object [kg/s]
-
-*h<sub>outlet,full</sub>*      = specific enthalpy of the coil outlet air during full-load operation at Speed 1 (no cycling) [J/kg]
-
-*h<sub>inlet</sub>           *            = specific enthalpy of the coil inlet air [J/kg]
-
-*CycRatio*    = cycling ratio at Speed 1, ratio of requested heating load to the full-load capacity of the coil at Speed 1 [dimensionless]
-
-It is assumed that the coil provides no cooling capacity when the coil is OFF, even if the supply air fan continues to operate.
-
-n Outlet air specific enthalpy
-
-The average specific enthalpy of the coil outlet air is then calculated based on the total delivered cooling capacity and the average air mass flow rate entering the coil:
-
-<div>$${h_{outlet,average}} = {h_{inlet}} - {{\raise0.7ex\hbox{${{Q_{coil,cycling}}}$} \!\mathord{\left/ {\vphantom {{{Q_{coil,cycling}}} {\mathop m\limits^\cdot  }}}\right.}\!\lower0.7ex\hbox{${\mathop m\limits^\cdot  }$}}_{inlet}}$$</div>
-
-where
-
-h<sub>outlet,average</sub>    = averaged specific enthalpy at the coil outlet [J/kg]
-
-h<sub>inlet</sub>             = specific enthalpy at the coil inlet [J/kg]
-
-Q<sub>coil,cycling</sub>      = total capacity at full load [W]
-
-<span>\({\mathop m\limits^\cdot_{inlet}}\)</span>         = mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the cooling coil is ON and the specified flow rate when the cooling coil is OFF for the time step being simulated.
-
-n Sensible capacity
-
-The minimum humidity ratio (HR<sub>min</sub> ) is based on humidity ratios between inlet and full load outlet as:
-
-HR<sub>min</sub> = Minimum(HR<sub>inlet</sub>, HR<sub>full</sub>)
-
-where
-
-HR<sub>inlet</sub>           = Humidity ratio at the inlet [kg/kg]
-
-HR<sub>full</sub>            = Full load humidity ratio at the outlet [kg/kg]
-
-The coil sensible capacity may be calculated as:
-
-<div>$${Q_{coil,sens}} = {\mathop m\limits^\cdot_{Speed1}}*CycRatio*[{h_{inlet}}({T_{inlet}},H{R_{\min }}) - {h_{outlet,full}}({T_{outlet,full}},H{R_{\min }})]$$</div>
-
-where
-
-Q<sub>coil,sens</sub>        = delivered sensible cooling capacity [W]
-
-h<sub>outlet,full</sub>         = full load specific enthalpy at the coil outlet as a function of outlet dry-bulb temperature at the full load, and the minimum humidity ratio [J/kg]
-
-h<sub>inlet</sub>             = specific enthalpy at the coil inlet [J/kg]
-
-n Latent capacity
-
-The latent capacity is the difference between total and sensible capacities
-
-<div>$${Q_{coil,latent}} = {Q_{coil,cycling}} - {Q_{coil,sens}}$$</div>
-
-where
-
-Q<sub>coil,latent</sub>        = delivered latent cooling capacity [W]
-
-n Average outlet air humidity ratio
-
-The averaged outlet HR can be calculated as:
-
-<div>$$H{R_{outlet,average}} = H{R_{inlet}} - {{\raise0.7ex\hbox{${{Q_{coil,latent}}}$} \!\mathord{\left/ {\vphantom {{{Q_{coil,latent}}} {\mathop {\lambda m}\limits^\cdot  }}}\right.}\!\lower0.7ex\hbox{${\mathop {\lambda m}\limits^\cdot  }$}}_{inlet}}$$</div>
-
-where
-
-λ     = heat of vaporization as a function of HR<sub>min</sub> and CycRatio\*T<sub>outlet,full</sub>+(1-CycRatio)\*T<sub>inlet</sub> [J/kg]
-
-n Average outlet air temperature
-
-Using the above averaged outlet humidity ratio and specific enthalpy, the averaged outlet temperature can be calculated using the psych function of PsyTdbFnHW.
-
-The main reason using the above approach is that outlet conditions are calculated in the same way in low and high speed operation.
-
-The crankcase heater defined for this DX cooling coil is enabled during the time that the compressor is not running for either heating or cooling. The crankcase heater power use from either heating or cooling is reported in the heating coil (Coil:Heating:DX:MultiSpeed).
-
-#### Higher Speed Operation
-
-This section describes how higher speed operation is simulated. When the required sensible load is less than the full load sensible capacity at Speed n (Speed Number &gt; 1), the following calculations are performed:
-
-n Bypass factor at Speed n-1 and Speed n
-
-<div>$$BypassFacto{r_n} = f(RatedBypassFacto{r_n},RatedFlowRat{e_n},ActualFowRat{e_n})$$</div>
-
-<div>$$BypassFacto{r_{n - 1}} = f(RatedBypassFacto{r_{n - 1}},RatedFlowRat{e_{n - 1}},ActualFowRat{e_{n - 1}})$$</div>
-
-where
-
-BypassFactor<sub>i</sub>         = bypass factor at actual flow rate conditions at Speed i [dimensionless]
-
-RatedBypassFactor<sub>i</sub>            = bypass factor at the rated conditions at Speed i [dimensionless]
-
-RatedFowRate<sub>i</sub>        = air mass flow rate at the rated conditions at Speed i [kg/s]
-
-ActualFowRate<sub>i</sub>       = actual air mass flow rate at Speed i [kg/s]
-
-i     = Speed n or Speed n-1
-
-The bypass factor at Speed n is a function of the bypass factor at the rated conditions, rated airflow rate, and actual flow rate at Speed n. The calculation is performed by a function, called AdjustCBF in the DXCoil module.
-
-n Total capacity at Speed n-1 and Speed n
-
-<span>\(TotCa{p_{n - 1}} = f(RatedCa{p_{n - 1}},TotCapTempModFa{c_{n - 1}},TotCapFlowModFa{c_{n - 1}},BypassFacto{r_{n - 1}})\)</span><span>\(TotCa{p_n} = f(RatedCa{p_n},TotCapTempModFa{c_n},TotCapFlowModFa{c_n},BypassFacto{r_n})\)</span>
-
-where
-
-TotCap<sub>i             </sub> = total cooling capacity at given temperatures and flow rates at Speed i [w]
-
-RatedCap<sub>i     </sub> = cooling capacity at the rated conditions at Speed i [W]
-
-TotCapTempModFac<sub>i                    </sub> = total cooling capacity modifier as a function of indoor web-bulb temperature and outdoor air dry-bulb temperature at Speed i
-
-TotCapFlowModFac<sub>i                      </sub> = total cooling capacity modifier as a function of the ratio of the actual flow rate across the cooling coil to the rated airflow rate at Speed i
-
-i     = Speed n or Speed n-1
-
-
-
-The calculation is performed by a subroutine, called CalcTotCapSHR in the DXCoil module.
-
-n EIR at Speed n-1 and Speed n
-
-<div>$$EI{R_{n - 1}} = RatedEI{R_{n - 1}}*EIRTempModFa{c_{n - 1}}*EIRFlowModFa{c_{n - 1}}$$</div>
-
-<div>$$EI{R_n} = RateEI{R_n}*EIRTempModFa{c_n}*EIRFlowModFa{c_n}$$</div>
-
-where
-
-EIR<sub>i                        </sub> = Energy input ratio at given temperatures and flow rates at Speed i [w]
-
-RatedEIR<sub>i      </sub> = Energy input ratio at the rated conditions at Speed i [W]
-
-EIRTempModFac<sub>i       </sub> = Energy input ratio modifier as a function of indoor and outdoor air dry-bulb temperature at Speed i
-
-EIRFlowModFac<sub>i         </sub> = Energy input ratio modifier as a function of ratio of the actual flow rate across the heating coil to the rated airflow rate at Speed i
-
-i     = n or n-1
-
-n Full load outlet conditions at Speed n-1 and Speed n
-
-The calculation procedure of full load outlet conditions at Speed n-1 and Speed n is the same as the calculation procedure used in the Coil:Cooling:DX:SingleSpeed model (Ref. Coil:Cooling:DX:SingleSpeed). The difference is that the outlet conditions at Speed n-1 are calculated based on the total cooling capacity and mass flow rate at Speed n-1, while the outlet conditions at Speed n are calculated based on the total cooling capacity and mass flow rate at Speed n.
-
-n Effective total cooling capacity
-
-<div>$$\begin{array}{l}{Q_{coil,SpeedRatio}} = (SpeedRatio){\mathop m\limits^\cdot_{Speed{\kern 1pt} n}}({h_{inlet}} - {h_{outlet,full\_Speed\;n}})\\\;\;\;\;\;\;\;\;\; + (1 - SpeedRatio){\mathop m\limits^\cdot_{Speed\;n - 1}}({h_{inlet}} - {h_{outlet,full\_Speed\;n - 1}})\end{array}$$</div>
-
-where
-
-<span>\({Q_{coil,SpeedRatio}}\)</span><sub>                       </sub> = delivered sensible cooling capacity at a given speed ratio between two consecutive speeds [W]
-
-<span>\({\mathop m\limits^\cdot_{Speed\,n}}\)</span>      = air mass flow rate through cooling coil at Speed n as set by the parent object [kg/s]
-
-<span>\({\mathop m\limits^\cdot_{Speed\,\,n - 1}}\)</span>    = air mass flow rate through cooling coil at Speed 1 as set by the parent object [kg/s]
-
-h<sub>inlet</sub>             = specific enthalpy at the coil inlet [J/kg]
-
-h<sub>outlet,full\_Speed\\ n</sub> = full load specific enthalpy at the coil outlet at Speed n [J/kg]
-
-h<sub>outlet,full\_Speed\\ n-1</sub>           = full load specific enthalpy at the coil outlet at Speed n-1 [J/kg]
-
-n Average outlet air specific enthalpy
-
-<div>$${h_{outlet,average}} = {h_{inlet}} - {{\raise0.7ex\hbox{${{Q_{coil,SpeedRatio}}}$} \!\mathord{\left/ {\vphantom {{{Q_{coil,SpeedRatio}}} {\mathop m\limits^\cdot  }}}\right.}\!\lower0.7ex\hbox{${\mathop m\limits^\cdot  }$}}_{inlet}}$$</div>
-
-where
-
-h<sub>outlet,average</sub>    = averaged specific enthalpy at the coil outlet [J/kg]
-
-h<sub>inlet</sub>             = specific enthalpy at the coil inlet [J/kg]
-
-<span>\({\mathop m\limits^\cdot_{inlet}}\)</span>         = mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the heating coil is at Speed n and the specified flow rate when the heating coil is at Speed n-1 for the time step being simulated.
-
-n Effective sensible cooling capacity
-
-The minimum humidity ratio (HR<sub>min</sub> ) is calculated as
-
-HR<sub>min</sub> = Minimum[HR<sub>inlet</sub>, (SpeedRatio)HR<sub>full,n</sub>+(1.0-SpeedRatio)HR<sub>full,n-1</sub>)
-
-The effective sensible cooling capacity is expressed as:
-
-<div>$$\begin{array}{l}{Q_{coil,sens}} = {\mathop m\limits^\cdot_{Speed\;n}}(SpeedRatio)[{h_{inlet}}({T_{inlet}},H{R_{\min }}) - {h_{outlet,full\_Speed\,n}}({T_{outlet,n}},H{R_{\min }})]\\\;\;\;\;\;\;\;\;\;\;\;\;\;\; + {\mathop m\limits^\cdot_{Speed\;n - 1}}(1 - SpeedRatio)[{h_{inlet}}({T_{inlet}},H{R_{\min }}) - {h_{outlet,full\_Speed\;n - 1}}({T_{outlet,n - 1}},H{R_{\min }})]\end{array}$$</div>
-
-where
-
-Q<sub>coil,sens</sub>        = effective sensible cooling capacity [W]
-
-h<sub>outlet,full\_Speed\\ n</sub> = full load specific enthalpy at the coil outlet at Speed n as a function of outlet dry-bulb temperature at the full load, and the minimum humidity ratio [J/kg]
-
-h<sub>outlet,full\_Speed\\ n-1</sub> = full load specific enthalpy at the coil outlet at Speed n-1 as a function of outlet dry-bulb temperature at the full load, and the minimum humidity ratio [J/kg]
-
-h<sub>inlet</sub>             = specific enthalpy at the coil inlet [J/kg]
-
-n Aaverage outlet air humidity ratio and temperature
-
-The effective latent cooling capacity is the difference between the total and sensible capacity:
-
-<div>$${Q_{coil,latent}} = {Q_{coil,SpeedRatio}} - {Q_{coil,sens}}$$</div>
-
-Q<sub>coil,latent</sub>        = effective latent cooling capacity [W]
-
-The average outlet air HR can be calculated as:
-
-<div>$$H{R_{outlet,average}} = H{R_{inlet}} - {{\raise0.7ex\hbox{${{Q_{coil,latent}}}$} \!\mathord{\left/ {\vphantom {{{Q_{coil,latent}}} {\mathop {\lambda m}\limits^\cdot  }}}\right.}\!\lower0.7ex\hbox{${\mathop {\lambda m}\limits^\cdot  }$}}_{inlet}}$$</div>
-
-where
-
-λ     = heat of vaporization as a function of HR<sub>min</sub> and SpeedRatio\*T<sub>outlet,n</sub>+(1-SpeedRatio)\*T<sub>outlet,n-1</sub> [J/kg]
-
-At the given averaged outlet humidity ratio and specific enthalpy, the averaged outlet temperature can be calculated using the psych function of PsyTdbFnHW.
-
-n Calculate combined energy input
-
-When the input for the field ‘Apply Part Load Fraction to Speeds Greater than 1’ is No in the object (equivalent to a single compressor), the combined energy output is calculated as follows:
-
-<span>\(CoolingPower = (TotCa{p_n})(EI{R_n})(SpeedRatio) + (TotCa{p_{n - 1}})(EI{R_{n - 1}})(1.0 - SpeedRatio)\)</span> When the input for the field ’Apply Part Load Fraction to Speeds Greater than 1’ is Yes in the object (equivalent to multiple compressors), the combined energy output is calculated as follows:
-
-<div>$$CoolingPower = (TotCa{p_n})(EI{R_n})(RTF) + (TotCa{p_{n - 1}})(EI{R_{n - 1}})(1.0 - RTF)$$</div>
-
-where
-
-CoolingPower         = Power used in Watt
-
-RTF            = Run time fraction at Speed n
-
-n Latent degradation
-
-When the supply fan operation mode is ContinuousFanWithCyclingCompressorand the input of the Apply Latent Degradation to Speeds Greater than 1 is Yes, the latent degradation is included at Speed n. The calculation procedure is the same as one in the Coil:Cooling:DX:SingleSpeed object. The difference is that the rated values and run time fraction at Speed n are used. The adjusted SHR is used to calculate full load outlet conditions at Speed n.
-
-It is expected to have less latent degradation at Speed n than Speed 1. Therefore, smaller values of the latent degradation inputs at Speed n than those at Speed 1 are recommended.
-
-n Crankcase heater
-
-There is no power need at higher speed operation.
-
-#### Higher Speed Operation with Single Mode Operation
-
-This section describes how higher speed operation is simulated with single mode operation. When the required sensible load is less than the full load sensible capacity at Speed n (Speed Number > 1), its performance is almost the same as the performance for the Coil:Cooling:DX:SingleSpeed model at different flow rate and capacity with given Speed n. No linear interpolation is performed between two adjacent speeds.
-
-#### Waste heat calculation
-
-The waste heat generated by this coil object is calculated as:
-
-<div>$${Q_{WasteHeat}} = (Fraction)(TempModifier)(CoolingPowe)$$</div>
-
-where
-
-Fraction                  = rated waste heat fraction of the energy input
-
-TempModifer<sub>                    </sub> = waste heat modifier as a function of indoor and outdoor air dry-bulb temperature
-
-#### Basin Heater For Multi-Speed DX Coil
-
-Basin heater for the object Coil:Cooling:DX:MultiSpeed operates in the same manner as for Coil:Cooling:DX:SingleSpeed. Refer to the Basin Heater For Single-Speed DX Coil description above.
-
-#### Standard Rating of Multi-Speed DX Cooling Coils
-
-For multi-speed direct expansion cooling coils, the industry standard ratings of Standard Rating Seasonal Energy Efficiency Ratio (SEER) are calculated according to ANSI/AHRI Standard 210/240 (AHRI 2008). These standard ratings can be calculated using the user-entered information for the Coil:Cooling:DX:MultiSpeed object.  According to Standard 210/240, the Standard Rating SEER applies to air-to-air unitary heat pumps and air conditions with rated cooling capacities under 19,000 Watts (&lt;65,000 Btu/h). The Cooling Mode Test Conditions for Units Having two-capacity Compressor standard tests A<sub>2</sub>, B<sub>2</sub>, B<sub>1</sub>, and F<sub>1</sub> are also provided in Table 56. Cooling Mode Test Conditions for Units Having a Two-Capacity Compressor. The equations required to calculate the net cooling capacity and SEER value are described next.
-
-#### Standard Rating Cooling Capacity
-
-The standard net cooling capacity of multi-speed DX cooling coil is reported at the maximum speed and full load A2 test condition only. The Standard Rating (Net) Cooling Capacity calculation is the same as single speed DX cooling coil procedure when calculated at maximum speed.The procedure for calculating the Standard Rating Cooling Capacity is given by:
-
-<div>$${\dot Q_{StandardRating}} = \dot Q_{T,\,CRated}^{k = 2} \cdot CAPFT_{TestA2}^{k = 2} \cdot CAPFFF_{TestA2}^{k = 2}$$</div>
-
-<div>$${\dot Q_{Standard\,Rating\,Net}} = {\dot Q_{StandardRating}} - Fa{n_{Power,\,CRated}}$$</div>
-
-<div>$$Fa{n_{Power,\,CRated}} = FanPowerPerVolFlowRat{e^{k = 2}} \cdot \dot V_{CRated}^{k = 2}$$</div>
-
-where,
-
-<span>\({\dot Q_{StandardRating\,Net}}\)</span> =    total standard **(net)** cooling capacity (W) of the air-conditioning or heat pump equipment in cooling mode determined from ANSI/AHRI Standard 210/240 and A2 test conditions shown in Table 56. The standard cooling test conditions for air-cooled condenser are: indoor coil entering air dry-bulb and wet-bulb temperatures 26.7°C/19.4°C and outdoor coil entering air dry-bulb and wet-bulb temperatures 35.0°C/23.9°C.
-
-<span>\({\dot Q_{StandardRating}}\)</span> =        total standard cooling capacity (W) of the air-conditioning or heat pump equipment determined from ANSI/AHRI Standard 210/240 and A2 test conditions shown in Table 56. The standard cooling test conditions for air-cooled are: indoor coil entering air dry-bulb and wet-bulb temperatures 26.7°C/19.4°C and outdoor coil entering air dry-bulb and wet-bulb temperatures 35.0°C/23.9°C.
-
-<span>\(\dot Q_{T,\,CRated}^{k = 2}\)</span> = Rated total cooling capacity at maximum speed, user input (W)
-
-<span>\(CAPFT_{TestA2}^{k = 2}\)</span>= User-specified bi-quadratic curve evaluated at the indoor coil entering air wet-bulb temperature (19.4°C) and outdoor coil entering air dry-bulb temperature (35.0°C) for air-cooled condenser per A2 test condition as specified in Table 56, (dimensionless).
-
-<span>\(CAPFFF_{TestA2}^{k = 2}\)</span>= User-specified quadratic or cubic curve modifying the total cooling capacity as function of flow fraction, (dimensionless).  This curve is evaluated at a flow fraction of 1.0.
-
-<span>\(Fa{n_{Power,\,Rated}}\)</span>= Supply air fan power at rated conditions at high (maximum) compressor speed, (W).
-
-<span>\(\dot V_{_{CRated}}^{k = 2}\)</span>= Rated Air Volume Flow Rate at high (maximum) compressor speed, user input (m<sup>3</sup>/s)
-
-<span>\(FanPowerPerVolFlowRat{e^{k = 2}}\)</span>= The Rated Indoor Coil Fan Power Per Volume Flow rate is a user-entered value, with a default of 773.3 W/(m<sup>3</sup>/s)) if the user leaves this input field blank. The default value is taken from ANSI/ASHRAE Standard 210/240 -2008 where it is defined for systems which do not have an indoor coil fan furnished as part of the system. See the description given below how this value is calculated. User input ( W/(m<sup>3</sup>/s)).
-
-The Rated Evaporator (Indoor Coil) Fan Power Per Volume Flow rate is a user-entered value, with a default of 773.3 W/(m<sup>3</sup>/s)) if the user leaves this input field blank. The default value is taken from ANSI/ASHRAE Standard 210/240-2008 where it is defined for systems which do not have an Indoor Coil (Evaporator) fan furnished as part of the system. The test conditions in ANSI/AHRI Standard 210/240 vary the external static pressure (i.e., pressure drop associated with ductwork and other devices external to the indoor fan/coil section) seen by the supply air fan based on the standard rating cooling capacity.
-
-#### Seasonal Energy Efficiency Ratio (SEER) for Multi-Speed DX Coil
-
-The SEER value for multi-speed compressor air conditioner or air-to-air heat pumps per AHRI/ANSI Std. 210/240 – 2008 is calculated as follows:
-
-<div>$$SEER = \frac{{\sum\limits_{j = 1}^8 {\frac{{{q_c}({T_j})}}{N}} }}{{\sum\limits_{j = 1}^8 {\frac{{{e_c}({T_j})}}{N}} }}$$</div>
-
-For multi-speed compressor the SEER value is weighted average performance at different outdoor air temperature bins.  The eight outdoor air temperature bins and the corresponding weight are provided in Table 57. Distribution of Fractional Hours with in Cooling Season Temperature Bins.
-
-Where,
-
-*q<sub>c</sub>*(T<sub>j</sub>)/N =  = the ratio of space cooling capacity provided by the unit during periods of the space cooling season when the outdoor temperature fell within the range represented by bin temperature *T<sub>j</sub>* to the total number of hours in the cooling season (N), (W)
-
-*e<sub>c</sub>*(T<sub>j</sub>)/N = the ratio of the electrical energy consumed by the unit during periods of the space cooling season when the outdoor temperature fell within the range represented by bin temperature Tj to the total number of hours in the cooling season (N), W.
-
-*j*      = the bin number, dimensionless. For cooling season j ranges from 1 to 8.
-
-*T<sub>j</sub>*    =          outdoor air bin temperature, °C. Outdoor temperatures are “binned� such that calculations are only performed based one temperature within the bin. Bins of 2.8 °C with 8 cooling season bin temperatures being 19.44°C, 22.22°C, 25.0°C, 27.78°C, 30.56°C, 33.33°C, 36.11°C, 38.89°C.
-
-The steady-state cooling capacity delivered and the electric power inputs when the DX coil is operating at minimum compressor speed (*k=1*), and outdoor air temperature *T<sub>j</sub>*, are determined by linear interpolation using the values of B1 and F1 tests as follows:
-
-<div>$$\dot Q_c^{k = 1}({T_j}) = \dot Q_c^{k = 1}(19.44) + \frac{{\dot Q_c^{k = 1}(27.78) - \dot Q_c^{k = 1}(19.44)}}{{27.78 - 19.44}}\left( {{T_j} - 19.44} \right)$$</div>
-
-<div>$$\dot E_c^{k = 1}({T_j}) = \dot E_c^{k = 1}(19.44) + \frac{{\dot E_c^{k = 1}(27.78) - \dot E_c^{k = 1}(19.44)}}{{27.78 - 19.44}}\left( {{T_j} - 19.44} \right)$$</div>
-
-The steady-state cooling capacities and electric power inputs at the minimum speed and test condition *B<sub>1</sub>* and *F<sub>1</sub>* are calculated from the minimum (low) speed performance curves as follows:
-
-<div>$$\dot Q_c^{k = 1}(27.78) = \dot Q_{T,\,CRated}^{k = 1} \cdot CAPFT_{TestB1}^{k = 1} \cdot CAPFFF_{TestB1}^{k = 1} - FanPower_{CRated}^{k = 1}$$</div>
-
-<div>$$\dot E_c^{k = 1}(27.78) = \left[ {\frac{{\dot Q_c^{k = 1}(27.78)}}{{COP_{CRated}^{k = 1}}}} \right] \cdot EIRFT_{TestB1}^{k = 1} \cdot EIRFFF_{TestB1}^{k = 1} + FanPower_{CRated}^{k = 1}$$</div>
-
-<div>$$\dot Q_c^{k = 1}(19.44) = \dot Q_{T,\,CRated}^{k = 1} \cdot CAPFT_{TestF1}^{k = 1} \cdot CAPFFF_{TestF1}^{k = 1} - FanPower_{CRated}^{k = 1}$$</div>
-
-<div>$$\dot E_c^{k = 1}(19.44) = \left[ {\frac{{\dot Q_c^{k = 1}(19.44)}}{{COP_{CRated}^{k = 1}}}} \right] \cdot EIRFT_{TestF1}^{k = 1} \cdot EIRFFF_{TestF1}^{k = 1} + FanPower_{CRated}^{k = 1}$$</div>
-
-<div>$$FanPower_{CRated}^{k = 1} = FanPowerPerVolFlowRat{e^{k = 1}} \cdot {\rm{\dot V}}_{CRated}^{k = 1}$$</div>
-
-Where,
-
-<span>\(\dot Q_{T,\,CRated}^{k = 1}\)</span>=   rated total cooling capacity at minimum compressor speed specified by users, (W)
-
-<span>\(COP_{CRated}^{k = 1}\)</span>=            rated gross COP at minimum compressor speed specified by users, (-)
-
-<span>\(CAPFT_{TestB1}^{k = 1}\)</span>=cooling capacities modifier curve for temperature at minimum compressor speed and B1 test condition, (-)
-
-<span>\(CAPFFF_{TestB1}^{k = 1}\)</span>=      cooling capacities modifier curve for flow fraction at minimum compressor speed and B1 test condition, (-)
-
-<span>\(EIRFT_{TestB1}^{k = 1}\)</span>=EIR modifier curve for temperature at minimum compressor speed and B1 test condition, (-)
-
-<span>\(EIRFFF_{TestB1}^{k = 1}\)</span>=EIR modifier curve for flow fraction at minimum compressor speed and B1 test condition, (-)
-
-<span>\(CAPFT_{TestF1}^{k = 1}\)</span>=cooling capacities modifier curve for temperature at minimum compressor speed and F1 test condition, (-)
-
-<span>\(CAPFFF_{TestF1}^{k = 1}\)</span>=cooling capacities modifier curve for flow fraction at minimum compressor speed and F1 test condition, (-)
-
-<span>\(EIRFT_{TestF1}^{k = 1}\)</span>=EIR modifier curve for temperature at minimum compressor speed and F1 test condition, (-)
-
-<span>\(EIRFFF_{TestF1}^{k = 1}\)</span>=EIR modifier curve for flow fraction at minimum compressor speed and F1 test condition, (-)
-
-<span>\(FanPower_{CRated}^{k = 1}\)</span>=the rated supply air fan power when the unit is operating at minimum compressor speed, (W)
-
-<span>\(V_{CRated}^{k = 1}\)</span>=rated cooling supply air volume flow rate at minimum compressor speed specified by users, (-)
-
-<span>\(FanPowerPerVolFlowRat{e^{k = 1}}\)</span> =  the rated Indoor Coil fan power per volume flow rate at low (minimum) compressor speed specified value by the user, (W/(m3/s))
-
-The steady-state cooling capacity delivered and the electric power inputs when the DX cooling coil is operating at maximum (high) compressor speed (*k=2*), and outdoor air temperature *T<sub>j</sub>*, are determined as follows:
-
-<div>$$\dot Q_c^{k = 2}({T_j}) = \dot Q_c^{k = 2}(27.78) + \frac{{\dot Q_c^{k = 2}(35.0) - \dot Q_c^{k = 2}(27.78)}}{{35.0 - 27.78}}\left( {{T_j} - 27.78} \right)$$</div>
-
-<div>$$\dot E_c^{k = 2}({T_j}) = \dot E_c^{k = 2}(27.78) + \frac{{\dot E_c^{k = 2}(35.0) - \dot E_c^{k = 2}(27.7)}}{{35.0 - 27.78}}\left( {{T_j} - 27.78} \right)$$</div>
-
-The steady-state cooling capacities and electric power input at the maximum speed and test condition *A<sub>2</sub>* and *B<sub>2</sub>* are determined from the maximum (high) speed performance curves as follows:
-
-<div>$$\dot Q_c^{k = 2}(35.0) = \dot Q_{T,\,CRated}^{k = 2} \cdot CAPFT_{TestA2}^{k = 2} \cdot CAPFFF_{TestA2}^{k = 2} - FanPower_{CRated}^{k = 2}$$</div>
-
-<div>$$\dot E_c^{k = 2}(35.0) = \left[ {\frac{{\dot Q_c^{k = 2}(35.0)}}{{COP_{CRated}^{k = 2}}}} \right] \cdot EIRFT_{TestA2}^{k = 2} \cdot EIRFFF_{TestA2}^{k = 2} + FanPower_{CRated}^{k = 2}$$</div>
-
-<span>\(\dot Q_c^{k = 2}(27.78) = \dot Q_{T,\,CRated}^{k = 2} \cdot CAPFT_{TestB2}^{k = 2} \cdot CAPFFF_{TestB2}^{k = 2} - FanPower_{CRated}^{k = 2}\)</span> <span>\(\dot E_c^{k = 2}(27.78) = \left[ {\frac{{\dot Q_c^{k = 2}(19.44)}}{{COP_{CRated}^{k = 2}}}} \right] \cdot EIRFT_{TestB2}^{k = 2} \cdot EIRFFF_{TestB2}^{k = 2} + FanPower_{CRated}^{k = 2}\)</span>
-
-<div>$$FanPower_{CRated}^{k = 2} = FanPowerPerVolFlowRat{e^{k = 2}} \cdot {\rm{\dot V}}_{CRated}^{k = 2}$$</div>
-
-Where,
-
-<span>\(\dot Q_{T,\,CRated}^{k = 2}\)</span> = rated total cooling capacity at maximum (high) compressor speed specified by users, (W)
-
-<span>\(COP_{CRated}^{k = 2}\)</span> = rated gross COP at maximum (high) compressor speed specified by users, (-)
-
-<span>\(CAPFT_{TestA2}^{k = 2}\)</span> = cooling capacity modifier curve for temperature at maximum (high) compressor speed and *A*<sub>2</sub> test condition, (-)
-
-<span>\(CAPFFF_{TestA2}^{k = 2}\)</span>        =cooling capacity modifier curve for flow fraction at maximum (high) compressor speed and *A*<sub>2</sub> test condition, (-)
-
-<span>\(EIRFT_{TestA2}^{k = 2}\)</span> = EIR modifier curve for temperature at maximum (high) compressor speed and *A*<sub>2</sub> test condition, (-)
-
-<span>\(EIRFFF_{TestA2}^{k = 2}\)</span> = EIR modifier curve for flow fraction at maximum (high)  compressor speed and *A*<sub>2</sub> test condition, (-)
-
-<span>\(CAPFT_{TestB2}^{k = 2}\)</span> = cooling capacity modifier curve for temperature at maximum (high) compressor speed and *B*<sub>2</sub> test condition, (-)
-
-<span>\(CAPFFF_{TestB2}^{k = 2}\)</span>        =cooling capacity modifier curve for flow fraction at maximum (high) compressor speed and *B*<sub>2</sub> test condition, (-)
-
-<span>\(EIRFT_{TestB2}^{k = 2}\)</span> = EIR modifier curve for temperature at maximum (high) compressor speed and *B*<sub>2</sub> test condition, (-)
-
-<span>\(EIRFFF_{TestB2}^{k = 2}\)</span> = EIR modifier curve for flow fraction at maximum (high) compressor speed and *B*<sub>2</sub> test condition, (-)
-
-<span>\(FanPower_{CRated}^{k = 2}\)</span> = the rated supply air fan power when the unit is operating at maximum (high) compressor speed, (W)
-
-<span>\(V_{CRated}^{k = 2}\)</span> = rated supply air volume flow rate at maximum (high) compressor speed specified by users, (-)
-
-<span>\(FanPowerPerVolFlowRate{k^{k = 2}}\)</span> =the Rated Evaporator (Indoor Coil) Fan Power Per Volume Flow rate at maximum (high) compressor speed specified value by the user, (W/(m3/s))
-
-The above steps show how the cooling capacity and electric power inputs are determined when the DX cooling coil is operating at minimum (low) and maximum (high) compressor speeds.  But the unit may operate at minimum (low) speed capacity, cycle on–off, cycle between successiave lower and higher compressor speed capacity, or operate at maximum (high) speed capacity depending on the building cooling load. The operating range of the DX cooling coil is determined based on the building cooling load for each binned outside air temperature. The building cooling load at an outdoor air temperature *T<sub>j</sub>*, is calculated as follows:
-
-<div>$$BL({T_j}) = \left( {\frac{{{T_j} - 18.3}}{{35.0 - 18.3}}} \right)\left( {\frac{{\dot Q_c^{k = 2}(35.0)}}{{1.1}}} \right)$$</div>
-
-Where,
-
-*BL(T<sub>j</sub>)*          =the building space cooling load corresponding to outdoor temperature of *T<sub>j</sub>*, (W).
-
-<span>\(\dot Q_c^{k = 2}(35.0)\)</span>=the cooling capacity determined from the standard A2 test, (W)
-
-The temperatures 35.0 °C and 18.3 °C in the building load calculation equation represent the outdoor design air temperature, and zero-load base temperature, respectively (ANSI/ASHRAE, 2008).  1.1 is a sizing factor.
-
-The cooling capacity delivered and the electric power inputs calculations when the DX cooling coil is cycling on-off, operating at minimum (low) compressor speed, cycling between successive minimum (low) and maximum (high) compressor speed, or operating at maximum (high) compressor speed are described next.
-
-*Case 1*:  The steady state cooling capacity when the unit is operating at or below the minimum (low) speed compressor capacity, i.e., when the building cooling load is less or equal to the minimum (low) compressor speed capacity, is calculated as follows:
-
-<div>$$\dot Q_c^{k = 1}({T_j}) \ge BL({T_j})$$</div>
-
-<div>$$\frac{{{q_c}({T_j})}}{N} = \left[ {{X^{k = 1}}({T_j}) \cdot \dot Q_c^{k = 1}({T_j})} \right] \cdot \frac{{{n_j}}}{N}$$</div>
-
-<div>$$\frac{{{e_c}({T_j})}}{N} = \left[ {\frac{{{X^{k = 1}}({T_j})}}{{PL{F_j}}}\dot E_c^{k = 1}({T_j})} \right] \cdot \frac{{{n_j}}}{N}$$</div>
-
-<div>$${X^{k = 1}}({T_j}) = \frac{{BL({T_j})}}{{\dot Q_c^{k = 1}({T_j})}}$$</div>
-
-<div>$$PL{F_j} = 1 - C_D^c\left[ {1 - {X^{k = 1}}({T_j})} \right]$$</div>
-
-Where,
-
-*X(T<sub>j</sub>)* = the cooling mode load factor or part-load ratio for temperature bin j, (-)
-
-n<sub>i</sub>/N = fractional bin hours for the cooling season; the ratio of the number of hours during the cooling season when the outdoor temperature fell within the range represented by bin temperature *T<sub>j</sub>* to the total number of hours in the cooling season, (-). (see Table 57)
-
-<span>\(C_D^c\)</span> = cooling coefficient of degradation, default value is 0.25.
-
-*Case 2*:  The unit cycles between successive the minimum (low) and maximum (high) compressor speed capacity to meet the building cooling load at outdoor air temperature *T<sub>j</sub>*.  That is, the cooling building load is between the units successive minimum (low) and maximum (high) compressor speed capacities:
-
-<div>$$\dot Q_c^{k = 1}({T_j}) &lt; BL({T_j}) &lt; \dot Q_c^{k = 2}({T_j})$$</div>
-
-<span>\(\frac{{{q_c}({T_j})}}{N} = \left[ {{X^{k = 1}}({T_j}) \cdot \dot Q_c^{k = 1}({T_j}) + \left( {1 - {X^{k = 1}}({T_j})} \right) \cdot \dot Q_c^{k = 2}({T_j})} \right] \cdot \frac{{{n_j}}}{N}\)</span><span>\(\frac{{{e_c}({T_j})}}{N} = \left[ {{X^{k = 1}}({T_j}) \cdot \dot E_c^{k = 1}({T_j}) + \left( {1 - {X^{k = 1}}({T_j})} \right) \cdot \dot E_c^{k = 2}({T_j})} \right] \cdot \frac{{{n_j}}}{N}\)</span>
-
-<div>$${X^{k = 1}}({T_j}) = \frac{{\dot Q_c^{k = 2}({T_j}) - BL({T_j})}}{{\dot Q_c^{k = 2}({T_j}) - \dot Q_c^{k = 1}({T_j})}}$$</div>
-
-*Case 3*:  The steady-state cooling capacity when the unit is operating continuously at maximum (high) compressor speed capacity at outdoor air temperature *T<sub>j</sub>*. That is the building cooling load is greater or equal to the available capacity at maximum (high) compressor speed:
-
-<div>$$BL({T_j}) \ge \dot Q_c^{k = 2}({T_j})$$</div>
-
-For units when operating continuously at maximum (high) compressor speed (k=2) at temperature *T<sub>j</sub>*, the delivered cooling capacity and electric power inputs are calculated as follows:
-
-<div>$$\frac{{{q_c}({T_j})}}{N} = \left[ {\dot Q_c^{k = 2}({T_j})} \right] \cdot \frac{{{n_j}}}{N}$$</div>
-
-<div>$$\frac{{{e_c}({T_j})}}{N} = \left[ {\dot E_c^{k = 2}({T_j})} \right] \cdot \frac{{{n_j}}}{N}$$</div>
-
-Table 56. Cooling Mode Test Conditions for Units Having a Two-Capacity Compressor
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="7">Source: AHRI Standard 210-240, 2008; Table 5, Page 65</th>
-  </tr>
-  <tr>
-    <td>Test Description</td>
-    <td>Air Entering Indoor Unit Temperature (F / C)</td>
-    <td></td>
-    <td>Air Entering Outdoor Unit Temperature (F / C)</td>
-    <td></td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Dry Bulb</td>
-    <td>Wet Bulb</td>
-    <td>Dry Bulb</td>
-    <td>Wet Bulb</td>
-    <td>Compressor Capacity</td>
-    <td>Cooling Air Volume Rate</td>
-  </tr>
-  <tr>
-    <td>A2 Test-required (steady, wet coil)</td>
-    <td>80.0/26.7</td>
-    <td>67.0/19.4</td>
-    <td>95.0/35.0</td>
-    <td>75.0/23.9</td>
-    <td>High</td>
-    <td>Cooling Full-load</td>
-  </tr>
-  <tr>
-    <td>B2 Test-required (steady, wet coil)</td>
-    <td>80.0/26.7</td>
-    <td>67.0/19.4</td>
-    <td>82.0/27.8</td>
-    <td>65.0/18.3</td>
-    <td>High</td>
-    <td>Cooling Full-load</td>
-  </tr>
-  <tr>
-    <td>B1 Test-required (steady, wet coil)</td>
-    <td>80.0/26.7</td>
-    <td>67.0/19.4</td>
-    <td>82.0/27.8</td>
-    <td>65.0/18.3</td>
-    <td>Low</td>
-    <td>Cooling Minimum</td>
-  </tr>
-  <tr>
-    <td>C2 Test-optional (steady, dry coil)</td>
-    <td>80.0/26.7</td>
-    <td></td>
-    <td>82.0/27.8</td>
-    <td></td>
-    <td>High</td>
-    <td>Cooling Full-load</td>
-  </tr>
-  <tr>
-    <td>D2 Test-required (cyclic, dry coil)</td>
-    <td>80.0/26.7</td>
-    <td></td>
-    <td>82.0/27.8</td>
-    <td></td>
-    <td>High</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>C1 Test-optional (steady, dry coil)</td>
-    <td>80.0/26.7</td>
-    <td></td>
-    <td>82.0/27.8</td>
-    <td></td>
-    <td>Low</td>
-    <td>Cooling Minimum</td>
-  </tr>
-  <tr>
-    <td>D1 Test-optional (cyclic, dry coil)</td>
-    <td>80.0/26.7</td>
-    <td></td>
-    <td>82.0/27.8</td>
-    <td></td>
-    <td>Low</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>F1 Test-optional (steady, dry coil)</td>
-    <td>80.0/26.7</td>
-    <td>67.0/19.4</td>
-    <td>67.0/19.4</td>
-    <td>53.5/11.9</td>
-    <td>High</td>
-    <td>Cooling Minimum</td>
-  </tr>
-</table>
-
-Table 57. Distribution of Fractional Hours with in Cooling Season Temperature Bins
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="4">Source: AHRI Standard 210-240, 2008; Table 16, Page 94</th>
-  </tr>
-  <tr>
-    <td>Bin Number j</td>
-    <td>Bin Temperature Range (C)</td>
-    <td>Representative Temperature for bin (C)</td>
-    <td>Fraction of Total Temperature Bin Hours Nj/N</td>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td>Dry Bulb</td>
-    <td>Wet Bulb</td>
-    <td>Dry Bulb</td>
-  </tr>
-  <tr>
-    <td>2</td>
-    <td>18.33 - 20.56</td>
-    <td>19.44</td>
-    <td>0.214</td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>21.11 - 23.33</td>
-    <td>22.22</td>
-    <td>0.231</td>
-  </tr>
-  <tr>
-    <td>4</td>
-    <td>23.89 - 26.11</td>
-    <td>25</td>
-    <td>0.216</td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>26.67 - 28.89</td>
-    <td>27.78</td>
-    <td>0.161</td>
-  </tr>
-  <tr>
-    <td>6</td>
-    <td>29.44 - 31.67</td>
-    <td>30.56</td>
-    <td>0.104</td>
-  </tr>
-  <tr>
-    <td>7</td>
-    <td>32.22 - 34.44</td>
-    <td>33.33</td>
-    <td>0.052</td>
-  </tr>
-  <tr>
-    <td>8</td>
-    <td>35.00 - 37.22</td>
-    <td>36.11</td>
-    <td>0.018</td>
-  </tr>
-</table>
-
-#### References
-
-See the references for the single speed DX cooling coil earlier in this document.
-
-### Two-Speed Electric DX Air Cooling Coil
-
-#### Overview
-
-The input object Coil:Cooling:DX:TwoSpeed provides a model that is meant to represent either a 2 speed (fan and compressor) DX cooling unit (compressor, evaporator, condenser) or a variable speed DX cooling unit in which the variation of compressor speed and air flow rate is nearly linear as a function of cooling part load. In EnergyPlus Coil:Cooling:DX:TwoSpeed is used as the cooling coil in packaged variable volume systems (PVAV). The model is based upon the single speed DX unit Coil:Cooling:DX:SingleSpeed. Basically the model for Coil:Cooling:DX:TwoSpeed employs a separate single speed model at high speed (full load) and low speed (minimum load) and interpolates between these 2 states to obtain the needed cooling output. Below minimum load the unit cycles on/off, just like the single speed unit.
-
-#### Inputs and Data
-
-The input is similar to that for Coil:Cooling:DX:SingleSpeed except there needs to be two complete sets of performance data. The user inputs a rated total cooling capacity, rated SHR, rated COP, and rated air volumetric flow rate for the high speed and low speed states. Performance curves – cooling capacity as a function of entering air wet-bulb temperature and outside dry-bulb temperature (wet-bulb if there is an evaporatively cooled condenser), EIR as a function of the same two temperatures – must be defined and referenced for both high and low speed states. The performance characteristics of the evaporative condenser, if present, also need to be given at high and low speed states: effectiveness, air volumetric flow rate, and pump power consumption. The full list of inputs is given in the Input/Output Reference document.
-
-The data for Coil:Cooling:DX:TwoSpeed is stored in the array structure *DXCoil* in the program module *DXCoils*
-
-#### Calculation
-
-Calculation is performed in routine *CalcMultiSpeedDXCoil* in module *DXCoils*. The inputs to the calculation are the coil index (denoting a specific coil with its particular performance parameters), the speed ratio, and the cycling ratio. The speed ratio is an artificial parameter between 0 and 1. If the speed ratio (*SR*) is greater than zero, the performance of the unit will be:
-
-<div>$$SR\cdot HighSpeedPerformance + (1 - SR)\cdot LowSpeedPerformance$$</div>
-
-Here *HighSpeedPerformance* means the electricity consumption, cooling output, and outlet conditions of the unit if the unit were operating at high speed (full load). Similarly *LowSpeed Performance* means the electricity consumption, cooling output, and outlet conditions if the unit were operating at low speed (minimum non-cycling load). The calculations for each state are the same as for the single speed, cycling DX unit Coil:Cooling:DX:SingleSpeed.
-
-If the speed ratio is zero and the cycling ratio is &gt; 0, the unit will be in cycling mode. The unit will be on for *cycling ratio* fraction of the time step, off for the remainder of the time step. While on, the unit will perform according to the low speed performance parameters.
-
-#### Simulation and Control
-
-Coil:Cooling:DX:TwoSpeed is not used by itself; it is used as part of an encompassing component or system that provides control for the unit. In setting up a PVAV system, for instance, Coil:Cooling:DX:TwoSpeed is part of the component CoilSystem:Cooling:DX, which controls Coil:Cooling:DX:TwoSpeed. When used in the CoilSystem:Cooling:DX component, the simulation allows for either temperature *or* temperature and dehumidification control based on a dehumidification control selection in the CoilSystem:Cooling:DX component. If None is selected the simulation runs the DX unit to satisfy a supply air temperature setpoint. It typically varies the speed ratio in an iterative solution process to establish the operating point that will give the desired unit outlet air temperature. If CoolReheat is selected, the simulation first runs the DX unit to satisfy a supply air temperature setpoint. However, in this case if the DX unit outlet air humidity ratio is above the humidity ratio setpoint, the simulation will increase the speed and/or cycling ratio to meet the desired unit outlet air humidity ratio. The humidity ratio setpoint is specified through the use of a humidistat (ref. ZoneControl:Humidistat) and a setpoint manager (ref. SetpointManager:SingleZone:Humidity:Maximum, SetpointManager:MultiZone:MaximumHumidity:Average,  SetpointManager:MultiZone:Humidity:Maximum or SetpointManager:OudoorAirPretreat). When used with the CoilSystem:Cooling:DX component, the dehumidification control type Multimode is not allowed.
-
-#### Basin Heater For Two-Speed DX Coil
-
-Basin heater for the object Coil:Cooling:DX:TwoSpeed operates in the same manner as for Coil:Cooling:DX:SingleSpeed. Refer to the “Basin Heater For Single-Speed DX Coil� description above.
-
-#### Standard Ratings
-
-The Coil:Cooling:DX:TwoSpeed object includes industry standard ratings of Standard Rating Cooling Capacity, Energy Efficiency Ratio (EER), and Integrated Energy Efficiency Ratio (IEER) which are calculated according to ANSI/AHRI Standard 340/360-2007 with Addenda 1 and 2 (AHRI 2007). These ratings apply to unitary air conditioners with air-cooled condensers with standard rated cooling capacities from 19 kW (65,000 Btu/h) to below 220 kW (760,000 Btu/h).
-
-For the Coil:Cooling:DX:TwoSpeed object in EnergyPlus, these standard ratings are not direct inputs to the model. However, these standard ratings can be calculated using user-entered information for the Coil:Cooling:DX:TwoSpeed object. These standard rating values are provided in the eplusout.eio output file (Ref. OutputDetailsAndExamples.pdf) and also in the predefined tabular output reports (Output:Table:SummaryReports object, Equipment Summary report, DX Cooling Coil table and VAV DX Cooling Standard Rating Details table). Currently, the standard ratings are only calculated and output for Packaged VAV cooling coils with air-cooled condensers and variable-air-volume fans. If the two-speed DX coling coil is specified with an evaporatively-cooled condenser or along with a constant volume fan, then no standard ratings are output from EnergyPlus at this time.
-
-The standard rating cooling capacity is calculated as follows:
-
-<div>$$\begin{array}{l}{{\dot Q}_{StandardRating}} = \,\,{{\dot Q}_{Total,Rated}}\left( {TotCapTempModFa{c_{Rated}}} \right)\left( {TotCapFlowModFa{c_{Rated}}} \right)\,\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, - \,\left( {FanHeatCorrection} \right)\end{array}$$</div>
-
-where,
-
-<span>\({\dot Q_{StandardRating}}\)</span> = Standard Rating (Net) Cooling Capacity (W)
-
-<span>\({\dot Q_{Total,Rated}}\)</span> = Rated Total (Gross) Cooling Capacity, user input (W)
-
-<span>\(TotCapTempModFa{c_{Rated}}\)</span>= Total Cooling Capacity Function of Temperature Curve evaluated with 19.4°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
-
-<span>\(TotCapFlowModFa{c_{Rated}}\)</span>= Total Cooling Capacity Function of Flow Fraction Curve evaluated at a flow fraction of 1.0 (dimensionless)
-
-<span>\(FanHeatCorrection\)</span>= The rate that air is heated by the supply fan ( W )
-
-
-
-<span>\(FanHeatCorrection\)</span> is calculated in one of two ways depending on the user’s input for the field called Unit Internal Static Air Pressure.  If this field was left blank then the fan heat is calculated using
-
-<div>$$FanHeatCorrection = {\dot V_{RatedHighSpeed}}*773.3$$</div>
-
-where
-
-<span>\({\dot V_{RatedHighSpeed}}\)</span>= Rated Air Volume Flow Rate at high speed, user input (m<sup>3</sup>/s)
-
-The value of 773.3 W/(m<sup>3</sup>/s) (365 W/1000cfm) is specified by ANSI/AHRI 340/360 for indoor-coil-only units that are not provided with a supply fan.
-
-If an internal static pressure is provided, then the fan heat is modeled by evaluating the full model for Fan:VariableVolume.  This is different that the ratings calculated for single-speed DX equipment which does not use data from an associated fan object.  The program detects the VAV fan associated with the two-speed coil and uses the input data for that fan but with a different total air pressure rise.  The total pressure is the sum of the internal pressure and the external pressure (i.e., pressure drop associated with ductwork and other devices external to the indoor fan/coil section). The test conditions in ANSI/AHRI Standard 340/360 vary the (minimum) external static pressure seen by the supply air fan based on the standard rating cooling capacity (see Table # 5 in ANSI/AHRI Standard 340/360).  For the part load test points the supply air flow is reduced and the external pressure varies with the square of the flow ratio (see Note 1 in Table # 6 in ANSI/AHRI Standard 340/360-2007 with Addenda 1 and 2). The entire VAV fan model in EnergyPlus is evaluated at the specified air flow rate and the total static pressure for rating and the fan heat is calculated using
-
-<div>$$FanHeatCorrection = Enthalp{y_{leavingFan}} - Enthalp{y_{enteringFan}}$$</div>
-
-Energy Efficiency Ratio (EER) is another standard rating (AHRI 2007), and it is defined as the ratio of the total cooling capacity to the total power input at any given set of rating conditions, expressed in W/W (or Btu/W-h). For this class of air-cooled DX cooling coils, EER is calculated at rated test conditions as follows:
-
-<div>$$EE{R_{}} = \frac{{{{\dot Q}_{Standard\,Rating}}}}{{Powe{r_{Total,Rated}}}}$$</div>
-
-<div>$$\begin{array}{l}Powe{r_{Total,Rated}} = \left( {{{\dot Q}_{Total,Rated}}(TotCapTempModFa{c_{Rated}})(TotCapFlowModFa{c_{Rated}})} \right)\, \cdot EI{R_{Rated}}\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + \,\,\left( {FanPowerCorrection} \right)\end{array}$$</div>
-
-<div>$$EI{R_{Rated}} = \left( {\frac{1}{{CO{P_{Rated}}}}} \right)(EIRTempModFa{c_{Rated}})(EIRFlowModFa{c_{Rated}})$$</div>
-
-where,
-
-*EER*  = Energy Efficiency Ratio (W/W)
-
-<span>\(Powe{r_{Total,Rated}}\)</span>= Total electric power (compressors, condenser fans and evaporator fan) with 19.4°C wet-bulb temperature air entering the cooling coil, 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser, and air flow rate across the evaporator at the rated high speed air flow rate. Similar to the fan heat correction, the fan power correction is calculated in one of two ways depending on the input for internal static pressure.  If no internal static is provided, fan power is calculated using:
-
-<div>$$FanPowerCorrection = {\dot V_{RatedHighSpeed}}*773.3$$</div>
-
-If the internal static pressure is provided, then the entire VAV fan model in EnergyPlus is evaluated at the rated high speed air flow rate and the total static pressure for rating and the then the fan power calculated by the fan model is used for the fan power correction.
-
-<span>\(TotCapTempModFa{c_{Rated}}\)</span> = Total Cooling Capacity Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
-
-<span>\(EIRTempModFa{c_{Rated}}\)</span> = Energy Input Ratio Function of Temperature Curve evaluated with 19.44°C wet-bulb temperature air entering the cooling coil and 35.0°C dry-bulb temperature air entering the air-cooled (outdoor) condenser (dimensionless)
-
-The Integrated Energy Efficiency Ratio (IEER) is intended to be a measure of merit for the cooling coil’s part-load efficiency. IEER replaced Integrated Part-Load Value (IPLV) as the part-load performance metric in Std. 340/360 as of January 1, 2010. Full details regarding the IEER calculation are available in ANSI/AHRI Std. 340/360 (AHRI 2007). A summary of the IEER calculations made by EnergyPlus for two-speed air-cooled DX cooling coils is provided below:
-
-<div>$$IEER = \,(0.02 \cdot EE{R_A}) + (0.617 \cdot EE{R_B}) + (0.238 \cdot EE{R_C}) + (0.125 \cdot EE{R_D})$$</div>
-
-where,
-
-<span>\(EE{R_A}\)</span> =     *EER* at 100% net capacity at AHRI standard rating conditions (same as EER calculation shown above but in Btu/h)
-
-<span>\(EE{R_B}\)</span> =     *EER* at 75% net capacity and reduced outdoor air temperature Btu/h
-
-<span>\(EE{R_C}\)</span> =     *EER* at 50% net capacity and reduced outdoor air temperature Btu/h
-
-<span>\(EE{R_D}\)</span>=      *EER* at 25% net capacity and reduced outdoor air temperature Btu/h
-
-The following table summarizes the test points.
-
-Table 58.  Test points for Two-Speed DX Coil Ratings
-
-<table class="table table-striped">
-  <tr>
-    <th>Point</th>
-    <th>Net Capacity</th>
-    <th>Coil inlet wetbulb</th>
-    <th>Coil inlet drybulb</th>
-    <th>Condenser inlet drybulb</th>
-    <th>Supply air flow rate</th>
-  </tr>
-  <tr>
-    <td>A</td>
-    <td>100%</td>
-    <td>19.4C</td>
-    <td>26.7C</td>
-    <td>35.0C</td>
-    <td>Rated High speed flow rate</td>
-  </tr>
-  <tr>
-    <td>B</td>
-    <td>75%</td>
-    <td>19.4C</td>
-    <td>26.7C</td>
-    <td>27.5C</td>
-    <td rowspan="3">Regula falsi result where coil leaving drybulb matches Point A</td>
-  </tr>
-  <tr>
-    <td>C</td>
-    <td>50%</td>
-    <td>19.4C</td>
-    <td>26.7C</td>
-    <td>20.0C</td>
-  </tr>
-  <tr>
-    <td>D</td>
-    <td>25%</td>
-    <td>19.4C</td>
-    <td>26.7C</td>
-    <td>18.3C</td>
-  </tr>
-</table>
-
-The units are assumed to be VAV and Standard 340/360 is be applied as for VAV indoor supply fan.  Because the standard stipulates “the airflow rate at part load should be adjusted to maintain the full load measured leaving dry-bulb temperature,� the part load rating test points “B�, “C�, and “D� are evaluated by using the entire DX coil model calculations to obtain the supply air conditions leaving the coil and iterating on supply air flow rate to find the supply air flow rate.  The numerical method called Regula Falsi is used to find the supply flow rate at each of the part load test points.  Once the supply air flow rate is known, the two-speed DX coil model results are used to determine EER at the part load test points.
-
-When evaluating the two-speed DX coil model, the speed ratio and cycling ratio are specified based on the desired or target net capacity.  When the low speed net capacity is lower than the target part load net capacity, the speed ratio is calculated using
-
-<div>$$SpeedRatio = \frac{{DesiredNetCapacity - LowSpeedNetCapacity}}{{HighSpeedNetCapacity - LowSpeedNetCapacity}}$$</div>
-
-When the low speed net capacity is higher than a target part load net capacity then the unit must cycle to meet the lower load.  The speed ratio is then set to 0.0 (minimum unloading) and the cycling ratio is calculated using
-
-<div>$$CyclingRatio = \frac{{DesiredNetCapacity}}{{LowSpeedNetCapacity}}$$</div>
-
-The results for EER, COP, and supply air mass flow rate at the part load test points are reported to the EIO file and a predefined table report called VAV DX Cooling Standard Rating Details.
-
-#### References
-
-See the references for the single speed DX cooling coil earlier in this document.
-
-### Variable Speed DX Cooling Coil
-
-#### Overview
-
-The Coil:Cooling:DX:VariableSpeed object will simulate the performance of a DX cooling coil used in combination with a variable-speed unitary air conditioner and air-to-air heat pump. It fits into the parent objects of AirLoopHVAC:UnitaryHeatCool, ZoneHVAC:PackagedTerminalAirConditioner, AirLoopHVAC:UnitaryHeatPump:AirToAir and ZoneHVAC:PackagedTerminalHeatPump, etc.
-
-The rated conditions for obtaining the capacities, COPs and SHR  are indoor dry-bulb temperature at 26.67 ˚C (80 ˚F), wet bulb temperature at 19.44 ˚C (67 ˚F),  and the source side entering air temperature at 35 ˚C (95 ˚F).
-
-Variable-speed cooling coils lead to varied dehumidification behaviors, that the Bypass Factor (BF) is not only dependent on the indoor air flow rate, but also on the refrigerant mass flow rate, i.e. the compressor speed. The methods of calculating Bypass factor and Sensible Heat Transfer Ratio at each speed are the same as the water source variable-speed cooling coil (object name Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit).
-
-#### Model Description
-
-The Coil:Cooling:DX:VariableSpeed object is modeled in a manner similar to Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit. Of course, rather than referencing a water-cooled condenser, the new coil object references to outdoor air-cooled condenser, and has the air entering temperature in place of the condenser water entering temperature.
-
-It shall be noted for the total cooling capacity and flow rate inputs, two fields are autosizable, which are Rated Total Cooling Capacity at Selected Nominal Speed Level and Rated Volumetric Air Flow Rate at Selected Nominal Speed Level. They are used to scale the performances of an actual unit and correlate with the actual loop flow. Except the two fields, all other total cooling capacity and flow rate inputs at individual speed levels should be directly obtained from Reference Unit catalog.
-
-The Rated Total Cooling Capacity at Selected Nominal Speed Level contains the rated total cooling capacity to match the building sensible or latent cooling load.  The rated cooling capacity is used to determine a capacity scaling factor, as compared to the Reference Unit catalog capacity at the nominal speed level.
-
-<div>$${\rm{CapacityScaleFactor}} = \frac{{{\rm{RatedTotalCoolingCapacity}}}}{{{\rm{ReferenceUnitTotalCoolingCapacity}}@{\rm{NominalSpeedLevel}}}}$$</div>
-
-And then, this scaling factor is used to determine capacities at rated condition for other speed levels, as below,
-
-<div>$${\rm{RatedTotalCoolingCapacity}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = {\rm{CapacityScaleFactor}} \times {\rm{ReferenceUnitTotalCoolingCapacity}}@{\rm{SpeedLevel}}({\rm{x}})$$</div>
-
-The Rated Volumetric Air Flow Rate is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects, as follows:
-
-<div>$${\rm{AirFlowScaleFactor}} = \frac{{{\rm{RatedVolumetricAirFlowRate}}}}{{{\rm{ReferenceUnitVolAirFlowRate}}@{\rm{NominalSpeedLevel}} \times {\rm{CapacityScaleFactor}}}}$$</div>
-
-And the loop volumetric air flow rates in the parent objects are calculated as below,
-
-<div>$${\rm{LoopVolumetricAirFlowRate}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = {\rm{AirFlowScaleFactor}} \times {\rm{ReferenceUnitVolAirFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) \times {\rm{CapacityScaleFactor}}$$</div>
-
-If the volumetric air flow rate at one speed level is higher than the flow rate allowed by the fan in the parent object, the flow rate will be set back to the fan flow rate.
-
-If <span>\({\rm{AirFlowScaleFactor}}\)</span> equals to unity, the loop air flow rate become the design flow rates of the original unit (after scaled by the rated total cooling capacity). The Rated Volumetric Air Flow Rate is introduced here to correlate with the actual flow rate in the air loop, in case that these differ from the design specifications. Certainly, it is recommended that the Rated Volumetric Air Flow Rate is selected in the way that <span>\({\rm{AirFlowScaleFactor}}\)</span> is unity, so as to get more accurate results from the performance curves.
-
-If the condenser is evaporatively cooled, it is necessary to know the condenser air flow rate, so as to calculate the water evaporation rate. We will have fields for specifying the Reference Unit condenser volumetric air flow rates at individual speed levels, and these inputs are optional. If the condenser air flow rates are not inputted by the user, default values of condenser volumetric air flow rate as a function of the rated total cooling capacity will be used. Condenser air flow rates of the simulated unit are calculated as below,
-
-<div>$$\begin{array}{l}{\rm{CondenserVolumetricAirFlowRate}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = \\\quad \quad {\rm{ReferenceUnitCondenserVolAirFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) \times \\\quad \quad \quad {\rm{CapacityScaleFactor}}\end{array}$$</div>
-
-#### Performance Curves:
-
-This object includes 4 curve objects at each individual speed level.
-
-1)  Total cooling capacity modifier curve (function of temperature)
-
-2)  Total cooling capacity modifier curve (function of air flow fraction)
-
-3)  Energy input ratio (EIR) modifier curve (function of temperature)
-
-4)  Energy input ratio (EIR) modifier curve (function of air flow fraction)
-
-The flow fraction modifier curves are used as a placeholder, to account for off-design flow rates if needed. If the manufacturer doesn’t provide the off-design performances, we can simply use a default modification multiplier of 1.0.
-
-At the lowest speed, there will be one additional performance curve to correlate the part-load condition, i.e.
-
-5) Part load fraction correlation (function of part load ratio)
-
-1)     Total cooling capacity modifier curve (function of temperature)
-
-The total cooling capacity modifier as a function of temperature curve (CAP-FT) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil and the condenser entering air temperature. The output of this curve is multiplied by the rated total cooling capacity at the speed, to give the total cooling capacity at the specific entering air WB and condenser inlet air DB at which the DX unit is operating (i.e., at temperatures different from the rating point temperatures).
-
-Note: The data used to develop the total cooling capacity modifier curve (function of temperature) should represent performance when the cooling coil is ‘wet’ (i.e., coil providing sensible cooling and at least some dehumidification). Performance data when the cooling coil is ‘dry’ (i.e., not providing any dehumidification) should not be included when developing this modifier curve. This model automatically detects and adjusts for ‘dry coil’ conditions.
-
-<div>$${\rm{TotCapTempModFac}} = {\rm{a}} + {\rm{b*W}}{{\rm{B}}_{\rm{i}}} + {\rm{c*WB}}_{\rm{i}}^2 + {\rm{d*D}}{{\rm{B}}_{\rm{o}}} + {\rm{e*D}}{{\rm{B}}_{\rm{o}}}^2 + {\rm{f*W}}{{\rm{B}}_{\rm{i}}}{\rm{*D}}{{\rm{B}}_{\rm{o}}}$$</div>
-
-where
-
-WB<sub>i</sub> = wet-bulb temperature of the air entering the indoor cooling coil, °C
-
-DB<sub>o</sub> = dry-bulb temperature of the air entering the condenser coil, °C
-
-a-f = regression curve-fit coefficients.
-
-2)     Total cooling capacity modifier curve (function of air flow fraction)
-
-The total cooling capacity modifier curve (function of air flow fraction) is a cubic curve with the independent variable being the ratio of the actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of design flow at the speed).
-
-<div>$${\rm{TotCapAirFlowModFac}} = {\rm{a}} + {\rm{b*f}}{{\rm{f}}_{\rm{a}}} + {\rm{c*ff}}_{\rm{a}}^2 + {\rm{d*ff}}_{\rm{a}}^3$$</div>
-
-where
-
-ff<sub>a</sub> = actual air mass flow rate/design air mass flow rate, at one speed level.
-
-          <span>\(\begin{array}{l}{\rm{DesignAirMassFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) = {\rm{}}\\\quad \quad \quad {\rm{ReferenceUnitAirMassFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) \times {\rm{CapacityScaleFactor}}\end{array}\)</span>
-
-a-d = regression curve fit coefficients, if no data for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-3) Energy input ratio (EIR) modifier curve (function of temperature)
-
-The energy input ratio modifier curve as a function of temperature (EIR-FT) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil and the condenser entering air temperature. The output of this curve is multiplied by the rated EIR (inverse of the rated COP) at the speed level, to give the EIR at the specific entering air temperatures at which the DX unit is operating (i.e., at temperatures different from the rating point temperatures).
-
-<div>$${\rm{EIRTempModFac}} = {\rm{a}} + {\rm{b*W}}{{\rm{B}}_{\rm{i}}} + {\rm{c*WB}}_{\rm{i}}^2 + {\rm{d*D}}{{\rm{B}}_{\rm{o}}} + {\rm{e*D}}{{\rm{B}}_{\rm{o}}}^2 + {\rm{f*W}}{{\rm{B}}_{\rm{i}}}{\rm{*D}}{{\rm{B}}_{\rm{o}}}$$</div>
-
-where
-
-a-f = regression curve fit coefficients
-
-4) Energy input ratio (EIR) modifier curve (function of air flow fraction)
-
-<div>$${\rm{EIRAirFlowModFac}} = {\rm{a}} + {\rm{b*f}}{{\rm{f}}_{\rm{a}}} + {\rm{c*ff}}_{\rm{a}}^2 + {\rm{d*ff}}_{\rm{a}}^3$$</div>
-
-where
-
-a-d = regression curve fit coefficients, if no data available for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-5) Part load fraction correlation (function of part load ratio)
-
-This field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, Sensible or Latent Load/Steady-State Sensible or Latent Capacity  for Speed 1). The description of the part load fraction correlation for the variable-speed DX cooling coil is similar to the variable-speed DX heating coil.
-
-#### Lowest Speed Operation:
-
-The lowest speed operation of the variable-speed DX cooling coil is similar to the single speed DX cooling coil. The total (gross) cooling capacity of the variable-speed DX coil is calculated as follows:
-
-<div>$$\begin{array}{l}{{\rm{Q}}_{{\rm{total}},1}} = {\rm{RatedTotalCoolingCapacity}}@{\rm{SpeedLevel}}\left( 1 \right){\rm{*}}\\\quad \quad {\rm{TotCapTempModFa}}{{\rm{c}}_1}{\rm{*TotCapAirFlowModFa}}{{\rm{c}}_1}\end{array}$$</div>
-
-And the EIR is calculated as:
-
-<div>$${\rm{EI}}{{\rm{R}}_1} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}(1)}}{\rm{EIRTempModFa}}{{\rm{c}}_1}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_1}$$</div>
-
-And the power consumption excluding the indoor fan is,
-
-<div>$${\rm{Powe}}{{\rm{r}}_1} = {{\rm{Q}}_{{\rm{total}},1}}{\rm{*EI}}{{\rm{R}}_1}{\rm{*RTF}}$$</div>
-
-At the lowest speed, the dehumidification calculation is exactly the same as the single speed DX coil. That is to use the rated SHR and the design air flow rate at the lowest speed to calculate rated bypass factor of BF<sub>rated,1</sub>, and the corresponding effective surface area of A<sub>o,1</sub>. With A<sub>o,1</sub><sub></sub>known, the coil BF can be adjusted for non-rated air flow rates.
-
-And the part load ratio for sensible cooling is,
-
-<div>$${\rm{PLR}} = {\rm{SensibleCoolingLoad}}/({{\rm{Q}}_{{\rm{total}},1}}{\rm{*SH}}{{\rm{R}}_1})$$</div>
-
-For latent cooling,
-
-<div>$${\rm{PLR}} = {\rm{LatentCoolingLoad}}/[{{\rm{Q}}_{{\rm{total}},1}}{\rm{*}}(1.0 - {\rm{SH}}{{\rm{R}}_1})]$$</div>
-
-#### Higher Speed Operation:
-
-At the speed level between the lowest and the highest, there is no part-load loss. A parameter of speed ratio (SpeedRatio) is used to define the capacity partition between Speed x-1 and Speed x.
-
-The design air flow rate at the speed ratio are given as following:
-
-<div>$$\begin{array}{l}{\rm{DesignAirFlowRateSpeedRatio}} = {\rm{ReferenceUnitAirMassFlowRate}}@{\rm{SpeedLevel}}\left( {{\rm{x}} - 1} \right){\rm{*}}\\\quad \quad \quad {\rm{CapacityScaleFactor*}}\left( {1{\rm{}}--{\rm{SpeedRatio}}} \right) + \\\quad \quad {\rm{ReferenceUnitAirMassFlowRate}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right){\rm{*}}\\\quad \quad \quad {\rm{CapacityScaleFactor*SpeedRatio}}\end{array}$$</div>
-
-And the fraction of air flow is given:
-
-<span>\({\rm{f}}{{\rm{f}}_{{\rm{a}},{\rm{x}} - 1}}\)</span>=<span>\({\rm{f}}{{\rm{f}}_{{\rm{a}},{\rm{x}}}}\)</span>= actual air mass flow rate/DesignAirFlowRateSpeedRatio
-
-The total cooling capacities and EIRs at Speed x-1 and Speed x are calculated:
-
-<div>$$\begin{array}{l}{{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}} = {\rm{RatedTotalCoolingCapacity}}@{\rm{SpeedLevel}}\left( {{\rm{x}} - 1} \right){\rm{*}}\\\quad \quad \quad {\rm{TotCapTempModFa}}{{\rm{c}}_{{\rm{x}} - 1}}{\rm{*TotCapAirFlowModFa}}{{\rm{c}}_{{\rm{x}} - 1}}\end{array}$$</div>
-
-<div>$$\begin{array}{l}{{\rm{Q}}_{{\rm{total}},{\rm{x}}}} = {\rm{RatedTotalCoolingCapacity}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right){\rm{*}}\\\quad \quad \quad {\rm{TotCapTempModFa}}{{\rm{c}}_{\rm{x}}}{\rm{*TotCapAirFlowModFa}}{{\rm{c}}_{\rm{x}}}\end{array}$$</div>
-
-<div>$${\rm{EI}}{{\rm{R}}_{{\rm{x}} - 1}} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}({\rm{x}} - 1)}}{\rm{EIRTempModFa}}{{\rm{c}}_{{\rm{x}} - 1}}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_{{\rm{x}} - 1}}$$</div>
-
-<div>$${\rm{EI}}{{\rm{R}}_{\rm{x}}} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}\left( {\rm{x}} \right)}}{\rm{EIRTempModFa}}{{\rm{c}}_{\rm{x}}}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_{\rm{x}}}$$</div>
-
-The total cooling capacity at the corresponding speed ratio is:
-
-<div>$${{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}} = \left( {1.0 - {\rm{SpeedRatio}}} \right){\rm{*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}} + {\rm{SpeedRatio*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}}}}$$</div>
-
-And the power consumption, excluding the indoor fan, is
-
-<div>$${\rm{Powe}}{{\rm{r}}_{{\rm{SpeedRatio}}}} = \left( {1.0 - {\rm{SpeedRatio}}} \right){\rm{*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}}{\rm{*EI}}{{\rm{R}}_{{\rm{x}} - 1}} + {\rm{SpeedRatio*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}}}}{\rm{*EI}}{{\rm{R}}_{\rm{x}}}$$</div>
-
-And the net heat discharged from the condenser:
-
-<div>$${{\rm{Q}}_{{\rm{cond}},{\rm{SpeedRatio}}}} = {\rm{Powe}}{{\rm{r}}_{{\rm{SpeedRatio}}}} + {{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}}$$</div>
-
-And the effective surface area in the correlations of BF factor is calculated as below:
-
-<div>$${{\rm{A}}_{{\rm{o}},{\rm{SpeedRatio}}}} = \left( {1 - {\rm{SpeedRatio}}} \right){\rm{*}}{{\rm{A}}_{{\rm{o}},{\rm{x}} - 1}} + {\rm{SpeedRatio*}}{{\rm{A}}_{{\rm{o}},{\rm{x}}}}$$</div>
-
-Using A<sub>o,SpeedRatio</sub> in the same BF and SHR calculation procedure as the single speed DX cooling coil, we can get BF<sub>SpeedRatio</sub>, and SHR<sub>SpeedRatio</sub>. And the sensible cooling capacity is calculated:
-
-<div>$${{\rm{Q}}_{{\rm{sensible}},{\rm{SpeedRatio}}}} = {{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}}{\rm{*SH}}{{\rm{R}}_{{\rm{SpeedRatio}}}}$$</div>
-
-If the variable-speed DX cooling coil used to match the sensible cooling load,
-
-<div>$${{\rm{Q}}_{{\rm{sensible}},{\rm{SpeedRatio}}}} = {\rm{SensibleLoad}}$$</div>
-
-If it intends to match the latent cooling load,
-
-<div>$${{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}}{\rm{*}}\left( {1.0 - {\rm{SH}}{{\rm{R}}_{{\rm{SpeedRatio}}}}} \right) = {\rm{LatentLoad}}$$</div>
-
-If the speed reaches the highest level, the speed ratio becomes 1.0, and Speed n represents the highest speed.
-
-#### Evaporatively Cooled Condenser:
-
-If using evaporative pre-cooling pad upstream of the condenser, the user must also enter the appropriate evaporative effectiveness for the media at each compressor speed, so as to correlate variation of the effectiveness as a function of compressor speed, i.e. the variation of condenser air flow rate. The evaporative effectiveness is interpolated between speed levels, i.e.
-
-<div>$${\rm{Effectivenes}}{{\rm{s}}_{{\rm{SpeedRatio}}}} = \left( {1.0 - {\rm{SpeedRatio}}} \right){\rm{*Effectivenes}}{{\rm{s}}_{{\rm{x}} - 1}} + {\rm{SpeedRatio*Effectivenes}}{{\rm{s}}_{\rm{x}}}$$</div>
-
-The interpolated effectiveness at the speed ratio is used to calculate the air temperature reduction across the evaporative cooling pad, and the decreased air temperature entering the condenser coil is used in place of the ambient temperature, i.e.
-
-<div>$${{\rm{T}}_{{\rm{c}},{\rm{i}}}} = {{\rm{T}}_{{\rm{wb}},{\rm{o}}}} + (1.0 - {\rm{Effectivenes}}{{\rm{s}}_{{\rm{SpeedRatio}}}}){\rm{*}}({{\rm{T}}_{{\rm{db}},{\rm{o}}}} - {{\rm{T}}_{{\rm{wb}},{\rm{o}}}})$$</div>
-
-Where
-
-<span>\({{\rm{T}}_{{\rm{c}},{\rm{i}}}}\)</span> is the condenser entering air temperature, °C.
-
-<span>\({{\rm{T}}_{{\rm{wb}},{\rm{o}}}}\)</span> is the outdoor air wet bulb temperature, °C.
-
-<span>\({{\rm{T}}_{{\rm{db}},{\rm{o}}}}\)</span> is the outdoor air dry bulb temperature, °C.
-
-And the water consumption rate is calculated based on the interpolated condenser air flow rate at the speed ratio, i.e. the condenser flow rate at the speed ratio,
-
-<div>$${\dot m_{condair,{\rm{}}SpeedRatio}} = \left( {1.0 - SpeedRatio} \right){\rm{*}}{\dot m_{condair,{\rm{}}x - 1}} + SpeedRatio{\rm{*}}{\dot m_{condair,{\rm{}}x}}$$</div>
-
-### Electric Air Heating Coil
-
-The electric air heating coil (object name: Coil:Heating:Electric) is a simple capacity model with a user-input efficiency.  In many cases, this efficiency for the electric coil will be 100%.  This coil only has air nodes to connect it in the system.  The coil can be used in the air loop simulation or in the zone equipment as a reheat coil.  Depending on where it is used determines if this coil is temperature or capacity controlled.  If used in the air loop simulation it will be controlled to a specified temperature on the setpoint node by the SetpointManager.  If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand.  See Input Output Reference for additional information.
-
-For a coil that is controlled to meet the zone demand and will meet the capacity necessary for that zone unless it exceeds the capacity of the coil specified by the user.
-
-  ! Control output to meet load QCoilReq
-
-  IF((AirMassFlow .GT. 0.0 .AND. HeatingCoil(CoilNum)%NominalCapacity &gt; 0.0) .and. &
-
-     (GetCurrentScheduleValue(HeatingCoil(CoilNum)%SchedPtr) .gt. 0.0) .and. &
-
-     (QCoilReq .gt. 0.0) .and. (TempSetPoint == 0.0)) THEN
-
-      !check to see if the Required heating capacity is greater than the user! specified capacity.
-
-      IF(QCoilReq &gt; HeatingCoil(CoilNum)%NominalCapacity) Then
-
-        QCoilCap = HeatingCoil(CoilNum)%NominalCapacity
-
-      Else
-
-        QCoilCap = QCoilReq
-
-      End IF
-
-
-
-      TempAirOut=TempAirIn + QCoilCap/CapacitanceAir
-
-      HeatingCoilLoad = QCoilCap
-
-
-
-     !The HeatingCoilLoad is the change in the enthalpy of the Heating
-
-      HeatingCoil(CoilNum)%ElecUseLoad = HeatingCoilLoad/Effic
-
-For a temperature setpoint coil the delta temperature from the coil inlet temperature to the setpoint is determined and the capacity of the coil is calculated and is met if less than the user specified capacity.
-
-   ! Control coil output to meet a setpoint temperature.
-
-   Else IF((AirMassFlow .GT. 0.0 .AND. HeatingCoil(CoilNum)%NominalCapacity &gt; 0.0) .and. &
-
-     (GetCurrentScheduleValue(HeatingCoil(CoilNum)%SchedPtr) .gt. 0.0) .and. &
-
-     (QCoilReq == 0.0) .and. &
-
-     (ABS(TempSetPoint-TempAirIn) .gt. TempControlTol) ) THEN
-
-      QCoilCap = CapacitanceAir\*(TempSetPoint - TempAirIn)
-
-      ! check to see if setpoint above enetering temperature. If not, set
-
-      ! output to zero.
-
-      IF(QCoilCap .LE. 0.0) THEN
-
-        QCoilCap = 0.0
-
-        TempAirOut = TempAirIn
-
-      !check to see if the Required heating capacity is greater than the user
-
-      ! specified capacity.
-
-      Else IF(QCoilCap &gt; HeatingCoil(CoilNum)%NominalCapacity) Then
-
-        QCoilCap = HeatingCoil(CoilNum)%NominalCapacity
-
-        TempAirOut=TempAirIn + QCoilCap/CapacitanceAir
-
-      Else
-
-        TempAirOut = TempSetPoint
-
-      End IF
-
-
-
-      HeatingCoilLoad = QCoilCap
-
-
-
-     !The HeatingCoilLoad is the change in the enthalpy of the Heating
-
-      HeatingCoil(CoilNum)%ElecUseLoad = HeatingCoilLoad/Effic
-
-### Gas Air Heating Coil
-
-The gas-powered heating coil (object name: Coil:Heating:Gas) is a simple capacity model with user inputted gas burner efficiency.  The default for the gas burner efficiency is 80%.  This coil only has air nodes to connect it in the system.  The coil can be used in the air loop simulation or in the zone equipment as a reheat coil.  Depending on where it is used determines if this coil is temperature or capacity controlled.  If used in the air loop simulation it will be controlled to a specified temperature scheduled from the SetpointManager.  If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand.  The gas coil has additional features that can add a part load correction and a parasitic gas or electric load.
-
-The parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.  This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation time step.
-
-The parasitic gas load associated with the gas coil’s operation (Watts), such as a standing pilot light.  The model assumes that this parasitic load is consumed only for the portion of the simulation time step where the gas heating coil is not operating.
-
-#### Field: Part Load Fraction Correlation (function of part load ratio)
-
-The part load correction defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of gas consumption rate by the heating coil as a function of the part load ratio (PLR, sensible heating load/nominal capacity of the heating coil).  For any simulation time step, the nominal gas consumption rate (heating load/burner efficiency) is divided by the part-load fraction (PLF) if a part-load curve has been defined.  The part-load curve accounts for efficiency losses due to transient coil operation.
-
-The part-load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the heating coil runs continuously for the simulation time step).  For PLR values between 0 and 1 ( 0 &lt;= PLR &lt; 1), the following rules apply:
-
-**PLF &gt;= 0.7   and   PLF &gt;= PLR**
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds.  The runtime fraction of the heating coil is defined a PLR/PLF. If PLF &lt; PLR, then a warning message is issues and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional gas heating coil (e.g., residential furnace) would be:
-
-<div>$$PLF = 0.8 + 0.2\cdot PLR$$</div>
-
-For a better understanding of how the coil meets the temperature setpoint in the air loop or the zone demand as zone equipment, see Coil:Electric:Heating for additional information.  Also see Input Output Reference for additional input information.
-
-### Multi-Stage Electric and Gas Air Heating Coil
-
-#### Overview
-
-These models (object names Coil:Heating:Electric:MultiStage and Coil:Heating:Gas:MultiStage) simulate the performance of multi stage electric and gas heating systems with two to four discrete air flow stages. Each stage has a set of user inputted gas burner efficiency, Nominal capacity, and Parasitic electric load (for gas coil only). The full load supply airflow rate is dependent on the stage number and is set by its parent object (Ref: AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed). The part-load impact on coil energy use is automatically applied to the lowest stage.
-
-When the model determines performance at Stage 1 (the lowest stage) or cycling between OFF and Stage 1, its performance is almost the same as the performance for the Coil:Heating:Electric and  Coil:Heating:Gas models. However, the outlet conditions are calculated slightly differently. Therefore, the Coil:Heating:Electric and  Coil:Heating:Gas model may be considered as subsets of the multistage model described here. When the multistage coil model determines performance at higher stages (above 1), the model linearly interpolates the performance at two consecutive stages (n-1 and n) as needed to meet the heating load, with the fraction of time at each speed established by the speed ratio. For the time being, this coil model can only be called by the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
-
-#### Model Inputs
-
-The model inputs are also very similar to the inputs of the Coil:Heating:Electric and  Coil:Heating:Gas objects. The main difference is that this multistage model requires a set of fields at each speed, such as nominal capacity, and efficiency.
-
-#### Stage 1 Operation
-
-The following procedure provides the detailed description of the exception.
-
-n Total delivered heating capacity
-
-The total delivered heating capacity for Stage 1 operating at the cycling ratio needed to meet the requested heating load is:
-
-<div>$${Q_{coil,cycling}} = {\mathop m\limits^\cdot_{Speed\,1}}\left( {CycRatio} \right)({h_{inlet}} - {h_{outlet,full}})$$</div>
-
-where,
-
-*Q<sub>coil,cycling</sub>*      = delivered sensible heating capacity for Stage 1 operating at a specific cycling ratio [W]
-
-<span>\({\mathop m\limits^\cdot_{Speed\,\,1}}\)</span>      = air mass flow rate through heating coil at Speed 1 as set by the parent object [kg/s]
-
-*h<sub>outlet,full</sub>*      = specific enthalpy of the coil outlet air during full-load operation at Stage 1 (no cycling) [J/kg]
-
-*h<sub>inlet</sub>           *            = specific enthalpy of the coil inlet air [J/kg]
-
-*CycRatio*    = cycling ratio at Stage 1, ratio of requested heating load to the full-load capacity of the coil at Stage 1 [dimensionless]
-
-It is assumed that the coil provides no heating capacity when the coil is OFF, even if the supply air fan continues to operate.
-
-n Outlet air specific enthalpy
-
-The average specific enthalpy of the coil outlet air is then calculated based on the delivered sensible heating capacity and the average air mass flow rate entering the coil:
-
-<div>$${h_{outlet,average}} = {h_{inlet}} - {{\raise0.7ex\hbox{${{Q_{coil,cycling}}}$} \!\mathord{\left/ {\vphantom {{{Q_{coil,cycling}}} {\mathop m\limits^\cdot  }}}\right.}\!\lower0.7ex\hbox{${\mathop m\limits^\cdot  }$}}_{inlet}}$$</div>
-
-where,
-
-*h<sub>outlet,average</sub>*  = average specific enthalpy at the coil outlet [J/kg]
-
-<span>\({\mathop m\limits^\cdot_{inlet}}\)</span>         = mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiStage, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the heating coil is ON and the specified flow rate when the heating coil is OFF for the time step being simulated.
-
-n Outlet air temperature
-
-The heating coil’s outlet air humidity ratio equals the inlet air humidity ratio since the coil does not change the moisture content of the air. So the average outlet air temperature is calculated based on the inlet air humidity ratio and the average outlet air enthalpy using the psychrometric function PsyTdbFnHW.
-
-The main reason for using the above approach is that outlet air conditions are calculated in the same way for all operating Stages.
-
-#### Higher Stage Operation
-
-This section describes how higher Stage operation is simulated. When the required sensible load is less than the full load sensible capacity at Stage n (Stage Number &gt; 1), the following calculations are performed:
-
-n Total delivered heating capacity at Stage n-1 and Stage n
-
-<div>$$TotCa{p_{n - 1}} = MSNominalCa{p_{n - 1}}$$</div>
-
-<div>$$TotCa{p_n} = MSNominalCa{p_n}$$</div>
-
-where,
-
-*TotCap<sub>i</sub>*<sub>           </sub> = total delivered heating capacity at given temperatures and flow rates at Stage i [W]
-
-*MSNominalCap<sub>i</sub>*<sub>        </sub> = heating capacity at the rated conditions at Stage i [W]
-
-i     = Stage n or Stage n-1
-
-n Full load outlet air specific enthalpy at Stage n-1 and Stage n
-
-<div>$${h_{outlet,full\_Speed\_n}} = {h_{inlet}} - (MSNominalCa{p_n}/{\mathop m\limits^._{inlet}})$$</div>
-
-<div>$${h_{outlet,full\_Speede\_n - 1}} = {h_{inlet}} - (MSNominalCa{p_{n - 1}}/{\mathop m\limits^._{inlet}})$$</div>
-
-
-
-where,
-
-*h<sub>outlet,full\_Stage\_n</sub>*         = specific enthalpy of the coil outlet air during full-load operation at Stage n (no cycling) [J/kg]
-
-*h<sub>outlet,full\_Stage\_n-1</sub>*       = specific enthalpy of the coil outlet air during full-load operation at Stage n-1 (no cycling) [J/kg]
-
-n Effective total heating capacity
-
-<div>$$\begin{array}{l}{Q_{coil,SpeedRatio}} = \left( {SpeedRatio} \right){\mathop m\limits^\cdot_{Speed\,n}}({h_{inlet}} - {h_{outlet,full\_Speed\,n}})\\\;\;\;\;\;\;\;\;\;\; + (1 - SpeedRatio){\mathop m\limits^\cdot_{Speed\,n - 1}}({h_{inlet}} - {h_{outlet,full\_Speed\,n - 1}})\end{array}$$</div>
-
-where,
-
-<span>\({{Q_{coil,SpeedRatio}}}\)</span><sub>                       </sub> = delivered sensible heating capacity at a given Stage ratio between two consecutive Stages [W]
-
-<span>\({\mathop {{\rm{ }}m}\limits_{Speed{\kern 1pt} n}^ \cdot  }\)</span>      = air mass flow rate through heating coil at Stage n as set by the parent object [kg/s]
-
-<span>\({\mathop {{\rm{ }}m}\limits_{Speed{\kern 1pt} n - 1}^ \cdot  }\)</span>    = air mass flow rate through heating coil at Stage 1 as set by the parent object [kg/s]
-
-
-
-n Average outlet air enthalpy
-
-<div>$${h_{outlet,average}} = {h_{inlet}} - {{\raise0.7ex\hbox{${{Q_{coil,SpeedRatio}}}$} \!\mathord{\left/ {\vphantom {{{Q_{coil,SpeedRatio}}} {\mathop m\limits^\cdot  }}}\right.}\!\lower0.7ex\hbox{${\mathop m\limits^\cdot  }$}}_{inlet}}$$</div>
-
-where,
-
-*h<sub>outlet,average</sub>*  = average specific enthalpy at the coil outlet [J/kg]
-
-*h<sub>inlet</sub>           *            = specific enthalpy of the coil inlet air [J/kg]
-
-<span>\({\dot m_{inlet}}\)</span>         = Mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiStage, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the heating coil is at Stage n and the specified flow rate when the heating coil is at Stage n-1 for the time step being simulated.
-
-n Average outlet air temperature
-
-The heating coil’s outlet air humidity ratio equals the inlet air humidity ratio since the coil does not change the moisture content of the air. So the average outlet air temperature is calculated based on the inlet air humidity ratio and the average outlet air enthalpy using the psychrometric function PsyTdbFnHW.
-
-n Full load energy inputs at Stage n-1 and Stage n
-
-<div>$$HeatingPowe{r_n} = MSNominalCa{p_n}/MSEfficienc{y_n}$$</div>
-
-<div>$$HeatingPowe{r_{n - 1}} = MSNominalCa{p_{n - 1}}/MSEfficienc{y_{n - 1}}$$</div>
-
-where,
-
-*MSEfficiency<sub>n</sub>*        = Efficiency at stage n
-
-*MSEfficiency<sub>n-1</sub>*      = Efficiency at stage n-1
-
-n Calculate combined energy input
-
-<div>$$HeatingPower = HeatingPowe{r_n}\left( {SpeedRatio} \right) + HeatingPowe{r_{n - 1}}(1.0 - SpeedRatio)$$</div>
-
-where,
-
-HeatingPower          = Power used in Watt
-
-### Single-Speed Electric Heat Pump DX Air Heating Coil
-
-#### Overview
-
-This model (object name Coil:Heating:DX:SingleSpeed) simulates the performance of an air-to-air direct expansion (DX) heating system. The model uses performance information at rated conditions along with curve fits for variations in total capacity, energy input ratio and part-load fraction to determine the performance of the unit at part-load conditions (DOE 1982).  Adjustment factors are applied to total capacity and input power to account for frost formation on the outdoor coil.
-
-This model simulates the thermal performance of the indoor DX heating coil, and the power consumption of the outdoor unit (compressors, fans, crankcase heaters and defrost heaters). The performance of the indoor supply air fan varies widely from system to system depending on control strategy (e.g., constant fan vs. AUTO fan, constant air volume vs. variable air volume, etc.), fan type, fan motor efficiency and pressure losses through the air distribution system. Therefore, this DX system model does not account for the thermal effects or electric power consumption of the indoor supply air fan. EnergyPlus contains separate models for simulating the performance of various indoor fan configurations, and these models can be easily linked with the DX system model described here to simulate the entire DX system being considered (e.g., see AirLoopHVAC:UnitaryHeatPump:AirToAir).
-
-#### Model Inputs
-
-The user must input the total heating capacity, coefficient of performance (COP) and the volumetric airflow rate across the heating coil at rated conditions. The capacity and COP inputs should be “gross� values, excluding any thermal or energy impacts due to the indoor supply air fan. The rating condition is considered to be outdoor air at 8.33C dry-bulb and 6.11C wet-bulb temperatures (i.e., air entering the outdoor coil), with air entering the indoor DX heating coil at 21.11C dry-bulb and 15.55C wet-bulb temperatures. The rated volumetric air flow across the DX heating coil should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of rated total heating capacity (300 – 450 cfm/ton).
-
-Depending on the defrost strategy that is selected, the user must also input up to six performance curves that describe the change in total heating capacity and efficiency at part-load conditions, and efficiency during reverse-cycle defrosting:
-
-n The total heating capacity modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the rated total heating capacity to give the total heating capacity at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
-
-<div>$$TotCapTempModFac = \,a + \,b\left( {{T_{db,o}}} \right)\,\, + \,\,c{\left( {{T_{db,o}}} \right)^2}$$</div>
-
-or
-
-<div>$$TotCapTempModFac = \,a + \,b\left( {{T_{db,o}}} \right)\,\, + \,\,c{\left( {{T_{db,o}}} \right)^2}\,\, + \,\,d{\left( {{T_{db,o}}} \right)^3}$$</div>
-
-<div>$$TotCapTempModFac = \,a + \,b\left( {{T_{db,i}}} \right)\,\, + \,\,c{\left( {{T_{db,i}}} \right)^2}\,\, + \,\,d\left( {{T_{db,o}}} \right) + e{\left( {{T_{db,o}}} \right)^2} + f\left( {{T_{db,i}}} \right)\left( {{T_{db,o}}} \right)$$</div>
-
-where
-
-<span>\({T_{db,i}}\)</span>     = dry-bulb temperature of the air entering the indoor coil, °C
-
-<span>\({T_{db,o}}\)</span>     = dry-bulb temperature of the air entering the outdoor coil, °C
-
-n The total heating capacity modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated total heating capacity and the total heating capacity modifier curve (function of temperature) to give the total heating capacity at the specific temperature and air flow conditions at which the coil is operating.
-
-<div>$$TotCapFlowModFac = \,a + \,b\left( {ff} \right)\,\, + \,\,c{\left( {ff} \right)^2}$$</div>
-
-or
-
-<div>$$TotCapFlowModFac = \,a + \,b\left( {ff} \right)\,\, + \,\,c{\left( {ff} \right)^2}\,\, + \,\,d{\left( {ff} \right)^3}$$</div>
-
-where
-
-<div>$$ff = flow{\rm{ }}fraction = \left( {\frac{{Actual{\rm{ }}air{\rm{ }}mass{\rm{ }}flow{\rm{ }}rate}}{{Rated{\rm{ }}air{\rm{ }}mass{\rm{ }}flow{\rm{ }}rate}}} \right)$$</div>
-
-**Note:**  The actual volumetric airflow rate through the heating coil for any simulation time step where the DX unit is operating should be between 0.00002684 m<sup>3</sup>/s and .00008056 m<sup>3</sup>/s per watt of rated total heating capacity (200 - 600 cfm/ton). The simulation will issue a warning message if this airflow range is exceeded.
-
-n The energy input ratio (EIR) modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
-
-<div>$$EIRTempModFac = \,a + \,b\left( {{T_{db,o}}} \right)\,\, + \,\,c{\left( {{T_{db,o}}} \right)^2}$$</div>
-
-or
-
-<div>$$EIRTempModFac = \,a + \,b\left( {{T_{db,o}}} \right)\,\, + \,\,c{\left( {{T_{db,o}}} \right)^2}\,\, + \,\,d{\left( {{T_{db,o}}} \right)^3}$$</div>
-
-or
-
-<div>$$EIRTempModFac = \,a + \,b\left( {{T_{db,i}}} \right)\,\, + \,\,c{\left( {{T_{db,i}}} \right)^2}\,\, + \,\,d\left( {{T_{db,o}}} \right) + e{\left( {{T_{db,o}}} \right)^2} + f\left( {{T_{db,i}}} \right)\left( {{T_{db,o}}} \right)$$</div>
-
-n The energy input ratio (EIR) modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating.
-
-<div>$$EIRFlowModFac = \,a + \,b\left( {ff} \right)\,\, + \,\,c{\left( {ff} \right)^2}$$</div>
-
-or
-
-<div>$$EIRFlowModFac = \,a + \,b\left( {ff} \right)\,\, + \,\,c{\left( {ff} \right)^2}\, + \,\,d{\left( {ff} \right)^3}$$</div>
-
-n The part-load fraction correlation (function of part-load ratio) is a quadratic or cubic curve with the independent variable being part-load ratio (sensible heating load / steady-state heating capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the “effective� EIR for a given simulation time step. The part-load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
-
-<div>$$PartLoadFrac = \,PLF\, = \,a + \,b\left( {PLR} \right)\,\, + \,\,c{\left( {PLR} \right)^2}$$</div>
-
-or
-
-<div>$$PartLoadFrac = \,a + \,b\left( {PLR} \right)\,\, + \,\,c{\left( {PLR} \right)^2}\,\, + \,\,d{\left( {PLR} \right)^3}$$</div>
-
-where
-
-<div>$$PLR = part - load\,ratio = \left( {\frac{{sensible\,heating\,load}}{{steady - state\,sensible\,heating\,capacity}}} \right)$$</div>
-
-The part-load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation time step). For PLR values between 0 and 1 ( 0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7   and   PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined a PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional, single-speed DX heating coil (e.g., residential heat pump) would be:
-
-            PLF = 0.85 + 0.15(PLR)
-
-n The defrost energy input ratio (EIR) modifier curve (function of temperature) is a bi-quadratic curve with two independent variables: outdoor air dry-bulb temperature and the heating coil entering air wet-bulb temperature. The output of this curve is multiplied by the heating coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the coil is operating. This curve is only required when a reverse-cycle defrost strategy is specified.
-
-<div>$$DefrostEIRTempModFac = \,a + \,b\left( {{T_{wb,i}}} \right)\,\, + \,\,c{\left( {{T_{wb,i}}} \right)^2} + \,\,d\left( {{T_{db,o}}} \right)\,\, + \,\,e{\left( {{T_{db,o}}} \right)^2} + f\left( {{T_{wb,i}}} \right)\left( {{T_{db,o}}} \right)$$</div>
-
-where
-
-<span>\({T_{wb,i}}\)</span>      = wet-bulb temperature of the air entering the indoor heating coil, °C
-
-<span>\({T_{db,o}}\)</span>     = dry-bulb temperature of the air entering the outdoor coil, °C
-
-All six curves are accessed through EnergyPlus’ built-in performance curve equation manager (curve:quadratic, curve:cubic and curve:biquadratic). It is not imperative that the user utilize all coefficients shown in the preceding equations { through } in items (1) through (6) if their performance equation has fewer terms (e.g., if the user’s PartLoadFrac performance curve is linear instead of quadratic or cubic, simply enter the appropriate values for the coefficients a and b, and set the remaining coefficients to zero).
-
-The next input item for the Heating DX single speed coil is the supply air fan operation mode. Either the supply air fan runs continuously while the DX coil cycles on/off, or the fan and coil cycle on/off together. The next two inputs define the minimum outdoor dry-bulb temperature that the heat pump compressor will operate and the maximum outdoor dry-bulb temperature for defrost operation. Crankcase heater capacity and crankcase heater cutout temperature are entered in the following two inputs. The final four inputs cover the type of defrost strategy (reverse-cycle or resistive), defrost control (timed or on-demand), the fractional defrost time period (timed defrost control only), and the resistive defrost heater capacity if a resistive defrost strategy is selected.
-
-#### Model Description
-
-The general flow of the model is as follows:
-
-1)    If the outdoor air dry-bulb temperature is below the specified minimum temperature for compressor operation or the DX heating coil is not scheduled to operate, simply pass through the heating coil inlet air conditions as the coil outlet conditions, set power and heating rates equal to zero, and set crankcase heater power equal to the crankcase heater capacity value specified by the input file.
-
-2)    If the outdoor air dry-bulb temperature is above the specified minimum temperature for compressor operation and the DX heating coil is scheduled to operate, then:
-
-a.    If the outdoor dry-bulb temperature is below the specified maximum outdoor dry-bulb temperature for defrost operation, calculate a heating capacity multiplier, input power multiplier and fractional defrost time period depending on the defrost strategy and defrost control type specified for the heating coil.
-
-b.   Using the rated heating capacity and COP, the part-load curves specified for the DX heating coil, the defrost multipliers calculated above (if applicable), and the part-load ratio that is being requested of the heating coil, determine the following: heating coil exiting air conditions (dry-bulb temperature, humidity ratio and enthalpy), total DX coil heating rate, electric power during heating (compressors and outdoor fans), electric power during defrost, and crankcase heater power.
-
-The following paragraphs give a detailed description of the model calculations that are performed when the DX heating coil is operating (i.e., scenario \# 2 above).
-
-#### Frost Adjustment Factors
-
-Frost formation on the outdoor coil, and the need to periodically defrost this coil, has a significant impact on heating capacity and energy use by the DX heating system. If the outdoor air dry-bulb temperature is below the specified maximum temperature for defrost operation, then the model calculates adjustment factors for heating capacity and input power due to frost formation, and the fractional defrost time period, depending on the defrost strategy and defrost control type specified for the heating coil. This method of accounting for the impacts of frosting/defrost was taken from the model used in DOE-2.1E (ESTSC 2001, Miller and Jaster 1985).
-
-The model first estimates the outdoor coil temperature according to a linear empirical relationship with outdoor air dry-bulb temperature as the independent variable.
-
-<div>$${T_{coil,out}} = 0.82{T_{db,o}} - 8.589$$</div>
-
-The difference between the outdoor air humidity ratio (from the weather file) and the saturated air humidity ratio at the estimated outdoor coil temperature is then calculated, and this value is used as an indication of frost formation on the outdoor coil.
-
-<div>$$\Delta {\omega_{\,coil,out}}\, = \,MAX\left[ {1.0E - 6,\,\,\,{\omega_{outdoor}}\, - \,\,{\omega_{sat}}\left( {{T_{coil,out}}\,,{\rm{OutBaroPress}}} \right)} \right]$$</div>
-
-Frost formation on the outdoor coil must be periodically removed. The fraction of compressor runtime when the coil is being defrosted is either entered by the user (for timed defrost) or is calculated by the model (for on-demand defrost) using an empirical equation and <span>\(\Delta {\omega_{\,coil,out}}\)</span>. Adjustment factors to total heating coil capacity and input power due to frost formation on the outdoor coil are also calculated by empirical models with <span>\(\Delta {\omega_{\,coil,out}}\)</span> or fractional defrost time period as the independent variable. The defrost time period fraction and adjustment factors due to frost formation on the outdoor coil vary depending on the defrost control type as shown below.
-
-*Timed Defrost*:
-
-<div>$$Fractional\,Defrost\,Time\, = \,time\,period\,specified\,by\,user = {t_{frac,defrost}}$$</div>
-
-<div>$$Heating\,Capacity\,Multiplier\, = \,0.909 - \,107.33\left( {\Delta {\omega_{\,coil,out}}} \right)$$</div>
-
-<div>$$Input\,Power\,Multiplier\, = \,0.9 - \,36.45\left( {\Delta {\omega_{\,coil,out}}} \right)$$</div>
-
-*On-Demand Defrost*:
-
-<div>$$Fractional\,Defrost\,Time\, = \,\frac{1}{{1 + \left( {\frac{{0.01446}}{{\Delta {\omega_{\,coil,out}}}}} \right)}} = {t_{frac,defrost}}$$</div>
-
-<div>$$Heating\,Capacity\,Multiplier\, = \,0.875\left( {1 - {t_{frac,defrost}}} \right)$$</div>
-
-<div>$$Input\,Power\,Multiplier\, = \,0.954\left( {1 - {t_{frac,defrost}}} \right)$$</div>
-
-If the outdoor air dry-bulb temperature is above the specified maximum temperature for defrost operation, the fractional defrost time period is set to zero and the heating capacity/input power multipliers are set to unity.
-
-#### Defrost Operation
-
-If the fractional defrost time period is greater than zero for the simulation time step, then the model calculates the electrical power used during defrost. The method for calculating defrost power varies based on the defrost strategy specified (i.e., reverse-cycle or resistive). In the case of reverse-cycle defrost, the additional heating load due to defrost (indoor cooling during defrost) is also calculated so that it may be added to the existing heating load when calculating input power for the compressor(s) and outdoor coil fan(s).
-
-*Reverse-Cycle*:
-
-<div>$${Q_{defrost}}\, = \,0.01\left( {{t_{frac,defrost}}} \right)\left( {7.222 - {T_{db,o}}} \right)\left( {\frac{{{Q_{total,rated}}}}{{1.01667}}} \right)$$</div>
-
-<div>$${P_{defrost}}\, = \,DefrostEIRTempModFac\left( {\frac{{{Q_{total,rated}}}}{{1.01667}}} \right)\left( {{t_{frac,defrost}}} \right)\left( {RTF} \right)$$</div>
-
-*Resistive*:
-
-<div>$${Q_{defrost}}\, = \,0.0$$</div>
-
-<div>$${P_{defrost}}\, = \,\left( {{Q_{cap,defrost}}} \right)\left( {{t_{frac,defrost}}} \right)\left( {RTF} \right)$$</div>
-
-where:
-
-<span>\({Q_{defrost}}\)</span>        = additional indoor heating load due to reverse-cycle defrost (*W*)
-
-<span>\({Q_{total,rated}}\)</span>    = total full-load heating capacity of the coil at rated conditions (W)
-
-<span>\({P_{defrost}}\)</span>        = average defrost power for the simulation time step (W)
-
-<span>\({Q_{cap,defrost}}\)</span>   = capacity of the resistive defrost heating element (W)
-
-*DefrostEIRTempModFac* = energy input ratio modifier curve applicable during defrost
-
-<div>$${\rm{RTF  =  }}\left( {{\raise0.7ex\hbox{${{\rm{PLR}}}$} \!\mathord{\left/ {\vphantom {{{\rm{PLR}}} {{\rm{PartLoadFrac}}}}}\right.}\!\lower0.7ex\hbox{${{\rm{PartLoadFrac}}}$}}} \right)\,\,{\rm{ = }}\,\,runtime fraction of the heating coil$$</div>
-
-#### Heating Operation
-
-For any simulation time step, the total heating capacity of the DX unit is calculated as follows:
-
-<div>$$Qtotal = Qtotal,rated\left( {TotCapTempModFac} \right)\left( {TotCapFlowModFac} \right)$$</div>
-
-If the outdoor air dry-bulb temperature is below the maximum temperature for defrost operation, then the total heating capacity is further adjusted due to outdoor coil frost formation based on the results of Equation and Equation or .
-
-<div>$$Qtotal = Qtotal\left( {HeatingCapacityMultiplier} \right)$$</div>
-
-In a similar fashion, the electrical power draw by the DX unit (compressors plus outdoor coil fans) for any simulation time step is calculated. For a reverse-cycle defrost strategy, the additional heating load (*Q<sub>defrost</sub>*) generated during defrost operation is added to the heating load being requested by adjusting the part-load ratio. If a resistive defrost strategy is selected, *Q<sub>defrost</sub>* = 0. The part-load fraction correlation for the heating coil (user input, Equation or ) is used in the calculation of electrical power draw to account for efficiency losses due to compressor cycling.
-
-
-
-<div>$$PLR = \,MIN\left( {1.0\,,\,PLR + \left( {{\raise0.7ex\hbox{${{Q_{defrost}}}$} \!\mathord{\left/ {\vphantom {{{Q_{defrost}}} {{Q_{total}}}}}\right.}\!\lower0.7ex\hbox{${{Q_{total}}}$}}} \right)} \right)$$</div>
-
-<div>$$PartLoadFrac = \,a + \,b\left( {PLR} \right)\,\, + \,\,c{\left( {PLR} \right)^2}\,\, + \,\,d{\left( {PLR} \right)^3}$$</div>
-
-<div>$${P_{heating}} = \frac{{\left( {{Q_{total}}} \right)\left( {EIR} \right)\left( {PLR} \right)}}{{PartLoadFrac}} \times InputPowerMultiplier$$</div>
-
-where
-
-      <span>\({P_{heating}}\)</span>  = average compressor and outdoor fan power for the simulation time step(W)
-
-<span>\({Q_{total}}\)</span>    = total heating capacity W, Eqn.
-
-<div>$$EIR = \,Energy\,input\,ratio\, = \,\left( {\frac{1}{{CO{P_{rated}}}}} \right)\left( {EIRTempModFac} \right)\left( {EIRFlowModFac} \right)$$</div>
-
-<span>\(CO{P_{rated}}\)</span> = coefficient of performance at rated conditions (user input)
-
-*InputPowerMultiplier* = power adjustment due to frost if applicable -Eqn. or
-
-The crankcase heater is assumed to operate when the heating coil’s compressor is OFF, and the average crankcase heater power for the simulation time step is calculated as follows:
-
-<div>$${P_{crankcase}} = {Q_{cap,crankcase}}\left( {1 - RTF} \right)$$</div>
-
-<span>\({\rm{RTF  =  }}\left( {{\raise0.7ex\hbox{${{\rm{PLR}}}$} \!\mathord{\left/ {\vphantom {{{\rm{PLR}}} {{\rm{PartLoadFrac}}}}}\right.}\!\lower0.7ex\hbox{${{\rm{PartLoadFrac}}}$}}} \right)\,\,{\rm{ = }}\,\,runtime fraction of the heating coil\)</span>   
-
-where
-
-<span>\({P_{crankcase}}\)</span> = average crankcase heater power for the simulation time step (W)
-
-<span>\({Q_{cap,crankcase}}\)</span>= crankcase heater capacity (W)
-
-If this heating coil is used as part of an air-to-air heat pump (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir), the crankcase heater defined for this DX heating coil is enabled during the time that the compressor is not running for either heating or cooling (and the crankcase heater power defined in the DX cooling coil object is disregarded in this case). In this instance, RTF in the above equations would be the runtime fraction of the heat pump’s heating coil or cooling coil, whichever is greater.
-
-The properties of the air leaving the heating coil at full-load operation are calculated using the following equations:
-
-<div>$${h_{outlet}} = {h_{inlet}} + {\raise0.7ex\hbox{${{Q_{total}}}$} \!\mathord{\left/ {\vphantom {{{Q_{total}}} {\mathop m\limits^ \bullet  }}}\right.}\!\lower0.7ex\hbox{${\mathop m\limits^ \bullet  }$}}$$</div>
-
-<div>$${\omega_{outlet}}\, = \,{\omega_{inlet}}$$</div>
-
-<div>$${T_{db,outlet}}\, = \,PsyTdbFnHW({h_{outlet}},\,\,\,{\omega_{outlet}})$$</div>
-
-where
-
-<span>\({h_{outlet}}\)</span>         = enthalpy of the air leaving the heating coil (J/kg)
-
-<span>\(\,{\omega_{outlet}}\)</span>        = leaving air humidity ratio (kg/kg)
-
-<span>\(\,{T_{db,outlet}}\)</span>    = leaving air dry-bulb temperature (°C)
-
-*PsyTdbFnHW* = EnergyPlus psychrometric function, returns dry-bulb temp given enthalpy and humidity ratio
-
-#### Condenser Inlet Air Temperature
-
-The air temperature entering the outdoor condenser is based on the weather data used during a simulation. This temperature is either taken directly from the weather data, or can be adjusted based on the height of the outdoor condenser. Since this DX heating coil can only be used in conjunction with a DX cooling coil, the input for Condenser Air Inlet Node Name in the DX cooling coil object can be used to control this optional feature. If this input is left blank, the air temperature entering the condenser is based solely on the weather data. If this input is not blank, then the node name specified must also be listed in an OutdoorAir:Node or OutdoorAir:NodeList object. When the node name is listed in an OutdoorAir:NodeList object, the air temperature entering the condenser is based solely on the weather data. When the node name is listed in an OutdoorAir:Node object, the height of the node determines the air temperature entering the outdoor condenser (see description of Local Outdoor Air Temperature Calculation in the Atmospheric Variation section of this document for further details).
-
-#### Supply Air Fan Control: Cycling vs. Continuous
-
-One of the inputs to the DX coil model is the supply air fan operation mode: cycling fan, cycling compressor (CyclingFanAndCompressor) or continuous fan, cycling compressor (ContinuousFanWithCyclingCompressor). The first operation mode is frequently referred to as “AUTO fan�, where the compressor(s) and supply air fan operate in unison to meet the zone heating load, and cycle off together when the heating load has been met. The second operation mode is often referred to as “fan ON�, where the compressor(s) cycle on and off to meet the zone heating load but the supply air fan operates continuously regardless of compressor operation.
-
-Since this DX heating coil can only be used in conjunction with a DX cooling coil (i.e. heat pumps), and these coils are used in AC equipment that specifies a fan operation mode schedule (e.g AirLoopHVAC:UnitaryHeatPump:AirToAir), the selection made in the DX heating coil is currently ignored and the fan operation mode schedule value determines the fan operation mode for each time step throughout the simulation. A fan operation mode schedule value of 0 specifies AUTO fan mode operation while values other than 0 specify fan ON operation. The use of a schedule allows the fan operation mode to change based on time-of-day or with changes in season.
-
-The EnergyPlus methodology for determining the impact that HVAC equipment has on an air stream is to calculate the mass flow rate and air properties (e.g., enthalpy, dry-bulb temperature, humidity ratio) exiting the equipment. These exiting conditions are passed along as inlet conditions to the next component model in the air stream. Eventually the flow rate and properties of the air being supplied to the conditioned zone are used in the zone energy balance to determine the resulting zone air temperature and humidity ratio.
-
-With this methodology, the determination of the air mass flow rate and air properties for the two different supply air fan operation modes is slightly different. For the case of cycling fan/cycling compressor, the conditions of the air leaving the heating coil are the steady-state values calculated using equations , and above. However the air mass flow rate passed along to the next component (and eventually to the conditioned zone) is the average air mass flow rate for the system simulation time step (determined by the heating system; see AirLoopHVAC:UnitaryHeatPump:AirToAir). For this fan control type, the heating coil part-load fraction (Equation or ) is also passed to Fan:OnOff (if used) to properly calculate the supply air fan power and associated fan heat.
-
-For the case of continuous fan/cycling compressor, the air mass flow rate is constant. However, the air properties leaving the heating coil are calculated as the average conditions during the system simulation time step. The model assumes that the exiting air conditions are the steady-state values calculated using equations , and above when the compressor(s) operate. For the remainder of the system simulation time step, it is assumed that the air exiting the DX coil has the same properties as the air entering the coil. For this supply air fan operating strategy, the leaving air properties are calculated as follows:
-
-<div>$${h_{outlet,ContFanCycComp}}\, = \,{h_{outlet}}\,\left( {PLR} \right) + \,{h_{inlet}}\,\,\left( {1 - PLR} \right)$$</div>
-
-<div>$${\omega_{outlet,ContFanCycComp}}\, = \,{\omega_{outlet}}\,\left( {PLR} \right) + \,{\omega_{inlet}}\,\,\left( {1 - PLR} \right)$$</div>
-
-<div>$${T_{db,outlet,ContFanCycComp}} = \,PsyTdbFnHW({h_{outlet,\,ContFanCycComp}}\,,\,\,\,\,\,\,\,{\omega_{outlet,ContFanCycComp}})$$</div>
-
-#### References
-
-DOE. 1982. *DOE-2 engineers manual*, version 2.1A. LBL-11353. Berkeley, CA: Lawrence Berkeley National Laboratory.
-
-ESTSC. 2001. DOE-2.1E Version 110 (source code).Oak Ridge, TN: Energy Science and Technology Software Center.
-
-Miller, R.L. and Jaster, H. 1985. Performance of Air-Source Heat Pumps. EM-4226. Palo Alto, CA: Electric Power Research Institute.
-
-### Single-Speed DX Heating Coil Standard Ratings
-
-For single-speed direct expansion (DX) heating coils, the industry standard ratings of High Temperature Heating Standard (Net) Rating Capacity, Low Temperature Heating Standard (Net) Rating Capacity and Heating Seasonal Performance Factor (HSPF) are calculated according to ANSI/AHRI Standard 210/240 (AHRI 2008). The rated Energy Efficiency Ratio (EER) is not calculated for any DX heatings coils at this time.
-
-For the Coil:Heating:DX:SingleSpeed object in EnergyPlus, these standard ratings are not direct inputs to the model. However, these standard ratings can be calculated using user-entered information for the Coil:Heating:DX:SingleSpeed object. These standard rating values are provided in the eplusout.eio output file (Ref. OutputDetailsAndExamples.pdf) and also in the predefined tabular output reports (Output:Table:SummaryReports object, Equipment Summary). Currently, the standard ratings are only calculated and output for single-speed DX heating coils..
-
-Note: The standard ratings described in this section require that the DX heating coil model be evaluated at specific operating conditions (i.e., specific temperatures for air entering the heating coil and for air entering the air-cooled [outdoor] condenser). If the heating coil performance curves can not be evaluated at the required test conditions, then a standard rating value will be calculated at user specified curve limit as an output and a warning message will written to eplusout.err. For example, if the curve object (Curve:Biquadratic) for Total Heating Capacity Function of Temperature Curve has a minimum value of -5C for dry-bulb temperature entering the condenser coil, the HSPF calculation requires that heating capacity and EIR be calculated at -8.33C, so this would result in HSPF value calculated at -5C as an output and a warning message in the eplusout.err file.
-
-#### High Temperature Heating Standard (Net) Rating Capacity
-
-The procedure for calculating the Standard Rating Heating Capacity is given by:
-
-<div>$${\dot Q_{HighStandardRating}} = {\dot Q_{total,Rated}}\left( {TotCapTempModFa{c_{Rated}}} \right)$$</div>
-
-<div>$${\dot Q_{HighStandard\,Rating\,Net}} = {\dot Q_{HighStandardRating}} + Fa{n_{Power,\,Rated}}$$</div>
-
-where,
-
-<span>\({\dot Q_{HighStandardRating\,Net}}\)</span> = Total standard (net) heating capacity (W) of the air-source heat pump equipment in heating mode determined from ANSI/AHRI Standard 210/240 and test conditions shown in Table 59. The standard heating test conditions for air-cooled condenser are: indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb 8.33°C.
-
-<span>\({\dot Q_{HighStandardRating}}\)</span> = Total standard heating capacity (W) of the air-source heat pump equipment in heating mode determined from ANSI/AHRI Standard 210/240 and test conditions shown in Table 60. The standard heating test conditions for air-cooled condenser are: indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb 8.33°C.
-
-<span>\({\dot Q_{total,Rated}}\)</span> = Rated total heating capacity, user input (W)
-
-<span>\(TotCapTempModFa{c_{Rated}}\)</span>= User-specified bi-quadratic curve evaluated at the indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb 8.33°C for air-cooled condenser as specified in Table 59, (dimensionless).
-
-<span>\(Fa{n_{Power,Rated}}\)</span>= Supply air fan power at rated conditions, (W). The Rated Indoor Coil Fan Power Per Volume Flow rate is a user-entered value, with a default of 773.3 W/(m3/s)) if the user leaves this input field blank. The default value is taken from ANSI/ASHRAE Standard 210/240-2008 where it is defined for systems which do not have an Indoor Coil fan furnished as part of the system. See the description given at the end of this section for how this value is calculated.
-
-#### Low Temperature Heating Standard (Net) Rating Capacity
-
-The procedure for calculating the Low Temperature Standard Rating Heating Capacity is given by:
-
-<div>$${\dot Q_{LowStandardRating}} = {\dot Q_{total,Rated}}\left( {TotCapTempModFa{c_{H3Test}}} \right)$$</div>
-
-<div>$${\dot Q_{LowStandard\,Rating\,Net}} = {\dot Q_{LowStandardRating}} + Fa{n_{Power,\,Rated}}$$</div>
-
-where,
-
-<span>\({\dot Q_{LowStandardRating\,Net}}\)</span> = Total standard (net) heating capacity (W) of the air-source heat pump equipment in heating mode determined from ANSI/AHRI Standard 210/240 and test conditions shown in Table 60. The standard heating test conditions for air-cooled condenser are: indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb (-8.33) °C.
-
-<span>\({\dot Q_{LowStandardRating}}\)</span> =    Total standard heating capacity (W) of the air-source heat pump equipment in heating mode determined from ANSI/AHRI Standard 210/240 and test conditions shown in Table 59. The standard heating test conditions for air-cooled condenser are: indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb (-8.33) °C.
-
-<span>\({\dot Q_{total,Rated}}\)</span> = Rated total heating capacity, user input (W)
-
-<span>\(TotCapTempModFa{c_{H3Test}}\)</span>= User-specified bi-quadratic curve evaluated at the indoor coil entering air dry-bulb 21.1°C and outdoor coil entering air dry-bulb (-8.33) °C for air-cooled condenser as specified in Table 60, (dimensionless).
-
-<span>\(Fa{n_{Power,Rated}}\)</span>= Supply air fan power at rated conditions, (W). The Rated Indoor Coil Fan Power Per Volume Flow rate is a user-entered value, with a default of 773.3 W/(m3/s)) if the user leaves this input field blank. The default value is taken from ANSI/ASHRAE Standard 210/240-2008 where it is defined for systems which do not have an Indoor Coil fan furnished as part of the system. See the description given at the end of this section for how this value is calculated.
-
-#### Heating Seasonal Performance Factor (HSPF)
-
-Heating Seasonal Performance Factor (HSPF) is defined as the total space heating required during the space heating season, divided by the total electrical energy consumed by the heat pump system during the same season.
-
-Calculations of HSPF of a heat pump having a single-speed compressor that was tested with a fixed speed indoor fan installed, a constant-air-volume-rate indoor fan installed, or with no indoor fan installed is given below.
-
-<div>$$HSPF = \frac{{\sum\limits_j^J {\left[ {\frac{{{n_j}}}{N} \cdot BL({T_j})} \right]} }}{{\sum\limits_j^J {\left[ {\frac{{{e_h}({T_j})}}{N}} \right]}  + \sum\limits_j^J {\left[ {\frac{{RH({T_j})}}{N}} \right]} }} \cdot {F_{def}}$$</div>
-
-Where,
-
-<span>\(\frac{{{e_h}({T_j})}}{N}\)</span> = The ratio of the electrical energy consumed by the heat pump during periods of the  space heating season when the outdoor temperature fell within the range represented by bin temperature <span>\({T_j}\)</span> to the total number of hours in the heating season (N), W.
-
-<span>\(\frac{{RH({T_j})}}{N}\)</span>= The ratio of the electrical energy used for resistive space heating during periods when the outdoor temperature fell within the range represented by bin temperature <span>\({T_j}\)</span> to the total number of hours in the heating season (N),W.
-
-<span>\({T_j}\)</span>= The outdoor bin temperature, °C. Outdoor temperatures are “binned� such that calculations are only performed based one temperature within the bin. Bins of 2.78 °C are used.
-
-<span>\(\frac{{{n_j}}}{N}\)</span>= Fractional bin hours for the heating season; the ratio of the number of hours during the heating season when the outdoor temperature fell within the range represented by bin temperature <span>\({T_j}\)</span> to the total number of hours in the heating season, dimensionless. Obtain <span>\(\frac{{{n_j}}}{N}\)</span> values from Table # 17 of AHRI Std. 210/240-2008 (Table 60 below).
-
-<div>$$j$$</div>= The bin number, dimensionless.
-
-<span>\(J\)</span>= For each generalized climatic region, the total number of temperature bins, dimensionless. Referring to Table # 17, <span>\(J\)</span> is the highest bin number (<div>$$j$$</div>) having a nonzero entry for the fractional bin hours for the generalized climatic region of interest.
-
-<span>\({F_{def}}\)</span>= The demand defrost credit described in section 3.9.2 of AHRI Std. 210/240-2008, dimensionless.  For simplification, assigned a value of 1 for timed defrost control and a value of 1.03 for demand defrost control.
-
-<span>\(BL({T_j})\)</span>= The building space conditioning load corresponding to an outdoor temperature of<span>\({T_j}\)</span>; the heating season building load also depends on the generalized climatic region's outdoor design temperature and the design heating requirement, W.
-
-Building heating load can be evaluated by using the following equation
-
-<div>$$BL({T_j}) = \frac{{\left( {18.33 - {T_j}} \right)}}{{\left( {18.33 - {T_{OD}}} \right)}} \cdot C \cdot DHR$$</div>
-
-Where,
-
-<span>\({T_{OD}}\)</span>= The outdoor design temperature, °C. An outdoor design temperature is specified for each generalized climatic region in Table # 17 of AHRI Std. 210/240-2008 (Table 60 below).
-
-
-
-<span>\(C\)</span>= 0.77, a correction factor which tends to improve the agreement between calculated and measured building loads, dimensionless.
-
-<span>\(DHR\)</span> = Design Heating Requirement, W. This is the amount of heating required to maintain a given indoor temperature at a particular outdoor design temperature.
-
-For a single speed heat pump with a fixed speed indoor fan installed, a constant-air-volume-rate indoor fan installed, or with no indoor fan installed, the minimum and maximum design heating requirements for each generalized climatic region can be calculated as follows:
-
-<div>$$
-  DH{R_{\min }} = \left\{ 
-    \begin{array}{l}
-      {\mathop Q\limits^ \cdot_h}(8.33) \cdot (1.8) \cdot \left[ {\frac{{18.33 - {T_{OD}}}}{{60.0}}} \right] , {\rm{ for regions I,II,III,IV, and VI}} \\
-      {\mathop Q\limits^ \cdot_h}(8.33),{\rm{                     for regions V}}
-    \end{array}
-  right\}
-$$</div>
-
-<div>$$DH{R_{\max }} = \left\{ \begin{array}{l}2 \cdot {\mathop Q\limits^ \cdot_h}(8.33) \cdot (1.8) \cdot \left[ {\frac{{18.33 - {T_{OD}}}}{{60}}} \right],{\rm{ for regions I,II,III,IV, and VI}}\\\\2.2 \cdot {\mathop Q\limits^ \cdot_h}(8.33),{\rm{                     for regions V}}\end{array} \right\}$$</div>
-
-Both <span>\(DH{R_{\min }}\)</span>and <span>\(DH{R_{\max }}\)</span>above should be rounded to the nearest standardized DHR given in Table 61.
-
-The intermediate term used in the calculations of HSPF can be calculated using the equations described below.
-
-<div>$$\frac{{{e_h}({T_j})}}{N} = \frac{{X({T_j}) \cdot \mathop {{E_h}}\limits^ \cdot  ({T_j}) \cdot \delta ({T_j})}}{{PL{F_j}}} \cdot \frac{{{n_j}}}{N}$$</div>
-
-<div>$$\frac{{RH({T_j})}}{N} = \left[ {BL({T_j}) - \left( {X({T_j}) \cdot \mathop {{Q_h}}\limits^ \cdot  ({T_j}) \cdot \delta ({T_j})} \right)} \right] \cdot \frac{{{n_j}}}{N}$$</div>
-
-Where,
-
-<div>$$
-  X({T_j}) = \left\{ 
-    \begin{array}{l}
-      BL({T_J})/\mathop {{Q_h}}\limits^ \cdot  ({T_j}) \\
-      {\rm{Or}} \\
-      1
-    \end{array}
-  \right\}
-$$</div>
-
-whichever is less; the heating mode load factor for temperature bin <div>$$j$$</div>, dimensionless.
-
-<span>\(\mathop {{Q_h}}\limits^ \cdot  ({T_j})\)</span>= the space heating capacity of the heat pump when operating at outdoor temperature <span>\({T_j}\)</span>,  W.
-
-<span>\(\mathop {{E_h}}\limits^ \cdot  ({T_j})\)</span>= the electrical power consumption of the heat pump when operating at outdoor temperature <span>\({T_j}\)</span>, W.
-
-<span>\(\delta ({T_j})\)</span>= the heat pump low temperature cut-out factor, dimensionless.
-
-<span>\(PL{F_j}\)</span> = the part load factor, dimensionless.
-
-Part load factor is determined as follows:
-
-<div>$$PL{F_j} = 1 - {C_{{D^h}}}[1 - X({T_j})]$$</div>
-
-Where,
-
-<span>\({C_{{D^h}}}\)</span>= Degradation coefficient which is defaulted to the value of 0.25
-
-Low temperature cut-out factor <span>\(\delta ({T_j})\)</span>is determined as follows:
-
-<div>$$
-  \delta ({T_j}) = \left\{ 
-    \begin{array}{l}
-      {\rm{0, if }}{T_j} \le {T_{off}}{\rm{ or }}\frac{{\mathop {{Q_h}}\limits^ \cdot  ({T_j})}}{{\mathop {{E_h}}\limits^ \cdot  ({T_j})}} &lt; 1 \\
-      {\rm{1/2, if }}{T_{off}} &lt; {T_j} \le {T_{on}}{\rm{ and }}\frac{{\mathop {{Q_h}}\limits^ \cdot  ({T_j})}}{{\mathop {{E_h}}\limits^ \cdot  ({T_j})}} \ge 1 \\
-      {\rm{1, if }}{T_j} > {T_{on}}{\rm{ and }}\frac{{\mathop {{Q_h}}\limits^ \cdot  ({T_j})}}{{\mathop {{E_h}}\limits^ \cdot  ({T_j})}} \ge 1
-    \end{array}
-  \right.
-$$</div>
-
-where,
-
-<span>\({T_{off}}\)</span> = the outdoor temperature when the compressor is automatically shut off, °C. (If no such temperature exists, <span>\({T_j}\)</span>is always greater than <span>\({T_{off}}\)</span>and<span>\({T_{on}}\)</span>).
-
-<span>\({T_{on}}\)</span>= the outdoor temperature when the compressor is automatically turned back on, if applicable, following an automatic shut-off, °C.
-
-Calculate <span>\(\mathop {{Q_h}}\limits^ \cdot  ({T_j})\)</span>and <span>\(\mathop {{E_h}}\limits^ \cdot  ({T_j})\)</span> using,
-
-<div>$$\mathop {{Q_h}}\limits^ \cdot  ({T_j}) = \left\{ \begin{array}{l}\mathop {{Q_h}}\limits^ \cdot  ( - 8.33) + \frac{{\left[ {\mathop {{Q_h}}\limits^ \cdot  (8.33) - \mathop {{Q_h}}\limits^ \cdot  ( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{16.67}}{\rm{, if }}{T_j} \ge 7.22^\circ {\rm{C or }}{T_j} \le  - 8.33^\circ {\rm{C}}\\\mathop {{Q_h}}\limits^ \cdot  ( - 8.33) + \frac{{\left[ {\mathop {{Q_h}}\limits^ \cdot  (1.67) - \mathop {{Q_h}}\limits^ \cdot  ( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{10}}{\rm{, if }} - 8.33^\circ {\rm{C}} &lt; {T_j} &lt; 7.22^\circ {\rm{C}}\end{array} \right.$$</div>
-
-<div>$$\mathop {{E_h}}\limits^ \cdot  ({T_j}) = \left\{ \begin{array}{l}\mathop {{E_h}}\limits^ \cdot  ( - 8.33) + \frac{{\left[ {\mathop {{E_h}}\limits^ \cdot  (8.33) - \mathop {{E_h}}\limits^ \cdot  ( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{16.67}}{\rm{, if }}{T_j} \ge 7.22^\circ {\rm{C or }}{T_j} \le  - 8.33^\circ {\rm{C}}\\\mathop {{E_h}}\limits^ \cdot  ( - 8.33) + \frac{{\left[ {\mathop {{E_h}}\limits^ \cdot  (1.67) - \mathop {{E_h}}\limits^ \cdot  ( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{10}}{\rm{, if }} - 8.33^\circ {\rm{C}} &lt; {T_j} &lt; 7.22^\circ {\rm{C}}\end{array} \right.$$</div>
-
-<span>\(\mathop {{Q_h}}\limits^ \cdot  ( - 8.33),\mathop {{Q_h}}\limits^ \cdot  (1.67),\mathop {{Q_h}}\limits^ \cdot  (8.33),\mathop {{E_h}}\limits^ \cdot  ( - 8.33),\mathop {{E_h}}\limits^ \cdot  (1.67)\)</span> and <span>\(\mathop {{E_h}}\limits^ \cdot  (8.33)\)</span> are the **(net)** values calculated using performance curves entered by the user and supply fan power per rated air flow rate.
-
-Table 59. Heating Mode Test Conditions for Units Having a Single-Speed Compressor and a Fixed-Speed Indoor Fan, a Constant Air Volume Rate Indoor Fan, or No Indoor Fan
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="6">Source: Table 9, Page 74, ANSI/AHRI Standard 210/240 -2008</th>
-  </tr>
-  <tr>
-    <td rowspan="2">Test description</td>
-    <td colspan="2">Air Entering Indoor UnitTemperature (°C)</td>
-    <td colspan="2">Air Entering Outdoor UnitTemperature (°C)</td>
-    <td rowspan="2">Heating Air Volume Rate</td>
-  </tr>
-  <tr>
-    <td>Dry Bulb</td>
-    <td>Wet Bulb</td>
-    <td>Dry Bulb</td>
-    <td>Wet Bulb</td>
-  </tr>
-  <tr>
-    <td>H1 Test (Required, Steady)</td>
-    <td>21.11</td>
-    <td>15.56</td>
-    <td>8.33</td>
-    <td>6.11</td>
-    <td>Heating Full-load</td>
-  </tr>
-  <tr>
-    <td>H1C Test (Required, Steady)</td>
-    <td>21.11</td>
-    <td>15.56</td>
-    <td>8.33</td>
-    <td>6.11</td>
-    <td>(2)</td>
-  </tr>
-  <tr>
-    <td>H2 Test (Required, Steady)</td>
-    <td>21.11</td>
-    <td>15.56</td>
-    <td>1.67</td>
-    <td>0.56</td>
-    <td>Heating Full-load</td>
-  </tr>
-  <tr>
-    <td>H3 Test (Required, Steady)</td>
-    <td>21.11</td>
-    <td>15.56</td>
-    <td>-8.33</td>
-    <td>-9.44</td>
-    <td>Heating Full-load</td>
-  </tr>
-  <tr>
-    <td colspan="6">Notes: <br>1) Heating air volume arte are defined in section 3.1.4.4 of ANSI/AHRI 210/240-2008<br>2) Maintain the airflow nozzles static pressure difference ro velocity pressure during the ON periodat the same pressure difference or velocity pressure as measured during the H1 Test</td>
-  </tr>
-</table>
-
-Table 60. Generalized Climatic Region Information
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="8">Source: Table 17, Page 99, ANSI/AHRI Standard 210/240 -2008</th>
-  </tr>
-  <tr>
-    <th colspan="2">Region Number</th>
-    <th>I</th>
-    <th>II</th>
-    <th>III</th>
-    <th>IV</th>
-    <th>V</th>
-    <th>VI</th>
-  </tr>
-  <tr>
-    <th colspan="2">Heating Load Hours, HLH</th>
-    <td>750</td>
-    <td>1250</td>
-    <td>1750</td>
-    <td>2250</td>
-    <td>2750</td>
-    <td>*2750</td>
-  </tr>
-  <tr>
-    <th colspan="2">Outdoor Design Temperature, <span>\({T_{OD}}\)</span>(&deg;C)</th>
-    <td>2.78</td>
-    <td>-2.78</td>
-    <td>-8.33</td>
-    <td>-15</td>
-    <td>-23.33</td>
-    <td>-1.11</td>
-  </tr>
-  <tr>
-    <td><div>$$j$$</div></td>
-    <td><span>\({T_j}\)</span>(&deg;C)</td>
-    <td colspan="6">Fractional Bin Hours <span>\(\frac{{{n_j}}}{N}\)</span></td>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td>16.67</td>
-    <td>.291</td>
-    <td>.215</td>
-    <td>.153</td>
-    <td>.132</td>
-    <td>.106</td>
-    <td>.113</td>
-  </tr>
-  <tr>
-    <td>2</td>
-    <td>13.89</td>
-    <td>0.239</td>
-    <td>0.189</td>
-    <td>0.142</td>
-    <td>0.111</td>
-    <td>0.092</td>
-    <td>0.206</td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>11.11</td>
-    <td>0.194</td>
-    <td>0.163</td>
-    <td>0.138</td>
-    <td>0.103</td>
-    <td>0.086</td>
-    <td>0.215</td>
-  </tr>
-  <tr>
-    <td>4</td>
-    <td>8.33</td>
-    <td>0.129</td>
-    <td>0.143</td>
-    <td>0.137</td>
-    <td>0.093</td>
-    <td>0.076</td>
-    <td>0.204</td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>5.56</td>
-    <td>0.081</td>
-    <td>0.112</td>
-    <td>0.135</td>
-    <td>0.1</td>
-    <td>0.078</td>
-    <td>0.141</td>
-  </tr>
-  <tr>
-    <td>6</td>
-    <td>2.78</td>
-    <td>0.041</td>
-    <td>0.088</td>
-    <td>0.118</td>
-    <td>0.109</td>
-    <td>0.087</td>
-    <td>0.076</td>
-  </tr>
-  <tr>
-    <td>7</td>
-    <td>0</td>
-    <td>0.019</td>
-    <td>0.056</td>
-    <td>0.092</td>
-    <td>0.126</td>
-    <td>0.102</td>
-    <td>0.034</td>
-  </tr>
-  <tr>
-    <td>8</td>
-    <td>-2.78</td>
-    <td>0.005</td>
-    <td>0.024</td>
-    <td>0.042</td>
-    <td>0.087</td>
-    <td>0.094</td>
-    <td>0.008</td>
-  </tr>
-  <tr>
-    <td>9</td>
-    <td>-5.56</td>
-    <td>0.001</td>
-    <td>0.008</td>
-    <td>0.021</td>
-    <td>0.055</td>
-    <td>0.074</td>
-    <td>0.003</td>
-  </tr>
-  <tr>
-    <td>10</td>
-    <td>-8.33</td>
-    <td>0</td>
-    <td>0.002</td>
-    <td>0.009</td>
-    <td>0.036</td>
-    <td>0.055</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>11</td>
-    <td>-11.11</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0.005</td>
-    <td>0.026</td>
-    <td>0.047</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>12</td>
-    <td>-13.89</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0.002</td>
-    <td>0.013</td>
-    <td>0.038</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>13</td>
-    <td>-16.67</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0.001</td>
-    <td>0.006</td>
-    <td>0.029</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>14</td>
-    <td>-19.44</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0.002</td>
-    <td>0.018</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>15</td>
-    <td>-22.22</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0.001</td>
-    <td>0.01</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>16</td>
-    <td>-25</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0.005</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>17</td>
-    <td>-27.78</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0.002</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>18</td>
-    <td>-30.56</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0.001</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td colspan="8">* Pacific Coast Region</td>
-  </tr>
-</table>
-
-Table 61. Standardized Design Heating Requirements (W)
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="4">Source: Table 18, Page 100, ANSI/AHRI Standard 210/240 -2008</th>
-  </tr>
-  <tr>
-    <td>1465.356</td>
-    <td>7326.78</td>
-    <td>14653.56</td>
-    <td>26376.41</td>
-  </tr>
-  <tr>
-    <td>2930.712</td>
-    <td>8792.136</td>
-    <td>17584.27</td>
-    <td>29307.12</td>
-  </tr>
-  <tr>
-    <td>4396.068</td>
-    <td>10257.49</td>
-    <td>20514.98</td>
-    <td>32237.83</td>
-  </tr>
-  <tr>
-    <td>5861.424</td>
-    <td>11722.85</td>
-    <td>23445.7</td>
-    <td>38099.26</td>
-  </tr>
-</table>    
-
-### Multi-Speed Electric Heat Pump DX Air Heating Coil
-
-#### Overview
-
-This model (object name Coil:Heating:DX:MultiSpeed:) simulates the performance of an air-to-air direct expansion (DX) heating system. The main difference compared to the other heating coil model (Coil:Heating:DX:SingleSpeed) is that this heating coil allows modeling of two to four discrete compressor speeds. Each speed has a set of corresponding performance information at rated conditions along with curve fits for variations in total capacity, energy input ratio and part-load fraction to determine the performance of the unit at part-load conditions (DOE 1982). The full load supply airflow rate is dependent on the speed number and is set by its parent object (Ref: AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed). The part-load impact on coil energy use is automatically applied to the lowest speed. A choice is provided to determine whether part-load impacts on coil energy use are applied when the coil is operating at speeds greater than Speed 1. Adjustment factors applied to total capacity and input power to account for frost formation on the outdoor coil are calculated at each speed.
-
-This model simulates the thermal performance of the indoor DX heating coil, and the power consumption of the outdoor unit (multispeed compressor, fans, crankcase heaters and defrost heaters). The performance of the indoor supply air fan varies widely from system to system depending on control strategy (e.g., constant fan vs. AUTO fan), fan type, fan motor efficiency and pressure losses through the air distribution system. Therefore, this DX system model does not account for the thermal effects or electric power consumption of the indoor supply air fan. EnergyPlus contains separate models for simulating the performance of various indoor fan configurations, and these models can be easily linked with the DX system model described here to simulate the entire DX system being considered. For the time being, this coil model can only be called by the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
-
-When the model determines performance at Speed 1 (the lowest speed) or cycling between OFF and Speed 1, its performance is almost the same as the performance for the Coil:Heating:DX:SingleSpeed model. However, the outlet conditions are calculated slightly differently. Therefore, the Coil:Heating:DX:SingleSpeed model may be considered as a subset of the model described here. When the multispeed coil model determines performance at higher speeds (above 1), the model linearly interpolates the performance at two consecutive speeds (n-1 and n) as needed to meet the heating load, with the fraction of time at each speed established by the speed ratio.
-
-When single mode operation is specified at higher speeds (above 1), defined in the UnitarySystemPerformance:Multispeed object, a child object of AirLoopHVAC:UnitarySystem, its performance is almost the same as the performance for the Coil:Heating:DX:SingleSpeed model at different flow rate and capacity with given speed number. No linear interpolation is performed between two adjacent speeds. The highest speed which does not exceed the sensible load is used for each HVAC timestep. This operation does not apply to speed 1 operation and the case when the sensible load is above the highest sensible capacity.
-
-#### Model Inputs
-
-The model inputs are also very similar to the inputs of the Coil:Heating:DX:SingleSpeed object. The main difference is that this multispeed model requires a set of fields at each speed, such as rated capacity, rated COP, two capacity modifiers, two energy input ratio modifiers, and part-load correction. The inputs also include waste heat fraction and modifier as a function of temperature to calculate recoverable waste heat for heat recovery, which are not available in the similar Coil:Heating:DX:SingleSpeed object.
-
-#### Speed 1 Operation
-
-The calculation procedures in this model, including defrost and crankcase heater, are indentical to the Coil:Heating:DX:SingleSpeed object (Ref: Coil:Heating:DX:SingleSpeed) with one exception: outlet node condition calculation when the supply air fan operation mode is ContinuousFanWithCyclingCompressor. The following procedure provides the detailed description of the exception.
-
-n Total delivered heating capacity
-
-The total delivered heating capacity for speed 1 operating at the cycling ratio needed to meet the requested heating load is:
-
-<div>$${Q_{coil,cycling}} = {\mathop m\limits^\cdot_{Speed\,1}}\left( {CycRatio} \right)({h_{inlet}} - {h_{outlet,full}})$$</div>
-
-where,
-
-*Q<sub>coil,cycling</sub>*      = delivered sensible heating capacity for Speed 1 operating at a specific cycling ratio [W]
-
-<span>\(\mathop {{\rm{ }}m}\limits_{Speed{\kern 1pt} 1}^ \cdot  \)</span>      = air mass flow rate through heating coil at Speed 1 as set by the parent object [kg/s]
-
-*h<sub>outlet,full</sub>*      = specific enthalpy of the coil outlet air during full-load operation at Speed 1 (no cycling) [J/kg]
-
-*h<sub>inlet</sub>           *            = specific enthalpy of the coil inlet air [J/kg]
-
-*CycRatio*    = cycling ratio at Speed 1, ratio of requested heating load to the full-load capacity of the coil at Speed 1 [dimensionless]
-
-It is assumed that the coil provides no heating capacity when the coil is OFF, even if the supply air fan continues to operate.
-
-n Outlet air specific enthalpy
-
-The average specific enthalpy of the coil outlet air is then calculated based on the delivered sensible heating capacity and the average air mass flow rate entering the coil:
-
-<div>$${h_{outlet,average}} = {h_{inlet}} - {{\raise0.7ex\hbox{${{Q_{coil,cycling}}}$} \!\mathord{\left/ {\vphantom {{{Q_{coil,cycling}}} {\mathop m\limits^\cdot  }}}\right.}\!\lower0.7ex\hbox{${\mathop m\limits^\cdot  }$}}_{inlet}}$$</div>
-
-where,
-
-*h<sub>outlet,average</sub>*  = average specific enthalpy at the coil outlet [J/kg]
-
-<span>\({\dot m_{inlet}}\)</span>         = mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the heating coil is ON and the specified flow rate when the heating coil is OFF for the time step being simulated.
-
-n Outlet air temperature
-
-The heating coil’s outlet air humidity ratio equals the inlet air humidity ratio since the coil does not change the moisture content of the air. So the average outlet air temperature is calculated based on the inlet air humidity ratio and the average outlet air enthalpy using the psychrometric function PsyTdbFnHW.
-
-The main reason for using the above approach is that outlet air conditions are calculated in the same way for all operating speeds.
-
-The crankcase heater defined for this DX heating coil is enabled during the time that the compressor is not running for either heating or cooling. The crankcase heater power use from either heating or cooling is reported in the heating coil.
-
-#### Higher Speed Operation
-
-This section describes how higher speed operation is simulated. When the required sensible load is less than the full load sensible capacity at Speed n (Speed Number &gt; 1), the following calculations are performed:
-
-n Total delivered heating capacity at Speed n-1 and Speed n
-
-<span>\(TotCa{p_{n - 1}} = RatedCa{p_{n - 1}}\left( {TotCapTempModFa{c_{n - 1}}} \right)\left( {TotCapFlowModFa{c_{n - 1}}} \right)\)</span><span>\(TotCa{p_n} = RatedCa{p_n}\left( {TotCapTempModFa{c_n}} \right)\left( {TotCapFlowModFa{c_n}} \right)\)</span>
-
-where,
-
-*TotCap<sub>i</sub>*<sub>           </sub> = total delivered heating capacity at given temperatures and flow rates at Speed i [W]
-
-*RatedCap<sub>i</sub>*<sub>   </sub> = heating capacity at the rated conditions at Speed i [W]
-
-*TotCapTempModFac<sub>i</sub>* = total heating capacity modifier as a function of indoor and outdoor air dry-bulb temperature at Speed i
-
-*TotCapFlowModFac<sub>i</sub>* = total heating capacity modifier as a function of the ratio of the actual flow rate across the heating coil to the rated airflow rate at Speed i
-
-i     = Speed n or Speed n-1
-
-n EIR at Speed n-1 and Speed n
-
-<div>$$EI{R_{n - 1}} = RatedEI{R_{n - 1}}\left( {EIRTempModFa{c_{n - 1}}} \right)\left( {EIRFlowModFa{c_{n - 1}}} \right)$$</div>
-
-<div>$$EI{R_n} = RateEI{R_n}\left( {EIRTempModFa{c_n}} \right)\left( {EIRFlowModFa{c_n}} \right)$$</div>
-
-where,
-
-*EIR<sub>i</sub>*<sub>                      </sub> = energy input ratio at given temperatures and flow rates at Speed i [W]
-
-*RatedEIR<sub>i</sub>*<sub>    </sub> = energy input ratio at the rated conditions at Speed i [W]
-
-*EIRTempModFac<sub>i</sub>* = energy input ratio modifier as a function of indoor and outdoor air dry-bulb temperature at Speed i
-
-*EIRFlowModFac<sub>i</sub>* = energy input ratio modifier as a function of the ratio of the actual flow rate across the heating coil to the rated airflow rate at Speed i
-
-i     = Speed n or Speed n-1
-
-n Full load outlet air specific enthalpy at Speed n-1 and Speed n
-
-<div>$${h_{outlet,full\_Speed\,n}} = {h_{inlet}} - {{\raise0.7ex\hbox{${\left( {TotCa{p_n}*HeatingCapacityMultiplier} \right)}$} \!\mathord{\left/ {\vphantom {{\left( {TotCa{p_n}*HeatingCapacityMultiplier} \right)} {\mathop m\limits^\cdot  }}}\right.}\!\lower0.7ex\hbox{${\mathop m\limits^\cdot  }$}}_{inlet}}$$</div>
-
-<div>$${h_{outlet,full\_Speed\,n - 1}} = {h_{inlet}} - {{\raise0.7ex\hbox{${\left( {TotCa{p_{n - 1}}*HeatingCapacityMultiplier} \right)}$} \!\mathord{\left/ {\vphantom {{\left( {TotCa{p_{n - 1}}*HeatingCapacityMultiplier} \right)} {\mathop m\limits^\cdot  }}}\right.}\!\lower0.7ex\hbox{${\mathop m\limits^\cdot  }$}}_{inlet}}$$</div>
-
-where,
-
-*HeatingCapacityMultiplier*            = frost adjustment factor for heating capacity (See Ref. Coil:Heating:DX:SingleSpeed)
-
-*h<sub>outlet,full\_Speed\\ n</sub>*         = specific enthalpy of the coil outlet air during full-load operation at Speed n (no cycling) [J/kg]
-
-*h<sub>outlet,full\_Speed\\ n-1</sub>*       = specific enthalpy of the coil outlet air during full-load operation at Speed n-1 (no cycling) [J/kg]
-
-n Effective total heating capacity
-
-<div>$$\begin{array}{l}{Q_{coil,SpeedRatio}} = \left( {SpeedRatio} \right){\mathop m\limits^\cdot_{Speed\,n}}({h_{inlet}} - {h_{outlet,full\_Speed\,n}})\\\;\;\;\;\;\;\;\;\;\; + (1 - SpeedRatio){\mathop m\limits^\cdot_{Speed\,n - 1}}({h_{inlet}} - {h_{outlet,full\_Speed\,n - 1}})\end{array}$$</div>
-
-where,
-
-<span>\({{Q_{coil,SpeedRatio}}}\)</span><sub>                       </sub> = delivered sensible heating capacity at a given speed ratio between two consecutive speeds [W]
-
-<span>\({\mathop {{\rm{ }}m}\limits_{Speed{\kern 1pt} n}^ \cdot  }\)</span>      = air mass flow rate through heating coil at Speed n as set by the parent object [kg/s]
-
-<span>\({\mathop {{\rm{ }}m}\limits_{Speed{\kern 1pt} n - 1}^ \cdot  }\)</span>    = air mass flow rate through heating coil at Speed 1 as set by the parent object [kg/s]
-
-
-
-n Average outlet air enthalpy
-
-<div>$${h_{outlet,average}} = {h_{inlet}} - {{\raise0.7ex\hbox{${{Q_{coil,SpeedRatio}}}$} \!\mathord{\left/ {\vphantom {{{Q_{coil,SpeedRatio}}} {\mathop m\limits^\cdot  }}}\right.}\!\lower0.7ex\hbox{${\mathop m\limits^\cdot  }$}}_{inlet}}$$</div>
-
-where,
-
-*h<sub>outlet,average</sub>*  = average specific enthalpy at the coil outlet [J/kg]
-
-*h<sub>inlet</sub>           *            = specific enthalpy of the coil inlet air [J/kg]
-
-<span>\({\dot m_{inlet}}\)</span>         = Mass flow rate at the inlet to the coil as established by the parent object (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed, Mass Flow Rate Calculation). This flow rate is the average value determined by the parent object, accounting for the specified flow rate when the heating coil is at Speed n and the specified flow rate when the heating coil is at Speed n-1 for the time step being simulated.
-
-n Average outlet air temperature
-
-The heating coil’s outlet air humidity ratio equals the inlet air humidity ratio since the coil does not change the moisture content of the air. So the average outlet air temperature is calculated based on the inlet air humidity ratio and the average outlet air enthalpy using the psychrometric function PsyTdbFnHW.
-
-n Full load energy inputs at Speed n-1 and Speed n
-
-<div>$$HeatingPowe{r_n} = TotCa{p_n}\left( {EI{R_n}} \right)\left( {HeatingCapacityMultiplier} \right)\left( {InputPowerMultiplier} \right)$$</div>
-
-<div>$$HeatingPowe{r_{n - 1}} = TotCa{p_{n - 1}}\left( {EI{R_{n - 1}}} \right)\left( {HeatingCapacityMultiplier} \right)\left( {InputPowerMultiplier} \right)$$</div>
-
-where,
-
-*InputPowerMultiplier*        = Frost adjustment factor for heating power calculation (Ref. Coil:Heating:DX:SingleSpeed)
-
-n Calculate combined energy input
-
-When the input for the field ‘Apply Part Load Fraction to Speeds Greater than 1’ is No (equivalent to a single compressor), the combined energy output is calculated as follows:
-
-<div>$$HeatingPower = HeatingPowe{r_n}\left( {SpeedRatio} \right) + HeatingPowe{r_{n - 1}}(1.0 - SpeedRatio)$$</div>
-
-When the input for the field ’Apply Part Load Fraction to Speeds Greater than 1’ is Yes (equivalent to multiple compressors), the combined energy output is calculated as follows:
-
-<div>$$HeatingPower = HeatingPowe{r_n}\left( {RTF} \right) + HeatingPowe{r_{n - 1}}(1.0 - RTF)$$</div>
-
-where,
-
-HeatingPower          = Power used in Watt
-
-RTF                        = Run time fraction (SpeedRatio/Part-load Fraction) at Speed n
-
-n Calculate defrost power
-
-When the defrost strategy is resistive, the power calculation is the same as Speed 1 operation (Ref. Coil:Heating:DX:SingleSpeed). When the defrost strategy is reverse-cycle, the following calculations are performed:
-
-<div>$${Q_{defrost,n}} = 0.01({t_{frac,defrost}})(7.222 - {T_{db,o}})\left( {\frac{{{Q_{total,rated,n}}}}{{1.01667}}} \right)$$</div>
-
-<div>$${P_{defrost,n - 1}} = DefrostEIRTempModFac\left( {\frac{{{Q_{total,rated,n - 1}}}}{{1.01667}}} \right)({t_{frac,defrost}})$$</div>
-
-<div>$${P_{defrost,n}} = DefrostEIRTempModFac\left( {\frac{{{Q_{total,rated,n}}}}{{1.01667}}} \right)({t_{frac,defrost}})$$</div>
-
-where:
-
-<span>\({Q_{defrost,n}}\)</span>     = additional indoor heating load due to reverse-cycle defrost at Speed n (*W*)
-
-<span>\({Q_{total,rated,n}}\)</span>  = total full-load heating capacity of the coil at rated conditions at Speed n (W)
-
-<span>\({P_{defrost,n - 1}}\)</span>    = full load defrost power for the simulation time step at Speed n-1 (W)
-
-<span>\({P_{defrost,n}}\)</span>      = full load defrost power for the simulation time step at Speed n (W)
-
-<span>\({Q_{total,rated,n - 1}}\)</span>= capacity of the resistive defrost heating element at Speed n-1 (W)
-
-<span>\({Q_{total,rated,n}}\)</span>= capacity of the resistive defrost heating element at Speed n (W)
-
-DefrostEIRTempModFac     = defrost energy input ratio (EIR) modifier curve (Ref. Coil:Heating:DX:SingleSpeed).
-
-T<sub>frac,defrost</sub>       =  fractional defrost time (Ref. Coil:Heating:DX:SingleSpeed)
-
-When the input for the field ‘Apply Part Load Fraction to Speeds Greater than 1’ is No (equivalent to a single compressor), the average defrost power is calculated as follows:
-
-<div>$${P_{defrost}} = {P_{defrost,n}}(SpeedRatio) + {P_{defrost,n - 1}}(1.0 - SpeedRatio)$$</div>
-
-When the input for the field ’Apply Part Load Fraction to Speeds Greater than 1’ is Yes (equivalent to multiple compressors), the combined defrost energy is calculated as follows:
-
-<div>$${P_{defrost}} = {P_{defrost,n}}(RTF) + {P_{defrost,n - 1}}(1.0 - RTF)$$</div>
-
-where,
-
-<span>\({P_{defrost}}\)</span>        = average defrost power used in Watt
-
-RTF            = Run time fraction (SpeedRatio/Part-load Fraction) at Speed n
-
-n Crankcase heater
-
-There is no power need at higher speed operation.
-
-#### Higher Speed Operation with Single Mode Operation
-
-This section describes how higher speed operation is simulated with single mode operation. When the required sensible load is less than the full load sensible capacity at Speed n (Speed Number > 1), its performance is almost the same as the performance for the Coil:Heating:DX:SingleSpeed model at different flow rate and capacity with given Speed n. No linear interpolation is performed between two adjacent speeds. The highest speed which does not exceed the sensible load is used for each HVAC timestep. This operation does not apply to the case when the sensible load is above the highest sensible capacity.
-
-#### Waste heat calculation
-
-The waste heat generated by this coil object is calculated as:
-
-<div>$${Q_{WasteHeat}} = (Fraction)(TempModifier)(HeatingPowe)$$</div>
-
-where
-
-Fraction                  = rated waste heat fraction of the energy input
-
-TempModifier<sub>                  </sub> = waste heat modifier as a function of indoor and outdoor air dry-bulb temperature
-
-#### Standard Rating of Multi-Speed DX Heating Coils
-
-For multi-speed direct expansion heating coils, the industry standard ratings of Standard Rating Heating Seasonal Performance Factor (HSPF) are calculated according to NSI/AHRI Standard 210/240 (AHRI 2008). These standard ratings can be calculated using the user-entered information for the Coil:Heating:DX:MultiSpeed object.  According to Standard 210/240, the Standard Rating HSPF applies to air-to-air unitary heat pumps with rated heating capacities under 19,000 watts (65,000 Btu/h). The Heating Mode Test Conditions for Units Having two-capacity Compressor standard tests H0<sub>1</sub>, H1<sub>1</sub>, H2<sub>1</sub>, H3<sub>1</sub>, H1<sub>2</sub>, H2<sub>2</sub>, and H3<sub>2</sub> are also provided in Table 62. The rated Energy Efficiency Ratio (EER) is not calculated for any DX Heating Coils as this time. The equations required to calculate the net heating capacity and HSPF values are described next.
-
-#### Standard Ratings Heating Capacity
-
-*The Standard Rating (Net) Heating Capacity calculation is calculated using the same procedure as the single speed DX heating coils except the capacities are evaluated at the maximum speed only.  Refer to the standard ratings calculation for Coil:DX:Heating:SingelSpeed for description of the procedure.*
-
-The Rated Supply Fan Power Per Volume Flow Rate is a user-entered value, with a default of 773.3 W/(m<sup>3</sup>/s)) if the user leaves this input field blank. The default value is taken from ANSI/ASHRAE Standard 210/240-2008 where it is defined for systems which do not have an Indoor Coil (Evaporator) fan furnished as part of the system. The test conditions in ANSI/AHRI Standard 210/240 vary the external static pressure (i.e., pressure drop associated with ductwork and other devices external to the indoor fan/coil section) seen by the supply air fan based on the standard rating cooling capacity. New input field Rated Supply Fan Power Per Volume Flow Rate for each speed will be added to the IDD.
-
-#### Heating seasonal performance factors (HSPF) for Multi-Speed DX Coil
-
-The following section describes the test condition for heating mode tests for Air-Source Heat Pumps, including heating-only heat pumps, and the equations required to calculate the HSPF. The HSPF for multi-speed compressor heat pumps in Btu/W-h is given by:
-
-<div>$$HSPF{\rm{ = }}\frac{{\sum\limits_{\rm{j}}^{\rm{M}} {\frac{{{n_j}}}{N} \cdot BL\left( {{T_j}} \right)} }}{{\sum\limits_{\rm{j}}^{\rm{M}} {\frac{{{e_h}\left( {{T_j}} \right)}}{N}{\rm{ + }}} \sum\limits_{\rm{j}}^{\rm{M}} {\frac{{RH\left( {{T_j}} \right)}}{N}} }} \cdot {F_{def}}$$</div>
-
-
-
-Where,
-
-BL(T<sub>j</sub>)          =          the building space conditioning load corresponding to an outdoor temperature of T<sub>j</sub>; the heating season building load also depends on the generalized climatic region's outdoor design temperature and the design heating requirement, Btu/h.
-
-e<sub>h</sub>(T<sub>j</sub>)/N        =          the ratio of the electrical energy consumed by the heat pump during periods of the space heating season when the outdoor temperature fell within the range represented by bin temperature T<sub>j</sub> to the total number of hours in the heating season (N), W. For heat pumps having a heat comfort controller, this ratio may also include electrical energy used by resistive elements to maintain a minimum air delivery temperature.
-
-RH(T<sub>j</sub>)/N      =          the ratio of the electrical energy used for resistive space heating during periods when the outdoor temperature fell within the range represented by bin temperature T<sub>j</sub> to the total number of hours in the heating season (N),W. Resistive space heating is modeled as being used to meet that portion of the building load that the heat pump does not meet because of insufficient capacity or because the heat pump automatically turns off at the lowest outdoor temperatures.
-
-T<sub>j</sub>    =          the outdoor bin temperature, °C. Outdoor temperatures are “binned� such that calculations are only performed based one temperature within the bin. Bins of 2.78°C are used.
-
-n<sub>j</sub>/N =          Fractional bin hours for the heating season; the ratio of the number of hours during the heating season when the outdoor temperature fell within the range represented by bin temperature T<sub>j</sub> to the total number of hours in the heating season, dimensionless, given in Table 60.
-
-j     =          the bin number, dimensionless.
-
-M   =          for each generalized climatic region, the total number of temperature bins, dimensionless. Referring to Table 60, M is the highest bin number (j) having a nonzero entry for the fractional bin hours for the generalized climatic region of interest.
-
-<span>\({F_{def}}\)</span>= The demand defrost credit described in section 3.9.2 of AHRI Std. 210/240-2008, dimensionless.  For simplification, assigned a value of 1 for timed defrost control and a value of 1.03 for demand defrost control.
-
-The building heating load is calculated as follows:
-
-<div>$$BL\left( {{T_j}} \right){\rm{ = }}\frac{{{\rm{18}}{\rm{.33 - }}{T_j}}}{{{\rm{18}}{\rm{.33 - }}{T_{OD}}}} \cdot C \cdot DHR$$</div>
-
-The minimum and maximum design heating requirements for each generalized climate regions are given by:
-
-<div>$$
-  {\rm{DH}}{{\rm{R}}_{\min }}{\rm{ = }}\left\{ 
-    \begin{array}{l}
-      {\rm{\dot Q}}_h^{k = 2}{\rm{(8}}{\rm{.33)}} \cdot \left[ {\frac{{{\rm{18}}{\rm{.33 - }}{{\rm{T}}_{{\rm{OD}}}}}}{{{\rm{33}}{\rm{.33}}}}} \right]{\rm{,}}\quad {\rm{for}}\,{\rm{regions}}\,{\rm{I,}}\,{\rm{II,}}\,{\rm{III,}}\,{\rm{IV,}}\,\,{\rm{VI}} \\
-      {\rm{\dot Q}}_h^{k = 2}{\rm{(8}}{\rm{.33),}}\quad {\rm{for}}\,{\rm{region}}\,{\rm{V}}
-    \end{array}
-  \right\}
-$$</div>
-
-and
-
-<div>$$
-  \rm{DH}}{{\rm{R}}_{\max }}{\rm{ = }}\left\{
-    \begin{array}{l}
-      \rm{2} \cdot {\rm{\dot Q}}_h^{k = 2}{\rm{(8}}{\rm{.33)}} \cdot \left[ {\frac{{{\rm{18}}{\rm{.33 - }}{{\rm{T}}_{{\rm{OD}}}}}}{{{\rm{33}}{\rm{.33}}}}} \right]{\rm{,}}\quad {\rm{for}}\,{\rm{regions}}\,{\rm{I,}}\,{\rm{II,}}\,{\rm{III,}}\,{\rm{IV,}}\,\,{\rm{VI}} \\
-      \rm{2}{\rm{.2}} \cdot {\rm{\dot Q}}_h^{k = 2}{\rm{(8}}{\rm{.33),}}\quad {\rm{for}}\,{\rm{region}}\,{\rm{V}}
-    \end{array}
-  \right\}
-$$</div>
-
-Where,
-
-C    =          0.77, a correction factor which tends to improve the agreement between calculated and measured building loads dimensionless.
-
-DHR           =          the design heating requirement for each generalized climate region, Btu/h.
-
-<span>\(\dot Q_h^{k = 2}(8.33)\)</span>=          the heating capacity determined from H1<sub>2</sub> test, (W)
-
-The heating capacity delivered and electric power input of the heat pump when operating at minimum (low) compressor capacity and outdoor air temperature of *T<sub>j</sub>* is given by:
-
-<div>$$
-  {\rm{\dot Q}}_h^{k = 1}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{) = }}\left\{ 
-    \begin{array}{l}
-      {\rm{\dot Q}}_h^{k = 1}(8.33) + \;\frac{{\left[ {{\rm{\dot Q}}_h^{k = 1}{\rm{(16}}{\rm{.67) - \dot Q}}_h^{k = 1}{\rm{(8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} - 8.33} \right)}}{{\left( {16.67 - 8.33} \right)}}\,{\rm{if}}\,{{\rm{T}}_{\rm{j}}} \ge 4.44{\rm{^\circ C}} \\
-      {\rm{\dot Q}}_h^{k = 1}( - 8.33) + \;\frac{{\left[ {{\rm{\dot Q}}_h^{k = 1}{\rm{(1}}{\rm{.67) - \dot Q}}_h^{k = 1}{\rm{( - 8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} + 8.33} \right)}}{{\left( {1.67 + 8.33} \right)}}\,{\rm{if}}\, - 8.33{\rm{^\circ C}} \le {{\rm{T}}_{\rm{j}}} &lt; 4.44{\rm{^\circ C}} \\
-      {\rm{\dot Q}}_h^{k = 1}( - 8.33) + \;\frac{{\left[ {{\rm{\dot Q}}_h^{k = 1}{\rm{(8}}{\rm{.33) - \dot Q}}_h^{k = 1}{\rm{( - 8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} + 8.33} \right)}}{{\left( {8.33 + 8.33} \right)}}\,{\rm{if }}{{\rm{T}}_{\rm{j}}} &lt;  - 8.33{\rm{^\circ C}}\,
-    \end{array}
-  \right\}
-$$</div>
-
-<div>$$
-  {\rm{\dot E}}_h^{k = 1}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{) = }}\left\{
-    \begin{array}{l}
-      {\rm{\dot E}}_h^{k = 1}(8.33) + \;\frac{{\left[ {{\rm{\dot E}}_h^{k = 1}{\rm{(16}}{\rm{.67) - \dot E}}_h^{k = 1}{\rm{(8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} - 8.33} \right)}}{{\left( {16.67 - 8.33} \right)}}\,{\rm{if}}\,{{\rm{T}}_{\rm{j}}} \ge 4.44{\rm{^\circ C}} \\
-      {\rm{\dot E}}_h^{k = 1}( - 8.33) + \;\frac{{\left[ {{\rm{\dot E}}_h^{k = 1}{\rm{(1}}{\rm{.67) - \dot E}}_h^{k = 1}{\rm{( - 8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} + 8.33} \right)}}{{\left( {1.67 + 8.33} \right)}}\,{\rm{if}}\, - 8.33{\rm{^\circ C}} \le {{\rm{T}}_{\rm{j}}} &lt; 4.44{\rm{^\circ C}} \\
-      {\rm{\dot E}}_h^{k = 1}( - 8.33) + \;\frac{{\left[ {{\rm{\dot E}}_h^{k = 1}{\rm{(8}}{\rm{.33) - \dot E}}_h^{k = 1}{\rm{( - 8}}{\rm{.33)}}} \right] \cdot \left( {{{\rm{T}}_{\rm{j}}} + 8.33} \right)}}{{\left( {8.33 + 8.33} \right)}}\,{\rm{if }}{{\rm{T}}_{\rm{j}}} &lt;  - 8.33{\rm{^\circ C}}\,
-    \end{array}
-  \right\}
-$$</div>
-
-Where,
-
-<span>\({\rm{\dot Q}}_h^{k = 1}\left( {{\rm{16}}{\rm{.67}}} \right),\,{\rm{and}}\,{\rm{\dot E}}_h^{k = 1}\left( {{\rm{16}}{\rm{.67}}} \right)\)</span> are determined from H0<sub>1</sub> test and
-
-<span>\({\rm{\dot Q}}_h^{k = 1}\left( {{\rm{8}}{\rm{.33}}} \right),\,{\rm{and}}\,{\rm{\dot E}}_h^{k = 1}\left( {{\rm{8}}{\rm{.33}}} \right)\)</span> are determined from H1<sub>1</sub> test and
-
-<span>\({\rm{\dot Q}}_h^{k = 1}\left( {{\rm{1}}{\rm{.67}}} \right),\,{\rm{and}}\,{\rm{\dot E}}_h^{k = 1}\left( {{\rm{1}}{\rm{.67}}} \right)\)</span> are determined from H2<sub>1</sub> test, and
-
-<span>\({\rm{\dot Q}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right),\,{\rm{and}}\,{\rm{\dot E}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right)\)</span> are determined from H3<sub>1</sub> test.
-
-An alternative to conducting or evaluating the performance at H2<sub>1</sub> test is to approximate the capacity and electric power inputs as follows:
-
-<div>$${\rm{\dot Q}}_h^{k = 1}\left( {{\rm{1}}{\rm{.67}}} \right) = 0.9 \cdot \left\{ {{\rm{\dot Q}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right) + 0.6\left[ {{\rm{\dot Q}}_h^{k = 1}\left( {{\rm{8}}{\rm{.33}}} \right) - {\rm{\dot Q}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right)} \right]} \right\}$$</div>
-
-<div>$${\rm{\dot E}}_h^{k = 1}\left( {{\rm{1}}{\rm{.67}}} \right) = 0.985 \cdot \left\{ {{\rm{\dot E}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right) + 0.6\left[ {{\rm{\dot E}}_h^{k = 1}\left( {{\rm{8}}{\rm{.33}}} \right) - {\rm{\dot E}}_h^{k = 1}\left( {{\rm{ - 8}}{\rm{.33}}} \right)} \right]} \right\}$$</div>
-
-The heating capacity delivered and electric power input of the heat pump when operating at maximum (high) compressor speed and outdoor air temperature of *T<sub>j</sub>* is given by:
-
-<div>$$\dot Q_h^{k = 2}({T_j}) = \left\{ \begin{array}{l}\dot Q_h^{k = 2}( - 8.33) + \frac{{\left[ {\dot Q_h^{k = 2}(8.33) - \dot Q_h^{k = 2}( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{8.33 + 8.33}},\quad IF\,{T_j} \ge 7.2^\circ C\,or\,{T_j} \le  - 8.33^\circ C\\\dot Q_h^{k = 2}( - 8.33) + \frac{{\left[ {\dot Q_h^{k = 2}(1.67) - \dot Q_h^{k = 2}( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{1.67 + 8.33}},\quad IF\, - 8.33^\circ C &lt; {T_j} &lt; 7.2^\circ C\end{array} \right.$$</div>
-
-<div>$$\dot E_h^{k = 2}({T_j}) = \left\{ \begin{array}{l}\dot E_h^{k = 2}( - 8.33) + \frac{{\left[ {\dot E_h^{k = 2}(8.33) - \dot E_h^{k = 2}( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{8.33 + 8.33}},\quad IF\,{T_j} \ge 7.2^\circ C\,or\,{T_j} \le  - 8.33^\circ C\\\dot E_h^{k = 2}( - 8.33) + \frac{{\left[ {\dot E_h^{k = 2}(1.67) - \dot E_h^{k = 2}( - 8.33)} \right] \cdot \left( {{T_j} + 8.33} \right)}}{{1.67 + 8.33}},\quad IF\, - 8.33^\circ C &lt; {T_j} &lt; 7.2^\circ C\end{array} \right.$$</div>
-
-Where,
-
-<span>\(\dot Q_h^{k = 2}\left( {{\rm{8}}{\rm{.33}}} \right),\,{\rm{and}}\,\dot E_h^{k = 2}\left( {{\rm{8}}{\rm{.33}}} \right)\)</span>are determined from H1<sub>2</sub> test
-
-<span>\(\dot Q_h^{k = 2}\left( {{\rm{1}}{\rm{.67}}} \right),\,{\rm{and}}\,\dot E_h^{k = 2}\left( {{\rm{1}}{\rm{.67}}} \right)\)</span>are determined from H2<sub>2</sub> test
-
-<span>\(\dot Q_h^{k = 2}\left( {{\rm{ - 8}}{\rm{.33}}} \right),\,{\rm{and}}\,\dot E_h^{k = 2}\left( {{\rm{ - 8}}{\rm{.33}}} \right)\)</span>are determined from H3<sub>2</sub> test
-
-The electric energy used by the heat pumps differs depending up on whether the heat pump would operate at low (minimum) capacity, cycle between successive lower and higher speed capacities, or operate at high speed capacity in responding to the building load.  The procedure for each operation cases is described next.
-
-*Case 1*:  The steady state heating capacity when the unit is operating at minimum or low capacity, i.e., when the building heating load is less or equal to the low capacity:
-
-<div>$$\dot Q_c^{k = 1}\left( {{T_j}} \right) \ge BL\left( {{T_j}} \right)$$</div>
-
-<div>$$\frac{{{{\rm{e}}_h}\left( {{{\rm{T}}_{\rm{j}}}} \right)}}{{\rm{N}}}{\rm{ = }}\frac{{{{\rm{X}}^{k = 1}}\left( {{{\rm{T}}_{\rm{j}}}} \right) \cdot {\rm{\dot E}}_h^{k = 1}\left( {{{\rm{T}}_{\rm{j}}}} \right) \cdot {\rm{\delta }}\left( {{{\rm{T}}_{\rm{j}}}} \right)}}{{PL{F_j}}} \cdot \frac{{{{\rm{n}}_{\rm{j}}}}}{{\rm{N}}}$$</div>
-
-<div>$$\frac{{RH\left( {{{\rm{T}}_{\rm{j}}}} \right)}}{{\rm{N}}}{\rm{ = }}BL\left( {{{\rm{T}}_{\rm{j}}}} \right) \cdot \left[ {{\rm{1 - }}{{\rm{\delta }}^\prime}\left( {{{\rm{T}}_{\rm{j}}}} \right)} \right] \cdot \frac{{{{\rm{n}}_{\rm{j}}}}}{{\rm{N}}}$$</div>
-
-<div>$${{\rm{X}}^{k = 1}}\left( {{{\rm{T}}_{\rm{j}}}} \right){\rm{ = MIN}}\left\{ \begin{array}{l}BL\left( {{{\rm{T}}_{\rm{j}}}} \right){\rm{/\dot Q}}_h^{k = 1}\left( {{{\rm{T}}_{\rm{j}}}} \right)\\1.0\end{array} \right\}$$</div>
-
-<div>$${\delta ^\prime}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{) = }}\left\{ \begin{array}{l}0,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{off}}}}\,\\1/2,\quad {\rm{if}}\,{{\rm{T}}_{{\rm{off}}}} &lt; {{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{on}}}}\\1,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, > \,{{\rm{T}}_{{\rm{on}}}}\end{array} \right\}$$</div>
-
-<div>$$PL{F_{\rm{j}}}{\rm{ = 1 - }}C_D^h \cdot \left[ {{\rm{1 - }}{{\rm{X}}^{k = 1}}{\rm{(}}{T_j}{\rm{)}}} \right]$$</div>
-
-<div>$$C_D^h{\rm{ = MIN}}\left\{ \begin{array}{l}{\rm{C}}_{\rm{D}}^{\rm{h}},\,{\rm{calculated}}\,{\rm{using}}\,{\rm{Equation}}\,{\rm{24}}\\0.25\end{array} \right\}$$</div>
-
-*Case 2*:  The unit cycles between the low (minimum) and high (maximum) compressor capacity to meet the building heating load at outdoor air temperature *T<sub>j</sub>*.  That is, the heating building load is between the unit low and high compressor capacities:
-
-<div>$$\dot Q_h^{k = 1}({T_j}) &lt; BL({T_j}) &lt; \dot Q_h^{k = 2}({T_j})$$</div>
-
-<div>$$\frac{{{e_c}({T_j})}}{N} = \left[ {{X^{k = 1}}({T_j}) \cdot \dot E_h^{k = 1}({T_j}) + {X^{k = 2}}({T_j}) \cdot \dot E_h^{k = 2}({T_j})} \right] \cdot {\delta ^\prime}({T_j}) \cdot \frac{{{n_j}}}{N}$$</div>
-
-<div>$$\frac{{RH\left( {{{\rm{T}}_{\rm{j}}}} \right)}}{{\rm{N}}}{\rm{ = BL}}\left( {{{\rm{T}}_{\rm{j}}}} \right) \cdot \left[ {{\rm{1 - }}{{\rm{\delta }}^\prime}\left( {{{\rm{T}}_{\rm{j}}}} \right)} \right] \cdot \frac{{{n_j}}}{N}$$</div>
-
-<div>$${\delta ^\prime}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{) = }}\left\{ \begin{array}{l}0,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{off}}}}\,\\ {\textstyle{1 \over 2}},\quad {\rm{if}}\,{{\rm{T}}_{{\rm{off}}}} &lt; {{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{on}}}}\\ 1,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, > \,{{\rm{T}}_{{\rm{on}}}}\end{array} \right\}$$</div>
-
-<div>$${X^{k = 1}}({T_j}) = \frac{{\dot Q_h^{k = 2}({T_j}) - BL({T_j})}}{{\dot Q_h^{k = 2}({T_j}) - \dot Q_h^{k = 1}({T_j})}}$$</div>
-
-<div>$${X^{k = 2}}({T_j}) = 1 - {X^{k = 1}}({T_j})$$</div>
-
-*Case 3*:  The steady-state heating capacity when the unit is operating continuously at high or maximum compressor capacity at outdoor air temperature *T<sub>j</sub>*. The building heating load is greater than the available capacity at maximum or high compressor capacity:
-
-<div>$$BL\left( {{T_j}} \right) \ge \dot Q_c^{k = 2}\left( {{T_j}} \right)$$</div>
-
-For units when operating continuously at maximum compressor speed (k=2) speed at temperature *T<sub>j</sub>*, the delivered heating capacity and electric power inputs are calculated as follows:
-
-<div>$$\frac{{{e_c}({T_j})}}{N} = \left[ {\dot E_h^{k = 2}({T_j}) \cdot {\delta ^``}({T_j})} \right] \cdot \frac{{{n_j}}}{N}$$</div>
-
-<div>$$\frac{{RH\left( {{T_j}} \right)}}{N}{\rm{ = }}\left\{ {BL\left( {{{\rm{T}}_{\rm{j}}}} \right) - \left[ {{\rm{\dot Q}}_h^{k = 2}\left( {{{\rm{T}}_{\rm{j}}}} \right) \cdot {{\rm{\delta }}^``}\left( {{{\rm{T}}_{\rm{j}}}} \right)} \right]} \right\} \cdot \frac{{{n_j}}}{N}$$</div>
-
-<div>$${\delta ^``}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{) = }}\left\{ \begin{array}{l}0,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{off}}}}\,{\rm{or}}\,\frac{{{\rm{\dot Q}}_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}}{{\dot E_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}}\, &lt; \,1\\ {\textstyle{1 \over 2}},\quad {\rm{if}}\,{{\rm{T}}_{{\rm{off}}}} &lt; {{\rm{T}}_{\rm{j}}}\, \le \,{{\rm{T}}_{{\rm{on}}}}\,{\rm{and}}\,\frac{{{\rm{\dot Q}}_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}}{{\dot E_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}} \ge \,1\;\\1,\quad {\rm{if}}\,{{\rm{T}}_{\rm{j}}}\, > \,{{\rm{T}}_{{\rm{on}}}}\,{\rm{and}}\,\frac{{{\rm{\dot Q}}_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}}{{\dot E_h^{k = 2}{\rm{(}}{{\rm{T}}_{\rm{j}}}{\rm{)}}}} \ge \,1\;\end{array} \right\}$$</div>
-
-X(T<sub>j</sub>)            =          the heating mode load factor for temperature bin j, (-)
-
-<span>\({{\rm{\dot Q}}_{\rm{h}}}\left( {{{\rm{T}}_{\rm{j}}}} \right)\)</span>     =          space heating capacity of the heat pump when operating at outdoor temperature T<sub>j</sub>, W
-
-<span>\({{\rm{\dot E}}_{\rm{h}}}\left( {{{\rm{T}}_{\rm{j}}}} \right)\)</span>      =          electrical power consumption of the heat pump when operating at outdoor temperature T<sub>j</sub>, W
-
-<span>\({\rm{\delta }}\left( {{{\rm{T}}_{\rm{j}}}} \right)\)</span>        =          the heat pump low temperature cut-off factor, (-)
-
-T<sub>off</sub>  =          the outdoor temperature when the compressor is automatically shut off, °C. (If no such temperature exists, Tj is always greater than T<sub>off</sub> and T<sub>on</sub>).
-
-T<sub>on</sub>  =          the outdoor temperature when the compressor is automatically turned back on, if applicable, following an automatic shut-off, °C.
-
-Table 62. Heating Mode Test Conditions for Units Having Two-Capacity Compressor
-
-<table class="table table-striped">
-  <tr>
-    <th rowspan="2">Test Description</th>
-    <th colspan="2">Air Entering Indoor Unit Temperature</th>
-    <th colspan="2">Air Entering Outdoor Unit Temperature</th>
-    <th rowspan="2">Compressor Speed</th>
-    <th rowspan="2">Heating Air Volume Flow Rate</th>
-  </tr>
-  <tr>
-    <td>Dry Bulb C (F)</td>
-    <td>Wet Bulb C (F)</td>
-    <td>Dry Bulb C (F)</td>
-    <td>Wet Bulb C (F)</td>
-  </tr>
-  <tr>
-    <td>H01 Test (required,steady)</td>
-    <td>21.1 (70)</td>
-    <td>15.6 (60) (max)</td>
-    <td>16.7 (62)</td>
-    <td>18.3 (56.5)</td>
-    <td>Low</td>
-    <td>Heating Minimum (1)</td>
-  </tr>
-  <tr>
-    <td>H12 Test (required,steady)</td>
-    <td>21.1 (70)</td>
-    <td>15.6 (60) (max)</td>
-    <td>8.33 (47)</td>
-    <td>6.11 (43)</td>
-    <td>High</td>
-    <td>Heating Full-Load (2)</td>
-  </tr>
-  <tr>
-    <td>H1C2 Test (required, cyclic)</td>
-    <td>21.1 (70)</td>
-    <td>15.6 (60) (max)</td>
-    <td>8.33 (47)</td>
-    <td>6.11 (43)</td>
-    <td>High</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>H11 Test (required,steady)</td>
-    <td>21.1 (70)</td>
-    <td>15.6 (60) (max)</td>
-    <td>8.33 (47)</td>
-    <td>6.11 (43)</td>
-    <td>Low</td>
-    <td>Heating Minimum (1)</td>
-  </tr>
-  <tr>
-    <td>H1C1 Test (required, cyclic)</td>
-    <td>21.1 (70)</td>
-    <td>15.6 (60) (max)</td>
-    <td>8.33 (47)</td>
-    <td>6.11 (43)</td>
-    <td>Low</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>H22 Test (required)</td>
-    <td>21.1 (70)</td>
-    <td>15.6 (60) (max)</td>
-    <td>1.67 (35)</td>
-    <td>0.56 (33)</td>
-    <td>High</td>
-    <td>Heating Full-Load</td>
-  </tr>
-  <tr>
-    <td>H21 Test (required)</td>
-    <td>21.1 (70)</td>
-    <td>15.6 (60) (max)</td>
-    <td>1.67 (35)</td>
-    <td>0.56 (33)</td>
-    <td>Low</td>
-    <td>Heating Minimum</td>
-  </tr>
-  <tr>
-    <td>H32 Test (required,steady)</td>
-    <td>21.1 (70)</td>
-    <td>15.6 (60) (max)</td>
-    <td>-8.33 (17)</td>
-    <td>-9.44 (15)</td>
-    <td>High</td>
-    <td>Heating Full-Load</td>
-  </tr>
-  <tr>
-    <td>H31 Test (required,steady)</td>
-    <td>21.1 (70)</td>
-    <td>15.6 (60) (max)</td>
-    <td>-8.33 (17)</td>
-    <td>-9.44 (15)</td>
-    <td>Low</td>
-    <td>Heating Minimum</td>
-  </tr>
-</table>
-
-#### References:
-
-AHRI 2008. ANSI/AHRI Standard 210/240: 2008 Standard for Performance Rating of Unitary Air-Conditioning & Air-Source Heat Pump Equipment.  Arlington, VA:  Air-Conditioning, Heating, and Refrigeration Institute.
-
-See the references for the single speed DX heating coil earlier in this document.
-
-### Variable Speed DX Heating Coil
-
-#### Overview
-
-The latest technology for commercial air conditioners and air-to-air heat pumps can utilize a variable speed compressor with a variable speed indoor blower and outdoor fan. The indoor and outdoor air flow rates are usually a function of the compressor speed. Refrigerant mass flow rate is a function of compressor speed as well as outdoor heat exchanger entering air temperature and indoor dry bulb or wet bulb. The control system adjusts the equipment capacity based on zone temperature measurements relative to the thermostat set point. The control logic determines what compressor speed is required to control to the zone temperature requirement in response to increased or decreased capacity (heating or cooling load). The compressor, fan and blower speeds are not discrete values and can be considered to vary infinitesimally between the minimum and maximum compressor speed. At the minimum compressor speed (which is different for heating and cooling), for a continuous fan, the supply airflow is fixed and the unit will have to cycle for reduced part loads below this point. For a cycling fan, the fan will cycle with the compressor.
-
-Similar to variable-speed water source heat pump, we expand the number of speed levels and the corresponding curve sets up to ten. The number of speed levels is selectable by the user. The user can provide speed levels at any number from 1 to 10. In the case that the given speed levels are above 1, the model would do linear interpolation between neighboring speeds. The more curves, the more accurate. Furthermore, using linear interpolation and inputting air flow rates at individual speed levels facilitates arbitrary relationships of flow rate as a function of the compressor speed level.
-
-The Coil:Heating:DX:VariableSpeed object will simulate the performance of a DX heating coil used in combination with a variable-speed air-to-air heat pump. It will fit into the parent objects of AirLoopHVAC:UnitaryHeatPump:AirToAir and
-
-ZoneHVAC:PackagedTerminalHeatPump, etc.
-
-The rated conditions for obtaining the capacities and COPs  are at indoor dry-bulb temperature of 21.1 ˚C (70 ˚F) and the source side entering air temperature of 8.3 ˚C (47 ˚F). Some equations are provided below to help explain the function of the various performance curves and data fields.
-
-#### Model Description
-
-The Coil:Heating:DX:VariableSpeed object is modeled similar to Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit. Of course, rather than referencing a water source evaporator, the new coil object references an air source and has defrosting operation. The evaporator entering air temperature is used in  lieu of the entering  water temperature.
-
-It shall be noted for the capacity and flow rate inputs, two fields are autosizable, which are Rated Heating Capacity at the Selected Nominal Speed Level and the Rated Volumetric Air Flow Rate at the Selected Nominal Speed Level. They are used to scale the performances of a specific unit and correlate with the actual loop flow. Except these two fields, all other capacity and flow rate inputs at individual speed levels should be directly obtained from Reference Unit catalog data, specific to an actual unit.
-
-The Rated Heating Capacity at Selected Nominal Speed Level contains the rated capacity to match the building heating load at the design day.  The rated heating capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
-
-<div>$${\rm{CapacityScaleFactor}} = \frac{{{\rm{RatedTotalHeatingCapacity}}}}{{{\rm{ReferenceUnitTotalHeatingCapacity}}@{\rm{NominalSpeedLevel}}}}$$</div>
-
-And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below:
-
-<div>$$\begin{array}{l}{\rm{RatedTotalHeatingCapacity}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = {\rm{CapacityScaleFactor}} \times \\ \quad \quad \quad {\rm{ReferenceUnitTotalHeatingCapacity}}@{\rm{SpeedLevel}}({\rm{x}})\end{array}$$</div>
-
-The Rated Volumetric Air Flow Rate is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects, as follows:
-
-<div>$${\rm{AirFlowScaleFactor}} = \frac{{{\rm{RatedVolumetricAirFlowRate}}}}{{{\rm{ReferenceUnitVolAirFlowRate}}@{\rm{NominalSpeedLevel}} \times {\rm{CapacityScaleFactor}}}}$$</div>
-
-And the loop volumetric air flow rates at various speed levels in the parent objects are calculated as below:
-
-<div>$$\begin{array}{l}{\rm{LoopVolumetricAirFlowRate}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = {\rm{AirFlowScaleFactor}} \times \\\quad \quad \quad {\rm{ReferenceUnitVolAirFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) \times {\rm{CapacityScaleFactor}}\end{array}$$</div>
-
-If the volumetric air flow rate at one speed level is higher than the flow rate allowed by the fan in the parent object, the flow rate will be set back to the fan flow rate.
-
-If <span>\({\rm{AirFlowScaleFactor}}\)</span> equals unity, the loop air flow rate becomes the design flow rate of the Reference Unit (after scaled by the rated heating capacity). The Rated Volumetric Air Flow Rate is introduced here to correlate with the actual flow rate in the air loop, in case that it differs from the design specification. Certainly, it is recommended that the Rated Volumetric Air Flow Rate is selected in the way that <span>\({\rm{AirFlowScaleFactor}}\)</span> is unity, so as to get more accurate results from the performance curves.
-
-#### Performance curves:
-
-This object includes 4 curve objects at each individual speed level.
-
-1)  Total heating capacity modifier curve (function of temperature).
-
-2)  Total heating capacity modifier curve (function of air flow fraction).
-
-3)  Energy input ratio (EIR) modifier curve (function of temperature).
-
-4)  Energy input ratio (EIR) modifier curve (function of air flow fraction).
-
-The flow fraction modifier curves are used as a placeholder, to account for off-design flow rates if needed. If the manufacturer doesn’t provide off-design performances, we can simply use a default modification multiplier of 1.0.
-
-At the lowest speed, there will be one additional performance curve to account for the part-load condition, i.e.
-
-5)  Part load fraction correlation (function of part load ratio).
-
-1) Total heating capacity modifier curve (function of temperature)
-
-The total heating capacity modifier as a function of temperature curve (CAP-FT) is a biquadratic curve with two independent variables: dry-bulb temperature of the air entering the heating coil and the air DB temperature entering the evaporator coil. The output of this curve is multiplied by the rated total heating capacity at the speed, to give the total heating capacity at the specific entering air temperatures at which the ASHP unit is operating (i.e., at temperatures different from the rating point temperatures). 
-
-<div>$${\rm{TotCapTempModFac}} = {\rm{a}} + {\rm{b*D}}{{\rm{B}}_{\rm{i}}} + {\rm{c*DB}}_{\rm{i}}^2 + {\rm{d*D}}{{\rm{B}}_{\rm{o}}} + {\rm{e*D}}{{\rm{B}}_{\rm{o}}}^2 + {\rm{f*D}}{{\rm{B}}_{\rm{i}}}{\rm{*D}}{{\rm{B}}_{\rm{o}}}$$</div>
-
-where
-
-DB<sub>i</sub> = dry-bulb temperature of the air entering the heating coil, °C
-
-DB<sub>o</sub> = dry-bulb temperature of the air entering the outdoor coil, °C
-
-a-f = regression curve-fit coefficients
-
-2) Total heating capacity modifier curve (function of air flow fraction)
-
-<div>$${\rm{TotCapAirFlowModFac}} = {\rm{a}} + {\rm{b*f}}{{\rm{f}}_{\rm{a}}} + {\rm{c*ff}}_{\rm{a}}^2 + {\rm{d*ff}}_{\rm{a}}^3$$</div>
-
-where
-
-ff<sub>a</sub> = actual air mass flow rate/design air mass flow rate, at one speed level;
-
-<div>$$\begin{array}{l}{\rm{DesignAirMassFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) = {\rm{ReferenceUnitAirMassFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) \times \\\quad \quad \quad {\rm{CapacityScaleFactor}}\end{array}$$</div>
-
-a-d = regression curve-fit coefficients, if no data available for the correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-3) Energy input ratio (EIR) modifier curve (function of temperature)
-
-The energy input ratio modifier curve as a function of temperature (EIR-FT) is a biquadratic curve with two independent variables DB<sub>i</sub>  and DB<sub>o</sub>. The output of this curve is multiplied by the rated EIR at the speed (inverse of the rated COP), to give the EIR at the specific entering air temperatures at which the ASHP coil unit is operating (i.e., at temperatures different from the rating point temperatures).
-
-<div>$${\rm{EIRTempModFac}} = {\rm{a}} + {\rm{b*D}}{{\rm{B}}_{\rm{i}}} + {\rm{c*DB}}_{\rm{i}}^2 + {\rm{d*D}}{{\rm{B}}_{\rm{o}}} + {\rm{e*D}}{{\rm{B}}_{\rm{o}}}^2 + {\rm{f*D}}{{\rm{B}}_{\rm{i}}}{\rm{*D}}{{\rm{B}}_{\rm{o}}}$$</div>
-
-where
-
-a-f = regression curve fit coefficients.
-
-4) Energy input ratio (EIR) modifier curve (function of air flow fraction)
-
-<div>$${\rm{EIRAirFlowModFac}} = {\rm{a}} + {\rm{b*f}}{{\rm{f}}_{\rm{a}}} + {\rm{c*ff}}_{\rm{a}}^2 + {\rm{d*ff}}_{\rm{a}}^3$$</div>
-
-where
-
-a-d = regression curve-fit coefficients, if no data available for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-5) Part load fraction correlation (function of part load ratio)
-
-This field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, heating load/steady-state heating capacity for Speed 1),
-
-<div>$${\rm{PartLoadFrac}} = {\rm{a}} + {\rm{b*PLR}} + {\rm{c*PL}}{{\rm{R}}^2} + {\rm{d*PL}}{{\rm{R}}^3}$$</div>
-
-And
-
-RTF = (PLR/PartLoadFrac) = runtime fraction of the heating coil.
-
-The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor runs continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7 and PLF &gt;= PLR
-
-If PLF &lt; 0.7, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, the runtime fraction of the coil is limited to 1.0. A typical part load fraction correlation would be:
-
-<div>$${\rm{PLF}} = 0.85 + 0.15 \times {\rm{PLR}}$$</div>
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-<div>$${\rm{PLF}} = 0.85 + 0.0 \times {\rm{PLR}}$$</div>
-
-#### Lowest Speed Operation:
-
-The lowest speed operation of the variable-speed DX heating coil is similar to the single speed DX heating coil. The total (gross) heating capacity of the variable-speed DX coil is calculated as follows:
-
-<div>$$\begin{array}{l}{{\rm{Q}}_{{\rm{total}},1}} = {\rm{RatedTotalHeatingCapacity}}@{\rm{SpeedLevel}}\left( 1 \right){\rm{*}}\\\quad \quad \quad {\rm{TotCapTemModFa}}{{\rm{c}}_1}{\rm{*TotCapAirFlowModFa}}{{\rm{c}}_1}\end{array}$$</div>
-
-And the EIR is calculated as:
-
-<div>$${\rm{EI}}{{\rm{R}}_1} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}(1)}}{\rm{*EIRTempModFa}}{{\rm{c}}_1}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_1}$$</div>
-
-And the power consumption including the compressor, outdoor fan and accessories (not including indoor fan power) is,
-
-<div>$${\rm{Powe}}{{\rm{r}}_1} = {{\rm{Q}}_{{\rm{total}},1}}{\rm{*EI}}{{\rm{R}}_1}{\rm{*RTF}}$$</div>
-
-The fraction of the actual air mass flow to the design air mass flow rate is calculated:
-
-<div>$${\rm{f}}{{\rm{f}}_{{\rm{a}},1}} = \frac{{{\rm{actualairmassflowrate}}}}{{({\rm{ReferenceUnitAirMassFlowRate}}@{\rm{SpeedLevel}}(1) \times {\rm{CapacityScaleFactor}})}}{\rm{}}$$</div>
-
-#### Higher Speed Operation:
-
-At the speed level between the lowest and the highest, there is no part-load loss. A parameter of speed ratio (SpeedRatio) is used to define the capacity partition between Speed x-1 and Speed x.
-
-The design air flow rate at the speed ratio are given as following:
-
-<div>$$\begin{array}{l}{\rm{DesignAirFlowRateSpeedRatio}} = {\rm{ReferenceUnitAirMassFlowRate}}@{\rm{SpeedLevel}}\left( {{\rm{x}} - 1} \right){\rm{*}}\\\quad \quad \quad {\rm{CapacityScaleFactor*}}\left( {1{\rm{}}--{\rm{SpeedRatio}}} \right) + \\\quad \quad {\rm{ReferenceUnitAirMassFlowRate}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right){\rm{*}}\\\quad \quad \quad {\rm{CapacityScaleFactor*SpeedRatio}}\end{array}$$</div>
-
-And the fractions of air flow is given:
-
-<span>\({\rm{f}}{{\rm{f}}_{{\rm{a}},{\rm{x}} - 1}}\)</span>=<span>\({\rm{f}}{{\rm{f}}_{{\rm{a}},{\rm{x}}}}\)</span>= actual air mass flow rate/DesignAirFlowRateSpeedRatio
-
-The total heating capacities and EIRs at Speed x-1 and Speed x are given:
-
-<div>$${{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}} = {\rm{RatedTotalHeatingCapacity}}@{\rm{SpeedLevel}}\left( {{\rm{x}} - 1} \right){\rm{*TotCapTempModFa}}{{\rm{c}}_{{\rm{x}} - 1}}{\rm{*TotCapAirFlowModFa}}{{\rm{c}}_{{\rm{x}} - 1}}$$</div>
-
-<div>$${{\rm{Q}}_{{\rm{total}},{\rm{x}}}} = {\rm{RatedTotalHeatingCapacity}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right){\rm{*TotCapTempModFa}}{{\rm{c}}_{\rm{x}}}{\rm{*TotCapAirFlowModFa}}{{\rm{c}}_{\rm{x}}}$$</div>
-
-<div>$${\rm{EI}}{{\rm{R}}_{{\rm{x}} - 1}} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}({\rm{x}} - 1)}}{\rm{EIRTempModFa}}{{\rm{c}}_{{\rm{x}} - 1}}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_{{\rm{x}} - 1}}$$</div>
-
-<div>$${\rm{EI}}{{\rm{R}}_{\rm{x}}} = \frac{{1.0}}{{{\rm{ReferenceUnitCOP}}@{\rm{Speed}}({\rm{x}})}}{\rm{EIRTempModFa}}{{\rm{c}}_{\rm{x}}}{\rm{*EIRAirFlowModFa}}{{\rm{c}}_{\rm{x}}}$$</div>
-
-The total heating capacity at the corresponding speed ratio is:
-
-<div>$${{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}} = \left( {1.0 - {\rm{SpeedRatio}}} \right){\rm{*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}} + {\rm{SpeedRatio*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}}}}$$</div>
-
-And the power consumption is
-
-<div>$${\rm{Powe}}{{\rm{r}}_{{\rm{SpeedRatio}}}} = \left( {1.0 - {\rm{SpeedRatio}}} \right){\rm{*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}} - 1}}{\rm{*EI}}{{\rm{R}}_{{\rm{x}} - 1}} + {\rm{SpeedRatio*}}{{\rm{Q}}_{{\rm{total}},{\rm{x}}}}{\rm{*EI}}{{\rm{R}}_{\rm{x}}}$$</div>
-
-The total amount of heat absorbed by the outdoor evaporator is calculated as:
-
-<div>$${{\rm{Q}}_{{\rm{evap}},{\rm{SpeedRatio}}}} = {{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}} - {\rm{Powe}}{{\rm{r}}_{{\rm{SpeedRatio}}}}$$</div>
-
-At last,
-
-<div>$${{\rm{Q}}_{{\rm{total}},{\rm{SpeedRatio}}}} = {\rm{HeatingLoad}}$$</div>
-
-If the speed reaches the highest level, the speed ratio becomes 1.0, and Speed x represents the highest speed.
-
-#### Defrost Operation:
-
-The defrost operation of a variable-speed DX heating coil is treated the same as the single-speed DX heating coil, except using the total heating capacity at the max speed level to replace the rated heating capacity of the single-speed DX coil, when a reverse-cycle defrost strategy is specified.
-
-We keep the defrost energy input ratio (EIR) modifier curve (function of temperature) as the single speed DX heating coil. It is a biquadratic curve with two independent variables: outdoor air dry-bulb temperature and the heating coil entering air wet-bulb temperature. The output of this curve is multiplied by the heating coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the coil is operating. This curve is only required when a reverse-cycle defrost strategy is specified.
-
-<div>$${\rm{DefrostEIRTempModFac}} = {\rm{a}} + {\rm{b*W}}{{\rm{B}}_{\rm{i}}} + {\rm{c*WB}}_{\rm{i}}^2 + {\rm{d*D}}{{\rm{B}}_{\rm{o}}} + {\rm{e*D}}{{\rm{B}}_{\rm{o}}}^2 + {\rm{f*W}}{{\rm{B}}_{\rm{i}}}{\rm{*D}}{{\rm{B}}_{\rm{o}}}$$</div>
-
-where
-
-WB<sub>i</sub> = wet-bulb temperature of the air entering the indoor coil, °C
-
-DB<sub>o</sub> = dry-bulb temperature of the air entering the outdoor coil, °C
-
-a-f = regression curve-fit coefficients
-
-#### Crankcase Heater Operation:
-
-It is the same as the single-speed DX heating coil.
-
-### Desuperheater-Recovery-Based Air Heating Coil
-
-#### Overview
-
-The input object Coil:Heating:Desuperheater provides a model that simulates the thermal performance of a refrigerant-to-air heating coil and the parasitic electric consumption of its control valves or other auxiliary devices. The model assumes that the heating energy provided by this coil is reclaimed from the superheated refrigerant gas leaving a compressor and does not impact the performance of the compressor. The objects from which this coil can obtain its heating energy are:
-
-Coil:Cooling:DX:SingleSpeed
-
-Coil:Cooling:DX:TwoSpeed
-
-Coil:Cooling:DX:TwoStageWithHumidityControlMode
-
-Refrigeration:CompressorRack
-
-Refrigeration:Condenser\* (multiple objects)
-
-The heat reclaim recovery efficiency (specified by the user) defines the amount of heat available for use by this coil. Approximately 25-30% of the energy rejected by typical refrigeration system condensers is to reduce the superheated refrigerant vapor temperature to the condensing temperature. Recovery efficiencies higher than 30% may cause the refrigerant gas to condense which in turn impacts the performance of the refrigeration compressor rack. For this reason, the maximum heat reclaim recovery efficiency for this coil for all sources except the Refrigeration:Condenser:(Air, Water, or Evap)Cooled is 30%.For these refrigeration condensers, the amount of waste energy available in the superheat region is explicitly calculated, so for these condensers the maximum heat recovery efficiency is 90% of this superheat energy. Also, for these refrigeration condensers, an estimate of the temperature of the reclaimed heat source is made and compared to the inlet air temperature for the coil. If the reclaimed heat source is too cool, the amount of available reclaim energy is set to zero.
-
-NOTE: When the heating source is a refrigeration compressor rack, the heat rejection location in the Refrigeration:CompressorRack object must be “Outdoors�. If the compressor rack heat rejection location is “Zone�, the total amount of heat rejection available for reclaim (e.g., by this desuperheater heating coil) is set to zero by the compressor rack object and the simulation proceeds.
-
-The sources for the waste heat can also be used to supply other coils.  To avoid double-counting this waste heat, the amount available is corrected to reflect these other uses. For the three DX Cooling Coil sources, this correction is made within the same time step loop.  For the two refrigeration system sources, the correction is made using the value from the previous time step.
-
-The desuperheater heating coil can be used in air loop simulations for various air heating applications. For example, it can be used as an air reheat coil for high humidity control in the compound objects AirLoopHVAC:Unitary:Furnace:HeatCool and AirLoopHVAC:UnitaryHeatCool (see High Humidity Control With HeatCool Configuration). For this application, the desuperheater coil is controlled based on the calculated heating load to maintain the zone temperature and humidity setpoints (load-based control). The source of reclaimed heat could be the direct expansion (DX) cooling coil itself (Coil:Cooling:DX:SingleSpeed) or a refrigerated case compressor rack (Refrigeration:CompressorRack).
-
-The desuperheater heating coil can also be used with cooling/heating systems that maintain specific air loop (deck) temperatures. For example, Figure 171 shows a schematic diagram of the desuperheater heating coil used in conjunction with the CoilSystem:Cooling:DX object. The desuperheater heating coil must be placed downstream of the DX cooling coil when reclaiming heat from that cooling coil’s compressor(s). Desuperheating heating coil placement is unrestricted when reclaiming heat from a refrigeration compressor rack or refrigeration condenser. The configuration in Figure 171 shows the heating coil being controlled via a temperature-based strategy. In this example, the DX cooling coil could be used to the maintain its discharge air temperature at 11°C for zone dehumidification. The desuperheater heating coil could then raise the air dry-bulb temperature to 16°C providing a dry supply air stream at a temperature which does not require much additional heating by terminal units to meet the zone temperature setpoint.
-
-![Schematic\_DesuperheaterHeatingCoil](media/image4016.png)
-
-Figure 171. Desuperheater Heating Coil Used as a Reheat Coil with CoilSystem:Cooling:DX
-
-
-
-Since the heating provided by the desuperheater coil is based on available waste heat from another system, the selection of fan control for the air loop equipment is essential for proper modeling. When the coil’s heating source is a direct expansion cooling coil (Coil:Cooling:DX:SingleSpeed, Coil:Cooling:DX:TwoSpeed, or Coil:Cooling:DX:TwoStageWithHumidityControlMode), the air loop’s fan control mode may be auto fan (cycling fan cycling coil), constant fan, or variable volume since the desuperheater heating coil cycles on/off with the DX cooling coil. When the heating source is a compressor rack or condenser for refrigerated cases, the supply air fan control should be either variable volume or constant fan since the desuperheater heating coil will typically be available the entire simulation time step.
-
-NOTE: Use of the desuperheater heating coil in variable air volume systems should be done with caution since the model assumption of a fixed heat reclaim recovery efficiency may not be valid if the air flow rate over the coil varies significantly.
-
-The following sections describe the calculations used for both the load-based and temperature-based strategies that can control the desuperheater heating coil.
-
-#### Model Inputs
-
-A minimum of seven inputs must be defined for the desuperheater heating coil. The user must input the coil’s name, an availability schedule name, and the heat reclaim recovery efficiency (default of 25%, with a range of 0% to 30% except for detailed refrigeration condensers which have a default of 80%, with a range of 0% to 90%). The next two inputs are the heating coil’s inlet and outlet air node names. The user must also enter the desuperheater heat source type and name which are validated when the model inputs are read into the program.
-
-The final two fields are optional. The first of these is the coil temperature setpoint node name. This field is used when the desuperheater heating coil is controlled based on an air loop temperature and a setpoint manager (Ref. SetpointManager:\*) is used to place a temperature setpoint on this air node. The latter of these optional fields is the parasitic electric load. This field allows the user to define the electric energy use of parasitic equipment associated with the desuperheater heating coil (e.g. control valves).
-
-#### Model Description
-
-The model calculates the thermal performance of the heating coil based on the control strategy used. When a temperature setpoint node name is not entered, the control type is assumed to be load-based operation. This method should be used when this coil is specified as the air reheat coil for high humidity control with the compound object AirLoopHVAC:Unitary:Furnace:HeatCool or AirLoopHVAC:UnitaryHeatCool. If the temperature setpoint node name is entered, the control type is temperature-based operation. This method is used when the heating coil is controlled to maintain a dry-bulb temperature setpoint in an air loop.
-
-#### Load-Based Operation
-
-When load-based operation is selected, a load to be met by the heating coil is requested by the parent object (e.g., AirLoopHVAC:Unitary:Furnace:HeatCool). The model first calculates the heating coil capacity based on the total condenser waste heat rejected by the heating source.
-
-<div>$${\dot Q_{coil}} = {\dot Q_{cond}} \times {\varepsilon_{reclaim}}$$</div>
-
-where:
-
-<span>\({\dot Q_{coil}}\)</span>          = heating capacity of the desuperheater coil (W)
-
-<span>\({\dot Q_{cond}}\)</span>         = total amount of condenser waste heat rejected by the heating source (W)
-
-<span>\({\varepsilon_{reclaim}}\)</span>       = heat reclaim recovery efficiency
-
-The model then compares the coil’s heating capacity to the heating load being requested. If the heating capacity is greater than the heating load, then the amount of reclaimed heat (average heating rate over the simulation time step) is set equal to the requested load and the desuperheater heating coil will cycle off when the requested load is satisfied.
-
-<div>$${\dot Q_{reclaim}} = {\dot Q_{load}}$$</div>
-
-Otherwise the amount of reclaimed heat is set equal to the coil’s heating capacity and the desuperheater heating coil will operate the entire time that the waste heat source operates.
-
-<div>$${\dot Q_{reclaim}} = {\dot Q_{coil}}$$</div>
-
-In either case, the coil’s leaving air temperature is then calculated based on the amount of heat recovered and the air mass flow rate through the coil.
-
-<div>$${T_{out}} = {T_{in}} + \frac{{{{\dot Q}_{reclaim}}}}{{\dot m{C_p}}}$$</div>
-
-where:
-
-<span>\({T_{out}}\)</span>= coil outlet air temperature (°C)
-
-<span>\({T_{in}}\)</span>= coil inlet air temperature (°C)
-
-                                                     <span>\(\)</span>
-
-<span>\(\dot m\)</span>  = air mass flow rate through the heating coil (kg/s)
-
-<span>\({C_p}\)</span> = specific heat of air entering the heating coil (J/kg-C)
-
-A final calculation is made to determine the runtime fraction of the desuperheater heating coil. Since the maximum amount of reclaim heat available is dependent on the runtime fraction of the waste heat source, the runtime fraction of the desuperheater heating coil is the product of the waste heat source’s runtime fraction and the ratio of the amount of heat reclaimed to the desuperheater coil’s heating capacity.
-
-<div>$$RT{F_{coil}} = RT{F_{source}}\left( {\frac{{{{\dot Q}_{reclaim}}}}{{{{\dot Q}_{coil}}}}} \right)$$</div>
-
-where:
-
-<span>\(RT{F_{coil}}\)</span>      = runtime fraction of the desuperheater heating coil
-
-<span>\(RT{F_{source}}\)</span>    = runtime fraction of the desuperheater heating source
-
-The heating coil’s outlet air humidity ratio and air mass flow rate are simply set equal to the coil inlet air values. The outlet air enthalpy is calculated based on the outlet air dry-bulb temperature and the outlet air humidity ratio.
-
-<div>$${h_{out}}\, = \,PsyHFnTdbW({T_{out}},\,\,{\omega_{out}})$$</div>
-
-where
-
-<span>\({h_{out}}\)</span>         = enthalpy of the air leaving the heating coil, J/kg
-
-<span>\(\,{\omega_{out}}\)</span>        = humidity ratio of the air leaving the heating coil, kg/kg
-
-*PsyHFnTdbW* = EnergyPlus psychrometric function, returns enthalpy given dry-bulb temperature and humidity ratio
-
-#### Temperature-Based Operation
-
-When temperature-based operation is selected, the model first calculates the heating coil capacity based on the total condenser waste heat rejected by the heating source (same as for load-based operation).
-
-<div>$${\dot Q_{coil}} = {\dot Q_{cond}} \times {\varepsilon_{reclaim}}$$</div>
-
-The model then calculates the heating load required to reach the desired setpoint temperature.
-
-<div>$${\dot Q_{load}} = \dot m{C_p}\left( {{T_{setpoint}} - {T_{in}}} \right)$$</div>
-
-where:
-
-<span>\({\dot Q_{load}}\)</span>          = heating load to meet the desired dry-bulb temperature setpoint (W)
-
-<span>\({T_{setpoint}}\)</span>       = desired dry-bulb temperature setpoint (°C)
-
-A comparison is then made to determine if the desuperheater heating coil should be energized. If the calculated load is less than or equal to 0, the coil’s inlet air dry-bulb temperature is at or above the setpoint. In this case the desuperheater heating coil is not active and the outlet air dry-bulb temperature is set equal to the inlet air dry-bulb temperature.
-
-<div>$${\dot Q_{reclaim}} = 0$$</div>
-
-<div>$${T_{out}}{\rm{ }} = {\rm{ }}{T_{in}}$$</div>
-
-If the amount of heat required to meet the setpoint is larger than the desuperheater coil’s heating capacity, then the amount of reclaimed heat is set equal to the coil heating capacity and the outlet air dry-bulb temperature is calculated.
-
-<div>$${\dot Q_{reclaim}} = {\dot Q_{coil}}$$</div>
-
-<div>$${T_{out}} = {T_{in}} + \frac{{{{\dot Q}_{reclaim}}}}{{\dot m{C_p}}}$$</div>
-
-If the amount of heat required to meet the setpoint is less than the desuperheater coil’s heating capacity, the amount of reclaimed heat is set equal to the calculated heating load and the outlet air dry-bulb temperature is set equal to the setpoint temperature. In this case the desuperheater heating coil will cycle off when the requested load is satisfied.
-
-<div>$${\dot Q_{reclaim}} = {\dot Q_{load}}$$</div>
-
-<div>$${T_{out}}\quad  = \;{T_{setpoint}}$$</div>
-
-A final calculation is made to determine the runtime fraction of the desuperheater heating coil. Since the maximum amount of reclaim heat available is dependent on the runtime fraction of the waste heat source, the runtime fraction of the desuperheater heating coil is the product of the waste heat source’s runtime fraction and the ratio of the amount of heat reclaimed to the desuperheater coil’s heating capacity.
-
-<div>$$RT{F_{coil}} = RT{F_{source}}\left( {\frac{{{{\dot Q}_{reclaim}}}}{{{{\dot Q}_{coil}}}}} \right)$$</div>
-
-The heating coil’s outlet air humidity ratio and air mass flow rate are simply set equal to the coil inlet air values. The outlet air enthalpy is calculated based on the outlet air dry-bulb temperature and the outlet air humidity ratio.
-
-<div>$${h_{out}}\, = \,PsyHFnTdbW({T_{out}},\,\,{\omega_{out}})$$</div>
-
-#### Parasitic Electric Load
-
-The parasitic electric load attributed to the desuperheater heating coil is calculated using the user-supplied input value (<span>\({P_{parasitic}}\)</span>) and the desuperheater heating coil runtime fraction calculated above.
-
-<div>$${P_{elec}} = {P_{parasitic}} \times RT{F_{coil}}$$</div>
-
-The model assumes that this electric load is small and does not contribute to heating the air stream.
-
-
-
-#### References
-
-Kosar, D. 2006. Dehumidification Enhancements, ASHRAE Journal, Vol. 48, No. 2, February 2006.
-
-Kosar, D. et al. 2006. Dehumidification Enhancement of Direct Expansion Systems Through Component Augmentation of the Cooling Coil. 15<sup>th</sup> Symposium on Improving Building Systems in Hot and Humid Climates, July 24-26, 2006.
-
-Nimmo, B.G. et al. 1993.DEAC: Desiccant Enhancement of Cooling-Based Dehumidification. ASHRAE Transactions, Vol.99, Part 1, Paper number CH-93-4-4, pp. 842-848.
-
-### Desuperheater-Recovery-Based Water Heating Coil
-
-#### Overview
-
-The input object Coil:WaterHeating:Desuperheater provides a model that simulates the thermal performance of a refrigerant-to-water heating coil and the electric consumption of its water circulation pump, control valves, and other auxiliary devices. The model assumes that the heating energy provided by this coil is reclaimed from the superheated refrigerant gas leaving a compressor and does not impact the performance of the compressor. The objects from which this coil can obtain its heating energy are:
-
-Coil:Cooling:DX:SingleSpeed
-
-Coil:Cooling:DX:TwoSpeed
-
-Coil:Cooling:DX:TwoStageWithHumidityControlMode
-
-Refrigeration:CompressorRack
-
-Refrigeration:Condenser\* (multiple objects)
-
-The heat reclaim recovery efficiency (specified by the user) defines the amount of heat available for use by this coil. Approximately 25-30% of the energy rejected by typical refrigeration system condensers is to reduce the superheated refrigerant vapor temperature to the condensing temperature. Recovery efficiencies higher than 30% may cause the refrigerant gas to condense, which in turn impacts the performance of the refrigeration compressor rack. For this reason, the maximum heat reclaim recovery efficiency for this coil for all sources except the Refrigeration:Condenser:(Air, Water, or Evap)Cooled is 30%.For these refrigeration condensers, the amount of waste energy available in the superheat region is explicitly calculated, so for these condensers the maximum heat recovery efficiency is 90% of this superheat energy. Also, for these refrigeration condensers, an estimate of the temperature of the reclaimed heat source is made and compared to the inlet air temperature for the coil. If the reclaimed heat source is too cool, the amount of available reclaim energy is set to zero. For all heat sources, the model includes the ability to modify the heat reclaim recovery efficiency based on variations in inlet water temperature and outdoor air dry-bulb temperature.
-
-NOTE: When the heating source is a refrigerated case compressor rack, the heat rejection location in the Refrigeration:CompressorRack object must be “Outdoors�. If the compressor rack heat rejection location is “Zone�, the total amount of heat rejection available for reclaim (e.g., by this desuperheater heating coil) is set to zero by the compressor rack object and the simulation proceeds.
-
-To model a desuperheater water heating coil, the input data file must include the following objects:
-
-·        Coil:WaterHeating:Desuperheater
-
-·        WaterHeater:Mixed
-
-·        Coil:Cooling:DX:\* or Refrigeration:CompressorRack, or Refrigeration:Condenser:\*
-
-A schematic diagram showing the desuperheater water heating coil with its water heater and DX system condenser is shown below.
-
-![DesuperheaterSchematic\_DS](media/image4049.png)
-
-Figure 172.  Schematic of Desuperheater Water Heating Coil
-
-#### Model Description
-
-The desuperheater heating coil input requires a setpoint temperature schedule and dead band temperature difference, which are independent from the setpoint temperature schedule and dead band temperature difference for the heater (element or burner) associated with the water heater tank. The cut-in temperature for the desuperheater coil is defined as the desuperheater coil’s setpoint temperature minus its dead band temperature difference.
-
-<div>$${T_{cut - in}}\,\, = \,\,{T_{set\,point}}\,\, - \,\,{T_{dead\,band}}$$</div>
-
-where:
-
-<span>\({T_{cut - in}}\)</span>         = Cut-in temperature (°C)
-
-<span>\({T_{set\,point}}\)</span>       = Setpoint temperature (°C)
-
-<span>\({T_{dead\,band}}\)</span>     = Dead band temperature difference (°C)
-
-Desuperheater water heating coils are typically used to offset energy consumption by the water tank’s heater (element or burner). Therefore, the cut-in temperature of the desuperheater coil should always be higher than the water heater tank’s setpoint temperature. At times when the water heater tank’s setpoint temperature is greater than or equal to the cut-in temperature of the desuperheater coil, the desuperheater is disabled and the water heater tank heating element is used to heat the water. An additional input parameter sets the maximum inlet water temperature allowed for desuperheater heat reclaim. Any time the inlet water temperature to the desuperheater coil is above this maximum allowed temperature, heat reclaim is restricted so that the tank water does exceed this temperature.
-
-When the desuperheater coil is scheduled off by its availability schedule, the water heater tank’s setpoint temperature is greater than or equal to the desuperheater coil cut-in temperature, or if the DX system’s compressor (source of heat reclaim) is off, the water heating capacity and water mass flow rate for the desuperheater coil are set to zero and the water heater tank is simulated with the desuperheater heating coil disabled. Otherwise, the simulation proceeds by first determining the maximum amount of heat available for heat reclaim. If a heat reclaim efficiency modifier curve object is specified by the user, this bi-quadratic curve is evaluated using the desuperheater coil inlet water temperature and the outdoor air dry-bulb temperature; otherwise, the output is assumed to be equal to 1.
-
-<div>$$\begin{array}{l}IF\left( {HEffFTemp\,\,is\,\,specified} \right)THEN\\\,\,\,\,\,\,HEffFTemp = \,\,MAX\,\left( {0.0,\,\,f\left( {{T_{water,inlet}},{T_{DB,outdoor}}} \right)} \right)\\ELSE\\\,\,\,\,\,\,HEffFTemp = 1.0\\ENDIF\end{array}$$</div>
-
-where:
-
-<span>\(HEffFTemp\)</span>= Heat reclaim efficiency modifier
-
-<span>\({T_{water,inlet}}\)</span>     = Desuperheater coil inlet water temperature (°C)
-
-<span>\({T_{DB,outdoor}}\)</span>    = Outdoor air dry-bulb temperature (°C)
-
-Except for the detailed condenser source, heat reclaim recovery efficiencies higher than 30% may cause the refrigerant gas to condense which in turn impacts the performance of the refrigeration system. The model is unable to account for this refrigeration system impact, so the product of the rated heat reclaim recovery efficiency and heat reclaim efficiency modifier is not allowed to exceed 0.3.  For the detailed refrigeration condenser, the limit for the heat reclaim efficiency has been set at 0.9 as follows:
-
-<div>$${\rm{IF}}\left( {{\varepsilon_{{\rm{reclaim,rated}}}}} \right)\left( {HEfFTemp} \right) > Limit,{\rm{ then }}HeffFTemp = \frac{{Limit}}{{{\varepsilon_{{\rm{reclaim,rated}}}}}}$$</div>
-
-where:
-
-Limit           = 0.3 for most sources, =0.9 for detailed condensers
-
-<span>\({\varepsilon_{reclaim,rated}}\)</span> = rated heat reclaim recovery efficiency
-
-The heating capacity of the desuperheater coil is then calculated based on the product of total amount of condenser waste heat rejected by the heating source, the desuperheater coil’s rated heat reclaim recovery efficiency, and the heat reclaim efficiency modifier.
-
-<div>$${\dot Q_{coil}} = {{\left( {{{\dot Q}_{cond}}} \right)\left( {{\varepsilon_{reclaim,rated}}} \right)HEffFTemp} \mathord{\left/ {\vphantom {{\left( {{{\dot Q}_{cond}}} \right)\left( {{\varepsilon_{reclaim,rated}}} \right)HEffFTemp} {DXSystemPLR}}} \right. } {DXSystemPLR}}$$</div>
-
-where:
-
-<span>\({\dot Q_{coil}}\)</span>          = water heating capacity of the desuperheater coil (W)
-
-<span>\({\dot Q_{cond}}\)</span>         = average rate of condenser waste heat rejected by the heating source (W)
-
-<span>\(DXSystemPLR\)</span> = part load ratio for the desuperheater coil heating source (1.0 for refrigerated case compressor rack and detailed refrigeration condenser)
-
-The desuperheater is assumed to have a water circulation pump located downstream of the refrigerant-to-water coil. Pump heat is added to the desuperheater water heating capacity based on a user-defined fraction as follows:
-
-<div>$${\dot Q_{coil}} = {\dot Q_{coil}} + {P_{pump}}\left( {Fra{c_{pumptowater}}} \right)$$</div>
-
-where:
-
-<span>\({P_{pump}}\)</span>                     = water pump power (W)
-
-<span>\(Fra{c_{pumptowater}}\)</span>        = fraction of pump heat to water
-
-The temperature of the water leaving the desuperheater is then calculated as
-
-<span>\({T_{water,outlet}} = {T_{water,inlet}} + \frac{{{Q_{coil}}}}{{{{\dot m}_{water}}\cdot {C_{p,water}}}}\)</span> for <span>\({\dot m_{water}}\)</span> &gt; 0
-
-<span>\({T_{water,outlet}} = {T_{water,inlet}}\)</span> for <span>\({\dot m_{water}}\)</span> = 0
-
-Simulation of the desuperheater heating coil is based on its current mode of operation. This mode of operation is either floating (heating coil off and tank water temperature has not fallen below the heater cut-in temperature) or heating (tank water temperature dropped below the heater cut-in temperature on a previous time step but was unable to reach the heater setpoint temperature). Each mode is handled differently and they will be discussed separately.
-
-#### Float Mode
-
-When the water heater tank temperature is floating between the desuperheater coil’s cut-in and cut-out temperatures at the end of the previous simulation time step, both the desuperheater coil and the water heater tank’s heating element are disabled and a resulting tank temperature is calculated. If the resulting tank temperature is below the desuperheater coil cut-in temperature the desuperheater coil part-load ratio is estimated using a ratio of temperature differences as shown below. The part-load ratio can not be less than zero or greater than the part-load ratio of the DX system from which the desuperheater coil is reclaiming heat.
-
-<div>$$PLR = \,MIN\left( {DXSystemPLR,MAX\left( {0.0,\,\,\left( {\frac{{{T_{cut - in}} - {T_{tank,float}}}}{{{T_{tank,initial}} - {T_{tank,float}}}}} \right)} \right)} \right)$$</div>
-
-where:
-
-<span>\(PLR\)</span>         = part load ratio of desuperheater heating coil
-
-<span>\({T_{tank,float}}\)</span>     = tank temperature in float mode when heating capacity is set to zero (°C)
-
-<span>\({T_{tank,initial}}\)</span>    = tank water temperature at the beginning of a simulation time step (°C)
-
-Since the water pump is assumed to cycle on and off with the desuperheater coil, the average water mass flow rate through the desuperheater coil is then set proportional to the PLR calculated above:
-
-<div>$$\dot mwater,avg = \dot mwater\left( {PLR} \right)$$</div>
-
-where:
-
-<span>\(\dot mwater,avg\)</span>       = average desuperheater water mass flow rate for the time step (kg/s)
-
-The water tank temperature is then calculated based on desuperheater heating coil operation (outlet water temperature and average water mass flow rate as calculated above) and with the water tank’s heater element enabled. If the resulting water tank temperature is above the desuperheater coil’s setpoint temperature, then the part-load ratio is reduced in the same manner described in the heating mode section below.
-
-#### Heating Mode
-
-When the desuperheater heating coil is in heating mode at the end of the previous simulation time step (i.e., desuperheater coil operated during the previous simulation time step but was unable to achieve the setpoint temperature), both the desuperheater and the water heater tank’s heating element are enabled. The desuperheater coil outlet water temperature is calculated (as described above) and the water mass flow rate through the desuperheater coil is set to the maximum operating flow rate:
-
-**<span>\(\dot mwater,avg = \dot mwater\left( {DXSystemPLR} \right)\)</span>**
-
-If the resulting tank water temperature is above the desuperheater coil’s setpoint (cut-out) temperature, the part load ratio of the desuperheater coil is reduced and the water heater tank is simulated again. The process is performed iteratively until the part load ratio of the desuperheater coil achieves the desired setpoint temperature.
-
-
-
-#### Model Outputs
-
-After completing the float mode or heating mode calculations and the final desuperheater part load ratio has been determined, the output (report) variables are calculated as follows:
-
-<div>$$Desuperheater\,Part\,Load\,Ratio = MIN\left( {\frac{{\dot mwater,avg}}{{\dot mwater}},DXSystemPLR} \right)\,\,$$</div>
-
-<div>$$Desuperheater\,\,Water\,Heating\,Rate\,\,(W) = {\dot Q_{coil}}\left( {PLR} \right)$$</div>
-
-<div>$$Desuperheater\,\,Water\,Heating\,Energy\,\,(J) = {\dot Q_{coil}}\left( {PLR} \right)(3600)\left( {{t_{sys}}} \right)$$</div>
-
-<div>$$Desuperheater\,\,Pump\,\,Electric\,\,Power\,\,(W) = {P_{pump}}\left( {PLR} \right)$$</div>
-
-<div>$$Desuperheater\,\,Pump\,\,Electric\,\,Consumption\,\,(J) = {P_{pump}}\left( {PLR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)$$</div>
-
-<div>$$Desuperheater Heat Reclaim Efficiency Modifier Curve Output\,\, = \,\,HEffFTemp$$</div>
-
-<div>$$Desuperheater\,\,On{\rm{ - }}Cycle\,Parasitic\,Electric\,Power\,(W)\,\, = \,\,{P_{parasiticload,on}}\left( {PLR} \right)$$</div>
-
-<div>$$Desuperheater\,\,On{\rm{ - }}Cycle\,Parasitic\,Electric\,Consumption\,(J)\,\, = \,\,{P_{parasiticload,on}}\left( {PLR} \right)\left( {3600} \right){t_{sys}}$$</div>
-
-<div>$$Desuperheater\,\,Off{\rm{ - }}Cycle\,Parasitic\,Electric\,Power\,(W)\,\, = \,\,{P_{parasiticload,off}}\left( {1 - PLR} \right)$$</div>
-
-<div>$$Desuperheater\,\,Off{\rm{ - }}Cycle\,Parasitic\,Electric\,Consumption\,(J)\,\, = \,\,{P_{parasiticload,off}}\left( {1 - PLR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)$$</div>
-
-where:
-
-<span>\({P_{parasiticload,on}}\)</span>           = on-cycle parasitic electric load (W)
-
-<span>\({P_{parasiticload,off}}\)</span>          = off-cycle parasitic electric load (W)
-
-<span>\({t_{sys}}\)</span>                         = HVAC system simulation time step (hours)
-
-
-
-Note: All output variables, including off cycle parasitic electrical power and energy, equal 0 when the desuperheater heating coil availability schedule equals 0.
-
-### Heat Exchanger Assisted Air Cooling Coil Systems
-
-An air-to-air heat exchanger can be used to enhance the dehumidification performance of a conventional cooling coil. EnergyPlus has two compound objects to model this scenario: CoilSystem:Cooling:DX:HeatExchangerAssisted and CoilSystem:Cooling:Water:HeatExchangerAssisted. The input syntax for these compound objects can be found in the EnergyPlus Input/Output Reference.
-
-As shown in Figure 173, the air-to-air heat exchanger pre-conditions the air entering the cooling coil, and reuses this energy to post-condition the supply air leaving the cooling coil. This heat exchange process improves the latent removal performance of the cooling coil by allowing it to dedicate more of its cooling capacity toward dehumidification (lower sensible heat ratio).
-
-
-
-![GenericHXAssisted](media/image4091.png)
-
-Figure 173. Schematic of a Heat Exchanger Assisted Cooling Coil
-
-NOTE: Node naming shown in Figure 173 is representative for HeatExchanger:AirToAir:SensibleAndLatent. For HeatExchanger:AirToAir:FlatPlate, the exhaust air nodes are referred to as ‘secondary air’ nodes. For HeatExchanger:Desiccant:BalancedFlow (heat exchanger assisted DX coil only), the supply air nodes are referred to as ‘regeneration air’ nodes and the exhaust air nodes as ‘process air’ nodes.
-
-The dehumidification performance of cooling coils can be enhanced using a sensible-only heat exchanger (e.g., heat pipes, runaround coils, cross-flow heat exchangers). For example, a CoilSystem:Cooling:DX:HeatExchangerAssisted object could be used with a HeatExchanger:AirToAir:FlatPlate object or HeatExchanger:AirToAir:SensibleAndLatent object with only sensible effectiveness specified (see resulting psychrometric process in Figure 174). The dehumidification performance of cooling coils can also be enhanced using heat exchangers that transfer both sensible and latent energy (e.g., rotary desiccant heat exchanger). For example, a CoilSystem:Cooling:DX:HeatExchangerAssisted object could be used with a HeatExchanger:Desiccant:BalancedFlow object (see resulting psychrometric process in Figure 175).
-
-Note that while the HeatExchanger:AirToAir:SensibleAndLatent and HeatExchanger:Desiccant:BalancedFlow objects can transfer both sensible and latent heat between two air streams, the HeatExchanger:Desiccant:BalancedFlow object with appropriate Performance Data Type object is the proper heat exchanger model to use for the heat exchanger assisted cooling coil described here. The HeatExchanger:AirToAir:SensibleAndLatent object should only be used to model the sensible-only heat exchange case (Figure 174).
-
-
-
-![PsychChart\_SensibleHXAssisted](media/image4092.png)
-
-Figure 174. Psychrometric Process for Heat Exchanger Assisted Cooling Coil (Sensible HX Only)
-
-
-
-![PsychChart\_SensPlusLatHXAssisted](media/image4093.png)
-
-Figure 175. Psychrometric Process for Heat Exchanger Assisted Cooling Coil (Sensible+Latent HX)
-
-Modeling of the heat exchanger assisted cooling coil is performed by consecutively modeling the air-to-air heat exchanger and the cooling coil until convergence on a solution is achieved. The detailed modeling calculations for the individual components (air-to-air heat exchangers and cooling coils) are described elsewhere in this document.
-
-Modeling of the heat exchanger assisted cooling coil begins by initializing the air mass flow rate (based on the air mass flow rate placed on the compound object’s inlet air node) and passing this value to the exhaust air inlet node of the air-to-air heat exchanger. The heat exchanger and cooling coil are then successively modeled using the calculation routines specific to the type of heat exchanger and cooling coil selected. The air temperature exiting the cooling coil is compared with the air temperature exiting the cooling coil on the previous modeling iteration for this simulation time step. Convergence is reached when the change in this air temperature for successive iterations is within a specified tolerance (0.0005°C). Consecutive modeling of the heat exchanger and cooling coil is terminated and a warning message is issued if the number of modeling iterations exceeds 50.
-
-For the CoilSystem:Cooling:DX:HeatExchangerAssisted object, heat exchanger operation can be controlled based on high humidity levels in a zone. By default, the heat exchanger is assumed to always provide its heat transfer when the associated DX cooling coil is operating and no humidity control mechanism is specified. However, the heat exchanger’s energy transfer may be controlled (i.e., turned on and off) based on a zone air humidity level using either a humidistat alone (Figure 176) or a humidistat and a maximum humidity setpoint manager (Figure 177) depending on the HVAC system that is utilizing the heat exchanger assisted cooling coil.
-
-The heat exchanger assisted DX cooling coil may be used with furnaces or unitary systems located in an air loop (ref. AirLoopHVAC:Unitary:Furnace:HeatCool or AirLoopHVAC:UnitaryHeatCool). These system objects have three options for dehumidification control (None, Multimode, and CoolReheat). When no dehumidification control is specified in the furnace or unitary system object (None), the heat exchanger is always active when the cooling coil is operating. When multimode or coolreheat dehumidification control is specified, a humidistat is required as shown in Figure 176. For the case of multimode dehumidification control, the heat exchanger is only active when the zone air humidity level is above the humidistat setpoint (i.e., the system’s cooling coil can’t meet the latent cooling load when operating without heat exchanger energy transfer) while the AC system operates to meet the sensible (dry-bulb cooling thermostat) load. For the case of coolreheat dehumidification control, the heat exchanger is always active when the cooling coil operates and this system tries to meet both the sensible (thermostat) and latent (humidistat) loads.
-
-![GenericHXAssisted\_humidistat](media/image4094.png)
-
-Figure 176. Schematic of a heat exchanger assisted DX cooling coil with optional humidistat
-
-The heat exchanger assisted DX cooling coil may also be used with a DX system located in an air loop (ref. CoilSystem:Cooling:DX). This system object also has three options for dehumidification control (None, Multimode, and CoolReheat). When no dehumidification control is specified (None), the heat exchanger is always active when the cooling coil is operating. When multimode or coolreheat dehumidification control is specified, a humidistat and a maximum humidity setpoint manager are required as shown in Figure 177 (setpoint needs to be placed on the DX system’s control node). For multimode dehumidification control, the heat exchanger is only active when the zone humidity levels are above the humidistat setpoint (i.e., the system’s cooling coil can’t meet the maximum humidity ratio setpoint when operating without heat exchanger energy transfer) while the AC system operates to meet the sensible (dry-bulb cooling thermostat) load. For coolreheat dehumidification control, the heat exchanger is always active when the cooling coil operates and this system tries to meet both the sensible (thermostat) and latent (humidistat) loads.
-
-When the heat exchanger assisted cooling coil is used with a furnace or unitary system (ref. AirLoopHVAC:Unitary:Furnace:HeatCool or AirLoopHVAC:UnitaryHeatCool) or DX system (ref. CoilSystem:Cooling:DX) located in an air loop (or DX system used in an outside air system), an ecomizier function may be customized as necessary. For economizer control, an outdoor air controller (ref. Controller:OutdoorAir) is used to define the economizer control inputs and determine when economizer mode is active. The heat exchanger (ref. HeatExchanger:\*) object provides an economizer lockout feature which disables heat recovery any time the economizer is active. This feature can be turned on and off using the heat exchanger lockout input. Heat exchanger assisted cooling coils used with the zone equipment described below disregard this economizer control feature.
-
-![GenericHXAssisted\_humidistat\_Plus\_Setpointmanager](media/image4095.png)
-
-Figure 177. Schematic of Heat Exchanger Assisted DX Coil with Humidistat and Setpoint Manager
-
-The heat exchanger assisted DX cooling coil may also be used with the unitary changeover bypass system and the unitary air-to-air heat pump system (ref. AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass and AirLoopHVAC:UnitaryHeatPump:AirToAir); however, the heat exchanger is assumed to always provide its heat transfer when the cooling coil operates and can not be turned on and off based on a zone air humidity setpoint (ref. Figure 173). Two zone air conditioners may also use this heat exchanger/coil assembly model for improved dehumidification. The first type is the packaged terminal heat pump (ref. ZoneHVAC:PackagedTerminalHeatPump) where the heat exchanger’s heat transfer is always active whenever the cooling coil operates (ref. Figure 173). The second type is the window air conditioner (ref. ZoneHVAC:WindowAirConditioner) where the heat exchanger’s heat transfer is always active when the cooling coil operates and no humidity control mechanism is specified (ref. Figure 173), or the heat exchanger’s heat transfer may be controlled based on zone air humidity level when a humidistat and high humidity setpoint manager are specified (maximum humidity ratio setpoint must be placed on the heat exchanger’s exhaust air outlet node). For this case, the heat exchanger is only active when the zone air humidity level is above the humidistat setpoint (i.e., the system’s cooling coil can’t meet the maximum humidity ratio setpoint when operating without heat exchanger energy transfer) while only the sensible (dry-bulb cooling thermostat) load is met by the AC system (ref. Figure 177).
-
-For the CoilSystem:Cooling:Water:HeatExchangerAssisted object, there is currently no method to enable or disable heat exchange based on zone air humidity level. Heat exchange will occur whenever the heat exchanger is available to operate (via its availability schedule) and a temperature difference exists between the two air streams.
-
-#### References
-
-Kosar, D. 2006. Dehumidification Enhancements, ASHRAE Journal, Vol. 48, No. 2, February 2006.
-
-Kosar, D. et al. 2006. Dehumidification Enhancement of Direct Expansion Systems Through Component Augmentation of the Cooling Coil. 15<sup>th</sup> Symposium on Improving Building Systems in Hot and Humid Climates, July 24-26, 2006.
-
-Nimmo, B.G. et al. 1993.DEAC: Desiccant Enhancement of Cooling-Based Dehumidification. ASHRAE Transactions, Vol.99, Part 1, Paper number CH-93-4-4, pp. 842-848.
-
-### Single-Speed Electric Heat Pump DX Water Heating Coil
-
-#### Overview
-
-The input object `Coil:WaterHeating:AirToWaterHeatPump:\*` provides a model used in a heat pump water heater (HPWH) consisting of a water heater tank (e.g., `WaterHeater:Mixed` or `WaterHeater:Stratified`), a direct expansion (DX) “coil� (i.e., an air-to-water DX compression system which includes a water heating coil, air coil, compressor, and water pump), and a fan to provide air flow across the air coil associated with the DX compression system. These objects work together to model a system which heats water using zone air, outdoor air, or a combination of zone and outdoor air as the primary heat source. The heat pump water heater (Ref. `WaterHeater:HeatPump:*`), water heater tank (Ref. `WaterHeater:Mixed` and `WaterHeater:Stratified`), and fan (Ref. `Fan:\*`) objects are described elsewhere in this document.
-
-
-
-![HPWHSchematic\_EAplusOA](media/image4096.png)
-
-Figure 178. Schematic of a Heat Pump Water Heater using Optional Mixer/Splitter Nodes
-
-The heat pump water heater DX coil model described here determines the thermal performance and energy consumption of the DX compression system, which includes a water heating coil (condenser), a coil used to extract heat from air (evaporator), and the compressor. This model also simulates the performance of a condenser water pump that is assumed to cycle on and off with the compressor.
-
-![HeatPumpWaterHeater\_Schematic2](media/image4097.png)
-
-Figure 179. Schematic of the Heat Pump Water Heater DX Coil
-
-Virtually all of the inputs to this DX coil model relate to its water heating performance and energy consumption. Model inputs differ between the `Coil:WaterHeating:AirToWaterHeatPump:Pumped` and `Coil:WaterHeating:AirToWaterHeatPump:Wrapped` to include only the relevant inputs for `WaterHeater:HeatPump:PumpedCondenser` and `WaterHeater:HeatPump:WrappedCondenser`, respectively. The air-side cooling capacity of this DX system is derived from user inputs and some model assumptions. The sensible/latent cooling capacity split is defined by the user at rated conditions, and the model adjusts this split at off-rated conditions.
-
-#### Model Description
-
-The user must input the heating capacity, coefficient of performance (COP), and the sensible heat ratio (SHR) of the evaporator coil at rated inlet fluid temperatures and flow rates that are also specified by the user. The evaporator SHR should be a “gross� value, excluding any thermal impacts due to the indoor supply air fan. The user may also input up to seven performance curves that describe the change in total water heating capacity and efficiency at off-rated and part-load conditions.
-
-1)    Heating capacity modifier curve (function of temperature)
-
-2)    Heating capacity modifier curve (function of air flow fraction)
-
-3)    Heating capacity modifier curve (function of water flow fraction, pumped condenser only)
-
-4)    Heating COP modifier curve (function of temperature)
-
-5)    Heating COP modifier curve (function of air flow fraction)
-
-6)    Heating COP modifier curve  (function of water flow fraction, pumped condenser only)
-
-7)    Part load fraction correlation (function of part load ratio)
-
-Note: The air dry-bulb or wet-bulb temperature used in the following curve objects is the inlet air temperature to the HPWH evaporator coil/fan assembly. If the fan placement specified in the `WaterHeater:HeatPump:*` compound object is draw-through, then the inlet air temperature represents the temperature of the air entering the evaporator coil itself. If blow-through fan placement is specified, then the inlet air temperature represents air conditions entering the fan located immediately in front (upstream) of the evaporator coil.
-
-The heating capacity as a function of temperature modifier curve defines the variation in DX coil heating capacity as a function of inlet fluid (air and water) temperatures. The curve object may use either a bi-quadratic or cubic form. The bi-quadratic curve uses inlet air temperature (dry-bulb or wet-bulb temperature based on the input field Evaporator Air Temperature Type for Curve Objects) and condenser inlet water temperature as the independent variables. The cubic curve uses inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The curve should be normalized to have the value of 1.0 at the rating point temperatures specified by the user.
-
-<div>$$HCapFTemp = a + b\left( {{T_{evap,in}}} \right) + c{\left( {{T_{evap,in}}} \right)^2} + d\left( {{T_{cond,in}}} \right) + e{\left( {{T_{cond,in}}} \right)^2} + f\left( {{T_{evap,in}}} \right)\left( {{T_{cond,in}}} \right)$$</div>
-
-or
-
-<div>$$HCapFTemp = a + b\left( {{T_{evap,in}}} \right) + c{\left( {{T_{evap,in}}} \right)^2} + d{\left( {{T_{evap,in}}} \right)^3}$$</div>
-
-where:
-
-<span>\({T_{evap,in}}\)</span>  = dry-bulb or wet-bulb temperature of the air entering the evaporator coil/fan assembly based on the Evaporator Air Temperature Type for Curve Objects specified by the user (°C)
-
-<span>\({T_{cond,in}}\)</span>  = temperature of the water entering the DX coil condenser (°C)
-
-The heating capacity as a function of air flow fraction modifier curve is a quadratic or cubic curve that defines the variation in DX coil heating capacity as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate (i.e., fraction of full load air flow rate). When used, the output of this curve should be normalized to have the value of 1.0  at an air flow fraction of 1.
-
-<div>$$HCapFAirFlow = \,a + \,b\left( {f{f_{air}}} \right)\,\, + \,\,c{\left( {f{f_{air}}} \right)^2}$$</div>
-
-or
-
-<div>$$HCapFAirFlow = \,a + \,b\left( {f{f_{air}}} \right)\,\, + \,\,c{\left( {f{f_{air}}} \right)^2}\,\, + \,\,d{\left( {f{f_{air}}} \right)^3}$$</div>
-
-where:
-
-<div>$$f{f_{air}} = air\,flow\,fraction = \left( {\frac{{Actual\,air\,mass\,flow\,rate}}{{Rated\,air\,mass\,flow\,rate}}} \right)$$</div>
-
-Note: The actual volumetric air flow rate through the evaporator coil/fan assembly for any simulation time step where the compressor is operating must be between 0.00002684 m<sup>3</sup>/s and .00008056 m<sup>3</sup>/s per watt of rated total heating capacity. The simulation will issue a warning message if this air flow range is exceeded, but the simulation will continue.
-
-The heating capacity as a function of water flow fraction modifier curve is a quadratic or cubic curve that defines the variation in DX coil heating capacity as a function of the ratio of actual water flow rate through the condenser to the rated condenser water flow rate (i.e., fraction of full load water flow rate). *It is only used for the pumped condenser configuration.* When used, the output of this curve should be normalized to have the value of 1.0 at a water flow fraction of 1.
-
-<div>$$HCapFWaterFlow = \,a + \,b\left( {f{f_{water}}} \right)\,\, + \,\,c{\left( {f{f_{water}}} \right)^2}$$</div>
-
-or
-
-<div>$$HCapFWaterFlow = \,a + \,b\left( {f{f_{water}}} \right)\,\, + \,\,c{\left( {f{f_{water}}} \right)^2}\,\, + \,\,d{\left( {f{f_{water}}} \right)^3}$$</div>
-
-where:
-
-<div>$$f{f_{water}} = water\,flow\,fraction = \left( {\frac{{Actual\,water\,mass\,flow\,rate}}{{Rated\,water\,mass\,flow\,rate}}} \right)$$</div>
-
-The heating COP as a function of temperature modifier curve defines the variation in DX coil heating COP as a function of inlet fluid (air and water) temperatures. The curve object may use either a bi-quadratic or cubic form. The bi-quadratic curve uses inlet air temperature (dry-bulb or wet-bulb temperature based on the input field Evaporator Air Temperature Type for Curve Objects) and condenser inlet water temperature as the independent variables. The cubic curve uses inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The curve should be normalized to have the value of 1.0 at the rating point temperatures specified by the user.
-
-<div>$$HCOPFTemp = a + b\left( {{T_{evap,in}}} \right) + c{\left( {{T_{evap,in}}} \right)^2} + d\left( {{T_{cond,in}}} \right) + e{\left( {{T_{cond,in}}} \right)^2} + f\left( {{T_{evap,in}}} \right)\left( {{T_{cond,in}}} \right)$$</div>
-
-or
-
-<div>$$HCOPFTemp = a + b\left( {{T_{evap,in}}} \right) + c{\left( {{T_{evap,in}}} \right)^2} + d{\left( {{T_{evap,in}}} \right)^3}$$</div>
-
-The heating COP as a function of air flow fraction modifier curve is a quadratic or cubic curve that defines the variation in DX coil heating COP as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate (i.e., fraction of full load air flow rate). When used, the output of this curve should be normalized to have the value of 1.0 at an air flow fraction of 1.
-
-<div>$$HCOPFAirFlow = \,a + \,b\left( {f{f_{air}}} \right)\,\, + \,\,c{\left( {f{f_{air}}} \right)^2}$$</div>
-
-or
-
-<div>$$HCOPFAirFlow = \,a + \,b\left( {f{f_{air}}} \right)\,\, + \,\,c{\left( {f{f_{air}}} \right)^2}\,\, + \,\,d{\left( {f{f_{air}}} \right)^3}$$</div>
-
-The heating COP as a function of water flow fraction modifier curve is a quadratic or cubic curve that defines the variation in DX coil heating COP as a function of the ratio of actual water flow rate through the condenser to the rated condenser water flow rate (i.e., fraction of full load water flow rate). *It is only used for the pumped condenser configuration.* When used, the output of this curve should be normalized to have the value of 1.0 at a water flow fraction of 1.
-
-<div>$$HCOPFWaterFlow = \,a + \,b\left( {f{f_{water}}} \right)\,\, + \,\,c{\left( {f{f_{water}}} \right)^2}$$</div>
-
-or
-
-<div>$$HCOPFWaterFlow = \,a + \,b\left( {f{f_{water}}} \right)\,\, + \,\,c{\left( {f{f_{water}}} \right)^2}\,\, + \,\,d{\left( {f{f_{water}}} \right)^3}$$</div>
-
-The part load fraction as a function of part load ratio correlation curve parameterizes the variation of electrical power input to the heat pump DX coil as a function of the part load ratio (PLR, heating delivered/steady-state heating capacity). The part load ratio divided by the part load fraction yields the runtime fraction of the DX heating coil for a given simulation time step. The part load fraction correlation accounts for efficiency losses due to compressor cycling.
-
-<div>$$PartLoadFrac = PLF = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2}$$</div>
-
-or
-
-<div>$$PartLoadFrac = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2} + d{\left( {PLR} \right)^3}$$</div>
-
-where:
-
-<div>$$PLR = part\,load\,ratio = \left( {\frac{{water\,heating\,delivered}}{{steady{\rm{ - }}state\,water\,heating\,capacity}}} \right)$$</div>
-
-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor runs continuously for the simulation time step). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7   and   PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
-
-When the part load fraction correlation for a heat pump water heater DX coil is unknown, the typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential or small commercial unit) may be used:
-
-            PLF = 0.85 + 0.15(PLR)
-
-All seven curves are accessed through EnergyPlus’ built-in performance curve equation manager (curve:quadratic, curve:cubic and curve:biquadratic). It is not imperative that the user utilize all coefficients shown in the equations above if their performance equation has fewer terms (e.g., if the user’s part load fraction correlation curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero).
-
-Note: If any of the above performance curves are not specified by the user, the output of that curve is assumed to be 1 for the entire simulation.
-
-For any simulation time step, the heating capacity of the heat pump water heater DX coil is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{heating}} = {\mathop Q\limits^ \bullet_{heating,rated}}\left( {HCapFTemp} \right)\left( {HCapFAirFlow} \right)\left( {HCapFWaterFlow} \right)$$</div>
-
-In a similar fashion, the coefficient of performance for the DX coil for any simulation time step is calculated using the following equation:
-
-<div>$$CO{P_{heating}} = CO{P_{heating,rated}}\left( {HCOPFTemp} \right)\left( {HCOPFAirFlow} \right)\left( {HCOPFWaterFlow} \right)$$</div>
-
-The electric power for the heat pump water heater DX coil is then calculated using the water heating capacity and coefficient of performance calculated above.
-
-
-
-<div>$${P_{heating}} = \left( {\frac{{{{\mathop Q\limits^ \bullet  }_{heating}}}}{{CO{P_{heating}}}}} \right)$$</div>
-
-where:
-
-
-
-<span>\({\mathop Q\limits^ \bullet_{heating}}\)</span>       = water heating capacity at the current operating conditions (W)
-
-<span>\({\mathop Q\limits^ \bullet_{heating,rated}}\)</span> = water heating capacity at rated conditions, user input (W)
-
-<span>\(CO{P_{heating}}\)</span>  = coefficient of performance at the current operating conditions (W/W)
-
-<span>\(CO{P_{heating,rated}}\)</span>= coefficient of performance at rated conditions, user input (W/W)
-
-<span>\({P_{heating}}\)</span>        = DX heating coil power (electricity consumption rate) at the current                                   operating conditions (W)
-
-The heating capacity calculated above may or may not include the impact of pump heat. For this reason, the user input Condenser Pump Heat Included in Rated Heating Capacity and Rated COP is used to determine the total water heating capacity including pump heat.
-
-<div>$$\begin{array}{l}IF\left( {Condenser\,Pump\,Heat\,Included\,In\,Rated\,Heating\,Capacity\,and\,Rated\,COP} \right)\\\,\,\,{\mathop Q\limits^ \bullet_{heating,total}} = {\mathop Q\limits^ \bullet_{heating}}\\ELSE\\\,\,\,{\mathop Q\limits^ \bullet_{heating,total}} = {\mathop Q\limits^ \bullet_{heating}} + {P_{pump}}\left( {Fra{c_{pumptowater}}} \right)\\END\,IF\end{array}$$</div>
-
-where:
-
-<span>\({\mathop Q\limits^ \bullet_{heating,total}}\)</span>  = total water heating capacity including condenser pump heat (W)
-
-<span>\({P_{pump}}\)</span>         = condenser water pump power, user input (W)
-
-<span>\(Fra{c_{pumptowater}}\)</span>= fraction of condenser pump heat to water, user input
-
-Compressor power (electricity consumption rate) is then calculated based on two additional inputs provided by the user. The first input specifies if the condenser pump heat is included in the rated heating capacity and rated COP. If the condenser pump heat is included in the rated heating capacity and COP, then condenser pump power must be subtracted from the DX heating coil power calculated above to determine the compressor power.
-
-The second of these inputs specifies if the evaporator fan power is included in the rated heating COP. If evaporator fan power is included in the rated COP, then fan power must also be subtracted from the DX heating coil power to determine the compressor power as follows:
-
-<div>$$\begin{array}{l}IF\left( {Evap\,Fan\,Power\,In\,COP} \right)\,\,THEN\\\,\,\,\,IF\left( {Cond\,Pump\,Power\,In\,COP} \right)\,\,THEN\\\,\,\,\,\,\,\,{P_{comp}} = {P_{heating}} - {P_{pump}} - {P_{fan}}\\\,\,\,\,ELSE\\\,\,\,\,\,\,\,{P_{comp}} = {P_{heating}} - {P_{fan}}\\\,\,\,\,END\;IF\end{array}$$</div>
-
-where:
-
-<span>\({P_{comp}}\)</span> = Compressor power (electric consumption rate) at the current operating conditions (W)
-
-<span>\({P_{fan}}\)</span>  = Fan power, specified in Fan:OnOff object (W)
-
-If fan power is not included in the rated heating COP, then the calculation of compressor power only includes condenser pump power and does not involve the fan:
-
-<div>$$\begin{array}{l}IF\left( {.NOT.\,\,\,\,Evap\,Fan\,Power\,In\,COP} \right)\,\,THEN\\\,\,\,\,IF\left( {Cond\,Pump\,Power\,In\,COP} \right)\,\,THEN\\\,\,\,\,\,\,\,\,{P_{comp}} = {P_{heating}} - {P_{pump}}\\\,\,\,\,ELSE\\\,\,\,\,\,\,\,\,{P_{comp}} = {P_{heating}}\\\,\,\,\,END\;IF\end{array}$$</div>
-
-The model assumes that all compressor power is rejected as heat via the DX heating coil. Therefore, the evaporator total cooling capacity at the current operating conditions is determined depending on the user input for pump heat:
-
-<div>$$\begin{array}{l}IF\left( {Condenser\,Pump\,Heat\,Included\,In\,Rated\,Heating\,Capacity\,and\,Rated\,COP} \right)\\\,\,\,\,\,{\mathop Q\limits^ \bullet_{evap}} = {\mathop Q\limits^ \bullet_{heating}} - {P_{comp}} - \left( {{P_{pump}}Fra{c_{pumptowater}}} \right)\\ELSE\\\,\,\,\,\,{\mathop Q\limits^ \bullet_{evap}} = {\mathop Q\limits^ \bullet_{heating}} - {P_{comp}}\\END\;IF\end{array}$$</div>
-
-where:
-
-<span>\({\mathop Q\limits^ \bullet_{evap}}\)</span> = Total evaporator cooling capacity at the current operating conditions (W)
-
-
-
-This evaporator cooling capacity is used to calculate the air-side performance of the heat pump water heater DX coil. The sensible heat ratio of the cooling capacity at rated conditions is specified by the user in the input for this DX coil object. The calculation of sensible heat ratio at off-rated conditions uses the ADP/BF approach described for the DX cooling coil model (Ref. Coil Model – DX Cooling Coil Model). The exiting air conditions for the HPWH DX coil are calculated the same way as they are for the DX cooling coil model (cycling fan, cycling coil). The crankcase heater power and consumption are also calculated using the same equations used for the DX cooling coil model.
-
-The runtime fraction of the DX coil compressor is calculated as the ratio of the compressor part load ratio to the part load fraction correlation entered by the user. The part load ratio of the DX coil is determined by the heat pump water heater compound object (Ref. `WaterHeater:HeatPump:*`) and is used by the DX coil to determine the run time fraction of the compressor.
-
-<div>$$RTF = \left( {{\raise0.7ex\hbox{${PLR}$} \!\mathord{\left/ {\vphantom {{PLR} {PartLoadFrac}}}\right.}\!\lower0.7ex\hbox{${PartLoadFrac}$}}} \right) = runtime\,fraction\,of\,the\,compressor$$</div>
-
-Finally, the condenser water outlet temperature is calculated based on the total water heating capacity of the DX coil and the actual condenser water mass flow rate.
-
-<div>$${T_{cond,out}} = {T_{cond,in}} + \left( {\frac{{{{\mathop Q\limits^ \bullet  }_{heating,total}}}}{{\mathop m\limits^ \bullet  cond\,\,\,{C_p}}}} \right)$$</div>
-
-where:
-
-<span>\({T_{cond,out}}\)</span> = condenser outlet water temperature when the DX coil is operating (˚C)
-
-<span>\({T_{cond,in}}\)</span> = condenser inlet water temperature (˚C)
-
-<span>\({C_p}\)</span> = specific heat of water entering the condenser coil (J/kg-C)
-
-<span>\(\mathop m\limits^ \bullet  cond\)</span> = actual condenser water mass flow rate when the coil is operating,                                 defined in the WaterHeater:HeatPump:PumpedCondenser parent object (kg/s)
-
-
-
-#### Model Outputs
-
-After completing the calculations for heating capacity and power and the final compressor part load ratio has been determined, the output (report) variables are calculated as follows:
-
-<div>$$DX\,Coil\,Total\,Water\,Heating\,Rate\,(W) = {\mathop Q\limits^ \bullet_{heating,total}}\left( {PLR} \right)$$</div>
-
-<div>$$DX\,Coil\,Total\,Water\,Heating\,Energy\,(J) = {\mathop Q\limits^ \bullet_{heating,total}}\left( {PLR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)$$</div>
-
-<div>$$DX\,Coil\,Water\,Heating\,Electric\,Power\,(W) = \left( {{P_{comp}} + {P_{pump}}} \right)\left( {RTF} \right)$$</div>
-
-<div>$$DX\,Coil\,Water\,Heating\,Electric\,Consumption\,(J) = \left( {{P_{comp}} + {P_{pump}}} \right)\left( {RTF} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)$$</div>
-
-<div>$$DX\,Coil\,Total\,Cooling\,Rate\,(W) = \,{\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)$$</div>
-
-<div>$$DX\,Coil\,Total\,Cooling\,Energy\,\,(J) = \,{\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)$$</div>
-
-<div>$$DX\,Coil\,Sensible\,Cooling\,Rate\,(W) = \,{\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)\left( {SHR} \right)$$</div>
-
-<div>$$DX\,Coil\,Sensible\,Cooling\,Energy\,(J) = \,{\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)\left( {SHR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)$$</div>
-
-<div>$$DX\,Coil\,Latent\,Cooling\,Rate\,(W) = \,{\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)\left( {1.0 - SHR} \right)$$</div>
-
-<div>$$DX\,Coil\,Latent\,Cooling\,Energy\,\,(J) = {\mathop Q\limits^ \bullet_{evap}}\left( {PLR} \right)\left( {1.0 - SHR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)$$</div>
-
-<div>$$DX\,Coil\,Runtime\,Fraction = \left( {{\raise0.7ex\hbox{${PLR}$} \!\mathord{\left/ {\vphantom {{PLR} {PartLoadFrac}}}\right.}\!\lower0.7ex\hbox{${PartLoadFrac}$}}} \right)$$</div>
-
-<div>$$DX\,Coil\,Crankcase\,Heater\,Power\,(W) = \,\left( {{P_{crankcase}}} \right)\left( {1.0 - RTF} \right)$$</div>
-
-<div>$$DX\,Coil\,Crankcase\,Heater\,Consumption\,(J) = \,\left( {{P_{crankcase}}} \right)\left( {1.0 - RTF} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)$$</div>
-
-where:
-
-*t<sub>sys</sub>             =* HVAC system simulation time step, hr
-
-*SHR*           = sensible heat ratio at the current inlet air conditions and air flow rate                            (Ref. Coil Model – DX Cooling Coil Model, ADP/BF approach)
-
-*P<sub>crankcase</sub>     *= Crankcase heater capacity, user input (W)
-
-### Water Source Electric DX Air Cooling Coil
-
-There are two objects for water-to-air heat pumps in cooling mode: Coil:Cooling:WaterToAirHeatPump:EquationFit and Coil:Cooling:WaterToAirHeatPump:ParameterEstimation.  These are described elsewhere.
-
-### Water Source Electric Heat Pump DX Air Heating Coil
-
-There are two objects for water-to-air heat pumps in heating mode:  Coil:Heating:WaterToAirHeatPump:EquationFit and Coil:Heating:WaterToAirHeatPump:ParameterEstimation.  These are described elsewhere.
-
-### Steam-Based Air Heating Coil
-
-The steam coils are included in the discussion on steam loops, see: Steam To Air Heat Exchanger.
-
-### Variable Refrigerant Flow Cooling Coil
-
-#### Overview
-
-The variable refrigerant flow (VRF) DX cooling coil model is identical to the single-speed DX cooling coil model (Ref. Coil:Cooling:DX:SingleSpeed) when the compressor operates at it’s maximum speed. The calculations used when the VRF heat pump operates at part-load are slightly different than the single-speed DX cooling coil model. For this reason, an adaptation of the single-speed DX cooling coil model is used to model the variable-speed compression system used in the VRF model. The difference in model calculations occur when the VRF DX cooling coil’s electronic expansion device reduces refrigerant flow through the cooling coil. When the refrigerant flow is reduced, the coil’s apparatus dew point (ADP) temperature changes, as well as the coil’s sensible heat ratio (SHR). Since the single-speed DX cooling coil model is able to determine the ADP and SHR of a cooling coil at various operating conditions, this same model concept will be used to determine the ADP and SHR of the variable refrigerant flow DX cooling coil.
-
-#### Model Description
-
-The user must input the total cooling capacity and the volumetric air flow rate across the cooling coil at rated conditions. The capacity input should be “gross� values, excluding any thermal or energy impacts due to the indoor supply air fan. The rated volumetric air flow should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of rated total cooling capacity (300 – 450 cfm/ton).
-
-The user is required to input a performance curve in the heat pump object (ref: AirConditioner: VariableRefrigerantFlow) that describes the change in total cooling capacity at various operating conditions (i.e. at cooling coil inlet air wet-bulb and condenser entering air dry-bulb temperatures different than those used to define total capacity). Each DX cooling coil uses two Cooling Capacity Ratio Modifier curves to define the DX cooling coil performance. The first curve defines the full load performance solely as a function of indoor wet-bulb temperature or uses both indoor wet-bulb temperature and outdoor dry-bulb temperature as the independent variables. The specific performance curves are:
-
-Total cooling capacity modifier curve (function of temperature)
-
-Total cooling capacity modifier curve (function of flow fractionl)
-
-·        The total cooling capacity modifier curve (function of temperature) defines the performance of the DX cooling coil as a function of operating conditions. These operating conditions may be specified as either a linear, quadratic or cubic equation using coil entering air wet-bulb temperature as the independent variable or as a biquadratic equation using both coil entering air wet-bulb temperature and outdoor dry-bulb temperuate as the independent variables. Since the variable refrigerant flow system modulates the compressor speed to serve the individual cooling coils, the single indpendent variable equation is likely to be sufficient to define the DX cooling coil performance. However, if other more accurate information is available, a biquadratic curve using two independent variables may be used. The output of this curve is multiplied by the rated total cooling capacity to give the total cooling capacity at the specific entering air temperatures at which the DX coil unit is operating (i.e., at temperatures different from the rating point temperatures).
-
-<div>$$TotCapTempModFac = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d{\left( {{T_{wb,i}}} \right)^3}$$</div>
-
-- or -
-
-<div>$$TotCapTempModFac = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d\left( {{T_{c,i}}} \right) + e{\left( {{T_{c,i}}} \right)^2} + f\left( {{T_{wb,i}}} \right)\left( {{T_{c,i}}} \right)$$</div>
-
-where
-
-<span>\({{T_{wb,i}}}\)</span> = wet-bulb temperature of the air entering the cooling coil, °C
-
-<span>\({{T_{c,i}}}\)</span> = dry-bulb temperature of the air entering an air-cooled condenser
-
-or wet-bulb temperature of the air entering an evaporative-cooled condenser, °C
-
-The total cooling capacity modifier curve (function of flow fraction) is a linear, quadratic, or cubic curve with the independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the operating (modulated) total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the total cooling capacity at the specific temperature and air flow conditions at which the DX unit is operating. The cubic form of the equation is:
-
-<div>$$TotCapFlowModFac = \,a + \,b\left( {ff} \right)\,\, + \,\,c{\left( {ff} \right)^2}\,\, + \,\,d{\left( {ff} \right)^3}$$</div>
-
-where
-
-<div>$$ff = flow{\rm{ }}fraction = \left( {\frac{{Actual{\rm{ }}air{\rm{ }}mass{\rm{ }}flow{\rm{ }}rate}}{{Rated{\rm{ }}air{\rm{ }}mass{\rm{ }}flow{\rm{ }}rate}}} \right)$$</div>
-
-**Note:**  The actual volumetric air flow rate through the cooling coil for any simulation time step where the DX unit is operating must be between 0.00002684 m<sup>3</sup>/s and .00006713 m<sup>3</sup>/s per watt of rated total cooling capacity (200 - 500 cfm/ton). The simulation will issue a warning message if this air flow range is exceeded.
-
-For any simulation time step, the total (gross) cooling capacity of the DX unit is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{total}} = {\mathop Q\limits^ \bullet_{reference}}\left( {TotCapTempModFac} \right)\left( {TotCapFlowModFac} \right)$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{total}}\)</span>= Total available cooling capacity, W
-
-<span>\({\mathop Q\limits^ \bullet_{reference}}\)</span>= Total reference (rated) cooling capacity, W
-
-In addition to calculating the total cooling capacity provided by the DX cooling coil, it is important to properly determine the break down of total cooling capacity into its sensible (temperature) and latent (dehumidification) components. The model computes the sensible/ latent split using the SHR and ADP/BF approach (Carrier et al. 1959). When the DX coil model is initially called during an EnergyPlus simulation, the rated total capacity and rated SHR are used to calculate the coil bypass factor (BF) at rated conditions. The rated total capacity and rated SHR are first used to determine the ratio of change in air humidity ratio to air dry-bulb temperature:
-
-<div>$$SlopeRated = {\left( {\frac{{{\omega_{in}} - {\omega_{out}}}}{{{T_{db,in}} - {T_{db,out}}}}} \right)_{rated}}$$</div>
-
-where
-
-*ω<sub>in</sub>* = humidity ratio of the air entering the cooling coil at rated conditions, kg/kg
-
-*ω<sub>out</sub>* = humidity ratio of the air leaving the cooling coil at rated conditions, kg/kg
-
-*T<sub>db,in</sub>* = dry-bulb temperature of the air entering the cooling coil at rated conditions, °C
-
-*T<sub>db,out</sub>* = dry-bulb temperature of the air leaving the cooling coil at rated conditions, °C
-
-Along with the rated entering air conditions, the algorithm then searches along the saturation curve of the psychrometric chart until the slope of the line between the point on the saturation curve and the inlet air conditions matches *SlopeRated*. Once this point, the apparatus dew point, is found on the saturation curve the coil bypass factor at rated conditions is calculated as follows:
-
-<div>$$B{F_{rated}} = \frac{{{h_{out,rated}} - {h_{ADP}}}}{{{h_{in,rated}} - {h_{ADP}}}}$$</div>
-
-where
-
-*h<sub>out,rated</sub>* <sub> </sub>= enthalpy of the air leaving the cooling coil at rated conditions, J/kg
-
-*h<sub>in,rated</sub>* <sub> </sub>= enthalpy of the air entering the cooling coil at rated conditions, J/kg
-
-*h<sub>ADP</sub>* <sub> </sub>= enthalpy of saturated air at the coil apparatus dew point, J/kg
-
-The coil bypass factor is analogous to the “ineffectiveness� (1-ε) of a heat exchanger, and can be described in terms of the number of transfer of unit (NTU).
-
-<div>$$BF = {e^{ - NTU}} = {e^{{{ - \left( {\frac{{UA}}{{{c_p}}}} \right)} \mathord{\left/ {\vphantom {{ - \left( {\frac{{UA}}{{{c_p}}}} \right)} {\dot m}}} \right. } {\dot m}}}} = {e^{ - Ao/\dot m}}$$</div>
-
-For a given coil geometry, the bypass factor is only a function of air mass flow rate. The model calculates the parameter A<sub>o</sub> in the equation above based on BF<sub>rated</sub> and the rated air mass flow rate. With A<sub>o</sub> known, the coil BF can be determined for non-rated air flow rates.
-
-For each simulation time step when the DX cooling coil operates, the total cooling capacity and coil bypass factor at the actual operating conditions are calculated. The coil bypass factor is used to calculate the operating sensible heat ratio (SHR) of the cooling coil using the following equations. Here is where the differnce in models occur for the VRF DX cooling coil and single-speed DX cooling coil. The original coil model (ref: Coil:Cooling:DX:SingleSpeed) calculates the full load outlet air enthalpy and, considering the bypass factor, finds the coil surface temperture (h<sub>ADP</sub>) at full load (i.e., PLR = 1). Conversely, the VRF coil model modulates refrigerant flow to the VRF DX cooling coil which is why this model uses the full load coil capacity multipled by the part-load ratio (the modulated refrigerant flow). The effectively finds the coil surface temperature for a variable refrigerant flow DX cooling coil and the operating sensible heat ratio (SHR) can be calculated.
-
-<span>\({h_{ADP}} = {h_{in}} - \frac{{\left( {{{\mathop Q\limits^ \bullet  }_{total}}\,\,/\,\mathop m\limits^ \bullet  } \right)}}{{1 - BF}}\)</span>            ;  single-speed DX coil model (h<sub>ADP1</sub> in figure below),
-
-<span>\({h_{ADP}} = {h_{in}} - \frac{{\left( {{{\mathop Q\limits^ \bullet  }_{total}}\,x\,PLR} \right)\,/\,\mathop m\limits^ \bullet  }}{{1 - BF}}\)</span>  ;  variable refrigerant flow DX coil model
-
-<div>$$SHR = Minimum\left( {\left( {\frac{{{h_{Tin,wADP}} - {h_{ADP}}}}{{{h_{in}} - {h_{ADP}}}}} \right),1} \right)$$</div>
-
-where
-
-<span>\({{h_{in}}}\)</span>          = enthalpy of the air entering the cooling coil, J/kg
-
-<span>\({{h_{ADP}}}\)</span>       = enthalpy of air at the apparatus dew point condition, J/kg
-
-<span>\({{h_{Tin,wADP}}}\)</span> = enthalpy of air at the entering coil dry-bulb temperature and humidity ratio at ADP, J/kg
-
-<span>\(\dot m\)</span>            = air mass flow rate, kg/s
-
-With the SHR for the coil at the current operating conditions, the properties of the air leaving the cooling coil are calculated using the following equations:
-
-<div>$${h_{out}} = {h_{in}} - \left( {\left( {{{\mathop Q\limits^ \bullet  }_{total}}\,xPLR} \right)\,\,/\,\mathop m\limits^ \bullet  } \right)$$</div>
-
-<div>$${h_{Tin,\omega out}} = {h_{in}} - \left( {1 - SHR} \right)\left( {{h_{in}} - {h_{out}}} \right)$$</div>
-
-<div>$${\omega_{out}} = PsyWFnTdbH\left( {{T_{in}},{h_{Tin,\omega out}}} \right)$$</div>
-
-<div>$${T_{db,out}} = PsyTdbFnHW\left( {{h_{out}},{\omega_{out}}} \right)$$</div>
-
-where
-
-<span>\({{h_{out}}}\)</span>         = enthalpy of the air leaving the cooling coil, J/kg
-
-<span>\({{h_{Tin,\omega out}}}\)</span>  = enthalpy of air at the entering coil dry-bulb temperature and leaving air humidity ratio, J/kg
-
-<span>\({{\omega_{out}}}\)</span>        = leaving air humidity ratio, kg/kg
-
-<span>\({T_{db,out}}\)</span>    = leaving air dry-bulb temperature, °C
-
-*PsyWFnTdbH* = EnergyPlus psychrometric function, returns humidity ratio given dry-bulb temperature and enthalpy
-
-*PsyTdbFnHW* = EnergyPlus psychrometric function, returns dry-bulb temperature given enthalpy and humidity ratio
-
-The following figure shows this process on a psychrometric chart. This variable refrigerant flow DX cooling coil model follows the dotted process line from h<sub>in</sub> towards the outlet air enthalpy (the clear circles, ο) based on the modulated refrigerant flow (PLR). The coil surface temperature (ADP, apparatus dew point) is found by drawing a straight line through these points. The process line from h<sub>in</sub> to h<sub>ADP1</sub> represents the full load (PLR=1). This would be what the original DX cooling coil model calculates. At this point the sensible heat ratio is at the design point (assuming h<sub>in</sub> is the rating point and the coil operates at the rated air mass flow rate). As the coil load is reduced, the refrigerant flow rate is restricted and the outlet air condition rides up the dotted line. The outlet air condition and associated h<sub>ADP2</sub> is shown for a PLR of 0.7 (for example purposes only). Here the sensible heat ratio is higher than that found at full load operation. As the load continues to reduce, the refrigerant flow rate continues to throttle back and there comes a point where the coil’s ADP is equal to the inlet air dew point temperature (h<sub>ADP3</sub>). At this point, and for all other PLR’s less than this value, the coil surface becomes dry (at PLR=0.4 in this example) and the coil’s sensible heat ratio = 1. Between this PLR and PLR=0, the coil outlet air condition follows the dotted line back towards H<sub>in</sub>.
-
-<span>\(\cdot \)</span> ![](media/image4182.png)
-
-Figure 180. Process on psychrometric chart
-
-#### Dry Coil Conditions
-
-If the model determines that the cooling coil is dry (ω<sub>in</sub> &lt; ω<sub>ADP</sub>), then the equation for total cooling capacity is invalid since it is a function of entering wet-bulb temperature. Under dry-coil conditions, coil performance is a function of dry-bulb temperature rather than wet-bulb temperature. In this case, the model recalculates the performance of the DX cooling unit using the calculation procedure described above but with ω<sub>in\\ =</sub> ω<sub>dry,</sub> where ω<sub>dry</sub> is the inlet air humidity ratio at the coil dry-out point (SHR = 1.0).
-
-#### Condenser Options:  Air Cooled vs. Evaporative Cooled
-
-As described previously, this model can simulate the performance of air-cooled or evaporative-cooled DX air conditioners. The choice of condenser type impacts the air dry-bulb temperature entering the heat pump’s condenser. Although the actual input for the selection is contained in the variable refrigerant flow air conditioner object, the calculations are repeated here to aid the user in understanding the condenser option choices. The following paragraphs describe three modeling options.
-
-If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) will utilize the outdoor dry-bulb temperature.
-
-If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = EvapCooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) will utilize the outdoor wet-bulb temperature.
-
-If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = EvapCooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) will utilize the condenser inlet air temperature as calculated below:
-
-<div>$${T_{c,i}} = \left( {{T_{wb,o}}} \right) + \left( {1 - EvapCondEffectiveness} \right)\left( {{T_{db,o}} - {T_{wb,o}}} \right)$$</div>
-
-where
-
-*T<sub>c,i</sub>* = the temperature of the air entering the condenser coil, °C
-
-*T<sub>wb,o</sub>* = the wet-bulb temperature of the outdoor air, °C
-
-*T<sub>db,o</sub>* = the dry-bulb temperature of the outdoor air, °C
-
-The Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for the variable refrigerant flow air conditioner object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
-
-#### Condenser Inlet Air Temperature
-
-The air temperature entering the outdoor condenser is based on the weather data used during a simulation. This temperature is either taken directly from the weather data, or can be adjusted based on the height of the outdoor condenser. The input for Condenser Air Inlet Node Name can be used to control this optional feature. If this input is left blank, the air temperature entering the condenser is based solely on the weather data. If this input is not blank, then the node name specified must also be listed in an Outside Air Node or Outside Air Inlet Node List object. When the node name is listed in an Outside Air Inlet Node List object, the air temperature entering the condenser is based solely on the weather data. When the node name is listed in an Outside Air Node object, the height of the node determines the air temperature entering the outdoor condenser (see description of Local Outdoor Air Temperature Calculation in the Atmospheric Variation section of this document for further details).
-
-#### Supply Air Fan Control: Cycling vs. Continuous
-
-One of the inputs to the variable refrigerant flow terminal unit model is the supply air fan operation mode: cycling fan, cycling compressor or continuous fan, cycling compressor. The mode specified in the terminal unit object is passed to the DX cooling coil for use in the model calculations. The first operation mode is frequently referred to as “AUTO fan�, where the compressor(s) and supply air fan operate in unison to meet the zone cooling load, and cycle off together when the cooling load has been met. The second operation mode is often referred to as “fan ON�, where the compressor(s) cycle on and off to meet the zone cooling load but the supply air fan operates continuously regardless of compressor operation.
-
-The fan operation mode schedule value determines the fan operation mode for each time step throughout the simulation. A fan operation mode schedule value of 0 specifies AUTO fan mode operation while values other than 0 specify fan ON operation. The use of a schedule allows the fan operation mode to change based on time-of-day or with changes in season.
-
-The EnergyPlus methodology for determining the impact that HVAC equipment has on an air stream is to calculate the mass flow rate and air properties (e.g., enthalpy, dry-bulb temperature, humidity ratio) exiting the equipment. These exiting conditions are passed along as inlet conditions to the next component model in the air stream. Eventually the flow rate and properties of the air being supplied to the conditioned zone are used in the zone energy balance to determine the resulting zone air temperature and humidity ratio.
-
-With this methodology, the determination of the air mass flow rate and air properties for the two different supply air fan operation modes is slightly different. For the case of cycling fan/cycling compressor, the conditions of the air leaving the cooling coil are the steady-state values calculated using the equations described above. However the air mass flow rate passed along to the next component (and eventually to the conditioned zone) is the average air mass flow rate for the system simulation time step.
-
-For the case of continuous fan/cycling compressor, the air mass flow rate is constant. However, the air properties leaving the cooling coil are calculated as the average conditions during the system simulation time step. The model assumes that the exiting air conditions are the steady-state values calculated using the equations described above when the heat pump operates.  For the remainder of the system simulation time step, it is assumed that the air exiting the DX coil has the same properties as the air entering the coil. For this supply air fan operating strategy, the leaving air properties are calculated as follows:
-
-<div>$${h_{out,\,ContFanCycComp}} = {h_{out}}\left( {CyclingRatio} \right) + {h_{in}}\left( {1 - CyclingRatio} \right)$$</div>
-
-<div>$${\omega_{out,\,ContFanCycComp}} = {\omega_{out}}\left( {CyclingRatio} \right) + {\omega_{in}}\left( {1 - CyclingRatio} \right)$$</div>
-
-<div>$${T_{db,out,ContFanCycComp}} = PsyTdbFnHW\left( {{h_{out,ContFanCycComp}},{\omega_{out,ContFanCycComp}}} \right)$$</div>
-
-#### Average Air Flow Calculations
-
-The variable refrigerant flow (VRF) terminal unit operates based on user-specified (or autosized) air flow rates. The VRF terminal unit’s supply air flow rate during cooling operation may be different than the supply air flow rate during heating operation. In addition, the supply air flow rate when no cooling or heating is required but the supply air fan remains ON can be different than the air flow rates when cooling or heating is required. The outside air flow rates can likewise be different for cooling and heating operating modes. The model takes these different flow rates into account when modeling the heat pump, and the average air flow rate for each simulation time step is reported on the inlet/outlet air nodes of the various terminal unit components in proportion to the calculated cycling ratio of the coil.
-
-The average supply air and outdoor air mass flow rates through the heat pump for the HVAC simulation time step are calculated based on the cycling ratio of the DX cooling coil or heating coil (whichever coil is operating) as follows:
-
-<div>$$\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\,\, = \,\,\mathop m\limits^ \bullet  {\,_{SA,coil\,\,on}}\left( {CyclingRatio} \right) + \mathop m\limits^ \bullet  {\,_{SA,\,\,coil\,\,off}}\left( {1 - CyclingRatio} \right)$$</div>
-
-<div>$$\mathop m\limits^ \bullet  {\,_{OA,\,\,avg\,\,}} = \,\,\mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,on}}\left( {CyclingRatio} \right) + \mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,off}}\left( {1 - CyclingRatio} \right)$$</div>
-
-where:
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\)</span>      = average supply air mass flow rate during the time step, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,coil\,\,on}}\)</span>   = supply air mass flow rate when the coil is ON, kg/s
-
-*CyclingRatio*  = cycling ratio of the coil (heating or cooling)
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,\,\,coil\,\,off}}\)</span>  = supply air mass flow rate when the coil is OFF, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{OA,\,\,avg\,\,}}\)</span>     = average outside air mass flow rate during the time step, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,on}}\)</span>  = average outside air mass flow rate when the coil is ON, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,off}}\)</span> = average outside air mass flow rate when the coil is OFF, kg/s
-
-The supply air and outside air flow rates when the DX cooling or DX heating coil is ON are specified by the user (e.g., supply air volumetric flow rate during cooling operation, supply air volumetric flow rate during heating operation, outside air volumetric air flow rate during cooling operation, and outside air volumetric air flow rate during heating operation) and are converted from volumetric to mass flow rate. If the user has specified cycling fan operation, then the supply air and outside air mass flow rates when the coil is OFF are zero. If the user has specified constant fan operation, then the user-defined air flow rates when no cooling or heating is needed are used when the coil is OFF.
-
-There is one special case. If the user has specified constant fan operation and they specify that the supply air volumetric flow rate when no cooling or heating is needed is zero (or field is left blank), then the model assumes that the supply air and outside air mass flow rates when the coil is OFF are equal to the corresponding air mass flow rates when the coil was last operating (ON).
-
-### Variable Refrigerant Flow Heating Coil
-
-The variable refrigerant flow (VRF) DX heating coil model uses performance information at rated conditions along with performance curves for variations in total capacity, energy input ratio and part load fraction to determine performance at part-load conditions. The impacts of defrost operation is modeled based a combination of user inputs and empirical models taken from the air-to-air heat pump algorithms in DOE-2.1E. The VRF DX heating coil model is very similar to the DX heating coil model used in the single-speed heat pump. The only difference being that the energy performance curves were moved to the parent object (Ref. AirConditioner:VariableRefrigerantFlow). See the DX Heating Coil model description for further details.
-
-### Variable Speed Water to Air Heat Pump (Heating & Cooling)
-
-#### Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit
-
-#### Overview
-
-A Variable Speed Water Source Heat Pump (let’s call it VS WSHP) has a system control which dictates the refrigerant flow rate, the design unit supply airflow and the required water flow rate at each compressor speed. The air and water flow rates are usually a function of the compressor speed. Refrigerant mass flow rate is a function of compressor speed as well as entering water temperature and indoor dry bulb or wet bulb. The control system adjusts the equipment capacity based on zone temperature measurements relative to the thermostat set point. The control logic determines what compressor speed is required to control to the zone temperature requirement in response to increased or decreased capacity (heating or cooling load). The compressor, fan and pump speeds are not discrete values and can be considered to vary infinitesimally between the minimum and maximum compressor speed. At the minimum compressor speed (which is different for heating and cooling), for a continuous fan, the supply airflow is fixed and the unit will have to cycle for reduced part loads below this point. For a cycling fan, the fan will cycle with the compressor.
-
-Present EnergyPlus is capable of modeling multiple-speed DX air-to-air coils. The number of speed levels is up to four. In some cases, four sets of performance curves are not sufficient to include all the information for a variable speed equipment. There is a need to expand the space for containing more performance curves. Here, we expand the number of speed levels and the corresponding curve sets up to ten. The number of speed levels is selectable by the user. The user can provide speed levels at any number from 2 to 10. In any case, our model would just do linear interpolation between neighboring speeds. The more curves, the more accurate. Furthermore, using linear interpolation and inputting air and water flow rates at individual speed levels facilitates arbitrary relationships of flow rates as a function of the compressor speed level.
-
-This model (object name Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit) simulates the performance of a variable-speed water-to-air heat pump with heating capability. It fits in the parent objects of *AirLoopHVAC:UnitaryHeatPump:WaterToAir* and *ZoneHVAC:WaterToAirHeatPump*. The rated conditions for obtaining the Reference Unit total heating capacities and COPs  are indoor dry-bulb temperature at 21.1 ˚C (70 ˚F) and the source side entering water temperature at 21.1 ˚C (70 ˚F).
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-#### Model Description
-
-The Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit object is modeled in a manner similar to the multi-speed DX heating coil model (Ref. Coil:Heating:DX:MultiSpeed). Of course, rather than referencing an air source evaporator or defrost object, the new coil object references to the water loop, and has the entering water temperature in place of the indoor air entering dry bulb temperature.
-
-It shall be noted for the capacity and flow rate inputs, three fields are autosizable, which are Rated Heating Capacity at the Selected Nominal Speed Level (Numeric Field 3), Rated Volumetric Air Flow Rate (Numeric Field 4) and Rated Volumetric Water Flow Rate (Numeric Field 5). They are used to scale the performances of a specific unit and correlate with the actual loop flows. Except these three fields, all other capacity and flow rate inputs at individual speed levels should be directly obtained from Reference Unit catalog data, specific to an actual unit.
-
-The Rated Heating Capacity at Selected Nominal Speed Level contains the rated capacity to match the building heating load at the design day.  The rated heating capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
-
-<div>$$CapacityScaleFactor = \frac{{RatedTotalHeatingCapacity}}{{ReferenceUnitTotalHeatingCapacity@NominalSpeedLevel}}$$</div>
-
-And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below:
-
-<div>$$\begin{array}{l}RatedTotalHeatingCapacity@SpeedLevel\left( x \right) = CapacityScaleFactor\\\quad \quad \quad  \times ReferenceUnitTotalHeatingCapacity@SpeedLevel(x)\end{array}$$</div>
-
-The Rated Volumetric Air Flow Rate is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects, as follows:
-
-<div>$$AirFlowScaleFactor = \frac{{RatedVolumetricAirFlowRate}}{{ReferenceUnitVolAirFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}$$</div>
-
-And the loop volumetric air flow rates at various speed levels in the parent objects are calculated as below:
-
-<div>$$\begin{array}{l}LoopVolumetricAirFlowRate@SpeedLevel\left( x \right) = AirFlowScaleFactor\\\quad \quad \quad \quad  \times ReferenceUnitVolAirFlowRate@SpeedLevel(x)\\\quad \quad \quad \quad  \times CapacityScaleFactor\end{array}$$</div>
-
-If the volumetric air flow rate at one speed level is higher than the flow rate allowed by the fan in the parent object, the flow rate will be set back to the fan flow rate.
-
-This Rated Volumetric Water Flow Rate is used to determine an internal scaling factor, and calculate the loop water flow rates.
-
-<div>$$WaterFlowScaleFactor = \frac{{RatedVolumetricWaterFlowRate}}{{ReferenceUnitVolWaterFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}$$</div>
-
-And the required volumetric water flow rates in the parent objects are calculated as below,
-
-<div>$$\begin{array}{l}LoopVolumetricWaterFlowRate@SpeedLevel\left( x \right) = WaterFlowScaleFactor\\\quad \quad \quad  \times ReferenceUnitWaterVolFlowRate@SpeedLevel(x)\\\quad \quad \quad  \times CapacityScaleFactor\end{array}$$</div>
-
-The required volumetric water flow rate as above should be restricted by the pump in the water loop.
-
-If <span>\(AirFlowScaleFactor\)</span> and <span>\(WaterFlowScaleFactor\)</span> equal unity, the loop flow rates become the design flow rates of the Reference Unit (after scaled by the rated heating capacity). The Rated Volumetric Air Flow Rate and Rated Volumetric Water Flow Rate are introduced here to correlate with the actual flow rates in the air and water loops, in case that these differ from the design specification. Certainly, it is recommended that the Rated Volumetric Air Flow Rate and Rated Volumetric Water Flow Rate are selected in the way that <span>\(AirFlowScaleFactor\)</span> and <span>\(WaterFlowScaleFactor\)</span> are unity, so as to get more accurate results from the performance curves.
-
-Performance curves:
-
-This object includes 7 curve objects at each individual speed level.
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-1)  Total heating capacity modifier curve (function of temperature).
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-2)  Total heating capacity modifier curve (function of air flow fraction).
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-3)  Total heating capacity modifier curve (function of water flow fraction).
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-4)  Energy input ratio (EIR) modifier curve (function of temperature).
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-5)  Energy input ratio (EIR) modifier curve (function of air flow fraction).
-
-6)  Energy input ratio (EIR) modifier curve (function of water flow fraction).
-
-7) Recoverable heat modifier as a function of indoor air dry-bulb and water entering temperatures.
-
-Curves 3) and 6) are new curves as compared to those used for Multi-Speed Electric DX Air Heating Coil, as to correlate the change in water flow rate at the speed. The flow fraction modifier curves are used as a placeholder, to account for off-design flow rates if needed. If the manufacturer doesn’t provide off-design performances, we can simply use a default modification multiplier of 1.0.
-
-At the lowest speed, there will be one additional performance curve to account for the part-load condition, i.e.
-
-8)  Part load fraction correlation (function of part load ratio)
-
-
-
-1) Total heating capacity modifier curve (function of temperature)
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-The total heating capacity modifier as a function of temperature curve (CAP-FT) is a biquadratic curve with two independent variables: dry-bulb temperature of the air entering the heating coil and the VS WSHP’s entering water temperature. The output of this curve is multiplied by the rated total heating capacity at the speed, to give the total heating capacity at the specific entering air and water temperatures at which the WSHP unit is operating (i.e., at temperatures different from the rating point temperatures). 
-
-<div>$$TotCapTempModFac = a + b*D{B_i} + c*DB_i^2 + d*EWT + e*EW{T^2} + f*D{B_i}*EWT$$</div>
-
-where
-
-DB<sub>i</sub> = dry-bulb temperature of the air entering the heating coil, °C
-
-EWT = entering water temperature, °C
-
-a-f = regression curve-fit coefficients
-
-2) Total heating capacity modifier curve (function of air flow fraction)
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-<div>$$TotCapAirFlowModFac = a + b*f{f_a} + c*ff_a^2 + d*ff_a^3$$</div>
-
-where
-
-ff<sub>a</sub> = actual air mass flow rate/design air mass flow rate, at one speed level;
-
-<div>$$\begin{array}{l}DesignAirMassFlowRate@SpeedLevel(x) = \\\quad \quad \quad ReferenceUnitAirMassFlowRate@SpeedLevel(x)\\\quad \quad \quad \quad  \times CapacityScaleFactor\end{array}$$</div>
-
-a-d = regression curve-fit coefficients, if no data available for the correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-3) Total heating capacity modifier curve (function of water flow fraction)
-
-<div>$$TotCapWaterFlowModFac = a + b*f{f_w} + c*ff_w^2 + d*ff_w^3$$</div>
-
-where
-
-ff<sub>w</sub> = actual water mass flow rate/design water mass flow rate, at one speed level;
-
-<div>$$\begin{array}{l}DesignWaterMassFlowRate@SpeedLevel(x) = \\\quad \quad \quad ReferenceUnitWaterMassFlowRate@SpeedLevel(x)\\\quad \quad \quad  \times CapacityScaleFactor\end{array}$$</div>
-
-a-d = regression curve-fit coefficients, if no data available for the correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-4) Energy input ratio (EIR) modifier curve (function of temperature)
-
-The energy input ratio modifier curve as a function of temperature (EIR-FT) is a biquadratic curve with two independent variables: dry-bulb temperature of the air entering the heating coil and the WSHP’s entering water temperature. The output of this curve is multiplied by the rated EIR at the speed (inverse of the rated COP), to give the EIR at the specific entering air and water temperatures at which the WSHP coil unit is operating (i.e., at temperatures different from the rating point temperatures).
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-<div>$$EIRTempModFac = a + b*D{B_i} + c*DB_i^2 + d*EWT + e*EW{T^2} + f*D{B_i}*EWT$$</div>
-
-where
-
-DB<sub>i</sub> = dry-bulb temperature of the air entering the heating coil, °C
-
-EWT = entering water temperature, °C
-
-a-f = regression curve fit coefficients.
-
-5) Energy input ratio (EIR) modifier curve (function of air flow fraction)
-
-<div>$$EIRAirFlowModFac = a + b*f{f_a} + c*ff_a^2 + d*ff_a^3$$</div>
-
-where
-
-a-d = regression curve-fit coefficients, if no data available for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-6) Energy input ratio (EIR) modifier curve (function of water flow fraction)
-
-<div>$$EIRWaterFlowModFac = a + b*f{f_w} + c*ff_w^2 + d*ff_w^3$$</div>
-
-where
-
-a-d = regression curve fit coefficients, if no data available for the correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-7) Recoverable heat modifier as a function of indoor dry-bulb and water entering temperatures.
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-Recoverable heat modifier function accounts for the recoverable waste heat at the condensing side, as a fraction to the input power. This part of heat doesn’t added to the supply side.
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-<div>$$WasteHeatTempModFac = a + b*D{B_i} + c*DB_i^2 + d*EWT + e*EW{T^2} + f*D{B_i}*EWT$$</div>
-
-where
-
-a-f = regression curve-fit coefficients.
-
-8) Part load fraction correlation (function of part load ratio)
-
-This field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, heating load/steady-state heating capacity for Speed 1),
-
-<div>$$PartLoadFrac = a + b*PLR + c*PL{R^2} + d*PL{R^3}$$</div>
-
-And
-
-RTF = (PLR/PartLoadFrac) = runtime fraction of the heating coil
-
-The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor runs continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7 and PLF &gt;= PLR
-
-If PLF &lt; 0.7, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, the runtime fraction of the coil is limited to 1.0. A typical part load fraction correlation would be:
-
-<div>$${\rm{PLF}} = 0.85 + 0.15 \times {\rm{PLR}}$$</div>
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-<div>$${\rm{PLF}} = 0.85 + 0.0 \times {\rm{PLR}}$$</div>
-
-Lowest Speed Operation:
-
-The lowest speed operation of the VS WSHP is similar to the single speed DX heating coil. The total (gross) heating capacity of the WSHP unit is calculated as follows:
-
-<span>\(\begin{array}{l}{Q_{total,1}} = RatedTotalHeatingCapacity@SpeedLevel\left( 1 \right)\\\quad \quad \quad *TotCapTemModFa{c_1}\\\quad \quad \quad *TotCapAirFlowModFa{c_1}\\\quad \quad \quad *TotCapWaterFlowModFa{c_1}\end{array}\)</span>* *
-
-And the EIR is calculated as:
-
-<div>$$\begin{array}{l}EI{R_1} = \frac{{1.0}}{{ReferenceUnitCOP@Speed(1)}}EIRTempModFa{c_1}\\\quad \quad \quad *EIRAirFlowModFa{c_1}\\\quad \quad \quad *EIRWaterFlowModFa{c_1}\end{array}$$</div>
-
-And the power consumption including the compressor and accessories (not including pump and indoor fan powers) is,
-
-<div>$$Powe{r_1} = {Q_{total,1}}*EI{R_1}*RTF$$</div>
-
-The waste heat generated by this coil object is calculated as:
-
-<div>$$\begin{array}{l}{Q_{RecoverHeat,1}} = ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( 1 \right)\\\quad \quad \quad *Powe{r_1}\\\quad \quad \quad *WasteHeatTempModFa{c_1}\end{array}$$</div>
-
-where
-
-<span>\(ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( 1 \right)\)</span> = waste heat fraction of the energy input at Speed 1, from the Reference Unit data.
-
-The total amount of heat absorbed by the evaporator is calculated as:
-
-<div>$${\rm{Q}}{{\rm{}}_{evap,1}} = {Q_{total,1}} + {\rm{}}{Q_{RecoverHeat,1}} - Powe{r_1}$$</div>
-
-The fraction of the actual air mass flow to the design air mass flow rate is calculated:
-
-<div>$$\begin{array}{l}f{f_{a,1}} = actualairmassflowrate/\\\quad \quad \quad (ReferenceUnitAirMassFlowRate@SpeedLevel(1)\\\quad \quad \quad  \times CapacityScaleFactor)\end{array}$$</div>
-
-The fraction of the actual water mass flow to the design water mass flow rate is calculated:
-
-<span>\(\begin{array}{l}f{f_{w,1}} = actualwatermassflowrate/\\\quad \quad \quad (ReferenceUnitWaterMassFlowRate@SpeedLevel(1)\\\quad \quad \quad  \times CapacityScaleFactor)\end{array}\)</span>* *
-
-Higher Speed Operation:
-
-At the speed level between the lowest and the highest, there is no part-load loss. A parameter of speed ratio (SpeedRatio) is used to define the capacity partition between Speed x-1 and Speed x.
-
-The design air and water flow rate at the speed ratio are given as following:
-
- <span>\(\begin{array}{l}{\rm{DesignAirFlowRateSpeedRatio}} = ReferenceUnitAirMassFlowRate@SpeedLevel\left( {x - 1} \right)\\\quad \quad \quad *CapacityScaleFactor\\\quad \quad \quad {\rm{*}}\left( {1{\rm{}}--{\rm{SpeedRatio}}} \right)\\\quad \quad \quad  + ReferenceUnitAirMassFlowRate@SpeedLevel\left( x \right)\\\quad \quad \quad *CapacityScaleFactor\\\quad \quad \quad *SpeedRatio{\rm{}}\end{array}\)</span>
-
-<div>$$\begin{array}{l}{\rm{DesignWaterFlowRateSpeedRatio}} = ReferenceUnitWaterMassFlowRate@SpeedLevel\left( {x - 1} \right)\\\quad \quad \quad *CapacityScaleFactor\\\quad \quad \quad {\rm{*}}\left( {1{\rm{}}--{\rm{SpeedRatio}}} \right)\\\quad \quad \quad  + ReferenceUnitWaterMassFlowRate@SpeedLevel\left( x \right)\\\quad \quad \quad *CapacityScaleFactor\\\quad \quad \quad *SpeedRatio\end{array}$$</div>
-
-And the fractions of air flow and water flow are given:
-
-<span>\(f{f_{a,x - 1}}\)</span>= <span>\(f{f_{a,x}}\)</span>= actual air mass flow rate/DesignAirFlowRateSpeedRatio
-
-<span>\(f{f_{w,x - 1}}\)</span>= <span>\(f{f_{w,x}}\)</span>= actual water mass flow rate/DesignWaterFlowRateSpeedRatio
-
-The total heating capacities and EIRs at Speed x-1 and Speed x are given:
-
-<div>$$\begin{array}{l}{Q_{total,x - 1}} = RatedTotalHeatingCapacity@SpeedLevel\left( {x - 1} \right)\\\quad \quad \quad *TotCapTempModFa{c_{x - 1}}\\\quad \quad \quad *TotCapAirFlowModFa{c_{x - 1}}\\\quad \quad \quad *TotCapWaterFlowModFa{c_{x - 1}}\end{array}$$</div>
-
-<div>$$\begin{array}{l}{Q_{total,x}} = RatedTotalHeatingCapacity@SpeedLevel\left( x \right)\\\quad \quad \quad *TotCapTempModFa{c_x}\\\quad \quad \quad *TotCapAirFlowModFa{c_x}\\\quad \quad \quad *TotCapWaterFlowModFa{c_x}\end{array}$$</div>
-
-<span>\(\begin{array}{l}EI{R_{x - 1}} = \frac{{1.0}}{{ReferenceUnitCOP@Speed(x - 1)}}EIRTempModFa{c_{x - 1}}\\\quad \quad \quad *EIRAirFlowModFa{c_{x - 1}}\\\quad \quad \quad *EIRWaterFlowModFa{c_{x - 1}}\end{array}\)</span>* *
-
-<div>$$\begin{array}{l}EI{R_x} = \frac{{1.0}}{{ReferenceUnitCOP@Speed(x)}}EIRTempModFa{c_x}\\\quad \quad \quad *EIRAirFlowModFa{c_x}\\\quad \quad \quad *EIRWaterFlowModFa{c_x}\end{array}$$</div>
-
-The total heating capacity at the corresponding speed ratio is:
-
-<div>$${Q_{total,SpeedRatio}} = \left( {1.0 - SpeedRatio} \right)*{Q_{total,x - 1}} + SpeedRatio*{Q_{total,x}}$$</div>
-
-And the power consumption is
-
-<div>$$Powe{r_{SpeedRatio}} = \left( {1.0 - SpeedRatio} \right)*{Q_{total,x - 1}}*EI{R_{x - 1}} + SpeedRatio*{Q_{total,x}}*EI{R_x}$$</div>
-
-The waste heat generated by this coil object is calculated as:
-
-<span>\(\begin{array}{l}{Q_{RecoverHeat,SpeedRatio}} = \left( {1.0 - SpeedRatio} \right)\\\quad \quad \quad *ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( {x - 1} \right)\\\quad \quad \quad *WasteHeatTempModFa{c_{x - 1}}*{Q_{total,x - 1}}*EI{R_{x - 1}}\\\quad \quad \quad  + SpeedRatio\\\quad \quad \quad *ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( x \right)\\\quad \quad \quad *WasteHeatTempModFa{c_x}\\\quad \quad \quad *{Q_{total,x}}*EI{R_x}\end{array}\)</span>* *
-
-The total amount of heat absorbed by the evaporator is calculated as:
-
-<div>$${Q_{evap,SpeedRatio}} = {Q_{total,SpeedRatio}} + {\rm{}}{Q_{RecoverHeat,SpeedRatio}} - Powe{r_{SpeedRatio}}$$</div>
-
-At last,
-
-<div>$${Q_{total,SpeedRatio}} = HeatingLoad$$</div>
-
-If the speed reaches the highest level, the speed ratio becomes 1.0, and Speed x represents the highest speed.
-
-#### Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit
-
-#### Overview
-
-This model (object name Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit) simulates the performance of an variable-speed water-to-air heat pump with cooling capability. It fits in the parent objects of *AirLoopHVAC:UnitaryHeatPump:WaterToAir* and *ZoneHVAC:WaterToAirHeatPump*. It has the same logic for varying the compressor, indoor fan and pump speeds as the *Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit* object. The rated conditions for obtaining the capacities, COPs and SHR  are indoor dry-bulb temperature at 26.67 ˚C (80 ˚F), wet bulb temperature at 19.44 ˚C (67 ˚F),  and the source side entering water temperature at 29.4 ˚C (85 ˚F).
-
-Variable-speed cooling coils lead to varied dehumidification behaviors, that the Bypass Factor (BF) is not only dependent on the indoor air flow rate, but also on the refrigerant mass flow rate, i.e. the compressor speed. It is necessary to assess the BF approach for single-speed DX coil, to be used for the variable-speed systems.
-
-TheDOE/ORNL Heat Pump Design Model(HPDM) is a steady-state vapor compression equipment simulation model, which is able to simulate the performance of a VS WSHP system. We rana calibrated HPDM model to produce performance data of a 2.5-ton, VS WSHPunit in space cooling mode. We ran the model to get the total cooling capacities and SHRs, by specifying the EWT at 65˚F, indoor air DB at 80˚F and relative humidity at 0.5, and then varying the indoor air flow rate from 400 scfm to 1000 scfm, the compressor speed from 30 HZ to 90 HZ in a 7×7 matrix. Based on the performance results, we used EES (Engineering Equation Solver) to back-calculate the corresponding BF factors and the A<sub>o</sub> (effective coil surface area) parameters,using the BF equations for the single speed DX cooling coil in EnergyPlus Engineering Reference.
-
-And then, we plotted the resultant A<sub>o</sub> as a function of indoor air flow rate and compressor speed, as below:
-
-![](media/image4240.svg.png)
-
-Figure 181. Effective Surface Area (Ao) Changing with Compressor Speed and Indoor SCFM
-
-![](media/image4241.svg.png)
-
-Figure 182. Bypass Factor (BF) Changing with Compressor Speed and Indoor SCFM
-
-As indicated in the two figures above, the compressor speed is a significant factor impacting the A<sub>o</sub> parameter and the BF factor. So, the current BF factor approach should be upgraded to accommodate variable-speed cooling coils.
-
-As shown in the A<sub>o</sub> figure, we can almost assume that the A<sub>o</sub> parameter mainly depends on the compressor speed. And thus, for enhancing the VS WSHP model, in the IDF file, we need to input SHRs at individual compressor speeds (this is similar to the current multi-speed DX cooling coil). And then, within the VS WSHP module, we calculate the A<sub>o</sub> parameter specific to each compressor speed at the design air flow rates, and then do linear interpolation of A<sub>o</sub> between neighboring compressor speeds. For calculating SHRs in energy simulations, we first calculate the A<sub>o</sub> parameter related to the actual compressor speed, and then use the simulated A<sub>o</sub> parameter in the original BF correlation to correlate effect of the varied indoor air flow rate.
-
-#### Model Description
-
-The Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit object is modeled in a manner similar to the multiple-speed DX cooling coil model (Ref. Coil:Cooling:DX:MultiSpeed). Of course, rather than referencing an air-cooled condenser, the new coil object references the water loop, and have the water entering temperature in place of the condenser air entering dry bulb temperature.
-
-It shall be noted for the total cooling capacity and flow rate inputs, three fields are autosizable, which are Rated Total Cooling Capacity (Numeric Field 3) at Selected Nominal Speed Level, Rated Volumetric Air Flow Rate (Numeric Field 4)  and Rated Volumetric Water Flow Rate (Numeric Field 5). They are used to scale the performances of an actual unit and correlate with the actual loop flows. Except the three fields, all other total cooling capacity and flow rate inputs at individual speed levels should be directly obtained from Reference Unit catalog data, specific to an actual unit.
-
-The Rated Total Cooling Capacity at Selected Nominal Speed Level contains the rated total cooling capacity to match the building sensible or latent cooling load.  The rated cooling capacity is used to determine a capacity scaling factor, as compared to the Reference Unit catalog capacity at the nominal speed level. 
-
-<div>$$CapacityScaleFactor = \frac{{RatedTotalCoolingCapacity}}{{ReferenceUnitTotalCoolingCapacity@NominalSpeedLevel}}$$</div>
-
-And then, this scaling factor is used to determine capacities at rated condition for other speed levels, as below,
-
-<div>$$\begin{array}{l}RatedTotalCoolingCapacity@SpeedLevel\left( x \right) = CapacityScaleFactor\\\quad \quad \quad  \times ReferenceUnitTotalCoolingCapacity@SpeedLevel(x)\end{array}$$</div>
-
-The Rated Volumetric Air Flow Rate is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects, as follows:
-
-<div>$$\begin{array}{l}AirFlowScaleFactor = \\\quad \quad \quad \frac{{RatedVolumetricAirFlowRate}}{{ReferenceUnitVolAirFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}\end{array}$$</div>
-
-And the loop volumetric air flow rates in the parent objects are calculated as below,
-
-<div>$$\begin{array}{l}LoopVolumetricAirFlowRate@SpeedLevel\left( x \right) = \\\quad \quad \quad AirFlowScaleFactor \times ReferenceUnitVolAirFlowRate@SpeedLevel(x) \times CapacityScaleFactor\end{array}$$</div>
-
-If the volumetric air flow rate at one speed level is higher than the flow rate allowed by the fan in the parent object, the flow rate will be set back to the fan flow rate.
-
-This Rated Volumetric Water Flow Rate is used to determine an internal scaling factor, and calculate the loop water flow rates.
-
-<div>$$\begin{array}{l}WaterFlowScaleFactor = \\\quad \quad \quad \frac{{RatedVolumetricWaterFlowRate}}{{ReferenceUnitVolWaterFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}\end{array}$$</div>
-
-And the required volumetric water flow rates in the parent objects are calculated as below,
-
-<div>$$\begin{array}{l}LoopVolumetricWaterFlowRate@SpeedLevel\left( x \right) = \\\quad \quad \quad WaterFlowScaleFactor \times ReferenceUnitVolWaterFlowRate@SpeedLevel(x) \times CapacityScaleFactor\end{array}$$</div>
-
-The required volumetric water flow rate as above is restricted by the pump in the parent object.
-
-If <span>\(AirFlowScaleFactor\)</span> and <span>\(WaterFlowScaleFactor\)</span> are equal to unity, the loop flow rates become the design flow rates of the original unit (after scaled by the rated total cooling capacity). The Rated Volumetric Air Flow Rate and Rated Volumetric Water Flow Rate are introduced here to correlate with the actual flow rates in the air and water loops, in case that these differ from the design specifications. Certainly, it is recommended that the Rated Volumetric Air Flow Rate and Rated Volumetric Water Flow Rate are selected in the way that <span>\(AirFlowScaleFactor\)</span> and <span>\(WaterFlowScaleFactor\)</span> are unity, so as to get more accurate results from the performance curves.
-
-Performance Curves:
-
-This object includes 7 curve objects at each individual speed level.
-
-1)  Total cooling capacity modifier curve (function of temperature)
-
-2)  Total cooling capacity modifier curve (function of air flow fraction)
-
-3)  Total cooling capacity modifier curve (function of water flow fraction)
-
-4)  Energy input ratio (EIR) modifier curve (function of temperature)
-
-5)  Energy input ratio (EIR) modifier curve (function of air flow fraction)
-
-6)  Energy input ratio (EIR) modifier curve (function of water flow fraction)
-
-7) Recoverable heat modifier as a function of indoor air wet-bulb and water entering temperatures.
-
-Curves 3) and 6) are new curves as compared to those used for Multi-Speed Electric DX Air Cooling Coil, to correlate the change in water flow rate at the speed. The flow fraction modifier curves are used as a placeholder, to account for off-design flow rates if needed. If the manufacturer doesn’t provide the off-design performances, we can simply use a default modification multiplier of 1.0.
-
-At the lowest speed, there will be one additional performance curve to correlate the part-load condition, i.e.
-
-**8)** Part load fraction correlation (function of part load ratio)
-
-1)     Total cooling capacity modifier curve (function of temperature)
-
-The total cooling capacity modifier as a function of temperature curve (CAP-FT) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil and the WSHP’s entering water temperature. The output of this curve is multiplied by the rated total cooling capacity at the speed, to give the total cooling capacity at the specific entering air WB and water temperatures at which the WSHP unit is operating (i.e., at temperatures different from the rating point temperatures).
-
-Note: The data used to develop the total cooling capacity modifier curve (function of temperature) should represent performance when the cooling coil is ‘wet’ (i.e., coil providing sensible cooling and at least some dehumidification). Performance data when the cooling coil is ‘dry’ (i.e., not providing any dehumidification) should not be included when developing this modifier curve. This model automatically detects and adjusts for ‘dry coil’ conditions.
-
-<div>$$TotCapTempModFac = a + b*W{B_i} + c*WB_i^2 + d*EWT + e*EW{T^2} + f*W{B_i}*EWT$$</div>
-
-where
-
-WB<sub>i</sub> = wet-bulb temperature of the air entering the heating coil, °C
-
-EWT = entering water temperature, °C
-
-a-f = regression curve-fit coefficients.
-
-2)     Total cooling capacity modifier curve (function of air flow fraction)
-
-The total cooling capacity modifier curve (function of air flow fraction) is a cubic curve with the independent variable being the ratio of the actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of design flow at the speed).
-
-<div>$$TotCapAirFlowModFac = a + b*f{f_a} + c*ff_a^2 + d*ff_a^3$$</div>
-
-where
-
-ff<sub>a</sub> = actual air mass flow rate/design air mass flow rate, at one speed level;
-
-<div>$$\begin{array}{l}DesignAirMassFlowRate@SpeedLevel(x) = \\\quad \quad \quad ReferenceUnitAirMassFlowRate@SpeedLevel(x) \times CapacityScaleFactor\end{array}$$</div>
-
-a-d = regression curve fit coefficients, if no data for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-3)     Total cooling capacity modifier curve (function of water flow fraction)
-
-The total cooling capacity modifier curve (function of water flow fraction) is a cubic curve with the independent variable being the ratio of the actual water flow rate across the water-to-refrigerant heat exchanger to the design water flow rate (i.e., fraction of design flow at the speed).
-
-<div>$$TotCapWaterFlowModFac = a + b*f{f_w} + c*ff_w^2 + d*ff_w^3$$</div>
-
-where
-
-ff<sub>w</sub> = actual water mass flow rate/design water mass flow rate, at one speed level;
-
-<div>$$\begin{array}{l}DesignWaterMassFlowRate@SpeedLevel(x) = \\\quad \quad \quad ReferenceUnitWaterMassFlowRate@SpeedLevel(x) \times CapacityScaleFactor\end{array}$$</div>
-
-a-d = regression curve-fit coefficients, if no data available for the correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-4) Energy input ratio (EIR) modifier curve (function of temperature)
-
-The energy input ratio modifier curve as a function of temperature (EIR-FT) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil and the WSHP’s entering water temperature. The output of this curve is multiplied by the rated EIR (inverse of the rated COP) at the speed level, to give the EIR at the specific entering air and water temperatures at which the WSHP unit is operating (i.e., at temperatures different from the rating point temperatures).
-
-<div>$$EIRTempModFac = a + b*W{B_i} + c*WB_i^2 + d*EWT + e*EW{T^2} + f*W{B_i}*EWT$$</div>
-
-where
-
-WB<sub>i</sub> = wet-bulb temperature of the air entering the cooling coil, °C
-
-EWT = entering water temperature, °C
-
-a-f = regression curve fit coefficients
-
-5) Energy input ratio (EIR) modifier curve (function of air flow fraction)
-
-<div>$$EIRAirFlowModFac = a + b*f{f_a} + c*ff_a^2 + d*ff_a^3$$</div>
-
-where
-
-a-d = regression curve fit coefficients, if no data available for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-6) Energy input ratio (EIR) modifier curve (function of water flow fraction)
-
-<div>$$EIRWaterFlowModFac = a + b*f{f_w} + c*ff_w^2 + d*ff_w^3$$</div>
-
-where
-
-a-d = regression curve fit coefficients, if no data available for correction, the user can simply put a = 1.0, and the other coefficients as 0.0.
-
-7) Recoverable heat modifier as a function of indoor wet-bulb and water entering temperatures.
-
-Recoverable heat modifier function is to account for the recoverable heat at the condensing side, as a fraction to the power input, which doesn’t discharged to the water side.
-
-<div>$$WasteHeatTempModFac = a + b*W{B_i} + c*WB_i^2 + d*EWT + e*EW{T^2} + f*W{B_i}*EWT$$</div>
-
-where
-
-a-f = regression curve fit coefficients
-
-8) Part load fraction correlation (function of part load ratio)
-
-This field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, Sensible or Latent Load/Steady-State Sensible or Latent Capacity  for Speed 1). The description of the part load fraction correlation for the VS WSHP cooling coil is similar to the VS WSHP heating coil.
-
-
-
-Lowest Speed Operation:
-
-The lowest speed operation of the VS WSHP is similar to the single speed DX cooling coil. The total (gross) cooling capacity of the WSHP unit is calculated as follows:
-
-<div>$$\begin{array}{l}{Q_{total,1}} = RatedTotalCoolingCapacity@SpeedLevel\left( 1 \right)\\\quad \quad \quad *TotCapTempModFa{c_1}\\\quad \quad \quad {\rm{*}}TotCapAirFlowModFa{c_1}\\\quad \quad \quad *TotCapWaterFlowModFa{c_1}\end{array}$$</div>
-
-And the EIR is calculated as:
-
-<span>\(\begin{array}{l}EI{R_1} = \frac{{1.0}}{{ReferenceUnitCOP@Speed(1)}}EIRTempModFa{c_1}\\\quad \quad \quad *EIRAirFlowModFa{c_1}\\\quad \quad \quad *EIRWaterFlowModWaterFa{c_1}\end{array}\)</span>* *
-
-And the power consumption excluding the indoor fan and the water pump is,
-
-<div>$$Powe{r_1} = {Q_{total,1}}*EI{R_1}*RTF$$</div>
-
-Where RTF is the run-time fraction.
-
-The recoverable waste heat is:
-
-<div>$$\begin{array}{l}{Q_{RecoverHeat,1}} = ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( 1 \right)\\\quad \quad \quad *Powe{r_1}\\\quad \quad \quad *WasteHeatTempModFa{c_1}\end{array}$$</div>
-
-And the net heat discharged to the water loop is calculated as following:
-
-<span>\({Q_{cond,1}} = Powe{r_1} + {Q_{total,1}} - {Q_{RecoverHeat,1}}\)</span>.
-
-At the lowest speed, the dehumidification calculation is exactly the same as the single speed DX coil. That is to use the rated SHR and the design air flow rate at the lowest speed to calculate rated bypass factor of BF<sub>rated,1</sub>, and the corresponding effective surface area of A<sub>o,1</sub>. Wh A<sub>o,1</sub> known, the coil BF can be adjusted for non-rated air flow rates. It shall be noted if choosing to add hot gas reheating to the supply side,  <span>\({Q_{RecoverHeat,1}}\)</span> should be subtracted from bh the total cooling capacity and the sensible cooling capacity.
-
-And the part load ratio for sensible cooling is,
-
-<div>$$PLR = SensibleCoolingLoad/({Q_{total,1}}*SH{R_1})$$</div>
-
-For latent cooling,
-
-<span>\(PLR = LatentCoolingLoad/[{Q_{total,1}}*(1.0 - SH{R_1})]\)</span>*.*
-
-Higher Speed Operation:
-
-At the speed level between the lowest and the highest, there is no part-load loss. A parameter of speed ratio (SpeedRatio) is used to define the capacity partition between Speed x-1 and Speed x.
-
-
-
-the design air and water flow rate at the speed ratio are given as following:
-
-<div>$$\begin{array}{l}{\rm{DesignAirFlowRateSpeedRatio}} = ReferenceUnitAirMassFlowRate@SpeedLevel\left( {x - 1} \right)\\\quad \quad \quad *CapacityScaleFactor{\rm{*}}\left( {1{\rm{}}--{\rm{SpeedRatio}}} \right)\\\quad \quad \quad  + ReferenceUnitAirMassFlowRate@SpeedLevel\left( x \right)\\\quad \quad \quad *CapacityScaleFactor*SpeedRatio\end{array}$$</div>
-
-<span>\(\begin{array}{l}{\rm{DesignWaterFlowRateSpeedRatio}} = ReferenceUnitWaterMassFlowRate@SpeedLevel\left( {x - 1} \right)\\\quad \quad \quad *CapacityScaleFactor{\rm{*}}\left( {1{\rm{}}--{\rm{SpeedRatio}}} \right)\\\quad \quad \quad  + ReferenceUnitWaterMassFlowRate@SpeedLevel\left( x \right)\\\quad \quad \quad *CapacityScaleFactor*SpeedRatio\end{array}\)</span>.
-
-And the fractions of air flow and water flow are given:
-
-<span>\(f{f_{a,x - 1}}\)</span>. = <span>\(f{f_{a,x}}\)</span>= actual air mass flow rate/DesignAirFlowRateSpeedRatio
-
-<span>\(f{f_{w,x - 1}}\)</span><span>\(f{f_{w,x}}\)</span>= actual water mass flow rate/DesignWaterFlowRateSpeedRatio
-
-The total cooling capacities and EIRs at Speed x-1 and Speed x are calculated:
-
-<span>\(\begin{array}{l}{Q_{total,x - 1}} = RatedTotalCoolingCapacity@SpeedLevel\left( {x - 1} \right)\\\quad \quad \quad *TotCapTempModFa{c_{x - 1}}\\\quad \quad \quad *TotCapAirFlowModFa{c_{x - 1}}\\\quad \quad \quad *TotCapWaterFlowModFa{c_{x - 1}}\end{array}\)</span>* *
-
-<span>\(\begin{array}{l}{Q_{total,x}} = RatedTotalCoolingCapacity@SpeedLevel\left( x \right)\\\quad \quad \quad *TotCapTempModFa{c_x}\\\quad \quad \quad *TotCapAirFlowModFa{c_x}\\\quad \quad \quad *TotCapWaterFlowModFa{c_x}\end{array}\)</span>* *
-
-<span>\(\begin{array}{l}EI{R_{x - 1}} = \frac{{1.0}}{{ReferenceUnitCOP@Speed(x - 1)}}EIRTempModFa{c_{x - 1}}\\\quad \quad \quad *EIRAirFlowModFa{c_{x - 1}}\\\quad \quad \quad *EIRWaterFlowModFa{c_{x - 1}}\end{array}\)</span>* *
-
-The total heating capacity at the corresponding speed ratio is:
-
-<div>$${Q_{total,SpeedRatio}} = \left( {1.0 - SpeedRatio} \right)*{Q_{total,x - 1}} + SpeedRatio*{Q_{total,x}}$$</div>
-
-And the power consumption, excluding the fan and pump power consumptions, is
-
-<div>$$Powe{r_{SpeedRatio}} = \left( {1.0 - SpeedRatio} \right)*{Q_{total,x - 1}}*EI{R_{x - 1}} + SpeedRatio*{Q_{total,x}}*EI{R_x}$$</div>
-
-*The recoverable waste heat is:*
-
-<div>$$\begin{array}{l}{Q_{RecoverHeat,SpeedRatio}} = \left( {1.0 - SpeedRatio} \right)\\\quad \quad \quad *ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( {x - 1} \right)\\\quad \quad \quad *{\rm{WasteHeatTempModFa}}{{\rm{c}}_{x - 1}}*{Q_{total,x - 1}}*EI{R_{x - 1}}\\\quad \quad \quad  + SpeedRatio\\\quad \quad \quad *ReferenceUnitWasteHeatFractionofEnergyInput@SpeedLevel\left( x \right)\\\quad \quad \quad *{\rm{WasteHeatTempModFa}}{{\rm{c}}_x}\\\quad \quad \quad *{Q_{total,x}}*EI{R_x}\end{array}$$</div>
-
-And the net heat discharged to the water loop is calculated as following:
-
-<div>$${Q_{cond,SpeedRatio}} = Powe{r_{SpeedRatio}} + {Q_{total,SpeedRatio}} - {Q_{RecoverHeat,SpeedRatio}}$$</div>
-
-And the effective surface area in the correlations of BF factor  is calculated as below:
-
-<div>$${A_{o,SpeedRatio}} = \left( {1 - SpeedRatio} \right)*{A_{o,x - 1}} + SpeedRatio*{A_{o,x}}$$</div>
-
-Using A<sub>o,SpeedRatio</sub> in the same BF and SHR calculation procedure as the single speed DX cooling coil, we can get BF<sub>SpeedRatio</sub>, and SHR<sub>SpeedRatio.</sub> And the sensible cooling capacity is calculated:
-
-<div>$${Q_{sensible,SpeedRatio}} = {Q_{total,SpeedRatio}}*SH{R_{SpeedRatio}}$$</div>
-
-It should be noted if choosing to add hot gas reheating to the supply side, <span>\({Q_{RecoverHeat,SpeedRatio}}\)</span> should be subtracted from both the total cooling capacity and the sensible cooling capacity.
-
-At last, if the VS WSHP is used to match the sensible cooling load,
-
-<div>$${Q_{sensible,SpeedRatio}} = SensibleLoad$$</div>
-
-If it intends to match the latent cooling load,
-
-<div>$${Q_{total,SpeedRatio}}*\left( {1.0 - SH{R_{SpeedRatio}}} \right) = LatentLoad$$</div>
-
-If the speed reaches the highest level, the speed ratio becomes 1.0, and Speed n represents the highest speed.
-
-#### References
-
-Keith C. Rice, 2011, DOE/ORNL Heat Pump Design Model:
-
-S.A. Klein 2011, User Manual of Engineering Equation Solver V8
-
-#### Secondary Coils of DX Systems and Heat Pumps
-
-#### Overview
-
-Secondary coils reject to or remove heat from a secondary zone. Secondary coil refers to a condenser of a DX system or a heat pump in cooling operating mode or an evaporator of a heat pump in heating mode. The secondary coil (e.g. condenser) of DX system or heat pumps is commonly installed outdoor but when installed indoor either heat is dumped to or extracted from the secondary zone. A secondary zone is a conditioned or unconditioned zone where the secondary coil is installed. Secondary coils are not standalone DX coil objects but they are add-on features on existing DX coil objects. A secondary DX coil is modelled by specifying additional inputs in single speed and multi speed DX coil objects: The additional inputs allow us to model the heat rejected or extracted by the secondary coil while the primary coil serves another controlled zone as shown in [Figure](#SchematicDXCoil).  A secondary coil is not controlled directly but responds to the requirements of the primary DX coil. The operating mode of a secondary DX coil is determined by the primary DX coil serving the conditioned zone. If the primary DX coil is in cooling mode, then the secondary coil is rejecting heat (heating mode) to the secondary zone, or else if the  primary DX coil is in heating mode, then the secondary coil is extracting heat (cooling mode) from the secondary zone. Heat rejected to a secondary zone by a condenser of a DX system or a heat pump is considered as sensible only. Whereas energy extracted from a secondary zone may contain sensible and latent components. The condenser type of the primary DX coils should be AirCooled. There is no need to specify the condenser air inlet node. The model uses zone air node as the secondary coil air inlet node. Air drawn by the secondary coil fan passes through the secondary coil and dumped back into the secondary zone. The previous time step zone condition is used as an inlet condition to the current time for the secondary DX coil model.
-
-![SchematicDXCoil](media/image8002.png)<a name="SchematicDXCoil"></a>
-
-Figure: Schematic of DX System in cooling operating mode
-
-Applications of this technology include: inter-zone heat pump in NTED (Dixon, 2010), and PTAC or PTHP serving Offices attached to a Warehouse, where the office partially or fully enclosed by the warehouse and the condenser is placed inside the Warehouse. The heat rejected or extracted by the secondary DX coil is estimated from the delivered capacity and electric power input of the primary DX coils. And the rejected or extracted heat is treated as internal gain of the secondary zone. Currently secondary DX coil are allowed in single speed, two speed and multi speed DX coil objects: _Coil:Cooling:DX:SingleSpeed_, _Coil:Heating:DX:SingleSpeed_, _Coil:Cooling:DX:TwoSpeed_, _Coil:Cooling:DX:MultiSpeed_, and _Coil:Heating:DX:MultiSpeed_.
-
-#### Model Description:
-The secondary coil performance calculation is invoked using inputs in the DX coil objects.  The input required for cooling and heating operation of the primary DX coils are different. In the DX cooling coils the only required input is the zone name where the secondary coil is installed. In heating DX coils six inputs are required for single speed coils and a minimum of 11 input fields are required for multispeed DX heating coils.  And five more inputs are required for every additional compressor speed. The extensible five input fields are used for splitting the total heat extraction rate into sensible and latent components. These five input fields are: rated sensible heat ratio, secondary air flow rates, scaling factor for auto-sizing secondary air flow rates, sensible heat ratio modifier curves as a function of temperature and sensible heat ratio modifier curves as a function of secondary air flow fraction. The secondary coil model assumes that liquid water from defrosting operation is drained to the outdoor and has no impact on the zone air heat balance. 
-
-**Cooling Operating Mode:** the primary DX cooling coil of a DX system serving a primary zone is on and heat is rejected by the secondary coil (condenser) into a secondary zone. The secondary zone name is specified in DX cooling coil objects.  This operating mode applies to a DX cooling system and cooling operating mode of air-to-air single and multi-speed heat pumps. The heat rejected by the secondary coil (condenser) of a DX system or heat pump operating in cooling mode is given by:
-
-<div>$$Q_\rm{cond}=Q_\rm{Evap}+P_\rm{CompCondFan}$$</div>
-
-where
-
-* \(Q_\rm{Evap}\) is the cooling load delivered by the primary DX cooling coil system, W 
-* \(P_\rm{CompCondFan}\) is the compressor and evaporator fan electric power input of a heat pump in heating mode, W
-* \(Q_\rm{cond}\) is the heat rejected by the secondary coil (condenser) of a DX system or heat pump, W
-
-Heat rejected by a secondary coil (condenser) calculated at each time step becomes internal gain of the secondary zone as shown in [Figure](#SchematicDXAndSecondary). Whenever a secondary zone name is specified in DX cooling coil objects, the secondary DX coil model calculation is invoked.  New input field required as add-on to the DX cooling coil objects is "_Zone Name for Secondary Coil (condenser) Placement_".
-
-![SchematicDXAndSecondary](media/image8003.png)<a name="SchematicDXCoil"></a>
-
-Figure: Schematic of DX system and secondary coil (condenser)
-
-**Heating Operating Mode:** When a heat pump operates in heating mode then energy is extracted from the secondary zone.  The total energy extracted is estimated by rearranging the equation above as follows:
-
-<div>$$Q_\text{Evap} = Q_\text{cond} - P_\text{CompCondFan}$$</div>
-
-where
-
-* \(Q_\text{cond}\) is the heat delivered by the primary heating DX coil to the primary zone, W
-* \(P_\text{CompCondFan}\) is the compressor and condenser fan electric power input of a DX system or heat pump in cooling mode, W
-* \(Q_\text{Evap}\) is the energy extracted by secondary coil (evaporator) from the secondary zone, W
-
-The total energy extracted from a secondary zone may contain sensible and latent components.  The secondary coil model checks for the coil inlet and full load outlet air condition to determine whether dehumidification will occur. The sensible and latent split of the energy extracted is done using a user specified rated sensible heat ratio (SHR) and SHR modifier curves for temperature and the secondary air flow fraction.  If the secondary coil operation is dry, then the SHR is set to 1.0.  In addition, the model assumes that defrosting operation is on, then the defrosting melts the frost and the liquid water from the collecting pan is drained to outside. Thus defrosting energy is not included in the zone energy balance. The heat extracted from the secondary zone may contain sensible and latent components and the secondary coil model does the sensible/latent heat split calculation.
-
-#### Sensible Heat Ratio Calculation
-
-The SHR calculation method uses user specified SHR modifying curves for temperature and flow fraction.  The modifying curves correct the rated SHR value for a given secondary DX coil (evaporator) entering air temperatures and air mass flow fraction for a given speed. If these SHR modifying curves are not specified a constant SHR will be assumed.  These two curves are a biquadratic SHR modifier curve for temperature (SHRFT), and a quadratic SHR correction curve for flow fraction (SHRFFF). The SHR is given by:
-
-<div>$$SHR = SHR_\text{rated}\cdot SHRFT\left(T_\text{wb,secondaryZone},T_\text{db,primaryCoil}\right)\cdot SHRFFF(FF)$$</div>
- 
-where
-
-* \(SHRFT\) is the sensible heat ratio modifier normalized biquadratic curve as a function of secondary DX coil entering air wet-bulb and primary DX coil entering air dry-bulb temperatures, (-). The secondary DX coil (evaporator) entering air wet-bulb temperature is the secondary zone air wet-bulb temperature.
-* \(SHRFFF\) is the sensible heat ratio modifier normalized quadratic curve as a function of air mass flow fraction.  Flow fraction is the ratio of actual to rated mass flow rate of air through the secondary DX coil, (-).
-* \(SHR_\text{rated}\) is the sensible heat ratio at rated condition, (-).
-
-For multispeed secondary DX coils when the system is cycling between two speeds of _n_ and _n_-1 the operating SHR is weighted using _SpeedRatio_ as follows:
-
-<div>$$SHR = SHR_n \cdot SpeedRatio +  SHR_{n-1} (1 - SpeedRatio)$$</div>
- 
-where
-
-* \(SHR_n\) is the sensible heat ratio at speed n determined from user specified rated SHR, and SHR modifier curves at speed _n_, (-)
-* \(SHR_{n-1}\) is the sensible heat ratio at speed _n_-1 determined from user specified rated SHR, and _SHR_ modifier curves at speed _n_-1, (-).
-* _SpeedRatio_ is a parameter that relates performance between successive compressor speeds, (-).
-
-#### Sensible and Latent Split
-The air enthalpy difference across the secondary DX coil (evaporator) at full load is given by:
-
-<div>$$h_\text{Delta} = \frac{\left(Q_\text{Evap}/PLR\right)}{\dot{m}_\text{cond}}$$</div>
-
-The coil outlet enthalpy is calculated as follows:
-
-<div>$$h_\text{Outlet}=h_\text{Inlet}-h_\text{Delta}$$</div>
-
-Using the SHR calculated above and secondary DX coil outlet temperature is given by:
-
-<div>$$T_\text{OutletNode} = T_\text{ZoneAirNode} -  \frac{\left(Q_\text{Evap}/PLR\right)\cdot SHR}{\dot{m}_\text{cond}c_p}$$</div>
-
-Calculate the saturated outlet temperature at the outlet enthalpy and check the secondary outlet air condition if super-saturation has occurred:
-
-<div>$$T_\text{OutletNode, Sat} = T_\text{SAT}\left(h_\text{Outlet}, P_\text{Tot}\right)$$</div>
-
-    IF(\(T_\text{OutletNode} > T_\text{OutletNode, Sat}\)) Then
-        \(\omega_\text{OutletNode} > \omega_\text{InletNode}\)
-    ELSE
-        (\(T_\text{OutletNode} = T_\text{OutletNode, Sat}\)
-        The coil outlet humidity ratio is determined using psychrometric functions as follows.
-        \(\omega_\text{OutletNode} = \omega\left(T_\text{OutletNode,Sat},h_\text{Outlet}\right)\)
-    ENDIF
-
-where
-
-*\(h_\text{Inlet}\) is the enthalpy of air entering the passive coil, (J/kg)
-*\(h_\text{Outlet}\) is the enthalpy of air leaving the passive coil, (J/kg)
-*\(\dot{m}_\text{sec}\) is the secondary DX coil mass flow rate, (kg/s)
-*\(PLR\) is the primary DX cooling coil compressor part-load ratio, (-)
-*\(P_\text{Tot}\) is the total pressure at the inlet of secondary DX coil, (Pa)
-*\(T_\text{OutletNode}\) is the secondary coil outlet air temperature, (degC)
-*\(T_\text{OutletNode,Sat}\) is the secondary coil saturated air temperature at the outlet enthalpy, (degC)
-*\(\omega_\text{InletNode}\) is the secondary coil inlet node air humidity ratio, (kgH2O/kgDryair)
-*\(\omega_\text{OutletNode}\) is the secondary coil outlet node air humidity ratio, (kgH2O/kgDryair)
-
-Reference: Dixon, Erin Elizabeth, "Energy Model Development and Heating Energy Investigation of the Nested Thermal Envelope Design (NTED (tm))" (2010). Theses and dissertations. Paper 974.
-
-### Packaged Thermal Storage Cooling Coil
-
-The DX cooling coil model for Coil:Cooling:DX:SingleSpeed:ThermalStorage is described in this section. The following diagram shows the main aspects of the model for packaged thermal energy storage cooling coil.  This model allows charging and discharging to shift cooling energy use. The dashed line shows the boundary of the empirical "black box" model.  The main parts are the Condenser, Evaporator, Compressor, and Thermal Energy Storage (TES) tank.  The model interacts with the surroundings via a condenser inlet and outlet nodes, evaporator inlet and outlet nodes, heat transfer between TES tank and surrounding ambient environment, and optional added plant connection to the TES tank.
-
-![](media/image4287.png)
-
-Figure 183. Highlights of Packaged Thermal Storage Cooling Coil
-
-Depending on the operating mode, different parts are active.  There are six modes to consider.
-
-**Off Mode** is when the unit is not running but the TES tank still interacts with ambient and the model needs to track the state of charge in the tank.
-
-![](media/image4288.png)
-
-Figure 184. Thermal Storage Cooling Coil Off Mode
-
-Governing equations for Off Mode include:
-
-<span>\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} = 0\)</span>      (water tank)
-
-<span>\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} = 0\)</span>     (ice tank)
-
-<div>$${\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)$$</div>
-
-<div>$${\dot Q_{Plant}} = \dot m\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)$$</div>
-
-
-
-**Cooling Only Mode** is when the unit is running but since it is neither charging nor discharging the TES tank, the model is essentially the same as a normal single speed DX cooling coil.  The latent degradation model is not available.  The model uses SHR curves  from user input.
-
-![](media/image4293.png)
-
-Figure 185. Thermal Storage Coil Cooling Only Modee
-
-
-
-The governing equations for Cooling Only Mode include:
-
-<span>\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} = 0\)</span>      (water tank)
-
-<span>\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} = 0\)</span>    (ice tank)
-
-<div>$$\dot W + {\dot Q_{Evap}} + {\dot Q_{Cond}} = 0$$</div>
-
-<div>$${\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)$$</div>
-
-<div>$${\dot Q_{Plant}} = \dot m{c_p}\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)$$</div>
-
-
-
-The input correlations are used in the following manner to determine cooling capacity and energy consumption for a given set of operationg conditions.
-
-One total evaporator cooling capacity modifier curve is a function of evaporator inlet wetbulb temperature and condenser inlet drybulb temperature.
-
-<div>$$EvapCapTempModFac = {f_{}}\left( {{T_{evap,wb}},{\rm{}}{T_{cond,db}}} \right)$$</div>
-
-Another total evaporator cooling capacity modifier curve is a function of air flow fraction through the evaporator section where air flow fraction is the ratio of current air mass flow rate to the rated air mass flow rate.
-
-<div>$$EvapCapFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,{\rm{}}air}}} {{{\dot m}_{evap,{\rm{}}airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}airRated}}}$}}} \right)$$</div>
-
-One energy input ratio modifier curve is a function of evaporator inlet wetbulb temperature and condenser inlet drybulb temperature.
-
-<div>$$EIRTempModFac = f\left( {{T_{evap,wb}},{\rm{}}{T_{cond,db}}} \right)$$</div>
-
-Another energy input ratio modifier curve is a function of flow fraction.
-
-<div>$$EIRFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,{\rm{}}air}}} {{{\dot m}_{evap,{\rm{}}airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}airRated}}}$}}} \right)$$</div>
-
-Part load degradation curve is a function of part load ratio.
-
-<div>$$EvapPartLoadFac = f\left( {PLR} \right)$$</div>
-
-The results of the performance curves are applied as follows to determine cooling capacity and energy performance:
-
-<div>$${\dot Q_{Evap}} = {\dot Q_{Evap,RatedCoolOnly}}\left( {EvapCapTempModFac} \right)\left( {EvapCapFlowModFac} \right)$$</div>
-
-<div>$${\dot W_{elec}} = \frac{{{{\dot Q}_{evap}}\left( {EIRTempModFac} \right)\left( {EIRFlowModFac} \right)\left( {PLR} \right)}}{{\left( {CO{P_{Rated,{\rm{}}CoolOnly}}} \right)\left( {EvapPartLoadFac} \right)}}$$</div>
-
-The sensible heat ratio (SHR) is determined by a rated SHR and two performance curves. The SHR temperature modifying factor is a function of evaporator entering wetbulb and evaporator entering drybulb temperature.
-
-<div>$$SHRTempModFac = f\left( {{T_{evap,wb}},{T_{evap,db}}} \right)$$</div>
-
-The SHR flow fraction modifying factor is a function of air flow fraction through the evaporator section where air flow fraction is the ratio of current air mass flow rate to the rated air mass flow rate.
-
-<div>$$SHRFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,{\rm{}}air}}} {{{\dot m}_{evap,{\rm{}}airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}airRated}}}$}}} \right)$$</div>
-
-The results of the performance curves are applied as follows to determine SHR:
-
-<div>$$SHR = SH{R_{rated}}*SHRTempModFac*SHRFlowModFac$$</div>
-
-Cool and Charge Mode is when the unit is both cooling and charging the TES, then all the parts are active. The electric power into the compressor is split into two terms to accommodate devices that actually have dual compressors.
-
-![](media/image4309.png)
-
-Figure 186. Thermal Storage Coil Cool and Charge Modes
-
-Governing Equations for “Cool and Charge Mode�
-
-<span>\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\)</span>      (water tank)
-
-<span>\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\)</span>    (ice tank)
-
-<div>$${\dot W_{Evap}} + {\dot W_{TES}} + {\dot Q_{Evap}} + {\dot Q_{Cond}} + {\dot Q_{TES}} = 0$$</div>
-
-<div>$${\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)$$</div>
-
-<span>\({\dot Q_{Plant}} = \dot m{c_p}\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\)</span><div>$${\dot Q_{Plant}} = \dot m\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)$$</div>
-
-The input correlations are used in the following manner to determine cooling capacity, chargine capacity, and energy consumption for a given set of operationg conditions.
-
-One total evaporator cooling capacity modifier curve is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES, <span>\({S_{TES}}\)</span> (temperature of water or fraction of ice).
-
-<div>$$EvapCapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)$$</div>
-
-Another total evaporator cooling capacity modifier curve is a function of flow fraction.
-
-<div>$$EvapCapFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,air}}} {{{\dot m}_{evap,airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,airRated}}}$}}} \right)$$</div>
-
-One evaporator energy input ratio modifier curve, function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
-
-<div>$$EIREvapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)$$</div>
-
-Another energy input ratio modifier curve is a function of flow fraction.
-
-<div>$$EIREvapFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,air}}} {{{\dot m}_{evap,airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,airRated}}}$}}} \right)$$</div>
-
-Part load degradation curve is a function of evaporator part load ratio.
-
-<div>$$EvapPartLoadFac = f\left( {PLR} \right)$$</div>
-
-One storage charge capacity modifier curve is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
-
-<div>$$TESCapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)$$</div>
-
-Another storage charge capacity modifier curve is a function of evaporator part load ratio.
-
-<div>$$TESCapPartLoadFac = f\left( {PLR} \right)$$</div>
-
-The results of the performance curves are applied as follows to determine cooling capacity and energy performance:
-
-<div>$${\dot Q_{Evap}} = {\dot Q_{Evap,RatedCoolAndCharge}}\left( {EvapCapTempModFac} \right)\left( {EvapCapFlowModFac} \right)$$</div>
-
-<div>$${\dot Q_{TES}} = {\dot Q_{Charge,Rated}}\left( {TESCapTempModFac} \right)\left( {TESCapPartLoadFac} \right)$$</div>
-
-<div>$${\dot W_{Evap,elec}} = \frac{{\left( {{{\dot Q}_{Evap}}} \right)\left( {EIRTempModFac} \right)\left( {EIRFlowModFac} \right)\left( {EvapPLR} \right)}}{{\left( {CO{P_{Rated,Cooling}}} \right)\left( {EvapPartLoadFac} \right)}}$$</div>
-
-<span>\({\dot W_{TES,elec}} = \frac{{\left( {{{\dot Q}_{TES}}} \right)\left( {EIRStorTempModFac} \right)\left( {EIRStorFlowModFac} \right)\left( {StorPLR} \right)}}{{\left( {CO{P_{Rated,Charging}}} \right)\left( {StorPartLoadFac} \right)}}\)</span>.
-
-The sensible heat ratio (SHR) is determined by a rated SHR and two performance curves. There are two options for the SHR temperature modifying factor, it can either be a function of evaporator entering wetbulb and evaporator entering drybulb temperature or it can add a third independent variable for the state of charge of TES.
-
-<div>$$\begin{array}{l}SHRTempModFac = \left\{ \begin{array}{l}f\left( {{T_{evap,wb}},{T_{evap,db}}} \right)\\f\left( {{T_{evap,wb}},{T_{evap,db}},{S_{TES}}} \right)\end{array} \right.\\\end{array}$$</div>
-
-The SHR flow fraction modifying factor is a function of air flow fraction through the evaporator section where air flow fraction is the ratio of current air mass flow rate to the rated air mass flow rate.
-
-<div>$$SHRFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,{\rm{}}air}}} {{{\dot m}_{evap,{\rm{}}airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}airRated}}}$}}} \right)$$</div>
-
-The results of the performance curves are applied as follows to determine SHR:
-
-<div>$$SHR = SH{R_{rated}}*SHRTempModFac*SHRFlowModFac$$</div>
-
-
-
-**Cool and Discharge Mode** is when the unit is both cooling and discharging the TES, then all the parts are active. The electric power into the compressor is split into two terms to accommodate devices that actually have dual compressors.
-
-
-
-
-
-![](media/image4331.png)
-
-Figure 187. Thermal Storage Coil Cool and Discharge Modes
-
-
-
-Governing Equations for “Cool and Discharge Mode�
-
-<span>\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\)</span>      (water tank)
-
-<span>\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\)</span>    (ice tank)
-
-<div>$${\dot W_{Evap}} + {\dot W_{TES}} + {\dot Q_{Evap}} + {\dot Q_{Cond}} + {\dot Q_{TES}} = 0$$</div>
-
-<div>$${\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)$$</div>
-
-<span>\({\dot Q_{Plant}} = \dot m{c_p}\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\)</span><div>$${\dot Q_{Plant}} = \dot m\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)$$</div>
-
-The input correlations are used in the following manner.
-
-One total evaporator cooling capacity modifier curve is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
-
-<div>$$EvapCapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)$$</div>
-
-Another Total evaporator cooling capacity modifier curve is a function of flow fraction.
-
-<div>$$EvapCapFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,air}}} {{{\dot m}_{evap,airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,airRated}}}$}}} \right)$$</div>
-
-One evaporator energy input ratio modifier curve is a function of of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
-
-<div>$$EIREvapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)$$</div>
-
-Another evaporator energy input ratio modifier curve is a function of flow fraction.
-
-<div>$$EIREvapFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,air}}} {{{\dot m}_{evap,airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,airRated}}}$}}} \right)$$</div>
-
-Evaporator part load degradation curve is a function of evaporator part load ratio.
-
-<div>$$EvapPartLoadFac = f\left( {EvapPLR} \right)$$</div>
-
-One storage discharge capacity modifier curve is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
-
-<div>$$TESCapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)$$</div>
-
-Another storage discharge capacity modifier curve is a function of evaporator part load ratio.
-
-<div>$$TESCapPartLoadFac = f\left( {EvapPLR} \right)$$</div>
-
-One storage energy input ratio modifier curve is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
-
-<div>$$EIRStorTempModFac = {f_{triquadratic}}\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)$$</div>
-
-Another storage energy input ratio modifier curve is a function of flow fraction.
-
-<div>$$EIRStorFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,air}}} {{{\dot m}_{evap,airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,airRated}}}$}}} \right)$$</div>
-
-Storage part load degradation curve is a function of storage discharge part load ratio.
-
-<div>$$StorPartLoadFac = f\left( {StorPLR} \right)$$</div>
-
-The results of the performance curves are applied as follows to determine cooling capacity and energy performance:
-
-<div>$${\dot Q_{Evap}} = {\dot Q_{Evap,RatedCoolAndDischarge}}\left( {EvapCapTempModFac} \right)\left( {EvapCapFlowModFac} \right)$$</div>
-
-<div>$${\dot Q_{TES}} =  - {\dot Q_{Discharge,Rated}}\left( {TESCapTempModFac} \right)\left( {TESCapPartLoadFac} \right)$$</div>
-
-<div>$${\dot W_{Evap,elec}} = \frac{{\left( {{{\dot Q}_{Evap}}} \right)\left( {EIREvapTempModFac} \right)\left( {EIREvapFlowModFac} \right)\left( {EvapPLR} \right)}}{{\left( {CO{P_{Rated,Cooling}}} \right)\left( {EvapPartLoadFac} \right)}}$$</div>
-
-<div>$${\dot W_{TES,elec}} = \frac{{\left( {{{\dot Q}_{TES}}} \right)\left( {EIRStorTempModFac} \right)\left( {EIRStorFlowModFac} \right)\left( {StorPLR} \right)}}{{\left( {CO{P_{Rated,Discharging}}} \right)\left( {StorPartLoadFac} \right)}}$$</div>
-
-The sensible heat ratio (SHR) is determined by a rated SHR and two performance curves. There are two options for the SHR temperature modifying factor, it can either be a function of evaporator entering wetbulb and evaporator entering drybulb temperature or it can add a third independent variable for the state of charge of TES.
-
-<div>$$\begin{array}{l}SHRTempModFac = \left\{ \begin{array}{l}f\left( {{T_{evap,wb}},{T_{evap,db}}} \right)\\f\left( {{T_{evap,wb}},{T_{evap,db}},{S_{TES}}} \right)\end{array} \right.\\\end{array}$$</div>
-
-The SHR flow fraction modifying factor is a function of air flow fraction through the evaporator section where air flow fraction is the ratio of current air mass flow rate to the rated air mass flow rate.
-
-<div>$$SHRFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,{\rm{}}air}}} {{{\dot m}_{evap,{\rm{}}airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}airRated}}}$}}} \right)$$</div>
-
-The results of the performance curves are applied as follows to determine SHR:
-
-<div>$$SHR = SH{R_{rated}}*SHRTempModFac*SHRFlowModFac$$</div>
-
-
-
-**Charge Only Mode** is when the unit is only charging, there is no heat flow at the evaporator.  There is no modulation or part loading, when charging the unit charges at its nominal design rate (adjusted for conditions).
-
-
-
-
-
-![](media/image4355.png)
-
-Figure 188. Thermal Storage Coil Charge Only Mode
-
-
-
-The governing equations for “Charge Only Mode�
-
-<span>\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\)</span>      (water tank)
-
-<span>\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\)</span>    (ice tank)
-
-<div>$$\dot W + {\dot Q_{Cond}} + {\dot Q_{TES}} = 0$$</div>
-
-<div>$${\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)$$</div>
-
-<span>\({\dot Q_{Plant}} = \dot m{c_p}\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\)</span><div>$${\dot Q_{Plant}} = \dot m\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)$$</div>
-
-The input correlations are used in the following manner.
-
-
-
-Storage charge capacity modifier factor is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
-
-<div>$$TESCapTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)$$</div>
-
-Energy input ratio modifier factor is a function of evaporator inlet wetbulb and condenser inlet drybulb temperatures and state of TES.
-
-<div>$$EIRTempModFac = f\left( {{T_{evap,wb}},{T_{cond,db}},{S_{TES}}} \right)$$</div>
-
-<div>$${\dot Q_{TES}} = \left( {{{\dot Q}_{Charge,Rated}}} \right)\left( {TESCapTempModFac} \right)$$</div>
-
-<div>$${\dot W_{elec}} = \left( {{{\dot Q}_{TES}}} \right)\left( {\frac{1}{{CO{P_{Rated,ChargeOnly}}}}} \right)\left( {EIRTempModFac} \right)$$</div>
-
-
-
-
-
-**Discharge Only Mode** is when the unit is only discharging, there is no heat flow at the condenser. The rate of discharge will modulate to meet part loading at the evaporator.
-
-![](media/image4366.png)
-
-Figure 189. Thermal Storage Coil Discharge Only Mode
-
-The governing equations for “Discharge Only Mode�
-
-<span>\(- M{c_p}\frac{{DT}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\)</span>      (water tank)
-
-<span>\(- M{h_{fs}}\frac{{DF}}{{Dt}} + {\dot Q_{Amb}} + {\dot Q_{Plant}} + {\dot Q_{TES}} = 0\)</span>    (ice tank)
-
-<div>$$\dot W + {\dot Q_{Evap}} + {\dot Q_{TES}} = 0$$</div>
-
-<div>$${\dot Q_{Amb}} = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)$$</div>
-
-<span>\({\dot Q_{Plant}} = \dot m{c_p}\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\)</span><span>\({\dot Q_{Plant}} = \dot m\varepsilon \left( {{T_{TES}} - {T_{w,in}}} \right)\)</span>
-
-The input correlations are used in the following manner.
-
-
-
-One total evaporator cooling capacity modifier factor is a function of evaporator inlet wetbulb temperature and state of TES.
-
-<div>$$EvapCapTempModFac = f\left( {{T_{evap,wb}},{S_{TES}}} \right)$$</div>
-
-Another total evaporator cooling capacity modifier factor is a function of flow fraction.
-
-<div>$$EvapCapFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,air}}} {{{\dot m}_{evap,airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,airRated}}}$}}} \right)$$</div>
-
-One energy input ratio modifier factor is a function of evaporator inlet wetbulb temperature and state of TES.
-
-<div>$$EIRTempModFac = f\left( {{T_{evap,wb}},{S_{TES}}} \right)$$</div>
-
-Another energy input ratio modifier factor is a function of flow fraction.
-
-<div>$$EIRFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,air}}} {{{\dot m}_{evap,airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,airRated}}}$}}} \right)$$</div>
-
-Part load degradation curve is a function of evaporator part load ratio.
-
-<div>$$EvapPartLoadFac = f\left( {EvapPLR} \right)$$</div>
-
-<span>\({\dot Q_{Evap}} = \left( {{{\dot Q}_{Evap,RatedDischargeOnly}}} \right)\left( {EvapCapTempModFac} \right)\left( {EvapCapFlowModFac} \right)\)</span>. <span>\({\dot W_{elec}} = \frac{{\left( {{{\dot Q}_{evap}}} \right)\left( {EIRStorTempModFac} \right)\left( {EIRStorFlowModFac} \right)\left( {EvapPLR} \right)}}{{\left( {CO{P_{Rated,DischargeOnly}}} \right)\left( {EvapPartLoadFac} \right)}}\)</span>
-
-<div>$${\dot Q_{TES}} = {\dot Q_{Evap}} + {\dot W_{elec}}$$</div>
-
-The sensible heat ratio (SHR) is determined by a rated SHR and two performance curves. There are two options for the SHR temperature modifying factor, it can either be a function of evaporator entering wetbulb and evaporator entering drybulb temperature or it can add a third independent variable for the state of charge of TES.
-
-<div>$$\begin{array}{l}SHRTempModFac = \left\{ \begin{array}{l}f\left( {{T_{evap,wb}},{T_{evap,db}}} \right)\\f\left( {{T_{evap,wb}},{T_{evap,db}},{S_{TES}}} \right)\end{array} \right.\\\end{array}$$</div>
-
-The SHR flow fraction modifying factor is a function of air flow fraction through the evaporator section where air flow fraction is the ratio of current air mass flow rate to the rated air mass flow rate.
-
-<div>$$SHRFlowModFac = f\left( {{\raise0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}air}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{evap,{\rm{}}air}}} {{{\dot m}_{evap,{\rm{}}airRated}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{evap,{\rm{}}airRated}}}$}}} \right)$$</div>
-
-The results of the performance curves are applied as follows to determine SHR:
-
-<div>$$SHR = SH{R_{rated}}*SHRTempModFac*SHRFlowModFac$$</div>
-
-
-
-HVAC Controllers <a name="Controllers"></a>
-----------------
-
-### Control Valve for Water-Based Air System Coils
-
-The input object Controller:WaterCoil provides a simple controller model for adjusting water flow rates to meet the desired air side conditions. It is really a solution inverter. For a water coil the simulation cannot be inverted where the mass flow rate of the water through the coil can be solved directly given an air temperature. Thus, this “controller� will numerically step through all of the water flow possibilities by a root finding technique until the mass flow rate is determined to meet the specified outlet air temperature within a specified user tolerance.
-
-#### Model Description
-
-The figure below illustrates the use of a simple controller used with a central chilled water coil (control variable Temperature). The controller reads the desired temperature setpoint from the control node (established by a SetpointManager) and modulates the chilled water flow rate at the actuator node in order to meet the desired supply (coil outlet) air temperature.
-
-![TemperatureControlledWaterCoil](media/image4384.png)
-
-Figure 190. Controller:WaterCoil used with Central Chilled Water Coil
-
-In this case, the controller simply senses the temperature at the control node and compares this value with the desired temperature setpoint. If the sensed temperature is above the desired setpoint temperature, the chilled water flow rate is increased. This controller may be used for both chilled water and hot water coils. The action parameter input is set to REVERSE for chilled water cooling coils and NORMAL for hot water heating coils.
-
-The simple controller may also be used to control both high temperature and high humidity levels by controlling the water flow rate through a chilled water coil. Setting the controller’s control variable to TemperatureAndHumidityRatio enables this feature. In this case, the controller monitors two setpoint values, one for temperature control and the other for high humidity control. Note that two setpoint managers must be used to establish these setpoints as shown in the figure below. The limiting case for either temperature or high humidity control (i.e., the minimum supply air temperature required to meet both setpoints) is used for controlling the water flow rate through the chilled water coil. If high humidity control is the limiting case then colder supply air will be delivered by the cooling coil to achieve proper dehumidification and some form of air reheat may be required to avoid overcooling of the zones being served by this air loop.
-
-![TempHumRatControlledWaterCoil](media/image4385.png)
-
-Figure 191. Two Setpoint managers used in Controller:WaterCoil
-
-When the control variable TemperatureAndHumidityRatio is used, the controller modulates water flow through a chilled water coil to meet both a temperature and a humidity ratio setpoint. These two setpoints are placed on the control node by setpoint managers.
-
-The model first calculates the approach temperature using the dry-bulb temperature and dewpoint temperature of the air leaving the water coil:
-
-<div>$${T_{dp}} = {\rm{PsyTdpFnWPb}}\left( {{\omega_{SA}},P} \right)$$</div>
-
-<div>$${T_{approach}} = {T_{SA}} - {T_{dp}}$$</div>
-
-where:
-
-<span>\({T_{approach}}\)</span>= approach temperature, ËšC
-
-<span>\({\omega_{SA}}\)</span> = supply (outlet) air humidity ratio, kg/kg
-
-<span>\(P\)</span>   = outdoor barometric pressure, Pa
-
-<span>\({T_{dp}}\)</span>  = supply (outlet) air dewpoint temperature, ˚C
-
-<span>\({T_{SA}}\)</span> = supply (outlet) air dry-bulb temperature, ˚C
-
-<span>\({\rm{PsyTdpFnWPb}}\)</span>= EnergyPlus psychrometric function, returns dewpoint temperature given humidity ratio and barometric pressure
-
-The supply air dewpoint temperature required to meet the humidity ratio setpoint (placed on the control node by SetpointManager:SingleZone:Humidity:Maximum, SetpointManager:MultiZone:MaximumHumidity:Average  or SetpointManager:MultiZone:Humidity:Maximum) is then calculated as a function of the humidity ratio setpoint and barometric pressure as follows:
-
-<div>$${T_{dp,SP}} = {\rm{PsyTdpFnWPb}}\left( {{\omega_{SP}},P} \right)$$</div>
-
-where:
-
-<span>\({T_{dp,SP}}\)</span>= dewpoint temperature corresponding to *w<sub>SP</sub>*, ËšC
-
-<span>\({\omega_{SP}}\)</span>= humidity ratio setpoint, kg/kg
-
-In order for the dewpoint temperature of the coil’s supply (outlet) air to reach <span>\({T_{dp,SP}}\)</span> the dry-bulb temperature of air leaving the cooling coil must be at <span>\({T_{dp,SP}} + {T_{approach}}\)</span>:
-
-<div>$${T_{HR,SP}} = {T_{dp,SP}} + {T_{approach}}$$</div>
-
-where:
-
-<span>\({T_{HR,SP}}\)</span>= supply air dry-bulb temperature setpoint required to achieve the specified humidity ratio setpoint, ËšC
-
-The supply air temperature setpoint required to achieve the specified humidity ratio setpoint is then compared to the setpoint temperature required for zone temperature control, and the minimum of these two setpoint values is used as the setpoint temperature for controlling the chilled water coil.
-
-<div>$${T_{SP}} = MIN\left( {{T_{Temp,SP}},{T_{HR,SP}}} \right)$$</div>
-
-where:
-
-<span>\({T_{SP}}\)</span>= chilled water coil supply air temperature setpoint, ËšC
-
-<span>\({T_{Temp,SP}}\)</span>= supply air temperature setpoint required for zone temperature control, ËšC
-
-As described previously, the controller varies the chilled water flow rate through the coil using a root finding technique until the actual supply air temperature reaches *T<sub>sp</sub>*within the specified tolerance:
-
-<div>$${T_{Actual}} - {T_{SP}}\,\, \le \,\,\,Controller\,Convergence\,Tolerance$$</div>
-
-where:
-
-<span>\({T_{Actual}}\)</span>= actual air temperature leaving the cooling coil, ËšC
-
-### Outdoor Air Damper Controller for Air Systems
-
-When the heat exchanger assisted cooling coil is used with a furnace or unitary system (ref. AirLoopHVAC:Unitary:Furnace:HeatCool or AirLoopHVAC:UnitaryHeatCool) or DX system (ref. CoilSystem:Cooling:DX) located in an air loop (or DX system used in an outside air system), an ecomizier function may be customized as necessary. For economizer control, an outdoor air controller (ref. Controller:OutdoorAir) is used to define the economizer control inputs and determine when economizer mode is active. The heat exchanger (ref. HeatExchanger:\*) object provides an economizer lockout feature which disables heat recovery any time the economizer is active. This feature can be turned on and off using the heat exchanger lockout input. Heat exchanger assisted cooling coils used with the zone equipment described below disregard this economizer control feature. The heat recovery bypass control input may also be used to selectively control heat recovery.
-
-#### Inputs
-
-§ Controller Name
-
-§ Relief air node
-
-§ Return air node
-
-§ Control node (the mixed air node)
-
-§ Actuated node (the outside air inlet node)
-
-§ Minimum outside air flow rate (at design) [m<sup>3</sup>/s]
-
-§ Maximum outside air flow rate  (<span>\({\dot V_{oa,\max }}\)</span>) [m<sup>3</sup>/s]
-
-§ EconomizerChoice: *FixedDryBulbr* | *FixedEnthalpy* | * DifferentialDryBulb * | * DifferentialEnthalpy* | *  ElectronicEnthalpy* | *  FixedDewPointAndDryBulb   * | *DifferentialDryBulbAndEnthalpy * | *NoEconomizer*
-
-§ Bypasschoice: *MinimumFlowWithBypass* | *ModulateFlow*
-
-§ High temperature limit (<span>\({T_{high}}\)</span>) [C]
-
-§ High specific enthalpy limit (<span>\({h_{high}}\)</span> ) [J/kg]
-
-§ High dewpoint temperature limit (<span>\({T_{DP,high}}\)</span>) [C]
-
-§ Electronic Enthalpy limit (quadratic or cubic curve object)
-
-§ Low temperature limit (<span>\({T_{low}}\)</span>) [C]
-
-§ Lockout: *LockoutWithHeating* | *LockoutWithCompressor*
-
-§ MinimumLimit: *FixedMinimum* | *ProportionalMinimum*
-
-§ Minimum outside air schedule (schedule values multiply the minimum outside air flow rate)
-
-§ Minimum Outside air flow Schedule(schedule values sets the limit on minimum outside air)
-
-§ Maximum Outside air flow Schedule(schedule values sets the maximum amount of outside air possible in the system)
-
-§ Name of Controller:MechanicalVentilation object
-
-§ Time-of-day economizer control schedule (economizer active when schedule values are greater than 0)
-
-§ High humidity control flag: *Yes* | *No*
-
-§ Humidstat control zone name (zone name where humidistat is located)
-
-§ Control high indoor humidity based on outdoor humidity ratio: *Yes* | *No*
-
-§ High humidity outside air flow ratio (this flow ratio is multiplied by the maximum outside air flow rate during periods of high indoor relative humidity)
-
-§ Heat Recovery Bypass Control Type: BypassWhenWithinEconomizerLimits | BypassWhenOAFlowGreaterThanMinimum
-
-#### Economizer Limits
-
-Economizer limits may be used to create single-point or multi-point controllers. The figure below shows several examples of each type of controller. Single-point economizer controllers use a single independent variable to specify the operation of the economizer. In all cases, the economizer is disabled (OFF) when the outdoor weather condition exceeds the limit. However, when a low temperature limit is used the economizer is disabled when the outdoor temperature is *below* the low dry-bulb temperature limit.
-
-Economizer limits may also be used to create multi-point controllers where two or more limits specify the economizer operating region. The economizer is disabled (OFF) if any single multi-point economizer limit is exceeded.
-
-![EconomizerLimitContrrol](media/image4411.png)
-
-Figure 192. Economizer Limit Controls
-
-#### Simulation
-
-The simulation contains 4 steps.
-
-#### Step 1: calculate the minimum outside air flow rate
-
-The user inputs the minimum outside air flow rate (or it is automatically calculated by the program from the user’s design inputs). This is converted to a mass flow rate <span>\({\dot m_{oa,\min ,des}}\)</span>using the density of dry air at 20 degrees C. If the economizer is on an air loop then the minimum outside air flow fraction is initialized to:
-
-<div>$${f_{oa,\min }} = {\dot m_{oa,\min ,des}}/{\dot m_{s,des}}$$</div>
-
-Where <span>\({\dot m_{s,des}}\)</span>is the design supply air mass flow rate. If the economizer is not on an air loop the minimum outside air flow fraction is initialized to:
-
-<div>$${f_{oa,\min }} = {\dot m_{oa,\min ,des}}/{\dot m_{oa,\max ,des}}$$</div>
-
-where <span>\({\dot m_{oa,\max ,des}}\)</span>is the user input maximum outside air volumetric flow rate converted to mass flow rate in the same manner as for the minimum outside air flow rate. If a minimum outside air schedule has been input, <span>\({f_{oa,\min }}\)</span>is multiplied by the current schedule value.
-
-#### Step 2: calculate an initial outside air signal
-
-We now define an initial outside air signal <span>\({S_{oa,init}}\)</span>.
-
-If <span>\(\left| {{T_{_r}} - {T_{in}}} \right| > \Delta {T_{small}}\)</span>then:
-
-<span>\({S_{oa,init}} = ({T_r} - {T_{mix,set}})/({T_r} - {T_i})\)</span>.
-
-Otherwise:
-
-if <span>\({T_r} &lt; {T_{mix,set}}\)</span>and <span>\({T_r} \ge {T_i}\)</span> , <span>\({S_{oa,init}}\)</span>is set to -1;
-
-if <span>\({T_r} &lt; {T_{mix,set}}\)</span> and <span>\({T_r} &lt; {T_i}\)</span>, <span>\({S_{oa,init}}\)</span>  is set to 1;
-
-if <span>\({T_r} \ge {T_{mix,set}}\)</span>and <span>\({T_r} \ge {T_i}\)</span>, <span>\({S_{oa,init}}\)</span> is set to 1;
-
-if <span>\({T_r} \ge {T_{mix,set}}\)</span> and <span>\({T_r} &lt; {T_i}\)</span>, <span>\({S_{oa,init}}\)</span> is set to -1.
-
-Finally, <span>\({S_{oa,init}}\)</span>is constrained to be: <span>\({f_{oa,\min }} \le {S_{oa,init}} \le 1\)</span>. Basically, if the outside air can not accomplish cooling, <span>\({S_{oa,init}}\)</span> is set to <span>\({f_{oa,\min }}\)</span>. If it can do cooling, <span>\({S_{oa,init}}\)</span> is greater than the minimum outside air flow fraction but not greater than1. Here
-
-      *T<sub>r</sub>*  is the return air temperature [C];
-
-*      T<sub>i</sub>* is the outside air inlet temperature [C];
-
-*      T<sub>mix,set</sub>* is the mixed air setpoint [C];
-
-*      <span>\(\Delta {T_{small}}\)</span>*is a small temperature difference [delta C], equal to .00001.
-
-#### Step 3: do the on/off and limit checks
-
-·        If *EconomizerChoice* = *No Economizer*, <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>.
-
-·        If <span>\({\dot V_{oa,\max }} &lt; {\dot V_{small}}\)</span>, <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>; <span>\({\dot V_{small}}\)</span>is.001 m<sup>3</sup>/s.
-
-·        If the economizer is locked out, <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>.
-
-Note: the above three checks also set the *EconomizerOperationFlag* and *HighHumidityControlFlag* to *false* (economizer and high humidity control not operating).
-
-·        If <span>\({T_i} > {T_{mix,set}}\)</span> , <span>\({S_{oa,init}} = 1\)</span>.
-
-·        If Differential dry-bulb was input as Economizer choiceand <span>\({T_i} > {T_r}\)</span>, then <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>.
-
-·        If Differential Enthalpy was input as Economizer choiceand <span>\({h_i} > {h_r}\)</span>, then <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>, where *h<sub>i</sub>* and *h<sub>r</sub>* are the outside air inlet and return air enthalpies.
-
-Setpoints are checked after this which include check for Fixed dry-bulb temperature  limit, Enthalpy Limit, Dewpoint Limit and Humidity ratio limit if specified.
-
-·        If Differential Enthalpy was input as Economizer choiceand <span>\({h_i} > {h_r}\)</span>, then <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>, where *h<sub>i</sub>* and *h<sub>r</sub>* are the outside air inlet and return air enthalpies.
-
-Setpoints are checked after this which include check for Fixed dry-bulb temperature limit, Enthalpy Limit, Dewpoint Limit and Humidity ratio limit if specified.
-
-·        If a FixedDryBulb / FixedEnthalpy / FixedDewPointAndDryBulb / ElectronicEnthalpy was input as the economizer choice then the limits are checked as before.
-
-·        Limits are checked as follows
-
-o   If a high temperature limit was input and <span>\({T_{oa}} > {T_{high}}\)</span>, <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>; where *T<sub>oa</sub>* is the outside air temperature.
-
-o   If an enthalpy limit was input and <span>\({h_{oa}} > {h_{high}}\)</span>, <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>; where *h<sub>oa</sub>* is the outside air specific enthalpy.
-
-o   If a dewpoint temperature limit was input and <span>\({T_{DP,OA}} > {T_{DP,high}}\)</span>, <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>; where T<sub>DP,OA</sub> is the outside air dewpoint temperature and T<sub>DP,high</sub> is dewpoint temperature limit.
-
-o   If an electronic enthalpy curve was input and <span>\({w_{OA}} > {w_{CurveOutput}}\)</span>, <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>; where *w*<sub>OA</sub> is the outside air humidity ratio and *w*<sub>CurveOutput</sub> is the curve’s humidity ratio output as a function of outdoor air dry-bulb temperature.
-
-·        Another Economizer choice called DifferentialDryBulbAndEnthalpy checks the outside air temperature against return temperature and outside air enthalpy against return air enthalpy and also checks the setpoints.
-
-·        If a low temperature limit was input and <span>\({T_{oa}} &lt; {T_{low}}\)</span>, <span>\({S_{oa,init}} = {f_{oa,\min }}\)</span>.
-
-Note: the above nine cases set the *EconomizerOperationFlag* to *false*       (economizer not operating), otherwise the economizer is active.
-
-·        If high humidity control is specified and the zone humidistat indicates a moisture load (i.e. zone relative humidity greater than the relative humidity setpoint), the *HighHumidityOperationFlag* is set to *true.* If high humidity control is based on the outdoor humidity ratio then the *HighHumidityOperationFlag* is set to *true* only when the outdoor air humidity ratio is less than the humidstat’s zone humidity ratio. A *true* HIghHumidityOperationFlag also enables economizer operation in the heat exchangers as if the economizer flag used here was also set to *true* (Ref. HeatExchanger:\* - field Economizer Lockout).
-
-The economizer schedule is then checked to determine if a “push-button� type economizer control is used. When schedule values are greater than 0, the economizer is active (*EconomizerOperationFlag* = *true)*. This test overrides the economizer limit checks described above in Step 3.
-
-#### Step 4: calculate the final outside air signal
-
-If *S<sub>oa,init</sub>* is greater than <span>\({f_{oa,\min }}\)</span>and less than 1 and the mixed air mass flow rate is greater than <span>\({\dot m_{verysmall}}\)</span>(<span>\({10^{ - 30}}\)</span>) and night venting is not occuring and *HighHumidityOperationFlag* is false then
-
-·        we calculate a final outside air signal *S<sub>oa</sub>* by using the regula falsi method routine *SolveRegulaFalsi* to zero the residual <span>\({T_{mix,set}} - {T_{mix}}\)</span>by varying the outside air mass flow rate <span>\({S_{oa}}\cdot {\dot m_{mix}}\)</span>. Mass and energy balance are used to obtain the mixed air humidity ratio and enthalpy from the recirculated air and outside air inlet conditions. The psychrometric function *PsyTdbFnHW* is used to obtain *T<sub>mix</sub>* from the mixed air enthalpy and humidity ratio.
-
-Otherwise
-
-·        <span>\({S_{oa}} = {S_{oa,init}}\)</span>.
-
-#### Step 5: calculate the outside air flow rate and apply final constraints
-
-·        If *BypassChoice* =*True and HighHumidityOperationFlag = false*, <span>\({S_{oa}} = {f_{oa,\min }}\)</span>.
-
-1)   If the *HighHumidityOperationFlag* is *true* then
-
-<div>$${S_{oa}} = MAX\left[ {{f_{oa,\min }},OAFlowRati{o_{HighRH}}\left( {{\raise0.7ex\hbox{${{{\dot m}_{oa,\max ,des}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{oa,\max ,des}}} {{{\dot m}_{mix}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot m}_{mix}}}$}}} \right)} \right]$$</div>
-
-·        If night ventilation is occuring, <span>\({S_{oa}} = 1\)</span>.(Night Ventilation has priority over the above constraints)
-
-·        If the Minimum Outside air flow Schedule and the Maximum outside air flow schedule is available , Out Air signal *S oa*,*init*  is checked against those fractions from the schedule.
-
-      S<sub>oa</sub>  = Maximum( Minimum OA fraction, S<sub>oa</sub>)
-
-      S<sub>oa</sub>    = Minimum(Maximum OA fraction, S<sub>oa</sub>)
-
-Now the outside air flow rate is calculated:
-
-<div>$${m_{oa}} = {S_{oa}}*{m_{mix}}$$</div>
-
-Calculate the outside air mass flow rate:
-
-If EconomizerOperationFlag is true and HighHumidityOperationFlag is false  then
-
-<div>$${\dot m_{oa}} = {S_{oa}}\cdot {\dot m_{oa,\max ,des}}$$</div>
-
-Otherwise
-
-<div>$${\dot m_{oa}} = {S_{oa}}\cdot {\dot m_{mix}}$$</div>
-
-Then the following constraints are applied.
-
-·        <span>\({\dot m_{oa}}\)</span> must be greater than or equal to the air primary loop total exhaust air mass flow rate (<span>\({\dot m_{exhaust}}\)</span>).
-
-·        If *MinimumLimit* = *Fixed Minimum*, <span>\({\dot m_{oa}}\)</span> must be greater than or equal to the minimum outside air mass flow rate.
-
-·        <span>\({\dot m_{oa}}\)</span> must be <span>\(\le {\dot m_{mix}}\)</span>.
-
-·        <span>\({\dot m_{oa}}\)</span> must be <span>\(\le \)</span> the maximum outside air mass flow rate.
-
-If heat recovery bypass control is selected, the type of control determines how heat recovery is simulated. If BypassWhenWithinEconomizerLimits is selected, heat recovery is only active when the EconomizerOperationFlag is false. If BypassWhenOAFlowGreaterThanMinimum is selected *and* the EconomizerOperationFlag is true *and* the outside air mass flow rate is greater than the minimum flow rate, heat recovery is disabled, otherwise heat recovery is active. The heat recovery bypass control option is used to optimize heat recovery in heating mode. Heat recovery is commonly used to reduce the cooling load when outdoor conditions are higher than indoor conditions, however, when outdoor conditions are favorable the heat exchanger can be turned off and the economizer may be used to also reduce the cooling load. Economizer mode is typically involves increasing the outdoor air flow rate. At some point the outdoor air flow rate must be reduced and the heat exchanger should be turned back on to reduce or avoid an indoor heating requirement. This option will typically be used with some form of supply air temperature control used with the heat recovery equipment (Ref. HeatExchanger).
-
-#### Step 6: set the relief air mass flow rate
-
-<div>$${\dot m_{relief}} = \max (0,{\dot m_{oa}} - {\dot m_{exhaust}})$$</div>
-
-
-
-### Outdoor Air Damper Controller for Zone Energy Recovery Ventilator
-
-The stand alone energy recovery ventilator (ERV) controller is used solely in conjunction with a stand alone energy recovery ventilator (see figure below).
-
-![Schematic\_StandAloneERV](media/image4482.png)
-
-Figure 193. Schematic of the ZoneHVAC:EnergyRecoveryVentilator Compound Object
-
-This controller object mimics virtually all of the control logic available for a conventional air-side economizer as embodied in the object Controller:OutdoorAir. However, this controller is only used with the stand alone energy recovery ventilator object (dedicated to serving a single zone, without a traditional air distribution system) while the Controller:OutdoorAir is used with systems that utilize an air loop to provide conditioned air to one or more zones. The purpose of this controller is to signal the object HeatExchanger:AirToAir:SensibleAndLatent that favorable conditions are available for free cooling and heat exchange should be suspended (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped). A time-of-day schedule may also be used to simulate a “push-button� type economizer. The air flow rate through the stand alone ERV remains the same regardless of whether the controller is signaling for economizer (free cooling) operation or not. In this way, this controller is very similar to Controller:OutdoorAir with the field Economizer Control Action Type set to “MinimumFlowWithBypass�. However, the supply and exhaust air flow rates may be modified in response to a high indoor humidity condition (i.e., when the zone relative humidity is “predicted� to exceed the setpoint, at times the actual zone relative humidity may be slightly below the setpoint. Ref. Zone/Sys Moisture Load Rate Predicted.) and works in a similar fashion to the outside air controller where the air flow rates are adjusted based on a user specified air flow *ratio*.
-
-#### Controller Logic
-
-In many ways, the logic for this controller follows that established for the object Controller:OutdoorAir. Nearly the same computations (source code) are used for this controller as for Controller:OutdoorAir, except the addition of a few calculations that are unique for this stand alone ERV controller. Refer to the *Simulation* discussion for the outdoor air controller to review the calculation procedure. In some instances local variables used in the Controller:OutdoorAir computations are set to specific values for ZoneHVAC:EnergyRecoveryVentilator:Controller to allow the same computations and logic to be used for both controllers. The logic that is being applied for ZoneHVAC:EnergyRecoveryVentilator:Controller is presented below.
-
-As explained above the controller senses when air conditions are such that heat exchange by the air-to-air heat exchanger should be suspended to provide free cooling to the zone, thereby reducing the amount of mechanical cooling that needs to be provided by other equipment. The inputs for this controller specify temperature and/or enthalpy conditions that are used to trigger economizer operation. An economizer lockout input is provided in the heat exchanger object and is used for customizing heat exchanger performance during economizer operation. Heat exchange is suspended only if the heat exchanger’s economizer lockout input is set to Yes.
-
-The user can enter a high and low temperature limit for economizer operation. When the supply inlet (outdoor) air is between these two values, heat exchange is suspended while air flow rates remain unchanged. This logic represents a conventional single-point temperature economizer control. If the user wishes to model differential temperature control, EXHAUST AIR TEMP LIMIT should be specified in the proper input field. In this case, heat exchange is suspended whenever the temperature of the exhaust air is greater than the temperature of the outdoor air. The user still needs to set the low temperature limit to restart the heat exchange process when the outdoor temperature falls too low.
-
-A high dewpoint temperature limit may also be specified. When the supply inlet (outdoor) air is below this limit, heat exchange is suspended while air flow rates remains unchanged. The user still needs to set the low temperature limit to restart the heat exchange process when the outdoor temperature falls too low.
-
-Similar logic can be used with air enthalpy. The user can enter a high enthalpy limit, and heat exchange between the supply and exhaust air streams will be suspended when the outdoor air enthalpy falls below this value. This logic represents single-point enthalpy economizer control. If the user wishes to model differential enthalpy control, EXHAUST AIR ENTHALPY LIMIT should be specified in the proper input field. Regardless of modeling single-point enthalpy or differential enthalpy control, the user still needs to set the low temperature limit to restart the heat exchange process when the outdoor temperature falls too low.
-
-The user may also specify an electronic enthalpy curve object to represent a variable enthalpy controller. A quadratic or cubic curve is used in this case. The output of this curve would represent the maximum outdoor humidity ratio allowed as a function of outdoor dry-bulb temperature.
-
-The air flow rates through the stand alone ERV may also be modified based on a high indoor relative humidity condition. The change in air flow rates may occur at any time the indoor relative humidity is high or when the indoor relative humidity is high *and* the outdoor humidity ratio is lower than the indoor humidity ratio. This control mode modifies the air flow rates according to the user specified high humidity outside air flow ratio. When high humidity control is active, heat exchange is suspended in the same manner as if an economizer were used and, as with economizer operation, heat exchange is suspended only if the heat exchanger’s economizer lockout input is set to Yes.
-
-The model is flexible, and checks all limits established by the user in the object’s input data. The model initially assumes that heat exchange should be suspended, and then checks each one of the limits that the user has set (single-point temperature, differential temperature, single-point enthalpy and differential point enthalpy, single-point dewpoint or electronic (variable) enthalpy). If any of the limits entered by the user is exceeded, then economizer operation is terminated and heat exchange between the supply and exhaust air streams is modeled.
-
-Baseboard Heaters <a name="Baseboards"></a>
------------------
-
-### Hot Water Baseboard Heater with Only Convection
-
-#### Overview
-
-The convective water baseboard heater (Ref. ZoneHVAC:Baseboard:Convective:Water) is a simple model for establishing a convective-only heat addition to a space through a baseboard heater.  In most situations, the baseboard heater does give a significant amount of heat off via natural convection, but some heat is given off via radiation.  In this model, the radiant component is ignored and all heat is assumed to be delivered to the space via convection.  The baseboard heater is supplied with hot water from the primary system which is circulated through the inside of a finned tube within the space.  Heat is transferred from the water inside the pipe, through the tube and fins, and eventually convected to the surrounding air within the space.  EnergyPlus then assumes that this heat is evenly spread throughout the space thus having an immediate impact on the zone air heat balance which is used to calculate the mean air temperature (MAT) within the space.
-
-The model requests an effective UA value to handle the heat exchange between the water loop and the zone air.  From there, it employs an effectiveness-NTU heat exchanger model to determine the heat transfer between the water and the zone air.  This is necessary because during the simulation only the inlet water and “inlet air� (assumed to be zone air) is known.  As a result, the effectiveness-NTU heat exchanger methodology is better suited to determine the performance of the system.
-
-#### Model Description
-
-#### Convective Water Baseboard Heater Inputs
-
-Like many other HVAC components, the convective-only water baseboard model requires a unique identifying name, an availability schedule, and water side inlet and outlet nodes.  These define the availability of the unit for providing condition to the space and the node connections that relate to the primary system.  In addition, a convergence tolerance is requested of the user to help define the ability of the local controls to tightly control the system output.  In almost all cases, the user should simply accept the default value for the convergence tolerance unless engaged in an expert study of controls logic in EnergyPlus.
-
-The input also requires a UA value and a maximum design flow rate for the unit.  Both of these parameters can be chosen to be auto-sized by EnergyPlus.  The UA value corresponds to the convective heat transfer from the water to the tube, the conduction through the tube and fin material, and the natural convection from the tube/fins to the zone air.  The maximum flow rate and UA value define the performance and maximum output of the baseboard unit.
-
-#### Simulation and Control
-
-The simulation of the convective water baseboard unit follows standard effectiveness-NTU methodology.  It begins by calculating the product of the specific heat and mass flow rate for both the air and water sides of the unit (heat exchanger).  In the initialization of the model, it is assumed that the air mass flow rate is equal to 2.0 times the water mass flow rate.  The purpose of this calculation is to provide some reasonable estimate of the air mass flow rate so that the model can calculate system performance correctly.  This calculation is kept constant throughout the rest of the simulation.
-
-Each system time step, the baseboard attempts to meet any remaining heating requirement of the zone through the following calculations:
-
-<div>$${C_{water}} = {c_{p,water}}{\dot m_{water}}$$</div>
-
-<div>$${C_{air}} = {c_{p,air}}{\dot m_{air}}$$</div>
-
-<div>$${C_{\max }} = MAX\left( {{C_{air}},{C_{water}}} \right)$$</div>
-
-<div>$${C_{\min }} = MIN\left( {{C_{air}},{C_{water}}} \right)$$</div>
-
-<div>$${C_{ratio}} = {{{C_{\min }}} \mathord{\left/ {\vphantom {{{C_{\min }}} {{C_{\max }}}}} \right. } {{C_{\max }}}}$$</div>
-
-<div>$$\varepsilon  = 1 - {e^{\left( {\frac{{NT{U^{0.22}}}}{{{C_{ratio}}}}{e^{\left( { - {C_{ratio}}NT{U^{0.78}}} \right)}} - 1} \right)}}$$</div>
-
-Once the effectiveness is determined, the outlet conditions for and output from the unit are determined using the following equations:
-
-<div>$${T_{air,outlet}} = {T_{air,inlet}} + \varepsilon {{\left( {{T_{water,inlet}} - {T_{air,inlet}}} \right){C_{\min }}} \mathord{\left/ {\vphantom {{\left( {{T_{water,inlet}} - {T_{air,inlet}}} \right){C_{\min }}} {{C_{air}}}}} \right. } {{C_{air}}}}$$</div>
-
-<div>$${T_{water,outlet}} = {T_{water,inlet}} - \left( {{T_{air,outlet}} - {T_{air,inlet}}} \right){{{C_{air}}} \mathord{\left/ {\vphantom {{{C_{air}}} {{C_{water}}}}} \right. } {{C_{water}}}}$$</div>
-
-<div>$$Output\left( {Convective} \right) = {C_{water}}\left( {{T_{water,inlet}} - {T_{water,outlet}}} \right)$$</div>
-
-If the unit was scheduled off or there is no water flow rate through the baseboard unit, then there will be no convection from the unit.  The model assumes no heat storage in the baseboard unit itself and thus no residual heat transfer in future system time steps due to heat storage in the water or metal of the baseboard unit.
-
-#### References
-
-The effectiveness-NTU method is taken from Incropera and DeWitt, Fundamentals of Heat and Mass Transfer, Chapter 11.4, p. 523, eq. 11.33.  The user can always refer to the ASHRAE Handbook series for general information on different system types as needed.
-
-### Electric Baseboard Heater with Only Convection
-
-#### Overview
-
-The input object ZoneHVAC:Baseboard:Convective:Electric provides a model for electric baseboard heaters that assumes only convective heat addition to a space from a baseboard heater.  In most situations, the baseboard heater does give a significant amount of heat off via natural convection, but some heat is given off via radiation.  In this model, the radiant component is ignored and all heat is assumed to be delivered to the space via convection.  The baseboard heater is transferred to the unit via electric resistance heating.  EnergyPlus then assumes that this heat is evenly spread throughout the space thus having an immediate impact on the zone air heat balance which is used to calculate the mean air temperature (MAT) within the space.
-
-#### Model Description
-
-#### Convective Electric Baseboard Heater Inputs
-
-Like many other HVAC components, the convective-only electric baseboard model requires a unique identifying name and an availability schedule.  The availability schedule defines the availability of the unit for providing condition to the space.
-
-The input also requires a capacity and efficiency for the unit.  While the efficiency is a required input that defaults to unity, the capacity can be chosen to be auto-sized by EnergyPlus.
-
-#### Simulation and Control
-
-When the unit is available and there is a heating load within a space, the electric baseboard unit will meet the entire remaining provided that it has enough capacity to do so.  The energy consumption of the baseboard heat is calculated using the user-supplied efficiency and the current load on the baseboard unit as follows:
-
-<div>$$Energ{y_{electric}} = {{Heatin{g_{baseboard}}} \mathord{\left/ {\vphantom {{Heatin{g_{baseboard}}} {Efficiency}}} \right. } {Efficiency}}$$</div>
-
-If the unit was scheduled off or there is no heating load for the zone, then there will be no convection from the unit.  The model assumes no heat storage in the baseboard unit itself and thus no residual heat transfer in future system time steps due to heat storage in the metal of the baseboard unit.
-
-#### References
-
-No specific reference.  Refer to the ASHRAE Handbook series for general information on different system types as needed.
-
-### Hot Water Baseboard Heater with Radiation and Convection
-
-#### Overview
-
-The water baseboard heater model is intended to calculate the mass flow rate of the water by determining the actual system impact not only to the surrounding air via convection but also to the surfaces and people via radiation. The actual system impact by the heater in the zone is the sum of the additional convective heat transfer from the surfaces to the zone air after they have been heated as well as radiant heat transferred to people and the convective heat transfer to the zone. This actual convective power tries to meet any remaining heating requirement in the zone. The model thus improves the accuracy of thermal comfort predictions and system responses.
-
-The radiant components are calculated to interact with the surfaces in the zone through the radiant distribution fractions. Heat is also delivered to the space via convection. The baseboard heater is supplied with hot water from the primary system which is circulated through the inside of a finned tube within the space. This could also be used to model a hot water radiator (convector in the UK). Heat is transferred from the water inside the pipe, through the tube and fins. It is also not only convected to the surrounding air but also radiated to the surfaces within the space. The user is allowed to specify the percentage of radiant heat from the heater to the surfaces. In addition, the user is allowed the ability to define what fraction of radiation leaving the heater is incident directly on a person within the zone for thermal comfort purposes. This amount of heat is then used in the thermal comfort models as the high temperature radiant heater model.
-
-This model calculates the UA values using the log mean temperature difference (LMTD) method. The calculation is based on standard conditions of both fluids obtained in a rating document or manufacturer’s literature. Overall energy balances to the hot water and air handle the heat exchange between the water loop and the zone air. Once the UA for the baseboard heater has been determined, the model employs an effectiveness-NTU heat exchanger method to determine the heat transfer between the water and zone air. This is necessary because during the simulation only the inlet water and “inlet air� (assumed to be zone air) temperatures are known. As a result, the effectiveness-NTU heat exchanger methodology is suited to determine the performance of the system during the simulation.
-
-#### Model Description
-
-#### Water Baseboard Heater Inputs
-
-Like many other HVAC components, the water baseboard model requires a unique identifying name, an available schedule, and water inlet and outlet nodes. These define the availability of the unit for providing conditions to the space and the node connections that relate to the primary system. For the calculation of the UA value of the unit, standard conditions of both fluids are necessary. The user can specifies such standard conditions from manufacturers’ information such as I=B=R rating document. The user provides the rated capacity, average water temperature, water mass flow rate, and standard inlet air temperature. However, the model also has the ability to autosize the rated capacity, which allows the user simulate and design any baseboard units when manufacturer’s data is unavailable.
-
-The UA value corresponds to the convective heat transfer from the water to the tube, the conduction through the tube and fin material, the natural convection from the tube/fins to the zone air, and radiation to the surfaces. In addition, a convergence tolerance is requested of the user to help define the ability of the local controls to tightly control the system output. In almost all cases, the user should simply accept the default value for the convergence tolerance unless engaged in an expert study of controls logic in EnergyPlus.
-
-Many of the inputs for the radiant heat calculation are the same as the high temperature radiant heater model. User inputs of the fraction radiant and of the fraction of radiant energy incident both on people and on surfaces are required to calculate radiant energy distribution from the heater to the people and surfaces. The sum of radiant energy of these distribution fractions must sum to unity, and each water baseboard heater is allowed to distribute energy to up to 20 surfaces.
-
-#### Simulation and Control
-
-The simulation of the main algorithm of this water baseboard model with radiation and convection is similar to the convection-only baseboard model. However, this model determines the UA value of the unit based on rated heating capacities available in the manufacturer’s literature. Almost all baseboards or radiators are rated under standard conditions such as water flow rate, inlet air temperature and average water temperature. Those standard conditions should thus be obtained from manufacturers’ information. The model then determines the UA value of the unit, employing the log mean temperature difference (LMTD) method so that the heating output from the heater can be determined more correctly than other models.
-
-This model initializes all the conditions at the inlet node such as mass flow rates, temperatures, and specific heat capacities. It calculates the UA value once from standard conditions of the air and water during initialization and it is kept throughout the simulation of the unit.
-
-In case that the user has manufacturer’s information regarding the rated capacity, the rated water flow rate, and the rated average water temperature, standard conditions such as the rated heating capacity, *q<sub>std</sub>*, average water temperature, <span>\({T_{w,avg}}\)</span>, and water mass flow rate, <span>\(\dot m{}_w\)</span>, are known from the user inputs. The standard water inlet temperature, <span>\({T_{w,in}}\)</span>, and outlet temperature, <span>\({T_{w,out}}\)</span>, are thus obtained from expressions
-
-<div>$${T_{w,in}} = \frac{{{q_{std}}}}{{2\dot m{}_w{c_{p,w}}}} + {T_{w,avg}}$$</div>
-
-<div>$${T_{w,out}} = 2{T_{w,avg}} - {T_{w,in}}$$</div>
-
-where <span>\({c_{p,w}}\)</span> is the specific heat capacity of the water.
-
-The model then assumes the air mass flow rate is given by the following expression: 
-
-<div>$${\dot m_{a,std}} = {0.0062 + .0000275 \dot Q_{design}}$$<div>
-
-Since the inlet air temperature, <span>\({T_{a,in}}\)</span>, of 18°C and the heating capacity of the unit, i.e. rated capacity, are known, the outlet air temperature, <span>\({T_{a,out}}\)</span>, can be obtained from expression
-
-<div>$${T_{a,out}} = \frac{{{q_{std}}}}{{\dot m_{a,std}{c_{p,a}}}} + {T_{a,in}}$$</div>
-
-where <span>\({c_{p,a}}\)</span> is the specific heat capacity of the air.
-
-All temperatures at each node are now known. The mean temperature difference, <span>\(\Delta {T_{lm}}\)</span>, is thus obtained from the following expressions:
-
-<div>$$\Delta {T_1} = {T_{w,in}} - {T_{a,out}}$$</div>
-
-<div>$$\Delta {T_2} = {T_{w,out}} - {T_{a,in}}$$</div>
-
-<div>$$\Delta {T_{lm}} = \frac{{\Delta {T_1} - \Delta {T_2}}}{{\log \left( {\frac{{\Delta {T_1}}}{{\Delta {T_2}}}} \right)}}$$</div>
-
-The UA value of the unit is thus
-
-<div>$$UA = \frac{{{q_{std}}}}{{\Delta {T_{lm}}}}$$</div>
-
-The model allows the user requests to autosize the rated capacity when the user does not know a particular baseboard unit. It also has the ability to perform parametric study to design the unit based on the design heating load in the zone. The user is also able to modify both rated average water temperature and rated water mass flow rate when manufactures’ information is available while the model assumes the default values for both fields if unavailable.
-
-In case that the user requests autosizing the rated capacity, the model employs the design heating load and design water mass flow rate in the zone, so that the standard water inlet and outlet temperatures are estimated as
-
-<div>$${T_{w,in}} = \frac{{{q_{design}}}}{{2\dot m{}_{w,design}{c_{p,w}}}} + {T_{w,avg}}$$</div>
-
-<div>$${T_{w,out}} = 2{T_{w,avg}} - {T_{w,in}}$$</div>
-
-where <span>\({q_{design}}\)</span> is the design heating load estimated by EnergyPlus in the zone.
-
-Similarly, the model estimates the air outlet temperature using the air mass flow rate calculated above:
-
-<div>$${T_{a,out}} = \frac{{{q_{design}}}}{{\dot m_{a,std} {c_{p,a}}}} + {T_{a,in}}$$</div>
-
-Temperatures at the nodes are now known and the UA value is determined in the same fashion as the previous case.
-
-Once the UA value is determined, the model employs an effectiveness-NTU heat exchanger method to determine the heat transfer between the water and the zone air as convection-only model does (see “Hot Water Baseboard Heater with Only Convection� model). During this calculation the air mass flow rate is proportioned to the water mass flow rate:
-
-<div>$${\dot m_a} = {{\dot m_{a,std}} \frac{\dot m_w}{\dot m_{w,max}}}$$<div>
-
-The model then determines the radiant heat addition by
-
-<div>$${q_{rad}} = q \cdot Fra{c_{rad}}$$</div>
-
-where *q* is the total heating capacity of the heater and *Frac<sub>rad</sub>* is the user-defined fraction.
-
-The model now distributes the radiant heat additions to the appropriate surfaces, people for thermal comfort purpose, and the air in the zone. The surface heat balances are then recalculated to determine all heat sources or sinks for radiant systems in the zone. It is assumed that the radiant heat incident on people in the zone is converted to convection to the zone so that the zone heat balance includes this amount of heat which will be lost (see High Temperature Radiant Heater Model). The load met, the actual convective system impact, for the baseboard heater, *q<sub>req</sub>*, is therefore determined as
-
-<div>$${q_{req}} = ({q_{surf,c}} - {q_{surf,z}}) + {q_{conv}} + {q_{people}}$$</div>
-
-where *q<sub>surf,c</sub>*  is convection from the surfaces to the air in the zone with radiant systems; *q<sub>surf,z</sub>* is zero source convection from the surfaces when radiant systems are unavailable; *q<sub>conv</sub>* is the convective heat transfer from the heater to the zone air; and *q<sub>people</sub>* is radiant heat to the people.
-
-The radiant heat simulation in the water baseboard heater is very similar to the high temperature radiant system model. The controls are the same as shown in Figure 271.  Variable Flow Low Temperature Radiant System Controls.  After all system time steps have been simulated, an “average� zone heat balance calculation is done (similar to the radiant systems). If the unit was scheduled off or there is no water flow rate through the baseboard unit, then, there will be no heat transfer from the unit. The model assumes no heat storage in the unit itself and thus no residual heat transfer in future system time steps due to heat storage in the water or metal of the unit.
-
-#### References
-
-I=B=R Ratings for Boilers. 2009. Baseboard Radiation, Finned Tube (Commercial) Radiation, and Indirect Fired Water Heaters, January 2009 Edition
-
-Incropera and DeWitt. Fundamentals of Heat and Mass Transfer, Chapter 11.3 and 11.4, eq. 11.15, 11.17, and 11.33.
-
-Li Lianzhong and M. Zaheeruddin. 2006. Dynamic modeling and simulation of a room with hot water baseboard heater, International Journal of Energy Research; 30, pp. 427–445
-
-Electric Baseboard Heater with Radiation and Convection
--------------------------------------------------------
-
-### Overview
-
-The input object ZoneHVAC:Baseboard:RadiantConvective:Electric provides a model for electric baseboard heaters that include both convective and radiant heat addition to a space from a baseboard heater. The radiant heat transfer to people as well as surfaces within a space is determined in the same fashion as both hot water and steam baseboard heater with radiation and convection models. The electric baseboard heater transfers energy via electric resistance heating. Radiant heat calculated by the user-defined fraction from the heating capacity of a baseboard unit impacts the surface heat balances and thermal comfort of occupants in a space. EnergyPlus then assumes that the remaining convective gains from the unit are evenly spread throughout the space thus having an immediate impact on the zone air heat balance which is used to calculate the mean air temperature (MAT) within the space.
-
-### Model Description
-
-#### Convective Electric Baseboard Heater Inputs
-
-Like many other HVAC components, the electric baseboard model requires a unique identifying name and an availability schedule. The availability schedule defines the availability of the unit for providing condition to the space. The input also requires a capacity and efficiency for the unit. While the efficiency is a required input that defaults to unity, the capacity can be chosen to be autosized by EnergyPlus.
-
-All inputs for the radiant heat calculation are the same as the water and steam baseboard heater with radiation and convection models in EnergyPlus. Users are required to input fractions that specify total radiant heat directly delivered to surfaces as well as people in a space. The sum of radiant energy of these distribution fractions must sum to unity, and each baseboard heater is allowed to distribute energy to up to 20 surfaces.
-
-#### Simulation and Control
-
-When the unit is available and there is a heating load within a space, the electric baseboard unit will meet the entire remaining provided that it has enough capacity to do so. The model sets the heating capacity of a baseboard unit to the remaining heating load in the space, which any primary heating system does not meet. Note that it is set to the maximum nominal capacity of the unit, if a heating load in a space is greater than the maximum. The model then determines the radiant heat source through the simulation as
-
-<div>$${q_{rad}} = q \cdot Fra{c_{rad}}$$</div>
-
-where *q<sub>rad</sub>* is the total radiant heating capacity, *q* is the heating capacity of the unit, and *Frac<sub>rad</sub>* is the user-defined fraction for the radiation. The radiant heat additions to people and surfaces are thus
-
-<div>$${q_{people}} = {q_{rad}} \cdot Fra{c_{people}}$$</div>
-
-<div>$${q_{surface}} = \sum {{q_{rad}} \cdot Fra{c_{surface,i}}} $$</div>
-
-where *q<sub>people</sub>* is the radiant heat transfer to people, *q<sub>surface</sub>* is the heat radiated to surfaces, *Frac<sub>people</sub>* is the fraction of the heat radiated to people, and *Frac<sub>surface,i</sub>* is the fraction of the heat radiated to surface i.
-
-Once the radiant heat sources are determined, the model distributes the radiant heat sources to the appropriate surfaces and people for thermal comfort purposes, and EnergyPlus recalculates the surface heat balances. The model then determines differences in convection from the surfaces to the air before and after the surface heat balances are impacted due to radiant heat additions from the unit. Note that the model converts the radiant heat transfer to people to convective energy so that the heat balance includes this amount of energy, which will be lost (see High Temperature Radiant Heater Model). The model calculates the actual convective system impact of an electric baseboard heater unit as
-
-<div>$${q_{req}} = ({q_{surf,c}} - {q_{surf,z}}) + {q_{conv}} + {q_{people}}$$</div>
-
-where *q<sub>req</sub>* is the actual heating load that the unit should meet, *q<sub>surf,c</sub>* is the convection from the surfaces to the air after the radiant heat distribution, *q<sub>surf,z</sub>* is the convection from the surfaces to the air before the radiant heat distribution, and *q<sub>conv</sub>* is the convective heat transfer to the air.
-
-The energy consumption of the baseboard heater is calculated using the user-supplied efficiency and the actual convective system impact calculated as
-
-<div>$${Q_{elec}} = \frac{q}{\eta }$$</div>
-
-where *Q<sub>elec</sub>* is the energy consumption and ***η*** is the efficiency of the unit.
-
-If the unit was scheduled off or there is no heating load for the zone, then there will be no heat transfer from the unit. The model assumes no heat storage in the baseboard unit itself and thus no residual heat transfer in future system time steps due to heat storage in the metal of the baseboard unit.
-
-#### References
-
-No specific reference. Refer to the ASHRAE Handbook series for general information on different system types as needed.
-
-### Steam Baseboard Heater with Radiation and Convection
-
-#### Overview
-
-The steam baseboard heater model is intended to calculate the mass flow rate of the steam to meet remaining heating demand by determining the actual system impact not only to the surrounding air via convection but also to the surfaces and people via radiation. The actual system impact by the heater is the sum of the additional convective heat transfer from the surfaces to the zone air after they have been heated as well as radiant heat transferred to people and the convective heat transfer to the zone. This actual convective power tries to meet any remaining heating requirement in the zone. The model thus improves the accuracy of thermal comfort predictions and system responses. The calculation of radiant heat addition is the same as that of water baseboard heater model in EnergyPlus.
-
-This model determines the heating capacity from the sum of the latent heat transfer and sensible cooling of water as current steam coil model in EnergyPlus does. Overall energy balances to the steam and air handle the heat exchange between the steam loop and the zone air. The mass flow rate of steam is determined based on the heating demand in the zone. The model requests the user input the desired degree of subcooling so that it determines the heating rate from the heater due to the cooling of the condensate. The user input is also used to determine the condensate outlet conditions.
-
-#### Model Description
-
-#### Steam Baseboard Heater Inputs
-
-The steam baseboard model requires a unique identifying name, an available schedule, and steam inlet and outlet nodes. These define the availability of the unit for providing conditions to the space and the node connections that relate to the primary system. It also requires the desired degree of subcooling to calculate the heating capacity and temperature of the condensate. A maximum design flow rate is required, and the user can request this parameter to be auto-sized by EnergyPlus. In addition, a convergence tolerance is requested of the user to help define the ability of the local controls to tightly control the system output. In almost all cases, the user should simply accept the default value for the convergence tolerance unless engaged in an expert study of controls logic in EnergyPlus.
-
-All of the inputs for the radiant heat calculation are the same as the water baseboard heater model in EnergyPlus. User inputs of the radiant fraction and of the fraction of radiant energy incident both on people and on surfaces are required to calculate radiant energy distribution from the heater to the people and surfaces. The sum of radiant energy of these distribution fractions must sum to unity, and each steam baseboard heater is allowed to distribute energy to up to 20 surfaces.
-
-#### Simulation and Control
-
-The simulation of the main algorithm of this steam baseboard model with radiation and convection is similar to steam coil model in EnergyPlus while the simulation of radiant component is the same as the water baseboard models. This model initializes all conditions at the inlet node such as mass flow rate, temperature, enthalpy, and humidity ratio. The model then determines the heating capacity of steam baseboard, *q*, as
-
-<div>$$q = {\dot m_5}({h_{fg}} + {c_{pw}}\Delta t)$$</div>
-
-where <span>\({\dot m_s}\)</span>is the mass flow rate of steam in kg/s, <span>\({h_{fg}}\)</span>is the heat of vaporization of steam in J/kg, <span>\({c_{pw}}\)</span>is the specific heat of water in J/kg.K, and <span>\(\Delta t\)</span> is the degree of subcooling in degree C.
-
-The outlet steam temperature is thus
-
-<div>$${T_{s,out}} = {T_{s,in}} - \Delta t$$</div>
-
-Once the heating capacity of the unit is determined, the model determines the radiant heat addition by
-
-<div>$${q_{rad}} = q \cdot Fra{c_{rad}}$$</div>
-
-where *q* is the total heating capacity of the heater and *Frac<sub>rad</sub>* is the user-defined fraction.
-
-The model now distributes the radiant heat additions to the appropriate surfaces, people for thermal comfort purpose, and the air in the zone. The surface heat balances are then recalculated to determine all heat sources or sinks for radiant systems in the zone. It is assumed that the radiant heat incident on people in the zone is converted to convection to the zone so that the zone heat balance includes this amount of heat which will be lost (see High Temperature Radiant Heater Model). The load met, the actual convective system impact, for the baseboard heater, *q<sub>req</sub>*, is therefore determined as
-
-<div>$${q_{req}} = ({q_{surf,c}} - {q_{surf,z}}) + {q_{conv}} + {q_{people}}$$</div>
-
-where *q<sub>surf,c </sub>* is convection from the surfaces to the air in the zone with radiant systems; *q<sub>surf,z</sub>* is zero source convection from the surfaces when radiant systems are unavailable; *q<sub>conv</sub>* is the convective heat transfer from the heater to the zone air; and *q<sub>people</sub>* is radiant heat to the people.
-
-The simulation of radiant heat addition is the same as the water baseboard heater model. The controls are the same as shown in Figure 271.  Variable Flow Low Temperature Radiant System Controls. After all system time steps have been simulated, an “average� zone heat balance calculation is done (similar to the high temperature radiant system). If the unit was scheduled off or there is no steam flow rate through the baseboard unit, then, there will be no heat transfer from the unit. The model assumes no heat storage in the unit itself and thus no residual heat transfer in future system time steps due to heat storage in the steam or metal of the unit.
-
-#### References
-
-No specific reference.  Refer to the ASHRAE Handbook series for general information on different system types as needed.
-
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-<!--RemoveStart-->
-Simulation Models – Encyclopedic Reference 
-==========================================
-
-The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of “Heat Balance�, “HVAC�, and “Plant�.  With the integrated solution, these designations signify where the effects of these models have their first impacts.
-
-Main Sections:
-
-* [Cooling Towers and Evaporative Fluid Coolers](#TowersAndCoolers)
-* [Demand Controlled Ventilation](#DCV)
-* [Evap Coolers](#EvapCoolers)
-* [Air System Fans](#Fans)
-* [Air System Component Groups](#AirComponentGroups)
-* [VRF Systems](#VRF)
-* [Heat Exchangers](#HX)
-* [Humidifiers](#Humidifiers)
-<!--RemoveEnd-->
-
-Cooling Towers and Evaporative Fluid Coolers <a name="TowersAndCoolers"></a>
---------------------------------------------
-
-### One, Two, and Variable Speed Cooling Towers and Evaporative Fluid Coolers
-
-#### Overview
-
-The input objects CoolingTower:SingleSpeed, CoolingTower:TwoSpeed, and CoolingTower:VariableSpeed:Merkel provide models for single-speed, two-speed, and variable-speed cooling towers that are based on Merkel’s theory (Merkel 1925), which is also the basis for the tower model included in ASHRAE’s HVAC1 Toolkit for primary HVAC system energy calculations (ASHRAE 1999, Bourdouxhe et al. 1994). Cooling tower performance is modeled using effectiveness-NTU relationships for counterflow heat exchangers. The model can be used to simulate the performance of both single speed, two speed, and variable speed mechanical-draft cooling towers. The model will also account for tower performance in the “free convection� regime, when the tower fan is off but the water pump remains on. For part-load operation, the model assumes a simple linear interpolation between two steady-state regimes without accounting for any cycling losses.
-
-For single speed cooling towers, the capacity control can be fan cycling or fluid bypass. In fluid bypass mode, portion of the water goes through the tower media and gets cooled while the remaining water flow gets bypassed, two water flows then mix together trying to meet the tower exiting water setpoint temperature. In both the free convection cooling when fan is off and normal cooling when fan is on for the entire time step, if the tower exiting water temperature is lower than the setpoint, the tower operates in fluid bypass mode. The model determines the fluid bypass fraction by iterations until the mixed water meets the tower exiting water temperature setpoint. In the fluid bypass mode, except the free convection, the tower fan runs at full speed for the entire time step. The maximum amount of tower water that can be bypassed is bounded by the freezing point of the tower water – the tower exiting water temperature cannot be lower than the freezing setpoint.
-
-Evaporative fluid coolers are modeled very similar to cooling towers. The main difference between the two is in the “Performance input method� input field. Cooling tower has two choices for this field namely “UFactorTimesAreaAndDesignWaterFlowRate� and “Nominal capacity�. The nominal capacity is specified for the standard conditions i.e. entering water at 35C (95F), leaving water at 29.44C (85F), entering air at 25.56C (78F) wet-bulb temperature and 35C (95F) dry-bulb temperature. On the other hand evaporative fluid cooler has three choices for “Performance input method� which are “UFactorTimesAreaAndDesignWaterFlowRate�, “StandardDesignCapacity� and “UserSpecifiedDesignCapacity�. First method is same for both tower and fluid cooler. Standard design capacity is specified for the same conditions which are used to specify nominal capacity for tower as described above. If the capacity of fluid cooler for conditions other than the standard ones is known then UserSpecifiedDesignCapacity method should be used. In this case, the conditions for which the fluid cooler capacity is known i.e. entering water temperature, entering air temperature and entering air wet bulb temperature must be specified in the input. To calculate evaporation loss for fluid cooler, spray water flow rate which is different than the process fluid flow rate must be specified for all the performance input methods. This is not required for cooling tower because cooled fluid i.e. water is in direct contact with the air so the water loss is calculated by using cooled fluid flow rate only. Unlike cooling tower, evaporative fluid cooler model does not account for free convection.
-
-Cooling tower model is described below which holds equally good for evaporative fluid cooler. The differences are mentioned whenever required.
-
-#### Model Description
-
-Based on Merkel’s theory, the steady-state total heat transfer between the air and water entering the tower can be defined by the following equation:
-
-<div>$$d{\dot Q_{total}} = \frac{{UdA}}{{cp}}\left( {{h_s} - {h_a}} \right)$$</div>
-
-where
-
-*h<sub>s</sub>* = enthalpy of saturated air at the wetted-surface temperature, J/kg
-
-*h<sub>a</sub>* = enthalpy of air in the free stream, J/kg
-
-*c<sub>p</sub>* = specific heat of moist air, J/kg-<sup>o</sup>C
-
-*U* = cooling tower overall heat transfer coefficient, W/m<sup>2</sup>- <sup>o</sup>C
-
-*A* = heat transfer surface area, m<sup>2</sup>
-
-Equation is based on several assumptions:
-
-n air and water vapor behave as ideal gases
-
-n the effect of water evaporation is neglected
-
-n fan heat is neglected
-
-n the interfacial air film is assumed to be saturated
-
-n the Lewis number is equal to 1
-
-In this model, it is also assumed that the moist air enthalpy is solely a function of the wet-bulb temperature and that the moist air can be treated as an equivalent ideal gas with its mean specific heat defined by the following equation:
-
-<div>$$\bar cpe = \frac{{\Delta h}}{{\Delta {T_{wb}}}}$$</div>
-
-where
-
-Δ*h* = enthalpy difference between the air entering and leaving the tower, J/kg
-
-Δ*T<sub>wb</sub>*= wet-bulb temperature difference between the air entering and leaving the tower, <sup>o</sup>C
-
-Since the liquid side conductance is much greater than the gas side conductance, the wetted-surface temperature is assumed to be equal to the water temperature. Based on this assumption and equations and , the expression for total heat transfer becomes:
-
-<div>$$d{\dot Q_{total}} = UedA\left( {{T_w} - {T_{wb}}} \right)$$</div>
-
-where
-
-<div>$$Ue = \frac{{U\,\bar cpe}}{{cp}}$$</div>
-
-*T<sub>wb</sub>* = wet-bulb temperature of the air, <sup>o</sup>C
-
-*T<sub>w</sub>* = temperature of the water, <sup>o</sup>C
-
-An energy balance on the water and air sides of the air/water interface yields the following equations:
-
-<div>$$d{\dot Q_{total}} = {\dot m_w}cpw\,\,\,dTw$$</div>
-
-<div>$$d{\dot Q_{total}} = {\dot m_a}\bar cpe\,\,\,dTwb$$</div>
-
-where
-
-<span>\({\dot m_w}\)</span> = mass flow rate of water, kg/s
-
-<span>\({\dot m_a}\)</span> = mass flow rate of air, kg/s
-
-Assuming that the heat capacity rate (<span>\(\dot mcp\)</span>) for the cooling tower water is less than that for the air,the effectiveness of the cooling tower can be defined by analogy to the effectiveness of a simple heat exchanger:
-
-<div>$$\varepsilon  = \frac{{{T_{win}} - {T_{wout}}}}{{{T_{win}} - {T_{wbin}}}}$$</div>
-
-where
-
-*ε* = heat exchanger effectiveness
-
-*T<sub>win</sub>* = inlet water temperature, <sup>o</sup>C
-
-*T<sub>wout</sub>* = outlet water temperature, <sup>o</sup>C
-
-*T<sub>wbin</sub>* = wet-bulb temperature of the inlet air, <sup>o</sup>C
-
-Combining equations , , and and integrating over the entire heat transfer surface area, and combining the result with equation provides the following expression for cooling tower effectiveness:
-
-<div>$$\varepsilon \,\, = \,\frac{{1 - \exp \left\{ { - NTU\left[ {1 - \left( {\frac{{{{\dot C}_w}}}{{{{\dot C}_a}}}} \right)} \right]} \right\}}}{{1 - \left( {\frac{{{{\dot C}_w}}}{{{{\dot C}_a}}}} \right)\exp \left\{ { - NTU\left[ {1 - \left( {\frac{{{{\dot C}_w}}}{{{{\dot C}_a}}}} \right)} \right]} \right\}}}$$</div>
-
-where
-
-<span>\({\dot C_w} = {\dot m_w}c{p_w}\)</span> and <span>\({\dot C_a} = {\dot m_a}\bar c{p_e}\)</span>
-
-<div>$$NTU = Number\,of\,Transfer\,Units = \frac{{UAe}}{{{{\dot C}_w}}}$$</div>
-
-This equation is identical to the expression for effectiveness of an indirect contact (i.e., fluids separated by a solid wall) counterflow heat exchanger (Incropera and DeWitt 1981). Therefore, the cooling tower can be modeled, in the steady-state regime, by an equivalent counterflow heat exchanger as shown in the following figure.
-
-![](media/image4542.png)
-
-Figure 194. Cooling Tower Schematic
-
-The first fluid is water and the second fluid is an equivalent fluid entering the heat exchanger at temperature T<sub>wbin</sub> and specific heat <span>\(\bar cpe\)</span>. The heat exchanger is characterized by a single parameter, its overall heat transfer coefficient-area product UA<sub>e</sub>. The actual cooling tower heat transfer coefficient-area product is related to UA<sub>e</sub> by the following expression:
-
-<div>$$UA = UAe\frac{{cp}}{{\bar cpe}}$$</div>
-
-This heat transfer coefficient-area product is assumed to be a function of the air mass flow rate only and can be estimated from laboratory test results or manufacturers’ catalog data.
-
-The model for the variable speed Merkel tower also includes Scheier’s modifications.  Scheier has extended the Merkel model to also include terms that adjust UA with three factors that model how UA values change when the tower is operating away from its rated conditions.  The first factor, <span>\({f_{UA,wetbulb}}\)</span>, adjusts UA for the current outdoor wetbulb temperature.  The user enters a performance curve or lookup table that is a function of one independent variable.  The independent variable is the difference between the design wetbulb temperature and the current wetbulb temperature, in degrees Celsius.
-
-<div>$${f_{UA,wetbulb}} = func\left( {\left( {{T_{des,wetbulb}} - {T_{current,wetbulb}}} \right)} \right)$$</div>
-
-The second factor, <span>\({f_{UA,airflow}}\)</span>, adjusts UA for the current air flow rate.  The user enters a performance curve or lookup table that is a function of one independent variable.  The independent variable is the ratio of the current air flow rate to the design air flow rate at full speed.
-
-<div>$${f_{UA,airflow}} = func\left( {AirFlowRatio} \right)$$</div>
-
-The third factor, <span>\({f_{UA,waterflow}}\)</span>, adjusts UA for the current water flow rate.  The user enters a performance curve or lookup table that is a function of one independent variable.  The independent variable is the ratio of the current water flow rate to the design water flow rate.
-
-<div>$${f_{UA,waterflow}} = func\left( {WaterFlowRatio} \right)$$</div>
-
-Then the UA value at any given time is calculated using
-
-<div>$$U{A_e} = U{A_{design}} \bullet {f_{UA,wetbulb}} \bullet {f_{UA,airflow}} \bullet {f_{UA,waterflow}}$$</div>
-
-#### Method for Calculating Steady-State Exiting Water Temperature
-
-The objective of the cooling tower model is to predict the exiting water temperature and the fan power required to meet the exiting water setpoint temperature. Since only the inlet air and inlet water temperatures are known at any simulation time step, an iterative procedure is required to determine the exiting fluid temperatures using the equations defined in the previous section. In the case of the EnergyPlus model, the iterations are performed to determine the exiting wet-bulb temperature of the air. The exiting water temperature is then calculated based on an energy balance that assumes that the energy absorbed by the air is equivalent to the energy removed from the water. The procedure for calculating the steady-state, exiting air wet-bulb temperature is outlined below.
-
-As explained previously, it is assumed that the moist air enthalpy can be defined by the wet-bulb temperature alone. Therefore, the first step in the procedure is to calculate the enthalpy of moist air entering the cooling tower based on the ambient wet-bulb temperature from the weather file. Since an iterative solution is required, a first guess of the outlet air wet-bulb temperature is then made and the enthalpy of this estimated outlet air wet-bulb temperature is calculated. Based on these inlet and outlet air conditions, the mean specific heat of the air is calculated based on equation , repeated here:
-
-<div>$$\bar cpe = \frac{{\Delta h}}{{\Delta Twb}}$$</div>
-
-With the overall heat transfer coefficient-area product for the cooling tower entered by the user, the effective heat transfer coefficient-area product is calculated by rearranging equation :
-
-<div>$$UAe = UA\frac{{\bar cpe}}{{cp}}$$</div>
-
-With <span>\(\bar cpe\)</span> and <span>\(UAe\)</span> known, the effectiveness of the heat exchanger is then calculated:
-
-<div>$$\varepsilon \,\, = \,\frac{{1 - \exp \left\{ { - NTU\left[ {1 - \left( {\frac{{{{\dot C}_{\min }}}}{{{{\dot C}_{\max }}}}} \right)} \right]} \right\}}}{{1 - \left( {\frac{{{{\dot C}_{\min }}}}{{{{\dot C}_{\max }}}}} \right)\exp \left\{ { - NTU\left[ {1 - \left( {\frac{{{{\dot C}_{\min }}}}{{{{\dot C}_{\max }}}}} \right)} \right]} \right\}}}$$</div>
-
-where
-
-<span>\({\dot C_{\min }} = \,Minimum\,({\dot C_w},\,{\dot C_a})\)</span> and <span>\({\dot C_{\max }} = \,Maximum\,({\dot C_w},\,{\dot C_a})\)</span>
-
-<span>\({\dot C_w} = {\dot m_w}c{p_w}\)</span> and <span>\({\dot C_a} = {\dot m_a}\bar cpe\)</span>
-
-<div>$$NTU = Number\,of\,Transfer\,Units = \frac{{UAe}}{{{{\dot C}_{\min }}}}$$</div>
-
-The heat transfer rate is then calculated as follows:
-
-<div>$$\dot Qtotal = \,\varepsilon \,{\dot C_{\min }}\left( {Twin\, - \,Twbin} \right)$$</div>
-
-The outlet air wet-bulb temperature is then recalculated:
-
-<div>$${T_{wbout}} = {T_{wbin}} + \frac{{{{\dot Q}_{total}}}}{{{{\dot C}_a}}}$$</div>
-
-The iterative process of calculating <span>\({T_{wbout}}\)</span> continues until convergence is reached.
-
-Finally, the outlet water temperature is calculated as follows:
-
-<div>$${T_{wout}} = {T_{win}} + \frac{{{{\dot Q}_{total}}}}{{{{\dot C}_w}}}$$</div>
-
-#### Calculating the Actual Exiting Water Temperature and Fan Power
-
-The previous section describes the methodology used for calculating the steady-state temperature of the water leaving the cooling tower. This methodology is used to calculate the exiting water temperature in the free convection regime (water pump on, tower fan off) and with the tower fan operating (including low and high fan speed for the two-speed tower). The exiting water temperature calculations use the fluid flow rates (water and air) and the UA-values entered by the user for each regime.
-
-The cooling tower model seeks to maintain the temperature of the water exiting the cooling tower at (or below) a setpoint. The model obtains the target temperature setpoint from the setpoints placed on either the tower outlet node or the loop’s overall setpoint node (typically set to the supply side outlet node). The model checks to see if the outlet node has a setpoint placed on it and uses that if it does.  If the outlet node does not have a temperature setpoint then the model uses the loop-level outlet node specified in the input field called Loop Temperature Setpoint Node Name in the PlantLoop or CondenserLoop object. The model first checks to determine the impact of “free convection�, if specified by the user, on the tower exiting water temperature. If free convection is not specified by the user, then the exiting water temperature is initially set equal to the entering tower water temperature. If the user specifies “free convection� and the steady-state exiting water temperature based on “free convection� is at or below the setpoint, then the tower fan is not turned on.
-
-If the exiting water temperature remains above the setpoint after “free convection� is modeled, then the tower fan is turned on to reduce the exiting water temperature to the setpoint. The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (e.g., tower fan on for the entire simulation time step and tower fan off for the entire simulation time step). Cyclic losses are not taken into account.
-
-The fraction of time that the tower fan must operate is calculated based on the following equation:
-
-<div>$$\omega \,\, = \frac{{{T_{set}} - {T_{wout,off}}}}{{{T_{wout,on}} - {T_{wout,off}}}}$$</div>
-
-where
-
-<span>\({T_{set}}\)</span> = exiting water setpoint temperature, <sup>o</sup>C
-
-<span>\({T_{wout,off}}\)</span> = exiting water temperature with tower fan off, <sup>o</sup>C
-
-<span>\({T_{wout,on}}\)</span> = exiting water temperature with tower fan on, <sup>o</sup>C
-
-The average fan power for the simulation time step is calculated by multiplying <span>\(\omega \,\)</span>by the steady-state fan power specified by the user.
-
-The calculation method for the two-speed tower is similar to that for the single-speed tower example described above. The model first checks to see if “free convection� is specified and if the resulting exiting water temperature is below the setpoint temperature. If not, then the model calculates the steady-state exiting water temperature with the tower fan at low speed. If the exiting water temperature at low fan speed is below the setpoint temperature, then the average fan power is calculated based on the result of equation and the steady-state, low speed fan power specified by the user. If low-speed fan operation is unable to reduce the exiting water temperature below the setpoint, then the tower fan is increased to its high speed and the steady-state exiting water temperature is calculated. If this temperature is below the setpoint, then a modified version of equation is used to calculate runtime at high fan speed:
-
-<div>$$\omega \,\, = \frac{{{T_{set}} - {T_{wout,low}}}}{{{T_{wout,high}} - {T_{wout,low}}}}$$</div>
-
-where
-
-<span>\({T_{set}}\)</span> = exiting water setpoint temperature, <sup>o</sup>C
-
-<span>\({T_{wout,low}}\)</span> = exiting water temperature with tower fan at low speed, <sup>o</sup>C
-
-<span>\({T_{wout,high}}\)</span> = exiting water temperature with tower fan at high speed, <sup>o</sup>C
-
-The average fan power for the simulation time step is calculated for the two-speed cooling tower as follows:
-
-<div>$${P_{fan,avg}}\, = \,\omega \,({P_{fan,high}})\, + \,\left( {1 - \omega } \right)\left( {{P_{fan,low}}} \right)$$</div>
-
-The calculation method for the variable-speed Merkel/Scheier model is different from the one- and two-speed models.  Whereas the other towers are setpoint driven, the variable speed Merkel/Scheier model is driven by the load dispatched from the plant operation scheme, such as PlantEquipmentOperation:CoolingLoad.  The plant operation scheme provides the cooling tower model with a target load to meet and the tower is controlled to meet that load (as opposed to meeting a leaving setpoint).  This allows complex configurations with more than one cooling tower to be properly dispatched using all the features available in the various plant operation schemes.  The model first evaluates the load provided with the fans off using only free convection.  If the free convection mode meets or exceeds the target load then the tower runs in free convection mode.  The model then evaluates the load provided by running the fans at full speed.  If the full fan speed load provided is less than or equal to the target load then the tower runs at full speed.  The model then evaluates the load provided with the variable speed fan running at the minimum air speed ratio, which is a user input (default is 0.2).  If the minimum fan speed load provided meets or exceeds the target load, then tower runs at the minimum fan speed.  If the target load is between the load provided by minimum and maximum fans speeds, then the model solves for an airflow rate ratio that just meets the target load using Regula Falsi numerical method.  The variable speed Merkel/Scheier model does not model bypass and may provided excess cooling at times when running in free convection or at the minimum fan speed.  Fan power for the variable speed Merkel/Scheier model is then calculated from the airflow rate ratio using a design fan power and a performance curve or lookup table with one independent variable for the airflow ratio.
-
-<div>$${P_{fan}} = {P_{fan,des}} \bullet func\left( {AirFlowRatio} \right)$$</div>
-
-#### Tower Basin Heater
-
-The tower basin heater operates in the same manner as the variable speed cooling tower basin heater. Refer to the variable speed cooling tower basin heater description in the following section.
-
-#### Cooling Tower Makeup Water Usage
-
-The cooling tower makeup water usage is the same as the variable speed cooling tower makeup water usage. Refer to the variable speed cooling tower makeup water usage description in the following section.
-
-#### References
-
-Rosaler, Robert C. 1995. Standard Handbook of Plant Engineering, 2<sup>nd</sup> Ed. New York, NY: McGraw-Hill, pp. 6-36-37.
-
-### Variable Speed Cooling Towers Empirical Models
-
-#### Overview
-
-The input object CoolingTower:VariableSpeed provides models for variable speed towers that are based on empirical curve fits of manufacturer’s performance data or field measurements. The user specifies tower performance at design conditions, and empirical curves are used to determine the approach temperature and fan power at off-design conditions. The user defines tower performance by entering the inlet air wet-bulb temperature, tower range, and tower approach temperature at the design conditions. The corresponding water flow rate, air flow rate, and fan power must also be specified. The model will account for tower performance in the “free convection� regime, when the tower fan is off but the water pump remains on and heat transfer still occurs (albeit at a low level). Basin heater operation and makeup water usage (due to evaporation, drift, and blowdown) are also modeled.
-
-The cooling tower seeks to maintain the temperature of the water exiting the cooling tower at (or below) a setpoint. The setpoint temperature is defined by the setpoints placed on either the tower outlet node or the loop’s overall setpoint node (typically set to the supply side outlet node). The model checks to see if the outlet node has a setpoint placed on it and uses that if it does.  If the outlet node does not have a temperature setpoint then the model uses the loop-level outlet node specified in the input field called Loop Temperature Setpoint Node Name in the PlantLoop or CondenserLoop object. The model simulates the outlet water temperature in four successive steps:
-
-·        The model first determines the tower outlet water temperature with the tower fan operating at maximum speed. If the outlet water temperature is above the setpoint temperature, the fan runs at maximum speed.
-
-·        If the outlet water temperature with maximum fan speed is below the setpoint temperature, then the model next determines the impact of “free convection� (water flowing through tower with fan off). If the exiting water temperature based on “free convection� is at or below the setpoint, then the tower fan is not turned on.
-
-·        If the outlet water temperature remains above the setpoint after “free convection� is modeled, then the tower fan is turned on at the minimum fan speed (minimum air flow rate ratio) to reduce the leaving water temperature. If the outlet water temperature is below the setpoint at minimum fan speed, the tower fan is cycled on and off to maintain the outlet water setpoint temperature.
-
-·        If the outlet water temperature remains above the setpoint after minimum fan speed is modeled, then the tower fan is turned on and the model determines the required air flow rate and corresponding fan speed to meet the desired setpoint temperature.
-
-#### Model Description
-
-The variable speed tower model utilizes user-defined tower performance at design conditions along with empirical curves to determine tower heat rejection and fan power at off-design conditions. Basin heater operation and makeup water usage are also modeled based on user inputs, tower entering air conditions, and tower operation. The following sections describe how each of these tower performance areas is modeled.
-
-#### Tower Heat Rejection
-
-Heat rejection by the variable speed cooling tower is modeled based on the CoolTools correlation, YorkCalc correlation, or user-defined coefficients for either the CoolTools or YorkCalc correlations. These purely-empirical correlations model the tower approach temperature using a polynomial curve fit with a large number of terms and either three or four independent variables.
-
-The CoolTools correlation has 35 terms with four independent variables:
-
-    Approach =   Coeff(1)  +  Coeff(2)•FRair  +  Coeff(3)•(FRair)<sup>2</sup>  +
-
-Coeff(4)•(FRair)<sup>3</sup>  +  Coeff(5)•FRwater  +
-
-Coeff(6)•FRair•FRwater  +  Coeff(7)•(FRair)<sup>2</sup>•FRwater  +
-
-Coeff(8)•(FRwater)<sup>2</sup>  +  Coeff(9)•FRair•(FRwater)<sup>2</sup>  +
-
-Coeff(10)•(FRwater)<sup>3</sup>  +  Coeff(11)•Twb  +  Coeff(12)•FRair•Twb  +
-
-Coeff(13)•(FRair)<sup>2</sup>•Twb  +  Coeff(14)•FRwater•Twb  +
-
-Coeff(15)•FRair•FRwater•Twb  +  Coeff(16)•(FRwater)<sup>2</sup>•Twb  +
-
-Coeff(17)•(Twb)<sup>2</sup>  +  Coeff(18)•FRair•(Twb)<sup>2</sup>  +
-
-Coeff(19)•FRwater•(Twb)<sup>2</sup>  +  Coeff(20)•(Twb)<sup>3</sup>  +  Coeff(21)•Tr  +
-
-Coeff(22)•FRair•Tr  +  Coeff(23)•(FRair)<sup>2</sup>•Tr  +
-
-Coeff(24)•FRwater•Tr  +  Coeff(25)•FRair•FRwater•Tr  +
-
-Coeff(26)•(FRwater)<sup>2</sup>•Tr  +  Coeff(27)•Twb•Tr  +
-
-Coeff(28)•FRair•Twb•Tr  +  Coeff(29)•FRwater•Twb•Tr  +
-
-Coeff(30)•(Twb)<sup>2</sup>•Tr  +  Coeff(31)•(Tr)<sup>2</sup> + Coeff(32)•FRair•(Tr)<sup>2 </sup> +
-
-Coeff(33)•FRwater•(Tr)<sup>2 </sup> +  Coeff(34)•Twb•(Tr)<sup>2 </sup> +  Coeff(35)•(Tr)<sup>3</sup>
-
-where:
-
-Approach = approach temperature (<sup>o</sup>C) = outlet water temperature minus inlet air wet-bulb temperature
-
-FRair = air flow rate ratio (actual air flow rate divided by design air flow rate)
-
-FRwater = water flow rate ratio (actual water flow rate divided by design water flow rate)
-
-Tr = range temperature (<sup>o</sup>C) = inlet water temperature minus outlet water temperature
-
-Twb = inlet air wet-bulb temperature (<sup>o</sup>C)
-
-Coeff(\#) = correlation coefficients
-
-If the user selects Tower Model Type = CoolToolsCrossFlow, then the 35 coefficients derived for the CoolTools simulation model (Benton et al. 2002) are used and these coefficients are already defined within EnergyPlus as shown in Table 63. If the user specifies Tower Model Type = CoolToolsUserDefined, then the user must enter a CoolingTowerPerformance:CoolTools object to define the 35 coefficients that will be used by the CoolTools approach temperature correlation.
-
-Table 63. Approach Temperature Correlation Coefficients
-
-<table class="table table-striped">
-  <tr>
-    <th rowspan="2">Coefficient Number</th>
-    <th colspan="2">Coefficient Value</th>
-  </tr>
-  <tr>
-    <td>CoolTools</td>
-    <td>YorkCalc</td>
-  </tr>
-  <tr>
-    <td>Coeff(1)</td>
-    <td>0.52049709836241</td>
-    <td>-0.359741205</td>
-  </tr>
-  <tr>
-    <td>Coeff(2)</td>
-    <td>-10.617046395344</td>
-    <td>-0.055053608</td>
-  </tr>
-  <tr>
-    <td>Coeff(3)</td>
-    <td>10.7292974722538</td>
-    <td>0.0023850432</td>
-  </tr>
-  <tr>
-    <td>Coeff(4)</td>
-    <td>-2.74988377158227</td>
-    <td>0.173926877</td>
-  </tr>
-  <tr>
-    <td>Coeff(5)</td>
-    <td>4.73629943913743</td>
-    <td>-0.0248473764</td>
-  </tr>
-  <tr>
-    <td>Coeff(6)</td>
-    <td>-8.25759700874711</td>
-    <td>0.00048430224</td>
-  </tr>
-  <tr>
-    <td>Coeff(7)</td>
-    <td>1.57640938114136</td>
-    <td>-0.005589849456</td>
-  </tr>
-  <tr>
-    <td>Coeff(8)</td>
-    <td>6.51119643791324</td>
-    <td>0.0005770079712</td>
-  </tr>
-  <tr>
-    <td>Coeff(9)</td>
-    <td>1.50433525206692</td>
-    <td>-1.342427256E-05</td>
-  </tr>
-  <tr>
-    <td>Coeff(10)</td>
-    <td>-3.2888529287801</td>
-    <td>2.84765801111111</td>
-  </tr>
-  <tr>
-    <td>Coeff(11)</td>
-    <td>0.02577861453538</td>
-    <td>-0.121765149</td>
-  </tr>
-  <tr>
-    <td>Coeff(12)</td>
-    <td>0.18246428931525</td>
-    <td>0.0014599242</td>
-  </tr>
-  <tr>
-    <td>Coeff(13)</td>
-    <td>-0.08189472914009</td>
-    <td>1.680428651</td>
-  </tr>
-  <tr>
-    <td>Coeff(14)</td>
-    <td>-0.21501000399629</td>
-    <td>-0.0166920786</td>
-  </tr>
-  <tr>
-    <td>Coeff(15)</td>
-    <td>0.01867413096353</td>
-    <td>-0.0007190532</td>
-  </tr>
-  <tr>
-    <td>Coeff(16)</td>
-    <td>0.053682417759</td>
-    <td>-0.025485194448</td>
-  </tr>
-  <tr>
-    <td>Coeff(17)</td>
-    <td>-0.00270968955115</td>
-    <td>4.87491696E-05</td>
-  </tr>
-  <tr>
-    <td>Coeff(18)</td>
-    <td>0.00112277498589</td>
-    <td>2.719234152E-05</td>
-  </tr>
-  <tr>
-    <td>Coeff(19)</td>
-    <td>-0.00127758497498</td>
-    <td>-0.06537662555556</td>
-  </tr>
-  <tr>
-    <td>Coeff(20)</td>
-    <td>7.60420796601607E-05</td>
-    <td>-0.002278167</td>
-  </tr>
-  <tr>
-    <td>Coeff(21)</td>
-    <td>1.43600088336017</td>
-    <td>0.0002500254</td>
-  </tr>
-  <tr>
-    <td>Coeff(22)</td>
-    <td>-0.5198695909109</td>
-    <td>-0.0910565458</td>
-  </tr>
-  <tr>
-    <td>Coeff(23)</td>
-    <td>0.11733957691051</td>
-    <td>0.00318176316</td>
-  </tr>
-  <tr>
-    <td>Coeff(24)</td>
-    <td>1.50492810819924</td>
-    <td>3.8621772E-05</td>
-  </tr>
-  <tr>
-    <td>Coeff(25)</td>
-    <td>-0.13589890592697</td>
-    <td>-0.0034285382352</td>
-  </tr>
-  <tr>
-    <td>Coeff(26)</td>
-    <td>-0.15257758186651</td>
-    <td>8.56589904E-06</td>
-  </tr>
-  <tr>
-    <td>Coeff(27)</td>
-    <td>-0.05338438281146</td>
-    <td>-1.516821552E-06</td>
-  </tr>
-  <tr>
-    <td>Coeff(28)</td>
-    <td>0.00493294869566</td>
-    <td>N/A</td>
-  </tr>
-  <tr>
-    <td>Coeff(29)</td>
-    <td>-0.00796260394174</td>
-    <td>N/A</td>
-  </tr>
-  <tr>
-    <td>Coeff(30)</td>
-    <td>0.00022261982862</td>
-    <td>N/A</td>
-  </tr>
-  <tr>
-    <td>Coeff(31)</td>
-    <td>-0.05439520015681</td>
-    <td>N/A</td>
-  </tr>
-  <tr>
-    <td>Coeff(32)</td>
-    <td>0.00474266879162</td>
-    <td>N/A</td>
-  </tr>
-  <tr>
-    <td>Coeff(33)</td>
-    <td>-0.01858546718156</td>
-    <td>N/A</td>
-  </tr>
-  <tr>
-    <td>Coeff(34)</td>
-    <td>0.00115667701294</td>
-    <td>N/A</td>
-  </tr>
-  <tr>
-    <td>Coeff(35)</td>
-    <td>0.00080737066446</td>
-    <td>N/A</td>
-  </tr>
-</table>
-
-Similarly, the YorkCalc correlation has 27 terms with three independent variables:
-
-    Approach =   Coeff(1)  +  Coeff(2)•Twb +  Coeff(3)•Twb<sup>2</sup>  +  Coeff(4)•Tr  +
-
-Coeff(5)•Twb•Tr  +  Coeff(6)•Twb<sup>2</sup>•Tr  +  Coeff(7)•Tr<sup>2</sup>  +
-
-Coeff(8)•Twb•Tr<sup>2 </sup> +  Coeff(9)•Twb<sup>2</sup>•Tr<sup>2 </sup> +  Coeff(10)•LGRatio  +
-
-Coeff(11)•Twb•LGRatio  + Coeff(12)•Twb<sup>2</sup>•LGRatio  +
-
-Coeff(13)•Tr•LGRatio  +  Coeff(14)•Twb•Tr•LGRatio  +
-
-Coeff(15)•Twb<sup>2</sup>•Tr•LGRatio  +  Coeff(16)•Tr<sup>2</sup>•LGRatio  +
-
-Coeff(17)•Twb•Tr<sup>2</sup>•LGRatio  + Coeff(18)•Twb<sup>2</sup>•Tr<sup>2</sup>•LGRatio +
-
-Coeff(19)•LGRatio<sup>2 </sup> +  Coeff(20)•Twb•LGRatio<sup>2</sup>  +
-
-Coeff(21)• Twb<sup>2</sup>•LGRatio<sup>2 </sup> +  Coeff(22)•Tr•LGRatio<sup>2 </sup> +
-
-Coeff(23)•Twb•Tr•LGRatio<sup>2 </sup> +  Coeff(24)•Twb<sup>2</sup>•Tr•LGRatio<sup>2 </sup> +
-
-Coeff(25)•Tr<sup>2</sup>•LGRatio<sup>2 </sup> +  Coeff(26)•Twb•Tr<sup>2</sup>•LGRatio<sup>2 </sup> +
-
-Coeff(27)•Twb<sup>2</sup>•Tr<sup>2</sup>•LGRatio<sup>2</sup>
-
-where:
-
-            Approach = approach temperature (<sup>o</sup>C) = outlet water temperature minus inlet air wet-bulb temperature
-
-            Tr = range temperature (<sup>o</sup>C) = inlet water temperature minus outlet water temperature
-
-            Twb = inlet air wet-bulb temperature (<sup>o</sup>C)
-
-            LGratio = liquid-to-gas ratio = ratio of water flow rate ratio (FRwater) to air flow rate ratio (FRair)
-
-      Coeff(\#) = correlation coefficients
-
-
-
-If the user selects Tower Model Type = YorkCalc, then the 27 coefficients derived for the YorkCalc simulation model (York International Corp. 2002) are used and these coefficients are already defined within EnergyPlus as shown in Table 63. If the user specifies Tower Model Type = YorkCalcUserDefined, then the user must enter a CoolingTowerPerformance:YorkCalc object to define the 27 coefficients that will be used by the YorkCalc approach temperature correlation.
-
-The approach temperature correlations for the CoolTools and YorkCalc simulation models are valid for a range of conditions defined in Table 64. If the user defines their own model coefficients (CoolingTowerPerformance:CoolTools or CoolingTowerPerformance:YorkCalc), then they must also define in that same object the range of conditions for which the model is valid. For all of these correlation variables, the program issues warnings if the actual values are beyond the minimum/maximum values specified for the correlation being used. For inlet air wet-bulb temperature and water mass flow rate ratio, the values of these variables used in the calculation of approach temperature are limited to be within the valid minimum/maximum range. For approach, range, and liquid-to-gas ratio the warnings are issued if the values are beyond the specified minimum/maximum range but the actual values are still used. The warnings issued do not necessarily indicate a poor estimate of tower performance at the condition(s) which caused the warning, but are provided to identify conditions outside the defined correlation limits. Exceeding the defined limits by a small amount may not introduce significant errors, but large deviations may be problematic. It is for this reason that we recommend using a very broad range of cooling tower performance data (i.e., data covering the entire range expected during the simulation) when generating user-defined coefficients for the variable speed tower model.
-
-
-
-
-
-Table 64. Minimum and Maximum Limits for Approach Temperature Correlation Variables
-
-<table class="table table-striped">
-<tr>
-<td>Independent Variable Limit</td>
-<td>CoolTools</td>
-<td>YorkCalc</td>
-</tr>
-<tr>
-<td>Minimum Inlet Air Wet-Bulb Temperature</td>
-<td>-1.0°C</td>
-<td>-34.4°C</td>
-</tr>
-<tr>
-<td>Maximum Inlet Air Wet-Bulb Temperature</td>
-<td>26.7°C</td>
-<td>26.7°C</td>
-</tr>
-<tr>
-<td>Minimum Tower Range Temperature</td>
-<td>1.1°C</td>
-<td>1.1°C</td>
-</tr>
-<tr>
-<td>Maximum Tower Range Temperature</td>
-<td>11.1°C</td>
-<td>22.2°C</td>
-</tr>
-<tr>
-<td>Minimum Tower Approach Temperature</td>
-<td>1.1°C</td>
-<td>1.1°C</td>
-</tr>
-<tr>
-<td>Maximum Tower Approach Temperature</td>
-<td>11.1°C</td>
-<td>40°C</td>
-</tr>
-<tr>
-<td>Minimum Water Flow Rate Ratio</td>
-<td>0.75</td>
-<td>0.75</td>
-</tr>
-<tr>
-<td>Maximum Water Flow Rate Ratio</td>
-<td>1.25</td>
-<td>1.25</td>
-</tr>
-<tr>
-<td>Maximum Liquid-to-Gas Ratio</td>
-<td>N/A</td>
-<td>8.0</td>
-</tr>
-
-</table>
-
-The approach temperature correlation(s) used to simulate cooling tower heat rejection are based on water and air flow rate “ratios� and are not directly dependent on the size of the tower or the actual air and water flow rates through the tower. However, the model correlations are developed based on a reference condition. For Model Types “CoolToolsCrossFlow� and “YorkCalc�, the reference condition is a water flow rate of 0.000043 m<sup>3</sup>/s per kW of heat rejected (2.4 gal/min per ton of heat rejected) with 25.6<sup>o</sup>C (78<sup>o</sup>F) enter air wet-bulb temperature, 35<sup>o</sup>C (95<sup>o</sup>F) hot water inlet temperature, and 29.4<sup>o</sup>C (85<sup>o</sup>F) cold water outlet temperature. The reference condition may be different if the user defines tower model coefficients using CoolingTowerPerformance:CoolTools or CoolingTowerPerformance:YorkCalc.
-
-Due to the inherent reference condition used to generate the tower performance curves, the water flow rate at the reference condition must be determined using the design performance information specified by the user and the tower model’s approach temperature correlation. This is done by using the model’s approach temperature correlation (described earlier in this section) to calculate the water flow rate ratio which yields the user-defined design approach temperature based on an air flow rate ratio of 1.0 (*FR<sub>air</sub>* = 1.0), the design inlet air wet-bulb temperature, and the design range temperature. The calculated approach temperature (using the model correlation) must satisfy the following two equations:
-
-<span>\({T_{water,outlet,design}} = {T_{wb,air,design}} + {T_{approach,design}}\quad \{ F{R_{air}} = 1.0\} \)</span><span>\({T_{water,inlet,design}} = {T_{wb,air,design}} + {T_{approach,design}} + {T_{range,design}}\quad \{ F{R_{air}} = 1.0\} \)</span>
-
-where:
-
-<span>\({T_{water,outlet,design}}\)</span>= design outlet water temperature (<sup>o</sup>C)
-
-<span>\({T_{water,inlet,design}}\)</span>= design inlet water temperature (<sup>o</sup>C)
-
-<span>\({T_{wb,air,design}}\)</span>= design inlet air wet-bulb temperature (<sup>o</sup>C)
-
-<span>\({T_{approach,design}}\)</span>= design approach temperature (<sup>o</sup>C)
-
-<span>\({T_{range,design}}\)</span>= design range temperature (<sup>o</sup>C)
-
-<span>\(F{R_{air}}\)</span>= air flow rate ratio (actual air flow rate divided by design air flow rate)
-
-The water flow rate ratio used in the approach temperature correlation which satisfies these two equations is the ratio of the design water flow rate (specified by the user) to the water flow rate at the reference condition. This ratio is used to calculate the reference water volumetric flow rate, which is then used throughout the simulation to determine the actual water flow rate ratio used in the approach temperature correlation for each simulation time step.
-
-<div>$${\dot V_{reference}} = \frac{{{{\dot V}_{design}}}}{{F{R_{water\;reference}}}}$$</div>
-
-where:
-
-<span>\({\dot V_{reference}}\)</span>= water volumetric flow rate at the reference condition (m<sup>3</sup>/s)
-
-<span>\({\dot V_{design}}\)</span>= design water volumetric flow rate specified by the user (m<sup>3</sup>/s)
-
-<span>\(F{R_{water,reference}}\)</span>= design water flow rate divided by the reference water flow rate
-
-The cooling tower seeks to maintain the temperature of the water exiting the cooling tower at (or below) a setpoint. The setpoint temperature is defined by the field “Condenser Loop Temperature Setpoint schedule or reference� for the CondenserLoop object. The model simulates the outlet water temperature in four successive steps:
-
-·        The model first determines the tower outlet water temperature with the tower fan operating at maximum speed. If the outlet water temperature is above the setpoint temperature, the fan runs at maximum speed.
-
-·        If the outlet water temperature with maximum fan speed is below the setpoint temperature, then the model next determines the impact of “free convection� (water flowing through tower with fan off). If the exiting water temperature based on “free convection� is at or below the setpoint, then the tower fan is not turned on.
-
-·        If the outlet water temperature remains above the setpoint after “free convection� is modeled, then the tower fan is turned on at the minimum fan speed (minimum air flow rate ratio) to reduce the leaving water temperature. If the outlet water temperature is below the setpoint at minimum fan speed, the tower fan is cycled on and off to maintain the outlet water setpoint temperature.
-
-·        If the outlet water temperature remains above the setpoint after minimum fan speed is modeled, then the tower fan is turned on and the model determines the required air flow rate and corresponding fan speed to meet the desired setpoint temperature.
-
-For each simulation time step, the model first calculates the outlet water temperature with the tower fan operating at maximum speed (FRair = 1.0). The calculated approach temperature (using the correlations described above), inlet air wet-bulb temperature (weather data), and range temperature are used to determine the tower outlet water temperature as follows:
-
-<div>$$\begin{array}{l}{T_{water,outlet,fanMAX}} = {T_{wb,air}} + \,\,{T_{approach}}\,\,\,\,\,\{ F{R_{air}} = 1.0\} \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\quad \,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, = \,{T_{water,inlet}}\, + \,\,{T_{range}}\end{array}$$</div>
-
-where:
-
-<span>\({T_{water,outlet,fanMAX}}\)</span> = tower outlet water temperature at maximum fan speed (<sup>o</sup>C)
-
-<span>\({T_{wb,air}}\)</span> = tower inlet air wet-bulb temperature (<sup>o</sup>C)
-
-<span>\({T_{approach}}\)</span>= approach temperature at current operating conditions (<sup>o</sup>C)
-
-<span>\({T_{range}}\)</span>= range temperature at current operating conditions (<sup>o</sup>C)
-
-Note that the approach temperature correlation as described previously is a function of range temperature, so the equations above must be solved iteratively to converge on a solution. If the resulting outlet water temperature is above the desired setpoint temperature, then the fan runs at maximum speed and does not cycle on/off (fan part-load ratio = FanPLR = 1.0 and *FR<sub>air</sub>* = 1.0).
-
-If the outlet water temperature with maximum fan speed is below the setpoint temperature, then the model next determines the impact of “free convection� (water flowing through tower with fan off). In the free convection regime, the outlet water temperature is calculated using a fraction of the water temperature difference through the tower when the fan is at its maximum speed. This fraction is defined by the user (Fraction of Tower Capacity in Free Convection Regime).
-
-<div>$${T_{water,outlet,fanOFF}} = {T_{water,inlet}}\,\,\,\, - \,\,\left[ {Fra{c_{freeconv}}\left( {{T_{water,inlet}}\,{\rm{ - }}\,\,{T_{water,outlet,fanMAX}}} \right)} \right]$$</div>
-
-where:
-
-<span>\({T_{water,outlet,fanOFF}}\)</span> = tower outlet water temperature in free convection regime (<sup>o</sup>C)
-
-<span>\({T_{water,inlet}}\)</span> = tower inlet water temperature (<sup>o</sup>C)
-
-<span>\(Fra{c_{freeconv}}\)</span>= fraction of tower capacity in free convection regime (user specified)
-
-If the outlet water temperature in the free convection regime is below the setpoint temperature, the tower fan is not turned on and the fan part-load ratio is set equal to 0. In addition, the air flow rate ratio through the tower is assumed to be equal to the fraction of tower capacity in the free convection regime.
-
-<div>$$FanPLR\,\, = \,\,FanPL{R_{freeconv}} = 0.0$$</div>
-
-<div>$$F{R_{air}}\, = F{R_{air,freeconv}} = Fra{c_{freeconv}}$$</div>
-
-where:
-
-<span>\(FanPLR\)</span>= fan part-load ratio
-
-<span>\(FanPL{R_{freeconv}}\)</span>= fan part-load ratio in free convection regime
-
-<span>\(F{R_{air,freeconv}}\)</span> = air flow rate ratio in free convection regime
-
-If the outlet water temperature in the free convection regime is above the setpoint temperature, then the fan is turned on at the minimum fan speed (minimum air flow rate ratio, FR<sub>air,min</sub> , entered by the user) and the outlet water temperature is calculated as the inlet air wet-bulb temperature plus the calculated approach temperature:
-
-<div>$$F{R_{air}} = F{R_{air,\min }}$$</div>
-
-<div>$${T_{water,outlet,fanMIN}} = {T_{wb,air}}{\rm{ + }}\,{T_{approach}}\,\,\,\,\{ F{R_{air}}\, = \,F{R_{air,\min }}\} $$</div>
-
-where:
-
-<span>\({T_{water,outlet,FanMIN}}\)</span> = outlet water temperature at minimum fan speed (<sup>o</sup>C)
-
-<span>\(F{R_{air,\min }}\)</span> = air flow rate ratio at the minimum fan speed
-
-If the outlet water temperature at minimum fan speed is below the setpoint temperature, the cooling tower fan cycles on and off at the minimum air flow rate ratio in order to meet the setpoint temperature.
-
-<div>$$FanPLR = \left( {\frac{{{T_{water,outlet,fanOFF}} - {T_{{\rm{setpoint}}}}}}{{{T_{water,outlet,fanOFF}} - {T_{water,outlet,fanMIN}}}}} \right)$$</div>
-
-where:
-
-<span>\({T_{{\rm{setpoint}}}}\)</span> = outlet water setpoint temperature (<sup>o</sup>C)
-
-If the outlet water temperature at minimum fan speed is above the outlet water temperature setpoint, then the cooling tower fan speed (*FR<sub>air</sub>*) is increased until the calculated approach temperature produces the required outlet water temperature to meet the setpoint.
-
-<div>$${T_{approach}} = f\left( {F{R_{air}}} \right)$$</div>
-
-<div>$${T_{water,outlet}} = {T_{{\rm{setpoint}}}}\, = {T_{wb,air}}{\rm{ + }}\,{T_{approach}}$$</div>
-
-<span>\(FanPLR = 1.0\)</span> *(i.e., fan does not cycle on/off)*
-
-#### Fan Power
-
-When the cooling tower fan is operating, fan electric power is calculated based on the air flow rate ratio required to meet the above conditions. If the user has entered a fan power curve object (cubic curve), the output of that curve is multiplied by the design fan power. Otherwise, tower fan power is assumed to be directly proportional to the cube of the air flow rate ratio. In either case, the fan part-load ratio is applied to account for times when the tower fan cycles on/off to meet the setpoint temperature. Fan energy consumption is calculated each simulation time step.
-
-<div>$$\begin{array}{l}IF\left( {FanPowerCurveObject\,\,\,is\,Defined} \right)THEN\\\quad {P_{fan}} = \left( {CurveOutput} \right)\left( {FanPLR} \right){P_{fan,design}}\\ELSE\\\quad {P_{fan}} = \left( {{P_{fan,design}}} \right)\left( {FanPLR} \right){\left( {F{R_{air}}} \right)^{\rm{3}}}\\ENDIF\end{array}$$</div>
-
-<div>$${E_{fan}} = \left( {{P_{fan}}} \right)\left( {TimeStepSys} \right)3600.$$</div>
-
-where:
-
-<span>\(FanPowerCurveObject\)</span> = name of fan power ratio as a function of air flow rate ratio curve
-
-<span>\({P_{fan}}\)</span> = tower fan electric power (W)
-
-<span>\({E_{fan}}\)</span> = tower fan electric consumption (J)
-
-<span>\(CurveOutput\)</span> = output of FanPowerCurveObject evaluated at the operating air flow rate ratio (*FR<sub>air</sub>*)
-
-<span>\({P_{fan,design}}\)</span> = design fan power at design (maximum) air flow through the tower (W)
-
-*TimeStepSys* = HVAC system simulation time step (hr)
-
-#### Tower Basin Heater
-
-Calculations are also made to estimate the electric power input to the tower basin heater. A schedule may be used to disable the basin heater during regular maintenance periods or other time periods (e.g., during summer). If a schedule is not provided, the basin heater is assumed to be available the entire simulation time period. The basin heater operates when it is scheduled on, the outdoor air dry-bulb temperature is below the basin heater setpoint temperature, and the cooling tower is not active (i.e., water is not flowing through the tower). The user is required to enter a basin heater capacity (watts per degree Kelvin) and a heater setpoint temperature (<sup>o</sup>C) if they want to model basin heater electric power.
-
-<div>$$\begin{array}{l}{P_{{\rm{heater,basin}}}}{\rm{ = }}0.0\\IF\,(WaterNotFlowingThroughTower)\,THEN\\\,\,\,\,\,\,IF\left( {Schedul{e_{{\rm{heater,basin}}}}\,is\,Defined} \right)THEN\\\quad \,\,\,\,\,\,IF({\rm{CA}}{{\rm{P}}_{{\rm{heater,basin}}}}\,{\rm{ >  }}0\,\,.AND.\,\,\,Schedul{e_{{\rm{heater,basin}}}} = ON)\,\,THEN\\\quad \quad \,\,\,\,\,{P_{{\rm{heater,basin}}}}\,{\rm{ = }}\,\,{\rm{MAX}}\left( {{\rm{0}}{\rm{.0,CA}}{{\rm{P}}_{{\rm{heater,basin}}}}\left( {{{\rm{T}}_{{\rm{setpoint,basin}}}}{\rm{ - }}{{\rm{T}}_{{\rm{db,outdoor}}}}} \right)} \right)\,\,\,\\\,\,\,\quad \,\,ENDIF\\\,\,\,\,\,\,ELSE\\\quad \,\,\,\,\,\,IF(\,{\rm{CA}}{{\rm{P}}_{{\rm{heater,basin}}}}\,{\rm{ >  }}0)\,\,THEN\\\,\,\,\quad \,\,\,\,\,\,\,\,{P_{{\rm{heater,basin}}}}\,{\rm{ = }}\,{\rm{MAX}}\left( {{\rm{0}}{\rm{.0,CA}}{{\rm{P}}_{{\rm{heater,basin}}}}\left( {{{\rm{T}}_{{\rm{setpoint,basin}}}}{\rm{ - }}{{\rm{T}}_{{\rm{db,outdoor}}}}} \right)} \right)\\\,\,\,\,\,\,\,\,\,\,\,ENDIF\\\,\,\,\,\,\,ENDIF\\ENDIF\end{array}$$</div>
-
-<div>$${E_{{\rm{heater,basin}}}} = \left( {{P_{{\rm{heater,basin}}}}} \right)\left( {TimeStepSys} \right){\rm{3600}}{\rm{.}}$$</div>
-
-where:
-
-<span>\({P_{{\rm{heater,basin}}}}\)</span> = tower basin heater electric power (W)
-
-<span>\({E_{{\rm{heater,basin}}}}\)</span> = tower basin heater electric consumption (J)
-
-*T<sub>setpoint,basin</sub>* = basin heater setpoint temperature (<sup>o</sup>C)
-
-*T<sub>db,outdoor</sub>*    = outdoor air dry-bulb temperature (<sup>o</sup>C)
-
-CAP*<sub>heater,basin</sub>* = basin heater capacity (W/K)
-
-*Schedule<sub>heater,basin</sub>* = basin heater schedule (schedule value &gt; 0 means ON)
-
-#### References
-
-ASHRAE 1999. HVAC1 Toolkit: A Toolkit for Primary HVAC System Energy Calculations. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Benton, D.J., Bowman, C.F., Hydeman, M., Miller, P. 2002. An Improved Cooling Tower Algorithm for the CoolTools<sup>TM</sup> Simulation Model. *ASHRAE Transactions,* Vol. 108, Part 1, pp.760-768.
-
-Bourdouxhe, J.P., M. Grodent, J. Lebrun and C. Silva. 1994. Cooling tower model developed in a toolkit for primary HVAC system energy calculation: part 1. Proceedings of the fourth international conference on system simulation in buildings, Liege (Belgium), December 5-7, 1994.
-
-Incropera, F.P. and D.P. DeWitt. 1981. Fundamentals of Heat Transfer. New York: John Wiley & Sons.
-
-Merkel, F.  1925. Verduftungskuhlung. VDI Forschungarbeiten, No 275, Berlin.
-
-Rosaler, Robert C. 1995. Standard Handbook of Plant Engineering, 2<sup>nd</sup> Ed. New York, NY: McGraw-Hill, pp. 6-36-37.
-
-Scheier, L. 2013. Personal communication.
-
-York International Corporation, 2002. “YORKcalc<sup>TM</sup> Software, Chiller-Plant Energy-Estimating Program�, Form 160.00-SG2 (0502).
-
-### Cooling Towers with Multiple Cells
-
-Many towers are constructed to be capable of being grouped together to achieve the desired capacity. Thus, many cooling towers are assemblies of two or more individual cooling towers or “cells.� The number of cells they have, e.g., an eight-cell tower, often refers to such towers.
-
-For the operation of multi-cell towers, the first step is to determine the number of cells *n,* which will be operating during the timestep using the calculation logic from DOE-2.1E.
-
-The maximum and minimum flow rates per cell are determined according to the input fractions (*Minimum  Water Flow Rate Fraction:*<span>\({k_{min}}\)</span>* * and *Maximum  Water Flow Rate Fraction:* <span>\({k_{max}}\)</span>) as follows:
-
-<div>$$
-  \left\{
-    \begin{array}{rl}
-      {{\dot m}_{w,min}} =  & \frac{{{{\dot m}_{w,des}}}}{{{n_{tot}}}} \times {k_{min}} \\
-      {{\dot m}_{w,max}} =  & \frac{{{{\dot m}_{w,des}}}}{{{n_{tot}}}} \times {k_{max}}
-    \end{array}
-  \right.
-$$</div>
-
-where <span>\({{{\dot m}_{w,des}}}\)</span> is the design water flow rate through the entire cooling tower.
-
-Then, we determine the minimum and maximum number of cells that can operate with this water flow rate:
-
-<div>$$
-  \left\{
-    {\begin{array}{c}
-      {{n_{min}} &= MIN\left( {\frac{{{{\dot m}_{w,tot}}}}{{{{\dot m}_{w,max}}}},{n_{tot}}} \right)} \\
-      {{n_{max}} &= MIN\left( {\frac{{{{\dot m}_{w,tot}}}}{{{{\dot m}_{w,min}}}},{n_{tot}}} \right)}
-    \end{array}}
-  \right.
-$$</div>
-
-where *n<sub>tot</sub>* is the total number of cells of the tower, and<span>\({{{\dot m}_{w,tot}}}\)</span> is the water flow rate to the tower.
-
-The number of cells operating*n* is set accordingly:
-
-If the *Cell Control* method is *MinimalCell,*
-
-*n =* <span>\({{n_{min}}}\)</span>
-
-If the *Cell Control* method is *MaximalCell,*
-
-*n =* <span>\({{n_{max}}}\)</span>
-
-Finally, the water mass flow rate per cell (<span>\({{\dot m}_w})\)</span> will be:
-
-<div>$${{\dot m}_w} = \frac{{{{\dot m}_{w,tot}}}}{n}$$</div>
-
-Then we simulate the performance of one cell with this flow rate per cell (calling the SimSimpleTower subroutine for single and two speed cooling tower objects). As we assume that each cell is identical, the UA of one cell is calculated dividing the UA of the whole tower (obtained from the input or from the auto sizing calculations). The air flow rate per cell is also equal to the one of the whole tower divided by the number of cells operating:
-
-<div>$$U{A_{cell}} = \frac{{U{A_{cell}}}}{{{n_{tot}}}}$$</div>
-
-<div>$${\dot m_{air,cell}} = \frac{{{{\dot m}_{air,tot}}}}{n}$$</div>
-
-At the end, the total fan power of the tower operating with a certain number of cells is given by:
-
-<div>$$FanPower = FanPowe{r_{tot}} \times \frac{n}{{{n_{tot}}}}$$</div>
-
-If the cells operating do not meet the loads, we increase the number of cells if spare cells are available and the water flow through each cell is within the user specified minimum and maximum water flow rate fractions range. This is an iteration process.
-
-### Cooling Tower Makeup Water Usage
-
-Makeup water use for all types of cooling towers is made up of three components: evaporation, drift, and blowdown.  The first is the amount of water evaporated to reduce the water’s temperature as it passes through the cooling tower. There are two methods that evaporation makeup water can be modeled in EnergyPlus.  The first method assumes that the tower outlet air conditions are saturated (which may not always be the case for certain operating conditions).  For this “Saturated Exit� mode, the enthalpy of the tower’s outlet air is calculated as the inlet air enthalpy plus the water side heat transfer divided by the air mass flow rate through the tower.
-
-<div>$${\dot Q_{water}} = {\dot m_{_{water}}}{C_p}\left( {{T_{{\rm{water,inlet}}}} - {T_{{\rm{water,outlet}}}}} \right)$$</div>
-
-<div>$${h_{sat\,air,outlet}} = {h_{air,inlet}} + \left( {\frac{{{{\dot Q}_{water}}}}{{{{\dot m}_{air}}}}} \right)$$</div>
-
-where:
-
-<span>\({\dot Q_{water}}\)</span> = water-side heat transfer (W)
-
-<span>\({\dot m_{_{water}}}\)</span> = mass flow rate of water through the tower (kg/s)
-
-<span>\({C_p}\)</span> = specific heat of water (W/kg-K)
-
-<span>\({h_{sat\,air,outlet}}\)</span> = saturated outlet air enthalpy (J/kg)
-
-<span>\({h_{air,inlet}}\)</span> = inlet air enthalpy (J/kg)
-
-<span>\({\dot m_{air}}\)</span> = mass flow rate of air through the tower (kg/s)
-
-The saturation temperature and humidity ratio are then calculated for the tower’s outlet air.
-
-<div>$${T_{sat\,air,outlet}} = PsyTsatFnHPb\left( {{h_{sat\,air,outlet}},{\rm{OutBaroPress}}} \right)$$</div>
-
-<div>$${\omega_{sat\,air,outlet}} = PsyWFnTdbH\left( {{T_{sat\,air,outlet}},{h_{sat\,air,outlet}}} \right)$$</div>
-
-where:
-
-<span>\({T_{sat\,air,outlet}}\)</span> = saturated outlet air temperature (<sup>o</sup>C)
-
-<span>\(PsyTsatFnHPb\)</span> = EnergyPlus psychrometric function, returns saturation temperature given enthalpy and barometric pressure
-
-<span>\({\rm{OutBaroPress}}\)</span> = outdoor barometric pressure (Pa)
-
-<span>\({\omega_{sat\,air,outlet}}\)</span> = saturated outlet air humidity ratio (kg<sub>water</sub>/kg<sub>dry\\ air</sub>)
-
-<span>\(PsyWFnTdbH\)</span> = EnergyPlus psychrometric function, returns humidity ratio given dry-bulb temperature and enthalpy
-
-The makeup water quantity required to replenish the water lost due to evaporation is then calculated as the product of the air mass flow rate and the difference between the entering and leaving air humidity ratio divided by the density of water.
-
-<div>$${\dot V_{evaporation,makeup}} = \frac{{{{\dot m}_{air}}\left( {{\omega_{sat\,air,outlet}} - {\omega_{air,inlet}}} \right)}}{{{\rho_{water}}}}$$</div>
-
-where:
-
-<span>\({\dot V_{evaporation,makeup}}\)</span> = makeup water usage due to evaporation (m<sup>3</sup>/s)
-
-<span>\({\dot m_{air}}\)</span> = mass flow rate of air through tower (kg/s)
-
-<span>\({\omega_{air,inlet}}\)</span> = humidity ratio of tower inlet air (kg<sub>water</sub>/kg<sub>dry\\ air</sub>)
-
-<span>\({\rho_{water}}\)</span> = density of water evaluated at the tower inlet air temperature (kg/m<sup>3</sup>)
-
-The second method available for calculating water makeup for evaporation is for the user to provide a value for a loss factor.  The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water.  The value provided by the user is in units of percent-per-degree Kelvin.  The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water.  Typical values are from 0.15 to 0.27 [percent/K]. The default is 0.2.  The rate of water makeup for evaporation is then calculated by multiplying this factor times the condenser water flow rate and the temperature decrease in the condenser water flow rate. For evaporative fluid coolers, a numerical value of loss factor can be entered in the same manner as for cooling towers. If this field is blank, an empirical correlation will be used to calculate the value based on current outdoor dry bulb temperature and relative humidity. The following correlation from Qureshi and Zubair (2007) is used to calculate the loss factor:
-
-<div>$$Loss\;Factor = (113 - 8.417\phi  + 1.6147{t_{db}})*{10^{ - 5}}$$</div>
-
-where:
-
-<span>\(\phi \)</span> = relative humidity of inlet air
-
-<span>\({t_{db}}\)</span> = Dry-bulb temperature of inlet air
-
-Additional makeup water usage is modeled as a percentage of design water flow rate through the tower to account for drift, and as a scheduled flow rate to model blowdown. Drift is water loss due to the entrainment of small water droplets in the air stream passing through the tower. Drift is defined by the model user as a percentage of the tower’s design water flow rate, and is assumed to vary with tower air flow rate ratio as follows:
-
-<div>$${\dot V_{drift,makeup}} = {\dot m_{water,design}}\left( {\frac{{PercentWatertoDrift}}{{100.0}}} \right)F{R_{air}}$$</div>
-
-where:
-
-<span>\({\dot V_{drift,makeup}}\)</span> = makeup water usage due to drift (m<sup>3</sup>/s)
-
-<span>\({\dot m_{water,design}}\)</span> = design (volumetric) water flow rate (m<sup>3</sup>/s)
-
-<span>\(PercentWatertoDrift\)</span> = percent of design water flow rate lost to drift at the tower design air flow rate
-
-<span>\(F{R_{air}}\)</span>= ratio of actual air flow rate to tower design air flow rate
-
-Blowdown is water flushed from the basin on a periodic basis to purge the concentration of mineral scale or other contaminants. There are two ways that blowdown is calculated in EnergyPlus.  Blowdown water rates can be scheduled so that we have:.
-
-<div>$$\begin{array}{l}IF\left( {Schedul{e_{blowdown}}\,is\,defined} \right)THEN\\\quad {{\dot V}_{blowdown,makeup}} = ScheduleValu{e_{blowdown}}\\ELSE\\\quad {{\dot V}_{blowdown,makeup}} = 0.0\\ENDIF\end{array}$$</div>
-
-where:
-
-<span>\({\dot V_{blowdown,makeup}}\)</span> = makeup water usage due to blowdown (m<sup>3</sup>/s)
-
-*ScheduleValue<sub>blowdown</sub>* = blowdown schedule value for the time step being simulated (m<sup>3</sup>/s)
-
-The second (and default) way that blowdown can be calculated is to assume that blowdown water is continually introduced at a rate that will provide a constant concentration ratio.  As water evaporates it leaves behind minerals and the like causing the concentration of water impurities to be higher in the tower than in the makeup water.  Acceptable concentration ratios are in the range of 3 to 5 depending on the purity of the make up water.  Water lost as drift does not evaporate and decrease the water needed for blowdown.  Using the “Concentration Ratio� method, the rate of blowdown can be calculated using:
-
-<div>$${\dot V_{blowdown,makeup}} = \frac{{{{\dot V}_{evaporation,makeup}}}}{{{R_{concentration}} - 1}} - {\dot V_{drift,makeup}}$$</div>
-
-where,
-
-<span>\({R_{concentration}}\)</span> is the concentration ratio or the ratio of solids in the blowdown water to solids in the makeup water.
-
-The tower makeup water consumption (m<sup>3</sup>) for each simulation time step is calculated as the sum of the individual components of makeup water usage multiplied by the simulation time step in hours and the conversion for hours to seconds (3600 sec/hr). Makeup water usage is only calculated when the cooling tower is active and water is flowing through the cooling tower.
-
-<div>$${V_{water,\;makeup}} = \left( {{{\dot V}_{evaporation,makeup}} + {{\dot V}_{drift,makeup}} + {{\dot V}_{blowdown,makeup}}} \right)\cdot TimeStepSys\cdot 3600.$$</div>
-
-where:
-
-<span>\({V_{water,makeup}}\)</span> = tower makeup water consumption (m<sup>3</sup>)
-
-#### References
-
-Robert C. Rosaler. 1995. Standard Handbook of Plant Engineering, 2<sup>nd</sup> Ed. McGraw-Hill, New York, NY, pp 6-36-37.
-
-Quereshi, B.A. and S.M.Zubair. 2007. Prediction of evaporation losses in evaporative fluid coolers, Applied Thermal Engineering 27 pp. 520-527
-
-
-
-### One and Two Speed Fluid Coolers
-
-#### Overview
-
-The input objects FluidCooler:SingleSpeed and FluidCooler:TwoSpeed provide models for dry fluid coolers. Fluid cooler’s performance is modeled using effectiveness-NTU relationships for cross flow heat exchanger with both streams unmixed. The model can be used to simulate the performance of both single speed and two speed mechanical-draft fluid coolers. For part-load operation, the model assumes a simple linear interpolation between two steady-state regimes without accounting for any cycling losses.
-
-#### Model Description
-
-The expression for fluid cooler effectiveness is as follows:
-
-<div>$$\varepsilon  = 1 - {\mathop{\rm e}\nolimits} \left[ {{\raise0.7ex\hbox{${\{ {{\mathop{\rm e}\nolimits} ^{( - NTU{C_r}\eta )}} - 1\} }$} \!\mathord{\left/ {\vphantom {{\{ {{\mathop{\rm e}\nolimits} ^{( - NTU{C_r}\eta )}} - 1\} } {{C_r}\eta }}}\right.}\!\lower0.7ex\hbox{${{C_r}\eta }$}}} \right]$$</div>
-
-Where
-
-<span>\(\varepsilon \)</span><span>\(\varepsilon \)</span>* *= heat exchanger effectiveness
-
-<div>$${C_r} = \frac{{{{\dot C}_{\min }}}}{{{{\dot C}_{\max }}}}$$</div>
-
-<span>\({\dot C_a} = {\dot m_a}{c_{pa}}\)</span><span>\({\dot C_a} = {\dot m_a}{c_{pa}}\)</span> and<span>\({\dot C_w} = {\dot m_w}{c_{pw}}\)</span>
-
-<span>\({\dot C_{\max }} = Max({\dot C_a},{\dot C_w})\)</span><span>\({\dot C_{\max }} = Max({\dot C_a},{\dot C_w})\)</span>;<span>\({\dot C_{\min }} = Min({\dot C_a},{\dot C_w})\)</span>
-
-<div>$$NTU = \frac{{UA}}{{{{\dot C}_{\min }}}}$$</div>
-
-<span>\(\eta  = NT{U^{( - 0.22)}}\)</span><span>\(\eta  = NT{U^{( - 0.22)}}\)</span>
-
-The first fluid is water and the second fluid is air entering the heat exchanger at temperature <span>\({T_{db,in}}\)</span><span>\({T_{db,in}}\)</span> and specific heat <span>\({c_{pa}}\)</span><span>\({c_{pa}}\)</span>. The heat exchanger is characterized by a single parameter, its overall heat transfer coefficient-area product UA.
-
-When the user selects the nominal capacity method, the UA is calculated as follows:
-
-The model inputs (other than the UA) and the fluid cooler load that it must meet are specified at design conditions. Then the fluid cooler model converges to a UA value, using the regulafalsi method that will enable it to meet the design fluid cooler load given at the specified inputs.
-
-#### Method for Calculating Steady-State Exiting Water Temperature
-
-The objective of the fluid cooler model is to predict the exiting water temperature and the fan power required to meet the exiting water setpoint temperature. The exiting water temperature is calculated based on an energy balance that assumes that the energy absorbed by the air is equivalent to the energy removed from the water. The procedure for calculating the steady-state, exiting air dry-bulb temperature is outlined below.
-
-With the overall heat transfer coefficient-area product for the fluid cooler calculated by the nominal capacity information entered by the user, the effectiveness of the heat exchanger is then calculated as:
-
-<div>$$\varepsilon  = 1 - {\mathop{\rm e}\nolimits} \left[ {{\raise0.7ex\hbox{${\{ {{\mathop{\rm e}\nolimits} ^{( - NTU{C_r}\eta )}} - 1\} }$} \!\mathord{\left/ {\vphantom {{\{ {{\mathop{\rm e}\nolimits} ^{( - NTU{C_r}\eta )}} - 1\} } {{C_r}\eta }}}\right.}\!\lower0.7ex\hbox{${{C_r}\eta }$}}} \right]$$</div>
-
-The heat transfer rate is then calculated as follows:
-
-<span>\(\dot Q = \varepsilon {\dot C_{\min }}({T_{w,in}} - {T_{db,in}})\)</span><span>\(\dot Q = \varepsilon {\dot C_{\min }}({T_{w,in}} - {T_{db,in}})\)</span>
-
-Then the outlet air dry-bulb and outlet water temperature are calculated:
-
-<div>$${T_{db,out}} = {T_{db,in}} + \frac{{\mathop Q\limits^. }}{{{{\mathop C\limits^. }_a}}}$$</div>
-
-<div>$${T_{w,out}} = {T_{w,in}} - \frac{{\mathop Q\limits^. }}{{{{\mathop C\limits^. }_w}}}$$</div>
-
-<span>\({T_{w,in}}\)</span>= inlet water temperature, <sup>o</sup>C
-
-<span>\({T_{w,out}}\)</span>= outlet water temperature, <sup>o</sup>C
-
-<span>\({T_{db,in}}\)</span> = dry-bulb temperature of the inlet air, <sup>o</sup>C
-
-<span>\({T_{db,out}}\)</span>= dry-bulb temperature of the outlet air, <sup>o</sup>C
-
-#### Calculating the Actual Exiting Water Temperature and Fan Power
-
-The previous section describes the methodology used for calculating the steady-state temperature of the water leaving the fluid cooler. This methodology is used to calculate the exiting water temperature with the fluid cooler fans operating (including low and high fan speed for the two-speed fluid cooler). The exiting water temperature calculations use the fluid flow rates (water and air) and the Nominal capacity information entered by the user for each regime.
-
-The fluid cooler model seeks to maintain the temperature of the water exiting the fluid cooler at (or below) a setpoint. The setpoint schedule is defined by the field “Loop Temperature Setpoint  Node or reference� for the CondenserLoop object.
-
-The fluid cooler fans are turned on to reduce the exiting water temperature to the setpoint. The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (e.g., Fluid cooler fans on for the entire simulation time step and fluid cooler fans off for the entire simulation time step). Cyclic losses are not taken into account. If the outlet water temperature is less than the set-point then the fraction of time for which the fluid cooler must operate to meet the set-point is calculated by using the following equation:
-
-<div>$$\omega \,\, = \frac{{{T_{set}} - {T_{wout,off}}}}{{{T_{wout,on}} - {T_{wout,off}}}}$$</div>
-
-Where
-
-<span>\({T_{set}}\)</span> = exiting water setpoint temperature, <sup>o</sup>C
-
-<span>\({T_{wout,off}}\)</span> = exiting water temperature with all fluid cooler fans off, <sup>o</sup>C
-
-<span>\({T_{wout,on}}\)</span> = exiting water temperature with all fluid cooler fans on, <sup>o</sup>C
-
-The average fan power for the simulation time step is calculated by multiplying <span>\(\omega \,\)</span>by the steady-state fan power specified by the user.
-
-The calculation method for the two-speed fluid cooler is similar to that for the single-speed fluid cooler example described above. The model first calculates the steady-state exiting water temperature with the fluid cooler fans at low speed. If the exiting water temperature at low fan speed is below the setpoint temperature, then the average fan power is calculated based on the result of previous equation and the steady-state, low speed fan power specified by the user.  If low-speed fan operation is unable to reduce the exiting water temperature below the setpoint, then the fluid cooler fans’ speed is increased to high speed and the steady-state exiting water temperature is calculated. If this temperature is below the setpoint, then a modified version of previous equation is used to calculate runtime at high fan speed:
-
-<div>$$\omega \,\, = \frac{{{T_{set}} - {T_{wout,low}}}}{{{T_{wout,high}} - {T_{wout,low}}}}$$</div>
-
-where
-
-<span>\({T_{set}}\)</span> = exiting water setpoint temperature, <sup>o</sup>C
-
-<span>\({T_{wout,low}}\)</span> = exiting water temperature with fluid cooler fans at low speed, <sup>o</sup>C
-
-<span>\({T_{wout,high}}\)</span> = exiting water temperature with fluid cooler fans at high speed, <sup>o</sup>C
-
-The average fan power for the simulation time step is calculated for the two-speed fluid cooler as follows
-
-<div>$${P_{fan,avg}}\, = \,\omega \,({P_{fan,high}})\, + \,\left( {1 - \omega } \right)\left( {{P_{fan,low}}} \right)$$</div>
-
-Demand Controlled Ventilation <a name="DCV"></a>
------------------------------
-
-ASHRAE Standard 62.1, Ventilation for Acceptable Indoor Air Quality, contains provisions that allow building ventilation systems to vary the amount of outdoor ventilation air delivered to occupied zones based on feedback from sensors that monitor various indoor air contaminants (ASHRAE 2007). Although not a contaminant of concern in most buildings, carbon dioxide (CO<sub>2</sub>) levels can be monitored as an indicator of building occupancy and the associated human bioeffluent concentration. Demand controlled ventilation (DCV) is being increasingly used to modulate outdoor ventilation air based on real-time occupancy (Emmerich and Persily 1997, Schell et al. 1998, Schell and Int-Hout 2001). Modulating the outdoor ventilation air while maintaining proper indoor air quality has the potential for large energy savings compared to constant rate ventilation systems that are typically designed to provide outdoor ventilation air based on maximum anticipated occupancy.
-
-EnergyPlus can model DCV by the ventilation rate procedure (VRP) defined in ASHRAE Standard 62.1-2007/2010 for single and multiple path systems, and the indoor air quality procedure (IAQP) defined in Standard 62. The VRP first calculates the breathing-zone outdoor air flow rate based on two components – the zone occupant component and the zone floor area component, then it calculates the zone supply outdoor air flow rate considering the zone air distribution effectiveness and secondary recirculation (for mult-path systems only), and finally calculates the system outdoor air flow rate considering the zone diversity and system ventilation efficiency. The user must include the following five objects in their input data file in order to model DCV (using VRP or IAQP):
-
-n **AirLoopHVAC:OutdoorAirSystem** to simulate the mixed air box of the air loop
-
-n **Controller:MechanicalVentilation** with the DCV flag set to 'Yes' to determine the minimum outdoor air flow rate to be provided by the mixed air box
-
-n **Controller:OutdoorAir** to control the outside air flow rate introduced via the mixed air box
-
-n **DesignSpecification:OutdoorAir** to describe the outdoor air requirements for each zone
-
-n **DesignSpecification:ZoneAirDistribution** to describe air distribution effectiveness and secondary recirculation (for multi-path ventilation systems) for each zone
-
-The outdoor air system (AirLoopHVAC:OutdoorAirSystem) is a subsystem of an AirLoopHVAC which handles the mixed air portion of the primary air system: the system relief air, the outside air inlet, and any components and controllers associated with the system relief air and outside air streams. The inputs for this object are fully described in the EnergyPlus Input Output Reference. Determining the outdoor air ventilation rate and introducing this ventilation via the mixed air box are accomplished by the mechanical ventilation and outdoor air controller objects.
-
-The VRP currently requires outdoor air ventilation rates to be determined based on the floor area of each occupied zone plus the number of people in each zone. The number of people varies based on the setting of the DCV flag in the Controller:MechanicalVentilation object. For using occupancy at every time step, the DCV flag must be set to 'Yes'. The outdoor air ventilation rate can then be reset dynamically as operating conditions change (e.g., variations in occupancy). The Controller:MechanicalVentilation object simplifies the procedure for calculating these outdoor air ventilation requirements and resetting them based on varying occupancy levels. This is particularly useful for large air distribution systems that serve a number of different zone types with varying occupancy levels.
-
-The IAQP (ASHRAE 2007) is a design procedure in which outdoor air intake and other system design parameters are based on an analysis of contaminant sources, and contaminant concentration targets. Although carbon dioxide is not considered as an indoor contaminant but is considered as an indicator of indoor air quality in buildings, EnergyPlus uses IAQP to control carbon dioxide. In addition, a generic contaminant may be introduced. The current IAQP in EnergyPlus allows credit to be taken for controls that can be reliably demonstrated to result in indoor carbon dioxide and generic contaminant concentrations equal to or lower that those achieved using the VRP. The IAQP may also be used where the design is intended to attain specific target carbon dioxide and generic contaminant levels.
-
-### Ventilation Rate Procedure
-
-#### Calculation of zone minimum outdoor air flow
-
-For the i-th zone, first the breathing-zone outdoor air flow is calculated:
-
-<div>$${V_{bz,i}} = {R_{p,i}} \times {P_i} + {R_{a,i}} \times {A_i}$$</div>
-
-Where:
-
-<span>\({V_{bz,i}}\)</span>= the breathing-zone outdoor air flow, m³/s
-
-<span>\({R_{p,i}}\)</span>= the ventilation rate per person, m³/s-person
-
-<span>\({P_i}\)</span>  = the number of occupants for the zone
-
-<span>\({R_{a,i}}\)</span>= the ventilation rate per floor area, m³/s-m²
-
-<span>\({A_i}\)</span>  = the floor area of the zone, m²
-
-<span>\(i\)</span>    = the index of the zone or zone list
-
-Next, the i-th zone outdoor air flow is calculated:
-
-<div>$${V_{oz,i}} = {V_{bz,i}}/{E_i}$$</div>
-
-Where:
-
-<span>\({V_{oz,i}}\)</span>= the zone outdoor air flow, m³/s
-
-<span>\({E_i}\)</span>= the zone air distribution effectiveness, see following figure for ASHRAE recommended values.
-
-![](media/image4716.png)
-
-Figure 195. Zone Air Distribution Effectiveness Typical Values (Source: ASHRAE Standard 62.1-2010)
-
-#### Calculation of system minimum outdoor air flow
-
-For single zone systems, the system outdoor air flow,
-
-<div>$${V_{ot}} = {V_{oz}}$$</div>
-
-For 100% outdoor air multi-zone systems, the system outdoor air flow,
-
-<div>$${V_{ot}} = \mathop \sum \limits_{i = 1}^{allzones} {V_{oz,i}}$$</div>
-
-For non 100% outdoor air multi-zone systems, the system outdoor air flow,
-
-<div>$${V_{ot}} = {V_{ou}}/{E_v}$$</div>
-
-Where:
-
-<span>\({V_{ou}}\)</span> the uncorrected system outdoor air flow, m³/s
-
-<div>$${V_{ou}} = \mathop \sum \limits_{i = 1}^{allzones} ({R_{p,i}} \times {P_i}) + \mathop \sum \limits_{i = 1}^{allzones} ({R_{a,i}} \times {A_i})$$</div>
-
-<span>\({X_s}\)</span> = the uncorrected system outdoor air fraction
-
-<div>$${X_s} = {V_{ou}}/{V_{ps}}$$</div>
-
-<span>\({V_{ps}}\)</span>= the system supply air flow, m³/s
-
-<span>\({Z_{d,i}}\)</span> = the zone outdoor air fraction
-
-<div>$${Z_{d,i}} = {V_{oz,i}}/{V_{dz,i}}$$</div>
-
-<span>\({V_{dz,i}}\)</span> = the zone supply air flow, m³/s
-
-<span>\({E_v}\)</span> = the system ventilation efficiency, determined as the minimum of the zone ventilation efficiency among all ventilation zones served by the air handler.
-
-*Ev*= minimum (*Evz*)
-
-*Evz*  = the zone ventilation efficiency, determined differently for single-path and multi-path systems.
-
-***For single-path systems,***
-
-Evz= 1+ Xs– Z<sub>d,i</sub>
-
-***For multi-path systems,***
-
-*Evz =* *(Fa+ Xs·Fb– Z<sub>d,i</sub>·Ep·Fc)/Fa*
-
-where system air fractions *Fa*, *Fb*, and *Fc*are determined as follows
-
-*Fa= Ep+* *(1 – Ep) ·Er*
-
-*Fb= Ep*
-
-*Fc= 1 –* *(1 – Ez) · (1 – Er) · (1 – Ep)*
-
-*Ep   =* the zone primary air fraction. For dual-fan dual-duct systems, the zone primary air is the air from the cold duct.
-
-*Ep= Vpz/Vdz,i*
-
-*Er*   = the zone secondary recirculation fraction
-
-Single-path systems are special cases of multi-path systems where *Er* = 0, *Ep* = 1, *Fa* = *Fb =* *Fc* = 1.0
-
-The zone secondary recirculation fraction Er is determined by the designer based on system configuration. For plenum return systems with secondary recirculation (e.g., fan-powered VAV with plenum return) Er is usually less than 1.0, although values may range from 0.1 to 1.2 depending upon the location of the ventilation zone relative to other zones and the air handler. For ducted return systems with secondary recirculation (e.g., fan-powered VAV with ducted return), Er is typically 0.0, while for those with system-level recirculation (e.g, dual-fan dual-duct systems with ducted return) Er is typically 1.0. For other system types, Er is typically 0.75.
-
-The program then calculates the minimum outdoor air flow fraction based on the information provided in the object Controller:MechanicalVentilation and the maximum branch air flow rate as follows:
-
-MechVentOutsideAirMinFrac = <span>\({V_{ot}}\)</span> RhoStd / <span>\(\dot m{_{maxbranch}}\)</span>here:
-
-MechVentOutsideAirMinFrac = outdoor air minimum fraction based on all zones specified in the Controller:MechanicalVentilation object
-
-Controller:OutdoorAir controls the amount of outdoor ventilation air introduced via the mixed air box based on several user inputs. The user can define the minimum outdoor air flow rate as a percentage of the system’s supply air flow rate (e.g., for a variable-air volume system) or a fixed minimum outdoor air flow rate (not as a percentage but a fixed value) (field MinimumLimit). DCV, using the Controller:MechanicalVentilation object in conjunction with the Controller:OutdoorAir object, allows a third option for setting the minimum outdoor air flow. Economizer operation can also be specified to increase the outdoor air flow above the minimum flow rate to provide free cooling when conditions permit (Controller:OutdoorAir, field Economizer Control Type).
-
-EnergyPlus uses the largest outdoor air flow rate calculated by the various methods described above when modeling system performance (as long this rate doesn’t exceed the maximum flow rate specified for the main air loop branch or for the outdoor air controller itself).
-
-The method used to calculate the outdoor ventilation air flow rate for each system simulation time step is described in more detail below. The figure below schematically illustrates air flow paths used in the calculation of outdoor air flow rate.
-
-
-
-![](media/image4731.png)
-
-Figure 196.  Demand Control Ventilation -- Air Flow Paths
-
-The minimum outdoor air flow rate is first calculated based on the minimum outdoor air flow rate and the minimum outdoor air schedule value as defined by the user inputs for the object Controller:OutdoorAir:
-
-<div>$${\mathop m\limits^ \bullet_{\min OA}} = \,{\mathop V\limits^ \bullet_{\min OA}} * \,\,MinOAScheduleValue * \,RhoStd\,$$</div>
-
-where:
-
-<span>\({\mathop m\limits^ \bullet_{_{\min OA}}}\)</span>       = minimum outdoor air flow rate for this time step, kg/s
-
-<span>\({\mathop V\limits^ \bullet_{_{\min OA}}}\)</span>        = minimum outdoor air flow rate defined in Controller:OutdoorAir, m<sup>3</sup>/s
-
-*MinOAScheduleValue* = minimum outdoor air schedule value defined by the schedule identified in Controller:OutdoorAir
-
-*RhoStd*      = standard air density (1.204 kg/m<sup>3</sup>) adjusted for the local barometric pressure (standard barometric pressure corrected for altitude, ASHRAE 1997 HOF pg. 6.1).
-
-The outdoor air minimum fraction is then calculated as the ratio of the minimum outdoor air flow rate calculated above to the maximum air flow rate defined in the Branch statement for the main air loop (converted to mass flow rate).
-
-<div>$$OutAirMinFrac = \left( {{\raise0.7ex\hbox{${{{\mathop m\limits^ \bullet  }_{_{\min OA}}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop m\limits^ \bullet  }_{_{\min OA}}}} {{{\mathop m\limits^ \bullet  }_{_{\max branch}}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop m\limits^ \bullet  }_{_{\max branch}}}}$}}} \right)$$</div>
-
-where:
-
-<span>\({\mathop m\limits^ \bullet_{\max branch}}\)</span>    = Max branch air volume flow rate times *RhoStd,* kg/s
-
-The program then calculates the minimum outdoor air flow fraction (*MechVentOutsideAirMinFrac*) according to the VRP based on the information provided in the object Controller:MechanicalVentilation and the maximum branch air flow rate.
-
-The algorithm then uses the larger of these outdoor air minimum fractions in subsequent calculations, and also makes sure that the resulting fraction is between 0 and 1.
-
-<div>$$OutAirMinFrac = \,\,MAX\left( {OutAirMinFrac,MechVentOutsideAirMinFrac} \right)$$</div>
-
-<div>$$OutAirMinFrac = \,\,MIN\left( {MAX\left( {OutAirMinFrac,0.0} \right),\,1.0} \right)$$</div>
-
-The algorithm goes on to determine if economizer operation is possible based on the user inputs and the current conditions of the outdoor air and return air. If conditions permit economizer operation, the outdoor air flow fraction is increased beyond the minimum fraction to meet the mixed air setpoint temperature (setpoint temperature assigned to the node defined in field “Control\_Node� of Controller:OutdoorAir).
-
-<div>$$OAFrac = \,MAX\,(OutAirMinFrac,\,EconomizerOAFrac)$$</div>
-
-The mass flow rate of outdoor air is then calculated based on the outdoor air fraction determined above and the mixed (supply) air mass flow rate:
-
-<div>$${\dot m_{OA}} = OAFrac * {\dot m_{MixedAir}}$$</div>
-
-where:
-
-<span>\({\dot m_{OA}}\)</span>           = mass flow rate of outdoor air, kg/s
-
-<span>\(OAFrac\)</span>    = fraction of outdoor air in the mixed (supply) air stream
-
-<span>\({\mathop m\limits^ \bullet_{MixedAir}}\)</span>     = mass flow rate of the mixture of return air and outdoor ventilation air, kg/s
-
-The algorithm checks to make sure the calculated outdoor air mass flow rate is greater than or equal to the air flow rate being exhausted.
-
-<div>$${\dot m_{OA}} = MAX\left( {{{\dot m}_{OA}},{{\dot m}_{ExhaustAir}}} \right)$$</div>
-
-If a fixed minimum outdoor air flow rate is specified (field Minimum Limit Type in Controller:OutdoorAir) for a continuous air flow system, the program makes sure that the outdoor air mass flow rate is greater than or equal to the minimum outdoor air flow rate specified by the user.
-
-<div>$${\dot m_{OA}} = MAX\left( {{{\dot m}_{OA}},{{\dot m}_{\min OA}}} \right)$$</div>
-
-The outdoor air mass flow rate should be less than or equal to the mixed (supply) air flow rate, and the outdoor air flow rate is reset if necessary.
-
-<div>$${\dot m_{OA}} = MIN\left( {{{\dot m}_{OA}},{{\dot m}_{MixedAir}}} \right)$$</div>
-
-The outdoor air mass flow rate should also be less than or equal to the maximum outdoor air flow rate specified by the user, and the outdoor air flow rate is reset if necessary.
-
-<div>$${\dot m_{OA}} = MIN\left( {{{\dot m}_{OA}},{{\dot m}_{MaxOA}}} \right)$$</div>
-
-where:
-
-<span>\({\dot m_{MaxOA}}\)</span>= maximum outdoor air mass flow rate, kg/s = maximum outdoor air volume flow rate from Controller:OutdoorAir times *RhoStd*
-
-Finally, the relief air flow rate is calculated as the difference between the outside and exhaust air mass flow rates.
-
-<div>$${\dot m_{ReliefAir}} = MAX\left( {{{\dot m}_{OA}} - \,{{\dot m}_{ExhaustAir}}\,,0.0} \right)$$</div>
-
-### Indoor Air Quality Procedure
-
-Like VRP, the user must include the following three objects in their input data file in order to model CO<sub>2</sub>-based DCV with IAQP:
-
-n AirLoopHVAC:OutdoorAirSystem to simulate the mixed air box of the air loop
-
-n Controller:MechanicalVentilation to determine the minimum outside air flow rate to be provided by the mixed air box
-
-n Controller:OutdoorAir to control the outside air flow rate introduced via the mixed air box
-
-The outdoor air mass flow rate provided by the air loop is calculated as below:
-
-<div>$${\dot m_{OA}} = \sum\limits_i^N {{{\dot m}_{OA,z,i}}} $$</div>
-
-where:
-
-<span>\({\dot m_{OA,z,i}}\)</span>= outdoor air mass flow rate for the ith zone as calculated according to section Carbon Dioxide Prediction located elsewhere in this document.
-
-N = number of zones served by the air loop, which is provided in the input for a Controller:MechanicalVentilation object
-
-### Proportional Control
-
-The control has two choices: ProportionalControlBasedonOccupancySchedule and ProportionalControlBasedonDesignOccupancy. The difference is occupancy level. The former uses real time occupancy, while the latter uses design occupancy level. Like Ventilation Rate Procedure and the Indoor Air Quality Procedure, the following three objects must be included in the input data file in order to model CO<sub>2</sub>-based DCV with Proportional Control:
-
-n **AirLoopHVAC:OutdoorAirSystem** to simulate the mixed air box of the air loop
-
-n **Controller:MechanicalVentilation** to determine the minimum outside air flow rate to be provided by the mixed air box
-
-n **Controller:OutdoorAir** to control the outside air flow rate introduced via the mixed air box
-
-For the i-th zone, the outdoor air mass flow rate provided by the air loop is calculated as below:
-
-1)   The required intake flow of outdoor air for the design zone population, *P<sub>z,i</sub>*
-
-<div>$${V_{ot - design,i}} = \frac{{\left( {{R_{p,i}}.{P_{z,i}}} \right) + ({R_{a,i}}.{A_{z,i}})}}{{{E_i}}}$$</div>
-
-2)   The required intake flow of outdoor air when the zone is unoccupied i.e.  *P<sub>z,i</sub>* = 0
-
-<div>$${V_{ot - min,i}} = \frac{{({R_{a,i}}.{A_{z,i}})}}{{{E_i}}}$$</div>
-
-3)   The target indoor CO<sub>2</sub> concentration at <span>\({V_{ot - design,i}}\)</span>
-
-<div>$${C_{s - design,i}} = {C_o} + \frac{N}{{\left( {{V_{ot - design,i}}/{P_{z,i}}} \right)}}$$</div>
-
-4)   The target indoor CO<sub>2</sub> concentration at <span>\({V_{ot - min}}\)</span> is either a user input in the object ZoneControl:ContaminantController or equal to the outdoor CO<sub>2</sub> concentration. The default is outdoor CO<sub>2</sub> concentration.
-
-<div>$${C_{s - min,i}} = {C_o}$$</div>
-
-When the indoor CO<sub>2</sub> concentration equals <span>\({C_{s - design,i}}\)</span>, <span>\({V_{ot}}\)</span> should equal <span>\({V_{ot - design,i}}\)</span>. When the indoor CO<sub>2</sub> concentration equals <span>\({C_{s - min,i}}\)</span>, <span>\({V_{ot}}\)</span> should equal <span>\({V_{ot - min,i}}\)</span>. When the indoor CO<sub>2</sub> concentration is between <span>\({C_{s - min,i}}\)</span> and <span>\({C_{s - design,i}}\)</span>, a controller should adjust outdoor air intake flow <span>\({V_{ot}}\)</span> proportionally between <span>\({V_{ot - min,i}}\)</span> and <span>\({V_{ot - design,i}}\)</span>:
-
-<div>$${V_{ot,i}} = {V_{ot - min,i}} + ({V_{ot - design,i}} - {V_{ot - min,i}})\frac{{({C_{s - actual,i}} - {C_{s - min,i}})}}{{({C_{s - design,i}} - {C_{s - min,i}})}}$$</div>
-
-Where,
-
-<span>\({R_{p,i}}\)</span> = Required outdoor air flow rate per person, (m<sup>3</sup>/s)/person
-
-<span>\({R_{a,i}}\)</span> = Required outdoor air flow rate per unit area, (m<sup>3</sup>/s)/m<sup>2</sup>
-
-<span>\({P_{z,i}}\)</span> = Design zone population, number of people
-
-When ProportionalControlBasedonDesignOccupancy is specified, number of people = design occupancy * current schedule value. When ProportionalControlBasedonDesignOccupancy is specified, number of people = design occupancy.
-
-
-<span>\({A_{z,i}}\)</span> = Zone floor area, m<sup>2</sup>
-
-<span>\({E_i}\)</span> = The zone air distribution effectiveness
-
-<span>\(N\)</span> = CO<sub>2</sub> generation rate, (m<sup>3</sup>/s)/person (Specified in the People object)
-
-<span>\({C_o}\)</span> = CO<sub>2</sub> concentration in the outdoor air, ppm
-
-<span>\({C_{s - design,i}}\)</span> = CO<sub>2</sub> concentration in the space for the design conditions, ppm
-
-<span>\({C_{s - min,i}}\)</span> = Minimum CO<sub>2</sub> concentration in the space, ppm
-
-<span>\({C_{s - actual,i}}\)</span> = Actual CO<sub>2</sub> concentration in the space, ppm
-
-<span>\({V_{ot - design,i}}\)</span> = Required intake of outdoor air flow rate at <span>\({C_{s - design}}\)</span>, (m<sup>3</sup>/s)
-
-<span>\({V_{ot - min,i}}\)</span> = Required intake of outdoor air flow rate at <span>\({C_{s - min}}\)</span>, (m<sup>3</sup>/s)
-
-<span>\({V_{ot,i}}\)</span> = Required intake of outdoor air flow rate at <span>\({C_{s - actual}}\)</span>, (m<sup>3</sup>/s)
-
-Except <span>\({C_{s - min,i}}\)</span> above, all other variables are already available in EnergyPlus (See Eng. Reference for “Ventilation Rate Procedure� above for further details). <span>\({C_{s - min}}\)</span> can be specified in the ZoneControl:ContaminantController object as a schedule. If  <span>\({C_{s - min}}\)</span> is not specified in the ZoneControl:ContaminantController object, then outdoor air CO2 concentration will be used as the minimum. In order for “ProportionalControl� to be active, the following conditions must be met, otherwise default “VentilationProcedure� will be modeled and a warning will be issued during runtime:
-
-1)   “Carbon Dioxide Control Availability Schedule Name� input field in the ZoneControl:ContaminantController object must be greater than zero.
-
-2)   CO2 gain from people in the zone must be greater than zero.
-
-3)   “Outdoor air flow per person� and “Outdoor air flow per zone floor area� in the corresponding “DesignSpecification:OutdoorAir� object must be greater than zero.
-
-### References
-
-ASHRAE. 2007. *ANSI/ASHRAE Standard 62.1-2007, Ventilation for acceptable indoor air quality*. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2010. *ANSI/ASHRAE Standard 62.1-2010, Ventilation for acceptable indoor air quality*. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Emmerich, S.J. and A.K. Persily. 1997. Literature review on CO<sub>2</sub>-based demand-controlled ventilation. *ASHRAE Transactions* 103(2):229-243.
-
-Schell, M.B., S.C. Turner, R.O. Shim. 1998. Application of CO<sub>2</sub>-based demand controlled ventilation using ASHRAE Standard 62-1989. *ASHRAE Transactions* 104(2):1213-1225.
-
-Schell, M. and D. Int-Hout. 2001. Demand control ventilation using CO<sub>2</sub>. *ASHRAE Journal*, February.
-
-Evaporative Coolers <a name="EvapCoolers"></a>
--------------------
-
-This section describes the evaporative coolers models for HVAC in EnergyPlus.
-
-### Direct Evaporative Cooler
-
-The input object EvaporativeCooler:Direct:CelDekPad provides a model of a direct stage evaporative cooler, shown in the figure below, that consists of a rigid media evaporative pad, with water recirculated from a reservoir.  The water is pumped from the reservoir to a water distribution header, for water feed by gravity from above the media.  The evaporative pad provides the area for the adiabatic saturation of the air.  While the process provides a lower dry-bulb temperature, the moisture content of the leaving air is higher than the entering condition.  The direct stage is used for comfort cooling in a building where adding humidity to the air can be tolerated.
-
-![](media/image4789.png)
-
-Figure 197.  Direct Stage Evaporative Cooler
-
-The thermodynamic process is a simultaneous heat and mass transfer, or adiabatic cooling, and follows a constant enthalpy line on the psychrometric chart; it is shown in the figure below as a process from A to B.  Since the deviation of the constant wet-bulb line and the constant enthalpy line is small, it is assumed that the wet-bulb temperature is constant across the direct evaporative stage.
-
-![](media/image4790.png)
-
-Figure 198.  Psychrometric Chart -- Constant Enthalpy
-
-If the direct evaporative process were 100% efficient, the leaving dry-bulb temperature would equal the entering wet-bulb temperature.  The efficiency of the direct evaporative process is less than 100% and by defining saturation efficiency (ese) for the direct stage or evaporative pad, the leaving dry-bulb temperature can be expressed by the following equation.
-
-<div>$${T_{dbsupout}} - {T_{dbsupin}} = {\varepsilon_{se}} \cdot \left( {{T_{odb}} - {T_{owb}}} \right)$$</div>
-
-#### Saturation Efficiency
-
-Since the evaporative process is not 100% efficient the saturation efficiency is defined by.
-
-<div>$${\varepsilon_{se}} = \frac{{{T_{dbsupin}} - {T_{dbsupout}}}}{{{T_{odb}} - {T_{owb}}}}$$</div>
-
-The saturation efficiency is determined from manufacturer's data, and the least squares curve fit is discussed in Curve Fitting Evaporative Media section.
-
-Using the saturation efficiency (ese) for the direct stage evaporative pad, the leaving dry-bulb temperature can be determined directly.  The evaporative process approximately follows a constant wet-bulb line.  Therefore, with the leaving dry-bulb temperature and assuming adiabatic heat transfer across the direct stage, the outlet conditions for the direct stage are known.
-
-The saturation efficiency of the direct evaporative cooler is a function of the pad geometry and airflow rate.  The pad geometry is constant throughout the simulation, but the airflow rate can change from hour to hour when the evaporative cooler is used with an air economizer.  The saturation efficiency would then be determined from the flow for that hour with the geometry of the direct evaporative cooler.  This gives the dry-bulb temperature leaving the evaporative cooler.  Assuming adiabatic heat transfer across the direct stage, the evaporative process follows the constant wet-bulb line or the constant enthalpy line on the psychrometric chart, therefore the wet-bulb temperature is constant from inlet to outlet.
-
-Some things that can cause departure from the ideal adiabatic saturation process in the direct evaporative cooler are:
-
-·        makeup water entering the sump,
-
-·        friction from water re-circulation,
-
-·        heat transfer from surroundings,
-
-·        solar radiation (sun upon a cooler).
-
-Thus, adiabatic saturation in evaporative cooling is only an approximation, however the adiabatic saturation assumption in the rigid-media cooler is good, since the water recirculates rapidly and approximates the wet-bulb temperature at steady state operation.
-
-#### Curve Fitting Evaporative Media
-
-The saturation efficiency is usually reported as a function of airflow, pad face velocity, and pad thickness.  The Figure below shows a typical graph of manufacturer's data for the saturation efficiency.  A multi-variate least squares curve fit of the data was used to generate saturation efficiency functions for the evaporative models that use the CelDek rigid media pad.
-
-![](media/image4793.png)
-
-Figure 199.  Graph of Saturation Efficiency
-
-The curve fit for saturation efficiency was obtained using the functions listed below.  The model uses the air velocity (Airvel) through the pad and the depth of the media (Depth).  The least squares routine produced the following model that is used for the evaporative cooling rigid media pad.  The least squares routine produced an eleven-term multi-variate fit using a third order quadratic.
-
-ese = 0.792714 + 0.958569 (Depth) - 0.25193 (Airvel) - 1.03215 (Depth<sup>2</sup>) + 0.0262659 (Airvel<sup>2</sup>) + 0.914869 (Depth \* Airvel) - 1.48241 (Airvel \* Depth<sup>2</sup>) - 0.018992 (Airvel<sup>3</sup> \* Depth) + 1.13137 (Depth<sup>3</sup> \* Airvel) + 0.0327622 (Airvel<sup>3</sup> \* Depth<sup>2</sup>) - 0.145384 (Depth<sup>3</sup> \* Airvel<sup>2</sup>)
-
-Where Airvel is in meters per second and Depth is in meters.  This curve fit is used for the rigid media in the EvapCooler:Direct:CelDekPad and EvapCooler:InDirect:CelDekPad.
-
-### Dry Coil Indirect Evaporative Cooler
-
-The input object EvaporativeCooler:Indirect:CelDekPad provides a model of a dry coil indirect evaporative cooler, shown in the figure below, that has a rigid media pad, similar to the direct evaporative stage, where the adiabatic cooling takes place.  The secondary air leaves the rigid media pad and enters an air-to-air heat exchanger where it cools the supply air flowing through the heat exchanger tubes.  The moist secondary air is then exhausted to the environment.  The secondary air stream has its own fan and includes consists of a rigid media evaporative pad, with water recirculated from a reservoir.  The water is pumped from the reservoir to a water distribution header, for water feed by gravity from above the media.  The evaporative pad provides the area for the adiabatic saturation of the air.
-
-![](media/image4794.png)
-
-Figure 200.  Evaporative Cooler -- Indirect Dry Coil
-
-The process that the secondary air goes through, A to C to D, is shown by the dashed lines in  the following figure.  Process A to C is adiabatic cooling in the rigid media pad.  Then the air enters the shell side of the heat exchanger and is sensibly heated from C to D by the warm supply air passing through the tube side.
-
-![](media/image4795.png)
-
-Figure 201.  Secondary Air Process -- Indirect Dry Coil Evap Cooler
-
-The advantage of the dry coil heat exchanger is that the heat exchanger does not have the evaporation taking place on the outside of the tubes, thus no mineral deposits are left on the heat exchange surface to reduce the efficiency of the heat exchanger.  The rigid media pads are designed to flush the mineral deposits to the sump, so the saturation efficiency of the pad stays relatively constant.
-
-The following equations are used to determine the dry-bulb temperature leaving the evaporative media, given pad geometry and secondary airflow information.  The heat transfer in the heat exchanger can be determined with the effectiveness of the heat exchanger according.
-
-Tdb sup out = Tdb sup in - ese\*(Todb - Towb )
-
-QHx = eHx \* Min( CFMsec , CFMsupply) \* rair \* cp air \* ( Todb - Tdb sec out)
-
-After the heat transfer for the heat exchanger has been determined, an energy balance is done on the supply airside to determine the dry-bulb temperature leaving the indirect evaporative cooler.  This assumes all the energy for is provided by the primary air stream so the effectiveness value includes the air-to-air effectiveness of the heat exchanger.
-
-Tdb sup out =  Tdb sup in   -  <span>\(\frac{{{Q_{Hx}}}}{{{r_{air}}*{c_{pair}}*CF{M_{\sup ply}}}}\)</span>
-
-The wet-bulb temperature is determined from psychrometric routines using the leaving dry-bulb temperature, humidity ratio, and barometric pressure, since humidity ratio is constant for the supply air across the indirect stage.  The effectiveness of the heat exchanger is determined from a parameter estimation using manufacturer's performance data.  For the indirect evaporative cooler it was found that a value of 0.67 represented reasonable default effectiveness.
-
-### Wet Coil Indirect Evaporative Cooler
-
-The input object EvaporativeCooler:Indirect:WetCoil provides a model for a wetted coil evaporative cooler, shown in the figure below, that has water sprayed directly on the tubes of the heat exchanger where latent cooling takes place.  The vaporization of the water on the outside of the heat exchanger tubes allows the simultaneous heat and mass transfer which removes heat from the supply air on the tube side.  Then the moist secondary air is exhausted.  The secondary air stream has its own fan.
-
-
-
-![](media/image4797.png)
-
-Figure 202.  Wet Coil Indirect Evaporative Cooler
-
-The process that the secondary air goes through, A to C on the following figure, is a path of simultaneous heat and mass transfer, but it does not follow a line of constant enthalpy as in the direct stage.  The process is not adiabatic due to the heat gain from the supply air flowing through the tubes of the heat exchanger.
-
-![](media/image4798.png)
-
-Figure 203.  Secondary Air Process – Indirect Wet Coil Evaporative Cooler
-
-The wet coil heat exchanger can have a higher stage efficiency than the dry coil due to a higher heat transfer rate on the outside of the heat exchanger tubes.  Over the operating lifetime of the heat exchanger, the vaporization taking place on the heat exchange surface can leave mineral deposits that will decrease the effectiveness of the heat exchanger.
-
-#### Efficiencies of the Indirect Stage
-
-In an indirect stage of an evaporative cooler, the secondary or wet side air stream acts as a heat sink for the supply air.  The efficiency of the indirect stage is given as the effectiveness of the sensible heat exchange, eHx, and the saturation efficiency on the wet streamside, ese.  These are expressed as:
-
-eHx = <span>\(\frac{q}{{{q_{max}}}}\)</span>=  <span>\(\frac{{{C_{sup}}({T_{supin}} - {T_{supout}})}}{{{C_{min}}({T_{secin}} - {T_{secout}})}}\)</span>,
-
-ese =  <span>\(\frac{{{T_{dbsecin}} - {T_{dbsecout}}}}{{{T_{odb}} - {T_{owb}}}}\)</span>,
-
-where Tdb sup in = Tdb sec in  for the indirect cooler.  The maximum heat transfer possible would be obtained if the supply stream was cooled all the way to the wet-bulb temperature.  So the efficiency of the indirect evaporative cooler is defined by:
-
-eind =  <span>\(\frac{{({T_{dbsupin}} - {T_{dbsupout}})}}{{({T_{odb}} - {T_{owb}})}}\)</span>.
-
-Using the combination of the effectiveness and saturation efficiency, the total efficiency of the indirect stage can be expressed by:
-
-eind = eHx  ese  <span>\(\frac{{{C_{sup}}}}{{{C_{min}}}}\)</span>.
-
-In many cases Csup = Cmin and the efficiency of the indirect stage reduces to:
-
-eind = eHx  ese.
-
-An intuitive model determining the performance of the wet coil indirect model was developed.  This model can be used for all indirect models by curve fitting data from the evaporative cooler of interest.  The model development starts with the total efficiency of the indirect evaporative cooler:
-
-eind =  <span>\(\frac{{({T_{dbsupin}} - {T_{dbsupout}})}}{{({T_{odb}} - {T_{owb}})}}\)</span>
-
-Solving for T db sup out gives the leaving conditions of the supply air at a constant humidity ratio:
-
-T db sup out = Tdb sup in - eind \* (Todb - Towb)
-
-A form for the efficiency of the indirect stage was devised using a maximum efficiency with a coefficient to reduce the efficiency depending on the ratio of the airflows.
-
-eind = emax - C1 \* (<span>\(\frac{{CF{M_{sup}}}}{{CF{M_{sec}}}}\)</span>)
-
-C1 is the "Flow Efficiency Ratio" and is determined from performance data.
-
-A check of limits will verify that it makes physical sense.  As the magnitude of the secondary flow increases, the second term of equation above becomes smaller.  This would make the efficiency tend to go to the maximum efficiency.  Physically this would be true since the convective terms for heat and mass transfer would increase on the outside of the tube with the additional mass flow rate.  Similarly, if the supply air flow goes to zero with a constant secondary air flow, the second term of the equation above again becomes small, and the overall efficiency of the stage would approach the maximum.  The constant C1 tells how quickly the efficiency of the stage would decrease with a mismatch of the supply and secondary flows.
-
-The maximum efficiency of the stage is a combination of the efficiency due to the simultaneous heat and mass transfer on the outside of the tube and the efficiency of the heat exchanger.  This value can be higher than the dry coil overall efficiency since the convective coefficients on the outside of the tube are larger.  For example, a least squares fit for the maximum efficiency showed this value was approximately 0.8 compared to the dry coil indirect value of approximately 0.65 (0.67 \* 0.97).  (The maximum efficiency for the dry coil indirect was determined at the condition where flow through the evaporative pad in the secondary air stream approached zero, for a 12-inch thick pad.)  It should be noted again that over the operating life of the wet coil heat exchanger, the mineral deposits that are left can decrease the effectiveness of the heat exchanger unless appropriate maintenance has taken place.  Therefore, if modeling an older system, the manufacturer’s data may no longer describe the equipment effectiveness.
-
-### Two Stage Direct/Indirect Evaporative Cooler
-
-A two stage cooler can be modeled by combining either a wet coil or the dry coil indirect evaporative cooler staged with a direct evaporative cooler.  The figure below shows a dry coil indirect evaporative cooler with a direct evaporative cooler.  This configuration is mainly used for total comfort cooling for a building and would not normally be used as a pre-cooler for a refrigeration coil, since the direct stage would increase the latent load on a refrigeration coil.
-
-![](media/image4806.png)
-
-Figure 204.  Two Stage Evaporative Cooler
-
-The thermodynamic process for the supply air is shown below, going from A to B to C.  The process from A to B is sensible cooling in the indirect stage.  The process from B to C is simultaneous heat and mass transfer following a constant enthalpy line.  The air leaving the final stage has a lower dry-bulb and wet-bulb temperature, and an increase in moisture from the direct stage.
-
-![](media/image4807.png)
-
-Figure 205.  Thermodynamic Process for Supply Air Through Two Stage Evaporative Cooler
-
-Two stage evaporative coolers can be accomplished by putting the EvaporativeCooler:Direct:CelDekPad, EvaporativeCooler:Indirect:CelDekPad, EvaporativeCooler:Indirect:WetCoil in series in any combination the user desires in the supply air loop.
-
-### Indirect Evaporative Cooler Special Research Model
-
-This section summarizes the model implemented in the component EvaporativeCooler:Indirect:ResearchSpecial.  Examples of this evaporative cooler are shown in the following figures, without and with a relief valve. This model differs from the other indirect evaporative coolers in that, under part load conditions, it can modulate so that the air leaving the cooler just meets a drybulb temperature setpoint.
-
-The indirect research special evaporative cooler (IEC) machine provides improved modeling features needed for data center and other hybrid cooling applications.  The new model includes performance curves for variable effectiveness, fan power, and pump power.  It is intended to be able to model IEC machines that have 1) variable speed secondary fans, 2) variable speed pumps for water recirculation and spraying, and 3) ability to operate in a dry mode.  Such IEC machines can modulate the cooling power during operation by varying either the secondary side fan speed or the intensity of water spray or both.  To simplify the model it is assumed that the device’s internal controls are such that, when it is operating as a “Wet� evaporative cooler, secondary fan and spray pump operation are linked together so that there is a one-to-one mapping between them at any given part load situation.  This allows formulating the fan and pump power performance curves to be based on the same independent variable, secondary air flow fraction.
-
-![figure 166 renamed](media/image4808.png)
-
-Figure 206. Research Special Indirect Evaporative Cooler
-
-#### Model Formulation
-
-Each time the model is called it takes the inputs on the left and produces the outputs on the right as shown in [Figure](#IndEvapCoolerFig2). “sys� is primary air stream and typically sits on an AirLoop HVAC branch. “sec� is secondary purge air stream and is typically outdoor air.  The model will set node flow rates and “out_sec� state variables on the secondary outlet. 
-
-![](media/image8005.png)
-
-Figure: Illustration of Inputs-Outputs of Indirect Evaporative Cooler Research Special <a name="IndEvapCoolerFig2"></a>
-
-The model runs either in dry mode or wet mode depending entering air conditions of the primary and secondary air sides. Different effectiveness values are used depending on the operating modes.
-
-#### Wet Mode Operation
-
-If running “wet,� use wet bulb effectiveness and wet bulb temperature depression for delta T:
-
-<div>$$  \begin{array}{rl}
-  \epsilon_{wb,op} &= \epsilon_{wb,design}\cdot f_{wb,mod}\left(\text{flowRatio}\right) \\
-  \text{flowRatio} &= \frac{\dot{m}_{sec}}{\dot{m}_{sys}}
-\end{array}$$</div>
-
-Where:
-
-* <span>\(\epsilon_{wb,op}\)</span> = current operation effectiveness with respect to wet bulb temperature depression.
-
-* <span>\(\epsilon_{wb,design}\)</span> = user input for effectiveness at design air flow rates and full spray power
-
-* <span>\(f_{wb,mod}\)</span> = normalized wet mode operation effectiveness modifier performance curve as a function of flow fraction. The curve value describes how effectiveness varies at different flow rates.  When conditions are appropriate, this curve is numerically inverted to find a FlowRatio that just meets a setpoint. 
-
-* <span>\(\dot{m}_{sys}\)</span> = primary air current time step mass flow rate in kg/s
-
-* <span>\(\dot{m}_{sec}\)</span> = secondary air current time step mass flow rate in kg/s
-
-The leaving primary air dry bulb temperature in wet operating mode is calculated as follows:
-
-<div>$$ T_{db,out,sys} = T_{db,in,sys} - \epsilon_{wb,op} \left( T_{db,in,sys} - T_{wb,in,sec} \right) $$ </div>
-
-Then check that there is sufficient heat capacitance flux (mcT) in the secondary air stream to provide the conditioning.  The following steps are for checking and adjusting for non-physical outcomes that could happen with low secondary flow rates.
-
-1. Calculate heat transfer rate
-
-The secondary air entering wet-bulb temperature would be the loswest limit allowed, although this temperature cannot be attained in most practical situations.  This is checked as a limiting case.
-
-<div>$$
-  \begin{array}{rl}
-    T_{db,out,sys} &= \max\left(T_{db,out,sys},T_{db,out,setpoint}\right) \\
-    \dot{Q}_{HX} &= \left(\dot{m}c_p\right)_{sys,in} \cdot \left(T_{db,in,sys}-T_{db,out,sys}\right)
-  \end{array}
-$$</div>
-
-2. Calculate outlet enthalpy of the secondary air
-
-<div>$$
-  \text{enahalpy}_{out,sec} = \text{enthalpy}_{in,sec} + \frac{\dot{Q}_{HX}}{\dot{m}_{sec}}
-$$</div>
-
-One approximation that can be made is the outlet condition of the temperature and humidity ratio combination that produces the outlet enthalpy of the secondary air calculated above.  A conservative approach is that the secondary air leaves with water added at such a rate that it results in the secondary air to leave at the same dry bulb temperature and all the total heat transfer results in humidity ratio increases, i.e., latent heat transfer. Following this assumption the secondary air outlet humidity ratio can be calculated in step 3. 
-
-3. Calculate outlet humidity ratio of the secondary air
-
-<div>$$
-  \begin{array}{rl}
-    T_{db,out,sec} &= T_{db,in,sec} \\
-    \text{HumRat}_{out,sec} &= \text{PsyWFnTbH}\left(T_{db,out,sec},\text{enthalpy}_{out,sec}\right) \\
-    \dot{V}_{water} &= \frac{QHX / \left[ \left(\text{HumRat}_{out,sec}-\text{HumRat}_{in,sec}\right) \cdot h_{fg,in,sec}\right]}{\rho_{water,Tdb,in,sec}} \\
-    or &= \\
-    \dot{V}_{water} &= \frac{QHX / \left[ \left(\text{enthalpy}_{out,sec}-\text{enthalpy}_{in,sec}\right) \right]}{\rho_{water,Tdb,in,sec}}
-  \end{array}
-$$</div>
-
-Dry Operation Mode
-
-Similarly, if running “dry� use dry bulb effectiveness and dry bulb based delta T
-
-<div>$$ \epsilon_{db,op} = \epsilon_{db,design} \cdot f_{db,mod}\left(\text{flowRatio}\right) $$</div>
-
-Where:
-
-* <span>\(\epsilon_{db,op} \)</span> = current operation effectiveness with respect to dry bulb temperature depression.
-
-* <span>\(\epsilon_{db,design} \)</span> = user input for effectiveness at design air flow rates and dry operation mode (no water spray on the secondary air side)
-
-* <span>\(f_{db,mod} \)</span> = normalized dry mode operation effectiveness modifier performance curve as a function of flow fraction.  The curve value describes how the dry mode effectiveness varies with different flow rates.  When conditions are appropriate, this curve is numerically inverted to find a FlowRatio that just meets a setpoint 
-
-The leaving primary air dry bulb temperature in dry operating mode is calculated as follows:
-
-<div>$$T_{db,out,sys} = T_{db,in,sys} - \epsilon{db,op}\left(T_{db,in,sys}-T_{db,in,sec}\right)$$</div>
-
-Then check that there is sufficient heat capacitance flux (mcT) in the secondary air stream to provide the conditioning.  For dry operation, it should be sufficient to simply use inlet moist air properties for density and specific heat.  The following steps are for checking and adjusting for non-physical outcomes that could happen with low secondary flow rates.
-
-1. Calculate heat transfer
-
-<div>$$ \dot{Q}_{HX} = \left(\dot{m}c_{p}\right)_{sys,in} \left(T_{db,in,sys}-T_{db,out,sys}c\right) $$</div>
-
-2. Calculate secondary/scavenger leaving dry-bulb
-
-<div>$$ T_{db,out,sec} = T_{db,in,sec} + \frac{\dot{Q}_{HX}}{ \left(\dot{m}c_{p}\right)_{sys,in}} $$</div>
-
-3. Check for energy imbalance and adjust if need
-
-<div>$$ \text{IF} \left(T_{db,out,sec}>T_{db,in,sys}\right) \text{THEN} T_{db,out,sec} = T_{db,in,sys}-0.2 C $$</div>
-
-4. Recalculate heat transfer limit if imbalance found in step 3 using new secondary outlet drybulb
-
-<div>$$ \dot{Q}_{HX,lim} = \left(\dot{m}c_{p}\right)_{sec,in}\cdot \left( T_{db,out,sec}-T_{db,in,sec} \right) $$</div>
-
-5. Recalculate leaving supply air dryblub using new heat transfer rate from step 4
-
-<div>$$ T_{db,out,sys} = T_{db,in,sec} + \frac{\dot{Q}_{HX}}{ \left(\dot{m}c_{p}\right)_{sys,in}} $$</div>
-
-The IEC in dry and wet operating mode transfers no moisture to the primary system air, so the humidity ratio remains the same:
-
-<div>$$\text{HumRat}_{out,sys} = \text{HumRat}_{in,sys}$$</div>
-
-#### Secondary Air Flow Fraction
-
-The secondary air mass flow rate will either be set to <span>\(\dot{m}_{sec}\)</span> or solved for numerically as described below. The secondary side flow fraction, <span>\(ff_{sec}\)</span>, is defined as.  (Note this is another flow ratio that differs from the one used above which combined both streams into one ratio in effectiveness modifier curves.)  
-
-<div>$$ff_{sec} = \frac{\dot{m}_{sec}}{\dot{m}_{sec,design}}$$</div>
-
-The secondary air mass flow rate will either be set to  or solved for numerically as described below. The secondary side flow fraction, , is defined as.  (Note this is another flow ratio that differs from the one used above which combined both streams into one ratio in effectiveness modifier curves.)  
-
-<div>$$P_{sec,fan} = P_{sec,fan,design}\cdot f_{sec,fan,mod}\left(ff_{sec}\right) $$</div>
-
-Where:
-
-<span>\(P_{sec,fan} \)</span> = secondary air fan electric power value at current secondary air flow rate in W.
-
-<span>\(P_{sec,fan,design} \)</span> = secondary air fan electric power value at design air flow rate in W.
-
-<span>\(f_{sec,fan,mod} \)</span> = secondary air fan power modifier normalized performance curve as a function of secondary air flow fraction.
-
-<span>\(\dot{m}_{sec,design} \)</span> = secondary air design mass flow rate in kg/s
-
-Recirculation and spray pump electric power is calculated using design pump electric power and a normalized pump power modifier performance curve that describes how power varies as a function of the secondary air flow fraction is given by:
-
-<div>$$P_{pump} = P_{pump,design}\cdot f_{pump,mod}\left(ff_{sec}\right) $$</div>
-
-Where:
-
-<span>\(P_{pump} \)</span> = recirculation and spray pump power value at current operation in W.
-
-<span>\(P_{pump,design} \)</span> = recirculation and spray pump power value at design air flow rate in W.
-
-<span>\(f_{pump,mod} \)</span> = recirculation and spray pump power modifier normalized performance curve as a function of secondary air flow fraction.
-
-User specified three operating temperature limits are included in the model.  These allow controlling when operation should shift from wet to dry and when the cooler should just be shut down because the outdoor conditions are too warm or too wet to do anything beneficial. 
-
-<span>\(T_{db,evapMinLimit} \)</span> = Evaporative Operation Minimum Limit Outdoor Drybulb Temperature, user input.  Shut down wet mode with outdoor temperature is lower than this limit, typically shifting to dry mode.  
-
-<span>\(T_{wb,evapMaxLimit} \)</span> = Evaporative Operation Maximum Limit Outdoor Wetbulb Temperature, user input.  Shut down fan and pump and don’t operate when outdoor Wetbulb is higher than this limit.  The wet bulb is maybe warmer than the return air and attempting evaporative cooling is wasteful. 
-
-<span>\(T_{db,evapMaxLimit} \)</span> = Dry Operation Maximum Limit Outdoor Drybulb Temperature, user input.  Shut down dry operation attempts and don’t operate secondary fan when outdoor dry bulb is higher than this limit.  The dry bulb is maybe warmer than the return air and attempting to do heat exchange is wasteful. 
-
-Algorithm to determine cooler operation proceeds as follows
-
-1. Retrieve leaving setpoint, <span>\(T_{db,out,setpoint}\)</span>
-
-2. Calculate leaving dry bulb for max cooling power available at full secondary air flow rate for dry operation, <span>\(T_{db,out,sys,dry,min}\)</span>
-
-3. Check if dry operation limit (input field called Evaporative Operation Minimum Limit Outdoor Dry-Bulb Temperature) reached, <span>\(T_{db,in,sec}<T_{db,evapMinLimit}\)</span>
-
-4. If dry limit not exceeded, then leaving dry bulb for max cooling power available at full secondary air flow rate for wet operation, <span>\(T_{db,out,sys,wet,min}\)</span>
-
-5. Compare setpoint temperature needed to temperatures available, evaluate limits and choose which case for operation is called for. The following table outlines the five cases in order of increasing cooling power.
-
-INSERT TABLE
-
-“Modulated� cases solve for a secondary flow rate using numerical method, such as regula falsi.  Residual is formulated by a difference between the dry bulb temperature leaving the cooler and the setpoint.  As the solver progress it varies flow rate on the secondary side until the setpoint is met.  For each iteration, a new effectiveness is calculated as a function of Flow Ratio.  The new flow is used for the <span>\(\left(\dot{m}c_{p}\right)_{min}\)</span> term and the new effectiveness is used to calculate a result for leaving drybulb.  The numerical method is the same for dry and wet operation, only the functions will use different curves and state variables to describe performance. The regula falsi solver can vary secondary flow rate, <span>\(\dot{V}_{sec}\)</span>, to drive the following residual to zero:
-
-<div>$$\text{residual} = T_{db,out,sys} - T_{db,out,setpoint}$$</div> 
-
-“Dry or Wet Op Modulated� is the most complex situation.  There is an overlap and the cooler could deliver the setpoint air using either dry operation or wet operation.  The model proceeds separately to calculate both wet and dry operation, with separate numerical solvers for modulation in each mode.  Then the fan and pump power is calculated for each mode.  Select the lowest power mode as the preferred choice.  (This doesn’t really count the value of water, could bring in a source factor but …). Discard results for the unused mode. 
-
-The purge air, or secondary airside, is the stream that evaporates water and indirectly cools the primary, or system air.  The result from Equation is then compared to a lower bound, <span>\({T_{db,out,bound}}\)</span>, determined from the dewpoint of the incoming purge air using Equation .
-
-<div>$${T_{db,out,bound}} = {T_{db,in,sys}} - \beta ({T_{db,in,sys}} - {T_{dew,in,purge}})$$</div>
-
-where,
-
-<span>\({T_{dew,in,purge}}\)</span>  is the dewpoint of purge air entering the wet side of cooler [ºC]
-
-<span>\(\beta \)</span>              is a factor for how close to dewpoint is possible (eg. 0.9)
-
-The final result (for PLF = 1) is the larger of the results from Equations and .
-
-The indirect cooler has the ability to overcool the air and therefore needs some form of modulation.  A Part Load Fraction, PLF, is used to model the implications of controlling the amount of cooling.  It is assumed that through on/off cycling that the cooling power can be varied to exactly meet the desired temperature when PLF is less than unity.
-
-<div>$${\dot Q_{Full}} = \dot m\left( {{h_{out,sys}} - {h_{in,sys}}} \right)$$</div>
-
-<div>$${\dot Q_{{\mathop{\rm Re}\nolimits} quired}} = \dot m\left( {{h_{out,desired}} - {h_{in,sys}}} \right)$$</div>
-
-<div>$$PLF = \frac{{{{\dot Q}_{{\mathop{\rm Re}\nolimits} quired}}}}{{{{\dot Q}_{Full}}}}$$</div>
-
-where,
-
-<span>\(PLF\)</span>                     is the Part Load Fraction
-
-When PLF is less than 1.0 it is assumed that the cooler will deliver the desired temperature air (as long as it is less than the inlet; it doesn’t need heating).  The PLF is used to modify the auxiliary fan power when the fan power modifier curve is not specified and find when the unit will overcool.
-
-<div>$${P_{fan}} = \Delta P\cdot \dot V\cdot e\cdot PLF$$</div>
-
-Water pump power is also derated using the PLF.
-
-A third air stream input to the cooler was implemented in order to allow mixing building exhaust air with outdoor air on the purge/secondary side of the cooler. The assumption when relief/tertiary air is used is that all of the available relief zone air is used and the remainder made up with outdoor air.  Moisture and energy balances are drawn to compute humidity ratio and enthalpy of mixed secondary air.  The volume is determined by the design volume flow rate (from secondary fan size).
-
-#### Water Consumption
-
-Water consumption is an important consideration when evaluating evaporative coolers.  Water consumption of the evaporative cooler is modeled using Equation .
-
-<div>$${\dot V_{water}} = {\dot V_{evap}} + {\dot V_{drift}} + {\dot V_{blowdown}}$$</div>
-
-The three components of water consumption are evaporation, drift, and blowdown.  Evaporation is the water evaporated as the normal part of the evaporative cooler thermodynamic process and is calculated using:
-
-<div>$${\dot V_{evap}} = \frac{{{{\dot Q}_{IEC}}}}{{{\rho_{water}}{h_{fg}}}}$$</div>
-
-where,
-
-<span>\({\dot V_{evap}}\)</span> is the volume flow rate of useful water evaporation [m<sup>3</sup>/s]
-
-<span>\({h_{fg}}\)</span> is the heat of vaporization of water (taken as 2,500,000 J/kg)
-
-<span>\({\dot Q_{IEC}}\)</span> is the rate of heat transfer calculated as by Equation or Equation [W]
-
-<span>\({\rho_{water}}\)</span> is the density of water [kg/m3]
-
-Drift is water that leaves the secondary side as droplets and does not contribute to the evaporative cooling process in a useful manner.  It is calculated using a user input factor that describes drift as a fraction of <span>\({\dot V_{evap}}\)</span>.
-
-<div>$${\dot V_{drift}} = {\dot V_{evap}} * {f_{drift}}$$</div>
-
-Blowdown is water drained from the sump to counter the build up of solids in the water that would otherwise occur because of evaporation.  It is calculated using a user input factor for the blowdown concentration ratio ,<span>\({R_{concentration}}\)</span> , which is the ratio of solids in in the blowdown water compared to the solids in the fresh makeup water and is limited to values of 2 or higher.  The make up water needed for blowdown is calculated using:
-
-<div>$${\dot V_{blowdown}} = \frac{{{{\dot V}_{evap}}}}{{\left( {{R_{concentration}} - 1.0} \right)}} - {\dot V_{drift}}$$</div>
-
-![figure 167 renamed](media/image4833.png)
-
-Figure 207. Research Special Indirect Evaporative Cooler Using Relief Air
-
-#### Indirect Evaporative Cooler Sizing
-
-The model for the object called EvaporativeCooler:Indirect:ResearchSpecial has a field for the secondary fan flow rate that can be autosized.  
-
-##### Secondary Air DesignFan Flow Rate
-
-The secondary air design flow rate fan is not part of an airstream that is directly modeled in EnergyPlus.  Because the primary side air flows can be autosized as part of the air system, it is convenentconvenient to also scale the size of the secondary flow.   If the cooler is part of the main loop of a central air system, then the secondary fan flow rate is sized to equal to the main design flow rate. 
-
-User inputs for autosizing scaling factors are included so that when modeling an autosized IEC, all the design values can be scaled off of Primary Design Air Flow Rate.  User input for Secondary Air Flow Sizing Factor is multiplied by DesMainVolFlow<sub>sys</sub> as follows:
-
-<div>$$ \dot{V}_{sec,design} = \text{DesMainVolFlow}_{sys}\cdot\text{SecAirFlowScalingFactor} $$</div>
-
-If the cooler is part of the outdoor air path of a central air system, then the secondary air design flow rate is sized to be the maximum of either the design minimum outdoor air flow rate or one-half of the main design flow rate. 
-
-<div>$$ \dot{V}_{sec,design} = \max\left(\text{DesOutAirVolFlow},0.5\cdot\text{DesMainVolFlow}_{sys}\right)\cdot\text{SecAirFlowScalingFactor} $$</div>
- 
-##### Secondary Fan Design Power
-
-The Secondary Fan Design Power is outosized from secondary air design flow rate and user input for Secondary Fan Sizing Specific Power in units of W/(m3/s) as follows:
-
-<div>$$ P_{sec,fan,design} = \dot{V}_{sec,design}\cdot\text{FanPowerScalingFactor} $$</div>
-
-##### Recirculating Water Design Pump Power
-
-The Recirculating Water Design Pump Power is sized from secondary air design flow rate and user input for recirculating and spraying Water Pump Power Sizing Factor in units of W/(m3/s) or W-s/m3 and is given by:
-
-<div>$$P_{pump,design} = \dot{V}_{sec,design}\cdot\text{PumpPowerScalingFactor}$$</div>
-
-Where,
-
-<span>\(\dot{V}_{sys,design} \)</span> = primary air design volume flow rate in m3/s
-
-<span>\(\dot{V}_{sec,design} \)</span> = secondary air design volume flow rate in m3/s
-
-<span>\(\text{SecAirFlowScalingFactor} \)</span> = user specified Secondary air flow sizing factor in units of W/(m3/s) for secondary design air flow rate calculation.
-
-<span>\(\text{FanPowerScalingFactor} \)</span> = user specified secondary air fan sizing specific power in units of W/(m3/s) for design fan power calculation.
-
-<span>\(\text{PumpPowerScalingFactor} \)</span> = user specified recirculating and spraying water pump power sizing factor in units of W/(m3/s) for design pump power calculation.
-
-### Direct Evaporative Cooler Special Research Model
-
-This section summarizes the model implemented in the component EvaporativeCooler:Direct:ResearchSpecial.  This model can use a simple constant effectiveness or a variable effectiveness model that, under part load conditions, can modulate so that the air leaving the cooler just meets a drybulb temperature setpoint.  The algorithm used to determine the changes to the system air proceeds in four steps:
-
-1) Calculate the current operation effectiveness using effectiveness modifying curve
-
-2) Calculate full load performance using a part load fraction (PLF)=1 and Equation .
-
-3) Calculate PLF using Equations , , and .
-
-4) Recalculate cooler performance using the PLF.
-
-<div>$$\begin{array}{rl}
-  \epsilon_{op} &= \epsilon_{design}\cdot f_{mod}\left(flowRatio\right) \\
-  T_{db,out,sys} &= T_{db,in,sys} - \epsilon_{op}\cdot\left(T_{db,in,sys}-T_{wb,in,sys}\right) \\
-  T_{db,out} &= T_{db,in}-\epsilon\left(T_{db,in}-T_{wb,in}\right)
-\end{array}$$</div>
-
-where,
-
-* <span>\({T_{db,out,sys}}\)</span> is the drybub temperature of the air leaving the cooler [ºC],
-
-* <span>\({T_{db,in,sys}}\)</span> is the drybulb temperature of the air entering the cooler [ºC],
-
-* <span>\({T_{wb,in,sys}}\)</span> is the wetbulb temperature of the air entering the cooler [ºC], and
-
-* <span>\(\epsilon_{design} \)</span> is the cooler design effectiveness.
-
-* <span>\(\epsilon_{op} \)</span> is the cooler current operation effectiveness.
-
-* <span>\(f_{mod} \)</span> is the effectiveness modifier curve as a function of system air flow fraction
-
-The wetbulb temperature of air leaving a direct cooler is the same as the wetbulb temperature entering the cooler.  The leaving humidity ratio of the air is calculated using psychrometric functions with leaving drybulb and wetbulb temperatures and outdoor air pressure as inputs.  The leaving enthalpy of air is calculated using psychrometric functions with leaving drybulb temperature, leaving humidity ratio, and outdoor air pressure as inputs.
-
-The direct cooler sometimes has the ability to overcool the air and therefore some form of modulation is useful for analysis.  The special research model includes a Part Load Fraction, PLF, used to model the implications of controlling the amount of cooling.  It is assumed that through some sort of on/off cycling or wetness control that the cooling electric power can be varied to exactly meet the desired temperature when PLF is less than unity.  The auxiliary water pump power is then varied using pump power modifier curve or linearly using a Part Load Fraction when the pump power modifier curve is not specified.
-
-<div>$${\rm{FullOutput}} = {T_{db,out}} - {T_{db,in}}$$</div>
-
-<div>$${\rm{RequiredOutput}} = {T_{db,desired}} - {T_{db,in}}$$</div>
-
-<div>$$PLF = \frac{{{\rm{RequiredOutput}}}}{{{\rm{FullOutput}}}}$$</div>
-
-When PLF is less than 1.0 it is assumed that the cooler will deliver the desired temperature air (as long as it is less than the inlet; it doesn’t need heating).  Water pump power is also derated using the user specified pump modifier curve or using PLF when the pump modifier curve is not specified.
-
-#### Water Consumption
-
-Water consumption is an important consideration when evaluating evaporative coolers.  Water consumption of the evaporative cooler is modeled using Equation .
-
-<div>$${\dot V_{water}} = {\dot V_{evap}} + {\dot V_{drift}} + {\dot V_{blowdown}}$$</div>
-
-The three components of water consumption are evaporation, drift, and blowdown.  Evaporation is the water evaporated as the normal part of the evaporative cooler thermodynamic process and is calculated using:
-
-<div>$${\dot V_{evap}} = \frac{{\dot m\left( {{w_{out}} - {w_{in}}} \right)}}{{{\rho_{water}}}}$$</div>
-
-where,
-
-<span>\({\dot V_{evap}}\)</span> is the volume flow rate of useful water evaporation [m<sup>3</sup>/s]
-
-<span>\({w_{out}}\)</span> is the humidity ratio of the air leaving the cooler [kg/kg]
-
-<span>\({w_{in}}\)</span> is the humidity ratio of air entering the cooler [kg/kg]
-
-<span>\(\dot m\)</span> is the mass flow rate of air moving through the cooler [kg/s]
-
-<span>\({\rho_{water}}\)</span> is the density of water [kg/m3]
-
-Drift is water that leaves the cooler (and supply air duct) as droplets and does not contribute to the evaporative cooling process in a useful manner.  It is calculated using a user input factor that describes drift as a fraction of <span>\({\dot V_{evap}}\)</span>.
-
-<div>$${\dot V_{drift}} = {\dot V_{evap}} * {f_{drift}}$$</div>
-
-Blowdown is water drained from the sump to counter the build up of solids in the water that would otherwise occur because of evaporation.  It is calculated using a user input factor for the blowdown concentration ratio ,<span>\({R_{concentration}}\)</span>, which is the ratio of solids in the blowdown water compared to the solids in the fresh makeup water and is limited to values of 2 or higher.  The make up water needed for blowdown is calculated using:
-
-<div>$${\dot V_{blowdown}} = \frac{{{{\dot V}_{evap}}}}{{\left( {{R_{concentration}} - 1.0} \right)}} - {\dot V_{drift}}$$</div>
-
-Air System Fans <a name="Fans"></a>
----------------
-
-### Overview
-
-Three input objects (Fan:ConstantVolume, Fan:VariableVolume, and Fan:OnOff) provide models for fans -- the prime movers in most of the air loop and zonal air conditioning systems in EnergyPlus. For these input objects, EnergyPlus uses a simple polynomial-based curve-fit model to describe the relation between the volumetric flow rate and the fan electric power, with no explicit modeling of fan pressure rise. Consequently, duct-static-pressure reset strategies cannot be modeled using this approach. For CAV and VAV central air-handling systems, a fourth input object (Fan:ComponentModel) provides a simple physics-based model for flow-dependent fan pressure rise and detailed models for fan, belt, motor, and variable-frequency-drive efficiencies and energy use. This latter input object provides the capability to analyze the effects of duct-static-pressure reset strategies, as well as changes in fan system element performance. All of these fan models calculate the fan energy usage, which is often a large fraction of HVAC energy use and a significant portion of the building energy consumption. They also calculate the temperature rise in the air stream caused by the static pressure increase as the air goes through the fan. If the motor and belt are in the air stream, waste heat from the motor and belt also acts to raise the air stream temperature.
-
-### Model
-
-Each of the four fan models is a forward type: the model inputs describe the fan characteristics and the conditions of the air at the fan inlet; the outputs are the fan electrical power consumption and the conditions of the air at the fan outlet. The model algorithms and data are contained in the *Fans* module in EnergyPlus.
-
-#### Inputs and Data
-
-For the Fan:ConstantVolume, Fan:VariableVolume, and Fan:OnOff models, the user describes the fan by entering values for the design pressure rise across the fan, the design volumetric flow rate, the fan total efficiency, and the fan motor efficiency. The user also needs to specify the fraction of the fan waste heat that will enter the air stream (usually 0 or 1). For the Fan:VariableVolume model, the user must also enter the coefficients of a 4<sup>th</sup> order polynomial that relates the fan mass flow rate to the fan power consumption.The independent variable is the volumetric flow fraction; the dependent variable is the fan power part load ratio. For multi-speed fans, the user must enter a fan power ratio as a function of speed ratio performance curve name. Multi-speed fans can only be simulated in a parent object which allows multiple fan speeds (e.g., AirLoopHVAC:Unitary:Furnace:HeatCool, ZoneHVAC:PackagedTerminalAirConditioner, etc.). An optional efficiency curve may also be used when simulating multi-speed fans to adjust the fan total efficiency as the fan speed changes.
-
-For the Fan:ComponentModel object, the user describes the fan in more detail, and also describes the duct system characteristics as seen by the fan. In particular, the user specifies a pressure rise curve with four coefficients that relates the fan total pressure rise to the volumetric flow through the fan, the duct-static-pressure set-point, and the static pressure of the spaces surrounding the ducts. If duct-static-pressure reset is used, the user enters a linear curve with two coefficients that relates the pressure set-point to the volumetric flow through the fan. For the fan itself, the user specifies the fan geometry (wheel diameter and outlet area), maximum efficiency, the Euler number corresponding to the maximum efficiency, the maximum dimensionless flow, the names of four curves with several coefficients that describe the variation of fan efficiency and dimensionless flow with the Euler number in the normal and stall operation regions of the fan, and a sizing factor (applied to the maximum flow through the fan). For the belt, the user specifies the maximum efficiency (or a curve with five coefficients that defines the maximum efficiency as a function of maximum fan shaft input power), three curves with three coefficients each that relate the belt part-load efficiency to belt fractional output torque, the motor/fan pulley diameter ratio, the belt output torque capacity, and a sizing factor (applied to the maximum output torque of the belt). For the motor, the user specifies the maximum efficiency (or a curve with three coefficients that define the maximum efficiency as a function of maximum belt input power), a curve with three coefficients that relate the motor part-load efficiency to motor fractional output power, and a sizing factor (applied to the maximum output power of the motor). For the variable-frequency-drive (VFD), the user specifies a curve with three coefficients that relate the VFD part-load efficiency to motor fractional input power or to motor fractional speed, and a sizing factor (applied to the maximum output power of the VFD).
-
-#### Control
-
-The models must decide whether the fan is on or off. The primary on/off trigger is the fan schedule. This is an on/off schedule associated with each fan: a value of 1 indicates the fan is on; a value of 0 indicates the fan is off. The fan schedule can be overruled by flags set by system availability managers. If the flag *TurnFansOn* is true, a zero fan schedule value will be overridden and the fan will be turned on. If the flag *TurnFansOff* is true the fan will be forced off. The inlet air mass flow rate must be greater than zero for the fan to be on.
-
-Generally the fan is a passive component: it accepts the mass flow on its inlet node, uses it in its calculations of energy consumption and temperature rise, and passes it to the outlet node. However the fan maximum and minimum airflow rates act as absolute limits on the airflow rate.
-
-For multi-speed fans, the parent object determines the fan speed ratio (i.e., the selected speed of the fan motor) and uses this value in conjunction with the fan power ratio performance curve to calculate the full load fan power. This full load fan power is then used to determine the part-load performance of the fan and motor assembly.
-
-#### Simulation
-
-Simple (Single Speed) Fan Model
-
-The following equations define the model for this fan:
-
-<div>$${\dot Q_{tot}} = \dot m\cdot \Delta P/({e_{tot}}\cdot {\rho_{air}})$$</div>
-
-<div>$${\dot Q_{shaft}} = {e_{motor}}\cdot {\dot Q_{tot}}$$</div>
-
-<div>$${\dot Q_{toair}} = {\dot Q_{shaft}} + ({\dot Q_{tot}} - {\dot Q_{shaft}})\cdot {f_{motortoair}}$$</div>
-
-<div>$${h_{out}} = {h_{in}} + {\dot Q_{toair}}/\dot m$$</div>
-
-<div>$${w_{out}} = {w_{in}}$$</div>
-
-<div>$${T_{out}} = PsyTdbFnHW({h_{out}},{w_{out}})$$</div>
-
-On/Off Fan Model
-
-The on/off fan model is similar to the simple fan model with the exception that the on/off fan may cycle on and off during a simulation time step. The cycling rate of the fan is known as the run time fraction. The calculation of run time fraction accounts for the part-load losses of other equipment used in the HVAC system. A part-load factor (a.k.a. part-load ratio) is first calculated for the fan as the ratio of the actual operating mass flow rate to the maximum fan mass flow rate. The run time fraction is then calculated as the part-load factor divided by the part-load fraction. The part-load fraction is determined by other HVAC equipment in the simulation (Ref. DX coil) for use by this specific fan model.
-
-<div>$${f_{flow}} = {\raise0.7ex\hbox{${\mathop m\limits^ \bullet  }$} \!\mathord{\left/ {\vphantom {{\mathop m\limits^ \bullet  } {{{\mathop m\limits^ \bullet  }_{\max }}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop m\limits^ \bullet  }_{\max }}}$}}$$</div>
-
-<div>$$RTF = {\raise0.7ex\hbox{${{f_{flow}}}$} \!\mathord{\left/ {\vphantom {{{f_{flow}}} {PLF}}}\right.}\!\lower0.7ex\hbox{${PLF}$}}$$</div>
-
-The total fan power is then calculated as the maximum fan power multipled by the run time fraction.
-
-<div>$${\mathop Q\limits^\cdot_{tot}} = RTF\left[ {\mathop m\limits^\cdot  \cdot \Delta P/\left( {{e_{tot}}\cdot {\rho_{air}}} \right)} \right]$$</div>
-
-The remaining calculations are the same as those described in the simple single-speed fan mode.
-
-Multi-Speed Fan Model
-
-The model used to simulate a multi-speed fan relies on the general fan laws to correct for speed changes in the fan’s motor and the corresponding change in fan power and fan total efficiency. Two performance curves are used to define the change in power and efficiency as shown below. The power ratio curve must be used to simulate a multi-speed fan. The power ratio curve modifies the fan power based on a change in fan speed according to the cubic fan law. Exponents other than 3 are allowed. The efficiency ratio curve is used to correct for changes in nominal efficiency at alternate fan speeds. If either or both of these curves are not provided, the ratio is assumed to be 1.
-
-The power ratio term is evaluated using an exponent performance curve. The form of the exponent curve equation is shown below.
-
-<div>$$ExponentCurveOutput = C1 + C2*{x^{C3}}$$</div>
-
-The exponent performance curve is used to evaluate the power ratio as a function of speed ratio (x in the equation above). For typical fan performance, coefficient C1 = 0 and coefficient C2 = 1. The exponent (C3) is typically equal to 3 (cubed fan law) but other values are allowed.
-
-<div>$$PowerRatio = f{\left( {{N_{ratio}}} \right)^n} = ExponentCurveOutput$$</div>
-
-The efficiency ratio curve is a quadratic or cubic curve used to evaluate the efficiency ratio as a function of speed ratio (x in the following equation). The cubic equation form is shown below.
-
-<div>$$EfficiencyCurveOutput = C1 + C2{\left( x \right)^2} + C3{\left( x \right)^3}$$</div>
-
-The curve coefficients are determine by correlating the normalized fan total efficiency (i.e., the actual fan total efficiency divided by the nominal fan total efficiency at a speed ratio of 1) to the speed ratio (i.e., the ratio of actual air flow rate through the fan to the maximum fan air flow rate).
-
-<div>$$EfficiencyRatio = f\left( {{N_{ratio}}} \right) = EfficiencyCurveOutput$$</div>
-
-To account for the change in fan speed and to ensure that the run time fraction is accurately calculated, an adjustment to the previous calculation for run time fraction is made. This adjusts the calculated run time fraction to account for times when the fan speed has been reduced and the new speed is now considered the fan’s maximum speed. The speed adjusted run time fraction is then used in the fan power calculation.
-
-<div>$$RTF = {\raise0.7ex\hbox{${RTF}$} \!\mathord{\left/ {\vphantom {{RTF} {{N_{ratio}}}}}\right.}\!\lower0.7ex\hbox{${{N_{ratio}}}$}}$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{tot}} = RTF\left[ {\frac{{\mathop m\limits^ \bullet  \Delta P}}{{{e_{tot}}{\rho_{air}}}}} \right]\left( {\frac{{PowerRatio}}{{EfficiencyRatio}}} \right)$$</div>
-
-Each of the performance curves described above may be used to model the performance of a multi-speed fan motor, however, the power ratio curve must be used to envoke the multi-speed simulation. These curves are used when the fan is used in an HVAC system having multiple flow rates (i.e., different flow rates in cooling and heating mode). If an HVAC system operates at the same speed in either cooling or heating mode, these curves are not required. When these curves are not used, the associated ratio term in the equation above is assumed to be 1. The remaining calculations are identical to the simple single-speed fan model described above.
-
-Variable Speed Fan Model
-
-The model for the variable speed fan is similar to the simple single-speed fan model except for a part load factor that multiplies the fan power consumption.
-
-<div>$${f_{flow}} = \dot m/{\dot m_{design}}$$</div>
-
-<div>$${f_{pl}} = {c_1} + {c_2} \cdot {f_{flow}} + {c_3} \cdot f_{flow}^2 + {c_4} \cdot f_{flow}^3 + {c_5} \cdot f_{flow}^4$$</div>
-
-<div>$${\dot Q_{tot}} = {f_{pl}}\cdot {\dot m_{design}}\cdot \Delta P/\left( {{e_{tot}}\cdot {\rho_{air}}} \right)$$</div>
-
-The rest of the calculation is the same as for the simple fan.
-
-#### Nomenclature for Simple Models
-
-<span>\({\dot Q_{tot}}\)</span> is the fan power in watts;
-
-<span>\(\dot m\)</span>is the air mass flow in kg/s;
-
-<span>\({\dot m_{design}}\)</span>is the design (maximum) air flow in kg/s;
-
-<span>\(\Delta P\)</span>is the fan design pressure increase in Pascals;
-
-<span>\({e_{tot}}\)</span> is the fan total efficiency;
-
-<span>\({\rho_{air}}\)</span>is the air density at standard conditions in kg/m<sup>3</sup>;
-
-<span>\({e_{motor}}\)</span> is the motor efficiency;
-
-<span>\({\dot Q_{shaft}}\)</span>is the fan shaft power in watts;
-
-<span>\({\dot Q_{toair}}\)</span>is the power entering the air in watts;
-
-<span>\({N_{ratio}}\)</span>is the ratio of actual fan flow rate (or speed) to maximum fan flow rate (or speed)
-
-<span>\({h_{in}},{h_{out}}\)</span> are the inlet and outlet air stream specific enthalpies in J/kg;
-
-<span>\({w_{in}},{w_{out}}\)</span> are the inlet and outlet air stream humidity ratios;
-
-<span>\({T_{out}}\)</span> is the outlet air temperature in degrees C;
-
-<span>\(PsyTdbFnHW\)</span>is the EnergyPlus psychrometric routine relating enthalpy and humidity ratio to temperature;
-
-<span>\({f_{flow}}\)</span>is the flow fraction or part-load ratio;
-
-<span>\({f_{pl}}\)</span> is the part load factor.
-
-Component Fan Model
-
-The Fan:ComponentModel object is based upon combining: modified forms of fan, belt, motor, and variable-frequency-drive (VFD) element models (Stein and Hydeman 2004); a simplified fan pressure rise model with distribution system leakage, duct static pressure, and conditioned space pressure control effects included (Sherman and Wray 2010); and a diagnostic-based simplified duct static-pressure reset (SPR) scheme for air-handling systems (Federspiel 2004, 2005).
-
-Fan *electric* power depends on fan *air* power (product of the airflow through and pressure rise across the fan), mechanical efficiencies (fan and belt), and electrical efficiencies (motor and drive). For systems with variable flows, none of these parameters is constant and all are interrelated. For example, Figure 208 shows that fan efficiency strongly depends on fan flow *as well as* pressure rise, although this is not obvious from the manufacturer’s power and speed performance map (top left). Fan efficiency maps can be derived from the manufacturer’s performance map using a commercially-available software-based data extraction tool such as DigitizeIt and by applying the following equation to the extracted data:
-
-<span>\({\eta_{fan}} = \frac{{\Delta {P_{fan}} \cdot {Q_{fan}}}}{{{H_{fan}}}}\)</span>                                                                                     ()
-
-where **Δ***P<sub>fan</sub>*is the fan pressure rise (Pa); *Q<sub>fan</sub>* is the fan flow at standard conditions (m<sup>3</sup>/s); and *H<sub>fan</sub>* is the fan shaft power (W). Fan speed values also can be derived from the manufacturer’s performance map using a similar software-based data extraction tool.
-
-Fan pressure rise must be sufficient to overcome the air-handling system pressure drop, which depends on duct static pressure, on duct and equipment leakage, and on pressure drops across duct and duct-like elements (e.g., dampers, fittings), coils, and filters that are connected to the fan. Duct and duct-like pressure drops increase approximately as the square of the flow through them. However, pressure drops across coils and filters behave differently: they are proportional to the flow raised to a power n, which can approach one for high-efficiency filters and wet coils (Liu et al. 2003, Trane 1999).
-
-The relation between system pressure drop and flow defines what is commonly called a “system curve�. When system characteristics change, such as when the duct static pressure set point is varied, a family of system curves results. The intersections of these curves with fan curves (e.g., power as a function of pressure rise and flow) on a pressure versus flow plot define one or more loci of unique fan operating points. Each of these points has an associated fan efficiency, power, and speed.
-
-![Fancomp1](media/image4888.png)
-
-Figure 208. Example Fan Performance Maps - Manufacturer’s Data from Loren Cook Company, plus Derived Static Efficiency (Three-Dimensional and Contours)
- (Dashed Parabolic Curve is “Do Not Select Line�)
-
-*Fan Pressure Rise Model*: To calculate fan pressure rise based on flow through the fan, Sherman and Wray (2010) have developed a simple physics-based data-driven four parameter duct system model for the purpose of simulating its system curve. The embodiment of the model for a fixed outdoor air fraction that can be applied to constant- or variable-volume central air-handling systems is:
-
-<span>\(\Delta {P_{fan,tot}} = {A_{fpr}}Q_{fan}^2 + {B_{fpr}}Q_{fan}^{} + {C_{fpr}}Q_{fan}^{}\sqrt {{P_{sm}} - {P_o}}  + {D_{fpr}}\left( {{P_{sm}} - {P_o}} \right)\)</span>                            ()
-
-where **Δ***P<sub>fan,tot</sub>* is the fan total pressure rise (Pa); *Q<sub>fan</sub>* is the fan flow at standard conditions (m<sup>3</sup>/s); *P<sub>sm</sub>* is the duct static pressure set point (Pa); *P<sub>o</sub>* is the static pressure of the spaces surrounding the ducts (Pa); and *A<sub>fpr</sub>*, *B<sub>fpr</sub>*, *C<sub>fpr</sub>*, and *D<sub>fpr</sub>* are constant coefficients that represent different aspects of the fan pressure rise model as described below.
-
-Fan static pressure rise is determined from the total pressure rise by subtracting the outlet velocity pressure:
-
-<span>\(\Delta {P_{fan}} = \Delta {P_{fan,tot}} - \frac{\rho }{2}{\left( {\frac{{{Q_{fan}}}}{{{A_{fan,out}}}}} \right)^2}\)</span>                                                                         ()
-
-where *A<sub>fan,out</sub>* is the fan outlet area (m<sup>2</sup>) and *�* is the air density at the fan inlet (kg/m<sup>3</sup>).
-
-The first term in Equation looks like the common system curve in which the fan pressure rise is proportional to the square of the fan flow, but here it also depends implicitly on supply and return pressure losses, and in part on the fraction of the fan flow that is outdoor air (essentially “leaks� into and out of the return side of the system). Very often it is the only term considered, but that would only be correct with fixed-position dampers, no distribution system leakage, no linear resistance components, and no duct static pressure control.
-
-The second term accounts for significant flow resistances in the system where the pressure difference is linearly proportional to the flow. Some filters and coils in the return may need this term to be adequately described. This term could be ignored if there are no linear components or if their pressure drops are very small compared to the other terms.
-
-The third term, which depends on the fan flow and square root of the supply duct pressure *P<sub>sm</sub>*, accounts in part for air leakage from the supply system when damper positions are fixed or are changed independently of static pressure or fan flow. In this case, reducing or eliminating supply leakage results in a different system curve. This, however, might be only a minor “correction� to the simple system curves generally used. The third term is zero when VAV box dampers are modulated to control flow. Consequently, with variable-position supply dampers, reducing or eliminating supply leakage does not change the system curve.
-
-The last term also accounts in part for leakage from the supply system when damper positions are fixed or are changed independently of static pressure or fan flow. This term indicates that the same fan pressure rise can be achieved by raising the duct pressure and closing dampers. The only change in the system in such a case is that the leakage flow may increase. The coefficient for this term is equal to one when the VAV box dampers are modulated to control flow. In both cases, this term may be the most important “correction� to the simple system curves generally used, especially at low flows.
-
-In principle, especially for research applications of Energy Plus, the four individual fan pressure rise coefficients can be determined using duct design calculation tools for the entire system (e.g., Right-CommDuct, UNI-DUCT, Ductsize, Varitrane Duct Designer, T-Duct). In practice, however, especially for existing buildings, the necessary details may not be known sufficiently. In that case, one can make active measurements at different combinations of fan flows, outside air fractions, damper positions (if they are variable), and duct static pressures and then use non-linear system identification techniques to fit the data and determine the coefficients. If passive measurements can be made over a sufficiently long time so that a wide range of outside air settings, damper positions, and fan flows is obtained, one could instead regress the data to find all of the parameters in the equation. Unfortunately, there are no standardized test procedures available to draw upon, even though some standards appear to be related (e.g., ASHRAE 1999, 2008). Consequently, field test protocols need to be developed to determine the parameters for the new duct system model. These protocols then need to be integrated into standardized data collection and analysis tools such as Pacific Gas and Electric’s “Universal Translator� tool. The California Energy Commission is funding such a project; data, procedures, and tools from this project will support the EnergyPlus implementation of the fan and duct system models described here.
-
-*SPR Model*: The model for duct-static-pressure reset (SPR) is based on a simple diagnostic procedure and a linear correlation between duct static pressure and supply fan airflow (Federspiel 2004, 2005). The diagnostic method involves measuring the static pressure at the duct static pressure sensor and the velocity pressure at the fan inlet (represents the fan flow) at multiple points over the fan’s operating range, while the VAV box dampers attempt to control flow in response to a constant thermostat setpoint. The goal of the test is to define the lowest duct static pressure where all VAV boxes are still in control (dampers modulating). In the model, the correlation between *P<sub>sm</sub>* and *Q<sub>fan</sub>* is as follows for *Q<sub>fan,min</sub>* ≤ *Q<sub>fan</sub>* ≤ *Q<sub>fan,max</sub>*:
-
-<span>\({P_{sm}} = {P_{sm,\min }} + \left( {{P_{sm,\max }} - {P_{sm,\min }}} \right)*\frac{{\left( {{Q_{fan}} - {Q_{fan,\min }}} \right)}}{{\left( {{Q_{fan,\max }} - {Q_{fan,\min }}} \right)}} = {C_1} + {C_2}*{Q_{fan}}\)</span>                         ()
-
-Where
-
- <span>\({C_1} = {P_{sm,\min }} - {C_2}*{Q_{fan,\min }}\)</span> and <span>\({C_2} = \frac{{\left( {{P_{sm,\max }} - {P_{sm,\min }}} \right)}}{{\left( {{Q_{fan,\max }} - {Q_{fan,\min }}} \right)}}\)</span>                                ()
-
-For *Q<sub>fan</sub>* &lt; *Q<sub>fan,min</sub>*, *P<sub>sm</sub>* = *P<sub>sm,min</sub>*;for*Q<sub>fan</sub>* &gt; *Q<sub>fan,max</sub>*, *P<sub>sm</sub>* = *P<sub>sm,max</sub>*
-
-*Fan Efficiency and Shaft Input Power Model*: A dimensionless parameter in the form of an Euler number can be used to simplify the description of fan static efficiency variations:
-
-<span>\(Eu = \frac{{\left( {\Delta {P_{fan}} * D_{fan}^4} \right)}}{{\left( {\rho  * Q_{fan}^2} \right)}}\)</span>                                                                                      ()
-
-where **Δ***P<sub>fan</sub>* is the fan static pressure rise (Pa), *D<sub>fan</sub>* is the fan wheel outer diameter (m), *�* is the air density at the fan inlet (kg/m<sup>3</sup>), and *Q<sub>fan</sub>* is the fan flow at standard conditions (m<sup>3</sup>/s). *Eu* is nominally the ratio of pressure forces across the fan to inertial forces at the fan wheel exit.
-
-By plotting the normalized fan static efficiency (*static efficiency / maximum static efficiency*) versus the logarithm base 10 of the normalized Euler number (*Eu* */* *Eu* *at maximum static efficiency*), the dimensionless performance of various fan sizes is very similar (as one might expect from the “fan laws�), but so also is the dimensionless performance of different *types* of fans (e.g., single-inlet plenum fans, double-inlet housed centrifugal fans, mixed flow fans, vane axial fans, fans with backward or forward curved blades). An example of this correlation for the “normal operation� (non-stall) and stall regions of eight fans is shown in Figure 209.
-
-![Fancomp2](media/image4895.png)
-
-Figure 209. Normalized Efficiency Curves for Eight Fans in Dimensionless Space
- *(BC=backward curved, FC=forward curved; SI=single inlet, DI=double inlet)*
-
-This model uses a continuous function to represent the normalized fan efficiency (*η<sub>fan</sub>*) variation. The normalized exponential-conditioned skew-normal functional relationship is:
-
-<span>\(\frac{{{\eta_{fan}}({x_{fan}})}}{{{\eta_{fan,\max }}}} = \frac{{{e^{( - 0.5*Z_1^2)}}[1 + \frac{{{Z_2}}}{{\left| {{Z_2}} \right|}} \bullet erf\left( {\frac{{\left| {{Z_2}} \right|}}{{\sqrt 2 }}} \right)}}{{{e^{( - 0.5*Z_3^2)}}[1 + \frac{{{Z_3}}}{{\left| {{Z_3}} \right|}} \bullet erf\left( {\frac{{\left| {{Z_3}} \right|}}{{\sqrt 2 }}} \right)}}\)</span>                                                   ()
-
-where
-
-x<sub>fan</sub> = log<sub>10</sub>(Eu / Eu<sub>max</sub>)
-
-Z<sub>1</sub> = (x<sub>fan</sub> - a<sub>fan</sub>) / b<sub>fan</sub>;  Z<sub>2</sub> = ((e<sup>(c</sup>fan<sup>\*x</sup>fan<sup>)</sup>\*d<sub>fan</sub>\*x<sub>fan</sub>) - a<sub>fan</sub>) / b<sub>fan</sub>;  Z<sub>3</sub> = -a<sub>fan</sub> / b<sub>fan</sub>
-
-For conceptual design when only rough estimates are needed, a generic curve (also shown in Figure 209) can be used and then one only needs to know the maximum efficiency (*η<sub>fan,max</sub>*) and *Eu* at that maximum (*Eu<sub>max</sub>*) to entirely model the fan efficiency and hence fan power. The dimensionless coefficients for the generic normalized fan efficiency curve are as follows:
-
-*a<sub>fan</sub>*= -2.732094, *b<sub>fan</sub>* = 2.273014,*c<sub>fan</sub>* = 0.196344, *d<sub>fan</sub>* = 5.267518
-
-In this case, the coefficient of determination R<sup>2</sup> is 0.994. Also, the average and RMS differences between the efficiency values based on extracted data and the fitted generic curve are, respectively, about 0.5% and 1.4%; maximum differences are about ±9%.
-
-If more accuracy is needed for a specific fan, a similarly shaped curve can be developed for that fan (using extracted data, Equation , and least-squares regression techniques), segmented into normal operation and stall regions with specific coefficients fitted for each region. Figure 210 shows an example, using the data from Figure 208.
-
-![](media/image4897.svg.png)
-
-Figure 210. Example Normalized Efficiency Data for One Fan
-
-For this specific fan, the coefficients are:
-
-Table 65. Normalized Fan Efficiency Coefficients for Specific Backward-Curved Plenum Fan
-
-<table class="table table-striped">
-<tr>
-<td>Operating Region</td>
-<td>a<sub>fan</sub></td>
-<td>b<sub>fan</sub></td>
-<td>c<sub>fan</sub></td>
-<td>d<sub>fan</sub></td>
-</tr>
-<tr>
-<td>Normal (Non-Stall)</td>
-<td>0.072613</td>
-<td>0.833213</td>
-<td>0</td>
-<td>0.013911</td>
-</tr>
-<tr>
-<td>Stall</td>
-<td>-2.354091</td>
-<td>2.117493</td>
-<td>0</td>
-<td>2.753264</td>
-</tr>
-
-</table>
-
-
-
-In this case, the average and RMS differences between the efficiency values based on extracted data and fitted specific curve (R<sup>2</sup> is 0.999) are, respectively, about -0.1% and 0.3%; maximum differences are about ±0.7%. Field tests are especially needed to determine the coefficients for installed fans because fans are susceptible to “system effects� (e.g., inlet obstructions) that are not included in the manufacturer test data (AMCA 1990a).
-
-To determine fan efficiency and fan shaft power at a particular time step, first calculate the fan pressure rise (**Δ***P<sub>fan</sub>*) using the time step fan flow (*Q<sub>fan</sub>*) and Equation (and also using Equations and if there is SPR). Next, calculate *Eu* using Equation and then *x<sub>fan</sub>* (log<sub>10</sub> normalized *Eu*), which is based on *Eu* and the specified *Eu<sub>max</sub>* (*Eu* at maximum efficiency) for the fan. The corresponding normalized efficiency (*η<sub>fan</sub>*(*x<sub>fan</sub>*) */ η<sub>fan,max</sub>*) is obtained using Equation . The fan efficiency (*η<sub>fan</sub>*(*x<sub>fan</sub>*)) therefore is:
-
-<span>\({\eta_{fan}}\left( {{x_{fan}}} \right) = {\eta_{fan,\max }}\left[ {\frac{{{\eta_{fan}}\left( {{x_{fan}}} \right)}}{{{\eta_{fan,\max }}}}} \right]\)</span>                                                                  ()
-
-The fan shaft input power (mechanical, W) is:
-
-<span>\({H_{fan}} = \frac{{\Delta {P_{fan}} \cdot {Q_{fan}}}}{{{\eta_{fan}}\left( {{x_{fan}}} \right)}}\)</span>                                                                                      ()
-
-*Fan Shaft Speed and Torque Modeling*: For rotating elements, power (*H*) is the product of torque (*τ*) and rotational speed (ω), or conversely, torque is power divided by rotational speed (*τ =H / ω*).
-
-The Stein and Hydeman variable-frequency-drive (VFD) component model correlates VFD efficiency as a linear function of VFD fractional output power (i.e., motor input power). Available data for about 50 drives from Saftronics were apparently used to develop their model, but those data represent VFD efficiency as a function of motor fractional speed
- (*ω<sub>motor</sub> / ω<sub>motor,max</sub>*, or nominally, drive output frequency divided by maximum output frequency, if motor slip is ignored).
-
-To make use of the available data, the Stein and Hydeman linear correlation must intrinsically make an assumption that motor speed and torque have some fixed relationship. Although not documented, their assumption might be the common belief that fractional torque (Ï„/ Ï„<sub>max</sub>) for a motor is simply the square of its fractional speed. For fans serving duct systems with components such as filters and coils, with relatively low pressure drops elsewhere in the system, and for systems that have a non-zero controlled duct static pressure, this assumption may be inappropriate. Consequently, to make use of the available data and to avoid such assumptions, one needs to know the fraction of full speed at which fan components operate.
-
-For the fan, dimensionless flow (*φ*) can be defined as (ASHRAE 1993):
-
-<span>\(\varphi  = \frac{{{Q_{fan}}}}{{{\omega_{fan}} \cdot D_{fan}^3}}\)</span>                                                                                           ()
-
-where *ω<sub>fan</sub>* is the fan speed (rad/s). This parameter can be calculated for each operating point on the fan manufacturer’s performance map that represents fan speed as a function of flow and fan pressure rise. To simplify the data representation to a single curve (as we have done for fan efficiency), one can plot normalized dimensionless flow (dimensionless flow divided by maximum dimensionless flow, (*φ*(*x<sub>fan</sub>*) */* *φ<sub>max</sub>*) as a function of the log base 10 of the normalized Euler (*Eu*) parameter (*x<sub>fan</sub>*). Figure 211 shows an example plot derived from the manufacturer’s data in Figure 208.
-
-![](media/image4901.svg.png)
-
-Figure 211. Example Normalized Dimensionless Flow Data for One Fan
-
-Equation describes the sigmoidal functional form for normalized *φ*:
-
-<span>\(\frac{{\varphi \left( {{x_{fan}}} \right)}}{{{\varphi_{\max }}}} = ({A_{spd}} + {B_{spd}}/({(1 + {e^{\left[ {{{({C_{spd}} - {x_{spd}})} \mathord{\left/ {\vphantom {{({C_{spd}} - {x_{spd}})} {{D_{spd}}}}} \right. } {{D_{spd}}}}} \right]}})^{{E_{spd}}}})\)</span>                                             ()
-
-where *A<sub>spd</sub>*, *B<sub>spd</sub>*, *C<sub>spd</sub>*, *D<sub>spd</sub>*, and *E<sub>spd</sub>* are coefficients for the fan. Separate sets of coefficients for the normal operation and stall regions can be specified. For the curve shown in Figure 211, these coefficients are:
-
-Table 66. Dimensionless Flow Coefficients – Specific Backward-Curved Fan
-
-<table class="table table-striped">
-<tr>
-<td>Operating Region</td>
-<td>A<sub>spd</sub></td>
-<td>B<sub>spd</sub></td>
-<td>C<sub>spd</sub></td>
-<td>D<sub>spd</sub></td>
-<td>E<sub>spd</sub></td>
-</tr>
-<tr>
-<td>Normal (Non-Stall)</td>
-<td>0</td>
-<td>1.001423</td>
-<td>0.123935</td>
-<td>-0.476026</td>
-<td>1</td>
-</tr>
-<tr>
-<td>Stall</td>
-<td>0</td>
-<td>5.924993</td>
-<td>-1.916316</td>
-<td>-0.851779</td>
-<td>1</td>
-</tr>
-
-</table>
-
-
-
-For a generic centrifugal fan with backward-curved blades, the coefficients are:
-
-Table 67. Dimensionless Flow Coefficients – Generic Backward-Curved Fan
-
-<table class="table table-striped">
-<tr>
-<td>Operating Region</td>
-<td>A<sub>spd</sub></td>
-<td>B<sub>spd</sub></td>
-<td>C<sub>spd</sub></td>
-<td>D<sub>spd</sub></td>
-<td>E<sub>spd</sub></td>
-</tr>
-<tr>
-<td>Normal (Non-Stall)</td>
-<td>-0.551396</td>
-<td>1.551467</td>
-<td>-0.442200</td>
-<td>-0.414006</td>
-<td>0.234867</td>
-</tr>
-<tr>
-<td>Stall</td>
-<td>0.000608</td>
-<td>0.586366</td>
-<td>0.021775</td>
-<td>-0.063218</td>
-<td>0.072827</td>
-</tr>
-
-</table>
-
-For any operating point of flow (*Q<sub>fan</sub>*) and fan pressure rise (**Δ***P<sub>fan</sub>*), one can calculate the corresponding Euler number (*Eu*) for the given fan, and then determine the corresponding normalized dimensionless flow (*φ*(*x<sub>fan</sub>*) */* *φ<sub>max</sub>*) from the sigmoidal dimensionless flow function (Equation ). With *φ*(*x<sub>fan</sub>*) */* *φ<sub>max</sub>* determined and knowing *φ<sub>max</sub>* for the fan, the dimensionless flow is:
-
-<span>\(\varphi \left( {{x_{fan}}} \right) = {\varphi_{\max }}\left[ {\frac{{\varphi \left( {{x_{fan}}} \right)}}{{{\varphi_{\max }}}}} \right]\)</span>                                                                              ()
-
-With *φ*(*x<sub>fan</sub>*) determined, the fan rotational speed (rad/s) is:
-
-<span>\({\omega_{fan}} = \frac{{{Q_{fan}}}}{{\left( {\varphi ({x_{fan}}) * D_{fan}^3} \right)}}\)</span>                                                                                ()
-
-Fan shaft torque (N∙m), which the belt drive must supply to the fan shaft, is then:
-
-<span>\({\tau_{fan}} = \frac{{{H_{fan}}}}{{{\omega_{fan}}}}\)</span>                                                                                                ()
-
-The fraction of full-load driven torque for the belt (*τ<sub>fan</sub> / τ<sub>belt,max</sub>*), which is typically called “belt load�, is thus *τ<sub>fan</sub>* divided by the belt torque capacity (*τ<sub>belt,max</sub>*). For a particular belt type and cross-section, belt torque capacity can be determined from manufacturer’s information such as a shaft speed versus power chart.
-
-Ignoring belt slip, motor shaft speed (*ω<sub>motor</sub>*, rad/s) can then be determined using the fan speed (*ω<sub>fan</sub>*) and the motor/fan pulley diameter ratio (*D<sub>pulley,motor</sub> / D<sub>pulley,fan</sub>*), which is typically called the “drive� ratio:
-
-<span>\({\omega_{motor}} = \frac{{{\omega_{fan}}}}{{\left( {\frac{{{D_{pulley,motor}}}}{{{D_{pulley,fan}}}}} \right)}}\)</span>                                                                                 ()
-
-*Belt, Motor, and Variable-Frequency-Drive Efficiency and Input Power Models – Overview*: The models for belt drives, motors, and VFDs that Stein and Hydeman included in their air-handling system model represent maximum efficiency as a function of power input to the adjacent downstream component (e.g., the power input to a fan shaft by a belt drive), but they do not include part-load models. The part-load models are needed, because part-load efficiency for these components can fall off rapidly at low load (e.g., to zero at zero load) and many systems operate occasionally (and some much of the time) at low loads, in part because of current practices that result in substantial oversizing of components.
-
-*Belt Efficiency and Input Power Model:* Figure 212 shows three maximum efficiency (*η<sub>belt,max</sub>*) curves for belts (low, medium, and high) as a function of maximum fan shaft torque. This set of efficiency curves is based on belt drive loss data from AMCA Publication 203 (1990b), which reportedly is an aggregation of data from over 400 tests.
-
-To determine *η<sub>belt,max</sub>* if data for a specific belt are not available, first use the maximum fan shaft input power (*H<sub>fan,max</sub>*) for the load spectrum to calculate the natural logarithm of belt power capacity:
-
-*x<sub>belt,max</sub> =*ln(*H<sub>fan,max</sub>*) with *H<sub>fan,max</sub>* expressed in terms of hp                        ()
-
-Then, use Equations and , along with a choice of low, medium, or high efficiency coefficients from Table 68, to calculate *η<sub>belt,max</sub>*.
-
-![](media/image4907.svg.png)
-
-Figure 212. Belt Maximum Efficiency vs. Fan Shaft Power Input
-
-The quartic polynomial curves in Figure 212 and their coefficients are as follows:
-
-<span>\({\eta_{belt,\max ,\ln }} = {c_1} + {c_2} \cdot {x_{belt,\max }} + {c_3} \cdot x_{_{belt,\max }}^2 + {c_4} \cdot x_{_{belt,\max }}^3 + {c_5} \cdot x_{_{belt,\max }}^4\)</span>                    ()
-
-Table 68. Belt Maximum Efficiency Curve Coefficients
-
-<table class="table table-striped">
-<tr>
-<td>Efficiency Class (Loss)</td>
-<td>c<sub>1</sub></td>
-<td>c<sub>2</sub></td>
-<td>c<sub>3</sub></td>
-<td>c<sub>4</sub></td>
-<td>c<sub>5</sub></td>
-</tr>
-<tr>
-<td>High (Low Loss)</td>
-<td>-6.502E-2</td>
-<td>2.475E-2</td>
-<td>-6.841E-3</td>
-<td>9.383E-4</td>
-<td>-5.168E-5</td>
-</tr>
-<tr>
-<td>Medium (Medium Loss)</td>
-<td>-9.504E-2</td>
-<td>3.415E-2</td>
-<td>-8.897E-3</td>
-<td>1.159E-3</td>
-<td>-6.132E-5</td>
-</tr>
-<tr>
-<td>Low (High Loss)</td>
-<td>-1.422E-1</td>
-<td>5.112E-2</td>
-<td>-1.353E-2</td>
-<td>1.814E-3</td>
-<td>-9.909E-5</td>
-</tr>
-
-</table>
-
-
-
-The belt maximum efficiency is therefore:
-
-<span>\({\eta_{belt,\max }} = {e^{{\eta_{belt,\max ,\ln }}}}\)</span>                                                                                   ()
-
-The normalized *part-load* belt efficiency model is provided to modify the maximum efficiency of the belt. This model is based on part-load data for belts in ACEEE’s handbook on motor systems (Nadel et al. 2002). To determine the normalized belt efficiency at part-load (*η<sub>belt</sub>*(*x<sub>belt</sub>*)/* η<sub>belt,max</sub>*), use the fan shaft (belt output) fractional torque (*x<sub>belt</sub>* = *τ<sub>belt</sub>* / *τ<sub>belt,max;</sub> τ<sub>belt</sub> = τ<sub>fan</sub>*) as the belt fractional load in Equation or (select the equation for the region that contains *x<sub>belt</sub>*) and use coefficients from Table 69 that correspond to that region and the belt type: V-Belt or synchronous (toothed). Figure 213 shows a graphical representation of the curves defined by these equations and coefficients.
-
-![](media/image4910.svg.png)
-
-Figure 213. Belt Normalized Efficiency vs. Belt Fractional Load)
-
-The belt normalized (part-load) efficiency curves in Figure 213 for Regions 1 and 3 (single rectangular hyperbola type 2) and Region 2 (exponential decay), respectively, and their coefficients are as follows:
-
-Region 1 (0 &lt;= *x<sub>belt</sub>* &lt; *x<sub>belt,trans</sub>*) and Region 3 (*x<sub>belt</sub>* &gt; 1):
-
-<span>\(\frac{{{\eta_{belt}}({x_{belt}})}}{{{\eta_{belt,\max }}}} = \left[ {\frac{{{a_{belt}} \cdot {x_{belt}}}}{{{b_{belt}} + {x_{belt}}}}} \right] + {c_{belt}} \cdot {x_{belt}}\)</span>                                                             ()
-
-Region 2 (*x<sub>belt,trans</sub>* &lt;= *x<sub>belt</sub>* &lt;= 1):
-
-<span>\(\frac{{{\eta_{belt}}({x_{belt}})}}{{{\eta_{belt,\max }}}} = {a_{belt}} + {b_{belt}} \cdot {e^{\left( {{c_{belt}} \cdot {x_{belt}}} \right)}}\)</span>                                                               ()
-
-where x<sub>belt</sub> = <span>\(\tau \)</span><sub>belt</sub> / <span>\(\tau \)</span><sub>belt,max</sub>
-
-
-
-Belt efficiency therefore is:
-
-<span>\({\eta_{belt}}({x_{belt}}) = {\eta_{belt,\max }}\left[ {\frac{{{\eta_{belt}}({x_{belt}})}}{{{\eta_{belt,\max }}}}} \right]\)</span>                                                                   ()
-
-Belt input power (mechanical, W) at the motor shaft is:
-
-<span>\({H_{belt}} = \frac{{{H_{fan}}}}{{{\eta_{belt}}({x_{belt}})}}\)</span>                                                                                       ()
-
-Table 69. Belt Normalized Efficiency Curve Coefficients
-
-<table class="table table-striped">
-  <tr>
-    <th>Belt Type</th>
-    <th>x belt,trans</th>
-    <th>Region</th>
-    <th>a<sub>belt</sub></th>
-    <th>b<sub>belt</sub></th>
-    <th>c<sub>belt</sub></th>
-  </tr>
-  <tr>
-    <td rowspan="3">V-Belt</td>
-    <td rowspan="3">0.167</td>
-    <td>1</td>
-    <td>0.920797</td>
-    <td>0.026269</td>
-    <td>0.151594</td>
-  </tr>
-  <tr>
-    <td>2</td>
-    <td>1.011965</td>
-    <td>-0.339038</td>
-    <td>-3.43626</td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>1.037778</td>
-    <td>0.010307</td>
-    <td>-0.026815</td>
-  </tr>
-  <tr>
-    <td rowspan="3">Synchronous</td>
-    <td rowspan="3">0.137</td>
-    <td>1</td>
-    <td>0.982167</td>
-    <td>0.049135</td>
-    <td>0.158164</td>
-  </tr>
-  <tr>
-    <td>2</td>
-    <td>1.002134</td>
-    <td>-0.531885</td>
-    <td>-5.295707</td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>1</td>
-    <td>0</td>
-    <td>0</td>
-  </tr>
-</table>
-
-*Motor Efficiency and Input Power Model:* Figure 214 shows three maximum efficiency (*η<sub>motor,max</sub>*) curves for motors (low, medium, and high) as a function of rated motor output power (belt input power). This set of efficiency curves is based on maximum efficiency data in DOE’s MotorMaster+ database (2003) from about 800 tests. It is provided for use in the absence of manufacturer’s data.
-
-![](media/image4917.svg.png)
-
-Figure 214. Maximum Motor Efficiency vs. Belt Power Input (Motor Output)
-
-To determine *η<sub>motor,max</sub>* if data for a specific motor are not available (e.g., as listed in Table 71), first use the maximum belt input power (*H<sub>belt,max</sub>*) for the load spectrum (multiplied by whatever oversizing factor may be desired) to calculate the natural logarithm of belt power capacity:
-
-*x<sub>motor,max</sub> =*ln(*H<sub>belt,max</sub>*) with *H<sub>belt,max</sub>* expressed in terms of hp                     ()
-
-Then, use Equation , along with a choice of low, medium, or high efficiency coefficients from Table 70, to calculate *η<sub>motor,max</sub>*.
-
-The maximum motor efficiency curves in Figure 214 (single rectangular hyperbola type 1) and their coefficients are as follows:
-
-<span>\({\eta_{motor,\max }} = \left[ {\frac{{{a_{motor,\max }} \cdot {x_{motor,\max }}}}{{{b_{motor,\max }} + {x_{motor,\max }}}}} \right] + {c_{motor,\max }}\)</span>                                              ()
-
-Table 70. Motor Maximum Efficiency Curve Coefficients
-
-<table class="table table-striped">
-<tr>
-<td>Case</td>
-<td>a<sub>motor,max</sub></td>
-<td>b<sub>motor,max</sub></td>
-<td>c<sub>motor,max</sub></td>
-</tr>
-<tr>
-<td>High-Efficiency</td>
-<td>0.196205</td>
-<td>3.653654</td>
-<td>0.839926</td>
-</tr>
-<tr>
-<td>Mid-Efficiency</td>
-<td>0.292280</td>
-<td>3.368739</td>
-<td>0.762471</td>
-</tr>
-<tr>
-<td>Low-Efficiency</td>
-<td>0.395895</td>
-<td>3.065240</td>
-<td>0.674321</td>
-</tr>
-
-</table>
-
-
-
-The normalized *part-load* motor efficiency model is provided to modify the maximum efficiency of the motor. This model is based on part-load data for motors from DOE’s MotorMaster+ database (2003). To determine the normalized motor efficiency at part-load (*η<sub>motor</sub>*(*x<sub>motor</sub>*)/* η<sub>motor,max</sub>*), use the motor fractional power output (*x<sub>motor</sub> =H<sub>belt</sub>* / *H<sub>belt,max</sub>*) as the fraction of motor output power in Equation and use coefficients from Table 71, or for a specific motor, determined from DOE MotorMaster+ data or from manufacturer’s data. Figure 215 shows a graphical representation of eight example curves defined by these equations and coefficients.
-
-![](media/image4919.svg.png)
-
-Figure 215. Motor Normalized Efficiency vs. Motor Load Fraction
-
-The example motor normalized efficiency curves (single rectangular hyperbola type 2) and their coefficients as a function of motor load fraction in Figure 215 are determined from DOE MotorMaster+ data and are as follows:
-
-<span>\(\frac{{{\eta_{motor}}({x_{motor}})}}{{{\eta_{motor,\max }}}} = \left[ {\frac{{{a_{PLmotor}} \cdot {x_{motor}}}}{{{b_{PLmotor}} + {x_{motor}}}}} \right] + {c_{PLmotor}} \cdot {x_{motor}}\)</span>                                             ()
-
-Table 71. Example Motor Normalized Efficiency Curve Coefficients
-
-<table class="table table-striped">
-  <tr>
-    <th>Poles</th>
-    <th>Motor Rated Output (hp)</th>
-    <th>Maximum Efficiency</th>
-    <th>a Plmotor</th>
-    <th>b Plmotor</th>
-    <th>c Plmotor</th>
-  </tr>
-  <tr>
-    <td>8</td>
-    <td>1</td>
-    <td>0.6675</td>
-    <td>1.096694</td>
-    <td>0.097126</td>
-    <td>0.002011</td>
-  </tr>
-  <tr>
-    <td rowspan="8">4</td>
-    <td>1</td>
-    <td>0.7787</td>
-    <td>1.092165</td>
-    <td>0.08206</td>
-    <td>-0.0072</td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>0.84</td>
-    <td>1.223684</td>
-    <td>0.08467</td>
-    <td>-0.135186</td>
-  </tr>
-  <tr>
-    <td>10</td>
-    <td>0.8745</td>
-    <td>1.146258</td>
-    <td>0.045766</td>
-    <td>-0.110367</td>
-  </tr>
-  <tr>
-    <td>25</td>
-    <td>0.8991</td>
-    <td>1.137209</td>
-    <td>0.050236</td>
-    <td>-0.08915</td>
-  </tr>
-  <tr>
-    <td>50</td>
-    <td>0.9129</td>
-    <td>1.088803</td>
-    <td>0.029753</td>
-    <td>-0.064058</td>
-  </tr>
-  <tr>
-    <td>75</td>
-    <td>0.9259</td>
-    <td>1.07714</td>
-    <td>0.029005</td>
-    <td>-0.04935</td>
-  </tr>
-  <tr>
-    <td>100</td>
-    <td>0.9499</td>
-    <td>1.035294</td>
-    <td>0.012948</td>
-    <td>-0.024708</td>
-  </tr>
-  <tr>
-    <td>125</td>
-    <td>0.9527</td>
-    <td>1.030968</td>
-    <td>0.010696</td>
-    <td>-0.023514</td>
-  </tr>
-</table>
-
-
-Motor efficiency therefore is:
-
-<span>\({\eta_{motor}}({x_{motor}}) = {\eta_{motor,\max }}\left[ {\frac{{{\eta_{motor}}({x_{motor}})}}{{{\eta_{motor,\max }}}}} \right]\)</span>                                                          ()
-
-Motor input power (electrical, W) is:
-
-<span>\({H_{motor}} = \frac{{{H_{belt}}}}{{{\eta_{motor}}({x_{motor}})}}\)</span>                                                                                  ()
-
-*VFD Efficiency and Input Power Model:* For VFDs, published performance data are limited. Data from DOE (2008) suggest using a functional relation similar to that used for motors to represent VFD efficiency (*η<sub>VFD</sub>*) as a function of the fraction of full-load motor input power (*x<sub>VFD</sub> =H<sub>motor</sub>* / *H<sub>motor,max</sub>*), as shown in Figure 216, or as a function of the fraction of full-load speed (*x<sub>VFD</sub> =ω<sub>motor</sub> / ω<sub>motor,max</sub>*), as shown in Figure 217.
-
-![](media/image4923.svg.png)
-
-Figure 216. VFD Efficiency vs. Fraction of Motor Full-Load Input Power
- (*Source: DOE 2008*)
-
-![](media/image4924.svg.png)
-
-Figure 217. VFD Efficiency vs. Fraction of Full-Load Motor Speed
- (*Courtesy of Saftronics*)
-
-The performance curve (single rectangular hyperbola type 2) used here for VFD efficiency is:
-
-<span>\({\eta_{VFD}} = \left[ {\frac{{{a_{VFD}} \cdot {x_{VFD}}}}{{{b_{VFD}} + {x_{VFD}}}}} \right] + {c_{VFD}} \cdot {x_{VFD}}\)</span>                                                              ()
-
-Example coefficients derived from the DOE data as a function of the fraction of full-load motor input power are listed in Table 72.
-
-Table 72. Example VFD Efficiency Curve Coefficients
-
-<table class="table table-striped">
-<tr>
-<td>VFD Rated Output Power (hp)</td>
-<td>a<sub>vfd</sub></td>
-<td>b<sub>vfd</sub></td>
-<td>c<sub>vfd</sub></td>
-</tr>
-<tr>
-<td>3</td>
-<td>0.978856</td>
-<td>0.034247</td>
-<td>-0.007862</td>
-</tr>
-<tr>
-<td>5</td>
-<td>0.977485</td>
-<td>0.028413</td>
-<td>-0.002733</td>
-</tr>
-<tr>
-<td>10</td>
-<td>0.978715</td>
-<td>0.022227</td>
-<td>0.001941</td>
-</tr>
-<tr>
-<td>20</td>
-<td>0.984973</td>
-<td>0.017545</td>
-<td>-0.000475</td>
-</tr>
-<tr>
-<td>30</td>
-<td>0.987405</td>
-<td>0.015536</td>
-<td>-0.005937</td>
-</tr>
-<tr>
-<td>50</td>
-<td>0.987910</td>
-<td>0.018376</td>
-<td>-0.001692</td>
-</tr>
-<tr>
-<td>60</td>
-<td>0.971904</td>
-<td>0.014537</td>
-<td>0.011849</td>
-</tr>
-<tr>
-<td>75</td>
-<td>0.991874</td>
-<td>0.017897</td>
-<td>-0.001301</td>
-</tr>
-<tr>
-<td>100</td>
-<td>0.982384</td>
-<td>0.012598</td>
-<td>0.001405</td>
-</tr>
-<tr>
-<td>&gt;= 200</td>
-<td>0.984476</td>
-<td>0.009828</td>
-<td>-0.004560</td>
-</tr>
-
-</table>
-
-
-
-VFD input power (electrical, W) is:
-
-<span>\({H_{VFD}} = \frac{{{H_{motor}}}}{{{\eta_{VFD}}}}\)</span>                                                                                          ()
-
-*System Total Efficiency: T*he combined efficiency of the fan system components (i.e., fan, belt, motor, and VFD) is:
-
-<span>\({\eta_{TOTAL}} = {\eta_{fan}} \cdot {\eta_{belt}} \cdot {\eta_{motor}} \cdot {\eta_{VFD}}\)</span>    <span>\(\left( { = \frac{{{Q_{fan}} \cdot \Delta {P_{fan}}}}{{{H_{VFD}}}}} \right)\)</span>                                     ()
-
-*Heat Loss to Air*: To calculate the temperature rise from waste heat entering the air stream from the fan, belt, and motor, it is assumed that the user-specified “motor in air fraction� applies to the belt and motor but not to the VFD. The power “lost� to the air (W) is:
-
-<span>\({\dot Q_{toair}} = {H_{fan}} + \left( {{H_{motor}} - {H_{fan}}} \right) \cdot {f_{motortoair}}\)</span>                                                    ()
-
-### References
-
-AMCA. 1990a. “Fans and Systems�. Publication 201-90. Arlington Heights, IL: Air Movement and Control Association International.
-
-AMCA. 1990b. “Field Performance Measurement of Fan Systems�. Publication 203-90. Arlington Heights, IL: Air Movement and Control Association International.
-
-ASHRAE. 1993. HVAC 2 Toolkit: Algorithms and Subroutines for Secondary HVAC System Energy Calculations. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 1999. “ANSI/ASHRAE Standard 120 Method of Testing to Determine Flow Resistance of HVAC Ducts and Fittings�. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2008. “ANSI/ASHRAE Standard 126 Method of Testing HVAC Air Ducts and Fittings�. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-DOE. 2003. “MotorMaster 4.0 User Guide�. U.S. Department of Energy, Industrial Technologies Program.
-
-
-
-DOE. 2008. “Energy Tips – Motor: Motor Tip Sheet \#11�. U.S. Department of Energy, Industrial Technologies Program. June.
-
-
-
-Federspiel, C. 2004. “Detecting Optimal Fan Pressure�. Final Report of Federspiel Controls to the CEC Energy Innovations Small Grant Program. Grant \#: 02-03.
-
-Federspiel, C. 2005. “Detecting Critical Supply Duct Pressure�. ASHRAE Transactions, Vol. 111, Part 1. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Heredos, Francis P. 1987. Selection and Application of Multispeed Motors, IEEE Transactions on Industry Applications, Vol. 1A-23, No. 2, March/April.
-
-Liu, M., D.E. Claridge, and S. Deng. 2003. “An Air Filter Pressure Loss Model for Fan Energy Calculation in Air-Handling Units�. International Journal of Energy Research. Vol. 27, pp. 589-600.
-
-Nadel, S., R.N. Elliot, M. Shepard, S. Greenberg, G. Katz, and A.T. de Almeida. 2002. “Energy-Efficient Motor Systems: A Handbook on Technology, Program, and Policy Opportunities� 2nd Edition. Washington, DC: American Council for an Energy Efficient Economy. p.188.
-
-Sherman, M.H. and C.P. Wray. 2010. “Parametric System Curves: Correlations Between Fan Pressure Rise and Flow for Large Commercial Buildings�. Lawrence Berkeley National Laboratory Report, LBNL-3542E.
-
-Stein, J. and M.M. Hydeman. 2004. “Development and Testing of the Characteristic Curve Fan Model�. ASHRAE Transactions, Vol. 110, Part 1. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Trane. 1999. “Delta-Flo Coils: Data Catalog PL-AH-COIL-000-D-2-799�. LaCrosse, WI: The Trane Company. July.
-
-Air System Compound Component Groups <a name="AirComponentGroups"></a>
-------------------------------------
-
-### Unitary Systems
-
-#### Overview
-
-The input object AirLoopHVAC:UnitarySystem provide a “virtual� component that collect and control a set of components: fan, heating coil, cooling coil, and/or reheat coil. Reheat coil is modeled for controlling high zone humidity levels. The unit may be configured to have either a blow through or draw through fan. In a blow through configuration, fan is generally the fist component upstream of heating ro cooling coil. In a draw through fan configuration, fan is placed directly after the heating coil and before reheat coil.
-
-![](media/image4930.png)
-
-Figure 218. Schematic of the EnergyPlus Unitary System (Blow Through Configuration)
-
-#### Model Description
-
-As described previously, the unitary system is a “virtual� component consisting of a fan, heating coil, cooling coil and reheat coil. The sole purpose of the unitary system model is to properly coordinate the operation of the various system components. The following sections describe the flow of information within the model, as well as the differences between cycling and continuous supply air fan operation.
-
-#### Controls
-
-There are two types of control types allowed to be specified in the unitary system which are setpoint based and load based. Each control type is described in detail below.
-
-
-
-####Setpoint based control:
-
-The unitary system calculates the current sensible load using the temperature of the inlet node and the System Node Setpoint Temp on the control node. If the control node is not the outlet node, the desired outlet node temperature is adjusted for the current temperature difference between the outlet node and the control node. Likewise, the current latent load is calculated using the humidity ratio of the inlet node and the System Node Humidity Ratio Max on the control node. The controls determine the required coil run-time fraction and dehumidification mode (if applicable) using the steps outlined below.
-
-##### Step 1 – Meet Sensible Load Requirement
-
-The controls first attempt to meet the sensible requirement. The specified coil model is called with a part-load ratio (PLR) of 1.0 to determine the full-load output of the coil. This is compared with the desired outlet node temperature and a sensible PLR is calculated. If the PLR is &lt;1.0, a Regula-Falsi iteration routine is called to determine the coil run-time fraction which results in the desired outlet node temperature. For a variable-speed DX cooling coil, if the load is smaller than the sensible capacity at the lowest speed, the coil run-time fraction is determined in the same way as a single-speed DX cooling coil. Otherwise, its speed number and speed ratio between two neighboring speeds are selected to match the load.
-
-##### Step 2 – Meet Latent Load Requirement (if activated)
-
-If dehumidification controls are active, the leaving humidity ratio resulting from operation to meet the sensible load (Step 1 above) is compared with the desired outlet node humidity ratio. If the humidity requirement is already met, then no further control action is taken. If the humidity requirement has not been met, then the coil is re-simulated depending on the type of humidity control.
-
-##### Step 2a – Humidity Control = MultiMode
-
-If the humidity control type is MultiMode, then the coil's enhanced dehumidification mode is activated when the coil type is Coil:Cooling:DX:TwoStageWithHumidityControlMode and Step 1 above is repeated to meet the sensible load using the coil performance resulting from the enhanced dehumidificaiton mode. This is a semi-passive approach to dehumidification which may fall short or may exceed the dehumidification requirement.
-
-##### Step 2b – Humidity Control = CoolReheat
-
-If the humidity control type is CoolReheat, the coil is re-simulated to achieve the desired outlet node humidity ratio. This option is valid for all cooling coil types. When the coil type is Coil:Cooling:DX:TwoStageWithHumidityControlMode, only the cooling performance mode is used for this step and enhanced dehumidification mode is not activated.
-
-
-
-####Load based control:
-
-While the unitary system may be configured to serve multiple zones, system operation is controlled by a thermostat located in a single “control� zone. One of the key parameters for the unitary system component is the fraction of the total system air flow that goes through the control zone. This fraction is calculated as the ratio of the maximum air mass flow rate for the air loop’s supply inlet node for the control zone (e.g., AirTerminal:SingleDuct:Uncontrolled, field = Maximum Air Flow Rate, converted to mass flow) to the sum of the maximum air mass flow rates for the air loop’s supply inlet nodes for all zones served by this air loop. The unitary system module scales the calculated load for the control zone upward based on this fraction to determine the total load to be met by the unitary system. The module then proceeds to calculate the required part-load ratio for the system coil and the supply air fan to meet this total load. The heating or cooling capacity delivered by the unitary system is distributed to all of the zones served by this system via the terminal units that supply air to each zone. The supply air fraction that goes though the control zone is calculated as follows:
-
-<div>$$Control Zone Air Flow\,Fraction = \frac{{{{\dot m}_{TUMax\,ControlZone}}}}{{\sum\limits_{j = 1}^{NumOfZones} {{{\dot m}_{TUMax\,Zone\,j}}} }}$$</div>
-
-where:
-
-<span>${\dot m_{TUMax\,ControlledZone}}$</span>    =    maximum air mass flow rate for the air loop’s supply inlet node (terminal unit) for the control zone (kg/s)
-
-<span>${\dot m_{TUMax\,Zone\,j}}$</span>            =    maximum air mass flow rate for the air loop’s supply inlet node for the jth zone (kg/s)
-
-<span>$NumOfZones$</span>                =    number of zones, or number of air loop supply air inlet nodes for all zones served by the air loop (-)
-
-The unitary system component is able to model supply air fan operation in two modes: cycling fan – cycling coil (i.e., AUTO fan) and continuous fan – cycling coil (i.e., fan ON). Fan:OnOff must be used to model AUTO fan, while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON. The fan operation mode is specified using a supply air fan operating mode schedule where schedule values of 0 denote cycling fan operation and schedule values other than 0 (a 1 is usually used) denote continuous fan operation. Using this schedule, the unitary system fan may be cycled with cooling or heating coil operation or operated continuously based on time of day (e.g., cycling fan operation at night and continuous fan operation during the daytime). If the fan operating mode schedule name field is left blank in the unitary system object, the unitary system assumes cycling or AUTO fan mode operation throughout the simulation.
-
-The unitary system operates based on the user-specified (or autosized) design supply air flow rate(s). The ‘design’ supply air mass flow rate may be different for cooling, heating, and when no cooling or heating is required and the fan operates continuously based on user-specified inputs.
-
-**Cooling Operation**
-
-If EnergyPlus determines that the unitary system must supply cooling to the control zone to meet the zone air temperature setpoint, then the model computes the total sensible cooling load to be met by the unitary system based on the control zone sensible cooling load and the fraction of the unitary system air flow that goes through the control zone.
-
-<div>$$UnitarySystemCoolingLoad = \frac{{ControlZoneCoolingLoad}}{{ControlZoneAirFlowFraction}}$$</div>
-
-If the supply air fan operating mode schedule requests cycling fan operation, the model first checks for the presence of an ecomomizer in the outside air system serving the unitary system’s air loop (Ref. AirLoopHVAC:OutdoorAirSystem). If an outside air system is not present or if an air-side economizer is not used, the unitary system’s compressor is used to meet the unitary system cooling load. If an air-side economizer is used and is active (i.e., economizer controls indicate that conditions are favorable to increase the outside air flow rate), the unitary system will try to meet the cooling load by operating only the supply air fan. If the fan is able to satisfy the unitary system cooling load, the compressor remains off for the entire simulation time step. If the operation of the fan alone is unable to meet the entire cooling load, then the compressor is enabled and additional calculations are performed to determine the compressor’s part-load ratio.
-
-The model then calculates the unitary system’s sensible cooling energy rate delivered to the zones being served when the system runs at full-load conditions and when the cooling coil is OFF. If the supply air fan cycles with the compressor, then the sensible cooling energy rate is zero when the cooling coil is OFF. However if the fan is configured to run continuously regardless of coil operation, then the sensible cooling energy rate will probably not be zero when the cooling coil is OFF. Calculating the sensible cooling energy rate involves modeling the supply air fan (and associated fan heat), the cooling coil, and the heating and reheat coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and cooling coil OFF), the sensible cooling energy rate delivered by the unitary system is calculated as follows:
-
-
-<div>$$Full\;Cool\;Output = (Mass\;Flow\;Rat{e_{full\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}$$</div>
-
-<div>$$No\;Cool\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}$$</div>
-
-where:
-
-*Mass Flow Rate<sub>full load</sub>* = air mass flow rate through unitary system at full-load conditions, kg/s
-
-*h<sub>out, full load</sub>* = enthalpy of air exiting the unitary system at full-load conditions, J/kg
-
-*h<sub>control zone</sub>*<sub> </sub> = enthalpy of air in the control zone (where thermostat is located), J/kg
-
-*HR<sub>min</sub>      =* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the unitary system exiting air or the air in the control zone
-
-*Mass Flow Rate<sub>coil off</sub>* = air mass flow rate through the unitary system with the cooling coil OFF, kg/s
-
-*h<sub>out, coil off</sub>*  = enthalpy of air exiting the unitary system with the cooling coil OFF, J/kg
-
-Δ<sub>sen,</sub> *<sub>full load</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;full\;load}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{full\;load}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;full\;load}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-where:
-
-Frac = Control zone air fraction with respect to the system mass flow rate
-
-Δ<sub>sen,coil off</sub>=Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;coil\;off}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{coil\;off}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;coil\;off}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-With the calculated sensible cooling energy rates and the total sensible cooling load to be met by the system, the part-load ratio for the unitary system is estimated.
-
-<div>$$PartLoadRatio = MAX\left( {0.0,\frac{{\left( {UnitarySystemCoolingLoad - NoCoolOutput} \right)}}{{\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)$$</div>
-
-Since the part-load performance of the cooling coil is frequently non-linear, and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the unitary system’s cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system’s cooling output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemCoolingLoad - {Q_{UnitarySystem}}} \right)}}{{UnitarySystemCoolingLoad}}$$</div>
-
-where:
-
-<span>${Q_{UnitarySystem}}$</span>= Unitary system delivered sensible capacity (W)
-
-If the unitary system has been specified with cycling fan/cycling coil (AUTO fan), then the unitary system’s operating supply air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. In this case, the air conditions at nodes downstream of the cooling coil represent the full-load (steady-state) values when the coil is operating.
-
-If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the unitary system is calculated as the average of the user-specified air flow rate when the cooling coil is ON and the user-specified air flow rate when the cooling coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
-
-<div>$${{\mathop m\limits^ \bullet  }_{UnitarySystem}} = PartLoadRatio\left( {{{\mathop m\limits^ \bullet  }_{CoolCoilON}}} \right) + \left( {1 - PartLoadRatio} \right)\left( {{{\mathop m\limits^ \bullet  }_{CoilOFF}}} \right)$$</div>
-
-where:
-
-<span>$\mathop m\limits^ \bullet  <sub>CoolCoilON</sub>$</span> = air mass flow rate through unitary system when the cooling coil is ON (kg/s)
-
-<span>$\mathop m\limits^ \bullet  <sub>CoilOFF</sub>$</span> = air mass flow rate through unitary system when no cooling or heating is needed (kg/s)
-
-In this case, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF).
-
-
-
-**Cooling Operation (multi or variable speed coils)**
-
-After the unitary system cooling load is determined as described in Eq. above, the multi or variable speed cooling coil models calculations are described in this section.
-
-The model calculates the unitary system’s sensible cooling energy rate delivered to the zones being served when the system runs at full-load conditions at the highest speed and when the DX cooling coil is OFF. If the supply air fan cycles with the compressor, then the sensible cooling energy rate is zero when the cooling coil is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible cooling energy rate will not be zero when the cooling coil is OFF. Calculating the sensible cooling energy rate involves modeling the supply air fan (and associated fan heat) and the multi/variable speed DX cooling coil. The multi/variable speed DX heating coil and the supplemental heating coil are also modeled, but only to pass the air properties and mass flow rate from their inlet nodes to their outlet nodes. For each of these cases (full load at highest cooling speed and DX cooling coil OFF), the sensible cooling energy rate delivered by the unitary system is calculated as follows:
-
-<div>$$FullCoolOutpu{t_{Highest\;Speed}} = ({\dot m_{HighestSpeed}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;HighestSpeed}}$$</div>
-<div>$$NoCoolOutput = ({\dot m_{CoilOff}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}$$</div>
-
-where:
-
-*<span>${\dot m_{HighestSpeed}}$</span>* = air mass flow rate through unitary system at the highest cooling speed [kg/s]
-
-*h<sub>out, full load</sub>*   = enthalpy of air exiting the unitary system at full-load conditions [J/kg]
-
-*h<sub>control zone</sub>*   = enthalpy of air leaving the control zone (where thermostat is located) [J/kg]
-
-*HR<sub>min</sub>=* the minimum humidity ratio of the unitary system exiting air or the air leaving the control zone [kg/kg]
-
-<span>${\dot m_{CoilOff}}$</span> = air mass flow rate through the unitary system with the cooling coil OFF [kg/s]
-
-*h<sub>out,coil off</sub>*    = enthalpy of air exiting the unitary system with the cooling coil OFF [J/kg]
-
-Δ<sub>*sen,*</sub> *<sub>HighestSpeed</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions
-
-Δ<sub>*sen,coil off*</sub>=Sensible load difference between the system output node and the zone inlet node with the cooling coil OFF conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;HighestSpeed}} = \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad \quad  + \left( {{{\dot m}_{_{HighestSpeed}}} - \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;full\;load}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;coil\;off}} = \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {{{\dot m}_{_{coil\;off}}} - \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;coil\;off}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-where:
-
-Frac = Control zone air fraction with respect to the system mass flow rate
-
-If the unitary system’s sensible cooling rate at the highest speed (full load, no cycling) is insufficient to meet the entire cooling load, the controlled zone conditions will not be met. The reported cycling rate and speed ratio are 1, and the speed number is set to the highest index number. If the total sensible cooling load to be met by the system is less than the sensible cooling rate at the highest speed, then the following steps are performed.
-
-·        Calculate the sensible cooling energy rate at Speed 1
-
-<div>$$FullCoolOutpu{t_{Speed1}} = ({\dot m_{Speed1}}){({h_{out,fullload}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;Speed1}}$$</div>
-
-where
-
-*<span>${\dot m_{Speed1}}$</span>* = air mass flow rate through unitary system at Speed 1 [kg/s]
-
-Δ<sub>*sen,*</sub> <sub>*Speed1*</sub>=Sensible load difference between the system output node and the zone inlet node at full-load conditions at Speed 1
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;Speed1}} = \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {{{\dot m}_{_{Speed1}}} - \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;full\;load}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-·        If the sensible cooling energy rate delivered by the unitary system at Speed 1 is greater or equal to the sensible load, the cycling ratio (part-load ratio) for the unitary system is estimated.
-
-<div>$$\begin{array}{l}CyclingRatio = \frac{{\left( {ABS(CoolingCoilSensibleLoad)} \right)}}{{FullCoolingCoilCapacity}}\\ = MAX\left( {0.0,\frac{{\left( {UnitarySystemCoolingLoad - AddedFanHeat} \right)}}{{\left( {FullCoolOutpu{t_{Speed1}} - AddedFanHea{t_{Speed1}}} \right)}}} \right)\end{array}$$</div>
-
-
-
-where
-
-*AddedFanHeat*  = generated supply air fan heat, which is a function of part load ratio and as internal component cooling load [W].
-
-*AddedFanHeat<sub>Speed1</sub>*        = generated supply air fan heat at Speed 1 (part load ratio=1) [W].
-
-Since the part-load performance of the DX cooling coil is frequently non-linear,and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the unitary system’s cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system’s cooling output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemOutpu{t_{cycling}} - {Q_{UnitarySystem}}} \right)}}{{UnitarySystemCoolingLoad}}$$</div>
-
-where:
-
-Unitary systemOutput<sub>Cycling</sub> = unitary system delivered sensible capacity for Speed 1 operating at a specific cycling ratio (W)
-
-<div>$$UnitarySystemOutpu{t_{cycling}} = {\mathop m\limits^ \bullet_{UnitarySystem}}{\left( {{h_{out}} - {h_{ControlZone}}} \right)_{HR\min }} - {\Delta_{cycling}}$$</div>
-
-where
-
-<span>${\dot m{_{UnitarySystem}}}$</span>      = average air mass flow rate defined in the next section [kg/s]
-
-*h<sub>out,</sub>*        = enthalpy of air exiting the unitary system at part load conditions [J/kg]
-
-Δ<sub>*cycling*</sub>    =average sensible load difference between the system output node and the zone inlet node
-
-<div>$${\Delta_{cycling}} = \frac{{{{\mathop m\limits^ \bullet  }_{ZoneInlet}}}}{{frac}}\left( {{h_{ZoneInlet}} - {h_{ControlZone}}} \right) + \left( {{{\mathop m\limits^ \bullet  }_{UnitarySystem}} - \frac{{{{\mathop m\limits^ \bullet  }_{ZoneInlet}}}}{{frac}}} \right)\left( {{h_{Out}} - {h_{ControlZone}}} \right)$$</div>
-
-
-
-<span>${\dot m{_{ZoneInlet}}}$</span> = Air mass flow rate in the supply inlet node in the controlled zone [kg/s]
-
-For this case where speed 1 operation was able to meet the required cooling load, the speed ratio is set to zero and speed number is equal to 1.
-
-·        If the unitary system’s cooling output at full load for Speed 1 is insufficient to meet the entire cooling load, the Cycling ratio is set equal to 1.0 (compressor and fan are not cycling). Then the cooling speed is increased and the delivered sensible capacity is calculated. If the full load sensible capacity at Speed n is greater than or equal to the sensible load, the speed ratio for the unitary system is estimated:
-
-<div>$$SpeedRatio = \frac{{ABS\left( {UnitarySystemCoolingLoad - AddedFanHeat - FullCoolOutpu{t_{Speedn - 1}}} \right)}}{{ABS\left( {FullCoolOutpu{t_{Speedn}} - FullCoolOutpu{t_{Speedn - 1}}} \right)}}$$</div>
-
-Although a linear relationship is assumed by applying the speed ratio to obtain the effective capacity and mass flow rate between speed n and n-1, the outlet air node conditions are dependent on the combined outputs and may not be linear. In addition, the supply air fan heat varies with the speed ratio due to different supply mass flow rates between speed n and n-1 . Therefore, the final speed ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the unitary system’s cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system’s cooling output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemCoolingLoad - UnitarySystemOutpu{t_{SpeedRatio}}} \right)}}{{UnitarySystemCoolingLoad}}$$</div>
-
-where:
-
-*UnitarySystemOutput<sub>Speedn</sub>*= unitary system delivered sensible capacity between two consecutive speeds at a specific speed ratio (W)
-
-<div>$$\begin{array}{l}UnitarySystemOutpu{t_{SpeedRatio}} = (SpeedRatio)FullCoolOutpu{t_{Speedn}} + \\\quad \quad \quad \quad \quad (1 - SpeedRatio)FullCoolOutpu{t_{Speedn - 1}} - AddedFanHea{t_{SpeedRatio}}\end{array}$$</div>
-
-Where
-
-*AddedFanHeat<sub>SpeedRatio</sub>*          = generated supply air fan heat at a specific speed ratio [W]
-
-In this case, the reported cycling ratio is 1 and speed number is equal to n.
-
-##### Air Mass Flow Rate Calculation
-
-Speed 1 operation
-
-If the unitary system has been specified with cycling fan/cycling coil (AUTO fan), then the unitary system’s operating supply air mass flow rate is determined by the cycling ratio (PartLoadRatio) for Speed 1. The supply air mass flow rate is multiplied by the cycling ratio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the cooling coils represent the full-load (steady-state) values when the coil is operating.
-
-<div>$${{\mathop m\limits^ \bullet  }_{UnitarySystem}} = \left( {CyclingRatio} \right){{\mathop m\limits^ \bullet  }_{Speed1}}$$</div>
-
-If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the unitary system is calculated as the average of the user-specified air flow rate when the unitary system cooling coil is ON at Speed 1 and the user-specified air flow rate when the unitary system cooling coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
-
-<div>$${{\mathop m\limits^ \bullet  }_{UnitarySystem}} = \left( {CyclingRatio} \right){{\mathop m\limits^ \bullet  }_{Speed1}} + \left( {1 - CyclingRatio} \right){{\mathop m\limits^ \bullet  }_{CoilOff}}$$</div>
-
-where:
-
-<span>${\dot m_{UnitarySystem}}$</span> = average air mass flow rate through unitary system [kg/s]
-
-<span>${\dot m_{Speed1}}$</span>= air mass flow rate through unitary system when cooling coil is ON at Speed 1 [kg/s]
-
-<span>${\dot m_{CoilOff}}$</span> = air mass flow rate through unitary system when no heating or cooling is needed [kg/s]
-
-In this case, the air conditions at nodes downstream of the cooling coils are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF).
-
-##### Higher Speed Operation
-
-When the unitary system operates at higher speeds to meet the required cooling load, the supply air mass flow rate is linearly interpolated between two consecutive speeds:
-
-<div>$${{\mathop m\limits^ \bullet  }_{UnitarySystem}} = \left( {SpeedRatio} \right){{\mathop m\limits^ \bullet  }_{Speedn}} + \left( {1 - SpeedRatio} \right){{\mathop m\limits^ \bullet  }_{Speedn - 1}}$$</div>
-
-where:
-
-<span>${{\mathop m\limits^ \bullet  }_{UnitarySystem}}$</span>= average air mass flow rate through the unitary system for the time step [kg/s]
-
-<span>${\dot m_{Speedn}}$</span>= air mass flow rate through unitary system when cooling coil is ON at Speed n [kg/s]
-
-<span>${\dot m_{Speedn - 1}}$</span>= air mass flow rate through unitary system when cooling coil is ON at Speed n-1 [kg/s]
-
-For this case of higher speed operation, the air conditions at nodes downstream of the cooling coils are determined by the delivered cooling capacity and supply air mass flow rates between two consecutive speeds.
-
-Although the above sections present the capacity and air mass flow rate calculation separately, they are dependent and change every iteration until convergence is reached for the time step being simulated.
-
-
-
-**Heating Operation**
-
-Calculations for heating operation are similar to those for cooling operation in most respects. However, due to the inclusion of a supplemental heating coil, additional calculations are necessary to properly meet the total heating load for the zones being served.
-
-If EnergyPlus determines that the unitary system must supply heating to the control zone to meet the zone air temperature setpoint, then the unitary system model computes the total sensible heating load to be delivered to the zones being served based on the control zone sensible heating load and the control zone airflow fraction.
-
-<div>$$UnitarySystemHeatingLoad = \frac{{ControlZoneHeatingLoad}}{{ControlZoneAirFlowFraction}}$$</div>
-
-The model then calculates the unitary system’s sensible heating energy rate delivered to the zones being served when the system runs at full-load conditions and when the heating coil is OFF (without supplemental heater operation in either case). If the supply air fan cycles with the compressor, then the sensible heating energy rate is zero when the compressor is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible heating energy rate will not be zero when the compressor is OFF. Calculating the sensible heating energy rate involves modeling the supply air fan (and associated fan heat), the  cooling coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node), the  heating coil, and the supplemental heating coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and  heating coil OFF, without supplemental heater operation in either case), the sensible heating energy rate delivered by the unitary system is calculated as follows:
-
-<div>$$Full\;Heat\;Output = (Mass\;Flow\;Rat{e_{ful\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}$$</div>
-
-<div>$$No\;Heat\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}$$</div>
-
-where:
-
-*Mass Flow Rate <sub>full load</sub>*  = air mass flow rate through unitary system at full-load conditions, kg/s
-
-*h<sub>out, full load</sub>*  = enthalpy of air exiting the unitary system at full-load conditions, J/kg
-
-*h<sub>control zone</sub>*  = enthalpy of air leaving the control zone (where thermostat is located), J/kg
-
-*HR<sub>min</sub>=* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the unitary system exiting air or the air leaving the control zone
-
-*Mass Flow Rate <sub>coil off</sub>*  = air mass flow rate through the unitary system with the heating coil OFF, kg/s
-
-*h<sub>out, coil off</sub>*  = enthalpy of air exiting the unitary system with the heating coil OFF, J/kg
-
-Δ<sub>sen,</sub> *<sub>full load</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;full\;load}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{full\;load}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;full\;load}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-where:
-
-Frac = Control zone air fraction with respect to the system mass flow rate
-
-Δ<sub>sen,coil off</sub>=Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;coil\;off}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{coil\;off}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;coil\;off}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-With the calculated sensible heating energy rates and the total sensible heating load to be met by the system, the part-load ratio for the unitary system is estimated.
-
-<div>$$PartLoadRatio = MAX\left( {0.0,\frac{{\left( {UnitarySystemHeatingLoad - NoHeatOutput} \right)}}{{\left( {FullHeatOutput - NoHeatOutput} \right)}}} \right)$$</div>
-
-Since the part-load performance of the  heating coil is frequently non-linear, and the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the unitary system’s heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system’s heating output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemHeatingLoad - {Q_{UnitarySystem}}} \right)}}{{UnitarySystemHeatingLoad}}$$</div>
-
-where:
-
-<span>${Q_{UnitarySystem}}$</span>= Unitary system delivered sensible capacity (W)
-
-If the unitary system’s  heating coil output at full load is insufficient to meet the entire heating load, PartLoadRatio is set equal to 1.0 (compressor and fan are not cycling) and the remaining heating load is passed to the supplemental heating coil. If the unitary system model determines that the outdoor air temperature is below the minimum outdoor air temperature for compressor operation, the compressor is turned off and the entire heating load is passed to the supplemental gas or electric heating coil. The unitary system exiting air conditions and energy consumption are calculated and reported by the individual component models (fan,  heating coil, and supplemental gas or electric heating coil).
-
-If the unitary system has been specified with cycling fan/cycling coil (AUTO fan), then the unitary system’s operating supply air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the heating coils represent the full-load (steady-state) values when the coils are operating. If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the unitary system is calculated as the average of the user-specified air flow rate when the unitary system heating coil is ON and the user-specified air flow rate when the unitary system heating coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
-
-<div>$${{\mathop m\limits^ \bullet  }_{UnitarySystem}} = PartLoadRatio\left( {{{\mathop m\limits^ \bullet  }_{HeatCoilON}}} \right) + \left( {1 - PartLoadRatio} \right)\left( {{{\mathop m\limits^ \bullet  }_{CoilOFF}}} \right)$$</div>
-
-where:
-
-<span>${\dot m_{HeatCoilON}}$</span> = air mass flow rate through unitary system when the heating coil is ON (kg/s)
-
-<span>${\dot m_{CoilOFF}}$</span> = air mass flow rate through unitary system when no heating or cooling is needed (kg/s)
-
-In this case, the air conditions at nodes downstream of the heating coils are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coils are operating and inlet air conditions when the coils are OFF).
-
-#### Heating Operation (multi or variable speed coils )
-
-After the unitary system heating load is determined as described in Eq. above, the multi or variable speed heating coil models calculation are described in this section.
-
-The model calculates the unitary system’s sensible heating energy rate delivered to the zones being served when the system runs at full-load conditions at the highest speed and when the DX heating coil is OFF (without supplemental heater operation in either case). If the supply air fan cycles with the compressor, then the sensible heating energy rate is zero when the compressor is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible heating energy rate will not be zero when the compressor is OFF. Calculating the sensible heating energy rate involves modeling the supply air fan (and associated fan heat), the DX cooling coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node), the DX heating coil, and the supplemental heating coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and DX heating coil OFF, without supplemental heater operation in either case), the sensible heating energy rate delivered by the unitary system is calculated as follows:
-
-<div>$$FullHeatOutpu{t_{Highest\;Speed}} = ({\dot m_{HighestSpeed}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;HighestSpeed}}$$</div>
-
-<div>$$NoHeatOutput = ({\dot m_{CoilOff}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}$$</div>
-
-where:
-
-*<span>${\dot m_{HighestSpeed}}$</span>* = air mass flow rate through unitary system at the highest heating speed [kg/s]
-
-*h<sub>out, full load</sub>*   = enthalpy of air exiting the unitary system at full-load conditions [J/kg]
-
-*h<sub>control zone</sub>*   = enthalpy of air leaving the control zone (where thermostat is located) [J/kg]
-
-*HR<sub>min</sub>=* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the unitary system exiting air or the air leaving the control zone
-
-<span>${\dot m_{CoilOff}}$</span>= air mass flow rate through the unitary system with the heating coil OFF [kg/s]
-
-*h<sub>out,coil off</sub>*    = enthalpy of air exiting the unitary system with the heating coil OFF [J/kg]
-
-Δ<sub>sen,</sub> *<sub>full load</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;HighestSpeed}} = \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad \quad  + \left( {{{\dot m}_{_{HighestSpeed}}} - \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;full\;load}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-where:
-
-Frac = Control zone air fraction with respect to the system mass flow rate
-
-Δ*<sub>sen,coil off</sub>*=Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;coil\;off}} = \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {{{\dot m}_{_{coil\;off}}} - \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;coil\;off}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-If the unitary system’s DX heating coil output full load at the highest speed is insufficient to meet the entire heating load, the remaining heating load is passed to the supplemental heating coil. If the unitary system model determines that the outdoor air temperature is below the minimum outdoor air temperature for compressor operation (specified by the user), the compressor is turned off and the entire heating load is passed to the supplemental gas or electric heating coil. The unitary system exiting air conditions and energy consumption are calculated and reported by the individual component models (fan, DX heating coil, and supplemental gas or electric heating coil).
-
-If the total heating load to be met by the system is less than the sensible heating rate at the highest speed, then the following steps are performed.
-
-1.    Calculate the sensible heating energy rate at Speed 1
-
-<div>$$FullHeatOutpu{t_{Speed1}} = ({\dot m_{Speed1}}){({h_{out,fullload}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;Speed1}}$$</div>
-
-where:
-
-*<span>${\dot m_{Speed1}}$</span>* = air mass flow rate through unitary system at Speed 1 [kg/s]
-
-Δ*<sub>sen,</sub> <sub>Speed1</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions at Speed 1
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;Speed1}} = \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {{{\dot m}_{_{Speed1}}} - \frac{{{{\dot m}_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;full\;load}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-2.    If the sensible heating energy rate delivered by the unitary system at Speed 1 is greater or equal to the sensible load, the cycling ratio (part-load ratio) for the unitary system is estimated.
-
-<div>$$\begin{array}{l}CyclingRatio = \frac{{\left( {ABS(HeatingCoilSensibleLoad)} \right)}}{{FullHeatingCoilCapacity}}\\ = MAX\left( {0.0,\frac{{\left( {UnitarySystemHeatingLoad - AddedFanHeat} \right)}}{{\left( {FullHeatOutpu{t_{speed1}} - AddedFanHea{t_{speed1}}} \right)}}} \right)\end{array}$$</div>
-
-
-
-where
-
-*AddedFanHeat*        = generated supply air fan heat, which is a function of part load ratio and as internal component heating load [W].
-
-*AddedFanHeat<sub>Speed1</sub>*  = generated supply air fan heat at Speed 1 (part load ratio=1) [W].
-
-Since the part-load performance of the DX heating coil is frequently non-linear, and the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the unitary system’s heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system’s heating output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemHeatingLoad - UnitarySystemOutpu{t_{cycling}}} \right)}}{{UnitarySystemHeatingLoad}}$$</div>
-
-where:
-
-*UnitarySystemOutput<sub>cycling</sub>* = unitary system delivered sensible capacity for Speed 1 operating at a specific cycling ratio (W)
-
-<div>$$UnitarySystemOutpu{t_{cycling}} = {{\mathop m\limits^ \bullet  }_{UnitarySystem}}{\left( {{h_{out}} - {h_{ControlZone}}} \right)_{HR\min }} - {\Delta_{cycling}}$$</div>
-
-where
-
-<span>${{\mathop m\limits^ \bullet  }_{UnitarySystem}}$</span> = average air mass flow rate defined in the next section [kg/s]
-
-*h<sub>out,</sub>*              = enthalpy of air exiting the unitary system at part load conditions [J/kg]
-
-Δ*<sub>cycling</sub>*          =average sensible load difference between the system output node and the zone inlet node
-
-<div>$${\Delta_{cycling}} = \frac{{{{\mathop m\limits^ \bullet  }_{ZoneInlet}}}}{{frac}}\left( {{h_{ZoneInlet}} - {h_{ControlZone}}} \right) + \left( {{{\mathop m\limits^ \bullet  }_{UnitarySystem}} - \frac{{{{\mathop m\limits^ \bullet  }_{ZoneInlet}}}}{{frac}}} \right)\left( {{h_{Out}} - {h_{ControlZone}}} \right)$$</div>
-
-<span>${\dot m_{ZoneInlet}}$</span>       = Air mass flow rate in the supply inlet node in the controlled zone [kg/s]
-
-For this case where Speed 1 operation was able to meet the required heating load, the speed ratio is set to zero and speed number is equal to 1.
-
-3.    If the unitary system’s heating output at full load for Speed 1 is insufficient to meet the entire heating load, the Cycling ratio (PartLoadRatio) is set equal to 1.0 (compressor and fan are not cycling). Then the heating speed is increased and the delivered sensible capacity is calculated. If the full load sensible capacity at Speed n is greater than or equal to the sensible load, the speed ratio for the unitary system is estimated:
-
-<div>$$SpeedRatio = \frac{{ABS\left( {UnitarySystemHeatingLoad - AddedFanHeat - FullHeatOutpu{t_{Speedn - 1}}} \right)}}{{ABS\left( {FullHeatOutpu{t_{Speedn}} - FullHeatOutpu{t_{Speedn - 1}}} \right)}}$$</div>
-
-Although a linear relationship is assumed by applying the speed ratio to obtain the effective capacity and air mass flow rate between speed n and n-1, the outlet node conditions are dependent on the combined outputs and may not be linear. In addition, the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan). Therefore, the final speed ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the unitary system’s heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the unitary system’s heating output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge \frac{{\left( {UnitarySystemHeatingLoad - UnitarySystemOutpu{t_{SpeedRatio}}} \right)}}{{UnitarySystemHeatingLoad}}$$</div>
-
-where:
-
-*UnitarySystemOutput<sub>SpeedRatio</sub>*= unitary system delivered sensible capacity between two consecutive speeds at a specific ratio [W]
-
-<div>$$\begin{array}{l}UnitarySystemOutpu{t_{SpeedRatio}} = (SpeedRatio)FullHeatOutpu{t_{speedn}} + \\\quad \quad \quad \quad (1 - SpeedRatio)FullHeatOutpu{t_{speedn - 1}} - AddedFanHea{t_{SpeedRatio}}\end{array}$$</div>
-
-Where
-
-*AddedFanHeat<sub>SpeedRatio</sub>*          = generated supply air fan heat at a specific speed ratio [W]
-
-In this case, the reported cycling ratio is 1 and speed number is equal to n.
-
-##### Air Mass Flow Rate Calculation
-
-The air mass flow rate calculations during heating operation are the same as those described above for cooling operation for multi/variable speed.
-
-#### High Humidity Control
-
-The specific configuration of the unitary system with supplemental heating coil is shown above (see Figure 227). This figure shows the fan placement when a blow through fan is specified. If a draw through fan is specified, the fan is located between the heating coil and the supplemental heating coil. The system is controlled to keep the high relative humidity in the control zone from exceeding the setpoint specified in the object ZoneControl:Humidistat. This option is available when the supply air fan operates continuously (i.e., the supply air fan operating mode schedule values are never equal to 0) or the supply air fan cycles with the compressor. In addition, when high humidity control is specified and the compressor operates, the unitary system operates at the cooling air flow rate when a zone heating load is present as determined by the zone thermostat. High humidity control is specified as either None, MultiMode, or CoolReheat in the Dehumidification Control Type input field. MultiMode is specified when a heat exchanger is used to improve the dehumidification performance of the cooling coil. The heat exchanger will be activated when the sensible part-load ratio is insufficient to meet the zone latent load. CoolReheat is specified when a cooling coil is used to over-cool the supply air stream in order to meet the zone latent load. In this case, a supplemental heating coil will ensure the zone temperature does not fall below the zone heating temperature set point. When a heat exchanger is used in conjunction with a cooling coil and CoolReheat is specified as the Dehumidification Control Type, the heat exchanger is “locked on� to meet either the sensible or latent cooling load. If the dehumidification control type is selected as None and a heat exchanger assisted cooling coil is used, the heat exchanger is “locked on� and the air conditioner runs only to meet the sensible cooling load. A supplemental heating coil is required for all dehumidification control types.
-
-The model first calculates the *PartLoadRatio* required to meet the sensible cooling load.  The unitary system’s sensible cooling load is determined from the control zone sensible cooling load to the cooling setpoint and the control zone air flow fraction to maintain the dry-bulb temperature setpoint in the control zone.:
-
-<div>$$UnitarySystemCoolingLoad = \frac{{ControlZoneCoolingLoad}}{{ControlZoneAirFlowFraction}}$$</div>
-
-
-
-The unitary system’s sensible cooling load to be met and the full load cooling output are used to calculate the sensible the part-load ratio iteratively based on user specified convergence criterion.
-
-<div>$$PartLoadRatio = MAX\left( {0.0,\frac{{\left( {UnitarySystemCoolingLoad - NoCoolOutput} \right)}}{{\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)$$</div>
-
-When the unitary system’s sensible cooling capacity meets the system sensible cooling load at a given sensible part load ratio, then the Unitary system meets the controlled zone cooling setpoint temperature. If a moisture (latent) load exists because the control zone humidity has exceeded the setpoint, the total moisture load to be met by the unitary systems (Unitary systemMoistureLoad) is calculated based on the control zone moisture load and the control zone air flow fraction.
-
-<div>$$UnitarySystemMoistureLoad = \frac{{ControlZoneMoistureLoad}}{{ControlZoneAirFlowFraction}}$$</div>
-
-Then the *LatentPartLoadRatio* required to meet the high humidity setpoint is calculated as follows:
-
-<div>$$LatentPartLoadRatio = MIN\left( {PL{R_{Min}},\frac{{\left( {UnitarySystemMoistureLoad - NoLatentOutput} \right)}}{{\left( {FullLatentOutput - NoLatentOutput} \right)}}} \right)$$</div>
-The model uses the greater of the two part-load ratios, *PartLoadRatio* or *LatentPartLoadRatio*, to determine the operating part-load ratio of the Unitary system’s DX cooling coil.
-
-<div>$$LatentPartLoadRatio = MAX\left( {PartLoadRatio,LatentPartLoadRatio} \right)$$</div>
-
-As previously described, iterations are performed to converge on the solution within the convergence tolerance.
-
-Where,
-
-<span>$ControlZoneCoolingLoad$</span>= the control zone sensible cooling load to the cooling setpoint, (W).
-
-<span>$ControlZoneMoistureLoad$</span>          = the control zone moisture load to the dehumidifying relative humidity setpoint, (W).
-
-<span>$ControlZoneAirFlowFraction$</span>     = the supply air fraction that goes though the control zone, (-).
-
-<span>$FullLatentOutput$</span> =the Unitary system’s latent cooling energy rate at full-load conditions, W
-
-<span>$NoLatentOutput$</span>   = the Unitary system’s latent cooling energy rate with cooling coil OFF, W
-
-<span>$PartLoadRatio$</span>     = the unitary system’s part-load-ratio required to meet system sensible load, (-).
-
-<span>$LatentPartLoadRatio$</span>= the unitary system’s part-load-ratio required to meet system moisture load, (-).
-
-<span>$PL{R_{Min}}$</span>*=*the minimum part-load ratio, which is usually 0.0. For the case when the latent capacity degradation model is used (Ref: DX Cooling Coil Model), this value is the minimum part-load ratio at which the cooling coil will dehumidify the air.
-
-When the predicted zone air temperature is above the heating setpoint and if there is a dehumidification load, the supplemental heating coil load is required to offset the excess cooling as shown in Figure 228. If the model determines that the LatentPartLoadRatio is to be used as the operating part-load ratio of the unitary system’s cooling coil, the supplemental heating coil is used to offset the excess sensible capacity provided by the unitary system cooling coil. The model first checks the sensible load that exists for the current simulation time step (predicted zone temperature with no HVAC operation compared to the thermostat setpoint temperatures). If a sensible cooling load or no sensible cooling or heating load exists, the model calculates the difference between the sensible heating load required to reach or maintain the heating dry-bulb temperature setpoint and the actual sensible cooling energy rate delivered by the unit (with LatentPartLoadRatio). In this case, the supplemental heating coil is used to offset the excess sensible cooling energy provided by the cooling coil (if any) that could have caused an overshoot of the heating dry-bulb temperature setpoint. Note that when a humidistat is used and high humidity control is required, the zone dry-bulb temperature will typically move toward the heating temperature setpoint when a high moisture (latent) load exists.
-
-![HiHumidControl](media/image5015.png)
-
-Figure 219. Supplemental heating coil load when predicted zone air temperature is above the heating Setpoint
-
-If a heating load exists (Figure 229), the supplementalheating coil is used to meet the heating coil load and at the same time offset the entire sensible cooling energy rate of the cooling coil (to meet the humidistat setpoint). Note that when a heating load exists and high humidity control is required, the unitary system operates at the user-specified cooling air flow rate for the entire simulation time step. As with the fan, and cooling coil, report variables associated with supplemental heating coil performance (e.g., heating coil energy, heating coil rate, heating coil gas or electric energy, heating coil runtime fraction, etc.) are managed in the supplemental (heating) coil object.
-
-![HiHumidControl-1](media/image5016.png)
-
-Figure 220. Supplemental heating coil load when predicted zone air temperature is below the heating setpoint
-
-#### Waste Heat Calculation
-
-Waste heat calculations are done when the multi speed cooling and heating coils are specified in the unitary system and the heat recovery is active (the value of the Design Heat Recovery Water Flow Rate field is greater than 0), the outlet node temperature of heat recovery is calculated based on the recoverable waste heat generated by the child objects Coil:Cooling:DX:MultiSpeed and Coil:Heating:DX:MultiSpeed:
-
-<div>$${T_{outlet}} = {T_{inlet}} + \frac{{{Q_{WasteHeat}}}}{{{C_p}{{\dot m}_{hr}}}}$$</div>
-
-where
-
-*T<sub>outlet</sub>*            = outlet node temperature of heat recovery, C
-
-*T<sub>inlet</sub>* = inlet node temperature of heat recovery, C
-
-*Q<sub>WasteHeat</sub>*      = recoverable waste heat generated by its child objects, W
-
-*C<sub>p</sub>*              = inlet node temperature of heat recovery, C
-
-<span>${\dot m_{hr}}$</span>            = mass flow rate of heat recovery, kg/s
-
-If the outlet node temperature is above the value of the Maximum Temp for Heat Recovery field, the outlet node temperature is reset to the value of Maximum Temp for Heat Recovery.
-
-#### Multi-Speed Fan with Water Coils In Unitary System 
-
-When modeling multi-speed fan and water coils in unitary system object, the coil's capacity is modulated using speed ratio or part-load ratio.  The system load is met by varying the supply air fan speed while operating the coils at maximum water flow. When there is no system load to meet, the water control valve is fully closed.  This method of capacity control is called two-position coil control. When the supply fan is cycling between stages, then the speed ratio is calculated, but when the unit cycles between the minimum fan speed and off-position, part-load ratio is calculated. The fan may be off or run at lowest speed continuously to provide ventilation air depending the fan operating schedule. When the fan is operating at the lowest fan speed (Speed = 1), then the water flow rate is reported as the average for the time step by multiplying the maximum water flow by part load ratio. The speed ratio and part-load ratio are calculated iteratively. The set of equations used for the multi-speed fan capacity control in unitary system for water coil AHU modeling are summarized next
-
-##### Cycling Between Stages:
-When the supply fan is cycling between consecutive speeds, then the speed ratio (SR) and the average mass flow rate are calculated as follows:
-
-<div>$${SR_{n}} = Abs({SystemLoad} - {FullLoadOutput_{n-1}}) / Abs({FullLoadOutput_{n}} - {FullLoadOutput_{n-1}})$$</div>
-<div>$${\dot m} = {\dot m_{on, n}} {SR_{n}} + {\dot m_{on, n-1}} (1 - {SR_{n}})$$</div>
-<div>$${\dot m{w}} = {\dot m_{w, max}}$$</div>
-
-##### Cycling OnOff at Lowest Stage:
-The average supply air flow rate calculation when the fan is running at the lowest fan speed level depends on the fan operating schedule and load. The unitary system part load ratio is given by:
-
-<div>$${PLR} = Abs({SystemLoad} - {NoLoadOutput}) / Abs({FullLoadOutput_{1}} - {NoLoadOutput})$$</div>
-
-###### Continuous Fan:
-<div>$${\dot m} = {\dot m_{on, 1}} {PLR} + {\dot m_{off}} (1 - {PLR})$$</div>
-
-###### Cycling Fan:
-<div>$${\dot m} = {\dot m_{on, 1}} {PLR}$$</div>
-<div>$${\dot m{w}} = {\dot m_{w, max}} * {PLR}$$</div>
-
-where:
-
-{SR_{n}}		=	 speed ratio of the water coil unitary system at speed n, (-)
-
-{PLR}			=	 part load ratio of the unitary system at speed 1, (-)
-
-{\dot m}		=	 average mass flow rate of supply air, (kg/s
-
-{\dot m_{on, n-1}}	=	mass flow rate of supply air at fan speed level n-1, (kg/s)
-
-{\dot m_{on, n}}}	=	mass flow rate of supply air at fan speed level n, (kg/s)
-
-{\dot m_{off}}	=	mass flow rate of supply air when the coils are off, (kg/s)
-
-{\dot m_{w}}	=	 average mass flow rate of chilled or hot water, (kg/s)
-
-{\dot m_{w, max}}	=	maximum or full mass flow rate of chilled or hot water, (kg/s)
-
-SystemLoad 	= system load to be met by the unitary system, (W)
-
-{FullLoadOutput_{n-1}} 	= fully load system output at fan speed level n-1, (W)
-
-{FullLoadOutput_{n}} 	= fully load system output at fan speed level n, (W)
-
-
-### Forced-Air Furnace and Central Air Conditioning
-
-#### Overview
-
-The input objects AirLoopHVAC:Unitary:Furnace:HeatOnly and AirLoopHVAC:Unitary:Furnace:HeatCool provide a “virtual� component that collect and control a set of components:  an on/off or constant volume fan component and a gas or electric heating coil component. If the HeatCool version is selected, then a DX cooling coil is also modeled as part of the system as shown in Figure 221 below. For the HeatCool version, an optional reheat coil may also be modeled for controlling high zone humidity levels and the furnace’s configuration when specifying this option is shown in Figure 222 below. The unit may be configured to have either a blow through or draw through fan. If a blow through fan configuration is specified, the furnace fan is placed before the heating coil for the HeatOnly version, or before the cooling coil for the HeatCool version as shown in the figure below. If a draw through fan configuration is specified, the fan is placed directly after the heating coil.
-
-Note: the coil order shown here has been revised from previous versions of Energyplus to configure the cooling coil upstream of the heating coil. This configuration provides uniformity with all unitary equipment. However, for unitary HeatCool systems that do not use a reheat coil, the heating coil can also be placed upstream of the cooling coil. This optional coil placement is retained to allow compatibility with previous versions of Energyplus. For input files developed using previous versions of Energyplus, it is recommended that the coil order be revised according to the figure below.
-
-![FurnaceSchematic\_BlowThru](media/image5019.png)
-
-Figure 221. Schematic of the EnergyPlus Furnace (Blow Through Configuration)
-
-While the furnace may be configured to serve multiple zones, system operation is controlled by a thermostat located in a single “control� zone. One of the key parameters for the furnace component is the fraction of the total system air flow that goes through the control zone. This fraction is calculated as the ratio of the maximum air mass flow rate for the air loop’s supply inlet node for the control zone (e.g., AirTerminal:SingleDuct:Uncontrolled, field = Maximum Air Flow Rate, converted to mass flow) to the sum of the maximum air mass flow rates for the air loop’s supply inlet nodes for all zones served by this air loop. The furnace module scales the calculated load for the control zone upward based on this fraction to determine the total load to be met by the furnace. The module then proceeds to calculate the required part-load ratio for the system coil and the supply air fan to meet this total load. The heating or cooling capacity delivered by the furnace is distributed to all of the zones served by this system via the terminal units that supply air to each zone. The supply air fraction that goes though the control zone is calculated as follows:
-
-<div>$$Control Zone Air Flow\,Fraction = \frac{{{{\dot m}_{TUMax\,ControlZone}}}}{{\sum\limits_{j = 1}^{NumOfZones} {{{\dot m}_{TUMax\,Zone\,j}}} }}$$</div>
-
-where:
-
-<span>\({\dot m_{TUMax\,ControlledZone}}\)</span>    =    maximum air mass flow rate for the air loop’s supply inlet node (terminal unit) for the control zone (kg/s)
-
-<span>\({\dot m_{TUMax\,Zone\,j}}\)</span>            =    maximum air mass flow rate for the air loop’s supply inlet node for the jth zone (kg/s)
-
-<span>\(NumOfZones\)</span>                =    number of zones, or number of air loop supply air inlet nodes for all zones served by the air loop (-)
-
-The furnace component is able to model supply air fan operation in two modes: cycling fan – cycling coil (i.e., AUTO fan) and continuous fan – cycling coil (i.e., fan ON). Fan:OnOff must be used to model AUTO fan, while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON. The fan operation mode is specified using a supply air fan operating mode schedule where schedule values of 0 denote cycling fan operation and schedule values other than 0 (a 1 is usually used) denote continuous fan operation. Using this schedule, the furnace fan may be cycled with cooling or heating coil operation or operated continuously based on time of day (e.g., cycling fan operation at night and continuous fan operation during the daytime). If the fan operating mode schedule name field is left blank in the furnace object, the furnace assumes cycling or AUTO fan mode operation throughout the simulation.
-
-The only output variables reported by the furnace object are the fan part-load ratio and the compressor part-load ratio (HeatCool only). The fan part-load ratio is defined as the actual air mass flow rate through the system for the time step divided by the design supply air mass flow rate specified for the furnace (<span>\({{{{\dot m}_{actual}}} \mathord{\left/ {\vphantom {{{{\dot m}_{actual}}} {{{\dot m}_{design}}}}} \right. } {{{\dot m}_{design}}}}\)</span>)..The furnace operates based on the user-specified (or autosized) design supply air flow rate(s). The ‘design’ supply air mass flow rate may be different for cooling, heating, and when no cooling or heating is required and the fan operates continuously based on user-specified inputs (HeatCool only). For the HeatCool version, If alternate air flow rates are specified for cooling, heating, and when no cooling or heating is required, the design supply air mass flow rate is the maximum of these specified values. Also for the HeatCool version, the compressor part-load ratio is reported as the ratio of the actual cooling load to the full-load sensible capacity (see Eqn. ). Reporting of other variables of interest for the furnace (heating rate, cooling rate, energy consumption, etc.) is done by the individual system components (fan, heating coil and DX cooling coil).
-
-#### Model Description
-
-As described previously, the furnace is a “virtual� component consisting of a fan, heating coil and, for the HeatCool version, a cooling coil with an optional reheat coil. The sole purpose of the furnace model is to properly coordinate the operation of the various system components. The following sections describe the flow of information within the model for both the HeatOnly and HeatCool configurations, as well as the differences between cycling and continuous supply air fan operation. The last section describes the optional control of high zone humidity with a reheat coil for the HeatCool configuration.
-
-#### HeatOnly Configuration
-
-The HeatOnly configuration consists of an on/off or constant volume fan and an electric or gas heating coil. When the model is first called during an EnergyPlus simulation, all of the input data specified for each furnace in the input data file are read into data structures for use throughout the remainder of the simulation.
-
-For each simulation time step when the performance of a heat-only furnace is being modeled, the first step is to retrieve the heating load required to meet the thermostat setpoint for the “control� zone (see Figure 221. Schematic of the EnergyPlus Furnace). See the section “Summary of Predictor-Corrector Procedure� elsewhere in this document for more details regarding load calculations. Since the furnace may be specified to serve several zones but controlled based on the load calculated for the “control� zone, the total heating load to be met by the furnace is determined from the following equation:
-
-<div>$$Furnace\,Heating\,Load\, = \frac{{Control\,Zone\,Heating\,Load}}{{Control\,Zone\,Air\,Flow\,Fraction}}$$</div>
-
-The model then calculates the furnace’s sensible heating energy rate delivered to the zones being served when the system runs at full-load conditions and when the heating coil is OFF. If the supply air fan cycles on and off with the heater, then the sensible heating energy rate is zero when the heating coil is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible heating energy rate will not be zero when the heating coil is OFF. Calculating the sensible heating energy rate involves modeling the supply air fan (and associated fan heat) and the heating coil. For each of these cases (full load and heating coil OFF), the sensible heating energy rate delivered by the furnace is calculated as follows:
-
-<div>$$Full\;Heat\;Output = (Mass\;Flow\;Rat{e_{ful\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}$$</div>
-
-<div>$$No\;Heat\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}$$</div>
-
-where:
-
-*Mass Flow Rate<sub>full\\ load</sub>* = air mass flow rate through furnace at full-load conditions, kg/s
-
-*h<sub>out,\\ full\\ load</sub>* = enthalpy of air exiting the furnace at full-load conditions, J/kg
-
-*h<sub>control\\ zone</sub>*<sub> </sub> = enthalpy of air in the control zone (where thermostat is located), J/kg
-
-*HR<sub>min</sub>      =* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio
-
-of the furnace exiting air or the air in the control zone
-
-*Mass Flow Rate<sub>coil\\ off</sub>* = air mass flow rate through the furnace with the heating coil OFF, kg/s
-
-*h<sub>out,\\ coil\\ off</sub>*  = enthalpy of air exiting the furnace with the heating coil OFF, J/kg
-
-Δ<sub>sen,</sub> *<sub>full\\ load</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;full\;load}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{full\;load}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{_{Out,\;full\;load}}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-where:
-
-Frac = Control zone air fraction with respect to the system mass flow rate
-
-Δ<sub>sen,coil\\ off</sub>**=Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,coil\;off}} = \frac{{Mass\;Flow\;Rat{e_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \; + \left( {Mass\;Flow\;Rat{e_{coil\;off}} - \frac{{Mass\;Flow\;Rat{e_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {{h_{Out,coil\;off}} - {h_{Control\;Zone}}} \right)_{HR\min }}\end{array}$$</div>
-
-With the calculated sensible heating energy rates and the total sensible heating load to be met by the system, the part-load ratio for the furnace is estimated.
-
-<div>$$PartLoadRatio\, = \,MAX\left( {0.0,MIN\left( {1.0,\frac{{ABS\left( {FurnaceHeatingLoad - NoHeatOutput} \right)}}{{ABS(FullHeatOutput - NoHeatOutput)}}} \right)} \right)$$</div>
-
-
-
-The part-load ratio calculated above is used to determine the required heating coil capacity as <span>\(Qheating\,coil = Qdesign\,*PartLoadRatio\)</span> where *Q<sub>design</sub>* is the nominal heating coil capacity as specified in the heating coil object. If the fan cycles on and off with the heating coil (i.e.,  when the supply air fan operating mode schedule values are equal to 0), then this part-load ratio is also used to determine the operating mass flow rate of the furnace as
-
-<div>$${\dot m_{furnace}} = {\dot m_{design}}*PartLoadRatio$$</div>
-
- If the fan operates continuously (i.e. fan ON), the operating mass flow rate is specified as <span>\({\dot m_{design}}\)</span>. The furnace’s fan and heating coil are then re-simulated to determine the furnace’s delivered sensible heating capacity at the above calculated part-load ratio.
-
-<div>$${Q_{furnace}} = \left( {{{\dot m}_{furnace}}} \right){\left( {{h_{out,actual}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,\;actual}}$$</div>
-
-where:
-
-<span>\(Qfurnace\)</span>          =sensible heating capacity delivered by the furnace (W)
-
-<span>\({\dot m_{furnace}}\)</span>          = air mass flow rate through the furnace (kg/s)
-
-*h<sub>out,\\ actual</sub>*<sub>          \\      </sub> = enthalpy of air exiting the furnace (J/kg)
-
-*h<sub>out,\\ control\\ zone</sub>*  = enthalpy of air in the control zone (J/kg)
-
-*HR<sub>min</sub>      *       = enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio
-
-of the furnace exiting air or the air in the control zone
-
-Δ<sub>sen,\\ actual</sub> =Sensible load difference between the system output node and the zone inlet node at the above calculated part-load ratio.
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;actual}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;actual}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {{{\dot m}_{furnace}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;actual}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-Since the part-load performance of the heating coil can be non-linear, and the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the heating coil and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the furnace’s heating output matches the heating load to be met within the heating convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the furnace’s heating output divided by the load to be met.
-
-<div>$$Tolerance = {\raise0.7ex\hbox{${\left( {FurnaceHeatingLoad - {Q_{furnace}}} \right)}$} \!\mathord{\left/ {\vphantom {{\left( {FurnaceHeatingLoad - {Q_{furnace}}} \right)} {FurnaceHeatingLoad}}}\right.}\!\lower0.7ex\hbox{${FurnaceHeatingLoad}$}} = 0.001$$</div>
-
-If the furnace has been specified with cycling fan/cycling coil (AUTO fan), then the furnace’s design air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the heating coil represent the full-load (steady-state) values when the coil is operating. If the supply air fan is specified to run continuously (fan ON), then the air mass flow rate remains at the furnace’s design air mass flow rate. In this case, the air conditions at nodes downstream of the heating coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF).
-
-For the case where the furnace is scheduled to operate with continuous supply air fan operation, but no heating load is required to meet the setpoint temperature in the control zone, the supply air fan model is still called to determine the fan exiting air conditions. The heating coil model is also called, but for the case with no heating load the heating coil model simply passes the inlet air conditions and mass flow rate from its inlet node to its outlet node. The air exiting the heating coil is then sent to the direct air units for distribution to each zone served by the furnace, where the zone heat balance is performed to determine the resulting zone air conditions. The furnace exiting air conditions and energy consumption are calculated and reported by the individual component models (fan and heating coil).
-
-#### HeatCool Configuration
-
-The HeatCool configuration consists of an on/off or constant volume fan, a DX cooling coil, and an electric or gas heating coil. For the cases where a heating load is calculated for the control zone or no heating/cooling load is calculated for the control zone, the model follows nearly identical computational steps as described in the HeatOnly Configuration section above. The only difference is the air mass flow rate during no cooling/heating operation with continuous supply air fan operation can be different from the air mass flow rate during heater operation for the HeatCool configuration. If a cooling load is calculated by EnergyPlus for the control zone, the solution methodology is also virtually identical and is described here for completeness.
-
-If EnergyPlus determines that the furnace must supply cooling to the control zone to meet the zone air temperature setpoint, then the model computes the total sensible cooling load to be met by the furnace based on the control zone sensible cooling load and the fraction of the furnace air flow that goes through the control zone.
-
-<div>$$Furnace\,Cooling\,Load\, = \frac{{Control\,Zone\,Cooling\,Load}}{{Control\,Zone\,Air\,Flow\,Fraction}}$$</div>
-
-If the supply air fan operating mode schedule requests cycling fan operation, the model first checks for the presence of an ecomomizer in the outside air system serving the furnace’s air loop (Ref. AirLoopHVAC:OutdoorAirSystem). If an outside air system is not present or if an air-side economizer is not used, the furnace’s compressor is used to meet the furnace cooling load. If an air-side economizer is used and is active (i.e., economizer controls indicate that conditions are favorable to increase the outside air flow rate), the furnace will try to meet the cooling load by operating only the supply air fan. If the fan is able to satisfy the furnace cooling load, the compressor remains off for the entire simulation time step. If the operation of the fan alone is unable to meet the entire cooling load, then the compressor is enabled and additional calculations are performed to determine the compressor’s part-load ratio.
-
-
-
-The model then calculates the furnace’s sensible cooling energy rate delivered to the zones being served when the system runs at full-load conditions and when the DX cooling coil is OFF. If the supply air fan cycles with the compressor, then the sensible cooling energy rate is zero when the cooling coil is OFF. However if the fan is configured to run continuously regardless of coil operation, then the sensible cooling energy rate will probably not be zero when the cooling coil is OFF. Calculating the sensible cooling energy rate involves modeling the supply air fan (and associated fan heat), the DX cooling coil, and the heating coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and DX cooling coil OFF), the sensible cooling energy rate delivered by the furnace is calculated as follows:
-
-
-
-<div>$$Full\;Cool\;Output = (Mass\;Flow\;Rat{e_{ful\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}$$</div>
-
-<div>$$No\;Cool\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}$$</div>
-
-where:
-
-*Mass Flow Rate<sub>full\\ load</sub>* = air mass flow rate through furnace at full-load conditions, kg/s
-
-*h<sub>out,\\ full\\ load</sub>* = enthalpy of air exiting the furnace at full-load conditions, J/kg
-
-*h<sub>control\\ zone</sub>*<sub> </sub> = enthalpy of air in the control zone (where thermostat is located), J/kg
-
-*HR<sub>min</sub>      =* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio
-
-of the furnace exiting air or the air in the control zone
-
-*Mass Flow Rate<sub>coil\\ off</sub>* = air mass flow rate through the furnace with the cooling coil OFF, kg/s
-
-*h<sub>out,\\ coil\\ off</sub>*  = enthalpy of air exiting the furnace with the cooling coil OFF, J/kg
-
-Δ<sub>sen,</sub> *<sub>full\\ load</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;full\;load}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{full\;load}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;full\;load}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-where:
-
-Frac = Control zone air fraction with respect to the system mass flow rate
-
-Δ<sub>sen,coil\\ off</sub>**=Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;coil\;off}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{coil\;off}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;coil\;off}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-With the calculated sensible cooling energy rates and the total sensible cooling load to be met by the system, the part-load ratio for the furnace is estimated.
-
-<div>$$PartLoadRatio\, = \,MAX\left( {0.0,\frac{{ABS\left( {Furnace\,Cooling\,Load - NoCoolOutput} \right)}}{{ABS\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)$$</div>
-
-Since the part-load performance of the DX cooling coil is frequently non-linear (Ref: DX Cooling Coil Model), and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the furnace’s cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the furnace’s cooling output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge {\raise0.7ex\hbox{${\left( {FurnaceCoolingLoad - {Q_{furnace}}} \right)}$} \!\mathord{\left/ {\vphantom {{\left( {FurnaceCoolingLoad - {Q_{furnace}}} \right)} {FurnaceCoolingLoad}}}\right.}\!\lower0.7ex\hbox{${FurnaceCoolingLoad}$}}$$</div>
-
-where:
-
-<span>\(Qfurnace\)</span>= Furnace delivered sensible capacity (W)
-
-If the furnace has been specified with cycling fan/cycling coil (AUTO fan) and high humidity control *has not* been specified, then the furnace’s operating supply air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the cooling coil represent the full-load (steady-state) values when the coil is operating. If a cycling fan is used and high humidity control *has* been specified, the calculation of average air mass flow rate is based on the greater of the heating or cooling part-load ratio (see following section on high humidity control). When the heating part-load ratio is greater than the cooling part-load ratio, the air conditions at nodes downstream of the cooling coil represent the weighted average of full-load conditions when the cooling coil is operating and inlet air conditions when the cooling coil is off (i.e., the fan continues to operate due to a heating requirement where the heating PLR is greater than the cooling PLR). If the supply air fan is specified to run continuously (fan ON), then the air mass flow rate continues to operate at the user-specified supply air mass flow rate when no cooling or heating is required. In this case, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF). The furnace exiting air conditions and energy consumption are calculated and reported by the individual component models (fan and DX cooling coil).
-
-#### High Humidity Control with HeatCool Configuration
-
-An optional reheat coil can be specified with the HeatCool configuration to allow the furnace to control high zone humidity levels. The specific configuration of the HeatCool Furnace with high humidity control option is shown in Figure 222. The figure below shows the fan placement when a blow through fan is specified. If a draw through fan is specified, the fan is located between the heating coil and the reheat coil. The system is controlled to keep the relative humidity in the control zone from exceeding the setpoint specified in the object ZoneControl:Humidistat. This option is available when the supply air fan operates continuously (i.e., the supply air fan operating mode schedule values are never equal to 0) or the supply air fan cycles with the compressor. For the case of cycling fan mode when the high humidity control is specified as CoolReheat *and* the heating part-load ratio is greater than the compressor part-load ratio, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions during the duration of fan operation (i.e., the weighted average of full load conditions when the coil is operating and inlet air conditions when the coil is off and the fan continues to operate to meet the heating load). For the case where cycling fan mode is used *and* the heating part-load ratio is less than the compressor part-load ratio, the air conditions at the nodes downstream of the cooling coil are simply the full load (steady-state) values when the coil is operating. In addition, when high humidity control is specified and the compressor operates, the furnace operates at the cooling air flow rate when a zone heating load is present as determined by the zone thermostat.
-
-High humidity control is specified as either None, MultiMode, or CoolReheat in the Dehumidification Control Type input field. MultiMode is specified when a heat exchanger is used to improve the dehumidification performance of the cooling coil. The heat exchanger will be activated when the sensible part-load ratio is insufficient to meet the zone latent load. CoolReheat is specified when a DX cooling coil is used to over-cool the supply air stream in order to meet the zone latent load. In this case, a reheat coil will ensure the zone temperature does not fall below the zone heating temperature set point. When a heat exchanger is used in conjunction with a DX cooling coil and CoolReheat is specified as the Dehumidification Control Type, the heat exchanger is “locked on� to meet either the sensible or latent cooling load. If the dehumidification control type is selected as None and a heat exchanger assisted cooling coil is used, the heat exchanger is “locked on� and the air conditioner runs only to meet the sensible cooling load. Although a reheat coil is required when CoolReheat is specified in the Dehumidification Control Type input field, this reheat coil may optionally be present for the other Dehumidification Control Types (e.g., None and Multimode). If the reheat coil is present and the dehumidification control type input is not specified as CoolReheat, the reheat coil will not be active. This allows changing the dehumidification control option without requiring a change in the unit’s coil configuration.
-
-The model first calculates the PartLoadRatio required to meet the sensible cooling load as described above (see Eqn. ) to maintain the dry-bulb temperature setpoint in the control zone. If a moisture (latent) load exists because the control zone humidity has exceeded the setpoint, the total moisture load to be met by the HeatCool furnace (SystemMoistureLoad) is calculated based on the control zone moisture load and the control zone air flow fraction. The model then calculates the LatentPartLoadRatio required to meet the humidistat setpoint.
-
-<div>$$SystemMoistureLoad\, = \frac{{Control\,Zone\,Moisture\,Load}}{{Control\,Zone\,Air\,Flow\,Fraction}}$$</div>
-
-<div>$$LatentPartLoadRatio\, = \,MAX\left( {MinPLR,\frac{{ABS\left( {SystemMoistureLoad - NoLatentOutput} \right)}}{{ABS\left( {FullLatentOutput - NoLatentOutput} \right)}}} \right)$$</div>
-
-where:
-
-*FullLatentOutput  *= the furnace’s latent cooling energy rate at full-load conditions, W
-
-*NoLatentOutput*     = the furnace’s latent cooling energy rate with the cooling coil OFF, W
-
-*MinPLR*                = the minimum part-load ratio, which is usually 0.0. For the case when the latent capacity degradation model is used (Ref: DX Cooling Coil Model), this value is the minimum part-load ratio at which the cooling coil will dehumidify the air.
-
-The model uses the greater of the two part-load ratios, PartLoadRatio or LatentPartLoadRatio, to determine the operating part-load ratio of the furnace’s DX cooling coil. As previously described, iterations are performed to converge on the solution within the convergence tolerance.
-
-![FurnaceSchematic\_BlowThru\_HighRHControl](media/image5049.png)
-
-Figure 222. Schematic for Blow Through Furnace with High Humidity Control
-
-If the model determines that the LatentPartLoadRatio is to be used as the operating part-load ratio of the furnace’s cooling coil, the reheat coil is used to offset the excess sensible capacity provided by the unit. The model first checks the sensible load that exists for the current simulation time step (predicted zone temperature with no HVAC operation compared to the thermostat setpoint temperatures). If a sensible cooling load or no sensible cooling or heating load exists (Figure 223), the model calculates the difference between the sensible heating load required to reach or maintain the heating dry-bulb temperature setpoint and the actual sensible cooling energy rate delivered by the unit (with LatentPartLoadRatio). In this case, the reheat coil is used to offset the excess sensible cooling energy provided by the DX cooling coil (if any) that could have caused an overshoot of the heating dry-bulb temperature setpoint. Note that when a humidistat is used and high humidity control is required, the zone dry-bulb temperature will typically move toward the heating temperature setpoint when a high moisture (latent) load exists. If a heating load exists (Figure 224), the reheat coil is used to offset the entire sensible cooling energy rate of the DX cooling coil (to meet the humidistat setpoint) and the heating coil is used to meet the entire heating load as described in the HeatOnly configuration section above. Note that when a heating load exists and high humidity control is required, the furnace operates at the user-specified cooling air flow rate for the entire simulation time step. As with the fan, DX cooling coil, and heating coil, report variables associated with reheat coil performance (e.g., heating coil energy, heating coil rate, heating coil gas or electric consumption, heating coil runtime fraction, etc.) are managed in the reheat (heating) coil object.
-
-![ZoneLoadSchematic](media/image5050.png)
-
-Figure 223. Reheat Coil Load when Predicted Zone Temperature is Above Heating Setpoint
-
-![ZoneLoadSchematic2](media/image5051.png)
-
-Figure 224. Reheat Coil Load when Predicted Zone Temperature is Below Heating Setpoint
-
-### Unitary Systems
-
-The input objects AirLoopHVAC:UnitaryHeatCool and AirLoopHVAC:UnitaryHeatOnly provides models that are identical to the Furnace and Central Air models described above.  Please reference the previous section for details.
-
-### Unitary System with Changeover-Bypass-Variable Air Volume
-
-#### Overview
-
-The input object AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass provides a model for a changeover-bypass variable air volume (CBVAV) unitary system that is a compound object made up of other components. Each CBVAV system consists of an outside air mixer, direct expansion (DX) cooling coil, heating coil, and a supply air fan as shown in the figures below. Zone thermostats and terminal units are required in each zone served by this system. The terminal units are specific to this system type and are either AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat or AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat. A zone humidistat and single zone max humidity setpoint manager may also be specified to help control high humidity levels. These individual components are described elsewhere in this document. The CBVAV unitary system object coordinates the operation of these components and is modeled as a type of air loop equipment (Ref. AirLoopHVAC).
-
-
-
-![DrawthruCBVAV](media/image5052.png)
-
-
-
-Figure 225. Schematic of a Changeover Bypass VAV Unitary System with Draw Through Fan
-
-
-
-![BlowthruCBVAV](media/image5053.png)
-
-Figure 226. Schematic of Changeover Bypass VAV Unitary System with Blow Through Fan
-
-The CBVAV unitary system conditions one or more zones and is controlled by thermostats located in each zone (the use of a single humidistat is also allowed when using multi-mode DX cooling coils). The CBVAV system operates to meet the zone sensible cooling or sensible heating requirements as dictated by the thermostat schedule(s). The priority control input determines the mode of operation and is specified as Cooling Priority, Heating Priority, or Zone Priority. If Cooling Priority is specified, the system operates to meet the cooling load when any zone served by this system (air loop) requires cooling. If Heating Priority is specified, the system operates to meet the heating load when any zone requires heating. If Zone Priority is specified, the system operates based on the maximum number of zones requiring either heating or cooling.
-
-Once the operating mode is determined, the CBVAV model calculates a target supply air temperature required to operate a single terminal unit at its maximum air flow rate. The remaining terminal units will modulate as required to maintain the dry-bulb temperature in the zone they are serving according to the thermostat schedule for their respective zone. The system air flow rate (through the supply air fan, cooling coil and heat coil) remains constant during cooling operation, heating operation, and no cooling/heating mode as specified by the user. Therefore, as the zone terminal units modulate to reduce zone air flow rates, the excess system air flow is “bypassed� from the bypass duct splitter node back to the bypass duct mixer node of the CBVAV system (see figures above).
-
-The CBVAV system is able to model supply air fan operation in two modes: cycling fan – cycling coil (i.e., AUTO fan) and continuous fan – cycling coil (i.e., fan ON). A Fan:OnOff or Fan:ConstantVolume is used in either case. Since the excess system air flow is bypassed while the zone terminal units modulate, the supply air fan operates the entire simulation time step when heating or cooling is required. For this reason, AUTO fan only allows the supply air fan to turn off when no cooling or heating is required. If fan ON is specified, the supply air fan runs the entire time the system is scheduled to operate (via its availability schedule). The mode of operation for the supply air fan is specified through a fan operating mode schedule where a value of 0 in the schedule indicates cycling fan mode and a value greater than 0 indicates continuous fan mode. If the schedule is not provided, the supply air fan operating mode is considered to be continuous (fan ON).
-
-Output variables reported for the CBVAV system include the supply air fan part-load ratio, the compressor part-load ratio, and the electric consumption of the CBVAV system. Additional output variables report the total heating rate and total cooling rate provided by the CBVAV system. The sensible and latent components for total system cooling and heating are also available as output variables. Reporting of other variables of interest for the CBVAV system (DX coil cooling rate, heating rate, crankcase electric power and energy, supply air fan electric power, etc.) is done by the individual system components (fan, DX cooling coil, and heating coil).
-
-#### Model Description
-
-As described previously, the CBVAV system conditions one or more zones and is controlled by zone thermostats (Ref. ZoneControl:Thermostat). For each simulation time step, EnergyPlus performs a zone air heat balance to determine if cooling or heating is required to meet the zone thermostat setpoints, excluding any impacts from CBVAV system operation. CBVAV system performance is then modeled with all heating/cooling coils off but with the supply air fan operating according to the user specified supply air fan operating mode schedule. If the zone air heat balance plus the impact of CBVAV system operation with coils off results in no requirement for heating or cooling by the CBVAV coils, or if the CBVAV system is scheduled off (via its availability schedule), then the CBVAV coils do not operate and the compressor part-load ratio output variable is set to 0. If the model determines that cooling or heating is required and the CBVAV system is scheduled to operate, the model calculates a target supply air temperature required to maintain a single terminal unit at it’s maximum air flow rate, the amount of bypass air returning to the bypass duct mixer node, and the part-load ratio of the cooling or heating coils in order to meet the target supply air temperature.
-
-When high humidity control is desired, a ZoneControl:Humidistat input object and a SetpointManager:SingleZone:Humidity:Maximum, SetpointManager:MultiZone:MaximumHumidity:Average    or SetpointManager:MultiZone:Humidity:Maximum object are required. The air outlet node of the CBVAV system is used as the control node for the setpoint manager. For this reason, only a single humidistat should be specified for one of the zones being served by this system. If humidistat/setpoint manager objects are specified for more than one zone served by this system, only the last of the SetpointManager:SingleZone:Humidity:Maximum objects is used (the setpoint manager objects are read in order of occurrence in the input file). Since the outlet node of the CBVAV system is always used as the control node, the setpoints calculated by the previous setpoint managers are overwritten by the last setpoint manager in the input. When a heat exchanger is used to improve the dehumidification performance of the cooling coil (i.e. CoilSystem:Cooling:DX:HeatExchangerAssisted), the heat exchanger is always active and can not be turned on and off based on zone humidity levels.
-
-The remainder of this section describes the calculations performed when cooling or heating coil operation is required. For any HVAC simulation time step, the CBVAV system can only cool or heat the air, not both. Because the CBVAV system bypasses system air flow back to the inlet of the CBVAV unit, the system operates for the entire simulation time step. If the user specifies continuous fan operation, then the supply air fan continues to operate at a user-specified flow rate even during periods when the coils cycle off. If the user specifies AUTO fan operation, then the supply air fan cycles off for the entire simulation time step only when no cooling or heating is required.
-
-##### Operating Mode
-
-The first step in modeling a CBVAV system is to obtain the cooling or heating load for each zone as calculated by EnergyPlus based on the zone thermostat setpoint temperature(s). The calculated loads for each zone are used to determine the total cooling and heating requirements for all zones served by this system. In addition to summing the zone cooling and heating loads, the number of zones in cooling and the number of zones in heating are totalized. The priority control mode specified by the user is then used to determine the operating mode for this simulation time step.
-
-If Cooling Priority is specified and the total cooling requirement in all zones is not equal to zero, then cooling is selected as the operating mode. If the total cooling requirement is equal to zero and the total heating requirement is not equal to zero, then heating is selected as the operating mode. If the total cooling requirement and total heating requirement are equal to zero then the zones are allowed to float (no heating or cooling provided).
-
-If Heating Priority is specified and the total heating requirement in all zones is not equal to zero, then heating is selected as the operating mode. If the total heating requirement is equal to zero and the total cooling requirement is not equal to zero, then cooling is selected as the operating mode. If the total cooling requirement and total heating requirement are equal to zero then the zones are allowed to float (no heating or cooling provided).
-
-If Zone Priority is specified and the total number of zones requiring cooling is greater than the total number of zones requiring heating, then cooling is selected as the operating mode. If the total number of zones requiring heating is greater than the total number of zones requiring cooling, then heating is selected as the operating mode. If the total number of zones requiring cooling is equal to the total number of zones requiring heating, then the magnitude of the total cooling and heating requirements for all zones sets the operating mode. In this case, if the magnitudes of the cooling and heating requirements are zero, then the zones are allowed to float (no heating or cooing provided). If the magnitudes of the cooling and heating requirements are non-zero and identical, then cooling is selected as the operating mode.
-
-##### Calculation of Bypass Duct Mixer Node Conditions
-
-The operation of this system is unique in that it uses constant-air-volume equipment to provide variable air volume to the conditioned zones. This is accomplished with the use of a bypass duct (shown in the figures above) which shunts excess system air flow from the bypass duct splitter node at the system’s outlet back to the bypass duct mixer node at the system’s inlet. The air conditions at the bypass duct mixer node are based on the inlet air to the CBVAV system, the system outlet air conditions required to meet the zone loads, and the fraction of bypassed air. The following calculations are performed each simulation time step.
-
-<div>$$BypassFrac = 1.0 - \left( {\frac{{{{\dot m}_{supply}}}}{{{{\dot m}_{system}}}}} \right)$$</div>
-
-<div>$${T_{bypassductmixernode}} = \left( {1 - BypassFrac} \right){T_{inlet}} + \left( {BypassFrac} \right){T_{outlet}}$$</div>
-
-<div>$${\omega_{bypassductmixernode}} = \left( {1 - BypassFrac} \right){\omega_{inlet}} + \left( {BypassFrac} \right){\omega_{outlet}}$$</div>
-
-<div>$${h_{bypassductmixernode}} = PsyHFnTdbW\left( {{T_{mixerinlet}},{\omega_{mixerinlet}}} \right)$$</div>
-
-where:
-
-<span>\(BypassFrac\)</span>      = fraction of system air directed to the bypass duct mixer node
-
-<span>\({\dot m_{supply}}\)</span>                 = Air mass flow rate at the system’s air outlet node, kg/s
-
-<span>\({\dot m_{system}}\)</span>                 = Air mass flow rate through CBVAV system (coils and supply air fan), kg/s
-
-<span>\({T_{bypassductmixernode}}\)</span>    = Air temperature at the bypass duct mixer node, °C
-
-<span>\({T_{inlet}}\)</span>                    = Air inlet node temperature, °C
-
-<span>\({T_{outlet}}\)</span>                   = Air outlet node temperature, °C
-
-<span>\({\omega_{bypassductmixernode}}\)</span>   = Air humidity ratio at the bypass duct mixer node, kg/kg
-
-<span>\({\omega_{inlet}}\)</span>                   = Air inlet node humidity ratio, kg/kg
-
-<span>\({\omega_{outlet}}\)</span>                  = Air outlet node humidity ratio, kg/kg
-
-<span>\({h_{bypassductmixernode}}\)</span>    = Air enthalpy at the bypass duct mixer node, J/kg
-
-<span>\(PsyHFnTdbW\)</span>  = Psychrometric function calculating enthalpy given dry-bulb temperature and humidity ratio
-
-##### Cooling Operation
-
-If the model determines that the CBVAV system must supply cooling to the zones, the model first calculates a target outlet air dry-bulb temperature required to operate a single terminal unit at its maximum air flow rate. The minimum target temperature for all zones is used to control the CBVAV system in cooling mode.
-
-<div>$$T_{target}^i = T_{Zone}^i + \left( {{\raise0.7ex\hbox{${Q_{Zone}^i}$} \!\mathord{\left/ {\vphantom {{Q_{Zone}^i} {\dot m_{zone,max}^i*{C_p}}}}\right.}\!\lower0.7ex\hbox{${\dot m_{zone,max}^i*{C_p}}$}}} \right);i = 1,n$$</div>
-
-<div>$${T_{target}} = MIN\left( {T_{target}^i} \right);\,\,i = 1,n$$</div>
-
-where:
-
-<span>\(T_{target}^i\)</span>      = Target supply air temperature for zone *i*, °C
-
-<span>\(T_{zone}^i\)</span>        = Air temperature in zone *i*, °C
-
-<span>\(Q_{zone}^i\)</span>       = Cooling or heating load for zone *i* (cooling loads are negative values,      heating loads are positive values), W
-
-<span>\(Cp\)</span>          = Specific heat of supply air with coils off, J/kg-K
-
-<span>\(\dot m_{zone,max}^i\)</span>  = Maximum terminal unit mass flow rate in zone *i*, kg/s
-
-<span>\(T_{target}^{}\)</span>      = Target supply (outlet) air temperature for the CBVAV system, °C
-
-The model then calculates the part-load ratio of the DX compressor required to meet the target supply (outlet) air temperature. Since the part-load performance of the DX cooling coil is frequently non-linear (Ref: Coil:Cooling:DX:SingleSpeed model), the actual part-load ratio for the cooling coil compressor is determined through iterative calculations (successive modeling of the DX cooling coil model) until the CBVAV system’s outlet air temperature (including on/off cycling effects of the DX coil) matches the target supply (outlet) air temperature within a small temperature convergence tolerance (1E-5 ˚C).
-
-Since the supply air fan operates continuously for each simulation time step (or is OFF for the entire HVAC system time step), the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of coil’s outlet node conditions when the coil is operating and the coil’s inlet node conditions when the coil is OFF).
-
-##### Heating Operation
-
-Modeling the CBVAV system’s DX heating coil is identical to the calculations described above for cooling operation except that the maximum target supply air temperature for all zones is used to control the CBVAV system in heating mode.
-
-<div>$${T_{target}} = MAX\left( {T_{target}^i} \right);\,\,i = 1,n$$</div>
-
-Iterative calculations (successive modeling of the DX heating coil model) are used to determine the final heating coil part-load ratio to account for the non-linear performance of the DX heating coil at part-load conditions.
-
-When a gas or electric heating coil is used instead of a DX heating coil, the amount of heat required by the coil is calculated based on the target supply (outlet) air temperature and the coil inlet air temperature as follows:
-
-<div>$${Q_{heating}} = {\dot m_{system}}{C_p}({T_{target}} - {T_{inlet,heatcoil}})$$</div>
-
-where:
-
-<span>\({Q_{heating}}\)</span>       = Heating coil load, W
-
-<span>\({C_p}\)</span>             = Specific heat of heating coil inlet air, J/kg-K
-
-<span>\({T_{inlet,heatcoil}}\)</span>  = Heating coil inlet air temperature, °C
-
-##### Floating Operation (no cooling or heating)
-
-When the zone thermostats determine that there is no cooling or heating requirement in any zone, the CBVAV coils are OFF and the zone temperatures are allowed to float. However, a special case exists where the user specifies continuous supply air fan operation and no cooling or heating requirements exist in any zone. In this case, the outlet air temperature of the CBVAV system (with fan ON and coils OFF) is compared to the target outlet air temperatures required to maintain the zone’s cooling and heating setpoint temperatures. If the outlet air temperature with the supply fan ON and coils OFF is below the target outlet air temperature required to maintain the heating setpoint, then heating mode is enabled to avoid overshooting the zone heating setpoint temperature. Conversely, if the outlet air temperature with the supply fan ON and coils OFF is above the target outlet air temperature required to maintain the cooling setpoint, then cooling mode is enabled to avoid overshooting the zone cooling setpoint temperature. This special case is handled at any time a no load condition is reported by the thermostats and overshooting the zone air temperature setpoint is possible regardless of the priority control mode selected by the user.
-
-##### Minimum and Maximum Outlet Air Temperature in Cooling/Heating Operation
-
-The user also specifies a minimum outlet air temperature during cooling operation and a maximum outlet air temperature during heating operation. The target outlet air temperature, as calculated above, is compared to each of these limits during each simulation time step. The resulting target outlet air temperature is used to control the heating and cooling coils.
-
-<div>$${T_{target}} = MAX\left( {{T_{target}},\,\,{T_{min,cooling}}} \right)$$</div>
-
-<div>$${T_{target}} = MIN\left( {{T_{target}},\,\,{T_{max,heating}}} \right)$$</div>
-
-where:
-
-<span>\({T_{min,cooling}}\)</span>= Minimum outlet air temperature during cooling operation, °C
-
-<span>\({T_{max,heating}}\)</span>= Maximum outlet air temperature during heating operation, °C
-
-##### Air Flow Calculations
-
-The changeover-bypass VAV system operates based on user-specified (or autosized) air flow rates. The CBVAV system air flow rate (i.e., air flow through the supply air fan and heating/cooling coils) during cooling operation may be different than the system air flow rate during heating operation. In addition, the system air flow rate when no cooling or heating is required but the supply air fan remains ON can be different than the air flow rates when cooling or heating is required. The outside air flow rates can likewise be different in these various operating modes. The model takes these different air flow rates into account when simulating the performance of the CBVAV system. The system air flow rate for each simulation time step is based on the current operating mode (cooling, heating, or no cooling/heating) and is reported on the inlet/outlet air nodes of the various CBVAV components (e.g. fan, cooling coil, and heating coil). The supply air flow rate delivered to the individual zones is calculated based on the sum of the air flow rates through each terminal unit and is reported at the air inlet and outlet nodes of the CBVAV system each simulation time step. The difference between the system air mass flow rate and the supply air mass flow rate delivered to all zones is equal to the bypass air mass flow rate which is also reported each simulation time step.
-
-The system and outside air flow rates when a system coil is ON (e.g., system air volumetric flow rate during cooling operation, system air volumetric flow rate during heating operation, outside air volumetric air flow rate during cooling operation, and outside air volumetric air flow rate during heating operation) or the system coils are OFF and the fan operates continuously (e.g., system air volumetric flow rate when no cooling or heating is needed and outside air volumetric air flow rate when no cooling or heating is needed) are specified by the user, or can be autosized, and are converted from volumetric flow rate to mass flow rate at standard conditions. If the user has specified cycling fan operation, then the system air and outside air mass flow rates when the system coils are OFF the entire time step are zero. If the user has specified constant fan operation, then the air flow rates when no cooling or heating is needed are used when the system coils are OFF the entire time step.
-
-There is one special case. If the user has specified constant fan operation and they specify that the system air volumetric flow rate when no cooling or heating is needed is zero (or if the field is left blank), then the model assumes that the system air mass flow rate when the system coils are OFF the entire time step is equal to the corresponding air mass flow rate when any system coil was last operating (ON). This model handles the zero (or blank) entry for outside air volumetric flow rate when no cooling or heating is needed in an analogous fashion.
-
-<div>$${\dot m_{system}} = {\rho_{air,std}}*{\dot V_{mode}}$$</div>
-
-<div>$${\dot m_{system,OA}} = {\rho_{air,std}}*{\dot V_{mode,OA}}$$</div>
-
-<div>$${\dot m_{supply}} = \sum\limits_{i = 1}^n {{{\dot m}_{zone}}} $$</div>
-
-<div>$${\dot m_{bypass}} = {\dot m_{system}} - {\dot m_{supply}}$$</div>
-
-where:
-
-<span>\(\rho air,std\)</span>             = standard air density (1.204 kg/m<sup>3</sup>) adjusted for the local barometric pressure (standard barometric pressure corrected for altitude, ASHRAE 1997 HOF pg. 6.1), kg/m<sup>3</sup>
-
-<span>\({\dot V_{mode}}\)</span>                = User-specified system volumetric flow rate in cooling, heating, or no cooling or heating mode, m<sup>3</sup>/s
-
-<span>\({\dot m_{system,OA}}\)</span>          = Outdoor air mass flow rate introduced through the CBVAV system, kg/s
-
-<span>\({\dot V_{mode,OA}}\)</span>            = User-specified outdoor air volumetric flow rate in cooling, heating, or no cooling or heating mode, m<sup>3</sup>/s
-
-##### Calculation of System Heating and Cooling Rates
-
-At the end of each HVAC simulation time step, this object reports the heating or cooling rate and energy delivered by the system, as well as the electric power and consumption by the system. In terms of thermal energy delivered by the system, the sensible, latent and total energy transfer rates for the system are calculated as follows:
-
-<div>$${\dot Q_{total}} = ({\dot m_{supply}})({h_{outlet}} - {h_{inlet}})$$</div>
-
-<div>$${\dot Q_{sensible}} = ({\dot m_{supply}}){({h_{outlet}} - {h_{inlet}})_{HRmin}}$$</div>
-
-<div>$${\dot Q_{latent}} = {\dot Q_{total}} - {\dot Q_{sensible}}$$</div>
-
-where:
-
-<sub><span>\({\dot Q_{total}}\)</span>            </sub>= total energy transfer rate by the system, W
-
-<sub><span>\({\dot Q_{sensible}}\)</span>        </sub>= sensible energy transfer rate by the system, W
-
-<sub><span>\({\dot Q_{latent}}\)</span>           </sub>= latent energy transfer rate by the system, W
-
-*h<sub>inlet</sub>*                        = enthalpy of the air entering the unit at its inlet node, J/kg
-
-*h<sub>outlet</sub>*          = enthalpy of the air leaving the unit at its outlet node, J/kg
-
-<span>\(H{R_{min}}\)</span>        = minimum of the inlet air and outlet air humidity ratio, kg/kg
-
-Since each of these energy transfer rates can be calculated as positive or negative values, individual reporting variables are established for cooling and heating and only positive values are reported. The following calculations are representative of what is done for each of the energy transfer rates:
-
-<div>$$\begin{array}{l}If\;({{\dot Q}_{total}} &lt; 0.0)\;Then\\\quad {{\dot Q}_{total,cooling}} = ABS({{\dot Q}_{total}})\\\quad {{\dot Q}_{total,heating}} = 0.0\\Else\\\quad {{\dot Q}_{total,cooling}} = 0.0\\\quad {{\dot Q}_{total,heating}} = {{\dot Q}_{total}}\\Endif\end{array}$$</div>
-
-where:
-
-<sub><span>\({\dot Q_{total,cooling}}\)</span>          </sub>= output variable ‘Unitary System Total Cooling Rate, W’
-
-<sub><span>\({\dot Q_{total,heating}}\)</span>          </sub>= output variable ‘Unitary System Total Heating Rate, W’
-
-In addition to heating and cooling rates, the heating and cooling energy supplied by the system are also calculated for the time step being reported. The following example for total zone cooling energy is representative of what is done for the sensible and latent energy as well as the heating counterparts.
-
-<div>$${Q_{total,cooling}} = {\dot Q_{total,cooling}}*TimeStepSys*3600$$</div>
-
-where:
-
-<sub><span>\({Q_{total,cooling}}\)</span>      </sub>= output variable ‘Unitary System Total Cooling Energy, J’
-
-*TimeStepSys*  = HVAC system simulation time step, hr
-
-3600              = conversion factor, sec/hr
-
-#### Changeover-bypass VAV Unitary System Sizing
-
-The changeover-bypass VAV system is modeled as an air loop component and is sized according to the methodology described elsewhere in this document (Ref. System Design Loads and Air Flow Rates). The following volumetric air flow rates may be autosized:
-
-·        system air volumetric flow rate during cooling operation
-
-·        system air volumetric flow rate during heating operation
-
-·        system air volumetric flow rate when no cooling or heating is needed
-
-·        outside air volumetric air flow rate during cooling operation
-
-·        outside air volumetric air flow rate during heating operation
-
-·        outside air volumetric air flow rate when no cooling or heating is needed
-
-### Unitary Air-To-Air Heat Pump
-
-#### Overview
-
-The input object AirLoopHVAC:UnitaryHeatPump:AirToAir provides a model for an air-to-air heat pump that is a “virtual� component that consists of an on/off or constant volume fan component, a DX cooling coil, a DX heating coil, and a gas or electric supplemental heating coil. The specific configuration of the blow through heat pump is shown in the following figure. For a draw through heat pump, the fan is located between the DX heating coil and the supplemental heating coil.
-
-![FurnaceSchematic\_HeatPump](media/image5106.png)
-
-Figure 227. Schematic of a Blow Through Air-to-Air Heat Pump
-
-While the heat pump may be configured to serve multiple zones, system operation is controlled by a thermostat located in a single “control� zone. One of the key parameters for the heat pump component is the fraction of the total system airflow that goes through the control zone. This fraction is calculated as the ratio of the maximum air mass flow rate for the air loop’s supply inlet node for the control zone (e.g., AirTerminal:SingleDuct:Uncontrolled, field = Maximum Air Flow Rate, converted to mass flow) to the sum of the maximum air mass flow rates for the air loop’s supply inlet nodes for all zones served by this air loop. The heat pump module scales the calculated load for the control zone upward based on this fraction to determine the total load to be met by the heat pump. The module then proceeds to calculate the required part-load ratio for the system coil and the supply air fan to meet this total load. The heating or cooling capacity delivered by the heat pump is distributed to all of the zones served by this system via the direct air units that supply air to each zone. The supply air fraction that goes though the control zone is calculated as follows:
-
-<div>$$Control Zone Air Flow\,Fraction = \frac{{{{\dot m}_{TUMax\,ControlZone}}}}{{\sum\limits_{j = 1}^{NumOfZones} {{{\dot m}_{TUMax\,Zone\,j}}} }}$$</div>
-
-where:
-
-<span>\({\dot m_{TUMax\,ControlledZone}}\)</span>    =    maximum air mass flow rate for the air loop’s supply inlet node (terminal unit) for the control zone (kg/s)
-
-<span>\({\dot m_{TUMax\,Zone\,j}}\)</span>            =    maximum air mass flow rate for the air loop’s supply inlet node for the jth zone (kg/s)
-
-<span>\(NumOfZones\)</span>                =    number of zones, or number of air loop supply air inlet nodes for all zones served by the air loop (-)
-
-The heat pump component is able to model supply air fan operation in two modes: cycling fan – cycling coil (i.e., AUTO fan) and continuous fan – cycling coil (i.e., fan ON). Fan:OnOff must be used to model AUTO fan, while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON. The fan operation mode is specified using a supply air fan operating mode schedule where schedule values of 0 denote cycling fan operation and schedule values other than 0 (a 1 is usually used) denote continuous fan operation. Using this schedule, the furnace fan may be cycled with cooling or heating coil operation or operated continuously based on time of day (e.g. cycling fan operation at night and continuous fan operation during the day). If the fan operating mode schedule name field is left blank in the heat pump object, the heat pump assumes cycling or AUTO fan mode operation throughout the simulation.
-
-The output variables reported by the heat pump object are fan part-load ratio and compressor part-load ratio. Fan part-load ratio is defined as the actual air mass flow rate through the system for the time step divided by the operating supply air mass flow rate specified for the heat pump (<span>\({{\mathop m\limits^\cdot  actual} \mathord{\left/ {\vphantom {{\mathop m\limits^\cdot  actual} {\mathop m\limits^\cdot  }}} \right. } {\mathop m\limits^\cdot  }}ON\)</span>). The operating supply air mass flow rate may be different for cooling, heating, and when no cooling or heating is required and the fan operates continuously. Compressor part-load ratio is the actual load for the time step divided by the full-load sensible capacity (see Eqn. or Eqn.). Reporting of other variables of interest for the heat pump (heating rate, cooling rate, energy consumption, etc.) is done by the individual system components (fan, DX cooling coil, DX heating coil, and supplemental heating coil).
-
-#### Model Description
-
-As described previously, the heat pump is a “virtual� component consisting of a fan, DX cooling coil, DX heating coil and a supplemental heating coil. The sole purpose of the heat pump model is to properly coordinate the operation of the various system components. The following sections describe the flow of information within the model, as well as the differences between cycling and continuous supply air fan operation.
-
-#### Cooling Operation
-
-If EnergyPlus determines that the heat pump must supply cooling to the control zone to meet the zone air temperature setpoint, then the heat pump model computes the total sensible cooling load to be delivered to the zones being served based on the control zone sensible cooling load and the fraction of the heat pump air flow that goes through the control zone.
-
-<div>$$Heat\,Pump\,Cooling\,Load\, = \frac{{Control\,Zone\,Cooling\,Load}}{{Control\,Zone\,Air\,Flow\,Fraction}}$$</div>
-
-If the supply air fan operating mode schedule requests cycling fan operation, the model first checks for the presence of an ecomomizer in the outside air system serving the heat pump’s air loop (Ref. AirLoopHVAC:OutdoorAirSystem). If an outside air system is not present or if an air-side economizer is not used, the heat pump’s compressor is used to meet the heat pump cooling load. If an air-side economizer is used and is active (i.e., economizer controls indicate that conditions are favorable to increase the outside air flow rate), the heat pump will try to meet the cooling load by operating only the supply air fan. If the fan is able to satisfy the heat pump cooling load, the compressor remains off for the entire simulation time step. If the operation of the fan alone is unable to meet the entire cooling load, then the compressor is enabled and additional calculations are performed to determine the compressor’s part-load ratio.
-
-The model then calculates the heat pump’s sensible cooling energy rate delivered to the zones being served when the system runs at full-load conditions and when the DX cooling coil is OFF. If the supply air fan cycles with the compressor, then the sensible cooling energy rate is zero when the cooling coil is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible cooling energy rate will not be zero when the cooling coil is OFF. Calculating the sensible cooling energy rate involves modeling the supply air fan (and associated fan heat) and the DX cooling coil. The DX heating coil and the supplemental heating coil are also modeled, but only to pass the air properties and mass flow rate from their inlet nodes to their outlet nodes. For each of these cases (full load and DX cooling coil OFF), the sensible cooling energy rate delivered by the heat pump is calculated as follows:
-
-<div>$$Full\;Cool\;Output = (Mass\;Flow\;Rat{e_{ful\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}$$</div>
-
-<div>$$No\;Cool\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}$$</div>
-
-where:
-
-*Mass Flow Rate<sub>full \\ load</sub>*  = air mass flow rate through heat pump at full-load conditions, kg/s
-
-*h<sub>out,\\ full\\ load</sub>*   = enthalpy of air exiting the heat pump at full-load conditions, J/kg
-
-*h<sub>control \\ zone</sub>*   = enthalpy of air leaving the control zone (where thermostat is located), J/kg
-
-*HR<sub>min</sub>=* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the heat pump exiting air or the air leaving the control zone
-
-*Mass Flow Rate<sub>coil\\ off</sub>*  = air mass flow rate through the heat pump with the cooling coil OFF, kg/s
-
-*h<sub>out,coil \\ off</sub>*    = enthalpy of air exiting the heat pump with the cooling coil OFF, J/kg
-
-Δ<sub>sen,</sub> *<sub>full\\ load</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;full\;load}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{full\;load}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;full\;load}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-where:
-
-Frac = Control zone air fraction with respect to the system mass flow rate
-
-Δ<sub>sen,coil\\ off</sub>**=Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;coil\;off}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{coil\;off}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;coil\;off}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-With the calculated sensible cooling energy rates and the total sensible cooling load to be met by the system, the part-load ratio for the heat pump is estimated.
-
-<div>$$PartLoadRatio\, = \,MAX\left( {0.0,\frac{{ABS\left( {Heat\,Pump\,Cooling\,Load - NoCoolOutput} \right)}}{{ABS\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)$$</div>
-
-Since the part-load performance of the DX cooling coil is frequently non-linear, and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the heat pump’s cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump’s cooling output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge {\raise0.7ex\hbox{${\left( {HeatPumpCoolingLoad - {Q_{HeatPump}}} \right)}$} \!\mathord{\left/ {\vphantom {{\left( {HeatPumpCoolingLoad - {Q_{HeatPump}}} \right)} {HeatPumpCoolingLoad}}}\right.}\!\lower0.7ex\hbox{${HeatPumpCoolingLoad}$}}$$</div>
-
-where:
-
-<span>\(QHeatPump\)</span>= Heat pump delivered sensible capacity (W)
-
-If the heat pump has been specified with cycling fan/cycling coil (AUTO fan), then the heat pump’s operating supply air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. In this case, the air conditions at nodes downstream of the cooling coil represent the full-load (steady-state) values when the coil is operating.
-
-If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the heat pump is calculated as the average of the user-specified air flow rate when the cooling coil is ON and the user-specified air flow rate when the cooling coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
-
-<div>$$\mathop m\limits^ \bullet  furnace = PartLoadRatio\left( {\mathop m\limits^ \bullet  CoolCoilON} \right) + \left( {1 - PartLoadRatio} \right)\left( {\mathop m\limits^ \bullet  CoilOFF} \right)$$</div>
-
-where:
-
-<span>\(\mathop m\limits^ \bullet  CoolCoilON\)</span> = air mass flow rate through heat pump when the cooling coil is ON (kg/s)
-
-<span>\(\mathop m\limits^ \bullet  CoilOFF\)</span> = air mass flow rate through heat pump when no cooling or heating is needed (kg/s)
-
-In this case, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF).
-
-Heating Operation
-
-Calculations for heating operation are similar to those for cooling operation in most respects. However, due to the inclusion of a supplemental heating coil, additional calculations are necessary to properly meet the total heating load for the zones being served.
-
-If EnergyPlus determines that the heat pump must supply heating to the control zone to meet the zone air temperature setpoint, then the heat pump model computes the total sensible heating load to be delivered to the zones being served based on the control zone sensible heating load and the control zone airflow fraction.
-
-<div>$$Heat\,Pump\,Heating\,Load\, = \frac{{Control\,Zone\,Heating\,Load}}{{Control\,Zone\,Air\,Flow\,Fraction}}$$</div>
-
-The model then calculates the heat pump’s sensible heating energy rate delivered to the zones being served when the system runs at full-load conditions and when the DX heating coil is OFF (without supplemental heater operation in either case). If the supply air fan cycles with the compressor, then the sensible heating energy rate is zero when the compressor is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible heating energy rate will not be zero when the compressor is OFF. Calculating the sensible heating energy rate involves modeling the supply air fan (and associated fan heat), the DX cooling coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node), the DX heating coil, and the supplemental heating coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and DX heating coil OFF, without supplemental heater operation in either case), the sensible heating energy rate delivered by the heat pump is calculated as follows:
-
-<div>$$Full\;Heat\;Output = (Mass\;Flow\;Rat{e_{ful\;load}}){({h_{out,full\;load}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;full\;load}}$$</div>
-
-<div>$$No\;Heat\;Output = (Mass\;Flow\;Rat{e_{coil\;off}}){({h_{out,\;coil\;off}} - {h_{control\;zone}})_{HR\min }} - {\Delta_{sen,\;coil\;off}}$$</div>
-
-where:
-
-*Mass Flow Rate <sub>full\\ load</sub>*  = air mass flow rate through heat pump at full-load conditions, kg/s
-
-*h<sub>out,\\ full\\ load</sub>*  = enthalpy of air exiting the heat pump at full-load conditions, J/kg
-
-*h<sub>control \\ zone</sub>*  = enthalpy of air leaving the control zone (where thermostat is located), J/kg
-
-*HR<sub>min</sub>=* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the heat pump exiting air or the air leaving the control zone
-
-*Mass Flow Rate <sub>coil \\ off</sub>*  = air mass flow rate through the heat pump with the heating coil OFF, kg/s
-
-*h<sub>out,\\ coil \\ off</sub>*  = enthalpy of air exiting the heat pump with the heating coil OFF, J/kg
-
-Δ<sub>sen,</sub> *<sub>full\\ load</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;full\;load}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{full\;load}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;full\;load}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-where:
-
-Frac = Control zone air fraction with respect to the system mass flow rate
-
-Δ<sub>sen,coil\\ off</sub>**=Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
-
-<div>$$\begin{array}{l}{\Delta_{sen,\;coil\;off}} = \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}{\left( {{h_{Out,\;coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }}\\\quad \quad \quad \quad  + \left( {Mass\;Flow\;Rat{e_{_{coil\;off}}} - \frac{{Mass\;Flow\;Rat{e_{_{Zone\;Inlet}}}}}{{Frac}}} \right){\left( {{h_{Out,\;coil\;off}} - {h_{_{Control\;Zone}}}} \right)_{HR\min }}\end{array}$$</div>
-
-With the calculated sensible heating energy rates and the total sensible heating load to be met by the system, the part-load ratio for the heat pump is estimated.
-
-<div>$$PartLoadRatio\, = \,MAX\left( {0.0,\frac{{ABS\left( {Heat\,Pump\,Heating\,Load - NoHeatOutput} \right)}}{{ABS\left( {FullHeatOutput - NoHeatOutput} \right)}}} \right)$$</div>
-
-Since the part-load performance of the DX heating coil is frequently non-linear (Ref: Single-Speed Electric Heat Pump DX Air Heating Coil), and the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the heat pump’s heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump’s heating output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge {\raise0.7ex\hbox{${\left( {HeatPumpHeatingLoad - {Q_{HeatPump}}} \right)}$} \!\mathord{\left/ {\vphantom {{\left( {HeatPumpHeatingLoad - {Q_{HeatPump}}} \right)} {HeatPumpHeatingLoad}}}\right.}\!\lower0.7ex\hbox{${HeatPumpHeatingLoad}$}}$$</div>
-
-where:
-
-<span>\(QHeatPump\)</span>= Heat pump delivered sensible capacity (W)
-
-If the heat pump’s DX heating coil output at full load is insufficient to meet the entire heating load, PartLoadRatio is set equal to 1.0 (compressor and fan are not cycling) and the remaining heating load is passed to the supplemental heating coil. If the heat pump model determines that the outdoor air temperature is below the minimum outdoor air temperature for compressor operation, the compressor is turned off and the entire heating load is passed to the supplemental gas or electric heating coil. The heat pump exiting air conditions and energy consumption are calculated and reported by the individual component models (fan, DX heating coil, and supplemental gas or electric heating coil).
-
-If the heat pump has been specified with cycling fan/cycling coil (AUTO fan), then the heat pump’s operating supply air mass flow rate is multiplied by PartLoadRatio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the heating coils represent the full-load (steady-state) values when the coils are operating. If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the heat pump is calculated as the average of the user-specified air flow rate when the heat pump heating coil is ON and the user-specified air flow rate when the heat pump heating coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
-
-<div>$$\mathop m\limits^ \bullet  HeatPump = PartLoadRatio\left( {\mathop m\limits^ \bullet  HeatCoilON} \right) + \left( {1 - PartLoadRatio} \right)\left( {\mathop m\limits^ \bullet  CoilOFF} \right)$$</div>
-
-where:
-
-<span>\(\mathop m\limits^ \bullet  HeatCoilON\)</span> = air mass flow rate through heat pump when the heating coil is ON (kg/s)
-
-<span>\(\mathop m\limits^ \bullet  CoilOFF\)</span> = air mass flow rate through heat pump when no heating or cooling is needed (kg/s)
-
-In this case, the air conditions at nodes downstream of the heating coils are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coils are operating and inlet air conditions when the coils are OFF).
-
-#### High Humidity Control with AirToAir HeatPump Model
-
-The specific configuration of the AirToAir HeatPump with supplemental heating coil is shown above (see Figure 227). This figure shows the fan placement when a blow through fan is specified. If a draw through fan is specified, the fan is located between the heating coil and the supplemental heating coil. The system is controlled to keep the high relative humidity in the control zone from exceeding the setpoint specified in the object ZoneControl:Humidistat. This option is available when the supply air fan operates continuously (i.e., the supply air fan operating mode schedule values are never equal to 0) or the supply air fan cycles with the compressor. In addition, when high humidity control is specified and the compressor operates, the heatpump operates at the cooling air flow rate when a zone heating load is present as determined by the zone thermostat. High humidity control is specified as either None, MultiMode, or CoolReheat in the Dehumidification Control Type input field. MultiMode is specified when a heat exchanger is used to improve the dehumidification performance of the cooling coil. The heat exchanger will be activated when the sensible part-load ratio is insufficient to meet the zone latent load. CoolReheat is specified when a DX cooling coil is used to over-cool the supply air stream in order to meet the zone latent load. In this case, a supplemental heating coil will ensure the zone temperature does not fall below the zone heating temperature set point. When a heat exchanger is used in conjunction with a DX cooling coil and CoolReheat is specified as the Dehumidification Control Type, the heat exchanger is “locked on� to meet either the sensible or latent cooling load. If the dehumidification control type is selected as None and a heat exchanger assisted cooling coil is used, the heat exchanger is “locked on� and the air conditioner runs only to meet the sensible cooling load. A supplemental heating coil is required for all dehumidification control types.
-
-The model first calculates the *PartLoadRatio* required meeting the sensible cooling load.  The heatpump’s sensible cooling load is determined from the control zone sensible cooling load to the cooling setpoint and the control zone air flow fraction to maintain the dry-bulb temperature setpoint in the control zone.:
-
-<div>$$HeatPumpCoolingLoad = \,\frac{{ControlZoneCoolingLoad}}{{ControlZoneAirFlowFraction}}$$</div>
-
-The heatpump’s sensible cooling load to be met and the full load cooling output are used to calculate the sensible the part-load ratio iteratively based on user specified convergence criterion.
-
-<div>$$PartLoadRatio = MAX\left( {0.0,\,\frac{{ABS\left( {HeatPumpCoolingLoad - NoCoolOutput} \right)}}{{ABS\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)$$</div>
-
-When the heat pump’s sensible cooling capacity meets the system sensible cooling load at a given sensible part load ratio, then the Heat pump meets the controlled zone cooling setpoint temperature. If a moisture (latent) load exists because the control zone humidity has exceeded the setpoint, the total moisture load to be met by the heat pumps (HeatPumpMoistureLoad) is calculated based on the control zone moisture load and the control zone air flow fraction.
-
-<div>$$HeatPumpMoistureLoad = \,\frac{{ControlZoneMoitureLoad}}{{ControlZoneAirFlowFraction}}$$</div>
-
-Then the *LatentPartLoadRatio* required to meet the high humidity setpoint is calculated as follows:
-
-<div>$$LatentPartLoadRatio = MIN\left( {PL{R_{Min}},\,\frac{{ABS\left( {HeatPumpMoistureLoad - NoLatentOutput} \right)}}{{ABS\left( {FullLatentOutput - NoLatentOutput} \right)}}} \right)$$</div>
-
-The model uses the greater of the two part-load ratios, *PartLoadRatio* or *LatentPartLoadRatio*, to determine the operating part-load ratio of the Heat Pump’s DX cooling coil.
-
-<div>$$LatentPartLoadRatio = MAX\left( {PartLoadRatio,\,LatentPartLoadRatio} \right)$$</div>
-
-As previously described, iterations are performed to converge on the solution within the convergence tolerance.
-
-Where,
-
-<span>\(ControlZoneCoolingLoad\)</span>= the control zone sensible cooling load to the cooling setpoint, (W).
-
-<span>\(ControlZoneMoistureLoad\)</span>         = the control zone moisture load to the dehumidifying relative humidity setpoint, (W).
-
-<span>\(ControlZoneAirFlowFraction\)</span>     = the supply air fraction that goes though the control zone, (-).
-
-*FullLatentOutput*      =         the Heat Pump’s latent cooling energy rate at full-load conditions, W
-
-*NoLatentOutput*       =          the Heat Pump’s latent cooling energy rate with cooling coil OFF, W
-
-<span>\(PartLoadRatio\)</span>     =          the heat pump’s part-load-ratio required to meet system sensible load, (-).
-
-<span>\(LatentPartLoadRatio\)</span>      =          the heat pump’s part-load-ratio required to meet system moisture load, (-).
-
-<span>\(PL{R_{MIN}}\)</span>*       =  *the minimum part-load ratio, which is usually 0.0. For the case when the latent capacity degradation model is used (Ref: DX Cooling Coil Model), this value is the minimum part-load ratio at which the cooling coil will dehumidify the air.
-
-When the predicted zone air temperature is above the heating setpoint and if there is a dehumidification load, the supplemental heating coil load is required to offset the excess cooling as shown in Figure 228. If the model determines that the LatentPartLoadRatio is to be used as the operating part-load ratio of the heatpump’s cooling coil, the supplemental heating coil is used to offset the excess sensible capacity provided by the heat pump DX cooling coil. The model first checks the sensible load that exists for the current simulation time step (predicted zone temperature with no HVAC operation compared to the thermostat setpoint temperatures). If a sensible cooling load or no sensible cooling or heating load exists (see Figure 2),  the model calculates the difference between the sensible heating load required to reach or maintain the heating dry-bulb temperature setpoint and the actual sensible cooling energy rate delivered by the unit (with LatentPartLoadRatio). In this case, thesupplemental heating coil is used to offset the excess sensible cooling energy provided by the DX cooling coil (if any) that could have caused an overshoot of the heating dry-bulb temperature setpoint. Note that when a humidistat is used and high humidity control is required, the zone dry-bulb temperature will typically move toward the heating temperature setpoint when a high moisture (latent) load exists.
-
-![HiHumidControl](media/image5145.png)
-
-Figure 228. Supplemental heating coil load when predicted zone air temperature is above the heating Setpoint
-
-If a heating load exists (Figure 229), the supplementalheating coil is used to meet the heating coil load and at the same time offset the entire sensible cooling energy rate of the DX cooling coil (to meet the humidistat setpoint). Note that when a heating load exists and high humidity control is required, the heat pump operates at the user-specified cooling air flow rate for the entire simulation time step. As with the fan, and DX cooling coil, report variables associated with supplemental heating coil performance (e.g., heating coil energy, heating coil rate, heating coil gas or electric energy, heating coil runtime fraction, etc.) are managed in the supplemental (heating) coil object.
-
-![HiHumidControl-1](media/image5146.png)
-
-Figure 229. Supplemental heating coil load when predicted zone air temperature is below the heating setpoint
-
-### Unitary Multi-Speed Air-To-Air Heat Pump
-
-#### Overview
-
-The input object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed provides a model for a multispeed air-to-air heat pump that is a “virtual� component that consists of an on/off or constant volume fan component, a multispeed DX cooling coil, a multispeed DX heating coil, and a gas or electric supplemental heating coil. The main difference between this heat pump object and other EnergyPlus heat pump objects is that this object allows from two to four discrete compressor speeds for heating and cooling operation (instead of a single speed for each mode). The specific configuration of the blow through heat pump is shown in the following figure. For a draw through heat pump, the fan is located between the DX heating coil and the supplemental heating coil.
-
-![FurnaceSchematic\_BlowThru\_Multispeed](media/image5147.png)
-
-Figure 230. Schematic of a Multispeed Air-to-Air Heat Pump (Blow-through Configuration)
-
-While the heat pump may be configured to serve multiple zones, system operation is controlled by a thermostat located in a single “control� zone. One of the key parameters for the heat pump component is the fraction of the total system airflow that goes through the control zone. This fraction is calculated as the ratio of the maximum air mass flow rate for the air loop’s supply inlet node for the control zone (e.g., AirTerminal:SingleDuct:Uncontrolled, field = Maximum Air Flow Rate, converted to mass flow) to the sum of the maximum air mass flow rates for the air loop’s supply inlet nodes for all zones served by this air loop. The heat pump module scales the calculated load for the control zone upward based on this fraction to determine the total load to be met by the heat pump. The module then proceeds to calculate the required cycling ratio, speed ratio and speed number for the system coil and determines the supply air mass flow rate to meet this total load based on the speed number. The cycling ratio is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the multispeed heat pump’s DX heating or cooling coil at Speed 1 for the entire system time step. It is equivalent to the part load ratio for a single speed DX coil. The value is between 0.0 and 1.0 when the system operates at its lowest speed (Speed 1) and 1.0 when the multispeed heat pump operates at speeds above 1. The speed ratio is the ratio of time in a system time step that the compressor is at rated speed between two consecutive speed numbers ([Compressor Speed - Compressor speed at Speed i-1] / [Compressor speed at Speed i - Compressor speed at Speed i-1]). The compressor speed ratio is between 0.0 and 1.0 when the speed number is above 1 and is 0.0 during Speed 1 operation. The speed number is the lowest index number whose corresponding full-load sensible capacity at the given air mass flow rate is greater than or equal to the sensible load (heating or cooling) in a system time step. The heating or cooling capacity delivered by the heat pump is distributed to all of the zones served by this system via the direct air units that supply air to each zone.
-
-The heat pump component is able to model supply air fan operation in two modes: cycling fan – cycling coil (i.e., AUTO fan) and continuous fan – cycling coil (i.e., fan ON). Fan:OnOff must be used to model AUTO fan, while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON. The fan operation mode is specified using a supply air fan operating mode schedule where schedule values of 0 denote cycling fan operation and schedule values other than 0 (a 1 is usually used) denote continuous fan operation. Using this schedule, the supply air fan may be cycled with cooling or heating coil operation or operated continuously based on time of day (e.g. cycling fan operation at night and continuous fan operation during the day).
-
-Several output variables are reported by the heat pump object including fan part-load ratio, compressor part-load ratio, cycling ratio, speed ratio and speed number. Fan part-load ratio is defined as the actual air mass flow rate through the system for the time step divided by the operating supply air mass flow rate specified for the heat pump (<span>\({{{{\dot m}_{actual}}} \mathord{\left/ {\vphantom {{{{\dot m}_{actual}}} {{{\dot m}_{design}}}}} \right. } {{{\dot m}_{ON}}}}\)</span>) at speed 1. Fan part-load ratio is set to 1.0 when the heat pump operates at speeds above 1. The operating supply air mass flow rate may be different for cooling, heating, and when no cooling or heating is required. Compressor part-load ratio is the actual load for the time step divided by the full-load sensible capacity (see Eqn. or Eqn.). If the defrost strategy is reverse cycle for a DX heating coil, the compressor part-load ratio is the sum of the actual load and the defrost load divided by the full-load sensible capacity. Therefore, the compressor part load ratio for the DX heating coil may be greater than the cycling ratio. This heat pump object also reports the sensible, latent and total cooling and heating rate, as well as the electricity consumption for the unit with separate accounting of auxiliary electric consumption. Furthermore, five report variables related to waste heat recovery are available if the user chooses to model this option.
-
-#### Model Description
-
-As described previously, the heat pump is a “virtual� component consisting of a fan, multispeed DX cooling coil, multispeed DX heating coil and supplemental heating coil. The sole purpose of the heat pump model is to properly coordinate the operation of the various system components. The following sections describe the flow of information within the model, as well as the differences between cycling and continuous supply air fan operation.
-
-#### Cooling Operation
-
-The description of heat pump cooling operation is divided in two sections: sensible capacity and average supply air flow rate. Actually, the determinations of capacity and supply air flow rate are related, so these calculations are performed in unison.
-
-##### Capacity calculation
-
-If EnergyPlus determines that the heat pump must supply cooling to the control zone to meet the zone air temperature setpoint, then the heat pump model computes the total sensible cooling load (negative) to be delivered to the zones being served based on the control zone sensible cooling load and the fraction of the heat pump air flow that goes through the control zone.
-
-<div>$$Heat\;Pump\;Cooling\;Load = \frac{{Control\;Zone\;Cooling\;Load}}{{Control\;Zone\;Air\;Flow\;Fraction}}$$</div>
-
-The model then calculates the heat pump’s sensible cooling energy rate delivered to the zones being served when the system runs at full-load conditions at the highest speed and when the DX cooling coil is OFF. If the supply air fan cycles with the compressor, then the sensible cooling energy rate is zero when the cooling coil is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible cooling energy rate will not be zero when the cooling coil is OFF. Calculating the sensible cooling energy rate involves modeling the supply air fan (and associated fan heat) and the multispeed DX cooling coil. The multispeed DX heating coil and the supplemental heating coil are also modeled, but only to pass the air properties and mass flow rate from their inlet nodes to their outlet nodes. For each of these cases (full load at highest cooling speed and DX cooling coil OFF), the sensible cooling energy rate delivered by the heat pump is calculated as follows:
-
-<span>\(FullCoolOutpu{t_{Highest\;Speed}} = \left( {{{\dot m}_{HighestSpeed}}} \right){\left( {{h_{out,full\;load}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,HighestSpeed}}\)</span><span>\(NoCoolOutput = \left( {{{\dot m}_{CoilOff}}} \right){\left( {{h_{out,coil\;off}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,coil\;off}}\)</span>
-
-where:
-
-*<span>\({\dot m}_{HighestSpeed}\)</span>* = air mass flow rate through heat pump at the highest cooling speed [kg/s]
-
-*h<sub>out,\\ full\\ load</sub>*   = enthalpy of air exiting the heat pump at full-load conditions [J/kg]
-
-*h<sub>control \\ zone</sub>*   = enthalpy of air leaving the control zone (where thermostat is located) [J/kg]
-
-*HR<sub>min</sub>=* the minimum humidity ratio of the heat pump exiting air or the air leaving the control zone [kg/kg]
-
-<span>\({\dot m}_{CoilOff}\)</span> = air mass flow rate through the heat pump with the cooling coil OFF [kg/s]
-
-*h<sub>out,coil \\ off</sub>*    = enthalpy of air exiting the heat pump with the cooling coil OFF [J/kg]
-
-Δ<sub>sen,</sub> *<sub>full\\ load</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions
-
-<div>$${\Delta_{sen,HighestSpeed}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} + \left( {{{\dot m}_{HighestSpeed}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {h_{Out,full\;load} - {h_{Control\;Zone}}} \right)_{HR\min }}$$</div>
-
-where:
-
-Frac = Control zone air fraction with respect to the system mass flow rate
-
-Δ<sub>sen,coil\\ off</sub>**=Sensible load difference between the system output node and the zone inlet node with the cooling coil OFF conditions
-
-<div>$${\Delta_{sen,coil\;off}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} + \left( {{{\dot m}_{coil\;off}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {{h_{Out,coil\;off}} - {h_{Control\;Zone}}} \right)_{HR\min }}$$</div>
-
-
-
-If the heat pump’s sensible cooling rate at the highest speed (full load, no cycling) is insufficient to meet the entire cooling load, the controlled zone conditions will not be met. The reported cycling rate and speed ratio are 1, and the speed number is set to the highest index number. If the total sensible cooling load to be met by the system is less than the sensible cooling rate at the highest speed, then the following steps are performed.
-
-·        Calculate the sensible cooling energy rate at Speed 1
-
-<div>$$FullCoolOutpu{t_{Speed1}} = \left( {{{\dot m}_{Speed1}}} \right){\left( {{h_{out,fullload}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,Speed1}}$$</div>
-
-where
-
-*<span>\({{{\dot m}_{Speed1}}}\)</span>* = air mass flow rate through heat pump at Speed 1 [kg/s]
-
-Δ<sub>sen,</sub> <sub>Speed1</sub>**=Sensible load difference between the system output node and the zone inlet node at full-load conditions at Speed 1
-
-<div>$${\Delta_{sen,Speed1}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} + \left( {{{\dot m}_{Speed1}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {{h_{Out,full\;load}} - {h_{Control\;Zone}}} \right)_{HR\min }}$$</div>
-
-·        If the sensible cooling energy rate delivered by the heat pump at Speed 1 is greater or equal to the sensible load, the cycling ratio (part-load ratio) for the heat pump is estimated.
-
-<div>$$\begin{array}{l}CyclingRatio = \frac{{ABS(HeatingCoilSensibleLoad)}}{{FullHeatingCoilCapacity}}\\\;\;\;\;\;\;\;\; = MAX\left( {0.0,\frac{{ABS(Heat\;Pump\;Heating\;Load - AddedFanHeat)}}{{ABS(FullHeatOutpu{t_{Speed1}} - AddedFanHea{t_{Speed1}})}}} \right)\end{array}$$</div>
-
-where
-
-AddedFanHeat  = generated supply air fan heat, which is a function of part load ratio and as internal component cooling load [W].
-
-AddedFanHeat<sub>Speed1</sub>        = generated supply air fan heat at Speed 1 (part load ratio=1) [W].
-
-Since the part-load performance of the DX cooling coil is frequently non-linear,and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the heat pump’s cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump’s cooling output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge \frac{{\left( {Heat\,Pump\,Cooling\,Load - HeatPumpOutpu{t_{Cycling}}} \right)}}{{Heat\,Pump\,Cooling\,Load}}$$</div>
-
-where:
-
-HeatPumpOutput<sub>Cycling</sub> = heat pump delivered sensible capacity for Speed 1 operating at a specific cycling ratio (W)
-
-<div>$$HeatPumpOutpu{t_{cycling}} = {\dot m_{_{HeatPump}}}{\left( {{h_{out}} - {h_{Control\;Zone}}} \right)_{HR\min }} - {\Delta_{cycling}}$$</div>
-
-where
-
-<span>\({\dot m_{HeatPump}}\)</span>          = average air mass flow rate defined in the next section [kg/s]
-
-h<sub>out,</sub>        = enthalpy of air exiting the heat pump at part load conditions [J/kg]
-
-Δ<sub>cycling</sub>    =average sensible load difference between the system output node and the zone inlet node
-
-<div>$$\begin{array}{l}\;{\Delta_{cycling}} = \frac{{{{\dot m}_{_{ZoneInlet}}}}}{{frac}}\left( {{h_{ZoneInlet}} - {h_{Control\;Zone}}} \right) + \left( {{{\dot m}_{_{HeatPump}}} - \frac{{{{\dot m}_{_{ZoneInlet}}}}}{{frac}}} \right)\left( {{h_{Out}} - {h_{Control\;Zone}}} \right)\\\;\end{array}$$</div>
-
-<span>\({{{\dot m}_{ZoneInlet}}}\)</span> = Air mass flow rate in the supply inlet node in the controlled zone [kg/s]
-
-For this case where speed 1 operation was able to meet the required cooling load, the speed ratio is set to zero and speed number is equal to 1.
-
-·        If the heat pump’s cooling output at full load for Speed 1 is insufficient to meet the entire cooling load, the Cycling ratio is set equal to 1.0 (compressor and fan are not cycling). Then the cooling speed is increased and the delivered sensible capacity is calculated. If the full load sensible capacity at Speed n is greater than or equal to the sensible load, the speed ratio for the heat pump is estimated:
-
-<span>\(Speed{\kern 1pt} Ratio = \frac{{ABS(Heat{\kern 1pt} Pump{\kern 1pt} Cooling{\kern 1pt} Load - AddeFanHeat - Full{\kern 1pt} Cool{\kern 1pt} Outpu{t_{Speed{\kern 1pt} n - 1}})}}{{ABS(Full{\kern 1pt} CoolOutpu{t_{Speed{\kern 1pt} n}} - Full{\kern 1pt} CoolOutpu{t_{Speed{\kern 1pt} n - 1}})}}\)</span>Although a linear relationship is assumed by applying the speed ratio to obtain the effective capacity and mass flow rate between speed n and n-1, the outlet air node conditions are dependent on the combined outputs and may not be linear. In addition, the supply air fan heat varies with the speed ratio due to different supply mass flow rates between speed n and n-1 . Therefore, the final speed ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the cooling coil and fan) until the heat pump’s cooling output matches the cooling load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump’s cooling output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge \frac{{Heat\,Pump\,Cooling\,Load - HeatPumpOutpu{t_{SpeedRatio}}}}{{Heat\,Pump\,Cooling\,Load}}$$</div>
-
-where:
-
-HeatPumpOutput<sub>Speed,n</sub>= heat pump delivered sensible capacity between two consecutive speeds at a specific speed ratio (W)
-
-       <span>\(\begin{array}{l}HeatPumpOutpu{t_{SpeedRatio}} = (SpeedRatio)FullCoolOutpu{t_{Speed\;n}}\\\;\;\;\;\;\;\; = (1 - SpeedRatio)FullCoolOutpu{t_{Speed\;n - 1}} - AddedFanHea{t_{SpeedRatio}}\end{array}\)</span>
-
-Where
-
-AddedFanHeat<sub>SpeedRatio</sub>          = generated supply air fan heat at a specific speed ratio [W]
-
-In this case, the reported cycling ratio is 1 and speed number is equal to n.
-
-
-
-
-
-##### Air Mass Flow Rate Calculation
-
-Speed 1 operation
-
-If the heat pump has been specified with cycling fan/cycling coil (AUTO fan), then the heat pump’s operating supply air mass flow rate is determined by the cycling ratio (PartLoadRatio) for Speed 1. The supply air mass flow rate is multiplied by the cycling ratio to determine the average air mass flow rate for the system simulation time step. The air conditions at nodes downstream of the cooling coils represent the full-load (steady-state) values when the coil is operating.
-
-<div>$${\dot m_{HeatPump}} = (CyclingRatio){\dot m_{Speed1}}$$</div>
-
-If the fan operates continuously (i.e., when the supply air fan operating mode schedule values are NOT equal to 0), the operating air mass flow rate through the heat pump is calculated as the average of the user-specified air flow rate when the heat pump cooling coil is ON at Speed 1 and the user-specified air flow rate when the heat pump cooling coil is OFF (user-specified supply air volumetric flow rates converted to dry air mass flow rates).
-
-<div>$${\dot m_{HeatPump}} = (CyclingRatio){\dot m_{Speed1}} + (1.0 - CyclingRatio){\dot m_{CoilOff}}$$</div>
-
-where:
-
-<span>\({\dot m_{HeatPump}}\)</span> = average air mass flow rate through heat pump [kg/s]
-
-<span>\({{{\dot m}_{Speed1}}}\)</span>= air mass flow rate through heat pump when cooling coil is ON at Speed 1 [kg/s]
-
-<span>\({{{\dot m}_{CoilOff}}}\)</span> = air mass flow rate through heat pump when no heating or cooling is needed [kg/s]
-
-In this case, the air conditions at nodes downstream of the cooling coils are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and inlet air conditions when the coil is OFF).
-
-##### Higher Speed Operation
-
-When the heat pump operates at higher speeds to meet the required cooling load, the supply air mass flow rate is linearly interpolated between two consecutive speeds:
-
-<div>$${\mathop m\limits^ \bullet_{HeatPump}} = (SpeedRatio)\mathop m\limits^ \bullet  {{\kern 1pt}_{Speed{\kern 1pt} n}} + (1.0 - SpeedRatio)\mathop m\limits^ \bullet  {{\kern 1pt}_{Speed{\kern 1pt} n - 1}}$$</div>
-
-where:
-
-<span>\({\dot m_{HeatPump}}\)</span>= average air mass flow rate through the heat pump for the time step [kg/s]
-
-<span>\({\dot m_{Speed\;n}}\)</span>= air mass flow rate through heat pump when cooling coil is ON at Speed n [kg/s]
-
-<span>\({\dot m_{Speed\;n - 1}}\)</span>= air mass flow rate through heat pump when cooling coil is ON at Speed n-1 [kg/s]
-
-For this case of higher speed operation, the air conditions at nodes downstream of the cooling coils are determined by the delivered cooling capacity and supply air mass flow rates between two consecutive speeds.
-
-Although the above sections present the capacity and air mass flow rate calculation separately, they are dependent and change every iteration until convergence is reached for the time step being simulated.
-
-#### Heating Operation
-
-The description of heat pump heating operation is divided in two sections: total (sensible) capacity and average supply air flow rate. Actually, the determinations of capacity and supply air flow rate are related, so these calculation are performed in unison.
-
-##### Capacity calculation
-
-If EnergyPlus determines that the heat pump must supply heating to the control zone to meet the zone air temperature setpoint, then the heat pump model computes the total sensible heating load (positive) to be delivered to the zones being served based on the control zone sensible heating load and the fraction of the heat pump air flow that goes through the control zone.
-
-<div>$$Heat\;Pump\;Heating\,Load = \frac{{Control\;Zone\;Heating\,Load}}{{Control\;Zone\;Air\;Flow\;Fraction}}$$</div>
-
-The model then calculates the heat pump’s sensible heating energy rate delivered to the zones being served when the system runs at full-load conditions at the highest speed and when the DX heating coil is OFF (without supplemental heater operation in either case). If the supply air fan cycles with the compressor, then the sensible heating energy rate is zero when the compressor is OFF. However if the fan is scheduled to run continuously regardless of coil operation, then the sensible heating energy rate will not be zero when the compressor is OFF. Calculating the sensible heating energy rate involves modeling the supply air fan (and associated fan heat), the DX cooling coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node), the DX heating coil, and the supplemental heating coil (simply to pass the air properties and mass flow rate from its inlet node to its outlet node). For each of these cases (full load and DX heating coil OFF, without supplemental heater operation in either case), the sensible heating energy rate delivered by the heat pump is calculated as follows:
-
-<div>$$FullHeatOutpu{t_{Highest\;Speed}} = \left( {{{\dot m}_{HighestSpeed}}} \right){\left( {{h_{out,full\;load}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,HighestSpeed}}$$</div>
-
-<div>$$NoHeatOutput = \left( {{{\dot m}_{CoilOff}}} \right){\left( {{h_{out,coil\;off}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,coil\;off}}$$</div>
-
-where:
-
-*<span>\({\dot m}_{HighestSpeed}\)</span>* = air mass flow rate through heat pump at the highest heating speed [kg/s]
-
-*h<sub>out,\\ full\\ load</sub>*   = enthalpy of air exiting the heat pump at full-load conditions [J/kg]
-
-*h<sub>control \\ zone</sub>*   = enthalpy of air leaving the control zone (where thermostat is located) [J/kg]
-
-*HR<sub>min</sub>=* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the heat pump exiting air or the air leaving the control zone
-
-<span>\({\dot m}_{CoilOff}\)</span>= air mass flow rate through the heat pump with the heating coil OFF [kg/s]
-
-*h<sub>out,coil \\ off</sub>*    = enthalpy of air exiting the heat pump with the heating coil OFF [J/kg]
-
-Δ<sub>sen,</sub> *<sub>full\\ load</sub>*=Sensible load difference between the system output node and the zone inlet node at full-load conditions
-
-<div>$${\Delta_{sen,HighestSpeed}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} + \left( {{{\dot m}_{HighestSpeed}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {h_{Out,full\;load} - {h_{Control\;Zone}}} \right)_{HR\min }}$$</div>
-
-where:
-
-Frac = Control zone air fraction with respect to the system mass flow rate
-
-Δ<sub>sen,coil\\ off</sub>**=Sensible load difference between the system output node and the zone inlet node with the heating coil OFF conditions
-
-<div>$${\Delta_{sen,coil\;off}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,coil\;off}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} + \left( {{{\dot m}_{coil\;off}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {{h_{Out,coil\;off}} - {h_{Control\;Zone}}} \right)_{HR\min }}$$</div>
-
-If the heat pump’s DX heating coil output full load at the highest speed is insufficient to meet the entire heating load, the remaining heating load is passed to the supplemental heating coil. If the heat pump model determines that the outdoor air temperature is below the minimum outdoor air temperature for compressor operation (specified by the user), the compressor is turned off and the entire heating load is passed to the supplemental gas or electric heating coil. The heat pump exiting air conditions and energy consumption are calculated and reported by the individual component models (fan, DX heating coil, and supplemental gas or electric heating coil).
-
-If the total heating load to be met by the system is less than the sensible heating rate at the highest speed, then the following steps are performed.
-
-1.    Calculate the sensible heating energy rate at Speed 1
-
-<div>$$FullHeatOutpu{t_{Speed1}} = \left( {{{\dot m}_{Speed1}}} \right){\left( {{h_{out,fullload}} - {h_{control\;zone}}} \right)_{HR\min }} - {\Delta_{sen,Speed1}}$$</div>
-
-where:
-
-*<span>\({{{\dot m}_{Speed1}}}\)</span>* = air mass flow rate through heat pump at Speed 1 [kg/s]
-
-Δ<sub>sen,</sub> <sub>Speed1</sub>**=Sensible load difference between the system output node and the zone inlet node at full-load conditions at Speed 1
-
-<div>$${\Delta_{sen,Speed1}} = \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}{\left( {{h_{Out,full\;load}} - {h_{Zone\;Inlet}}} \right)_{HR\min }} + \left( {{{\dot m}_{Speed1}} - \frac{{{{\dot m}_{Zone\;Inlet}}}}{{Frac}}} \right){\left( {{h_{Out,full\;load}} - {h_{Control\;Zone}}} \right)_{HR\min }}$$</div>
-
-2.    If the sensible heating energy rate delivered by the heat pump at Speed 1 is greater or equal to the sensible load, the cycling ratio (part-load ratio) for the heat pump is estimated.
-
-<div>$$\begin{array}{l}CyclingRatio = \frac{{ABS(HeatingCoilSensibleLoad)}}{{FullHeatingCoilCapacity}}\\\;\;\;\;\;\;\; = MAX\left( {0.0,\frac{{ABS(Heat\;Pump\;Heating\;Load - AddedFanHeat)}}{{ABS(FullHeatOutpu{t_{Speed1}} - AddedFanHea{t_{Speed1}})}}} \right)\end{array}$$</div>
-
-where
-
-AddedFanHeat        = generated supply air fan heat, which is a function of part load ratio and as internal component heating load [W].
-
-AddedFanHeat<sub>Speed1</sub>  = generated supply air fan heat at Speed 1 (part load ratio=1) [W].
-
-Since the part-load performance of the DX heating coil is frequently non-linear (Ref: Single-Speed Electric Heat Pump DX Air Heating Coil), and the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan), the final part-load ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the heat pump’s heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump’s heating output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge \frac{{Heat\,Pump\,Heating\,Load - HeatPumpOutpu{t_{Cycling}}}}{{Heat\,Pump\,Heating\,Load}}$$</div>
-
-where:
-
-HeatPumpOutput<sub>Cycling</sub>= heat pump delivered sensible capacity for Speed 1 operating at a specific cycling ratio (W)
-
-<div>$$HeatPumpOutpu{t_{cycling}} = {\dot m_{_{HeatPump}}}{\left( {{h_{out}} - {h_{Control\;Zone}}} \right)_{HR\min }} - {\Delta_{cycling}}$$</div>
-
-where
-
-<span>\({\dot m_{HeatPump}}\)</span>    = average air mass flow rate defined in the next section [kg/s]
-
-h<sub>out,</sub>              = enthalpy of air exiting the heat pump at part load conditions [J/kg]
-
-Δ<sub>cycling</sub>          =average sensible load difference between the system output node and the zone inlet node
-
-<div>$$\begin{array}{l}\;{\Delta_{cycling}} = \frac{{{{\dot m}_{_{ZoneInlet}}}}}{{frac}}\left( {{h_{ZoneInlet}} - {h_{Control\;Zone}}} \right) + \left( {{{\dot m}_{_{HeatPump}}} - \frac{{{{\dot m}_{_{ZoneInlet}}}}}{{frac}}} \right)\left( {{h_{Out}} - {h_{Control\;Zone}}} \right)\\\;\end{array}$$</div>
-
-<span>\({{{\dot m}_{ZoneInlet}}}\)</span>       = Air mass flow rate in the supply inlet node in the controlled zone [kg/s]
-
-For this case where speed 1 operation was able to meet the required heating load, the speed ratio is set to zero and speed number is equal to 1.
-
-3.    If the heat pump’s heating output at full load for Speed 1 is insufficient to meet the entire heatling load, the Cycling ratio (PartLoadRatio) is set equal to 1.0 (compressor and fan are not cycling). Then the heating speed is increased and the delivered sensible capacity is calculated. If the full load sensible capacity at Speed n is greater than or equal to the sensible load, the speed ratio for the heat pump is estimated:
-
-<div>$$Speed{\kern 1pt} Ratio = \frac{{ABS(Heat{\kern 1pt} Pump{\kern 1pt} Heating{\kern 1pt} Load - AddeFanHeat - Full{\kern 1pt} Heat{\kern 1pt} Outpu{t_{Speed{\kern 1pt} \;n - 1}})}}{{ABS(Full{\kern 1pt} HeatOutpu{t_{Speed\;n}} - Full{\kern 1pt} HeatOutpu{t_{Speed\;n - 1}})}}$$</div>
-
-Although a linear relationship is assumed by applying the speed ratio to obtain the effective capacity and air mass flow rate between speed n and n-1, the outlet node conditions are dependent on the combined outputs and may not be linear. In addition, the supply air fan heat varies based on heating coil operation for the case of cycling fan/cycling coil (AUTO fan). Therefore, the final speed ratio for the heating coil compressor and fan are determined through iterative calculations (successive modeling of the heating coil and fan) until the heat pump’s heating output matches the heating load to be met within the convergence tolerance. The convergence tolerance is fixed at 0.001 and is calculated based on the difference between the load to be met and the heat pump’s heating output divided by the load to be met.
-
-<div>$$Tolerance = 0.001 \ge \frac{{Heat\,Pump\,Heating\,Load - HeatPumpOutpu{t_{SpeedRatio}}}}{{Heat\,Pump\,Heating\,Load}}$$</div>
-
-where:
-
-HeatPumpOutput<sub>SpeedRatio</sub>= heat pump delivered sensible capacity between two consecutive speeds at a specific ratio [W]
-
-       <span>\(\begin{array}{l}HeatPumpOutpu{t_{SpeedRatio}} = (SpeedRatio)FullHeatOutpu{t_{Speed\;n}}\\\;\;\;\;\;\;\; = (1 - SpeedRatio)FullHeatOutpu{t_{Speed\;n - 1}} - AddedFanHea{t_{SpeedRatio}}\end{array}\)</span>
-
-Where
-
-AddedFanHeat<sub>SpeedRatio</sub>          = generated supply air fan heat at a specific speed ratio [W]
-
-In this case, the reported cycling ratio is 1 and speed number is equal to n.
-
-##### Air Mass Flow Rate Calculation
-
-The air mass flow rate calculations during heating operation are the same as those described above for cooling operation.
-
-#### Fan Placement
-
-Supply air fan placement impacts the iteration strategy. When the fan placement type is blow through, the air mass flow rate and coil part load factor (PLF) affect the fan outlet conditions. Since the fan is upstream of the coil components with this fan placement, the fan outlet conditions are calculated without knowing the next component’s performance at the beginning of each iteration. DX coil performance is strongly dependent on the inlet conditions, so without correct inlet conditions the DX coil components may not be simulated correctly. Therefore, the heat pump components are called twice for each iteration when fan placement is ‘blow through’. The correct part load factor for the fan component is obtained after the first call, so that the more realistic fan outlet conditions are used to simulate the coil performance in the second call. This extra call to the heat pump components is not required for the draw through fan since the supply air fan is located downstream of the DX coils with this fan placement.
-
-#### Waste Heat Calculation
-
-When the heat recovery is active (the value of the Design Heat Recovery Water Flow Rate field is greater than 0), the outlet node temperature of heat recovery is calculated based on the recoverable waste heat generated by its child objects (Coil:Cooling:DX:MultiSpeed and Coil:Heating:DX:MultiSpeed):
-
-<div>$${T_{outlet}} = {T_{inlet}} + \frac{{{Q_{WasteHeat}}}}{{{C_p}{{\dot m}_{hr}}}}$$</div>
-
-where
-
-T<sub>outlet</sub>            = outlet node temperature of heat recovery, C
-
-T<sub>inlet</sub> = inlet node temperature of heat recovery, C
-
-Q<sub>WasteHeat</sub>      = recoverable waste heat generated by its child objects, W
-
-C<sub>p</sub>              = inlet node temperature of heat recovery, C
-
-<span>\({{{\dot m}_{hr}}}\)</span>            = mass flow rate of heat recovery, kg/s
-
-If the outlet node temperature is above the value of the Maximum Temp for Heat Recovery field, the outlet node temperature is reset to the value of Maximum Temp for Heat Recovery.
-
-### DX Cooling Package
-
-#### Overview
-
-The DX cooling package subsystem model provides a “virtual� component that consists of a DX air cooling coil component as shown in the figure below. The CoilSystem:Cooling:DX input object provides a container component that controls the associated DX cooling coil which is specified in a separate object. This coil can be specified anywhere in the air loop simulation and is controlled by the setpoint(s) on the control node. Optional dehumidification controls may also be specified. CoilSystem:Cooling:DX assumes continuous fan operation for any given time step, because it is not able to control cycling fan operation in the way that other AirLoopHVAC:Unitary\* systems can.
-
-This system does not need any plant specification and will provide the electric consumption necessary to operate the compressor and the condenser fan.
-
-![](media/image5198.png)
-
-Figure 231.  Schematic of Packaged DX Cooling Subsystem in Air Loop for a Blow-Thru Application
-
-#### Controls
-
-The system calculates the current sensible load using the temperature of the inlet node and the System Node Setpoint Temp on the control node. If the control node is not the outlet node, the desired outlet node temperature is adjusted for the current temperature difference between the outlet node and the control node. Likewise, the current latent load is calculated using the humidity ratio of the inlet node and the System Node Humidity Ratio Max on the control node. The controls determine the required coil run-time fraction and dehumidification mode (if applicable) using the steps outlined below.
-
-##### Step 1 – Meet Sensible Load Requirement
-
-The controls first attempt to meet the sensible requirement. The specified DX coil model is called with a part-load ratio (PLR) of 1.0 to determine the full-load output of the coil. This is compared with the desired outlet node temperature and a sensible PLR is calculated. If the PLR is &lt;1.0, a Regula-Falsi iteration routine is called to determine the coil run-time fraction which results in the desired outlet node temperature. For a variable-speed DX cooling coil, if the load is smaller than the sensible capacity at the lowest speed, the coil run-time fraction is determined in the same way as a single-speed DX cooling coil. Otherwise, its speed level and speed ratio between two neighboring speeds are selected to match the load.
-
-If the cooling coil type is specified as CoilSystem:Cooling:DX:CoolingHeatExchanganerAssisted and the dehumidification control type is specified as CoolReheat, the heat exchanger is active during this attempt to meet the sensible requirement.
-
-##### Step 2 – Meet Latent Load Requirement (if activated)
-
-If dehumidification controls are active, the leaving humidity ratio resulting from operation to meet the sensible load (Step 1 above) is compared with the desired outlet node humidity ratio. If the humidity requirement is already met, then no further control action is taken. If the humidity requirement has not been met, then the coil is re-simulated depending on the type of humidity control.
-
-##### Step 2a – Humidity Control = MultiMode
-
-If the humidity control type is MultiMode, then the coil's enhanced dehumidification mode is activated when the coil type is Coil:Cooling:DX:TwoStageWithHumidityControlMode or the heat exchanger is activated when the coil type is CoilSystem:Cooling:DX:CoolingHeatExchangerAssisted and Step 1 above is repeated to meet the sensible load using the coil performance resulting from the enhanced dehumidificaiton mode. This is a semi-passive approach to dehumidification which may fall short or may exceed the dehumidification requirement. If the user has specified Run on Latent Load = Yes in the CoilSystem:Cooling:DX object, and there is no sensible load to be met, then the system will try to meet the entire dehumidification load. If dehumidification mode should not be active when there is no sensible load, then choose Run on Latent Load = No.
-
-##### Step 2b – Humidity Control = CoolReheat
-
-If the humidity control type is CoolReheat, the coil is re-simulated to achieve the desired outlet node humidity ratio. This option is valid for all cooling coil types. When the coil type is Coil:Cooling:DX:TwoStageWithHumidityControlMode, only the cooling performance mode is used for this step and enhanced dehumidification mode is not activated.
-
-### DX Heating Package
-
-#### Overview
-
-The DX heating package subsystem model provides a “virtual� component that consists of a DX air-to-air heating coil component and associated controls. The CoilSystem:Heating:DX input object provides a container component that controls the associated DX heating coil  which is specified in a separate object. See the entry called Single-Speed and Variable-Speed Electric Heat Pump DX Air Heating Coil for details of the coil model itself.  This coil can be specified anywhere in the air loop simulation and is controlled by the setpoint on the heating coil’s outlet node. This model is analogous to the model for CoilSystem:Cooling:DX which is similar but for cooling.  The model assumes continuous fan operation for any given time step, because it is not able to control cycling fan operation in the way that other AirLoopHVAC:Unitary\* systems can.
-
-This system does not need any plant specification and will provide the electric consumption necessary to operate the compressor and the condenser fan.
-
-#### Controls
-
-The DX heating package system calculates how the coil should operate to meet current sensible load using the temperature of the inlet node and the System Node Setpoint Temp on the outlet node. The controls determine the required coil run-time fraction to meet the sensible requirement. The Single-Speed Electric Heat Pump DX Air Heating Coil model is called with a part-load ratio (PLR) of 1.0 to determine the full-load output of the coil. If the PLR is &lt;1.0, a Regula-Falsi iteration routine is called to determine the coil run-time fraction which results in the desired outlet node temperature. For a variable-speed DX heating coil, if the load is smaller than the heating capacity at the lowest speed, the coil run-time fraction is determined in the same way as a single-speed DX heating coil. Otherwise, its speed level and speed ratio between two neighboring speeds are selected to match the load.
-
-### Desiccant Dehumidifier Package
-
-#### Overview
-
-The input object Dehumidifier:Desiccant:System provides a model that packages components for a desiccant-based subsystem that dehumidifies an air stream, normally called the process air stream. A second heated air stream, called the regeneration air stream, is used to remove the collected moisture from the desiccant heat exchanger and this moisture-laden air is then usually exhausted from the building. This Dehumidifier:Desiccant:System object is similar to the Dehumidifier:Desiccant:NoFans object but has some additional modeling capabilities.
-
-The Dehumidifier:Desiccant:System desiccant dehumidifier object in EnergyPlus is a compound object that can be placed anywhere in an air loop. Common locations for this object are in an AirLoopHVAC:OutdoorAirSystem or in the main air loop downstream of a cooling coil (postcooling desiccant dehumidifier). This compound object coordinates the operation of several ‘children’ objects: a desiccant heat exchanger, a regeneration air fan, and an optional regeneration air heater. If this dehumidifier is placed in the main air loop immediately downstream of a direct expansion (DX) cooling coil, then the dehumidifier’s operation can be coordinated with the operation of the companion DX coil and it is also possible to specify that the DX system’s condenser waste heat can be used to help regenerate the desiccant heat exchanger. For the case of condenser waste heat regeneration, an optional exhaust fan can also be modeled by this desiccant dehumidifier compound object to help maintain a setpoint temperature for air entering the regeneration side of the desiccant heat exchanger. Refer to the EnergyPlus Input Output Reference for the specific input syntax for this desiccant dehumidifier object.
-
-![DesiccantDehumidifier\_DrawThrough](media/image5199.png)
-
-Figure 232. Schematic of a Desiccant Dehumidifier with Draw Through Regeneration Fan Placement
-
-
-
-![DesiccantDehumidifier\_BlowThrough](media/image5200.png)
-
-Figure 233. Schematic of a Desiccant Dehumidifier in Blow Through Regeneration Fan Placement
-
-#### Control Logic
-
-The model first decides if the dehumidifier can operate for the simulation time step, based on its availability schedule and if there is air flow detected on the process air inlet node. If available to operate, then the target humidity ratio for the process outlet air is determined based on the maximum humidity ratio setpoint on the control node (System Node Setpoint Humidity Ratio Max). If the control node is not the process air outlet node, the target humidity ratio is adjusted for the current humidity ratio difference between the process air outlet node and the control node. If the humidity ratio of the process inlet air is greater than the target humidity ratio for the process outlet air, then the dehumidifier operates to meet the target to the extent possible.
-
-Once it is determined that the dehumidifier should operate, the components upstream of the desiccant heat exchanger’s regeneration inlet are modeled. The actual components that are modeled depend on the configuration specified by the user.
-
-If the waste heat from the companion cooling coil is being used to heat the regeneration air, then this model determines the temperature of the air leaving the cooling coil condenser. The user may also specify a setpoint temperature for the regeneration air entering the desiccant heat exchanger and an optional exhaust fan, which can impact the condenser leaving air temperature. For this case, the exhaust fan is used to control the condenser leaving air temperature by boosting the air flow rate through the condenser to meet the setpoint temperature (minus regeneration fan heat if blow through fan placement).
-
-Note: If the desiccant dehumidifier is OFF for a simulation time step but its companion cooling coil is operating and is specified to provide regeneration air heating, then the exhaust fan operates at the maximum air flow rate (i.e., this fan serves at the condenser fan for the companion cooling coil system when regeneration air heating is specified, so the inputs for the companion cooling coil object should not include the condenser fan energy since the condenser fan energy is modeled by the Dehumidifier:Desiccant:SystemDesiccant Dehumidifier object).
-
-The exhaust fan power is determined as follows:
-
-<div>$$\begin{array}{l}If\,dehumidifier\,is\,operating:\\\,\,\,PL{R_{exhaust}} = \,\frac{{{{\mathop m\limits^ \bullet  }_{exhaust}}}}{{\left( {{\rho_{Std}} * {{\mathop {\rm{V}}\limits^ \bullet  }_{exhaust,\,max}}} \right)}}\\\,\,\,{P_{exhaust}} = \,{P_{exhaust,\,max}} * \,ExhFanModFac\\\\If\,dehumidifier\,\,is\,\,not\,\,operating\,\,but\,\,companion\,\,coil\,\,is\,\,operating:\\\,\,\,{P_{exhaust}} = \,{P_{exhaust,\,max}} * \,PL{R_{companion\,coil}}\end{array}$$</div>
-
-where:
-
-<span>\(PL{R_{exhaust}}\)</span>  = part load ratio of the exhaust fan
-
-<span>\({\mathop {\rm{V}}\limits^ \bullet_{exhaust,\,max}}\)</span>  = exhaust fan maximum volumetric flow rate, user input (m<sup>3</sup>/s)
-
-<span>\({\rho_{Std}}\)</span>           = density of air at standard temperature and pressure [dry air at 20°C] (m<sup>3</sup>/kg)
-
-<span>\({P_{exhaust,\,max}}\)</span>   = exhaust fan maximum power, user input (W)
-
-<span>\(ExhFanModFac\)</span>= exhaust fan power modifier curve evaluated at PLR<sub>exhaust</sub>. If modifier                                        curve not provided by the user, then this factor is assumed to be 1.0.
-
-<span>\(PL{R_{companion\,coil}}\)</span>     = part load ratio of the companion cooling coil
-
-<span>\({P_{exhaust}}\)</span>        = output variable ‘Dehumidifier Exhaust Fan Electric Power, W’
-
-The exhaust fan electric consumption is then calculated as:
-
-<div>$${E_{exhaust}} = {P_{exhaust}}*\,\,TimeStepSys\,\,*\,\,3600.$$</div>
-
-where:
-
-<span>\({E_{exhaust}}\)</span>          = output variable ‘Dehumidifier Exhaust Fan Electric Energy, J’
-
-<span>\(TimeStepSys\)</span>= HVAC system simulation time step, hr
-
-Once the outlet conditions from the companion coil condenser are determined (if present), then the regeneration air fan (if blow through configuration) and regeneration air heater (if present) are simulated. To the extent possible (e.g., if the heater is available to operate based on its availability schedule and it has sufficient heating capacity), the regeneration air heater operates to raise its outlet air temperature to the specified regeneration inlet air setpoint temperature.
-
-With the inlet air conditions to the regeneration and process sides of the desiccant heat exchanger now known, the performance of the desiccant heat exchanger is modeled. If the desiccant dehumidifier is specified with a companion cooling coil upstream of the heat exchanger’s process inlet, then the model assumes that the dehumidifier operates at the same time as the companion coil (same part-load ratio). If not, then the desiccant dehumidifier model calculates the fraction of time it must operate to meet the process outlet air maximum humidity target (setpoint) using the following equation:
-
-<div>$$\begin{array}{l}\,DDPartLoadRatio = \,\frac{{\left( {{w_{Proc,\,\,in}} - {w_{max, set\,point}}} \right)}}{{\left( {{w_{Proc,\,\,in}} - {w_{Proc,\,\,out,HXon}}} \right)}}\\DDPartLoadRatio = MAX\left( {0.0,DDPartLoadRatio} \right)\\DDPartLoadRatio = MIN\,\left( {1.0,DDPartLoadRatio} \right)\end{array}$$</div>
-
-where:
-
-<span>\(\,DDPartLoadRatio\)</span> = output variable ‘Dehumidifier Part Load Ratio’
-
-<span>\({w_{Proc,\,\,in}}\)</span>      = process inlet air humidity ratio (kg/kg)
-
-<span>\({w_{max, set\,point}}\)</span> = target humidity ratio (setpoint) for the process outlet air (kg/kg)
-
-<span>\({w_{Proc,\,\,out,HXon}}\)</span>= process outlet air humidity ratio when the desiccant heat exchanger operates       (kg/kg)
-
-After all of the desiccant dehumidifier components are modeled at the appropriate part load ratio, the water removal rate and water removed are calculated.
-
-<div>$$
-  \begin{array}{rl}
-    {\mathop m\limits^ \bullet_{water\_removed,Proc}} &= \,{\mathop m\limits^ \bullet_{Proc,in}}\left( {{w_{Proc,\,\,in}} - {w_{Proc,\,\,out}}} \right) \\
-    {m_{water\_removed,Proc}}                         &= {\mathop m\limits^ \bullet_{water\_removed,Proc}}*\,\,TimeStepSys\,\,*\,\,3600.
-  \end{array}
-$$</div>
-
-where:
-
-<span>\({\mathop m\limits^ \bullet_{water\_removed,Proc}}\)</span> = output variable ‘Dehumidifier Removed Water Mass Flow Rate, kg/s’
-
-<span>\({\mathop m\limits^ \bullet_{Proc,in}}\)</span>       = air mass flow rate at the process air inlet node (kg/s)
-
-<span>\({w_{Proc,\,\,out}}\)</span>     = process outlet air humidity ratio (kg/kg)
-
-<span>\({m_{water\_removed,Proc}}\)</span>= output variable ‘Dehumidifier Removed Water Mass, kg’
-
-#### References
-
-ASHRAE. 2004. Chapter 22: Desiccant Dehumidification and Pressure-Drying Equipment. 2004 ASHRAE HVAC Systems and Equipment Handbook. Atlanta, GA: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Kosar, D. 2006. Dehumidification Enhancements, ASHRAE Journal, Vol. 48, No. 2, February 2006.
-
-Kosar, D. et al. 2006. Dehumidification Enhancement of Direct Expansion Systems Through Component Augmentation of the Cooling Coil. 15<sup>th</sup> Symposium on Improving Building Systems in Hot and Humid Climates, July 24-26, 2006.
-
-### Unitary Water-To-Air Heat Pump
-
-#### Overview
-
-The input object AirLoopHVAC:UnitaryHeatPump:WaterToAir provides a model for a water-to-Air heat pump that is a “virtual� component that consists of an on/off fan component, a water-to-air heat pump cooling coil, a water-to-air heat pump heating coil, and a gas or electric supplemental heating coil. The specific configuration of the blowthru heat pump is shown in the following figure. For a drawthru heat pump, the fan is located between the water-to-air heat pump heating coil and the supplemental heating coil. The configuration of the water-to-air heat pump in the air loop is similar to an air-to-air heat pump. In addition, a water-to-air heat pump has a water loop connection on its source side. The water loop can be served by a condenser loop (like GHE for Ground source systems), or by a cooling tower/ boiler plant loop (for water loop systems).
-
-![FurnaceSchematic\_WSHP](media/image5222.png)
-
-Figure 234.  Source Side and Load Side Configuration of a BlowThru WateroToAir Heat Pump
-
-There are two different models for water-to-air heat pump cooling and heating coils. Cooling and heating coils are modeled using a Single Speed or Variable Speed Equation Fit model or a Parameter Estimation model. The parameter estimation procedure is quite detailed and the equation fit model is designed to simplify the user inputs. Each model is discussed in short in the following sections. The Variable-Speed Equation Fit model is described in a separate section, as Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit and Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit.
-
-#### Single Speed Equation-Fit Model:
-
-This section describes the equation-fit model for Water-to-Air heat pump  (Object names: **Coil:Cooling:WaterToAirHeatPump:EquationFit** and **Coil:Heating:WaterToAirHeatPump:EquationFit**). This documentation is derived from the M.S. dissertation of Tang (2005) which is available on the Oklahoma State University web site . The model uses five non-dimensional equations or curves to predict the heat pump performance in cooling and heating mode. The methodology involved using the generalized least square method to generate a set of performance coefficients from the catalog data at indicated reference conditions. Then the respective coefficients and indicated reference conditions are used in the model to simulate the heat pump performance. The variables or inlet conditions that influenced the water-to-air heat pump performance are load side inlet water temperature, source side inlet temperature, source side water flow rate and load side water flow rate. The governing equations for the cooling and heating mode are as following:
-
-Cooling Mode:
-
-<div>$$\frac{{Q{}_{total}}}{{Q{}_{total,ref}}} = A1 + A2\left[ {\frac{{{T_{wb}}}}{{{T_{ref}}}}} \right] + A3\left[ {\frac{{T{}_{w,in}}}{{T{}_{ref}}}} \right] + A4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + A5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]$$</div>
-
-<div>$$\frac{{{Q_{sens}}}}{{{Q_{sens,ref}}}} = B1 + B2\left[ {\frac{{T{}_{db}}}{{T{}_{ref}}}} \right] + B3\left[ {\frac{{T{}_{wb}}}{{T{}_{ref}}}} \right] + B4\left[ {\frac{{T{}_{w,in}}}{{T{}_{ref}}}} \right] + B5\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + B6\left[ {\frac{{\dot V{}_w}}{{\dot V{}_{w,ref}}}} \right]$$</div>
-
-<div>$$\frac{{Power{}_c}}{{Power{}_{c,ref}}} = C1 + C2\left[ {\frac{{{T_{wb}}}}{{{T_{ref}}}}} \right] + C3\left[ {\frac{{T{}_{w,in}}}{{T{}_{ref}}}} \right] + C4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + C5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]$$</div>
-
-Heating Mode:
-
-<div>$$\frac{{{Q_h}}}{{Q{}_{h,ref}}} = E1 + E2\left[ {\frac{{{T_{db}}}}{{{T_{ref}}}}} \right] + E3\left[ {\frac{{T{}_{w,in}}}{{T{}_{ref}}}} \right] + E4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + E5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]$$</div>
-
-<div>$$\frac{{Powe{r_h}}}{{Power{}_{h,ref}}} = F1 + F2\left[ {\frac{{{T_{db}}}}{{{T_{ref}}}}} \right] + F3\left[ {\frac{{T{}_{w,in}}}{{T{}_{ref}}}} \right] + F4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + F5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]$$</div>
-
-Assuming no losses, the source side heat transfer rate for cooling and heating mode is calculated as following;
-
-<div>$${Q_{source,c}} = {Q_{total}} + Powe{r_c}$$</div>
-
-<div>$${Q_{source,h}} = {Q_h} - Powe{r_h}$$</div>
-
-where:
-
-<span>\(A1 - F5\)</span>     = Equation fit coefficients for the cooling and heating mode
-
-<span>\({T_{ref}}\)</span>            = 283K
-
-<span>\({T_{w,in}}\)</span>           = Entering water temperature, K
-
-<span>\({T_{db}}\)</span>             = Entering air dry-bulb temperature, K
-
-<span>\({T_{wb}}\)</span>            = Entering air wet-bulb temperature, K
-
-<span>\({\dot V_{air}}\)</span>            = Load side air volumetric flow rate, m<sup>3</sup>/s
-
-<span>\({\dot V_w}\)</span>                         = Source side water volumetric flow rate, m<sup>3</sup>/s
-
-<span>\({Q_{total}}\)</span>          = Total cooling capacity, W
-
-<span>\({Q_{sens}}\)</span>          = Sensible cooling capacity, W
-
-<span>\(Powe{r_c}\)</span>     = Power consumption (cooling mode), W
-
-<span>\({Q_{source,c}}\)</span>      = Source side heat transfer rate (cooling mode), W
-
-<span>\({Q_h}\)</span>                         = Total heating capacity, W
-
-<span>\(Powe{r_h}\)</span>     = Power consumption (heating mode), W
-
-<span>\({Q_{source,h}}\)</span>      = Source side heat transfer rate (heating mode), W
-
-The inlet conditions or variables are divided by the reference conditions. This formulation allows the coefficients to fall into smaller range of values. Moreover, the value of the coefficient indirectly represents the sensitivity of the output to that particular inlet variable. The reference conditions used when generating the performance coefficients must be the same as the reference conditions used later in the model. The reference temperature <span>\({T_{ref}}\)</span>is fixed at 283K. Temperature unit of Kelvin is used instead of Celsius to keep the ratio of the water inlet temperature and reference temperature positive value should the water inlet temperature drop below the freezing point.
-
-For cooling mode, the reference conditions; reference load side air volumetric flow rate <span>\(\left( {{{\dot V}_{air,ref}}} \right)\)</span>,reference source side water volumetric flow rate<span>\(\left( {{{\dot V}_{w,ref}}} \right)\)</span>,reference sensible capacity <span>\(\left( {{Q_{sens,ref}}} \right)\)</span> and reference power input <span>\(\left( {Powe{r_{c,ref}}} \right)\)</span> are the conditions when the heat pump is operating at the highest cooling capacity or reference cooling capacity<span>\(\left( {{Q_{total,ref}}} \right)\)</span> indicated in the manufacturer’s catalog. Note that the reference conditions for heating mode might differ from the reference conditions specified for the cooling mode.
-
-#### Coefficient estimation procedure:
-
-The generalized least square method is used to generate the coefficients. This method utilizes an optimization method which calculates the coefficients that will give the least amount of differences between the model outputs and the catalog data. A set of coefficients for the cooling mode is generated which includes A1-A5 for total cooling capacity, B1-B6 for sensible cooling capacity, and C1-C5 for power consumption. The same procedure is repeated for the heating mode to generate the coefficients E1-E5 and F1-F5. An information flow chart showing the inputs, reference conditions, performance coefficients and outputs are shown in the figure below:
-
-![](media/image5250.png)
-
-Figure 235. Information Flow Chart for Water-to-Air Heat Pump Equation Fit Model (Tang 2005)
-
-#### High Humidity Control with WaterToAir HeatPump Equation Fit model
-
-The specific configuration of the WaterToAir HeatPump with supplemental heating coil is shown above (see Figure 234). This figure shows the fan placement when a blow through fan is specified. If a draw through fan is specified, the fan is located between the heating coil and the reheat coil. The system is controlled to keep the high relative humidity in the control zone from exceeding the setpoint specified in the object ZoneControl:Humidistat. When high humidity control is specified and the compressor operates, the heatpump always operates at the cooling air flow rate when a zone heating load is present as determined by the zone thermostat. High humidity control is specified as either None, or CoolReheat in the Dehumidification Control Type input field. CoolReheat is specified when a DX cooling coil is used to over-cool the supply air stream in order to meet the zone latent load. In this case, a supplemental heating coil will ensure the zone temperature does not fall below the zone heating temperature set point. If the dehumidification control type is selected as None, the WaterToAir HeatPump uns only to meet the sensible cooling load. A supplemental heating coil is required for all dehumidification control types.
-
-The model first calculates the *PartLoadRatio* required meeting the sensible cooling load.  The heatpump’s sensible cooling load is determined from the control zone sensible cooling load to the cooling setpoint and the control zone air flow fraction to maintain the dry-bulb temperature setpoint in the control zone:
-
-<div>$$HeatPumpCoolingLoad = \,\frac{{ControlZoneCoolingLoad}}{{ControlZoneAirFlowFraction}}$$</div>
-
-The heatpump’s sensible cooling load to be met and the full load cooling output are used to calculate the sensible the part-load ratio iteratively based on user specified convergence criterion.
-
-<div>$$PartLoadRatio = MAX\left( {0.0,\,\frac{{ABS\left( {HeatPumpCoolingLoad - NoCoolOutput} \right)}}{{ABS\left( {FullCoolOutput - NoCoolOutput} \right)}}} \right)$$</div>
-
-When the heat pumps sensible cooling capacity meets the system sensible cooling load at a given sensible part load ratio, then the Heat pump meets the controlled zone cooling setpoint temperature.  If a moisture (latent) load exists because the control zone humidity has exceeded the setpoint, the total moisture load to be met by the heat pumps (HeatPumpMoistureLoad) is calculated based on the control zone moisture load and the control zone air flow fraction.
-
-<div>$$HeatPumpMoistureLoad = \,\frac{{ControlZoneMoitureLoad}}{{ControlZoneAirFlowFraction}}$$</div>
-
-Then the *LatentPartLoadRatio* required to meet the high humidity setpoint is calculated as follows:
-
-<div>$$LatentPartLoadRatio = MIN\left( {PL{R_{Min}},\,\frac{{ABS\left( {HeatPumpMoistureLoad - NoLatentOutput} \right)}}{{ABS\left( {FullLatentOutput - NoLatentOutput} \right)}}} \right)$$</div>
-
-The model uses the greater of the two part-load ratios, *PartLoadRatio* or *LatentPartLoadRatio*, to determine the operating part-load ratio of the Heat Pump’s DX cooling coil.
-
-<div>$$LatentPartLoadRatio = MAX\left( {PartLoadRatio,\,LatentPartLoadRatio} \right)$$</div>
-
-As previously described, iterations are performed to converge on the solution within the convergence tolerance.
-
-Where,
-
-<span>\(ControlZoneCoolingLoad\)</span>= the control zone sensible cooling load to the cooling setpoint, (W).
-
-<span>\(ControlZoneMoistureLoad\)</span>         = the control zone moisture load to the dehumidifying relative humidity setpoint, (W).
-
-<span>\(ControlZoneAirFlowFraction\)</span>     = the supply air fraction that goes though the control zone, (-).
-
-*FullLatentOutput*      =         the Heat Pump’s latent cooling energy rate at full-load conditions, W
-
-*NoLatentOutput*       =          the Heat Pump’s latent cooling energy rate with cooling coil OFF, W
-
-<span>\(PartLoadRatio\)</span>     =          the heat pump’s part-load-ratio required to meet system sensible load, (-).
-
-<span>\(LatentPartLoadRatio\)</span>      =          the heat pump’s part-load-ratio required to meet system moisture load, (-).
-
-<span>\(PL{R_{MIN}}\)</span>*       =  *the minimum part-load ratio, which is usually 0.0. For the case when the latent capacity degradation model is used (Ref: DX Cooling Coil Model), this value is the minimum part-load ratio at which the cooling coil will dehumidify the air.
-
-When the predicted zone air temperature is above the heating setpoint and if there is a dehumidification load, the supplemental heating coil load is required to offset the excess cooling as shown in Figure 236. If the model determines that the LatentPartLoadRatio is to be used as the operating part-load ratio of the heatpump’s cooling coil, the supplemental coil is used to offset the excess sensible capacity provided by the unit. The model first checks the sensible load that exists for the current simulation time step (predicted zone temperature with no HVAC operation compared to the thermostat setpoint temperatures). If a sensible cooling load or no sensible cooling or heating load exists (see Figure 236),  the model calculates the difference between the sensible heating load required to reach or maintain the heating dry-bulb temperature setpoint and the actual sensible cooling energy rate delivered by the heat pump (with LatentPartLoadRatio). In this case, thesupplemental heating coil is used to offset the excess sensible cooling energy provided by the DX cooling coil (if any) that could have caused an overshoot of the heating dry-bulb temperature setpoint. Note that when a humidistat is used and high humidity control is required, the zone dry-bulb temperature will typically move toward the heating temperature setpoint when a high moisture (latent) load exists.
-
-
-
-![HiHumidControl-2](media/image5262.png)
-
-Figure 236. Supplemental heating coil load when predicted zone air temperature is above the heating Setpoint
-
-If a heating load exists (Figure 237), the supplementalheating coil is used to meet the heating coil load and at the same time offset the entire sensible cooling energy rate of the DX cooling coil (to meet the humidistat setpoint). Note that when a heating load exists and high humidity control is required, the heat pump operates at the user-specified cooling air flow rate for the entire simulation time step. As with the fan, and DX cooling coil, report variables associated with supplemental heating coil performance (e.g., heating coil energy, heating coil rate, heating coil gas or electric energy, heating coil runtime fraction, etc.) are managed in the supplemental (heating) coil object.
-
-![HiHumidControl-3](media/image5263.png)
-
-Figure 237. Supplemental heating coil load when predicted zone air temperature is below the heating setpoint
-
-#### Parameter Estimation Model
-
-The steady state simulation model (Object: AirLoopHVAC:UnitaryHeatPump:WaterToAir) for a water-to-air vapor compression heat pump is described in this section. The model is implemented under the air-loop manager similar to the algorithm discussed under AirLoopHVAC:UnitaryHeatPump. The heat pump 'coil' objects (Coil:Cooling:WaterToAirHeatPump:ParameterEstimation and
- Coil:Heating:WaterToAirHeatPump:ParameterEstimation) actually consist of a steady state simulation of the unitary heat pump in cooling or heating mode respectively.  This documentation is derived from the Ph.D. dissertation of Hui Jin which is available on the Oklahoma State University web site .  The model parameters, solution technique and solution algorithm are all identical to that of the water to water heat pump.  The only difference between the two models is in the modeling of the water to air heat exchanger.
-
-The effectiveness of this heat exchanger is given by
-
-<div>$$\varepsilon  = 1 - {e^{ - NTU}}$$</div>
-
-Where NTU is defined by
-
-<div>$$NTU = \frac{{UA}}{{(\dot mC{}_p){}_{water/air}}}$$</div>
-
-UA for the source side and the load side are two of the parameters estimated in the parameter estimation procedure.
-
-Additional model details and a discussion of the parameters and parameter estimation technique are described in the following section on Water to Water Heat Pumps.
-
-### Water To Water Heat Pumps
-
-There are two water-water heat pump models available in EnergyPlus which are **parameter estimation based model** and **equation-fit model**. Detailed descriptions of the model are available in the references Tang and Jin
-
-### Equation Fit Water To Water Heat Pump Model
-
-This section describes the equation-fit model for water-to-water heat pump. (Object names: HeatPump:WaterToWater:EquationFit:Cooling & HeatPump:WaterToWater:EquationFit:Heating). This documentation is derived from the M.S. dissertation of Tang (2005) which is available on the Oklahoma State University web site . The model uses four non-dimensional equations or curves to predict the heat pump performance in cooling and heating mode. The methodology involved using the generalized least square method to generate a set of performance coefficients from the catalog data at indicated reference conditions. Then the respective coefficients and indicated reference conditions are used in the model to simulate the heat pump performance. The variables that influenced the water-to-water heat pump performance are load side inlet water temperature, source side inlet temperature, source side water flow rate and load side water flow rate. The governing equations for the cooling and heating mode are as following:
-
-Cooling Mode:
-
-<div>$$\frac{{Q{}_c}}{{Q{}_{c,ref}}} = A1 + A2\left[ {\frac{{T{}_{L,in}}}{{T{}_{ref}}}} \right] + A3\left[ {\frac{{T{}_{S,in}}}{{T{}_{ref}}}} \right] + A4\left[ {\frac{{{{\dot V}_L}}}{{{{\dot V}_{L,ref}}}}} \right] + A5\left[ {\frac{{{{\dot V}_S}}}{{{{\dot V}_{S,ref}}}}} \right]$$</div>
-
-<div>$$Powe{r_c} = B1 + B2\left[ {\frac{{T{}_{L,in}}}{{T{}_{ref}}}} \right] + B3\left[ {\frac{{T{}_{S,in}}}{{T{}_{ref}}}} \right] + B4\left[ {\frac{{{{\dot V}_L}}}{{{{\dot V}_{L,ref}}}}} \right] + B5\left[ {\frac{{{{\dot V}_S}}}{{{{\dot V}_{S,ref}}}}} \right]$$</div>
-
-Heating Mode:
-
-<div>$$\frac{{{Q_h}}}{{Q{}_{h,ref}}} = C1 + C2\left[ {\frac{{T{}_{L,in}}}{{T{}_{ref}}}} \right] + C3\left[ {\frac{{T{}_{S,in}}}{{T{}_{ref}}}} \right] + C4\left[ {\frac{{{{\dot V}_L}}}{{{{\dot V}_{L,ref}}}}} \right] + C5\left[ {\frac{{{{\dot V}_S}}}{{{{\dot V}_{S,ref}}}}} \right]$$</div>
-
-<div>$$Powe{r_h} = D1 + D2\left[ {\frac{{T{}_{L,in}}}{{T{}_{ref}}}} \right] + D3\left[ {\frac{{T{}_{S,in}}}{{T{}_{ref}}}} \right] + D4\left[ {\frac{{{{\dot V}_L}}}{{{{\dot V}_{L,ref}}}}} \right] + D5\left[ {\frac{{{{\dot V}_S}}}{{{{\dot V}_{S,ref}}}}} \right]$$</div>
-
-Assuming no losses, the source side heat transfer rate for cooling and heating mode is calculated as following;
-
-<div>$${Q_{source,c}} = {Q_c} + Powe{r_c}$$</div>
-
-<div>$${Q_{source,h}} = {Q_h} - Powe{r_h}$$</div>
-
-
-
-Where:
-
-<span>\(A1 - D5\)</span>            = Equation fit coefficients for the cooling and heating mode
-
-<span>\({T_{ref}}\)</span>          = 283.15K
-
-<span>\({T_{L,in}}\)</span>         = Entering load side water temperature, K
-
-<span>\({T_{S,in}}\)</span>         = Entering source side water temperature, K
-
-<span>\({\dot V_L}\)</span>         = Load side volumetric flow rate, m<sup>3</sup>/s
-
-<span>\({\dot V_S}\)</span>         = Source side volumetric flow rate, m<sup>3</sup>/s
-
-<span>\({Q_c}\)</span>              = Load side heat transfer rate (cooling mode), W
-
-<span>\(Powe{r_c}\)</span>          = Power consumption (cooling mode), W
-
-<span>\({Q_{source,c}}\)</span>      = Source side heat transfer rate (cooling mode), W
-
-<span>\({Q_h}\)</span>              = Load side heat transfer rate (heating mode), W
-
-<span>\(Powe{r_h}\)</span>          = Power consumption (heating mode), W
-
-<span>\({Q_{source,h}}\)</span>     = Source side heat transfer rate (heating mode), W
-
-*COP<sub>c</sub>*                   = Cooling coefficient of performance, W/W
-
-*COP<sub>h</sub>*                   = Heating coefficient of performance, W/W
-
-
-
-If the load side heat transfer rate (*Q<sub>c</sub>* or *Q<sub>h</sub>*) or power consumption (*Power<sub>c</sub>* or *Power<sub>h</sub>*) are less than or equal to zero, then the heat pump is turned off for that simulation time step, a warning is issued, and the simulation continues.
-
-The inlet conditions or variables are divided by the reference conditions. This formulation allows the coefficients to fall into smaller range of values. Moreover, the value of the coefficient indirectly represents the sensitivity of the output to that particular inlet variable. The reference conditions used when generating the performance coefficients must be the same as the reference conditions used later in the model. The reference temperature <span>\({T_{ref}}\)</span>is fixed at 283K. Temperature unit of Kelvin is used instead of Celsius to keep the ratio of the water inlet temperature and reference temperature positive value should the water inlet temperature drop below the freezing point.
-
-For cooling mode, the reference conditions; reference load side volumetric flow rate, <span>\({\dot V_{L,ref}}\)</span>, reference source side volumetric flow rate, <span>\({\dot V_{S,ref}}\)</span>, <span>\(Powe{r_{c,ref}}\)</span>  and reference source side heat transfer rate, <span>\({Q_{source,c,ref}}\)</span>  are the conditions when the heat pump is operating at the highest cooling capacity or reference cooling capacity, <span>\({Q_{c,ref}}\)</span> indicated in the manufacturer’s catalog. Note that the reference conditions for heating mode might differ from the reference conditions specified for the cooling mode.
-
-#### Coefficient estimation procedure:
-
-The generalized least square method is used to generate the coefficients. This method utilizes an optimization method which calculates for the coefficients that will give the least amount of differences between the model outputs and the catalog data. A set of coefficients for the cooling mode is generated which includes A1-A5 for load side heat transfer. The same procedure is repeated B, C, and D coefficients. An information flow chart showing the inputs, reference conditions, performance coefficients and outputs are shown in the figure below:
-
-![](media/image5290.png)
-
-Figure 238.  Information Flow Chart for Water-To-Water Heat Pump Equation Fit (Tang 2005)
-
-### Parameter Estimation Water-To-Water Heat Pump Model
-
-A steady state simulation model for a water-to-water reciprocating vapor compression heat pump (Object names: HeatPump:WaterToWater:ParameterEstimation:Cooling & HeatPump:WaterToWater:ParameterEstimation:Heating) is described in this section. This documentation is derived from the Ph.D. dissertation of Hui Jin which is available on the Oklahoma State University web site . The model incorporates a multivariable unconstrained optimization algorithm to estimate several unspecific parameters. The aim of the model is to describe the detailed physical geometry and operation of each component and replicate the performance of the actual unit in operation. Assuming the thermodynamic process in the expansion device and the pressure drop at the suction and discharge valves to be isenthalpic the heat balance equation is given by
-
-<div>$${\dot Q_s} = \dot W + {\dot Q_{_L}}$$</div>
-
-Where:
-
-<span>\({\dot Q_s}\)</span> = Source side heat transfer rate
-
-<span>\({\dot Q_L}\)</span> = Load side heat transfer rate
-
-<span>\(\dot W\)</span>= Compressor power input
-
-The compressor model is based on an isentropic process shown in Figure 239 governed by
-
-<span>\(P{V^\gamma }\)</span> = Constant
-
-Where:
-
-P = Pressure
-
-v = Specific volume
-
-![](media/image5296.png)
-
-Figure 239.  Schematic indicator diagram for a reciprocating Compressor(Jin 2002)
-
-Since the refrigerant vapor in the clearance volume as shown in the previous figure goes through a re-expansion procedure, the mass flow rate of the compressor refrigerant is a decreasing function of the pressure ratio.
-
-<div>$$\mathop m\limits^ \bullet   = \frac{{PD}}{{\nu {}_{suc}}}(1 + C - C{(\frac{{P{}_{dis}}}{{P{}_{suc}}})^{\frac{1}{\gamma }}}$$</div>
-
-Where:
-
-<span>\(\mathop m\limits^ \bullet  \)</span>  = refrigerant mass flow rate
-
-PD = Piston displacement
-
-C   = Clearance factor
-
-<span>\(P{}_{dis}\)</span> = discharge pressure
-
-<span>\(P{}_{suc}\)</span> = Suction pressure
-
-<span>\(\gamma \)</span>     = Isentropic exponent
-
-#### Parameter estimation procedure:
-
-A set of parameters for the cooling mode is defined on the basis of the equations used in the model. An information flowchart indicating the parameters, inputs to the model and the resulting outputs acquired are shown in Figure 240. The estimation of parameters is conducted using the catalog data.
-
-The parameter definition include:
-
-n Piston displacement, PD
-
-n Clearance factor, C
-
-n Pressure drop across the suction and discharge valves, <span>\({\rm{\Delta P}}\)</span>
-
-n Loss factor used to define the electromechanical losses supposed to be proportional to the theoretical power, <span>\({\rm{\eta }}\)</span>
-
-n Superheat in <sup>ο</sup>C or F, <span>\({\rm{\Delta T}}{}_{{\rm{sh}}}\)</span>
-
-n Constant part of the electromechanical losses,<span>\({\rm{W}}{}_{{\rm{loss}}}\)</span>
-
-n Source side heat transfer coefficient, (UA)<sub>S</sub>
-
-n Load side heat transfer coefficient, (UA)<sub>L</sub>
-
-![](media/image5306.png)
-
-Figure 240.  Information Flowchart for Water-To-Water Heat Pump Parameter Estimation Mmodel implementation (Jin 2002)
-
-Where:
-
-TWiL   = Entering water Load side temperature
-
-TWiS   = Entering water Source side temperature
-
-<span>\(\mathop {\rm{m}}\limits^ \bullet  {}_{{\rm{WiL}}}\)</span>= Entering water Load side mass flow rate
-
-<span>\(\mathop {\rm{m}}\limits^ \bullet  {}_{{\rm{WiS}}}\)</span>= Entering water Source side mass flow rate
-
-S      =  Thermostatic Signal
-
-The parameter estimation procedure incorporates an objective function that computes the difference between the model outputs and the catalog outputs.  The objective function is then minimized by using a multi variable unconstrained multi modal Nelder Mead optimization algorithm. As the objective function value lowers after each iteration, the model outputs approach the catalog outputs consequently leading to convergence and the correct parameters are estimated for the respective model. The inputs to the model include the entering water temperatures and mass flow rates on the load side and the source side. The calculation of the objective function is shown in the form of a formula flowchart in Figure 241. The square of the sum of the errors (SSQE) for a given set of parameter values that will be minimized is given by
-
-<div>$$SSQE = \sum\limits_{i = 1} {{{\left( {\frac{{\left( {\mathop {W{}_{cat}}\limits^{} } \right) - \left( {\mathop W\limits^{} } \right){}_i}}{{\left( {\mathop {W{}_{cat}}\limits^{} } \right)}}} \right)}^2}}  + \left( {\frac{{\left( {\mathop {QL{}_{cat}}\limits^{} } \right) - \left( {\mathop {QL}\limits^{} } \right){}_i}}{{\left( {\mathop {QL{}_{cat}}\limits^{} } \right)}}} \right)$$</div>
-
-Where
-
-<span>\({\rm{W}}{}_{{\rm{cat}}}\)</span>= Catalog power consumption
-
-<span>\({\rm{W}}{}_{}\)</span> = Model power consumption
-
-<span>\({\rm{QL}}{}_{{\rm{cat}}}\)</span>= Catalog load side heat transfer
-
-<span>\({\rm{QL}}{}_{}\)</span> = Model load side heat transfer
-
-Extrapolation beyond the catalog data grants the parameter estimation model an upper hand in comparison with the equation fit and deterministic models. However, the detailed model is computationally more intensive. Moreover, when the model is implemented within a transient system simulation program, it may come across figures that are random and unplanned by the manufacturer such as low water flow rates or extreme temperatures. This oddity may result in unrealistic set of results.
-
-![Jin's flow chart](media/image5314.png)
-
-Figure 241.  Flow diagram of EnergyPlus Water to Water HeatPump implementation
-
-#### Control Strategy:
-
-Both water-to-water heat pump models; parameter estimation based model and curve-fit model use the “cycle time control logic� developed by Murugappan (2002).
-
-This strategy keeps the heat pump from short-cycling whereby the heat pump will stay on or off for the specified cycle time after switching states. The control logic is identical to the operation of a physical heat pump whereby the heat pump does not switch between on and off instantly. Refer to Muraggapan (2002) for the further details on the control strategy.
-
-#### References
-
-Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from [http://www.hvac.okstate.edu/](http://www.hvac.okstate.edu))
-
-Tang,C. C. 2005. Modeling Packaged Heat Pumps in Quasi-Steady State Energy Simulation Program. M.S. Thesis. Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from [http://www.hvac.okstate.edu/](http://www.hvac.okstate.edu))
-
-Murugappan, Arun. 2002.  Implementing Ground Source Heat Pump and Ground Loop Heat Exchanger Models in the EnergyPlus Simulation Environment, M.S. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University (downloadable from [http://www.hvac.okstate.edu/](http://www.hvac.okstate.edu))
-
-
-
-Variable Refrigerant Flow Heat Pumps <a name="VRF"></a>
-------------------------------------
-
-A Variable Refrigerant Flow (VRF, or Variable Refrigerant Volume) system is an air-conditioning system that varies the refrigerant flow rate using variable speed compressor(s) in the outdoor unit, and the electronic expansion valves (EEVs) located in each indoor unit. The system meets the space cooling or heating load requirements by maintaining the zone air temperature at the setpoint. The ability to control the refrigerant mass flow rate according to the cooling and/or heating load enables the use of as many as 60 or more indoor units with differing capacities in conjunction with one single outdoor unit. This unlocks the possibility of having individualized comfort control, simultaneous heating and cooling in different zones, and heat recovery from one zone to another. It may also lead to more efficient operations during part-load conditions.
-
-There are two common types of VRF systems. 
-
- * Heat Pump (HP) type: the most general type that can be used for either cooling or heating, but not simultaneously. 
- 
- * Heat Recovery (HR) type: can deliver simultaneous heating and cooling to different zones by transferring heat between the cooling and heating indoor units. This generally occurs in the winter season in medium-sized to large-sized commercial buildings with a substantial core such as computer rooms.
-
-There are two alternative VRF models availabe in EnergyPlus to simulate the energy performance of Variable Refrigerant Flow (VRF, or Variable Refrigerant Volume) air-conditioning systems: 
-
- 1. **System Curve based Model (VRF-SysCurve)**. In this model, a number of system level curves are used to describe the VRF system performance. It corresponds to the *AirConditioner:VariableRefrigerantFlow* object. 
- 
- 2. **Physics based Model (VRF-FluidTCtrl)**. This model is able to consider the dynamics of more operational parameters and is applicable for fluid temperature control. This model corresponds to the *AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl* object.
- 
- 
-### Variable Refrigerant Flow Heat Pump Model (System Curve Based Model)
-
-#### Overview
-
-This section describes the System Curve based VRF Model (VRF-SysCurve), which can address both the heat pump and heat recovery operating modes and support air-, evaporatively-, or water-cooled condenser equipment ( throughout this section, the term “condenser� refers to the outdoor unit where the compressor is located. )
-
-The figure below schematically depicts the AirConditioner:VariableRefrigerantFlow (VRF AC) system. The outdoor unit is connected directly to the zone terminal units using a zone terminal unit list (ref: ZoneTerminalUnitList). The VRF AC system conditions multiple zones and is controlled by thermostats located in each zone. Zone terminal units operate to meet the zone sensible cooling or sensible heating requirements as determined by the zone thermostat schedule. 
-
-When the heat pump does not operate to reclaim waste heat, the VRF AC system can only operate in either cooling *or* heating mode. Based on the master thermostat priority control selection, the operating mode is determined by polling the appropriate zone(s) served by the VRF HP system. When the system is operating in cooling mode, the cooling coils will be enabled only in the terminal units where zone cooling is required. When the system is operating in heating mode, the heating coils will be enabled only in the terminal units where zone heating is required. Supply air fans will continue to operate if the zone terminal unit’s fan operating mode is set to continuous fan.
-
-When the heat pump does operate to reclaim waste heat, the VRF AC system can simultaneously cool and heat multiple zones. The heat pump will select an operating mode according to the dominant load as reported by the zone thermostat(s). The calculation of the dominant load is based on the master thermostat priority control selection and may either be based on individual zone loads, the number of zones requiring cooling or heating, the master thermostat zone load, or an operating mode schedule. The heat pump will operate in cooling mode, and provide waste heat to zones with a heating load, when the dominant load among all zone terminal units is cooling. The heat pump will operate in heating mode, and absorb heat from zones with a cooling load, when the dominant load among all zone terminal units is heating.
-
-The figure below shows the VRF AC terminal units with draw through fan placement. Blow through fan placement can also be modeled by connecting the supply air fan inlet node to the outside air mixer’s mixed air node if an outdoor air mixer is used or to the zone terminal unit inlet node if an outdoor air mixer is not used. The variable refrigerant flow heat pump coordinates the operation of these components and is modeled as a type of zone equipment where the *zone terminal units* are specified in a zone equipment list (Ref. ZoneHVAC: EquipmentList and ZoneHVAC:EquipmentConnections). The AirConditioner: VariableRefrigerantFlow object *is not* specified in an air primary loop or a zone equipment list object.
-
-![](media/image5315.png)
-
-Figure 242. Variable Refrigerant Flow Heat Pump (draw through fan placement)
-
-
-
-![](media/image5316.png)
-
-Figure 243. Energyplus object connections for VRF-SysCurve model 
-
-The terminal unit is able to model supply air fan operation in two modes: cycling fan – cycling coil (i.e., AUTO fan) and continuous fan – cycling coil (i.e., fan ON). Fan:Simple:OnOff must be used to model AUTO fan, while Fan:Simple:OnOff or Fan:Simple:ConstVolume can be used to model fan ON.
-
-Output variables reported by the VRF AC object include the heat pump’s operating capacity (cooling or heating), electric consumption, operating COP, defrost electric consumption, part-load ratio (ratio of actual capacity to available capacity), runtime fraction (when cycling), cycling ratio (actual compressor cycling rate), crankcase heater power, and other report variables associated with an evaporative condenser. Report variables are also available to indicate the maximum available terminal unit cooling or heating capacity (i.e., when the condensers available capacity is insufficient to supply the capacity requested by all terminal units). Reporting of other variables of interest for the VRF AC (fan electric power, DX coil cooling rate, DX coil heating rate, terminal unit total cooling rate, etc.) is done by the individual system components (e.g., fan, DX cooling coil, DX heating coil, and zone terminal unit). For convenience, the total cooling and heating coil capacities (i.e., the coil loads) is also reported.
-
-#### Model Description
-
-As described previously, the VRF AC system conditions multiple zones and is controlled by one or more zone thermostats (ZoneControl:Thermostatic). Each simulation time step, EnergyPlus performs a zone air heat balance to determine if cooling or heating is required to meet each zone’s thermostat set point. When heat pump mode is selected (i.e., heat recovery is not selected), an operating mode is chosen based on the master thermostat priority control and all terminal units are operated in that specific mode. When heat recovery mode is selected, the dominant load is determined based on the master thermostat priority control and the outdoor unit operates in this mode. The indoor terminal units operate in either cooling or heating mode based on the individual coil loads The heat pump condenser is then modeled to determine any impact the condensing unit might have on the zone terminal units (i.e., capacity limitations due to oversized terminal units, operating limitations due to allowable operating temperature range, impacts of defrost operation, changes in performance when heat recovery mode is active, etc.). The following sections describe the performance calculations for cooling and heating.
-
-#### Cooling Operation
-
-The operating capacity of the heat pump is calculated based on the user defined input for the heat pump’s rated cooling capacity, the ratio of indoor terminal unit capacity to outdoor unit capacity (combination ratio), the actual operating conditions, and whether or not the system’s heat recovery mode is active. Performance correction factors are used to correct for off-design performance as follows:
-
-#### Cooling Combination Ratio Correction Factor
-
-The cooling combination ratio correction factor is defined as the total terminal unit rated cooling capacity divided by the heat pump’s rated cooling capacity. The combination ratio is important when multiple terminal units (or DX coils) are attached to a single variable-speed condensing unit. If the combination ratio is less than 1, the condenser’s rated capacity is assumed to be able to meet the indoor terminal unit’s demand request. However, if the combination ratio is determined to be greater than 1, the maximum cooling capacity available from the heat pump’s condenser may be higher than the user specified rated cooling capacity. The combination ratio capacity correction factor is based on a linear, quadratic or cubic curve and provides a multiplier &gt; 1 to correct for combination ratio’s greater than 1. For example, a combination ratio of 1.3 (130%) may result in a combination ratio capacity correction factor of 1.06 (outdoor condenser can actually provide 106% of rated capacity) . The cooling combination ratio correction factor is applied to cooling performance calculations. If the cooling combination ratio correction curve name is not specified by the user, the cooling combination ratio correction factor (CR <sub>cooling,\\ correction</sub>) in the following equation is assumed to be equal to 1.
-
-<div>$$C{R_{cooling\,,\,rated\,}} = {\raise0.7ex\hbox{${\sum\limits_1^n {{{\mathop Q\limits^ \bullet  }_{coil(i)\,,\,cooling,\,rated}}} }$} \!\mathord{\left/ {\vphantom {{\sum\limits_1^n {{{\mathop Q\limits^ \bullet  }_{coil(i)\,,\,cooling,\,rated}}} } {{{\mathop Q\limits^ \bullet  }_{cooling,\,total,\,\,rated}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{cooling,\,total,\,\,rated}}}$}}$$</div>
-
-<div>$$C{R_{\,cooling\,,\,correction}} = a + b\left( {C{R_{cooling\,,\,rated}}} \right) + c{\left( {C{R_{cooling\,,\,rated}}} \right)^2} + d{\left( {C{R_{cooling\,,\,rated}}} \right)^3}$$</div>
-
-<div>$$C{R_{\,cooling\,,\,correction}} = MAX\left( {1.0\,\,,\,\,C{R_{\,cooling\,,\,correction}}} \right)$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{coil(i)\,,\,cooling\,,\,rated}}\)</span> = rated total (sensible + latent) cooling capacity in zone *i* (W)
-
-<span>\({\mathop Q\limits^ \bullet_{cooling,\,total\,,\,rated}}\)</span>   = rated total cooling capacity of heat pump (W)
-
-<span>\(C{R_{\,cooling\,,\,correction}}\)</span> = Cooling Combination Ratio capacity correction factor at rated conditions (this value is reported in the eio file)
-
-<span>\(a - d\)</span>                = equation coefficients for cooling combination ratio correction factor
-
-<span>\(C{R_{cooling\,,\,rated}}\)</span>      = the cooling combination ratio defined as the total indoor terminal unit’s rated total cooling capacity divided by the rated total cooling capacity of the heat pump condenser.
-
-The sum of the individual zone total cooling requirements is used to calculate the performance of the outdoor condensing unit. The operating capacities of the indoor cooling coils are calculated based on the indoor cooling coil’s rated cooling capacity and the actual operating conditions. The operating capacity of the heat pump condenser is calculated in a similar fashion using a load-weighted average indoor wet-bulb temperature of all operating cooling coils.
-
-#### Cooling Capacity Ratio Modifier Function of Low Temperature
-
-The heat pump’s cooling capacity correction factor (function of temperature) is determined by averaging the zone cooling coil inlet air wet-bulb temperature for all operating cooling coils. A load-weighted average inlet air wet-bulb temperature is used in the calculations. The weighted average cooling coil inlet air wet-bulb temperature and the outdoor condenser entering air dry-bulb temperature are then used to calculate the temperature correction factor in cooling mode for the heat pump condenser. The actual zone air wet-bulb temperature is used to calculate the operating capacity of the individual zone cooling coils.
-
-<div>$${\mathop Q\limits^ \bullet_{zone,\,total}} = \sum\limits_1^i {{{\mathop Q\limits^ \bullet  }_{zone(i)}}} $$</div>
-
-<div>$${T_{wb,avg}} = \sum\limits_1^i {\left( {{T_{wb,i}}} \right)} \left( {{\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{zone(i)}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{zone(i)}}} {{{\mathop Q\limits^ \bullet  }_{zone,\,total}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{zone,\,total}}}$}}} \right)$$</div>
-
-The operating capacity of the heat pump is calculated using a bi-quadratic equation using a load-weighted average indoor wet-bulb temperature and outdoor dry-bulb temperature as the independent variables.
-
-<div>$$CAPF{T_{HP,cooling}} = a + b\left( {{T_{wb,avg}}} \right) + c{\left( {{T_{wb,avg}}} \right)^2} + d\left( {{T_c}} \right) + e{\left( {{T_c}} \right)^2} + f\left( {{T_{wb,avg}}} \right)\left( {{T_c}} \right)$$</div>
-
-The operating capacity of the terminal unit’s DX cooling coil is calculated using either a linear, quadratic, or cubic curve. If more information is available to more accurately model the DX cooling coil, a bi-quadratic curve may be used (i.e., if the performance of the DX cooling coil is also a function of outdoor dry-bulb temperature).
-
-<div>$$CAPF{T_{coil,\,cooling}} = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d{\left( {{T_{wb,i}}} \right)^3}$$</div>
-
- - or -
-
-<div>$$CAPF{T_{coil,cooling}} = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d\left( {{T_c}} \right) + e{\left( {{T_c}} \right)^2} + f\left( {{T_{wb,i}}} \right)\left( {{T_c}} \right)$$</div>
-
-where
-
-<span>\({T_{wb,i}}\)</span> = wet-bulb temperature of the air entering the cooling coil in zone *i* (°C)
-
-<span>\({T_{wb,avg}}\)</span>= load-weighted average wet-bulb temperature of the air entering all operating cooling coils (°C)
-
-<span>\({\mathop Q\limits^ \bullet_{zone(i)}}\)</span> = total (sensible + latent) cooling load in zone *i* (W)
-
-<span>\({\mathop Q\limits^ \bullet_{zone,\,total}}\)</span> =total (sensible + latent) cooling load in all zones (W)
-
-<span>\(CAPF{T_{\,HP,cooling}}\)</span> = heat pump Cooling Capacity Ratio Modifier (function of temperature)
-
-<span>\(CAPF{T_{\,coil,cooling}}\)</span> = zone coil Cooling Capacity Ratio Modifier (function of temperature)
-
-<span>\(a - f\)</span>  = equation coefficients for Cooling Capacity Ratio Modifier
-
-<span>\({T_c}\)</span>    = temperature of the air entering an air-cooled or evaporatively-cooled condenser (°C)
-
-#### Using multiple curves to define Cooling Capacity Ratio Modifier
-
-The cooling capacity ratio modifier determines the change in total (sensible + latent) capacity with respect to the heat pump rated cooling capacity. This modifier corrects for off-design performance and provides the operating total (sensible + latent) cooling capacity for the heat pump condenser. The performance data for VRF AC systems may be specified using a single curve object, however, if the performance data does not reflect a smooth change in performance as outdoor conditions vary, the overall performance of the system may be described using two cooling capacity ratio modifier curves (i.e., a separate curve at low and high outdoor temperatures) and a boundary curve (i.e., the curve defining the separation at specific outdoor temperatures).
-
-#### Application of Dual Performance Curves
-
-Two additional inputs are available to more accurately model the cooling performance of a VRF AC system. The first additional input is a boundary curve which is used to distinguish differences in performance at “low� and “high� outdoor temperature regions and the second input is a cooling capacity performance curve for the “high� outdoor temperature region. The boundary curve is a linear, quadratic or cubic curve defining the outdoor temperature as a function of average indoor wet-bulb temperature. The cooling capacity ratio function of high temperature curve is a biquadratic curve using average indoor wet-bulb temperature and outdoor dry-bulb temperature as the two independent variables. These additional curves are used to define the performance over two separate performance regions as shown in Figure 244. The red circles in the figure identify the points at which the performance changes abruptly (i.e., slopes or shapes are significantly different) and are used to create the boundary curve. The performance on either side of the boundary curve can be a smooth curve changing with outdoor condition or a flat plateau where system controls maintain a constant operating condition. This type of performance cannot be accurately simulated using a single performance curve object. For this reason, dual capacity performance curves may be used.
-
-Note: If the cooling performance can be described using a single performance curve object, the boundary and high temperature performance curve objects are not required.
-
-Manufacturers may also provide this information in a tabular format. In this case the data should first be graphically displayed to identify any non-linearities and to also identify where an abrupt change in performance occurs so that a boundary curve can be created.
-
-The cooling capacity ratio boundary curve object is used to differentiate between dual cooling capacity ratio performance curves. This curve defines the outdoor temperature below which the cooling capacity ratio function of low temperature curve object is used, otherwise, the cooling capacity ratio function of high temperature curve object is used.
-
-<div>$${T_{OA,DB}} = a + b\left( {{T_{I,WB}}} \right) + c{\left( {{T_{I,WB}}} \right)^2} + d{\left( {{T_{I,WB}}} \right)^3}$$</div>
-
-where
-
-T<sub>OA,DB</sub> = Outside air dry-bulb temperature (C)
-
-a-d = coefficients for cooling capacity ratio boundary curve object
-
-T<sub>I,WB</sub> = Weighted average indoor wet-bulb temperature (C)
-
-For the performance data shown below, the boundary curve would be created by identifying the outdoor dry-bulb temperature at which the performance changed abruptly for each of the indoor wet-bulb temperature curves shown in the figure. The following example shows the data interpreted from the figure used to regress the cooling capacity ratio boundary curve coefficients. For this example, the regression coefficients were found to be: A1 = 29.87396, B1 = -0.6928, C1= 0.01928, D1 = -0.000532
-
-Table 73. Performance Data for Variable Refrigerant Flow Air Conditioner Model
-
-![](media/image5339.svg.png)
-
-Although the capacity and energy performance curves each have an independent boundary curve input, in this example the same boundary curve may be used for both the capacity and energy input ratio curves. When the “low� and “high� predicted performance data do not line up at the boundary curve points, the boundary curve may have to be modified slightly to allow a smooth transition in performance from the “low� to “high� temperature region. In this case, the boundary curves for capacity and energy may be different.
-
-![](media/image5340.png)
-
-Figure 244. Non-Linear Performance of VRF Heat Pump in Cooling Mode
-
-A regression is then performed on the data to the left of the boundary curve to calculate the low temperature cooling performance curve coefficients. A regression is also performed on the data to the right of the boundary curve to create the high temperature cooling performance curve coefficients. The model then uses the boundary curve to determine which performance curve (low or high) to use during the simulation. For example, given a particular average indoor wet-bulb temperature, if the boundary curve object calculates an outdoor dry-bulb temperature that is above the actual outdoor dry-bulb temperature then the cooling capacity ratio function of low temperature performance curve is used to determine AC system performance for that specific simulation time step. When creating the boundary curve, be careful to make sure the low and high performance curves meet, as closely as possible, at the boundary curve points (i.e., that discontinuities do not exist or are minimized to the extent possible). Tabular data (ref: Table:TwoIndependentVariables) may also be used to specify performance and will usually eliminate the need for dual performance curves.
-
-#### Determining Cooling Coil Sensible Capacity
-
-The zone terminal unit’s cooling coil is controlled by a zone thermostat and must meet a zone “sensible� load. The cooling coil’s sensible capacity is defined as the cooling coil’s total capacity multiplied by the coil’s sensible heat ratio (SHR) at the current operation conditions. Since the SHR of the variable refrigerant flow cooling coil changes as the inlet air wet-bulb temperature and the operating part-load ratio change, an iterative solution technique must be used to determine the coil’s sensible capacity. The target solution is found when the sensible capacity of the zone cooling coil equals the zone sensible cooling load (if sufficient capacity is available). The iterative solution converges when the difference (error) between the zone sensible cooling load and the terminal unit sensible cooling capacity is within tolerance (0.001) or the terminal unit has insufficient capacity to meet the zone sensible cooling load. Refer to the description of the VRF cooling coil model for further details (ref: Variable Refrigerant Flow Cooling Coil).
-
-<div>$${\mathop Q\limits^ \bullet_{coil(i)\,,\,cooling\,,\,total}} = {\mathop Q\limits^ \bullet_{coil(i)\,,\,cooling\,,\,rated}}\left( {CAPF{T_{coil,cooling}}} \right)$$</div>
-
-<div>$$PL{R_i} = 1$$</div>
-
-<div>$$\begin{array}{l}Iteration\,\,Loop(PL{R_i}) -  -  -  -  -  -  -  -  -  -  -  -  -  - \\\,\,\,\,SH{R_{PLR}} = f\left( {{T_{wb,\,i}},\,PL{R_i},\,{{\mathop m\limits^ \bullet  }_i}} \right)\\\,\,\,\,{\mathop Q\limits^ \bullet_{coil(i),\,cooling,\,sensible}} = {\mathop Q\limits^ \bullet_{coil(i),\,cooling,\,total}}\left( {SH{R_{PLR}}} \right)\left( {PL{R_i}} \right)\\\,\,\,\,Error = \left( {{{\mathop Q\limits^ \bullet  }_{zone(i)}} - {{\mathop Q\limits^ \bullet  }_{coil(i),\,cooling,\,sensible}}} \right)/{\mathop Q\limits^ \bullet_{zone(i)}}\\End\,Iteration\,Loop -  -  -  -  -  -  -  -  -  -  -  -  -  -  -  - \end{array}$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{coil(i)\,,\,cooling\,,\,total}}\)</span>= zone terminal unit total (sensible + latent) cooling capacity, [W], report variable “Zone VRF Air Terminal Total Cooling Rate�
-
-<span>\({\mathop Q\limits^ \bullet_{coil(i),\,cooling,\,sensible}}\)</span>= zone terminal unit sensible cooling capacity [W], report variable “Zone VRF Air Terminal Sensible Cooling Rate�
-
-<span>\(PL{R_i}\)</span>= cooling coil sensible part-load ratio in zone *i*
-
-<span>\(SH{R_{PLR}}\)</span> = cooling coil sensible heat ratio (function of PLR, inlet air wet-bulb temperature, and cooling coil inlet air mass flow rate)
-
-<span>\({\mathop m\limits^ \bullet_{_i}}\)</span> = cooling coil inlet air mass flow rate [m<sup>3</sup>/s]
-
-The terminal unit total cooling (sensible + latent) capacity is then summed to provide the total terminal unit cooling requirement. The cooling coils capacity includes the impacts of fan heat and any outdoor air provided to the zone.
-
-<div>$${\mathop Q\limits^ \bullet_{cooling,TerminalUnits}} = \sum\limits_1^i {\left( {{{\mathop Q\limits^ \bullet  }_{coil(i),cooling,total}}} \right)\left( {PLR(i)} \right)} $$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{cooling,\,TerminalUnits\,}}\)</span>= total terminal unit cooling requirement (sensible + latent) in all zones, [W]
-
-The piping correction factor is then used to adjust the total zone cooling requirement to account for piping losses in the air conditioner’s refrigeration piping system.
-
-#### Cooling Piping Correction Factor in cooling mode
-
-The cooling piping correction factor is calculated using either one or two independent variables. Both the equivalent piping length and the combination ratio are used together to determine piping losses, or the equivalent piping length itself is used. The vertical height specified by the user is also added to the result calculated by either. If a single independent variable is used, a linear, quadratic, or cubic equation is used to determine the equivalent length correction factor. If two independent variables are used, a biquadratic equation is used to determine the equivalent length correction factor. The program will automatically use the correct equation based on the performance curve type. In either case, a single coefficient adjusts the piping correction factor based on the difference in height from the highest to lowest terminal unit. Coefficients a-d (e) in the following equation(s) are inputs in the piping correction factor for length in cooling mode performance curve object. Coefficient f is a direct input to the VRF model as the piping correction factor for height in cooling mode coefficient. The equivalent piping length in cooling mode (P<sub>EQ,cooling</sub>) is also a direct input in the VRF model. The cooling combination ratio (CR<sub>cooling</sub>) is automatically calculated by the program. The vertical height, the difference between the highest and lowest terminal unit (e.g., 12 m higher than condenser – 3 m lower than condenser = 9 m height), is a common input for both cooling and heating. When all terminal units are above or below the outdoor unit, an average positive or negative value is used. The limits on the calculated cooling piping correction factor are 0.5 &lt; P<sub>correction,cooling</sub> &lt; 1.
-
-<div>$$C{R_{cooling}} = {\raise0.7ex\hbox{${\sum\limits_1^n {{{\mathop Q\limits^ \bullet  }_{coil(i),cooling,rated}}} }$} \!\mathord{\left/ {\vphantom {{\sum\limits_1^n {{{\mathop Q\limits^ \bullet  }_{coil(i),cooling,rated}}} } {{{\mathop Q\limits^ \bullet  }_{cooling,total,rated}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{cooling,total,rated}}}$}}$$</div>
-
-<div>$${P_{correction,\,cooling}} = a + b\left( {{P_{EQ,\,cooling}}} \right) + c{\left( {{P_{EQ,\,cooling}}} \right)^2} + d{\left( {{P_{EQ,\,cooling}}} \right)^3} + f\left( {{P_H}} \right)$$</div>
-
-- or  -
-
-<div>$$\begin{array}{l}{P_{correction,\,cooling}} = a + b\left( {{P_{EQ,\,cooling}}} \right) + c{\left( {{P_{EQ,\,cooling}}} \right)^2} + d\left( {C{R_{cooling}}} \right) + e{\left( {C{R_{cooling}}} \right)^2}\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + f\left( {{P_{EQ,\,cooling}}} \right)\left( {C{R_{cooling}}} \right) + g\left( {{P_H}} \right)\end{array}$$</div>
-
-where
-
-<span>\({P_{\,correction,\,cooling}}\)</span> = Piping Correction Factor in Cooling Mode
-
-*a - f*       = equation coefficients for piping correction factor in cooling mode
-
-*g*              = user specified piping correction factor for height in cooling mode coefficient
-
-<span>\({P_{\,EQ,\,cooling}}\)</span> = user specified equivalent piping length in cooling mode [m]
-
-<span>\(C{R_{cooling}}\)</span> = combination ratio in cooling mode (total rated indoor terminal unit capacity divided by the rated condenser cooling capacity) (reported to eio file)
-
-<span>\({P_H}\)</span>           = user specified vertical height used for piping correction factor calculation [m]
-
-An example piping correction factor chart is shown in the following figure. The height selected for use in the equation above is selected to minimize the piping correction factor and serves to identify the worst case piping losses.
-
-![PipingFactorCorrectionChart](media/image5358.png)
-
-Figure 245. Typical Piping Factor Correction Chart
-
-The total demand on the heat pump condenser is then calculated as the quotient of the total terminal unit cooling capacity and the cooling piping correction factor. The piping losses are fixed throughout the simulation (i.e., these losses are not based on which terminal units are requesting refrigerant).
-
-<div>$${\mathop Q\limits^ \bullet_{cooling,\,total\,}} = {\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{cooling,\,TerminalUnits\,}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{cooling,\,TerminalUnits\,}}} {{P_{correction\,,\,cooling}}}}}\right.}\!\lower0.7ex\hbox{${{P_{correction\,,\,cooling}}}$}}$$</div>
-
-The heat pump’s total available cooling capacity is then calculated as:
-
-<div>$${\mathop Q\limits^ \bullet_{HP,\,cooling,\,\,total}} = {\mathop Q\limits^ \bullet_{cooling,\,\,total,\,\,rated}}\left( {CAPF{T_{HP,\,\,cooling}}} \right)\left( {C{R_{cooling,\,\,correction}}} \right)$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{cooling\,,\,total}}\)</span> = total heat pump condenser cooling load (W)
-
-<span>\({\mathop Q\limits^ \bullet_{HP,\,cooling,\,\,total}}\)</span> = heat pump total available cooling capacity (W)
-
-#### Heat Recovery Cooling Capacity Modifier
-
-When operating in heat recovery mode, the heat pump’s available cooling capacity is typically different than the available capacity when operating in cooling only mode. This modifier is used to adjust the available cooling capacity using a fraction when heat recovery is active. This fraction is based on a bi-quadratic equation with indoor and outdoor temperatures used as the independent terms.
-
-*HRCapMod* *<sub>HP,cooling</sub>* = <span>\(a + b\left( {T{}_{ent}} \right) + c{\left( {T{}_{ent}} \right)^2} + d\left( {{T_{cond}}} \right) + e{\left( {{T_{cond}}} \right)^2} + f\left( {T{}_{ent}} \right)\left( {{T_{cond}}} \right)\)</span>
-
-This equation can be used to provide a constant fractional difference for available cooling capacity in heat recovery mode (i.e., only *a* is non-zero) or a fractional term that varies with indoor and outdoor conditions. With very limited performance data available at this time, it is recommended that only the constant (a) term be used at this time. When the VRF system is not operating in heat recovery mode, this fraction is set to 1.The available cooling capacity in heat recovery mode is then:
-
-<div>$${\mathop Q\limits^ \bullet_{HR,cooling,\,total}} = {\mathop Q\limits^ \bullet_{HP,\,cooling,\,\,total}}\left( {HRCapMo{d_{HP,\,cooling}}} \right)$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{HR,cooling,\,total}}\)</span> = heat recovery total available cooling capacity (W)
-
-The figure below shows VRF system laboratory data for cooling only mode (solid characters) and heat recovery mode (dotted characters). Using the limited laboratory data, the available cooling capacity fraction used to model heat recovery mode is approximately 0.91 and the cooling energy fraction is approximately 1.14. This is the only data available at this time to estimate the impact of heat recovery mode on performance. In the bi-quadratic equation, only coefficient a should be used until more complete data sets exist. Laboratory testing will eventually provide more data and better estimates of performance in heat recovery mode.
-
-![](media/image5366.png)
-
-Figure 246.  Comparison of cooling only and heat recovery mode operation
-
-#### Transition from Cooling Only mode to Heat Recovery mode
-
-When the VRF system transitions from cooling only operation to heat recovery operation, this transition takes some finite amount of time. During the transition period the available cooling capacity can change significantly, The following figure illustrates the transition between cooling only mode and heat recovery mode. For this test, the VRF system was turned on and allowed to reach steady-state operation. Three of the four indoor terminal units were operating in cooling mode, When the fourth terminal unit was enabled in heating mode, the transition from cooling only mode to heat recovery mode took approximately 45 minutes. During this time, the available cooling is significantly reduced and recovers over time. When the system again reaches steady-state operation, the available cooling capacity and power consumption are markedly different. Although computer models do not typically simulate this type of transitional performance, efforts to model this aspect of performance were included in the VRF AC heat recovery model. The initial heat recovery cooling capacity fraction and heat recovery cooling capacity time constant are used to model this transition period. The initial heat recovery cooling capacity fraction identifies the fraction of available heat recovery mode cooling capacity at the start of the transition period, the heat recovery cooling capacity time constant identifies the time needed to recover to 99% of the steady-state value. This exponential model used for simulating the transition period can be turned off by setting the initial heat recovery cooling capacity fraction to 1.
-
-
-
-
-
-![](media/image5367.png)
-
-Figure 247.  Laboratory test identifies performance changes during transition period
-
-#### Heat Recovery Cooling Capacity Fraction and Time Constant
-
-When the heat pump changes operating modes (i.e., from cooling only to heat recovery mode), the transition does not happen immediately. There is a time delay, and a period of time where the available cooling capacity is well below the steady-state capacity available after the system has had time to adjust. When this type of transition is modeled, an exponential decay curve is used. At the start of the transition period, only a fraction (*k<sub>cool</sub>*) of the steady-state capacity in heat recovery mode is available. The remaining capacity is recovered over a period of 5 time constants (t<sub>c</sub>) and is modeled with the following equation. This equation was used to replicate both the cooling capacity and condenser power curves in the previous figure.
-
-<div>$${\mathop Q\limits^ \bullet_{HR,avail,\,cooling}} = {k_{cool}}\left( {{{\mathop Q\limits^ \bullet  }_{HR,cooling,\,total}}} \right) + \left( {1 - {k_{cool}}} \right)\left( {{{\mathop Q\limits^ \bullet  }_{HR,cooling,\,total}}} \right)\left( {1 - {e^{\left( {{\raise0.7ex\hbox{${ - t}$} \!\mathord{\left/ {\vphantom {{ - t} {{\tau_c}}}}\right.}\!\lower0.7ex\hbox{${{\tau_c}}$}}} \right)}}} \right)$$</div>
-
-where:
-
-*k<sub>cool</sub>* = fraction of steady-state capacity at beginning of heat recovery mode
-
-*t<sub>c</sub>* = time constant to reach steady-state operation, 5 time constants equals 99% of steady-state capacity (hr)
-
-*Q<sub>HR,avail,cooling</sub>* = available cooling capacity in heat recovery mode (W)
-
-*<span>\(\left( {1 - {e^{\left( {{\raise0.7ex\hbox{${ - t}$} \!\mathord{\left/ {\vphantom {{ - t} {{t_{c,cool}}}}}\right.}\!\lower0.7ex\hbox{${{t_{c,cool}}}$}}} \right)}}} \right)\)</span>*= The multiplier used during the transition period from cooling mode to heat recovery mode. This multiplier can be viewed using the report variable “VRF Heat Pump Heat Recovery Status Change Multiplier� (ref: object Output:Variable).
-
-
-
-The operating part-load ratio of the VRF system can then be calculated:
-
-<div>$$PLR = {\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{cooling,\,total}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{cooling,\,total}}} {{{\mathop Q\limits^ \bullet  }_{HR,\,avail,\,cooling}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{HR,\,avail,\,cooling}}}$}}$$</div>
-
-<span>\(PLR\)</span>         = heat pump part-load ratio, report variable “VRF Heat Pump Part Load Ratio�
-
-Note: for calculation purposes <span>\({\mathop Q\limits^ \bullet_{HR,\,avail,\,cooling}}\)</span> is equivalent to <span>\({\mathop Q\limits^ \bullet_{HR,\,cooling,\,total}}\)</span> when heat recovery mode is not active.
-
-The heat pump total available cooling capacity must be greater than or equal to the total cooling capacity requested by the zone terminal units. When the total operating capacity of all terminal unit’s will be greater than the available operating capacity of the heat pump condenser, one or more of the terminal unit’s operating capacity must be reduced to the point where the sum of the indoor terminal unit demand request plus piping losses is equal to the total available cooling capacity of the outdoor condenser. At this point, the part-load ratio of the heat pump condenser will be equal to 1.
-
-A maximum terminal unit cooling capacity limit is used to restrict the cooling capacity of each indoor terminal unit. The capacity limit is equivalent to a maximum allowed operating capacity for all zone terminal units. This limit is used to conserve energy between multiple indoor terminal units and a single outdoor condensing unit. Assuming no terminal unit can provide more capacity than can be delivered by the outdoor condenser, the terminal unit total cooling capacity calculation previously discussed is revised as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{coil(i),\,\,cooling}} = \sum\limits_1^i {MIN\left( {\left( {{{\mathop Q\limits^ \bullet  }_{coil(i),cooling,total}}} \right)\left( {PLR(i)} \right),\,\,CoolingCapacityLimit} \right)} $$</div>
-
-where:
-
-<span>\(CoolingCapacityLimit(C{L_{cooling}})\)</span>= Report variable (ref: Output:Variable) describing the “VRF Heat Pump Maximum Capacity Cooling Rate�, W
-
-When multiple terminal units are operating, the terminal units near their maximum capacity are more likely to be capacity limited than those terminal units operating well below their available capacity. The assumption here is that terminal units that are not capacity limited can provide more refrigerant to meet the same load. When the model finds that there is no terminal unit capacity limit, this variable will report 1E+20 indicating that no limit exists.  The figure below demonstrates the application of the capacity limit factor for the case where all indoor terminal units are operating at different capacities. A solution is reached when the sum of the indoor terminal unit’s cooling capacities (accounting for piping losses) is equal to the heat pump condenser’s available cooling capacity.
-
-![](media/image5376.png)
-
-Figure 248. Example of Cooling Capacity Limit
-
-When the heat pump’s part-load ratio is less than 1 (i.e., the total capacity of all terminal unit’s is less than the actual operating capacity of the heat pump condenser), the heat pump’s part-load ratio is compared to the minimum heat pump part-load ratio. If the heat pump’s part-load ratio is less than the minimum heat pump part-load ratio, the heat pump will cycle on and off to meet the cooling load. A correction factor is used to account for startup losses of the compression system.
-
-***Cooling Part-Load Fraction Correlation (function of cycling ratio)***
-
-The cooling part-load fraction correlation (function of heat pump cycling ratio) is a linear, quadratic or cubic curve with the independent variable being cycling ratio (part-load ratio / minimum part-load ratio). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the “effective� EIR for a given simulation time step.
-
-<div>$$CyclingRatioFrac = a + b\left( {CyclingRatio} \right) + c{\left( {CyclingRatio} \right)^2} + d{\left( {CyclingRatio} \right)^3}$$</div>
-
-where
-
-<div>$$CyclingRatio = {\raise0.7ex\hbox{${PLR}$} \!\mathord{\left/ {\vphantom {{PLR} {PL{R_{min}}}}}\right.}\!\lower0.7ex\hbox{${PL{R_{min}}}$}}$$</div>
-
-a-c (d) = coefficients for the quadratic (cubic) cycling ratio correlation curve equation
-
-The cycling ratio can be viewed using the report variable “VRF Heat Pump Cycling Ratio� (ref: Output:Variable).
-
-The cooling part-load ratio correlation should be normalized to a value of 1.0 when the cycling ratio equals 1.0 (i.e., no efficiency losses when the heat pump runs continuously [PLR ≥ PLR<sub>min</sub>] for the simulation time step). For cycling ratio values between 0 and 1 (0 &lt;= CyclingRatio &lt; 1), the following rules apply:
-
-      CyclingRatioFrac &gt;= 0.7   and   CyclingRatioFrac &gt;= CyclingRatio
-
-If CyclingRatioFrac &lt; 0.7 a warning message is issued, the program resets the CyclingRatioFrac value to 0.7, and the simulation proceeds. The runtime fraction of the heat pump is defined as CyclingRatio/CyclingRatioFrac. If CyclingRatioFrac &lt; CyclingRatio, the runtime fraction will exceed 1. In this case a warning message is issued and the runtime fraction of the heat pump is limited to 1.0.
-
-<div>$$Heat\,Pump\,Runtime\,Fraction\,(HPRTF) = {\raise0.7ex\hbox{${CyclingRatio}$} \!\mathord{\left/ {\vphantom {{CyclingRatio} {CyclingRatioFrac}}}\right.}\!\lower0.7ex\hbox{${CyclingRatioFrac}$}}$$</div>
-
-The heat pump runtime fraction can be viewed using the report variable “VRF Heat Pump Runtime Fraction� (ref: Output:Variable).
-
-Since manufacturers data do not typically provide information defining the cycling losses of VRF AC systems, a typical part-load fraction correlation for a conventional DX refrigeration system (e.g., residential or small commercial unit) may be substituted here as:
-
-      CyclingRatioFrac = 0.85 + 0.15(CyclingRatio)
-
-The electrical power consumed by the heat pump condenser is then calculated based on the heat pump’s rated electric power consumption (including condenser fan power), the actual operating conditions, and the cycling ratio of the refrigeration system. Performance correction factors are used here to correct for off-design performance as follows:
-
-#### Cooling Energy Input Ratio Modifier Function of Low Temperature
-
-As described previously (Ref. Application of Dual Performance Curves), the cooling energy input ratio modifier curve can either be applied as a single curve object as shown below, or applied using dual performance curve objects. The equation form used for a single or dual performance curve application is shown here.
-
-<div>$$EIRF{T_{\,cooling}} = a + b\left( {{T_{wb,avg}}} \right) + c{\left( {{T_{wb,avg}}} \right)^2} + d\left( {{T_c}} \right) + e{\left( {{T_c}} \right)^2} + f\left( {{T_{wb,avg}}} \right)\left( {{T_c}} \right)$$</div>
-
-where
-
-<span>\(EIRF{T_{\,cooling}}\)</span> = cooling energy input ratio modifier (function of temperature)
-
-#### Cooling Energy Input Ratio Modifier Function of Part-Load Ratio
-
-The cooling energy input ratio calculation is based on 2 EIR curves. One is used when the heat pump part-load ratio is less than or equal to 1, and a second curve is used to describe the variation of cooling energy input ratio when the part-load ratio is greater than 1. The part-load ratio curve when PLR&gt;1 is not a required input and when not used, the energy use is assumed to be constant when PLR &gt; 1.
-
-<div>$$\begin{array}{l}IF\left( {PLR \le 1} \right)THEN\\\,\,\,\,EIRFPL{R_{cooling}} = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2} + d{\left( {PLR} \right)^3}\\ELSE\\\,\,\,\,EIRFPL{R_{cooling}} = e + f\left( {PLR} \right) + g{\left( {PLR} \right)^2} + h{\left( {PLR} \right)^3}\end{array}$$</div>
-
-where
-
-<span>\(EIRFPL{R_{cooling}}\)</span> = cooling energy input ratio correction factor (function of part-load ratio)
-
-a-d = coefficient for cooling energy input ratio correlation when part-load ratio ≤ 1
-
-e-h = coefficient for cooling energy input ratio correlation when part-load ratio &gt; 1
-
-The total power consumed by the heat pump condenser in cooling mode is based on the user specified coefficient of performance (COP) and calculated as:
-
-<div>$$CoolingPower = \left( {\frac{{{{\mathop Q\limits^ \bullet  }_{cooling,total,rated}}CAPF{T_{cooling}}}}{{CO{P_{cooling,\,\,reference}}}}} \right)\left( {EIRF{T_{cooling}}} \right)\left( {EIRFPL{R_{cooling}}} \right)\left( {HPRTF} \right)$$</div>
-
-The cooling COP is then calculated as the ratio of the outdoor unit cooling capacity divided by the total electric consumption rate of all components associated with the outdoor unit. Although included in the equiation, defrost power is typically 0 during cooling mode operation.
-
-<div>$$CO{P_{cooling}} = {\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{cooling,total}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{cooling,total}}} {\left( {CoolingPower + {P_{CrankaseHeater}} + {P_{EvapCoolerPower}} + {P_{defrost}}} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {CoolingPower + {P_{CrankaseHeater}} + {P_{EvapCoolerPower}} + {P_{defrost}}} \right)}$}}$$</div>
-
-COP<sub>cooling</sub>        = operating coefficient of performance, report variable “VRF Heat Pump Cooling COP�
-
-CoolingPower = operating electric consumption rate, [W], report variable “VRF Heat Pump Cooling Electric Power�
-
-P<sub>CrankcaseHeater</sub> = report variable for electric consumption rate of crankcase heater (W)
-
-P<sub>EvapCoolerPump</sub> = report variable for electric consumption rate of evaporatively-cooled condenser water pump (W)
-
-<span>\({P_{defrost}}\)</span>         = report variable for average defrost power for the simulation time step (W)
-
-When operating in heat recovery mode, equations similar to those used for available cooling capacity are used to model heating electric consumption rate.
-
-*HREIRMod* *<sub>HP,cooling</sub>* = <span>\(a + b\left( {{T_{ent}}} \right) + c{\left( {{T_{ent}}} \right)^2} + d\left( {{T_{cond}}} \right) + e{\left( {{T_{cond}}} \right)^2} + f\left( {{T_{ent}}} \right)\left( {{T_{cond}}} \right)\)</span>
-
-This equation can be used to provide a constant fractional difference for cooling electric consumption rate in heat recovery mode (i.e., only *a* is non-zero) or a fractional term that varies with indoor and outdoor conditions. With very limited performance data available at this time, it is recommended that only the constant (a) term be used at this time. When the VRF system is not operating in heat recovery mode, this fraction is set to 1. The cooling electric consumption rate in heat recovery mode is then:
-
-
-
-<div>$$CoolingPowe{r_{HR}} = CoolingPower\left( {HREIRMo{d_{HP,\,cooling}}} \right)$$</div>
-
-<span>\(Powe{r_{HR}} = {k_{EIR,\,cool}}\left( {CoolingPowe{r_{HR}}} \right) + \left( {1 - {k_{EIR,\,cool}}} \right)\left( {CoolingPowe{r_{HR}}} \right)\left( {1 - {e^{\left( {{\raise0.7ex\hbox{${ - t}$} \!\mathord{\left/ {\vphantom {{ - t} {{\tau_{c,\,EIR,\,cool}}}}}\right.}\!\lower0.7ex\hbox{${{\tau_{c,\,EIR,\,cool}}}$}}} \right)}}} \right)\)</span>where:
-
-*k<sub>EIR,\\ copl</sub>* = fraction of steady-state cooling electric consumption rate at beginning of heat recovery mode
-
-*t<sub>c,EIR,\\ cool</sub>* = time constant to reach steady-state operation, 5 time constants equals 99% of steady-state capacity (hr)
-
-*CoolingPower<sub>HR</sub>* = cooling electric consumption rate in heat recovery mode (W)
-
-*<span>\(\left( {1 - {e^{\left( {{\raise0.7ex\hbox{${ - t}$} \!\mathord{\left/ {\vphantom {{ - t} {{\tau_{c,\,EIR,\,cool}}}}}\right.}\!\lower0.7ex\hbox{${{\tau_{c,\,cool}}}$}}} \right)}}} \right)\)</span>*= The multiplier used during the transition period from cooling mode to heat recovery mode. This multiplier can be viewed using the report variable “VRF Heat Pump Heat Recovery Status Change Multiplier� (ref: Output:Variable).
-
-#### Heating Operation
-
-Calculations of the heat pump’s heating performance is nearly identical to the calculations described above for cooling operation.
-
-The sum of the individual zone total heating requirements are used to calculate the performance of the outdoor condensing unit. The operating capacity of the indoor heating coils are calculated based on the indoor heating coil’s nominal heating capacity and the actual operating conditions. A capacity correction factor is used to correct for off-design performance as follows:
-
-***Heating Combination Ratio Correction Factor (function of capacity ratio)***
-
-The heating combination ratio correction factor is defined as the total terminal unit rated heating capacity divided by the heat pump’s rated heating capacity. In some instances, the cooling combination ratio may be used to define the correction factor used to modify the heat pump’s rated heating capacity and is manufacturer specific. The combination ratio is important when multiple terminal units (or DX coils) are attached to a single variable-speed condensing unit. If the combination ratio is less than 1, the condenser has sufficient capacity to meet the indoor terminal unit’s capacity request. However, if the combination ratio is determined to be greater than 1, the maximum heating capacity available from the heat pump’s condenser may be higher than the user specified rated heating capacity. The combination ratio capacity correction factor is based on a linear, quadratic or cubic curve and provides a multiplier &gt; 1 to correct for combination ratio’s greater than 1. For example, a combination ratio of 1.3 (130%) may result in a combination ratio capacity correction factor of 1.06 (outdoor condenser can actually provide 106% of rated capacity) . The heating combination ratio correction factor is applied to heating performance calculations. If the heating combination ratio correction curve name is not specified by the user, the heating combination ratio correction factor (CR <sub>heating,\\ correction</sub>) in the following equation is assumed to be equal to 1.
-
-<div>$$C{R_{heating}} = {\raise0.7ex\hbox{${\sum\limits_1^n {{{\mathop Q\limits^ \bullet  }_{coil(i),heating,rated}}} }$} \!\mathord{\left/ {\vphantom {{\sum\limits_1^n {{{\mathop Q\limits^ \bullet  }_{coil(i),heating,rated}}} } {{{\mathop Q\limits^ \bullet  }_{heating,total,rated}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{heating,total,rated}}}$}}$$</div>
-
-<div>$$C{R_{heating,correction}} = a + b\left( {C{R_{heating}}} \right) + c{\left( {C{R_{heating}}} \right)^2} + d{\left( {C{R_{heating}}} \right)^3}$$</div>
-
-<div>$$C{R_{\,heating\,,\,\,correction}} = MAX\left( {1.0\,\,,\,\,C{R_{\,heating\,,\,\,correction}}} \right)$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{coil(i)\,,\,heating\,,\,rated}}\)</span> = rated total heating capacity in zone *i* (W)
-
-<span>\({\mathop Q\limits^ \bullet_{heating,\,total\,,\,rated}}\)</span> = rated total heating capacity of heat pump (W)
-
-<span>\(C{R_{\,heating\,,\,\,correction}}\)</span> = Heating Combination Ratio capacity correction factor at rated conditions
-
-<span>\(a - d\)</span>        = cubic equation coefficients for heating combination ratio correction factor
-
-<span>\(C{R_{heating}}\)</span> = combination ratio in heating mode (total rated indoor terminal unit capacity divided by the rated condenser heating capacity) (reported to eio file)
-
-#### Heating Capacity Ratio Modifier (function of temperature)
-
-As described previously (Ref. Application of Dual Performance Curves), the heating capacity ratio modifier curve can either be applied as a single curve object as shown below, or applied using dual performance curve objects. The single curve object application is described here.
-
-The heat pump’s heating capacity ratio modifier (function of temperature) is determined by averaging the zone heating coil inlet air dry-bulb temperature for all operating heating coils. A zone load-weighted average is used when calculating the performance of the heat pump condenser. This weighted-average heating coil inlet air dry-bulb temperature and the outdoor condenser entering air wet-bulb temperature are then used to calculate the heat pump’s temperature correction factor in heating mode.
-
-Note that some manufacturers do not provide performance data as a function of outdoor wet-bulb temperature. In this case, substituting outdoor dry-bulb temperature is permitted and the Heating Performance Curve Outdoor Temperature Type input should be specified as DryBulbTemperature. This also means that performance curve coefficients for both capacity (CAPFT) and energy (EIRFT) should be calculated using indoor and outdoor dry-bulb temperature.
-
-<div>$${T_{db,avg}} = \sum\limits_1^i {\left( {{T_{db,i}}} \right)} \left( {{\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{zone(i)}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{zone(i)}}} {{{\mathop Q\limits^ \bullet  }_{zone,\,total}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{zone,\,total}}}$}}} \right)$$</div>
-
-<div>$$CAPF{T_{HP,heating}} = a + b\left( {{T_{db,avg}}} \right) + c{\left( {{T_{db,avg}}} \right)^2} + d\left( {{T_c}} \right) + e{\left( {{T_c}} \right)^2} + f\left( {{T_{db,avg}}} \right)\left( {{T_c}} \right)$$</div>
-
-<div>$$CAPF{T_{coil,heating}} = a + b\left( {{T_{db,i}}} \right) + c{\left( {{T_{db,i}}} \right)^2} + d\left( {{T_c}} \right) + e{\left( {{T_c}} \right)^2} + f\left( {{T_{db,i}}} \right)\left( {{T_c}} \right)$$</div>
-
-where
-
-<span>\({T_{db,i}}\)</span>= dry-bulb temperature of the air entering the heating coil in zone *i*, °C
-
-<span>\({T_{db,avg}}\)</span>= weighted-average dry-bulb temperature of the air entering all operating heating coils, °C
-
-<span>\(CAPF{T_{\,heating}}\)</span> = Heating Capacity Correction Factor (function of temperature)
-
-<span>\(a - f\)</span>  = bi-quadratic equation coefficients
-
-<span>\({T_c}\)</span>    = wet-bulb temperature of the air entering an air-cooled condenser, °C
-
-The total terminal unit heating capacity required is the simple sum of the terminal unit capacity. If the heat pump is off or there is no zone heating requirement, the terminal unit total heating requirement will be zero. The heating coils capacity includes the impacts of fan heat and any outdoor air provided to the zone.
-
-<div>$${\mathop Q\limits^ \bullet_{heating,TerminalUnits}} = \sum\limits_1^i {\left( {{{\mathop Q\limits^ \bullet  }_{coil(i),\,heating,total}}} \right)\left( {PLR(i)} \right)} $$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{heating\,,\,TerminalUnits\,}}\)</span>= heat pump’s outdoor condenser total zone heating requirement (W)
-
-<span>\({\mathop Q\limits^ \bullet_{coil(i),\,heating,\,total}}\)</span>= zone terminal unit total heating capacity [W], report variable “Zone VRF Air Terminal Total Heating Rate�
-
-The piping correction factor is then used to adjust the zone heating requirement to account for piping losses in the AC refrigeration system.
-
-#### Piping Correction Factor in heating mode
-
-The piping correction factor in heating mode is calculated based on the length of the farthest terminal unit and the difference in height from the highest to lowest terminal unit. The piping losses are fixed throughout the simulation (i.e., these losses are not based on which terminal units are requesting refrigerant). Coefficients a-f in the following equations are inputs in the piping correction factor for length in heating mode curve object. The curve may use either one or two independent variables. Coefficient g is a direct input to the VRF model as piping correction factor for height in heating mode coefficient. The equivalent piping length in heating mode (P<sub>EQ,heating</sub>) is also a direct input in the VRF model. The vertical height (P<sub>H</sub>), the difference between the highest and lowest terminal unit (e.g., 12 m higher than condenser – 3 m lower than condenser = 9 m height), is a common input for both cooling and heating.
-
-<div>$${P_{correction,\,heating}} = a + b\left( {{P_{EQ,\,heating}}} \right) + c{\left( {{P_{EQ,\,heating}}} \right)^2} + d{\left( {{P_{EQ,\,heating}}} \right)^3} + g\left( {{P_H}} \right)$$</div>
-
-- or -
-
-<div>$$\begin{array}{l}{P_{correction,\,heating}} = a + b\left( {{P_{EQ,\,heating}}} \right) + c{\left( {{P_{EQ,\,heating}}} \right)^2} + d\left( {C{R_{heating}}} \right) + e{\left( {C{R_{heating}}} \right)^2}\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + f\left( {{P_{EQ,\,heating}}} \right)\left( {C{R_{heating}}} \right) + g\left( {{P_H}} \right)\end{array}$$</div>
-
-where
-
-<span>\({P_{correction,\,heating}}\)</span> = Piping Correction Factor in Heating Mode
-
-*a-f* = equation coefficients for piping correction factor in heating mode
-
-*g  * = user specified piping correction factor for height in heating mode coefficient
-
-<span>\({P_{EQ,\,heating}}\)</span>= the equivalent piping length for heating specified by the user [m]
-
-<span>\({P_H}\)</span>          = user specified vertical height used for piping correction factor [m]
-
-The heat pump’s total available heating capacity is then determined using the previously described modifiers.
-
-<div>$${\dot Q_{HP,cooling,total}} = {\dot Q_{cooling,total,rated}}\left( {CAPF{T_{HP,cooling}}} \right)\left( {C{R_{cooling,correction}}} \right)$$</div>
-
-#### Heat Recovery Heating Capacity Modifier
-
-When operating in heat recovery mode, the heat pump’s available heating capacity is typically different than the available capacity when operating in heating only mode. This modifier is used to adjust the available heating capacity using a fraction when heat recovery is active. This fraction is based on a bi-quadratic equation with indoor and outdoor temperatures used as the independent terms.
-
-*HRCapMod* *<sub>HP,heating</sub>* = <span>\(a + b\left( {{T_{ent}}} \right) + c{\left( {{T_{ent}}} \right)^2} + d\left( {{T_{cond}}} \right) + e{\left( {{T_{cond}}} \right)^2} + f\left( {{T_{ent}}} \right)\left( {{T_{cond}}} \right)\)</span>
-
-This equation can be used to provide a constant fractional difference for available heating capacity in heat recovery mode (i.e., only *a* is non-zero) or a fractional term that varies with indoor and outdoor conditions. With very limited performance data available at this time, it is recommended that only the constant (a) term be used at this time. The available heating capacity in heat recovery mode is then:
-
-<div>$${\mathop Q\limits^ \bullet_{HR,heating,\,total}} = {\mathop Q\limits^ \bullet_{HP,\,heating,\,\,total}}\left( {HRCapMo{d_{HP,\,heating}}} \right)$$</div>
-
-#### Transition from Heating Only mode to Heat Recovery mode
-
-When the VRF system transitions from heating only operation to heat recovery operation, this transition takes some finite amount of time. During the transition period the available heating capacity can change significantly, As described for the transition from cooling only operating to heat recovery mode, the initial heat recovery heating capacity fraction and heat recovery heating capacity time constant are used to model the transition from heating only mode to heat recovery mode. The initial heat recovery heating capacity fraction identifies the fraction of available heat recovery mode heating capacity at the start of the transition period, the heat recovery heating capacity time constant identifies the time needed to recover to 99% of the steady-state value. This exponential model used for modeling the transition period can be turned off by setting the initial heat recovery heating capacity fraction to 1.0.
-
-#### Heat Recovery Heating Capacity Fraction and Time Constant
-
-When the heat pump changes operating modes (i.e., from heating only to heat recovery mode), the transition does not happen immediately. There is a time delay, and a period of time where the available heating capacity is different from the steady-state capacity available after the system has had time to adjust. When this type of transition is modeled, an exponential decay curve is used. At the start of the transition period, only a fraction (*k<sub>heat</sub>*) of the steady-state capacity in heat recovery mode is available. The remaining capacity is recovered over a period of 5 time constants (t<sub>c,\\ heat</sub>) and is modeled with the following equation. This equation was used to replicate both the cooling capacity and condenser power curves in the previous figure.
-
-<div>$${\mathop Q\limits^ \bullet_{HR,\,avail,\,heating}} = {k_{heat}}\left( {{{\mathop Q\limits^ \bullet  }_{HR,\,heating,\,\,total}}} \right) + \left( {1 - {k_{heat}}} \right)\left( {{{\mathop Q\limits^ \bullet  }_{HR,\,heating,\,\,total}}} \right)\left( {1 - {e^{\left( {{\raise0.7ex\hbox{${ - t}$} \!\mathord{\left/ {\vphantom {{ - t} {{\tau_{c,\,heat}}}}}\right.}\!\lower0.7ex\hbox{${{\tau_{c,\,heat}}}$}}} \right)}}} \right)$$</div>
-
-where:
-
-*k<sub>heat</sub>*= fraction of steady-state heating capacity at beginning of heat recovery mode
-
-*t<sub>c,\\ heat</sub>* = time constant to reach steady-state operation, 5 time constants equals 99% of steady-state capacity (hr)
-
-*Q<sub>HR,avail,heating</sub>* = available heating capacity in heat recovery mode (W)
-
-*<span>\(\left( {1 - {e^{\left( {{\raise0.7ex\hbox{${ - t}$} \!\mathord{\left/ {\vphantom {{ - t} {{t_{c,heat}}}}}\right.}\!\lower0.7ex\hbox{${{t_{c,heat}}}$}}} \right)}}} \right)\)</span>*= The multiplier used during the transition period from heating mode to heat recovery mode. This multiplier can be viewed using the report variable “VRF Heat Pump Heat Recovery Status Change Multiplier� (ref: Output:Variable).
-
-#### Defrost Energy Input Ratio Modifier (function of temperature)
-
-The defrost energy input ratio (EIR) modifier curve (function of temperature) is a bi-quadratic curve with two independent variables: heating coil average entering air wet-bulb temperature and outdoor air dry-bulb temperature. The output of this curve is multiplied by the heating coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the coil is operating. The use of outdoor wet-bulb temperature is explicit in this curve object and the defrost equation below and is independent of the selection for Heating Performance Curve Outdoor Temperature Type.
-
-<div>$$DefrostEIRTempModFac = a + b\left( {{T_{wb,avg}}} \right) + c{\left( {{T_{wb,avg}}} \right)^2} + d\left( {{T_c}} \right) + e{\left( {{T_c}} \right)^2} + f\left( {{T_{wb,avg}}} \right)\left( {{T_c}} \right)$$</div>
-
-The heat pump condenser’s total heating load is then calculated as the quotient of the total terminal unit capacity and the piping correction factor. Additional load due to defrost is also included (see following section).
-
-<div>$${\mathop Q\limits^ \bullet_{heating,\,total}} = \left( {{\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{heating,\,TerminalUnits}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{heating,\,TerminalUnits}}} {{P_{correction,\,heating}}}}}\right.}\!\lower0.7ex\hbox{${{P_{correction,\,heating}}}$}}} \right) + {\mathop Q\limits^ \bullet_{defrost}}$$</div>
-
-The heat pump’s total (gross) heating capacity is then calculated based on the capacity correction factor as a function of temperatures. The impact of defrost on total heat pump heating capacity is also accounted for (see following section). The part-load ratio of the heat pump condenser can then be calculated.
-
-<div>$${\mathop Q\limits^ \bullet_{HP\,,\,total}} = {\mathop Q\limits^ \bullet_{total,\,\,rated}}\left( {CAPF{T_{\,HP,\,heating}}} \right)\left( {C{R_{heating,\,\,correction}}} \right)\left( {HCA{P_{defrost}}} \right)$$</div>
-
-<div>$$PLR = {\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{heating,\,total\,}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{heating,\,total\,}}} {{{\mathop Q\limits^ \bullet  }_{HP\,,\,total}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{HP\,,\,total}}}$}}$$</div>
-
-where
-
-<span>\({\mathop Q\limits^ \bullet_{HP\,,\,total}}\)</span> = heat pump total available heating capacity (W)
-
-<span>\(PLR\)</span>     = heat pump part-load ratio
-
-<span>\(HCA{P_{defrost}}\)</span>= heating capacity correction factor for defrost mode
-
-As described for cooling operation, the available heating capacity of the heat pump is compared to the requested heating capacity of all indoor terminal units. If the requested heating capacity of all indoor terminal units is greater than the available heating capacity of the heat pump, one or more of the indoor terminal unit’s capacity is limited such that the sum of the zone terminal unit heating demand plus piping losses is equal to the available heat pump heating capacity (including the impact due to defrost).
-
-The electrical power consumed by the heat pump condenser is calculated based on the heat pump’s nominal electric power consumption in heating mode and the actual operating conditions. A performance correction factor is used to correct for off-design performance as follows:
-
-Heating Part-Load Fraction Correlation (function of heat pump cycling ratio)
-
-The part-load fraction correlation (function of heat pump cycling ratio) is a linear, quadratic or a cubic curve with the independent variable being cycling ratio (part-load ratio / minimum part-load ratio). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the “effective� EIR for a given simulation time step. The cycling ratio correlation accounts for startup losses of the heat pump’s compression system.
-
-<div>$$CyclingRatioFrac = a + b\left( {CyclingRatio} \right) + c{\left( {CyclingRatio} \right)^2}$$</div>
-
-or
-
-<div>$$CyclingRatioFrac = a + b\left( {CyclingRatio} \right) + c{\left( {CyclingRatio} \right)^2} + d{\left( {CyclingRatio} \right)^3}$$</div>
-
-where
-
-<div>$$CyclingRatio = {\raise0.7ex\hbox{${PLR}$} \!\mathord{\left/ {\vphantom {{PLR} {PL{R_{\min }}}}}\right.}\!\lower0.7ex\hbox{${PL{R_{\min }}}$}}$$</div>
-
-The cycling ratio can be viewed using the report variable “VRF Heat Pump Cycling Ratio� (ref: Output:Variable).
-
-The cycling ratio correlation should be normalized to a value of 1.0 when the cycling ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation time step). For cycling ratio values between 0 and 1 (0 &lt;= CyclingRatio &lt; 1), the following rules apply:
-
-      CyclingRatioFrac &gt;= 0.7   and   CyclingRatioFrac &gt;= CyclingRatio
-
-If CyclingRatioFrac &lt; 0.7 a warning message is issued, the program resets the CyclingRatioFrac value to 0.7, and the simulation proceeds. The runtime fraction of the heat pump is defined as CyclingRatio/CyclingRatioFrac. If CyclingRatioFrac &lt; CyclingRatio, then a warning message is issued and the runtime fraction of the heat pump is limited to 1.0.
-
-<div>$$Heat\,Pump\,Runtime\,Fraction\left( {HPRTF} \right) = {\raise0.7ex\hbox{${CyclingRatio}$} \!\mathord{\left/ {\vphantom {{CyclingRatio} {CyclingRatioFrac}}}\right.}\!\lower0.7ex\hbox{${CyclingRatioFrac}$}}$$</div>
-
-The heat pump runtime fraction can be viewed using the report variable “VRF Heat Pump Runtime Fraction� (ref: Output:Variable).
-
-Since manufacturers data do not typically provide information defining the cycling losses of VRF AC systems, a typical part-load fraction correlation for a conventional DX refrigeration system (e.g., residential or small commercial unit) may be substituted here as:
-
-      CyclingRatioFrac = 0.85 + 0.15(CyclingRatio)
-
-Heating Energy Input Ratio Modifier (function of temperature)
-
-As described previously (Ref. Application of Dual Performance Curves), the heating energy input ratio modifier curve can either be applied as a single curve object as shown below, or applied using dual performance curve objects. The single curve object application is discussed here.
-
-<div>$$EIRF{T_{\,heating}} = a + b\left( {{T_{db,avg}}} \right) + c{\left( {{T_{db,avg}}} \right)^2} + d\left( {{T_c}} \right) + e{\left( {{T_c}} \right)^2} + f\left( {{T_{db,avg}}} \right)\left( {{T_c}} \right)$$</div>
-
-where
-
-<span>\(EIRF{T_{\,heating}}\)</span> = heating energy input ratio correction factor (function of temperature) (0-1)
-
-Heating Energy Input Ratio Modifier (function of part-load ratio)
-
-<div>$$\begin{array}{l}IF\left( {PLR \le 1} \right)THEN\\\,\,\,\,EIRFPL{R_{heating}} = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2} + d{\left( {PLR} \right)^3}\\ELSE\\\,\,\,\,EIRFPL{R_{heating}} = e + f\left( {PLR} \right) + g{\left( {PLR} \right)^2} + h{\left( {PLR} \right)^3}\end{array}$$</div>
-
-where
-
-<span>\(EIRFPL{R_{heating}}\)</span> = heating energy input ratio modifier (function of part-load ratio)
-
-a-d = coefficient for heating energy input ratio modifier when part-load ratio ≤ 1
-
-e-h = coefficient for heating energy input ratio modifier when part-load ratio &gt; 1
-
-The total power consumed by the heat pump condenser in heating mode is then calculated. A correction for power consumed due to defrost is also included (see following section).
-
-The total power consumed by the heat pump condenser in heating mode is based on the user specified coefficient of performance (COP). A correction for power consumed due to defrost is also included (see following section).
-
-<div>$$HeatingPower = \left( {\frac{{{{\mathop Q\limits^ \bullet  }_{heating,\,total,rated}}CAPF{T_{heating}}}}{{CO{P_{heating,reference}}}}} \right)\left( {EIRF{T_{heating}}} \right)\left( {EIRFPL{R_{heating}}} \right)\left( {HPRTF} \right)\left( {EI{R_{defrost}}} \right)$$</div>
-
-The operating COP is then calculated as:
-
-The heating COP is then calculated as the ratio of the outdoor unit heating capacity divided by the total electric consumption rate of all components associated with the outdoor unit. Evaporatively-cooled condenser pump power is typically 0 during heating mode operation.<span>\(CO{P_{heating}} = {\raise0.7ex\hbox{${{{\mathop Q\limits^ \bullet  }_{heating,total}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop Q\limits^ \bullet  }_{heating,total}}} {\left( {HeatingPower + {P_{CrankaseHeater}} + {P_{EvapCoolerPower}} + {P_{defrost}}} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {HeatingPower + {P_{CrankaseHeater}} + {P_{EvapCoolerPower}} + {P_{defrost}}} \right)}$}}\)</span>
-
-COP<sub>heating</sub>        = operating coefficient of performance, report variable “VRF Heat Pump Heating COP�
-
-HeatingPower = operating electric consumption rate, [W], report variable “VRF Heat Pump Heating Electric Power�
-
-When operating in heat recovery mode, equations similar to those used for available heating capacity are used to model operating power.
-
-*HREIRMod* *<sub>HP,heating</sub>* = <span>\(a + b\left( {{T_{ent}}} \right) + c{\left( {{T_{ent}}} \right)^2} + d\left( {{T_{cond}}} \right) + e{\left( {{T_{cond}}} \right)^2} + f\left( {{T_{ent}}} \right)\left( {{T_{cond}}} \right)\)</span>
-
-This equation can be used to provide a constant fractional difference for heating electric consumption rate in heat recovery mode (i.e., only *a* is non-zero) or a fractional term that varies with indoor and outdoor conditions. With very limited performance data available at this time, it is recommended that only the constant (a) term be used at this time. When the VRF system is not operating in heat recovery mode, this fraction is set to 1.The available heating electric consumption rate in heat recovery mode is then calculated as:
-
-<div>$$HeatingPowe{r_{HR}} = HeatingPower\left( {HREIRMo{d_{HP,\,heating}}} \right)$$</div>
-
-<div>$$Powe{r_{HR}} = {k_{EIR,\,heat}}\left( {HeatingPowe{r_{HR}}} \right) + \left( {1 - {k_{EIR,\,heat}}} \right)\left( {HeatingPowe{r_{HR}}} \right)\left( {1 - {e^{\left( {{\raise0.7ex\hbox{${ - t}$} \!\mathord{\left/ {\vphantom {{ - t} {{\tau_{c,\,EIR,\,heat}}}}}\right.}\!\lower0.7ex\hbox{${{\tau_{c,\,EIR,\,heat}}}$}}} \right)}}} \right)$$</div>
-
-where:
-
-*k<sub>EIR,\\ heat</sub>* = fraction of steady-state heating electric consumption rate at beginning of heat recovery mode
-
-*t<sub>c,EIR,\\ heat</sub>* = time constant to reach steady-state operation, 5 time constants equals 99% of steady-state capacity (hr)
-
-*HeatingPower<sub>HR</sub>* = heating electric consumption rate in heat recovery mode (W)
-
-*<span>\(\left( {1 - {e^{\left( {{\raise0.7ex\hbox{${ - t}$} \!\mathord{\left/ {\vphantom {{ - t} {{\tau_{c,\,EIR,\,heat}}}}}\right.}\!\lower0.7ex\hbox{${{\tau_{c,\,EIR,\,heat}}}$}}} \right)}}} \right)\)</span>*= The multiplier used during the transition period from heating mode to heat recovery mode. This multiplier can be viewed using the report variable “VRF Heat Pump Heat Recovery Status Change Multiplier� (ref: Output:Variable).
-
-#### Operating Coefficient of Performance
-
-Similar to the cooling and heating COP report variables, a report variable is included to identify the overall COP of the system. The numerator represents the total cooling and heating coil capacities (or loads) where piping losses have been accounted for. If heat recovery is not used only one of these terms is non-zero. When heat recovery is used, one or both of these terms can be non-zero, therefore, the operating COP includes recovered energy. The denominator includes the electric consumption rates of all system components. For water-cooled VRF AC systems, the plant pump power is not included.
-
-<div>$$CO{P_{operating}} = \frac{{\left( {{{\mathop Q\limits^ \bullet  }_{cooling,TerminalUnits}} + {{\mathop Q\limits^ \bullet  }_{heating,TerminalUnits}}} \right)}}{{\left( {OutdoorUnitPower + {P_{CrankaseHeater}} + {P_{EvapCoolerPower}} + {P_{defrost}} + {P_{TU,fan}} + {P_{TU,parasitic}}} \right)}}$$</div>
-
-where:
-
-OutdoorUnitPower = Cooling or heating electric consumption rate of outdoor unit (W)
-
-P<sub>TU,fan</sub> = electric consumption rate of all terminal unit fans (W)
-
-P<sub>TU,parasitic</sub> = electric consumption rate of all terminal unit parasitic electric (W)
-
-
-
-#### Defrost Adjustment Factors
-
-Frost formation on the outdoor coil, and the need to periodically defrost this coil, has a significant impact on heating capacity and energy use by the DX heating system. This model uses a timed reverse-cycle defrost model. If the outdoor air dry-bulb temperature is below the specified maximum temperature for defrost operation, then the model calculates adjustment factors for heating capacity and input power due to frost formation This method of accounting for the impacts of frosting/defrost was taken from the model used in DOE-2.1E (ESTSC 2001, Miller and Jaster 1985).
-
-The model first estimates the outdoor coil temperature according to a linear empirical relationship with outdoor air dry-bulb temperature as the independent variable.
-
-<div>$${T_{coil,out}} = 0.82{T_{db,o}} - 8.589$$</div>
-
-The difference between the outdoor air humidity ratio (from the weather file) and the saturated air humidity ratio at the estimated outdoor coil temperature is then calculated, and this value is used as an indication of frost formation on the outdoor coil.
-
-<div>$$\Delta {\omega_{coil,out}} = MAX\left[ {1.0E - 6,{\omega_{outdoor}} - {\omega_{sat}}\left( {{T_{coil,out}},OutBaroPress} \right)} \right]$$</div>
-
-Frost formation on the outdoor coil must be periodically removed. The fraction of compressor runtime when the coil is being defrosted is entered by the user. Adjustment factors to total heating coil capacity and input power due to frost formation on the outdoor coil are calculated by an empirical model with <span>\(\Delta {\omega_{coil,out}}\)</span> as the independent variable as shown below.
-
-<div>$$HCA{P_{defrost}} = 0.909 - 107.33\left( {\Delta {w_{coil\,,\,out}}} \right)$$</div>
-
-<div>$$EI{R_{defrost}} = 0.9 - 36.45\left( {\Delta {w_{coil\,,\,out}}} \right)$$</div>
-
-If the outdoor air dry-bulb temperature is above the specified maximum temperature for defrost operation, the fractional defrost time period is set to zero and the heating capacity/input power multipliers are set to unity (1).
-
-#### Defrost Operation
-
-If the fractional defrost time period is greater than zero for the simulation time step, then the model calculates the electrical power used during defrost. The additional heating load due to defrost (indoor cooling during defrost) is also calculated so that it may be added to the existing heating load when calculating input power for the compressor(s) and outdoor coil fan(s).
-
-<div>$${Q_{defrost}} = 0.01\left( {{t_{frac,defrost}}} \right)\left( {7.222 - {T_{db,o}}} \right)\left( {\frac{{{Q_{total,rated}}}}{{1.01667}}} \right)$$</div>
-
-<div>$${P_{defrost}} = DefrostEIRTempModFac\left( {\frac{{{Q_{total,rated}}}}{{1.01667}}} \right)\left( {{t_{frac,defrost}}} \right)\left( {RTF} \right)$$</div>
-
-where:
-
-<span>\({Q_{defrost}}\)</span>        = additional indoor heating load due to reverse-cycle defrost (*W*)
-
-<span>\({{Q_{total,rated}}}\)</span>= total full-load heating capacity of the coil at rated conditions (W)
-
-<span>\({P_{defrost}}\)</span>         = report variable for average defrost power for the simulation time step (W)
-
-*DefrostEIRTempModFac* = energy input ratio modifier curve applicable during defrost
-
-<span>\({t_{frac\,,\,defrost}}\)</span>= defrost time period fraction specified by user
-
-<div>$$RTF = \left( {{\raise0.7ex\hbox{${PLR}$} \!\mathord{\left/ {\vphantom {{PLR} {PartLoadFrac}}}\right.}\!\lower0.7ex\hbox{${PartLoadFrac}$}}} \right) = runtime\;fraction\;of\;the\;heating\;coil$$</div>
-
-
-### Variable Refrigerant Flow Heat Pump Model (Physics Based Model)
-
-#### Overview
-
-This section describes the Physics based VRF Model (VRF-FluidTCtrl) to simulate the energy performance of Variable Refrigerant Flow (VRF) systems in the heat pump (HP) operation mode (either cooling or heating is provided but not simultaneously). 
-
-Compared with the VRF-SysCurve model, VRF-FluidTCtrl model is more physics-based and thus able to consider the dynamics of more operational parameters which is essential for the description of many enhanced control logics (e.g., the adjustment of superheating degrees during small load operations). Furthermore, this model implements component-level curves rather than the system-level curves, and thus requires much fewer curves as model inputs. The definition of VRF performance data for simulation as part of ASHRAE Standard 205 will ensure VRF manufacturers provide adequate data to create the required performance curves.
-
-The main features of the VRF-FluidTCtrl model include:
-
- * Introduction of separate curves for capacities and power inputs of indoor and outdoor units instead of overall curves for the entire system.
-
- * Allowing of variable evaporating and condensing temperatures in the indoor and outdoor units under various operational conditions.
-
- * Allowing of variable fan speed based on the temperature and zone load in the indoor unit.
-
- * Allowing of further modifications of operational parameters (e.g., evaporating temperature, superheating degrees, and supply air flow rate) during low load conditions.
-
- * Development of a physics-based model to calculate thermal loss in the refrigerant piping network (varies with refrigerant flow rate, operational conditions, pipe length, and pipe and insulation materials) instead of a constant correction factor.
-
-These features enhance the simulation accuracy of the VRF system performance in both heating and cooling modes, especially during low load operations. In addition, these features enable the modeling of a multi-stage control strategy to adjust the system capacity during low load conditions, as shown in Figure VRF-FluidTCtrl-1. Further more, the VRF-FluidTCtrl model enables the potential simulation of demand response of VRF systems by directly slowing down the speed of compressors in the outdoor units with invertor technology.
-
-![](media/VRF-FluidTCtrl-1a.png)
-
-Figure VRF-FluidTCtrl-1a. Multi-stage control strategy to adjust the system capacity during low load conditions
-
-Note that a number of calculation steps are coupled together in the VRF-FluidTCtrl model, for instance, the piping loss calculation and the system performance calculation. More specifically, the piping loss changes the operating conditions of the system, which may lead to a different control strategy and thus in reverse affect the amount of piping loss. This makes it difficult to obtain an analytical solution for a number of operational parameters (e.g., enthalpy of refrigerant entering the indoor unit), and therefore numerical iterations are employed to address this problem (refer to Figure VRF-FluidTCtrl-3 for more details). Therefore, the VRF-FluidTCtrl model can have a longer execution time to perform the simulation than the VRF-SysCurve model. 
-
-The object connections for VRF-FluidTCtrl model is similar to those for VRF-SysCurve model. The difference lies in the object used to describe a specific components. For example, VRF-SysCurve model uses  *AirConditioner:VariableRefrigerantFlow* object to describe the VRF outdoor unit performance, while in VRF-FluidTCtrl model the *AirConditioner:VariableRefrigerantFlow* object is used.
-
-![](media/VRF-FluidTCtrl-1b.png)
-
-Figure VRF-FluidTCtrl-1b. Energyplus object connections for VRF-FluidTCtrl model 
-
-
-#### Model Description
-
-Figures VRF-FluidTCtrl-2 and VRF-FluidTCtrl-3 illustrate the overall logic of the VRF-FluidTCtrl algorithms. Detailed calculation procedures and explanations of equations are described in the following sections.
-
-![](media/VRF-FluidTCtrl-2a.png)
-
-*(a)	Heating Mode*
-
-![](media/VRF-FluidTCtrl-2b.png)
-
-*(b)	Cooling Mode*
-
-Figure VRF-FluidTCtrl-2. Schematic Pressure-Enthalpy Diagram for VRF Operation 
-
-![](media/VRF-FluidTCtrl-3a.png)
-
-*(a)	Heating Mode*
-
-![](media/VRF-FluidTCtrl-3b.png)
-
-*(b)	Cooling Mode*
-
-Figure VRF-FluidTCtrl-3. Flow Chart of the VRF-FluidTCtrl Model 
-
-The VRF-FluidTCtrl algorithms are described in details below, including the models of both the indoor and outdoor unit(s) of the VRF system. Because of the different control algorithms used in the outdoor unit for cooling and heating modes, the heating and cooling modes are described separately.
-
-#### *Modeling of the indoor unit (I/U) - Part I*
-
-##### Step 1.1: Obtaining zonal load/condition information
-
-Obtain the following information for each zone from the zone modules within EnergyPlus: 
-
-* zone sensible loads <span>$Q_{in, sensible}$</span>
-
-* zone total loads <span>$Q_{in, total}$</span>
-
-* indoor air temperature <span>$T_{in}$</span>
-
-* indoor air humidity ratio <span>$W_{in}$</span>
-
-The operation mode of the VRF system can therefore be determined from <span>$Q_{in, sensible}$</span>.
-
-##### Step 1.2: Calculate I/U required evaporator/condenser temperature
-
-Evaluate the required coil surface air temperature <span>$T_{fs}$</span> and the required evaporator/condenser refrigerant temperature <span>$T_{e,req}/{T_{c,req}}$</span> for each indoor unit. 
-
-Assuming the coil air flow rate is at the maximum (<span>$G_{a,rate}$</span>), the entering air temperature after the indoor coil fan can be calculated for each indoor unit:
-
-<div>$$T_{coil,in}=T_{in}+Q_{fan}/(G_{a,rate}\times{c_p}\times\rho_{in})$$</div>
-
-Where
-
-<span>$c_p$</span>	air heat capacity (kJ/(kg<span>$\cdot$</span>K))
-
-<span>$G_{a,rate}$</span>	volumetric flow rate of the air through the indoor unit, at the rated conditions (m<sup>3</sup>/s)
-
-<span>$Q_{fan}$</span>	sensible heat released by fan (W)
-
-<span>$T_{coil,in}$</span>	temperature of air entering the indoor coil (°C)
-
-<span>$\rho_{in}$</span>  	density of indoor air, <span>$f_{\rho}(T_{in},W_{in})$</span>  (kg/m<sup>3</sup>)
-
-The supply air temperature <span>$T_{out}$</span> can be calculated by:
-
-<div>$$T_{out}=T_{coil,in}-Q_{in, sensible}/(G_{a,rate}\times{c_p}\times\rho_{in})$$</div>
-
-Where
-
-<span>$T_{out}$</span>	temperature of the air leaving the indoor unit (supply air) (°C)
-
-The coil surface air temperature <span>$T_{fs}$</span> can be calculated, given the bypass factor <span>$BF$</span>:
-
-<div>$$T_{fs}= T_{coil,in}-(T_{coil,in}-T_{out})/(1-BF)$$</div>
-
-Where
-
-<span>$BF$</span>	bypass factor (different values for cooling mode and heating mode) 
-
-<span>$T_{fs}$</span>	indoor unit coil surface air temperature (°C)
-
-In the cooling mode, the superheating degree <span>$SH$</span> is given and thus the required evaporating temperature <span>$Te_{req}$</span> for the associated indoor unit can be obtained:
-
-<div>$$Te_{req}=T_{fs}-[A_c\cdot SH^2+B_c\cdot SH+C_c]$$</div>
- 
-Where
-
-<span>$A_c$</span>, <span>$B_c$</span>, <span>$C_c$</span>   	coefficients (°C)
-
-<span>$SH$</span> 		superheating degrees for the indoor unit (°C) 
-
-<span>$SH_{ref}$</span> 		reference superheating degrees for the indoor unit (e.g., 3) (°C)
-
-<span>$Te_{req}$</span>		required evaporating temperature for a specific indoor unit (°C)
-
-In the heating mode, the subcooling degree <span>$SC$</span> is given and thus the required condensing temperature <span>$Tc_{req}$</span> for the associated indoor unit can be obtained:
-
-<div>$$Tc_{req}=T_{fs}+[A_h\cdot SC^2+B_h\cdot SC+C_h]$$</div>
- 
-Where
-
-<span>$A_h$</span>, <span>$B_h$</span>, <span>$C_h$</span>  	coefficients (°C)
-
-<span>$SC$</span> 		subcooling degrees for the indoor unit (°C) 
-
-<span>$SC_{ref}$</span> 		reference subcooling degrees for the indoor unit (e.g., 5) (°C)
-
-<span>$Tc_{req}$</span>		required condensing temperature for a specific indoor unit (°C)
-
-##### Step 1.3: Calculate effective evaporating /condensing temperature
-
-There are two refrigerant temperature control strategies for the indoor unit: (1) *ConstantTemp*, (2) *VariableTemp*.
-
- - In the *ConstantTemp* strategy, <span>$T_e$</span> and <span>$T_c$</span> are kept at constant values provided by the user.
-
- - In the *VariableTemp* strategy, <span>$T_e$</span> and <span>$T_c$</span> are determined using the equations below:
-
-In the cooling mode:
-
-<div>$$Te=min\{max[min(Te_{req,i}),Te_{min}],Te_{max}\}$$</div>
- 
-Where
-
-<span>$Te_{req,i}$</span>		required evaporating temperature for the ith indoor unit (°C)
-
-<span>$Te_{min}$</span>		minimum evaporating temperature for the indoor unit (e.g. 3) (°C)
-
-<span>$Te_{max}$</span>		maximum evaporating temperature for the indoor unit (e.g. 13) (°C)
-
-In the heating mode:
-
-<div>$$Tc=min\{max[min(Tc_{req,i}),Tc_{min}],Tc_{max}\}$$</div>
- 
-Where
-
-<span>$Tc_{req,i}$</span>		required condensing temperature for the ith indoor unit (°C)
-
-<span>$Tc_{min}$</span>		minimum condensing temperature for the indoor unit (e.g. 42) (°C)
-
-<span>$Tc_{max}$</span>		maximum condensing temperature for the indoor unit (e.g. 46) (°C)
-
-#### *Modeling of the outdoor unit (O/U) - Cooling Mode*
-
-##### Step 2c.1: Piping loss calculation in the cooling mode
-
-Piping loss occurs when the refrigerant flows through the main pipe connecting the indoor and outdoor units. It includes both the refrigerant pressure drop and heat loss. It affects the VRF system operation in several ways. First, the heat loss creates an extra load to the system and leads to higher energy consumptions. Second, the pressure drop and heat loss changes the operational conditions of the compressor (i.e., compressor suction pressure and compressor suction temperature) and thus affects its operational performance. Therefore, the piping loss calculation is critical for the analysis of the whole system.
-
-Note that the change of compressor operational conditions may lead to different control strategies of the system, which in reverse affects the amount of piping loss. So the piping loss analysis and system performance analysis are coupled together. Numerical iterations are designed to address the coupling effect, as described below.
-
-Calculate the refrigerant flow rate for each indoor unit using assumed <span>$h_{Hexin}$</span>:
-
-<div>$$G_i=Q_i/(h_{Hexout,i}-h_{Hexin})$$</div>
-
-Where
-
-<span>$G_i$</span>   	refrigerant flow rate for the i<sup>th</sup> indoor unit (kg/s) 
-
-<span>$Q_i$</span>   	total cooling load of the i<sup>th</sup> zone (W) 
-
-<span>$h_{Hexin}$</span>	enthalpy of the refrigerant entering the indoor unit (kJ/kg)
-
-<span>$h_{Hexout,i}$</span>	enthalpy of the refrigerant leaving a specific indoor unit (kJ/kg)
-
-<span>$h_{Hexout,i}$</span> is a function of <span>$P_e$</span>, <span>$T_e$</span>, and <span>$SH_i$</span>. It can be calculated using refrigerant thermodynamic property equations <span>$f_{g\_h}(P_e,T_e+SH_i)$</span>.
-
-The enthalpy of the refrigerant in the main loop <span>$h_{Hexout}$</span> can be obtained by calculating the weighted average of the enthalpy of the refrigerant in each indoor unit:
-
-<div>$$h_{Hexout}=\sum(h_{Hexout,i}\times{G_i}/{G_{tot}})$$</div>
-
-<div>$$G_{tot}=\sum{G_i}$$</div>
-
-Where
-
-<span>$G_{tot}$</span>   	refrigerant flow rate in the main loop (kg/s) 
-
-<span>$h_{Hexout}$</span>	enthalpy of the main loop refrigerant leaving indoor units (kJ/kg)
-
-The viscosity of the refrigerant within the pipe can be calculated via:
-
-<div>$$k_{v,1}=P_e/4926000$$</div>
-
-<div>$$k_{v,2}=h_{Hexout}/383.55$$</div>
-
-<div>$$k_{v,3}=(T_{Hexout}+273.15)/344.39$$</div>
-
-<div>$$\mu=10^6\times(4.302\times{k_{v,1}}+0.81622\times{k_{v,1}}^2-120.98\times{k_{v,2}}+139.17\times{k_{v,2}}^2+118.76\times{k_{v,3}}+81.04\times{k_{v,3}}^2+5.7858\times{k_{v,1}}\times{k_{v,2}}-8.3817\times{k_{v,1}}\times{k_{v,3}}-218.48\times{k_{v,2}}\times{k_{v,3}}+21.58)$$</div>
-
-Where
-
-<span>$\mu$</span>	viscosity of the refrigerant within the pipe (Pa-s)
-
-<span>$k_{v,i}$</span>	coefficients to calculate the refrigerant viscosity 
-
-<span>$T_{Hexout}$</span>	temperature of main loop refrigerant leaving indoor units, <span>$f_{g\_t}(P_e,h_{Hexout})$</span> (°C)
-
-<span>$f_{g\_t}$</span> 	functions calculating the temperature of superheating refrigerant 
-
-Given <span>$h_{Hexout}$</span> and <span>$P_e=f_{s\_p}(T_e)$</span>, the following dimensionless quantities describing the refrigerant flow state can be obtained:
-
-<div>$$Re=G_{tot}/3600/(0.25\times\pi\times{D^2})\times{D}/\mu$$</div>
-
-<div>$$Pr=\mu\times{f_{g\_Cp}(P_e,h_{Hexout})}\times{0.001}/f_{g\_\lambda}(P_e,h_{Hexout})$$</div>
-
-<div>$$Nu=0.023\times{Re^{0.8}\times{Pr^{0.3}}}$$</div>
-
-<div>$$St=Nu/Re/Pr$$</div>
-
-Where
-
-<span>$P_e$</span>  	evaporating pressure (Pa) 
-
-<span>$Re$</span> 	Reynolds number 
-
-<span>$Pr$</span> 	Prandtl number 
-
-<span>$Nu$</span> 	Nusselt number 
-
-<span>$St$</span> 	Stanton number 
-
-<span>$\mu$</span>	viscosity of the refrigerant within the pipe (Pa-s)
-
-<span>$f_{s\_p}$</span> 	functions calculating the pressure of saturated refrigerant 
-
-<span>$f_{g\_Cp}$</span> 	functions calculating the specific heat of superheating refrigerant 
-
-<span>$f_{g\_\lambda}$</span>	functions calculating the conductivity of superheating refrigerant 
-
-Then the piping pressure loss <span>$\Delta{P_{pipe}}$</span> can be obtained using the above dimensionless quantities:
-
-<div>$$\Delta{P_{pipe}}=8\times{St}\times{Pr^{2/3}}\times{L/D}\times{f_{g\_\rho}(P_e,h_{Hexout})}\times{V^2}/2+H\times{f_{g\_\rho}(P_e,h_{Hexout})}\times9.80665$$</div>
-
-<div>$$P_s=P_e-\Delta{P_{pipe}}$$</div>
-
-Where
-
-<span>$f_{g\_\rho}$</span>	functions calculating the density of superheating refrigerant 
-
-<span>$D$</span>   	main pipe diameter (m) 
-
-<span>$H$</span> 	height difference between the outdoor unit node and indoor unit node of the main pipe (m)
-
-<span>$L$</span>   	main pipe length (m) 
-
-<span>$P_s$</span>   	compressor suction pressure (Pa) 
-
-<span>$\Delta{P_{pipe}}$</span>	pressure drop in the pipe (Pa)
-
-<span>$V$</span>	refrigerant flow velocity (m/s)
-
-The suction saturated temperature <span>$T'_e$</span> (i.e., saturated vapor temperature corresponding to the compressor suction pressure) can be obtained via refrigerant thermodynamic property equations:
-
-<div>$$T'_e=f_{s\_t}(P_e-\Delta{P_{pipe}})$$</div>
-
-Where
-
-<span>$f_{s\_t}$</span>	functions calculating the temperature of saturated refrigerant
-
-<span>$T'_e$</span>   	suction saturated temperature at the compressor inlet (°C)
-
-The heat loss through the pipe can be obtained via:
-
-<div>$$k_1=Nu\times{f_{g\_\lambda}(P_e,h_{Hexout})}$$</div>
-
-<div>$$k_2=2\times{\lambda_i}/Ln(1+2\times{W_i}/D)$$</div>
-
-<div>$$k_3=h\times(D+2\times{W_i})$$</div>
-
-<div>$$Q_{pipe}=(\pi\times{L})\times(T_a-T_{Hexout})/(1/k_1+1/k_2+1/k_3)$$</div>
-
-Where
-
-<span>$f_{g\_\lambda}$</span>	functions calculating the conductivity of superheating refrigerant 
-
-<span>$Q_{pipe}$</span> 	heat loss through the pipe (W)
-
-<span>$T_a$</span> 	average of outdoor air temperature and indoor temperature (°C)
-
-<span>$T_{Hexout}$</span>	temperature of main pipe refrigerant leaving indoor units (°C) 
-
-<span>$w_i$</span>	pipe insulation thickness (m) 
-
-<span>$k_i$</span>	coefficients for the piping loss calculation  
-
-Note that <span>$Q_{pipe}$</span> is calculated using an assumed <span>$h_{Hexin}$</span>. Its value affects the compressor operation calculations as shown in Step 2c.2~2c.6 and may change the value of condensing temperature <span>$T_c$</span>. This leads to an updated <span>$h_{Hexin}=f(P_c,T_c-SC)$</span>. If the difference between the calculated <span>$h_{Hexin}$</span> and the assumed <span>$h_{Hexin}$</span> is higher than the assigned tolerance (5%), a new round of iteration is performed using the calculated <span>$h_{Hexin}$</span>.
-
-##### Step 2c.2: Initialize O/U operation conditions
-
-The compressor operation is coupled with a number operational parameters, which makes it difficult to obtain an analytical solution. In the algorithm, an iterative approach is designed to obtain the energy consumption of the compressor (Step 2c.2 – 2c.6).
-
-For the first iteration, 
-
-* Initialize outdoor unit <span>$SC$</span> with the reference value (from IDF input, e.g., 5°C)
-
-* Initialize the compressor power <span>$N_{comp}$</span> with the value calculated from the reference <span>$COP$</span> (e.g., 3.5):
-
-<div>$$N'_{comp}=\frac{\sum_iQ_{in,total,i}}{COP}$$</div>
-
-Where
-
-<span>$N_{comp}$</span>	compressor power (W)
-
-<span>$N'_{comp}$</span>	assumed compressor power for the first iteration (W)
-
-<span>$Q_{in,total,i}$</span>	total cooling load for zone <span>$i$</span> (W)
-
-For the following iterations,
-
-* Initialize <span>$SC$</span> with the calculated value in the previous iteration  
-
-* Initialize the compressor power <span>$N_{comp}$</span> with the calculated value in the previous iteration
-
-The heat rate released from the outdoor unit can be calculated by:
-
-<div>$$Q_{out}=\sum_iQ_{in,total,i}+N_{comp}+Q_{pipe}$$</div> 
-
-Where
-
-<span>$Q_{out}$</span>	heat rate released from the outdoor unit (W)
-
-<span>$Q_{pipe}$</span> 	heat loss through the pipe (W)
-
-##### Step 2c.3: Calculate O/U effective condensing temperature
-
- (1) Calculate the required coil surface air temperature <span>${T_{fs}}'$</span> for the outdoor unit.
-
-The temperature of the air leaving the outdoor unit <span>${T_{out}}'$</span> can be calculated by:
- 
-<div>$${T_{out}}'={T_{in}}'+Q_{out}/({G_{a,rate}}'\times{c_p}\times{{\rho_{in}}'})$$</div>
- 
-Where
-
-<span>${G_{a,rate}}'$</span>	volumetric flow rate of the air through the outdoor unit, at the rating conditions (m<sup>3</sup>/s)
-
-<span>${T_{out}}'$</span>	temperature of the air leaving the outdoor unit (°C)
-
-<span>${T_{in}}'$</span>	temperature of the air entering the outdoor unit, i.e., outdoor air (°C)
-
-<span>${\rho_{in}}'$</span>  	air density at outdoor conditions,<span>$f_{\rho}({T_{in}}',{W_{in}}')$</span>   (kg/m<sup>3</sup>)
-
-The condenser surface temperature <span>${T_{fs}}'$</span> can be calculated by:
- 
-<div>$${T_{fs}}'={T_{in}}'+({T_{out}}'-{T_{in}}')/(1-{BF_c}')$$</div>
- 
-Where
-
-<span>${BF_c}'$</span> 	bypass factor for the outdoor unit  
-
-(2) Calculate required condensing temperature for the outdoor unit <span>$Tc_{req}$</span> and then the effective condensing temperature <span>$Tc$</span> (between 42-46°C)
- 
-<div>$$Tc_{req}={T_{fs}}'+[A_h\cdot SC^2+B_h\cdot SC+C_h]$$</div>
-
-<div>$$Tc=Tc_{req}$$</div>
-
-Where	
-
-<span>$A_h$</span>,<span>$B_h$</span>,<span>$C_h$</span>   	coefficients (°C)
-
-<span>$SC$</span> 		subcooling degrees for the outdoor unit (°C)
-
-<span>$SC_{ref}$</span> 		reference subcooling degrees for the outdoor unit (°C)
-
-<span>$Tc_{req}$</span>		required condensing temperature for the outdoor unit (°C)
-
-<span>$Tc$</span>		effective condensing temperature (°C)
-
-##### Step 2c.4: Calculate required Loading Index 
-
-Loading Index is used to describe the operational mode of the compressor system. The first index represents minimal capacity operation, while the last index represents full capacity operation. 
-
-The required Loading Index can be calculated by the following procedures. 
-
-a. Calculate the evaporative capacity at a variety of Loading Index:
-
-<div>$$M_{cap}=(r_1+r_2T_c+r_3{T_e}'+r_4T_c^2+r_5T_c{T_e}'+r_6{T_e}'^2)$$</div>
-<div>$$Q_{rps}=C_{cap,system} \times M_{cap} \times Q_{ref} $$</div>
-
-Where	
-
-<span>$C_{cap,system}$</span>	evaporative capacity correction factor, describing the possible system configuration difference between test bed and real system (a constant value obtained from manufacturer data)  
-
-<span>$r_1$</span>,…,<span>$r_6$</span>  	empirical coefficients corresponding to <span>$rps$</span>  
-
-<span>$rps$</span>	compressor speed (r/s) 
-
-<span>${T_e}'$</span>   	suction saturated temperature at the compressor inlet (°C)
-
-<span>$T_c$</span>	effective condensing temperature (°C)
-
-<span>$M_{cap}$</span>	multiplier for the evaporative capacity calculation (--)
-
-<span>$Q_{rps}$</span>	evaporative capacity corresponding to <span>$rps$</span> (W) 
-
-<span>$Q_{ref}$</span>	rated evaporative capacity (W) 
-
-An example of resulting capacity for different <span>$rps$</span> (at <span>$T_c$</span>=36°C and <span>${T_e}'$</span>=9°C) is presented in Table 1.
-
-Table 1– Evaporative capacity at different Loading Index 
-
-| Loading Index (<span>$rps$</span>) | Evaporative Capacity (kW),<span>$T_c$</span>=36°C,<span>${T_e}'$</span>=9°C| Loading Index (<span>$rps$</span>) | Evaporative Capacity (kW),<span>$T_c$</span>=36°C,<span>${T_e}'$</span>=9°C|
-|---------------------|-----------------------------|---------------------|-----------------------------|
-|    1 (18)           |    3.951                    |    2 (25)           |    5.400                    |
-|    3 (30)           |    6.435                    |    4 (36)           |    8.516                    |
-|    5 (45)           |    10.756                   |    6 (60)           |    14.445                   |
-|    7 (75)           |    18.412                   |    8 (90)           |    22.045                   |
-|    9 (108)          |    26.162                   |                     |                             |
-
-b. Find the <span>$rps$</span> range that covers the required evaporative capacity <span>$Q_{rps,modify}$</span>.  
-
-<div>$$Q_{rps,modify}=C_{cap,operation}\times(\sum{Q_{in,total}}+Q_{pipe})$$</div>
-
-<div>$$C_{cap,operation}=C_{cap,density}\times{C_{cap,enthalpy}}$$</div>
-
-<div>$$C_{cap,density}=\rho_{test}/\rho_{real}$$</div>
-
-<div>$$C_{cap,enthalpy}=\frac{h_{Evapout,test}-h_{Evapin,test}}{h_{Compin,real}-h_{Evapin,real}}$$</div>
-
-<div>$$h_{Compin,real}=h_{Hexout,real}+Q_{pipe}/G_{tot}$$</div>
-
-Where	
-
-<span>$C_{cap,operation}$</span> evaporative capacity correction factor, describing the operational difference between test cases and real cases (i.e., <span>$SH$</span> and <span>$SC$</span>)  
-
-<span>$C_{cap,density}$</span> evaporative capacity correction factor, describing the variations of refrigerant density at test conditions and real operational conditions  
-
-<span>$C_{cap,enthalpy}$</span> evaporative capacity correction factor, describing the variations of refrigerant enthalpy at test conditions and real operational conditions  
-
-<span>$G_{tot}$</span>   	refrigerant flow rate in the main loop (kg/s) 
-
-<span>$h_{Evapin,real}$</span> enthalpy of refrigerant entering the evaporators (IU) at real conditions [kJ/kg]
-
-<span>$h_{Evapout,real}$</span> average enthalpy of refrigerant leaving the evaporators (IU) at real conditions [kJ/kg] 
-
-<span>$h_{Evapin,test}$</span> enthalpy of refrigerant entering the evaporator at test conditions (It corresponds to <span>$SC$</span> at test condition(e.g., 5 °C)  and Tc) (kJ/kg)
-
-<span>$h_{Evapout,test}$</span> enthalpy of refrigerant leaving the evaporator at test conditions  (It corresponds to <span>$SH$</span> at test condition(e.g., 8 °C)  and Te) (kJ/kg) 
-
-<span>$h_{Compin}$</span>	enthalpy of refrigerant entering the compressor (kJ/kg)
-
-<span>$Q_{pipe}$</span> 	heat loss through the pipe (W)
-
-For example, if the required capacity is 8 kW, the <span>$rps$</span> range is 30 to 36.
-
-c. Calculate the <span>$rps$</span> that meets the required capacity by interpolation. In the above example, the resulting <span>$rps$</span> is 34.5 <span>$rps$</span>.
-
-d. If the calculated <span>$rps$</span> is lower than the minimum <span>$rps$</span> (e.g. 18<span>$rps$</span>), go to Step 2c.5, otherwise skip Step 2c.5 and directly go to Step 2c. 6.
-
-##### Step 2c.5: Modify evaporating temperature to further reduce outdoor unit capacity
-
-If the calculated <span>$rps$</span> is lower than the minimum <span>$rps$</span> (e.g. 18<span>$rps$</span>), it means that the zone cooling load is even lower than the system evaporative capacity corresponding to the minimum compressor speed. In this situation, the evaporating temperature <span>$T_e$</span> as well as the superheating degree <span>$SH$</span> is modified to further reduce the outdoor unit capacity. More specifically: 
-
-a. Set <span>$rps$</span> at its minimum value (e.g., 18 <span>$rps$</span>).
-
-b. Update <span>${T_e}'$</span> to meet the required evaporative capacity, using equations described in Step 2c.4a.
-
-c. Update <span>$T_e$</span> to meet the updated <span>${T_e}'$</span>. Note that due to the <span>$T_e$</span> updates, the refrigerant state and flow rate are changed and thus the piping loss analysis should also be repeated (Step 2c.1). So is the calculation of <span>$C_{cap,operation}$</span> (Step 2c.2-2c.3).
-
-d. <span>$SH$</span> can be updated based on the updated <span>$T_e$</span>, using the equations shown in Step 1.2. 
-
-##### Step 2c.6: Calculate the compressor power
-
-(1) Calculate the compressor power by the following procedures.
-
-a. Calculate the compressor power at a variety of loading index using the following equation. The resulting table (Table 2) from the same example used above is shown below. 
-
-<div>$$M_{comp}=c_1+c_2T_c+c_3{T_e}'+c_4T_c^2+c_5T_c{T_e}'+c_6{T_e}'^2$$</div>
-<div>$$N_{comp,rps}=M_{comp} \times N_{comp,ref}$$</div>
-
-Where	
-
-<span>$c_1$</span>,…,<span>$c_6$</span>   	empirical coefficients corresponding to <span>$rps$</span>  
-
-<span>${T_e}'$</span> 		suction saturated temperature at the compressor inlet (°C)
-
-<span>$T_c$</span>		effective condensing temperature (°C)
-
-<span>$M_{comp}$</span>		multiplier for the compressor power calculation (--)
-
-<span>$N_{comp,ref}$</span>	rated compressor power  (W)
-
-<span>$N_{comp,rps}$</span>	compressor power corresponding to <span>$rps$</span> (W)
-
-Table 2 – Outdoor unit compressor power at different Loading Index 
-
-| Loading Index (<span>$rps$</span>) | Elec. Power (kW), <span>$T_c$</span>=36°C, <span>${T_e}'$</span>=9°C| Loading Index (<span>$rps$</span>) | Elec. Power (kW), <span>$T_c$</span>=36°C, <span>${T_e}'$</span>=9°C|
-|---------------------|----------------------------|---------------------|----------------------------|
-|    1 (18)           |    0.527                   |    2 (25)           |    0.766                   |
-|    3 (30)           |    0.936                   |    4 (36)           |    1.227                   |
-|    5 (45)           |    1.546                   |    6 (60)           |    2.149                   |
-|    7 (75)           |    2.760                   |    8 (90)           |    3.357                   |
-|    9 (108)          |    4.359                   |                     |                            |
-
-b. According to the <span>$rps$</span> range determined, calculate the compressor power <span>$N_{comp}$</span>  by interpolation. In the above example, the compressor power is 1.155 kW. 
-
-(2) Compare the calculated <span>$N_{comp}$</span> above with the initialized <span>${N_{comp}}'$</span> in Step 2c.2:
-
-* If  <span>${N_{comp}}'-N_{comp}>\delta$</span> then go to Step 2c.2 for a new round of iteration.
-
-* Else, end the iteration and go to Step 2c.7.
-
-##### Step 2c.7: Total power consumption of the outdoor unit
-
-Calculate the total electric power consumption by the outdoor unit:
-
-<div>$$N_{out}=N_{fan}+N_{comp}/e_{inv}$$</div>
-
-Where	
-
-<span>$e_{inv}$</span>	efficiency of the inverter of compressor  
-
-<span>$N_{fan}$</span>	electric power consumption by the outdoor fan (W)
-
-<span>$N_{out}$</span>	total electric power consumption by the outdoor unit (W)
-
-#### *Modeling of the outdoor unit (O/U) - Heating Mode*
-
-##### Step 2h.1: Piping loss calculation in the heating mode
-
-Similarly to that in the cooling mode, the piping loss analysis in the heating mode needs to address the coupling effect between the piping loss and system operations. However, due to the control strategy difference between the two modes, the piping loss algorithm in the heating mode requires different calculation steps and more numerical iterations, as shown below.
-
-Calculate the refrigerant flow rate for each indoor unit using assumed <span>$h_{Hexin}$</span>:
-
-<div>$$G_i=Q_i/(h_{Hexin}-h_{Hexout,i})$$</div>
-
-Where
-
-<span>$G_i$</span>   	refrigerant flow rate for the i<sup>th</sup> indoor unit (kg/s) 
-
-<span>$Q_i$</span>   	total heating load of the i<sup>th</sup> zone (W) 
-
-<span>$h_{Hexin}$</span>	enthalpy of the refrigerant entering the indoor unit (kJ/kg)
-
-<span>$h_{Hexout,i}$</span>	enthalpy of the refrigerant leaving a specific indoor unit (kJ/kg)
-
-<span>$h_{Hexout,i}$</span> is a function of <span>$P_c$</span>, <span>$T_c$</span>, and <span>$SC_i$</span>. It can be calculated using refrigerant thermodynamic property equations <span>$f_{g\_h}(P_c,T_c-SC_i)$</span>.
-
-The refrigerant flow rate in the main loop can be obtained by summing up the flow rate in each indoor unit:
-
-<div>$$G_{tot}=\sum{G_i}$$</div>
-
-Where
-
-<span>$G_{tot}$</span>   	refrigerant flow rate in the main loop (kg/s) 
-
-Calculate the average refrigerant pressure and enthalpy within the pipes, using assumed piping pressure loss <span>$\Delta{P_{pipe}}$</span> and <span>$h_{Tdi}$</span>: 
-
-<div>$$P_{ave}=P_c+\Delta{P_{pipe}}/2$$</div>
-
-<div>$$h_{ave}=(h_{Hexin}+h_{Tdi})/2$$</div>
-
-Where
-
-<span>$h_{ave}$</span> 	average refrigerant enthalpy within the main pipe (kJ/kg)
-
-<span>$h_{Hexin}$</span>	enthalpy of the refrigerant entering the indoor unit (kJ/kg)
-
-<span>$h_{Tdi}$</span> enthalpy of the refrigerant leaving the compressor (kJ/kg)
-
-<span>$P_{ave}$</span> 	average refrigerant pressure within the main pipe (Pa)
-
-<span>$P_c$</span>   	condensing pressure (Pa) 
-
-<span>$\Delta{P_{pipe}}$</span>	pressure drop in the main pipe (Pa)
-
-The viscosity of the refrigerant within the pipe can be calculated given <span>$P_{ave}$</span> and <span>$h_{ave}$</span>, using the following equations:
-
-<div>$$k_{v,1}=P_{ave}/4926000$$</div>
-
-<div>$$k_{v,2}=h_{ave}/383.55$$</div>
-
-<div>$$k_{v,3}=(T_{ave}+273.15)/344.39$$</div>
-
-<div>$$\mu=10^6\times(4.302\times{k_{v,1}}+0.81622\times{k_{v,1}}^2-120.98\times{k_{v,2}}+139.17\times{k_{v,2}}^2+118.76\times{k_{v,3}}+81.04\times{k_{v,3}}^2+5.7858\times{k_{v,1}}\times{k_{v,2}}-8.3817\times{k_{v,1}}\times{k_{v,3}}-218.48\times{k_{v,2}}\times{k_{v,3}}+21.58)$$</div>
-
-Where
-
-<span>$\mu$</span>	viscosity of the refrigerant within the pipe (Pa-s)
-
-<span>$k_{v,i}$</span>	coefficients to calculate the refrigerant viscosity 
-
-<span>$h_{ave}$</span> 	average refrigerant enthalpy within the pipes (kJ/kg)
-
-<span>$P_{ave}$</span> 	average refrigerant pressure within the pipes (Pa)
-
-<span>$T_{ave}$</span>	average temperature of refrigerant leaving indoor units, which corresponds to <span>$P_{ave}$</span> and <span>$h_{ave}$</span> (°C)
-
-Given <span>$P_{ave}$</span> and <span>$h_{ave}$</span>, the following dimensionless quantities describing the refrigerant flow state can be obtained:
-
-<div>$$Re=G_{tot}/3600/(0.25\times\pi\times{D^2})\times{D}/\mu$$</div>
-
-<div>$$Pr=\mu\times{f_{g\_Cp}(P_{ave},h_{ave})}\times{0.001}/f_{g\_\lambda}(P_{ave},h_{ave})$$</div>
-
-<div>$$Nu=0.023\times{Re^{0.8}\times{Pr^{0.4}}}$$</div>
-
-<div>$$St=Nu/Re/Pr$$</div>
-
-Where
-
-<span>$Re$</span> 	Reynolds number 
-
-<span>$Pr$</span> 	Prandtl number 
-
-<span>$Nu$</span> 	Nusselt number 
-
-<span>$St$</span> 	Stanton number 
-
-<span>$\mu$</span>	viscosity of the refrigerant within the pipe (Pa-s)
-
-<span>$f_{g\_Cp}$</span> 	functions calculating the specific heat of superheating refrigerant 
-
-<span>$f_{g\_\lambda}$</span>	functions calculating the conductivity of superheating refrigerant 
-
-Then the piping pressure loss <span>$\Delta{P_{pipe}}$</span> can be obtained using the above dimensionless quantities:
-
-<div>$$\Delta{P_{pipe}}=8\times{St}\times{Pr^{2/3}}\times{L/D}\times{f_{g\_\rho}(P_{ave},h_{ave})}\times{V^2}/2-H\times{f_{g\_\rho}(P_{ave},h_{ave})}\times9.80665$$</div>
-
-Where
-
-<span>$f_{g\_\rho}$</span>	functions calculating the density of superheating refrigerant 
-
-<span>$D$</span>   	main pipe diameter (m) 
-
-<span>$H$</span> 	height difference between the outdoor unit node and indoor unit node of the main pipe (m)
-
-<span>$L$</span>   	main pipe length (m) 
-
-<span>$St$</span> 	Stanton number 
-
-<span>$Re$</span> 	Reynolds number 
-
-<span>$Pr$</span> 	Prandtl number 
-
-<span>$\Delta{P_{pipe}}$</span>	pressure drop in the pipe (Pa)
-
-<span>$V$</span>	refrigerant flow velocity (m/s)
-
-Compare the calculated <span>$\Delta{P_{pipe}}$</span> and the one assumed above. If the difference is higher than the assigned tolerance (5%), a new round of iteration is performed using the calculated <span>$\Delta{P_{pipe}}$</span>.
-
-The compressor discharge saturated temperature <span>$T'_c$</span> (i.e., saturated vapor temperature corresponding to compressor discharge pressure) can be obtained via:
-
-<div>$$T'_c=f_{s\_t}(P_c+\Delta{P_{pipe}})$$</div>
-
-Where
-
-<span>$f_{s\_t}$</span>	functions calculating the temperature of saturated refrigerant
-
-<span>$T'_c$</span>    	discharge saturated temperature at the compressor outlet (°C)
-
-<span>$P_c$</span>    	condensing pressure (Pa)
-
-<span>$\Delta{P_{pipe}}$</span>	pressure drop in the pipe (Pa)
-
-The heat loss through the pipe can be obtained via:
-
-<div>$$k_1=Nu\times{f_{g\_\lambda}(P_{ave},h_{ave})}$$</div>
-
-<div>$$k_2=2\times{\lambda_i}/Ln(1+2\times{W_i}/D)$$</div>
-
-<div>$$k_3=h\times(D+2\times{W_i})$$</div>
-
-<div>$$Q_{pipe}=(\pi\times{L})\times(T_a-T_{Hexin})/(1/k_1+1/k_2+1/k_3)$$</div>
-
-Where
-
-<span>$f_{g\_\lambda}$</span>	functions calculating the conductivity of superheating refrigerant 
-
-<span>$Q_{pipe}$</span> 	heat loss through the pipe (W)
-
-<span>$T_a$</span> 	average of outdoor air temperature and indoor temperature (°C)
-
-<span>$T_{Hexin}$</span>	average of entering indoor units (°C)
-
-<span>$w_i$</span>	pipe insulation thickness (m) 
-
-<span>$k_i$</span>	coefficients for the piping loss calculation  
-
-The enthalpy of the refrigerant entering the indoor unit can be updated using the calculated <span>$Q_{pipe}$</span>:
-
-<div>$$h_{Tdi}=h_{Hexin}+Q_{pipe}/G_{tot}$$</div>
-
-Where
-
-<span>$h_{Hexin}$</span>	enthalpy of the refrigerant entering the indoor unit (kJ/kg)
-
-<span>$h_{Tdi}$</span> enthalpy of the refrigerant leaving the compressor (kJ/kg)
-
-<span>$G_{tot}$</span>   	refrigerant flow rate in the main loop (kg/s) 
-
-Compare the calculated <span>$h_{Tdi}$</span> and the one assumed above. If the difference is higher than the assigned tolerance (5%), a new round of iteration is performed using the calculated <span>$h_{Tdi}$</span>.
-
-Note that <span>$Q_{pipe}$</span> is calculated using an assumed <span>$h_{Hexin}$</span> at the beginning of the piping loss algorithm. Its value affects the compressor operation calculations as shown in Step 2h.2~2h.6 and may change the value of evaporating temperature <span>$T_e$</span>. This leads to an updated <span>$h_{Hexin}=f(P_e,T_e+SH,N_{comp},G_{tot})$</span>. If the difference between the calculated result and the assumed value is higher than the assigned tolerance (5%), a new round of iteration is performed using the calculated <span>$h_{Hexin}$</span>.
-
-##### Step 2h.2: Initialize O/U operation conditions
-
-Similar to that in cooling mode, an iteration approach is designed to determine the energy consumption of the compressor (Step 2h. 2 to Step 2h. 6).
-
-For the first iteration, 
-
-* Initialize outdoor unit <span>$SH$</span> with the reference value (from IDF input, e.g., 1.5°C)
-
-* Iinitialize the compressor power <span>$N_{comp}$</span> with the value calculated from the reference <span>$COP$</span> (e.g., 3.5):
-
-<div>$$N'_{comp}=\frac{\sum_iQ_{in,total,i}}{COP}$$</div>
-
-Where
-
-<span>$N_{comp}$</span>	compressor power (W)
-
-<span>$N'_{comp}$</span>	assumed compressor power for the first iteration (W)
-
-<span>$Q_{in,total,i}$</span>	total heating load for zone <span>$i$</span> (W)
-
-For the following iterations,
-
-* Initialize <span>$SH$</span> with the calculated value in the previous iteration  
-
-* Initialize the compressor power <span>$N_{comp}$</span> with the calculated value in the previous iteration
-
-Calculate the heat rate extracted by the outdoor unit by:
-
-<div>$$Q_{out}=\sum_iQ_{in,total,i}+Q_{pipe}-N_{comp}$$</div> 
-
-Where
-
-<span>$Q_{out}$</span>	heat rate extracted by the outdoor unit (W)
-
-<span>$Q_{pipe}$</span> 	heat loss through the pipe (W)
-
-##### Step 2h.3: Calculate O/U effective evaporating temperature
-
-(1) Calculate the required coil surface air temperature <span>${T_{fs}}'$</span> for the outdoor unit.
-
-The enthalpy of the air leaving the outdoor unit can be calculated by:
- 
-<div>$${H_{fs}}'={H_{in}}'-Q_{out}/({G_{a,rate}}'\times{\rho_o})/(1-BF')$$</div>
-
-The coil surface air temperature <span>${T_{fs}}'$</span> can be calculated from the <span>${H_{fs}}'$</span>:
-
-<div>$$if\quad{H_{fs}}'<H_{98\%,W_o}\quad{then}\quad{T_{fs}}'=f({H_{fs}}',98\%)$$</div>
-
-<div>$$if\quad{H_{fs}}'\ge{H_{98\%,W_o}}\quad{then}\quad{T_{fs}}'=f({H_{fs}}',W_o)$$</div>
- 
-Where
-
-<span>$BF'$</span> 	bypass factor for the outdoor unit  
-
-<span>${G_{a,rate}}'$</span>	volumetric flow rate of the air through the outdoor unit, at the rating conditions (m<sup>3</sup>/s)
-
-<span>${H_{fs}}'$</span>	enthalpy of the air leaving the outdoor unit (kJ/kg)
-
-<span>${H_{in}}'$</span>	enthalpy of the air entering the outdoor unit, i.e., outdoor air (kJ/kg)
-
-<span>$W_o$</span>       humidity ratio of the outdoor air (kg/kg)
-
-<span>$\rho_o$</span>     density of the outdoor air (kg/m<sup>3</sup>)
-
-(2) Calculate required evaporating temperature for the outdoor unit <span>$Te_{req}$</span> and then the effective evaporating temperature <span>$Te$</span>.
- 
-<div>$$Te_{req}={T_{fs}}'-[{A_c}'\cdot SH^2+{B_c}'\cdot SH+{C_c}']$$</div>
-
-<div>$$Te=Te_{req}$$</div>
-
-Where	
-
-<span>${A_c}'$</span>,<span>${B_c}'$</span>,<span>${C_c}'$</span>   	coefficients (°C)
-
-<span>$SH$</span>			superheating degrees for the outdoor unit (°C)
-
-<span>$SH_{ref}$</span>	reference superheating degrees for the outdoor unit (°C)
-
-<span>$Te_{req}$</span>	required evaporating temperature for the outdoor unit (°C)
-
-<span>$Te$</span>		effective evaporating temperature (°C)
-
-##### Step 2h.4: Calculate required compressor Loading Index
-
-Calculate the required compressor Loading Index by the following procedures.
-
-a. Calculate the evaporative capacity at a variety of speeds:
-
-<div>$$M_{cap}=C_{cap,system}\times(r_1+r_2{T_c}'+r_3T_e+r_4{T_c}'^2+r_5{T_c}'T_e+r_6T_e^2)$$</div>
-<div>$$Q_{rps}=C_{cap,system} \times M_{cap} \times Q_{ref}$$</div>
-
-Where	
-
-<span>$C_{cap,system}$</span>	evaporative capacity correction factor, describing the possible system configuration difference between test bed and real system (obtained from manufacturer data)  
-
-<span>$r_1$</span>,…,<span>$r_6$</span>  	empirical coefficients corresponding to <span>$rps$</span>  
-
-<span>$rps$</span>	compressor speed (r/s) 
-
-<span>$T_e$</span>   	effective evaporating temperature (°C)
-
-<span>$M_{cap}$</span>	multiplier for the evaporative capacity calculation (--)
-
-<span>${T_c}'$</span>	discharge saturated temperature at the compressor outlet (°C)
-
-<span>$Q_{rps}$</span>	evaporative capacity corresponding to <span>$rps$</span> (W) 
-
-<span>$Q_{ref}$</span>	rated evaporative capacity (W) 
-
-An example of resulting capacity for different <span>$rps$</span> (at <span>${T_c}'$</span>=36°C and <span>$T_e$</span>=9°C) is presented in Table 3.
-
-Table 3– evaporative capacity at different Loading Index 
-
-| Loading Index (<span>$rps$</span>) | Evaporative Capacity (kW),<span>${T_c}'$</span>=36°C,<span>$T_e$</span>=9°C| Loading Index (<span>$rps$</span>) | Evaporative Capacity (kW),<span>${T_c}'$</span>=36°C,<span>$T_e$</span>=9°C|
-|---------------------|-----------------------------|---------------------|-----------------------------|
-|    1 (18)           |    3.951                    |    2 (25)           |    5.400                    |
-|    3 (30)           |    6.435                    |    4 (36)           |    8.516                    |
-|    5 (45)           |    10.756                   |    6 (60)           |    14.445                   |
-|    7 (75)           |    18.412                   |    8 (90)           |    22.045                   |
-|    9 (108)          |    26.162                   |                     |                             |
-
-b. Find the <span>$rps$</span> range that covers the required evaporative capacity <span>$Q_{rps,modify}$</span>.  
-
-<div>$$Q_{rps,modify}=C_{cap,operation}\times(\sum{Q_{in,total}}+Q_{pipe}-N_{comp})$$</div>
-
-<div>$$C_{cap,operation}=C_{cap,density}\times{C_{cap,enthalpy}}$$</div>
-
-<div>$$C_{cap,density}=\rho_{test}/\rho_{real}$$</div>
-
-<div>$$C_{cap,enthalpy}=\frac{h_{Evapout,test}-h_{Condout,test}}{h_{Compin,real}-h_{Condout,real}}$$</div>
-
-Where	
-
-<span>$C_{cap,operation}$</span>	evaporative capacity correction factor, describing the operational difference between test cases and real cases (i.e., <span>$SH$</span> and <span>$SC$</span>)  
-
-<span>$C_{cap,density}$</span>	evaporative capacity correction factor, describing the variations of refrigerant density at test conditions and real operational conditions  
-
-<span>$C_{cap,enthalpy}$</span>	evaporative capacity correction factor, describing the variations of refrigerant enthalpy at test conditions and real operational conditions  
-
-<span>$h_{Condout,test}$</span> 	enthalpy of refrigerant leaving the condensers (IU) at test conditions  (It corresponds to <span>$SH$</span> at test condition(e.g., 8°C)  and <span>$Te$</span>) (kJ/kg) 
-
-<span>$h_{Condout,real}$</span> 	average enthalpy of refrigerant leaving the condensers (IU) at real conditions (kJ/kg)
-
-<span>$h_{Compin,real}$</span>	enthalpy of refrigerant entering the compressor at real conditions (It corresponds to <span>$SH$</span> and <span>$Te$</span> at real conditions) (kJ/kg)
-
-<span>$Q_{pipe}$</span> 	heat loss through the pipe (W)
-
-For example, if the required capacity is 8 kW, the <span>$rps$</span> range is 30 to 36 <span>$rps$</span> based on Table 3.
-
-c. Calculate the <span>$rps$</span> that meets the need by interpolation. In the above example, the resulting <span>$rps$</span> is 34.5 <span>$rps$</span>.
-
-d. If the calculated <span>$rps$</span> is lower than the minimum <span>$rps$</span> (e.g. 18<span>$rps$</span>), go to Step 2h. 5; otherwise, skip Step 2h. 5 and go to Step 2h. 6.
-
-##### Step 2h.5: Modify evaporating temperature to further reduce outdoor unit capacity 
-
-If the calculated <span>$rps$</span> is lower than the minimum <span>$rps$</span> (e.g. 18 <span>$rps$</span>), it means that the zone heating load (indoor unit side) is so low that it leads to an evaporative capacity (outdoor unit side) which is even lower than the system evaporative capacity corresponding to the minimum compressor speed. In this situation, the evaporating temperature <span>$Te$</span> as well as the superheating degree <span>$SH$</span> is modified to further reduce the outdoor unit capacity. More specifically: 
-
-a. Set <span>$rps$</span> at its minimum value (e.g., 18 <span>$rps$</span>).
-
-b. Update <span>$Te$</span> to meet the required evaporative capacity, using equations described in Step 2h.4a.
-
-c. <span>$SH$</span> for each indoor unit can be updated using the equations shown in Step 1.2.
-
-It should be noted that, different from the corresponding step in the cooling mode (Step 2c.5), the <span>$Te$</span> and <span>$SH$</span> updates in the heating mode do not affect the refrigerant state and flow rate calculations (as shown in Step 2h.1). Therefore, the piping loss analysis does not need to be repeated here.
-
-##### Step 2h.6: Calculate the compressor power
-
-(1) Calculate the compressor power by the following procedures.
-
-a. Calculate the compressor power at a variety of Loading Index using the following equation. The resulting table (Table 4) from the same example is shown below.
-
-<div>$$M_{comp}=c_1+c_2{T_c}'+c_3T_e+c_4{T_c}'^2+c_5{T_c}'T_e+c_6T_e^2$$</div>
-<div>$$N_{comp,rps}=M_{comp} \times N_{comp,ref}$$</div>
-
-Where
-
-<span>$c_1$</span>,…,<span>$c_6$</span>   	empirical coefficients corresponding to <span>$rps$</span>  
-
-<span>$T_e$</span>		effective evaporating temperature (°C)
-
-<span>$T_{e,ref}$</span>		reference evaporating temperature (°C)
-
-<span>${T_c}'$</span>   		discharge saturated temperature at the compressor outlet (°C)
-
-<span>$T_{c,ref}$</span>		reference condensing temperature (°C) 
-
-<span>$M_{comp}$</span>		multiplier for the compressor power calculation (--)
-
-<span>$N_{comp,ref}$</span>	rated compressor power  (W)
-
-<span>$N_{comp,rps}$</span>	compressor power corresponding to <span>$rps$</span> (W)
-
-Table 4 – Outdoor unit compressor power at different Loading Index 
-
-| Loading Index (<span>$rps$</span>) | Elec. Power (kW), <span>${T_c}'$</span>=36°C, <span>$T_e$</span>=9°C| Loading Index (<span>$rps$</span>) | Elec. Power (kW), <span>${T_c}'$</span>=36°C, <span>$T_e$</span>=9°C|
-|---------------------|----------------------------|---------------------|----------------------------|
-|    1 (18)           |    0.527                   |    2 (25)           |    0.766                   |
-|    3 (30)           |    0.936                   |    4 (36)           |    1.227                   |
-|    5 (45)           |    1.546                   |    6 (60)           |    2.149                   |
-|    7 (75)           |    2.760                   |    8 (90)           |    3.357                   |
-|    9 (108)          |    4.359                   |                     |                            |
-
-b. According to the <span>$rps$</span> range determined, calculate the compressor power <span>$N_{comp}$</span>  by interpolation. In the above example, the compressor power is 1.155 kW. 
-
-(2) Compare the calculated <span>$N_{comp}$</span> above with the initialized <span>${N_{comp}}'$</span> in Step 2h.2:
-
-* If  <span>${N_{comp}}'-N_{comp}>\delta$</span> then go to Step 2h.2 for a new round of iteration.
-
-* Else, end the iteration and go to Step 2h.7.
-
-##### Step 2h.7: Total power consumption of the outdoor unit
-
-Same as that in the cooling mode (Step 2c. 7)
-
-#### *Modeling of the indoor unit (I/U) - Part II - Cooling Mode*
-##### Step 3c.1: Update air flow rate for each indoor unit
-(1) Calculate coil surface temperature for each indoor unit:
-
-<div>$$T_{fs}=T_e+[A_c\cdot SH^2+B_c\cdot SH+C_c]$$</div>
-
-Where	
-
-<span>$T_e$</span>	evaporating temperature decided in the outdoor unit calculations (°C)
-
-<span>$T_{fs}$</span>	coil surface temperature (°C)
-
-<span>$SH$</span>	superheating degrees decided in the outdoor unit calculations (°C)
-
-2)	Calculate the enthalpy of the air at the coil surface, <span>$H_{fs}$</span>:
-
-<div>$$if\quad{T_{fs}}<T_{98\%,W_{in}}\quad{then}\quad{H_{fs}}=f(T_{fs},98\%)$$</div>
-
-<div>$$if\quad{T_{fs}}\ge{T_{98\%,W_{in}}}\quad{then}\quad{H_{fs}}=f(T_{fs},W_{in})$$</div>
-
-Where
-
-<span>$T_{98\%,W_{in}}$</span>	dew point temperature of the indoor air (°C)
-
-<span>$H_{fs}$</span> 		enthalpy of the air at the coil surface (kJ/kg)
-
-3)	Calculate the required air flow rate <span>$G_a$</span> for each indoor unit:
-
-<div>$$G_a=Q_{in,total}/[(H_{coil,in}-H_{fs})\times{(1-BF)}\times{\rho_{in}}]$$</div> 
-
-Where
-
-<span>$Q_{in,total}$</span>	total cooling load for the zone (W)
-
-<span>$H_{coil,in}$</span>	enthalpy of the entering air of the indoor unit (kJ/kg)
-
-<span>$\rho_{in}$</span> density of indoor air,<span>$f_{\rho}(T_{in},W_{in})$</span> (kg/m<sup>3</sup>)
-
-4)	Decide whether to modify <span>$SH$</span> for further indoor unit capacity reduction.
-
-* If <span>$G_a$</span> < <span>$G_{a,min}$</span> (e.g., <span>$0.7\times$</span><span>$G_{a,rate}$</span>) go to Step 3c. 2
-
-* Else, directly go to Step 3c. 3
-
-##### Step 3c.2: Modify <span>$SH$</span> to adjust the indoor unit capacity 
-
-Set <span>$G_a$</span> at its minimum value (e.g., <span>$0.7\times$</span><span>$G_{a,rate}$</span>).
-
-The required coil surface temperature <span>$T_{fs}$</span> can be determined as described in Step 1.2.
-
-Given <span>$T_{fs}$</span> and <span>$T_e$</span>, <span>$SH$</span> can be determined using the equation shown in Step 1.3.
-
-* If <span>$SH$</span> > 15°C, Set <span>$SH$</span> as 15°C. On/Off control strategy may be implemented when needed.
-
-#####Step 3c. 3: Total power consumption of the indoor unit
-
-The power consumption of the indoor unit comes from the fan operations. This can be calculated using the existing VAV fan model in EnergyPlus. Please refer to the current EnergyPlus Engineering Reference for more details.
-
-#### *Modeling of the indoor unit (I/U) - Part II - Heating Mode*
-
-#####Step 3h.1:  Update air flow rate for each indoor unit.
-
-1)	Calculate coil surface temperature for all the indoor units:
-
-<div>$$T_{fs}=T_c-[A_h\cdot SC^2+B_h\cdot SC+C_h]$$</div>
-
-Where
-
-<span>$T_c$</span>	condensing temperature decided in the outdoor unit calculations (°C)
-
-<span>$T_{fs}$</span>	coil surface temperature (°C)
-
-<span>$SC$</span>	subcooling degrees decided in the outdoor unit calculations (°C)
-
-2)	Calculate the required air flow rate <span>$G_a$</span> for each indoor unit:
-
-<div>$$G_a=Q_{in,total}/[(T_{fs}-T_{coil,in})\times{(1-BF)}\times{\rho_{in}}]$$</div> 
-
-Where
-
-<span>$Q_{in,total}$</span>	total heating load for the zone (W)
-
-<span>$T_{coil,in}$</span>	temperature of the entering air of the indoor unit (°C)
-
-<span>$\rho_{in}$</span>density of indoor air,<span>$f_{\rho}(T_{in},W_{in})$</span>   (kg/m<sup>3</sup>)
-
-3)	Decide whether to modify <span>$SH$</span> for further indoor unit capacity reduction
-
-* If <span>$G_a$</span> < <span>$G_{a,min}$</span> (e.g., <span>$0.7\times$</span><span>$G_{a,rate}$</span>) go to Step 3h. 2
-
-* Else, directly go to Step 3h. 3 
-
-##### Step 3h.2:  Modify <span>$SC$</span> to modify the indoor unit capacity
-
-Set <span>$G_a$</span> at its minimum value (<span>$0.7\times$</span><span>$G_{a,rate}$</span>).
-
-The required coil surface temperature <span>$T_{fs}$</span> can be determined as described in Step 2.
-
-Given <span>$T_{fs}$</span> and <span>$T_e$</span>, <span>$SC$</span> can be determined using the equation shown in Step 1.3.
-
-* If <span>$SC$</span> > 20°C, Set <span>$SC$</span> as 20°C. On/Off control strategy may be implemented when needed.
-
-##### Step 3h.3: Total power consumption of the indoor unit
-
-Calculate electric power consumption by the indoor unit using the existing VAV fan model in EnergyPlus. Please refer to the current EnergyPlus Engineering Reference for more details.
-
-#### Additional energy consumption by defrost and crankcase heater 
-
-There may be additional energy consumption due to the defrost operation and crankcase heater operation. These components have no impact on the heat pump operations. The calculation methods in the VRF-FluidTCtrl model are the same as those in VRF-SysCurve model. Please refer to the VRF-SysCurve section for more details.
-
-
-### Zone Terminal Unit List
-
-The zone terminal unit list identifies the terminal units that are connected to a single variable refrigerant flow heat pump. The zone terminal unit list is used exclusively in the variable refrigerant flow (VRF) heat pump object (ref: AirConditioner:VariableRefrigerantFlow) and VRF zone terminal units (ref: ZoneHVAC: TerminalUnit:VariableRefrigerantFlow). Up to 20 terminal units may be connected to a single VRF outdoor condensing unit. This list is extensible if additional indoor terminal units are required. The following figure shows the connection scheme between the zone terminal units, the zone terminal unit list, and finally the VRF AC system. The zone terminal units are connected to the zone through zone inlet and outlet zone nodes. Each zone terminal unit is entered in a list which represents all terminal units connected to a single VRF AC system. And finally, the zone terminal unit list name is entered in the corresponding VRF AC object.
-
-![](media/image5454.png)
-
-Figure 249. Zone Terminal List connections in EnergyPlus objects
-
-
-#### References
-
-Raustad R. A variable refrigerant flow heat pump computer model in EnergyPlus, ASHRAE Transactions (2013), 119 (1):1–9.
-
-Hong T, Sun K, Zhang R, Hinokuma R, Kasahara S, Yura Y. Development and Validation of a New VRF Model in EnergyPlus. ASHRAE Winter Conference.
-
-
-Heat Exchangers <a name="HX"></a>
----------------
-
-### Air System Air-To-Air Sensible and Latent Effectiveness Heat Exchanger
-
-#### Overview
-
-The input object HeatExchanger:AirToAir:SensibleAndLatent provides a model for a generic, sensible and latent air-to-air heat exchanger that is an HVAC air system component that consists of a heat exchanger and primary/secondary airflow bypass dampers. The specific configuration of the component is shown in the following figure.
-
-![](media/image5455.png)
-
-
-
-Figure 250. Schematic of the Sensible and Latent Air-to-Air Heat Exchanger
-
-The sensible and latent air-to-air heat exchanger is typically used for exhaust or relief air heat recovery. Heat exchanger performance can be specified to transfer sensible energy, latent energy or both between the supply and exhaust air streams. The input requires no geometric data. Performance is defined by specifying sensible and/or latent effectiveness at 75% and 100% of the nominal (rated) supply air flow rate in both heating and cooling conditions (Table 74).
-
-Table 74.  Operating Conditions for Defining Heat Exchanger Performance
-
-<table>
-  <tr>
-    <th rowspan="2">Parameter</th>
-    <th colspan="2">Conditions</th>
-  </tr>
-  <tr>
-    <td>Heating</td>
-    <td>Cooling</td>
-  </tr>
-  <tr>
-    <td>Entering supply air temperature:<BR>Dry-bulb<BR>Wet-bulb</td>
-    <td><BR>1.7°C (35°F)<BR>0.6°C (33°F)</td>
-    <td><BR>35°C (95°F)<BR>26°C (78°F)</td>
-  </tr>
-  <tr>
-    <td>Entering exhaust air temperature:<BR>Dry-bulb<BR>Wet-bulb</td>
-    <td><BR>21°C (70°F)<BR>14°C (58°F)</td>
-    <td><BR>24°C (75°F)<BR>17°C (63°F)</td>
-  </tr>
-  <tr>
-    <td colspan="3">Note: Conditions consistent with the Air-Conditioning and Refrigeration Institute’s Standard 1060 (ARI 2001).</td>
-  </tr>
-</table>
-
-Heat exchange between the supply and exhaust air streams occurs whenever the unit is scheduled to be available (availability schedule) and supply/exhaust air flows are present. This heat exchanger object can be used in conjunction with a conventional air-side economizer (i.e., specify an appropriate economizer control type in the Controller:OutdoorAir object), whereby heat exchange is suspended whenever the air-side economizer is active (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped). This object is also able to suspend heat exchange for the purpose of providing free cooling operation in the absence of a conventional air-side economizer (i.e., specify MinimumFlowWithBypass in the Controller:Outside Air object). Suspension of heat exchange during economizer mode may be customized as necessary using the economizer lockout field. Note that the Economizer Type must be set to something other than NoEconomizer for this control interaction to function.
-
-Several methods of frost control are available to warm the heat exchanger core to prevent frost formation. Available methods are preheat, exhaust only, exhaust air recirculation, and minimum exhaust temperature. Preheat frost control uses a separate heater object placed in the supply inlet air stream to keep the air temperature above the frost threshold temperature. All other frost control methods are modeled within this heat exchanger object.
-
-This heat exchanger object can also control the supply air outlet temperature to a setpoint when a setpoint manager and temperature schedule are used. This temperature control is accomplished through wheel speed modulation or bypassing supply air around the heat exchanger to maintain the desired setpoint and avoid overheating or overcooling the supply air.
-
-#### Model Description
-
-The heat exchanger object models energy transfer between the supply air stream and the exhaust air stream according to the effectiveness values that are specified by the user in the input data file (see IO Reference Document, HeatExchanger:AirToAir:SensibleAndLatent). The operating volumetric air flow rate through the heat exchanger (i.e., the average of the actual supply and exhaust air flow rates for the simulation time step) should be between 50% and 130% of the nominal supply air flow rate specified for the heat exchanger. Operating air flow rates outside this range result in a warning message and a recommendation to adjust air flow rates to within the appropriate range.
-
-The user must enter the sensible and latent effectiveness of the heat exchanger for heating and cooling conditions (Table 74) with balanced air flow (supply flow equal to the exhaust flow) at two flow rates: 75% and 100% of the nominal supply air flow rate. Heat exchanger manufacturers can typically provide this performance information, and it is also available for equipment contained in ARI’s Certified Product Directory for Air-to-Air Energy Recovery Ventilation Equipment (ARI 2003). Values may be entered for sensible effectiveness, latent effectiveness, or both. The model assumes default values of 0.0 for sensible and latent effectiveness, thus requiring the user to input representative values for the heat exchanger being modeled.
-
-To obtain the “operating� effectiveness of the heat exchanger at different air flow rates, the model first calculates the average volumetric air flow rate through the heat exchanger (average of the supply and exhaust air flow rates) for each simulation time step. Air flows through the heat exchanger may be unbalanced (supply greater than exhaust, or vice versa), but an unbalanced air flow ratio greater than 2:1 is not recommended  (beyond this range a warning message is issued). The model determines the operating effectiveness of the heat exchanger by linear interpolation or extrapolation of the 100% flow and 75% flow effectiveness values specified in the input data file, using the average volumetric air flow rate through the heat exchanger. Extrapolation is allowed down to 50% and up to 130% of the nominal supply air flow rate (beyond this range a warning message is issued).
-
-<span>\({\varepsilon_{operating,sensible}} = {\varepsilon_{sensible,75\% \,flow}} + ({\varepsilon_{sensible,100\% \,flow}} - {\varepsilon_{sensible,75\% \,flow}})\left( {\frac{{H{X_{flowratio}} - 0.75}}{{1 - 0.75}}} \right)\)</span>  
-
-<div>$${\varepsilon_{operating,latent}} = {\varepsilon_{latent,75\% \,flow}} + ({\varepsilon_{latent,100\% \,flow}} - {\varepsilon_{latent,75\% \,flow}})\left( {\frac{{H{X_{flowratio}} - 0.75}}{{1 - 0.75}}} \right)$$</div>
-
-*where*:
-
-<span>\({\varepsilon_{operating,sensible}}\)</span> = operating sensible effectiveness of the heat exchanger
-
-<span>\({\varepsilon_{operating,latent}}\)</span>    = operating latent effectiveness of the heat exchanger
-
-<span>\({\varepsilon_{sensible,75\% \,flow}}\)</span>  =  sensible effectiveness at 75% airflow condition
-
-<span>\({\varepsilon_{sensible,100\% \,flow}}\)</span> =  sensible effectiveness at 100% airflow condition
-
-<span>\({\varepsilon_{latent,75\% \,flow}}\)</span>  =  latent effectiveness at 75% airflow condition
-
-<span>\({\varepsilon_{latent,100\% \,flow}}\)</span> =  latent effectiveness at 100% airflow condition
-
-<span>\(H{X_{flowratio}}\)</span> = the ratio of the average operating volumetric air flow rate [(supply flow plus exhaust flow) / 2.0] to the nominal supply air flow rate
-
-If the heat exchanger’s supply air inlet temperature is less than the exhaust air inlet temperature, the operating sensible and latent effectivenesses are calculated using the 75% and 100% heating condition values; otherwise, the 75% and 100% cooling effectiveness values are used in Equations and .
-
-The supply air conditions leaving the heat exchanger are determined using the heat exchanger operating effectiveness calculated above, the ratio of the air stream with the minimum heat capacity rate to the supply air stream heat capacity rate, and the difference in temperature or humidity ratio between the supply and exhaust inlet air:
-
-<div>$$\mathop m\limits^ \bullet  cp,\min \, = MIN(\mathop m\limits^ \bullet  cp,\sup \,,\,\mathop {\,m}\limits^ \bullet  cp,exh)$$</div>
-
-<div>$${T_{SupAirOut}} = {T_{SupAirIn}} + {\varepsilon_{operating,sensible}}\left( {\frac{{\mathop m\limits^ \bullet  cp,\min }}{{\mathop m\limits^ \bullet  cp,\sup }}} \right)({T_{ExhAirIn}} - {T_{SupAirIn}})$$</div>
-
-<div>$${\omega_{SupAirOut}} = {\omega_{SupAirIn}} + {\varepsilon_{operating,latent}}\left( {\frac{{\mathop m\limits^ \bullet  cp,\min }}{{\mathop m\limits^ \bullet  cp,\sup }}} \right)({\omega_{ExhAirIn}} - {\omega_{SupAirIn}})$$</div>
-
-*where*:
-
-<span>\(\mathop m\limits^ \bullet  cp,\min \)</span>           = minimum heat capacity rate (W/K)
-
-<span>\(\mathop m\limits^ \bullet  cp,\sup \)</span>            = heat capacity rate of the supply air stream (W/K)
-
-<span>\(\mathop {\,m}\limits^ \bullet  cp,exh\)</span>           = heat capacity rate of the exhaust air stream (W/K)
-
-*T<sub>SupAirOut</sub>*<sub>                     </sub> = supply air temperature leaving the heat exchanger (°C)
-
-*T<sub>SupAirIn</sub>*<sub>                         </sub> = supply air inlet temperature (°C)
-
-*T<sub>ExhAirIn</sub>*<sub>                         </sub> = exhaust air inlet temperature (°C)
-
-<span>\({\omega_{SupAirOut}}\)</span>          = supply air humidity ratio leaving the heat exchanger (kg/kg)
-
-<span>\({\omega_{SupAirIn}}\)</span>           = supply air inlet humidity ratio (kg/kg)
-
-<span>\({\omega_{ExhAirIn}}\)</span>           = exhaust air inlet humidity ratio (kg/kg)
-
-Using the supply air outlet temperature and humidity ratio, the enthalpy of the supply air leaving the heat exchanger is calculated.
-
-<div>$${h_{SupAirOut}} = PsyHFnTdbW({T_{SupAirOut}},{\omega_{SupAirOut}})$$</div>
-
-where:
-
-*h<sub>SupAirOut</sub>*<sub>             </sub>= enthalpy of the supply air leaving the heat exchanger (J/kg)
-
-*PsyHFnTdbW* = psychrometric routine calculating air enthalpy as a function of
-
-    temperature and humidity ratio
-
-If the predicted conditions of the supply air leaving the heat exchanger exceed the saturation curve (&gt;100% RH), then the temperature and humidity ratio of the air are reset to saturated conditions (= 100% RH) at the enthalpy condition calculated above (*h<sub>SupAirOut</sub>).*
-
-Next, the sensible and total heat recovery rates of the heat exchanger are calculated:
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible}} = \left( {\mathop m\limits^ \bullet  cp,\sup } \right)({T_{SupAirIn}} - {T_{SupAirOut}})$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Total}} = {\mathop m\limits^ \bullet_{SupAir}}({h_{SupAirIn}} - {h_{SupAirOut}})$$</div>
-
-where:
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible}}$$</div>            = sensible heat recovery rate (W)
-
-<span>\({\mathop Q\limits^ \bullet_{Total}}\)</span>               = total heat recovery rate (W)
-
-*h<sub>SupAirIn</sub>*            = supply air inlet enthalpy (J/kg)
-
-<span>\({\mathop m\limits^ \bullet_{SupAir}}\)</span>             = mass flow rate of the supply air stream (kg/s)
-
-The conditions of the exhaust (secondary) air leaving the heat exchanger are then calculated:
-
-<div>$${T_{ExhAirOut}} = {T_{ExhAirIn}}\, + \,\,\frac{{{{\mathop Q\limits^ \bullet  }_{Sensible}}}}{{\mathop m\limits^ \bullet  cp,exh}}$$</div>
-
-<div>$${h_{ExhAirOut}} = {h_{ExhAirIn}}\, + \,\,\frac{{\mathop Q\limits^ \bullet  {\,_{Total}}}}{{{{\mathop m\limits^ \bullet  }_{_{ExhAir}}}}}$$</div>
-
-<div>$${\omega_{ExhAirOut}} = PsyWFnTdbH({T_{ExhAirOut}},{h_{ExhAirOut}})$$</div>
-
-*where*:
-
-*T<sub>ExhAirOut</sub>*<sub>                     </sub> = exhaust air temperature leaving the heat exchanger (°C)
-
-*h<sub>ExhAirOut</sub>*           = exhaust air enthalpy leaving the heat exchanger (J/kg)
-
-<span>\({\mathop m\limits^ \bullet_{ExhAir}}\)</span>             = mass flow rate of the exhaust air stream (kg/s)
-
-<span>\({\omega_{ExhAirOut}}\)</span>          = exhaust air humidity ratio leaving the heat exchanger (kg/kg)
-
-*PsyWFnTdbH* = psychrometric routine calculating air humidity ratio as a function of temperature and enthalpy
-
-As was done for the supply air, calculated exhaust air conditions beyond the saturation curve are reset to saturation conditions at the calculated air enthalpy value.
-
-Once the air conditions leaving each side of the heat exchanger (supply and exhaust) are calculated, this air is blended with any bypass air that was directed around the heat exchanger core to determine the final air conditions leaving the heat exchanger unit. These outlet air conditions are used in Equations and to determine the sensible and total heat recovery rate for the overall heat exchanger unit. The latent heat recovery rate for the overall unit is then calculated as the difference between the total and sensible heat recovery rates:
-
-<div>$${\mathop Q\limits^ \bullet_{Latent}} = {\mathop Q\limits^ \bullet_{Total}}\,\, - \,{\mathop {\,Q}\limits^ \bullet_{Sensible}}$$</div>
-
-Heat recovery electric power is the electric consumption rate of the unit in watts. The nominal electric power rate for the heat exchanger is specified in the input data file, and can be used to model controls (transformers, relays, etc.) and/or a motor for a rotary heat exchanger. The model assumes that this electric power is consumed whenever the heat exchanger is scheduled to operate and supply/exhaust air flow rates exist. The electric power is assumed to be zero for all other times or if heat exchange is suspended to provide free cooling (economizer operation). None of this electric power is assumed to contribute thermal load to either of the heat exchanger air streams.
-
-At the end of each HVAC simulation time step, this object reports the sensible, latent and total heat recovery rates for the overall unit as calculated above. The heat recovery rates are reported separately for times when the supply air is heated and when it is cooled (Ref: HeatExchanger:AirToAir:SensibleAndLatent in the EnergyPlus Input Output Reference). The heat recovery electric power is also reported for each simulation time step. In addition to the heat recovery rates and electric power, heating/cooling energy transferred to the supply air and the electric energy consumption by the heat exchanger unit are calculated for the time step being reported as follows:
-
-<div>$$\,{Q_{SensibleCooling}} = \,\,{\mathop Q\limits^ \bullet_{SensibleCooling}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.$$</div>
-
-<div>$$\,{Q_{LatentCooling}} = \,\,{\mathop Q\limits^ \bullet_{LatentCooling}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.$$</div>
-
-<div>$$\,{Q_{TotalCooling}} = \,\,{\mathop Q\limits^ \bullet_{TotalCooling}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.$$</div>
-
-<div>$$\,{Q_{SensibleHeating}} = \,\,{\mathop Q\limits^ \bullet_{SensibleHeating}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.$$</div>
-
-<div>$$\,{Q_{LatentHeating}} = \,\,{\mathop Q\limits^ \bullet_{LatentHeating}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.$$</div>
-
-<div>$$\,{Q_{TotalHeating}} = \,\,{\mathop Q\limits^ \bullet_{TotalHeating}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.$$</div>
-
-<div>$$\,{E_{HXUnit}} = \,\,{P_{HXUnit}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.$$</div>
-
-where:
-
-<sub><span>\({Q_{SensibleCooling}}\)</span>             </sub>= output variable ‘Heat Exchanger Sensible Cooling Energy, J’
-
-<span>\(\,{\mathop Q\limits^ \bullet_{SensibleCooling}}\)</span>          = output variable ‘Heat Exchanger Sensible Cooling Rate, W’ = <div>$${\mathop Q\limits^ \bullet_{Sensible}}$$</div>
-
-                                   during times when the supply air is cooled
-
-*TimeStepSys*           = HVAC system simulation time step, hr
-
-<sub><span>\({Q_{LatentCooling}}\)</span>                               </sub>= output variable ‘Heat Exchanger Latent Cooling Energy, J’
-
-<span>\(\,{\mathop Q\limits^ \bullet_{LatentCooling}}\)</span>           = output variable ‘Heat Exchanger Latent Cooling Rate, W’ = <div>$${\mathop Q\limits^ \bullet_{Latent}}$$</div>
-
-   during times when the supply air is dehumidified
-
-<sub><span>\({Q_{TotalCooling}}\)</span>                 </sub>= output variable ‘Heat Exchanger Total Cooling Energy, J’
-
-<span>\(\,{\mathop Q\limits^ \bullet_{TotalCooling}}\)</span>             = output variable ‘Heat Exchanger Total Cooling Rate, W’ = <span>\({\mathop Q\limits^ \bullet_{Total}}\)</span>during
-
-    times when the supply air enthalpy is reduced
-
-<sub><span>\({Q_{SensibleHeating}}\)</span>             </sub>= output variable ‘Heat Exchanger Sensible Heating Energy, J’
-
-<span>\(\,{\mathop Q\limits^ \bullet_{SensibleHeating}}\)</span>          = output variable ‘Heat Exchanger Sensible Heating Rate, W’ = <div>$${\mathop Q\limits^ \bullet_{Sensible}}$$</div>
-
-   during times when the supply air is heated
-
-<sub><span>\({Q_{LatentHeating}}\)</span>                               </sub>= output variable ‘Heat Exchanger Latent Heating Energy, J’
-
-<sub><span>\({Q_{LatentHeating}}\)</span>                               </sub>= output variable ‘Heat Exchanger Latent Gain Energy, J’
-
-<span>\(\,{\mathop Q\limits^ \bullet_{LatentHeating}}\)</span>           = output variable ‘Heat Exchanger Latent Gain Rate, W’ = <div>$${\mathop Q\limits^ \bullet_{Latent}}$$</div> during times when the supply air is humidified
-
-<sub><span>\({Q_{TotalHeating}}\)</span>                 </sub>= output variable ‘Heat Exchanger Total Heating Energy, J’
-
-<span>\(\,{\mathop Q\limits^ \bullet_{TotalHeating}}\)</span>             = output variable ‘Heat Exchanger Total Heating Rate, W’ = <span>\({\mathop Q\limits^ \bullet_{Total}}\)</span>during times when the supply air enthalpy is increased
-
-<span>\(\,{E_{HXUnit}}\)</span>                  = output variable ‘Heat Exchanger Electric Energy, J’
-
-<span>\({P_{HXUnit}}\)</span>                   = output variable ‘Heat Exchanger Electric Power, W’
-
-#### Frost Control Methods
-
-In cold weather, frost can form on the heat exchanger causing a reduction in air flow and heat recovery performance. Various strategies can be employed to limit frost formation. Heat exchangers that transfer total energy (sensible plus latent) usually have a lower frost threshold temperature than sensible-only heat exchangers. Frost threshold temperatures for sensible-only heat exchangers may be -1°C to -12°C for plate and rotary heat exchangers respectively, while those for comparable total (sensible plus latent) heat exchangers may be 10°C lower. The frost threshold temperature for a specific application is dependent on the exhaust air dry-bulb temperature and relative humidity, heat exchanger type (e.g., sensible-only or total heat exchange, flat plate or rotary), and the heat exchanger effectiveness. Consult manufacturer’s literature to obtain specific frost threshold temperatures for the heat exchanger being modeled.
-
-Four frost control strategies can be modeled for this air-to-air heat exchanger unit. Each of these four strategies is discussed in detail below.
-
-#### Preheat
-
-One method to control frost formation is to preheat the cold outdoor (supply) air entering the heat exchanger. When a preheat coil is used for frost control, a separate heating coil object must be placed in the supply air stream at the inlet to the heat exchanger (Coil:Heating:Water, Coil:Heating:Electric or Coil:Heating:Gas). The preheat coil should be controlled to maintain a minimum supply air inlet temperature thereby eliminating frost buildup on the heat exchanger core. When modeling preheat frost control, specify “None� as the frost control method in the heat exchanger object. When modeling this heat exchanger as part of an air loop, refer to the objects AirLoopHVAC:OutdoorAirSystem and SetpointManager:Scheduled the EnergyPlus Input Output Reference for additional information on specifying a preheat coil and controlling its supply air temperature.This frost control method is not currently available when this heat exchanger is being used as part of the compound object ZoneHVAC:EnergyRecoveryVentilator.
-
-#### Exhaust Only
-
-This method of frost control bypasses the incoming supply air around the heat exchanger core thereby warming the core using the exiting exhaust air. This method is similar to ‘supply air off’ frost control where the supply air fan is turned off for a predetermined period of time while the exhaust air fan continues to operate. For the ‘supply air off’ method, the supply air flow is stopped for a period of time thereby reducing the ventilation air supplied to the zone(s). In addition, the building may be negatively pressurized for the period of time that the supply air flow is stopped since the exhaust air fan continues to operate. On the other hand, the ‘exhaust only’ method of frost control modeled by EnergyPlus continues to provide outdoor ventilation air to the zone(s), but this air is simply bypassed around the heat exchanger core for a portion of the time and the potential problem with negatively pressurizing the building is avoided. Since the supply airflow rate through the heat exchanger core is purposely reduced to control frost formation, average volumetric airflow rates below 50% of nominal are allowed when this frost control is active and no warning message is issued.
-
-The user enters a threshold temperature, an initial defrost time fraction, and a rate of defrost time fraction increase. When the temperature of the supply air (e.g., outdoor air) entering the heat exchanger is equal to or below the specified threshold temperature, the fractional amount of time that the supply air is bypassed around the heat exchanger core is determined from the following equation:
-
-<div>$${X_{DefrostTime}} = {X_{Initial}} + {X_{RateofIncrease}}({T_{Threshold}} - {T_{SupAirIn}})$$</div>
-
-where:
-
-<span>\({X_{DefrostTime}}\)</span>  = Fractional time period for frost control <span>\(\left( {0\,\, \le \,\,\,{X_{DefrostTime}}\,\, \le \,\,1} \right)\)</span>
-
-<span>\({X_{Initial}}\)</span>        = Initial defrost time fraction
-
-<span>\({X_{RateofIncrease}}\)</span>= Rate of defrost time fraction increase (K<sup>-1</sup>)
-
-<span>\({T_{Threshold}}\)</span>     = Threshold temperature (°C)
-
-<span>\({T_{SupAirIn}}\)</span>       = Supply air inlet temperature (°C)
-
-During the defrost time, supply air flow is fully bypassed around the heat exchanger core and no heat transfer takes place. For the remainder of the time period, no air is bypassed and full heat exchange is achieved. The average supply air flow bypassed around the heat exchanger core is calculated as follows:
-
-<div>$${\mathop m\limits^ \bullet_{_{SupAirBypass}}} = ({X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAir}}}$$</div>
-
-To determine the average heat transfer rates for the simulation time step, the supply air outlet conditions are first calculated as if the heat exchanger were not in defrost mode (see previous section, Model Description). The sensible and total heat transfer rates are then calculated and multiplied by the fractional time period that the heat exchanger is not in defrost mode (1-*X<sub>DefrostTime</sub>*).
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible}} = (1 - {X_{DefrostTime}})\left( {\mathop m\limits^ \bullet  cp,\sup } \right)({T_{SupAirIn}} - {T_{SupAirOut}})$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Total}} = (1 - {X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAir}}}({h_{SupAirIn}} - {h_{SupAirOut}})$$</div>
-
-Once the average heat transfer rates are determined, the average conditions of the supply air exiting the overall heat exchanger unit are calculated as follows:
-
-<div>$${T_{SupAirOut}} = {T_{SupAirIn\,}}\,\,\, - \,\,\,\frac{{{{\mathop Q\limits^ \bullet  }_{Sensible}}}}{{\mathop m\limits^ \bullet  cp,\sup }}$$</div>
-
-<div>$${h_{SupAirOut}} = {h_{SupAirIn}}\,\,\, - \,\,\,\frac{{{{\mathop Q\limits^ \bullet  }_{_{Total}}}}}{{{{\mathop m\limits^ \bullet  }_{_{SupAir}}}}}$$</div>
-
-<div>$${\omega_{SupAirOut}} = PsyWFnTdbH({T_{SupAirOut}},{h_{SupAirOut}})$$</div>
-
-As described previously, if the predicted conditions of the exiting supply air exceed the saturation curve (&gt;100% RH), then the temperature and humidity ratio of the air are reset to saturated conditions (= 100% RH) at the enthalpy condition calculated above (*h<sub>SupAirOut</sub>).*If the supply air temperature is reset, the average sensible heat transfer rate is recalculated before the exhaust air outlet conditions are determined:
-
-<div>$${T_{ExhAirOut}} = {T_{ExhAirIn}}\,\,\, + \,\,\,\frac{{{{\mathop Q\limits^ \bullet  }_{Sensible}}}}{{\mathop m\limits^ \bullet  cp,exh}}$$</div>
-
-<div>$${h_{ExhAirOut}} = {h_{ExhAirIn}}\,\,\,\, + \,\,\,\frac{{{{\mathop Q\limits^ \bullet  }_{_{Total}}}}}{{{{\mathop m\limits^ \bullet  }_{_{ExhAir}}}}}$$</div>
-
-<div>$${\omega_{ExhAirOut}} = PsyWFnTdbH({T_{ExhAirOut}},{h_{ExhAirOut}})$$</div>
-
-#### Exhaust Air Recirculation
-
-This method of frost control routes exhaust (outlet) air back through the supply side of the heat exchanger to warm the core. Since this method routes exhaust air back into the building, the building is typically not depressurized when this frost control is active. However, the incoming supply (outdoor ventilation) air flow is stopped for the fractional period of time that frost control is active. If significant periods of time exist when outdoor temperatures are below the selected threshold temperature and outdoor ventilation air is continuously required, an alternative method of frost control should be considered.
-
-The user enters a threshold temperature, an initial defrost time fraction, and a rate of defrost time fraction increase. When the temperature of the inlet supply air (e.g., outdoor air) is equal to or below the specified threshold temperature, the fractional amount of time that this heat exchanger frost control strategy is active is determined from the following equation:
-
-<div>$${X_{DefrostTime}} = {X_{Initial}} + {X_{RateofIncrease}}({T_{Threshold}} - {T_{SupAirIn}})$$</div>
-
-The air mass flow rate of the supply air leaving the heat exchanger unit is then calculated using the defrost time fraction calculated above the mass flow rates of supply and exhaust air entering the unit.
-
-<div>$${\mathop m\limits^ \bullet_{_{SupAirOut}}} = (1 - {X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAirIn}}}\,\, + \,\,{X_{DefrostTime}}{\mathop m\limits^ \bullet_{_{ExhAirIn}}}$$</div>
-
-The model assumes that no heat exchange occurs during defrost, and the average supply supply air conditions are simply a blend of the conditions when the unit is not in defrost and the exhaust air inlet conditions during defrost operation:
-
-<div>$${T_{SupAirOut}} = \,\,\frac{{(1 - {X_{DefrostTime}}){{\mathop m\limits^ \bullet  }_{_{SupAirIn}}}{T_{SupAirOut,NoDefrost\,}} + \,\,{X_{DefrostTime}}{{\mathop m\limits^ \bullet  }_{_{ExhAirIn}}}{T_{ExhAirIn\,}}}}{{{{\mathop m\limits^ \bullet  }_{_{SupAirOut}}}}}$$</div>
-
-<div>$${\omega_{SupAirOut}} = \,\,\frac{{(1 - {X_{DefrostTime}}){{\mathop m\limits^ \bullet  }_{_{SupAirIn}}}{\omega_{SupAirOut,NoDefrost\,}} + \,\,{X_{DefrostTime}}{{\mathop m\limits^ \bullet  }_{_{ExhAirIn}}}{\omega_{ExhAirIn\,}}}}{{{{\mathop m\limits^ \bullet  }_{_{SupAirOut}}}}}$$</div>
-
-<div>$${h_{SupAirOut}} = PsyHFnTdbW({T_{SupAirOut}},{\omega_{SupAirOut}})$$</div>
-
-The operating effectivenesses of the heat exchanger are initially calculated according to Equations and assuming no defrost operation. Since the supply air flow across the heat exchanger core is not reduced during defrost operation, the sensible and latent effectiveness are therefore derated (for reporting purposes) in direct proportion to the fraction of time that frost control is not active.
-
-<div>$${\varepsilon_{operating,sensible}} = (1 - {X_{DefrostTime}}){\varepsilon_{operating,sensible}}$$</div>
-
-<div>$${\varepsilon_{operating,latent}} = (1 - {X_{DefrostTime}}){\varepsilon_{operating,latent}}$$</div>
-
-Since the exhaust outlet air is recirculated through the supply side of the heat exchanger core, the incoming supply air and exiting exhaust air flows are stopped for the fraction of the time when frost control is active. The average air mass flow rate at the supply air inlet and the exhaust air outlet nodes are therefore reduced accordingly.
-
-<div>$${\mathop m\limits^ \bullet_{_{SupAirIn}}} = (1 - {X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAirIn}}}$$</div>
-
-<div>$${\mathop m\limits^ \bullet_{_{ExhAirOut}}} = (1 - {X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{ExhAirOut}}}$$</div>
-
-The conditions of the exiting (outlet) exhaust air (temperature, humidity ratio and enthalpy) are reported as the values when frost control is not active (i.e., the conditions when exhaust air is actually leaving the unit).
-
-#### Minimum Exhaust Temperature
-
-With this frost control method, frost formation is avoided by continuously maintaining the temperature of the exhaust air leaving the heat exchanger core above a specified setpoint. The minimum exhaust air temperature is maintained by modulating heat exchanger rotational speed or by bypassing supply air around a plate heat exchanger. For this frost control method, the user must only enter the threshold (minimum) temperature.
-
-For the case of modulating heat exchanger rotation, the operating effectivenesses and outlet air conditions are first calculated as if the heat exchanger is not in defrost mode (see Model Description). If the resulting temperature of the exhaust air leaving the heat exchanger core is below the specified threshold temperature, then the operating effectivenesses are reduced as follows:
-
-<div>$${X_{DefrostTime}} = \frac{{({T_{Threshold}} - {T_{ExhAirOut}})}}{{({T_{ExhAirIn}} - {T_{ExhAirOut}})}}$$</div>
-
-<div>$${\varepsilon_{operating,sensible}} = (1 - {X_{DefrostTime}}){\varepsilon_{operating,sensible}}$$</div>
-
-<div>$${\varepsilon_{operating,latent}} = (1 - {X_{DefrostTime}}){\varepsilon_{operating,latent}}$$</div>
-
-The supply air and exhaust air outlet conditions are then recalculated using these reduced effectiveness values. Finally the sensible, latent and total heat recovery rates are calculated along with the unit’s electric power and electric consumption.
-
-The calculation procedure is slightly different for the case of a plate heat exchanger where the supply air is bypassed around the heat exchanger core. Since the volumetric air flow rate through the heat exchanger core is reduced when frost control is active, an iterative process is used to determine the operating effectiveness of the heat exchanger. The operating effectivenesses and outlet air conditions are first calculated as if the heat exchanger is not in defrost mode (see Model Description). If the resulting temperature of the exhaust air leaving the heat exchanger core is below the specified threshold temperature, then the fractional defrost time is calculated as follows:
-
-<div>$${X_{DefrostTime}} = \frac{{({T_{Threshold}} - {T_{ExhAirOut}})}}{{({T_{ExhAirIn}} - {T_{ExhAirOut}})}}$$</div>
-
-The iteration process then begins to determine the heat exchanger effectiveness and the exhaust air outlet temperature as if frost control were active. The operating mass flow rate through the supply side of the heat exchanger core is calculated.
-
-*Beginning of iteration process:*
-
-<div>$${\mathop m\limits^ \bullet_{_{SupAirCore}}} = (1 - {X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAirIn}}}$$</div>
-
-<div>$${\mathop m\limits^ \bullet_{_{SupAirBypass}}} = ({X_{DefrostTime}}){\mathop m\limits^ \bullet_{_{SupAirIn}}}$$</div>
-
-The ratio of average volumetric flow rate through the heat exchanger core to heat exchanger’s nominal volumetric flow rate (*HX<sub>flowratio</sub>*) is then determined and used to calculate the operating effectiveness of the heat exchanger using Equations and . Since the supply airflow rate through the heat exchanger core is purposely reduced to control frost formation, average volumetric airflow rates below 50% of nominal are allowed and no warning message is issued. Supply air outlet temperature (leaving the heat exchanger core), sensible heat transfer, and exhaust air outlet temperature are then calculated using the revised heat exchanger effectiveness.
-
-<div>$${T_{SupAirOut}} = {T_{SupAirIn}} + {\varepsilon_{operating,sensible}}\left( {\frac{{\mathop m\limits^ \bullet  cp,\min }}{{\mathop m\limits^ \bullet  cp,\sup }}} \right)({T_{ExhAirIn}} - {T_{SupAirIn}})$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible}} = (1 - {X_{DefrostTime}})\left( {\mathop m\limits^ \bullet  cp,\sup } \right)({T_{SupAirInlet}} - {T_{SupAirOutlet}})$$</div>
-
-<div>$${T_{ExhAirOut}} = {T_{ExhAirIn}} + \frac{{{{\mathop Q\limits^ \bullet  }_{Sensible}}}}{{\mathop m\limits^ \bullet  cp,exh}}$$</div>
-
-The error between the exhaust outlet temperature and the threshold temperature for frost control and a new defrost time fraction are subsequently calculated.
-
-<div>$$Error = {T_{ExhAirOut}} - {T_{Threshold}}$$</div>
-
-<div>$${X_{DefrostTime}} = \,{X_{DefrostTime}}\,\left( {\frac{{{T_{ExhAirIn}} - {T_{ExhAirOut}}}}{{{T_{ExhAirIn}} - {T_{Threshold}}}}} \right)$$</div>
-
-*End of iteration process:*
-
-The iteration process ends when the calculated error is within an error tolerance of 0.001.  The air streams passing through the heat exchanger core and bypassing the core through the bypass damper are then blended together to provide the air conditions leaving the heat exchanger unit. Finally the sensible, latent and total heat recovery rates are calculated along with the unit’s electric power and electric consumption.
-
-#### Economizer Operation
-
-A conventional air-side economizer may be used in conjunction with this heat exchanger object. The air-side economizer is specified through the use of an outside air controller (see object: Controller:OutdoorAir). Specify the appropriate economizer control type, and provide the required control points and air flow rates as defined in the outside air controller object. Energy transfer provided by the heat exchanger will be suspended whenever free cooling is available (i.e., when the air-side economizer is activated) and *the user specified economizer lockout input is specified as Yes*. For plate heat exchangers, heat transfer is suspended by fully bypassing the supply and exhaust air around the heat exchanger core. For rotary heat exchangers, air flows continue through the core but it is assumed that heat exchanger rotation is stopped.
-
-Heat exchange can also be suspended for the purposes of providing free cooling operation in the absence of a conventional air-side economizer. In this case specify “MinimumFlowWithBypass� as the economizer choice and again provide the required control points as defined in the outside air controller object. Energy transfer provided by the heat exchanger will be suspended whenever free cooling is available and *the user specified economizer lockout input is specified as Yes*, however the supply air flow rate will remain at the minimum value specified in the outside air controller object. Note that the Economizer Type must be set to something other than NoEconomizer for this control interaction to function.
-
-If economizer operation is not required, specify “NoEconomizer� as the economizer control type in the outside air controller object. The heat exchanger will operate according to its availability schedule and free cooling will not be provided. . If economizer operation *is* required and the heat exchanger *should not* provide free cooling, specify the input for the heat exchanger’s economizer lockout as No and heat recovery will remain active during economizer mode.
-
-Heat recovery for this heat exchanger may also be suspended during a high humidity control event (see object Controller:OutdoorAir) in a similar manner. Specifying Yes for economizer lockout will also suspend heat recovery when high humidity control is activated. The default value for economizer lockout is Yes and must be specifically entered as No to disable the economizer or high humidity control lockout feature.
-
-#### Supply Air Outlet Temperature Control
-
-This heat exchanger object can also control the supply air outlet temperature to a setpoint to avoid overheating or overcooling the supply air. This temperature control is accomplished through wheel speed modulation or bypassing supply air around the heat exchanger. To model this temperature control, the user must specify ‘Yes’ for the Supply Air Outlet Temperature Control field in this heat exchanger object, and a separate setpoint manager (see object: SetpointManager:Scheduled) and temperature schedule  must be specified for the heat exchanger unit’s supply air outlet node.
-
-This control strategy is typically used in conjunction with economizer operation (see object Controller:OutdoorAir), and an example control profile is shown in the figure below. When the outdoor air temperature falls to the specified maximum limit for economizer operation, heat exchange is suspended (air is fully bypassed around the heat exchanger core or heat exchanger rotation is stopped). The figure below shows economizer operation being initiated based on outdoor temperature but other triggers can be used (e.g. differential temperature [outdoor temperature with respect to exhaust air temperature], single point enthalpy or differential enthalpy). Heat exchange remains suspended until the outdoor temperature falls to the minimum temperature (temperature lower limit) for economizer control. The setpoint for the supply air outlet temperature control should match the economizer temperature lower limit.
-
-As the outdoor air temperature falls further below the setpoint for the supply air outlet temperature (same as the economizer lower temperature limit), the heat exchanger bypass dampers will modulate closed to maintain the desired supply air temperature for a plate heat exchanger. For a rotary heat exchanger the rotary heat exchanger speed will gradually increase to maintain the desired supply air temperature. Modulation of heat exchanger performance will continue until the supply air temperature setpoint can no longer be maintained. This control will attempt to achieve the desired temperature set point whether the heat exchanger is cooling or heating the supply air stream. Care should be used to set the supply outlet air temperature set point to the desired value for proper control.
-
-![](media/image5550.png)
-
-Figure 251.  Air to Air Heat Exchanger with Supply Air Temperature Control
-
-Other types of temperature setpoint control may also be used. For example, the operation described here is used to minimize heating energy and proper control of the supply air temperature set point could also be used to minimize cooling energy or minimize both heating and cooling energy.
-
-#### References
-
-ARI. 2001. Rating Air-to-Air Heat Exchangers for Energy Recovery Ventilation Equipment. Arlington, Virginia: Air-Conditioning & Refrigeration Institute.
-
-ARI. 2003. Certified Product Directory for Air-to-Air Energy Recovery Ventilation Equipment. Arlington, Virginia: Air-Conditioning & Refrigeration Institute.
-
-### Air System Air-To-Air Flat Plate Heat Exchanger
-
-#### Overview
-
-The input object HeatExchanger:AirToAir:FlatPlate provides an NTU – effectiveness model of a static flat plate air-to-air heat exchanger. Humidity issues are ignored in this model. A full, detailed description of the model can be found in the reference.
-
-The inputs for the model are the design values for the primary air flow rate, primary air inlet and outlet temperature,  secondary air flow rate, and secondary air inlet temperature. No design UAs are required: instead, the ratio (at design conditions) of the primary *hA* to the secondary *hA* (*r<sub>hA</sub>*) is input. The flow configuration is also an input (counter, parallel, or crossflow).
-
-n An important feature of this model is that the heat exchanger total *UA* is a time varying function of the primary and secondary mass flow rates and inlet temperatures.
-
-#### Model Description
-
-The design inlet / outlet conditions determine a design effectiveness *eff*<sub>des</sub>. From the design capacity flow ratio, the flow arrangement, and *eff*<sub>des,</sub> the NTU – effectiveness formulas give the *NTU<sub>des</sub>* and *UA<sub>des</sub>*.
-
-The time varying calculations proceed as follows. First the *UA* is determined:
-
-<div>$$UA = U{A_{des}}({r_{hA}} + 1)/({({\dot m_{p,des}}{T_{p,des}}/{\dot m_p}{T_p})^{.78}} + {r_{hA}}{({\dot m_{s,des}}{T_{s,des}}/{\dot m_s}{T_s})^{.78}})$$</div>
-
-where *des* means *design*, *p* means *primary*, *s* means *secondary*, *T* is air stream temperature, and <span>\(\dot m\)</span>is air stream mass flow rate. From the *UA* and the capacity flow ratio the *NTU* is determined: <span>\(NTU = UA/{C_{\min }}\)</span>. Then the NTU – effectiveness formulas are used to calculate the effectiveness. From the effectiveness and the inlet conditions, outlet condtions are determined.
-
-#### Economizer Operation
-
-A conventional air-side economizer may be used in conjunction with this heat exchanger object. The air-side economizer is specified through the use of an outside air controller (see object: Controller:OutdoorAir). Specify the appropriate economizer control type, and provide the required control points and air flow rates as defined in the outside air controller object. Energy transfer provided by the heat exchanger will be suspended whenever free cooling is available (i.e., when the air-side economizer is activated) or high humidity control is active and *the user specified economizer lockout input is specified as Yes*. For this flat plate heat exchanger, heat transfer is suspended by fully bypassing the supply and exhaust air around the heat exchanger core. If the economizer lockout is specified as No, the flat plate heat exchanger is operational even when economizer or high humidity mode is active. The default value for economizer lockout is Yes and must be specifically entered as No to disable the economizer or high humidity control lockout feature.
-
-#### References
-
-M. Wetter. 1999. *Simulation Model: Air-To-Air Plate Heat Exchanger*, LBNL-42354. This document can be downloaded from [*http://simulationresearch.lbl.gov*](http://simulationresearch.lbl.gov).
-
-### Air System Air-To-Air Balanced Flow Desiccant Heat Exchanger
-
-#### Overview
-
-The input object HeatExchanger:Desiccant:BalancedFlow provides a model for a desiccant heat exchanger that is an HVAC component used to model both temperature (sensible) and moisture (latent) heat exchange between two air streams (Figure 252). The model assumes balanced air flow through the regeneration and process sides of the heat exchanger (i.e., regeneration and process air volume flow rates and face velocities are the same). Heat exchanger performance is specified through a performance data type object (e.g., Heat Exchanger:Desiccant:BalancedFlow:Performance Data Type 1). Refer to the EnergyPlus Input Output Reference for the specific input syntax for this desiccant heat exchanger object.
-
-![BalancedFlowDesiccantHeatExchanger\_Schematic](media/image5554.png)
-
-Figure 252. Schematic of the Balanced Flow Desiccant Heat Exchanger
-
-EnergyPlus has another air-to-air heat exchanger object for modeling sensible and latent heat transfer between two air streams that uses the input object HeatExchanger:AirToAir:SensibleAndLatent. That heat exchanger model uses effectiveness values specified by the user to determine exiting air conditions from each side of the heat exchanger. In contrast, the balanced flow desiccant heat exchanger references a performance data type object (e.g., HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1) which defines the model equations, user-specified model coefficients, and min/max limits for the model’s independent and dependent variables.
-
-#### Model Description
-
-This heat exchanger is a simple object that performs three basic functions:
-
-1.    Informs the associated performance data type object (e.g., HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1) if it should calculate heat exchange for a simulation time step, or if heat exchange is suspended for the time step (i.e., bypass air flow around a fixed-plate heat exchanger or stop the rotation of a rotary heat exchanger),
-
-2.    Passes the process and regeneration air inlet conditions (e.g., dry-bulb temperature, humidity ratio, air mass flow rate) to the associated performance data type object, and
-
-3.    Reports the total, sensible and latent cooling/heating rates and electric power based on the results from the performance data type model that is specified.
-
-While the desiccant heat exchanger object’s availability to provide heat exchange between the two air streams is determined by the user-specified availability schedule, other objects that call this heat exchanger object can also control its heat exchange during a simulation time step. Currently, this desiccant heat exchanger model can be referenced by two compound objects: CoilSystem:Cooling:DX:HeatExchangerAssisted and Dehumidifier:Desiccant:System, both of which are used to provide enhanced dehumidification over conventional systems. If this heat exchanger is referenced by a compound object, the compound object will control heat exchanger operation (i.e., tell the heat exchanger if heat exchange is needed or not for each simulation time step). Details for how the compound objects control exchanger operation are described elsewhere in this document (ref. CoilSystem:Cooling:DX:HeatExchangerAssisted and Dehumidifier:Desiccant:System).
-
-This desiccant heat exchanger object may also be specified directly in a AirLoopVHAC (air loop BranchList) or in an AirLoopHVAC:OutdoorAirSystem:EquipmentList without being referenced by a compound object. If specified directly in a AirLoopHVAC loop or AirLoopHVAC:OutdoorAirSystem:EquipmentList, then the heat exchanger can be controlled to provide heat exchange based on a maximum and/or minimum humidity setpoint placed on the process air outlet node (ref. SetpointManagers). If no humidity setpoints are provided on this node, then heat exchange will be provided whenever the heat exchanger is available to operate (via its availability schedule) and there is a temperature and/or humidity ratio difference between the two air streams. Further details regarding heat exchanger control via humidity setpoints on the process air outlet node are described in the section for the associated data type object (e.g., HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1).
-
-The balanced flow desiccant heat exchanger model first checks for three conditions to be true before calling the specified performance data type model to calculate heat exchanger performance:
-
-·        Non-zero air mass flow rates on the process and regeneration inlet air nodes,
-
-·        Desiccant heat exchanger is available to operate based on its availability schedule,
-
-·        If a compound object is calling this desiccant heat exchanger, it is requesting that heat exchange be provided.
-
-If any of these conditions is false, then heat exchange is suspended and the model simply passes the air conditions on the process and regeneration air inlet nodes to the respective outlet air nodes. In addition, the heat exchanger electric power is set to zero.
-
-If all of the above conditions are true, then heat exchange is active and the specified performance data type model is called to calculate the process and regeneration outlet air conditions and heat exchanger electric power. Immediately before this call to the performance data type model, a check is made to determine if the operating air flow rates through the heat exchanger (i.e., the actual air flow rates for the simulation time step) are equal (balanced flow). If a difference of more than 2% exists between the process and regeneration air flow rates at any time during the simulation, a warning is issued.
-
-After the specified performance data type model calculates the process/regeneration air outlet conditions and heat exchanger electric power, the balanced flow desiccant heat exchanger model uses that information to report overall performance. Specifically, the heat exchanger’s sensible, latent and total heating and cooling rates are calculated for the process air side of the heat exchanger. Since energy must be conserved, the same heating or cooling rates apply to the regeneration air stream although they are opposite in heat transfer direction (e.g., a sensible cooling rate on the process air side of the heat exchanger would indicate an equivalent sensible heating rate on the regeneration air side).
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible}} = \,{\mathop m\limits^ \bullet_{Proc}}C{p_{Proc,\,\,in}}\left( {{T_{Proc,\,\,out}}\, - \,{T_{Proc,\,\,in}}} \right)$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Total}} = \,{\mathop m\limits^ \bullet_{Proc}}\left( {{h_{Proc,\,\,out}}\, - \,{h_{Proc,\,\,in}}} \right)$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Latent}} = \,{\mathop Q\limits^ \bullet_{Total}}\, - \,{\mathop Q\limits^ \bullet_{Sensible}}$$</div>
-
-where:
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible}}$$</div>      = sensible heat transfer rate to the process air stream (W)
-
-<span>\({\mathop Q\limits^ \bullet_{Total}}\)</span>         = total heat transfer rate to the process air stream (W)
-
-<div>$${\mathop Q\limits^ \bullet_{Latent}}$$</div>        = latent heat transfer rate to the process air stream (W)
-
-<span>\({\mathop m\limits^ \bullet_{Proc}}\)</span>         = process air mass flow rate (kg/s)
-
-<span>\(C{p_{Proc,\,\,in}}\)</span>     = specific heat of inlet process air (J/kg-K)
-
-<span>\({T_{Proc,\,\,out}}\)</span>      = process air outlet temperature (°C)
-
-<span>\({T_{Proc,\,\,in}}\)</span>        = process air inlet temperature (°C)
-
-<span>\({h_{Proc,\,\,out}}\)</span>      = process air outlet enthalpy (J/kg)
-
-<span>\({h_{Proc,\,\,in}}\)</span>        = process air inlet enthalpy (J/kg)
-
-
-
-To simplify the accounting of heat exchanger performance, the sensible, latent, and total heat transfer rates for the process side of the heat exchanger are stored in cooling and heating report variables. For example, if the sensible heat transfer rate is negative, the absolute value is stored in a “cooling� rate report variable. Conversely, if the sensible heat transfer rate is positive, the value is stored in a “heating� rate report variable. Similar accounting is performed for the latent and total heat transfer rate variables as follows:
-
-<div> $$ IF\left( {{{\mathop Q\limits^ \bullet  }_{Sensible}} &lt;  = 0} \right){\mathop Q\limits^ \bullet_{SensibleCooling}} = ABS\left( {{{\mathop Q\limits^ \bullet  }_{Sensible}}} \right) $$ </div>
-
-<div>$$IF\left( {{{\mathop Q\limits^ \bullet  }_{Sensible}} > 0} \right){\mathop Q\limits^ \bullet_{SensibleHeating}} = {\mathop Q\limits^ \bullet_{Sensible}}$$</div>
-
-<div>$$IF\left( {{{\mathop Q\limits^ \bullet  }_{Latent}} &lt;  = 0} \right){\mathop Q\limits^ \bullet_{LatentCooling}} = ABS\left( {{{\mathop Q\limits^ \bullet  }_{Latent}}} \right)$$</div>
-
-<div>$$IF\left( {{{\mathop Q\limits^ \bullet  }_{Latent}} > 0} \right){\mathop Q\limits^ \bullet_{LatentHeating}} = {\mathop Q\limits^ \bullet_{Latent}}$$</div>
-
-<div>$$IF\left( {{{\mathop Q\limits^ \bullet  }_{Total}} &lt;  = 0} \right){\mathop Q\limits^ \bullet_{TotalCooling}} = ABS\left( {{{\mathop Q\limits^ \bullet  }_{Total}}} \right)$$</div>
-
-<div>$$IF\left( {{{\mathop Q\limits^ \bullet  }_{Total}} > 0} \right){\mathop Q\limits^ \bullet_{TotalHeating}} = {\mathop Q\limits^ \bullet_{Total}}$$</div>
-
-At the end of each HVAC simulation time step, this object reports the sensible, latent and total cooling/heating energy and electric consumption for the heat exchanger as follows:
-
-<div>$${Q_{SensibleCooling}} = {\dot Q_{SensibleCooling}}*TimeStepSys*3600.$$</div>
-
-<div>$${Q_{LatentCooling}} = {\dot Q_{LatentCooling}}*TimeStepSys*3600.$$</div>
-
-<div>$${Q_{TotalCooling}} = {\dot Q_{TotalCooling}}*TimeStepSys*3600.$$</div>
-
-<div>$${Q_{SensibleHeating}} = {\dot Q_{SensibleHeating}}*TimeStepSys*3600.$$</div>
-
-<div>$${Q_{LatentHeating}} = {\dot Q_{LatentHeating}}*TimeStepSys*3600.$$</div>
-
-<div>$${Q_{TotalHeating}} = {\dot Q_{TotalHeating}}*TimeStepSys*3600.$$</div>
-
-<div>$${E_{HXUnit}} = {P_{HXUnit}}*TimeStepSys*3600.$$</div>
-
-where:
-
-<sub><span>\({Q_{SensibleCooling}}\)</span>             </sub>= output variable ‘Heat Exchanger Sensible Cooling Energy, J’
-
-<span>\({\dot Q_{SensibleCooling}}\)</span>          = output variable ‘Heat Exchanger Sensible Cooling Rate, W’ = <div>$${\dot Q_{Sensible}}$$</div>
-
-                                   during times when the process air is cooled
-
-*TimeStepSys*           = HVAC system simulation time step, hr
-
-<sub><span>\({Q_{LatentCooling}}\)</span>               \\                </sub>= output variable ‘Heat Exchanger Latent Cooling Energy, J’
-
-<span>\({\dot Q_{LatentCooling}}\)</span>           = output variable ‘Heat Exchanger Latent Cooling Rate, W’ = <span>\({\dot Q_{Latent}}\)</span>
-
-   during times when the process air is dehumidified
-
-<sub><span>\({Q_{TotalCooling}}\)</span>                 </sub>= output variable ‘Heat Exchanger Total Cooling Energy, J’
-
-<span>\({\dot Q_{TotalCooling}}\)</span>             = output variable ‘Heat Exchanger Total Cooling Rate, W’ = <span>\({\dot Q_{Total}}\)</span>during
-
-    times when the process air enthalpy is reduced
-
-<sub><span>\({Q_{SensibleHeating}}\)</span>             </sub>= output variable ‘Heat Exchanger Sensible Heating Energy, J’
-
-<span>\({\dot Q_{SensibleHeating}}\)</span>          = output variable ‘Heat Exchanger Sensible Heating Rate, W’ = <span>\({\dot Q_{Sensible}}\)</span>
-
-   during times when the process air is heated
-
-<sub><span>\({Q_{LatentHeating}}\)</span>               </sub>= output variable ‘Heat Exchanger Latent Gain Energy, J’
-
-<span>\({\dot Q_{LatentHeating}}\)</span>           = output variable ‘Heat Exchanger Latent Gain Rate, W’ = <span>\({\dot Q_{Latent}}\)</span> during times when the process air is humidified
-
-<sub><span>\({Q_{TotalHeating}}\)</span>                 </sub>= output variable ‘Heat Exchanger Total Heating Energy, J’
-
-<span>\({\dot Q_{TotalHeating}}\)</span>             = output variable ‘Heat Exchanger Total Heating Rate, W’ = <span>\({\dot Q_{Total}}\)</span>during times when the process air enthalpy is increased
-
-<span>\({E_{HXUnit}}\)</span>                  = output variable ‘Heat Exchanger Electric Energy, J’
-
-<span>\({P_{HXUnit}}\)</span>                   = output variable ‘Heat Exchanger Electric Power, W’
-
-#### Economizer Operation
-
-A conventional air-side economizer may be used in conjunction with this heat exchanger object. The air-side economizer is specified through the use of an outside air controller (see object: Controller:OutdoorAir). Specify the appropriate economizer control type, and provide the required control points and air flow rates as defined in the outside air controller object. Energy transfer provided by the heat exchanger will be suspended whenever free cooling is available (i.e., when the air-side economizer is activated) or high humidity control is active and *the user specified economizer lockout input is specified as Yes*. For the desiccant heat exchanger, heat transfer is assumed to be provided by a rotating heat exchanger core. For this reason, air continues to flow through the core when the outdoor air economizer is active but it is assumed that the rotation of the heat exchanger core is stopped. If the economizer lockout is specified as No, the desiccant heat exchanger is operational even when economizer or high humidity mode is active. This specific type of heat exchanger is typically *not* controlled by an outdoor air economizer. For this reason, the default value for economizer lockout is No and must be specifically entered as Yes to enable the economizer or high humidity control lockout feature.
-
-#### Desiccant Heat Exchanger Performance Data
-
-##### Overview
-
-The input object HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 specifies a performance model and model coefficients for a balanced flow desiccant heat exchanger. The HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 object is referenced by a HeatExchanger:Desiccant:BalancedFlow object. This performance data object is used to specify the thermal performance and electric consumption of the heat exchanger. Some representative inputs for this object are provided in the EnergyPlus Reference DataSets (PerfCurves.idf).
-
-This model predicts the regeneration air stream outlet temperature and humidity ratio values based on the entering regeneration and process air stream temperature, humidity ratio and face velocity. The process air stream outlet humidity ratio and temperatures are calculated based on a simple heat and moisture balance. The model requires that the user enter the nominal volumetric flow rate and a nominal face velocity, electric power consumption, empirical model coefficients for the regeneration outlet air temperature and humidity ratio equations, and the applicable minimum and maximum values for both the independent and dependent variables for the empirical model coefficients provided. Refer to the EnergyPlus Input Output Reference for details regarding the input syntax for this object.
-
-##### Heat Exchanger Face Area and Air Velocity
-
-The user is required to enter a nominal volumetric air flow rate and a nominal face velocity. From these inputs, a heat exchanger face area (applicable for both the regeneration and process sides of the heat exchanger) is calculated and used to determine the operating face velocity during the simulation.
-
-<div>$${A_{face}}\, = \,{\raise0.7ex\hbox{${{V_{face,nom}}}$} \!\mathord{\left/ {\vphantom {{{V_{face,nom}}} {{{\mathop v\limits^ \bullet  }_{face,nom}}}}}\right.}\!\lower0.7ex\hbox{${{{\mathop v\limits^ \bullet  }_{face,nom}}}$}}$$</div>
-
-<div>$$RFV\, = \,{\raise0.7ex\hbox{${{{\mathop m\limits^ \bullet  }_{Reg,in}}}$} \!\mathord{\left/ {\vphantom {{{{\mathop m\limits^ \bullet  }_{Reg,in}}} {\left( {{\rho_{Std}}{A_{face}}} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {{\rho_{Std}}{A_{face}}} \right)}$}}$$</div>
-
-where:
-
-<span>\({A_{face}}\)</span>          = heat exchanger face area (m<sup>2</sup>)
-
-<span>\({V_{face,nom}}\)</span>      = nominal air volume flow rate specified for the heat exchanger (m<sup>3</sup>/s)
-
-<span>\({\mathop v\limits^ \bullet_{face,nom}}\)</span>      = nominal air face velocity specified for the heat exchanger (m/s)
-
-<span>\(RFV\)</span>         = face velocity of the regeneration (and process) air stream (m/s)
-
-<span>\({\mathop m\limits^ \bullet_{Reg,in}}\)</span>       = mass flow rate of the regeneration air stream (kg/s)
-
-<span>\({\rho_{Std}}\)</span>           = density of air at standard temperature and pressure [dry air at 20°C] (m<sup>3</sup>/kg)
-
-
-
-The face velocity calculated each simulation time step is used in the empirical equations (see ‘Model Calculations’ below) and should be within the minimum and maximum velocity boundaries specified for the model coefficients (see ‘Empirical Model Boundaries (Minimum and Maximum)‘ below). When the calculated air velocity exceeds one of the boundaries, a warning is issued and the velocity is reset to the appropriate boundary value before being passed to the empirical equations for calculating regeneration air outlet temperature and humidity ratio. If the user is confident in their empirical model coefficients, the minimum and maximum velocity boundaries may be expanded slightly (caution should be used here) to allow extrapolation of the empirical equations during the simulation.
-
-##### Model Calculations
-
-The model coefficients may be obtained by curve fitting field measurements or the results from other computer models that accurately reflect the performance of a balanced flow desiccant heat exchanger. A wide range of data is necessary to properly define the performance of the desiccant heat exchanger such that all operating conditions expected during a simulation are included in the range of data used to obtain the model coefficients. The minimum and maximum boundaries for the independent variables used to generate the empirical model coefficients are used by this model to ensure that model extrapolation does not occur at any point during the simulation. For this reason, it is recommended that the widest possible range of data be used to determine the model coefficients.
-
-The dry-bulb temperature of the regeneration outlet air is determined using the equation shown below.
-
-<div>$$RTO = B1 + B2*RWI + B3*RTI + B4*\left( {\frac{{RWI}}{{RTI}}} \right) + B5*PWI + B6*PTI + B7*\left( {\frac{{PWI}}{{PTI}}} \right) + B8*RFV$$</div>
-
-where:
-
-<span>\(RTO\)</span> = regeneration outlet air dry-bulb temperature (°C)
-
-<span>\(RWI\)</span> = regeneration inlet air humidity ratio (kg/kg)
-
-<span>\(RTI\)</span>  = regeneration inlet air dry-bulb temperature (°C)
-
-<span>\(PWI\)</span> = process inlet air humidity ratio (kg/kg)
-
-<span>\(PTI\)</span>  = process inlet air dry-bulb temperature (°C)
-
-<span>\(RFV\)</span> = regeneration (and process) face velocity (m/s)
-
-
-
-Similarly, the humidity ratio of the regeneration outlet air is defined using the same empirical equation form; however, different coefficients are used as follows:
-
-<div>$$RWO = C1 + C2*RWI + C3*RTI + C4*\left( {\frac{{RWI}}{{RTI}}} \right) + C5*PWI + C6*PTI + C7*\left( {\frac{{PWI}}{{PTI}}} \right) + C8*RFV$$</div>
-
-where:
-
-<span>\(RWO\)</span> = regeneration outlet air humidity ratio (kg/kg)
-
-
-
-If the regeneration outlet air conditions exceed the saturation curve, RTO and RWO are reset to saturated conditions (100% RH) at the enthalpy calculated based on the original RTO and RWO values.
-
-Once the regeneration outlet air conditions are determined as described above, the dry-bulb temperature and humidity ratio differences across the regeneration side of the heat exchanger are calculated.
-
-<div>$${T_{diff}} = \,RTO - {T_{Reg,\,\,in}}$$</div>
-
-<div>$${w_{diff}} = \,RWO - {w_{Reg,\,\,in}}$$</div>
-
-where:
-
-<span>\({T_{Reg,\,\,in}}\)</span>         = actual regeneration inlet air dry-bulb temperature (°C)
-
-<span>\({w_{Reg,\,\,in}}\)</span>        = actual regeneration inlet air humidity ratio (kg/kg)
-
-<span>\({T_{diff}}\)</span>           = regeneration air temperature difference based on empirical model (°C)
-
-<span>\(wdiff\)</span>          = regeneration air humidity ratio difference based on empirical model (kg/kg)
-
-
-
-The regeneration outlet air conditions described above represent the full load outlet conditions under steady-state operation. However, there are times when the heat exchanger may not operate for the entire simulation time step (i.e., bypass air flow around a fixed-plate heat exchanger or stop the rotation of a rotary heat exchanger for a portion of the time step). For example, the parent object calling this heat exchanger model may request that it only provide heat exchange for a portion of the time step (*HXPartLoadRatio*). Another example would be if this heat exchanger is not called by a parent object but is instead placed directly in a AirLoopHVAC or AirLoopHVAC:OutdoorAirSystem and a setpoint manager is used to place a minimum and/or maximum humidity ratio setpoint on the process air outlet node. For this case the humidity setpoints, if present, are used to calculate a part-load ratio for the heat exchanger assuming the full-load process air humidity ratio difference is equivalent (but opposite in sign) to the regeneration air humidity ratio difference (*w<sub>diff</sub>*):
-
-
-
-<span>\(\begin{array}{l}IF\,\,\left( {{w_{diff}} > 0.0} \right)\,\,THEN\,\,!\,\,Regen\,\,air\,humidified,\,process\,air\,dehumidified\\\,\,\,\,\,\,\,\,HXPartLoadRatio = \,\frac{{\left( {{w_{Proc,\,\,in}} - {w_{max, set\,point}}} \right)}}{{{w_{diff}}}}\\ELSE\,IF\,\left( {{w_{diff}} &lt; 0.0} \right)\,\,THEN\,\,!\,\,Regen\,\,air\,dehumidified,\,process\,air\,humidified\\\,\,\,\,\,\,\,\,HXPartLoadRatio = \,\frac{{\left( {{w_{Proc,\,\,in}} - {w_{min, set\,point}}} \right)}}{{{w_{diff}}}}\\END\,IF\\HXPartLoadRatio = MAX\left( {0.0,HXPartLoadRatio} \right)\\HXPartLoadRatio = MIN\,\left( {1.0,HXPartLoadRatio} \right)\end{array}\)</span>
-
-If this heat exchanger is not being called by a parent object and no humidity setpoints are placed on the process air outlet node, then the model assumes that the heat exchanger operates for the entire simulation time step when it is available to operate (based on its availability schedule) and there is a temperature and/or humidity ratio difference between the two air streams.
-
-EnergyPlus has an established convention for placing information on outlet air nodes. If the air flow rate is continuous but the device only operates for a portion of the simulation time step, then the average outlet conditions (temperature, humidity and enthalpy) are placed on the outlet air node. If the air flow rate cycles on and off during the simulation time step, then the full load outlet conditions are placed on the outlet air node along with the average air mass flow rate for the simulation time step. To account for these cases, this model uses the following logic:
-
-<div>$$\begin{array}{l}IF(FanOpMode\,\,.EQ.\,\,CycFanCycComp\,\,.OR.\,\,RegAirInletIsOANode)\,THEN\\\,\,\,\,\,\,\,\,{T_{Reg,\,\,out}}\, = \,{T_{Reg,\,\,in}} + {T_{diff}}\\\,\,\,\,\,\,\,\,{w_{Reg,\,\,out}}\, = \,{w_{Reg,\,\,in}} + {w_{diff}}\\ELSE\\\,\,\,\,\,\,\,\,{T_{Reg,\,\,out}}\, = \,{T_{Reg,\,\,in}} + \left( {{T_{diff}}*HXPartLoadRatio} \right)\\\,\,\,\,\,\,\,\,{w_{Reg,\,\,out}}\, = \,{w_{Reg,\,\,in}} + \left( {{w_{diff}}*HXPartLoadRatio} \right)\\ENDIF\end{array}$$</div>
-
-where:
-
-<span>\({T_{Reg,\,\,out}}\)</span>       = regeneration outlet air dry-bulb temperature (°C)
-
-<span>\({w_{Reg,\,\,out}}\)</span>      = regeneration outlet air humidity ratio (kg/kg)
-
-<span>\(HXPartLoadRatio\)</span> = heat exchanger part-load ratio (determined by parent object calling this model, or calculated based on a minimum/maximum humidity ratio setpoints as shown above).
-
-
-
-In the logic shown above, *RegAirInletIsOANode* is true if the regeneration air inlet node is an outside air node. If so, the model assumes that the air flow through the regeneration side of the heat exchanger cycles on and off as required during the simulation time step. Also, the regeneration outlet air humidity ratio is limited to be between 1E-5 and 1.0.
-
-The regeneration outlet air enthalpy is then calculated using the regeneration outlet air temperature and humidity ratio.
-
-<div>$${h_{Reg,\,\,out}} = \,PsyHFnTdbW\left( {{T_{Reg,\,\,out}}\,,\,\,{w_{Reg,\,\,out}}} \right)$$</div>
-
-Using the regeneration outlet air conditions, the heat transfer on the regeneration side of the heat exchanger is then calculated:
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible,Reg}} = \,{\mathop m\limits^ \bullet_{Reg}}C{p_{Reg,\,\,in}}\left( {{T_{Reg,\,\,out}}\, - \,{T_{Reg,\,\,in}}} \right)$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Total,Reg}} = \,{\mathop m\limits^ \bullet_{Reg}}\left( {{h_{Reg,\,\,out}}\, - \,{h_{Reg,\,\,in}}} \right)$$</div>
-
-where:
-
-<span>\({\mathop Q\limits^ \bullet_{Sensible,Reg}}\)</span>  = sensible heat transfer rate to the regeneration air stream (W)
-
-<span>\({\mathop Q\limits^ \bullet_{Total,Reg}}\)</span>     = total heat transfer rate to the regeneration air stream (W)
-
-<span>\({\mathop m\limits^ \bullet_{Reg}}\)</span>          = regeneration air mass flow rate (kg/s)
-
-<span>\(C{p_{Reg,\,\,in}}\)</span>      = specific heat of inlet regeneration air (J/kg-K)
-
-
-
-Since the model assumes that total and sensible heat transfer is conserved, these heat transfer rates are then used to calculate the process air outlet conditions:
-
-<div>$${h_{Proc, out}} = \,{h_{Proc,in}} - \left( {\frac{{{{\mathop Q\limits^ \bullet  }_{Total,Reg}}}}{{{{\mathop m\limits^ \bullet  }_{Proc}}}}} \right)$$</div>
-
-<div>$${T_{Proc, out}} = \,{T_{Proc,in}} - \left( {\frac{{{{\mathop Q\limits^ \bullet  }_{Sensible,Reg}}}}{{{{\mathop m\limits^ \bullet  }_{Proc}}C{p_{Proc,in}}}}} \right)$$</div>
-
-<div>$${w_{Proc,\,\,out}} = \,PsyWFnTdbH\left( {{T_{Proc,\,\,out}}\,,\,\,{h_{Proc,\,\,out}}} \right)$$</div>
-
-where:
-
-<span>\({h_{Proc,\,\,out}}\)</span>      = process outlet air enthalpy (J/kg)
-
-<span>\({T_{Proc,\,\,out}}\)</span>      = process outlet air dry-bulb temperature (°C)
-
-<span>\({w_{Proc,\,\,out}}\)</span>      = process outlet air humidity ratio (kg/kg)
-
-<span>\({\dot m_{Proc}}\)</span>         = process air mass flow rate (kg/s)
-
-<span>\(C{p_{Proc,in}}\)</span>     = specific heat of inlet process air (J/kg-K)
-
-Like the regeneration outlet air conditions, the process outlet air conditions are also checked for exceeding saturated conditions and, if detected, the temperature and humidity ratio are reset assuming constant enthalpy.
-
-<div>$$\begin{array}{l}{T_{sat}} = \,PsyTsatFnHPb\left( {{h_{Proc,\,\,out}}\,,\,\,PB} \right)\\IF({T_{sat}} > \,{T_{Proc,out}})\,THEN\\\,\,\,\,\,\,\,\,\,\,{T_{Proc,out}} = {T_{sat}}\\\,\,\,\,\,\,\,\,\,\,{w_{Proc,out}} = PsyWFnTdbH\left( {{T_{Proc,out}}\,,\,\,{h_{Proc,out}}} \right)\\END\,IF\end{array}$$</div>
-
-Heat recovery electric power is the electric consumption rate of the unit in watts. The nominal electric power for the heat exchanger is specified in the input data file, and can be used to model controls (transformers, relays, etc.) and/or a motor for a rotary heat exchanger. The model assumes that this electric power is consumed whenever the heat exchanger operates. The electric power is assumed to be zero for all other times. None of this electric power is assumed to contribute thermal load to either of the heat exchanger air streams. As with the thermal performance of the heat exchanger, the power used by the heat exchanger is also proportional to the heat exchanger part load ratio.
-
-<div>$${P_{HXUnit}}\, = \,{P_{HX,\,nom}}\left( {HXPartLoadRatio} \right)$$</div>
-
-where:
-
-<span>\({P_{HXUnit}}\)</span>       = output variable ‘Heat Exchanger Electric Power, W’ reported by the HeatExchanger:Desiccant:BalancedFlow object.
-
-<span>\({P_{HX,\,nom}}\)</span>       = user specified ‘Nominal Electric Power, W’
-
-##### Empirical Model Boundaries (Minimum and Maximum)
-
-Since this model uses empirical equations and extrapolation can cause unexpected results, the entering air conditions to both the regeneration and process sides of the heat exchanger are checked during each simulation time step to make sure they are within the valid range defined by the user. If any of the independent variables used in the equations for RTO and RWO above are outside the minimum and maximum limits specified for each independent variable, the values for these specific independent variables are limited to the appropriate boundary (min/max) value for use by the empirical equations and a warning is issued.
-
-Additional model checks occur by testing the regeneration and process inlet air relative humidities. In this case, the process and regeneration inlet air relative humidities are calculated and compared to the minimum/maximum values specified by the user. If the calculated relative humidity exceeds the specified range at any point during the simulation when the heat exchanger is operating, a warning message is issued but the simulation proceeds.
-
-If the user is confident in their empirical model coefficients, the minimum and maximum independent variable boundaries may be expanded (caution should be used here) to allow extrapolation of the empirical equations during the simulation.
-
-In addition to checking the inlet air conditions, the model allows the user to specify limits for the regeneration air outlet conditions (RTO and RWO). If the calculated value for RTO or RWO exceeds the minimum/maximum limits specified by the user, then the calculated value is reset to the appropriate boundary (min/max) value and a warning message is issued.
-
-This model also assumes that the performance of the desiccant heat exchanger (i.e., the output of the empirical equations) conforms to the following two guidelines.
-
-1.    The regeneration outlet air temperature (RTO) is always less than or equal to the regeneration inlet air temperature (*T<sub>RegIn</sub>*)
-
-2.    The regeneration outlet air humidity ratio (RWO) is always greater than or equal to the regeneration inlet air humidity ratio (*w<sub>RegIn</sub>*)
-
-When the calculated regeneration outlet air conditions do not follow these guidelines, a warning is issued and the simulation proceeds.
-
-### Plant Loop Deep-Ground-To-Water Vertical U-Tube Field Heat Exchanger
-
-This model (Object: GroundHeatExchanger:Vertical) documentation is derived from the M.S. thesis of Arunachalam Murugappan, which is available on the Oklahoma State University web site [http://www.hvac.okstate.edu/](http://www.hvac.okstate.edu/).  Eskilson (1987) Yavuzturk and Spitler (1999) developed the long and short time response factors respectively, which are used in determining the borehole temperature responses. Response factors are infinite series of numbers, which relate the current value of a variable to past values of other variables at discrete time intervals.  These response factors are referred as *g*-functions. The variable time-step model presented here uses both long time-step *g*-functions and short time-step *g*-functions to predict the boreholes response to short term fluctuations in the load.
-
-#### Long Time-Step Response Factors
-
-Eskilson developed *g*-functions for various borehole configurations. He plotted the g function curves for different sets of borehole spacing to borehole length ratio <span>\(B/H\)</span> typically for .05, 0.1, 0.15, 0.2, 0.3 and ∞ (∞ represents the single borehole configuration. All the plots were for the ratio of 0.0005 between the borehole radius and the borehole length <span>\({r_b}/H\)</span>. For any other radius a simple relation between the two radii as given by Eskilson (1987) can be used. Eskilson gives the *g*-function curves for 38 different configurations.
-
-Figure 253 shows the *g*-function plotted against the non-dimensional time defined as <span>\(\ln (t/{t_s})\)</span>, <span>\({t_s} = {H^2}/9\alpha \)</span> for various configurations of vertical boreholes with *B/H* ratio of .1 along with single borehole. It is seen from this figure that the thermal interaction between boreholes increases with time and with the number of boreholes in field.
-
-![](media/image5651.png)
-
-Figure 253.  Short Time Step g Function Curve as an Extension of Long Time Step g Function Curves for Different Configuration of Boreholes (Eskilson 1987, Yavuzturk 1999).
-
-The *g*-functions developed by Eskilson are valid only after time estimated by Eskilson as <span>\(5r_b^2/\alpha \)</span>. This time varies from 3-6 hours for a typical borehole field. This is because the analytical line source model, based on which the Eskilson’s model was developed, does not give a prompt increase in borehole wall temperature at <span>\(r = {r_b}\)</span>. It gives acceptable results only after the non-dimensional times of <span>\(\alpha t/r_b^2 > 5\)</span>. But to model short time responses of a borehole we need response factors, which can give accurate results down to minutes.
-
-#### Short Time-Step Response Factors
-
-Yavuzturk and Spitler (1999) developed short time step response factors using a transient, two-dimensional, implicit finite volume model on a polar grid.
-
-The circular u-tube pipe in the ground loop heat exchanger was approximated as a pie sector of equivalent perimeter.  A constant heat flux for the heat transfer form/to U-tube, a zero heat flux in the angular direction and a constant far field temperature in the radial axis makes up the three boundary condition and undisturbed far field temperature as the initial condition. The numerical model accounts for the thermal resistance due to individual borehole elements; such as resistance of the pipe and grout material and the convection resistance due to the heat transfer fluid in the pipes. The long time step *g*-functions discussed in the previous section do not account for such effects.
-
-The short time-step *g*-functions are the same for different borehole configurations. This is because there is no thermal interaction between the boreholes for times less than 200 hrs during which the short time-step *g*-functions apply. So it is suggested to use the short time-step *g* function for time steps in the range of 2.5 min and 200 hours and the long time-step *g*-functions for time steps longer than 200 hours. The *g* function for any time can be found by linear interpolation between the bounding known values.
-
-#### Development of the Variable Short Time Step Model
-
-The variable time step model was developed as an extension of the model presented by Yavuzturk and Spitler (1999). The variable, short time step model uses a similar algorithm and extends it to accommodate sub-hourly responses, variable time steps and explicit equations to calculate the outlet fluid temperature of the ground loop heat exchanger.
-
-The uniform time-steps model developed by Yavuzturk and Spitler (1999) is able to pre-calculate all the g-functions at the beginning of the simulation. The variable time-step model on the other hand must calculate the *g*-functions when the borehole response calculation for each time step is carried out. For every time step a different set of *g*-functions is needed in the variable time step model as the time at which the *g*-function is to be applied for the past loads changes for each time-steps.
-
-This is made clear from the illustration in Figure 254, which shows a simulation in progress. The boxes with numbers represent the sub-hourly loads. The time (in hrs) at which these loads occurred are shown by solid arrows above the respective load boxes. The right-most solid arrow gives the current simulation time, which is 3.31 hrs. The times given below the boxes, pointed by dashed arrows, are the time at which the *g*-functions are to be estimated and applied to the respective sub hourly loads (boxes) for the current time.
-
-For example, let us take the sub hourly loads 1,2 & 3. These loads occurred at 0 hrs, 0.16 hrs & 0.28 hrs. The response of the borehole temperature for the current time step is calculated by applying the *g­-*functions at 3.15 hrs, 3.03 hrs & 2.5 hrs respectively. Thus to calculate the present borehole temperature, the sub hourly loads 1-12 are superposed using the corresponding *g* functions at times given by the dashed lines.  This gives the borehole temperature at hr 3.31. However, for the previous time step, which occurred at 3.15 hrs, the g-functions for the loads 1, 2 & 3 are at 2.99 hrs 2.87 hrs and 2.42 hrs, and the over all response is obtained by superposing the loads 1-11.
-
-Thus for each time step since the time step increments are not uniform we need to store the simulation times at which these time-steps occurred, and calculate corresponding *g*-functions at each time-step.
-
-![](media/image5655.png)
-
-Figure 254.  Variable Timestep Ground Loop Heat Exchanger Model Schematic Explaining the *g* Function Estimation.
-
-Yavuzturk model calculates the outlet fluid temperature by iteration beginning with the undisturbed mean temperature of the surrounding ground as an initial guess. This aggravates the time taken by an already computationally intensive algorithm. To circumvent this a set of explicit equations were formulated to estimate the outlet fluid temperature.
-
-#### Description of the Load Aggregation Scheme
-
-A load aggregation scheme was developed for energy simulation software with variable short time steps down to one minute. A major issue in the development was the calculation of the *g*-functions.  As discussed previously in the variable time step environments, the time step increments are not uniform. As a result, g-functions cannot e pre-calculated. Figure 255 shows a schematic of the variable time step ground loop heat exchanger model. The figure shows the larger monthly block loads, hourly loads and sub hourly loads and along with the time of occurrence of those loads. The figure also shows the time at which the *g*-functions are applied to different load blocks.
-
-![](media/image5656.png)
-
-Figure 255.  Schematic of Variable Time Step Model *g* Function Calculation.
-
-To calculate the response of a past load on the borehole temperature we apply the *g*-function corresponding to the time elapsed since the load was applied. This is easily understood form the schematic. For example, to calculate the response of the aggregated load 1� (at the end of 730hrs.) for the current time step (2193.733hrs) we apply a *g*-function at 1463.73hrs. The *g*-function for the same block 1� at the previous time step, which occurred at 2193.25 hrs, would be at 1463.25hrs. From the schematic it is also seen that for the other two aggregated monthly loads 2�, 3� the *g*-function are applied at 733.73 hrs and 3.73 hrs for the current time-step and at 733.25 hrs and 3.25 hrs respectively for the previous time-step. The same scheme applies to hourly and sub-hourly. Thus to estimate the time at which the past monthly, hourly or sub-hourly loads occur, we might be tempted to store the simulation times at each time step for the entire simulation, storing load times for the whole length of simulation for a multi year simulation with a variable short time step would require a large amount of memory. But little consideration shows that it is not necessary.  Since the monthly and hourly loads occur at equal intervals of time 730hrs and 1hr respectively, the *g*-functions can be estimated with the current simulation time and the time at which the load block ends, which is a multiple of the monthly duration of the block size. Only the sub-hourly loads require storage of simulation times.
-
-For example from the schematic (Figure 256), for the sub hourly load 1, which occurred at the end of 2193.25 a *g*-function at .48 hrs has to be applied and for the next load 2 a *g*-function at 0.34 hrs has to be applied. Since the time intervals are not even for the sub hourly loads, we need to store the time steps at which those loads occurred. These times are required to estimate the time elapsed between the current simulation time and the time at which the sub hourly loads occurred.
-
-Thus, the algorithm keeps track of the sub hourly loads along with their time of occurrence for a user-defined length of time during which the sub hourly calculations are made. The algorithm also estimates the time weighted hourly load from their corresponding sub hourly loads as each hour passes. The sub-hourly loads are time weighted because of the irregular intervals at which the time-step occurs. This is also illustrated in Figure 256. The sub hourly loads 1,2 &3 occur for varying length of time. The load 3 occurs for a longer duration than 1 and 2 in that order. This implies that the load 3 has to be given more weight than 1 and 2. So the sub hourly loads for a particular hour are multiplied by the length of their respective period of occurrence and averaged over the hour. This is further explained by the schematic in Figure 5.
-
-![](media/image5657.png)
-
-Figure 256.  Schematic Showing the Calculation of Hourly Load from the Sub Houly Loads.
-
-The bottom text in the boxes represents the magnitude of the sub hourly loads in W/m for each time step. The duration of the occurrence of each time-step for the each block is shown below the respective block. The first hourly load is given by the expression
-
-<div>$${\overline q_1} = \left[ \begin{array}{l}\left( {8.36 \times .159} \right) + \left( {6.51 \times .339} \right) + \left( {10.3 \times .107} \right)\\ + \left( {6.92 \times .162} \right) + \left( {9.03 \times .181} \right) + \left( {12 \times .05} \right)\end{array} \right] = 7.993W/m$$</div>
-
-Where <span>\({\overline q_1}\)</span> = the first hourly load in W/m
-
-The algorithm keeps track of enough of these past hourly loads to calculate the monthly load. As each month or user defined time passes, hourly loads over the entire month or user defined time “blocks� are averaged and stored in arrays for the respective monthly user defined block of time.
-
-The borehole temperature for any time step is computed by superposing the monthly (larger time block loads) hourly and sub-hourly loads for each time step. To understand more clearly consider the schematic in Figure 256 where the borehole temperature at 2193.733 hour is to be estimated. Here the monthly block time is 730 hrs. We have three monthly aggregated load blocks for 730 hrs, 1460 hrs and 2190 hrs and hourly loads from 2191<sup>st</sup> hr to 2193<sup>rd</sup> hour. For the remaining 0.733 hours a sub hourly calculation is done. The three monthly aggregated load blocks when superposed using long time *g-*functions, yields the borehole temperature at the end of 2190<sup>th</sup> hour. Then the hourly loads from 2191<sup>st</sup> to 2193<sup>rd</sup> hrs are superposed using the corresponding short time step *g* functions values yielding the borehole temperature at the end of 2193<sup>rd</sup> hour. The sub-hourly variations for the current hour are obtained, by superposing the sub-hourly loads. From the schematic, we see there are two sub-hourly loads, 1 and 2. Thus the borehole temperature at the end of 2193.733 is expressed as:
-
-<div>$${T_{2193.733}} = {T_{ground}} + \sum\limits_{m = 1}^3 {\left[ {\frac{{{{\overline{\overline q} }_m} - {{\overline{\overline q} }_{m - 1}}}}{{2\pi {k_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_{730(m - 1)}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-<div>$$ + \sum\limits_{n = 2190}^{2193} {\left[ {\frac{{{{\overline q }_n} - {{\overline q }_{n - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_{n - 1}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-<div>$$ + \sum\limits_{p = 2193}^{2193.733} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-Where
-
-<span>\(\overline{\overline q} \)</span> = The average monthly loads
-
-<span>\(\overline q \)</span>  = The average hourly loads
-
-*Q* = the sub-hourly loads
-
-*m* = index for monthly aggregated blocks
-
-*p* = array index for sub hourly loads
-
-*t* = time
-
-t<sub>p</sub>  =  the sub hourly time steps over the history period. (here increment is not always unity)
-
-Superposing the temperature responses of monthly (larger) blocks over the shorter, namely the hourly and sub hourly, introduces some error in the borehole temperature calculation at the beginning of every month. Yavuzturk and Spitler suggest a method to reduce the error in borehole temperature prediction by using a minimum hourly history period during which only the short time step superposition is carried out. In our model this idea is extended to sub hourly loads as well. Thus a user specified minimum sub-hourly history period is included along with the minimum hourly history period to model the sub-hourly variations. During this period only sub-hourly and hourly superpositions are made. This guarantees that at any given time step the superposition of temperature responses involves a minimum period of short time responses, which ensures a better estimation of borehole temperature. For example, a minimum hourly history period of 96 hrs and a minimum sub hourly history period of 5 hours would result in only 2 monthly aggregation blocks (1� and 2�). The last monthly aggregation does not occur because neither of the minimum hourly history period of 96 hours or sub-hourly history period of five hrs is met. So an hourly superposition of the load is carried out for the third month until the minimum sub-hourly history period after which sub hourly superposition is carried out. The equation becomes
-
-<div>$${T_{2193.733}} = {T_{ground}} + \sum\limits_{m = 1}^2 {\left[ {\frac{{{{\overline{\overline q} }_m} - {{\overline{\overline q} }_{m - 1}}}}{{2\pi {k_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_{730(m - 1)}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-<div>$$ + \sum\limits_{n = 1460}^{2188} {\left[ {\frac{{{{\overline q }_n} - {{\overline q }_{n - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_{n - 1}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-<div>$$ + \sum\limits_{p = 2188}^{2193.733} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{2193.733}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-Yavuzturk and Spitler have done a detailed analysis on the effect of minimum hourly history period. They found that a minimum hourly history period of 192 hrs for an annual simulation would reduce the running time by 90%.  They also found that for a 20year simulation, the computation time of the aggregated load scheme is just 1% of the non-aggregated load scheme.
-
-#### Summary of Variable Short Time Step Response Factor Model
-
-The load aggregation scheme developed in line with the above example is summarized eight steps as follows:
-
-1.    Define monthly load blocks duration (mb) in hrs (generally 730 hrs) and the minimum hourly history period and minimum sub hourly history period.
-
-2.    Read Borehole Geometry Parameters: number of boreholes, borehole length radius thickness of the pipe etc. Read Ground and Fluid thermal properties: Ground conductivity, volumetric specific heat capacity of the ground and heat carrier fluid. Read the short and long time-step *g-*functions into arrays with their respective non-dimensionalized times.
-
-3.    Start Simulation from p=1 to nts. Here “nts� is the number of time steps that have occurred since the start of simulation. (Note that P in not a count of number of hour elapsed in the simulation)
-
-4.    Compute the hourly loads as each hour passes. This is done by averaging the sub hourly loads during the past hour. The monthly loads are calculated by averaging the hourly loads during that month. This is done by summing the hourly loads during that monthly period and dividing the sum by 730 hours NumMonths(the number of months used in aggregation calculations) is set to the number of months of simulation (current number of aggregated load blocks)
-
-5.    If the simulation time is less than the minimum sub hourly history period the borehole temperature is estimated with no aggregation. Only sub hourly loads are superposed as given by the following equation.
-
-<div>$${T_{nts}} = {T_{ground}} + \sum\limits_{p = 1}^{nts} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-6.    . If the simulation time is less than sum of minimum hourly history and sub hourly history periods, then decomposed hourly aggregated loads are superposed using their corresponding g function until the sub hourly history required. Then the sub hourly temperature differences are found by superposing the decomposed sub hourly loads with their short time step *g* functions. Average borehole temperature is found by superposing the hourly and sub hourly temperature differences with the following equation
-
-<div>$${T_{nts}} = \sum\limits_{n = 1}^{nh - sh} {\left[ {\frac{{{{\overline q }_n} - {{\overline q }_{n - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_{n - 1}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]}  + \sum\limits_{p = nts - sh}^{nts} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-7.    If the simulation time is greater then the sum of a monthly period, sub hourly history and the hourly history period. Then monthly load aggregation is performed. Here if the difference between the simulation time and product of a monthly block period and the current number of monthly blocks is greater than the sum of the minimum hourly history and sub hourly history periods then the average borehole temperature is found by the following equation.
-
-<div>$${T_{nts}} = {T_{ground}} + \sum\limits_{m = 1}^{calb} {\left[ {\frac{{{{\overline{\overline q} }_m} - {{\overline{\overline q} }_{m - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_{mb[m - 1]}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-<div>$$ + \sum\limits_{n = nh - [calb(mb) + sh]}^{nh - sh} {\left[ {\frac{{{{\overline q }_n} - {{\overline q }_{n - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_{n - 1}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-**<span>\(+ \sum\limits_{p = nts - sh}^{nts} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} \)</span>                                                       **
-
-8.    If the difference between the simulation time and product of a monthly block period and the current number of monthly blocks is less than the sum of the minimum hourly history and sub hourly history periods, then NumMonths is set to one month less than the actual number of months of simulation completed. The average borehole temperature is calculated by superposing the long and time step temperature differences using the following equation.
-
-<div>$${T_{nts}} = {T_{ground}} + \sum\limits_{m = 1}^{calb - 1} {\left[ {\frac{{{{\overline{\overline q} }_m} - {{\overline{\overline q} }_{m - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_{mb[m - 1]}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-<div>$$ + \sum\limits_{n = nh - [(calb - 1)(mb) + sh]}^{nh - sh} {\left[ {\frac{{{{\overline q }_n} - {{\overline q }_{n - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_{n - 1}}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} $$</div>
-
-**<span>\(+ \sum\limits_{p = nts - sh}^{nts} {\left[ {\frac{{{q_p} - {q_{p - 1}}}}{{2\pi {\kappa_{ground}}}}g\left( {\frac{{{t_{nts}} - {t_p}}}{{{t_s}}},\frac{{{r_b}}}{H}} \right)} \right]} \)</span>                          **
-
-Define Monthly block duration, minimum hourly history period and minimum sub hourly history period (step 1)
-
-
-
-Read Borehole Geometry parameters, Ground and carrier fluid properties and read short and long time-step *g* functions. (Step 2)
-
-** **
-
-**Do until** p = 1 to number of time-steps (nts) (Step 3)
-
-Compute the Ground Load for the current time step using Entering Fluid temperature (For the first time-step *T*<sub>FarField</sub> may be used)
-
-Compute the hourly loads as each hour and monthly loads as each month passes. Calculate the number of monthly blocks (NumMonths)(**Step 4**)
-
-**If** (Current time less than minimum sub hourly history) (**Step 5**)
-
-**   ** use Equation
-
-**Else If** (Current Simulation Time less than sum of minimum hourly history and minimum sub hourly history) (**step 6**)
-
-    use Equation
-
-    **Else**
-
-**If** (Difference between current simulation    time and duration of the total number months is Greater than sum of minimum hourly and sub hourly histories) (**step 7**)
-
-    use Equation
-
-           **Else** (**step 8**)
-
-                  use Equation
-
-           **End if**
-
-    **End if**
-
-**End do**
-
-
-#### References
-
-Eskilson, P. 1987. Thermal Analysis of Heat Extraction Boreholes. Ph.D. Thesis, Department of Mathematical Physics, University of Lund, Lund, Sweden.
-
-Yavuzturk, C. 1999. Modeling of Vertical Ground Loop Heat Exchangers for Ground Source Heat Pump Systems. Ph.D. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University, Stillwater, Oklahoma.
-
-Yavuzturk, C., J.D. Spitler. 1999.[ A Short Time Step Response Factor Model for Vertical Ground Loop Heat Exchangers.](http://www.hvac.okstate.edu/research/Documents/ASHRAE/Yavuzturk_Spitler_99.pdf) *ASHRAE Transactions*. 105(2):475-485.
-
-### GroundHeatExchanger:Slinky
-
-This model reuses much of the same code including the load aggregation and temperature response caluclations which are described above in the GroundHeatExchanger:Vertical model. As a result, that section can also be used as reference material. This model is unique in that it generates it’s own temperature response factor g-functions, rather than relying on the other software or data to generate the g-functions. These are generated based on the work by Xiong et al. 2015.
-
-#### Horizontal Slinky Temperature Response Functions
-
-Equation used for calculating the g-function temperature response factors for the horizontal Slinky HX are seen below.
-
-<div>$$   
- g_s\left(t\right) = \sum_{i=1}^{N_{ring}} \sum_{j=1}^{N_{ring}} \frac{R}{4\pi N_{ring}} \int_0^{2\pi} \int_0^{2\pi} 
-            \left[ 
-                \frac{erfc\left(d\left(P_j,P_i\right)/2\sqrt{\alpha t}\right)}{d\left(P_j,P_i\right)} - 
-                \frac{erfc\left(\sqrt{d\left(P_j,P_i\right)^2+4h^2/\left(2\sqrt{\alpha t}\right)}\right)}{\sqrt{d\left(P_j,P_i\right)^2+4h^2} }
-            \right]d\omega d\varphi
-$$</div>
-
-Where:
-
-<div>$$
-  d\left(P_j,P_i\right) = \frac{d\left(P_{ii},P_j\right) + d\left(P_{io},P_j\right)}{2}
-$$</div>
-
-<div>$$
-  d\left(P_{ii},P_j\right) = \sqrt{\left[x_{0i} + \left(R-r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i} + \left(R-r\right)\sin \varphi - y_{0j}-R\sin \omega\right]^2}
-$$</div>
-
-<div>$$
-  d\left(P_{io},P_j\right) = \sqrt{\left[x_{0i} + \left(R-r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i} + \left(R+r\right)\sin \varphi - y_{0j}-R\sin \omega\right]^2}
-$$</div>
-
-#### Vertical Slinky Temperature Response Functions
-
-Equations used for calculating the g-function temperature response factors for the vertical Slinky HX are seen below.
-
-<div>$$   
- g_s\left(t\right) = \sum_{i=1}^{N_{ring}} \sum_{j=1}^{N_{ring}} \frac{R}{4\pi N_{ring}} \int_0^{2\pi} \int_0^{2\pi} 
-            \left[ 
-                \frac{erfc\left(d\left(P_j,P_i\right)/2\sqrt{\alpha t}\right)}{d\left(P_j,P_i\right)} - 
-                \frac{erfc\left(d\left(P_{j'},P_i\right)/2\sqrt{\alpha t}\right)}{d\left(P_{j'},P_i\right)}
-            \right]d\omega d\varphi
-$$</div>
-
-Where: 
-
-<div>$$
-  d\left(P_j,P_i\right) = \frac{d\left(P_{ii},P_j\right) + d\left(P_{io},P_j\right)}{2}
-$$</div>
-
-<div>$$
-  d\left(P_{j'},P_i\right) = \frac{d\left(P_{ii},P_{j'}\right) + d\left(P_{io},P_{j'}\right)}{2}
-$$</div>
-
-<div>$$
-  d\left(P_{ii},P_j\right) = \sqrt{\left[x_{0i} + \left(R-r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i}-y_{0j}\right]^2 + \left[z_{0i} + \left(R-r\right)\sin \varphi - z_{0j}-R\sin \omega\right]^2}
-$$</div>
-
-<div>$$
-  d\left(P_{io},P_j\right) = \sqrt{\left[x_{0i} + \left(R+r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i}-y_{0j}\right]^2 + \left[z_{0i} + \left(R+r\right)\sin \varphi - z_{0j}-R\sin \omega\right]^2}
-$$</div>
-
-<div>$$
-  d\left(P_{ii},P_{j'}\right) = \sqrt{\left[x_{0i} + \left(R-r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i}-y_{0j}\right]^2 + \left[z_{0i} + \left(R-r\right)\sin \varphi - z_{0j} - 2h - R\sin \omega\right]^2}
-$$</div>
-
-<div>$$
-  d\left(P_{io},P_{j'}\right) = \sqrt{\left[x_{0i} + \left(R+r\right)\cos \varphi - x_{0j}-R\cos \omega\right]^2 + \left[y_{0i}-y_{0j}\right]^2 + \left[z_{0i} + \left(R+r\right)\sin \varphi - z_{0j} - 2h - R\sin \omega\right]^2}
-$$</div>
-
-#### Model Simplifications for Computational Efficiency
-
-Several simplifications were used to ensure the g-function temperature response factors are computationally efficient. The first simplification is achieved by taking advantage of symmetry. In the [Figure](#SlinkyGHX1) below we can see that by taking advantage of symmettry the temperature response for only one quarter of the rings needs be calculated.
-
-The second simplification occurs by realizing that the effect between two rings decreases exponentially as the distance between the rings increases. Near-field rings are defined as rings whose centers are within 2.5m + D distance from the center of ring i as is seen in [Figure](#SlinkyGHX1). Far-field rings are defined as rings whose centers are beyond 10m + D, with middle-field rings occupying the space in between the near-field and far-field rings. Near-field ring temperature response factors are determined as indicated above for horzontal or vertical slinkys. Middle-field rings are considerably simplified – the interaction between ring is approximated as that of two point sources at their centers. Thermal effect of far-field rings are ignored.
-
-The third and final simplification takes advantatge of geometric similarity that ring share. Ring pairs that are geometrically similar do not require recalculation of distances or reponse factors. Thus the calculations for geometrically similar ring pairs can be reused.
-
-For more information, see [Xiong et al. 2015](#SlinkyReferenceXiong).
-
-![](media/image8001.png)
-
-Figure: Schematic of first and second improvements to the algorithm for computational efficiency. <a name="SlinkyGHX1"></a>
-
-#### References
-
-Xiong, Z., D.E. Fisher, and J.D. Spitler. 2015. Development and Validation of a Slinky(TM) Ground Heat Exchanger Model. Applied Energy 141: 57-69. <a name="SlinkyReferenceXiong"></a>
-
-### Plant Loop Pond-To-Water Heat Exchanger
-
-The pond model (Object: GroundHeatExchanger:Pond) is a ‘lumped parameter’ model where the pond is represented by a single node with thermal mass. The pond surface temperature is the same as the temperature at this node, i.e. the surface temperature is the same as the bulk temperature. A first order differential equation is solved in the model to calculate the pond temperature at each time step. This type of heat rejecter is modeled as several circuits connected in parallel.
-
-![](media/image5676.png)
-
-Figure 257.  Heat Transfer Mechanisms in a Pond (Chiasson 1999)
-
-Rees(2002) implemented the model developed by Chiasson(1999) for the shallow ponds. The model is based on the assumption that thermal gradients in shallow ponds are negligible, especially during times of heat rejection. Using the lumped parameter approach, an overall energy balance for the pond may be devised as
-
-<div>$$q{}_{in} - q{}_{out} = V\rho C{}_p\frac{{dT}}{{dt}}$$</div>
-
-Where
-
-<span>\(q{}_{in}\)</span>   =   Heat transfer to the pond
-
-<span>\(q{}_{out}\)</span>  =   Heat transfer from the pond
-
-<span>\(V\)</span>     =   Pond Volume
-
-<span>\(\rho \)</span>     =   Density of pond water
-
-<span>\({q_{in}}\)</span> = Heat transfer to the pond
-
-<span>\(C{}_p\)</span> = Specific heat capacity of pond water
-
-<span>\(\frac{{dT}}{{dt}}\)</span> = rate of change of temperature of the pond water
-
-Rate of change in average pond temperature is given as
-
-<div>$$\frac{{dT}}{{dt}} = \frac{{q{}_{solar} + q{}_{thermal} + q{}_{convection} + q{}_{groundwater} + q{}_{evaporation} + q{}_{fluid}}}{{V\rho C{}_p}}$$</div>
-
-Where
-
-q<sub>solar   \\                    \\     </sub>= Solar radiation heat gain to the pond
-
-q<sub>thermal       \\          </sub>= Thermal radiation heat transfer at the pond surface.
-
-q<sub>convection           </sub> = Convection heat transfer at the pond surface
-
-q<sub>ground\\                   \\    </sub>= Heat transfer to/from ground to the pond
-
-q<sub>groundwater\\          \\    </sub>= Heat transfer due to ground water inflow/outflow
-
-q<sub>evaporation        </sub> = Heat transfer due to evaporation at the pond surface
-
-q<sub>fluid                    </sub> = Total heat transfer to/from the heat exchanging fluid flowing in all spools or  coils in the pond
-
-A heat balance is calculated at a single node that represents the pond. Heat transfer takes place by surface convection, long-wave radiation to the sky, absorption of solar energy, ground heat transfer and heat exchange with the fluid. A heat exchanger analogy is used to calculate the heat transfer between the heat transfer fluid and the pond. The differential equation defined by the heat balance is solved using a fourth order Runge-Kutta numerical integration method. The implementation along with the model equations are summarized in the figure below.
-
-![](media/image5686.png)
-
-Figure 258.  Pond Model Component Configuration (Chiasson 1999)
-
-The model overall pond model consists in a number of sub-models which are enumerated below.
-
-#### Solar radiation heat gain to the pond
-
-<div>$$\rho ' = {\tau_a} - \tau $$</div>
-
-where
-
-<span>\(\rho '\)</span>is the reflectance
-
-<span>\(\tau \)</span> is the transmittance of solar radiation by the pond surface and the subscript ‘a’ refers to the absorbed component.
-
-<div>$${\tau_a} = {e^{\frac{{ - \mu 'd}}{{\cos {\theta_r}}}}}$$</div>
-
-and
-
-<div>$$\tau  = \frac{1}{2}\left( {\frac{{1 - {r_{par}}}}{{1 + {r_{par}}}} + \frac{{1 - {r_ \bot }}}{{1 + {r_ \bot }}}} \right){e^{\frac{{ - \mu 'd}}{{\cos {\theta_r}}}}}$$</div>
-
-where
-
-<span>\(\mu '\)</span>is the extinction coefficient for water
-
-<span>\(d\)</span> is the pond depth
-
-<span>\({r_{par}}\)</span>represents the parallel component of unpolarized radiation and
-
-<span>\({r_ \bot }\)</span>represents the perpendicular component of unpolarized radiation which are computed by Duffie and Beckman (1991) as:
-
-<sub><span>\({r_{par}} = \frac{{{{\tan }^2}\left( {{\theta_r} - \theta } \right)}}{{{{\tan }^2}\left( {{\theta_r} + \theta } \right)}}\)</span></sub>
-
-<sub><span>\({r_ \bot } = \frac{{{{\sin }^2}\left( {{\theta_r} - \theta } \right)}}{{{{\sin }^2}\left( {{\theta_r} - \theta } \right)}}\)</span></sub>
-
-Finally, the amount of solar radiation absorbed by the pond (<span>\({q_{solar}}\)</span>) is expressed as:
-
-<div>$${q_{solar}} = I\left( {1 - \rho '} \right){A_{pond}}$$</div>
-
-where
-
-<span>\(I\)</span>is the solar radiation flux incident on the pond surface (here, the total reflectance is approximated by the beam reflectance)
-
-<span>\({A_{pond}}\)</span>is the area of the pond surface.
-
-The model also accepts solar radiation in the form of beam <span>\(\left( {{I_b}} \right)\)</span>and diffuse <span>\(\left( {{I_d}} \right)\)</span> components, in which case <span>\(I\)</span>is computed from:
-
-<div>$$I = {I_b}\cos \theta  + {I_d}$$</div>
-
-#### Thermal radiation heat transfer at the pond surface
-
-<div>$$q{}_{thermal} = \sigma \alpha (T{{}_{surface}^4} - T{{}_{sky}^4})$$</div>
-
-Where
-
-<span>\(\alpha \)</span>= Thermal absorptivity
-
-<span>\(\sigma \)</span>= Stefan Boltzman constant
-
-#### Convection heat transfer at the pond surface
-
-<div>$$q{}_{convection} = h{}_c(T{}_{pond} - T{}_{db})$$</div>
-
-ASHRAE simple convection coefficient model is used to obtain the convection coefficient for external surfaces. Initializing of pond temps to mean of dry-bulb temperature T<sub>db</sub> and ground temperatures is useful because repeated warm up days tend to drive the initial pond temperature toward the dry-bulb temperature Hence, for each environment the simulation starts the pond temperature T<sub>pond</sub> midway between the dry-bulb and ground temperature.
-
-#### Heat transfer to/from ground to the pond
-
-Hull et al (1984) expressed the following equation for ground heat losses from any pond. The equations are also based on the assumption that, for all practical purposes, the constant temperature sink is the ground water table (Kishore and Joshi 1984)
-
-<div>$$q{}_{ground} = U{}_{ground}A{}_{ground}(T{}_{groundwater} - T{}_{pond})$$</div>
-
-<div>$$U{}_{ground} = 0.999\left( {\frac{{k{}_{ground}}}{{d{}_{groundwater} - d{}_{pond}}}} \right) + 1.37\left( {\frac{{k{}_{ground}P{}_{pond}}}{{A{}_{pond}}}} \right)$$</div>
-
-Where
-
-<span>\(k{}_{ground}\)</span>        = Thermal conductivity of the ground
-
- <span>\(d{}_{groundwater}\)</span> = depth of water table
-
-<span>\(d{}_{pond}\)</span>          = Pond depth
-
-<span>\(P{}_{pond}\)</span>         = Pond perimeter
-
-#### Heat transfer due to evaporation at the pond surface
-
-Evaporation is calculated assuming a fixed Lewis number unlike the Chaisson model.
-
-<div>$$q{}_{evaporation} = {\left( {\frac{{\Pr }}{{Sc}}} \right)^{2/3}}\left( {\frac{{h{}_c}}{{Cp{}_{air}}}} \right)\left( {HR{}_f - HR{}_a} \right)\left( {q{}_l} \right)$$</div>
-
-Where
-
-Pr =Prandtl number for air
-
-Sc = Schmidt number for air
-
-Hc = convection coefficient
-
-HRf= humidity ratio at pond surface/film temperature
-
-HRa= humidity ratio of air
-
-ql  = Latent heat of air
-
-Air properties are obtained by applying the existing the psychometric functions of EnergyPlus.
-
-#### Total heat transfer to/from the heat exchanging fluid flowing in all spools or coils in the pond
-
-<div>$$q{}_{fluid} = UA{}_{pipe}(T{}_{fluid} - T{}_{pond})N{}_{circuit}$$</div>
-
-Where
-
-<span>\(UA{}_{pipe}\)</span> = overall heat transfer coefficient expressed in terms of inside pipe area
-
-<span>\(N{}_{circuit}\)</span>= number of spools installed in the pond
-
-The fluid temperature Tfluid is computed as the average fluid temperatures of the inlet and the outlet node at a given temperature.
-
-<div>$$U{A_{pipe}} = \frac{{2\pi {r_i}\cdot {L_{spool}}}}{{\sum {{r_t}} }}$$</div>
-
-where
-
-<span>\({r_i}\)</span>= inner pipe radius
-
-<span>\({L_{spool}}\)</span>l= length of one spool
-
-<span>\(\sum {{r_t}} \)</span>= composite thermal resistance defined as
-
-<span>\(\sum {{r_t}} \)</span>=Resistance due to fluid flow in the pipe +external pipe thermal resistance +fouling factor
-
-#### References
-
-Chiasson, A.D. 1999. *Advances in modeling of groundsourceheat pump systems*. Master’s thesis,Oklahoma State University, Stillwater, OK
-
-Duffie, J.A., and W.A. Beckman. 1991. *Solar engineering of thermal processes,* 2d ed. New York: John Wiley & Sons.
-
-Hull, J.R., K.V. Liu, W.T. Sha, J. Kamal, and C.E. Nielsen. 1984. Dependence of ground heat losses upon solar pond size and perimeter insulation—Calculated and experimental results. *Solar Energy* 33(1): 25-33
-
-Kishore, V.V.N., and V. Joshi. 1984. A practical collector efficiency equation for nonconvecting solar ponds. *Solar Energy* 33(5): 391-395.
-
-Rees, S.J., J.D. Spitler and X. Xiao, X 2002.[Transient Analysis of Snow-melting System Performance](http://www.hvac.okstate.edu/pdfs/Rees_Spitler_Xiao_02.pdf).*ASHRAE Transactions.*108(2):406-423.
-
-### Plant Loop Surface-Ground-To-Water Heat Exchanger
-
-This model (Object: GroundHeatExchanger:Surface) is based on the QTF formulation of heat transfer through building elements with embedded heat sources/sinks. The model uses a heat exchanger analogy to relate the inlet fluid temperature to the net heat transfer rate and consequently outlet temperature. The model is entirely passive, i.e. it does not set any flow rates or incorporate any controls. In order to deal with the non-linear boundary conditions at the top surface due to the presence of ice/snow fluxes have to be calculated by the QTF model and temperature calculated from the surface heat balance. This requires some iteration. Note, top surface variables correspond to ‘outside’ variables in standard CTF/QTF definition. Bottom surface variables correspond to ‘inside’ variables.
-
-For given current surface temperatures the terms of the QTF equations can be grouped into constant terms, and those depending on the current source flux. The surface heat balance may be given by the following equation (Strand,1997)
-
-<div>$$QS{}_{} = \sum\limits_{m = 1}^M {X{}_{k,m}} T{}_{i,t - m + 1} - \sum\limits_{m = 1}^M {Y{}_{k,m}} T{}_{o,t - m + 1} + \sum\limits_{m = 1}^k {F{}_m} q{}_{i,t - m} + \sum\limits_{m = 1}^M {W{}_m} {q''}{}_{source,t - m + 1}$$</div>
-
-<div>$$T{}_S{}_{} = \sum\limits_{m = 1}^M {X{}_{k,m}} T{}_{i,t - m + 1} - \sum\limits_{m = 1}^M {Y{}_{k,m}} T{}_{o,t - m + 1} + \sum\limits_{m = 1}^k {F{}_m} q{}_{i,t - m} + \sum\limits_{m = 1}^M {W{}_m} q''{}_{source,t - m + 1}$$</div>
-
-Where
-
-T<sub>s</sub>    = temperature of the node where the heat source or sink is present
-
-<span>\(QS\)</span>= Surface heat balance
-
-<span>\({q''}\)</span>= Heat flux
-
-T   = Temperature
-
-i    =  inside of the building element
-
-o   = outside of the building element
-
-t    = current time step
-
-X Y F = Conduction transfer functions
-
-The surface balance equation includes terms for incident solar energy, radiation heat transfer from internal sources, linearized radiation between surfaces using the mean radiation temperature concept and convection to the surrounding air.
-
-The heat balance on the water loop is given by
-
-<div>$$q = \dot mc{}_p(T{}_{wi} - T{}_{wo})$$</div>
-
-Where
-
-q = heat transferred between the water loop and the building elements.
-
-<span>\(\dot m\)</span>= mass flow rate of water
-
-<span>\(T{}_{wi}\)</span>= Inlet water temperature
-
-<span>\(T{}_{wo}\)</span>= Outlet water temperature
-
-From the second law of thermodynamics the maximum amount of heat transfer is
-
-<div>$$q{}_{\max } = (\dot mc{}_p){}_{water}(T{}_{wi} - T{}_s)$$</div>
-
-Where
-
-T<sub>s</sub> = temperature at the source location
-
-The effectiveness of the heat exchanger is given by
-
-<div>$$\varepsilon  = 1 - {e^{ - NTU}}$$</div>
-
-Where NTU is defined by
-
-<div>$$NTU = \frac{{UA}}{{(\dot mC{}_p){}_{water}}}$$</div>
-
-<div>$$UA = h\pi DL$$</div>
-
-h is the convection coefficient, D is the interior tube diameter and L is the total length of the tube.
-
-The Colburn equation is used to define the Nusselt number Nu
-
-<div>$$Nu = \frac{{hD}}{k} = 0.023{\mathop{\rm Re}\nolimits} {{}_D^{4/5}}{\Pr ^{1/3}}$$</div>
-
-Pr is the Prandtl number, Re is the Reynolds number and k is the thermal conductivity of the fluid
-
-<div>$${\mathop{\rm Re}\nolimits} {}_D = \frac{{4\dot m}}{{\pi \mu D}}$$</div>
-
-with <span>\(\mu \)</span> being the absolute viscosity of water
-
-### Plant Loop Fluid-to-Fluid Heat Exchanger
-
-This component (Object: HeatExchanger:FluidToFluid) is a simple hydronic heat exchanger that can be used to couple two (hydronic) plant or condenser loops.  Sizing and nominal capacity calculations are discussed elsewhere in this document, see the section called Plant Heat Exchanger Sizing. This section first discusses the heat transfer modeling and the control issues.
-
-Heat exchanger performance modeling uses classic effectiveness-NTU correlations. The heat exchanger model can be specified as one of seven types:  cross flow both fluid streams unmixed, cross flow both fluid streams mixed, cross flow maximum capacity flow mixed min), counter flow, parallel flow, or ideal. The model correlations determine a heat transfer effectiveness value, <span>\(\varepsilon \)</span>, which is a function of heat exchanger UA, the mass flow rates through boths sides, and the specific heat of the fluids in the streams.  The effectiveness of an ideal heat exchanger is set to 1.0 and no correlation is needed.
-
-Because the heat exchanger is intended to be generic, its two sides are distinguished by the nature of loop side being connected.  One side is called “Loop Supply Side� to indicate the heat exchanger is situated on the supply side of a loop. The other side is called “Loop Demand Side� to indicate it is on the demand side of a loop.  The heat exchanger is intended to act as a supply component for the loop connected to it as the “Loop Supply Side� and as a demand component for the loop connected to it as the “Loop Demand Side.�  From the point of view of the heat exchanger component itself, the Loop Demand Side acts like a supply source/sink for the Loop Supply Side which acts like a demand to the component.
-
-The mass flow rates and specific heat capacity are multiplied together to evaluate flow thermal capacity for each side and the minimum, maximum, and capacity ratio, <span>\({R_C}\)</span>, are determined.
-
-<div>$${\left( {\dot m{c_p}} \right)_{SupLoop}} = {\dot m_{SupLoop}}*{c_p}_{SupLoop}$$</div>
-
-<div>$${\left( {\dot m{c_p}} \right)_{DmdLoop}} = {\dot m_{DmdLoop}}*{c_p}_{DmdLoop}$$</div>
-
-<div>$${\left( {\dot m{c_p}} \right)_{Min}} = MIN\left( {{{\left( {\dot m{c_p}} \right)}_{SupLoop}},{{\left( {\dot m{c_p}} \right)}_{DmdLoop}}} \right)$$</div>
-
-<div>$${\left( {\dot m{c_p}} \right)_{Max}} = MAX\left( {{{\left( {\dot m{c_p}} \right)}_{SupLoop}},{{\left( {\dot m{c_p}} \right)}_{DmdLoop}}} \right)$$</div>
-
-<div>$${R_C} = \frac{{{{\left( {\dot m{c_p}} \right)}_{Min}}}}{{{{\left( {\dot m{c_p}} \right)}_{Max}}}}$$</div>
-
-NTU, or Number of Transfer Units, is calculated using:
-
-<div>$$NTU = \frac{{UA}}{{{{\left( {\dot m{c_p}} \right)}_{Min}}}}$$</div>
-
-For a counter flow heat exchanger, effectiveness is calculated using:
-
-<div>$$\varepsilon  = \frac{{1 - exp\left[ { - NTU\left( {1 - {R_C}} \right)} \right]}}{{1 - {R_C}exp\left[ { - NTU\left( {1 - Rc} \right)} \right]}}$$</div>
-
-For a parallel flow heat exchanger, effectiveness is calculated using:
-
-<div>$$\varepsilon  = \frac{{1 - exp\left[ { - NTU\left( {1 + {R_C}} \right)} \right]}}{{\left( {1 + {R_C}} \right)}}$$</div>
-
-For a cross flow heat exchanger with both streams unmixed, effectiveness is calculated using:
-
-<div>$$\varepsilon  = 1 - exp\left\{ {\frac{{NT{U^{0.22}}}}{{{R_C}}}\left[ {exp\left( { - {R_C}NT{U^{0.78}}} \right) - 1} \right]} \right\}$$</div>
-
-For a cross flow heat exchanger with both streams mixed, the effectiveness is calculated using:
-
-<div>$$\varepsilon  = {\left[ {\frac{1}{{1 - exp\left( { - NTU} \right)}} + \frac{{{R_C}}}{{1 - exp\left( { - {R_C}NTU} \right)}} - \frac{1}{{NTU}}} \right]^{ - 1}}$$</div>
-
-For a cross flow heat exchanger with the stream with the higher capacity mixed and the stream with the lower capacity unmixed, the effectiveness is calculated using:
-
-<div>$$\varepsilon  = \frac{1}{{{R_C}}}\left\{ {1 - exp\left[ {{R_C}\left( {exp\left( { - NTU} \right) - 1} \right)} \right]} \right\}$$</div>
-
-For a cross flow heat exchanger with the stream with higher capacity unmixed and the stream with lower capacity mixed, the effectiveness is calculated using:
-
-<div>$$\varepsilon  = 1 - exp\left\{ { - \frac{1}{{{R_C}}}\left[ {1 - exp\left( { - {R_C}NTU} \right)} \right]} \right\}$$</div>
-
-Effectiveness values are always limited to be no higher than 1.0.  The program code protects from evaluating the exponential with operands that are too large or too small. Once the effectiveness value is determined, the heat transfer rate is calculated using:
-
-<div>$$\dot Q = \varepsilon {\left( {\dot m{c_p}} \right)_{Min}}\left( {{T_{SupLoop,In}} - {T_{DmdLoop,In}}} \right)$$</div>
-
-Lastly, the fluid temperatures leaving the heat exchanger are calculated using:
-
-<div>$${T_{SupLoop,Out}} = {T_{SupLoop,In}} - \frac{{\dot Q}}{{{{\left( {\dot m{c_p}} \right)}_{SupLoop}}}}$$</div>
-
-<div>$${T_{DmdLoop,Out}} = {T_{DmdLoop,In}} + \frac{{\dot Q}}{{{{\left( {\dot m{c_p}} \right)}_{DmdLoop}}}}$$</div>
-
-The plant heat exchanger offers a number of control options for a wide variety of applications.  This section documents the control decision logic. The general goal of the control is to provide appropriate conditioning of the fluid at the Loop Supply Side connection.  The basic control action is to request the appropriate flow rates for each side of the heat exchanger.  For all of the control modes, there is also an availability schedule that provides a level of supervisory control to determine if the heat exchange is available to run at all.  If the device is scheduled off, then zero flow is requested for both connections. All the control modes can also use minimum and maximum temperature limits.  If the limits are used and either of the two inlet temperatures exceeds the limit, the zero flow is requested for both connections.
-
-**UncontrolledOn. ** This control type is very simple.  If scheduled on it requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
-
-**OperationSchemeModulated. ** This control type uses the plant operation schemes. Any of the various plant (or condenser) operation schemes (e.g. PlantEquipmentOperation:CoolingLoad or PlantEquipmentOperation:HeatingLoad ). When the heat exchanger is called, the operation scheme will pass a value for the load to be met.  If the absolute value of the load is less than a small tolerance (1 W), then zero flow is requested for both connections.  If load is significant and negative, then the heat exchanger will attempt to provide cooling.  If the load is significant and positive, then it will attempt to provide heating.  The two inlet fluid temperatures are compared and if their difference exceeds the minimum temperature difference and has the correct sign for heating or cooling as needed, then the heat exchanger is turned “on.�  The model requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then a flow rate for the Loop Demand Side is found to attempt to meet the load.  The load value is converted to a target temperature for the fluid leaving the Loop Supply Side connection.  The target temperature is then used with the numerical method Regula Falsi to solve for the flow rate.
-
-**OperationSchemeOnOff**.  This control type uses the plant operation schemes. Any of the various plant (or condenser) operation schemes (e.g. PlantEquipmentOperation:CoolingLoad or PlantEquipmentOperation:HeatingLoad). When the heat exchanger is called, the operation scheme will pass a value for the load to be met.  If the absolute value of the load is less than a small tolerance (1 W), then zero flow is requested for both connections.  If load is significant and negative, then the heat exchanger will attempt to provide cooling.  If the load is significant and positive, then it will attempt to provide heating.  The two inlet fluid temperatures are compared and if their difference exceeds the minimum temperature difference and has the correct sign for heating or cooling as is needed, then the heat exchanger is turned “on.�  The model requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
-
-**HeatingSetpointModulated**.  This control scheme uses a node setpoint. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible.  The temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if heating is desired.  If heating is both desired and possible, then the heat exchanger is turned “on.�  The model requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then a flow rate for the Loop Demand Side is found to attempt to meet the setpoint.  The setpoint temperature is then used with the numerical method Regula Falsi to solve for the flow rate.
-
-**HeatingSetpointOnOff**.  This control scheme uses a node setpoint. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible.  The temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if heating is desired.  If heating is both desired and possible, then the heat exchanger is turned “on.�  The model requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
-
-**CoolingSetpointModulated**.  This control scheme uses a node setpoint. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.  The temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if cooling is desired.  If cooling is both desired and possible, then the heat exchanger is turned “on.�  The model requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then a flow rate for the Loop Demand Side is found to attempt to meet the setpoint.  The setpoint temperature is then used with the numerical method Regula Falsi to solve for the flow rate.
-
-**CoolingSetpointOnOff**.  This control scheme uses a node setpoint. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.  The temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if cooling is desired.  If cooling is both desired and possible, then the heat exchanger is turned “on.�  The model requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
-
-**CoolingSetpointOnOffWithComponentOverride**.  This control scheme uses one of three different control signals, a node setpoint, outdoor air drybulb temperature, or outdoor air wetbulb temperature. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.  The control signal is compared to the inlet temperature for the Loop Supply Side to see if cooling is desired.  If cooling is both desired and possible, then the heat exchanger is turned “on.�  When the heat exchanger is on, the remote chiller component is turned off.  The model requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
-
-**CoolingDifferentialOnOff**.  This control scheme is based on a simple temperature difference. The two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.  If cooling is possible then it is assumed to be desired and the heat exchanger is turned “on.�  The model requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
-
-**DualDeadbandSetpointModulated**.  This control scheme uses dual setpoints on a node. The basic idea is that the heat exchanger will condition the Loop Supply Side connection to drive its temperature into the deadband whenever its inlet temperature is outside the deadband.  The model expects dual temperature setpoints to be placed on the setpoint, for example using the object SetpointManager:Scheduled:DualSetpoint.
-
-The heat exchanger will operate to cool the Loop Supply Side fluid when the following three conditions are all met:
-
-1)  the two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible,
-
-2) the higher temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible, and
-
-3)  the higher temperature setpoint on the reference node is compared to the inlet temperature for the Loop Demand Side to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.
-
-The heat exchanger will operate to heat the Loop Supply Side fluid when the following three conditions are all met:
-
-1)  the two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible,
-
-2)  the lower temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible, and
-
-3) the lower temperature setpoint on the reference node is compared to the inlet temperature for the Loop Demand Side to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible.
-
-When the heat exchanger is turned “on.�  The model requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then a flow rate for the Loop Demand Side is found to attempt to meet the setpoint.  The setpoint temperature is then used with the numerical method Regula Falsi to solve for the flow rate.
-
-**DualDeadbandSetpointOnOff**. This control scheme uses dual setpoints on a node. The basic idea is that the heat exchanger will condition the Loop Supply Side connection to drive its temperature into the deadband whenever its inlet temperature is outside the deadband.  The model expects dual temperature setpoints to be placed on the setpoint, for example using the object SetpointManager:Scheduled:DualSetpoint.
-
-The heat exchanger will operate to cool the Loop Supply Side fluid when the following three conditions are all met:
-
-1)  the two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible,
-
-2) the higher temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible, and
-
-3)  the higher temperature setpoint on the reference node is compared to the inlet temperature for the Loop Demand Side to see if their difference exceeds the minimum temperature difference and has the correct sign for cooling to be possible.
-
-The heat exchanger will operate to heat the Loop Supply Side fluid when the following three conditions are all met:
-
-1)  the two inlet fluid temperatures are compared to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible,
-
-2)  the lower temperature setpoint on the reference node is compared to the inlet temperature for the Loop Supply Side to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible, and
-
-3) the lower temperature setpoint on the reference node is compared to the inlet temperature for the Loop Demand Side to see if their difference exceeds the minimum temperature difference and has the correct sign for heating to be possible.
-
-When the heat exchanger is turned “on,� the model requests the full design flow rate on the Loop Supply Side connection.  If the Loop Supply Side flow rate exceeds a small tolerance, then the full design flow rate is requested for the Loop Demand Side connection.
-
-### References
-
-Strand, R.K. and C.O. Pedersen, 1997.  Implementation of a Radiant Heating and Cooling Model Into an Integrated Building Energy Analysis Program, ASHRAE Transactions v. 103, n. 1, pp 949-958, 1997.
-
-Incropera, F.P. and D.P. DeWitt. 1981. Fundamentals of Heat Transfer. New York: John Wiley & Sons.
-
-Mills, A.F.1999. Heat Transfer, Second Edition. Prentice Hall. New Jersey.
-
-Presentation by Taylor Engineering.
-
-Air System Humidifiers <a name="Humidifiers"></a>
-----------------------
-
-### Overview
-
-Air system humidifiers are components that add moisture to the supply air stream. They fall into 2 broad categories: spray type humidifiers which act like direct evaporative coolers, cooling the supply air as well as humidifying it; and dry steam humidifiers, which humidify the supply air stream while causing almost no change to the supply air stream temperature. The EnergyPlus electric and gas fired steam humidifier uses electrical energy and thermal energy, respectively, to convert ordinary tap water to steam which it then injects into the supply air stream by means of a blower fan. The actual electric dry steam unit might be an electrode-type humidifier or a resistance-type humidifier.
-
-### Electric and Gas Steam Humidifier
-
-The electric and gas steam humidifier models (object names: Humidifier:Steam:Electric and Humidifier:Steam:Gas) are based on moisture and enthalpy balance equations plus standard psychrometric relationships. The approach is similar to that taken in the ASHRAE HVAC 2 Toolkit, page 4-112 (ASHRAE 1993). EnergyPlus contains its own module of psychrometric routines; the psychrometric theory and relations are given in the 2001 edition of ASHRAE Fundamentals, Chapter 6 (ASHRAE 2001). The model contains both an ideal controller and the component. The control model assumes that there is a minimum humidity setpoint on the component air outlet node. This setpoint is established by a setpoint manager described elsewhere.
-
-#### Model
-
-The component model is a forward model: its inputs are its inlet conditions; its outputs are its outlet conditions and its energy consumption. The inputs are the temperature, humidity ratio, and mass flow rate of the inlet air stream, which are known; and the water addition rate (kg/s) which is determined by the controller.  The moisture mass balance and psychometric calculations are identical for both gas and electric dry steam humidifiers.  The only difference is how a heat source (electric or gas) is used to generate the steam.
-
-#### Controller
-
-The controller first decides whether the humidifier is on or off. For the humidifier to be on:
-
-* the humidifier schedule value must be nonzero;
-
-* the inlet air mass flow must be greater than zero;
-
-* the inlet air humidity ratio must be less than the minimum humidity ratio setpoint.
-
-If the humidifier is off, the water addition rate is set to zero. If the humidifier is on, the water addition rate needed to meet the humidity setpoint is calculated.
-
-<div>$${\dot m_a} \cdot {w_{in}} + {\dot m_{w,add,needed}} = {\dot m_a} \cdot {w_{set}}$$</div>
-
-where
-
-<span>\({\dot m_a}\)</span> = the air mass flow rate [kg/s]
-
-<span>\({w_{in}}\)</span>= the inlet air humidity ratio [kg/kg]
-
-<span>\({\dot m_{w,add,needed}}\)</span> = water addition rate needed to meet the setpoint [kg/s]
-
-<span>\({w_{set}}\)</span>= the humidity ratio setpoint [kg/kg]
-
-Equation is the moisture balance equation for the component. It is solved for <span>\({\dot m_{w,add,needed}}\)</span> (the other variables are known) which is passed to the humidifier component model as its desired inlet water addition rate.
-
-#### Component
-
-The inputs to the component model are the air inlet conditions and mass flow rate and the water addition rate set by the controller. The outputs are the air outlet conditions. First the desired water addition rate is checked against component capacity.
-
-<div>$${\dot m_{w,add,needed,{\rm{max}}}} = Min({\dot m_{w,add}},Ca{p_{nom}})$$</div>
-
-where
-
-<span>\(Ca{p_{nom}}\)</span> = the humidifier nominal capacity [kg/s], a user input.
-
-If <span>\({\dot m_{w,add,needed,{\rm{max}}}}\)</span> is zero, the outlet conditions are set to the inlet conditions and the water addition rate is set to zero. If the humidifier is scheduled on the component power consumption is set to the standby power consumption: <span>\({W_{hum}} = {W_{stby}}\)</span>. Otherwise <span>\({W_{hum}}\)</span> = 0.
-
-If <span>\({\dot m_{w,add,needed,{\rm{max}}}}\)</span> &gt; 0, then the moisture and enthalpy balance equations
-
-<div>$${\dot m_a} \cdot {w_{in}} + {\dot m_w} = {\dot m_a} \cdot {w_{out}}$$</div>
-
-<div>$${\dot m_a} \cdot {h_{in}} + {\dot m_w} \cdot {h_w} = {\dot m_a} \cdot {h_{out}}$$</div>
-
-with <span>\({\dot m_w}\)</span> set equal to <span>\({\dot m_{w,add,needed,{\rm{max}}}}\)</span> are solved for <span>\({w_{out}}\)</span> and <span>\({h_{out}}\)</span>. Here
-
-<span>\({\dot m_a}\)</span> = the air mass flow rate [kg/s]
-
-<span>\({w_{in}}\)</span>= the inlet air humidity ratio [kg/kg]
-
-<span>\({\dot m_w}\)</span> = the inlet water addition rate [kg/s]
-
-<span>\({w_{out}}\)</span> = the outlet air humidity ratio [kg/kg]
-
-<span>\({h_{in}}\)</span> = the inlet air specific enthalpy [J/kg]
-
-<span>\({h_w}\)</span> = the steam specific enthalpy = 2676125.  [J/kg] at 100 <sup>o</sup>C
-
-<span>\({h_{out}}\)</span> = the outlet air specific enthalpy [J/kg]
-
-The outlet temperature is obtained from
-
-<div>$${T_{out}} = PsyHFnTdbW({h_{out}},{w_{out}})$$</div>
-
-where
-
-<span>\({T_{out}}\)</span> = outlet air temperature [<sup>o</sup>C],
-
-<span>\(PsyHFnTdbW({h_{out}},{w_{out}})\)</span> is an EnergyPlus psychrometric function.
-
-The humidity ratio at saturation at the outlet temperature is
-
-<div>$${w_{out,sat}} = PsyWFnTdbRhPb({T_{out}},1.0,{P_{atmo}})$$</div>
-
-where
-
-<span>\({P_{atmo}}\)</span> = the barometric pressure [Pa],
-
-1.0 is the relative humidity at saturation,
-
-<span>\(PsyWFnTdbRhPb\)</span> is an EnergyPlus psychrometric function.
-
-IF <span>\({w_{out}} \le {w_{out,sat}}\)</span> then the outlet condition is below the saturation curve and the desired moisture addition rate can be met. <span>\({\dot m_{w,add}}\)</span> is set to <span>\({\dot m_{w,add,needed,{\rm{max}}}}\)</span> and the calculation of outlet conditions is done. But if <span>\({w_{out}} > {w_{out,sat}}\)</span> then it is assumed that this condition will be detected and the steam addition rate throttled back to bring the outlet conditions back to the saturation condition. We need to find the point where the line drawn between state 1 (inlet) and state 2 (our desired outlet) crosses the saturation curve. This will be the new outlet condition. Rather than iterate to obtain this point, we find it approximately by solving for the point where 2 lines cross: the first drawn from state 1 to state 2, the second from <span>\({T_1}\)</span>, <span>\({w_{1,sat}}\)</span> to <span>\({T_2}\)</span>, <span>\({w_{2,sat}}\)</span>; where
-
-<span>\({w_{1,sat}}\)</span> is the inlet temperature [<sup>o</sup>C],
-
-<span>\({w_{2,sat}}\)</span> is the humidity ratio at saturation at temperature <span>\({w_{1,sat}}\)</span> [kg/kg],
-
-<span>\({T_2}\)</span> is the desired outlet temperature [<sup>o</sup>C],
-
-<span>\({w_{2,sat}}\)</span> is the humidity ratio at saturation at temperature <span>\({T_2}\)</span> [kg/kg].
-
-The 2 lines are given by the equations:
-
-<div>$$w = {w_1} + (({w_2} - {w_1})/({T_2} - {T_1})) \cdot (T - {T_1})$$</div>
-
-<div>$$w = {w_{1,sat}} + (({w_{2,sat}} - {w_{1,sat}})/({T_2} - {T_1})) \cdot (T - {T_1})$$</div>
-
-Solving for the point (state 3) where the lines cross:
-
-<div>$${w_3} = {w_1} + (({w_2} - {w_1}) \cdot ({w_{1,sat}} - {w_1}))/({w_2} - {w_{2,sat}} + {w_{1,sat}} - {w_1})$$</div>
-
-<div>$${T_3} = {T_1} + ({w_3} - {w_1}) \cdot (({T_2} - {T_1})/({w_2} - {w_1}))$$</div>
-
-This point isn't quite on the saturation curve since we made a linear approximation of the curve, but the temperature should be very close to the correct outlet temperature. We will use this temperature as the outlet temperature and move to the saturation curve for the outlet humidity and enthalpy. Thus we set <span>\({T_{out}}\)</span> = <span>\({T_3}\)</span> and
-
-<div>$${w_{out}} = PsyWFnTdbRhPb({T_{out}},1.0,{P_{atmo}})$$</div>
-
-<div>$${h_{out}} = PsyHFnTdbW({T_{out}},{w_{out}})$$</div>
-
-where <span>\(PsyHFnTdbW\)</span> is an EnergyPlus psychrometric function. The water addition rate is set to
-
-<div>$${\dot m_{w,add}} = {\dot m_a} \cdot ({w_{out}} - {w_{in}})$$</div>
-
-We now have the outlet conditions and the adjusted steam addition rate for the case where the desired outlet humidity results in an outlet state above the saturation curve.  The energy consumption of the electric and gas steam humidifiers is calculated separately.
-
-The electric steam humidifier electric consumption is given by
-
-<div>$${W_{hum}} = ({\dot m_{w,add}}/Ca{p_{nom}}) \cdot {W_{nom}} + {W_{fan}} + {W_{stby}}$$</div>
-
-where
-
-<span>\({W_{fan}}\)</span> = nominal fan power [W], a user input,
-
-<span>\({W_{stby}}\)</span> = standby power [W], a user input.
-
-The gas steam humidifier performance calculation is done for fixed and variable entering water temperature. The calculation procedure for fixed and variable entering water temperature are as follows.
-
-#### Fixed Inlet WaterTemperature:
-
-The gas steam humidifier gas consumption rate for fixed entering water temperature is given by:
-
-<div>$$\dot{Q}_{NG} = \frac{\dot{m}_{w,add}}{\dot{m}_{cap,nom}}Q_{NG,nom}$$</div>
-
-The actual gas use rate accounting for gas fired humidifier thermal efficiency variation with part load ratio is given by: 
-
-<div>$$ Q_{NG}=\dot{Q}_{NG}\frac{\eta_{rated}}{\eta_{actual}} $$</div>
-
-<div>$$ \eta_{actual} = \eta_{rated} \times \rm{EffModCurveValue}\left(PLR\right) $$</div>
-
-<div>$$ \rm{PLR} = \frac{\dot{Q}_{NG}}{Q_{NG,nom}} $$</div>
-
-where,
-EffModCurveValue = thermal efficiency modifier curve value as function of part load ratio. This curve is generated from manufacturer’s part load performance data. 
-PLR = part load ratio, (-).
-Q_NG_nom = nominal or rated gas use rate, (Watts).
-Q_NG = actual gas use rate, (Watts).
-eta_rated = nominal or rated thermal efficiency of gas fired steam humidifier, (-)
-eta_actual = actual thermal efficiency of gas fired steam humidifier accounting for part load performance, (-). 
-
-#### Variable Inlet WaterTemperature: 
-
-The gas use rate is determined from the theoretical gas input rate and actual thermal efficiency. The actual thermal efficiency is the rated thermal efficiency corrected for part load ratio operation. At steady state the gas use rate is given by:
-
-<div>$$ Q_{NG}=\frac{\dot{m}_w \left(h_{fg}+c_{p,w}\left(100-T_{w,inlet}\right)\right)}{\eta_{rated}} $$</div>
-
-<div>$$ \rm{PLR} = \frac{\dot{Q}_{NG}}{Q_{NG,nom}} $$</div>
- 
-<div>$$ \eta_{actual} = \eta_{rated} \times \rm{EffModCurveValue}\left(PLR\right) $$</div>
- 
-<div>$$ Q_{NG}=\dot{Q}_{NG}\frac{\eta_{rated}}{\eta_{actual}} $$</div> 
-
-where,
-T_w_inlet = temperature of water entering the gas steam humidifier, °C. This value depends on the water source.  
-
-If the rated gas use rated input field is not autosized, then user specified thermal efficiency will be overriden with a value calculated from user specified rated gas use rate, nominal  capacity (m3/s) and design conditions as follows:
-
-<div>$$ \eta_{rated}=\frac{\dot{V}_{cap,nom} \rho_w \left(h_{fg}+c_{p,w}\Delta T_w}{Q_{NG,nom}} $$</div>
-
-The gas steam humidifier requires electric power input to the blower fan and associated control units.  The auxiliary electric power input rate of the gas steam humidifier is given by:
-
-<div>$$W_{aux} = W_{fan} + W_{controls}$$</div>
- 
-where
-W_fan = nominal fan power [W], a user input,
-W_controls = control electric power [W], a user input.
-
-The water consumption rate is, in m3/s, for electric and steam humidifier at a reference temperature of 5.05 C is given by.
-
-<div>$${\dot V_{cons}} = {\dot m_{w,add}}/{\rho_w}$$</div>
-
-where
-
-<span>\({\dot V_{cons}}\)</span> = the water consumption rate [m<sup>3</sup>],
-
-<span>\({\rho_w}\)</span> = water density (998.2 kg/m<sup>3</sup>).
-
-#### References
-
-ASHRAE. 1993. HVAC 2 Toolkit: A Toolkit for Secondary HVAC System Energy Calculations. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2001. 2001 ASHRAE Handbook Fundamentals. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
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-
-<!--RemoveStart-->
-Simulation Models – Encyclopedic Reference
-==========================================
-
-The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of “Heat Balance�, “HVAC�, and “Plant�.  With the integrated solution, these designations signify where the effects of these models have their first impacts.
-
-Main Sections:
-
-* [Zone Internal Gains](#ZoneGains)
-* [Indoor Swimming Pool ](#IndoorSwimmingPool)
-* [Pipes](#Pipes)
-* [Pumps](#Pumps)
-* [Ideal Loads Air System](#IdealLoads)
-* [District Cooling](#DistrictCooling)
-* [District Heating](#DistrictHeating)
-* [CentralHeatPumpSystem](#CentralHeatPumpSystem)
-* [ChillerHeater](#ChillerHeater)
-* [Plant Temperature Source Component](#PlantComponents)
-<!--RemoveEnd-->
-
-Zone Internal Gains <a name="ZoneGains"></a>
--------------------
-
-### Sources and Types of Gains
-
-Internal heat gains from lights, people, and equipment of various types are often significant elements in the zone thermal balance.  EnergyPlus allows the user to specify heat gains for several equipment types including people, lights, gas/electric equipment, and several other types.  The total heat gain is comprised of convective, radiant and latent gains in various proportions from these sources.  Convective gains are instantaneous additions of heat to the zone air.  Radiant gains are distributed on the surfaces of the zone, where they are first absorbed and then released back into the room (with some fraction conducted through the surface) according to the surface heat balances. {See Surface Heat Balance Manager / Processes in this document}.  Latent gains must be handled by ventilation or air conditioning equipment.  Recommended heat gains are given by ASHRAE [1].  These recommendations include the sensible (convective plus radiative) and latent proportions.  Sensible gains from equipment are primarily radiant.  The user can specify the heat gains and proportions for any type of equipment.  Determining the gains from lights, people and baseboard heat are slightly more complicated.
-
-### Heat Gain from Lights
-
-The input object Lights provides a model for internal gains from lights.  Radiant gains from lights must be handled differently from other radiant gains for reasons described here (long wavelength description).  The total radiant gains from lights must be divided into visible and thermal portions.  For example, the total electric input to typical incandescent lights is converted to 10% visible radiation, 80% thermal radiation, and 10% convective gain.  In contrast, the electric input to typical fluorescent lights is converted to 20% visible radiation, 20% thermal radiation, and 60% convective gain [2].  These percentage splits are under user control with the Lights input object.
-
-### Heat Gain from People
-
-The input object People provides a model for internal gains from occupants.  Heat is generated in the human body by oxidation at a rate called the metabolic rate (see Thermal Comfort discussion for more details).  This heat is dissipated from the body surface and respiratory tract by a combination of radiation, convection, and evaporation.  The relative proportions of sensible (radiation plus convection) and latent (evaporation) heat from people is a complex function of the metabolic rate and the environmental conditions.  EnergyPlus uses a polynomial function to divide the total metabolic heat gain into sensible and latent portions.  That function is based on a fit to data [3] at average adjusted metabolic rates of 350, 400, 450, 500, 750, 850, 1000 and 1450 Btu/h each at temperatures of 70, 75, 78, 80, 82 degrees Fahrenheit.  Sensible gains of 0 at 96 F and sensible gains equal to the metabolic rate at 30 F were assumed in order to give reasonable values beyond the reported temperature range.
-
-Average adjusted metabolic rate [3] is the metabolic rate to be applied to a mixed group of people with a typical percent composition based on the following factors:
-
-Metabolic rate, adult female=Metabolic rate, adult male X 0.85
-
-Metabolic rate, children = Metabolic rate, adult male X 0.75
-
-The original data was in I-P (Inch-Pound) units, but the following correlation is in SI (Systems-International) units.
-
-<div>$$\begin{array}{c}S = 6.461927 + .946892\cdot M + .0000255737\cdot {M^2}\\ + 7.139322\cdot T - .0627909\cdot T\cdot M + .0000589172\cdot T\cdot {M^2}\\ - .198550\cdot {T^2} + .000940018\cdot {T^2}\cdot M - .00000149532\cdot {T^2}\cdot {M^2}\end{array}$$</div>
-
-where
-
-M=Metabolic Rate (W)
-
-T=Air Temperature (C)
-
-S=Sensible Gain (W)
-
-Latent Gain is simply the total gain (metabolic rate) – sensible gain:
-
-<div>$$LatentGain = MetabolicRate - SensibleGain$$</div>
-
-![](media/image5820.png)
-
-Figure 259.  Sensible Heat Gain from People Correlation
-
-The function for sensible gain calculation is compared to the original data points in the following figure.  The radiant fraction of the sensible gain is a user input on the People object.
-
-### Heat Gain from IT Equipment
-
-The input object ElectricEquipment:ITE:AirCooled describes air-cooled electric information technology equipment (ITE) which has variable power consumption as a function of loading and temperature. The calculations are described below.
-
-#### Variable Definitions – User Inputs:
-
-* PDesign = Design power input when fully loaded and entering air temperature is at the user-specified design inlet temperature [W]
-* PFanFracDesign = Design fan power input fraction of total power input when fully loaded and entering air temperature is at the user-specified design inlet temperature
-* SchDesignLevel = Scheduled fraction of this equipment which is powered up
-* SchCPULoading = Scheduled fraction of CPU loading
-* TAirInDesign = Air inlet temperature at design condition [C]
-* VAirDesign = Air volume flow rate at design condition [m3/s]
-* VAirfLoadTAir = Air volume flow rate modifier function of TAirIn and SchCPULoading
-* PCPUfLoadTAir = CPU power input modifier function of TAirIn and SchCPULoading
-* PFanfFlowFrac = Fan power input modifier function of air flow fraction
-* RecircFracDesign = Recirculation Fraction at design condition [C]
-* RecircfLoadTAir = Recirculation Fraction modifier function of TAirSupply and SchCPULoading
-* UPSEfficDesign = Design electric power supply efficiency
-* UPSEfficfPLR = Electric power supply efficiency function of part load ratio
-* UPSLossFracToZone = Fraction of electric power supply losses to zone
- 
-#### Variable Definitions – Simulation Inputs:
-
-* TAirIn = Air inlet temperature at current conditions [C]
-* TAirSupply = Supply air node temperature at current conditions [C]
-* TZone = Zone air temperature at current conditions [C]
-* TRoomAirNodeIn = Room air model inlet node air temperature at current conditions [C]
-* RhoAir = Air density [kg/m3]
-* CpAir = Air specific heat [J/kg-K]
- 
-#### Variable Definitions – Intermediate Calculations:
-
-* PCPUDesign = Design CPU power input when fully loaded and entering air temperature is at the user-specified design inlet temperature [W]
-* PFanDesign = Design fan power input when fully loaded and entering air temperature is at the user-specified design inlet temperature [W]
-* UPSPLR = Electric power supply part load ratio (can be greater than 1.0)
- 
-#### Variable Definitions – Outputs:
-
-* PCPU = CPU power input [W]
-* PFan = Fan power input [W]
-* PUPS = Electric power supply net power input [W]
-* TAirOut = Air outlet temperature [C]
-* VAir = Air volume flow rate [m3/s]
-* FlowFrac = Air volume flow rate fraction of design flow rate
-* RecircFrac = Recirculation fraction
-* QAir = Air cooling rate [W]
-* QUPS = Electric power supply heat loss rate to zone [W]
-* QConv = Convective heat gain rate to zone heat balance [W]
-* SHI = Supply heat index
-* SHIZone = Zone average supply heat index
- 
-#### Calculations
-
-The design power input is first split into portions for the CPU (everything in the equipment except the cooling fans) and the fan(s).
-
-PCPUDesign = PDesign * (1 - PFanFracDesign)
- 
-PFanDesign = PDesign * PFanFracDesign
- 
-For each time step, the air inlet temperature is calculated depending on the type of air node connection.
- 
-TAirIn:
-
-* If Air Node Connection Type = AdjustedSupply
-    * RecircFrac = RecircFracDesign * RecircfLoadTAir(SchCPULoading TAirSupply)
-    * TAirIn = TAirSupply * (1 – RecircFrac) +TAirZone * RecircFrac
- 
-* If Air Node Connection Type = ZoneAirNode
-    * TAirIn = TAirZone
- 
-* If Air Node Connection Type = RoomAirModel
-    * TAirIn = TRoomAirNodeIn
- 
-Using the air inlet temperature, the CPU power consumption, air flow rate, fan power consumption, and power supply power consumption are calculated.
- 
-PCPU = PCPUDesign * SchDesignLevel * PfLoadTAir(SchCPULoading, TAirIn)
- 
-FlowFrac = VAirfLoadTAir(SchCPULoading, TAirIn)
- 
-VAir = VAirDesign * FlowFrac
- 
-PFan = PFanDesign * SchDesignLevel * PFanfFlowFrac(FlowFrac)
- 
-UPSPLR = (PCPU + PFan) / (PCPUDesign + PFanDesign)
- 
-PUPS = (PCPU + PFan) * (1 - UPSEfficDesign * UPSEfficfPLR (UPSPLR))
- 
-The convective heat gain to the zone and the air outlet temperature are then calculated. The user specified fration of power supply losses are always added to the general zone heat balace convective heat gain. For air node connection types AdjustedSupply and ZoneAirNode, the CPU and fan power consumption are also added to the zone convective heat gain. For air connection type RoomAirModel, the gains from the CPU and fan power consumption are added to the outlet room air model node.
- 
-QAir = PCPU + PFan
- 
-QUPS = PUPS * UPSLossFracToZone
- 
-QConv:
-
-* If Air Node Connection Type = AdjustedSupply OR ZoneAirNode
-    * QConv = QAir + QUPS
- 
-* If Air Node Connection Type = RoomAirModel
-    * QConv = QUPS
- 
-TAirOut = TAirIn + QAir / (VAir * RhoAir * CpAir)
- 
-The individual ITE supply heat index is calculated as shown below.
- 
-SHI = (TAirIn – TAirSupply) / (TAirOut - TAirSupply)
- 
-The zone average ITE supply heat index is weighted by the air flow rate of each ITE object.
- 
-SHIZone = ∑ [VAir * (TAirIn – TAirSupply)] / ∑ [VAir * (TAirOut - TAirSupply)]
-
-### Heat Gain from Baseboard Heat
-
-The input object ZoneBaseboard:OutdoorTemperatureControlled provides a model for an outdoor temperature controlled baseboard heater that adds energy to the zone according a control profile as shown in the following figure.  At TA = T2, the baseboard heat gain is Q2.  For TA &gt; T2, there is no heat gain.  For TA &lt; T1, a maximum amount of energy, Q1, is added to the zone.  There is proportional control between those two temperatures:
-
-![](media/image5821.png)
-
-Figure 260.  Control of Outdoor Temperature Controlled Baseboard Heat
-
-<div>$$Q = Q2 - \frac{{(Q2 - Q1)\cdot (T2 - TA)}}{{(T2 - T1)}}$$</div>
-
-These temperature and capacity fields can be autosized based upon envelope, infiltration, and ventilation loads. To autosize these fields, users may set a design zone heating temperature that is assumed to be 20°C if blank.
-
-The capacity at low temperature is the maximum capacity of the unit. It includes external envelope conduction load, infiltration load, and ventilation load in a space where the unit serves. The model first finds the lowest outdoor air temperature throughout design days included in the simulation, and determines the conduction load through external envelop as:
-
-<div>$${q_{Cond}} = UA\left( {{T_{Htg}} - {T_L}} \right)$$</div>
-
-where
-
-*q<sub>Cond</sub>* is conduction load through external envelope, W
-
-*U* is heat transfer coefficient of external wall, W/m<sup>2</sup>K
-
-*A* is area of external wall, m<sup>2</sup>
-
-*T<sub>Htg</sub>* is baseboard zone heating setpoint temperature, °C
-
-*T<sub>L</sub>* is low temperature, °C
-
-
-
-The capacity at low temperature that is the maximum capacity of the unit is thus expressed as:
-
-<div>$$Ca{p_{{T_L}}} = {q_{Cond}} + {q_I} + {q_V}$$</div>
-
-where
-
-<span>\(Ca{p_{{T_L}}}\)</span>is capacity at low temperature, W
-
-*q<sub>I</sub>* is design infiltration sensible load, W
-
-*q<sub>V</sub>* = design ventilation sensible load, W
-
-
-
-The capacity at high temperature is then prorated against the reference low and high temperatures as:
-
-<div>$$Ca{p_{{T_H}}} = Ca{p_{{T_L}}}\frac{{\left( {{T_{Htg}} - {T_H}} \right)}}{{\left( {{T_{Htg}} - {T_L}} \right)}}$$</div>
-
-where
-
-<span>\(Ca{p_{{T_H}}}\)</span> is capacity at high temperature, W
-
-*T<sub>H</sub>* is high temperature, °C
-
-
-
-### Distribution of Radiant Gains
-
-It is useful to consider the distribution of short wavelength (including visible) radiant energy separate from long wavelength (thermal) radiant energy because many materials have different optical properties at different wavelengths.  An extreme example is glass that is opaque to the long wavelengths and transparent to the short.  Properties of materials vary across the entire spectrum of wavelengths.  In EnergyPlus, all radiant interactions are represented in terms of only two wavelengths: “short� and “long�.  Short wavelength refers to the distribution given by a ~6000K black body source such as the sun.  Long wavelengths refer to radiation from ~300K sources such as walls or people.  There is negligible overlap between these two distributions.  Some sources, such as lights, must be considered as emitting both long and short wavelength radiation in proportions that approximate their actual effects on room surfaces.
-
-Long wavelength radiation from all internal sources, such as people, lights and equipment, is combined and then distributed over surfaces. (see Internal Long-Wave Radiation Exchange).
-
-Some fraction of the beam solar radiation transmitted into the zone is directly absorbed by the interior surfaces according to the solar distribution algorithm (see Solar Distribution) selected by the user.  The beam radiation not directly absorbed, plus the diffuse sky and ground-reflected radiation, plus the short wavelength radiation from lights are combined and distributed over the surfaces of the zone according to:
-
-<div>$$QS{I_i} = Q{S_n}\cdot {\alpha_i}/\sum\limits_{i = 1}^{NS} {{S_i}\cdot (1 - {\rho_i})} $$</div>
-
-If all surfaces in the room are opaque, the radiation is distributed in proportion to the area\*absorptance product of each surface.  For surfaces which are transparent,
-
-<div>$${\rho_i} = 1 - {\alpha_i} - {\tau_i}$$</div>
-
-That fraction of radiation represented by <span>\({\tau_i}\)</span> is lost from the zone.
-
-The transmittance and absorptance of transparent surfaces (windows or glass doors) are calculated as in section Window Calculation Module based on the optical properties of the window material layers.  The total absorptance of the window is computed for the interior shading device, the inside surface, and the outside surface for diffuse solar radiation incident from outside the zone.  Those absorptances are used for short wavelength radiation incident from inside the zone.  In most cases, this should not cause significant error.  When movable insulation covers the window, the radiation that would have been transmitted is absorbed at the outer surface of the window (thermally equal to the inside surface of the insulation).
-
-### References
-
-ASHRAE. 2001. Handbook of Fundamentals, pp 29.8-29.13, Atlanta: ASHRAE.
-
-Carrier Air Conditioning Company. 1965a. Handbook of Air Conditioning System Design, pp 1-99 to 1-100. New York: McGraw Hill.
-
-Carrier Air Conditioning Company. 1965b. Handbook of Air Conditioning System Design, pp 1-100, Table # 48. New York: McGraw Hill.
-
-Indoor Swimming Pool <a name="IndoorSwimmingPool"></a>
------
-
-The modeling of the indoor swimming pool is integrated into the surface heat balance procedures already in EnergyPlus with special modifications for radiation between the pool water surface and the surrounding of the space, convection to the surrounding air, evaporation of water, conduction to the pool bottom, and solar radiation absorbed in the pool water, the pool heating system, the presence of a cover, etc.  Effectively, the pool water mass is “added� to or lumped into the inside face of the surface to which the pool is “linked�.  Conduction through the floor uses the standard CTF formulation, however the heat balance is modified to include other terms specific to the pool water.
-
-Some assumptions of the model are given below, followed by more details of individual components of the model.
-
-* The pool water is lumped together at the inside face of a surface and follows the standard EnergyPlus heat balance methodology with some modifications based on the pool model details described in this section.
-* The pool itself must reference a surface that is specifically defined as a floor and it covers the entire floor to which it is linked.
-* The pool cannot by part of a low temperature radiant system (meaning that the construction of the floor cannot have any embedded pipes for heating or cooling).  In addition, the floor/pool cannot be defined with any movable insulation or be defined as a ventilated slab.
-* The pool/floor surface must use the standard CTF solution algorithm.
-* The pool may be covered and the fraction covered is defined by user input.  This value may vary from 0.0 to 1.0.
-* The pool cover has an impact on evaporation, convection, short-wavelength radiation, and long-wavelength radiation.  Each of these has a separate user input that reduces the heat transfer parameter from the maximum achieved with a cover.  While the cover percentage is allowed to vary via a user schedule input, each individual parameter for these four heat transfer modes is a fixed constant.  For evaporation and convection, the factors simply reduce the amount of heat transfer proportionally.  For the radiation terms, the factors reduce the amount of radiation that impacts the surface (pool) directly.  The remaining radiation is assumed to be convected off of the pool cover to the zone air.
-* Pool water heating is achieved by defining the pool as a component on the demand side of a plant loop.
-* Makeup water replaces any evaporation of water from the pool surface and the user has control over the temperature of the makeup water.
-* The pool is controlled to a particular temperature defined by user input.
-* Evaporation of water from the pool is added to the zone moisture balance and affects the zone humidity ratio.
-* The pool depth is small in comparison to its surface area.  Thus, heat transfer through the pool walls is neglected.  This is in keeping with the standard assumption of one-dimensional heat transfer through surfaces in EnergyPlus.
-
-### Energy Balance of Indoor Swimming Pool
-
-Heat losses from indoor swimming pools occur by a variety of mechanisms. Sensible heat transfer by convection, latent heat loss associated with evaporation, and net radiative heat exchange with the surrounding occur at the pool surface. Conductive heat losses take place through the bottom of the pool.  Other heat gains/losses are associated with the pool water heating system, the replacement of evaporated water with makeup water The energy balance of the indoor swimming pool estimates the heat gains/losses occurring due to:
-
-* convection from the pool water surface
-* evaporation from the pool water surface
-* radiation from the pool water surface
-* conduction to bottom of pool
-* fresh pool water supply
-* pool water heating by the plant
-* changes in the pool water temperature
-
-Detailed methods for estimating these heat losses and gains of the indoor swimming pools are described in the subsections below.
-
-### Convection from the pool water surface
-
-The convection between the pool water and the zone are defined using:
-
-<div>$$Q_{conv} = h \cdot A \cdot (T_p – T_a)$$</div>
-
-<div>$$h = 0.22 \cdot (T_p – T_a)1/3$$</div>
-
-where
-
-$Q_{conv}$ = Convective heat transfer rate (Btu/h·ft2)
-
-$h$ = Convection heat transfer coefficient (Btu/h· ft2·�F)
-
-$T_p$ = Pool water temperature (�F)
-
-$T_a$ = Air temperature over pool (�F)
-
-When a cover is present, the cover and the cover convection factor reduce the heat transfer coefficient proportionally.  For example, if the pool is half covered and the pool cover reduces convection by 50%, the convective heat transfer coefficient is reduced by 25% from the value calculated using the above equation.
-
-### Evaporation from the pool water surface 
-
-There are 5 main variables used to calculate the evaporation rate ($Q_{evap}$):
-
-* Pool water surface area 
-* Pool water temperature
-* Room air temperature
-* Room air relative humidity
-* Pool water agitation and Activity Factor
-
-<div>$$\dot{m}_{evap} = 0.1 \cdot A \cdot AF \cdot (P_w – P_{dp})$$</div>
-
-where
-
-$\dot{m}_{evap}$ = Evaporation Rate of pool water (lb/h)
-
-$A$ = Surface area of pool water (ft²)
-
-$AF$ = Activity factor
-
-$P_w$ = Saturation vapor pressure at surface of pool water (in. Hg)
-
-$P_{dp}$ = Partial vapor pressure at room air dew point (in. Hg)
-
-Typical Activity Factor (AF)
-
-<table class="table table-striped">
-
-<tr>
-<th>Type of Pool</th><th>Activity Factor (AF)</th>
-</tr>
-<tr>
-<td>Recreational</td><td>0.5</td>
-</tr>
-<tr>
-<td>Physical Therapy</td><td>0.65</td>
-</tr>
-<tr>
-<td>Competition</td><td>0.65</td>
-</tr>
-<tr>
-<td>Diving</td><td>0.65</td>
-</tr>
-<tr>
-<td>Elderly Swimmers</td><td>0.5</td>
-</tr>
-<tr>
-<td>Hotel</td><td>0.8</td>
-</tr>
-<tr>
-<td>Whirlpool, Spa</td><td>1.0</td>
-</tr>
-<tr>
-<td>Condominium</td><td>0.65</td>
-</tr>
-<tr>
-<td>Fitness Club</td><td>0.65</td>
-</tr>
-<tr>
-<td>Public, Schools</td><td>1.0</td>
-</tr>
-<tr>
-<td>Wave Pool, Water Slides</td><td>1.5 – 2.0</td>
-</tr>
-
-</table>
-
-When a cover is present, the cover and the cover evaporation factor reduce the amount of evaporation proportionally.  For example, if the pool is half covered and the pool cover reduces convection by 50%, the convective heat transfer coefficient is reduced by 25% from the value calculated using the above equation.
-The value is converted to a latent gain (loss) through multiplication of the evaporation rate by the heat of vaporization of water.
-
-### Radiation exchange with the pool water surface 
-
-This uses the EnergyPlus internal short- and long-wavelength radiation balances already in place.  When a cover is present, it acts to reduce the amount of radiation that arrives at the pool water surface in comparison to the no cover case.  Any reduction in either type of radiation is accounted for by adding a convective gain/loss to the zone air.  So, in effect, the cover absorbs some radiation and then convects it to the zone air.
-
-### Conduction through the bottom of the pool
-
-The model ignores 2-d effects of pool walls and assume that pool depth is much less than the pool area. Conduction is calculated using the Conduction Transfer Function (CTF) equation with the outside temperature determined by the outside heat balance and the inside surface temperature calculated using the pool water heat balance that is lumped together with the inside surface heat balance.
-
-### Makeup pool water supply
-
-<div>$$Q_{fw} = m_{fw} \cdot cw \cdot (T_p – T_{fw})$$</div>
-
-where
-
-$m_{fw}$ = Mass flow rate
-
-$c_w$ = Specific heat of water 
-
-$T_p$ = Pool water temperature
-
-$T_{fw}$ = Fresh water supply temperature
-
-### Heat Gain from People
-
-The input for the swimming pool requires that the user enter the maximum number of people in the pool, a schedule modifying the maximum number of people for different pool occupancies, and a heat gain per person schedule for differing activities.  These three parameters allow for the calculation of a total heat gain from () ̇during a given time.  It is assumed that all of the heat gain from people is via convection to the pool water.
-
-### Heat from auxiliary pool heater
-
-<div>$$Q_{fw} = m_{hw} \cdot c_w \cdot (T_p – T_{hw})$$</div>
-
-where
-
-$m_{hw}$ = Mass flow rate (lb·s)
-
-$c_w$ = Specific heat of water (Btu/lb·�F)
-
-$T_p$ = Pool water temperature (�F)
-
-$T_{hw}$ = Heated water supply temperature (�F)
-
-### Pool Heating to Control the Pool Water Temperature
-
-The equation used to determine the flow rate request of hot water from the plant is an extremely simplified version of the pool heat balance.  This is because the mass of the pool is so much larger than any of the other heat flows.  As a result, for the sake of establishing a heated water flow rate, the following equation is used:
-
-<div>$$\frac{m_w c_p}{\Delta t} (T_{set}-T_{old}) = \dot{m}_p \cdot c_p \cdot (T_{in} - T_{set} )$$</div>
-
-where
-
-$m_w$ = mass of pool water
-
-$cp$ = specific heat of water
-
-$\Delta t$ = time step length
-
-$T_{set}$ = desired pool water temperature
-
-$T_{old}$ = temperature of water at the last time step
-
-$m_p$ = needed mass flow rate of water from the plant
-
-$T_{in}$ = inlet water temperature from the plant
-
-This equation is rearranged to solve for the needed mass flow rate of water from the plant since all of the other terms are known or given based on user input.  This establishes a flow request to the plant and is capped at the maximum value defined in input by the user.
-
-### Pool/Surface Heat Balance Equation Summary
-
-The following equation is the basis for the pool/surface heat balance.  As has been mentioned previously, the pool water is “merged� with the inside surface heat balance which is essentially the same thing as lumping the entire water of the pool in the inside surface heat balance.
-
-<div>$$\frac{m_w \cdot c_p}{\Delta t} (T_{set} - T_{old}) = Q_{cond} + Q_{conv} + Q_{lwrad} + Q_{swrad} + Q_{damp} + Q_{muw} + Q_{heater} + Q_{evap}$$</div>
-
-where
-
-$\frac{m_w \cdot c_p}{\Delta t} (T_{set} - T_{old} )$ = the change in energy stored in the pool water
-
-$Q_{cond}$ = net conduction to/from the pool water to the floor
-
-$Q_{conv}$ = net convection between the pool water and the zone air
-
-$Q_{lwrad}$ = net long-wavelength radiation between the pool water/floor and the surrounding surfaces as well as from internal heat gains
-
-$Q_{swrad}$ = net short-wavelength radiation to the pool water/floor from solar and internal heat gains
-
-$Q_{damp}$ = standard damping term used in the inside heat balance to avoid large swings in the radiation balance that sometimes cause instability in the solution (see the standard heat balance information for more details)
-
-$Q_{muw}$ = net gain/loss from replacing water evaporated from the pool with makeup water
-
-$Q_{heater}$ = net heat added to the pool via the plant loop (controlled to maintain a setpoint temperature as described above)
-
-$Q_{evap}$ = net heat loss due to evaporation of pool water to the zone air
-
-Details on each of these terms was either provided in previous parts of this section or in the standard EnergyPlus heat balance discussion elsewhere in the Engineering Reference.
-
-### Other additional information
-
-The following subsections are some useful information that those wishing to model a swimming pool in EnergyPlus might find helpful.  Further information can be found on-line or in reputable sources such as the ASHRAE Handbooks.
-
-### Swimming Pool Flow Rate
-
-The flow rate of the circulating pump is designed to turn over (circulate) the entire volume of water in the pool in 6 to 8 hours, or 3 or 4 times in 24 hours. About 1 or 2 percent of the pumped circulation rate should be provided as continuous makeup water demand to overcome losses from evaporation, bleed-off, and spillage. To fill the pool initially, a separate quick-fill line should be provided to do the job in 8 to 16 hours; however, filling is usually done at off-peak hours. Thus, the demand flow rate need not be considered in the system demand calculations, unless it out-weighs the demand of all other demands even during the off-peak hours.
-
-### Comfort and Health
-
-Indoor pools are normally maintained between 50 and 60% RH for two reasons:
-
-* Swimmers leaving the water feel chilly at lower relative humidity due to evaporation off the body
-* It is considerably more expensive (and unnecessary) to maintain 40% RH instead of 50% RH
-
-### Air Delivery Rates (Indoor Pool)
-
-Most codes require a minimum of 6 ACH, except where mechanical cooling is used. This rate may prove inadequate for some occupancy and use. Where mechanical dehumidification is provided, air delivery rates should be established to maintain appropriate conditions of temperature and humidity. The following rates are typically desired:
-
-* Pools with no spectator areas, 4 ~ 6 ACH
-* Spectator areas, 6 ~ 8 ACH
-* Therapeutic pools, 4 ~ 6 ACH
-
-Typical Swimming Pool Design Conditions
-
-<table class="table table-striped">
-<tr>
-<th>Type of Pool</th><th>Air Temperature, �C</th><th>Water Temperature, �C</th>
-</tr>
-<tr>
-<td>Recreational</td><td>24-30</td><td>24-30</td>
-</tr>
-<tr>
-<td>Physical Therapy</td><td>26-30</td><td>30-32</td>
-</tr>
-<tr>
-<td>Competition</td><td>26-29</td><td>24-28</td>
-</tr>
-<tr>
-<td>Diving</td><td>27-29</td><td>27-32</td>
-</tr>
-<tr>
-<td>Elderly Swimmers</td><td>29-32</td><td>29-32</td>
-</tr>
-<tr>
-<td>Hotel</td><td>28-29</td><td>28-30</td>
-</tr>
-<tr>
-<td>Whirlpool / Spa</td><td>27-29</td><td>36-40</td>
-</tr>
-</table>
-
-
-### References
-
-ASHRAE (2011). 2011 ASHRAE Handbook – HVAC Applications. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc., p.5.6-5.9.
-
-Janis, R. and W. Tao (2005). Mechanical and Electrical Systems in Buildings. 3rd ed. Upper Saddle River, NJ: Pearson Education, Inc., p.246.
-
-Kittler, R. (1989). Indoor Natatorium Design and Energy Recycling. ASHRAE Transactions 95(1), p.521-526.
-
-Smith, C., R. Jones, and G. Löf (1993). Energy Requirements and Potential Savings for Heated Indoor Swimming Pools. ASHRAE Transactions 99(2), p.864-874.
-
-
-Pipes <a name="Pipes"></a>
------
-
-### Heat Transfer Pipes (Objects: Pipe:Indoor & Pipe:Outdoor)
-
-#### Heat Loss and Time Delay in Pipes
-
-The effects of heat loss and time delay in plant loop pipes exposed to air (Pipe:Indoor and Pipe:Outdoor) can be modeled explicitly in EnergyPlus. Users can select the environment with which the pipe transfers heat. Currently users have three options: ‘OutdoorAir’, ‘Zone’ and ‘Schedule’. Simulation for each of the environments is similar except the way in which the heat transfer between the pipe outer wall and the surrounding environment is calculated. When using the ‘OutdoorAir’ option, the current outdoor dry-bulb temperature and wind velocity from the weather file (or design day input) are used. When the environment is specified as ‘Zone’, the mean air temperature and room air velocity of the corresponding zone are used.
-
-In the case of a pipe in a zone, the heat loss or gain is accounted for in the pipe heat transfer calculation and is also included in the zone air heat balance calculations. When the environment is specified as ‘Schedule’, the user specifies a temperature and velocity schedule which will be used to calculate the heat transfer.
-
-Pipe heat transfer in EnergyPlus is simulated by discretizing the pipe length into a number of nodes (20) and is an implementation of the model by Hanby et al. (2002). A control volume drawn around a node in the pipe is shown in Figure 261. Three nodes are defined at each discrete section of the pipe and represent the fluid, pipe wall and external environment. The fluid and pipe have defined thermal capacitance (mass). The insulation around the pipe is currently modeled as steady-state (no thermal mass), and so the effect of this resistance is accounted for within the h<sub>f</sub> term in the following description.  For the fluid, there is one-dimensional flow from each upstream node.
-
-![PipeDelay](media/image5831.png)
-
-Figure 261. Control Volume drawn around node *i*
-
-The model is formulated from the heat balances on the fluid and wall nodes.
-
-<div>$${M_{f,i}}{C_{P,f}}\frac{{d{T_{f,i}}}}{{dt}} = \dot m{C_{P,f}}\left( {{T_{f,i - 1}} - {T_{f,i}}} \right) - {h_f}{A_i}\left( {{T_{f,i}} - {T_{w,i}}} \right)$$</div>
-
-<div>$${M_{w,i}}{C_{P,w}}\frac{{d{T_{w,i}}}}{{dt}} = {h_f}{A_i}\left( {{T_{f,i}} - {T_{w,i}}} \right) - {h_e}{A_i}\left( {{T_{w,i}} - {T_e}} \right)$$</div>
-
-Where, subscript *w*, *f* and *e* denote the values for pipe wall, fluid and environment respectively. The current node is represented by a subscript of *i*, while the previous node is represented by *i-1*.
-
-<span>\(M\)</span> = Mass
-
-<span>\({C_p}\)</span> = Specific Heat
-
-<span>\(\dot m\)</span> = Mass flow rate of fluid in pipe
-
-<span>\(T\)</span>  = Temperature
-
-<span>\(A\)</span>  =  Heat Transfer Area
-
-<span>\(h\)</span>  = Film convective resistance
-
-<span>\(t\)</span>   = time
-
-The exterior film convective resistance is calculated based on either wind speed, room air velocity, or a scheduled value based on the type of pipe heat transfer object. However, when the velocity gets too low, natural convection must be modeled. This is handled within the program by having a lower limit on the Nusselt number. For natural convection from a horizontal cylinder, a constant Nusselt number is assumed based on information from Spang (referenced below). This Nusselt number is 0.36. The Nusselt number used in calculating the exterior convection coefficient (Incropera and Dewitt 1996) is the maximum of the Nusselt number from the forced convection coefficient correlation and this natural convection Nusselt number (0.36).
-
-In addition, the exterior resistance from the pipe wall inner surface to the environment will include resistance values for the pipe wall itself and any insulation specified around the pipe. This is treated as steady state value, so the simulation results are not affected by a change in insulation specific heat. However, the resistance is calculated based on thermal conductivity and thickness (using radial coordinate system), so the simulation results will vary with material conductivity changes. Again, this resistance is added in series with the exterior surface film convective resistance such that h<sub>f</sub> contains film and insulation resistance.
-
-Approximating the derivatives using backward differencing enables these equations to be represented as simultaneous algebraic equations. For the fluid, at time step n, the heat balance is:
-
-<div>$$\frac{{{M_{f,i}}{C_{P,f}}}}{{\Delta t}}\left( {T_{f,i}^n - T_{f,i}^{n - 1}} \right) = \dot m{C_{P,f}}\left( {T_{f,i - 1}^n - T_{f,i}^n} \right) - {h_f}{A_i}\left( {T_{f,i}^n - T_{w,i}^n} \right)$$</div>
-
-Rearranging gives,
-
-<div>$$T_{f,i}^n\left[ {{M_{f,i}}{C_{P,f}} + \dot m{C_{P,f}}\Delta t + {h_f}{A_i}\Delta t} \right] = \dot m{C_{P,f}}\Delta tT_{f,i - 1}^n + {h_f}{A_i}\Delta tT_{w,i}^n + {M_{f,i}}{C_{P,f}}T_{f,i}^{n - 1}$$</div>
-
-or,
-
-<div>$${a_1}T_{f,i}^n = {a_2}T_{f,i - 1}^n + {a_3}T_{w,i}^n + {a_4}T_{f,i}^{n - 1}$$</div>
-
-where,
-
-<div>$$\begin{array}{l}{a_1} = {M_{f,i}}{C_{P,f}} + \dot m{C_{P,f}}\Delta t + {h_f}{A_i}\Delta t\\ {a_2} = \dot m{C_{P,f}}\Delta t\\ {a_3} = {h_f}{A_i}\Delta t\\ {a_4} = {M_{f,i}}{C_{P,f}}\end{array}$$</div>
-
-Similarly, taking backwards differences for the conduit wall at time step n, the heat balance becomes,
-
-<div>$$\frac{{{M_{w,i}}{C_{P,w}}}}{{\Delta t}}\left( {T_{w,i}^n - T_{w,i}^{n - 1}} \right) = {h_f}{A_i}\left( {T_{f,i}^n - T_{w,i}^n} \right) - {h_e}{A_i}\left( {T_{w,i}^n - T_e^n} \right)$$</div>
-
-Rearranging gives,
-
-<div>$$T_{w,i}^n\left[ {{M_{w,i}}{C_{P,w}} + {h_f}{A_i}\Delta t + {h_e}{A_i}\Delta t} \right] = {h_f}{A_i}\Delta tT_{f,i}^n + {h_e}{A_i}\Delta tT_e^n + {M_{w,i}}{C_{P,w}}T_{w,i}^{n - 1}$$</div>
-
-or,
-
-<div>$${b_1}T_{w,i}^n = {b_2}T_{f,i}^n + {b_3}T_{e,i}^n + {b_4}T_{w,i}^{n - 1}$$</div>
-
-where,
-
-<div>$$\begin{array}{l}{b_1} = {M_{w,i}}{C_{P,w}} + {h_f}{A_i}\Delta t + {h_e}{A_i}\Delta t\\ {b_2} = {h_f}{A_i}\Delta t\\ {b_3} = {h_e}{A_o}\Delta t\\ {b_4} = {M_{w,i}}{C_{P,w}}\end{array}$$</div>
-
-Substituting into gives an equation for the current fluid temperature:
-
-<div>$${a_1}T_{f,i}^n = {a_2}T_{f,i - 1}^n + {a_3}\left( {{b_2}T_{f,i}^n + {b_3}T_{e,i}^n + {b_4}T_{w,i}^{n - 1}} \right)/{b_1} + {a_4}T_{f,i}^{n - 1}$$</div>
-
-<div>$$T_{f,i}^n = \frac{1}{{\left( {{a_1} - {a_3}{b_2}/{b_1}} \right)}}\left[ {{a_2}T_{f,i - 1}^n + {a_3}\left( {{b_3}T_{e,i}^n + {b_4}T_{w,i}^{n - 1}} \right)/{b_1} + {a_4}T_{f,i}^{n - 1}} \right]$$</div>
-
-The conduit is simulated by solving Eq. followed by Eq. for each of the twenty cells in the model and incrementing the time step. The fluid temperature of the last node is taken to be the pipe outlet temperature.
-
-#### References
-
-Hanby, V.I., Wright, J.A., Fletcher, D.W and Jones, D.N.T. 2002. Modeling the Dynamic Response of Conduits. International Journal of HVACR&R, Vol.8, No.1. pp. 1-12.
-
-Incropera, F.P. and Dewitt, D.P. 1996. Fundamentals of Heat Transfer, 4th Edition, pp. 369-370.
-
-Spang, Bernhard. Correlations for Convective Heat Transfer. Chemical Engineers’ Resource Page:
-
-### Underground Pipe (Object: Pipe:Underground)
-
-#### Description of Model
-
-The buried pipe model in EnergyPlus is similar to the other pipe heat transfer objects (i.e., Pipe:Indoor and Pipe:Outdoor) except for the way in which the pipe boundary condition is developed. For a buried pipe the ground between the pipe and the surface must be modeled. For a shallow buried pipe, the GroundHeatExchanger:Surface object may be used, which uses modified conduction transfer functions to model the ground. However, beyond a certain thickness, the transfer function method fails, and EnergyPlus will respond with a fatal error due to convergence problems. Therefore, when a pipe is buried deeper than about one meter, this new buried pipe model should be used. When the pipe is buried shallower than one meter, either model may be used. Due to the finite difference nature of the Pipe:Underground model, the GroundHeatExchanger:Surface may be slightly faster and therefore more desirable.
-
-The buried model develops a grid around the pipe. The grid was based originally on a model by Piechowski (1999), and still carries the model nomenclature. The grid extends from the ground surface down to a calculated distance below the pipe. The domain extends sideways from the symmetric center of the pipe to a calculated distance from the pipe. The grid stretches along the full length of the pipe. At each cross section, transient 2D Cartesian finite difference equations are used, updating each node except the node centered on the pipe. Axial heat transfer is not modeled in the soil. The large view of the outer Cartesian grid system is shown in Figure 262.
-
-![](media/image5851.png)
-
-Figure 262. Pipe:Underground Outer Finite Difference Grid
-
-When the model encounters the pipe node, the existing model for Pipe:Interior and Pipe:Exterior pipes is used. The finite difference temperatures neighboring the pipe, grid spacing and soil properties are used to create an average boundary temperature for the pipe along with a conductance value. With a boundary temperature available and a conductance value mimicking the convection coefficient, the simulation continues exactly as with the other pipe heat transfer objects. To avoid redundancy, see the Pipe:Indoor or Pipe:Outdoor objects for a detailed description of the pipe model.
-
-#### Boundary Conditions
-
-The boundary conditions for this model include a symmetric vertical boundary centered on the pipe, the ground surface, a ‘far-field’, and a ‘deep ground’. The ground surface boundary uses current simulation outdoor dry-bulb temperature, and the user-entered convection coefficient. The ‘far-field’ and ‘deep ground’ temperatures come from the "undisturbed" ground temperature object specified in the input. 
-
-Currently, the model is set up to be exposed to open soil above the pipe. If the user intends on simulating this buried pipe under a foundation slab, the effects can be approximating by use of the basement/slab heat transfer preprocessor program. This program takes in general building information, and performs a simulation which generates ground temperatures. Typically these effects are used to generate boundary conditions for the floor zone, but they may also be used in generating the ground surface temperatures for this pipe model. The data from the slab program will be monthly temperatures, so the user can use these as a surface ground temperature object which provides boundary data to the Pipe:Underground model.
-
-#### Geometry
-
-The model develops the pipe depth and ground thickness from the user-entered construction information. The soil, pipe wall, and optional pipe insulation are entered as materials (with inherent thicknesses). The soil is entered as a standalone material, while the pipe insulation (if applicable) and the pipe wall should be given as a construction containing one or two materials. With knowledge of each individual thickness, the pipe geometry is obtained. The pipe length and inside diameter are the only additional geometry inputs.
-
-#### Model Assumptions
-
-* Constant properties throughout domain
-
-* Moisture is not directly involved with the model operation, so careful selection of soil thermal conductivity is a priority
-
-* Negligible axial heat transfer compared to radial heat transfer
-
-* Axisymmetric heat transfer in near pipe region
-
-* Surface convection coefficient is constant throughout simulation (does not vary with wind speed)
-
-#### References
-
-Kusuda, T. & Achenbach, P. 1965. ‘Earth Temperature and Thermal Diffusivity at Selected Stations in the United States’, ASHRAE Transactions Vol. 71, Part 1, pp. 61–75.
-
-Piechowski, M. 1999. ‘Heat and Mass Transfer Model of a Ground Heat Exchanger: Theoretical Development’, Energy Research 23 (7), pp. 571–588.
-
-### PipingSystem:Underground Simulation
-
-In order to simulate diverse underground piping systems, a generalized model has been implemented which allows placement of pipes in a solid medium (soil).  The model simulates circuiting effects of multiple pipes by allowing fluid to flow in the pipes in different directions.  The model also has the capability of simulating interaction with zone surfaces to account for things such as basement heat transfer in a foundation heat exchanger.  Different aspects of the modelling approach are described in this section which can assist the user in determining if this model is appropriate for a particular application, and determining input parameter values.
-
-An alternative interface is implemented which provides a simpler set of inputs for simulating horizontal trench heat exchangers.  The key limitations of the simpler inputs include all piping in the domain being on a single circuit, all trenches equidistance apart, and each trench with the same burial depth.  If this is satisfactory for an application, the GroundHeatExchanger:HorizontalTrench object is a suitable object.  The object uses the same underlying simulation algorithms and data structures as the detailed piping system model, but with a simpler set of input parameters.  For other cases and more detailed studies, the PipingSystem:Underground:\* objects provide full flexibility.
-
-A dual-coordinate system finite volume heat transfer model of pipes buried in a conducting medium is employed.  The dual-coordinate system consists of a coarse Cartesian system in the conducting region (the soil, for example) with a refined radial system in the near-pipe region.  The pipes are connected as objects on the plant loop and are simulated as needed during loop convergence, while the ground itself is only simulated once per system time step.
-
-#### Approach:
-
-#### General Development and Solution Scheme
-
-A new heat transfer model is implemented to handle a diverse set of buried pipe conditions.  The model uses a dual-coordinate system approach to solve a finite volume domain in a computationally efficient manner.  The main idea behind the dual coordinate system technique is to focus the computational effort to the region where it is most needed: near the pipe(s).  To this end, a coarse grid Cartesian coordinate system is used to solve the slow-moving ground heat transfer.  Then, within one of these cells, a radial coordinate system is configured around the pipe/insulation with a specialized interface cell between the systems.  Figure 263 shows an example of cells surrounding a pipe, including the radial region in the near-pipe cell, while Figure 264 shows a zoomed-in view of the near-pipe cell itself.
-
-![](media/image5852.png)
-
-Figure 263. Radial "near-pipe" cell within a Cartesian cell
-
-![](media/image5853.png)
-
-Figure 264. Close-up view of example radial cell
-
-The ground heat transfer model can be set up in a fully-3D or quasi-3D manner.  In either case, there is a three-dimensional grid of Cartesian cells placed in the domain.  In fully-3D mode, the axial heat transfer is accounted for; in quasi-3D mode, the axial effects are ignored and the result is essentially a set of 2D slices along the length of the domain.  The determination of which method will be utilized in the final model shall be based upon final testing and on a balance between accuracy vs. computation time.  This option could be left to the end-user, but this will likely be unnecessary input overhead.
-
-A fully implicit (and thus numerically stable) formulation is used to describe all cells, which means an iteration loop must be implemented.  In this solver, an outer iteration loop is used to bring the entire domain to convergence, while an inner iteration loop is used over all the radial cells.  This is intended to focus the computational effort even further.  The outer region may converge within one or two iterations, while the “near-pipe� cells may take much more iteration.  For this reason, it does not make sense to iterate over the entire domain a large number of times.
-
-#### Boundary Conditions
-
-The farfield boundary condition is defined by a Kusuda and Achenbach (1965) correlation, which requires annual ground surface temperature data.  As with the current Pipe:Underground model, the user will be able to enter the correlation parameters directly, or information from the monthly ground temperature input object will be used to infer the parameters.
-
-The ground surface boundary condition is defined by an energy balance between the surrounding interior cells and the ground surface, including convection and radiation.  As with the Pipe:Underground object, the ground surface sun exposure may be an optional input to allow for a shaded ground surface.  In addition to the standard conduction, convection, and both short- and long-wave solar radiation at the surface, the ground surface boundary condition also includes the effects of evapotranspiration in the surface vegetation—the heat loss due to evaporation from soil to plant surface, and transpiration internal to the plant itself.  The evapotranspiration rate is calculated as a moisture loss by using the Walter et al. (2005) model, and translated into a heat loss by multiplication with the density and latent heat of evaporation of water.  The evapotranspiration rate is dependent on the type of vegetation at the surface; the user can vary the surface vegetation from anywhere between a concrete surface and a fairly tall grass (about 7�).
-
-Based on the application, an adiabatic boundary condition will also be implemented and employed on particular surfaces of the domain.  For the case where a basement or under-slab region is present, for example, an adiabatic boundary will represent the vertical line of symmetry.
-
-#### “Pipe Cell� Simulation
-
-The ground is discretized into coarse Cartesian cells, some of which will contain a pipe.  These “pipe-cells� are further discretized into a radial system with a specialized interface cell to couple these systems.  The radial cells consist of a number of ground cells, with an optional insulation cell, then the pipe cell, followed by the fluid itself.
-
-The fluid is modeled as a cylindrical cell interacting with incoming fluid and heat transfer to the pipe.  When there is no flow in the system, the cell essentially becomes radially adiabatic so that the fluid temperature will float during off periods.  It will not be equal to ground temperatures, unless it is off for a long time and the transient heat is allowed to dissipate.  When there is flow in the system, the incoming fluid and heat transfer from the pipe wall balance with the mass of the cell to come up with a new fluid temperature for that cell, to be passed downstream to the next cell.
-
-The fluid within the cells is modeled directionally, so that the flow can be circuited through multiple pipe segments in different directions.  The flow direction in each pipe is specified by a choice field input.
-
-#### Basement Interaction
-
-The model can also interact with basement surfaces.  The interaction is split into two sections: floor surfaces and wall surfaces.  For each of these, the analysis is lumped, i.e., all walls are treated as one average wall surface and all floors are treated as one average floor surface.  The distance that the basement impinges within the domain is defined by a simple width and height specification.  The domain is then *cutaway* for that region.  Note that these distances then refer to the exterior surface of the wall or floor.
-
-The ground heat transfer model does not perform any transient simulation of the basement surfaces.  The transient condition through these surfaces are left to the appropriate surface heat balance algorithms.  Instead, this model interacts directly at the outer boundary through the use of an *OtherSideConditions* model.  The ground heat transfer model will take the current exterior surface heat flux and use that as the boundary for neighboring cells.  Once convergence is achieved, the ground model will then effectively apply a constant surface temperature boundary condition by using a very high value of convection coefficient.  The surface heat balance algorithms will then pick this up during the next zone time step.
-
-#### Mesh Development
-
-The mesh is developed by using a few simple parameters.  There are two distinct categories, the large-scale Cartesian mesh and the near-pipe refined radial mesh.
-
-* X, Y, Z mesh
-
-* Mesh Layout
-
-* Cell density
-
-* Radial mesh
-
-* Radial mesh thickness
-
-* Cell count
-
-The Cartesian mesh uses a cell density parameter to define the number of cells to use in the simulation.  Instead of requiring a detailed specification of all cell regions in the domain, this one parameter is used to specify a mesh density and is applied to all domain regions.  The cell density parameter represents the number of cells within any two domain partitions.  A domain partition is a basement wall or a pipe placed in the domain.  Once these partitions are all laid out and validated, the regions between them are populated with the number of cells specified in the cell density parameter.  Although this may lead to a variation of cell size within the domain, it is assumed that this will help focus computational intensity in the domain.  Of course, the number of cells (cell density parameter) can be different for each of the X, Y, and Z directions to allow for further fine tuning of the domain.
-
-The Cartesian mesh is laid out in either a uniform or symmetric-geometric fashion.  In the former, the cells between any two domain partitions are equally sized.  In the latter, the cells are smaller near the partitions to again help fine-tuning computational intensity.  If the latter is selected, the amount of non-uniformity is specified by an additional parameter.
-
-The radial coordinate system is always uniform for the soil cells, The two parameters to be specified for this region are the cell count (the number of soil cells to be generated outside of the pipe cell), and the radial mesh thickness (the radial distance from pipe outer wall to the cell boundary).  Each soil cell will then have a radial thickness equal to the radial mesh thickness divided by the cell count.
-
-#### Simulation Methodology
-
-The actual simulation of this model is performed in two parts: the ground simulation and the pipe cell simulation.
-
-Since the ground is likely to be slow-moving and easily converging, it is simulated once per system time step.  This will simulate all the cells in the domain which do not contain a pipe segment.  The boundary conditions for this step are then the current surface conditions and farfield model along with the previous values for pipe cell temperature.  This small lag should provide suitable accuracy as the system time step will usually be smaller than the time constant of the pipe cell.  This decoupling leverages the core of the model development by again placing computational effort where it is needed most, near the pipes.
-
-The ground simulation is performed once per time step, but the pipe cell simulation is performed at each call to the component.  Each pipe will be placed on a plant loop, but not necessarily on the same plant loop or loop side.  Thus, at each call to the object, that pipe will use the temperatures of the ground cells near the pipe as boundary conditions to simulate the “near-pipe� radial cells and fluid cell.  In this manner, the pipes will simulate numerous times following the convergence flow of the plant loop system.
-
-#### References
-
-Kusuda, T. & Achenbach, P. 1965. ‘Earth Temperature and Thermal Diffusivity at Selected Stations in the United States’, ASHRAE Transactions Vol. 71, Part 1, pp. 61–75.
-
-Allen, R.G., Walter, I.A., Elliott, R.L., Howell, T.A., Itenfisu, D., Jensen, M.E., Snyder, R.L. 2005. The ASCE standardized reference evapotranspiration equation. Reston, VA:American Society of Civil Engineers. 59 p.
-
-
-
-Pumps <a name="Pumps"></a>
------
-
-The water pump is quite simply the component that drives the flow in plant and condenser loops. How it reacts depends on several different conditions. In total, there are three different decision variables, two of which are defined by user input. These three deciding factors are whether the pump is constant or variable speed, whether the pump operation is continuous or intermittent, and whether or not there is a load on the loop. The pump is simulated first on the supply side loop after the demand side loop has determined what the demand on the loop will be. For further reference look at sections Pump Control for Plant and Condenser Loops, Plant/Condenser Supply Side, and Plant/Condenser Demand Side in the Plant Flow Resolver of this document.
-
-### Summary of Pump Rules
-
-* Pumps in Plant Loop can be on the supply side or demand side
-
-* A Pump, if present, in the demand side of plant loop must be the first component of the inlet branch.
-
-* Pumps in Condenser loop must be on supply side
-
-* Pumps can operate as constant or variable flow.
-
-* Pumps can run continuously or intermittently.
-
-* Single boiler/chiller with NO bypass, use Pump:ConstantSpeed
-
-* Boiler/chiller should be constant flow
-
-* Pump should be intermittent
-
-* Single boiler/chiller with NO bypass, Pump:VariableSpeed
-
-* Boiler/chiller should be variable flow, regardless of whether pump is intermittent or continuous (runs at the minimum if demand is less than minimum, this includes zero.)
-
-* Single boiler/chiller with bypass, Pump:ConstantSpeed
-
-* Boiler/chiller can be constant or variable flow
-
-* Pump may be intermittent or continuous as long as the bypass can handle the entire pump volume when the boiler is not operating
-
-Multiple branches add more complexity, but it is nothing more than continuity. If the pump is putting out flow then it has to have a branch to flow down whether it is a chiller or a bypass. It can be safer to add the bypass for a simulation. If the active machines require the flow the bypass will be dry. If performing a pressure simulation, and the flow goes through a machine which is off, the pressure drop will be accounted for, but no heat transfer through the machine will be calculated.
-
-If the user designates a pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop. If the pump is scheduled, the schedule modifies the Rated Volumetric Flow Rate of the pump on a time basis. The default is that the pump is ON and runs according to its other operational requirements.
-
-Shown below is the calculation of the total efficiency of the pump and the actual pumping efficiency when the motor efficiency is accounted for either the variable or constant volume pumps.
-
-!  Total\_Efficiency % = Rated\_Volume\_Flow\_Rate \* Rated\_Pump\_Head / Rated\_Power\_Use
-
- TotalEffic =   PumpEquip(PumpNum)%NomVolFlowRate \*
-
-                   PumpEquip(PumpNum)%NomPumpHead /
-
-                     PumpEquip(PumpNum)%NomPowerUse
-
-
-
-!     Calculated Pump\_Efficiency % =Total\_Efficiency % / Motor\_Efficiency %
-
-      PumpEquip(PumpNum)%PumpEffic =  TotalEffic /
-
-                   PumpEquip(PumpNum)%MotorEffic
-
-### Dynamic Pump Pressure Head
-
-There is an option when performing plant/condenser loop simulations to account for dynamically changing loop pressure drop. For the current implementation, the loop pressure drop is calculated based on pressure drop data on each branch of the loop, then this total pressure drop is set as the pump pressure head. There is no pump curve implemented yet, so it is assumed that the pump can always handle this pressure value. This is a first approximation to actually having the pump ride a curve, and this initial implementation allows the user to enter minimal data, and yet get a more dynamic output for pump power, which is calculated based on current pressure drop and flow rate. The equation for pump power is now:
-
-<div>$$Pump\;Electric\;Power = Pump\;Volume\;Flow\;Rate*\frac{{Pump\;Head}}{{Total\;Efficiency}}$$</div>
-
-Without the pressure simulation, the pump power is based on the rated value entered with the pump object. For further information, see the input-output reference for Branch objects, and PlantLoop/CondenserLoop objects; as well as the Plant/Condenser loop section of this engineering reference.
-
-### Variable Speed Pump
-
-A variable speed pump (object name: Pump:VariableSpeed) is defined with maximum and minimum flow rates that are the physical limits of the device. The pump will operate and select a flow somewhere between the minimum and maximum limits. In the case where the pump is running, the pump will try to meet the flow request made by demand side components.
-
-All of the pump rules and efficiency and power calculations are applicable from the introduction in the pump group section. The main difference between the the variable volume pump and the constant volume pump is the Part Load Performance Curve.The fraction of full load power is determined by the cubic equation:
-
-<div>$$FractionFullLoadPower = {C_1} + {C_2}PLR + {C_3}PL{R^2} + {C_4}PL{R^3}$$</div>
-
-where C<sub>1</sub>,C<sub>2</sub>,C<sub>3</sub>,and C<sub>4</sub> are Coefficients 1 – 4 and PLR is the Part Load Ratio. In the pseudo code below the FracFullLoadPower modifies the NomPowerUse for the total pump “Power� and shows the “ShaftPower� and the “PumpHeattoFluid�.
-
-VolFlowRate = PumpMassFlowRate / LoopDensity
-
-
-
-  PartLoadRatio = VolFlowRate / PumpEquip(PumpNum)%NomVolFlowRate
-
-
-
-  FracFullLoadPower =   PumpEquip(PumpNum)%PartLoadCoef(1)                     &
-
-                      + PumpEquip(PumpNum)%PartLoadCoef(2) \* PartLoadRatio     &
-
-                      + PumpEquip(PumpNum)%PartLoadCoef(3) \* PartLoadRatio\*\*2  &
-
-                      + PumpEquip(PumpNum)%PartLoadCoef(4) \* PartLoadRatio\*\*3
-
-
-
-  Power = FracFullLoadPower \* PumpEquip(PumpNum)%NomPowerUse
-
-
-
-  ShaftPower = Power \* PumpEquip(PumpNum)%MotorEffic
-
-
-
-! This adds the pump heat based on User input for the pump
-
-! We assume that all of the heat ends up in the fluid eventually since this is a closed loop
-
-!  PumpHeattoFluid = ShaftPower\*(1-PumpEquip(PumpNum)%PumpEffic)  &
-
-
-
-  PumpHeattoFluid = ShaftPower + (Power - ShaftPower)\*PumpEquip(PumpNum)%FracMotorLossToFluid
-
-
-
-  Node(OutletNode)%Temp = Node(InletNode)%Temp+PumpHeattoFluid/(PumpMassFlowRate \* LoopCp)
-
-
-
-  PumpEquip(PumpNum)%Power = Power
-
-### Pressure-based Flow for Variable Speed Pumps
-
-With the introduction of pressure simulations in plant loops, the variable speed pump object now has the capability to model a more realistic variable speed operation. There are two operation modes which are introduced: differential pressure control is a widely used VFD control method while most VFDs also have a manual control mode in which the user determines the input frequency of the electric motor. The mode can be selected as ‘ManualControl’ or ‘PressureSetpointControl’ in the VFD Control Type input in Pump:VariableSpeed objects.
-
-In manual VFD control mode the specified schedule will determine the current pump rotational speed throughout the simulation. This RPM value will be used to scale the pump curve which is entered by the user in non-dimensional form. Once the pump curve has been fixed then the successive substitution method will use this curve with the system curve to resolve the operating point. VFD manual control mode is implemented in EnergyPlus with the use of the RPM schedule input.
-
-Differential pressure based control will maintain the differential pressure within the specified range. The pressure drop corresponding to the mass flow request will be calculated using the effective pressure constant of the system. This pressure drop will be checked against the pressure set point range. If the pressure drop is within the user specified range, then the mass flow rate will be checked against mass flow rates of operating points corresponding to maximum and minimum rotational speeds. Maximum and minimum differential pressure and rotational speeds are schedule inputs and can be entered as constant schedule.
-
-The allowable mass flow rate range for the Differential pressure control is explained in the figure below:
-
-![](media/image5856.png)
-
-Figure 265. Allowable mass flow rate range for the Differential pressure control
-
-### Constant Speed Pump
-
-The operation of a constant speed pump (object name: Pump:ConstantSpeed) is fairly straightforward. The user designates a maximum flow rate and when this pumpo operates it will run at that capacity. The main difference between the constant speed pump and the variable speed pump is that the fraction of full load power is always = 1. In the pseudo code below the FracFullLoadPower is = 1.0, therefore the Power is always the full power.
-
-VolFlowRate = PumpMassFlowRate / LoopDensity
-
-
-
-  PartLoadRatio = VolFlowRate / PumpEquip(PumpNum)%NomVolFlowRate
-
-
-
-  FracFullLoadPower = 1.0
-
-
-
-  Power = FracFullLoadPower \* PumpEquip(PumpNum)%NomPowerUse
-
-
-
-  ShaftPower = Power \* PumpEquip(PumpNum)%MotorEffic
-
-
-
-! This adds the pump heat based on User input for the pump
-
-! We assume that all of the heat ends up in the fluid eventually since this is a closed loop
-
-!  PumpHeattoFluid = ShaftPower\*(1-PumpEquip(PumpNum)%PumpEffic)  &
-
-
-
-  PumpHeattoFluid = ShaftPower + (Power - ShaftPower)\*PumpEquip(PumpNum)%FracMotorLossToFluid
-
-
-
-  Node(OutletNode)%Temp = Node(InletNode)%Temp+PumpHeattoFluid/(PumpMassFlowRate \* LoopCp)
-
-
-
-  PumpEquip(PumpNum)%Power = Power
-
-### Pressure-based Flow for Constant Speed Pumps
-
-The constant speed pump can flow can also be overridden dynamically based on a response to the plant loop pressure drop. In “single-loop-pump� simulations (no branch pumps, no common pipe), the user can enter a dimensionless pump curve on the Pump:ConstantSpeed (see I/O ref) object which represents the single speed pressure-flow relationship of the pump. In the process of determining the operating flow rate for the pump, the pump will check to see if a valid pressure simulation is being performed. If it is, a flow will be prescribed based on a resolution between system pressure characteristics and the pump pressure curve. This will cause the pump flow to be “unpredictable,� meaning that it will not always be a constant, expected value, which is basically what the constant speed pump gives you without the pressure simulation. There is more detail on the pressure based simulation in the Plant/Condenser loop sections of this documentation.
-
-### Pump Heat Addition to the Loop
-
-Due to the fact that a pump is a mechanical device that acts on the fluid it is circulating, it causes the fluid to increase in temperature. The EnergyPlus model assumes that all pressure increase caused by the pump will eventually be lost due to friction, and that friction will be added as heat to the fluid. Since the plant and condenser loops are not yet true pressure-based models, EnergyPlus assumes that all of the heat resulting from the pump itself and from friction throughout the loop. Therefore, as of version 7, the pump heat is added to the plant loop interface by injecting the heat into the mixed tanks used to model loop thermal capacitance(previously it was added at the outlet node of the pump). The amount of heat added to the fluid is calculated using the following two equations:
-
-<div>$$ShaftPower = PumpPower * PumpMotorEfficiency$$</div>
-
-<div>$$PumpHeatToFluid = ShaftPower + \left( {PumpPower - ShaftPower} \right) * FracMotorLossToFluid$$</div>
-
-where the pump motor efficiency is defined by the user input and the FracMotorLossToFluid is the amount of heat generated by the pump motor that is added to the fluid loop (as opposed to being lost to the environment where the pump is located). FracMotorLossToFluid is also a user input.
-
-Note that the shaft power relates to the increase in head through the pump. Since all of this head is lost through the piping network due to frictional heat, this represents a heat gain by the fluid throughout the network. For simplicity, this heat is added along with the heat resulting from the pump motor. The difference between the pump power and the shaft power is the inefficiency of the pump—or the amount of energy input into the pump that the motor converts to heat rather than mechanical energy. Some of this heat is added to the fluid being pumped. These two terms are shown in the PumpHeatToFluid equation shown above. As of version 7, this heat is added to the loop capacitance tank(s) rather than at the pump’s outlet and so the outlet temperatue is equal to the inlet temperaure.
-
-### Pump Heat Addition to Surrounding Zone
-
-If the user input includes naming a Zone that surrounds the pump, then the pump becomes a source of internal heat gain to that zone.  The amount of heat transmitted to the surrounding zone is simply the difference between power input and the rate of heat transferred to the fluid. The user can also input a fraction,<span>\({f_{rad}}\)</span> , that controls the overall split between thermal radiation and sensible convection.  The pump’s sensible zone gains are determined using the following equations:
-
-<div>$$TotalZoneGain = PumpPower - PumpHeatToFluid$$</div>
-
-<div>$$ConvectiveZoneGain = \left( {1 - {f_{rad}}} \right)*TotalZoneGain$$</div>
-
-<div>$$RadiativeZoneGain = {f_{rad}}*TotalZoneGain$$</div>
-
-### Headered Pumps
-
-The input objects HeaderedPumps:ConstantSpeed and HeaderedPumps:VariableSpeed  provide models for headered pumps that consist of two or more pumps connected in parallel. The headered pump is simulated as a single component, and it is specified as an integer number of a specific pump. The flow rate provided by the headered pump is determined by the number of pumps in operation and the flow rate of the individual pump. The total flow rate is calculated as
-
-<div>$$FlowProvided = NumPumpsON*IndividualPumpFlowRate$$</div>
-
-The simulation starts by turning ON all pumps in the group. The pumps are then turned OFF one at a time until the flow provided is less than the flow requested. Finally the last pump is turned back ON to meet the remaining flow (FlowDifference) requested. The flow rate of the last pump depends on the pump bank type. For constant speed headered pumps, the last pump runs at the nominal flow rate, thereby giving a final headered pump flow which is equal to or greater than the flow requested. In a variable speed headered pump the last pump runs at part load so that the flow provided matches the flow requested. The power of the headered pump is then calculated as
-
-<div>$$Power = (P{R_{FL}}{\rm{*N}}{}_{{\rm{FL}}} + {\rm{P}}{{\rm{R}}_{{\rm{PL}}}}{\rm{*}}{{\rm{N}}_{{\rm{PL}}}}{\rm{)*}}{{\rm{P}}_{{\rm{Nom}}}}{\rm{  }}$$</div>
-
-Where;
-
-*Power* = Power consumed by the pump bank
-
-*PR<sub>FL</sub>* = Power ratio at full load (Generally equal to 1)
-
-*N<sub>FL</sub>* = Number of pumps running at full load
-
-*PR<sub>PL</sub>* = Power ratio at part load
-
-*N<sub>PL</sub>* = Number of pumps running at part load
-
-*P<sub>Nom</sub>* = Nominal power consumption of individual pumps
-
-For a constant speed headered pump *N<sub>PL</sub>* is zero. For a variable speed headered pump *N<sub>PL</sub>* is equal to one.
-
-### Condensate Pumps
-
-The input object Pump:VariableSpeed:Condensate provides a model for steam condensate pumps, see the discussion for steam loops, reference: Condensate Pump.
-
-Ideal Loads Air System <a name="IdealLoads"></a>
-----------------------
-
-### Overview
-
-The input object ZoneHVAC:IdealLoadsAirSystem provides a model for an ideal HVAC system. It occupies a place in the program hierarchy corresponding to a zone HVAC unit. It is not connected to a central air system – instead each ZoneHVAC:IdealLoadsAirSystem object supplies cooling or heating air to a zone in sufficient quantity to meet the zone load or up to its limits, if specified. The supply air conditions are controlled based on specifications in the ZoneHVAC:IdealLoadsAirSystem input. The system has options for humidity control, outdoor air, economizer, demand controlled ventilation, and heat recovery.
-
-### Model
-
-The ZoneHVAC:IdealLoadsAirSystem object is modeled as an ideal VAV terminal unit with variable supply temperature and humidity. The supply air flow rate is varied between zero and the maximum in order to satisfy the zone heating or cooling load, zone humidity controls, outdoor air requirements, and other constraints, if specified.
-
-#### Inputs and Data
-
-The user specifies some or all of the following data for each ZoneHVAC:IdealLoadsAirSystem object:
-
-·        name of unit availability schedule
-
-·        name of the zone inlet node;
-
-·        name of the zone exhaust node;
-
-·        maximum supply air temperature when in heating mode *T<sub>max,heating</sub>* [C];
-
-·        minimum supply air temperature when in cooling mode *T<sub>min,cooling</sub>* [C];
-
-·        maximum supply air humidity ratio when in heating mode *W<sub>max,humid</sub>* [kg water/kg dry air];
-
-·        minimum supply air humidity ratio when in cooling mode *W<sub>min,dehum</sub>* [kg water/kg dry air];
-
-·        heating limit type flag (*LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity* or *NoLimit*) *HeatingLimit*;
-
-·        maximum heating air flow rate  [m<sup>3</sup>/s]
-
-·        maximum sensible heating capacity  [W]
-
-·        cooling limit type flag (*LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity* or *NoLimit*) *CoolingLimit*
-
-·        maximum cooling air flow rate  [m<sup>3</sup>/s]
-
-·        maximum total cooling capacity  [W]
-
-·        name of heating availability schedule
-
-·        name of cooling availability schedule
-
-·        dehumidification control type flag (*ConstantSensibleHeatRatio, Humidistat, None,* or *ConstantSupplyHumidityRatio*) *DehumidCtrlType*
-
-·        cooling sensible heat ratio
-
-·        humidification control type flag (*Humidistat, None,* or *ConstantSupplyHumidityRatio*) *HumidCtrlType*
-
-·        name of a DesignSpecification:OutdoorAir object
-
-·        outdoor air inlet node name
-
-·        demand controlled ventilation control type flag (*None, OccupancySchedule or CO2Setpoint*)
-
-·        outdoor air economizer type flag (*NoEconomizer, DifferentialDryBulb, or DifferentialEnthalpy*)
-
-·        heat recovery type flag (*None, Sensible, or Enthalpy*)
-
-·        sensible heat recovery effectiveness
-
-·        latent heat recovery effectiveness
-
-#### All input data for the ZoneHVAC:IdealLoadsAirSystem is stored in the array PurchAir. The model and data are encapsulated in the module PurchasedAirManager.Calculation
-
-·        Set the unit on/off flag *UnitOn*.
-
-The unit is off (*UnitOn* = *False*) if the unit availability schedule value is &lt;=0; otherwise the unit is on (*UnitOn* = *True*). If the unit is on, the calculation proceeds through the remaining steps. If the unit is off, the zone inlet node conditions are set to the zone node condition, the inlet node mass flow rate is set to zero, and the unit outputs are set to zero.
-
-·        Calculate the minimum outdoor air mass flow rate based on the specifications in the DesignSpecification:OutdoorAir object, if specified.
-
-·        Calculate the sensible and latent impact of the outdoor air flow relative to the zone conditions
-
-·        Determine if the unit needs to heat or cool
-
-o   If outdoor air sensible impact is &gt;= load to zone cooling setpoint and the current thermostat type is not SingleHeatingSetPoint, then unit is in cooling mode
-
-o   If outdoor air sensible impact is &lt; load to zone heating setpoint then unit is in heating mode
-
-o   Else if neither condition is true, then unit is in deadband mode (provides outdoor air but shuts off economizer and heat recovery and all humidity control options except *Humidistat* option)
-
-·        If in cooling mode, simulate outdoor air economizer and adjust outdoor air mass flow rate
-
-·        Calculate supply air mass flow rate
-
-o   If outdoor air flow rate exceeds applicable maximum flow rate (heating or cooling) then reduce outdoor air mass flow rate, issue warning, and set supply air mass flow rate equal to outdoor air mass flow rate
-
-Else
-
-o   Calculate supply air mass flow rate required to meet zone sensible load at the applicable (heating or cooling) supply temperature limit (*T<sub>max,heating</sub>* or *T<sub>min,cooling</sub>*)
-
-<div>$${\dot m_s} = {\dot Q_z}/({c_{p,air}}\cdot ({T_s} - {T_z}))$$</div>
-
-
-
-o   If *DehumidCtrlType*= Humidistat (and other conditions are met, see below), then calculate the supply air mass flow rate required to meet the humidistat dehumidification setpoint at *W<sub>min,dehum</sub>*
-
-o   If *HumidCtrlType*= Humidistat (and other conditions are met, see below), then calculate the supply air mass flow rate required to meet the humidistat humidification setpoint at *W<sub>max,humid</sub>*
-
-o   Set the supply air mass flow rate to the greatest of these, but limit to the applicable (heating or cooling) maximum flow rate
-
-·        Calculate the mixed air conditions, modeling heat recovery, if applicable
-
-o   The recirculation air conditions are set equal to the zone return air node conditions; if there is no return air node the recirculation air conditions are set equal to the conditions at the zone node.
-
-o   The unit entering conditions are then:
-
-If <span>\({\dot m_s}\)</span>&gt; <span>\({\dot m_{oa}}\)</span> then
-
-<div>$${h_{ma}} = ({\dot m_{oa}} \cdot {h_{oa}} + ({\dot m_s} - {\dot m_{oa}}) \cdot {h_{recirc}})/{\dot m_s}$$</div>
-
-<div>$${W_{ma}} = ({\dot m_{oa}} \cdot {W_{oa}} + ({\dot m_s} - {\dot m_{oa}}) \cdot {W_{recirc}})/{\dot m_s}$$</div>
-
-<div>$${T_{ma}} = {\mathop{\rm PsyHFnTdbW}\nolimits} ({h_{ma}},{W_{ma}})$$</div>
-
-Otherwise the entering air conditions are set equal to the outside air conditions.
-
-·        Calculate the supply air temperature required to meet the zone sensible load at the supply air mass flow rate, but limit to the applicable (heating or cooling) supply temperature limit (*T<sub>max,heating</sub>* or *T<sub>min,cooling</sub>*)
-
-<div>$${T_s} = {T_z} + {\dot Q_z}/({c_{p,air}}\cdot {\dot m_s})$$</div>
-
-·        Calculate the supply humidity ratio based on the specified humidity control types, but limit to the applicable (heating or cooling) supply humidity ratio limit
-
-o   *DehumidCtrlType = None* sets the supply air humidity ratio equal to the mixed air humidity ratio.
-
-o   *DehumidCtrlType = Humidistat,* this will actively dehumidify to the humidistat dehumidification setpoint during cooling and deadband operation, and during heating operation if *HumidCtrlType = Humidistat*
-
-o   *DehumidCtrlType = ConstantSensibleHeatRatio* sets the supply air humidity ratio using the cooling sensible heat ratio.
-
-o   *DehumidCtrlType = ConstantSupplyHumidityRatio* sets the supply air humidity ratio = *W<sub>min,dehum</sub>*.
-
-o   *HumidCtrlType = None* sets the supply air humidity ratio equal to the mixed air humidity ratio.
-
-o   *HumidCtrlType = Humidistat,* this will actively humidify to the humidistat humidifying setpoint during heating and deadband operation, and during cooling operation if *DehumidCtrlType = Humidistat*
-
-o   *HumidCtrlType = ConstantSupplyHumidityRatio* sets the supply air humidity ratio = *W<sub>max,humid</sub>*.
-
-·        Limit supply humidity ratio to saturation at the supply temperature
-
-·        Check the applicable capacity limits (sensible heating and total cooling) and adjust supply air temperature and humidity if needed.
-
-·        Set the zone inlet node conditions to the supply air mass flow rate, temperature, and humidity ratio.
-
-·        Calculate the unit output and load components.
-
-### References
-
-No specific references.
-
-District Cooling <a name="DistrictCooling"></a>
-----------------
-
-When the user is not interested in a plant simulation or there is some centralized source of chilled water, the following model can be used in the input.  This allows the user to achieve a simulation without specifying operating parameters or curve fits for chiller models.  This model only needs the connections to the loop and the nominal capacity to simulate.  See the InputOutput Reference for additional information (Object: DistrictCooling).  This model calculates the output capacity necessary from the inlet temperature to the setpoint temperature for that loop with the given mass flow rate in Watts.
-
-District Heating <a name="DistrictHeating"></a>
-----------------
-
-When the user is not interested in a plant simulation or there is some centralized source of hot water, the following model can be used in the input.  This allows the user to achieve a simulation without specifying operating parameters or curve fits for boiler models.  This model only needs the connections to the loop and the nominal capacity to simulate.  See the InputOutput Reference for additional information (Object: DistrictHeating).  This model calculates the output capacity necessary from the inlet temperature to the setpoint temperature for that loop with the given mass flow rate in Watts.
-
-CentralHeatPumpSystem <a name="CentralHeatPumpSystem"></a>
----------------------
-
-### Overview
-
-The CentralHeatPumpSystem object simulates the performance of a central heat pump system containing one or more chiller-heater objects. The main function of the object is to call relevant calculation methods for the chiller-heater objects depending on their operating modes, and to calculate temperatures at the outlet nodes and the total energy transfer. The object can be connected to plant loops and a source loop (see Input-Output Reference document), and the node connections are solely dependent on individual chiller-heaters’ operating modes. The central system receives water flows from each plant and source loop and then distributes them to individual chiller-heaters as requested. The conditioned water flows leaving the chiller-heaters are then returned to the system, and in turn flow back to the plant loops and source loop to produce heating and cooling, or exchange heat with the source loop.
-
-### Model Description
-
-The model first determines operating modes based on the cooling and heating loads on the system, and then decides which calculation algorithm is called. It calls the cooling calculation subroutine when cooling load is demanded, the heating calculation subroutine when heating load is demanded, and both cooling and heating calculation subroutines when both cooling and heating loads are demanded, i.e., simultaneous cooing-heating mode. It then calculates mass-weighed temperatures and heat transfer energy. Six different operating modes (0 through 5) are possible:
-
-0: off
-
-1: cooling-only mode
-
-2: heating-only mode
-
-3: heat recovery mode
-
-4: cooling dominant simultaneous cooling-heating mode
-
-5: heating dominant simultaneous cooling-heating mode.
-
-The model reads different node information over the operating mode so that outlet water conditions at each node of the system can be appropriately determined.
-
-In cooling-only mode (mode 1), the system is connected to the chilled water loop and source loop. It thus reads the evaporator outlet temperatures and mass flow rates of the chiller-heaters to calculate a mass-weighed chilled water temperature at the system outlet node, and the condenser outlet temperatures and mass flow rates of the chiller-heaters to calculate a mass-weighed source water temperature at the system outlet node. In heating-only mode (mode 2), the system is connected to the hot water loop and source loop. It thus reads the condenser temperatures and mass flow rates of the chiller-heaters to calculate a mass-weighed hot water temperature at the system outlet node, and the evaporator temperatures and mass flow rates of the chiller-heaters to calculate a mass-weighed source temperature at the system outlet node.
-
-In simultaneous cooling-heating mode, three different operating modes (mode 3 through 5) are possible. The model checks which simultaneous cooling-heating mode (3, 4, or 5) each chiller-heater is in, and calculates relevant mass-weighed temperatures. The system may be connected to three loops such as chilled water loop, hot water loop, and source water loop in mode 4 or mode 5.
-
-In heat recovery mode, both evaporator temperatures and condenser temperatures are read and a mass-weighed temperature for both chilled water and hot water is calculated. The chiller-heaters in mode 3 do not exchange heat with source water. At least one of the chiller-heaters within the system is in heat recovery mode during simultaneous cooling-heating mode. The system may be only connected to both chilled water loop and hot water loop if all operating chiller-heaters are in heat recovery mode.
-
-The following nomenclature is used in the following equations:
-
-<span>\({\dot m_{cw,bypass}}\)</span> = chilled water bypass mass flow rate in the system [kg/s]
-
-<span>\({\dot m_{hw,bypass}}\)</span>= hot water bypass mass flow rate in the system [kg/s]
-
-<span>\({\dot m_{src,bypass}}\)</span> =source water bypass mass flow rate in the system [kg/s]
-
-<span>\({\dot m_{cw,CH}}\)</span> =chilled water mass flow rate of i<sup>th</sup> chiller-heater’s evaporator [kg/s]
-
-<span>\({\dot m_{hw,CH}}\)</span> =hot water mass flow rate of i<sup>th</sup> chiller-heater’s condenser [kg/s]
-
-<span>\({\dot m_{src,CH}}\)</span> =source water mass flow rate of i<sup>th</sup> chiller-heater, which varies with operating modes [kg/s]
-
-<span>\({\dot m_{cw,sys}}\)</span> =chilled water mass flow rate of the system [kg/s]
-
-<span>\({\dot m_{hw,sys}}\)</span> =hot water mass flow rate of the system [kg/s]
-
-<span>\({\dot m_{src,sys}}\)</span> =source water mass flow rate of the system [kg/s]
-
-<span>\({T_{cw,sys}}\)</span> =chilled water outlet temperature of the system [C]
-
-<span>\({T_{hw,sys}}\)</span> =hot water outlet temperature of the system [C]
-
-<span>\({T_{src,sys}}\)</span> =source water outlet temperature of the system [C]
-
-<span>\({T_{cw,bypass}}\)</span> =mass-weighed bypass chilled water temperature in the system [C]
-
-<span>\({T_{hw,bypass}}\)</span> =mass-weighed bypass hot water temperature in the system [C]
-
-<span>\({T_{src,bypass}}\)</span> =mass-weighed bypass source water temperature in the system [C]
-
-<span>\({T_{cw,CH}}\)</span> =mass-weighed chilled water outlet temperature from chiller-heaters [C]
-
-<span>\({T_{hw,CH}}\)</span> =mass-weighed hot water outlet temperature from chiller-heaters [C]
-
-<span>\({T_{src,CH}}\)</span> =mass-weighed source water outlet temperature from chiller-heaters [C]
-
-<span>\({T_{cw,i}}\)</span> =chilled water inlet temperature of the system [C]
-
-<span>\({T_{hw,i}}\)</span> =hot water inlet temperature of the system [C]
-
-<span>\({T_{src,i}}\)</span> =source water inlet temperature of the system [C]
-
-<span>\({T_{cw,out}}\)</span> =chilled water outlet temperature of i<sup>th</sup> chiller-heater [C]
-
-<span>\({T_{hw,out}}\)</span> =hot water outlet temperature of i<sup>th</sup> chiller-heater [C]
-
-<span>\({T_{src,out}}\)</span> =source water outlet temperature of i<sup>th</sup> chiller-heater [C]
-
-The model reads node information and local variables of individual chiller-heaters. The nodes and local variables vary with the operating modes as described above in order to calculate mass-weighed temperatures. In the cooling-only mode, it calculates a mass-weighed chilled water temperature (*T<sub>cw,CH</sub>*) and a source water temperature (*T<sub>src,CH</sub>*) as follows:
-
-<div>$${T_{cw,CH}} = \sum\limits_{CH = 1}^n {{T_{cw,out}}} \frac{{{{\dot m}_{cw,CH}}}}{{{m_{cw,sys}}}}$$</div>
-
-***<span>\({T_{src,CH}} = \sum\limits_{CH = 1}^n {{T_{src,out}}} \frac{{{{\dot m}_{src,CH}}}}{{{m_{src,sys}}}}\)</span> ***.
-
-In heating-only mode, it calculates a mass-weighed hot water temperature (*T<sub>hw,CH</sub>*) and a source water temperature (*T<sub>src,CH</sub>*) as follows:
-
-***<span>\({T_{hw,CH}} = \sum\limits_{CH = 1}^n {{T_{hw,out}}} \frac{{{{\dot m}_{hw,CH}}}}{{{m_{hw,sys}}}}\)</span> ***
-
-***<span>\({T_{src,CH}} = \sum\limits_{CH = 1}^n {{T_{src,out}}} \frac{{{{\dot m}_{src,CH}}}}{{{m_{src,sys}}}}\)</span> ***.
-
-When all chiller-heaters are in heat recovery mode, it calculates a mass-weighed chilled water temperature (*T<sub>cw,CH</sub>*) and hot water temperature (*T<sub>hw,CH</sub>*) as follows:
-
-***<span>\({T_{cw,CH}} = \sum\limits_{CH = 1}^n {{T_{cw,out}}} \frac{{{{\dot m}_{cw,CH}}}}{{{m_{cw,sys}}}}\)</span>***
-
-***<span>\({T_{hw,CH}} = \sum\limits_{CH = 1}^n {{T_{hw,out}}} \frac{{{{\dot m}_{hw,CH}}}}{{{m_{hw,sys}}}}\)</span> ***.
-
-In cooling or heating dominant simultaneous cooling-heating mode (mode 4 and 5), at least one chiller-heater should be in heat recovery mode, and the other(s) are in either mode 4 or mode 5. The system is connected to three loops such as chilled water loop, hot water loop, and source water loop. The model thus calculates a mass-weighed chilled water temperature (*T<sub>cw,CH</sub>*), hot water temperature (*T<sub>hw,CH</sub>*), and source water temperature (*T<sub>src,CH</sub>*) as follows:
-
-***<span>\({T_{cw,CH}} = \sum\limits_{CH = 1}^n {{T_{cw,out}}} \frac{{{{\dot m}_{cw,CH}}}}{{{m_{cw,sys}}}}\)</span>***
-
-***<span>\({T_{hw,CH}} = \sum\limits_{CH = 1}^n {{T_{hw,out}}} \frac{{{{\dot m}_{hw,CH}}}}{{{m_{hw,sys}}}}\)</span>***
-
-***<span>\({T_{src,CH}} = \sum\limits_{CH = 1}^n {{T_{src,out}}} \frac{{{{\dot m}_{src,CH}}}}{{{m_{src,sys}}}}\)</span>*** .
-
-The model then calculates a mass-weighed temperature for the by-pass flows remained in the system as follows:
-
-<div>$${T_{cw,bypass}} = {T_{cw,i}}\frac{{{{\dot m}_{cw,bypass}}}}{{{m_{cw,sys}}}}$$</div>
-
-<div>$${T_{hw,bypass}} = {T_{hw,i}}\frac{{{{\dot m}_{hw,bypass}}}}{{{m_{hw,sys}}}}$$</div>
-
-<div>$${T_{src,bypass}} = {T_{src,i}}\frac{{{{\dot m}_{src,bypass}}}}{{{m_{src,sys}}}}$$</div>
-
-The outlet temperatures at each outlet node of the system are then determined as it sums both mass-weighed temperatures up as follows:
-
-<div>$${T_{cw,sys}} = {T_{cw,CH}} + {T_{cw,bypass}}$$</div>
-
-<div>$${T_{hw,sys}} = {T_{hw,CH}} + {T_{hw,bypass}}$$</div>
-
-<span>\({T_{src,sys}} = {T_{src,CH}} + {T_{src,bypass}}\)</span>.
-
-The total heat transfer energy of the system is also calculated in the same manner as the temperature calculations. The model simply sums all heat transfer energy of the chiller-heaters depending on their operating modes.
-
-ChillerHeaterPerformance:Electric:EIR <a name="ChillerHeater"></a>
--------------------------------------
-
-### Overview
-
-The object simulates the performance of a chiller-heater which can receive pre-cooled or pre-heated water from the source loop, and provide cooling, heating, or simultaneous cooling-heating. The object needs to work with the Central Heat Pump System object to be controlled properly. This model does not simulate the thermal performance or the power consumption of associated pumps or cooling towers. The Central Heat Pump System object holds the input/output nodes connection of the chiller-heater and its control scheme, once the chiller-heater is properly referred.
-
-### Model Description
-
-The model uses user-input performance information at design conditions along with three performance curves (curve objects) for cooling capacity and efficiency to determine chiller operation at off-design conditions. Three additional performance curves for heating capacity and efficiency are used when the chiller is operating in a heating-only mode or simultaneous cooling-heating mode.
-
-#### Cooling-only mode
-
-The following nomenclature is used in the cooling equations:
-
-*CompMotorEffic* =compressor motor efficiency
-
-*CompPower<sub>clg</sub>* =compressor power [W]
-
-*CompPower<sub>@PLRmin</sub>*  =compressor power at the minimum part-load ratio [W]
-
-<span>\({C_{p,cw}}\)</span> =chilled water specific heat  [J/kgK]
-
-*CyclingRatio*<sub></sub> =compressor cycling ratio =*PLR<sub>actual</sub>* / *PLR<sub>min</sub>*
-
-*EvapCapAvail<sub>clg</sub>* =available full-load cooling capacity at current conditions [W]
-
-*EvapCapFT<sub>clg</sub>* =cooling capacity function of temperature curve
-
-*EIRFT<sub>clg</sub>* =electric input to cooling output factor for temperature function curve
-
-*EIRFPLR<sub>clg</sub>* =electric input to cooling output factor for part-load function curve
-
-<span>\({\dot m_{cw}}\)</span> =chilled water mass flow rate [kg/s]
-
-<span>\({\dot m_{avail,cw}}\)</span> =chilled water maximum available mass flow rate [kg/s]
-
-*PLR<sub>clg</sub>* =cooling part-load ratio = *CoolingLoad* / *EvapCapAvail<sub>clg</sub>*
-
-*PLR<sub>actual</sub>* =actual part-load ratio at current conditions
-
-*PLR<sub>min</sub>* =minimum part-load ratio
-
-<span>\(QCon{d_{c\lg }}\)</span> =total condenser heat transfer energy [J]
-
-<span>\(\dot QCon{d_{c\lg }}\)</span> =condenser heat transfer rate [W]
-
-<span>\(QEva{p_{c\lg }}\)</span> =total evaporator heat transfer energy [J]
-
-<span>\(\dot QEva{p_{c\lg }}\)</span> =evaporator heat transfer rate [W]
-
-<span>\({\dot Q_{falseloading,c\lg }}\)</span> =false loading rate [W]
-
-*RefCOP<sub>clg</sub>* =reference coefficient of performance [W/W]
-
-*RefEvapCap<sub>clg</sub>* =reference evaporator capacity [W]
-
-*FullLoadPwr<sub>clg</sub>* =reference full load power = *EvapCapAvail<sub>clg</sub>* / *RefCOP<sub>clg</sub>* [W]
-
-*T<sub>cond</sub>* =either entering or leaving condenser water temperature depending on user input for condenser water independent variable. *T<sub>cond,l</sub>*, if “LeavingCondenser� is chosen, or *T<sub>cond,e</sub>*, if “EnteringCondenser� is chosen.
-
-*T<sub>cond,e</sub>* =entering condenser water temperature [C]
-
-*T<sub>cond,l</sub>* =leaving condenser water temperature [C]
-
-*T<sub>cw,e</sub>* =entering chilled water  temperature [W]
-
-*T<sub>cw,l</sub>* =leaving chilled water  temperature [W]
-
-<span>\(\Delta {T_{cw}}\)</span> =chilled water inlet and outlet temperature difference [C]
-
-<span>\(\Delta {T_{cw}}_{,\max }\)</span> =maximum chilled water inlet and outlet temperature difference [C]
-
-The model sequentially calls each chiller-heater module in the order defined in the Central Heat Pump System object. It then determines cooling load that each chiller-heater needs to meet and water flow rates delivered to each chiller-heater. Once each chiller-heater is assumed to operate, it determines cooling capacity and efficiency using user-supplied performance information.
-
-Three performance curves are used in the calculation of cooling capacity and efficiency as follows:
-
-1)   Cooling mode cooling capacity function of temperature curve (*EvapCapFT<sub>clg</sub>*)
-
-2)   Cooling mode electric input to cooling output ratio function of temperature curve (*EIRFT<sub>clg</sub>*)
-
-3)   Cooling mode electric input to cooling output ratio function of part load ratio curve (*EIRFPLR<sub>clg</sub>*)
-
-The Cooling Capacity Function of Temperature Curve (*EvapCapFT<sub>clg</sub>*) represents the fraction of the cooling capacity of the chiller-heater as it varies by temperature. The curve should have a value of 1.0 at the reference conditions. The output of a bi-quadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature is given by:
-
-***<span>\(EvapCapF{T_{c\lg }} = a + b{T_{cw,l}} + c{T_{cw,l}}^2 + d{T_{Cond}} + e{T_{Cond}}^2 + f{T_{cw,l}}{T_{Cond}}\)</span>***.
-
-The Cooling Mode Electric Input to Cooling Output Ratio Function of Temperature (EIRFT<sub>clg</sub>) curve represents the fraction of electricity to the chiller-heater at full load as it varies by temperature. The output of a bi-quadratic curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature is given by:
-
-***<span>\(EIRF{T_{c\lg }} = a + b{T_{cw,l}} + c{T_{cw,l}}^2 + d{T_{Cond}} + e{T_{Cond}}^2 + f{T_{cw,l}}{T_{Cond}}\)</span>***.
-
-The Cooling Mode Electric Input to Cooling Output Ratio Function of Part Load Ratio (EIRFPLR<sub>clg</sub>) curve represents the fraction of electricity to the chiller-heater as the load on the chiller varies at a given set of operating temperatures. The curve is normalized so that at full load the value of the curve should be 1.0. Note that the bi-cubic formulation below is generally only valid when LeavingCondenser variable is chosen for the field of Cooling Mode Condenser Water Temperature Curve Input Variable whereas the quadratic curve can be used for both choices, i.e., LeavingCondenser and EnteringCondenser. Bi-cubic may also be used when the chiller-heater uses a variable-speed compressor motor drive. The output of this curve can be determined by one of the following three performance curves:
-
-<div>$$EIRFPL{R_{c\lg }} = a + b{T_{Cond,l}} + c{T_{Cond,l}}^2 + dPLR + ePL{R^2} + f{T_{Cond,l}}PLR + g \cdot 0 + hPL{R^3} + i \cdot 0 + j \cdot 0$$</div>
-
-<div>$$EIRFPL{R_{c\lg }} = a + bPLR + cPL{R^2}$$</div>
-
-<div>$$EIRFPL{R_{c\lg }} = a + bPLR + cPL{R^2} + dPL{R^3}$$</div>
-
-The full-load cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the design temperatures) is then computed as follows:
-
-***<span>\(EvapCapAvai{l_{c\lg }} = RefEvapCa{p_{c\lg }} \cdot EvapCapF{T_{c\lg }}\)</span>***.
-
-The model then determines current chiller-heater’s evaporator heat transfer rate based on the total cooling load required a central heat pump system to meet and the maximum available chiller-heater cooling capacity. The maximum evaporator temperature difference between the entering chilled water temperature (*T<sub>cw,e</sub>*) and the leaving chilled water temperature (*T<sub>cw,l</sub>*) obtained from the plant loop setpoint temperature can also be determined. It then calculates mass flow rate for variable flow control chiller-heaters and the temperature difference for constant flow control chiller-heaters, setting the cooling load each chiller-heater needs to meet equal to the evaporator heat transfer rate.
-
-As for variable flow control chiller-heaters, the chilled water mass flow rate is computed as follows:
-
-***<span>\({\dot m_{cw}} = \frac{{\dot QEva{p_{c\lg }}}}{{{C_{p,cw}}\Delta {T_{cw,\max }}}}\)</span>***.
-
-The chilled water mass flow rate calculated is then compared to the maximum available mass flow rate for individual chiller-heaters. If the calculated one is bigger than the maximum, the model sets the chilled water mass flow rate equal to the maximum. It then adjusts the temperature difference based on the evaporator heat transfer rate and the maximum mass flow rate. If the adjusted temperature difference also exceeds the maximum, the model finally adjusts the evaporator heat transfer rate at the maximum temperature difference and mass flow rate as follows:
-
-***<span>\(\dot QEva{p_{c\lg }} = {\dot m_{avail,cw}}{C_{p,cw}}\Delta {T_{cw,\max }}\)</span>***.
-
-As for constant flow control chiller-heaters, the model calculates chilled water temperature difference as follows:
-
-***<span>\(\Delta {T_{cw}} = \frac{{\dot QEva{p_{c\lg }}}}{{{{\dot m}_{avail,cw}}{C_{p,cw}}}}\)</span>***.
-
-The temperature difference calculated is then compared to the maximum temperature difference allowed. If the calculated one is bigger than the maximum, the model sets the chilled water temperature difference equal the maximum, and then adjusts the evaporator heat transfer rate at the given conditions as follows:
-
-***<span>\(\dot QEva{p_{c\lg }} = {\dot m_{avail,cw}}{C_{p,cw}}\Delta {T_{cw,\max }}\)</span>***.
-
-The model then calculates the part-load ratio as the ratio of the evaporator heat transfer rate to the available chiller-heater capacity as follows:
-
-***<span>\(PL{R_{c\lg }} = \frac{{\dot QEva{p_{c\lg }}}}{{\dot QEvapAvai{l_{c\lg }}}}\)</span>***.
-
-The part-load ratio calculated is set to be between the maximum of 1.0 and the minimum of 0.0 when it is out of the range. Once the part-load ratio is calculated the cycling ratio and false loading rate can be obtained as follows:
-
-<div>$$CyclingRatio = \frac{{PL{R_{{\rm{actual}}}}}}{{PL{R_{{\rm{min}}}}}}$$</div>
-
-<span>\({\dot Q_{falseloading,c\lg }} = EvapCapAvai{l_{{\rm{clg}}}} \cdot PL{R_{c\lg }} \cdot CyclingRatio - \dot QEva{p_{{\rm{clg}}}}\)</span>.
-
-The compressor power demand is then computed by:
-
-<span>\(CompPowe{r_{c\lg }} = RefFullLoadPowe{r_{{\rm{clg}}}} \cdot {\rm{ }}EIRF{T_{c\lg }}{\rm{ }} \cdot EIRFPL{R_{c\lg }} \cdot CyclingRatio\)</span>.
-
-The heat transfer rate for the chiller-heater condenser can then be computed as follows:
-
-<span>\(\dot QCon{d_{c\lg }} = ComPowe{r_{c\lg }} \cdot CompMotorEffic + \dot QEva{p_{c\lg }} + {\dot Q_{falseloading,c\lg }}\)</span> .
-
-The total heat transfer energy by the evaporator and condenser can be calculated as follows:
-
-<div>$$QEva{p_{c\lg }} = \dot QEva{p_{c\lg }} \cdot TimeStepSys \cdot 3600$$</div>
-
-<span>\(QCon{d_{c\lg }} = \dot QCon{d_{c\lg }} \cdot TimeStepSys \cdot 3600\)</span> .
-
-#### Heating-only mode and Simultaneous cooling-heating mode
-
-The following nomenclature is used in the heating equations:
-
-*CompMotorEffic* =compressor motor efficiency
-
-*CompPower<sub>htg</sub>* =compressor power demand [W]
-
-*CompPower<sub>@PLRmin</sub>*  =compressor power at the minimum part-load ratio [W]
-
-<span>\({C_{p,evap}}\)</span> =evaporator water specific heat  [J/kgK]
-
-<span>\({C_{p,hw}}\)</span> =hot water specific heat  [J/kgK]
-
-*CyclingRatio*<sub></sub> =compressor cycling ratio =*PLR<sub>actual</sub>* / *PLR<sub>min</sub>*
-
-*EvapCapAvail<sub>htg</sub>* =available full-load cooling capacity at current conditions [W]
-
-*EvapCapFT<sub>htg</sub>* =heating mode cooling capacity function of temperature curve
-
-*EIRFT<sub>htg</sub>* =electric input to cooling output factor for temperature function curve
-
-*EIRFPLR<sub>htg</sub>* =electric input to cooling output factor for part-load function curve
-
-<span>\({\dot m_{avail,evap}}\)</span> =evaporator water maximum available mass flow rate [kg/s]
-
-<span>\({\dot m_{avail,hw}}\)</span> =condenser water maximum available mass flow rate [kg/s]
-
-<span>\({\dot m_{hw}}\)</span> =hot water mass flow rate [kg/s]
-
-*PLR<sub>htg</sub>* =cooling part-load ratio = *RefCap* / *EvapCapAvail<sub>htg</sub>*
-
-*PLR<sub>max</sub>* =maximum part-load ratio at current conditions
-
-*PLR<sub>min</sub>* =minimum part-load ratio
-
-<span>\(QCon{d_{htg}}\)</span> =total condenser heat transfer energy [J]
-
-<span>\(\dot QCondAvai{l_{htg}}\)</span> =available full-load heating capacity at current conditions [W]
-
-<span>\(\dot QCon{d_{htg}}\)</span> =condenser heat transfer rate [W]
-
-<span>\(QEva{p_{htg}}\)</span> =total evaporator heat transfer energy [J]
-
-<span>\(\dot QEva{p_{htg}}\)</span> =evaporator heat transfer rate [W]
-
-<span>\({\dot Q_{falseloading,htg}}\)</span> =false loading rate [W]
-
-*RefCOP<sub>htg</sub>* =reference coefficient of performance [W/W]
-
-*RefEvapCap<sub>htg</sub>* =reference evaporator capacity [W]
-
-*FullLoadPwr<sub>htg</sub>* =reference full load power = *EvapCapAvail<sub>htg</sub>*/ *RefCOP<sub>htg</sub>* [W]
-
-*T<sub>cond</sub>* =either entering or leaving condenser water temperature depending on user input for condenser water independent variable. *T<sub>cond,l</sub>*, if “LeavingCondenser� is chosen, or *T<sub>cond,e</sub>*, if “EnteringCondenser� is chosen.
-
-*T<sub>cond,e</sub>* =entering condenser water temperature [C]
-
-*T<sub>cond,l</sub>* =leaving condenser water temperature [C]
-
-*T<sub>cw,l</sub>* =leaving chilled water  temperature [C]
-
-*T<sub>hw,e</sub>* =entering hot water temperature [C]
-
-*T<sub>hw,l</sub>* =leaving hot water temperature [C]
-
-<span>\(\Delta {T_{evap}}\)</span> =evaporator inlet and outlet water temperature difference [C]
-
-<span>\(\Delta {T_{hw}}\)</span> =hot water inlet and outlet temperature difference [C]
-
-<span>\(\Delta {T_{hw}}_{,\max }\)</span> =maximum hot water inlet and outlet temperature difference [C]
-
-The calculations for the evaporator side are similar to the cooling-only mode calculations. The evaporator capacity and efficiency is determined by a different set of three performance curves read in the cooling-only mode, and the performance curve set is used for both heating-only mode and simultaneous cooling-heating mode. During these modes, the evaporator side is not connected to the chilled water loop, but source water loop. The model thus assumes that each chiller-heater does not meet the plant loop chilled water setpoint temperature while the evaporator operates at the full load capacity to produce heating at a constant water flow rate.
-
-The model sequentially calls each chiller-heater module in the order of the definition in the central heat pump system. It then determines heating load that each chiller-heater needs to meet and water flow rates delivered to each chiller-heater. Once each chiller-heater is assumed to operate, it determines heating capacity and efficiency using the following performance curves:
-
-1)   Heating mode cooling capacity function of temperature curve (*EvapCapFT<sub>htg</sub>*)
-
-2)   Heating mode electric input to cooling output ratio function of temperature curve (*EIRFT<sub>htg</sub>*)
-
-3)   Heating mode electric input to cooling output ratio function of part load ratio curve (*EIRFPLR<sub>htg</sub>*)
-
-The output of a Heating Mode Cooling Capacity Function of Temperature curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature is given by:
-
-***<span>\(EvapCapF{T_{htg}} = a + b{T_{cw,l}} + c{T_{cw,l}}^2 + d{T_{Cond}} + e{T_{Cond}}^2 + f{T_{cw,l}}{T_{Cond}}\)</span>***
-
-The output of a Heating Mode Cooling Output Ratio Function of Temperature curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature is given by:
-
-***<span>\(EIRF{T_{htg}} = a + b{T_{cw,l}} + c{T_{cw,l}}^2 + d{T_{Cond}} + e{T_{Cond}}^2 + f{T_{cw,l}}{T_{Cond}}\)</span>***.
-
-The output of Heating Mode Cooling Output Ratio Function of Part Load Ratio curve can be determined by one of the following three performance curves as follows:
-
-<div>$$EIRFPL{R_{htg}} = a + b{T_{Cond,l}} + c{T_{Cond,l}}^2 + dPLR + ePL{R^2} + f{T_{Cond,l}}PLR + g \cdot 0 + hPL{R^3} + i \cdot 0 + j \cdot 0$$</div>
-
-<div>$$EIRFPL{R_{htg}} = a + bPLR + cPL{R^2}$$</div>
-
-<div>$$EIRFPL{R_{htg}} = a + bPLR + cPL{R^2} + dPL{R^3}$$</div>
-
-The full-load evaporator capacity at specific temperature operating conditions is then given by:
-
-***<span>\(EvapCapAvai{l_{htg}} = RefEvapCa{p_{htg}} \cdot EvapCapF{T_{htg}}\)</span>***.
-
-The part-load ratio is set to be between zero and the maximum, and the evaporator heat transfer rate is computed by:
-
-***<span>\(\dot QEva{p_{htg}} = EvapCapAvai{l_{htg}}PL{R_{htg}}\)</span>***The evaporator inlet and outlet temperature difference is then given by:
-
-***<span>\(\Delta {T_{evap}} = \frac{{\dot QEva{p_{htg}}}}{{{{\dot m}_{avail,evap}}{C_{p,evap}}}}\)</span>***
-
-Once the part-load ratio is calculated the cycling ratio and false loading rate are computed by:
-
-<div>$$CyclingRatio = \frac{{PL{R_{{\rm{actual}}}}}}{{PL{R_{{\rm{min}}}}}}$$</div>
-
-<span>\({\dot Q_{falseloading,htg}} = EvapCapAvai{l_{{\rm{htg}}}} \cdot PL{R_{htg}} \cdot CyclingRatio - \dot QEva{p_{{\rm{htg}}}}\)</span>.
-
-The compressor power demand is then computed by:
-
-***<span>\(CompPowe{r_{htg}} = FullLoadPowe{r_{{\rm{htg}}}} \cdot {\rm{ }}EIRF{T_{htg}}{\rm{ }} \cdot EIRFPL{R_{htg}} \cdot CyclingRatio\)</span>***
-
-The heat transfer rate of the chiller-heater condenser is then computed as follows:
-
-<div>$$\dot QCondAvai{l_{htg}} = ComPowe{r_{htg}} \cdot CompMotorEffic + \dot QEva{p_{htg}} + {\dot Q_{falseloading,htg}}$$</div>
-
-Once condenser available heating capacity is determined, the model calculates current chiller-heater’s condenser heat transfer rate based on the total heating load required a central heat pump system to meet as well as available heating capacity of the chiller-heater. The maximum condenser temperature difference between the entering hot water temperature (*T<sub>hw,e</sub>*) and the leaving hot water temperature (*T<sub>hw,l</sub>*) obtained from the plant loop setpoint temperature can also be obtained. It then calculates condenser water mass flow rate for variable flow control chiller-heaters and the hot water temperature difference for constant flow control chiller-heaters, setting the cooling load that each chiller-heater needs to meet equal the evaporator heat transfer rate.
-
-As for variable flow control chiller-heaters, the condenser water mass flow rate is computed as follows:
-
-***<span>\({\dot m_{hw}} = \frac{{\dot QCon{d_{htg}}}}{{{C_{p,hw}}\Delta {T_{hw,\max }}}}\)</span>***.
-
-The condenser water mass flow rate calculated is then compared to the maximum available mass flow rate for individual chiller-heaters. If the calculated one is bigger than the maximum, the model sets the condenser water mass flow rate equal the maximum. It then adjusts the hot water temperature difference at the maximum mass flow rate. If the adjusted temperature difference also exceeds the maximum, the model finally adjusts the condenser heat transfer rate at the maximum allowable conditions as follows:
-
-***<span>\(\dot QCon{d_{htg}} = {\dot m_{avail,hw}}{C_{p,hw}}\Delta {T_{hw,\max }}\)</span>***.
-
-As for constant flow control chiller-heaters, the model calculates condenser temperature difference as follows:
-
-***<span>\(\Delta {T_{hw}} = \frac{{\dot QCon{d_{htg}}}}{{{{\dot m}_{avail,hw}}{C_{p,hw}}}}\)</span>***.
-
-The temperature difference calculated is then compared to maximum hot water temperature difference. If the calculated one is bigger than the maximum, the model sets the hot water temperature difference equal the maximum, and then adjusts the condenser heat transfer rate at the given conditions as follows:
-
-***<span>\(\dot QCon{d_{htg}} = {\dot m_{avail,hw}}{C_{p,hw}}\Delta {T_{hw,\max }}\)</span>***.
-
-Finally, the total heat transfer energy by the evaporator and condenser can then be calculated as follows:
-
-***<span>\(QEva{p_{htg}} = \dot QEva{p_{htg}} \cdot TimeStepSys \cdot 3600\)</span>***
-
-***<span>\(QCon{d_{htg}} = \dot QCon{d_{htg}} \cdot TimeStepSys \cdot 3600\)</span>***.
-
-### References
-
-Central Geothermal Systems, Applications Engineering Manual, Trane Company, April 2010, SYS-APM009-EN.
-
-Plant Temperature Source Component <a name="PlantComponent"></a>
-----------------------------------
-
-This component (Object: PlantComponent:TemperatureSource) is a simple object used to simulate systems with a known supply temperature.  This could include a river, well, or other configuration where a known temperature is pumped back into the plant system.  This fluid could be isolated from chilled water and other loops by using a heat exchanger connection between the loops.
-
-The temperature of the source of this object can be either constant or scheduled.  If scheduled, it could also be actuated by EMS to allow a calculated temperature at run-time.
-
-The logic of this component is quite simple: if there is flow through the component, the outlet temperature is always the source temperature.  The component requests flow from the design flow rate, which can be autosized.
-
-#### References
-
-No specific references.
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-
-<!--RemoveStart-->
-Simulation Models – Encyclopedic Reference
-==========================================
-
-The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of “Heat Balance�, “HVAC�, and “Plant�.  With the integrated solution, these designations signify where the effects of these models have their first impacts.
-
-Main Sections:
-
-* [Radiant System Models](#RadiantSystems)
-* [Refrigeration Equipment](#Refrigeration)
-* [Setpoint Managers](#SetpointManagers)
-* [Solar Collectors](#SolarCollectors)
-* [System Availability Managers](#AvailManagers)
-<!--RemoveEnd-->
-
-Radiant System Models <a name="RadiantSystems"></a>
----------------------
-
-### Low Temperature Radiant System Model
-
-The input objects ZoneHVAC:LowTemperatureRadiant:ConstantFlow, ZoneHVAC:LowTemperatureRadiant:VariableFlow, and ZoneHVAC:LowTemperatureRadiant:Electric provide models for low temperature radiant heating and cooling systems that appear, on the surface, to be relatively simple systems.  The system circulates hot or cold fluid through tubes embedded in a wall, ceiling, or floor or runs current through electric resistance wires embedded in a surface or a panel.  Energy is thus either added to or removed from the space, and zone occupants are conditioned by both radiation exchange with the system and convection from the surrounding air that is also affected by the system.  Unless specifically required for indoor air quality considerations, fans, ductwork, dampers, etc. are not needed.
-
-Despite the relative simplicity of the low temperature radiant systems, the integration of such a system within an energy analysis program requires one to overcome several challenges.  First, for systems with significant thermal mass, the conduction transfer function method for modeling transient conduction must be extended to include embedded heat sources or sinks.  Second, one must integrate this formulation within an energy analysis program like EnergyPlus.  Finally, one must overcome the fact that the radiant system is both a zone heat balance element and a conditioning system.  Each of these issues will be addressed in the next several subsections.
-
-#### One Dimensional Heat Transfer Through Multilayered Slabs
-
-One of the most important forms of heat transfer in energy analysis is heat conduction through building elements such as walls, floors, and roofs.  While some thermally lightweight structures can be approximated by steady state heat conduction, a method that applies to all structures must account for the presence of thermal mass within the building elements.  Transient one dimensional heat conduction through a homogeneous layer with constant thermal properties such as the one shown in Figure 266 is governed by the following equation:
-
-<div>$$\frac{{{\partial ^2}T}}{{\partial {x^2}}} = \frac{1}{\alpha }\frac{{\partial T}}{{\partial t}}$$</div>
-
-where: T is the temperature as a function of position and time,
-
-x is the position,
-
-t is the time,
-
-<span>\(\alpha  = \frac{k}{{\rho {c_p}}}\)</span> is the thermal diffusivity of the layer material,
-
-k is its thermal conductivity,
-
-r is its density, and
-
-cp is its specific heat.
-
-This equation is typically coupled with Fourier’s law of conduction that relates the heat flux at any position and time to temperature as follows:
-
-<div>$$q''\left( {x,t} \right) =  - k\frac{{\partial T\left( {x,t} \right)}}{{\partial x}}$$</div>
-
-![](media/image5973.png)
-
-Figure 266. Single Layered Building Element
-
-While analytical solutions exist for the single homogeneous layer shown in Figure 266, the solution becomes extremely tedious for the multiple layered slab shown in Figure 267.
-
-![](media/image5974.png)
-
-Figure 267. Multilayered Building Element
-
-#### Time Series Solutions:  Conduction Transfer Functions
-
-Equations and can be solved numerically in a variety of ways.  As mentioned in the previous section, other models have used control theory and numerical methods such as finite difference and finite element.  However, each of these methods have drawbacks which render them inappropriate for use within an energy analysis program which requires both accuracy and efficiency from the simulation.
-
-Another possible modeling method is a time series solution.  Several of the detailed energy analysis programs such as EnergyPlus use a time series solution to transient heat conduction.  The most basic time series solution is the response factor equation which relates the flux at one surface of an element to an infinite series of temperature histories at both sides as shown by:
-
-<div>$${q''_{i,t}} = \sum\limits_{m = 1}^\infty  {{X_m}{T_{i,t - m + 1}}}  - \sum\limits_{m = 1}^\infty  {{Y_m}{T_{o,t - m + 1}}} $$</div>
-
-where q� is heat flux, T is temperature, i signifies the inside of the building element, o signifies the outside of the building element, and t represents the current time step.
-
-While in most cases the terms in the series decay fairly rapidly, the infinite number of terms needed for an exact response factor solution makes it less than desirable.  Fortunately, the similarity of higher order terms can be used to replace them with flux history terms.  The new solution contains elements that are called conduction transfer functions (CTFs).  The basic form of a conduction transfer function solution is shown by the following equation:
-
-<div>$${q''_{i,t}} = \sum\limits_{m = 1}^M {{X_m}{T_{i,t - m + 1}}}  - \sum\limits_{m = 1}^M {{Y_m}{T_{o,t - m + 1}}}  + \sum\limits_{m = 1}^k {{F_m}{{q''}_{i,t - m}}} $$</div>
-
-where k is the order of the conduction transfer functions, M is a finite number defined by the order of the conduction transfer functions, and X, Y, and F are the conduction transfer functions.  This equation states that the heat flux at the interior surface of any generic building element for which the assumption of one dimensional conduction heat transfer is valid is linearly related to the current and some of the previous temperatures at both the interior and exterior surface as well as some of the previous flux values at the interior surface.  A similar equation holds for the heat flux at the exterior surface.
-
-The final CTF solution form reveals why it is so elegant and powerful.  With a single, relatively simple equation, the conduction heat transfer through an element can be calculated.  The coefficients (CTFs) in the equation are constants that only need to be determined once.  The only storage of data required is the CTFs themselves and a limited number of temperature and flux terms.  The formulation is valid for any surface type and does not require the calculation or storage of element interior temperatures.
-
-As the next several sections will detail, there are two main methods for calculating conduction transfer functions:  the Laplace Transform method and the State Space method.  Both methods are well suited for the main focus of this research, the extension of conduction transfer functions to include heat sources or sinks.
-
-#### Laplace Transform Formulation
-
-The traditional method for calculating conduction transfer functions is described in detail by Hittle (1981).  Beginning with the transient one dimensional heat conduction equation {Equation } and Fourier's law of conduction {Equation }, the Laplace transform method is used to convert the governing equations into the s-domain for a single layer such as the one shown in Figure 266.
-
-<div>$$\frac{{{d^2}T\left( {x,s} \right)}}{{d{x^2}}} = \frac{s}{\alpha }T\left( {x,s} \right)$$</div>
-
-<div>$$q''\left( {x,s} \right) =  - k\frac{{dT\left( {x,s} \right)}}{{dx}}$$</div>
-
-The transformed equations are solved and then put in matrix form as shown below:
-
-<div>$$
-  \left[ 
-    {\begin{array}{*{20}{c}}
-      {{T_1}\left( s \right)} \\ {{q_1}\left( s \right)}
-    \end{array}}
-  \right] = \left[ 
-    {\begin{array}{*{20}{c}}
-      {{A_1}\left( s \right)}&{{B_1}\left( s \right)} \\
-      {{C_1}\left( s \right)}&{{D_1}\left( s \right)}
-    \end{array}}
-  \right] \left[ 
-    {\begin{array}{*{20}{c}}
-      {{T_2}\left( s \right)} \\
-      {{q_2}\left( s \right)}
-    \end{array}}
-  \right]
-$$</div>
-
-where: T1(s), T2(s), q1(s), and q2(s) are the temperature and flux terms in the Laplace domain,
-
-<span>\({A_1}\left( s \right) = \cosh \left( {{\ell_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} } \right)\)</span>,
-
-<span>\({B_1}\left( s \right) = \left( {{1 \mathord{\left/ {\vphantom {1 {{k_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} }}} \right. } {{k_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} }}} \right)\sinh \left( {{\ell_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} } \right)\)</span>,
-
-<span>\({C_1}\left( s \right) = {k_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} \sinh \left( {{\ell_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} } \right)\)</span>,
-
-<span>\({D_1}\left( s \right) = \cosh \left( {{\ell_1}\sqrt {{s \mathord{\left/ {\vphantom {s {{\alpha_1}}}} \right. } {{\alpha_1}}}} } \right)\)</span>,
-
-k1 is the thermal conductivity of the layer,
-
-a1 is the thermal diffusivity of the layer, and
-
-<span>\({\ell_1}\)</span> is the thickness of the layer.
-
-The 2 x 2 matrix consisting of A1(s), B1(s), C1(s), and D1(s) is called the transmission matrix and contains all of the thermophysical properties of the layer necessary to calculate transient conduction heat transfer through it.  It can easily be shown that a second layer could be characterized in a similar way as:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_2}\left( s \right)}\\ {{q_2}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_3}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right]$$</div>
-
-where A2(s), B2(s), C2(s), and D2(s) are calculated using the properties of the second layer.  This can be substituted into Equation to provide insight how the extension to multilayered slabs is achieved.
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_3}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right]$$</div>
-
-Thus, for a multilayered element as shown in Figure 267, each separate layer has a transmission matrix of Ai(s), Bi(s), Ci(s), and Di(s) associated with it.  The form of the matrix equation for the multilayered element is the same as the equation for a single layer:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{A\left( s \right)}&{B\left( s \right)}\\ {C\left( s \right)}&{D\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_{n + 1}}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right]$$</div>
-
-but the transmission matrix is replaced by:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{A\left( s \right)}&{B\left( s \right)}\\ {C\left( s \right)}&{D\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right] \cdots \left[ {\begin{array}{*{20}{c}}{{A_n}\left( s \right)}&{{B_n}\left( s \right)}\\ {{C_n}\left( s \right)}&{{D_n}\left( s \right)}\end{array}} \right]$$</div>
-
-Equation is typically rearranged as follows:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{q_1}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{D\left( s \right)}}{{B\left( s \right)}}}&{\frac{{ - 1}}{{B\left( s \right)}}}\\ {\frac{1}{{B\left( s \right)}}}&{\frac{{ - A\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{T_{n + 1}}\left( s \right)}\end{array}} \right]$$</div>
-
-which relates the flux at either surface of the element to the temperature histories at both surfaces.  When the temperature histories are formulated as triangular pulses made up of simple ramp functions, the roots of this equation can be found and result in response factors.  The response factors can be simplified as described above through the introduction of flux history terms to form conduction transfer functions.  A simplified method of finding the roots of the Laplace domain equations is described by Hittle and Bishop (1983) and is used by the current version of BLAST.
-
-#### State Space Formulation
-
-Recently, another method of finding conduction transfer functions starting from a state space representation has begun receiving increased attention (Ceylan and Myers 1980; Seem 1987; Ouyang and Haghighat 1991).  The basic state space system is defined by the following linear matrix equations:
-
-<div>$$\frac{{d\left[ x \right]}}{{dt}} = \left[ A \right]\left[ x \right] + \left[ B \right]\left[ u \right]$$</div>
-
-<div>$$\left[ y \right] = \left[ C \right]\left[ x \right] + \left[ D \right]\left[ u \right]$$</div>
-
-where x is a vector of state variables, u is a vector of inputs, y is the output vector, t is time, and A, B, C, and D are coefficient matrices.  Through the use of matrix algebra, the vector of state variables (x) can be eliminated from the system of equations, and the output vector (y) can be related directly to the input vector (u) and time histories of the input and output vectors.
-
-This formulation can be used to solve the transient heat conduction equation by enforcing a finite difference grid over the various layers in the building element being analyzed.  In this case, the state variables are the nodal temperatures, the environmental temperatures (interior and exterior) are the inputs, and the resulting heat fluxes at both surfaces are the outputs.  Thus, the state space representation with finite difference variables would take the following form:
-
-<div>$$\frac{{d\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right]}}{{dt}} = \left[ A \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right] + \left[ B \right]\left[ {\begin{array}{*{20}{c}}{{T_i}}\\ {{T_o}}\end{array}} \right]$$</div>
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{{q''}_i}}\\ {{{q''}_o}}\end{array}} \right] = \left[ C \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right] + \left[ D \right]\left[ {\begin{array}{*{20}{c}}{{T_i}}\\ {{T_o}}\end{array}} \right]$$</div>
-
-where T1, T2, ..., Tn-1, Tn are the finite difference nodal temperatures, n is the number of nodes, Ti and To are the interior and exterior environmental temperatures, and <span>\({q''_i}\)</span> and <span>\({q''_o}\)</span> are the heat fluxes (desired output).
-
-Seem (1987) shows that for a simple one layer slab with two interior nodes as in Figure 268 and convection at both sides the resulting finite difference equations are given by:
-
-<div>$$C\frac{{d{T_1}}}{{dt}} = hA\left( {{T_o} - {T_1}} \right) + \frac{{{T_2} - {T_1}}}{R}$$</div>
-
-<div>$$C\frac{{d{T_2}}}{{dt}} = hA\left( {{T_i} - {T_2}} \right) + \frac{{{T_1} - {T_2}}}{R}$$</div>
-
-<div>$${q''_i} = h\left( {{T_i} - {T_2}} \right)$$</div>
-
-<div>$${q''_o} = h\left( {{T_1} - {T_o}} \right)$$</div>
-
-where:         <span>\(R = \frac{\ell }{{kA}}\)</span>  , thermal resistance
-
-<span>\(C = \frac{{\rho {c_p}\ell A}}{2}\)</span> , thermal capacitance
-
-<span>\({T_o}\)</span>= outside temperature
-
-<span>\({T_i}\)</span>= inside temperature
-
-<span>\({T_1}\)</span>=temperature of node 1
-
-<span>\({T_2}\)</span>=temperature of node 2
-
-and
-
-A is the area of the surface exposed to the environmental temperatures.
-
-In matrix format:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{\frac{{d{T_1}}}{{dt}}}\\ {\frac{{d{T_2}}}{{dt}}}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{ - 1}}{{RC}} - \frac{{hA}}{C}}&{\frac{1}{{RC}}}\\ {\frac{1}{{RC}}}&{\frac{{ - 1}}{{RC}} - \frac{{hA}}{C}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ {{T_2}}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{\frac{{hA}}{C}}&0\\0&{\frac{{hA}}{C}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\end{array}} \right]$$</div>
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{{q''}_i}}\\ {{{q''}_o}}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}0&{ - h}\\h&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ {{T_2}}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0&h\\ { - h}&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\end{array}} \right]$$</div>
-
-![](media/image6008.svg.png)
-
-Figure 268. Two Node State Space Example
-
-The important aspect of the state space technique is that through the use of relatively simple matrix algebra the state space variables (nodal temperatures) can be eliminated to arrive at a matrix equation that gives the outputs (heat fluxes) as a function of the inputs (environmental temperatures) only.  This eliminates the need to solve for roots in the Laplace domain.  In addition, the resulting matrix form has more physical meaning than complex functions required by the Laplace transform method.  The current version of EnergyPlus uses the state space method for computing CTFs.
-
-The accuracy of the state space method of calculating CTFs has been addressed in the literature.  Ceylan and Myers (1980) compared the response predicted by the state space method to various other solution techniques including an analytical solution.  Their results showed that for an adequate number of nodes the state space method computed a heat flux at the surface of a simple one layer slab within 1% of the analytical solution.  Ouyang and Haghighat (1991) made a direct comparison between the Laplace and state space methods.  For a wall composed of insulation between two layers of concrete, they found almost no difference in the response factors calculated by each method.
-
-#### Extension of Time Series Solutions to Include Heat Sources and Obtain Internal Temperatures
-
-#### Laplace Transform Formulation
-
-Degiovanni (1988) proposed two methodologies for including sources or sinks in the Laplace Transform Formulation.  The first method shows how a source that varies as a function of time and location can be incorporated.  The resulting equations involve some fairly complicated terms including spatial derivatives.
-
-The second method that will be analyzed in more detail involves the addition of a source or sink at the interface between two layers.  The derivation of the necessary equations is begun by analyzing the simple two layer element shown in Figure 269.
-
-![](media/image6009.png)
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_2}\left( s \right)}\\ {{q_2}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_3}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right]$$</div>
-
-Figure 269.  Two Layer Example for Deriving the Laplace Transform Extension to Include Sources and Sinks
-
-For the first layer, it was determined that in the Laplace domain
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_2}\left( s \right)}\\ {{q_2}\left( s \right)}\end{array}} \right]$$</div>
-
-For the second layer:
-
-
-
-To link the two layers and include the heat source between them, the following substitution is made:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_2}\left( s \right)}\\ {{q_2}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{T_{2 + }}\left( s \right)}\\ {{q_{2 + }}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]$$</div>
-
-which results in:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left\{ {\left[ {\begin{array}{*{20}{c}}{{T_{2 + }}\left( s \right)}\\ {{q_{2 + }}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]} \right\}$$</div>
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left\{ {\left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_3}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]} \right\}$$</div>
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{A_2}\left( s \right)}&{{B_2}\left( s \right)}\\ {{C_2}\left( s \right)}&{{D_2}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_3}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{{A_1}\left( s \right)}&{{B_1}\left( s \right)}\\ {{C_1}\left( s \right)}&{{D_1}\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]$$</div>
-
-While Degiovanni concludes with this formula, some insight into what the generic equation for an element that has n layers might look like is gained by working with Equation .  If a layer is added to the left of the first layer, the entire right hand side of Equation is multiplied by the transmission matrix of the new layer.  Conversely, if a layer is added to the right of the second layer in Figure 269, the vector containing the Laplace transform of the temperature and heat flux at interface 3 is replaced by the product of the transmission matrix of the new layer and the vector for temperature and heat flux at the next interface, and the term dealing with the heat source is not affected.  The general equation for a building element with n layers and m layers between the left hand surface and the heat source can be derived as:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left( {\prod\limits_{i = 1}^n {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]} } \right)\left[ {\begin{array}{*{20}{c}}{{T_{n + 1}}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right] + \left( {\prod\limits_{i = 1}^m {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]} } \right)\left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]$$</div>
-
-or in more compact form:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{q_1}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{A\left( s \right)}&{B\left( s \right)}\\ {C\left( s \right)}&{D\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_{n + 1}}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{a\left( s \right)}&{b\left( s \right)}\\ {c\left( s \right)}&{d\left( s \right)}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}0\\ {{q_{source}}\left( s \right)}\end{array}} \right]$$</div>
-
-where:  <span>\(\left[ {\begin{array}{*{20}{c}}{A\left( s \right)}&{B\left( s \right)}\\ {C\left( s \right)}&{D\left( s \right)}\end{array}} \right] = \prod\limits_{i = 1}^n {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]} \)</span>  and  <span>\(\left[ {\begin{array}{*{20}{c}}{a\left( s \right)}&{b\left( s \right)}\\ {c\left( s \right)}&{d\left( s \right)}\end{array}} \right] = \prod\limits_{i = 1}^m {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]} \)</span> .
-
-Next, Equation must be rearranged to match the form of Equation , which relates the heat flux at both sides of the element to the temperature at each side.  The matrix equation that is obtained shows that:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{q_1}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{D\left( s \right)}}{{B\left( s \right)}}}&{\frac{{ - 1}}{{B\left( s \right)}}}\\ {\frac{1}{{B\left( s \right)}}}&{\frac{{ - A\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{T_{n + 1}}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{d\left( s \right) - \frac{{D\left( s \right)b\left( s \right)}}{{B\left( s \right)}}}\\ {\frac{{b\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {{q_{source}}\left( s \right)} \right]$$</div>
-
-This equation bears a striking resemblance to Equation .  If the source term in Equation is dropped, then the equation is identical to Equation .  This result conforms with the superposition principle which was used to develop the conduction transfer functions from the summation of a series of triangular pulses or ramp sets.  Now, the effect of the heat source is simply added to the response to the temperature inputs.
-
-While Equation is correct for any single or multilayered element, the first term in the heat source transmission matrix does not appear to match the compactness of the other terms in the matrix equation.  It can be shown (see Strand 1995: equations 32 through 42 which detail this derivation) that the heat source transmission term for a two-layer problem reduces to
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{q_1}\left( s \right)}\\ {{q_3}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{D\left( s \right)}}{{B\left( s \right)}}}&{\frac{{ - 1}}{{B\left( s \right)}}}\\ {\frac{1}{{B\left( s \right)}}}&{\frac{{ - A\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{T_3}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{\frac{{{B_2}\left( s \right)}}{{B\left( s \right)}}}\\ {\frac{{{B_1}\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {{q_{source}}\left( s \right)} \right]$$</div>
-
-If this is extended to a slab with n layers and a source between the m and m+1 layers, the general matrix equation for obtaining heat source transfer functions using the Laplace transform method is:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{q_1}\left( s \right)}\\ {{q_{n + 1}}\left( s \right)}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{D\left( s \right)}}{{B\left( s \right)}}}&{\frac{{ - 1}}{{B\left( s \right)}}}\\ {\frac{1}{{B\left( s \right)}}}&{\frac{{ - A\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}\left( s \right)}\\ {{T_{n + 1}}\left( s \right)}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{\frac{{\bar b\left( s \right)}}{{B\left( s \right)}}}\\ {\frac{{b\left( s \right)}}{{B\left( s \right)}}}\end{array}} \right]\left[ {{q_{source}}\left( s \right)} \right]$$</div>
-
-where: <span>\(\left[ {\begin{array}{*{20}{c}}{A\left( s \right)}&{B\left( s \right)}\\ {C\left( s \right)}&{D\left( s \right)}\end{array}} \right] = \prod\limits_{i = 1}^n {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]} \)</span> ,
-
-<span>\(\left[ {\begin{array}{*{20}{c}}{a\left( s \right)}&{b\left( s \right)}\\ {c\left( s \right)}&{d\left( s \right)}\end{array}} \right] = \prod\limits_{i = 1}^m {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]} \)</span> , and
-
-<span>\(\left[ {\begin{array}{*{20}{c}}{\bar a\left( s \right)}&{\bar b\left( s \right)}\\ {\bar c\left( s \right)}&{\bar d\left( s \right)}\end{array}} \right] = \prod\limits_{i = m + 1}^n {\left[ {\begin{array}{*{20}{c}}{{A_i}\left( s \right)}&{{B_i}\left( s \right)}\\ {{C_i}\left( s \right)}&{{D_i}\left( s \right)}\end{array}} \right]} \)</span> .
-
-At first glance, the terms in the heat source transmission matrix may appear to be reversed.  It is expected that only the layers to the left of the source will affect q1(s), but the presence of <span>\(\bar b\left( s \right)\)</span> in the element multiplied by qsource(s) to obtain q1(s) seems to be contradictory.  In fact, the entire term, <span>\({{\bar b\left( s \right)} \mathord{\left/ {\vphantom {{\bar b\left( s \right)} {B\left( s \right)}}} \right. } {B\left( s \right)}}\)</span>, must be analyzed to determine the effect of qsource(s) on q1(s).  In essence, the appearance of <span>\(\bar b\left( s \right)\)</span> removes the effects of the layers to the right of the source from B(s) leaving only the influence of the layers to the left of the source.  The form displayed by Equation is, however, extremely convenient because the terms in the heat source transmission matrix have the same denominators, and thus roots, as the terms in the temperature transmission matrix.  Thus, the same roots that are calculated for the CTFs can be used for the QTFs, saving a considerable amount of computer time during the calculation of the transfer functions.
-
-Once Equation is inverted from the Laplace domain back into the time domain, the combined CTF–QTF solution takes the following form:
-
-<div>$${q''_{i,t}} = \sum\limits_{m = 1}^M {{X_m}{T_{i,t - m + 1}}}  - \sum\limits_{m = 1}^M {{Y_m}{T_{o,t - m + 1}}}  + \sum\limits_{m = 1}^k {{F_m}{{q''}_{i,t - m}}}  + \sum\limits_{m = 1}^M {{W_m}{q_{source,t - m + 1}}} $$</div>
-
-This relation is identical to Equation except for the presence of the QTF series that takes the heat source or sink into account.
-
-#### State Space Formulation
-
-The two-node example introduced by Seem (1987) can be utilized to examine the extension of the state space method to include heat sources or sinks.  Figure 270 shows the simple two node network with a heat source added at node 1.
-
-The nodal equations for the finite difference network shown in Figure 270 are:
-
-<div>$$C\frac{{d{T_1}}}{{dt}} = hA\left( {{T_o} - {T_1}} \right) + \frac{{{T_2} - {T_1}}}{R} + {q_{source}}A$$</div>
-
-<div>$$C\frac{{d{T_2}}}{{dt}} = hA\left( {{T_i} - {T_2}} \right) + \frac{{{T_1} - {T_2}}}{R}$$</div>
-
-<div>$${q''_i} = h\left( {{T_i} - {T_2}} \right)$$</div>
-
-<div>$${q''_o} = h\left( {{T_1} - {T_o}} \right)$$</div>
-
-![](media/image6034.svg.png)
-
-Figure 270.  Two Node State Space Example with a Heat Source
-
-In obtaining the matrix equivalent for this set of equations, it should be noted that the source term is not a constant but rather an input that varies with time.  Thus, it must be grouped with the environmental temperatures as inputs.  The resulting matrix equations take the following form:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{\frac{{d{T_1}}}{{dt}}}\\ {\frac{{d{T_2}}}{{dt}}}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}{\frac{{ - 1}}{{RC}} - \frac{{hA}}{C}}&{\frac{1}{{RC}}}\\ {\frac{1}{{RC}}}&{\frac{{ - 1}}{{RC}} - \frac{{hA}}{C}}\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ {{T_2}}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}{\frac{{hA}}{C}}&0&{\frac{A}{C}}\\0&{\frac{{hA}}{C}}&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\\ {{q_{source}}}\end{array}} \right]$$</div>
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{{q''}_1}}\\ {{{q''}_2}}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}0&{ - h}\\h&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ {{T_2}}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0&h&0\\ { - h}&0&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\\ {{q_{source}}}\end{array}} \right]$$</div>
-
-Equation appears to suggest that the source term has no direct effect on the heat flux at either side of the element because its coefficients are zero.  This is not the case.  Equation only relates variables that have a direct influence on heat flux.  So, while Ti has no direct influence on<span>\({q''_o}\)</span>, it does have an indirect influence through the nodal network.  The same would hold for the influence of qsource.
-
-If this analysis is extended to a finite difference network with n nodes, the corresponding matrix equations can be shown to be:
-
-<div>$$\frac{{d\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right]}}{{dt}} = \left[ A \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right] + \left[ B \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\\ {{q_{source}}}\end{array}} \right]$$</div>
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{{q''}_i}}\\ {{{q''}_o}}\end{array}} \right] = \left[ C \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right] + \left[ D \right]\left[ {\begin{array}{*{20}{c}}{{T_o}}\\ {{T_i}}\\ {{q_{source}}}\end{array}} \right]$$</div>
-
-The influence of the heat source is also confirmed by the final solution form, which is identical to the Laplace transform result shown in Equation .  As with the Laplace solution method, the state space method results in a set of QTFs that relate the heat source at the current time step and several previous time steps to the current heat flux at the surface of the element.
-
-Other similarities between the two solution methods are evident.  It is interesting to note that as with the Laplace method there is no alteration of the CTFs calculated by the state space method.  Thus, the principle of superposition is still valid.  Furthermore, the introduction of the source term did not substantially increase the computing effort required to calculate the additional transfer functions.  In the Laplace method, this was shown by the common roots, B(s), shared by both the CTFs and the QTFs.  In the state space method, it can be noted that the A matrices in Equations and are identical.  Since the state space method requires the inversion and the exponentiation of the A matrix only, the additional QTF terms will not require a substantial amount of additional computing time for their calculation.
-
-#### Determination of Internal Temperatures
-
-One aspect of low temperature radiant systems that has not been addressed to this point is the appropriateness of specifying the effect of the system on slab response via a heat source term.  For a heating system that employs electrical resistance heating, the use of a heat source as the input variable is logical.  The heat produced by such a system can easily be related to the current passing through the heating wire.  However, for a hydronic heating or cooling system, the known quantity is not heat but rather the temperature of the water being sent to the building element.
-
-The use of a temperature to simulate the presence of a heating or cooling system presents one major obstacle.  When fluid is not being circulated, there is no readily available temperature value available for use as an input variable.
-
-In a hydronic system, a link between the fluid temperature being sent to the slab and the heat delivered to the slab exist.  The most effective way of relating these two variables is to consider the slab to be a heat exchanger.  Using heat exchanger relationships, an equation could then be formulated to obtain the heat delivered to the slab based on the inlet fluid temperature.
-
-Most heat exchangers are used to thermally link two fluids.  In the case of a hydronic radiant system, there is only one fluid and a stationary solid.  Presumably, if the inlet fluid temperature, the system geometry, and the solid temperature are known, then the outlet temperature and thus the heat transfer to the building element can be computed.  This leads to an interesting question:  what is the solid temperature?
-
-By definition, for one dimensional conduction heat transfer, the solid temperature is the temperature of the building element at the depth where the hydronic loop is located.  Typically, this temperature is not known because it is not needed.  The goal of both methods of calculating CTFs was the elimination of internal temperatures that were not needed for the simulation.  For a hydronic system, it is necessary to extract this information to solve for the heat source term.  Two methods of accomplishing this are described below.
-
-Returning to the two layer example shown in Figure 269, it can be shown that the final solution form in the time domain for the slab with a source at the interface between the two layers is:
-
-<div>$${q''_{1,t}} = \sum\limits_{m = 1}^M {{X_{k,m}}{T_{1,t - m + 1}}}  - \sum\limits_{m = 1}^M {{Y_{k,m}}{T_{3,t - m + 1}}}  + \sum\limits_{m = 1}^k {{F_m}{{q''}_{1,t - m}}}  + \sum\limits_{m = 1}^M {{W_m}{q_{source,t - m + 1}}} $$</div>
-
-A similar equation could be written for the response of the first layer in absence of any source term and is given by:
-
-<div>$${q''_{1,t}} = \sum\limits_{m = 1}^M {{x_{k,m}}{T_{1,t - m + 1}}}  - \sum\limits_{m = 1}^M {{y_{k,m}}{T_{2,t - m + 1}}}  + \sum\limits_{m = 1}^k {{f_m}{{q''}_{1,t - m}}} $$</div>
-
-While the current temperature at the interface is not known, presumably the previous values of this parameter will be known.  In addition, the temperatures and the flux histories at surface 1 are also know.  The unknowns in Equation are the current heat flux at surface 1 and the temperature at surface 2.  However, Equation does define the current value of the heat flux at surface 1 based on temperature, heat flux, and heat source histories.  Thus, if this value is used in Equation , the only remaining unknown in this equation is the current temperature at surface 2, the surface where the heat source or sink is present.  Rearranging Equation provides an equation from which the temperature at the source location may be calculated:
-
-<div>$${T_{2,t}} = \sum\limits_{m = 1}^M {{{\bar X}_{k,m}}{T_{1,t - m + 1}}}  - \sum\limits_{m = 1}^{M - 1} {{{\bar Y}_{k,m}}{T_{2,t - m}}}  + \sum\limits_{m = 1}^{k + 1} {{{\bar F}_m}{{q''}_{1,t - m + 1}}} $$</div>
-
-where the new coefficients are obtained from the standard conduction transfer functions for the first layer via the following equations:
-
-<div>$${\bar X_{k,m}} = \frac{{{x_{k,m}}}}{{{y_1}}}\left( {m = 1, \cdots ,M} \right)$$</div>
-
-<div>$${\bar Y_{k,m}} = \frac{{{y_{k,m + 1}}}}{{{y_1}}}\left( {m = 1, \cdots ,M - 1} \right)$$</div>
-
-<div>$${\bar F_1} = \frac{1}{{{y_1}}}$$</div>
-
-<div>$${\bar F_m} = \frac{{{f_{m - 1}}}}{{{y_1}}}\left( {m = 2, \cdots ,k + 1} \right)$$</div>
-
-This system for backing out an internal temperature through the use of a second, rearranged CTF equation is valid regardless of whether the Laplace transform or state space method is utilized to calculate the CTFs and QTFs.  The state space method, however, offers a more direct method of obtaining an internal temperature through its definition as an additional output variable.
-
-Consider again the state space example shown in Figure 270.  Two output variables were defined for this example: <span>\({q''_i}\)</span> and <span>\({q''_o}\)</span>.  The temperature of the node where the source is present can also be defined as an output variable through the identity equation:
-
-<div>$${T_1} = {T_1}$$</div>
-
-When this equation for T1 is added to Equation , the resulting output matrix equation for the heat flux at both surfaces and the internal temperature is:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{{q''}_i}}\\ {{{q''}_o}}\\ {{T_1}}\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}0&{ - h}\\h&0\\1&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ {{T_2}}\end{array}} \right] + \left[ {\begin{array}{*{20}{c}}0&h&0\\ { - h}&0&0\\0&0&0\end{array}} \right]\left[ {\begin{array}{*{20}{c}}{{T_i}}\\ {{T_o}}\\ {{q_{source}}}\end{array}} \right]$$</div>
-
-The only difference between this relation and Equation is the presence of T1 on both the right and left hand side of the equation.  The dual role of T1 as a state variable and an output parameter may seem to contradict the goal of the state space method of eliminating the state variables.  However, due to the flexibility of the formulation, nodal temperatures can be extracted in the same manner that any other output quantity would be obtained.  For an element with n layers, Equation becomes:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{{{q''}_i}}\\ {{{q''}_o}}\\ {{T_s}}\end{array}} \right] = \left[ C \right]\left[ {\begin{array}{*{20}{c}}{{T_1}}\\ \vdots \\ {{T_n}}\end{array}} \right] + \left[ D \right]\left[ {\begin{array}{*{20}{c}}{{T_i}}\\ {{T_o}}\\ {{q_{source}}}\end{array}} \right]$$</div>
-
-where Ts is the temperature of the node where the heat source or sink is present.  The transfer function equation for the calculation of Ts that results from Equation is identical in form to Equation :
-
-<div>$${T_{s,t}} = \sum\limits_{m = 1}^M {{x_{k,m}}{T_{i,t - m + 1}}}  - \sum\limits_{m = 1}^M {{y_{k,m}}{T_{o,t - m + 1}}}  + \sum\limits_{m = 1}^k {{f_m}{T_{s,t - m}}}  + \sum\limits_{m = 1}^M {{w_m}{q_{source,t - m + 1}}} $$</div>
-
-Instead of the flux at either side of the element characterized as a function of temperature, flux, and source history terms, the temperature at the source location is related to source and temperature histories including histories of Ts.  The validity of these internal temperature calculation methods as well as heat source transfer functions in general will be discussed in the next chapter.
-
-#### Low Temperature Radiant System Controls
-
-The use of this equation allows the low temperature radiant system to be handled like any other surface within the heat balance framework.  Heat balances at the inside and outside surfaces take on the same form as other surfaces, and the participation of the radiant system in the radiation balance within the space and thermal comfort models is automatically included.  Thus, the radiant system model is fully integrated into the heat balance, and any improvements that are made in areas such as convection coefficients, shading models, etc. are immediately available to the radiant system as part of the overall heat balance solution.
-
-Once the transient nature of the system is accounted for, one must then turn to the next difficult issue: controls.  Controls are problematic for almost any simulation program.  The problem is not whether something can be simulated because typically a simulation program offers the ability to experiment with many different control strategies.  Rather, the problem is typically the diversity of controls that are implemented and keeping the controls that can be simulated up to date.  EnergyPlus offers two different control schemes: variable flow (ZoneHVAC:LowTemperatureRadiant:VariableFlow) and variable temperature (ZoneHVAC:LowTemperatureRadiant:ConstantFlow).  The control strategies are different enough that they were developed as separate system types.  More details of the controls are described below.
-
-The controls for variable flow low temperature radiant systems within EnergyPlus are fairly simple though there is some flexibility through the use of schedules.  The program user is allowed to define a setpoint temperature as well as a throttling range through which the system varies the flow rate of water (or current) to the system from zero to the user defined maximum flow rate.  The flow rate is varied linearly with the flow reaching 50% of the maximum when the controlling temperature reaches the setpoint temperature.  Setpoint temperatures can be varied on an hourly basis throughout the year if desired.  The controlling temperature can be the mean air temperature, the mean radiant temperature, or the operative temperature of the zone, and this choice is also left to the user’s discretion.  (Operative temperature for radiant system controls is the average of MAT and MRT.)  Since flow rate is varied, there is no explicit control on the inlet water temperature or mixing to achieve some inlet water temperature in a hydronic system.  However, the user does have the ability to specify on an hourly basis through a schedule the temperature of the water that would be supplied to the radiant system.
-
-Graphical descriptions of the controls for the low temperature radiant system model in EnergyPlus are shown in Figure 271 for a hydronic system.  In a system that uses electric resistance heating, the power or heat addition to the system varies in a manner similar to mass flow rate variation shown in Figure 271.
-
-In the constant flow-variable temperature systems, the controls are also considered piecewise linear functions, but in this case the user selects both the control temperatures and the water temperatures via schedules.  This offers greater flexibility for defining how the radiant system operates though it may not model every situation.  Figure 272 shows how the “desired� inlet water temperature is controlled based on user schedules.  The user has the ability to specify the high and low water and control temperature schedules for heating and cooling (separately; a total of eight temperature schedules).  Note that this inlet temperature is a “desired� inlet temperature in that there is no guarantee that the system will provide water to the system at that temperature.  The model includes a local loop that attempts to meet this demand temperature through mixing and recirculation.
-
-![](media/image6053.png)
-
-Figure 271.  Variable Flow Low Temperature Radiant System Controls
-
-![](media/image6054.png)
-
-Figure 272.  Variable Temperature Low Temperature Radiant System Controls
-
-The constant flow (variable temperature) low temperature radiant system model is actually a combination of mixing valves, a pump (constant speed, but the maximum flow can be modified by a schedule), and the radiant system (surface, panel, or group of surfaces/panels).  This is connected to the main loop through the standard inlet connections as shown in Figure 273.  The system controls determine the desired inlet temperature and system flow rate while loop controls determine the flow rate and temperature of the loop.  Note that pump heat also factors into the model through a simple constant speed pump model and user input.
-
-There are four possible conditions (separate for heating and cooling).  First, if the loop has adequate temperature and flow to meet system requests, then the model sets the radiant system inlet temperature and controls to the desired values based on the controls and simulates.  This is the best condition and recirculation and bypass amounts are adjusted accordingly based on radiant system outlet temperatures.  Second, if the loop temperature is adequate but the loop flow rate is less than the radiant system flow rate, we may or may not be able to meet the desired inlet temperature since recirculation might lower the temperature below the desired temperature.  In this second case, the model first simulates the radiant system with the desired conditions and then resimulates it to solve for the actual inlet temperature (see later in this section) if it cannot achieve the desired inlet temperature.  Third, if the loop flow is greater than the radiant flow but the temperature of the loop is not adequate, then there is no amount of mixing that will solve this problem.  All of the radiant flow comes from the loop and the loop temperature (after pump heat addition) becomes the radiant system inlet regardless of the temperature controls.  Finally, if both the temperature and the flow of the loop are inadequate, then the model simply solves for the actual radiant system inlet temperature and does not try to meet the controls (merely tries to get as close as physically possible given the loop conditions).
-
-![](media/image6055.png)
-
-Figure 273.  Variable Temperature Low Temperature Radiant System Component Details
-
-One remaining challenge is the merging of the low temperature radiant system model with an integrated building simulation program.  In the past, most simulation programs have simulated the building envelope, the space conditioning systems, and the central plant equipment in three separate steps.  While this had some advantages and was partly due to a lack of computing capacity, the large drawback for this arrangement is that there is no feedback from the space conditioning system or central plant response to the building conditions.  Thus, if the system or plant was undersized, it was reported as an “unmet load� and does not affect the temperatures experienced within the building.  IBLAST, a predecessor (Taylor 1991) to EnergyPlus, resolved this issue by integrating all three major components of a building simulation and thus allowing feedback between the equipment and the building envelope.
-
-This integration was not a trivial task and required that the systems be simulated at shorter time steps in some cases to maintain solution stability.  In essence, the system simulation will shorten its time step whenever it senses that conditions are changing too rapidly.  While this is effective in maintaining solution stability, it can present problems for a radiant system.  The radiant system has either a direct or an indirect impact on the surfaces within a building.  So, it must be simulated with the building envelope.  Yet, it is also a space conditioning system that must act on the space like any other system and thus must also be simulated at the system time step, which can be less than the building time step and can also vary within EnergyPlus.
-
-This issue was handled using a multi-step approach.  In EnergyPlus, the heat balance is always simulated first.  When this happens, the radiant system is temporarily shut-off to find how the building would respond if there was no heat source/sink.  Then, as the system and plant are simulated at multiple shorter time steps, the radiant system is allowed to operate per the controls specified by the user.  Flow rate is allowed to vary at each system time step, and the radiant system model is simulated at each time step as if the current flow rate was being used throughout the entire zone time step.  This means that each time the heat source/sink in the radiant system is varied during the system simulation the zone heat balance must be recomputed to see what the reaction of the rest of the zone is to this change in the conditions of one (or more) of the surfaces.
-
-In reality, this is not physically correct because each change in the flow rate throughout the system simulation will have an impact on the system time steps remaining before the heat balance is simulated during the next zone time step.  Yet, other approaches to solving the mismatch between the system and the zone response of radiant systems are not feasible.  One could force the system to run at the same time step as the zone, but this could result in instabilities in other types of systems that might be present in the simulation.  On the other hand, one could try to force the zone to run at the shorter time steps of the system, but this could lead to instability within the heat balance due to limits on the precision of the conduction transfer function coefficients.
-
-Despite the fact that the simulation algorithm described above may either over- or under-predict system response dependent on how the system has been controlled in previous system time steps, it is reasonable to expect that the effect of these variations will balance out over time even though it might lead to slightly inaccurate results at any particular system time step.  The long-term approach is also in view in the final simulation step at each zone time step.  After the system has simulated through enough system time steps to equal a zone time step, the radiant system will rerun the heat balance using the average heat source/sink over all of the system time steps during the past zone time step.  This maintains the conservation of energy within the heat balance simulation over the zone time steps and defines more appropriate temperature and flux histories at each surface that are critical to the success of a conduction transfer function based solution.  A graphical picture of this somewhat complex multiple step simulation is shown in the figure below.
-
-![](media/image6056.png)
-
-Figure 274.  Resolution of Radiant System Response at Varying Time Steps
-
-#### Heat Exchanger Formulation for Hydronic Systems
-
-As has been mentioned previously, the actual heat transferred between the building element and the hydronic loop is related to the temperature of the building element at the source location as well as the water system inlet and outlet temperatures.  In EnergyPlus, it is assumed that the inlet temperature to the slab (defined by a user schedule and the plant simulation) and the mass flow rate (determined by the control algorithm) are known and that the remaining parameters must be calculated.  However, the heat balance equations require the heat transferred to the building element from the water loop in order to calculate the heat transferred from the element to the building environment.
-
-Even though systems defined by this model can vary somewhat, the same characteristic link between the system variables exist.  For modeling purposes, the overall water/slab system can be thought of as a heat exchanger.  While in principle there are two alternative heat exchanger methodologies, it is more convenient to use the effectiveness-NTU method in this case.
-
-Several assumptions will be incorporated into the heat exchanger analysis.  It is assumed that the building element that contains the hydronic loop is stationary and that its temperature along the length of the tubing is constant.  The latter part of this assumption stems from assumptions made in both the one and two dimensional heat source transfer function derivations.  In either case, the source was added at a single node that was characterized by a single temperature.  For consistency, this assumption must be made again in the heat exchanger analysis.  Another assumption for the current EnergyPlus model is that the fluid in the tubing is water.  Additionally, it is assumed that the thermal properties of the water do not vary significantly over the length of the tubing and that the water flows at a constant flow rate.  Finally, the temperature at the inside surface of the water tubing is assumed to be equal to the temperature at the source location.  In other words, it is assumed that the water tubing itself has no appreciable effect on the heat transfer process being modeled.
-
-Using these assumptions and the effectiveness-NTU heat exchanger algorithm, several equations can be defined which establish the relationship between the heat source and the water temperatures.  First, a heat balance on the water loop results in:
-
-<div>$$q = {\left( {\dot m{c_p}} \right)_{water}}\left( {{T_{wi}} - {T_{wo}}} \right)$$</div>
-
-where q is the energy transferred between the water loop and the building element, <span>\(\dot m\)</span> is the mass flow rate of the water, cp is the specific heat of the water, Twi is the inlet water temperature, and Two is the outlet water temperature.
-
-The maximum amount of heat transfer that is possible according to the Second Law of Thermodynamics is:
-
-<div>$${q_{\max }} = {\left( {\dot m{c_p}} \right)_{water}}\left( {{T_{wi}} - {T_s}} \right)$$</div>
-
-where qmax is the maximum amount of energy transfer that is possible and Ts is the temperature at the source location.
-
-The effectiveness of the heat exchanger, e, is defined as the ratio of the actual energy transfer to the maximum possible, or:
-
-<div>$$\varepsilon  \equiv \frac{q}{{{q_{\max }}}}$$</div>
-
-For a heat exchanger where one fluid is stationary, the effectiveness can be related to NTU, the number of transfer units, by the following equation (Incropera and DeWitt 1985):
-
-<div>$$\varepsilon  = 1 - {e^{ - NTU}}$$</div>
-
-where NTU is defined by:
-
-<div>$$NTU \equiv \frac{{UA}}{{{{\left( {\dot m{c_p}} \right)}_{water}}}}$$</div>
-
-Since the water tubes were assumed to have no effect on the heat transfer process, the only term present in the overall heat transfer coefficient, UA, is a convection term.  Thus, the equation for UA is:
-
-<div>$$UA = h\left( {\pi DL} \right)$$</div>
-
-where h is the convection coefficient, D is the interior tube diameter, and L is the total length of the tube.
-
-The convection coefficient can be obtained from internal flow correlations that relate the Nusselt dimensionless number to other flow properties.  For laminar flow in a tube of constant surface temperature, the Nusselt number is defined by:
-
-<div>$$N{u_D} = \frac{{hD}}{k} = 3.66$$</div>
-
-where k is the thermal conductivity of the water.
-
-For turbulent internal flow, the Colburn equation can be used to define the Nusselt number:
-
-<div>$$N{u_D} = \frac{{hD}}{k} = 0.023{\mathop{\rm Re}\nolimits}_D^{{4 \mathord{\left/ {\vphantom {4 5}} \right. } 5}}{\Pr ^{{1 \mathord{\left/ {\vphantom {1 3}} \right. } 3}}}$$</div>
-
-where Pr is the Prandtl number of water and ReD is the Reynolds number which is defined by:
-
-<div>$${{\mathop{\rm Re}\nolimits}_D} = \frac{{4\dot m}}{{\pi \mu D}}$$</div>
-
-The parameter m is the absolute viscosity of water.  For internal pipe flow, the flow is assumed to be turbulent for ReD ≥ 2300.
-
-Knowledge of the flow conditions allows Equations through to be calculated.  This essentially eliminates e as an unknown in Equation .  The controls and the plant define the water mass flow rate and the inlet water temperature, leaving two equations (Equations and ) and three unknowns.  The third equation that can be used in conjunction with Equations and is Equation , which is the CTF/QTF equation for the temperature at the source location.
-
-Knowing the inlet water temperature and water mass flow rate, the calculation procedure is somewhat involved and requires, in addition to Equations , , and , the use of a modified form of Equation .  Equation is the standard conduction transfer function formula for a building element with an embedded source/sink of heat.  In EnergyPlus, the surface flux on the left hand side of the equation is replaced with a surface heat balance:
-
-<div>$$\left[ {\begin{array}{*{20}{c}}{Surface}\\ {Heat}\\ {Balance}\end{array}} \right] = \sum\limits_{m = 1}^M {{X_{k,m}}{T_{1,t - m + 1}}}  - \sum\limits_{m = 1}^M {{Y_{k,m}}{T_{3,t - m + 1}}}  + \sum\limits_{m = 1}^k {{F_m}{{q''}_{1,t - m}}}  + \sum\limits_{m = 1}^M {{W_m}{q_{source,t - m + 1}}} $$</div>
-
-The surface heat balance includes terms for incident solar energy, radiation heat transfer from internal heat sources such as lights and electrical equipment, radiation between surfaces using Hottel’s Gray Interchange concept, and convection to the surrounding air.  The presence of the surface temperature in the heat balance does not pose any problems since Equation will be rearranged to solve for this temperature.  Since the radiation heat balance is dependent on conditions at the other surfaces, an iteration loop is required to provide a more accurate estimate of the radiative exchange within the building.  This is not the case with the mean air temperature.  An assumption of the heat balance is that the mean temperature of the surrounding air is equal to the final air temperature of the previous time step.  Using this estimate in the heat balance avoids a second iterative loop around the radiative iteration loop.
-
-Thus, the terms of the heat balance on the left hand side of the equation have been set with the only unknown quantity being Ti, the inside surface temperature at the current time step.  On the right hand side of Equation , most of the terms are already defined since they depend on known values from previous time steps (temperature, flux, and source histories).  The only terms which are not defined are the inside surface temperature (Ti), outside surface temperature (To), and internal heat source/sink (qsource) of the current time step.
-
-The outside surface temperature will depend on the type of environment to which it is exposed.  For example, if the surface is a slab on grade floor, the outside surface temperature is defined as ground temperature and does not require an outside surface heat balance.  If the element is an interior surface which has both surfaces exposed to the same air space, the outside surface temperature is redefined to be equal to the inside surface temperature.  In cases where the outside surface temperature is not simply defined such as a surface exposed to the exterior environment, a heat balance similar to Equation is required to define the outside surface temperature.  However, to again avoid iteration, the heat balance equation for the outside surface assumes that conditions at the inside surface were the same as the previous time step.  In most cases, since the influence of the current inside surface temperature on the outside surface temperature is very small, this is a valid assumption.  In cases were the inside surface temperature has a significant effect, an approximate inside surface heat balance which defines the inside surface temperature is used.  This approximate inside balance uses mean air and radiant temperatures from the previous time step.
-
-At this point in the simulation algorithm then, all of the terms in Equation have been defined except the value at the current time step of the inside surface temperature and the heat source/sink.  Thus, Equation can be rewritten in a simpler form:
-
-<div>$${T_{i,t}} = {C_1} + {C_2}{q_{source,t}}$$</div>
-
-where the variable C1 includes surface heat balance and past history terms as well as the influence of the current outside temperature.  The term C2 will depend on the heat source transfer function term and the coefficients of terms linked directly to Ti,t.
-
-Equation , which was the CTF/QTF equation for the temperature at the source location, can be simplified in a similar manner.  Grouping the temperature and source history terms which are known quantities together with the effect of the outside surface temperature which is defined as described above, the original equation
-
-<div>$${T_{s,t}} = \sum\limits_{m = 1}^M {{x_{k,m}}{T_{i,t - m + 1}}}  - \sum\limits_{m = 1}^M {{y_{k,m}}{T_{o,t - m + 1}}}  + \sum\limits_{m = 1}^k {{f_m}{T_{s,t - m}}}  + \sum\limits_{m = 1}^M {{w_m}{q_{source,t - m + 1}}} $$</div>
-
-can be reduced to:
-
-<div>$${T_s} = {C_3} + {C_4}{q_{source,t}} + {C_5}{T_{i,t}}$$</div>
-
-where C3 includes all of the history terms and the effect of the current outside temperature, C4 is the heat source transfer function for the current time step, and C5 is the conduction transfer function for the inside surface temperature at the current time step.
-
-Substituting Equation into Equation and noting that qsource,t is the same quantity as q in Equations and results in:
-
-<div>$${T_s} = {C_3} + {C_4}q + {C_5}\left( {{C_1} + {C_2}q} \right)$$</div>
-
-When this equation is combined with Equation , the heat source, which results from a known water inlet temperature, can be shown to be:
-
-<div>$$q = \frac{{{T_{wi}} - {C_3} - {C_1}{C_5}}}{{\frac{1}{{\varepsilon {{\left( {\dot m{c_p}} \right)}_{water}}}} + {C_4} + {C_2}{C_5}}}$$</div>
-
-With both q and Twi known, it is a trivial matter to calculate Two and Ts from Equations and , respectively.  Even though the coefficients in Equation are fairly complex, the final equation relating the heat source directly to inlet water temperature is compact and does not require any iteration.  As with flux control, once the heat source/sink is defined, the inside surface heat balance can be performed to determine the surface temperatures.
-
-It should be noted that Equations through are a slight simplification of the actual implementation in EnergyPlus.  The development shown above follows the heat balance conventions that assume previous values of the inside temperature to calculate the outside temperature.  This, in reality, is not necessary and since the radiant system can be significantly influenced by the delay that such an assumption might cause, the initial implementation of radiant systems in EnergyPlus used a development (shown below) that does not lag either the inside or the outside surface temperature.  In effect, we can establish three basic equations for the temperature at the inside and outside surface as well as at the location of the heat source/sink:
-
-<div>$${T_{inside}} = {C_a} + {C_b}{T_{outside}} + {C_C}q''$$</div>
-
-<div>$${T_{outside}} = {C_d} + {C_e}{T_{inside}} + {C_f}q''$$</div>
-
-<div>$${T_{source}} = {C_g} + {C_h}q'' + {C_i}{T_{inside}} + {C_j}{T_{outside}}$$</div>
-
-where:  T<sub>inside</sub> is the temperature at the inside surface
-
-T<sub>outside</sub> is the temperature at the outside surface
-
-T<sub>source</sub> is the temperature within the radiant system at the location of the source/sink
-
-C<sub>a</sub> is all of the other terms in the inside heat balance (solar, LW exchange, conduction history terms, etc.)
-
-C<sub>b</sub> is the current cross CTF term
-
-C<sub>c</sub> is the QTF inside term for the current heat source/sink
-
-C<sub>d</sub> is all of the other terms in the outside heat balance (solar, LW exchange, conduction history terms, etc.)
-
-C<sub>e</sub> is the current cross CTF term (should be equal to Cb)
-
-C<sub>f</sub> is the QTF outside term for the current heat source/sink
-
-C<sub>g</sub> is the summation of all temperature and source history terms at the source/sink location
-
-C<sub>h</sub> is the QTF term at the source/sink location for the current heat source/sink
-
-C<sub>i</sub> is the CTF inside term for the current inside surface temperature
-
-C<sub>j</sub> is the CTF outside term for the current outside surface temperature
-
-Equations and above can be solved to remove the other surface temperature.  Substituting the new equations for T<sub>inside</sub> and T<sub>outside</sub> as a function of C and q" into the equation for Tsource and simplifying results in the following equation:
-
-<div>$${T_{source}} = {C_k} + {C_l}q''$$</div>
-
-where:         <span>\({C_k} = {C_g} + \frac{{{C_i}\left( {{C_a} + {C_b}{C_d}} \right) + {C_j}\left( {{C_d} + {C_e}{C_a}} \right)}}{{1 - {C_e}{C_b}}}\)</span>
-
-<div>$${C_l} = {C_h} + \frac{{{C_i}\left( {{C_c} + {C_b}{C_f}} \right) + {C_j}\left( {{C_f} + {C_e}{C_c}} \right)}}{{1 - {C_e}{C_b}}}$$</div>
-
-Combining this with heat exchanger analysis as shown above, we eventually arrive at the following equation to relate the flux to the slab to the water inlet temperature and mass flow rate:
-
-<div>$$q'' = \frac{{{T_{water,in}} - {C_k}}}{{\frac{{{C_l}}}{A} + \frac{1}{{\varepsilon {{\left( {\dot m{c_p}} \right)}_{water}}}}}}$$</div>
-
-which includes all of the inside and outside heat balance terms (“hidden� in the C<sub>k</sub> and C<sub>l</sub> coefficients).  Once the flux to the slab is known, the remaining terms of interest (outlet water temperature, inside and outside surface temperatures, etc.) can be calculated using the relatively simpler equations shown above.
-
-Note that the above development is valid for both the hydronic (variable flow) low temperature radiant system and for constant flow (variable temperature) low temperature radiant systems where the inlet temperature is known (based on controls).  However, when due to loop conditions and the presence of recirculation, it is not possible to know the inlet temperature to the radiant system without simulating it, we must either iterate or perform more mathematics to arrive at the inlet temperature.  The implementation in EnergyPlus chose to avoid iteration and solved for the inlet temperature as shown in the next paragraphs.
-
-The previous equation combines with the following equation which is valid for an surface in the current radiant system:
-
-<div>$${{\rm{q}}_{\rm{j}}}{\rm{  =  }}{{\rm{\dot m}}_{\rm{j}}}{{\rm{c}}_{\rm{p}}}{\rm{(}}{{\rm{T}}_{{\rm{water,in}}}}{\rm{  -  }}{{\rm{T}}_{{\rm{water,out,j}}}}{\rm{)}}$$</div>
-
-where q<sub>j</sub> is the heat transfer to the jth surface in the radiant system, m<sub>j</sub> is the mass flow rate only to this surface, and T<sub>water,out,j</sub> is the outlet temperature for the jth surface.  Combining the previous two equations results in:
-
-<div>$${\rm{(}}{{\rm{T}}_{{\rm{water,in}}}}{\rm{  -  }}{{\rm{T}}_{{\rm{water,out,j}}}}{\rm{)}} = \frac{{{\varepsilon_j}\left( {{{\rm{T}}_{{\rm{water,in}}}} - {C_{k,j}}} \right)}}{{1 + \frac{{{\varepsilon_j}{{\dot m}_j}{c_p}{C_{l,j}}}}{A}}}$$</div>
-
-If for each surface in the radiant system, we let:
-
-<div>$${{\rm{C}}_{m,j}} = \frac{{{\varepsilon_j}}}{{1 + \frac{{{\varepsilon_j}{{\dot m}_j}{c_p}{C_{l,j}}}}{A}}}$$</div>
-
-then the previous equations because the slightly less complex:
-
-<div>$${\rm{(}}{{\rm{T}}_{{\rm{water,in}}}}{\rm{  -  }}{{\rm{T}}_{{\rm{water,out,j}}}}{\rm{)}} = {C_{m,j}}\left( {{{\rm{T}}_{{\rm{water,in}}}} - {C_{k,j}}} \right)$$</div>
-
-Rearranging to obtain the outlet temperature for the jth surface:
-
-<div>$${{\rm{T}}_{{\rm{water,out,j}}}} = \left( {1 - {C_{m,j}}} \right){{\rm{T}}_{{\rm{water,in}}}} + {C_{m,j}}{C_{k,j}}$$</div>
-
-The overall outlet temperature from the radiant system is just a simple mixing of all of the surface outlet temperatures based on flow fraction and results in T<sub>water,out</sub>.
-
-An energy balance on the mixing valve-pump group results in the following equation that relates the radiant system inlet temperature (T<sub>water,in</sub>) to the loop inlet water temperature (T<sub>loop,in</sub>), the radiant system outlet temperature (T<sub>water,out</sub>), and the pump heat addition:
-
-<div>$${{\rm{T}}_{{\rm{water,in}}}} = \frac{{{{\dot m}_{loop}}}}{{{{\dot m}_{system}}}}{{\rm{T}}_{{\rm{loop,in}}}} + \frac{{{{\dot m}_{recirc}}}}{{{{\dot m}_{system}}}}{{\rm{T}}_{{\rm{water,out}}}} + \frac{{PumpHeat}}{{{{\dot m}_{system}}{c_p}}}$$</div>
-
-Plugging in the definition of T<sub>water,out</sub> based on the summation of T<sub>water,out,j</sub> equations results in:
-
-<div>$${{\rm{T}}_{{\rm{water,in}}}} = \frac{{LoopTerm + {\mathop{\rm Re}\nolimits} circTerm}}{{TwiCoeff}}$$</div>
-
-where:
-
-<div>$${\rm{L}}oopTerm = \frac{{{{\dot m}_{loop}}}}{{{{\dot m}_{system}}}}{{\rm{T}}_{{\rm{loop,in}}}} + \frac{{PumpHeat}}{{{{\dot m}_{system}}{c_p}}}$$</div>
-
-<div>$${\mathop{\rm Re}\nolimits} circTerm = \frac{{{{\dot m}_{recirc}}}}{{{{\dot m}_{system}}}}\sum\limits_{\rm{j}} {{\rm{FlowFractio}}{{\rm{n}}_{\rm{j}}}{{\rm{T}}_{{\rm{water,out,j}}}}} $$</div>
-
-<div>$$TwiCoeff = \left( {1 - \frac{{{{\dot m}_{recirc}}}}{{{{\dot m}_{system}}}}} \right)\sum\limits_{\rm{j}} {\left[ {{\rm{FlowFractio}}{{\rm{n}}_{\rm{j}}}\left( {1 - {C_{m,j}}} \right)} \right]} $$</div>
-
-Once the actual water inlet temperature is calculated with this equation, it is then possible to calculate individual outlet temperatures for each surface, the overall outlet temperature, and finally all of the necessary flow and loop quantities.  This procedure avoids iteration but is somewhat complex to follow.  However, this second mathematical process is only needed for select cases of the constant flow radiant system when the inlet temperature is not known explicitly.  With the proper establishment of input data, it can be avoided.
-
-**NOTE:** In some “low-energy� applications, it is possible that during cooling mode the elevated water temperatures may result in a heat source (or net heating) to the radiant system.  To avoid heating the slab when cooling is desired, EnergyPlus performs a temperature limit check.  If heating would result during cooling mode or cooling during heating mode, the model will cut-off the flow rate until the inlet water temperature will produce the proper effect.
-
-### High Temperature Radiant Heater Model
-
-The input object ZoneHVAC:HighTemperatureRadiant provides a model for a high temperature radiant heater that is intended to encapsulate an entire class of heating devices that seek to heat the occupants within a zone by direct radiation.  This encompasses a wide variety of heaters including both gas-fired and electric.  In most cases, the heater appears much like a lamp or a tube that is suspended from the ceiling of a space, and the surface temperatures are high enough that the heaters must be a safe distance away from the occupied portion of the space for safety concerns.
-
-In EnergyPlus, the high temperature radiant heater model allows the user a reasonable amount of flexibility.  Rather than specifying an exact location for the radiant heater(s), the user is allowed to specify the percentage of heat leaving the heater as radiation and then on which surfaces this radiation is incident.  In addition, the user is also allowed the ability to define what fraction of radiation leaving the heater is incident directly on a person within the zone for thermal comfort purposes.  This amount of heat is then used in the thermal comfort models as shown in Equations for Fanger, for Pierce Two-Node and for KSU Two-node. These equations are similar in form to the equation promoted by Fanger (1970).  The input parameters for the high temperature radiant heater model are shown in Figure 275.
-
-<div>$${T_{radiant}} = {\left[ {\left( {T_{MRT}^4} \right) + \left( {\frac{{{Q_{heater \to person}}}}{{\sigma {A_{person}}}}} \right)} \right]^{0.25}}$$</div>
-
-HIGH TEMP RADIANT SYSTEM,! Program keyword for high temp. radiant heaters
-
-  Zone 1 Radiant Heater, ! Zone name
-
-  Radiant Operation,     ! Availability schedule
-
-  SHOP ZONE,             ! Zone name (name of zone system is serving)
-
-  10000,                 ! maximum power input (in Watts)
-
-  GAS,                   ! type of heater (either gas or electric)
-
-  0.85,                  ! combustion efficiency (ignored for elec. heaters)
-
-  0.75,                  ! fraction radiant
-
-  0.05,                  ! fraction latent
-
-  0.05,                  ! fraction lost
-
-  OPERATIVE,             ! temperature control type (MAT, MRT also possible)
-
-  2.0 ,                  ! heating throttling range (in C)
-
-  Heating Setpoints,     ! schedule of heating setpoint temperatures
-
-  0.05,                  ! fraction of radiant energy to people
-
-  Zn001:Flr001, 0.75,    ! surface/fraction of radiant energy incident on it
-
-  Zn001:Wall001, 0.05,   ! surface/fraction of radiant energy incident on it
-
-  Zn001:Wall002, 0.05,   ! surface/fraction of radiant energy incident on it
-
-  Zn001:Wall003, 0.05,   ! surface/fraction of radiant energy incident on it
-
-  Zn001:Wall004, 0.05;   ! surface/fraction of radiant energy incident on it
-
-Figure 275.  Input Description for High Temperature Radiant Heaters
-
-The input for the high temperature radiant heater has two additive relationships that are assumed.  First, the fractions of radiant, convective, latent, and lost heat must sum to unity.  The user is required to enter the fractions radiant, latent, and lost with the remainder assumed to be convective energy.  The fraction latent is added to the latent energy balance and will affect moisture levels within the zone.  The fraction lost is assumed to have no impact on the energy balance of the zone and is assumed to be lost or vented to the exterior environment.
-
-The second additive relationship is within the distribution of the radiant fraction.  This energy is distributed to people and to the surfaces within the zone.  The sum of all of these distribution fractions (the last six lines of input shown in Figure 275) must sum to unity.  Note that each high temperature radiant heater is allowed to distribute energy to up to 20 surfaces and that radiant energy placed on a surface using these distribution fractions is assumed to be completely absorbed.  Thus, the distribution fractions should also take into account any differences in long wavelength absorptivity among the surfaces.
-
-Several things should be noted about the fraction of heat that is radiated directly to people.  This parameter is somewhat sensitive and will have a direct impact on the thermal comfort models.  This is exactly the intent of the high temperature radiant heaters; however, one must use caution when determining this fraction since overestimation of this number might lead to predictions of thermal comfort where in fact it does not exist.  In addition, this fraction of radiant energy to people does not have a direct impact on any of the surface heat balances.  The thermal comfort energy balance is completely separate from and has no bearing on the zone air or the surface heat balances.  Thus, in order to not “lose� this amount of energy from the perspective of the zone air or the surface heat balances, the model assumes that any radiation from the high temperature radiant heater that is incident directly on people is accounted for in the thermal comfort model using Equation but is also assumed to be added to the zone air heat balance via convection from people to the surrounding air.  This guarantees that the people within the space feel the direct radiative effect of the heaters and that this quantity of energy is not “lost� within the heat balance routines.
-
-Many of the control and integration aspects of the high temperature radiant system model in EnergyPlus are very similar to the low temperature radiant system model.  The controls are the same as shown in “Figure 271.  Variable Flow Low Temperature Radiant System Controls� where the amount of heat generated by the radiant heater varies as a function of the difference between the controlling and the setpoint temperatures.  As with the low temperature radiant system, the controlling temperature is allowed to be the mean air, the mean radiant, or the operative temperature, and the setpoint temperature is allowed to vary hourly based on a user defined schedule.  (Operative temperature for radiant system controls is the average of MAT and MRT.)  Also, since the high temperature radiant heater has a direct impact on the surfaces within a zone, the surface heat balances are recalculated to determine an approximate response to the radiation from the heater.  A final “average� heat balance calculation is done after all of the system time steps have been simulated to maintain continuity within the surface heat balances.  The algorithm shown in “Figure 274.  Resolution of Radiant System Response at Varying Time Steps is also used for high temperature radiant heaters.
-
-#### References
-
-Ceylan, H.T. and G.E. Myers.  1980.  Long-time solutions to heat conduction transients with time-dependent inputs.  ASME Journal of Heat Transfer, Volume 102, Number 1, pp. 115-120.
-
-Degiovanni, A.  1988.  Conduction dans un “mur� multicouche avec sources:  extension de la notion de quadripole.  International Journal of Heat and Mass Transfer, Volume 31, Number 3, pp. 553-557.
-
-Fanger, P.O. 1970. Thermal Comfort-Analysis and Applications in Environmental Engineering, Danish Technical Press, Copenhagen.
-
-Hittle, D.C.  1981.  Calculating building heating and cooling loads using the frequency response of multilayered slabs.  Ph.D. Thesis, Department of Mechanical and Industrial Engineering, University of Illinois at Urbana-Champaign and Technical Manuscript E-169, United States Army Construction Engineering Research Laboratory, Champaign, IL.
-
-Hittle, D.C. and R. Bishop.  1983.  An improved root-finding procedure for use in calculating transient heat flow through multilayered slabs.  International Journal of Heat and Mass Transfer, Volume 26, Number 11, pp. 1685-1693.
-
-Hottel, H.C. and A.F. Sarofim. 1967. Radiative Transfer, McGraw-Hill, New York.
-
-Incropera, F.P. and D.P. DeWitt.  1985.  Introduction to Heat Transfer.  New York:  John Wiley & Sons.
-
-Lee, J. and R.K. Strand. 2001. “An Analysis of the Effect of the Building Envelope on Thermal Comfort using the EnergyPlus Program�, submitted for publication in the proceedings of the 2001 ACSA (Association of Collegiate Schools of Architecture) Technology Conference, Austin, TX.
-
-Liesen, R.J. and C.O. Pedersen. 1997. “An Evaluation of Inside Surface Heat Balance Models for Cooling Load Calculations�, ASHRAE Transactions, Volume 103, Part 2.
-
-Maloney, D. 1987. “Development of a radiant heater model and the incorporation of thermal comfort considerations into the BLAST energy analysis program�, M.S. thesis, University of Illinois at Urbana-Champaign, Department of Mechanical and Industrial Engineering.
-
-McClellan, T.M. and C.O. Pedersen. 1997. “Investigation of Outside Heat Balance Models for Use in a Heat Balance Cooling Load Calculation Procedure�, ASHRAE Transactions, Volume 103, Part 2.
-
-Pedersen, C.O., D.E. Fisher, and R.J. Liesen. 1997. “Development of a Heat Balance Procedure for Cooling Loads�, ASHRAE Transactions, Volume 103, Part 2.
-
-Pedersen, C.O., D.E. Fisher, J.D. Spitler, and R.J. Liesen. 1998. Cooling and Heating Load Calculation Principles, ASHRAE.
-
-Seem, J.E.  1987.  Modeling of heat transfer in buildings.  Ph.D. Thesis, University of Wisconsin-Madison.
-
-Strand, R.K., and C.O. Pedersen. 1994. “Analytical verification of heat source transfer functions�, First Joint Conference of International Simulation Societies, Zürich, Switzerland.
-
-Strand, R.K. 1995. “Heat source transfer functions and their application to low temperature radiant heating systems�, Ph.D. dissertation, University of Illinois at Urbana-Champaign, Department of Mechanical and Industrial Engineering.
-
-Strand, R.K. and C.O. Pedersen. 1997. “Implementation of a Radiant Heating and Cooling Model into an Integrated Building Energy Analysis Program�, ASHRAE Transactions, Volume 103, Part 1.
-
-Strand, R.K. and C.O. Pedersen. 2001. “Modularization and Simulation Techniques for Heat Balance Based Energy and Load Calculation Programs: the Experience of the ASHRAE LOADS Toolkit and EnergyPlus�, International Building Performance Simulation Association, Conference Proceedings of Building Simulation 2001, Rio de Janeiro, Brazil.
-
-Taylor, R.D., C.O. Pedersen, D. Fisher, R. Liesen, and L. Lawrie. 1991. “Impact of simultaneous simulation of building and mechanical systems in heat balance based energy analysis programs on system response and control�, International Building Performance Simulation Association, Conference Proceedings of Building Simulation 1991, Nice, France.
-
-Refrigeration Equipment <a name="Refrigeration"></a>
------------------------
-
-### Overview
-
-EnergyPlus can model refrigerated case equipment consisting of a compressor rack, multiple refrigerated cases and walk-in coolers, secondary loop equipment, and  optional heat reclaim air and water heating coils. The refrigerated case equipment models perform four major functions:
-
-n calculate the electric consumption of refrigerated cases and walk-in coolers connected to a compressor rack
-
-n determine the impact of refrigerated cases and walk-in coolers on zone cooling and dehumidification loads (i.e., case credits), including the effects of HVAC duct configuration
-
-n calculate the electric consumption and COP of the compressor rack, and the electric and water (if applicable) consumption related to cooling the compressor rack’s condenser.
-
-n determine the total amount of heat rejected by the compressor rack’s condenser and store this information for use by waste heat recovery models (e.g., using Desuperheater heating coil (object: Coil:Heating:Desuperheater) as an air reheat coil for high humidity control in a supermarket)
-
-The case and walk-in models account for nearly all performance aspects of typical supermarket refrigeration equipment. Refrigerated case and walk-in performance are based on the combined effects of evaporator load, fan operation, lighting, defrost type, and anti-sweat heater operation. Optional air and water heating coils can be modeled to reclaim available waste heat (superheat) from the compressor rack.
-
-The user has two options when describing the balance of the system. Energy used to cool the condenser is simulated in both approaches. The simplest option is to use a compressor rack object, combining the compressors and condenser into a single unit with the performance determined by the heat rejection environment and the total case load. An example schematic of a compressor rack system is shown in Figure 276 below.
-
-A detailed refrigeration system object models compressor and condenser performance separately. The detailed refrigeration system also includes the ability to transfer refrigeration load from one system to another using subcoolers, cascade condensers, and secondary loops. An example schematic of the detailed refrigeration system is shown in Figure 277 below. Subcooler \#2 is shown twice on  Figure 277 because it represents a liquid suction heat exchanger. This type of subcooler uses the cool suction gas to subcool the warmer condensed liquid. Subcoolers \#1 and \#3 on Figure 277 represent mechanical subcoolers. These subcoolers are used to subcool the condensate on a lower-temperature system using the cold liquid refrigerant from a higher temperature system. On this example, only subcoolers \#1 and \#2 would be defined as a part of the refrigeration system. However, subcooler \#3 would place a refrigerating load, similar to the load of a refrigerated case, on the system.
-
-![racksystem\_low](media/image6091.png)
-
-Figure 276. Typical Compressor Rack Equipment Schematic
-
-![DetailedSystem](media/image6092.png)
-
-Figure 277. Typical Detailed Refrigeration System Equipment Schematic
-
-Four classes of secondary refrigeration loops can be modeled:
-
-n a separate water loop is used to remove heat rejected by the condenser,
-
-n a lower-temperature refrigeration system rejects heat to a higher-temperature refrigeration system via a cascade condenser,
-
-n a fluid, such as a brine or glycol solution, is cooled in a secondary evaporator and is then circulated to chill the refrigerated cases and walk-ins, and
-
-n a refrigerant, such as CO<sub>2</sub>, is partially evaporated in the refrigerated cases and walk-ins in a liquid-overfeed circuit, and then condensed in a secondary evaporator.
-
-The first two classes of secondary loops are modeled using Refrigeration:System objects with Refrigeration:Condenser:WaterCooled and Refrigeration:Condenser:Cascade objects, respectively.  Figure 277 shows how cascade condensers and secondary evaporators are treated as a refrigeration load on a primary detailed system. The second two classes are modeled with a Refrigeration:SecondarySystem object described later in this section.
-
-The compressor rack, detailed and secondary refrigeration systems, refrigerated case, and other component models are described below. The optional air and water heating coils are described elsewhere in this document (Ref. objects Coil:Heating:Desuperheater and Coil:WaterHeating:Desuperheater).
-
-### Refrigeration Compressor Racks
-
-The refrigerated case compressor rack object works in conjunction with the refrigerated case and walk-in cooler objects (Refrigeration:Case and Refrigeration:WalkIn) to simulate the performance of a simple supermarket-type refrigeration system. This object (Refrigeration:CompressorRack) models the electric consumption of the rack compressors and the cooling of the compressor rack’s condenser. Heat removed from the refrigerated cases and walk-ins and compressor/condenser fan heat can be rejected either outdoors or to a zone. Compressor rack condenser waste heat can also be reclaimed for use by an optional air heating coil (Ref. object Coil:Heating:Desuperheater) or by a user-defined plant water loop (Ref. object Coil:WaterHeating:Desuperheater).
-
-The performance of the compressor rack is simulated using the sum of the evaporator loads for all refrigerated cases and walk-ins connected to the rack. Whether a single refrigerated case is connected to a rack (e.g., stand-alone refrigerated case, meat cooler, or produce cooler) or several cases are connected to a rack, the rack electric consumption is calculated based on the total evaporator load for the connected cases and walk-ins and the coefficient of performance (COP) for the compressor rack. At least one refrigerated case or walk-in must be connected to the compressor rack. The model assumes the compressor rack has sufficient capacity to meet the connected refrigeration load for any simulation time step. Additionally, the model neglects compressor cycling losses at part-load conditions.
-
-For condenser heat rejection to the outdoors, condenser cooling can be modeled as dry air cooling, wet evaporative cooling, or water loop cooling. Using evaporative cooling rather than dry air cooling will allow for more efficient condenser heat rejection based on the entering air approaching the wet-bulb temperature rather than the dry-bulb temperature. Analyses under the International Energy Agency’s (IEA) Heat Pumping Programme Annex 26 indicates that this measure can improve refrigeration system efficiency by up to 10% (IEA 2003). The use of an evaporative-cooled condenser requires a water pump and, optionally, a basin sump water heater (to protect against freezing). Makeup water will also be required to replace that lost by evaporation. In colder climates, some evaporative-cooled condensers are drained for the winter months and run as dry air units. This scenario can be modeled by using an optional evaporative condenser availability schedule.
-
-The simulation of the evaporative cooled condenser utilizes an effective air dry-bulb temperature that is assumed to be the result of evaporation of water in the air stream (similar to object EvaporativeCooler:Direct:CelDekPad). As discussed below, this effective temperature is used by performance curves that are a function of temperature. While some designs of evaporative coolers use water film cascading across the condenser coil for evaporative cooling, the current model uses the effective temperature method as a surrogate for the more complex water film on coil calculations.
-
-If the condenser heat rejection is specified as water cooled, an appropriate plant water loop must be defined by the user (see documentation on *Plant/Condenser Loops* for additional details about plant loops).  This will include defining cooling supply components, such as pumps, water storage tanks, and cooling towers, as well as related branches, nodes, and connectors. The heat rejection from the refrigeration condenser is modeled as a cooling demand, which is satisfied by heat extraction devices (e.g., water tank and cooling tower) on the cooling supply side of a water loop. An example of such an arrangement is shown in Figure 278.
-
-![watertankheatrecoveryschematic](media/image6093.png)
-
-Figure 278. Example Of Condenser Heat Recovery To Water Storage Tank
-
-#### Compressor Energy Use
-
-Calculation of compressor rack electric power uses a simple model based on the total evaporator load (sum of the evaporator loads for all refrigerated cases and walk-ins connected to a rack) and the compressor rack operating COP which accounts for the air temperature entering the condenser:
-
-<div>$$CO{P_{operating}} = CO{P_{design}}\left( {COPfTemp} \right)$$</div>
-
-where:
-
-<span>\(CO{P_{operating}}\)</span>              = compressor coefficient of performance at actual operating conditions (W/W)
-
-<span>\(CO{P_{design}}\)</span>     = compressor coefficient of performance at design conditions (W/W)
-
-<span>\(COPfTemp\)</span> = output of the normalized “Compressor Rack COP as a Function of Temperature Curve� (dimensionless)
-
-Because the COP curve is defined only as a function of the condensing temperature, it is important that this curve definition corresponds to the lowest evaporating temperature served by the compressor rack. The air temperature used to evaluate the “Compressor Rack COP as a Function of Temperature Curve� depends on where the compressor rack’s condenser is located (Heat Rejection Location). When modeling condenser heat rejected directly to a zone (typical of a stand-alone packaged refrigerated case with integral condenser located in a building zone), the zone air dry-bulb temperature is used to calculate the change in compressor COP from the design value. If more than one refrigerated case and no walk-ins are attached to a compressor rack that rejects its condenser heat to a zone, then all cases served by this rack must reside in the same zone. When modeling a compressor rack serving at least one walk-in, OR with condenser heat rejected to outdoors, the refrigerated cases and walk-ins connected to this rack may be located in different zones. If the condenser type is specified as “Air Cooled�, the outdoor air dry-bulb temperature is used to evaluate the “Compressor Rack COP as a Function of Temperature Curve.�  If the condenser type is specified as “Evap Cooled�, the air temperature leaving the condenser is related to the effectiveness of the evaporative cooling system. If the evaporative process were 100% effective, the effective temperature of air leaving the evaporative media would equal the air wet-bulb temperature. However, the efficiency of the direct evaporative process is typically less than 100%, and the effective temperature leaving the condenser is determined by:
-
-<div>$${T_{effective}} = {T_{owb}} + (1 - \varepsilon )*[{T_{odb}} - {T_{owb}}]$$</div>
-
-where:
-
-<span>\({T_{effective}}\)</span>       = effective dry-bulb temperature of air leaving the condenser cooling coil (°C)
-
-<span>\({T_{owb}}\)</span>           = outdoor air wet-bulb temperature (°C)
-
-<span>\({T_{odb}}\)</span>           = outdoor air dry-bulb temperature (°C)
-
-<span>\(\varepsilon \)</span>               = evaporative condenser effectiveness.
-
-If the user is modeling an evaporative cooled condenser and is using COPfTemp curve data (e.g., manufacturer’s data) based on wet-bulb temperature rather than dry-bulb temperature, the evaporative condenser effectiveness should be set to 1.0 for consistency.
-
-If the condenser is water cooled, the effective temperature experienced by the condenser is based on the return water temperature from the plant loop heat rejection system (e.g., cooling tower) that is defined by the user. This return water temperature is typically related to the outdoor ambient conditions at each time step.
-
-The electric power input to the rack compressor(s) is calculated for each simulation time step as the sum of the connected refrigerated case evaporator loads divided by the operating COP:
-
-<div>$${P_{{\rm{rack}}}} = \frac{{\sum {{{\dot Q}_{case}} + \sum {{{\dot Q}_{walkin}}} } }}{{CO{P_{operating}}}}$$</div>
-
-where:
-
-<span>\({P_{rack}}\)</span>  = output variable “Refrigeration Compressor Rack Electric Power [W]�, electric power input to the rack compressor(s)
-
-<span>\({\dot Q_{case}}\)</span>  = evaporator load for each refrigerated case connected to the rack (W)
-
-<span>\({\dot Q_{walkin}}\)</span>= refrigeration load for each walk-in connected to the rack (W)
-
-#### Condenser Heat Rejection, Energy Use, and Water Use
-
-The compressor rack can reject heat to an air-, water-, or evaporative-cooled condenser. The condenser type determines the heat rejection temperature used for the compressor rack COP calculation. The compressor rack also allows superheat heat reclaim and heat rejection to a conditioned zone.
-
-##### Condenser Fan Energy Use
-
-Condenser fan power for any simulation time step is calculated by multiplying the design fan power by the condenser fan power as a function of temperature curve.
-
-<div>$${P_{CondFan}}\,\, = {P_{CondFan,design}}\left( {CondFanfTemp} \right)$$</div>
-
-where:
-
-<span>\({P_{CondFan}}\)</span>                  = output variable “Refrigeration Compressor Rack Condenser Fan Electric Energy [W]�
-
-<span>\({P_{CondFan,design}}\)</span>           = design condenser fan power (W)
-
-<span>\(CondFanfTemp\)</span>    = output of the optional “Condenser Fan Power as a Function of Temperature Curve�
-
-Similar to the compressor rack energy use described above, the air temperature used to evaluate the “Condenser Fan Power as a Function of Temperature Curve� depends on where the condenser rack’s condenser is located (i.e., zone air dry-bulb temperature if the condenser is located in a zone, outdoor air dry-bulb temperature if the condenser is located outdoors and is specified as air cooled, or effective temperature if the condenser is outdoors and is specified as evaporative cooled). If the sum of the evaporator loads for the refrigerated cases connected to the rack is equal to zero, the condenser fan power is set equal to zero. If the user does not provide a “Condenser Fan Power as a Function of Temperature Curve�, then the model assumes the condenser fan power is at the design power level when any of the refrigerated cases connected to this rack are operating.
-
-If the user is modeling an evaporative cooled condenser and is using CondFanfTemp curve data based on wet-bulb temperature rather than dry-bulb temperature, the evaporative condenser effectiveness should be set to 1.0 for consistency.
-
-For a water cooled condenser, there is no fan load at the condenser (i.e., the  water/refrigerant heat exchanger). Any fan load would be related to and accounted for at the heat rejection object (e.g., cooling tower).
-
-##### Superheat Reclaim Heating Coil
-
-EnergyPlus can simulate waste heat being reclaimed from a compressor rack for use by a refrigerant-to-air or refrigerant to water heating coil. Heat reclaimed from the compressor rack is assumed to be recovered from the superheated refrigerant gas leaving the compressor(s) and does not directly impact the performance of the compressor rack or refrigerated cases connected to the rack. The total heat rejected by the condenser (in Watts) is calculated each time step as follows:
-
-<div>$${\dot Q_{condenser}} = \left( {\sum {{{\dot Q}_{case}} + \left. {\sum {{{\dot Q}_{walkin}}} } \right)} } \right.\left( {1 + \left. {\frac{1}{{CO{P_{operating}}}}} \right)} \right.$$</div>
-
-The heat reclaim heating coil is able to transfer a fixed percentage of this total amount of rejected energy (not to exceed 30%) and use it to heat air and water. Refer to objects Coil:Heating:Desuperheater and Coil:WaterHeating:Desuperheater for a complete description of how these coils are modeled.
-
-NOTE: When modeling a heat reclaim coil, the heat rejection location in the Refrigeration:CompressorRack object must be “Outdoors�. If the compressor rack heat rejection location is “Zone�, the total amount of waste heat available for reclaim (e.g., by a desuperheater heating coil) is set to zero by the compressor rack object and the simulation proceeds.
-
-##### Heat Rejection to Zone
-
-The compressor rack model can simulate condenser heat being rejected to a zone. As explained previously, if this heat rejection option is selected then all refrigerated cases connected to the rack must be located in the same zone and a superheat heat reclaim heating coil can not be modeled (Ref. Superheat Reclaim Heating Coil).
-
-The refrigerated case and walk-in objects (Refrigeration:Case and Refrigeration:WalkIn) already calculate and report the sensible case credits which impact the zone air heat balance (Ref. Sensible Case Credits). When refrigerated cases and/or walk-ins are served by a compressor rack that rejects condenser waste heat directly to the zone (e.g., a stand-alone refrigerated case with integral compressor and condenser), this condenser waste heat also impacts the zone air heat balance and offsets some or all of the sensible case credits.
-
-If only cases are served, the amount of condenser waste heat rejected to the zone and/or the HVAC return air (zone return air path outlet node) is calculated and reported by the refrigerated case compressor rack object as follows:
-
-<div>$${\dot Q_{Zone,heating}}\,\,\, = \,\,\,\frac{{\sum {\left( {{{\dot Q}_{case}}[1 - RAF]} \right)} }}{{\sum {\left( {{{\dot Q}_{case}}} \right)} }}\,\left( {{{\dot Q}_{condenser}}\,\, + \,\,{P_{CondFan}}} \right)$$</div>
-
-<div>$${\dot Q_{HVAC,heating}}\,\,\, = \,\,\left( {{{\dot Q}_{condenser}}\,\, + \,\,{P_{CondFan}}} \right) - \,{\dot Q_{zone,heating}}$$</div>
-
-where:
-
-<span>\({\dot Q_{Zone,heating}}\)</span> = output variable “Refrigeration Compressor Rack Zone Sensible Heating Rate [W] “
-
-*RAF*           = return air factor for each case connected to the rack (Ref. Figure 279)
-
-<span>\({\dot Q_{HVAC,heating}}\)</span>= output variable “Refrigeration Compressor Rack Return Air Sensible Heating Rate [W] “
-
-If the HVAC system is off for a simulation time step (no return air mass flow), the rack condenser heat normally attributed to the HVAC return is set equal to zero and all condenser heat energy is applied to the zone air heat balance.
-
-If, however, walk-in cooler(s) are also served by this compressor rack, no condenser heat is rejected to the HVAC return air. For walk-in cooler(s), the user must specify the zone that accepts the condenser heat rejection (because walk-ins can exchange heat with multiple zones). In that case:
-
-<div>$${\dot Q_{Zone,heating}} = {\dot Q_{condenser}} + {P_{CondFan}}$$</div>
-
-##### Water Cooled Condenser
-
-If the refrigeration condenser is water cooled, a water plant loop must be defined in the input file. At a minimum, the loop must contain a pump and one or more heat sinks of sufficient capacity to remove the condenser heat load. In the system shown in Figure 278, the heat sinks are the water heater tank and the cooling tower. The water pump in the loop can be either constant (Ref. Pump:ConstantSpeed)  or variable speed (Ref. Pump:VariableSpeed). A variable speed pump permits the loop flow to vary and allows for a setpoint to be established on the condenser outlet water temperature. As the refrigeration condenser heat load varies through time, the speed of the pump can be adjusted to achieve a mass flow consistent with a desired outlet water temperature according to
-
-<div>$$m = \frac{{{Q_{condenser}}}}{{{c_p} \cdot ({T_{out}} - {T_{in}})}}$$</div>
-
-where:
-
-*m*               = mass flow in the water loop
-
-*Q<sub>condenser</sub>      * = heat rejected by the condenser
-
-*c<sub>p</sub>  *             = specific heat of water
-
-*T<sub>out</sub> *             = desired water outlet temperature
-
-*T<sub>in</sub>               =* return water inlet temperature.
-
-The desired water outlet temperature is specified using a schedule, subject to a maximum water outlet temperature (input specified). The maximum temperature is typically defined by constraints on the refrigerant loop pressures and temperatures. The desired mass flow in the water loop to meet the temperature schedule is also compared to the user-supplied maximum flow rate. If the desired mass flow is greater than the maximum allowed flow, the flow rate is set to the maximum value and the resulting water outlet temperature is determined.
-
-The return water inlet temperature is a function of the cooling system defined by the user. A minimum return water temperature may need to be taken into consideration to prevent lowering the resulting refrigerant condensing pressure to the point that refrigerant expansion valve operation becomes impaired. When ambient conditions produce low temperature warnings based on the minimum return water temperature, an outlet temperature setpoint control may need to be placed on the water heat sink object (e.g., cooling tower) to keep the return water temperature above the minimum.
-
-If the water loop flow is constant (i.e., driven by a constant speed pump), then the outlet water temperature will vary with the amount of heat rejected by the condenser.    Using the equation above, the resulting water outlet temperature is calculated as
-
-<div>$${T_{out}} = \frac{{{Q_{condenser}}}}{{{c_p} \cdot m}} + {T_{in}}$$</div>
-
-##### Evaporative Condenser Water Pump
-
-If the condenser type is specified as “Evap Cooled�, a water pump is required to circulate water in the evaporative condenser. The pump power can be input directly or be autocalculated using a relationship of 0.004266 W per watt [15 W/ton] of rated total cooling capacity where the total cooling capacity is the sum of the rated total cooling capacities for the refrigeration load connected to this compressor rack. Following manufacturer’s recommendations regarding the avoidance of scaling, the water pump does not cycle when there is no cooling demand (i.e., when the compressors are not running), but rather runs continuously. However, if the evaporative condenser availability schedule is set such that evaporative cooling is not available (e.g., during very cold months to avoid freezing), then the pump power consumption will be zero during that period.
-
-##### Evaporative Condenser Water Consumption
-
-With evaporative cooling of the condenser’s entering air, makeup water is needed to replenish the water lost due to evaporation. The quantity required is calculated as the product of the air mass flow rate and the difference between the entering and leaving air humidity ratio, divided by the density of water. The air mass flow rate is determined by multiplying the evaporative condenser air volume flow rate times the density of the entering air (i.e., at the condenser air inlet node if provided, or outdoor air conditions [e.g., no adjustment for height above ground] if the condenser air inlet node field is left blank). The volumetric air flow rate is either specified directly in the user input or is autocalculated using the relationship 0.000144 m<sup>3</sup>/s per watt of rated total cooling capacity [850 cfm/ton] where the total cooling capacity is the sum of the rated total cooling capacities for the refrigerated cases and walk-ins connected to this compressor rack (Ref. Refrigeration:Case and Refrigeration:WalkIn). The air mass flow rate is multiplied by the variable *CondFanfTemp*, described above, to simulate the modulation of air flow by the condenser fans (e.g., staging, multi-speed, or variable speed) as a function of temperature. Mathematically,
-
-<div>$${\dot V_{evaporation,makeup}} = \frac{{{{\dot m}_{air}}\left( {CondFanfTemp} \right)({\omega_{air,outlet}} - {\omega_{air,inlet}})}}{{{\rho_{water}}}}$$</div>
-
-where:
-
-<span>\(\mathop {{{\dot V}_{evaporation,makeup}}}\limits^{} \)</span>= Refrigeration Compressor Rack Evaporative Condenser Water Volume Flow Rate (m<sup>3</sup>/s)
-
-<span>\({\dot m_{air}} = \)</span> mass flow rate of air through the evaporative condenser (kg/s)
-
-<span>\({\omega_{air,outlet}}\)</span> = humidity ratio of air leaving the evaporative media (kg<sub>water</sub>/kg<sub>dry\\ air</sub>) based on the effective dry-bulb temperature *T<sub>effective</sub>*, as described above, outdoor air wet-bulb temperature, and outdoor barometric pressure
-
-<span>\({\omega_{air,inlet}}\)</span> = humidity ratio of inlet air (kg<sub>water</sub>/kg<sub>dry\\ air</sub>) based on conditions at the condenser air inlet node if provided, or outdoor air conditions (e.g., no adjustment for height above ground) if the condenser air inlet node field is left blank
-
-<span>\({\rho_{water}}\)</span> = density of water evaluated at the effective air temperature (kg/m<sup>3</sup>)
-
-The source of the makeup water may be specified as a water storage tank. If not specified, the makeup water is assumed to come from the building mains (Ref. Water Mains Temperatures).
-
-##### Evaporative Condenser Basin Heater
-
-In cold climates, a basin heater may be needed to prevent freezing of the evaporative cooling water. This feature is included in the model whereby an electric basin heater provides heat to the sump water only when the condenser cooling system is idle (i.e., no refrigeration load) and when the outdoor air dry-bulb temperature is below a user-specified setpoint. Since heat balances and basin water temperatures are not explicitly determined, a linear loading relationship, as a function of the difference in outdoor air dry-bulb temperature and the setpoint temperature, is used calculate the power demand at a given time step by the basin heater.
-
-<div>$${P_{ba\sinh eater}} = {P_{heatercapacity}}*({T_{setpo{\mathop{\rm int}} }} - {T_{OutDb}})$$</div>
-
-where:
-
-<span>\({P_{ba\sinh eater}}\)</span>= electric power demand for basin heater in current time step (W)
-
-<span>\({P_{heatercapacity}}\)</span>= electric heater capacity as a function of differential temperature (W/deg K)
-
-<span>\({T_{setpo{\mathop{\rm int}} }}\)</span>= setpoint temperature below which the heater turns on (°C)
-
-<span>\({T_{OutDb}}\)</span> = outdoor air dry-bulb temperature (°C)
-
-A default value for the basin heater capacity of 200 W/deg K has been established based on manufacturer data.
-
-##### Evaporative Condenser Availability Schedule
-
-Some manufacturer’s evaporative cooling systems for refrigeration condensers permit seasonal draining in the colder months and operation as an air-cooled system during that time. This optional feature is available through an availability schedule. This is important in climates subject to freezing weather in order to avoid excessive ice formation on the condenser surfaces and surroundings. (The Availability Schedule is the correct way to model the use of evaporative condensers in cold climates. However, some users may take a single input description and use it to model a building with a refrigeration system in a variety of climates. To avoid modeling the use of evaporative coolers in freezing weather, the code includes a cutout to switch to dry operation whenever the outdoor drybulb temperature drops below 4C.) During periods when evaporative cooling is not available, the outdoor condenser behaves as an air-cooled system with no water consumption or pump and basin heater loads. The effective temperature of air entering the condenser coil during this period (used to evaluate COPfTemp and CondFanfTemp) is equal to the outdoor air dry-bulb temperature at the condenser air inlet node if provided, or outdoor air conditions (e.g., no adjustment for height above ground) if the condenser air inlet node field is left blank.
-
-### Refrigerated Cases
-
-The refrigerated case object (Refrigration:Case) works in conjunction with the compressor rack, detailed refrigeration system, or secondary refrigeration system object (Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem) to simulate the performance of a refrigerated case system. The refrigerated case model uses performance information at rated conditions along with performance curves for latent case credits and defrost heat load to determine performance at off-rated conditions. Energy use for lights, fans and anti-sweat heaters is modeled based on inputs for nominal power, schedules, and control type. The refrigerated case model accounts for the sensible and latent heat exchange with the surrounding environment (termed "case credits") which impacts the temperature and humidity in the zone where the case is located. The simplified model described here provides the flexibility to simulate a broad range of refrigerated case types.
-
-The total load on the refrigerated case evaporator is made up of various components:
-
-<div>$${\dot Q_{case}} = {\dot Q_{walls}} + {\dot Q_{rad}} + {\dot Q_{{\rm{inf,sens}}}} + {\dot Q_{{\rm{inf,lat}}}} + {\dot Q_{lights}} + {\dot Q_{as}} + {\dot Q_{def}} + {\dot Q_{fan}} + {\dot Q_{restock}}$$</div>
-
-where:
-
-<span>\({\dot Q_{case}}\)</span>    = total load on the refrigerated case evaporator (W)
-
-<span>\({\dot Q_{walls}}\)</span>   = heat transfer through case walls due to the difference between the refrigerated case operating dry-bulb temperature and the zone air dry-bulb temperature (W)
-
-<span>\({\dot Q_{rad}}\)</span>     = radiant heat transfer to the refrigerated case (W)
-
-<span>\({\dot Q_{{\rm{inf,}}sens}}\)</span> = sensible heat transfer by air infiltration to the refrigerated case through the air curtain or via door openings (W)
-
-<span>\({\dot Q_{{\rm{inf,lat}}}}\)</span>   = latent heat transfer by air infiltration to the refrigerated case through the air curtain or via door openings (W)
-
-<span>\({\dot Q_{lights}}\)</span>   = lighting heat load (W)
-
-<span>\({\dot Q_{as}}\)</span>      = anti-sweat heater load (W)
-
-<span>\({\dot Q_{def}}\)</span>     = defrost heat load (W)
-
-<span>\({\dot Q_{fan}}\)</span>     = fan heat load (W)
-
-<span>\({\dot Q_{restock}}\)</span> = sensible load on the refrigerated case due to restocking of products that are at a higher temperature than the case (W)
-
-The model assumes that these load components are known for a refrigerated case at rated ambient air conditions (typically 23.9ËšC [75ËšF] and 55% relative humidity) and the specified case operating temperature. A combination of user input curves and fixed correlations (defined within EnergyPlus) adjust for case performance at off-rated conditions. Several of the load components are typically provided by the case manufacturer (e.g., total rated load, fan, lighting, anti-sweat heater, and defrost loads). The remaining load components are not usually provided by the manufacturer and must be estimated (heat conduction through case walls, radiation heat transfer, sensible/latent air infiltration, and restocking).
-
-For estimating the latent air infiltration load, the model requires that the user provide the latent heat ratio (LHR) for the refrigerated case at rated conditions. Research results are available to provide guidance in selecting this value (ASHRAE 2002, Howell 1993a, Howell 1993b). The rated LHR for refrigerated cases typically ranges from 0.1 to 0.3 depending on case configuration (e.g., glass door reach-in versus multi-deck open case) and case operating temperature.
-
-The case loads due to wall heat conduction, radiation, and sensible air infiltration are estimated by the model as a single lumped value (sensible case credits). The sensible case credits are calculated by subtracting the known loads at rated conditions (fan, lighting, anti-sweat heater, defrost and latent case credits) from the rated total cooling capacity of the case which is provided by the case manufacturer (<span>\({\dot Q_{case,rated}}\)</span>).
-
-Using these assumptions and the schedule inputs provided by the user, the refrigerated case evaporator load components in Equation are determined for each simulation time step. The variation in certain loads with respect to changes in ambient air temperature and/or humidity (e.g., latent and sensible case credits, defrost load, and anti-sweat heater load) are factored into the calculation based on user-provided inputs or by the model itself.
-
-Whenever the total heat load on the case is greater than the available evaporator capacity, such as during defrost (when the evaporator capacity is set to zero) or restocking, the load is accumulated to be met during subsequent time steps. This accounts for the energy required to bring the case back down to the rated operating temperature even though the rise in case temperature during defrost or restocking is not explicitly modeled. Following defrost, it may take multiple time steps to meet this accumulated load.
-
-The specific calculations for case evaporator load components and electric power for these loads (as applicable) are provided below.
-
-#### Case Evaporator Fan
-
-The refrigerated case evaporator fan electric power is calculated for each simulation time step as the product of the operating case fan power per unit length of case, the length of the refrigerated case, and the fraction of time that the case is not being defrosted. For cases with hot-gas or electric defrost (with or without temperature termination), the fan is disabled during the entire scheduled defrost drip-down time period. The evaporator fan operates continuously for off-cycle defrost or no defrost.
-
-<div>$${P_{fan}}\,\,\,\, = \,\,\,\,{P'}_{fan,oper}\left( {{L_{case}}} \right)\left( {1 - SC{H_{defrost,dripdown}}} \right)$$</div>
-
-where:
-
-<span>\({P_{fan}}\)</span>           = output variable “Refrigerated Case Evaporator Fan Electric Power [W]�
-
-<span>\({P'}_{fan,oper}\)</span>     = operating case fan power per unit length (W/m)
-
-<span>\({L_{case}}\)</span>          = case length (m)
-
-<span>\(SC{H_{defrost,dripdown}}\)</span> = fraction of time case is being defrosted (0 to 1), including drip-down period (based on the defrost drip-down schedule) for hot-gas or electric defrost. For off-cycle defrost or no defrost, this value is set to zero for this calculation.
-
-The model assumes that the evaporator fan is entirely contained within the thermal envelope of the case, and that all fan power results in a direct heat load on the case evaporator:
-
-<div>$${\dot Q_{fan}} = \,{P_{fan}}$$</div>
-
-#### Case Lighting
-
-The refrigerated case lighting electric power is calculated for each simulation time step as the product of the installed case lighting power per unit length of case, the lighting schedule value, and the length of the refrigerated case:
-
-<div>$${P_{{\rm{lights}}}} = P{'_{{\rm{lights,  installed}}}}({L_{{\rm{case}}}})(SC{H_{{\rm{lights}}}})$$</div>
-
-where:
-
-<span>\({P_{lights}}\)</span>          = output variable “Refrigerated Case Lighting Electric Power [W]�
-
-<span>\(P{'_{{\rm{lights,  installed}}}}\)</span>          = installed case lighting power per unit length (W/m)
-
-<span>\(SC{H_{lights}}\)</span>    = case lighting schedule value (0 to 1)
-
-A maximum schedule value of 1.0 means the lights are fully on at the installed case lighting power level. Schedule values of 0.0 indicate the lights are off and 0.5 at half-power.
-
-The user can specify the fraction of lighting energy that directly contributes to the case evaporator heat load:
-
-<div>$${\dot Q_{lights}} = \,{P_{lights}}\left( {{F_l}} \right)$$</div>
-
-where:
-
-<span>\({F_l}\)</span>  = fraction of lighting energy to case
-
-The remainder of the lighting energy (1 - *F<sub>l</sub>*) is a heating load to the zone where the case is located, which is discussed further in section Sensible Case Credits below. This fraction (1 - *F<sub>l</sub>*) can be used to represent lighting ballasts and/or bulbs located outside the air curtain of the refrigerated case.
-
-#### Anti-Sweat Heater Performance
-
-Anti-sweat heaters warm the refrigerated case rails or doors to provide protection from moisture condensation. Different anti-sweat heater control strategies are used depending on the case temperature and the type of anti-sweat heater installed. Several types of anti-sweat heater control strategies can be simulated with this model: constant, linear variation with ambient relative humidity or dewpoint temperature, and a theoretical model that determines the minimum anti-sweat heater power required to maintain the case surface just above the temperature where condensation would occur. Additionally, anti-sweat heater performance can be disregarded if the type of refrigerated case does not warrant its use. For the control strategies described below (except “None� and “Constant Method�), the model does not allow the anti-sweat heater power to be less than the minimum power nor greater than the case anti-sweat heater power specified by the user. Each anti-sweat heater control type is described in detail below.
-
-##### None
-
-Used for refrigerated cases that do not require an anti-sweat heater.
-
-<div>$${\dot Q_{as}} = 0$$</div>
-
-where:
-
-<span>\({\dot Q_{as}}\)</span>            = anti-sweat heater load on the case evaporator (W)
-
-##### Constant Method
-
-For refrigerated cases requiring constant anti-sweat heater output, the power use is simply calculated as the case anti-sweat heater power per unit length multiplied by the length of the case. This method is used when the manufacturer recommends that cycling of the heaters not occur.
-
-<div>$${P_{as}} = {P'}_{as}\,\left( {{L_{case}}} \right)$$</div>
-
-where:
-
-<span>\({P_{as}}\)</span>             = output variable “Refrigerated Case Anti-Sweat Heater Electric Power [W]�
-
-<span>\({P'}_{as}\)</span>           = case anti-sweat heater power per unit length (W)
-
-##### Relative Humidity Method
-
-Anti-sweat heater power can be reduced at lower ambient relative humidity levels to save energy while still protecting from moisture condensation on cold surfaces. For this control type, anti-sweat heater power use is reduced linearly based on case anti-sweat heater power at the rated ambient relative humidity (typically 55% RH), the relative humidity specified by the user where no anti-sweat heater power is required, and the relative humidity of the ambient (zone) air surrounding the case.
-
-<div>$${P_{as}} = {P'}_{as}\left( {{L_{case}}} \right)\left( {1 - \left[ {\frac{{R{H_{rated}} - R{H_{air}}}}{{R{H_{rated}} - R{H_{\min }}}}} \right]} \right)$$</div>
-
-where:
-
-<span>\(R{H_{air}}\)</span>        = relative humidity of the ambient (zone) air (%)
-
-<span>\(R{H_{rated}}\)</span>      = rated ambient relative humidity (%)
-
-<span>\(R{H_{\min }}\)</span>       = relative humidity at zero anti-sweat heater energy (%)
-
-##### Dewpoint Method
-
-Anti-sweat heater power can also be reduced as a function of ambient air dewpoint temperature based on a similar correlation to that used by the relative humidity method. This control method varies the anti-sweat heater power linearly based on the ambient air dewpoint temperature, the case operating temperature, and the rated ambient dewpoint temperature (calculated by the model using the rated ambient temperature and rated ambient relative humidity entered by the user).
-
-<div>$${P_{as}} = {P'}_{as}\left( {{L_{case}}} \right)\left( {\frac{{{T_{dp,air}} - {T_{case}}}}{{{T_{dp,rated}} - {T_{case}}}}} \right)$$</div>
-
-where:
-
-<span>\({T_{dp,air}}\)</span>         = dewpoint temperature of the ambient (zone) air (˚C)
-
-<span>\({T_{dp,rated}}\)</span>       = rated ambient dewpoint temperature (˚C)
-
-<span>\({T_{case}}\)</span>           = case operating temperature (˚C)
-
-
-
-##### Heat Balance Method
-
-A theoretical model may also be used to simulate the performance of anti-sweat heater operation at various indoor dewpoint temperatures (Henderson and Khattar 1999). The model calculates that amount of heat required to hold the case or door surface at (or slightly above) the dewpoint temperature of the ambient air using the following simple heat balance equation:
-
-<div>$${P_{as}} = \,\,\left( {\frac{{\left( {{T_{dp,air}} - {T_{db,air}}} \right){H_{case}}}}{{{R_{air}}}} + \frac{{\left( {{T_{dp,air}} - {T_{case}}} \right){H_{case}}}}{{{R_{case}}}}} \right){L_{case}}$$</div>
-
-where:
-
-<span>\({T_{dp,air}}\)</span>         = dewpoint temperature of the ambient (zone) air (˚C)
-
-<span>\({T_{db,air}}\)</span>         = dry-bulb temperature of the ambient (zone) air (˚C)
-
-<span>\({H_{case}}\)</span>         = height of the case (m)
-
-<span>\({R_{air}}\)</span>           = air film resistance (assumed constant at 0.3169 m<sup>2</sup>-˚C/W)
-
-<span>\({R_{case}}\)</span>          = heat transfer resistance of case (m<sup>2</sup>-˚C/W)
-
-<span>\({T_{case}}\)</span>           = case operating temperature (˚C)
-
-<span>\({L_{case}}\)</span>          = case length (m)
-
-The model above provides a linear relationship of anti-sweat heater power with varying ambient air dewpoint temperature at constant ambient air dry-bulb and case temperatures. By assuming that the ‘nominal’ anti-sweat heater power entered by the user is required to avoid moisture condensation at rated ambient air conditions, the value of <span>\({R_{case}}\)</span> can be determined by rearranging the equation and solving as follows:
-
-<div>$${R_{case}} = \frac{{\left( {{T_{dp,rated}} - {T_{case}}} \right)}}{{\left( {\frac{{{P'}_{as}}}{{{H_{case}}}}} \right) - \left( {\frac{{{T_{dp,rated}} - {T_{db,rated}}}}{{{R_{air}}}}} \right)}}$$</div>
-
-where:
-
-<span>\({T_{db,rated}}\)</span>       = rated ambient temperature (˚C)
-
-With *R<sub>case</sub>*known, *P<sub>as</sub>* can be calculated for each simulation time step using the actual ambient (zone) air dry-bulb and dewpoint temperatures.
-
-##### All Anti-Sweat Heater Control Methods
-
-For all control methods, the user can specify the fraction of anti-sweat heater energy that directly contributes to the case evaporator heat load:
-
-<div>$${\dot Q_{as}} = \,{P_{as}}\left( {{F_{as}}} \right)$$</div>
-
-where:
-
-<span>\({F_{as}}\)</span>            = fraction of anti-sweat heater energy to case
-
-The remainder of the anti-sweat heater energy (1 - *F<sub>as</sub>*) is a heating load to the zone where the case is located, which is discussed further in section Sensible Case Credits below.
-
-#### Case Restocking
-
-The impact of restocking the refrigerated case with product that is not at the case operating temperature is modeled with the case restocking schedule. The schedule is entered as a heat gain rate per unit length of the refrigerated case (W/m). The heat load due to restocking is calculated as the scheduled load multiplied by the length of the refrigerated case. The load due to product restocking is assumed to be only sensible (temperature) heat; a latent (moisture) component is not modeled.
-
-<div>$${\dot Q_{restock}} = SC{H_{restock}}\left( {{L_{case}}} \right)$$</div>
-
-where:
-
-<span>\(SC{H_{restock}}\)</span>  = refrigerated case restocking schedule value (W/m)
-
-The restocking heat load is removed by the refrigerated case evaporator any time the case is not being defrosted and excess sensible cooling capacity is available. If the evaporator cooling capacity is insufficient to remove the entire restocking load, the unmet portion is carried over to the next simulation time step.
-
-#### Case Defrost
-
-Eight refrigerated case defrost strategies can be simulated: none, off-cycle, electric, electric with temperature termination, hot-gas, hot-gas with temperature termination, hot-brine, and hot-brine with temperature termination. Some research has shown that the defrost times for cases defrosted using hot brine can be significantly shorter than defrost times for electric or hot gas.(Terrell, W. J. Jr., 1999) For each of these strategies, the refrigerated case evaporator is turned off for the required time period to allow accumulated frost to melt. Additional time can be scheduled (drip-down) to allow the water to drip from the evaporator and drain from the case.
-
-Refrigerated cases typically require a specific number of defrost cycles per day for a pre-determined length of time. Refer to manufacturer’s recommendations for proper defrost frequency and duration. For example, a refrigerated case may have a single defrost period each day with defrost scheduled from 7:00 – 7:40 am and defrost drip-down scheduled from 7:00 – 7:55 am. Notice the drip-down schedule and the defrost schedule start at the same time, and the drip-down schedule is longer than the defrost schedule. These schedules should normally repeat for each day of the year.
-
-For electric, hot gas, and hot brine defrost types, energy use by the defrost heater occurs during the scheduled defrost period. For defrost with temperature termination, the energy is also multiplied by the defrost ratio simulating a defrost duration shorter than the defined (maximum) period. For all non-electric defrost types, defrost electric power is set equal to zero (and is not available as an output variable). For hot gas and hot brine defrost types in cases served by a detailed system, the condenser heat rejection load is reduced by the amount of heat recovered for use in the defrost system. This condenser credit is not applied for the simple compressor rack system.
-
-<div>$$\begin{array}{l}If\,(DefrostType\, = \,Electric)\,\,Then\\ ,\,\,\,\,\,{P_{def}} = {P'}_{def}\left( {{L_{case}}} \right)\left( {SC{H_{defrost}}} \right)\\ElseIf\,(DefrostType\, = \,ElectricWithTempTermination)\,Then\\ ,\,\,\,\,\,{P_{def}} = {P'}_{def}\left( {{L_{case}}} \right)\left( {SC{H_{defrost}}} \right)(DefrostRatio)\\Else\\ ,\,\,\,\,\,{P_{def}} = 0.0\\EndIf\end{array}$$</div>
-
-where:
-
-<span>\({P_{def}}\)</span>           = output variable “Refrigerated Case Defrost Electric Power [W]�
-
-<span>\({P'}_{def}\)</span>          = case defrost power per unit length (W)
-
-<span>\({L_{case}}\)</span>          = case length (m)
-
-<span>\(SC{H_{defrost}}\)</span>  = case defrost schedule value (0 to 1)
-
-<span>\(DefrostRatio\)</span> = fraction of maximum defrost time, used with temperature termination
-
-Frost accumulation on the case evaporator will vary with the humidity level in the ambient air surrounding the case. Therefore, defrost heater operation can be reduced when ambient air humidity levels are low. Several methods are used to reduce unnecessary defrost heater operation, including terminating heater operation when the measured evaporator temperature indicates that the accumulated frost has been completely melted. For modeling refrigerated cases with temperature-terminated defrost, EnergyPlus allows the user to specify a defrost energy correction curve to account for variations in defrost energy as ambient air humidity levels change. The user can select from four correction curve types: None, Case Temperature Method, Relative Humidity Method, or Dewpoint Method.
-
-<div>$$\begin{array}{l}{\rm{None (default):}}\\ ,\,\,\,DefrostRatio = 1\\ {\rm{Case}}\,{\rm{Temperature}}\,{\rm{Method:}}\\ ,\,\,\,DefrostRatio = 1 - \left( {R{H_{rated}} - R{H_{air}}} \right)\left[ {a + b\left( {{T_{case}}} \right) + c{{\left( {{T_{case}}} \right)}^2} + d{{\left( {{T_{case}}} \right)}^3}} \right]\,\\ {\rm{RH}}\,{\rm{method:}}\\ ,\,\,\,DefrostRatio = e + f\left( {R{H_{air}}} \right) + g{\left( {R{H_{air}}} \right)^2} + h{\left( {R{H_{air}}} \right)^3}\\ {\rm{Dewpoint}}\,{\rm{method:}}\\ ,\,\,\,DefrostRatio = i + j\left( {{T_{dp,air}}} \right) + k{\left( {{T_{dp,air}}} \right)^2} + l{\left( {{T_{dp,air}}} \right)^3}\end{array}$$</div>
-
-where:
-
-<span>\(R{H_{rated}}\)</span>      = rated ambient relative humidity (%)
-
-<span>\(R{H_{air}}\)</span>        = relative humidity of the ambient (zone) air (%)
-
-<span>\({T_{case}}\)</span>           = case operating temperature (˚C)
-
-<span>\({T_{dp,air}}\)</span>         = dewpoint temperature of the ambient (zone) air (˚C)
-
-a…l                        = user-defined coefficients using a cubic curve object (Curve:Cubic)
-
-The user specifies the defrost energy correction curve type and the name of the cubic curve object (Curve:Cubic) that defines the curve coefficients. Representative curve coefficients for curve type “Case Temperature Method� are provided in Table 75.
-
-Table 75. Representative Defrost Energy Correction Curve Coefficients for Case Temperature Method
-
-<table class="table table-striped">
-<tr>
-<td>Coefficient</td>
-<td>Single-shelf horizontal
-display case</td>
-<td>Multi-shelf vertical
-display case</td>
-</tr>
-<tr>
-<td>a</td>
-<td>2.3632E-2</td>
-<td>2.4598E-2</td>
-</tr>
-<tr>
-<td>b</td>
-<td>6.2320E-4</td>
-<td>7.6439E-4</td>
-</tr>
-<tr>
-<td>c</td>
-<td>2.8320E-5</td>
-<td>-3.8637E-5</td>
-</tr>
-<tr>
-<td>d</td>
-<td>4.4035E-7</td>
-<td>7.45686E-7</td>
-</tr>
-
-</table>
-
-Note: Coefficients derived for *RH<sub>rated</sub>* = 55% and a rated ambient temperature of 23.9˚C (75˚F). Source:  Howell 1993b.
-
-As mentioned above, the refrigerated case evaporator is turned off while it is being defrosted. Heat gains during defrost must be removed once the defrost period (drip-down schedule) has ended. The model assumes that heat gains due to defrost heater operation are at least partially offset by converting accumulated frost to liquid water (condensate) which drains from the case. Frost accumulation during each simulation time step is estimated by the model using the actual latent heat transfer to the refrigerated case and the heat of vaporization plus the heat of fusion for water. The model assumes that frost is not accumulated on the evaporator during the defrost drip-down time period.
-
-<div>$$Frost = Frost + \left( {\frac{{{{\dot Q}_{case,rated}}\left( {{L_{case}}} \right)\left( {RT{F_{rated}}} \right)\left( {LH{R_{rated}}} \right)\left( {LatentRatio} \right)\left( {{t_{zn}}} \right)}}{{\left( {{h_f} + {h_{fg}}} \right)}}} \right)\left( {1 - SC{H_{defrost,dripdown}}} \right)$$</div>
-
-where:
-
-<span>\(Frost\)</span>        = amount of accumulated frost on the case evaporator (kg)
-
-<span>\({\dot Q_{case,rated}}\)</span>    = case rated total cooling capacity per unit length (W/m)
-
-<span>\({L_{case}}\)</span>          = case length (m)
-
-<span>\(RT{F_{rated}}\)</span>     = runtime fraction of the refrigerated case at rated conditions
-
-<span>\(LH{R_{rated}}\)</span>    = latent heat ratio of the refrigerated case at rated conditions
-
-<span>\(LatentRatio\)</span> = ratio of actual latent load to rated latent load on the case, based on latent case credit curve (see section Latent Case Credits below)
-
-<span>\({t_{zn}}\)</span>             = duration of zone simulation time step (s)
-
-<span>\({h_{fg}}\)</span>                        = heat of vaporization of water (assumed constant at 2,498,000 J/kg)
-
-<span>\({h_f}\)</span>             = heat of fusion of water (335,000 J/kg)
-
-<span>\(SC{H_{defrost,dripdown}}\)</span>    = defrost drip-down schedule value (0 to 1)
-
-During defrost (SCHdefrost), the model assumes that the hot gas, hot brine, or electric heater energy directly contributes to melting the frost (heat of fusion of water). Defrost energy not attributed to melting frost from the evaporator coil results in a heat load on the refrigerated case evaporator (<sub><span>\({\dot Q_{def}}\)</span></sub>). When the defrost drip-down time period ends, this defrost energy heat load is added to the actual case load (up to the maximum evaporator capacity) until the total defrost energy heat load is removed (which may take several simulation time steps)
-
-<div>$$\begin{array}{l}If\left( {DefrostType = Electric\;or\;HotGas\;or\;HotBrine} \right)\;Then\\ quad \quad {{\dot Q}_{def}} = MAX\left( {0.0,\left[ {P_{def}'({L_{case}})(SC{H_{def}}) - \frac{{Frost({h_f})}}{{{t_{zn}}}}} \right]} \right)\\Else\\ quad \quad {{\dot Q}_{def}} = 0.0\\Endif\end{array}$$</div>
-
-where:
-
-<span>\({\dot Q_{def}}\)</span>     = defrost heat load (W)
-
-#### Sensible Case Credits
-
-Refrigerated cases remove sensible energy from the surrounding environment (termed “sensible case credits�). In this model, the sensible case credits are composed of wall heat conduction, radiation heat transfer, and sensible heat transfer by air infiltration (<span>\({\dot Q_{walls}}\)</span>+ <span>\({\dot Q_{rad}}\)</span>+ <span>\({\dot Q_{{\rm{inf,sens}}}}\)</span> in equation ). To quantify this energy transfer, the model first calculates the rated sensible case credits by subtracting the known loads at rated conditions (fan, lighting, and anti-sweat heater) from the rated sensible cooling capacity of the case. It should be noted that the lighting and fan heat discussed here are for standard-efficiency equipment. Manufacturers typically provide ratings for both standard and high-efficiency fan and lighting equipment; however, the standard equipment is used to determine rated sensible case credits. (Some manufacturers no longer include any lighting in their rated capacity values. For these cases, P’<sub>lights,std</sub> will equal zero.)
-
-<div>$$\dot Qc{c_{sens,rated}} = \left[ {{{\dot Q}_{case,rated}}\left( {RT{F_{rated}}} \right)\left( {1 - LH{R_{rated}}} \right) - {P'}_{lights,std}\left( {{F_l}} \right) - {P'}_{as}\left( {{F_{as}}} \right) - {P'}_{fan,std}} \right]{L_{case}}$$</div>
-
-where:
-
-<span>\(\dot Qc{c_{sens,rated}}\)</span>  = sensible case credits at rated conditions (W)
-
-<span>\({\dot Q_{case,rated}}\)</span>    = case rated total cooling capacity per unit length (W/m)
-
-<span>\(RT{F_{rated}}\)</span>     = runtime fraction of the refrigerated case at rated conditions
-
-<span>\(LH{R_{rated}}\)</span>    = latent heat ratio of the refrigerated case at rated conditions
-
-<span>\({P'}_{lights,std}\)</span>    = standard case lighting power per unit length (W/m)
-
-<span>\({F_l}\)</span>              = fraction of lighting energy to case
-
-<span>\({P'}_{as}\)</span>           = case anti-sweat heater power per unit length (W)
-
-<span>\({F_{as}}\)</span>                        = fraction of anti-sweat heater energy to case
-
-<span>\({P'}_{fan,std}\)</span>      = standard case fan power per unit length (W/m)
-
-<span>\({L_{case}}\)</span>          = case length (m)
-
-For every simulation time step, the rated sensible case credits are then adjusted to account for variations at off-rated ambient air temperatures. The model also allows the user to define a case credit fraction using a schedule object. This case credit fraction can be useful for modeling cases that operate differently during specific time periods. For example, metal or plastic coverings may be installed on refrigerated display cases during unoccupied hours which would significantly reduce case credits (e.g., air infiltration) compared to occupied hours when the coverings are removed. If the user does not define a case credit fraction schedule, then the fraction is assumed to be 1 for the entire simulation.
-
-<div>$$\dot Qc{c_{sens}} = \dot Qc{c_{sens,rated}}\left( {\frac{{{T_{db,air}} - {T_{case}}}}{{{T_{db,rated}} - {T_{case}}}}} \right)\left( {SC{H_{cc}}} \right)$$</div>
-
-where:
-
-<span>\(\dot Qc{c_{sens}}\)</span>      = sensible case credits adjusted for ambient temperature and case credit fraction (W)
-
-<span>\({T_{db,air}}\)</span>         = dry-bulb temperature of the ambient (zone) air (˚C)
-
-<span>\({T_{case}}\)</span>           = case operating temperature (˚C)
-
-<span>\({T_{db,rated}}\)</span>       = rated ambient (zone) dry-bulb temperature (˚C)
-
-<span>\(SC{H_{cc}}\)</span>       = case credit fraction (schedule value, 0 to 1)
-
-The sensible case credits calculated above are considered heat loads on the refrigerated case evaporator. The ***net*** impact of the case credits on the surrounding zone includes adjustment for the portion of the lighting and anti-sweat heater power that does not directly contribute to the case evaporator load. Sensible case credits are negative values when heat is removed from the zone load.
-
-<div>$$\dot Qc{c_{sens,NET}} = {P_{lights}}(1 - {F_l})\,\, + \,\,{P_{as}}(1 - {F_{as}})\,\, - \,\,\dot Qc{c_{sens}}$$</div>
-
-where:
-
-<span>\(\dot Qc{c_{sens,NET}}\)</span> = net impact of the sensible case credits on the surrounding zone, negative for cooling (W)
-
-<span>\({P_{lights}}\)</span>          = case lighting electric power (W)
-
-<span>\({F_l}\)</span>              = fraction of lighting energy to case
-
-<span>\({P_{as}}\)</span>             = anti-sweat heater electric power (W)
-
-<span>\({F_{as}}\)</span>                        = fraction of anti-sweat heater energy to case
-
-When refrigerated cases are served by a compressor rack that rejects condenser waste heat directly to the zone (e.g., a stand-alone refrigerated case with integral compressor and condenser), this condenser waste heat offsets some or all of the sensible case credits. The amount of condenser waste heat rejected to the zone is calculated and reported by the refrigerated case compressor rack object (Ref. Heat Rejection to Zone).
-
-#### Latent Case Credits
-
-Refrigerated cases also remove latent energy (moisture) from the surrounding environment (termed “latent case credits�). In this model, the latent case credit is composed solely of the latent heat transfer by air infiltration <span>\({\dot Q_{inf,lat}}\)</span>in equation . The latent case credits are calculated as the product of the case length and the total cooling capacity per unit length, latent heat ratio, and runtime fraction at rated conditions. As described previously (Ref. Sensible Case Credits), a case credit fraction schedule is used to model cases that operate differently during specific time periods. The same case credit fraction is used to modify both the sensible and latent case credits. If the user does not define a case credit fraction schedule, then the fraction is assumed to be 1 for the entire simulation. The calculation of latent case credits also includes a factor (*LatentRatio*) that accounts for lower ambient humidity levels. Latent case credits are set to zero during the defrost-dripdown periods.
-
-<div>$${\dot Q_{{\rm{inf}},lat}} = \,\,\,\, - \dot Qc{c_{lat}}\,\, = \,\,{\dot Q_{case,rated}}\left( {LH{R_{rated}}} \right)\left( {RT{F_{rated}}} \right)\left( {SC{H_{cc}}} \right)\left( {LatentRatio} \right){L_{case}}$$</div>
-
-where:
-
-<span>\({\dot Q_{{\rm{inf,lat}}}}\)</span>         = latent load on the refrigerated case evaporator at current ambient conditions (W)
-
-<span>\(\dot Qc{c_{lat}}\)</span>        = latent case credit impact on zone load, negative for dehumidification (W)
-
-<span>\({\dot Q_{case,rated}}\)</span>  = case rated total cooling capacity per unit length (W/m)
-
-<span>\(LH{R_{rated}}\)</span>  = latent heat ratio of the refrigerated case at rated conditions
-
-<span>\(RT{F_{rated}}\)</span>   = runtime fraction of the refrigerated case at rated conditions
-
-SCH<sub>CC</sub>     = case credit fraction (schedule value, 0 to 1)
-
-<span>\(LatentRatio\)</span> = ratio of actual latent load to rated latent load on the case, based on latent case credit curve
-
-<span>\({L_{case}}\)</span>         = case length (m)
-
-Latent load on the refrigerated case evaporator will vary with ambient humidity levels. Therefore, the refrigerated case model allows the user to specify a latent case credit curve to adjust case credits based on ambient humidity, and the user can select from three curve types: Case Temperature Method, Relative Humidity Method, or Dewpoint Method.
-
-<div>$$\begin{array}{l}{\rm{Case}}\,{\rm{Temperature}}\,{\rm{Method:}}\\ ,\,\,\,LatentRatio = 1 - \left( {R{H_{rated}} - R{H_{air}}} \right)\left[ {m + n\left( {{T_{case}}} \right) + o{{\left( {{T_{case}}} \right)}^2} + p{{\left( {{T_{case}}} \right)}^3}} \right]\,\\ {\rm{RH}}\,{\rm{method:}}\\ ,\,\,\,LatentRatio = q + r\left( {R{H_{air}}} \right) + s{\left( {R{H_{air}}} \right)^2} + t{\left( {R{H_{air}}} \right)^3}\\ {\rm{Dewpoint}}\,{\rm{method:}}\\ ,\,\,\,LatentRatio = u + v\left( {{T_{dp,air}}} \right) + w{\left( {{T_{dp,air}}} \right)^2} + x{\left( {{T_{dp,air}}} \right)^3}\end{array}$$</div>
-
-where:
-
-<span>\(R{H_{rated}}\)</span>      = rated ambient relative humidity (%)
-
-<span>\(R{H_{air}}\)</span>        = relative humidity of the ambient (zone) air (%)
-
-<span>\({T_{case}}\)</span>           = case operating temperature (˚C)
-
-<span>\({T_{dp,air}}\)</span>         = dewpoint temperature of the ambient (zone) air (˚C)
-
-m…x          = user-defined coefficients using a cubic curve object (Curve:Cubic)
-
-The user specifies the latent case credit curve type and the name of the cubic curve object (Curve:Cubic) that defines the curve coefficients. Representative curve coefficients for curve type “Case Temperature Method� are provided in Table 76.
-
-Table 76. Representative Latent Case Credit Curve Coefficients for Case Temperature Method
-
-<table class="table table-striped">
-<tr>
-<td>Coefficient</td>
-<td>Single-shelf horizontal</td>
-<td>Multi-shelf vertical</td>
-</tr>
-<tr>
-<td>m</td>
-<td>2.0376E-2</td>
-<td>2.6520E-2</td>
-</tr>
-<tr>
-<td>n</td>
-<td>2.4378E-4</td>
-<td>1.0780E-3</td>
-</tr>
-<tr>
-<td>o</td>
-<td>1.1400E-5</td>
-<td>-6.0256E-5</td>
-</tr>
-<tr>
-<td>p</td>
-<td>1.8110E-7</td>
-<td>1.2373E-6</td>
-</tr>
-
-</table>
-
-
- Note: Coefficients derived for *RH<sub>rated</sub>* = 55% and a rated ambient temperature of 23.9˚C (75˚F). Source:  Howell 1993b.
-
-#### Refrigerated Case Credits With Under Case Return Air
-
-For certain refrigerated case types, the sensible case credits provided to the zone can create an uncomfortably cold environment in the surrounding area. For this reason, return air ducts are frequently placed behind these cases to draw this cold air under the case and direct it back to the HVAC system. This reduces localized over-cooling and improves occupant comfort.
-
-![RAFraction](media/image6247.png)
-
-Figure 279. Return Air Factor Versus Under Case HVAC Return Air Fraction
-
-Since under case return ducts reduce the temperature and humidity of the air being recirculated to the HVAC system, this can impact HVAC system performance. Figure 279 shows the relationship that is used by the refrigerated case model to determine the fraction of case credits that directly cool and dehumidify the HVAC system return air. This fraction, referred to as the Return Air Factor (RAF), is a function of the fraction of the HVAC system return air that comes from under the cases. The remaining fraction of the case credits (1-RAF) becomes part of the overall zone air energy balance. If the HVAC system is off for a simulation time step (no return air mass flow), the sensible and latent case credits normally attributed to the HVAC return are set equal to zero (even though they get calculated and reported here as non-zero values) and all case credit energy is applied to the zone air heat balance.
-
-<div>$$\dot Qc{c_{sens,zone}} = \dot Qc{c_{sens,NET}}\left( {1 - RAF} \right)$$</div>
-
-<div>$$\dot Qc{c_{lat,zone}} = \dot Qc{c_{lat}}\left( {1 - RAF} \right)$$</div>
-
-<div>$$\dot Qc{c_{sens,HVAC}} = \dot Qc{c_{sens,NET}}\left( {RAF} \right)$$</div>
-
-<div>$$\dot Qc{c_{lat,HVAC}} = \dot Qc{c_{lat}}\left( {RAF} \right)$$</div>
-
-where:
-
-<span>\(\dot Qc{c_{sens,zone}}\)</span> = sensible case credit applied to the zone air heat balance (W)
-
-<span>\(\dot Qc{c_{lat,zone}}\)</span>   = latent case credit applied to the zone air heat balance (W)
-
-<span>\(\dot Qc{c_{sens,HVAC}}\)</span>= sensible case credit applied to the HVAC return air (zone return air path outlet node) (W)
-
-<span>\(\dot Qc{c_{lat,HVAC}}\)</span> = latent case credit applied to the HVAC return air (zone return air path outlet node) (W)
-
-RAF            = return air factor (see Figure 279 above)
-
-#### Variable Evaporator Temperature
-
-Control systems are now available that increase the evaporator temperature to improve compressor efficiency whenever the total loads on a system are less than the system capacity. To model these systems, a variable evaporator temperature is an option available with the detailed refrigeration system object (Refrigeration:System). If this option is selected, the model will compare the refrigeration load on each case to the load at rated conditions. If the case load in a particular time step is less than the rated load, an acceptable elevated evaporator temperature is determined for that case. The evaporator temperature for the whole refrigeration system is then set by the minimum evaporator temperature needed for any particular case.
-
-<div>$$\begin{array}{l}L{F_{case}} = \frac{{{{\dot Q}_{case,actual}}}}{{{{\dot Q}_{case,rated}}}};0.5 \le L{F_{case}} \le 1.0\\ {T_{{\rm{Evap,Allowed}}}} = {T_{case}} - L{F_{case}}({T_{case}} - {T_{Evap,Design}})\end{array}$$</div>
-
-where:
-
-LF<sub>case</sub>          = Load factor for a particular case
-
-Tevap         = Evaporator temperature, C.
-
-### Walk-In Coolers and Freezers
-
-The walk-in object (Refrigeration:WalkIn) is another type of refrigeration load that can be placed on either a refrigeration compressor rack, detailed refrigeration system, or secondary refrigeration system object (Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem). Walk-in coolers and freezers differ from refrigerated cases in that they may have surfaces facing more than one zone and in that they are always equipped with doors, that is, they do not have open shelves. Their sensible and latent exchange with zones is therefore calculated in a different manner than for refrigerated cases. Also, the walk-in model does not interact directly with the HVAC system, that is, the return air fraction option available in the refrigerated case model is not included.
-
-The walk-in cooler performance is based on the ASHRAE load model, which includes infiltration through door openings and sensible loss through walls/ceilings described by the user for each zone.(ASHRAE 2006d, ASHRAE 2006e, Gosney, W.B., Olama, G.A.-L. 1975) All equipment loads (fan, light, heaters) are modeled as well.  Sensible and latent exchange with multiple adjoining zones is included. A master schedule is used for the Walk In operation and  additional schedules control the lights, defrost, and heater operation.  Just as for cases, unmet refrigeration loads are accumulated to be met the following time step.  This usually occurs during defrost and  restocking.
-
-#### Walk-In Sensible and Latent Heat Exchange
-
-A walk-in can exchange both sensible and latent energy with multiple zones.  The heat transfer calculations are performed separately for each zone so that the heat transfer impact, or zone credits, can be determined. The area of all walls and ceilings facing each zone are described by the user by their thermal conductance and area. Sensible energy exchange takes place between these surfaces and the surrounding zones.  Because these walls interface with conditioned zones at relatively constant temperatures, this heat exchange is modeled very simply:
-
-Q<sub>SurfacesZn</sub> = U<sub>SurfacesZn</sub> x A<sub>SurfacesZn</sub> x ΔT<sub>Zn</sub>
-
-Q<sub>DoorSensZn</sub>     =  U<sub>DoorZn</sub>  x  Area<sub>DoorZn</sub>  x ΔT<sub>Zn</sub>
-
-The heat transfer through the floor is similarly modeled.
-
-Q<sub>Floor</sub> = A<sub>Floor</sub> x U<sub>Floor</sub> x (T<sub>Ground</sub> – T<sub>WalkIn</sub>)
-
-Where:
-
-A<sub>Floor</sub>           = Area of the walkin floor, m<sup>2</sup>
-
-A<sub>SurfacesZn           </sub> = Area of surfaces facing Zone n, m<sup>2</sup>
-
-Q<sub>DoorSensZn</sub>     = Sensible heat transfer through the closed door(s) facing Zone n, W
-
-Q<sub>surfacesZn</sub>      = Sensible heat transfer through walls and ceilings facing Zone n, W
-
-T<sub>Ground</sub>          = Ground temperature, C
-
-T<sub>WalkIn</sub>          = Walk-in operating temperature, C
-
-U<sub>Floor</sub>           = Thermal conductance of floor, W/m2-K
-
-U<sub>DoorZn</sub>         = Thermal conductance of doors facing Zone n, W/m2-K
-
-U<sub>SurfacesZn\\           </sub> = Thermal conductance of surfaces facing Zone n, W/m2-K
-
-ΔT<sub>Zn</sub>            = Difference between walk-in operating temperature and Zone n drybulb temperature, C
-
-Infiltration through doorways places both a sensible and a latent load upon the walk-in, and corresponding credits upon the adjacent zone.  Two types of doors are available, nominally called ‘stock’ and ‘glass’ doors, to enable the user to model doors that differ in thermal conductance, door protection type, and frequency of opening.  The sensible and latent infiltration loads are modeled according to the guidance specified in (ASHRAE 2006d, ASHRAE 2009, and Gosney and Olama, 1975).  The air within the cooler is assumed to be at 90% relative humidity. Equal air exchange is assumed, that is, the mass of dry air infiltrating into the walkin is assumed to equal the mass of dry air infiltrating out of the walkin.
-
-Q<sub>Infiltration</sub> = Q<sub>FullFlow</sub>  x  Factor<sub>DoorOpen</sub>  x Factor<sub>Flow</sub>  x (1 - Factor<sub>Protection</sub>)
-
-Q<sub>FullFlow</sub>=0.221\*A<sub>Door</sub>(h<sub>ZoneAir</sub>-h<sub>AirWalkIn</sub>)�<sub>AirWalkIn</sub>(1-�<sub>ZoneAir</sub>/�<sub>AirWalkIn</sub>)<sup>0.5</sup>(g\*H<sub>Door</sub>)<sup>0.5</sup>Factor<sub>Density</sub>
-
-Factor<sub>Density</sub> = (2 /(1 + (�<sub>AirWalkIn</sub> / �<sub>ZoneAir</sub>)<sup>0.333</sup>)) <sup>1.5</sup>
-
-m<sub>DryAir</sub> = Q<sub>Infiltration</sub> / (h<sub>ZoneAir</sub> - h<sub>AirWalkIn</sub>)
-
-m<sub>Water</sub> =  m<sub>DryAir</sub>  x (W<sub>ZoneAir</sub> - W<sub>AirWalkIn</sub>)
-
-Q<sub>WalkInLatentZn</sub> = m<sub>Water</sub> x Δh<sub>IcetoVapor</sub>  x (1  - SCH<sub>Defrost,DripDown</sub>)
-
-Q<sub>WalkInSensInfZn</sub>  = Q<sub>Infiltration</sub> - (m<sub>Water</sub> x Δh<sub>IcetoVapor</sub>)
-
-Where:
-
-A<sub>door</sub>            =  Area of door facing Zone n, m<sup>2</sup>
-
-Factor<sub>DoorOpen</sub> = Value scheduled by user, fraction of time door open during time step
-
-Factor<sub>Flow</sub>    =  Doorway flow factor, = 0.8 if ΔT<sub>Zn</sub> &gt; 11C; =1.1 if ΔT<sub>Zn</sub> &lt;= 11C
-
-Factor<sub>Protection</sub> = Doorway protection factor, = 0 for no protection; =  0.5 for an air curtain; and 0.9 for a strip curtain
-
-g    =  Gravitational constant
-
-h<sub>AirWalkIn               </sub> =  enthalpy of the air within the walk in, =  f(T<sub>WalkIn</sub>,P<sub>Oudoor</sub>, 90%RH), J/kg
-
-h<sub>ZoneAir                  </sub> =  enthalpy of the air in Zone n, J/kg
-
-H<sub>door</sub>            =  Height of door facing Zone n, m
-
-Q<sub>FullFlow</sub>        = Sensible and latent refrigeration load for fully established flow, W
-
-Q<sub>Infiltration</sub>       = Average infiltration (sensible and latent) refrigeration load for the time step, W
-
-Q<sub>WalkInLatentZn</sub> = Latent load upon the walk in facing Zone n, W
-
-Q<sub>WalkInSensInfZn</sub>  = Sensible load due to infiltration upon the walkin facing Zone n, W
-
-m<sub>DryAir</sub>          = Mass of dry air infiltrating into the walk-in, kg/s
-
-m<sub>Water</sub>          = Mass of water removed from the infiltrating air, kg/s
-
-P<sub>Oudoor                  </sub> =  Outdoor air pressure, Pa
-
-SCH<sub>Defrost,DripDown</sub> = value from 0 to 1 indicating whether the system is in the dripdown period
-
-W<sub>AirWalkIn            </sub> =  Humidity ratio of the air within the walk in, =  f(T<sub>WalkIn</sub>,P<sub>Oudoor</sub>, 90%RH), kg/kg
-
-W<sub>ZoneAir</sub>        =  Humidity ratio of Zone n air, kg/kg
-
-Δh<sub>IcetoVapor</sub>     =  Latent heat absorbed to change ice to vapor, J/kg
-
-�<sub>AirWalkIn               </sub> =  Density of the air within the walk in =  f(T<sub>WalkIn</sub>,P<sub>Oudoor</sub>, 90%RH), kg/m<sup>3</sup>
-
-�<sub>ZoneAir</sub>          =  Density of air in Zone n, kg/m<sup>3</sup>
-
-
-
-The sensible load on the case and the sensible credit to the zone continue throughout the defrost and dripdown periods.  However, to be consistent with the treatment of refrigerated cases, there is no latent credit to the zone or latent load upon the cooler during the dripdown period. Latent load and latent credit are both based on reducing the infiltrating vapor to ice. The sensible heat exchange between the walk in and the zone is then the total of the heat transfer through the doors and surfaces and the infiltration sensible load. The latent load upon the walkin is converted to the amount of frost added to the coils during each time step.  This accumulating value is used later to determine the load placed upon the walkin during the defrost cycle.
-
-Q<sub>WalkInSensZn </sub>  = Q<sub>WalkInSensInfZn</sub> + Q<sub>DoorZn</sub> + Q<sub>surfacesZn</sub>
-
-Q<sub>ZoneLatent</sub>  = - Q<sub>WalkInLatentZn</sub>
-
-Q<sub>ZoneSens</sub>  = - Q<sub>WalkInSensZn</sub>
-
-ΔFrost<sub>Zn</sub> = (m<sub>Water</sub> \*Δtime)\* (1- SCH<sub>Defrost,DripDown</sub>)
-
-Where:
-
-Q<sub>WalkInSensZn    </sub>  = Total sensible heat exchange between the walkin and Zone n, W
-
-Q<sub>ZoneLatent</sub>      = Latent load upon the Zone n, W
-
-Q<sub>ZoneSens</sub>       = Sensible load upon Zone n , W
-
-ΔFrost<sub>Zn           </sub> = Change in frost inventory, kg
-
-Δtime          = Length of time step, s
-
-After the heat exchange with each zone is calculated, the total load on the walkin is calculated:
-
-Q<sub>WalkInLatentTot</sub> = ∑Q<sub>WalkInLatentZn</sub>
-
-Q<sub>WalkInSensTot  </sub> = ∑Q<sub>WalkInSensZn</sub> + Q<sub>Light</sub>+ Q<sub>Fan</sub>+ Q<sub>Heater</sub> + Q<sub>Defrost\\ +</sub> Q<sub>Stocking\\ +</sub> Q<sub>Floor</sub>
-
-Q<sub>WalkInTotal</sub> = Q<sub>WalkInLatentTot</sub> + Q<sub>WalkInSensTot</sub>
-
-ΔFrost<sub>Tot</sub> = ∑ΔFrost<sub>Zn</sub>
-
-Where Q<sub>Light</sub>, Q<sub>Fan</sub>, Q<sub>Heater</sub> , Q<sub>Stocking</sub> , and Q<sub>Defrost</sub> are described below.
-
-#### Walk-In Fans, Heaters, Lighting, and Restocking
-
-Sensible heat loads are placed on a walk-in by fans, heaters, and lighting. Unlike refrigerated cases, there is no option to allocate any portion of these heat loads to the surrounding zone(s). Larger walk-ins will have separate fans at the cooling coil and for general circulation. The general circulation fan is assumed to run at all times. The cooling coil fan is assumed to be off for Hot-Fluid and Electric defrost. Lighting, heating, and restocking are modeled according to the schedule values entered by the user. For lighting and heating, the maximum power is entered along with a scheduled ratio (between 0 and 1) to be applied for any point in time.  The heating power includes all heaters except those used for defrost purposes. The heater power should include anti-sweat, door, floor, and drain-pan heaters. For restocking, the total sensible load in Watts is scheduled for each point in time (the restocking latent load is assumed to be zero).
-
-Q<sub>Light</sub> = RatedQ<sub>Lighting</sub> \* SCH<sub>Lighting</sub>
-
-Q<sub>Fan</sub> =  Power<sub>CircFan</sub> + Power<sub>CoilFan</sub> \* ( 1 - SCH<sub>DripDown</sub> )
-
-Q<sub>Heater</sub> = Power<sub>Heater</sub> \* SCH<sub>Heater</sub>
-
-Q<sub>Stocking</sub> = SCH<sub>Stocking</sub>
-
-Where:
-
-Q<sub>Light                      </sub> = Refrigeration load due to lighting during current time step, W
-
-RatedQ<sub>Lighting</sub> = Maximum lighting load specified for the walk-in, W
-
-SCH<sub>Lighting        </sub> = Scheduled value between 0 and 1 for the current time step
-
-Q<sub>Fan</sub>            =  Refrigeration load due to fan power during the current time step, W
-
-Power<sub>CircFan</sub> =  Rated circulating fan power, W
-
-Power<sub>CoilFan</sub> =  Rated coil fan power, W
-
-SCH<sub>DripDown    </sub> = Scheduled value between 0 and 1 for the current time step
-
-Q<sub>Heater</sub>          = Refrigeration load due to heaters during current time step, W
-
-Power<sub>Heater</sub>   = Rated total heater(s) power (including anti-sweat, floor, door, etc.) , W
-
-SCH<sub>Heater\\          </sub> = Scheduled value between 0 and 1 for the current time step
-
-Q<sub>Stocking</sub>        = Refrigeration load due to stocking during the time step, W
-
-SCH<sub>Stocking</sub>    = Scheduled value of load due to stocking, W
-
-#### Defrost
-
-The defrost types available for the walk-in model include none, off-cycle, electric, and hot-fluid. Defrosts are started according to scheduled times and can be ended either by schedule or by temperature termination. Dripdown schedules are used to keep the cooling coil off long enough to drain any condensate from the system.
-
-For defrost types none and off-cycle, the refrigeration load on the walk-in due to defrost is zero.  For off-cycle, the walk-in refrigeration capacity is set to zero during the drip-down scheduled time.
-
-The energy required for hot-fluid defrost is assumed to be reclaimed from the compressor exhaust (for detailed systems, this energy appears as a credit against the heat rejection needed at the condenser). The energy used by electric defrost is available as an output variable.
-
-If the defrost cycle is controlled by the schedule, the refrigeration load placed upon the walk-in is calculated as the product of the defrost capacity and the defrost schedule. The load is then reduced according to the amount of accumulated ice melted during that time step.
-
-Q<sub>Defrost</sub> = Capacity<sub>Defrost</sub>\*SCH<sub>Defrost</sub> – Δfrost x Δh<sub>IceMelt</sub> / Δtime
-
-Where:
-
-Q<sub>Defrost</sub>         = Refrigeration load imposed by defrost heat, W
-
-Capacity<sub>Defrost</sub> = Rated defrost power, W
-
-SCH<sub>Defrost         </sub> = Scheduled value between 0 and 1 for the current time step
-
-Δfrost         = amount of frost melted during time step, kg
-
-Δh<sub>IceMelt</sub>        = heat of fusion for ice, J/kg
-
-Δtime          = time in time step, s
-
-If the defrost is controlled by temperature termination, the defrost cycle is assumed to end when all the ice is melted.  However, we need to recognize not all defrost heat goes to melt ice. Some of the defrost heat goes to raising the temperature of the coil mass to greater than 0C, and some is transferred to the walk-in environment as some of the coils are defrosted before others.  The user enters a ‘defrost energy fraction’ to specify the portion of the defrost energy that goes directly to melting ice.  The default for defrost energy fraction is 0.7 for electric defrost and 0.3 for warm fluid defrost.( Baxter, V. D., Mei, V.C., 2002) For this type of defrost control, the model calculates the amount of energy available to melt the ice in each time step. The accumulated amount of ice is then reduced accordingly. When all the ice is melted, the defrost schedule value is set to zero and no further defrost load is placed upon the walk-in cooler.  If the defrost schedule ends before the ice is melted, the schedule is used and the ice continues to accumulate until the next defrost cycle. The refrigeration capacity is kept at zero until the end of the drip-down schedule. Until the accumulated ice is melted, the defrost heat load upon the walk-in is:
-
-Q<sub>Defrost</sub> = Capacity<sub>Defrost</sub> x SCH<sub>Defrost</sub> x (1- Fraction<sub>DefrostEnergy</sub>)
-
-### Air Chillers and Air Chiller Sets
-
-The Air Chiller object (Refrigeration:AirChiller) is another type of refrigeration load that can be placed on either a refrigeration compressor rack, detailed refrigeration system, or secondary refrigeration system object (Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem). Air chillers are used to model the type of equipment typically used in refrigerated warehouses. For that reason, there is a major difference between the air chiller model and those for refrigerated cases or walk-ins. For cases and walk-ins, a portion of the model is directed toward calculating the amount of refrigeration needed to maintain the refrigerated volume at the desired temperature due to heat exchange with the surrounding zone, and that zone is conditioned to a nearly constant temperature.  In a refrigerated warehouse, the refrigeration load is caused by heat exchange with a variable external environment.  For that reason, the loads for these zones are calculated by the usual EnergyPlus zone heat balance.  The amount of refrigeration needed to maintain the specified temperature set points is then passed to the air chiller model, in a similar fashion to the load passed to a window air conditioner model. The air chillers are therefore solved using the system time step, not the zone time step used for cases and walk-ins.
-
-The air chiller performance is based on three types of manufacturers ratings, Unit Load Factor, Total Capacity Map, or a set of European standards. Correction factors for material and refrigerant are applied to all of these ratings.
-
-#### Unit Load Factor Capacity
-
-Bruce Nelson has provided a useful description of the Unit Load Factor approach.(Nelson, B.I., 2010)
-
-*“One well-known method used to calculate the sensible cooling capacity of evaporators is the effectiveness method.(Kays,* *W.M., A.L. London, 1964)  Heat exchanger effectiveness is defined as the ratio of the actual amount of heat transferred to the maximum possible amount of heat that could be transferred with an infinite area. This method is extremely useful because cooling capacity can be calculated directly knowing only the dimensional characteristics of the coil and the initial temperature difference (entering air temperature minus the evaporating temperature). This initial temperature difference is referred to as “DT1� … in the refrigeration industry. Sensible cooling capacity is calculated as follows:*
-
-<div>$${q_{{\rm{sens}}}} = \dot m \times {c_p} \times \varepsilon  \times ({T_{{\rm{coil inlet}}}} - {T_{{\rm{evap}}}}) = \dot m \times {c_p} \times \varepsilon  \times DT1$$</div>
-
-*For a given size of coil operating with constant airflow rate, the effectiveness can be considered constant over the small op- erating temperature ranges typical of refrigeration applications, and therefore, capacity can be considered to be proportional to the ratio of DT1. Hence, if evaporator coil sensible capac- ity is known for a given DT1, then capacity at a new initial temperature difference, DT1�, can be found by multiplying the original capacity by the ratio DT1�/DT1.�*
-
-Where:
-
-q<sub>sens</sub>            = Cooling capacity (sensible only), W
-
-<span>\(\dot m\)</span>              = mass flow rate of air, kg/s
-
-<span>\({c_p}\)</span>             = specific heat capacity of moist air, J/kg-C
-
-<span>\(\varepsilon \)</span>               = effectiveness (=(T<sub>coil\\ inlet</sub> – T<sub>coil</sub> exit)/(T<sub>coil\\ inlet</sub> - T<sub>evap</sub>)
-
-T<sub>coil\\ inlet</sub>         = dry-bulb air temperature entering the coil, C
-
-T<sub>evap</sub>            = average refrigeratnt evaporating temperature, C
-
-T<sub>coil\\ exit</sub>          = dry-bulb air temperature leaving the coil, C
-
-DT1            = initial temperature difference, C
-
-
-
-Using this approach, the manufacturer specifies the Unit Load Factor in terms of sensible capacity per degree of temperature difference.
-
-<div>$$ULF = Capacit{y_{Rated,Sensible}}/DT{1_{Rated}}$$</div>
-
-*The total capacity is the sum of the sensible and latent capacity. The sensible heat ratio (SHR) is the sensible heat transfer divided by the total (sensible plus latent) heat transfer. Again, from Nelson,* (Nelson, B.I., 2010)
-
-*The mass transfer process is much more “thermally effective� than the sensible heat transfer process, that is, the heat flux through the evaporator surfaces during the mass transfer process is extremely high.(AHRI, 2001) Consequently, if the surface effectiveness of the coil were to remain constant, the increase in the evaporator cooling capacity during combined sensible and latent cooling would be equal to the sensible cooling capacity divided by the SHR… However, the increase in heat flux through the fin surfaces has the effect of decreasing fin efficiency and overall surface effectiveness due to an increase in the fin surface temperature gradient.7 The result is a slightly lower total cooling capacity.*
-
-<div>$$\begin{array}{*{20}{c}}{{Q_{ideal}} = \frac{{{q_{sens}}}}{{SHR}};}&{SHR = \frac{{{q_{sens}}}}{{{Q_{total}}}}}\end{array}$$</div>
-
-Where:
-
-<span>\({Q_{{\rm{ideal}}}}\)</span>          = Cooling capacity (total) if fin efficiency and total effectiveness were constant, W
-
-<span>\({Q_{{\rm{Total}}}}\)</span>         = Cooling capacity (total), actual
-
-
-
-The total capacity is therefore a function of the sensible heat ratio, which is a function of the total capacity, and they are both, of course a function of the psychometrics of the air flowing through the chiller. This is handled with a two step estimation process.
-
-<div>$$\begin{array}{l}\Delta T = {\rm{Minimum}}(\Delta {T_{{\rm{max}}}},({T_{{\rm{Coil inlet}}}} - {T_{{\rm{evap}}}}))\\ {q_{{\rm{sens,max}}}} = ULF*\Delta T \times (1 - SC{H_{{\rm{Defrost,DripDown}}}}) \times SC{H_{{\rm{Coil}}}}\\ {T_{{\rm{Coil exit estimate}}}} = {T_{{\rm{Coil inlet}}}} - \frac{{{q_{{\rm{sens,max}}}}}}{{{{\dot m}_{{\rm{DryA ir}}}} \times {c_{p,{\rm{Coil Inlet Dry Air}}}}}}\\ {h_{{\rm{Coil exit estimate}}}} = f({T_{{\rm{Coil exit estimate}}}},{P_{{\rm{Barometric}}}}){\rm{at a Relative Humidity of 1}}{\rm{.0}}\\ {Q_{{\rm{Total estimate}}}} = ({h_{{\rm{Coil Inlet}}}} - {h_{{\rm{Coil exit estimate}}}}) \times {{\dot m}_{{\rm{max}}}}\\SHR = \frac{{{q_{{\rm{sens,max}}}}}}{{{Q_{{\rm{Total estimate}}}}}}\\ {\rm{Correction}} = f(SHR);{\rm{Function input by user, linear or quadratic curve}}\\ {Q_{{\rm{Total}}}} = {\rm{Correction}} \times {q_{{\rm{sens,max}}}}\end{array}$$</div>
-
-Where:
-
-<span>\(\Delta T\)</span>            = Temperature difference between the inlet air and the average evaporating temperature, C
-
-<span>\(\Delta T{}_{Max}\)</span>       = Maximum temperature difference specified by the user, C
-
-SCH<sub>Coil</sub>        = Coil availability schedule
-
-h<sub>Coil\\ exit</sub>         = Enthalpy of air at the coil exit
-
-h<sub>Coil\\ inlet</sub>         = Enthalpy of air at the coil inlet
-
-P<sub>Barometric</sub>      =Barometric air pressure,Pa
-
-
-
-The “Correction� function must be obtained from the chiller manufacturer. Some curves typical of ammonia chillers have been published (see, for example, Fig. 2 in (Nelson, B.I., 2010)). A default linear approximation of this curve is provided as an input option.
-
-#### European Standard Ratings
-
-Five standard rating conditions have been defined in a European rating system. The capacity is reported at the rating condition as either the “Nominal� or “Standard� capacity. The “Nominal� capacity includes both latent and sensible loads and the “Standard� capacity includes sensible loads only. “Wet Coil Factors� are provided with the ratings to translate between the two, along with a chart giving the impact of Air Inlet Temperature on the Wet Coil Factor. The user identifies the rating condition used and whether the capacity input is “Nominal� or “Standard�. These rating factors, along with the air inlet temperature and evaporating temperature are used to calculate the actual cooling capacity.
-
-<div>$${Q_{{\rm{Total}}}} = {Q_{{\rm{Nominal}}}} \times \frac{{WetCoilFactor({T_{{\rm{Coil inlet}}}})}}{{WetCoilFactor({\rm{Standard Condition}})}} \times \frac{{\Delta T}}{{\Delta {T_{{\rm{Rated}}}}}}$$</div>
-
-#### Total Capacity Map
-
-Some manufacturers are beginning to provide more comprehensive performance information. For these air chillers, the manufacturers specify a Rated Total Capacity at a given inlet air relative humidity.  A table or set of curves is then provided to calculate the total capacity Q<sub>Total</sub>,  as a function of the inlet air temperature and relative humidity, and the average evaporating temperature.
-
-#### Sensible and Latent Capacity
-
-The sensible and latent loads served are then calculated as:
-
-<div>$$\begin{array}{l}{h_{{\rm{Coil exit}}}} = {h_{{\rm{Coil Inlet}}}} - \frac{{{Q_{{\rm{Total}}}}}}{{{{\dot V}_{{\rm{A ir,Max}}}} \times {\rho_{{\rm{Coil Inlet}}}}}}\\ {T_{{\rm{Coil exit}}}} = f({h_{{\rm{Coil exit}}}}){\rm{at a Relative Humidity of 1}}{\rm{.0}}\\H{R_{{\rm{Coil exit}}}} = f({T_{{\rm{Coil exit}}}},{h_{{\rm{Coil exit}}}})\\ {{\dot m}_{Water}} = {{\dot m}_{dryair,\max }} \times (H{R_{{\rm{Coil exit}}}} - H{R_{{\rm{Coil inlet}}}})\\ {q_{latent}} = {{\dot m}_{water}} \times {h_{icetovapor}}\\ {q_{{\rm{sens}}}} = {Q_{Total}} - {q_{latent}}\end{array}$$</div>
-
-Where:
-
-<span>\({\dot V_{Air,Max}}\)</span>       = Maximum air flow, m<sup>3</sup>/s
-
-HR              = Humidity Ratio, kg water/kg dry air
-
-h<sub>ice\\ to\\ vapor</sub>  =   enthalpy of phase change from vapor to ice
-
-When the sensible capacity provided is greater than the sensible load requested from the zone energy balance, the coil fan speed is varied as described later for the condenser fan. The latent load and amount of water condensed from the air are scaled accordingly.
-
-The frost accumulation and defrost cycles are handled as described previously for walk-in coolers.
-
-The net sensible heat impact on the zone is the difference between the coil’s sensible cooling capacity and any energy added during that time step by heaters, fan motors, and defrost.
-
-
-
-### Detailed Refrigeration Systems
-
-The detailed refrigeration system object (Refrigeration:System) is an alternative to the refrigeration compressor rack object (Refrigeration:CompressorRack). Either works in conjunction with the refrigerated case and walk-in objects (Refrigeration:Case and Refrigeration:WalkIn) to simulate the performance of a retail refrigeration system. The detailed system model differs from the compressor rack model in that it:
-
-1)    requires performance data for each compressor (see the RefrigerationCompressorCurves dataset),
-
-2)    requires condenser performance curves for air- and evaporative-cooled condensers,
-
-3)    explicitly calculates the amount of superheat available for reclaim in an optional air or water heating coil,
-
-4)    allows the suction temperature to rise when the case loads are less than the design loads, thus improving compressor efficiency,
-
-5)    allows the transfer of loads from one system to another, including cascade condensers and secondary systems typically used to reduce the amount of refrigerant inventory in the primary system, and mechanical subcoolers typically used to transfer a part of the refrigeration load from a lower-temperature system to a more efficient higher-temperature system,
-
-6)    allows the use of liquid suction heat exchangers which will improve the cycle efficiency for some refrigerants,
-
-7)    models three condenser fan types,
-
-8)    allows the user to keep track of refrigerant inventory,
-
-9)    does not assume that the compressor and condenser capacity is sufficient to meet the case loads, but carries unmet load over to the next time step,
-
-10) provides optional suction piping heat gain for comparison to distribution piping heat gain for secondary systems. [Note, these piping heat gains are also reflected in the zone heat balance. This piping heat gain is not to be confused with the pressure change in the suction piping, even though this pressure change is typically expressed in terms of an change in the saturated suction temperature].
-
-#### Refrigeration System Loads and Convergence
-
-The refrigeration loads for refrigerated cases and walk-ins are added to provide the first value for the refrigeration load on a detailed system, as well as the evaporating temperature. (If there are no cases or walk-ins served directly by a system, that system is not solved until the energy transfer loads are available.) The user can also choose to include suction pipe heat gain as a load on the system. The performance of refrigeration compressors is dependent upon the condensing and evaporating temperatures. The calculation starts with an estimated condensing temperature, which is used to calculate the compressor power use.
-
-<div>$${\dot Q_{{\rm{Refrigeration}}}} = \sum {{{\dot Q}_{case}}}  + \sum {{{\dot Q}_{walkin}}} ( + \sum {{{\dot Q}_{PipeHeatGain}}} )$$</div>
-
-<div>$${\dot Q_{System,Estimated}} = {\dot Q_{{\rm{Refrigeration}}}} + {P_{Compressors,Estimated}}$$</div>
-
-These values are in turn used to determine the total heat rejection load on the condenser, which produces a new estimate for the condensing temperature. A few iterations are usually necessary to converge upon the final condensing temperature and compressor power for each time step for each system.
-
-After each detailed refrigeration system has been solved, all energy transfers (subcoolers, secondary loops, and cascade condensers) among the systems are made.
-
-<div>$$\begin{array}{*{20}{c}}{{{\dot Q}_{Transfer}} = \sum {{{\dot Q}_{CascadeCondenser}} + \sum {{{\dot Q}_{SecondaryLoop}} + \sum {{{\dot Q}_{MechanicalSubcooler}}} } } }\\ {{{\dot Q}_{{\rm{Refrigeration}}}} = \sum {{{\dot Q}_{Case}} + \sum {{{\dot Q}_{WalkIn}} + \sum {{{\dot Q}_{Transfer}}( + \sum {{{\dot Q}_{PipeHeatGain}}} )} } } }\end{array}$$</div>
-
-This two step process is repeated twice to ensure that all the energy transfers among systems are balanced.
-
-Suction piping heat gain is an optional element in the load calculation.  Typically, the suction pipe heat gain is small compared to the other loads.  However, when comparing DX systems to secondary systems, this portion of the total load can be very different. (Hinde, D., et al. 2009)  To calculate the pipe heat gain load, the user must first calculate the U-value and area for the suction piping.  The U-value is the total conductance from the inside skin coefficient to the outside skin coefficient. This value must be multiplied by the area to provide the “sum of the UA in W/C,�  required in the input.
-
-#### Compressor Energy Use
-
-The compressor object (Refrigeration:Compressor) calculations start with the determination of the inlet (suction) and outlet (discharge) conditions. The suction pressure is defined by the saturated suction temperature (equal to the evaporating temperature in the refrigeration loads connected to the suction group) minus the pressure drop in the suction pipes. With proper design, this pressure drop typically corresponds to a saturated suction temperature drop of about 1C. The saturated discharge pressure is defined by the condensing temperature plus the pressure drop in the discharge pipes. With proper design, this discharge pipe pressure drop typically corresponds to a saturated discharge temperature increase of about 0.5C (ASHRAE 2006a). These two temperatures are then used with the manufacturer’s performance curves for each compressor. The performance curves are defined in ARI Standard 540 and take the following form (ARI 2004):
-
-<div>$$\begin{array}{l}X = {C_1} + {C_2}(S) + {C_3}(D) + {C_4}({S^2}) + {C_5}(SD) + {C_6}({D^2}) + {C_7}({S^3}) + {C_8}(D{S^2}) + {C_9}(S{D^2}) + {C_{10}}({D^3})\\S = {T_{evap}} - 1.\\D = {T_{condense}} + 0.5\end{array}$$</div>
-
-where:
-
-X    = can represent power input (W), or cooling capacity(W)
-
-C      = compressor performance coefficient (be sure to see the IO Reference guide because the Energy Plus input order for this equation does not match this ARI form)
-
-S    = Saturation temperature corresponding to the suction pressure (C)
-
-D    = Saturation temperature corresponding to the discharge pressure (C)
-
-T<sub>evap</sub>            = Evaporating temperature (C)
-
-The rated values for the cooling capacity and power consumption from the manufacturer include a specified amount of subcooling before the thermal expansion valve and a certain amount of superheat in the suction gas. Adjustments must be made to these rated values to reflect the actual subcooling and superheat conditions. Actual subcooling is determined by the condenser’s rated subcooling and by the subcooling provided by optional subcoolers. The actual superheat is determined by the refrigerated case superheat (usually set to ensure that there is no liquid in the suction lines leading to the compressors), set here at 4C, and the effect from any optional subcoolers(ASHRAE 2006b). These various state points are shown in Figure 280.
-
-![CorrectedPHcycledrawing](media/image6275.png)
-
-Figure 280. State Points and Energy Flows for Detailed Refrigeration System
-
-Once the corrected capacity is calculated for each compressor, the compressors are dispatched one at a time until the system load is met. The last compressor dispatched is assumed to run at full load for the fraction of the time step necessary to meet the load, That is, the model neglects compressor cycling losses at part-load conditions. Using the state point identification from Figure 280, these corrections are shown in the following equations. If the capacity available from all the compressors is less than the sum of the case loads for that time period, the unmet load is accumulated to be met in succeeding time steps. If this accumulated unmet load becomes too great, a warning message is generated.
-
-<div>$$\begin{array}{*{20}{c}}{Ca{p_{corrected}} = \frac{{{\rho_{1b}}}}{{{\rho_{1c}}}} \times \frac{{({h_{1b}} - {h_4})}}{{({h_{1c}} - {h_{4c}})}}Ca{p_{rated}}}\\ {\dot m = \frac{{Ca{p_{corrected}}}}{{({h_{1b}} - {h_4})}}}\end{array}$$</div>
-
-where:
-
-<span>\(\dot m\)</span>= mass flow rate of refrigerant, kg/s
-
-�    = density, kg/m<sup>3</sup>
-
-h    = enthalpy, J/kg
-
-Cap            = refrigeration capacity of an individual compressor, W
-
-Compressor performance can also be improved by allowing the suction pressure to rise whenever the sum of the loads on the refrigerated cases served by the compressors is less than the design load. The calculation of the maximum allowable evaporator temperature is described in “Variable Evaporator Temperature� in the discussion of Refrigeration Cases.
-
-#### Two-Stage Compression Systems
-
-In addition to the single-stage compression refrigeration system illustrated above, two-stage compression systems can be modeled.  For low temperature applications where the pressure ratio between the low- and high-pressure sides of the system could be 1:10 or more, it may be beneficial to utilize two stages of compressions (Evans 2008).  Two smaller compressors in series have a smaller displacement and usually operate more efficiently than one large compressor that covers the entire pressure range from the evaporator to the condenser.  This is especially true in ammonia refrigeration systems due to the large amount of superheating that occurs during the compression process (ASHRAE 2009b).
-
-Between the two stages of compression, an intercooler is used to cool the discharge gas exiting the low-stage compressor before it enters the high-stage compressor.  The cooling is performed within the intercooler by refrigerant at an intermediate pressure.  The degree to which intercooling reduces the power requirement of a refrigeration cycle depends on the refrigerant which is being used as well as the temperature lift between the evaporator and the condenser.
-
-Several methods of two-stage compression and intercooling have been used.  For large industrial refrigeration systems, typical of ammonia systems used in refrigerated warehouses, both shell-and-coil intercooling (Figure 281) and flash intercooling (Figure 282) are used.  The two stages of compression in these systems may be performed by separate low- and high-stage compressors or with a compound compressor containing both the low and high stages within the same compressor body.
-
-![](media/image6278.png)
-
-Figure 281.  Two-Stage Compression System with a Shell-and-Coil Intercooler.
-
-
-
-![](media/image6279.png)
-
-Figure 282.  Two-Stage Compression System with a Flash Intercooler.
-
-For two-stage compression systems with intercooling, there is an optimum intermediate pressure that minimizes the total power consumption of the system.  In the case of an ideal intercooler in which the refrigerant gas enters the high-stage compressor at the same temperature as it enters the low-stage compressor, the minimum compressor work is achieved using the same pressure ratio across both compressors (Baek et al. 2005).  Typically, the optimum intermediate pressure is approximated as the geometric mean pressure of the system as follows:
-
-<div>$${P_{{\mathop{\rm int}} ercooler}} = \sqrt {\left( {{P_{evaporator}}} \right)\left( {{P_{condenser}}} \right)} $$</div>
-
-where *P<sub>intercooler</sub>* is the pressure within the intercooler shell, *P<sub>evaporator</sub>* is the evaporating pressure and *P<sub>condenser</sub>* is the condensing pressure.
-
-The low-stage compressors operate between the evaporator pressure and the intercooler pressure while the high-stage compressors operate between the intercooler pressure and the condensing pressure.  The performance of both the low-stage and high-stage compressors are modeled using the compressors’ performance curves defined by ARI Standard 540 (ARI 2004), as discussed previously in the “Compressor Energy Use� section.  In addition, capacity corrections are applied to the compressor performance curves to account for deviations between the actual operating conditions and the rated conditions.
-
-Refering to Figure 281 for a two-stage system with a shell-and-coil intercooler, the performance of the intercooler is modeled with a “Shell-and-Coil Intercooler Effectiveness�, defined as follows:
-
-<div>$$\eta  = \frac{{{T_4} - {T_{5a}}}}{{{T_4} - {T_3}}}$$</div>
-
-where *η* is the shell-and-coil intercooler effectiveness, *T*<sub>4</sub> is the inlet temperature of the liquid refrigerant at Location 4, *T*<sub>5*a*</sub> is the outlet temperature of the liquid refrigerant at Location 5a, and *T*<sub>3</sub> is the saturated refrigerant temperature within the intercooler shell.  Valid values for the effectiveness range from 0.0 to 1.0.  An effectiveness of zero indicates that no heat is transferred from the refrigerant in the shell-side of the intercooler to the liquid refrigerant in the coil-side of the the intercooler, and thus, there is no change in the temperature of the liquid refrigerant from Location 4 to Location 5a.  An effectiveness of 1.0 indicates that the temperature of the liquid exiting the coil-side of the intercooler at Location 5a is equal to the temperature of the saturated refrigerant in the shell-side of the intercooler.  The user may specify a value for the intercooler effectiveness and a default value of 0.8 is used if no value is specified.  Furthermore, it is assumed that saturated vapor refrigerant exits the shell-and-coil intercooler at Location 9.
-
-For the flash intercooler shown in Figure 282, it is assumed that saturated liquid exits the intercooler at Location 3a and saturated vapor refrigerant exits the intercooler at Location 7.
-
-The two-stage compression refrigeration system may include an optional mechanical subcooler or liquid-suction subcooler.  These subcoolers cool the liquid refrigerant which exits the intercooler before the refrigerant enters the thermal expansion valve.  Further details regarding the modeling of mechanical and liquid-suction subcoolers may be found in the “Subcoolers� section.
-
-#### Condenser Performance
-
-Only one condenser is allowed per system. However, multiple refrigeration systems can reject heat through the same condenser. If a single condenser is used by multiple refrigeration systems, the code will iterate just as it does for loads transferred between systems to ensure that the total load on the condenser is accounted for in determining the saturated condensing temperature.
-
-The condenser can be modeled as dry air cooling, wet evaporative cooling, water loop cooling, or cascade cooling. (The detailed system can not be used for a compressor rack discharging heat into a conditioned zone.) The condenser performance is modeled to determine: (1) the condensing temperature and enthalpy of the refrigerant entering the refrigerated cases attached to the suction group, both of which will influence the efficiency of the compressors, (2) auxiliary power consumption for fans and pumps, and (3) water consumption for evaporative and water-cooled condensers.
-
-EnergyPlus can simulate waste heat being reclaimed from a detailed refrigeration system for use by refrigerant-to-air and refrigerant-to-water heating coils. (Refer to objects Coil:Heating:Desuperheater and Coil:WaterHeating:Desuperheater for a complete description of how these coils are modeled.) Heat reclaimed from the detailed refrigeration system is limited to the portion of the rejected heat in the superheat region. Using the state point nomenclature from Figure 280, this value is calculated by the detailed compressor and condenser models each time step as follows:
-
-<span>\(\)</span><span>\({\dot Q_{AvailableSuperheat}} = \dot m\left( {{h_{{\rm{2}}a}} - {h_{2b}}} \right)\)</span>
-
-Heat reclaimed for hot gas or hot brine defrost is not limited to the superheat range. However, if an excessive amount of the system rejected heat is diverted for that purpose, a warning is issued advising the user to increase the diversity of the defrost schedules.
-
-The total heat rejection load on the condenser is the sum of the case and walk-in loads, any transfer loads (e.g., mechanical subcooler or secondary system (see object Refrigeration:SecondarySystem)) on the system(s), and the total compressor power. The condenser load is reduced by any heat reclaimed by desuperheating coils for HVAC or water heating purposes and hot gas or hot brine defrost. If a secondary system or cascade condenser is served by the system(s) using this condenser, any defrost heat rejection credits from loads on the secondary system are assigned to this condenser.
-
-<div>$${\dot Q_{Rejected}} = \sum {{{\dot Q}_{System}}}  - \sum {{{\dot Q}_{Reclaimed}}} $$</div>
-
-where:
-
-<sub><span>\({\dot Q_{Rejected}}\)</span></sub>     = Heat rejected by the condenser (W)
-
-<span>\(\sum {{{\dot Q}_{Reclaimed}}} \)</span>= Sum of all the heat reclaimed by desuperheater coils and hot gas and hot brine defrost (W)
-
-Depending upon the condenser type, the heat rejection environment is set to the ambient conditions, conditions corresponding to a defined ouside air node (sometimes used to represent condensers located above ground level) or zone node, to a temperature specified for a water-cooled condenser, or according to the evaporating temperature for a higher-temperature loop (used for cascade condensers).
-
-The enthalpy of the condensed refrigerant leaving the condenser is equal to:
-
-<div>$${h_{condenser,out}} = {h_{sat,liquid}}({T_{condense}}) - {c_{p,sat,liquid}}({T_{condense}}) \times \Delta {T_{RatedSubcooling}}$$</div>
-
-where
-
-h<sub>condenser,out</sub>     = enthalpy leaving the condenser, J/kg
-
-h<sub>sat,liquid</sub>         = enthalpy of saturated liquid at the condensing temperature, J/kg
-
-c<sub>p,sat,liquid             </sub> = specific heat of saturated liquid at the condensing temperature, J/kg-C
-
-ΔT<sub>RatedSubcooling</sub>            = Amount of subcooling included in condenser rated heat rejection, C
-
-A minimum condensing temperature is specified for the detailed refrigeration system, and is usually required to maintain acceptable thermal expansion valve performance. When the calculated condensing temperature is less than this minimum, the air flow for air and evaporative-cooled condensers is reduced to reduce the condenser capacity and maintain the required condensing temperature.
-
-##### Air-Cooled Condensers
-
-The heat rejection capacity of a dry air-cooled condenser object (Refrigeration:Condenser:AirCooled) is directly proportional to the difference between the condensing temperature and the drybulb temperature for the heat rejection environment. The manufacturers typically provide the performance data, at one standard atmosphere, in a linear relationship between heat rejection and temperature difference. A correction factor is applied to account for the variation in air density with elevation (Carrier 1999).
-
-<div>$$\begin{array}{l}Hre{j_{Rated}} = {C_1} + {C_2} \times ({T_{condense}} - {T_{drybulb}})\\Hre{j_{Rated,corrected}} = Hre{j_{Rated}} \times \left( {1 - 7.17E - 5 \times Elevation} \right)\end{array}$$</div>
-
-where:
-
-Hrej<sub>Rated              </sub> = Manufacturer’s rated heat rejected by the condenser (W)
-
-C<sub>1</sub>   = Intercept taken from manufacturer’s condenser performance data (W)
-
-C<sub>2</sub>   = Coefficient taken from the manufacturer’s condenser performance data (W/C)
-
-T<sub>condense</sub> = Condensing temperature (C)
-
-T<sub>drybulb</sub>  = Drybulb temperature for the local environment (C)
-
-Elevation = Local elevation (m)
-
-The manufacturer’s form of performance data is used internally to define the condensing temperature as a function of the heat rejection load.
-
-<div>$${T_{condense}} = {T_{drybulb}} + \left( {\frac{{Hrej - {C_1}}}{{{C_2}}}} \right) \div (1 - 7.17E - 5 \times Elevation)$$</div>
-
-This calculated condensing temperature is then compared to the minimum condensing temperature allowed for that system. If necessary, the air flow to the condenser is reduced to maintain the condensing temperature at or above that minimum value.
-
-##### Condenser Fan Energy Use
-
-Condenser fan power for air-cooled condensers is determined by the type of fan control, fixed, variable speed, or two-speed. For all three fan control types, the fan power is set equal to the rated fan power whenever the calculated condensing temperature is greater than or equal to the minimum allowed condensing temperature. If the calculated temperature is less than the minimum allowed, the condenser air flow must be reduced. The reduced rated capacity is calculated using the previous equation for *Hrej<sub>Rated</sub>* with the specified minimum condensing temperature. (Note, the minimum condensing temperature is often determined by the expansion valve performance, and is therefore input with the system description, not with the condenser description.) The air flow for the reduced condenser capacity is:
-
-<div>$$\begin{array}{l}Hrej \propto {\left( {AirVelocity} \right)^N}\\ {\rm{Air Velocity}} \propto {\left( {Hrej} \right)^{1/N}}\\ {\rm{Air Volume Ratio}} = {\left( {\frac{{Hrej}}{{Hre{j_{Rated}}}}} \right)^{1/N}}\end{array}$$</div>
-
-where:
-
-N    =          0.633 for turbulent air flow over cylinders (ASHRAE 2005)
-
-The Air Volume Ratio is limited by a minimum value, which may be specified by the user. The default for this value is 0.2,
-
-
-
-Four fan curves are built into the condenser fan model to represent four types of fan control, as shown in Figure 283. (Lawrence Berkeley Laboratory and Resource Dynamics, April 2003)
-
-![](media/image6291.svg.png)
-
-Figure 283. Condenser fan power curve options
-
-For a fixed-speed fan, the air flow is reduced through either the use of dampers or by cycling the fan on and off.
-
-For a cycling fan, the power variation with air flow volume is approximately linearabove the minimum air volume ratio as shown in the following equation for the option “FixedLinear�:
-
-<div>$${P_{CondFan}} = ({\rm{Air Volume Ratio}}){P_{CondFan,design}}$$</div>
-
-where:
-
-<span>\({P_{CondFan}}\)</span>                  = output variable “Refrigerated Case Condenser Fan Electric Power [W]�, not allowed to exceed the design condenser fan power
-
-<span>\({P_{CondFan,design}}\)</span>           = design condenser fan power (W)
-
-For a fixed speed fan with damper (corresponding to the option “Fixed�), the shape of the power fraction curve is as shown above, and calculated using:
-
-<div>$${P_{CondFan}} = ({\rm{Air Volume Ratio}}){e^{(1 - {\rm{Air Volume Ratio}})}}{P_{CondFan,design}}$$</div>
-
-For an ideal variable speed fan, the power is proportional to the cube of the air flow. To reflect non-ideal real systems, an exponent of 2.5 is used as shown in the following equation:
-
-<div>$${P_{CondFan}} = {({\rm{Air Volume Ratio}})^{2.5}}{P_{CondFan,design}}$$</div>
-
-For a two-speed fan, the fan power is varied as for a constant speed fan with dampers for Air Volume Ratios greater than or equal to 0.6. For lower Air Volume Ratios,  which correspond to a half-speed fan setting, the power is reduced to the variable fan power value at that point and then varied as for damper control below Air Volume Ratios of 0.6.
-
-<div>$$\begin{array}{*{20}{c}}{{P_{CondFan}} = ({\rm{Air Volume Ratio}})\left( {{e^{(1 - {\rm{Air Volume Ratio}})}}} \right){P_{CondFan,design}}{\rm{      for Air Volume Ratio}} \ge 0.6}\\ {{P_{CondFan}} = \left( {\frac{{{\rm{Air Volume Ratio }} + {\rm{ 0}}{\rm{.4}}}}{{{{\rm{2}}^{{\rm{2}}{\rm{.5}}}}}}} \right)\left( {{e^{(1 - {\rm{Air Volume Ratio}})}}} \right)\left( {{P_{CondFan,design}}} \right){\rm{    for Air Volume Ratio }} &lt; {\rm{ 0}}{\rm{.6}}}\end{array}$$</div>
-
-For a water cooled condenser, there is no fan load at the condenser (i.e., the  water/refrigerant heat exchanger). Any fan load would be related to and accounted for at the heat rejection object (e.g., cooling tower)
-
-##### Evaporative-Cooled Condensers
-
-The input object Refrigeration:Condenser:EvaporativeCooled allows using evaporative cooling rather than dry air cooling which will allow for more efficient condenser heat rejection based on the entering air approaching the wet-bulb temperature rather than the dry-bulb temperature. Analyses under the International Energy Agency’s (IEA) Heat Pumping Programme Annex 26 indicates that this measure can improve refrigeration system efficiency by up to 10% (IEA 2003). The basin heater energy and water pumping power consumption for evaporative condensers in the detailed refrigeration system is modeled as described for the Refrigeration:CompressorRack. Just as for air-dried condensers, an elevation correction is needed to adjust for the variation in density of the air. This correction factor was derived by combining the barometric pressure correction from ARI 490 and a standard correlation for barometric pressure as a function of elevation(ARI 2008, NASA 1976).
-
-<div>$$\begin{array}{l}Hre{j_{Rated,Corrected}} = Hre{j_{Rated}} \times \left[ {1 + {k_1}B{P_{std}}(1 - {e^{(A \times Elev)}})} \right]\\A = \frac{{{g_0} \times {M_0}}}{{{R^*} \times {T_b}}} =  - 0.00012{m^{ - 1}}\end{array}$$</div>
-
-where
-
-k<sub>1</sub>               =          0.0023 for pressure stated in kPa, (ARI 2008)
-
-BP<sub>std</sub>           =          Standard atmosphere at rating conditions (101.0 kPa)
-
-g<sub>0</sub>               =          Gravitational constant (9.80665 m/s<sup>2</sup>)
-
-R\*               =          Universal gas constant (8.31432E3 N-m/kmol-K
-
-M<sub>0</sub>              =          Molar mass of air (28.9644 kg/kmol)
-
-T<sub>b</sub>               =          Standard temperature (288.15 K)
-
-Although based upon an exponential relationship, the resulting correction is very nearly linear within the range of elevations found upon dry land, so the following form of correction is used:
-
-<div>$$Hre{j_{Rated,Corrected}} = Hre{j_{Rated}} \times (1 - 3.07E - 5 \times Elevation)$$</div>
-
-To calculate the condensing temperature for an evaporative cooled condenser, it is necessary to provide the manufacturer’s performance data. The manufacturers typically provide this data as a table of condensing temperature as a function of both entering wet-bulb temperature and the ratio of the heat rejected to the rated heat rejected. This data can be well represented, as shown in Figure 284, by a regression of the form:
-
-<div>$$\begin{array}{l}({T_{condense}} - {T_{wetbulb}}) = {C_1} + {C_2} \times HRCF + \frac{{{C_3}}}{{HRCF}} + {C_4}{T_{wetbulb}},or\\ {T_{condense}} = {C_1} + {C_2} \times HRCF + \frac{{{C_3}}}{{HRCF}} + (1 + {C_4}){T_{wetbulb}}\\ {\rm{where:  }}HRCF = \frac{{Hre{j_{Rated}}}}{{Hrej}}\end{array}$$</div>
-
-C<sub>1</sub>, C<sub>2</sub>, C<sub>3</sub>, and C<sub>4</sub>     =          Coefficients determined by regression from manufacturer’s data.
-
-Figure 284 shows a comparison between this equation form, which produced an adjusted R<sup>2</sup> of 0.998 and a maximum residual of 0.7C, for one manufacturer of evaporative condensers. Data from two other manufacturers showed similar agreement with this parameterization.
-
-![](media/image6301.svg.png)
-
-Figure 284. Comparison of the condensing temperature predicted by four-factor equation to manufacturer's data
-
-Again, the condensing temperature is not allowed to fall below the system’s minimum allowed condensing temperature. Just as with an air-cooled condenser, the air flow through the condenser is controlled to maintain this minimum condensing temperature and the air velocity reduction is a function of the decreased capacity (Manske, 1999). For an evaporative condenser, relevant capacity is not the amount of heat rejected, but the rated capacity at that reduced air flow. That decreased rated capacity must first be calculated based upon the specified minimum condensing temperature. Using Equation , the specified condensing temperature is used to calculate the reduced HRCF, which is used with the current heat rejection to calculate the “reduced Rated Heat Rejection�.
-
-<div>$$\begin{array}{l}{\rm{0}} = {C_2} \times HRC{F^2} + (({C_1} + {C_4}{T_{wetbulb}} - ({T_{condense}} - {T_{wetbulb}})) \times HRCF + {C_3}\\ {\rm{Reduced Rated Heat Rejection}} = HRCF \times Hrej\\ {\rm{Air Volume Ratio}} = {\left( {\frac{{{\rm{Reduced Rated Heat Rejection}}}}{{Hre{j_{Rated}}}}} \right)^{1/N}}\end{array}$$</div>
-
-where:
-
-N = exponent for evaporative condensers, set to 0.76 (Manske, 1999)
-
-The water consumption for an evaporative condenser is calculated based upon the air flow rate, the total heat rejection, and the heat rejection environment. The amount of water consumption also includes the amount of water that is purged to reduce the concentration of contaminants. The purge water is estimated as proportional to the heat rejection, at a rate of 5.0E-10 m<sup>3</sup>/s per Watt of heat rejection (B.A.C., 2007). (This value, which corresponds to 3 gal./min. per 100 tons, is slightly more conservative than the value quoted by ASHRAE, 2004.) For the compressor racks, the condenser effectiveness was input as a function of the environmental wetbulb temperature. For the detailed evaporative condenser, the input data instead describes the capacity as a function of environmental conditions and loading. From that data, the water evaporation is calculated using the effectiveness corresponding to a fully loaded condenser. When the condenser is operating outside the bounds of the manufacturer’s data, the effectiveness is limited to a maximum value of 0.9.
-
-<div>$$\begin{array}{l}\eta  = \frac{{Hrej}}{{{{\dot V}_{air,rated}} \times {\rho_{air}} \times ({{\left. h \right|}_{Tcondense,sat}} - {h_{air,in}})}}\\ {h_{air,out}} = {h_{air,in}} + \eta  \times ({\left. h \right|_{Tcondense,sat}} - {h_{air,in}})\\ {T_{air,out}} = {T_{saturated}}({h_{air,out}},{P_{barometric}})\\ {{\dot V}_{evaporation}} = \frac{{AirVolumeRatio \times {{\dot V}_{air,rated}} \times {\rho_{air,dry}} \times ({\omega_{air,out}} - {\omega_{air,in}})}}{{{\rho_{water}}}}\\ {{\dot V}_{makeup}} = {{\dot V}_{evaporation}} + {{\dot V}_{purge}}\end{array}$$</div>
-
-where:
-
-<span>\({\left. h \right|_{Tcondense,sat}}\)</span>=enthalpy of saturated air at the calculated condensing temperature
-
-h<sub>air,out</sub> = enthalpy of the air leaving the condenser,
-
-h<sub>air,in</sub> = enthalpy of the inlet air, psychometric function of inlet air drybulb temperature and humidity ratio
-
-<span>\({\dot V_{air,rated}}\)</span>= rated volumetric air flow for the evaporative condenser (input value) m<sup>3</sup>/s
-
-�<sub>air</sub> = density of air evaluated at environmental conditions
-
-�<sub>air,dry</sub> = density of dry air evaluated at environmental temperature
-
-T<sub>air,out</sub> = air temperature leaving the condenser, psychometric function of saturated air at the enthalpy leaving the condenser and the barometric pressure
-
-<span>\({\dot V_{evaporation}}\)</span>= Volumetric rate of water evaporation in the condenser, m<sup>3</sup>/s
-
-ω<sub>air,out</sub>= humidity ratio (kg<sub>water</sub>/kg<sub>dry\\ air</sub>) of the air leaving the condenser, psychometric function of T<sub>air,out</sub> and the barometric pressure
-
-ω<sub>air,in</sub>= humidity ratio (kg<sub>water</sub>/kg<sub>dry\\ air</sub>) of the air at environmental conditions
-
-�<sub>water</sub> = density of water evaluated at the environmental wetbulb temperature (kg/m<sup>3</sup>)
-
-<span>\({\dot V_{purge}}\)</span>= Volumetric rate of water purged in the condenser, m<sup>3</sup>/s
-
-<span>\({\dot V_{makeup}}\)</span>= Volumetric rate of water makeup in the condenser, m<sup>3</sup>/s
-
-The source of the makeup water may be specified as a water storage tank. If not specified, the makeup water is assumed to come from the building mains (Ref. Water Mains Temperatures).
-
-An evaporative condenser can be scheduled, using the Evaporative Condenser Availability Schedule described previously, so that it operates in a dry mode for a portion of the year. This is important in climates subject to freezing weather in order to avoid excessive ice formation on the condenser surfaces and surroundings. (The Availability Schedule is the correct way to model the use of evaporative condensers in cold climates. However, some users may take a single input description and use it to model a building with a refrigeration system in a variety of climates. To avoid modeling the use of evaporative coolers in freezing weather, the code includes a cutout to switch to dry operation whenever the outdoor drybulb temperature drops below 4C.) Dry operation can also reduce water use when the dry heat rejection capacity of the equipment is sufficient to meet the load during times of the year when the outside drybulb temperature is reduced. In dry operation, the condenser heat rejection capacity is approximately one third of the rated wetted heat rejection capacity(Manske, 2000). In dry operation, the condensing temperature is estimated by using the same four-factor equation, but using the air drybulb temperature instead of the wetbulb temperature and using the reduced heat rejection capacity factor.
-
-<div>$$\begin{array}{l}HRC{F_{{\rm{dry operation}}}} = HRC{F_{{\rm{wet operation}}}}/3.0\\ {T_{{\rm{condense,dry operation}}}} = {C_1} + {C_2} \times HRC{F_{{\rm{dry operation}}}} + \frac{{{C_3}}}{{HRC{F_{{\rm{dry operation}}}}}} + (1 + {C_4}){T_{drybulb}}\end{array}$$</div>
-
-##### Water-Cooled Condensers
-
-If the condenser heat rejection is specified as water cooled (input object Refrigeration:Condenser:WaterCooled), the model uses the same algoithms described above for Refrigeration Compressor Racks. The condensing temperature is set equal to the inlet water temperature plus an approach temperature equal to the difference between the rated values for water inlet temperature and condensing temperature.
-
-##### Cascade Condensers
-
-A cascade condenser joins two full detailed refrigeration systems; that is, both systems joined by the cascade condenser have loads, compressor(s), and a condenser, as shown in Figure 285.
-
-![Cascade](media/image6310.png)
-
-Figure 285. A cascade condenser is used to reject heat from a low-temperature detailed refrigeration system to a higher-temperature detailed refrigeration system
-
-The input object, Refrigeration:Condenser:Cascade, allows the use of a higher temperature refrigeration system (primary system) to serve as a heat rejection sink for a lower temperature refrigeration system (secondary system). The selection of the condensing temperature represents a trade-off in performance between the primary system absorbing the heat rejection and the secondary system rejecting heat. (Lee et al., 2006) If the condensing temperature control type is ‘fixed,’ then the secondary system condensing temperature is held constant at the temperature specified for that cascade condenser (which should be greater than or equal to the secondary system’s specified minimum condensing temperature). If the condensing temperature control type is ‘float’, the condensing temperature is allowed to float according to the minimum required evaporating temperature for other loads served by the primary system.
-
-For fixed control:  T<sub>condense</sub> = T<sub>condense,rated</sub>
-
-For floating control: T<sub>condense</sub> = ΔT<sub>approach</sub> + T<sub>evap,min</sub>
-
-where
-
-T<sub>condense,rated</sub>    =          Rated condensing temperature for the cascade condenser, C
-
-ΔT<sub>approach</sub>      =          Rated approach temperature difference for the cascade condenser, DeltaC
-
-T<sub>evap,min</sub>         =          Evaporating temperature required to meet other loads on the primary system, C.
-
-The approach temperature difference (the difference between the condensing and evaporating temperatures) in the cascade condenser, is held constant at the rated value.  That is, the approach temperature difference is not varied according to the load on the condenser.
-
-For cases and walk-ins served by cascade condensers, energy needed for hot brine or hot gas defrost is reclaimed from the primary system.  The refrigeration load the cascade condenser places upon the primary system is classified as a ‘transfer load’, because it transfers load from one system to another. This load is the sum of all case and walk-in loads served by the secondary system, any suction piping heat gains on the secondary loop, plus the secondary loop’s compressor power. The same name (Ref. Refrigeration:Condenser:Cascade, field “Name�) used to identify the condenser in the secondary loop is used to identify the transfer load on the primary system.
-
-<div>$${\dot Q_{{\rm{Cascade}}}} = {\sum {\dot Q}_{{\rm{Case}}}} + \sum {{{\dot Q}_{{\rm{Walkin}}}} + } \sum {{{\dot Q}_{{\rm{Compressor}}}}} \left( { + \sum {{{\dot Q}_{{\rm{PipeHeatGain}}}}} } \right)$$</div>
-
-where
-
-<span>\({\dot Q_{Cascade}}\)</span>      = Total refrigeration load the cascade condenser places upon the primary system, W
-
-<span>\({\dot Q_{Case}}\)</span>         = Case load on the secondary loop , W
-
-<span>\({\dot Q_{Walkin}}\)</span>        = Walk-in load on the secondary loop, W
-
-<span>\({\dot Q_{Compressor}}\)</span>   = Power input to a compressor on the secondary loop, W
-
-<span>\({\dot Q_{PipeHeatGain}}\)</span>= Heat gain in secondary loop suction pipe, W
-
-**Even though a cascade condenser is considered to be a part of a secondary loop, that loop is described with the Refrigeration:System object, not with the object, Refrigeration:SecondarySystem, described below.**
-
-#### Subcoolers
-
-Subcooler objects (Refrigeration:Subcooler) reduce the temperature of the liquid refrigerant after it leaves the condenser and before it reaches the thermal expansion valve, corresponding to state point, 3b, on Figure 280. The detailed refrigeration system permits the use of two type of subcoolers, mechanical and liquid suction. A mechanical subcooler is used to transfer refrigeration load from a lower-temperature system to a higher-temperature system. For example, the compressors that are used to provide cooling for dairy products could be used to subcool the refrigerant in another system that is serving frozen food cases. For the system providing the cooling, the mechanical subcooler acts like another refrigerated case load. For the system receiving the cooling, the mechanical subcooler reduces the enthalpy of the refrigerant from point 3a to point 3b on Figure 280, and thus reduces the required refrigerant flow rate. Mechanical subcooler performance is defined by the controlled temperature of the subcooled liquid as follows:
-
-<div>$$\begin{array}{l}\dot Q = \dot m \times {c_p}({T_{3a}} - {T_{control}})\\ {h_{3b}} = {h_{3a}} - {c_{p,liquid}}({T_{3a}} - {T_{control}})\end{array}$$</div>
-
-where:
-
-<span>\(\dot Q\)</span>= subcooler load, W
-
-<span>\(\dot m\)</span>= mass flow rate of refrigerant, kg/s
-
-c<sub>p,liquid</sub>          = specific heat of saturated liquid at the condensing temperature, J/kg-C
-
-T<sub>control</sub>           =control temperature specified for the mechanical subcooler, C
-
-h    = enthalpy, J/kg
-
-A liquid suction heat exchanger (LSHX) subcooler uses the cold gas exiting the refrigerated cases to subcool the condensed liquid refrigerant in the same system. Depending upon the shape of the refrigerant’s saturation curve and the operating condensing and evaporating temperature, this can save significant energy by reducing the required refrigerant flow (ASHRAE 2006a). (This model neglects the pressure drop through the suction side of the heat exchanger, although this pressure drop will cause the compressor to operate at a lower suction pressure.) A liquid suction heat exchanger is defined by specifying the design values for: inlet liquid temperature, inlet vapor temperature, and liquid temperature change. A liquid suction heat exchanger subcooler will also increase the superheat of the gas returning to the compressor, as shown by the difference between state points 1a and 1b in Figure 280:
-
-<div>$$\begin{array}{l}{\eta_{LSHX}} = \frac{{\Delta {T_{Design}}}}{{\left( {{T_{{\rm{Liquid Design}}}} - {T_{{\rm{Vapor Design}}}}} \right)}}\\ dot Q = \dot m \times {c_{p,liquid}}{\eta_{LSHX}}({T_{3a}} - {T_{1a}})\\ {T_{1b}} = {T_{1a}} + \frac{{\dot Q}}{{\dot m{c_{p,vapor}}}}\\ {h_{3b}} = {h_{3a}} - \frac{{\dot Q}}{{\dot m}}\end{array}$$</div>
-
-where:
-
-ηLSHX        = subcooler effectiveness, dimensionless
-
-c<sub>p,vapor</sub>          = specific heat of saturated vapor at the evaporating temperature, J/kg-C
-
-ΔT<sub>Design</sub>        =design liquid temperature difference, DeltaC
-
-T<sub>LiquidDesign</sub>     = design liquid inlet temperature, C
-
-T<sub>VaporDesign</sub>     = design vapor inlet temperature, C
-
-If a system is subcooled by both a mechanical subcooler and a liquid subcooler, the liquid subcooler will follow the mechanical subcooler and those points labeled ‘3a’ in the liquid suction equations would correspond to the points labeled ‘3b’ in the mechanical subcooler equations, that is, the inlet of the LSHX would be the outlet of the mechanical subcooler.
-
-Any one system can be cooled (i.e., have energy removed between points ‘3a’ and ‘3b’) by at most one liquid suction heat exchanger and one mechanical subcooler. However, a system can provide cooling to multiple mechanical subcoolers. For example if a building had one high temperature refrigeration system (perhaps cooling fresh produce) and three low temperature systems (perhaps cooling frozen foods and meat), each of the three low temperature systems could include a mechanical subcooler with the refrigeration energy for all three absorbed by the one high-temperature system. For the compressors and condenser on the high-temperature system, these three mechanical subcoolers would represent a load very similar to that of the refrigerated cases served by that system.
-
-#### Suction Piping Heat Gains
-
-Suction piping heat gain is an optional element in the load calculation.  Typically, the suction pipe heat gain is small compared to the other loads.  However, when comparing DX systems to secondary systems, this portion of the total load can be very different. (Hinde, D., et al. 2009)  To include the suction pipe heat gain load, the user must first calculate the U-value and outer surface area for the suction piping. The U-value is the total conductance from the inside skin coefficient, through the pipe insulation, to the outside skin coefficient. This value must be multiplied by the external surface area of the pipe insulation to provide the sum of the UA required in the input.  These piping heat gains are also reflected in the zone heat balance.
-
-<span>\({\dot Q_{PipeHeatGain}}\)</span> = ∑U\*A (T<sub>zone</sub> – T<sub>SaturatedSuction</sub>)
-
-Where:
-
-    <span>\({\dot Q_{PipeHeatGain}}\)</span>  =  Heat load on the detailed refrigeration system due to suction pipe heat gains (W)
-
-    ∑U\*A =   Sum of the product of the conductance times the surface area for the suction piping (W/C)
-
-### Secondary Refrigeration Systems
-
-The object, Refrigeration:SecondarySystem, is used to model systems that do not have compressors, but have a circulating pump and a heat exchanger (called the secondary evaporator) where evaporating refrigerant in the primary loop absorbs heat rejected by the secondary loop.  The purpose of the secondary refrigeration system model is to determine: the refrigerating load placed upon the primary system via the Secondary Evaporator, the required evaporating temperature in the Secondary Evaporator, any heat recovered for defrost purposes, and the total pump power.
-
-If your secondary loop includes compressors and a cascade condenser, do NOT use a Refrigeration:SecondarySystem object.  Use a Refrigeration:System object with a Refrigeration:Condenser:Cascade object and list that condenser as a transfer load in the input description of the primary system.
-
-In the secondary loop shown in Figure 286, the secondary evaporator serves to chill a brine or glycol solution (single phase) that in turn chills the refrigeration loads on the secondary loop.  In Figure 287, the secondary evaporator serves as a condenser for a refrigerant that has been partially vaporized(two-phase) while circulating through the refrigeration loads on the secondary loop. Every secondary system includes a refrigeration load made up of refrigerated cases and/or walkins, a heat exchanger (called the Secondary Evaporator), and circulating pump(s). The loop performance at any one time step is determined by the effectiveness of the heat exchanger, the refrigeration load, and the pumping power needed to meet that load. The fluid temperature entering the cases and walk-ins is maintained at a set value.
-
-
-
-![brinesecondary](media/image6323.png)
-
-Figure 286. Secondary loop with brine or glycol solution circulation
-
-
-
-![liquidoverfeedsecondary](media/image6324.png)
-
-Figure 287. Secondary loop with liquid-overfeed refrigerant circulation
-
-For both types of secondary loops, the primary refrigeration system absorbs the load by providing cold refrigerant that evaporates in the secondary evaporator.  We classify this secondary load as a ‘transfer load’ because it transfers load from one ‘system’ to another. (Cascade condenser loads are also considered transfer loads.) Just as with any DX refrigeration evaporator, the variable load from the secondary system is served by varying the primary system refrigerant flow to the evaporator side of the secondary evaporator.  Unmet load will be carried over to the next time step anytime the load on the secondary condenser/evaporator exceeds the rated capacity for the specified temperatures.  (A warning will be generated if the total unmet energy grows excessively large.)  The main differences between the single-phase secondary loop model and the two-phase secondary loop model lie in the definition and performance of the secondary evaporator and the way input data is processed to define evaporator capacity.
-
-For a brine system, the secondary loop capacity is matched to the case and walk-in load by varying the brine flow rate. (*Throughout this section, ‘brine’ will be used when referring to the secondary loop heat transfer fluid for systems where the secondary circulating fluid remains in the liquid state.)* When selecting the brine loop design parameters, it is important to consider the performance trade-off between pumping energy and the temperature difference, or range, in the heat exchanger. The circulating fluid selection is also critical in determining the performance of brine loop, with large variations caused by differences in viscosity and density (which impact pumping power requirements) and specific heat (which determines the required fluid flow rate).  (Kazachki, G. S., and Hinde, D. K., 2006, Faramarzi, R. T., and Walker, D. H. 2004, ASHRAE. 2006c)
-
-For a secondary loop to accommodate a two-phase secondary coolant, additional hardware is required and the system control mode changes. A separator/receiver is required to separate the wet mixture of liquid and gas returning from the refrigeration load, as shown in Figure 287.  (In the following discussion, we will refer to the secondary fluid in a liquid-overfeed system as CO<sub>2</sub>.) In Figure 288, which focuses in on the secondary loop alone, the gaseous CO<sub>2</sub> moves via thermosiphon effect to the secondary evaporator, where heat is absorbed by the primary system to condense the CO<sub>2</sub>, which then returns via gravity flow to the separator/revceiver.  The liquid CO<sub>2</sub> is pulled from the bottom of the separator/receiver and pumped to the load. The term ‘liquid overfeed ratio’ refers to the ratio of the total pumped mass flow rate (at the point labeled “1� on Figure 288) of CO<sub>2</sub> to the mass rate of CO<sub>2</sub> evaporated at the load (vapor portion of the flow at the point labled “5� on Figure 288). With a variable flow rate(obtained with either a variable-speed pump or multiple constant-speed pumps), the liquid overfeed ratio is maintained at or above the specified value. With a constant flow rate (obtained by specifying a single constant-speed pump), the liquid overfeed ratio will vary to match the capacity of the variable refrigeration load.(Hinde et al 2009) Even though a greater amount of CO<sub>2</sub> is circulated than is evaporated, the pumping power requirements are still much less than those for a single-phase secondary coolant.
-
-![DanfossCO2cycle](media/image6325.png)
-
-Figure 288. Thermodynamic cycle for a liquid overfeed secondary loop
-
-If the defrost type for any of the cases or walkins on the secondary loop is ‘HotBrine’ or ‘HotGas’, the defrost energy is assumed to come from the hot compressed gas leaving the compressors on the primary system, as shown in Figure 286 and Figure 287.(Minea, V. 2007) Therefore, the amount of heat rejected by the condenser for that primary system is reduced by the amount needed for defrost. Some research has shown that the defrost times for cases and walk-ins defrosted using hot brine can be significantly shorter than defrost times for electric or hot gas.(Terrell, W. J. Jr., 1999) The user should consider this factor when describing the input data for cases and walk-ins served by a secondary loop.
-
-#### Secondary Evaporator in a Single-Phase Secondary Loop (Brine or Glycol Loop)
-
-For a single-phase secondary system, the heat exchanger effectiveness is calculated based upon the input rating data, which includes the evaporating temperature, approach and range temperature differences, and heat exchanger capacity. The rated capacity for the heat exchanger can be specified by either providing the capacity in Watts, or the rated mass flow rate. The density and specific heat both correspond to those properties at the average temperature of the heat exchange fluid within the secondary loop heat exchanger.
-
-These variables are specified by the chiller manufacturer at rated conditions:
-
-  ΔT<sub>Approach</sub>                = the approach temperature difference, DeltaC
-
-  ΔT<sub>Range</sub>                  = range temperature difference, DeltaC
-
-  T<sub>EvapDesign</sub>                =  heat exchanger evaporating temperature, C
-
-  Flow<sub>RatedVolume</sub>          = brine flow rate through the heat exchanger  (kg/s)
-
-  Capacity<sub>Rated</sub>          = Heat exchanger cooling capacity (W)
-
-The rated conditions are used to calculate:
-
-  T<sub>BrineOutRated</sub> = T<sub>EvapDesign</sub> + ΔT<sub>Approach</sub>
-
-  T<sub>BrineInRated</sub>  = T<sub>BrineOutRated</sub> + ΔT<sub>Range</sub>
-
-  Eta = Capacity<sub>Rated</sub> / (Flow<sub>RatedMass</sub> \* C<sub>pBrine</sub> \* (T<sub>BrineInRated</sub> - T<sub>EvapDesign</sub>))
-
-  T<sub>BrineAverage</sub>= (T<sub>BrineOutRated</sub> + T<sub>BrineInRated</sub>)/2
-
-If the capacity is specified and the flow rate is not, then the flow rate is calculated as:
-
-Flow<sub>RatedMass</sub>= Capacity<sub>Rated</sub>/(C<sub>pBrine</sub>\*ΔT<sub>Range</sub>)
-
-Flow<sub>RatedVol </sub> = Flow<sub>RatedMass</sub> / �<sub>Brine</sub>
-
-If the flow rate is specified and the capacity is not, the capacity is calculated as:
-
-Flow<sub>RatedMass</sub> =Flow<sub>RatedVol</sub>\*�<sub>Brine</sub>
-
-Capacity<sub>Rated</sub> = Flow<sub>RatedMass</sub> \* C<sub>pBrine</sub>\*ΔT<sub>Range</sub>
-
-Where:
-
-  Eta                       = heat exchanger effectiveness, dimensionless and less than one
-
-  T<sub>BrineInRated\\      </sub>            = heat exchanger brine inlet temperature at rated conditions (C)
-
-  T<sub>BrineOutRated</sub>              = heat exchanger brine outlet temperature at rated conditions (C)
-
-  T<sub>BrineAverage</sub>               = average brine temperature in the heat exchanger (C)
-
-  Flow<sub>RatedMass</sub>           = brine flow rate through the heat exchanger  (kg/s)
-
-  Flow<sub>RatedVol</sub>             = brine flow rate through the heat exchanger  (m<sup>3</sup>/s)
-
-  C<sub>pBrine</sub>                    = brine specific heat (J/kg-C)
-
-  �<sub>Brine</sub>                      = brine density (kg/m<sup>3</sup>)
-
-After the heat exchanger effectiveness has been calculated, the value for the heat exchanger design brine flow rate is compared to the design flow rate for the secondary loop pump(s).  The maximum flow rate in the loop is limited to the smaller of these two values. The heat transfer capacity corresponding to this maximum flow rate is then calculated and compared to the rated heat exchanger capacity. The maximum load on the heat exchanger is limited to the lesser of these two values, the rated heat exchanger capacity or the capacity corresponding ot the maximum loop flow rate.
-
-Flow<sub>MaxVol</sub> = Minimum(Flow<sub>RatedVol</sub> ,Flow<sub>RatedPumpVol</sub>)
-
-Capacity<sub>AtMaxVolFlow</sub> =Flow<sub>MaxVol</sub> \*Eta\*( C<sub>pBrine</sub> \* Density<sub>Brine</sub>)\*( T<sub>BrineInRated</sub> – T<sub>EvapDesign</sub>)
-
-Capacity<sub>Max</sub> = Minmum(Capacity<sub>Rated</sub> , Capacity<sub>AtMaxVolFlow</sub>)
-
-Where:
-
-Flow<sub>MaxVol</sub>                 = Maximum loop volume flow, limited by either the pump rating or the heat exchanger rating (m<sup>3</sup>/s)
-
-Capacity<sub>AtMaxVolFlow</sub>     = Secondary loop capacity corresponding to the maximum loop flow rate (W)
-
-Capacity<sub>Max</sub>              = Maximum secondary evaporator capacity (W)
-
-#### Secondary Evaporator in a Two-Phase Secondary Loop  (Liquid-Overfeed Loop, e.g., CO<sub>2</sub>)
-
-For a two-phase system, the secondary evaporator effectiveness is not calculated. Both the evaporating and condensing sides of the heat exchanger are assumed to operate at fixed temperatures.  If the capacity of the secondary evaporator is not input, it will be calculated as the sum of the rated loads plus the rated pump power.
-
-<div>$$\begin{array}{*{20}{c}}{Capacit{y_{{\rm{Rated}}}} = {\rm{Input,  OR}}}\\ {Capacit{y_{{\rm{Rated}}}} = \sum {{{\dot Q}_{{\rm{Case}}}} + \sum {{{\dot Q}_{{\rm{WalkIn}}}} + Powe{r_{{\rm{Pump}}}}} } }\\ {Capacit{y_{{\rm{Max}}}} = Capacit{y_{{\rm{Rated}}}}}\end{array}$$</div>
-
-If the flow rate through the evaporator is not input, it will be calculated based upon the input value for the Circulating Rate.
-
-<div>$$Flo{w_{{\rm{RatedVol}}}} = \frac{{\sum {{{\dot Q}_{{\rm{Case}}}} + \sum {{{\dot Q}_{{\rm{WalkIn}}}} + Powe{r_{{\rm{Pump}}}}} } }}{{{\rho_{Liquid}}\Delta {h_{fg}}}}$$</div>
-
-Where:
-
-  Ρ<sub>Liquid</sub>                     = liquid density (kg/m<sup>3</sup>)
-
-Δh<sub>fg</sub>                        = heat of vaporization (J/kg)
-
-#### Secondary Loop Distribution Piping and Receiver Shell Heat Gains
-
-Distribution piping and receiver shell heat gains are optional elements in the load calculation.  Typically, the distribution pipe and receiver shell heat gains are small compared to the other loads.  However, when comparing direct expansion systems to secondary systems, this portion of the total load can be very different. (Hinde, D., et al. 2009) To calculate the pipe heat gain load, the user must first calculate the U-value and area for the distribution piping. The U-value is the total conductance from the inside skin coefficient to the outside skin coefficient. This value must be multiplied by the piping external surface area to provide the sum of the UA required in the input.  Note that these piping and receiver shell heat gains are also reflected in the zone heat balance, similar to the zone cooling credits provided by refrigerated cases.
-
-<span>\({\dot Q_{PipeHeatGain}}\)</span> = ∑U\*A (T<sub>zone</sub> – T<sub>BrineAverage</sub>)
-
-Where:
-
-<span>\({\dot Q_{PipeHeatGain}}\)</span>  =  Heat load on the secondary loop due to pipe heat gains, output variable “Refrigeration Secondary Loop Pipe Heat Gain Rate [W]�
-
-∑U\*A =   Sum of the product of the conductance times the surface area for the piping (W/C)
-
-The receiver shell heat gains are calculated in the same manner.
-
-#### Secondary Loop Pumping Power and Secondary Loop Load
-
-Pump ratings are typically given in the form of curves. The input values for the pumps should correspond to the full-load design conditions, with respect to fluid viscosity, density, and temperature, as well as pressure drop. For these conditions, the user provides either the total pump power or the total head, as well as the flow rate. *These values must be representative of the selected heat transfer fluid at the average loop operating temperature and pressure.* If the pump head at design conditions is specified, the pump power is calculated as:
-
-Power<sub>PumpRated</sub> = Flow<sub>RatedPumpVol</sub>\* Head<sub>Rated</sub>/ (Efficiency<sub>PumpImpeller</sub>\*Efficiency<sub>PumpMotor</sub>)
-
-Where:
-
-Power<sub>PumpRated</sub>           =   Total pumping power for the secondary loop at rated conditions (W)
-
-Head<sub>Rated</sub>                 =  Pressure drop through the entire secondary loop circulation at rated conditions, including at the pumps, the chiller, supply and return piping, and through the case and walk-in coils (pipes are typically sized to produce a total head ranging from 0.25E6 to 0.3E6 Pa (ASHRAE. 2006c))(Pa)
-
-Efficiency<sub>PumpImpeller</sub>   = Pump impeller efficiency, dimensionless
-
-Efficiency<sub>PumpMotor</sub>     = Pump motor efficiency, dimensionless
-
-The pump impeller efficiency is assumed to be 78%. (ASHRAE 2006c) The pump motor efficiency is assumed to be 85%.(ITT 2009)  If a semi-hermetic motor is specified, all the pump power is translated to heat within the fluid. The total heat load placed upon the loop by the pumps is therefore:
-
-<span>\({\dot Q_{Pump}}\)</span> = Power<sub>PumpRated</sub> \* Ratio<sub>PowertoHeat</sub>
-
-Where:
-
-<span>\({\dot Q_{Pump}}\)</span>                     = total heat load placed upon the secondary loop by the pumps (W)
-
-Ratio<sub>PowertoHeat</sub>           = Ratio of total motor energy rejected to the circulating fluid to the total pump power used (input by the user, suggest 1.0 for semi-hermetic motors and 0.85 for others)
-
-A variable speed pump can be modeled by providing a cubic curve for pump power as a function of the ratio of total flow needed to the total flow specified at full load design conditions.
-
-<div>$${\dot Q_{Pump}} = \left[ {A{{\left( {L{F_{Pump}}} \right)}^3} + B{{\left( {L{F_{Pump}}} \right)}^2} + C\left( {L{F_{Pump}}} \right) + D} \right] \times {\rm{Powe}}{{\rm{r}}_{{\rm{PumpRated}}}} \times {\rm{Rati}}{{\rm{o}}_{{\rm{PowertoHeat}}}}$$</div>
-
-Where:
-
-LF<sub>Pump</sub>         = ratio of total flow needed to the total flow specified at full load design conditions
-
-The user may also specify multiple constant-speed pumps.  Multiple pumps, or pump staging, are often used to reduce the total pumping power requirements while still providing the capacity and constant pressure drop needed to meet peak design loads.(Faramarzi, R. T., and Walker, D. H. 2004) When multiple pumps are specified, the flow rate provided by one pump is compared to the flow rate needed to meet the refrigeration load on the loop during that time step. If that flow rate is insufficient, another pump is added, and the process is continued until the needed flow rate is met or all the pumps are included. The incremental power for each pump is added to determine the total pump power for the loop. Each pump is assumed to operate at full load if it is needed at all.  A bypass is assumed to carry any fluid flow not needed to meet the load.  An iterative solution is required for the total pump load on the heat exchanger because the flow rate is determined by the load, which includes the pump power that is determined by the necessary flow rate. For the first estimate, the pump power load is assumed to be zero.
-
-<div>$$\begin{array}{*{20}{c}}{{{\dot Q}_{{\rm{Refrigeration}}}} = \sum {{{\dot Q}_{{\rm{Case}}}} + \sum {{{\dot Q}_{{\rm{WalkIn}}}}} } }\\ {{{\dot Q}_{{\rm{TotalSecondary}}}} = {{\dot Q}_{{\rm{Refrigeration}}}} + {{\dot Q}_{{\rm{Pump}}}} + \left( {\sum {{{\dot Q}_{{\rm{Pipe and Receiver Shell heat gains}}}}} } \right)}\\ {{\rm{Flo}}{{\rm{w}}_{{\rm{needed}}}}{\rm{ }} = {\rm{ }}\frac{{{{\dot Q}_{{\rm{TotalSecondary}}}}}}{{Eta({C_{{\rm{p,Brine}}}})({\rho_{{\rm{Brine}}}})({T_{{\rm{BrineOutRated}}}} - {T_{{\rm{evap}}}})}}}\end{array}$$</div>
-
-Where:
-
-<span>\({\dot Q_{{\rm{Refrigeration}}}}\)</span> = output variable “Refrigeration Secondary Loop Load Heat Transfer Rate�
-
-<span>\({\dot Q_{{\rm{TotalSecondary}}}}\)</span> = Total load the secondary loop transfers to the primary system, output variable “Refrigeration Secondary Loop Total Heat Transfer Rate [W]�
-
-<span>\({\dot Q_{{\rm{Pump}}}}\)</span> = Pump power, function of Flow<sub>Needed</sub>, output variable “Refrigeration Secondary Loop Pump Electric Power [W]�
-
-Flow<sub>Needed</sub> = Flow rate needed to meet the loop refrigeration load, , output variable “Refrigeration Secondary Loop Volume Flow Rate [m3/]s�
-
-The needed flow rate is used to determine the number of pumps required and the total pumping power, which produces a new estimate for the total load. A few iterations converge upon the final secondary loop load for each time step.  The total load on the heat exchanger is therefore the sum of the refrigeration loads, any pipe heat gains, and the portion of the pump power that is absorbed by the circulating fluid.
-
-### Transcritical CO<sub>2</sub> Refrigeration System
-
-The Refrigeration:TranscriticalSystem object allows users to model detailed transcritical carbon dioxide (CO<sub>2</sub>) booster refrigeration systems used in supermarkets.  The object allows for modeling either a single stage system with medium-temperature loads or a two stage system with both medium- and low-temperature loads.
-
-The input objects required to model a detailed transcritical CO<sub>2</sub> refrigeration system include the following:
-
-n One Refrigeration:TranscriticalSystem object,
-
-n At least one refrigeration load object which may include any combination of the following:
-
-n Refrigeration:Case,
-
-n Refrigeration:WalkIn,
-
-n Refrigeration:CaseAndWalkInList (may include both cases and/or walk-in cooler names),
-
-n At least one Refrigeration:Compressor object (multiple compressors are entered using a Refrigeration:CompressorList),
-
-n One Refrigeration:GasCooler:AirCooled object,
-
-Output variables are available to describe the total heat exchange between all the refrigeration objects and the zones containing these objects.
-
-At least one refrigeration load object must be defined which may be one of two types of loads, including a refrigerated display case and a walk-in cooler, (Ref. Refrigeration:Case, and Refrigeration:WalkIn).  If multiple loads are served by the same system, the user should use the refrigerated case and walk-in list object available to assign all cases and walk-ins cooled directly by this system (Ref. Refrigeration:CaseAndWalkInList).
-
-The name of at least one compressor must be defined and a list object is available if the system is served by more than one compressor (Ref. Refrigeration:Compressor and Refrigeration:CompressorList).
-
-Heat is rejected to the outdoors via an air-cooled gas cooler (Ref. Refrigeration:GasCooler:AirCooled).
-
-The Refrigeration:TranscriticalSystem object coordinates the energy flows between the other refrigeration objects and is used to set system parameters.
-
-The inputs for the refrigeration system object, in addition to the names of the other refrigeration objects described above, include a name for this system, the minimum condensing temperature, and the refrigeration system working fluid.  Optional input fields are also provided for users seeking to keep track of refrigerant inventory and suction pipe heat gains.
-
-#### Transcritical CO<sub>2</sub> Refrigeration Cycles
-
-Transcritical CO<sub>2</sub> refrigeration cycles are characterized by a subcritical evaporation process and a supercritical “gas cooling� process.  In the subcritical evaporation process which occurs in the evaporator, the CO<sub>2</sub> changes phase from a liquid and vapor mixture to a superheated vapor.  In doing so, the CO<sub>2</sub> absorbs heat, thereby creating the cooling effect.  This process is similar to the evaporation process in a standard vapor-compression refrigeration cycle.
-
-After the CO<sub>2</sub> exits the evaporator and is compressed into the supercritical region, the CO<sub>2</sub> gas is cooled.  This gas cooling process differs from the condensation process which occurs in the standard vapor-compression refrigeration system.  In the standard refrigeration cycle, the refrigerant vapor is first desuperheated and then condensed to a liquid in the condenser.  In the transcritical CO<sub>2</sub> cycle, a “gas cooler� rather than a condenser is used to cool the supercritical CO<sub>2</sub> from the compressor discharge temperature to the expansion device inlet temperature.  No condensation occurs in this process.  Rather, the temperature and density of the CO<sub>2</sub> continuously changes from that at the compressor discharge to that at the expansion device inlet.
-
-EnergyPlus is capable of modeling the transcritical booster refrigeration cycle. Figure 289 shows a schematic of the booster cycle while Figure 290 shows the corresponding pressure-enthalpy (*p-H*) diagram of the booster cycle.
-
-
-
-![](media/image6337.png)
-
-Figure 289.  Schematic of the Transcritical CO<sub>2</sub> Booster Refrigeration Cycle.
-
-
-
-![](media/image6338.png)
-
-Figure 290.  Pressure-Enthalpy (*p-H*) Diagram for the Transcritical CO<sub>2</sub> Booster Refrigeration Cycle.
-
-Carbon dioxide exits the gas cooler at Location 1 and passes through the suction line heat exchanger, exiting at Location 2, during which the refrigerant is cooled by the suction gas.  An intermediate expansion occurs between Locations 2 and 3, and saturated CO<sub>2</sub> enters the receiver.  Saturated liquid CO<sub>2</sub> exits the receiver at Location 6, which is then expanded and fed to the medium-temperature loads (between Locations 7 and 8) and the low-temperature loads (between Locations 9 and 10).  Saturated vapor CO<sub>2</sub> exits the receiver bypass at Location 4 and is expanded to the medium-temperature pressure level at Location 5.  Carbon dioxide vapor exiting the low temperature loads is compressed to the medium-temperature pressure level (Location 10 to 11).  The CO<sub>2</sub> from the discharge of the low pressure compressors, the outlet of the medium-temperature loads and the outlet of the receiver bypass are then combined at Location 13.  The CO<sub>2</sub> suction gas then passes through the suction line heat exchanger where the refrigerant is heated, exiting at Location 14.  The carbon dioxide is finally compressed to the gas cooler pressure level at Location 15 and heat is rejected to the surroundings in the gas cooler between Locations 15 and 1.
-
-#### CO<sub>2</sub> Compressor Performance Modeling
-
-To model the performance of the CO<sub>2</sub> compressors during subcritical and transcritical operation, cubic polynomials are used to curve fit manufacturers’ performance data.  This technique is similar to that described in AHRI Standard 540 (AHRI 2004).  For subcritical operation, the power consumption and cooling capacity of a CO<sub>2</sub> compressor is a function of the saturated suction temperature, *t<sub>ss</sub>* (°C), and the saturated discharge temperature, *t<sub>sd</sub>* (°C), as follows:
-
-<div>$$z = {C_1} + {C_2}{t_{ss}} + {C_3}{t_{sd}} + {C_4}t_{ss}^2 + {C_5}{t_{ss}}{t_{sd}} + {C_6}t_{sd}^2 + {C_7}t_{ss}^3 + {C_8}t_{ss}^2{t_{sd}} + {C_9}{t_{ss}}t_{sd}^2 + {C_{10}}t_{sd}^3$$</div>
-
-where *z* is either power consumption (W) or cooling capacity (W) and *C<sub>x</sub>* are the corresponding correlation coefficients.
-
-For transcritical operation, the power consumption (in Watts) of a CO<sub>2</sub> compressor, *W*, is a function of the saturated suction temperature and the gas cooler pressure, *p<sub>gc</sub>* (Pa), as follows (Ge and Tassou 2011):
-
-<div>$$W = {C_1} + {C_2}{t_{ss}} + {C_3}{p_{gc}} + {C_4}t_{ss}^2 + {C_5}{t_{ss}}{p_{gc}} + {C_6}p_{gc}^2 + {C_7}t_{ss}^3 + {C_8}t_{ss}^2{p_{gc}} + {C_9}{t_{ss}}p_{gc}^2 + {C_{10}}p_{gc}^3$$</div>
-
-The cooling capacity (in Watts) of a transcritical CO<sub>2</sub> compressor, *Q*, is a function of the saturated suction temperature and the gas cooler outlet enthalpy, *h<sub>go</sub>* (J/kg), as follows (Ge and Tassou 2011):
-
-<div>$$Q = {C_1} + {C_2}{t_{ss}} + {C_3}{h_{go}} + {C_4}t_{ss}^2 + {C_5}{t_{ss}}{h_{go}} + {C_6}h_{go}^2 + {C_7}t_{ss}^3 + {C_8}t_{ss}^2{h_{go}} + {C_9}{t_{ss}}h_{go}^2 + {C_{10}}h_{go}^3$$</div>
-
-The correlation coefficients, *C<sub>x</sub>*, are obtained either directly from CO<sub>2</sub> compressor manufacturers or from cubic curve fits performed on their published CO<sub>2</sub> compressor performance data.  For convenience, correlation coefficients for CO<sub>2</sub> compressors from several manufacturers have been included in the EnergyPlus refrigeration compressor coefficient database.
-
-The rated values for the cooling capacity and power consumption from the manufacturer include a specified amount of subcooling before the thermal expansion valve and a certain amount of superheat in the suction gas.  Adjustments must be made to these rated values to reflect the actual subcooling and superheat conditions.  Actual subcooling is determined by the condenser’s rated subcooling and by the subcooling provided by optional subcoolers. The actual superheat is determined by the refrigerated case superheat (usually set to ensure that there is no liquid in the suction lines leading to the compressors), set here at 10°C, and the effect from any optional subcoolers.  See the section, “Detailed Refrigeration Systems�, for a description of the compressor corrections.
-
-Once the corrected capacity is calculated for each compressor, the compressors are dispatched one at a time until the system load is met.  The last compressor dispatched is assumed to run at full load for the fraction of the time step necessary to meet the load.  That is, the model neglects compressor cycling losses at part-load conditions.  If the capacity available from all the compressors is less than the sum of the case loads for that time period, the unmet load is accumulated to be met in succeeding time steps.  If this accumulated unmet load becomes too great, a warning message is generated.
-
-#### Gas Cooler Performance
-
-Only one gas cooler is allowed per transcritical refrigeration system. However, multiple refrigeration systems can reject heat through the same gas cooler.  Currently, only air-cooled gas coolers are modeled.  The gas cooler performance is modeled to determine the gas cooler pressure, gas cooler outlet temperature and outlet enthalpy of the refrigerant, and the auxiliary power consumption for the fans.
-
-##### Optimal Gas Cooler Pressure for Transcritical CO<sub>2</sub> Cycles
-
-When the compressor discharge conditions are such that the CO<sub>2</sub> is in the supercritical region, then the high-side operating pressure is independent of the gas cooler exit temperature (Sawalha 2008).  Thus, for a given gas cooler exit temperature, there is an optimum pressure to achieve the maximum coefficient of performance (COP).  Figure 291 illustrates the variation in COP of a transcritical CO<sub>2</sub> cycle with discharge pressure at different gas cooler exit temperatures.
-
-![](media/image6342.png)
-
-Figure 291.  COP of CO<sub>2</sub> Transcritical Cycle vs. Discharge Pressure at Different Gas Cooler Exit Temperatures (Sawalha 2008).
-
-Several researchers have developed correlations to determine the optimum gas cooler pressure in CO<sub>2</sub> refrigeration systems (Chen and Gu 2005; Ge and Tassou 2011; Kauf 1998; Liao and Zhao 2000; Sawalha 2008).  Using a similar curve-fitting procedure, the following optimum gas cooler pressure correlations are used in EnergyPlus:
-
-<div><!-- $${p_{gc}} = \left\{ {\begin{array}{*{20}{c}}{7.5 \times {{10}^6},{\rm{}}![](1101-1200/html/1101-1200_files/image145.png) {T_{amb}} &lt; 27}\\ {2.3083 \times {{10}^5}{T_{amb}} + 1.190 \times {{10}^6},{\rm{}}![](1101-1200/html/1101-1200_files/image145.png) {T_{amb}} \ge 27}\end{array}} \right.$$ --> </div>
-
-<div>$${p_{gc}} = \left\{ {\begin{array}{*{20}{c}}{7.5 \times {{10}^6},{\rm{}} {T_{amb}} &lt; 27}\\ {2.3083 \times {{10}^5}{T_{amb}} + 1.190 \times {{10}^6},{\rm{}} {T_{amb}} \ge 27}\end{array}} \right.$$</div>
-
-where *p<sub>gc</sub>* is the optimum gas cooler pressure (Pa) and *T<sub>amb</sub>* (°C) is the ambient temperature surrounding the gas cooler.  The corresponding gas cooler exit temperature, *T<sub>gco</sub>* (°C), is determined as follows:
-
-<div>$${T_{gco}} = {T_{amb}} + \Delta {T_{approach}}$$</div>
-
-where Δ*T<sub>approach</sub>* is the approach temperature of the gas cooler, defined as the difference between the gas cooler exit temperature and the entering ambient air temperature.
-
-During transcritical operation, the gas cooler outlet pressure is not allowed to fall below 7.5 × 10<sup>6</sup> Pa to ensure proper operation.
-
-##### Condensing Temperature and Pressure for Subcritical Operation
-
-During subcritical operation, the gas cooler behaves as a condenser and the condensing pressure is allowed to float with the ambient conditions.  The condensing temperature, *T<sub>cond</sub>* (°C), is determined according to the following:
-
-<div> <!--$${T_{cond}} = \left\{ {\begin{array}{*{20}{c}}{{T_{cond,min}},{\rm{}}![](1101-1200/html/1101-1200_files/image147.png) {T_{amb}} \le {T_{cond,min}} - \Delta T}\\ {{T_{amb}} + \Delta T,{\rm{}}![](1101-1200/html/1101-1200_files/image147.png) {T_{cond,min}} - \Delta T &lt; {T_{amb}} \le {T_{trans}} - \Delta T}\\ {{T_{trans}},{\rm{}}![](1101-1200/html/1101-1200_files/image147.png) {T_{trans}} - \Delta T &lt; {T_{amb}} &lt; {T_{trans}}}\\ {{T_{sat,{\rm{}}P = 7.2{\rm{}}MPa}},{\rm{}}![](1101-1200/html/1101-1200_files/image147.png) {T_{trans}} \le {T_{amb}} &lt; 30.978}\end{array}} \right.$$ --> </div>
-
-<div>$${T_{cond}} = \left\{ {\begin{array}{*{20}{c}}{{T_{cond,min}},{\rm{}} {T_{amb}} \le {T_{cond,min}} - \Delta T}\\ {{T_{amb}} + \Delta T,{\rm{}} {T_{cond,min}} - \Delta T &lt; {T_{amb}} \le {T_{trans}} - \Delta T}\\ {{T_{trans}},{\rm{}} {T_{trans}} - \Delta T &lt; {T_{amb}} &lt; {T_{trans}}}\\ {{T_{sat,{\rm{}}P = 7.2{\rm{}}MPa}},{\rm{}} {T_{trans}} \le {T_{amb}} &lt; 30.978}\end{array}} \right.$$</div>
-
-where *T<sub>amb</sub>* is the ambient temperature (°C), Δ*T* is the temperature difference between the condensing temperature and the ambient temperature (°C), *T<sub>cond</sub>*<sub>,*min*</sub> is the minimum allowable condensing temperature (°C), and *T<sub>trans</sub>* is the ambient air transition temperature between subcritical and transcritical operation (°C).  The condensing pressure, *P<sub>cond</sub>* (Pa), is determined as the saturation pressure corresponding to the condensing temperature.
-
-##### Gas Cooler Fan Energy Use
-
-Gas cooler fan power for air-cooled gas coolers is determined by the type of fan control, which can either be fixed, variable speed, or two-speed.  For all three fan control types, the gas cooler fan energy is calculated in the same fashion as that for air-cooled condensers, as described in the section, “Detailed Refrigeration Systems�.
-
-#### Suction Line Heat Exchanger
-
-The performance of the transcritical CO<sub>2</sub> booster system can be enhanced by using a suction line heat exchanger.  As shown in Figure 289, the suction gas entering the heat exchanger at location 13 is used to cool the refrigerant after it leaves the gas cooler at location 1.  The performance of this heat exchanger is modeled with the heat exchanger effectiveness, ε:
-
-<div>$$\varepsilon  = \frac{{{h_{14}} - {h_{13}}}}{{{h_{{T_1},{P_{13}}}} - {h_{13}}}} = \frac{{{h_1} - {h_2}}}{{{h_{{T_1},{P_{13}}}} - {h_{13}}}}$$</div>
-
-where *h*<sub>1</sub>, *h*<sub>2</sub>, *h*<sub>13</sub>, and *h*<sub>14</sub> are the enthalpies of carbon dioxide at the respective locations in the refrigeration cycle, as shown in Figure 289 and Figure 290, and <span>\({h_{{T_1},{P_{13}}}}\)</span> is the enthalpy of carbon dioxide evaluated at temperature *T*<sub>1</sub> and pressure *P*<sub>13</sub>.
-
-In EnergyPlus, the value of the suction line heat exchanger effectiveness, ε, is specified by the user as an input, and the enthalpies at the exit of the heat exchanger, *h*<sub>2</sub> and *h*<sub>14</sub>, are determined from the definition of heat exchanger effectiveness given above.  In EnergyPlus, the default value of heat exchanger effectiveness is 0.4.
-
-**Thermodynamic Properties of CO<sub>2</sub>**
-
-Modeling of transcritical CO<sub>2</sub> booster refrigeration cycles requires the thermodynamic properties of CO<sub>2</sub> in the saturated (liquid and vapor), superheated and supercritical regions.  The refrigerant properties database within EnergyPlus includes saturated, superheated and supercritical thermodynamic data for CO<sub>2</sub>, including temperature, pressure, density, enthalpy and specific heat.
-
-### References
-
-AHRI, 2001. Standard 410, Forced-Circulation Air-Cooling and Air-Heating Coils, Section 6.2.1, Air-Conditioning Heating & Refrigeration Institute
-
-ARI. 2003. Standard for Remote Mechanical-Draft Evaporatively-Cooled Refrigerant Condensers, Standard 490, Air-Conditioning & Refrigeration Institute, Arlington, VA
-
-ARI. 2004. Standard for Performance Rating of Positive Displacement Refrigerant Compressors and Compressor Units, Standard 540, Air-Conditioning & Refrigeration Institute, Arlington, VA
-
-ARI. 2005. Standard for Performance Rating of Remote Mechanical-Draft Air-Cooled Refrigerant Condensers, Standard 460, Air-Conditioning & Refrigeration Institute, Arlington, VA
-
-ARI. 2007. Standard for Performance Rating of Water-Cooled Refrigerant Condensers, Remote Type, Standard 450, Air-Conditioning & Refrigeration Institute, Arlington, VA
-
-ASHRAE. 2002. *Refrigeration Handbook*, Chapter 47. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2004. *HVAC Systems and Equipment Handbook*, Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2006a. *Refrigeration Handbook*, Chapter 2. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2006b. *Refrigeration Handbook*, Chapter 44. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2006c. *Refrigeration Handbook*, Chapter 4. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2006d. *Refrigeration Handbook*, Chapter 13. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2009. *Fundamentals Handbook*, Chapter 1. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE. 2009b. *Fundamentals Handbook*, Chapter 2. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-B.A.C. 2007. Baltimore AirCoil Company Product and Application Handbook, Volume II, Baltimore, MD
-
-Baek, J.S., Groll, E.A., and Lawless, P.B. 2005. Theoretical Perfromance of Transcritical Carbon Dioxide Cycle with Two-Stage Compression and Intercooling. *Proceedings of the Institution of Mechanical Engineers, Part E: Journal of Process Mechanical Engineering* 219, 187-195.
-
-Baxter, V. D., Mei, V.C. 2002.Warm Liquid Defrosting Technology For Supermarket Display Cases, P.S. Hrnjak, Ed., International Conference New Technologies in Commercial Refrigeration, University of Illinois at Urbana-Champaign, Urbana, IL, July 22-23, 2002
-
-Chen, Y., and Gu, J. 2005. The Optimum High Pressure for CO<sub>2</sub> Transcritical Refrigeration Systems with Internal Heat Exchangers. *International Journal of Refrigeration* 28(8), 1238-1249.
-
-Evans, J. 2008. Chapter 15, Minimising Energy Consumption Associated with Chilling, Refrigerated Storage and Cooling Systems in the Food Industry. In *Handbook of Water and Energy Management in Food Processing*. Cambridge:  Woodhead Publishing Limited.
-
-Faramarzi, R. T., and Walker, D. H. 2004. Investigation of Secondary Lop Supermarket Refrigeration Systems, prepared for California Energy Commission Public Interest Energy Research Program, prepared by Southern California Edison and Foster-Miller, PIER 500-04-013
-
-Ge, Y., and Tassou, S. 2011. Performance Evaluation and Optimal Design of Supermarket Refrigeration Systems with Supermarket Model "Supersim", Part I: Model Description and Validation. *International Journal of Refrigeration* 34(2), 527-539.
-
-Gosney, W.B., Olama, G.A.-L. 1975. Heat and Enthalpy Gains through Cold Room Doorways,  Proceedings of the Institute of Refrigeration, vol. 72, pp 31-41
-
-Henderson, H.I. and Khattar, M. 1999. Measured Impacts of Supermarket Humidity Level on Defrost Performance and Refrigerating System Energy Use. *ASHRAE Transactions* 105(1), 508-520. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Hinde, D., Zha, S., and Lan, L. 2009. Carbon Dioxide in North American Supermarkets, ASHRAE Journal, Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.,February 2009
-
-Howell, R.H. 1993. Effects of Store Relative Humidity on Refrigerated Display Case Performance. *ASHRAE Transactions* 99(1), 667-678. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Howell, R.H. 1993. Calculation of Humidity Effects on Energy Requirements of Refrigerated Display Cases. *ASHRAE Transactions* 99(1), 679-693. Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-IEA Heat Pump Centre. 2003. *Advanced Supermarket Refrigeration/Heat Recovery Systems Vol. 1 - Executive Summary*, Report HPP-AN26-2, April.
-
-ITT. 2009. Goulds Pumps Industrial  Products Moter Terms
-
-Kauf, F. 1998. Determination of the Optimum High Pressure for Transcritical CO<sub>2</sub>-Refrigeration Cycles. *International Journal of Thermal Sciences* 38(4), 325-330.
-
-Kays, W.M., A.L. London, 1964, compact Heat Exchangers, Second Edition, Chap. 2, pp 15-24, McGraw-Hill Book Company
-
-Kazachki, G. S., and Hinde, D. K. 2006, Secondary Cooplant Systems for Supermarkets, ASHRAE Journal, Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc., September 2006
-
-Lawrence Berkeley Laboratory and Resource Dynamics, Improving Fan Systrem Performance, A Sourcebook for Industry, DOE/GO-102003-1294, April 2003
-
-Lee, T-S., Liu, C-H., and Chen, T-W. 2006. Thermodynamic Analysis of Optimal Condensing Temperature of Cascade-Condenser in CO<sub>2</sub>/NH<sub>3</sub> Cascade Refrigeration Systems, International Journal of Refrigeration 29 (2006) 1100-1108, Elsevier Ltd.
-
-Liao, S., and Zhao, T. J. 2000. A Correlation of Optimal Heat Rejection Pressures in Transcritical Carbon Dioxide Cycles. *Applied Thermal Engineering* 20(9), 831-841.
-
-Manske, K.A., 2000. Performance Optimization of Industrial Refrigeration Systems, M.S.Thesis Mechanical Engineering, Solar Energy Laboratory, University of Wisconsin-Madison.
-
-Minea, V. 2007. Supermarket Refrigeration System with Completely Secondary Loops, ASHRAE Journal, Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.,  September 2007
-
-Mitchell, J.W., et al. 1992.Analysis of Supermarket Dehumidification Alternatives. Final Report to Electric Power Research Institute, Report TR-100352, November.
-
-NASA. 1976. U. S. Standard Atmosphere, NASA-TM-74335, National Oceanic and Atmosperic Administration , National Aeronautics and Space Administration
-
-Nelson, B. I., 2010, Refrigeration Air Cooler Rating Methods, ASHRAE Journal, American Society of Heating, Refrigeration and Air-Conditioning Engineers, Inc., August
-
-Sawalha, S. 2008. Theoretical Evaluation of Trans-Critical CO<sub>2</sub> Systems in Supermarket Refrigeration. Part I: Modeling, Simulation and Optimization of Two System Solutions. *International Journal of Refrigeration* 31, 516-524.
-
-Terrell, W.J.Jr., Mao, Y., Hrnjak, P.S. 1999. Evaluation of Secondary Fluids for Use in Low-Temperature Supermarket Applications, ACRC CR-15, Air Conditioning and Refrigeration Center, University of Illinois, Urbana, IL, April 1999.
-
-Setpoint Managers <a name="SetpointManagers"></a>
------------------
-
-### Overview
-
-Setpoint Managers are one of the high-level control constructs in EnergyPlus. A Setpoint Manager is able to access data from any of the HVAC system nodes and use this data to calculate a setpoint (usually a temperature setpoint) for one or more other HVAC system nodes. Setpoints are then used by Controllers as a goal for their control actions.
-
-Setpoint managers are executed at the start of each HVAC time step, and they reside outside the HVAC system iteration loops. Thus, the Setpoint Managers are executed once per HVAC time step, and they use previous time step information (except for zone load) to calculate their setpoints.
-
-All temperatures in the following descriptions are in degrees C, loads are in Watts, mass flow rates are in kg/s.
-
-### Scheduled
-
-The input object SetpointManager:Scheduled provides the simplest setpoint manager that allows the user to specify a seasonal (or other) scheduled reset, for example, of the supply air temperature setpoint.
-
-<div>$${T_{set}} = {T_{sched}}$$</div>
-
-where <span>\({T_{set}}\)</span>is the supply air temperature setpoint and <span>\({T_{sched}}\)</span>is the current value (°C) from the user input temperature schedule. In this case, <span>\({T_{set}}\)</span>will be applied to the node or nodes specified in the input object SetpointManager:Scheduled.  There are a number of other types of setpoints that can be set, by choosing different control variables in the object, including:
-
-1)   Maximum temperature of fluid at node (°C)
-
-2)   Minimum temperature of fluid at node (°C)
-
-3)   Humidity ratio of fluid at node (kg water/ kg dry air)
-
-4)   Maximum humidity ratio of fluid at node (kg water/ kg dry air)
-
-5)   Minimum humidity ratio of fluid at node (kg water/ kg dry air)
-
-6)   Mass flow rate of fluid at node (kg/s)
-
-7)   Maximum mass flow rate of fluid at node (kg/s)
-
-8)   Minimum mass flow rate of fluid at node (kg/s)
-
-### Outdoor Air Reset
-
-The input object SetpointManager:OutdoorAirReset provides a setpoint manager that implements an outdoor air reset strategy for the supply air temperature. The user defines a reset rule for this strategy by specifying two setpoint temperatures at two outside drybulb temperatures. Generally the lower setpoint temperature is matched with the higher drybulb temperature and the higher setpoint temperature with the lower drybulb temperature. The user can specify two reset rules and schedule their usage. A schedule value of 1 indicates use of the 1st rule; 2 indicates use of the 2nd.
-
-IF *SchedVal =2*
-
-<div>$${T_{out,low}} = {T_{2,out,low}}$$</div>
-
-<div>$${T_{out,high}} = {T_{2,out,high}}$$</div>
-
-<div>$${T_{set,atOAlow}} = {T_{2,set,atOAlow}}$$</div>
-
-<div>$${T_{set,atOAhigh}} = {T_{2,set,atOAhigh}}$$</div>
-
-otherwise
-
-<div>$${T_{out,low}} = {T_{1,out,low}}$$</div>
-
-<div>$${T_{out,high}} = {T_{1,out,high}}$$</div>
-
-<div>$${T_{set,atOAlow}} = {T_{1,set,atOAlow}}$$</div>
-
-<span>\({T_{set,atOAhigh}} = {T_{1,set,atOAhigh}}\)</span>.
-
-If <span>\({T_{out,low}} &lt; {T_{out,high}}\)</span>and <span>\({T_{set,atOAlow}} > {T_{set,atOAhigh}}\)</span> then
-
-      If <span>\({T_{out}} \le {T_{out,low}}\)</span> then
-
-      <span>\({T_{set}} = {T_{out,low}}\)</span>
-
-      if <span>\({T_{out}} \ge {T_{out,high}}\)</span> then
-
-      <span>\({T_{set}} = {T_{out,high}}\)</span>
-
-      otherwise
-
-      <span>\({T_{set}} = {T_{set,atOAlow}} - (({T_{out}} - {T_{out,low}})/({T_{out,high}} - {T_{out,low}}))\cdot ({T_{set,atOAlow}} - {T_{set,atOAhigh}})\)</span>
-
-otherwise
-
-      <span>\({T_{set}} = 0.5({T_{set,atOAlow}} + {T_{set,atOAhigh)}}\)</span>.
-
-*<span>\({T_{set}}\)</span>*will be applied to the node or nodes specified in the *SetpointManager:OutdoorAirReset* object input.
-
-### Single Zone Reheat Heating and Cooling
-
-The input object SetpointManager:SingleZone:Reheat provides a setpoint manager that is used to implement a variable supply air setpoint temperature in which the setpoint is varied  each timestep to meet the heating or cooling load in a control zone. The manager operates in the following manner.
-
-<div>$${T_{set}} = {T_z} + {\dot Q_z}/({C_{p,air}}\cdot {\dot m_z})$$</div>
-
-where <span>\({T_z}\)</span>is the control zone temperature, <span>\({\dot Q_z}\)</span>is the zone load (greater than zero for heating, less than zero for cooling), <span>\({\dot m_z}\)</span>is the zone supply air mass flow rate, and <span>\({C_{p,air}}\)</span>is the specific heat of air. If <span>\({\dot m_z}\)</span>is very small (<span>\(\le .001\)</span> kg/s) <span>\({T_{set}}\)</span> is set equal to <span>\({T_{set,min}}\)</span> if the control zone has a cooling load and to <span>\({T_{set,max}}\)</span>if the control zone has a heating load. <span>\({T_{set,min}}\)</span> is the user specified minimum setpoint and <span>\({T_{set,max}}\)</span> is the user specified maximum setpoint. <span>\({T_{set}}\)</span>will be applied to the node or nodes specified in the SetpointManager:SingleZone:Reheat object input.
-
-### Single Zone Heating Only
-
-The input object SetpointManager:SingleZone:Heating provides a model that detects the control zone load to meet the current heating setpoint (Report Variable "Zone Predicted Sensible Load to Heating Setpoint Heat Transfer Rate [W]", zone inlet node flow rate, and zone node temperature, and calculates a setpoint temperature for the supply air that will satisfy the zone heating load for the control zone.  "Zone Predicted Sensible Load to Heating Setpoint Heat Transfer Rate [W]" &gt; 0 indicates a heating load.  The following rules are applied:
-
-·        If there is no zone heating load, then the setpoint is set at the specified minimum supply air temperature.
-
-·        If there is a zone heating load  and the zone supply mass flow rate is less than 0.001 kg/s, then the setpoint is set at the specified maximum supply air temperature.
-
-·        If there is a zone heating load  and the zone supply mass flow rate is greater than 0.001 kg/s, then the setpoint is set calculated as follows:
-
-*SetPoint = ZoneTemp + ZoneLoadtoHeatSP/(CpAir\*ZoneMassFlow)*
-
-where:
-
-*SetPoint =* Setpoint temperature applied to the specified setpoint node(s)
-
-*ZoneTemp =* Current zone temperature
-
-*ZoneLoadtoHeatSP =* Zone heating load (Report Variable " Zone Predicted Sensible Load to Heating Setpoint Heat Transfer Rate [W]")
-
-*CpAir =* Specific heat of zone supply air
-
-*ZoneMassFlow =* Zone supply air mass flow rate
-
-### Single Zone Cooling Only
-
-The input object SetpointManager:SingleZone:Cooling provides a model that detects the control zone load to meet the current cooling setpoint (Report Variable "Zone Predicted Sensible Load to Cooling Setpoint Heat Transfer Rate [W]", zone inlet node flow rate, and zone node temperature, and calculates a setpoint temperature for the supply air that will satisfy the zone cooling load for the control zone.  "Zone Predicted Sensible Load to Cooling Setpoint Heat Transfer Rate [W]" &lt; 0 indicates a cooling load.  The following rules are applied:
-
-·        If there is no zone cooling load, then the setpoint is set at the specified maximum supply air temperature.
-
-·        If there is a zone cooling load  and the zone supply mass flow rate is less than 0.001 kg/s, then the setpoint is set at the specified minimum supply air temperature.
-
-·        If there is a zone cooling load  and the zone supply mass flow rate is greater than 0.001 kg/s, then the setpoint is set calculated as follows:
-
-*SetPoint = ZoneTemp + ZoneLoadtoCoolSP/(CpAir\*ZoneMassFlow)*
-
-where:
-
-*SetPoint* = Setpoint temperature applied to the specified setpoint node(s)
-
-*ZoneTemp* = Current zone temeprature
-
-*ZoneLoadtoCoolSP* = Zone cooling load (Report Variable "Zone Predicted Sensible Load to Cooling Setpoint Heat Transfer Rate [W]")
-
-*CpAir* = Specific heat of zone supply air
-
-*ZoneMassFlow* = Zone supply air mass flow rate
-
-### Single Zone Minimum Humidity
-
-The input object SetpointManager:SingleZone:Humidity:Minimum provides a model where the zone moisture load from ZoneTempPredictorCorrector (via DataZoneEnergyDemands) is used to calculate the minimum/maximum supply air humidity ratio needed to meet minimum/maximum zone relative humidity requirement.  For the Max setpoint manager is currently used in Controller:WaterCoil, when the control variable "TemperatureAndHumidityRatio".  A negative MoistureLoad means a dehumidification load for the coil controller.  This could be used for any system.
-
-### Single Zone Maximum Humidity
-
-The input object SetpointManager:SingleZone:Humidity:Maximum provides a setpoint manager that allows the control of high air humidity levels in a single zone. This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level in a single control zone and uses air/moisture mass balances to calculate the supply air humidity ratio needed to maintain the zone relative humidity at or below a given setpoint. The calculated supply air humidity ratio is then entered as a setpoint on a designated supply air stream node. A dehumidification component placed upstream of this node can then use the humidity ratio setpoint to control its moisture removal rate (e.g. desiccant dehumidifiers). In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determine the minimum supply air temperature required to meet both the temperature (sensible) and humidity (latent) load in the control zone. (Ref: Controller:WaterCoil).
-
-#### Model Description
-
-The user must input the required information according to the IO Reference Manual (ref: SetpointManager:SingleZone:Humidity:Maximum). Specific inputs include an object name, control variable (HumidityRatio), name of the schedule defining the maximum relative humidity for the control zone, setpoint node name or list, and the zone air node name associated with the control zone (ref: ZoneHVAC:EquipmentConnections). The schedule name must refer to a valid schedule type (range 0-1) and contain values of fractional relative humidity.
-
-This setpoint manager first converts the desired relative humidity setpoint for the control zone to humidity ratio based on the control zone dry-bulb temperature, the scheduled maximum relative humidity setpoint and outdoor barometric pressure.
-
-<div>$${\omega_{sp}} = \,{\rm{PsyWFnTdbRhPb}}\left( {{T_{db}},R{H_{sp}},P} \right)$$</div>
-
-where:
-
-<span>\({\omega_{sp}}\)</span> = humidity ratio setpoint, kg H<sub>2</sub>O/kg air
-
-PsyWFnTdbRHPb = EnergyPlus psychrometric function, returns humidity ratio as a function of dry-bulb temperature, relative humidity, and barometric pressure
-
-<span>\({T_{db}}\)</span>= dry-bulb temperature in the control zone, °C
-
-<span>\(R{H_{sp}}\)</span>= maximum relative humidity setpoint, fraction
-
-<span>\(P\)</span> = outdoor barometric pressure, Pa
-
-The model then calculates the supply air humidity ratio required to reduce the control zone relative humidity to the desired level. Using the humidity ratio setpoint (<span>\({\omega_{sp}}\)</span>) calculated above,
-
-<div>$${\omega_{sa}} = \,{\omega_{sp}} + \frac{{{{\mathop Q\limits^ \bullet  }_l}}}{{\mathop m\limits^ \bullet  }}$$</div>
-
-where:
-
-<span>\({\omega_{sa}}\)</span> = maximum supply air humidity ratio setpoint, kg H<sub>2</sub>O/kg air
-
-<span>\(\mathop {{Q_l}}\limits^ \bullet  \)</span> = control zone latent load, kg H<sub>2</sub>O/s (calculated by Zone Control:Humidistat)
-
-<span>\(\mathop m\limits^ \bullet  \)</span> = control zone mass flow rate, kg/s
-
-All setpoint managers are executed at the beginning of the simulation time step. Therefore, the calculated setpoint is based on the resulting control zone air temperature and air mass flow rate for the previous simulation time step.
-
-The maximum supply air humidity ratio setpoint is placed on the node(s) specified in the input for this object (using node property Humidity Ratio Maximum).
-
-### Mixed Air
-
-The input object SetpointManager:MixedAir provides a setpoint manager that takes an already established setpoint (usually the supply air outlet node setpoint temperature), subtracts the supply fan heat gain, and applies the result as the setpoint temperature at the mixed air node (or any other node the user specifies).
-
-<div>$${T_{set}} = {T_{set,ref}} - ({T_{fan,outlet}} - {T_{fan,inlet}})$$</div>
-
-When inputs of optional fields, Cooling Coil Inlet Node Name, Cooling coil Outlet Node Name, and Minimum Temperature at Cooling Coil Outlet Node, are provided, the setpoint temperature at the mixed air node is given below based on supply fan placement and reference node location:
-
-Blow through placement:
-
-<div>$${T_{set}} = max(T_{set,ref}, T_{min}) - ({T_{coil,outlet}} - {T_{coil,inlet}}) - ({T_{fan,outlet}} - {T_{fan,inlet}})$$</div>
-
-Draw through placement:
-
-When the reference node is the cooling coil outlet node:
-
-<div>$${T_{set}} = max(T_{set,ref}, T_{min}) - ({T_{coil,outlet}} - {T_{coil,inlet}})$$</div>
-
-When the reference node is the unitary system outlet node:
-
-<div>$${T_{set}} = max(T_{set,ref} - ({T_{fan,outlet}} - {T_{fan,inlet}}), T_{min}) - ({T_{coil,outlet}} - {T_{coil,inlet}})$$</div>
-
-### Outdoor Air Pretreat
-
-The input object SetpointManager:OutdoorAirPretreat provides a setpoint manager that is meant to be used in conjunction with an OutdoorAir:Mixer. The outdoor air pretreat setpoint manager is used to establish a temperature or humidity ratio setpoint in the outdoor air stream flowing into the outdoor air stream node of an outdoor air mixer. This setpoint manager determines the required setpoint in the outdoor air stream to produce the reference setpoint in the mixed air stream after mixing with return air. For example, if the temperature setpoint at the mixed air node is 15C, the return air temperature is 20C, and the outdoor air flow fraction is 0.5, the outdoor air pretreat setpoint would be set to 10C. This setpoint manager references four user-specified nodes to obtain the following values:
-
-·        Reference setpoint node – desired mixed flow condition = RefNodeSetPoint
-
-·        Mixed air stream node – mixed air flow rate = MixedOutNodeMassFlowRate
-
-·        Outdoor air stream node – outdoor air flow rate = OAInNodeMassFlowRate
-
-·        Return air stream node – return air condition = ReturnInValue
-
-The following calculations are used to determine the new setpoint value (SetPoint):
-
-*OAFraction = OAInNodeMassFlowRate / MixedOutNodeMassFlowRate*
-
-*SetPoint = ReturnInValue + (RefNodeSetPoint - ReturnInValue)/OAFraction*
-
-Depending on the specified control variable type, the setpoints and conditions may be humidity ratio (max or min) or temperature.  Note that zero is not allowed as the computed setpoint humidity ratio, because zero is used as a special value to indicate that no humidification or dehumidification is needed.  If the reference humidity ratio setpoint value is zero, the zero value will be passed directly to the setpoint Node(s).
-
-### Warmest Zone Supply Air Reset
-
-The input object SetpointManager:Warmest provides a setpoint manager that attempts to establish a supply air setpoint that will meet the cooling load of the zone needing the coldest air at the maximum zone supply air flowrate. The algorithm loops over all the zones that the system can cool and calculates
-
-<div>$${T_{set,z}} = {T_z} + {\dot Q_z}/({C_{p,air}}\cdot {\dot m_{z,max}})$$</div>
-
-Note that for cooling <span>\({\dot Q_z} &lt; 0.\)</span>The lowest <span>\({T_{set,z}}\)</span>is chosen as <span>\({T_{set}}\)</span>. <span>\({T_{set}}\)</span>is constrained to be less than or equal to the maximum setpoint temperature (user input) and greater than or equal to the minimum setpoint temperature (user input). If the sum of the zone cooling loads is very small, the setpoint temperature is set to the maximum. <span>\({T_{set}}\)</span>will be applied to the node or nodes specified in the SetpointManager:Warmest object input.
-
-### Coldest Zone Supply Air Reset
-
-The input object SetpointManager:Coldest provides a setpoint manager that attempts to establish a supply air setpoint that will meet the heating load of the zone needing the warmest air at the maximum zone supply air flowrate. The algorithm loops over all the zones that the system can heat and calculates
-
-<div>$${T_{set,z}} = {T_z} + {\dot Q_z}/({C_{p,air}}\cdot {\dot m_{z,max}})$$</div>
-
-Note that for heating <span>\({\dot Q_z} > 0.\)</span>The highest <span>\({T_{set,z}}\)</span>is chosen as <span>\({T_{set}}\)</span>. <span>\({T_{set}}\)</span>is constrained to be less than or equal to the maximum setpoint temperature (user input) and greater than or equal to the minimum setpoint temperature (user input). If the sum of the zone heating loads is very small, the setpoint temperature is set to the minimum. <span>\({T_{set}}\)</span>will be applied to the node or nodes specified in the SetpointManager:Coldest object input.
-
-### Return Air Bypass Flow
-
-The input object SetpointManager:ReturnAirBypassFlow provides a setpoint manager that sets the air flow rate in a bypass duct such that when the bypassed and non-bypassed air are mixed the resutant air stream will be at the user-specified setpoint temperature.
-
-The user specifies the desired setpoint temperature *T<sub>set</sub>* through a input temperature schedule.
-
-This temperature is modified to account for any potential fan heat gain:
-
-<div>$${T_{set,mod}} = {T_{set}} - ({T_{loop,out}} - {T_{mixer,out}})$$</div>
-
-Here <span>\({T_{loop,out}}\)</span>is the temperature at the air loop outlet node and <span>\({T_{mixer,out}}\)</span> is the temperature at the outlet node of the bypass – nonbypass air mixer. Depending on the system configuration these may be the same node. Then
-
-<div>$${\dot m_{bypass}} = ({\dot m_{tot}}\cdot {T_{set,mod}} - {\dot m_{nonbypass}}\cdot {T_{nonbypass}})/{T_{bypass}}$$</div>
-
-where <span>\({\dot m_{tot}}\)</span>is the total supply air flowrate in kg/s sent to the zones, <span>\({\dot m_{nonbypass}}\)</span>is the nonbypassed air flowrate (the conditioned air), <span>\({T_{nonbypass}}\)</span>is the corresponding temperature just before mixing with the bypassed air, and <span>\({T_{bypass}}\)</span>is the temperature of the bypassed (unconditioned) air. The resulting <span>\({\dot m_{bypass}}\)</span> is the mass flow rate setpoint for the bypass air branch.
-
-### Warmest Temp Flow
-
-The input object SetpointManager:WarmestTemperatureFlow provides a setpoint manager that attempts to establish a supply air setpoint that will meet the cooling load of the zone needing the coldest air at the maximum zone supply air flowrate. The supply air temperature setpoint is established by SetpointManager:WarmestTemperatureFlow using one of two strategies: 'Temp First' sets the supply air temperature to the highest temperature that will meet the cooling load of the coolest zone at minimum cfm. 'Flow First' sets the supply air temperature to the highest temperature that will meet the cooling load of the warmest zone at maximum cfm.  'Temp First' gives higher priority to reducing fan energy whereas 'Flow First' gives higher priority to reducing chiller energy.
-
-The algorithm loops over all the zones that the system can cool and calculates according to strategy:
-
-**Temp First:**
-
-<div>$${T_{set,z}} = {T_z} + {\raise0.7ex\hbox{${{{\dot Q}_z}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_z}} {({C_{p,air}}\cdot {{\dot m}_{z,\min }})}}}\right.}\!\lower0.7ex\hbox{${({C_{p,air}}\cdot {{\dot m}_{z,\min }})}$}}$$</div>
-
-**Flow First:**
-
-<div>$${T_{set,z}} = {T_z} + {\raise0.7ex\hbox{${{{\dot Q}_z}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_z}} {({C_{p,air}}\cdot {{\dot m}_{z,\max }})}}}\right.}\!\lower0.7ex\hbox{${({C_{p,air}}\cdot {{\dot m}_{z,\max }})}$}}$$</div>
-
-where <span>\({\dot m_{z,\min }}\)</span>is the minimum air flow rate to the zone produced by reducing the capacity of the supply fan or by reducing the opening of the damper in the terminal box, if present, and  <span>\({\dot m_{z,\max }}\)</span> is the design air flow rate to the zone.
-
-Note that for cooling <span>\({\dot Q_z} &lt; 0.\)</span> The lowest <span>\({T_{set,z}}\)</span>is chosen as <span>\({T_{set}}\)</span>. <span>\({T_{set}}\)</span>is constrained to be less than or equal to the maximum setpoint temperature (user input) and greater than or equal to the minimum setpoint temperature (user input). If the unconstrained value of <span>\({T_{set}}\)</span>is less than the minimum setpoint temperature and there are no VAV terminal boxes, the fan capacity is increased so as to meet the zone cooling loads with the constrained value of <span>\({T_{set}}\)</span>:
-
-
-
-<div>$${\dot m_{fan}} = \sum\limits_z {{{\dot m}_{z,\min }}}  = \sum\limits_z {{{\dot Q}_z}/[{C_{p,air}} \cdot ({T_{set}} - {T_z})]} $$</div>
-
- This is more likely to occur in the ‘Temp First’ case. If the sum of the zone cooling loads is very small, the setpoint temperature is set to the maximum. <span>\({T_{set}}\)</span>will be applied to the node or nodes specified in the SetpointManager:WarmestTemperatureFlow object input.
-
-### Multizone Heating Average
-
-The input object SetpointManager:MultiZone:Heating:Average provides a setpoint manager that attempts to establish a supply air heating setpoint that will meet the heating load of multiple zones served by an HVAC air loop. The algorithm aggregates the predicted heating loads for all controlled zones served by an air loop (i.e., zones that have a thermostat object), and calculates the multizone average supply air heating setpoint temperature as follows:
-
-
-
-IF ( <span>\({\dot Q_{zj}}\)</span>&gt; 0 ) THEN
-
-<div>$$\overline {{T_{SP}}}  = \overline {{T_Z}}  + \left( {\frac{{\sum\limits_{j = 1}^{NumControlZones} {{{\dot Q}_{Zi}}} }}{{\sum\limits_{j = 1}^{NumControlZones} {{{\dot m}_{Zi}}\cdot C{p_j}} }}} \right)$$</div>
-
-END IF
-
-<div>$${\bar T_z} = {{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{zj}} \bullet } C{p_j} \bullet {T_{zj}}} \right)} \mathord{\left/ {\vphantom {{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{zj}} \bullet } C{p_j} \bullet {T_{zj}}} \right)} {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{zj}} \bullet } C{p_j}} \right)}}} \right. } {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{zj}} \bullet } C{p_j}} \right)}}$$</div>
-
-
-
-where,
-
-<span>\({\bar T_{SP}}\)</span>                  = average supply air setpoint temperature (°C)
-
-<span>\(NumControlZones\)</span>= number of controlled zones (i.e., zones that contain thermostat objects) served by the air loop (-)
-
-<span>\({\dot Q_{Zj}}\)</span>= sensible heating load required to reach the zone air temperature setpoint for the *j*<sup>th</sup> controlled zone at current time step (W)
-
-<span>\({\dot m_{Zj}}\)</span>= air mass flow rate being supplied by the air loop to the *j*<sup>th</sup> controlled zone, lagged by one HVAC simulation time step (kg/s)
-
-<span>\(C{p_j}\)</span>= specific heat of supply air for the j<sup>th</sup> controlled zone (J/kg-K)
-
-<span>\({T_{Zj}}\)</span>= air node temperature for the *j*<sup>th</sup> controlled zone (°C)
-
-<span>\({\overline T_Z}\)</span>= average zone air node temperature weighted by the heat capacity rate of the supply air streams for the controlled zones served by the air loop (°C)
-
-<span>\(TotZones\)</span>= total number of zones served by the air loop (-)
-
-Note that for heating <span>\({\dot Q_{Zj}} > 0.\)</span> The average supply air setpoint temperature <span>\({\bar T_{SP}}\)</span> is constrained to be less than or equal to the maximum setpoint temperature (user input) and greater than or equal to the minimum setpoint temperature (user input). If the sum of the zone sensible heating loads is extremely small (i.e., no heating load), the setpoint temperature is set to the minimum. <span>\({\bar T_{SP}}\)</span>will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:Heating:Average object.
-
-### Multizone Cooling Average
-
-The input object SetpointManager:MultiZone:Cooling:Average provides a setpoint manager that attempts to establish a supply air cooling setpoint that will meet the cooling load of multiple zones served by an HVAC air loop. The algorithm aggregates the predicted cooling loads for all controlled zones served by an air loop (i.e., zones that have a thermostat object), and calculates the multizone average supply air cooling setpoint temperature as follows:
-
-
-
-IF ( <span>\({\dot Q_{zj}}\)</span>&lt; 0 ) THEN
-
-<div>$$\overline {{T_{SP}}}  = \overline {{T_Z}}  + \left( {\frac{{\sum\limits_{j = 1}^{NumControlZones} {{{\dot Q}_{Zi}}} }}{{\sum\limits_{j = 1}^{NumControlZones} {{{\dot m}_{Zi}}\cdot C{p_j}} }}} \right)$$</div>
-
-END IF
-
-<div>$${\bar T_z} = {{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{Zj}} \bullet } C{p_j} \bullet {T_{zj}}} \right)} \mathord{\left/ {\vphantom {{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{Zj}} \bullet } C{p_j} \bullet {T_{zj}}} \right)} {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{Zj}} \bullet } C{p_j}} \right)}}} \right. } {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{Zj}} \bullet } C{p_j}} \right)}}$$</div>
-
-Note that for cooling <span>\({\dot Q_{Zj}} &lt; 0.\)</span> The average supply air setpoint temperature <span>\({\bar T_{SP}}\)</span>is constrained to be less than or equal to the maximum setpoint temperature (user input) and greater than or equal to the minimum setpoint temperature (user input). If the sum of the zone sensible cooling loads is extremely small (i.e., no cooling load), the setpoint temperature is set to the maximum. <span>\({\bar T_{SP}}\)</span>will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:Cooling:Average object.
-
-### Multizone Minimum Humidity Average
-
-The input object SetpointManager:MultiZone:MinimumHumidity:Average provides a setpoint manager that attempts to establish a supply air minimum humidity ratio setpoint that will meet the humidification load of multiple zones served by an HVAC air loop.  This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level for all controlled zones served by an air loop (i.e., zones that have a humidistat object with a humidifying setpoint schedule), and uses moisture mass balances to calculate the average supply air minimum humidity ratio setpoint as follows:
-
-IF ( <span>\({\dot Q_{lzj}}\)</span>&gt; 0 ) THEN
-
-<div>$${\bar \omega_{SP}} = {\bar \omega_Z} + {{\left( {\sum\limits_{j = 1}^{NumControlZones} {{{\dot Q}_{l,Zj}}} } \right)} \mathord{\left/ {\vphantom {{\left( {\sum\limits_{j = 1}^{NumControlZones} {{{\dot Q}_{l,Zj}}} } \right)} {\left( {\sum\limits_{j = 1}^{NumControlZones} {{{\dot m}_{ZJ}}} } \right)}}} \right. } {\left( {\sum\limits_{j = 1}^{NumControlZones} {{{\dot m}_{ZJ}}} } \right)}}$$</div>
-
-END IF
-
-<div>$${\bar \omega_Z}{ =_\,}{{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{\,Zj}}\cdot {\omega_{Zj}}} } \right)} \mathord{\left/ {\vphantom {{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{\,Zj}}\cdot {\omega_{Zj}}} } \right)} {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{\,Zj}}} } \right)}}} \right. } {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{\,Zj}}} } \right)}}$$</div>
-
-where,
-
-<span>\({\bar \omega_{SP}}\)</span>= average supply air minimum humidity ratio setpoint (kg H<sub>2</sub>O/kg air)
-
-<span>\(NumControlZones\)</span>= number of controlled zones (i.e., zones that contain humidistat objects with humidifying setpoint schedule) served by the air loop (-)
-
-<span>\({\dot Q_{lZj}}\)</span>= latent (humidification) load required to reach the zone air humidifying setpoint for the *j*<sup>th</sup> controlled zone at current time step (kg H<sub>2</sub>O/s)
-
-<span>\({\dot m_{Zj}}\)</span>= air mass flow rate being supplied by the air loop to the *j*<sup>th</sup> controlled zone, lagged by one HVAC simulation time step (kg/s)
-
-<span>\({\omega_{Zj}}\)</span>= air node humidity ratio for the jth controlled zone (kg H<sub>2</sub>O/kg air)
-
-<span>\({\bar \omega_Z}\)</span>= average zone air node humidity ratio weighted by supply air mass flow rate for the controlled zones served by the air loop (kg H<sub>2</sub>O/kg air)
-
-<span>\(TotZones\)</span>= total number of zones served by the air loop (-)
-
-Note that a positive latent load means humidification is required. The average supply air minimum humidity ratio setpoint <span>\({\bar \omega_{SP}}\)</span>is constrained to be less than or equal to the maximum setpoint humidity ratio (user input) and greater than or equal to the minimum setpoint humidity ratio (user input). If the sum of the zone latent humidification loads is extremely small (i.e., no humidification load), the humidity ratio setpoint is set to the minimum. <span>\({\bar \omega_{SP}}\)</span>will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:MinimumHumidity:Average object. A humidification component (e.g., an electric humidifier) placed upstream of this node can then use the humidity ratio setpoint to control its moisture addition rate.
-
-All setpoint managers are executed at the beginning of the simulation time step. Therefore, the calculated setpoint is based on the resulting zone air node humidity ratios and supply air mass flow rates for the previous simulation time step.
-
-### Multizone Maximum Humidity Average
-
-The input object SetpointManager:MultiZone:MaximumHumidity:Average provides a setpoint manager that attempts to establish a supply air maximum humidity ratio setpoint that will meet the dehumidification load of multiple zones served by an HVAC air loop. This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level for all controlled zones served by an air loop (i.e., zones that have a humidistat object with a dehumidifying setpoint schedule), and uses moisture mass balances to calculate the average supply air maximum humidity ratio as follows:
-
-IF ( <span>\({\dot Q_{lzj}}\)</span>&lt; 0 ) THEN
-
-<div>$${\bar \omega_{SP}} = {\bar \omega_Z} + {{\left( {\sum\limits_{j = 1}^{NumControlZones} {{{\dot Q}_{l,Zj}}} } \right)} \mathord{\left/ {\vphantom {{\left( {\sum\limits_{j = 1}^{NumControlZones} {{{\dot Q}_{l,Zj}}} } \right)} {\left( {\sum\limits_{j = 1}^{NumControlZones} {{{\dot m}_{ZJ}}} } \right)}}} \right. } {\left( {\sum\limits_{j = 1}^{NumControlZones} {{{\dot m}_{ZJ}}} } \right)}}$$</div>
-
-END IF
-
-<div>$${\bar \omega_Z}{ =_\,}{{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{\,Zj}}\cdot {\omega_{Zj}}} } \right)} \mathord{\left/ {\vphantom {{\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{\,Zj}}\cdot {\omega_{Zj}}} } \right)} {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{\,Zj}}} } \right)}}} \right. } {\left( {\sum\limits_{j = 1}^{TotZones} {{{\dot m}_{\,Zj}}} } \right)}}$$</div>
-
-Note that a negative latent load means dehumidification is required. The average supply air maximum humidity ratio setpoint <span>\({\bar \omega_{SP}}\)</span>is constrained to be less than or equal to the maximum setpoint humidity ratio (user input) and greater than or equal to the minimum setpoint humidity ratio (user input). If the sum of the zone latent dehumidification loads is extremely small (i.e., no dehumidification load), the humidity ratio setpoint is set to the maximum. <span>\({\bar \omega_{SP}}\)</span>will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:MaximumHumidity:Average object. A dehumidification component (e.g., an desiccant dehumidifier) placed upstream of this node can then use the humidity ratio setpoint to control its moisture removal rate. In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determines the minimum supply air temperature required to meet both the temperature (sensible) and humidity (latent) load in the control zone (ref: Controller:WaterCoil).
-
-### MultiZone Minimum Humidity Supply Air Reset
-
-The input object SetpointManager:MultiZone:Humidity:Minimum provides a setpoint manager that attempts to establish a supply air minimum humidity ratio setpoint that will meet the humidification load of zone with the critical humidification requirement at each time step served by an HVAC air loop at the zone actual supply air mass flow rate.  This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level for all controlled zones served by an air loop (i.e., zones that have a humidistat object with a humidifying setpoint schedule), and uses moisture mass balances to calculate the supply air minimum humidity ratio setpoint.  The algorithm loops over all the zones that the system can humidify and calculates the setpoint based on a zone with the highest humidity ratio setpoint requirement as follows:
-
-IF (<span>\({\dot Q_{lzj}}\)</span>&gt; 0) THEN
-
-<div>$${\omega_{SP\;Zj}} = {\omega_{Zj}} + {{{{\dot Q}_{lZj}}} \mathord{\left/ {\vphantom {{{{\dot Q}_{lZj}}} {{{\dot m}_{Zj}}}}} \right. } {{{\dot m}_{Zj}}}}$$</div>
-
-END IF
-
-<div>$${\omega_{SP\;Zj}} = MAX\left( {{\omega_{SP\;Zj}},\;{\omega_{SP\;Min}}} \right)$$</div>
-
-<div>$${\omega_{SP}} = MIN\left( {{\omega_{SP\;Zj}},\;{\omega_{SP\;Max}}} \right)$$</div>
-
-where,
-
-<span>\({\omega_{SP}}\)</span>= supply air humidity ratio setpoint (kg/kg)
-
-<span>\({\dot Q_{lzj}}\)</span>= latent load required to reach the zone air setpoint for the *j*<sup>th</sup> controlled zone at current time step (kg H<sub>2</sub>O/s)
-
-<span>\({\dot m_{Zj}}\)</span>= actual mass flow rate supplied by the air loop to the *j*<sup>th</sup> controlled zone, (kg/s)
-
-<span>\({\omega_{Zj}}\)</span>= air node humidity ratio for the j<sup>th</sup> controlled zone (kg/kg)
-
-<span>\({\omega_{SP\;Zj}}\)</span>= supply air humidity ratio setpoint for the j<sup>th</sup> controlled zones (kg/kg)
-
-<span>\({\omega_{SP\;Min}}\)</span>= user-specified supply air minimum humidity ratio setpoint (kg/kg)
-
-<span>\({\omega_{SP\;Max}}\)</span>= user-specified supply air maximum humidity ratio setpoint (kg/kg)
-
-Note that a positive latent load means humidification is required. The supply air minimum humidity ratio setpoint <span>\({\omega_{SP}}\)</span>is constrained to be less than or equal to the maximum setpoint humidity ratio (user input) and greater than or equal to the minimum setpoint humidity ratio (user input). If the humidification load for all zones in the air loop is extremely small (i.e., no humidification load), the humidity ratio setpoint is set to the user input minimum value. <span>\({\omega_{SP}}\)</span>will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:Humidity:Minimum object. A humidification component (e.g., an electric humidifier) placed upstream of this node can then use the humidity ratio setpoint to control its moisture addition rate.
-
-### MultiZone Maximum Humidity Supply Air Reset
-
-The input object SetpointManager:MultiZone:Humidity:Maximum provides a setpoint manager that attempts to establish a supply air maximum humidity ratio setpoint that will meet the dehumidification load of the zone with the critical dehumidification requirement at each time step served by an HVAC air loop at the zone actual supply air mass flow rate. This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level for all controlled zones served by an air loop (i.e., zones that have a humidistat object with a dehumidifying setpoint schedule), and uses moisture mass balances to calculate the supply air maximum humidity ratio setpoint.  The algorithm loops over all the zones that the system can dehumidify and calculates the setpoint based on a zone with the lowest humidity ratio setpoint requirement as follows:
-
-IF (<span>\({\dot Q_{lzj}}\)</span>&lt; 0) THEN
-
-<div>$${\omega_{SP\;Zj}} = {\omega_{Zj}} + {{{{\dot Q}_{lZj}}} \mathord{\left/ {\vphantom {{{{\dot Q}_{lZj}}} {{{\dot m}_{Zj}}}}} \right. } {{{\dot m}_{Zj}}}}$$</div>
-
-END IF
-
-<div>$${\omega_{SP\;Zj}} = MAX\left( {{\omega_{SP\;Zj}},\;{\omega_{SP\;Min}}} \right)$$</div>
-
-<div>$${\omega_{SP}} = MIN\left( {{\omega_{SP\;Zj}},\;{\omega_{SP\;Max}}} \right)$$</div>
-
-Note that a negative latent load means dehumidification is required. The supply air maximum humidity ratio setpoint <span>\({\omega_{SP}}\)</span>is constrained to be less than or equal to the maximum setpoint humidity ratio (user input) and greater than or equal to the minimum setpoint humidity ratio (user input). If the dehumidification load for all zones in the air loop is extremely small (i.e., no dehumidification load), the humidity ratio setpoint is set to the user input maximum value. <span>\({\omega_{SP}}\)</span>will be applied to the setpoint node or nodes specified in the SetpointManager:MultiZone:Humidity:Maximum object. A dehumidification component (e.g., an desiccant dehumidifier) placed upstream of this node can then use the humidity ratio setpoint to control its moisture removal rate. In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determines the minimum supply air temperature required to meet both the temperature (sensible) and dehumidification (latent) load in the control zone (ref: Controller:WaterCoil).
-
-### Follow Outdoor Air Temperature
-
-The input object SetpointManager:FollowOutdoorAirTemperature provides a setpoint manager that is used to place a temperature setpoint on a system node that is derived from the current outdoor air environmental conditions.  The outdoor air conditions are obtained from the weather information during the simulation.
-
-IF (ReferenceTemperatureType == OutdoorWetBulb)
-
-    Setpoint = OutdoorWetBulbTemp + OffSet
-
-ELSEIF (ReferenceTemperatureType == OutdoorDryBulb)
-
-    Setpoint = OutdoorDryBulbTemp + OffSet
-
-ENDIF
-
-Setpoint = MAX(Setpoint, MinSetPoint)
-
-Setpoint = MIN(Setpoint, MaxSetPoint)
-
-MinSetPoint, MaxSetPoint and Offset are specified by the user as the input in object SetpointManager:FollowOutdoorAirTemperature.
-
-### Follow System Node Temperature
-
-The input object SetpointManager:FollowSystemNodeTemperature provides a temperature setpoint on a system node that is derived from the current temperatures at a separate system node.  The current value of the temperature at a reference node are obtained and used to generate setpoint on a second system node.  If the reference node is also designated to be an outdoor air (intake) node, then this setpoint manager can be used to follow outdoor air conditions that are adjusted for altitude.
-
-IF (ReferenceTemperatureType == NodeWetBulb)
-
-    Setpoint = NodeWetbulbTemp + OffSet
-
-ELSEIF (ReferenceTemperatureType == NodeDryBulb)
-
-    Setpoint = NodeDrybulbTemp + OffSet
-
-ENDIF
-
-
-
-Setpoint = MAX(Setpoint, MinSetPoint)
-
-Setpoint = MIN(Setpoint, MaxSetPoint)
-
-MinSetPoint, MaxSetPoint and Offset are specified by the user as the input in object SetpointManager:FollowSystemNodeTemperature.
-
-### Follow Ground Temperature
-
-The input object SetpointManager:FollowGroundTemperature provides a temperature setpoint on a system node that is derived from a current ground temperature.  The ground temperatures are specified in different Site:GroundTemperature:\* objects and used during the simulation.  This setpoint manager is primarily intended for condenser or plant loops using some type of ground heat exchanger.
-
-
-
-IF (ReferenceGroundTemperatureObjectType == BuildingSurface)
-
-    Setpoint = GroundTemp + OffSet
-
-ELSEIF (ReferenceGroundTemperatureObjectType == Shallow)
-
-    Setpoint = GroundTemp\_Surface + OffSet
-
-ELSEIF (ReferenceGroundTemperatureObjectType == Deep)
-
-    Setpoint = GroundTemp\_Deep + OffSet
-
-ELSEIF (ReferenceTGroundTemperatureObjectType == FCfactorMethod)
-
-    Setpoint = GroundTemp\_FC + OffSet
-
-ENDIF
-
-Setpoint = MAX(Setpoint, MinSetPoint)
-
-Setpoint = MIN(Setpoint, MaxSetPoint)
-
-* *
-
-Where,
-
-GroundTemp = Current ground temperature (C)
-
-(Ref: Site:GroundTemperature:BuildingSurface)
-
-GroundTemp\_Surface = Current surface ground temperature  (C)
-
-(Ref: Site:GroundTemperature:Shallow)
-
-GroundTemp\_Deep  = Current deep ground temperature  (C)
-
-(Ref: Site:GroundTemperature:Deep)
-
-GroundTemp\_FC = Current ground temperature defined F or C factor method (C)
-
-(Ref: Site:GroundTemperature:FCfactorMethod)
-
-MinSetPoint, MaxSetPoint and Offset are specified by the user as the input in object SetpointManager:FollowGroundTemperature.
-
-### Condenser Entering Water Temperature Reset
-
-The object resets the condenser entering water temperature to the optimal cooling tower water set point temperature that will result in minimum net energy consumption for the chiller and cooling tower plant. This chiller-tower optimization scheme uses one curve to determine the optimum condenser entering water temperature for a given time step and two other curves to place limit conditions on the “optimized� set point value. The optimized condenser entering water temperature may not be valid every timestep then will be limited algorithmically by two boundary curves. The first of these boundary curves is given by:
-
-*MinDsnWB = C1 + C2\*OaWb + C3\*WPLR + C4\*TwrDsnWB + C5\*NF*
-
-where:
-
-*C1-C5* = curve coefficients
-
-*OaWb* = outside air wetbulb for current timestep, C
-
-*TwrDsnWB* = Tower design inlet Air Wet-Bulb Temperature, C
-
-*WPLR* = Weighted PLR
-
-    = ChillerCoolingLoadThisTimestep / NominalChillerCapacity
-
-NF = Normalized condenser water flow per unit of tower capacity, m3/W
-
-      = Design Tower Flow Rate / Design Tower Capacity *(typically 5.382E-8 m3/s, i.e., 3 gpm/ton)*
-
-MinDsnWB is compared against the design tower wetbulb. This curve is usually a function of Weighted PLR and NF. So if NF is constant at 5.382E-8 m3/s (3 gpm/ton), the curve can be depicted as follows:
-
-![](media/image6482.png)
-
-Figure 292. Minimum Tower Design Wet Bulb Boundary Condition
-
-The second boundary curve is given by:
-
-*MinActualWb = C1 + C2\*MinDsnWB + C3\*WPLR + C4\*TwrDsnWB + C5\*NF*
-
-where,
-
-*C1-C5 = curve coefficients*
-
-*MinDsnWB = from first boundary equation, C*
-
-*TwrDsnWB = Tower design inlet Air Wet-Bulb Temperature, C*
-
-*WPLR = Weighted PLR*
-
-*           = ChillerCoolingLoadThisTimestep / NominalChillerCapacity*
-
-*NF = Normalized condenser water flow per unit of tower capacity, m3/W*
-
-*      = Design Tower Flow Rate / Design Tower Capacity (typically 5.382E-8 m3/s, i.e., 3 gpm/ton)*
-
-MinActualWb is compared against this time step’s outside air wet bulb. This curve is usually a function of MinDesignWB, WeightedRatio and TwrDesignWB. So if TwrDesignWB is constant at 25.6 °C (78 °F), and NF = 5.382E-8 m3/s (3 gpm/ton), the curve can be depicted as follows:
-
-![](media/image6483.png)
-
-Figure 293. Minimum Wet Bulb Boundary Condition
-
-The Optimized Condenser Entering Water Temperature is calculated with this equation:
-
-*OptCondEntTemp = C1 + C2\*OaWb + C3\*WPLR + C4\*TwrDsnWB + C5\*NF*
-
-where,
-
-*C1-C5 = curve coefficients*
-
-*OaWB = this timestep’s outside air wetbulb, C*
-
-*TwrDsnWB = Tower design inlet Air Wet-Bulb Temperature, C*
-
-*WPLR = Weighted PLR*
-
-*           = ChillerCoolingLoadThisTimestep / NominalChillerCapacity*
-
-*NF = Normalized condenser water flow per unit of tower capacity, m3/W*
-
-*      = Design Tower Flow Rate / Design Tower Capacity (typically 5.382E-8 m3/s, i.e., 3 gpm/ton)*
-
-A graph of the curve can be depicted as follows:
-
-![](media/image6484.png)
-
-Figure 294. Optimum EWT vs PLR & OaWb
-
-The optimized condenser entering water temperature is calculated but is not necessarily used each timestep. If OptCondEntTemp does not fall within the bounds established by MinDsnWB and MinActualWb, then the value from the Default Condenser Entering Water Temperature Schedule is used for the Condenser Entering Water Set Point instead.
-
-#### Special Note for Multiple Towers
-
-This control scheme is available for multiple towers by following two steps:
-
- - Use average tower conditions in the curves for the independent variables related to the towers
- - Make sure the setpoint is applied to either the condenser supply outlet node or use a node list to apply it to each tower outlet node
-
-### Ideal Condenser Entering Water Temperature Reset
-
-The object determines a “near-optimal� condenser water entering set point at each time step that will result in minimum net energy consumption for the chiller and cooling tower plant. The “ideal� chiller-tower optimization scheme uses a search algorithm to find the ideal optimal setpoint at a given timestep. This requires resimulating HVAC systems at each timestep until finding an “optimal� condenser water entering setpoint (OptSetpoint) which gives the minimum total chiller, cooling tower, chilled water pump and condenser water pump power consumption (TEC). The OptSetpoint falls between realistic minimum and maximum boundaries, which are set by the user. The minimum boundary is determined based on the minimum lift (user input) and evaporator leaving water temperature. The maximum boundary is specified by the user. It is assumed that a single minimum point exists between these boundaries. The following steps are used to find “optimal� setpoint:
-
-1)   Set an initial setpoint value for the iteration to a user-defined maximum condenser entering water temperature (Toptset<sub>1</sub>) and calculate TEC.
-
-2)   Decrease the setpoint value by 1˚C (Toptset<sub>2</sub>=Toptset<sub>1</sub>–1˚C) and calculate TEC.
-
-3)   Compare the TEC in Step 1 (TEC<sub>1</sub>) and TEC in Step 2 (TEC<sub>2</sub>), i.e., (dTEC<sub>1</sub>=TEC<sub>1</sub>–TEC<sub>2</sub>).
-
-4)   If dTEC<sub>1</sub> is negative, stop the iteration and set the “optimal� setpoint to Toptset<sub>1</sub>.
-
-5)   If dTEC<sub>1</sub> is positive, Decrease the setpoint value by 1˚C and calculate TEC. Compare the TECs and repeat this step (i.e., dTEC<sub>N</sub>=TEC<sub>N</sub>–TEC<sub>N+1</sub>) until either Toptset<sub>N+1</sub> reaches to the minimum boundary value or dTEC<sub>N</sub> becomes negative.
-
-6)   If Toptset<sub>N</sub> reaches to the minimum boundary value and still dTEC<sub>N</sub> is positive, set the “optimal� setpoint to Toptset<sub>N+1</sub>.
-
-7)   If TEC<sub>N</sub> becomes negative, decrease Toptset<sub>N-1</sub> by 0.2˚C and calculate TEC. Compare the TECs and repeat this step (i.e., dTEC<sub>M</sub>=TEC<sub>M</sub>–TEC<sub>M+1</sub>) until dTEC<sub>M</sub> becomes negative. Then set the “optimal� setpoint to Toptset<sub>M+1</sub>.
-
-### Plant Return Water Control Setpoint Reset
-
-The input objects:
-
-* SetpointManager:ReturnTemperature:ChilledWater, and 
-
-* SetpointManager:ReturnTemperature:HotWater
-
-allow for controlling the temperature of the water (or a different fluid defined for the plant) that is returning back to the plant supply equipment.  In a typical chilled water loop configuration, this is essentially controlling the temperature of the water entering the chiller.  In a typical hot water loop configuration, this is essentially controlling the temperature of the water entering the boiler.
-
-The target return temperature can be specified by:
-
-* providing a constant value to use throughout the simulation, or
-
-* scheduling the value to vary through the simulation (which then allows custom EMS overriding of the scheduled value), or
-
-* using a separate setpoint manager to set the setpoint on the return node itself, which is then retrieved by this reset manager.  
-
-#### Operation
-
-The setpoint manager senses conditions on two named nodes, which should correspond to a central plant's supply side inlet and outlet nodes, the return and supply nodes, respectively.  The temperature and flow rate information is used in a series of calculations in order to determine a setpoint to specify on the supply outlet node which will in turn provide the target desired return temperature on the supply inlet node.  The calculations are summarized for a chilled water loop here:
-
-1. Use the current supply and demand temperatures to calculate an average temperature for property calculation: <span>\(C_p = f\left(T_{avg}\right) = f\left(\frac{T_{ret}+T_{sup}}{2}\right)\)</span>
-
-2. Calculate the current loop demand using: <span>\(\dot{Q} = \dot{m} * C_p * \left(T_{ret} - T_{sup}\right)\)</span>
-
-3. Assuming that this load will be the same moving forward, we can calculate what supply temperature we should target in order to meet the desired return temperature.
-
-4. So retrieve the current target return temperature, <span>\(T_{ret,target}\)</span>, either from a schedule or constant value.
-
-5. Then calculate the supply temperature setpoint using: <span>\(T_{sup,sp} = T_{ret,target} - \frac{\dot{Q}}{\dot{m} C_p}\)</span>
-
-6. Constrain the value to user-specified limiting min/max values
-
-For a chilled water loop, the user-specified minimum is the default setpoint used in cases of no-load or negative-load.  In a hot-water loop the user-specified maximum is used for these situations.  Also, in a hot-water loop the sign of the demand will be reversed.
-
-#### Key control note
-
-The setpoint will be reset at the beginning of a system time step, and remain that way through that time step.  The setpoint is calculated based on the latest known value of loop demand and loop flow rate.  If the demand and flow rate remain the same for the currently calculated time step, the loop will maintain control well.  However, if either changes, there will be a lag effect while the loop attempts to maintain control.  Consider the following plot, with a short description following:
-
-![](media/SetPointManager-ResetForReturnControl1.png)
-
-Throughout the day, the heat addition (green line) to the loop increases.  Each time it increases, there is a small period of time where the loop attempts to regain control of the return temperature.  The setpoint is only reset at the beginning of the system time step, so as the plant converges within a single time step, the load will vary and the return temperature may not be exactly on target.
-
-This isn't necessarily a big problem.  However, some users may be especially interested in very tight control of the return temperature.  This can be done very easily by simply reducing the simulation time step.  For example, in the following plot, the time step was reduced from 10 minutes to 1 minute, with some description following the plot:
-
-![](media/SetPointManager-ResetForReturnControl2.png)
-
-With the smaller time step, the reporting frequency is higher.  But more importantly, with the smaller time step, the setpoint can be corrected much more often.  Because of this, the return temperature regains control much quicker than with the larger time step.  
-
-However, these examples are for a jagged demand profile full of discontinuous step changes in loop demand.  As a final example, this return water temperature control is applied to the large office reference building chilled water loop.  Here is the response:
-
-![](media/SetPointManager-ResetForReturnControl3.png)
-
-Note the control is working properly, maintaining a return temperature around the target of 12 degrees where possible.  Since the load profile is a typical -smooth- profile, the control is also much smoother.  This should be a good representation of the capabilities of this setpoint manager.
-
-For jagged load profiles, if tight control is highly important, choosing a smaller timestep (~1 minute) is recommended.  For normal building profiles, the typical range of timesteps (~15 minute) should be fully satisfactory.
-
-Solar Collectors <a name="SolarCollectors"></a>
-----------------
-
-Solar collectors are devices that convert solar energy into thermal energy by raising the temperature of a circulating heat transfer fluid.  The fluid can then be used to heat water for domestic hot water usage or space heating.  Flat-plate solar collectors using water as the heat transfer fluid, Integral-Collector Storage solar collectors using water and unglazed transpired solar collectors using air are currently the only types of collector available in EnergyPlus.
-
-### Flat-Plate Solar Collectors
-
-The input object SolarCollector:FlatPlate:Water provides a model for flat-plate solar collectors that are the most common type of collector.  Standards have been established by ASHRAE for the performance testing of these collectors (ASHRAE 1989; 1991) and the Solar Rating and Certification Corporation (SRCC) publishes a directory of commercially available collectors in North America (SRCC 2003).
-
-The EnergyPlus model is based on the equations found in the ASHRAE standards and Duffie and Beckman (1991).  This model applies to glazed and unglazed flat-plate collectors, as well as banks of tubular, i.e. evacuated tube, collectors.
-
-#### Solar and Shading Calculations
-
-The solar collector object uses a standard EnergyPlus surface in order to take advantage of the detailed solar and shading calculations.  Solar radiation incident on the surface includes beam and diffuse radiation, as well as radiation reflected from the ground and adjacent surfaces.  Shading of the collector by other surfaces, such as nearby buildings or trees, is also taken into account.  Likewise, the collector surface can shade other surfaces, for example, reducing the incident radiation on the roof beneath it.
-
-#### Thermal Performance
-
-The thermal efficiency of a collector is defined as the ratio of the useful heat gain of the collector fluid versus the total incident solar radiation on the gross surface area of the collector.
-
-<div>$$\eta  = \frac{{(q/A)}}{{{I_{solar}}}}$$</div>
-
-where
-
-q = useful heat gain
-
-A = gross area of the collector
-
-I<sub>solar</sub> = total incident solar radiation
-
-Notice that the efficiency h is only defined for I<sub>solar</sub> &gt; 0.
-
-An energy balance on a solar collector with double glazing shows relationships between the glazing properties, absorber plate properties, and environmental conditions.
-
-<div>$$\frac{q}{A} = {I_{solar}}{\tau_{g1}}{\tau_{g2}}{\alpha_{abs}} - \frac{{T_{abs}^4 - T_{g2}^4}}{{{R_{rad}}}} - \frac{{{T_{abs}} - {T_{g2}}}}{{{R_{conv}}}} - \frac{{{T_{abs}} - {T_{air}}}}{{{R_{cond}}}}$$</div>
-
-where
-
-t<sub>g1</sub> = transmittance of the first glazing layer
-
-t<sub>g2</sub> = transmittance of the second glazing layer
-
-a<sub>abs</sub> = absorptance of the absorber plate
-
-R<sub>rad</sub> = radiative resistance from absorber to inside glazing
-
-R<sub>conv</sub> = convective resistance from absorber to inside glazing
-
-R<sub>cond</sub> = conductive resistance from absorber to outdoor air through the insulation
-
-T<sub>abs</sub> = temperature of the absorber plate
-
-T<sub>g2</sub> = temperature of the inside glazing
-
-T<sub>air</sub> = temperature of the outdoor air
-
-The equation above can be approximated with a simpler formulation as:
-
-<div>$$\frac{q}{A} = {F_R}\left[ {{I_{solar}}(\tau \alpha ) - {U_L}({T_{in}} - {T_{air}})} \right]$$</div>
-
-where
-
-F<sub>R</sub> = an empirically determined correction factor
-
-(ta) = the product of all transmittance and absorptance terms
-
-U<sub>L</sub> = overall heat loss coefficient combining radiation, convection, and conduction terms
-
-T<sub>in</sub> = inlet temperature of the working fluid
-
-Substituting this into Equation ,
-
-<div>$$\eta  = {F_R}(\tau \alpha ) - {F_R}{U_L}\frac{{({T_{in}} - {T_{air}})}}{{{I_{solar}}}}$$</div>
-
-A linear correlation can be constructed by treating F<sub>R</sub>(ta) and -F<sub>R</sub>U<sub>L</sub> as characteristic constants of the solar collector:
-
-<div>$$\eta  = {c_0} + {c_1}\frac{{\left( {{T_{in}} - {T_{air}}} \right)}}{{{I_{solar}}}}$$</div>
-
-Similarly, a quadratic correlation can be constructed using the form:
-
-<div>$$\eta  = {c_0} + {c_1}\frac{{\left( {{T_{in}} - {T_{air}}} \right)}}{{{I_{solar}}}} + {c_2}\frac{{{{\left( {{T_{in}} - {T_{air}}} \right)}^2}}}{{{I_{solar}}}}$$</div>
-
-Both first- and second-order efficiency equation coefficients are listed in the *Directory of SRCC Certified Solar Collector Ratings*.
-
-#### Incident Angle Modifiers
-
-As with regular windows the transmittance of the collector glazing varies with the incidence angle of radiation.  Usually the transmittance is highest when the incident radiation is normal to the glazing surface.  Test conditions determine the efficiency coefficients for normal incidence.  For off-normal angles, the transmittance of the glazing is modified by an *incident angle modifier* coefficient.
-
-<div>$${K_{\tau \alpha }} = \frac{{\left( {\tau \alpha } \right)}}{{{{\left( {\tau \alpha } \right)}_n}}}$$</div>
-
-Additional testing determines the incident angle modifier as a function of incident angle q.  This relationship can be fit to a first-order, linear correlation:
-
-<div>$${K_{\tau \alpha }} = 1 + {b_0}\left( {\frac{1}{{\cos \theta }} - 1} \right)$$</div>
-
-or a second-order, quadratic correlation:
-
-<div>$${K_{\tau \alpha }} = 1 + {b_0}\left( {\frac{1}{{\cos \theta }} - 1} \right) + {b_1}{\left( {\frac{1}{{\cos \theta }} - 1} \right)^2}$$</div>
-
-The incident angle modifier coefficients *b<sub>0</sub>* and *b<sub>1</sub>* are usually negative, although some collectors have a positive value for *b<sub>0</sub>*.  Both first- and second-order incident angle modifier equation coefficients are listed in the *Directory of SRCC Certified Solar Collector Ratings*.
-
-The SRCC incident angle modifier equation coefficients are only valid for incident angles of 60 degrees or less.  Because these curves can be valid yet behave poorly for angles greater than 60 degree, the EnergyPlus model cuts off collector gains for incident angles greater than 60 degrees.
-
-For flat-plate collectors, the incident angle modifier is generally symmetrical.  However, for tubular collectors the incident angle modifier is different depending on whether the incident angle is parallel or perpendicular to the tubes.  These are called bi-axial modifiers.  Some special flat-plate collectors may also exhibit this asymmetry.  The current model cannot yet handle two sets of incident angle modifiers.  In the meantime it is recommended that tubular collectors be approximated with caution using either the parallel or perpendicular correlation.
-
-Incident angle modifiers are calculated separately for sun, sky, and ground radiation.  The net incident angle modifier for all incident radiation is calculated by weighting each component by the corresponding modifier.
-
-<div>$${K_{\tau \alpha ,net}} = \frac{{{I_{beam}}{K_{\tau \alpha ,beam}} + {I_{sky}}{K_{\tau \alpha ,sky}} + {I_{gnd}}{K_{\tau \alpha ,gnd}}}}{{{I_{beam}} + {I_{sky}} + {I_{gnd}}}}$$</div>
-
-For sky and ground radiation the incident angle is approximated using Brandemuehl and Beckman's equations:
-
-<div>$${\theta_{sky}} = 59.68 - 0.1388\phi  + 0.001497{\phi ^2}$$</div>
-
-<div>$${\theta_{ground}} = 90.0 - 0.5788\phi  + 0.002693{\phi ^2}$$</div>
-
-where f is the surface tilt in degrees.
-
-The net incident angle modifier is then inserted into the useful heat gain equation :
-
-<div>$$\frac{q}{A} = {F_R}\left[ {{I_{solar}}{K_{\tau \alpha ,net}}{{(\tau \alpha )}_n} - {U_L}({T_{in}} - {T_{air}})} \right]$$</div>
-
-Equation is also modified accordingly.
-
-<div>$$\eta  = {F_R}{K_{\tau \alpha ,net}}{(\tau \alpha )_n} - {F_R}{U_L}\frac{{({T_{in}} - {T_{air}})}}{{{I_{solar}}}}$$</div>
-
-#### Outlet Temperature
-
-Outlet temperature is calculated using the useful heat gain q as determined by Equation , the inlet fluid temperature T<sub>in</sub>, and the mass flow rate available from the plant simulation:
-
-<div>$$\frac{q}{A} = \dot m{c_p}({T_{out}} - {T_{in}})$$</div>
-
-where
-
-<span>\(\dot m\)</span> = fluid mass flow rate through the collector
-
-c<sub>p</sub> = specific heat of the working fluid
-
-Solving for T<sub>out</sub>,
-
-<div>$${T_{out}} = {T_{in}} + \frac{q}{{\dot m{c_p}A}}$$</div>
-
-If there is no flow through the collector, T<sub>out</sub> is the stagnation temperature of the fluid.  This is calculated by setting the left side of Equation to zero and solving for T<sub>in</sub> (which also equals T<sub>out</sub> for the no flow case).
-
-#### References
-
-ASHRAE.  1989.  ASHRAE Standard 96-1980 (RA 89):  Methods of Testing to Determine the Thermal Performance of Unglazed Flat-Plate Liquid-Type Solar Collectors.  Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-ASHRAE.  1991.  ASHRAE Standard 93-1986 (RA 91):  Methods of Testing to Determine the Thermal Performance of Solar Collectors.  Atlanta: American Society of Heating, Refrigerating and Air-Conditioning Engineers, Inc.
-
-Duffie, J. A., and Beckman, W. A.  1991.  Solar Engineering of Thermal Processes, Second Edition.  New York:  Wiley-Interscience.
-
-Solar Rating and Certification Corporation.  2004.  Directory of SRCC Certified Solar Collector Ratings, OG 100.  Cocoa, Florida:  Solar Rating and Certification Corporation.
-
-### Integral-collector-storage (ICS) Solar Collector
-
-Solar collectors with integral storage unit models use SolarCollector:IntegralCollectorStorage object, and the characteristics parameter inputs of this collector are provided by the SolarCollectorPerformance:IntegralCollectorStorage object. This model is based on detailed Energy Balance equations of solar collectors that integrates storage in it. This model has two options to represent the collector bottom outside boundary conditions: AmbientAir, and OtherSideConditionsModel. AmbientAir simply applies outside air temperature using combined convection and radiation conductance, and the OtherSideConditionsModel applies combined radiation and convection models that exiats in a naturally ventilated cavity to represent the collector bottom outside boundary condition. The later boundary condition accounts for the shading of the collector on the underlying surface, hence, the ICS collector can be assumed as an integral part of the building envelope. Schematic diagram of a rectangular ICS solar collector is shown in Figure 295 below:
-
-![](media/image6502.png)
-
-Figure 295. Schematic diagram of rectangular Integrated Collector Storage unit
-
-#### Solar and Shading Calculations
-
-The solar collector object uses a standard EnergyPlus surface in order to take advantage of the detailed solar and shading calculations. Solar radiation incident on the surface includes beam and diffuse radiation, as well as radiation reflected from the ground and adjacent surfaces. Shading of the collector by other surfaces, such as nearby buildings or trees, is also taken into account. Likewise, the collector surface shades the roof surface beneath it, hence no direct solar radiation incident on the roof surface. The collector and the roof outside boundary conditions should be specified as OtherSideConditionModel to account for solar collector shading impact on the roof surface.
-
-#### Mathematical Model
-
-The integral-collector-storage (ICS) solar collector is represented using two transient energy balance equations shown below.  These equations represent the energy balance equation for the absorber plate, and the water in the collector.
-
-<div>$${m_p}{C_p}\frac{{d{T_p}}}{{dt}} = A \cdot \left[ {{{\left( {\tau \alpha } \right)}_e} \cdot {I_t} - {h_{pw}}\left( {{T_p} - {T_w}} \right) - {U_t}\left( {{T_p} - {T_a}} \right)} \right]$$</div>
-
-<div>$${m_w}{C_w}\frac{{d{T_w}}}{{dt}} = A \cdot \left[ {{h_{pw}}\left( {{T_p} - {T_w}} \right) - {U_b}\left( {{T_w} - {T_{OSC}}} \right) - {U_s}\left( {{T_w} - {T_a}} \right)} \right] - {\dot m_w}{C_w}\left( {{T_w} - {T_{wi}}} \right)$$</div>
-
-Where,
-
-*m<sub>p</sub>C<sub>p</sub>*<sub>      </sub>= thermal capacity of the absorber surface, J/°C
-
-A        = collector gross area, m<sup>2</sup>
-
-*(ta)*<sub>e</sub>    = transmittance-absorptance product of the absorber plate and cover system
-
-*I<sub>t</sub>*        = total solar irradiation, (W/m<sup>2</sup>)
-
-*h<sub>pw</sub>*      = convective heat transfer coefficient from absorber plate to water, (W/m2°K)
-
-*U<sub>t</sub>*        = overall heat loss coefficient from absorber to the ambient air, (W/m2 °K)
-
-*T<sub>p</sub>*        = absorber plate average temperature, (°C)
-
-*T<sub>w</sub>*       = collector water average temperature, (°C)
-
-*T<sub>a</sub>*        = ambient air temperature, (°C)
-
-*m<sub>w</sub>C<sub>pw</sub>* = thermal capacity of the water mass in the collector, (J/°C)
-
-*U<sub>s</sub>*       = area-weighted conductance of the collector side insulation, (W/m<sup>2</sup>×°K)
-
-*U<sub>b</sub>*       = conductance of the collector bottom insulation, (W/m<sup>2</sup>×°K)
-
-*T<sub>osc</sub>*      =    outside temperature of bottom insulation determined from the other side condition model, (°C)
-
-*T<sub>wi</sub>*       = Entering makeup or mains water temperature, (°C)
-
-<span>\({\dot m_w}{C_w}\)</span>= water capacity flow through the collector, (W/°C)
-
-The other side condition model boundary condition represented by the *T<sub>osc</sub>*, allows us to apply a realistic outside boundary condition for a collector mounted on a building roof.  This also accounts for the shading impact of the collector on the under-laying surface (roof).  On the other hand if ambient air boundary condition is specified, then the collector does not shade the underlying surface it is mounted on.
-
-The two energy balance equation can be written as non-homogeneous first order DE with constant coefficients. The initial conditions for these equations are the absorber plate average temperature and the collector water average temperature at previous time steps.
-
-<div>$$\frac{{d{T_p}}}{{dt}} = {a_1}{T_p} + {a_2}{T_w} + {a_3}$$</div>
-
-<div>$$\frac{{d{T_w}}}{{dt}} = {b_1}{T_p} + {b_2}{T_w} + {b_3}$$</div>
-
-<div>$${a_1} =  - \left( {A \cdot {h_{pw}} + A \cdot {U_t}} \right)/\left( {{m_p} \cdot {C_p}} \right)$$</div>
-
-<div>$${a_2} = A \cdot {h_{pw}}{T_w}/\left( {{m_p} \cdot {C_p}} \right)$$</div>
-
-<div>$${a_3} = A \cdot {\left( {\tau \alpha } \right)_e} \cdot {I_t} + A \cdot {U_t}{T_a}$$</div>
-
-<div>$${b_1} = A \cdot {h_{pw}}{T_p}/\left( {{m_w} \cdot {C_w}} \right)$$</div>
-
-<div>$${b_2} =  - \left( {A \cdot {h_{pw}} + A \cdot {U_b} + A \cdot {U_s} + {{\dot m}_w}{C_w}} \right)$$</div>
-
-<div>$${{\rm{b}}_{\rm{3}}} = {\rm{ }}\left( {A \cdot {U_b}{T_{osc}} + A \cdot {U_s}{T_a} + {{\dot m}_w}{C_w}{T_{wi}}} \right)$$</div>
-
-The two coupled first order differential equation are solved analytically.  Auxiliary equation of the the coupled homogeneous differential equation is given by:
-
-<div>$${\lambda ^2} - ({a_1} + {b_2}) + ({a_1}{b_2} - {a_2}{b_1}) = 0$$</div>
-
-This auxiliary quadratic equation has always two distinct real roots (l<sub>1</sub> and l<sub>2</sub>) hence the solution of the homogeneous equation is exponential, and the general solutions of the differential equations are given by:
-
-<div>$${T_p} =  {c_1}{e^{{l_1}t}} + {c_2}{e^{{l_2}t}} + A$$</div>
-
-<div>$${T_w} =  {r_1}{c_1}{e^{{l_1}t}} + {r_2}{c_2}{e^{{l_2}t}} + B$$</div>
-
-The constant terms *A* and *B* are the particular solution of the non-homogeneous differential equations, the coefficients of the exponential terms (*c<sub>1</sub>*, *c<sub>2</sub>*, *r<sub>1</sub>*, and *r<sub>2</sub>*) are determined from the initial conditions of the absorber and collector water temperatures (*T<sub>p0</sub>*, *T<sub>w0</sub>*) and are given by:
-
-<div>$${r_1} =  ({l_1} - {a_1})/{a_2};\quad {r_2} =  ({l_2} - {a_1})/{a_2}$$</div>
-
-<div>$$A =  ( - {a_3}{b_2} + {b_3}{a_2})/({a_1}{b_2} - {b_1}{a_2});\quad B =  ( - {a_1}{b_3} + {b_1}{a_3})/({a_1}{b_2} - {b_1}{a_2})$$</div>
-
-<div>$${c_1} =  ({r_2}{T_{p0}} - {T_{w0}} - {r_2}A + B)/({r_2} - {r_1});\quad {c_2} =  ({T_{w0}} - {r_1}{T_{p0}} + {r_1}A - B)/({r_2} - {r_1})$$</div>
-
-#### Thermal Network Model:
-
-The thermal network model requires energy balance for each of the collector covers as well.  The heat balance equation of the collector covers is assumed to obey steady state formulation by ignoring their thermal mass. The thermal-network representation of the ICS collector is shown in Figure 296. Also, the heat balance at each cover surface requires knowledge of the amount of solar fraction absorbed, which is determined from the ray tracing analysis. For the thermal network model shown above the overall top heat loss coefficient is determined from combination of the resistances in series as follows:
-
-<div>$${U_t} = {\left[ {{R_1} + {R_2} + {R_3}} \right]^{ - 1}}$$</div>
-
-Or
-
-<div>$${U_t} = {\left[ {\frac{1}{{{h_{c,\,c1 - a}} + {h_{r,\,c1 - a}}}} + \frac{1}{{{h_{c,\,c2 - c1}} + {h_{r,\,c2 - c1}}}} + \frac{1}{{{h_{c,\,p - c2}} + {h_{r,\,p - c2}}}}} \right]^{ - 1}}$$</div>
-
-The convection and radiation heat transfer coefficients in equation above are calculated based on temperatures at the previous time step and determined as described in the *Heat Transfer Coefficients* section.
-
-![](media/image6522.png)
-
-Figure 296. Thermal network diagram for ICS Solar Collector
-
-***Collector Cover Heat Balance***
-
-Ignoring the thermal mass of the collector cover, a steady state heat balance equations are formulated for each cover that allow us to determine cover temperatures.  The cover surface heat balance representation is shown in Figure 297 below.
-
-![](media/image6523.png)
-
-Figure 297. Collector Cover Surface Heat Balance
-
-The steady state cover heat balance equation is given by:
-
-<div>$${q_{LWR,{\kern 1pt} 1}} + {q_{CONV,{\kern 1pt} 1}} + {q_{solar,{\kern 1pt} abs}} + {q_{LWR,{\kern 1pt} 2}} + {q_{CONV,{\kern 1pt} 2}} = 0$$</div>
-
-Linearizing the longwave radiation exchange and representing the convection terms using the classical equation for Newton’s law of cooling, the equations for the temperatures of covers 1 and 2 are given by:
-
-<div>$${T_{c{\rm{1}}}} = \frac{{{\alpha_{c1}}{I_t} + {h_{r,{\kern 1pt} c1 - a}}{T_a} + {h_{c,{\kern 1pt} c1 - a}}{T_a} + {h_{r,{\kern 1pt} c2 - c1}}{T_{c2}} + {h_{c,{\kern 1pt} c2 - c1}}{T_{c2}}}}{{{h_{r,{\kern 1pt} c1 - a}} + {h_{c,{\kern 1pt} c1 - a}} + {h_{r,{\kern 1pt} c2 - c1}} + {h_{c,{\kern 1pt} c2 - c1}}}}$$</div>
-
-<div>$${T_{c2}} = \frac{{{\alpha_{c2}}{I_t} + {h_{r,{\kern 1pt} c2 - c1}}{T_{c1}} + {h_{c,{\kern 1pt} c2 - c1}}{T_{c1}} + {h_{r,{\kern 1pt} p - c2}}{T_p} + {h_{c,{\kern 1pt} p - c2}}{T_p}}}{{{h_{r,{\kern 1pt} c2 - c1}} + {h_{c,{\kern 1pt} c2 - c1}} + {h_{r,{\kern 1pt} p - c2}} + {h_{c,{\kern 1pt} p - c2}}}}$$</div>
-
-Where,
-
-*a<sub>c</sub>*   = the weighted average solar absorptance of covers *1* and *2*, (-)
-
-*h<sub>r,c1-a</sub>*           = adjusted radiation heat transfer coefficient between cover *1* and the ambient air, (W/m<sup>2</sup>×K)
-
-*h<sub>c,c1-a</sub>*           = convection heat transfer coefficient between cover *1* and the ambient, (W/m<sup>2</sup>×K)
-
-*h<sub>r,c2-c1</sub>*          = radiation heat transfer coefficient between covers *1* and *2*, (W/m<sup>2</sup>×K)
-
-*h<sub>c,c2-c1</sub>*          = convection heat transfer coefficient between covers *1* and *2*, (W/m<sup>2</sup>×K)
-
-*h<sub>r,p-c2</sub>*           = radiation heat transfer coefficient between covers *2* and the absorber plate, (W/m<sup>2</sup>×K)
-
-*h<sub>c,p-c2</sub>*           = convection heat transfer coefficient between covers *2* and the absorber plate, (W/m<sup>2</sup>×K)
-
-*q<sub>LWR,1</sub>*          = longwave radiation exchange flux on side *1* of the collector cover, (W/m<sup>2</sup>)
-
-*q<sub>CONV,1</sub>*         = convection heat flux on side *1* of the collector cover, (W/m<sup>2</sup>)
-
-*q<sub>LWR,2</sub>*          = longwave radiation exchange flux on side *2* of the collector cover, (W/m<sup>2</sup>)
-
-*q<sub>CONV,2</sub>*         = convection heat flux on side *2* of the collector cover, (W/m<sup>2</sup>)
-
-*q<sub>solar,abs</sub>*         = net solar radiation absorbed by the collector cover, (W/m<sup>2</sup>)
-
-*R*    = thermal resistance for each section along the heat flow path, (m<sup>2</sup>K/W)
-
-#### Other Side Condition Model
-
-ICS Solar Collectors are commonly mounted on building heat transfer surfaces hence the collectors shade the underlying heat transfer surface and require a unique boundary condition that reflects the air cavity environment created between the bottom of the collector surface and the underlying surface. The other side condition model that allows us to estimate the other side temperature, *T<sub>osc</sub>*, can be determined based on steady state heat balance using the known collector water temperature at the previous time step.
-
-![](media/image6527.png)
-
-Figure 298. Illustration for Other Side Condition Model
-
-Ignoring thermal mass of the collector bottom insulation, steady state surface heat balance can be formulated on the outer plane of the collector bottom surface facing the cavity as shown in Figure 4.  The heat balance equation on the outer plane of the collector bottom surface is given by:
-
-<div>$${q_{cond}} + {q_{conv,{\kern 1pt} cav}} + {q_{rad,{\kern 1pt} cav}} = 0$$</div>
-
-Substituting the equations for each term in the above equation yields:
-
-<div>$${U_L}\left( {{T_w} - {T_{osc}}} \right) + {h_{c,{\kern 1pt} cav}}\left( {{T_{a,{\kern 1pt} cav}} - {T_{osc}}} \right) + {h_{r,{\kern 1pt} cav}}\left( {{T_{so}} - {T_{osc}}} \right) = 0$$</div>
-
-Simplifying yields the bottom insulation other side condition temperature:
-
-<div>$${T_{osc}} = \frac{{{U_L}{T_w} + {h_{c,{\kern 1pt} cav}}{T_{a,{\kern 1pt} cav}} + {h_{r,{\kern 1pt} cav}}{T_{so}}}}{{{U_L} + {h_{c,{\kern 1pt} cav}} + {h_{r,{\kern 1pt} cav}}}}$$</div>
-
-The cavity air temperature is determined from cavity air heat balance as follows:
-
-<div>$${T_{a,{\kern 1pt} cav}} = \frac{{{h_{c,{\kern 1pt} cav}}A{T_{osc}} + {{\dot m}_{vent}}Cp{T_a} + {h_{c,{\kern 1pt} cav}}A{T_{so}}}}{{{h_{c,{\kern 1pt} cav}}A + {{\dot m}_{vent}}Cp + {h_{c,{\kern 1pt} cav}}A}}$$</div>
-
-Where
-
-*h<sub>r,\\ cav</sub>*            = linearized radiation coefficient for underlying surface in the cavity, (W/m<sup>2</sup>×K)
-
-*h<sub>c,\\ cav</sub>*           = convection coefficient for underlying surface in the cavity, (W/m<sup>2</sup>×K)
-
-*T<sub>so</sub>*   = the outside face temperature of the underlying heat transfer surface, (ºC)
-
-<span>\({\dot m_{vent}}\)</span>          = air mass flow rate due to natural ventilation, (kg/s)
-
-*q<sub>cond</sub>*            = conduction heat flux though the insulation bottom and, (W/m<sup>2</sup>)
-
-*q<sub>conv,cav</sub>*         = convection heat flux between the collector bottom outside surface and the cavity air, (W/m<sup>2</sup>)
-
-*q<sub>rad,cav</sub>*          =          longwave radiation exchange flux between the collector bottom outside surface and the outside surface of the underlying surface, (W/m<sup>2</sup>)
-
-The cavity air temperature is determined from the cavity air energy balance.  The air heat balance requires the ventilated cavity air natural ventilation rates.  The calculation of the ventilation rate is described else where in this document. The SurfaceProperty:ExteriorNaturalVentedCavity, object is required to describe the surface properties, the characteristics of the cavity and opening for natural ventilation.
-
-#### Heat Transfer Coefficients
-
-The equations used to determine for the various heat transfer coefficients in the absorber and water heat balance equations are given below. The absorbed solar energy is transferred to the water by convection.  Assuming natural convection dominated heat transfer for a hot surface facing down and a clod surface facing down the following correlation for Nusselt number by Fujii and Imura (1972).  The Nusselt number for hot surface facing down ward is given by:
-
-<div>$$Nu = 0.56{\left( {Gr \cdot \Pr  \cdot cos{\kern 1pt} \theta } \right)^{1/5}}\quad {10^5} &lt; Gr \cdot Pr &lt; {10^{11}}$$</div>
-
-The Nusselt number for hot surface upward and cold surface facing down is given by:
-
-<div>$$Nu = 0.13{\left( {Gr \cdot \Pr } \right)^{1/3}}\quad Gr \cdot Pr &lt; 5.0 \times {10^8}$$</div>
-
-<div>$$Nu = 0.16{\left( {Gr \cdot \Pr } \right)^{1/3}}\quad Gr \cdot Pr > 5.0 \times {10^8}$$</div>
-
-<div>$$Gr = {{g{\beta_{\rm{v}}}\left( {{T_p} - {T_w}} \right)L_c^3} \mathord{\left/ {\vphantom {{g{\beta_{\rm{v}}}\left( {{T_p} - {T_w}} \right)L_c^3} {{\nu ^2}}}} \right. } {{\nu ^2}}}$$</div>
-
-<div>$$\Pr  = {\nu  \mathord{\left/ {\vphantom {\nu  \alpha }} \right. } \alpha }$$</div>
-
-<div>$${T_r} = {T_p} - 0.25\left( {{T_p} - {T_w}} \right)$$</div>
-
-<div>$${h_w} = {{Nu \cdot k} \mathord{\left/ {\vphantom {{Nu \cdot k} {{L_c}}}} \right. } {{L_c}}}$$</div>
-
-Where,
-
-<span>\(\theta \)</span>= angle of inclination of the collector to the vertical, radians
-
-*g*    = gravitation force constant, 9.806 (m/s<sup>2</sup>)
-
-*T<sub>r</sub>*   = reference properties where the thermo-physical properties are calculated, (°C)
-
-*L<sub>c</sub>*   = characteristic length for the absorber plate, (m)
-
-*k*    = thermal conductivity of water at reference temperature, (W/m×K)
-
-*n*    = kinematic viscosity of water at reference temperature, (m<sup>2</sup>/s)
-
-*a*    = thermal diffusivity of water at reference temperature, (m<sup>2</sup>/s)
-
-*β<sub>v</sub>*   = volumetric expansion coefficient evaluated at Tv, Tv =Tw+0.25(Tp-Tw), (K-1)
-
-*Nu*  = Nusselt number calculated for water properties at the reference temperature, (-)
-
-*Gr*   = Grashof number calculated for water properties at the reference temperature, (-)
-
-*Pr*   = Prandtle number calculated for water properties at the reference temperature, (-)
-
-The various radiation and convection heat transfer coefficients are given by the following equations.  The convection heat transfer coefficients between the covers and the absorber plate are estimated from the empirical correlation for the Nusselt number for air gap between two parallel plates developed by Hollands et al. (1976) is:
-
-<div>$$N{u_a} = 1 + 1.44\left\{ {1 - \frac{{1708{{\left( {\sin 1.8\beta } \right)}^{1.6}}}}{{Ra\cos \beta }}} \right\}{\left\{ {1 - \frac{{1708}}{{Ra\cos \beta }}} \right\}^ + } + {\left\{ {{{\left( {\frac{{Ra\cos \beta }}{{5830}}} \right)}^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.}\!\lower0.7ex\hbox{$3$}}}} - 1} \right\}^ + }$$</div>
-
-<div>$${h_c} = {{Nu \cdot k} \mathord{\left/ {\vphantom {{Nu \cdot k} L}} \right. } L}$$</div>
-
-<div>$${h_{rp - c2}} = \frac{{\sigma \left( {{T_p} + {T_{c2}}} \right)\left( {T_p^2 + T_{c2}^2} \right)}}{{1/{\varepsilon_p} + 1/{\varepsilon_{c2}} - 1}}$$</div>
-
-<div>$${h_{rc1 - c2}} = \frac{{\sigma \left( {{T_{c1}} + {T_{c2}}} \right)\left( {T_{c1}^2 + T_{c2}^2} \right)}}{{1/{\varepsilon_{c1}} + 1/{\varepsilon_{c2}} - 1}}$$</div>
-
-The long wave radiation exchange coefficients between the outer collector cover and the sky and ground referencing the ambient air temperature for mathematical simplification are given.
-
-<div>$${h_{rc1 - s}} = \frac{{{F_s}{\varepsilon_{c1}}\sigma \left( {{T_{c1}} + {T_s}} \right)\left( {T_{c1}^2 + T_s^2} \right)\left( {{T_{c1}} - {T_s}} \right)}}{{\left( {{T_{c1}} - {T_a}} \right)}}$$</div>
-
-<div>$${h_{rc1 - g}} = \frac{{{F_g}{\varepsilon_{c1}}\sigma \left( {{T_{c1}} + {T_g}} \right)\left( {T_{c1}^2 + T_g^2} \right)\left( {{T_{c1}} - {T_g}} \right)}}{{\left( {{T_{c1}} - {T_a}} \right)}}$$</div>
-
-<div>$${h_{cc1 - a}} = {h_{cc1 - s}} + {h_{cc1 - g}}$$</div>
-
-The convection heat transfer coefficient from the outer cover to the surrounding air is given by:
-
-<div>$${h_{cc1 - a}} = 2.8 + 3.0{V_w}$$</div>
-
-When the bottom surface boundary condition is AmbientAir, the combined conductance from the outer cover to the surrounding is calculated from the equation below (Duffie and Beckman, 1991).
-
-<div>$${h_{comb}} = 5.7 + 3.8{V_w}$$</div>
-
-The overall loss coefficient through the bottom and side of the collector-storage is estimated as follows:
-
-<div>$${U_b} = {U_{Lb}}\left( {{A_b}/A} \right)$$</div>
-
-<div>$${U_s} = {\left[ {\frac{1}{{{U_{Ls}}\left( {{A_s}/A} \right)}} + \frac{1}{{{h_{comb}}}}} \right]^{ - 1}}$$</div>
-
-Where,
-
-*e<sub>c1</sub>*   = thermal emissivity of collector cover *1*, (-)
-
-*e<sub>c2</sub>*   = thermal emissivity of collector cover *2*, (-)
-
-*F<sub>s</sub>*   = view factor from the collector to the sky, (-)
-
-*F<sub>g</sub>*   = view factor from the collector to the ground, (-)
-
-*T<sub>c1</sub>* = temperature of collector cover *1*, (K)
-
-*T<sub>c2</sub>* = temperature of collector cover *2*, (K)
-
-*T<sub>s</sub>*   = sky temperature, (K)
-
-*T<sub>g</sub>*   = ground temperature, (K)
-
-*k*    = thermal conductivity of air, (W/m K)
-
-*L*    = air gap between the covers, (m)
-
-*β*    = inclination of the plates or covers to the horizontal, (radian)
-
-*V<sub>w</sub>* = wind speed, (m/s)
-
-*U<sub>Lb</sub>*  = user specified bottom heat loss conductance, W/m<sup>2</sup>×K
-
-*U<sub>Ls</sub>*  = user specified side heat loss conductance, W/m<sup>2</sup>×K
-
-*A<sub>b</sub>*   = collector bottom heat transfer area, m<sup>2</sup>
-
-*A<sub>s</sub>*   = collector side area, m<sup>2</sup>
-
-*h<sub>comb</sub>*            = combined conductance from the outer cover to the ambient air, W/m<sup>2</sup>×K
-
-***Transmittance-Absorptance Product***
-
-The transmittance-absorptance product of solar collector is determined using ray tracing method for any incident angle (Duffie and Beckman, 1991).  This requires optical properties of the cover and absorber materials and the the transmittance-absorptance product for any incident angle is given by:
-
-<div>$${\left( {\tau \alpha } \right)_\theta } = \frac{{\tau \alpha }}{{1 - \left( {1 - \alpha } \right){\rho_d}}}$$</div>
-
-The transmittance of the cover system for single and two cover are given by:
-
-<div>$$\tau  = \frac{1}{2}\left[ {{{\left( {\frac{{{\tau_1} \cdot {\tau_2}}}{{1 - {\rho_1}{\rho_2}}}} \right)}_ \bot } + {{\left( {\frac{{{\tau_1} \cdot {\tau_2}}}{{1 - {\rho_1}{\rho_2}}}} \right)}_\parallel }} \right]$$</div>
-
-<div>$$\rho  = \frac{1}{2}\left[ {{{\left( {{\rho_1} + \frac{{\tau  \cdot {\rho_2} \cdot {\tau_1}}}{{{\tau_2}}}} \right)}_ \bot } + {{\left( {{\rho_1} + \frac{{\tau  \cdot {\rho_2} \cdot {\tau_1}}}{{{\tau_2}}}} \right)}_\parallel }} \right]$$</div>
-
-The effective transmittance, reflectance and absorptance of a single cover are given by:
-
-<div>$$\tau  = \frac{{{\tau_a}}}{2}\left\{ {\frac{{1 - {r_ \bot }}}{{1 + {r_ \bot }}}\left[ {\frac{{1 - r_ \bot ^2}}{{1 - {{\left( {{r_ \bot }{\tau_a}} \right)}^2}}}} \right] + \frac{{1 - {r_\parallel }}}{{1 + {r_\parallel }}}\left[ {\frac{{1 - r_\parallel ^2}}{{1 - {{\left( {{r_\parallel }{\tau_a}} \right)}^2}}}} \right]} \right\}$$</div>
-
-<div>$$\rho  = \frac{1}{2}\left\{ {\left[ {{r_ \bot } + \frac{{{{\left( {1 - {r_ \bot }} \right)}^2}\tau_a^2{r_ \bot }}}{{1 - {{\left( {{r_ \bot }{\tau_a}} \right)}^2}}}} \right] + \left[ {{r_\parallel } + \frac{{{{\left( {1 - {r_\parallel }} \right)}^2}\tau_a^2{r_\parallel }}}{{1 - {{\left( {{r_\parallel }{\tau_a}} \right)}^2}}}} \right]} \right\}$$</div>
-
-<div>$$\alpha  = \frac{{\left( {1 - {\tau_a}} \right)}}{2}\left\{ {\left( {\frac{{1 - {r_ \bot }}}{{1 - {r_ \bot }{\tau_a}}}} \right) + \left( {\frac{{1 - {r_\parallel }}}{{1 - {r_\parallel }{\tau_a}}}} \right)} \right\}$$</div>
-
-The transmittance of the cover system with absorption only considered *t*<sub>a</sub>, is defined as:
-
-<div>$${\tau_a} = \exp \left( { - \frac{{KL}}{{\cos \,{\theta_2}}}} \right)$$</div>
-
-<div>$${\theta_2} = {\sin ^{ - 1}}\left( {\sin {\theta_1} \cdot \frac{{{n_1}}}{{{n_2}}}} \right)$$</div>
-
-The reflectance of un-polarized radiation on passing from medium 1 with reflective index *n*<sub>1</sub> to medium 2 with reflective index *n*<sub>2</sub> is given by:
-
- <span>\({r_ \bot } = \frac{{{{\sin }^2}\left( {{\theta_2} - {\theta_1}} \right)}}{{{{\sin }^2}\left( {{\theta_2} + {\theta_1}} \right)}}\)</span>
-
-<div>$${r_\parallel } = \frac{{{{\tan }^2}\left( {{\theta_2} - {\theta_1}} \right)}}{{{{\tan }^2}\left( {{\theta_2} + {\theta_1}} \right)}}$$</div>
-
-The sky and ground reflected diffuse radiations average equivalent incident angles are approximated by Brandemuehl and Beckman correlation (Duffie and Beckman, 1991) as follows:
-
-<div>$${\theta_{sd}} = 59.68 - 0.1388\beta  + 0.001497{\beta ^2}$$</div>
-
-<div>$${\theta_{gd}} = 90 - 0.5788\beta  + 0.002693{\beta ^2}$$</div>
-
-where,
-
-*t*     = transmittance of the cover system, (-)
-
-*t*<sub>1</sub>    = transmittance of the cover 1, (-)
-
-*t*<sub>2</sub>    = transmittance of the cover 2, (-)
-
-*a*    = absorptance of the absorber plate, (-)
-
-*r*<sub>d</sub>    = diffuse reflectance of the inner cover, (-)
-
-*L*    = thickness of a cover material, (m)
-
-*K*    = extinction coefficient of a cover material, (m<sup>-1</sup>)
-
-*q*<sub>1</sub>   = angle of incidence, degree
-
-*q*<sub>2</sub>    = angle of refraction, degree
-
-<span>\({r_ \bot }\)</span>  = parallel component of reflected un-polarized radiation, (-)
-
-<span>\({r_\parallel }\)</span>   = perpendicular component of reflected un-polarized radiation, (-)
-
-*b*    = slope of the collector, degree
-
-*q*<sub>sd</sub> = equivalent incident angle for sky diffuse solar radiation, degree
-
-*q*<sub>gd</sub>  = equivalent incident angle for ground diffuse solar radiation, degree
-
-The integral collector storage unit thermal performance parameters are calculated as follows:
-
-<div>$${Q_{delivered}} = {\dot m_w}{C_w}\left( {{T_w} - {T_{wi}}} \right)$$</div>
-
-<div>$${Q_{Stored}} = {m_w}{C_w}\frac{{d{T_w}}}{{dt}}$$</div>
-
-<div>$${Q_{SkinLoss}} = A \cdot \left[ {{U_t}\left( {{T_p} - {T_w}} \right) + {U_b}\left( {{T_w} - {T_{OSC}}} \right) + {U_s}\left( {{T_w} - {T_a}} \right)} \right]$$</div>
-
-<div>$${\eta_{thermal}} = \frac{{{m_w}{C_w}\frac{{d{T_w}}}{{dt}} + {{\dot m}_w}{C_w}\left( {{T_w} - {T_{wi}}} \right)}}{{A \cdot {I_t}}}$$</div>
-
-### References:
-
-Duffie, J.A., and W.A. Beckman. 1991. *Solar Engineering of Thermal Processes,* 2d ed. New York: John Wiley & Sons.
-
-Kumar, R. and M.A. Rosen. Thermal performance of integrated collector storage solar water heater with corrugated absorber surface. Applied Thermal Engineering:  30 (2010) 1764–1768.
-
-Fujii, T., and H. Imura. Natural convection heat transfer from aplate with arbitrary inclination. International Journal of Heat and Mass Transfer: 15(4), (1972), 755-764.
-
-### Photovoltaic Thermal Flat-Plate Solar Collectors
-
-Photovoltaic-Thermal solar collectors (PVT) combine solar electric cells and thermal working fluid to collect both electricity and heat.  Athough there are currently comparatively few commercial products, PVT research has been conducted for the past 30 years and many different types of collectors have been studied.  Zondag (2008) and Charalambous et. al (2007) provide reviews of the PVT literature.  Because PVT is much less commercially-mature, there are no standards or rating systems such as for thermal-only, hot-water collectors.  EnergyPlus currently has one simple model based on user-defined efficiencies but a more detailed model based on first-principles and a detailed, layer-by-layer description is under development.
-
-The PVT models reuse the PV models for electrical production. These are described elsewhere in this document in the section on Photovoltaic Arrays-Simple Model
-
-#### Simple PVT Thermal Model
-
-The input object SolarCollector:FlatPlate:PhotovoltaicThermal provides a simple PVT model that is provided for quick use during design or policy studies.  The user simply provides values for a thermal efficiency and the incident solar heats the working fuild.  The model also includes a cooling mode for air-based systems where a user-provided surface emmittance is used to model cooling of the working fluid to the night sky (water-based cooling will be made available once a chilled water storage tank is available).  No other details of the PVT collector’s construction are required as input data.
-
-The simple model can heat either air or liquid.  If it heats air, then the PVT is part of HVAC air system loop with air nodes connected to an air system.  If it heats liquid, then the PVT is part of plant loop with nodes connected to a plant loop and the plant operating scheme determines flows.
-
-Air-system-based PVT modeling include a modulating bypass damper arrangement.  Control logic decides if the air should bypass the collector to better meet setpoint.  The model requires a drybulb temperature setpoint be placed on the outlet node.  The model assume the collector is intended and available for heating when the incident solar is greater than 0.3 W/m<sup>2</sup> and otherwise it is intended for cooling.  The inlet temperature is compare to the setpoint on the outlet node to determine if cooling or heating are beneficial.  If they are, then the PVT thermal models are applied to condition the air stream.  If they are not beneficial, then the PVT is completely bypassed and the inlet node is passed directly to the outlet node to model a completely bypassed damper arrangement.  A report variable is available for bypass damper status.
-
-Plant-based PVT do not include a bypass (although one could be used in the plant loop).  The collector requests its design flow rate but it otherwise relies on the larger plant loop for control.
-
-When the PVT themal collector is controlled to be “on,� in heating mode, and working fluid is flowing, the model calculates the outlet temperature based on the inlet temperature and the collected heat using the following equations.
-
-<div>$${Q_{therm}} = {A_{surf}} \cdot {f_{activ}} \cdot {G_T} \cdot {\eta_{thermal}}$$</div>
-
-where,
-
-<span>\({Q_{therm}}\)</span> is the thermal energy collected [W]
-
-<span>\({A_{surf}}\)</span> is the net area of the surface [m<sup>2</sup>]
-
-<span>\({f_{activ}}\)</span>is the fraction of surface aire with active PV/T collector, and
-
-<span>\({\eta_{thermal}}\)</span>is the thermal conversion efficiency.
-
-<div>$${T_{out}} = {T_{in}} + \frac{{{Q_{therm}}}}{{\dot m{c_p}}}$$</div>
-
-where,
-
-<span>\({T_{out}}\)</span> is the temperature of the working fluid leaving the PV/T
-
-<span>\({T_{in}}\)</span> is the temperature of the working fluid entering the PV/T
-
-<span>\(\dot m\)</span> is the entire mass flow of the working fluid through the PV/T
-
-<span>\({c_p}\)</span> is the specific heat of the working fluid.
-
-For air-based systems, the value of <span>\({T_{out}}\)</span>is then compared to the temperature setpoint on the outlet node.  If <span>\({T_{out}}\)</span> exceeds the desired outlet temperature, <span>\({T_{set,out}}\)</span>,then a bypass fraction is calculated to model a modulating bypass damper using:
-
-<div>$${f_{bypass}} = \frac{{\left( {{T_{set,out}} - {T_{out}}} \right)}}{{\left( {{T_{in}} - {T_{out}}} \right)}}$$</div>
-
-When the PVT themal collector is controlled to be “on,� in cooling mode, and working fluid is flowing, the model calculates the outlet temperature based on the inlet temperature and the heat radiated and convected to the ambient using a heat balance on the outside face of the collector:
-
-<div>$$\dot m{c_p}\left( {{T_{in}} - {T_{out}}} \right) = {\dot Q_{LWR}} + {\dot Q_{conv}}$$</div>
-
-Where,
-
-<span>\({\dot Q_{LWR}}\)</span> is the net rate of long wavelength (thermal) radiation exchange with the air, night sky, and ground.  See the section “External Longwave Radiation� in the Outside Surface Heat Balance, for full discussion of how this modeled in EnergyPlus using linearized radiation coefficients.
-
-<span>\({\dot Q_{conv}}\)</span> is the net rate of convective flux exchange with outdoor air. See the section “Exterior/External Convection� in the Outside Surface Heat Balance, for full discussion of how this modeled in EnergyPlus.  The surface roughness is assumed to be “very smooth.�
-
-The simple model assumes that the effective collector temperature, <span>\({T_{col}}\)</span>, is the average of the working fluid inlet and outlet temperatures so that we can make the following substitution:
-
-<div>$${T_{out}} = 2{T_{col}} - {T_{in}}$$</div>
-
-Substituting and solving for <span>\({T_{col}}\)</span> we obtain the following model for collector temperatures during a (possible) cooling process :
-
-<div>$${T_{col}} = \frac{{2\dot m{c_p}{T_{in}} + {A_{surf}}{f_{activ}}\left( {{h_{r,gnd}}{T_{gnd}} + {h_{r,sky}}{T_{sky}} + {h_{r,air}}{T_{air}} + {h_{c,ext}}{T_{air}}} \right)}}{{2\dot m{c_p} + {A_{surf}}{f_{activ}}\left( {{h_{r,gnd}} + {h_{r,sky}} + {h_{r,air}} + {h_{c,ext}}} \right)}}$$</div>
-
-Then the outlet temperature can be calculated and heat losses determined.  However, the model allows only sensible cooling of the air stream and limits the outlet temperature to not go below the dewpoint temperature of the inlet.
-
-PVT collectors have a design volume flow rate for the working fluid that is autosizable.  For air-based systems used as pre-conditioners, the volume flow rate is sized to meet the maximum outdoor air flow rate.  For water-based systems on the supply side of a plant loop, each of the PVT collectors are sized to the overall loop flow rate.  For water-based systems on the demand side of a plant loop, the collectors are sized using a rule-of-thumb for typical flow rates per unit of collector area.  This rule-of-thumb is based on a constant factor of 1.905x10<sup>-5</sup> m<sup>3</sup>/s-m<sup>2</sup> that was developed by analyzing SRCC data set for conventional solar collectors (see data set SolarCollectors.idf) and averaging the ratio for all 171 different collectors.
-
-#### References
-
-Charalambous, P.G., Maidment, G.G., Kalagirou, S.A., and Yiakoumetti, K., Photovoltaic thermal (PV/T) collectors: A review. Applied Thermal Engineering 27 (2007) 275-286.
-
-Zondag, H.A. 2008. Flat-plate PV-Thermal collectors and systems: A review.  Renewable and Sustainable Energy Reviews 12 (2008) 891-959.
-
-### Unglazed Transpired Solar Collectors
-
-The input object SolarCollector:UnglazedTranspired provides a model for transpired collectors that are perhaps one of the most efficient ways to collect solar energy with demonstrated instantaneous efficiencies of over 90% and average efficiencies of over 70%.  They are used for preheating outdoor air needed for ventilation and processes such as crop drying.
-
-In EnergyPlus, an unglazed transpired solar collector (UTSC) is modeled as a special component attached to the outside face of a heat transfer surface that is also connected to the outdoor air path.  A UTSC affects both the thermal envelope and the HVAC air system.  From the air system’s point of view, a UTSC is heat exchanger and the modeling needs to determine how much the device raises the temperature of the outdoor air.  From the thermal envelope’s point of view, the presence of the collector on the outside of the surface modifies the conditions experienced by the underlying heat transfer surfaces.  EnergyPlus models building performance throughout the year and the UTSC will often be “off� in terms of forced airflow, but the collector is still present.  When the UTSC is “on� there is suction airflow that is assumed to be uniform across the face.  When the UTSC is “off� the collector acts as a radiation and convection baffle situated between the exterior environment and the outside face of the underlying heat transfer surface.  We distinguish these two modes of operation as *active* or *passive* and model the UTSC component differently depending on which of these modes it is in.
-
-#### Heat Exchanger Effectiveness
-
-The perforated absorber plate is treated as a heat exchanger and modeled using a traditional effectiveness formulation.  The heat exchanger effectiveness, <span>\({\varepsilon_{HX}}\)</span>, is determined from correlations derived from small-scale experiments.  Two correlations available in the literature are implemented in EnergyPlus.  The first is based on research by Kutscher at the National Renewable Energy Laboratory. The second is based on the research by Van Decker, Hollands, and Brunger at the University of Waterloo.  Because both correlations are considered valid, the choice of which correlation to use is left to the user.
-
-
-
-#### Kutscher Correlation
-
-Kutscher’s (1994) correlation encompasses surface convection between the collector and the incoming outdoor air stream that occurs on the front face, in the holes, and along the back face of the collector. The correlation uses a Reynolds number based on the hole diameter as a length scale and the mean velocity of air as it passes through the holes as the velocity scale:
-
-<div>$${{\mathop{\rm Re}\nolimits}_D} = \frac{{{V_h}D}}{\nu }$$</div>
-
-where,
-
-      <span>\({V_h}\)</span> is the velocity through the holes [m/s]
-
-      <span>\(D\)</span> is the hole diameter [m]
-
-      <span>\(\nu \)</span> is the kinematic viscosity of air  [m<sup>2</sup>/s]
-
-The correlation is a function of Reynolds number, hole geometry, the free stream air velocity, and velocity through the holes:
-
-<div>$$N{u_D} = 2.75\left[ {{{\left( {\frac{P}{D}} \right)}^{ - 1.2}}{\mathop{\rm Re}\nolimits}_D^{0.43} + 0.011\sigma {{{\mathop{\rm Re}\nolimits} }_D}{{\left( {\frac{{{U_\infty }}}{{{V_h}}}} \right)}^{0.48}}} \right]$$</div>
-
-where,
-
-      <span>\(P\)</span> is the pitch, or distance between holes, [m],
-
-      <span>\(D\)</span> is the diameter of the holes, [m],
-
-      <span>\(\sigma \)</span> is the porosity, or area fraction of the holes, [dimensionless],
-
-      <span>\({V_h}\)</span> is the mean velocity of air passing through the holes, [m/s],
-
-      <span>\({U_\infty }\)</span> is the free stream velocity (local wind speed) [m/s].
-
-The Nusselt number is formulated as:
-
-<div>$$N{u_D} = \frac{{U\;D}}{k}$$</div>
-
-where,
-
-      <span>\(U\)</span>is the overall heat transfer coefficient based on log mean temperature difference, [W/m<sup>2</sup>·K], and
-
-      <span>\(k\)</span> is the thermal conductivity of air [W/m·K].
-
-The heat exchanger effectiveness is:
-
-<div>$${\varepsilon_{HX}} = 1 - {e^{\left[ { - \frac{{U\,A}}{{\dot m\,{c_p}}}} \right]}}$$</div>
-
-Kutscher’s relation was formulated for triangular hole layout, but based on Van Decker et al. (2001) we allow using the correlation for square hole layout and scale <span>\(P\)</span> by a factor of 1.6.
-
-#### Van Decker, Hollands, and Brunger Correlation
-
-Van Decker et. al. extended Kutscher’s measurements to include a wider range of collector parameters including plate thickness, pitch, suction velocities, and square hole patterns.  Their model formulation differs from Kutscher’s in that the model was built up from separate effectiveness models for the front, back, and holes of the collector.  Their published correlation is:
-
-<div>$${\varepsilon_{HX}} = \left[ {1 - \left( {1 + {{{\mathop{\rm Re}\nolimits} }_s}Max{{\left( {1.733{\mathop{\rm Re}\nolimits}_w^{ - {\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 2}}\right.}\!\lower0.7ex\hbox{$2$}}},0.02136} \right)}^{ - 1}}} \right)} \right] \times \left[ {1 - {{\left( {1 + 0.2273{\mathop{\rm Re}\nolimits}_b^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 2}}\right.}\!\lower0.7ex\hbox{$2$}}}} \right)}^{ - 1}}} \right] \times {e^{\left( { - 0.01895\frac{P}{D} - \frac{{20.62}}{{{{{\mathop{\rm Re}\nolimits} }_D}}}\frac{t}{D}} \right)}}$$</div>
-
-where,
-
-      <span>\({{\mathop{\rm Re}\nolimits}_s} = \frac{{{V_s}P}}{v}\)</span>
-
-      <span>\({{\mathop{\rm Re}\nolimits}_w} = \frac{{{U_\infty }P}}{v}\)</span>
-
-      <span>\({{\mathop{\rm Re}\nolimits}_b} = \frac{{{V_h}P}}{v}\)</span>
-
-      <span>\({V_s}\)</span> is the average suction velocity across the front face of the collector [m/s]
-
-      <span>\(t\)</span> is the collector plate thickness
-
-
-
-#### Heat Exchanger Leaving Temperature
-
-Using either of the correlations above allows determining the heat exchanger effectiveness from known values.  By definition the heat exchanger effectiveness is also:
-
-<div>$${\varepsilon_{HX}} = \frac{{{T_{a,HX}} - {T_{amb}}}}{{{T_{s,coll}} - {T_{amb}}}}$$</div>
-
-where,
-
-      <span>\({T_{{\rm{a,HX}}}}\)</span> is the temperature of the air leaving the collector and entering the plenum [ºC]
-
-      <span>\({T_{s,coll}}\)</span> is the temperature of the collector’s absorber plate, [ºC], and
-
-      <span>\({T_{amb}}\)</span> is the temperature of the ambient outdoor air [ºC].
-
-By rewriting equation to solve for <span>\({T_{{\rm{a,HX}}}}\)</span> we see that the temperature of the heated outdoor air entering the plenum can be determined once the collector surface temperature is known,
-
-<div>$${T_{a,HX}} = {\varepsilon_{HX}}{T_{s,coll}} + \left( {1 - {\varepsilon_{HX}}} \right){T_{amb}}$$</div>
-
-#### Collector Heat Balance
-
-The collector is assumed to be sufficiently thin and high-conductivity so that it can be modeled using a single temperature (for both sides and along its area).  This temperature <span>\({T_{s,coll}}\)</span>is determined by formulating a heat balance on a control volume that just encapsulates the collector surface.  The heat balances are formulated separately for active and passive modes and are diagrammed in the following figure.
-
-Observe that for the passive case, we do not use the heat exchanger relations to directly model the interaction of ventilating air with the collector.  This is because these relations are considered to not apply when the UTSC is in passive mode.  They were developed for uni-directional flow (rather than the balanced-in-and-out flow expected from natural forces) and for specific ranges of suction face velocity.  Therefore, this heat transfer mechanism is handled using classical surface convection models (as if the collector was not perforated).  (Air exchanges are modeled as ventilation in the plenum air heat balance but do not interact with the hole edges in the collector surface.)
-
-![](media/image6620.png)
-
-Figure 299.  Transpired Collector Heat Balance
-
-When the UTSC is active, the heat balance on the collector surface control volume is:
-
-<div>$${q''_{\alpha sol}} + {q''_{LWR,Env}} + {q''_{conv,wind}} - {q''_{HX}} + {q''_{LWR,plen}} + {q''_{source}} = 0$$</div>
-
-where:
-
-<sub><span>\({q''_{\alpha sol}}\)</span> </sub>is absorbed direct and diffuse solar (short wavelength) radiation heat flux.
-
-<span>\({q''_{LWR,Env}}\)</span> is net long wavelength (thermal) radiation flux exchange with the air and surroundings.
-
-<span>\({q''_{conv,wind}}\)</span> is surface convection flux exchange with outdoor air under high wind and rain conditions.  Note that this term is usually assumed to be zero in UTSC model development but we add the term to allow for deteriorated performance of the UTSC under poor conditions.
-
-<sub><span>\({q''_{HX}}\)</span> </sub> is heat exchanger flux from collector to incoming outdoor air.
-
-<sub><span>\({q''_{LWR,plen}}\)</span> </sub>is net long wavelength (thermal) radiation flux exchange with the outside face of the underlying surface(s).
-
-<span>\({q''_{source}}\)</span> is a source/sink term that accounts for energy exported out of the control volume when the collecter’s absorber plate is a hybrid device such as a photovoltaic panel.
-
-While the heat balance on the passive collector surface control volume is:
-
-<div>$${q''_{\alpha sol}} + {q''_{LWR,Env}} + {q''_{conv,Env}} + {q''_{LWR,plen}} + {q''_{conv,plen}} + {q''_{source}} = 0$$</div>
-
-where:
-
-<sub><span>\({q''_{conv,Env}}\)</span> </sub>= surface convection flux exchange with outdoor air.
-
-<sub><span>\({q''_{conv,plen}}\)</span> </sub>= surface convection flux exchange with plenum air.
-
-All terms are positive for net flux to the collector except the heat exchanger term, which is taken to be positive in the direction from collector to incoming air stream.  Each of these heat balance components is introduced briefly below.
-
-#### External SW Radiation
-
-<sub><span>\({q''_{\alpha sol}}\)</span> </sub> is calculated using procedures presented elsewhere in this manual and includes both direct and diffuse incident solar radiation absorbed by the surface face.  This is influenced by location, surface facing angle and tilt, shading surfaces, surface face material properties, weather conditions, etc.
-
-#### External LW Radiation
-
-<span>\({q''_{LWR,Env}}\)</span> is a standard radiation exchange formulation between the surface, the sky, the ground, and the atmosphere.  The radiation heat flux is calculated from the surface absorptivity, surface temperature, sky, air, and ground temperatures, and sky and ground view factors.  Radiation is modeled using linearized coefficients.
-
-#### External Convection
-
-<sub><span>\({q''_{conv,Env}}\)</span> </sub>is modeled using the classical formulation: <span>\({q''_{conv}}\)</span> <sub> </sub>= h<sub>co</sub>(T<sub>air</sub> - T<sub>o</sub>) where h<sub>co</sub>, is the convection coefficient.  This coefficient will differ depending on whether or not the UTSC is active or passive.  When the UTSC is passive, h<sub>co</sub> is treated in the same way as an outside face with ExteriorEnvironment conditions.  When the UTSC is active, the special suction airflow situation of a transpired collector during operation means that h<sub>co</sub> is often zero because the suction situation can eliminate mass transport away from the collector.  However when the winds are high, the strong turbulence and highly varying pressures can cause the suction flow situation to breakdown.  Therefore, we include the <span>\({q''_{conv,wind}}\)</span> term in the heat balance and use a special coefficient <span>\({h_{c,wind}}\)</span> to model this lost heat transfer.  In addition, when it is raining outside, we assume the collector gets wet and model the enhanced surface heat transfer using a large value for <span>\({h_{c,wind}}\)</span>.
-
-#### Heat Exchanger
-
-<sub><span>\({q''_{HX}}\)</span> </sub>is modeled using the classical formulation <span>\({q''_{HX}} = \frac{{\dot m{c_p}({T_{a,HX}} - {T_{amb}})}}{A}\)</span><sub> </sub>where <span>\({T_{{\rm{a,HX}}}}\)</span> is determined using correlations described above.  When the UTSC is active, the air mass flow is determined from the operation of the outdoor air mixer component.  When the UTSC is off, this term is zero.
-
-#### Plenum LW Radation
-
-<span>\({q''_{LWR,plen}}\)</span>is a standard radiation exchange formulation between the collector surface and the underlying heat transfer surface located across the plenum.  Radiation is modeled using linearized coefficients.
-
-#### Plenum Convection
-
-<sub><span>\({q''_{conv,plen}}\)</span> </sub>is modeled using the classical formulation: <span>\({q''_{conv}}\)</span> <sub> </sub>= h<sub>cp</sub>(T<sub>air</sub> - T<sub>o</sub>) where h<sub>cp</sub>, is the convection coefficient.  This coefficient is taken as zero when the UTSC is operating because of the suction airflow situation.  When the UTSC is off, the value for h<sub>cp</sub> is obtained from correlations used for window gaps from ISO (2003) standard 15099.
-
-Substituting models into and solving for <span>\({T_{s,coll}}\)</span> yields the following equation when the UTSC is active (“on�):
-
-
-
-<div>$${T_{s,coll}} = \frac{{\left( {{I_s}\alpha  + {h_{r,atm}}{T_{amb}} + {h_{r,sky}}{T_{sky}} + {h_{r,gnd}}{T_{amb}} + {h_{r,plen}}{T_{so}} + {h_{c,wind}}{T_{amb}} + \frac{{\dot m{c_p}}}{A}{T_{amb}} - \frac{{\dot m{c_p}}}{A}\left( {1 - {\varepsilon_{HX}}} \right){T_{amb}} + {{q''}_{source}}} \right)}}{{\left( {{h_{r,atm}} + {h_{r,sky}} + {h_{r,gnd}} + {h_{r,plen}} + {h_{c,wind}} + \frac{{\dot m{c_p}}}{A}{\varepsilon_{HX}}} \right)}}$$</div>
-
-and substituting into yields the following equation when the UTSC is passive (“off�):
-
-<div>$${T_{s,coll}} = \frac{{\left( {{I_s}\alpha  + {h_{co}}{T_{amb}} + {h_{r,atm}}{T_{amb}} + {h_{r,sky}}{T_{sky}} + {h_{r,gnd}}{T_{amb}} + {h_{r,plen}}{T_{so}} + {h_{c,plen}}{T_{a,plen}} + {{q''}_{source}}} \right)}}{{\left( {{h_{co}} + {h_{r,air}} + {h_{r,sky}} + {h_{r,gnd}} + {h_{r,plen}} + {h_{c,plen}}} \right)}}$$</div>
-
-where,
-
-      <span>\({I_s}\)</span> is the incident solar radiation of all types [W/m<sup>2</sup>],
-
-      <span>\(\alpha \)</span> is the solar absorptivity of the collector [dimensionless],
-
-      <span>\({h_{r,atm}}\)</span>is the linearized radiation coefficient for the surrounding atmosphere [W/m<sup>2</sup>·K],
-
-      <span>\({T_{amb}}\)</span> is the outdoor drybulb from the weather data, also assumed for ground surface [ºC],
-
-      <span>\({h_{r,sky}}\)</span> is the linearized radiation coefficient for the sky [W/m<sup>2</sup>·K],
-
-      <span>\({T_{sky}}\)</span> is the effective sky temperature [ºC],
-
-      <span>\({h_{r,gnd}}\)</span> is the linearized radiation coefficient for the ground [W/m<sup>2</sup>·K],
-
-      <span>\({h_{r,plen}}\)</span> is the linearized radiation coefficient for the underlying surface [W/m<sup>2</sup>·K],
-
-      <span>\({h_{c,wind}}\)</span> is the convection coefficient for the outdoor environment when the UTSC is active and winds are high or it is raining [W/m<sup>2</sup>·K],
-
-      <span>\({T_{so}}\)</span> is the temperature of the outside face of the underlying heat transfer surface [ºC],
-
-      <span>\(\dot m\)</span> is the air mass flow rate when in active mode [kg/s],
-
-      <span>\({c_p}\)</span> is the specific heat of air at constant pressure [J/kg·K],
-
-      <span>\(A\)</span> is the area of the collector [m<sup>2</sup>],
-
-      <span>\({h_{co}}\)</span> is the convection coefficient for the outdoor environment [W/m<sup>2</sup>·K],
-
-      <span>\({h_{c,plen}}\)</span> is the convection coefficient for the surfaces facing the plenum [W/m<sup>2</sup>·K], and
-
-      <span>\({T_{a,plen}}\)</span> is the air drybulb for air in the plenum and entering the outdoor air system [ºC].
-
-
-
-#### Plenum Heat Balance
-
-The *plenum* is the volume of air located between the collector and the underlying heat transfer surface.  The plenum air is modeled as well-mixed.  The uniform temperature of the plenum air, <span>\({T_{a,plen}}\)</span>, is determined by formulating a heat balance on a control volume of air as diagrammed below.
-
-Note that we have formulated the control volumes with slight differences for the active and passive cases.  For the active case, the suction air situation and heat exchanger effectiveness formulations dictate that the collector surface control volume encompass part of the air adjacent to both the front and back surfaces of the collector.  However for the passive case, the collector surface control volume has no air in it and the plenum air control volume extends all the way to the surface of the collector. 
-
-
-
-![](media/image6664.png)
-
-Figure 300.  Transpired Collector Plenum Air Heat Balance
-
-
-
-When the UTSC is active, the heat balance on the plenum air control volume is:
-
-<div>$${\dot Q_{air}} + {\dot Q_{co}}_{} = 0$$</div>
-
-where,
-
-<span>\({\dot Q_{air}}\)</span>is the net rate of energy added by suction air convecting through the control volume.
-
-<sub><span>\({\dot Q_{co}}\)</span> </sub> is the net rate of energy added by surface convection heat transfer with the underlying surface.
-
-
-
-When the UTSC is passive, the heat balance on the plenum air control volume is:
-
-<div>$${\dot Q_{vent}} + {\dot Q_{co}} + {\dot Q_{c,coll}} = 0$$</div>
-
-where,
-
-      <span>\({\dot Q_{vent}}\)</span> is the net rate of energy added from infiltration – where outdoor ambient air exchanges with the plenum air.
-
-      <span>\({\dot Q_{c,coll}}\)</span>is the net rate of energy added by surface convection heat transfer with the collector.
-
-
-
-Substituting into and solving for <span>\({T_{a,plen}}\)</span> yields the following equation for when the UTSC is active:
-
-<div>$${T_{a,plen}} = \frac{{\left( {\dot m{c_p}{T_{a,HX}} + {h_{c,plen}}A\,{T_{so}}} \right)}}{{\left( {\dot m{c_p} + {h_{c,plen}}A} \right)}}$$</div>
-
-And substituting into yields the following equation when the UTSC is passive:
-
-<div>$${T_{a,plen}} = \frac{{\left( {{h_{c,plen}}A\,{T_{so}} + {{\dot m}_{vent}}{c_p}{T_{amb}} + {h_{c,plen}}A\,{T_{s,coll}}} \right)}}{{\left( {{h_{c,plen}}A + {{\dot m}_{vent}}{c_p} + {h_{c,plen}}A} \right)}}$$</div>
-
-where,
-
-      <span>\({\dot m_{vent}}\)</span> is the air mass flow from natural forces [kg/s]
-
-The literature on UTSC does not appear to address the passive mode of operation and no models for <span>\({\dot m_{vent}}\)</span> have been identified.  Nevertheless, natural buoyancy and wind forces are expected to drive air exchange between the plenum and ambient and some method of modeling <span>\({\dot m_{vent}}\)</span> is needed.  Reasoning that the configuration is similar to single-side natural ventilation, we elect to use correlations for natural ventilation presented in Chapter 26. of ASHRAE HOF (2001).
-
-
-
-<div>$${\dot m_{vent}} = \rho \,{{\rm{\rlap{--} \dot V}}_{{\rm{tot}}}}$$</div>
-
-where,
-
-      <span>\(\rho \)</span> is the density of air [kg/m<sup>3</sup>], and
-
-      <span>\({{\rm{\rlap{--} \dot V}}_{{\rm{tot}}}} = {{\rm{\rlap{--} \dot V}}_{{\rm{wind}}}} + \,{{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}}\)</span> is the total volumetric flow rate of air ventilating in and out of the plenum.
-
-
-
-<div>$${{\rm{\rlap{--} \dot V}}_{{\rm{wind}}}} = {C_v}{A_{in}}{U_\infty }$$</div>
-
-<span>\({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}} = {C_D}{A_{in}}\sqrt {2g\Delta {H_{NPL}}\left( {{T_{a,plen}} - {T_{amb}}} \right)/{T_{a,plen}}} \)</span>  (if <span>\({T_{a,plen}} > {T_{amb}}\)</span>)
-
-<span>\({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}} = {C_D}{A_{in}}\sqrt {2g\Delta {H_{NPL}}\left( {{T_{amb}} - {T_{a,plen}}} \right)/{T_{amb}}} \)</span>  (if <span>\({T_{amb}} > {T_{a,plen}}\)</span> and UTSC vertical)
-
-<span>\({C_v}\)</span> is the effectiveness of the openings that depends on opening geometry and the orientation with respect to the wind.  ASHRAE HoF (2001) indicates values ranging from 0.25 to 0.6.  In the UTSC model, this value is available for user input and defaulted to 0.25.
-
-<span>\({C_D}\)</span> is the discharge coefficient for the opening and depends on opening geometry.  In the UTSC model, this value is available for user input and defaulted to 0.65.
-
-Mass continuity arguments lead to modeling the area of the openings as one half of the total area of the holes, so we have:
-
-<div>$${A_{in}} = \frac{{A\,\sigma }}{2}$$</div>
-
-<span>\(g\)</span> is the gravitational constant taken as 9.81 [m/s<sup>2</sup>].
-
-<span>\(\Delta {H_{NPL}}\)</span> is the height from midpoint of lower opening to the Neutral Pressure Level.  This is taken as one-fourth the overall height of the UTSC if it is mounted vertically.  For tilted collectors, the nominal height is modified by the sine of the tilt.  If the UTSC is mounted horizontally (e.g. on the roof) then the <span>\(\Delta {H_{NPL}}\)</span> is taken as the gap thickness of the plenum.
-
-If the UTSC is horizontal and <span>\({T_{amb}} > {T_{a,plen}}\)</span> then <span>\({{\rm{\rlap{--} \dot V}}_{{\rm{thermal}}}}{\rm{  =  0}}\)</span> because this is a stable situation.
-
-#### Underlying Heat Transfer Surface
-
-The UTSC is applied to the outside of a heat transfer surface.  This surface is modeled using the usual EnergyPlus methods for handling heat capacity and transients – typically the CTF method.  These native EnergyPlus Heat Balance routines are used to calculate <span>\({T_{so}}\)</span>.  The UTSC model is coupled to the underlying surface using the OtherSideConditionsModel mechanism.  The UTSC model provides values for <span>\({h_{r,plen}}\)</span>,<span>\({T_{s,coll}}\)</span>, <span>\({h_{c,plen}}\)</span>, and <span>\({T_{a,plen}}\)</span> for use with the Heat Balance Model calculations for the outside face of the underlying surface (described elsewhere in this manual).
-
-
-
-#### Solar and Shading Calculations
-
-The transpired collector object uses a standard EnergyPlus surface in order to take advantage of the detailed solar and shading calculations.  Solar radiation incident on the surface includes beam and diffuse radiation, as well as radiation reflected from the ground and adjacent surfaces.  Shading of the collector by other surfaces, such as nearby buildings or trees, is also taken into account.
-
-#### Local Wind Speed Calculations
-
-The outdoor wind speed affects terms used in modeling UTSC components.  The wind speed in the weather file is assumed to be measured at a meteorological station located in an open field at a height of 10 m.  To adjust for different terrain at the building site and differences in the height of building surfaces, the local wind speed is calculated for each surface.
-
-The wind speed is modified from the measured meteorological wind speed by the equation (ASHRAE 2001):
-
-<div>$${U_\infty } = {V_{met}}{\left( {\frac{{{\delta_{met}}}}{{{z_{met}}}}} \right)^{{a_{met}}}}{\left( {\frac{z}{\delta }} \right)^a}$$</div>
-
-where z is the height of the centroid of the UTSC, z<sub>met</sub> is the height of the standard metereological wind speed measurement, and a and d are terrain-dependent coefficients.  d is the boundary layer thickness for the given terrain type.  The values of a and d are shown in the following tables:
-
-Table 77. Terrain-Dependent Coefficients (ASHRAE 2001).
-
-<table class="table table-striped">
-
-
-
-
-
-
-
-<tr>
-<td>Terrain</td>
-<td>Description</td>
-<td>Exponent, a</td>
-<td>Layer Thickness,d (m)</td>
-</tr>
-<tr>
-<td>1</td>
-<td>Flat, open country</td>
-<td>0.14</td>
-<td>270</td>
-</tr>
-<tr>
-<td>2</td>
-<td>Rough, wooded country</td>
-<td>0.22</td>
-<td>370</td>
-</tr>
-<tr>
-<td>3</td>
-<td>Towns and cities</td>
-<td>0.33</td>
-<td>460</td>
-</tr>
-<tr>
-<td>4</td>
-<td>Ocean</td>
-<td>0.10</td>
-<td>210</td>
-</tr>
-<tr>
-<td>5</td>
-<td>Urban, industrial, forest</td>
-<td>0.22</td>
-<td>370</td>
-</tr>
-
-</table>
-
-The UTSC can be defined such that it has multiple underlying heat transfer surfaces.  The centroid heights for each surface are area-weighted to determine the average height for use in the local wind calculation.
-
-#### Convection Coefficients
-
-UTSC modeling requires calculating up to three different coefficients for surface convection heat transfer.  These coefficients are defined in the classic way by:
-
-<div>$${h_c} = \frac{{{T_{air}} - {T_{surf}}}}{{{{q''}_{conv}}}}$$</div>
-
-First, <span>\({h_{co}}\)</span> is the convection coefficient for the collector surface facing the outdoors when the UTSC is passive.  It is modeled in exactly the same way as elsewhere in EnergyPlus and will depend on the user setting for Outside Convection Algorithm – Outside Surface Heat Balance entry elsewhere in this document.
-
-
-
-Second, <span>\({h_{c,plen}}\)</span> is the convection coefficient for surfaces facing the plenum.  This coefficient is applied to just the underlying surface’s convection when the UTSC is active and to both the collector and the underlying surface when the UTSC is passive.  When the UTSC is active, we use the convection correlation for forced air developed by McAdams (1954) as published by ASHRAE HoF (2001):
-
-<div>$${h_{c,plen}} = 5.62 + 3.9{V_p}$$</div>
-
-where,
-
-      <span>\({V_p}\)</span> is the mean velocity in the plenum determined from <span>\({V_p} = \frac{{\dot m}}{{2\rho \,{A_p}}}\)</span> where <span>\({A_p}\)</span> is the effective cross section area of the plenum perpendicular to the primary flow direction.  When the UTSC is passive, we model the convection in the same way used in EnergyPlus to model air gaps in windows.  These correlations vary by Rayleigh number and surface tilt and are based on the work of various research including Hollands et. al., Elsherbiny et. al., Wright, and Arnold.  The formulations are documented in ISO (2003) standard 15099.  For the UTSC implementation, the routines were adapted from Subroutine NusseltNumber in WindowManager.f90 (by F. Winkelmann), which itself was derived from Window5 subroutine “nusselt�.
-
-Third, <span>\({h_{c,wind}}\)</span> is the convection coefficient used to degrade the UTSC performance under environmental conditions with high wind or rain.  If the weather file indicates it is raining, then we set <span>\({h_{c,wind}}\)</span> = 1000.0 which has the effect of making the collector the same temperature as ambient air.  The heat exchanger effectiveness correlations described above account for a moderate amount of wind, but the correlations appear confined to the range 0 to 5.0 m/s.  Therefore we set <span>\({h_{c,wind}}\)</span> equal to zero if <span>\({U_\infty }\)</span> is &lt;= 5.0 m/s.  If <span>\({U_\infty }\)</span> is &gt; 5.0 m/s then we use the McAdams correlation but with a reduced velocity magnitude:
-
-<span>\(\)</span><span>\({h_{c,wind}} = 5.62 + 3.9({U_\infty } - 5.0)\)</span>
-
-#### Radiation Coefficients
-
-UTSC modeling requires calculating up to four different linearized coefficients for radiation heat transfer.  Whereas radiation calculations usually use temperature raised to the fourth power, this greatly complicates solving heat balance equations for a single temperature.  Linearized radiation coefficients have the same units and are used in the same manner as surface convection coefficients and introduce very little error for the temperature levels involved.
-
-The radiation coefficient, <span>\({h_{r,plen}}\)</span>, is used to model thermal radiation between the collector surface and the outside face of the underlying heat transfer surface.  We assume a view factor of unity.  It is calculated using:
-
-<div>$${h_{r,plen}} = {\sigma_{SB}}{e_{coll}}{e_{so}}\frac{{\left( {T_{s,coll}^4 - T_{so}^4} \right)}}{{\left( {{T_{s,coll}} - {T_{so}}} \right)}}$$</div>
-
-where,
-
-      all temperatures are converted to Kelvin,
-
-      <span>\({\sigma_{SB}}\)</span> is the Stefan-Boltzmann constant,
-
-      <span>\({e_{coll}}\)</span> is the longwave thermal emmittance of the collector, and
-
-      <span>\({e_{so}}\)</span> is the longwave thermal emmittance of the underlying heat transfer surface.
-
-The three other coefficients, <span>\({h_{r,atm}}\)</span>, <span>\({h_{r,sky}}\)</span>, and <span>\({h_{r,gnd}}\)</span> are used elsewhere in EnergyPlus for the outside face surface heat balance and are calculated in the same manner as equation for UTSC collectors.  [This is accomplished by calling subroutine InitExteriorConvectionCoeffs in the file HeatBalanceConvectionCoeffs.f90. ]
-
-#### Bypass Control
-
-The UTSC is assumed to be arranged so that a bypass damper controls whether or not air is drawn directly from the outdoors or through the UTSC.  The control decision is based on whether or not it will be beneficial to heat the outdoor air.  There are multiple levels of control including an availability schedule, whether or not the outdoor air is cooler than the mixed air setpoint, or whether or not the zone air temperature is lower than a so-called free heating setpoint.
-
-#### Sizing Warnings
-
-Although the design of the transpired collector is left to the user, the program issues warnings when the suction airflow velocity falls outside the range 0.003 to 0.08 m/s.
-
-#### Overall Efficiency
-
-The overall thermal efficiency of the UTSC is a useful output report and is defined as the ratio of the useful heat gain of the entire system versus the total incident solar radiation on the gross surface area of the collector.
-
-<div>$$\eta  = \frac{{(\dot Q/A)}}{{{I_{sc}}}} = \frac{{\dot m\,{c_p}\left( {{T_{a,plen}} - {T_{amb}}} \right)}}{{{I_{sc}}A}}$$</div>
-
-where
-
-<span>\(\dot Q\)</span> is useful heat gain
-
-<span>\({I_{sc}}\)</span> is total incident solar radiation
-
-Note that the efficiency <span>\(\eta \)</span> is only defined for <span>\({I_{solar}} > 0\)</span>.  This efficiency includes heat recovered from the underlying wall and can exceed 1.0.
-
-#### Collector Efficiency
-
-The thermal efficiency of the collector is a useful output report and is defined as the ratio of the useful heat gain of the collector fluid versus the total incident solar radiation on the gross surface area of the collector.
-
-<div>$$\eta  = \frac{{\dot m\,{c_p}\left( {{T_{a,HX}} - {T_{amb}}} \right)}}{{{I_{sc}}A}}$$</div>
-
-Note that the efficiency <span>\(\eta \)</span> is only defined for <span>\({I_{solar}} > 0\)</span>
-
-#### References
-
-Kutscher, C.F. 1994. Heat exchange effectiveness and pressure drop for air flow through perforated plates with and without crosswind. *Journal of Heat Transfer*. May 1994, Vol. 116, p. 391. American Society of Mechanical Engineers.
-
-Van Decker, G.W.E., K.G.T. Hollands, and A.P. Brunger. 2001. Heat-exchange relations for unglazed transpired solar collectors with circular holes on a square of triangular pitch. *Solar Energy*. Vol. 71, No. 1. pp 33-45, 2001.
-
-ISO. 2003. ISO 15099:2003. Thermal performance of windows, doors, and shading devices – Detailed calculations. International Organization for Standardization.
-
-System Availability Managers <a name="AvailManagers"></a>
-----------------------------
-
-### Overview
-
-System availability managers, or AvailabilityManagers, are one of the high-level control constructs in EnergyPlus. An AvailabilityManager is able to access data from any of the HVAC system nodes and use this data to set flags telling a central air system or plant loop to turn on or off. Also, some of the HVACZone:\* components can use these same availability managers to turn their supply air fan on or off. Each type of availability manager encapsulates a specific high-level on-off control strategy. For instance, the input object AvailabilityManager:NightVentilation allows the user to specify a control strategy for pre-cooling the building with night-time ventilation.
-
-Availability managers are contained in the program module *SystemAvailabilityManager*. The Availability managers are executed at the start of each HVAC time step by a call to *ManageSystemAvailability*, and they reside outside the HVAC system iteration loops. Thus, the availability managers are executed once per HVAC time step, and they use previous time step information to calculate their control actions.
-
-If a given instance of an AvailabilityManager is specific to an AirLoopHVAC or to a PlantLoop, then in the input, each loop references its availability managers through a AvailabilityManagerAssignmentList. Once the data has been read in and processed, the AvailabilityManager data for each loop is stored in array *PriAirSysAvailMgr* in *DataAirLoop* (for AirLoopHVAC) and in array *PlantAvailMgr*  in *DataPlant* for plant loops.
-
-The availability status for each AirLoopHVAC (*PriAirSysAvailMgr*) is also passed to a zone equipment availability status array (*ZoneEquipAvail*) for possible use by the zones served by that air loop. This sets the availability for certain zone equipment which are assumed to operate in conjunction with the air loop. Specifically, the availability of zone exhaust fans (Ref. Fan:ZoneExhaust) and terminal unit fans (Ref. AirTerminal:SingleDuct:SeriesPIU: Reheat, AirTerminal:SingleDuct: ParallelPIU:Reheat, and AirTerminal:SingleDuct:VAV: Reheat:VariableSpeedFan), if specified in the input, will be the same as the corresponding AirLoopHVAC availability if an AvailabilityManager is specified. Other zone equipment are not affected by the AirLoopHVAC system availability managers (e.g., Window AC, PTAC and PTHP).
-
-However, system availability managers can separately be specified for zone components (currently only allowed for Window AC, PTAC, PTHP, Unit Heater, Unit Ventilator, Zone Water to Air Heat Pump, Zone Terminal Unit (VRF), Standalone Energy Recovery Ventilator, Outdoor Air Unit, Fan Coil Unit, and Ventilated Slab). Similar to AirLoopHVAC or PlantLoop, inputs of these zone components refer to their availability managers through a AvailabilityManagerAssignmentList. System availability managers only operate when zone components are available. If the Window AC (or any other unit) is scheduled off then the system availability manager will not operate until the Window AC is scheduled on. The functioning of the system availability manager for zone components is same as for AirLoopHVAC or PlantLoop. Except night ventilation SAM, all other SAMs can be specified for these zone components.
-
-The actual action of turning on or off a loop is taken by the loop prime movers: fans for AirLoopHVACs and pumps for plant loops. For instance when a fan is deciding whether it is on or off, it checks its on/off schedule and whether the loop availability status flag is *CycleOn* or *ForceOff*. If the schedule is on and the status flag is *ForceOff*, the fan will be off. If the fan schedule says off and the status flag is *CycleOn*, the fan will be on. Thus the availability managers overrule the fan on/off schedule.
-
-### Scheduled
-
-The input object AvailabilityManager:Scheduled provides the simplest availability manager. The sole input for this manager is a schedule name. If the current schedule value is &gt; 0.0, the availability status flag is set to *CycleOn*; otherwise it is set to *ForceOff*.
-
-### Scheduled On
-
-An alternative to the AvailabilityManager:Scheduled object is the *AvailabilityManager:ScheduledOn* that is used specifically to turn equipment on while other availability managers may be used to turn the equipment off. The sole input for this manager is a schedule name. If the current schedule value is &gt; 0.0, the availability status flag is set to *CycleOn*; otherwise it is set to *NoAction*.
-
-### Scheduled Off
-
-An alternative to the AvailabilityManager:Scheduled object is the *AvailabilityManager:ScheduledOff* that is used specifically to turn equipment off while other availability managers may be used to turn the equipment on. The sole input for this manager is a schedule name. If the current schedule value is = 0.0, the availability status flag is set to *ForceOff*; otherwise it is set to *NoAction*.
-
-### Night Cycle
-
-The input object AvailabilityManager:NightCycle is to specify when a system that has been scheduled off during unoccupied hours should cycle on to prevent building temperatures from becoming too hot or too cold. This manager can not be used to force a system off. The inputs are:
-
-·        A manager applicability schedule;
-
-·        The name of the fan schedule this manager will override;
-
-·        The control type: *Stay Off*, *Cycle On Any*, *Cycle On Control Zone*, or *Cycle On Any - Zone Fans Only*;
-
-·        Thermostat on/off tolerance *T<sub>tol</sub>* (degrees C);
-
-·        Cycling run time in seconds; used to calculate a stop time (in time steps since the start of the current run period) once the status has become *Cycle On*.
-
-If the fan schedule current value is &gt; 0 or the applicability schedule value is <span>\(\le \)</span> 0 or if the program is in warmup, *AvailStatus = NoAction*.
-
-Otherwise,
-
-1.    if current time (in time steps since the start of the run period) is greater than the start time and less than the stop time, *AvailStatus = CycleOn* (or *CycleOnZoneFansOnly* if the control type is *Cycle On Any – Zone Fans only*).
-
-2.    If the current time equals the stop time, *AvailStatus = NoAction*  and the fan schedule will determine if the system is on.
-
-3.     If the current time is greater than the stop time, the manager can potentially cycle the system on.
-
-a.    For control types *Cycle On Any* and *Cycle On Any – Zone Fans Only* the manger looks at each zone served by the air loop and detects whether the zone temperature at the thermostat is greater than the cooling setpoint plus ½*T<sub>tol</sub>* or less than the heating setpoint minus ½*T<sub>tol</sub>*. If it is, *AvailStatus* is set to *CycleOn* (or *CycleOnZoneFansOnly*). If not, *AvailStatus* is set to *NoAction*.
-
-b.   For control type *Cycle On Control Zone*, the manager does the same check just for the control zone.
-
-Lastly if the new status is CycleOn the start time is reset to the current time and the stop time is reset. When this availability manager is specified for a zone component then the only allowed control types are *Stay Off* *and* *Cycle On Control Zone.*
-
-### Night Ventilation
-
-The input object AvailabilityManager:NightVentilation is a manager that looks at indoor and outdoor conditions to see if night ventilation might be beneficial. In addition to being able to cycle the air system on, this manager can specify what the ventilation air flow rate should be.  The inputs are:
-
-·        A manager applicability schedule;
-
-·        The name of the fan schedule this manager will override;
-
-·        A ventilation temperature schedule;
-
-·        A ventilation delta T;
-
-·        A ventilation low limit temperature;
-
-·        The night ventilation flow fraction;
-
-·        The name of the control zone.
-
-If the fan schedule current value is &gt; 0 or the applicability schedule value is <span>\(\le \)</span> 0 or if the program is in warmup, *AvailStatus = NoAction*.
-
-Otherwise, the manager performs 3 limit checks.
-
-1)    If for all the zones connected to the air loop the room temperature at the thermostat of any zone is greater than the ventilation temperature schedule value, this check is true.
-
-2)    If for all the zones connected to the air loop the room temperature at the thermostat of any zone is less than the ventilation low limit temperature, this check is true.
-
-3)    If the difference between the control zone room temperature at the thermostat and the outside temperature is greater than the specified night venting delta T, this check is true.
-
-If 1) and 3) are true and 2) is false, the status is set to *CycleOn*; otherwise the status is *NoAction*.  If the status is *CycleOn* this manager sets some additional values in the *AirLoopControlInfo* data structure (a flag is set to indicate night ventilation is occurring and a flag is set to indicate that the air system flow rate has been specified by a manager) and in the * AirLoopFlow* data structure (the system flow fraction is specified). The night ventilation flag indicates to the fan that it should use alternate performance characteristics if they have been specified in a FanPerformance:NightVentilation object.
-
-### Differential Thermostat
-
-The input object AvailabilityManager:DifferentialThermostat is a manager that overrides fan or pump schedules depending on the temperature difference between two nodes. A typical use would be for one node to be an outdoor air node and the other a zone node. The inputs are:
-
-·        name of the hot node;
-
-·        name of the cold node;
-
-·        temperature difference for turning the system on (*DeltaT<sub>on</sub>*);
-
-·        temperature difference for turning the system off (*DeltaT<sub>off</sub>*).
-
-Note that there is no applicability schedule for this manager. Also, this manager always returns a status of *CycleOn* or *ForceOff*, never *NoAction*.
-
-*DeltaT* = *T<sub>hot\\ node</sub>* – *T<sub>cold\\ node</sub>*
-
-If *DeltaT* &gt;= *DeltaT<sub>on</sub>*  then
-
-*AvailStatus = CycleOn*
-
-      Else if *DeltaT* &lt;= *DeltaT<sub>off</sub>*  then
-
-*AvailStatus = ForceOff*
-
-Else
-
-*AvailStatus* remains in its previous state.
-
-### High Temperature Turn Off
-
-The input object AvailabilityManager:HighTemperatureTurnOff is used to turn off a central air system or a plant loop if a sensed node temperature exceeds a temperature limit. The inputs are:
-
-·        name of the sensed node;
-
-·        limit temperature (*T<sub>u</sub>*).
-
-If *T<sub>sensed\\ node</sub>* &gt;= *T<sub>u</sub>* then
-
-*AvailStatus* = *ForceOff*
-
-Else
-
-*AvailStatus* = *NoAction*
-
-### High Temperature Turn On
-
-The input object AvailabilityManager:HighTemperatureTurnOn is used to turn on a central air system or a plant loop if a sensed node temperature exceeds a temperature limit. The inputs are:
-
-·        name of the sensed node;
-
-·        limit temperature (*T<sub>u</sub>*).
-
-If *T<sub>sensed\\ node</sub>* &gt;= *T<sub>u</sub>* then
-
-*AvailStatus* = *CycleOn*
-
-Else
-
-*AvailStatus* = *NoAction*
-
-### Low Temperature Turn Off
-
-The input object AvailabilityManager:LowTemperatureTurnOff is used to turn off a central air system or a plant loop if a sensed node temperature is lower than a temperature limit. The inputs are:
-
-·        name of the sensed node;
-
-·        limit temperature (*T<sub>l</sub>*);
-
-·        applicability schedule name.
-
-If the applicability schedule exists and has a current value of &lt;= 0, the manager returns an availability status of *NoAction*.
-
-Otherwise,
-
-If *T<sub>sensed\\ node</sub>* &lt;= *T<sub>l</sub>*  then
-
-*AvailStatus* = *ForceOff*
-
-Else
-
-*AvailStatus* = *NoAction*
-
-### Low Temperature Turn On
-
-The input object AvailabilityManager:LowTemperatureTurnOn is used to turn on a central air system or a plant loop if a sensed node temperature is less than a temperature limit. The inputs are:
-
-·        name of the sensed node;
-
-·        limit temperature (*T<sub>l</sub>*).
-
-If *T<sub>sensed\\ node</sub>* &lt;= *T<sub>l</sub>*  then
-
-*AvailStatus* = *CycleOn*
-
-Else
-
-*AvailStatus* = *NoAction*
-
-### Hybrid Ventilation Control
-
-The input object AvailabilityManager:HybridVentilation serves two purposes: 1) it prevents simultaneous natural ventilation and HVAC system operation, and 2) it allows users to examine various strategies to maximize natural ventilation in order to reduce heating/cooling loads. This availability manager works with either the AirflowNetwork model or the simple airflow objects to provide controlled natural ventilation. The controlled natural ventilation objects referred to here are either AirflowNetwork:Multizone:ComponentDetailedOpening and AirflowNetwork:Multizone:ComponentSimpleOpening objects, or ZoneVentilation and ZoneMixing objects. The simple airflow objects are not allowed to work with the AirflowNetwork objects simultaneously. If there is no air loop, this availability manager can still be applied to controlled zone specified in the object. In order to apply hybrid ventilation manager to the controlled zone not served by any air loop, the HVAC air loop name input field must be left blank. Currently, zone component objects such as unit heater, unit ventilator, packaged terminal air conditioner, packaged terminal heat pump, zone water source heat pump, window air conditioner, variable refrigerant flow, energy recovery ventilator, outdoor air unit, fan coil unit, and ventilated slab can individually use hybrid ventilation managers to make a decision regarding whether their fan should be on or off. Also, hybrid ventilation manager can be applied to zones served by the ideal load zone component to turn them off when natural ventilation is active. Currently, hybrid ventilation manager is restricted to one per zone. It can either be applied through the air loop or directly to the zone. If hybrid ventilation manager is applied to an air loop and one of the zones served by the air loop also has hybrid ventilation manager, then zone hybrid ventilation manager is disabled. This availability manager performs somewhat differently from the other availability managers:
-
-n This availability manager is called before the program estimates (predicts) the cooling or heating load that needs to be met by the cooling/heating systems for the simulation time step. On the other hand, the other availability managers are called after the system cooling/heating load prediction. The main reason for calling AvailabilityManager:HybridVentilation early is that this manager determines whether natural ventilation is allowed or not, and the loads from natural ventilation are used to predict system loads.
-
-n This availability manager has its own control schedule and does not work in tandem with *AvailabilityManager:Scheduled*.
-
-n AvailabilityManager:HybridVentilation works completely independent of the other system availability managers, so this manager is not a valid system availability manager type in the AvailabilityManagerAssignmentList object.
-
-#### Control logic
-
-The control logic for each ventilation control mode is described below.
-
-#### Temperature control
-
-This control mode checks whether the outdoor air dry-bulb temperature is between the Minimum Outdoor Temperature and Maximum Outdoor Temperature specified. If the outdoor temperature is between the two values then natural ventilation is allowed, else natural ventilation is not allowed.
-
-When natural ventilation is allowed, the control then checks the temperature difference between the zone temperature and the temperature setpoint(s) in the controlled zone based on the specified temperature control type (four available temperature control types) to make a final decision:
-
-*Single Heating Setpoint:*
-
-If the zone temperature is below the setpoint, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid overcooling a space, which could result in additional heating load.
-
-*Single Cooling Setpoint:*
-
-If the zone temperature is above the setpoint, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid overheating a space, which could result in additional cooling load.
-
-*Single Heating Cooling Setpoint:*
-
-Since this temperature control type requires only a single setpoint, natural ventilation is not allowed. A recurring warning message is issued.
-
-*Dual Setpoint with DeadBand:*
-
-If the zone temperature is beyond the deadband, the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid either overcooling a space, which could result in additional heating load when the zone temperature is below the heating setpoint, or overheating a space, which could result in additional cooling load when the zone temperature is above the cooling setpoint.
-
-#### Enthalpy control
-
-This control mode checks whether the outdoor air enthalpy is between the Minimum Outdoor Enthalpy and Maximum Outdoor Enthalpy specified. If the outdoor enthalpy is between the two values then natural ventilation is allowed, else natural ventilation is not allowed.
-
-When natural ventilation is allowed, the control then checks the temperature difference between the zone temperature and the temperature setpoint(s) in the controlled zone based on the specific temperature control type to make a final decision. This procedure is the same as defined above for the temperature control mode.
-
-*Single Heating Setpoint:*
-
-If the zone temperature is below the setpoint, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid overcooling a space, which could result in additional heating load.
-
-*Single Cooling Setpoint:*
-
-If the zone temperature is above the setpoint, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid overheating a space, which could result in additional cooling load.
-
-*Single Heating Cooling Setpoint:*
-
-Since this temperature control type requires only a single setpoint, natural ventilation is not allowed. A recurring warning message is issued.
-
-*Dual Setpoint with DeadBand:*
-
-If the zone temperature is beyond the deadband, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid either overcooling a space, which could result in additional heating load when the zone temperature is below the heating setpoint, or overheating a space, which could result in additional cooling load when the zone temperature is above the cooling setpoint.
-
-#### Dew-Point control
-
-This control mode checks whether the outdoor air dewpoint temperature is between the Minimum Outdoor Dew-Point and Maximum Outdoor Dew-Point specified. If the outdoor dewpoint temperature is between the two values then natural ventilation is allowed, else national ventilation is not allowed.
-
-When natural ventilation is allowed and a humidistat is available in the controlled zone, the control then checks the humidity ratio difference between the zone air humidity ratio and humidistat setpoint in the controlled zone to make a final decision. It should be pointed out that the humidistat object provides the setpoint of relative humidity, the value of relative humidity has to be converted into the setpoint of humidity ratio using the actual zone air temperature for comparison. Since the humidistat only provides a single value for relative humidity, there are two possible scenarios:
-
-If the actual zone air humidity ratio is below the humidity ratio setpoint and the controlled zone needs humidification as the first scenario, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid dehumidifying a space, which could result in additional humidification load.
-
-If the actual zone air humidity ratio is above the humidity ratio setpoint and the controlled zone needs dehumidification as the second scenario, then the initial decision is overridden and natural ventilation is not allowed. This is intended to avoid humidifying a space, which could result in additional dehumidification load.
-
-#### Outdoor ventilation air control
-
-This control mode does not require any additional checks. The control only works with Airflow Network opening objects only, and is not allowed to work with ZoneVentilation and ZoneMixing objects.
-
-#### Availability Status
-
-After the hybrid ventilation control determines whether natural ventilation is allowed or not, the availability status flag is set as follows:
-
-If *Natural Ventilation* then
-
-*AvailStatus* = *CycleOn*
-
-Else
-
-*AvailStatus = ForceOn*
-
-### **Optimum Start Controls**
-
-#### Overview
-
-Optimum start is often also referred to as optimum recovery time. Commercial buildings are often operated intermittently by lowering heating set-point and increasing cooling set-point during unoccupied period. The building should return to set-point just before occupancy period starts. Therefore it is important to start the operation of heating and cooling plant before building is occupied. If the operation is started too early before the occupants return, energy is wasted. If it is started too late the occupants will be uncomfortable. An optimum start time for operation will save energy without compromising comfort.
-
-![](media/image6731.png)
-
-Figure 301. Optimal Start Control
-
-In practice a few proprietary algorithms are used to predict this start time value for preheating and precooling operation. ASHRAE Handbook refers to work done by (Seem, Armstrong, & Hancock, 1989) which compares seven different equations and suggests a set of equations for preheating and precooling time prediction.
-
-#### Algorithms
-
-There are a few algorithms to predict the start time for the HVAC system. Among these algorithms following are the promising ones that can be implemented in a simulation environment.
-
-#### Constant Start Time
-
-This is the simplest format of the optimum start algorithm. The HVAC system will start the HVAC system at a fixed number of hours before occupancy as specified by the user.
-
-#### Constant Temperature Gradient
-
-In practice most of the HVAC control manufacturers use a temperature gradient as a thermal capacity factor, in which temperature rise per unit time i.e. °C/hour is measured for the unoccupied building and then the difference between space temperature and set-point temperature is divided by this factor to calculate the actual number of hours before occupancy are needed to start the HVAC system.
-
-#### Adaptive Temperature Gradient
-
-Adaptive control is used to modify the temperature gradient depending on the time required to meet the set-point on the prior days. The adaptive algorithm takes the arithmetic average of the actual temperature gradients calculated for the specified number of previous days. 
-
-#### Adaptive ASHRAE Algorithm
-
-The equations suggested in the ASHRAE Handbook are used in combination with a recursive linear least square method to determine the optimum start/recovery time empirically. Depending on heating or cooling operation the start time is categorized as preheating or precooling time. According to (Seem, Armstrong, & Hancock, 1989) the preheating time is a strong function of outdoor temperature whereas precooling time is not strong function of outdoor temperature if space temperature is close or less than the setback temperature. Thus, two different equations are suggested for preheating and precooling time.
-
-n Precooling time
-
-<div>$${t_i} = {a_0} + {a_1}{T_{z,i}} + {a_2}T_{z,i}^2$$</div>
-
-
-
-Preheating time
-
-<div>$${t_i} = {a_0} + \left( {1 - {w_i}} \right)({a_1}{T_{z,i}} + {a_2}T_{z,i}^2) + {w_i}{a_3}{T_{o,i}}$$</div>
-
-Where, on *i*<sup>th</sup> day
-
-*t<sub>i</sub>* = start/recovery time,
-
-*T<sub>z,i</sub>* =           zone temperature
-
-*T<sub>o,i</sub>* =           outdoor temperature
-
-‘*w<sub>i</sub>*’ is a weighting factor which determines weighting given to outside and zone temperature.
-
-<div>$${w_i} = {1000^{ - \frac{{\left( {{T_{z,i}} - {T_{unocc}}} \right)}}{{\left( {{T_{occ}} - {T_{unocc}}} \right)}}}}$$</div>
-
-*T<sub>unocc</sub>* and *T<sub>occ</sub>* are setpoint temperatures during unoccupied (setback) and occupied periods.
-
-Coefficients *a<sub>0</sub>, a<sub>1</sub>, a<sub>2</sub>* (and *a<sub>3</sub>*) are separately calculated for heating and cooling operation and are updated from the optimum times from last three days thus; these coefficients carry history and adapt the trend from previous days.
-
-The optimum time for past days is determined using,
-
-<div>$${t_{opt,\left( {i - 1} \right)}} = {k_{\left( {i - 1} \right)}}\Delta t - \Delta t\left( {1 - \frac{{{q_{\left( {i - 1} \right)}}}}{{{q_{max}}}}} \right)$$</div>
-
-*k* = time steps required for recovery
-
-Δ*t* =            time-step
-
-*t<sub>opt,(i-1)</sub>* = recovery time on (*i*-1)<sup>th</sup> day
-
-*q<sub>(i-1)</sub>* =          energy extracted or added during last time step
-
-*q<sub>max</sub>* =          maximum capacity of the equipments
-
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-<!--RemoveStart-->
-Simulation Models – Encyclopedic Reference
-==========================================
-
-The following descriptions are grouped alphabetically (as much as possible) with some also having additional tags of “Heat Balance�, “HVAC�, and “Plant�.  With the integrated solution, these designations signify where the effects of these models have their first impacts.
-
-Main Sections:
-
-* [Thermal Comfort](#ThermalComfort)
-* [Trombe Walls](#TrombeWalls)
-* [Water Thermal Tanks](#WaterTanks)
-* [Water Systems](#WaterSystems)
-* [Zone Controls](#ZoneControls)
-* [Zone Equipment and Zone Forced Air Units](#ZoneEquip)
-<!--RemoveEnd-->
-
-Occupant Thermal Comfort <a name="ThermalComfort"></a>
-------------------------
-
-The integration of a sophisticated building thermal analysis tool with thermal comfort models allows one to perform an energy analysis on a zone and simultaneously determine if the environmental control strategy will be sufficient for the occupants to be thermally comfortable. This chapter is intended to provide background on thermal comfort, present an overview of state of the art thermal comfort models and present the mathematical models that have been incorporated into Energy Plus.
-
-Thermal comfort modeling is controlled primarily by the People input object. This includes input for selecting the type of thermal comfort model that is desired by the user as well as parameters that serve as inputs to all of the thermal comfort models. This includes the activity level, the work efficiency, the air velocity, and the clothing insulation level for people within the space.  All four of these parameters can be scheduled. More information on the People input object can be found in the EnergyPlus Input/Output Reference. More information on how each of these parameters is used and the specific modeling equations for the thermal comfort models can be found below.
-
-### Background on Thermal Comfort Models
-
-Throughout the last few decades, researchers have been exploring the thermal, physiological and psychological response of people in their environment in order to develop mathematical models to predict these responses. Researchers have empirically debated building occupants' thermal responses to the combined thermal effect of the personal, environmental and physiological variables that influence the condition of thermal comfort.
-
-There are two personal variables that influence the condition of thermal comfort: the thermal resistance of the clothing (I<sub>cl</sub>), and the metabolic rate (H/A<sub>Du</sub>). The thermal resistance of the clothing (I<sub>cl</sub>) is measured in units of "clo." The 1985 ASHRAE Handbook of Fundamentals (ASHRAE 1985) suggests multiplying the summation of the individual clothing items clo value by a factor of 0.82 for clothing ensembles.
-
-The metabolic rate (H/A<sub>Du</sub>), is a measure of the internal heat production rate of an occupant (H) w/hr. in per unit of "Dubois" body surface area (A<sub>Du</sub>) in units of m<sup>2</sup>. The DuBois body surface area is given by :
-
-<div>$${A_{Du}} = 0.202{(weight)^{0.425}}{(height)^{0.725}}$$</div>
-
-Using this equation, an area of 1.8 m<sup>2</sup> represents the surface area of an average person of weight 70 kg. and height 1.73 m (Fanger 1967). The metabolic rate is measured in mets, where 1 met = 58.2 W/m<sup>2</sup>.
-
-The environmental variables that influence the conditions of thermal comfort include:
-
-(1) Air Temperature (T<sub>a</sub>),
-
-(2) Mean Radiant Temperature (T<sub>r</sub>),
-
-(3) Relative air velocity (v),
-
-(4) Water vapor pressure in ambient air (P<sub>a</sub>)
-
-The Air Temperature (T<sub>a</sub>), a direct environmental index, is the dry-bulb temperature of the environment. The Mean Radiant Temperature (T<sub>r</sub>) is a rationally derived environmental index defined as the uniform black-body temperature that would result in the same radiant energy exchange as in the actual environment. The Relative air velocity (v) a direct environmental index is a measure of the air motion obtainable via a hot wire or vane anemometers. The Water vapor pressure in ambient air (P<sub>a</sub>) is a direct environmental index.
-
-The physiological variables that influence the conditions of thermal comfort include:
-
-(1) Skin Temperature (T<sub>sk</sub>),
-
-(2) Core or Internal Temperature (T<sub>cr</sub>),
-
-(3) Sweat Rate,
-
-(4) Skin Wettedness (w),
-
-(5) Thermal Conductance (K) between the core and skin.
-
-Where the Skin Temperature (T<sub>sk</sub>), the Core Temperature (T<sub>cr</sub>) and the Sweat Rate are physiological indices. The Skin Wettedness (w) is a rationally derived physiological index defined as the ratio of the actual sweating rate to the maximum rate of sweating that would occur if the skin were completely wet.
-
-One more consideration is important in dealing with thermal comfort - the effect of asymmetrical heating or cooling. This could occur when there is a draft or when there is a radiant flux incident on a person (which is what is of primary interest to us here). Fanger (1967) noted that the human regulatory system is quite tolerant of asymmetrical radiant flux. A reasonable upper limit on the difference in mean radiant temperature (T<sub>r</sub>) from one direction to the opposing direction is 15°C. (ASHRAE 1984). This limit is lower if there is a high air velocity in the zone.
-
-Table 78.  General Nomenclature list for Thermal Comfort Models
-
-<table class="table table-striped">
-
-
-
-
-
-
-
-
-<tr>
-<td>Mathematical variable</td>
-<td>Description</td>
-<td>Units
- </td>
-<td>Range</td>
-<td>FORTRAN variable</td>
-</tr>
-<tr>
-<td>A<sub>Du</sub></td>
-<td>Dubois body surface area</td>
-<td>m<sup>2</sup></td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>H</td>
-<td>Internal heat production rate of an occupant per unit area
-= M – W</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>IntHeatProd</td>
-</tr>
-<tr>
-<td>I<sub>cl</sub></td>
-<td>Thermal resistance of the clothing</td>
-<td>clo</td>
-<td>-</td>
-<td>CloUnit</td>
-</tr>
-<tr>
-<td>M</td>
-<td>Metabolic rate per unit area</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>ActLevel</td>
-</tr>
-<tr>
-<td>P<sub>a</sub></td>
-<td>Water vapor pressure in ambient air</td>
-<td>Torr</td>
-<td>-</td>
-<td>VapPress</td>
-</tr>
-<tr>
-<td>T<sub>a</sub></td>
-<td>Air temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>AirTemp</td>
-</tr>
-<tr>
-<td>T<sub>cr</sub></td>
-<td>Core or internal temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>CoreTemp</td>
-</tr>
-<tr>
-<td>T<sub>r</sub></td>
-<td>Mean radiant temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>RadTemp</td>
-</tr>
-<tr>
-<td>T<sub>sk</sub></td>
-<td>Skin temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>v</td>
-<td>Relative air velocity</td>
-<td>m/s</td>
-<td>-</td>
-<td>AirVel</td>
-</tr>
-<tr>
-<td>W</td>
-<td>The rate of heat loss due to the performance of work</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>WorkEff</td>
-</tr>
-<tr>
-<td>w</td>
-<td>Skin wettedness</td>
-<td>-</td>
-<td>-</td>
-<td>-</td>
-</tr>
-
-</table>
-
-### Mathematical Models for Predicting Thermal Comfort
-
-Many researchers have been exploring ways to predict the thermal sensation of people in their environment based on the personal, environmental and physiological variables that influence thermal comfort. From the research done, some mathematical models that simulate occupants' thermal response to their environment have been developed. Most thermal comfort prediction models use a seven or nine point thermal sensation scale, as in the following tables.
-
-Table 79.  Seven point Thermal Sensation Scale
-
-<table class="table table-striped">
-
-
-
-
-
-<tr>
-<td>Sensation</td>
-<td>Description</td>
-</tr>
-<tr>
-<td>3</td>
-<td>Hot</td>
-</tr>
-<tr>
-<td>2</td>
-<td>Warm</td>
-</tr>
-<tr>
-<td>1</td>
-<td>slightly warm</td>
-</tr>
-<tr>
-<td>0</td>
-<td>neutral</td>
-</tr>
-<tr>
-<td>-1</td>
-<td>slightly cool</td>
-</tr>
-<tr>
-<td>-2</td>
-<td>cool</td>
-</tr>
-<tr>
-<td>-3</td>
-<td>cold</td>
-</tr>
-
-</table>
-
-
-
-
-
-Table 80.  Nine point Thermal Sensation Scale
-
-<table class="table table-striped">
-
-
-
-
-
-<tr>
-<td>Sensation Value</td>
-<td>Description</td>
-</tr>
-<tr>
-<td>4</td>
-<td>very hot</td>
-</tr>
-<tr>
-<td>3</td>
-<td>hot</td>
-</tr>
-<tr>
-<td>2</td>
-<td>warm</td>
-</tr>
-<tr>
-<td>1</td>
-<td>slightly warm</td>
-</tr>
-<tr>
-<td>0</td>
-<td>neutral</td>
-</tr>
-<tr>
-<td>-1</td>
-<td>slightly cool</td>
-</tr>
-<tr>
-<td>-2</td>
-<td>cool</td>
-</tr>
-<tr>
-<td>-3</td>
-<td>cold</td>
-</tr>
-<tr>
-<td>-4</td>
-<td>very cold</td>
-</tr>
-
-</table>
-
-The most notable models have been developed by P.O. Fanger (the Fanger Comfort Model), the J. B. Pierce Foundation (the Pierce Two-Node Model), and researchers at Kansas State University (the KSU Two-Node Model). Berglund (1978) presents a detailed description of the theory behind these three models.
-
-Note for all Thermal Comfort reporting:  Though the published values for thermal comfort “vote� have a discrete scale (e.g. –3 to +3 or –4 to +4), the calculations in EnergyPlus are carried out on a continuous scale and, thus, reporting may be “off the scale� with specific conditions encountered in the space.  This is not necessarily an error in EnergyPlus – rather a different approach that does not take the “limits� of the discrete scale values into account.
-
-The main similarity of the three models is that all three apply an energy balance to a person and use the energy exchange mechanisms along with experimentally derived physiological parameters to predict the thermal sensation and the physiological response of a person due to their environment. The models differ somewhat in the physiological models that represent the human passive system (heat transfer through and from the body) and the human control system (the neural control of shivering, sweating and skin blood flow). The models also differ in the criteria used to predict thermal sensation. However, all three models use information from the People statement and the thermal comfort model is selected via the People statement in a user’s input file. Scheduled parameters such as the activity level, work efficiency, air velocity, and clothing insulation level all have a direct bearing on the thermal comfort models. For more information on the input of these parameters, see the People statement in the EnergyPlus Input/Output Reference. For more information on how each individual thermal comfort model uses these parameters, please consult the next several sections.
-
-The main similarity of the three models is that all three apply an energy balance to a person and use the energy exchange mechanisms along with experimentally derived physiological parameters to predict the thermal sensation and the physiological response of a person due to their environment. The models differ somewhat in the physiological models that represent the human passive system (heat transfer through and from the body) and the human control system (the neural control of shivering, sweating and skin blood flow). The models also differ in the criteria used to predict thermal sensation.
-
-### Fanger Comfort Model
-
-Fanger's Comfort model was the first one developed. It was published first in 1967 (Fanger 1967) and then in 1970 (Fanger 1970), and helped set the stage for the other two models. The mathematical model developed by P.O. Fanger is probably the most well known of the three models and is the easiest to use because it has been put in both chart and graph form.
-
-#### Fanger Model Nomenclature List
-
-Table 81.  Nomenclature list for Fanger model
-
-<table class="table table-striped">
-
-
-
-
-
-
-
-
-<tr>
-<td>Mathematical variable</td>
-<td>Description</td>
-<td>Units</td>
-<td>Range</td>
-<td>FORTRAN variable</td>
-</tr>
-<tr>
-<td>A<sub>Du</sub></td>
-<td>Dubois body surface area</td>
-<td>m<sup>2</sup></td>
-<td>-</td>
-<td>BodySurfaceArea</td>
-</tr>
-<tr>
-<td>C<sub>res</sub></td>
-<td>The rate of dry respiratory heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>DryRespHeatLoss</td>
-</tr>
-<tr>
-<td>E<sub>dif</sub></td>
-<td>The rate of heat loss from the diffusion of water vapor through the skin</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>EvapHeatLossDiff</td>
-</tr>
-<tr>
-<td>E<sub>res</sub></td>
-<td>The rate of latent respiratory heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>LatRespHeatLoss</td>
-</tr>
-<tr>
-<td>E<sub>rsw,req</sub></td>
-<td>The rate of heat loss from the evaporation of regulatory sweating at the state of comfort</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>EvapHeatLossRegComf</td>
-</tr>
-<tr>
-<td>E<sub>sk</sub></td>
-<td>Total evaporative heat loss from skin</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>EvapHeatLoss</td>
-</tr>
-<tr>
-<td>f<sub>cl</sub></td>
-<td>The ratio of clothed body</td>
-<td>-</td>
-<td> </td>
-<td>CloBodyRat</td>
-</tr>
-<tr>
-<td>f<sub>eff</sub></td>
-<td>The fraction of surface effective for radiation
-(= 0.72)</td>
-<td>-</td>
-<td>-</td>
-<td>RadSurfEff</td>
-</tr>
-<tr>
-<td>H</td>
-<td>Internal heat production rate of an occupant per unit area (= M – W)</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>IntHeatProd</td>
-</tr>
-<tr>
-<td>h<sub>c</sub></td>
-<td>Convective heat transfer coefficient</td>
-<td>W/m<sup>2</sup>°C</td>
-<td>-</td>
-<td>Hc</td>
-</tr>
-<tr>
-<td>L</td>
-<td>All the modes of energy loss from body</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>M</td>
-<td>Metabolic rate per unit area</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>ActLevel</td>
-</tr>
-<tr>
-<td>P<sub>a</sub></td>
-<td>Water vapor pressure in ambient air</td>
-<td>Torr</td>
-<td>-</td>
-<td>VapPress</td>
-</tr>
-<tr>
-<td>PMV</td>
-<td>Predicted Mean Vote</td>
-<td>-</td>
-<td>-4~4</td>
-<td>PMV</td>
-</tr>
-<tr>
-<td>PPD</td>
-<td>Predicted Percentage of Dissatisfied</td>
-<td>-</td>
-<td>0~100%</td>
-<td>PPD</td>
-</tr>
-<tr>
-<td>Q<sub>c</sub></td>
-<td>The rate of convective heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>ConvHeatLoss</td>
-</tr>
-<tr>
-<td>Q<sub>dry</sub></td>
-<td>Sensible heat flow from skin</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>DryHeatLoss</td>
-</tr>
-<tr>
-<td>Q<sub>r</sub></td>
-<td>The rate of radiative heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>RadHeatLoss</td>
-</tr>
-<tr>
-<td>Q<sub>res</sub></td>
-<td>The rate of respiratory heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>RespHeatLoss</td>
-</tr>
-<tr>
-<td>T<sub>a</sub></td>
-<td>Air temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>AirTemp</td>
-</tr>
-<tr>
-<td>T<sub>cl</sub></td>
-<td>Clothing surface temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>CloSurfTemp</td>
-</tr>
-<tr>
-<td>T<sub>cla</sub></td>
-<td>Clothing surface temperature (Absolute)</td>
-<td>°K</td>
-<td>-</td>
-<td>AbsCloSurfTemp</td>
-</tr>
-<tr>
-<td>T<sub>ra</sub></td>
-<td>Mean radiant temperature</td>
-<td>°K</td>
-<td>-</td>
-<td>AbsRadTemp</td>
-</tr>
-<tr>
-<td>W</td>
-<td>The rate of heat loss due to the performance of work</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>WorkEff</td>
-</tr>
-<tr>
-<td>e</td>
-<td>The emissivity of clothing-skin surface</td>
-<td>-</td>
-<td>-</td>
-<td>SkinEmiss</td>
-</tr>
-<tr>
-<td>s</td>
-<td>The Stefan-Boltzman constant (= 5.67×10<sup>-8</sup>)</td>
-<td>W/m<sup>2</sup>K<sup>4</sup></td>
-<td>-</td>
-<td>StefanBoltz</td>
-</tr>
-
-</table>
-
-#### Description of the model and algorithm
-
-Fanger developed the model based on the research he performed at Kansas State University and the Technical University of Denmark. Fanger used the seven-point form of a thermal sensation scale along with numerous experiments involving human subjects in various environments. He related the subjects in response to the variables, which influence the condition of thermal comfort. Fanger's model is based upon an energy analysis that takes into account all the modes of energy loss (L) from the body, including: the convection and radiant heat loss from the outer surface of the clothing, the heat loss by water vapor diffusion through the skin, the heat loss by evaporation of sweat from the skin surface, the latent and dry respiration heat loss and the heat transfer from the skin to the outer surface of the clothing. The model assumes that the person is thermally at steady state with his environment.
-
-<span>\(M = L\)</span>                                                                                     W/m<sup>2</sup>
-
-<span>\(L = {Q_{res}} + {Q_{dry}} + {E_{sk}} + W\)</span>                                                         W/m<sup>2</sup>
-
-<span>\({Q_{res}} = {E_{res}} + {C_{res}} = 0.000017M(5867 - {P_a}) + 0.0014M(34 - {T_a})\)</span>     W/m<sup>2</sup>
-
-LatRespHeatLoss = 0.000017\*ActLevel\*(5867. - VapPress)
-
-DryRespHeatLoss = 0.0014\*ActLevel\*(34.- AirTemp)
-
-RespHeatLoss = LatRespHeatLoss + DryRespHeatLoss
-
-<span>\({Q_c} = {h_c} \times {f_{cl}}({T_{cl}} - {T_a})\)</span>                                                               W/m<sup>2</sup>
-
-<span>Q<sub>r</sub> = 3.96\*f<sub>cl</sub>\*[(0.01\*T<sub>cla</sub>)^4 - (0.01\*T<sub>ra</sub>)^4]</span>                                                       W/m<sup>2</sup>
-
-<span>\({Q_{dry}} = {Q_c} + {Q_r}\)</span>                                                                         W/m<sup>2</sup>
-
-ConvHeatLos = CloBodyRat\*Hc\*(CloSurfTemp - AirTemp)
-
-RadHeatLoss = 3.96\*CloBodyRat &
-
-\*[(0.01\*AbsCloSurfTemp)\*\*4 - (0.01\*AbsRadTemp)\*\*4]
-
-DryHeatLoss = ConvHeatLoss + RadHeatLoss
-
-For<span>\(H > 58.2\)</span>, <span>\({E_{rsw}} = 0.42(H - 58.2)\)</span>                                      W/m<sup>2</sup>
-
-For <span>\(H \le 58.2\)</span>, <span>\({E_{rsw}} = 0\)</span>                                                           W/m<sup>2</sup>
-
-<span>E<sub>diff</sub> = 0.00305\*(5733.0 - 6.99H - P<sub>a</sub>)</span>                        W/m<sup>2</sup>
-
-<span>\({E_{sk}} = {E_{rsw}} + {E_{diff}}\)</span>                                                                      W/m<sup>2</sup>
-
-EvapHeatLossRegComf = 0.42\*(IntHeatProd - ActLevelConv)
-
-EvapHeatLossRegComf = 0.0
-
-EvapHeatLossDiff = 0.00305\*(5733.0 - 6.99\*IntHeatProd - VapPress)
-
-EvapHeatLoss = EvapHeatLossRegComf + EvapHeatLossDiff
-
-The Fanger model was developed using the thermal sensation votes from subjects at KSU and Denmark, and the Predicted Mean Vote (PMV) thermal sensation scale is based on how the energy loss (L) deviates from the metabolic rate (M) in the following form:
-
-<div>$$PMV = (0.303{e^{ - 0.036M}} + 0.028)(H - L)$$</div>
-
-ThermSensTransCoef = 0.303\*EXP(-0.036\*ActLevel) + 0.028
-
-PMV = ThermSensTransCoef\*(IntHeatProd - EvapHeatLoss - RespHeatLoss - DryHeatLoss)
-
-Predicted Percent of Dissatisfied (PPD) people at each PMV is calculated as follows:
-
-PPD = 100.0 - 95.0\*EXP(-0.03353\*PMV\*\*4 - 0.2179\*PMV\*\*2)
-
-### Pierce Two-Node Model
-
-The Pierce Two-Node model was developed at the John B. Pierce Foundation at Yale University. The model has been continually expanding since its first publication in 1970 (Gagge et.al. 1970). The most recent version on the model appears in the 1986 ASHRAE Transactions (Gagge et.al. 1986).
-
-#### Pierce Two-Node Model Nomenclature List
-
-Table 82.  Nomenclature list for Pierce Two-Node model
-
-<table class="table table-striped">
-
-
-
-
-
-
-
-
-<tr>
-<td>Mathematical variable</td>
-<td>Description</td>
-<td>Units
- </td>
-<td>Range</td>
-<td>FORTRAN variable</td>
-</tr>
-<tr>
-<td>C<sub>dil</sub></td>
-<td>Constant for skin blood flow</td>
-<td> </td>
-<td> </td>
-<td>SkinBloodFlowConst</td>
-</tr>
-<tr>
-<td>C<sub>res</sub></td>
-<td>The rate of dry respiratory heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>DryRespHeatLoss</td>
-</tr>
-<tr>
-<td>C<sub>sw</sub></td>
-<td>Proportionality constant for sweat control</td>
-<td>g/m<sup>2</sup>hr</td>
-<td> </td>
-<td>SweatContConst</td>
-</tr>
-<tr>
-<td>DISC</td>
-<td>Predicted discomfort vote</td>
-<td>-</td>
-<td>-5~5</td>
-<td>DISC</td>
-</tr>
-<tr>
-<td>E<sub>dif</sub></td>
-<td>The rate of heat loss from the diffusion of water vapor through the skin</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>EvapHeatLossDiff</td>
-</tr>
-<tr>
-<td>E<sub>max</sub></td>
-<td>Maximum evaporative heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>EvapHeatLossMax</td>
-</tr>
-<tr>
-<td>E<sub>sk</sub></td>
-<td>Total evaporative heat loss from skin</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>EvapHeatLoss</td>
-</tr>
-<tr>
-<td>E<sub>res</sub></td>
-<td>The rate of latent respiratory heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>LatRespHeatLoss</td>
-</tr>
-<tr>
-<td>E<sub>rsw</sub></td>
-<td>The rate of heat loss from the evaporation of regulatory sweating</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>EvapHeatLossRegSweat</td>
-</tr>
-<tr>
-<td>E<sub>rsw,req</sub></td>
-<td>The rate of heat loss from the evaporation of regulatory sweating at the state of comfort</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>EvapHeatLossRegComf</td>
-</tr>
-<tr>
-<td>ET*</td>
-<td>Effective Temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>ET</td>
-</tr>
-<tr>
-<td>f<sub>cl</sub></td>
-<td>The ratio of clothed body</td>
-<td>-</td>
-<td> </td>
-<td>CloBodyRat</td>
-</tr>
-<tr>
-<td>f<sub>eff</sub></td>
-<td>The fraction of surface effective for radiation
-(= 0.72)</td>
-<td>-</td>
-<td>-</td>
-<td>RadSurfEff</td>
-</tr>
-<tr>
-<td>H</td>
-<td>Internal heat production rate of an occupant per unit area (= M – W)</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>IntHeatProd</td>
-</tr>
-<tr>
-<td>h</td>
-<td>Combined heat transfer coefficient</td>
-<td>W/m<sup>2</sup>°C</td>
-<td> </td>
-<td>H</td>
-</tr>
-<tr>
-<td>h<sub>c</sub></td>
-<td>Convective heat transfer coefficient</td>
-<td>W/m<sup>2</sup>°C</td>
-<td>-</td>
-<td>Hc</td>
-</tr>
-<tr>
-<td>h<sub>e</sub>’</td>
-<td>Combined evaporative heat transfer coefficient</td>
-<td>W/(m<sup>2</sup>kP<sub>a</sub>)</td>
-<td> </td>
-<td>-</td>
-</tr>
-<tr>
-<td>h<sub>r</sub></td>
-<td>Radiant heat transfer coefficient</td>
-<td>W/m<sup>2</sup>°C</td>
-<td>-</td>
-<td>Hr</td>
-</tr>
-<tr>
-<td>I<sub>cl</sub></td>
-<td>Clothing insulation</td>
-<td>m<sup>2</sup>°C/W</td>
-<td> </td>
-<td>-</td>
-</tr>
-<tr>
-<td>L</td>
-<td>All the modes of energy loss from body</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>L<sub>ET*</sub></td>
-<td>All the modes of energy loss from body at ET*</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>-</td>
-</tr>
-<tr>
-<td>L<sub>SET*</sub></td>
-<td>All the modes of energy loss from body at SET*</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>-</td>
-</tr>
-<tr>
-<td>M</td>
-<td>Metabolic rate per unit area</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>ActLevel</td>
-</tr>
-<tr>
-<td>M<sub>act</sub></td>
-<td>Metabolic heat production due to activity</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>-</td>
-</tr>
-<tr>
-<td>M<sub>shiv</sub></td>
-<td>Metabolic heat production due to shivering</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>ShivResponse</td>
-</tr>
-<tr>
-<td>P<sub>a</sub></td>
-<td>Water vapor pressure in ambient air</td>
-<td>Torr</td>
-<td>-</td>
-<td>VapPress</td>
-</tr>
-<tr>
-<td>PMV*</td>
-<td>Predicted Mean Vote modified by ET* or SET*</td>
-<td>-</td>
-<td>-4~4</td>
-<td>PMVET
-PMVSET</td>
-</tr>
-<tr>
-<td>P<sub>SET*</sub></td>
-<td>Water vapor pressure at SET*</td>
-<td>°C</td>
-<td> </td>
-<td>StdVapPressSET</td>
-</tr>
-<tr>
-<td>P<sub>sk</sub></td>
-<td>Saturated water vapor pressure at required skin temperature</td>
-<td>Torr</td>
-<td>-</td>
-<td>SatSkinVapPress</td>
-</tr>
-<tr>
-<td>Q<sub>c</sub></td>
-<td>The rate of convective heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>ConvHeatLoss</td>
-</tr>
-<tr>
-<td>Q<sub>crsk</sub></td>
-<td>Heat flow from core to skin</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>HeatFlow</td>
-</tr>
-<tr>
-<td>Q<sub>dry</sub></td>
-<td>Sensible heat flow from skin</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>DryHeatLoss</td>
-</tr>
-<tr>
-<td>Q<sub>r</sub></td>
-<td>The rate of radiative heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>RadHeatLoss</td>
-</tr>
-<tr>
-<td>Q<sub>res</sub></td>
-<td>The rate of respiratory heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>RespHeatLoss</td>
-</tr>
-<tr>
-<td>S<sub>cr</sub></td>
-<td>Heat storage in core compartment</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>CoreheatStorage</td>
-</tr>
-<tr>
-<td>SET*</td>
-<td>Standard Effective Temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>SET</td>
-</tr>
-<tr>
-<td>SIG<sub>b</sub></td>
-<td>Thermal signal of body</td>
-<td>°C</td>
-<td> </td>
-<td>BodyThermSigCold
-BodyThermSigWarm</td>
-</tr>
-<tr>
-<td>SIG<sub>cr</sub></td>
-<td>Thermal signal of core</td>
-<td>°C</td>
-<td> </td>
-<td>CoreThermSigCold
-CoreThermSigWarm</td>
-</tr>
-<tr>
-<td>SIG<sub>sk</sub></td>
-<td>Thermal signal of skin</td>
-<td>°C</td>
-<td> </td>
-<td>SkinThermSigCold
-SkinThermSigWarm</td>
-</tr>
-<tr>
-<td>SKBF</td>
-<td>Skin blood flow</td>
-<td>L/m<sup>2</sup>hr</td>
-<td> </td>
-<td>SkinBloodFlow</td>
-</tr>
-<tr>
-<td>S<sub>sk</sub></td>
-<td>Heat storage in skin compartment</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>SkinHeatStorage</td>
-</tr>
-<tr>
-<td>S<sub>tr</sub></td>
-<td>Constriction constant of skin blood flow for average person</td>
-<td> </td>
-<td> </td>
-<td>Str</td>
-</tr>
-<tr>
-<td>SW<sub>reg</sub></td>
-<td>The rate of regulatory sweating</td>
-<td>g/m<sup>2</sup>hr</td>
-<td> </td>
-<td>RegSweat</td>
-</tr>
-<tr>
-<td>T<sub>a</sub></td>
-<td>Air temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>AirTemp</td>
-</tr>
-<tr>
-<td>T<sub>b</sub></td>
-<td>Mean body temperature</td>
-<td> </td>
-<td> </td>
-<td>AvgBodyTemp</td>
-</tr>
-<tr>
-<td>T<sub>b-c</sub></td>
-<td>Mean body temperature when DISC is zero (lower limit)</td>
-<td>°C</td>
-<td> </td>
-<td>AvgBodyTempLow</td>
-</tr>
-<tr>
-<td>T<sub>b-h</sub></td>
-<td>Mean body temperature when HSI is 100 (upper limit)</td>
-<td>°C</td>
-<td> </td>
-<td>AvgBodyTempHigh</td>
-</tr>
-<tr>
-<td>T<sub>cl</sub></td>
-<td>Clothing surface temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>CloSurfTemp</td>
-</tr>
-<tr>
-<td>T<sub>cr</sub></td>
-<td>Core or internal temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>CoreTemp</td>
-</tr>
-<tr>
-<td>T<sub>r</sub></td>
-<td>Mean radiant temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>RadTemp</td>
-</tr>
-<tr>
-<td>TSENS</td>
-<td>Thermal sensation vote</td>
-<td>-</td>
-<td>-5~5</td>
-<td>TSENS</td>
-</tr>
-<tr>
-<td>T<sub>sk</sub></td>
-<td>Skin temperature</td>
-<td>°C</td>
-<td> </td>
-<td>SkinTemp</td>
-</tr>
-<tr>
-<td>W</td>
-<td>The rate of heat loss due to the performance of work</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>WorkEff</td>
-</tr>
-<tr>
-<td>w<sub>dif</sub></td>
-<td>Skin wettedness due to diffusion trough the skin</td>
-<td> </td>
-<td> </td>
-<td>SkinWetDiff</td>
-</tr>
-<tr>
-<td>w<sub>rsw</sub></td>
-<td>Skin wettedness due to regulatory sweating</td>
-<td> </td>
-<td> </td>
-<td>SkinWetSweat</td>
-</tr>
-<tr>
-<td>e</td>
-<td>The emissivity of clothing-skin surface</td>
-<td>-</td>
-<td>-</td>
-<td>SkinEmiss</td>
-</tr>
-<tr>
-<td>s</td>
-<td>The Stefan-Boltzman constant (= 5.67×10<sup>-8</sup>)</td>
-<td>W/m<sup>2</sup>K<sup>4</sup></td>
-<td>-</td>
-<td>StefanBoltz</td>
-</tr>
-
-</table>
-
-#### Description of the model and algorithm
-
-The Pierce model thermally lumps the human body as two isothermal, concentric compartments, one representing the internal section or core (where all the metabolic heat is assumed to be generated and the skin comprising the other compartment). This allows the passive heat conduction from the core compartment to the skin to be accounted for. The boundary line between two compartments changes with respect to skin blood flow rate per unit skin surface area (SKBF in L/h•m<sup>2</sup>) and is described by alpha – the fraction of total body mass attributed to the skin compartment (Doherty and Arens 1988).
-
-<div>$$\alpha  = 0.0417737 + 0.7451832/(SKBF + 0.585417)$$</div>
-
-SkinMassRat = 0.0417737 + 0.7451832/(SkinBloodFlow + 0.585417)
-
-Furthermore, the model takes into account the deviations of the core, skin, and mean body temperature weighted by alpha from their respective setpoints. Thermoregulatory effector mechanisms (Regulatory sweating, skin blood flow, and shivering) are defined in terms of thermal signals from the core, skin and body (Doherty and Arens 1988).
-
-<span>\(SI{G_{cr}} = {T_{cr}} - 36.8\)</span>                                                                    °C
-
-<span>\(SI{G_{sk}} = {T_{sk}} - 33.7\)</span>                                                                    °C
-
-<span>\(SI{G_b} = {T_b} - 36.49\)</span>                                                                    °C
-
-SkinThermSigWarm = SkinTemp - SkinTempSet
-
-SkinThermSigCold = SkinTempSet - SkinTemp
-
-CoreThermSigWarm = CoreTemp - CoreTempSet
-
-CoreThermSigCold = CoreTempSet - CoreTemp
-
-BodyThermSigWarm = AvgBodyTemp - AvgBodyTempSet
-
-BodyThermSigCold = AvgBodyTempSet-AvgBodyTemp
-
-<span>\(SKBF = (6.3 + C{}_{dil} \times SI{G_{cr}})/(1 + {S_{tr}} \times ( - SI{G_{sk}}))\)</span>                      L/hr•m<sup>2</sup>
-
-VasodilationFac = SkinBloodFlowConst\*CoreWarmDelTemp
-
-VasoconstrictFac = Str\*SkinColdDelTemp
-
-SkinBloodFlow = (6.3 + VasodilationFac)/(1. + VasoconstrictFac)
-
-<span>\(S{W_{reg}} = {C_{sw}}SI{G_b}{e^{(SI{G_{sk}}/10.7)}}\)</span>                                                       g/hr•m<sup>2</sup>
-
-RegSweat = SweatContConst\*BodyWarmDelTemp\*EXP(SkinWarmDelTemp/10.7)
-
-<span>\({M_{shiv}} = 19.4( - SI{G_{cr}})( - SI{G_{sk}})\)</span>                                                 W/m<sup>2</sup>
-
-ShivResponse = 19.4\*SkinThermSigCold\*CoreThermSigCold
-
-The latest version of the Pierce model (Fountain and Huizenga 1997) discusses the concepts of SET\* and ET\*. The Pierce model converts the actual environment into a "standard environment" at a Standard Effective Temperature, SET\*. SET\* is the dry-bulb temperature of a hypothetical environment at 50% relative humidity for subjects wearing clothing that would be standard for the given activity in the real environment. Furthermore, in this standard environment, the same physiological strain, i.e. the same skin temperature and skin wettedness and heat loss to the environment, would exist as in the real environment. The Pierce model also converts the actual environment into a environment at an Effective Temperature, ET\*, that is the dry-bulb temperature of a hypothetical environment at 50% relative humidity and uniform temperature (Ta = MRT) where the subjects would experience the same physiological strain as in the real environment.
-
-In the latest version of the model it is suggested that the classical Fanged PMV be modified by using ET\* or SET\* instead of the operative temperature. This gives a new index PMV\* which is proposed for dry or humid environments. It is also suggested that PMV\* is very responsive to the changes in vapor permeation efficiency of the occupants clothing.
-
-<span>\(M = {M_{act}} + {M_{shiv}}\)</span>                                                                     W/m<sup>2</sup>
-
-ActLevel = ActLevel + ActShiv
-
-<span>\(L = {Q_{res}} + {Q_{dry}} + {E_{sk}} + W\)</span>                                                         W/m<sup>2</sup>
-
-<span>\(\begin{array}{l}{Q_{res}} = {E_{res}} + {C_{res}} = 0.0023M(44 - {P_{a(torr)}}) + 0.0014M(34 - {T_a})\\ = 0.017251M(5.8662 - {P_{a(kPa)}}) + 0.0014M(34 - {T_a})\end{array}\)</span>W/m<sup>2</sup>
-
-LatRespHeatLoss = 0.017251\*ActLevel\*(5.8662 - VapPress)
-
-DryRespHeatLoss = 0.0014\*ActLevel\*(34.- AirTemp)
-
-RespHeatLoss = LatRespHeatLoss + DryRespHeatLoss
-
-<span>\({Q_c} = {h_c} \times {f_{cl}}({T_{cl}} - {T_a})\)</span>                                                               W/m<sup>2</sup>
-
-<span>\({Q_r} = {h_r} \times {f_{cl}}({T_{cl}} - {T_r})\)</span>                                                               W/m<sup>2</sup>
-
-<span>\({Q_{dry}} = {Q_c} + {Q_r}\)</span>                                                                         W/m<sup>2</sup>
-
-DryHeatLoss = CloBodyRat\*(Hc\*(CloSurfTemp - AirTemp) + Hr\*(CloSurfTemp - RadTemp))
-
-In Pierce model, the convective heat transfer coefficient, h<sub>c</sub>, varies with the air velocity around body and metabolic rate. The model uses the maximum value of following equations.
-
-<span>\({h_c} = 8.6 \times {v^{_{0.53}}}\)</span>                                                                           W/m<sup>2</sup>°C
-
-<span>\({h_c} = 5.66{(M/58.2 - 0.85)^{0.39}}\)</span>                                                  W/m<sup>2</sup>°C
-
-Hc = 8.6\*AirVel\*\*0.53
-
-HcAct = 5.66\*(ActMet - 0.85)\*\*0.39
-
-Also, in the model, the radiant heat transfer coefficient, h<sub>r</sub>, is defined by following equation (Doherty and Arens 1988):
-
-<span>\({h_r} = 4. \times {f_{eff}}\varepsilon \sigma {(({T_{cl}} + {T_r})/2 + 273.15)^3}\)</span>                                    W/m<sup>2</sup>°C
-
-Hr = 4.\*RadSurfEff\*StefanBoltz\*((CloSurfTemp + RadTemp)/2. + TAbsConv)\*\*3
-
-In the Pierce model, T<sub>cl</sub> is estimated by each iteration using following equation:
-
-<span>\({T_{cl}} = ({T_{sk}}/{I_{cl}} + {f_{cl}}({h_c}{T_a} - {h_r}{T_r}))/(1/{I_{cl}} + {f_{cl}}({h_c} + {h_r}))\)</span>              °C
-
-CloSurfTemp = (CloCond\*SkinTemp + CloBodyRat\*(Hc\*AirTemp &
-
-+ Hr\*RadTemp))/(CloCond + CloBodyRat\*(Hc + Hr))
-
-Total evaporative heat loss from the skin, E<sub>sk</sub>, includes evaporation of water produced by regulatory sweating, E<sub>rsw</sub>, and evaporation of water vapor that diffuses through the skin surface, E<sub>diff</sub>.
-
-<span>\({E_{sk}} = {E_{rsw}} + {E_{diff}}\)</span>                                                                      W/m<sup>2</sup>
-
-EvapHeatLoss = EvapHeatLossRegSweat + EvapHeatLossRegDiff
-
-<span>\({E_{rsw}} = 0.68 \times S{W_{reg}}\)</span>                                                                  W/m<sup>2</sup>
-
-<span>\({E_{diff}} = {w_{diff}} \times {E_{\max }}\)</span>                                                                    W/m<sup>2</sup>
-
-RegHeatLoss = 0.68\*RegSweat
-
-DiffHeatLoss = SkinWetDiff\*MaxEvapHeatLoss
-
-Where,
-
-0.68 is the passive water vapor diffusion rate in g/h·m<sup>2</sup>·Torr
-
-and,
-
-<div>$${w_{diff}} = 0.06(1 - {w_{rsw}})$$</div>
-
-<span>\({E_{\max }} = {h_e}'({P_{sk}} - {P_a})\)</span>                                                                 W/m<sup>2</sup>
-
-<div>$${w_{rsw}} = {E_{rsw}}/{E_{\max }}$$</div>
-
-SkinWetDiff = (1.-SkinWetSweat)\*.06
-
-MaxEvapHeatLoss = (1./TotEvapHeatResist)\*(SatSkinVapPress - VapPress)
-
-SkinWetSweat = EvapHeatLossRegSweat/MaxEvapHeatLoss
-
-The Pierce model has one additional heat flow term describing the heat transfer between the internal core compartment and the outer skin shell (Doherty and Arens 1988).
-
-<span>\({Q_{crsk}} = (5.28 + 1.163SKBF)({T_{cr}} - {T_{sk}})\)</span>                                     W/m<sup>2</sup>
-
-HeatFlow = (CoreTemp-SkinTemp)\*(5.28 + 1.163\*SkinBloodFlow)
-
-Where
-
-5.28 is the average body tissue conductance in W/m<sup>2</sup>•°C
-
-1.163 is the thermal capacity of blood in W•h/L•°C
-
-Thus, individual heat balance equations for core and skin compartments are expressed using this term, Q<sub>c-s</sub>. New temperatures of core, skin and body are calculated by each iteration from rates of heat storage in the core and skin.
-
-<span>\({S_{sk}} = {Q_{c - s}} - {Q_c} - {Q_r} - {E_{sk}}\)</span>                                                        W/m<sup>2</sup>°C
-
-SkinHeatStorage = HeatFlow - DryHeatLoss - EvapHeatLoss
-
-<span>\({S_{cr}} = M - W - {Q_{res}} - {Q_{c - s}}\)</span>                                                        W/m<sup>2</sup>°C
-
-CoreHeatStorage = IntHeatProd - RespHeatLoss  - HeatFlow
-
-Thus,
-
-<div>$$PMVET = (0.303{e^{ - 0.036M}} + 0.028)(H - {L_{ET*}})$$</div>
-
-<div>$$PMVSET = (0.303{e^{ - 0.036M}} + 0.028)(H - {L_{SET*}})$$</div>
-
-ThermSensTransCoef = 0.303\*EXP(-0.036\*ActLevel) + 0.028
-
-PMVET = ThermSensTransCoef\*(IntHeatProd - EvapHeatLossDiff  &
-
-- EvapHeatLossRegComf - RespHeatLoss - DryHeatLossET)
-
-PMVSET = ThermSensTransCoef\*(IntHeatProd - EvapHeatLossDiff  &
-
-- EvapRegHeatLossReg Comf - RespHeatLoss - DryHeatLossSET)
-
-Besides PMV\*, the Pierce Two Node Model uses the indices TSENS and DISC as predictors of thermal comfort. Where TSENS is the classical index used by the Pierce foundation, and is a function of the mean body temperature. DISC is defined as the relative thermoregulatory strain that is needed to bring about a state of comfort and thermal equilibrium. DISC is a function of the heat stress and heat strain in hot environments and equal to TSENS in cold environments. In summary, the Pierce Model, for our purposes, uses four thermal comfort indices; PMVET-a function of ET\*, PMVSET- a function of SET\*, TSENS and DISC.
-
-<span>\({T_{b - c}} = (0.185/58.2)(M - W) + 36.313\)</span>                                    °C
-
-<span>\({T_{b - h}} = (0.359/58.2)(M - W) + 36.664\)</span>                                    °C
-
-<span>\(TSEN{S_c} = 0.68175({T_b} - {T_{b - c}})\)</span>                                                  <span>\({T_b} \le {T_{b - c}}\)</span>
-
-<span>\(TSEN{S_h} = 4.7({T_b} - {T_{b - c}})/({T_{b - h}} - {T_{b - c}})\)</span>                                      <span>\({T_b} > {T_{b - c}}\)</span>
-
-<div>$$DISC = 5.({E_{rsw}} - {E_{rsw - comf}})/({E_{\max }} - {E_{rsw - comf}} - {E_{diff}})$$</div>
-
-AvgBodyTempLow = (0.185/ActLevelConv)\*IntHeatProd + 36.313
-
-AvgBodyTempHigh = (0.359/ActLevelConv)\*IntHeatProd + 36.664
-
-TSENS = .68175\*(AvgBodyTemp-AvgBodyTempLow)
-
-TSENS = 4.7\*(AvgBodyTemp - AvgBodyTempLow)/ &
-
-(AvgBodyTempHigh - AvgBodyTempLow)
-
-DISC = 5.\*(EvapHeatLossRegSweat - EvapHeatLossRegComf)/ &
-
-(MaxEvapHeatLoss - EvapHeatLossRegComf - DiffHeatLoss)
-
-### KSU Two-Node Model
-
-The KSU two-node model, developed at Kansas State University, was published in 1977 (Azer and Hsu 1977). The KSU model is quite similar to that of the Pierce Foundation. The main difference between the two models is that the KSU model predicts thermal sensation (TSV) differently for warm and cold environment.
-
-#### KSU Two Node Model Nomenclature List
-
-Table 83.  Nomenclature list for KSU Two-Node model
-
-<table class="table table-striped">
-
-
-
-
-
-
-
-
-<tr>
-<td>Mathematical variable</td>
-<td>Description</td>
-<td>Units
- </td>
-<td>Range</td>
-<td>FORTRAN variable</td>
-</tr>
-<tr>
-<td>C<sub>cr</sub></td>
-<td>Specific heat of body core</td>
-<td>Whr/kg°C</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>C<sub>sk</sub></td>
-<td>Specific heat of skin</td>
-<td>Whr/kg°C</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>C<sub>res</sub></td>
-<td>The rate of dry respiratory heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>DryRespHeatLoss</td>
-</tr>
-<tr>
-<td>E<sub>dif</sub></td>
-<td>The rate of heat loss from the diffusion of water vapor through the skin</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>EvapHeatLossDiff</td>
-</tr>
-<tr>
-<td>E<sub>max</sub></td>
-<td>Maximum evaporative heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>EvapHeatLossMax</td>
-</tr>
-<tr>
-<td>E<sub>sk</sub></td>
-<td>Total evaporative heat loss from skin</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>EvapHeatLoss</td>
-</tr>
-<tr>
-<td>E<sub>sw</sub></td>
-<td>Equivalent evaporation heat loss from the sweat secreted</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>EvapHeatLossSweat</td>
-</tr>
-<tr>
-<td>E<sub>sw.d</sub></td>
-<td>Sweat function for warm and dry skin</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>DrySweatRate</td>
-</tr>
-<tr>
-<td>E<sub>res</sub></td>
-<td>The rate of latent respiratory heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>LatRespHeatLoss</td>
-</tr>
-<tr>
-<td>F<sub>cl</sub></td>
-<td>The Burton thermal efficiency factor for clothing</td>
-<td> </td>
-<td>-</td>
-<td>CloThermEff</td>
-</tr>
-<tr>
-<td>F<sub>pcl</sub></td>
-<td>Permeation efficiency factor for clothing</td>
-<td> </td>
-<td>-</td>
-<td>CloPermeatEff</td>
-</tr>
-<tr>
-<td>H</td>
-<td>Internal heat production rate of an occupant per unit area
-= M - W</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>IntHeatProd</td>
-</tr>
-<tr>
-<td>H</td>
-<td>Combined heat transfer coefficient</td>
-<td>W/m<sup>2</sup>°C</td>
-<td> </td>
-<td>H</td>
-</tr>
-<tr>
-<td>h<sub>c</sub></td>
-<td>Convective heat transfer coefficient</td>
-<td>W/m<sup>2</sup>°C</td>
-<td>-</td>
-<td>Hc</td>
-</tr>
-<tr>
-<td>h<sub>r</sub></td>
-<td>Radiant heat transfer coefficient</td>
-<td>W/m<sup>2</sup>°C</td>
-<td>-</td>
-<td>Hr</td>
-</tr>
-<tr>
-<td>KS</td>
-<td>Overall skin thermal conductance</td>
-<td>W/m<sup>2</sup>°C</td>
-<td> </td>
-<td>ThermCndct</td>
-</tr>
-<tr>
-<td>KS<sub>o</sub></td>
-<td>Skin conductance at thermal neutrality</td>
-<td>W/m<sup>2</sup>°C</td>
-<td> </td>
-<td>ThermCndctNeut</td>
-</tr>
-<tr>
-<td>KS<sub>(-4)</sub></td>
-<td>Skin conductance at thermal sensation very cold</td>
-<td>W/m<sup>2</sup>°C</td>
-<td> </td>
-<td>ThermCndctMin</td>
-</tr>
-<tr>
-<td>M</td>
-<td>Metabolic rate per unit area</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>ActLevel</td>
-</tr>
-<tr>
-<td>M<sub>shiv</sub></td>
-<td>Metabolic heat production due to shivering</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>ShivResponse</td>
-</tr>
-<tr>
-<td>P<sub>a</sub></td>
-<td>Water vapor pressure in ambient air</td>
-<td>Torr</td>
-<td>-</td>
-<td>VapPress</td>
-</tr>
-<tr>
-<td>P<sub>sk</sub></td>
-<td>Saturated water vapor pressure at required skin temperature</td>
-<td>Torr</td>
-<td>-</td>
-<td>SatSkinVapPress</td>
-</tr>
-<tr>
-<td>PT<sub>accl</sub></td>
-<td>The pattern of acclimation</td>
-<td> </td>
-<td> </td>
-<td>AcclPattern</td>
-</tr>
-<tr>
-<td>Q<sub>c</sub></td>
-<td>The rate of convective heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>ConvHeatLoss</td>
-</tr>
-<tr>
-<td>Q<sub>dry</sub></td>
-<td>Sensible heat flow from skin</td>
-<td>W/m<sup>2</sup></td>
-<td> </td>
-<td>DryHeatLoss</td>
-</tr>
-<tr>
-<td>Q<sub>r</sub></td>
-<td>The rate of radiative heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>RadHeatLoss</td>
-</tr>
-<tr>
-<td>Q<sub>res</sub></td>
-<td>The rate of respiratory heat loss</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>RespHeatLoss</td>
-</tr>
-<tr>
-<td>RH</td>
-<td>Relative humidity</td>
-<td> </td>
-<td> </td>
-<td>RelHum</td>
-</tr>
-<tr>
-<td>T<sub>a</sub></td>
-<td>Air temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>AirTemp</td>
-</tr>
-<tr>
-<td>T<sub>cr</sub></td>
-<td>Core or internal temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>CoreTemp</td>
-</tr>
-<tr>
-<td>T<sub>o</sub></td>
-<td>Operative temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>OpTemp</td>
-</tr>
-<tr>
-<td>T<sub>r</sub></td>
-<td>Mean radiant temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>RadTemp</td>
-</tr>
-<tr>
-<td>T<sub>sk</sub></td>
-<td>Skin temperature</td>
-<td>°C</td>
-<td> </td>
-<td>SkinTemp</td>
-</tr>
-<tr>
-<td>TSV</td>
-<td>Thermal sensation vote</td>
-<td> </td>
-<td>-4~4</td>
-<td>TSV</td>
-</tr>
-<tr>
-<td>V</td>
-<td>Relative air velocity</td>
-<td>m/s</td>
-<td>-</td>
-<td>AirVel</td>
-</tr>
-<tr>
-<td>W</td>
-<td>The rate of heat loss due to the performance of work</td>
-<td>W/m<sup>2</sup></td>
-<td>-</td>
-<td>WorkEff</td>
-</tr>
-<tr>
-<td>W</td>
-<td>Skin wettedness</td>
-<td>-</td>
-<td>-</td>
-<td>SkinWet</td>
-</tr>
-<tr>
-<td>W<sub>cr</sub></td>
-<td>Mass of body core per unit body surface</td>
-<td>kg/m<sup>2</sup></td>
-<td> </td>
-<td>-</td>
-</tr>
-<tr>
-<td>w<sub>rsw</sub></td>
-<td>Skin wettedness due to regulatory sweating</td>
-<td> </td>
-<td> </td>
-<td>SkinWetSweat</td>
-</tr>
-<tr>
-<td>w<sub>rsw-o</sub></td>
-<td>Skin wettedness at thermal neutrality</td>
-<td> </td>
-<td> </td>
-<td>SkinWetSweatNeut</td>
-</tr>
-<tr>
-<td>W<sub>sk</sub></td>
-<td>Mass of skin per unit body surface</td>
-<td>kg/m<sup>2</sup></td>
-<td> </td>
-<td>-</td>
-</tr>
-
-</table>
-
-#### Description of the model and algorithm
-
-The KSU two-node model is based on the changes that occur in the thermal conductance between the core and the skin temperature in cold environments, and in warm environments it is based on changes in the skin wettedness.
-
-In this model metabolic heat production is generated in the core which exchanges energy with the environment by respiration and the skin exchanges energy by convection and radiation. In addition, body heat is dissipated through evaporation of sweat and/or water vapor diffusion through the skin. These principles are used in following passive system equations.
-
-<span>\({W_{cr}}{C_{cr}}d{T_{cr}}/dt = M - W - {Q_{res}} - KS({T_{cr}} - {T_{sk}})\)</span>                         W/m<sup>2</sup>
-
-<span>\({W_{sk}}{C_{sk}}d{T_{sk}}/dt = KS({T_{cr}} - {T_{sk}}) - {Q_{dry}} - {E_{sk}}\)</span>                               W/m<sup>2</sup>
-
-Where
-
-<span>\({Q_{res}} = {E_{res}} + {C_{res}} = 0.0023M(44 - {P_{a(torr)}}) + 0.0014M(34 - {T_a})\)</span>               W/m<sup>2</sup>
-
-LatRespHeatLoss = 0.0023\*ActLevelTot\*(44. - VapPress)
-
-DryRespHeatLoss = 0.0014\*ActLevelTot\*(34. - AirTemp)
-
-RespHeatLoss = LatRespHeatLoss + DryRespHeatLoss
-
-<span>\({Q_{dry}} = {Q_c} + {Q_r} = {h_{}}{f_{cl}}{F_{cl}}({T_{sk}} - {T_o})\)</span>                                           W/m<sup>2</sup>
-
-DryHeatLoss = H\*CloBodyRat\*CloThermEff\*(SkinTemp - OpTemp)
-
-<span>\(h = {h_c} + {h_r}\)</span>                                                                               W/m<sup>2</sup>°C
-
-<span>\({h_c} = 8.3\sqrt v \)</span>                                                                              W/m<sup>2</sup>°C
-
-<span>\({h_r} = 3.87 + 0.031{T_r}\)</span>                                                                  W/m<sup>2</sup>°C
-
-H = Hc + Hr
-
-Hc = 8.3\*SQRT(AirVel)
-
-Hr = 3.87 + 0.031\*RadTemp
-
-<span>\({T_o} = ({h_c}{T_a} + {h_r}{T_r})/({h_c} + {h_r})\)</span>                                                      °C
-
-OpTemp = (Hc\*AirTemp + Hr\*RadTemp)/H
-
-and
-
-For <span>\({E_{sw}} \le {E_{\max }}\)</span>, <span>\({E_{sk}} = {E_{sw}} + (1 - {w_{rsw}}){E_{diff}}\)</span>                               W/m<sup>2</sup>
-
-For <span>\({E_{sw}} > {E_{\max }}\)</span>, <span>\({E_{sk}} = {E_{\max }}\)</span>                                                      W/m<sup>2</sup>
-
-<span>\({E_{diff}} = 0.408({P_{sk}} - {P_a})\)</span>                                                             W/m<sup>2</sup>
-
-<span>\({E_{\max }} = 2.2{h_c}{F_{pcl}}({P_{sk}} - {P_a})\)</span>                                                        W/m<sup>2</sup>
-
-EvapHeatLoss = SkinWetSweat\*EvapHeatLossMax+(1. - SkinWetSweat)\*EvapHeatLossDiff
-
-SkinWetSweat = EvapHeatLossDrySweat/EvapHeatLossMax
-
-EvapHeatLossDiff = 0.408\*(SkinVapPress - VapPress)
-
-EvapHeatLossMax = 2.2\*Hc\*(SkinVapPress - VapPress)\*CloPermeatEff
-
-Here, control signals, based on setpoint temperatures in the skin and core, are introduced into passive system equations and these equations are integrated numerically for small time increments or small increments in core and skin temperature. The control signals modulate the thermoregulatory mechanism and regulate the peripheral blood flow, the sweat rate, and the increase of metabolic heat by active muscle shivering. The development of the controlling functions of skin conductance (KS), sweat rate (E<sub>sw</sub>), and shivering (M<sub>shiv</sub>) is based on their correlation with the deviations in skin and core temperatures from their setpoints.
-
-<div>$$\begin{array}{l}KS = 5.3 + [6.75 + 42.45({T_{cr}} - 36.98) + 8.15{({T_{cr}} - 35.15)^{0.8}}({T_{sk}} - 33.8)]\\/[1.0 + 0.4(32.1 - {T_{sk}})]\end{array}$$</div>
-
-SkinCndctDilation = 42.45\*CoreSignalWarmMax &
-
-+ 8.15\*CoreSignalSkinSens\*\*0.8\*SkinSignalWarmMax
-
-SkinCndctConstriction = 1.0 + 0.4\*SkinSignalColdMax
-
-ThermCndct = 5.3+(6.75+SkinCndctDilation)/SkinCndctConstriction
-
-<div>$$\begin{array}{l}{E_{sw}} = \phi  \times [260({T_{cr}} - 36.9) + 26({T_{sk}} - 33.8)]\exp [({T_{sk}} - 33.8)/8.5]\\/[1.0 + 0.05{(33.37 - {T_{sk}})^{2.4}}]\end{array}$$</div>
-
-WeighFac = 260.+70.\*AcclPattern
-
-SweatCtrlFac = 1. + 0.05\*SkinSignalSweatColdMax\*\*2.4
-
-DrySweatRate = ((WeighFac\*CoreSignalSweatMax &
-
-+ 0.1\*WeighFac\*SkinSignalSweatMax) &
-
-\*EXP(SkinSignalSweatMax/8.5))/SweatCtrlFac
-
-Where
-
-<span>\(\phi  = 1.0\)</span>                                                                                    <span>\(w \le 0.4\)</span>
-
-<span>\(\phi  = 0.5 + 0.5\exp [ - 5.6(w - 0.4)]\)</span>                                              <span>\(w > 0.4\)</span>
-
-SweatSuppFac = 1.
-
-SweatSuppFac = 0.5 + 0.5\*EXP(-5.6\*SkinWetSignal)
-
-<span>\({M_{shiv}} = 20(36.9 - {T_{cr}})(32.5 - {T_{sk}}) + 5(32.5 - {T_{sk}})\)</span>                     W/m<sup>2</sup>
-
-ShivResponse = 20.\*CoreSignalShivMax\*SkinSignalShivMax + 5.\*SkinSignalShivMax
-
-In KSU model, two new parameters are introduced and used in correlating thermal sensations with their associated physiological responses. In stead of correlating warm thermal sensations with skin wettedness, it is here correlated with a wettedness factor defined by
-
-<div>$${\varepsilon_{wsw}} = ({w_{rsw}} - {w_{rsw - o}})/(1.0 - {w_{rsw - o}})$$</div>
-
-SkinWetFac = (SkinWetSweat - SkinWetNeut)/(1. - SkinWetNeut)
-
-Where
-
-<div>$${w_{wsw}} = {E_{sw}}/{E_{\max }}$$</div>
-
-<div>$${w_{wsw - o}} = 0.2 + 0.4\{ 1.0 - \exp [ - 0.6(H/58.2 - 1.0)]\} $$</div>
-
-SkinWetSweat = DrySweatRate/EvapHeatLossMax
-
-SkinWetNeut = 0.02 + 0.4\*(1.-EXP(-0.6\*(IntHeatProdMetMax - 1.)))
-
-and instead of correlating cold thermal sensation with the skin temperature, it is here correlated with a factor identified as vasoconstriction factor defined by
-
-<div>$${\varepsilon_{vc}} = (K{S_o} - KS)/(K{S_o} - K{S_{( - 4)}})$$</div>
-
-VasoconstrictFac = (ThermCndctNeut - ThermCndct) &
-
-/(ThermCndctNeut - ThermCndctMin)
-
-Thus, TSV in the cold is a function of a vasoconstriction factor (ε<sub>vc</sub>) as:
-
-<div>$$TSV =  - 1.46 \times {\varepsilon_{vc}} + 3.75 \times {\varepsilon_{vc}}^2 - 6.17 \times {\varepsilon_{vc}}^3$$</div>
-
-TSV = -1.46153\*VasoconstrictFac + 3.74721\*VasoconstrictFac\*\*2 &
-
-                 - 6.168856\*VasoconstrictFac\*\*3
-
-and for the warm environments, TSV is defined as:
-
-<div>$$TSV = [5.0 - 6.56(RH - 0.5)] \times {\varepsilon_{wsw}}$$</div>
-
-TSV = (5. - 6.56\*(RelHum - 0.50))\*SkinWetFac
-
-The KSU model's TSV was developed from experimental conditions in all temperature ranges and from clo levels between .05 clo to 0.7 clo and from activities levels of 1 to 6 mets (Berglund 1978).
-
-**Adaptive Comfort Model**
-
-Adaptive comfort model, intended for use in naturally ventilated buildings, determines the acceptability of indoor conditions given the monthly mean outdoor air temperature and the indoor operative temperature. This is used as an index for occupant adaptation to outdoor conditions, and determines the acceptability of indoor conditions. The model also accounts for people’s clothing adaptation in naturally conditioned spaces by relating the acceptable range of indoor temperatures to the outdoor climate, so it is not necessary to estimate the clothing values for the space. No humidity or air-speed limits are required when this option is used. This section summarizes the adaptive comfort models based on the ASHRAE Standard 55-2010 and CEN 15251. Details are available in the two standards.
-
-**Adaptive Comfort Model Based on ASHRAE Standard 55-2010**
-
-In ASHRAE Standard 55, the monthly mean outdoor air temperature, used in the adaptive comfort model, is defined as the simple running average of the previous thirty daily average outdoor air temperatures.
-
-The model defines two comfort regions: 80% Acceptability, and 90% Acceptability. If the monthly mean outdoor air temperature is not within the specified domain of 10.0 to 33.5C, the model is not applicable.
-
-![](media/image6814.png)
-
-Figure 302. Acceptable operative temperature ranges for naturally conditioned spaces (ASHRAE Standard 55-2010)
-
-The central line of the model (shown in red), or comfort temperature, is defined as
-
-<div>$${T_{ot}} = 0.31\cdot {T_o} + 17.8$$</div>
-
-Where
-
-T<sub>ot</sub> – operative temperature (°C), calculated as the average of the indoor air dry-bulb temperature and the mean radiant temperature of zone inside surfaces
-
-T<sub>o</sub> – monthly mean outdoor air dry-bulb temperature (°C).
-
-If the .stat file is provided for the simulation, T<sub>o</sub> is drawn directly from the daily average temperatures in the .stat file, which provides a value for each month.  If no .stat file is provided, the monthly mean outdoor temperature is a simple running average of the previous thirty daily average temperatures, calculated directly from the weather file (.epw):
-
-<div>$${T_o} = \frac{{\left( {{T_{od - 1}} + {T_{od - 2}} + ... + {T_{od - 30}}} \right)}}{{30}}$$</div>
-
-<div>$${T_o} = (1 - \alpha )\cdot {T_{od - 1}} + \alpha \cdot {T_{od - 1}}$$</div>
-
-<div>$$\alpha  = \frac{{29}}{{30}}$$</div>
-
-T<sub>od-i</sub> is defined as the daily average temperature of the i<sup>th</sup> previous day.
-
-Note that the weather file must be a standard .epw containing a full year of data.
-
-The comfort regions for 80% and 90% acceptability are symmetric about the central line.
-
-90% Acceptability Limits: T<sub>ot</sub> = 0.31\* T<sub>o</sub> + 17.8± 2.5
-
-80% Acceptability Limits: T<sub>ot</sub> = 0.31\* T<sub>o</sub> + 17.8± 3.5
-
-If, using either method, T<sub>o</sub> is less than 10°(C) or greater than 33.5°(C), the model is not applicable.
-
-For a detailed description of this model, please see *ASHRAE Standard 55-2010, Thermal Environmental Conditions for Human Occupancy*.
-
-### Adaptive Comfort Model Based on European Standard EN15251-2007
-
-The EN15251-2007 is similar to ASHRAE 55-2010, but with slightly different curves of the indoor operative temperature and acceptability limits (Fig. 2). The model, intended for use in naturally ventilated buildings, determines the acceptability of indoor conditions given the 7-day weighted mean outdoor air temperature and the indoor operative temperature. The 7-day weighted mean outdoor air temperature (T<sub>rm</sub>) is defined as the weighted running average of the previous 7 daily average outdoor air temperatures.
-
-This weighted running average is calculated from a full annual weather file that must be specified for the simulation. This is used as an index for occupant adaptation to outdoor conditions, and determines the acceptability of indoor conditions. The model also accounts for people’s clothing adaptation in naturally conditioned spaces by relating the acceptable range of indoor temperatures to the outdoor climate, so it is not necessary to estimate the clothing values for the space. No humidity or air-speed limits are required when this option is used. The model defines three comfort regions: Category I (90%) Acceptability, Category II (80%) Acceptability, and Category III (65%) Acceptability. If T<sub>rm</sub> is not within the specified domain of 10.0 to 30.0C, the model is not applicable.
-
-![](media/image6819.png)
-
-Figure 303. Categories for European Standard EN15251-2007
-
-
-
-![](media/image6820.png)
-
-Figure 304. Acceptable operative temperature ranges for naturally conditioned spaces (CEN EN15251-2007)
-
-Central line (shown as redFigure 304): Tot = 0.33\*To + 18.8
-
-Category I, 90% Acceptability Limits: Tot = 0.33\*To + 18.8± 2.0
-
-Category II, 80% Acceptability Limits: Tot = 0.33\*To + 18.8± 3.0
-
-Category III, 65% Acceptability Limits: Tot = 0.33\*To + 18.8± 4.0
-
-For 10°(C) &lt; T<sub>rm</sub> &lt; 15°(C), the comfort temperature of the lower boundaries of the comfort regions is T<sub>comf</sub> = 23.75°(C). That is, the lower boundaries are constant according to the same ranges above:
-
-Category I, 90% Acceptability Limits: Tot = 23.75- 2.0
-
-Category II, 80% Acceptability Limits: Tot = 23.75 - 3.0
-
-Category III, 65% Acceptability Limits: Tot = 23.75 -4.0
-
-Where
-
-Tot – operative temperature (°C) , calculated as the average of the indoor air dry-bulb temperature and the mean radiant temperature of zone inside surfaces
-
-To – mean outdoor air dry-bulb temperature (°C), calculated as the weighted mean of the previous 7-day daily mean outdoor air dry-bulb temperature (T<sub>od</sub>):
-
-T<sub>o</sub> = (1 - α)\*{T<sub>od-1</sub> + α \*T<sub>od-2</sub> + α<sup>2</sup> \*T<sub>od-3</sub> + α<sup>3</sup> \*T<sub>od-4</sub> + α<sup>4</sup> \*T<sub>od-5</sub> + α<sup>5</sup> \*T<sub>od-6</sub> + α<sup>6</sup> \*T<sub>od-7</sub>}
-
-T<sub>o</sub> = (1 - α)\*T<sub>od-1</sub> + α \*T<sub>o-1</sub>
-
-α  = 0.8
-
-### Dynamic Clothing Model
-
-In most building energy simulations, thermal comfort condition is calculated based on the assumption that the clothing insulation is equal to a constant value of 0.5 clo during the cooling season and 1.0 clo during heating season. Usually those two values are used and the change from 0.5 to 1 or vice-versa is made suddenly from one day to another. In addition, there is no standardized guideline on how to set clothing insulation schedules in the international standards. This simplified assumption may lead to systems that are incorrectly sized and operated and to the incorrect assessment of comfort conditions. In reality, occupants frequently adjust their clothing depending on the thermal conditions around them, as opposed to the assumption of constant clothing values. Therefore, the clothing insulation variation should be captured during the building simulation to realistically model HVAC systems. In order to overcome the limitations of the constant clothing insulation assumption, three new predictive clothing insulation models were developed by Schiavon and Lee (2012) based on 6,333 selected observations taken from ASHRAE RP-884 and RP-921 databases. The first and third models vary the clothing insulation as a function of outdoor air temperature measured at 6 o’clock and the second model takes into account both 6 o’clock outdoor air temperature and indoor operative temperature when adjusting the clothing insulation. The dynamic clothing models should be implemented in dynamic building energy simulation.
-
-The model proposed to ASHRAE 55 is described below.
-
-For t<sub>a(out,6) </sub> &lt; -5°C, <span>\({I_{cl}} = 1\)</span>.00
-
-For -5°C ≤ t<sub>a(out,6)</sub> &lt; 5°C, <span>\({I_{cl}} = 0.818 - 0.0364{\rm{*}}{t_{a\left( {out,6} \right)}}\)</span>
-
-For 5°C ≤ t<sub>a(out,6)</sub> &lt; 26°C <span>\({I_{cl}} = {10^{\left( { - 0.1635 - 0.0066{\rm{*}}{t_{a\left( {out,6} \right)}}} \right)}}\)</span>
-
-or t<sub>a(out,6)</sub> ≥ 26°C <span>\({I_{cl}} = 0.46\)</span>
-
-Where, *I<sub>cl</sub>* is the clothing insulation value, *t<sub>a(out,\\ 6)</sub>* is the outdoor air temperature measured at 6 o’clock in the morning. The following figure illustrates the proposed clothing insulation model.
-
-![](media/image6825.png)
-
-Figure 305. Clothing Schedule Illustration
-
-In the figure above, clothing insulation schedule for a fixed model (blue) typically used in energy simulation software and for the clothing model based on outdoor air temperature measured at 6 o’clock. Climate data for Chicago O’hare International Airport has been used.
-
-The following figure illustrates the new clothing insulation model.
-
-![](media/image6826.png)
-
-Figure 306. Graphical representation of the proposed clothing insulation model
-
-The dynamic predictive clothing insulation model is implemented into EnergyPlus for realistic energy simulation. Addenda A to ASHRAE 55 with the clothing model has been approved by the ASHRAE committee and the chance to be included in ASHRAE 55-2013 is high.
-
-#### References
-
-Schiavon S, Lee KH. 2013. Dynamic predictive clothing insulation models based on outdoor air and indoor operative temperatures. Building and Environment. Volume 59, 250-260. [http://dx.doi.org/10.1016/j.buildenv.2012.08.024](http://dx.doi.org/10.1016/j.buildenv.2012.08.024)  (link to the journal) [http://escholarship.org/uc/item/3338m9qf](http://escholarship.org/uc/item/3338m9qf)  (link to the freely available pre-print version)
-
-Lee KH, Schiavon S. 2013. Influence of three dynamic predictive clothing insulation models on building energy use, HVAC sizing and thermal comfort. Submitted to Journal. [http://escholarship.org/uc/item/3sx6n876](http://escholarship.org/uc/item/3sx6n876)  (link to the freely available pre-print version)
-
-### Mean Radiant Temperature Calculation
-
-There are three options to calculate mean radiant temperature in the thermal comfort models. One is the zone averaged MRT, another is the surface weighted MRT, and the other is angle factor MRT. The zone averaged MRT is calculated on the assumption that a person is in the center of a space, whereas the surface weighted MRT is calculated in consideration of the surface that a person is closest to, and the angle factor MRT is calculated based on angle factors between a person and the different surfaces in a space. Here, the surface weighted MRT is the average temperature of the selected surface and zone averaged MRT and is intended to represent conditions in the limit as a person gets closer and closer to a particular surface.  In that limit, half of the person’s radiant field will be dominated by that surface and the other half will be exposed to the rest of the zone.  Note that the surface weighted MRT is only an approximation. The angle factor MRT is the mean temperature of the surrounding surface temperatures weighted according to the magnitude of the respective angle factors and allows the user to more accurately predict thermal comfort at a particular location within a space.
-
-Table 84.  Nomenclature and variable list for MRT calculation
-
-<table class="table table-striped">
-
-
-
-
-
-
-
-
-<tr>
-<td>Mathematical variable</td>
-<td>Description</td>
-<td>Units
- </td>
-<td>Range</td>
-<td>FORTRAN variable</td>
-</tr>
-<tr>
-<td>T<sub>r</sub></td>
-<td>Mean radiant temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>RadTemp</td>
-</tr>
-<tr>
-<td>T<sub>r-avg</sub></td>
-<td>Zone averaged radiant temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>ZoneRadTemp</td>
-</tr>
-<tr>
-<td>T<sub>surf</sub></td>
-<td>Surface temperature</td>
-<td>°C</td>
-<td>-</td>
-<td>SurfaceTemp</td>
-</tr>
-<tr>
-<td>F<sub>surf</sub></td>
-<td>Angle factor between person and surface</td>
-<td>-</td>
-<td>0~1</td>
-<td>AngleFactor</td>
-</tr>
-
-</table>
-
-#### Description of the model and algorithm
-
-The zone averaged MRT is calculated without weighting any surface temperature of the space.
-
-<div>$${T_r} = {T_{r - avg}}$$</div>
-
-RadTemp = MRT(ZoneNum)
-
-The surface weighted MRT is the average temperature of the zone averaged MRT and the temperature of the surface that a person is closest to.
-
-<div>$${T_r} = ({T_{r - avg}} + {T_{surf}})/2$$</div>
-
-ZoneRadTemp = MRT(ZoneNum)
-
-SurfaceTemp = GetSurfaceTemp(People(PeopleNum)%SurfacePtr)
-
-RadTemp = (ZoneRadTemp + SurfaceTemp)/2.0
-
-The angle factor MRT is the mean value of surrounding surface temperatures weighted by the size of the respective angle factors between a person and each surface.
-
-<div>$${T_r} = {T_{surf - 1}}{F_{surf - 1}} + {T_{surf - 2}}{F_{surf - 2}} + ......... + {T_{surf - n}}{F_{surf - n}}$$</div>
-
-SurfTempAngleFacSummed = SurfTempAngleFacSummed &
-
-+ SurfaceTemp \* AngleFactorList(AngleFacNum)%AngleFactor(SurfNum)
-
-RadTemp = SurfTempAngleFacSummed
-
-### References
-
-ASHRAE. 1984. “High Intensity Infrared Radiant Heating�, 1984 Handbook of Systems and Equipment, American Society of Heating, Refrigerating and Air Conditioning Engineers, Atlanta, GA, Chapter 18.
-
-ASHRAE. 1985. “Physiological Principles for Comfort and Health,� 1985 Handbook of Fundamentals, American Society of Heating, Refrigerating and Air Conditioning Engineers, Atlanta, GA, Chapter 8.
-
-ASHRAE. 1993. “Physiological Principles and Thermal Comfort�, 1993 ASHRAE Handbook of Fundamentals, American Society of Heating, Refrigerating and Air Conditioning Engineers, Atlanta, GA, Chapter 8.
-
-ASHRAE. 2010. “Standard 55-2010 -- Thermal Environmental Conditions for Human Occupancy (ANSI approved)�, American Society of Heating, Refrigerating and Air Conditioning Engineers, Atlanta, GA.
-
-Azer, N.Z., Hsu, S. 1977. “The prediction of Thermal Sensation from Simple model of Human Physiological Regulatory Response�, ASHRAE Trans., Vol.83, Pt 1.
-
-Berglund, Larry. 1978. “Mathematical Models for Predicting the Thermal Comfort Response of Building Occupants�, ASHRAE Trans., Vol.84.
-
-Doherty, T.J., Arens, E. 1988. “Evaluation of the Physiological Bases of Thermal Comfort Models�, ASHRAE Trans., Vol.94, Pt 1.
-
-Du Bois, D. and E.F. 1916. “A Formula to Estimate Approximate Surface Area, if Height and Weight are Known�, Archives of internal Medicine, Vol.17.
-
-CEN. 2007. “Standard EN15251 Indoor environmental input parameters for design and assessment of energy performance of buildings addressing indoor air quality, thermal environment, lighting and acoustics�. Bruxelles: European committee for Standardisation.
-
-Fanger, P.O. 1970. Thermal Comfort-Analysis and Applications in Environmental Engineering, Danish Technical Press, Copenhagen.
-
-Fanger, P.O. 1986. “Radiation and Discomfort�, ASHRAE Journal. February 1986.
-
-Fanger P.O. 1967. “Calculation of Thermal Comfort: Introduction of a Basic Comfort Equation�, ASHRE Trans., Vol.73, Pt 2.
-
-Fountain, Marc.E., Huizenga, Charlie. 1997 “A Thermal Sensation Prediction Tool for Use by the Profession�, ASHRAE Trans., Vol.103, Pt 2.
-
-Gagge, A.P., Stolwijk, J. A. J., Nishi, Y. 1970. “An Effective Temperature Scale Based on a Simple Model of Human Physiological Regulatory Response�, ASHRAE Trans., Vol.70, Pt 1.
-
-Gagge, A.P., Fobelets, A.P., Berglund, L. G. 1986. “A Standard Predictive Index of Human Response to the Thermal Environment�,  ASHRAE Trans., Vol.92, Pt 2.
-
-Hsu, S. 1977. “A Thermoregulatory Model for Heat Acclimation and Some of its Application�, Ph. D. Dissertation, Kansas State University.
-
-Int-Hout, D. 1990. “Thermal Comfort Calculation / A Computer Model�, ASHRAE Trans., Vol.96, Pt 1.
-
-ISO. 1983. “Determination of the PMV and PPD Indices and Specification of the Conditions for Thermal Comfort�, DIS 7730, Moderate Thermal Environment, 1983.
-
-Trombe Walls <a name="TrombeWalls"></a>
-------------
-
-Trombe walls are passive solar devices designed for thermal storage and delivery.  It consists of a thick wall (150mm to 300mm) [8" to 16"] faced with a selective surface solar absorber, air gap, and high transmissivity glass pane.  Trombe walls are usually South facing (in the Northern Hemisphere) for maximum sun exposure.  An overhang above the wall is used to decrease exposure in the summer when the sun is high in the sky and heating is not required, yet still allows for full exposure in the winter when the sun is low in the sky and heating is desirable.
-
-In EnergyPlus, there is no Trombe wall object per se; rather, it is composed of other existing EnergyPlus objects in the input file (except for a special key choice for Zone Inside Convection Algorithm in the Zone input object).  This approach provides flexibility in specifying the various wall parameters and allows the freedom to explore unusual configurations.  On the other hand, this approach puts more of a burden on the user to be sure that all parts of the Trombe wall are correctly specified; otherwise unexpected results may be obtained.
-
-To simulate the Trombe wall, a very narrow zone is coupled to the desired surface via an interzone partition.  The depth of the zone corresponds to the size of the air space usually 18mm to 150mm (¾" to 6").  In most cases the Trombe zone will be a sealed zone with no ventilation.  The exterior wall of the Trombe zone contains a single or double-pane window.  Optimally, the window covers nearly all of the wall area and has a very high transmissivity to allow the maximum amount of solar flux into the Trombe zone.  Frames and dividers can be defined as usual for the window.  The interior wall is usually constructed of very thick masonry materials with a solar absorber surface as the innermost layer of the wall.  The absorber is a selective surface material with very high absorptivity and very low emissivity, e.g. copper with a special black surface treatment.  It is important to make sure the Solar Distribution field in the **Building** object is set to FullInteriorAndExterior so that the majority of the solar flux is directed on the absorber surface and not just on the very small area of the Trombe zone floor.  The Zone Inside Convection Algorithm for the Trombe’s Zone object should also be set to TrombeWall to correctly model the air space.  As is the case for all interzone partitions, the wall construction of the adjoining zone must be the mirror image of the wall construction in the Trombe zone.  Finally, an overhang is optionally attached to the Trombe zone to control the amount of seasonal sun exposure.  Since the user selects all of the Trombe wall parameters in the input file, there is considerable freedom to experiment with different materials, sizes, and configurations.
-
-
-
-![](media/image6830.png)
-
-Figure 307. Building with Trombe Wall
-
-
-
-### Passive Trombe Wall
-
-Passive Trombe walls perform without the assistance of any additional mechanical equipment.  Most Trombe walls are passive Trombe walls.  They can be either sealed or naturally ventilated.
-
-For a sealed or unvented Trombe wall, the *Zone Inside Convection Algorithm* field in the Zone object should be set to "TrombeWall".  This algorithm correctly calculates the convection coefficients for a narrow sealed vertical cavity based on the ISO 15099 standard.  Refer to the "Trombe Wall Algorithm" subsection (under Interior Convection, above) for a complete description of the algorithm.  The EnergyPlus modeling approach for the sealed passive Trombe wall has been validated with experimental data (Ellis 2003).
-
-For a naturally ventilated Trombe wall, there is no built-in algorithm for calculating the correct convection coefficients on the inside of the cavity walls.  One option is to use the "Detailed" convection algorithm.  This algorithm takes into account some natural convection effects but is intended for a normal sized room.  Therefore, some error may be incurred when used with a narrow cavity.  Another option is to use the SurfaceProperty:ConvectionCoefficients object to schedule coefficients that have been determined beforehand by the user.
-
-#### Input File
-
-An input file (PassiveTrombeWall.idf) is provided to demonstrate a sample sealed Trombe wall implementation.  In this file two separated fictional buildings are simulated for summer and winter design days in Zion, Utah.  The buildings are identical in size and construction except that one has a Trombe wall and the other does not.  The buildings have uncontrolled zones with no internal loads and heavy insulation.  All floors use interzone partitions to disconnect them from the ground.  The window on the Trombe zone is a 3 mm, low iron, single pane glazing with very high transmissivity (0.913 visible, 0.899 solar).  The absorber surface is a Tabor solar absorber with an emittance of 0.05 and absorptance of 0.85.
-
-#### Results
-
-The resulting temperature profiles for winter and summer design days are plotted below.
-
-![](media/image6831.png)
-
-Figure 308. Passive Trombe Wall Winter
-
-
-
-![](media/image6832.png)
-
-Figure 309. Passive Trombe Wall Summer
-
-#### References
-
-Ellis, Peter G.  2003.  *Development and Validation of the Unvented Trombe Wall Model in EnergyPlus*, Master's Thesis, University of Illinois at Urbana-Champaign.
-
-ISO 15099.  2000.  "Thermal Performance of Windows, Doors, and Shading Devices-Detailed Calculations".  International Standards Organization, Draft, July 18, 2000.
-
-
-
-### Active Trombe Wall
-
-The active Trombe wall is the same as the passive Trombe wall with the addition of a simple fan system to circulate air between the Trombe zone and the main zone.  The fan is scheduled to operate only during winter daylight hours to improve the heat transfer from the Trombe zone.
-
-As with the passive Trombe wall, there is no EnergyPlus object for the active Trombe wall; it is simulated using a collection of other EnergyPlus objects.  Like the passive Trombe wall, the active Trombe wall uses a narrow zone coupled to the main zone with interzone partitions.  However, the unique part of the active Trombe wall is that the Trombe zone is used to define a zone supply plenum object which allows the Trombe zone to be integrated into the air system.  A constant volume fan is the main component of the air system.  To make the zone connections, the Direct Air component is used.
-
-For the active Trombe wall, there is no built-in algorithm for calculating the correct convection coefficients due to forced convection on the inside of the cavity walls.  One approach is to use the SurfaceProperty:ConvectionCoefficients object to schedule coefficients that have been determined beforehand by the user.
-
-#### Input File
-
-An input file (ActiveTrombeWall.idf) is provided to demonstrate a sample active Trombe wall implementation.  The building and Trombe wall in this file are identical to the ones described above for PassiveTrombeWall.idf.  However, this input file adds a system in the form of a low flow rate (0.1 m<sup>3</sup>/s) constant volume fan and the necessary duct connections.  The fan is scheduled to operate October through March from 10 AM to 8 PM.
-
-#### Results
-
-The resulting temperature profile for the winter design day is plotted below.  The plot for the summer design day is not shown because it is identical to Figure 309 above since the fan is not scheduled to operate in the summer.
-
-![](media/image6833.png)
-
-Figure 310. Active Trombe Wall Winter
-
-Water Thermal Tanks (includes Water Heaters) <a name="WaterTanks"></a>
---------------------------------------------
-
-Water thermal tanks are devices for storing thermal energy in water.  The most common types are water heaters. devices for storing and heating water.  Typical water heater applications are for domestic hot water heating, low-temperature radiant space heating, and energy storage for solar hot water systems or waste heat recovery.  In EnergyPlus, water heater objects can be coupled to a plant loop simulation or used stand-alone.  There are also chilled water storage tanks that can be used to hold cold water
-
-### Mixed Water Thermal Tank
-
-The input object WaterHeater:Mixed provides a model that simulates a well-mixed water tank, i.e. non-stratified, and is appropriate for simulating many types of water heaters and storage tanks, including gas and electric residential water heaters, a variety of large commercial water heaters, and also instantaneous, tankless water heaters.  This model is used for both the mixed water heater and the mixed chilled water storage tanks.
-
-#### Energy Balance
-
-The well-mixed assumption implies that all water in the tank is at the same temperature.  To calculate the water temperature, the model analytically solves the differential equation governing the energy balance of the water tank:
-
-<div>$$\rho V{c_p}\frac{{dT}}{{dt}} = {q_{net}}$$</div>
-
-where
-
-*r* = density of water
-
-*V* = volume of the tank
-
-*c<sub>p</sub>* = specific heat of water
-
-*T* = temperature of the tank water
-
-*t* = time
-
-*q<sub>net</sub>* = net heat transfer rate to the tank water
-
-The density and volume can be replaced with the total mass *m* of water in the tank to get:
-
-<div>$$m{c_p}\frac{{dT}}{{dt}} = {q_{net}}$$</div>
-
-The net heat transfer rate *q<sub>net</sub>* is the sum of gains and losses due to multiple heat transfer pathways.
-
-<div>$${q_{net}} = {q_{heater}} + {q_{oncycpara}} + {q_{offcycpara}} + {q_{oncycloss}} + {q_{offcycloss}} + {q_{use}} + {q_{source}}$$</div>
-
-where
-
-*q<sub>heater</sub>* = heat added by the heating element or burner
-
-*q<sub>oncycpara</sub>* = heat added due to on-cycle parasitic loads (zero when off)
-
-*q<sub>offcycpara</sub>* = heat added due to off-cycle parasitic loads (zero when on)
-
-*q<sub>oncycloss</sub>* = heat transfer to/from the ambient environment (zero when off)
-
-*q<sub>offcycloss</sub>* = heat transfer to/from the ambient environment (zero when on)
-
-*q<sub>use</sub>* = heat transfer to/from the use side plant connections
-
-*q<sub>source</sub>* = heat transfer to/from the source side plant connections
-
-*q<sub>oncycloss</sub>* and *q<sub>offcycloss</sub>* are defined as:
-
-<div>$${q_{oncycloss}} = U{A_{oncyc}}\left( {{T_{amb}} - T} \right)$$</div>
-
-<div>$${q_{offcycloss}} = U{A_{offcyc}}\left( {{T_{amb}} - T} \right)$$</div>
-
-where
-
-*UA<sub>oncyc</sub>* = on-cycle loss coefficient to ambient environment (zero when off)
-
-*UA<sub>offcyc</sub>* = off-cycle loss coefficient to ambient environment (zero when on)
-
-*T<sub>amb</sub>* = temperature of ambient environment
-
-*q<sub>use</sub>*, and *q<sub>source</sub>* are defined as:
-
-<div>$${q_{use}} = {\varepsilon_{use}}{\dot m_{use}}{c_p}\left( {{T_{use}} - T} \right)$$</div>
-
-<div>$${q_{source}} = {\varepsilon_{source}}{\dot m_{source}}{c_p}\left( {{T_{source}} - T} \right)$$</div>
-
-where
-
-*e<sub>use</sub>* = heat exchanger effectiveness for the use side plant connections
-
-<span>\({\dot m_{use}}\)</span>= mass flow rate for the use side plant connections
-
-*T<sub>use</sub>* = inlet fluid temperature of the use side plant connections
-
-*e<sub>source</sub>* = heat exchanger effectiveness for the source side plant connections
-
-<span>\({\dot m_{source}}\)</span>= mass flow rate for the source side plant connections
-
-*T<sub>source</sub>* = inlet fluid temperature of the use side plant connections
-
-Incorporating all of these equations into the original differential equation,
-
-<div>$$\begin{array}{c}m{c_p}\frac{{dT}}{{dt}} = {q_{heater}} + {q_{oncyc}} + {q_{offcyc}} + U{A_{oncyc}}\left( {{T_{amb}} - T} \right) + U{A_{offcyc}}\left( {{T_{amb}} - T} \right)\\ + {\varepsilon_{use}}{{\dot m}_{use}}{c_p}\left( {{T_{use}} - T} \right) + {\varepsilon_{source}}{{\dot m}_{source}}{c_p}\left( {{T_{source}} - T} \right)\end{array}$$</div>
-
-Associating terms not dependent on temperature *T* and terms dependent on temperature *T* yields:
-
-<div>$$\begin{array}{c}\frac{{dT}}{{dt}} = \left[ {\frac{1}{{m{c_p}}}\left( \begin{array}{l}{q_{heater}} + {q_{oncyc}} + {q_{offcyc}} + U{A_{oncyc}}{T_{amb}} + U{A_{offcyc}}{T_{amb}}\\ + {\varepsilon_{use}}{{\dot m}_{use}}{c_p}{T_{use}} + {\varepsilon_{source}}{{\dot m}_{source}}{c_p}{T_{source}}\end{array} \right)} \right]\\ + \left[ {\frac{{ - 1}}{{m{c_p}}}\left( {U{A_{oncyc}} + U{A_{offcyc}} + {\varepsilon_{use}}{{\dot m}_{use}}{c_p} + {\varepsilon_{source}}{{\dot m}_{source}}{c_p}} \right)} \right]T\end{array}$$</div>
-
-The differential equation now has the form
-
-<div>$$\frac{{dT}}{{dt}} = a + bT$$</div>
-
-where
-
-<div>$$a = \frac{1}{{m{c_p}}}\left( \begin{array}{l}{q_{heater}} + {q_{oncyc}} + {q_{offcyc}} + U{A_{oncyc}}{T_{amb}} + U{A_{offcyc}}{T_{amb}}\\ + {\varepsilon_{use}}{{\dot m}_{use}}{c_p}{T_{use}} + {\varepsilon_{source}}{{\dot m}_{source}}{c_p}{T_{source}}\end{array} \right)$$</div>
-
-<div>$$b = \frac{{ - 1}}{{m{c_p}}}\left( {U{A_{oncyc}} + U{A_{offcyc}} + {\varepsilon_{use}}{{\dot m}_{use}}{c_p} + {\varepsilon_{source}}{{\dot m}_{source}}{c_p}} \right)$$</div>
-
-The solution to the differential equation can be written in terms of *a* and *b* as:
-
-<div>$$T\left( t \right) = \left( {\frac{a}{b} + {T_i}} \right){e^{bt}} - \frac{a}{b}$$</div>
-
-where
-
-*T(t)* = temperature of the tank water at time *t*
-
-*T<sub>i</sub>* = initial temperature of the tank water at time *t* = 0
-
-However, if *b* = 0, the solution instead is:
-
-<div>$$T\left( t \right) = at + {T_i}$$</div>
-
-Since the control algorithm must sometimes calculate the time needed to reach a specified temperature, the equations above can also be rearranged to solve for *t*.
-
-<div>$$t = \frac{1}{b}\ln \left( {\frac{{{\raise0.7ex\hbox{$a$} \!\mathord{\left/ {\vphantom {a b}}\right.}\!\lower0.7ex\hbox{$b$}} + {T_f}}}{{{\raise0.7ex\hbox{$a$} \!\mathord{\left/ {\vphantom {a b}}\right.}\!\lower0.7ex\hbox{$b$}} + {T_i}}}} \right)$$</div>
-
-or, if *b* = 0,
-
-<div>$$t = \frac{{{T_f} - {T_i}}}{a}$$</div>
-
-where
-
-*T<sub>f</sub>* = final temperature of the tank water at time t.
-
-In the special case where *b* = 0 and *a* = 0, and *T<sub>f</sub>* &lt;&gt; *T<sub>i</sub>*, the time *t* is infinity.
-
-#### Water Heater Control Algorithm
-
-For water heaters, control options allow the heater to cycle or modulate to meet the load.  When cycling, the heater element or burner is either on or off.  The heater remains fully on while heating the tank up to the setpoint temperature.  When the setpoint is reached, the heater turns off.  The heater remains off until the tank temperature falls below the "cut-in" temperature, i.e., the setpoint temperature minus the deadband temperature difference.  The heater continuously cycles on and off to maintain the tank temperature within the deadband.  Most storage-tank water heaters cycle.
-
-When modulating, the heater power varies between the maximum and minimum heater capacities.  The heater stays on as long as the required total demand is above the minimum capacity.  Below the minimum capacity, the heater will begin to cycle on and off based on the deadband temperature difference.  Most tankless/instantaneous water heaters modulate.
-
-Within a time step, the differential equation is solved separately for when the heater element or burner is "on" (on-cycle) and when it is "off" (off-cycle).  This approach allows ambient losses and parasitic loads to be divided into on-cycle and off-cycle effects and accounted for in detail.
-
-An illustration of how the control algorithm cycles on and off is shown below.  Ambient losses cool the tank temperature until the bottom of the deadband is reached (50 C) at which point the heater cycles on and reheats the tank back to the setpoint (60 C).  A water draw causes hot water to be replaced with cold water from the water mains.  The incoming cold water rapidly cools the tank.  In this example the heater cannot keep up with the water draw and the tank temperature continues to drop until the water draw ends.
-
-Although the instantaneous tank water temperature may vary considerably within a timestep (due to cycling, etc.), only the average temperature over the timestep is reported.  The model calculates the average by piece-wise integration of the area under the instantaneous temperature curve for each unique set of conditions.  The instantaneous temperature is preserved internally by the program and is propogated from the end of one timestep to the beginning of the next.
-
-![](media/image6852.png)
-
-Figure 311. Water Heater Cycle Control Algorithm
-
-#### Chilled Water Tank Control Algorithm
-
-The input objects ThermalStorage:ChilledWater:Mixed and ThermalStorage:ChilledWater:Stratified provide chilled water tank models that do not include active cooling elements, there is only indirect cooling by remote devices such as a chiller.  The tank’s setpoint controls are used to determine if flow is to be requested through the source side of the tank.  The setpont and deadband control scheme is similar to the water heater but the logic is flipped around for cooling instead of heating.  The setpoint temperatue is the “cut-out� temperature and the setpoint plus deadband is the “cut-in� temperature.  If the tank temperature ( or tank sensing node for stratified tanks) is above the “cut-in� temperature, then flow is requested.  If temperatures are below the “cut-out� temperature, then flow is not requested.  The chilled water tanks also have separate availability schedules for the use side and source side for additional control options.
-
-#### Standard Ratings
-
-For water heaters, the industry standard ratings of Recovery Efficiency and Energy Factor are calculated according to the 10CFR430 test procedure.  To emulate the test procedure, a 24-hour simulation of the water heater is performed internally using the specified test conditions:
-
-n Setpoint Temperature = 57.2 C (135 F)
-
-n Ambient Temperature = 19.7 C (67.5 F)
-
-n Ambient Relative Humidity = 50% (used for heat pump water heaters)
-
-n Inlet Temperature (Water Mains) = 14.4 C (58 F)
-
-For heat pump water heaters, the water heater tank’s heating element and water heater tank parasitic loads are disabled and the user-defined water heating capacity, energy use, and parasitic loads for the heat pump are used to calculate Recovery Efficiency and Energy Factor.
-
-The simulated test procedure performs six equal draws of approximately 0.041 m<sup>3</sup> (10.7 gal) in each of the first six hours of the simulation.  Each draw occurs over the first timestep of the hour.
-
-The Recovery Efficiency is calculated when the water heater recovers to the setpoint after the first draw.
-
-<div>$$RE = \frac{{{m_1}{c_p}\left( {57.2 - 14.4} \right)}}{{{E_1}}}$$</div>
-
-where
-
-*m<sub>1</sub>* = water mass of the first draw
-
-*c<sub>p</sub>* = specific heat of water
-
-*E<sub>1</sub>* = fuel energy consumed until the setpoint is recovered (including parasitics)
-
-Note: When the standards rating for a heat pump water heater is calculated, the fuel energy consumed refers to the total energy consumed by the heat pump compressor, evaporator fan, condenser pump, and parasitic loads. It is assumed that the parasitic loads for a heat pump water heater do not contribute to heating the water (ref. Heat Pump Water Heater).
-
-The Energy Factor is calculated at the end of the 24-hour simulation period.
-
-<div>$$EF = \frac{{{m_{total}}{c_p}\left( {57.2 - 14.4} \right)}}{{{E_{total}}}}$$</div>
-
-where
-
-*m<sub>total</sub>* = total water mass of all six draws
-
-*c<sub>p</sub>* = specific heat of water
-
-*E<sub>total</sub>* = total fuel energy consumed over 24 hours (including parasitics)
-
-Under certain input parameters, the rating method will not succeed and a warning message will be generated.  Problems occur when inputs do not allow the tank to recover to the setpoint temperature within the test period.  This can occur if the maximum heater capacity is undersized, or if the deadband temperature difference is large enough that the first draw of the test does not trigger the heater to come on.  In either case, the Recovery Efficiency test will not compute properly because recovery to the setpoint was not achieved.
-
-#### References
-
-10CFR430.  *Title 10, Code of Federal Regulations, Part 430 - Energy Conservation Program for Consumer Products, Appendix E to Subpart B - Uniform Test Procedure for Measuring the Energy Consumption of Water Heaters*.
-
-### Heat Pump Water Heater
-
-#### Overview
-
-The input objects `WaterHeater:HeatPump:*` provide models for a heat pump water heater (HPWH) that is a compound object consisting of a water heater tank (e.g., `WaterHeater:Mixed` or `WaterHeater:Stratified`), a direct expansion (DX) “coil� (i.e., an air-to-water DX compression system which includes a water heating coil, air coil, compressor, and water pump), and a fan to provide air flow across the air coil associated with the DX compression system. These objects work together to model a system which heats water using zone air, outdoor air, or a combination of zone and outdoor air as the primary heat source.
-
-There are two types of heat pump water heater models available:
-
-1. `WaterHeater:HeatPump:PumpedCondenser`: This model is used to represent a heat pump water heater where water is removed from the tank, pumped through a condenser, and returned to the tank at a higher temperature. 
-2. `WaterHeater:HeatPump:WrappedCondenser`: This model is used for heat pump water heaters that are more typical in the residential building context where the heating coil is wrapped around or submerged in the tank.
-
-Each type of `WaterHeater:HeatPump:*` object is compatible with certain `Coil:WaterHeating:AirToWaterHeatPump:*` objects as shown in the following table:
-
-<table class="table table-striped">
-  <tr>
-    <th>WaterHeater:HeatPump:*</th>
-    <th>Coil:WaterHeating:AirToWaterHeatPump:*</th>
-  </tr>
-  <tr>
-    <td rowspan="2">PumpedCondenser</td>
-    <td>Pumped</td>
-  </tr>
-  <tr>
-    <td>VariableSpeed</td>
-  </tr>
-  <tr>
-    <td>WrappedCondenser</td>
-    <td>Wrapped</td>
-  </tr>
-</table>
-
-Additionally the `WaterHeater:HeatPump:WrappedCondenser` object is only compatible with stratified tanks. Therefore `WaterHeater:HeatPump:*` has the following tank compatibility matrix:
-
-<table class="table table-striped">
-  <tr>
-    <th rowspan="2">WaterHeater:HeatPump:*</th>
-    <th colspan="2">WaterHeater:*<br></th>
-  </tr>
-  <tr>
-    <th>Mixed</th>
-    <th>Stratified</th>
-  </tr>
-  <tr>
-    <td>Pumped</td>
-    <td>X</td>
-    <td>X</td>
-  </tr>
-  <tr>
-    <td>Wrapped</td>
-    <td></td>
-    <td>X</td>
-  </tr>
-</table>
-
-Numerous configurations of tank location, inlet air source, and DX coil compressor location can be modeled. The DX coil compressor may be located in a zone, outdoors, or the ambient temperature surrounding the compressor may be scheduled. The location of the compressor controls the operation of its crankcase heater. The water heater tank location is specified in the water heater tank object and is independent of the compressor location. In addition, the inlet air configuration may be specified in one of several ways. The heat pump water heater air coil and fan assembly may draw its inlet air from the zone and outdoor air using an optional mixer and splitter assembly as shown in the first figure below. When used, the mixer and splitter air streams are controlled by a single inlet air mixer schedule. When the HPWH draws its inlet air solely from a zone, the mixer/splitter assembly is not required as shown in the second figure below. In this case, the inlet air to the evaporator and fan assembly is made up entirely of zone air and the heat pump outlet air is directed back to the zone. The final figure illustrates a HPWH that draws its inlet air solely from outdoors and exhausts its outlet air outdoors as well. Each of these configurations may also be connected to a plant hot water loop (via the water heater tank use nodes).
-
-![HPWHSchematic\_EAplusOA](media/image6855.png)
-
-Figure 312. Schematic of a heat pump water heater using optional mixer/splitter nodes
-
-![HPWH](media/image6856.png)
-
-Figure 313. Schematic of a Heat Pump Water Heater with Inlet Air from a Zone
-
-![HPWHSchematic\_outdoors](media/image6857.png)
-
-Figure 314. Schematic of a Heat Pump Water Heater with Inlet Air from Outdoors
-
-Note: The water heater tank location shown in the figures above is completely independent of the heat pump water heater’s inlet air configuration and its compressor location. The water heater tank may be located outdoors, in a zone, or the ambient temperature surrounding the tank can be scheduled as described in the mixed water heater section below.
-
-#### Model Description
-
-The heat pump water heater input requires a compressor setpoint temperature schedule and dead band temperature difference, which are independent from the setpoint temperature schedule and dead band temperature difference for the heater (element or burner) associated with the water heater tank. The cut-in temperature for the heat pump compressor is defined as the heat pump compressor’s setpoint temperature minus its dead band temperature difference.
-
-<div>$${T_{HP,\,cut - in}}\,\, = \,\,{T_{HP,set\,point}}\,\, - \,\,{T_{HP,dead\,band}}$$</div>
-
-where:
-
-<span>\({T_{HP,\,cut - in}}\)</span>     = Cut-in temperature for the heat pump compressor (°C)
-
-<span>\({T_{HP,set\,point}}\)</span>   = Heat pump compressor setpoint temperature (°C)
-
-<span>\({T_{HP,dead\,band}}\)</span> = Heat pump compressor dead band temperature difference (°C)
-
-In this model, the heat pump water heater’s DX compression system is considered the primary heat source and the water tank’s heater (element or burner) provides supplemental heat as necessary. Therefore, the cut-in temperature for the heat pump compressor (setpoint minus dead band temperature difference) is usually higher than the setpoint temperature for the heater (element or burner) in the associated water heater tank object. At times when the water heater tank setpoint temperature is greater than the cut-in temperature of the heat pump compressor, the heat pump compressor is disabled and the tank’s heater is used to heat the water.
-
-The simulation starts by first calculating the air conditions entering the air coil (evaporator)/fan assembly based on the inlet air configuration of the heat pump water heater and the presence of the optional mixer/splitter nodes. When the HPWH draws its inlet air from the zone and outdoors using the optional mixer/splitter nodes (i.e., Inlet Air Configuration = Zone and Outdoor Air), the inlet air conditions are calculated as follows:
-
-<div>$$Frac = GetScheduleValue(MixerInletAirSchedule)$$</div>
-
-<div>$${T_{inlet}} = {T_{outdoor}}\left( {Frac} \right) + {T_{zone}}\left( {1 - Frac} \right)$$</div>
-
-<div>$${\omega_{inlet}} = {\omega_{outdoor}}\left( {Frac} \right) + {\omega_{zone}}\left( {1 - Frac} \right)$$</div>
-
-where:
-
-<span>\(Frac\)</span> = current value of the inlet air mixer schedule (fraction of outdoor air, 0-1)
-
-<span>\({T_{inlet}}\)</span> = inlet air dry-bulb temperature to the HPWH evaporator/fan assembly (°C)
-
-<span>\({T_{outdoor}}\)</span> = outdoor air dry-bulb temperature (°C)
-
-<span>\({T_{zone}}\)</span>  = zone (exhaust) air dry-bulb temperature (°C)
-
-<span>\({\omega_{inlet}}\)</span> = inlet air humidity ratio to the HPWH evaporator/fan assembly (kg/kg)
-
-<span>\({\omega_{outdoor}}\)</span>= outdoor air humidity ratio (kg/kg)
-
-<span>\({\omega_{zone}}\)</span>  = zone (exhaust) air humidity ratio (kg/kg)
-
-When the heat pump water heater draws its inlet air solely from the zone (i.e., Inlet Air Configuration = Zone Air Only), the inlet air conditions to the evaporator/fan assembly are simply set equal to the zone (exhaust) air conditions. If the heat pump water heater draws its inlet air solely from outdoors (i.e., Inlet Air Configuration = Outdoor Air Only), the inlet air conditions to the evaporator/fan assembly are simply set equal to the outdoor air conditions. When the inlet air to the heat pump water heater evaporator and fan assembly is scheduled (i.e., Inlet Air Configuration = Schedule), the inlet air conditions are determined directly from the user-supplied schedules as follows.
-
-<div>$${T_{inlet}} = GetScheduleValue(InletAirTemperatureSchedule)$$</div>
-
-<div>$$RHinlet = GetScheduleValue(InletAirHumiditySchedule)$$</div>
-
-<div>$${\omega_{inlet}} = PsyWFnTdbRhPb({T_{inlet}},R{H_{inlet}},OutBaroPress)$$</div>
-
-where:
-
-<span>\(R{H_{inlet}}\)</span>= inlet air relative humidity to heat pump water heater evaporator/fan assembly (0-1)
-
-<span>\(PsyWFnTdbRhPb\)</span>= psychrometric function returning air humidity ratio given dry-bulb temperature, relative humidity, and barometric pressure
-
-<span>\(OutBaroPress\)</span>= outdoor barometric pressure (Pa)
-
-For each simulation time step, the heat pump water heating capacity, energy use, and air-side/water-side mass flow rates are set to zero and the water heater tank is simulated with the heat pump compressor disabled when any of the following conditions apply:
-
-·        the HPWH is scheduled off by its availability schedule,
-
-·        the water heater tank setpoint temperature is greater than or equal to the heat pump compressor cut-in temperature,
-
-·        the inlet air dry-bulb temperature to the evaporator/fan assembly is less than the Minimum Inlet Air Temperature for Heat Pump Compressor Operation (as specified by the user in the HPWH input object), or
-
-·        the HPWH setpoint temperature is greater than or equal to the Maximum Temperature Limit (specified in the Water Heater:Mixed object).
-
-Otherwise, simulation of the heat pump water heater is based on its current mode of operation. This mode of operation is either floating (heat pump compressor is off and tank water temperature has not fallen below the heat pump compressor cut-in temperature) or heating (tank water temperature dropped below the compressor cut-in temperature on a previous time step but was unable to reach the compressor setpoint temperature). Each mode is handled differently and they will be discussed separately.
-
-If the heat pump water heater is using the stratified tank model, then there is more than one value for the tank temperature.  The model includes input for where the heat pump controls detect the temperature. The input data in the associated WaterHeater:Stratified includes up to two heights in the tank where the temperature is measured and a weight associated with each. The associated stratified tank nodes are selected based on these heights. When the heat pump model needs to evaluate the tank temperature of a stratified tank, it evaluates the temperature at the tank nodes associated with these locations.
-
-#### Float Mode
-
-When the heat pump water heater tank temperature is floating between the heat pump compressor’s cut-in and cut-out temperatures at the end of the previous simulation time step, both the heat pump compressor and the water heater tank’s heating element are disabled and a resulting tank temperature is calculated. If the resulting tank temperature is below the heat pump compressor’s cut-in temperature, the heat pump compressor part-load ratio is estimated using the ratio of the temperature differences shown below. The part-load ratio can not be less than zero or greater than one.
-
-<div>$$PLR = MIN\left( {1.0,\,\,MAX\left( {0.0,\,\,\left( {\frac{{{T_{HP,\,cut - in}} - {T_{tank,float}}}}{{{T_{tank,initial}} - {T_{tank,float}}}}} \right)} \right)} \right)$$</div>
-
-where:
-
-<span>\(PLR\)</span>         = part-load ratio of the heat pump water heater compressor
-
-<span>\(Ttank,float\)</span>    = tank temperature in float mode when heating capacity is set to zero(°C)
-
-<span>\({T_{tank,initial}}\)</span>    = tank temperature at the beginning of the simulation time step (°C)
-
-Since the pump and fan are assumed to cycle on and off with the heat pump compressor, the average condenser water (for pumped condensers only) and evaporator air mass flow rates for the simulation time step are calculated based on the PLR calculated above:
-
-<div>$${\dot m_{water,avg}} = \dot Vwater\left( {{\rho_{water}}} \right)\left( {PLR} \right)$$</div>
-
-<div>$$\dot mair,avg = \dot Vair\left( {{\rho_{air}}} \right)\left( {PLR} \right)$$</div>
-
-where:
-
-<span>\(\dot mwater,avg\)</span>       = average condenser water mass flow rate for the time step (kg/s)
-
-<span>\(\dot Vwater\)</span>            = condenser water volumetric flow rate, user input (m<sup>3</sup>/s)
-
-<span>\({\rho_{water}}\)</span>            = density of condenser inlet water (kg/m<sup>3</sup>)
-
-<span>\(\dot mair,avg\)</span>         = average evaporator/fan air mass flow rate for the time step (kg/s)
-
-<span>\(\dot Vair\)</span>               = evaporator/fan air volumetric flow rate, user input (m<sup>3</sup>/s)
-
-<span>\({\rho_{air}}\)</span>              = density of evaporator/fan inlet air (kg/m<sup>3</sup>)
-
-The water tank temperature is then calculated based on heat pump operation at the part-load ratio estimated above and with the water tank’s heating element enabled. If the resulting water tank temperature is above the heat pump compressor’s setpoint (cut-out) temperature, then the part-load ratio is reduced and the water heater tank is simulated again. The process is performed iteratively until the part-load ratio of the heat pump compressor achieves the desired setpoint temperature (to the extent possible).
-
-#### Heating Mode
-
-When the HPWH is in heating mode at the end of the previous simulation time step (i.e., the heat pump compressor operated during the previous simulation time step but was unable to achieve the setpoint temperature), both the heat pump compressor and the water heater tank’s heating element are enabled. The part-load ratio of the heat pump compressor is set to 1, and the condenser water (for pumped condensers) and evaporator air mass flow rates are set to their maximum flow rates.
-
-<div>$${\dot m_{water,avg}} = {\dot V_{water}}\left( {{\rho_{water}}} \right)$$</div>
-
-<div>$$\dot mair,avg = \dot Vair\left( {\rho air} \right)$$</div>
-
-If the resulting tank temperature is above the heat pump compressor’s setpoint (cut-out) temperature, the part-load ratio of the heat pump compressor is reduced and the water heater tank is simulated again. The process is performed iteratively until the part-load ratio of the heat pump compressor achieves the desired setpoint temperature (to the extent possible).
-
-The air-side outlet conditions of the HPWH are calculated through simulation of the fan and DX coil with either a blow through or draw through fan placement (user selectable). If mixer/splitter nodes are used, the HPWH model splits the heat pump outlet air mass flow rate with exhaust air flow equaling the outdoor air flow, and the balance of the outlet air being sent to the zone supply air node (i.e., ensures that the heat pump water heater does not contribute to zone pressurization or depressurization). Calculations of heat pump water heating capacity, energy use, air-side performance, and water-side temperature difference are performed in the associated DX Coil object. See the engineering reference section for the Coil:WaterHeating:AirToWaterHeatPump object for details.
-
-#### Model Outputs
-
-After completing the float mode or heating mode calculations and the final part-load ratio has been determined, the output (report) variables are calculated as follows:
-
-<div>$$Heat\,Pump\,Water\,Heater\,Compressor\,Part{\rm{ - }}Load\,Ratio = PLR\,\,$$</div>
-
-<div>$$Heat\,Pump\,Water\,Heater\,\,On{\rm{ - }}Cycle\,Parasitic\,Electric\,Power\,(W)\,\, = \,\,{P_{parasitic,on}}\left( {PLR} \right)$$</div>
-
-<span>\(Heat\,Pump\,Water\,Heater\,\,On{\rm{ - }}Cycle\,Parasitic\,Electric\,Consumption\,(J)\,\, = \,\,{P_{parasitic,on}}\left( {PLR} \right)\left( {3600} \right){t_{sys}}\)</span><span>\(Heat\,Pump\,Water\,Heater\,\,Off{\rm{ - }}Cycle\,Parasitic\,Electric\,Power\,(W)\,\, = \,\,{P_{parasitic,off}}\left( {1 - PLR} \right)\)</span><span>\(Heat\,Pump\,Water\,Heater\,\,Off{\rm{ - }}Cycle\,Parasitic\,Electric\,Consumption\,(J)\,\, = \,\,{P_{parasitic,off}}\left( {1 - PLR} \right)\left( {3600} \right)\left( {{t_{sys}}} \right)\)</span>
-
-where:
-
-<span>\({P_{parasitic,on}}\)</span>   = on-cycle parasitic electric load, user input (W)
-
-<span>\({P_{parasitic,off}}\)</span>  = off-cycle parasitic electric load, user input (W)
-
-<span>\({t_{sys}}\)</span>             = HVAC system simulation time step (hours)
-
-Note: All heat pump water heater output variables, including off-cycle ancillary electric power and consumption, equal 0 when the heat pump water heater availability schedule equals 0 (i.e., the heat pump water heater is scheduled OFF).
-
-### Stratified Water Thermal Tank
-
-The input objects WaterHeater:Stratified and ThermalStorage:ChilledWater:Stratified provide models for a stratified water thermal tank that divides the water tank into multiple nodes of equal volume.  This model is used for both the stratified water heater and the stratified chilled water storage tank. The nodes are coupled by vertical conduction effects, internode fluid flow, and temperature inversion mixing.  The object simultaneously solves the differential equations governing the energy balances on the nodes using the Forward-Euler numerical method.  The system time step is divided into one second substeps that allow the simulation to capture events that occur on a very short time scale.
-
-#### Energy Balance
-
-Similar to the well-mixed model, the stratified model solves the same fundamental differential equation governing the energy balance on a mass of water:
-
-<div>$$m{c_p}\frac{{dT}}{{dt}} = {q_{net}}$$</div>
-
-where
-
-*m* = mass of water
-
-*c<sub>p</sub>* = specific heat of water
-
-*T* = temperature of water
-
-*t* = time
-
-*q<sub>net</sub>* = net heat transfer rate
-
-The difference for the stratified model is that it must solve the energy balance on *n* number of nodes simultaneously.  Node 1 is at the top of the water tank and node *n* is at the bottom of the water tank.
-
-<div>$${m_n}{c_p}\frac{{d{T_n}}}{{dt}} = {q_{net,n}}$$</div>
-
-where
-
-*m<sub>n</sub>* = mass of water for node *n*
-
-*c<sub>p</sub>* = specific heat of water
-
-*T<sub>n</sub>* = temperature of water for node *n*
-
-*t* = time
-
-*q<sub>net,n</sub>* = net heat transfer rate for node *n*
-
-The net heat transfer rate *q<sub>net</sub>* is the sum of gains and losses due to multiple heat transfer pathways.
-
-<div>$$\begin{array}{l}{q_{net,n}} = {q_{heater,n}} + {q_{oncycpara,n}} + {q_{offcycpara,n}} + {q_{oncycloss,n}} + {q_{offcycloss,n}}\\ + {q_{cond,n}} + {q_{use,n}} + {q_{source,n}} + {q_{flow,n}} + {q_{invmix,n}}\end{array}$$</div>
-
-where
-
-*q<sub>heater,n</sub>* = heat added by Heater 1 or Heater 2
-
-*q<sub>oncycpara,n</sub>* = heat added due to on-cycle parasitic loads (zero when off)
-
-*q<sub>offcycpara,n</sub>* = heat added due to off-cycle parasitic loads (zero when on)
-
-*q<sub>oncycloss,n</sub>* = heat transfer to/from the ambient environment (zero when off)
-
-*q<sub>offcycloss,n</sub>* = heat transfer to/from the ambient environment (zero when on)
-
-*q<sub>cond,n</sub>* = heat transfer due to conduction between the node above and below
-
-*q<sub>use,n</sub>* = heat transfer to/from the use side plant connections
-
-*q<sub>source,n</sub>* = heat transfer to/from the source side plant connections
-
-*q<sub>flow,n</sub>* = heat transfer due to fluid flow from the node above and below
-
-*q<sub>invmix,n</sub>* = heat transfer due to inversion mixing from the node above and below
-
-*q<sub>oncycloss,n</sub>* and *q<sub>offcycloss,n</sub>* are defined as:
-
-<div>$${q_{oncycloss,n}} = ({UA_{tank}} + UA_add,n)({T_{amb}} - {T_n})$$</div>
-
-<div>$${q_{offcycloss,n}} = ({UA_{tank} + UA_{flue}})({T_{amb}} - {T_n})$$</div>
-
-where
-
-*UA<sub>tank</sub>* = loss coefficient to ambient environment for the tank
-
-*UA<sub>add,n</sub>* = additional node loss coefficient
-
-*UA<sub>flue</sub>* = additional off-cycle flue loss coefficient to ambient environment  (zero when on)
-
-*T<sub>amb</sub>* = temperature of ambient environment
-
-*q<sub>cond,n</sub>* is defined as:
-
-<div>$${q_{cond,n}} = \frac{{k{A_{n + 1}}}}{{{L_{n + 1}}}}({T_{n + 1}} - {T_n}) + \frac{{k{A_{n - 1}}}}{{{L_{n - 1}}}}({T_{n - 1}} - {T_n})$$</div>
-
-where
-
-*k* = fluid thermal conductivity of water, 0.6 W/m-K
-
-*A<sub>n+1</sub>* = shared surface area between node *n* and node *n+1*
-
-*L<sub>n+1</sub>* = distance between the center of mass of node *n* and n*+1*
-
-*T<sub>n+1</sub>* = temperature of node *n+1*
-
-*A<sub>n-1</sub>* = shared surface area between node *n* and node *n-1*
-
-*L<sub>n-1</sub>* = distance between the center of mass of node *n* and n*-1*
-
-*T<sub>n-1</sub>* = temperature of node *n-1*
-
-*q<sub>use,n</sub>*, and *q<sub>source,n</sub>* are defined as:
-
-<div>$${q_{use}} = {\varepsilon_{use}}{\dot m_{use}}{c_p}\left( {{T_{use}} - T} \right)$$</div>
-
-<div>$${q_{source}} = {\varepsilon_{source}}{\dot m_{source}}{c_p}\left( {{T_{source}} - T} \right)$$</div>
-
-where
-
-*e<sub>use</sub>* = heat exchanger effectiveness for the use side plant connections
-
-<span>\({\dot m_{use}}\)</span>= mass flow rate for the use side plant connections
-
-*T<sub>use</sub>* = inlet fluid temperature of the use side plant connections
-
-*e<sub>source</sub>* = heat exchanger effectiveness for the source side plant connections
-
-<span>\({\dot m_{source}}\)</span>= mass flow rate for the source side plant connections
-
-*T<sub>source</sub>* = inlet fluid temperature of the source side plant connections
-
-*q<sub>flow,n</sub>* is defined as:
-
-<div>$${q_{flow,n}} = {\dot m_{n + 1}}{c_p}({T_{n + 1}} - {T_n}) + {\dot m_{n - 1}}{c_p}({T_{n - 1}} - {T_n})$$</div>
-
-where
-
-<span>\({\dot m_{n + 1}}\)</span>= mass flow rate from node *n+1*
-
-<span>\({\dot m_{n - 1}}\)</span>= mass flow rate from node *n-1*
-
-*q<sub>invmix,n</sub>* is defined as:
-
-<div>$${q_{invmix,n}} = {\dot m_{invmix,n + 1}}{c_p}({T_{n + 1}} - {T_n}) + {\dot m_{invmix,n - 1}}{c_p}({T_{n - 1}} - {T_n})$$</div>
-
-where
-
-<span>\({\dot m_{invmix,n + 1}}\)</span>= mass flow rate from node *n+1* due to temperature inversion mixing
-
-<span>\({\dot m_{invmix,n - 1}}\)</span>= mass flow rate from node *n-1* due to temperature inversion mixing
-
-Inversion mixing occurs when the node below is warmer than the node above.  The difference in temperatures drives a difference in density that causes the nodes to mix.  Usually inversion mixing occurs very rapidly.  In this algorithm, the inversion mixing rate is selected to be the maximum value that will provide a stable solution given the node mass and the substep interval:
-
-<div>$${\dot m_{invmix}} = 0.5*{m_n}/\Delta t$$</div>
-
-where
-
-*Dt* = the substep time interval.
-
-The use and source fluid steam outlet temperatures calculation procedure depends on the values of the effectiveness.  If the effectiveness is 1.0, then complete mixing of these fluid steam and the tank water is assumed.  In this case the outlet temperatures for the use and source streams will be simply the tank water temperatures at point of the outlet nodes. When the effectiveness is less than 1.0, an indirect heat exchange is assumed between the use or source stream and the water in the stratified thermal storage tank.  When the effectiveness is less than 1.0, the use and source outlet temperatures are calculated using *Q<sub>use</sub>* and *Q<sub>source</sub>*, and energy balance equations as follows:
-
-<div>$${T_{use\;out,\,n}} = {T_{use,\,n}} + \frac{{{q_{use,n}}}}{{{{\dot m}_{use}}{c_p}}}$$</div>
-
-<div>$${T_{source\;out,\,n}} = {T_{source,\,n}} - \frac{{{q_{source,n}}}}{{{{\dot m}_{source}}{c_p}}}$$</div>
-
- where,
-
-*T<sub>use\\ out</sub>*<sub> </sub>= outlet fluid temperature of the use side plant connections
-
-*T<sub>source\\ out</sub>*<sub> </sub>= outlet fluid temperature of the source side plant connections
-
-#### Numerical Solution
-
-The system of simultaneous differential equations is solved using the Forward-Euler numerical method.  The system time step is divided into one-second substeps.  The new temperature for a given node is calculated using the following equation:
-
-<div>$${T_n} = {T_{n,old}} + \frac{{{q_{net,n}}\Delta t}}{{{m_n}{c_p}}}$$</div>
-
-All node temperatures for *q<sub>net,n</sub>* are the old temperatures from the previous substep.
-
-Before each system time step is calculated the following evaluations are made:
-
-§ Use and source inlet flow rates are applied to the inlet nodes
-
-§ Internode flow is determined and net flow rates are determined
-
-Before each substep is calculated, the following evaluations are made:
-
-1)   Thermostatic controls for heater 1 and heater 2 are evaluated to determine if the heater elements should turn on or off
-
-2)   Node 1 temperature is compared against the maximum limit to determine if venting is necessary
-
-3)   Adjoining node temperatures are compared to determine if there are any temperature inversions for which the inversion mixing rate should be used.
-
-The solution continues looping through all substeps until the system time step is completed.
-
-#### References
-
-Duffie, J., and W. Beckman. 1980. *Solar Engineering of Thermal Processes*.  John Wiley & Sons.
-
-Newton, B. 1995. *Modeling of Solar Storage Tanks*.  Master's Dissertation, University of Wisconsin-Madison.
-
-### Water Heating Sizing
-
-Some inputs for water heaters can be autosized using the input object WaterHeater:Sizing.  This section describes the sizing calculations for water heaters.  There are six general methods for sizing tank volume and heating capacity.
-
-#### Autosizing Tank Volume
-
-The volume a water heater can be sized in the following ways depending on the design method chosen by the user.
-
-·        Peak Draw.  The volume is determined from the loop design flow rate.  The water heater is positioned on the supply side of a plant loop.  After the plant sizing routines have run, the model  obtains the design flow rate for all components on the demand side.  The tank volume is then: <span>\(V = {\dot V_{loop.des}}*{t_{draw}}\)</span>,
-
-·        Residential HUD-FHA Minimum.  The volume is determined from a set of rules defined by the table below.  This is from Chapter 48 of 1999 ASHRAE Handbook HVAC Applications, Americal Society of Heating Refrigeration and Air-conditioning Engineeers, Atlanta GA.  (also used in the Building America Benchmark).
-
-Table 85. Residential HUD-FHA Minimum
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="13">Residential HUD-FHA Minimum DHW Storage and Burner Capacity (ASHRAE 1999)</th>
-  </tr>
-  <tr>
-    <td># Bedrooms</td>
-    <td>1</td>
-    <td colspan="3">2</td>
-    <td colspan="3">3</td>
-    <td colspan="3">4</td>
-    <td>5</td>
-    <td>6</td>
-  </tr>
-  <tr>
-    <td># Bathrooms</td>
-    <td>All</td>
-    <td>&lt;= 1.5</td>
-    <td>2 - 2.5</td>
-    <td>&gt;= 3</td>
-    <td>&lt;= 1.5</td>
-    <td>2 - 2.5</td>
-    <td>&gt;= 3</td>
-    <td>&lt;= 1.5</td>
-    <td>2 - 2.5</td>
-    <td>&gt;= 3</td>
-    <td>All</td>
-    <td>All</td>
-  </tr>
-  <tr>
-    <th>Gas</th>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Storage (gal)</td>
-    <td>20</td>
-    <td>30</td>
-    <td>30</td>
-    <td>40</td>
-    <td>30</td>
-    <td>40</td>
-    <td>40</td>
-    <td>40</td>
-    <td>40</td>
-    <td>50</td>
-    <td>50</td>
-    <td>50</td>
-  </tr>
-  <tr>
-    <td>Burner (kBtu/hr)</td>
-    <td>27</td>
-    <td>36</td>
-    <td>36</td>
-    <td>36</td>
-    <td>36</td>
-    <td>36</td>
-    <td>38</td>
-    <td>36</td>
-    <td>38</td>
-    <td>38</td>
-    <td>47</td>
-    <td>50</td>
-  </tr>
-  <tr>
-    <th>Electric</th>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Storage (gal)</td>
-    <td>20</td>
-    <td>30</td>
-    <td>40</td>
-    <td>50</td>
-    <td>40</td>
-    <td>50</td>
-    <td>50</td>
-    <td>50</td>
-    <td>50</td>
-    <td>66</td>
-    <td>66</td>
-    <td>80</td>
-  </tr>
-  <tr>
-    <td>Burner (kW)</td>
-    <td>2.5</td>
-    <td>3.5</td>
-    <td>4.5</td>
-    <td>5.5</td>
-    <td>4.5</td>
-    <td>5.5</td>
-    <td>5.5</td>
-    <td>5.5</td>
-    <td>5.5</td>
-    <td>5.5</td>
-    <td>5.5</td>
-    <td>5.5</td>
-  </tr>
-</table>
-
-·        Per Person.  The tank volume is determined by summing the design level of people in the model and multiplying by a user-entered volume per person factor.
-
-·        Per Floor Area.  The tank volume is determined by summing the floor area in all the zones in the model and multiplying by a user-entered volume per floor area factor.
-
-·        Per Unit.  The tank volume is determined by multiplying a user-entered volume per unit and a user-entered number of units.
-
-·        Per Solar Collector Area.  The tank volume is determined by summing the collector area in all the hot water solar collectors in the model and multiplying by a user-entered volume per collector area factor.
-
-#### Autosizing Heater Capacity
-
-The heater capacity can be sized in the following ways depending on the design method chosen by the user.
-
-·        Peak Draw.  The heater capacity is determined from the tank volume, assumed start and finish temperatures and a user defined time for recovery.  The heater capacity is then
-
-<div>$$$$</div><span>\({q_{heat}} = V\rho \,{c_p}({T_{finish}} - {T_{start}})\)</span>
-
-where,
-
-<div>$${T_{finish}} = 57.2C$$</div>
-
-<div>$${T_{start}} = 14.4C$$</div>
-
-·        Residential HUD-FHA Minimum.  The heater capacity is determined from a set of rules defined by the table above.  This is from 1999 ASHRAE Handbook HVAC Applications, Americal Society of Heating Refrigeration and Air-conditioning Engineeers, Atlanta GA.  (also used the Building America Benchmark).
-
-·        Per Person.  The heater capacity is determined by summing the design level of people in the model and using a user-entered factor for recovery capacity per person.  The heater capacity is then:
-
-<div>$${q_{heat}} = \frac{{{N_{people}}{f_{{\mathop{\rm Re}\nolimits} {\mathop{\rm cov}} eryPerPerson}}({T_{finish}} - {T_{start}})\rho \,{c_p}}}{{3600}}$$</div>
-
-·        Per Floor Area.  The heater capacity is determined by summing the floor area in all the zones in the model and using a user-entered factor for recovery capacity per floor area.  The heater capacity is then:
-
-<div>$$$$</div><span>\({q_{heat}} = \frac{{{A_{floors}}{f_{{\mathop{\rm Re}\nolimits} {\mathop{\rm cov}} eryPerFloorArea}}({T_{finish}} - {T_{start}})\rho \,{c_p}}}{{3600}}\)</span>
-
-·        Per Unit.  The heater capacity is determined from a user-entered Recovery Capacity per unit and a user-entered number of units.  The heater capacity is then:
-
-<div>$${q_{heat}} = \frac{{{N_{units}}{f_{{\mathop{\rm Re}\nolimits} {\mathop{\rm cov}} eryPerUnit}}({T_{finish}} - {T_{start}})\rho \,{c_p}}}{{3600}}$$</div>
-
-·        Per Solar Collector Area. The water heater is assumed to be used for solar hot water storage and the heater capacity is set to zero.
-
-#### Autosizing Tank Height
-
-If the water heater is Stratified, then the geometry is important and the height of the tank can be scaled with changes in volume.  For tank shapes of Vertical Cylinder, the user defined height aspect ratio, *AR*,  is used to calculate a tank height, *H*, using
-
-<div>$$H = {\left( {\frac{{4\,V\;A{R^2}}}{\pi }} \right)^{1/3}}$$</div>
-
-#### Autosizing Plant Connection Flow Rates
-
-When the water thermal tank is connected to a plant loop, it is convient to autosize the design volume flow rates through the plant connections.  When the water thermal tank is connected to the supply side of plant loop and flow rates are autosized, the flow rate is the sum of the flow requests of all the various components on the demand side of that plant loop.  When the water thermal tank is connected on the demand side of a plant loop (e.g. as for indirect water heating with a boiler) and flow rates are autosized, the design flow rates are calculated with the following equation,
-
-<div>$$\dot V =  - \left( {\frac{V}{{{t_{{\mathop{\rm Re}\nolimits} {\mathop{\rm cov}} er}} * 3600 * \varepsilon }}} \right) * Ln\left[ {\frac{{\left( {{T_{PlantDesign}} - {T_{Setpo{\mathop{\rm int}} }}} \right)}}{{\left( {{T_{PlantDesign}} - {T_{start}}} \right)}}} \right]$$</div>
-
-where
-
-*V* = volume of the tank
-
-<span>\({t_{{\mathop{\rm Re}\nolimits} {\mathop{\rm cov}} er}}\)</span> = User parameter for the time it takes for the tank to recover from assumed starting temperature to an assumed setpoint temperature.  For water heaters, the starting temperature is 14.4ºC and the final assumed setpoint temperature is 57.2ºC.  For chilled water tanks, the starting temperature is 14.4 ºC and the final temperature is 9.0ºC.
-
-<span>\(\varepsilon \)</span> = *e<sub>use</sub>*   or *e<sub>source</sub>*
-
-<span>\({T_{PlantDesign}}\)</span>= the exit temperature specified in the Plant Sizing object
-
-<span>\({T_{setpo{\mathop{\rm int}} }}\)</span> =  the final tank temperature of 57.2ºC for heaters and 9.0ºC for chilled water tanks.
-
-<span>\({T_{start}}\)</span> = the initial tank temperature of 14.4ºC
-
-If the demand side connections are autosized and a water heater’s tank volume is autosized, then the problem cannot be readily solved in EnergyPlus because the demand side connection flows need to be reported earlier in the simulation and the tank volume is not yet available.  This situation is resolved by using an interim, nominal tank volume for sizing the connections and the actual volume is calculated later in the simulation.
-
-Water Systems  <a name="WaterSystems"></a>
--------------
-
-Water systems include a variety of components that simulate water consumption, production, and storage, including:
-
-1.    Water Use Equipment and Connections
-
-2.    Rainwater Collection
-
-3.    Groundwater Well
-
-4.    Water Storage Tanks
-
-### Water Mains Temperatures
-
-The input object Site:WaterMainsTemperature provides a model for the temperature of water mains that deliver water to a building via underground pipes.  The water mains temperatures are an important input for plant equipment that require make-up water from the water mains, such as for domestic hot water systems.
-
-Water mains temperatures are a function of outdoor climate conditions and vary with time of year.  A correlation has been formulated to predict water mains temperatures based on two weather inputs:
-
-average annual outdoor air temperature (dry-bulb)
-
-maximum difference in monthly average outdoor air temperatures
-
-These values can be easily calculated from annual weather data using a spreadsheet.
-
-The correlation was developed by Craig Christensen and Jay Burch and is described in Hendron et al. (2004).  The correlation is:
-
-
-
-T<sub>mains</sub> = (T<sub>out,avg</sub> + 6) + ratio \* (ΔT<sub>out,maxdiff</sub> / 2) \* SIN(0.986 \* (day - 15 - lag) - 90)
-
-
-
-where
-
-T<sub>mains</sub> = water mains temperature (°F)
-
-T<sub>out,avg</sub> = average annual outdoor air temperature (°F)
-
-ΔT<sub>out,maxdiff</sub> = maximum difference in monthly average outdoor air temperatures (°F)
-
-day = Julian day of the year (1-365)
-
-ratio = 0.4 + 0.01 \* (Tamb,avg - 44)
-
-lag = 35 - 1.0 \* (Tamb,avg - 44) (°F)
-
-
-
-For the Chicago-O'Hare TMY2 weather file, T<sub>out,avg</sub> = 9.69 C and ΔT<sub>out,maxdiff</sub> = 28.1 C.  The resulting water mains temperature profile is graphed below.
-
-
-
-![](media/image6936.png)
-
-#### References
-
-Hendron, R., Anderson, R., Christensen, C., Eastment, M., and Reeves, P.  2004.  "Development of an Energy Savings Benchmark for All Residential End-Uses", Proceedings of SimBuild 2004, IBPSA-USA National Conference, Boulder, CO, August 4 - 6, 2004.
-
-### Water Use Equipment and Connections
-
-Essential parts of most water systems are the end uses where the water is utilized for a purpose.  These end uses are characterized by familiar pieces of equipment such as sinks, showers, dishwashers, clothes washers, and toilets.  End uses can also include outdoor uses such as landscape irrigation and agricultural irrigation.
-
-Water end-use modeling in EnergyPlus is accomplished via two input objects:
-
-§ WaterUse:Equipment
-
-§ WaterUse:Connections
-
-The WaterUse:Equipment object simulates all different types of water end uses.  The WaterUse:Connections object manages multiple pieces of water equipment with a common supply and return, internally providing the services of a splitter and a mixer.  The WaterUse:Connections object also allows water consuming equipment to be simulated in a closed plant loop by supplying makeup water from the water mains.
-
-### Unconnected Water Use Equipment
-
-Common water equipment, such as sinks and showers, requires mixing of hot and cold water to provide a desired temperature at the tap.  Water use equipment that is simulated in "unconnected" mode, i.e., without being referenced by a WaterUse:Connections object, presents a relatively simple modeling problem illustrated by the diagram below:
-
-![Water Use Connections ENG Diagram 1](media/image6937.png)
-
-Figure 315. Hot and Cold Water Mixing
-
-The variables are defined as:
-
-<span>\({\dot m_{hot}}\)</span>= hot water supply mass flow rate
-
-<span>\({T_{hot}}\)</span>= hot water supply temperature
-
-<span>\({\dot m_{cold}}\)</span>= cold water supply mass flow rate
-
-<span>\({T_{cold}}\)</span>= cold water supply temperature
-
-<span>\({\dot m_{target}}\)</span>= target mass flow rate at the tap
-
-<span>\({T_{target}}\)</span>= target temperature at the tap
-
-The basic physics of the problem are described by two equations representing conservation of mass and conservation of energy respectively:
-
-<div>$${\dot m_{target}} = {\dot m_{hot}} + {\dot m_{cold}}$$</div>
-
-<div>$${\dot m_{target}}{T_{target}} = {\dot m_{hot}}{T_{hot}} + {\dot m_{cold}}{T_{cold}}$$</div>
-
-The hot and cold water supply temperatures, <span>\({T_{hot}}\)</span> and <span>\({T_{cold}}\)</span>, are specified by the user with schedules (or indirectly from the water mains temperatures).  The target flow rate and target temperature, <span>\({\dot m_{target}}\)</span> and <span>\({T_{target}}\)</span>, at the tap are also specified with schedules.  The target conditions can be thought of as a way to simulate occupant behavior; a person at a sink will adjust the hot and cold flow rates to get the overall water flow and temperature that is desired.
-
-The two equations above are easily solved to calculate the necessary hot and cold flow rates needed to attain the target conditions.
-
-<div>$${\dot m_{hot}} = {\dot m_{target}}\left( {\frac{{{T_{target}} - {T_{cold}}}}{{{T_{hot}} - {T_{cold}}}}} \right)$$</div>
-
-<div>$${\dot m_{cold}} = {\dot m_{target}} - {\dot m_{hot}}$$</div>
-
-Even though hot and cold flow rates are unlimited in "unconnected" mode, it is still possible to fail to meet the target conditions if <span>\({T_{target}}\)</span> &gt; <span>\({T_{hot}}\)</span>.  In this case, the actual mixed water temperature at the tap, <span>\({T_{mixed}}\)</span>, is set equal to <span>\({T_{hot}}\)</span>.  The target flow rate is always met.
-
-Water equipment that omits schedules for the target temperature and/or hot water suppy temperature implies that no hot water is needed.  The result is all cold water at the target flow rate.
-
-For "unconnected" water equipment, the heating rate and energy that is required to supply the hot water is calculated by the following equations.
-
-<div>$$Q = {\dot m_{hot}}{c_p}\left( {{T_{hot}} - {T_{cold}}} \right)$$</div>
-
-<div>$$\Delta E = Q\Delta t$$</div>
-
-where
-
-<span>\(Q\)</span>= heating rate
-
-<span>\({c_p}\)</span>= specific heat of water
-
-<span>\(\Delta E\)</span>= heating energy
-
-<span>\(\Delta t\)</span>= time step interval
-
-All heating is assigned to "Purchased Heating".
-
-### Zone Heat Gain from Water Use Equipment
-
-Some water use equipment can be a significant source of sensible and latent heat gain when located in a zone.  Showers, for example, add a noticeable latent gain as some of the hot water evaporates into the zone air (and at the same time adding some sensible gain).  Other types of equipment may contribute greater sensible gain but less latent gain.
-
-Calculating the amount of sensible and latent heat gain can be extremely complicated and depends on many variables.  One set of variables is related to the initial conditions of the entering water and the undisturbed zone air, namely:
-
-* Entering water temperature
-
-* Entering water flow rate
-
-* Ambient zone air temperature
-
-* Ambient zone humidity
-
-* Ambient zone barometric pressure
-
-A second set of variables is tied to the specifics of the water equipment which describe the heat and mass transfer processes that occur as the water passes through the zone.  These variables might include the velocity of the water in the zone air, the surface area of water exposed to the zone air, the dwell time of water in the zone, and possibly others.  The complexity of these variables cannot be easily cast into a generalized EnergyPlus input object.  Consider that in a shower, the velocity of water droplets is increasing as they fall, and the surface area of the spray is increasing.  How to even determine the surface area of the spray at any point?
-
-The approach taken here is to utilize the first set of initial condition variables and forego the overly-complex second set.  The initial conditions can be used to calculate a maximum possible change in sensible and latent energy between the entering water conditions and the leaving water conditions at an infinite time later.  Sensible and latent energy are calculated separately and represent the maximum heat gain, respectively, that could be added to the zone air.  The user simply specifies a fraction of the maximum heat gain for sensible and latent that is actually added to the zone air.  The fraction is specified with a schedule to account for different modes of operation.  The split between sensible and latent will vary depending on the type of equipment that is to be modeled.  Typically, both fractions should be small numbers.
-
-![Water Use Connections ENG Diagram 2](media/image6962.png)
-
-Figure 316.  Zone Heat Gain from Water Use Equipment
-
-The maximum sensible heat gain rate is calculated by assuming that all of the water flow is allowed to cool to the zone dry-bulb temperature.  The actual sensible zone heat gain rate is found by multiplying the maximum by the user fraction.
-
-<div>$${Q_{sens}} = {f_{sens}}{\dot m_{target}}{c_p}\left( {{T_{target}} - {T_{zone}}} \right)$$</div>
-
-<div>$$\Delta {E_{sens}} = {Q_{sens}}\Delta t$$</div>
-
-where
-
-<span>\({Q_{sens}}\)</span> = sensible heat gain rate
-
-<span>\({f_{sens}}\)</span> = user fraction of maximum sensible heat
-
-<span>\({\dot m_{target}}\)</span>= target mass flow rate at the tap
-
-<span>\({c_p}\)</span>= specific heat of water
-
-<span>\({T_{target}}\)</span>= target temperature at the tap
-
-<span>\({T_{zone}}\)</span> = zone dry-bulb air temperature
-
-<span>\(\Delta {E_{sens}}\)</span>= sensible heat gain
-
-<span>\(\Delta t\)</span>= time step interval
-
-The maximum latent heat gain rate is calculated by assuming that the maximum amount of water is evaporated into the zone air during the time step.  The actual latent zone heat gain rate is found by multiplying the maximum by the user fraction.
-
-<div>$${m_{evap,zonemax}} = \left( {{W_{sat}} - {W_{zone}}} \right){\rho_{zone}}{V_{zone}}$$</div>
-
-<div>$${m_{evap,flowmax}} = {\dot m_{target}}\Delta t$$</div>
-
-<div>$${m_{evap,max}} = MIN({m_{evap,zonemax}},{m_{evap,flowmax}})$$</div>
-
-<div>$${m_{evap}} = {f_{lat}}{m_{evap,max}}$$</div>
-
-<div>$${\dot m_{evap}} = {m_{evap}}/\Delta t$$</div>
-
-<div>$${Q_{lat}} = {h_{fg}}{\dot m_{evap}}$$</div>
-
-<div>$$\Delta {E_{lat}} = {Q_{lat}}\Delta t$$</div>
-
-where
-
-<span>\({m_{evap,zonemax}}\)</span>= mass of water that can be absorbed by the zone air in one timestep
-
-<span>\({W_{sat}}\)</span>= fully-saturated zone humidity ratio (function of air temperature and pressure)
-
-<span>\({W_{zone}}\)</span> = zone humidity ratio
-
-<span>\({\rho_{zone}}\)</span> = zone dry-air density (function of air temperature and pressure)
-
-<span>\({V_{zone}}\)</span> = zone air volume
-
-<span>\({m_{evap,flowmax}}\)</span>= mass of water available in the flow in one timestep
-
-<span>\({\dot m_{target}}\)</span>= target mass flow rate at the tap
-
-<span>\(\Delta t\)</span>= time step interval
-
-<span>\({m_{evap,max}}\)</span>= maximum mass of water that can be evaporated
-
-<span>\({m_{evap}}\)</span>= actual mass of water evaporated into the zone air
-
-<span>\({f_{lat}}\)</span> = user fraction of maximum latent heat
-
-<span>\({\dot m_{evap}}\)</span>= mass rate of water evaporation into the zone air
-
-<span>\({Q_{lat}}\)</span> = latent heat gain rate
-
-<span>\({h_{fg}}\)</span>= heat of vaporization for water
-
-<span>\(\Delta {E_{lat}}\)</span>= latent heat gain
-
-Sensible and latent heat gains to the zone are lagged by one zone time step.
-
-Note that this method allows the heat gain to vary dynamically according to changing water and zone conditions instead of the fixed or scheduled value that is traditionally used.  However, sensible and latent fractions may be difficult to estimate.  Experimental measurement is probably the best way to determine the fractions.
-
-A related result of any zone heat and moisture gain is that the water undergoes an equal heat and moisture loss.  For a shower the water will generally leave the zone at a cooler temperature and slightly reduced flow rate when compared to the entering water conditions.
-
-<div>$${\dot m_{drain}} = {\dot m_{target}} - {\dot m_{evap}}$$</div>
-
-<div>$${T_{drain}} = \frac{{{{\dot m}_{target}}{c_p}{T_{target}} - {Q_{sens}} - {Q_{lat}}}}{{{{\dot m}_{drain}}{c_p}}}$$</div>
-
-where
-
-<span>\({\dot m_{drain}}\)</span>= drainwater mass flow rate at the drain
-
-<span>\({\dot m_{target}}\)</span>= target mass flow rate at the tap
-
-<span>\({\dot m_{evap}}\)</span>= mass rate of water evaporation into the zone air
-
-<span>\({T_{drain}}\)</span>= water temperature at the drain
-
-<span>\({c_p}\)</span>= specific heat of water
-
-<span>\({T_{target}}\)</span>= target temperature at the tap
-
-<span>\({Q_{sens}}\)</span> = sensible heat gain rate
-
-<span>\({Q_{lat}}\)</span> = latent heat gain rate
-
-The change in leaving water conditions has implications for drainwater heat recovery and storage tank conditions.
-
-### Connected Water Use Equipment
-
-Water use equipment referenced by a WaterUse:Connections object is considered to be in "connected" mode.  The WaterUse:Connections object manages multiple pieces of water equipment with a common supply and return, internally providing the services of a splitter and a mixer.  The connections object also offers three internal configurations for drainwater heat recovery.  External connections are available for coupling to plant loop nodes or water storage tanks for graywater reuse or reclamation.
-
-Keep in mind that water use equipment in "connected" mode does not imply that it is connected to a plant loop.  WaterUse:Equipment objects are never directly connected to a plant loop; they are connected indirectly through the WaterUse:Connections object.  WaterUse:Connections can operate either within a plant loop or in stand-alone mode, i.e., without plant loop connections.
-
-The WaterUse:Connections object overrides the hot and cold water supply temperatures of its subordinate WaterUse:Equipment objects based on the specified schedules, plant loop conditions, or water storage tank conditions.  But the WaterUse:Equipment objects still maintain their individual target flow rates and target temperatures.
-
-Solving the water subsystem described by the WaterUse:Connections object is appreciably more difficult than solving a single, unconnected piece of water use equipment.  The subsystem is illustrated below.
-
-![Water Use Connections ENG Diagram 3](media/image7005.png)
-
-Figure 317. Water Use Connections Subsystem
-
-The nomenclature here uses uppercase letters to indicate variables related to the connections object and lowercase letters to indicate variables related to the equipment objects.  The variables are defined as:
-
-<span>\({\dot M_{hot}}\)</span>= hot water supply mass flow rate
-
-<span>\({T_{hot}}\)</span>= hot water supply temperature
-
-<span>\({\dot M_{cold}}\)</span>= cold water supply mass flow rate
-
-<span>\({T_{cold}}\)</span>= cold water supply temperature
-
-<span>\({\dot M_{drain}}\)</span>= drainwater mass flow rate at the drain
-
-<span>\({T_{drain}}\)</span>= water temperature at the drain
-
-<span>\({T_{waste}}\)</span>= wastewater temperature after the drain
-
-<span>\({\dot M_{return}}\)</span>= return water mass flow rate back to the plant loop
-
-<span>\({T_{return}}\)</span>= return temperature of makeup water back to the plant loop
-
-### Water Use Equipment Calculations
-
-The solution method proceeds in steps:
-
-* *InitConnectionsTemps*
-
-* *CalcConnectionsFlowRates*
-
-* *CalcConnectionsDrainTemp*
-
-* *UpdateConnectionsNodes*
-
-#### Initialize Connections Temperatures
-
-Initializes the hot and cold supply water temperatures, <span>\({T_{hot}}\)</span> and <span>\({T_{cold}}\)</span>, for the common supply to all the equipment.  If plant-coupled, <span>\({T_{hot}}\)</span> is taken from the plant loop inlet node.  If stand-alone, <span>\({T_{hot}}\)</span> is taken from the schedule.
-
-<span>\({T_{cold}}\)</span> is taken from the supply water storage tank, if specified.  Otherwise <span>\({T_{cold}}\)</span> is taken from the schedule.  If a schedule is not specified, <span>\({T_{cold}}\)</span> is taken from the water mains.
-
-#### Calculate Connections Flow Rates
-
-First calls on each piece of equipment to simulate itself with the given supply water temperatures <span>\({T_{hot}}\)</span> and <span>\({T_{cold}}\)</span>.  The desired hot and cold flow rates for <span>\({\dot m_{hot,i}}\)</span> and <span>\({\dot m_{cold,i}}\)</span> are calculated (as described earlier) and passed back to the connections object.  The total flow rates for <span>\({\dot M_{hot}}\)</span> and <span>\({\dot M_{cold}}\)</span> are then calculated:
-
-<span>\({\dot M_{hot}} = \mathop \sum \limits_i {\dot m_{hot,i}}\)</span>           <span>\({\dot M_{cold}} = \mathop \sum \limits_i {\dot m_{cold,i}}\)</span>
-
-If plant-coupled, <span>\({\dot M_{hot}}\)</span> is compared to the maximum flow rate available in the plant loop (after the first HVAC iteration).  If <span>\({\dot M_{hot}}\)</span> &gt; <span>\({\dot M_{hot,max}}\)</span>, the actual flow rate is reset to equal the maximum:  <span>\({\dot M_{hot}}\)</span> = <span>\({\dot M_{hot,max}}\)</span>.  New hot and cold flow rates, <span>\({\dot m'_{hot,i}}\)</span> and <span>\({\dot m'_{cold,i}}\)</span>, at the equipment level are then recalculated, decreasing the hot flow rate and increasing the cold flow rate in order to still meet the target flow rate.
-
-<div>$$\alpha  = \frac{{{{\dot M}_{hot,max}}}}{{{{\dot M}_{hot}}}}$$</div>
-
-<div>$${\dot m'_{hot,i}} = \alpha {\dot m_{hot,i}}$$</div>
-
-<div>$${\dot m'_{cold,i}} = {\dot m_{target,i}} - {\dot m'_{hot,i}}$$</div>
-
-A new mixed water temperature is also recalculated at the equipment level.
-
-Although water storage tanks can also have a maximum flow rate on the cold side, the cold flow rate is not limited in this implementation.
-
-#### Calculate Connections Drain Temperature
-
-At this point zone heat gains are calculated for all equipment in zones.  The final drainwater temperatures and flow rates are determined for each piece of equipment by subtracting the lost heat and moisture (see above).  The total drainwater temperature and flow rate for the subsystem are calculated:
-
-<span>\({\dot M_{drain}} = \mathop \sum \limits_i {\dot m_{drain,i}}\)</span>           <span>\({T_{drain}} = \frac{{\mathop \sum \limits_i {{\dot m}_{drain,i}}{t_{drain,i}}}}{{{{\dot M}_{drain}}}}\)</span>
-
-In the case of no drainwater heat recovery, the subsystem wastewater temperature, <span>\({T_{waste}}\)</span>, is equal to the drainwater temperature, <span>\({T_{drain}}\)</span>.  (For drainwater heat recovery, see below.)  The wastewater temperature and flow rate are propogated to the reclamation water storage tank, if specified.
-
-#### Update Connections Nodes
-
-Finally, if plant-coupled, the return water temperature, <span>\({T_{return}}\)</span>, is passed on to the plant outlet node.  <span>\({T_{return}}\)</span> is taken from the cold water supply schedule or the water mains.  The return flow rate is equal to the hot water supply flow rate in order to preserve a closed plant loop:  <span>\({\dot M_{return}}\)</span> = <span>\({\dot M_{hot}}\)</span>.
-
-For "connected" water equipment, the heating rate and energy that is required to supply the hot water for individual water equipment is calculated by the following equations. 
-
-<div>$$Q = {\dot m_{hot}}{c_p}\left( {{T_{hot}} - {T_{return}}} \right)$$</div>
-
-<div>$$\Delta E = Q\Delta t$$</div>
-
-where
-
-<span>\(Q\)</span>= heating rate
-
-<span>\({c_p}\)</span>= specific heat of water
-
-<span>\(\Delta E\)</span>= heating energy
-
-<span>\(\Delta t\)</span>= time interval
-
-The heating rate and energy for the WaterUse:Connections is the sum of the values for its constituent water equipment objects.  If the WaterUse:Connections object is stand-alone, all heating is assigned to "Purchased Heating" by the individual water equipment objects.  If the WaterUse:Connections object is coupled to a plant loop, all heating is supplied by the plant loop equipment.
-
-### Drainwater Heat Recovery
-
-Drainwater heat recovery adds one more complication to the water connections subsystem.  A heat exchanger is added between the drain and the waste outlet to recover some heat from the water before it leaves the system.  The heat is usually recovered by preheating the incoming makeup water from the mains.
-
-The heat exchanger can be modeled as "ideal", "counterflow", or "crossflow".  One common type of drainwater heat exchanger is the gravity-film exchanger (GFX).  The GFX can be approximated with a counterflow heat exchanger.
-
-The destination of the preheated makeup water can be plumbed in three possible configurations:  "plant", "equipment", "plant and equipment".  In the "plant" configuration, all preheated water flow is returned to the plant loop to match the makeup water for the hot water supply flow.  In the "equipment" configuration, all preheated water flow is directed internally within the WaterUse:Connections object to provide the makeup water for the cold water supply flow for the local water use equipment.  In the "plant and equipment" configuration, the preheated water is split between both of the previous configurations.  This is the only configuration where the flow rate is equal on both sides of the heat exchanger.
-
-![Water Use Connections ENG Diagram 4](media/image7054.png)
-
-Figure 318. Water Use Connections Subsystem with Drainwater Heat Recovery
-
-The new variables added here are defined as:
-
-<span>\({\dot M_{recovery}}\)</span>= makeup water mass flow rate in the heat exchanger
-
-<span>\({T_{recovery}}\)</span>= water temperature leaving the heat exchanger
-
-<span>\({T_{makeup}}\)</span>= cold makeup water temperature supplied to various flows
-
-Another subroutine is inserted into the solution method:
-
-* *InitConnectionsTemps*
-
-* *CalcConnectionsFlowRates*
-
-* *CalcConnectionsDrainTemp*
-
-* ***CalcConnectionsHeatRecovery***
-
-* *UpdateConnectionsNodes*
-
-For the "equipment" and "plant and equipment" configurations, the solution requires iteration to solve because the preheated water leaving the heat exchanger is connected to the cold water supply water, creating a feedback loop.
-
-#### Calculate Connections Heat Recovery
-
-Based on the selected configuration, the flow rate through the heat exchanger is first determined.  For the "plant" configuration, <span>\({\dot M_{recovery}} = {\dot M_{hot}}\)</span>.  For the "equipment" configuration, <span>\({\dot M_{recovery}} = {\dot M_{cold}}\)</span>.  For the "plant and equipment" configuration, <span>\({\dot M_{recovery}} = {\dot M_{hot}} + {\dot M_{cold}}\)</span>.
-
-The heat capacity rates on both sides of the heat exchanger are calculated and the minimum and maximum heat capacity rates, <span>\({C_{min}}\)</span> and <span>\({C_{max}}\)</span>, are determined.
-
-<div>$${C_{drain}} = {\dot M_{drain}}{c_p}$$</div>
-
-<div>$${C_{recovery}} = {\dot M_{recovery}}{c_p}$$</div>
-
-<div>$${C_{min}} = MIN({C_{drain}},{C_{recovery}})$$</div>
-
-<div>$${C_{max}} = MAX({C_{drain}},{C_{recovery}})$$</div>
-
-<div>$${R_c} = \frac{{{C_{min}}}}{{{C_{max}}}}$$</div>
-
-where <span>\({R_c}\)</span> = the heat capacity ratio.
-
-The effectiveness <span>\(\varepsilon \)</span> is then calculated for the given type of heat exchanger.  For the "ideal" heat exchanger, <span>\(\varepsilon  = 1\)</span>.
-
-For the "counterflow" and "crossflow" heat exchangers, the effectiveness is calculated using the effectiveness-NTU method, where:
-
-<div>$$NTU = \frac{{UA}}{{{C_{min}}}}$$</div>
-
-For the "counterflow" heat exchanger:
-
-<span>\(\varepsilon  = \frac{{NTU}}{{1 + NTU}}\)</span>, if <span>\({R_c}\)</span> = 1
-
-<span>\(\varepsilon  = \frac{{1 - EXP\left( { - NTU\left( {1 - {R_c}} \right)} \right)}}{{1 - {R_c}EXP\left( { - NTU\left( {1 - {R_c}} \right)} \right)}}\)</span>, if <span>\({R_c}\)</span> &lt; 1
-
-For the "crossflow" heat exchanger:
-
-<div>$$\varepsilon  = 1 - EXP\left( {\frac{{NT{U^{0.22}}}}{{{R_c}}}\left( {EXP\left( { - {R_c}NT{U^{0.78}}} \right) - 1} \right)} \right)$$</div>
-
-The heat recovery rate is then calculated.
-
-<div>$${Q_{recovery}} = \varepsilon {C_{min}}\left( {{T_{drain}} - {T_{makeup}}} \right)$$</div>
-
-The outlet water temperatures can then be calculated for both sides of the heat exchanger.
-
-<div>$${T_{recovery}} = {T_{makeup}} + \frac{{{Q_{recovery}}}}{{{{\dot M}_{recovery}}{c_p}}}$$</div>
-
-<div>$${T_{waste}} = {T_{drain}} - \frac{{{Q_{recovery}}}}{{{{\dot M}_{drain}}{c_p}}}$$</div>
-
-At each iteration the difference between <span>\({T_{recovery}}\)</span> and <span>\({T_{cold}}\)</span>is compared and checked for convergence.
-
-<div>$$\Delta {T_{error}} = \left| {{T_{recovery}} - {T_{cold}}} \right|$$</div>
-
-Once the temperatures have converged, the solution is complete.  <span>\({T_{waste}}\)</span> is then passed on to a storage tank, if specified.
-
-Zone Controls <a name="ZoneControls"></a>
--------------
-
-### Thermostatic Zone Control
-
-The input object ZoneControl:Thermostat provides a way for the zone to be controlled to a specified temperature.  ZoneControl:Thermostat references a control type schedule and one or more control type objects which in turn reference one or more setpoint schedules.
-
-The control type schedule and the list of control type/name pairs are directly related.  The schedule defines the type of control that is to be used during for each hour.  Valid control types are
-
-0 - Uncontrolled (No specification or default)
-
-1 - Single Heating Setpoint
-
-2 - Single Cooling SetPoint
-
-3 - Single Heating/Cooling Setpoint
-
-4 - Dual Setpoint (Heating and Cooling) with deadband
-
-If the schedule referenced in the ZoneControl statement has a value of 4 for a particular hour, this indicates that during that hour "dual setpoint with deadband control" is to be used.  The specific "dual setpoint with deadband" control object to be used is specified in the list of control type/name pairs.  Then the specific control type objects reference the thermostat setpoint temperature schedule to be used.  Because only one control can be specified for each control type in a ZoneControl statement, there are only four pairs possible in a particular ZoneControl type/name list.  This is because individual controls can be defined hourly, thus giving the user a full range of flexibility.  Since putting in the name of the control type directly in the schedule would be very cumbersome, the control types are assigned a number which is used in the hourly schedule profile.
-
-For more information see ZoneControl:Thermostat in the Input Output Reference and succeeding sections in this document.
-
-### Zone Thermostats
-
-The schema for the current set of four zone thermostats is given below.  In each case, the keyword is accompanied by an identifying name and either one or two schedule names (depending on whether the control is a single or dual setpoint control).  The schedule defines a temperature setpoint for the control type.  The schedule would be defined through the standard schedule syntax described earlier in this document.  For an uncontrolled zone no thermostat is specified or necessary.  See the Input Output Reference for more details.
-
-The control type schedule and the list of control type/name pairs are directly related.  The schedule defines the type of control that is to be used during for each hour.  Valid Control Types are
-
-<table class="table table-striped">
-<tr>
-<td>Control Type Value</td>
-<td>Control Type Name</td>
-</tr>
-<tr>
-<td>0</td>
-<td>Uncontrolled (No specification or default)</td>
-</tr>
-<tr>
-<td>1</td>
-<td>Single Heating Setpoint (input object ThermostatSetpoint:SingleHeating)</td>
-</tr>
-<tr>
-<td>2</td>
-<td>Single Cooling SetPoint (input object ThermostatSetpoint:SingleCooling)</td>
-</tr>
-<tr>
-<td>3</td>
-<td>Single Heating/Cooling Setpoint (input object ThermostatSetpoint:SingleHeatingOrCooling)</td>
-</tr>
-<tr>
-<td>4</td>
-<td>Dual Setpoint (Heating and Cooling) with deadband (input object ThermostatSetpoint:DualSetpoint)</td>
-</tr>
-
-</table>
-
-For the Uncontrolled case no heating or cooling requirement is calculated for the system to meet.
-
-CASE (0)
-
-  ! Uncontrolled Zone
-
-  LoadToHeatingSetPoint = 0.0
-
-  LoadToCoolingSetPoint = 0.0
-
-  ZoneSysEnergyDemand(ZoneNum)%TotalOutputRequired = 0.0
-
-For the Single Heating Setpoint there would be a heating only thermostat.  The setpoint can be scheduled and varied throughout the simulation but only heating is allowed with this control type.
-
-CASE (SingleHeatingSetPoint)
-
-  ! Determine zone load based on
-
-  ! Qload + Qsys = 0 and Qsys = mCp(Tsys-Tzone)
-
-  ! System Load Sign Convention:
-
-  !     - -&gt; Cooling required to reach setpoint
-
-  !     + -&gt; Heating required to reach setpoint
-
-
-
-  LoadToHeatingSetPoint = (TempDepZnLd(ZoneNum) \*
-
-                           TempZoneThermostatSetPoint(ZoneNum) –
-
-                           TempIndZnLd(ZoneNum))
-
-
-
-  IF ((ZoneSysEnergyDemand(ZoneNum)%TotalOutputRequired - 1.0) &lt; 0.0) THEN
-
-    DeadBandOrSetback(ZoneNum) = .TRUE.
-
-  ENDIF
-
-For the Single Cooling Setpoint there would be a cooling only thermostat.  The setpoint can be scheduled and varied throughout the simulation but only cooling is allowed with this control type.
-
-CASE (SingleCoolingSetPoint)
-
-
-
-  LoadToCoolingSetPoint = (TempDepZnLd(ZoneNum) \*
-
-                           TempZoneThermostatSetPoint(ZoneNum) –
-
-                           TempIndZnLd(ZoneNum))
-
-
-
-  ZoneSysEnergyDemand(ZoneNum)%TotalOutputRequired = LoadToCoolingSetPoint
-
-
-
-  IF ((ZoneSysEnergyDemand(ZoneNum)%TotalOutputRequired + 1.0) &gt; 0.0) THEN
-
-    DeadBandOrSetback(ZoneNum) = .TRUE.
-
-  ENDIF
-
-For the Single Heat Cool Setpoint there would be a cooling only thermostat there would be a heating and cooling thermostat.  The setpoint can be scheduled and varied throughout the simulation for both heating and cooling. With this control type only 1 setpoint profile is needed or used.
-
-CASE (SingleHeatCoolSetPoint)
-
-
-
-  LoadToHeatingSetPoint = (TempDepZnLd(ZoneNum) \*
-
-                           TempZoneThermostatSetPoint(ZoneNum) –
-
-                           TempIndZnLd(ZoneNum))
-
-  LoadToCoolingSetPoint = (TempDepZnLd(ZoneNum) \*
-
-                           TempZoneThermostatSetPoint(ZoneNum) –
-
-                           TempIndZnLd(ZoneNum))
-
-
-
-! Possible combinations:
-
-! 1/  LoadToHeatingSetPoint &gt; 0 & LoadToCoolingSetPoint &gt; 0 --&gt;  Heating required
-
-! 2/  LoadToHeatingSetPoint &gt; 0 & LoadToCoolingSetPoint &lt; 0 --&gt;  Not Feasible
-
-! 3/  LoadToHeatingSetPoint &lt; 0 & LoadToCoolingSetPoint &lt; 0 --&gt;  Cooling Required
-
-! 4/  LoadToHeatingSetPoint &lt; 0 & LoadToCoolingSetPoint &gt; 0 --&gt;  Dead Band Operation
-
-
-
-  IF (LoadToHeatingSetPoint &gt; 0.0 .AND. LoadToCoolingSetPoint &gt; 0.0) THEN
-
-    ZoneSysEnergyDemand(ZoneNum)%TotalOutputRequired = LoadToHeatingSetPoint
-
-    ZoneSetPoint = ZoneThermostatSetPointLo(ZoneNum)
-
-  ELSEIF (LoadToHeatingSetPoint &lt; 0.0 .AND. LoadToCoolingSetPoint &lt; 0.0) THEN
-
-    ZoneSysEnergyDemand(ZoneNum)%TotalOutputRequired = LoadToCoolingSetPoint
-
-    ZoneSetPoint = ZoneThermostatSetPointHi(ZoneNum)
-
-  ELSEIF (LoadToHeatingSetPoint &lt; 0.0 .AND. LoadToCoolingSetPoint &gt; 0.0) THEN
-
-    ZoneSysEnergyDemand(ZoneNum)%TotalOutputRequired = 0.0
-
-    IF(Zone(ZoneNum)%SystemZoneNodeNumber &gt; 0) THEN
-
-      ZoneSetPoint = Node(Zone(ZoneNum)%SystemZoneNodeNumber)%Temp
-
-    ENDIF
-
-    DeadBandOrSetback(ZoneNum) = .TRUE.
-
-  ENDIF
-
-For Dual Setpoint with DeadBand there would be a heating and cooling thermostat.  For this case both a heating and cooling setpoint can be scheduled for any given time period.  The setpoint can be scheduled and varied throughout the simulation for both heating and cooling.
-
-CASE (DualSetPointWithDeadBand)
-
-
-
-  LoadToHeatingSetPoint = (TempDepZnLd(ZoneNum) \*
-
-                           ZoneThermostatSetPointLo(ZoneNum) –
-
-                           TempIndZnLd(ZoneNum))
-
-  LoadToCoolingSetPoint = (TempDepZnLd(ZoneNum) \*
-
-                           ZoneThermostatSetPointHi(ZoneNum) –
-
-                           TempIndZnLd(ZoneNum))
-
-
-
-! Possible combinations:
-
-! 1/  LoadToHeatingSetPoint &gt; 0 & LoadToCoolingSetPoint &gt; 0 --&gt;  Heating required
-
-! 2/  LoadToHeatingSetPoint &gt; 0 & LoadToCoolingSetPoint &lt; 0 --&gt;  Not Feasible
-
-! 3/  LoadToHeatingSetPoint &lt; 0 & LoadToCoolingSetPoint &lt; 0 --&gt;  Cooling Required
-
-! 4/  LoadToHeatingSetPoint &lt; 0 & LoadToCoolingSetPoint &gt; 0 --&gt;  Dead Band Operation
-
-  IF (LoadToHeatingSetPoint &gt; 0.0 .AND. LoadToCoolingSetPoint &gt; 0.0) THEN
-
-    ZoneSysEnergyDemand(ZoneNum)%TotalOutputRequired = LoadToHeatingSetPoint
-
-    ZoneSetPoint = ZoneThermostatSetPointLo(ZoneNum)
-
-  ELSEIF (LoadToHeatingSetPoint &lt; 0.0 .AND. LoadToCoolingSetPoint &lt; 0.0) THEN
-
-    ZoneSysEnergyDemand(ZoneNum)%TotalOutputRequired = LoadToCoolingSetPoint
-
-    ZoneSetPoint = ZoneThermostatSetPointHi(ZoneNum)
-
-  ELSEIF (LoadToHeatingSetPoint &lt; 0.0 .AND. LoadToCoolingSetPoint &gt; 0.0) THEN
-
-    ZoneSysEnergyDemand(ZoneNum)%TotalOutputRequired = 0.0
-
-    IF(Zone(ZoneNum)%SystemZoneNodeNumber &gt; 0) THEN
-
-      ZoneSetPoint = Node(Zone(ZoneNum)%SystemZoneNodeNumber)%Temp
-
-    ENDIF
-
-    DeadBandOrSetback(ZoneNum) = .TRUE.
-
-  ENDIF
-
-### Operative Temperature Control
-
-The input object ZoneControl:Thermostat:OperativeTemperature provides a model where the behavior of the zone thermostats described above can be modified to accommodate operative temperature control. The ZoneControl:Thermostat:OperativeTemperature input object is used to modify the behavior of any of the thermostatic control types described above.  When this object is used, the zone can be controlled by a weighted mixture of radiant and air temperatures (rather than just zone air temperatures).
-
-In EnergyPlus, operative temperature, <span>\({T_{OP}}\)</span>, is defined as ,
-
-<div>$${T_{OP}} = \gamma {T_{MRT}} + (1 - \gamma ){T_{drybulb}}$$</div>
-
-where,
-
-<span>\(\gamma \)</span>  is the radiative fraction,
-
-<span>\({T_{MRT}}\)</span> is the mean radiant temperature for the thermal zone, and
-
-<span>\({T_{drybulb}}\)</span>is the mean zone air temperature.
-
-The radiative fraction <span>\(\gamma \)</span> is selected by the user and can be scheduled to vary during the simulation.  A typical value is 0.5.  The maximum value needs to be less than 0.9 and the minimum is 0.0.  A value of 0.0 is the same as controlling on only zone air temperature.  If air velocities are higher than 0.2 m/s, then lower values for radiative fraction might apply.  Niu and Burnett (1998) cite International Standard ISO 77300 in recommending the values for this fraction listed in the following table.
-
-Table 86.  Operative Temperature - Radiative Fraction vs Air Velocity
-
-<table class="table table-striped">
-<tr>
-<td>Air Velocity (m/s)</td>
-<td>&lt; 0.2</td>
-<td>0.2 to 0.6</td>
-<td>0.6 to 1.0</td>
-</tr>
-<tr>
-<td><span>\(\gamma \)</span></td>
-<td>0.5</td>
-<td>0.4</td>
-<td>0.3</td>
-</tr>
-
-</table>
-
-The control is accomplished using the load to setpoint formulation that is fundamental to HVAC system control in EnergyPlus. Although real systems will not know the loads and operate on temperature-based control, EnergyPlus needs to be able to function at zone timesteps up to one hour and this is too long of a timeframe for true temperature-based zone control.  Load-based control is an important method of determining the average HVAC system response to zone conditions over the time step.  For operative temperature control, the same methods and routines are used for calculating loads to setpoints but the setpoints are shifted to emulate operative temperature control rather than air temperature control.
-
-The user-defined setpoint for <span>\({T_{OP}}\)</span> is an input in degrees Celsius. <span>\({T_{MRT}}\)</span> is continually modeled by the full zone heat balance method and includes all the interactions between thermal loads and HVAC systems.  A new setpoint for the zone’s <span>\({T_{drybulb}}\)</span> is obtained for each zone timestep by rearranging the definition of <span>\({T_{OP}}\)</span> to put <span>\({T_{drybulb}}\)</span> on the left hand side.
-
-<div>$${T_{drybulb,setpo{\mathop{\rm int}} }} = \frac{{{T_{OP,setpo{\mathop{\rm int}} }} - \gamma {T_{MRT}}}}{{(1 - \gamma )}}$$</div>
-
-This adjustment to the target zone air drybulb temperature is made every timestep for every zone immediately after the setpoints are obtained from the schedule.
-
-Reference: J. Niu and J. Burnett. 1998. Integrating Radiant/Operative Temperature Controls into Building Energy Simulations. ASHRAE Transactions Vol. 104. Part 2. page 210.  ASHRAE.  Atlanta, GA.
-
-### Temperature And Humidity Control
-
-##### The input object ZoneControl:Thermostat:TemperatureAndHumidity is used to modify the behavior of ZoneControl:Thermostat objects (control types ThermostatSetpoint:SingleCooling and ThermostatSetpoint:DualSetpoint only) based on zone air humidity conditions. Specifically, this TemperatureAndHumidity zone control resets the ZoneControl:Thermostat’s cooling setpoint temperature downward when the zone air relative humidity exceeds the Dehumidifying Relative Humidity Setpoint defined in this object. The reduced cooling setpoint temperature typically results in longer cooling coil runtimes and additional dehumidification. While additional dehumidification (lower absolute humidity level in the zone air) may be achieved, the resulting dry-bulb temperature and absolute humidity of the zone air will determine if the zone air **relative humidity** is reduced.
-
-##### The rate at which the cooling setpoint temperature is reduced is dictated by the user-specified Overcool Control Ratio. The maximum reduction in cooling setpoint temperature is defined by the user-entered Overcool Range, although the Overcool Range may be reduced from the user-defined value when this TemperatureAndHumidity control is used in tandem with a dual setpoint thermostat (see discussion below). Note that occupants are sensitive to overcooling and can experience discomfort if the overcool range is too large.
-
-This control is accomplished using the load to setpoint formulation that is fundamental to HVAC system control in EnergyPlus. Although real systems will not know the loads and operate on temperature-based control, EnergyPlus needs to be able to function at zone timesteps up to one hour and this is too long of a timeframe for true temperature-based zone control. Load-based control is an important method of determining the average HVAC system response to zone conditions over the time step. For TemperatureAndHumidity control, the same methods and routines are used for calculating loads to setpoints but the cooling setpoint is shifted to emulate TemperatureAndHumidity control, as described above.
-
-The overcool range limits the extent of the zone air temperature reduction below the cooling setpoint. When a dual setpoint thermostat is being modified by this TemperatureAndHumidity control, the maximum overcool range must be less than or equal to the temperature difference between the dual setpoint thermostat’s cooling and heating setpoints:
-
-<div>$$\Delta {T_{OvercoolRange,MAX}} = MIN\left( {\Delta {T_{OvercoolRange}},\,\Delta {T_{Setpoints}}} \right)$$</div>
-
-where,
-
-<span>\(\Delta {T_{OvercoolRange,MAX}}\)</span>= maximum overcool range for the zone air (°C)
-
-<span>\(\Delta {T_{OvercoolRange}}\)</span>= overcool range for the zone air (°C).  User input.
-
-<span>\(\Delta {T_{Setpoints}}\)</span>= temperature difference between the cooling and heating setpoints (°C)
-
-If a single cooling setpoint thermostat is being modified by this control, the maximum overcool range is equal to the user-defined overcool range.
-
-The extent that the zone air relative humidity exceeds the user-entered dehumidifying relative humidity setpoint is given by:
-
-<div>$$\Delta \phi  = MAX\left( {0.0,{\phi_{ZoneLagged}} - {\phi_{CSP}}} \right)$$</div>
-
-The actual cooling setpoint reduction (overcooling) is calculated for the condition when the zone air relative humidity exceeds the dehumidifying setpoint (i.e., <span>\(\Delta \phi \)</span>&gt;0), as described below:
-
-<div>$$\begin{array}{l}IF\,\,(\Delta \phi \, > \,0)\,\,THEN\\ ,\,\,\,\,\Delta {T_{Overcool,Actual}} = MIN\left( {\Delta {T_{OvercoolRange,MAX}},\,{{\Delta \phi } \mathord{\left/ {\vphantom {{\Delta \phi } {\Delta {\phi_{adjust}}}}} \right. } {\Delta {\phi_{adjust}}}}} \right)\\ELSE\\ ,\,\,\,\,\Delta {T_{Overcool,Actual}} = 0\\ENDIF\end{array}$$</div>
-
-The cooling setpoint temperature is then adjustedas follows:
-
-<span>\({T_{CSP,adj}} = \left( {{T_{CSP}} - \Delta {T_{Overcool,Actual}}} \right)\)</span>where,
-
-<span>\({T_{CSP,adj}}\)</span>= adjusted cooling setpoint temperature (°C)
-
-<span>\({T_{CSP}}\)</span>= zone air cooling setpoint temperature for the current time step (°C).  User input.
-
-<span>\(\Delta {\phi_{adjust}}\)</span>= user-defined overcool control ratio (%/K)
-
-<span>\(\Delta \phi \)</span>= difference between the zone air relative humidity and the user-defined dehumidifying setpoint (%)
-
-<span>\({\phi_{ZoneLagged}}\)</span> = zone air relative humidity calculated at the last system time step (%)
-
-<span>\({\varphi_{CSP}}\)</span>= dehumidifying relative humidity setpoint at the current time step (%).  User input.
-
-This adjusted cooling setpoint temperature is made every timestep for every zone immediately after the original thermostat setpoint is obtained from the user-defined setpoint schedule.
-
-### Humidistat
-
-The input object ZoneControl:Humidistat provides a way for the zone to be controlled to a single relative humidity setpoint schedule, or dual humidity schedules (humidifying and dehumidifying with deadband). The schedules consist of relative humidities, expressed as a percentage (0-100), to be used for the zone moisture prediction calculation. Only one control statement can be specified for each zone.  Individual relative humidity values can be defined for every time step, thus giving the user a full range of flexibility. For a single setpoint humidistat, if the control relative humidity is below the calculated load and the equipment specified can humidify then that equipment will try and meet the requirement.  The opposite is true if the calculated value is above the setpoint and the equipment can dehumidify. For a dual setpoint humidistat, if the zone relative humidity is below the **humidifying** relative humidity setpoint and the equipment specified can humidify then that equipment will try and meet the zone’s humidification load. The opposite is true if the zone relative humidity is above the **dehumidifying** relative humidity setpoint and the equipment can dehumidify.
-
-If the ZoneControl:Humidistat is used by a furnace or unitary system then no other objects are required. The signal from the humidistat is used directly by that component. If the Zone Control:Humidistat is used to control a Humidifier or used in conjunction with the Controller:Simple object with control variable "TemperatureAndHumidityRatio", then either the “SetpointManager:SingleZone:Humidity:Minimum�, “SetpointManager:MultiZone:Humidity:Minimum�,   “SetpointManager:SingleZone:Humidity:Maximum� or “SetpointManager:MultiZone:Humidity:Maximum� objects are required to determine a setpoint for those components to meet for the single setpoint humidistat. For a dual setpoint humidistat, a minimum humidity setpoint manager object  (“SetpointManager:SingleZone:Humidity:Minimum� or “SetpointManager:MultiZone:Humidity:Minimum�) and a maximum humidity setpoint manager object (“SetpointManager:SingleZone:Humidity:Maximum� or “SetpointManager:MultiZone:Humidity:Maximum�) are required to determine the setpoints for the corresponding humidification and dehumidification components. Note that the “SetpointManager:Scheduled� object can also be used to directly set humidity ratio setpoints on the exit node of the humidifier component.
-
-For the single setpoint humidistat case, the model takes into account all of the moisture gains and/or losses from sources except the HVAC system contribution, and then calculates a moisture removal or addition rate based on the provided setpoint value, like the temperature predictor. The algorithm uses a 3rd Order derivative to predict zone moisture addition or removal to smooth the changes using the zone air capacitance. Positive values of moisture load mean that this amount of moisture must be added to the zone to reach the setpoint. Negative values represent the amount of moisture that must be removed by the system.
-
-<div>$${\rm{MoistLoadHumidSetPoint = massflow}}\cdot {\rm{HumidityRatio = kg air/sec}}\cdot {\rm{kg }}{{\rm{H}}_{\rm{2}}}{\rm{O/kg air = kg }}{{\rm{H}}_{\rm{2}}}{\rm{O/sec}}$$</div>
-
-This routine also calculates the zone required humidity ratio, Wsetpoint, which is required and takes into account the zone multiplier. At this time the Wsp is not stored in a derived type to make it available for SetpointManagers. It was setup to be analogous to the temperature thermostat.
-
-For the dual setpoint humidistat case, the model takes into account all of the moisture gains and/or losses from sources except the HVAC system contribution, and then calculates moisture addition and removal rates based on the provided humidifying and dehumidifying setpoint values, like the temperature predictor. The algorithm uses a Third Order Backward Difference , Analytical Solution, or Euler Method in subroutine CalcPredictedHumidityRatio to predict zone moisture addition and removal to smooth the changes using the zone air capacitance. The program calculates the humidifying (addition) and dehumidifying (removal) moisture loads based on the specified humidifying and dehumidifying setpoints, respectively. The calculated humidifying moisture load is passed to subroutine CalcSingZoneMinHumSetPoint and CalcMultiZoneMinHumSetPoint in the SetpointManager module to calculate the requested supply air humidity ratio at the setpoint node (Ref. SetpointManager:SingleZone:Humidity:Minimum and SetpointManager:MultiZone:Humidity:Minimum objects). The calculated dehumidifying moisture load is passed to subroutine CalcSingZoneMaxHumSetPoint and CalcMultiZoneMaxHumSetPoint in the SetpointManager module to calculate the requested supply air humidity ratio at the setpoint node (Ref. SetpointManager:SingleZone:Humidity:Maximum and SetpointManager:MultiZone:Humidity:Maximum objects). At the same time, the dehumidifying load is also passed directly to a furnace or unitary system if it is defined for the simulation, and that system will operate to meet this load based on its configuration and control settings.
-
-### Thermal Comfort Zone Control
-
-The input object ZoneControl:Thermostat:ThermalComfort provides a way for the zone to be controlled to a specified temperature based on a selected thermal comfort model.  ZoneControl:Thermostat:ThermalComfort references a thermal comfort control type schedule and one or more thermal comfort control type objects which in turn reference one or more setpoint schedules.
-
-The thermal comfort control type schedule and the list of thermal comfort control type/name pairs are directly related.  The schedule defines the type of thermal comfort control that is to be used during for each simulation time step.  Valid Control Types are
-
-<table class="table table-striped">
-<tr>
-<td>Control Type</td>
-<td>Control Type Name/Object</td>
-</tr>
-<tr>
-<td>0</td>
-<td>No thermal comfort control</td>
-</tr>
-<tr>
-<td>1</td>
-<td>ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating</td>
-</tr>
-<tr>
-<td>2</td>
-<td>ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling</td>
-</tr>
-<tr>
-<td>3</td>
-<td>ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling</td>
-</tr>
-<tr>
-<td>4</td>
-<td>ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint</td>
-</tr>
-
-</table>
-
-If the schedule referenced in the ZoneControl statement has a value of 4 for a particular time step, this indicates that during that time step "ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint� control is to be used.  The specific "ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint" control object to be used is specified in the list of thermal comfort control type/name pairs.  Then the specific thermal comfort control type objects reference the thermal comfort PMV setpoint schedule to be used.  Because only one thermal comfort control can be specified for each thermal comfort control type in a ZoneControl statement, there are only four pairs possible in a particular ZoneControl type/name list.  This is because individual thermal comfort controls can be defined for specific times, thus giving the user a full range of flexibility.  Since putting in the name of the thermal comfort control type directly in the schedule would be very cumbersome, the thermal comfort control types are assigned a number which is used in the schedule profile.
-
-For more information see ZoneControl:Thermostat:ThermalComfort in the InputOutput Reference and Zone Fanger Thermal Comfort in the Engineering Documentation.
-
-#### Zone Control Based on Fanger Thermal Comfort
-
-The syntax for the current set (4) of zone thermal comfort control types is given below. In each case, the keyword is accompanied by an identifying name and either one or two schedule names (depending on whether the control type is a single or dual setpoint control). The schedule defines a PMV setpoint for the control type. The schedule would be defined through the standard schedule syntax described earlier in this document. For an uncontrolled thermal comfort zone, no Fanger thermal comfort object is specified or necessary. See the Input Output Reference for more details.
-
-The control type schedule and the list of control type/name pairs are directly related.  The schedule defines the type of control that is to be used during for each hour.  Valid Control Types are
-
-<table class="table table-striped">
-<tr>
-<td>Control Type</td>
-<td>Control Type Name/Object</td>
-</tr>
-<tr>
-<td>0</td>
-<td>No thermal comfort control</td>
-</tr>
-<tr>
-<td>1</td>
-<td>ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating</td>
-</tr>
-<tr>
-<td>2</td>
-<td>ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling</td>
-</tr>
-<tr>
-<td>3</td>
-<td>ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling</td>
-</tr>
-<tr>
-<td>4</td>
-<td>ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint</td>
-</tr>
-
-</table>
-
-For the no thermal comfort control (uncontrolled) case, the control will revert to thermostat control if specified. If the thermal comfort control is specified as “uncontrolled� for a particular period and thermostat control is not specified in the input, then conditions will float.
-
-For the ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating case there would be a heating only thermal comfort setpoint temperature.  The setpoint is calculated based on the selected thermal comfort model and varied throughout the simulation but only heating is allowed with this thermal comfort control type.
-
-      CASE (Single Thermal Comfort Heating Setpoint:Fanger)
-
-      TempControlType(ZoneNum)= SingleHeatingSetpoint
-
-      TempZoneThermostatSetPoint(ZoneNum) = Calculated Zone Setpoint from Fanger heating setpoint PMV
-
-For the ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling case there would be a cooling only thermal comfort setpoint temperature.  The setpoint is calculated based on the selected thermal comfort model and varied throughout the simulation but only cooling is allowed with this thermal comfort control type.
-
-      CASE (Single Thermal Comfort Cooling Setpoint:Fanger)
-
-
-
-      TempControlType(ZoneNum)= SingleCoolingSetPoint
-
-      TempZoneThermostatSetPoint(ZoneNum) = Calculated Zone Setpoint from Fanger cooling setpoint PMV
-
-For the ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling there would be heating and cooling thermal comfort zone control objects.  The setpoint is calculated based on the selected thermal comfort model and varied throughout the simulation for both heating and cooling. With this thermal comfort control type only 1 setpoint profile is needed or used.
-
-      CASE (Single Thermal Comfort Heating Cooling Setpoint:Fanger)
-
-
-
-      TempControlType(ZoneNum)= SingleHeatCoolSetPoint
-
-      TempZoneThermostatSetPoint(ZoneNum) = Calculated Zone Setpoint from Fanger heating and cooling
-
-                                            setpoint PMV
-
-For ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint there would be heating and cooling thermal comfort control objects.  For this case both a heating and cooling setpoint can be calculated based on the selected thermal comfort model for any given time period.  The thermal comfort setpoint temperature can be varied throughout the simulation for both heating and cooling.
-
-      CASE (Dual Thermal Comfort Setpoint with Deadband:Fanger)
-
-
-
-      TempControlType(ZoneNum)= DualSetPointWithDeadBand
-
-      ZoneThermostatSetPointLo(ZoneNum) = Calculated Zone Setpoint from Fanger heating setpoint PMV
-
-      ZoneThermostatSetPointHi(ZoneNum) = Calculated Zone Setpoint from Fanger cooling setpoint PMV
-
-Zone Equipment and Zone Forced Air Units <a name="ZoneEquip"></a>
-----------------------------------------
-
-### Air Distribution Terminal Unit
-
-#### Overview
-
-The ZoneHVAC:AirDistributionUnit is a special piece of zone equipment – it connects centrally conditioned air with a zone. It encompasses the various types of air terminal units in EnergyPlus: *AirTerminal:DualDuct:ConstantVolume*, *AirTerminal:SingleDuct:VAV:Reheat*, etc. It is a generalized component that accesses the calculations for the different types of air terminal unit.
-
-#### Model
-
-The air distribution function is encapsulated in the module *ZoneAirEquipmentManager*. The object and module function only to invoke the individual air terminal unit simulations.
-
-#### Inputs and Data
-
-The data for this unit consists of the unit name, the air outlet node name (which should be the same as one of the zone inlet nodes), the type of air terminal unit (air distribution equipment), and the name of the air terminal unit.
-
-All input data for air distribution units is stored in the array *AirDistUnit* in data module *DataDefineEquip*.
-
-#### Calculation
-
-There is no calculation associated with ZoneHVAC:AirDistributionUnit.
-
-#### Simulation and Control
-
-*SimZoneAirLoopEquipment* in module *ZoneAirEquipmentManager* calls the individual air terminal unit simulations.
-
-#### References
-
-No specific references.
-
-### Inlet Side Mixer Air Terminal Unit
-
-#### Overview
-
-The input object AirTerminal:SingleDuct:InletSideSideMixer provides a means for using a zonal air conditioning unit as a terminal unit by mixing central system conditioned air with the inlet air stream of the zonal unit. Usually the central system would be a Direct Outside Air System (DOAS) providing centrally conditioned ventilation air to the zones.
-
-#### Model
-
-The inlet side mixer uses the equations for adiabatic mixing of two moist air streams. Namely, dry air mass balance, water mass balance, and enthalpy balance.
-
-#### Inputs and Data
-
-The only input data are the name and type of the zonal air conditioning unit plus the node names of the 2 input air nodes and the outlet air node. No flow rate data is needed.
-
-All input data for the inlet side mixer air terminal unit is stored in the data structure *SysATMixer*.
-
-#### Calculation
-
-The following equations for the mixing of two moist air streams are used:
-
-<div>$${\dot m_{da1}}{h_1} + {\dot m_{da2}}{h_2} = {\dot m_{da3}}{h_3}$$</div>
-
-<div>$${\dot m_{da1}} + {\dot m_{da2}} = {\dot m_{da3}}$$</div>
-
-<div>$${\dot m_{da1}}{W_1} + {\dot m_{da2}}{W_2} = {\dot m_{da3}}{W_3}$$</div>
-
-where <span>\({\dot m_{da}}\)</span>is dry air mass flow rate in kg/s, *h* is specific enthalpy in J/kg, and W is humidity ratio in (kg of water)/(kg of dry air).
-
-In this case, the outlet air mass flow rate has been set by the zonal unit. The air mass flow rate of one of the inlets - the primary air from the central system - is also known. So the air mass balance equation is used to obtain the secondary air mass flow rate.
-
-The inlet conditions - specific enthalpy and humidity ratio - for both inlet air streams are known. Now that both inlet air streams' mass flow rate is known, the enthalpy and water mass balance equations are used to get the outlet conditions.
-
-#### Simulation and Control
-
-The inlet side mixer model is invoked from within the zonal AC model. Basically the inlet side mixer becomes a subcomponent of the zonal unit model. This allows the zonal unit to allow for the mixing of central supply air with its inlet stream in calculating how much cooling or heating it needs to do in order to meet the zone load.
-
-#### References
-
-See Chapter 1, page 1.17 of the 2013 ASHRAE Handbook of Fundamentals
-
-### Supply Side Mixer Air Terminal Unit
-
-#### Overview
-
-The input object AirTerminal:SingleDuct:SupplySideSideMixer provides a means for using a zonal air conditioning unit as a terminal unit by mixing central system conditioned air with the outlet air stream of the zonal unit. Usually the central system would be a Direct Outside Air System (DOAS) providing centrally conditioned ventilation air to the zones.
-
-#### Model
-
-The supply side mixer uses the equations for adiabatic mixing of two moist air streams. Namely, dry air mass balance, water mass balance, and enthalpy balance. In this case the inlet conditions and flow rates are known so the outlet condition and flow rate is calculated.
-
-#### Inputs and Data
-
-The only input data are the name and type of the zonal air conditioning unit plus the node names of the 2 input air nodes and the outlet air node. No flow rate data is needed.
-
-All input data for the supply side mixer air terminal unit is stored in the data structure *SysATMixer*.
-
-#### Calculation
-
-Given the needed inputs, the output is calculated in subroutine *CalcATMixer*. The input flow rates, humidity ratios, and enthalpies are taken from the inlet nodes' data. The balance equations are then used to calculate the outlet flow rate and conditions:
-
-<div>$${\dot m_{da1}}{h_1} + {\dot m_{da2}}{h_2} = {\dot m_{da3}}{h_3}$$</div>
-
-<div>$${\dot m_{da1}} + {\dot m_{da2}} = {\dot m_{da3}}$$</div>
-
-<div>$${\dot m_{da1}}{W_1} + {\dot m_{da2}}{W_2} = {\dot m_{da3}}{W_3}$$</div>
-
-where <span>\({\dot m_{da}}\)</span>is dry air mass flow rate in kg/s, *h* is specific enthalpy in J/kg, and W is humidity ratio in (kg of water)/(kg of dry air).
-
-#### Simulation and Control
-
-The supply side mixer model is invoked from within the zonal AC model. Basically the supply side mixer becomes a subcomponent of the zonal unit model. This allows the zonal unit to allow for the mixing of central supply air with its outlet stream in calculating how much cooling or heating it needs to do in order to meet the zone load.
-
-#### References
-
-See Chapter 1, page 1.17 of the 2013 ASHRAE Handbook of Fundamentals
-
-### Simple Duct Leakage Model
-
-#### Overview
-
-The input object ZoneHVAC:AirDistributionUnit also provides access to a model for duct leakage that can be a significant source of energy inefficiency in forced-air HVAC systems. Evaluating duct leakage energy losses can involve considerable user effort and computer resources if an airflow network is defined through a detailed description of the system components and airflow paths (including leakage paths). A nonlinear pressure-based solver is used to solve for pressures and flow rates in the network. By making certain assumptions and approximations for certain well defined configurations, however, it is possible to obtain accurate results with a simple mass and energy balance calculation and thus avoid the input and calculation costs of doing a full pressure-based airflow network simulation.
-
-The Simple Duct Leakage Model (SDLM) assumes a central VAV air conditioning system with a constant static pressure setpoint. The model assumes that the leaks are in the supply ducts and that the system returns air through a ceiling plenum that contains the ducts. Thus, the ducts leak into the return plenum, and this part of the supply does not reach the conditioned zones. With the additional assumptions described below, it is possible to model this configuration with heat and mass balance equations and avoid the use of a nonlinear pressure-based solver. In the EnergyPlus context, this means that use of AirflowNetwork is avoided and the leakage calculations are obtained in the course of the normal thermal simulation.
-
-#### Principles and Description
-
-Constant Flow Rate
-
-The airflow rate through a duct leak is a function of the pressure difference between the duct and the surrounding space:
-
-<div>$${\dot V_{leak}} = {C_1} \cdot \Delta p_{duct - space}^n$$</div>
-
-The exponent *n* is 0.5 for leaks that look like orifices (holes that are large relative to the thickness of the duct wall); for leaks that resemble cracks (e.g., lap joints), *n* is approximately 0.6 to 0.65.
-
-For a duct with constant flow rate and a linear pressure drop through the duct, the average static pressure in the duct will equal half of the duct static pressure drop. Assuming turbulent flow in the duct, the duct pressure drop is proportional to the square of the airflow through the duct. This can be expressed as:
-
-<div>$$\Delta {p_{duct - space}} = \frac{{\Delta {p_{duct}}}}{2} = {C_2}\left( {\frac{{\dot V_{duct}^2}}{2}} \right)$$</div>
-
-Combining equations and and assuming the leaks are large holes (*n* equals 0.5). gives:
-
-<div>$${\dot V_{leak}} = {C_1} \cdot \Delta p_{duct - space}^{0.5} = {C_3} \cdot {\dot V_{duct}}$$</div>
-
-where
-
-<div>$${C_3} = {C_1} \cdot {({C_2}/2)^{0.5}}$$</div>
-
-Thus the leakage fraction *C*<sub>3</sub> remains constant regardless of the duct flow rate or static pressure. This result depends on the following assumptions:
-
-·        the duct airflow is turbulent;
-
-·        the duct pressure varies linearly along the duct;
-
-·        the average duct pressure approximates the pressure drop across the duct;
-
-·        the leaks are large and have pressure exponent 0.5.
-
-Effects of Constant Pressure Upstream and Variable Flow and Pressure Downstrean
-
-Commonly VAV systems maintain a constant static pressure at some point in the duct system upstream of the VAV terminal units. That is, airflow rate will vary depending on the cooling requirement, but a constant pressure will be maintained at the static pressure sensor. Consequently, the leakage flow for a leak upstream of the VAV boxes will be approximately constant. Or to put it another way, the leakage fraction will vary in proportion to the flow rate.
-
-For leaks downstream of the VAV terminal units, the airflow through the duct and the pressure in the downstream duct will vary as the box damper modulates in response to the differential between the room temperature and the thermostat setpoint. In this case, the situation is similar to the constant flow case: for an orifice-like leak, the pressure difference across the leak will vary linearly with the air speed (or flow rate); i.e., the leakage fraction will be approximately constant.
-
-SDLM
-
-For SDLM, our leakage model is then:
-
-·        for leaks upstream of the terminal units, the leakage flow rate will be constant;
-
-·        for leaks downstream of the terminal units, the leakage fraction will be constant.
-
-This model assumes, in addition to the assumptions given above, that the VAV system is controlled to a constant static pressure setpoint. In EnergyPlus SDLM is not currently applicable to systems using static pressure reset. Using SDLM would require knowledge of static pressure as a function of system air flow rate.
-
-#### Inputs and Data
-
-User data for the SDLM is entered through The ZoneHVAC:AirDistributionUnit (ADU) object. There are 2 data items per ADU:
-
-1.    the upstream nominal leakage fraction;
-
-2.    the downstream fixed leakage fraction.
-
-Both inputs are leakage fractions. Input (1) is the leakage fraction at design flow rate, which together can be used to determine the constant leakage flow rate upstream of the VAV boxes; this leakage fraction varies with the flow rate. Input (2) is a fixed leakage fraction and is constant as the flow rate varies.
-
-#### Implementation
-
-The various zone mass flow rates are related in the following manner.
-
-<div>$${\dot m_{s,us}} = {\dot m_{tu}} + {\dot m_{lk,us}}$$</div>
-
-<div>$${\dot m_{tu}} = {\dot m_{lk,ds}} + {\dot m_{s,z}}$$</div>
-
-<div>$${\dot m_{lk,us}} = Fra{c_{us}} \cdot {\dot m_{s,us,max}}$$</div>
-
-<span>\({\dot m_{lk,ds}} = Fra{c_{ds}} \cdot {\dot m_{tu}}\)</span>                                                                                <span>\(\)</span>
-
-Here
-
-<span>\({\dot m_{s,us}}\)</span>is the constant zone supply air mass flow rate upstream of the leaks [kg/s];
-
-<span>\({\dot m_{tu}}\)</span>is the air mass flow rate through the terminal unit [kg/s];
-
-<span>\({\dot m_{lk,us}}\)</span>is the upstream leakage air mass flow rate [kg/s];
-
-<span>\({\dot m_{lk,ds}}\)</span>is the downstream leakage air mass flow rate [kg/s];
-
-<span>\({\dot m_{s,us,max}}\)</span>is the maximum upstream supply air mass flow rate (program input) [kg/s];
-
-<span>\({\dot m_{s,z}}\)</span>is the supply air mass flow rate delivered to the zone [kg/s];
-
-<span>\(Fra{c_{us}}\)</span>is the design upstream leakage fraction (program input);
-
-<span>\(Fra{c_{ds}}\)</span>is the constant downstream leakage fraction (program input);
-
-<span>\({\dot m_{tu}}\)</span>is calculated in the VAV terminal unit model in the usual manner: the mass flow rate is varied to meet the zone load. The limits on the mass flow rate variation are set by the <span>\({\dot m_{MaxAvail}}\)</span> and <span>\({\dot m_{MinAvail}}\)</span>values stored at the terminal unit’s air inlet node. To account for upstream leakage the maximum air mass flow rate available is reset to:
-
-<div>$${\dot m'_{MaxAvail}} = {\dot m_{MaxAvail}} - {\dot m_{lk,us}}$$</div>
-
-Downstream leakage must also be accounted for because not all of <span>\({\dot m_{tu}}\)</span>will reach the zone. This is done by having <span>\({\dot m_{tu}}\)</span>meet an adjusted zone load:
-
-<div>$${\dot Q_{z,adjusted}} = \frac{1}{{1 - Fra{c_{ds}}}}{\dot Q_z}$$</div>
-
-Here <span>\({\dot Q_z}\)</span>[watts] is the actual zone load (met by <span>\({\dot m_{s,z}}\)</span>) and <span>\({\dot Q_{z,adjusted}}\)</span>is the load used in the VAV terminal unit model to obtain <span>\({\dot m_{tu}}\)</span>.
-
-Once <span>\({\dot m_{tu}}\)</span> is known, all the other flow rates can be calculated. <span>\({\dot m_{s,us}}\)</span>is assigned to the air distribution unit’s air inlet node and <span>\({\dot m_{s,z}}\)</span>is assigned to the unit’s air outlet node. Thus, air mass flow is not conserved through the unit: the two air leakage flow rates disappear. These two vanished flow rates are stored in the air distribution unit data structure. When the downstream return air plenum mass and energy balances are calculated, the leakage flow rate data is accessed and added back in as inlets to the return air plenum. Thus, the overall air system preserves a mass balance.
-
-#### References
-
-Wray, C.P. 2003. “Duct Thermal Performance Models for Large Commercial Buildings�, Lawrence Berkeley National Laboratory Report to the California Energy Commission. LBNL-53410.
-
-Wray, C.P. and N.E. Matson. 2003. “Duct Leakage Impacts on VAV System Performance in California Large Commercial Buildings�, Lawrence Berkeley National Laboratory Report to the California Energy Commission. LBNL-53605.
-
-Wray, C.P., R.C. Diamond, and M.H. Sherman. 2005. “Rationale for Measuring Duct Leakage Flows in Large Commercial Buildings�. Proceedings – 26th AIVC Conference, Brussels, Belgium, September. LBNL-58252.
-
-### Fan Coil Unit
-
-#### Overview
-
-The input object ZoneHVAC:FourPipeFanCoil provides a model for a 4 pipe fan coil zonal hydronic unit that can supply heating and cooling to a zone. It contains a hot water or electric heating coil, a chilled water coil, and a fan. It can supply a fixed amount of outdoor air, but cannot operate in an economizer mode. The fan runs at constant speed – control is achieved by throttling the hot or cold water flow. The fan coil configuration and control is rather limited. The fan position is always *blow-through*, control is always by varying the water flow, never by holding the water flow constant and cycling the fan.
-
-#### Model
-
-The 4 pipe fan coil unit is modeled as a compound component consisting of 4 sub-components: an outdoor air mixer, a fan, a cooling coil, and a heating coil. In terms of EnergyPlus objects these are:
-
-1.    *OutdoorAir:Mixer*
-
-2.    *Fan:ConstantVolume*
-
-3.    *Coil:Cooling:Water, Coil:Cooling:Water:DetailedGeometry,* or *CoilSystem:Cooling:Water:HeatExchangerAssisted*
-
-4.    *Coil:Heating:Water or Coil:Heating:Electric*
-
-The unit is a forward model: its inputs are defined by the state of its inlets: namely its 2 air streams – recirculated and outdoor air. The outputs of the model are the conditions of the outlet air stream: flow rate, temperature and humidity ratio. The unit data and simulation are encapsulated in the module *FanCoilUnits.*
-
-#### Inputs and Data
-
-The user describes the 4 pipe fan coil unit by inputting the names of the outdoor air mixer, the fan, the heating coil, and the cooling coil. The heating and cooling coil types must also be specified.
-
-The unit is connected to the overall HVAC system by specifying node names for the unit air inlet (for recirculated air) node, air outlet node, outdoor air node, relief node, inlet hot water node, and inlet chilled water node. The individual components comprising the fan coil must also be input and connected together properly. Specifically the outdoor air mixer mixed air node must be the same as the fan inlet node; the fan outlet node must be the same as the cooling coil air inlet node; the cooling coil air outlet node must be the same as the heating coil air inlet node; and the heating coil air outlet node must be the same as the unit air outlet node; the outdoor air mixer inlet nodes must match the unit inlet nodes; and the outdoor air mixer relief node must match the unit relief node.
-
-The user needs to also specify (unless the unit is autosized) various maximum flow rates: the supply air flow rate, the outdoor air inlet flow rate, the maximum (and minimum) chilled water flow rate, and the maximum (and minimum) hot water flow rate. Heating and cooling convergence tolerances need to be specified or defaulted. And there is an on/off availability schedule for the unit.
-
-All the input data for the fan coil unit is stored in the array *FanCoil*.
-
-#### Calculation
-
-Given the needed inputs, the output is calculated in subroutine *Calc4PipeFanCoil*. The temperature, humidity ratio and flow rate of the recirculated and outdoor air streams are taken from the inlet air nodes The inlet hot and chilled water flow rates have been set by local controllers – temperatures are taken from the inlet water nodes. Then
-
-1.    The outdoor air mixer is simulated (Call *SimOAMixer*);
-
-2.    the fan is simulated (Call *SimulateFanComponents*);
-
-3.    the cooling coil is simulated (Call *SimulateWaterCoilComponents* or *SimHXAssistedCoolingCoil*);
-
-4.    the heating coil is simulated (Call *SimulateWaterCoilComponents or SimulateHeatingCoilComponents*).
-
-The load met (sensible cooling or heating) is calculated and passed back to the calling routine:
-
-   <span>\({\dot Q_{sens,out}} = {\dot m_{tot}}\cdot ({\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{out}}{\rm{,}}{{\rm{W}}_{{\rm{in}}}}{\rm{) - }}{\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{in}},{W_{in}}))\)</span>
-
-where *PsyHFnTdbW* is the EnergyPlus function for calculating the specific enthalpy of air given the drybulb temperature and the humidity ratio. The subscript *in* indicates the conditions at the inlet recirculated air node.
-
-#### Simulation and Control
-
-From the result of the zone simulation we have the current heating/cooling demand on the unit <span>\({\dot Q_{z,req}}\)</span>. The first step is to decide whether the unit is on for the current time step. If the load is less than 1 watt or the flow rate is less than .001 kg/s, the unit is off. If the availability schedule is off, the mass flow rate is set to zero, so the second condition holds. When the unit is off there will be no air flow through the unit and outlet conditions will be equal to inlet conditions.
-
-<span>\({\dot Q_{z,req}}\)</span> is not the demand on the heating or cooling coil. To obtain the actual coil load, we need to calculate the unit output with no heating or cooling by the coils (<span>\({\dot Q_{unit,no{\rm{ }}hc}}\)</span>). We obtain this by calling *Calc4PipeFanCoil* with the water flow rates set to zero. Then the coil loads are calculated:
-
-<div>$${\dot Q_{hc}} = {\dot Q_{z,hsp}} - {\dot Q_{unit,no{\rm{ }}hc}}$$</div>
-
-<div>$${\dot Q_{cc}} = {\dot Q_{z,csp}} - {\dot Q_{unit,no{\rm{ }}hc}}$$</div>
-
-where <span>\({\dot Q_{hc}}\)</span>is the heating coil load, <span>\({\dot Q_{z,hsp}}\)</span>is the current zone load to the heating setpoint, <span>\({\dot Q_{cc}}\)</span>is the cooling coil load, and <span>\({\dot Q_{z,csp}}\)</span>is the current zone load to the cooling setpoint.
-
-If the unit is on and <span>\({\dot Q_{cc}}\)</span>&lt; 0 and the thermostat type is not “single heating setpoint�, *ControlCompOutput* is called with the control node set to the cold water inlet node. *ControlCompOutput* is a general component control routine. In this case calls *Calc4PipeFanCoil* repeatedly while varying the cold water flow rate and minimizing <span>\(({\dot Q_{sens,out}} - {\dot Q_{z,csp}})/{\dot Q_{z,csp}}\)</span>to within the cooling convergence tolerance. Similarly if the unit is on and <span>\({\dot Q_{hc}}\)</span>&gt;0 and the thermostat type is not “single cooling setpoint�, *ControlCompOutput* is called with the control node set to the hot water inlet node (for hydronic heating coil only). *ControlCompOutput* varies the hot water flow rate or the electric heating coil part-load ratio is varied to minimize <span>\(({\dot Q_{sens,out}} - {\dot Q_{z,hsp}})/{\dot Q_{z,hsp}}\)</span> to within the heating tolerance. *ControlCompOutput* executes a slow but safe interval halving algorithm to do its minimization. Once control is achieved, the total cooling/heating output is calculated:
-
-     <span>\({\dot Q_{tot,out}} = \dot m\cdot ({\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{out}},{W_{out}}) - {\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{in,}}{W_{in}})\)</span>
-
-
-##### Multi-Speed Fan In FanCoil
-
-When modeling multi-speed fan in FanCoil unit, capacity is modulated using speed ratio or part load ratio.  The supply air fan speed is varied while operating the coils at maximum water flow. When there is no system load to meet, the water control valve is fully closed. When the FanCoil fan is cycling between two consecutive fan speed levels a speed ratio is calculated, but when the FanCoil unit cycles between the minimum fan speed and off-position, then part load ratio is calculated. The fan may be off or run continuously at lowest speed to provide ventilation air depending the fan operating schedule specified. When the FanCoil is operating at the lowest fan speed (Speed = 1), the water flow rate is reported as the average for the time step by multiplying the maximum water flow by part load ratio. The speed ratio and part-load ratio are calculated such that the FanCoil unit satisfies the required system zone cooling or heating load.The set of equations used for the multi-speed fan capacity control methods in FanCoil unit are summarized next.
-
-###### Cycling Between Speeds
-
-When the supply fan is cycling between consecutive speeds, then the speed ratio (SR) and the average mass flow rate are calculated as follows:
-
-<div>$${SR_{n}} = Abs({SystemLoad} - {FullLoadOutput_{n-1}}) / Abs({FullLoadOutput_{n}} - {FullLoadOutput_{n-1}})$$</div>
-<div>$${\dot m} = {\dot m_{on, n}} {SR_{n}} + {\dot m_{on, n-1}} (1 - {SR_{n}})$$</div>
-<div>$${\dot m{w}} = {\dot m_{w, max}}$$</div>
-
-###### Cycling OnOff at Lowest Speed
-
-The average supply air flow rate calculation when the fan is running at the lowest fan speed level depends on the fan operating schedule and load. The fan coil unit part load ratio is given by:
-
-<div>$${PLR} = Abs({SystemLoad} - {NoLoadOutput}) / Abs({FullLoadOutput_{1}} - {NoLoadOutput})$$</div>
-
-
-####### Continuous Fan
-
-<div>$${\dot m} = {\dot m_{on, 1}} {PLR} + {\dot m_{off}} (1 - {PLR})$$</div>$$
-
-####### Cycling Fan:
-
-<div>$${\dot m} = {\dot m_{on, 1}} {PLR}$$</div>$$
-<div>$${\dot m{w}} = {\dot m_{w, max}} * {PLR}$$</div>$$
-
-where:
-
-{SR_{n}}		=	 speed ratio of the fan coil unit at speed n, (-)
-
-{PLR}			=	 part load ratio of the fan coil uni at speed 1, (-)
-
-{\dot m}		=	 average mass flow rate of supply air, (kg/s
-
-{\dot m_{on, n-1}}	=	mass flow rate of supply air at fan speed level n-1, (kg/s)
-
-{\dot m_{on, n}}}	=	mass flow rate of supply air at fan speed level n, (kg/s)
-
-{\dot m_{off}}	=	mass flow rate of supply air when the coils are off, (kg/s)
-
-{\dot m_{w}}	=	 average mass flow rate of chilled or hot water, (kg/s)
-
-{\dot m_{w, max}}	=	maximum or full mass flow rate of chilled or hot water, (kg/s)
-
-SystemLoad 	= system load to be met by the fan coil unit, (W)
-
-{FullLoadOutput_{n-1}} 	= fully load fan coil unit output at fan speed level n-1, (W)
-
-{FullLoadOutput_{n}} 	= fully load fan coil unit output at fan speed level n, (W)
-
-##### ASHRAE 90.1
-
-The ASHRAE90.1 control method uses a simple technique to adjust fan speed based on zone design sensible load. The specific section of the Standard is described as:
-
-    Section 6.4.3.10 (“Single Zone Variable-Air-Volume Controls�) of ASHRAE Standard 90.1-2010.
-    HVAC systems shall have variable airflow controls as follows:
-    (a) Air-handling and fan-coil units with chilled-water cooling coils and supply fans with motors 
-        greater than or equal to 5 hp shall have their supply fans controlled by two-speed motors or
-        variable-speed drives. At cooling demands less than or equal to 50%, the supply fan controls
-        shall be able to reduce the airflow to no greater than the larger of the following:
-        • One-half of the full fan speed, or
-        • The volume of outdoor air required to meet the ventilation requirements of Standard 62.1.
-    (b) Effective January 1, 2012, all air-conditioning equipment and air-handling units with direct
-        expansion cooling and a cooling capacity at AHRI conditions greater than or equal to 110,000
-        Btu/h that serve single zones shall have their supply fans controlled by two-speed motors or
-        variable-speed drives. At cooling demands less than or equal to 50%, the supply fan controls
-        shall be able to reduce the airflow to no greater than the larger of the following:
-        • Two-thirds of the full fan speed, or
-        • The volume of outdoor air required to meet the ventilation requirements of Standard 62.1.
-
-This control method assumes that a simulation sizing run is performed to determine the zone design sensible cooling and heating load <span>\({\dot Q_{z,design}}\)</span>.
-
-For fan coil units, the limit used to determine if reduced zone loads are met with reduced fan speed is the fan coil's Low Speed Supply Air Flow Ratio input.
-
-<div>$${\dot Q_{reduced}} = {\dot Q_{z,design}} * {Ratio_{fan,low{\rm{ }}speed}}$$</div>
-
-If the zone load, <span>\({\dot Q_{z,req}}\)</span>, is less than <span>\({Q_{reduced}}\)</span> then the fan is maintained at the reduced speed while the water coils (or electric heating coil) are modulated to meet the zone load.
-
-If the zone load is greater than the design zone sensible load, <span>\({\dot Q_{z,design}}\)</span>, the fan will operate at the maximum supply air flow rate and the water or electric heating coils will modulate to meet the zone load.
-
-If the zone load is between these two extremes, the fan and coil will modulate to meet the zone load.
-
-An example of the ASHRAE 90.1 control method is provided in the following figure. In this figure, the X-axis represents the zone cooling (-) or heating (+) load.
-
-![](media/SZVAV_Fan_Control_FanCoil.jpg)<br>
-Single-Zone VAV Fan Control for Fan Coil Units
-
-#### References
-
-No specific references.
-
-
-
-### Window Air Conditioner
-
-#### Overview
-
-The input object ZoneHVAC:WindowAirConditioner provides a model for a window air conditioner unit that is a packaged unit that supplies cooling to a zone (it is part of zone equipment, not part of the air loop equipment). It contains a fan, a DX cooling coil, and an outdoor air inlet. The coil meets the cooling load by cycling on/off. The fan can operate continuously or cycle on/off in conjunction with the coil.
-
-#### Model
-
-The window air conditioner is modeled as a compound component consisting of 3 sub-components: an outdoor air mixer, a fan, and a DX coil. In terms of EnergyPlus objects these are OutdoorAir:Mixer, Fan:ConstantVolume or Fan:OnOff, and Coil:Coolilng:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted. The unit is a forward model: its inputs are defined by the state of its inlets: namely its 2 air streams – recirculated and outdoor air. The outputs of the model are the conditions of the outlet air stream: flow rate, temperature and humidity ratio. The model is also an averaged model: the performance of the unit is averaged over the time step. That is, the unit is assumed to cycle on/off during the time step and this on/off cycling is averaged over the simulation time step. The unit data and simulation are encapsulated in the module WindowAC.
-
-#### Inputs and Data
-
-The user describes the window air conditioner by inputting the names of the outdoor air mixer, the fan, and the cooling coil. The user can also choose fan placement – blow through or draw through; fan operation – cycling or continuous; and cooling coil type – normal DX or DX with heat exchanger assistance.
-
-The connectivity of the unit needs to be specified: a recirculated (inlet) air node (same as a zone exhaust node); an air outlet node (same as a zone inlet node); an outdoor air inlet node; and a relief air node. The individual components comprising the window air conditioner must of course also be input and connected together properly. For instance, for a blow through fan configuration the outdoor air mixer mixed air node must be the same as the fan inlet node; the fan outlet node must be the same as the coil inlet node; the coil outlet node must be the same as the unit outlet node; the outdoor air mixer inlet nodes must match the unit inlet nodes; and the outdoor air mixer relief node must match the unit relief node.
-
-The user also specifies the air conditioner flow rate delivered to the zone (when cycled on) and the outdoor air flow rate. The user also needs to specify an availability schedule for the unit (this is an on/off schedule).
-
-Note that there is no input specifying the unit’s design cooling capacity. This is an input in the DX coil object and is not repeated here.
-
-All the input data for the window air conditioner is stored in the array *WindAC*.
-
-#### Calculation
-
-Given the needed inputs, the output is calculated in subroutine CalcCyclingWindowAC. The temperature, humidity ratio and flow rate of the recirculated and outdoor air streams are taken from the inlet air nodes. The part load ratio is specified by the calling routine. Then
-
-·        The outdoor air mixer is simulated (Call SimOAMixer);
-
-·        For blow-through fan position:
-
-·        the fan is simulated (Call SimulateFanComponents);
-
-·        the coil is simulated (Call SimDXCoil or SimHXAssistedCoolingCoil).
-
-For draw-through fan position, the simulation order of the fan and coil is reversed. Note that data is never explicitly passed between the sub-components. This is all handled automatically by the node connections and the data stored on the nodes.
-
-#### Simulation and Control
-
-From the result of the zone simulation we have the heating/cooling demand on the unit <span>\({\dot Q_{z,req}}\)</span>. The first step is to decide whether the unit is on for the current time step. For a unit with a cycling fan, the entire unit is assumed to be off if there is no cooling load, the cooling load is very small (less than 1 watt), the unit is scheduled off, or the zone temperature is in the deadband. For a unit with a continuous flow the fan operates if the unit is scheduled on, whether or not there is a cooling demand. The coil however only operates if there is a cooling demand and the zone temperature is not in the deadband.
-
-If the unit is determined to be on, the next step is to find the unit part load fraction that will satisfy the cooling load. This is done in *ControlCycWindACOutput*. In this routine *CalcCyclingWindowAC*  is first called with part load fraction equal to 0, then with part load fraction equal to 1. These calls establish the minimum and maximum cooling output possible by the unit given the current conditions. An initial estimate of the part load fraction is then made:
-
-<div>$$PLF = ({\dot Q_{z,req}} - {\dot Q_{out,min}})/|{\dot Q_{out,max}} - {\dot Q_{out,min}}|$$</div>
-
-Since the unit’s cooling output is a nonlinear function of the part load fraction, this *PLF* will not give exactly the desired <span>\({\dot Q_{z,req}}\)</span>. To obtain the exact *PLF* that will give <span>\({\dot Q_{z,req}}\)</span>, it is necessary to iteratively call *CalcCyclingWindowAC*, varying *PLF* until the desired cooling output is obtained, within the error tolerance specified by the user in the input.
-
-Once *PLF* is determined, *ControlCycWindACOutput* is exited. One last call to *CalcCyclingWindowAC* is made to establish the final outlet conditions at the unit’s air outlet node. Finally, the inlet and outlet node conditions are used to calculate the reporting variables: sensible and total cooling output.
-
-<div>$${\dot Q_{sens,out}} = \dot m\cdot ({\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{out}},{W_{in}}) - {\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{in,}}{W_{in}}))$$</div>
-
-<div>$${\dot Q_{sens,out}} = \dot m\cdot ({\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{out}},{W_{out}}) - {\mathop{\rm PsyHFnTdbW}\nolimits} ({T_{in,}}{W_{in}})$$</div>
-
-where *PsyHFnTdb* is the EnergyPlus function giving enthalpy as a function of temperature and humidity ratio.
-
-#### References
-
-No specific references.
-
-
-
-### Packaged Terminal Air Conditioner
-
-#### Overview
-
-The input object ZoneHVAC:PackagedTerminalAirConditioner provides a model for a packaged terminal air conditioner (PTAC) that is a compound object made up of other components. Each PTAC consists of an outdoor air mixer, direct expansion (DX) cooling coil, heating coil (gas, electric, hot water, or steam) and a supply air fan. While the figure below shows the PTAC with draw through fan placement, blow through fan placement can also be modeled by positioning the supply air fan between the outdoor air mixer and DX cooling coil. The packaged terminal air conditioner coordinates the operation of these components and is modeled as a type of zone equipment (Ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
-
-![PTAC\_Drawthrough](media/image7172.png)
-
-Figure 319. Schematic of a Packaged Terminal Air Conditioner with Draw Through Fan Placement
-
-The PTAC conditions a single zone and is controlled by a thermostat located in that zone. The PTAC operates to meet the zone sensible cooling or sensible heating requirements as dictated by the thermostat schedule. The model calculates the required part-load ratio for the air conditioner’s coils and the supply air fan to meet the cooling/heating requirements. The heating or cooling energy provided by the PTAC is delivered to the zone via the zone air inlet node.
-
-The PTAC is able to model supply air fan operation in two modes: cycling fan – cycling coil (i.e., AUTO fan) and continuous fan – cycling coil (i.e., fan ON). Supply air fan operation is coordinated with the use of a supply air fan operating mode schedule. Schedule values of 0 denote cycling fan operation (AUTO fan). Schedule values other than 0 denote continuous fan operation (fan ON). Fan:OnOff must be used to model AUTO fan (i.e. if schedule values of 0 occur in the supply air fan operating mode schedule), while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON (i.e. if schedule values of 0 do not occur in the supply air fan operating mode schedule). The supply air fan operating mode schedule specified for the PTAC overrides the operating mode specified in the DX cooling coil object.
-
-Output variables reported by the PTAC object include the supply air fan part-load ratio, the air conditioner’s part-load ratio (cooling or heating), and the electric consumption of the PTAC. Additional output variables report the total zone heating rate and the total zone cooling rate provided by the air conditioner. The sensible and latent components of zone cooling are also available as output variables. Reporting of other variables of interest for the PTAC (DX coil cooling rate, coil heating rate, crankcase heater power, fan power, etc.) is done by the individual system components (fan, DX cooling coil and heating coil).
-
-#### Model Description
-
-As described previously, the PTAC conditions a single zone and is controlled by a zone thermostat (ZoneControl:Thermostatic). Each simulation time step, EnergyPlus performs a zone air heat balance to determine if cooling or heating is required to meet the thermostat setpoints, excluding any impacts from PTAC operation. PTAC performance is then modeled with all heating/cooling coils off but the supply air fan operates as specified by the user. If the zone air heat balance plus the impact of PTAC operation with coils off results in no requirement for heating or cooling by the PTAC coils, or if the PTAC is scheduled off (via its availability schedule), then the PTAC coils do not operate and the air conditioner’s part-load ratio output variable is set to 0. If the model determines that cooling or heating is required and the PTAC is scheduled to operate, the model calculates the average air flow rate through the unit and the part-load ratio of the cooling and heating coils in order to meet the thermostat setpoint temperature.
-
-The remainder of this section describes the calculations performed during the latter situation, when cooling or heating coil operation is required. For any HVAC simulation time step, the PTAC can only be cooling or heating, not both. Because the PTAC cycles its coil(s) on and off to meet the required load, the coil(s) operate for a portion of the time step and are off for the rest of the time step. If the user specifies continuous fan operation (i.e. supply air fan operating mode schedule value is greater than 0), then the supply air fan continues to operate at a user-specified flow rate even during periods when the coils cycle off. If the user specifies AUTO fan operation (i.e. supply air fan operating mode schedule value is equal to 0), then the supply air fan cycles on and off with the coils. The model accounts for these variations in air flow through the PTAC within a simulation time step when it determines the total cooling or heating energy delivered to the zone, the average supply air conditions and air flow rate, and the energy consumed by the air conditioner.
-
-#### Cooling Operation
-
-If EnergyPlus determines that the air conditioner must supply cooling to the zone in order to meet the zone air temperature setpoint, then the model first calculates the PTAC’s sensible cooling rate to the zone under two conditions: when the unit runs at full-load (steady-state) conditions and when the DX cooling coil is OFF. If the supply air fan cycles on/off with the compressor, then the sensible cooling rate is zero when the cooling coil is OFF. However if the fan is configured to run continuously regardless of coil operation, then the sensible cooling rate will not be zero when the cooling coil is OFF. Calculating the sensible cooling rate involves modeling the supply air fan (and associated fan heat), the outdoor air mixer, and the DX cooling coil. The heating coil is also modeled, but only to pass the air properties and mass flow rate from it’s inlet node to it’s outlet node. For each of these cases (full load and DX cooling coil OFF), the sensible cooling rate delivered to the zone by the PTAC is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{cooling,\,max\,}} = \left( {{{\mathop m\limits^ \bullet  }_{\,SA,full\,\,load}}} \right){\left( {{h_{out,\,full\,\,load}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{cooling,\,min\,}} = \left( {{{\mathop m\limits^ \bullet  }_{\,SA,coil\,\,off}}} \right){\left( {{h_{out,\,coil\,\,off}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-where:
-
-<span>\({\mathop Q\limits^ \bullet_{cooling,\,max\,}}\)</span> = maximum PTAC sensible cooling rate with cooling coil ON, W
-
-<span>\({\mathop m\limits^ \bullet_{\,SA,full\,\,load}}\)</span> = supply air mass flow rate at full-load (steady-state) conditions, kg/s
-
-*h<sub>out,\\ full\\ load</sub>* = enthalpy of air exiting the PTAC at full-load conditions, J/kg
-
-*h<sub>zone\\ air</sub>*<sub>            </sub> = enthalpy of zone (exhaust) air, J/kg
-
-*HR<sub>min</sub>        =* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the PTAC exiting air or the zone (exhaust) air
-
-<span>\({\mathop Q\limits^ \bullet_{cooling,\,min\,}}\)</span>  = minimum PTAC sensible cooling rate with cooling coil OFF, W
-
-<span>\({\mathop m\limits^ \bullet_{\,SA,coil\,\,off}}\)</span>   = supply air mass flow rate with the cooling coil OFF, kg/s
-
-*h<sub>out,\\ coil\\ off</sub>*  = enthalpy of air exiting the PTAC with the cooling coil OFF, J/kg
-
-
-
-With the calculated PTAC sensible cooling rates and the zone sensible cooling load to be met, the compressor part-load ratio for the PTAC is approximately equal to:
-
-<div>$$PartLoadRatio = MAX\left( {0.0,\frac{{ABS\left( {{{\mathop Q\limits^ \bullet  }_{zone,cooling}} - {{\mathop Q\limits^ \bullet  }_{cooling,\,min\,}}} \right)}}{{ABS\left( {{{\mathop Q\limits^ \bullet  }_{cooling,\,max\,}} - {{\mathop Q\limits^ \bullet  }_{cooling,\,min\,}}} \right)}}} \right)$$</div>
-
-where:
-
-<span>\(PartLoadRatio\)</span>= compressor part-load ratio required to meet the zone load
-
-<span>\({\mathop Q\limits^ \bullet_{zone,cooling}}\)</span> = required zone sensible cooling rate to meet setpoint, W
-
-Since the part-load performance of the DX cooling coil is frequently non-linear (Ref: DX Cooling Coil Model), and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the actual part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the individual PTAC component models) until the PTAC’s cooling output (including on/off cycling effects) matches the zone cooling load requirement.
-
-If the PTAC has been specified with cycling fan/cycling coil (AUTO fan), then the user-defined supply air flow rate during cooling operation (volumetric flow rate converted to mass flow rate) is multiplied by the final PartLoadRatio value to determine the average supply air mass flow rate for the HVAC system simulation time step. For this case, the air conditions (temperature, humidity ratio and enthalpy) at nodes downstream of the cooling coil represent the full-load (steady-state) values when the coil is operating. If the supply air fan is specified to run continuously (fan ON), then the supply air mass flow rate is calculated as the average of the air mass flow rate when the compressor is on and the air mass flow rate when the compressor is off. In this case, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and mixed inlet air conditions when the coil is OFF). Additional discussion regarding the calculation of the average supply air flow and supply air conditions is provided later in this section.
-
-#### Heating Operation
-
-Calculations of the PTAC’s sensible heating rate delivered to the zone at full load and with the heating coil OFF are identical to the calculations described above for cooling operation.
-
-<div>$${\mathop Q\limits^ \bullet_{heating,\,max\,}} = \left( {{{\mathop m\limits^ \bullet  }_{\,SA,full\,\,load}}} \right){\left( {{h_{out,\,full\,\,load}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{heating,\,min\,}} = \left( {{{\mathop m\limits^ \bullet  }_{\,SA,coil\,\,off}}} \right){\left( {{h_{out,\,coil\,\,off}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-where:
-
-<span>\({\mathop Q\limits^ \bullet_{heating,\,max\,}}\)</span> = maximum PTAC sensible heating rate with heating coil ON, W
-
-<span>\({\mathop Q\limits^ \bullet_{heating,\,min\,}}\)</span>  = minimum PTAC sensible heating rate with heating coil OFF, W
-
-
-
-With the calculated PTAC sensible heating rates and the zone sensible heating load to be met, the heating coil part-load ratio for the PTAC is approximately equal to:
-
-<div>$$PartLoadRatio = MAX\left( {0.0,\frac{{ABS\left( {{{\mathop Q\limits^ \bullet  }_{zone,heating}} - {{\mathop Q\limits^ \bullet  }_{heating,\,min\,}}} \right)}}{{ABS\left( {{{\mathop Q\limits^ \bullet  }_{heating,\,max\,}} - {{\mathop Q\limits^ \bullet  }_{heating,\,min\,}}} \right)}}} \right)$$</div>
-
-where:
-
-<span>\(PartLoadRatio\)</span>= heating coil part-load ratio required to meet the zone load
-
-<span>\({\mathop Q\limits^ \bullet_{zone,heating}}\)</span>             = required zone sensible heating rate to meet setpoint, W
-
-
-
-Iterative calculations (successive modeling of the individual PTAC component models) are used to determine the final heating part-load ratio to account for the non-linear performance of the heating coil at part-load conditions and the variation in supply air fan heat for the case of cycling fan/cycling coil (AUTO fan). If heating coil operation at full load is unable to meet the entire zone heating load (e.g., the heating coil capacity is insufficient or the coil is scheduled OFF), the air conditioner’s part-load ratio is set to 1 to meet the zone heating load to the extent possible.
-
-#### Average Air Flow Calculations
-
-The packaged terminal air conditioner operates based on user-specified (or autosized) air flow rates. The PTAC’s supply air flow rate during cooling operation may be different than the supply air flow rate during heating operation. In addition, the supply air flow rate when no cooling or heating is required but the supply air fan remains ON can be different than the air flow rates when cooling or heating is required. The outdoor air flow rates can likewise be different in these various operating modes. The model takes these different flow rates into account when modeling the air conditioner, and the average air flow rate for each simulation time step is reported on the inlet/outlet air nodes of the various PTAC components in proportion to the calculated part-load ratio of the coil.
-
-The average supply air and outdoor air mass flow rates through the air conditioner for the HVAC simulation time step are calculated based on the part-load ratio of the DX cooling coil or heating coil (whichever coil is operating) as follows:
-
-<div>$$\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\,\, = \,\,\mathop m\limits^ \bullet  {\,_{SA,coil\,\,on}}\left( {PartLoadRatio} \right) + \mathop m\limits^ \bullet  {\,_{SA,\,\,coil\,\,off}}\left( {1 - PartLoadRatio} \right)$$</div>
-
-<div>$$\mathop m\limits^ \bullet  {\,_{OA,\,\,avg\,\,}} = \,\,\mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,on}}\left( {PartLoadRatio} \right) + \mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,off}}\left( {1 - PartLoadRatio} \right)$$</div>
-
-where:
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\)</span>      = average supply air mass flow rate during the time step, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,coil\,\,on}}\)</span>   = supply air mass flow rate when the coil is ON, kg/s
-
-*PartLoadRatio* = part-load ratio of the coil (heating or cooling)
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,\,\,coil\,\,off}}\)</span>  = supply air mass flow rate when the coil is OFF, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{OA,\,\,avg\,\,}}\)</span>    = average outdoor air mass flow rate during the time step, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,on}}\)</span>  = average outdoor air mass flow rate when the coil is ON, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,off}}\)</span>  = average outdoor air mass flow rate when the coil is OFF, kg/s
-
-
-
-The supply air and outdoor air flow rates when the DX cooling coil or the heating coil is ON are specified by the user (i.e., supply air volumetric flow rate during cooling operation, supply air volumetric flow rate during heating operation, outdoor air volumetric air flow rate during cooling operation, and outdoor air volumetric air flow rate during heating operation) and are converted from volumetric to mass flow rate. If the user has specified cycling fan operation (i.e. supply air fan operating mode schedule value is equal to 0), then the supply air and outdoor air mass flow rates when the coil is OFF are zero. If the user has specified constant fan operation (i.e. supply air fan operating mode schedule value is greater than 0), then the user-defined air flow rates when no cooling or heating is needed are used when the coil is OFF.
-
-There is one special case. If the supply air fan operating mode schedule value specifies constant fan operation and the user also specifies that the supply air volumetric flow rate when no cooling or heating is needed is zero (or field is left blank), then the model assumes that the supply air and outdoor air mass flow rates when the coil is OFF are equal to the corresponding air mass flow rates when the cooling or heating coil was last operating (ON).
-
-#### Calculation of Outlet Air Conditions
-
-When the supply air fan cycles on and off with the PTAC coils (AUTO fan), the calculated outlet air conditions (temperature, humidity ratio, and enthalpy) from the heating coil or the DX cooling coil at full-load (steady-state) operation are reported on the appropriate coil outlet air node. The air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the part-load ratio of the coil (see Average Air Flow Calculations above).
-
-When the supply air fan operates continuously while the PTAC coils cycle on and off (fan ON), the air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the part-load ratio of the coil (see Average Air Flow Calculations above). Since the air flow rate can be different when the coil is ON compared to when the coil is OFF, then the average outlet air conditions from the heating coil or the DX cooling coil are reported on the appropriate coil outlet air node.
-
-For hot water or steam coils, the water or steam mass flow rate is also proportional to the part-load ratio of the coil regardless of the supply air fan operating mode. Refer to the sections in the document that describe the heating and DX cooling coils for further explanation on how they report their outlet air (and water or steam) conditions.
-
-#### Calculation of Zone Heating and Cooling Rates
-
-At the end of each HVAC simulation time step, this compound object reports the heating or cooling rate and energy delivered to the zone, as well as the electric power and consumption by the air conditioner. In terms of thermal energy delivered to the zone, the sensible, latent and total energy transfer rate to the zone is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{Total}} = \left( {\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\,\,} \right)\left( {{h_{out,\,avg}} - {h_{zone\,\,air}}} \right)$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible}} = \left( {\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\,\,} \right){\left( {{h_{out,\,avg}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Latent}} = {\mathop Q\limits^ \bullet_{Total}} - {\mathop Q\limits^ \bullet_{Sensible}}$$</div>
-
-where:
-
-<sub><span>\({\mathop Q\limits^ \bullet_{Total}}\)</span>           </sub>= total energy transfer rate to the zone, W
-
-<sub><span>\({\mathop Q\limits^ \bullet_{Sensible}}\)</span>        </sub>= sensible energy transfer rate to the zone, W
-
-<sub><span>\({\mathop Q\limits^ \bullet_{Latent}}\)</span>        </sub>= latent energy transfer rate to the zone, W
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\)</span>      = average mass flow rate of the supply air stream, kg/s
-
-*h<sub>out,avg</sub>*       = enthalpy of the air being supplied to the zone, J/kg
-
-
-
-Since each of these energy transfer rates can be calculated as positive or negative values, individual reporting variables are established for cooling and heating and only positive values are reported. The following calculations are representative of what is done for each of the energy transfer rates:
-
-IF (<span>\({\mathop Q\limits^ \bullet_{Total}}\)</span>* &lt; 0.0 )*THEN
-
-                  <span>\({\mathop Q\limits^ \bullet_{TotalCooling}}\)</span> =  ABS (<span>\({\mathop Q\limits^ \bullet_{Total}}\)</span>)
-
-                  <span>\({\mathop Q\limits^ \bullet_{TotalHeating}}\)</span><sub> </sub> =  *0.0*
-
-ELSE
-
-                  <span>\({\mathop Q\limits^ \bullet_{TotalCooling}}\)</span><sub> </sub> =  *0.0*
-
-                  <span>\({\mathop Q\limits^ \bullet_{TotalHeating}}\)</span><sub> </sub> =  <span>\({\mathop Q\limits^ \bullet_{Total}}\)</span>
-
-
-
-where:
-
-<sub><span>\({\mathop Q\limits^ \bullet_{TotalCooling}}\)</span>   </sub>= output variable ‘Packaged Terminal Air Conditioner Total Zone Cooling Rate, W’
-
-<sub><span>\({\mathop Q\limits^ \bullet_{TotalHeating}}\)</span>   </sub>= output variable ‘Packaged Terminal Air Conditioner Total Zone Heating Rate, W’
-
-
-
-In addition to heating and cooling rates, the heating and cooling energy supplied to the zone is also calculated for the time step being reported. The following example for total zone cooling energy is representative of what is done for the sensible and latent energy as well as the heating counterparts.
-
-<div>$$\,{Q_{TotalCooling}} = \,\,{\mathop Q\limits^ \bullet_{TotalCooling}}\,\, * \,\,TimeStepSys\,\, * \,\,3600.$$</div>
-
-where:
-
-<sub><span>\({Q_{TotalCooling}}\)</span>   </sub>= output variable ‘Packaged Terminal Air Conditioner Total Zone Cooling Energy, J’
-
-*TimeStepSys* = HVAC system simulation time step, hr
-
-### Packaged Terminal Heat Pump
-
-#### Overview
-
-The input object ZoneHVAC:PackagedTerminalHeatPump provides a model for a packaged terminal heat pump (PTHP) that is a compound object made up of other components. Each PTHP consists of an outdoor air mixer, direct expansion (DX) cooling coil, DX heating coil, supply air fan, and a supplemental heating coil. While the figure below shows the PTHP with draw through fan placement, blow through fan placement can also be modeled by moving the supply air fan before the DX cooling coil. The packaged terminal heat pump coordinates the operation of these components and is modeled as a type of zone equipment (Ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
-
-![PTHP](media/image7215.png)
-
-Figure 320.  Schematic of a Packaged Terminal Heat Pump (Draw Through Fan Placement)
-
-The PTHP conditions a single zone and is controlled by a thermostat located in that zone. The PTHP operates to meet the zone sensible cooling or sensible heating requirements as dictated by the thermostat schedule. The model calculates the required part-load ratio for the heat pump’s coils and the supply air fan to meet the cooling/heating requirements. The heating or cooling energy provided by the PTHP is delivered to the zone via the zone air inlet node.
-
-The PTHP is able to model supply air fan operation in two modes: cycling fan – cycling coil (i.e., AUTO fan) and continuous fan – cycling coil (i.e., fan ON). Fan:OnOff must be used to model AUTO fan, while Fan:OnOff or Fan:ConstantVolume can be used to model fan ON.
-
-Output variables reported by the PTHP object include the supply air fan part-load ratio, the compressor part-load ratio, and the electric consumption of the PTHP. Additional output variables report the total zone heating rate and the total zone cooling rate provided by the heat pump. The sensible and latent components of zone cooling are also available as output variables. Reporting of other variables of interest for the PTHP (DX coil cooling rate, DX coil heating rate, crankcase heater power, fan power, etc.) is done by the individual system components (fan, DX cooling coil, DX heating coil, and supplemental heating coil).
-
-#### Model Description
-
-As described previously, the PTHP conditions a single zone and is controlled by a zone thermostat (ZoneControl:Thermostat). Each simulation time step, EnergyPlus performs a zone air heat balance to determine if cooling or heating is required to meet the thermostat setpoints, excluding any impacts from PTHP operation. PTHP performance is then modeled with all heating/cooling coils off but the supply air fan operates as specified by the user. If the zone air heat balance plus the impact of PTHP operation with coils off results in no requirement for heating or cooling by the PTHP coils, or if the PTHP is scheduled off (via its availability schedule), then the PTHP coils do not operate and the compressor part-load ratio output variable is set to 0. If the model determines that cooling or heating is required and the PTHP is scheduled to operate, the model calculates the average air flow rate through the unit and the part-load ratio of the cooling and heating coils in order to meet the thermostat setpoint temperature.
-
-The remainder of this section describes the calculations performed during the latter situation, when cooling or heating coil operation is required. For any HVAC simulation time step, the PTHP can only be cooling or heating, not both. Because the PTHP cycles its coil(s) on and off to meet the required load, the coil(s) operate for a portion of the time step and are off for the rest of the time step. If the user specifies continuous fan operation (supply air fan operating mode schedule value &gt; 0), then the supply air fan continues to operate at a user-specified flow rate even during periods when the coils cycle off. If the user specifies AUTO fan operation (supply air fan operating mode schedule value = 0), then the supply air fan cycles on and off with the coils. The model accounts for these variations in air flow through the PTHP within a simulation time step when it determines the total cooling or heating energy delivered to the zone, the average supply air conditions and air flow rate, and the energy consumed by the heat pump.
-
-#### Cooling Operation
-
-If EnergyPlus determines that the heat pump must supply cooling to the zone in order to meet the zone air temperature setpoint, then the model first calculates the PTHP’s sensible cooling rate to the zone under two conditions: when the unit runs at full-load (steady-state) conditions and when the DX cooling coil is OFF. If the supply air fan cycles on/off with the compressor, then the sensible cooling rate is zero when the cooling coil is OFF. However if the fan is configured to run continuously regardless of coil operation, then the sensible cooling rate will not be zero when the cooling coil is OFF. Calculating the sensible cooling rate involves modeling the supply air fan (and associated fan heat), the outdoor air mixer, and the DX cooling coil. The DX heating coil and the gas or electric supplemental heating coil are also modeled, but only to pass the air properties and mass flow rate from their inlet nodes to their outlet nodes. For each of these cases (full load and DX cooling coil OFF), the sensible cooling rate delivered to the zone by the PTHP is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{cooling,\,max\,}} = \left( {{{\mathop m\limits^ \bullet  }_{\,SA,full\,\,load}}} \right){\left( {{h_{out,\,full\,\,load}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{cooling,\,min\,}} = \left( {{{\mathop m\limits^ \bullet  }_{\,SA,coil\,\,off}}} \right){\left( {{h_{out,\,coil\,\,off}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-where:
-
-<span>\({\mathop Q\limits^ \bullet_{cooling,\,max\,}}\)</span> = maximum PTHP sensible cooling rate with cooling coil ON, W
-
-<span>\({\mathop m\limits^ \bullet_{\,SA,full\,\,load}}\)</span> = supply air mass flow rate at full-load (steady-state) conditions, kg/s
-
-*h<sub>out,\\ full\\ load</sub>*   = enthalpy of air exiting the PTHP at full-load conditions, J/kg
-
-*h<sub>zone\\ air</sub>*<sub> \\              </sub> = enthalpy of zone (exhaust) air, J/kg
-
-*HR<sub>min</sub>        =* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio of the PTHP exiting air or the zone (exhaust) air
-
-<span>\({\mathop Q\limits^ \bullet_{cooling,\,min\,}}\)</span>  = minimum PTHP sensible cooling rate with cooling coil OFF, W
-
-<span>\({\mathop m\limits^ \bullet_{\,SA,coil\,\,off}}\)</span>   = supply air mass flow rate with the cooling coil OFF, kg/s
-
-*h<sub>out,\\ coil\\ off</sub>*    = enthalpy of air exiting the PTHP with the cooling coil OFF, J/kg
-
-With the calculated PTHP sensible cooling rates and the zone sensible cooling load to be met, the compressor part-load ratio for the PTHP is approximately equal to:
-
-<div>$$PartLoadRatio = MAX\left( {0.0,\frac{{ABS\left( {{{\mathop Q\limits^ \bullet  }_{zone,cooling}} - {{\mathop Q\limits^ \bullet  }_{cooling,\,min\,}}} \right)}}{{ABS\left( {{{\mathop Q\limits^ \bullet  }_{cooling,\,max\,}} - {{\mathop Q\limits^ \bullet  }_{cooling,\,min\,}}} \right)}}} \right)$$</div>
-
-where:
-
-<span>\(PartLoadRatio\)</span>= compressor part-load ratio required to meet the zone load
-
-<span>\({\mathop Q\limits^ \bullet_{zone,cooling}}\)</span> = required zone sensible cooling rate to meet setpoint, W
-
-Since the part-load performance of the DX cooling coil is frequently non-linear (Ref: DX Cooling Coil Model), and the supply air fan heat varies based on cooling coil operation for the case of cycling fan/cycling coil (AUTO fan), the actual part-load ratio for the cooling coil compressor and fan are determined through iterative calculations (successive modeling of the individual PTHP component models) until the PTHP’s cooling output (including on/off cycling effects) matches the zone cooling load requirement within the cooling convergence tolerance that is specified.
-
-If the PTHP is specified to operate with cycling fan/cycling coil (AUTO fan), then the user-defined supply air flow rate during cooling operation (volumetric flow rate converted to mass flow rate) is multiplied by the final PartLoadRatio value to determine the average supply air mass flow rate for the HVAC system simulation time step. For this case, the air conditions (temperature, humidity ratio and enthalpy) at nodes downstream of the cooling coil represent the full-load (steady-state) values when the coil is operating. If the supply air fan is specified to operate continuously (fan ON), then the supply air mass flow rate is calculated as the average of the air mass flow rate when the compressor is on and the air mass flow rate when the compressor is off. In this case, the air conditions at nodes downstream of the cooling coil are calculated as the average conditions over the simulation time step (i.e., the weighted average of full-load conditions when the coil is operating and mixed inlet air conditions when the coil is OFF). Additional discussion regarding the calculation of the average supply air flow and supply air conditions is provided later in this section.
-
-#### Heating Operation
-
-Calculations of the PTHP’s sensible heating rate delivered to the zone at full load and with the DX heating coil OFF are identical to the calculations described above for cooling operation.
-
-<div>$${\mathop Q\limits^ \bullet_{heating,\,max\,}} = \left( {{{\mathop m\limits^ \bullet  }_{\,SA,full\,\,load}}} \right){\left( {{h_{out,\,full\,\,load}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{heating,\,min\,}} = \left( {{{\mathop m\limits^ \bullet  }_{\,SA,coil\,\,off}}} \right){\left( {{h_{out,\,coil\,\,off}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-where:
-
-<span>\({\mathop Q\limits^ \bullet_{heating,\,max\,}}\)</span> = maximum PTHP sensible heating rate with DX heating coil ON, W
-
-<span>\({\mathop Q\limits^ \bullet_{heating,\,min\,}}\)</span>  = minimum PTHP sensible heating rate with DX heating coil OFF, W
-
-With the calculated PTHP sensible heating rates and the zone sensible heating load to be met, the compressor part-load ratio for the PTHP is approximately equal to:
-
-<div>$$PartLoadRatio = MAX\left( {0.0,\frac{{ABS\left( {{{\mathop Q\limits^ \bullet  }_{zone,heating}} - {{\mathop Q\limits^ \bullet  }_{heating,\,min\,}}} \right)}}{{ABS\left( {{{\mathop Q\limits^ \bullet  }_{heating,\,max\,}} - {{\mathop Q\limits^ \bullet  }_{heating,\,min\,}}} \right)}}} \right)$$</div>
-
-where:
-
-<span>\(PartLoadRatio\)</span>= compressor part-load ratio required to meet the zone load
-
-<span>\({\mathop Q\limits^ \bullet_{zone,heating}}\)</span>             = required zone sensible heating rate to meet setpoint, W
-
-Iterative calculations (successive modeling of the individual PTHP component models) are used to determine the final heating part-load ratio to account for the non-linear performance of the DX heating coil at part-load conditions and the variation in supply air fan heat for the case of cycling fan/cycling coil (AUTO fan). If DX heating coil operating at full load is unable to meet the entire zone heating load (e.g., the DX heating coil capacity is insufficient or the coil is scheduled OFF, or the outdoor temperature is below the PTHP’s minimum outdoor dry-bulb temperature for compressor operation), the supplemental heating coil is activated to meet the remaining zone heating load to the extent possible.
-
-#### Average Air Flow Calculations
-
-The packaged terminal heat pump operates based on user-specified (or autosized) air flow rates. The PTHP’s supply air flow rate during cooling operation may be different than the supply air flow rate during heating operation. In addition, the supply air flow rate when no cooling or heating is required but the supply air fan remains ON can be different than the air flow rates when cooling or heating is required. The outdoor air flow rates can likewise be different in these various operating modes. The model takes these different flow rates into account when modeling the heat pump, and the average air flow rate for each simulation time step is reported on the inlet/outlet air nodes of the various PTHP components in proportion to the calculated part-load ratio of the DX coil compressor.
-
-The average supply air and outdoor air mass flow rates through the heat pump for the HVAC simulation time step are calculated based on the part-load ratio of the DX cooling coil or DX heating coil (whichever coil is operating) as follows:
-
-<div>$$\dot m{\,_{SA,\,\,avg}}\,\, = \,\,\dot m{\,_{SA,comp\,\,on}}\left( {PartLoadRatio} \right) + \dot m{\,_{SA,\,\,comp\,\,off}}\left( {1 - PartLoadRatio} \right)$$</div>
-
-<div>$$\dot m{\,_{OA,\,\,avg\,\,}} = \,\,\dot m{\,_{OA,\,\,comp\,\,on}}\left( {PartLoadRatio} \right) + \dot m{\,_{OA,\,\,comp\,\,off}}\left( {1 - PartLoadRatio} \right)$$</div>
-
-where:
-
-<span>\(\dot m{\,_{SA,\,\,avg}}\)</span>      = average supply air mass flow rate during the time step, kg/s
-
-<span>\(\dot m{\,_{SA,comp\,\,on}}\)</span>  = supply air mass flow rate when the DX coil compressor is ON, kg/s
-
-*PartLoadRatio* = part-load ratio of the DX coil compressor (heating or cooling)
-
-<span>\(\dot m{\,_{SA,\,\,comp\,\,off}}\)</span>            = supply air mass flow rate when the DX coil compressor is OFF, kg/s
-
-<span>\(\dot m{\,_{OA,\,\,avg\,\,}}\)</span>    = average outdoor air mass flow rate during the time step, kg/s
-
-<span>\(\dot m{\,_{OA,\,\,comp\,\,on}}\)</span> = average outdoor air mass flow rate when the DX coil compressor is ON, kg/s
-
-<span>\(\dot m{\,_{OA,\,\,comp\,\,off}}\)</span>= average outdoor air mass flow rate when the DX coil compressor is OFF, kg/s
-
-The supply air and outdoor air flow rates when the DX cooling or DX heating coil compressor is ON are specified by the user (e.g., supply air volumetric flow rate during cooling operation, supply air volumetric flow rate during heating operation, outdoor air volumetric air flow rate during cooling operation, and outdoor air volumetric air flow rate during heating operation) and are converted from volumetric to mass flow rate. If the user has specified cycling fan operation (supply air fan operating mode schedule value = 0), then the supply air and outdoor air mass flow rates when the DX compressor is OFF are zero. If the user has specified constant fan operation (supply air fan operating mode schedule value &gt; 0), then the user-defined air flow rates when no cooling or heating is needed are used when the DX compressor is OFF.
-
-There is one special case. If the user has specified constant fan operation (supply air fan operating mode schedule value &gt; 0) and they specify that the supply air volumetric flow rate when no cooling or heating is needed is zero (or field is left blank), then the model assumes that the supply air and outdoor air mass flow rates when the DX coil compressor is OFF are equal to the corresponding air mass flow rates when the compressor was last operating (ON).
-
-#### Calculation of Outlet Air Conditions
-
-When the supply air fan cycles on and off with the PTHP coils (AUTO fan), the calculated outlet air conditions (temperature, humidity ratio, and enthalpy) from the DX heating or DX cooling coil at full-load (steady-state) operation are reported on the appropriate coil outlet air node. The air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the part-load ratio of the DX coil compressor (see Average Air Flow Calculations above).
-
-When the supply air fan operates continuously while the PTHP coils cycle on and off (fan ON), the air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the part-load ratio of the DX coil compressor (see Average Air Flow Calculations above). Since the air flow rate can be different when the coil is ON compared to when the coil is OFF, then the average outlet air conditions from the DX heating or DX cooling coil are reported on the appropriate coil outlet air node.
-
-Refer to the sections in the document that describe the DX heating and DX cooling coils for further explanation on how they report their outlet air conditions.
-
-#### Calculation of Zone Heating and Cooling Rates
-
-At the end of each HVAC simulation time step, this compound object reports the heating or cooling rate and energy delivered to the zone, as well as the electric power and consumption by the heat pump. In terms of thermal energy delivered to the zone, the sensible, latent and total energy transfer rate to the zone is calculated as follows:
-
-<div>$${\dot Q_{Total}} = \left( {\dot m{\,_{SA,\,\,avg}}\,\,} \right)\left( {{h_{out,\,avg}} - {h_{zone\,\,air}}} \right)$$</div>
-
-<div>$${\dot Q_{Sensible}} = \left( {\dot m{\,_{SA,\,\,avg}}\,\,} \right){\left( {{h_{out,\,avg}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-<div>$${\dot Q_{Latent}} = {\dot Q_{Total}} - {\dot Q_{Sensible}}$$</div>
-
-where:
-
-<sub><span>\({\dot Q_{Total}}\)</span>           </sub>= total energy transfer rate to the zone, W
-
-<sub><span>\({\dot Q_{Sensible}}\)</span>       </sub>= sensible energy transfer rate to the zone, W
-
-<sub><span>\({\dot Q_{Latent}}\)</span>          </sub>= latent energy transfer rate to the zone, W
-
-<span>\(\dot m{\,_{SA,\,\,avg}}\)</span>      = average mass flow rate of the supply air stream, kg/s
-
-*h<sub>out,avg</sub>*         = enthalpy of the air being supplied to the zone, J/kg
-
-Since each of these energy transfer rates can be calculated as positive or negative values, individual reporting variables are established for cooling and heating and only positive values are reported. The following calculations are representative of what is done for each of the energy transfer rates:
-
-IF (<span>\({\dot Q_{Total}}\)</span>*&lt; 0.0 )*THEN
-
-                  <span>\({\dot Q_{TotalCooling}}\)</span> =  ABS (<span>\({\dot Q_{Total}}\)</span>)
-
-                  <span>\({\dot Q_{TotalHeating}}\)</span><sub> </sub> =  *0.0*
-
-ELSE
-
-                  <span>\({\dot Q_{TotalCooling}}\)</span><sub> </sub> =  *0.0*
-
-                  <span>\({\dot Q_{TotalHeating}}\)</span><sub> </sub> =  <span>\({\dot Q_{Total}}\)</span>
-
-where:
-
-<sub><span>\({\dot Q_{TotalCooling}}\)</span>         </sub>= output variable ‘Packaged Terminal Heat Pump Total Zone Cooling Rate, W’
-
-<sub><span>\({\dot Q_{TotalHeating}}\)</span>         </sub>= output variable ‘Packaged Terminal Heat Pump Total Zone Heating Rate, W’
-
-In addition to heating and cooling rates, the heating and cooling energy supplied to the zone is also calculated for the time step being reported. The following example for total zone cooling energy is representative of what is done for the sensible and latent energy as well as the heating counterparts.
-
-<div>$${Q_{TotalCooling}} = {\dot Q_{TotalCooling}}*TimeStepSys*3600.$$</div>
-
-where:
-
-<sub><span>\({Q_{TotalCooling}}\)</span>   </sub>= output variable ‘Packaged Terminal Heat Pump Total Zone Cooling Energy, J’
-
-*TimeStepSys* = HVAC system simulation time step, hr
-
-
-
-### Zone Single Speed Water-To-Air Heat Pump
-
-#### Overview
-
-The input object ZoneHVAC:WaterToAirHeatPump provides a zone equipment model for a water-to-air heat pump that is a “virtual� component consisting of an on/off fan component, a water-to-air heat pump cooling coil, a water-to-air heat pump heating coil, and a gas or electric supplemental heating coil. The specific configuration of the blowthru heat pump is shown in the following figure. For a drawthru heat pump, the fan is located between the water-to-air heat pump heating coil and the supplemental heating coil. In addition, a water-to-air heat pump has a water loop connection on its source side. The water loop can be served by a condenser loop (like GHE for Ground source systems), or by a cooling tower/ boiler plant loop (for water loop systems).
-
-![Schematic\_ZoneWSHP](media/image7258.png)
-
-Figure 321.  Source Side and Load Side Configuration of a Zone WaterToAir Heat Pump
-
-There are two models for zone water-to-air heat pump cooling and heating coils, i.e. Single-Speed and Variable-Speed Equation Fit models. Cooling and heating coils are modeled using the Equation Fit model described here.
-
-#### Single Speed Equation-Fit Model:
-
-This section describes the equation-fit model for Water-to-Air heat pump
-  (Object names: Coil:Cooling:WaterToAirHeatPump:EquationFit and
- Coil:Heating:WaterToAirHeatPump:EquationFit). This documentation is derived from the M.S. dissertation of Tang (2005) which is available on the Oklahoma State University web site . The model uses five non-dimensional equations or curves to predict the heat pump performance in cooling and heating mode. The methodology involves using the generalized least square method to generate a set of performance coefficients from the catalog data at indicated reference conditions. Then the respective coefficients and indicated reference conditions are used in the model to simulate the heat pump performance. The variables or inlet conditions that influenced the water-to-air heat pump performance are load side inlet water temperature, source side inlet temperature, source side water flow rate and load side water flow rate. The governing equations for the cooling and heating mode are as following:
-
-Cooling Mode:
-
-<div>$$\frac{{{Q_{total}}}}{{{Q_{total,ref}}}} = A1 + A2\left[ {\frac{{{T_{wb}}}}{{{T_{ref}}}}} \right] + A3\left[ {\frac{{{T_{w,in}}}}{{{T_{ref}}}}} \right] + A4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + A5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]$$</div>
-
-<div>$$\frac{{{Q_{sens}}}}{{{Q_{sens,ref}}}} = B1 + B2\left[ {\frac{{{T_{db}}}}{{{T_{ref}}}}} \right] + B3\left[ {\frac{{{T_{wb}}}}{{{T_{ref}}}}} \right] + B4\left[ {\frac{{{T_{w,in}}}}{{{T_{ref}}}}} \right] + B5\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + B6\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]$$</div>
-
-<div>$$\frac{{Powe{r_c}}}{{Powe{r_{c,ref}}}} = C1 + C2\left[ {\frac{{{T_{wb}}}}{{{T_{ref}}}}} \right] + C3\left[ {\frac{{{T_{w,in}}}}{{{T_{ref}}}}} \right] + C4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + C5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]$$</div>
-
-Heating Mode:
-
-<div>$$\frac{{{Q_h}}}{{{Q_{h,ref}}}} = E1 + E2\left[ {\frac{{{T_{db}}}}{{{T_{ref}}}}} \right] + E3\left[ {\frac{{{T_{w,in}}}}{{{T_{ref}}}}} \right] + E4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + E5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]$$</div>
-
-<div>$$\frac{{Powe{r_h}}}{{Powe{r_{h,ref}}}} = F1 + F2\left[ {\frac{{{T_{db}}}}{{{T_{ref}}}}} \right] + F3\left[ {\frac{{{T_{w,in}}}}{{{T_{ref}}}}} \right] + F4\left[ {\frac{{{{\dot V}_{air}}}}{{{{\dot V}_{air,ref}}}}} \right] + F5\left[ {\frac{{{{\dot V}_w}}}{{{{\dot V}_{w,ref}}}}} \right]$$</div>
-
-Assuming no losses, the source side heat transfer rate for cooling and heating mode is calculated as following;
-
-<div>$${Q_{source,c}} = {Q_{total}} + Powe{r_c}$$</div>
-
-<div>$${Q_{source,h}} = {Q_h} - Powe{r_h}$$</div>
-
-where:
-
-<span>\(A1 - F5\)</span>     = Equation fit coefficients for the cooling and heating mode
-
-<span>\({{T_{ref}}}\)</span>            = 283K
-
-<span>\({{T_{w,in}}}\)</span>           = Entering water temperature, K
-
-<span>\({{T_{db}}}\)</span>             = Entering air dry-bulb temperature, K
-
-<span>\({{T_{wb}}}\)</span>            = Entering air wet-bulb temperature, K
-
-<span>\({{{\dot V}_{air}}}\)</span>            = Load side air volumetric flow rate, m<sup>3</sup>/s
-
-<span>\({{{\dot V}_{w}}}\)</span>                         = Source side water volumetric flow rate, m<sup>3</sup>/s
-
-<span>\({{Q_{total}}}\)</span>          = Total cooling capacity, W
-
-<span>\({{Q_{sens}}}\)</span>          = Sensible cooling capacity, W
-
-<span>\({Powe{r_c}}\)</span>     = Power consumption (cooling mode), W
-
-<span>\({{Q_{source,c}}}\)</span>      = Source side heat transfer rate (cooling mode), W
-
-<span>\({{Q_{h}}}\)</span>                         = Total heating capacity, W
-
-<span>\({Powe{r_h}}\)</span>     = Power consumption (heating mode), W
-
-<span>\({{Q_{source,h}}}\)</span>      = Source side heat transfer rate (heating mode), W
-
-The inlet conditions or variables are divided by the reference conditions. This formulation allows the coefficients to fall into smaller range of values. Moreover, the value of the coefficient indirectly represents the sensitivity of the output to that particular inlet variable. The reference conditions used when generating the performance coefficients must be the same as the reference conditions used later in the model. The reference temperature <span>\({{T_{ref}}}\)</span>is fixed at 283K. Temperature unit of Kelvin is used instead of Celsius to keep the ratio of the water inlet temperature and reference temperature positive should the water inlet temperature drop below the freezing point.
-
-For cooling mode, the reference conditions; reference load side air volumetric flow rate <span>\(\left( {{{\dot V}_{air,ref}}} \right)\)</span>,reference source side water volumetric flow rate<span>\(\left( {{{\dot V}_{w,ref}}} \right)\)</span>,reference sensible capacity <span>\(\left( {{Q_{sens,ref}}} \right)\)</span> and reference power input <span>\(\left( {Powe{r_{c,ref}}} \right)\)</span> are the conditions when the heat pump is operating at the highest cooling capacity or reference cooling capacity<span>\(\left( {{Q_{total,ref}}} \right)\)</span> indicated in the manufacturer’s catalog. Note that the reference conditions for heating mode might differ from the reference conditions specified for the cooling mode.
-
-#### Coefficient estimation procedure:
-
-The generalized least square method is used to generate the coefficients. This method utilizes an optimization method which calculates the coefficients that will give the least amount of differences between the model outputs and the catalog data. A set of coefficients for the cooling mode is generated which includes A1-A5 for total cooling capacity, B1-B6 for sensible cooling capacity, and C1-C5 for power consumption. The same procedure is repeated for the heating mode to generate the coefficients E1-E5 (total heating capacity) and F1-F5 (power consumption). An information flow chart showing the inputs, reference conditions, performance coefficients and outputs are shown in the figure below:
-
-
-
-![](media/image7286.png)
-
-Figure 322. Information Flow Chart for Water-to-Air Heat Pump Equation Fit Model (Tang 2005)
-
-### Zone Air DX Dehumidifier
-
-#### Overview
-
-This model, object name ZoneHVAC:Dehumidifier:DX, simulates the thermal performance and electric power consumption of conventional mechanical dehumidifiers. These systems use a direct expansion (DX) cooling coil to cool and dehumidify an airstream. Heat from the DX system’s condenser section is rejected into the cooled/dehumidified airstream, resulting in warm dry air being supplied from the unit. In EnergyPlus, this object is modeled as a type of zone equipment (ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
-
-![Dehumidifier\_Schematic](media/image7287.png)
-
-Figure 323. Mechanical Dehumidifier Schematic
-
-The model assumes that this equipment dehumidifies and heats the air. If used in tandem with another system that cools and dehumidifies the zone air, then the zone dehumidifier should be specified as the lowest cooling priority in the ZoneHVAC:EquipmentList object for best control of zone temperature and humidity levels. With this zone equipment prioritization, the other cooling and dehumidification system would operate first to meet the temperature setpoint (and possibly meet the high humidity setpoint as well). If additional dehumidification is needed, then the zone dehumidifier would operate. The sensible heat generated by the dehumidifier is carried over to the zone air heat balance for the next HVAC time step.
-
-#### Model Description
-
-The user must input water removal, energy factor and air flow rate at rated conditions (26.7°C, 60% RH).  Three performance curves must also be specified to characterize the change in water removal and energy consumption at part-load conditions:
-
-1)    Water removal curve (function of inlet air temperature and relative humidity)
-
-2)    Energy factor curve (function of inlet air temperature and relative humidity)
-
-3)    Part load fraction correlation (function of part load ratio)
-
-·        The water removal modifier curve is a biquadratic curve with two independent variables: dry-bulb temperature and relative humidity of the air entering the dehumidifier. The output of this curve is multiplied by the Rated Water Removal to give the water removal rate at the specific entering air conditions at which the dehumidifier is operating (i.e., at temperature/relative humidity different from the rating point conditions). If the output of this curve is negative, then a warning message is issued and it is reset to 0.0.
-
-<div>$$WaterRemovalModFac = \,a + \,b\left( {{T_{in}}} \right)\,\, + \,\,c{\left( {{T_{in}}} \right)^2}\,\, + \,\,d\left( {R{H_{in}}} \right) + e{(R{H_{in}})^2} + f({T_{in}})(R{H_{in}})$$</div>
-
-where
-
-*T<sub>in</sub>*  = dry-bulb temperature of the air entering the dehumidifier, °C
-
-*RH<sub>in</sub>* = relative of the air entering the dehumidifier, % (0-100)
-
-·        The energy factor modifier curve is a biquadratic curve with two independent variables: dry-bulb temperature and relative humidity of the air entering the dehumidifier. The output of this curve is multiplied by the Rated Energy Factor to give the energy factor at the specific entering air conditions at which the dehumidifier is operating (i.e., at temperature/relative humidity different from the rating point conditions). If the output of this curve is negative, then a warning message is issued and it is reset to 0.0.
-
-<div>$$EFModFac = \,a + \,b\left( {{T_{in}}} \right)\,\, + \,\,c{\left( {{T_{in}}} \right)^2}\,\, + \,\,d\left( {R{H_{in}}} \right) + e{(R{H_{in}})^2} + f({T_{in}})(R{H_{in}})$$</div>
-
-·        The part load fraction (PLF) correlation curve is a quadratic or a cubic curve with the independent variable being part load ratio (PLR = water removal load to be met / dehumidifier steady-state water removal rate). The part load ratio is divided by the output of this curve to determine the dehumidifier runtime fraction. The part load fraction correlation accounts for efficiency losses due to compressor cycling.
-
-<div>$$PartLoadFrac = PLF = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2}$$</div>
-
-or
-
-<div>$$PartLoadFrac = a + b\left( {PLR} \right) + c{\left( {PLR} \right)^2} + d{\left( {PLR} \right)^3}$$</div>
-
-where
-
-<div>$$PLR = \,part - load\,ratio\,\, = \left( {\frac{{water\,removal\,load\,to\,be\,met}}{{dehumidifier\,steady - state\,water\,removal\,rate}}} \right)$$</div>
-
-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the dehumidifier runs continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-0.7 &lt;= PLF &lt;= 1.0   and   PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the dehumidifier is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the dehumidifier is set to 1.0.
-
-Mechanical dehumidifier typically have long runtimes with minimal compressor cycling. So, a typical part load fraction correlation might be:
-
-      PLF = 0.95 + 0.05(PLR)
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-      PLF = 1.0 + 0.0(PLR)
-
-All three part-load curves are accessed through EnergyPlus’ built-in performance curve equation manager (Curve:Quadratic, Curve:Cubic and Curve:Biquadratic). It is not imperative that the user utilize all coefficients shown in curve equations above if their performance equation has fewer terms (e.g., if the user’s PartLoadFrac performance curve is linear instead of quadratic, simply enter the values for a and b, and set coefficient c equal to zero).
-
-For any simulation time step when there is a water removal load to be met, the dehumidifier is available to operate (via availability schedule), and the inlet air dry-bulb temperature is within the minimum and maximum dry-bulb temperature limits specified in the input file for this object, the water removal rate for the dehumidifier is calculated as follows:
-
-<div>$${\dot m_{_{water,ss}}} = \frac{{{\rho_{water}}\left( {{{\dot V}_{_{water,rated}}}} \right)\left( {WaterRemovalModFac} \right)}}{{\left( {24\,hr/dy} \right)\left( {3600sec/hr} \right)\left( {1000L/{m^3}} \right)}}$$</div>
-
-where
-
-<span>\({\dot m_{_{water,ss}}}\)</span>  =  dehumidifier steady-state water removal rate, kg/s
-
-<span>\({\rho_{water}}\)</span> = density of water, kg/m<sup>3</sup>
-
-<span>\({\dot V_{_{water,rated}}}\)</span>  = rated water removal rate (user input), L/day
-
-The Zone Dehumidifier Part-Load Ratio (output variable) is then calculated, with the result constrained to be from 0.0 to 1.0:
-
-<div>$$PLR = \,\frac{{water\,removal\,load\,to\,be\,met}}{{{{\dot m}_{_{water,ss}}}}},\,\,\,0.0 \le PLR \le 1.0$$</div>
-
-The steady-state and average electrical power consumed by the dehumidifier are calculated next using the following equations:
-
-<div>$$\begin{array}{l}{P_{dehumid,ss}} = \frac{{{{\dot V}_{_{water,rated}}}\left( {WaterRemovalModFac} \right)\left( {1000\,\,W/kW} \right)}}{{E{F_{rated}}\left( {EFModFac} \right)\left( {24\,hr/day} \right)}}\\ {P_{dehumid,avg}} = {P_{dehumid,ss}}\left( {RTF} \right) + \left( {{P_{off - cycle}}*\left( {1 - RTF} \right)} \right)\end{array}$$</div>
-
-where
-
-<span>\({P_{dehumid,ss}}\)</span>= dehumidifier steady-state electric power, W
-
-<span>\({P_{dehumid,avg}}\)</span>= Zone Dehumidifier Electric Power, W (output variable)
-
-<div>$$RTF = \frac{{PLR}}{{PLF}}\, = \,Zone Dehumidifier\,\,Runtime\,\,Fraction (output variable)$$</div>
-
-<span>\(E{F_{rated}}\)</span>  = rated energy factor (user input), L/kWh
-
-<span>\({P_{off - cycle}}\)</span>  = off-cycle parasitic electric load (user input), W
-
-If the dehumidifier is unavailable to operate for the time period (via the specified availability schedule) then Zone Dehumidifier Electric Power is set equal to zero.
-
-The average water removal rate (kg/s) for the simulation time step is then calculated:
-
-<div>$${\dot m_{water,\,avg}} = {\dot m_{water,\,ss}}\left( {PLR} \right) = {\rm{Zone Dehumidifier Removed Water Mass Flow Rate}},\;{\rm{kg/s}}\,\left( {{\rm{output}}\,{\rm{variable}}} \right)$$</div>
-
-The Zone Dehumidifier Sensible Heating Rate (output variable) is calculated as follows:
-
-<div>$${\dot Q_{_{sensible,avg}}} = {\dot m_{_{water,avg}}}\left( {{h_{fg}}} \right) + \,{P_{dehumid,avg}}$$</div>
-
-where
-
-*h<sub>fg</sub>* = enthalpy of vaporization of air, J/kg
-
-The Zone Dehumidifier Sensible Heating Rate (W) is calculated during each HVAC simulation time step, and the results are averaged for the timestep being reported. However, this sensible heating is carried over to the zone air heat balance for the next HVAC time step (i.e., it is reported as an output variable for the current simulation time step but actually impacts the zone air heat balance on the following HVAC time step).
-
-The air mass flow rate through the dehumidifier is determined using the Rated Air Flow Rate (m<sup>3</sup>/s) entered in the input, PLR, and converting to mass using the density of air at rated conditions (26.7C, 60% RH) and local barometric pressure accounting for altitude
-
-p=101325\*(1-2.25577E-05\*Z)\*\*5.2559  where p=pressure in Pa and Z=altitude in m:
-
-<div>$${\dot m_{_{air,avg}}} = {\rho_{air}}\left( {{{\dot V}_{_{air,rated}}}} \right)\left( {PLR} \right)$$</div>
-
-where
-
-<span>\({\dot m_{_{air,avg}}}\)</span>= average air mass flow rate through dehumidifier, kg/s
-
-<span>\({\dot V_{_{air,rated}}}\)</span>= rated air flow rate (user input), m<sup>3</sup>/s
-
-<span>\({\rho_{air}}\)</span> = density of air at 26.7°C , 60% RH and local barometric pressure, kg/m<sup>3</sup>
-
-The dry-bulb temperature and humidity ratio of the air leaving the dehumidifier are calculated as follows:
-
-<div>$$\begin{array}{l}{T_{out}} = {T_{in}} + \left( {\frac{{{P_{dehumid,ss}} + \left( {{{\dot m}_{_{water,ss}}}} \right)\left( {{h_{fg}}} \right)}}{{{\rho_{air}}\left( {{{\dot V}_{_{air,rated}}}} \right)\left( {{C_p}} \right)}}} \right)\,\\ {w_{out}} = {w_{in}} - \left( {\frac{{{{\dot m}_{_{water,avg}}}}}{{{{\dot m}_{air,avg}}}}} \right)\end{array}$$</div>
-
-where
-
-*T<sub>out</sub>* =    Zone Dehumidifier Outlet Air Temperature, C (output variable). Represents the
-
-outlet air temperature when the dehumidifier is operating.
-
-*T<sub>in</sub>* = inlet air dry-bulb temperature, C
-
-<span>\({C_p}\)</span>= heat capacity of air, J/kg
-
-*w<sub>in</sub>* = inlet air humidity ratio, kg/kg
-
-*w<sub>out</sub>* = outlet air humidity ratio, kg/kg
-
-If the dehumidifier does not operate for a given HVAC simulation time step, then the outlet air dry-bulb temperature and humidity ratio are set equal to the corresponding inlet air values.
-
-
-
-Since the sensible heating rate impacts the zone air heat balance on the following HVAC time step and is passed to the heat balance via an internal variable, the dry-bulb temperature of the dehumidifier’s HVAC outlet air node (System Node Temperature) will always be set equal to the dehumidifier’s HVAC inlet air node temperature. Therefore, when the dehumidifier operates the Zone Dehumidifier Outlet Air Temperature (output variable) will not be equal to the System Node Temperature for the dehumidifier’s HVAC outlet node.
-
-Finally, the following additional output variables are calculated:
-
-<div>$${Q_{_{sensible}}} = {\dot Q_{_{sensible,avg}}}*TimeStepSys*3600.$$</div>
-
-<div>$${E_{Dehumid}} = {P_{Dehumid,avg}}*TimeStepSys*3600.$$</div>
-
-<div>$${P_{off - cycle,avg}} = {P_{off - cycle}}\left( {1 - RTF} \right)$$</div>
-
-<div>$${E_{off - cycle}} = {P_{off - cycle,avg}}*TimeStepSys*3600.$$</div>
-
-<div>$${m_{_{water}}} = {\dot m_{_{water,avg}}}*TimeStepSys*3600.$$</div>
-
-<div>$${\dot V_{_{water,avg}}} = {\raise0.7ex\hbox{${{{\dot m}_{_{water,avg}}}}$} \!\mathord{\left/ {\vphantom {{{{\dot m}_{_{water,avg}}}} {{\rho_{water}}}}}\right.}\!\lower0.7ex\hbox{${{\rho_{water}}}$}}$$</div>
-
-<div>$${V_{_{water}}} = {\dot V_{_{water,avg}}}*TimeStepSys*3600.$$</div>
-
-where
-
-*Q<sub>sensible  </sub>*= output variable ‘Zone Dehumidifier Sensible Heating Energy [J]’
-
-*E<sub>dehumid</sub>*   = output variable ‘Zone Dehumidifier Electric Energy [J]’
-
-*P<sub>off-cycle,avg</sub>* = output variable ‘Zone Dehumidifier Off Cycle Parasitic Electric Power [W]’
-
-*E<sub>off-cycle</sub>* = output variable ‘Zone Dehumidifier Off Cycle Parasitic Electric Energy [J]’
-
-*m<sub>water</sub>*= output variable ‘Zone Dehumidifier Removed Water Mass [kg]’
-
-<span>\({\dot V_{_{water,avg}}}\)</span>*<sub> </sub>*= output variable ‘Zone Dehumidifier Condensate Volume Flow Rate [m<sup>3</sup>/s]’
-
-<span>\({V_{_{water}}}\)</span>  = output variable ‘Zone Dehumidifier Condensate Volume [m<sup>3</sup>]’
-
-### Energy Recovery Ventilator
-
-The input object ZoneHVAC:EnergyRecoveryVentilator provides a model for a stand alone energy recovery ventilator (ERV) that is a single-zone HVAC component used for exhaust air heat recovery (see figure below). This compound object consists of three required components: a generic air-to-air heat exchanger (see object HeatExchanger:AirToAir:SensibleAndLatent), a supply air fan, and an exhaust air fan (see object Fan:OnOff). An optional controller (see object  ZoneHVAC:EnergyRecoveryVentilator:Controller) may be used to simulate economizer (free cooling) operation.
-
-![Schematic\_StandAloneERV](media/image7321.png)
-
-Figure 324. Schematic of the Energy Recovery Ventilator:Stand Alone compound object
-
-This compound object models the basic operation of supply and exhaust air fans and an air-to-air heat exchanger. The stand alone ERV operates whenever the unit is scheduled to be available (Availability schedule). The stand alone ERV object can be used in conjunction with an economizer feature whereby heat exchange is suspended whenever free cooling is available (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped).
-
-To model a stand alone ERV connected to a single zone, the input data file should include the following objects:
-
-* ZoneHVAC:EnergyRecoveryVentilator
-
-* HeatExchanger:AirToAir:SensibleAndLatent
-
-* Fan:OnOff (supply air)
-
-* Fan:OnOff (exhaust air)
-
-* ZoneHVAC:EnergyRecoveryVentilator:Controller (if economizer [free cooling] operation is desired)
-
-* SetpointManager:Scheduled (if supply air outlet temperature control is used, Ref. HeatExchanger:AirToAir:SensibleAndLatent)
-
-* ZoneHVAC:EquipmentConnections
-
-* ZoneHVAC:EquipmentList
-
-* OutdoorAir:NodeList
-
-#### Model Description
-
-The purpose of this compound component is to simply call the individual component models and optional controller for each energy recovery ventilator. Since this equipment is not associated with an air loop, the compound object sets the supply and exhaust air mass flow rates through the ventilator. This compound object is also used to report the total, sensible and latent energy supplied to the zone, as well as the total electrical energy consumed by all of the individual components (supply air fan, exhaust air fan and heat exchanger parasitics).
-
-During each simulation time step, the air mass flow rate at the supply air and exhaust air inlets is set based on the stand alone ERV’s availability schedule and the specified volumetric air flow rates as follows:
-
-IF (availability schedule value &gt; 0) THEN
-
- <span>\({\mathop m\limits^ \bullet_{Supply}} = \rho {\mathop V\limits^ \bullet_{Supply}}\)</span>
-
-<div>$${\mathop m\limits^ \bullet_{Exhaust}} = \rho {\mathop V\limits^ \bullet_{Exhaust}}$$</div>
-
-ELSE
-
-<div>$${\mathop m\limits^ \bullet_{Supply}} = {\mathop m\limits^ \bullet_{Exhaust}} = 0.0$$</div>
-
-*where*:
-
-<span>\({\mathop m\limits^ \bullet_{Supply}}\)</span>             = mass flow rate of the supply air stream, kg/s
-
-<span>\({\mathop m\limits^ \bullet_{Exhaust}}\)</span>            = mass flow rate of the exhaust air stream, kg/s
-
-<span>\(\rho \)</span>                    = density of dry air at local barometric pressure (adjusted for altitude)        and 20 ºC, kg/m<sup>3</sup>
-
-<span>\({\mathop V\limits^ \bullet_{Supply}}\)</span>             = volumetric flow rate of the supply air stream, m<sup>3</sup>/s
-
-<span>\({\mathop V\limits^ \bullet_{Exhaust}}\)</span>            = volumetric flow rate of the exhaust air stream, m<sup>3</sup>/s
-
-With the supply and exhaust inlet air mass flow rates set, the compound object then calls the generic air-to-air heat exchanger model to determine its supply air and exhaust air exiting conditions based on the inputs specified in the heat exchanger object. The supply air and exhaust air fans are then modeled to determine the final conditions of the air streams exiting the stand alone energy recovery ventilator. The heat exchanger and fan models are described in detail elsewhere in this document (reference: HeatExchanger:AirToAir:SensibleAndLatent and Fan:OnOff).
-
-The sensible heat transfer rate to the zone by the stand alone ventilator is then calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible}}\, = \,{\mathop {\,m}\limits^ \bullet_{Supply}}{\left( {{h_{SupplyOutlet}}\, - \,{h_{ExhaustInlet}}} \right)_{HR\min }}$$</div>
-
- where:
-
-<sub><span>\({\mathop Q\limits^ \bullet_{Sensible}}\)</span>        </sub>= sensible energy transfer rate to the zone, W
-
-<span>\({\mathop m\limits^ \bullet_{Supply}}\)</span>       = mass flow rate of the supply air stream, kg/s
-
-*h<sub>SupplyOutlet</sub>*   = enthalpy of the air being supplied to the zone, J/kg
-
-*h<sub>ExhaustInlet</sub>*<sub> \\     </sub> = enthalpy of the air being exhausted from the zone through the ventilator, J/kg
-
-*HR<sub>min</sub>        =* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio
-
-   of the supply air outlet or the exhaust air inlet
-
-The resulting sensible energy transfer rate is passed to the zone equipment manager and added to the zone load to be met by other heating or cooling equipment. Since the stand alone ERV is intended to reduce the outdoor air load through heat exchange and not meet that load completely, the stand alone heat exchanger must be modeled first in the list of zone equipment. This is accomplished by setting the stand alone ERV priority for cooling and heating higher than that of other zone cooling or heating equipment (reference: ZoneHVAC:EquipmentList).
-
-When economizer (free cooling) operation is desired, a controller is coupled to the stand alone ERV by providing the name of the controller object in the ERV controller input field. This controller determines when the air-side economizer is active (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped) based on the controller inputs (Ref. ZoneHVAC:EnergyRecoveryVentilator:Controller).
-
-At the end of each HVAC simulation time step, this compound object reports the heating or cooling rate and energy delivered to the zone, as well as the electric power and consumption by the ventilator. In terms of thermal energy delivered to the zone, the sensible, latent and total energy transfer rate to the zone is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{Total}}\, = \,\,{\mathop m\limits^ \bullet_{Supply}}{\left( {{h_{SupplyOutlet}}\, - \,{h_{ExhaustInlet}}} \right)_{}}$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible}}\, = \,\,{\mathop m\limits^ \bullet_{Supply}}{\left( {{h_{SupplyOutlet}}\, - \,{h_{ExhaustInlet}}} \right)_{HR\min }}$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Latent}}\, = \,\,{\mathop Q\limits^ \bullet_{Total}}\, - \,{\mathop Q\limits^ \bullet_{Sensible}}$$</div>
-
- where:
-
-<sub><span>\({\dot Q_{Total}}\)</span>           </sub>= total energy transfer rate to the zone, W
-
-<sub><span>\({\dot Q_{Sensible}}\)</span>        </sub>= sensible energy transfer rate to the zone, W
-
-<sub><span>\({\dot Q_{Latent}}\)</span>        </sub>= latent energy transfer rate to the zone, W
-
-<span>\({\mathop m\limits^ \bullet_{Supply}}\)</span>       = mass flow rate of the supply air stream, kg/s
-
-*h<sub>SupplyOutlet</sub>*   = enthalpy of the air being supplied to the zone, J/kg
-
-*h<sub>ExhaustInlet</sub>*<sub> \\     </sub> = enthalpy of the air being exhausted from the zone through the ventilator, J/kg
-
-*HR<sub>min</sub>        =* enthalpies evaluated at a constant humidity ratio, the minimum humidity ratio
-
-   of the supply air outlet or the exhaust air inlet
-
-
-
-Since each of these energy transfer rates can be calculated as positive or negative values, individual reporting variables are established for cooling and heating and only positive values are reported. The following calculations are representative of what is done for each of the energy transfer rates:
-
-IF (<span>\({\dot Q_{Total}}\)</span>* &lt; 0.0 )*THEN
-
-                  <span>\({\dot Q_{TotalCooling}}\)</span> =  ABS (<span>\({\dot Q_{Total}}\)</span>)
-
-                  <span>\({\dot Q_{TotalHeating}}\)</span><sub> </sub> =  *0.0*
-
-ELSE
-
-                  <span>\({\dot Q_{TotalCooling}}\)</span><sub> </sub> =  *0.0*
-
-                  <span>\({\dot Q_{TotalHeating}}\)</span><sub> </sub> =  <span>\({\dot Q_{Total}}\)</span>
-
-
-
-where:
-
-<sub><span>\({\dot Q_{TotalCooling}}\)</span>   </sub>= output variable ‘Zone Ventilator Total Cooling Rate, W’
-
-<sub><span>\({\dot Q_{TotalHeating}}\)</span>   </sub>= output variable ‘Zone Ventilator Total Heating Rate, W’
-
-
-
-In addition to heating and cooling rates, the heating and cooling energy supplied to the zone is also calculated for the time step being reported. The following example for total cooling energy is representative of what is done for the sensible and latent energy as well as the heating counterparts.
-
-<div>$${Q_{TotalCooling}} = {\dot Q_{TotalCooling}}*TimeStepSys*3600.$$</div>
-
-where:
-
-<sub><span>\({\dot Q_{TotalCooling}}\)</span>   </sub>= output variable ‘Zone Ventilator Total Cooling Energy, J’
-
-*TimeStepSys* = HVAC system simulation time step, hr
-
-### Zone Evaporative Cooler Unit
-
-The input object ZoneHVAC:EvaporativeCoolerUnit provides a zone equipment model for evaporative cooling.  This is a compound object that combines a fan and one or two evaporative coolers in a zone unit.  The fan and evaporative cooler component models are described elsewhere. In this section we describe how the zone unit is controlled.
-
-#### Controls
-
-There are three choices for control methods.
-
-**ZoneTemperatureDeadbandOnOffCycling**. This control method operates the cooler unit in a manner similar to how a normal, real-world themostat operates.  The control uses input for throttling temperature range, <span>\(\Delta {T_{throttle}}\)</span>, the most recent result for zone air node temperature, <span>\({T_{zone}}\)</span>, and the current cooling setpoint temperature, <span>\({T_{set}}\)</span>.  The controller also stores the history of whether or not the unit was operating during the previous timestep to model hysteresis control where the unit retains its mode when it passes through the throttling range (to avoid short cycling).
-
-The following algorithm is used to determine if the unit will operate.
-
-If <span>\(\left[ {{T_{zone}} &lt; \left( {{T_{set}} - 0.5*\Delta {T_{throttle}}} \right)} \right]\)</span> is true, then do not operate cooler unit.
-
-If <span>\(\left[ {{T_{zone}} > \left( {{T_{set}} + 0.5*\Delta {T_{throttle}}} \right)} \right]\)</span> is true, then operate the cooler unit (at full speed).
-
-If zone air temperature is within the throttling range, <span>\(\left[ {\left( {{T_{set}} - 0.5*\Delta {T_{throttle}}} \right) &lt; {T_{zone}} &lt; \left( {{T_{set}} + 0.5*\Delta {T_{throttle}}} \right)} \right]\)</span>, then continue to operate the cooler if it was running during the previous timestep and do not operate the cooler if it was not running during the previous timestep.
-
-Whenever the unit is operating, it runs at the full design air mass flow rate regardless if the fan is constant or variable speed.
-
-**ZoneCoolingLoadOnOffCycling.** This control method operates the cooler similar to how a thermostat would behave, but instead of using temperatures it uses the predicted zone load to cooling setpoint.  The control uses input for the threshold value for a load that is considered a significant, <span>\({\dot Q_{thresh}}\)</span>, and the result from the Predictor for the zone’s load to cooling setpoint, <span>\({\dot Q_{CoolLoad}}\)</span>. The following algorithm is used to determine if the unit will operate.
-
-If <span>\(\left[ {{{\dot Q}_{CoolLoad}} \le {{\dot Q}_{thresh}}} \right]\)</span> is true, then do not operate cooler unit.
-
-If <span>\(\left[ {{{\dot Q}_{CoolLoad}} > {{\dot Q}_{thresh}}} \right]\)</span> is true, then operate the cooler unit (at full speed).
-
-Whenever the unit is operating, it runs at the full design air mass flow rate regardless if the fan is constant or variable speed.
-
-**ZoneCoolingLoadVariableSpeedFan.** This control method also operates the cooler using the predicted zone load to cooling setpoint but instead of on/off cycling, it modulates the fan speed to meet the cooling load.  This control method is only applicable to cooler units with variable speed supply fans. The control uses input for the threshold value for a load that is considered a significant, <span>\({\dot Q_{thresh}}\)</span>, and the result from the Predictor for the zone’s cooling load to setpoint, <span>\({\dot Q_{CoolLoad}}\)</span>. The following algorithm is used to determine if the unit will operate.
-
-If <span>\(\left[ {{{\dot Q}_{CoolLoad}} \le {{\dot Q}_{thresh}}} \right]\)</span> is true, then do not operate cooler unit.
-
-If <span>\(\left[ {{{\dot Q}_{CoolLoad}} > {{\dot Q}_{thresh}}} \right]\)</span> is true, then operate the cooler unit.
-
-When the unit operates, the model first operates the unit at the highest fan speed, a fan speed ratio of 1.0, and determines the sensible cooling provided by the unit to the zone, <span>\({\dot Q_{FullOutput}}\)</span>.  If <span>\({\dot Q_{FullOutput}} \le {\dot Q_{CoolLoad}}\)</span>then the unit operates at full fan speed because the cooler cannot meet the entire zone cooling load.  If <span>\({\dot Q_{FullOutput}} > {\dot Q_{CoolLoad}}\)</span> then the model solves for a fan speed ratio between 0.0 and 1.0 that satisifies <span>\(ABS\left( {\dot Q{}_{Output} - {{\dot Q}_{CoolLoad}}} \right) &lt; 0.01\)</span> using the non-linear numerical method called regula falsi.
-
-### Unit Heater
-
-(Note: Some of this information also appears in the Input Output Reference for EnergyPlus.  It is repeated here for clarity.)
-
-The input object ZoneHVAC:UnitHeater provides a model for unit heaters that are zone equipment units which are assembled from other components and are a simplification of unit ventilators.  They contain only a fan and a heating coil. These components are described elsewhere in this document. The unit heater input simply requires the names of these components, which have to be described elsewhere in the input. The input also requires the name of an availability schedule, maximum airflow rate, and maximum and minimum hot water volumetric flow rates. The unit is connected to the zone inlet and exhaust nodes by specifying unit inlet and outlet node names. Note that the unit air inlet node should be the same as a zone exhaust node and the unit outlet node should be the same as a zone inlet node.
-
-#### Controls
-
-While the control of the heating coil is similar to the fan coil units and the unit ventilator, the overall control of the unit heater is much different.  There are four different modes in which a unit heat can operate based on the user input:
-
-**OFF:** In this mode, the unit has been scheduled off.  All flow rates are set to zero, and the temperatures are set to zone conditions.
-
-**NO LOAD OR COOLING/�NO�** for “Supply Air Fan Operation During No Heating� input field **:** In this mode, the unit is available, but there is no heating load.  With “No� specified for “Supply Air Fan Operation During No Heating� and the supply fan operating mode schedule value of 0, the fan will only run when there is a heating load.  Since there is no heating load in this mode and the fan is in cycling operating mode, all flow rates are set to zero, and the temperatures are set to zone conditions.  Since the unit heater is designed only to provide heating, the presence of a cooling load signifies that the unit should not be running.
-
-**NO LOAD OR COOLING/�YES�** for “Supply Air Fan Operation During No Heating� input field**:** In this mode, the unit is available and the fan is controlled to be running continuously. For OnOff fan type the supply fan operating mode schedule value should be greater than 0.  If it is scheduled to be available and the supply fan operating mode schedule value is greater than 0, then the fan runs and circulates air to the space.  While no direct heating is provided, any heat added by the fan is introduced into the space with the circulation of the air.  If the fan is scheduled off, the fan will not run (this is identical to “NO� control with no load).
-
-With “Yes� specified for “Supply Air Fan Operation During No Heating�, and the supply fan operating mode schedule value is 0  (for onOff fan type), then supply fan will not run.  Since there is no heating load in this mode and the fan is in cycling mode, all flow rates are set to zero. This control mode allows to schedule the supply fan operation by specifying different operating modes during the day regardless of the heating load.
-
-**HEATING:** In this mode, the unit and fan are on/available, and there is a heating load.  The heating coil is modulated (constant fan speed) to meet the heating load.  When the fan is not cycling then the control of the heating coil and its flow rate is identical to the fan coil unit.  The flow rate of air through the unit is controlled by the user input and schedules. In the case of OnOff fan the fan cycles with heating coil if the current timestep supply fan operating mode schedule value is 0, or the supply fan runs continuously for the entire timestep if the current timestep fan operating mode schedule value is greater than 0.  When the fan is cycling the average supply air flow rate is proportional to the heating load at current time step, or else when the fan is scheduled to run continuously the fan supplies the maximum flow rate specified.
-
-### Unit Ventilator
-
-(Note: Some of this information also appears in the Input Output Reference for EnergyPlus.  It is repeated here for clarity.)
-
-The input object ZoneHVAC:UnitVentilator provides a model for unit ventilators that are zone equipment units which are assembled from other components. They contain a built-in outdoor air mixer, a fan, a heating coil, and a cooling coil. These components are described elsewhere in this document, except the built-in outdoor air mixer which is contained within the unit ventilator statement. The unit ventilator input simply requires the names of these other three components, which have to be described elsewhere in the input. The input also requires the name of an availability schedule, maximum airflow rate, outdoor air control information (control type and schedules), an outdoor airflow rate, and maximum and minimum hot and cold water mass flow rates. The unit is connected to the zone inlet and exhaust nodes and the outdoor air by specifying unit inlet, outlet, outdoor air and exhaust (relief) air node names. Note that the unit air inlet node should be the same as a zone exhaust node and the unit outlet node should be the same as a zone inlet node. In general, the unit ventilator input is very similar to the fan coil unit input, and the unit is connected to a hot water loop (demand side) through its hot water coil and to a chilled water loop (demand side) through its cooling coil.
-
-#### Controls and Outdoor Air
-
-The main difference between the fan coil and unit ventilator input is that the unit ventilator has a built-in outdoor air mixer with its own specialized controls. The outdoor air control type can be selected from one of the following options: “variable percent�, “fixed temperature� or “fixed amount�. In fixed temperature control, the amount of outdoor air is varied between the minimum outdoor air fraction (specified by a schedule) and 100% outdoor air to obtain a mixed air temperature as close as possible to the temperature schedule defined in the input. Variable percent control will also vary the amount of outdoor air between the minimum and maximum fractions (both specified in input by the user) to meet the load without the use of a coil if possible. In fixed amount control, the outdoor air flow rate is fixed to the specified value by the user. In this control strategy, the maximum outdoor air flow rate and schedule are automatically set to be equal to the minimum outdoor air flow rate and schedule. These control types are based on the 2004 ASHRAE Systems and Equipment Handbook (pp. 31.1-31.3) description of unit ventilator systems.
-
-The unit is controlled to meet the zone (remaining) heating or cooling demand. If there is a heating demand, the cooling coil is off and the hot water flow through the heating coil is throttled to meet the demand. The hot water control node must be specified (same as the hot water coil inlet node) as well as maximum and minimum possible hot water volumetric flow rates. If there is a cooling demand from the zone, the hot water coil is off and the chilled water flow through the cooling coil is throttled to meet the load. The cooling coil control node must be specified (same as the cooling coil inlet node) and the maximum and minimum chilled water volumetric flow rates must be given. Finally both heating and cooling require a convergence tolerance, which is the tolerance denoting how closely the fan coil unit will meet the heating or cooling load. The tolerance is always relative to the zone load.
-
-Overall, control of the unit must consider the outdoor air for continuously running and cycling fans. For cycling fan operating mode, the outdoor air mass rate is capped by the actual supply air flow rate if the former is greater than the latter; otherwise, uses the amount calculated by the outdoor air control. Here is a more detailed description of the overall unit control:
-
-**OFF:** Unit is schedule off or there is no load on it. All flow rates are set to zero and the temperatures are set to zone conditions (except for the outdoor air inlet). Outdoor air requirements will not override this condition.
-
-**HEATING/NO COIL/VARIABLE PERCENT:** The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and variable percent outdoor air control type has been specified. In this case, the variable percent outdoor air controls what happens with the outdoor air. If the outside temperature is greater than the return temperature, then the outdoor air is set to the maximum as defined by the user input. If the outdoor air temperature is less than the return temperature from the zone, then the outdoor air is set to the minimum outdoor air flow rate as defined by the user. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
-
-**HEATING/NO COIL/FIXED TEMPERATURE:** The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate.
-
-**HEATING/NO COIL/FIXED AMOUNT:** The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
-
-**HEATING/WITH COIL/VARIABLE PERCENT:** The unit is on, there is a heating load, and variable percent control is specified. The outdoor air fraction is set to the minimum outdoor air fraction (schedule based), and the heating coil is activated. The heating coil attempts to meet the remaining load on the zone being served by the unit ventilator.
-
-**HEATING/WITH COIL/FIXED AMOUNT:** The unit is on, there is a heating load, a heating coil is present and is scheduled on, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. The heating coil then attempts to meet any remaining zone heating load.
-
-**COOLING/NO COIL/VARIABLE PERCENT:** The unit is on, there is a cooling load, no coil is present or it has been scheduled off, and variable percent outdoor air control type has been specified. In this case, the variable percent outdoor air controls what happens with the outdoor air. If the outside temperature is greater than the return temperature, then the outdoor air is set to the minimum as defined by the user input. If the outdoor air temperature is less than the return temperature from the zone, then the outdoor air is set to the maximum outdoor air flow rate as defined by the user. This may be somewhat simplistic in that it could result in overcooling of the space. However, since a temperature goal was not established, this is the best that can be done by the simulation. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
-
-**COOLING/NO COIL/FIXED TEMPERATURE:** The unit is on, there is a cooling load, no cooling coil is present or it has been scheduled off, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate in the same fashion as the variable percent outdoor air control.
-
-**COOLING/NO COIL/FIXED AMOUNT:** The unit is on, there is a cooling load, no cooling coil is present or it has been scheduled off, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
-
-**COOLING/WITH COIL/VARIABLE PERCENT:** The unit is on, there is a cooling load, a coil is present and is scheduled on, and variable percent outdoor air control type has been specified. In this case, the percentage of outdoor air is set to the minimum flow outdoor air flow rate. The coil then attempts to meet any remaining zone load.
-
-**COOLING/WITH COIL/FIXED TEMPERATURE:** The unit is on, there is a cooling load, a cooling coil is present and is scheduled on, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate in the same fashion as the fixed temperature outdoor air control for the “no coil� conditions. The cooling coil then attempts to meet any remaining zone load.
-
-**COOLING/WITH COIL/FIXED AMOUNT:** The unit is on, there is a cooling load, a cooling coil is present and is scheduled on, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. The cooling coil then attempts to meet any remaining zone cooling load.
-
-Note: the unit ventilator controls are strictly temperature based and do not factor humidity into the equation (not an enthalpy economy cycle but rather a simple return air economy cycle). In addition, temperature predictions are not strict energy balances here in the control routine though in the mixing routine an energy balance is preserved.
-
-### Variable Refrigerant Flow Terminal Unit
-
-Variable refrigerant flow zone terminal units are used exclusively with variable refrigerant flow (VRF) air conditioning systems (ref: AirConditioner:VariableRefrigerantFlow and ZoneTerminalUnitList). The terminal units operate to satisfy a heating or cooling load in a zone based on a zone thermostat temperature set point. A direct-expansion (DX) cooling and/or DX heating coil is specified depending on the operating mode required. Outdoor ventilation air is modeled with the use of an outside air mixer object. Outside air may be provided to the zone only when the coil is operating or can be supplied continuously even when the coil is not operating. A supply air fan is also required and can be modeled as either draw through as shown in the figure below or as blow through where the fan inlet node would be connected to the outside air mixer mixed air node. If an outside air mixer is not used, the fan inlet node would be connected to the zone exhaust node.
-
-![](media/image7369.png)
-
-Figure 325. Zone Terminal Unit Schematic
-
-#### Overview
-
-As described previously, the terminal units operate to satisfy a heating or cooling load in a zone based on a zone thermostat temperature set point (Zone Control:Thermostatic). Each simulation time step, EnergyPlus performs a zone air heat balance to determine if cooling or heating is required to meet the zone thermostat set points, excluding any impacts from zone terminal unit operation.
-
-Terminal unit performance is then modeled with all heating/cooling coils off but the supply air fan operates as specified by the user. If the zone air heat balance plus the impact of terminal unit operation with coils off results in no requirement for heating or cooling by the terminal unit coils, or if the terminal unit is scheduled off (via its availability schedule), then the terminal unit coils do not operate and the terminal unit’s part-load ratio output variable is set to 0. If the model determines that cooling or heating is required and the terminal unit is scheduled to operate, the model calculates the part-load ratio of the cooling and heating coils in order to meet the thermostat set point temperature.
-
-The following sections describe the performance calculations for cooling-mode and heating-mode.
-
-#### Model Description
-
-Zone terminal units meet a zone load as determined by a zone thermostat. The DX coils within a zone terminal unit will operate to meet a sensible zone load and all terminal units are controlled to either meet a zone sensible cooling load or a zone sensible heating load. This model does not provide for simultaneous cooling and heating.
-
-Given a zone load, the model calculates the part-load ratio of the terminal unit such that the terminal unit’s “net� sensible capacity is equal to the zone load (if sufficient capacity is available). If it is determined that the part-load ratio of the zone terminal unit will be equal to 1, the DX cooling coil’s capacity is calculated in the same manner as described for single-speed DX cooling coils (ref: Coil:Cooling:DX:SingleSpeed). When it is determined that the part-load ratio of the zone terminal unit will be less than 1, the DX cooling coil’s capacity will be modulated through a reduction in refrigerant flow rate and an iterative solution technique will be used to calculate the performance of the DX cooling coil. For DX heating coils, capacity is calculated in the same manner as described for single-speed DX heating coils (ref: Coil:Heating:DX:SingleSpeed).
-
-The “net� sensible full load cooling capacity is then compared to the zone sensible load. If the “net� sensible full load capacity is less than or equal to the absolute value of the zone sensible load, the DX coil operates at the *maximum* available capacity and, as a result, the zone air heat balance adjusts the zone air temperature. If the “net� sensible full load capacity is greater than the absolute value of the zone sensible load, an iterative solution technique is used to determine the total capacity required to meet the zone sensible load. This iteration loop entails successive modeling of DX coil performance and the loop iterates on the required total capacity until the operating “net� sensible capacity is equal to the zone sensible load.
-
-#### Average Air Flow Calculations
-
-The variable refrigerant flow (VRF) terminal unit operates based on user-specified (or autosized) air flow rates. The VRF terminal unit’s supply air flow rate during cooling operation may be different than the supply air flow rate during heating operation. In addition, the supply air flow rate when no cooling or heating is required but the supply air fan remains ON can be different than the air flow rates when cooling or heating is required. The outside air flow rates can likewise be different in these various operating modes. The model takes these different flow rates into account when modeling the terminal unit, and the average air flow rate for each simulation time step is reported on the inlet/outlet air nodes of the various VRF terminal unit components in proportion to the calculated cycling ratio of the heat pump condenser. If the compressor does not cycle for a specific simulation time step then the heating or cooling air flow rate as specified by the user is assumed for the entire time step.
-
-The average supply air and outdoor air mass flow rates through the terminal unit for the HVAC simulation time step are calculated based on the cycling ratio of the heat pump condenser as follows:
-
-<div>$$\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\,\, = \,\,\mathop m\limits^ \bullet  {\,_{SA,coil\,\,on}}\left( {CyclingRatio} \right) + \mathop m\limits^ \bullet  {\,_{SA,\,\,coil\,\,off}}\left( {1 - CyclingRatio} \right)$$</div>
-
-<div>$$\mathop m\limits^ \bullet  {\,_{OA,\,\,avg\,\,}} = \,\,\mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,on}}\left( {CyclingRatio} \right) + \mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,off}}\left( {1 - CyclingRatio} \right)$$</div>
-
-where:
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\)</span>      = average supply air mass flow rate during the time step, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,coil\,\,on}}\)</span>   = supply air mass flow rate when the coil is ON, kg/s
-
-*CyclingRatio* = cycling ratio of the heat pump condenser (heating or cooling)
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,\,\,coil\,\,off}}\)</span>  = supply air mass flow rate when the coil is OFF, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{OA,\,\,avg\,\,}}\)</span>    = average outside air mass flow rate during the time step, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,on}}\)</span>  = average outside air mass flow rate when the coil is ON, kg/s
-
-<span>\(\mathop m\limits^ \bullet  {\,_{OA,\,\,coil\,\,off}}\)</span>  = average outside air mass flow rate when the coil is OFF, kg/s
-
-The supply air and outside air flow rates when the DX cooling coil or the DX heating coil is ON are specified by the user (i.e., supply air volumetric flow rate during cooling operation, supply air volumetric flow rate during heating operation, outside air volumetric air flow rate during cooling operation, and outside air volumetric air flow rate during heating operation) and are converted from volumetric to mass flow rate. If the user has specified cycling fan/cycling coil operation (i.e. supply air fan operating mode schedule value is equal to 0), then the supply air and outside air mass flow rates when the coil is OFF are zero. If the user has specified constant fan/cycling coil operation (i.e. supply air fan operating mode schedule value is greater than 0), then the user-defined air flow rates when no cooling or heating is needed are used when the coil is OFF.
-
-There is one special case. If the supply air fan operating mode schedule value specifies constant fan operation and the user also specifies that the supply air volumetric flow rate when no cooling or heating is needed is zero (or field is left blank), then the model assumes that the supply air and outside air mass flow rates when the coil is OFF are equal to the corresponding air mass flow rates when the cooling or heating coil was last operating (ON).
-
-#### Calculation of Outlet Air Conditions
-
-When the supply air fan cycles on and off with the terminal unit coils (AUTO fan), the calculated outlet air conditions (temperature, humidity ratio, and enthalpy) from the DX heating coil or the DX cooling coil at full-load (steady-state) operation are reported on the appropriate coil outlet air node. The air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the cycling ratio of the coil (see Average Air Flow Calculations above).
-
-When the supply air fan operates continuously while the terminal unit coils cycle on and off (fan ON), the air mass flow rate reported on the air nodes is the average air mass flow rate proportional to the cycling ratio of the coil (see Average Air Flow Calculations above). Since the air flow rate can be different when the coil is ON compared to when the coil is OFF, then the average outlet air conditions from the DX heating coil or the DX cooling coil are reported on the appropriate coil outlet air node.
-
-#### Calculation of Zone Heating and Cooling Rates
-
-At the end of each HVAC simulation time step, this compound object reports the heating or cooling rate and energy delivered to the zone. In terms of thermal energy delivered to the zone, the sensible, latent and total energy transfer rate to the zone is calculated as follows:
-
-<div>$${\mathop Q\limits^ \bullet_{Total}} = \left( {\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\,\,} \right)\left( {{h_{out,\,avg}} - {h_{zone\,\,air}}} \right)$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Sensible}} = \left( {\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\,\,} \right){\left( {{h_{out,\,avg}} - {h_{zone\,\,air}}} \right)_{HRmin}}$$</div>
-
-<div>$${\mathop Q\limits^ \bullet_{Latent}} = {\mathop Q\limits^ \bullet_{Total}} - {\mathop Q\limits^ \bullet_{Sensible}}$$</div>
-
-where:
-
-<sub><span>\({\dot Q_{Total}}\)</span>                 </sub> = total energy transfer rate to the zone, W
-
-<sub><span>\({\dot Q_{Sensible}}\)</span>            </sub> = sensible energy transfer rate to the zone, W
-
-<sub><span>\({\dot Q_{Latent}}\)</span>             </sub> = latent energy transfer rate to the zone, W
-
-<span>\(\mathop m\limits^ \bullet  {\,_{SA,\,\,avg}}\)</span>= average mass flow rate of the supply air stream, kg/s
-
-*h<sub>out,avg</sub>*          = enthalpy of the air being supplied to the zone, J/kg
-
-The terminal unit’s energy transfer rate is used by the program in the zone air heat balance to determine the final zone air conditions. If the terminal unit is capable of meeting the zone thermostat set point temperature, then these report variables are indicative of the zone loads and may be compared directly to the report variables for predicted zone loads (ref: Output:Variable, e.g., Zone Predicted Sensible Load to Setpoint Heat Transfer Rate).
-
-Since each of these energy transfer rates can be calculated as positive or negative values, individual reporting variables are established for cooling and heating and only positive values are reported. The following calculations are representative of what is done for each of the energy transfer rates:
-
-IF (<span>\({\dot Q_{Total}}\)</span>* &lt; 0.0 )* THEN
-
-      <span>\({\dot Q_{TotalCooling}}\)</span> =  ABS (<span>\({\dot Q_{Total}}\)</span>)
-
-      <span>\({\dot Q_{TotalHeating}}\)</span><sub> </sub> =  *0.0*
-
-ELSE
-
-      <span>\({\dot Q_{TotalCooling}}\)</span><sub> </sub> =  *0.0*
-
-      <span>\({\dot Q_{TotalHeating}}\)</span><sub> </sub> =  <span>\({\dot Q_{Total}}\)</span>
-
-ENDIF
-
-where:
-
-<sub><span>\({\dot Q_{TotalCooling}}\)</span>    </sub> = output variable ‘Zone VRF Air Terminal Total Cooling Rate, W’
-
-<sub><span>\({\dot Q_{TotalHeating}}\)</span>    </sub> = output variable ‘Zone VRF Air Terminal Total Heating Rate, W’
-
-In addition to heating and cooling rates, the heating and cooling energy supplied to the zone is also calculated for the time step being reported. The following example for total zone cooling energy is representative of what is done for the sensible and latent energy as well as the heating counterparts.
-
-<div>$${Q_{TotalCooling}} = {\dot Q_{TotalCooling}}*TimeStepSys*3600.$$</div>
-
-where:
-
-<sub><span>\({\dot Q_{TotalCooling}}\)</span>      </sub> = output variable ‘Zone VRF Air Terminal Total Cooling Energy, J’
-
-*TimeStepSys* = HVAC system simulation time step, hr
-
-### Ventilated Slab
-
-#### Model Overview
-
-The input object ZoneHVAC:VentilatedSlab provides a model for ventilated slab systems that in general use outdoor air to “precool� slabs with colder nighttime air. This method of precooling the thermal mass of a space can be very effective when nighttime temperatures are low and the mass of the system is high enough to provide a significant amount of cooling potential during the day to counteract internal heat gains within a zone. Nearly all ventilated slabs are simple systems such as that shown in the right side of Figure 326. The fan is shown in a blow through position, but the model will allow either a blow or draw through configuration.
-
-![Slide1](media/image7396.png)
-
-Figure 326. Basic System for the Ventilated Slab Module
-
-It should be noted that in Figure 326 the use of “unit ventilator� and “low temperature radiant system� do not imply that the user must also specify these elements in the input file. The ventilated slab model combines aspects of these two existing EnergyPlus features into a single model that the user specifies through the input shown in the Input/Output Reference.
-
-The ventilated slab system has been implemented in a fashion that is similar to the “unit ventilator� system in EnergyPlus. The unit ventilator is a system that allows the user to bring in outdoor air (ventilation) that may or may not be tempered with a heating or cooling coil as shown the left side of Figure 326. The air can be delivered to the slab only (Figure 327), to the slab then to the space(Figure 328), and to several slabs in different areas in series (Figure 329). The model essentially combines the functionality of the low temperature radiant system (using air as a transport medium rather than water) and the unit ventilator. In some cases, the system may not meet all the zone heating and cooling load because it is operated not by setpoint of the zone but control temperature range and coil outlet air temperature set by user input.**Note that no coils are shown in Figure 329 for diagram simplicity but the implementation of the system shown in Figure 329 includes coils as in Figure 327 and Figure 328.
-
-![Slide2](media/image7397.png)
-
-Figure 327. Model with Air Delivered to Slab. (Slab Only Mode)
-
-![Slide3](media/image7398.png)
-
-Figure 328. Zone Supply Model using Ventilated Slab (Slab and Zone mode)
-
-![Slide4](media/image7399.png)
-
-Figure 329. Multiple Slabs model with Several Zones (Series Slabs Mode)
-
-#### Connections to the Heat Balances
-
-The ventilated slab systems shown in the above diagrams connect or will connect to the various EnergyPlus heat balance equations in a variety of ways. All of the systems send outside or conditioned air through a slab or building element. This portion of the system acts in a fashion that is identical to the low temperature radiant systems. These surfaces that have the air being blown through them will impact the zone and air heat balances through the normal surface heat balances that interact with this surface. The ventilated slab will participate in the surface heat balances by exchanging radiation with other surfaces in the zone and in the air heat balances via convection to the zone air. So, the ventilated slab is handled identically to the low temperature radiant systems with respect to the zone and air heat balances. This information is valid for all three of the systems shown in the figures above.
-
-Figure 328 shows that the air, instead of being circulated through the slab and then sent back to the ventilation portion of the system, gets circulated through the space after it gets sent through the slab. When this system is selected in EnergyPlus, it will have an additional impact on the zone air heat balance because air will be introduced into the space at conditions different than the zone air. Thus, it will have an energy impact on the air directly through the circulation of air from the slab to the zone and then back to the ventilated slab system. It will still have an impact on the slab surface convection and radiation as with the other systems.
-
-For more information on the impact on the zone and air heat balances by the ventilated slab system, please consult the low temperature radiant system documentation and the EnergyPlus code.
-
-### CoolTower
-
-#### Overview
-
-The Cool Tower (object ZoneCoolTower:Shower) is available for modeling a cooltower (which is sometimes referred to as s wind tower or a shower cooling tower) which is a component that is intended to model a passive downdraught evaporative cooling (PDEC) that is designed to capture the wind at the top of a tower and cool the outdoor air using water evaporation before delivering it to a space. The air flow in these systems is natural as the evaporation process increases the density of the air causing it to fall through the tower and into the space without the aid of a fan. A cooltower typically consists of a water spray or an evaporative pad, a shaft, and a water tank or reservoir. Wind catchers to improve the wind-driven performance at the top of the tower are optional. Water is pumped over an evaporative device by water pump which is the only component consumed power for this system. This water cools and humidifies incoming air and then the cool, dense air naturally falls down through shaft and leaves through large openings at the bottom of cooltowers.
-
-The shower cooling tower shown in figure below is controlled by a schedule and the specification of maximum water flow rate and volume flow rate as well as minimum indoor temperature. The actual flow rate of water and air can be controlled as users specify the fractions of water loss and flow schedule. The required input fields include effective tower height and exit area to obtain the temperature and flow rate of the air exiting the tower. A schedule and rated power for the water pump are also required to determine the power consumed. The component typically has a stand-alone water system that is not added to the water consumption from mains. However, users are required to specify the water source through an optional field, the name of water supply storage tank, in case any water comes from a water main.
-
-![cooltower config](media/image7400.svg.png)
-
-Figure 330. Typical Cooltower Configuration
-
-The cooltower model employing a model of the inertial shower cooling tower is intended to establish the actual mass flow rate of the air that leaves the cooltower and the evaporation rate consumed during the processes within the cooltower. Like infiltration, ventilation, and earth tubes, the air is assumed to be immediately mixed with the zone air. The determination of simultaneous heat and mass transfer that occurs during natural evaporative cooling in cooltower is complicated. Therefore, some assumptions have been made to obtain the conditions of the air and water. All cooltowers are executed at the start of each time step called by HVAC manager, and the conditions of air temperature and humidity ratio in the zone will be corrected with any other air that enters the zone.
-
-All temperatures in the following descriptions are in degrees C, mass flow rates are in kg/s, and volume flow rates are in m3/s.
-
-#### Model Description
-
-The user must input the required information according to the Input Output Reference Manual (ref: ZoneCoolTower:Shower). The cooltower model requires a unique identifying name, an availability schedule, and the name of the zone being served. The schedule name must refer to a valid schedule type (range 0-1) and contain values of fractional cooltower operation as well as water pump operation. For the determination of the exit temperature and actual air volume flow rate, four additional inputs are required: effective tower height, exit area, fraction of flow schedule, and fraction of water loss. These define the conditions of the exit air, obtaining the conditions of outdoor air from the weather data and thus allow EnergyPlus to correct both the temperature and humidity level in the zone. The power consumed by the water pump can be directly determined by the schedule and rated power that the user inputs. The component is also controlled by the specification of minimum indoor temperature, maximum volume flow rate, and maximum water flow rate. These allow the model to prevent overcooling the zone or overestimation of the air volume flow rate. In addition, the user must input a flow control type according to the information that the user is able to obtain.
-
-#### Simulation and Control
-
-The cooltower model first determines the temperature and volume flow rate of the exit air.  Both parameters can be directly determined in case of water flow schedule control when the water flow rate is known. With the outdoor temperatures obtained from weather data, the exit air temperature (*T<sub>out</sub>)* can be directly determined as functions of outdoor dry bulb temperature (DB), outdoor wet bulb temperature (WB), effective tower height (*H*) and water flow rate (WF) in l/min by using following equation.
-
-<div>$${T_{out}} = DB - (DB - WB)(1 - \exp ( - 0.8H))(1 - \exp ( - 0.15WF)$$</div>
-
-The volume flow rate of the exit air (Q) can also be directly obtained as functions of water flow rate and effective tower height from the following equation.
-
-<div>$$Q = 0.0125WF \cdot {H^{0.5}}$$</div>
-
-In case of that the calculated air volume flow rate is greater than maximum air volume flow rate in this control, which leads to overestimation of actual volume flow rate of the exit air, the calculated air volume flow rate is replaced with the maximum.
-
-For the simulation of wind-driven flow control where the water flow rate is unknown, the model determines velocity of the outlet air (*V<sub>out</sub>*) as functions of effective tower height and wind speed of outdoor air (WS) as
-
-<div>$${V_{out}} = 0.7{H^{0.5}} + 0.47(WS - 1)$$</div>
-
-The air volume flow rate (*Q*) is then calculated by
-
-<div>$${Q_{estimate}} = A \cdot {V_{out}}$$</div>
-
-where *A* is opening area at the bottom of cooltower.
-
-Substituting the air flow rate to the previous equation for *Q,* water flow rate is obtained as
-
-<div>$$WF = \frac{Q}{{0.0125 \cdot {H^{0.5}}}}$$</div>
-
-Once water flow rate is determined, the model checks the limit of water flow rate that the user inputs, so that the model prevents overestimation of actual volume flow rate of the exit air. If the calculated water flow rate is greater than the maximum water flow rate, the maximum will be chosen. The model also replaces the calculated air volume flow rate with the maximum volume flow rate from the user input when the calculated is greater than the maximum. Then, the model calculates the air volume flow rate and exit temperature using the previous equation for *Q* and *T<sub>out</sub>*.
-
-This cooltower model allows the user to specify water loss due to drift or blow down and the loss of air flow (example: a cooltower which delivers air to both the interior and exterior of the building). If the user inputs the fraction of water loss or flow schedule that means some amount of the air actually goes to outside, the fractional values will be applied to previously calculated ones so that the model calculates both actual water flow rate (*WF<sub>actual</sub>*) and air volume flow rate (*Q<sub>actual</sub>*) as follows:
-
-<div>$$W{F_{actual}} = WF(1.0 + Fraction)$$</div>
-
-<div>$${Q_{actual}} = Q(1.0 - Fraction)$$</div>
-
-The model then determines the exit humidity ratio (<span>\({\omega_{out}}\)</span>) from the relation of mass balances below.
-
-<div>$${\omega_{in}}({\dot m_{air}} + {\dot m_{water}}) = {\omega_{out}} \cdot {\dot m_{air}}$$</div>
-
-In this case, actual mass flow rate at the inlet and outlet of cooltower cannot be correctly calculated with limited information. Thus, the model estimates initial conditions of the air based on the outdoor temperatures, the calculated exit air temperature, enthalpy of outdoor air (*H<sub>in</sub>*) and outdoor barometric pressure (P). Assuming no enthalpy changes and pressure drops between inlet air and the initialized air, the humidity ratio and mass flow of the initialized air can be obtained by using EnergyPlus psychrometric functions and the following equation.
-
-<div>$${\omega_{in}} = PsyWRnTdbTwbPb({T_{d{b_{in}}}},{T_{w{b_{in}}}},P)$$</div>
-
-<div>$${\omega_{initial}} = PsyWRnTdbH({T_{out}},{H_{in}},P)$$</div>
-
-<div>$${\rho_{initial}}_{_{air}} = PsyRhoAirFnPbTdbW({T_{out}},{\omega_{initial}},P)$$</div>
-
-<div>$${\dot m_{air}} = {\rho_{initia{l_{air}}}} \cdot {Q_{actual}}$$</div>
-
-where <span>\({\omega_{initial}}\)</span>and <span>\({\rho_{initial}}\)</span> are the humidity ratio and air density of the initialized air and <span>\({\omega_{in}}\)</span>is the humidity ratio of outdoor air.
-
-Therefore, the humidity ratio of exit air, <span>\({\omega_{out}}\)</span>, is
-
-<div>$${\omega_{out}} = \frac{{{\omega_{in}}({{\dot m}_{air}} + {{\dot m}_{water}})}}{{{{\dot m}_{air}}}}$$</div>
-
-Once the humidity ratio at the exit is determined, the model can obtain the actual density (<span>\({\rho_{air}}\)</span>), specific heat (<span>\({c_p}_{,air}\)</span>), and mass flow rate (<span>\({\dot m_{cooltower}}\)</span>) of the air leaving cooltower by using EnergyPlus psychrometric function and following equation.
-
-<div>$${c_p}_{,air} = PsyCpAirFnWtdb({\omega_{out}},{T_{out}})$$</div>
-
-<div>$${\rho_{air}} = PsyRhoAirFnPbTdbW({T_{out}},{\omega_{out}},P)$$</div>
-
-<div>$${\dot m_{cooltower}} = {\rho_{air}} \cdot {Q_{actual}}$$</div>
-
-Assuming that the water temperature equals to outdoor wet bulb temperature, the model eventually determines density of the water and evaporation rate as bellows.
-
-<div>$${\rho_{water}} = RhoH2O({T_{w{b_{in}}}})$$</div>
-
-<div>$${Q_{water}} = \frac{{{{\dot m}_a}({\omega_{out}} - {\omega_{in}})}}{{{\rho_{water}}}}$$</div>
-
-### Earthtube
-
-The earth tube model (input object ZoneEarthtube) provides a simple earth tube model that uses a complex ground heat transfer model to establish the temperature of the soil at the depth of the earth tube.  The following information defines the basis for the model including the assumptions and mathematical equations.  It supplements the information for the ZoneEarthtube input object given in the Input/Output Reference for EnergyPlus.
-
-* Input Requirement
-
-Pipe : Pipe radius(m), Pipe thickness(m), Pipe length(m)
-
-Distance between the pipe outer surface and undisturbed soil (m),
-
-Pipe thermal conductivity (W/m-C),
-
-Air velocity inside pipe(m/s), Depth of the radial center of pipe below ground (m)
-
-Soil : Soil density(kg/m<sup>3</sup>), Soil specific heat(J/kg°C),
-
-Soil thermal Conductivity(W/m°C), Absorption coefficient,
-
-Fraction of evaporation rate
-
-* Assumption(s)
-
-* Convection flow inside the pipe is hydrodynamically and thermally developed.
-
-* Soil temperature in the pipe vicinity is uniform after the particular distance from the center of the pipe(thickness of the annulus), so that pipe surface temperature is uniform after the distance ‘r’ from the center of the pipe, where ‘r’is the pipe radius.
-
-* The temperature profile in the pipe vicinity is not affected by the presence of the pipe, so that pipe surface temperature is uniform at axial direction.
-
-* The soil surrounding the pipe has homogeneous thermal conductivity.
-
-* Pipe has uniform cross section area at axial direction.
-
-Wind velocity (m/s), u, is the annual average value. This is calculated from EnergyPlus weather data by averaging individual wind velocity values of the whole year. The convective heat transfer coefficient at the soil surface (W/m<sup>2</sup>°C), *h<sub>s</sub>*, is function of wind speed u. According to McAdams(1954) *h<sub>s</sub>* can be approximated by the following correlation (Krarti, 1995).
-
-<div>$${h_s} = 5.7 + 3.8u$$</div>
-
-In case of *h<sub>e</sub>* and *h<sub>r</sub>*, they can be determined by the following equations.
-
-<div>$${h_e} = {h_s}\left( {1 + 0.0168af} \right)$$</div>
-
-<div>$${h_r} = {h_s}\left( {1 + 0.0168a{r_a}f} \right)$$</div>
-
-with a = 103 Pa/°C.
-
-Average air temperature (°C), *T<sub>ma</sub>*, is also calculated from EnergyPlus weather data by averaging individual air temperature values of the whole year.
-
-The appropriate value of hemispherical emittance of the ground surface, *ε,* is 0.93~0.96. Radiation constant (W/m<sup>2</sup>), *ΔR,* depends on soil radiative properties, air relative humidity, and effective sky temperature. An appropriate value of *ΔR* according to Krarti (1995) is 63 W/m<sup>2</sup>.
-
-The absorption coefficient, *β*, depends on the soil absorptance and shading condition. The coefficient *β* is approximately equal to one minus the soil surface albedo. Albedo depends on soil cover and moisture content. Albedo=0.1 corresponds to wet soils, albedo=0.2 to moderate soils, and albedo=0.3 to dry soils.
-
-Average solar radiation (W/m<sup>2</sup>), *S<sub>m</sub>*, is determined from EnergyPlus weather data by averaging individual global horizontal solar radiation values of the whole year.
-
-The fraction of evaporation rate, *f*, also depends mainly on the soil cover and the soil moisture level. Based on the results reported by Penman, it is recommended to estimate the fraction f as follows. For bare soil, *f* is directly proportional to soil moisture content. For instance, f=1 corresponds to saturated soils, f=0.6~0.8 to wet soils, f=0.4~0.5 to moist soils, f=0.1~0.2 to arid soils. For dry soils, f = 0, since no evaporation occurs. For covered soils, the fraction f is obtained by multiplying 0.7 by the value of f for bare soil depending on the soil moisture content (Krarti, 1995).
-
-Relative humidity, *r<sub>a</sub>*, is also calculated from EnergyPlus weather data by averaging individual relative humidity values of the whole year.
-
-The soil thermal diffusivity (m<sup>2</sup>/s), *α<sub>s</sub>*, and conductivity (W/m°C), *k<sub>s</sub>*, varies with the density and moisture content. From Table 3.3, pg. 26 of ASHRAE's Ground Source Heat Pumpss--Design of Geothermal Systems for Commercial and Institutional Buildings, 1997, the following values are recommended under different conditions.
-
-<table>
-  <tr>
-    <th></th>
-    <th>Moisture Content</th>
-    <th>5%</th>
-    <th>5%</th>
-    <th>10%</th>
-    <th>10%</th>
-    <th>15%</th>
-    <th>15%</th>
-    <th>20%</th>
-    <th>20%</th>
-  </tr>
-  <tr>
-    <td>Soil <br>Type</td>
-    <td>Dry Density<br>[kg/m3]</td>
-    <td>k<br>[W/m-K]</td>
-    <td>α<sub>s</sub><br>[m2/s]</td>
-    <td>k<br>[W/m-K]</td>
-    <td>α<sub>s</sub><br>[m2/s]</td>
-    <td>k<br>[W/m-K]</td>
-    <td>α<sub>s</sub><br>[m2/s]</td>
-    <td>k<br>[W/m-K]</td>
-    <td>α<sub>s</sub><br>[m2/s]</td>
-  </tr>
-  <tr>
-    <td>Coarse 100%<br>Sand</td>
-    <td>1922</td>
-    <td>2.77</td>
-    <td>1.34E-06</td>
-    <td>2.94</td>
-    <td>1.24E-06</td>
-    <td>3.29</td>
-    <td>1.18E-06</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>1602</td>
-    <td>1.90</td>
-    <td>1.18E-06</td>
-    <td>2.34</td>
-    <td>1.18E-06</td>
-    <td>2.51</td>
-    <td>1.08E-06</td>
-    <td>2.68</td>
-    <td>8.82E-07</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>1281</td>
-    <td>1.38</td>
-    <td>1.18E-06</td>
-    <td>1.56</td>
-    <td>9.14E-07</td>
-    <td>1.56</td>
-    <td>8.06E-07</td>
-    <td>1.47</td>
-    <td>6.99E-07</td>
-  </tr>
-  <tr>
-    <td>Fine Grain<br>100% Clay</td>
-    <td>1922</td>
-    <td>1.21</td>
-    <td>5.91E-07</td>
-    <td>1.21</td>
-    <td>4.84E-07</td>
-    <td>1.64</td>
-    <td>5.70E-07</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>1602</td>
-    <td>0.95</td>
-    <td>5.70E-07</td>
-    <td>0.95</td>
-    <td>4.73E-07</td>
-    <td>1.12</td>
-    <td>4.73E-07</td>
-    <td>1.21</td>
-    <td>5.16E-07</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>1281</td>
-    <td>0.69</td>
-    <td>4.84E-07</td>
-    <td>0.74</td>
-    <td>4.62E-07</td>
-    <td>0.81</td>
-    <td>4.73E-07</td>
-    <td>0.87</td>
-    <td>4.09E-07</td>
-  </tr>
-</table>
-
-The following information is also available for reference from Table 4, pg. 34.6 of the ASHRAE Applications Handbook, 2015.
-
-<table>
-  <tr>
-    <th>Soils</th>
-    <th>Moisture<br>Content</th>
-    <th>Density<br>[kg/m3]</th>
-    <th>k<br>[W/m-K]</th>
-    <th>α<sub>s</sub><br>[m^2/s]</th>
-  </tr>
-  <tr>
-    <td>Heavy clay</td>
-    <td>15% water</td>
-    <td>1922</td>
-    <td>1.558</td>
-    <td>5.914E-07</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>5% water</td>
-    <td>1922</td>
-    <td>1.212</td>
-    <td>6.452E-07</td>
-  </tr>
-  <tr>
-    <td>Light clay</td>
-    <td>15% water</td>
-    <td>1281</td>
-    <td>0.865</td>
-    <td>4.624E-07</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>5% water</td>
-    <td>1281</td>
-    <td>0.692</td>
-    <td>4.839E-07</td>
-  </tr>
-  <tr>
-    <td>Heavy sand</td>
-    <td>15% water</td>
-    <td>1922</td>
-    <td>3.115</td>
-    <td>1.129E-07</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>5% water</td>
-    <td>1922</td>
-    <td>2.596</td>
-    <td>1.344E-06</td>
-  </tr>
-  <tr>
-    <td>Light sand</td>
-    <td>15% water</td>
-    <td>1281</td>
-    <td>1.558</td>
-    <td>8.065E-07</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>5% water</td>
-    <td>1281</td>
-    <td>1.385</td>
-    <td>9.677E-07</td>
-  </tr>
-</table>
-
-Annual angular frequency, *w*, is equal to 1.992 x 10<sup>-7</sup>rad/s, and dampening depth (m), D, is calculated from the following equation:
-
-<div>$$D = \sqrt {\frac{{2{\alpha_s}}}{w}} $$</div>
-
-The value of δ is evaluated as follows.
-
-<div>$$\delta  = \frac{{1 + i}}{D}$$</div>
-
-Amplitude of the air temperature (°C), *T<sub>va</sub>*, can be evaluated from EnergyPlus weather data by dividing the difference between the maximum and minimum air temperature value of the whole year by two. Similarly, amplitude of the solar radiation (W/m<sup>2</sup>), *S<sub>v</sub>*, can also be determined from weather data by dividing the difference between the maximum and minimum solar radiation value of the whole year by two.
-
-Phase angle between the insolation and the air temperature (rad), *φ<sub>I</sub>* , is calculated by subtracting insolation phase angle from air temperature phase angle. Phase angle of insolation and air temperature is the point from the beginning of the year at which the insolation and air temperature respectively reaches the minimum value among the whole year.
-
-Phase constant of the air (sec), *t<sub>0a</sub>*, is the time elapsed from the beginning of the year at which the air temperature reaches the minimum value in the year.
-
-By using all the input parameters and variables described above, average soil surface temperature (°C), *T<sub>m</sub>*, amplitude of the soil surface temperature variation (°C), *A<sub>s</sub>*, phase constant of the soil surface (sec), *t<sub>0</sub>*, and phase angle difference between the air and soil surface temperature (rad), *Φ<sub>s</sub>*, can be evaluated as follows <sup>1)</sup>:
-
-<div>$${T_m} = \frac{1}{{{h_e}}}\left[ {{h_r}{T_{ma}} - \varepsilon \Delta R + \beta {S_m} - 0.0168{h_s}fb\left( {1 - {r_a}} \right)} \right]$$</div>
-
-<div>$${A_s} = \left\| {\frac{{{h_r}{T_{va}} - \beta {S_v}{e^{i{\phi_I}}}}}{{\left( {{h_e} + \delta {k_s}} \right)}}} \right\|$$</div>
-
-<div>$${t_0} = {t_{0a}} + \frac{{{\phi_s}}}{w}$$</div>
-
-<div>$${\phi_s} =  - Arg\left[ {\frac{{{h_r}{T_{va}} - \beta {S_v}{e^{i{\phi_I}}}}}{{\left( {{h_e} + \delta {k_s}} \right)}}} \right]$$</div>
-
-(Note: T<sub>m</sub>, A<sub>s</sub>, and t<sub>0</sub> are calculated by the CalcSoilSurfTemp program and are inputs to EnergyPlus.  The remainder of this section describes what has been implemented in EnergyPlus.)
-
-The symbols ||  || and Arg denote the modulus and the argument of a complex number respectively. In order to calculate *A<sub>s</sub>* and *Φ<sub>s</sub>*, the complex number under consideration can be rearranged as the following form:
-
-<div>$$\begin{array}{l}\frac{{{h_r}{T_{va}} - \beta {S_v}{e^{i{\phi_I}}}}}{{\left( {{h_e} + \delta {k_s}} \right)}} = \\ frac{{\left( {{h_e} + \frac{{{k_s}}}{D}} \right)\left( {{h_r}{T_{va}} - \beta {S_v}\cos {\phi_I}} \right) + \frac{{{k_s}}}{D}\left( { - \beta {S_v}\sin {\phi_I}} \right)}}{{{{\left( {{h_e} + \frac{{{k_s}}}{D}} \right)}^2} + {{\left( {\frac{{{k_s}}}{D}} \right)}^2}}} + \\i\frac{{\left( {{h_e} + \frac{{{k_s}}}{D}} \right)\left( { - \beta {S_v}\sin {\phi_I}} \right) - \frac{{{k_s}}}{D}\left( {{h_r}{T_{va}} - \beta {S_v}\cos {\phi_I}} \right)}}{{{{\left( {{h_e} + \frac{{{k_s}}}{D}} \right)}^2} + {{\left( {\frac{{{k_s}}}{D}} \right)}^2}}}\end{array}$$</div>
-
-Assuming a homogeneous soil of constant thermal diffusivity, the temperature at any depth z and time t can be estimated by the following expression <sup>2)</sup>.
-
-<div>$${T_{z,t}} = {T_m} - {A_s}\exp \left[ { - z{{\left( {\frac{\pi }{{{\rm{365}}{\alpha_s}}}} \right)}^{1/2}}} \right]\cos \left\{ {\frac{{2\pi }}{{{\rm{365}}}}\left[ {t - {t_0} - \frac{z}{2}{{\left( {\frac{{{\rm{365}}}}{{\pi {\alpha_s}}}} \right)}^{1/2}}} \right]} \right\}$$</div>
-
-In this expression, the unit of time, *t*, and phase constant of the soil surface, *t<sub>0</sub>*, should be converted into days. Similarly, the unit of soil thermal diffusivity, *α<sub>s</sub>*, should also be converted into m<sup>2</sup>/days.
-
-By integrating the expression with respect to depth, the average temperature of a vertical soil profile ranging between depth z<sub>1</sub> and z<sub>2</sub> (°C ) can be determined as follows <sup>2)</sup>.
-
-<div>$${T_{{z_1},{z_2},t}} = {T_m} + \frac{{{A_s}}}{{\left( {{z_2} - {z_1}} \right)\gamma \sqrt 2 }}\left\{ {{e^{ - \gamma {z_1}}}\cos \left[ {\frac{{2\pi }}{{{\rm{365}}}}\left( {t - {t_0} - {z_1}L - 45.6} \right)} \right] - {e^{ - \gamma {z_2}}}\cos \left[ {\frac{{2\pi }}{{{\rm{365}}}}\left( {t - {t_0} - {z_2}L - 45.6} \right)} \right]} \right\}$$</div>
-
-
-
-where,
-
-<div>$$\gamma  = {\left( {\pi /{\rm{365}}{\alpha_s}} \right)^{1/2}}$$</div>
-
-<div>$$L = \frac{1}{2}{\left( {{\rm{365}}/\pi {\alpha_s}} \right)^{1/2}}$$</div>
-
-As the final step with regard to the heat transfer between soil and earth tube system, thermal conductivity of air (W/m°C), *k<sub>air</sub>*, and kinetic viscosity of air (m<sup>2</sup>/s), υ, should calculated first <sup>3)</sup>.
-
-<div>$${k_{air}} = 0.02442 + ({10^{ - 4}}(0.6992{T_a}))$$</div>
-
-<div>$$\upsilon  = {10^{ - 4}}(0.1335 + 0.000925{T_a})$$</div>
-
-By using the values of thermal conductivity of air, *k<sub>air</sub>*, and kinetic viscosity of air, υ, the convective heat transfer coefficient at the inner pipe surface (W/m<sup>2</sup>°C), *h<sub>c,</sub>* can be evaluated. It is a function of Reynolds number, Re, and Nusselt number, Nu <sup>4)</sup>, where
-
-<div>$${h_c} = \frac{{Nu{k_{air}}}}{{2{r_1}}}$$</div>
-
-<div>$$Nu = \frac{{({f_a}/2)({\mathop{\rm Re}\nolimits}  - 1000)\Pr }}{{1 + 12.7{{({f_a}/2)}^{1/2}}({{\Pr }^{2/3}} - 1)}}$$</div>
-
-<div>$${f_a} = {(1.58\ln {\mathop{\rm Re}\nolimits}  - 3.28)^{ - 2}}$$</div>
-
-<div>$${\mathop{\rm Re}\nolimits}  = \frac{{2{r_1}{V_a}}}{\nu }$$</div>
-
-<div>$$\Pr  = \frac{\nu }{{{\alpha_{air}}}}$$</div>
-
-where *r<sub>1</sub>* is inner pipe radius (m), and *V<sub>a</sub>* is average pipe air velocity (m/s).
-
-After determining the convective heat transfer coefficient, *R<sub>c</sub>*, *R<sub>p</sub>* and *R<sub>s</sub>* are respectively calculated as follows.
-
-<div>$${R_c} = \frac{1}{{2\pi {r_1}{h_c}}}$$</div>
-
-<div>$${R_p} = \frac{1}{{2\pi {k_p}}}\ln \frac{{{r_1} + {r_2}}}{{{r_1}}}$$</div>
-
-<div>$${R_s} = \frac{1}{{2\pi {k_s}}}\ln \frac{{{r_1} + {r_2} + {r_3}}}{{{r_1} + {r_2}}}$$</div>
-
-where *R<sub>c</sub>* is thermal resistance due to convection heat transfer between the air in the pipe and the pipe inner surface (m-C/W), *R<sub>p</sub>* is thermal resistance due to conduction heat transfer between the pipe inner and outer surface (m-C/W), and *R<sub>s</sub>* is thermal resistance due to conduction heat transfer between the pipe outer surface and undisturbed soil (m-C/W). In addition *r<sub>2</sub>* is pipe thickness (m), *r<sub>3</sub>* is distance between the pipe outer surface and undisturbed soil (m), and *L* is pipe length (m).
-
-Finally, the heat transfer between the soil and the air inside the pipe is equal to the amount of heat losses as air flows along the pipe (Jacovides and Mihalakakou, 1995).
-
-<div>$${U_t}\,\,\left[ {{T_a}(y) - {T_{z,t}}} \right]dy =  - {\dot m_a}{C_a}\left[ {d{T_a}(y)} \right]$$</div>
-
-with
-
-<div>$${U_t} = \frac{1}{{{R_t}}}$$</div>
-
-<div>$${R_t} = {R_c} + {R_p} + {R_s}$$</div>
-
-where *U<sub>t</sub>* is overall heat transfer coefficient of the whole earth tube system (W/C-m), *T<sub>a</sub>(y)* is air temperature of the pipe at the distance y from the pipe inlet (°C), and *m<sub>a</sub>* is mass flow rate of ambient air through pipe (kg/s). *C<sub>a</sub>* is specific heat of air (J/kg°C) and *R<sub>t</sub>* is total thermal resistance between pipe air and soil (m-C/W).
-
-Initial condition of inlet air temperature is equal to the ambient air temperature. Outlet air temperature is finally evaluated by solving the heat transfer equation above.
-
-Table 87.  Nomenclature for Earthtube Model
-
-<table class="table table-striped">
-<tr>
-<td>Variable</td>
-<td>Description</td>
-<td>Units</td>
-</tr>
-<tr>
-<td>A<sub>s</sub></td>
-<td>amplitude of the soil surface temperature variation</td>
-<td>(°C)</td>
-</tr>
-<tr>
-<td>C<sub>a</sub></td>
-<td>specific heat of air</td>
-<td>(J/kg°C)</td>
-</tr>
-<tr>
-<td>h<sub>c</sub></td>
-<td>convective heat transfer coefficient at the inner pipe surface</td>
-<td>(W/m<sup>2</sup>°C)</td>
-</tr>
-<tr>
-<td>h<sub>s</sub></td>
-<td>convective heat transfer coefficient at the soil surface</td>
-<td>(W/m<sup>2</sup>°C)</td>
-</tr>
-<tr>
-<td>k<sub>air</sub></td>
-<td>thermal conductivity of the air</td>
-<td>(W/m°C)</td>
-</tr>
-<tr>
-<td>k<sub>p</sub></td>
-<td>pipe thermal conductivity</td>
-<td>(W/m°C)</td>
-</tr>
-<tr>
-<td>k<sub>s</sub></td>
-<td>soil thermal conductivity</td>
-<td>(W/m°C)</td>
-</tr>
-<tr>
-<td>L</td>
-<td>pipe length</td>
-<td>(m)</td>
-</tr>
-<tr>
-<td>m<sub>a</sub></td>
-<td>mass flow rate of ambient air through pipe</td>
-<td>(kg/s)</td>
-</tr>
-<tr>
-<td>r<sub>a</sub></td>
-<td>relative humidity</td>
-<td> </td>
-</tr>
-<tr>
-<td>R<sub>c</sub></td>
-<td>thermal resistance due to convection heat transfer between the air in the pipe and the pipe inner surface</td>
-<td>(m-C/W)</td>
-</tr>
-<tr>
-<td>R<sub>p</sub></td>
-<td>thermal resistance due to conduction heat transfer between the pipe inner and outer surface</td>
-<td>(m-C/W)</td>
-</tr>
-<tr>
-<td>R<sub>s</sub></td>
-<td>thermal resistance due to conduction heat transfer between the pipe outer surface and undisturbed soil</td>
-<td>(m-C/W)</td>
-</tr>
-<tr>
-<td>R<sub>t</sub></td>
-<td>total thermal resistance between pipe air and soil</td>
-<td>(m-C/W)</td>
-</tr>
-<tr>
-<td>ΔR</td>
-<td>radiation constant</td>
-<td>(63W/m<sup>2</sup>)</td>
-</tr>
-<tr>
-<td>r<sub>1</sub></td>
-<td>inner pipe radius</td>
-<td>(m)</td>
-</tr>
-<tr>
-<td>r<sub>2</sub></td>
-<td>pipe thickness</td>
-<td>(m)</td>
-</tr>
-<tr>
-<td>r<sub>3</sub></td>
-<td>distance between the pipe outer surface and undisturbed soil</td>
-<td>(m)</td>
-</tr>
-<tr>
-<td>S<sub>m</sub></td>
-<td>average solar radiation</td>
-<td>(W/m<sup>2</sup>)</td>
-</tr>
-<tr>
-<td>S<sub>v</sub></td>
-<td>amplitude of the solar radiation</td>
-<td>(W/m<sup>2</sup>)</td>
-</tr>
-<tr>
-<td>t</td>
-<td>time elapsed from beginning of calendar year</td>
-<td>(days)</td>
-</tr>
-<tr>
-<td>T<sub>a</sub>(y)</td>
-<td>air temperature of the pipe at the distance y from the pipe inlet</td>
-<td>(°C)</td>
-</tr>
-<tr>
-<td>T<sub>m</sub></td>
-<td>average soil surface temperature</td>
-<td>(°C)</td>
-</tr>
-<tr>
-<td>T<sub>ma</sub></td>
-<td>average air temperature</td>
-<td>(°C)</td>
-</tr>
-<tr>
-<td>t<sub>0</sub></td>
-<td>phase constant of the soil surface</td>
-<td>(sec; days)</td>
-</tr>
-<tr>
-<td>t<sub>0a</sub></td>
-<td>phase constant of the air</td>
-<td>(sec; days)</td>
-</tr>
-<tr>
-<td>T<sub>va</sub></td>
-<td>amplitude of the air temperature</td>
-<td>(°C)</td>
-</tr>
-<tr>
-<td>T<sub>z,t</sub></td>
-<td>ground temperature at time t and depth z</td>
-<td>(°C)</td>
-</tr>
-<tr>
-<td>T<sub>z1,z2,t</sub></td>
-<td>soil profile temperature at time t, averaged over depths between z<sub>1</sub> and z<sub>2</sub></td>
-<td>(°C)</td>
-</tr>
-<tr>
-<td>u</td>
-<td> wind velocity above the ground surface</td>
-<td>(m/s)</td>
-</tr>
-<tr>
-<td>U<sub>t</sub></td>
-<td>overall heat transfer coefficient of the whole earth tube system</td>
-<td>(W/m-C)</td>
-</tr>
-<tr>
-<td>V<sub>a</sub></td>
-<td>average pipe air velocity</td>
-<td>(m/s)</td>
-</tr>
-<tr>
-<td>z</td>
-<td>depth of the radial center of pipe below soil surface</td>
-<td>(m)</td>
-</tr>
-<tr>
-<td>z<sub>1</sub></td>
-<td>upper bounds of some vertical profile in soil</td>
-<td>(m)</td>
-</tr>
-<tr>
-<td>z<sub>2</sub></td>
-<td>lower bounds of some vertical profile in soil</td>
-<td>(m)</td>
-</tr>
-<tr>
-<td>α<sub>s</sub></td>
-<td>soil thermal diffusivity</td>
-<td>(m<sup>2</sup>/s; m<sup>2</sup>/days)</td>
-</tr>
-<tr>
-<td>β</td>
-<td>soil absorption coefficient (= 1 – soil albedo)</td>
-<td> </td>
-</tr>
-<tr>
-<td>ε</td>
-<td>hemispherical emittance of the ground surface</td>
-<td> </td>
-</tr>
-<tr>
-<td>φ<sub>I</sub></td>
-<td>phase angle between the insolation and the air temperature</td>
-<td>(rad)</td>
-</tr>
-<tr>
-<td>Φ<sub>s</sub></td>
-<td>phase angle difference between the air and soil surface temperature</td>
-<td>(rad)</td>
-</tr>
-<tr>
-<td>Ï…</td>
-<td>kinetic viscosity of air</td>
-<td>(m<sup>2</sup>/s)</td>
-</tr>
-<tr>
-<td>w</td>
-<td>annual angular frequency (=1.992 x 10<sup>-7</sup>rad/s)</td>
-<td> </td>
-</tr>
-
-</table>
-
-#### References
-
-Krarti M., Lopez-Alonzo C., Claridge D. E. and Kreider J. F. 1995. Analytical model to predict annual soil surface temperature variation. Journal of Solar Energy Engineering 117, 91~99
-
-Labs K. In: Cook J., editor. 1989. Passive cooling. Cambridge Massachusetts, London, England: MIT Press
-
-Al-Ajmi F., Loveday D. L. and Hanby V. I. 2005. The Cooling Potential of Earth-air Heat Exchangers for Domestic Buildings in a Desert Climate, Building and Environment
-
-Necati Ozisik M. 1885. Heat transfer: A basic approach, McGraw-Hill Book Company
-
-Jacovides C. P. and Mihalakakou G. 1995. An Underground Pipe Systems as an Energy Source for Cooling/Heating Purposes. Renewable Energy 6, pp.893~900
-
-### Thermal Chimney Model
-
-The ZoneThermalChimney input object is available for modeling a thermal chimney which is a device that uses stack driven air movement to ventilate spaces within a building. These systems have been used successfully in buildings as small as the size of an outhouse up to large commercial buildings. The air within a thermal chimney is heated naturally using solar energy. The air increases in temperature which causes its density to drop. This drop in density results in a natural vertical movement of air and a local drop in pressure. The drop in pressure is relieved by drawing air from the building interior, and the heat gained within the thermal chimney does not enter the occupied portion of the building. These systems are often used in support of natural ventilation systems. The EnergyPlus model will seek to model the air heat balance effects of the thermal chimney, balance air movements caused by the thermal chimney, and report other appropriate system variables. The new model will be linked into the air heat balance in a fashion similar to the current infiltration and simple ventilation models but will not be linked to an HVAC air loop.  Any flow through the thermal chimney will be accounted for in the air mass balance in the HVAC calculations. However, other sophisticated ventilation strategies can be handled by other existing EnergyPlus components.
-
-* Thermal Chimney Input Requirements
-
-* Distance from the top of thermal chimney to each inlet (m),
-
-* Relative ratio of air flow rates passing through each inlet,
-
-* Width of the absorber wall (m),
-
-* Discharge coefficient,
-
-* Cross sectional area of air channel outlet (m<sup>2</sup>),
-
-* Cross sectional areas of each air channel inlet (m<sup>2</sup>)
-
-*  Assumptions
-
-* Surface temperature of the glass cover is uniformly distributed.
-
-* Surface temperature of the absorber wall is uniformly distributed.
-
-* The inlet temperature of the air channel in the thermal chimney is equal to the room air temperature.
-
-* Resistance to the air flow due to the surface friction is negligible.
-
-* The discharged amount of interior air induced by the thermal chimney is replaced by the outdoor air infiltration.
-
-![Thermal Chimney](media/image7454.png)
-
-Figure 331. Basic Composition of Thermal Chimney
-
-Mathematical model currently available for thermal chimneys has the capability to handle the thermal chimney having only one inlet. In other words, it is unlikely that thermal chimneys with multiple inlets due to multiple stories utilizing the common thermal chimney can be mathematically modeled without computational fluid dynamics. Therefore, if the thermal chimney to be modeled has multiple inlets, it will be assumed that it will have only one inlet. For this assumption, the user will be required to specify the relative ratio of air flow rates passing through each inlet to compute the overall length of the thermal chimney (m), *L*, overall room air temperature (K), *T<sub>r</sub>*, and overall cross sectional area of air channel inlet (m<sup>2</sup>), *A<sub>i</sub>*, as follows:
-
-<div>$$L = \frac{{{L_1}{r_1}{E_1} + {L_2}{r_2}{E_2} + {L_3}{r_3}{E_3} +  \cdot  \cdot  \cdot  + {L_n}{r_n}{E_n}}}{{{r_1}{E_1} + {r_2}{E_2} + {r_3}{E_3} +  \cdot  \cdot  \cdot  + {r_n}{E_n}}}$$</div>
-
-<div>$${T_r} = {T_{r1}}{r_1} + {T_{r2}}{r_2} + {T_{r3}}{r_3} +  \cdot  \cdot  \cdot  + {T_{rn}}{r_n}$$</div>
-
-<div>$${A_i} = {A_{i1}} + {A_{i2}} + {A_{i3}} +  \cdot  \cdot  \cdot  + {A_{in}}$$</div>
-
-Where, *A<sub>in</sub>* is the cross sectional area of nth air channel inlet (m<sup>2</sup>), *L<sub>n</sub>* is the distance from the top of thermal chimney to nth inlet (m), *E<sub>n</sub>* is the room air specific enthalpy corresponding to nth inlet (J/kg), *r<sub>n</sub>* is the relative ratio of air flow rate passing through nth inlet and *T<sub>rn</sub>* is the room air temperature corresponding to nth inlet (K). Among them, room air specific enthalpy, *E<sub>n</sub>*, and room air temperature corresponding to each inlet, *T<sub>rn</sub>*, are directly calculated inside EnergyPlus. In addition, the relative ratios should meet the following expression:
-
-<div>$${r_1} + {r_2} + {r_3} +  \cdot  \cdot  \cdot  + {r_n} = 1$$</div>
-
-After merging the multiple inlets into a single inlet condition based on the description above, the following algorithm which is widely used is employed for the modeling of the thermal chimney.
-
-The key output parameter in the thermal chimney model is the enhanced amount of natural ventilation rate caused by the presence of a thermal chimney. In order to determine the enhanced ventilation, the discharge air temperature from a thermal chimney should be calculated, which, in turn, should be computed based on the information on the absorber wall temperature, glass cover temperature and the vertical air temperature distribution within the thermal chimney. Among them, energy balances for the absorber wall and the glass cover are carried out using the existing algorithm currently available in EnergyPlus, which has the similar approach to the Trombe wall. On the other hand, the vertical air temperature distribution and the resultant discharge air temperature of the thermal chimney are computed using the separate thermal chimney algorithm described in the following paragraphs.
-
-Once the glass cover temperature and the absorber wall temperature are computed using the existing modeling algorithm in EnergyPlus, the energy balance for the fluid (air inside the thermal chimney) can be expressed as:
-
-<div>$${h_{wf}}({T_w} - \overline {{T_f}} ) = {h_{gf}}(\overline {{T_f}}  - {T_g}) + \frac{{\dot m{C_p}}}{w}\frac{{d{T_f}}}{{dx}}$$</div>
-
-Where, *m* is the total mass flow rate of the air (kg/s), *C<sub>p</sub>* is the specific heat of air (J/kg°C), *w* is the width of the absorber wall (m) and *x* is the elemental length of the absorber wall (m).
-
-Since the initial condition of inlet air temperature in this differential equation is equal to the room air temperature (i.e. *x = 0, T<sub>f,i</sub> = T<sub>r</sub>*), the outlet air temperature, *T<sub>fo</sub>*, can be finally evaluated.
-
-Finally, the total air flow rate caused by the thermal chimney (m<sup>3</sup>/s), *Q*, can be evaluated from the following expression [1]:
-
-<div>$$Q = {C_d}{A_o}\sqrt {\frac{{2(\frac{{{T_{fo}} - {T_r}}}{{{T_r}}})gL}}{{{{(1 + {A_r})}^2}}}} $$</div>
-
-<div>$${A_r} = {A_o}/{A_i}$$</div>
-
-Where, *C<sub>d</sub>* is the discharge coefficient, *A<sub>o</sub>* and *A<sub>i</sub>* is the cross sectional areas of air channel outlet and inlet (m<sup>2</sup>), respectively, *T<sub>fo</sub>* is the outlet air temperature (K), *T<sub>r</sub>* is the room air temperature (K) and *L* is the total length of the thermal chimney (m).
-
-Since multiple inlets are merged into a single inlet in the beginning, the air flow rate passing through each inlet due to the existence of the thermal chimney can be finally determined as follows:
-
-<span>\({Q_1} = Q{r_1}\)</span>,    <span>\({Q_2} = Q{r_2}\)</span>,    <span>\({Q_3} = Q{r_3}\)</span>,    ∙∙∙,    <span>\({Q_n} = Q{r_n}\)</span>
-
-Where, *Q<sub>n</sub>* is the air flow rate passing through nth inlet (m<sup>3</sup>/s) and *r<sub>n</sub>* is the relative ratio of air flow rate passing through nth inlet.
-
-The discharged amount of interior air from each zone caused by the presence of the thermal chimney is assumed to be replaced by the outdoor air infiltration.
-
-
-
-Table 88. Nomenclature of Thermal Chimney Model
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="2">Model Nomenclature</th>
-  </tr>
-  <tr>
-    <th>Variable</th>
-    <th>Description</th>
-  </tr>
-  <tr>
-    <td>A<sub>i</sub></td>
-    <td>cross sectional area of air channel inlet (m 2 )</td>
-  </tr>
-  <tr>
-    <td>A<sub>o</sub></td>
-    <td>cross sectional area of air channel outlet (m 2 )</td>
-  </tr>
-  <tr>
-    <td>C<sub>d</sub></td>
-    <td>discharge coefficient</td>
-  </tr>
-  <tr>
-    <td>C<sub>p</sub></td>
-    <td>specific heat of air (J/kg°C)</td>
-  </tr>
-  <tr>
-    <td>E<sub>n</sub></td>
-    <td>room air specific enthalpy corresponding to nth inlet (J/kg)</td>
-  </tr>
-  <tr>
-    <td>g</td>
-    <td>acceleration due to gravity (9.8 m/s 2 )</td>
-  </tr>
-  <tr>
-    <td>h<sub>gam</sub></td>
-    <td>convective heat transfer coefficients between the glass and ambient air (W/m 2 °C )</td>
-  </tr>
-  <tr>
-    <td>h<sub>gf</sub></td>
-    <td>convective heat transfer coefficients between the glass and the fluid (W/m 2 °C )</td>
-  </tr>
-  <tr>
-    <td>h<sub>iw</sub></td>
-    <td>convective heat transfer coefficients between absorber wall inner surface and the room air (W/m 2 °C )</td>
-  </tr>
-  <tr>
-    <td>h<sub>wf</sub></td>
-    <td>convective heat transfer coefficients between the absorber wall and the fluid (W/m 2 °C )</td>
-  </tr>
-  <tr>
-    <td>h<sub>wind</sub></td>
-    <td>The convective heat transfer coefficient due to the wind (W/m 2 °C )</td>
-  </tr>
-  <tr>
-    <td>H<sub>sr</sub></td>
-    <td>incident solar radiation on vertical surface (W/m 2 )</td>
-  </tr>
-  <tr>
-    <td>k<sub>air</sub></td>
-    <td>thermal conductivity of air (W/m°C)</td>
-  </tr>
-  <tr>
-    <td>L</td>
-    <td>total length of the thermal chimney (m)</td>
-  </tr>
-  <tr>
-    <td>M</td>
-    <td>mass flow rate of the air (kg/s)</td>
-  </tr>
-  <tr>
-    <td>r<sub>n</sub></td>
-    <td>relative ratio of air flow rate passing through nth inlet</td>
-  </tr>
-  <tr>
-    <td>S<sub>g</sub></td>
-    <td>solar radiation absorbed by the glass cover (W/m 2 )</td>
-  </tr>
-  <tr>
-    <td>S<sub>w</sub></td>
-    <td>solar radiation absorbed by the absorber wall (W/m 2 )</td>
-  </tr>
-  <tr>
-    <td>T<sub>am</sub></td>
-    <td>ambient air temperature (K)</td>
-  </tr>
-  <tr>
-    <td>T<sub>f</sub></td>
-    <td>fluid temperature averaged over the entire length of the thermal chimney (K)</td>
-  </tr>
-  <tr>
-    <td>T<sub>fi</sub></td>
-    <td>inlet air temperature of the thermal chimney (K)</td>
-  </tr>
-  <tr>
-    <td>T<sub>fo</sub></td>
-    <td>outlet air temperature of the thermal chimney (K)</td>
-  </tr>
-  <tr>
-    <td>T<sub>g</sub></td>
-    <td>glass cover temperature (K)</td>
-  </tr>
-  <tr>
-    <td>T<sub>r</sub></td>
-    <td>room air temperature (K)</td>
-  </tr>
-  <tr>
-    <td>T<sub>s</sub></td>
-    <td>surface temperature (K)</td>
-  </tr>
-  <tr>
-    <td>T<sub>w</sub></td>
-    <td>absorber wall temperature (K)</td>
-  </tr>
-  <tr>
-    <td>T<sub>inf</sub></td>
-    <td>fluid temperature (K)</td>
-  </tr>
-  <tr>
-    <td>u</td>
-    <td>wind speed (m/s)</td>
-  </tr>
-  <tr>
-    <td>U<sub>w</sub></td>
-    <td>Overall heat transfer coefficient from the room air and the absorber wall (W/m 2 °C )</td>
-  </tr>
-  <tr>
-    <td>w</td>
-    <td>width of the absorber wall (m)</td>
-  </tr>
-  <tr>
-    <td>x</td>
-    <td>elemental length of the absorber wall (m)</td>
-  </tr>
-  <tr>
-    <td>alpha<sub>g</sub></td>
-    <td>absorptance of glass cover</td>
-  </tr>
-  <tr>
-    <td>alpha<sub>w</sub></td>
-    <td>absorptance of absorber wall</td>
-  </tr>
-  <tr>
-    <td>beta</td>
-    <td>air volumetric coefficient of expansion (K -1 )</td>
-  </tr>
-  <tr>
-    <td>epsilon<sub>g</sub></td>
-    <td>emissivity of the glass cover</td>
-  </tr>
-  <tr>
-    <td>sigma</td>
-    <td>Stefan-Boltzmann constant (5.67x10 -8 W/m 2 K 4 )</td>
-  </tr>
-  <tr>
-    <td>T</td>
-    <td>transmittance of the glass cover</td>
-  </tr>
-  <tr>
-    <td>nu</td>
-    <td>kinematic viscosity of air (m 2 /s)</td>
-  </tr>
-</table>
-
-
-#### References
-
-N. K. Bansal, R. Mathur and M. S. Bhandari, Solar Chimney for enhanced Stack Ventilation, Building and Environment, 28, pp.373-377, 1993
-
-K. S. Ong, A Mathematical Model of a Solar Chimney, Renewable Energy, 28, pp.1047-1060, 2003
-
-N. K. Bansal, R. Mathur and M. S. Bhandari, A Study of Solar Chimney Assisted Wind Tower System for Natural Ventilation in Buildings, Building and Environment, 29, pp.495-500, 1994
-
-J. Marti-Herrero and M. R. Heras-Celemin, Dynamic Physical Model for a Solar Chimney, Solar Energy, 81, pp. 614-622, 2007
-
-M. M. Aboulnaga and S. N. Abdrabboh, Improving Night Ventilation into Low-rise Buildings in Hot-arid Climates Exploring a Combined Wall-roof Solar Chimney, Renewable Energy, 19, pp. 47-54, 2000
-
-
-
-### Zone Outdoor Air Unit
-
-The zone outdoor air unit (object ZoneHVAC:OutdoorAirUnit) is intended to model systems such as zone make-up air units and dedicated outside air systems.  These components are “zone equipment� meaning that they do not require an air loop but serve a zone directly.  The system is comprised of a supply fan (in either draw through or blow through configuration), an optional exhaust fan, and a variety of components such as heating coils, cooling coils, heat recovery, etc.  The object of the zone outdoor air unit is to bring in additional ventilation air into a zone.  These might be used for high ventilation spaces such as kitchens or laboratories where another system is primarily responsible for space conditioning while the zone outside air unit is primarily responsible for fresh air delivery to the zone.  Most of the information necessary to configure a zone outdoor air unit is contained in the EnergyPlus Input/Output Reference.  A diagram of the zone outdoor air unit is shown below.  As this system is relatively simple and does not contain any unique operating algorithm or equations, the discussion here is limited to the application of the user defined controls and how it relates to the operation of the device.
-
-![](media/image7466.png)
-
-Figure 332. Zone Outdoor Air Unit Schematic
-
-### Controls
-
-Three input parameters control the operation of the zone outdoor air unit.  The unit control type has two options: neutral or temperature.  If the temperature control type is selected, the user must also provide a high and low air temperature control schedule.  The algorithm for controlling the zone outdoor air unit is dependent on these parameters which are used as described below.
-
-***Neutral Control.***  If the user selects neutral control, the intent is to provide additional outside air to the zone without imposing any additional thermal load on the zone or any other systems serving the zone.  In other words, the unit will attempt to provide air to the zone at the zone mean air temperature.  Mathematically, this means:
-
-<div>$${T_{out}} = {T_{MAT}}$$</div>
-
-where:
-
-      T<sub>out</sub> = the outlet temperature of the zone outdoor air unit
-
-      T<sub>MAT</sub> = the mean air temperature of the zone being served by the unit
-
-It should be noted that to avoid excessive iteration that the zone mean air temperature that is used is the mean air temperature from the previous time step.  This will result in a slight lagging that may introduce a slight thermal load, but this should be minimal.
-
-***Temperature Control***.  If the user selects temperature control, the intent is to limit the outlet temperature of the unit for either heating or cooling or both or perhaps to provide unconditioned air to the space.  The algorithm used to determine the outlet temperature of the unit is as follows.  When the outdoor air temperature is at or below the low air temperature control schedule value, the outlet temperature is set to the low air temperature control schedule value and any heating equipment included in the unit description and available will attempt to provide enough heating to produce an outlet temperature equal to the low temperature schedule value.  When the outdoor air temperature is at or above the high air temperature control schedule value, the outlet temperature of the unit is set to the high air temperature control schedule value and any cooling equipment included in the unit description and available will attempt to provide enough cooling to produce an outlet air temperature equal to the high temperature schedule value.  When the outdoor air temperature is between the high and low temperature values, the unit will not provide any conditioning of outdoor air and will simply deliver it to the zone.  Mathematically, this can be summarized as:
-
-<div>$${T_{out}} = \left\{ {\begin{array}{*{20}{c}}{{T_{high}}\;if\;{T_{oa}} \ge {T_{high}}}\\ {{T_{oa}}\;if\;{T_{low}} &lt; {T_{oa}} &lt; {T_{high}}}\\ {{T_{low}}\;if\;{T_{oa}} \le {T_{low}}}\end{array}} \right.$$</div>
-
-where:
-
-      T<sub>out</sub> = the outlet temperature of the zone outdoor air unit
-
-      T<sub>oa</sub> = the outside air temperature
-
-      T<sub>high</sub> = the high control air temperature schedule value
-
-      T<sub>low</sub> = the low control air temperature schedule value
-
-If the user wishes to provide “unconditioned� air all of the time, the high and low control temperature values can be set very high and very low, respectively, to always force the unit to provide unconditioned air.  The same effect can also be realized by not specifying any conditioning components (such as coils) in the unit.  The user can also limit the device to cooling only by specifying a low control temperature schedule with extremely low values.  Conversely, the user can limit the device to heating only by specifying a high control temperature schedule with extremely high values.  The user can also limit the equipment specified as part of the device to either cooling or heating components to get similar effects.  In essence, the temperature control provides a variety of options in a single control type through the use of the high and low control temperature schedules.
-
-### Zone Exhaust Fan
-
-The zone exhaust fan (Fan:ZoneExhaust) is a simple model to account for the fan electric energy use and impact on central air handlers from bathroom and hood exhaust.  Because the fan only extracts air from the zone, it doesn’t directly impact the zone itself.
-
-The fan flow rate is either constant or variable depending on if the user input a flow fraction modifier schedule.   The value entered for maximum volume flow rate is converted to a design mass flow rate using standard (altitude-adjusted) density and used as the design flow rate.  If a flow fraction schedule is used, then its values, <span>\({f_{Fract}}\)</span>, are multiplied by the design flow rate to obtain the current mass flow.
-
-<div>$${\dot m_{Des}} = {\dot V_{Max}}{\rho_{air,std}}$$</div>
-
-<div>$$\dot m = {f_{Fract}}{\dot m_{Des}}$$</div>
-
-The exhaust fan model is similar to, but simpler than, the models used for air system fans.  The electric power calculation is simplified and uses a constant overall efficiency.  All of the fan power is added to the air stream.
-
-<div>$${\dot Q_{fan}} = \frac{{\dot m{\rm{}}\Delta P}}{{{e_{tot}}{\rho_{air}}}}$$</div>
-
-<div>$${h_{out}} = {h_{in}} + \frac{{{{\dot Q}_{fan}}}}{{\dot m}}$$</div>
-
-<div>$${w_{out}} = {w_{in}}$$</div>
-
-<div>$${T_{out}} = PsyTdbFnHW\left( {{h_{out}},{w_{out}}} \right)$$</div>
-
-The controls for determining if the the exhaust fan will operate can be based on a number of factors including: an on/off availability schedule, interaction with system availability managers, minimum zone air temperature control limits and a variable flow fraction schedule.  When the fan is coupled to the system availability managers then it will operate if either the local availability schedule or the system availability manager’s indicate that the fan should run.  When the fan is not coupled to the system availability manager, then it only uses the local availability schedule and ignores availability managers.  If using the flow fraction schedule and the resulting flow is zero, then fan will not run.  If using the minimum zone temperature limit schedule then the fan will only run if the fan inlet temperature is warmer than the limit.
-
-The exhaust fan’s interaction with the air system depends on the value, <span>\({f_{Bal}}\)</span>, of the schedule for the fraction of the exhaust that is balanced.  The model tracks the exhaust flows in two ways, balanced and unbalanced. Balanced exhaust air flow is considered to have been made up from simple airflow from infiltration, ventilation or zone mixing.  Unbalanced exhaust air flow is considered to not be balanced by simple air flows and needs to be balanced by the air system operation.  Both of these types of flow are summed at the zone and whole air system level.   In a zone, the return air node flow rate is reduced from what it would be with no exhaust by the portion of the zone’s exhaust flow that is unbalanced.  In an air handler with an outdoor air system, the outdoor air flow rate may be increased so as to be sufficient to provide all the unbalanced exhaust air for all the zones on the air handler (when possible).
-
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-On-Site Generation, Power Conversion, and Storage
-=================================================
-
-This section discusses on-site generation, electric storage, and power conversion models related to serving the facility with electric power.  EnergyPlus is usually predicting the electric energy consumed in a building and its HVAC equipment over time.  If this electric power all comes directly from the grid and the building has no power conversion devices (such as a transformer, inverter, battery, generators, solar panels etc.) then only some basic accounting is needed and none of the additional models described here are really needed.  The device models in this section are for when the electric power service system supplying the facility has some added equipment that is considered part of the building being modeled.   The purpose of electric power service modeling in EnergyPlus is to account for the energy performance of such equipment at each timestep of the building and HVAC simulation.  The building and HVAC simulation provides a current prediction of the electric load required by the facility and the electric power service simulation uses that information.   This is simplified power system model with the only goal being to account for power losses (in Watts) and energy consumed (in Joules) by key devices in the balance of system including:
-
- * Transformers, a building may have transformers and they are not 100% efficient. A facility may own its own transformer and have high voltage utility grid connection. An on-site generation system might have an isolation transformer.  The EnergyPlus model meters electric losses as a function of the power going through each transformer.
- * Fuel-fired generators, a building may have generators that consume one type of energy resource (natural gas, diesel, etc.) and generate electricity.  These generators need supervisory control to determine when and how hard to run the engine.  The generators may be used for cogeneration and include connections to a hot water plant in the HVAC models.  The generator models determine the efficiency as fuels are converted to electric power and heat. 
- * Renewable generators, a building may have wind turbines or solar photovoltaic panels.  The generator models determine the efficiency as wind and sun are converted to electricity.
- * Inverters, the direct current generated by solar photovoltaic or discharged from storage may need to be converted from DC to AC by an inverter.  The EnergyPlus models meter electric losses as a function of the power going through each inverter.
- * Storage, a building may have on-site electric storage and it is not 100% efficient.  Storage can be used to adjust utility demand profile or store on-site renewables.
-
-There is no explicit modeling of voltage and current between devices, just basic power and energy exchanges.  There is no modeling of power loss in conductors and distribution panels throughout the building.  There is no modeling of short term power draws as for a motor start -- power levels are modeled as single-valued averages for the entire system timestep ( 1 minute or longer).
-
-Whole-Facility Electric Service
------------------------------------------
-
-Whenever an EnergyPlus model includes anything that consumes electricity the program will do some basic modeling of what can be thought of as the main panel where utility grid connects to the building and HVAC loads.  The following output variables and meters are created and filled to report on the overall, whole-facility power flows at the main panel.  
-
-<span>$ {P_{purch}}  $</span>    Facility Total Purchased Electric Power [W]
-<span>$ {Q_{purch}}  $</span>    Facility Total Purchased Electric Energy [J]
-<span>$ {P_{net,purch}}  $</span>    Facility Net Purchased Electric Power [W]
-<span>$ {Q_{net,purch}}  $</span>    Facility Net Purchased Electric Energy [J]
-<span>$ {P_{surp}}  $</span>    Facility Total Surplus Electric Power [W]
-<span>$ {Q_{surp}}  $</span>    Facility Total Surplus Electric Energy [J]
-<span>$ {P_{bldg,dmd}}  $</span>    Facility Total Building Electric Demand Power [W]
-<span>$ {P_{HVAC,dmd}}  $</span>    Facility Total HVAC Electric Demand Power [W]
-<span>$ {P_{dmd}}  $</span>    Facility Total Electric Demand Power [W]
-<span>$ {P_{prod}}  $</span>    Facility Total Produced Electric Power [W]
-<span>$ {Q_{prod}}  $</span>   Facility Total Produced Electric Energy [J]
-
-The models for electric power service use the meter reporting system inside EnergyPlus to obtain data from all the other models in EnergyPlus for the electric power demand (and maybe power production).  The ElectricPowerServiceManager uses a query routine called "GetInstantMeterValue" which returns the sum for all the metered equipment for the specified meter.  Values for <span>$ {P_{bldg,dmd}}  $</span> and <span>$ {P_{HVAC,dmd}}  $</span> are both filled from the "Electricity:Facility" meter.  <span>$ {P_{bldg,dmd}}  $</span> is filled by passing an argument that triggers to return the "Building" electric load, which is at the zone timestep, while <span>$ {P_{HVAC,dmd}}  $</span> is filled by passing an argument that returns the "HVAC" electric load, which is at the system timestep.  The modeling is based on average power levels for the duration of the timestep. The return values are converted from energy in Joules to power in Watts by dividing by the number of seconds in the zone timestep for building loads and by the system timestep for the HVAC loads.  Then the total facility power demand is the sum of the building loads and the HVAC loads. 
-
-<div>$$ {P_{dmd}} =  {P_{bldg,dmd}} + {P_{HVAC,dmd}} $$</div>
-
-When the electric power service device models described below are being used, they also make use of the meter reporting system using the components of the ElectricityProduced:Facility ( ResourceType=ElectricityProduced) meter to determine aggregate on-site electricity production rate, <span>$ {P_{prod}}  $</span>.  This value rolls up all the power generated and consumed by the on-site generators, storage, and power conversion equipment.  
-
-<span>$ {P_{prod,cogen}}  $</span> is the power from fuel-fired generators, from meter Cogeneration:ElectricityProduced.
-<span>$ {P_{prod,pv}}  $</span> is the power from solar photovoltaics, from meter Photovoltaic:ElectricityProduced.
-<span>$ {P_{prod,wind}}  $</span> is the power from wind generators, from meter WindTurbine:ElectricityProduced.
-<span>$ {P_{prod,storage}}  $</span> is the power from electric storage, from meter ElectricStorage:ElectricityProduced, with storage charging negative and storage discharging positive.
-<span>$ {P_{prod,conversion}}  $</span> is the power loss by converting between different voltages or AC and DC, from meter PowerConversion:ElectricityProduced which are metered as negative values that decrease the amount of electricity produced.
-
-<div>$$  {P_{prod}}= {P_{prod,cogen}} + {P_{prod,pv}} + {P_{prod,wind}} + {P_{prod,storage}} + {P_{prod,conversion}}  $$</div>
-
-Then the net purchased electricity, which can be either positive or negative (for export), is calculated using,
-
-<div>$$  {P_{net,purch}} = {P_{dmd}} - {P_{prod}}  $$</div>
-
-Only the positive portion of the net purchased power is the purchased power.
-
-<div>$$  {P_{purch}} = { max ( {P_{net,purch}}, 0.0 ) }  $$</div>
-
-The surplus electric power is exported out to the grid and is only positive. 
-
-<div>$$  {P_{surp}} =  { max ( ({P_{prod}} - {P_{dmd}}) , 0.0 ) }  $$</div>
-
-The energy versions of the power variables are calculated by multiplying the power level by the number of seconds in the system timestep. 
-
-
-Electric Load Center Distribution Manager
------------------------------------------
-
-### Overview
-
-The electric load center distribution manager (object name: ElectricLoadCenter:Distribution) is used organize power conversion devices and provides supervisory control over generators and storage.   Electric load centers can be thought of as subpanels connected to the facility's main electric panel.  Except for two applications for transformers that are located between the main panel and the utility grid connection, all other devices are associated with a specific load center.  The load center connects the “load� to the generators and “supply� power to the main panel serving the rest of the building.  A load center can have any number of generators but only one storage, (DC to AC) inverter, (AC to DC) converter or (isolation) transformer.  There are two separate operation schemes, one for generators and one for storage.  The generator operation scheme controls the on-site generators connected to a particular load center.  The storage operation scheme controls charging and discharging of electrical storage.  The generator operation is managed before the storage operation.  The internal meters used by EnergyPlus for reporting do all of the tracking. For more details on the individual inputs required see the Input Output Reference document.
-
-The electric load center manager sums all of the building and system electric loads and provides operating schemes for the generators. The electric load center objects are operated in the order they are defined in the input data file (IDF), and generators are dispatched sequentially in the order they are specified within the list referenced by each load center object. The electricity produced from photovoltaic arrays and wind turbines is handled somewhat separately and is always run rather than being dispatched by supervisory control.  What is not provided by the on-site generation equipment, and electric storage units, is met by (purchasing) off-site electricity. It is possible to prescribe a set of ElectricLoadCenter:Distribution objects with inconsistent or conflicting operating schemes, so users need to be careful.
-
-
-### Generator Operation Schemes
-
-The available generator operating schemes are “Baseload�, “DemandLimit�, “TrackElectrical,� “TrackSchedule,� “TrackMeter,� “FollowThermal� and “FollowThermalLimitElectrical.�  These operating schemes affect how loads are dispatched to the generators, in effect telling the generators whether or not to run and requesting power levels.
-
-The Baseload scheme operates the generators at their rated (requested) electric power output when the generator is scheduled ON (ref. ElectricLoadCenter:Generators in the Input Output Reference). The Baseload scheme requests all generators scheduled ON (available) to operate, even if the amount of electric power generated exceeds the total facility electric power demand.
-
-The DemandLimit scheme limits the amount of purchased electricity from the utility to the amount specified in the input. The Demand Limit scheme tries to have the generators meet all of the demand above the purchased electric limit defined by the user.
-
-The TrackElectrical scheme tries to have the generators meet all of the electrical demand for the building.
-
-The TrackMeter scheme tries to have the generators meet all the electrical demand from a meter chosen by the user rather than the usual meter for the entire facility. The meter can be a custom meter so that generators are tied to only certain loads in the building.
-
-The TrackSchedule scheme tries to have the generators meet all of the electrical demand determined by a user-defined schedule.
-
-The FollowThermal and FollowThermalLimitElectrical schemes run the generators to meet thermal demand. The thermal demand is determined from the plant modeling and depends on the flow requested by other components on the demand side of the plant loop, the loop temperatures, and the loop temperature setpoint. The electric load center distribution manager converts the thermal load to an electrical load using a nominal ratio of the thermal to electrical power production for each generator. For these schemes, the generator needs to be connected to the supply side of a plant loop and serve components that use hot water on the demand side of the plant loop. The thermal load request is obtained from the plant data structure (structure location in code is PlantLoop%LoopSide%Branch%Comp%MyLoad).The distribution manager converts the thermal load, <span>$ {q_{thermal}}  $</span>, to an electrical load using:
-
-<div>$${q_{Elect}} = \frac{{{q_{thermal}}}}{{ThermElectRatio}}$$</div>
-
-where,
-
-<span>\(ThermElectRatio\)</span> is a nominal, constant, user-defined value for the ratio of thermal production to electrical production for a cogenerator. This ratio is used for supervisory control and dispatch of the electric power request to the generator; however, the cogenerator model may determine that actual performance varies from this nominal value at different times in the simulation when operating conditions differ from those used for the nominal ratio.
-
-For all generator operating schemes except Baseload, a total electric load reduction target (or thermal load converted to electrical equivalent) is established for the load center based on the specific operating scheme. The load center then requests that its generators operate, one-by-one in the order specified in the generator list, until the target is met or exceeded. Generators that are not scheduled as ‘available’ for the simulation time step are not called to operate. The requested power demand to be met by each generator is the **smaller of** the nominal ‘rated’ electric power output (as specified in the ElectricLoadCenter:Generators object) or the remaining total electric load reduction target for the load center. After each electric generator is requested to operate, the actual electric power delivered by the generator, which may be greater than or less than the requested amount due to inputs specified in the generator performance model (e.g., Generator:CombustionTurbine, Generator:MicroTurbine, etc.), is used to update the remaining total electric power target for the other generators associated with this load center.
-
-Most of the operating schemes will sequentially load the available electric load centers and generators. EnergyPlus can accept multiple “ElectricLoadCenter:Distribution� objects with different operating schemes. Because of this, there are two levels of reporting, one for the whole building and a second for each load center. The whole-building results are managed with the internal meters for the entire model. The individual load-center results are summed for those generators connected to a particular load center. The total electricity purchased is reported both in power and energy units. This value is positive when the amount of energy is purchased from the utility. This value can be negative when the total electricity produced is greater than the facility electrical needs. The excess will either be available for storage or to sell back to the electric utility company.
-
-The order of input objects (ElectricLoadCenter:Distribution) in the input file is significant and used to structure how generators are dispatched with the first load centers and generators managed before the later ones. Therefore, load centers listed earlier in the file effectively have a higher priority.
-
-###  Load Center Buss Types
-
-Electric load centers can have one of five different configurations. Load centers can get fairly complicated and include power conditioning and storage. Separate inverter models are used to condition DC power from photovoltaics into AC power for the building and utility. The other generators may have inverters inside the devices but these are already embedded in the generator models. The load center can also supervise electrical storage controls and depend on the buss configuration. The transformer is optional for all buss types but if included in the load center it can be used to model an isolation or voltage matching transformer acting on the load center.
-
-The most basic configuration is selected with the keyword “AlternatingCurrent� for the Electrical Buss Type, shown in the following diagram.
-
-
-![ACtopology](media/ACBussDiagram.png)
-
-Figure 333. Basic Alternating Current Schematic
-
-The *AlternatingCurrent* load centers have AC generators with no storage and behave in the following way. All electric demand not met by the sum of the electrical power produced by the available generators will be met by purchased electricity.  If a generator is needed in the simulation for a small load and the load is less than the generator’s minimum part load ratio, the generator will operate at the minimum part load ratio and the excess will either reduce demand or the excess energy will be exported back to the electric utility company. 
-
-A configuration with AC generators with on-site electrical storage is selected with the keyword “AlternatingCurrentWithStorage� and is shown in the following diagram. 
-
-
-![ACwithStorageTopology](media/ACStorageBussDiagram.png)
-
-Figure 334. AC Generators with On-site Electrical Storage Schematic
-
-The *AlternatingCurrentWithStorage* load centers attempt to augment the generator electricity production so that the power requests are met. Storage control logic is discussed below under Storage Operation Scheme.
-
-The basic configuration for photovoltaic generators is selected using the “DirectCurrentWithInverter� keyword and is shown in the following diagram.
-
-
-![DCwithInverterTopology](media/DCInverterBussDiagram.png)
-
-Figure 335. Direct Current With Inverter Photovoltaic Generators Schematic
-
-The *DirectCurrentWithInverter* load centers collect DC power from various generators, usually PV arrays, run the DC power through an inverter and produce AC power. The PV arrays produce DC power based on the availability of sunshine and do not respond to load requests made by the electric load center. 
-
-If the PV-based load center is equipped with DC electrical storage that is connected before the inverter, then the buss type should be “DirectCurrentWithInverterDCStorage� and is shown in the following diagram.
-
-
-![DCwithInverterDCStorageTopology](media/DCInverterWithDCStorageBussDiagram.png)
-
-Figure 336. PV based Load Center with DC Electrical Storage Schematic
-
-The *DirectCurrentWithInverterDCStorage* load centers charge or draw DC power to meet the requested electrical load depending on the storage operation scheme.
-
-If the PV-based load center is equipped with AC electrical storage that is connected after the inverter, then the buss type should be “DirectCurrentWithInverterACStorage� and is shown in the following diagram.
-
-
-![DCWithInverterACStorage](media/DCInverterWithACStorageBussDiagram.png)
-
-Figure 337. PV Based Load Center with AC Electrical Storage Schematic
-
-The *DirectCurrentWithInverterACStorage* load centers charge or draw AC power to meet the requested electrical load.  They can also draw power from the main panel into the load center to charge storage from grid-supplied electric power.
-
-### Electric Load Center Generators
-
-The electric load center generators (object name: ElectricLoadCenter:Generators) provide a set of scheduled electric generators for supervisory control over electric power generation. Here is where the user lists what generators and PVs are available at any given time. For more details on the individual inputs required see the EnergyPlus Input Output Reference.
-
-### Inverters
-
-EnergyPlus includes three models for converting Direct Current (DC) electric power into Alternating Current (AC) electric power. The DC power into the inverter, <span>$ {P_{DC,in}} $</span>, is converted to AC power out, <span>$ {P_{AC,out}}  $</span>, of the inverter using:
-
-<div>$$  {P_{AC,out}} = {P_{DC,in}} \cdot {\varepsilon_{inverter}}  $$</div>
-
-The inverter efficiency is determined using one of the three models. For the“Simple� inverter model, efficiency is constant and input by the user. For the “Look Up Table� model, the efficiency is calculated using linear interpolation. For the “Function of Power� model, the efficiency is calculating using a single-variable curve object. For both the Look Up Table and Function of Power models, the power production is normalized by <span>$ {P_{DC,in}} $</span>.
-
-The conversion power losses are calculated from the difference between <span>$ {P_{DC,in}} $</span> and <span>$ {P_{AC,out}} $</span> and are metered as negative values on PowerConversion:ElectricityProduced.  The thermal losses include the conversion power losses plus any ancillary power consumed during standby.  The ancillary electric power consumption occurs when the inverter is scheduled to be available but it is not conditioning any power flows at the time. 
-
-### Converter
-
-EnergyPlus includes a model for converting Alternating Current (AC) electric power into Direct Current (DC) electric power.  This device is used to charge DC electric storage devices with AC drawn from the main panel.  Although the physical device may be a two-way inverter, the modeling is separated so that the converter appears on its own in the modeling. The AC power into the converter, <span>$ {P_{AC,in}} $</span>, is converted to DC power out,<span>$ {P_{DC,out}} $</span>, of the converter using: 
-
-<div>$$ {P_{DC,out}} = {P_{AC,in}} \cdot {\varepsilon_{converter}}  $$</div>
-
-The converter efficiency is determined using one of two method.  For the "SimpleFixed" method the efficiency is constant and input by the user.  For the "FunctionOfPower" method the user defined performance curve or lookup table is evaluated using the normalized power into the converter.
-
-The conversion power losses are calculated from the difference between <span>$ {P_{AC,in}} $</span> and <span>$ {P_{DC,out}} $</span> and are metered as negative values on PowerConversion:ElectricityProduced.  The thermal losses include the conversion power losses plus any ancillary power consumed during standby.  The ancillary electric power consumption occurs when the converter is scheduled to be available but it is not conditioning any power flows at the time. 
-
-### Storage Operation Schemes
-
-The available storage operation schemes are "TrackFacilityElectricDemandStoreExcessOnSite", "TrackMeterDemandStoreExcessOnSite", "TrackChargeDischargeSchedules", and "FacilityDemandLeveling".  
-
-The following diagram shows the control volume and electrical power flows that are used to model all of the storage operation schemes.  Conservation of energy is used to formulate the calculations based on this control volume and the five terms shown in the diagram.  This control volume is inside a given load center. 
-
-![StorageOpSchemeCV](media/StorageOperationControlVolume.png)
-
-<span>$ {P_{gen}}  $</span>  This is the sum of electric power produced by the generators on the load center entering the control volume.  The generator operation is run before the storage operation so that this value is current at the time the storage operation control is evaluated 
-<span>$ {P_{feed}}  $</span>  This is the flow of electric power out of the control volume feeding toward the main panel.  This is power being supplied by the generators and storage and serving the building loads or perhaps being exported.  This power level might be reduced by power conversion losses before it reaches the main panel.  The method used to determine <span>$ {P_{feed}}  $</span> depends on the operation scheme.
-<span>$ {P_{draw}}  $</span>  This is the flow of electric power into the control volume drawing from the main panel.  This is power being drawn in order to charge storage as desired by the storage operation scheme.  This power level might be increased by power conversion losses once it is drawn from the main panel.  
-<span>$ {P_{charge}}  $</span>  This is the flow of electric power into the storage device from the control volume.  This is power being supplied by the generators and/or drawn from the main panel and then directed into storage to charge the device.
-<span>$ {P_{discharge}}  $</span>  This is the flow of electric power out of the storage device into the control volume.  This power is being pulled from storage and added to the power from generators to feed toward the main panel. 
-
-The **TrackFacilityElectricDemandStoreExcessOnSite** method tries to run the storage to follow the facility electric demand while storing any excess on-site power production that is above what is needed to run the facility.  This is mainly appropriate for island operation.  This is the intended legacy behavior before version 8.5.  This scheme does not draw from the main panel to charge, so we have <span>$ {P_{draw}} = 0.0  $</span>.  The value for <span>$ {P_{feed}}  $</span> is determined from the whole-facility total electric power demand.  (When there is more than one load center in the model, it is actually the portion of the total that remains after previous load centers have been simulated.)  This requested feed in rate is adjusted to be increased by any power conversion losses that may occur in an inverter or a transformer.  This adjusted feed in request is used for <span>$ {P_{feed}}  $</span>. 
-
-If <span>$ {P_{gen}} > {P_{feed}} $</span> ,  then we have charging, 
-
-<div>$$  {P_{charge}} = {P_{gen}} - {P_{feed}}  $$</div>
-<div>$$  {P_{discharge}} = 0.0   $$</div>
-
-If <span>$ {P_{gen}} < {P_{feed}} $</span> , then we have discharging
-
-<div>$$  {P_{discharge}} =  {P_{feed}} - {P_{gen}} $$</div>
-<div>$$  {P_{charge}} = 0.0  $$</div>
-
-The **TrackMeterDemandStoreExcessOnSite** method is very similar to the TrackFacilityElectricDemandStoreExcessOnSite method except that instead of using the whole-facility total electric demand, the value for <span>$ {P_{feed}}  $</span> is determined from a user-specified meter.  The same charge and discharge logic is used. 
-
-The **TrackChargeDischargeSchedules** method tries to run the storage to follow user-defined schedules and design power levels for charging and discharging.  The user inputs a design charge rate <span>$ {P_{charge,design}} $</span> , a charge modification schedule <span>$ {f_{sched,charge}} $</span>, a design discharge rate <span>$ {P_{discharge,design}} $</span>, and a discharge modification schedule <span>$ {f_{sched,discharge}} $</span>.  The scheduled power flows will be used to determine charging and discharging as long as other limits on rates or state of charge are not triggered.  The schedules should be arranged to only charge or only discharge at a given time.  
-
-If charging, we have  
-
-<div>$$  {P_{charge}} = {P_{charge,design}} * {f_{sched,charge}} $$</div>
-<div>$$  {P_{discharge}} = 0.0   $$</div>
-
-If <span>$ {P_{gen}} > {P_{charge}} $</span> ,  then we have excess to feed toward main panel,
-
-<div>$$  {P_{feed}} = {P_{gen}} - {P_{charge}} $$</div>
-<div>$$  {P_{draw}} = 0.0  $$</div>
-
-If <span>$ {P_{gen}} < {P_{charge}} $</span> , the we have a shortfall and we draw from main panel,
-
-<div>$$  {P_{draw}} = {P_{charge}} - {P_{gen}}  $$</div>
-<div>$$  {P_{feed}} = 0.0  $$</div>
-
-If discharging, we have 
-
-<div>$$  {P_{discharge}} = {P_{discharge,design}} * {f_{sched,discharge}} $$</div>
-<div>$$  {P_{charge}} = 0.0 $$</div>
-<div>$$  {P_{feed}} = {P_{discharge}} + {P_{gen}} $$</div>
-<div>$$  {P_{draw}} = 0.0  $$</div>
-
-The **FacilityDemandLeveling** method tries to run the storage to follow a user-defined schedule for the net purchased power, <span>$ {P_{net,purch}}  $</span>.  This is similar to demand limit operation but instead of just attempting to cap the facility demand, it will also manipulate storage to increase utility grid supply electric to meet the target for net purchased power.  The user inputs a design demand target for net purchase power rate, <span>$ {P_{net,purch,design}}  $</span> , and a demand level modification schedule <span>$ {f_{sched,dmd,target}} $</span>.  
-
-<div>$$  {P_{net,purch,target}} = {P_{net,purch,design}} *{f_{sched,dmd,target}}  $$</div>
-
-This target is compared to an adjusted feed in request, <span>$ {P_{feed, request}}  $</span>, from the (remaining, adjusted) whole-facility total electric power demand. 
-
-<div>$$  {P_{feed}} = {P_{feed,request}} - {P_{net,purch,target}}  $$</div>
-
-If <span>$ {P_{feed}} > 0.0 $</span>, then we have a situation where the facility needs more power that the target demand.  We therefore feed that power toward the main panel, but it is not necessarily the full power request that could be served.  Iff <span>$ {P_{gen}} < {P_{feed}} $</span> , then we still have some power supply to make up by discharging,
-
-<div>$$  {P_{discharge}} =  {P_{feed}} - {P_{gen}} $$</div>
-<div>$$  {P_{charge}} = 0.0  $$</div>
-
-Or if <span>$ {P_{gen}} > {P_{feed}} $</span> ,  then we have excess power we can use for charging.
-
-<div>$$  {P_{charge}} = {P_{gen}} - {P_{feed}}  $$</div>
-<div>$$  {P_{discharge}} = 0.0   $$</div>
-
-However, if <span>$ {P_{feed}} < 0.0 $</span>, then the facility needs less power than the target demand.  We therefore draw power from the main panel to increase power purchased to meet target demand level. 
-
-<div>$$ {P_{draw}} = { abs( {P_{feed}} )}   $$</div>
-<div>$$  {P_{feed}} = 0.0  $$</div>
-<div>$$  {P_{charge}} = {P_{draw}} + {P_{gen}}  $$</div>
-
-### Electrical Storage - Simple Energy Balance Model
-
-EnergyPlus includes two models for storing electrical energy: a simple model that is not intended to represent any specific type of storage technology and a battery model that represents the kinetic battery model originally developed by Manwell and McGowan which discussed in the next section.
-
-The simple model treats the battery as a black box, counting energy added and removed, with losses due to charge/discharge inefficiencies. The model is a reasonable starting point for simulation of Li-ion and other battery technologies without significant rate limitations. The simple model might be called constrained bucket with energy losses.  The bucket holds a quantity of Joules of electrical energy, referred to as the state of charge. There are losses and limits to storing and drawing power but otherwise the bucket just holds electricity. The user sets constraints on the rates of charging,<span>\({P_{stor - {\rm{charge - max}}}}\)</span>, and drawing, <span>\({P_{stor - {\rm{d}}raw{\rm{ - max}}}}\)</span>. The user defines efficiencies for charging,<span>\({\varepsilon_{{\rm{charge}}}}\)</span>, and drawing, <span>\({\varepsilon_{draw}}\)</span>. 
-
-The user defines an initial state of charge and a maximum state of charge. The storage operation scheme makes supervisory control decisions and determines a value for the charging power, <span>\({P_{stor - ch\arg e}}\)</span>, or the discharging power, <span>\({P_{stor - draw}}\)</span> and passes in control limits for the minimum and maximum state of charge fraction.  The maximum state of charge is the physical capacity of the storage device, however the storage control applies a separate layer of minimum and maximum state of charge used to model controller behavior designed to protect the battery from abuse. 
-
-The control requests are constrained by the device's physical limits for how fast it can be charged or discharged, <span>\({P_{stor - {\rm{charge - max}}}}\)</span> and <span>\({P_{stor - {\rm{d}}raw{\rm{ - max}}}}\)</span> are applied.
-
-If charging, the new state of charge, <span>\(Q_{stor}^{t + \Delta t}\)</span>, is determined using:
-
-<div>$$Q_{stor}^{t + \Delta t} = Q_{stor}^t + {P_{stor - ch\arg e}} \cdot {\varepsilon_{{\rm{charge}}}} \cdot \Delta t$$</div>
-
-If drawing, the new state of charge is:
-
-<div>$$Q_{stor}^{t + \Delta t} = Q_{stor}^t - \frac{{{P_{stor - draw}} \cdot \Delta t}}{{{\varepsilon_{draw}}}}$$</div>
-
-Where <span>\(\Delta t\)</span> is the length of the system time step in seconds.
-
-The storage device has an availability schedule. If it is not available then no power can be drawn or stored.  The state of charge minimum and maximum that are passed into the storage model are used to decide if the device can be further charged or discharged.  The separate control limits allow modeling battery preservation strategies where the full capacity of the storage device is not really used. 
-
-The gross electric power drawn and stored includes losses in the form of heat. These thermal losses are calculated from the user-specified efficiencies for charging and drawing and gross electric power stored and drawn. The thermal (heat) losses are included in a zone heat balance if the user specifies a thermal zone. A user-defined radiative split is used to divide thermal losses into radiation and convection portions. If no zone is specified, then the thermal losses are simply disregarded (e.g., rejected to outdoors and do not impact the zone air heat balance).
-
-### Electrical Storage – Kinetic Battery Model with Cycle Life Estimation
-
-The Kinetic Battery Model (KiBaM) (object: ElectricLoadCenter:Storage:Battery) was originally developed by Manwell and McGowan (1993) for use in time series performance models of hybrid energy systems. The model is called kinetic because it is based on a chemical kinetics process to simulate the battery charging and discharging behavior. The model, with different improvements and modifications, has been incorporated into the software Hybrid2 and HOMER as the electrical storage module of hybrid and distributed power systems. In 2005, KiBaM was implemented as a stand-alone application in support of the European Union Benchmarking research project (Bindner et al. 2005). The model is intended to represent technologies such as Pb-acid that encounter significant rate or kinetic limitations.
-
-The Kinetic Battery Model assumes that the battery charge is distributed over two tanks: an available-charge tank and a bound-charge tank. The tank for available charges can supply electrons directly to the load, whereas the tank for chemically bound charges can only supply electrons to the available-charge tank. At any time, the total charge <span>\(q\)</span> in the battery is the sum of the available charge (<span>\({q_1}\)</span>) and bound charge (<span>\({q_2}\)</span>). That is:
-
-<div>$$q = {q_1} + {q_2}$$</div>
-
-Based on the governing equations on the change of charge in both tanks (Manwell and McGowan 1993), the battery capacity can be related to a constant charge/discharge current (<span>\(I\)</span>) as the following equation:
-
-<div>$${q_{\max }}(I) = \frac{{{q_{\max }}k \cdot c \cdot t}}{{1 - {e^{ - kt}} + c(kt - 1 + {e^{ - kt}})}}$$</div>
-
-where,
-
-<span>\({q_{\max }}(I)\)</span>  : Maximum capacity (Ah) at charge or discharge current I
-
-<span>\({q_{\max }}\)</span>       : Maximum capacity (Ah) at infinitesimal current
-
-<span>\(t\)</span>            : Charge or discharge time (hr), defined by <span>\(t = \frac{{{q_{\max }}(I)}}{I}\)</span>
-
-<span>\(k\)</span>           : Constant coefficient (hr<sup>-1</sup>)
-
-<span>\(c\)</span>           : Parameter indicating the ratio of available charge capacity to total capacity
-
-Assuming that a constant current is used in any time step for charging and discharging, the available charge (<span>\({q_1}\)</span>) and bound charge (<span>\({q_2}\)</span>) at any time step are given by:
-
-<div>$${q_1} = {q_{1,0}}{e^{ - k\Delta t}} + \frac{{({q_0}kc - I)(1 - {e^{ - k\Delta t}})}}{k} - \frac{{Ic(k\Delta t - 1 + {e^{ - k\Delta t}})}}{k}$$</div>
-
-<div>$${q_2} = {q_{2,0}}{e^{ - k\Delta t}} + {q_0}(1 - c)(1 - {e^{ - k\Delta t}}) - \frac{{I(1 - c)(k\Delta t - 1 + {e^{ - k\Delta t}})}}{k}$$</div>
-
-where,
-
-<span>\({q_{1,0}}\)</span>  :  Available charge at the beginning of time step (Ah)
-
-<span>\({q_{2,0}}\)</span> :  Bound charge at the beginning of time step (Ah)
-
-<span>\({q_0}\)</span>   :  Total charge at the beginning of time step (Ah), <span>\({q_0} = {q_{1,0}} + {q_{2,0}}\)</span>
-
-<span>\(\Delta t\)</span>   :  Length of time step (hr)
-
-KiBaM views the battery as a voltage source in series with an electric resistance (Figure 338). The internal resistance is assumed to be constant and the open circuit voltage varies with current and state of charge.
-
-![](media/image7528.svg.png)
-
-Figure 338. Electrical equivalent model for KiBaM
-
-The battery’s open circuit voltage is modeled in the same form for charging and discharging, but with different coefficients. The open circuit voltage in charging (<span>\({E_c}\)</span>) and in discharging (<span>\({E_d}\)</span>) can be respectively expressed as:
-
-<div>$${E_c} = {E_{0,d}} + {A_c}{X_c} + \frac{{{C_c}{X_c}}}{{{D_c} - {X_c}}}$$</div>
-
-<div>$${E_d} = {E_{0,c}} + {A_d}{X_d} + \frac{{{C_d}{X_d}}}{{{D_d} - {X_d}}}$$</div>
-
-where,
-
-<span>\({E_{0,c}}\)</span>               : Open circuit voltage for a fully charged battery
-
-<span>\({E_{0,d}}\)</span>               : Open circuit voltage for a fully discharged battery
-
-<span>\({A_c}\)</span>, <span>\({C_c}\)</span>, <span>\({D_c}\)</span>   : Constant parameters for charging
-
-<span>\({A_d}\)</span>, <span>\({C_d}\)</span>, <span>\({D_d}\)</span>  : Constant parameters for discharging
-
-<span>\({X_c}\)</span>, <span>\({X_d}\)</span>        : Normalized maximum capacity at a given charging or discharging current, calculated as:
-
-<div>$$
-  X = \left\{
-    \begin{array}{cl}
-      q_0 / q_{max}(I) & \; (charging) \\
-      (q_{max}-q_0)/q_{max}(I) & \; (discharging)
-    \end{array}
-  \right.
-$$</div>
-
-It needs to be noted that the performance curve (Curve:RectangularHyperbola2) used in the model input covers the 2<sup>nd</sup> and the 3<sup>rd</sup> item of the open circuit voltage equation. Due to the reformatting of performance curve, the voltage function regression coefficients can map to the curve coefficients as follows:
-
-<span>\({C_1} =  - C\)</span> ;<span>\({C_2} =  - D\)</span>;<span>\({C_3} = A\)</span>
-
-With open circuit voltage, the battery terminal voltage (V) can be calculated as:
-
-<div>$$V = E - IR$$</div>
-
-where, R is the battery internal resistance in Ohms; the current is positive for discharging and negative for charging.
-
-Given desired power in/out of the battery, the desired charge or discharge current can be calculated from the basic power equation: <span>\(P = VI\)</span>. In this calculation, iteration is needed to ensure the electric current has converged and the battery operation satisfies all specified technical constraints such as maximum discharge current and charge rate limit.
-
-KiBaM assumes that battery life is a primary function of charge/discharge cycles. One cycle is defined as the process of starting from a certain state of charge (SOC), the battery is discharged to a lower SOC and then recharged back to the starting SOC. It is regarded that the magnitude of cycle plays more important than the average of SOC during the cycle. This means that in terms of the impact on battery life, the cycle from 90% to 70% and then recharge back to 90% of SOC is equivalent to another cycle from 50% to 30% and then recharge back to 50% of SOC.  Battery life in terms of the number of cycles is predicted as a function of the cycle range measured by the fractional depth of discharge. A double exponential equation is used to capture the damage to batteries due to cycling. The equation takes the following form where the coefficients need to be derived from battery test data via curve fitting.
-
-<div>$${C_F} = {C_1} + {C_2}{e^{{C_3}R}} + {C_4}{e^{{C_5}R}}$$</div>
-
-where,
-
-<span>\({C_F}\)</span>    :    Cycles to failure
-
-<span>\({C_1}\)</span>-<span>\({C_5}\)</span>:    Regression coefficients
-
-R       :    Cycle range in terms of fractional SOC
-
-Following Hybrid2, the rainflow counting method (Downing and Socie 1982) is used to count battery cycles within a state of charge time series. Based on the number of cycles for each fractional SOC range, the battery damage is estimated as:
-
-<div>$$D = \sum\limits_{i = 1}^{} {\left( {{N_i}\frac{1}{{{C_{F,i}}}}} \right)} $$</div>
-
-where,
-
-D    : Fractional battery damage. For example, a value of 0.5 at the end of simulation means that half of the battery life is used up after the length of the simulation period.
-
-<span>\({C_{F,i}}\)</span>: Number of cycles to failure for the i-th cycle range
-
-<span>\({N_i}\)</span>  : Total number of cycles over the simulation with the i-th cycle range
-
-It needs to be noted that the temperature effects on battery performance and battery self-discharge are not supported in the current model.
-
-#### References
-
-Bindner H., Cronin T., Lundsager P., Manwell J.F., Abdulwahid U., and Baring-Gould I. 2005. Lifetime Modeling of Lead Acid Batteries. Riso National Laboratory, Roskilde, Denmark.
-
-Downing S. D. and Socie D. F. 1982.  Simple rainflow counting algorithms, International Journal of Fatigue, 1982.
-
-Manwell J. F. and McGowan J. G. 1993. A lead acid battery storage model for hybrid energy systems, Solar Energy 50(5): 399- 405.
-
-### Electric Load Center Transformers
-
-Transformers (object name: ElectricLoadCenter:Transformer) are an integral part of the electric distribution system. They have two broad applications closely related to building energy simulation. First, transformers are used to lower the voltage of electricity from utility primary circuits to customer secondary circuits, and in this case they are called distribution transformers. Second, transformers are used to output the surplus power from onsite generators to the electricity grid.
-
-Distribution transformers reduce the voltage on utility distribution lines (34.5 kV or less) to a lower secondary voltage (600 V or less) suitable for customer equipment. Distribution transformers are usually categorized according to the medium used for cooling and insulation (liquid or air), the voltage class that they serve (low or medium), and the number of phases (single phase or three phase).
-
-Liquid-immersed transformers rely on oil or other fire resistant liquid around the coils for cooling. In contrast, dry type transformers rely only on the natural convection of air for insulation and cooling. Medium-voltage transformers step from utility line voltage down to a lower secondary voltage, depending on the application. The secondary voltage from a medium-voltage transformer is usually at 277 V for single phase and 480 V for three phase. This secondary voltage can be directly used as 480 V three-phase power for large motors or as 277 V single-phase power for some fluorescent lighting. However, for most industrial and commercial facilities, low-voltage transformers are needed to reduce the above voltages further to 208/120 V. Common 120 V loads are wall plugs and incandescent lighting.
-
-Most liquid-immersed transformers are owned by utilities and they are of the medium-voltage type. Virtually all dry type transformers are owned by commercial and industrial customers (Barnes et al. 1996). Of the dry type transformers, those of the medium-voltage type are generally special-order items while those of the low-voltage type are commodity items. The efficiency requirement of distribution transformers is covered by the NEMA (National Electrical Manufactures Association) Standard TP 1. ASHRAE 90.1-2010 will cite the NEMA Standard TP 1 to stipulate the efficiency requirement for the low-voltage dry type distribution transformers.
-
-There are two main types of energy losses in transformers: no load loss and load loss. The no load loss comes primarily from the switching of the magnetic fields in the core material. Hence, it is also called the core loss. The no load (core) loss is roughly constant and exists continuously in the core material as long as the transformer is energized. The load loss comes from the electrical resistance in the windings when there is a load on the transformer. Hence, the load loss is also called the winding loss. The load (winding) loss is proportional to the load squared with a small temperature correction.
-
-Given the no load loss (NL) and the load loss (LL) at rated load and conditions, the total energy losses in a transformer at time t is calculated as:
-
-<div>$$TL(t) = NL + LL(t) = NL + LL*P{(t)^2}*{f_T}(t)$$</div>
-
-where,
-
-<span>\(TL(t)\)</span>        Total energy loss at time t (W)
-
-<span>\(LL(t)\)</span>        Load loss at time t (W)
-
-<span>\(P(t)\)</span>          Per unit load at time t
-
-<span>\({f_T}(t)\)</span>         Temperature correction factor for the load loss at time t
-
-
-
-The per unit load at time t is calculated as:
-
-<div>$$P(t) = \frac{{Load(t)}}{{{S_B}}}$$</div>
-
-where,
-
-<span>\(Load(t)\)</span>Transformer load at time t (W)
-
-<span>\({S_B}\)</span> Transformer nameplate rating (VA)
-
-The temperature correction factor at time t is calculated as (NEMA 2002):
-
-<div>$${f_T}(t) = {L_{dc}}*\frac{{R(t)}}{{{R_{ref}}}} + {L_{eddy}}*\frac{{{R_{ref}}}}{{R(t)}}$$</div>
-
-where,
-
-<span>\({L_{dc}}\)</span>            Per unit load loss due to electrical resistance
-
-<span>\({L_{eddy}}\)</span>          Per unit load loss due to eddy currents
-
-<span>\(R(t)\)</span>          Winding electrical resistance at time t
-
-<span>\({R_{ref}}\)</span>           Winding electrical resistance at the full load reference conditions
-
-The ratio of winding electrical resistance is calculated as:
-
-<div>$$\frac{{R(t)}}{{{R_{ref}}}} = \frac{{F + {T_{winding}}(t) + {T_{amb}}(t)}}{{F + {T_{winding,ref}} + {T_{amb,ref}}}}$$</div>
-
-where,
-
-<span>\(F\)</span>  Thermal coefficient of resistance for the winding material (=225 for aluminum and 234.5 for copper)
-
-<span>\({T_{winding,ref}}\)</span>Winding temperature rise at the full load reference conditions (°C)
-
-<span>\({T_{winding}}(t)\)</span>Winding temperature rise at time t (°C)
-
-<span>\({T_{amb,ref}}\)</span>       Ambient temperature at the reference condition (=20 °C)
-
-<span>\({T_{amb}}(t)\)</span>      Ambient temperature at time t (°C)
-
-The Ambient temperature <span>\({T_{amb}}(t)\)</span>is equal to the zone temperature if a thermal zone is specified in the input; otherwise, it is assumed equal to 20 °C. The winding temperature rise at time t is calculated as (Barnes et al. 1997):
-
-<div>$${T_{winding}}(t) = P{(t)^{1.6}}*{T_{winding.ref}}$$</div>
-
-Based on the derived total energy losses in a transformer, the transformer efficiency at time t can be calculated according to the following equation:
-
-<div>$$\eta (t) = \frac{{Load(t)}}{{Load(t) + NL + LL(t)}}$$</div>
-
-The above procedure describes how to calculate the total transformer energy losses based on the no load loss and load loss at rated conditions. The transformer model also supports the case when the nominal transformer efficiency is given. In this case, the user needs to provide the nameplate efficiency and the corresponding per unit load, the maximum efficiency and the corresponding per unit load, and the reference conductor temperature at which the nameplate efficiency is measured. Given these information, both no load loss and load loss at rated conditions can be derived as below.
-
-The nameplate efficiency can be expressed as:
-
-<div>$${\eta_{np}} = \frac{{{S_B}*{P_{np}}}}{{{S_B}*{P_{np}} + NL + LL*P_{np}^2*{f_{T,np}}}}$$</div>
-
-where,
-
-<span>\({\eta_{np}}\)</span>            Nameplate efficiency
-
-<span>\({S_B}\)</span> Nameplate rating (VA)
-
-<span>\({P_{np}}\)</span>            Per unit load at which the nameplate efficiency is measured
-
-<span>\({f_{T,np}}\)</span>          Applied temperature correction factor for the nameplate efficiency
-
-Maximum efficiency generally occurs when the load loss is equal to the no-load loss. Because the no-load loss does not vary with the load on the transformer, the following relationship can be established:
-
-<div>$$NL = L{L_{\max ,\eta }} = LL*P_{\max ,\eta }^2*{f_{T,\max  - \eta }}$$</div>
-
-where,
-
-<span>\({P_{\max ,\eta }}\)</span>         Per unit load at which the maximum efficiency is obtained
-
-<span>\({f_{T,\max  - \eta }}\)</span>     Applied temperature correction factor for the maximum efficiency
-
-Transformers typically have close per unit loads for the nameplate efficiency and the maximum efficiency. Therefore, it is reasonable to assume that the applied temperature correction factors are equal at those two efficiencies. This implies that:
-
-<div>$$\frac{{L{L_{np}}}}{{L{L_{\max ,\eta }}}} = \frac{{LL*{P_{np}}^2*{f_{T,np}}}}{{LL*{P_{\max ,\eta }}^2*{f_{T,\max  - \eta }}}} = {\left( {\frac{{{P_{np}}}}{{{P_{\max ,\eta }}}}} \right)^2}$$</div>
-
-Rearranging Equation and combining it with Equation leads to:
-
-<div>$$L{L_{np}} = L{L_{\max ,\eta }}*{\left( {\frac{{{P_{np}}}}{{{P_{\max ,\eta }}}}} \right)^2} = NL*{\left( {\frac{{{P_{np}}}}{{{P_{\max ,\eta }}}}} \right)^2}$$</div>
-
-Combining Equations and , we can obtain the no load loss as:
-
-<div>$$NL = \frac{{{S_B}*{P_{np}}*(1 - {\eta_{np}})}}{{{\eta_{np}}*\left[ {1 + {{\left( {\frac{{{P_{ref}}}}{{P{}_{\max ,\eta }}}} \right)}^2}} \right]}}$$</div>
-
-Substitute NL into Equation , we can calculate the load loss at rated conditions as:
-
-<div>$$LL = \frac{{NL}}{{{f_{T,\max  - \eta }}*P_{\max ,\eta }^2}} = \frac{{NL}}{{{f_{T,np}}*P_{\max ,\eta }^2}}$$</div>
-
-Since both no load and load losses at rated conditions are known, the total energy losses in a transformer at time t can then be calculated according to Equation
-
-#### References:
-
-Barnes, PR., JW. Van Dyke, BW. McConnell, and S. Das. 1996. Determination Analysis of Energy Conservation Standards for Distribution Transformer, ORNL-6847. Oak Ridge National Laboratory, Oak Ridge, TN.
-
-Barnes, PR., S. Das, BW. McConnell, and JW. Van Dyke. 1997. Supplement to the “Determination Analysis� (ORNL-6847) and Analysis of the NEMA Efficiency Standard for Distribution Transformer, ORNL-6925. Oak Ridge National Laboratory, Oak Ridge, TN.
-
-NEMA. 2002. NEMA Standards Publication TP 1-2002: Guide for Determining Energy Efficiency for Distribution Transformers. National Electrical Manufactures Association, Rosslyn, VA.
-
-Photovoltaic Arrays
--------------------
-
-The Photovoltaics.f90 module includes three different models referred to as “Simple�, “Equivalent One-Diode� and “Sandia� and the choice will determine the mathematical models (and input data) used to determine the energy produced by solar/electric conversion panels. The EnergyPlus photovoltaic array models are called one at a time at the HVAC system timestep along with other electrical generation components such as gas turbines and diesel engines.
-
-All of the photovoltaic models share the same models for predicting incident solar radiation that are also used for the solar thermal calculations and are described in the section Climate, Sky and Solar/Shading Calculations.
-
-Note that some of the terminology used to discussed photovoltaics overlaps with terminology used to discuss Fortran programs. The word *module* may refer to a PV panel or to a fortran90 programming entity. *Model* may refer to a manufacturers production model for a specific type of PV module or to a mathematical model used for engineering analysis. *Array* may refer to a collection of PV modules wired together or to a mathematical variable with multiple elements.
-
-The PV modules are assumed to always run when the total incident solar is greater than 0.3 Watts. If the incident solar is less than 0.3, then the modules produce no power.
-
-PV arrays are managed by an electric load center. The load center is a “load� with respect to generating equipment but is a “supply center� for the rest of the building. PV arrays need to be connected to ElectricLoadCenter:Distribution objects that have a DC buss type.
-
-### Simple Model
-
-The Generator:PV:Simple object describes about the simplest model for predicting photovoltaic energy production. In this model the user specifies the efficiency with which surfaces convert incident solar radiation to electricity. (In the other models this efficiency is determined as part of the model.)  The full geometric model for solar radiation is used, including sky models, shading, and reflections, to determine the incident solar resource. The model accepts arbitrary conversion efficiencies and does not require actual production units be tested to obtain empirical performance coefficients. (The Energy+.idd sets the range of conversion efficiencies to be on [0..1], but the user could alter the Energy+.idd to extend this range if desired.)
-
-#### Mathematical Description
-
-Table 89. Nomenclature for Simple Photovoltaic model
-
-<table class="table table-striped">
-<tr>
-<th>Mathematical variable</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>P</td>
-<td>Electrical power produced by photovoltaics [W]</td>
-</tr>
-<tr>
-<td>A<sub>surf</sub></td>
-<td>Net area of surface  [m<sup>2</sup>]</td>
-</tr>
-<tr>
-<td>f<sub>activ</sub></td>
-<td>Fraction of surface area with active solar cells [ ]</td>
-</tr>
-<tr>
-<td>G<sub>T</sub></td>
-<td>Total solar radiation incident on PV array [W/m<sup>2</sup>]</td>
-</tr>
-<tr>
-<td>h<sub>cell</sub></td>
-<td>Module conversion efficiency [ ]</td>
-</tr>
-<tr>
-<td>h<sub>invert</sub></td>
-<td>DC to AC conversion efficiency  [ ]</td>
-</tr>
-
-</table>
-
-
-
-The usable electrical power produced by a PV surface are calculated using:
-
-<div>$$P = {A_{surf}} \cdot {f_{activ}} \cdot {G_T} \cdot {\eta_{cell}} \cdot {\eta_{invert}}$$</div>
-
-On the right hand side of this equation, only G<sub>T</sub> is calculated by EnergyPlus and the rest are user inputs. Power levels are assumed constant over the timestep to arrive at energy production.
-
-There are two modes that can be selected by the user that govern how the PV system is coupled to the building surfaces. If the integration mode is selected as ‘DECOUPLED’ then no adjustments are made to account for energy extracted in the form of electricity. If the integration mode is selected as ‘INTEGRATED’ then the energy extracted in the form of electricity is removed from surface heat transfer calculations using a sink term. This sink term is lagged from the previous timestep.
-
-### Equivalent One-Diode Model
-
-This model predicts the electrical performance of a photovoltaic (PV) array. This model is also known as the “TRNSYS PV� model.
-
-Mathematically speaking, the EnergyPlus PV module employs equations for an empirical equivalent circuit model to predict the current-voltage characteristics of a single module. This circuit consists of a DC current source, diode, and either one or two resistors. The strength of the current source is dependent on solar radiation and the IV characteristics of the diode are temperature-dependent. The results for a single module equivalent circuit are extrapolated to predict the performance of a multi-module array.
-
-The module employs a “four-parameter� equivalent circuit to model crystalline (both mono and poly) PV modules developed at the University of Wisconsin – Madison [2]. The values of these parameters cannot normally be obtained directly from manufacturers’ catalogs. However, the PV module will automatically calculate them from commonly available data. The PV module also includes an optional incidence angle modifier correlation to calculate how the reflectance of the PV module surface varies with the angle of incidence of solar radiation.
-
-The module determines PV current as a function of load voltage. Other OUTPUTS include current and voltage at the maximum power point along the IV curve, open-circuit voltage, short circuit current as well as electrical load met and unmet.
-
-Table 90. General Nomenclature for the PV model
-
-<table class="table table-striped">
-<tr>
-<th>Mathematical variable</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>b</td>
-<td>Slope of PV array [degrees]</td>
-</tr>
-<tr>
-<td>g</td>
-<td>Empirical PV curve-fitting parameter</td>
-</tr>
-<tr>
-<td>e<sub>g</sub></td>
-<td>Semiconductor bandgap [eV]</td>
-</tr>
-<tr>
-<td>h<sub>c</sub></td>
-<td>Module conversion efficiency</td>
-</tr>
-<tr>
-<td>m<sub>Isc</sub></td>
-<td>Temperature coefficient of short-circuit current [A/K]</td>
-</tr>
-<tr>
-<td>m<sub>Voc</sub></td>
-<td>Temperature coefficient of open-circuit voltage [V/K]</td>
-</tr>
-<tr>
-<td>q</td>
-<td>Angle of incidence for solar radiation [degrees]</td>
-</tr>
-<tr>
-<td>ta</td>
-<td>Module transmittance-absorptance product</td>
-</tr>
-<tr>
-<td>ta<sub>normal</sub></td>
-<td>Module transmittance-absorptance product at normal incidence</td>
-</tr>
-<tr>
-<td>G<sub>T</sub></td>
-<td>Total radiation incident on PV array</td>
-</tr>
-<tr>
-<td>G<sub>T,beam</sub></td>
-<td>Beam component of incident radiation</td>
-</tr>
-<tr>
-<td>G<sub>T,diff</sub></td>
-<td>Diffuse component of incident radiation</td>
-</tr>
-<tr>
-<td>G<sub>T,gnd</sub></td>
-<td>Ground-reflected component of incident radiation</td>
-</tr>
-<tr>
-<td>G<sub>T,NOCT</sub></td>
-<td>Incident radiation at NOCT conditions</td>
-</tr>
-<tr>
-<td>G<sub>T,ref</sub></td>
-<td>Incident radiation at reference conditions</td>
-</tr>
-<tr>
-<td>I</td>
-<td>Current</td>
-</tr>
-<tr>
-<td>I<sub>L</sub></td>
-<td>Module photocurrent</td>
-</tr>
-<tr>
-<td>I<sub>L,ref</sub></td>
-<td>Module photocurrent at reference conditions</td>
-</tr>
-<tr>
-<td>I<sub>o</sub></td>
-<td>Diode reverse saturation current</td>
-</tr>
-<tr>
-<td>I<sub>o,ref</sub></td>
-<td>Diode reverse saturation current at reference conditions</td>
-</tr>
-<tr>
-<td>I<sub>sc</sub></td>
-<td>Short-circuit current</td>
-</tr>
-<tr>
-<td>I<sub>sc,ref</sub></td>
-<td>Short-circuit current at reference conditions</td>
-</tr>
-<tr>
-<td>I<sub>mp</sub></td>
-<td>Current at maximum power point along IV curve</td>
-</tr>
-<tr>
-<td>I<sub>mp,ref</sub></td>
-<td>Current at maximum power point along IV curve, reference conditions</td>
-</tr>
-<tr>
-<td>IAM</td>
-<td>Dimensionless incidence angle modifier</td>
-</tr>
-<tr>
-<td>K</td>
-<td>Boltzmann constant [J/K]</td>
-</tr>
-<tr>
-<td>NP</td>
-<td>Number of modules in parallel in array</td>
-</tr>
-<tr>
-<td>NS</td>
-<td>Number of modules in series in array</td>
-</tr>
-<tr>
-<td>N<sub>s</sub></td>
-<td>Number of individual cells in module</td>
-</tr>
-<tr>
-<td>P</td>
-<td>PV output power</td>
-</tr>
-<tr>
-<td>P<sub>max</sub></td>
-<td>PV output power at maximum power point along IV curve</td>
-</tr>
-<tr>
-<td>Q</td>
-<td>Electron charge constant</td>
-</tr>
-<tr>
-<td>R<sub>s</sub></td>
-<td>Module series resistance [W]</td>
-</tr>
-<tr>
-<td>R<sub>sh</sub></td>
-<td>Module shunt resistance [W]</td>
-</tr>
-<tr>
-<td>T­<sub>c</sub></td>
-<td>Module temperature [K]</td>
-</tr>
-<tr>
-<td>T<sub>c,NOCT</sub></td>
-<td>Module temperature at NOCT conditions [K]</td>
-</tr>
-<tr>
-<td>T<sub>c,ref</sub></td>
-<td>Module temperature at reference conditions [K]</td>
-</tr>
-<tr>
-<td>U<sub>L</sub></td>
-<td>Array thermal loss coefficient</td>
-</tr>
-<tr>
-<td>V</td>
-<td>Voltage</td>
-</tr>
-<tr>
-<td>V<sub>mp</sub></td>
-<td>Voltage at maximum power point along IV curve</td>
-</tr>
-<tr>
-<td>V<sub>mp,ref</sub></td>
-<td>Voltage at maximum power point along IV curve, reference conditions</td>
-</tr>
-<tr>
-<td>V­<sub>oc</sub></td>
-<td>Open-circuit voltage</td>
-</tr>
-<tr>
-<td>V<sub>oc,ref</sub></td>
-<td>Open-circuit voltage at reference conditions [V]</td>
-</tr>
-
-</table>
-
-#### Mathematical Description
-
-##### PV Section 1: Four-Parameter Model
-
-The four-parameter equivalent circuit model was developed largely by Townsend [1989] and is detailed by Duffie and Beckman [1991]. The model was first incorporated into a component for the TRNSYS simulation package by Eckstein [1990]. The EnergyPlus module employs the Eckstein model for crystalline PV modules, using it whenever the short-circuit IV slope is set to zero or a positive value as modified by Ulleberg [2000]. The four parameter model assumes that the slope of the IV curve is zero at the short-circuit condition:
-
-<div>$${\left( {\frac{{dI}}{{dV}}} \right)_{v = 0}} = 0$$</div>
-
-This is a reasonable approximation for crystalline modules. The “four parameters� in the model are *I<sub>L,ref</sub>*, *I<sub>o,ref,</sub>* g, and *R<sub>s</sub>.* These are empirical values that cannot be determined directly through physical measurement. The EnergyPlus model calculates these values from manufactures’ catalog data as discussed in the following section on calculating these parameters
-
-The four-parameter equivalent circuit is shown in the following figure:
-
-![](media/image7592.svg.png)
-
-Figure 339. Equivalent circuit in the four parameter model
-
-*V* is the load voltage and *I* is the current flowing through the load and PV.
-
-**Determining Performance under Operating Conditions**
-
-The IV characteristics of a PV change with both insolation and temperature. The PV model employs these environmental conditions along with the four module constants *I<sub>L,ref</sub>*, *I<sub>o,ref,</sub>* g, and *R<sub>s</sub>* to generate an IV curve at each timestep.
-
-The current-voltage equation of circuit shown in the previous figure is as follows:
-
-<div>$$I = {I_L} - {I_o}\left[ {\exp \left( {\frac{q}{{\gamma k{T_c}}}\left( {V + I{R_s}} \right)} \right) - 1} \right]$$</div>
-
-*R<sub>s</sub>* and g are constants. The photocurrent *I<sub>L</sub>* depends linearly on incident radiation:
-
-<div>$${I_L} = {I_{L,ref}}\frac{{{G_T}}}{{{G_{T,ref}}}}$$</div>
-
-The reference insolation *G<sub>ref</sub>*  is nearly always defined as 1000 W/m<sup>2</sup>. The diode reverse saturation current *I<sub>o</sub>* is a temperature dependent quantity:
-
-<div>$$\frac{{{I_o}}}{{{I_{o,ref}}}} = {\left( {\frac{{{T_c}}}{{{T_{c,ref}}}}} \right)^3}$$</div>
-
-Equation gives the current implicitly as a function of voltage. Once *I<sub>o</sub>* and *I<sub>L</sub>* are found from Eqs. 3 and 4, Newton’s method is employed to calculate the PV current. In addition, an iterative search routine finds the current (*I<sub>mp</sub>*)  and voltage (*V<sub>mp</sub>*)  at the point of maximum power along the IV curve.
-
-**Calculating *I<sub>L,ref</sub>*, *I<sub>o,ref,</sub>*** **g, and *R<sub>s</sub>***
-
-The Idf specification for the PV model include several values which must be read from manufacturers’ PV module catalogs. The manufactures’ values are used to determine the equivalent circuit characteristics *I<sub>L,ref</sub>*, *I<sub>o,ref,</sub>* g, and *R<sub>s</sub>*. These characteristics define an equivalent circuit that is employed to find the PV performance at each timestep, as described previously. This section describes the algebra and calculation algorithms used to solve for the four equivalent circuit characteristics.
-
-Three of these values, *I<sub>L,ref</sub>*, *I<sub>o,ref,</sub>* g, may be isolated algebraically. The first step is to substitute the current and voltage into Eq. at the open-circuit, short circuit, and maximum power conditions:
-
-<div>$$0 = {I_{L,ref}} - {I_{o,ref}}\left[ {\exp \left( {\frac{q}{{\gamma k{T_{c,ref}}}}{V_{oc,ref}}} \right) - 1} \right] - \frac{{{V_{oc,ref}}}}{{{R_{sh}}}}$$</div>
-
-<div>$${I_{sc,ref}} = {I_{L,ref}} - {I_{o,ref}}\left[ {\exp \left( {\frac{{q{I_{sc,ref}}{R_s}}}{{\gamma k{T_{c,ref}}}}} \right) - 1} \right] - \frac{{{I_{sc,ref}}{R_s}}}{{{R_{sh}}}}$$</div>
-
-<div>$${I_{mp,ref}} = {I_{L,ref}} - {I_{o,ref}}\left[ {\exp \left( {\frac{q}{{\gamma k{T_{c,ref}}}}\left( {{V_{mp,ref}} + {I_{mp,ref}}{R_s}} \right)} \right) - 1} \right] - \frac{{{V_{mp,ref}} + {I_{mp,ref}}{R_s}}}{{{R_{sh}}}}$$</div>
-
-In each case the “-1� term is may be dropped to simplify the algebra. This approximation has little influence on the right side of the equations since because the magnitude of *I<sub>o</sub>* is very small, generally on the order of 10<sup>-6</sup> A. Some rearrangement then yields the following three expressions which isolate *I<sub>L,ref</sub>*, *I<sub>o,ref,</sub>* g:
-
-<div>$${I_{L,ref}} \approx {I_{sc,ref}}$$</div>
-
-<div>$$\gamma  = \frac{{q\left( {{V_{mp,ref}} - {V_{oc,ref}} + I_{mp,ref}^{}{R_s}} \right)}}{{k{T_{c,ref}}\ln \left( {1 - \frac{{{I_{mp,ref}}}}{{{I_{sc,ref}}}}} \right)}}$$</div>
-
-<div>$${I_{o,ref}} = \frac{{{I_{sc,ref}}}}{{\exp \left( {\frac{{q{V_{oc,ref}}}}{{\gamma k{T_{c,ref}}}}} \right)}}$$</div>
-
-At this point an additional equation is needed in order to determine the last unknown parameter. Taking the analytical derivative of voltage with respect to temperature at the reference open-circuit condition derives the fourth equation. This analytical value is matched to the open-circuit temperature coefficient, a catalog specification:
-
-<div>$$\frac{{\partial {V_{oc}}}}{{\partial {T_c}}} = {\mu_{voc}} = \frac{{\gamma k}}{q}\left[ {\ln \left( {\frac{{{I_{sc,ref}}}}{{{I_{o,ref}}}}} \right) + \frac{{{T_c}\mu_{isc}^{}}}{{{I_{sc,ref}}}} - \left( {3 + \frac{{q\varepsilon }}{{Ak{T_{c,ref}}}}} \right)} \right]$$</div>
-
-where
-
-<div>$$A = \frac{\gamma }{{{N_s}}}$$</div>
-
-The “TRNSYS PV model� uses an iterative search routine in these four equations to calculate the equivalent circuit characteristics. The first step is to set upper and lower bounds for the series resistance parameter *R<sub>s</sub>*:  physical constraints require the *R<sub>s</sub>* value to lie between 0 and the value such that g = *N<sub>s</sub>*. The initial guess for *R<sub>s</sub>* is midway between these bounds. g and *I<sub>o,ref</sub>*  are found from Eq. and Eq. , while Eq. gives a trivial solution for *I<sub>L,ref</sub>*.  The model then employs Eq. to compare the analytical and catalog values for m<sub>voc</sub>. When all other variables are held constant, the analytical value for m<sub>voc</sub> increases monotonically with series resistance (Townsend 1989). If the analytical voltage coefficient is less than the catalog value, the lower bound for *R<sub>s</sub>* is reset to the present guess value. Likewise, the upper bound is set to the current value if the calculated m<sub>voc</sub> is too large. After resetting the upper or lower bound for *R<sub>s</sub>*, a new guess value is found by averaging the bounds. This procedure repeats until *R<sub>s</sub>* and g converge. Note that for *I<sub>L,ref</sub>*, *I<sub>o,ref,</sub>* g, and *R<sub>s</sub>* are assumed to be constant and are calculated only on the first call in the simulation. Alternatively, the user may enter a known series resistance by entering a **positive** value in the IDF. In this case the iterative routine described above is skipped and Eqs. , , and find *I<sub>L,ref</sub>*, *I<sub>o,ref,</sub>* and g directly from the given value of *R<sub>s</sub>*.
-
-##### PV Section 2 : Module Operating Temperature
-
-The PV model uses one of five methods for determining cell temperature data. The cell temperature of a PV module is important because the hotter the temperature of the panel, the lower its electrical output. The cell temperature calculation method is chosen by the user in the EnergyPlus IDF file through a parameter choice in the IDD entry called Integration and Cell Temperature Mode.
-
-If the value of this parameter is “**Decoupled NOCT Conditions**� then the cell temperature of the PV is modeled using the method from the Duffie and Beckman (1991) for estimating cell temperature. This is based upon the standard NOCT (Nominal Operating Cell Temperature) measurements to compute the module temperature Tc at each timestep. The NOCT temperature (Tc,NOCT) is the operating temperature of the module with a wind speed of 1 m/s, no electrical load, and a certain specified insolation and ambient temperature [Beckman and Duffie, 1991]. The values for insolation GT,NOCT  and ambient temperature *T<sub>a,NOCT</sub>* are usually 800 W/m<sup>2</sup> and 20º C. *h<sub>c</sub>* is the convesion efficiency of the module, which varies with ambient conditions. ta is a user-defined constant.
-
-The equation is:
-
-<div>$${T_c} = {T_a} + \frac{{\left( {1 - {\raise0.7ex\hbox{${{\eta_c}}$} \!\mathord{\left/ {\vphantom {{{\eta_c}} {\tau \alpha }}}\right.}\!\lower0.7ex\hbox{${\tau \alpha }$}}} \right)}}{{\left( {{\raise0.7ex\hbox{${{G_T}\tau \alpha }$} \!\mathord{\left/ {\vphantom {{{G_T}\tau \alpha } {{U_L}}}}\right.}\!\lower0.7ex\hbox{${{U_L}}$}}} \right)}}$$</div>
-
-If the user specifies the “**Decoupled Ulleberg Dynamic�** mode for calculating cell temperature, then a method developed by Ulleberg is used:
-
-<div>$${\left. {{T_{cell}}} \right|_t} = {T_{ambient}} + \left( {{{\left. {{T_{cell}}} \right|}_{t - 1}} - {T_{ambient}}} \right)*{e^{\frac{{ - UL}}{{Cap}}\Delta t}}$$</div>
-
-In other words, the cell temperature is a function of the privious cell temperature and the thermal capacity of the PV module material.
-
-If the user specifies “**Integrated Surface Outside Face�** for this parameter, then the temperature result from EnergyPlus’s modeling of surfaces is used for the cell temperature. Also the energy exported from the surface as electricity becomes a sink in the internal source modeling for the heat transfer surface.
-
-If the user specifies “**Integrated Transpired Collector�** for this parameter, then the temperature result for the unglazed transpired collector surfaces is used for the cell temperature. Also the energy exported from the collector surface as electricity is deprecated using a source term in the collector’s temperature modeling.
-
-If the user specifies “**Integrated Exterior Vented Cavity�** for this parameter, then the temperature result for the exterior cavity is used for the cell temperature. Also the energy exported from the baffle surface as electricity is deprecated using a source term in the baffle’s temperature modeling.
-
-##### PV Section 3 : Multi-Array Modules
-
-The electrical calculations discussed in the sections above deal only with a single module. The EnergyPlus PV component may be used to simulate arrays with any number of modules. The IDF defines the number of modules in series (NS) and modules in parallel (NP) for the entire array. The total number of modules in the array is the product of NS and NP. When simulating a single module only, both NS and NP are set to 1. The single-module values for all currents and voltages discussed in PV Section 1 are multiplied by NP or NS to find values for the entire array. This approach neglects module mismatch losses.
-
-With the above equations, and the assumption that the panels operate at the maximum power point, it is a direct calculation to determine DC power production. The performance of an array of identical modules is assumed to be linear with the number of modules in series and parallel. The inverter efficiency is applied linearly to derate the energy production. The inverter capacity forms a limit for power production from a PV generator. A ‘load’ is passed the PV array acting as a generator and various trivial calculations compare PV production to this load. If the PV array is associated with a surface that is associated with a zone, then if the zone has any multipliers associated with it, electricity production will be multiplied accordingly.
-
-#### References
-
-Duffie, John A. and William A. Beckman. 1991. *Solar Engineering of Thermal Processes*. New York: John Wiley & Sons, Inc..
-
-Eckstein, Jürgen Helmut. 1990. *Detailed Modeling of Photovoltaic Components*. M. S. Thesis – Solar Energy Laboratory, University of Wisconsin, Madison: 1990.
-
-Ulleberg, Øystein. *HYDROGEMS Component Library for TRNSYS 15 User Manual*, Institute for Energy Technology, Kjeller, Norway * *
-
-### Sandia Photovoltaic Performance Model
-
-The third model available in EnergyPlus for predicting the electricity generated by photovoltaics is referred to as the Sandia model. This model is based on work done at Sandia National Lab, Albuquerque, NM by David King -- with the help of many others. The model consists of a series of empirical relationships with coefficients that are derived from actual testing. Once the coefficients for a particular module are available, it is straightforward matter to use the model equations to calculate five select points on the current-voltage curve.
-
-The implementation in EnergyPlus is also based on work done by Greg Barker (2003) for the National Renewable Energy Lab who implemented the Sandia model in FORTRAN77 as a custom type (Type101) for the TRNSYS computer program.
-
-There are several climate and solar orientation inputs to the model that are managed elsewhere in EnergyPlus including: incident beam solar, incident diffuse solar, incidence angle of beam solar, solar zenith Angle, outdoor drybulb, wind speed, and elevation.
-
-#### Mathematical Description
-
-This section presents the mathematical description of the Sandia model from a draft report by King et, al. (2003). The core of the model predicts the performance of a single PV module. The following nomenclature and equations summarize the Sandia model.
-
-Table 91. Nomenclature for Sandia PV model
-
-<table class="table table-striped">
-<tr>
-<th>Mathematical variable</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>I<sub>sc</sub></td>
-<td>Short-circuit current (A)</td>
-</tr>
-<tr>
-<td>I<sub>mp</sub></td>
-<td>Current at the maximum-power point (A)</td>
-</tr>
-<tr>
-<td>I<sub>x</sub></td>
-<td>Current at module V = 0.5 V<sub>oc</sub>, defines 4th point on I-V curve</td>
-</tr>
-<tr>
-<td>I<sub>xx</sub></td>
-<td>Current at module V = 0.5 (V<sub>oc</sub> + V<sub>mp</sub>), defines a 5th point on the I-V curve</td>
-</tr>
-<tr>
-<td>V<sub>oc</sub></td>
-<td>Open-circuit voltage (V)</td>
-</tr>
-<tr>
-<td>V<sub>mp</sub></td>
-<td>Voltage at maximum-power point (V)</td>
-</tr>
-<tr>
-<td>P<sub>mp</sub></td>
-<td>Power at maximum-power point (W)</td>
-</tr>
-<tr>
-<td>fd</td>
-<td>Fraction of diffuse irradiance used by module</td>
-</tr>
-<tr>
-<td>N<sub>s</sub></td>
-<td>Number of cells in series in a module’s cell-string</td>
-</tr>
-<tr>
-<td>N<sub>p</sub></td>
-<td>Number of cell-strings in parallel in module</td>
-</tr>
-<tr>
-<td>k</td>
-<td>Boltzmann’s constant, 1.38066E-23 (J/k)</td>
-</tr>
-<tr>
-<td>q</td>
-<td>Elementary charge, 1.60218E-19 (coulomb)</td>
-</tr>
-<tr>
-<td>T<sub>c</sub></td>
-<td>Cell temperature inside module (°C)</td>
-</tr>
-<tr>
-<td>&sigma;(T<sub>c</sub>)</td>
-<td>‘Thermal voltage’ per cell at temperature T<sub>c</sub>, approximately 1 volt for a typical 26-cell crystalline silicon module</td>
-</tr>
-<tr>
-<td>E<sub>e</sub></td>
-<td>‘Effective’ solar irradiance</td>
-</tr>
-<tr>
-<td>E<sub>b</sub></td>
-<td>Beam solar irradiance</td>
-</tr>
-<tr>
-<td>E<sub>diff</sub></td>
-<td>Diffuse solar irradiance</td>
-</tr>
-<tr>
-<td>C<sub>0</sub> , C<sub>1</sub></td>
-<td>Empirical coefficients relating I<sub>mp</sub> to E<sub>e</sub> , C<sub>0</sub> + C<sub>1</sub>= 1 (both dimensionless)</td>
-</tr>
-<tr>
-<td>C<sub>2</sub> , C<sub>3</sub></td>
-<td>Empirical coefficients relating V<sub>mp</sub> to E<sub>e</sub>(C<sub>2</sub> dimensionless, C<sub>3</sub> is 1/V)</td>
-</tr>
-<tr>
-<td>C<sub>4</sub> , C<sub>5</sub></td>
-<td>Empirical coefficients relating I<sub>x</sub> to E<sub>e</sub>, C<sub>4</sub> + C<sub>5</sub> = 1 (both dimensionless)</td>
-</tr>
-<tr>
-<td>C<sub>6</sub> , C<sub>7</sub></td>
-<td>Empirical coefficients relating I<sub>xx</sub> to E<sub>e,</sub> C<sub>6</sub> + C<sub>7</sub> = 1 (both dimensionless)</td>
-</tr>
-<tr>
-<td>n</td>
-<td>Empirically determined ‘diode factor’ for individual cells</td>
-</tr>
-<tr>
-<td>AMa</td>
-<td>Absolute Air Mas</td>
-</tr>
-<tr>
-<td>AOI</td>
-<td>Solar angle-of-incidence (degrees) from normal</td>
-</tr>
-<tr>
-<td>f<sub>1</sub>(AM<sub>a</sub>)</td>
-<td>Empirical polynomial function used to relate short-circuit current to the solar spectrum via air mass</td>
-</tr>
-<tr>
-<td>f<sub>2</sub>(AOI)</td>
-<td>Empirical polynomial function used to relate short-circuit current to the solar angle-of-incidence</td>
-</tr>
-<tr>
-<td>a<sub>0</sub>, a<sub>1</sub>, a<sub>2</sub>, a<sub>3</sub>, a<sub>4</sub></td>
-<td>Empirical coefficients for f<sub>1</sub>(AM<sub>a</sub>) polynomial</td>
-</tr>
-<tr>
-<td>b<sub>0</sub>, b<sub>1</sub>, b<sub>2</sub>, b<sub>3</sub>, b<sub>4</sub>,b<sub>5</sub>,b<sub>6</sub></td>
-<td>Empirical coefficients for f<sub>1</sub>(AOI) polynomial</td>
-</tr>
-<tr>
-<td>T<sub>o</sub></td>
-<td>Reference cell temperature for rating, typically fixed at 25°C</td>
-</tr>
-<tr>
-<td>I<sub>sco</sub></td>
-<td>Short circuit current at reference conditions</td>
-</tr>
-<tr>
-<td>I<sub>mpo</sub></td>
-<td>Max power point current at reference conditions</td>
-</tr>
-<tr>
-<td>V<sub>mpo</sub></td>
-<td>Voltage at max power at reference conditions</td>
-</tr>
-<tr>
-<td>V<sub>oco</sub></td>
-<td>Open circuit voltage at reference conditions</td>
-</tr>
-<tr>
-<td>I<sub>xo</sub></td>
-<td>Current at V = 0.5 Voc and at reference conditions</td>
-</tr>
-<tr>
-<td>I<sub>xxo</sub></td>
-<td>Current at V = 0.5 (Vmp + Voc) and at reference conditions</td>
-</tr>
-<tr>
-<td>&alpha;<sub>Isc</sub></td>
-<td>Normalized temperature coefficient for I<sub>sc</sub> (1/°C)</td>
-</tr>
-<tr>
-<td>&alpha;<sub>Imp</sub></td>
-<td>Normalized temperature coefficient for I<sub>mp</sub> (1/°C)</td>
-</tr>
-<tr>
-<td>&beta;<sub>Voc</sub>(E<sub>e</sub>)</td>
-<td>Temperature coefficient for module open-circuit-voltage as function of E<sub>e</sub></td>
-</tr>
-<tr>
-<td>&beta;<sub>Voco</sub></td>
-<td>Temperature coefficient for module open-circuit-voltage at reference conditions</td>
-</tr>
-<tr>
-<td>m<sub>&beta;Voco</sub></td>
-<td>Coefficient for irradiance dependence of open-circuit-voltage-temperature coefficient, often zero (V/°C)</td>
-</tr>
-<tr>
-<td>&beta;<sub>Vmp</sub>(E<sub>e</sub>)</td>
-<td>Temperature coefficient for module maximum-power-voltage as a function of E<sub>e</sub></td>
-</tr>
-<tr>
-<td>&beta;<sub>Vmpo</sub></td>
-<td>Temperature coefficient for module maximum-power-voltage at reference conditions</td>
-</tr>
-<tr>
-<td>m<sub>&beta;Vmpo</sub></td>
-<td>Cofficient for irradiance dependence of maximum-power-voltage-temperature coefficient, often zero (V/°C)</td>
-</tr>
-<tr>
-<td>T<sub>m</sub></td>
-<td>PV module temperature at back suface (°C)</td>
-</tr>
-<tr>
-<td>T<sub>a</sub></td>
-<td>Ambient outdoor drybulb temperature (°C)</td>
-</tr>
-<tr>
-<td>E</td>
-<td>Solar irradiance incident on module surface (W/m<sup>2</sup>)</td>
-</tr>
-<tr>
-<td>WS</td>
-<td>Wind speed at standard 10-m height (m/s)</td>
-</tr>
-<tr>
-<td>a</td>
-<td>Empirical coefficient relating module temperature at low wind and high solar irradiance</td>
-</tr>
-<tr>
-<td>b</td>
-<td>Empirical coefficient relating module temperature decrease with increasing wind speed</td>
-</tr>
-<tr>
-<td>T<sub>c</sub></td>
-<td>Temperature of solar cell inside module (°C)</td>
-</tr>
-<tr>
-<td>E<sub>o</sub></td>
-<td>Reference solar irradiance (1000 W/m<sup>2</sup>)</td>
-</tr>
-<tr>
-<td>&delta;T</td>
-<td>Temperature difference between T<sub>c</sub> and T<sub>m</sub>at E<sub>o</sub>(°C),
-(This is d(Tc) in Sandia database)</td>
-</tr>
-
-</table>
-
-The current implementation in EnergyPlus focuses on determining performance at the maximum power-point but also calculates, and reports, four other points on the I-V curve so that the data are available for analyses outside of EnergyPlus. The equations below use the module performance parameters that are available in a database provided by Sandia National Laboratory (see www.sandia.gov/pv). The following equations form the basis of the Sandia model implemented in EnergyPlus:
-
-<div>$${I_{sc}} = {I_{sco}} \cdot {f_1}\left( {A{M_a}} \right) \cdot \left\{ {\left( {{E_b} \cdot {f_2}\left( {AOI} \right) + {f_d} \cdot {E_{diff}}} \right)/{E_o}} \right\} \cdot \left\{ {1 + {\alpha_{Isc}} \cdot \left( {{T_c} - {T_o}} \right)} \right\}$$</div>
-
-<div>$${I_{mp}} = {I_{mpo}} \cdot \left\{ {{C_o} \cdot {E_e} + {C_1} \cdot E_e^2} \right\} \cdot \left\{ {1 + {\alpha_{{\mathop{\rm Im}\nolimits} p}} \cdot ({T_c} - {T_o}} \right\}$$</div>
-
-<div>$${V_{oc}} = {V_{oco}} + {N_s} \cdot \delta ({T_c}) \cdot \ln ({E_e}) + {\beta_{Voc}}({E_e}) \cdot \left( {{T_c} - {T_o}} \right)$$</div>
-
-<div>$${V_{mp}} = {V_{mpo}} + {C_2} \cdot {N_s} \cdot \delta \left( {T_c^{}} \right) \cdot \ln \left( {{E_e}} \right) + {C_3} \cdot {N_3} \cdot {\left\{ {\delta \left( {T_c^{}} \right) \cdot \ln \left( {{E_e}} \right)} \right\}^2} + {\beta_{Vmp}}({E_e}) \cdot ({T_c} - {T_o})$$</div>
-
-<div>$${P_{mp}} = {I_{mp}} \cdot {V_{mp}}$$</div>
-
-<div>$${I_x} = {I_{xo}} \cdot \left\{ {{C_4} \cdot {E_e} + {C_5} \cdot E_e^2} \right\} \cdot \left\{ {1 + ({\alpha_{Isc}}) \cdot ({T_c} - {T_o})} \right\}$$</div>
-
-<div>$${I_{xx}} = {I_{xxo}} \cdot \left\{ {{C_6} \cdot {E_e} + {C_7} \cdot E_e^2} \right\} \cdot \left\{ {1 + ({\alpha_{{\mathop{\rm Im}\nolimits} p}}) \cdot ({T_c} - {T_{o)}}} \right\}$$</div>
-
-where,
-
-<div>$${E_e} = {I_{sc}}/\left[ {{I_{sco}} \cdot \left\{ {1 + {\alpha_{Isc}} \cdot ({T_c} - {T_o})} \right\}} \right]$$</div>
-
-<div>$$\delta ({T_c}) = n \cdot k \cdot ({T_c} + 273.15)/q$$</div>
-
-<div>$${f_1}\left( {A{M_a}} \right) = {a_0} + {a_1}A{M_a} + {a_2}{\left( {A{M_a}} \right)^2} + {a_3}{\left( {A{M_a}} \right)^3} + {a_4}{\left( {A{M_a}} \right)^4}$$</div>
-
-<div>$${f_2}\left( {AOI} \right) = {b_0} + {b_1} \cdot AOI + {b_2}{\left( {AOI} \right)^2} + {b_3}{\left( {AOI} \right)^3} + {b_4}{\left( {AOI} \right)^4} + {b_5}{\left( {AOI} \right)^5}$$</div>
-
-<div>$${\beta_{Voc}}({E_e}) = {\beta_{Voco}} + {m_{\beta Voc}} \cdot (1 - {E_e})$$</div>
-
-<div>$${\beta_{Vmp}}({E_e}) = {\beta_{Vmpo}} + {m_{\beta Vmp}} \cdot (1 - {E_e})$$</div>
-
-<div>$${T_m} = E \cdot \left\{ {{e^{a + b \cdot WS}}} \right\} + {T_a}$$</div>
-
-<div>$${T_c} = {T_m} + \frac{E}{{{E_o}}} \cdot \Delta T$$</div>
-
-With the above equations, and the assumption that the panels operate at the maximum power point, it is a direct calculation to determine DC power production. The performance of an array of identical modules is assumed to be linear with the number of modules in series and parallel. The inverter efficiency is applied linearly to derate the energy production. The inverter capacity forms a limit for power production from a PV generator. A ‘load’ is passed the PV array acting as a generator and various trivial calculations compare PV production to this load. If the PV array is associated with a surface that is associated with a zone, then if the zone has any multipliers associated with it, electricity production will be multiplied accordingly.
-
-The equation above for T<sub>m</sub> is used to predict back-of-module temperature when the mode ‘SANDIA RACK’ is selected. This would be appropriate for most rack mounted PV installations. If the user selects ‘EPLUS INTEGRATED’ then the back-of-module temperature is obtained from the outside face surface temperature calculated by the full complement of Heat Balance models using Conduction Transfer Functions that is native to EnergyPlus. And energy exported from the surface is accounted for using a source/sink term that is lagged from the previous timestep (pingpong).
-
-#### References
-
-King, D.L., Boyson, W.E., Kratochvil J.A. 2003. Photovoltaic Array Performance Model. Sandia National Laboratories, Albuquerque, NM 87185, November 2003  currently in DRAFT
-
-Barker, G. 2003 (unknown). Predicting Long-Term Performance of Photovoltaic Arrays. Submitted as deliverable for NREL subcontract LAX-1-30480-02. Currently in DRAFT
-
-Davis, M.W., Fanney, A.H., and Dougherty B.P. 2002. Measured Versus Predicted Performance of Building Integrated Photovoltaics. from the conference Solar 2002, Sunrise on the Reliable Energy Economy, June 15-19, 2002, Reno, NV. Available from NIST website.
-
-King, D.L. 1996. Photovoltaic Module and Array Performance Characterization Methods for All System Operating Conditions. Sandia National Laboratory. Albuquerque, NM 87185
-
-Generators
-----------
-
-### Internal Cumbustion Engine
-
-The engine-driven generator model was originally developed for the BLAST program and was subsequently adapted for use in EnergyPlus. The model uses the following set of equations all of which are quadratic fits to the PLR (Part Load Ratio) of the generator.  The coefficients must be derived from manufacturers data.
-
-<div>$$\frac{{electric\,\,energy\,\,output}}{{fuel\,\,energy\,\,input}} = \frac{{electric\,\,energy\,\,output}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {a_1} + {a_2}PLR + {a_3}PL{R^2}$$</div>
-
-The electrical load and engine generator nominal load capacity are used to compute the part load ratio.
-
-<div>$$PLR = \frac{{Electric energy output}}{{nominal generating capacity}}$$</div>
-
-The exhaust gas temp and flow rate are used if a stack heat exchanger is used to recover waste heat from the exhaust.  This temperature is the inlet temperature to the heat exchanger which is modeled in a UA-effectiveness form:
-
-<div>$$\frac{{Total\,Exhaust\,heat}}{{fuel\,energy\,input}} = \frac{{Total\,\,Exhaust\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {d_1} + {d_2}PLR + {d_3}PL{R^2}$$</div>
-
-<div>$$\frac{{Exhaust\,\,Gas\,\,Temp\,\,\left\{ K \right\}}}{{fuel\,\,energy\,\,input}} = \frac{{Exhaust\,\,Gas\,\,Temp\,\,\left\{ K \right\}}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {e_1} + {e_2}PLR + {e_3}PL{R^2}$$</div>
-
-The exhaust flow rate is then calculated as:
-
-<div>$${\dot m_{exhaust}} = \frac{{Total\,\,Exhaust\,\,heat}}{{C{p_{exhaust}} \cdot \left( {{T_{exhaust}} - {T_{reference}}} \right)}}$$</div>
-
-where T<sub>reference</sub> is the reference temperature for the fuel lower heating value, and is given as 25°C in manufacturer’s data, and
-
-<div>$${T_{stack}} = {T_{DesignMinExhaust}} + {\frac{{\left( {{T_{exhaust}} - {T_{DesignMinExhaust}}} \right)}}{{{\rm{exp}}\left( {\frac{{{\rm{UA}}}}{{{{{\rm{\dot m}}}_{{\rm{exhaust}}}}C{p_{exhaust}}}}} \right)}}^2}$$</div>
-
-Finally heat recovered from the lube oil and the water jacket are accounted for as follows:
-
-<div>$$\frac{{Recoverable\,\,jacket\,\,heat}}{{fuel\,\,energy\,\,input}} = \frac{{Recoverable\,\,jacket\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {b_1} + {b_2}PLR + {b_3}PL{R^2}$$</div>
-
-<div>$$\frac{{Recoverable\,\,lube\,\,oil\,\,heat}}{{fuel\,\,energy\,\,input}} = \frac{{Recoverable\,\,lube\,\,oil\,\,heat}}{{\left( {{{\dot m}_{fuel}}\left\{ {kg/s} \right\} \cdot LHV\left\{ {J/kg} \right\}} \right)}} = {c_1} + {c_2}PLR + {c_3}PL{R^2}$$</div>
-
-The manufacturer must supply the recoverable water jacket heat, lube oil heat and exhaust heat and associated fuel consumption for a range of load conditions.  This data is then fit to the PLR to obtain the fifteen a,b,c,d, and e coefficients.
-
-### Turbine Generator
-
-The combustion turbine generator model was originally developed for the BLAST program and was subsequently adapted for use in EnergyPlus. The model uses the following set of equations all of which are equation fits to the PLR (Part Load Ratio) of the generator and the entering air temperature. The coefficients must be derived from manufacturers data. For electric power generated in Watts, the fuel input rate is calculated in J/s.
-
-<div>$$\frac{{{\rm{fuel energy input rate}}}}{{{\rm{electric power output}}}} = \left[ {{a_1} + {a_2}PLR + {a_3}PL{R^2}} \right] * \left[ {{b_1} + {b_2}\Delta T + {b_3}\Delta {T^2}} \right]$$</div>
-
-The electrical load and engine generator nominal load capacity are used to compute the part load ratio.
-
-<div>$$PLR = \frac{{{\rm{Electric energy output}}}}{{{\rm{nominal generating capacity}}}}$$</div>
-
-The temperature difference shows the deviation of ambient air temperature from the manufacturers design air temperature.
-
-<div>$$\Delta T = {T_{air}} - {T_{design}}$$</div>
-
-A second curve fit calculates the exhaust temperature (C) by multiplying the exhaust temperature (C) for a particular part load by a correction factor based on the deviation from design temperature.
-
-<div>$${{\rm{T}}_{exhaust}} = \left[ {{c_1} + {c_2}PLR + {c_3}PL{R^2}} \right] * \left[ {{d_1} + {d_2}\Delta T + {d_3}\Delta {T^2}} \right]$$</div>
-
-The exhaust gas temp is used if a stack heat exchanger is used to recover waste heat from the exhaust.  This temperature is the inlet temperature to the heat exchanger which is modeled in a UA-effectiveness form:
-
-<div>$${T_{stack}} = {T_{DesignMinExhaust}} + {\frac{{\left( {{T_{exhaust}} - {T_{DesignMinExhaust}}} \right)}}{{{\rm{exp}}\left( {\frac{{{\rm{UA}}}}{{{{{\rm{\dot m}}}_{{\rm{exhaust}}}}C{p_{exhaust}}}}} \right)}}^2}$$</div>
-
-Where the design minimum exhaust temperature is a user input to the model and the exhaust mass flow rate and the UA are fit from manufacturers data as follows:
-
-<div>$$UA = {e_3}{{\rm{(Nominal Generating Capacity)}}^{e4}}$$</div>
-
-<div>$$\frac{{{\rm{exhaust gas flow rate}}}}{{{\rm{Nominal Generating Capacity}}}} = \left[ {{f_1} + {f_2}\Delta T + {f_3}\Delta {T^2}} \right]$$</div>
-
-Finally, heat recovered from the lube oil is accounted for as follows:
-
-<div>$$\frac{{{\rm{Recoverable lube oil heat}}}}{{{\rm{electric power generated}}}} = {g_1} + {g_2}PLR + {g_3}PL{R^2}$$</div>
-
-### Microturbine Generator
-
-Microturbine generators are small combustion turbines that produce electricity on a relatively small scale (e.g., 25kW to 500kW). This model uses nominal performance at reference conditions along with several modifier curves to determine electrical power output and fuel use at non-reference conditions. The modifier curve coefficients must be derived from manufacturers data. Standby and ancillary power can also be taken into account.
-
-Exhaust air energy recovery for heating water can be also be modeled. Similar to electrical power output, thermal power (heat recovery to water) output is calculated using nominal performance at reference conditions with modifier curves to account for variations at non-reference conditions. The ElectricLoadCenter:Generators and ElectricLoadCenter:Distribution objects are used to define the availability and control of the electric generators included in the simulation (ref. ElectricLoadCenter:Generators and ElectricLoadCenter:Distribution).
-
-For each simulation time step that the generator is being asked to operate (i.e., produce electrical power as determined by the ElectricLoadCenter), the full load electrical output of the generator is determined using the user-defined reference electrical power output along with a bi-quadratic modifier curve to account for differences in the combustion air inlet temperature and elevation for the current simulation time step compared to the reference temperature and elevation (i.e., the modifier curve should evaluate to 1.0 at the reference combustion air inlet temperature and reference elevation).
-
-<div>$${P_{Elec,Full\,Load\,}} = {P_{Elec,Ref}}\left( {PowerFTempElev} \right)$$</div>
-
-<div>$$PowerFTempElev = {a_1} + {a_2}\left( {{T_{a,i}}} \right) + {a_3}{\left( {{T_{a,i}}} \right)^2} + {a_4}\left( {Elev} \right) + {a_5}{\left( {Elev} \right)^2} + {a_6}\left( {{T_{a,i}}} \right)\left( {Elev} \right)$$</div>
-
-where:
-
-<span>\({P_{Elec,Full\,Load}}\)</span>= Full load electrical power output (W)
-
-<span>\({P_{Elec,Ref}}\)</span>= Reference Electrical Power Output, user input (W)
-
-<span>\(PowerFTempElev\)</span>= User-defined Electric Power Modifier Curve (function of temperature and elevation) evaluated at the current combustion air inlet temperature and elevation
-
-<span>\({T_{a,i}}\)</span>= Combustion air inlet temperature (°C)
-
-<span>\(Elev\)</span>= Elevation (m). This value obtained from the Location object or the weather file.
-
-The full load electrical power output of the generator is then checked against the minimum and maximum full load electrical power outputs specified by the user:
-
-<div>$${P_{Elec,Full\,Load}} = MIN\left( {{P_{Elec,Full\,Load}},{P_{FL\_Max}}} \right)$$</div>
-
-<div>$${P_{Elec,Full\,Load}} = MAX\left( {{P_{Elec,Full\,Load}},{P_{FL\_Min}}} \right)$$</div>
-
-<span>\({P_{FL\_Max}}\)</span> = Maximum Full Load Electrical Power Output, user input (W)
-
-<span>\({P_{FL\_Min}}\)</span> = Minimum Full Load Electrical Power Output, user input (W)
-
-The actual (operating) electrical power output from the generator is determined next based on the load requested by the Electric Load Center, the generator’s minimum and maximum part-load ratios, and the ancillary power.
-
-<div>$${P_{Elec,Operating}} = MAX\left( {0.0,\left( {Load + {P_{Ancillary}}} \right)} \right)$$</div>
-
-<div>$${P_{Elec,Operating}} = MIN\left( {{P_{Elec,Operating}},{P_{Elec,Full\,Load}}} \right)$$</div>
-
-```
- IF (P_elec_fullload > 0) THEN
-   PLR = P_elec_operating / P_elec_fullload
-   PLR = MIN( PLR, PLR_max )
-   PLR = MAX( PLR, PLR_min )
- ELSE
-   PLR = 0
- END IF
- P_elec_operating = P_elec_fullload * PLR
-```
-
-where:
-
-<span>\({P_{Elec,Operating}}\)</span>= Actual (operating) electrical power output (W)
-
-<span>\(Load\)</span>  = Electrical power output being requested by the Electric Load Center (W)
-
-<span>\({P_{Ancillary}}\)</span> = Ancillary Power, user input (W)
-
-<span>\(PLR\)</span>= Part-load ratio of the electric generator
-
-<span>\(PL{R_{\max }}\)</span>= Maximum part-load ratio of the electric generator (i.e., the maximum value for the independent variable [PLR] defined in the Curve:Quadratic or Curve:Cubic object for the Electrical Efficiency Modifier Curve [function of part-load ratio])
-
-<span>\(PL{R_{\min }}\)</span>= Minimum part-load ratio of the electric generator (i.e., the minimum value for the independent variable [PLR] defined in the Curve:Quadratic or Curve:Cubic object for the Electrical Efficiency Modifier Curve [function of part-load ratio])
-
-The generator’s electrical efficiency is then calculated based on the user-specified reference electrical efficiency (lower heating value [LHV] basis) and two electrical efficiency modifier curves.
-
-<div>$$ElecEfficiencyFTemp = {b_1} + {b_2}\left( {{T_{a,i}}} \right) + {b_3}{\left( {{T_{a,i}}} \right)^2}\,\,\,\,or\,\,\,\,\,{b_1} + {b_2}\left( {{T_{a,i}}} \right) + {b_3}{\left( {{T_{a,i}}} \right)^2} + {b_4}{\left( {{T_{a,i}}} \right)^3}$$</div>
-
-<div>$$ElecEfficiencyFPLR = {c_1} + {c_2}\left( {PLR} \right) + {c_3}{\left( {PLR} \right)^2}\,\,\,\,or\,\,\,\,\,{c_1} + {c_2}\left( {PLR} \right) + {c_3}{\left( {PLR} \right)^2} + {c_4}{\left( {PLR} \right)^3}$$</div>
-
-<div>$$ElecEf{f_{Operating}} = ElecEf{f_{Ref,LHV}}\left( {ElecEfficiencyFTemp} \right)\left( {ElecEfficiencyFPLR} \right)$$</div>
-
-where:
-
-<span>\(ElecEfficiencyFTemp\)</span> = User-defined Electrical Efficiency Modifier Curve (function of temperature) evaluated at the current combustion air inlet temperature
-
-<span>\(ElecEfficiencyFPLR\)</span> = User-defined Electrical Efficiency Modifier Curve (function of part-load ratio) evaluated at the current operating part-load ratio
-
-<span>\(ElecEf{f_{Operating}}\)</span> = Electrical efficiency at the current operating conditions
-
-<span>\(ElecEf{f_{Ref,LHV}}\)</span> = Reference Electrical Efficiency (LHV [lower heating value] Basis),     user input
-
-The fuel energy consumption rate (LHV Basis) is then calculated as follows:
-
-<div>$${\dot Q_{Fuel,LHV}} = {\raise0.7ex\hbox{${{P_{Elec,Operating}}}$} \!\mathord{\left/ {\vphantom {{{P_{Elec,Operating}}} {ElecEf{f_{Operating}}}}}\right.}\!\lower0.7ex\hbox{${ElecEf{f_{Operating}}}$}}$$</div>
-
-where:
-
-<span>\({\dot Q_{Fuel,LHV}}\)</span> = Fuel energy consumption rate, LHV basis (W)
-
-If *ElecEff<sub>Operating</sub>* is equal to zero, then *P<sub>Operating</sub>* and <span>\({\dot Q_{Fuel,LHV}}\)</span><sub> </sub>are set to zero. The fuel mass flow rate is then calculated.
-
-<div>$${\dot m_{fuel}} = {\raise0.7ex\hbox{${{{\dot Q}_{Fuel,LHV}}}$} \!\mathord{\left/ {\vphantom {{{{\dot Q}_{Fuel,LHV}}} {\left( {LHV*1000} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {LHV*1000} \right)}$}}$$</div>
-
-where:
-
-<span>\({\dot m_{fuel}}\)</span> = Mass flow rate of fuel being consumed by the generator (kg/s), report variable “Generator &lt;FuelType&gt; Mass Flow Rate [kg/s]�
-
-*LHV* = Fuel Lower Heating Value, user input (kJ/kg)
-
-The ancillary power is calculated next using the user-specified ancillary power and ancillary power modifier curve. The ancillary power modifier curve is a quadratic function with the generator’s fuel mass flow rate as the independent variable. If an ancillary power modifier curve is not specified in the input file, the modifier is assumed to be 1.0 and the ancillary power will be constant throughout the simulation.
-
-<div>$$AnciPowFMdotFuel = {d_1} + {d_2}\left( {{{\dot m}_{fuel}}} \right) + {d_3}{\left( {{{\dot m}_{fuel}}} \right)^2}$$</div>
-
-<div>$${P_{Ancillary,Operating}} = {P_{Ancillary}}\left( {AnciPowFMdotFuel} \right)$$</div>
-
-where:
-
-<span>\(AnciPowFMdotFuel\)</span> = User-defined Ancillary Power Modifier Curve (function of fuel input) evaluated at the actual fuel mass flow rate. This multiplier is assumed to be 1.0 if an ancillary power modifier curve name is not specified in the input.
-
-<span>\({P_{Ancillary}}\)</span> = Ancillary power, user input (W)
-
-<span>\({P_{Ancillary,Operating}}\)</span> = Ancillary electric power at the current fuel mass flow rate (W), report variable “Generator Ancillary Electric Power [W]�.
-
-If ancillary power is constant for the simulation (e.g., no modifier curve defined), then the calculations continue as described below. However, if an ancillary power modifier curve has been defined, then the calculations described above for *P<sub>ElecOperating</sub>*, *ElecEff<sub>Operating</sub>*, <span>\({\dot Q_{Fuel,LHV}}\)</span><sub> </sub>and *P<sub>Ancillary,Operating</sub>* are recalculated in sequence until the solution converges.
-
-The generator’s “net� electrical power output is calculated as the difference between the generator’s actual power output and the ancillary electric power as follows.
-
-<div>$${P_{Elec,Produced}} = {P_{Elec,Operating}} - {P_{Ancillary,Operating}}$$</div>
-
-where:
-
-<span>\({P_{Elec,Produced}}\)</span> = Generator net electric power output, report variable “Generator Produced Electric Power [W]�
-
-The fuel energy consumption rate (higher heating value basis) for the generator is then calculated as follows:
-
-<div>$${\dot Q_{Fuel,HHV}} = {\dot m_{fuel}}\left( {HHV} \right)\left( {1000} \right)$$</div>
-
-where:
-
-<span>\({\dot Q_{Fuel,HHV}}\)</span> = fuel energy consumption rate (W), report variables “Generator &lt;FuelType&gt; HHV Basis Rate [W]� and “Generator Fuel HHV Basis Rate [W]�
-
-<span>\(HHV\)</span>= Fuel Higher Heating Value, user input (kJ/kg)
-
-Standby electrical power may also be modeled to simulate controls or other parasitics used by the generator. The standby power is calculated only when the generator is not operating (i.e., *Load* from the Electric Load Center is zero). If the generator operates for a given timestep (i.e., *Load* &gt; 0.0), the standby power is set equal to 0.
-
-<div>$$\begin{array}{l}IF\,\,\left( {Load\, &lt;  = 0.0} \right)\,\,THEN\\\,\,\,\,\,{P_{Standby}} = {P_{Standby,user\,input}}\\ELSE\\\,\,\,\,\,{P_{Standby}} = 0.0\\END\,IF\end{array}$$</div>
-
-where:
-
-<span>\({P_{Standby,user\,input}}\)</span> = Standby power, user input (W)
-
-<span>\({P_{Standby}}\)</span> = Report variable “Generator Standby Electric Power� (W)
-
-Report variables for electric energy produced, electric efficiency (LHV basis), fuel consumption (HHV basis), standby electric consumption and ancillary electric consumption are calculated as follows:
-
-<div>$${E_{Elec,Produced}} = {P_{Elec,Produced}}\left( {TimeStepSys} \right)\left( {3600} \right)$$</div>
-
-<div>$$ElecEf{f_{Operating,LHV}} = {\raise0.7ex\hbox{${{P_{Elec,Produced}}}$} \!\mathord{\left/ {\vphantom {{{P_{Elec,Produced}}} {{{\dot Q}_{Fuel,LHV}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot Q}_{Fuel,LHV}}}$}}$$</div>
-
-<div>$${Q_{Fuel,HHV}} = {\dot Q_{Fuel,HHV}}\left( {TimeStepSys} \right)\left( {3600} \right)$$</div>
-
-<div>$${E_{Standby}} = {P_{Standby}}\left( {TimeStepSys} \right)\left( {3600} \right)$$</div>
-
-<div>$${E_{Ancillary}} = {P_{Ancillary,Operating}}\left( {TimeStepSys} \right)\left( {3600} \right)$$</div>
-
-where:
-
-<span>\({E_{Elec,Produced}}\)</span> = Report variable “Generator Produced Electric Energy [J]�
-
-<span>\(ElecEf{f_{Operating,LHV}}\)</span>= Report variable “Generator LHV Basis Electric Efficiency [-]�
-
-<span>\({Q_{Fuel,HHV}}\)</span> = Report variables “Generator &lt;FuelType&gt; HHV Basis Energy [J]� and “Generator Fuel HHV Basis Energy [J]�
-
-<span>\({E_{Standby}}\)</span> = Report variable “Generator Standby Electric Energy [J]�
-
-<span>\({E_{Ancillary}}\)</span> =  Report variable “Generator Ancillary Electric Energy [J]�
-
-*TimeStepSys*= HVAC system simulation time step (hr)
-
-In addition to calculating electric power production and fuel usage, the model is able to determine thermal power (heat recovery) output for heating water.  For this case, the water flow rate through the heat recovery heat exchanger is established first. If the Heat Recovery Water Flow Operating Mode (user input) is set to Plant Control, then the Reference Heat Recovery Water Flow Rate (user input) is requested whenever the generator operates (constant value), but the actual flow rate may be restricted by other plant components (e.g., pump). If the Heat Recovery Water Flow Operating Mode is set to Internal Control, then the requested water flow when the generator operates is determined by the Reference Heat Recovery Water Flow Rate and a flow rate modifier curve.
-
-<div>$$\begin{array}{l}IF\,\,\left( {Plant\,Control} \right)\,\,THEN\\\,\,\,\,\,{{\dot m}_w} = {{\dot V}_{w,Ref}}\left( {{\rho_w}} \right)\\ELSEIF\,\left( {Internal\,Control} \right)\,THEN\\\,\,\,\,\,\,HeatRecFlowFTempPow = {e_1} + {e_2}\left( {{T_{w,i}}} \right) + {e_3}{\left( {{T_{w,i}}} \right)^2} + {e_4}\left( {{P_{net}}} \right) + {e_5}{\left( {{P_{net}}} \right)^2} + {e_6}\left( {{T_{w,i}}} \right)\left( {{P_{net}}} \right)\\\,\,\,\,\,\,{{\dot m}_w} = {{\dot V}_{w,Ref}}\left( {{\rho_w}} \right)\left( {HeatRecFlowFTempPow} \right)\\END\,IF\end{array}$$</div>
-
- where:
-
-<span>\({\dot m_w}\)</span>= Report variable “Generator Heat Recovery Water Mass Flow Rate [kg/s]�
-
-<span>\({\dot V_{w,Ref}}\)</span>= Reference Heat Recovery Water Flow Rate (m<sup>3</sup>/s), user input
-
-<span>\({\rho_w}\)</span>= Density of water (kg/m<sup>3</sup>) at 5.05°C
-
-<span>\(HeatRecFlowFTempPow\)</span>= User-defined Heat Recovery Water Flow Rate Modifier Curve (function of temperature and power) evaluated at the current inlet water temperature and net electrical power output. This multiplier is assumed to be 1.0 if a water flow rate modifier curve name is not specified in the input.
-
-<span>\({T_{w,i}}\)</span>= Heat recovery inlet water temperature (°C), report variable “Generator Heat Recovery Inlet Temperature [C]�
-
-<span>\({P_{net}}\)</span>= Net electrical power output from the generator (W)
-
-The methodology for determining thermal power (heat recovery to water) is similar to that used for calculating electric power production. The generator’s steady-state thermal efficiency is calculated based on the user-specified reference thermal efficiency (LHV basis) and a thermal efficiency modifier curve.
-
-<div>$$ThermalEf{f_{SS\,}} = ThermalEf{f_{Ref,LHV}}\left( {ThermalEffFTempElev} \right)$$</div>
-
-<div>$$ThermalEffFTempElev = {f_1} + {f_2}\left( {{T_{a,i}}} \right) + {f_3}{\left( {{T_{a,i}}} \right)^2} + {f_4}\left( {Elev} \right) + {f_5}{\left( {Elev} \right)^2} + {f_6}\left( {{T_{a,i}}} \right)\left( {Elev} \right)$$</div>
-
-where:
-
-<span>\(ThermalEf{f_{SS}}\)</span>= Steady-state thermal efficiency at current conditions
-
-<span>\(ThermalEf{f_{Ref,LHV}}\)</span>= Reference Thermal Efficiency (LHV Basis), user input
-
-<span>\(ThermalEffFTempElev\)</span>= User-defined Thermal Efficiency Modifier Curve (function of temperature and elevation) evaluated at the current combustion air inlet temperature and elevation. This multiplier is assumed to be 1.0 if a thermal efficiency modifier curve name is not specified in the input.
-
-The steady-state thermal power produced (heat recovery rate) is then calculated:
-
-<div>$${P_{Thermal,SS}} = ThermalEf{f_{SS}}\left( {{{\dot Q}_{Fuel,LHV}}} \right)$$</div>
-
-The actual (operating) thermal power is then calculated using the steady-state thermal power and three modifier curves:
-
-<span>\({P_{Thermal,Operating}} = {P_{Thermal,SS}}\left( {HeatRecRateFPLR} \right)\left( {HeatRecRateFTemp} \right)\left( {HeatRecRateFFlow} \right)\)</span><span>\(\begin{array}{l}HeatRecRateFPLR = {g_1} + {g_2}\left( {PLR} \right) + {g_3}{\left( {PLR} \right)^2}\,\,\,\,\, - \,or\, - \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,{g_1} + {g_2}\left( {PLR} \right) + {g_3}{\left( {PLR} \right)^2} + {g_4}{\left( {PLR} \right)^3}\end{array}\)</span>
-
-<div>$$HeatRecRateFTemp = {h_1} + {h_2}\left( {{T_{w,i}}} \right) + {h_3}{\left( {{T_{w,i}}} \right)^2}$$</div>
-
-<div>$$HeatRecRateFFlow = {i_1} + {i_2}\left( {{{\dot m}_w}} \right) + {i_3}{\left( {{{\dot m}_w}} \right)^2}$$</div>
-
-where:
-
-<span>\({P_{Thermal,Operating}}\)</span>= Report variable “Generator Produced Thermal Rate [W]�
-
-<span>\(HeatRecRateFPLR\)</span>= User-defined Heat Recovery Rate Modifier Curve (function of part-load ratio) evaluated at the current operating part-load ratio. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
-
-<span>\(HeatRecRateFTemp\)</span>= User-defined Heat Recovery Rate Modifier Curve (function of inlet water temperature) evaluated at the current inlet water temperature. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
-
-<span>\(HeatRecRateFFlow\)</span>= User-defined Heat Recovery Rate Modifier Curve (function of water flow rate) evaluated at the current heat recovery water flow rate. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
-
-The heat recovery output water temperature is then calculated.
-
-<div>$${T_{w,o}} = {\rm{ }}{T_{w,i}}{\rm{ }} + {\rm{ }}{\raise0.7ex\hbox{${{P_{Thermal,Operating}}}$} \!\mathord{\left/ {\vphantom {{{P_{Thermal,Operating}}} {\left( {{{\dot m}_w}{\rm{ }}*{\rm{ }}C{p_w}} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {{{\dot m}_w}{\rm{ }}*{\rm{ }}C{p_w}} \right)}$}}$$</div>
-
-where:
-
-<span>\({T_{w,o}}\)</span>= Heat recovery outlet water temperature (°C), report variable “Generator Heat Recovery Outlet Temperature [C]�
-
-<span>\(C{p_w}\)</span>= Heat capacity of water (J/kg-K)
-
-If the calculated heat recovery outlet water temperature exceeds to Maximum Heat Recovery Water Temperature (user input), then the outlet water temperature is reset to the maximum temperature (user input) and the thermal power is recalculated.
-
-If combustion air inlet and outlet node names are specified in the input, along with exhaust air flow rate and exhaust air temperature information, then the model calculates the exhaust air conditions for each simulation time step. The exhaust air mass flow rate is first calculated based on the Reference Exhaust Air Mass Flow Rate, two modifier curves and an air density adjustment. Since fans are volumetric flow devices, the ratio of the air density at actual inlet air conditions to air density at reference inlet air conditions is used as an adjustment factor.
-
-<span>\({\dot m_{ExhAir}} = {\dot m_{ExhAir,Ref}}\left( {ExhFlowFTemp} \right)\left( {ExhFlowFPLR} \right)\left( {{\raise0.7ex\hbox{${{\rho_{a,i}}}$} \!\mathord{\left/ {\vphantom {{{\rho_{a,i}}} {{\rho_{a,Ref}}}}}\right.}\!\lower0.7ex\hbox{${{\rho_{a,Ref}}}$}}} \right)\)</span><span>\(\begin{array}{l}ExhFlowFTemp = {j_1} + {j_2}\left( {{T_{a,i}}} \right) + {j_3}{\left( {{T_{a,i}}} \right)^2}\,\,\,\,\, - \,or\, - \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,{j_1} + {j_2}\left( {{T_{a,i}}} \right) + {j_3}{\left( {{T_{a,i}}} \right)^2} + {j_4}{\left( {{T_{a,i}}} \right)^3}\end{array}\)</span>
-
-<div>$$\begin{array}{l}ExhFlowFPLR = {k_1} + {k_2}\left( {PLR} \right) + {k_3}{\left( {PLR} \right)^2}\,\,\,\,\, - \,or\, - \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,{k_1} + {k_2}\left( {PLR} \right) + {k_3}{\left( {PLR} \right)^2} + {k_4}{\left( {PLR} \right)^3}\end{array}$$</div>
-
-where:
-
-<span>\({\dot m_{ExhAir}}\)</span>= Exhaust air mass flow rate (kg/s)
-
-<span>\({\dot m_{ExhAir,Ref}}\)</span>= Reference Exhaust Air Mass Flow Rate (kg/s), user input
-
-<span>\(ExhFlowFTemp\)</span>= User-defined Exhaust Air Flow Rate Modifier Curve (function of temperature) evaluated at the current combustion air inlet temperature. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
-
-<span>\(ExhFlowFPLR\)</span> = User-defined Exhaust Air Flow Rate Rate Modifier Curve (function of part-load ratio) evaluated at the current operating part-load ratio. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
-
-<span>\({\rho_{a,i}}\)</span>= Density of the combustion inlet air (kg/m<sup>3</sup>)
-
-<span>\({\rho_{a,Ref}}\)</span>= Density of combustion inlet air at reference conditions (kg/m<sup>3</sup>)
-
-In an analogous fashion, the exhaust air temperature is calculated using the Nominal (reference) Exhaust Air Outlet Temperature and two modifier curves.
-
-<span>\({T_{a,o}} = {T_{a,o,Nom}}\left( {ExhAirTempFTemp} \right)\left( {ExhAirTempFPLR} \right)\)</span><span>\(\begin{array}{l}ExhAirTempFTemp = {l_1} + {l_2}\left( {{T_{a,i}}} \right) + {l_3}{\left( {{T_{a,i}}} \right)^2}\,\,\,\,\, - \,or\, - \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,{l_1} + {l_2}\left( {{T_{a,i}}} \right) + {l_3}{\left( {{T_{a,i}}} \right)^2} + {l_4}{\left( {{T_{a,i}}} \right)^3}\end{array}\)</span>
-
-<div>$$\begin{array}{l}ExhAirTempFPLR = {m_1} + {m_2}\left( {PLR} \right) + {m_3}{\left( {PLR} \right)^2}\,\,\,\,\, - \,or\, - \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,{m_1} + {m_2}\left( {PLR} \right) + {m_3}{\left( {PLR} \right)^2} + {m_4}{\left( {PLR} \right)^3}\end{array}$$</div>
-
-where:
-
-<span>\({T_{a,o}}\)</span>= Exhaust air outlet temperature (°C)
-
-<span>\({T_{a,o,Nom}}\)</span>= Nominal Exhaust Air Outlet Temperature (°C), user input
-
-<span>\(ExhAirTempFTemp\)</span>= User-defined Exhaust Air Temperature Modifier Curve (function of temperature) evaluated at the current combustion air inlet temperature. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
-
-<span>\(ExhAirTempFPLR\)</span> = User-defined Exhaust Air Flow Rate Rate Modifier Curve (function of part-load ratio) evaluated at the current operating part-load ratio. This multiplier is assumed to be 1.0 if a modifier curve name is not specified in the input.
-
-The above calculations for exhaust air outlet temperature assume no heat recovery to water is being done.  If thermal power (water heating) is being produced, then the exhaust air outlet temperature is recalculated as follows:
-
-<div>$${T_{a,o}} = {T_{a,o}} - {\raise0.7ex\hbox{${{P_{Thermal,Operating}}}$} \!\mathord{\left/ {\vphantom {{{P_{Thermal,Operating}}} {\left( {{{\dot m}_{ExhAir}}*C{p_{air}}} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {{{\dot m}_{ExhAir}}*C{p_{air}}} \right)}$}}$$</div>
-
-where:
-
-<span>\(C{p_{air}}\)</span>= Heat capacity of air at the actual combustion air inlet conditions (J/kg-K)
-
-The exhaust air outlet humidity ratio is also calculated.
-
-<div>$${w_{a,o}} = {w_{a,i}} + {\raise0.7ex\hbox{${\left[ {{{{{\dot m}_{fuel}}\left( {HHV - LHV} \right)\left( {1000} \right)} \mathord{\left/ {\vphantom {{{{\dot m}_{fuel}}\left( {HHV - LHV} \right)\left( {1000} \right)} {\left( {{h_{fg,16}}} \right)}}} \right. } {\left( {{h_{fg,16}}} \right)}}} \right]}$} \!\mathord{\left/ {\vphantom {{\left[ {{{{{\dot m}_{fuel}}\left( {HHV - LHV} \right)\left( {1000} \right)} \mathord{\left/ {\vphantom {{{{\dot m}_{fuel}}\left( {HHV - LHV} \right)\left( {1000} \right)} {\left( {{h_{fg,16}}} \right)}}} \right. } {\left( {{h_{fg,16}}} \right)}}} \right]} {\left( {{{\dot m}_{ExhAir}}} \right)}}}\right.}\!\lower0.7ex\hbox{${\left( {{{\dot m}_{ExhAir}}} \right)}$}}$$</div>
-
-where:
-
-<span>\({w_{a,o}}\)</span>= Exhaust air outlet humidity ratio (kg/kg)
-
-<span>\({w_{a,i}}\)</span>= Exhaust air inlet humidity ratio (kg/kg)
-
-<span>\({h_{fg,16}}\)</span>= Enthalpy of vaporization of moisture at 16°C (J/kg)
-
-The remaining report variables are calculated as follows.
-
-<div>$${E_{Thermal,Produced}} = {P_{Thermal,Operating}}\left( {TimeStepSys} \right)\left( {3600} \right)$$</div>
-
-<div>$$ThermalEf{f_{Operating,LHV}} = {\raise0.7ex\hbox{${{P_{Thermal,Operating}}}$} \!\mathord{\left/ {\vphantom {{{P_{Thermal,Operating}}} {{{\dot Q}_{Fuel,LHV}}}}}\right.}\!\lower0.7ex\hbox{${{{\dot Q}_{Fuel,LHV}}}$}}$$</div>
-
-where:
-
-<span>\({E_{Thermal,Produced}}\)</span>= Report variable “Generator Produced Thermal Energy [J]�
-
-<span>\(ThermalEf{f_{Operating,LHV}}\)</span>= Report variable “Generator Thermal Efficiency LHV Basis [-]�
-
-### Micro-Cogenerator
-
-The input object Generator:MicroCHP provides a model that is a direct implementation of a model developed by IEA Annex 42 – The Simulation of Building-Integrated Fuel Cell and Other Cogeneration Systems (FC+COGEN-SIM).  Annex 42 was formed as a working group within the International Energy Agency (IEA) program on Energy Conservation in Buildings and Community Systems (ECBCS). A full description of the model specification can be found in the report by Subtask B of FC+COGEN-SIM with the title “Specifications for Modelling Fuel Cell and Combustion-Based Residential Cogeneration Device within Whole-Building Simulation Programs.�  The “Micro CHP� model in EnergyPlus is the one referred to as “A Generic Model for Combustion-based Residential Cogeneration Devices.�
-
-The Micro CHP model is a straightforward empirical model with the exception that it is dynamic with respect to thermal heat recovery where performance is cast as a function of engine temperature.  It is also dynamic with respect to possible warm up and cool down periods that may affect the ability of the generator to deliver the requested power.  The relevant model equations are:
-
-<div>$${\eta_e} = f({\dot m_{cw}},{T_{cw,i}},{P_{net,ss}})$$</div>
-
-<div>$${\eta_q} = f({\dot m_{cw}},{T_{cw,i}},{P_{net,ss}})$$</div>
-
-<div>$${q_{gross}} = {P_{net,ss}}/{\eta_e}$$</div>
-
-<div>$${q_{gen,ss}} = {\eta_q}{q_{gross}}$$</div>
-
-<div>$${\dot N_{fuel}} = {q_{gross}}/LH{V_{fuel}}$$</div>
-
-<div>$$
-  \dot m_{fuel}^{t+\Delta t} = \left\{
-    \begin{array}{cl}
-      \dot m_{fuel,demand}^{t+\Delta t}       &\; if d\dot m_{fuel} / dt \le (d\dot m_{fuel}/dt)_{max} \\
-      \dot m_{fuel,demand}^t \pm (d\dot m_{fuel}/dt)_{max}      &\; if d\dot m_{fuel} / dt \gt (d\dot m_{fuel}/dt)_{max} 
-    \end{array}
-  \right.
-$$</div>
-
-<div>$${\dot m_{air}} = f({P_{net,ss}})$$</div>
-
-<div>$$
-  P_{net}^{t+\Delta t} = \left\{
-    \begin{array}{cl}
-      P_{net,ss}^{t+\Delta t}       &\; if dP_{net} / dt \le (dP_{net}/dt)_{max} \\
-      P_{net,ss}^t \pm (dP_{net}/dt)_{max}      &\; if dP_{net} / dt \gt (dP_{net}/dt)_{max} 
-    \end{array}
-  \right.
-$$</div>
-
-<div>$${[MC]_{eng}}\frac{{d{T_{eng}}}}{{dt}} = U{A_{HX}}\left( {{T_{cw,p}} - {T_{eng}}} \right) + U{A_{loss}}\left( {{T_{room}} - {T_{eng}}} \right) + {q_{gen,ss}}$$</div>
-
-<div>$${[MC]_{cw}}\frac{{d{T_{cw,o}}}}{{dt}} = {[\dot m{c_p}]_{cw}}\left( {{T_{cw,i}} - {T_{cw,o}}} \right) + U{A_{HX}}\left( {{T_{eng}} - {T_{cw,o}}} \right)$$</div>
-
-where,
-
-<span>\({\eta_e}\)</span> is the steady-state, part load, electrical conversion efficiency of the engine (-)
-
-<span>\({\eta_q}\)</span> is the steady-state part load, thermal conversion efficiency of the engine (-)
-
-<span>\({\dot m_{cw}}\)</span> is the mass flow rate of plant fluid through the heat recovery section [kg/s]
-
-<span>\({T_{cw,i}}\)</span> is the bulk temperature of the plant fluid entering the heat recovery section (<sup>o</sup>C)
-
-<span>\({T_{cw,o}}\)</span> is the bulk temperature of the plant fluid leaving the heat recovery section (<sup>o</sup>C)
-
-<span>\({P_{net,ss}}\)</span>is the steady-state electrical output of the system (W),
-
-<span>\({q_{gross}}\)</span> is the gross heat input into the engine (W),
-
-<span>\({q_{gen,ss}}\)</span> is the steady-state rate of heat generation within the engine (W)
-
-<span>\(LH{V_{fuel}}\)</span> is the lower heating value of the fuel used by the system (J/kg or J/kmol),
-
-<span>\({\dot N_{fuel}}\)</span> is the molar fuel flow rate (kmol/s)
-
-<span>\({\dot m_{fuel}}\)</span> is the mass fuel flow rate (kg/s)
-
-<span>\({\dot m_{air}}\)</span> is the mass flow rate of air thru the engine (kg/s)
-
-<span>\({[MC]_{eng}}\)</span> is the thermal capacitance of the engine control volume (W/K)
-
-<span>\({T_{eng}}\)</span> is the temperature of the engine control volume (C)
-
-<span>\(U{A_{HX}}\)</span>is the effective thermal conductance between the engine control volume and the cooling water control volume (W/K).
-
-<span>\(U{A_{loss}}\)</span> is the effective thermal conductance between the engine control volume and the surrounding environment (W/K)
-
-<span>\({T_{room}}\)</span> is the air temperature of the surrounding environment (C)
-
-<span>\({[MC]_{cw}}\)</span> is the thermal capacitance of the encapsulated cooling water and heat exchanger shell in immediate thermal contact (J/K)
-
-<span>\({[\dot m{c_p}]_{cw}}\)</span> is the thermal capacity flow rate associated with the cooling water (W/K)
-
-The functional forms for <span>\({\eta_e}\)</span> and <span>\({\eta_q}\)</span> are 2<sup>nd</sup> order trivariate polynomials with all of the cross terms.
-
-EnergyPlus solves these for state values for the engine mass temperature, <span>\({T_{eng}}\)</span>, and the outlet plant node, <span>\({T_{cw,o}}\)</span>, in the following manner. The last two equations are interrelated but otherwise ordinary differential equations with the general form
-
-<div>$$\frac{{dT}}{{dt}} = a + bT$$</div>
-
-and have analytical solution
-
-<div>$$T = \left( {{T_o} + {\raise0.7ex\hbox{$a$} \!\mathord{\left/ {\vphantom {a b}}\right.}\!\lower0.7ex\hbox{$b$}}} \right){e^{bt}} - {\raise0.7ex\hbox{$a$} \!\mathord{\left/ {\vphantom {a b}}\right.}\!\lower0.7ex\hbox{$b$}}$$</div>
-
-The engine temperature at the current timestep is calculated using
-
-<div>$$a = \frac{{U{A_{HX}}}}{{{{[MC]}_{eng}}}}*{T_{cw,o}} + \frac{{U{A_{loss}}}}{{{{[MC]}_{eng}}}}*{T_{room}} + \frac{{{q_{gen,ss}}}}{{{{[MC]}_{eng}}}}$$</div>
-
-<div>$$b =  - \left( {\frac{{U{A_{HX}}}}{{{{[MC]}_{eng}}}} + \frac{{U{A_{loss}}}}{{{{[MC]}_{eng}}}}} \right)$$</div>
-
-The plant node outlet fluid temperature (heat recovered) is solved using
-
-<div>$$a = \frac{{{{[\dot m{c_p}]}_{cw}}}}{{{{[MC]}_{cw}}}}*{T_{cw,i}} + \frac{{U{A_{HX}}}}{{{{[MC]}_{cw}}}}*{T_{eng}}$$</div>
-
-<div>$$b =  - \left( {\frac{{{{[\dot m{c_p}]}_{cw}}}}{{{{[MC]}_{cw}}}} + \frac{{U{A_{HX}}}}{{{{[MC]}_{cw}}}}} \right)$$</div>
-
-The interrelation of these two is handled by sequential substitution using an iteration scheme that alternates between calculations of <span>\({T_{eng}}\)</span> and <span>\({T_{cw,o}}\)</span>.  The iteration loop exits once the energy is determined to be balanced using the following criteria:
-
-Number of iterations &gt; 3\\
-
-<div>$$\frac{{{{\left( {{q_{gen,ss}}} \right)}_{\max }}}}{{10000000}} > U{A_{HX}}\left( {{T_{cw,o}} - {T_{eng}}} \right) + U{A_{loss}}\left( {{T_{room}} - {T_{eng}}} \right) + {q_{gen,ss}} - {[MC]_{eng}}\frac{{d{T_{eng}}}}{{dt}}$$</div>
-
-<div>$$\frac{{{{\left( {{q_{gen,ss}}} \right)}_{\max }}}}{{10000000}} > {[\dot m{c_p}]_{cw}}\left( {{T_{cw,i}} - {T_{cw,o}}} \right) + U{A_{HX}}\left( {{T_{eng}} - {T_{cw,o}}} \right) - {[MC]_{cw}}\frac{{d{T_{cw,o}}}}{{dt}}$$</div>
-
-The Micro CHP model has a number of different operating modes.  The operating mode for a given system timestep is determined from the mode during the previous timestep, user inputs, and high-level controls from elsewhere in EnergyPlus.  The operating mode is reported for the state at the end of each timestep.  The following table summarizes the various operating modes and the criteria for switching to a new mode for any given timestep.  The EnergyPlus implementation adds the “Off� mode to the modes specified by Annex 42 which corresponds to the unit being scheduled to be unavailable.  The difference between OFF and Standby modes determines whether or not standby power is consumed.
-
-<table class="table table-striped">
-<tr>
-<th>Operating mode</th>
-<th>Main Criteria</th>
-<th>Notes</th>
-</tr>
-<tr>
-<td>Off</td>
-<td>Availability schedule value = 0</td>
-<td>No consumption of power or fuel.</td>
-</tr>
-<tr>
-<td>Stand By</td>
-<td>Availability schedule value &neq; 0</td>
-<td>Consumes stand by power but no fuel</td>
-</tr>
-<tr>
-<td>Warm Up</td>
-<td>Load (thermal or electric) &gt; 0.0
-Availability schedule value &neq; 0
-Time Delay &lt; elapsed time since entering warm up mode
-Engine temp &lt; nominal engine temp</td>
-<td>Two alternate sub-modes:  Stirling Engines use warm up by “nominal engine temperature� while Internal Combustion Engines use “time delay�
-Fuel is consumed but no power is produced</td>
-</tr>
-<tr>
-<td>Normal Operation</td>
-<td>Load (thermal or electric) &gt; 0.0 Availability schedule value &neq; 0 Time Delay &gt; elapsed time since entering warm up mode
-Engine temp &gt;= nominal temp</td>
-<td>Fuel is consumed and power is produced</td>
-</tr>
-<tr>
-<td>Cool Down</td>
-<td>Load (thermal or electric) = 0.0
-Availability schedule value &neq; 0</td>
-<td>Two alternate sub-modes where engine can be forced to go thru a complete cool down cycle before allowed to go back into warm up or normal mode.
-No fuel is consumed and no power is produced.</td>
-</tr>
-
-</table>
-
-For timesteps where the generator switches from warm up mode to normal mode in the middle of the timestep, part load ration values are calculated for the portion of the time step that the generator is in normal operation.
-
-The engine and heat recovery thermal conditions are modeled for all modes so, for example, an engine that is off but still warm could provide some hot water recovery.
-
-The engine model can use an arbitray fuel mixture that is defined by the user – see the entry for Generator:FuelSupply.
-
-#### References
-
-Kelly, N. and A. Ferguson. 2007. A Generic Model Specification for Combustion-based Residential Cogeneration Devices. In *Specifications for Modelling Fuel Cell and Combustion-Based Residential Cogeneration Device within Whole-Building Simulation Programs*. I. Beausoleil-Morrison and N. Kelly editors.  Draft report of Annex 42 of the International Energy Agency ECBCS.
-
-### Fuel Cell Cogenerator
-
-The Generator:FuelCell input objects provides a model which is a direct implementation of a model developed by IEA Annex 42 – The Simulation of Building-Integrated Fuel Cell and Other Cogeneration Systems (FC+COGEN-SIM).  Annex 42 was formed as a working group within the International Energy Agency (IEA) program on Energy Conservation in Buildings and Community Systems (ECBCS).  A full description of the model specification can be found in the report by Subtask B of FC+COGEN-SIM with the title “Specifications for Modelling Fuel Cell and Combustion-Based Residential Cogeneration Device within Whole-Building Simulation Programs.�  The “Specifications for Modelling Fuel Cell Cogeneration Devices within Whole-Building Simulation Programs.�
-
-The Annex 42 Fuel Cell model is characterized as a “grey box� empirical model where a mixture of thermodynamic principles and empirical performance maps are used to model the cogeneration performance of a fairly complex device with many individual subsystems.  In EnergyPlus, the individual subsystems are separate into individual input objects such as Generator:FuelCell:PowerModule or Generator:FuelCell:ExhaustGasToWaterHeatExchanger. The resulting model is relatively complex requiring on the order of one hundred inputs.  The model is not for the faint of heart; this model is far more involved than most component models in building simulation.  This stems from the fact that fuel cell cogenerators are complicated devices that interact with the built environment in a number of ways.  Fuel cells could drawn in gas/fuel, air, and water with as many as six separate streams.  In addition to electricity and heated water, they also give off heat in the form of convection and radiation and exhaust air out of the zone.  The devices may take a long time to start up and include storage to follow loads rather than attempt to vary the power the fuel cell.  The fuel cell model allows examining system level interactions over annual timeframes that include all the important interactions with a building’s energy and comfort systems.
-
-The Annex 42 fuel cell model is described more thoroughly in the references (see below).  Here we provide a summary of the relevant model equations which are taken from the Annex 42 model specification.  The first equation is the main energy balance for the fuel cell power module (includes the fuel reformation and fuel cell stacks).  This energy balance is used to model the enthalpy of the product gases that leave the fuel cell power module.
-
-<div>$$\begin{array}{l}{\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\hat h}_i} - {\Delta_f}\hat h_i^o} \right]} \right)}_{fuel}} + {\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\hat h}_i} - {\Delta_f}\hat h_i^o} \right]} \right)}_{air}} + {{\dot N}_{liq - water}} \cdot \left( {{{\left[ {\hat h - {\Delta_f}{{\hat h}^o}} \right]}_{{H_2}O,liq}} - {\Delta_f}\hat h_{{H_2}O,fg}^o} \right)\\\quad \quad  + {{\dot H}_{dilution - air - in}} + {{\dot N}_{fuel}} \cdot LH{V_{fuel}} + {P_{el,ancillaries - AC}}\\ = {P_{el}} + {\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\ddot h}_i} - {\Delta_f}\hat h_i^o} \right]} \right)}_{FCPM - cg}} + {q_{s - cool}} + {q_{skin - loss}} + {{\dot H}_{dilution - air - out}}\end{array}$$</div>
-
-The remaining equations describe various terms and the balance of systems.  The electrical efficiency is modeled using:
-
-<div>$${\varepsilon_{el}} = \left[ {{\varepsilon_0} + {\varepsilon_1} \cdot {P_{el}} + {\varepsilon_2} \cdot P_{el}^2} \right] \cdot \left[ {1 - {N_{stops}} \cdot D} \right] \cdot \left[ {1 - (MAX(\int\limits_{} {dt - {t_{threshold}},0.0))}  \cdot L} \right]$$</div>
-
-<div>$${P_{blower - el}} = {b_0} + {b_1} \cdot {\dot N_{air}} + {b_2} \cdot \dot N_{air}^2 + {b_3} \cdot \dot N_{air}^3$$</div>
-
-In several places the model is formulated to offer different options.  For example, the flow rate of process air can be described either as a function of electrical power produced or the fuel flow rate.
-
-<div>$${\dot N_{air}} = \left[ {{a_0} + {a_1} \cdot {P_{el}} + {a_2} \cdot P_{el}^2} \right].\left[ {1 + {a_3} \cdot {T_{air}}} \right]$$</div>
-
-or
-
-<div>$${\dot N_{air}} = \left[ {{a_0} + {a_1} \cdot {{\dot N}_{fuel}} + {a_2} \cdot \dot N_{fuel}^2} \right].\left[ {1 + {a_3} \cdot {T_{air}}} \right]$$</div>
-
-<div>$${\dot N_{liq - water}} = {w_0} + {w_1} \cdot {\dot N_{fuel}} + {w_2} \cdot \dot N_{fuel}^2$$</div>
-
-<div>$${P_{pump - el}} = {p_0} + {p_1} \cdot {\dot N_{water}} + {p_2} \cdot \dot N_{water}^2 + {p_3} \cdot \dot N_{water}^3$$</div>
-
-<div>$${P_{comp - el}} = {c_0} + {c_1} \cdot {\dot N_{fuel}} + {c_2} \cdot \dot N_{fuel}^2 + {c_3} \cdot \dot N_{fuel}^3$$</div>
-
-<div>$${P_{el,ancillaries - AC}} = an{c_0} + an{c_1} \cdot {\dot N_{fuel}}$$</div>
-
-<div>$${P_{el,aux - ancillaries}} = {x_0} + {x_1} \cdot {\dot N_{aux - fuel}}$$</div>
-
-<div>$${q_{HX}} = {\varepsilon_{HX}} \cdot {\left( {\dot N{{\hat c}_p}} \right)_{\min }} \cdot \left( {{T_{aux - mix}} - {T_{water,in}}} \right)$$</div>
-
-<div>$${q_{HX}} = {\left( {UA} \right)_{eff}} \cdot \frac{{\left( {{T_{aux - mix}} - {T_{water,out}}} \right) - \left( {{T_{HX - exh}} - {T_{water,in}}} \right)}}{{\ln \left( {\frac{{{T_{aux - mix}} - {T_{water,out}}}}{{{T_{HX - exh}} - {T_{water,in}}}}} \right)}}$$</div>
-
-<div>$${\left( {UA} \right)_{eff}} = h{x_{s,0}} + h{x_{s,1}} \cdot {\dot N_{water}} + h{x_{s,2}} \cdot \dot N_{water}^2 + h{x_{s,3}} \cdot {\dot N_{aux - mix}} + h{x_{s,4}} \cdot \dot N_{aux - mix}^2$$</div>
-
-or
-
-<div>$${\left( {UA} \right)_{eff}} = {\left[ {\frac{1}{{{{\left( {hA} \right)}_{gas}}}} + \frac{1}{{{{(hA)}_{water}}}} + {F_{HX}}} \right]^{ - 1}}$$</div>
-
-where,
-
-<span>\({F_{HX}}\)</span> is an adjustment factor,
-
-<div>$$h_{gas} = h_{gas}^0 \left( \frac{\dot N_{gas}}{\dot N_{gas}^0} \right)^n}$$</div>
-
-<div>$${h_{water}} = h_{water}^0 \cdot {\left( {\frac{{{{\dot N}_{water}}}}{{\dot N_{water}^0}}} \right)^m}$$</div>
-
-<div>$${q_{HX}} = {\left( {UA} \right)_{eff}} \cdot \frac{{\left( {{T_{aux - mix}} - {T_{water,out}}} \right) - \left( {{T_{HX - exh}} - {T_{water,in}}} \right)}}{{\ln \left( {\frac{{{T_{aux - mix}} - {T_{water,out}}}}{{{T_{HX - exh}} - {T_{water,in}}}}} \right)}} + {\dot N_{{H_2}O - cond}} \cdot {\hat h_{fg}}$$</div>
-
-<div>$${\dot N_{{H_2}O - cond}} = \left( {{T_{cond - threshold}} - {T_{water,in}}} \right) \cdot \left[ {h{x_{l,1}} \cdot \left( {\frac{{{{\dot N}_{{H_2}O}}}}{{{{\dot N}_{aux - mix}}}}} \right) + h{x_{l,2}} \cdot {{\left( {\frac{{{{\dot N}_{{H_2}O}}}}{{{{\dot N}_{aux - mix}}}}} \right)}^2}} \right]$$</div>
-
-<div>$${q_{aux - skin - losses}} = {(UA)_{aux}} \cdot ({T_{aux - mix}} - {T_{room}})$$</div>
-
-<div>$${q_{skin - loss}} = {s_0} + {s_1} \cdot {\dot N_{fuel}} + {s_2} \cdot \dot N_{fuel}^2$$</div>
-
-<div>$$Q_{battery}^{t + \Delta t} = Q_{battery}^t + {P_{battery - charge}} \cdot {\varepsilon_{charge}} \cdot \Delta t$$</div>
-
-<div>$${\eta_{PCU}} = {u_0} + {u_1} \cdot {P_{PCU - in}} + {u_2} \cdot P_{PCU - in}^2$$</div>
-
-<div>$${q_{s - cool}} = \left[ {{r_0} + {r_1}\left( {{T_{stack}} - T_{stack}^o} \right)} \right] \cdot \left[ {1 + {r_2}{P_{el}} + {r_3}P_{el}^2} \right]$$</div>
-
-<div>$${\left( {UA} \right)_{s - cogen}} = {\left[ {\frac{1}{{{{\left( {hA} \right)}_{s - cogen}}}} + {F_{s - cogen}}} \right]^{ - 1}}$$</div>
-
-<div>$${h_{s - cogen}} = h_{s - cogen}^0 \cdot {\left( {\frac{{{{\dot N}_{s - cogen}}}}{{\dot N_{s - cogen}^0}}} \right)^{{n_s}}}$$</div>
-
-<div>$${P_{s - air - el}} = {f_0} + {f_1} \cdot {q_{s - air}} + {f_2} \cdot q_{s - air}^2$$</div>
-
-The Annex 42 fuel cell was implemented directly in EnergyPlus.  A sequential substitution method is used to handle all the interactions between the different subsystems.  The main energy balance drawn for the fuel cell power module is rearranged to put all the terms on the right hand side.  The enthalpy of the product gas stream is determined from this energy balance.  The Shomate equation is used to evaluate the enthalpy and specific heat of the various streams.  The EnergyPlus implementation evaluates fluid properties using the average temperature of inlet and outlet streams whereas the Annex 42 specification often uses just the inlet temperature.  The Shomate equation is inverted using the regula falsi numerical method available within EnergyPlus to calculate the temperature of the product gases from their enthalpy.
-
-#### References
-
-Beausoleil-Morrison, I., A. Schatz, and F. Marechal. 2006. A model for simulating the thermal and electrical production of small-scale solid-oxide fuel cell cogeneration systems within building simulation programs.  *HVAC & R Research*. Amer. Soc. Heating, Ref. Air-Conditioning Eng. Inc. Atlanta, GA.
-
-Beausoleil-Morrison, I., A. Weber, F. Marechal, and B. Griffith. 2007. Specifications for Modelling Fuel Cell Cogeneration Devices within Whole-Building Simulation Programs. In *Specifications for Modelling Fuel Cell and Combustion-Based Residential Cogeneration Device within Whole-Building Simulation Programs*. I. Beausoleil-Morrison and N. Kelly editors.  **Draft** report of Annex 42 of the International Energy Agency ECBCS.
-
-### Custom Fuel Supply for Generators
-
-The Generator:FuelSupply input object in EnergyPlus implements a fairly comprehensive capability to calculate properties of fuel mixtures from a description of the molar composition of all the constituents.  The fuel supply modeling is based on the specifications prepared by IEA Annex 42 for their generator models.  This modeling capability allows taking into consideration the exact gas composition of local natural gas service.  Or the user can explore the implications of an various alternative fuels such as alcohols or biogas.  An unlimited number of possible mixtures can be analyzed.
-
-Gas phase thermochemistry calculations and data are programmed into EnergyPlus to handle the set of constituents listed in the table below.  The relevant properties of each fuel constituent, *i*, are calculated as a function of temperature using the Shomate equation:
-
-<div>$${\hat h_i} - {\Delta_f}\hat h_i^o = A \cdot \left( {\frac{T}{{1000}}} \right) + \frac{B}{2} \cdot {\left( {\frac{T}{{1000}}} \right)^2} + \frac{C}{3} \cdot {\left( {\frac{T}{{1000}}} \right)^3} + \frac{D}{4} \cdot {\left( {\frac{T}{{1000}}} \right)^4} - \frac{E}{{\left( {\frac{T}{{1000}}} \right)}} + F - H$$</div>
-
-where,
-
-<span>\({\hat h_i}\)</span> is the enthalpy (J/kmol)
-
-<span>\({\Delta_f}\hat h_i^o\)</span> is the molar enthalpy at the standard state (J/kmol)
-
-<span>\(T\)</span> is the temperature of the gas (K)
-
-A, B, C, D, E, F, H are the coefficients for the Shomate equation.
-
-The lower heating value (LHV) of a fuel mixture is calculated from the molar fractions using:
-
-<div>$$LH{V_{fuel}} = \sum\limits_i {\left( {{\chi_i} \cdot LH{V_i}} \right)} $$</div>
-
-Where,
-
-<div>$$LH{V_i} = \left[ {{\Delta_f}\hat h_{{C_x}{H_y}}^o - x \cdot {\Delta_f}\hat h_{C{O_2}}^o - \frac{y}{2} \cdot {\Delta_f}\hat h_{{H_2}O}^o} \right]$$</div>
-
-*x* is the number of carbon atoms
-
-*y* is the number of hydrogen atoms
-
-Similarly, the higher heating value (HHV) of the fuel mixture is calculated using:
-
-<div>$$HH{V_{fuel}} = \sum\limits_i {\left( {{\chi_i} \cdot HH{V_i}} \right)} $$</div>
-
-Where,
-
-<div>$$HH{V_i} = \left[ {{\Delta_f}\hat h_{{C_x}{H_y}}^o - x \cdot {\Delta_f}\hat h_{C{O_2}}^o - \frac{y}{2} \cdot {\Delta_f}\hat h_{{H_2}O}^o + \frac{y}{2} \cdot \left( {{\Delta_f}\hat h_{{H_2}O}^o - {H_{liq}}} \right)} \right]$$</div>
-
-The Shomate coefficients used in EnergyPlus are listed in the table below.  Data source “NIST� indicates the data were directly from Chemistry WebBook.  Data source “CHEMKIN� indicates the data were developed by curve fitting library data for the CHEMKIN commercial program (which uses the Gorden-McBride polynomial rather than the Shomate formulation).
-
-<table class="table table-striped">
-<tr>
-<th>Constituent</th>
-<th>A</th>
-<th>B</th>
-<th>C</th>
-<th>D</th>
-<th>E</th>
-<th>F</th>
-<th>H</th>
-<th>Source</th>
-</tr>
-<tr>
-<td>N<sub>2</sub></td>
-<td>26.092</td>
-<td>8.218801</td>
-<td>-1.976141</td>
-<td>0.159274</td>
-<td>0.044434</td>
-<td>-7.98923</td>
-<td>0.0</td>
-<td>NIST</td>
-</tr>
-<tr>
-<td>O<sub>2</sub></td>
-<td>29.659</td>
-<td>6.137261</td>
-<td>-1.186521</td>
-<td>0.09578</td>
-<td>-0.219663</td>
-<td>-9.861391</td>
-<td>0.0</td>
-<td>NIST</td>
-</tr>
-<tr>
-<td>Ar</td>
-<td>20.786</td>
-<td>2.8259E-7</td>
-<td>-1.4642E-7</td>
-<td>1.0921E-8</td>
-<td>-3.6614E-8</td>
-<td>-6.19735</td>
-<td>0.0</td>
-<td>NIST</td>
-</tr>
-<tr>
-<td>CO<sub>2</sub></td>
-<td>24.99735</td>
-<td>55.18696</td>
-<td>-33.69137</td>
-<td>7.948387</td>
-<td>-0.136638</td>
-<td>-403.6075</td>
-<td>-393.5224</td>
-<td>NIST</td>
-</tr>
-<tr>
-<td>H<sub>2</sub>O(gas)</td>
-<td>29.0373</td>
-<td>10.2573</td>
-<td>2.81048</td>
-<td>-0.95914</td>
-<td>0.11725</td>
-<td>-250.569</td>
-<td>-241.8264</td>
-<td>CHEMKIN</td>
-</tr>
-<tr>
-<td>H<sub>2</sub>O(liq)</td>
-<td>-203.606</td>
-<td>1523.29</td>
-<td>-3196.413</td>
-<td>2474.455</td>
-<td>3.85533</td>
-<td>-256.5478</td>
-<td>-285.8304</td>
-<td>NIST</td>
-</tr>
-<tr>
-<td>H<sub>2</sub></td>
-<td>33.066178</td>
-<td>-11.363417</td>
-<td>11.432816</td>
-<td>-2.772874</td>
-<td>-0.158558</td>
-<td>-9.9808</td>
-<td>0.0</td>
-<td>NIST</td>
-</tr>
-<tr>
-<td>CH<sub>4</sub></td>
-<td>-0.703029</td>
-<td>108.4773</td>
-<td>-42.52157</td>
-<td>5.862788</td>
-<td>0.678565</td>
-<td>-76.84376</td>
-<td>-74.8731</td>
-<td>NIST</td>
-</tr>
-<tr>
-<td>C<sub>2</sub>H<sub>6</sub></td>
-<td>-3.03849</td>
-<td>199.202</td>
-<td>-84.9812</td>
-<td>11.0348</td>
-<td>0.30348</td>
-<td>-90.0633</td>
-<td>-83.8605</td>
-<td>CHEMKIN</td>
-</tr>
-<tr>
-<td>C<sub>3</sub>H<sub>8</sub></td>
-<td>-23.1747</td>
-<td>363.742</td>
-<td>-222.981</td>
-<td>56.253</td>
-<td>0.61164</td>
-<td>-109.206</td>
-<td>-103.855</td>
-<td>CHEMKIN</td>
-</tr>
-<tr>
-<td>C<sub>4</sub>H<sub>10</sub></td>
-<td>-5.24343</td>
-<td>426.442</td>
-<td>-257.955</td>
-<td>66.535</td>
-<td>-0.26994</td>
-<td>-149.365</td>
-<td>-133.218</td>
-<td>CHEMKIN</td>
-</tr>
-<tr>
-<td>C<sub>5</sub>H<sub>12</sub></td>
-<td>-34.9431</td>
-<td>576.777</td>
-<td>-338.353</td>
-<td>76.8232</td>
-<td>1.00948</td>
-<td>-155.348</td>
-<td>-146.348</td>
-<td>CHEMKIN</td>
-</tr>
-<tr>
-<td>C<sub>6</sub>H<sub>14</sub></td>
-<td>-46.7786</td>
-<td>711.187</td>
-<td>-438.39</td>
-<td>103.784</td>
-<td>1.23887</td>
-<td>-176.813</td>
-<td>-166.966</td>
-<td>CHEMKIN</td>
-</tr>
-<tr>
-<td>CH<sub>3</sub>OH</td>
-<td>14.1952</td>
-<td>97.7218</td>
-<td>-9.73279</td>
-<td>-12.8461</td>
-<td>0.15819</td>
-<td>-209.037</td>
-<td>-201.102</td>
-<td>CHEMKIN</td>
-</tr>
-<tr>
-<td>C<sub>2</sub>H<sub>5</sub>OH</td>
-<td>-8.87256</td>
-<td>282.389</td>
-<td>-178.85</td>
-<td>46.3528</td>
-<td>0.48364</td>
-<td>-241.239</td>
-<td>-234.441</td>
-<td>CHEMKIN</td>
-</tr>
-
-</table>
-
-#### References
-
-Beausoleil-Morrison, I., A. Weber, F. Marechal, and B. Griffith. 2007. Specifications for Modelling Fuel Cell Cogeneration Devices within Whole-Building Simulation Programs. In *Specifications for Modelling Fuel Cell and Combustion-Based Residential Cogeneration Device within Whole-Building Simulation Programs*. I. Beausoleil-Morrison and N. Kelly editors.  Report of Annex 42 of the International Energy Agency ECBCS.
-
-NIST. 2003. Chemistry WebBook, National Institute of Standards and Technology Standard Reference Database Number 69, March 2003 Release, .
-
-Gordon S. and B.J. McBride. 1971. Computer program for calculation of complex chemical equilibrium composition, rocket performance, incident and reflected shocks and Chapman-Jouguet detonations.  NASA SP-273.
-
-### Wind Turbine
-
-#### Overview
-
-The wind turbine (object Generator:WindTurbine) model is intended to estimate the production of electric power of both horizontal and vertical axis wind turbine systems. Due to the cubic relationship between the wind speed and the power produced by a wind turbine, the performance of these systems is highly dependent on local wind conditions. However, differences between typical meteorological year (TMY) wind data attached to the simulation and local wind data at the site where wind turbine system is installed typically appear. The model thus estimates the air density and wind speed at the particular height of the system and factors differences between the wind speed from the TMY weather data and the local wind speed. The weather data file should thus be included in the simulation. The model also requires inputs of both an annual average wind speed that represents accurate wind profile at the location and the height where this annual average wind speed was determined.
-
-The model calculates the power production by both horizontal axis wind turbines (HAWT) and vertical axis wind turbines (VAWT) from generic mathematical equations. Currently, a variable speed control scheme is available in EnergyPlus. The model assumes constant power generation at the rated power and the rated wind speed when the ambient wind speed is between the rated wind speed and cut out wind speed. The model does not attempt to model various types of subsystems of the entire wind turbine system such as shafts, generators and inverters due to computational convergence, time, and usability. Instead, the total system efficiency includes both conversion losses occurring during the DC-AC-DC conversion processes and delivery losses.
-
-#### Model Description
-
-The wind turbine is modeled as a generation component that produces electricity and delivers it directly to buildings. Wind turbine components are executed at the beginning of each time step called by the HVAC manager, and the electric load will be corrected with electricity from the wind turbine. The model calculates electricity production that both HAWTs and VAWTs produce from general mathematical equations. The model then passes the electricity to the electric load center in EnergyPlus at each HVAC system time step. The electric load center then determines the whole building electrical demand, deducting the power output by wind turbine along with any power production by photovoltaic components from the total electrical demand requested in the building. Excessive production of electricity greater than needed from wind turbine along with photovoltaic components is either sold or stored as the user specifies.
-
-#### Input and Data
-
-The user must input the required information according to the IO Reference Manual (ref: Generator:WindTurbine). The wind turbine model in EnergyPlus requires a unique identifying name and an availability schedule. The schedule name must refer to a valid schedule type (range 0-1) and contain values of fractional operation. Various inputs describes wind turbine configuration such as rotor type, control type, rotor diameter, overall height, and number of blades. Rated data provided in the manufacturer’s literature determines overall electricity production by using generic equations. These inputs include rated power, rated wind speed, cut in wind speed, cut out wind speed, fraction system efficiency, and maximum tip speed ratio. Two inputs such as annual local average wind speed and height for local average wind speed define local wind conditions at a specific location so that the model predicts wind speed and air density at the height of the wind turbine at the location.
-
-HAWT systems need a maximum power coefficient and empirical power coefficient parameters *C<sub>1</sub>* through *C<sub>6</sub>*. The maximum power coefficient controls overall performance of the rotor which defines the power extraction efficiency from the ambient air stream. The model predicts power generation more accurately when the user inputs the empirical power coefficients *C<sub>1</sub>* through *C<sub>6</sub>* for a specific wind turbine. Three additional inputs for VAWT system are required. The model requests blade lift and drag coefficients corresponding to the maximum tip speed ratio so that tangential and normal force coefficients are obtained. Blade chord area is also requested for calculating forces on a single blade.
-
-#### Simulation and Control
-
-Given the inputs needed, the wind turbine model analyzes local wind speed since wind speed is critical to determine the production of electricity of wind turbine systems. To minimize uncertainty involved with wind data, it factors differences between annual average wind speed from weather data and local annual average wind speed at the particular height of the local meteorological station. It reads annual average wind speed from statistical weather file that is automatically copied during the simulation. Note that the user should attach a weather data to the simulation (for a design day simulation, the wind speed data from the design day description is used). This annual average wind speed is converted into a wind speed at the height at which local annual average wind speed that the user inputs is measured and then factored as:
-
-<div>$${V_{LocalTMY}} = {V_{AnnualAvg}}{\left( {\frac{{{\delta_{met}}}}{{{H_{met}}}}} \right)^{{a_{met}}}}{\left( {\frac{H}{\delta }} \right)^a}$$</div>
-
-<div>$${F_V} = \frac{{{V_{LocalTMY}}}}{{{V_{Local}}}}$$</div>
-
-Note that the wind speed factor *F<sub>v</sub>* of 1.0 is assigned, if the user does not input the local wind conditions or the weather data file is not attached to the simulation.
-
-The local air density can be obtained by using EnergyPlus psychrometric functions as follows:
-
-<div>$${T_{Local}} = OutDryBulbTempAt(Z)$$</div>
-
-<div>$${P_{Local}} = OutBaro\Pr essAt(Z)$$</div>
-
-<div>$${\omega_{Local}} = PsyWFnTdbTwbPb({T_{Local}},{T_{wb}},{P_{Local}})$$</div>
-
-<div>$${\rho_{Local}} = PsyRhoAirFnPbTdbW({P_{Local}},{T_{Local}},{\omega_{initial}})$$</div>
-
-The model converts TMY wind speed into a wind speed at the specific height of the wind turbine rotor (*V<sub>z</sub>*) at the location by using EnergyPlus function as:
-
-<div>$${V_Z} = WindSpeedAt(Z)$$</div>
-
-The local wind speed at the rotor height (*V<sub>Local</sub>*) at the location is thus:
-
-<div>$${V_{Local}} = \frac{{{V_Z}}}{{{F_v}}}$$</div>
-
-The tip speed ratio (TSR) can be obtained as:
-
-<div>$$\lambda  = \frac{{\omega R}}{{{V_{Local}}}}$$</div>
-
-#### Horizontal Axis Wind Turbine
-
-Once the local wind speed and air density are determined, the model calculates electrical power produced by a wind turbine system according to the rotor type. For HAWT systems, two different approximations are available. The model uses an analytical approximation when the user inputs all six empirical coefficient parameters *C<sub>1</sub>* through *C<sub>6</sub>*. The equations that define the analytical approximation are:
-
-<div>$${C_p} = {C_1}(\frac{{{C_2}}}{{{\lambda_i}}} - {C_3}\theta  - {C_4}{\theta ^x} - {C_5}){e^{ - \frac{{{C_6}(\lambda ,\theta )}}{{{\lambda_i}}}}}$$</div>
-
-<div>$$\frac{1}{{{\lambda_i}}} = \frac{1}{{\lambda  + 0.08\theta }} - \frac{{0.035}}{{{\theta ^3} + 1}}$$</div>
-
-Note that the model allows changing the rotor speed to meet the maximum tip speed ratio at each time step. That is, the tip speed ratio calculated is limited by the maximum tip speed ratio. Similarly, the power coefficient calculated is also set to the maximum if the calculated is greater than the maximum.
-
-Assuming maximum of rotor angle, i.e. zero, the power production of the wind turbine is thus obtained by:
-
-<div>$${P_W} = \frac{1}{2}{\rho_{Local}}{A_R}V_{_{Local}}^3{C_p}(\lambda ,\theta )$$</div>
-
-The model assumes the simple approximation, if any of empirical power coefficient parameters is not input. The power production of wind turbine is directly obtained from the kinetic energy equation:
-
-<div>$${P_W} = \frac{1}{2}{\rho_{Local}}{A_R}V_{_{Local}}^3{C_{p,\max }}(\lambda ,\theta )$$</div>
-
-Here, the model defines *P<sub>W</sub>* as rated power output at the rated wind speed, if either the power production of wind turbine or local wind speed is greater than the rated power or rated wind speed, respectively. The power coefficient in this particular case is thus recalculated as:
-
-<div>$${C_p} = \frac{{{P_W}}}{{0.5{\rho_{Local}}AV_{_{Local}}^3}}$$</div>
-
-The overall power production that includes conversion loss and delivery loss is thus:
-
-<div>$$P = \eta {P_W}$$</div>
-
-#### Vertical Axis Wind Turbine
-
-![WindTurbine-1](media/image7837.png)
-
-Figure 340. Flow velocities and force diagram of a single blade airfoil
- (Adapted from Mazharul Islam et al., 2008)
-
-If tip speed ratio at the time step is greater than the maximum tip speed ratio, the model estimates actual rotor speed at the time step as:
-
-<div>$$\omega R = \lambda {V_{Local}}$$</div>
-
-The model then employs general mathematical expressions for the aerodynamic analysis of straight-bladed Darrieus-type VAWTs to predict the power production by VAWTs. Assuming quasi-steady state, the induced wind speed (*V<sub>a</sub>*) on the rotor is defined as:
-
-<div>$${V_a} = \frac{2}{3}{V_{Local}}$$</div>
-
-The chordal velocity (*V<sub>c</sub>*), normal velocity (*V<sub>n</sub>*), and relative flow velocity (*W*) as shown in figure above can be expressed as:
-
-<div>$${V_c} = \omega R + {V_a}\cos \theta $$</div>
-
-<div>$${V_n} = {V_a}\sin \theta $$</div>
-
-<div>$$W = \sqrt {V_c^2 + V_n^2} $$</div>
-
-The expression for the non-dimensional angle of attack (*&alpha;*) with no consideration of blade pitch is:
-
-<div>$$\alpha  = {\tan ^{ - 1}}\left[ {\frac{{\sin \theta }}{{{{(\omega R} \mathord{\left/ {\vphantom {{(\omega R} {{V_{Local}})/({{{V_a}} \mathord{\left/ {\vphantom {{{V_a}} {{V_{Local}}}}} \right. } {{V_{Local}}}}}}} \right. } {{V_{Local}})/({{{V_a}} \mathord{\left/ {\vphantom {{{V_a}} {{V_{Local}}}}} \right. } {{V_{Local}}}}}}) + \cos \theta }}} \right]$$</div>
-
-The tangential and normal force coefficients, respectively, are expressed as:
-
-<div>$${C_t} = {C_l}\sin \alpha  + {C_d}\cos \alpha $$</div>
-
-<div>$${C_n} = {C_l}\cos \alpha  + {C_d}\sin \alpha $$</div>
-
-The net tangential and normal forces are obtained from the following expressions:
-
-<div>$${F_t} = {C_t}\frac{1}{2}{\rho_{Local}}{A_c}{W^2}$$</div>
-
-<div>$${F_n} = {C_n}\frac{1}{2}{\rho_{Local}}{A_c}{W^2}$$</div>
-
-Average tangential force on a single blade can be defined as:
-
-<div>$${F_{ta}} = \frac{1}{{2\pi }}\int_0^{2\pi } {{F_t}(\theta )d\theta } $$</div>
-
-Substituting the values of *F<sub>t</sub>* and arranging tangential force on azimuth angle, <span>\(\theta \)</span>, equation above can be written as:
-
-<div>$${F_{ta}} = \frac{1}{{4\pi }}{C_t}{\rho_{Local}}{A_c}(\int_0^{2\pi } {{{(\omega R)}^2}}  + \int_0^{2\pi } {V_a^2} )$$</div>
-
-The expression of the total torque for the number of blades is defined as:
-
-<div>$$Q = N{F_{ta}}$$</div>
-
-The power production of wind turbine is thus:
-
-<div>$${P_W} = Q\omega $$</div>
-
-The model also defines *P<sub>W</sub>* as the rated power output at the rated wind speed, if either the power production of wind turbine or local wind speed is greater than the rated power.
-
-The overall power production delivered from a wind turbine system is thus:
-
-<div>$$P = \eta {P_W}$$</div>
-
-Table 92. Nomenclature for Wind Turbine model
-
-<table class="table table-striped">
-<tr>
-<th>Variable</th>
-<th>Description</th>
-<th>Units</th>
-</tr>
-<tr>
-<td>A<sub>R</sub></td>
-<td>swept area of rotor</td>
-<td>m2</td>
-</tr>
-<tr>
-<td>A<sub>C</sub></td>
-<td>blade chord area</td>
-<td>m2</td>
-</tr>
-<tr>
-<td>a</td>
-<td>site wind exponent, 0.22</td>
-<td> </td>
-</tr>
-<tr>
-<td>a<sub>met</sub></td>
-<td>wind exponent, 0.14</td>
-<td> </td>
-</tr>
-<tr>
-<td>C<sub>d</sub></td>
-<td>blade drag coefficient, 0.9</td>
-<td> </td>
-</tr>
-<tr>
-<td>C<sub>l</sub></td>
-<td>blade lift coefficients, 0.05</td>
-<td> </td>
-</tr>
-<tr>
-<td>C<sub>n</sub></td>
-<td>normal force coefficient</td>
-<td> </td>
-</tr>
-<tr>
-<td>C<sub>p</sub></td>
-<td>power coefficient (performance coefficient)</td>
-<td> </td>
-</tr>
-<tr>
-<td>C<sub>t</sub></td>
-<td>tangential force coefficient</td>
-<td> </td>
-</tr>
-<tr>
-<td>C<sub>1-6</sub></td>
-<td>empirical power coefficient parameters</td>
-<td> </td>
-</tr>
-<tr>
-<td>g<sub>o</sub></td>
-<td>standard gravity</td>
-<td>m/s2</td>
-</tr>
-<tr>
-<td>F<sub>n</sub></td>
-<td>normal force in radial direction</td>
-<td>N.m (J)</td>
-</tr>
-<tr>
-<td>F<sub>t</sub></td>
-<td>tangential force</td>
-<td>N.m (J)</td>
-</tr>
-<tr>
-<td>F<sub>ta</sub></td>
-<td>average tangential force</td>
-<td>N.m (J)</td>
-</tr>
-<tr>
-<td>F<sub>v</sub></td>
-<td>wind speed factor</td>
-<td> </td>
-</tr>
-<tr>
-<td>H</td>
-<td>height of local wind speed measurement</td>
-<td>m</td>
-</tr>
-<tr>
-<td>H<sub>met</sub></td>
-<td>height of turbine, 10</td>
-<td>m</td>
-</tr>
-<tr>
-<td>N</td>
-<td>number of blade</td>
-<td> </td>
-</tr>
-<tr>
-<td>P</td>
-<td>overall power production delivered to building </td>
-<td>W</td>
-</tr>
-<tr>
-<td>P<sub>Local</sub></td>
-<td>outdoor static air pressure at rotor height</td>
-<td>Pa</td>
-</tr>
-<tr>
-<td>P<sub>W</sub></td>
-<td>wind turbine power produced</td>
-<td>W</td>
-</tr>
-<tr>
-<td>Q</td>
-<td>overall torque</td>
-<td>N.m</td>
-</tr>
-<tr>
-<td>R</td>
-<td>turbine radius</td>
-<td>m</td>
-</tr>
-<tr>
-<td>T<sub>Local</sub></td>
-<td>local air temperature at rotor height</td>
-<td>&deg;C</td>
-</tr>
-<tr>
-<td>v</td>
-<td>ambient wind speed</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>v<sub>1</sub></td>
-<td>upstream wind speed</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>v<sub>2</sub></td>
-<td>wind speed on the turbine</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>v<sub>3</sub></td>
-<td>downstream wake velocity</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>V<sub>a</sub></td>
-<td>induced velocity</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>V<sub>AnnualAvg</sub></td>
-<td>annual average wind speed from TMY weather data</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>V<sub>Local</sub></td>
-<td>local wind speed at the location of the system</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>V<sub>LocalTMY</sub></td>
-<td>annual average wind speed converted at the local station height</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>V<sub>c</sub></td>
-<td>chordal velocity component</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>V<sub>n</sub></td>
-<td>normal velocity component</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>V<sub>Z</sub></td>
-<td>wind speed adjusted at rotor height</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>W</td>
-<td>relative flow velocity</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>Z</td>
-<td>height of wind turbine rotor</td>
-<td>m</td>
-</tr>
-<tr>
-<td>&alpha;</td>
-<td>blade angle of attack</td>
-<td>deg</td>
-</tr>
-<tr>
-<td>&theta;</td>
-<td>azimuth angle in VAWT and pitch angle in HAWT</td>
-<td>deg</td>
-</tr>
-<tr>
-<td>&rho;<sub>Local</sub></td>
-<td>local density of air at rotor height</td>
-<td>kg/m3</td>
-</tr>
-<tr>
-<td>&omega;</td>
-<td>angular velocity of turbine</td>
-<td>rad/s</td>
-</tr>
-<tr>
-<td>&omega;<sub>Local</sub></td>
-<td>local humidity ratio at rotor height</td>
-<td>kg-H2O/kg-air</td>
-</tr>
-<tr>
-<td>x</td>
-<td>exponent, 1.5</td>
-<td> </td>
-</tr>
-<tr>
-<td>&lambda;</td>
-<td>tip speed ratio</td>
-<td> </td>
-</tr>
-<tr>
-<td>&lambda;<sub>i</sub></td>
-<td>tip speed ratio at the i<sup>th</sup> pitch</td>
-<td> </td>
-</tr>
-<tr>
-<td>&sigma;<sub>met</sub></td>
-<td>wind boundary layer thickness of meteorological station, 270</td>
-<td>m</td>
-</tr>
-<tr>
-<td>&sigma;</td>
-<td>site boundary layer thickness, 370</td>
-<td>m</td>
-</tr>
-<tr>
-<td>&eta;</td>
-<td>wind turbine system efficiency</td>
-<td> </td>
-</tr>
-
-</table>
-
-#### References
-
-Siegfried Heier. 2006. Grid Integration of Wind Energy Conversion Systems, Second Edition. Wiley, Chap. 2, pp.31-44.
-
-Mazharul Islam, David S.K. Ting and Amir Fartaj. 2008. Aerodynamic Models for Darrieus-type Sraight-bladed Vertical Axis Wind Turbines. Renewable & Sustainable Energy Reviews, Volume 12, pp.1087-1109.
-
-ASHRAE. 2005. Handbook of Fundamentals, pp 16.3-16.4, Atlanta: ASHRAE.
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-
-Performance Curves and Lookup Tables
-====================================
-
-The following section describes the use of performance curves and lookup tables. Each of these objects may be used in any valid input field where a performance curve name is required.
-
-Performance curves are used directly to simulate the performance of HVAC equipment. The curves are typically created by performing a regression analysis on tabular data for a particular equipment performance metric. The regression analysis determines the equation coefficients which are the primary input to all performance curve objects. Performance tables are similar to performance curves in that they are meant to replicate a particular performance curve. Input to performance tables are made up of data pairs, the same data pairs that would be used to create performance curve coefficients. Performance tables can be interpolated using up to a 4<sup>th</sup> order polynomial equation for one independent variable tables or using a 2<sup>nd</sup> order polynomial for two independent variable tables. A regression analysis can be performed on performance tables when the simulation is instructed to use the regression analysis during the simulation (i.e., ride the curve). In addition, a performance curve object is created that can be used in future simulations and can be written to the eio file. The performance curve is written to the eio file only when the diagnostics flag is set to DisplayAdvancedReportVariables (ref. Output:Diagnostics, DisplayAdvancedReportVariables;). Lookup tables are similar to performance tables in that tabular data is used for input, however, the input 1) is more compact, 2) a regression analysis may only be performed for one and two independent variable cases, and 3) the tabular data can be read from an external file.
-
-Performance curves and data tables are created using empirical data that are derived from information gathered through observation, experience, or experimental means. Once a curve or table object is defined, these objects can be used to generically describe HVAC equipment performance. Performance curves and performance tables may be used interchangeably in Energyplus objects as required.
-
-Performance Curves
-------------------
-
-Performance curves define a polynomial equation which represents a conditional response to a model input. A polynomial is a mathematical expression which uses a sum of powers in one or more variables. The equation below represents an n<sup>th</sup> order univariate polynomial. The highest power in the equation represents its order or degree (n).
-
-<div>$$y = {a_0} + {a_1}x + {a_2}{x^2} + {a_3}{x^3} + ... + {a_n}{x^n}$$</div>
-
-A polynomial in two independent variables (multi-variate) is given by:
-
-<div>$$z = {a_{00}} + {a_{10}}x + {a_{01}}y + {a_{11}}xy + {a_{21}}{x^2}y + {a_{12}}x{y^2} + {a_{22}}{x^2}{y^2}... + {a_{nm}}{x^n}{y^m}$$</div>
-
-In Energyplus, the result of an equation, the dependent variable, represents the response a system or component has given an input (the independent variable) to the system or component model. This response represents the equipment performance related to the mechanism that causes this change (e.g., the change in capacity or power based on a conditional change in temperature, part-load ratio, or other phenomenon). A variety of performance curves are available to describe the most common forms of engineering equations. The coefficients (a-z) in the following equations are entered in the associated curve object to define a specific phenomenon. Minimum and maximum limits may be applied to both the independent and the dependent variables as necessary.
-
-### Curves based on a single independent variable
-
-A polynomial having only a single independent variable represents a one-dimensional relationship between a condition (the model input) and response (the model output). The previously described n<sup>th</sup> order univariate polynomial is representative of the following performance curves.
-
-#### Linear Curves
-
-A performance curve having an order or degree of 1.
-
-<div>$$y = a + bx$$</div>
-
-#### Quadratic Curves
-
-A performance curve having an order or degree of 2.
-
-<div>$$y = a + bx + c{x^2}$$</div>
-
-#### Cubic Curves
-
-A performance curve having an order or degree of 3.
-
-<div>$$y = a + bx + c{x^2} + d{x^3}$$</div>
-
-#### Quartic Curves
-
-A performance curve having an order or degree of 4.
-
-<div>$$y = a + bx + c{x^2} + d{x^3} + e{x^4}$$</div>
-
-#### Exponent Curves
-
-A performance curve having an order or degree of c.
-
-<div>$$y = a + b{x^c}$$</div>
-
-### Curves based on two independent variables
-
-A polynomial having two independent variables represents a two-dimensional relationship between a condition (the model inputs) and response (the model output). The previously described n<sup>th</sup> order multi-variate polynomial is representative of the following performance curves.
-
-#### QuadraticLinear Curves
-
-A performance curve having an order or degree of 2 in two independent variables.
-
-<div>$$z = a + bx + c{x^2} + dy + exy + f{x^2}y$$</div>
-
-#### CubicLinear Curves
-
-A performance curve having an order or degree of 3 in two independent variables.
-
-<div>$$z = a + bx + c{x^2} + d{x^3} + ey + fxy$$</div>
-
-#### BiQuadratic Curves
-
-A performance curve having an order or degree of 2 in two independent variables.
-
-<div>$$z = a + bx + c{x^2} + dy + e{y^2} + fxy$$</div>
-
-#### BiCubic Curves
-
-A performance curve having an order or degree of 3 in two independent variables.
-
-<div>$$z = a + bx + c{x^2} + dy + e{y^2} + fxy + g{x^3} + h{y^3} + i{x^2}y$$</div>
-
-Calulating performance curve coefficients in a spreadsheet is a simple matter of finding the data required to perform the regression analysis. For example, the biquadratic equation shown above is representative of the cooling capacity as a function of temperature performance curve for DX cooling coils. The fundamental equation for DX cooling coil capacity is:
-
-<div>$$TotCapTempModFac = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d\left( {{T_{c,i}}} \right) + e{\left( {{T_{c,i}}} \right)^2} + f\left( {{T_{wb,i}}} \right)\left( {{T_{c,i}}} \right)$$</div>
-
-where
-
-Twb,i = wet-bulb temperature of the air entering the cooling coil, °C
-
-Tc,i (or Tdb,i)= dry-bulb temperature of the air entering an air-cooled condenser, °C
-
-Given the data set shown in the table below, each of the independent variables would be calculated according to the fundamental equation above (i.e., the T, T<sup>2</sup>, and cross-product terms would be multiplied out). The data would be converted to degrees celcius and the cooling capacity would be converted to Watts. The data would also be normalized using the ARI rating point shown as highlighted in the table.
-
-![DataTable](media/image7865.png)
-
-The fundamental equation would be used to determine the number of independent variables and also the form of the equation. Given the example described here, the spreadsheet would be set up to look like the equation as shown in the following table. A regression analysis could then be performed on the data set. The first five columns are the independent variables and the last column is the dependent variable. A spreadsheet tool is selected to perform the regression analysis, and the coefficients are calculated and displayed in the spreadsheet.
-
-![RegressionAnalysis](media/image7866.png)
-
-
-
-The regression analysis and summary statistical output is shown below. The equation coefficients are shown highlighted. In this example, the equation coefficents are: a = 0.757382, b = 0.014666, c= 0.000459, d = -0.00095, e = -6.7E-05, and f = -0.00015. These coefficients would be entered in a Curve:BiQuadratic object and used to describe the cooling capacity as a function of temperature for the DX cooling coil model. Minimum and Maximum values from the tabular data are entered as Min/Max values for the curve object. The values may be relaxed slightly with care to allow extrapolation as needed. A performance table may be used to automatically perform the regression analysis as described in the following section.
-
-
-
-![RegressionSummaryOutput](media/image7867.png)
-
-
-
-```idf
-  Curve:Biquadratic,
-    CoolCapFTExample,        !- Name
-    0.757382,                !- Coefficient1 Constant
-    0.014666,                !- Coefficient2 x
-    0.000459,                !- Coefficient3 x**2
-    -0.00095,                !- Coefficient4 y
-    -0.000067,               !- Coefficient5 y**2
-    -0.00015,                !- Coefficient6 x*y
-    17.22222,                !- Minimum Value of x
-    21.66667,                !- Maximum Value of x
-    18.33333,                !- Minimum Value of y
-    46.11111,                !- Maximum Value of y
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature,             !- Input Unit Type for Y
-    Dimensionless;           !- Output Unit Type
-```
-
-
-
-
-### Curves based on three independent variables
-
-A polynomial having three independent variables represents a three-dimensional relationship between a condition (the model inputs) and response (the model output).
-
-#### TriQuadratic Curves
-
-A performance curve having an order or degree of 2 in three independent variables.
-
-<div>$$\begin{array}{l}Output = a + b{x^2} + cx + d{y^2} + ey + f{z^2} + gz + h{x^2}{y^2} + ixy + jx{y^2} + k{x^2}y\\\,\,\,\, + l{x^2}{z^2} + mxz + nx{z^2} + o{x^2}z + p{y^2}{z^2} + qyz + ry{z^2} + s{y^2}z + t{x^2}{y^2}{z^2}\\\,\,\,\, + u{x^2}{y^2}z + u{x^2}y{z^2} + vx{y^2}{z^2} + w{x^2}yz + x\left( {x{y^2}x} \right) + y\left( {xy{z^2}} \right) + z\left( {xyz} \right)\end{array}$$</div>
-
-### Pressure drop curve
-
-#### Functional Pressure Drop Curve
-
-A performance curve representing the minor loss and/or friction calculations in plant pressure simulations.
-
-<div>$$\Delta P = \left[ {K + f\left( {L/D} \right)} \right]\left( {\rho {V^2}} \right)/2$$</div>
-
-Performance Tables
-------------------
-
-Performance tables provide a method to enter specific performance data in tabular form. Tabular data represent equipment performance in a manner similar to performance curves, however, the necessity to formulate the equation coefficient is not required. Tabular data may be used to directly interpolate the actual data within the tables independent variable limits or a regression analysis may be performed to calculate the equation coefficients and use these coefficients for the associated engineering calculations. When direct interpolation is selected, the tabular data is interpolated linearly between the first independent variable and then, if used, the second independent variable. The name of a table object may be used interchangeably in any valid field where a performance curve name is required.
-
-### Tables based on a single independent variable
-
-The tabular data entered for polynomials with a single independent variable represent x and outupt data pairs as described in the previous section for performance curves.  The x in each of the previous equations represent the independent variable (model input) and the output represents the dependent variable. The data pairs are organized as the data point for the independent variable followed by the data point for the dependent variable. The data pairs form a one-dimensional array that may either be linearly interpolated, interpolated based on a polynomial equation, or this data may be used to calculate the equation coefficients (a-e) as described in the previous section.
-
-The equation form is user selected as either linear, quadratic, cubic, quartic, or exponent. This choice determines: 1) where this table object may be used (i.e., certain objects may required a specific form of the equation), and 2) the degree or order used to calculate the regression coefficients. The following example describes the methodology used when tabular input data is used in place of common performance curve objects. Although Energyplus does not use a performance curve in the manner described in this example, this example is ideally suited for teaching the basics of tabular data entry.
-
-Given a generic manufacturers fan data for a fan having a maximum flow rate of 5 m3/s and power of 125 W, the power is shown in the table below to be proportional to the cube of flow rate. Since, in this example, the flow rate is not a valid input for calculating fan power, the flow rate will be converted to flow fraction (or PLR). The power data is entered as the actual fan power and will be normalized by the program according to the maximum power of 125W. Also shown here are the performance curve outputs using the regression coefficients calculated by the program. The performance curve outputs represent the fan power ratio as a function of flow fraction. Additional significant digits are included to show the impact a given data set may have on the resulting coefficients (i.e., not quite 0 at the zero crossing, rounding causes slight errors in the actual coefficient values, etc).
-
-
-
-<table class="table table-striped">
-<tr>
-<th>Air Flow (m3/s)</th>
-<th>Flow Fraction  or Fan PLR</th>
-<th>Power (W)</th>
-<th>Power Ratio Curve Output</th>
-</tr>
-<tr>
-<td>0</td>
-<td>0</td>
-<td>0</td>
-<td>-1.1102230246E-16</td>
-</tr>
-<tr>
-<td>0.5</td>
-<td>0.1</td>
-<td>0.125</td>
-<td>0.00100000000000018</td>
-</tr>
-<tr>
-<td>1</td>
-<td>0.2</td>
-<td>1</td>
-<td>0.00800000000000004</td>
-</tr>
-<tr>
-<td>3</td>
-<td>0.6</td>
-<td>27</td>
-<td>0.215999999999995</td>
-</tr>
-<tr>
-<td>4</td>
-<td>0.8</td>
-<td>64</td>
-<td>0.51199999999999</td>
-</tr>
-</table>
-
-
-
-The tabular data can be entered directly into a table object. The data for flow fraction (or fan part-load ratio) and power are entered as data pairs. As this example describes how the fan power changes with changes in air flow, the curve type selected is Cubic and, therefore, the minimum number of data pairs equals 4 (i.e., number of coefficients in a cubic equation) although 5 are used in this example. In addition, since calculating regression coefficients for this data set would yield more accurate results than linearly interpolating this data set, the selection is made to evaluate the curve to the limits specified. In this example, the fan in question is capable of operating up to 5 m3/s at 125 Watts (which is purposely not provided in this set of tabular data). We need this information because we want to create a fan power ratio equation with an input of 0-1 for fan part-load ratio and a table output of 0-1 for fan power ratio. Therefore, the tabular data need to be normalized at a part-load ratio of 1 (i.e., normalized to the power at full flow). The following table object describes the input necessary for this particular data set.
-
-
-
-```idf
-Table:OneIndependentVariable,
-MyFanPower,   !- Name  [Fit from catalog performance data]
-Cubic,     !- Curve Type
-EvaluateCurveToLimits,  !- Interpolation Type
-0,         !- Minimum Value of X1,
-1,         !- Maximum Value of X1,
-0,         !- Minimum Table Output
-64,        !- Maximum Table Output
-Dimensionless,  !- Input Unit Type for X1
-Dimensionless,  !- Output Unit Type
-125,       !- Normalization Point
-0.8,64,    !- X Value #1, Output Value #1
-0,0.0,     !- X Value #2, Output Value #2
-0.2,1,     !- X Value #3, Output Value #3
-0.1,0.125, !- X Value #4, Output Value #4
-0.6,27;    !- X Value #5, Output Value #5
-```
-
-
-
-Notice in this example that:
-
-1)    The data pairs do not need to be entered in ascending order, this data set will automatically be re-ordered in ascending order by the program.
-
-2)    The minimum and maximum table output entered by the user uses the same units as the output values and are subsequently normalized in the same manner as the dependent variable in the data pairs.
-
-3)    For the resulting curve object (see below), the minimum (maximum) limits are based on the lesser (greater) of the user entered value and the lower (upper) limit of the tabular data. When linearly interpolating tabular data, the limits of the data set are used unless the user entered maximum is more restrictive (e.g., 64 W in this example is not more restrictive than the data set).
-
-4)    For the resulting curve object, the calculated coefficients may not perfectly represent the data set (i.e., in this example coefficient 1, 2, and 3 should have been 0). Duplicating the 0,0 data pair four additional times (to weight the 0 crossing) yields constant coefficients of 0. This could also be changed manually in the curve object created by the program.
-
-5)    Referring to the figure below, a selection of LinearInterpolationOfTable would interpolate the tabular data within the limits of the data set (blue circles) resulting in a maximum X and Curve value of 0.8 and 0.512 (i.e., 64/125), respectively. Selecting EvaluateCurveToLimits allows extrapolation of the data set up to a power ratio of 1 had 125 W been entered as the maximum table output in this example.
-
-6)    In the graph below, the linearly interpolated tabular data (blue line) represent a less accurate fan power ratio curve than the performance curve itself (red line). In this specific example, it is more accurate to rely on the performance curve results (i.e., Interpolation Type = EvaluateCurveToLimits in table object). In addition, the performance curve is able to extrapolate outside the limits of the data set since the regression analysis provides a smooth continuous curve through 1. Selecting the LagrangeInterpolationLinearExtrapolation interpolation method with a cubic curve type is similar to the performance curve results.
-
-7)    Including additional data in the table object (e.g., data points for flow fractions = 0.4 and 1) would allow direct linear interpolation of the tabular data without significant loss of accuracy compared to the performance curve or lagrange methods.
-
-
-
-Curve output in eio file (when using Output:Diagnostics, DisplayAdvancedReportVariables):
-
-```
-!...GENERATING NEW CURVE OBJECT
-! Input as Table:OneIndependentVariable "MYFANPOWER"
-! RSquared = 1.0000000000
-! Standard Error = 7.3549798168E-016
-! Degrees of Freedom = 5
-Curve:Cubic,
- MYFANPOWER,         !- Name
- -1.1102230246E-016, !- Coefficient1 Constant
- 5.0571599639E-015,  !- Coefficient2 x
- -2.1582431250E-014, !- Coefficient3 x**2
- 1.0000000000,       !- Coefficient3 x**3
- 0.0000000000,       !- Minimum Value of x
- 1.0000000000,       !- Maximum Value of x
- 0.0000000000,       !- Minimum Curve Output
- 1.0000000000;       !- Maximum Curve Output
-!...END GENERATING NEW CURVE OBJECT
-```
-
-![FanPowerRatioExample](media/image7870.png)
-
-### Tables based on two independent variables
-
-The tabular data entered for polynomials with two independent variables represent x, y and output data pairs as described in the previous section for performance curves.  The x and y in each of the previous equations represent the independent variables (model inputs) and the output represents the dependent variable. The data pairs are organized as the data points for the independent variables followed by the data point for the dependent variable. The order of the data is significant in that the x and y data are entered in the same order as shown in the model’s fundamental equation. The data pairs form a two-dimensional array that may either be linearly interpolated, interpolated using a second order polynomial, or this data may be used to calculate the equation coefficients (a-f) as described in the previous section.
-
-The equation order or degree is user selected as biquadratic or quadraticlinear. This choice determines: 1) where this table object may be used (i.e., certain objects may required a specific form of the equation), and 2) the fundamental equation used to calculate the regression coefficients. The following example describes the methodology used when tabular input data is used in place of common performance curve objects.
-
-Given a generic manufacturers air conditioner data for an AC system having a rated total cooling capacity of 7735.1 W, the change in capacity is shown in the table to be a function of both cooling coil entering air wet-bulb temperature and condenser entering air dry-bulb temperature. The tabular data is entered as the actual cooling capacity and will be normalized by the program according to the rated capacity of 7735.1 W. The cooling coil EIR curve could be developed in a similar fashion, except that EIR (Power / TotCap) must first be calculated from the tabular data below BEFORE entering this data into a table object. In this example, only data highlighted in yellow will be used.
-
-![NormalizedCapacity](media/image7871.png)
-
-The tabular data can be entered directly into a table object. As an example, for an air-cooled DX cooling coil object in Energyplus, the capacity as a function of temperature has the following fundamental equation (Ref. Single-Speed Electric DX Air Cooling Coil):
-
-<div>$$TotCapTempModFac = a + b\left( {{T_{wb,i}}} \right) + c{\left( {{T_{wb,i}}} \right)^2} + d\left( {{T_{c,i}}} \right) + e{\left( {{T_{c,i}}} \right)^2} + f\left( {{T_{wb,i}}} \right)\left( {{T_{c,i}}} \right)$$</div>
-
-where
-
-Twb,i = wet-bulb temperature of the air entering the cooling coil, °C
-
-Tc,i = dry-bulb temperature of the air entering an air-cooled condenser, °C
-
-Given this form of the fundamental equation, the data pairs for the cooling coil are entered as entering air wet-bulb temperature, condenser entering dry-bulb temperature, and total cooling capacity. These 3 values, in this precise order, make up each data pair. As this example describes how the DX coil cooling capacity changes with changes in indoor and outdoor temperature, the curve type selected is BiQuadratic and, therefore, the minimum number of data pairs equals 6 (i.e., number of coefficients in the equation above). Evaluating this tabular data based on regression coefficients may be less desirable to the user since the data in the lower right corner of the table is somewhat flat due to controls or other hardware constraints. For the sake of this example, the regression analysis is chosen. In this example, the DX cooling coil total cooling capacity at the ARI rating point is used to normalize the capacity data (e.g., 7735.1 W at 19.4 °C EWB and 35 °C outdoor dry-bulb temperature). In addition, the minimum and maximum limits are chosen such that extrapolation of the performance curve is allowed. Notice in the example below that:
-
-1)    The data pairs do not need to be entered in ascending order, this data set will automatically be re-ordered in ascending order by the program.
-
-2)    As shown in the table object below, only three of the five entries for entering air wet-bulb temperature were entered in the table object and therefore used for the regression analysis. This data entry technique may save time when entering a large data set, however, it may have unforeseen consequences on the resulting regression coefficients (i.e., the coefficients may provide less accuracy than desired). Note in the figure below the difference between the manufacturers data at 19.4 °C entering air wet-bulb temperature vs the prediction made by the regression coefficients. Since this data set (i.e., the 4 data points at 19.4°C entering air wet-bulb temperature from the table above) was left out of the regression analysis, the predicted capacity at this condition is slightly under-estimated.
-
-3)    The minimum and maximum table output entered by the user uses the same units as the output values and are subsequently normalized in the same manner as the dependent variable in the data pairs.
-
-4)    For the resulting curve object, the minimum (maximum) limits are based on the lesser (greater) of the user entered value and the lower (upper) limit of the tabular data. When linearly interpolating tabular data, only the limits of the data set are used.
-
-5)    For the resulting curve object, the calculated coefficients may not perfectly represent the entire data set since all data was not used (i.e., in this example the regressed data do not line up exactly with all the manufacturers data, however, do line up well with the data included in the table object).
-
-6)    Selecting LinearInterpolationOfTable would interpolate the tabular data within the limits of the data set (characters) resulting in a maximum X1, X2 and Curve value of 22.2, 40.8 and 1.25 (i.e., 9206.0/7375.1), respectively. Note how these maximum values compare to the maximum values in the generated curve object below which chose the EvaluateCurveToLimits option instead (i.e., the user min/max inputs were used to generate these fields when creating the curve object). The minimum values would be affected in a similar manner. Selecting Lagrange or EvaluateCurveToLimits allows extrapolation of the data set to values specified by the user.
-
-7)    In the graph below, the linearly interpolated tabular data (character data set representing manufacturers data) may better represent the capacity ratio than the performance curve (lines representing the regressed data) given the non-linear relationship between capacity and temperature shown in the table and/or graph. However, extrapolation of the data set is performed linearly and the second order affects of temperature would be lost when extrapolating. Either the data set would be expanded to include other relevant data (e.g., data at colder outdoor temperatures where cooling may be required) which could then be interpolated or additional existing data could be added to the table object to allow more accurate regression coefficients to be used to predict data outside the table data limits.
-
-
-
-```idf
-Table:TwoIndependentVariables,
-CCoolCapFT,       !- Name  [Fit from catalog performance data]
-BiQuadratic,      !- Curve Type
-EvaluateCurveToLimits,  !- Interpolation Type
-1,                !- Minimum Value of x,
-30,               !- Maximum Value of x,
-5,                !- Minimum Value of y,
-50,               !- Maximum Value of y,
-4500,             !- Minimum Table Output
-15000,            !- Maximum Table Output
-Temperature,      !- Input Unit Type for x
-Temperature,      !- Input Unit Type for y
-Dimensionless,    !- Output Unit Type
-7735.1,           !- Normalization Point
-17.2,29.4,7462.6, !- X, Y, and Output data pair #1
-17.2,23.9,7735.1, !- X, Y, and Output data pair #2
-13.9,29.4,7283.9, !- X, Y, and Output data pair #3
-13.9,23.9,7474.4, !- X, Y, and Output data pair #4
-13.9,35,7067.1,   !- X, Y, and Output data pair #5
-13.9,40.8,6818.0, !- X, Y, and Output data pair #6
-17.2,35,7157.9,   !- X, Y, and Output data pair #7
-17.2,40.8,6818.0, !- X, Y, and Output data pair #8
-22.2,35,8552.6,   !- X, Y, and Output data pair #9
-22.2,29.4,8898.3, !- X, Y, and Output data pair #10
-22.2,23.9,9206.0, !- X, Y, and Output data pair #11
-22.2,40.8,8165.8; !- X, Y, and Output data pair #12
-```
-
-Curve output in eio file (when using Output:Diagnostics, DisplayAdvancedReportVariables):
-
-```
-CREATING NEW CURVE OBJECT
-! Input as Table:TwoIndependentVariables "CCOOLCAPFT"
-! RSquared       = 0.9993993101
-! Standard Error = 3.4649248573E-003
-! Sample Size    = 12
-Curve:BiQuadratic,
-FromTable_CCOOLCAPFT,  !- Name
-  1.7214120578,  !- Coefficient1 Constant
-  -0.1011737262,  !- Coefficient2 x
-  3.7738833967E-003,  !- Coefficient3 x**2
-  2.8686934910E-003,  !- Coefficient4 y
-  -5.3785351258E-005,  !- Coefficient5 y**2
-  -3.4086036156E-004,  !- Coefficient6 x*y
-  1.0000000000,  !- Minimum Value of x
-  30.0000000000,  !- Maximum Value of x
-   5.0000000000,  !- Minimum Value of y
-  50.0000000000,  !- Maximum Value of y
-  0.5817636488,  !- Minimum Curve Output
-  1.9392121627;  !- Maximum Curve Output
-END CREATING NEW CURVE OBJECT
-```
-
-![NormalizedCapacity](media/image7873.png)
-
-### Lookup Tables
-
-Lookup tables provide a method to evaluate a group of data that may or may not conform to a fundamental equation. Only tabular data which conform to existing performance curve equations are currently allowed (i.e., that lookup table name is entered where any valid performance curve is allowed therefore the table data must conform to the models fundamental equation for that specific curve). Efforts to include this lookup table in the energy management system would allow custom use of lookup tables, however, calling lookup tables from the EMS system is not currenly possible. Lookup tables can interpolate the actual data using a non-linear polynomial equation (order higher than 1). As with other table or curve objects, the lookup table can be used anywhere a valid curve object name is allowed. Care must be taken to ensure the table data format is consistent with the associate model that is using the performance curve (e.g., DX cooling coil capacity as a function of temperature where independent variable X1 = indoor wet-bulb temperature and independent variable X2 = outdoor dry-bulb temperature).
-
-The lookup tables are evaluated using the Lagrange form of the interpolation polynomial or the previously described interpolation methods of LinearInterpolationOfTable and EvaluateCurveToLimits. When using the Lagrange method, the number of points used in the interpolation is equal to 1 plus the polynomial order (e.g., a second order interpolation would use 3 points).
-
-<div>$${p_n}\left( x \right) = \sum\limits_{i = 0}^n {{y_i}{l_i}\left( x \right)} $$</div>
-
-<div>$${l_i}\left( x \right) = \mathop \Pi \limits_{j \ne i} \left( {\frac{{x - {x_j}}}{{{x_i} - {x_j}}}} \right)\,\,\,\,\,\,i = 0,1,...,n$$</div>
-
-First-order Lagrange interpolation polynomial:
-
-<div>$${p_1}\left( x \right) = \frac{{\left( {x - {x_1}} \right)}}{{\left( {{x_0} - {x_1}} \right)}}{y_0} + \frac{{\left( {x - {x_0}} \right)}}{{\left( {{x_1} - {x_0}} \right)}}{y_1}$$</div>
-
-Second-order Lagrange interpolation polynomial:
-
-<div>$${p_2}\left( x \right) = \frac{{\left( {x - {x_1}} \right)\left( {x - {x_2}} \right)}}{{\left( {{x_0} - {x_1}} \right)\left( {{x_0} - {x_2}} \right)}}{y_0} + \frac{{\left( {x - {x_0}} \right)\left( {x - {x_2}} \right)}}{{\left( {{x_1} - {x_0}} \right)\left( {{x_1} - {x_2}} \right)}}{y_1} + \frac{{\left( {x - {x_0}} \right)\left( {x - {x_1}} \right)}}{{\left( {{x_2} - {x_0}} \right)\left( {{x_2} - {x_1}} \right)}}{y_2}$$</div>
-
-Third-order Lagrange interpolation polynomial:
-
-<div>$$\begin{array}{l}{p_3}\left( x \right) = \frac{{\left( {x - {x_1}} \right)\left( {x - {x_2}} \right)\left( {x - {x_3}} \right)}}{{\left( {{x_0} - {x_1}} \right)\left( {{x_0} - {x_2}} \right)\left( {{x_0} - {x_3}} \right)}}{y_0} + \frac{{\left( {x - {x_0}} \right)\left( {x - {x_2}} \right)\left( {x - {x_3}} \right)}}{{\left( {{x_1} - {x_0}} \right)\left( {{x_1} - {x_2}} \right)\left( {{x_1} - {x_3}} \right)}}{y_1} + \\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\frac{{\left( {x - {x_0}} \right)\left( {x - {x_1}} \right)\left( {x - {x_3}} \right)}}{{\left( {{x_2} - {x_0}} \right)\left( {{x_2} - {x_1}} \right)\left( {{x_2} - {x_3}} \right)}}{y_2} + \frac{{\left( {x - {x_0}} \right)\left( {x - {x_1}} \right)\left( {x - {x_2}} \right)}}{{\left( {{x_2} - {x_0}} \right)\left( {{x_2} - {x_1}} \right)\left( {{x_2} - {x_2}} \right)}}{y_3}\end{array}$$</div>
-
-where:
-
-x = interpolation point
-
-x<sub>n</sub> = x value of tabular data
-
-y<sub>n</sub> = y value of tabular data
-
-p<sub>i</sub>(n) = polynomial (table) output
-
-The lookup table is interpolated using the interpolation polynomial shown above. If the table input value (interpolation point) is near the bottom edge or exceeds the table boundaries, a linear extrapolation is used (2-point extrapolation). The interpolation order is determined by the user entered number of interpolation points.
-
-A regression analysis may be performed on any lookup table having one or two indpenedent variables. As with performance tables, the resulting performance curve coefficients are calculated and used in the simulation only when the interpolation method is selected as EvaluateCurveToLimits. In addition, the performance curve is only written to the eio file when the output diagnostics flag is set to DisplayAdvancedReportVariables (ref. Output:Diagnostics, DisplayAdvancedReportVariables;)..
-
-Using the example provided in the section above for Tables based on two indpendent variables, the lookup table object would be defined as follows:
-
-```idf
-Table:MultiVariableLookup,
-CCoolCapFT,
-EvaluateCurveToLimits,
-3,
-BiQuadratic,
-SingleLineIndependentVariableWithMatrix,
-,
-ASCENDING,
-ASCENDING,
-7735.1,  !- Normalization reference
-1,       !- Minimum Value of X1
-30,      !- Maximum Value of X1
-5,       !- Minimum Value of X2
-50,      !- Maximum Value of X2
-,        !- Minimum Value of X3
-,        !- Maximum Value of X3
-,        !- Minimum Value of X4
-,        !- Maximum Value of X4
-,        !- Minimum Value of X5
-,        !- Maximum Value of X5
-4500,    !- Minimum Table Output
-15000,   !- Maximum Table Output
-Temperature,  !- Input Unit Type for X1
-Temperature,  !- Input Unit Type for X2
-,        !- Input Unit Type for X3
-,        !- Input Unit Type for X4
-,        !- Input Unit Type for X5
-Dimensionless,    !- Output Unit Type
-   2, 3, 4,
-  13.9, 17.2, 22.2,
-  23.9, 29.4, 35.0, 40.8,
-  7474.4,  7735.1,  9206.0,
-  7283.9,  7462.6,  8898.3,
-  7067.1,  7157.9,  8552.6,
-  6818.0,  6818.0,  8165.8;
-```
-
-
-
-
diff --git a/doc/src/docs/EngineeringReference/16-Economics.md b/doc/src/docs/EngineeringReference/16-Economics.md
deleted file mode 100644
index 46c22260e07..00000000000
--- a/doc/src/docs/EngineeringReference/16-Economics.md
+++ /dev/null
@@ -1,482 +0,0 @@
-Economics Calculations
-======================
-
-Component Costs
----------------
-
-EnergyPlus provides simple cost estimating capabilities as an aid to design analysis and for life cycle costs.  There are three broad steps involved.  The first involves determining *construction* costs by summing individual “line items.�  The second involves determining *project* costs by adjusting construction costs to account for things like profit and design fees.  The third involves comparing the current simulation to a reference case so that marginal increases can be calculated.  The reference documentation contained in this section pertains to the following input object names.
-
-* **ComponentCost:LineItem**
-
-* **ComponentCost:Adjustments**
-
-* **ComponentCost:Reference**
-
-### Line Item Costs
-
-Line item cost calculations are generally trivial involving simple multiplication and summation.  This section documents details of how line item costs are calculated.  The program code consists mainly of a **Case** construct where the **Line Item Type** is used to control the details of how calculations are performed.
-
-The overall philosophy is to provide methods of calculating items using either direct entry of needed data (**‘General’** using object type), or using component descriptive data entered elsewhere in the input file (e.g. **‘Lights’**), or by using quantities that are calculated by the program during the simulation (e.g. **‘Coil:DX’** and **‘Chiller:Electric’**). 
-
-The rest of this section provides details by organized by the type of line item.
-
-#### General
-
-The line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-Each, *P<sub>e</sub>*:
-
-<div>$$L = N * {P_e}$$</div>
-
-#### Construction
-
-This line item type is called “Construction� but is used to estimate the costs of surfaces in the model.  The Construction attribute of Surface objects is useful for categorizing surfaces.  The number of units, *N*, is determined by summing the Area, *A*, of Surface objects that have the type of construction specified in the **Item Name** field.  Surfaces are screened to eliminate any duplicates that may exist for interior partitions creating a list of 1 to *m* unique surfaces.  If a surface is associated with a Zone, then zone multiplier, *M<sub>Z</sub>*, and list multipliers, *M<sub>G</sub>*, are applied (these are usually defaulted to 1).
-
-<div>$$N = \sum\limits_1^m {(A*{M_Z} * {M_G}} )$$</div>
-
-The line item subtotal, *L*, is calculated by multiplying the number of units (actually units of are here), *N* (m<sup>2</sup>) by the Cost-per-Area, *P<sub>a</sub>* , ($/m<sup>2</sup>):
-
-<div>$$L = N * {P_a}$$</div>
-
-#### Coil:DX and Coil:Cooling:DX:SingleSpeed
-
-DX coil costs can be estimated in one of three ways: per-each, per-kW, per-kW-COP.  The program determines which method to use based on there being non-zero values in appropriate input fields.
-
-If **cost per each** is greater than 0.0 then the number of units, *N*, is the number of cooling coils.  This will be 1 if the **Item Name** is the name of a specific coil described elsewhere.  If the name is set to the wildcard (\*) then this will equal the total number of DX:Coils in the model.  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-Each, *P<sub>e</sub>*:
-
-<div>$$L = N * {P_e}$$</div>
-
-If **cost per kilowatt** is greater than 0.0 then the number of units, *N*, is the number of kilowatts of total, rated, cooling capacity.  This will be based on all the DX:Coils in the model if **Item Name** is set to the wildcard (\*) and will be that of the named coil if set to a valid coil name.  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-kilowatt, *P<sub>kW</sub>*:
-
-<div>$$L = N * {P_{kW}}$$</div>
-
-If **Cost per kilowatt per coefficient-of-performance** is greater than 0.0 then the number of units, *N*, is the number of kilowatts of total, rated, cooling capacity multiplied by the nominal coefficient of performance (COP) of the DX:Coils.  This will be based on all the DX:Coils in the model if **Item Name** is set to the wildcard (\*) and will be that of the named coil if set to a valid coil name.  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-kilowatt-per-COP, *P<sub>kW-COP</sub>*:
-
-<div>$$L = N * {P_{kW - COP}}$$</div>
-
-#### Coil:Heating:Gas
-
-Gas-fired heating coil costs can be estimated in one of three ways: per-each, per-kW, per-kW-COP.  The program determines which method to use based on there being non-zero values in appropriate input fields.
-
-If **cost per each** is greater than 0.0 then the number of units, *N*, is the number of heaters.  This will be 1 if the **Item Name** is the name of a specific heater described elsewhere.  If the name is set to the wildcard (\*) then this will equal the total number of Coil:Heating:Gas objects in the model.  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-Each, *P<sub>e</sub>*:
-
-<div>$$L = N * {P_e}$$</div>
-
-If **Cost per kilowatt** is greater than 0.0 then the number of units, *N*, is the number of kilowatts of total, rated, heating capacity.  This will be based on all the Coil:Heating:Gas objects in the model if **Item Name** is set to the wildcard (\*) and will be that of the named coil if set to a valid coil name.  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-kilowatt, *P<sub>kW</sub>*:
-
-<div>$$L = N * {P_{kW}}$$</div>
-
-If **Cost per kilowatt per coefficient-of-performance** is greater than 0.0 then the number of units, *N*, is the number of kilowatts of total, rated, heating capacity multiplied by the theoretical efficiency of the heater(s).  (Here we are treating gas heating efficiency as a Coefficient of Performance (COP)).  This will be based on all the Coil:Heating:Gas objects in the model if **Item Name** is set to the wildcard (\*) and will be that of the named coil if set to a valid coil name.  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-kilowatt-per-COP, *P<sub>kW-COP</sub>*:
-
-<div>$$L = N * {P_{kW - COP}}$$</div>
-
-#### Chiller:Electric
-
-Electric chiller costs can be estimated in one of three ways: per-each, per-kW, per-kW-COP.  The program determines which method to use based on there being non-zero values in appropriate input fields.
-
-If **cost per each** is greater than 0.0 then the number of units, *N*, is the number of chillers.  This will be 1 if the **Item Name** is the name of a specific coil described elsewhere.  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-Each, *P<sub>e</sub>*:
-
-<div>$$L = N * {P_e}$$</div>
-
-If **Cost per kilowatt** is greater than 0.0 then the number of units, *N*, is the number of kilowatts of total, rated, cooling capacity for the specified chiller.  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-kilowatt, *P<sub>kW</sub>*:
-
-<div>$$L = N * {P_{kW}}$$</div>
-
-If **Cost per kilowatt per coefficient-of-performance** is greater than 0.0, then the number of units, *N*, is the number of kilowatts of total, rated, cooling capacity multiplied by the nominal coefficient of performance (COP) of the chiller.  This will be based on the named chiller (if set to a valid coil name).  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-kilowatt-per-COP, *P<sub>kW-COP</sub>*:
-
-<div>$$L = N * {P_{kW - COP}}$$</div>
-
-#### Daylighting:Controls
-
-The costs of controllers for harvesting daylight are determined by the number of reference points.  The cost for each controller, *P<sub>e</sub>* , are input.  The of units, *N*, is determined from the number of daylight reference points in all the zones if the **Item Name** is the wildcard (\*).  If **Item Name** is set to a valid Zone name then N is the number of daylight reference points in just that zone (zones can have more than one daylight controllers).  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-Each, *P<sub>e</sub>*:
-
-<div>$$L = N * {P_e}$$</div>
-
-#### Shading:Zone:Detailed
-
-Shading surfaces need to be handled separately because they do not have the **Construction** attribute.  The **Item Name** must be set to a valid name for a **Shading:Zone:Detailed** object defined elsewhere in the file.  The number of units, N, is determined from the area of the named surface multiplied by zone multiplier, *M<sub>Z</sub>*, and list multipliers, *M<sub>G</sub>*:
-
-<div>$$N = A*{M_Z} * {M_g}$$</div>
-
-The line item subtotal, *L*, is calculated by multiplying the number of units, *N* (m<sup>2</sup>) by the Cost-per-Area, *P<sub>a</sub>* , ($/m<sup>2</sup>):
-
-<div>$$L = N * {P_a}$$</div>
-
-#### Lights
-
-The cost of electric lighting systems can be modeled in two ways: per-each and per-kW.  The program determines which method to use based on there being non-zero values in appropriate input fields.  The **Item Name** must be the name of a valid Zone defined elsewhere in the input.
-
-If **cost per each** is greater than 0.0, then the number of units, *N*, is the number lighting systems in the zone and is assumed to be 1.  Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-Each, *P<sub>e</sub>*:
-
-<div>$$L = N * {P_e}$$</div>
-
-If **Cost per kilowatt** is greater than 0.0 then the number of units, *N*, is the number of kilowatts in the design level for electric lighting systems defined in Lights objects associated with the zone.  The **Item Name** must be the name of a valid Zone defined elsewhere in the input.  *N* is then the sum of all the Lights associated with the named Zone. Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-kilowatt, *P<sub>kW</sub>*:
-
-<div>$$L = N * {P_{kW}}$$</div>
-
-#### Generator:Photovoltaic
-
-The costs of simple photovoltaic power systems can be modeled using cost per kilowatt.  The number of units, N, is the nominal rated peak power of the photovoltaic panels.  The photovoltaic generator must be modeled using the PhotovoltaicPerformance:Simple input object which is a very simplistic model and does not include input for the nominal rated peak power of the system.  Therefore a peak power is calculated using the usual 1000 W/m<sup>2</sup> of incident solar radiation, *G<sub>p</sub>*, multiplied by the active solar cell area, *A* and the efficiency, *E*, and converted to units of kilowatts.
-
-<div>$$N = \frac{{{G_p} * A * E}}{{1000.0}}$$</div>
-
-Where, the cell area A is calculated by multiplying the area of the surface associated with the simple photovoltaic system and the active area fraction defined in the PhotovoltaicPerformance:Simple. Then the line item subtotal, *L*, is calculated by multiplying the number of units, *N*, by the Cost-per-kilowatt, *P<sub>kW</sub>*:
-
-<div>$$L = N * {P_{kW}}$$</div>
-
-### Adjustments
-
-Various adjustments are available to model total project costs from the component costs modeled using individual line items.  These adjustments are provided to allow propagating how changes in component costs are amplified by things like design fees, profit, bonding, and taxes.
-
-The subtotal of individual line items, *S<sub>L</sub>*, is obtained by summing all line item subtotals, *L*:
-
-<div>$${S_L} = \sum L $$</div>
-
-For the reference building, *S<sub>L,</sub>*is user input (typically from a prior run of baseline building model).
-
-The subtotal for miscellaneous construction costs (typically those costs not explicitly included as line items), *S<sub>m</sub>*, are calculated by multiplying the **Miscellaneous Cost Model** (per Square Meter), *C<sub>m</sub>*,  by the total conditioned floor area, *A<sub>c</sub>*:
-
-<div>$${S_m} = {A_c} * {C_m}$$</div>
-
-The subtotal for the amount that the construction costs should be altered because of regional differences in material and labor costs (e.g. when using national average data), *S<sub>r</sub>*, is determined by multiplying the Regional Adjustment Factor, *R<sub>f\\ ,</sub>* by the sum of *S<sub>L </sub>* and *S<sub>m:</sub>*
-
-<div>$${S_r} = ({S_L} + {S_m}){R_f}$$</div>
-
-Remaining adjustments are applied to the subtotal for construction costs, *S<sub>c</sub>*, which is the sum of *S<sub>L</sub>*, *S<sub>m,</sub>*, and *S<sub>r:</sub>*
-
-<div>$${S_C} = {S_L} + {S_m} + {S_r}$$</div>
-
-The **Design and Engineering Fee Fraction**,*F<sub>d</sub>*,is the fraction of construction costs, *S<sub>c</sub>*, attributable to costs associated with architectural and engineering services needed for the project.  The subtotal for costs associated with these fees, *S<sub>D</sub>*, are determined by multiplying *S<sub>C</sub>* by *F<sub>d</sub>*:
-
-<div>$${S_D} = {S_c}*{F_D}$$</div>
-
-The **Contractor Fee Fraction**,*F<sub>c</sub>*,is the fraction of construction costs, *S<sub>c</sub>*, attributable to costs associated with the contractor’s profit that should be included in the project.  The subtotal for costs associated with contracting, *S<sub>P</sub>*, are determined by multiplying *S<sub>C</sub>* by *F<sub>d</sub>*:
-
-<div>$${S_P} = {S_c}*{F_C}$$</div>
-
-The **Contingency Fraction**,*F<sub>S</sub>*,is the fraction of construction costs, *S<sub>c</sub>*, which should be included in a cost estimate to provide for contingencies (perhaps related to errors and uncertainty in the estimate and project).  The subtotal for contingency costs, *S<sub>S</sub>*, are determined by multiplying *S<sub>C</sub>* by *F<sub>S</sub>*:
-
-<div>$${S_S} = {S_c}*{F_S}$$</div>
-
-The **Permits, Bonding, Insurance Fraction,***F<sub>B</sub>*,is the fraction of construction costs, *S<sub>c</sub>*, which should be included in a cost estimate to provide for things like taxes, bonding, insurance, and permits.  The subtotal for these extra costs, *S<sub>B</sub>*, are determined by multiplying *S<sub>C</sub>* by *F<sub>B</sub>*:
-
-<div>$${S_B} = {S_c}*{F_B}$$</div>
-
-The **Commissioning Fee Fraction,***F<sub>CX</sub>*,is the fraction of construction costs, *S<sub>c</sub>*, which should be included in a cost estimate to provide for commissioning the building systems.  The subtotal for these extra costs, *S<sub>CX</sub>*, are determined by multiplying *S<sub>C</sub>* by *F<sub>CX</sub>*:
-
-<div>$${S_{CX}} = {S_c}*{F_{CX}}$$</div>
-
-Finally, the cost estimate total, *T*, is obtained by summing the various subtotals:
-
-<div>$$T = {S_L} + {S_m} + {S_r} + {S_D} + {S_P} + {S_S} + {S_B} + {S_{CX}}$$</div>
-
-The normalized total cost estimate, C, is calculated by dividing *T* by the total conditioned floor area, *A<sub>c</sub>*:
-
-<div>$$C = \frac{T}{{{A_C}}}$$</div>
-
-### Comparisons
-
-The capability of comparing the current cost estimate to that of a reference building is provided because is common to consider the marginal increases in costs associated with applying different energy design measures.  EnergyPlus calculates and reports the difference between the current model and a reference case for all the subtotals and totals discussed above.  The reported differences are the reference values subtracted from the current value.
-
-Tariff Computation
-------------------
-
-The EnergyPlus economic (Utility Costs) objects related to computing utility bills include:
-
-* UtilityCost:Tariff
-
-* UtilityCost:Qualify
-
-* UtilityCost:Charge:Simple
-
-* UtilityCost:Charge:Block
-
-* UtilityCost:Ratchet
-
-* UtilityCost:Variable
-
-* UtilityCost:Computation
-
-This section builds upon the discussion that appears in the Input Output Reference under the heading “EnergyPlus Economics.�  The actual computation of monthly utility bills is not difficult since it is mostly consists of multiplying energy consumptions or demands by the price on a per unit basis and adding different bill components.  The implementation in EnergyPlus becomes more complex since the objects were crafted to allow a great deal of  flexibility in specifying a utility tariff while, at the same time, being as simple as possible.
-
-The following discussion on variables and hierarchies is based on the text that appears in the Input Output Reference.
-
-### Conceptual Framework – Variables and Hierarchy
-
-To understand how to use the utility bill calculation portion of EnergyPlus you first need to understand some important concepts of variables and hierarchy.  A variable, for the purposes of this section, is simply a named holder of a series of numbers. In most cases, the variable will be a named holder of 12 numbers, one number for each monthly utility bill. Here is a visualization of a variable called Electric Energy Use:
-
-<table class="table table-striped">
-<tr>
-<th>Month</th>
-<th>Electric Energy Use</th>
-</tr>
-<tr>
-<td>January</td>
-<td>12143</td>
-</tr>
-<tr>
-<td>February</td>
-<td>13454</td>
-</tr>
-<tr>
-<td>March</td>
-<td>14178</td>
-</tr>
-<tr>
-<td>April</td>
-<td>14876</td>
-</tr>
-<tr>
-<td>May</td>
-<td>15343</td>
-</tr>
-<tr>
-<td>June</td>
-<td>16172</td>
-</tr>
-<tr>
-<td>July</td>
-<td>16105</td>
-</tr>
-<tr>
-<td>August</td>
-<td>15762</td>
-</tr>
-<tr>
-<td>September</td>
-<td>14543</td>
-</tr>
-<tr>
-<td>October</td>
-<td>13987</td>
-</tr>
-<tr>
-<td>November</td>
-<td>13287</td>
-</tr>
-<tr>
-<td>December</td>
-<td>12403</td>
-</tr>
-
-</table>
-
-If you have ever done any computer programming, you can think of a variable as an array.  Many of the names used in the utility bill calculation portion of EnergyPlus are names of variables.  In the case of the UtilityCost:Charge objects, the name of the object is also used as a name of a variable.
-
-In many of today’s utility rates, the charges for energy or demand are broken into distribution and supply charges.  To allow for this, more than one charge may to be defined for a particular category.  The variables assigned to the same category are added together.
-
-The categories are combined in following hierarchy:
-
-#### ![](media/image7909.png)
-
-Any charges included in the EnergyCharges category are added together. The EnergyCharges, DemandCharges and ServiceCharges are added together to form the Basis. The Basis, Adjustments and Surcharges are added together to form the Subtotal. The Subtotal and Taxes are added together to be the Total.  The total represents the total monthly charges on that tariff for the energy source used.  The combining of categories together is performed automatically unless the user specifies the UtilityCost:Computation.  In addition, each category, which is also a variable, may be used as a source. For example, a tax that is 5% of the subtotal would be shown as:
-
-```idf
-UtilityCost:Charge:Simple,
-  TaxOfFivePercent,        ! Charge Variable Name
-  TariffExample1,          ! Tariff Name
-  Subtotal,                ! Source Variable
-  Annual,                  ! Season
-  Taxes,                   ! Category Variable Name
-  0.05;                    ! Cost Per Unit Value (or Variable)
-```
-
-As you can see, the UtilityCost:Charge:Simple and UtilityCost:Charge:Block objects do most of the “work� of computing the annual energy cost.  The benefit of using this categorization is that totals of each category are shown in the output reports and it organizes the charges in the monthly calculations in a logical way that fits almost all tariffs.  If no categorization is desired, theoretically, all charges could be assigned to the Total category. The categories themselves are simply variable names. Charges may also be assigned to the “NotIncluded� category if the result of the charge is used as an intermediate calculation and should not be included in the Total.
-
-The objects that create variables are:
-
-* UtilityCost:Qualify
-
-* UtilityCost:Charge:Simple
-
-* UtilityCost:Charge:Block
-
-* UtilityCost:Ratchet
-
-* UtilityCost:Variable
-
-### Default Order of Computation
-
-The user has the option of two different ways to determine the order of computation. If an UtilityCost:Computation object is specified for the tariff, the sequence specified in that object is used for computing the various variables. If no UtilityCost:Computation object is specified, a sequence of computational steps is automatically derived and shown as part of the report. The routine that creates this automatic sequence of computation steps is called CreateDefaultComputation as part of the EconomicTariff module.
-
-The order in which the computation should be made is complicated by the fact that the objects can each have variables that are inputs and others that are outputs.  Since any of the variables can be used as inputs, we must ensure that they are computed prior to being used. In other words, because the objects allow a great deal of flexibility, there is no simple default order that the computations should be made.
-
-Luckily there are known algorithms for sorting though these types of interdependencies.  In fact, the method that spreadsheets use for sorting through the dependencies of cell formulas referencing other cells with formula is very similar.  In addition, linkers (used as part of the computer language compiling process) face similar issues of sorting through dependences. Figuring out the optimal path in a complex project represented by a PERT Chart also uses a similar algorithm.
-
-Generically, dependency problems are usually characterized as Directed Acycle Graphs (DAGs). A DAG shows the individual formulas as circles and uses arrows between the circles to show which formula is dependent on which other formulas.  One of the simplest explanations can be seen at the following website:
-
- (Click on lecture 14 “Critical Path�).
-
-The lecture and site was created by Alison Cawsey, Department of Computing and Electrical Engineering, Heriot-Watt University Edinburgh EH14 4AS, UK.  The specific algorithm that was used in EnergyPlus is described at this site and is quoted below:
-
-Calculate, for each node, the in-degree of that node (ie, now many edges end up there). Store these in array D.
-
-Repeat:
-
-– Remove (output) node such that D[n]=0.
-
-– Decrement D[x] for all nodes x that are neighbors of n (edge from n to x).
-
-Of course in this case “node� has nothing to do with EnergyPlus nodes but is just describing one of the formulas in a DAG.  This is just one of several different methods to solve a DAG.  The general method for solving a DAG is called a topological sort. The algorithm used in EnergyPlus is one of the simplest methods available and is appropriate given the number of dependencies.  More efficient algorithms are known but are probably only appropriate for much larger number of dependencies.
-
-One important note, if after the algorithm is exercised, and some of the formulas still have a count on the number of dependencies, it must be the result of a circular dependency and an error condition is flagged in the ERR file.
-
-The objects have specific variables that are used as inputs and outputs, and thus the outputs are dependent on the inputs, are shown in the following table:
-
-
-
-***Object Variables Inputs and Outputs***
-
-<table class="table table-striped">
-<tr>
-<th>Object</th>
-<th>Outputs</th>
-<th>Inputs</th>
-</tr>
-<tr>
-<td>Qualify</td>
-<td>Name</td>
-<td>Source</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>Threshold</td>
-</tr>
-<tr>
-<td>Charge:Simple</td>
-<td>Name</td>
-<td>Source</td>
-</tr>
-<tr>
-<td> </td>
-<td>Category</td>
-<td>Cost Per Unit</td>
-</tr>
-<tr>
-<td>Charge:Block</td>
-<td>Name</td>
-<td>Source</td>
-</tr>
-<tr>
-<td> </td>
-<td>Category</td>
-<td>Block Size Multiplier</td>
-</tr>
-<tr>
-<td> </td>
-<td>Remaining</td>
-<td>Block Size</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>Block Cost</td>
-</tr>
-<tr>
-<td>Ratchet</td>
-<td>Name</td>
-<td>Baseline</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>Adjustment</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>Multiplier</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>Offset</td>
-</tr>
-</table>
-
-
-
-In addition, the hierarchy shown in the first diagram in this section also represents dependencies that are included when determining the order of computation.
-
-The resulting order of computation is shown at the bottom of the economics report.
-
-### Computation Steps
-
-Once the order that the formulas should be computed is known, the actual evaluation of the formulas is based on a simple Last In First Out (LIFO) stack.  This is a common method to compute expressions where values are stored on the stack and operands work off of the top of the stack.
-
-Life-Cycle Cost Computations
-----------------------------
-
-The objects used for performing a life-cycle cost analysis are:
-
-* LifeCycleCost:Parameters
-
-* LifeCycleCost:RecurringCosts
-
-* LifeCycleCost:NonrecurringCost
-
-* LifeCycleCost:UsePriceEscalation
-
-* LifeCycleCost:UseAdjustment
-
-The computation of life-cycle costs is broken into three main routines which are described below.
-
-### ExpressAsCashFlows
-
-Step 1. If the input file has ComponentCost:\* items, then create an additional instance of a nonrecurring cost to hold the total.
-
-Step 2. Get the costs for each resource that has non-zero utility costs.
-
-Step 3. Compute the inflation on a monthly basis. For cases where the inflation approach is constant dollars, the inflation is set to 1.0 for all months. For current dollar analyses, compute the inflation rate on a monthly basis. Just using 1/12 of the annual inflation is almost correct but introduces a small error so instead the inverse of the formula 4-32 from Newnan (Engineering Economic Analysis Ninth Edition by Donald Newnan, Ted Eschenbach, and Jerome Lavelle):
-
-inflationPerMonth = ((inflation + 1.00) \*\* (1.0/12.0)) - 1
-
-Then the inflation is applied for each month:
-
-monthlyInflationFactor(jMonth) = (1 + inflationPerMonth) \*\* (jMonth - 1)
-
-Step 4. Put the nonrecurring, nonrecurring, and utility costs into a monthly array for the entire length of the study period.
-
-Step 5. Multiply the monthly costs by the monthly inflation which was set to 1.0 for constant dollar analyses.
-
-Step 6. Multiply the monthly costs for resources with use adjustments.
-
-Step 7. Sum the monthly costs by category.
-
-Step 8. Based on the base date, accumulate the monthly costs into yearly costs.
-
-### ComputePresentValue
-
-Step 1. For each year of the study compute the discount factor (SPV) using the following formula:
-
-SPV<sub>yr</sub> = 1 / ((1 + curDiscountRate) \*\* effectiveYear)
-
-This formula is based on formula D.2.1.1 from NIST Handbook 135 Life Cycle Costing Manual for the Federal Energy Management Program by Sieglinde K. Fuller and Stephen R. Petersen.
-
-Where the effectiveYear depends on the discount convention. If end of year discounting is used than the effectiveYear is the year. If middle of the year discounting is used than the effectiveYear is reduced by 0.5. If the beginning of year discounting is used, than the effectiveYear is reduced by 1.0.
-
-For energy costs, the use price escalations are multiplied by the discount factors.
-
-Step 2. Compute the present value for each month by multiply the monthly costs by the discount factor for each year.
-
-Step 3. Sum the costs by category.
-
-### ComputeTaxAndDepreciation
-
-Step 1. Depending on the depreciation method selected the depreciation factors are set to various constants. Depreciation factors are based on IRS Publication 946 for 2009 "How to Depreciate Property." The MACRS values are based on Modified Accelerated Cost Recovery System GDS for 3, 5, 7, 10 year property are based on 200% depreciation method shown in Appendix A of IRS Publication 946 using half year. 15 and 20 are based on 150% (Chart 1 of IRS Publication 946). For Straight Line depreciation GDS is used for 27 years (actually 27.5) 31 years (actually 31.5 years) and 39 years using mid month. For 40 years ADS is used (chart 2) Table A-1 is used for 3, 4, 5, 10, 15 and 20 years. Table A-6 is for 27 years. Table A-7 for 31 years. Table A-7a for 39 years. Table A-13 for 40 years. These years are a classification of property and should not be confused with the length of the study. For 27 years, 31 years, 39 years and 40 years the June value was used. All references in this paragraph are to IRS Publication 946.
-
-Step 2. Apply the annual depreciation factors to the capital costs.
-
-Step 3. For each year the taxable income is the grand total of all costs minus the depreciated capital costs.
-
-Step 4. Taxes are the taxable income times the tax rate.
-
-Step 5. The after tax present value is
-
-AfterTaxPresentValue<sub>yr</sub> = GrandTotal<sub>yr</sub> - Taxes<sub>yr</sub> \* SPV<sub>yr</sub>
-
-All major results are presented on the tabular report.
-
-
-
-
-
diff --git a/doc/src/docs/EngineeringReference/17-SpecialModulesReporting.md b/doc/src/docs/EngineeringReference/17-SpecialModulesReporting.md
deleted file mode 100644
index 44b178b8496..00000000000
--- a/doc/src/docs/EngineeringReference/17-SpecialModulesReporting.md
+++ /dev/null
@@ -1,2504 +0,0 @@
-Special Modules/Reporting
-=========================
-
-Environmental Impacts
----------------------
-
-Typically when a new building technology is evaluated the energy performance of a baseline building is compared to the energy and life-cycle costs of alternatives to determine cost-effectiveness. But what if the lowest energy or life-cycle cost alternative is not the cleanest or lowest environmental impact?  By calculating environmental impact, designers can compare alternatives not only in terms of their energy performance but also their environmental performance—working towards a more sustainable design (Liesen 1997; Stroot, Nemeth, and Fournier 1996).  Environmental impacts are quantified, in part, by modeling the amount of emissions and in EnergyPlus this is done using the input objects “EnvironmentalImpactFactors,� “FuelFactors,� and “Output:EnvironmentalImpactFactors.�
-
-Based on emissions factors entered by the user, EnergyPlus calculates the mass or volume of thirteen different pollutants: CO<sub>2</sub> (carbon dioxide), CO (carbon monoxide), CH<sub>4</sub> (methane), NO<sub>x</sub> (nitrogen oxides), N<sub>2</sub>O (nitrous oxide), SO<sub>2</sub> (sulphur dioxide), PM (particulate matter), PM<sub>10</sub> (particulate matter 10&gt;PM<sub>10</sub>&gt;2.5 microns), PM<sub>2.5</sub> (particulate matter&lt;2.5 microns), NH<sub>3</sub> (ammonia), NMVOC (non-methane volatile organic compounds), Hg (mercury), and Pb (lead) as well as water consumed through evaporation in thermo- and hydro-electric generation and high- and low-level nuclear waste from nuclear electricity generation for on- and off-site energy production.  Note that while these comprise the largest proportion of pollutants, more than one hundred other pollutants are emitted from fossil fuel combustion or electricity generation. Much of the information compiled here for fossil fuel combustion comes from *AP-42 Compilation of Air Pollutant Emission Factors* (EPA 1998a, 1998b, 1996).  For more information on pollutants, see the U.S. Environmental Protection Agency (EPA) Clearinghouse for Inventories & Emission Factors ([www.epa.gov/ttn/chief/efinformation.html](http://www.epa.gov/ttn/chief/efinformation.html)).
-
-EnergyPlus models energy performance of on-site fossil fuels and purchased electricity (generated from a variety of fuels including natural gas, oil, gasoline, diesel, coal, hydroelectric, nuclear, wind, solar power, and biomass).  The energy performance calculated by EnergyPlus is converted into a mass or volume of pollutants emitted.  From a baseline building, alternative energy and pollution saving technologies can be explored, and the energy savings and pollution reduction can be calculated.  Figure 341 and Figure 342 illustrate a comparison of two buildings simulated using Chicago weather data in EnergyPlus and the calculated pollutant levels (based on U.S. national average pollutants) (Crawley 2003).
-
-To calculate the mass or volume of each pollutant, consumption is multiplied by an emissions factor for each fuel (natural gas, electricity, fuel oil, diesel, or coal). In future versions, users will be able to schedule how the emissions factors by time of day, month, season and year.  For electricity, the mix of generation fuel sources—whether utility, state or regional—is used to adjust the emission factors.  If a user has emissions factors specific to the building site and equipment, these can be entered directly.  **There are no default emissions factors**.
-
-### Types of Pollutants
-
-EPA categorizes pollutants as either Criteria Pollutants or Hazardous Pollutants. Criteria pollutants are the six substances for which EPA has set health-based standards, including carbon monoxide (CO), nitrogen oxides (NO<sub>x</sub>), sulfur dioxide (SO<sub>2</sub>), and particulate matter (PM10 and PM2.5), ozone (O<sub>3</sub>), and lead (Pb).  Because ozone is created in atmospheric photochemical reactions of volatile organic compounds, ammonia, and other substances rather than direct building-related energy emissions, we do not calculated ozone emissions in EnergyPlus.  But we do include ozone precursors: methane (CH<sub>4</sub>), non-methane volatile organic compounds (NMVOC), and ammonia (NH<sub>3</sub>). Hazardous pollutants are substances that are known or suspected to cause serious health problems such as cancer.  We include typical hazardous substances associated with energy production and use including lead (Pb) and mercury (Hg). We also include CO<sub>2</sub> (carbon dioxide) since it is largest greenhouse gas in terms of impact.
-
-![](media/image7910.svg.png)
-
-Figure 341.  Example Annual Atmospheric Pollutants and Water Consumption
-
-![](media/image7911.svg.png)
-
-Figure 342.  Example Annual Total Carbon Equivalent for Major Greenhouse Gases
-
-### Carbon Equivalent
-
-The Intergovernmental Panel on Climate Change has studied the effects on the relative radiative forcing effects of various greenhouse gases.  This effect, called Global Warming Potential (GWP), is described in terms of the Carbon Equivalent of a particular greenhouse gas.  This equivalent is based on a factor of 1.0 for carbon.  This group of gases includes carbon dioxide (CO<sub>2</sub>), carbon monoxide, nitrous oxide, methane, halocarbon emission, hydrofluorocarbons (HFC), perfluorocarbons (PFC), and chlorofluorocarbons (CFC).  For building energy use, the main gases of concern are carbon dioxide, carbon monoxide, methane, and nitrous oxide.  Although carbon monoxide has a relatively short life, CO emissions into the atmosphere may have a significant impact on climate forcing due to chemical impact on CH<sub>4</sub> lifetime, and tropospheric O<sub>3</sub> and CO<sub>2</sub> photochemical production normally reacts to produce carbon dioxide, but it can’t be ignored since it is produced in incomplete combustion and the carbon remains to interact as CO<sub>2.</sub> Yet there is no agreement on its carbon equivalent (IPCC 2001). The carbon equivalent of carbon dioxide, methane, and nitrous oxide are calculated and then multiplied by their GWP on a 100 year time frame.  The Carbon Equivalents of the following gases have been determined and used in the program are shown in the following table.
-
-Table 93. Carbon Equivalents (IPCC 2001)
-
-<table class="table table-striped">
-<tr>
-<th>Gas</th>
-<th>Carbon Equivalent</th>
-</tr>
-<tr>
-<td>NO<sub>x</sub></td>
-<td>80.7272</td>
-</tr>
-<tr>
-<td>CH<sub>4</sub></td>
-<td>6.2727</td>
-</tr>
-<tr>
-<td>CO<sub>2</sub></td>
-<td>0.2727</td>
-</tr>
-</table>
-
-The resulting carbon equivalents by fuel type are shown in the output of the program along with the individual gas pollutants.
-
-### Fossil Fuel Emissions Factors
-
-Emission factors for on-site fossil fuel consumption are based on Section 1.4 Natural Gas Combustion in EPA (1998a) Table 94 shows the greenhouse gas and precursors and criteria pollutant emissions factors for natural gas.  Similar emissions factors are shown for residual fuel oil (No. 4 and No. 6 fuel oil) [Table 95], distillates (No. 1 and No. 2 fuel oil) [Table 96], residential oil furnace [Table 97], LPG (butane and propane) [Table 98], gasoline and diesel [Table 99], and coal [Table 100] in the indicated tables.  Note that a zero for a pollutant in the table may mean that no data were available, not that there are no emissions of that pollutant.
-
-Table 94.  Emission Factors for Natural Gas
-
-<table class="table table-striped">
-<tr>
-<th>Pollutant</th>
-<th>Emission Factor<sup>a</sup>   (g/MJ)</th>
-</tr>
-<tr>
-<td>Carbon Dioxide (CO<sub>2</sub>)</td>
-<td>50.23439</td>
-</tr>
-<tr>
-<td>Carbon Monoxide (CO)</td>
-<td>3.51641E-02</td>
-</tr>
-<tr>
-<td>Methane (CH<sub>4</sub>)</td>
-<td>9.62826E-04</td>
-</tr>
-<tr>
-<td>Nitrogen Oxides (NO<sub>X</sub>)</td>
-<td>4.18620E-02</td>
-</tr>
-<tr>
-<td>Nitrous Oxide (N<sub>2</sub>O)<sup>b</sup></td>
-<td>9.20964E-04</td>
-</tr>
-<tr>
-<td>Sulphur Dioxide (SO<sub>2</sub>)<sup>c</sup></td>
-<td>2.51172E-04</td>
-</tr>
-<tr>
-<td>Particulate Matter (PM)<sup>d</sup></td>
-<td>3.18151E-03</td>
-</tr>
-<tr>
-<td>Particulate Matter (PM10)<sup>d</sup></td>
-<td>2.38613E-03</td>
-</tr>
-<tr>
-<td>Particulate Matter (PM2.5)<sup>d</sup></td>
-<td>7.95378E-04</td>
-</tr>
-<tr>
-<td>Ammonia (NH<sub>3</sub>)</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Volatile Organic Compounds (NMVOC)</td>
-<td>2.30241E-03</td>
-</tr>
-<tr>
-<td>Mercury (Hg)</td>
-<td>1.08841E-07</td>
-</tr>
-<tr>
-<td>Lead (Pb)</td>
-<td>2.09310E-07</td>
-</tr>
-<tr>
-<td colspan="2">a Based on data from Tables 1.4-1, 1.4.-2 and 1.4.4  in EPA (1998a), Natural gas heat value of 1027 Btu/ft3 based on data for 2003 in Table A-4 in DOE (2004)</td>
-</tr>
-<tr>
-<td colspan="2">b Values shown are for uncontrolled burner.  For controlled-low NO<sub>X</sub> burner, use 0.64 lb/106 ft3, 0.000627 lb/MMBtu, 0.0002679 g/MJ</td>
-</tr>
-<tr>
-<td colspan="2">c Based on 100% conversion of fuel sulfur to SO<sub>2</sub>. Assumes sulfur content is natural gas of 2,000 grains/106 ft3. The SO2 emission factor can be converted to other natural gas sulfur contents by multiplying the SO<sub>2</sub> emission factor by the ratio of the site-specific sulfur content (grains/106 ft3) to 2,000 grains/106 ft3.</td>
-</tr>
-<tr>
-<td colspan="2">d PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively.</td>
-</tr>
-<tr>
-<td colspan="2">e No data</td>
-</tr>
-</table>
-
-Table 95.  Emission Factors for Residual Fuel Oil (No. 4 and No. 6 Fuel Oil)
-<table class="table table-striped">
-  <tr>
-    <th>Pollutant</th>
-    <th>Emission Factor <sup>a</sup> (g/MJ)</th>
-  </tr>
-  <tr>
-    <td>Carbon Dioxide (CO 2 )</td>
-    <td>50.23439</td>
-  </tr>
-  <tr>
-    <td>Carbon Monoxide (CO)</td>
-    <td>3.52E-002</td>
-  </tr>
-  <tr>
-    <td>Methane (CH 4 )</td>
-    <td>9.63E-004</td>
-  </tr>
-  <tr>
-    <td>Nitrogen Oxides (NO X )</td>
-    <td>4.19E-002</td>
-  </tr>
-  <tr>
-    <td>Nitrous Oxide (N 2 O) <sup>b</sup></td>
-    <td>9.21E-004</td>
-  </tr>
-  <tr>
-    <td>Sulphur Dioxide (SO 2 ) <sup>c</sup></td>
-    <td>2.51E-004</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM) <sup>d</sup></td>
-    <td>3.18E-003</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM10) <sup>d</sup></td>
-    <td>2.39E-003</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM2.5) <sup>d</sup></td>
-    <td>7.95E-004</td>
-  </tr>
-  <tr>
-    <td>Ammonia (NH 3 )</td>
-    <td>0 <sup>e</sup></td>
-  </tr>
-  <tr>
-    <td>Volatile Organic Compounds (NMVOC)</td>
-    <td>2.30E-003</td>
-  </tr>
-  <tr>
-    <td>Mercury (Hg)</td>
-    <td>1.09E-007</td>
-  </tr>
-  <tr>
-    <td>Lead (Pb)</td>
-    <td>2.09E-007</td>
-  </tr>
-  <tr>
-    <td colspan="2"><sup>a</sup> Based on data from Tables 1.4-1, 1.4.-2 and 1.4.4 in EPA (1998a), Natural gas heat value of 1027 Btu/ft3 based on data for 2003 in Table A-4 in DOE (2004)</td>
-  </tr>
-  <tr>
-    <td colspan="2"><sup>b</sup> Values shown are for uncontrolled burner. For controlled-low NOX burner, use 0.64 lb/106 ft3, 0.000627 lb/MMBtu, 0.0002679 g/MJ</td>
-  </tr>
-  <tr>
-    <td colspan="2"><sup>c</sup> Based on 100% conversion of fuel sulfur to SO2. Assumes sulfur content is natural gas of 2,000 contents by multiplying the SO2 emission factor by the ratio of the site-specific sulfur content (grains/106 ft3) to 2,000 grains/106 ft3. grains/106 ft3. The SO2 emission factor can be converted to other natural gas sulfur</td>
-  </tr>
-  <tr>
-    <td colspan="2"><sup>d</sup> PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively.</td>
-  </tr>
-  <tr>
-    <td colspan="2"><sup>e</sup> No data.</td>
-  </tr>
-</table>
-
-Table 96.  Emission Factors for Distillates (No. 1 and No. 2 Fuel Oil)
-
-<table class="table table-striped">
-  <tr>
-    <th>Pollutant</th>
-    <th>No. 1 Fuel Oil Emission Factor<sup>a</sup> (g/MJ)</th>
-    <th>No. 2 Fuel Oil Emission Factor<sup>a</sup> (g/MJ)</th>
-  </tr>
-  <tr>
-    <td>Carbon Dioxide (CO<sub>2</sub>)</td>
-    <td>66.0233</td>
-    <td>68.47998</td>
-  </tr>
-  <tr>
-    <td>Carbon Monoxide (CO)</td>
-    <td>1.54E-002</td>
-    <td>1.54E-002</td>
-  </tr>
-  <tr>
-    <td>Methane (CH<sub>4</sub>)</td>
-    <td>6.63E-004</td>
-    <td>6.63E-004</td>
-  </tr>
-  <tr>
-    <td>Nitrogen Oxides (NO<sub>X</sub>)</td>
-    <td>6.14E-002</td>
-    <td>7.37E-002</td>
-  </tr>
-  <tr>
-    <td>Nitrous Oxide (N<sub>2</sub>O)</td>
-    <td>3.38E-004</td>
-    <td>3.38E-004</td>
-  </tr>
-  <tr>
-    <td>Sulphur Dioxide (SO<sub>2</sub>)<sup>b</sup></td>
-    <td>4.36E-001</td>
-    <td>4.82E-001</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM)<sup>c</sup></td>
-    <td>6.14E-003</td>
-    <td>6.14E-003</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM10)<sup>c</sup></td>
-    <td>3.32E-003</td>
-    <td>3.32E-003</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM2.5)<sup>c</sup></td>
-    <td>2.55E-003</td>
-    <td>2.55E-003</td>
-  </tr>
-  <tr>
-    <td>Ammonia (NH<sub>3</sub>)</td>
-    <td>0<sup>d</sup></td>
-    <td>0<sup>d</sup></td>
-  </tr>
-  <tr>
-    <td>Volatile Organic Compounds (NMVOC)</td>
-    <td>1.04E-003</td>
-    <td>1.04E-003</td>
-  </tr>
-  <tr>
-    <td>Mercury (Hg)</td>
-    <td>3.47E-006</td>
-    <td>3.47E-006</td>
-  </tr>
-  <tr>
-    <td>Lead (Pb)</td>
-    <td>4.64E-006</td>
-    <td>4.64E-006</td>
-  </tr>
-  <tr>
-    <td>a Based on data from Tables 1.3-1, 1.3-3, 1-3.8, 1.3-10 and 1.3-12 in EPA (1998b).</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>b Based on 100% conversion of fuel sulfur to SO<sub>2</sub>. Assumes 1% sulfur content. The SO<sub>2</sub> emission factor in this table can be converted to other natural gas sulfur contents by multiplying the SO<sub>2</sub> emission factor by percentage sulfur content.</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>c PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>d No data.</td>
-    <td></td>
-    <td></td>
-  </tr>
-</table>
-
-
-Table 97.  Emission Factors for Residential Oil Furnace
-
-<table class="table table-striped">
-<tr>
-<th>Pollutant</th>
-<th>Emission Factor<sup>a</sup>   (g/MJ)</th>
-</tr>
-<tr>
-<td>Carbon Dioxide (CO<sub>2</sub>)</td>
-<td>68.48237</td>
-</tr>
-<tr>
-<td>Carbon Monoxide (CO)</td>
-<td>1.53543E-02</td>
-</tr>
-<tr>
-<td>Methane (CH<sub>4</sub>)</td>
-<td>5.46612E-02</td>
-</tr>
-<tr>
-<td>Nitrogen Oxides (NO<sub>X</sub>)</td>
-<td>5.52753E-02</td>
-</tr>
-<tr>
-<td>Nitrous Oxide (N<sub>2</sub>O)</td>
-<td>1.53543E-04</td>
-</tr>
-<tr>
-<td>Sulphur Dioxide (SO<sub>2</sub>)<sup>b</sup></td>
-<td>4.36061E-01</td>
-</tr>
-<tr>
-<td>Particulate Matter (PM)<sup>c</sup></td>
-<td>2.14960E-02</td>
-</tr>
-<tr>
-<td>Particulate Matter (PM10)<sup>c</sup></td>
-<td>1.58763E-02</td>
-</tr>
-<tr>
-<td>Particulate Matter (PM2.5)<sup>c</sup></td>
-<td>5.89603E-03</td>
-</tr>
-<tr>
-<td>Ammonia (NH<sub>3</sub>)</td>
-<td>0<sup>d</sup></td>
-</tr>
-<tr>
-<td>Volatile Organic Compounds (NMVOC)</td>
-<td>2.18952E-03</td>
-</tr>
-<tr>
-<td>Mercury (Hg)</td>
-<td>3.47006E-06</td>
-</tr>
-<tr>
-<td>Lead (Pb)</td>
-<td>4.63699E-06</td>
-</tr>
-<tr>
- <td colspan="2">a Based on data from Tables 1.3-1, 1.3-3, 1.3-8, 1.3-10, and 1.3-12 in EPA (1998b).</td>
-</tr>
-<tr>
- <td colspan="2">b Based on 100% conversion of fuel sulfur to SO<sub>2</sub>. Assumes 1% sulfur content. The SO<sub>2</sub> emission factor in this table can be converted to other natural gas sulfur contents by multiplying the SO<sub>2</sub> emission factor by percentage sulfur content.</td>
-</tr>
-<tr>
- <td colspan="2">c PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively.</td>
-</tr>
-<tr>
- <td colspan="2">d No data.</td>
-</tr>
-</table>
-
-Table 98.  Emission Factors for LPG (butane and propane)
-
-<table class="table table-striped">
-  <tr>
-    <th>Pollutant</th>
-    <th>LPG (butane) Emission Factor <sup>a</sup> (g/MJ)</th>
-    <th>Propane Emission Factor <sup>a</sup> (g/MJ)</th>
-  </tr>
-  <tr>
-    <td>Carbon Dioxide (CO<sub>2</sub>)</td>
-    <td>66.0233</td>
-    <td>68.47998</td>
-  </tr>
-  <tr>
-    <td>Carbon Monoxide (CO)</td>
-    <td>1.54E-002</td>
-    <td>1.54E-002</td>
-  </tr>
-  <tr>
-    <td>Methane (CH<sub>4</sub>)</td>
-    <td>6.63E-004</td>
-    <td>6.63E-004</td>
-  </tr>
-  <tr>
-    <td>Nitrogen Oxides (NO<sub>X</sub>)</td>
-    <td>6.14E-002</td>
-    <td>7.37E-002</td>
-  </tr>
-  <tr>
-    <td>Nitrous Oxide (N<sub>2</sub>O)</td>
-    <td>3.38E-004</td>
-    <td>3.38E-004</td>
-  </tr>
-  <tr>
-    <td>Sulphur Dioxide (SO<sub>2</sub>)<sup>b</sup></td>
-    <td>4.36E-001</td>
-    <td>4.82E-001</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM)<sup>c</sup></td>
-    <td>6.14E-003</td>
-    <td>6.14E-003</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM10)<sup>c</sup></td>
-    <td>3.32E-003</td>
-    <td>3.32E-003</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM2.5)<sup>c</sup></td>
-    <td>2.55E-003</td>
-    <td>2.55E-003</td>
-  </tr>
-  <tr>
-    <td>Ammonia (NH<sub>3</sub>)</td>
-    <td>0<sup>d</sup></td>
-    <td>0<sup>d</sup></td>
-  </tr>
-  <tr>
-    <td>Volatile Organic Compounds (NMVOC)</td>
-    <td>1.04E-003</td>
-    <td>1.04E-003</td>
-  </tr>
-  <tr>
-    <td>Mercury (Hg)</td>
-    <td>3.47E-006</td>
-    <td>3.47E-006</td>
-  </tr>
-  <tr>
-    <td>Lead (Pb)</td>
-    <td>4.64E-006</td>
-    <td>4.64E-006</td>
-  </tr>
-  <tr>
-    <td colspan="3">a Based on data from Table # 1.5-1 in EPA (1996); Higher Heating value of 1.02 MMBtu/gal for butane and 0.915 MMBtu/gal for propane based on data in EPA (1996).</td>
-  </tr>
-  <tr>
-    <td colspan="3">b Based on 100% conversion of fuel sulfur to SO<sub>2</sub>. Assumes sulphur content is 0.18 gr/100 ft3.The SO<sub>2</sub> emission factor can be converted to other LPG sulphur contents by multiplying the SO<sub>2</sub> emission factor by the ratio of the site-specific sulphur content gr/100 ft3 to 0.18 gr/100 ft3.</td>
-  </tr>
-  <tr>
-    <td colspan="3">c PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns; respectively.</td>
-  </tr>
-  <tr>
-    <td colspan="3">d No data.</td>
-  </tr>
-</table>
-
-Table 99.  Emission Factors for Gasoline and Diesel
-
-<table class="table table-striped">
-  <tr>
-    <th>Pollutant</th>
-    <th>Gasoline Emission Factor<sup>a</sup> (g/MJ)</th>
-    <th>Diesel Emission Factor<sup>a</sup> (g/MJ)</th>
-  </tr>
-  <tr>
-    <td>Carbon Dioxide (CO<sub>2</sub>)</td>
-    <td>66.20808</td>
-    <td>70.50731</td>
-  </tr>
-  <tr>
-    <td>Carbon Monoxide (CO)</td>
-    <td>2.70E+001</td>
-    <td>4.08E-001</td>
-  </tr>
-  <tr>
-    <td>Methane (CH<sub>4</sub>)</td>
-    <td>0<sup>c</sup></td>
-    <td>0<sup>c</sup></td>
-  </tr>
-  <tr>
-    <td>Nitrogen Oxides (NO<sub>X</sub>)</td>
-    <td>7.01E-001</td>
-    <td>1.90E+000</td>
-  </tr>
-  <tr>
-    <td>Nitrous Oxide (N<sub>2</sub>O)</td>
-    <td>0<sup>c</sup></td>
-    <td>0<sup>c</sup></td>
-  </tr>
-  <tr>
-    <td>Sulphur Dioxide (SO<sub>2</sub>)</td>
-    <td>3.61E-002</td>
-    <td>1.25E-001</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM)<sup>b</sup></td>
-    <td>0<sup>c</sup></td>
-    <td>0<sup>c</sup></td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM10)<sup>b</sup></td>
-    <td>4.30E-002</td>
-    <td>1.33E-001</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM2.5)<sup>b</sup></td>
-    <td>0<sup>c</sup></td>
-    <td>0<sup>c</sup></td>
-  </tr>
-  <tr>
-    <td>Ammonia (NH<sub>3</sub>)</td>
-    <td>0<sup>c</sup></td>
-    <td>0<sup>c</sup></td>
-  </tr>
-  <tr>
-    <td>Volatile Organic Compounds (NMVOC)</td>
-    <td>9.03E-001</td>
-    <td>1.50E-001</td>
-  </tr>
-  <tr>
-    <td>Mercury (Hg)</td>
-    <td>0<sup>c</sup></td>
-    <td>0<sup>c</sup></td>
-  </tr>
-  <tr>
-    <td>Lead (Pb)</td>
-    <td>0<sup>c</sup></td>
-    <td>0<sup>c</sup></td>
-  </tr>
-  <tr>
-    <td colspan="3">a Based on data from Table # 3.3-1 in EPA (1996); Diesel higher heating value of 19300 Btu/lb and gasoline higher heating value of 20300 Btu/lb based on data in EPA (1996).</td>
-  </tr>
-  <tr>
-    <td colspan="3">b PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns; respectively.</td>
-  </tr>
-  <tr>
-    <td colspan="3">c No data.</td>
-  </tr>
-</table>
-
-
-Table 100.  Emission Factors for Coal
-
-<table class="table table-striped">
-  <tr>
-    <th>Pollutant</th>
-    <th>Bituminous Emission Factor<sup>a</sup> (g/MJ)</th>
-    <th>Anthracite Emission Factor<sup>a</sup> (g/MJ)</th>
-    <th>Lignite Emission Factor<sup>a</sup> (g/MJ)</th>
-  </tr>
-  <tr>
-    <td>Carbon Dioxide (CO<sub>2</sub>)</td>
-    <td>91.11052</td>
-    <td>99.26669</td>
-    <td>152.12646</td>
-  </tr>
-  <tr>
-    <td>Carbon Monoxide (CO)</td>
-    <td>8.27E-003</td>
-    <td>1.05E-002</td>
-    <td>8.27E-003</td>
-  </tr>
-  <tr>
-    <td>Methane (CH<sub>4</sub>)</td>
-    <td>6.61E-004</td>
-    <td>0<sup>f</sup></td>
-    <td>0<sup>f</sup></td>
-  </tr>
-  <tr>
-    <td>Nitrogen Oxides (NO<sub>X</sub>)</td>
-    <td>1.98E-001</td>
-    <td>3.15E-001</td>
-    <td>2.35E-001</td>
-  </tr>
-  <tr>
-    <td>Nitrous Oxide (N<sub>2</sub>O)</td>
-    <td>4.96E-004</td>
-    <td>0<sup>f</sup></td>
-    <td>0<sup>f</sup></td>
-  </tr>
-  <tr>
-    <td>Sulphur Dioxide (SO<sub>2</sub>)<sup>d</sup></td>
-    <td>6.28E-001</td>
-    <td>6.82E-001</td>
-    <td>9.92E-001</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM)<sup>e</sup></td>
-    <td>1.65E-001</td>
-    <td>1.75E-001</td>
-    <td>2.18E-001</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM10)<sup>e</sup></td>
-    <td>3.80E-002</td>
-    <td>4.02E-002</td>
-    <td>7.61E-002</td>
-  </tr>
-  <tr>
-    <td>Particulate Matter (PM2.5)<sup>e</sup></td>
-    <td>9.92E-003</td>
-    <td>1.05E-002</td>
-    <td>2.18E-002</td>
-  </tr>
-  <tr>
-    <td>Ammonia (NH<sub>3</sub>)</td>
-    <td>0<sup>f</sup></td>
-    <td>0<sup>f</sup></td>
-    <td>0<sup>f</sup></td>
-  </tr>
-  <tr>
-    <td>Volatile Organic Compounds (NMVOC)</td>
-    <td>9.92E-004</td>
-    <td>2.15E-002</td>
-    <td>1.32E-003</td>
-  </tr>
-  <tr>
-    <td>Mercury (Hg)</td>
-    <td>6.94E-006</td>
-    <td>2.27E-006</td>
-    <td>2.74E-006</td>
-  </tr>
-  <tr>
-    <td>Lead (Pb)</td>
-    <td>1.37E-006</td>
-    <td>1.56E-004</td>
-    <td>1.39E-005</td>
-  </tr>
-  <tr>
-    <td colspan="4">a Based on data on pulverized coal from Tables 1.1-3, 1.1-6, 1.1-18, 1.1-19 in EPA (1998a), Coal average higher heating value of 26.0 MMBtu/ton based on EPA (1998a).</td>
-  </tr>
-  <tr>
-    <td colspan="4">b Based on data on pulverized coal from Tables 1.2-1, 1.2-2, 1.2-3, 1.2-4, 1.2-7 in EPA (1996), Coal average higher heating value of 24.6 MMBtu/ton based on EPA (1996).</td>
-  </tr>
-  <tr>
-    <td colspan="4">c Based on data on pulverized coal from Tables 1.7-1, 1.7-3, 1.7-7, 1.7-14 in EPA (1998b), Coal average higher heating value of 13.0 MMBtu/ton based on EPA (1998b).</td>
-  </tr>
-  <tr>
-    <td colspan="4">d Based on 100% conversion of fuel sulfur to SO<sub>2</sub>. Assumes 1% sulfur content. The SO<sub>2</sub> emission factor in this table can be converted to other natural gas sulfur contents by multiplying the SO<sub>2</sub> emission factor by percentage sulfur content.</td>
-  </tr>
-  <tr>
-    <td colspan="4">e PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 are particles smaller than 10 and 2.5 microns, respectively. Expressed in terms of coal ash content, assumes 1% ash content.  Multiply weight % ash content of coal (as fired) by the value.</td>
-  </tr>
-  <tr>
-    <td colspan="4">f No data.</td>
-  </tr>
-</table>
-
-### Off-Site Electricity Generation Emissions
-
-While estimating emissions from on-site fossil fuel combustion can be fairly straight-forward, emissions from off-site electricity is more challenging.  How the electricity is generated, i.e., from gas, oil, coal, nuclear, renewable sources (wind, PV) or hydroelectric, and the mix of generation determines the resulting level of emissions.  While data are available at utility and even power plant level (from the sources cited), data are shown here for United States national- and state-level average emissions from electricity generation. Table 101 provides average greenhouse gas and precursors and criteria pollutant emissions factors for the entire United States from electricity generation. Table 102 provides average electricity emissions factors by state, for greenhouse gas and precursors, and Table 103 for criteria pollutant emission factors. These two tables also include a ratio of heat input to electric output (efficiency of electricity generation) including distribution and transmission losses to allow calculation of source energy.
-
-As mentioned in the introduction to this section, EnergyPlus also calculates water consumed through evaporation in thermo-electric and hydro-electric generation. Torcellini, Long, and Judkoff (2004) provide data on average water consumption by generator type by state.  These data are summarized in units suitable for EnergyPlus in Table 101, for national and state average water consumption for thermal-electric, hydro-electric, and Table 102 for weighted total electricity generation.
-
-Table 101.  United States National Average Emission Factors for Electricity Generation
-
-<table class="table table-striped">
-<tr>
-<td> </td>
-<th>Efficiency Ratio (J/J)</th>
-</tr>
-<tr>
-<td>Ratio of Heat Input to Electricity Output<sup>a</sup></td>
-<td>2.253</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<th>Pollutant</th>
-<th>Emission Factor   (g/MJ)</th>
-</tr>
-<tr>
-<td>Carbon Dioxide (CO<sub>2</sub>)<sup>b</sup></td>
-<td>168.333168</td>
-</tr>
-<tr>
-<td>Carbon Monoxide (CO)<sup>c</sup></td>
-<td>4.20616E-02</td>
-</tr>
-<tr>
-<td>Methane (CH<sub>4</sub>)<sup>b</sup></td>
-<td>1.39858E-03</td>
-</tr>
-<tr>
-<td>Nitrogen Oxides (NO<sub>X</sub>)<sup>a</sup></td>
-<td>4.10753E-01</td>
-</tr>
-<tr>
-<td>Nitrous Oxide (N<sub>2</sub>O)<sup>b</sup></td>
-<td>2.41916E-03</td>
-</tr>
-<tr>
-<td>Sulphur Dioxide (SO<sub>2</sub>)<sup>a</sup></td>
-<td>8.65731E-01</td>
-</tr>
-<tr>
-<td>Particulate Matter (PM)<sup>c,d</sup></td>
-<td>2.95827E-02</td>
-</tr>
-<tr>
-<td>Particulate Matter (PM10)<sup>c,d</sup></td>
-<td>1.80450E-02</td>
-</tr>
-<tr>
-<td>Particulate Matter (PM2.5)<sup>c,d</sup></td>
-<td>1.15377E-02</td>
-</tr>
-<tr>
-<td>Ammonia (NH<sub>3</sub>)<sup>c</sup></td>
-<td>1.10837E-03</td>
-</tr>
-<tr>
-<td>Volatile Organic Compounds (NMVOC)<sup>a</sup></td>
-<td>3.72332E-03</td>
-</tr>
-<tr>
-<td>Mercury (Hg)<sup>c</sup></td>
-<td>3.36414E-06</td>
-</tr>
-<tr>
-<td>Lead (Pb)</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
- <td colspan="2"><sup>a</sup> Data based on 1999 data from *eGRID* version 2.01 (EPA 2003a).</td>
-</tr>
-<tr>
- <td colspan="2"><sup>b</sup> Data based on 1998-2000 average data in DOE (2002).</td>
-</tr>
-<tr>
- <td colspan="2"><sup>c</sup> Data based on tier emissions report for criteria air pollutants in EPA (2003b).</td>
-</tr>
-<tr>
- <td colspan="2"><sup>d</sup> PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively.</td>
-</tr>
-<tr>
- <td colspan="2"><sup>e</sup> No data.</td>
-</tr>
-</table>
-
-Table 102.  U. S. State Average Greenhouse Gas Emission Factors for Electricity Generation, in g/MJ
-
-<table class="table table-striped">
-  <tr>
-    <th></th>
-    <th>Ratio of Heat Input to Electric Output</th>
-    <th>Carbon Dioxide (CO 2 ) b</th>
-    <th>Carbon Monoxide (CO) c</th>
-    <th>Methane (CH4) b</th>
-    <th>Nitrogen Oxides (NO X ) a</th>
-    <th>Nitrous Oxide (N 2 O) b</th>
-    <th>Sulphur Dioxide (SO 2 ) a</th>
-  </tr>
-  <tr>
-    <td>Alabama</td>
-    <td>2.23</td>
-    <td>165.30922</td>
-    <td>1.45E+003</td>
-    <td>1.73E-003</td>
-    <td>4.02E-001</td>
-    <td>2.81E-003</td>
-    <td>1.14E+000</td>
-  </tr>
-  <tr>
-    <td>Alaska</td>
-    <td>2.734</td>
-    <td>173.87708</td>
-    <td>3.72E+002</td>
-    <td>8.57E-004</td>
-    <td>7.29E-001</td>
-    <td>1.12E-003</td>
-    <td>2.38E-001</td>
-  </tr>
-  <tr>
-    <td>Arizona</td>
-    <td>1.694</td>
-    <td>132.29777</td>
-    <td>8.27E+002</td>
-    <td>8.57E-004</td>
-    <td>2.74E-001</td>
-    <td>1.94E-003</td>
-    <td>2.28E-001</td>
-  </tr>
-  <tr>
-    <td>Arkansas</td>
-    <td>2.207</td>
-    <td>162.03327</td>
-    <td>6.42E+002</td>
-    <td>1.57E-003</td>
-    <td>2.87E-001</td>
-    <td>2.56E-003</td>
-    <td>4.25E-001</td>
-  </tr>
-  <tr>
-    <td>California</td>
-    <td>1.422</td>
-    <td>76.35472</td>
-    <td>2.91E+003</td>
-    <td>8.44E-004</td>
-    <td>6.56E-002</td>
-    <td>4.66E-004</td>
-    <td>3.05E-002</td>
-  </tr>
-  <tr>
-    <td>Colorado</td>
-    <td>3.101</td>
-    <td>242.67192</td>
-    <td>1.51E+003</td>
-    <td>1.60E-003</td>
-    <td>4.74E-001</td>
-    <td>3.64E-003</td>
-    <td>5.84E-001</td>
-  </tr>
-  <tr>
-    <td>Connecticut</td>
-    <td>1.72</td>
-    <td>118.69</td>
-    <td>3.21E+002</td>
-    <td>2.19E-003</td>
-    <td>1.82E-001</td>
-    <td>1.51E-003</td>
-    <td>3.79E-001</td>
-  </tr>
-  <tr>
-    <td>Delaware</td>
-    <td>2.736</td>
-    <td>230.57612</td>
-    <td>1.31E+002</td>
-    <td>1.55E-003</td>
-    <td>4.13E-001</td>
-    <td>2.86E-003</td>
-    <td>1.11E+000</td>
-  </tr>
-  <tr>
-    <td>District of Columbia</td>
-    <td>4.844</td>
-    <td>172.1131</td>
-    <td>8.95E+000</td>
-    <td>1.49E-003</td>
-    <td>7.30E-001</td>
-    <td>2.60E-003</td>
-    <td>1.62E+000</td>
-  </tr>
-  <tr>
-    <td>Florida</td>
-    <td>2.694</td>
-    <td>175.64105</td>
-    <td>6.13E+003</td>
-    <td>1.89E-003</td>
-    <td>4.73E-001</td>
-    <td>2.27E-003</td>
-    <td>1.01E+000</td>
-  </tr>
-  <tr>
-    <td>Georgia</td>
-    <td>2.119</td>
-    <td>172.1131</td>
-    <td>1.06E+003</td>
-    <td>1.63E-003</td>
-    <td>4.00E-001</td>
-    <td>2.85E-003</td>
-    <td>1.12E+000</td>
-  </tr>
-  <tr>
-    <td>Hawaii</td>
-    <td>2.95</td>
-    <td>209.40848</td>
-    <td>1.18E+002</td>
-    <td>2.70E-003</td>
-    <td>7.28E-001</td>
-    <td>2.31E-003</td>
-    <td>5.44E-001</td>
-  </tr>
-  <tr>
-    <td>Idaho</td>
-    <td>0.213</td>
-    <td>3.52794</td>
-    <td>0</td>
-    <td>1.01E-003</td>
-    <td>1.07E-002</td>
-    <td>4.16E-004</td>
-    <td>1.06E-002</td>
-  </tr>
-  <tr>
-    <td>Illinois</td>
-    <td>1.694</td>
-    <td>146.66153</td>
-    <td>1.85E+003</td>
-    <td>1.03E-003</td>
-    <td>4.42E-001</td>
-    <td>2.27E-003</td>
-    <td>1.12E+000</td>
-  </tr>
-  <tr>
-    <td>Indiana</td>
-    <td>3.281</td>
-    <td>261.5716</td>
-    <td>2.14E+003</td>
-    <td>1.80E-003</td>
-    <td>7.30E-001</td>
-    <td>4.07E-003</td>
-    <td>1.89E+000</td>
-  </tr>
-  <tr>
-    <td>Iowa</td>
-    <td>3.033</td>
-    <td>237.12801</td>
-    <td>7.58E+002</td>
-    <td>1.74E-003</td>
-    <td>5.61E-001</td>
-    <td>3.75E-003</td>
-    <td>1.05E+000</td>
-  </tr>
-  <tr>
-    <td>Kansas</td>
-    <td>2.826</td>
-    <td>212.18043</td>
-    <td>8.66E+002</td>
-    <td>1.41E-003</td>
-    <td>5.59E-001</td>
-    <td>3.20E-003</td>
-    <td>7.07E-001</td>
-  </tr>
-  <tr>
-    <td>Kentucky</td>
-    <td>3.234</td>
-    <td>253.00374</td>
-    <td>1.51E+003</td>
-    <td>1.76E-003</td>
-    <td>8.41E-001</td>
-    <td>4.04E-003</td>
-    <td>1.79E+000</td>
-  </tr>
-  <tr>
-    <td>Lousiana</td>
-    <td>2.624</td>
-    <td>148.4255</td>
-    <td>1.68E+004</td>
-    <td>1.18E-003</td>
-    <td>3.42E-001</td>
-    <td>1.41E-003</td>
-    <td>5.06E-001</td>
-  </tr>
-  <tr>
-    <td>Maine</td>
-    <td>2.191</td>
-    <td>107.35019</td>
-    <td>4.93E+002</td>
-    <td>7.12E-003</td>
-    <td>1.80E-001</td>
-    <td>3.40E-003</td>
-    <td>4.04E-001</td>
-  </tr>
-  <tr>
-    <td>Maryland</td>
-    <td>2.277</td>
-    <td>172.1131</td>
-    <td>4.90E+002</td>
-    <td>1.49E-003</td>
-    <td>5.38E-001</td>
-    <td>2.60E-003</td>
-    <td>1.39E+000</td>
-  </tr>
-  <tr>
-    <td>Massachusetts</td>
-    <td>2.729</td>
-    <td>161.02529</td>
-    <td>7.89E+002</td>
-    <td>2.19E-003</td>
-    <td>2.89E-001</td>
-    <td>2.00E-003</td>
-    <td>8.01E-001</td>
-  </tr>
-  <tr>
-    <td>Michigan</td>
-    <td>2.616</td>
-    <td>199.07665</td>
-    <td>1.69E+003</td>
-    <td>1.84E-003</td>
-    <td>4.92E-001</td>
-    <td>3.15E-003</td>
-    <td>9.77E-001</td>
-  </tr>
-  <tr>
-    <td>Minnesota</td>
-    <td>2.331</td>
-    <td>163.04126</td>
-    <td>6.96E+002</td>
-    <td>1.66E-003</td>
-    <td>5.02E-001</td>
-    <td>2.08E-003</td>
-    <td>5.07E-001</td>
-  </tr>
-  <tr>
-    <td>Mississippi</td>
-    <td>2.404</td>
-    <td>231.8361</td>
-    <td>2.18E+003</td>
-    <td>1.59E-003</td>
-    <td>4.67E-001</td>
-    <td>3.63E-003</td>
-    <td>8.98E-001</td>
-  </tr>
-  <tr>
-    <td>Missouri</td>
-    <td>2.857</td>
-    <td>192.02077</td>
-    <td>1.30E+003</td>
-    <td>1.98E-003</td>
-    <td>6.42E-001</td>
-    <td>3.11E-003</td>
-    <td>9.07E-001</td>
-  </tr>
-  <tr>
-    <td>Montana</td>
-    <td>1.936</td>
-    <td>180.68096</td>
-    <td>4.13E+002</td>
-    <td>1.36E-003</td>
-    <td>3.58E-001</td>
-    <td>2.86E-003</td>
-    <td>2.01E-001</td>
-  </tr>
-  <tr>
-    <td>Nebraska</td>
-    <td>2.195</td>
-    <td>176.39703</td>
-    <td>4.68E+002</td>
-    <td>1.20E-003</td>
-    <td>3.94E-001</td>
-    <td>2.76E-003</td>
-    <td>5.29E-001</td>
-  </tr>
-  <tr>
-    <td>Nevada</td>
-    <td>2.615</td>
-    <td>191.26478</td>
-    <td>3.82E+002</td>
-    <td>1.13E-003</td>
-    <td>4.02E-001</td>
-    <td>2.46E-003</td>
-    <td>4.03E-001</td>
-  </tr>
-  <tr>
-    <td>New Hampshire</td>
-    <td>1.394</td>
-    <td>85.93055</td>
-    <td>2.64E+002</td>
-    <td>2.17E-003</td>
-    <td>2.03E-001</td>
-    <td>1.78E-003</td>
-    <td>8.71E-001</td>
-  </tr>
-  <tr>
-    <td>New Jersey</td>
-    <td>1.451</td>
-    <td>88.9545</td>
-    <td>2.27E+003</td>
-    <td>9.70E-004</td>
-    <td>1.77E-001</td>
-    <td>9.95E-004</td>
-    <td>2.31E-001</td>
-  </tr>
-  <tr>
-    <td>New Mexico</td>
-    <td>3.307</td>
-    <td>254.26372</td>
-    <td>8.56E+002</td>
-    <td>1.65E-003</td>
-    <td>6.58E-001</td>
-    <td>3.73E-003</td>
-    <td>5.70E-001</td>
-  </tr>
-  <tr>
-    <td>New York</td>
-    <td>1.808</td>
-    <td>108.10618</td>
-    <td>1.94E+003</td>
-    <td>1.02E-003</td>
-    <td>1.69E-001</td>
-    <td>1.12E-003</td>
-    <td>4.68E-001</td>
-  </tr>
-  <tr>
-    <td>North Carolina</td>
-    <td>1.969</td>
-    <td>156.48937</td>
-    <td>1.10E+003</td>
-    <td>1.32E-003</td>
-    <td>4.69E-001</td>
-    <td>2.56E-003</td>
-    <td>1.00E+000</td>
-  </tr>
-  <tr>
-    <td>North Dakota</td>
-    <td>3.244</td>
-    <td>282.48725</td>
-    <td>9.01E+002</td>
-    <td>1.85E-003</td>
-    <td>6.45E-001</td>
-    <td>4.27E-003</td>
-    <td>1.53E+000</td>
-  </tr>
-  <tr>
-    <td>Ohio</td>
-    <td>2.736</td>
-    <td>226.79619</td>
-    <td>1.59E+003</td>
-    <td>1.64E-003</td>
-    <td>7.68E-001</td>
-    <td>3.63E-003</td>
-    <td>2.34E+000</td>
-  </tr>
-  <tr>
-    <td>Oklahoma</td>
-    <td>3.024</td>
-    <td>216.96835</td>
-    <td>1.67E+003</td>
-    <td>1.39E-003</td>
-    <td>5.11E-001</td>
-    <td>2.81E-003</td>
-    <td>5.11E-001</td>
-  </tr>
-  <tr>
-    <td>Oregon</td>
-    <td>0.526</td>
-    <td>35.5314</td>
-    <td>1.87E+002</td>
-    <td>4.16E-004</td>
-    <td>5.27E-002</td>
-    <td>4.28E-004</td>
-    <td>7.51E-002</td>
-  </tr>
-  <tr>
-    <td>Pennsylvania</td>
-    <td>1.827</td>
-    <td>159.26132</td>
-    <td>1.86E+003</td>
-    <td>1.35E-003</td>
-    <td>3.29E-001</td>
-    <td>2.56E-003</td>
-    <td>1.26E+000</td>
-  </tr>
-  <tr>
-    <td>Rhode Island</td>
-    <td>2.561</td>
-    <td>132.54977</td>
-    <td>1.68E+002</td>
-    <td>8.57E-004</td>
-    <td>6.21E-002</td>
-    <td>5.92E-004</td>
-    <td>4.54E-003</td>
-  </tr>
-  <tr>
-    <td>South Carolina</td>
-    <td>1.3</td>
-    <td>105.08223</td>
-    <td>8.39E+002</td>
-    <td>1.15E-003</td>
-    <td>2.54E-001</td>
-    <td>1.83E-003</td>
-    <td>6.05E-001</td>
-  </tr>
-  <tr>
-    <td>South Dakota</td>
-    <td>1.192</td>
-    <td>100.54631</td>
-    <td>9.79E+001</td>
-    <td>6.68E-004</td>
-    <td>5.45E-001</td>
-    <td>1.52E-003</td>
-    <td>5.81E-001</td>
-  </tr>
-  <tr>
-    <td>Tennessee</td>
-    <td>1.902</td>
-    <td>163.29325</td>
-    <td>9.10E+002</td>
-    <td>1.32E-003</td>
-    <td>5.10E-001</td>
-    <td>2.67E-003</td>
-    <td>1.18E+000</td>
-  </tr>
-  <tr>
-    <td>Texas</td>
-    <td>2.749</td>
-    <td>184.4609</td>
-    <td>9.63E+003</td>
-    <td>9.70E-004</td>
-    <td>3.28E-001</td>
-    <td>1.84E-003</td>
-    <td>4.91E-001</td>
-  </tr>
-  <tr>
-    <td>Utah</td>
-    <td>3.095</td>
-    <td>243.6799</td>
-    <td>5.13E+002</td>
-    <td>1.69E-003</td>
-    <td>5.27E-001</td>
-    <td>3.88E-003</td>
-    <td>2.13E-001</td>
-  </tr>
-  <tr>
-    <td>Vermont</td>
-    <td>0.306</td>
-    <td>3.52794</td>
-    <td>1.38E+002</td>
-    <td>1.21E-003</td>
-    <td>1.94E-002</td>
-    <td>4.91E-004</td>
-    <td>2.14E-003</td>
-  </tr>
-  <tr>
-    <td>Virginia</td>
-    <td>1.924</td>
-    <td>146.66153</td>
-    <td>9.13E+002</td>
-    <td>1.73E-003</td>
-    <td>3.65E-001</td>
-    <td>2.42E-003</td>
-    <td>7.87E-001</td>
-  </tr>
-  <tr>
-    <td>Washington</td>
-    <td>0.414</td>
-    <td>30.99548</td>
-    <td>4.30E+002</td>
-    <td>4.66E-004</td>
-    <td>5.30E-002</td>
-    <td>5.04E-004</td>
-    <td>1.90E-001</td>
-  </tr>
-  <tr>
-    <td>West Virginia</td>
-    <td>2.917</td>
-    <td>248.97181</td>
-    <td>1.28E+003</td>
-    <td>1.73E-003</td>
-    <td>7.78E-001</td>
-    <td>3.98E-003</td>
-    <td>1.87E+000</td>
-  </tr>
-  <tr>
-    <td>Wisconsin</td>
-    <td>2.68</td>
-    <td>206.88852</td>
-    <td>1.00E+003</td>
-    <td>1.74E-003</td>
-    <td>4.97E-001</td>
-    <td>3.28E-003</td>
-    <td>9.25E-001</td>
-  </tr>
-  <tr>
-    <td>Wyoming</td>
-    <td>3.534</td>
-    <td>270.39145</td>
-    <td>9.01E+002</td>
-    <td>1.85E-003</td>
-    <td>5.59E-001</td>
-    <td>4.26E-003</td>
-    <td>5.79E-001</td>
-  </tr>
-  <tr>
-    <td colspan="8">a Data based on 1999 data from eGRID version 2.01 (EPA 2003a).</td>
-  </tr>
-  <tr>
-    <td colspan="8">b Data based on 1998-2000 average data in DOE (2002).</td>
-  </tr>
-  <tr>
-    <td colspan="8">c Data based on tier emissions report for criteria air pollutants in EPA (2003b).</td>
-  </tr>
-  <tr>
-    <td colspan="8">d PM is the sum of all particulate matter including PM10 and PM2.5. PM10 and PM2.5 stand for particles smaller than 10 and 2.5 microns, respectively.</td>
-  </tr>
-  <tr>
-    <td colspan="8">e No data.</td>
-  </tr>
-</table>
-
-Table 103.  U. S. State Average Criteria Pollutant Emission Factors for Electricity Generation, in g/MJ
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Particulate Matter (PM)<sup>cd</sup></th>
-<th>Particulate Matter (PM10)<sup>cd</sup></th>
-<th>Particulate Matter (PM2.5)<sup>cd</sup></th>
-<th>Ammonia (NH<sub>3</sub>)<sup>c</sup></th>
-<th>Volatile Organic Compounds (NMVOC)<sup>a</sup></th>
-<th>Mercury (Hg)<sup>c</sup></th>
-<th>Lead (Pb)<sup>e</sup></th>
-</tr>
-<tr>
-<td>Alabama</td>
-<td>7.91048E-03</td>
-<td>7.86328E-03</td>
-<td>4.72023E-05</td>
-<td>3.55049E-05</td>
-<td>4.66784E-03</td>
-<td>5.14071E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Alaska</td>
-<td>8.96502E-03</td>
-<td>8.85977E-03</td>
-<td>1.05247E-04</td>
-<td>6.51454E-06</td>
-<td>2.82297E-03</td>
-<td>3.27594E-07</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Arizona</td>
-<td>1.70555E-02</td>
-<td>1.69322E-02</td>
-<td>1.23202E-04</td>
-<td>1.80226E-04</td>
-<td>2.27385E-03</td>
-<td>1.88997E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Arkansas</td>
-<td>9.27803E-03</td>
-<td>9.19307E-03</td>
-<td>8.49561E-05</td>
-<td>4.59383E-04</td>
-<td>3.46429E-03</td>
-<td>2.73415E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>California</td>
-<td>7.16813E-03</td>
-<td>7.07819E-03</td>
-<td>8.99402E-05</td>
-<td>4.02651E-03</td>
-<td>2.62453E-03</td>
-<td>1.38598E-07</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Colorado</td>
-<td>7.29822E-03</td>
-<td>7.23699E-03</td>
-<td>6.12291E-05</td>
-<td>9.56430E-05</td>
-<td>4.36770E-03</td>
-<td>1.62537E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Connecticut</td>
-<td>1.22734E-02</td>
-<td>1.21694E-02</td>
-<td>1.04033E-04</td>
-<td>2.22944E-03</td>
-<td>3.93896E-03</td>
-<td>1.18438E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Delaware</td>
-<td>1.39283E-02</td>
-<td>1.38287E-02</td>
-<td>9.96131E-05</td>
-<td>1.54469E-03</td>
-<td>4.74441E-03</td>
-<td>3.62874E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>District of Columbia</td>
-<td>2.88269E-02</td>
-<td>2.84861E-02</td>
-<td>3.40760E-04</td>
-<td>8.76496E-03</td>
-<td>2.30080E-02</td>
-<td>0</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Florida</td>
-<td>4.33040E-02</td>
-<td>4.29055E-02</td>
-<td>3.98460E-04</td>
-<td>1.58386E-03</td>
-<td>3.39110E-03</td>
-<td>1.71357E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Georgia</td>
-<td>2.05237E-02</td>
-<td>2.03865E-02</td>
-<td>1.37175E-04</td>
-<td>7.51637E-05</td>
-<td>2.16686E-03</td>
-<td>3.20035E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Hawaii</td>
-<td>5.97339E-03</td>
-<td>5.90409E-03</td>
-<td>6.92999E-05</td>
-<td>3.55697E-03</td>
-<td>7.01715E-03</td>
-<td>1.77657E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Idaho</td>
-<td>0</td>
-<td>0</td>
-<td>0</td>
-<td>0</td>
-<td>0</td>
-<td>0</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Illinois</td>
-<td>1.53276E-01</td>
-<td>1.52156E-01</td>
-<td>1.12047E-03</td>
-<td>5.93583E-03</td>
-<td>2.77818E-02</td>
-<td>4.62412E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Indiana</td>
-<td>2.18862E-02</td>
-<td>2.17008E-02</td>
-<td>1.85453E-04</td>
-<td>5.75861E-04</td>
-<td>4.87283E-03</td>
-<td>4.86352E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Iowa</td>
-<td>2.34564E-02</td>
-<td>2.32698E-02</td>
-<td>1.86674E-04</td>
-<td>9.09228E-05</td>
-<td>4.78644E-03</td>
-<td>6.19910E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Kansas</td>
-<td>2.41783E-02</td>
-<td>2.39535E-02</td>
-<td>2.24799E-04</td>
-<td>4.19292E-04</td>
-<td>5.39089E-03</td>
-<td>4.93912E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Kentucky</td>
-<td>1.69397E-02</td>
-<td>1.68139E-02</td>
-<td>1.25825E-04</td>
-<td>4.35029E-05</td>
-<td>3.80922E-03</td>
-<td>4.71232E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Lousiana</td>
-<td>1.79917E-02</td>
-<td>1.77843E-02</td>
-<td>2.07304E-04</td>
-<td>1.66720E-03</td>
-<td>1.02357E-02</td>
-<td>1.41118E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Maine</td>
-<td>3.36399E-03</td>
-<td>3.34131E-03</td>
-<td>2.26813E-05</td>
-<td>1.55132E-03</td>
-<td>9.62614E-03</td>
-<td>4.53592E-07</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Maryland</td>
-<td>2.13382E-02</td>
-<td>2.12038E-02</td>
-<td>1.34391E-04</td>
-<td>7.21581E-04</td>
-<td>2.78881E-03</td>
-<td>4.88872E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Mass-achusetts</td>
-<td>8.85244E-03</td>
-<td>8.76617E-03</td>
-<td>8.62772E-05</td>
-<td>1.70282E-03</td>
-<td>3.49171E-03</td>
-<td>1.88997E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Michigan</td>
-<td>9.08755E-03</td>
-<td>9.00520E-03</td>
-<td>8.23449E-05</td>
-<td>2.22140E-04</td>
-<td>2.79017E-03</td>
-<td>3.67914E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Minnesota</td>
-<td>4.04781E-02</td>
-<td>4.01455E-02</td>
-<td>3.32617E-04</td>
-<td>6.74889E-05</td>
-<td>4.13240E-03</td>
-<td>3.30114E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Mississippi</td>
-<td>5.44446E-02</td>
-<td>5.37910E-02</td>
-<td>6.53601E-04</td>
-<td>4.06289E-02</td>
-<td>1.54329E-02</td>
-<td>2.45696E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Missouri</td>
-<td>1.25537E-02</td>
-<td>1.24368E-02</td>
-<td>1.16929E-04</td>
-<td>6.48638E-05</td>
-<td>4.98085E-03</td>
-<td>4.67452E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Montana</td>
-<td>3.67504E-03</td>
-<td>3.64126E-03</td>
-<td>3.37798E-05</td>
-<td>4.01020E-05</td>
-<td>3.14400E-03</td>
-<td>3.77994E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Nebraska</td>
-<td>1.33751E-02</td>
-<td>1.32829E-02</td>
-<td>9.21636E-05</td>
-<td>6.90470E-05</td>
-<td>5.23031E-03</td>
-<td>3.59094E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Nevada</td>
-<td>2.09146E-02</td>
-<td>2.07657E-02</td>
-<td>1.48886E-04</td>
-<td>3.79659E-04</td>
-<td>3.33440E-03</td>
-<td>1.36078E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>New Hampshire</td>
-<td>3.09503E-02</td>
-<td>3.06487E-02</td>
-<td>3.01568E-04</td>
-<td>7.16019E-04</td>
-<td>2.45937E-03</td>
-<td>3.40194E-07</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>New Jersey</td>
-<td>3.45712E-02</td>
-<td>3.41460E-02</td>
-<td>4.25200E-04</td>
-<td>1.24216E-04</td>
-<td>1.52830E-02</td>
-<td>1.28518E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>New Mexico</td>
-<td>5.20754E-02</td>
-<td>5.16748E-02</td>
-<td>4.00653E-04</td>
-<td>4.41665E-04</td>
-<td>5.12951E-03</td>
-<td>8.41666E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>New York</td>
-<td>5.35802E-03</td>
-<td>5.31301E-03</td>
-<td>4.50068E-05</td>
-<td>2.22325E-03</td>
-<td>4.26008E-03</td>
-<td>1.33558E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>North Carolina</td>
-<td>3.40955E-02</td>
-<td>3.38325E-02</td>
-<td>2.62976E-04</td>
-<td>3.00504E-05</td>
-<td>1.73434E-03</td>
-<td>3.33894E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>North Dakota</td>
-<td>5.17162E-02</td>
-<td>5.13979E-02</td>
-<td>3.18277E-04</td>
-<td>6.41672E-05</td>
-<td>6.88995E-03</td>
-<td>8.71905E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Ohio</td>
-<td>1.38722E-02</td>
-<td>1.37957E-02</td>
-<td>7.64501E-05</td>
-<td>1.11541E-04</td>
-<td>2.59201E-03</td>
-<td>6.24949E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Oklahoma</td>
-<td>1.83971E-02</td>
-<td>1.82479E-02</td>
-<td>1.49160E-04</td>
-<td>9.73713E-04</td>
-<td>4.68484E-03</td>
-<td>3.88073E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Oregon</td>
-<td>3.47911E-03</td>
-<td>3.46199E-03</td>
-<td>1.71186E-05</td>
-<td>4.43277E-06</td>
-<td>5.31933E-04</td>
-<td>3.77994E-07</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Pennsylvania</td>
-<td>2.21604E-02</td>
-<td>2.20060E-02</td>
-<td>1.54356E-04</td>
-<td>1.47657E-04</td>
-<td>1.51542E-03</td>
-<td>6.56449E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Rhode Island</td>
-<td>1.03973E-03</td>
-<td>1.02744E-03</td>
-<td>1.22906E-05</td>
-<td>0</td>
-<td>2.25247E-03</td>
-<td>0</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>South Carolina</td>
-<td>2.45530E-02</td>
-<td>2.43803E-02</td>
-<td>1.72632E-04</td>
-<td>2.51344E-05</td>
-<td>1.16735E-03</td>
-<td>1.54977E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>South Dakota</td>
-<td>4.67825E-03</td>
-<td>4.63562E-03</td>
-<td>4.26239E-05</td>
-<td>8.82976E-05</td>
-<td>4.63562E-03</td>
-<td>1.22218E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Tennessee</td>
-<td>2.51650E-02</td>
-<td>2.48944E-02</td>
-<td>2.70575E-04</td>
-<td>2.70034E-05</td>
-<td>2.88396E-03</td>
-<td>2.98615E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Texas</td>
-<td>1.73147E-02</td>
-<td>1.71765E-02</td>
-<td>1.38283E-04</td>
-<td>1.26310E-03</td>
-<td>4.32150E-03</td>
-<td>3.52794E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Utah</td>
-<td>1.47314E-02</td>
-<td>1.46364E-02</td>
-<td>9.50155E-05</td>
-<td>9.59315E-05</td>
-<td>2.48737E-03</td>
-<td>9.70184E-07</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Vermont</td>
-<td>1.16247E-03</td>
-<td>1.14873E-03</td>
-<td>1.37415E-05</td>
-<td>1.80704E-05</td>
-<td>2.12073E-03</td>
-<td>0</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Virginia</td>
-<td>1.22315E-02</td>
-<td>1.21362E-02</td>
-<td>9.53635E-05</td>
-<td>2.93259E-04</td>
-<td>2.50975E-03</td>
-<td>2.21756E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Washington</td>
-<td>5.37627E-04</td>
-<td>5.32210E-04</td>
-<td>5.41708E-06</td>
-<td>6.46409E-06</td>
-<td>6.87348E-04</td>
-<td>5.92190E-07</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>West Virginia</td>
-<td>2.39677E-03</td>
-<td>2.38177E-03</td>
-<td>1.50018E-05</td>
-<td>4.25792E-05</td>
-<td>3.09497E-03</td>
-<td>6.55189E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Wisconsin</td>
-<td>7.34187E-03</td>
-<td>7.28252E-03</td>
-<td>5.93472E-05</td>
-<td>6.45613E-05</td>
-<td>4.61829E-03</td>
-<td>4.83832E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-<tr>
-<td>Wyoming</td>
-<td>5.08215E-02</td>
-<td>5.06042E-02</td>
-<td>2.17349E-04</td>
-<td>5.19787E-05</td>
-<td>4.78782E-03</td>
-<td>5.27931E-06</td>
-<td>0<sup>e</sup></td>
-</tr>
-</table>
-
-Table 104.  United States National Average Water Consumption Factors<sup>a</sup>
-
-<table class="table table-striped">
- <tr>
-  <th></th>
-  <th colspan="2">ThermoElectric Generation</th>
-  <th colspan="2">HydroElectric Generation</th>
-  <th>Weighted Total Water Consumption</th>
- </tr>
- <tr>
-  <th></th>
-  <th>L/MJ</th>
-  <th>Percent of Total Generation</th>
-  <th>L/MJ</th>
-  <th>Percent of Total Generation</th>
-  <th>L/MJ</th>
- </tr>
- <tr>
-  <th>United States</th>
-  <td>0.4960</td>
-  <td>89.4%</td>
-  <td>19.2095</td>
-  <td>8.6%</td>
-  <td>2.1007</td>
- </tr>
- <tr>
-  <td colspan="6">a Based on data from Torcellini, Long, and Judkoff (2004).</td>
- </tr>
-</table>
-
-Table 105.   U.S. State Average Water Consumption Factors for Electricity Generation<sup>a</sup>
-
-<table class="table table-striped">
-  <tr>
-    <th></th>
-    <th colspan="2">ThermoElectric Generation</th>
-    <th colspan="2">HydroElectric Generation</th>
-    <th>Weighted Total Water Consumption</th>
-  </tr>
-  <tr>
-    <th>State</th>
-    <th>L/MJ</th>
-    <th>Percent of Total Generation</th>
-    <th>L/MJ</th>
-    <th>Percent of Total Generation</th>
-    <th>L/MJ</th>
-  </tr>
-  <tr>
-    <td>Alabama</td>
-    <td>0.1503</td>
-    <td>89.80%</td>
-    <td>38.9053</td>
-    <td>6.4%</td>
-    <td>2.6274</td>
-  </tr>
-  <tr>
-    <td>Alaska</td>
-    <td>0.3295</td>
-    <td>86.20%</td>
-    <td>--</td>
-    <td>13.8%</td>
-    <td>0.2839</td>
-  </tr>
-  <tr>
-    <td>Arizona</td>
-    <td>0.3313</td>
-    <td>88.30%</td>
-    <td>68.1928</td>
-    <td>11.7%</td>
-    <td>8.2533</td>
-  </tr>
-  <tr>
-    <td>Arkansas</td>
-    <td>0.3</td>
-    <td>89.50%</td>
-    <td>--</td>
-    <td>5.7%</td>
-    <td>0.2684</td>
-  </tr>
-  <tr>
-    <td>California</td>
-    <td>0.0511</td>
-    <td>74.10%</td>
-    <td>21.943</td>
-    <td>22.0%</td>
-    <td>4.8739</td>
-  </tr>
-  <tr>
-    <td>Colorado</td>
-    <td>0.5368</td>
-    <td>96.00%</td>
-    <td>18.8333</td>
-    <td>4.0%</td>
-    <td>1.26</td>
-  </tr>
-  <tr>
-    <td>Connecticut</td>
-    <td>0.086</td>
-    <td>90.80%</td>
-    <td>--</td>
-    <td>1.5%</td>
-    <td>0.0781</td>
-  </tr>
-  <tr>
-    <td>Delaware</td>
-    <td>0.0132</td>
-    <td>99.90%</td>
-    <td>--</td>
-    <td>0.0%</td>
-    <td>0.0132</td>
-  </tr>
-  <tr>
-    <td>District of Columbia</td>
-    <td>1.6959</td>
-    <td>100.00%</td>
-    <td>--</td>
-    <td>0.0%</td>
-    <td>1.6959</td>
-  </tr>
-  <tr>
-    <td>Florida</td>
-    <td>0.1506</td>
-    <td>95.70%</td>
-    <td>--</td>
-    <td>0.1%</td>
-    <td>0.1441</td>
-  </tr>
-  <tr>
-    <td>Georgia</td>
-    <td>0.6267</td>
-    <td>93.60%</td>
-    <td>49.8599</td>
-    <td>2.3%</td>
-    <td>1.7339</td>
-  </tr>
-  <tr>
-    <td>Hawaii</td>
-    <td>0.044</td>
-    <td>92.40%</td>
-    <td>--</td>
-    <td>1.1%</td>
-    <td>0.0407</td>
-  </tr>
-  <tr>
-    <td>Idaho</td>
-    <td>0</td>
-    <td>2.70%</td>
-    <td>8.9528</td>
-    <td>92.2%</td>
-    <td>8.2501</td>
-  </tr>
-  <tr>
-    <td>Illinois</td>
-    <td>1.1093</td>
-    <td>99.40%</td>
-    <td>--</td>
-    <td>0.1%</td>
-    <td>1.1032</td>
-  </tr>
-  <tr>
-    <td>Indiana</td>
-    <td>0.435</td>
-    <td>99.60%</td>
-    <td>--</td>
-    <td>0.3%</td>
-    <td>0.4331</td>
-  </tr>
-  <tr>
-    <td>Iowa</td>
-    <td>0.1229</td>
-    <td>97.30%</td>
-    <td>--</td>
-    <td>2.5%</td>
-    <td>0.1196</td>
-  </tr>
-  <tr>
-    <td>Kansas</td>
-    <td>0.6099</td>
-    <td>100.00%</td>
-    <td>--</td>
-    <td>0.0%</td>
-    <td>0.6098</td>
-  </tr>
-  <tr>
-    <td>Kentucky</td>
-    <td>1.1521</td>
-    <td>97.20%</td>
-    <td>162.2884</td>
-    <td>2.8%</td>
-    <td>5.599</td>
-  </tr>
-  <tr>
-    <td>Louisiana</td>
-    <td>1.6411</td>
-    <td>94.20%</td>
-    <td>--</td>
-    <td>0.9%</td>
-    <td>1.5461</td>
-  </tr>
-  <tr>
-    <td>Maine</td>
-    <td>0.3049</td>
-    <td>40.40%</td>
-    <td>--</td>
-    <td>28.7%</td>
-    <td>0.1231</td>
-  </tr>
-  <tr>
-    <td>Maryland</td>
-    <td>0.0343</td>
-    <td>95.30%</td>
-    <td>7.0617</td>
-    <td>2.7%</td>
-    <td>0.2259</td>
-  </tr>
-  <tr>
-    <td>Massachusetts</td>
-    <td>0</td>
-    <td>92.40%</td>
-    <td>--</td>
-    <td>2.4%</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>Michigan</td>
-    <td>0.5221</td>
-    <td>95.80%</td>
-    <td>--</td>
-    <td>1.4%</td>
-    <td>0.4999</td>
-  </tr>
-  <tr>
-    <td>Minnesota</td>
-    <td>0.4657</td>
-    <td>93.40%</td>
-    <td>--</td>
-    <td>2.4%</td>
-    <td>0.4351</td>
-  </tr>
-  <tr>
-    <td>Mississippi</td>
-    <td>0.4145</td>
-    <td>94.40%</td>
-    <td>--</td>
-    <td>0.0%</td>
-    <td>0.3912</td>
-  </tr>
-  <tr>
-    <td>Missouri</td>
-    <td>0.3213</td>
-    <td>97.40%</td>
-    <td>--</td>
-    <td>2.5%</td>
-    <td>0.313</td>
-  </tr>
-  <tr>
-    <td>Montana</td>
-    <td>1.0051</td>
-    <td>55.80%</td>
-    <td>38.6619</td>
-    <td>44.1%</td>
-    <td>17.5997</td>
-  </tr>
-  <tr>
-    <td>Nebraska</td>
-    <td>0.202</td>
-    <td>94.50%</td>
-    <td>2.2888</td>
-    <td>5.5%</td>
-    <td>0.3165</td>
-  </tr>
-  <tr>
-    <td>Nevada</td>
-    <td>0.5936</td>
-    <td>90.60%</td>
-    <td>77.1023</td>
-    <td>9.2%</td>
-    <td>7.626</td>
-  </tr>
-  <tr>
-    <td>New Hampshire</td>
-    <td>0.1231</td>
-    <td>83.90%</td>
-    <td>--</td>
-    <td>8.6%</td>
-    <td>0.1033</td>
-  </tr>
-  <tr>
-    <td>New Jersey</td>
-    <td>0.0747</td>
-    <td>97.60%</td>
-    <td>--</td>
-    <td>0.0%</td>
-    <td>0.0729</td>
-  </tr>
-  <tr>
-    <td>New Mexico</td>
-    <td>0.6609</td>
-    <td>99.30%</td>
-    <td>71.507</td>
-    <td>0.7%</td>
-    <td>1.1886</td>
-  </tr>
-  <tr>
-    <td>New York</td>
-    <td>0.8951</td>
-    <td>81.30%</td>
-    <td>5.8535</td>
-    <td>16.7%</td>
-    <td>1.704</td>
-  </tr>
-  <tr>
-    <td>North Carolina</td>
-    <td>0.2445</td>
-    <td>95.50%</td>
-    <td>10.9089</td>
-    <td>3.1%</td>
-    <td>0.5751</td>
-  </tr>
-  <tr>
-    <td>North Dakota</td>
-    <td>0.3809</td>
-    <td>91.70%</td>
-    <td>60.773</td>
-    <td>8.3%</td>
-    <td>5.3968</td>
-  </tr>
-  <tr>
-    <td>Ohio</td>
-    <td>0.9972</td>
-    <td>99.10%</td>
-    <td>--</td>
-    <td>0.3%</td>
-    <td>0.9884</td>
-  </tr>
-  <tr>
-    <td>Oklahoma</td>
-    <td>0.5378</td>
-    <td>93.70%</td>
-    <td>144.0133</td>
-    <td>5.8%</td>
-    <td>8.8254</td>
-  </tr>
-  <tr>
-    <td>Oregon</td>
-    <td>0.8633</td>
-    <td>18.40%</td>
-    <td>4.6351</td>
-    <td>80.7%</td>
-    <td>3.899</td>
-  </tr>
-  <tr>
-    <td>Pennsylvania</td>
-    <td>0.57</td>
-    <td>97.60%</td>
-    <td>--</td>
-    <td>1.0%</td>
-    <td>0.5563</td>
-  </tr>
-  <tr>
-    <td>Rhode Island</td>
-    <td>0</td>
-    <td>98.20%</td>
-    <td>--</td>
-    <td>0.1%</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>South Carolina</td>
-    <td>0.2754</td>
-    <td>97.20%</td>
-    <td>--</td>
-    <td>1.9%</td>
-    <td>0.2677</td>
-  </tr>
-  <tr>
-    <td>South Dakota</td>
-    <td>0.0143</td>
-    <td>36.70%</td>
-    <td>120.7558</td>
-    <td>63.2%</td>
-    <td>76.3811</td>
-  </tr>
-  <tr>
-    <td>Tennessee</td>
-    <td>0.0026</td>
-    <td>90.80%</td>
-    <td>45.5853</td>
-    <td>8.3%</td>
-    <td>3.7833</td>
-  </tr>
-  <tr>
-    <td>Texas</td>
-    <td>0.4595</td>
-    <td>99.00%</td>
-    <td>--</td>
-    <td>0.3%</td>
-    <td>0.455</td>
-  </tr>
-  <tr>
-    <td>Utah</td>
-    <td>0.5959</td>
-    <td>96.60%</td>
-    <td>77.115</td>
-    <td>3.4%</td>
-    <td>3.209</td>
-  </tr>
-  <tr>
-    <td>Vermont</td>
-    <td>0.3642</td>
-    <td>71.50%</td>
-    <td>--</td>
-    <td>20.9%</td>
-    <td>0.2605</td>
-  </tr>
-  <tr>
-    <td>Virginia</td>
-    <td>0.0693</td>
-    <td>94.90%</td>
-    <td>--</td>
-    <td>0.9%</td>
-    <td>0.0657</td>
-  </tr>
-  <tr>
-    <td>Washington</td>
-    <td>0.3013</td>
-    <td>15.70%</td>
-    <td>3.3506</td>
-    <td>83.2%</td>
-    <td>2.8344</td>
-  </tr>
-  <tr>
-    <td>West Virginia</td>
-    <td>0.618</td>
-    <td>99.00%</td>
-    <td>--</td>
-    <td>1.0%</td>
-    <td>0.6119</td>
-  </tr>
-  <tr>
-    <td>Wisconsin</td>
-    <td>0.5199</td>
-    <td>93.60%</td>
-    <td>--</td>
-    <td>3.3%</td>
-    <td>0.4867</td>
-  </tr>
-  <tr>
-    <td>Wyoming</td>
-    <td>0.519</td>
-    <td>97.10%</td>
-    <td>144.0177</td>
-    <td>2.7%</td>
-    <td>4.3654</td>
-  </tr>
-  <tr>
-    <td colspan="6">a Based on data from Torcellini, Long, and Judkoff (2004).</td>
-  </tr>
-</table>
-
-
-### Other Energy-Related Pollutants and Sources of Other Information
-
-EnergyPlus (with user entered-data) will also calculate high- and low-level nuclear waste from electricity generation. Few utilities now provide data on nuclear waste resulting from electricity generation and no US national or state-level data are yet available (this will be added as data become available).  Two Illinois utilities regularly report nuclear waste in terms of pounds per kWh or MWh for high-level waste and cubic feet per kWh or MWh for low-level waste.  For these two utilities, high level nuclear waste values range from 0.0042 to 0.01 lb/MWh (7000 to 16000 g/MJ); low-level nuclear waste ranges from 0.0001 to 0.0002 ft<sup>3</sup>/MWh (0.01 to 0.02 m<sup>3</sup>/MJ) depending on relative proportion of nuclear as compared with other electricity generation sources.
-
-IEA (2003) contains carbon dioxide (CO<sub>2</sub>) emissions factors for electricity generation by country and region. Carbon dioxide (CO<sub>2</sub>) is responsible for over 60% of the anthropogenic greenhouse effect (UNEP 2002). Because only limited greenhouse gas emissions factors and data (other than CO<sub>2</sub>) is available for other countries, an interim method for estimating emission factors would be to compare the CO<sub>2</sub> emission factor for the particular country from IEA (2003) and match it to the state with the closest CO<sub>2</sub> emission factor in Table 102—using the other emissions factors for that state. Since the Kyoto Protocol (UNFCCC 1997) requires each country to report emissions of the major greenhouse gases [carbon dioxide (CO<sub>2</sub>), methane (CH<sub>4</sub>), and nitrous oxide (N<sub>2</sub>O)] as well as ozone-depleting substances [hydrofluorocarbons (HFC), perfluorocarbons (PFC), and sulphur hexafluoride (SF<sub>6</sub>)] and all energy consumption in their annual ‘national communication’, more complete emission factors for a larger number of countries should become available over the next few years. More information and other resources for calculating emissions factors are available in IPCC (2000, 1997).
-
-### References
-
-Crawley, Drury B.  2003.  “Impact of Climate Change on Buildings,� in *Proceedings of the CIBSE/ASHRAE International Conference 2003*, September 2003, Edinburgh, Scotland.  London, England: CIBSE.
-
-Intergovernmental Panel on Climate Change.  2001.  *Climate Change 2001: The Scientific Basis*.  Cambridge: Cambridge University Press.
-
-Intergovernmental Panel on Climate Change. 2000. *Good Practice Guidance and Uncertainty Management in National Greenhouse Gas Inventories*, Paris, France: IPCC/OECD/IEA.
-
-Intergovernmental Panel on Climate Change. 1997. *Revised 1996 IPCC Guidelines for National Greenhouse Gas Inventories*, J.T. Houghton, L.G. Meira Filho, B. Lim, K. Treanton, I. Mamaty, Y. Bonduki, D.J. Griggs and B.A. Callender (editors).  Paris, France: IPCC/OECD/IEA.
-
-International Energy Agency.  2003. *CO<sub>2</sub> Emissions from Fuel Combustion 1971-2001 (2003) -- 2003 Edition*.  Paris, France: IEA.
-
-Liesen, Richard J. 1997. *Atmospheric Pollution Prediction in a Building Energy Simulation Program*, April 1997, BLAST Support Office, Department of Mechanical Engineering. Champaign, Illinois: University of Illinois.
-
-Stroot, Peter J., Robert J. Nemeth, & Donald F. Fournier.  1996.  *Pollution Reduction Through Energy Conservation, REEP Model*.  Champaign, Illinois: U S Army Construction Engineering Research Laboratory.
-
-Torcellini Paul A, Nicholas Long, and Ronald D. Judkoff.  2004. “Consumptive Water Use for U.S. Power Production,� in *ASHRAE Transactions,* Volume 110, Part 1. Atlanta, Georgia: ASHRAE.
-
-United Nations Environment Programme.  2002.  *Climate Change Information Kit*.  Châtelaine, Switzerland: UNEP.
-
-United Nations Framework Convention on Climate Change.  1997. *Kyoto* *Protocol to the United Nations Framework Convention on Climate Change.*  Bonn, Germany: UNFCCC.
-
-U.S. Department of Energy.  2004. *Monthly Energy Review*. Washington, DC:  Energy Information Administration, U S Department of Energy.
-
-U.S. Department of Energy.  2002. *Updated State-level Greenhouse Gas Emission Coefficients for Electricity Generation 1998-2000*.  April 2002, Energy Information Administration, Office of Integrated Analysis and Forecasting, Energy Information Administration.  Washington, DC: U.S. Department of Energy.
-
-U.S. Environmental Protection Agency.  2003a. *eGRID Emissions and Generation Resource Integrated Database*, May 2003, Washington, DC:  U.S. Environmental Protection Agency.
-
-U.S. Environmental Protection Agency.  2003b. *AirData,* Tier Emissions Report - Criteria Air Pollutants, 1999 data, May 2003. Washington, DC:  U.S. Environmental Protection Agency.
-
-U.S. Environmental Protection Agency.  1998a. *Compilation of Air Pollutant Emission Factors, AP-42, Fifth Edition, Volume I: Stationary Point and Area Sources*, Chapter 1 External Combustion Sources, Supplement D, July 1998. Research Triangle Park, North Carolina: U. S. Environmental Protection Agency.
-
-U.S. Environmental Protection Agency.  1998b. *Compilation of Air Pollutant Emission Factors, AP-42, Fifth Edition, Volume I: Stationary Point and Area Sources,* Chapter 1 External Combustion Sources, Supplement E, September 1998. Research Triangle Park, North Carolina: U. S. Environmental Protection Agency.
-
-U.S. Environmental Protection Agency.  1996. *Compilation of Air Pollutant Emission Factors, AP-42, Fifth Edition, Volume I: Stationary Point and Area Sources,* Chapter 1 External Combustion Sources, Supplement B, October 1996. Research Triangle Park, North Carolina: U. S. Environmental Protection Agency.
-
-Zone Component Loads Summary
-----------------------------
-
-Many building energy simulation programs provide reports that breakdown the design load into component contributions from  walls, roofs, floors, underground walls, windows, interior walls, infiltration, ventilation, occupancy, lighting, refrigeration cases, and internal equipment. Some of these components have both sensible and latent subcomponents. It is important to understand the difference between gains and loads. ASHRAE Handbook of Fundamentals 2009 describes the space heat gain as “.. the rate at which heat enters into and/or is generated within a space� while the space cooling load is “the rate at which sensible and latent heat must be removed fro the space to maintain a constant space air temperature and humidity.�  The difference is that the radiant heat gains which is “absorbed by walls, floors, furniture, etc., contributed to the space cooling load only after a time lag.�
-
-The heat balance algorithms used by  EnergyPlus result in a single combined design load for a given zone and some, but not all, of the zone instantaneous heat gains. This section describes the estimation procedure for the Zone Component Loads Summary report that shows an estimated breakdown of load components from each type of of heat gain for each zone.
-
-The Estimated Cooling Peak Load Components and Estimated Heating Peak Load Components subtables of the Zone Component Loads Summary report contain values that are estimated and are not part of the normal heat balance algorithms used in the rest of EnergyPlus.  In particular, the column described as Sensible-Delayed represents an estimate of the sensible load contributed at the peak time based on radiant contributions from various load components that have radiant portions in previous timesteps. The focus of this section will be on the Sensible-Delayed column.
-
-The columns labeled Sensible-Instant, Sensible-Return Air, and Latent are directly computed for people, lights, equipment, refrigeration, water use equipment,  HVAC equipment losses, power generation equipment, infiltration, zone ventilation and interzone mixing. For example, Lights objects have inputs for the fractions of the gains that are to return air, radiant, visible and the remainder is convected.  In this case, the fraction to return air is reported in the Sensible Return Air column and the fraction that is convected is reported in the Sensible-Instant column.
-
-At the time of the peak load, each surface in the zone is contributing a convective heat loss or heat gain depending on the inside surface temperature.
-
-The radiant portion of the internal heat gains from lighting, equipment, and incident solar are radiantly transmitted to the surfaces of the zone. The heat from these radiant gains is stored in the surfaces and retransmitted back into the zone over time as convective gains to the zone. By the time the heat is retransmitted, it is impossible to know the contribution of each possible radiant gain from past time steps on that surface into the convective gain for that timestep. The temperature change of the surface includes the impact of all of these radiant gains as well as any heat transfer through the surface.
-
-To disaggregate the delayed affect of zone radiant (delayed) portions of the peak load, a pulse of radiant internal loads is used to determine custom radiant to convective decay curves for heating and cooling, essentially replicating part of the method used for Radiant Time Series (see Chapter 18 of ASHRAE Handbook of Fundamentals 2009) to isolate the delayed impacts of internal loads. This is performed during the zone sizing routines.
-
-The response of each surface to a pulse of radiant heat is used to estimate the peak load components for solar gains and the radiant portion of internal gains. Subtracting these for each surface then leaves the peak load component from conduction through the surfaces. The approach is described in more detail below:
-
-1) When zone sizing is performed for cooling or heating, the heat convected from each opaque surface for each timestep during sizing day is saved to an array.
-
-2) For each type of internal gain, HVAC equipment gain, and solar energy entering the zone, the radiant and convective portions are saved for every timestep during sizing. In addition, for each type of radiant gain, the amount that lands on each surface in the zone is saved for evergy timestep during sizing.
-
-3) An additional "pulse sizing" run is performed for cooling and heating during zone sizing that includes an additional small, single timestep, pulse of radiant-only heat for each zone but is otherwise the same as a normal zone sizing simulation. This is equivalent to adding an ElectricEquipment object that is scheduled for a single timestep and is 100% radiant heat. The heat convected from each opaque surface for each timestep during sizing is saved to an array. This run is not used for sizing, but just to gather the impact of the pulse of radiant heat.
-
-4) For each surface, a "decay curve" is developed by subtracting the results from the normal sizing (1) from the "pulse" sizing run (3). This represents the delay in converting incoming radiant heat into convected heat for each surface in the zone. The graphs below show the decay curves for an exterior wall (RIGHT-1) and an interior wall (SB23) for a test file.
-
-![](media/image7912.png)
-
-Figure 343. Load Component - Decay Curve of Exterior Wall
-
-
-
-![](media/image7913.png)
-
-Figure 344. Load Component - Decay Curve of Interior Wall
-
-
-
-5) Using the internal and solar gain results saved from the normal sizing period in step (2), for each timestep prior to and including the time of the peak load during the sizing day, the decay curve is applied to each radiant gain on each surface for each timestep to generate a predicted delayed load component for the internal and solar gains for each timestep that comprise the peak load (based on Timesteps in Averaging Window). Timesteps just before the peak have much larger impacts than those just a few timesteps before the peak.  These results will be the radiant portion of the load for each type of internal and solar gain.
-
-6) The difference between the sum of the predicted convective loads from internal and solar gains from step (5) and the total convective loads for that surface for the timesteps that comprise the peak load from step (1) is assumed to be the load from heat transfer through that surface.  This is essentially subtracting out the radiant portions of the internal and solar gains on each surface for the sizing day.
-
-### Estimated Component Load Details
-
-In HeatBalanceInternalHeatGains, in the InitInternalHeatGains routine, the single timestep pulse is added to the thermal radiation absorbed on the inside surface. It is based on 0.01 W per square meter of the zone area. The time of the pulse and the amount received by each surface is also saved. A new routine GatherComponentLoadsIntGain was also added to that file that gathers the instantenous heat gains from people, lights, equipment, refrigeration equipment, water use, hvac losses, and power generation. Latent gains from people and refrigeration are also gathered along with the radiant portion of the gains from these same sources. EnergyPlus tracks internal gains by type, and these are grouped as follows for the rows of the report:
-
-The gains from “People� contain:
-
-* IntGainTypeOf\_People
-
-The gains from “Lights� contain:
-
-* IntGainTypeOf\_Lights
-
-The gains from “Equipment� contain:
-
-* IntGainTypeOf\_ElectricEquipment
-
-* IntGainTypeOf\_GasEquipment
-
-* IntGainTypeOf\_HotWaterEquipment
-
-* IntGainTypeOf\_SteamEquipment
-
-* IntGainTypeOf\_OtherEquipment
-
-The gains from “Refrigeration� contain:
-
-* IntGainTypeOf\_RefrigerationCase
-
-* IntGainTypeOf\_RefrigerationCompressorRack
-
-* IntGainTypeOf\_RefrigerationSystemAirCooledCondenser
-
-* IntGainTypeOf\_RefrigerationSystemSuctionPipe
-
-* IntGainTypeOf\_RefrigerationSecondaryReceiver
-
-* IntGainTypeOf\_RefrigerationSecondaryPipe
-
-* IntGainTypeOf\_RefrigerationWalkIn
-
-The gains from “Water Use Equipment� contain:
-
-* IntGainTypeOf\_WaterUseEquipment
-
-* IntGainTypeOf\_WaterHeaterMixed
-
-* IntGainTypeOf\_WaterHeaterStratified
-
-The gains from “HVAC Equipment Losses� which are gains to the zone due to the location of the equipment within the zone include:
-
-* IntGainTypeOf\_ZoneBaseboardOutdoorTemperatureControlled
-
-* IntGainTypeOf\_ThermalStorageChilledWaterMixed
-
-* IntGainTypeOf\_ThermalStorageChilledWaterStratified
-
-* IntGainTypeOf\_PipeIndoor
-
-* IntGainTypeOf\_Pump\_VarSpeed
-
-* IntGainTypeOf\_Pump\_ConSpeed
-
-* IntGainTypeOf\_Pump\_Cond
-
-* IntGainTypeOf\_PumpBank\_VarSpeed
-
-* IntGainTypeOf\_PumpBank\_ConSpeed
-
-* IntGainTypeOf\_PlantComponentUserDefined
-
-* IntGainTypeOf\_CoilUserDefined
-
-* IntGainTypeOf\_ZoneHVACForcedAirUserDefined
-
-* IntGainTypeOf\_AirTerminalUserDefined
-
-The gains from “Power Generation Equipment� include:
-
-* IntGainTypeOf\_GeneratorFuelCell
-
-* IntGainTypeOf\_GeneratorMicroCHP
-
-* IntGainTypeOf\_ElectricLoadCenterTransformer
-
-* IntGainTypeOf\_ElectricLoadCenterInverterSimple
-
-* IntGainTypeOf\_ElectricLoadCenterInverterFunctionOfPower
-
-* IntGainTypeOf\_ElectricLoadCenterInverterLookUpTable
-
-* IntGainTypeOf\_ElectricLoadCenterStorageBattery
-
-The ReportSurfaceHeatBalance routine in the HeatBalanceSurfaceManger module gathers the shortwave radiant heat gain from lighting and fenestration solar gains on each surface. In the same module, the CalcHeatBalanceInsideSurf routine gathers the surface by surface convection for both the normal and pulse zone sizing times along with the net radiation on the surface during the normal zone sizing times. In addition, a routine called GatherComponentLoadSurfAbsFact gathers the factors used in distributing the radiant heat from a zone to each surface (TMULT and ITABSF).
-
-The SizingManager module repeats the zone sizing portion of the procedure when this report is requested.  The pulse occurs at 10am during the zone sizing simulations. The 10am time was chosen after some testing that looked at pulses at different times of the day. It is  important that the pulse occurs while the system is running and stable not during start up hours. In addition, the plus timing needs to be early enough that the duration of the resulting decay curve can be appropriate applied to as many timesteps as possible during the peak day.
-
-The following subroutines in the OutputReportTabular module produce the report:
-
-* ComputeLoadComponentDecayCurve
-
-* GatherComponentLoadsSurface
-
-* GatherComonentLoadsHVAC
-
-* ComputeDelayedComponents
-
-* WriteZoneLoadComponentTable
-
-
-
-The ComputeLoadComponentDecayCurve routine determines the heating and cooling decay curves using the following (for cooling but repeated also for heating):
-
-```
-  TimeOfPulse = radiantPulseTimestep(ZoneNum,CoolDesSelected)
-  DO TimeStep = TimeOfPulse, NumOfTimeStepInHour* 24
-    IF (radiantPulseReceived(surfNum,CoolDesSelected) .NE. 0.0) THEN
-      diff = loadConvectedWithPulse(surfNum,TimeStep,CoolDesSelected)
-           - loadConvectedNormal(surfNum,TimeStep,CoolDesSelected)
-      decayCurveCool(surfNum, TimeStep - TimeOfPulse + 1) = -diff /
-          radiantPulseReceived(surfNum,CoolDesSelected)
-    ELSE
-      decayCurveCool(surfNum, TimeStep - TimeOfPulse + 1) = 0.0
-    END IF
-  END DO
-```
-
-The ComputeDelayedComponents routine applies the decay curve to the load components. It does the following for the heating and cooling sizing period that was selected and for each zone and each surface in the zone
-
-1. Determine the heat gain on the surface of people, equipment, hvac losses, power generation and long wave light radiation.
-
-2. For each time step backwards from the current timestep, estimate the delayed convected heat from people, equipment, HVAC losses, power generation, lighting long wave radiation, lighting short wave radiation, and fenestration solar by multiplying the decay curve with the value determined from (a).
-
-3. Accumulate the values on a zone basis
-
-4. Determine the remaining convective heat from surfaces that are not from these gains and remove the net surface radiation (output variable Surface Inside Face Convection Heat Gain Rate)
-
-5. Store the estimated values in a sequence to be later averaged over the averaging window.
-
-Output:Table:Annual
--------------------
-
-No special algorithms were employed to implement the Output:Table:Annual object.
-
diff --git a/doc/src/docs/EngineeringReference/OperationalFaults.md b/doc/src/docs/EngineeringReference/OperationalFaults.md
deleted file mode 100644
index 46b7b7a99fb..00000000000
--- a/doc/src/docs/EngineeringReference/OperationalFaults.md
+++ /dev/null
@@ -1,260 +0,0 @@
-
-Operational Faults
-===============
-
-### Introduction to Operational Faults Modeling
-
-Most of the buildings, either new or old, have operational faults in the sensors, controllers, meters, equipment and systems. Being able to model and simulate these faults and their impact on energy performance of buildings is crucial to improve accuracy of building simulations and to support the retrofit of buildings. 
-To date, the main practitioner use of EnergyPlus has been for new construction design. With the new high priority attached by USDOE to retrofit and improved operation of existing buildings, there is a need to extend the capabilities of EnergyPlus to model existing buildings, including faulty operation:
-
-* Retrofit analysis: starts with calibrated simulation; the ability to estimate the severity of common faults is expected to improve the accuracy and transparency of the calibrated model and hence the increase accuracy of the analysis of different retrofit measures.  
-* Commissioning providers can use the fault models to demonstrate the saving to be expected from fixing faults found in retro-commissioning
-* Support for building operation by using the calibrated model, including unfixed faults, as a real-time reference model to detect, and verify the diagnosis of, newly occurring faults.
-
-The users in these cases are practitioners, not power users, so it is needed to implement the fault models using conventional EnergyPlus objects rather than the EMS, which, in any case, could only be used to model limited types of faults.   
-
-EnergyPlus contains a number of objects to model operational faults of sensors, meters, equipment and systems. The current implementation allows the modeling of the following fault types: (1) sensor faults with air economizers, (2) thermostat/humidistat offset faults, and (3) heating and cooling coil fouling faults. 
-
-### Sensor Faults with Air Economizers
-
-#### Symptom
-
-The sensor readings deviate from the actual air conditions due to sensor offset, which leads to inappropriate operations of the air economizer and thus undesired resulting indoor conditions.
-
-#### Modeling Approach
-
-There are a number of sensors installed to support the air economizer operations. The sensors may be of different types. The objects used by EnergyPlus to model the sensor faults are as follows:
-
-* FaultModel:TemperatureSensorOffset:OutdoorAir
-* FaultModel:HumiditySensorOffset:OutdoorAir
-* FaultModel:EnthalpySensorOffset:OutdoorAir
-* FaultModel:TemperatureSensorOffset:ReturnAir
-* FaultModel:EnthalpySensorOffset:ReturnAir
-
-### Thermostat/Humidistat Offset 
-
-#### Symptom
-
-The zone air temperature/relative humidity readings deviate from the actual zone air conditions due to thermostat/humidistat offset, and thus leads to inappropriate operations of the HVAC system and undesired resulting indoor conditions.
-
-#### Modeling Approach
-
-The thermostat offset fault is described in the object FaultModel:ThermostatOffset, which refers to the object ZoneControl:Thermostat. The humidistat offset fault is described in the object FaultModel:HumidistatOffset, which refers to the object ZoneControl:Humidistat.
-The effect of an offset in a thermostat/humidistat whose sole use is for the calculation of difference between the set-points and the design values can be modeled as an equal and opposite offset in the thermostat/humidistat: 
-
-$$T_{s,f} = T_{s,ff}  - \Delta T$$
-
-$$RH_{s,f} = RH_{s,ff}  - \Delta RH$$
-
-Where, 
-
-$T_{s,f}$ thermostat value in the faulty case, C
-
-$T_{s,ff}$ thermostat value in the fault-free case (design value), C
-
-$RH_{s,f}$ humidistat value in the faulty case,
-
-$RH_{s,ff}$ humidistat value in the fault-free case (design value),
-
-$\Delta T / \Delta RH$ difference between the thermostat/humidistat readings and the actual zone air conditions. Positive values mean that the readings is higher than the actual air conditions.
-
-For the humidistat that is independent of the thermostat, $\Delta RH$ can be described by a pre-defined schedule. For the humidistat offset that is caused by the thermostat offset, $\Delta RH$ is related with both the thermostat offset level as well as the indoor air conditions which are dynamic, and therefore cannot be described with a pre-defined schedule. In this case, the humidistat offset level is calculated each time step. 
-
-$$\Delta RH = RH_{s,ff} - f(T_{real}, W_{s,f})$$
-
-Where,
-
-$T_{real}$ real-time temperature of the indoor air (real value), C
-
-$W_{s,f}$ humidistat ratio corresponding to $T_{real} - \Delta T and RH_{s,ff, kgWater/kgDryAir}$
-
-Note that the thermostat/humidistat settings are related with two major processes within EnergyPlus: one is the design load calculations and HVAC system sizing, and the other is the HVAC system operations. Only the latter is affected by the thermostat/humidistat offset fault, while the former is not. Therefore, the size of the corresponding HVAC equipment in the faulty cases is the same as that in the fault-free cases.
-
-When EMS is used to overwrite the ZoneControl:Thermostat/ZoneControl:Humidistat values, the offsets are applied to the EMS values rather than the original Thermostat/Humidistat values.
-
-### Heating and Cooling Coil Fouling 
-
-#### Symptom
-
-Reduced overall heat transfer coefficient (UA) causes reduced coil capacity, resulting in unmet loads and/or increased water flow rate and decreased water side temperature difference (“low ΔT� syndrome). 
-
-#### Modeling Approach
-
-The coil fouling fault is described in the object FaultModel:Fouling:Coil. The fault model currently applies only to the ‘simple’ water coils: Coil:Heating:Water and Coil:Cooling:Water.
-The FaultModel:Fouling:Coil object allows the user to describe the fouling information in either of the two methods: FouledUARated or FoulingFactor. Using FouledUARated method, user specifies the value of UAfouled directly. Using FoulingFactor method user specifies air/water side fouling factor, and the UAfouled value is further calculated via the equations shown below.
-
-$$UA_{fouled} = [UA_{air} - 1  +  R_{foul}  + UA_{water} - 1]-1$$
-
-Where, 
-
-$U_{Aair}$ heat transfer coefficient of the coil on the air side, W/K
-
-$UA_{fouled}$ overall heat transfer coefficient of the fouled coil, W/K
-
-$UA_{water}$ heat transfer coefficient of the coil on the water side, W/K
-
-$R_{foul}$ fouling factor, K/W
-
-$R_{foul}$ is determined by:
-
-$$R_{foul} = r_{air}/A_{air} + r_{water} / A_{water}$$
-
-Where, 
-
-$r_{air}$ Air side fouling factor, m2-K/W
-
-$r_{water}$ Water side fouling factor, m2-K/W 
-
-$A_{air}$ Air side coil surface area, m2
-
-$A_{water}$  Water side coil surface area, m2
-
-The pressure drop associated with the fouling is ignored in the current implementation.
-
-### Air Filter Fouling 
-
-#### Symptom
-
-Increased air loop system resistance, resulting in a different system curve. This directly affects the operation of corresponding fans. More specifically, it may lead to variations of the fan pressure rise, fan energy consumption, as well as the enthalpy of the fan outlet air. It may also lead to a reduction in the airflow rate and thus affects the performance of other system components (e.g., heat transfer performance of heating/cooling coils).
-
-#### Modeling Approach
-
-The fouling air filter fault is described in the object FaultModel:Fouling:AirFilter, which refers to the fan objects that describe the associated fan. The fan object can be Fan:ConstantVolume, Fan:OnOff, or Fan:VariableVolume. The design pressure rise variations of the associated fan in the faulty cases are described by the Pressure Fraction Schedule specified in FaultModel:Fouling:AirFilter object, which is used as a multiplier to the fault-free fan design pressure rise specified in the fan object. The variations of the design air flow rate of the fan can then be calculated with the Pressure Fraction Schedule and Fan Curve. When EMS is used to overwrite the the pressure/MassFlow, the EMS values are used.
-
-The effect of the fouling air filter on the fan performance is related with a number of factors, including the fan types, fan curves, and system design and operating conditions. In general, there are three possible situations to be addressed in modeling dirty air filters:
-
-**(a) The required airflow rate can be maintained by the variable speed fan running at higher speed.**
-
-In this case, the fan operation state changes from point A (intersection of the fan curve corresponding to a lower speed and the system curve with clean filters) to point B (intersection of the fan curve corresponding to a higher speed and the system curve with dirty filters), as shown in Figure 345. Point B corresponds to a higher fan pressure rise than Point A, and the same air flow rate.
-
-![](media/image8006.png)
-
-Figure 345. Effect of dirty air filter on variable speed fan operation – flow rate maintained 
-
-The required airflow rate m can be maintained while the fan pressure rise <span>$\Delta P$</span>  is increased to <span>$\Delta P_{df}$</span>. This leads to higher fan power <span>$\dot Q_{tot,df}$</span> and higher power entering the air <span>$\dot Q_{toair,df}$</span>, and thus changes the specific enthalpies of the fan outlet air stream (<span>$h_{out,df}$</span>).
-
-<div>$$ f_{flow,df} = m / m_{design,df} $$</div>
-
-<div>$$ f_{pl,df} = c_{1} + c_{2}*f_{flow,df} + c_{3}*f_{flow,df}^2 + c_{4}*f_{flow,df}^3 + c_{5}*f_{flow,df}^4 $$</div>
-
-<div>$$ \dot{Q}_{tot,df} = f_{pl,df} \times m_{design,df} \times \Delta P_{df} / (e_{tot} \times \rho_{air} ) $$</div>
-
-<div>$$ \dot{Q}_{shaft,df} = e_{motor} \times \dot{Q}_{tot, df} $$</div>
-
-<div>$$ \dot{Q}_{toair,df} = \dot{Q}_{shaft,df} +( \dot{Q}_{tot,df} - \dot{Q}_{shaft,df}) \times f_{motortoair} $$</div>
-
-<div>$$ h_{out,df} = h_{in} + \dot{Q}_{toair,df} / m $$</div>
-
-Where,
-
-$e_{tot}$ is the motor efficiency;
-
-$f_{flow}$ is the flow fraction or part-load ratio;
-
-$f_{pl}$ is the part load factor;
-
-$m$ is the air mass flow in kg/s;
-
-$h_{in}$ is the inlet air stream specific enthalpies in J/kg;
-
-$h_{out}$ is the outlet air stream specific enthalpies in J/kg;
-
-$\dot{Q}_{tot}$ is the fan power in watts;
-
-$\dot{Q}_{toair}$ is the power entering the air in watts;
-
-$\dot{Q}_{shaft}$ is the fan shaft power in watts;
-
-$\Delta P$ is the fan pressure increase in Pascal;
-
-$_{design}$ is for the parameters in the design condition;
-
-$_{df}$ is for the parameters in the dirty filter case.
-
-**(b) The variable speed fan cannot increase in speed sufficiently to maintain the required airflow rate.**
-
-In this case, the fan operation state changes from point A (intersection of the fan curve corresponding to a lower speed and the system curve with clean filters) to point B (intersection of the fan curve corresponding to a higher speed and the system curve with dirty filters), as shown in Figure 346. Point B corresponds to a higher fan pressure rise and a lower air flow rate than Point A.
-
-![](media/image8007.png)
-
-Figure 346. Effect of dirty air filter on variable speed fan operation – flow rate reduced 
-
-The airflow rate m is reduced to $m_{df}$ while the fan design pressure rise $\Delta P$ is increased to $\Delta P_{df}$. Similarly to case (a), the fan power (<span>$\dot Q_{tot}$</span>), the power entering the air (<span>$\dot Q_{toair}$</span>), and the specific enthalpies of the fan outlet air stream (<span>$h_{out}$</span>) are all affected. Different from case (a), however, the fan power (<span>$\dot Q_{tot}$</span>) may either increase or decrease, depending on the degree of the airflow rate decrease and pressure rise increase. Also note that <span>$f\_{flow,df}$</span> is always 1 in this case, since the fan runs at its maximum speed.
-
-<div>$$ f_{flow,df} = 1 $$</div>
-
-<div>$$ f_{pl,df} = c_{1} + c_{2}*f_{flow,df} + c_{3}*f_{flow,df}^2 + c_{4}*f_{flow,df}^3 + c_{5}*f_{flow,df}^4 $$</div>
-
-<div>$$ \dot{Q}_{tot,df} = f_{pl,df} \times m_{design,df} \times \Delta P_{df} / (e_{tot} \times \rho_{air} ) $$</div>
-
-<div>$$ \dot{Q}_{shaft,df} = e_{motor} \times \dot{Q}_{tot, df} $$</div>
-
-<div>$$ \dot{Q}_{toair,df} = \dot{Q}_{shaft,df} +( \dot{Q}_{tot,df} - \dot{Q}_{shaft,df}) \times f_{motortoair} $$</div>
-
-<div>$$ h_{out,df} = h_{in} + \dot{Q}_{toair,df} / m_{design,df} $$</div>
-
-Where,
-
-$e_{tot}$ is the motor efficiency;
-
-$f_{flow}$ is the flow fraction or part-load ratio;
-
-$f_{pl}$ is the part load factor;
-
-$m$ is the air mass flow in kg/s;
-
-$h_{in}$ is the inlet air stream specific enthalpies in J/kg;
-
-$h_{out}$ is the outlet air stream specific enthalpies in J/kg;
-
-$\dot{Q}_{tot}$ is the fan power in watts;
-
-$\dot{Q}_{toair}$ is the power entering the air in watts;
-
-$\dot{Q}_{shaft}$ is the fan shaft power in watts;
-
-$\Delta P$ is the fan pressure increase in Pascal;
-
-$_{design}$ is for the parameters in the design condition;
-
-$_{df}$ is for the parameters in the dirty filter case.
-
-**(c) The constant speed fan cannot maintain the design airflow rate.**
-
-In this case, the fan operation state changes from point A (intersection of the fan curve and the system curve with clean filters) to point B (intersection of the fan curve and the system curve with dirty filters), as shown in Figure 347. Point B corresponds to a higher fan pressure rise and a lower air flow rate than Point A.
-
-![](media/image8008.png)
-
-Figure 347. Effect of dirty air filter on constant speed fan operation
-
-Similarly to case (b), the airflow rate m is reduced to <span>$m_{df}$</span> while the fan pressure rise $\Delta P$ is increased to <span>$\Delta P_{df}$</span>. This results in the variations of the fan power (<span>$\dot Q_{tot}$</span>), the power entering the air (<span>$\dot Q_{toair}$</span>), and the specific enthalpies of the fan outlet air stream (<span>$h_{out}$</span>).
-
-<div>$$ \dot{Q}_{tot,df} = m_{design,df} \times \Delta P_{df} / (e_{tot} \times \rho_{air} ) $$</div>
-
-<div>$$ \dot{Q}_{shaft,df} = e_{motor} \times \dot{Q}_{tot, df} $$</div>
-
-<div>$$ \dot{Q}_{toair,df} = \dot{Q}_{shaft,df} +( \dot{Q}_{tot,df} - \dot{Q}_{shaft,df}) \times f_{motortoair} $$</div>
-
-<div>$$ h_{out,df} = h_{in} + \dot{Q}_{toair,df} / m_{design,df} $$</div>
-
-Where,
-
-$e_{tot}$ is the motor efficiency;
-
-$m$ is the air mass flow in kg/s;
-
-$h_{in}$ is the inlet air stream specific enthalpies in J/kg;
-
-$h_{out}$ is the outlet air stream specific enthalpies in J/kg;
-
-$\dot{Q}_{tot}$ is the fan power in watts;
-
-$\dot{Q}_{toair}$ is the power entering the air in watts;
-
-$\dot{Q}_{shaft}$ is the fan shaft power in watts;
-
-$\Delta P$ is the fan pressure increase in Pascal;
-
-$_{design}$ is for the parameters in the design condition;
-
-$_{df}$ is for the parameters in the dirty filter case.
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diff --git a/doc/src/docs/EngineeringReference/media/image1827.svg b/doc/src/docs/EngineeringReference/media/image1827.svg
deleted file mode 100644
index aca483c9a56..00000000000
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diff --git a/doc/src/docs/EngineeringReference/media/image1957.svg b/doc/src/docs/EngineeringReference/media/image1957.svg
deleted file mode 100644
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diff --git a/doc/src/docs/EngineeringReference/media/image1976.svg b/doc/src/docs/EngineeringReference/media/image1976.svg
deleted file mode 100644
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diff --git a/doc/src/docs/EngineeringReference/media/image34.svg b/doc/src/docs/EngineeringReference/media/image34.svg
deleted file mode 100644
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diff --git a/doc/src/docs/EngineeringReference/media/image4240.svg b/doc/src/docs/EngineeringReference/media/image4240.svg
deleted file mode 100644
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deleted file mode 100644
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diff --git a/doc/src/docs/EngineeringReference/media/image4897.svg b/doc/src/docs/EngineeringReference/media/image4897.svg
deleted file mode 100644
index d2c9a393c2c..00000000000
--- a/doc/src/docs/EngineeringReference/media/image4897.svg
+++ /dev/null
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diff --git a/doc/src/docs/EngineeringReference/media/image7528.svg b/doc/src/docs/EngineeringReference/media/image7528.svg
deleted file mode 100644
index aba198abef2..00000000000
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diff --git a/doc/src/docs/ExternalInterfaces_Application_Guide/ExternalInterfaces_Application_Guide.md b/doc/src/docs/ExternalInterfaces_Application_Guide/ExternalInterfaces_Application_Guide.md
deleted file mode 100644
index a517620605f..00000000000
--- a/doc/src/docs/ExternalInterfaces_Application_Guide/ExternalInterfaces_Application_Guide.md
+++ /dev/null
@@ -1,1306 +0,0 @@
-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>External Interface(s) Application Guide</h1>
-<h2>Guide for using EnergyPlus with External Interface(s)</h2>
-<br/>
-<p><i>(internalize these external details...)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-External Interface(s)
-=====================
-
-Introduction
-------------
-
-The ExternalInterface allows coupling EnergyPlus to the Building Controls Virtual Test Bed (BCVTB). It supports the import of Functional Mock-up Units (FMUs) for co-simulation as well as the export of EnergyPlus as a FMU for co-simulation. BCVTB is a software environment that allows expert users to couple different simulation programs for distributed simulation or for a real-time simulation that is connected to a building control system. For example, the BCVTB allows simulation of the building envelope and HVAC system in EnergyPlus and the control logic in MATLAB/Simulink, while exchanging data between the two programs as they simulate. The BCVTB can be downloaded from http://simulationresearch.lbl.gov/bcvtb. A FMU is a component which implements the Functional Mock-up Interface (FMI) standard (http://www.modelisar.com).
-
-Coupling EnergyPlus with the Building Controls Virtual Test Bed
----------------------------------------------------------------
-
-### Algorithm for data exchange
-
-The process in which at least two simulators solve initial-value differential equations that are coupled to each other is called co-simulation. Various algorithms are possible for the data exchange. In the BCVTB, data are exchanged between its client programs, including EnergyPlus, using a fixed synchronization time step. There is no iteration between the clients. In the co-simulation literature, this coupling scheme is referred to as *quasi-dynamic coupling*, *loose coupling* or *ping-pong coupling* (Hensen 1999, Zhai and Chen 2005).
-
-The algorithm for exchanging data is as follows: Suppose we have a system with two clients, with client 1 being EnergyPlus and client 2 being, for example, the Simulink program from Mathworks. Suppose each client solves an initial-value ordinary differential equation that is coupled to the differential equation of the other client. Let <span>\(N\in\mathbf{N}\)</span> denote the number of time steps and let <span>\(k\in\left\{1,...,N\right\}\)</span> denote the time steps. We will use the subscripts *1* and *2* to denote the state variable and the function that computes the next state variable of the simulator *1* and *2*, respectively.
-
-The simulator *1* computes, for <span>\(k\in\left\{1,...,N-1\right\}\)</span> the sequence
-
-*x<sub>1</sub>(k+1) = f<sub>1</sub>(x<sub>1</sub>(k), x<sub>2</sub>(k))*
-
-and, similarly, the simulator *2* computes the sequence
-
-*x<sub>2</sub>(k+1) = f<sub>2</sub>(x<sub>2</sub>(k), x<sub>1</sub>(k))*
-
-with initial conditions *x<sub>1</sub>(0) = x<sub>1,0</sub>* and *x<sub>2</sub>(0) = x<sub>2,0</sub>*.
-
-To advance from time *k* to *k+1*, each simulator uses its own time integration algorithm. At the end of the time step, the simulator *1* sends the new state *x<sub>1</sub>(k+1)* to the BCVTB and it receives the state *x<sub>2</sub>(k+1)* from the BCVTB. The same procedure is done with the simulator *2*. The BCVTB synchronizes the data in such a way that it does not matter which of the two simulators is called first.
-
-In comparison to numerical methods of differential equations, this scheme is identical to an explicit Euler integration, which is an integration algorithm that computes for an ordinary differential equation with specified initial values,
-
-*dx/dt = h(x),*
-
-*x(0)  = x<sub>0</sub>,*
-
-on the time interval *t* *∈ [0, 1]*, the following sequence:
-
-<table class="table table-striped">
-<tr>
-<td>Step 0:</td>
-<td>Initialize counter k=0 and number of steps <span>\(N\in\mathbf{N}\)</span>.</td>
-</tr>
-<tr>
-<td> </td>
-<td>Set initial state x(k) = x<sub>0</sub> and set time step Dt = 1/N.</td>
-</tr>
-<tr>
-<td>Step 1:</td>
-<td>Compute new state x(k+1) = x(k) + h(x(k)) Dt.</td>
-</tr>
-<tr>
-<td> </td>
-<td>Replace k by k+1.</td>
-</tr>
-<tr>
-<td>Step 2:</td>
-<td>If k=N stop, else go to Step 1.</td>
-</tr>
-</table>
-
-In the situation where the differential equation is solved using co-simulation, the above algorithm becomes
-
-<table class="table table-striped">
-<tr>
-<td>Step 0:</td>
-<td>Initialize counter k=0 and number of steps <span>\(N\in\mathbf{N}\)</span>.</td>
-</tr>
-<tr>
-<td> </td>
-<td>Set initial state x<sub>1</sub>(k) = x<sub>1,0</sub> and x<sub>2</sub>(k) = x<sub>2,0</sub>. Set the time step Dt = 1/N.</td>
-</tr>
-<tr>
-<td>Step 1:</td>
-<td>Compute new states
-  x<sub>1</sub>(k+1) = x<sub>1</sub>(k) + f<sub>1</sub>(x<sub>1</sub>(k), x<sub>2</sub>(k)) Dt, and
-  x<sub>2</sub>(k+1) = x<sub>2</sub>(k) + f<sub>2</sub>(x<sub>2</sub>(k), x<sub>1</sub>(k)) Dt.</td>
-</tr>
-<tr>
-<td> </td>
-<td>Replace k by k+1.</td>
-</tr>
-<tr>
-<td>Step 2:</td>
-<td>If k=N stop, else go to Step 1.</td>
-</tr>
-</table>
-
-This algorithm is implemented in the BCVTB. Note that there is no iteration between the two simulators.
-
-BCVTB Examples
---------------
-
-### Architecture of System
-
-The figure below shows the architecture of the connection between EnergyPlus and the BCVTB. The black objects are explained in this application guide, whereas the grey items are not specific to EnergyPlus and are explained in the BCVTB documentation. The BCVTB connects to the external interface in EnergyPlus. In the external interface, the input/output signals that are exchanged between the BCVTB and EnergyPlus are mapped to EnergyPlus objects. The subject of this External Interface Application Guide is how to configure this mapping and how to use these objects. For a detailed explanation of the grey items, we refer to the BCVTB documentation.
-
-![](media/image004.png)
-
-Figure 1: Architecture of the BCVTB with the EnergyPlus client (black) and other clients (grey).
-
-The external interface can map to three EnergyPlus input objects called ExternalInterface:Schedule, ExternalInterface:Actuator and ExternalInterface:Variable. The ExternalInterface:Schedule can be used to overwrite schedules, and the other two objects can be used in place of Energy Management System (EMS) actuators and EMS variables. The objects have similar functionality as the objects Schedule:Compact, EnergyManagementSystem:Actuator and EnergyManagementSystem:GlobalVariable, except that their numerical value is obtained from the external interface at the beginning of each zone time step, and will remain constant during this zone time step.
-
-Compared to EnergyManagementSystem:Actuator, the object ExternalInterface:Actuator has an optional field called “initial value.� If a value is specified for this field, then this value will be used during the warm-up period and the system sizing. If unspecified, then the numerical value for this object will only be used during the time stepping. Since actuators always overwrite other objects (such as a schedule), all these objects have values that are defined during the warm-up and the system sizing even if no initial value is specified. For the objects  ExternalInterface:Schedule and ExternalInterface:Variable, the field “initial value� is required, and its value will be used during the warm-up period and the system-sizing.
-
-ExternalInterface:Variable is a global variable from the point of view of the EMS language. Thus, it can be used within any EnergyManagementSystem:Program in the same way as an EnergyManagementSystem:GlobalVariable or an EnergyManagementSystem:Sensor can be used.
-
-Although variables of type ExternalInterface:Variable can be assigned to EnergyManagmentSystem:Actuator objects, for convenience, there is also an object called ExternalInterface:Actuator. This object behaves identically to EnergyManagmentSystem:Actuator, with the following exceptions:
-
-- Its value is assigned by the external interface.
-
-- Its value is fixed during the zone time step because this is the synchronization time step for the external interface.
-
-The external interface can also map to the EnergyPlus objects Output:Variable and EnergyManagementSystem:OutputVariable. These objects can be used to send data from EnergyPlus to the BCVTB at each zone time step.
-
-We will now present examples that use all of these objects. The following table shows which EnergyPlus features are used in the examples, which are all distributed with the BCVTB installation that can be obtained from the LBNL web site. Note – these examples are NOT distributed with EnergyPlus installation because you need the special software to make them work.
-
-Table 1. Overview of the EnergyPlus objects used in Examples
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Example 1</th>
-<th>Example 2</th>
-<th>Example 3</th>
-</tr>
-<tr>
-<td>ExternalInterface:Schedule</td>
-<td>x</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>ExternalInterface:Actuator</td>
-<td> </td>
-<td>X</td>
-<td> </td>
-</tr>
-<tr>
-<td>ExternalInterface:Variable</td>
-<td> </td>
-<td> </td>
-<td>x</td>
-</tr>
-<tr>
-<td>Output:Variable</td>
-<td>x</td>
-<td>X</td>
-<td>x</td>
-</tr>
-<tr>
-<td>EnergyManagementSystem:OutputVariable</td>
-<td> </td>
-<td> </td>
-<td>x</td>
-</tr>
-</table>
-
-To configure the data exchange, the following three steps are required from the user:
-
-1)   Create an EnergyPlus idf file.
-
-2)   Create an xml file that defines the mapping between EnergyPlus and BCVTB variables.
-
-3)   Create a Ptolemy model.
-
-These steps are described in the examples below. Prior to discussing the examples, we will explain the syntax of the xml configuration file that defines how data are mapped between the external interface and EnergyPlus.
-
-### XML Syntax
-
-This section describes the syntax of the xml file that configures the data mapping between EnergyPlus and the external interface.
-
-The data mapping between EnergyPlus and the external interface is defined in an xml file called variables.cfg. This file needs to be in the same directory as the EnergyPlus idf file.
-
-The file has the following header:
-
-&lt;?xml version="1.0" encoding="ISO-8859-1"?&gt;
-
-&lt;!DOCTYPE BCVTB-variables SYSTEM "variables.dtd"&gt;
-
-Following the header is an element of the form
-
-&lt;BCVTB-variables&gt;
-
-
-
-&lt;/BCVTB-variables&gt;
-
-This element will contain child elements that define the variable mapping. In between the element tags, a user needs to specify how the exchanged data is mapped to EnergyPlus objects. Hence, the order of these elements matter, and it need to be the same as the order of the elements in the input and output signal vector of the BCVTB actor that calls EnergyPlus. The exchanged variables are declared in elements that are called “variable� and have an attribute “source.� As described above, the external interface can send data to ExternalInterface:Schedule, ExternalInterface:Actuator, ExternalInterface:Variable. For these objects, the “source� attribute needs to be set to “Ptolemy,� because they are computed in Ptolemy. The xml elements for these objects look as follows:
-
-For ExternalInterface:Schedule, use
-
-&lt;variable source="Ptolemy"&gt;
-
-    &lt;EnergyPlus schedule="NAME"/&gt;
-
-  &lt;/variable&gt;
-
-where NAME needs to be the EnergyPlus schedule name. For ExternalInterface:Actuator, use
-
-&lt;variable source="Ptolemy"&gt;
-
-    &lt;EnergyPlus actuator="NAME" /&gt;
-
-  &lt;/variable&gt;
-
-where NAME needs to be the EnergyPlus actuator name. For ExternalInterface:Variable, use
-
-  &lt;variable source="Ptolemy"&gt;
-
-    &lt;EnergyPlus variable="NAME"/&gt;
-
-  &lt;/variable&gt;
-
-where NAME needs to be the EnergyPlus Energy Runtime Language (Erl) variable name.
-
-The external interface can also read data from any Output:Variable and EnergyManagementSystem:OutputVariable. For these objects, set the “source� attribute to “EnergyPlus,� because they are computed by EnergyPlus. The read an Output:Variable, use
-
-  &lt;variable source="EnergyPlus"&gt;
-
-    &lt;EnergyPlus name="NAME" type="TYPE"/&gt; 
-
-  &lt;/variable&gt;
-
-where NAME needs to be the EnergyPlus “Variable Name� (such as ZONE/SYS AIR TEMP) and TYPE needs to be the EnergyPlus “Key Value� (such as ZONE ONE). To read an EnergyManagementSystem:OutputVariable, use
-
-&lt;variable source="EnergyPlus"&gt;
-
-    &lt;EnergyPlus name="EMS" type="TYPE"/&gt;
-
-&lt;/variable&gt;
-
-i.e., the attribute “name� must be EMS, and the attribute “type� must be set to the EMS variable name.
-
-Complete examples of these xml files are presented below.
-
-### Example 1: Interface using ExternalInterface:Schedule
-
-In this example, a controller that is implemented in the BCVTB computes the room temperature set points for cooling and heating. The example can be found in the BCVTB distribution in the folder examples/ePlusX-schedule, where X stands for the EnergyPlus version number.
-
-Suppose we need to send from the BCVTB to EnergyPlus a schedule value, and from EnergyPlus to the BCVTB an output variable at each zone time step. This can be accomplished by using an object of type ExternalInterface:Schedule and an object of type Output:Variable.
-
-To interface EnergyPlus using the EMS feature, the following three items are needed:
-
-- An object that instructs EnergyPlus to activate the external interface.
-
-- EnergyPlus objects that write data from the external interface to the EMS.
-
-- A configuration file to configure the data exchange.
-
-#### Creating the EnergyPlus idf file
-
-The EnergyPlus idf file contains the following objects to activate and use the external interface:
-
-- An object that instructs EnergyPlus to activate the external interface.
-
-- An object of type ExternalInterface:Schedule. The external interface will write its values to these objects at each zone time-step.
-
-- Objects of type Output:Variable. Any EnergyPlus output variable can be read by the external interface.
-
-The code below shows how to declare these objects.
-
-To activate the external interface, we use:
-
-```idf
-ExternalInterface,           !- Object to activate the external interface
- PtolemyServer;              !- Name of external interface
-```
-
-To enter schedules to which the external interface writes, we use:
-
-```idf
-! Cooling schedule. This schedule is set directly by the external interface.
-! During warm-up and system-sizing, it is fixed at 24 degC.
-  ExternalInterface:Schedule,
-    TSetCoo,                 !- Name
-    Temperature,             !- ScheduleType
-    24;                      !- Initial value, used during warm-up
-
-
-! Heating schedule. This schedule is set directly by the external interface.
-! During warm-up and system-sizing, it is fixed at 20 degC.
-  ExternalInterface:Schedule,
-    TSetHea,                 !- Name
-    Temperature,             !- ScheduleType
-    20;                      !- Initial value, used during warm-up
-```
-
-
-These schedules can be used as other EnergyPlus schedules. In this example, they are used to change a thermostat setpoint:
-
-```idf
-ThermostatSetpoint:DualSetpoint,
-    DualSetPoint,            !- Name
-    BCVTB-SP-TH,             !- Heating Setpoint Temperature Schedule Name
-    BCVTB-SP-TC;             !- Cooling Setpoint Temperature Schedule Name
-```
-
-
-We also want to read from EnergyPlus output variables, which we declare as
-
-```idf
-Output:Variable,
-    TSetHea,        !- Key Value
-    Schedule Value, !- Variable Name
-    TimeStep;       !- Reporting Frequency
-
-
-Output:Variable,
-    TSetCoo,        !- Key Value
-    Schedule Value, !- Variable Name
-    TimeStep;       !- Reporting Frequency
-```
-
-
-To specify that data should be exchanged every 15 minutes of simulation time, enter in the idf file the section
-
-```idf
-  Timestep,
-    4;          !- Number of Timesteps per Hour
-```
-
-
-#### Creating the configuration file
-
-Note that we have not yet specified the order of the elements in the signal vector that is exchanged between EnergyPlus and the BCVTB. This information is specified in the file variables.cfg. The file variables.cfg needs to be in the same directory as the EnergyPlus idf file. For the objects used in the section above, the file looks like
-```idf
-<?xml version="1.0" encoding="ISO-8859-1"?>
-<!DOCTYPE BCVTB-variables SYSTEM "variables.dtd">
-<BCVTB-variables>
-  <!-- The next two elements send the set points to E+ -->
-  <variable source="Ptolemy">
-    <EnergyPlus schedule="TSetHea"/>
-  </variable>
-  <variable source="Ptolemy">
-    <EnergyPlus schedule="TSetCoo"/>
-  </variable>
-  <!-- The next two elements receive the outdoor and zone air temperature from E+ -->
-  <variable source="EnergyPlus">
-   <EnergyPlus name="ENVIRONMENT" type="SITE OUTDOOR AIR DRYBULB TEMPERATURE"/>
-  </variable>
-  <variable source="EnergyPlus">
-    <EnergyPlus name="ZSF1" type="ZONE AIR TEMPERATURE"/>
-  </variable>
-  <!-- The next two elements receive the schedule value as an output from E+ -->
-  <variable source="EnergyPlus">
-    <EnergyPlus name="TSetHea" type="Schedule Value"/>
-  </variable>
-  <variable source="EnergyPlus">
-    <EnergyPlus name="TSetCoo" type="Schedule Value"/>
-  </variable>
-</BCVTB-variables>
-```
-
-
-This file specifies that the actor in the BCVTB that calls EnergyPlus has an input vector with two elements that are computed by Ptolemy (Ptolemy is the name of the software on which the BCVTB is based) and sent to EnergyPlus, and that it has an output vector with four elements that are computed by EnergyPlus and sent to Ptolemy. The order of the elements in each vector is determined by the order in the above XML file. Hence, the input vector that contains the signals sent to EnergyPlus has elements
-
-TSetHea
-
-  TSetCoo
-
-and the output vector that contains values computed by EnergyPlus has elements
-
-Environment (Site Outdoor Air Drybulb Temperature)
-
-  ZSF1 (ZONE AIR TEMPERATURE)
-
-  TSetHea (Schedule Value)
-
-  TSetCoo (Schedule Value)
-
-##### **Creating the Ptolemy model**
-
-To start EnergyPlus from the BCVTB, you will need to create a Ptolemy model.
-
-The model bcvtb/example/ePlus40-schedule/system-windows.xml that is part of the BCVTB installation and that is shown below may be used as a starting point. (For Mac and Linux, use the file system.xml.) In this example, the time step is 15 minutes and the simulation period is four days.
-
-![](media/image005.png)
-
-Figure 2: System model in the BCVTB.
-
-In this model, the Simulator actor that calls EnergyPlus is configured for Windows as follows:
-
-![](media/image006.png)
-
-Figure 3: Configuration of the Simulator actor that calls EnergyPlus on Windows.
-
-Hence, it calls the file “RunEPlus.bat,� with arguments “EMSWindowShadeControl USA\_IL\_Chicago-OHare.Intl.AP.725300\_TMY3.� The working directory is the current directory and the console output is written to the file simulation.log. If EnergyPlus does not communicate with the BCVTB within 10 seconds, the BCVTB will terminate the connection. (See [http://simulationresearch.lbl.gov/bcvtb](http://simulationresearch.lbl.gov/bcvtb) for more detailed documentation about how to configure a BCVTB model that communicates with other programs.)
-
-For Mac OS X and Linux, the configuration is similar:
-
-![](media/image007.png)
-
-Figure 4: Configuration of the Simulator actor that calls EnergyPlus on Mac OS X and on Linux.
-
-This completes the configuration.
-
-### Example 2: Interface using ExternalInterface:Actuator
-
-In this example, a shading controller with a finite state machine is implemented in the BCVTB. Inputs to the controller are the outside temperature and the solar radiation that is incident on the window. The output of the controller is the shading actuation signal.
-
-This example describes how to set up EnergyPlus to exchange data between the BCVTB and EnergyPlus, using an Energy Management System (EMS) actuator. The example can be found in the BCVTB distribution in the folder examples/ePlusX-actuator, where X stands for the EnergyPlus version number.
-
-The object of type ExternalInterface:Actuator behaves identically to EnergyManagmentSystem:Actuator, with the following exceptions:
-
-- Its value is assigned by the external interface.
-
-- Its value is fixed during the zone time step because this is the synchronization time step for the external interface.
-
-To interface EnergyPlus using the EMS feature, the following three items are needed:
-
-1)   An object that instructs EnergyPlus to activate the external interface.
-
-2)   EnergyPlus objects that write data from the external interface to the EMS.
-
-3)   A configuration file to configure the data exchange.
-
-#### Creating the EnergyPlus idf file
-
-The code below shows how to set up an EnergyPlus file that uses EnergyManagmentSystem:Actuator. To activate the external interface, we use:
-
-```idf
-ExternalInterface,           !- Object to activate the external interface
- PtolemyServer;              !- Name of external interface
-```
-
-To declare an actuator that changes the control status of the window with name “Zn001:Wall001:Win001�, we use:
-
-```idf
-ExternalInterface:Actuator,
-    Zn001_Wall001_Win001_Shading_Deploy_Status,  !- Name
-    Zn001:Wall001:Win001,    !- Actuated Component Unique Name
-    Window Shading Control,  !- Actuated Component Type
-    Control Status,          !- Actuated Component Control Type
-     ;                       ! initial value
-```
-
-Thus, the entry is identical with EnergyManagmentSystem:Actuator, except for the additional optional field that specifies the initial value. If unspecified, then the actuator will only be used during the time stepping, but not during the warm-up and the system sizing. Since actuators always overwrite other objects (such as a schedule), all these objects have values that are defined during the warm-up and the system sizing even if no initial value is specified.
-
-We also want to read from EnergyPlus the outdoor temperature, the zone air temperature, the solar radiation that is incident on the window, and the fraction of time that the shading is on. Thus, we declare the output variables
-
-```idf
-Output:Variable,
-   Environment,                            !- Key Value
-   Site Outdoor Air Drybulb Temperature,   !- Variable Name
-   timestep;                               !- Reporting Frequency
-
-
-Output:Variable,
-   *,                                      !- Key Value
-   Zone Mean Air Temperature,              !- Variable Name
-   timestep;                               !- Reporting Frequency
-
-
-Output:Variable,
-   Zn001:Wall001:Win001,                   !- Key Value
-   Surface Outside Face Incident Solar Radiation Rate per Area, !- Var Name
-   timestep;                               !- Reporting Frequency
-
-
-Output:Variable,
-   *,                                      !- Key Value
-   Surface Shading Device Is On Time Fraction,  !- Variable Name
-   timestep;                               !- Reporting Frequency
-```
-
-
-To specify that data should be exchanged every 10 minutes of simulation time, we enter in the idf file the section
-
-```idf
-  Timestep,
-    6;          !- Number of Timesteps per Hour
-```
-
-##### **Creating the configuration file**
-
-Note that we have not yet specified the order of the elements in the signal vector that is exchanged between EnergyPlus and the BCVTB. This information is specified in the file variables.cfg. The file variables.cfg needs to be in the same directory as the EnergyPlus idf file. For the objects used in the section above, the file looks like
-
-```idf
-<?xml version="1.0" encoding="ISO-8859-1"?>
-<!DOCTYPE BCVTB-variables SYSTEM "variables.dtd">
-<BCVTB-variables>
-  <variable source="EnergyPlus">
-   <EnergyPlus name="ENVIRONMENT" type="SITE OUTDOOR AIR DRYBULB TEMPERATURE"/>
-  </variable>
-  <variable source="EnergyPlus">
-    <EnergyPlus name="WEST ZONE" type="Zone Mean Air Temperature"/>
-  </variable>
-  <variable source="EnergyPlus">
-    <EnergyPlus name="Zn001:Wall001:Win001" type="Surface Outside Face Incident Solar Radiation Rate per Area"/>
-  </variable>
-  <variable source="EnergyPlus">
-    <EnergyPlus name="Zn001:Wall001:Win001" type="Surface Shading Device Is On Time Fraction"/>
-  </variable>
-  <variable source="Ptolemy">
-    <EnergyPlus actuator="Zn001_Wall001_Win001_Shading_Deploy_Status" />
-  </variable>
-</BCVTB-variables>
-```
-
-
-This file specifies that the actor in the BCVTB that calls EnergyPlus has an input vector with one element that will be written to the actuator, and that it has an output vector with four elements that are computed by EnergyPlus and sent to Ptolemy. The order of the elements in each vector is determined by the order in the above XML file. Hence, the output vector that contains the signals computed by EnergyPlus has elements
-
-```
-  ENVIRONMENT (SITE OUTDOOR AIR DRYBULB TEMPERATURE)
-  WEST ZONE (Zone Mean Air Temperature)
-  Zn001:Wall001:Win001 (Surface Outside Face Incident Solar Radiation Rate per Area)
-  Zn001:Wall001:Win001 (Surface Shading Device Is On Time Fraction)
-```
-
-The configuration of the Ptolemy model is identical to the configuration in Example 1.
-
-### Example 3: Interface using ExternalInterface:Variable
-
-This example implements the same controller as the Example 2. However, the interface with EnergyPlus is done using an external interface variable instead of an external interface actuator. In addition, the example uses an EnergyManagementSystem:OutputVariable to set up data that will be read by the external interface.
-
-Similarly to EnergyManagementSystem:GlobalVariable, an ExternalInterface:Variable can be used in any EnergyManagementSystem:Program. The subject of this example is to illustrate how an ExternalInterface:Variable can be set up for use in an EnergyManagementSystem:Program. The example can be found in the BCVTB distribution in the folder examples/ePlusX-variable, where X stands for the EnergyPlus version number.
-
-To interface EnergyPlus using an external interface variable, the following items are needed:
-
-- An object that instructs EnergyPlus to activate the external interface.
-
-- EnergyPlus objects that write data from the external interface to the EMS.
-
-- A configuration file to configure the data exchange.
-
-#### Creating the EnergyPlus idf file
-
-To write data from the external interface to an EnergyPlus EMS variable, an EnergyPlus object of the following entry may be used in the idf file:
-
-```idf
-ExternalInterface,           !- Object to activate the external interface
-   PtolemyServer;            !- Name of external interface
-
-
-  ExternalInterface:Variable,
-    yShade,                  !- Name of Erl variable
-    1;                       !- Initial value
-```
-
-
-During the warm-up period and the system-sizing, the variable will be set to its initial value. Afterwards, the value will be assigned from the external interface at each beginning of a zone time step and kept constant during the zone time step. From the point of view of the EMS language, ExternalInterface:Variable can be used like any global variable. Thus, it can be used within any EnergyManagementSystem:Program in the same way as an EnergyManagementSystem:GlobalVariable or an EnergyManagementSystem:Sensor.
-
-This idf section above activates the external interface and declares a variable with name yShade that can be used in an Erl program to actuate the shading control of the window “Zn001:Wall001:Win001� as follows:
-
-```idf
-! EMS program. The first assignments sets the shading status and converts it into the
-!              EnergyPlus signal (i.e., replace 1 by 6).
-!              The second assignment sets yShade to
-!              an EnergyManagementSystem:OutputVariable
-!              which will be read by the external interface.
-  EnergyManagementSystem:Program,
-    Set_Shade_Control_State,          !- Name
-    Set Shade_Signal = 6*yShade,      !- Program Line 1
-    Set Shade_Signal_01 = yShade+0.1; !- Program Line 2
-
-
-! Declare an actuator to which the EnergyManagementSystem:Program will write
-  EnergyManagementSystem:Actuator,
-    Shade_Signal,  !- Name
-    Zn001:Wall001:Win001,             !- Actuated Component Unique Name
-    Window Shading Control,           !- Actuated Component Type
-    Control Status;                   !- Actuated Component Control Type
-
-
-! Declare a global variable to which the EnergyManagementSystem:Program will write
-  EnergyManagementSystem:GlobalVariable,
-    Shade_Signal_01;                  !- Name of Erl variable
-```
-
-
-We want to read from EnergyPlus the outdoor temperature, the zone air temperature and the solar radiation that is incident on the window. Thus, we declare
-
-```idf
-Output:Variable,
-   Environment,                 !- Key Value
-   Site Outdoor Air Drybulb Temperature,            !- Variable Name
-   timestep;                    !- Reporting Frequency
-
-
-  Output:Variable,
-  *,                          !- Key Value
-  Zone Mean Air Temperature,  !- Variable Name
-  timestep;                   !- Reporting Frequency
-
-
-  Output:Variable,
-  Zn001:Wall001:Win001,       !- Key Value
-  Surface Outside Face Incident Solar Radiation Rate per Area, !- Var Name
-  timestep;                   !- Reporting Frequency
-```
-
-
-In addition, we want to output the variable “Erl Shading Control Status� that has been set up as
-
-```idf
-! Declare an output variable. This variable is equal to the shahing signal + 0.1
-! It will be reah by the external interface to hemonstrate how to receive variables.
-  EnergyManagementSystem:OutputVariable,
-    Erl Shahing Control Status,  !- Name
-    Shahe_Signal_01,             !- EMS Variable Name
-    Averageh,                    !- Type of Data in Variable
-    ZoneTimeStep;                !- Uphate Frequency
-```
-
-
-To specify that data should be exchanged every 10 minutes of simulation time, enter in the idf file the section
-
-```idf
-  Timestep,
-    6;          !- Number of Timesteps per Hour
-```
-
-#### Creating the configuration file
-
-Note that we have not yet specified the order of the elements in the signal vector that is exchanged between EnergyPlus and the BCVTB. This information is specified in the file variables.cfg. The file variables.cfg needs to be in the same directory as the EnergyPlus idf file. For the objects used in the section above, the file looks like
-
-```idf
-<?xml version="1.0" encoding="ISO-8859-1"?>
-<!DOCTYPE BCVTB-variables SYSTEM "variables.dtd">
-<BCVTB-variables>
-  <variable source="Ptolemy">
-    <EnergyPlus variable="yShade"/>
-  </variable>
-  <variable source="EnergyPlus">
-    <EnergyPlus name="ENVIRONMENT" type="SITE OUTDOOR AIR DRYBULB TEMPERATURE"/>
-  </variable>
-  <variable source="EnergyPlus">
-    <EnergyPlus name="WEST ZONE" type="Zone Mean Air Temperature"/>
-  </variable>
-  <variable source="EnergyPlus">
-    <EnergyPlus name="Zn001:Wall001:Win001" type="Surface Outside Face Incident Solar Radiation Rate per Area"/>
-  </variable>
-  <variable source="EnergyPlus">
-    <EnergyPlus name="EMS" type="Erl Shading Control Status"/>
-  </variable>
-</BCVTB-variables>
-```
-
-
-This file specifies that the actor in the BCVTB that calls EnergyPlus has an input vector with one element that will be written to the actuator, and that it has an output vector with four elements that are computed by EnergyPlus and sent to Ptolemy. The order of the elements in each vector is determined by the order in the above XML file. Note that the fourth element has the name “EMS� because it is an EnergyManagementSystem:OutputVariable. Hence, the output vector that contains the signals computed by EnergyPlus has elements
-
-```
-  ENVIRONMENT (SITE OUTDOOR AIR DRYBULB TEMPERATURE)
-  WEST ZONE (Zone Mean Air Temperature)
-  Zn001:Wall001:Win001 (Surface Outside Face Incident Solar Radiation Rate per Area)
-  EMS (Erl Shading Control Status)
-```
-
-The configuration of the Ptolemy model is identical to the configuration in the previous examples.
-
-Coupling EnergyPlus with Functional Mock-up Units for co-simulation
--------------------------------------------------------------------
-
-The Functional Mock-up Unit (FMU) for co-simulation import for EnergyPlus allows EnergyPlus to conduct co-simulation with various programs that are packaged as FMUs. A FMU is a component which implements the Functional Mock-up Interface (FMI) standard (http://www.modelisar.com).
-
-A FMU is distributed in the form of a zip file that may contain physical models, model descriptions, source code, and executable programs for various platforms. The FMU for co-simulation import provides EnergyPlus with a standard interface to conduct and control co-simulation with an arbitrary number of FMUs without any middle-ware, such as the Building Controls Virtual Test Bed (BCVTB Documentation, 2011).
-
-The FMU for co-simulation import allows coupling of continuous-time and discrete-time models exported from different simulation programs. In the current implementation, EnergyPlus is implemented as the co-simulation master. It controls the data exchange between the subsystems and the synchronization of all slave simulation programs.
-
-The FMU for co-simulation import enables the direct link between the EnergyPlus kernel and other simulation tools. It will make the co-simulation easier to conduct as no middle-ware is involved. This direct link will decrease run-time by eliminating the transaction layer. In addition, by separating the co-simulation interface from the EnergyPlus kernel, the FMU interface is reusable when EnergyPlus is updated. Furthermore, the FMU contains executable files that have the same interface to EnergyPlus regardless of their original programming environment. Some commercial tools allow running their FMU without licensing requirement.
-
-**Notes:**
-
-1)   The current implementation of FMU for co-simulation is only supported on Windows and Linux.
-
-2)   FMUs must be in a folder to which the user has *write* access.
-
-### Data exchange between EnergyPlus and FMUs
-
-Prior to describing the data exchange between EnergyPlus and FMUs, some definitions and terminologies used in the remainder of this document will be introduced.
-
-A variable of a system described by a system of differential algebraic equations (DAE) is defined as differential variable if its derivatives are present in the DAE. A variable of a system described by a system of DAE is defined as algebraic if its derivatives do not appear explicitly in the DAE (Fabian et al., 2008).
-
-![](media/image008.png)
-
-Figure 5: System with two variables that could be either differential or algebraic variables.
-
-Because in subsequent discussions, it will be distinguished between algebraic and differential variables, a notation for different system of equations that involve algebraic and differential variables will be introduced. Let <span>\(q\in\mathbf{N}\)</span>, then
-
-- If x<sub>1</sub> and x<sub>2</sub> are differential variables, then the system is
-
-<span>\(F\left(\dot x_1,x_1,\dot x_2,x_2,u,t\right) = 0\)</span> with *F*: �<sup>n</sup> x �<sup>n</sup> x �<sup>m</sup> x �<sup>m</sup> x �<sup>q</sup> x � → �<sup>n+m</sup>.
-
-- If x<sub>1</sub> is a differential variable and x<sub>2</sub> is an algebraic variable, then the system is
-
-<span>\(G\left(\dot x_1,x_1,x_2,u,t\right) = 0\)</span> with *G*: �<sup>n</sup> x �<sup>n</sup> x �<sup>m</sup> x �<sup>q</sup> x � → �<sup>n+m</sup>.
-
-- If x<sub>1</sub> is an algebraic variable and x<sub>2</sub> is a differential variable, then the system is
-
-<span>\(H\left(x_1,\dot x_2,x_2,u,t\right) = 0\)</span> with *H:* �<sup>n</sup> x�<sup>m</sup> x�<sup>m</sup> x�<sup>q</sup> x� →�<sup>n+m</sup>.
-
-- If x<sub>1</sub> is an algebraic variable and x<sub>2</sub> is an algebraic variable, then the system is
-
-<span>\(I\left(x_1,x_2,u,t\right)=0\)</span> with *I*: �<sup>n</sup> x�<sup>m</sup> x�<sup>q</sup> x� →�<sup>n+m</sup>.
-
-Figure 6 shows a case where a FMU is linked to an EnergyPlus model for co-simulation. The FMU and EnergyPlus could be linked through differential or algebraic variables.
-
-![Picture5.png](media/image016.png)
-
-Figure 6: System with one FMU linked to EnergyPlus.
-HERHERHEHERHERHERHERH
-Table 2 shows the different system configurations that are possible.
-
-- In the first case, the variable x<sub>1</sub> and x<sub>2</sub> are differential variables in both systems.
-
-- In the second case, the variable x<sub>1</sub> is a differential variable and the variable x<sub>2</sub> is an algebraic variable.
-
-- In the third case, the variable x<sub>1</sub> is an algebraic variable and the variable x<sub>2</sub> is a differential variable.
-
-- In the fourth case, the variable x<sub>1</sub> is an algebraic variable and the variable x<sub>2</sub> is an algebraic variable.
-
-In the current implementation, it will be focused on the first and the second cases since the third and the fourth cases will constrain the FMU to be solved numerically in the iteration solver loop of EnergyPlus. This will necessitate the ability of the FMU to reject time steps (Modelisar, 2010) which is currently not implemented in the EnergyPlus FMU for co-simulation import. Applications for case 1 and 2 are described in the next sections.
-
-Table 2: Use cases with different system configurations
-
-<table class="table table-striped">
-<tr>
-<th>Case</th>
-<th>EnergyPlus</th>
-<th>FMU (e.g. from Modelica)</th>
-</tr>
-<tr>
-<td>(1)</td>
-<td>Model1 (Differential variable)</td>
-<td>Model2 (Differential variable)</td>
-</tr>
-<tr>
-<td>(2)</td>
-<td>Model1 (Differential variable)</td>
-<td>Model2 (Algebraic variable)</td>
-</tr>
-<tr>
-<td>(3)</td>
-<td>Model1 (Algebraic variable)</td>
-<td>Model2 (Differential variable)</td>
-</tr>
-<tr>
-<td>(4)</td>
-<td>Model1 (Algebraic variable)</td>
-<td>Model2 (Algebraic variable)</td>
-</tr>
-</table>
-
-### Case 1: Linking two systems through differential variables
-
-This case could be for an application where a wall with a phase change material (PCM) is modeled in a FMU and is linked to a room model in EnergyPlus. The room air temperature is the differential variable in EnergyPlus and the temperature of the wall with PCM is the differential variable in the FMU. Each system solves a differential equation that is connected to the differential equation of the other system. For simplicity, we assume that *y<sub>1</sub>(.)* = *x<sub>1</sub>(.) and y<sub>2</sub>(.)* = *x<sub>2</sub>(.).*The systems are described by the ordinary differential equations
-
-dx<sub>1</sub>/dt = f<sub>1</sub>(x<sub>1</sub>, x<sub>2</sub>), with x<sub>1</sub>(0) = x<sub>1,0</sub> ,
-
-dx<sub>2</sub>/dt = f<sub>2</sub>(x<sub>2</sub>, x<sub>1</sub>), with x<sub>2</sub>(0) = x<sub>2,0\\ .</sub>
-
-Let <span>\(N\in\textbf{N}\)</span> denote the number of time steps and let *t<sub>k</sub>* with <span>\(k\in\left\{1,...,N\right\}\)</span> denote the time steps. We will use the subscripts *1* and *2* to denote the variables and the functions that compute the next state variable of the simulator *1* and *2*, respectively.
-
-The first system computes, for <span>\(k\in\left\{0,...,N-1\right\}\)</span> and some <span>\(\tilde{F}_1\)</span>: �<sup>n</sup> x �<sup>m</sup> x � x � → �<sup>n</sup>, the sequence
-
-x<sub>1</sub>(t<sub>k+1</sub>) = <span>\(\tilde{F}_1\)</span>(x<sub>1</sub>(t<sub>k</sub>), x<sub>2</sub>(t<sub>k</sub>), t<sub>k</sub>, t<sub>k+1</sub>)
-
-and, similarly, the simulator *2* computes for some <span>\(\tilde{F}_2\)</span>: �<sup>m</sup> x �<sup>n</sup> x � x � → �<sup>m</sup> the sequence
-
-x<sub>2</sub>(t<sub>k+1</sub>) = <span>\(\tilde{F}_2\)</span>(x<sub>2</sub>(t<sub>k</sub>), x<sub>1</sub>(t<sub>k</sub>), t<sub>k</sub>, t<sub>k+1</sub>)
-
-with initial conditions *x<sub>1</sub>(0) = x<sub>1,0</sub>* and *x<sub>2</sub>(0) = x<sub>2,0.</sub>* <span>\(\tilde{F}_1\)</span> and <span>\(\tilde{F}_2\)</span> *are the functions that are used to compute the value of the state variables at the new time step
-
-To advance from time *t<sub>k</sub>* to *t<sub>k+1</sub>*, each system uses its own time integration algorithm. At the end of the time step, EnergyPlus sends the new state *x<sub>1</sub>(t<sub>k+1</sub>)* to the FMU and it receives the state *x<sub>2</sub>(t<sub>k+1</sub>)* from the FMU. The same procedure is done with the FMU.
-
-### Case 2: Linking two systems through algebraic and differential variables
-
-This case could be for an application where a fan is modeled in a FMU and is linked to a room model in EnergyPlus. The room temperature is the differential variable in EnergyPlus and the pressure difference of the fan is the algebraic variable in the FMU. For simplicity, we assume that *y<sub>1</sub>(.)* = *x<sub>1</sub>(.) and y<sub>2</sub>(.)* = *x<sub>2</sub>(.).* In this application, the systems are described by the following equations
-
-dx<sub>1</sub>/dt = g<sub>1</sub>(x<sub>1</sub>, x<sub>2</sub>), with x<sub>1</sub>(0) = x<sub>1,0,</sub>
-
-0 = g<sub>2</sub>(x<sub>2</sub>, x<sub>1</sub>).
-
-Let <span>\(N\in\mathbf{N}\)</span> denote the number of time steps and let *t<sub>k</sub>* with <span>\(k\in\left\{1,...,N\right\}\)</span> denote the time steps. We use the same subscripts *1* and *2* as for the first case to denote the variable and the function that computes the next variable of the simulator *1* and *2*, respectively.
-
-The first system computes, for <span>\(k\in\left\{0,...,N-1\right\}\)</span> and some <span>\(\tilde{G}_1\)</span>: �<sup>n</sup> x �<sup>m</sup> x � x � → �<sup>n</sup>, the sequence
-
-x<sub>1</sub>(t<sub>k+1</sub>) = <span>\(\tilde{G}_1\)</span>(x<sub>1</sub>(t<sub>k</sub>), x<sub>2</sub>(t<sub>k</sub>), t<sub>k</sub>, t<sub>k+1</sub>)
-
-and, similarly, the simulator *2* computes for some <span>\(\tilde{G}_2\)</span>: �<sup>m</sup> x �<sup>n</sup> x � → �<sup>m</sup> the sequence
-
-x<sub>2</sub>(t<sub>k+1</sub>) = <span>\(\tilde{G}_2\)</span>(x<sub>2</sub>(t<sub>k+1</sub>), x<sub>1</sub>(t<sub>k+1</sub>), t<sub>k+1</sub>)
-
-with initial condition *x<sub>1</sub>(0) = x<sub>1,0</sub>*. <span>\(\tilde{G}_1\)</span> and <span>\(\tilde{G}_2\)</span> are the functions that compute the value of the variables at the new time step.
-
-To advance from time *t<sub>k</sub>* to *t<sub>k+1</sub>*, each system uses its own time integration algorithm. At the end of the time step, EnergyPlus sends the new value *x<sub>1</sub>(t<sub>k+1</sub>)* to the FMU and it receives the value *x<sub>2</sub>(t<sub>k+1</sub>)* from the FMU. The same procedure is done with the FMU.
-
-### Requirements
-
-The current implementation for linking EnergyPlus with the FMUs has the following requirements:
-
-- The data exchange between EnergyPlus and the FMUs is done at the zone time step of EnergyPlus.
-
-- Each FMU is linked to EnergyPlus only through a differential variable in EnergyPlus (see Figure 7 for one FMU).
-
-![](media/image033.png)
-
-Figure 7:System with one FMU linked to EnergyPlus.
-
-- Two or multiple FMUs are linked together only through differential variables in EnergyPlus (see Figure 8 for two FMUs).
-
-![](media/image034.png)
-
-Figure 8: System with two FMUs linked to EnergyPlus.
-
-FMU Examples
-------------
-
-### Architecture of the FMU for co-simulation Import
-
-Figure 9 shows the architecture of the connection between EnergyPlus and two FMUs. EnergyPlus imports the FMUs that connect to its external interface. These FMUs are generated by external simulation environments that implement the FMI Application Programming Interface (API) for co-simulation. See http://www.modelisar.com/tools.html for a list of programs that export FMUs. In the external interface, the input/output signals that are exchanged between the FMUs and EnergyPlus are mapped to EnergyPlus objects. The subject of this External Interface Application Guide is how to configure this mapping and how to use these objects.
-
-![](media/image035.png)
-
-Figure 9: Architecture of the FMU for co-simulation import.
-
-The external interface can map to three EnergyPlus input objects called
-
-- ExternalInterface:FunctionalMockupUnitImport:To:Schedule
-
-- ExternalInterface:FunctionalMockupUnitImport:To:Actuator
-
-- ExternalInterface:FunctionalMockupUnitImport:To:Variable.
-
-The ExternalInterface:FunctionalMockupUnitImport:To:Schedule can be used to overwrite schedules, and the other two objects can be used in place of Energy Management System (EMS) actuators and EMS variables. The objects have similar functionality as the objects Schedule:Compact, EnergyManagementSystem:Actuator and EnergyManagementSystem:GlobalVariable, except that their numerical value is obtained from the external interface at the beginning of each zone time step, and will remain constant during this zone time step.
-
-The external interface also uses the ExternalInterface:FunctionalMockupUnitImport:From:Variable object which  maps to EnergyPlus objects Output:Variable and EnergyManagementSystem:OutputVariable to send data from EnergyPlus to FMUs at each zone time step.
-
-We will now present examples that use all of these objects. The following table shows which EnergyPlus features are used in the examples.
-
-Table 3. Overview of the EnergyPlus objects used in Examples
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Example 1</th>
-<th>Example 2</th>
-<th>Example 3</th>
-</tr>
-<tr>
-<td>ExternalInterface:FunctionalMockupUnitImport:From:Variable</td>
-<td>x</td>
-<td>x</td>
-<td>x</td>
-</tr>
-<tr>
-<td>ExternalInterface:FunctionalMockupUnitImport:To:Schedule</td>
-<td>x</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>ExternalInterface:FunctionalMockupUnitImport:To:Actuator</td>
-<td> </td>
-<td>x</td>
-<td> </td>
-</tr>
-<tr>
-<td>ExternalInterface:FunctionalMockupUnitImport:To:Variable</td>
-<td> </td>
-<td> </td>
-<td>x</td>
-</tr>
-<tr>
-<td>Output:Variable</td>
-<td>x</td>
-<td>x</td>
-<td>x</td>
-</tr>
-</table>
-
-Prior to discussing the examples, we will explain the pre-processing steps that are required to prepare EnergyPlus to be linked to FMUs for co-simulation.
-
-### Workflow of the FMU for co-simulation import
-
-To use the FMU for co-simulation import, there are two important steps: pre-processing and co-simulation.  The pre-processing step generates a section of an EnergyPlus input file (\*.idf) that can be used to configure the FMU for co-simulation import. The input file defines the input and output variables for both EnergyPlus and FMUs. The co-simulation step performs co-simulation.
-
-Figure 10 shows the work flow for pre-processing. First, a FMU Parser parses the FMU files (i.e. xxx.fmu) and generates a temporary EnergyPlus input file (i.e. xxxtmp.idf). The temporary EnergyPlus input file is not complete as it just contains information related to the FMU, such as names of the FMU and properties of each FMU variable including variable name, associated FMU name, input/output type, data type, units and definitions. The user will need to manually copy the FMU information from xxxtmp.idf into the EnergyPlus input file xxx.idf. The user then needs to modify the xxx.idf file to link the FMU variables with EnergyPlus variables.
-
-![](media/image036.png)
-
-Figure 10: Work flow for pre-processing.
-
-### FMU Parser
-
-The FMU parser is a code written in C. It includes Expat (Expat XML Parser, 2011) which is a XML parser library written in C. The low level implementation of the function (*parser*) that is used to process a FMU is *parser [options] xxx.fmu*, where *options* are as follows:
-
-- *--printidf*, prints a temporary xxxtmp.idf with FMU information to be printed,
-
-- *--unpack*, unpacks a FMU to be unpacked, and
-
-- *--delete*, deletes temporary files related to FMUs.
-
-A FMU is a zip file which may contain executable programs for specific platforms, description files and source code. In the pre-processing step, the FMU Parser will be called with the command option *--printidf.* This will cause the parser to parse the XML file with the model description of the FMU and write the FMU information in a format of the EnergyPlus input file (\*.idf). The parser will check if all the required fields from FMU (see next section for details) in the \*.idf file are correctly specified. If the check succeeds, the parser will successfully close. If the check fails, the parser will close with an error message. After the EnergyPlus executable (such as EnergyPlus.exe) terminates, the EnergyPlus batch file will delete all the temporary files that may have been generated.   The FMU Parser is distributed with EnergyPlus and can be found in the PreProcess folder (FMUParser) of the EnergyPlus installation.
-
-** **
-
-![](media/image037.png)
-
-Figure 11: Workflow of FMU parser for pre-processing.
-
-### Example 1: Interface using ExternalInterface:FunctionalMockupUnitImport:To:Schedule
-
-In this example, an HVAC system implemented in a FMU (MoistAir.fmu) is linked to a room model in EnergyPlus. The HVAC system computes sensible and latent heat gain required for maintaining a set point temperature. The FMU needs as input the outdoor dry-bulb (TDryBul) temperature, outdoor air relative humidity (outRelHum), the room dry-bulb temperature (TRooMea) and the room air relative humidity (rooRelHum). The outputs of the FMU are the latent (QLatent) and sensible (QSensible) heat transported across the thermodynamic boundary of air inlet and outlet of the thermal zone.
-
-To link the FMU with EnergyPlus, we need to send from the FMU to EnergyPlus two schedule values for the latent and sensible heat gain and from EnergyPlus to the FMU four output variables for outdoor dry-bulb temperature, outdoor air relative humidity, room dry-bulb temperature and room air relative humidity at each zone time step. This can be accomplished by using two objects of type ExternalInterface:FunctionalMockupUnitImport:To:Schedule and four objects of type ExternalInterface:FunctionalMockupUnitImport:From:Variable.
-
-To interface EnergyPlus, the following four items are needed:
-
-- An object that instructs EnergyPlus to activate the external interface.
-
-- An object that specifies the FMU and its instances.
-
-- EnergyPlus objects that read data from EnergyPlus and send to FMU.
-
-- EnergyPlus objects that read data from FMU and send to EnergyPlus.
-
-#### Creating the EnergyPlus idf file
-
-To create the EnergyPlus idf file the user should:
-
-- Use the *parser* to generate a temporary idf.
-
-- Copy the FMU information from the temporary idf into the full idf file.
-
-- Modify the full idf file to link the FMU variables with EnergyPlus variables.
-
-
-
-The code below shows how the objects will be in the idf.
-
-To activate the external interface, we use:
-
-
-```idf
-ExternalInterface,           !- Object to activate the external interface
- FunctionalMockupUnitImport; !- Name of external interface
-```
-
-To define the FMU that will be linked to EnergyPlus, we use:
-
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport,
-    MoistAir.fmu,            !- FMU Filename
-    15,                       !- FMU Timeout
-    0;                        !- FMU LoggingOn
-```
-
-
-To enter output variables from which the external interface read and send to FMUs, we use:
-
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-    Environment,                      !- EnergyPlus Key Value
-    Site Outdoor Air Drybulb Temperature,     !- EnergyPlus Variable Name
-    MoistAir.fmu,                     !- FMU Filename
-    Model1,                           !-FMU Model Name
-    TDryBul;                          !- FMU Model Variable Name
-
-
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-    ZONE ONE,                         !- EnergyPlus Key Value
-    Zone Mean Air Temperature,        !- EnergyPlus Variable Name
-    MoistAir.fmu,                     !- FMU Filename
-    Model1,                           !- FMU Model Name
-    TRooMea;                          !- FMU Model Variable Name
-
-
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-    Environment,                      !- EnergyPlus Key Value
-    Site Outdoor Air Relative Humidity,      !- EnergyPlus Variable Name
-    MoistAir.fmu,                     !- FMU Filename
-    Model1,                           !- FMU Model Name
-    outRelHum;                        !- FMU Model Variable Name
-
-
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-    ZONE ONE,                         !- EnergyPlus Key Value
-    Zone Air Relative Humidity,       !- EnergyPlus Variable Name
-    MoistAir.fmu,                     !- FMU Filename
-    Model1,                           !- FMU Model Name
-    rooRelHum;                        !- FMU Model Variable Name
-```
-
-
-These output variables need to be specified in the idf file:
-
-
-```idf
-Output:Variable,
-    Environment,                 !- Key Value
-    Site Outdoor Air Drybulb Temperature,            !- Variable Name
-    TimeStep;                    !- Reporting Frequency
-
-
-Output:Variable,
-    ZONE ONE,                    !- Key Value
-    Zone Mean Air Temperature,   !- Variable Name
-    TimeStep;                    !- Reporting Frequency
-
-
-Output:Variable,
-    Environment,                 !- Key Value
-    Site Outdoor Air Relative Humidity,   !- Variable Name
-    TimeStep;                    !- Reporting Frequency
-
-
-Output:Variable,
-    ZONE ONE,                    !- Key Value
-    Zone Air Relative Humidity,  !- Variable Name
-    TimeStep;                    !- Reporting Frequency
-```
-
-
-To enter schedules to which the external interface writes, we use:
-
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport:To:Schedule,
-    FMU_OthEquSen_ZoneOne,   !- EnergyPlus Variable Name
-    Any Number,              !- Schedule Type Limits Names
-    MoistAir.fmu,            !- FMU Filename
-    Model1,                  !- FMU Model Name
-    QSensible,               !- FMU Model Variable Name
-    0;                       !- Initial Value
-
-
-ExternalInterface:FunctionalMockupUnitImport:To:Schedule,
-    FMU_OthEquLat_ZoneOne,   !- EnergyPlus Variable Name
-    Any Number,              !- Schedule Type Limits Names
-    MoistAir.fmu,            !- FMU Filename
-    Model1,                  !- FMU Model Name
-    QLatent,                 !- FMU Model Variable Name
-    0;                       !- Initial Value
-```
-
-
-This completes the configuration that is required to simulate EnergyPlus with the FMU.
-
-### Example 2: Interface using ExternalInterface:FunctionalMockupUnitImport:To:Actuator
-
-In this example, a shading controller with a finite state machine is implemented in a FMU (ShadingController.fmu). Inputs of the FMU are the outside temperature (TRoo) and the solar irradiation (ISolExt) that is incident on the window. The output of the FMU is the shading actuation signal (yShade).This example describes how to set up EnergyPlus to exchange data between the FMU and EnergyPlus, using an Energy Management System (EMS) actuator.
-
-To interface EnergyPlus using the EMS feature, the following four items are needed:
-
-- An object that instructs EnergyPlus to activate the external interface.
-
-- An object that specifies the FMU and its instances.
-
-- EnergyPlus objects that read data from EnergyPlus and send to FMU.
-
-- EnergyPlus objects that read data from FMU and send to EnergyPlus.
-
-#### Creating the EnergyPlus idf file
-
-To create the EnergyPlus idf file the user should:
-
-- Use the *parser* to generate a temporary idf.
-
-- Copy the FMU information from the temporary idf into the full idf file.
-
-- Modify the full idf file to link the FMU variables with EnergyPlus variables
-
-The code below shows how the objects will be in the idf.
-
-To activate the external interface, we use:
-
-
-```idf
-ExternalInterface,           !- Object to activate the external interface
- FunctionalMockupUnitImport; !- Name of external interface
-```
-
-To define the FMU that will be linked to EnergyPlus, we use:
-
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport,
-    ShadingController.fmu,            !- FMU Filename
-    15,                       !- FMU Timeout in milli-seconds
-    0;                        !- FMU LoggingOn
-```
-
-To enter the two output variables from which the external interface read from and send to FMUs, we use:
-
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-    Zn001:Wall001:Win001,             !- EnergyPlus Key Value
-    Surface Outside Face Incident Solar Radiation Rate per Area,
-    ShadingController.fmu,            !- FMU Filename
-    Model1,                           !- FMU Model Name
-   ISolExt;                          !- FMU Model Variable Name
-
-
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-    WEST ZONE,                        !- EnergyPlus Key Value
-    Zone Mean Air Temperature,        !- EnergyPlus Variable Name
-    ShadingController.fmu,            !- FMU Filename
-    Model1,                           !- FMU Model Name
-    TRoo;                             !- FMU Model Variable Name
-```
-
-
-These output variables need to be specified in the idf file:
-
-
-```idf
-Output:Variable,
-    Zn001:Wall001:Win001,               !- Key Value
-    Surface Outside Face Incident Solar Radiation Rate per Area,  !- Var Name
-    TimeStep;                           !- Reporting Frequency
-
-
-Output:Variable,
-    WEST ZONE,                          !- Key Value
-    Zone Mean Air Temperature,          !- Variable Name
-    TimeStep;                           !- Reporting Frequency
-```
-
-
-To enter the actuator that changes the control status of the window with name “Zn001:Wall001:Win001�, we use:
-
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport:To:Actuator,
-Zn001_Wall001_Win001_Shading_Deploy_Status,  !- EnergyPlus Variable Name
-    Zn001:Wall001:Win001,                !- Actuated Component Unique Name
-    Window Shading Control,                  !- Actuated Component Type
-    Control Status,                      !- Actuated Component Control Type
-    ShadingController.fmu,                   !- FMU Filename
-    Model1,                                  !- FMU Model Name
-    yShade,                                  !- FMU Model Variable Name
-    6;                                       !- Initial Value
-```
-
-
-      This completes the configuration that is required to simulate EnergyPlus with the FMU.
-
-### Example 3: Interface using ExternalInterface:FunctionalMockupUnitImport:To:Variable
-
-This example implements the same controller as the Example 2. However, the interface with EnergyPlus is done using an external interface variable instead of an external interface actuator. Inputs of the FMU are the outside temperature (TRoo) and the solar irradiation (ISolExt) that is incident on the window. The output of the FMU is the shading actuation signal (yShade).
-
-To interface EnergyPlus using an external interface variable, the following items are needed:
-
-- An object that instructs EnergyPlus to activate the external interface.
-
-- An object that specifies the FMU and its instances.
-
-- EnergyPlus objects that read data from EnergyPlus and send to FMU.
-
-- EnergyPlus objects that read data from FMU and send to EnergyPlus.
-
-#### Creating the EnergyPlus idf file
-
-To create the EnergyPlus idf file the user should:
-
-- Use the *parser* to generate a temporary idf.
-
-- Copy the FMU information from the temporary idf into the full idf file.
-
-- Modify the full idf file to link the FMU variables with EnergyPlus
-
-The code below shows how the objects will be in the idf.
-
-To activate the external interface, we use:
-
-
-```idf
-ExternalInterface,           !- Object to activate the external interface
- FunctionalMockupUnitImport; !- Name of external interface
-```
-To define the FMU that will be linked to EnergyPlus, we use:
-
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport,
-    ShadingController.fmu,            !- FMU Filename
-    15,                       !- FMU Timeout in milli-seconds
-    0;                        !- FMU LoggingOn
-```
-
-To enter the two output variables from which the external interface read from and send to FMUs, we use:
-
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-    Zn001:Wall001:Win001,             !- EnergyPlus Key Value
-    Surface Outside Face Incident Solar Radiation Rate per Area,
-    ShadingController.fmu,            !- FMU Filename
-    Model1,                           !- FMU Model Name
-   ISolExt;                          !- FMU Model Variable Name
-
-
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-    WEST ZONE,                        !- EnergyPlus Key Value
-    Zone Mean Air Temperature,        !- EnergyPlus Variable Name
-    ShadingController.fmu,            !- FMU Filename
-    Model1,                           !- FMU Model Name
-    TRoo;                             !- FMU Model Variable Name
-```
-
-
-These output variables need to be specified in the idf file:
-
-
-```idf
-Output:Variable,
-    Zn001:Wall001:Win001,               !- Key Value
-    Surface Outside Face Incident Solar Radiation Rate per Area,  !- Var Name
-    TimeStep;                           !- Reporting Frequency
-
-
-Output:Variable,
-    WEST ZONE,                          !- Key Value
-    Zone Mean Air Temperature,          !- Variable Name
-    TimeStep;                           !- Reporting Frequency
-```
-
-
-To write data from the external interface to an EnergyPlus EMS variable, we use the following item in idf file:
-
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport:To:Variable,
-    Shade_Signal,            !- EnergyPlus Variable Name
-    ShadingController.fmu,   !- FMU Filename
-    Model1,                  !- FMU Model Name
-    yShade,                  !- FMU Model Variable Name
-    1;                       !- Initial Value
-```
-
-
-which declares a variable with name yShade that can be used in an Erl program to actuate the shading control of the window “Zn001:Wall001:Win001� as follows:
-
-
-```idf
-! EMS program. The first assignments sets the shading status and converts it into the
-!              EnergyPlus signal (i.e., replace 1 by 6).
-!              The second assignment sets yShade to
-!              an EnergyManagementSystem:OutputVariable
-!              which will be read by the external interface.
-  EnergyManagementSystem:Program,
-    Set_Shade_Control_State,          !- Name
-    Set Shade_Signal = 6*yShade,      !- Program Line 1
-    Set Shade_Signal_01 = yShade+0.1; !- Program Line 2
-
-
-! Declare an actuator to which the EnergyManagementSystem:Program will write
-  EnergyManagementSystem:Actuator,
-    Shade_Signal,  !- Name
-    Zn001:Wall001:Win001,             !- Actuated Component Unique Name
-    Window Shading Control,           !- Actuated Component Type
-    Control Status;                   !- Actuated Component Control Type
-
-
-! Declare a global variable to which the EnergyManagementSystem:Program will write
-  EnergyManagementSystem:GlobalVariable,
-    Shade_Signal_01;                  !- Name of Erl variable
-```
-
-
-This completes the configuration that is required to simulate EnergyPlus with the FMU.
-
-Exporting  EnergyPlus as a Functional Mock-up Unit for co-simulation
---------------------------------------------------------------------
-
-The FMU export of EnergyPlus allows EnergyPlus to be accessed from other simulation environments, as a FMU for co-simulation.
-
-FMUs are formally specified in the Functional Mock-up Interface (FMI) standard, an open standard designed to enable links between disparate simulation programs. The standard is available from [http://www.functional-mockup-interface.org/](http://www.functional-mockup-interface.org/.%20).
-
-To export EnergyPlus as a FMU for co-simulation, the Lawrence Berkeley National Laboratory has developed a utility which exports EnergyPlus as a FMU for co-simulation. This utility is freely available from http://SimulationResearch.lbl.gov.
-
-References
-==========
-
-Hensen, Jan L. M. 1999. “A comparison of coupled and de-coupled solutions for temperature and air flow in a building.� *ASHRAE Transactions 105 (2): 962–969*.
-
-Zhai, Zhiqiang John, and Qingyan Yan Chen. 2005. “Performance of coupled building energy and CFD simulations.� *Energy and Buildings 37 (4): 333–344*.
-
-BCVTB Documentation. 2011. Online available at: [http://simulationresearch.lbl.gov/bcvtb/releases/1.0.0/doc/manual/index.xhtml](http://simulationresearch.lbl.gov/bcvtb/releases/1.0.0/doc/manual/index.xhtml) [last accessed: 06/13/2011].
-
-Expat XML Parser. 2011. http://sourceforge.net/projects/expat/ *[Last accessed: 06/20/2011]*.
-
-G. Fábián, D.A. van Beek, J.E. Rooda. 2008. Substitute equations for index reduction and discontinuity handling.  In Proc. of the Third International Symposium on Mathematical Modeling, Vienna, Austria.
-
-Modelisar. 2010. “Functional Mock-up Interface for Co-Simulation.� [*http://www.modelisar.com/specifications/FMI\_for\_CoSimulation\_v1.0.pdf*](http://www.modelisar.com/specifications/FMI_for_CoSimulation_v1.0.pdf) *[Last accessed: 06/06/2011]*.
-
-
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-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Getting Started with EnergyPlus</h1>
-<h2>Basic Concepts Manual - Essential Information You Need about Running EnergyPlus</h2>
-<br/>
-<p><i>(and a start at building simulation)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-EnergyPlus Overview
-===================
-
-Welcome to EnergyPlus! This section offers a big picture view of what EnergyPlus is, what it does, why it exists, and what its goals are AND provides an overview to the **EnergyPlus documentation library**. While this document does not provide every detail on the program, it does give the reader a macroscopic view of EnergyPlus and how it is intended to fit into the energy analysis and thermal load simulation software continuum.
-
-What is EnergyPlus?
--------------------
-
-EnergyPlus has its roots in both the BLAST and DOE–2 programs. BLAST (Building Loads Analysis and System Thermodynamics) and DOE–2 were both developed and released in the late 1970s and early 1980s as energy and load simulation tools. Their intended audience is a design engineer or architect that wishes to size appropriate HVAC equipment, develop retrofit studies for life cycling cost analyses, optimize energy performance, etc. Born out of concerns driven by the energy crisis of the early 1970s and recognition that building energy consumption is a major component of the American energy usage statistics, the two programs attempted to solve the same problem from two slightly different perspectives. Both programs had their merits and shortcomings, their supporters and detractors, and solid user bases both nationally and internationally.
-
-Like its parent programs, EnergyPlus is an energy analysis and thermal load simulation program. Based on a user’s description of a building from the perspective of the building’s physical make-up, associated mechanical systems, etc., EnergyPlus will calculate the heating and cooling loads necessary to maintain thermal control setpoints, conditions throughout an secondary HVAC system and coil loads, and the energy consumption of primary plant equipment as well as many other simulation details that are necessary to verify that the simulation is performing as the actual building would. Many of the simulation characteristics have been inherited from the legacy programs of BLAST and DOE–2. Below is list of some of the features of the first release of EnergyPlus. While this list is not exhaustive, it is intended to give the reader and idea of the rigor and applicability of EnergyPlus to various simulation situations.
-
-- **Integrated, simultaneous solution** where the building response and the primary and secondary systems are tightly coupled (iteration performed when necessary)
-
-- **Sub-hourly, user-definable time steps** for the interaction between the thermal zones and the environment; variable time steps for interactions between the thermal zones and the HVAC systems (automatically varied to ensure solution stability)
-
-- **ASCII text based weather, input, and output files** that include hourly or sub-hourly environmental conditions, and standard and user definable reports, respectively
-
-- **Heat balance based solution** technique for building thermal loads that allows for simultaneous calculation of radiant and convective effects at both in the interior and exterior surface during each time step
-
-- **Transient heat conduction** through building elements such as walls, roofs, floors, etc. using conduction transfer functions
-
-- **Improved ground heat transfer modeling** through links to three-dimensional finite difference ground models and simplified analytical techniques
-
-- **Combined heat and mass transfer** model that accounts for moisture adsorption/desorption either as a layer-by-layer integration into the conduction transfer functions or as an effective moisture penetration depth model (EMPD)
-
-- **Thermal comfort models** based on activity, inside dry bulb, humidity, etc.
-
-- **Anisotropic sky model** for improved calculation of diffuse solar on tilted surfaces
-
-- **Advanced fenestration calculations** including controllable window blinds, electrochromic glazings, layer-by-layer heat balances that allow proper assignment of solar energy absorbed by window panes, and a performance library for numerous commercially available windows
-
-- **Daylighting controls** including interior illuminance calculations, glare simulation and control, luminaire controls, and the effect of reduced artificial lighting on heating and cooling
-
-- **Loop** **based configurable HVAC systems** (conventional and radiant) that allow users to model typical systems and slightly modified systems without recompiling the program source code
-
-- **Atmospheric pollution calculations** that predict CO<sub>2</sub>, SO<sub>x</sub>, NO<sub>x</sub>, CO, particulate matter, and hydrocarbon production for both on site and remote energy conversion
-
-- **Links to other popular simulation environments/components** such as WINDOW5, WINDOW6 and DElight to allow more detailed analysis of building components
-
-More details on each of these features can be found in the various parts of the EnergyPlus documentation library.
-
-No program is able to handle every simulation situation. However, it is the intent of EnergyPlus to handle as many building and HVAC design options either directly or indirectly through links to other programs in order to calculate thermal loads and/or energy consumption on for a design day or an extended period of time (up to, including, and beyond a year). While the first version of the program contained mainly features directly linked to the thermal aspects of buildings, later versions of the program also included other issues that are important to the built environment: water, electrical systems, etc.
-
-*Although it is important to note what EnergyPlus is, it is also important to remember what it is not.*
-
-- EnergyPlus is not a user interface. It is intended to be the simulation engine around which a third-party interface can be wrapped. Inputs and outputs are simple ASCII text that is decipherable but best left to a GUI (graphical user interface). This approach allows interface designers to do what they do best—produce quality tools specifically targeted toward individual markets and concerns. The availability of EnergyPlus frees up resources previously devoted to algorithm production and allows them to be redirected interface feature development in order to keep pace with the demands and expectations of building professionals.
-
-- EnergyPlus is currently not a life cycle cost analysis tool. It produces results that can then be fed into an LCC program. In general, calculations of this nature are better left to smaller “utility� programs which can respond more quickly to changes in escalation rates and changes to methodologies as prescribed by state, federal, and defense agencies.
-
-- EnergyPlus is not an architect or design engineer replacement. It does not check input, verify the acceptability or range of various parameters (expect for a limited number of very basic checks), or attempt to interpret the results. While many GUI programs assist the user in fine-tuning and correcting input mistakes, EnergyPlus still operates under the “garbage in, garbage out� standard. Engineers and architects will always be a vital part of the design and thermal engineering process.
-
-Why does EnergyPlus exist and what were its original goals?
------------------------------------------------------------
-
-The existence of EnergyPlus is directly related to some of the increasingly obvious shortcomings of its predecessor programs—BLAST and DOE–2. Both programs, though still valid tools that will continue to have utility in various environments, have begun to show their age in a variety of ways. Both BLAST and DOE–2 were written in older version of FORTRAN and used features that will eventually be obsolete in new compilers. Both programs consisted of a significant amount of “spaghetti code� and outdated structures that made it difficult to maintain, support, and enhance. Neither BLAST nor DOE–2 is able to correctly handle feedback from the HVAC system to the zone conditions.
-
-Finally, the speed with which new technology in the HVAC field is developed has far outpaced the ability of the support and development groups of both programs to keep the programs current and viable. This is really the key issue in the existence of EnergyPlus: there simply are not enough researchers worldwide who have enough experience with the complex code of the programs to keep pace with new technology. In addition, due to the years of experience necessary to make modifications to either BLAST or DOE–2, it is extremely expensive and time consuming to produce models or train someone to become proficient in either program’s code. The following paragraphs address how the goals of EnergyPlus have been carefully selected to solve the problems of the legacy programs and to make EnergyPlus an international repository for algorithms that can be made available to all interested parties.
-
-***Structure and Simulation Management:*** The “spaghetti code� nature of the parent programs resulted in great confusion as to how information flowed within the program, when data was modified or should be modified, and what was happening when. Thus, one of the goals of EnergyPlus development was to eliminate the interconnections between various program sections and the need to understand all parts of the code just to make an addition to a very limited part of the program. This goal was achieved through a program structure that implemented a “manager� philosophy. In effect, the program consists of many pieces (i.e., modules—see next paragraph) which when viewed graphically resemble an inverted tree. Instead of allowing lower level pieces of the program and calls to those sections of the code to infiltrate up to the highest level of the simulation, each branch exercises control over when its sub-branches are called. Thus, this is much like an organization chart where management over employees proceeds up a chain of command until it reaches the “CEO� of the simulation. In EnergyPlus, a subroutine called ManageSimulation serves the “CEO� role. This single subroutine controls four of the five main simulation loops (environment, day, hour, sub-hour time step; the system time step is controlled by the HVAC manager). In addition, this subroutine also sets global flags that are used by other subroutines and modules to determine the state of the simulation so that each part of the program knows whether to read input, initialize, simulate, report, etc. The manager philosophy makes the links between program modules simple and explicit. Typically, each module is accessible only through a call to its manager routine. Developers no longer have to worry about hidden and unexpected connections between and among program subroutines.
-
-***Modularity:*** One of the benefits of the structural improvements over the legacy programs is that the code can now be much more object-oriented and modular in nature. A result of the goal for improved structure in EnergyPlus was the definition of a well-organized, module concept that would facilitate adding features and links to other programs. It was decided that FORTRAN90 would be used for the initial release of EnergyPlus due to the fact that it:
-
-- is a modern, modular language with good compilers on many platforms
-
-- allows C-like data structures and mixed language modules
-
-- provides structure that begins to be object-based
-
-- allows long variable names (up to 32 characters)
-
-- provides backward compatibility with legacy code during the development process
-
-The key benefit of modularity is that researchers can develop modules concurrently without interfering with other modules under development and with only a limited knowledge of the entire program structure. This feature is critical to promoting both widespread use and broad development of program models. EnergyPlus can only be successful if the pool of potential model developers increases significantly so that interest and economics drives what models are added to the program rather than have its extensions limited by a lack of intellectual resources. Thus, modularity and structure improvements in EnergyPlus solve the problems of not having enough experts to keep up with technology and the large start-up time and expense previously needed to bring someone up to speed on program additions.
-
-Since the original version (2001), EnergyPlus code and structure continued to evolve and adopt the ever changing Fortran Standard.  However, in 2014, a full conversion of the simulation code to C++ was completed.  The development team also adapted workflows and open sourced the code and posted it on [Github](https://github.com/NREL/EnergyPlus).  Just like how the Fortran simulation code utilized modern Fortran standard capabilities, the C++ code utilizes modern (C++11...) C++ standard capabilities.
-
-***Established Links:*** The modularity of EnergyPlus makes it easier for other developers to quickly add other component simulation modules. This means that it will be significantly easier to establish links to other programming elements. Since initially the EnergyPlus code will contain a significant number of existing modules, there will be many places within the HVAC code where natural links to new programming elements can be established. These are fully documented to assist other developers in a swift integration of their research into EnergyPlus. In addition to these more natural links in the HVAC section of the code, EnergyPlus will also have other more fluid links in areas such as the heat balance that will allow for interaction where the modules might be more complex or less component based. Again, the goal of this feature of EnergyPlus is maximize the number of developers who can quickly integrate their work into EnergyPlus for the minimum investment of resources. The following diagram depicts how other programs have already been linked to EnergyPlus and a big picture view of how future work can impact the program.
-
-![](media/image001.png)
-
-Figure 1. EnergyPlus -- the big picture
-
-***Integration of Loads, Systems, and Plants:*** One of the strong points of EnergyPlus is the integration of all aspects of the simulation—loads, systems, and plants. Based on a research version of the BLAST program called IBLAST, system and plant output is allowed to directly impact the building thermal response rather than calculating all loads first, then simulating systems and plants. The simulation is coupled allowing the designer to more accurately investigate the effect of undersizing fans and equipment and what impact that might have on the thermal comfort of occupants within the building. The diagram below shows a basic overview of the integration of these important elements of a building energy simulation.
-
-![](media/image002.jpg)
-
-Figure 2. EnergyPlus -- Internal elements
-
-***“Open� Source Code:*** Another advantage of EnergyPlus that it shares with both BLAST and DOE–2 is that the source code of the program will be available and open for public inspection, revision, etc. The program is not intended to be a black box that is unintelligible to the users and developers around the world. While there are many conflicting ideas on what is meant by “open�, EnergyPlus is certainly not closed since this would be counter to the goals that have already been stated. The hope is that this access to source code will improve the accuracy and usability of the program over the long term and allow many developers to work on the program simultaneously. This “developer friendly� stance is critical to keeping EnergyPlus current and in step with technological advances.
-
-In summary, the goals of EnergyPlus are ambitious but achievable via the path described above. EnergyPlus aims to be a program that is relatively simple to work with from the perspective of both the users and the developer. The development team made tremendous efforts to keep simulation code and algorithms as separate as possible and as modular as possible to minimize the overall knowledge that someone would need to have to add models to the program. This will minimize the resource investment and maximize the impact of current research in the field of building energy analysis and thermal load calculations. Finally, the full coupling of building envelopes, systems, and plants will provide a better understanding of how a building responds not only to the environmental factors that impact the building but also the HVAC system as it attempts to meet the thermal loads on the building.
-
-It is also important to note that testing and verification are key issues in the development of any new program such as EnergyPlus. While there are large sections of EnergyPlus that consist of brand new code, the majority of the heat balance code can be traced back to the original parent programs. It should be noted that while this code has been significantly reengineered the team used what has been termed an “evolutionary reengineering� (ER) process. In ER, program code is modified stepwise in an effort to restructure it, modularize it, replace old obsolete data structures, etc. The ultimate goal is to bring it up to current programming standards without starting over with new code. At each step along the way, the program is exercised over a variety of input files and parameters to insure that what were intended to be algorithm neutral changes in the program have not resulted in changes to the output. This process was very successful and bolstered confidence in the program. In addition, comparisons could be made back to legacy programs to show that the new program is at a minimum as accurate as its predecessors. Beyond this, EnergyPlus has also been subjected to a lengthy and rigorous testing plan by an outside agency as well as numerous beta testers. This level of effort and collaboration is unprecedented in the history of energy analysis and thermal load calculation programs and has resulted in a much higher level of confidence in the results produced by EnergyPlus.
-
-EnergyPlus Documentation Library
---------------------------------
-
-The documentation library for EnergyPlus has historically been provided in the form of pdf's packaged with the release.  As of the 8.3.0 release, a major conversion was completed where the source of the docs was changed to Markdown.  This allows for numerous improvements:
-
-* Easy to automatically translate in between other markup languages, including html, thus making it easy to host as a web page.
-* Merging can be done automatically so the documentation source can stay alongside the source code, idd, and idfs, and all be merged at once.  With the ever-increasing visibility of EnergyPlus development, it is becoming key that documentation is directly in sync with the rest of the program files.
-* Since Markdown is clear text, it is platform-independent and maximizes the possibility for outside contributions to EnergyPlus.
-
-The Markdown source for the latest major release is converted to html which is then available at http://energyplus.net/documentation.  The current, or "daily" documentation is available at http://nrel.github.io/EnergyPlus, but since this is a moving target within a release cycle, it is recommended that users view the .net documentation page.
-
-Two key aspects of the documentation that are currently in development and should be completed soon are:
-
-* Search: the ability to search the online html docs easily
-* Download as pdf: the ability to download pdfs for local/offline access
-
-The Markdown based documentation is structured similarly to the pdfs, though the larger files are broken into smaller pieces for faster load times due to the dynamic nature of the math, especially in the engineering reference.  Each of the main documentation pieces are described here.
-
-### User Information Documents
-
-The following documents relate to using EnergyPlus, the engine. These documents cover a full range of questions and should be the first place a beginning or even experienced user would go to find out how the program works, what it expects as input, what it produces as output, etc. In general, the information in these documents is not highly technical, but it is detailed enough to use the basic capabilities of the program.
-
-***Getting Started with EnergyPlus – the Basics Manual:*** You are currently reading the Overview section of this document. The overview contains a “big picture� description of the EnergyPlus program as well as background of its development and the goals to which it ascribes. The remainder of the Getting Started document provides beginning users with an introduction into how to run EnergyPlus, what files are needed for EnergyPlus to execute, and what files are produced when EnergyPlus runs successfully. It also provides some guidance as to how to determine what potential sources of errors are when EnergyPlus runs into problems and how serious those problems might be.
-
-***Input and Output Reference:*** This document is a thorough description of the various input and output files related to EnergyPlus, the format of these files, and how the files interact and interrelate.
-
-***Output Details, Examples and Data Sets:*** While the Input and Output Reference document touch on some of the outputs from EnergyPlus, this document has more details and specific examples. It also addresses the reference data sets that are included.
-
-***Auxiliary Programs*:** This document contains information for the auxiliary programs that are part of the EnergyPlus package. For example, this document contains the user manual for the Weather Converter program, descriptions on using Ground Heat Transfer auxiliary programs with EnergyPlus, Compact HVAC descriptions, the Transition program/package and other assorted documents.
-
-### Engineering Reference Document
-
-The Engineering Reference provides more in-depth knowledge into the theoretical basis behind the various calculations contained in the program. This reference includes more information on modeling equations, limitations, literature references, etc. The document contains the following information and is structured along the lines of the above illustration (Figure 2. EnergyPlus -- Internal elements).
-
-***Heat Balance Overview and Reference:***  This section describes the heat balance calculations that form the basis of the EnergyPlus building model. It includes descriptions of shadowing calculations and other pieces of the model.
-
-***HVAC Overview and Reference:***This section contains a description of the loop-based approach used by EnergyPlus to model the HVAC systems: air loops, water loops, etc. It includes a description of the higher-level managers that control the simulation flow as well as some information on the various components that can be linked together to comprise an HVAC system.
-
-***HVAC Branch Based Input Description:***This section is a special extension of both the input document and the HVAC overview document. It contains more detail on the various HVAC input objects and how these different object link together to form an HVAC description. It contains vital information mainly for the interface developer but also provides users with an in-depth look at the inner workings of the loop approach adopted by EnergyPlus.
-
-***Encyclopedic Reference:***If the information did not fit in the above categories, then the last part of the Engineering Reference is a detailed description of the various models.
-
-### Application Guides
-
-The application guides are intended to address specific applications using EnergyPlus where the other documents may not provide cohesive examples of intended usage; that is, the techniques for doing certain things may be spread throughout other documents but warrant a more “how to� approach that will be present in these documents. The application guides are intended to become more prolific over time, specifically targeted to questions users have sent to the helpdesk support site.
-
-***Current Application Guides:***
-
-***EMS Application Guide:*** This guide contains information useful to use the advanced feature of EnergyPlus: Energy Management System tweaks. The Erl language is described and examples for use are given.
-
-***External Interface Application Guide:*** This guide contains information specific to using the external interface feature of EnergyPlus to connect other simulation systems.
-
-***Plant Application Guide:*** This guide details the methods for simulating real chilled and hot water plant systems within EnergyPlus.
-
-***Using EnergyPlus for Compliance Guide:*** This guide contains information specific to using EnergyPlus in Compliance and Standard Rating systems.
-
-***External Interface(s) Application Guide:*** This guide contains information about external interfaces (through the Building Controls Virtual Test Bed link) to EnergyPlus.
-
-***Tips & Tricks for Using EnergyPlus:*** This guide contains short tips and tricks for using various parts of EnergyPlus.
-
-### Developer Menu and Developer Information Documents
-
-The following documents will be most useful to potential developers of EnergyPlus, both Interface Developers and Module Developers. Interface Developers will be creating input and output wraps on EnergyPlus so that is it is usable to the architect, design engineers, and others. Module developers will be creating new modules within the EnergyPlus structure and framework.
-
-***Interface Developer’s Guide:*** This document is critically important to persons interested in developing an interface that provides input to and read output from EnergyPlus. It is a comprehensive guide to the input data dictionary and the input data files that contain a user’s building data. Each piece of input syntax is described in detail. In addition, the mechanism for obtaining output and the format in which output will be produced are discussed. This document also contains sections on weather files and units. Numerous samples and examples are given throughout the document with a full file length example provided in the appendix.
-
-***Module Developer’s Guide:*** This document contains a wealth of information that is intended to provide as much assistance as possible to persons interested in adding modules to the EnergyPlus program. It reviews the module concept as outlined in the programming standard and how they have been implemented in EnergyPlus. It provides a description of how the various modules work together and how the program is structured from a module tree (inverted tree) perspective. One of the most important features of this document is a list of standard EnergyPlus service subroutines and modules that greatly simplify the developers’ task of integrating their work into the program. Input and output issues are also addressed from the perspective of how modules actually obtain data from the input file and how each section of the code sends data to the output files.
-
-Getting Started with EnergyPlus
-===============================
-
-The remainder of this document is intended to give you a start on using the program with a few simple tools (EP-Launch to help run the simulation; IDFEditor to help create or look at input files) as well as some of the features (such as energy meters, simulation results) of using the program.
-
-For learning about a specific input file, or a specific input object, the install includes two documents in the ExampleFiles folder:
-
-- Example Files Summary (highlights of each example file)
-
-- Example Files Links to Objects (for any object, up to 3 files using that object are shown)
-
-The standard Windows install procedure has put the following information on your computer, in the directories/folders shown.
-
-The main EnergyPlus folder contains:
-* Energy+.idd
-* EnergyPlus.exe and dependent shared libraries (dll files)
-* RunEPlus.bat and other batch files for running EnergyPlus
-* readme file(s), license, etc.
-* EP-Macro.exe and other support binaries
-* bugreprt.txt 
-
-The general layout of folders from the install looks like:
-
-```
-. EnergyPlus main folder
-+-- Documentation
-|   +-- A link to find the documentation online, and any additional docs packaged with the installation
-+-- DataSets
-|   +-- Reference Data Sets (libraries)
-+-- MacroDataSets
-|   +-- Macroized Reference Data Sets (libraries)
-+-- PreProcess
-|   +-- FMUParser              Tool for external interface specific applications
-|   +-- IDFEditor              Program files for the IDFEditor
-|   +-- GrndTempCalc           Special program to calculate ground temperatures.
-|   +-- DOE2Translator         Simple translator for DOE-2 files
-|   +-- WeatherConverter       Tool for performing weather file creation and conversion
-|   +-- ParametricPreprocessor Parametric simulation tool
-|   +-- IDFVersionUpdater      Graphical tool for updating old EnergyPlus files to the latest version
-+-- PostProcess
-|   +-- ReadVarsEso            The simple post processor exe.
-|   +-- EPCompare              A graphical tool for comparing two EnergyPlus output sets
-+-- ExampleFiles               Sample input, output, results files shipped with the program.
-+-- WeatherData                Sample weather files shipped with the program.
-```
-
-
-Running EnergyPlus
-==================
-
-Introduction
-------------
-
-EnergyPlus is a simulation program designed for modeling buildings with all their associated heating, ventilating, and air conditioning equipment. EnergyPlus is a simulation *engine*: it was designed to be an element within a system of programs that would include a graphical user interface to describe the building. However, it can be run *stand alone* without such an interface. This document describes how to run EnergyPlus in such a stand alone fashion. This section will introduce you to the EP-Launch program, which helps you run EnergyPlus.  EP-Launch looks and acts pretty much like a standard Windows™ program, so if you just want to get started with some exercises, you can skip to the section “Tutorial Example for running EnergyPlus� first and come back to this section if you run into problems with EP-Launch.
-
-Like all simulation programs, EnergyPlus consists of more than just an executable file. EnergyPlus needs various input files that describe the building to be modeled and the environment surrounding it. The program produces several output files, which need to be described or further processed in order to make sense of the results of the simulation. Finally, even in stand-alone mode, EnergyPlus is usually not executed “by hand�, but rather by running a procedure file which takes care of finding input files and storing or further processing the output files.
-
-To assist those in the Windows environment, we have included the EP-Launch program. Review the next section for basic instructions. More advanced techniques of executing the program are contained in the Auxiliary Programs document under “Technical Details of running EnergyPlus�, including some advanced uses of the EP-Launch program. If you wish to learn about DOS/Command Line use for EnergyPlus, you will need to read that section in the Auxiliary Programs document.
-
-EP-Launch Program
------------------
-
-EP-Launch is an optional component of the EnergyPlus Windows installation (it is not available for Linux and Mac platforms). For users that want a simple way of selecting files and running EnergyPlus, EP-Launch provides this and more. In addition, EP-Launch can help open a text editor for the input and output files, open a spreadsheet for the postprocessor results files, a web browser for the tabular results file, and start up a viewer for the selected drawing file.
-
-
-
-![](media/image004.png)
-
-Figure 4. EP-Launch Screen
-
-### Start EP-Launch
-
-EP-Launch is located in the main directory/folder for EnergyPlus. In addition, it is available on the shortcut menu for EnergyPlus.  By double clicking on the EP-Launch icon you get the screen shown above (Figure 4) for running a single input file. The EP-Launch program simply starts other programs and allows you to avoid having to use the DOS command line prompt to run EnergyPlus. More help is provided for the program under the “Help� menu.
-
-### Selecting Input and Weather Files
-
-The input file and weather files can be selected on the Single Input File tab from the two pull down lists which show recently used files or you can press the "Browse…" buttons to locate an input or weather file that you have created yourself. If this is your first time using EP-Launch, the pull down lists will show some files from the ExampleFiles subdirectory. These are not the only examples, use browse to open other example files from the ExampleFiles subdirectory or other EnergyPlus input files.
-
-### Running a Single Input File
-
-On the Single Input File tab, after you select the weather and input files simply push the "Simulate…" button to start the EnergyPlus building energy simulation engine. At this point a black DOS window should pop up on your screen and show the progress of your simulation. The simulation is complete when the black DOS box closes. The EnergyPlus program black DOS window will show scrolling text as the simulation procedure progresses. If you would like to see these messages more slowly you have two options:
-
-1)   Press the "Control-S" key combination to try to stop the progress and any key to continue.
-
-2)   Under the "View" menu on the EP-Launch program, select “Options� then “Command Window� then check "Pause During Simulation" and this will pause the process immediately after EnergyPlus executes. To continue after the pause, press any key.
-
-If the file contains Parametric objects, the single input file may cause multiple simulations to be performed. If multiple simulations are performed, the output files will be listed on the History tab and will be named with either the file suffixes defined in the input file or with a serial number.
-
-Multiple single input file and group simulations can be started at the same time. On a computer with multiple-processors or multiple-cores, this will enable the simulations to complete more quickly than starting one after another.
-
-### Looking at the Results
-
-After you have run a simulation and the black DOS window closes, EnergyPlus has completed, and a status message is displayed see Figure 5:
-
-![](media/image005.jpg)
-
-Figure 5. EP-Launch Finish Status
-
-This status gives you a quick overview of whether there were warning (**should look at**), severe (**should probably fix**) or fatal (**must fix**) errors in the run as well as the time it took for the simulation to complete.  After pressing “OK� from this box, selecting “ERR/EIO/BND Output Files Only� from the “View� menu will display the ERR, EIO, and BND files – useful when errors may have occurred. Alternatively, pressing the F2 function key will display the same three files.
-
-Another way to open files easily is by using the View Results buttons shown in Figure 6. Two different panels of buttons can be used under View Results, one shown by using the “All� tab on the left edge and by using the “Sets� tab on the left edge. The “All� tab shows all the various files by file extension that can be viewed individually.  Files available for view  based on the current input file name are “enabled� (extension names clearly readable). The contents of each file extension is listed below.
-
-![](media/image006.png)
-
-Figure 6. EP-Launch with the Sets tab of View Results
-
-The figure above shows the same main screen of EP-Launch but with the “Sets� tab selected on the left edge of the View Results section. The buttons on this tab can open many files at the same time and are a shortcut to opening the files that may be commonly used. The Text Output Files, Drawing Files, and Spreadsheets buttons cause several different results files to open at once based on the currently selected Input File. The HTML file opens just the tabular results file if that file was produced (see *OutputContol:Table:Style*).
-
-The contents (along with examples) are discussed in the [Output Details](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf) document.
-
-You can also view the results using one of the three buttons ("Text Output Files," "Drawing File" and "Spreadsheets") in the "View Results" area of the main EP-Launch screen.
-
-By pressing the "Text Output Files� button, a text editor will open each of the text output files. Up to 29 files will open, if they exist. Selecting “Single File� from the ‘View “ menu displays a menu of all available output files from which any file can be opened individually. Each file may also be opened with an associated function key. The output files and function key shortcuts are listed below:
-
-1. Variable – tabulated results in comma, tab or space delimited format (generated by the ReadVarsESO postprocessor) (F4)
-
-2. ESO – raw report variable output (F5),
-
-3. RDD – list of output variables available from the run (F6).
-
-4. MDD – list of output meters available from the run (Shift-Ctrl-F3)
-
-5. EIO – additional EnergyPlus results (F7),
-
-6. ERR – list of errors and warnings (F8),
-
-7. BND – HVAC system node and component connection details (F9),
-
-8. MTR – raw report meter output (F11),
-
-9. MTD – list of meter component variables (F12)
-
-10. METER File – tabulated meter report in comma, tab or space delimited format (generated by the ReadVarsESO postprocessor) (Ctrl-F4)
-
-11. ZSZ – zone sizing details in comma, tab or space delimited format (Ctrl+F5)
-
-12. SSZ – system sizing details in comma, tab or space delimited format (Ctrl+F6)
-
-13. AUDIT – input file echo with input processor errors and warnings (Ctrl+F8)
-
-14. SLN – output from "report, surfaces, lines" (Ctrl+F9)
-
-15. DBG – output from the debug command (Ctrl+F11)
-
-16. SHD – output related to shading (Ctrl+F12)
-
-17. SVG - HVAC Diagram (Shift+ F4)
-
-18. EPMIDF – clean idf file after EP-Macro processing (Shift+F5)
-
-19. EPMDET – EP-Macro detailed output with errors and warnings (Shift+F6)
-
-20. MAP – daylighting illuminance map (Shift+F7)
-
-21. TABLE – tabulated report of bin and monthly data in comma, tab or space delimited or HTML format  (Shift+F8)
-
-22. VMRL – drawing file in VRML (Virtual Reality Markup Language) format (Shift F+F11)
-
-23. DXF – drawing file in AutoCAD DXF format (Shift+F12)
-
-24. Delight IN - DElight input generated from EnergyPlus processed input (Shift+Ctrl+F4)
-
-25. Delight OUT – Detailed DElight output (Shift+Ctrl+F5)
-
-26. Delight ELDMP – DElight reference point illuminance per time step (Shift+Ctrl+F6)
-
-27. Delight DFDMP – DElight warning and error messages (Shift+Ctrl+F7)
-
-28. EXPIDF – Expanded IDF when using HVACTemplate objects (Shift+Ctrl+F8)
-
-29. Group Error – combined error files for a group run. (Shift+Ctrl+F9)
-
-30. VCpErr – Transition program error file (Shift+Ctrl+F11)
-
-31. Screen (Shift+Ctrl+f12)
-
-32. Proc CSV – Simple statistiscs generated from CSVProc (also see Create Statistics File option under View-Options).
-
-33. EDD – Energy Management System details.
-
-Clicking on the "Drawing File" button will open the generated DXF file if an appropriate viewer has been configured (see *Selecting Viewers and Editors* below). The DXF file is a CAD format that displays the physical shape of the building being modeled in three dimensions. The “Drawing File� button also opens the HVAC diagram generated with the HVAC-Diagram utility (see Auxiliary Programs).
-
-Clicking on the "Spreadsheets" buttons will open any generated CSV files if an appropriate viewer has been configured (see *Selecting Viewers and Editors* below).
-
-### Viewing the Drawing File without Running a Simulation
-
-The "Drawing" button (or the View menu Drawing File option) will automatically run EPDrawGUI if the DXF file does not exist or it is older than the input file. This allows the building geometry to be viewed without running a full simulation. For more information about EPDrawGUI, see the [*Auxiliary Programs*](file:///E:\Docs4PDFs\AuxiliaryPrograms.pdf) document.
-
-### Editing the Input Files
-
-The input file, called IDF file that is selected from the top pull-down list, can be edited by pressing one of two buttons in the "Input File" area. The "Edit - Text Editor" button will start a text editor and the "Edit - IDF Editor" will start the separate program called the IDF Editor. Remember to save any changes you make in either editor before returning to EP-Launch to run the simulations again.
-
-### File Menu
-
-The File menu can be used for selecting input and weather files just like the "Browse…" buttons (see the *Selecting Input and Weather Files* section above).
-
-If you are upgrading from the previous version of EnergyPlus you can use the “File�, “Transition� menu option to upgrade your EnergyPlus input files (IDF and IMF) to the most recent version (see the [AuxiliaryPrograms](file:///E:\Docs4PDFs\AuxiliaryPrograms.pdf) document for more information about the Transition program). This EP-Launch option only works for upgrading input files one version.
-
-### Edit Menu
-
-No cutting or pasting is used in this program so the edit menu shows options that duplicate the functions of the "Edit – Text Editor" and "Edit – IDF Editor" buttons. In addition, the weather file and the postprocessor command file (rvi) may be opened in the text editor.
-
-### View Menu
-
-The View menu (Figure 7) duplicates the options in the "View Results" area of the main screen (see the *Looking at the Results* section above) and allows opening of selected output files. You can also open the folders that contain the active input and weather files. Opening a single file is under a submenu and is very similar to the Quick Open Panel for Single Simulation described above. Selecting “HTML File� from the “View� menu will open any user created files saved in the format: &lt;filename&gt;table.html (see *OutputControl:Table:Style*).
-
-![](media/image007.png)
-
-Figure 7. EP-Launch View Menu
-
-
-
-![](media/image008.png)
-
-Figure 8. EP-Launch Options Screen.
-
-The “View� menu also accesses the “Options� menu item shown in Figure 8 that is used to control many of the optional features of EP-Launch. These optional features are described below:
-
-#### Command Window Options
-
-**Pause During Simulation (Unless Minimized)** – Stops the progress of the EnergyPlus run at different points. This does not stop the simulation itself but pauses before or after important events as files are copied or utility programs are run. It is usually used only for diagnosing problems with the EPL-RUN batch file. The feature is also described in the *Running a Single Input File* section above.
-
-**Minimize Single Simulation Command Window** – For a single input file, minimizes the Command Window that EP-Launch uses to run EnergyPlus. The command window will appear only in the Windows taskbar and the command window will not be visible. You can restore the command window be clicking on the taskbar item labeled “EnergyPlus Process�. This option should be used with caution since you will not see any indication of the simulation being complete other than the “EnergyPlus Process� taskbar item will disappear.
-
-**Minimum Group Simulation Command Window** – For a group of input files, minimizes the Command Window that EP-Launch uses to run EnergyPlus. This is a good option when working on something else on your computer at the same time as the group of simulations is running since the command window normally becomes the front window each time a new simulation starts. This option prevents the command window coming to the front for each simulation. The command window will appear only in the Windows taskbar and the command window will not be visible. You can restore the command window be clicking on the taskbar item labeled “EnergyPlus Process�. This option should be used with caution since you will not see any indication of the simulation being complete other than the “EnergyPlus Process� taskbar item will not be present.
-
-**Number of Simultaneous Processes** – Select the maximum number of simulations that should be able to be run at the same time. For a computer with multiple processors or multiple cores, this will allow better utilization of the computers power. The value selected should correspond to the number of processors/cores but higher or lower number can be used as well.
-
-**Disable Multi-Threading** – Check this box if you wish to disable the built in multi-threading capabilities of EnergyPlus. Portions of EnergyPlus have been programmed to use more than one processor, or CPU core, at the same time during a single simulation. This multithreading may not be desirable when running more than one simulation at a time on the same computer (because it can actually run more slowly). When this check box is checked multi-threading is turned off. The check box sets the **EP\_OMP\_NUM\_THREADS** environmental variable to 1. The multi-threading capability of EnergyPlus can also be controlled using the **ProgramControl** object field called Number of Threads Allowed. That field takes precedence over the setting of the checkbox. Also note that when multiple simulations are started from EP-Launch, this automatically disables multithreading by setting the EP\_OMP\_NUM\_THREADS environmental variable to 1 whether this box is checked or not. The ProgramControl object is described in the Input Output Reference document.
-
-#### Interface Options
-
-**Extra Wide Window** – Select this option to make the main EP-Launch window wider. This is useful when files are used with very long file path names.
-
-**Alternative layout** – Changes the layout of the EP-Launch window to an alternative arrangement of buttons.
-
-#### Miscellaneous Options
-
-**Tab Delimited Open with Spreadsheet** – Selecting �Single File� and then “Main Results File� from the “View� menu or pressing the F4 function key will open TAB files with the default spreadsheet application rather than the text editor. Comma-separated variable (CSV) is the default setting for viewing tabulated results set in the RVI file. If the user changes the setting for viewing tabulated results to TAB or TXT format, selecting �Single File� and then “Main Results File� from the “View� menu or pressing the F4 function key will open the files in the default text editor.  TAB files, when selected, will also be opened by the text editor when the “Text Output Files� button is pressed after a successful run.
-
-**Allow More Than 250 Columns** – Tabulated data that exceeds 250 columns, the MS Excel maximum, will be truncated to that limit unless “Allow &gt;250 Columns� is selected. Excel versions prior to 2007 were limited to 255 columns in a sheet; later versions allow unlimited number of columns. This limitation may not be true for other spreadsheet programs.
-
-**Check VERSION Prior to Simulation** – Automatically check the VERSION object in the selected EnergyPlus input file prior to simulation and if it is an older version than the current version will run the Transition program to update the file.
-
-**Convert ESO/MTR to IP Units** – Runs the convertESOMTR utility program (see AuxiliaryPrograms documentation for more information). This utility will convert the ESO and MTR files into Inch-Pound units. The CSV file created from these files will also be in Inch-Pound units.
-
-**Create Statistics File** – Runs the CSVProc utility program (see the AuxiliaryPrograms documentation for more information) and creates the –Proc.csv file. This file contains some simple statistics on each variable in the normal CSV file.
-
-**Create Batch File to Run EnergyPlus** – Traditionally EP-Launch has created a batch file in order to execute EnergyPlus with the various options chosen. This can cause problems with some operating systems, such as Windows Vista, when set to a higher security setting.  This option can be unchecked and a batch file is not created when running EnergyPlus instead parameters are passed to an existing batch file.
-
-**Run ParametricPreprocessor** – When this option is checked, if Parametric objects are present in the file, the ParametricPreprocessor will be run prior to the first simulation and if multiple simulations are needed they will all be executed. See the Auxiliary Programs documentation for details.
-
-**Check for Updates to EnergyPlus** – When this option is checked, EP-Launch will check every seven days if an update to EnergyPlus or any of the files distributed with EnergyPlus are available to download. If they are available a message will be shown upon start up.  You can also manually check by going to HELP .. CHECK FOR UPDATES.
-
-#### Text Editor Options
-
-EP-Launch will start a text editor when editing a IDF file or when viewing many of the results files.  The text editor that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the text editor of your choice. The Auto Find button will automatically find the program that is associated with the TXT file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a text editor is available immediately. The most common text editor is NOTEPAD.EXE and is built into Windows but many other text editors are also available.
-
-#### Drawing Viewer Options
-
-The default drawing viewer is the application associated with DXF files. This can be changed to your favorite drawing program by using the Select button then locating the executable file for your favorite drawing software capable of reading a DXF file. The Auto Find button will automatically find the program that is associated with the DXF file extension and use that program. A variety of programs (free of charge) can render DXF files for viewing.  The [Output Details](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf) document lists some of these programs as well as displaying what a DXF rendered file looks like on the screen.
-
-#### VRML Viewer Options
-
-EP-Launch will start a VRML Viewer when a building drawing is created using the Report, Surfaces, VRML option in your IDF file.  The VRML Viewer that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the VRML Viewer of your choice. The Auto Find button will automatically find the program that is associated with the WRL file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a VRML Viewer is available immediately. Many other VRML Viewers are available.
-
-#### Spreadsheet Options
-
-EP-Launch will start a spreadsheet program when viewing many of the results files.  The spreadsheet that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the spreadsheet program of your choice. The Auto Find button will automatically find the program that is associated with the CSV file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a spreadsheet program is available immediately.
-
-#### Diagramming Options
-
-EP-Launch will start a diagramming program to view SVG files from HVAC Diagram.  The diagramming program that will be used is shown but can be changed by either pressing the Select button, the Auto Find button, the Use Firefox button or the Use Opera button. The Select button allows you to find the diagramming program of your choice but make sure it is capable of opening SVG files. The Auto Find button will automatically find the program that is associated with the SVG file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a spreadsheet program is available immediately.  Since both Firefox and Opera web browsers can view SVG files, those buttons will select those respective browsers if available.
-
-#### HTML Browser Options
-
-EP-Launch will start a HTML browser program when viewing the tabular results file when HTML is chosen in OutputControl:Table:Style object. The HTML browser that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the HTML browser of your choice. The Auto Find button will automatically find the program that is associated with the HTML file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a HTML browser is available immediately.
-
-#### ESO Viewer Options
-
-By default, ESO files are opened with a text editor. ESO files are the raw output file containing results from EnergyPlus for Output:Variable objects. They are often processed into CSV files to make it easier to view them. At least one utility program has been developed to view ESO files directly (see the EnergyPlus.gov web site under “Interfaces & Other Tools�, “Third-party EnergyPlus Tools).  The Auto Find and Select buttons work the same way as other viewer selectors. If no special ESO viewer is selected the box will be shown as empty. It can also be emptied by using the Clear button.
-
-#### PDF Viewer Options
-
-EP-Launch will start a PDF viewer program when opening the EnergyPlus documentation under the Help menu.  The PDF Viewer that will be used is shown but can be changed by either pressing the Select button or by pressing the Auto Find button. The Select button allows you to find the PDF Viewer of your choice. The Auto Find button will automatically find the program that is associated with the PDF file extension and use that program. Auto Find is invoked the first time EP-Launch is started so that a PDF Viewer is available immediately.
-
-#### File Association Options
-
-When installing EnergyPlus, you are given an option if you want IDF, IMF, and EPG files associated with EP-Launch. This allows double clicking on files with those extensions and having EP-Launch start automatically with those files. If during the install that option is not selected or if you have changed the program that opens IDF, IMF and EPG files and want to change it back to EP-Launch, the button for this option will do that.
-
-#### Reset Options
-
-Two reset options are available here.
-
-The **Auto Find All File Viewers** button will autofind all the file viewers in one step. This is equivalent to pressing the Auto Find button for each viewer program. 
-
-The **Reset All Options and Exit** button will clear all options and restore the default values used when first invoking EP-Launch for the first time. This also clears the list of recently used IDF and weather files.  This option will exit EP-Launch and you will have to start EP-Launch again.
-
-### Help Menu
-
-The Help menu can be used to open the EnergyPlus documentation files and the EP-Launch help file. In addition, you can check for updates to the EnergyPlus program and other files in the EnergyPlus distribution.
-
-### Recently Used Files
-
-The recently used input, weather and group file pull down lists can hold a maximum of twenty items. These lists, like the viewers selected, are saved between times you use the EP-Launch program.
-
-### Utilities Tab
-
-The utilities tab shown in the following figure allows several utility programs that come with EnergyPlus to be used directly. More information on each utility is also available in the AuxiliaryPrograms documentation.
-
-![](media/image009.png)
-
-Figure 9. EP-Launch Utilities Tab.
-
-For each utility, input files can be selected by using the Browse Button. The input file can be opened using a text editor and, for certain utilities, the IDF Editor. If a weather file is needed for a utility it can also be selected. For other utilities, no weather file is needed and that portion of the screen is not shown. The appropriate output files can be opened by the “Open� button near the bottom of the screen. To run the utility, use the “Run� button in the lower left corner of the screen above the “Exit� button.
-
-In addition, for each utility, a brief description of the function of the utility is shown in the about box but much more information is available in the AuxiliaryPrograms documentation.
-
-### Caveats
-
-Remember to save changes made in the editor before you run another simulation.
-
-The simulation cannot write new results to open files which are locked by another application.
-
-You will need to close the spreadsheet program that views the resulting CSV files prior to another simulation and you may need to close the text editor windows also (depending on your editor).
-
-The EPL-RUN.BAT batch file is used to run EnergyPlus from the EP-Launch program. It can be edited with care if other postprocessors or preprocessors are to be used.
-
-### When things go wrong
-
-Though EnergyPlus has had several releases (including beta releases prior to initial release), there still may be problems when input files meet with EnergyPlus. If you are using EP-Launch when this happens, you will see a window appear as in the figure below (Figure 10). Follow the instructions listed on the screen.
-
-![](media/image010.jpg)
-
-Figure 10. EnergyPlus crash within EP-Launch.
-
-### Bugs
-
-The EP-Launch program has been through several “releases� but there is still a chance you will find bugs. Please report them to the energyplus-support@gard.com address so that we can fix them prior to the release.
-
-If the pull-down lists ever are shown as blank the "reset" button may be used. This unlabeled button is very small in the lower left-hand corner of the main screen. It removes the items shown in the recently used file list and causes the program to forget the selected viewers and text editors; and exits the program. When you start EP-Launch again, you will need to make these selections (viewers and text editors) again.
-
-
-
-EnergyPlus File Extensions
---------------------------
-
-This section will present a list of common EnergyPlus file extensions and what they mean. This will help you after the EP-Launch program finishes.
-
-### Input Files
-
-The following files are input to the EnergyPlus program.
-
-#### IDD
-
-The *input data dictionary* (IDD) is an ASCII (text) file containing a list of all possible EnergyPlus objects and a specification of the data each object requires. This file is analogous to the DOE-2 keyword file. The *Guide for Interface Developers* contains a full description of the input data dictionary.
-
-#### idf
-
-The *input data file* (IDF) is an ASCII file containing the data describing the building and HVAC system to be simulated. Many example files are installed as part of the EnergyPlus installation. Additionally, a spreadsheet file “ExampleFiles.xls�  contains columnar descriptions of each file’s features.
-
-#### imf
-
-The *input macro file* (IMF) is an ascii file containing the data describing the building and HVAC system to be simulated and will have some contents of “macro� commands. The Auxiliary programs document describes use of the macro commands and the program that processes them – EP-Macro.   Many example files are installed as part of the EnergyPlus installation.
-
-#### ini
-
-This is the EnergyPlus initialization file. It is an optional ascii input file that allows the user to specify the path for the directory containing Energy+.idd. This file, using the actual directories of the install, will be created during the install. Unless you change where the EnergyPlus.exe file resides, you will not need to change this file.
-
-#### epw
-
-The *EnergyPlus weather* file is an ascii file containing the hourly or sub-hourly weather data needed by the simulation program. The data format is described in detail in the Auxiliary Programs Document. It is also described succinctly in the Input Output Reference document.
-
-### Primary Output Files
-
-The following output files are the most important for beginning users.  Then, there is the section on “other output� files.  And, more information about output files (complete list) is shown in the [Output Details and Examples](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf) Document.
-
-#### err
-
-A text file containing the error messages issued by EnergyPlus. **This is the first output that should be examined after a simulation.**Error messages may be issued by EnergyPlus during its input phase or during the simulation. There are three levels of error severity: *fatal*, *severe*, and *warning* as well as simple *“information�* lines. A fatal error causes the program to terminate immediately. The following table illustrates the necessary actions.
-
-Table 1. Error Message Levels – Required Actions
-
-<table class="table table-striped">
-<tr>
-<th>Error Level</th>
-<th>Action</th>
-</tr>
-<tr>
-<td>Information, shown as *********</td>
-<td>Informative, usually a follow-on to one of the others. No action required.</td>
-</tr>
-<tr>
-<td>**   ~~~   **</td>
-<td>This is a continuation of a previous message.  String all the words/sentences together to form the complete message.</td>
-</tr>
-<tr>
-<td>Warning</td>
-<td>Take note. Fix as applicable.</td>
-</tr>
-<tr>
-<td>Severe</td>
-<td>Should Fix</td>
-</tr>
-<tr>
-<td>Fatal</td>
-<td>Program will abort, Must Fix</td>
-</tr>
-</table>
-
-#### csv
-
-When run normally, EP-Launch and EnergyPlus automatically creates post-processed standard output (eso) and meter output (mtr) files into columnar csv (comma separated variable) files.  These files are ready to be read by spreadsheet programs (such as Excel™).
-
-#### htm/html
-
-Several of the report options produce html files that can be read in standard Web browsers.  These are very powerful, information packed files.  Though wary of information overload, the easiest way to see “everything� is to enter the following in your input file:
-
-```idf
-OutputControl:Table,
-   HTML;                    !- ColumnSeparator
-
-Output:Table:SummaryReports,
-    All Summary;
-```
-
-
-Note that you can also get this file in other formats (the OutputControl:Table option).
-
-### Other Output Files
-
-#### audit
-
-This is an text file which echoes the IDD and IDF files, flagging syntax errors in either file. Note that both *err* and *audit* will show most of the error messages caused by input syntax errors; however only *err* will show errors issued during the actual simulation. The *audit* can be used when you need to see the context of the error message to fully ascertain the cause. The *audit* file also contains potentially extra information that may be useful from the input scan.
-
-#### eso
-
-The *EnergyPlus Standard Output* (ESO) is a text file containing the time varying simulation output. The format of the file is discussed in the *Guide for Interface Developers* and the *InputOutputReference*. The contents of the file are controlled by *Output:Variable* commands in the IDF file. Although the ESO is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
-
-#### mtr
-
-The *EnergyPlus Meter Output* (MTR) is a text file containing the time varying simulation output. The format of the file is similar to the ESO file. As described in a later section of this document (see Energy Meters), meters are a powerful reporting tool in EnergyPlus. Values are grouped onto logical meters and can be viewed the same way that the ESO variables are used. The contents of the file are controlled by *Output:Meter* commands in the IDF file. Although the MTR is a text file, it is not easily interpretable by a human. Usually postprocessing will be done on this file in order to put it in a format that can be read by a spreadsheet; however a quick visual inspection of the file does show whether the expected variables are output at the desired time step.
-
-#### mtd
-
-This file contains all the details (i.e., which report variables are on a meter and, conversely, what meters contain) about meters.
-
-#### eio
-
-The *EnergyPlus Invariant Output* (EIO) is a text file containing output that does not vary with time. For instance, location information (latitude, longitude, time zone, altitude) appears on this file.
-
-#### rdd
-
-#### mdd
-
-The *Report (variable) Data Dictionary* (RDD) is a text file listing those variables available for reporting (on the ESO) for this particular simulation. Which variables are available for output depends on the actual simulation problem described in the IDF. The *Report (meter) Data Dictionary* (MDD) is a text file listing those variables available for reporting (on the MTR) for this particular simulation. Which meters are available for output depends on the actual simulation problem described in the IDF. A simulation with no chiller does not permit the output of any chiller report variables. The user may need to examine the RDD or MDD to find out which report variables are available in a particular simulation. The RDD and MDD are written only if the following is included in the IDF file.
-
-```idf
-Output:Reports, VariableDictionary;
-```
-
-A variant produces the same files in a IDF “ready� format.
-
-```idf
-Output:Reports, VariableDictionary, IDF;
-```
-
-#### dxf
-
-This is a file in AutoCadâ„¢ DXF format showing all the surfaces defined in the IDF file. It provides a means of viewing the building geometry. The DXF file from EnergyPlus highlights different building elements (shading, walls, subsurfaces) in differing colors. A number of programs can read and display DXF files. Output of this file is triggered by
-
-```idf
-Output:Reports, Surfaces, DXF;
-```
-
-in the IDF.
-
-Tutorial Example for running EnergyPlus
-=======================================
-
-The following example is taken directly from the training course “Introduction to EnergyPlus�, Exercise 1.  Of course, it is presented here without the benefit of classroom presentation and discussion but when followed step by step, should provide an introduction of actually using EnergyPlus.
-
-Running EnergyPlus, Building Envelope, Internal Loads, Reports
---------------------------------------------------------------
-
-### Overview
-
-- Rectangular single story building
-
-- Windows in east and west walls
-
-- Single zone with no interior partitions
-
-- Lightweight construction
-
-![Exercise1](media/image011.jpg)
-
-Figure 11. Schematic for Exercise 1
-
-The details of the building construction and operation are shown in the following tables and description. For tutorial purposes, the building is located in Chicago Illinois, one of the weather files supplied with EnergyPlus. These details are listed in a fashion to make for easy entry into EnergyPlus.
-
-### Details of the exercise
-
-#### Surface Constructions
-
-<table class="table table-striped">
-<tr>
-<th>Material  (listed from outside to inside)</th>
-<th>Conductivity (W/m-K)</th>
-<th>Thickness (m)</th>
-<th>U (W/m<sup>2</sup>-K)</th>
-<th>R (m<sup>2</sup>-K/W)</th>
-<th>Density (kg/m<sup>3</sup>)</th>
-<th>C<sub>p</sub> (J/kg-K)</th>
-</tr>
-<tr>
-<td>Walls</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>WOOD SIDING-1</td>
-<td>0.140</td>
-<td>0.009</td>
-<td>15.556</td>
-<td>0.064</td>
-<td>530</td>
-<td>900</td>
-</tr>
-<tr>
-<td>FIBERGLASS QUILT-1</td>
-<td>0.040</td>
-<td>0.066</td>
-<td>0.606</td>
-<td>1.650</td>
-<td>12</td>
-<td>840</td>
-</tr>
-<tr>
-<td>PLASTERBOARD-1</td>
-<td>0.160</td>
-<td>0.012</td>
-<td>13.333</td>
-<td>0.075</td>
-<td>950</td>
-<td>840</td>
-</tr>
-<tr>
-<td>Roof</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>ROOF DECK</td>
-<td>0.140</td>
-<td>0.019</td>
-<td>7.368</td>
-<td>0.136</td>
-<td>530</td>
-<td>900</td>
-</tr>
-<tr>
-<td>FIBERGLASS QUILT-2</td>
-<td>0.040</td>
-<td>0.066</td>
-<td>0.606</td>
-<td>1.650</td>
-<td>12</td>
-<td>840</td>
-</tr>
-<tr>
-<td>PLASTERBOARD-2</td>
-<td>0.160</td>
-<td>0.010</td>
-<td>1.60</td>
-<td>0.625</td>
-<td>950</td>
-<td>840</td>
-</tr>
-<tr>
-<td>Floor</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>C5 CONCRETE</td>
-<td>1.73</td>
-<td>0.1015</td>
-<td>17.04</td>
-<td>0.059</td>
-<td>2243</td>
-<td>837</td>
-</tr>
-</table>
-
-#### Window Properties
-
-<table class="table table-striped">
-<tr>
-<th>Type *</th>
-<th>Clear</th>
-</tr>
-<tr>
-<td>Number of panes</td>
-<td>2</td>
-</tr>
-<tr>
-<td>Pane thickness</td>
-<td>0.006 m</td>
-</tr>
-<tr>
-<td>Air-gap thickness</td>
-<td>0.0032 m</td>
-</tr>
-<tr>
-<td>Conductivity of glass</td>
-<td>0.9 W/m-K</td>
-</tr>
-</table>
-
-
-
-Refers to specific glass type included in the EnergyPlus datasets directory
-
- (**WindowGlassMaterials.idf**)
-
-<table class="table table-striped">
-<caption>Additional Model Details</caption>
-<tr>
- <th>Type</th>
- <th>Details</th>
-</tr>
-<tr>
- <td>Internal Loads</td>
- <td>Lights (1000 W), Office Lighting schedule, surface mount fluorescent</td>
-</tr>
-<tr>
- <td>Space Conditioning</td>
- <td>Heating setpoint 20C, cooling setpoint 24C, no setback</td>
-</tr>
-<tr>
- <td>Location</td>
- <td>Chicago, Illinois, USA; Summer and Winter design days</td>
-</tr>
-<tr>
- <td>Simulation Period</td>
- <td>Annual, Jan 1 - Dec 31</td>
-</tr>
-<tr>
- <td>Ground Temperatures</td>
- <td>18.2 C to 22.5 C (from Slab preprocessor, vary monthly)</td>
-</tr>
-</table>
-
-Instructions
-------------
-
-### Exercise 1A. Run Pre-Defined Building with no Windows
-
-Objective:  Learn to use EP-Launch to run an EnergyPlus input file and view output files.
-
-1. Open EP-Launch.
-
-2. Under “Input File�, browse for input file Exercise1A.idf.  This input file contains the 1-zone model described above without the windows and lights. This is located under the install folder &lt;root&gt;\\ExampleFiles\\BasicsFiles,
-
-3. Under “Weather File�, select “No Weather File� (at the top of the pull-down list).
-
-4. Press “Simulate�.
-
-5. When the simulation is complete, review output files:
-
-  - Press “Text Output Files� to see all text output.  Look especially at the eio and err output files.
-
-  - Press “Drawing Files� to see a dxf drawing of the building envelope.  (If using Voloview Express, right-click to switch between wireframe and shaded orbit view.  In DWG True View, use “View� -&gt; “Visual Styles� to switch between wireframe and solid views. In both programs, use “View� à“Named Views� to select isometric views.)
-
-  - An empty svg drawing file will also open (this will show HVAC system components in later exercises).  Note that the Adobe SVG viewer is a “plug-in� for Internet Explorer (IE), so IE will open when viewing an SVG file.  Depending on the security settings in IE, you may be prompted with a warning about “active� content.
-
-  - Press “Spreadsheets� to open the numeric csv output files.  In Exercise1a.csv, review the pattern of outdoor conditions and loads.  (To make it easier to read the column headings, select Row 1, format cells, and turn on wrap text; then select cell B2 and select “freeze panes�.)  In Exercise1aMeter.csv, review the facility district heating and cooling meters.
-
-  - Zone/Sys Air Temperature – the zone air temperatures are already being reported.
-
-  - Outdoor Dry Bulb – is being reported (so you can compare to outside temperature)
-
-  - The meter for the heating in the facility - DistrictHeating:Facility – is being reported. Facility is the entire building.
-
-  - The meter for the cooling in the facility - DistrictCooling:Facility – is being reported.
-
-### Exercise 1B. Add Windows
-
-Objective:  Learn how to add materials, constructions, and a surface using 3-D coordinates.
-
-1. In EP-Launch, with input file Exercise1A.idf still selected, press “Edit – IDF Editor�.  This will open Exercise1A.idf in the IDF Editor, a tool that assists in editing EnergyPlus input files (idf).
-
-2. In IDF Editor, select File -&gt; Save Options . . . and set “Saved Order� to “Original with New at Top�, and “Special Format for Some Objects� to “Yes.�  Check the “Set as Default� box.
-
-3. In IDF Editor, Select File -&gt; Save As . . . and save this file as Exercise1B.idf.
-
-4. Create the construction definition for the windows which are double-pane clear gas with an air space:
-
-  - Using File -&gt; Open Dataset, open the window glass materials dataset file, WindowGlassMaterials.idf
-
-  - Scroll down the Class list and select “**WindowMaterial:Glazing**�.
-    
-    -Hint:  In IDF Editor, View -&gt; Show Classes with Objects Only (or ctl-L) will hide all empty object types from the class list.
-
-  - Locate the object which defines the material properties for “CLEAR 6MM�.  Select this object (by clicking on the column heading).
-
-  - Using Edit -&gt; Copy Object (or the toolbar button, or ctl-C), copy this object.
-
-  - Switch windows to file Exercise1B.idf and paste the window material into this file.  (Verify that is had been added by going to **WindowMaterial:Glazing** to view the object.)
-
-  - Open dataset file WindowGasMaterials.idf.
-
-  - Locate “AIR 3MM�, copy it and paste it into Exercise1B.idf.
-
-  - In Exercise1B.idf, select the “**Construction**� class.  There are three constructions pre-defined for the walls, roof, and floor.
-
-  - Press “New Obj� to create a new blank **Construction** object.
-
-  - Name this new construction “DOUBLE PANE WINDOW�.
-
-  - Use the pulldown list to select “CLEAR 6MM� for the outside layer, then press “Enter� or “Return� to save this entry and move to the next field.
-
-  - Select “AIR 3MM� for Layer 2, and “CLEAR 6MM� for Layer 3.
-
-5. Add the east window (3m wide by 2m high, centered on wall, *see the drawing in* *Figure 11* *to determine coordinates):*
-
-  - Select “**FenestrationSurface:Detailed**� class.
-
-  - Add a new object named “EAST WINDOW�.
-
-  - Set the remaining fields as listed:
-
-  - Surface Type ................................................ = Window
-
-  - Construction Name ............ = DOUBLE PANE WINDOW
-
-  - Base Surface Name ............... = ZONE SURFACE EAST
-
-  - OutsideFaceEnvironment Object ................... = &lt;blank&gt;
-
-  - View Factor to Ground .......................... = autocalculate
-
-  - Name of shading control .............................. = &lt;blank&gt;
-
-  - WindowFrameAndDivider Name .................... = &lt;blank&gt;
-
-  - Multiplier ................................................................ = 1
-
-  - Number of Surface Vertex Groups ........................... = 4
-
-  - Vertex coordinates = *as determined from the drawing* *Figure 11*.  Coordinates in this input are in World Coordinates (all relative to the global origin of 0,0,0).  Coordinates are specified as viewed from the outside of the surface, using the rules specified in the SurfaceGeometry object.
-
-6. Add the west window, similar to the east window.
-
-7. Add a new **Output:Surfaces:List** object, type= Details.  This report produces a list of all surfaces in the eio output summarizing area, azimuth, tilt, etc.
-
-8. Save and close the IDF file, select Exercise1B.idf in EP-Launch, run the simulation and view outputs.
-
-  - Always review the err file for errors and warnings.  Fix problems if needed and re-run.
-
-  - Are the windows in the right place in the dxf drawing file. (Use the Drawing File button or select the DXF file from View -&gt; Single File or from the Quick-Open panel).
-
-  - Review the surface details report in the eio file, search for “Zone/Shading Surfaces� to find this report. (Use the Text Output button, Quick Open “eio� button, or select from the single file menu, or use F7).  This report is easier to read by pasting this section into a spreadsheet and using the text to columns function with comma as a delimiter).
-
-  - Open the csv output file and compare the heating and cooling loads with the results from Exercise1A.csv.
-
-### Exercise 1C. Add Internal Loads
-
-Objective:  Learn how to add schedules, internal loads, and report variables.
-
-1. Save Exercise1B.idf as Exercise1C.idf.
-
-2. Open the dataset file Schedules.idf:
-
-  - Copy the **Schedule:Compact** object named “Office Lighting�, and paste it into Exercise1C.idf.
-
-  - Copy the **ScheduleTypeLimits** object named “Fraction�, and paste it into Exercise1C.idf.
-
-3. In Exercise1C.idf, add a LIGHTS object named ZONE ONE Lights, using the Office Lighting schedule, peak input is 1000W.  Consult the EnergyPlus Input Output Reference section on **Lights** for values for the return, radiant, and visible fractions.  Assume the lights are surface mounted fluorescents.
-
-4. Save and close the IDF file, select Exercise1C.idf in EP-Launch, run the simulation and review outputs.
-
-5. Open the rdd file (the report variable data dictionary) and find report variable names related to **Lights**.  Add a new **Output:Variable** object to report the lighting electric consumption.
-
-6. Run the simulation and review outputs.
-
-  - Check the err file.
-
-  - Find the lighting electric consumption in the csv output file.
-
-7. Compare heating and cooling loads with Exercise1A and Exercise1B.
-
-8. Add more **Output:Variable** objects as desired.
-
-### Exercise 1D. Annual Simulation and Predefined Reports
-
-Objective:  Learn how to run an annual simulation using a weather data file and add table reports.
-
-1. Save Exercise1C.idf as Exercise1D.idf.
-
-2. Edit the **SimulationControl** object to turn off the design day simulations by setting “Run Simulation for Sizing Periods� to **No** and turn on the weather file (annual) simulation by setting “Run Simulation for Weather File Run Periods� to **Yes**..
-
-3. Add a RunPeriod object to run a full annual simulation, let other fields default or remain blank.
-
-4. Add a **Output:Table:SummaryReports** object, and select the following reports:  “Annual Building Performance Summary� (ABUPS), “Input Verification and Results Summary� (IVRS), “Climate Summary�, and “Envelope Summary�.
-
-5. Add a **OutputControl:Table:Style** object, and select HTML format (ColumnSeparator).
-
-6. Edit existing **Output:Variable** and **Output:Meter** objects and change the reporting frequency from Hourly to Monthly.
-
-7. Save and close the IDF file, select Exercise1D.idf in EP-Launch.
-
-8. Select Chicago TMY2 weather file (or the weather file of your choice) and run the simulation.
-
-9. Review outputs.
-
-  - Check the err file.
-
-  - Look at the monthly results in the csv output.
-
-  - Press the Table output button to view the predefined reports.
-
-### Solution: Exercise 1
-
-*Try not to look at this section until you have completed the Exercise.*
-
-#### List of New Objects
-
-This is a listing of new and modified objects created in this Exercise.
-
-```
-WindowMaterial:Glazing,
-    CLEAR 6MM,               !- Name
-    SpectralAverage,         !- Optical Data Type
-    ,                        !- Name of Window Glass Spectral Data Set
-    0.006,                   !- Thickness {m}
-    0.775,                   !- Solar Transmittance at Normal Incidence
-    0.071,                   !- Solar Reflectance at Normal Incidence: Front Side
-    0.071,                   !- Solar Reflectance at Normal Incidence: Back Side
-    0.881,                   !- Visible Transmittance at Normal Incidence
-    0.080,                   !- Visible Reflectance at Normal Incidence: Front Side
-    0.080,                   !- Visible Reflectance at Normal Incidence: Back Side
-    0.0,                     !- IR Transmittance at Normal Incidence
-    0.84,                    !- IR Hemispherical Emissivity: Front Side
-    0.84,                    !- IR Hemispherical Emissivity: Back Side
-    0.9;                     !- Conductivity {W/m-K}
-
-WindowMaterial:Gas,
-    AIR 3MM,                 !- Name
-    Air    ,                 !- Gas Type
-    0.0032;                  !- Thickness {m}
-
-Construction,
-    DOUBLE PANE WINDOW,      !- Name
-    CLEAR 6MM,               !- Outside Layer
-    AIR 3MM,                 !- Layer #2
-    CLEAR 6MM;               !- Layer #3
-
-FenestrationSurface:Detailed,
-    EAST WINDOW,             !- User Supplied Surface Name
-    WINDOW,                  !- Surface Type
-    DOUBLE PANE WINDOW,      !- Construction Name of the Surface
-    ZONE SURFACE EAST,       !- Base Surface Name
-    ,                        !- OutsideFaceEnvironment Object
-    autocalculate,           !- View Factor to Ground
-    ,                        !- Name of shading control
-    ,                        !- WindowFrameAndDivider Name
-    1,                       !- Multiplier
-    4,                       !- Number of vertices
-    8, 1.5, 2.35,            !- X,Y,Z  1 {m}
-    8, 1.5, 0.35,            !- X,Y,Z  2 {m}
-    8, 4.5, 0.35,            !- X,Y,Z  3 {m}
-    8, 4.5, 2.35;            !- X,Y,Z  4 {m}
-
-FenestrationSurface:Detailed,
-    WEST WINDOW,             !- User Supplied Surface Name
-    WINDOW,                  !- Surface Type
-    DOUBLE PANE WINDOW,      !- Construction Name of the Surface
-    ZONE SURFACE WEST,       !- Base Surface Name
-    ,                        !- OutsideFaceEnvironment Object
-    autocalculate,           !- View Factor to Ground
-    ,                        !- Name of shading control
-    ,                        !- WindowFrameAndDivider Name
-    1,                       !- Multiplier
-    4,                       !- Number of Vertices
-    0, 4.5, 2.35,            !- X,Y,Z  1 {m}
-    0, 4.5, 0.35,            !- X,Y,Z  2 {m}
-    0, 1.5, 0.35,            !- X,Y,Z  3 {m}
-    0, 1.5, 2.35;            !- X,Y,Z  4 {m}
-
-Output:Surfaces:List,Details;
-
-Schedule:Compact,
-    Office Lighting,         !- Name
-    Fraction,                !- ScheduleType
-    Through: 12/31,          !- Complex Field #1
-    For: Weekdays SummerDesignDay,  !- Complex Field #2
-    Until: 05:00, 0.05,      !- Complex Field #4
-    Until: 07:00, 0.1,       !- Complex Field #6
-    Until: 08:00, 0.3,       !- Complex Field #8
-    Until: 17:00, 0.9,       !- Complex Field #10
-    Until: 18:00, 0.5,       !- Complex Field #12
-    Until: 20:00, 0.3,       !- Complex Field #14
-    Until: 22:00, 0.2,       !- Complex Field #16
-    Until: 23:00, 0.1,       !- Complex Field #18
-    Until: 24:00, 0.05,      !- Complex Field #20
-    For: Saturday WinterDesignDay,  !- Complex Field #21
-    Until: 06:00, 0.05,      !- Complex Field #23
-    Until: 08:00, 0.1,       !- Complex Field #25
-    Until: 12:00, 0.3,       !- Complex Field #27
-    Until: 17:00, 0.15,      !- Complex Field #29
-    Until: 24:00, 0.05,      !- Complex Field #31
-    For: Sunday Holidays AllOtherDays,  !- Complex Field #32
-    Until: 24:00, 0.05;      !- Complex Field #34
-
-ScheduleTypeLimits,
-    Fraction,                !- ScheduleType Name
-    0.0,                     !- Lower Limit Value
-    1.0,                     !- Upper Limit Value
-    CONTINUOUS;              !- Numeric Type
-
-Lights,
-    ZONE ONE Lights,         !- Name
-    ZONE ONE,                !- Zone Name
-    Office Lighting,         !- Schedule Name
-    LightingLevel,           !- Design Level Calculation Method
-    1000,                    !- Lighting Level {W}
-    ,                        !- Watts per Zone Floor Area {W/m2}
-    ,                        !- Watts per Person {W/person}
-    0,                       !- Return Air Fraction
-    0.72,                    !- Fraction Radiant
-    0.18,                    !- Fraction Visible
-    1,                       !- Fraction Replaceable
-    General,                 !- End-Use Subcategory
-    No;                      !- Return Air Fraction Calculated from Plenum Temperature
-
-Output:Variable,*,Lights Electric Consumption ,hourly;
-
-RunPeriod,
-    1,                       !- Begin Month
-    1,                       !- Begin Day Of Month
-    12,                      !- End Month
-    31,                      !- End Day Of Month
-    UseWeatherFile,          !- Day Of Week For Start Day
-    Yes,                     !- Use WeatherFile Holidays/Special Days
-    Yes,                     !- Use WeatherFile DaylightSavingPeriod
-    No,                      !- Apply Weekend Holiday Rule
-    Yes,                     !- Use WeatherFile Rain Indicators
-    Yes,                     !- Use WeatherFile Snow Indicators
-    1;                       !- Number of years of simulation
-
-Output:Table:SummaryReports,
-    Annual Building Utility Performance Summary,  !- ReportName1
-    Input Verification and Results Summary,  !- ReportName2
-    Climate Summary,         !- ReportName3
-    Envelope Summary;        !- ReportName4
-
-OutputControl:Table,
-    HTML;                    !- ColumnSeparator
-
-SimulationControl,
-    No,                      !- Do the zone sizing calculation
-    No,                      !- Do the system sizing calculation
-    No,                      !- Do the plant sizing calculation
-    No,                      !- Do the design day simulations
-    Yes;                     !- Do the weather file simulation
-```
-
-Overall scheme/methodology for running EnergyPlus
-=================================================
-
-Building Simulation
--------------------
-
-If you are already familiar with modeling buildings, particularly modeling buildings for energy consumption, you may wish to skip to “IDF Editor – Brief Introduction�. The following steps are general guidelines for using any building simulation program.
-
-A Methodology for Using Energyplus
-----------------------------------
-
-This section provides a step by step outline that will help you streamline creating your building models for using EnergyPlus.
-
-### *Step 1*: Plan Ahead
-
-Some preliminary steps will facilitate the construction of your input file. EnergyPlus requires some information in specified, externally available formats; other information may require some lead time to obtain. The following checklist should be completed before you start to construct your input file.
-
-- Obtain location and design climate information for the city in which your building is located. If possible, use one of the weather files available for your weather period run.
-
-- Obtain sufficient *building* *construction* information to allow specification of overall building geometry and surface constructions (including exterior walls, interior walls, partitions, floors, ceilings, roofs, windows and doors).
-
-- Obtain sufficient *building* *use* information to allow specification of the lighting and other equipment (e.g. electric, gas, etc.) and the number of people in each area of the building.
-
-- Obtain sufficient *building* *thermostatic* *control* information to allow specification of the temperature control strategy for each area of the building.
-
-- Obtain sufficient *HVAC* *operation* information to allow specification and scheduling of the fan systems.
-
-- Obtain sufficient *central plant* information to allow specification and scheduling of the boilers, chillers and other plant equipment.
-
-### *Step 2: "*Zone" the Building
-
-A building "surface" is the fundamental element in the building model. In the general sense, there are two types of "surfaces" in EnergyPlus. These are:
-
-1.   heat transfer surfaces  and
-
-2.   heat storage surfaces
-
-The first rule of building modeling is, "*Always define a surface as a heat storage surface unless it must be defined as a heat transfer surface*". Any surface, which is expected to separate spaces of significantly different temperatures, must be defined as a *heat transfer surface.* Thus, exterior surfaces, such as outside walls, roofs and floors, are *heat transfer surfaces*. Interior surfaces (partitions) are *heat storage surfaces* if they separate spaces maintained at the same temperature and *heat transfer surfaces* if they separate spaces maintained at different temperatures. A discussion of how to define heat transfer and heat storage surfaces will occur in later steps. In order to correctly "zone" the building it is necessary only to distinguish between the two.
-
-A "zone" is a *thermal,* not a *geometric,* concept. A “zone� is an air volume at a uniform temperature plus all the heat transfer and heat storage surfaces bounding or inside of that air volume. EnergyPlus calculates the energy required to maintain each zone at a specified temperature for each hour of the day. Since EnergyPlus performs a zone heat balance, the first step in preparing a building description is to break the building into zones. The objective of this exercise is to define as *few* zones as possible without significantly compromising the integrity of the simulation.
-
-Although defining building zones is somewhat of an art, a few general rules will keep the new simulation user out of trouble. Consider the following figure, which shows the floor plan of an Adult Education Center.
-
-![](media/image012.png)
-
-Figure 12. Adult Education Center
-
-The question is, "How many *thermal* zones should be used to model this building?"  The inexperienced building modeler may be tempted to define each room in the building as a zone, but the thermal zone is defined as a volume of air at a uniform temperature. The general rule then is to *use the number of fan systems (and radiant systems) not the number of rooms to determine the number of zones in the building.* The minimum number of zones in a general simulation model will usually be equal to the number of systems serving the building. The collection of heat transfer and heat storage surfaces defined within each zone will include all surfaces bounding or inside of the space conditioned by the system.
-
-### Zoning – Concept 1 - Simple
-
-Complete estimates of the total building load (magnitude only) may be obtained with very simple models. For example the total building load calculated using a one-zone model of the Education Center (Figure 13) will **NOT** be significantly different from the total building load calculated using a more detailed model. The *distribution* of the load within the building cannot be estimated with the simplified building model, but its *magnitude* (such as would be used in sizing the central plant equipment) can be quickly estimated using a very simple model. For simplicity, assume there is no ground heat transfer; if you want to simulate ground heat transfer, you should use the slab and/or basement programs as described in the Auxiliary Programs document.
-
-![](media/image013.png)
-
-Figure 13. Single Zone Model of the Adult Education Center.
-
-### Zoning – Concept 2 - Detailed
-
-A more detailed model will allow you to determine more accurately the actual distribution of loads/energy within the building. In a more detailed model of the education center, five systems were designed to serve the Adult Education Center. These systems with the thermal zones they serve are shown in the table below. The location of each zone is shown in accompanying figure.
-
-Table 2. Zoning the Building by System Type.
-
-<table class="table table-striped">
-<tr>
-<th>System Number</th>
-<th>System Name</th>
-<th>CFM</th>
-<th>m/s</th>
-<th>Zone Served</th>
-</tr>
-<tr>
-<td>1</td>
-<td>Four Pipe Fan Coil</td>
-<td>3900</td>
-<td>19.812</td>
-<td>Zone 1</td>
-</tr>
-<tr>
-<td>1</td>
-<td>Four Pipe Fan Coil</td>
-<td>2500</td>
-<td>12.7</td>
-<td>Zone 2</td>
-</tr>
-<tr>
-<td>2</td>
-<td>Single Zone Draw Through</td>
-<td>1400</td>
-<td>7.112</td>
-<td>Zone 3</td>
-</tr>
-<tr>
-<td>3</td>
-<td>Single Zone Draw Through</td>
-<td>2250</td>
-<td>11.43</td>
-<td>Zone 5</td>
-</tr>
-<tr>
-<td>4</td>
-<td>Single Zone Draw Through</td>
-<td>2450</td>
-<td>12.446</td>
-<td>Zone 6</td>
-</tr>
-<tr>
-<td>5</td>
-<td>Unit Heater</td>
-<td>185</td>
-<td>.9398</td>
-<td>Zone 4</td>
-</tr>
-<tr>
-<td>5</td>
-<td>Unit Heater</td>
-<td>41</td>
-<td>.20828</td>
-<td>Zone 7</td>
-</tr>
-</table>
-
-
-
-![](media/image014.png)
-
-Figure 14. Thermal Zones in the Education Center
-
-Take note of Zone 1, Zone 2, Zone 4, and Zone 7. The two important zoning concepts can be demonstrated with the zoning to reinforce the idea of a thermal zone and encourage the use of simplified models.
-
-1.   Notice that Zones 4 and 7 include two rooms that are not adjacent to one another but are served by the same system. Because the air temperature in the two spaces is maintained at the same uniform temperature, the two spaces, though separated spatially, may be defined as a single zone. For our purposes, we will define them as separate zones.
-
-2.   Notice that Zone 1 and Zone 2 are served by the same fan system and could be defined as a single zone with 7650 cfm of conditioned air supplied to the space. The space was split into two zones because the designer expected higher solar loads on the South and West sides of the wing and wanted to examine the *distribution* as well as the *magnitude* of the load in the space.
-
-### *Step 3:* Prepare to Construct the Building Model
-
-Working from blueprints or sketches and following the guidelines in Step 2, the building zones were determined. It is recommended that the engineer sketch the building with its zones. Surface dimensions should be included in the sketch. Additional geometric and surface information is required before an input file describing the building can be constructed. Specifically the building model must:
-
-1.   Determine *heat transfer* and *heat storage* surfaces.
-
-2.   Define equivalent surfaces.
-
-3.   Specify surfaces and subsurfaces (windows, doors, etc.) construction and materials.
-
-4.   Compile surface and subsurface information.
-
-By the way, the file for this example, the 1 zone model are contained in your EnergyPlus installation ExampleFiles\\BasicFiles folder.
-
-#### Step 3.1.      Determine heat transfer and heat storage surfaces.
-
-The surfaces of the building can be described in any order; grouping surfaces by zone may help you read the input file. Specifics of the describing surfaces help categorize the surface’s heat transfer/storage as well as identify the surface construction information.
-
-The details of inputting surfaces are described in the Input/Output Reference document. The allowable surface types are shown in the following table:
-
-Table 3. Surface types and categorization
-
-<table class="table table-striped">
-<tr>
-<th>Surface Type</th>
-<th>Applicability</th>
-</tr>
-<tr>
-<td>BuildingSurface:Detailed</td>
-<td>Wall, Roof, Ceiling, Floor</td>
-</tr>
-<tr>
-<td>FenestrationSurface:Detailed</td>
-<td>Window, Door, Glassdoor</td>
-</tr>
-<tr>
-<td>InternalMass</td>
-<td>Areas internal to a zone</td>
-</tr>
-<tr>
-<td>Shading:Site:Detailed</td>
-<td>Shading devices external to the building face (other buildings, trees, etc.)</td>
-</tr>
-<tr>
-<td>Shading:Zone:Detailed</td>
-<td>Shading devices attached to the building (overhang, fin)</td>
-</tr>
-</table>
-
-The pieces of the definition that designate BuildingSurface:Detailed surfaces as either *heat transfer* or *heat storage* surfaces are:
-
-```idf
-  A5 , \field Outside Boundary Condition
-       \required-field
-       \type choice
-       \key Surface
-       \key Zone
-       \key Outdoors
-       \key Ground
-       \key OtherSideCoefficients
-       \key OtherSideConditionsModel
-  A6,  \field Outside Boundary Condition Object
-       \type object-list
-       \object-list OutFaceEnvNames
-       \note Non-blank only if the field Outside Boundary Condition is Surface, Zone, OtherSideCoefficients,
-       \note or OtherSideConditionsModel
-       \note If Surface, specify name of corresponding surface in adjacent zone or
-       \note specify current surface name for internal partition separating like zones
-       \note If Zone, specify the name of the corresponding zone and
-       \note the program will generate the corresponding interzone surface
-       \note If OtherSideCoefficients, specify name of SurfaceProperty:OtherSideCoefficients
-       \note If OtherSideConditionsModel, specify name of SurfaceProperty:OtherSideConditionsModel
-  A7 , \field Sun Exposure
-       \required-field
-       \type choice
-       \key SunExposed
-       \key NoSun
-       \default SunExposed
-  A8,  \field Wind Exposure
-       \required-field
-       \type choice
-       \key WindExposed
-       \key NoWind
-       \default WindExposed
-```
-
-
-Note that subsurfaces (windows, doors) on these base surfaces will inherit the base surface properties listed above. The following examples will use a bit more of the Surface definition to give context.
-
-Surfaces that specify “themselves� as the outside boundary condition are ceilings, floors and partitions that divide temperature-controlled spaces. The program assumes that the surface temperatures on both sides of the surface are the same. This means that even though heat may be stored in a partition, ceiling, or floor, no heat flows *through* it.
-
-Heat Storage Surfaces (Use current Surface name for ExteriorEnvironment), e.g.:
-
-```idf
-BuildingSurface:Detailed,Zn005:Wall006,  !- Base Surface Name
-  Wall,INTERIOR,  !- Class and Construction Name
-  MAINE WING,  !- Zone
-  Surface, Zn005:Wall006,  !- Exterior Conditions and Target
-   NoSun,  !- Solar Exposure
-   NoWind,  !- Wind Exposure
-  0.5000000    ,  !- VF to Ground
-           4, !-Rectangle
-   57.90000    ,   57.79000    ,   10.00000    ,
-   57.90000    ,   57.79000    ,  0.0000000E+00,
-   57.90000    ,   47.79000    ,  0.0000000E+00,
-   57.90000    ,   47.79000    ,   10.00000    ;
-```
-
-
-Some surfaces divide the temperature controlled space from the outside environment. Surfaces that are both sun and wind exposed (e.g. exterior walls, exposed floors, roofs) feel the full effect of both solar radiation and outside temperature, and the outside air film resistance for these surfaces changes with wind speed and wind direction. Surfaces that are not sun or wind exposed (a wall to an “uncontrolled� space) are not affected by solar radiation, wind speed or direction and have a constant outside convective air film resistance.
-
-Heat Transfer Surfaces Exposed to the Outside Environment, such as Exterior Walls, Roofs, Exposed Floors:
-
-```idf
-BuildingSurface:Detailed,Zn005:Wall002,  !- Base Surface Name
-  Wall,EXTERIOR,  !- Class and Construction Name
-  MAINE WING,  !- Zone
-  Outdoors,,  !- Exterior Conditions and Target (if applicable)
-   SunExposed,  !- Solar Exposure
-   WindExposed,  !- Wind Exposure
-  0.5000000    ,  !- VF to Ground
-           4, !-Rectangle
-   77.90000    ,   47.79000    ,   10.00000    ,
-   77.90000    ,   47.79000    ,  0.0000000E+00,
-   77.90000    ,   67.79000    ,  0.0000000E+00,
-   77.90000    ,   67.79000    ,   10.00000    ;
-```
-
-
-Surfaces such as basement walls and slab floors separate the space from the earth surrounding the surfaces. Therefore, the outside surface temperatures become the ground temperatures.
-
-Heat Transfer Surfaces in Contact with the Ground, such as Basement Walls or Slab Floors:
-
-```idf
-BuildingSurface:Detailed,Zn004:Flr001,  !- Base Surface Name
-  Floor,SLAB FLOOR,  !- Class and Construction Name
-  ARIZONA WING,  !- Zone
-  Ground,,  !- Exterior Conditions and Target (if applicable)
-   NoSun,  !- Solar Exposure
-   NoWind,  !- Wind Exposure
-   1.000000    ,  !- VF to Ground
-           4, !-Rectangle
-   38.01000    ,   8.510000    ,  0.0000000E+00,
-   18.01000    ,   8.510000    ,  0.0000000E+00,
-   18.01000    ,   28.51000    ,  0.0000000E+00,
-   38.01000    ,   28.51000    ,  0.0000000E+00;
-```
-
-Other surfaces separate zones that may be at different temperatures. These surface types allow heat transfer (by conduction through the walls) from a zone at a higher temperature to a zone at a lower temperature. The location of the heat storage surface in the zone is not important except in specialized solar studies. The surface above (wall to uncontrolled space) would be more correctly modeled as an interzone surface.
-
-Heat Transfer Surfaces Exposed to Another Zone, such as Interzone walls, ceilings or floors:
-
-```idf
-BuildingSurface:Detailed,Zn005:Wall005,  !- Base Surface Name
-  Wall,INTERIOR,  !- Class and Construction Name
-  MAINE WING,  !- Zone
-  Surface,Zn001:Wall009,  !- Exterior Conditions and Target
-   NoSun,  !- Solar Exposure
-   NoWind,  !- Wind Exposure
-  0.5000000    ,  !- VF to Ground
-           4, !-Rectangle
-   57.90000    ,   47.79000    ,   10.00000    ,
-   57.90000    ,   47.79000    ,  0.0000000E+00,
-   67.90000    ,   47.79000    ,  0.0000000E+00,
-   67.90000    ,   47.79000    ,   10.00000    ;
- 
-```
-
-
-#### Step 3.2.     Define equivalent surfaces as desired.
-
-When the building was zoned, our objective was to define as *few* zones as possible. Now we would like to extend this objective to include defining as *few* surfaces as possible without significantly compromising the integrity of the simulation. We reduce the number and complexity of surfaces in our input file by defining *equivalent* surfaces.
-
-Before dealing with equivalent surfaces, it is appropriate to take the concept of a thermal zone one step further. EnergyPlus performs heat balances on individual zone surfaces and on the zone air. For purposes of the heat transfer calculations, a *geometrically* correct rendering of the zone surfaces is not required. The surfaces do not even have to be connected. As long as the program knows to which thermal zone (mass of air) each surface transfers heat, it will calculate all heat balances correctly. For example, all heat storage surfaces of the same construction within a zone may be defined as a single rectangular surface. The size of this *equivalent* surface will equal the sum of all the areas of all the heat storage surfaces in the zone. A few simple rules will further explain what we mean by *equivalent* surfaces and how these surfaces may be used. Remember that these are guidelines for optional simplification of input. Each simplification must be evaluated to determine if it would significantly impact certain shading, interior solar gains, or daylighting features. The goal is to seek an adequate level of detail to capture the key features of the building envelope without spending excess time describing and computing results for details that are insignificant.
-
-1.   *Define all roofs and floors as rectangles regardless of the shape of the zone.* Each zone may have one rectangular roof and one rectangular floor of a given construction.
-
-2.   *Define all heat storage surfaces of the same construction within a zone as a single surface*. The size of the single surface is obtained by summing the individual surface areas exposed to the zone. Thus, if a partition is completely within a zone (both sides of the partition are exposed to the zone), the area of each side must be added to the area of the equivalent surface. On the other hand, if the partition separates two zones, the area of only one side should be added to the equivalent surface.
-
-3.   *Combine all windows on a given exterior surface into a single window*. Usually each exterior surface should have only one window of each type. Overhangs or other shading devices may require that more windows be specified or combined together. By using the WindowMaterial:Glazing construction for your glass door, they will be correctly modeled in EnergyPlus with sunlight transferring into the zone.
-
-The following figure shows the surfaces and subsurfaces required for a one-zone model, i.e., the education center. Since there were two types of partitions in the building, two heat storage surfaces ("internal mass") of different constructions were defined.
-
-![](media/image015.png)
-
-Figure 15. Simplifications Using Equivalent Surfaces
-
-#### Step3.3.      Specify construction elements
-
-BLAST, DOE-2 and other programs often have “libraries� of constructions, schedules, and other aspects of simulating the building. In EnergyPlus, we have a special set of files in the DataSets folder that represent many facets of building simulation. Data sets are usually IDF snippets or macro files. For constructions, using the guidelines in the ASHRAE Handbook of Fundamentals (2005), the file ASHRAE\_2005\_HOF\_Materials.idf contains materials and constructions from Chapters 30 and 25. Since Chapter 30 discusses heating and cooling loads, it includes constructions for light, medium and heavy weight buildings – these constructions are represented in the dataset file. For the education center, “medium� constructions are used. For the windows, we will use the Double Pane Window from the previous exercise.
-
-<table class="table table-striped">
-<tr>
-<th>Type (1)</th>
-<th>Name (2)</th>
-<th>Material (3)</th>
-</tr>
-<tr>
-<td>Wall</td>
-<td>Medium Exterior Wall</td>
-<td>M01 100mm brick</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>I02 50mm insulation board</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>F04 Wall air space resistance</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>G01a 19mm gypsum board</td>
-</tr>
-<tr>
-<td>Window</td>
-<td>Double Pane Window</td>
-<td>Clear 6MM</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>Air 3MM</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>Clear 6MM</td>
-</tr>
-<tr>
-<td>Partition</td>
-<td>Medium/Heavy Partitions</td>
-<td>G01a 19mm gypsum board</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>M01 100mm brick</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>M05 200mm concrete block</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>G01a 19mm gypsum board</td>
-</tr>
-<tr>
-<td>Partition</td>
-<td>Medium Partitions</td>
-<td>G01a 19mm gypsum board</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>F04 Wall air space resistance</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>G01a 19mm gypsum board</td>
-</tr>
-<tr>
-<td>Wall</td>
-<td>Heavy/Medium Partitions</td>
-<td>G01a 19mm gypsum board</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>M05 200mm concrete block</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>M01 100mm brick</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>G01a 19mm gypsum board</td>
-</tr>
-<tr>
-<td>Roof</td>
-<td>Medium Roof/Ceiling</td>
-<td>M14a 100mm heavyweight concrete</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>F05 Ceiling air space resistance</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>F16 Acoustic tile</td>
-</tr>
-<tr>
-<td>Floor</td>
-<td>Medium Floor</td>
-<td>F16 Acoustic tile</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>F05 Ceiling air space resistance</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td>M14a 100mm heavyweight concrete</td>
-</tr>
-</table>
-
-Table 4. Building Elements
-
-Notes:
-
-(1)  The surface type is a wall, floor, roof, window or door.
-
-(2) User supplies name for the element. For this example use name from the DataSet: **ASHRAE\_2005\_HOF\_Materials.idf**. Similarly, the window was constructed from the **Windows.idf** dataset.
-
-(3) Material's full name is as found in the ASHRAE\_2005\_HOF\_Materials.idf dataset.
-
-#### Step 3.4.     Compile surface and subsurface information.
-
-*Building information:*
-
-*Building North Axis:* This syntax simplifies building geometry specification by designating one wall of the building as the building’s north pointing axis. The building model North axis is measured from true (compass) North. Surface facing angles (see surface information below) are then specified relative to the building north axis. The *North Axis* entry in the Input Output Reference (duplicated here) illustrates specification of the building north axis.
-
-![](media/image016.png)
-
-Figure 16. Illustration of Building North Axis
-
-
-
-*Zone information:*
-
-1. *Wall height*: In a simple model, one should make all the walls the same height. Then, the simple, 1 zone model can entirely enclose the space. In more complex models, you may resize each wall accordingly.
-
-*Surface information:*
-
-1.   *Base* *Surface Type:* Heat Transfer/Heat Storage Surfaces may be of the following types: wall, floor, roof, internal mass, or subsurface
-
-2.   *Construction:* The type of construction of the surface (see previous table).
-
-*Subsurface information:*
-
-1.    *Subsurfaces* are Windows, Doors or GlassDoors
-
-2.   *Area:* Area of the subsurface.
-
-3.   *Reveal:* For windows only, the distance it is inset from the outside surface of a wall. For simplicity, put all the windows in the same physical plane as the wall they are on.
-
-For the single zone model, the following figure is a schematic representation of a one zone representation. The figure shows the length of all "base" surfaces and the areas of all "subsurfaces" (windows). Doors are shown and may be entered, if desired. In the table (Table 5), the surfaces are numbered counter-clockwise around the zone beginning at the lower left corner of the figure.  This table is the minimum required zone information compiled by the user. A few simple conventions should be followed to facilitate the construction of zone information tables:
-
-1.   Number all surfaces in order counter-clockwise around the zone.
-
-2.   Keep the subsurfaces with the base surface on which they are located.
-
-3.   Specify *lengths* for base surfaces and areas for subsurfaces and internal mass.
-
-4.    Specify the roof and floor as rectangles of the correct size.
-
-![OneZoneEducCenter-takeoff](media/image017.jpg)
-
-Figure 17. Schematic of One Zone Model with Exterior Wall length and Window Areas.
-
-**Full Building – 1 Zone model**
-
-<table class="table table-striped">
-<tr>
-<th>Surface</th>
-<th>type</th>
-<th>construction</th>
-<th>Length {m}</th>
-<th>Area {m<sup>2</sup>}</th>
-</tr>
-<tr>
-<td>1</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>15.25</td>
-<td> </td>
-</tr>
-<tr>
-<td>2</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>5.62</td>
-</tr>
-<tr>
-<td>3</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>4.9</td>
-<td> </td>
-</tr>
-<tr>
-<td>4</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>3.9</td>
-</tr>
-<tr>
-<td>5</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>34.44</td>
-<td> </td>
-</tr>
-<tr>
-<td>6</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>33.7</td>
-</tr>
-<tr>
-<td>7</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>13.2</td>
-<td> </td>
-</tr>
-<tr>
-<td>8</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>9.44</td>
-</tr>
-<tr>
-<td>9</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>10.4</td>
-<td> </td>
-</tr>
-<tr>
-<td>10</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>7.58</td>
-</tr>
-<tr>
-<td>11</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>20</td>
-<td> </td>
-</tr>
-<tr>
-<td>12</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>10.5</td>
-</tr>
-<tr>
-<td>13</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>12</td>
-<td> </td>
-</tr>
-<tr>
-<td>14</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>7.58</td>
-</tr>
-<tr>
-<td>15</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>20</td>
-<td> </td>
-</tr>
-<tr>
-<td>16</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>17.66</td>
-</tr>
-<tr>
-<td>17</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>6.1</td>
-<td> </td>
-</tr>
-<tr>
-<td>18</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>4.7</td>
-</tr>
-<tr>
-<td>19</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>3.1</td>
-<td> </td>
-</tr>
-<tr>
-<td>20</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>6.1</td>
-<td> </td>
-</tr>
-<tr>
-<td>21</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>3.71</td>
-</tr>
-<tr>
-<td>22</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>23</td>
-<td> </td>
-</tr>
-<tr>
-<td>23</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>19.39</td>
-</tr>
-<tr>
-<td>24</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>15.24</td>
-<td> </td>
-</tr>
-<tr>
-<td>25</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>7.8</td>
-</tr>
-<tr>
-<td>26</td>
-<td>exterior wall</td>
-<td>Medium Exterior Wall</td>
-<td>38</td>
-<td> </td>
-</tr>
-<tr>
-<td>27</td>
-<td>window</td>
-<td>Double Pane Window</td>
-<td> </td>
-<td>31</td>
-</tr>
-<tr>
-<td>28</td>
-<td>roof</td>
-<td>Medium Roof/Ceiling</td>
-<td>Equivalent area (square)</td>
-<td>1250.1</td>
-</tr>
-<tr>
-<td>29</td>
-<td>floor</td>
-<td>Medium Floor</td>
-<td>Equivalent area (square)</td>
-<td>1250.1</td>
-</tr>
-<tr>
-<td>30</td>
-<td>internal mass</td>
-<td>Medium Partitions</td>
-<td> </td>
-<td>956.9</td>
-</tr>
-<tr>
-<td>31</td>
-<td>internal mass</td>
-<td>Medium/Heavy Partitions</td>
-<td> </td>
-<td>1757.7</td>
-</tr>
-</table>
-
-Table 5. Compilation of Surface Information for the One Zone Model
-
-The column headings in the previous table have the following meanings:
-
-**Type:**  A shortened notation for the surface type in EnergyPlus to differentiate between heat storage surfaces and various types of heat transfer surfaces.
-
-**Construction:**  A name for the surface construction types.
-
-**Length:**  The length of base surfaces (i.e. Exterior Walls).
-
-**Area:**  The area of subsurfaces (windows), roofs, floors.
-
-### *Step 4:* Compile Internal Space Gain Data
-
-People, lights, equipment, outside air infiltration and ventilation all constitute "internal gains" for the thermal zone. These gains are described to EnergyPlus as a *design or* *peak* level with a *schedule* that specifies a fraction of the peak for each hour. The peak level is calculated by the user. Table 6. Internal Gain Data shows the internal loads for a single zone model of Ft. Monmouth and the schedule named to specify the hourly load.
-
-Table 6. Internal Gain Data
-
-<table class="table table-striped">
-<tr>
-<th>Zone</th>
-<th>Gain Type</th>
-<th>Size</th>
-<th>Schedule</th>
-</tr>
-<tr>
-<td>1</td>
-<td>People</td>
-<td>205</td>
-<td>Office occupancy</td>
-</tr>
-<tr>
-<td> </td>
-<td>Lights</td>
-<td>26360 W</td>
-<td>Office lighting</td>
-</tr>
-<tr>
-<td> </td>
-<td>ZoneInfiltration</td>
-<td>.75 m<sup>3</sup>/sec</td>
-<td>Constant</td>
-</tr>
-</table>
-
-
-
-The column headings in the table have the following meanings:
-
-**Gain Type:**  The code used to differentiate between various types of internal gains.
-
-**Size:**  The peak load. This is the actual size of the load for every hour that the schedule specifies "100%".
-
-**Schedule:**  The hourly schedule that specifies the percentage of peak load for each hour of the day.
-
-**HVAC:** Using the Compact HVAC models, purchased air can be used to calculate the energy needs of the building.
-
-As the following figure shows, the equivalent area floor/roof does not fit in the building perimeter. As an exercise, you might reconfigure both floor and roof to be a polygonal shape and compare results.
-
-![](media/image018.png)
-
-Figure 18. Full Building - Adult Education Center
-
-As an adjunct to the previous schematic layout for the one zone approach, the following figure shows the same building but with IP units:
-
-![](media/image019.jpg)
-
-Figure 19, Schematic for One Zone Building - IP Units
-
-Tutorial Exercise 2
-===================
-
-The following example is taken directly from the training course “Introduction to EnergyPlus�, Exercise 2.  Of course, it is presented here without the benefit of classroom presentation and discussion but when followed step by step, should provide an introduction of actually using EnergyPlus.
-
-Unitary System and VAV using HVACTemplate Inputs
-------------------------------------------------
-
-### Overview
-
-- Rectangular single story building with 5 occupied zones and a ceiling plenum
-
-- Packaged DX cooling with gas heat serving one zone
-
-- VAV with reheat and return plenum serving the other 4 zones
-
-- All equipment autosized using summer and winter design days
-
-
-
-![](media/image020.png)
-
-Figure 20. Schematic for Exercise 2.
-
-### Details of the Exercise
-
-#### Building Description
-
-- Single floor rectangular building 30.5 m (100 ft) by 15.2 m (50 ft) by 3m (10 ft) high.
-
-- Building is oriented with the long axis running east-west.
-
-- Floor Area 463.6 m2 (5000 ft2).
-
-- 5 occupied zones - 4 exterior, 1 interior, zone height 2.4 m (8 ft). Exterior zone depth is 3.7 m (12 ft).
-
-- 1 plenum zone 0.6 m (2 ft) high.
-
-- Windows on all 4 facades
-
-- South and north facades have glass doors.
-
-- South facing glass is shaded by overhangs.
-
-- Walls are wood shingle over plywood, insulation, and gypsum board.
-
-- Roof is gravel built up roof with mineral board insulation and plywood sheathing.
-
-- Floor slab is 0.1 m (4 in) heavy concrete.
-
-- Windows and glass doors are double pane Low-e clear glass with argon gap.
-
-- Window to wall ratio is approximately 0.3.
-
-- Lighting is 16 W/m2 (1.5 W/ft2).
-
-- Office electric equipment is 10.8 W/m2 (1.0 W/ft2).
-
-- 1 occupant per 9.3 m2 (100 ft2) of floor area.
-
-- Infiltration is 0.25 air changes per hour (always on, proportional to wind speed).
-
-- \* Refers to specific glass type included in the EnergyPlus datasets directory
-
--             (WindowGlassMaterials.idf)
-
-#### Space Conditioning
-
-- Heating setpoints:   21.1C (70F) occupied, 12.8C (55F) unoccupied
-
-- Cooling setpoints:   23.9C (75F) occupied, 40.0C (104F, system off) unoccupied
-
-- Plenum zone not controlled
-
-#### Environment
-
-- Location:                   Chicago, Illinois, USA
-
-- Design Days:             Summer, Winter
-
-- Annual Simulation Period:    Jan 1 – Dec 31
-
-- Ground Temperatures:         from Slab preprocessor (20.4 to 23.0 C)
-
-Instructions
-------------
-
-### Exercise 2A. Add Unitary System with DX Cooling and Gas Heating (Furnace) Serving a Single Zone
-
-Objective:  Learn how to describe a thermostat and unitary equipment using HVACTemplate objects.
-
-1)   Open Exercise2.idf and save it as Exercise2A.idf.  (Exercise2.idf contains the building envelope, internal loads, and some extra schedules to support the HVAC system descriptions which will be added in this Exercise.)
-
-2)   Add a **HVACTemplate:Thermostat** object to define the thermostat setpoints for this simulation.
-
-- Choose a name for the thermostat.  This name will be referenced in the next step.
-
-- For heating setpoints, use pre-defined schedule named "Office Heating Setpoints".
-
-- For cooling setpoints, use pre-defined schedule named "Office Cooling Setpoints".
-
-3)   Add a **HVACTemplate:Zone:Unitary** object serving the "NORTH PERIMETER" zone.  Choose a name for the air handling system which will be added in Step 4. Use the thermostat name from step 2 for the thermostat field. Retain the defaults for the remaining fields.
-
-4)   Add a **HVACTemplate:System:Unitary** object.  The name of this system object must be the same name used in the zone object for "Air Handling System Name" field (See Step 3).  Retain the defaults for all fields except the following:
-
-- Availability Schedule = Office HVAC (predefined)
-
-- Control Zone Name or Thermostat Location = NORTH PERIMETER
-
-- Supply Fan Operating Mode Schedule Name = Continuous
-
-- Heating Coil Type = Gas
-
-- Minimum Outdoor Air Schedule Name = Office Minimum OA (predefined)
-
-5)   Add a **Sizing:Parameters** object and set the sizing factor to 1.2 (for 20% oversizing).
-
-6)   Edit the **SimulationControl** object and set the Zone and System sizing flags to "Yes".
-
-7)   Run the simulation and review output files, especially:
-
-- err, there will be some warnings about meters that do no exist and the ABUPS report not being a full year.  These will go away as more features are added and an annual run is simulated.
-
-- DXF , drawing of building surfaces.  (Try selecting the Southwest Isometric named view, then see how each zone is a separate drawing layer.  In Voloview open the View -&gt; Layers dialog.  Click on the light bulbs to toggle display of each zone.  In TrueView click on the Layer Properties Manager toolbar button.  To toggle display of a layer, single-click a layer light bulb, then click apply.)
-
-- SVG, block diagram of the HVAC system components. (HINT: right-click in the drawing and read the Help to learn how to navigate in the SVG viewer.)
-
-- Main Results File (csv) and Meter File (Meter.csv).
-
-- eio, zone and system sizing results
-
-- Add output variables to report operation of the system (furnace) fan, heating coil, and cooling coil.  Reference the RDD output file for variable names.
-
-8)   Re-run the simulation and review results again.
-
-- Note during hour 7 of the summer design day that "NORTH PERIMETER:Zone/Sys Sensible Heating Rate[W](Hourly)" is nonzero, but the heating coil is off and the DX cooling coil shows a load.  Why?  This report variable reports the impact of the system on the zone (not the zone's demand for heating or cooling), averaged over the hour.  The system fan is scheduled on at 6 a.m., but the outside air dampers are closed.  The zone is not warm enough from the night to require cooling, so the circulating fan heat warms the zone slightly for a portion of the hour until the zone temperature exceeds the cooling setpoint and the DX coil comes on for the remainder of the hour.  If the economizer were active, this would not occur.
-
-### Exercise 2B. Add VAV System with Reheat Serving Four Zones with Chiller and Boiler Plant
-
-Objective:  Learn how to describe a VAV system with central plant using HVACTemplate objects.
-
-1)   Save Exercise2A.idf as Exercise2B.idf.
-
-2)   Add a **HVACTemplate:System:VAV** object.  Retain the defaults for all fields except the following:
-
-- Air Handling System Name = &lt;assign a name&gt;
-
-- System Availability Schedule = Office HVAC (predefined)
-
-- Cooling Coil Design Setpoint= 13C (55.4F)
-
-- Minimum Outdoor Air Schedule Name = Office Minimum OA (predefined)
-
-- Economizer Type = FixedDryBulb
-
-- Return Plenum Name = PLENUM
-
-3)   Add four **HVACTemplate:Zone:VAV** objects serving the four remaining zones (South Perimeter, East Perimeter, West Perimeter, and Core).  Retain the defaults for all fields except the following:
-
-- Specify the same air handler name added in Step 2 (use the dropdown list)
-
-- Specify the same thermostat control added in Exercise 2A Step 2 (again, use the dropdown list).
-
-- Supply Air Minimum Flow Fraction = 0.2
-
-- Reheat Coil Type = Hot Water
-
-- Heating Damper Action = Reverse
-
-- HINT:  Define one **HVACTemplate:Zone:VAV** object, make the above changes to defaults, then press "Dup Obj" three times to duplicate the object, then edit the remaining three zone names.
-
-4)   Add a **HVACTemplate:Plant:ChilledWaterLoop** object and assign a name.    Retain the defaults for all fields except the following:
-
-- Condenser Water Temperature Control Type = Specified Setpoint
-
-5)   Add a **HVACTemplate:Plant:Chiller** object, type Electric Reciprocating Chiller with a nominal COP of 3.6, water cooled.
-
-6)   Add a **HVACTemplate:Plant:Tower** object, type Two Speed.
-
-7)   Add a **HVACTemplate:Plant:HotWaterLoop** object and assign a name.  Retain the defaults for all fields.
-
-8)   Add a natural gas fired hot water boiler using **HVACTemplate:Plant:Boiler**.
-
-9)   Run the simulation, add desired report variables, and re-run the simulation.  Review results and compare with results from Exercise 2A:
-
-- Note how the heating and cooling rates for the NORTH PERIMETER zone are smaller than before.  Why?
-
-- Review the SVG drawing to see the components of the VAV system and water loops.
-
-- Browse the expidf file in a text editor (or open in IDF Editor from File, Open, setting file type to expidf) to see the full detailed description of the HVAC systems using native EnergyPlus objects (the expanded result of the HVACTemplate preprocessor).
-
-### Exercise 2C. Annual Simulation
-
-Objective:  Learn how to schedule report variables and create a monthly table report.
-
-1)   Save Exercise2B.idf as Exercise2C.idf.
-
-2)   Edit the **SimulationControl** object to turn off the design day simulations by setting “Run Simulation for Sizing Periods� to **No** and turn on the weather file (annual) simulation by setting “Run Simulation for Weather File Run Periods� to **Yes**..
-
-3)   Edit existing **Output:Variable** and **Output:Meter** objects and change the reporting frequency from Hourly to Monthly.
-
-4)   Locate the **Output:Variable** object for "Zone/Sys Air Temp" and duplicate it.  Edit the new object and add a schedule "Office Occupancy 2".  This object will report zone temperatures averaged only during occupied periods (when “Office Occupancy 2� is greater than zero).  The original instance of this report variable will average the zone temperatures over all hours.
-
-5)   Add a new **Output:Table:Monthly** object:
-
-- Name = Zone Temperature Report
-
-- Open the rdd output file for Exercise2B in the text editor and find the following report variable names to copy and paste into the fields of the Report:Table:Monthly object in IDF Editor.  Variable name and aggregation type are listed in pairs.
-
-- Zone Mean Air Temperature, SumOrAverage
-
-- Zone Mean Air Temperature, Maximum
-
-- Zone Mean Air Temperature, Minimum
-
-- Zone People Number of Occupants, HoursPositive
-
-- Zone Mean Air Temperature, SumOrAverageDuringHoursShown
-
-- Zone Mean Air Temperature, MaximumDuringHoursShown
-
-- Zone Mean Air Temperature, MinimumDuringHoursShown
-
-6)   Edit **Output:Table:SummaryReports** to add the “Equipment Summary� report.
-
-7)   Select Chicago TMY2 weather file and run the simulation.
-
-8)   Review outputs.  (Note the ABUPS report in the HTML file will now show a full year of results.)  Especially review the Zone Temperatures table report in the HTML file.  There will be a warning regarding **Output:Table:Monthly**, because there are no people in the PLENUM zone; this is normal.
-
-### Solution: Exercise 2
-
-This is a listing of new objects added in this Exercise.
-
-***Try not to look at this section until you have completed the Exercise.***
-
-#### Solution: Exercise 2A
-
-```idf
-HVACTemplate:Thermostat,
-    Office Thermostat,       !- Thermostat Name
-    Office Heating Setpoints,!- Thermostat Heating Setpoint Schedule
-    ,                        !- Thermostat Constant Heating Setpoint {C}
-    Office Cooling Setpoints,!- Thermostat Cooling Setpoint Schedule
-    ;                        !- Thermostat Constant Cooling Setpoint {C}
-
-
-HVACTemplate:Zone:Unitary,
-    NORTH PERIMETER,         !- Zone Name
-    North Zone Unitary,      !- Air Handling System Name
-    Office Thermostat,       !- Thermostat Name
-    autosize,                !- Zone Supply Air Max Flow Rate {m3/s}
-    ,                        !- Zone Supply Air Sizing Factor
-    Flow/Person,             !- Zone Outside Air Method
-    0.00944,                 !- Zone Outside Air Flow Rate per Person {m3/s}
-    0.0,                     !- Zone Outside Air Flow per Zone Area {m3/s-m2}
-    0.0,                     !- Zone Outside Air Flow per Zone {m3/s}
-    ,                        !- Zone Supply Plenum Name
-    ,                        !- Zone Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule
-    autosize;                !- Baseboard Heating Capacity {W}
-
-
-HVACTemplate:System:Unitary,
-    North Zone Unitary,      !- Air Handling System Name
-    Office HVAC,             !- System Availability Schedule
-    NORTH PERIMETER,         !- Control Zone Name or Thermostat Location
-    autosize,                !- Supply Fan Max Flow Rate {m3/s}
-    Continuous,              !- Supply Fan Operating Mode Schedule Name
-    0.7,                     !- Supply Fan Total Efficiency
-    600,                     !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    1,                       !- Supply Fan Motor in Air Stream Fraction
-    Single-speed DX,         !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule
-    autosize,                !- Cooling Coil Capacity {W}
-    autosize,                !- Cooling Coil Rated SHR
-    3,                       !- Cooling Coil Rated COP
-    Gas,                     !- Heating Coil Type
-    ,                        !- Heating Coil Availability Schedule
-    autosize,                !- Heating Coil Capacity {W}
-    0.8,                     !- Gas Heating Coil Efficiency
-    ,                        !- Gas Heating Coil Parasitic Electric Load {W}
-    autosize,                !- Maximum Outside Air Flow Rate {m3/s}
-    autosize,                !- Minimum Outside Air Flow Rate {m3/s}
-    Office Minimum OA,       !- Minimum Outside Air Schedule Name
-    NoEconomizer,            !- Economizer Type
-    NoLockout,               !- Economizer Lockout
-    ,                        !- Economizer Upper Temperature Limit {C}
-    ,                        !- Economizer Lower Temperature Limit {C}
-    ,                        !- Economizer Upper Enthalpy Limit {J/kg}
-    ,                        !- Supply Plenum Name
-    ,                        !- Return Plenum Name
-    BlowThrough,             !- Supply Fan Placement
-    StayOff,                 !- Night Cycle Control
-    ,                        !- Night Cycle Control Zone Name
-    None,                    !- Heat Recovery Type
-    0.7,                     !- Sensible Heat Recovery Effectiveness
-    0.65,                    !- Latent Heat Recovery Effectiveness
-    ,                        !- Dehumidification Control Type
-    ,                        !- Dehumidification Control Zone Name
-    ,                        !- Dehumidification Setpoint {percent}
-    ,                        !- Humidifier Type
-    ,                        !- Humidifier Availability Schedule
-    ,                        !- Humidifier Rated Capacity {m3/s}
-    ,                        !- Humidifier Rated Electric Power {W}
-    ,                        !- Humidifier Control Zone Name
-    ;                        !- Humidifier Setpoint {percent}
-
-
-Sizing:Parameters,
-    1.2;                     !- sizing factor
-
-
-Output:Variable,*,Furnace Fan Part-Load Ratio,hourly;
-Output:Variable,*,DX Cooling Coil Runtime Fraction,hourly;
-Output:Variable,*,Heating Coil Runtime Fraction,hourly;
-```
-
-#### Solution: Exercise 2B
-
-```idf
-HVACTemplate:System:VAV,
-   VAV with Reheat,         !- Air Handling System Name
-    Office HVAC,             !- System Availability Schedule
-    autosize,                !- Supply Fan Max Flow Rate {m3/s}
-    autosize,                !- Supply Fan Min Flow Rate {m3/s}
-    0.7,                     !- Supply Fan Total Efficiency
-    1000,                    !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    1,                       !- Supply Fan Motor in Air Stream Fraction
-    ChilledWater,            !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule
-    ,                        !- Cooling Coil Setpoint Schedule
-    13,                      !- Cooling Coil Design Setpoint {C}
-    None,                    !- Heating Coil Type
-    ,                        !- Heating Coil Availability Schedule
-    ,                        !- Heating Coil Setpoint Schedule
-    10.0,                    !- Heating Coil Design Setpoint {C}
-    0.8,                     !- Gas Heating Coil Efficiency
-    ,                        !- Gas Heating Coil Parasitic Electric Load {W}
-    None,                    !- Preheat Coil Type
-    ,                        !- Preheat Coil Availability Schedule
-    ,                        !- Preheat Coil Setpoint Schedule
-    7.2,                     !- Preheat Coil Design Setpoint {C}
-    0.8,                     !- Gas Preheat Coil Efficiency
-    ,                        !- Gas Preheat Coil Parasitic Electric Load {W}
-    autosize,                !- Maximum Outside Air Flow Rate {m3/s}
-    autosize,                !- Minimum Outside Air Flow Rate {m3/s}
-    ProportionalMinimum,     !- Minimum Outside Air Control Type
-    Office Minimum OA,       !- Minimum Outside Air Schedule Name
-    FixedDryBulb,            !- Economizer Type
-    NoLockout,               !- Economizer Lockout
-    ,                        !- Economizer Upper Temperature Limit {C}
-    ,                        !- Economizer Lower Temperature Limit {C}
-    ,                        !- Economizer Upper Enthalpy Limit {J/kg}
-    ,                        !- Supply Plenum Name
-    PLENUM,                  !- Return Plenum Name
-    DrawThrough,             !- Supply Fan Placement
-    InletVaneDampers,        !- Supply Fan Part-Load Power Coefficients
-    StayOff,                 !- Night Cycle Control
-    ,                        !- Night Cycle Control Zone Name
-    None,                    !- Heat Recovery Type
-    0.7,                     !- Sensible Heat Recovery Effectiveness
-    0.65,                    !- Latent Heat Recovery Effectiveness
-    None,                    !- Cooling Coil Setpoint Reset Type
-    None,                    !- Heating Coil Setpoint Reset Type
-    ,                        !- Dehumidification Control Type
-    ,                        !- Dehumidification Control Zone Name
-    ,                        !- Dehumidification Setpoint {percent}
-    ,                        !- Humidifier Type
-    ,                        !- Humidifier Availability Schedule
-    ,                        !- Humidifier Rated Capacity {m3/s}
-    ,                        !- Humidifier Rated Electric Power {W}
-    ,                        !- Humidifier Control Zone Name
-    ;                        !- Humidifier Setpoint {percent}
-
-
-HVACTemplate:Zone:VAV,
-    SOUTH PERIMETER,         !- Zone Name
-    VAV with Reheat,         !- Air Handling System Name
-    Office Thermostat,       !- Thermostat Name
-    autosize,                !- Zone Supply Air Max Flow Rate {m3/s}
-    ,                        !- Zone Supply Air Sizing Factor
-    0.2,                     !- Zone Supply Air Min Flow Fraction
-    Flow/Person,             !- Zone Outside Air Method
-    0.00944,                 !- Zone Outside Air Flow Rate per Person {m3/s}
-    0.0,                     !- Zone Outside Air Flow per Zone Area {m3/s-m2}
-    0.0,                     !- Zone Outside Air Flow per Zone {m3/s}
-    HotWater,                !- Reheat Coil Type
-    ,                        !- Reheat Coil Availability Schedule
-    Reverse,                 !- Zone Damper Heating Action
-    ,                        !- Zone Supply Plenum Name
-    ,                        !- Zone Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule
-    autosize;                !- Baseboard Heating Capacity {W}
-
-
-HVACTemplate:Zone:VAV,
-    EAST PERIMETER,          !- Zone Name
-    VAV with Reheat,         !- Air Handling System Name
-    Office Thermostat,       !- Thermostat Name
-    autosize,                !- Zone Supply Air Max Flow Rate {m3/s}
-    ,                        !- Zone Supply Air Sizing Factor
-    0.2,                     !- Zone Supply Air Min Flow Fraction
-    Flow/Person,             !- Zone Outside Air Method
-    0.00944,                 !- Zone Outside Air Flow Rate per Person {m3/s}
-    0.0,                     !- Zone Outside Air Flow per Zone Area {m3/s-m2}
-    0.0,                     !- Zone Outside Air Flow per Zone {m3/s}
-    HotWater,                !- Reheat Coil Type
-    ,                        !- Reheat Coil Availability Schedule
-    Reverse,                 !- Zone Damper Heating Action
-    ,                        !- Zone Supply Plenum Name
-    ,                        !- Zone Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule
-    autosize;                !- Baseboard Heating Capacity {W}
-
-
-HVACTemplate:Zone:VAV,
-    WEST PERIMETER,          !- Zone Name
-    VAV with Reheat,         !- Air Handling System Name
-    Office Thermostat,       !- Thermostat Name
-    autosize,                !- Zone Supply Air Max Flow Rate {m3/s}
-    ,                        !- Zone Supply Air Sizing Factor
-    0.2,                     !- Zone Supply Air Min Flow Fraction
-    Flow/Person,             !- Zone Outside Air Method
-    0.00944,                 !- Zone Outside Air Flow Rate per Person {m3/s}
-    0.0,                     !- Zone Outside Air Flow per Zone Area {m3/s-m2}
-    0.0,                     !- Zone Outside Air Flow per Zone {m3/s}
-    HotWater,                !- Reheat Coil Type
-    ,                        !- Reheat Coil Availability Schedule
-    Reverse,                 !- Zone Damper Heating Action
-    ,                        !- Zone Supply Plenum Name
-    ,                        !- Zone Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule
-    autosize;                !- Baseboard Heating Capacity {W}
-
-
-HVACTemplate:Zone:VAV,
-    CORE,                    !- Zone Name
-    VAV with Reheat,         !- Air Handling System Name
-    Office Thermostat,       !- Thermostat Name
-    autosize,                !- Zone Supply Air Max Flow Rate {m3/s}
-    ,                        !- Zone Supply Air Sizing Factor
-    0.2,                     !- Zone Supply Air Min Flow Fraction
-    Flow/Person,             !- Zone Outside Air Method
-    0.00944,                 !- Zone Outside Air Flow Rate per Person {m3/s}
-    0.0,                     !- Zone Outside Air Flow per Zone Area {m3/s-m2}
-    0.0,                     !- Zone Outside Air Flow per Zone {m3/s}
-    HotWater,                !- Reheat Coil Type
-    ,                        !- Reheat Coil Availability Schedule
-    Reverse,                 !- Zone Damper Heating Action
-    ,                        !- Zone Supply Plenum Name
-    ,                        !- Zone Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule
-    autosize;                !- Baseboard Heating Capacity {W}
-
-
-HVACTemplate:Plant:ChilledWaterLoop,
-  Chilled Water Plant,     !- Plant Loop Name
-  ,                        !- Pump Schedule
-  Intermittent,            !- Pump Control Type
-  Default,                 !- Chiller Plant Operation Scheme Type
-  ,                        !- Chiller Plant Operation Scheme Name
-  ,                        !- Chilled Water Setpoint Schedule
-  7.22,                    !- Chilled Water Design Setpoint {C}
-  ConstantPrimaryNoSecondary,  !- Chilled Water Pump Configuration
-  179352,                  !- Primary Chilled Water Pump Rated Head {Pa}
-  179352,                  !- Secondary Chilled Water Pump Rated Head {Pa}
-  Default,                 !- Condenser Plant Operation Scheme Type
-  ,                        !- Condenser Plant Operation Scheme List Name
-  SpecifiedSetpoint,       !- Condenser Water Temperature Control Type
-  ,                        !- Condenser Water Setpoint Schedule
-  29.4,                    !- Condenser Water Design Setpoint {C}
-  179352,                  !- Condenser Water Pump Rated Head {Pa}
-  None,                    !- Chilled Water Setpoint Reset Type
-  12.2,                    !- Chilled Water Setpoint at Outdoor Dry Bulb Low {C}
-  15.6,                    !- Chilled Water Reset Outdoor Dry Bulb Low {C}
-  6.7,                     !- Chilled Water Setpoint at Outdoor Dry Bulb High {C}
-  26.7;                    !- Chilled Water Reset Outdoor Dry Bulb High {C}
-
-
-HVACTemplate:Plant:Chiller,
-    Chiller 1,               !- Chiller Name
-    ElectricReciprocatingChiller,  !- Chiller Type
-    autosize,                !- Capacity {W}
-    3.6,                     !- COP {W/W}
-    WaterCooled,             !- Condenser Type
-    ;                        !- Priority
-
-
-HVACTemplate:Plant:Tower,
-    Tower 1,                 !- Tower Name
-    TwoSpeed,                !- Tower Type
-    autosize,                !- High-Speed Nominal Capacity {W}
-    autosize,                !- High-Speed Fan Power {W}
-    autosize,                !- Low-Speed Nominal Capacity {W}
-    autosize,                !- Low-Speed Fan Power {W}
-    autosize,                !- Free Convection Capacity {W}
-    ;                        !- Priority
-
-
-HVACTemplate:Plant:HotWaterLoop,
-  Hot Water Plant,         !- Plant Loop Name
-  ,                        !- Pump Schedule
-  Intermittent,            !- Pump Control Type
-  Default,                 !- Hot Water Plant Operation Scheme Type
-  ,                        !- Hot Water Plant Operation Scheme List Name
-  ,                        !- Hot Water Setpoint Schedule
-  82,                      !- Hot Water Design Setpoint {C}
-  ConstantFlow,            !- Hot Water Pump Configuration
-  179352,                  !- Hot Water Pump Rated Head {Pa}
-  None,                    !- Hot Water Setpoint Reset Type
-  82.2,                    !- Hot Water Setpoint at Outdoor Dry Bulb Low {C}
-  -6.7,                    !- Hot Water Reset Outdoor Dry Bulb Low {C}
-  65.6,                    !- Hot Water Setpoint at Outdoor Dry Bulb High {C}
-  10;                      !- Hot Water Reset Outdoor Dry Bulb High {C}
-
-
-HVACTemplate:Plant:Boiler,
-  Boiler 1,                !- Boiler Name
-  HotWaterBoiler,          !- Boiler Type
-  autosize,                !- Capacity {W}
-  0.8,                     !- Efficiency
-  NaturalGas,              !- Fuel Type
-  ;                        !- Priority
-
-
-Output:Variable,*,Damper Position,hourly;
-Output:Variable,*,Chiller Evap Heat Trans Rate,hourly;
-Output:Variable,*,Chiller COP,hourly;
-Output:Variable,*,Boiler Heating Output Rate,hourly;
-Output:Variable,*,Tower Heat Transfer,hourly;
-```
-
-
-#### Exercise 2C
-
-```idf
-Output:Variable,*,Zone/Sys Air Temperature,monthly,Office Occupancy 2;
-
-
-Output:Table:Monthly,
-    Zone Temperature Report, !- Name
-    2,                       !- DigitsAfterDecimal
-    Zone Mean Air Temperature,  !- VariableOrMeterName01
-    SumOrAverage,            !- AggregationType01
-    Zone Mean Air Temperature,  !- VariableOrMeterName02
-    Maximum,                 !- AggregationType02
-    Zone Mean Air Temperature,  !- VariableOrMeterName03
-    Minimum,                 !- AggregationType03
-    Zone People Number of Occupants,  !- VariableOrMeterName04
-    HoursPositive,           !- AggregationType04
-    Zone Mean Air Temperature,  !- VariableOrMeterName05
-    SumOrAverageDuringHoursShown,  !- AggregationType05
-    Zone Mean Air Temperature,  !- VariableOrMeterName06
-    MaximumDuringHoursShown, !- AggregationType06
-    Zone Mean Air Temperature,  !- VariableOrMeterName07
-    MinimumDuringHoursShown; !- AggregationType07
-```
-
-
-
-IDF Editor – Brief Introduction
-===============================
-
-EnergyPlus has several options for the user to create input files. For the purposes of this document, we will describe briefly the workings of the IDF Editor that is supplied with the EnergyPlus Installation.  The IDF Editor is a simple, “intelligent� editor that reads the EnergyPlus Data Dictionary (IDD) and allows creation/revision of EnergyPlus Input Files (IDF). It can be run from a shortcut in the main EnergyPlus directory (created as part of the install) or directly from EP-Launch.
-
-Full details of the IDF Editor can be found in the Auxiliary Programs document.  IDD Conventions (to be able to read the IDD) are found in the Input Output Reference document. EnergyPlus standard units are described in several places, including later in this document.
-
-IDF Editor is an optional component of the EnergyPlus installation. For users who want a simple way of creating or editing EnergyPlus input data files (IDF), IDF Editor provides this service.  The IDF Editor does not check inputs for validity, although some numeric fields are highlighted if out of range and some text fields are highlighted if they contain an invalid reference. For instructions and rules that must be followed when creating an IDF file the user should refer to the [*Input/Output Reference*](../../EnergyPlusFromStarTeam/EnergyPlusFromStarTeam/Documentation/sources/InputOutputReference.pdf) document.
-
-![](media/image021.jpg)
-
-Figure 21. IDF Editor Screen.
-
-### Start IDF Editor
-
-IDF Editor should be located in the EnergyPlus\\PreProcessor\\IDFEditor directory where you installed EnergyPlus. By double clicking on the IDF Editor icon you will get a screen similar to the one shown above. IDF Editor works in conjunction with the current EnergyPlus Input Data Directory (IDD) file that resides in the directory where EnergyPlus is installed. Another way to start the IDF Editor is from EP-Launch. Multiple IDF files can be opened at once.
-
-### Creating or Selecting an Input Data File
-
-Creating a new input data file or selecting an existing input data file can be accomplished either through use of the File menu on the menu bar at the top of the screen or through use of the New File icon button or Open File icon button on the tool bar.
-
-### Class List
-
-The class list shows how the items for the IDF are grouped.  This class list follows the Data Dictionary (IDD) description. Select a class from the list by clicking on and highlighting the class. The field to the left of the selected class in the ‘Class List’ will either contain [------] to indicate that this class has no objects in the IDF file or it will contain a number like [0003] to indicate the number of times the object currently appears in the IDF file. For example, for the BuildingSurface:Detailed class selected in the screen above under the Thermal Zone Description/Geometry group, there are 40 objects in the IDF file. The details for these 40 objects or any new object that is defined are displayed in columns within the grid. Each object is made up of fields and can be used to further define the object. Any units attached to each field are shown in the second column. You may need to scroll down the ‘field’ list or maximize the application to see all of the fields. Likewise, you may need to scroll to the right of the main grid to see other objects.
-
-Options under the view menu can change how you use the Class List. To display only classes that contain objects select the “show classes with objects only� option on the “View� menu. You can also toggle this feature on and off with CTRL+L. If the file is empty and has no objects, this toggle does not impact the display.
-
-The “Show Quick Select Dropdowns� view menu option adds two new input fields to the main screen. The input fields can be used to go quickly to different classes in the main list of classes. By typing in the top input field, the group that start with those letters are displayed. After selecting one and pressing the tab button, classes in that group are shown and by typing the first few letters, you can easily select a specific class. Pressing tab again displays that class and it objects. This method allow for quick selection of classes if you remember the group name and class name.
-
-### Changing Values
-
-By clicking and highlighting a value within an object, several things happen:
-
-1)   Any user comments from the IDF file will be displayed in the ‘Comments from IDF’ portion of the screen
-
-2)   Any notes contained in the IDD for this input field will be displayed in the ‘Explanation of Keyword’ portion of the screen
-
-3)   The value can be edited. Depending on the field, a drop down list may display the default value, maximum and minimum, or other keywords that can be used with the field.
-
-4)   Numeric fields that can be autosized will include "autosize" as a selection in the drop down list.
-
-5)   Some numeric fields have a maximum and/or minimum value specified in the IDD. If the value entered is outside this range, the cell will be highlighted in pale orange.
-
-6)   For values that are names of nodes, a new dialog box titled “Edit or Select Node Name� can be shown when the small button is pressed that is on the right side in each node name cell.
-
-### Working with Objects
-
-To delete an object, first click on any value for the object and then click on the “Del Obj� button. To add a new object, click on the “New Obj� button and a new object column with fields set to blanks, zeros, or default values will be added to the far right of the grid. The “Dup Obj� button is similar to “New Obj�, but copies the values of the fields of the currently selected object. Copying and pasting an object or groups of objects is also possible using the “Copy Obj� and “Paste Obj� buttons.  These allow objects to be copied between files are also good for copying from files in the DataSets subdirectory. (Also see the Edit menu to perform these functions.)
-
-### File Menu
-
-The File menu can be used for creating or selecting input files just like the buttons on the IDF Editor screen (see the *Creating or Selecting an Input File* section above). In addition, the File menu is used to save a file or exit the IDF Editor. More than one file can be opened at a time.
-
-The “File�, “Save Options� screen is shown below.
-
-
-
- ![](media/image022.png)
-
-Figure 22. IDF Editor Save Options Screen.
-
-The save options allow the order of the objects in the file to be sorted by type of object or to keep the original order of the objects (for an existing file). The placement of new objects when the original order is specified can be either at the top or bottom of the file.
-
-In addition, the Save Options also allow certain objects to be written to the file using a specific format that some users prefer. Selecting this option will format the following objects on a single line: Report, Report Meter, Report Variable, Version, Timestep in Hour, Inside Convection Algorithm, Outside Convection Algorithm, Solution Algorithm, Shadowing Calculations, Ground Reflectances, and GroundTemperatures:Deep. In addition, Schedule:Compact objects will be formatted to have two field for some lines. With this option, objects with geometric vertices are formatted to have the X, Y, and Z values on the same line. Those objects include: Surface:HeatTransfer, Surface:HeatTransfer:Sub, Surface:Shading:Detached:Fixed, Surface:Shading:Detached:Building and Surface:Shading:Attached.
-
-The settings for the save options are kept for each file saved from the IDF Editor.
-
-Also on the File menu is the Open DataSet menu and submenu. This allows you to open any input file that appears in the DataSet subdirectory and copy objects from them into another file. This is required because EnergyPlus does not read the DataSet files, it is up to you to include objects from them.
-
-### Edit Menu
-
-The Edit Menu offers options to create a new object, duplicate an object, and delete an object as well as finding and searching. The object options are the same operations as can be accomplished by using the ‘New Obj’, ‘Dup Obj’ and ‘Del Obj’ buttons (see the *Working with Objects* section above). In addition, the "Next Row after Enter" option can be toggled. When this option is on, the selection moves down one row after pressing Enter. The copy and paste object commands allow a single object to be copied within a file or between files. The pasted object appears as the last object in the class. This capability makes it easier to utilize the data in the DataSets directory. The Find Class and Search and Replace options can be used to search through the list of classes or the values of a file quickly. If renaming objects, the recommended approach is to rename the object and select the cell again and open the Search and Replace dialog. This will show other places in the file that use that object name that also may need to be changed.
-
-### View Menu
-
-The View menu offers options for units and column widths. The Narrow/Medium/Wide Column options set the standard column width for items in the object grid. Individual columns can also be resized by dragging the column separator. The displayed value is rounded and/or expressed in scientific notation to fit within the column width.
-
-EnergyPlus input files must always be in SI units. Selecting "Inch-Pound" (IP) units in the View menu displays and edits values in IP units.
-
-1)   The IP unit will be displayed in the units column of the object grid. Some SI units convert to multiple IP units. For example, W becomes Btu/hr for heating and cooling capacity but remains as W for lighting and electrical equipment.
-
-2)   All conversion factors used in the IDF editor are documented in a block of comments near the top of the Energy+.IDD file.
-
-3)   Schedules, fluid properties and curves now support IP unit conversions. For curves, the minimum and maximum values are converted but the coefficients are not.
-
-To display only classes that contain objects select the “show classes with objects only� option on the “View� menu. You can also toggle this feature on and off with CTRL+L. If the file is empty and has no objects, this toggle does not impact the display.
-
-The “Show Quick Select Dropdowns� view menu option adds two new input fields to the main screen. The input fields can be used to go quickly to different classes in the main list of classes.
-
-The “Validity Check� function has replaced and expanded upon the old  “Check Out-of-Range� function. It can also be started by using CTRL-R. The “Validity Check� function performs three kinds of validity checks. It displays the values and locations for objects with values that are either above the maximum or below the minimum values.  It also displays fields that contain invalid references. The “Validity Check� dialog also shows when an entry for a field is not one of the possible lists of choices. The Perform Validity Check When Saving File can be turned on and off and automatically performs the check whenever the file is saved.
-
-### Help Menu
-
-The Help menu offers options to open the EnergyPlus documentation files.
-
-
-
-Other Useful programs/information
-=================================
-
-HVACTemplate Objects
---------------------
-
-HVAC Template objects are available. These are intended to allow for several “usual� HVAC types to be expanded into EnergyPlus HVAC inputs with minimal user entries. These are described in the “Input/Output Reference� document under the Group “HVACTemplates� and the expansion process is described in the Auxiliary Programs document under “ExpandObjects�.
-
-Data Sets
----------
-
-EnergyPlus uses snippets of IDF files to create the library of data that may be useful for you. Two folders are created upon installation: DataSets – which contains IDF snippets and MacroDataSets – which also contain IDF snippets but are in a form such that they can be easily used with the EPMacro program.
-
-Slab and Basement Programs
---------------------------
-
-The Slab and Basement programs can be used to create accurate Ground Temperature profiles for your runs using minimal input about your building. These are used prior to an actual simulation. The programs are described in the Auxiliary Programs document.
-
-Coefficient Curve Generation
-----------------------------
-
-The CoeffConv and CoeffConv utility programs can be used to convert DOE-2 temperature dependent curves (Fahrenheit) to EnergyPlus temperature curves (Centigrade/Celsius). These programs are described in the Auxiliary Programs document.
-
-Useful Programs
----------------
-
-Several useful programs, not described fully here can be found in the Auxiliary Programs document.
-
-WeatherData
------------
-
-The E/E+ format is very flexible (as well as being ASCII and somewhat readable). In addition to the usual weather data (temperatures, solar radiation data), the format embodies other information from the location and weather data (e.g. design conditions, calculated ground temperatures, typical and extreme weather periods). The EPW (weather data format)  is described in [Auxiliary Programs](file:///E:\Docs4PDFs\AuxiliaryPrograms.pdf) Document. Other details including statistical reports, backgrounds on data sources and formats, use of the Weather Converter program (used both for processing data and reporting) are also provided in the Auxiliary Programs document.
-
-The web site for EnergyPlus (http://www.energyplus.gov) provides downloadable weather data for many sites throughout the world from several different formats. In addition, we are amenable to posting more weather data from users.
-
-Results Processing
-------------------
-
-Results from EnergyPlus (using EP-Launch) appear in several possible formats.  The most basic are the csv files for the time oriented output and the meter output.  These will appear as &lt;filename&gt;.csv and &lt;filename&gt;Meter.csv.  These can be quite detailed files (ref: Output:Variable, Output:Meter commands).  Other formats (such as Tabular outputs) can yield more summarized results.  These files and contents are described in more detail in the “[Output Details and Examples](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf)� document.
-
-As an example, here is what the normal “csv� file might look like in Excel™:
-
-![](media/image023.png)
-
-Figure 23. Results in Spreadsheet format
-
-Likewise, a tabular output (usually in HTML format – which can be read by any web browser) might look like:
-
-**End Uses**
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Electricity (GJ)</th>
-<th>Natural Gas (GJ)</th>
-<th>Other Fuel (GJ)</th>
-<th>Purchaseh Cooling (GJ)</th>
-<th>Purchaseh Heating (GJ)</th>
-<th>Water (m3)</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>0.00</td>
-<td>95.17</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>56.78</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>124.39</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>28.27</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>73.52</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>0.08</td>
-<td>85.39</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>363.07</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Total End Uses</td>
-<td>283.03</td>
-<td>180.56</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>363.07</td>
-</tr>
-</table>
-
-
-
-HVAC-Diagram
-------------
-
-Another post processing program (EnergyPlus versions 1.2 and later) is the HVAC-Diagram application. It reads one of the EnergyPlus output files (eplusout.bnd and produces a Scalable Vector Graphics (SVG) file. More information on the HVAC Diagram program is found in the [Auxiliary Programs](file:///E:\Docs4PDFs\AuxiliaryPrograms.pdf) document.
-
-CSVProc
--------
-
-This simple post processing program uses .csv files (such as created by ReadVarsESO) and performs some simple statistics on the contents. This program is described more fully in the Auxiliary Programs document.
-
-convertESOMTR
--------------
-
-This simple post processing program can be used seamlessly with EP-Launch to provide IP (inch-pound) unit output files rather than SI units. This program is described more fully in the Auxiliary Programs document.
-
-
-
-DataFiles
----------
-
-Some example files are installed during installation (Sample Files option). Each sample input file should contain comments about its purpose at the start of the file. Other example files are made available from the website (http://www.energyplus.gov/).
-
-Library Files
--------------
-
-Library files for EnergyPlus are embodied in the DataSets and MacroDataSets folders. DataSets are IDF excerpts – you must cut and paste from them in order to use them. Items in MacroDataSets can be used in conjunction with the EPMacro preprocessor program. All files are in the necessary form for processing with EnergyPlus.
-
-The files in the DataSets and MacroDataSets folders are described in more detail in the “[Output Details and Examples](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf)� document.
-
-
-
-
-
-
-
-Energy Meters
-=============
-
-Standard Energy Meters
-----------------------
-
-Meters provide one way for EnergyPlus to report energy use in a form that is pallatable to the users. The primary implemented method for output gives very fine detail (down to the variable level) for results from EnergyPlus. However, to get the required energy use, there may be several variables that need to be polled and accumulated. The meter implementation for EnergyPlus accomplishes this reporting.
-
-![EnergyMeters](media/image024.jpg)
-
-Figure 24. Illustration of Energy Metering
-
-Meters can be used to typify energy use by type and by component. The diagrams and tables illustrate how the meters have been incorporated into EnergyPlus.
-
-As shown in the figure above, energy use for the facility is grouped according to fuel type (see Table 8. Table of Metered Fuel Types), by meter type (see Table 7. Overall Meter Types) and by end use category type (see Table 9. End Use Category Types).
-
-Table 7. Overall Meter Types
-
-<table class="table table-striped">
-<tr>
-<th>Meters</th>
-</tr>
-<tr>
-<td>Facility</td>
-</tr>
-<tr>
-<td>Building</td>
-</tr>
-<tr>
-<td>Zone</td>
-</tr>
-<tr>
-<td>System</td>
-</tr>
-<tr>
-<td>Plant</td>
-</tr>
-</table>
-
-Both the fuel types and enduse types are set within the program by the developers. Current Fuel types are shown in the table below. There is also a special category called “EnergyTranser�.
-
-
-
-Table 8. Table of Metered Fuel Types
-
-<table class="table table-striped">
-  <tr>
-    <th>Utility/Fuel Types</th>
-  </tr>
-  <tr>
-    <td>Electricity</td>
-  </tr>
-  <tr>
-    <td>Gas</td>
-  </tr>
-  <tr>
-    <td>Gasoline</td>
-  </tr>
-  <tr>
-    <td>Diesel</td>
-  </tr>
-  <tr>
-    <td>Coal</td>
-  </tr>
-  <tr>
-    <td>FuelOil\#1</td>
-  </tr>
-  <tr>
-    <td>FuelOil\#2</td>
-  </tr>
-  <tr>
-    <td>Propane</td>
-  </tr>
-  <tr>
-    <td>Water</td>
-  </tr>
-  <tr>
-    <td>Steam</td>
-  </tr>
-  <tr>
-    <td>DistrictCooling</td>
-  </tr>
-  <tr>
-    <td>DistrictHeating</td>
-  </tr>
-</table>
-
-<table class="table table-striped">
-<tr>
-<th>Other Resource Types</th>
-</tr>
-<tr>
-<td>EnergyTransfer</td>
-</tr>
-</table>
-
-
-
-The end use types are shown in the following table:
-
-Table 9. End Use Category Types
-
-<table class="table table-striped">
-  <tr>
-    <th>End Use Types</th>
-  </tr>
-  <tr>
-    <td>InteriorLights</td>
-  </tr>
-  <tr>
-    <td>ExteriorLights</td>
-  </tr>
-  <tr>
-    <td>InteriorEquipment</td>
-  </tr>
-  <tr>
-    <td>ExteriorEquipment</td>
-  </tr>
-  <tr>
-    <td>Fans</td>
-  </tr>
-  <tr>
-    <td>Pumps</td>
-  </tr>
-  <tr>
-    <td>Heating</td>
-  </tr>
-  <tr>
-    <td>Cooling</td>
-  </tr>
-  <tr>
-    <td>HeatRejection</td>
-  </tr>
-  <tr>
-    <td>Humidifier</td>
-  </tr>
-  <tr>
-    <td>HeatRecovery</td>
-  </tr>
-  <tr>
-    <td>DHW</td>
-  </tr>
-  <tr>
-    <td>Cogeneration</td>
-  </tr>
-  <tr>
-    <td>Refrigeration</td>
-  </tr>
-  <tr>
-    <td>Miscellaneous</td>
-  </tr>
-</table>
-
-
-
-Additional End Use Types Only Used for EnergyTransfer:
-
-<table class="table table-striped">
-  <tr>
-    <th>AdditionalTypes</th>
-  </tr>
-  <tr>
-    <td>HeatingCoils</td>
-  </tr>
-  <tr>
-    <td>CoolingCoils</td>
-  </tr>
-  <tr>
-    <td>Chillers</td>
-  </tr>
-  <tr>
-    <td>Boilers</td>
-  </tr>
-  <tr>
-    <td>Baseboard</td>
-  </tr>
-  <tr>
-    <td>HeatRecoveryForCooling</td>
-  </tr>
-  <tr>
-    <td>HeatRecoveryForHeating</td>
-  </tr>
-</table>
-
-Custom Meters
--------------
-
-You can also define your own “custom meters� from variable names that are summed during the simulation.  You assign the proper fuel type during the definition (review Input Output Reference, objects: **Meter:Custom** and **Meter:CustomDecrement**) for further requirements.
-
-Standard EnergyPlus Units
-=========================
-
-EnergyPlus has adopted the standard SI units for input and output.
-
-ASCII with no spaces is used for abbreviations. Note that exponents appear without any indication of exponentiation: i.e., kg/m3 not kg/m^3 or kg/m\*\*3. Also note the use of dashes. We have W/m2-K not W/m2\*K or W/(m2\*K).
-
-At the end we note the “problem� variables – the inputs that have non-standard units. Inputs using these units will have to be changed and the code checked to see how the quantities are used internally.
-
-Table 10. Standard EnergyPlus Units
-
-<table class="table table-striped">
-<tr>
-<th>Quantity</th>
-<th>unit</th>
-<th>abbreviation</th>
-</tr>
-<tr>
-<td>angular degrees</td>
-<td>degree</td>
-<td>deg</td>
-</tr>
-<tr>
-<td>Length</td>
-<td>meter</td>
-<td>m</td>
-</tr>
-<tr>
-<td>Area</td>
-<td>square meter</td>
-<td>m2</td>
-</tr>
-<tr>
-<td>Volume</td>
-<td>cubic meter</td>
-<td>m3</td>
-</tr>
-<tr>
-<td>Time</td>
-<td>seconds</td>
-<td>s</td>
-</tr>
-<tr>
-<td>frequency</td>
-<td>Hertz</td>
-<td>Hz</td>
-</tr>
-<tr>
-<td>temperature</td>
-<td>Celsius</td>
-<td>C</td>
-</tr>
-<tr>
-<td>absolute temperature</td>
-<td>Kelvin</td>
-<td>K</td>
-</tr>
-<tr>
-<td>temperature difference</td>
-<td>Celsius</td>
-<td>deltaC</td>
-</tr>
-<tr>
-<td>Speed</td>
-<td>meters per second</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>energy (or work)</td>
-<td>Joules</td>
-<td>J</td>
-</tr>
-<tr>
-<td>Power</td>
-<td>Watts</td>
-<td>W</td>
-</tr>
-<tr>
-<td>Mass</td>
-<td>kilograms</td>
-<td>kg</td>
-</tr>
-<tr>
-<td>Force</td>
-<td>Newton</td>
-<td>N</td>
-</tr>
-<tr>
-<td>mass flow</td>
-<td>kilograms per second</td>
-<td>kg/s</td>
-</tr>
-<tr>
-<td>volume flow</td>
-<td>cubic meters per second</td>
-<td>m3/s</td>
-</tr>
-<tr>
-<td>Pressure</td>
-<td>Pascals</td>
-<td>Pa</td>
-</tr>
-<tr>
-<td>pressure difference</td>
-<td>Pascals</td>
-<td>Pa</td>
-</tr>
-<tr>
-<td>specific enthalpy</td>
-<td>Joules per kilogram</td>
-<td>J/kg</td>
-</tr>
-<tr>
-<td>Density</td>
-<td>kilograms per cubic meter</td>
-<td>kg/m3</td>
-</tr>
-<tr>
-<td>heat flux</td>
-<td>watts per square meter</td>
-<td>W/m2</td>
-</tr>
-<tr>
-<td>specific heat</td>
-<td>-------</td>
-<td>J/kg-K</td>
-</tr>
-<tr>
-<td>conductivity</td>
-<td>-------</td>
-<td>W/m-K</td>
-</tr>
-<tr>
-<td>Diffusivity</td>
-<td>-------</td>
-<td>m2/s</td>
-</tr>
-<tr>
-<td>heat transfer coefficient</td>
-<td>-------</td>
-<td>W/m2-K</td>
-</tr>
-<tr>
-<td>R-value</td>
-<td>-------</td>
-<td>m2-K/W</td>
-</tr>
-<tr>
-<td>heating or cooling capacity</td>
-<td>Watts</td>
-<td>W</td>
-</tr>
-<tr>
-<td>electric potential</td>
-<td>volts</td>
-<td>V</td>
-</tr>
-<tr>
-<td>electric current</td>
-<td>Amperes</td>
-<td>A</td>
-</tr>
-<tr>
-<td>illuminace</td>
-<td>lux</td>
-<td>lx</td>
-</tr>
-<tr>
-<td>luminous flux</td>
-<td>lumen</td>
-<td>lm</td>
-</tr>
-<tr>
-<td>luminous intensity</td>
-<td>candelas</td>
-<td>cd</td>
-</tr>
-<tr>
-<td>luminance</td>
-<td>candelas per square meter</td>
-<td>cd/m2</td>
-</tr>
-<tr>
-<td>vapor diffusivity</td>
-<td>m2/s</td>
-<td> </td>
-</tr>
-<tr>
-<td>Viscosity</td>
-<td>-------</td>
-<td>kg/m-s</td>
-</tr>
-<tr>
-<td>Dynamic Viscosity</td>
-<td>-------</td>
-<td>N-s/m2</td>
-</tr>
-<tr>
-<td>Porosity</td>
-<td>-------</td>
-<td>m3/m3</td>
-</tr>
-<tr>
-<td>thermal gradient coeff for moisture capacity</td>
-<td>-------</td>
-<td>kg/kg-K</td>
-</tr>
-<tr>
-<td>isothermal moisture capacity</td>
-<td>-------</td>
-<td>m3/kg</td>
-</tr>
-</table>
-
diff --git a/doc/src/docs/InputOutputReference/01a-InputOutputReference.md b/doc/src/docs/InputOutputReference/01a-InputOutputReference.md
deleted file mode 100644
index 371e5cbdd2f..00000000000
--- a/doc/src/docs/InputOutputReference/01a-InputOutputReference.md
+++ /dev/null
@@ -1,20189 +0,0 @@
-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Input Output Reference</h1>
-<h2>The Encyclopedic Reference to EnergyPlus Input and Output</h2>
-<br/>
-<p><i>(the ins and outs of EnergyPlus)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-
-Input-Output Reference
-======================
-
-This document is intended to be an encyclopedic reference for the EnergyPlus Input Data Dictionary (IDD), Input Data File (IDF) and potential resultant outputs (various output files).
-
-The following descriptions are “grouped� by the elements in the IDD (ref: Getting Started Document and the IDD Conventions). In some cases, the descriptions of reporting will be done for an object (e.g. Lighting electrical consumption or thermal comfort value for a group of people) and in some cases for the entire group (e.g., ambient condition reports).
-
-What’s different about EnergyPlus Input and Output?
----------------------------------------------------
-
-The usual procedure for non-interactive programs is to process all the input necessary to “do the job�, perform the actions required by the input, and somewhere along the way produce reports on the actions. Usually, there will be error messages on incorrect input statements and/or incorrect conditions detected during processing. Usually, the input is echoed in its entirety so that the context of errors is shown clearly.
-
-Results are typically output into reports as well as a compilation of various inputs reformatted into different groupings than were originally entered (defaults filled in, etc.)
-
-EnergyPlus does all the above. However, some nuances are different from the usual actions.
-
-### EnergyPlus Input Processing
-
-1)    EnergyPlus reads the data dictionary (Energy+.idd) and the input data file (in.idf) prior to doing anything else. Only after this is done does processing start. HOWEVER, the input processor only knows as much as the data dictionary has told it. It knows which fields should be alpha and which should be numeric. All of this information (including the IDD) is echoed to the audit file (audit.out) in case errors occur. Most of the errors show up (out of context) in the standard error file (eplusout.err) – there might be enough information to decipher where the error is or you may have to look at the more inclusive audit file. Invalid numeric fields are detected during this processing and default numeric fields are filled. For more information on the IDD, its structure and implications, please see the IDD Conventions discussion below.
-
-2)    The biggest difference between EnergyPlus and more traditional input processing is that EnergyPlus is modular in its actual filling in the details for the simulation. Because of the modular structure of EnergyPlus, each module is responsible for “getting� its own input. It receives this input from the input processor in the form of alpha and numeric fields. Each module typically gets all its input the first time it is called. The implication for the user is that error messages may show up in somewhat peculiar places. A further implication is that no order is needed in the input data file!  Data that is not needed by a particular simulation is not processed.
-
-3)    The data dictionary has the capability to do “automatic� range checking on numeric fields as well as fill in numeric defaults. Both filling in defaults and “automatic� range checking are done when the data is read. Other checks may need a combination of fields and won’t be done until the data is “processed� (after the simulation starts).
-
-4)    A couple of other differences that might not be true in other programs:  Blanks are significant in alpha fields **SO** DesignDay is not the same as Design Day (1 space between Design and Day) nor Design  Day (2 spaces between Design and Day). Alpha objects, however, *are* case insensitive SO DesignDay is the same as ‘designday’ or ‘SizingPeriod:DesignDay’.
-
-### General Input Rules
-
-Rules shown here are for the input data files. Rules about the Input Data Dictionary are shown in the Interface Developer’s Guide (there is much similarity and overlap) but most users don’t need to touch the IDD (Input Data Dictionary).
-
-The input data file is the primary file that EnergyPlus uses to create the building simulation. The only additional files are referenced by certain objects (such as the Schedule:File object). The input is order-independent; data can appear in any order and will be retrieved and sorted as necessary by the EnergyPlus simulation modules.  In addition, EnergyPlus allocates everything dynamically, so there are no limitations as to number of zones, surfaces, etc.
-
-- The initial line of an input object MUST have a comma or semicolon.
-
-- Fields do not extend over line boundaries.  Usually, if a comma or (as appropriate) semi-colon is not the last field value on a line, one will be inserted.  Of course, several fields may appear on a single line as long as they are comma separated. (And the last could be followed by a semi-colon).
-
-- Commas delimit fields – therefore, no fields can have embedded commas.  No error will occur but you won't get what you want. You cannot surround a field with “ to accommodate commas in the fields.
-
-- Blank lines are allowed.
-
-- The comment character is a exclamation “!�.  Anything on a line after the exclamation is ignored.
-
-- Input records (aka input line length) can be up to 500 characters in length.  If you go over that, no error will occur but you won't get what you want.
-
-- Each Alpha string in the input data file (aka alpha field length) can be up to 100 characters in length. Anything beyond that is truncated. This would apply to all names (such as zone name, node name, schedule name) in fields.
-
-- Each Alpha string (including Section and Class/Object keywords) is mapped to UPPER case during processing, unless the “*retaincase*� flag marks the field in the IDD.  Get routines from the EnergyPlus code that use the Section and Object keywords automatically map to UPPER case for finding the item.  The primary drawback with this is that error messages coming out of the input processor will be in UPPER case and may not appear exactly as input.
-
-- Special characters, such as tabs, should NOT be included in the file.  However, tabs can be accommodated and are turned into spaces.
-
-- All numbers can be flexibly input and are processed into single precision variables (i.e. 1.0, 1.000, 1, .1E+1 are all processed equally).
-
-### EnergyPlus Output Processing
-
-1)    Unlike the usual formatted output text formatted reports, EnergyPlus usual output is either at the summary or at the detailed (variable) level. Summary reports exist for many inputs as well as sizing results. The more detailed variable level reporting is produced as “stream of consciousness� (as the simulation happens) and must be post-processed for more sensible viewing. Note that the terms “output variable� and “output variable� (accessed by the Output:Variable and/or Output:Meter objects) are used interchangably in this document.
-
-2)    Most EnergyPlus reporting can be readily viewed in current spreadsheet programs – or other software that can process “delimited variable� reports. In these kind of reports, each “column� is separated from the next by a “delimiter�. Typical delimiters are “comma� and “tab�. Gradually, EnergyPlus reporting is moving from all comma separated reports to allow the user to select the delimiter via “style� objects.
-
-3)    Styled reports allow for more selectable output reporting but also increase the number of output files as we have chosen to create the report names with extensions that typify the actual reporting. Depending on the reporting, these can be:
-
-✓ Tab – reports with a .tab extension have tabs as the delimiter. These report files (directly from EnergyPlus) will be named something like “eplus&lt;xxx&gt;.tab� where the &lt;xxx&gt; is a short name of the kind of report (e.g. Zsz for Zone Sizing, Map for Daylighting Map)
-
-✓ Csv – reports with a .csv extension have commas as the delimiter. These are also specially formatted for use in spreadsheets (such as the compilation of results from the eplusout.eso file into the eplusout.csv file using the default post-processor program).
-
-✓ Txt – reports with a .txt extension have spaces as the “delimiter� but only certain of these are really formatted the way you might expect: where multiple spaces make printing with a non-proportional font would produce readable output.
-
-✓ Html – reports with a .html extension are “web-browser� ready.
-
-IDD Conventions
----------------
-
-The following is a basic description of the structure of the IDD (it’s actually taken directly from the IDD file). As noted within, **!** signifies a comment character as does the **\\**. **\\** has also been adopted as a convention for including more specific comments about each field in an object. These have been used with success in the IDFEditor and it is hoped the flexibility will provide other interface developers with useful information.
-
-```idd
-!IDD_Version **VERSION NUMBER**
-! **************************************************************************
-! This file is the Input Data Dictionary (IDD) for EnergyPlus.
-! The IDD defines the syntax and data model for each type of input "Object."
-! Lines in EnergyPlus input files (and IDD) are limited to 500 characters.
-!
-! Object Description
-! ------------------
-! To define an object (a record with data), develop a key word that is unique
-! Each data item to the object can be A (Alphanumeric string) or N (numeric)
-! Number each A and N.  This will show how the data items will be put into the
-! arrays that are passed to the Input Processor "Get" (GetObjectItem) routines.
-! All alpha fields are limited to 100 characters.  Numeric fields should be
-! valid numerics (can include such as 1.0E+05) and are placed into double
-! precision variables.
-!
-! NOTE: Even though a field may be optional, a comma representing that field
-!   must be included (unless it is the last field in the object).  Since the
-!   entire input is "field-oriented" and not "keyword-oriented", the EnergyPlus
-!   Input Processor must have some representation (even if blank) for each
-!   field.
-!
-! Object Documentation
-! --------------------
-! In addition, the following special comments appear one per line and
-! most are followed by a value.  Comments may apply to a field or the object
-! or a group of objects.
-!
-! Field-level comments:
-!
-!  \field           Name of field
-!                     (should be succinct and readable, blanks are encouraged)
-!
-!  \note            Note describing the field and its valid values. If multiple lines,
-!                   start each line with \note. Limit line length to 100 characters.
-!
-!  \required-field  To flag fields which may not be left blank
-!                     (this comment has no "value")
-!
-!  \begin-extensible  Marks the first field at which the object accepts an extensible
-!                   field set.  A fixed number of fields from this marker define the
-!                   extensible field set, see the object code \extensible for
-!                   more information.
-!
-!  \units           Units (must be from EnergyPlus standard units list)
-!                   EnergyPlus units are standard SI units
-!
-!  \ip-units        IP-Units (for use by input processors with IP units)
-!                   This is only used if the default conversion is not
-!                   appropriate.
-!
-!  \unitsBasedOnField  For fields that may have multiple possible units, indicates
-!                   the field in the object that can be used to determine
-!                   the units. The field reference is in the A2 form.
-!
-!  \minimum         Minimum that includes the following value
-!
-!  \minimum&gt;        Minimum that must be &gt; than the following value
-!
-!  \maximum         Maximum that includes the following value
-!
-!  \maximum<        Maximum that must be < than the following value
-!
-!  \default         Default for the field (if N/A then omit entire line)
-!
-!  \deprecated      This field is not really used and will be deleted from the object.
-!                   The required information is gotten internally or
-!                   not needed by the program.
-!
-!  \autosizable     Flag to indicate that this field can be used with the Auto
-!                   Sizing routines to produce calculated results for the
-!                   field.  If a value follows this, then that will be used
-!                   when the "Autosize" feature is flagged.  To trigger
-!                   autosizing for a field, enter Autosize as the field's
-!                   value.  Only applicable to numeric fields.
-!
-! \autocalculatable Flag to indicate that this field can be automatically
-!                   calculated. To trigger auto calculation for a field, enter
-!                   Autocalculate as the field's value.  Only applicable to
-!                   numeric fields.
-!
-!  \type            Type of data for the field -
-!                     integer
-!                     real
-!                     alpha       (arbitrary string),
-!                     choice      (alpha with specific list of choices, see
-!                                 \key)
-!                     object-list (link to a list of objects defined elsewhere,
-!                                  see \object-list and \reference)
-!                     external-list (uses a special list from an external source,
-!                                    see \external-list)
-!                     node        (name used in connecting HVAC components)
-!
-!  \retaincase      Retains the alphabetic case for alpha type fields
-!
-!  \key             Possible value for "\type choice" (blanks are significant)
-!                     use multiple \key lines to indicate all valid choices
-!
-!  \object-list     Name of a list of user-provided object names that are valid
-!                     entries for this field (used with "\reference")
-!                     see Zone and BuildingSurface:Detailed objects below for
-!                     examples.
-!                  ** Note that a field may have multiple \object-list commands.
-!
-!  \external-list   The values for this field should be selected from a special
-!                   list generated outside of the IDD file. The choices for the
-!                   special lists are:
-!                        autoRDDvariable
-!                        autoRDDmeter
-!                        autoRDDvariableMeter
-!                   When one of these are selected the options for the field
-!                   are taken from the RDD or MDD file or both.
-!
-!  \reference       Name of a list of names to which this object belongs
-!                     used with "\type object-list" and with "\object-list"
-!                     see Zone and BuildingSurface:Detailed objects below for
-!                     examples:
-!
-!                        Zone,
-!                          A1 , \field Name
-!                               \type alpha
-!                               \reference ZoneNames
-!
-!                        BuildingSurface:Detailed,
-!                          A4 , \field Zone Name
-!                               \note Zone the surface is a part of
-!                               \type object-list
-!                               \object-list ZoneNames
-!
-!             For each zone, the field "Name" may be referenced
-!             by other objects, such as BuildingSurface:Detailed, so it is
-!             commented with "\reference ZoneNames"
-!             Fields that reference a zone name, such as BuildingSurface:Detailed's
-!             "Zone Name", are commented as
-!             "\type object-list" and "\object-list ZoneNames"
-!             ** Note that a field may have multiple \reference commands.
-!             ** This is useful if the object belongs to a small specific
-!             object-list as well as a larger more general object-list.
-!
-! Object-level comments:
-!
-!  \memo            Memo describing the object. If multiple lines, start each line
-!                   with \memo.
-!                   Limit line length to 100 characters.
-!
-!  \unique-object   To flag objects which should appear only once in an idf
-!                     (this comment has no "value")
-!
-!  \required-object To flag objects which are required in every idf
-!                     (this comment has no "value")
-!
-!  \min-fields      Minimum number of fields that should be included in the
-!                   object.  If appropriate, the Input Processor will fill
-!                   any missing fields with defaults (for numeric fields).
-!                   It will also supply that number of fields to the "get"
-!                   routines using blanks for alpha fields (note -- blanks
-!                   may not be allowable for some alpha fields).
-!
-!  \obsolete        This object has been replaced though is kept (and is read)
-!                   in the current version.  Please refer to documentation as
-!                   to the dispersal of the object.  If this object is
-!                   encountered in an IDF, the InputProcessor will post an
-!                   appropriate message to the error file.
-!                   usage:  \obsolete New=&gt;[New object name]
-!
-!  \extensible:<\#&gt;  This object is dynamically extensible -- meaning, if you
-!           change the IDD appropriately (if the object has a simple list
-!           structure -- just add items to the list arguments (i.e. BRANCH
-!           LIST). These will be automatically redimensioned and used during
-!           the simulation. <\#&gt; should be entered by the developer to signify
-!           how many of the last fields are needed to be extended (and EnergyPlus
-!           will attempt to auto-extend the object).  The first field of the first
-!           instance of the extensible field set is marked with \begin-extensible.
-!
-!  \begin-extensible See previous item, marks beginning of extensible fields in
-!                   an object.
-!
-!  \format          The object should have a special format when saved in
-!                   the IDF Editor with the special format option enabled.
-!                   The options include SingleLine, Vertices, CompactSchedule,
-!                   FluidProperties, ViewFactors, and Spectral.
-!                   The SingleLine option puts all the fields for the object
-!                   on a single line. The Vertices option is used in objects
-!                   that use X, Y and Z fields to format those three fields
-!                   on a single line.
-!                   The CompactSchedule formats that specific object.
-!                   The FluidProperty option formats long lists of fluid
-!                   properties to ten values per line.
-!                   The ViewFactor option formats three fields related to
-!                   view factors per line.
-!                   The Spectral option formats the four fields related to
-!                   window glass spectral data per line.
-!
-!   \reference-class-name Adds the name of the class to the reference list
-!                   similar to \reference.
-!
-! Group-level comments:
-!
-!  \group          Name for a group of related objects
-!
-!
-! Notes on comments
-! -----------------
-!
-! 1.  If a particular comment is not applicable (such as units, or default)
-! then simply omit the comment rather than indicating N/A.
-!
-! 2.  Memos and notes should be brief (recommend 5 lines or less per block).
-! More extensive explanations are expected to be in the user documentation
-```
-
-### IDD – IP Units
-
-In addition, the IDD contains indications of IP (inch-pound) units for the EnergyPlus standard SI (Systems International) units. These may be used by input and output interfaces to display values in the IP system. As noted, if the IP units are “standard� (first block below), then no \\ip-units is expected in the field. Note that for some fields – due to their multiple use (for example, schedule values) – there cannot be a ip-unit designation.
-
-```idd
-! Default IP conversions (no \ip-units necessary)
-!      $/(m3/s)               =>   $/(ft3/min)         0.000472000059660808
-!      $/(W/K)                =>   $/(Btu/h-F)         0.52667614683731
-!      $/kW                   =>   $/(kBtuh/h)         0.293083235638921
-!      $/m2                   =>   $/ft2               0.0928939733269818
-!      $/m3                   =>   $/ft3               0.0283127014102352
-!      (kg/s)/W               =>   (lbm/sec)/(Btu/hr)  0.646078115385742
-!      1/K                    =>   1/F                 0.555555555555556
-!      1/m                    =>   1/ft                0.3048
-!      A/K                    =>   A/F                 0.555555555555556
-!      C                      =>   F                   1.8 (plus 32)
-!      cm                     =>   in                  0.3937
-!      cm2                    =>   inch2               0.15500031000062
-!      deltaC                 =>   deltaF              1.8
-!      deltaJ/kg              =>   deltaBtu/lb         0.0004299
-!      g/GJ                   =>   lb/MWh              0.00793664091373665
-!      g/kg                   =>   grains/lb           7
-!      g/MJ                   =>   lb/MWh              7.93664091373665
-!      g/mol                  =>   lb/mol              0.0022046
-!      g/m-s                  =>   lb/ft-s             0.000671968949659
-!      g/m-s-K                =>   lb/ft-s-F           0.000373574867724868
-!      GJ                     =>   ton-hrs             78.9889415481832
-!      J                      =>   Wh                  0.000277777777777778
-!      J/K                    =>   Btu/F               526.565
-!      J/kg                   =>   Btu/lb              0.00042986
-!      J/kg-K                 =>   Btu/lb-F            0.000239005736137667
-!      J/kg-K2                =>   Btu/lb-F2           0.000132889924714692
-!      J/kg-K3                =>   Btu/lb-F3           7.38277359526066E-05
-!      J/m2-K                 =>   Btu/ft2-F           4.89224766847393E-05
-!      J/m3                   =>   Btu/ft3             2.68096514745308E-05
-!      J/m3-K                 =>   Btu/ft3-F           1.49237004739337E-05
-!      K                      =>   R                   1.8
-!      K/m                    =>   F/ft                0.54861322767449
-!      kg                     =>   lb                  2.2046
-!      kg/J                   =>   lb/Btu              2325.83774250441
-!      kg/kg-K                =>   lb/lb-F             0.555555555555556
-!      kg/m                   =>   lb/ft               0.67196893069637
-!      kg/m2                  =>   lb/ft2              0.204794053596664
-!      kg/m3                  =>   lb/ft3              0.062428
-!      kg/m-s                 =>   lb/ft-s             0.67196893069637
-!      kg/m-s-K               =>   lb/ft-s-F           0.373316072609094
-!      kg/m-s-K2              =>   lb/ft-s-F2          0.207397818116164
-!      kg/Pa-s-m2             =>   lb/psi-s-ft2        1412.00523459398
-!      kg/s                   =>   lb/s                2.20462247603796
-!      kg/s2                  =>   lb/s2               2.2046
-!      kg/s-m                 =>   lb/s-ft             0.67196893069637
-!      kJ/kg                  =>   Btu/lb              0.429925
-!      kPa                    =>   psi                 0.145038
-!      L/day                  =>   pint/day            2.11337629827348
-!      L/GJ                   =>   gal/kWh             0.000951022349025202
-!      L/kWh                  =>   pint/kWh            2.11337629827348
-!      L/MJ                   =>   gal/kWh             0.951022349025202
-!      lux                    =>   foot-candles        0.092902267
-!      m                      =>   ft                  3.28083989501312
-!      m/hr                   =>   ft/hr               3.28083989501312
-!      m/s                    =>   ft/min              196.850393700787
-!      m/s                    =>   miles/hr            2.2369362920544
-!      m/yr                   =>   inch/yr             39.3700787401575
-!      m2                     =>   ft2                 10.7639104167097
-!      m2/m                   =>   ft2/ft              3.28083989501312
-!      m2/person              =>   ft2/person          10.764961
-!      m2/s                   =>   ft2/s               10.7639104167097
-!      m2-K/W                 =>   ft2-F-hr/Btu        5.678263
-!      m3                     =>   ft3                 35.3146667214886
-!      m3                     =>   gal                 264.172037284185
-!      m3/GJ                  =>   ft3/MWh             127.13292
-!      m3/hr                  =>   ft3/hr              35.3146667214886
-!      m3/hr-m2               =>   ft3/hr-ft2          3.28083989501312
-!      m3/hr-person           =>   ft3/hr-person       35.3146667214886
-!      m3/kg                  =>   ft3/lb              16.018
-!      m3/m2                  =>   ft3/ft2             3.28083989501312
-!      m3/MJ                  =>   ft3/kWh             127.13292
-!      m3/person              =>   ft3/person          35.3146667214886
-!      m3/s                   =>   ft3/min             2118.88000328931
-!      m3/s-m                 =>   ft3/min-ft          645.89
-!      m3/s-m2                =>   ft3/min-ft2         196.85
-!      m3/s-person            =>   ft3/min-person      2118.6438
-!      m3/s-W                 =>   (ft3/min)/(Btu/h)   621.099127332943
-!      N-m                    =>   lbf-in              8.85074900525547
-!      N-s/m2                 =>   lbf-s/ft2           0.0208857913669065
-!      Pa                     =>   psi                 0.000145037743897283
-!      percent/K              =>   percent/F           0.555555555555556
-!      person/m2              =>   person/ft2          0.0928939733269818
-!      s/m                    =>   s/ft                0.3048
-!      V/K                    =>   V/F                 0.555555555555556
-!      W                      =>   Btu/h               3.4121412858518
-!      W/(m3/s)               =>   W/(ft3/min)         0.0004719475
-!      W/K                    =>   Btu/h-F             1.89563404769544
-!      W/m                    =>   Btu/h-ft            1.04072
-!      W/m2                   =>   Btu/h-ft2           0.316957210776545
-!      W/m2                   =>   W/ft2               0.09290304
-!      W/m2-K                 =>   Btu/h-ft2-F         0.176110194261872
-!      W/m2-K2                =>   Btu/h-ft2-F2        0.097826
-!      W/m-K                  =>   Btu-in/h-ft2-F      6.93481276005548
-!      W/m-K2                 =>   Btu/h-F2-ft         0.321418310071648
-!      W/m-K3                 =>   Btu/h-F3-ft         0.178565727817582
-!      W/person               =>   Btu/h-person        3.4121412858518
-!
-! Other conversions supported (needs the \ip-units code)
-!
-!      kPa                    =>   inHg                0.29523
-!      m                      =>   in                  39.3700787401575
-!      m3/s                   =>   gal/min             15850.3222370511
-!      Pa                     =>   ftH2O               0.00033455
-!      Pa                     =>   inH2O               0.00401463
-!      Pa                     =>   inHg                0.00029613
-!      Pa                     =>   Pa                  1
-!      W                      =>   W                   1
-!      W/m2                   =>   W/m2                1
-!      W/m-K                  =>   Btu/h-ft-F          0.577796066000163
-!      W/person               =>   W/person            1
-!
-! Units fields that are not translated
-!      $
-!      1/hr
-!      A
-!      Ah
-!      A/V
-!      Availability
-!      Control
-!      cycles/hr
-!      days
-!      deg
-!      dimensionless
-!      eV
-!      hr
-!      J/J
-!      kg/kg
-!      kg-H2O/kg-air
-!      kmol
-!      kmol/s
-!      m3/m3
-!      minutes
-!      Mode
-!      ms
-!      ohms
-!      percent
-!      ppm
-!      rev/min
-!      s
-!      V
-!      VA
-!      W/m2 or deg C
-!      W/m2, W or deg C
-!      W/s
-!      W/W
-!      years
-! **************************************************************************
-```
-
-Input – Output Descriptions (Document)
---------------------------------------
-
-### Input Descriptions
-
-In the descriptions below, the fields for each input object will be described but the Energy+.idd descriptions will not be shown. Refer to the actual Energy+.idd file for complete specifications. Energy+.idd is a text file that can be viewed with many text editors or word processors. The Site:Location object will serve as an example.
-
-```idd
-Site:Location,
-       \unique-object
-       \min-fields 5
-  A1 , \field Name
-       \required-field
-       \type  alpha
-  N1 , \field Latitude
-       \units deg
-       \minimum -90.0
-       \maximum +90.0
-       \default 0.0
-       \note + is North, - is South, degree minutes represented in decimal (i.e. 30 minutes is .5)
-       \type real
-  N2 , \field Longitude
-       \units deg
-       \minimum -180.0
-       \maximum +180.0
-       \default 0.0
-       \note - is West, + is East, degree minutes represented in decimal (i.e. 30 minutes is .5)
-       \type real
-  N3 , \field Time Zone
-       \note basic these limits on the WorldTimeZone Map (2003)
-       \units hr
-       \minimum -12.0
-       \maximum +14.0
-       \default 0.0
-       \note  Time relative to GMT. Decimal hours.
-       \type real
-  N4 ; \field Elevation
-       \units m
-       \minimum -300.0
-       \maximum< 8900.0
-       \default 0.0
-       \type real
-```
-
-The IDD excerpt above is the complete definition as seen in the IDD file.
-
-First, the object name is given. (Site:Location)  This is followed by a comma in both the definition (IDD) and in an input file (IDF). In fact, all fields except the terminating field of an IDD class object and IDF object are followed by commas. The final field in an IDD class object or in an IDF object is terminated by a semi-colon.
-
-Next is an alpha field, the location name. As noted above, for input, spaces are significant in this field. The main inputs for Site:Location are numeric fields. These are numbered (as is the alpha field) for convenience. The \\ designations will show various information about the objects as described above in the IDD conventions discussion. Of importance for reading this document are the units and possible minimum and maximum values for a  field.
-
-There is automatic processing of the \\minimum, \\maximum and \\default data for numeric fields. Any infractions of the \\minimum, \\maximum fields are automatically detected and messages will appear in the standard error file. After all the input is checked, infractions will cause program termination (before the bulk of the simulation is completed). Defaults are also enforced if you leave the numeric field blank.
-
-Some objects need all the parameters listed by the definition; some do not. In the descriptions that follow, we will try to indicate which parts are optional. Usually, these will be the last fields in the object input or definition. Even if items are not used for a particular object (e.g. Multiplier in the FenestrationSurface:Detailed and type=Door), the field must be included unless it is the *last field in the object*. So, for this instance, one must include a multiplier field (must be numeric and would need to obey any \\minimum, \\maximum rules) for doors.
-
-Two spreadsheet files are included with the installation:
-
-- ExampleFiles.xls – shows many details about the included example files including highlights of features.
-
-- ExampleFiles-ObjectsLink.xls – shows, for each object, the first three occurrences of that object in an example file.
-
-### Output Descriptions
-
-In the descriptions below, we will endeavor to have each object’s output displayed as well as each of the outputs described. The output variables for a run are selected by choosing the Output:VariableDictionary object. This object displays the available output variables for a run on the **eplusout.rdd** (regular variables) and **eplusout.mdd** (meter variables) files. Two significant styles are available for these displays and the descriptions below may have one for some objects and another for other objects. The variables are the same but will look a bit different.  For clarity, the two displays are shown below:
-
-Note that the IDF-Editor can interpret both sets of files and assist you in getting output variables into your input files. But you will have to successfully run your input file first.
-
-The Simple (or regular) display looks like the following figure and is interpreted:
-
-**Zone/HVAC** – when the output is produced at the “Zone� timestep (ref: number of timesteps in each hour) or at the “HVAC� aka System timestep (which can vary for each hour).
-
-**Average/Sum** – whether this is a averaged value over the reporting period (such as a temperature or rate) or whether this is a summed value over the reporting period. Reporting periods are specified in the Output:Variable or Output:Meter objects.
-
-**&lt;Variable Name&gt;** -- The variable name one uses for reporting is displayed (e.g., Site Outdoor Drybulb Temperature) along with the units (e.g., [C]).
-
-Example from the **eplusout.rdd** file:
-
-* Zone,Average,Site Outdoor Air Drybulb Temperature [C]
-
-* Zone,Average,Site Outdoor Air Dewpoint Temperature [C]
-
-* Zone,Average,Site Outdoor Air Wetbulb Temperature [C]
-
-* Zone,Average,Site Outdoor Air Humidity Ratio [kgWater/kgAir]
-
-* Zone,Average,Site Outdoor Air Relative Humidity [%]
-
-* Zone,Average,Site Outdoor Air Barometric Pressure [Pa]
-
-* Zone,Average,Wind Speed [m/s]
-
-* Zone,Average,Site Wind Direction [deg]
-
-* Zone,Average,Site Sky Temperature [C]
-
-* HVAC,Sum,Zone Air System Sensible Heating Energy [J]
-
-* HVAC,Sum,Zone Air System Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Air System Sensible Heating Rate [W]
-
-* HVAC,Average,Zone Air System Sensible Cooling Rate [W]
-
-* HVAC,Average,Zone Air Temperature [C]
-
-* HVAC,Average,Zone Thermostat Air Temperature [C]
-
-Note that the **eplusout.mdd** file is similar, but meters are only available at the Zone timestep.
-
-* Zone,Meter,Electricity:Facility [J]
-
-* Zone,Meter,ExteriorLights:Electricity [J]
-
-* Zone,Meter,Grounds Lights:ExteriorLights:Electricity [J]
-
-* Zone,Meter,EnergyTransfer:Facility [J]
-
-* Zone,Meter,EnergyTransfer:Building [J]
-
-* Zone,Meter,EnergyTransfer:Zone:R13WALL WALLS [J]
-
-The IDF display has all the same information in an IDF-ready form (i.e., you could copy and paste it into your input file using a text editor).
-
-Example from the **eplusout.rdd** file:
-
-* Output:Variable,\*,Site Outdoor Air Drybulb Temperature,hourly; !- Zone Average [C]
-
-* Output:Variable,\*,Site Outdoor Air Dewpoint Temperature,hourly; !- Zone Average [C]
-
-* Output:Variable,\*,Site Outdoor Air Wetbulb Temperature,hourly; !- Zone Average [C]
-
-* Output:Variable,\*,Site Outdoor Air Humidity Ratio,hourly; !- Zone Average [kgWater/kgAir]
-
-* Output:Variable,\*,Site Outdoor Air Relative Humidity,hourly; !- Zone Average [%]
-
-* Output:Variable,\*,Site Outdoor Air Barometric Pressure,hourly; !- Zone Average [Pa]
-
-* Output:Variable,\*,Zone Air System Sensible Heating Energy,hourly; !- HVAC Sum [J]
-
-* Output:Variable,\*,Zone Air System Sensible Cooling Energy,hourly; !- HVAC Sum [J]
-
-* Output:Variable,\*,Zone Air System Sensible Heating Rate,hourly; !- HVAC Average [W]
-
-* Output:Variable,\*,Zone Air System Sensible Cooling Rate,hourly; !- HVAC Average [W]
-
-* Output:Variable,\*,Zone Air Temperature,hourly; !- HVAC Average [C]
-
-* Output:Variable,\*,Zone Thermostat Air Temperature,hourly; !- HVAC Average [C]
-
-All of the same information appears in a slightly different form and defaults to “hourly� reporting frequency (which, of course, can be changed when you put it into your input file). The “\*� is preselected so that you would be reporting for all those items.
-
-Group -- Simulation Parameters
-------------------------------
-
-This group of objects influences the simulation in various ways.
-
-### Version
-
-#### Field: Version Identifier
-
-The Version object allows you to enter the proper version that your IDF was created for. This is checked against the current version of EnergyPlus and a Severe error issued (non-terminating) if it does not match the current version string. Note that versions are often significant and there is no guarantee that the older file will run in the newer versions of the program. See IDF Version Updater (Auxiliary Programs Document) for methods of changing the older files to newer versions.
-
-### Timestep
-
-#### Field: Number of Timesteps per Hour
-
-The Timestep object specifies the "basic" timestep for the simulation. The value entered here is usually known as the Zone Timestep.  This is used in the Zone Heat Balance Model calculation as the driving timestep for heat transfer and load calculations.  The value entered here is the number of timesteps to use within an hour.  Longer length timesteps have lower values for Number of Timesteps per Hour.  For example a value of 6 entered here directs the program to use a zone timestep of 10 minutes and a value of 60 means a 1 minute timestep.  The user’s choice for Number of Timesteps per Hour must be evenly divisible into 60; the allowable choices are 1, 2, 3, 4, 5, 6, 10, 12, 15, 20, 30, and 60.
-
-The choice made for this field has important implications for modeling accuracy and the overall time it takes to run a simulation.  Here are some considerations when choosing a value:
-
-- The solution technique used in EnergyPlus has been designed to be stable with zone timesteps of up to sixty minutes (Number Timesteps in Hour = 1).  However, 60 minutes is considered a “long� timestep and it should only be used in rare occasions where there is no HVAC system, accuracy is not a concern, and short run times are critical.  Such long timesteps are not recommended to use because simulation results are more accurate for shorter timesteps, of say 10 minutes or less (Number of Timesteps per Hour of 6 or more).  Shorter zone timesteps improve the numerical solution of the Zone Heat Balance Model because they improve how models for surface temperature and zone air temperature are coupled together.  Longer timesteps introduce more lag and lead to more a dampened dynamic response.
-
-- Simulation run time increases with shorter timesteps or larger values for Number of Timesteps per Hour.  The effect varies with the nature of the model.  The user can test out different values on their particular model to understand the implications for his or her particular case.  Sometimes large models with multizone HVAC and Plant systems execute nearly as fast with 15 minute timesteps as with 60 minute timesteps because fewer iterations are required in the system modeling since the prior timestep’s results are close to the final outcome of next timestep.
-
-- The weather data files usually have 60-minute (or hourly) data.  However, it does not follow that this should be used as the basis for choosing the zone timestep because:
-
-  - EnergyPlus carefully interpolates the weather data between data points for use at shorter timesteps.  This is discussed in a later section: Weather Data Hourly Interpolation
-
-  - Many aspects of a model have time scales that differ from the that of the weather data.  A goal of the modeling is to predict how the building will respond to the weather.  However, the building’s response is not *governed* by the time scale that the weather data are available at, but rather the time scales of the dynamic performance of the thermal envelope as well as things like schedules for internal gains, thermostats, and equipment availability.
-
-- If the model will include calculating the cost of electricity, then the user should be aware that many electric utility tariffs base charges on demand windows of a specified length of time.  If the choice of Number of Timesteps per Hour is not consistent with the demand window, then unexpected results may be obtained.  For reasonable prediction of the maximum rates for electricity use for in calculating demand charges, the length of the zone timestep needs to be consistent with the tariff’s demand window.  The following table lists what values are consistent with various demand windows.
-
-<table class="table table-striped">
-<tr>
-<th>Demand Window</th>
-<th>Applicable Number of Timesteps per Hour</th>
-</tr>
-<tr>
-<td>QuarterHour</td>
-<td>4, 12, 20, or 60</td>
-</tr>
-<tr>
-<td>HalfHour</td>
-<td>2, 4, 6, 10, 12, 20, 30, or 60</td>
-</tr>
-<tr>
-<td>FullHour, Day, Week</td>
-<td>Any</td>
-</tr>
-</table>
-
-There is also second type of timestep inside EnergyPlus that is known as the System Timestep. This is a variable-length timestep that governs the driving timestep for HVAC and Plant system modeling.  The user cannot directly control the system timestep (except by use of the ConvergenceLimits object). When the HVAC portion of the simulation begins its solution for the current zone timestep, it uses the zone timestep as its maximum length but then can reduce the timestep, as necessary, to improve the solution.  The technical details of the approach are explained in the Engineering Documentation under "Integrated Solution Manager".
-
-Users can see the system timestep used if they select the "detailed" frequency option on an HVAC output variable (e.g. Zone Air Temperature). To contrast, the "Zone" variables will only be reported on the zone timestep (e.g. Zone Mean Air Temperature).
-
-And, the IDF example:
-
-```idf
-Timestep, 6;  !Suggested default for most system simulations
-```
-
-Suggested defaults are 4 for non-HVAC simulations, 6 for simulations with HVAC, 20 is the minimum for ConductionFiniteDifference and HeatAndMoistureFiniteElement simulations. Green roof (ref: Material:RoofVegetation) also may require more timesteps.
-
-Note that hourly data (such as outdoor conditions expressed by Design Days or Weather data) are interpolated to the Zone Timestep. This is discussed in a later section: Weather Data Hourly Interpolation
-
-### ConvergenceLimits
-
-This item is an “advanced� feature that should be used only with caution. It is specifically included to assist some users “speed up� calculations while not overly compromising accuracy. The user must judge for him/herself whether the reduced run time is useful.
-
-#### Field: Minimum System Timestep
-
-Usually the minimum system timestep is allowed to vary from the zone timestep (as maximum) to a minimum timestep of 1 minute during certain system calculations. This might be when the system turns on or off, for example. Entering 0 in this field sets the minimum system timestep to be the same as the zone timestep. Otherwise the units of the field are minutes. It’s probably a good idea to have any minimum entered be a divisor of the zone timestep.
-
-#### Field: Maximum HVAC Iterations
-
-The HVAC Manager will iterate to a solution or up to a set number of iterations. If not “converged�, then a warning error appears:
-
-SimHVAC: Maximum iterations (20) exceeded for all HVAC loops, at CHICAGO IL USA TMY2-94846 WMO\#=725300, 10/07 14:06 - 14:08
-
-In order to reduce time used in simulating your building, you may choose to enter a lesser number than the default of 20 for the maximum number of iterations to be used. Or, you may wish to enter a bigger number for certain buildings. To get more information printed with a “max iteration� message, you need to enter a “Output:Diagnostics, DisplayExtraWarnings;� command (which may also generate other warnings than just this one).
-
-#### Field: Minimum Plant Iterations
-
-The plant system modeling includes a solver that iterates within a single HVAC manager iteration.  This input field and the next one provide some control over how the plant solver iterates.  This field sets a minimum threshold for plant interations. The default for this field is the value “2� which indicates that a minimum of two full plant model interations will be performed every time plant is called by the HVAC manager.  For faster performance with simple plant systems, this input field could be set to the value “1�.  For complicated plant systems that present difficulties to solve, this value may need to be set higher to ensure accuracy but at the expense of speed.  Complicated plant systems include those with several interconnected loops, sizing miss-matches such that plant components are starved of flow compared to their desired flow, heat recovery systems, and thermal load following onsite generators.
-
-#### Field: Maximum Plant Iterations
-
-The plant system solver iterates within a single HVAC manager iteration.  This input field and the previous one provide some control over how the plant model iterates.  This field sets a maximum limit for plant interations.  The default for this field is the value “8� which indicates that the plant solver will exit after having completed eight full iterations.  This value can be raised for better accuracy with complex plants or lowered for faster speed with simple plants. The output variable called “Plant Solver Sub Iteration Count� (typically reported at the “detailed� frequency) is useful for understanding how many plant solver iterations are actually being used during a particular simulation.  The lower limit of the value for this field is “2.�
-
-Use in an IDF:
-
-```idf
-ConvergenceLimits,
-  0,        !- Minimum System Timestep (0=same as zone timestep)
-  25,       !- Maximum HVAC Iterations
-  3,        !- Minimum Plant Iterations
-  9;        !- Maximum Plant Iterations
-```
-
-### Building
-
-The Building object describes parameters that are used during the simulation of the building. There are necessary correlations between the entries for this object and some entries in the Site:WeatherStation and Site:HeightVariation objects, specifically the Terrain field.
-
-#### Field: Building Name
-
-Building name is specified for output convenience.
-
-#### Field: North Axis
-
-The Building North Axis is specified **relative to true North**. Buildings frequently do not line up with true north. For convenience, one may enter surfaces in a “regular� coordinate system and then shift them via the use of the North Axis. The value is specified in degrees from “true north� (clockwise is positive).
-
-The figure below shows how the building north axis can be rotated to correspond with one of the major axes of an actual building. The relevance of this field is described more completely under “GlobalGeometryRules�; in particular, the value of “North Axis� is *ignored* if a coordinate system other than “relative� is used.
-
-![](media/image001.svg)
-
-Figure 1. Illustration of Building North Axis
-
-#### Field: Terrain
-
-The site’s terrain affects how the wind hits the building – as does the building height. In addition, the external conduction method usually has its own parameters for the calculation. Please see the Engineering Documentation, External Conduction section for particulars. The legal values for this field are shown in the following table.
-
-Table 1. Values for "Terrain"
-
-<table class="table table-striped">
-  <tr>
-    <th>Terrain Type Value</th>
-    <th>Terrain Description</th>
-  </tr>
-  <tr>
-    <td>Country</td>
-    <td>Flat, Open Country</td>
-  </tr>
-  <tr>
-    <td>Suburbs</td>
-    <td>Rough, Wooded Country, Suburbs</td>
-  </tr>
-  <tr>
-    <td>City</td>
-    <td>Towns, city outskirts, center of large cities</td>
-  </tr>
-  <tr>
-    <td>Ocean</td>
-    <td>Ocean, Bayou flat country</td>
-  </tr>
-  <tr>
-    <td>Urban</td>
-    <td>Urban, Industrial, Forest</td>
-  </tr>
-</table>
-
-#### Warmup Convergence
-
-The following two fields along with the minimum and maximum number of warmup days (also in this object) define the user specified criteria for when EnergyPlus will “converge� at each environment (each sizing period or run period set as Yes in the SimulationControl object). EnergyPlus “runs� the first day of the environment (starting with a set of hard-coded initial conditions: temperatures are initialized to 23C and zone humidity ratios are initialized to the outdoor humidity ratio) until the loads/temperature convergence tolerance values are satisfied (next two fields) or until it reaches “maximum number of warmup days�. Note that setting the convergence tolerance values too loose will cause the program to be satisifed too early and you may not get the results you expect from the actual simulation.
-
-#### Field: Loads Convergence Tolerance Value
-
-This value represents the number at which the loads values must agree before “convergence� is reached. Loads tolerance value is a fraction of the load.
-
-#### Field: Temperature Convergence Tolerance Value
-
-This value represents the number at which the zone temperatures must agree (from previous iteration) before “convergence� is reached. (Units for this field is delta C).
-
-Convergence of the simultaneous heat balance/HVAC solution is reached when either the loads or temperature criterion is satisfied.
-
-All tolerances have units so the temperature tolerance is in degrees C (or degrees K) and the loads tolerance is in Watts. Both tolerances work the same way, just one looks at temperatures and one looks at heating and cooling loads. After the second warm-up day, the program compares the maximum temperature experienced in a space with the maximum temperature from the previous day. If those two temperatures are within the tolerance, then it has passed the first warm-up check.
-
-It does a similar comparison with lowest temperatures experience within all the zones. If the current simulation day and the previous day values are within the tolerance, then it has passed the second warm-up check. Similar things are done with the loads tolerance and the maximum heating and cooling loads that are experienced within the spaces. Those are compared individually to the values for the previous day. If they are both in tolerance, then the simulation has passed the third and fourth warm-up check. The simulation stays in the warm-up period until ALL FOUR checks have been passed. See Engineering Reference and Output Details document for further explanation and outputs.
-
-Please note--other "convergence tolerance" inputs are required for certain HVAC equipment (unit ventilator, unit heater, window AC, etc.). The purpose and units of these parameters are different from "load convergence tolerance" and "temperature convergence tolerance" in the BUILDING object.
-
-#### Field: Solar Distribution
-
-Setting this value determines how EnergyPlus treats beam solar radiation and reflectances from exterior surfaces that strike the building and, ultimately, enter the zone. There are five choices: **MinimalShadowing**, **FullExterior** and **FullInteriorAndExterior, FullExteriorWithReflections, FullInteriorAndExteriorWithReflections**.
-
-**MinimalShadowing**
-
-In this case, there is no exterior shadowing except from window and door reveals. All beam solar radiation entering the zone is assumed to fall on the floor, where it is absorbed according to the floor's solar absorptance. Any reflected by the floor is added to the transmitted diffuse radiation, which is assumed to be uniformly distributed on all interior surfaces. If no floor is present in the zone, the incident beam solar radiation is absorbed on all interior surfaces according to their absorptances. The zone heat balance is then applied at each surface and on the zone's air with the absorbed radiation being treated as a flux on the surface.
-
-**FullExterior, FullExteriorWithReflections**
-
-In this case, shadow patterns on exterior surfaces caused by detached shading, wings, overhangs, and exterior surfaces of all zones are computed. As for MinimalShadowing, shadowing by window and door reveals is also calculated. Beam solar radiation entering the zone is treated as for MinimalShadowing -- All beam solar radiation entering the zone is assumed to fall on the floor, where it is absorbed according to the floor's solar absorptance. Any reflected by the floor is added to the transmitted diffuse radiation, which is assumed to be uniformly distributed on all interior surfaces. If no floor is present in the zone, the incident beam solar radiation is absorbed on all interior surfaces according to their absorptances. The zone heat balance is then applied at each surface and on the zone's air with the absorbed radiation being treated as a flux on the surface.
-
-**FullInteriorAndExterior, FullInteriorAndExteriorWithReflections**
-
-This is the same as FullExterior except that instead of assuming all transmitted beam solar falls on the floor the program calculates the amount of beam radiation falling on each surface in the zone, including floor, walls and windows, by projecting the sun's rays through the exterior windows, taking into account the effect of exterior shadowing surfaces and window shading devices.
-
-If this option is used, you should be sure that the surfaces of the zone totally enclose a space. This can be determined by viewing the **eplusout.dxf** file with a program like AutoDesk’s Volo View Express. You should also be sure that the zone is **convex**. Examples of convex and non-convex zones are shown in Figure 2. The most common non-convex zone is an L-shaped zone. (A formal definition of convex is that any straight line passing through the zone intercepts at most two surfaces.)  If the zone’s surfaces do not enclose a space or if the zone is not convex you should use Solar Distribution = **FullExterior** instead of **FullInteriorAndExterior**.
-
-If you use **FullInteriorAndExterior** the program will also calculate how much beam radiation falling on the inside of an exterior window (from other windows in the zone) is absorbed by the window, how much is reflected back into the zone, and how much is transmitted to the outside. In this calculation the effect of a shading device, if present, is accounted for.
-
-
-
-![](media/image002.svg)
-
-Figure 2. Illustration of Convex and Non-convex Zones
-
-
-
-**Reflection calculations**
-
-Note: Using the reflection calculations can be very time-consuming. Even error-prone. As a possible alleviation, you can use the Output:Diagnostics,DoNotMirrorDetachedShading; in many cases to get past a fatal error.
-
-If using reflections, the program calculates beam and sky solar radiation that is reflected from exterior surfaces and then strikes the building. These reflecting surfaces fall into three categories:
-
-1)   **Shadowing surfaces**. These are surfaces like overhangs or neighboring buildings entered with Shading:Site, Shading:Building, Shading:Site:Detailed, Shading:Building:Detailed, Shading:Overhang, Shading:Overhang:Projection, Shading:Fin, Shading:Fin:Projection or Shading:Zone:Detailed objects. See Figure 3.
-
-These surfaces can have diffuse and/or specular (beam-to-beam)  reflectance values that are specified with the ShadingProperty:Reflectance object which specifies those parameters. They have a default value of .2 for both visible and diffuse reflection.
-
-2)   **Exterior building surfaces**. In this case one section of the building reflects solar radiation onto another section (and vice-versa). See Figure 4.
-
-The building surfaces are assumed to be diffusely reflecting if they are opaque (walls, for example) and specularly reflecting if they are windows or glass doors. The reflectance values for opaque surfaces are calculated by the program from the Solar Absorptance and Visible Absorptance values of the outer material layer of the surface’s construction (ref: Material object properties). The reflectance values for windows and glass doors are calculated by the program from the reflectance properties of the individual glass layers that make up surface’s construction assuming no shading device is present and taking into account inter-reflections among the layers (ref: Window Properties).
-
-3)   **The ground surface**. Reflection from the ground is calculated even if reflections option is not used;l but then the ground plane is considered unobstructed, i.e., the shadowing of the ground by the building itself or by obstructions such as neighboring buildings is ignored. Shadowing by the building itself or neighboring buildings is taken into account  when the “with reflections� option is used but then the “view factor to ground� is NOT used. This is shown in Figure 5.
-
-
-
-![](media/image003.svg)
-
-Figure 3.  Solar reflection from shadowing surfaces. Solid arrows are beam solar radiation; dashed arrows are diffuse solar radiation. (a) Diffuse reflection of beam solar radiation from the top of an overhang. (b) Diffuse reflection of sky solar radiation from the top of an overhang. (c) Beam-to-beam (specular) reflection from the façade of an adjacent highly-glazed building represented by a vertical shadowing surface.
-
-
-
-![](media/image004.svg)
-
-Figure 4.  Solar reflection from building surfaces onto other building surfaces. In this example beam solar reflects from a vertical section of the building onto a roof section. The reflection from the window is specular. The reflection from the wall is diffuse.
-
-
-
-![](media/image005.svg)
-
-Figure 5. Shadowing from building affects beam solar reflection from the ground. Beam-to-diffuse reflection from the ground onto the building occurs only for sunlit areas, A and C, not from shaded area, B.
-
-#### Field: Maximum Number of Warmup Days
-
-This field specifies the number of “warmup� days that might be used in the simulation before “convergence� is achieved. The default number, 25, is usually more than sufficient for this task; however, some complex buildings (with complex constructions) may require more days. If you enter less than 25 as a maximum, that is the number of maximum warmup days that will be used. An error message will occur when the simulation “runs� out of days and has not converged:
-
-```
-CheckWarmupConvergence: Loads Initialization, Zone="MAIN ZONE" did not converge after 30 warmup days.
-See Warmup Convergence Information in .eio file for details
-..Environment(SizingPeriod)="DENVER CENTENNIAL  GOLDEN   N ANN CLG 1% CONDNS DB=&gt;MWB"
-..Max Temp Comparison = 2.06E-002 vs Temperature Convergence Tolerance=0.50 – Pass Convergence
-..Min Temp Comparison = 5.95E-003 vs Temperature Convergence Tolerance=0.50 – Pass Convergence
-..Max Cool Load Comparison = 9.5082E-002 vs Loads Convergence Tolerance=5.00E-002 – Fail Convergence
-```
-
-As noted in the message, there will be more information in the .eio file. (Refer to Output Details document as well for examples.)
-
-You may be able to increase the Maximum Number of Warmup Days and get convergence, but some anomalous buildings may still not converge. Simulation proceeds for x warmup days until “convergence� is reached (see the discussion under the Temperature Convergence Tolerance Value field in this object, just above).
-
-#### Field: Minimum Number of Warmup Days
-
-This field specifies the minimum number of “warmup� days before EnergyPlus will check if it has achieved convergence and can thus start simulating the particular environment (design day, annual run) in question. Research into the minimum number of warmup days indicates that 6 warmup days is generally enough on the minimum end of the spectrum to avoid false predictions of convergence and thus to produce enough temperature and flux history to start EnergyPlus simulation. This was based on a study that used the benchmark reference buildings. It also was observed that convergence performance improved when the number of warmup days increased. As a result, the default value for the minimum warmup days has been set to 6. Users should decrease this number only if they have knowledge that a specific file converges more quickly than 6 days. Users may wish to increase the value in certain situations when, based on the output variables described in the Output Details document, it is determined that EnergyPlus has not converged. While this parameter should be less than the previous parameter, a value greater than the value entered in the field “Maximum Number of Warmup Days� above may be used when users wish to increase warmup days more than the previous field. In this particular case, the previous field will be automatically reset to the value entered in this field and EnergyPlus will run exactly the number of warmup days specified in this field.
-
-An example from an IDF:
-
-```idf
-Building,
-  PSI HOUSE DORM AND OFFICES,  !- Name
-  36.87000,               !- North Axis {deg}
-  Suburbs,                !- Terrain
-  0.04,                   !- Loads Convergence Tolerance Value
-  0.4000000,              !- Temperature Convergence Tolerance Value {deltaC}
-  FullInteriorAndExterior, !- Solar Distribution
-  40,                     !- Maximum Number of Warmup Days
-  6;                      !- Minimum Number of Warmup Days
-```
-
-
-### SurfaceConvectionAlgorithm:Inside
-
-This input object is used control the choice of models used for surface convection at the inside face of all the heat transfer surfaces in the model.  This object sets the selection for convection correlations in a global way. The Zone Inside Convection Algorithm input field in the Zone object may be used to selectively override this value on a zone-by-zone basis. Further, individual surfaces can refine the choice by each surface or surface lists – see  object SurfaceProperty:ConvectionCoefficients and object SurfaceProperty:ConvectionCoefficients:MultipleSurface.
-
-#### Field: Algorithm
-
-The model specified in this field is the default algorithm for the inside face all the surfaces.. The key choices are **Simple**, **TARP**, **CeilingDiffuser**, and **AdaptiveConvectionAlgorithm**.
-
-The **Simple** model applies constant heat transfer coefficients depending on the surface orientation.
-
-The **TARP** model correlates the heat transfer coefficient to the temperature difference for various orientations. This model is based on flat plate experiments.
-
-The **CeilingDiffuser** model is a mixed and forced convection model for ceiling diffuser configurations. The model correlates the heat transfer coefficient to the air change rate for ceilings, walls and floors. These correlations are based on experiments performed in an isothermal room with a cold ceiling jet. To avoid discontinuities in surface heat transfer rate calculations, all of correlations have been extrapolated beyond the lower limit of the data set (3 ACH) to a natural convection limit that is applied during the hours when the system is off.
-
-The **AdaptiveConvectionAlgorithm** model is an dynamic algorithm that organizes a large number of different convection models and automatically selects the one that best applies.  The adaptive convection algorithm can also be customized using the SurfaceConvectionAlgorithm:Inside:AdaptiveModelSelections input object.  These models are explained in detail in the EnergyPlus Engineering Reference Document.
-
-The default is **TARP**.
-
-IDF Example:
-
-
-```idf
-SurfaceConvectionAlgorithm:Inside,TARP;
-```
-
-
-### SurfaceConvectionAlgorithm:Outside
-
-Various exterior convection models may be selected for global use.  The optional Zone Outside Convection Algorithm input field in the Zone object may be used to selectively override this value on a zone-by-zone basis. Further, individual surfaces can refine the choice by each surface or surface lists – see  object SurfaceProperty:ConvectionCoefficients and object SurfaceProperty:ConvectionCoefficients:MultipleSurface.
-
-#### Field: Algorithm
-
-The available key choices are **SimpleCombined**, **TARP**, **MoWiTT**, **DOE-2**, and **AdaptiveConvectionAlgorithm**.
-
-The **Simple** convection model applies heat transfer coefficients depending on the roughness and windspeed. This is a combined heat transfer coefficient that includes radiation to sky, ground, and air. The correlation is based on Figure 1, Page 25.1 (Thermal and Water Vapor Transmission Data), 2001 ASHRAE Handbook of Fundamentals. Note that if **Simple** is chosen here or in the Zone field and a SurfaceProperty:ConvectionCoefficients object attempts to override the caulcation with a different choice, the action will still be one of combined calculation. To change this, you must select one of the other methods for the global default.
-
-All other convection models apply heat transfer coefficients depending on the roughness, windspeed, and terrain of the building’s location. These are *convection only* heat transfer coefficients; radiation heat transfer coefficients are calculated automatically by the program.
-
-The **TARP** algorithm was developed for the TARP software and combines natural and wind-driven convection correlations from laboratory measurements on flat plates.
-
-The **DOE-2** and **MoWiTT** were derived from field measurements. DOE-2 uses a correlation from measurements by Klems and Yazdanian for rough surfaces. MoWitt uses a correlation from measurements by Klems and Yazdanian for smooth surfaces and, therefore, is most appropriate for windows (see SurfaceProperty:ConvectionCoefficients:MultipleSurface for how to apply to only windows).
-
-The **AdaptiveConvectionAlgorithm** model is an dynamic algorithm that organizes a large number of different convection models and automatically selects the one that best applies.  The adaptive convection algorithm can also be customized using the SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections input object.  All algorithms are described more fully in the Engineering Reference.
-
-The default is **DOE-2**.
-
-Note that when the surface is wet (i.e. it is raining and the surface is exposed to wind) then the convection coefficient appears as a very large number (1000) and the surface is exposed to the Outdoor Wet-bulb Temperature rather than the Outdoor Dry-bulb Temperature.
-
-IDF Example:
-
-
-```idf
-SurfaceConvectionAlgorithm:Outside, AdaptiveConvectionAlgorithm;
-```
-
-
-### HeatBalanceAlgorithm
-
-The HeatBalanceAlgorithm object provides a way to select what type of heat and moisture transfer algorithm will be used for calculating the performance of the building’s surface assemblies.  This input controls the overall algorithm used for all the surfaces unless one or more of the SurfaceProperty:HeatTransferAlgorithm:\* objects are used to alter the selection for particular surfaces.
-
-#### Field: Algorithm
-
-Four values are allowed to select which solution will be used.
-
-- The **ConductionTransferFunction** selection is a sensible heat only solution and does not take into account moisture storage or diffusion in the construction elements.
-
-- The **MoisturePenetrationDepthConductionTransferFunction** selection is a sensible heat diffusion and an inside surface moisture storage algorithm that also needs additional moisture material property information. Sometimes, this is referred to as the Effective Moisture Penetration Depth or EMPD. See the moisture material property object for additional information and description of outputs:
-
-- MaterialProperty:MoisturePenetrationDepth:Settings
-
-- **Advanced/Research usage:**The **ConductionFiniteDifference** selection is a sensible heat only solution and does not take into account moisture storage or diffusion in the construction elements. This solution technique uses a 1-D finite difference solution in the construction elements. Outputs for the surfaces are described with the material property objects. The Conduction Finite Difference (aka CondFD) property objects are:
-
-- MaterialProperty:PhaseChange
-
-- MaterialProperty:VariableThermalConductivity
-
-- **Advanced/Research usage:** The **CombinedHeatAndMoistureFiniteElement** is a coupled heat and moisture transfer and storage solution. The solution technique uses a one dimensional finite difference solution in the construction elements and requires further materialproperties described in the Heat and Moisture Transfer material properties objects. Outputs from the algorithm are described with these objects. The Heat and Moisture Transfer property objects are:
-
-- MaterialProperty:HeatAndMoistureTransfer:Settings
-
-- MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm
-
-- MaterialProperty:HeatAndMoistureTransfer:Suction
-
-- MaterialProperty:HeatAndMoistureTransfer:Redistribution
-
-- MaterialProperty:HeatAndMoistureTransfer:Diffusion
-
-- MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity
-
-#### Field: Surface Temperature Upper Limit
-
-This field is a bit “advanced�.  It should only be used when the simulation fails AND you cannot determine a cause for the failure.  That is, you receive an error similar to:
-
-```
-   ** Severe  ** Temperature out of bounds (202.91) for surface=Wall1
-   **   ~~~   ** in Zone=Zone01
-   **   ~~~   **  Occurrence info=NEW YORK CITY NY SUMMER, 07/21 16:00 - 16:01
-   **   ~~~   ** A temperature out of bounds problem can be caused by several things.  The user
-   **   ~~~   ** should check the weather environment, the level of internal gains with respect
-   **   ~~~   ** to the zone, and the thermal properties of their materials among other things.
-   **   ~~~   ** A common cause is a building with no thermal mass -- all materials with
-   **   ~~~   ** Regular-R definitions.
-```
-
-And, after careful perusal, you cannot find a solution as suggested in the error description. You may then want to enter a higher number than the default for this field.
-
-#### Field: Minimum Surface Convection Heat Transfer Coefficient Value
-
-This optional field is used to set an overall minimum for the value of the coefficient for surface convection heat transfer (Hc) in W/m2-K.  A minimum is necessary for numerical robustness because some correlations for Hc can result in zero values and create numerical problems.   This field can be used to support specialized validation testing to suppress convection heat transfer and to investigate the implications of different minimum Hc values. The default is 0.1.
-
-#### Field: Maximum Surface Convection Heat Transfer Coefficient Value
-
-This optional field is used to set an overall maximum for the value of the coefficient for surface convection heat transfer (Hc) in W/m2-K.   High Hc values are used in EnergyPlus to approximate fixed surface temperature boundary conditions. This field can be used to alter the accepted range of user-defined Hc values.
-
-And, a default IDF example
-
-HeatBalanceAlgorithm,ConductionTransferFunction;   ! Solution Algorithm
-
-### HeatBalanceSettings:ConductionFiniteDifference
-
-This object is used to control the behavior of the Conduction Finite Difference algorithm for surface heat transfer.  The settings are global and affect how the model behaves for all the surfaces.
-
-#### Field: Difference Scheme
-
-This field determines the solution scheme used by the Conduction Finite Difference model.  There are two options CrankNicholsonSecondOrder and FullyImplicitFirstOrder.  The CrankNicholsonSecondOrder scheme is second order in time and may be faster.  But it can be unstable over time when boundary conditions change abruptly and severely.  The FullyImplicitFirstOrder scheme is first order in time and is more stable over time. But it may be slower. The default is FullyImplicitFirstOrder when ConductionFiniteDifference is selected as the Heat Balance Algorithm.
-
-#### Field: Space Discretization Constant
-
-This field controls the how the model determines spatial discretization, or the count of nodes across each material layer in the construction.  The model calculates the nominal distance associated with a node, <span>\(\Delta x\)</span>, using
-
-<div>\[\Delta x = \sqrt {C\alpha \Delta t} \]</div>
-
-Where
-
-<span>\(\alpha \)</span>is the thermal diffusivity of the material layer, in m<sup>2</sup>/s
-
-<span>\(\Delta t\)</span>is the length of the timestep in seconds.
-
-*C* is a constant set by this field.
-
-The default is 3.  Typical values are from 1 to 3.  Lower values for this constant lead to more nodes and finer-grained space discretization.
-
-#### Field: Relaxation Factor
-
-The finite difference solver includes under-relaxation for improved stability for interactions with the other surfaces. This input field can optionally be used to modify the starting value for the relaxation factor.  Larger numbers may solve faster, while smaller numbers may be more stable.  The default is 1.0.  If the program detects numerical instability, it may reduce the value entered here to something lower and more stable.
-
-#### Field: Inside Face Surface Temperature Convergence Criteria
-
-The surface heat balance model at the inside face has a numerical solver that uses a convergence parameter for a maximum allowable differences in surface temperature.  This field can optionally be used to modify this convergence criteria.  The default value is 0.002 and was selected for stability.  Lower values may further increase stability at the expense of longer runtimes, while higher values may decrease runtimes but lead to possible instabilities.  The units are in degrees Celsius.
-
-An example IDF object follows.
-
-
-
-```idf
-  HeatBalanceSettings:ConductionFiniteDifference,
-    FullyImplicitFirstOrder , !- Difference Scheme
-    3.0 ,  !- Space Discretization Constant
-    1.0,   !- Relaxation Factor
-    0.002 ;!- Inside Face Surface Temperature Convergence Criteria
-```
-
-
-### ZoneAirHeatBalanceAlgorithm
-
-The ZoneAirHeatBalanceAlgorithm object provides a way to select what type of solution algorithm will be used to calculate zone air temperatures and humidity ratios. This object is an optional object. If the default algorithm is used, this object is not required in an input file.
-
-#### Field: Algorithm
-
-Three choices are allowed to select which solution algorithm will be used. The **ThirdOrderBackwardDifference** selection is the default selection and uses the third order finite difference approximation to solve the zone air energy and moisture balance equations. The **AnalyticalSolution** selection uses the integration approach to solve the zone air energy and moisture balance equations. The **EulerMethod** selection uses the first order finite backward difference approximation to solve the zone air energy and moisture balance equations.
-
-And, a default IDF example is shown below:
-
-ZoneAirHeatBalanceAlgorithm, ThirdOrderBackwardDifference;   !- Algorithm
-
-### ZoneAirContaminantBalance
-
-The ZoneAirContaminantBalance object provides a way to select which contaminant type will be simulated. `Although carbon dioxide is not considered as an indoor contaminant but it is used as an indicator of indoor air quality in buildings. From modeling point of view EnergyPlus treats carbon dioxide as a type of contaminant. In addition to carbon dioxide, a generic contaminant type model was also added. `This object is optional, only required in the input data file if the user wishes to model contaminant concentration levels as part of their simulation.
-
-#### Field: Carbon Dioxide Concentration
-
-Input is Yes or No. The default is No. If Yes, simulation of carbon dioxide concentration levels will be performed. If No, simulation of carbon dioxide concentration levels will not be performed.
-
-#### Field: Outdoor Carbon Dioxide Schedule Name
-
-This field specifies the name of a schedule that contains outdoor air carbon dioxide level values in units of ppm. One source of monthly average CO<sub>2</sub> levels in the atmosphere is available at a NOAA ftpsite as .
-
-#### Field: Generic Contaminant Concentration
-
-Input is Yes or No. The default is No. If Yes, simulation of generic contaminant concentration levels will be performed. If No, simulation of generic contaminant concentration levels will not be performed.
-
-#### Field: Outdoor Generic Contaminant Schedule Name
-
-This field specifies the name of a schedule that contains outdoor air generic contaminant level values in units of ppm.
-
-
-
-An IDF example:
-
-```idf
-ZoneAirContaminantBalance,
-  Yes,                       !- Carbon Dioxide Concentration
-  Outdoor CO2 Schedule,      !- Outdoor Carbon Dioxide Schedule Name
-  Yes,                       !- Generic Contaminant Concentration
-  Generic Contaminant Schedule; !- Outdoor Generic Contaminant Schedule Name
-```
-
-
-
-
-### Carbon Dioxide Outputs
-
-The following output variables are available when Carbon Dioxide Concentration = Yes.
-
-HVAC,Average,Zone Air CO2 Internal Gain Volume Flow Rate
-
-HVAC,Average,Zone Air CO2 Concentration [ppm]
-
-#### Zone Air CO2 Concentration [ppm]
-
-This output variable represents the carbon dioxide concentration level in parts per million (ppm) for each zone. This is calculated and reported from the Correct step in the Zone Air Contaminant Predictor-Corrector module.
-
-#### Zone Air CO2 Internal Gain Volume Flow Rate [m3/s]
-
-This is the rate of carbon dioxide added to a zone from all types of sources or sinks, in m<sup>3</sup>/s.
-
-### Generic Contaminant Outputs
-
-The following output variable is available when Generic Contaminant Concentration = Yes.
-
-HVAC,Average,Zone Generic Air Contaminant Generation Volume Flow Rate [m3/s]
-
-HVAC,Average,Zone Air Generic Air Contaminant Concentration [ppm]
-
-#### Zone Air Generic Air Contaminant Concentration [ppm]
-
-This output variable represents the generic contaminant concentration level in parts per million (ppm) for each zone. This is calculated and reported from the Correct step in the Zone Air Contaminant Predictor-Corrector module.
-
-#### Zone Generic Air Contaminant Generation Volume Flow Rate [m3/s]
-
-This is the rate of generic air contaminant added (or subtracted) to a zone from all types of sources or sinks.
-
-### ShadowCalculation
-
-This object is used to control some details of EnergyPlus’s solar, shadowing and daylighting models. There are two basic methods available for the calculations. In order to speed up the calculations, shadowing calculations (sun position, etc.) for the default method are performed over a period of days. Note that this value may be very important for determining the amount of sun entering your building and by inference the amount of cooling or heating load needed for maintaining the building. Though termed “shadowing� calculations, it in affect determines the sun position for a particular day in a weather file period simulation. (Each design day will use the date of the design day object). Even though weather file data contains the amount of solar radiation, the internal calculation of sun position will govern how that affects various parts of the building. By default, the calculations are done for every 20 days throughout a weather run period; an average solar position is chosen and the solar factors (such as sunlit areas of surfaces) remain the same for that number of days. When more integrated calculations are needed for controlling dynamic windows or shades, a secod method is available where solar calculations are performed at each zone timestep.
-
-#### Field: Calculation Method
-
-This field is used to control how the solar, shading, and daylighting models are calculated with respect to the time of calculations during the simulation.  The default and fastest method is selected using the keyword AverageOverDaysInFrequency.  A more detailed and slower method can be selected using the keyword DetailedTimestepIntegration.  The later method is useful modeling dynamic fenestration and shading surfaces.
-
-#### Field: Calculation Frequency
-
-This numeric field will cause the shadowing calculations to be done periodically using the number in the field as the number of days in each period. This field is only used if the default method AverageOverDaysInFrequency is used in the previous field. Using this field will allow you to synchronize the shadowing calculations with changes in shading devices. Using the default of 20 days in each period is the average number of days between significant changes in solar position angles. For these shadowing calculations, an “average� (over the time period) of solar angles, position, equation of time are also used.
-
-#### Field: Maximum Figures in Shadow Overlap Calculations
-
-This numeric field will allow you to increase the number of figures in shadow overlaps. Due to the shadowing algorithm, the number of shadows in a figure may grow quite large even with fairly reasonable looking structures. Of course, the inclusion of more allowed figures will increase calculation time.  Likewise, too few figures may not result in as accurate calculations as you desire.
-
-#### Field: Polygon Clipping Algorithm
-
-This is an advanced feature. Prior to V7, the internal polygon clipping method was a special case of the Weiler-Atherton method. Now, two options are available: **SutherlandHodgman** (default) and **ConvexWeilerAtherton**. Theoretically, Sutherland-Hodgman is a simpler algorithm but it works well in cases where receiving surfaces (of shadows) are non-convex. The Weiler-Atherton implementation is only accurate where both casting and receiving surfaces are convex. Warnings/severe errors are displayed when necessary. More details on polygon clipping are contained in the Engineering Reference.
-
-#### Field: Sky Diffuse Modeling Algorithm
-
-Two choices are available here: SimpleSkyDiffuseModeling and DetailedSkyDiffuseModeling. **SimpleSkyDiffuseModeling** (default) performs a one-time calculation for sky diffuse properties. This has implications if you have shadowing surfaces with changing transmittance (i.e. not all opaque or not all transparent) during the year. The program checks to see if this might be the case and automatically selects **DetailedSkyDiffuseModeling** if the shading transmittance varies. Even if the transmittance doesn’t vary and the option for detailed modeling is used, that option is retained (though it will increase execution time) because you may be using EMS to vary the transmittance. When the detailed modeling is done, there will be a warning posted if the Calculation Frequency (above) is &gt; 1.
-
-In general (and you should also read the previous field description), if shadowing surfaces are used with the transmittance property, the user should be careful to synchronize this calculation with the scheduled occurrence of the transmittance (if any) (or use 1, which will be the most accurate but will cause more time in the calculations).
-
-This field applies to the method called “AverageOverDaysInFrequency.�  When the method called “DetailedTimestepIntegration� is used the diffuse sky modeling always uses DetailedSkyDiffuseModeling.
-
-Examples of this object in IDF: (note this object must be unique in an IDF)
-
-```idf
-ShadowCalculation,AverageOverDaysInFrequency,1;
-
-
-ShadowCalculation, AverageOverDaysInFrequency, 1, , SutherlandHodgman, DetailedSkyDiffuseModeling;
-```
-
-Note that the use of “1� in the examples is NOT the same as using DetailedTimestepIntegration – “1� causes daily calculation of the sun position variables but does not change the shadowing calculations more frequently than daily.
-
-### Output:Diagnostics
-
-Sometimes, messages only confuse users – especially new users. Likewise, sometimes certain output variables exist for only a certain condition but some take them at face value/name. Some features may be very important but under certain instances cause problems. Thus, we have added the **diagnostic output** object to be able to turn on or off certain messages, variables, and features depending on conditions.
-
-Both fields of the Output:Diagnostics command can accept all the applicable keys. More than one object may be entered.
-
-#### Field: key1, key2
-
-Allowable choices are:
-
-**DisplayAllWarnings** – use this to get all warnings (except the developer warnings “DisplayZoneAirHeatBalanceOffBalance�).  This key sets all other display warning values to on.
-
-**DisplayExtraWarnings** – use this to get all extra warnings. An example of an extra warning is when a user enters a ceiling height or volume with the Zone object and EnergyPlus calculates something significantly different based on the entered zone geometry.
-
-**DisplayUnusedSchedules** – use this to have the unused schedules (by name) listed at the end of the simulation.
-
-**DisplayUnusedObjects** – use this to have unused (orphan) objects (by name) listed at the end of the simulation.
-
-**DisplayAdvancedReportVariables** – use this to be able to use certain advanced output variables where the name may be misleading and you need to understand the concepts or reasons for use. If you put in this field, then you will be able to report on these features. They are noted in the descriptions of objects or output variables.
-
-**DisplayZoneAirHeatBalanceOffBalance** – this is a developer diagnostic which you can turn on, if you desire.
-
-**DoNotMirrorDetachedShading** – use this to turn off the automatic mirroring of detached shading surfaces. These surfaces are automatically mirrored so that the user does not need to worry about facing direction of the surface and the shading surface will shade the building as appropriate. Note that Shading:Zone:Detailed surfaces are also mirrored and there is no way to turn that “off�.
-
-**DisplayWeatherMissingDataWarnings** – use this to turn on the missing data warnings from the read of the weather file.
-
-**ReportDuringWarmup** – use this to allow reporting during warmup days. This can show you exactly how your facility is converging (or not) during the initial “warmup� days of the simulation.  Generally, only developers or expert simulation users would need this kind of detail.
-
-**ReportDetailedWarmupConvergence** – use this to produce detailed reporting (essentially each warmup day for each zone) for warmup convergence.
-
-**ReportDuringHVACSizingSimulation** – use this to allow controlling reporting to SQLite database during sizing period simulations done for HVAC Sizing Simulation.  The regular reporting is done in the usual way. This can show details of how advanced sizing adjustments were determined by documenting how the systems operated when doing the intermediate sizing periods.  Depending on the number of iterations performed for HVAC Sizing Simulation, there will be a number of sets of results with each set containing all the Sizing Periods.
-
-In IDF use:
-
-```idf
-Output:Diagnostics,
-  DisplayExtraWarnings;
-```
-
-
-### Output:DebuggingData
-
-There may be times when a particular input file requires additional debugging. The Output:DebuggingData object may be used to report all available node data (e.g., temperature, mass flow rate, set point, pressure, etc.). The debug data is reported to the DBG text file. The debug file first reports the node number and name, and then all available node information for each zone time step (Ref. Timestep).
-
-The 2 fields of the Output:DebuggingData object can accept either a 1 (turn on) or any other value (turn off). Only one object may be entered.
-
-#### Field: Report Debugging Data
-
-This field turns on debug reporting when a value of 1 is entered. Any other value (usually 0) disables debug reporting.
-
-#### Field: Report During Warmup
-
-This field allows the debug data to be reported during the warmup period. When a value of 1 is entered the data is reported at all times, even during warmup. Any other value (usually 0) disables “reporting at all time� and debug data is only reported for each environment (RunPeriod or SizingPeriod:DesignDay).
-
-In IDF use:
-
-```idf
-Output:DebuggingData,
-1,1;
-```
-
-
-### Output:PreprocessorMessage
-
-The Output:PreprocessorMessage object can be used by preprocessor programs to EnergyPlus for passing certain conditions/errors that might not be detected by scripts executing the EnergyPlus system of programs. This allows EnergyPlus to intercept problems and terminate gracefully rather than the user having to track down the exact conditions.
-
-There is no reason for a user to enter an Output:PreprocessorMessage object but you should encourage interface developers to use this feature. More than one Output:PreprocessorMessage objects may be entered. Of course, no preprocessor message objects are necessary if there is no error information to be passed.
-
-#### Field: Preprocessor Name
-
-The preprocessor name (e.g. EPMacro, ExpandObjects) is entered here.  Case is retained so that messages from EnergyPlus look very similar to what a preprocessor would produce.
-
-#### Field: Error Severity
-
-This is the error severity. If Fatal, EnergyPlus will terminate after showing all preprocessor messages.
-
-#### Fields: Message Line 1 through Message Line 10
-
-Each line is limited to 100 characters and an appropriate message can be composed.
-
-An IDF Example:
-
-```idf
-Output:PreprocessorMessage,
-   No Preprocessor Used,     !- preprocessor name
-   Information,              !- error severity
-   Illustrative Message,     !- message line 1
-   No problems for processing;  !- message line 2
-```
-
-
-And would appear in output:
-
-```
-Preprocessor="No Preprocessor Used" has the following Information messages:
-Illustrative Message
-No problems for processing
-```
-
-### ZoneCapacitanceMultiplier:ResearchSpecial
-
-This object is an advanced feature that can be used to control the effective storage capacity of the zone.  Capacitance multipliers of 1.0 indicate the capacitance is that of the (moist) air in the volume of the specified zone. This multiplier can be increased if the zone air capacitance needs to be increased for stability of the simulation or to allow modeling higher or lower levels of damping of behavior over time. The multipliers are applied to the base value corresponding to the total capacitance for the zone’s volume of air at current zone (moist) conditions.
-
-#### Field: Temperature Capacity Multiplier
-
-This field is used to alter the effective heat capacitance of the zone air volume. This affects the transient calculations of zone air temperature. Values greater than 1.0 have the effect of smoothing or damping the rate of change in the temperature of zone air from timestep to timestep.  Note that sensible heat capacity can also be modeled using internal mass surfaces.
-
-#### Field: Humidity Capacity Multiplier
-
-This field is used to alter the effective moisture capacitance of the zone air volume.  This affects the transient calculations of zone air humidity ratio.  Values greater than 1.0 have the effect of smoothing, or damping, the rate of change in the water content of zone air from timestep to timestep.
-
-#### Field: Carbon Dioxide Capacity Multiplier
-
-This field is used to alter the effective carbon dioxide capacitance of the zone air volume. This affects the transient calculations of zone air carbon dioxide concentration.  Values greater than 1.0 have the effect of smoothing or damping the rate of change in the carbon dioxide level of zone air from timestep to timestep.
-
-#### Field: Generic Contaminant Capacity Multiplier
-
-This field is used to alter the effective generic contaminantcapacitance of the zone air volume. This affects the transient calculations of zone air generic contaminantconcentration.  Values greater than 1.0 have the effect of smoothing or damping the rate of change in the generic contaminantlevel of zone air from timestep to timestep.
-
-### SimulationControl
-
-The input for SimulationControl allows the user to specify what kind of calculations a given EnergyPlus simulation will perform. For instance the user may want to perform one or more of the sizing calculations but not proceed to an annual weather file simulation. Or the user might have all flow rates and equipment sizes already specified and  desire an annual weather without any preceding sizing calculations. Sizing runs, even for large projects, are quickly run – they do not add much to the overall simulation time. The SimulationControl input allows all permutations of run selection by means of 5 yes/no inputs.
-
-Only one SimulationControl object is permitted for each EnergyPlus input file. While a SimulationControl is needed to trigger sizing calculations, it is optional for other runs (design days, run periods). The actions will still be shown in the eplusout.eio file (see Output Details and Examples Document).
-
-#### Field: Do Zone Sizing Calculation
-
-Input is Yes or No. The default is No. Zone Sizing (see Sizing:Zone object) performs a special calculation, using a theoretical ideal zonal system, and determines the zone design heating and cooling flow rates and loads, saving the results in the zone sizing arrays.
-
-#### Field: Do System Sizing Calculation
-
-Input is Yes or No. The default is No. System Sizing (see Sizing:System object) also performs a special calculation that, to oversimplify, sums up the results of the zone sizing calculation and saves the results in the system sizing arrays for reporting on component size requirements. Thus, in order to perform the system sizing calculations, the zone sizing arrays need to be filled and hence the zone sizing calculations must be performed in the same run. (This requirement is enforced by the program).
-
-#### Field: Do Plant Sizing Calculation
-
-Input is Yes or No. The default is No. Unlike Zone and System Sizing, Plant Sizing does not use the Zone or System sizing arrays. Plant Sizing uses the Sizing:Plant object fields and data on the maximum component flow rates. The data on component (such as coil) flow rates is saved and made available to the Plant code whether or not component autosizing is performed and whether or not zone sizing and/or system sizing is performed. Therefore, you can specify Plant Sizing without also specifying to do Zone Sizing or System Sizing calculations.
-
-#### Field: Run Simulation for Sizing Periods
-
-Input is Yes or No. The default is Yes. Yes implies that the simulation will be run on all the included SizingPeriod objects (i.e., SizingPeriod:DesignDay, SizingPeriod:WeatherFileDays, and SizingPeriod:WeatherFileConditionType). Note that each SizingPeriod object constitutes an “environment� and warmup convergence (see earlier topic under the Building object) will occur for each.
-
-#### Field: Run Simulation for Weather File Run Periods
-
-Input is Yes or No. The default is Yes. Yes implies the simulation will be run on all the included RunPeriod objects. Note that each RunPeriod object constitutes an “environment� and warmup convergence (see earlier topic under the Building object) will occur for each.
-
-#### Field: Do HVAC Sizing Simulation for Sizing Periods
-
-This field is optional.  It can be used to enable certain advanced sizing calculations that rely on simulating the sizing periods to collect information.  This is currently only applicable when sizing plant loops using the sizing option called Coincident.
-
-#### Field: Maximum Number of HVAC Sizing Simulation Passes
-
-This field is optional and is only used if the previous field is set to Yes.  The HVAC Sizing Simulation approach can use iteration to improve sizing calculations.  Each iteration is a Sizing Pass.  This field is used to manually place an upper limit the number of passes that the sizing algorithms can use.  
-
-An IDF example:
-
-```idf
-  SimulationControl,
-    No,                      !- Do Zone Sizing Calculation
-    No,                      !- Do System Sizing Calculation
-    No,                      !- Do Plant Sizing Calculation
-    Yes,                     !- Run Simulation for Sizing Periods
-    Yes;                     !- Run Simulation for Weather File Run Periods
-    No,                      !- Do HVAC Sizing Simulation for Sizing Periods
-    2;                       !- Maximum Number of HVAC Sizing Simulation Passes
-```
-
-### ProgramControl
-
-This object is currently disabled. The ProgramControl object can be used to control how the EnergyPlus program executes on the computer.  Portions of EnergyPlus have been programmed to use more than one processor, or CPU core, at the same time during a single simulation.  This multithreading may not be desireable when running more than one simulation at a time on the same computer (because it can actually run more slowly).  This input object is optional and allows controlling the number of threads (or cores, or processors) that EnergyPlus will use so that conflicts can be managed.  When this object is used, its input for the number of threads will take precedent over the value of the environment variable **“EP\_OMP\_NUM\_THREADS�** which is an alternate method of controlling the program’s threading. Since the primary method for OpenMP simulations currently (V7.1 and V7.2) is the interior radiant exchange to solve for inside surface temperatures, EnergyPlus sets the threads to 1 if the nominal number of surfaces is &lt;= 30.
-
-#### Field: Number of Threads Allowed
-
-This field is used to specify a limit on the number of threads EnergyPlus will use.  If a zero is entered then the program will set the number of threads to the maximum available on the computer.  If the number entered is larger than the number of processors or cores, then the hardware limits will take precedent over this limit.
-
-An example IDF object that sets the program to use only one thread follows.
-
-```idf
-  ProgramControl,
-    1 ; !- Number of Threads Allowed
-```
-
-
-### Meter:Custom
-
-A custom meter allows the user to group variables or meters onto a virtual meter that can be used just like a normal meter created by EnergyPlus. For consistency, the items being grouped must all be similar.
-
-#### Field: Name
-
-This is a user defined name for the custom meter. Names for custom meters cannot duplicate internal meter names.
-
-#### Field: Fuel Type
-
-A fuel type should be specified for the meter. All assignments to this meter will be checked to assure that the same fuel type is used. Additionally, this may be used in other objects (such as the Demand Limiting). Valid choices for this field are:
-
-- Electricity
-
-- NaturalGas
-
-- PropaneGas
-
-- FuelOil\#1
-
-- FuelOil\#2
-
-- Coal
-
-- Diesel
-
-- Gasoline
-
-- Water
-
-- Generic
-
-- OtherFuel1
-
-- OtherFuel2
-
-Fuel types are generally self-explanatory. Generic is included for convenience when a custom meter is defined that doesn’t quite fit the “fuel� categories.  See the examples below.
-
-#### Field: group(s) Key Name-Output Variable/Meter Name
-
-The rest of the object is filled with parameters of the key name/output variable or meter names. When a meter name is used, the key name field is left blank.
-
-#### Field: Key Name \#
-
-A key name field is used when the following field specifies an output variable. If the field is left blank, then all the output variables in the following field are assigned to the meter.
-
-#### Field: Output Variable or Meter Name \#
-
-This field must be a valid output variable name or a valid meter name.
-
-### Meter:CustomDecrement
-
-The decrement custom meter is very similar to the custom meter specification but additionally allows a predefined meter to be used as the “source� meter and the remaining items subtract from that predefined meter.
-
-#### Field: Name
-
-This is a user defined name for the custom meter. Names for custom meters cannot duplicate internal meter names.
-
-#### Field: Fuel Type
-
-A fuel type should be specified for the meter. All assignments to this meter will be checked to assure that the same fuel type is used. Additionally, this may be used in other objects (such as the Demand Limiting). Valid choices for this field are:
-
-- Electricity
-
-- NaturalGas
-
-- PropaneGas
-
-- FuelOil\#1
-
-- FuelOil\#2
-
-- Coal
-
-- Diesel
-
-- Gasoline
-
-- Water
-
-- Generic
-
-- OtherFuel1
-
-- OtherFuel2
-
-#### Field: Source Meter Name
-
-This name specifies the meter that will be used as the main source for the decrement custom meter. The remainder of the fields are subtracted from the value of this meter to create the meter value named above. The Source Meter is not changed in any way by including this custom meter.
-
-#### Field: group(s) Key Name-Output Variable/Meter Name
-
-The rest of the object is filled with parameters of the key name/output variable or meter names. When a meter name is used, the key name field is left blank.
-
-#### Field: Key Name \#
-
-A key name field is used when the following field specifies an output variable. If the field is left blank, then all the output variables in the following field are assigned to the meter.
-
-#### Field: Output Variable or Meter Name \#
-
-This field must be a valid output variable name or a valid meter name. Additionally, it must be contained on the Source Meter. Note that, if an error occurs, only the Variable in error will show – confusing things if what was entered was a meter name.
-
-### Custom Meter Examples
-
-Details of the Meter:Custom/Meter:CustomDecrement are shown on the Meter Details file.
-
-In the following examples, the custom meters are set up to illustrate the capabilities of custom meters. Custom meter “**MyGeneralLights**� duplicates the InteriorLights:Electricity meter. Custom meter “**MyBuildingElectric**� duplicates the Electricity:Building meter (by specifying that meter). Custom Meter (Decrement) “**MyBuildingOther**� uses the Electricity:Building meter as the source meter and subtracts out the values for MyGeneralLights (aka InteriorLights:Electricity). The resultant value for the MyBuildingOther meter should be equal to the value for the meters Electricity:Building – InteriorLights:Electricity.
-
-
-
-```idf
-Meter:Custom,
-    MyGeneralLights,         !- Name
-    Electricity,             !- Fuel Type
-    SPACE1-1,                !- Key Name 1
-    Lights Electric Energy,  !- Output Variable or Meter Name 1
-    SPACE2-1,                !- Key Name 2
-    Lights Electric Energy,  !- Output Variable or Meter Name 2
-    SPACE3-1,                !- Key Name 3
-    Lights Electric Energy,  !- Output Variable or Meter Name 3
-    SPACE4-1,                !- Key Name 4
-    Lights Electric Energy,  !- Output Variable or Meter Name 4
-    SPACE5-1,                !- Key Name 5
-    Lights Electric Energy;  !- Output Variable or Meter Name 5
-
-
-Meter:Custom,
-    MyBuildingElectric,      !- Name
-    Electricity,             !- Fuel Type
-    ,                        !- Key Name \#1
-    Electricity:Building;    !- Output Variable or Meter Name \#1
-
-
-
-
-Meter:CustomDecrement,
-    MyBuildingOther,         !- Name
-    Electricity,             !- Fuel Type
-    Electricity:Building,    !- Source Meter Name
-    ,                        !- Key Name \#1
-    MyGeneralLights;         !- Output Variable or Meter Name \#1
-```
-
-
-
-
-For an example of “generic� fuel type, one might put the Building Infiltration Heat Loss & Heat Gain on a set of custom meters:
-
-```idf
-  Meter:Custom,
-    Building Infiltration Heat Loss,  !- Name
-    Generic,             !- Fuel Type
-    *,                       !- Key Name 1
-    Zone Infiltration Total Heat Loss Energy;  !- Output Variable Name 1
-
-
-  Meter:Custom,
-    Building Infiltration Heat Gain,  !- Name
-    Generic,             !- Fuel Type
-    *,                       !- Key Name 1
-    Zone Infiltration Total Heat Gain Energy;  !- Output Variable Name 1
-```
-
-
-One can then report these values the same way one reports other standard meters.
-
-### Simulation Parameter Outputs
-
-These appear in the **eplusout.eio** file. For details of the reporting, please see the Output Details and Examples document.
-
-Group – Compliance Objects
---------------------------
-
-Not necessarily related directly to simulation, the Compliance Object group provides a repository for a group of objects that can be used directly or indirectly in reporting compliance (such as ASHRAE 90.1) to building standards.
-
-### Compliance:Building
-
-The Compliance:Building object describes parameters related to compliance to building standards, building codes, and beyond energy code programs.
-
-#### Field: Building Rotation for Appendix G
-
-Building Rotation for Appendix G allows for the building model to be rotated for use with compliance such as ASHRAE 90.1 Appendix G. Appendix G requires the building to be rotated 0, 90, 180 and 270 degrees and the values averaged to establish baseline energy use. This input works with relative or world coordinate systems.
-
-An example from an IDF:
-
-```idf
-Compliance:Building,
-    90;                 Building Rotation for Appendix G
-```
-
-
-Group -- Location – Climate – Weather File Access
--------------------------------------------------
-
-This group of objects describes the ambient conditions for the simulation.
-
-### Site:Location
-
-The location class describes the parameters for the building’s location. Only one location is allowed. Weather data file location, if it exists, will override any location data in the IDF. Thus, for an annual simulation, a Location does not need to be entered.
-
-#### Field: Name
-
-This alpha field is used as an identifying field in output reports.
-
-#### Field: Latitude
-
-This field represents the latitude (in degrees) of the facility. By convention, North Latitude is represented as positive; South Latitude as negative. Minutes should be represented in decimal fractions of 60. (15’ is 15/60 or .25)
-
-#### Field: Longitude
-
-This field represents the longitude (in degrees) of the facility. By convention, East Longitude is represented as positive; West Longitude as negative. Minutes should be represented in decimal fractions of 60. (15’ is 15/60 or .25)
-
-#### Field: Time Zone
-
-This field represents the time zone of the facility (relative to Greenwich Mean Time or the 0<sup>th</sup> meridian). Time zones west of GMT (e.g. North America) are represented as negative; east of GMT as positive. Non-whole hours can be represented in decimal (e.g. 6:30 is 6.5).
-
-#### Field: Elevation
-
-This field represents the elevation of the facility in meters (relative to sea level).
-
-Units with their abbreviations are shown in Appendix A.  And, as shown in an IDF:
-
-```idf
-Site:Location, DENVER COLORADO,     ! Name
-   39.75000    ,     ! Latitude {N+ S-}
-  -104.8700    ,     ! Longitude {W- E+}
-  -7.000000    ,     ! TimeZoneNumber {GMT+/-}
-  1610.26;           ! Elevation {m}
-```
-
-
-Most examples in this document include the comment lines that illustrate each data field’s value. However, this is not necessary (though it makes the IDF more readable). The previous example could also be:
-
-```idf
-Site:Location, DENVER COLORADO,39.75,-104.87,-7,1610.26;
-```
-
-
-### SizingPeriod:DesignDay
-
-The design day input describes the parameters to effect a “design day� simulation, often used for load calculations or sizing equipment. Using the values in these fields, EnergyPlus “creates� a complete days’ worth of weather data (air temperatures, solar radiation, etc.)  Normal operation uses the default range multipliers as shown in Figure 6 though users may choose to input their own multiplier schedule. Likewise, normal operation specifies one “humidity indicating condition� which is used to calculate the humidity ratio at maximum temperature – this is used as the constant humidity ratio for the entire day. Again, this can be overridden by specifying a relative humidity schedule or requesting generation of an hourly wet-bulb temperature profile.  Multiple design days may be specified.
-
-We refer you to the ASHRAE Handbook of Fundamentals for philosophy of what parameters are important for use as “design conditions� in sizing equipment.
-
-In the install, the “design day files� are included for the weather file locations that are included (weatherdata folder). All the design day definitions from the ASHRAE design conditions (latest publication date) are included, grouped by WMO region, on the main web site with the weather data. http://www.energyplus.gov/cfm/weather_data.cfm  These files are in “macro� form but it is easy to cut and paste the appropriate definition segments. These files include the location information as well as some locations have **RunPeriodControl:DaylightSavingTime** objects.
-
-#### Field: Name
-
-This field, like the location name, is used simply for reporting and identification. This name must be unique among the SizingPeriod names entered.
-
-#### Field: Month
-
-This numeric field specifies the month. That, in conjunction with the day of the month and location information, determines the current solar position and solar radiation values for each hour of the day.
-
-#### Field: Day of Month
-
-This numeric field specifies the day of the month. That, in conjunction with the month and location information, determines the current solar position and solar radiation values for each hour of the day.
-
-#### Field: Day Type
-
-This alpha field specifies the day type for the design day. This value indicates which day profile to use in schedules. For further information, see the Schedule discussion later in this document. (ref: Schedule)  Note that two of the possible day types are SummerDesignDay (for cooling) and WinterDesignDay (for heating) – allowing the user to customize schedules for the design conditions. That is, for design days tagged with a SummerDesignDay type, you can set schedules to be worst or typical schedules for a cooling season.
-
-#### Field: Maximum Dry-Bulb Temperature
-
-This numeric field should contain the day’s maximum dry-bulb temperature in degrees Celsius. (Reference Appendix A of this document for EnergyPlus standard units and abbreviations). The MacroDataSets design day files show extreme temperature for locations as indicated in the ASHRAE HOF design condition tables.
-
-#### Field: Daily Dry-bulb Temperature Range
-
-A design day can have a “high� temperature and a “low� temperature (or can be a constant temperature for each hour of the day). If there is a difference between high and low temperatures, this field should contain the difference from the high to the low. EnergyPlus, by default, distributes this range over the 24 hours in the day as shown in the figure below:
-
-![](media/image010.svg)
-
-Figure 6. Default Daily range Multiplier for Design Days
-
-The multipliers are taken from the ASHRAE 2009 HOF. More explicitly, EnergyPlus creates an air temperature for each timestep by using the entered maximum dry-bulb temperature in conjunction with the entered daily range and the above multiplier values. The actual equation used is shown below:
-
-<div>\[{T_{current}} = {T_{Max}} - {T_{range}}\cdot {T_{Multiplier}}\]</div>
-
-where
-
-T<sub>current</sub>= Air temperature of current Hour of Day
-
-T<sub>Max</sub>= User supplied Max Dry-bulb Temperature
-
-T<sub>range</sub>= User supplied Daily Temperature Range
-
-T<sub>Multiplier</sub>= Range multiplier as shown on the above graph
-
-The range multiplier values represent typical conditions of diurnal temperatures (i.e. the low temperature for the day occurring about 5:00 AM and the maximum temperature for the day occurring about 3:00 PM.  Note that EnergyPlus does not shift the profile based on the time of solar noon as is optionally allowed in ASHRAE procedures.
-
-ASHRAE research indicates that dry-bulb and wet-bulb temperatures typically follow the same profile, so EnergyPlus can use the default profile to generate humidity conditions (see Humidity Indicating Type = WetBulbProfileDefaultMultipliers below).
-
-#### Field: Dry-Bulb Temperature Range Modifier Type
-
-If you are happy with lows at 5am and highs at 3pm, you can ignore this field. If you want to specify your own temperature range multipliers (see earlier discussion at the Temperature Range field description), you can specify a type here and create a day schedule which you reference in the next field.
-
-If you specify **MultiplierSchedule** in this field, then you need to create a day schedule that specifies a multiplier applied to the temperature range field (above) to create the proper dry-bulb temperature range profile for your design day.
-
-If you specify **DifferenceSchedule** in this field, then you need to create a day schedule that specifies a number to be **subtracted** from dry-bulb maximum temperature for each timestep in the day. Note that numbers in the delta schedules cannot be negative as that would result in a higher maximum than the maximum previously specified.
-
-If you specify **TemperatureProfileSchedule** in this field, then you need to create a day schedule that specifies the actual dry-bulb temperatures throughout the day. You will not need to include a Maximum Dry-Bulb Temperature in that field.
-
-If you leave this field blank or enter **DefaultMultipliers**, then the default multipliers will be used as shown in the “temperature range� field above.
-
-#### Field: Dry-Bulb Temperature Range Modifier Day Schedule Name
-
-This field is the name of a **day schedule** (ref. Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List objects) with the values as specified in the Dry-Bulb Temperature Range Modifier Type field above.
-
-#### Field: Humidity Condition Type
-
-The values/schedules indicated here and in subsequent fields create the humidity values in the 24 hour design day conditions profile. Valid choices here are: **WetBulb**, **Dewpoint**, **WetBulbProfileDefaultMultipliers, WetBulbProfileDifferenceSchedule,** **WetBulbProfileMultiplierSchedule**, **HumidityRatio**, **Enthalpy**, and **Schedule.**
-
-The Humidity Condition Type fields have interacting uses and units, summarized as follows:
-
-Table 2. Humidity Indicating Field Interactions - Design Day
-
-<table class="table table-striped">
-<tr>
-<th>Humidity Condition Type</th>
-<th>Primary Humidity Indicating Field</th>
-<th>Humidity Indicating Day Schedule</th>
-</tr>
-<tr>
-<td>WetBulb</td>
-<td>Wetbulb or DewPoint at Maximum Dry-Bulb</td>
-<td>N/A (unused)</td>
-</tr>
-<tr>
-<td>DewPoint</td>
-<td>Wetbulb or DewPoint at Maximum Dry-Bulb</td>
-<td>N/A (unused)</td>
-</tr>
-<tr>
-<td>HumidityRatio</td>
-<td>Humidity Ratio at Maximum Dry-Bulb</td>
-<td>N/A (unused)</td>
-</tr>
-<tr>
-<td>Enthalpy</td>
-<td>Enthalpy at Maximum Dry-Bulb</td>
-<td>N/A (unused)</td>
-</tr>
-<tr>
-<td>WetBulbProfileDefaultMultipliers</td>
-<td>Wetbulb or DewPoint at Maximum Dry-Bulb</td>
-<td>N/A (unused)</td>
-</tr>
-<tr>
-<td>WetBulbProfileMultiplierSchedule</td>
-<td>Wetbulb or DewPoint at Maximum Dry-Bulb</td>
-<td>Fractions of wet-bulb daily range (0 – 1)</td>
-</tr>
-<tr>
-<td>WetBulbProfileDifferenceSchedule</td>
-<td>Wetbulb or DewPoint at Maximum Dry-Bulb</td>
-<td>Difference between maximum and hour/timestep wet-bulb temperature, C</td>
-</tr>
-<tr>
-<td>RelativeHumiditySchedule</td>
-<td>N/A</td>
-<td>Relative humidity (%, 0 – 100)</td>
-</tr>
-</table>
-
-Humidity conditions over the day are derived as follows:
-
-**WetBulb, DewPoint, HumidityRatio, or Enthalpy**:
-
-These four methods assume constant absolute humidity over the day.  Calculate W = humidity ratio at Maximum Dry-Bulb Temperature and Humidity Indicating Conditions.  Derive hourly/timestep humidity conditions from W and hour/timestep dry-bulb temperature.
-
-**WetBulbProfileDefaultMultipliers**
-
-Generate the wet-bulb temperature profile using Default Daily Range Multiplier for Design Days (shown in Figure 6 above) and Daily Wet-Bulb Temperature Range (below).  This method is analogous to DefaultMultiplier generation of the dry-bulb temperature profile and is the procedure recommended in Chapter 14 of ASHRAE 2009 HOF.
-
-**WetBulbProfileMultiplierSchedule**
-
-Generate the wet-bulb profile using multipliers from the Humidity Indicating Day Schedule and Daily Wet-Bulb Temperature Range (below).  Analogous to dry-bulb MultiplierSchedule.
-
-**WetBulbProfileDifferenceSchedule**
-
-Generate the wet-bulb profile by subtracting Humidity Indicating Day Schedule values from the daily maximum wet-bulb temperature (specified in Humidity Indicating Conditions at Maximum Dry-Bulb).  Analogous to dry-bulb DifferenceSchedule.
-
-**RelativeHumiditySchedule**
-
-Hourly relative humidity is specified in Humidity Indicating Day Schedule.
-
-In all cases, the humidity ratio is limited to saturation at the hour/timestep dry-bulb (that is, the dry-bulb temperature is used as specified, but the humidity ratio is modified as needed to be physically possible).  Once a valid air state is determined, a complete set of consistent hour/timestep psychrometric values (dewpoint, wet-bulb, and enthalpy) is derived.
-
-#### Field: Wetbulb or DewPoint at Maximum Dry-Bulb
-
-If you choose **Wetbulb** or **Dewpoint** in the Humidity Condition Type field, then this numeric field should contain that value. Note that this field is unnecessary when you put in a humidity indicating day schedule (described later in this section).
-
-#### Field: Humidity Condition Day Schedule Name
-
-Allows specification a day schedule (ref. Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List objects) of values for relative humidity or wet-bulb profile per Humidity Indicating Type field.
-
-#### Field: Humidity Ratio at Maximum Dry-Bulb
-
-If **HumidityRatio** is chosen for the Humidity Condition Type field, then this numeric field should contain the desired humidity ratio at maximum dry-bulb temperature (units kg Water / kg Dry Air).
-
-#### Field: Enthalpy at Maximum Dry-Bulb
-
-If **Enthalpy** is chosen for the Humidity Condition Type field, then this numeric field should contain the desired enthalpy at maximum dry-bulb temperature (units Joules /kg).
-
-#### Field: Daily Wet-Bulb Temperature Range
-
-The difference between the maximum and minimum wet-bulb temperatures on the design day (Celsius).  Used for generating daily profiles of humidity conditions when Humidity Condition Type field (above) is **WetBulbProfileDefaultMultipliers** or **WetBulbProfileMultiplierSchedule**.  Values for wet-bulb temperature range are tabulated by month for 5564 locations worldwide on the CD that accompanies the ASHRAE 2009 HOF.
-
-#### Field: Barometric Pressure
-
-This numeric field is the constant barometric pressure (Pascals) for the entire day.
-
-#### Field: Wind Speed
-
-This numeric field is the wind speed in meters/second (constant throughout the day) for the day. The MacroDataSets design day files includes wind speed values (99.6% - heating, 1% cooling) as indicated in ASHRAE HOF design condition tables. But, you should be aware that traditional values for these are 6.7056 m/s (15 mph) for heating and 3.3528 m/s (7 mph) for cooling. A reminder is shown in the comments for the wind speed values. The comments also note the extreme wind speeds from the ASHRAE tables.
-
-#### Field: Wind Direction
-
-This numeric field is the source wind direction in degrees. By convention, winds from the North would have a value of 0., from the East a value of 90.
-
-#### Field: Rain Indicator
-
-This field indicates whether or not the building surfaces are wet. If the value is Yes, then it is assumed that the building surfaces are wet. Wet surfaces may change the conduction of heat through the surface.
-
-#### Field: Snow Indicator
-
-This field indicates whether or not there is snow on the ground. If the value is Yes, then it is assumed there is snow on the ground. Snow on the ground changes the ground reflectance properties.
-
-#### Field: Daylight Saving Time Indicator
-
-This field specifies whether to consider this day to be a Daylight Saving Day. Yes in the field indicates that daylight saving time is operational for this day. Yes essentially adds 1 hour to the scheduling times used in items with schedules.
-
-#### Field: Solar Model Indicator
-
-This field allows the user to select **ASHRAEClearSky, ASHRAETau, ZhangHuang, or Schedule** for solar modeling in the calculation of the solar radiation in the design day.  ASHRAEClearSky and ZhangHuang use the Clearness value as part of their calculations.  ASHRAETau invokes the revised model specified in Chapter 14 of the ASHRAE 2009 HOF and uses Taub and Taud values (below).  Technical details of the models are described in the Engineering Reference.  The **Schedule** choice allows you to enter schedule values for the day’s profile (use the next two fields for the names).
-
-#### Field: Beam Solar Day Schedule Name
-
-This field allows the option for you to put in your own day profile of beam solar values (wh/m2). These values will replace the calculated values during design day processing. Only day schedules (ref. Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List objects) are used here.
-
-#### Field: Diffuse Solar Day Schedule Name
-
-This field allows the option for you to put in your own day profile of diffuse solar values (wh/m2).  These values will replace the calculated values during design day processing. Only day schedules (ref. Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List objects) are used here.
-
-#### Field: ASHRAE Clear Sky Optical Depth for Beam Irradiance (taub)
-
-Optical depth for beam radiation, used only when Solar Model Indicator is ASHRAETau.  See next field.
-
-#### Field: ASHRAE Clear Sky Optical Depth for Diffuse Irradiance (taud)
-
-Optical depth for diffuse radiation, used only when Solar Model Indicator is ASHRAETau.  Taub and Taud values are tabulated by month for 5564 locations worldwide on the CD that accompanies the ASHRAE 2009 HOF.
-
-#### Field: Sky Clearness
-
-If the choice in the Solar Model Indicator field is ASHRAEClearSky or ZhangHuang, then this numeric field should be entered. This value represents the “clearness� value for the day. This value, along with the solar position as defined by the Location information and the date entered for the design day, help define the solar radiation values for each hour of the day. Clearness may range from 0.0 to 1.2, where 1.0 represents a clear sky at sea level.  Values greated than 1.0 may be used for high altitude locations. Traditionally, one uses 0.0 clearness for Winter Design Days. Note that this “sky clearness� does not have the same meaning as output variable “Site Daylighting Model Sky Clearness�.
-
-IDF Examples:
-
-```idf
-! Phoenix Sky Harbor Intl Ap_AZ_USA Annual Cooling (WB=&gt;MDB)
-!   .4%, MDB=35.8°C WB=24.5°C
- SizingPeriod:DesignDay,
-  Phoenix Sky Harbor Intl Ap Ann Clg .4% Condns WB=&gt;MDB,     !- Name
-          7,      !- Month
-         21,      !- Day of Month
-  SummerDesignDay,!- Day Type
-       35.8,      !- Maximum Dry-Bulb Temperature {C}
-         12,      !- Daily Dry-Bulb Temperature Range {C}
- DefaultMultipliers, !- Dry-Bulb Temperature Range Modifier Type
-           ,      !- Dry-Bulb Temperature Range Modifier Schedule Name
-    Wetbulb,      !- Humidity Condition Type
-       24.5,      !- Wetbulb at Maximum Dry-Bulb {C}
-           ,      !- Humidity Indicating Day Schedule Name
-           ,      !- Humidity Ratio at Maximum Dry-Bulb {kgWater/kgDryAir}
-           ,      !- Enthalpy at Maximum Dry-Bulb {J/kg}
-           ,      !- Daily Wet-Bulb Temperature Range {deltaC}
-     97342.,      !- Barometric Pressure {Pa}
-        4.1,      ! Wind Speed {m/s}
-        260,      !- Wind Direction {Degrees; N=0, S=180}
-         No,      !- Rain {Yes/No}
-         No,      !- Snow on ground {Yes/No}
-         No,      !- Daylight Savings Time Indicator
-       ASHRAETau, !- Solar Model Indicator
-           ,      !- Beam Solar Day Schedule Name
-           ,      !- Diffuse Solar Day Schedule Name
-      0.588,     !- ASHRAE Clear Sky Optical Depth for Beam Irradiance (taub)
-      1.653;  !- ASHRAE Clear Sky Optical Depth for Diffuse Irradiance (taud)
-
-
-  SizingPeriod:DesignDay,
-    Denver Centennial Golden Ann Htg 99% Condns DB - sched solar,  !- Name
-    1,                       !- Month
-    13,                      !- Day of Month
-    WinterDesignDay,         !- Day Type
-    -16,                     !- Maximum Dry-Bulb Temperature {C}
-    0.0,                     !- Daily Dry-Bulb Temperature Range {deltaC}
-    ,                        !- Dry-Bulb Temperature Range Modifier Type
-    ,                    !- Dry-Bulb Temperature Range Modifier Schedule Name
-    Wetbulb,                 !- Humidity Condition Type
-    -16,                     !- Wetbulb or DewPoint at Maximum Dry-Bulb {C}
-    ,                        !- Humidity Indicating Day Schedule Name
-    ,               !- Humidity Ratio at Maximum Dry-Bulb {kgWater/kgDryAir}
-    ,                        !- Enthalpy at Maximum Dry-Bulb {J/kg}
-    ,                        !- Daily Wet-Bulb Temperature Range {deltaC}
-    83411.,                  !- Barometric Pressure {Pa}
-    2.3,                     !- Wind Speed {m/s}
-    180,                     !- Wind Direction {deg}
-    No,                      !- Rain Indicator
-    No,                      !- Snow Indicator
-    No,                      !- Daylight Saving Time Indicator
-    Schedule,                !- Solar Model Indicator
-    Winter (1/13) Beam Solar,!- Beam Solar Day Schedule Name
-    Winter (1/13) Diffuse Solar;  !- Diffuse Solar Day Schedule Name
-
-
-  Schedule:Day:Hourly,
-    Winter (1/13) Beam Solar,
-    Any Number,
-    0,0,0,0,0,0,0,190,698,852,892,919,957,953,856,700,213,0,0,0,0,0,0,0;
-
-
-  Schedule:Day:Hourly,
-    Winter (1/13) Diffuse Solar,
-    Any Number,
-    0,0,0,0,0,0,0,35,118,116,92,65,40,14,0,0,5,0,0,0,0,0,0,0;
-```
-
-
-
-
-Look at the example files 1ZoneUncontrolled\_DDChanges.idf and 1ZoneUncontrolled\_DD2009 for several examples of specifying Design Day inputs.
-
-### Sizing Period Design Day Outputs
-
-For the schedule fields in the object, several output variables can be used:
-
-* Zone,Average,Sizing Period Site Beam Solar Schedule Value [W/m2]
-
-* Zone,Average,Sizing Period Site Diffuse Solar Schedule Value [W/m2]
-
-* Zone,Average,Sizing Period Site Humidity Condition Schedule Value [%]
-
-* Zone,Average,Sizing Period Site Humidity Condition Schedule Value []
-
-* Zone,Average,Sizing Period Site Drybulb Temperature Range Modifier Schedule Value []
-
-* Zone,Average,Sizing Period Site Drybulb Temperature Range Modifier Schedule Value [deltaC]
-
-* Zone,Average,Sizing Period Site Drybulb Temperature Range Modifier Schedule Value [C]
-
-* Zone,Average,Sizing Period Site Sky Temperature Schedule Value [deltaC]
-
-* Zone,Average,Sizing Period Site Sky Temperature Schedule Value [C]
-
-
-#### Sizing Period Site Beam Solar Schedule Value [W/m2]
-
-#### Sizing Period Site Diffuse Solar Schedule Value [W/m2]
-
-This schedule value is active when any Design Day objects have / use the solar schedule option. For those objects that don’t have this option, the value will be displayed as -999.
-
-#### Sizing Period Site Humidity Condition Schedule Value [%]
-
-#### Sizing Period Site Humidity Condition Schedule Value []
-
-This schedule value is active when any Design Day objects have / use the humidity schedule option. For those objects that don’t have this option, the value will be displayed as -999.
-
-#### Sizing Period Site Drybulb Temperature Range Modifier Schedule Value []
-
-#### Sizing Period Site Drybulb Temperature Range Modifier Schedule Value [deltaC]
-
-#### Sizing Period Site Drybulb Temperature Range Modifier Schedule Value [C]
-
-This schedule value is active when any Design Day objects have / use the drybulb temperature range modifier chedule option. For those objects that don’t have this option, the value will be displayed as -999.
-
-#### Sizing Period Site Sky Temperature Schedule Value [deltaC]
-
-#### Sizing Period Site Sky Temperature Schedule Value [C]
-
-This schedule value is active when any Design Day objects have / use the WeatherProperties:SkyTemperature schedule option. For those objects that don’t have this option, the value will be displayed as -999.
-
-### Longer Design Periods
-
-Some features may benefit by using a longer design weather period for sizing or loads calculations.  Longer design periods may be created by using the **SizingPeriod:WeatherFileDays** or **SizingPeriod:WeatherFileConditionType** objects.  These two objects allow for selections from an attached weather file to be used in the sizing calculations.
-
-### SizingPeriod:WeatherFileDays
-
-The SizingPeriod:WeatherFileDays object describes using a selected period from the “attached� weather file to be used in load calculations or sizing equipment.  The period selected can be as small as a single day or larger.  Multiple periods may be input. While this object may be used for sizing calculations, you should also consider using design days that represent more long term extremes or conditions.
-
-#### Field: Name
-
-This field allows for an assigned name for this run period so it can be tracked easily in sizing and other outputs.
-
-#### Field: Begin Month
-
-This numeric field should contain the starting month number (1=January, 2=February, etc.) for the annual run period desired.
-
-#### Field: Begin Day of Month
-
-This numeric field should contain the starting day of the starting month (must be valid for month) for the annual run period desired.
-
-#### Field: End Month
-
-This numeric field should contain the ending month number (1=January, 2=February, etc.) for the annual run period desired.
-
-#### Field: End Day of Month
-
-This numeric field should contain the ending day of the ending month (must be valid for month) for the annual run period desired.
-
-#### Field: Day of Week for Start Day
-
-For flexibility, the day of week indicated on the weather file can be overridden by this field’s value. Valid days of the week (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday) or special days (SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2) must be entered in this field. To clarify, this value will be used as the Start Day (type) for this sizing period. When weekdays are used, each subsequent day in the period will be incremented.  When SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2 – are used, the day type will be applied for the entire period.
-
-#### Field: Use Weather File Daylight Saving Period
-
-Weather files can contain indicators of Daylight Saving Period days. For flexibility, you may want to ignore these designations on the weather file. This field should contain the word **Yes** if you will accept daylight saving period days as contained on the weather file (note: not all weather files may actually have this period) or **No** if you wish to ignore Daylight Saving Period days that may be on the weather file.
-
-Note that a blank or null field in this field will indicate **Yes**.
-
-#### Field: Use Weather File Rain and Snow Indicators
-
-Weather files can contain “rain� and “snow� indicators. (EPW field “Present Weather Codes� – described in the AuxiliaryPrograms document). In turn, rain indicates wet surfaces which changes the film convection coefficient for the surface. Other models may use rain as well (Ground Heat Exchangers). Snow indicators can change the ground reflectance if there is snow on the ground. Entering “**Yes**� in this field allows the weather file conditions to represent “Rain� and “Snow�;  entering “**No**� in the field “turns off� the rain/snow indicators for this period. You might use this to be able to compare two “same location� weather files of different years, origins, etc.
-
-IDF Example:
-
-```idf
-SizingPeriod:WeatherFileDays,
-    Summer including Extreme Summer days,  !- Name
-    7,18,7,25,                             !- Begin/end Day/Month
-    SummerDesignDay,                       !- Day type
-    No,                          !- Use Weather File Daylight Saving Period
-    No;                          !- Use Weather File Rain and Snow Indicators
-
-
-  SizingPeriod:WeatherFileDays,
-    Winter including Extreme Winter days,  !- Name
-    1,25,2,1,                              !- Begin/end Day/Month
-    WinterDesignDay,                       !- Day type
-    No,                          !- Use Weather File Daylight Saving Period
-    No;                          !- Use Weather File Rain and Snow Indicators
-```
-
-
-### SizingPeriod:WeatherFileConditionType
-
-When the EPW files are created, a heuristic procedure identifies extreme and typical periods in the actual weather file.  This object will allow one of those periods to be selected for sizing or load calculations (typically). Multiple objects may be input. While this object may be used for sizing calculations, you should also consider using design days that represent more long term extremes or conditions.
-
-#### Field: Name
-
-This field allows for an assigned name for this run period so it can be tracked easily in sizing and other outputs.
-
-#### Field: Period Selection
-
-This field allows the generic period calculated from the weather file to be selected for this run period.  It is not completely generic as there may be extreme cold periods in some weather files but extreme wet periods (tropical) in others. Not all weather files have all of the valid choices. The choices for this field are:
-
-- SummerExtreme
-
-- SummerTypical
-
-- WinterExtreme
-
-- WinterTypical
-
-- AutumnTypical
-
-- SpringTypical
-
-- WetSeason
-
-- DrySeason
-
-- NoDrySeason
-
-- NoWetSeason
-
-- TropicalHot
-
-- TropicalCold
-
-#### Field: Day of Week for Start Day
-
-For flexibility, the day of week indicated on the weather file can be overridden by this field’s value. Valid days of the week (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday) or special days (SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2) must be entered in this field. To clarify, this value will be used as the Start Day (type) for this sizing period. When weekdays are used, each subsequent day in the period will be incremented.  When SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2 – are used, the day type will be applied for the entire period.
-
-#### Field: Use Weather File Daylight Saving Period
-
-Weather files can contain indicators of Daylight Saving Period days. For flexibility, you may want to ignore these designations on the weather file. This field should contain the word **Yes** if you will accept daylight saving period days as contained on the weather file (note: not all weather files may actually have this period) or **No** if you wish to ignore Daylight Saving Period days that may be on the weather file.
-
-Note that a blank or null field in this field will indicate **Yes**.
-
-#### Field: Use Weather File Rain and Snow Indicators
-
-Weather files can contain “rain� and “snow� indicators. (EPW field “Present Weather Codes� – described in the AuxiliaryPrograms document). In turn, rain indicates wet surfaces which changes the film convection coefficient for the surface. Other models may use rain as well (Ground Heat Exchangers). Snow indicators can change the ground reflectance if there is snow on the ground. Entering “**Yes**� in this field allows the weather file conditions to represent “Rain� and “Snow�;  entering “**No**� in the field “turns off� the rain/snow indicators for this period. You might use this to be able to compare two “same location� weather files of different years, origins, etc.
-
-IDF Example:
-
-```idf
-  SizingPeriod:WeatherFileConditionType,
-    Extreme Summer Weather Period for Design,  !- Name
-    SummerExtreme,                             !- Period Selection
-    SummerDesignDay,                           !- Day Type
-    No,                          !- Use Weather File Daylight Saving Period
-    No;                          !- Use Weather File Rain and Snow Indicators
-
-
-  SizingPeriod:WeatherFileConditionType,
-    Extreme Winter Weather Period for Design,  !- Name
-    WinterExtreme,                             !- Period Selection
-    WinterDesignDay,                           !- Day Type
-    No,                          !- Use Weather File Daylight Saving Period
-    No;                          !- Use Weather File Rain and Snow Indicators
-```
-
-
-### RunPeriod
-
-The RunPeriod object describes the elements necessary to create a weather file simulation. Multiple run periods may be input. EnergyPlus accepts weather files in the special EnergyPlus weather format (described briefly below this document and in more detail in the Auxiliary Programs document). These files can describe Daylight Saving Time periods as well as holidays within their definitions. The RunPeriod object allows the user to override the use of both the Daylight Saving Period (i.e. use or ignore) and holidays that are embedded within the weather file. Note that the weather file also may contain design condition information, typical and extreme period information, ground temperatures based on air temperature calculations.
-
-#### Field: Name
-
-This optional field allows the RunPeriod to be named for output reporting. When left blank, the weather file location name is used. Note that the weather file location name will be appened to this name in tabular/summary reports.
-
-#### Field: Begin Month
-
-This numeric field should contain the starting month number (1=January, 2=February, etc.) for the annual run period desired.
-
-#### Field: Begin Day of Month
-
-This numeric field should contain the starting day of the starting month (must be valid for month) for the annual run period desired.
-
-#### Field: End Month
-
-This numeric field should contain the ending month number (1=January, 2=February, etc.) for the annual run period desired.
-
-#### Field: End Day of Month
-
-This numeric field should contain the ending day of the ending month (must be valid for month) for the annual run period desired.
-
-#### Field: Day of Week for Start Day
-
-For flexibility, the day of week indicated on the weather file can be overridden by this field’s value. Valid days of the week (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday) must be entered in this field. To clarify, this value will be used as the Start Day (type) for this run period and subsequent days will be implemented. If a blank or UseWeatherFile is entered here, then the starting day type will be calculated from the weather file (ref: Auxiliary Programs document about Data Periods).
-
-#### Field: Use Weather File Holidays and Special Days
-
-Weather files can contain holiday designations or other kinds of special days. These day types cause a corresponding day’s schedule (see SCHEDULE definitions below) to be used during that day. This field should contain the word **Yes** if holidays or other special days indicated directly on the weather file should retain their “day type� or **No** if holidays or other special days on the weather file should be ignored. Reference the RunPeriodControl:SpecialDays object below to enter your own special days and holidays.
-
-Note that a blank or null field in this field will indicate **Yes**.
-
-#### Field: Use Weather File Daylight Saving Period
-
-Weather files can contain indicators of Daylight Saving period days. For flexibility, you may want to ignore these designations on the weather file. This field should contain the word **Yes** if you will accept daylight saving period days as contained on the weather file (note: not all weather files may actually have this period) or **No** if you wish to ignore Daylight Saving period days that may be on the weather file.
-
-Note that a blank or null field in this field will indicate **Yes**.
-
-#### Field: Apply Weekend Holiday Rule
-
-In some countries (notably the US), when holidays fall on weekends, they are often observed on a weekday close to the holiday day. (Usually if the specific day falls on a Saturday, the observed day is Friday; if on a Sunday, the observed day is Monday). EnergyPlus will represent this custom using the value in this field. If the field is **Yes**, then specific date holidays that have a duration of one day, will be “observed� on the Monday after the day. (Specific day holidays are such as January 1 – a day-month combination).  If the field is blank or **No**, then the holiday will be shown on the day-month as entered. As this option is listed at the RunPeriod, all applicable special days for the run will use the rule – there is no override for individual special days.
-
-Note that a blank or null field in this field will indicate **No**.
-
-Note: EnergyPlus processed weather files available on the EnergyPlus web site: http://www.energyplus.gov/cfm/weather_data.cfm have neither special days specified nor daylight saving period. However, DDY (Design Day) files produced from the ASHRAE Design Conditions that accompany the EPW files may include a DaylightSavingPeriod object for certain locations.
-
-#### Field: Use Weather File Rain Indicators
-
-Weather files can contain “rain� indicators. (EPW field “Present Weather Codes� – described in the AuxiliaryPrograms document). In turn, rain indicates wet surfaces which changes the film convection coefficient for the surface. Other models may use rain as well (Ground Heat Exchangers). Entering “**Yes**� in this field allows the weather file conditions to represent “Rain�;  entering “**No**� in the field “turns off� the rain indicator for this period. You might use this to be able to compare two “same location� weather files of different years, origins, etc.
-
-#### Field: Use Weather File Snow Indicators
-
-Weather files can contain “snow� indicators. (EPW field “Snow Depth� &gt; 0 indicates “Snow on the ground�). In turn, snow changes the reflectivity of the ground and cascades changes of this reflectivity. Entering “**Yes**� in this field allows the weather file conditions to represent “Snow�;  entering “**No**� in the field “turns off� the snow indicator for this period. You might use this to be able to compare two “same location� weather files of different years, origins, etc.
-
-#### Field: Number of Times Runperiod to be Repeated
-
-This numeric field represents the number of times (usually years) the simulation has to be carried out in a multi runperiod simulation. The default value is set to 1. The number of years of simulation, in case of a Ground Loop Heat Exchanger (GLHE) simulation, should be equal to the length of simulation field in GLHE object. Note that you can specify a number of simulation years with a shorter run period (e.g. 1 week) and EnergyPlus will repeat the simulation of the shorter run period for that many times. Note that repeating will work with any weather file that contains the start date and end date in a “Data Period� (refer to Auxiliary Programs document for more documentation on weather file contents).
-
-#### Field: Increment Day of Week on Repeat
-
-When repeating RunPeriods (see previous field), you can choose to increment the day of week at the end of the period to have a more continuous day type. Enter **Yes** to increment the day of the week (default). An entry of **No** will keep the same day of week values as in the first time through.
-
-#### Field: Start Year
-
-When repeating a period, you might (for whatever reason), choose to have a specific year as a starting year. Enter an appropriate 4 digit year in this field. Refer to Auxiliary Programs document for more documentation on weather file contents, particularly in using leap year data (or not) within weather files.
-
-And, as shown in an IDF:
-
-```idf
- RunPeriod,  ! Winter Simulation
-    Winter Simulation,  !- Name
-    12,  !- Begin Month
-    1,  !- Begin Day of Month
-    3,  !- End Month
-    31,  !- End Day of Month
-    UseWeatherFile,  !- Day of Week for Start Day
-    Yes,  !- Use Weather File Holidays and Special Days
-    Yes,  !- Use Weather File Daylight Saving Period
-    No,  !- Apply Weekend Holiday Rule
-    Yes,  !- Use Weather File Rain Indicators
-    Yes;  !- Use Weather File Snow Indicators
-
-
-
-
- ! Multiple year simulation example
- RunPeriod,
-    Multiple Years,  !- Name
-    1,    !- Begin Month
-    1,    !- Begin Day of Month
-    12,   !- End Month
-    31,   !- End Day of Month
-    UseWeatherFile,  !- Day of Week for Start Day
-    Yes,  !- Use Weather File Holidays and Special Days
-    Yes,  !- Use Weather File Daylight Saving Period
-    No,   !- Apply Weekend Holiday Rule
-    Yes,  !- Use Weather File Rain Indicators
-    Yes,  !- Use Weather File Snow Indicators
-     3;   !- Number of Times Runperiod to be Repeated
-```
-
-### RunPeriod:CustomRange
-
-The RunPeriod:CustomRange object describes the elements necessary to use a specially crafted (likely multiple year) weather file in a simulation. These kinds of weather files and simulations might be useful for matching utility periods or simulating several years of differing weather data. Multiple run periods may be input. EnergyPlus accepts weather files in the special EnergyPlus weather format (described briefly below this document and in more detail in the Auxiliary Programs document). In order to effectively use this object, however, you will need to use a text editor (EnergyPlus weather files area simple text files) or possibly a spreadsheet program and then save to a csv (comma separated variable) file. Weather files can describe Daylight Saving Time periods as well as holidays within their definitions. The RunPeriod:CustomRange object allows the user to override the use of both the Daylight Saving Period (i.e. use or ignore) and holidays that are embedded within the weather file. Note that the weather file also may contain design condition information, typical and extreme period information, ground temperatures based on air temperature calculations.
-
-#### Field: Name
-
-This optional field allows the RunPeriod to be named for output reporting. When left blank, the weather file location name is used. Note that the weather file location name will be appened to this name in tabular/summary reports.
-
-#### Field: Begin Month
-
-This numeric field should contain the starting month number (1=January, 2=February, etc.) for the annual run period desired.
-
-#### Field: Begin Day of Month
-
-This numeric field should contain the starting day of the starting month (must be valid for month) for the annual run period desired.
-
-#### Field: Begin Year
-
-This numeric field should contain the beginning year for the custom range. Though all EnergyPlus (EPW) weather files contain a year/year field, the RunPeriod object does not use this field (previous object). The **RunPeriod:CustomRange** object causes the program to look specifically for the begin date specified by these three fields (i.e. Begin Month, Begin Day of Month, Begin Year).
-
-#### Field: End Month
-
-This numeric field should contain the ending month number (1=January, 2=February, etc.) for the annual run period desired.
-
-#### Field: End Day of Month
-
-This numeric field should contain the ending day of the ending month (must be valid for month) for the annual run period desired.
-
-#### Field: End Year
-
-This numeric field should contain the end year for the custom range. Though all EnergyPlus (EPW) weather files contain a year/year field, the RunPeriod object does not use this field (previous object). The **RunPeriod:CustomRange** object causes the program to look specifically for the end date specified by these three fields (i.e. End Month, End Day of Month, End Year).
-
-#### Field: Day of Week for Start Day
-
-For flexibility, the day of week indicated on the weather file can be overridden by this field’s value. Valid days of the week (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday) must be entered in this field. To clarify, this value will be used as the Start Day (type) for this run period and subsequent days will be implemented. If a blank or UseWeatherFile is entered here, then the starting day type will be calculated from the weather file (ref: Auxiliary Programs document about Data Periods).
-
-#### Field: Use Weather File Holidays and Special Days
-
-Weather files can contain holiday designations or other kinds of special days. These day types cause a corresponding day’s schedule (see SCHEDULE definitions below) to be used during that day. This field should contain the word **Yes** if holidays or other special days indicated directly on the weather file should retain their “day type� or **No** if holidays or other special days on the weather file should be ignored. Reference the RunPeriodControl:SpecialDays object below to enter your own special days and holidays.
-
-Note that a blank or null field in this field will indicate **Yes**.
-
-#### Field: Use Weather File Daylight Saving Period
-
-Weather files can contain indicators of Daylight Saving period days. For flexibility, you may want to ignore these designations on the weather file. This field should contain the word **Yes** if you will accept daylight saving period days as contained on the weather file (note: not all weather files may actually have this period) or **No** if you wish to ignore Daylight Saving period days that may be on the weather file.
-
-Note that a blank or null field in this field will indicate **Yes**.
-
-#### Field: Apply Weekend Holiday Rule
-
-In some countries (notably the US), when holidays fall on weekends, they are often observed on a weekday close to the holiday day. (Usually if the specific day falls on a Saturday, the observed day is Friday; if on a Sunday, the observed day is Monday). EnergyPlus will represent this custom using the value in this field. If the field is **Yes**, then specific date holidays that have a duration of one day, will be “observed� on the Monday after the day. (Specific day holidays are such as January 1 – a day-month combination).  If the field is blank or **No**, then the holiday will be shown on the day-month as entered. As this option is listed at the RunPeriod, all applicable special days for the run will use the rule – there is no override for individual special days.
-
-Note that a blank or null field in this field will indicate **No**.
-
-Note: EnergyPlus processed weather files available on the EnergyPlus web site: http://www.energyplus.gov/cfm/weather_data.cfm have neither special days specified nor daylight saving period. However, DDY (Design Day) files produced from the ASHRAE Design Conditions that accompany the EPW files may include a DaylightSavingPeriod object for certain locations.
-
-#### Field: Use Weather File Rain Indicators
-
-Weather files can contain “rain� indicators. (EPW field “Present Weather Codes� – described in the AuxiliaryPrograms document). In turn, rain indicates wet surfaces which changes the film convection coefficient for the surface. Other models may use rain as well (Ground Heat Exchangers). Entering “**Yes**� in this field allows the weather file conditions to represent “Rain�;  entering “**No**� in the field “turns off� the rain indicator for this period. You might use this to be able to compare two “same location� weather files of different years, origins, etc.
-
-#### Field: Use Weather File Snow Indicators
-
-Weather files can contain “snow� indicators. (EPW field “Snow Depth� &gt; 0 indicates “Snow on the ground�). In turn, snow changes the reflectivity of the ground and cascades changes of this reflectivity. Entering “**Yes**� in this field allows the weather file conditions to represent “Snow�;  entering “**No**� in the field “turns off� the snow indicator for this period. You might use this to be able to compare two “same location� weather files of different years, origins, etc.
-
-### RunPeriodControl:SpecialDays
-
-For weather file run periods, special day run periods can be described. These will always be in effect for the selected days in the run period. Depending on the Use Special Days value in the RunPeriod:\* object(s), these can augment any special days included on the weather file.
-
-Note: EnergyPlus processed weather files available on the EnergyPlus web site: http://www.energyplus.gov/cfm/weather_data.cfm have neither special days specified nor daylight saving period. However, DDY (Design Day) files produced from the ASHRAE Design Conditions that accompany the EPW files may include a DaylightSavingPeriod object for certain locations.
-
-#### Field: Name
-
-This alpha field is the title for the special day period. It must be unique among all the special day period objects entered.
-
-#### Field: Start Date
-
-This field is the starting date for the special day period. Dates in this field can be entered in several ways as shown in the accompanying table:
-
-Table 3. Date Field Interpretation
-
-<table class="table table-striped">
-<tr>
-<th>Field Contents</th>
-<th>Interpretation</th>
-</tr>
-<tr>
-<td>&lt;number&gt; / &lt;number&gt;</td>
-<td>Month / Day</td>
-</tr>
-<tr>
-<td>&lt;number&gt; Month</td>
-<td>Day and Month</td>
-</tr>
-<tr>
-<td>Month &lt;number&gt;</td>
-<td>Day and Month</td>
-</tr>
-<tr>
-<td>&lt;number&gt; Weekday in Month</td>
-<td>Numbered weekday of month</td>
-</tr>
-<tr>
-<td>Last Weekday In Month</td>
-<td>Last weekday of month</td>
-</tr>
-</table>
-
-In the table, Month can be one of (January, February, March, April, May, June, July, August, September, October, November, December). Abbreviations of the first three characters are also valid.
-
-In the table, Weekday can be one of (Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday). Abbreviations of the first three characters are also valid.
-
-#### Field: Duration
-
-This numeric field specifies how long (number of days) the special day period lasts.
-
-#### Field: Special Day Type
-
-This alpha field designates the “day type� for schedule use during the special period. It must be one of (Holiday, SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2).
-
-An example in the IDF would be:
-
-```idf
-RunPeriodControl:SpecialDays, President’s Day, 3rd Monday in February,1,Holiday;
-RunPeriodControl:SpecialDays, Thanksgiving, 4th Thursday in November, 1,Holiday;
-RunPeriodControl:SpecialDays, Halloween, 10/31, 1, Holiday;
-RunPeriodControl:SpecialDays, Vacation, 5/1, 14, CustomDay1;
-```
-
-### RunPeriodControl:DaylightSavingTime
-
-Similar to a special day period, a daylight saving period may be entered to be applied to weather file run periods. These will always be in effect, regardless of the value entered on the RunPeriod object. Note that this period will always override any daylight saving period specified in a weather file.
-
-Note: EnergyPlus processed weather files available on the EnergyPlus web site: http://www.energyplus.gov/cfm/weather_data.cfm have neither special days specified nor daylight saving period.
-
-**Note:  For EnergyPlus Output:Variable and Output:Meter reporting, the time stamps are always in standard time. When daylight saving time is active, scheduled loads and controls will shift one hour relative to standard time.**
-
-#### Field: Start Date
-
-This is the starting date of the daylight saving period. Note that it can be entered in several formats as shown in Table 3. Date Field Interpretation.
-
-#### Field: End Date
-
-This is the ending date of the daylight saving period. Note that it can be entered in several formats as shown in Table 3. Date Field Interpretation.
-
-
-
-And in the IDF:
-
-```idf
-! U.S. Standard for Daylight Saving
-RunPeriodControl:DaylightSavingTime,2nd Sunday in March, 1st Sunday in November; !2007
-! Brazil standard
-RunPeriodControl:DaylightSavingTime,1st Sunday in October, Last Sunday in February;
-! European Standard
-RunPeriodControl:DaylightSavingTime, Last Sunday in March, Last Sunday in October;
-! Syria Standard
-RunPeriodControl:DaylightSavingTime, 4/1, 10/1;
-```
-
-
-Of course, these could not all appear in the same IDF as only one DaylightSavingPeriod object per input file is allowed. More information on Daylight Saving Periods can be seen on the web at: http://www.webexhibits.org/daylightsaving/  The ASHRAE Handbook of Fundamentals [ASHRAE 2005] also contains information about daylight saving periods and their climatic information now includes start and end dates for many locations.
-
-### WeatherProperty:SkyTemperature
-
-Sky Temperature, or radiative sky temperature, is internally calculated by EnergyPlus using an algorithm using horizontal infrared radiation from sky, cloudiness factors and current temperaure. The algorithm is fully described in the Engineering Reference document. For flexibility, the following object can be entered to override the internal calculations. Much of the literature describes the sky temperature as relative to either drybulb or dewpoint temperature.
-
-#### Field: Name
-
-This name references an existing design period (i.e., SizingPeriod:DesignDay, SizingPeriod:WeatherFileDays, or SizingPeriod:WeatherFileConditionType) or run period (by name or blank for all run periods).
-
-#### Field: Calculation Type
-
-Allowable entries here are: **ScheduleValue**, **DifferenceScheduleDryBulbValue**, or **DifferenceScheduleDewPointValue**. In each case the following field must specify a valid schedule name. **ScheduleValue** – the values in the schedule are used as the sky temperature. **DifferenceScheduleDryBulbValue** – the values in the schedule are used as a difference to the drybulb temperature value (+values would then be greater than the drybulb temperature, -values would then be less than the drybulb temperature) for the resulting sky temperature value. **DifferenceScheduleDewPointValue** – the values in the schedule are used as a difference to the dewpoint temperature value (+values would then be greater than the dewpoint temperature, -values would then be less than the dewpoint temperature) for the resulting sky temperature value.
-
-#### Field: ScheduleName
-
-This field specifies a schedule name to accomplish the sky temperature calculation from the previous field. A Schedule:Day:\* (i.e., Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List) should be specified if the name in the name field matches a SizingPeriod:DesignDay object. If the name is one of the weather file period specifications (i.e. matches a SizingPeriod:WeatherFileDays, SizingPeriod:WeatherFileConditionType or RunPeriod), then the schedule name must match a full year schedule (i.e. Schedule:Year, Schedule:Compact, Schedule:File, or Schedule:Constant).
-
-An example of IDF usage (with DesignDay):
-
-```idf
-  SizingPeriod:DesignDay,
-    DENVER_STAPLETON Ann Clg 1% Sky Temperature modfier,  !- Name
-    32.6,               !- Maximum Dry-Bulb Temperature {C}
-    15.2,               !- Daily Temperature Range {deltaC}
-    15.5,               !- Humidity Indicating Conditions at Maximum Dry-Bulb
-    83411.,                  !- Barometric Pressure {Pa}
-    4,                       !- Wind Speed {m/s}
-    120,                     !- Wind Direction {deg}
-    1.00,                    !- Sky Clearness
-    0,                       !- Rain Indicator
-    0,                       !- Snow Indicator
-    25,                      !- Day of Month
-    7,                       !- Month
-    SummerDesignDay,         !- Day Type
-    0,                       !- Daylight Saving Time Indicator
-    WetBulb,                 !- Humidity Indicating Type
-    ,                        !- Relative Humidity Day Schedule Name
-    deltaschedule,           !- Dry-Bulb Temperature Range Modifier Type
-    temp range deltas; !-   Dry-Bulb Temperature Range Modifier Schedule Name
-
-
-  WeatherProperty:SkyTemperature,
-    DENVER_STAPLETON Ann Clg 1% Sky Temperature modfier,  !- Name
-    ScheduleValue,           !- Calculation Type
-    DaySchedule5;            !- Schedule Name
-
-
-  Schedule:Day:Interval,
-    DaySchedule5,            !- Name
-    Temperature,             !- Schedule Type Limits Name
-    Yes,                     !- Interpolate to Timestep
-    until: 24:00,            !- Time 1
-    5;                       !- Value Until Time 1
-```
-
-
-### Site:WeatherStation
-
-The Site:WeatherStation object is used to specify the measurement conditions for the climatic data listed in the weather file. These conditions indicate the height above ground of the air temperature sensor, the height above ground of the wind speed sensor, as well as coefficients that describe the wind speed profile due to the terrain surrounding the weather station. There are necessary correlations between the entries for this object and some entries in the Building object, specifically the **Terrain** field.
-
-Weather stations throughout the world (ref: WMO – World Meteorological Organization) take their measurements at standard conditions:
-
-- Air temperature is measured at approximately 1.5 m above ground
-
-- Wind speed is measured at 10 m above ground
-
-- Weather station is in a flat, open field with little protection from the wind.
-
-When using weather data from standard sources (e.g., TMY2, IWEC, TMY, or ASHRAE design day data), it is not necessary to use the **Site:WeatherStation** object. However, if you are using custom weather data or real-time weather data, you may need to read and understand the concepts in the **Site:WeatherStation** object.
-
-The measurement conditions at the weather station (i.e., the weather file) are used by EnergyPlus in conjunction with the *Terrain* field of the **Building** object, or optionally with the **Site:HeightVariation** object (see below), to calculate the local variation in atmospheric properties as a function of height above ground. Outdoor air temperature decreases with height, while wind speed increases with height. The algorithms for this calculation are in the Engineering Reference.
-
-The **Site:WeatherStation** object is useful when working with a custom weather file that includes data that were not measured at the WMO standard conditions. For example, the weather data could be measured on site, or on the roof top of a nearby building. The wind speed profile coefficients can be estimated from the table below or calculated beforehand using more sophisticated techniques such as CFD modeling of the weather station terrain.
-
-Table 4. Wind Speed Profile Coefficients (ASHRAE Fundamentals 2005).
-
-<table class="table table-striped">
-<tr>
-<th>Terrain Description</th>
-<th>Exponent</th>
-<th>Bounhary Layer Thickness (m)</th>
-</tr>
-<tr>
-<td>Flat, open country</td>
-<td>0.14</td>
-<td>270</td>
-</tr>
-<tr>
-<td>Rough, wooded country</td>
-<td>0.22</td>
-<td>370</td>
-</tr>
-<tr>
-<td>Towns and cities</td>
-<td>0.33</td>
-<td>460</td>
-</tr>
-<tr>
-<td>Ocean</td>
-<td>0.10</td>
-<td>210</td>
-</tr>
-<tr>
-<td>Urban, industrial, forest</td>
-<td>0.22</td>
-<td>370</td>
-</tr>
-</table>
-
-If the **Site:WeatherStation** object is omitted from the input file, the WMO standard measurement conditions are assumed.
-
-#### Field: Wind Sensor Height Above Ground
-
-The height [m] above ground for the wind speed sensor.
-
-#### Field: Wind Speed Profile Exponent
-
-The wind speed profile exponent for the terrain surrounding the weather station. The exponent can be estimated from the table above or calculated beforehand using more sophisticated techniques, such as CFD modeling of the weather station terrain.
-
-#### Field: Wind Speed Profile Boundary Layer Thickness
-
-The wind speed profile boundary layer thickness [m] for the terrain surrounding the weather station. The boundary layer can be estimated from the table above or calculated beforehand using more sophisticated techniques, such as CFD modeling of the weather station terrain.
-
-#### Field: Air Temperature Sensor Height Above Ground
-
-The height [m] above ground for the air temperature sensor.
-
-For example, if you are using weather data measured on the top of your building, you should set the *Wind Sensor Height Above Ground* and the *Air Temperature Sensor Height Above Ground* to equal the height of your building (say 30 m). The *Wind Speed Profile Exponent* and *Wind Speed Profile Boundary Layer Thickness* should be set to match the values associated with the *Terrain* field of the **Building** object, or the equivalent fields of the **Site:HeightVariation** object.
-
-Or, in IDF terms, with a building in a town or city:
-
-```idf
-Site:WeatherStation,
-    30,  !- Wind Sensor Height Above Ground {m}
-    0.33,  !- Wind Speed Profile Exponent {}
-    460,  !- Wind Speed Profile Boundary Layer Thickness {m}
-    30;  !- Air Temperature Sensor Height Above Ground {m}
-```
-
-
-This would change if you had a different wind speed profile exponent or wind speed profile boundary layer thickness at your site.
-
-### Site:HeightVariation
-
-The Site:HeightVariation object is used to specify the local variation in atmospheric properties at the site and should be used only if you require advanced control over the height-dependent variations for wind speed and temperature. The coefficients set by this object are used by EnergyPlus, in conjunction with the Site:WeatherStation object (see above), to calculate the local variation in atmospheric properties as a function of height above ground. Outdoor air temperature decreases with height, while wind speed increases with height. The local outdoor air temperature and wind speed are calculated separately for all zones and surfaces, and optionally for outdoor air nodes for which a height has been specified (see OutdoorAir:Node object). With the default inputs, wind speed falls significantly at heights lower than the weather station measurement height, and temperature increases slightly. The algorithms for this calculation are in the Engineering Reference. There are necessary correlations between the entries for this object and some entries in the Building object, specifically the **Terrain** field.
-
-Table 5. Atmospheric Variables at Two Different Heights Above Ground Level.
-
-<table class="table table-striped">
-<tr>
-<th>Variable</th>
-<th>1.5 m</th>
-<th>284 m</th>
-<th>Absolute Diff</th>
-<th>Percent Diff</th>
-</tr>
-<tr>
-<td>Air Temperature</td>
-<td>15°C</td>
-<td>13.15°C</td>
-<td>1.85°C</td>
-<td>12.3%</td>
-</tr>
-<tr>
-<td>Barometric Pressure</td>
-<td>101,325 Pa</td>
-<td>97,960 Pa</td>
-<td>3,365 Pa</td>
-<td>3.3%</td>
-</tr>
-<tr>
-<td>Wind Speed</td>
-<td>2.46 m/s</td>
-<td>7.75 m/s</td>
-<td>5.29 m/s</td>
-<td>215%</td>
-</tr>
-</table>
-
-
-
-Note that using this object overrides the wind speed profile coefficients implied by the *Terrain* field of the **Building** object even if the wind speed profile fields are left blank. The wind speed profile coefficients can be estimated from the table above (see **Site:WeatherStation**) or calculated beforehand using more sophisticated techniques such as CFD modeling of the site terrain.
-
-#### Field: Wind Speed Profile Exponent
-
-The wind speed profile exponent for the terrain surrounding the site. The exponent can be estimated from the table above (see **Site:WeatherStation**) or calculated beforehand using more sophisticated techniques, such as CFD modeling of the site terrain. Note that using this object overrides the wind speed profile coefficients implied by the *Terrain* field of the **Building** object even if this field is left blank. This field can be set to zero to turn off all wind dependence on height.
-
-#### Field: Wind Speed Profile Boundary Layer Thickness
-
-The wind speed profile boundary layer thickness [m] for the terrain surrounding the site. The boundary layer can be estimated from the table above (see **Site:WeatherStation**) or calculated beforehand using more sophisticated techniques, such as CFD modeling of the site terrain. Note that using this object overrides the wind speed profile coefficients implied by the *Terrain* field of the **Building** object even if this field is left blank.
-
-#### Field: Air Temperature Gradient Coefficient
-
-The air temperature gradient coefficient [K/m] is a research option that allows the user to control the variation in outdoor air temperature as a function of height above ground. The real physical value is 0.0065 K/m. This field can be set to zero to turn off all temperature dependence on height. Note that the *Air Temperature Sensor Height* in the **Site:WeatherStation** object should also be set to zero in order to force the local outdoor air temperatures to match the weather file outdoor air temperature. This change is required because the **Site:WeatherStation** object assumes an air temperature gradient of 0.0065 K/m. This field can be set to zero to turn off all temperature dependence on height.
-
-```idf
-  Site:HeightVariation,
-    0.22,  !- Wind Speed Profile Exponent
-    370,  !- Wind Speed Profile Boundary Layer Thickness {m}
-    0.0065;  !- Air Temperature Gradient Coefficient {deltaC/m}
-```
-
-
-### Site:GroundTemperature:BuildingSurface
-
-Ground temperatures are used for the ground heat transfer model. There can be only one ground temperature object included, and it is used as the outside surface temperature for all surfaces with Outside Boundary Condition=Ground. The object is options if you have no surfaces with ground contact. The outside surface temperature for individual surfaces can be specified using the OtherSideCoefficients (ref: SurfaceProperty:OtherSideCoefficients) object that allows Toutside to be set with a schedule. This permits using any number of different outside face temperatures in addition to the ground temperature.
-
-Caution: The “undisturbed� ground temperatures calculated by the weather converter should not be used in building losses but are appropriate to be used in the Site:GroundTemperature:Shallow and Site:GroundTemperature:Deep objects. The reasoning (for building losses) is that these values are too extreme for the soil under a conditioned building. For best results, use the Slab or Basement program described in this document to calculate custom monthly average ground temperatures (see the Ground Heat Transfer section). This is especially important for residential applications and very small buildings. If one of these ground temperature preprocessors is not used, for typical commercial buildings in the USA, a reasonable default value is 2C less than the average indoor space temperature.
-
-More information about determining appropriate ground temperatures is given in the Auxiliary Programs document.
-
-#### Field: Month Temperature(s) – 12 fields in all
-
-Each numeric field is the monthly ground temperature (degrees Celsius) used for the indicated month (January=1<sup>st</sup> field, February=2<sup>nd</sup> field, etc.)
-
-An IDF example:
-
-```idf
-Site:GroundTemperature:BuildingSurface,19,20,20,20,20,20,20,20,20,20,20,20;
-```
-
-### Site:GroundTemperature:Shallow
-
-Site:GroundTemperature:Shallow are used by the Surface Ground Heat Exchanger (i.e. object: GroundHeatExchanger:Surface). Only one shallow ground temperature object can be included.
-
-Note that the ground temperatures included in full year weather files may be suitable of being used for the values in these fields – namely, the .5 m depth temperatures that are calculated for “undisturbed� soil of “typical� conditions. However, you may wish to use some other change effect – based on the weather conditions of the building location.
-
-This object may be used for objects requiring "undisturbed" ground temperatures. In these instances, the "name" input field is not required. 
-
-#### Field: Month Temperature(s) – 12 fields in all
-
-Each numeric field is the monthly surface ground temperature (degrees Celsius) used for the indicated month (January=1<sup>st</sup> field, February=2<sup>nd</sup> field, etc.)
-
-An IDF example:
-
-```idf
-Site:GroundTemperature:Shallow,  4,4,6,6,10,10,15,15,14,14,8,8;
-```
-
-
-### Site:GroundTemperature:Deep
-
-Site:GroundTemperature:Deep are used by the Pond Ground Heat Exchanger object (i.e. object: GroundHeatExchanger:Pond). Only one deep ground temperature object can be included.
-
-Note that the ground temperatures included in full year weather files may be suitable of being used for the values in these fields – namely, the 4 m depth temperatures that are calculated for “undisturbed� soil of “typical� conditions. However, you may wish to use some other change effect – based on the weather conditions or special knowledge of the building location.
-
-This object may be used for objects requiring "undisturbed" ground temperatures. In these instances, the "name" input field is not required. 
-
-#### Field: Month Temperature(s) – 12 fields in all
-
-Each numeric field is the monthly deep ground temperature (degrees Celsius) used for the indicated month (January=1<sup>st</sup> field, February=2<sup>nd</sup> field, etc.)
-
-An IDF example:
-
-```idf
-Site:GroundTemperature:Deep,  16,16,16,16,16,16,16,16,16,16,16,16;
-```
-
-
-###Site:GroundTemperature:Undisturbed:FiniteDifference
-
-Site:GroundTemperature:Undisturbed:FiniteDifference may be used by all objects requiring "undisturbed" ground temperatures. The object uses a 1D finite difference heat transfer model which uses the weather file to obtain surface boundary conditions. An annual simulation is run on the model during it's initialization until the annual ground temperature profile has reached steady periodic behavior. Once steady periodic behavior is reached, the ground tempeatures are cached for retrieval during the rest of the simulation.
-
-#### Field: Soil Thermal Conductivity
-
-The thermal conductivity of the soil, in W/m-K.
-
-#### Field: Soil Density
-
-The bulk density of the soil, in kg/m3.
-
-#### Field: Soil Specific Heat
-
-The specific heat of dry soil, in J/kg-K.
-
-#### Field: Soil Moisture Content Volume Fraction
-
-A nominal value of soil moisture content to be used when evaluating soil thermal properties.
-
-#### Field: Soil Moisture Content Volume Fraction at Saturation
-
-A nominal value of soil moisture content when the soil is saturated, this is used in evaluating thermal properties of freezing soil.
-
-#### Field: Evapotranspiration Ground Cover Parameter
-
-Numeric field specifies the ground cover effects used in the evapotranspiration model at the ground surface heat balance. The values range from 0 (solid, non-permeable ground surface) to 1.5 (wild growth).
-
-An IDF example:
-
-```
-  Site:GroundTemperature:Undisturbed:FiniteDifference,
-    FDTemps,     !- Name of object
-    1.08,        !- Soil Thermal Conductivity {W/m-K}
-    962,         !- Soil Density {kg/m3}
-    2576,        !- Soil Specific Heat {J/kg-K}
-    30,          !- Soil Moisture Content Volume Fraction {percent}
-    50,          !- Soil Moisture Content Volume Fraction at Saturation {percent} 
-    0.408;       !- Evapotranspiration Ground Cover Parameter
-```
-
-
-###Site:GroundTemperature:Undisturbed:KusduaAchenbach
-
-Site:GroundTemperature:Undisturbed:KusudaAchenbach may be used by all objects requiring "undisturbed" ground temperatures. It provides an undisturbed ground temperature based on the correlation developed by Kusuda T. and P. Achenbach. 1965. The correlation uses three parameters for ground temperature at the surface to define a correlation for undisturbed ground temperatures as a function of depth and time. If one thinks of the ground temperature for a given depth as a sinusoid, the average ground temperature, amplitude (average difference between maximum ground temperature and minimum ground temperature), and the phase shift (day of minimum surface temperature) are all required to define the correlation.
-
-If the parameters are left blank they can be autocalculated by including soil surface temperatures in the input using the Site:GroundTemperature:Shallow object. They can also be calculated by using the CalcSoilSurfTemp preprocessor. 
-
-Kusuda, T. and P.R. Achenbach. 1965. 'Earth Temperatures and Thermal Diffusivity at Selected Stations in the United States.' *ASHRAE Transactions*. 71(1): 61-74.
-
-#### Field: Soil Thermal Conductivity
-
-The thermal conductivity of the soil, in W/m-K.
-
-#### Field: Soil Density
-
-The bulk density of the soil, in kg/m3.
-
-#### Field: Soil Specific Heat
-
-The specific heat of dry soil, in J/kg-K.
-
-#### Field: Average Annual Ground Surface Temperature
-
-This is the average ground surface temperature throughout the entire year, in °C.
-
-#### Field: Average Amplitude of Annual Ground Surface Temperature
-
-This is the average amplitude of the ground surface temperature, in °C.
-
-#### Field: Phase Shift of Minimum Surface Temperature
-
-This is day of the year which has the lowest ground surface temperature.
-
-An IDF example:
-
-```idf
-  Site:GroundTemperature:Undisturbed:KusudaAchenbach,
-    KATemps,    !- Name of object
-    1.08,       !- Soil Thermal Conductivity {W/m-K}
-    962,        !- Soil Density {kg/m3}
-    2576,       !- Soil Specific Heat {J/kg-K}
-    15.5,       !- Average Soil Surface Temperature {C}
-    12.0,       !- Average Amplitude of Surface Temperature {deltaC}
-    21;         !- Phase Shift of Minimum Surface Temperature {days}
-```
-
-
-###Site:GroundTemperature:Undisturbed:Xing
-
-Site:GroundTemperature:Undisturbed:Xing may be used by all objects requiring "undisturbed" ground temperatures. It provides an undisturbed ground temperature based on the correlation developed by Xing, 2014. The correlation is a 5 parameter, 2 harmonic model based on the work of Lord Kelvin (Thomson, 1862). The average soil surface temperature and two sets of surface temperature amplitude and phase shift must be provided. Parameters for 4000+ international locations can be found in Xing, 2014.
-
-Thomson, W. 1862. 'On the Reduction of Observations of Underground Temperature, with applications to Professor Forbes’ Edinburgh Observations and the continued Calton Hill Series.' Proceedings of the Royal Society of Edinburgh. IV: 342-346.
-
-Xing, L. 2014. Estimations of Undisturbed Ground Temperatures using Numerical and Analytical Modeling. Ph.D. Diss. Oklahoma State University, Stillwater, OK.
-
-#### Field: Soil Thermal Conductivity
-
-The thermal conductivity of the soil, in W/m-K.
-
-#### Field: Soil Density
-
-The bulk density of the soil, in kg/m3.
-
-#### Field: Soil Specific Heat
-
-The specific heat of dry soil, in J/kg-K.
-
-#### Field: Average Soil Surface Temperature
-
-The average annual surface temperature of the soil, in deg C.
-
-#### Field: Soil Surface Temperature Amplitude 1
-
-First soil surface temperature amplitude parameter, in deg C.
-
-#### Field: Soil Surface Temperature Amplitude 2
-
-Second soil surface temperature amplitude parameter, in deg C.
-
-#### Field: Phase Shift of Surface Temperature Amplitude 1
-
-Phase shift of surface temperature amplitude 1, in days.
-
-#### Field: Phase Shift of Surface Temperature Amplitude 2
-
-Phase shift of surface temperature amplitude 2, in days.
-
-An IDF example:
-
-```
-  Site:GroundTemperature:Undisturbed:Xing,
-    Chicago-Ohare,    !- Name of object
-    1.08,         !- Soil Thermal Conductivity {W/m-K}
-    962,          !- Soil Density {kg/m3}
-    2576,         !- Soil Specific Heat {J/kg-K}
-    11.1,         !- Average Soil Surface Tempeature {C}
-    13.4,         !- Soil Surface Temperature Amplitude 1 {deltaC}
-    0.7,          !- Soil Surface Temperature Amplitude 2 {deltaC}
-    25,           !- Phase Shift of Temperature Amplitude 1 {days}
-    30;           !- Phase Shift of Temperature Amplitude 2 {days}
-```
-
-
-### Site:GroundDomain:Slab
-
-This section documents the input object used to simulate ground coupled heat transfer with horizontal building surfaces within EnergyPlus. Horizontal ground surfaces within EnergyPlus interact with the Site:GroundDomain object by utilizing the SurfaceProperty:OtherSideConditionsModel object. By utilizing this object, multiple horizontal surfaces can be coupled to the same Site:GroundDomain object. Each horizontal surface may also have its unique ground domain, however, runtime will be adversely affected.
-
-Generally, there are two scenarios which Site:GroundDomain is equipped to model: in-grade slabs, and on-grade slabs.
-
-![](media/image012.png)
-
-Figure 7In-grade configuration.
-
-The in-grade slab option can be used to simulate situations when the upper slab surface is near the ground surface level. For this situation, slab’s upper surface must interact with the zone via an OSCM boundary. Due to this, the FloorConstruction object for the zone floor must include a thin layer of the upper floor material. Horizontal and vertical insulation are modeled by the GroundDomain in this scenario. Horizontal insulation can be modeled as covering the full horizontal surface, or it can be limited to the perimeter regions only. In the latter case, the perimeter insulation width must be specified.
-
-![](media/image013.png)
-
-Figure 8 On-grade configuration
-
-The on-grade slab option can be used to simulate situations when the lower slab surface is near the ground surface level. In this situation, the entire floor must be included within the floor construction object. Vertical insulation is modeled by the GroundDomain in this scenario.  Horizontal insulation can only be modeled as covering the full horizontal surface.
-
-#### Field: Name
-
-Alpha field used as a unique identifier for each ground domain.
-
-#### Field: Ground Domain Depth
-
-Numeric field used to determine the depth of the simulation domain, in meters.
-
-#### Field: Aspect Ratio
-
-Numeric field used to define the height to width ratio of the slab.
-
-#### Field: Perimeter Offset
-
-Numeric field used to determine the distance from the slab perimeter to the domain perimeter, in meters.
-
-#### Field: Soil Thermal Conductivity
-
-The thermal conductivity of the soil, in W/m-K.
-
-#### Field: Soil Density
-
-The bulk density of the soil, in kg/m3.
-
-#### Field: Soil Specific Heat
-
-The specific heat of dry soil, in J/kg-K. If moisture is defined in this object, moisture and freezing effects are accounted for by varying the specific heat value.
-
-#### Field: Soil Moisture Content Volume Fraction
-
-A nominal value of soil moisture content to be used when evaluating soil thermal properties.
-
-#### Field: Soil Moisture Content Volume Fraction at Saturation
-
-A nominal value of soil moisture content when the soil is saturated, this is used in evaluating thermal properties of freezing soil.
-
-#### Field: Type of Undisturbed Ground Temperature Object
-
-This is the type of undisturbed ground temperature object that is used to determine the ground temperature.
-
-#### Field: Name of Undisturbed Ground Temperature Object
-
-This is the name of the undisturbed ground temperature object that is used to determine the ground temperature.
-
-#### Field: Evapotranspiration Ground Cover Parameter
-
-Numeric field specifies the ground cover effects used in the evapotranspiration model at the ground surface heat balance. The values range from 0 (solid, non-permeable ground surface) to 1.5 (wild growth).
-
-#### Field: Slab Boundary Condition Model Name
-
-This is the name of the other side boundary condition model used.
-
-#### Field: Slab Location
-
-Alpha field indicates whether the slab is in-grade (top surface level with ground surface) or on-grade (bottoms surface level with ground surface). Options include “ONGRADE� and “INGRADE�.
-
-#### Field: Slab Material Name
-
-Name of the material object representing the slab material. Only applicable to in-grade situations.
-
-#### Field: Horizontal Insulation
-
-Alpha field indicates whether horizontal insulation is present. Options include “YES� and “NO�. Only applicable to in-grade situations.
-
-#### Field: Horizontal Insulation Material Name
-
-Name of material object representing the horizontal slab insulation. Optional argument only required if horizontal insulation is present.
-
-#### Field: Horizontal Insulation Extents
-
-Alpha field indicates whether the horizontal slab insulation extends to cover the full horizontal area of the slab, or only covers the slab perimeter. Optional argument only required if horizontal insulation is present. Options include “FULL� and “PERIMETER�.
-
-#### Field: Perimeter Insulation Width
-
-Numeric field indicating the width of the perimeter insulation measured from the slab edge. Valid range from &gt; 0 to &lt; half of smallest slab width.
-
-#### Field: Vertical Insulation
-
-Alpha field indicates whether vertical insulation is present. Options include “YES� and “NO�.
-
-#### Field: Vertical Insulation Name
-
-Name of material object representing the vertical slab insulation. Optional argument only required if vertical insulation is present.
-
-#### Field: Vertical Insulation Depth
-
-Numeric field indicates the depth measured in meters from the ground surface to which the vertical perimeter insulation extends. Valid range from &gt; Slab Thickness to &lt; Domain Depth.
-
-#### Field: Simulation Timestep
-
-Alpha field indicating whether the domain will update temperatures at each zone timestep, or at hourly intervals. Options include “timestep� and “hourly�.
-
-An IDF example of an in-grade slab.
-
-```idf
-Site:GroundDomain:Slab,
-    IngradeCoupledSlab, !- Name
-    5,                  !- Ground Domain Depth
-    1,                  !- Aspect Ratio
-    5,                  !- Domain Perimeter Offset
-    1.8,                !- Soil Thermal Conductivity
-    3200,               !- Soil Density
-    836,                !- Soil Specific Heat
-    30,                 !- Soil Moisture Content Volume Fraction
-    50,                 !- Soil Moisture Content Volume Fraction at Saturation
-    Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
-    KATemps;                            !- Name of Undisturbed Ground Temperature Object
-    1,    !- Evapotranspiration Ground Cover Parameter
-    GroundCoupledOSCM,      !- Name of Floor Boundary Condition Model
-    InGrade,                !- Slab Location (InGrade/OnGrade)
-    Slab Material-In-grade, !- Slab Material Name
-    Yes,                    !- Horizontal Insulation
-    Slab Insulation,    !- Horizontal Insulation Material Name
-    Perimeter,          !- Full Horizontal or Perimeter Only
-    1,                  !- Perimeter insulation width
-    Yes,                !- Vertical Insulation
-    Slab Insulation,    !- Vertical Insulation Name
-    2,                  !- Vertical perimeter insulation depth from surface
-    Hourly;             !- Simulation timestep</td>
-```
-
-And IDF example of an on-grade slab
-
-```idf
-Site:GroundDomain:Slab,
-    OngradeCoupledSlab, !- Name
-    5,                  !- Ground Domain Depth {m}
-    1,                  !- Aspect Ratio
-    5,                  !- Domain Perimeter Offset {m}
-    1.8,                !- Soil Thermal Conductivity {W/m-K}
-    3200,               !- Soil Density {kg/m3}
-    836,                !- Soil Specific Heat {J/kg-K}
-    30,                 !- Soil Moisture Content Volume Fraction
-    50,                 !- Soil Moisture Content Volume Fraction at Saturation
-    Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
-    KATemps;            !- Name of Undisturbed Ground Temperature Object
-    1,                  !- Evapotranspiration Ground Cover Parameter
-    GroundCoupledOSCM,  !- Name of Floor Boundary Condition Model
-    OnGrade,            !- Slab Location (InGrade/OnGrade)
-    ,                   !- Slab Material Name
-    ,                   !- Horizontal Insulation (Yes/No)
-    ,                   !- Horizontal Insulation Material Name
-    ,                   !- Full Horizontal or Perimeter Only
-    ,                   !- Perimeter insulation width (m)
-    Yes,                !- Vertical Insulation (Yes/No)
-    Slab Insulation,    !- Vertical Insulation Name
-    2,                  !- Vertical perimeter insulation depth from surface
-    Hourly;             !- Simulation timestep. (Timestep/Hourly)</td>
-```
-
-### Site:GroundDomain:Slab Outputs
-
-The following output variables are available.
-
-* Zone, Average, Zone Coupled Surface Heat Flux [W/m2]
-* Zone, Average, Zone Coupled Surface Temperature [C]</td>
-
-#### Zone Coupled Surface Heat Flux [W/m2]
-
-This is the value of the heat flux provided to the GroundDomain as a boundary condition. This is calculated by taking the average heat flux of all surfaces coupled to the domain's SurfaceProperty:OtherSideConditionsModel model.
-
-#### Zone Coupled Surface Temperature [C]
-
-This is the value of the SurfaceProperty:OtherSideConditionsModel surface temperature. This is the temperature provided to the ground coupled surfaces as an outside boundary condition.
-
-### Site:GroundDomain:Basement
-
-This section documents the input object used to simulate ground coupled heat transfer with underground zones within EnergyPlus. Zone surfaces within EnergyPlus interact with the Site:GroundDomain:Basement object by utilizing the SurfaceProperty:OtherSideConditionsModel object. Two separate OSCM are required for the basement vertical and horizontal surfaces. Vertical wall surfaces will interact with the first OSCM while the horizontal floor surface will interact with the second OSCM. Basement floor and wall surfaces are constructed normally by using the BuildingSurface:Detailed object, with the outside boundary condition being the OtherSideConditionsModel for the basement floor or wall. The outside surface of the wall being the interface between the ground domain and the EnergyPlus zone. Horizontal and vertical ground insulation are simulated by the ground domain, and therefore should not be included in the wall and floor construction objects.
-
-![](media/image900.png)
-
-Figure: Basement Configuration
-
-```idf
-Site:GroundDomain:Basement,
-    CoupledBasement,         !- Name
-    10,                      !- Ground Domain Depth {m}
-    1,                       !- Aspect ratio
-    5,                       !- Perimeter offset {m}
-    1.8,                     !- Soil Thermal Conductivity {W/m-K}
-    3200,                    !- Soil Density {kg/m3}
-    836,                     !- Soil Specific Heat {J/kg-K}
-    30,                      !- Soil Moisture Content Volume Fraction {percent}
-    50,                      !- Soil Moisture Content Volume Fraction at Saturation {percent}
-    Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
-    KATemps;                 !- Name of Undisturbed Ground Temperature Object
-    1,                       !- Evapotranspiration Ground Cover Parameter
-    BasementFloorOSCM,       !- Name of Basement Floor Boundary Condition Model
-    Yes,                     !- Basement Horizontal Underfloor Insulation Present (Yes/No)
-    Basement Insulation,     !- Basement Horizontal Insulation Underfloor Material Name
-    Full,                    !- Full Horizontal or Perimeter Only (Full/Perimeter)
-    ,                        !- Perimeter width (m)
-    2.5,                     !- Depth of Basement Wall In Ground Domain {m}
-    BasementWallOSCM,        !- Name of Basement Wall Boundary Condition Model
-    Yes,                     !- Basement Wall Vertical Insulation Present(Yes/No)
-    Basement Insulation,     !- Basement Wall Vertical Insulation Material Name
-    2.5,                     !- Vertical insulation depth from surface (m)
-    Hourly;                  !- Domain Update interval. (Timestep, Hourly)
-    4;                       ! Mesh Density Parameter
-```
-
-#### Field: Name
-
-Alpha field used as a unique identifier for each basement domain. Multiple basements domains can be simulated simultaneously, however, each domain must have a unique name. Additionally, despite the ability to simulate multiple domains simultaneously, these domains do not interact with each other and are treated as independent domains with boundary conditions given by the model parameters below.
-
-#### Field: Ground Domain Depth
-
-Numeric field used to determine the depth of the simulation domain, in meters. A value of 10 meters is the default.
-
-#### Field: Aspect Ratio
-
-Numeric field, which is the ratio of basement length to width, used to determine the aspect ratio of the basement. This field along with the total basement floor area, which is taken as the combination of all surfaces connected to the floor OtherSideConditionsModel, are used to determine the size and shape of the basement domain. Aspect ratios and the inverse of aspect ratios should produce identical results. i.e. AR = 2 equals AR = 0.5. This field has units of meters/meters.
-
-#### Field: Domain Perimeter Offset
-
-Numeric field used to determine the distance from the basement perimeter to the domain perimeter, in meters. A value of 5 is default.
-
-#### Field: Soil Thermal Conductivity
-
-The thermal conductivity of the soil, in W/m-K.
-
-#### Field: Soil Density
-
-The bulk density of the soil, in kg/m3.
-
-#### Field: Soil Specific Heat
-
-The specific heat of dry soil, in J/kg-K. If moisture is defined in this object, moisture and freezing effects are accounted for by varying the specific heat value.
-
-#### Field: Soil Moisture Content Volume Fraction
-
-A nominal value of soil moisture content to be used when evaluating soil thermal properties. 
-
-#### Field: Soil Moisture Content Volume Fraction at Saturation
-
-A nominal value of soil moisture content when the soil is saturated, this is used in evaluating thermal properties of freezing soil.
-
-#### Field: Type of Undisturbed Ground Temperature Object
-
-This is the type of undisturbed ground temperature object that is used to determine the ground temperature.
-
-#### Field: Name of Undisturbed Ground Temperature Object
-
-This is the name of the undisturbed ground temperature object that is used to determine the ground temperature.
-
-#### Field: Evapotranspiration Ground Cover Parameter
-
-Numeric field specifies the ground cover effects used in the evapotranspiration model at the ground surface heat balance. The values range from 0 (solid, non-permeable ground surface) to 1.5 (wild growth). Model can be sensitive to variations in this parameter, especially in dry climates.
-
-#### Field: Basement Floor Boundary Condition Model Name
-
-This is the name of the other side boundary condition model used for the basement floor surface. 
-
-#### Field: Horizontal Insulation 
-
-Alpha field indicates whether horizontal insulation is present. Options include “YES� and “NO�. 
-
-#### Field: Horizontal Insulation Name
-
-Name of material object representing the horizontal underfloor basement insulation. Optional argument only required if horizontal insulation is present.
-
-#### Field: Horizontal Insulation Extents
-
-Alpha field indicates whether the horizontal underfloor insulation extends to cover the full horizontal area of the basement floor, or only covers the basement floor perimeter. Optional argument only required if horizontal insulation is present. Options include “FULL� and “PERIMETER�.
-
-#### Field: Perimeter Insulation Width
-
-Numeric field indicating the width of the perimeter insulation measured from the basement floor edge. Valid range from > 0 to &lt; half of smallest basement floor width.
-
-#### Field: Basement Depth
-
-Depth of basement floor surface referenced from the ground surface, in meters. This domain should be the distance from the ground surface down to the basement floor surface. In cases where the ground surface is below the main above-ground building level, a separate wall surface should be employed between the basement walls and the main level walls.
-
-#### Field: Basement Wall Boundary Condition Model Name
-
-Name of the other side condition boundary model used for the basement walls.
-
-#### Field: Vertical Insulation 
-
-Alpha field indicates whether vertical insulation is present. Options include “YES� and “NO�.
-
-#### Field: Vertical Insulation Name
-
-Name of material object representing the vertical slab insulation. Optional argument only required if vertical insulation is present.
-
-#### Field: Vertical Insulation Depth
-
-Numeric field indicates the depth measured in meters from the ground surface to which the vertical perimeter insulation extends. Valid range from > 0 to &lt; Basement Depth.
-
-#### Field: Simulation Timestep
-
-Alpha field indicating whether the domain will update temperatures at each zone timestep, or at hourly intervals. Options include “timestep� and “hourly�.
-
-#### Mesh Density Parameter
-
-Integer field indicating the density of the finite difference ground domain cells between the basement and the far field boundaries. Default value is 4. Total number of ground domain cells, insulation cells, and ground surface cells are indicated as outputs to the eio file.
-
-### Site:GroundDomain:Basement Outputs
-
-The following output variables are available.
-
-* Wall Interface Heat Flux
-
-* Wall Interface Temperature
-
-* Floor Interface Heat Flux
-
-* Floor Interface Temperature
-
-#### Wall Interface Heat Flux [W/m2]
-
-This is the value of the heat flux provided to ground domain as a boundary condition for the basement walls. Should be equal to the basement wall outside heat flux.
-
-#### Wall Interface Temperature [C]
-
-This is the value of the SurfaceProperty:OtherSideConditionsModel surface temperature. This is the temperature provided to the basement wall surfaces as an outside boundary condition.
-
-#### Floor Interface Heat Flux [W/m2]
-
-This is the value of the heat flux provided to ground domain as a boundary condition for the basement floor. Should be equal to the basement floor outside heat flux.
-
-#### Floor Interface Temperature [C]
-
-This is the value of the SurfaceProperty:OtherSideConditionsModel surface temperature. This is the temperature provided to the ground coupled floor surfaces as an outside boundary condition.
-
-
-
-### Site:GroundTemperature:FCfactorMethod
-
-Site:GroundTemperature:FCfactorMethod is used only by the underground walls or slabs-on-grade or underground floors defined with C-factor (Construction:CfactorUndergroundWall) and F-factor (Construction:FfactorGroundFloor) method for code compliance calculations where detailed construction layers are unknown. Only one such ground temperature object can be included. The monthly ground temperatures for this object are close to the monthly outside air temperatures delayed by three months. If user does not input this object in the IDF file, it will be defaulted to the 0.5m set of monthly ground temperatures from the weather file if they are available. Entering these will also overwrite any ground temperatures from the weather file in the F and C factor usage. If neither is available, an error will result.
-
-#### Field: Month Temperature(s) – 12 fields in all
-
-Each numeric field is the monthly ground temperature (degrees Celsius) used for the indicated month (January=1<sup>st</sup> field, February=2<sup>nd</sup> field, etc.)
-
-And, the IDF example:
-
-```idf
-Site:GroundTemperature:FCfactorMethod,  9.5, 3.5, -0.7, -1.7, -0.6, 3.6, 9.3, 14, 18.2, 22.7, 21.2, 16.8;
-```
-
-
-### Site:GroundReflectance
-
-Ground reflectance values are used to calculate the ground reflected solar amount. This fractional amount (entered monthly) is used in this equation:
-
-<div>\[{\rm{GroundReflectedSolar = (BeamSolar}} \bullet {\rm{COS(SunZenithAngle) + DiffuseSolar)}} \bullet {\rm{GroundReflectance}}\]</div>
-
-Of course, the Ground Reflected Solar is never allowed to be negative. The ground reflectance can be further modified when snow is on the ground by the Snow Ground Reflectance Modifier. To use no ground reflected solar in your simulation, enter 0.0 for each month.
-
-#### Field: Month Average Ground Reflectance(s) – 12 fields in all
-
-Each numeric field is the monthly average reflectivity of the ground used for the indicated month (January=1<sup>st</sup> field, February=2<sup>nd</sup> field, etc.)
-
-And use in an IDF:
-
-```idf
-  Site:GroundReflectance,
-     0.600,     !January Ground Reflectance
-     0.600,     !February Ground Reflectance
-     0.400,     !March Ground Reflectance
-     0.300,     !April Ground Reflectance
-     0.200,     !May Ground Reflectance
-     0.200,     !June Ground Reflectance
-     0.200,     !July Ground Reflectance
-     0.200,     !August Ground Reflectance
-     0.200,     !September Ground Reflectance
-     0.200,     !October Ground Reflectance
-     0.300,     !November Ground Reflectance
-     0.400;     !December Ground Reflectance
-```
-
-### Site:GroundReflectance:SnowModifier
-
-It is generally accepted that snow resident on the ground increases the basic ground reflectance. EnergyPlus allows the user control over the snow ground reflectance for both “normal ground reflected solar� calculations (see above) and snow ground reflected solar modified for daylighting. These are entered under this object and both default to 1 (same as normal ground reflectance – no special case for snow which is a conservative approach).
-
-#### Field: Ground Reflected Solar Modifier
-
-This field is a decimal number which is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values).
-
-<div>\[{\rm{GroundReflectanc}}{{\rm{e}}_{{\rm{used}}}} = {\rm{GroundReflectance}} \bullet Modifie{r_{Snow}}\]</div>
-
-The actual Ground Reflectance is limited to [0.0,1.0].
-
-#### Field: Daylighting Ground Reflected Solar Modifier
-
-This field is a decimal number which is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values).
-
-<div>\[{\rm{DaylightingGroundReflectanc}}{{\rm{e}}_{{\rm{used}}}} = {\rm{GroundReflectance}} \bullet Modifie{r_{Snow}}\]</div>
-
-The actual Ground Reflectance is limited to [0.0,1.0].
-
-An IDF example:
-
-```idf
-  Site:GroundReflectance:SnowModifier,
-    1.0;                     !- Ground Reflected Solar Modifier
-```
-
-Outputs will show both the inputs from the above object as well as monthly values for both Snow Ground Reflectance and Snow Ground Reflectance for Daylighting.
-
-### Site:WaterMainsTemperature
-
-The Site:WaterMainsTemperature object is used to calculate water temperatures delivered  by underground water main pipes. The mains temperatures are used as default, make-up water temperature inputs for several plant objects, including:  **WaterUse:Equipment, WaterUse:Connections, WaterHeater:Mixed** and **WaterHeater:Stratified**. The mains temperatures are also used in the water systems objects to model the temperature of cold water supplies.
-
-Water mains temperatures are a function of outdoor climate conditions and vary with time of year. A correlation has been formulated to predict water mains temperatures based on two weather inputs:
-
-- average annual outdoor air temperature (dry-bulb)
-
-- maximum difference in monthly average outdoor air temperatures
-
-These values can be easily calculated from annual weather data using a spreadsheet or from the ".stat" file available with the EnergyPlus weather files at [www.energyplus.gov](http://www.energyplus.gov). Monthly statistics for dry-bulb temperatures are shown with daily averages. The daily averages are averaged to obtain the annual average. The maximum and minimum daily average are subtracted to obtain the maximum difference. For more information on the water mains temperatures correlation, see the *EnergyPlus Engineering Document*.
-
-Alternatively, the Site:WaterMainsTemperature object can read values from a schedule. This is useful for measured data or when water comes from a source other than buried pipes, e.g., a river or lake.
-
-If there is no Site:WaterMainsTemperature object in the input file, a default constant value of 10 C is assumed.
-
-#### Field: Calculation Method
-
-This field selects the calculation method and must have the keyword Schedule or Correlation.
-
-#### Field: Schedule Name
-
-If the calculation method is Schedule, the water mains temperatures are read from the schedule referenced by this field. If the calculation method is Correlation, this field is ignored.
-
-#### Field: Annual Average Outdoor Air Temperature
-
-If the calculation method is Correlation, this field is used in the calculation as the annual average outdoor air temperature (dry-bulb) [C]. If the calculation method is Schedule, this field is ignored.
-
-#### Field: Maximum Difference In Monthly Average Outdoor Air Temperatures
-
-If the calculation method is Correlation, this field is used in the calculation as the maximum difference in monthly average outdoor air temperatures [∆C]. If the calculation method is Schedule, this field is ignored.
-
-```idf
-  Site:WaterMainsTemperature,
-    Correlation,  !- Calculation Method {SCHEDULE | CORRELATION}
-    ,  !- Schedule Name
-    9.69,  !- Annual Average Outdoor Air Temperature {C}
-    28.1;  !- Maximum Difference In Monthly Average Outdoor Air Temperatures
-           !- {deltaC}
-```
-
-### Site:Precipitation
-
-The Site:Precipitation object is used to describe the amount of water precipitation at the building site over the course of the simulation run period. Precipitation includes both rain and the equivalent water content of snow. Precipitation is not yet described well enough in the many building weather data files. So this object can be used to provide the data using Schedule objects that define rates of precipitation in meters per hour.
-
-A set of schedules for site precipitation have been developed for USA weather locations and are provided with EnergyPlus in the data set called PrecipitationSchedulesUSA.idf.  The user can develop schedules however they want. The schedules in the data set were developed using EnergyPlus’ weather file (EPW) observations and the average monthly precipitation for the closest weather site provided by NOAA. EPW files for the USA that were based on TMY or TMY2 include weather observations for Light/Moderate/Heavy rainfall, however most international locations do not include these observations. The values were modeled by taking the middle of the ranges quoted in the EPW data dictionary. The assumed piecewise function is shown below.
-
-<div>\[Amount\,(m/hour) = \,\left\{ {\begin{array}{*{20}{c}}{Light = 0.0125}\\\{Moderate = 0.052}\\\{Heavy = 0.1}\end{array}} \right.\]</div>
-
-The values were inserted on hour by hour basis for the month based on the observations. Then each month was rescaled to meet the average precipitation for the month based on the 30-year average (1971-2000) provided by the NOAA/NCDC. Therefore, the flags in the EPW file match the precipitation schedules for the USA. Note that summing the average monthly precipitation values will not give you the average yearly precipitiation. The resulting value may be lower or higher than the average yearly value.
-
-Once the typical rainfall pattern and rates are scheduled, the Site:Precipitation object provides a method of shifting the total rainfall up or down for design purposes. Wetter or drier conditions can be modeled by changing the Design Annual Precipitation although the timing of precipitation throughout the year will not be changed.
-
-#### Field: Precipitation Model Type
-
-Choose rainfall modeling options. Only available option is ScheduleAndDesignLevel.
-
-#### Field: Design Level for Total Annual Precipitation
-
-Magnitude of total precipitation for an annual period to be used in the model. Value selected by the user to correspond with the amount of precipitation expected or being assumed for design purposes. The units are in meters. This field works with the following two fields to allow easily shifting the amounts without having to generate new schedules.
-
-#### Field: Precipitation Rate Schedule Name
-
-Name of a schedule defined elsewhere that describes the rate of precipitation. The precipitation rate schedule is analogous to weather file data. However, weather files for building simulation do not currently contain adequate data for such calculations. Therefore, EnergyPlus schedules are used to enter the pattern of precipitation events. The values in this schedule are the average rate of precipitation in meters per hour. The integration of these values over an annual schedule should equal the nominal annual precipitation.
-
-#### Field: Average Total Annual Precipitation
-
-Magnitude of annual precipitation associated with the rate schedule. This value is used to normalize the precipitation.
-
-IDF example:
-
-```idf
-Site:Precipitation,
-  ScheduledAndDesignLevel, !- Precipitation Model Type
-  0.75,                    !- Design Level Total Annual Precipitation {m/yr}
-  PrecipitationSchd,       !- Schedule Name for Precipitation Rates
-  0.80771;                 !- Average Total Annual Precipitation {m/yr}
-```
-
-
-### RoofIrrigation
-
-The RoofIrrigation object is used to describe the amount of irrigation on the ecoroof surface over the course of the simulation runperiod. This object is used to provide irrigation data using Schedule objects that define rates of irrigation in meters per hour. These schedules can be one of two types: Schedule, or SmartSchedule.
-
-#### Field: Irrigation Model Type
-
-Choose irrigation modeling options. Available options are **Schedule** and **SmartSchedule**. The **Schedule** type is used to force an irrigation schedule regardless of the current moisture state of the soil. The **SmartSchedule** type allows the precipitation schedule to be overridden if the current moisture state of the soil is greater than 40% saturated.
-
-#### Field: Irrigation Rate Schedule Name
-
-Name of a schedule defined elsewhere that describes the rate of irrigation. The values in this schedule are the average rate of irrigation in meters per hour.
-
-#### Field: Irrigation Maximum Saturation Threshold
-
-Used with the SmartSchedule option in the Irrigation Model Type field to override the default 40% saturation limit for turning off the irrigation: values of 0 to 100 (percent) can be entered with 40% being the default.
-
-IDF example:
-
-```idf
-RoofIrrigation,
-  Schedule, !- Irrigation Model Type
-  IrrigationSchd; !- Schedule Name for Irrigation Rates
-```
-
-
-### Solar and Visible Spectrum Objects
-
-The next two objects enable users to enter solar and visible spectrum which is used to calculate the thermal and visual performance of windows if their glazings are defined with full spectral data. EnergyPlus versions 8.0 and older hard-wired the solar and visible spectrum. The solar spectrum assumes air mass 1.5 terrestrial solar global spectral irradiance values (W/m2-micron) on a 37o tilted surface, based on ISO 9845-1 and ASTM E 892; derived from Optics5 data file ISO-9845GlobalNorm.std, 10-14-99. The visible/photopic spectrum is based on CIE 1931 observer; ISO/CIE 10527, CIE Standard Calorimetric Observers; derived from Optics5 data file "CIE 1931 Color Match from E308.txt", which is the same as WINDOW4 file Cie31t.dat.
-
-### Site:SolarAndVisibleSpectrum
-
-The SolarAndVisibleSpectrum object is used to specify the solar and visible spectrum data which is used as spectral weighting function to calculate the window performance (transmittance and absorptance) in EnergyPlus. This is a unique object, if it is missing from an IDF file, the default (same as EnergyPlus version 8.0) solar and visible spectrum data will be used.
-
-#### Field: Name
-
-This field specifies the name of the SolarAndVisibleSpectrum object.
-
-#### Field: Spectrum Data Method
-
-This field specifies the method used to enter the spectrum data. Two choices are available: Default and UserDefined. The choice Default will continue to use the hard-wired spectrum data in EnergyPlus (for backward compatibility). The choice UserDefined allows users to specify custom solar and visible spectrum data. The default choice is Default.
-
-#### Field: Solar Spectrum Data Name
-
-This field is required if the Spectrum Data Method is set to UserDefined. This field references a spectrum dataset for solar.
-
-#### Field: Visible Spectrum Data Name
-
-This field is required if the Spectrum Data Method is set to UserDefined. This field references a spectrum dataset for visible.
-
-IDF example:
-
-```idf
-Site:SolarAndVisibleSpectrum,
-  LocalSpectrum,             !- Name
-  UserDefined,               !- Spectrum Data Method: Default, UserDefined
-  SolarSpectrum,             !- Solar Spectrum Data Object Name
-  VisibleSpectrum;           !- Visible Spectrum Data Object
-```
-
-
-### Site:SpectrumData
-
-The Site:SpectrumData object holds the user defined solar or visible spectrum data. For solar spectrum, up to 107 pairs of (wavelength, spectrum) can be entered. For visible spectrum, up to 81 pairs can be entered.
-
-#### Field: Name
-
-This field specifies the name of the SpectrumData object. The name must be unique across all SpectrumData objects.
-
-#### Field: Spectrum Data Type
-
-This field specifies the type of spectrum data. Choices are Solar and Visible.
-
-#### Field: Wavelength &lt;n&gt;
-
-This field specifies the nth wavelength in micron.
-
-#### Field: Spectrum &lt;n&gt;
-
-This field specifies the nth spectrum corresponding to the nth wavelength.
-
-IDF example:
-
-```idf
-Site:SpectrumData,
-  SolarSpectrum,             !- Name
-  Solar,                     !- Spectrum Data Type
-  0.3,0,                     !- up to 107 pair of (wavelength, spectrum)
-  0.305,3.4,
-  0.31,15.6,
-  0.315,41.1,
-  0.32,71.2,
-  0.325,100.2,
-  0.33,152.4,
-  0.335,155.6,
-  0.34,179.4,
-  0.345,186.7,
-  0.35,212,
-  0.36,240.5,
-  0.37,324,
-  0.38,362.4,
-  ...;
-```
-
-
-### Climate Group Outputs
-
-Climate related variables appear in two places for EnergyPlus outputs. Certain objects that are invariant throughout a simulation period have lines appear in the eplusout.eio file. For descriptions of this reporting, please see the Output Details and Examples document.
-
-### Weather Data Related Outputs
-
-Variables related to ambient environment data are available at timestep and higher resolutions. Below is a variable dictionary of these variables and subsequent definitions:
-
-* Zone,Average,Site Outdoor Air Drybulb Temperature [C]
-
-* Zone,Average,Site Outdoor Air Dewpoint Temperature [C]
-
-* Zone,Average,Site Outdoor Air Wetbulb Temperature [C]
-
-* Zone,Average,Site Outdoor Air Humidity Ratio [kgWater/kgAir]
-
-* Zone,Average,Site Outdoor Air Relative Humidity [%]
-
-* Zone,Average,Site Outdoor Air Barometric Pressure [Pa]
-
-* Zone,Average,Site Wind Speed [m/s]
-
-* Zone,Average,Site Wind Direction [deg]
-
-* Zone,Average,Site Sky Temperature [C]
-
-* Zone,Average,Site Horizontal Infrared Radiation Rate per Area [W/m2]
-
-* Zone,Average,Site Diffuse Solar Radiation Rate per Area [W/m2]
-
-* Zone,Average,Site Direct Solar Radiation Rate per Area [W/m2]
-
-* Zone,Sum,Site Precipitation Depth [m]
-
-* Zone,Average,Site Ground Reflected Solar Radiation Rate per Area [W/m2]
-
-* Zone,Average,Site Ground Temperature [C]
-
-* Zone,Average,Site Surface Ground Temperature [C]
-
-* Zone,Average,Site Deep Ground Temperature [C]
-
-* Zone,Average,Site Simple Factor Model Ground Temperature [C]
-
-* Zone,Average,Site Outdoor Air Enthalpy [J/kg]
-
-* Zone,Average,Site Outdoor Air Density [kg/m3]
-
-* Zone,Average,Site Solar Azimuth Angle [deg]
-
-* Zone,Average,Site Solar Altitude Angle [deg]
-
-* Zone,Average,Site Solar Hour Angle [deg]
-
-* Zone,Average,Site Rain Status []
-
-* Zone,Average,Site Snow on Ground Status []
-
-* Zone,Average,Site Exterior Horizontal Sky Illuminance [lux]
-
-* Zone,Average,Site Exterior Horizontal Beam Illuminance [lux]
-
-* Zone,Average,Site Exterior Beam Normal Illuminance [lux]
-
-* Zone,Average,Site Sky Diffuse Solar Radiation Luminous Efficacy [lum/W]
-
-* Zone,Average,Site Beam Solar Radiation Luminous Efficacy [lum/W]
-
-* Zone,Average,Site Daylighting Model Sky Clearness []
-
-* Zone,Average,Sky Brightness for Daylighting Calculation []
-
-* Zone,Average,Site Daylight Saving Time Status []
-
-* Zone,Average,Site Day Type Index []
-
-* Zone,Average,Site Mains Water Temperature [C]
-
-* HVAC,Average,Site Precipitation Rate [m/s]
-
-* HVAC,Sum,Site Precipitation Depth [m]
-
-* HVAC,Sum,Water System Roof Irrigation Scheduled Depth[m]
-
-* HVAC,Sum,Water System Roof Irrigation Actual Depth[m]
-
-Note that these data values may be interpolated from “hour� points (ref: Weather Data Hourly Interpolation). Most of the data values represent the “average� over the reporting resolution period.
-
-#### Site Outdoor Air Drybulb Temperature [C]
-
-This is the outdoor dry-bulb temperature in degrees C.
-
-#### Site Outdoor Air Dewpoint Temperature [C]
-
-This is the outdoor dewpoint temperature in degrees C.
-
-#### Site Outdoor Air Wetbulb Temperature [C]
-
-The outdoor wet-bulb temperature is derived (at the timestep) from the values for dry-bulb temperature, humidity ratio and barometric pressure.
-
-#### Site Outdoor Air Humidity Ratio [kgWater/kgAir]
-
-The outdoor humidity ratio is derived (at the timestep) from the dry-bulb temperature, relative humidity and barometric pressure.
-
-#### Site Outdoor Air Relative Humidity [%]
-
-This is the outdoor relative humidity expressed in percent.
-
-#### Site Outdoor Air Barometric Pressure [Pa]
-
-This is the atmospheric/barometric pressure in Pa.
-
-#### Site Wind Speed [m/s]
-
-This is the outdoor wind speed in m/s.
-
-#### Site Wind Direction [deg]
-
-This is the wind direction (N=0, E=90, S=180, W=270).
-
-#### Site Sky Temperature [C]
-
-The sky temperature is derived from horizontal infrared radiation intensity. It is expressed in degrees C. The default calculation is shown below but this value may be modified by the WeatherProperty:SkyTemperature object. Note that Sigma is the Stefan-Boltzmann constant in the following equation:
-
-<div>\[Sky\;Temperature = {\left( {\frac{{Horizontal\;IR}}{{Sigma}}} \right)^{\frac{1}{4}}} - {273.15_{Conversion\;from\;Kelvin\;to\;Centigrade}}\]</div>
-
-#### Site Horizontal Infrared Radiation Rate per Area [W/m2]
-
-The horizontal infrared radiation intensity is expressed in W/m<sup>2</sup> based, if missing from the weather file, on opaque sky cover, sky emissivity, temperature and other factors. The general calculation of Site Horizontal Infrared Radiation Rate per Area is discussed in both the Engineering Reference and the Auxiliary Programs document.
-
-#### Site Diffuse Solar Radiation Rate per Area [W/m2]
-
-Diffuse solar is the amount of solar radiation in W/m<sup>2</sup> received from the sky (excluding the
-
-solar disk) on a horizontal surface.
-
-#### Site Direct Solar Radiation Rate per Area [W/m2]
-
-Site Direct Solar Radiation Rate per Area is amount of solar radiation in W/m<sup>2</sup> received within a 5.7° field of view centered on the sun. This is also known as Beam Solar.
-
-#### Site Precipitation Depth [m]
-
-This is the amount of liquid precipitation (m). The source of this field may be the weather file or the Site:Precipitation object. The weather file values are in millimeters, but the report here is in meters. Two separate entities are displayed – from the weather file the key value is “Environment�; from the Site:Precipitation object the key value is Site:Precipitation.
-
-If the weather file does not have a liquid precipitation field but does have the present weather fields, then a heuristic calculation is attempted for both flagging when it is raining and the amount of precipitation. If the weather file does have liquid precipitation fields, then the output (e.g. monthly) can be compared with the weather file stat file.
-
-#### Site Ground Reflected Solar Radiation Rate per Area [W/m2]
-
-The ground reflected solar amount (W/m<sup>2</sup>) is derived from the Beam Solar, Diffuse Solar, User specified Ground Reflectance (for month) and Solar Altitude Angle:
-
-<div>\[Groundreflectedsolar = \left( {Beamsolar\cdot COS(SolarAltitudeAngle) + Diffusesolar} \right)\cdot {\rm{Groundreflectanc}}{{\rm{e}}_{{\rm{month}}}}\]</div>
-
-where if the calculation returns a value &lt; 0.0, then 0.0 will be reported.
-
-#### Site Ground Temperature [C]
-
-The ground temperature is reported in degrees C – this is a user-specified input by month.
-
-#### Site Surface Ground Temperature [C]
-
-The ground temperature is reported in degrees C – this is a user-specified input (object: Site:GroundTemperature:Shallow) by month.
-
-#### Site Deep Ground Temperature [C]
-
-The ground temperature is reported in degrees C – this is a user-specified input (object: Site:GroundTemperature:Deep) by month.
-
-#### Site Simple Factor Model Ground Temperature [C]
-
-The Site Simple Factor Model Ground Temperature is reported in degrees C – this is a user-specified input (object: Site:GroundTemperature:FCfactorMethod) by month or gleaned from the weather file as noted in the description of the object.
-
-#### Site Outdoor Air Enthalpy [J/kg]
-
-Outdoor enthalpy is derived at each timestep from the Site Outdoor Air Drybulb Temperatureand the Site Outdoor Air Humidity Ratio. It is reported in J/kg.
-
-#### Site Outdoor Air Density [kg/m3]
-
-Outdoor air density is derived at each timestep from the Site Outdoor Air Barometric Pressure, the Outdoor Dry-bulb temperature and the Outdoor Humidity Ratio. It is reported in units kg/m<sup>3</sup>.
-
-#### Site Solar Azimuth Angle [deg]
-
-The Solar Azimuth Angle (f) is measured from the North (clockwise) and is expressed in degrees. This is shown more clearly in the following figure.
-
-![HorizonCoordinates](media/image020.png)
-
-Figure 9. Solar Position Illustration
-
-#### Site Solar Altitude Angle [deg]
-
-The Solar Altitude Angle (b) is the angle of the sun above the horizontal (degrees).
-
-#### Site Solar Hour Angle [deg]
-
-The Solar Hour Angle (*H*) gives the apparent solar time for the current time period (degrees). It is common astronomical practice to express the hour angle in hours, minutes and seconds of time rather than in degrees. You can convert the hour angle displayed from EnergyPlus to time by dividing by 15. (Note that 1 hour is equivalent to 15 degrees;  360° of the Earth’s rotation takes place every 24 hours.)  The relationship of angles in degrees to time is shown in the following table:
-
-Table 6. Relationship of Angles (degrees) to Time
-
-<table class="table table-striped">
-<tr>
-<th>Unit of Angle</th>
-<th>Equivalent time</th>
-</tr>
-<tr>
-<td>1 radian</td>
-<td>3.819719 hours</td>
-</tr>
-<tr>
-<td>1 degree</td>
-<td>4 minutes</td>
-</tr>
-<tr>
-<td>1 arcmin</td>
-<td>4 seconds</td>
-</tr>
-<tr>
-<td>1 arcsec</td>
-<td>0.066667 seconds</td>
-</tr>
-</table>
-
-#### Site Rain Status []
-
-This field shows whether or not (1=yes, 0=no) the weather shows “raining�. For a Design Day, one can denote rain for the entire day but not timestep by timestep. Weather files may indicate rain for a single time interval. This is an “averaged� field – thus a 1 shown for a time period (e.g. daily reporting) means that it was raining during each timestep of that period.
-
-#### Site Snow on Ground Status []
-
-This field shows whether or not (1=yes, 0=no) the weather shows “snow on the ground�. For a Design Day, one can denote snow for the entire day but not timestep by timestep. Weather files may indicate snow (snow depth) for a single time interval. This is an “averaged� field – thus a 1 shown for a time period (e.g. daily reporting) means that there was snow on the ground during each timestep of that period.
-
-#### Site Daylight Saving Time Status []
-
-This field shows when daylight saving time (1=yes, 0=no) is in effect. Though shown as an average variable, this value is only set on a daily basis.
-
-#### Site Day Type Index []
-
-This field shows what “day type� the current day is. Daytypes are (1=Sunday, 2=Monday, etc.) with Holiday=8, SummerDesignDay=9, WinterDesignDay=10, CustomDay1=11, CustomDay2=12. Though shown as an average variable, this value is only set on a daily basis.
-
-#### Site Mains Water Temperature [C]
-
-The value of the Water Mains Temperature is reported in C following the calculation shown in the Water Mains Temperature object.
-
-#### Site Precipitation Rate [m/s]
-
-#### Site Precipitation Depth [m]
-
-The rate and quantity of precipitation at the site. These outputs are only available if a Site Precipication object is used. Precipitation is measured in meters.
-
-#### Water System Roof Irrigation Scheduled Depth[m]
-
-This is the scheduled amount of irrigation for the green roof (ecoroof) based on the user input. Amount is measured in meters.
-
-#### Water System Roof Irrigation Actual Depth[m]
-
-This is the actual amount of irrigation for the green roof (ecoroof) based on the scheduled user input and moisture state/saturation of the soil. Amount is measured in meters.
-
-### Outputs for local temperature/wind speed calculations
-
-Local atmospheric properties for outdoor air temperature and wind speed are separately calculated and reported for all zones, surfaces, and outdoor air nodes. The output variables are associated with their respective objects:
-
-* Zone,Average,Zone Outdoor Air Drybulb Temperature [C]
-
-* Zone,Average,Zone Outdoor Air Wetbulb Temperature [C]
-
-* Zone,Average,Zone Outdoor Air Wind Speed [m/s]
-
-* Zone,Average,Surface Ext Outdoor Dry Bulb [C]
-
-* Zone,Average,Surface Ext Outdoor Wet Bulb [C]
-
-* Zone,Average,Surface Ext Wind Speed [m/s]
-
-* HVAC,Average,System Node Temperature [C]        (for OUTDOOR AIR NODE object)
-
-
-
-
-#### Zone Outdoor Air Drybulb Temperature [C]
-
-The outdoor air dry-bulb temperature calculated at the height above ground of the zone centroid.
-
-#### Zone Outdoor Air Wetbulb Temperature [C]
-
-The outdoor air wet-bulb temperature calculated at the height above ground of the zone centroid.
-
-#### Zone Outdoor Air Wind Speed [m/s]
-
-The outdoor wind speed calculated at the height above ground of the zone centroid.
-
-#### Surface Ext Outdoor Dry Bulb [C]
-
-The outdoor air dry-bulb temperature calculated at the height above ground of the surface centroid.
-
-#### Surface Ext Outdoor Wet Bulb [C]
-
-The outdoor air wet-bulb temperature calculated at the height above ground of the surface centroid.
-
-#### Surface Ext Wind Speed [m/s]
-
-The outdoor wind speed calculated at the height above ground of the surface centroid.
-
-#### System Node Temperature [C]
-
-When reporting for the **OutdoorAir:Node** object, this is the outdoor air dry-bulb temperature calculated at the height above ground of the node, if height is specified in the input.
-
-Group -- Schedules
-------------------
-
-This group of objects allows the user to influence scheduling of many items (such as occupancy density, lighting, thermostatic controls, occupancy activity). In addition, schedules are used to control shading element density on the building.
-
-EnergyPlus schedules consist of three pieces:  a day description, a week description, and an annual description. An optional element is the schedule type. Each description level builds off the previous sub-level. The day description is simply a name and the values that span the 24 hours in a day to be associated with that name. The week description also has an identifier (name) and twelve additional names corresponding to previously defined day descriptions. There are names for each individual day of the week plus holiday, summer design day, winter design day and two more custom day designations. Finally, the annual schedule contains an identifier and the names and FROM-THROUGH dates of the week schedules associate with this annual schedule. The annual schedule can have several FROM-THROUGH date pairs.  One type of schedule reads the values from an external file to facilitate the incorporation of monitored data or factors that change throughout the year.
-
-Schedules are processed by the EnergyPlus Schedule Manager, stored within the Schedule Manager and are accessed through module routines to get the basic values (timestep, hourly, etc). Values are resolved at the Zone Timestep frequency and carry through any HVAC timesteps.
-
-### Day Type
-
-A brief description of “Day Type� which is used in the SizingPeriod objects, RunPeriodControl:SpecialDays object, the Sizing objects and also used by reference in the Schedule:Week:Daily object (discussed later in this section).
-
-Schedules work on days of the week as well as certain specially designated days. Days of the week are the normal – Sunday, Monday, Tuesday, Wednesday, Thursday, Friday and Saturday. Special day types that can be designated are: Holiday, SummerDesignDay, WinterDesignDay, CustomDay1, CustomDay2. These day types can be used at the user’s convenience to designate special scheduling (e.g. lights, electric equipment, set point temperatures) using these days as reference.
-
-For example, a normal office building may have normal “occupancy� rules during the weekdays but significantly different use on weekend. For this, you would set up rules/schedules based on the weekdays (Monday through Friday, in the US) and different rules/schedules for the weekend (Saturday and Sunday, in the US). However, you could also specially designate SummerDesignDay and WinterDesignDay schedules for sizing calculations. These schedules can be activated by setting the Day Type field in the Design Day object to the appropriate season (**SummerDesignDay** for cooling design calculations; **WinterDesignDay** for heating design calculations).
-
-In a different building, such as a theater/playhouse, the building may only have occupancy during certain weeks of the year and/or certain hours of certain days. If it was every week, you could designate the appropriate values during the “regular� days (Sunday through Saturday). But this would also be an ideal application for the “CustomDay1� and/or “CustomDay2�. Here you would set the significant occupancy, lighting, and other schedules for the custom days and use unoccupied values for the normal weekdays. Then, using a weather file and setting special day periods as appropriate, you will get the “picture� of the building usage during the appropriate periods.
-
-### ScheduleTypeLimits
-
-Schedule types can be used to validate portions of the other schedules. Hourly day schedules, for example, are validated by range -- minimum/maximum (if entered) -- as well as numeric type (continuous or discrete). Annual schedules, on the other hand, are only validated for range – as the numeric type validation has already been done.
-
-#### Field: Name
-
-This alpha field should contain a unique (within the schedule types) designator. It is referenced wherever Schedule Type Limits Names can be referenced.
-
-#### Field: Lower Limit Value
-
-In this field, the lower (minimum) limit value for the schedule type should be entered. If this field is left blank, then the schedule type is not limited to a minimum/maximum value range.
-
-#### Field: Upper Limit Value
-
-In this field, the upper (maximum) limit value for the schedule type should be entered. If this field is left blank, then the schedule type is not limited to a minimum/maximum value range.
-
-#### Field: Numeric Type
-
-This field designates how the range values are validated. Using **Continuous** in this field allows for all numbers, including fractional amounts, within the range to be valid. Using **Discrete** in this field allows only integer values between the minimum and maximum range values to be valid.
-
-#### Field: Unit Type
-
-This field is used to indicate the kind of units that may be associated with the schedule that references the ScheduleTypeLimits object. It is used by IDF Editor to display the appropriate SI and IP units. This field is not used by EnergyPlus. The available options are shown below. If none of these options are appropriate, select **Dimensionless.**
-
-- Dimensionless
-
-- Temperature
-
-- DeltaTemperature
-
-- PrecipitationRate
-
-- Angle
-
-- Convection Coefficient
-
-- Activity Level
-
-- Velocity
-
-- Capacity
-
-- Power
-
-- Availability
-
-- Percent
-
-- Control
-
-- Mode
-
-Several IDF Examples will illustrate the use:
-
-```idf
-ScheduleTypeLimits,Any Number;  ! Not limited
-ScheduleTypeLimits,Fraction, 0.0 , 1.0 ,CONTINUOUS;
-ScheduleTypeLimits,Temperature,-60,200,CONTINUOUS;
-ScheduleTypeLimits,Control Type,0,4,DISCRETE;
-ScheduleTypeLimits,On/Off,0,1,DISCRETE;
-```
-
-
-### Day Schedules
-
-The day schedules perform the assignment of pieces of information across a 24 hour day. This can occur in various fashions including a 1-per hour assignment, a user specified interval scheme or a list of values that represent an hour or portion of an hour.
-
-### Schedule:Day:Hourly
-
-The Schedule:Day:Hourly contains an hour-by-hour profile for a single simulation day.
-
-#### Field: Name
-
-This field should contain a unique (within all DaySchedules) designation for this schedule. It is referenced by WeekSchedules to define the appropriate schedule values.
-
-#### Field: Schedule Type Limits Name
-
-This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
-
-#### Field: Hour Values (1-24)
-
-These fields contain the hourly values for each of the 24 hours in a day. (Hour field 1 represents clock time 00:00:01 AM to 1:00:00 AM, hour field 2 is 1:00:01 AM to 2:00:00 AM, etc.)  The values in these fields will be passed to the simulation as indicated for “scheduled� items.
-
-An IDF example:
-
-```idf
-Schedule:Day:Hourly, Day On Peak, Fraction,
-  0.,0.,0.,0.,0.,0.,0.,0.,0.,1.,1.,1.,1.,1.,1.,1.,1.,1.,0.,0.,0.,0.,0.,0.;
-```
-
-
-### Schedule:Day:Interval
-
-The Schedule:Day:Interval introduces a slightly different way of entering the schedule values for a day. Using the intervals, you can shorten the “hourly� input of the “Schedule:Day:Hourly� object to 2 fields. And, more importantly, you can enter an interval that represents only a portion of an hour. Schedule values are “given� to the simulation at the zone timestep, so there is also a possibility of “interpolation� from the entries used in this object to the value used in the simulation.
-
-#### Field: Name
-
-This field should contain a unique (within all DaySchedules) designation for this schedule. It is referenced by WeekSchedules to define the appropriate schedule values.
-
-#### Field: Schedule Type Limits Name
-
-This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
-
-#### Field: Interpolate to Timestep
-
-The value contained in this field directs how to apply values that aren’t coincident with the given timestep (ref: Timestep) intervals. If “Yes� is entered, then any intervals entered here will be interpolated/averaged and that value will be used at the appropriate minute in the hour. If “No� is entered, then the value that occurs on the appropriate minute in the hour will be used as the schedule value.
-
-For example, if “yes� is entered and the interval is every 15 minutes (say a value of 0 for the first 15 minutes, then .5 for the second 15 minutes) AND there is a 10 minute timestep for the simulation: the value at 10 minutes will be 0 and the value at 20 minutes will be .25. For the same input entries but “no� for this field, the value at 10 minutes will be 0 and the value at 20 minutes will be .5.
-
-#### Field-Set: Time and Value (extensible object)
-
-To specify each interval, both an “until� time (which includes the designated time) and the value must be given.
-
-#### Field: Time
-
-The value of each field should represent clock time (standard) in the format “Until: HH:MM�. 24 hour clock format (i.e. 1PM is 13:00) is used. Note that Until: 7:00 includes all times up through 07:00 or 7am.
-
-#### Field: Value
-
-This represents the actual value to be passed to the simulation at the appropriate timestep. (Using interpolation value as shown above). Limits on the values are indicated by the Schedule Type Limits Name field of this object.
-
-And an example of use:
-
-```idf
-Schedule:Day:Interval,
-    dd winter rel humidity,  !- Name
-    Percent,                 !- Schedule Type Limits Name
-    No,                      !- Interpolate to Timestep
-    until: 24:00,             !- Time 1
-    74;                      !- Value Until Time 1
-```
-
-
-### Schedule:Day:List
-
-To facilitate possible matches to externally generated data intervals, this object has been included. In similar fashion to the Schedule:Day:Interval object, this object can also include “sub-hourly� values but must represent a complete day in its list of values.
-
-#### Field: Name
-
-This field should contain a unique (within all day schedules) designation for this schedule. It is referenced by week schedules to define the appropriate schedule values.
-
-#### Field: Schedule Type Limits Name
-
-This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
-
-#### Field: Interpolate to Timestep
-
-The value contained in this field directs how to apply values that aren’t coincident with the given timestep (ref: Timestep) intervals. If “Yes� is entered, then any intervals entered here will be interpolated/averaged and that value will be used at the appropriate minute in the hour. If “No� is entered, then the value that occurs on the appropriate minute in the hour will be used as the schedule value.
-
-For example, if “yes� is entered and the minutes per item is 15 minutes (say a value of 0 for the first 15 minutes, then .5 for the second 15 minutes) AND there is a 10 minute timestep for the simulation: the value at 10 minutes will be 0 and the value at 20 minutes will be .25. For the same input entries but “no� for this field, the value at 10 minutes will be 0 and the value at 20 minutes will be .5.
-
-#### Field: Minutes Per Item
-
-This field allows the “list� interval to be specified in the number of minutes for each item. The value here must be &lt;= 60 and evenly divisible into 60 (same as the timestep limits).
-
-#### Field Value 1 (same definition for each value – up to 1440 (24\*60) allowed)
-
-This is the value to be used for the specified number of minutes.
-
-For example:
-
-```idf
-Schedule:Day:List,
-  Myschedule,  ! name
-  Fraction,   ! Schedule type
-  No,   ! Interpolate value
-  30,   ! Minutes per item
-  0.0,  ! from 00:01 to 00:30
-  0.5,  ! from 00:31 to 01:00
-  <snipped>
-```
-
-
-
-
-### Week Schedule(s)
-
-The week schedule object(s) perform the task of assigning the day schedule to day types in the simulation. The basic week schedule is shown next.
-
-### Schedule:Week:Daily
-
-#### Field: Name
-
-This field should contain a unique (within all WeekSchedules) designation for this schedule. It is referenced by Schedules to define the appropriate schedule values.
-
-#### Field: Schedule Day Name Fields (12 day types – Sunday, Monday, … )
-
-These fields contain day schedule names for the appropriate day types. Days of the week (or special days as described earlier) will then use the indicated hourly profile as the actual schedule value.
-
-An IDF example:
-
-```idf
-Schedule:Week:Daily, Week on Peak,
-        Day On Peak,Day On Peak,Day On Peak,
-        Day On Peak,Day On Peak,Day On Peak,
-        Day On Peak,Day On Peak,Day On Peak,
-        Day On Peak,Day On Peak,Day On Peak;
-```
-
-
-### Schedule:Week:Compact
-
-Further flexibility can be realized by using the Schedule:Week:Compact object. In this the fields, after the name is given, a “for� field is given for the days to be assigned and then a dayschedule name is used.
-
-#### Field:Name
-
-This field should contain a unique (within all WeekSchedules) designation for this schedule. It is referenced by Schedules to define the appropriate schedule values.
-
-#### Field-Set – DayType List\#, Schedule:Day Name \#
-
-Each assignment is made in a pair-wise fashion. First the “days� assignment and then the dayschedule name to be assigned. The entire set of day types must be assigned or an error will result.
-
-#### Field: DayType List \#
-
-This field can optionally contain the prefix “For� for clarity. Multiple choices may then be combined on the line. Choices are: Weekdays, Weekends, Holidays, Alldays, SummerDesignDay, WinterDesignDay, Sunday, Monday, Tuesday, Wednesday, Thursday, Friday, Saturday, CustomDay1, CustomDay2. In fields after the first “for�, AllOtherDays may also be used. Note that the colon (:) after the For is optional but is suggested for readability.
-
-#### Field: Schedule:Day Name \#
-
-This field contains the name of the day schedule (any of the Schedule:Day object names) that is to be applied for the days referenced in the prior field.
-
-Some IDF examples:
-
-```idf
-Schedule:Week:Compact, Week on Peak,
-        For: AllDays,
-        Day On Peak;
-Schedule:Week:Compact, WeekDays on Peak,
-        WeekDays,
-        Day On Peak,
-        AllOtherDays
-        Day Off Peak;
-```
-
-
-### Schedule:Year
-
-The yearly schedule is used to cover the entire year using references to week schedules (which in turn reference day schedules). If the entered schedule does not cover the entire year, a fatal error will result.
-
-#### Field: Name
-
-This field should contain a unique (between Schedule:Year, Schedule:Compact, and Schedule:File) designation for the schedule. It is referenced by various “scheduled� items (e.g. Lights, People, Infiltration) to define the appropriate schedule values.
-
-#### Field: Schedule Type Limits Name
-
-This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
-
-#### Field Set (WeekSchedule, Start Month and Day, End Month and Day)
-
-Each of the designated fields is used to fully define the schedule values for the indicated time period). Up to 53 sets can be used. An error will be noted and EnergyPlus will be terminated if an incomplete set is entered. Missing time periods will also be noted as warning errors; for these time periods a zero (0.0) value will be returned when a schedule value is requested. Each of the sets has the following 5 fields:
-
-#### Field: Schedule Week Name \#
-
-This field contains the appropriate WeekSchedule name for the designated time period.
-
-#### Field: Start Month \#
-
-This numeric field is the starting month for the schedule time period.
-
-#### Field: Start Day \#
-
-This numeric field is the starting day for the schedule time period.
-
-#### Field: End Month \#
-
-This numeric field is the ending month for the schedule time period.
-
-#### Field: End Day \#
-
-This numeric field is the ending day for the schedule time period.
-
-
-
-Note that there are many possible periods to be described. An IDF example with a single period:
-
-```idf
-Schedule:Year, On Peak, Fraction,
-        Week On Peak, 1,1, 12,31;
-```
-
-
-And a multiple period illustration:
-
-```idf
-Schedule:Year,CoolingCoilAvailSched,Fraction,
-        FanAndCoilAllOffWeekSched, 1,1, 3,31,
-        FanAndCoilSummerWeekSched, 4,1, 9,30,
-        FanAndCoilAllOffWeekSched, 10,1, 12,31;
-```
-
-
-The following definition will generate an error (if any scheduled items are used in the simulation):
-
-Schedule:Year,MySchedule,Fraction,4,1,9,30;
-
-### Schedule:Compact
-
-For flexibility, a schedule can be entered in “one fell swoop�. Using the Schedule:Compact object, all the features of the schedule components are accessed in a single command. Like the “regular� schedule object, each schedule:compact entry must cover all the days for a year. Additionally, the validations for DaySchedule (i.e. must have values for all 24 hours) and WeekSchedule (i.e. must have values for all day types) will apply. Schedule values are “given� to the simulation at the zone timestep, so there is also a possibility of “interpolation� from the entries used in this object to the value used in the simulation.
-
-This object is an unusual object for description. For the data the number of fields and position are not set, they cannot really be described in the usual Field \# manner. Thus, the following description will list the fields and order in which they must be used in the object. The name and schedule type are the exceptions:
-
-#### Field: Name
-
-This field should contain a unique (between Schedule:Year, Schedule:Compact, and Schedule:File) designation for the schedule. It is referenced by various “scheduled� items (e.g. Lights, People, Infiltration) to define the appropriate schedule values.
-
-#### Field: Schedule Type Limits Name
-
-This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
-
-#### Field-Set (Through, For, Interpolate, Until, Value)
-
-Each compact schedule must contain the elements Through (date), For (days), Interpolate (optional), Until (time of day) and Value. In general, each of the “titled� fields must include the “title�. Note that the colon (:) after these elements (Through, For, Until) is optional but is suggested for readability.
-
-#### Field: Through
-
-This field starts with “Through:� and contains the ending date for the schedule period (may be more than one). Refer to Table 3. Date Field Interpretation for information on date entry – note that only Month-Day combinations are allowed for this field. Each “through� field generates a new WeekSchedule named “Schedule Name�\_wk\_\# where \# is the sequential number for this compact schedule.
-
-#### Field: For
-
-This field starts with “For:� and contains the applicable days (reference the compact week schedule object above for complete description) for the 24 hour period that must be described. Each “for� field generates a new DaySchedule named “Schedule Name�\_dy\_\# where \# is the sequential number for this compact schedule.
-
-#### Field: Interpolate (optional)
-
-This field, if used, starts with “Interpolate:� and contains the word “Yes� or “No�. If this field is not used, it should not be blank – rather just have the following field appear in this slot. The definition of “Interpolate� in this context is shown in the interval day schedule above.
-
-#### Field: Until
-
-This field contains the ending time (again, reference the interval day schedule discussion above) for the current days and day schedule being defined.
-
-#### Field: Value
-
-Finally, the value field is the schedule value for the specified time interval.
-
-
-
-
-
-And, some IDF examples:
-
-```idf
-Schedule:Compact,
-  POFF,    !- Name
-  Fraction,  !- Schedule Type Limits Name
-  Through: 4/30,
-  For: AllDays,
-  Until: 24:00, 1.0,
-  Through: 12/31,
-  For: Weekdays,
-   Until: 7:00,   .1,
-   Until: 17:00, 1.0,
-   Until: 24:00,  .1,
-  For: Weekends Holidays,
-   Until: 24:00,  .1,
-  For: AllOtherDays,
-   Until: 24:00,  .1;
-
-
-! Schedule Continuous
-Schedule:Compact,
-  Continuous,
-  on/off,
-  Through: 12/31,
-  For: AllDays,
-  Until: 24:00, 1.0;
-
-
-! Schedule Daytime Ventilation
-Schedule:Compact,
-  Daytime Ventilation,
-  Fraction,
-  Through: 12/31,
-  For: Weekdays SummerDesignDay,
-  Until: 08:00, 0.0,
-  Until: 18:00, 1.0,
-  Until: 24:00, 0.0,
-  For: Weekends WinterDesignDay,
-  Until: 10:00, 0.0,
-  Until: 16:00, 1.0,
-  Until: 24:00, 0.0,
-  For: Holidays AllOtherDays,
-  Until: 24:00, 0.0;
-```
-
-
-### Schedule:Constant
-
-The constant schedule is used to assign a constant hourly value. This schedule is created when a fixed hourly value is desired to represent a period of interest (e.g., always on operation mode for supply air fan).
-
-#### Field: Name
-
-This field should contain a unique name designation for this schedule. It is referenced by Schedules to define the appropriate schedule value.
-
-#### Field: Schedule Type Limits Name
-
-This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
-
-#### Field: Hourly Value
-
-This field contains a constant real value. A fixed value is assigned as an hourly value.
-
-An IDF example:
-
-```idf
-Schedule:Constant,
-  AlwaysOn,                  !- Name
-  On/Off,                    !- Schedule Type Limits Name
-  1.0;                       !- Hourly Value
-
-
-ScheduleTypeLimits,
-    On/Off,                  !- Name
-    0,                       !- Lower Limit Value
-    1,                       !- Upper Limit Value
-    DISCRETE,                !- Numeric Type
-    Availability;            !- Unit Type
-```
-
-
-
-
-### Schedule:File
-
-At times, data is available from a building being monitored or for factors that change throughout the year. The Schedule:File object allows this type of data to be used in EnergyPlus as a schedule. Schedule:File can also be used to read in hourly or sub-hourly schedules computed by other software or developed in a spreadsheet or other utility.
-
-The format for the data file referenced is a text file with values separated by commas (or other optional delimiters) with one line per hour. The file may contain header lines that are skipped. The file should contain values for an entire year (8760 or 8784 hours of data) or a warning message will be issued. Multiple schedules may be created using a single external data file or multiple external data files may be used.  The first row of data must be for January 1, hour 1 (or timestep 1 for subhourly files).
-
-Schedule:File may be used along with the FuelFactors object and TDV files in the DataSets directory to compute Time Dependent Valuation based source energy as used by the California Energy Commission’s Title 24 Energy Code. See Fuel Factor for more discussion on Time Dependent Valuation.
-
-Two optional fields: **Interpolate to Timestep** and **Minutes per Item** allow for the input of sub-hourly schedules (similar to the Schedule:Day:List object).
-
-#### Field: Name
-
-This field should contain a unique (between Schedule:Year, Schedule:Compact, and Schedule:File) designation for the schedule. It is referenced by various “scheduled� items (e.g. Lights, People, Infiltration, FuelFactors) to define the appropriate schedule values.
-
-#### Field: Schedule Type Limits Name
-
-This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see ScheduleTypeLimits object above), then the restrictions from the referenced object will be used to validate the hourly field values (below).
-
-#### Field: File Name
-
-This field contains the name of the file that contains the data for the schedule. The field should include a full path with file name, for best results. The field must be &lt;= 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
-
-#### Field: Column Number
-
-The column that contains the value to be used in the schedule. The first column is column one. If no data for a row appears for a referenced column the value of zero is used for the schedule value for that hour.
-
-#### Field: Rows to Skip at Top
-
-Many times the data in a file contains rows (lines) that are describing the files or contain the names of each column. These rows need to be skipped and the number of skipped rows should be entered for this field. The next row after the skipped rows must contain data for January 1, hour 1.
-
-#### Field: Number of Hours of Data
-
-The value entered in this field should be either 8760 or 8784 as the number of hours of data. 8760 does not include the extra 24 hours for a leap year (if needed).  8784 will include the possibility of leap year data which can be processed according to leap year indicators in the weather file or specified elsewhere. Note if the simulation does not have a leap year specified but the schedule file contains 8784 hours of data, the first 8760 hours of data will be used. The schedule manager will not know to skip the 24 hours representing Feburary 29.
-
-#### Field: Column Separator
-
-This field specifies the character used to separate columns of data if the file has more than one column. The choices are: Comma, Tab, Fixed (spaces fill each column to a fixed width), or Semicolon. The default is Comma.
-
-#### Field: Interpolate to Timestep
-
-The value contained in this field directs how to apply values that aren’t coincident with the given timestep (ref: TimeStep object) intervals. If “Yes� is entered, then any intervals entered here will be interpolated/averaged and that value will be used at the appropriate minute in the hour. If “No� is entered, then the value that occurs on the appropriate minute in the hour will be used as the schedule value.
-
-For example, if “yes� is entered and the minutes per item is 15 minutes (say a value of 0 for the first 15 minutes, then .5 for the second 15 minutes) AND there is a 10 minute timestep for the simulation: the value at 10 minutes will be 0 and the value at 20 minutes will be .25. For the same input entries but “no� for this field, the value at 10 minutes will be 0 and the value at 20 minutes will be .5.
-
-#### Field: Minutes Per Item
-
-This field represents the number of minutes for each item – in this case each line of the file. The value here must be &lt;= 60 and evenly divisible into 60 (same as the timestep limits).
-
-Here is an IDF example:
-
-```idf
-Schedule:File,
-   elecTDVfromCZ01res,   !- Name
-   Any Number,           !- ScheduleType
-   TDV_kBtu_CTZ01.csv,   !- Name of File
-   2,                    !- Column Number
-   4,                    !- Rows to Skip at Top
-   8760,                 !- Number of Hours of Data
-   Comma;                !- Column Separator
-```
-
-
-or with a relational path:
-
-```idf
-Schedule:File,
-   elecTDVfromCZ01res,   !- Name
-   Any Number,           !- ScheduleType
-   DataSets\TDV\TDV_kBtu_CTZ01.csv,   !- Name of File
-   2,                    !- Column Number
-   4;                    !- Rows to Skip at Top
-```
-
-
-A sub-hourly indication. Note that this is identical to an hourly file because there are 60 minutes per item – the number of hours defaults to 8760 and the column separator defaults to a comma. If the number of minutes per item had been, say, 15, then the file would need to contain 8760\*4 or 35,040 rows for this item.
-
-```idf
-  Schedule:File,
-    elecTDVfromCZ06com,      !- Name
-    Any Number,              !- Schedule Type Limits Name
-    DataSets\TDV\TDV_2008_kBtu_CTZ06.csv,  !- File Name
-    1,                       !- Column Number
-    4,                       !- Rows to Skip at Top
-    ,                        !- Number of Hours of Data
-    ,                        !- Column Separator
-    ,                        !- Interpolate to Timestep
-    60;                      !- Minutes per Item
-```
-
-
-### Schedule Outputs
-
-An optional report can be used to gain the values described in the previous Schedule objects. This is a condensed reporting that illustrates the full range of schedule values – in the style of input: DaySchedule, WeekSchedule, Annual Schedule.
-
-! will give them on hourly increments (day schedule resolution)
-
-```idf
-Output:Reports, Schedules, Hourly;
-```
-
-
-! will give them at the timestep of the simulation
-
-```idf
-Output:Reports, Schedules, Timestep;
-```
-
-
-This report is placed on the eplusout.eio file. Details of this reporting are shown in the Output Details and Examples document.
-
-#### Schedule Value Output
-
-Zone,Average,Schedule Value []
-
-#### Schedule Value
-
-This is the schedule value (as given to whatever entity that uses it). It has no units in this context because values may be many different units (i.e. temperatures, fractions, watts). For best results, you may want to apply the schedule name when you use this output variable to avoid output proliferation. For example, the following reporting should yield the values shown above, depending on day of week and day type:
-
-```idf
-Output:Variable,People_Shopping_Sch,Schedule Value,hourly;
-Output:Variable,Activity_Shopping_Sch,Schedule Value,hourly;
-```
-
-
-Group – Surface Construction Elements
--------------------------------------
-
-This group of objects describes the physical properties and configuration for the building envelope and interior elements. That is, the walls, roofs, floors, windows, doors for the building.
-
-### Specifying the Building Envelope
-
-Building element constructions in EnergyPlus are built from the basic thermal and other material property parameters in physical constructions. Materials are specified by types  and named. Constructions are defined by the composition of materials. Finally, surfaces are specified for the building with geometric coordinates as well as referenced constructions.
-
-### Material and Material Properties
-
-There are several material “types� which may be used to describe layers within opaque construction elements. The choice of which of these types to use is left up to the user. However, some guidance as to which material type to use is appropriate before describing each in detail. The opaque types are:
-
-- Material
-
-- Material:NoMass
-
-- Material:AirGap
-
-- Material:RoofVegetation
-
-- Material:InfraredTransparent
-
-Material is the “preferred� type of material. This requires knowledge of many of the thermal properties of the material, but it allows EnergyPlus to take into account the thermal mass of the material and thus allows the evaluation of transient conduction effects. Material:NoMass is similar in nature but only requires the thermal resistance (R-value) rather than the thickness, thermal conductivity, density, and specific heat. Note that using a simple R-value only material forces EnergyPlus to assume steady state heat conduction through this material layer. Finally, Material:AirGap should only be used for an air gap between other layers in a construction. This type assumes that air is sufficiently lightweight to require only an R-value. In addition, since it is not exposed to any external environment, surface properties such as absorptance are not necessary. Material:RoofVegetation is used to help model “green roofs�. Material:InfraredTransparent is used similarly to the NoMass materials. Each of these materials is described in more detail below.
-
-There are several material additions that can be made to the basic material properties. These additional material types are:
-
-- MaterialProperty:MoisturePenetrationDepth:Settings
-
-- MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm
-
-- MaterialProperty:HeatAndMoistureTransfer:Diffusion
-
-- MaterialProperty:HeatAndMoistureTransfer:Settings
-
-- MaterialProperty:HeatAndMoistureTransfer:Redistribution
-
-- MaterialProperty:HeatAndMoistureTransfer:Suction
-
-- MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity
-
-- MaterialProperty:PhaseChange
-
-These material property objects are used in conjunction with the basic material specification and reference back to the name of the basic material type. Without the basic material type specified the program, will give a severe error and terminate. For example, specifying the moisture materials and changing the HeatBalanceAlgorithm to a moisture simulation will allow the moisture simulation to take place.
-
-### Material
-
-This definition should be used when the four main thermal properties (thickness, conductivity, density, and specific heat) of the material are known. This syntax is used to describe opaque construction elements only.
-
-When a Material is used for the Construction of a building surface, care should be taken to not attempt to model assemblies that were not included in the intended scope of applicability for the underlying heat transfer models.  The building surface models are for normal applications to building energy efficiency where the main focus is on assemblies with some thermal resistance. Extremely thin and/or highly conductive material layers should be neglected from the Construction rather than included because they will not contribute to the assembly’s overall thermal resistance or heat capacity. For some cases, thin and/or highly conductive materials are a serious problem for the heat transfer modeling and the values for thickness, conductivity, density and specific heat are checked for appropriateness. This check calculates the Material’s thermal diffusivity from the inputs for conductivity, density, and specific heat and compares it to a maximum threshold of 1.E-5 (m<sup>2</sup>/s). If the diffusivity is above this threshold, then the program checks if the layer is sufficiently thick and may issue a warning if it is too thin and highly conductive.
-
-The absorptance values in this object impart surface properties to the construction and should be applied to the thermally significant inner and outer layers in the overall assembly.  Attempting to trick the program by modeling thin “paint� layers to apply surface properties is not a good idea; the models were not intended to support such strategies.
-
-#### Field: Name
-
-This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data (ref: Construction object).
-
-#### Field: Roughness
-
-This alpha field defines the relative roughness of a particular material layer. This parameter only influences the convection coefficients, more specifically the exterior convection coefficient. A special keyword is expected in this field with the options being “VeryRough�, “Rough�, “MediumRough�, “MediumSmooth�, “Smooth�, and “VerySmooth� in order of roughest to smoothest options.
-
-#### Field: Thickness
-
-This field characterizes the thickness of the material layer in meters. This should be the dimension of the layer in the direction perpendicular to the main path of heat conduction. This value must be a positive. **Modeling layers thinner (less) than 0.003 m is not recommended; rather, add those properties to one of the adjacent layers.**
-
-#### Field: Conductivity
-
-This field is used to enter the thermal conductivity of the material layer. Units for this parameter are W/(m-K). Thermal conductivity must be greater than zero. **Modeling layers with conductivity higher than 5.0 W/(m-K) is not recommended; however, this may be appropriate for non-surfaces such as pipes and TDDs (ref. DaylightingDevice:Tubular object).**
-
-#### Field: Density
-
-This field is used to enter the density of the material layer in units of kg/m<sup>3</sup>. Density must be a positive quantity. **In some cases textbooks and references may use g/m<sup>3</sup>: be careful to not confuse units.**
-
-#### Field: Specific Heat
-
-This field represents the specific heat of the material layer in units of J/(kg-K). Note that these units are most likely different than those reported in textbooks and references which tend to use kJ/(kg-K) or J/(g-K). They were chosen for internal consistency within EnergyPlus. **Only values of specific heat of 100 or larger are allowed. Typical ranges are from 800 to 2000 J/(kg-K).**
-
-#### Field: Thermal Absorptance
-
-The thermal absorptance field in the Material input syntax represents the fraction of incident long wavelength radiation that is absorbed by the material. This parameter is used when calculating the long wavelength radiant exchange between various surfaces and affects the surface heat balances (both inside and outside as appropriate). For long wavelength radiant exchange, thermal emissivity and thermal emittance are equal to thermal absorptance. Values for this field must be between 0.0 and 1.0 (with 1.0 representing “black body� conditions). The default value for this field is 0.9.
-
-#### Field: Solar Absorptance
-
-The solar absorptance field in the Material input syntax represents the fraction of incident  solar radiation that is absorbed by the material. Solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident solar radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate). If solar reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.0 and 1.0. The default value for this field is 0.7.
-
-#### Field: Visible Absorptance
-
-The visible absorptance field in the Material input syntax represents the fraction of incident visible wavelength radiation that is absorbed by the material. Visible wavelength radiation is slightly different than solar radiation in that the visible band of wavelengths is much more narrow while solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident visible radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate) as well as the daylighting calculations. If visible reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.0 and 1.0. The default value for this field is 0.7.
-
-An IDF example:
-
-```idf
-Material,A2 - 4 IN DENSE FACE BRICK,  ! Material Name
- Rough,  ! Roughness
-  0.1014984    ,  ! Thickness {m}
-   1.245296    ,   ! Conductivity {W/M*K}
-   2082.400    ,   ! Density {Kg/M**3}
-  920.4800    ,   ! Specific Heat {J/Kg*K}
-  0.9000000    ,   ! Thermal Absorptance
-  0.9300000    ,   ! Solar Absorptance
-  0.9300000    ;   ! Visible Absorptance
-```
-
-
-### Material:NoMass
-
-Use this definition when only the thermal resistance (R value) of the material is known. This object is used to describe opaque construction elements.
-
-#### Field: Name
-
-This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data (ref: Construction object).
-
-#### Field: Roughness
-
-This alpha field defines the relative roughness of a particular material layer. This parameter only influences the convection coefficients, more specifically the exterior convection coefficient. A  keyword is expected in this field with the options being “**VeryRough**�, “**Rough**�, “**MediumRough**�, “**MediumSmooth**�, “**Smooth**�, and “**VerySmooth**� in order of roughest to smoothest options.
-
-#### Field: Thermal Resistance
-
-This field is used to enter the thermal resistance (R-value) of the material layer. Units for this parameter are (m<sup>2</sup>-K)/W. Thermal resistance must be greater than zero. Note that most R-values in the USA are calculated in Inch-Pound units and must be converted to the SI equivalent.
-
-#### Field: Thermal Absorptance
-
-The thermal absorptance field in the Material input syntax represents the fraction of incident long wavelength radiation that is absorbed by the material. This parameter is used when calculating the long wavelength radiant exchange between various surfaces and affects the surface heat balances (both inside and outside as appropriate). For long wavelength radiant exchange, thermal emissivity and thermal emittance are equal to thermal absorptance. Values for this field must be between 0.0 and 1.0 (with 1.0 representing “black body� conditions). The default value for this field is 0.9.
-
-#### Field: Solar Absorptance
-
-The solar absorptance field in the Material input syntax represents the fraction of incident  solar radiation that is absorbed by the material. Solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident solar radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate). If solar reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.0 and 1.0. The default value for this field is 0.7.
-
-#### Field: Visible Absorptance
-
-The visible absorptance field in the Material input syntax represents the fraction of incident visible wavelength radiation that is absorbed by the material. Visible wavelength radiation is slightly different than solar radiation in that the visible band of wavelengths is much more narrow while solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident visible radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate) as well as the daylighting calculations. If visible reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.0 and 1.0. The default value for this field is 0.7.
-
-An IDF example:
-
-```idf
-Material:NoMass,R13LAYER,  ! Material Name
- Rough,  ! Roughness
-   2.290965    ,  ! Resistance {M**2K/W}
-  0.9000000    ,   ! Thermal Absorptance
-  0.7500000    ,   ! Solar Absorptance
-  0.7500000    ;   ! Visible Absorptance
-```
-
-
-### Material:InfraredTransparent
-
-A Infrared Transparent surface is similar to a resistance-only surface.  The idd object for this type of surface is shown below.  The surface will actually participate in the transfer of visible and solar radiation by doing a wavelength transformation and making all short wave length radiation that is incident on the surface into long wave length radiation and having it participate in the long wavelength radiant exchange.  **Note the ConvectionCoefficient instructions that follow the Infrared Transparent construction object below**.
-
-#### Field: Name
-
-This field contains the unique name (across all Material objects) for the Infrared Transparent material.
-
-A Infrared Transparent surface should not participate in a convective/conductive exchange between the zones it separates.  In order to minimize this effect, the ConvectionCoefficients object must be used for the surfaces referencing the Infrared Transparent (IRT) construction.
-
-An example idf object specification for use with the IRT surface is shown below. Note that surfaces are not described in this example
-
-```idf
-Material:InfraredTransparent,
-    IRTMaterial1;            !- Name
-
-
-Construction,
-    IRTSurface,              !- Name
-    IRTMaterial1;            !- Outside Layer
-
-
-SurfaceProperty:ConvectionCoefficients,
-    Bottom:Top,              !- SurfaceName
-    Outside,                 !- Convection Type 1
-    value,                   !- Convection Value Type 1
-    0.1,                     !- Convection value 1 {W/m2-K}
-    ,                        !- Convection Schedule 1
-    Inside,                  !- Convection Type 2
-    value,                   !- Convection Value Type 2
-    0.1;                     !- Convection value 2 {W/m2-K}
-
-
-SurfaceProperty:ConvectionCoefficients,
-    SecondLevel:Bottom,      !- SurfaceName
-    Outside,                 !- Convection Type 1
-    value,                   !- Convection Value Type 1
-    0.1,                     !- Convection value 1 {W/m2-K}
-    ,                        !- Convection Schedule 1
-    Inside,                  !- Convection Type 2
-    value,                   !- Convection Value Type 2
-    0.1;                     !- Convection value 2 {W/m2-K}
-
-
-SurfaceProperty:ConvectionCoefficients,
-    SecondLevel:Top,         !- SurfaceName
-    Outside,                 !- Convection Type 1
-    value,                   !- Convection Value Type 1
-    0.1,                     !- Convection value 1 {W/m2-K}
-    ,                        !- Convection Schedule 1
-    Inside,                  !- Convection Type 2
-    value,                   !- Convection Value Type 2
-    0.1;                     !- Convection value 2 {W/m2-K}
-
-
-SurfaceProperty:ConvectionCoefficients,
-    ThirdLevel:Bottom,       !- SurfaceName
-    Outside,                 !- Convection Type 1
-    value,                   !- Convection Value Type 1
-    0.1,                     !- Convection value 1 {W/m2-K}
-    ,                        !- Convection Schedule 1
-    Inside,                  !- Convection Type 2
-    value,                   !- Convection Value Type 2
-    0.1;                     !- Convection value 2 {W/m2-K}
-```
-
-
-### Material:AirGap
-
-This material is used to describe the air gap in an opaque construction element. Glass elements use a different property (WindowGas) to describe the air between two glass layers.
-
-#### Field: Name
-
-This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data (ref: Construction object).
-
-#### Field: Thermal Resistance
-
-This field is used to enter the thermal resistance (R-value) of the material layer. Units for this parameter are (m<sup>2</sup>-K)/W. Thermal resistance must be greater than zero. Note that most R-values in the USA are calculated in Inch-Pound units and must be converted to the SI equivalent.
-
-An IDF example:
-
-```idf
-Material:AirGap,B1 - AIRSPACE RESISTANCE,  ! Material Name
-  0.1603675    ;  ! Resistance {M**2K/W}
-```
-
-
-
-### MaterialProperty:MoisturePenetrationDepth:Settings
-
-This material is used to describe the five moisture material properties that are used in the EMPD (Effective Moisture Penetration Depth) heat balance solution algorithm (known there as MoisturePenetrationDepthConductionTransferFunction). The EMPD algorithm is a simplified, lumped moisture model that simulates moisture storage and release from interior surfaces. The model uses "actual" convective mass transfer coefficients that are determined by existing heat and mass transfer relationships, e.g. the Lewis relation. An effective moisture penetration depth may be determined from either experimental or detailed simulation data by using actual surface areas and moisture sorption isotherms.
-
-This moisture model will be used when the appropriate EMPD moisture materials are specified and the Solution Algorithm parameter is set to EMPD.
-
-#### Field: Name
-
-This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data (ref: Construction object).
-
-#### Field: Moisture Penetration Depth
-
-This field is used to enter the effective moisture penetration depth of the material layer. Units for this parameter are (m).
-
-#### Field: Constants to Define Moisture Equilibrium Equation
-
-The next four fields, coefficients “a�, “b�, “c�, and “d�, help define the sorption isotherm curve used for building materials under equilibrium conditions. They are used to define the relationship between the material’s moisture content and the surface air relative humidity (ref: Effective Moisture Penetration Depth (EMPD) Model in the Engineering Reference):
-
-<div>\[U = a{\varphi ^b} + c{\varphi ^d}\]</div>
-
-where
-
-a,b,c,d               = Coefficients to define the relationship between the material’s moisture content and the surface air relative humidity
-
-U                      = Moisture content defined as the mass fraction of water contained in a material [kg/kg]
-
-<span>\(\varphi \)</span>                    = Surface air relative humidity [0 to 1]
-
-#### The next four fields are dimensionless coefficients:
-
-#### Field: Moisture Equation Coefficient a
-
-#### Field: Moisture Equation Coefficient b
-
-#### Field: Moisture Equation Coefficient c
-
-#### Field: Moisture Equation Coefficient d
-
-Ann IDF example showing how it is used in conjunction with Material in synchronous pairs:
-
-
-
-```idf
-  Material,
-    E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Name
-    Smooth,                  !- Roughness
-    1.9050000E-02,           !- Thickness {m}
-    0.7264224,               !- Conductivity {W/m-K}
-    1601.846,                !- Density {kg/m3}
-    836.8000,                !- Specific Heat {J/kg-K}
-    0.9000000,               !- Thermal Absorptance
-    0.9200000,               !- Solar Absorptance
-    0.9200000;               !- Visible Absorptance
-
-
-
-
- MaterialProperty:MoisturePenetrationDepth:Settings,
-    E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Name
-    0.004,                   !- Effective Moisture Penetration Depth {m}
-    0.072549,           !- Moisture Equation Coefficient a {dimensionless}
-    0.397173,           !- Moisture Equation Coefficient b {dimensionless}
-    0.007774,           !- Moisture Equation Coefficient c {dimensionless}
-    11.7057;            !- Moisture Equation Coefficient d {dimensionless}
-
-
-  Material,
-    C10 - 8 IN HW CONCRETE,  !- Name
-    MediumRough,             !- Roughness
-    0.2033016,               !- Thickness {m}
-    1.729577,                !- Conductivity {W/m-K}
-    2242.585,                !- Density {kg/m3}
-    836.8000,                !- Specific Heat {J/kg-K}
-    0.9000000,               !- Thermal Absorptance
-    0.6500000,               !- Solar Absorptance
-    0.6500000;               !- Visible Absorptance
-
-
- MaterialProperty:MoisturePenetrationDepth:Settings,
-    C10 - 8 IN HW CONCRETE,  !- Name
-    0.004,                   !- Effective Moisture Penetration Depth {m}
-    0.018062,             !- Moisture Equation Coefficient a {dimensionless}
-    0.451879,             !- Moisture Equation Coefficient b {dimensionless}
-    0.026178,             !- Moisture Equation Coefficient c {dimensionless}
-    10.8356;              !- Moisture Equation Coefficient d {dimensionless}
-```
-
-
-### Moisture Penetration Depth (EMPD) Outputs
-
-Output variables applicable to heat transfer surfaces using EMPD model:
-
-* Zone,Average,EMPD Surface Inside Face Water Vapor Density [kg/m3]
-
-* Zone,Average,EMPD Surface Inside Face Humidity Ratio [kgWater/kgDryAir]
-
-* Zone,Average,EMPD Surface Inside Face Relative Humidity [%]
-
-The following variables apply only to surfaces, where the material assigned to the inside layers is MaterialProperty:MoisturePenetrationDepth:Settings. The EMPD (Effective Moisture Penetration Depth) moisture balance solution algorithm is used to calculate the inside surface moisture levels.
-
-#### EMPD Surface Inside Face Water Vapor Density [kg/m3]
-
-The vapor density at the inside surface, where the EMPD moisture balance solution algorithm is applied.
-
-#### EMPD Surface Inside Face Humidity Ratio [kgWater/kgDryAir]
-
-The humidity ratio at the inside surface, where the EMPD moisture balance solution algorithm is applied.
-
-#### EMPD Surface Inside Face Relative Humidity [%]
-
-The relative humidity at the inside surface, where the EMPD moisture balance solution algorithm is applied.
-
-### MaterialProperty:PhaseChange
-
-**Advanced/Research Usage:** This material is used to describe the temperature dependent material properties that are used in the Conduction Finite Difference solution algorithm. This conduction model is done when the appropriate materials are specified and the Solution Algorithm parameter is set toConductionFiniteDifference. This permits simulating temperature dependent thermal conductivity and phase change materials (PCM) in EnergyPlus.
-
-#### Field: Name
-
-This field is a regular material name specifying the material with which this additional temperature dependent property information will be associated.
-
-#### Field: Temperature Coefficient for Thermal Conductivity
-
-This field is used to enter the temperature dependent coefficient for thermal conductivity of the material.  Units for this parameter are (W/(m-K<sup>2</sup>). This is the thermal conductivity change per unit temperature excursion from 20 C. The conductivity value at 20 C is the one specified with the basic material properties of the regular material specified in the name field. The thermal conductivity is obtained from:
-
-<div>\[k = {k_o} + {k_1}({T_i} - 20)\]</div>
-
-where:
-
-k<sub>o</sub> is the 20C value of thermal conductivity(normal idf  input)
-
-k<sub>1</sub> is the change in conductivity per degree temperature difference from 20C
-
-(this field).
-
-#### Field Set: Temperature-Enthalpy
-
-The temperature – enthalpy set of inputs specify a two column tabular temperature-enthalpy function for the basic material. Sixteen pairs can be specified. Specify only the number of pairs necessary. The tabular function must cover the entire temperature range that will be seen by the material in the simulation. It is suggested that the function start at a low temperature, and extend to 100C. Note that the function has no negative slopes and the lowest slope that will occur is the base material specific heat. Temperature values should be strictly increasing. Enthalpy contributions of the phase change are always added to the enthalpy that would result from a constant specific heat base material.  An example of a simple enthalpy temperature function is shown below.
-
-![Temp-Enth Example](media/image024.png)
-
-#### Field: Temperature x
-
-This field is used to specify the temperature of the temperature-enthalpy function for the basic material. Units are C.
-
-#### Field: Enthalpy x
-
-This field specifies the enthalpy that corresponds to the previous temperature of the temperature-enthalpy function. Units are J/kg.
-
-And, an IDF example showing how it is used in conjunction with the Material:
-
-Note, the following Heat Balance Algorithm is necessary (only specified once). Also, when using ConductionFiniteDifference, it is more efficient to set the zone timestep shorter than those used for the ConductionTransferFunction solution algorithm. It should be set to 12 timesteps per hour or greater, and can range up to 60.
-
-```idf
-HeatBalanceAlgorithm,
-ConductionFiniteDifference;
-
-
-Timestep,
-12;
-
-
-Material,
-    E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Name
-    Smooth,                  !- Roughness
-    1.9050000E-02,           !- Thickness {m}
-    0.7264224,               !- Conductivity {W/m-K}
-    1601.846,                !- Density {kg/m3}
-    836.8000,                !- Specific Heat {J/kg-K}
-    0.9000000,               !- Thermal Absorptance
-    0.9200000,               !- Solar Absorptance
-    0.9200000;               !- Visible Absorptance
-
-
-MaterialProperty:PhaseChange,
-    E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Name
-    0.0,             !- Temperature coefficient,thermal conductivity(W/m K2)
-    -20.,            !- Temperature 1, C
-    0.01,            !- Enthalpy 1 at –20C, (J/kg)
-    20.,             !- Temperature 2, C
-    33400,           !- Enthalpy 2, (J/kg)
-    20.5,            !- temperature 3, C
-    70000,           !- Ethalpy 3, (J/kg)
-    100.,            !- Temperature 4, C
-    137000;          !- Enthalpy 4, (J/kg)
-```
-
-
-### MaterialProperty:VariableThermalConductivity
-
-This object is used to describe the temperature dependent material properties that are used in the CondFD (Conduction Finite Difference) solution algorithm. This conduction model is used when the appropriate CondFD materials are specified and the Solution Algorithm parameter is set to condFD.
-
-#### Field: Name
-
-This field is a regular material name specifying the material with which this additional temperature dependent property information will be associated.
-
-#### Field Set: Temperature-Thermal Conductivity
-
-The temperature – conductivity set of inputs specify a two column tabular temperature-thermal conductivity function for the basic material. Ten pairs can be specified. Specify only the number of pairs necessary. Temperature values should be strictly increasing.
-
-#### Field: Temperature x
-
-This field is used to specify the temperature of the temperature-conductivity function for the basic material. Units are C.
-
-#### Field: Thermal Conductivity x
-
-This field specifies the conductivity that corresponds to the temperature (previous field) of the temperature-conductivity function. Units are W/m-K.
-
-And, an IDF example showing how it is used in conjunction with the Materials:
-
-Note, the following Heat Balance Algorithm is necessary (only specified once). Also, when using Conduction Finite Difference, it is more efficient to set the zone time step shorter than those used for the Conduction Transfer Function solution algorithm. It should be set to 12 time steps per hour or greater, and can range up to 60.
-
-```idf
-HeatBalanceAlgorithm,
-ConductionFiniteDifference;
-
-
-Timestep,
-12;
-
-
-Material,
-    PCMPlasterBoard ,      !- Name
-    Smooth,                  !- Roughness
-    1.9050000E-02,           !- Thickness {m}
-    4.2,                     !- Conductivity {W/m-K}
-    1601.846,                !- Density {kg/m3}
-    836.8000,                !- Specific Heat {J/kg-K}
-    0.9000000,               !- Thermal Absorptance
-    0.9200000,               !- Solar Absorptance
-    0.9200000;               !- Visible Absorptance
-
-
-MaterialProperty:VariableThermalConductivity,
-    PCMPlasterBoard,         !- Name
-    0,                       !- Temperature 1 {C}
-    4.2,                     !- Thermal Conductivity 1 {W/m-K}
-    22,                      !- Temperature 2 {C}
-    4.2,                     !- Thermal Conductivity 2 {W/m-K}
-    22.1,                    !- Temperature 3 {C}
-    2.5,                     !- Thermal Conductivity 3 {W/m-K}
-    100,                     !- Temperature 4 {C}
-    2.5;                     !- Thermal Conductivity 4 {W/m-K}
-```
-
-
-### Conduction Finite Difference (CondFD) Outputs
-
-The Conduction Finite Difference solution algorithm uses a finite difference solution technique, the surfaces are divided into a nodal arrangement. The only output specific to Conduction Finite Difference solution (that is not include in other surface outputs) is node temperatures.
-
-The following output variables are applicable to all opaque heat transfer surfaces when using Solution Algorithms ConductionFiniteDifference:
-
-* Zone,Sum,CondFD Inner Solver Loop Iteration Count []
-
-* Zone,Average,CondFD Surface Temperature Node <1> [C]
-
-
-#### CondFD Inner Solver Loop Iteration Count []
-
-This outputs the count of iterations on the inner solver loop of CondFD for each surface.
-
-#### CondFD Surface Temperature Node &lt;X&gt; [C]
-
-This will output temperatures for a node in the surfaces being simulated with ConductionFiniteDifference. The key values for this output variable are the surface name. The nodes are numbered from outside to inside of the surface. The full listing will appear in the RDD file
-
-#### CondFD Surface Heat Flux Node &lt;X&gt; [W/m2]
-
-This will output heat flux at each node in surfaces being simulated with ConductionFiniteDifference. The key values for this output variable are the surface name. The nodes are numbered from outside to inside of the surface. The full listing will appear in the RDD file. A positive value indicates heat flowing towards the inside face of the surface. Note that this matches the sign convention for Surface Inside Face Conduction Heat Transfer Rate per Area and is opposite the sign of Surface OUtside Face Conduction Heat Transfer Rate per Area.
-
-#### CondFD Surface Heat Capacitance Outer Half Node &lt;X&gt; [W/m2-K]
-#### CondFD Surface Heat Capacitance Inner Half Node &lt;X&gt; [W/m2-K]
-
-These will output the half-node heat capacitance in surfaces being simulated with ConductionFiniteDifference. The key values for this output variable are the surface name. The nodes are numbered from outside to inside of the surface. The full listing will appear in the RDD file. For this output, the heat capacitance is defined as the product of specific heat, density, and node thickness. Zero is reported for R-layer half-nodes and for undefined half-nodes.  There is no outer half-node for Node 1 which is the outside face of the surface, and there is no inner half-node for Node N which is the inside face of the surface. CondFD Surface Heat Capacitance is only available with Output:Diagnostics,DisplayAdvancedReportVariables.
-
-### MaterialProperty:HeatAndMoistureTransfer:Settings
-
-**Advanced/Research Usage:** This object is used to describe two of the seven additional material properties needed for the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm. The settings object is used when the solutions algorithm is set to CombinedHeatAndMoistureFiniteElement and the appropriate material properties are assigned to each material. This permits the simulation of the moisture dependant thermal properties of the material as well as the transfer of moisture through, into and out of the material into the zone or exterior.
-
-In addition to the Porosity and Initial Water content properties described here, five additional properties, described by tabulated relationships between variables, are required. These properties are;
-
-- MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm
-
-- MaterialProperty:HeatAndMoistureTransfer:Suction
-
-- MaterialProperty:HeatAndMoistureTransfer:Redistribution
-
-- MaterialProperty:HeatAndMoistureTransfer:Diffusion
-
-- MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity
-
-All materials in a construction are required to have all material properties defined for HAMT to work.
-
-Within the MaterialProperty:HeatAndMoistureTransfer:Settings object the following fields are defined.
-
-#### Field: Material Name
-
-This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
-
-#### Field: Porosity
-
-The porosity of a material is the maximum fraction, by volume, of a material that can be taken up with water. The units are [m3/m3].
-
-#### Field: Initial Water Content Ratio
-
-For this solution algorithm, the initial water content is assumed to be distributed evenly through the depth of the material. The units are [kg/kg].
-
-Below is an example input for the porosity and initial water content of a material.
-
-```idf
-MaterialProperty:HeatAndMoistureTransfer:Settings,
-      Concrete,     !- Name
-      0.76,     !- Porosity
-      0.2;     !- Initial (or typical) Water content
-```
-
-
-### MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm
-
-**Advanced/Research Usage:** This material property is used in conjunction with the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm.
-
-The Isotherm data relates the moisture, or water content [kg/m3] of a material with the relative humidity (RH). The water content is expected to increase as relative humidity increases, starting at zero content at 0.0relative humidity fraction and reaching a maximum, defined by the porosity, at 1.0 relative humidity fraction, which corresponds to 100% relatve humidity. Relative humidities are entered as fraction for this object ranging from 0.0 to 1.0. These two extremes (0.0 and 1.0) are automatically set by the HAMT solution. However, if they are entered they will be used as extra data points. Data should be provided with increasing RH and moisture content up to as high an RH as possible to provide a stable solution. One possible reason for the following error message may be that a material has a very rapid increase in water content for a small change in RH, which can happen if the last entered water content point is at a low RH and the material has a very high porosity.
-
-```
-  ** Warning ** HeatAndMoistureTransfer: Large Latent Heat for Surface ROOF
-```
-
-Another potential reason for this error being generated is the use of inappropriate values for Vapor Transfer Coefficients. See the SurfaceProperties:VaporCoefficients object in the Advanced Surface Concepts group.
-
-#### Field: Material Name
-
-This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
-
-#### Field: Number of data  Coordinates
-
-A maximum of 25 coordinates can be specified.
-
-#### Field Set: Relative Humidity-Moisture Content
-
-#### Field: Relative Humidity Fraction x
-
-The relative humidity of the x<sup>th</sup> coordinate. The relative humidity is entered as fraction, not in percent.
-
-#### Field: Moisture Content x
-
-The Moisture Content of the x<sup>th</sup> coordinate. The units are [kg/m3]
-
-Below is an example input for a material isotherm
-
-```idf
-MaterialProperty:HeatAndMoistureTransfer:SorptionIsotherm,
-      Concrete,     !- Name
-      10,     !- Number of data Coordinates
-      0.2205,    !- Relative Humidity fraction #1
-      22.31,     !- Moisture content #1
-      0.202,     !- Relative Humidity fraction #2
-      19.665,    !- Moisture content #2
-      0.449,     !- Relative Humidity fraction #3
-      40.02,     !- Moisture content #3
-      0.454,     !- Relative Humidity fraction #4
-      36.915,    !- Moisture content #4
-      0.6506,    !- Relative Humidity fraction #5
-      56.005,    !- Moisture content #5
-      0.655,     !- Relative Humidity fraction #6
-      52.325,    !- Moisture content #6
-      0.824,     !- Relative Humidity fraction #7
-      72.565,    !- Moisture content #7
-      0.8725,    !- Relative Humidity fraction #8
-      85.1,      !- Moisture content #8
-      0.924,     !- Relative Humidity fraction #9
-      91.08,     !- Moisture content #9
-      0.964,     !- Relative Humidity fraction #10
-      100.28;    !- Moisture content #10
-```
-
-
-### MaterialProperty:HeatAndMoistureTransfer:Suction
-
-**Advanced/Research Usage:**This material property is used in conjunction with the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm.
-
-The suction data relates the liquid transport coefficient, under suction, to the water content of a material. A data point at zero water content is required. The liquid transport coefficient at the highest entered water content value is used for all liquid transport coefficient values above this water content. These coefficients are used by HAMT when the rain flag is set in the weather file.
-
-#### Field: Material Name
-
-This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
-
-#### Field: Number of Suction points
-
-A maximum of 25 points can be specified.
-
-#### Field Set: Moisture Content-Liquid Transport Coefficient
-
-#### Field: Moisture Content x
-
-The moisture content of the x<sup>th</sup> point. The units are [kg/m3].
-
-#### Field: Liquid Transport Coefficient x
-
-The Liquid Transport Coefficient of the x<sup>th</sup> point. The units are [m2/s].
-
-Below is an example input for a material liquid transport coefficient under suction.
-
-```idf
-MaterialProperty:HeatAndMoistureTransfer:Suction,
-      Concrete,     !- Name
-      5,     !- Number of Suction points
-      0,     !- Moisture content 1
-      0,     !- Liquid Transport Coefficient 1
-      72,     !- Moisture content 2
-      0.0000000000741,     !- Liquid Transport Coefficient 2
-      85,     !- Moisture content 3
-      0.000000000253,     !- Liquid Transport Coefficient 3
-      100,     !- Moisture content 4
-      0.00000000101,     !- Liquid Transport Coefficient 4
-      118,     !- Moisture content 5
-      0.00000000128;     !- Liquid Transport Coefficient 5
-```
-
-
-### MaterialProperty:HeatAndMoistureTransfer:Redistribution
-
-**Advanced/Research Usage:**This material property is used in conjunction with the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm.
-
-The redistribution data relates the liquid transport coefficient to the water content of a material under normal conditions. A data point at zero water content is required. The liquid transport coefficient at the highest entered water content value is used for all liquid transport coefficient values above this water content. These coefficients are used by the Heat and Moisture Transfer algorithm when the rain flag is NOT set in the weather file.
-
-#### Field: Material Name
-
-This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
-
-#### Field: Number of Redistribution points
-
-A maximum of 25 points can be specified.
-
-#### Field Set: Moisture Content-- Liquid Transport Coefficient
-
-#### Field: Moisture Content x
-
-The moisture content of the x<sup>th</sup> point. The units are [kg/m3].
-
-#### Field: Liquid Transport Coefficient x
-
-The Liquid Transport Coefficient of the x<sup>th</sup> point. The units are [m2/s].
-
-Below is an example input for the object.
-
-```idf
-MaterialProperty:HeatAndMoistureTransfer:Redistribution,
-      Concrete,     !- Name
-      5,     !- Number of Redistribution points
-      0,     !- Moisture content 1
-      0,     !- Liquid Transport Coefficient 1
-      72,     !- Moisture content 2
-      0.00000000000741,     !- Liquid Transport Coefficient 2
-      85,     !- Moisture content 3
-      0.0000000000253,     !- Liquid Transport Coefficient 3
-      100,     !- Moisture content 4
-      0.000000000101,     !- Liquid Transport Coefficient 4
-      118,     !- Moisture content 5
-      0.000000000128;     !- Liquid Transport Coefficient 5
-```
-
-
-### MaterialProperty:HeatAndMoistureTransfer:Diffusion
-
-**Advanced/Research Usage:**This material property is used in conjunction with the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm.
-
-The MU data relates the vapor diffusion resistance factor (dimensionless) to the relative humidity as fraction(RH). A data point at zero RH is required. The vapor diffusion resistance factor at the highest entered relative humidity (RH) value is used for all vapor diffusion resistance factor values above this RH.  The relative humidity maximum value in fraction is 1.0.
-
-#### Field: Material Name
-
-This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
-
-#### Field: Number of Data Pairs
-
-A maximum of 25 pairs can be specified.
-
-#### Field Set: Relative Humidity-Vapor Diffusion Resistance Factor
-
-#### Field: Relative Humidity Fraction \#x
-
-The moisture content of the x<sup>th</sup> pair. The relative humidity is entered as fraction, not in percent.
-
-#### Field: Vapor Diffusion Resistance Factor \#x
-
-The Liquid Transport Coefficient of the x<sup>th</sup> pair.
-
-Below are some examples of the values for materials.
-
-```idf
-MaterialProperty:HeatAndMoistureTransfer:Diffusion,
-      Plywood,     !- Name
-      3,     !- Number of data Points
-      0,     !- Relative Humidity Fraction 1
-      700,     !- Water Vapor Diffusion Resistance Factor 1
-      0.5,     !- Relative Humidity Fraction 2
-      200,     !- Water Vapor Diffusion Resistance Factor 2
-      1,     !- Relative Humidity Fraction 3
-      20;     !- Water Vapor Diffusion Resistance Factor 3
-
-MaterialProperty:HeatAndMoistureTransfer:Diffusion,
-      Concrete,     !- Name
-      1,     !- Number of Mu Points
-      0,     !- Relative Humidity Fraction 1
-      180;     !- Water Vapor Diffusion Resistance Factor 1
-```
-
-
-### MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity
-
-**Advanced/Research Usage:**This material property is used in conjunction with the CombinedHeatAndMoistureFiniteElement heat balance solution algorithm.
-
-The thermal data relates the thermal conductivity [W/m-K] of a material to the moisture or water content [kg/m3]. A data point at zero water content is required. The thermal conductivity at the highest entered water content value is used for all thermal conductivity values above this water content. If this object is not defined for a material then the algorithm will use a constant value entered in the Material object for all water contents.
-
-#### Field: Material Name
-
-This field is a unique reference name that the user assigns to a particular material. This name can then be referred to by other input data.
-
-#### Field: Number of Thermal Coordinates
-
-A maximum of 25 coordinates can be specified.
-
-#### Field Set: Moisture Content- Thermal Conductivity
-
-#### Field: Moisture Content x
-
-The moisture content of the x<sup>th</sup> coordinate. The units are [kg/m3]
-
-#### Field: Thermal Conductivity x
-
-The Thermal Conductivity of the x<sup>th</sup> coordinate. The units are [W/m-K]
-
-Below is an example of values for a material.
-
-```idf
-MaterialProperty:HeatAndMoistureTransfer:ThermalConductivity
-      Concrete,     !- Name
-      2,     !- Number of Thermal Coordinates
-      0,     !- Moisture content \#1
-      1.6,     !- Thermal Conductivity \#1
-      180,     !- Moisture content \#2
-      2.602;     !- Thermal Conductivity \#2
-```
-
-
-### Heat and Moisture (HAMT) Outputs
-
-* Zone,Average,HAMT Surface Average Water Content Ratio [kg/kg]
-
-* Zone,Average,HAMT Surface Inside Face Temperature [C]
-
-* Zone,Average,HAMT Surface Inside Face Relative Humidity [%]
-
-* Zone,Average,HAMT Surface Inside Face Vapor Pressure [Pa]
-
-* Zone,Average,HAMT Surface Outside Face Temperature [C]
-
-* Zone,Average,HAMT Surface Outside Face Relative Humidity [%]
-
-* Zone,Average,HAMT Surface Inside Face Relative Humidity [%]
-
-
-#### HAMT Surface Average Water Content Ratio [kg/kg]
-
-This output is the summed water content [kg/kg] of all cells in a surface expressed as a fraction of the mass of the water to the material mass.
-
-#### HAMT Surface Inside Face Temperature [C]
-
-This output is the temperature [C] on the internal “surface� of the surface.
-
-#### HAMT Surface Inside Face Relative Humidity [%]
-
-#### HAMT Surface Inside Face Relative Humidity [%]
-
-This output is the relative humidity on the internal “surface� of the surface expressed as a percentage.
-
-#### HAMT Surface Inside Face Vapor Pressure [Pa]
-
-This output is the vapor pressure [Pa] on the internal “surface� of the surface.
-
-#### HAMT Surface Outside Face Temperature [C]
-
-This output is the temperature on the external “surface� of the surface.
-
-#### HAMT Surface Outside Face Relative Humidity [%]
-
-This output is the relative humidity on the external “surface� of the surface.
-
-Zone,Average,HAMT Surface Temperature Cell N [C]
-
-Zone,Average,HAMT Surface Water Content Cell N [kg/kg]
-
-Zone,Average,HAMT Surface Relative Humidity Cell N [%]
-
-Detailed profile data for the variables Temperature [C], Relative Humidity [%] and Water Content [kg/kg] within each surface can also be reported. To calculate the heat and moisture transfer through surfaces HAMT splits up surfaces into discrete cells. Each cell is composed of a single material and has a position within the surface. HAMT automatically assigns cells to construction objects so that there are more cells closer to boundaries between materials and also at the “surfaces� of the surface. It is not possible for users to define their own cells.
-
-#### HAMT Surface Relative Humidity Cell &lt;N&gt; [%]
-
-This is the relative humidity of the cell in the surface.
-
-#### HAMT Surface Temperature Cell &lt;N&gt; [C]
-
-This is the temperature of the cell in the surface.
-
-#### HAMT Surface Water Content Cell &lt;N&gt; [kg/kg]
-
-This is the relative water content of the cell in the surface.
-
-Each surface is made from a particular construction. The construction-surface relationship is output by HAMT to the eplusout.eio file with the following format.
-
-```
-! <HAMT cells>, Surface Name, Construction Name, Cell Numbers
-! <HAMT origins>, Surface Name, Construction Name, Cell origins (m)
-```
-
-The output also contains the HAMT cell origins and cell number for each construction – surface combination. The coordinate system origin is defined as the exterior surface of the construction. Users can select any one of the Temperature, Relative Humidity or Water Content variables for any cell to be reported, using the following naming scheme for the output variable.
-
-HAMT Profile Construction &lt;Variable&gt; Cell &lt;Cell\#&gt;
-
-It is better to specify the “key� or Surface Name in this output.
-
-So for example to output the temperature of the 10<sup>th</sup> cell in a surface, eg “East Wall� would require the following output variable.
-
-```idf
-Output:Variable,
-    East Wall,               !- Key Value
-    HAMT Profile Construction Temperature Cell 10,  !- Variable Name
-    Hourly;                  !- Reporting Frequency
-```
-
-
-By selecting a whole range of these reports and using the information in the eplusout.eio file it is possible to build up a temperature profile of the surface.
-
-### Materials for Glass Windows and Doors
-
-All the materials for glass windows and doors have the prefix “WindowMaterial�. The following  WindowMaterial descriptions (Glazing, Glazing:RefractionExtinctionMethod, Gas, GasMixture, Shade, Screen and Blind) apply to glass windows and doors. The property definitions described herein for Glazing, Gas and GasMixture are supported by the National Fenestration Rating Council as standard.
-
-“Front side� is the side of the layer opposite the zone in which the window is defined. “Back side� is the side closest to the zone in which the window is defined. Therefore, for exterior windows, “front side� is the side closest to the outdoors. For interior windows, “front side� is the side closest to the zone adjacent to the zone in which the window is defined.
-
-The solar radiation transmitted by the window layers enters the zone and is a component of the zone load. The solar radiation absorbed in each solid layer (glass, shade, screen or blind) participates in the window layer heat balance calculation. The visible transmittance and reflectance properties of the window are used in the daylighting calculation.
-
-### WindowMaterial:Glazing
-
-In the following, for exterior windows, “front side� is the side of the glass closest to the outside air and “back side� is the side closest to the zone the window is defined in. For interzone windows, “front side� is the side closest to the zone adjacent to the zone the window is defined in and “back side� is the side closest to the zone the window is defined in.
-
-#### Field: Name
-
-The name of the glass layer. It corresponds to a layer in a window construction.
-
-#### Field: Optical Data Type
-
-Valid values for this field are SpectralAverage, Spectral, BSDF.
-
-If Optical Data Type = SpectralAverage, the values you enter for solar transmittance and reflectance are assumed to be averaged over the solar spectrum, and the values you enter for visible transmittance and reflectance are assumed to be averaged over the solar spectrum and weighted by the response of  the human eye. There is an EnergyPlus Reference Data Set for WindowMaterial:Glazing that contains spectral average properties for many different types of glass.
-
-If Optical Data Type = Spectral, then, in the following field, you must enter the name of a spectral data set defined with the WindowGlassSpectralData object. In this case, the values of  solar and visible transmittance and reflectance in the fields below should be blank.
-
-If Optical Data Type = BSDF, the Construction:ComplexFenestrationState object must be used to define the window construction layers. The Construction:ComplexFenestrationState object contains references to the BSDF files which contain the optical properties of the Complex Fenestration layers. In this case,
-
-#### Field: Window Glass Spectral Data Set Name
-
-If Optical Data Type = Spectral, this is the name of a spectral data set defined with a WindowGlassSpectralData object.
-
-#### Field: Thickness
-
-The surface-to-surface thickness of the glass (m).
-
-#### Field: Solar Transmittance at Normal Incidence
-
-Transmittance at normal incidence averaged over the solar spectrum. Used only when Optical Data Type = SpectralAverage.
-
-For uncoated glass, when alternative optical properties are available—such as thickness, solar index of refraction, and solar extinction coefficient—they can be converted to equivalent solar transmittance and reflectance values using the equations given in “Conversion from Alternative Specification of Glass Optical Properties.�)
-
-#### Field: Front Side Solar Reflectance at Normal Incidence
-
-Front-side reflectance at normal incidence averaged over the solar spectrum. Used only when Optical Data Type = SpectralAverage.
-
-#### Field: Back Side Solar Reflectance at Normal Incidence
-
-Back-side reflectance at normal incidence averaged over the solar spectrum. Used only when Optical Data Type = SpectralAverage.
-
-#### Field: Visible Transmittance at Normal Incidence
-
-Transmittance at normal incidence averaged over the solar spectrum and weighted by the response of the human eye. Used only when Optical Data Type = SpectralAverage.
-
-For uncoated glass, when alternative optical properties are available—such as thickness, visible index of refraction, and visible extinction coefficient—they can be converted to equivalent visible transmittance and reflectance values using the equations given in “Conversion from Alternative Specification of Glass Optical Properties.�)
-
-#### Field: Front Side Visible Reflectance at Normal Incidence
-
-Front-side reflectance at normal incidence averaged over the solar spectrum and weighted by the response of the human eye. Used only when Optical Data Type = SpectralAverage.
-
-#### Field: Back Side Visible Reflectance at Normal Incidence
-
-Back-side reflectance at normal incidence averaged over the solar spectrum and weighted by the response of the human eye. Used only when Optical Data Type = SpectralAverage.
-
-#### Field: Infrared Transmittance at Normal Incidence
-
-Long-wave transmittance at normal incidence.
-
-#### Field: Front Side Infrared Hemispherical Emissivity
-
-Front-side long-wave emissivity.
-
-#### Field: Back Side Infrared Hemispherical Emissivity
-
-Back-side long-wave emissivity.
-
-#### Field: Conductivity
-
-Thermal conductivity (W/m-K).
-
-#### Field: Dirt Correction Factor for Solar and Visible Transmittance
-
-This is a factor that corrects for the presence of dirt on the glass. The program multiplies the fields “Solar Transmittance at Normal Incidence� and “Visible Transmittance at Normal Incidence� by this factor if the material is used as the outer glass layer of an exterior window or glass door.[[1]](#_ftn1) If the material is used as an inner glass layer (in double glazing, for example), the dirt correction factor is not applied because inner glass layers are assumed to be clean. Using a material with dirt correction factor &lt; 1.0 in the construction for an interior window will result in an error message.
-
-Representative values of the dirt correction factor are shown in Table 7.
-
-     Table 7. Dirt Correction Factors
-
-<table class="table table-striped">
-  <tr>
-    <th rowspan="2">Type of Location</th>
-    <th colspan="3">Angle of Glazing</th>
-  </tr>
-  <tr>
-    <td>Vertical</td>
-    <td>45</td>
-    <td>Horizontal</td>
-  </tr>
-  <tr>
-    <td>Non-industrial</td>
-    <td>0.9</td>
-    <td>0.8</td>
-    <td>0.7</td>
-  </tr>
-  <tr>
-    <td>Industrial</td>
-    <td>0.7</td>
-    <td>0.6</td>
-    <td>0.5</td>
-  </tr>
-  <tr>
-    <td>Very Dirty</td>
-    <td>0.6</td>
-    <td>0.5</td>
-    <td>0.4</td>
-  </tr>
-</table>
-
-From Appendix A, “Daylighting in Sports Halls, Report 2,� SportScotland, Nov. 2002
- (www.sportscotland.org.uk)
-
-The default value of the dirt correction factor is 1.0, which means the glass is clean.
-
-It is assumed that dirt, if present, has no effect on the IR properties of the glass.
-
-#### Field: Solar Diffusing
-
-Takes values No (the default) and Yes. If No, the glass is transparent and beam solar radiation incident on the glass is transmitted as beam radiation with no diffuse component. If Yes, the glass is translucent and beam solar radiation incident on the glass is transmitted as hemispherically diffuse radiation with no beam component.[[2]](#_ftn2) See Figure 10. Solar Diffusing = Yes should only be used on the *innermost* pane of glass in an exterior window; it does not apply to interior windows.
-
-For both Solar Diffusing = No and Yes, beam is reflected as beam with no diffuse component (see Figure 10). Solar Diffusing cannot be used with Window Shading Control devices (except Switchable Glazing). When attempted, the window property will be set to No for Solar Diffusing. The Surface Details report will reflect the override.
-
-If, in the Building object, Solar Distribution = FullInteriorAndExterior, use of Solar Diffusing = Yes for glass in an exterior window will change the distribution of interior solar radiation from the window. The result is that beam solar radiation that would be transmitted by a transparent window and get absorbed by particular interior surfaces will be diffused by a translucent window and be spread over more interior surfaces. This can change the time dependence of heating and cooling loads in the zone.
-
-In a zone with Daylighting:Detailed, translucent glazing---which is often used in skylights---will provide a more uniform daylight illuminance over the zone and will avoid patches of sunlight on the floor.
-
-![](media/image025.svg)
-
-Figure 10. Comparison between transmittance properties of transparent glass (Solar Diffusing = No) and translucent glass (Solar Diffusing = Yes).
-
-#### Field: Young’s modulus
-
-A measure of the stiffness of an elastic material.  It is defined as the ratio of the unaxial stress over the uniaxial strain in the range of stress in which Hooke’s Law holds. It is used only with complex fenestration systems defined through the Construction:ComplexFenestrationState object. The default value for glass is 7.2e10 Pa.
-
-#### Field: Poisson’s ratio
-
-The ratio, when a sample object is stretched, of the contraction or transverse strain (perpendicular to the applied load), to the extension or axial strain (in the direction of the applied load). This value is used only with complex fenestration systems defined through the Construction:ComplexFenestrationState object. The default value for glass is 0.22.
-
-
-
-IDF examples of Spectral average and using a Spectral data set:
-
-```idf
-MATERIAL:WINDOWGLASS, GLASS - CLEAR SHEET 1 / 8 IN,
-  SpectralAverage, ! Optical data type
-  0.003, ! Thickness {m} 1/8"
-  0.850, ! Solar transmittance at normal incidence
-  0.075, ! Solar reflectance at normal incidence: front side
-  0.075, ! Solar reflectance at normal incidence: back side
-  0.901, ! Visible transmittance at normal incidence
-  0.081, ! Visible reflectance at normal incidence: front side
-  0.081, ! Visible reflectance at normal incidence: back side
-  0.0,   ! IR transmittance at normal incidence
-  0.84,  ! IR hemispherical emissivity: front side
-  0.84,  ! IR hemispherical emissivity: back side
-  0.9;   ! Conductivity {W/m-K}
-
-
-WindowMaterial:Glazing ,SPECTRAL GLASS INNER PANE, ! Material name
-    Spectral, ! Optical data type {SpectralAverage or Spectral}
-    TestSpectralDataSet, ! Name of spectral data set
-    0.0099, ! Thickness {m}
-    ,  ! Solar transmittance at normal incidence
-    ,  ! Solar reflectance at normal incidence: front side
-    ,  ! Solar reflectance at normal incidence: back side
-    ,  ! Visible transmittance at normal incidence
-    ,  ! Visible reflectance at normal incidence: front side
-    ,  ! Visible reflectance at normal incidence: back side
-    0.0,   ! IR transmittance at normal incidence
-    0.84,  ! IR emissivity: front side
-    0.84,  ! IR emissivity: back side
-    0.798; ! Conductivity {W/m-K}
-```
-
-
-IDF example of Spectral Data Type = BSDF
-
-```idf
-WindowMaterial:Glazing,
-  Glass_5012_Layer,        !- Layer name : CLEAR_6.PPG
-  BSDF,                    !- Optical Data Type
-  ,                        !- Spectral Data name
-  0.005664,                !- Thickness
-  ,                        !- Solar Transmittance
-  ,                        !- Solar Front Reflectance
-  ,                        !- Solar Back Reflectance
-  ,                        !- Visible Transmittance
-  ,                        !- Visible Front Reflectance
-  ,                        !- Visible Back reflectance
-  0.000000,                !- IR Transmittance
-  0.840000,                !-Front Emissivity
-  0.840000,                !-Back Emissivity
-  1.000000,                !-Conductivity
-  ,                        !-Dirt Correction Factor for Sol/Vis Transmittance
-  ,                        !-Solar Diffusing
-  7.2e10,                  !-Young’s modulus
-  0.22;                    !-Poisson’s ratio
-```
-
-
-### WindowMaterial:Glazing:RefractionExtinctionMethod
-
-This is an alternative way of specifying glass properties. Index of refraction and extinction coefficient are given instead of the transmittance and reflectance values used in WindowMaterial:Glazing. However, unlike WindowMaterial:Glazing, WindowMaterial:Glazing:RefractionExtinctionMethod is restricted to cases where the front and back optical properties of the glass are the same. This means it cannot be used for glass with a coating on one side. In that case WindowMaterial:Glazing should be used. Also, unlike WindowMaterial:Glazing, WindowMaterial:Glazing:RefractionExtinctionMethod does not allow input of glass wavelength-by-wavelength (spectral) properties.
-
-#### Field: Name
-
-The name of the glass layer. It corresponds to a layer in a window construction.
-
-#### Field: Thickness
-
-The surface-to-surface thickness of the glass (m).
-
-#### Field: Solar Index of Refraction
-
-Index of refraction averaged over the solar spectrum.
-
-#### Field: Solar Extinction Coefficient
-
-Extinction coefficient averaged over the solar spectrum (m<sup>-1</sup>).
-
-#### Field: Visible Index of Refraction
-
-Index of refraction averaged over the solar spectrum and weighted by the response of the human eye.
-
-#### Field: Visible Extinction Coefficient
-
-Extinction coefficient averaged over the solar spectrum and weighted by the response of the human eye (m<sup>-1</sup>).
-
-#### Field: Infrared Transmittance at Normal Incidence
-
-Long-wave transmittance at normal incidence.
-
-#### Field: Infrared Hemispherical Emissivity
-
-Long-wave hemispherical emissivity, assumed the same on both sides of the glass.
-
-#### Field: Conductivity
-
-Thermal conductivity (W/m-K).
-
-#### Field: Dirt Correction Factor for Solar and Visible Transmittance
-
-This is a factor that corrects for the presence of dirt on the glass. It multiplies the solar and visible transmittance at normal Incidence (which the program calculates from the input values of thickness, solar index of refraction, solar extinction coefficient, etc.) if the material is used as the outer glass layer of an exterior window or glass door. If the material is used as an inner glass layer (in double glazing, for example), the dirt correction factor is not applied because inner glass layers are assumed to be clean. Using a material with dirt correction factor &lt; 1.0 in the construction for an interior window will result in an error message.
-
-Representative values of the direct correction factor are shown in Table 7.
-
-The default value of the dirt correction factor is 1.0, which means the glass is clean. It is assumed that dirt, if present, has no effect on the IR properties of the glass.
-
-#### Field: Solar Diffusing
-
-Takes values No (the default) and Yes. If No, the glass is transparent. If Yes, the glass is translucent and beam solar radiation incident on the glass is transmitted as hemispherically diffuse radiation with no beam component. (EnergyPlus does not model the “partially translucent� case in which beam solar radiation incident on the glass is transmitted as a combination of beam and diffuse.) Solar Diffusing = Yes should only be used on the innermost pane of glass in an exterior window; it does not apply to interior windows.
-
-If, in the Building object, Solar Distribution = FullInteriorAndExterior, use of Solar Diffusing = Yes for glass in an exterior window will change the distribution of interior solar radiation from the window. The result is that beam solar radiation that would be transmitted by a transparent window and get absorbed by particular interior surfaces will be diffused by a translucent window and be spread over more interior surfaces. This can change the time dependence of heating and cooling loads in the zone.
-
-In a zone with Daylighting:Detailed, translucent glazing, which is often used in skylights, will provide a more uniform daylight illuminance over the zone and will avoid patches of sunlight on the floor.
-
-An IDF example:
-
-```idf
-WindowMaterial:Glazing:RefractionExtinctionMethod,
-4MM CLEAR GLASS, !- Material name
-    0.004, !- Thickness {m}
-    1.526, !- Solar index of refraction
-    30.0 , !- Solar extinction coefficient (1/m)
-    1.526, !- Visible index of refraction
-    30.0 , !- Visible extinction coefficient (1/m)
-    0.0,   !- IR transmittance at normal incidence
-    0.84,  !- IR emissivity
-    0.9;   !- Conductivity {W/m-K}
-```
-
-
-### Glass Optical Properties Conversion
-
-#### Conversion from Glass Optical Properties Specified as Index of Refraction and Transmittance at Normal Incidence
-
-The optical properties of uncoated glass are sometimes specified by index of refraction, n, and transmittance at normal incidence, T.
-
-The following equations show how to convert from this set of values to the transmittance and reflectance values required by WindowMaterial:Glazing. These equations apply only to uncoated glass, and can be used to convert either spectral-average solar properties or spectral-average visible properties (in general, *n* and *T* are different for the solar and visible). Note that since the glass is uncoated, the front and back reflectances are the same and equal to the *R* that is solved for in the following equations.
-
-Given *n* and *T*, find *R*:
-
-<div>\[\begin{array}{l}r = {\left( {\frac{{n - 1}}{{n + 1}}} \right)^2}\\\tau  = \frac{{{{\left[ {{{(1 - r)}^4} + 4{r^2}{T^2}} \right]}^{1/2}} - {{(1 - r)}^2}}}{{2{r^2}T}}\\R = r + \frac{{{{(1 - r)}^2}r{\tau ^2}}}{{1 - {r^2}{\tau ^2}}}\end{array}\]</div>
-
-**Example:**
-
-*T* = 0.86156
-
-*n* = 1.526
-
-<div>\[\begin{array}{l}r = {\left( {\frac{{1.526 - 1}}{{1.526 + 1}}} \right)^2}\\\tau  = 0.93974\\R = 0.07846\end{array}\]</div>
-
-### WindowMaterial:GlazingGroup:Thermochromic
-
-Thermochromic (TC) materials have active, reversible optical properties that vary with temperature. Thermochromic windows are adaptive window systems for incorporation into building envelopes. Thermochromic windows respond by absorbing sunlight and turning the sunlight energy into heat. As the thermochromic film warms it changes its light transmission level from less absorbing to more absorbing. The more sunlight it absorbs the lower the light level going through it. By using the suns own energy the window adapts based solely on the directness and amount of sunlight. Thermochromic materials will normally reduce optical transparency by absorption and/or reflection, and are specular (maintaining vision).
-
-A thermochromic window is defined with a Construction object which references a special layer defined with a WindowMaterial:GlazingGroup:Thermochromic object. The WindowMaterial:GlazingGroup:Thermochromic object further references a series of WindowMaterial:Glazing objects corresponding to each specification temperature of the TC layer.
-
-This object specifies a layer of thermochromic glass, part of a thermochromic window. An example file ThermochromicWindow.idf is included in the EnergyPlus installation.
-
-#### Field: Name
-
-A unique user assigned name for a particular thermochromic glass material.
-
-#### Field Set (Optical Data Temperature, Window Material Glazing Name) is extensible.
-
-#### Field:Optical Data Temperature &lt;N&gt;
-
-The temperature of the TC glass layer corresponding to the optical data of the TC layer. Unit is °C.
-
-#### Field: Window Material Glazing Name &lt;N&gt;
-
-The window glazing (defined with WindowMaterial:Glazing) name that provides the TC glass layer performance at the above specified temperature.
-
-IDF Examples
-
-```idf
-  Construction,
-    window_const,             !- Name
-    Usual Glass,              !- Layer 1
-    AIR 6MM,                  !- Layer 2
-    TCGlazings,               !- Layer 3
-    AIR 6MM,                  !- Layer 4
-    Usual Glass;              !- Layer 5
-
-  WindowMaterial:Gas,
-    AIR 6MM,                 !- Name
-    Air,                     !- Gas Type
-    0.0063;                  !- Thickness {m}
-
-! Added for thermochromic glazings
-  WindowMaterial:GlazingGroup:Thermochromic,
-    TCGlazings,
-    0 ,  TCGlazing0,
-    20,  TCGlazing20,
-    25,  TCGlazing25,
-    30,  TCGlazing30,
-    35,  TCGlazing35,
-    40,  TCGlazing40,
-    45,  TCGlazing45,
-    50,  TCGlazing50,
-    55,  TCGlazing55,
-    60,  TCGlazing60,
-    65,  TCGlazing65,
-    75,  TCGlazing75,
-    85,  TCGlazing85;
-
-WindowMaterial:Glazing,
-  TCGlazing0,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing20,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing25,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing30,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing35,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing40,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing45,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing50,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing55,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing60,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing65,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing75,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-
-WindowMaterial:Glazing,
-  TCGlazing85,  !- Name
-  SpectralAverage,  !- Optical Data Type
-  ,        !- Window Glass Spectral Data Set Name
-  0.0030,  !- Thickness
-  0.2442,  !- Solar Transmittance at Normal Incidence
-  0.7058,  !- Front Side Solar Reflectance at Normal Incidence
-  0.7058,  !- Back Side Solar Reflectance at Normal Incidence
-  0.3192,  !- Visible Transmittance at Normal Incidence
-  0.6308,  !- Front Side Visible Reflectance at Normal Incidence
-  0.6308,  !- Back Side Visible Reflectance at Normal Incidence
-  0.0000,  !- Infrared Transmittance at Normal Incidence
-  0.9000,  !- Front Side Infrared Hemispherical Emissivity
-  0.9000,  !- Back Side Infrared Hemispherical Emissivity
-  0.0199,  !- Conductivity
-  1.0000,  !- Dirt Correction Factor for Solar and Visible Transmittance
-  No;      !- Solar Diffusing
-```
-
-
-### WindowMaterial:GlazingGroup:Thermochromic Outputs
-
-#### Surface Window Thermochromic Layer Temperature [C]
-
-The temperature of the TC glass layer of a TC window at each time step.
-
-#### Surface Window Thermochromic Layer Property Specification Temperature [C]
-
-The temperature under which the optical data of the TC glass layer are specified.
-
-The overall properties (U-factor/SHGC/VT) of the thermochromic windows at different specification temperatures are reported in the EIO file. These window constructions are created by EnergyPlus during run time. They have similar names with suffix “\_TC\_XX� where XX represents a specification temperature.
-
-### WindowMaterial:Gas
-
-This object specifies the properties of the gas between the panes of a multi-pane window. Gas Type = Custom allows you to specify the properties of gases other than air, Argon, Krypton or Xenon. There is an EnergyPlus Reference Data Set for Material:WindowGas that contains several types of gas of different thicknesses. See Material:WindowGasMixture for the case that the gas fill is a mixture of different gases.
-
-#### Field: Name
-
-The name of the gas fill. It refers to a layer in a window construction.
-
-#### Field: Gas Type
-
-The type of gas. The choices are Air, Argon, Krypton, or Xenon. If Gas Type = Custom you can use Conductivity Coefficient A, etc. to specify the properties of a different type of gas.
-
-#### Field: Thickness
-
-The thickness (m) of the gas layer.
-
-#### Properties for Custom Gas Types
-
-The following entries are used only if Gas Type = Custom. The A and B coefficients are those in the following expression that gives a property value as a function of temperature in degrees K:
-
-<div>\[Property = Coefficien{t_A} + Coefficien{t_B}*Temperatur{e_K}\]</div>
-
-#### Field: Conductivity Coefficient A
-
-The A coefficient for gas conductivity (W/m-K). Used only if Gas Type = Custom.
-
-#### Field: Conductivity Coefficient B
-
-The B coefficient for gas conductivity (W/m-K<sup>2</sup>). Used only if Gas Type = Custom.
-
-#### Field: Conductivity Coefficient C
-
-The C coefficient for gas conductivity (W/m-K<sup>3</sup>).  Used only if Gas Type = Custom.
-
-#### Field: Viscosity Coefficient A
-
-The A coefficient for gas viscosity (kg/m-s). Used only if Gas Type = Custom.
-
-#### Field: Viscosity Coefficient B
-
-The B coefficient for gas viscosity (kg/m-s-K). Used only if Gas Type = Custom.
-
-#### Field: Viscosity Coefficient C
-
-The C coefficient for gas viscosity (kg/m-s-K<sup>2</sup>).  Used only if Gas Type = Custom.
-
-#### Field: Specific Heat Coefficient A
-
-The A coefficient for gas specific heat (J/kg-K). Used only if Gas Type = Custom.
-
-#### Field: Specific Heat Coefficient B
-
-The B coefficient for gas specific heat (J/kg-K<sup>2</sup>). Used only if Gas Type = Custom.
-
-#### Field: Specific Heat Coefficient C
-
-The C coefficient for gas specific heat (J/kg-K<sup>3</sup>).  Used only if Gas Type = Custom.
-
-#### Field: Specific Heat Ratio
-
-The specific heat ratio for gas.  Used only if Gas Type = Custom.
-
-#### Field: Molecular Weight
-
-The molecular weight for gas.  The molecular weight is the mass of 1 mol of the substance.  This has a numerical value which is the average molecular mass of the molecules in the substance multiplied by Avogadro’s constant. (kg/kmol) (Shown in the IDD as g/mol for consistency)
-
-#### Field: Specific Heat Ratio
-
-The specific heat ratio for gas.  The specific heat ratio of a gas is the ratio of the specific heat at contant pressure, to the specific heat at constant volume.  Used only if Gas Type = Custom.
-
-An IDF example:
-
-```idf
-WindowMaterial:Gas,AIRGAP,
-  AIR,      ! Gas type (Air - Argon - Krypton - Xenon - Custom)]
-  0.0125;   ! Thickness {m} 1/2 inch
-```
-
-
-An IDF example to be used with a WindowMaterial:Gap definition (see below)
-
-```idf
-WindowMaterial:Gas,
-Gas_1_W_0_0100,                                     !- gap name - Air
-Air,                                                !- type
-0.0100;                                             !- thickness
-```
-
-
-
-
-An IDF example for a Custom Gas
-
-```idf
-WindowMaterial:Gas,
-Gas_16_W_0_0003,                   !- gap name
-Custom,                            !- type
-0.0003,                            !- thickness
-2.873000e-003,                     !- Conductivity Coefficient A
-7.760000e-005,                     !- Conductivity Coefficient B
-0.000000e+000,                     !- Conductivity Coefficient C
-3.723000e-006,                     !- Conductivity Viscosity A
-4.940000e-008,                     !- Conductivity Viscosity B
-0.000000e+000,                     !- Conductivity Viscosity C
-1002.737000,                       !- Specific Heat Coefficient A
-0.012324,                          !- Specific Heat Coefficient B
-0.000000,                          !- Specific Heat Coefficient C
-28.969999,                         !- Molecular Weight
-1.400000;                          !- Specific Heat Ratio
-```
-
-
-
-
-### WindowMaterial:GasMixture
-
-This object allows you to specify the fill between the panes of a multi-pane window to be a mixture of two, three or four different gases chosen from air, argon, krypton and xenon. It can also be used if only one type of gas in the fill. In this case you can also use WindowMaterial:Gas. Note that the fractions of gas types in the mixture should add up to 1.0.
-
-#### Field: Name
-
-The name of the gas mixture. It refers to a layer in a window construction.
-
-#### Field: Thickness
-
-The thickness (m) of the gas mixture layer.
-
-#### Field: Number of Gases in Mixture
-
-The number of different types of gas in the mixture ( a value from 1 to 4)
-
-#### Set: Gas Type-Fraction (up to 4)
-
-#### Field: Gas 1 Type
-
-The type of  the first gas in the mixture. Choices are Air, Argon, Krypton and Xenon.
-
-#### Field: Gas 1 Fraction
-
-The fraction of the first gas in the mixture.
-
-An IDF example:
-
-```idf
-WindowMaterial:GasMixture,ArgonKryptonMix,
-0.0125,   ! Thickness {m} 1/2 inch
-2,        ! Number of Gases in Mixture
-Argon,    ! Gas 1 Type
-0.6,      ! Gas 1 Fraction
-Krypton,  ! Gas 2 Type
-0.4;      ! Gas 2 Fraction
-```
-
-### WindowMaterial:Gap
-
-This input object is used to define the gap between two layers in a complex fenestration system, where the Construction:ComplexFenestrationState object is used. It references the gas or gas mixtures defined in the WindowMaterial:Gas and WindowMaterial:GasMixture objects. It is referenced as a layer in the Construction:ComplexFenestrationState object ;it cannot be referenced as a layer from the Construction object.
-
-#### Field: Name
-
-Unique name of the gap.
-
-#### Field: Thickness
-
-The thickness (m) of the gap layer.
-
-#### Field: Pressure
-
-The pressure (Pa) of the gas in the gap layer, used to calculate the gas properties of the glazing system gap. Default is atmospheric pressure, 101325 Pa.When modeling vacuum glazing, this value should represent the pressure in the evacuated glazing system. If this pressure is less that the ThermalModelParams:PressureLimit value, the the glazing system will be modeled as a vacuum glazing.
-
-#### Field: Deflection State
-
-This field is used when modeling the deflection of the glass layers in a window if the WinodowThermalModel:Params value for “deflection model� is “MeasuredDeflection�.
-
-#### Field: Support Pillar
-
-References the support pillar of the gap layer if vacuum glazing is being modeled.  If left empty, then it is considered that gap layer does not have support pillars.
-
-#### Field: Gas (or GasMixture)
-
-References gas (WindowMaterial:Gas) or gas mixture (WindowMaterial:GasMixture) of the gap layer.
-
-
-
-An IDF example for simple glazing:
-
-```idf
-WindowMaterial:Gas,
-Gas_1_W_0_0120,                                !- gap name - Air
-Air,                                           !- type
-0.0120;                                        !- thickness
-
-
-WindowMaterial:Gap,
-Gap_1_Layer,                                   !- gap name: Air
-0.0120,                                        !- thickness
-Gas_1_W_0_0120,                                !- Gas (or Gas Mixture) name
-101325.0000;                                   !- pressure
-```
-
-
-
-
-An IDF example for vacuum glazing:
-
-```idf
-WindowMaterial:Gap,
-Gap_16_Layer,                     !- gap name: Vacuum_0.001_pr-0.5_ps-50.8
-0.0003,                                             !- thicknessGas_16_W_0_0003,                                    !- Gas (or Gas Mixture) name
-0.1333,                                             !- pressure
-,                                                   !- deflection state
-SupportPillar_16_Gap_1;                             !- SupportPillar
-
-
-WindowGap:SupportPillar,
-SupportPillar_16_Gap_1,                             !- Name
-0.0508,                                             !- spacing
-0.0005;                                             !- radius
-```
-
-
-
-### WindowGap:DeflectionState
-
-This input object is used to enter data describing deflection state of the gap.  It is referenced from WindowMaterial:Gap object only and it is used only when deflection model is set to MeasuredDeflection (see WindowThermalModel:Params), otherwise it is ignored.
-
-#### Field: Name
-
-Unique name of the deflection state.
-
-#### Field: Deflected Thickness
-
-The thickness (m) of the gap in deflected state.  It represents value of deflection at point of maximum which is usualy at the center poing of glazing system.  It is used only with tarcog algorithm set to Measured Deflection (WindowThermalModel:Params), otherwise this field will be ignored.
-
-
-
-An IDF example where WindowThermalModel:Params Deflection Model = MeasuredDeflection:
-
-```idf
-WindowMaterial:Gap,
-Gap_1_Layer,                                  !- gap name: Air
-0.0120,                                       !- thickness
-Gas_1_W_0_0120,                               !- Gas (or Gas Mixture) name
-101325.0000,                                  !- pressure
-Gap_1_Deflection;                              !- deflection state
-
-
-WindowGap:DeflectionState,       !- deflection state of gap
-  Gap_1_Deflection,              !- name
-  0.011;                         !- gap thickness in deflected state
-```
-
-
-### WindowGap:SupportPillar
-
-This input object is used to enter data describing support pillar of the gap.  Support pillars are used in vacuum glazing in order to prevent deflection of glass layers.
-
-![](media/image029.png)
-
-Figure 11. Support Pillar
-
-#### Field: Name
-
-Unique name of the support pillar.
-
-#### Field: Spacing
-
-Distance (m) between support pillar centers (see the Engineering reference document for more information).
-
-#### Field: Radius
-
-The radius (m) of the support pillar (see Engineering reference document for more information).
-
-
-
-An IDF example for vacuum glazing (see Vacuum Glazing example in WindowMaterial:Gap above)
-
-```idf
-WindowGap:SupportPillar,       !- gap support pillar
-  SupportPillar_16_Gap_1,      !- basis matrix name
-  0.05,                        !- pillar spacing
-  0.005;                       !- pillar radius
-```
-
-
-### WindowMaterial:SimpleGlazingSystem
-
-This model should be used with caution. There may be significant differences in performance between the simple window system and the usual more detailed model.
-
-This input object differs from the other WindowMaterial objects in that it describes an entire glazing system rather than individual layers. This object is used when only very limited information is available on the glazing layers or when specific performance levels are being targeted. The layer by layer description offers superior method of modeling windows that should be used instead of this object when sufficient data are available. This object accesses a model that turns simple performance indices into a fuller model of the glazing system.
-
-The performance indices are U-factor and Solar Heat Gain Coefficient, and optionally Visible Transmittance. The values for these performance indices can be selected by the user to represent either glazing-only windows (with no frame) or an average window performance that includes the frame. Inside the program the model produces an equivalent window glazing layer with no frame. The properties of the modeled glazing layer are reported to the EIO file using the IDF input object syntax for the WindowMaterial:Glazing input object. This equivalent layer could be reused in subsequent models if desired, however there will be important differences in the modeled window performance because the simple glazing system model includes its own special model for angular dependence when incident beam solar is not normal to the plane of the window.
-
-When this object is referenced in a Construction object, it cannot be used with other glazing or gas material layers. Shades or blinds cannot be located between the glass, but these can be used on the inside or the outside of the glazing system.   If the glazing system does have between-the-glass shades or blinds, then the U and SHGC values entered in this object should include the impacts of those layers. Adding window treatment layers such as shades or screens will alter the overall performance to be different than the performance levels prescribed in this object.
-
-#### Field: Name
-
-The name of the glazing system.  This value is unique across all constructions.
-
-#### Field: U-Factor
-
-This field describes the value for window system U-Factor, or overall heat transfer coefficient. Units are in W/m<sup>2</sup>·K. This is the rated (NFRC) value for U-factor under winter heating conditions. The U-factor is assumed to be for vertically mounted products. Although the maximum allowable input is U-7.0 W/m<sup>2</sup>·K, the effective upper limit of the glazings generated by the underlying model is around U-5.8 W/m<sup>2</sup>·K.
-
-#### Field: Solar Heat Gain Coefficient
-
-This field describes the value for SHGC, or solar heat gain coefficient. There are no units. This is the rated (NFRC) value for SHGC under summer cooling conditions and represents SHGC for normal incidence and vertical orientation.
-
-#### Field: Visible Transmittance
-
-This field is optional. If it is omitted, then the visible transmittance properties are taken from the solar properties. If it is included then the model includes it when developing properties for the glazing system. This is the rated (NFRC) value for visible transmittance at normal incidence.
-
-An example of this object.
-
-```idf
-WindowMaterial:SimpleGlazingSystem,
-    SimpleWindow:DOUBLE PANE WINDOW , !- Name
-    2.716 , !-  U-Factor
-    0.763 , !-  Solar Heat Gain Coefficient
-    0.812 ; !-  Visible Transmittance
-```
-
-
-### WindowMaterial:Shade
-
-This object specifies the properties of window shade materials. Reflectance and emissivity properties are assumed to be the same on both sides of the shade. Shades are considered to be perfect diffusers (all transmitted and reflected radiation is hemispherically-diffuse) with transmittance and reflectance independent of angle of incidence. There is an EnergyPlus Reference Data Set for WindowMaterial:Shade that contains properties of generic window shades.
-
-Window shades can be on the inside of the window (“interior shades�), on the outside of the window (“exterior shades�), or between glass layers (“between-glass shades�). When in place, the shade is assumed to cover all of the glazed part of the window, including dividers; it does not cover any of the window frame, if present. The plane of the shade is assumed to be parallel to the glazing.
-
-WindowMaterial:Shade can be used for diffusing materials such as drapery and translucent roller shades. For slat-type shading devices, like Venetian blinds, that have a strong angular dependence of transmission, absorption and reflection, it is better to use WindowMaterial:Blind. WindowMaterial:Screen should be used to model wire mesh insect screens where the solar and visible transmission and reflection properties vary with the angle of incidence of solar radiation.
-
-Transmittance and reflectance values for drapery material with different color and openness of weave can be obtained from manufacturers or determined from 2001 ASHRAE Fundamentals, Chapter 30, Fig. 31.
-
-There are two methods of assigning a shade to a window:
-
-#### Method 1:
-
-1)   Define the construction of the window without the shade, the so-called “bare� construction.
-
-2)   Reference the bare construction in the FenestrationSurface:Detailed for the window.
-
-3)   Define the WindowMaterial:Shade.
-
-4)   Define a WindowProperty:ShadingControl for the window in which you (a) specify that this WindowMaterial:Shade is the window’s shading device and (b) specify how the shade is controlled.
-
-#### Method 2:
-
-1)   Define the Construction of the window without the shade, the so-called “bare� construction.
-
-2)   Reference the bare construction in the FenestrationSurface:Detailed for the window.
-
-3)   Define the WindowMaterial:Shade.
-
-4)   Define another Construction, called the “shaded construction,� that includes the WindowMaterial:Shade.
-
-5)   Define a WindowProperty:ShadingControl for the window in which you (a) reference the shaded construction and (b) specify how the shade is controlled.
-
-Note that WindowProperty:ShadingControl has to be used with either method, even if the shade is in place at all times. You will get an error message if you try to reference a shaded construction directly from FenestrationSurface:Detailed.
-
-#### Field: Name
-
-Name of the shade. It is referenced as an inside or outside layer in a window construction.
-
-#### Field: Solar Transmittance
-
-Transmittance averaged over the solar spectrum. Assumed independent of incidence angle.
-
-#### Field: Solar Reflectance
-
-Reflectance averaged over the solar spectrum. Assumed same on both sides of shade and independent of incidence angle.
-
-#### Field: Visible Transmittance
-
-Transmittance averaged over the solar spectrum and weighted by the response of the human eye. Assumed independent of incidence angle.
-
-#### Field: Visible Reflectance
-
-Reflectance averaged over the solar spectrum and weighted by the response of the human eye. Assumed same on both side of shade and independent of incidence angle.
-
-#### Field: Thermal Hemispherical Emissivity
-
-Effective long-wave emissivity. Assumed same on both sides of shade. We can approximate this  effective emissivity, *ε<sub>eff</sub>,*  as follows. Let *η* be the “openness� the shade, i.e.,  the ratio of the area of openings in the shade to the overall shade area (see Field: Air-Flow Permeability, below). Let the emissivity of  the shade material be ε. Then
-
-<div>\[{\varepsilon_{{\rm{eff}}}} \approx \varepsilon \left( {1 - \eta } \right)\]</div>
-
-For most non-metallic materials *ε*is about 0.9.
-
-#### Field: Thermal Transmittance
-
-Effective long-wave transmittance. Assumed independent of incidence angle. We can approximate this  effective long-wave transmittance, *τ<sub>eff</sub>,*  as follows. Let *η* be the “openness� the shade, i.e.,  the ratio of the area of openings in the shade to the overall shade area. Let the long-wave transmittance of the shade material be *τ*. Then
-
-<div>\[{T_{{\rm{eff}}}} \approx \eta  + T\left( {1 - \eta } \right)\]</div>
-
-For most materials* Ï„* is very close to zero, which gives
-
-<div>\[{T_{{\rm{eff}}}} \approx \eta \]</div>
-
-#### Field: Thickness
-
-Thickness of the shade material (m). If the shade is not flat, such as for pleated pull-down shades or folded drapery, the average thickness normal to the plane of the shade should be used.
-
-#### Field: Conductivity
-
-Shade material conductivity (W/m-K).
-
-#### Field: Shade to Glass Distance
-
-Distance from shade to adjacent glass (m). This is denoted by *s* in Figure 12 and Figure 13, below. If the shade is not flat, such as for pleated pull-down shades or folded drapery, the average shade-to-glass distance should be used. (The shade-to-glass distance is used in calculating the natural convective air flow between glass and shade produced by buoyancy effects.). Note used for between-glass shades.
-
-In the following, *H* is the glazing height and *W* is the glazing width.
-
-#### Field: Top Opening Multiplier
-
-Effective area for air flow at the top of the shade divided by *sW*, the horizontal area between glass and shade (see Figures below).
-
-#### Field: Bottom Opening Multiplier
-
-Effective area for air flow at the bottom of the shade divided by *sW*, the horizontal area between glass and shade (see Figures below).
-
-#### Field: Left-Side Opening Multiplier
-
-Effective area for air flow at the left side of the shade divided by *sH*, the vertical area between glass and shade (see Figures below).
-
-#### Field: Right-Side Opening Multiplier
-
-Effective area for air flow at the right side of the shade divided by *sH*, the vertical area between glass and shade (see Figures below).
-
-#### Field: Field: Air-Flow Permeability
-
-The fraction of the shade surface that is open to air flow, i.e., the total area of openings (“holes�) in the shade surface divided by the shade area, *HW*. If air cannot pass through the shade material, Air-Flow Permeability = 0. For drapery fabric and screens the Air-Flow Permeability can be taken as the “openness� of the fabric (see 2001 ASHRAE Fundamentals, Chapter 30, Fig. 31), which is 0.0 to 0.07 for closed weave, 0.07 to 0.25 for semi-open weave, and 0.25 and higher for open weave.
-
-![](media/image033.svg)
-
-Figure 12. Vertical section (a) and perspective view (b) of glass  and interior shade layers  showing variables used in the gap air flow analysis. In (b), the air-flow opening areas *A<sub>bot</sub>*, *A<sub>top</sub>*, *A<sub>l</sub>*, *A<sub>r</sub>* and *A<sub>h</sub>* are shown schematically. See *Engineering Manual* for definition of thermal variables.
-
-
-
-![](media/image034.svg)
-
-Figure 13. Examples of air-flow openings for an interior shade covering glass of height *H* and width *W*. Not to scale. (a) Horizontal section through shade with openings on the left and right sides (top view). (b) Vertical section through shade with openings at the top and bottom (side view). In (a) Left-Side Opening Multiplier = *A<sub>l</sub> /sH* = min(*l/s*,1) and Right-Side Opening Multiplier = *A<sub>r</sub> /sH* = min(*r/s*,1). In (b) Top Opening Multiplier = *A<sub>top</sub> /sW* = *t/s* and Bottom Opening Multiplier = *A<sub>bot</sub> /sW = b/s.*
-
-An IDF example:
-
-```idf
-WindowMaterial:Shade,
-    DRAPES - CLOSE WEAVE MEDIUM,  !- Name
-    0.05,                    !- Solar transmittance
-    0.3000000,               !- Solar Reflectance
-    .05,                     !- Visible transmittance
-    0.3000000,               !- Visible reflectance
-    0.9000000,               !- Thermal Hemispherical Emissivity
-    0.0,                     !- Thermal Transmittance
-    0.003,                   !- Thickness {m}
-    0.1,                     !- Conductivity {W/m-K}
-    0.050,                   !- Shade to glass distance {m}
-    1.0,                     !- Top opening multiplier
-    1.0,                     !- Bottom opening multiplier
-    0.0,                     !- Left-side opening multiplier
-    0.0,                     !- Right-side opening multiplier
-    0.0;                     !- Air flow permeability
-```
-
-
-### WindowMaterial:Blind
-
-This object specifies the properties of a window blind consisting of flat, equally-spaced slats. Unlike window shades, which are modeled as perfect diffusers, window blinds have solar and visible transmission and reflection properties that strongly depend on slat angle and angle of incidence of solar radiation. There is an EnergyPlus Reference Data Set for WindowMaterial:Blind that contains properties of generic window blinds.
-
-Blinds can be located on the inside of the window (“interior blinds�), on the outside of the window (“exterior blinds�), or between two layers of glass (“between-glass blinds�). When in place, the blind is assumed to cover all of the glazed part of the window, including dividers; it does not cover any of the window frame, if present. The plane of the blind is assumed to be parallel to the glazing. When the blind is retracted it is assumed to cover none of the window. The solar and thermal effects of the blind’s support strings, tapes or rods are ignored. Slat curvature, if present, is ignored.
-
-There are two methods of assigning a blind to a window:
-
-#### Method 1:
-
-1)   Define the construction of the window without the blind, the so-called “bare� construction.
-
-2)   Reference the bare construction in the FenestrationSurface:Detailed for the window.
-
-3)   Define the WindowMaterial:Blind.
-
-4)   Define a WindowProperty:ShadingControl for the window in which you (a) specify that this WindowMaterial:Blind is the window’s shading device and (b) specify how the blind is controlled.
-
-#### Method 2:
-
-1)   Define the Construction of the window without the blind, the so-called “bare� construction.
-
-2)   Reference the bare construction in the FenestrationSurface:Detailed for the window.
-
-3)   Define the WindowMaterial:Blind.
-
-4)   Define another Construction, called the “shaded construction,� that includes the WindowMaterial:Blind.
-
-5)   Define a WindowProperty:ShadingControl for the window in which you (a) reference the shaded construction and (b) specify how the blind is controlled.
-
-Note that WindowProperty:ShadingControl has to be used with either method, even if the blind is in place at all times. You will get an error message if you try to reference a construction with a blind directly from Window objects (FenestrationSurface:Detailed or Window).
-
-Note also that WindowProperty:ShadingControl is used to determine not only when the blind is in place, but how its slat angle is controlled.
-
-#### Field: Name
-
-Name of the blind. It is referenced as a layer in a window construction (ref: Construction object) or as a “Material Name of Shading Device� in a WindowProperty:ShadingControl object.
-
-#### Field: Slat Orientation
-
-The choices are Horizontal and Vertical. “Horizontal� means the slats are parallel to the bottom of the window; this is the same as saying that the slats are parallel to the X-axis of the window. “Vertical� means the slats are parallel to Y-axis of the window.
-
-#### Field: Slat Width
-
-The width of the slat measured from edge to edge (m). See Figure 14.
-
-#### Field: Slat Separation
-
-The distance between the front of a slat and the back of the adjacent slat (m). See Figure 14.
-
-#### Field: Slat Thickness
-
-The distance between the faces of a slat (m). See Figure 14.
-
-#### Field: Slat Angle
-
-The angle (degrees) between the glazing outward normal and the slat outward normal, where the outward normal points away from the front face of the slat (degrees). See Figure 14.
-
-If the WindowProperty:ShadingControl for the blind has Type of Slat Angle Control for Blinds = FixedSlatAngle, the slat angle is fixed at “Slat Angle.�
-
-If Type of Slat Angle Control for Blinds = BlockBeamSolar, the program automatically adjusts the slat angle so as just block beam solar radiation. In this case the value of “Slat Angle� is used only when the blind is in place and there is no beam solar radiation incident on the blind.
-
-If Type of Slat Angle Control for Blinds = ScheduledSlatAngle, the slat angle is variable. In this case “Slat Angle� is not applicable and the field should be blank.
-
-If Type of Slat Angle Control for Blinds = FixedSlatAngle and “Slat Angle� is less than the minimum or greater than the maximum allowed by Slat Width, Slat Separation and Slat Thickness, the slat angle will be reset to the corresponding minimum or maximum and a warning will be issued.
-
-#### Field: Slat Conductivity
-
-The thermal conductivity of the slat (W/m-K).
-
-#### Field: Slat Beam Solar Transmittance
-
-The beam solar transmittance of the slat, assumed to be independent of angle of incidence on the slat. Any transmitted beam radiation is assumed to be 100% diffuse (i.e., slats are translucent).
-
-#### Field: Front Side Slat Beam Solar Reflectance
-
-The beam solar reflectance of the front side of the slat, assumed to be independent of angle of incidence (matte finish). This means that slats with a large specularly-reflective component (shiny slats) are not well modeled.
-
-#### Field: Back Side Slat Beam Solar Reflectance
-
-The beam solar reflectance of the back side of the slat, assumed to be independent of angle of incidence (matte finish). This means that slats with a large specularly-reflective component (shiny slats) are not well modeled.
-
-#### Field: Slat Diffuse Solar Transmittance
-
-The slat transmittance for hemispherically diffuse solar radiation. This value should equal “Slat Beam Solar Transmittance.�
-
-#### Field: Front Side Slat Diffuse Solar Reflectance
-
-The front-side slat reflectance for hemispherically diffuse solar radiation. This value should equal “Front Side Slat Beam Solar Reflectance.�
-
-#### Field: Back Side Slat Diffuse Solar Reflectance
-
-The back-side slat reflectance for hemispherically diffuse solar radiation. This value should equal “Back Side Slat Beam Solar Reflectance.�
-
-#### Field: Slat Beam Visible Transmittance
-
-The beam visible transmittance of the slat, assumed to be independent of angle of incidence on the slat. Any transmitted visible radiation is assumed to be 100% diffuse (i.e., slats are translucent).
-
-#### Field: Front Side Slat Beam Visible Reflectance
-
-The beam visible reflectance on the front side of the slat, assumed to be independent of angle of incidence (matte finish). This means that slats with a large specularly-reflective component (shiny slats) are not well modeled.
-
-#### Field: Back Side Slat Beam Visible Reflectance
-
-The beam visible reflectance on the front side of the slat, assumed to be independent of angle of incidence (matte finish). This means that slats with a large specularly-reflective component (shiny slats) are not well modeled.
-
-#### Field: Slat Diffuse Visible Transmittance
-
-The slat transmittance for hemispherically diffuse visible radiation. This value should equal “Slat Beam Visible Transmittance.�
-
-#### Field: Front Side Slat Diffuse Visible Reflectance
-
-The front-side slat reflectance for hemispherically diffuse visible radiation. This value should equal “Front Side Slat Beam Visible Reflectance.�
-
-#### Field: Back Side Slat Diffuse Visible Reflectance
-
-The back-side slat reflectance for hemispherically diffuse visible radiation. This value should equal “Back Side Slat Beam Visible Reflectance..�
-
-#### Field: Slat Infrared Hemispherical Transmittance
-
-The slat Infrared transmittance. It is zero for solid metallic, wooden or glass slats, but may be non-zero in some cases (e.g., thin plastic slats).
-
-#### Field: Front Side Slat Infrared  Hemispherical Emissivity
-
-Front-side hemispherical emissivity of the slat. Approximately 0.9 for most materials. The most common exception is bare (unpainted) metal slats or slats finished with a metallic paint.
-
-#### Field: Back Side Slat Infrared  Hemispherical Emissivity
-
-Back-side hemispherical emissivity of the slat. Approximately 0.9 for most materials. The most common exception is bare (unpainted) metal slats or slats finished with a metallic paint.
-
-#### Field: Blind to Glass Distance
-
-For interior and exterior blinds, the distance from the mid-plane of the blind to the adjacent glass (m). See Figure 14. Not used for between-glass blinds. As for window shades (ref: WindowMaterial:Shade) this distance is used in calculating the natural convective air flow between glass and blind that is produced by buoyancy effects.
-
-#### Opening Multipliers
-
-The following opening multipliers are defined in the same way as for window shades (see WindowMaterial:Shade, Figure 12 and Figure 13). Note that, unlike window shades, there is no input for Air-Flow Permeability; this is automatically calculated by the program from slat angle, width and separation.
-
-#### Field: Blind Top Opening Multiplier
-
-Defined as for Material:WindowShade.
-
-#### Field: Blind Bottom Opening Multiplier
-
-Defined as for Material:WindowShade.
-
-#### Field: Blind Left-Side Opening Multiplier
-
-Defined as for Material:WindowShade.
-
-#### Field: Blind Right-Side Opening Multiplier
-
-Defined as for Material:WindowShade.
-
-#### Field: Minimum Slat Angle
-
-The minimum allowed slat angle (degrees). Used only if WindowProperty:ShadingControl (for the window that incorporates this blind) varies the slat angle (i.e., the WindowProperty:ShadingControl has Type of Slat Angle Control for Blinds = ScheduledSlatAngle or BlockBeamSolar). In this case, if the program tries to select a slat angle less than Minimum Slat Angle it will be reset to Minimum Slat Angle. (Note that if the Minimum Slat Angle itself is less than the minimum allowed by Slat Width, Slat Separation and Slat Thickness, it will be reset to that minimum.)
-
-#### Field: Maximum Slat Angle
-
-The maximum allowed slat angle (degrees). Used only if WindowProperty:ShadingControl (for the window that incorporates this blind) varies the slat angle (i.e., the WindowProperty:ShadingControl has Type of Slat Angle Control for Blinds = ScheduledSlatAngle or BlockBeamSolar). In this case, if the program tries to select a slat angle greater than Maximum Slat Angle the slat angle will be reset to Maximum Slat Angle. (Note that if the Maximum Slat Angle itself is greater than the maximum allowed by Slat Width, Slat Separation and Slat Thickness, it will be reset to that maximum.)
-
-An IDF example:
-
-```idf
-WindowMaterial:Blind,
- White Painted Metal Blind,   !- Name
- HORIZONTAL, !- Slat orientation
- 0.025   , !- Slat width (m)
- 0.01875 , !- Slat separation (m)
- 0.001   , !- Slat thickness (m)
- 45.0    , !- Slat angle (deg)
- 44.9    , !- Slat conductivity (W/m-K)
- 0.0     , !- Slat beam solar transmittance
- 0.8     , !- Front Side Slat beam solar reflectance
- 0.8     , !- Back Side Slat beam solar reflectance
- 0.0     , !- Slat diffuse solar transmittance
- 0.8     , !- Front Side Slat diffuse solar reflectance
- 0.8     , !- Back Side Slat diffuse solar reflectance
- 0.0     , !- Slat beam visible transmittance
- 0.7     , !- Front Side Slat beam visible reflectance
- 0.7     , !- Back Side Slat beam visible reflectance
- 0.0     , !- Slat diffuse visible transmittance
- 0.7     , !- Front Side Slat diffuse visible reflectance
- 0.7     , !- Back Side Slat diffuse visible reflectance
- 0.0     , !- Slat Infrared hemispherical transmittance
- 0.9     , !- Front Side Slat Infrared hemispherical emissivity
- 0.9     , !- Back Side Slat Infrared hemispherical emissivity
- 0.050   , !- Blind-to-glass distance
- 0.0     , !- Blind top opening multiplier
- 0.0     , !- Blind bottom opening multiplier
- 0.5     , !- Blind left-side opening multiplier
- 0.5     , !- Blind right-side opening multiplier
- ,         !- Minimum slat angle (deg)
- ;         !- Maximum slat angle (deg)
-```
-
-
-
-
-![](media/image035.svg)
-
-Figure 14. (a) Side view of a window blind with horizontal slats  (or top view of blind with vertical slats) showing slat geometry. The front face of a slat is shown by a heavy line. The slat angle is defined as the angle between the glazing outward normal and the slat outward normal, where the outward normal points away from the front face of the slat. (b) Slat orientations for representative slat angles. The slat angle varies from 0<sup>O</sup>, when the front of the slat is parallel to the glazing and faces toward the outdoors,  to 90<sup>O</sup>, when the slat is perpendicular to the glazing, to 180<sup>O</sup>, when the front of the slat is parallel to the glazing and faces toward the indoors. The minimum and maximum slat angles are determined by the slat thickness, width and separation.
-
-### WindowMaterial:ComplexShade
-
-This input object is used to define shade layers used in the Construction:ComplexFenestrationState object.
-
-#### Field: Name
-
-Unique name of the shading layer.
-
-#### Field: Shading Layer Type
-
-The type of shading layer.  The options are:
-
-- Venetian – for modeling venetian blinds
-
-- Woven – for modeling shading systems with a regular weave
-
-- Perforated – for modeling perforated screens
-
-- BSDF – for modeling shades whose properties are represented by a BSDF file
-
-- OtherShadingType – for modeling shading systems which do not belong to the any of the previous group
-
-#### Field: Thickness
-
-The thickness (m) of the shading layer. This value is ignored for ShadingLayerType = Venetian, because the program will calculate the thickness based on the slat angle. This value is needed for ShadingLayerType = Woven and Perforated
-
-#### Field: Conductivity
-
-The conductivity (W/mK) of the shading layer material. Default: 1.0
-
-- Venetian – the conductivity of the venetian blind slat material
-
-- Woven – the conductivity of the woven shade material (such as the thread for a fabric shade)
-
-- Perforated – for modeling perforated screens
-
-- BSDF – for modeling shades whose properties are represented by a BSDF file
-
-- OtherShadingType – for modeling shading systems which do not belong to the any of the previous group
-
-#### Field: IR Transmittance
-
-The IR transmittance of the shading layer. Minimum value: 0. Maximum value: 1. Default: 0.
-
-#### Field: Front Emissivity
-
-The front emissivity of the shading layer. Minimum value: 0. Maximum value: 1. Default: 0.90.
-
-#### Field: Back Emissivity
-
-The back emissivity of the shading layer. Minimum value: 0. Maximum value: 1. Default: 0.90.
-
-#### Field: Top Opening Multiplier
-
-The top opening multiplier value will depend on the location of the shading device within the glazing system. There are several possible scenarios which can occur and they can be divided into two groups:
-
-**Shading device on the indoor/outdoor side of the window**
-
-In this case the opening multiplier is calculated as the smallest distance between the shading device and the frame (d<sub>top</sub>), divided by the gap width (S).  There are three possible cases for the position of a shading device the on indoor/outdoor side (see Figure 15).
-
-![](media/image036.png)     ![](media/image038.png)
-
-Figure 15. Three cases for the D<sub>top</sub> calculation for an indoor/outdoor shade: Case a) A shading device between the frame; Case b) A shading device outside the frame, covering the frame; Case c) a shading device outside the frame, not covering the frame.
-
-In the case where the distance between the frame and the shading device is bigger than the gap width, the d<sub>top</sub> multiplier is equal to one. Therefore, the calculation of the D<sub>top</sub> opening multiplier is:
-
-A<sub>top</sub> = min(d<sub>top</sub>/S, 1)
-
-**Shading device between glass layers**
-
-In this case the opening multiplier is calculated as the smallest distance between the shading device and the frame or spacer (d<sub>top</sub>), divided by the smaller gap width (the minimum of (S<sub>1</sub> andS<sub>2</sub>)).
-
-![](media/image039.png)          ![](media/image040.png)
-
-Figure 16. Calculation of Dtop for a shading device between glass layers
-
-The D<sub>top</sub> opening multiplier for a between glass shade is calculated as:
-
-A<sub>top</sub> = min(d<sub>top</sub>/S<sub>min</sub>, 1)
-
-Where
-
-S<sub>min</sub> = min(S<sub>1</sub>, S<sub>2</sub>)
-
-#### Field: Bottom Opening Multiplier
-
-The bottom opening multiplier (d<sub>bot</sub>) is calculated in the same way as the top opening multiplier, with the rules applied to the bottom of the shading device.
-
-#### Field: Left Side Opening Multiplier
-
-The left side opening multiplier (d<sub>left</sub>) is calcuated in the same way as the top opening multiplier, with the rules applied to the left side of the shading device.
-
-#### Field: Right Side Opening Multiplier
-
-The right side opening multiplier (d<sub>right</sub>)  is calcuated in the same way as the top opening multiplier, with the rules applied to the right side of the shading device.
-
-#### Field: Front Opening Multiplier
-
-The fraction of glazing system area that is open on the front of the shading layer (see Figure 17). This fraction is calculated as follows: Afront / (W \* H), where Afront = Area of the front of the glazing system that is not covered by the shading system, W = the width of the glazing system (IGU) and H is height of the glazing system (IGU).
-
-![](media/image041.png)
-
-Figure 17. Front view of shading layer openings.
-
-#### Field: Slat Width
-
-The width (m) of the venetian slats.  Used only for ShadingLayerType = Venetian.
-
-#### Field: Slat Spacing
-
-The distance (m) between front sides of the venetian slats.  Used only for ShadingLayerType = Venetian.
-
-#### Field: Slat Thickness
-
-The thickness (m) of the venetian slats.  Used only for ShadingLayerType = Venetian.
-
-#### Field: Slat Angle
-
-The slat tilt angle (degrees) of the venetian slats.  Used only for ShadingLayerType = Venetian.  Range of slat angle is from -90 to 90 degrees.
-
-#### Field: Slat Conductivity
-
-The conductivity (W/mK) of the venetian slats.  Used only for ShadingLayerType = Venetian.
-
-#### Field: Slat Curve
-
-The curvature radius (m) of the venetian slats.  Setting this value to zero means there is no curvature in the slat (it is flat), while a non-zero value is the radius of the slat curve.  This value cannot be smaller than Slat Width / 2.  Used only for ShadingLayerType = Venetian.
-
-![](media/image042.png)
-
-Figure 18. Side view of horizontal venetian blind slats or top view of blinds with vertical slats.  Front face of slats is marked with red line.
-
-An IDF example for ShadingLayerType = Venetian
-
-```idf
-WindowMaterial:ComplexShade,       !- venetian blind layer
-  Shade_30001_Layer,               !- name
-  Venetian,                        !- shading layer type
-  0.005,                           !- thickness
-  160,                             !- layer conductivity
-  0.0,                             !- IR transmittance
-  0.9,                             !- front emissivity
-  0.9,                             !- back emissivity
-  0.0,                             !- top opening multiplier
-  0.0,                             !- bottom opening multiplier
-  0.0,                             !- left side opening multiplier
-  0.0,                             !- right side opening multiplier
-  0.05,                            !- front opening multiplier
-  0.016,                           !- venetian slat width
-  0.012,                           !- venetian slat spacing
-  0.0006,                          !- venetian slat thickness
-  -45.00,                          !- venetian slat angle
-  160.00,                          !- venetian slat conductivity
-  0.0000;                          !- venetian slat curve
-```
-
-
-An IDF example for ShadingLayerType = Woven
-
-(Note that it is not necessary to include “blank� lines for the venetian blind input for a Woven shade definition).
-
-```idf
-WindowMaterial:ComplexShade,       !- woven shade layer
-  Shade_30002_Layer,               !- name
-  Woven,                           !- shading layer type
-  0.011,                           !- thickness
-  1,                               !- layer conductivity
-  0.0,                             !- IR transmittance
-  0.9,                             !- front emissivity
-  0.9,                             !- back emissivity
-  0.0,                             !- top opening multiplier
-  0.0,                             !- bottom opening multiplier
-  0.0,                             !- left side opening multiplier
-  0.0,                             !- right side opening multiplier
-  0.17;                            !- front opening multiplier
-```
-
-
-### WindowMaterial:Screen
-
-This object specifies the properties of exterior window screen materials. The window screen model assumes the screen is made up of intersecting orthogonally-crossed cylinders. The surface of the cylinders is assumed to be diffusely reflecting, having the optical properties of a Lambertian surface.
-
-The beam solar radiation transmitted through a window screen varies with sun angle and is made up of two distinct elements: a direct beam component and a reflected beam component. The direct beam transmittance component is modeled using the geometry of the screen material and the incident angle of the sun to account for shadowing of the window by the screen material. The reflected beam component is an empirical model that accounts for the inward reflection of solar beam off the screen material surface. This component is both highly directional and small in magnitude compared to the direct beam transmittance component (except at higher incident angles, for which case the magnitude of the direct beam component is small or zero and the reflected beam component, though small in absolute terms can be many times larger than the direct beam component). For this reason, the reflected beam transmittance component calculated by the model can be a. disregarded, b. treated as an additive component to direct beam transmittance (and in the same direction), or c. treated as hemispherically-diffuse transmittance based on a user input to the model.
-
-![DirectReflectFigure](media/image043.png)
-
-Figure 19. Direct beam and reflected beam transmittance components
-
-The window screen “assembly� properties of overall beam solar reflectance and absorptance (including the screen material ‘cylinders’ and open area) also change with sun angle and are calculated based on the values of the beam solar transmittance components (direct and reflected components described above) and the physical properties of the screen material (i.e., screen material diameter, spacing, and reflectance).
-
-Transmittance, reflectance, and absorptance of diffuse solar radiation are considered constant values and apply to both the front and back surfaces of the screen. These properties are calculated by the model as an average value by integrating the screen’s beam solar properties over a quarter hemisphere of incident radiation. Long-wave emissivity is also assumed to be the same for both sides of the screen.
-
-There is an EnergyPlus Reference Data Set for WindowMaterial:Screen that contains properties for generic window screens. Window screens of this type can only be used on the outside surface of the window (“exterior screens�). When in place, the screen is assumed to cover all of the glazed part of the window, including dividers; it does not cover any of the window frame, if present. The plane of the screen is assumed to be parallel to the glazing.
-
-WindowMaterial:Screen can be used to model wire mesh insect screens where the solar and visible transmission and reflection properties vary with the angle of incidence of solar radiation. For diffusing materials such as drapery and translucent roller shades it is better to use the WindowMaterial:Shade object. For slat-type shading devices like Venetian blinds, which have solar and visible transmission and reflection properties that strongly depend on slat angle and angle of incidence of solar radiation, it is better to use WindowMaterial:Blind.
-
-There are two methods of assigning a screen to a window:
-
-#### Method 1:
-
-1)   Define the construction of the window without the screen, the so-called “bare� construction.
-
-2)   Reference the bare construction in the FenestrationSurface:Detailed for the window.
-
-3)   Define the WindowMaterial:Screen object.
-
-4)   Define a WindowProperty:ShadingControl for the window in which you (a) specify that this Material:WindowScreen is the window’s shading device, and (b) specify how the screen is controlled.
-
-#### Method 2:
-
-1)   Define the Construction of the window without the screen, the so-called “bare� construction.
-
-2)   Reference the bare construction in the FenestrationSurface:Detailed for the window.
-
-3)   Define the WindowMaterial:Screen object.
-
-4)   Define another Construction, called the “shaded construction,� that includes the WindowMaterial:Screen.
-
-5)   Define a WindowProperty:ShadingControl for the window in which you (a) reference the shaded construction, and (b) specify how the screen is controlled.
-
-Note that WindowProperty:ShadingControl has to be used with either method, even if the screen is in place at all times. You will get an error message if you try to reference a shaded construction directly from a FenestrationSurface:Detailed object.
-
-#### Field: Name
-
-Enter a unique name for the screen. This name is referenced as an outside layer in a window construction.
-
-#### Field: Reflected Beam Transmittance Accounting Method
-
-This input specifies the method used to account for screen-reflected beam solar radiation that is transmitted through the window screen (as opposed to being reflected back outside the building). Since this inward reflecting beam solar is highly directional and is not modeled in the direction of the actual reflection, the user is given the option of how to account for the directionality of this component of beam solar transmittance. Valid choices are DoNotModel, ModelAsDirectBeam (i.e., model as an additive component to direct solar beam and in the same direction), or ModelAsDiffuse (i.e., model as hemispherically-diffuse radiation). The default value is ModelAsDiffuse.
-
-#### Field: Diffuse Solar Reflectance
-
-This input specifies the solar reflectance (beam-to-diffuse) of the screen material itself (not the effective value for the overall screen “assembly� including open spaces between the screen material). The outgoing diffuse radiation is assumed to be Lambertian (distributed angularly according to Lambert’s cosine law). The solar reflectance is assumed to be the same for both sides of the screen. This value must be from 0 to less than 1.0. In the absence of better information, the input value for diffuse solar reflectance should match the input value for diffuse visible reflectance.
-
-#### Field: Diffuse Visible Reflectance
-
-This input specifies the visible reflectance (beam-to-diffuse) of the screen material itself (not the effective value for the overall screen “assembly� including open spaces between the screen material) averaged over the solar spectrum and weighted by the response of the human eye. The outgoing diffuse radiation is assumed to be Lambertian (distributed angularly according to Lambert’s cosine law). The visible reflectance is assumed to be the same for both sides of the screen. This value must be from 0 to less than 1.0.
-
-If diffuse visible reflectance for the screen material is not available, then the following guidelines can be used to estimate this value:
-
-* Dark-colored screen (e.g., charcoal):                  0.08 – 0.10
-
-* Medium-colored screen (e.g., gray):                   0.20 – 0.25
-
-* Light-colored screen (e.g., bright aluminum):       0.60 – 0.65
-
-Commercially-available gray scale or grayscale reflecting chart references can be purchased for improved accuracy in estimating visible reflectance (by visual comparison of screen reflected brightness with that of various known-reflectance portions of the grayscale).
-
-#### Field: Thermal Hemispherical Emissivity
-
-Long-wave emissivity *ε* of the screen material itself (not the effective value for the overall screen “assembly� including open spaces between the screen material). The emissivity is assumed to be the same for both sides of the screen.
-
-For most non-metallic materials, *ε*is about 0.9. For metallic materials, *ε*is dependent on material, its surface condition, and temperature. Typical values for metallic materials range from 0.05 – 0.1 with lower values representing a more finished surface (e.g. low oxidation, polished surface). Material emissivities may be found in Table 5 from the 2005 ASHRAE Handbook of Fundamentals, page 3.9. The value for this input field must be between 0 and 1, with a default value of 0.9 if this field is left blank.
-
-#### Field: Conductivity
-
-Screen material conductivity (W/m-K). This input value must be greater than 0. The default value is 221 W/m-K (aluminum).
-
-#### Field: Screen Material Spacing
-
-The spacing, S, of the screen material (m) is the distance from the center of one strand of screen to the center of the adjacent one. The spacing of the screen material is assumed to be the same in both directions (e.g., vertical and horizontal). This input value must be greater than the non-zero screen material diameter. If the spacing is different in the two directions, use the average of the two values.
-
-![AspectRatio](media/image044.png)
-
-Figure 20. Screen Material Spacing and Diameter
-
-#### Field: Screen Material Diameter
-
-The diameter, D, of individual strands or wires of the screen material (m). The screen material diameter is assumed to be the same in both directions (e.g., vertical and horizontal). This input value must be greater than 0 and less than the screen material spacing. If the diameter is different in the two directions, use the average of the two values.
-
-#### Field: Screen to Glass Distance
-
-Distance from the window screen to the adjacent glass surface (m). If the screen is not flat, the average screen to glass distance should be used. The screen-to-glass distance is used in calculating the natural convective air flow between the glass and the screen produced by buoyancy effects. This input value must be from 0.001 m to 1 m, with a default value of 0.025 m if this field is left blank.
-
-#### Field: Top Opening Multiplier
-
-Effective area for air flow at the top of the screen divided by the horizontal area between the glass and screen (see the same field for the Material:WindowShade object for additional description). The opening multiplier fields can be used to simulate a shading material that is offset from the window frame. Since window screens are typically installed against the window frame, the default value is equal to 0.This input value can range from 0 to 1.
-
-#### Field: Bottom Opening Multiplier
-
-Effective area for air flow at the bottom of the screen divided the horizontal area between the glass and screen (see the same field for the Material:WindowShade object for additional description). The opening multiplier fields can be used to simulate a shading material that is offset from the window frame. Since window screens are typically installed against the window frame, the default value is equal to 0. This input value can range from 0 to 1.
-
-#### Field: Left-Side Opening Multiplier
-
-Effective area for air flow at the left side of the screen divided the vertical area between the glass and screen (see the same field for the Material:WindowShade object for additional description). The opening multiplier fields can be used to simulate a shading material that is offset from the window frame. Since window screens are typically installed against the window frame, the default value is equal to 0. This input value can range from 0 to 1.
-
-#### Field: Right-Side Opening Multiplier
-
-Effective area for air flow at the right side of the screen divided the vertical area between the glass and screen (see the same field for the Material:WindowShade object for additional description). The opening multiplier fields can be used to simulate a shading material that is offset from the window frame. Since window screens are typically installed against the window frame, the default value is equal to 0. This input value can range from 0 to 1.
-
-#### Field: Angle of Resolution for Screen Transmittance Output Map
-
-Angle of resolution, in degrees, for the overall screen beam transmittance (direct and reflected) output map. The comma-separated variable file eplusscreen.csv (Ref. OutputDetailsandExamples.pdf) will contain the direct beam and reflected beam solar radiation that is transmitted through the window screen as a function of incident sun angle (0 to 90 degrees relative solar azimuth and 0 to 90 degrees relative solar altitude) in sun angle increments specified by this input field. The default value is 0, which means no transmittance map is generated. Other valid choice inputs are 1, 2, 3 and 5 degrees.
-
-An IDF example for this object, along with Construction and WindowProperty:ShadingControl objects, is shown below:
-
-```idf
-WindowMaterial:Screen,
-    EXTERIOR SCREEN,         !- Name
-    ModelAsDiffuse,        !- Reflected Beam Transmittance Accounting Method
-    0.6,                     !- Diffuse Solar Reflectance
-    0.6,                     !- Diffuse Visible Reflectance
-    0.9,                     !- Thermal Hemispherical Emissivity
-    221.0,                   !- Conductivity {W/m-K}
-    0.00154,                 !- Screen Material Spacing (m)
-    0.000254,                !- Screen Material Diameter (m)
-    0.025,                   !- Screen-to-Glass Distance {m}
-    0.0,                     !- Top Opening Multiplier
-    0.0,                     !- Bottom Opening Multiplier
-    0.0,                     !- Left-Side Opening Multiplier
-    0.0,                     !- Right-Side Opening Multiplier
-    0;                   !- Angle of Resolution for Output Map {deg}
-
-Construction,
-    DOUBLE PANE WITHOUT SCREEN,     !- Name
-    GLASS - CLEAR SHEET 1 / 8 IN,   !- Outside Layer
-    WinAirB1 - AIRSPACE RESISTANCE, !- Layer \#2
-    GLASS - CLEAR SHEET 1 / 8 IN;   !- Layer \#3
-
-WindowProperty:ShadingControl,
-    DOUBLE PANE WITH SCREEN, !- User Supplied Shading Control Name
-    ExteriorScreen,          !- Shading Type
-    ,                        !- Name of construction with shading
-    AlwaysOn,                !- Shading Control Type
-    ScreenSchedule,          !- Schedule Name
-    20.0,                    !- SetPoint {W/m2, W or deg C}
-    YES,                     !- Shading Control Is Scheduled
-    NO,                      !- Glare Control Is Active
-    EXTERIOR SCREEN,         !- Material Name of Shading Device
-    ,                        !- Type of Slat Angle Control for Blinds
-    ;                        !- Slat Angle Schedule Name
-```
-
-
-### WindowMaterial:Shade:EquivalentLayer
-
-This object specifies the properties of Equivalent Layer window shade (roller blind) materials. Shades are considered to be thin, flat and perfect diffusers (all transmitted and reflected radiation is hemispherically-diffuse). However, shades can have beam-beam transmittance by virtue of their material openness.  The beam-beam transmittnec is assumed to be the same for both sides of the shade and is the same as the openness area fraction. Beam-dffuse transmittance and reflectance, and emissivity properties can be different for front and back side of the shade.Window shades can be placed on the inside of the window, on the outside of the window, or between glass layers. WindowMaterial:Shade:EquivalentLayer is used for roller blinds. The off-normal solar property calculation of shades (roller blind) is based on a set of correlations developed from measurement of samples of commercially produced roller blind material with openness fraction less than 0.14. The model is not intended for materials with unusually high values of openness and should be limited to a mximum openness fraction of 0.20. The visible spectrum solar properties input fields are not used currently hence can be left blank.
-
-#### Field: Name
-
-Name of the shade. It is referenced as an inside, inbetween or outside layer in an equivalent layer  window construction.
-
-#### Field: Shade Beam-Beam Solar Transmittance
-
-This value is the beam-beam transmittance of the shade at normal incidence and it is the same as the openness area fraction of the shade material. Assumed to be the same for front and back sides of the roller blinds.  The minimum value is 0.0 and maximum value is less than 1.0.  The default value is 0.0. For most common shade materials (e.g. Roller Blinds) the material oppeness fraction doesn’t exceed 0.20.
-
-#### Field: Front Side Shade Beam-Diffuse Solar Transmittance
-
-This value is the front side beam-diffuse transmittance of the shade material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.  The default value is 0.0.
-
-#### Field: Back Side Shade Beam-Diffuse Solar Transmittance
-
-This value is the back side beam-diffuse transmittance of the shade material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.  The default value is 0.0.
-
-#### Field: Front Side Shade Beam-Diffuse Solar Reflectance
-
-This value is the front side beam-diffuse reflectance of the shade material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
-
-#### Field: Back Side Shade Beam-Diffuse Solar Reflectance
-
-This value is the back side beam-diffuse reflectance of the shade material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
-
-#### Field: Shade Beam-Beam Visible Transmittance
-
-This value is the beam-beam transmittance at normal incidence averaged over the visible spectrum of solar radiation. Assumed to be the same for front and back sides. The minimum value is 0.0 and maximum value is less than 1.0.  Currently this input field is not used.
-
-#### Field: Shade Beam-Diffuse Visible Transmittance
-
-This value is the beam-diffuse transmittance at normal incidence averaged over the visible spectrum of solar radiation. Assumed to be the same for front and back sides. The minimum value is 0.0 and maximum value is less than 1.0.  Currently this input field is not used.
-
-#### Field: Shade Beam-Diffuse Visible Reflectance
-
-This value is the beam-diffuse reflectance at normal incidence averaged over the visible spectrum of solar radiation. Assumed to be the same for front and back sides. The minimum value is 0.0 and maximum value is less than 1.0.  Currently this input field is not used.
-
-#### Field: Shade Material Infrared Transmittance
-
-This value is the long-wave transmittance of the shade material and assumed to be the same for front and back sides of the shade. The minimum value is 0.0 and maximum value is less than 1.0. Default value is 0.05.
-
-#### Field: Front Side Shade Material Infrared Emissivity
-
-This value is the front side long-wave hemispherical emissivity of shade material. The minimum value is 0.0 and maximum value is less than 1.0. Default value is 0.91. The front side effective emissivity of the shade layer is calculated using this value and the material openness specified above.
-
-#### Field: Back Side Shade Material Infrared Emissivity
-
-This value is the back side long-wave hemispherical emissivity of shade material. The minimum value is 0.0 and maximum value is less than 1.0. Default value is 0.91. The back side effective emissivity of the shade is calculated using this value and the material openness specified above.
-
-An IDF example for this object is shown below:
-
-```idf
-WindowMaterial:Shade:EquivalentLayer,
-  Shade1,        !- Name
-  0.190,         !- Shade Beam-Beam Solar Transmittance
-  0.206,         !- Front Side Shade Beam-Diffuse Solar Transmittance
-  0.206,         !- Back Side Shade Beam-Diffuse Solar Transmittance
-  0.499,         !- Front Side Shade Beam-Diffuse Solar Reflectance
-  0.499,         !- Back Side Shade Beam-Diffuse Solar Reflectance
-  0.0,           !- Shade Beam-Beam Visible Transmittance
-  0.0,           !- Shade Beam-Diffuse Vissible Transmittance
-  0.0,           !- Shade Vissible Reflectance
-  0.0,           !- Shade Material Infrared Transmittance
-  0.84,          !- Front Side Shade Material Infrared Emissivity
-  0.84;          !- Back Side Shade Material Infrared Emissivity
-```
-
-
-### WindowMaterial:Drape:EquivalentLayer
-
-Specifies the optical and thermal properties of equivalent layer window drape fabric materials.
-
-Drapery fabric shades are commonly placed on the the inside of the window. The long-wave (infrared) properties for commonly used drapery fabrics are assumed to be the same on both sides but different values can be specified when required. Drape fabric shade layers are considered to be perfect diffusers (reflected radiation is hemispherically-diffuse independent of angle of incidence). Unpleated drape fabric is treated as thin and flat layer.The off-normal optical properties of drapery fabric is determined from user specified optical properties at normal incidence using empirical correlations. Pleated drape fabric requires entering the pleated section average width and length as showsn in Figure 21.For pleated drapes the effective beam-beam and beam-diffuse solar properties are determined by tracking both radiation components, for a given incident angle solar radiation, through various interactions with a fabric pleated in a rectangular geometry shown in Figure 21.  The solar properties of the two different pleat facets are evaluated on the basis of the local solar incidence angle.  Therefore, the effective layer properties are influenced not just by horizontal solar profile angle, but also by incidence angle. The correlations used for drape fabrics optical property calculations reqiure that the solar absorptance of the fabric, at normal incidence, is not less than 1%.
-
-![](media/image045.svg)
-
-Figure 21. Geometry used for Pleated Drape Analysis
-
-#### Field: Name
-
-Name of the drape fabric shade layer. It is referenced as an inside, in between or outside layer in an equivalent layer window construction.
-
-#### Field: Drape Beam-Beam Solar Transmittance
-
-This value is the drape fabric beam-beam transmittance at normal incidence, and it is the same as the drape fabric openness area fraction.  Assumed to be the same for front and back sides of the drape fabric layer.  The minimum value is 0.0 and maximum value is less than 1.0. For most drape fabric materials the maximum frabric openness fraction do not exceed 0.2.  The default value is 0.0.
-
-#### Field: Front Side Drape Beam-Diffuse Solar Transmittance
-
-This value is the front side beam-diffuse solar transmittance of the drape fabric material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
-
-#### Field: Back Side Drape Beam-Diffuse Solar Transmittance
-
-This value is the back side beam-diffuse solar transmittance of the drape fabric material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
-
-#### Field: Front Side Drape Beam-Diffuse Solar Reflectance
-
-This value is the front side beam-diffuse solar reflectance of the drape fabric material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
-
-#### Field: Back Side Drape Beam-Diffuse Solar Reflectance
-
-This value is the back side beam-diffuse solar reflectance of the drape fabric material at normal incidence averaged over the entire spectrum of solar radiation. The minimum value is 0.0 and maximum value is less than 1.0.
-
-#### Field: Drape Beam-Beam Visible Transmittance
-
-This value is the drape fabric beam-beam visible transmittance at normal incidence averaged over the visible spectrum range of solar radiation.  Assumed to be the same for front and back sides of the drape fabric layer.  The minimum value is 0.0 and maximum value is less than 1.0.  The default value is 0.0.  This input field is not used currently.
-
-#### Field: Front Side Drape Beam-Diffuse Visible Reflectance
-
-This value is the front side drape fabric beam-diffuse visible reflectance at normal incidence averaged over the visible spectrum range of solar radiation.  Assumed to be the same for front and back sides of the drape.  The minimum value is 0.0 and maximum value is less than 1.0.  The default value is 0.0.  This input field is not used currently.
-
-#### Field: Back Side Drape Diffuse-Diffuse Visible Reflectance
-
-This value is the back side drape fabric diffuse-diffuse visible reflectance at normal incidence averaged over the visible spectrum range of solar radiation.  Assumed to be the same for front and back sides of the drape.  The minimum value is 0.0 and maximum value is less than 1.0.  The default value is 0.0.  This input field is not used currently.
-
-#### Field: Drape Material Infrared Transmittance
-
-This value is the long-wave hemispherical transmittance of the fabric material at zero fabric openness fraction.  Assumed to be the same for front and back sides of the drape fabric material layer. The minimum value is 0.0 and maximum value is less than 1.0.  The default value is 0.05.
-
-#### Field: Front Side Drape Material Infrared Emissivity
-
-This value is the front side long-wave hemispherical emissivity of fabric material at zero shade opennes. The minimum value is 0.0 and maximum value is less than 1.0. the default value is 0.87. The front side effective emissivity of the drape fabric layer is calculated using this value and the fabric openness area fraction specified above.
-
-#### Field: Back Side Drape Material Infrared Emissivity
-
-This value is the back side long-wave hemispherical emissivity of fabric material at zero fabric openness fraction. The minimum value is 0.0 and maximum value is less than 1.0. The default value is 0.87. The back side effective emissivity of the drape fabric layer is calculated using this value and the fabric openness area fraction specified above.
-
-#### Field: Width of Pleated Fabric
-
-This value is the width of the pleated section of the draped fabric, w(m). If the drape fabric is flat (unpleated), then the pleated section width is set to zero. The default value is 0.0, i.e., assumes flat drape fabric.
-
-#### Field: Length of Pleated Fabric
-
-This value is the length of the pleated section of the draped fabric, s(m). If the drape fabric is flat (unpleated), then the pleated section length is set to zero.  The default value is 0.0, i.e., assumes flat drape fabric.
-
-An IDF example for this object is shown below:
-
-```idf
-WindowMaterial:Drape:EquivalentLayer,
-  Drape02,            !- Name
-  0.14,               !- Shade Beam-Beam Solar Transmittance
-  0.10,               !- Front Side Shade Beam-Diffuse Solar Transmittance
-  0.10,               !- Back Side Shade Beam-Diffuse Solar Transmittance
-  0.40,               !- Front Side Shade Beam-Diffuse Solar Reflectance
-  0.50,               !- Back Side Shade Beam-Diffuse Solar Reflectance
-  0.0,                !- Shade Beam-Beam Visible Transmittance
-  0.0,                !- Shade Beam-Diffuse Visible Transmittance
-  0.0,                !- Shade Beam-Diffuse Visible Reflectance
-  0.10,               !- Shade Material Infrared Transmittance
-  0.90,               !- Front Side Shade Material Infrared Emissivity
-  0.80,               !- Back Side Shade Material Infrared Emissivity
-  0.01,               !- Width of Pleated Fabric
-  0.025;              !- Length of Pleated Fabric
-```
-
-
-### WindowMaterial:Blind:EquivalentLayer
-
-This object specifies the properties of an Equivalent Layer window blind consisting of thin and equally-spaced slats. The the model assumes that slats are flat and thin, and applies correction for the slat curvature effect based on the user specified slat crwon.  Slats are assumed to transmit and reflect diffusely.The effective shortwave optical and longwave optical properties of venetian blind layer is estimated analytically. The Equivalent Layer blind model requires optical properties and geometry of the slats shown ![](media/image046.svg)
-
-Figure 22. Geometry and Properties used for venetian blind analysis
-
-.  Likewise, effective longwave properties are obtained for the layer knowing longwave properties of the slats.
-
-![](media/image047.svg)
-
-Figure 22. Geometry and Properties used for venetian blind analysis
-
-The input data required to characterize a venetian blind are: front and back side reflectance and transmittance of the slat, geometry (Slat width, w, slat spacing, s, slat crown, c, and slat angle, f, and long wave emittance and transmittance of the slat. Blinds can be located on the inside of the window, on the outside of the window, or between two layers of glass. The blind is assumed to cover all of the glazed part of the window.
-
-#### Field: Name
-
-Name of the venetian blind. It is referenced as an inside, outside or in between layers in an equivalent layer window construction.
-
-#### Field: Slat Orientation
-
-The choices are Horizontal and Vertical. “Horizontal� means the slats are parallel to the bottom of the window; this is the same as saying that the slats are parallel to the X-axis of the window. “Vertical� means the slats are parallel to Y-axis of the window.  The default is “Horizontal�.
-
-#### Field: Slat Width
-
-This value is the width of the slat measured from edge to edge (m). The default value is 0.0254.
-
-#### Field: Slat Separation
-
-The distance between the front of a slat and the back of the adjacent slat (m). The default value is 0.025. The slat separation should not be greater than the slat width.
-
-#### Field: Slat Crown
-
-The perpendicular length between the slat cord  and the curve (m). Crown=0.0625x“Slat width�. Slat is assumed to be rectangular in cross section and flat. The crown accounts for curvature of the slat.  The minimum value is 0.0, and the default value is 0.0015m.
-
-#### Field: Slat Angle
-
-The angle (degrees) between the glazing outward normal and the slat outward normal, where the outward normal points away from the front face of the slat (degrees). If the “Slat Angle Control� input field below specified is “FixedSlatAngle�, then the slat angle is fixed at “Slat Angle� value entered.  Minimum value is zero, and the maximum value allowed is 180.0 degrees.  The default value is 45 degrees.
-
-#### Field: Front Side Slat Beam-Diffuse Solar Transmittance
-
-This value is the slat front side beam-diffuse solar transmittance at normal incidence averaged over the entire spectrum of solar radiation. Any transmitted beam radiation is assumed to be 100% diffuse (i.e., slats are translucent). Minimum value is 0.0, and the maximum value is less than 1.0. The default value is 0.0.
-
-#### Field: Back Side Slat Beam-Diffuse Solar Transmittance
-
-This value is the slat back side beam-diffuse solar transmittance at normal incidence averaged over the entire spectrum of solar radiation. Any transmitted beam radiation is assumed to be 100% diffuse (i.e., slats are translucent). Minimum value is 0.0,  and the maximum value is less than 1.0. The default value is 0.0.
-
-#### Field: Front Side Slat Beam-Diffuse Solar Reflectance
-
-This value is slat front side beam-diffuse solar reflectance at normal incidence averaged over the entire spectrum of solar radiation. All the reflected component is assumed to be diffuse. Minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Back Side Slat Beam-Diffuse Solar Reflectance
-
-This value is the slat back side beam-diffuse solar reflectance at normal incidence averaged over the entire spectrum of solar radiation. All the reflected component is assumed to be diffuse. Minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Front Side Slat Beam-Diffuse Visible Solar Transmittance
-
-This value is the slat front side beam-diffuse visible transmittance at normal incidence averaged over the visible spectrum range of solar radiation. Any transmitted beam radiation is assumed to be 100% diffuse (i.e., slats are translucent). Minimum value is 0.0, and the maximum value is less than 1.0. The default value is 0.0.
-
-#### Field: Back Side Slat Beam-Diffuse Visible Solar Transmittance
-
-This value is the slat back side beam-diffuse visible transmittance at normal incidence averaged the visible spectrum range of solar radiation. Any transmitted beam radiation is assumed to be 100% diffuse (i.e., slats are translucent). Minimum value is 0.0, and the maximum value is less than 1.0. The default value is 0.0.
-
-#### Field: Front Side Slat Beam-Diffuse Visible Solar Reflectance
-
-This value is the slat front side beam-diffuse visible reflectance at normal incidence averaged over the visible spectrum range of solar radiation. All the reflected component is assumed to be diffuse. Minimum value is 0.0, and the maximum value is less than 1.0
-
-#### Field: Back Side Slat Beam-Diffuse Visible Solar Reflectance
-
-This value is the slat back side beam-diffuse visible reflectance at normal incidence averaged over the visible spectrum range of solar radiation. All the reflected component is assumed to be diffuse. Minimum value is 0.0,  and the maximum value is less than 1.0
-
-#### Field: Slat Diffuse-Diffuse Solar Transmittance
-
-This value is the slat diffuse-diffuse solar transmittance for hemispherically diffuse solar radiation. This value is the same for front and back side of the slat.  Minimum value is 0.0,  and the maximum value is less than 1.0.
-
-#### Field: Front Side Slat Diffuse-Diffuse Solar Reflectance
-
-This value is the slat front side diffuse-diffuse solar reflectance for hemispherically diffuse solar radiation. Minimum value is 0.0,  and the maximum value is less than 1.0.
-
-#### Field: Back Side Slat Diffuse-Diffuse Solar Reflectance
-
-This value is the slat back side diffuse-diffuse solar reflectance for hemispherically diffuse solar radiation. Minimum value is 0.0,  and the maximum value is less than 1.0.
-
-#### Field: Slat Diffuse-Diffuse Visible Transmittance
-
-This value is the slat diffuse-diffuse visible transmittance for hemispherically diffuse visible spectrum range of solar radiation. This value is the same for front and back side of the slat.  Minimum value is 0.0,  and the maximumvalue is less than 1.0. This input field is not used currently.
-
-#### Field: Front Side Slat Diffuse-Diffuse Visible Reflectance
-
-This value is the slat front side diffuse-diffuse visible reflectance for hemispherically diffuse visible spectrum range of solar radiation. Minimum value is 0.0, and the maximum value is less than 1.0.  This input field is not used currently.
-
-#### Field: Back Side Slat Diffuse-Diffuse Visible Reflectance
-
-This value is the slat back side diffuse-diffuse visible reflectance for hemispherically diffuse visible spectrum range of solar radiation. Minimum value is 0.0, and the maximum value is less than 1.0.  This input field is not used currently.
-
-#### Field: Slat Infrared Transmittance
-
-This value is the long-wave hemispherical transmittance of the slat material. Assumed to be the same for both sides of the slat. The minimum value is 0.0, the maximum value is less than 1.0.  The default value is 0.0.
-
-#### Field: Front Side Slat Infrared Emissivity
-
-This value is the front side long-wave hemispherical emissivity of the slat material. The minimum value is 0.0, the maximum value is less than 1.0. The default value is 0.9.
-
-#### Field: Back Side Slat Infrared Emissivity
-
-This value is the back side long-wave hemispherical emissivity of the slat material. The minimum value is 0.0, the maximum value is less than 1.0.  The default value is 0.9.
-
-#### Field: Slat Angle Control
-
-This input field is used only if slat angle control is desired.  The three key choice inputsallowed are “FixedSlatAngle�, “MaximizeSolar�, and “BlockBeamSolar�.  The default value is “FixedSlatAngle�.If Type of Slat Angle Control for Blinds = MaximizeSolar the slat angle is adjusted to maximize solar gain. If Type of Slat Angle Control for Blinds = BlockBeamSolar, the slat angle is adjusted to maximize visibiity while eliminating beam solar radiation. If Type of Slat Angle Control for Blinds = FixedSlatAngle, then the model uses a fixed slat angle specified above.
-
-An IDF example for this object, is shown below:
-
-```idf
-WindowMaterial:Blind:EquivalentLayer,
-  VBU8D6+45SW1,      ! - Name
-  Horizontal,        ! - Slat Orientation
-  0.025,             ! - Slat Width
-  0.025,             ! - Slat Separation
-  0.0,               ! - Slat Crown
-  45.0,              ! - Slat Angle
-  0.0,               ! - Front Side Slat Beam-Diffuse Solar Transmittance
-  0.0,               ! - Back Side Slat Beam-Diffuse Solar Transmittance
-  0.0,               ! - Front Side Slat Beam-Diffuse Solar Reflectance
-  0.0,               ! - Back Side Slat Beam-Diffuse Solar Reflectance
-  0.0,               ! - Front Side Slat Beam-Diffuse Visible Transmittance
-  0.0,               ! - Back Side Slat Beam-Diffuse Visible Transmittance
-  0.0,               ! - Front Side Slat Beam-Diffuse Visible Reflectance
-  0.0,               ! - Back Side Slat Beam-Diffuse Visible  Reflectance
-  0.0,               ! - Slat Diffuse-Diffuse Solar Transmittance
-  0.80,              ! - Front Side Slat Diffuse-Diffuse Solar Reflectance
-  0.60,              ! - Back Side Slat Diffuse-Diffuse Solar Reflectance
-  0.0,               ! - Slat Diffuse-Diffuse Visible Transmittance
-  0.0,               ! - Front Side Slat Diffuse-Diffuse Visible Reflectance
-  0.0,               ! - Back Side Slat Diffuse-Diffuse Visible Reflectance
-  0.0,               ! - Slat Infrared Transmittance
-  0.90,              ! - Front Side Slat Infrared Emissivity
-  0.90,              ! - Back Side Slat Infrared Emissivity
-  FixedSlatAngle;    ! - Slat Angle Control
-```
-
-
-### WindowMaterial:Screen:EquivalentLayer
-
-This object specifies the optical and thermal properties of exterior screen materials for Equivalent Layer Window. Can only be placed on the exterior side of window construction. The window screen model assumes the screen is made up of intersecting orthogonally-crossed cylinders. The surface of the cylinders is assumed to be diffusely reflecting. The beam solar radiation transmitted through an equivalent Layer window screen varies with sun angle and is made up of two distinct elements: a beam-beam component and a beam-difuse component. The beam-beam transmittance component is calculated using screen openness area fraction determined from the geometry of the screen and the incident angle of the sun. Empirical correlations are used to obtain the effective off-normal solar and longwave properties of insect screens.  Insect screen geometry is shown in Figure 23.  The calculation of effective solar properties requires a set of properties measured at normal incidence.
-
-![](media/image048.svg)
-
-Figure 23. Geometry used for insect screen analysis
-
-The formulation of the model, assumption and correlations used to calculate effective solar and longwave properties of insect screens are described in the Engineering Reference.
-
-#### Field: Name
-
-Name of the insect screen. It is referenced as an outside layer in an equivalent layer window construction.
-
-#### Field: Screen Beam-Beam Solar Transmittance
-
-This value is the beam-beam transmittance of the screen material at normal incidence. This value is the same as the screen oppenness area fraction.  This value can be autocalculated from the wire spacing and wire diameter. It is the same for both sides of the screen. The minimum value is 0.0, and maximum value is less than 1.0.
-
-#### Field: Screen Beam-Diffuse Solar Transmittance
-
-This value is the beam-diffuse solar transmittance of the screen material at normal incidence averaged over the entire spectrum of solar radiation. Assumed to be the same for both sides of the screen. The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Screen Beam-Diffuse Solar Reflectance
-
-This value is the beam-diffuse solar reflectance of the screen material at normal incidence averaged over the entire spectrum of solar radiation. Assumed to be the same for both sides of the screen. The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Screen Beam-Beam Visible Transmittance
-
-This value is the beam-beam visible transmittance of the screen material at normal incidence averaged over the visible spectrum range of solar radiation.  Assumed to be the same for both sides of the screen. The minimum value is 0.0, and maximum value is less than 1.0. This input input field is not used currently.
-
-#### Field: Screen Beam-Diffuse Visible Transmittance
-
-This value is the beam-diffuse visible reflectance of the screen material at normal incidence averaged over the visible spectrum range of solar radiation. Assumed to be the same for both sides of the screen. The minimum value is 0.0, and the maximum value is less than 1.0. This input input field is not used currently.
-
-#### Field: Screen Beam-Diffuse Visible Reflectance
-
-This value is the beam-diffuse visible reflectance of the screen material at normal incidence averaged over the visible spectrum range of solar radiation. Assumed to be the same for both sides of the screen. The minimum value is 0.0, and the maximum value is less than 1.0. This input input field is not used currently.
-
-#### Field: Screen Infrared Transmittance
-
-This value is the long-wave hemispherical transmittance of the the screen material. Assumed to be the same for both sides of the screen material. The minimum value is 0.0, the maximum value is less than 1.0.  The default value is 0.02
-
-#### Field: Screen Infrared Emissivity
-
-This value is the long-wave hemispherical emissivity of the screen material. Assumed to be the same for both sides of the screen material. The minimum value is 0.0, the maximum value is less than 1.0. The default value is 0.93.
-
-#### Field: Screen Wire Spacing
-
-The spacing, S (m), of the screen material is the distance from the center of one strand of screen to the center of the adjacent one. The spacing of the screen material is assumed to be the same in both directions (e.g., vertical and horizontal). This input value must be greater than the non-zero screen material diameter. If the spacing is different in the two directions, use the average of the two values. Default value is 0.0025m.
-
-#### Field: Screen Wire Diameter
-
-The diameter, D (m), of individual strands or wires of the screen material. The screen material diameter is assumed to be the same in both directions (e.g., vertical and horizontal). This input value must be greater than 0 and less than the screen wire spacing. If the diameter is different in the two directions, use the average of the two values. Default value is 0.005m.
-
-An IDF example for this object, is shown below:
-
-```idf
-WindowMaterial:Screen:EquivalentLayer,
-  INSCRN,                !- Name
-  0.763,                 !- Screen Beam-Beam Solar Transmittance
-  0.052,                 !- Screen Beam-Diffuse Solar Transmittance
-  0.076,                 !- Screen Beam-Diffuse Solar Reflectance
-  0.0,                   !- Screen Beam-Beam Visible Transmittance
-  0.0,                   !- Screen Beam-Diffuse Visible Transmittance
-  0.0,                   !- Screen Beam-Diffuse Visible Reflectance
-  0.0,                   !- Screen Infrared Transmittance
-  0.84,                  !- Screen Infrared Emissivity
-  0.025,                 !- Screen Wire Spacing
-  0.005;                 !- Screen Wire Diameter
-```
-
-
-### WindowMaterial:Glazing:EquivalentLayer
-
-Glass material properties for equivalent layer window model.  Uses transmittance/reflectance input method.  For exterior windows, “front side� is the side of the glass closest to the outside air and “back side� is the side closest to the zone the window is defined in. For interzone windows, “front side� is the side closest to the zone adjacent to the zone the window is defined in and “back side� is the side closest to the zone the window is defined in.
-
-#### Field: Name
-
-The name of the glass layer. It corresponds to a layer in an equivalent layer window construction.
-
-#### Field: Optical Data Type
-
-Valid values for this field are SpectralAverage, or Spectral. If Optical Data Type = SpectralAverage, the values you enter for solar transmittance and reflectance are assumed to be averaged over the solar spectrum, and the values you enter for visible transmittance and reflectance are assumed to be averaged over the solar spectrum and weighted by the response of  the human eye. The spectral data input is not supported now.
-
-***Field: Window Glass Spectral Data Set Name***
-
-This input field is not used currently.
-
-#### Field: Front Side Beam-Beam Solar Transmittance
-
-This value is the front side beam-beam solar transmittance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Back Side Beam-Beam Solar Transmittance
-
-This value is the back side beam-beam solar transmittance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Front Side Beam-Beam Solar Reflectance
-
-This value is the front side beam-beam solar reflectance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Back Side Beam-Beam Solar Reflectance
-
-This value is the back side beam-beam solar reflectance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Front Side Beam-Beam Visible Transmittance
-
-This value is the front side beam-beam visible transmittance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Back Side Beam-Beam Visible Transmittance
-
-This value is the back side beam-beam visible transmittance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Front Side Beam-Beam Visible Reflectance
-
-This value is the front side beam-beam visible reflectance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Back Side Beam-Beam Visible Reflectance
-
-This value is the back side beam-beam visible reflectance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Front Side Beam-Diffuse Solar Transmittance
-
-This value is the front side beam-diffuse solar transmittance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage.  For clear glazing the beam-diffuse transmittance is zero. The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.
-
-#### Field: Back Side Beam-Diffuse Solar Transmittance
-
-This value is the back side beam-diffuse solar transmittance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage.  For clear glazing the beam-diffuse solar transmittance is zero. The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.
-
-#### Field: Front Side Beam-Diffuse Solar Reflectance
-
-This value is the front side beam-diffuse solar reflectance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.
-
-#### Field: Back Side Beam-Diffuse Solar Reflectance
-
-This value is the back side beam-diffuse solar reflectance of the glazing at normal incidence averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.
-
-#### Field: Front Side Beam-Diffuse Visible Transmittance
-
-This value is the front side beam-diffuse visible transmittance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage.  For clear glazing the beam-diffuse visible transmittance is zero. The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.  This input field is not used currently.
-
-#### Field: Back Side Beam-Diffuse Visible Transmittance
-
-This value is the back side beam-diffuse visible transmittance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage.  For clear glazing the beam-diffuse visible transmittance is zero. The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0.  This input field is not used currently.
-
-#### Field: Front Side Beam-Diffuse Visible Reflectance
-
-This value is the front side beam-diffuse visible reflectance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0. This input field is not used currently.
-
-#### Field: Back Side Beam-Diffuse Visible Reflectance
-
-This value is the back side beam-diffuse visible reflectance of the glazing at normal incidence averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage.  The minimum value is 0.0, and the maximum value is less than 1.0. Default value is 0.0. This input field is not used currently.
-
-#### Field: Diffuse-Diffuse Solar Transmittance
-
-This value is the diffuse-diffuse solar transmittance of the glazing averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage. The diffuse-diffuse transmittance is assumed to be the same for both sides of the glazing.  EnergyPlus automatically estimates the diffuse-diffuse solar transmittance from other inputs. If this input field is specified as “Autocalculate�, then the calculated transmittance will be used. The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Front Side Diffuse-Diffuse Solar Reflectance
-
-This value is the front side diffuse-diffuse solar reflectance of the glazing averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage. EnergyPlus automatically estimates the diffuse-diffuse reflectance from other inputs. If this input field is specified as “Autocalculate�, then the calculated reflectance will be used. The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Back Side Diffuse-Diffuse Solar Reflectance
-
-This value is the back side diffuse-diffuse solar reflectance of the glazing averaged over the entire spectrum of solar radiation.  Used only when Optical Data Type = SpectralAverage. EnergyPlus automatically estimates the diffuse-diffuse reflectance from other inputs. If this input field is specified as “Autocalculate�, then the calculated reflectance will be used. The minimum value is 0.0, and the maximum value is less than 1.0.
-
-#### Field: Diffuse-Diffuse Visible Solar Transmittance
-
-This value is the diffuse-diffuse visible transmittance of the glazing averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage. The diffuse-diffuse visible transmittance is assumed to be the same for both sides of the glazing.  If this input field is specified as “Autocalculate�, then the calculated transmittance will be used. The minimum value is 0.0, and the maximum value is less than 1.0. This input field is not used currently.
-
-#### Field: Front Side Diffuse-Diffuse Visible Reflectance
-
-This value is the front side diffuse-diffuse visible reflectance of the glazing averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage. EnergyPlus automatically estimates the front side diffuse-diffuse visible reflectance from front side beam-beam visible reflectance at normal incidence specified above. If this input field is specified as “Autocalculate�, then the calculated reflectance will be used. The minimum value is 0.0, and the maximum value is less than 1.0. This input field is not used currently.
-
-#### Field: Back Side Diffuse-Diffuse Visible Reflectance
-
-This value is the back side diffuse-diffuse visible reflectance of the glazing averaged over the visible spectrum range of solar radiation.  Used only when Optical Data Type = SpectralAverage. EnergyPlus automatically estimates the back side diffuse-diffuse visible reflectance from back side beam-beam visible reflectance at normal incidence specified above. If this input field is specified as “Autocalculate�, then the calculated reflectance will be used. The minimum value is 0.0, and the maximum value is less than 1.0. This input field is not used currently.
-
-#### Field: Infrared Transmittance (applies to front and back)
-
-This value is the long-wave hemispherical transmittance of the glazing. Assumed to be the same for both sides of the glazing. The minimum value is 0.0, the maximum value is less than 1.0.  The default value is 0.0.
-
-#### Field: Front Side Infrared Emissivity
-
-This value is the front side long-wave hemispherical emissivity of the glazing. The minimum value is 0.0, the maximum value is less than 1.0.  The default value is 0.84.
-
-#### Field: Back Side Infrared Emissivity
-
-This value is the back side long-wave hemispherical emissivity of the glazing. The minimum value is 0.0, the maximum value is less than 1.0.  The default value is 0.84.
-
-An IDF example for this object, is shown below:
-
-```idf
-WindowMaterial:Glazing:EquivalentLayer,
-  GLZCLR,                  !- Name
-  SpectralAverage,         !- Optical Data Type
-  ,                        !- Window Glass Spectral Data Set Name
-  0.83,                    !- Front Side Beam-Beam Solar Transmittance
-  0.83,                    !- Back Side Beam-Beam Solar Transmittance
-  0.08,                    !- Front Side Beam-Beam Solar Reflectance
-  0.08,                    !- Back Side Beam-Beam Solar Reflectance
-  0.0,                     !- Front Side Beam-Beam Visible Transmittance
-  0.0,                     !- Back Side Beam-Beam Visible Transmittance
-  0.0,                     !- Front Side Beam-Beam Visible Reflectance
-  0.0,                     !- Back Side Beam-Beam Visible Reflectance
-  0.0,                     !- Front Side Beam-Diffuse Solar Transmittance
-  0.0,                     !- Back Side Beam-Diffuse Solar Transmittance
-  0.0,                     !- Front Side Beam-Diffuse Solar Reflectance
-  0.0,                     !- Back Side Beam-Diffuse Solar Reflectance
-  0.0,                     !- Front Side Beam-Diffuse Visible Transmittance
-  0.0,                     !- Back Side Beam-Diffuse Visible Transmittance
-  0.0,                     !- Front Side Beam-Diffuse Visible Reflectance
-  0.0,                     !- Back Side Beam-Diffuse Visible Reflectance
-  0.76,                    !- Diffuse-Diffuse Solar Transmittance
-  0.14,                    !- Front Side Diffuse-Diffuse Solar Reflectance
-  0.14,                    !- Back Side Diffuse-Diffuse Solar Reflectance
-  0.0,                     !- Diffuse-Diffuse Visible Transmittance
-  0.0,                     !- Front Side Diffuse-Diffuse Visible Reflectance
-  0.0,                     !- Back Side Diffuse-Diffuse Visible Reflectance
-  0.0,                     !- Infrared Transmittance
-  0.84,                    !- Front Side Infrared Emissivity
-  0.84;                    !- Back Side Infrared Emissivity
-```
-
-
-### WindowMaterial:Gap:EquivalentLayer
-
-This object is used in windows equivalent layer construction object andspecifies the properties of the gap between the layers in multi-layer equivalent layer window object. There is an EnergyPlus Reference Data Set for Material:WindowGas that contains several types of gas. This object uses the gas types: Air, Argon, Xenon, Crypton, and Custom.  For Custom gas type users are required to entering the thermophicial properties.
-
-#### Field: Name
-
-The name of the gap. It refers to a layer in a window construction equivalent layer.
-
-#### Field: Gas Type
-
-The type of gas. The choices allowed are AIR, ARGON, XENON, KRYPTON, or CUSTOM.
-
-#### Field: Thickness
-
-The thickness (m) of the gap layer.
-
-#### Field: Gap Vent Type
-
-This inputfiled contains the valid key choice for gap vent type.  The valid vent types are: Sealed, VentedIndoor, and VentedOutdoor.  Sealed means the gap is enclosed and gas tight, i.e., no venting to indoor or outdoor environment. The gap types “VentedIndoor� and “VentedOutdoor� are used with gas type “Air� only. VentedIndoor means the air in the gap is naturally vented to indoor environment, and  VentedOutdoor means the air in the gap is naturally vented to the outdoor environment.
-
-#### Properties for Custom Gas Types
-
-The following entries are used only if Gas Type = Custom. The A, B and C coefficients are those in the following expression that gives a property value as a function of temperature in degrees K:
-
-<div>\[Property = Coef{f_A} + Coef{f_B} \times Temperatur{e_K} + Coef{f_C} \times Temperature_K^2\]</div>
-
-#### Field: Conductivity Coefficient A
-
-The A coefficient for gas conductivity (W/m-K). Used only if Gas Type = Custom.
-
-#### Field: Conductivity Coefficient B
-
-The B coefficient for gas conductivity (W/m-K<sup>2</sup>). Used only if Gas Type = Custom.
-
-#### Field: Conductivity Coefficient C
-
-The C coefficient for gas conductivity (W/m-K<sup>3</sup>).  Used only if Gas Type = Custom.
-
-#### Field: Viscosity Coefficient A
-
-The A coefficient for gas viscosity (kg/m-s). Used only if Gas Type = Custom.
-
-#### Field: Viscosity Coefficient B
-
-The B coefficient for gas viscosity (kg/m-s-K). Used only if Gas Type = Custom.
-
-#### Field: Viscosity Coefficient C
-
-The C coefficient for gas viscosity (kg/m-s-K<sup>2</sup>).  Used only if Gas Type = Custom.
-
-#### Field: Specific Heat Coefficient A
-
-The A coefficient for gas specific heat (J/kg-K). Used only if Gas Type = Custom.
-
-#### Field: Specific Heat Coefficient B
-
-The B coefficient for gas specific heat (J/kg-K<sup>2</sup>). Used only if Gas Type = Custom.
-
-#### Field: Specific Heat Coefficient C
-
-The C coefficient for gas specific heat (J/kg-K<sup>2</sup>).  Used only if Gas Type = Custom.
-
-#### Field: Specific Heat Ratio
-
-The specific heat ratio for gas.  Used only if Gas Type = Custom.
-
-#### Field: Molecular Weight
-
-The molecular weight for gas.  The molecular weight is the mass of 1 mol of the substance.  This has a numerical value which is the average molecular mass of the molecules in the substance multiplied by Avogadro’s constant. (kg/kmol) (Shown in the IDD as g/mol for consistency)
-
-#### Field: Specific Heat Ratio
-
-The specific heat ratio for gas.  The specific heat ratio of a gas is the ratio of the specific heat at contant pressure, to the specific heat at constant volume.  Used only if Gas Type = Custom.
-
-An IDF example for this object, is shown below:
-
-```idf
-WindowMaterial:Gap:EquivalentLayer,
-  Custom CO2 Sealed 12mm,    !- Name
-  CUSTOM,                    !- Gas Type
-  0.0120,                    !- Thickness {m}
-  Sealed,                    !- Gap Vent Type
- -5.8181E-3,                 !- Conductivity Coefficient A {W/m-K}
-  7.4714E-5,                 !- Conductivity Coefficient B {W/m-K2}
-  0.0,                       !- Conductivity Coefficient C {W/m-K3}
-  8.5571E-7,                 !- Viscosity Coefficient A {kg/m-s}
-  4.7143E-8,                 !- Viscosity Coefficient B {kg/m-s-K}
-  0.0,                       !- Viscosity Coefficient C {kg/m-s-K2}
-  5.76903E2,                 !- Specific Heat Coefficient A {J/kg-K}
-  9.18088E-2,                !- Specific Heat Coefficient B {J/kg-K2}
-  0.0,                       !- Specific Heat Coefficient C {J/kg-K3}
-  44.01;                     !- Molecular Weight {g/mol}
-```
-
-
-### Material:RoofVegetation
-
-This definition must be used in order to simulate the green roof (ecoroof) model. The material becomes the outside layer in a green roof construction (see example below). In the initial release of the green roof model, only one material may be used as a green roof layer though, of course, several constructions using that material may be used. In addition, the model has only been tested with the ConductionTransferFunction solution algorithm – a warning will be issued for other solution algorithm choices. This model was developed for low-sloped exterior surfaces (roofs). It is not recommended for high-sloped exterior surfaces (e.g., walls).
-
-#### Field: Name
-
-This field is a unique reference name that the user assigns to a particular ecoroof material. This name can then be referred to by other input data.
-
-#### Field: Height of Plants
-
-This field defines the height of plants in units of meters. This field is limited to values in the range 0.005 &lt; Height &lt; 1.00 m. Default is .2 m.
-
-#### Field: Leaf Area Index
-
-This is the projected leaf area per unit area of soil surface. This field is dimensionless and is limited to values in the range of 0.001 &lt; LAI &lt; 5.0. Default is 1.0. At the present time the fraction vegetation cover is calculated directly from LAI (Leaf Area Index) using an empirical relation. The user may find it necessary to increase the specified value of LAI in order to represent high fractional coverage of the surface by vegetation.
-
-#### Field: Leaf Reflectivity
-
-This field represents the fraction of incident solar radiation that is reflected by the individual leaf surfaces (albedo). Solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. Values for this field must be between 0.05 and 0.5. Default is .22. Typical values are .18 to .25.
-
-#### Field: Leaf Emissivity
-
-This field is the ratio of thermal radiation emitted from leaf surfaces to that emitted by an ideal black body at the same temperature. This parameter is used when calculating the long wavelength radiant exchange at the leaf surfaces. Values for this field must be between 0.8 and 1.0 (with 1.0 representing “black body� conditions). Default is .95.
-
-#### Field: Minimum Stomatal Resistance
-
-This field represents the resistance of the plants to moisture transport. It has units of s/m. Plants with low values of stomatal resistance will result in higher evapotranspiration rates than plants with high resistance. Values for this field must be in the range of 50.0 to 300.0. Default is 180.
-
-#### Field: Soil Layer Name
-
-This field is a unique reference name that the user assigns to the soil layer for a particular ecoroof. This name can then be referred to by other input data. Default is **Green Roof Soil**.
-
-#### Field: Roughness
-
-This alpha field defines the relative roughness of a particular material layer. This parameter only influences the convection coefficients, more specifically the exterior convection coefficient. A keyword is expected in this field with the options being “VeryRough�, “Rough�, “MediumRough�, “MediumSmooth�, “Smooth�, and “VerySmooth� in order of roughest to smoothest options. Default is MediumRough.
-
-#### Field: Thickness
-
-This field characterizes the thickness of the material layer in meters. This should be the dimension of the layer in the direction perpendicular to the main path of heat conduction. This value must be a positive number. Depths of .10m (4 inches) and .15m (6 inches) are common. Default if this field is left blank is .1. Maximum is .7m. Must be greater than .05 m.
-
-#### Field: Conductivity of Dry Soil
-
-This field is used to enter the thermal conductivity of the material layer. Units for this parameter are W/(m-K). Thermal conductivity must be greater than zero. Typical soils have values from .3 to .5. Minimum is .2 (specified in IDD). Default is .35 and maximum (in IDD) is 1.5.
-
-#### Field: Density of Dry Soil
-
-This field is used to enter the density of the material layer in units of kg/m<sup>3</sup>. Density must be a positive quantity. Typical soils range from 400 to 1000 (dry to wet). Minimum is 300, maximum is 2000 and default if field is left blank is 1100.
-
-#### Field: Specific Heat of Dry Soil
-
-This field represents the specific heat of the material layer in units of J/(kg-K). Note that these units are most likely different than those reported in textbooks and references which tend to use kJ/(kg-K) or J/(g-K). They were chosen for internal consistency within EnergyPlus. Only positive values of specific heat are allowed.
-
-#### Field: Thermal Absorptance
-
-The thermal absorptance field in the Material input syntax represents the fraction of incident long wavelength radiation that is absorbed by the material. This parameter is used when calculating the long wavelength radiant exchange between various surfaces and affects the surface heat balances (both inside and outside as appropriate). For long wavelength radiant exchange, thermal emissivity and thermal emittance are equal to thermal absorptance. Values for this field must be between 0.0 and 1.0 (with 1.0 representing “black body� conditions). Typical values are from .9 to .98. The default value for this field is 0.9.
-
-#### Field: Solar Absorptance
-
-The solar absorptance field in the Material input syntax represents the fraction of incident  solar radiation that is absorbed by the material. Solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident solar radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate). If solar reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.0 and 1.0. Typical values are from .6 to .85. The default value for this field is 0.7.
-
-#### Field: Visible Absorptance
-
-The visible absorptance field in the Material input syntax represents the fraction of incident visible wavelength radiation that is absorbed by the material. Visible wavelength radiation is slightly different than solar radiation in that the visible band of wavelengths is much more narrow while solar radiation includes the visible spectrum as well as infrared and ultraviolet wavelengths. This parameter is used when calculating the amount of incident visible radiation absorbed by various surfaces and affects the surface heat balances (both inside and outside as appropriate) as well as the daylighting calculations. If visible reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials). Values for this field must be between 0.5 and 1.0. The default value for this field is 0.75.
-
-#### Field: Saturation Volumetric Moisture Content of the Soil Layer
-
-The field allows for user input of the saturation moisture content of the soil layer. Maximum moisture content is typically less than .5. Range is [.1,.5] with the default being .3.
-
-#### Field: Residual Volumetric Moisture Content of the Soil Layer
-
-The field allows for user input of the residual moisture content of the soil layer. Default is .01, range is [.01,.1].
-
-#### Field: Initial Volumetric Moisture Content of the Soil Layer
-
-The field allows for user input of the initial moisture content of the soil layer. Range is (.05, .5] with the defaulte being .1.
-
-#### Field: Moisture Diffusion Calculation Method
-
-The field allows for two models to be selected: **Simple** or **Advanced**.
-
-**Simple** is the original Ecoroof model - based on a constant diffusion of moisture through the soil.  This model starts with the soil in two layers.  Every time the soil properties update is called, it will look at the two soils moisture layers and asses which layer has more moisture in it. It then takes moisture from the higher moisture layer and redistributes it to the lower moisture layer at a constant rate.
-
-**Advanced** is the later Ecoroof model. If you use it, you will need to increase your number of timesteps in hour for the simulation with a recommended value of 20. This moisture transport model is based on a project which looked at the way moisture transports through soil.  It uses a finite difference method to divide the soil into layers (nodes). It redistributes the soil moisture according the model described in:
-
-Marcel G Schaap and Martinus Th. van Genuchten, 2006, 'A modified Maulem-van Genuchten Formulation for Improved Description of the Hydraulic Conductivity Near Saturation’, Vadose Zone Journal 5 (1), p 27-34.
-
-An IDF example:
-
-```idf
-Material:RoofVegetation,
-    BaseEco,                 !- Name
-    0.5,                     !- Height of Plants {m}
-    5,                       !- Leaf Area Index {dimensionless}
-    0.2,                     !- Leaf Reflectivity {dimensionless}
-    0.95,                    !- Leaf Emissivity
-    180,                     !- Minimum Stomatal Resistance {s/m}
-    EcoRoofSoil,             !- Soil Layer Name
-    MediumSmooth,            !- Roughness
-    0.18,                    !- Thickness {m}
-    0.4,                     !- Conductivity of Dry Soil {W/m-K}
-    641,                     !- Density of Dry Soil {kg/m3}
-    1100,                    !- Specific Heat of Dry Soil {J/kg-K}
-    0.95,                    !- Thermal Absorptance
-    0.8,                     !- Solar Absorptance
-    0.7,                     !- Visible Absorptance
-   0.4,                     !- Saturation Volumetric Moisture Content of the Soil Layer
-    0.01,                    !- Residual Volumetric Moisture Content of the Soil Layer
-    0.2,                     !- Initial Volumetric Moisture Content of the Soil Layer
-    Advanced;                !- Moisture Diffusion Calculation Method
-
-
-  Material:RoofVegetation,
-    LowLAI,                  !- Name
-    0.5,                     !- Height of Plants {m}
-    0.5,                     !- Leaf Area Index {dimensionless}
-    0.2,                     !- Leaf Reflectivity {dimensionless}
-    0.95,                    !- Leaf Emissivity
-    180,                     !- Minimum Stomatal Resistance {s/m}
-    EcoRoofSoil,             !- Soil Layer Name
-    MediumSmooth,            !- Roughness
-    0.18,                    !- Thickness {m}
-    0.4,                     !- Conductivity of Dry Soil {W/m-K}
-    641,                     !- Density of Dry Soil {kg/m3}
-    1100,                    !- Specific Heat of Dry Soil {J/kg-K}
-    0.95,                    !- Thermal Absorptance
-    0.8,                     !- Solar Absorptance
-    0.7,                     !- Visible Absorptance
-   0.4,          !- Saturation Volumetric Moisture Content of the Soil Layer
-    0.01,         !- Residual Volumetric Moisture Content of the Soil Layer
-    0.2,          !- Initial Volumetric Moisture Content of the Soil Layer
-    Advanced;                !- Moisture Diffusion Calculation Method
-```
-
-
-And construction using the ecoroof material:
-
-```idf
-Construction,
-    ASHRAE 90.1-2004_Sec 5.5-2_Roof,  !- Name
-    BaseEco,                 !- Outside Layer
-    ASHRAE 90.1-2004_Sec 5.5-2_Roof Insulation_1,  !- Layer \#2
-    ASHRAE 90.1-2004_Sec 5.5-2_MAT-METAL;  !- Layer \#3
-```
-
-
-### Ecoroof / RoofVegetation outputs
-
-The following outputs are available for the Roof Vegetation surface.
-
-* Zone,Average,Green Roof Soil Temperature [C]
-
-* Zone,Average,Green Roof Vegetation Temperature [C]
-
-* Zone,Average,Green Roof Soil Root Moisture Ratio []
-
-* Zone,Average,Green Roof Soil Near Surface Moisture Ratio []
-
-* Zone,Average,Green Roof Soil Sensible Heat Transfer Rate per Area [W/m2]
-
-* Zone,Average,Green Roof Vegetation Sensible Heat Transfer Rate per Area [W/m2]
-
-* Zone,Average,Green Roof Vegetation Moisture Transfer Rate [m/s]
-
-* Zone,Average,Green Roof Soil Moisture Transfer Rate [m/s]
-
-* Zone,Average,Green Roof Vegetation Latent Heat Transfer Rate per Area [W/m2]
-
-* Zone,Average,Green Roof Soil Latent Heat Transfer Rate per Area [W/m2]
-
-* Zone,Sum,Green Roof Cumulative Precipitation Depth [m]
-
-* Zone,Sum,Green Roof Cumulative Irrigation Depth [m]
-
-* Zone,Sum,Green Roof Cumulative Runoff Depth [m]
-
-* Zone,Sum,Green Roof Cumulative Evapotranspiration Depth [m]
-
-* Zone,Sum,Green Roof Current Precipitation Depth [m]
-
-* Zone,Sum,Green Roof Current Irrigation Depth [m]
-
-* Zone,Sum,Green Roof Current Runoff Depth [m]
-
-* Zone,Sum,Green Roof Current Evapotranspiration Depth [m]
-
-
-#### Green Roof Soil Temperature [C]
-
-Temperature of the Soil layer temperature in C.
-
-#### Green Roof Vegetation Temperature [C]
-
-Temperature of the Vegetation layer temperature in C.
-
-#### Green Roof Soil Root Moisture Ratio []
-
-Mean value of root moisture (m<sup>3</sup>/m<sup>3</sup>)
-
-#### Green Roof Soil Near Surface Moisture Ratio []
-
-The moisture content in the soil near the surface (m<sup>3</sup>/m<sup>3</sup>)
-
-#### Green Roof Soil Sensible Heat Transfer Rate per Area [W/m2]
-
-Sensible heat flux to ground (W/m<sup>2</sup>)
-
-#### Green Roof Vegetation Sensible Heat Transfer Rate per Area [W/m2]
-
-Sensible heat transfer to foliage (W/m<sup>2</sup>)
-
-#### Green Roof Vegetation Moisture Transfer Rate [m/s]
-
-Water evapotranspiration rate associated with latent heat from vegetation (m/s)
-
-#### Green Roof Soil Moisture Transfer Rate [m/s]
-
-Water evapotranspiration rate associated with latent heat from ground surface (m/s)
-
-#### Green Roof Vegetation Latent Heat Transfer Rate per Area [W/m2]
-
-Latent heat flux from vegetation (W/m<sup>2</sup>)
-
-#### Green Roof Soil Latent Heat Transfer Rate per Area [W/m2]
-
-Latent heat flux from ground surface (W/m<sup>2</sup>)
-
-#### Green Roof Cumulative Precipitation Depth [m]
-
-#### Green Roof Current Precipitation Depth [m]
-
-Cumulative or current precipitation (m)
-
-#### Green Roof Cumulative Irrigation Depth [m]
-
-#### Green Roof Current Irrigation Depth [m]
-
-Cumulative or current irrigation (m)
-
-#### Green Roof Cumulative Runoff Depth [m]
-
-#### Green Roof Current Runoff Depth [m]
-
-Cumulative or current runoff (m). Multiply by roof area to get volume.
-
-#### Green Roof Cumulative Evapotranspiration Depth [m]
-
-#### Green Roof Current Evapotranspiration Depth [m]
-
-Cumulative or current evapotranspiration from soil and plants (m).
-
-### MaterialProperty:GlazingSpectralData
-
-With the MaterialProperty:GlazingSpectralData object, you can specify the wavelength-by-wavelength transmittance and reflectance properties of a glass material. To determine the  overall optical properties of a glazing system (solar and visible transmittance and solar absorptance vs. angle of incidence) EnergyPlus first calculates transmittance and absorptance vs. angle of incidence for each wavelength. This is then weighted by a standard solar spectrum to get the solar transmittance and absorptance vs. angle of incidence (for use in the solar heat gain calculations), and further weighted by the response of the human eye to get the visible transmittance vs. angle of incidence (for use in the daylighting calculation).
-
-MaterialProperty:GlazingSpectralData should be used for multi-pane windows when one or more of the glass layers is *spectrally selective*, i.e., the transmittance depends strongly on wavelength. An example is glass with a coating that gives high transmittance in the daylight part of the solar spectrum (roughly 0.4 to 0.7 microns) and low transmittance at longer wavelengths, thus providing better solar heat gain control than uncoated glass. If spectral data is not used in case, the overall optical properties of the glazing system that EnergyPlus calculates will not be correct.
-
-You can input up to 450 sets of values for wavelengths covering the solar spectrum. Each set consists of  {wavelength (microns), transmittance, front reflectance, back reflectance}
-
-Spectral data of this kind are routinely measured by glass manufacturers. Data sets for over 800 commercially available products are contained in an Optical Data Library maintained by the Windows Group at Lawrence Berkeley National Laboratory. This library can be downloaded from http://windows.lbl.gov/. You will have to edit entries from this library to put them in the format required by the EnergyPlus WindowGlassSpectralData object.
-
-An alternative to using the MaterialProperty:GlazingSpectralData object is to run the WINDOW window analysis program. This program has built-in access to the Optical Data Library and let’s you easily create customized, multi-layer glazing systems that can be exported for use in EnergyPlus. For more details, see “StormWindow�.
-
-#### Field: Name
-
-The name of the spectral data set. It is referenced by WindowMaterial:Glazing when Optical Data Type = Spectral.
-
-#### Fields 1-4 (repeated up to 450 times)
-
-Sets of values for wavelengths covering the solar spectrum (from about 0.25 to 2.5 microns [10<sup>-6</sup> m]). Each set consists of
-
-**{wavelength (microns), transmittance, front reflectance, back reflectance}**
-
-The wavelength values must be in ascending order. The transmittance and reflectance values are at normal incidence. “Front reflectance� is the reflectance for radiation striking the glass from the outside, i.e., from the side opposite the zone in which the window is defined. “Back reflectance� is the reflectance for radiation striking the glass from the inside, i.e., from the zone in which the window is defined. Therefore, for exterior windows, “front� is the side closest to the outdoors and “back� is the side closest to the zone in which the window is defined. For interior windows, “front� is the side closest to the adjacent zone and “back� is the side closest to the zone in which the window is defined.
-
-An IDF example:
-
-```idf
-MaterialProperty:GlazingSpectralData,
-      TestSpectralDataSet,
-       ! { from WINDOW 4 library }
-       ! { actual 9.91mm clear laminate: 15_mil PVB, ID:37966/50032-39-9 } 10.38
-       ! { conductivity PVB adjusted, W/M/K  } 0.798
-       ! { thermal IR transmittance, assumed } tir=0.00
-       ! { thermal IR hemispherical emittance, assumed } emis= 0.84 0.84
-
-
-       ! WL   T     Rfront Rback
-       .300, 0.000, 0.045, 0.045,
-       .310, 0.000, 0.044, 0.044,
-       .320, 0.000, 0.044, 0.044,
-       .330, 0.000, 0.042, 0.042,
-       .340, 0.000, 0.041, 0.041,
-       .350, 0.000, 0.040, 0.040,
-      <snip>
-      2.450, 0.200, 0.040, 0.040,
-      2.500, 0.214, 0.039, 0.039;
-```
-
-### Construction
-
-For walls, roofs, floors, windows, and doors, constructions are “built� from the included materials. Each layer of the construction is a material name listed in order from “outside� to “inside�. Up to ten layers (eight for windows) may be specified (one of the few limitations in EnergyPlus!). “Outside� is the layer furthest away from the Zone air (not necessarily the outside environment). “Inside� is the layer next to the Zone air. In the example floor below, for example, the outside layer is the acoustic tile below the floor, the next layer is the air space above the tile, and the inside layer is the concrete floor deck.
-
-![](media/image050.svg)
-
-Figure 24. Example Floor Construction illustration.
-
-Window constructions are similarly built up from items in the Window Materials set using similar layers.. See Figure 25. Illustration for material ordering in windows, which shows the case where an interior shading layer such as a blind is present. The gap between the inside glass layer (layer \#3) and the interior shading layer is not entered. Similarly, for an exterior shading layer, the gap between the outside glass layer and the shading layer is not entered.
-
-![](media/image051.svg)
-
-Figure 25. Illustration for material ordering in windows.
-
-However, for a between-glass shading device the gaps on either side of the shading layer must be entered and they must have the same gas type. In addition, the gap widths with and without the between-glass shading layer must be consistent (see Figure 26).
-
-A maximum of four glass layers and one shading layer is allowed. A gas layer must always separate adjacent glass layers in a multi-pane glazing without a between-glass shading layer.
-
-![](media/image052.svg)
-
-Figure 26. Window construction with and without a between-glass shading layer. Shown are gap widths *g*, *g<sub>1</sub>* and *g<sub>2</sub>*, and shading layer width, *w*. An error will result if *g<sub>1</sub>+g<sub>2</sub>+w* is not equal to *g*, where *w* is zero for a blind and greater than zero for a shade.
-
-Outside and inside air film resistances are never given as part of a construction definitions since they are calculated during the EnergyPlus simulation. Note also that constructions are assumed to be one-dimensional in a direction perpendicular to the surface.
-
-#### Field: Name
-
-This field is a user specified name that will be used as a reference by other input syntax. For example, a heat transfer surface (ref: Building Surfaces) requires a construction name to define what the make-up of the wall is. This name must be identical to one of the Construction definitions in the input data file.
-
-#### Field: Outside Layer
-
-Each construction must have at least one layer. This field defines the material name associated with the layer on the outside of the construction—outside referring to the side that is not exposed to the zone but rather the opposite side environment, whether this is the outdoor environment or another zone. Material layers are defined based on their thermal properties elsewhere in the input file (ref: Material and Material Properties and Zone,Average,HAMT Surface Average Water Content Ratio [kg/kg]
-
-Zone,Average,HAMT Surface Inside Face Temperature [C]
-
-Zone,Average,HAMT Surface Inside Face Relative Humidity [%]
-
-Zone,Average,HAMT Surface Inside Face Vapor Pressure [Pa]
-
-Zone,Average,HAMT Surface Outside Face Temperature [C]
-
-Zone,Average,HAMT Surface Outside Face Relative Humidity [%]
-
-Zone,Average,HAMT Surface Inside Face Relative Humidity [%]
-
-#### HAMT Surface Average Water Content Ratio [kg/kg]
-
-This output is the summed water content [kg/kg] of all cells in a surface expressed as a fraction of the mass of the water to the material mass.
-
-#### HAMT Surface Inside Face Temperature [C]
-
-This output is the temperature [C] on the internal “surface� of the surface.
-
-#### HAMT Surface Inside Face Relative Humidity [%]
-
-#### HAMT Surface Inside Face Relative Humidity [%]
-
-This output is the relative humidity on the internal “surface� of the surface expressed as a percentage.
-
-#### HAMT Surface Inside Face Vapor Pressure [Pa]
-
-This output is the vapor pressure [Pa] on the internal “surface� of the surface.
-
-#### HAMT Surface Outside Face Temperature [C]
-
-This output is the temperature on the external “surface� of the surface.
-
-#### HAMT Surface Outside Face Relative Humidity [%]
-
-This output is the relative humidity on the external “surface� of the surface.
-
-Zone,Average,HAMT Surface Temperature Cell N [C]
-
-Zone,Average,HAMT Surface Water Content Cell N [kg/kg]
-
-Zone,Average,HAMT Surface Relative Humidity Cell N [%]
-
-Detailed profile data for the variables Temperature [C], Relative Humidity [%] and Water Content [kg/kg] within each surface can also be reported. To calculate the heat and moisture transfer through surfaces HAMT splits up surfaces into discrete cells. Each cell is composed of a single material and has a position within the surface. HAMT automatically assigns cells to construction objects so that there are more cells closer to boundaries between materials and also at the “surfaces� of the surface. It is not possible for users to define their own cells.
-
-#### HAMT Surface Relative Humidity Cell &lt;N&gt; [%]
-
-This is the relative humidity of the cell in the surface.
-
-#### HAMT Surface Temperature Cell &lt;N&gt; [C]
-
-This is the temperature of the cell in the surface.
-
-#### HAMT Surface Water Content Cell &lt;N&gt; [kg/kg]
-
-This is the relative water content of the cell in the surface.
-
-Each surface is made from a particular construction. The construction-surface relationship is output by HAMT to the eplusout.eio file with the following format.
-
-! &lt;HAMT cells&gt;, Surface Name, Construction Name, Cell Numbers
-
-! &lt;HAMT origins&gt;, Surface Name, Construction Name, Cell origins (m)
-
-The output also contains the HAMT cell origins and cell number for each construction – surface combination. The coordinate system origin is defined as the exterior surface of the construction. Users can select any one of the Temperature, Relative Humidity or Water Content variables for any cell to be reported, using the following naming scheme for the output variable.
-
-HAMT Profile Construction &lt;Variable&gt; Cell &lt;Cell\#&gt;
-
-It is better to specify the “key� or Surface Name in this output.
-
-So for example to output the temperature of the 10<sup>th</sup> cell in a surface, eg “East Wall� would require the following output variable.
-
-```idf
-Output:Variable,
-    East Wall,               !- Key Value
-    HAMT Profile Construction Temperature Cell 10,  !- Variable Name
-    Hourly;                  !- Reporting Frequency
-```
-
-By selecting a whole range of these reports and using the information in the eplusout.eio file it is possible to build up a temperature profile of the surface.
-
-Materials for Glass Windows and Doors). As noted above, the outside layer should NOT be a film coefficient since EnergyPlus will calculate outside convection and radiation heat transfer more precisely.
-
-#### Field(s) 2-10: Layers
-
-The next fields are optional and the number of them showing up in a particular Construction definition depends solely on the number of material layers present in that construction. The data expected is identical to the outside layer field (see previous field description). The order of the remaining layers is important and should be listed in order of occurrence from the one just inside the outside layer until the inside layer is reached. As noted above, the inside layer should NOT be a film coefficient since EnergyPlus will calculate inside convection and radiation heat transfer more precisely.
-
-IDF Example (floor construction):
-
-```idf
-Construction, FLOOR38,  ! Material layer names follow:
-      E5 - ACOUSTIC TILE,
-      E4 - CEILING AIRSPACE,
-      C12 - 2 IN HW CONCRETE;
-```
-
-IDF Example (window construction, no shade):
-
-```idf
-Construction, DOUBLE PANE WINDOW,  !- Material layer names follow:
-      GLASS - CLEAR SHEET 1 / 8 IN,
-      WinAirB1 - AIRSPACE RESISTANCE,
-      GLASS - CLEAR SHEET 1 / 8 IN;
-```
-
-
-IDF Example (window construction, with interior shade):
-
-```idf
-Construction, DOUBLE PANE WITH ROLL SHADE,  !- Material layer names follow:
-      GLASS - CLEAR SHEET 1 / 8 IN,
-      WinAirB1 - AIRSPACE RESISTANCE,
-      GLASS - CLEAR SHEET 1 / 8 IN,
-      ROLL SHADE - LIGHT
-```
-
-
-### Site:GroundTemperature:FCfactorMethod
-
-Site:GroundTemperature:FCfactorMethod is used only by the underground walls or slabs-on-grade or underground floors defined with C-factor (Construction:CfactorUndergroundWall) and F-factor (Construction:FfactorGroundFloor) method for code compliance calculations where detailed construction layers are unknown. Only one such ground temperature object can be included. The monthly ground temperatures for this object are close to the monthly outside air temperatures delayed by three months. If user does not input this object in the IDF file, it will be defaulted to the 0.5m set of monthly ground temperatures from the weather file if they are available.
-
-#### Field: Month Temperature(s) – 12 fields in all
-
-Each numeric field is the monthly ground temperature (degrees Celsius) used for the indicated month (January=1<sup>st</sup> field, February=2<sup>nd</sup> field, etc.)
-
-And, the IDF example:
-
-```idf
-Site:GroundTemperature:FCfactorMethod,  9.5,3.5,-0.7,-1.7,-0.6,3.6,9.3,14,18.2,22.7,21.2,16.8;
-```
-
-### Constructions - Modeling Underground Walls and Ground Floors Defined with C and F Factors for Building Energy Code Compliance
-
-Building energy code and standards like ASHRAE 90.1, 90.2 and California Title 24 require the underground wall constructions and slabs-on-grade or underground floors not to exceed certain maximum values of C-factor and F-factor, which do not specify detailed layer-by-layer materials for the constructions.
-
-A simplified approach is introduced to create equivalent constructions and model the ground heat transfer through underground walls and ground floors for the building energy code compliance calculations. The approach is to create constructions based on the user defined C or F factor with two layers: one concrete layer (0.15 m thick) with thermal mass, and one fictitious insulation layer with no thermal mass. Three new objects were created for such purpose: **Construction:CfactorUndergroundWall**, **Construction:FfactorGroundFloor**, and **Site:GroundTemperature:FCfactorMethod**. Details of the approach are described in the Engineering Reference document. The wall and floor construction objects are described in this section; the ground temperature object is described with the other ground temperature objects.
-
-When a underground wall or ground floor surface (BuildingSurface:Detailed, Floor:Detailed, and Wall:Detailed) references one of the two construction objects, its field ‘Outside Boundary Condition’ needs to be set to GroundFCfactorMethod. For simple (rectangular) wall and floor objects, the outside boundary condition is inferred from the construction type.
-
-The Site:GroundTemperature:FCfactorMethod is described in the section for ground temperatures, the following section describes the two new construction objects.
-
-### Construction:CfactorUndergroundWall
-
-This input object differs from the usual wall construction object in that it describes an entire construction rather than individual layers. This object is used when only the wall height (depth to the ground) and the C-factor are available.  This object accesses a model that creates an equivalent layer-by-layer construction for the underground wall to approximate the heat transfer through the wall considering the thermal mass of the earth soil.
-
-This object is referenced by underground wall surfaces with their fields ‘Outside Boundary Condition’ set to GroundFCfactorMethod.
-
-#### Field: Name
-
-The name of the underground wall construction.
-
-#### Field: C-Factor
-
-C-Factor is the time rate of steady-state heat flow through unit area of the construction, induced by a unit temperature difference between the body surfaces. The C-Factor unit is W/m<sup>2</sup>·K. The C-factor does not include soil or air films. ASHRAE Standard 90.1 and California Title 24 specify maximum C-factors for underground walls depending on space types and climate zones.
-
-#### Field: Height
-
-This field describes the height of the underground wall, i.e. the depth to the ground surface. The unit is meters.
-
-IDF Example:
-
-```idf
-Construction:CfactorUndergroundWall,
-    CfactorUGWall,
-    0.436,           ! C-factor (W/m2K), does not include soil or air films
-    4.57;            ! Height (m)
-
-
-  BuildingSurface:Detailed,
-    Zn001:Wall001,           !- Name
-    Wall,                    !- Surface Type
-    CfactorUGWall,           !- Construction Name
-    ZONE ONE,                !- Zone Name
-    GroundFCfactorMethod,    !- Outside Boundary Condition
-    ,                        !- Outside Boundary Condition Object
-    NoSun,                   !- Sun Exposure
-    NoWind,                  !- Wind Exposure
-    0.0,                     !- View Factor to Ground
-    4,                       !- Number of Vertices
-    0.0,0.0,4.572,           !- X,Y,Z ==&gt; Vertex 1
-    0.0,0.0,0.0,             !- X,Y,Z ==&gt; Vertex 2
-    15.24,0.0,0.0,           !- X,Y,Z ==&gt; Vertex 3
-    15.24,0.0,4.572;         !- X,Y,Z ==&gt; Vertex 4
-```
-
-
-### Construction:FfactorGroundFloor
-
-This input object differs from the usual ground floor construction object in that it describes an entire construction rather than individual layers. This object is used when only the floor area, exposed perimeter, and the F-factor are available.  This object accesses a model that creates an equivalent layer-by-layer construction for the slab-on-grade or underground floor to approximate the heat transfer through the floor considering the thermal mass of the earth soil.
-
-This object is referenced by slab-on-grade or underground floor surfaces with their fields ‘Outside Boundary Condition’ set to GroundFCfactorMethod.
-
-#### Field: Name
-
-The name of the ground floor construction.
-
-#### Field: F-Factor
-
-F-Factor represents the heat transfer through the floor, induced by a unit temperature difference between the outside and inside air temperature, on the per linear length of the exposed perimeter of the floor. The unit for this input is W/m·K. ASHRAE Standard 90.1 and California Title 24 specify maximum F-factors for slab-on-grade or underground floors depending on space types and climate zones.
-
-#### Field: Area
-
-This field describes the area (in square meters) of the slab-on-grade or underground floor.
-
-#### Field: PerimeterExposed
-
-This field describes the exposed (direct contact with ambient air) perimeter (in meters) of the slab-on-grade or underground floor.
-
-IDF Example:
-
-```idf
-Construction:FfactorGroundFloor,
-    slabconst,
-    0.12,     !F-factor in W/m-K
-    232.26,   !Area in m2
-    61.0;     !Exposed perimeter in m
-
-
-  BuildingSurface:Detailed,
-    Zn001:Flr001,            !- Name
-    Floor,                   !- Surface Type
-    slabconst,               !- Construction Name, FLOOR
-    ZONE ONE,                !- Zone Name
-    GroundFCfactorMethod,    !- Outside Boundary Condition, Surface
-    ,                        !- Outside Boundary Condition Object, Zn001:Flr001
-    NoSun,                   !- Sun Exposure
-    NoWind,                  !- Wind Exposure
-    0,                       !- View Factor to Ground
-    4,                       !- Number of Vertices
-    15.24,0.0,0.0,           !- X,Y,Z ==&gt; Vertex 1
-    0.0,0.0,0.0,             !- X,Y,Z ==&gt; Vertex 2
-    0.0,15.240,0.0,          !- X,Y,Z ==&gt; Vertex 3
-    15.24,15.24,0.0;         !- X,Y,Z ==&gt; Vertex 4
-```
-
-
-### Construction:InternalSource
-
-In some cases such as radiant systems, a construction will actually have resistance wires or hydronic tubing embedded within the construction. Heat is then either added or removed from this building element to provide heating or cooling to the zone in question. In the case of building-integrated photovoltaics, the energy removed in the form of electricity will form a sink. It is possible to enter such constructions into EnergyPlus with the syntax described below. The definition is similar to the Construction definition with a few additions related to radiant or other systems that will lead to source/sink terms. The internal source capability is available with both the **ConductionTransferFunction** and **ConductionFiniteDifference** solution algorithms.  The only difference is that the two dimensional pipe arrangements are not available to ConductionFiniteDifference. Those fields are ignored in that implementation.
-
-#### Field: Name
-
-This field is a user specified name that will be used as a reference by other input syntax. For example, a heat transfer surface (ref: Building Surfaces) requires a construction name to define what the make-up of the wall is.
-
-#### Field: Source Present After Layer Number
-
-This field is an integer that relates the location of the heat source or sink. The integer refers to the list of material layers that follow later in the syntax and determines the layer after which the source is present. If a source is embedded within a single homogenous layer (such as concrete), that layer should be split into two layers and the source added between them. For example, a value of “2� in this field tells EnergyPlus that the source is located between the second and third material layers listed later in the construction description (see layer fields below).
-
-#### Field: Temperature Calculation Requested After Layer Number
-
-The nature of this field is similar to the source interface parameter (see previous field) in that it is an integer, refers to the list of material layers that follow, and defines a location after the layer number identified by the user-defined number. In this case, the user is specifying the location for a separate temperature calculation rather than the location of the heat source/sink. This feature is intended to allow users to calculate a temperature within the construction. This might be important in a radiant cooling system where condensation could be a problem. This temperature calculation can assist users in making that determination in absence of a full heat and mass balance calculation.
-
-#### Field: Dimensions for the CTF Calculation
-
-This field is also an integer and refers to the detail level of the calculation. A value of “1� states that the user is only interested in a one-dimensional calculation. This is appropriate for electric resistance heating and for hydronic heating (when boiler/hot water heater performance is not affected by return and supply water temperatures). A value of “2� will trigger a two-dimensional solution for this surface only. This may be necessary for hydronic radiant cooling situations since chiller performance is affected by the water temperatures provided.
-
-A few things should be noted about requesting two-dimensional solutions. First, the calculation of the conduction transfer functions (CTF) is fairly intensive and will require a significant amount of computing time. Second, the solution regime is two-dimensional internally but it has a one-dimensional boundary condition imposed at the inside and outside surface (i.e., surface temperatures are still isothermal is if the surface was one-dimensional).
-
-#### Field: Tube Spacing
-
-This field defines how far apart in meters the hydronic tubing or electrical resistance wires are spaced in the direction perpendicular to the main direction of heat transfer. Note that this parameter is only used for two-dimensional solutions (see previous field).
-
-#### Field: Outside Layer
-
-Each construction must have at least one layer. This field defines the material name associated with the layer on the outside of this construction—outside referring to the side that is not exposed to the zone but rather the opposite side environment, whether this is the outdoor environment or another zone. Material layers are defined based on their thermal properties elsewhere in the input file (ref: Material and Material Properties and Zone,Average,HAMT Surface Average Water Content Ratio [kg/kg]
-
-Zone,Average,HAMT Surface Inside Face Temperature [C]
-
-Zone,Average,HAMT Surface Inside Face Relative Humidity [%]
-
-Zone,Average,HAMT Surface Inside Face Vapor Pressure [Pa]
-
-Zone,Average,HAMT Surface Outside Face Temperature [C]
-
-Zone,Average,HAMT Surface Outside Face Relative Humidity [%]
-
-Zone,Average,HAMT Surface Inside Face Relative Humidity [%]
-
-#### HAMT Surface Average Water Content Ratio [kg/kg]
-
-This output is the summed water content [kg/kg] of all cells in a surface expressed as a fraction of the mass of the water to the material mass.
-
-#### HAMT Surface Inside Face Temperature [C]
-
-This output is the temperature [C] on the internal “surface� of the surface.
-
-#### HAMT Surface Inside Face Relative Humidity [%]
-
-#### HAMT Surface Inside Face Relative Humidity [%]
-
-This output is the relative humidity on the internal “surface� of the surface expressed as a percentage.
-
-#### HAMT Surface Inside Face Vapor Pressure [Pa]
-
-This output is the vapor pressure [Pa] on the internal “surface� of the surface.
-
-#### HAMT Surface Outside Face Temperature [C]
-
-This output is the temperature on the external “surface� of the surface.
-
-#### HAMT Surface Outside Face Relative Humidity [%]
-
-This output is the relative humidity on the external “surface� of the surface.
-
-Zone,Average,HAMT Surface Temperature Cell N [C]
-
-Zone,Average,HAMT Surface Water Content Cell N [kg/kg]
-
-Zone,Average,HAMT Surface Relative Humidity Cell N [%]
-
-Detailed profile data for the variables Temperature [C], Relative Humidity [%] and Water Content [kg/kg] within each surface can also be reported. To calculate the heat and moisture transfer through surfaces HAMT splits up surfaces into discrete cells. Each cell is composed of a single material and has a position within the surface. HAMT automatically assigns cells to construction objects so that there are more cells closer to boundaries between materials and also at the “surfaces� of the surface. It is not possible for users to define their own cells.
-
-#### HAMT Surface Relative Humidity Cell &lt;N&gt; [%]
-
-This is the relative humidity of the cell in the surface.
-
-#### HAMT Surface Temperature Cell &lt;N&gt; [C]
-
-This is the temperature of the cell in the surface.
-
-#### HAMT Surface Water Content Cell &lt;N&gt; [kg/kg]
-
-This is the relative water content of the cell in the surface.
-
-Each surface is made from a particular construction. The construction-surface relationship is output by HAMT to the eplusout.eio file with the following format.
-
-! &lt;HAMT cells&gt;, Surface Name, Construction Name, Cell Numbers
-
-! &lt;HAMT origins&gt;, Surface Name, Construction Name, Cell origins (m)
-
-The output also contains the HAMT cell origins and cell number for each construction – surface combination. The coordinate system origin is defined as the exterior surface of the construction. Users can select any one of the Temperature, Relative Humidity or Water Content variables for any cell to be reported, using the following naming scheme for the output variable.
-
-HAMT Profile Construction &lt;Variable&gt; Cell &lt;Cell\#&gt;
-
-It is better to specify the “key� or Surface Name in this output.
-
-So for example to output the temperature of the 10<sup>th</sup> cell in a surface, eg “East Wall� would require the following output variable.
-
-```idf
-Output:Variable,
-    East Wall,               !- Key Value
-    HAMT Profile Construction Temperature Cell 10,  !- Variable Name
-    Hourly;                  !- Reporting Frequency
-```
-
-
-By selecting a whole range of these reports and using the information in the eplusout.eio file it is possible to build up a temperature profile of the surface.
-
-Materials for Glass Windows and Doors). As noted above, the outside layer should NOT be a film coefficient since EnergyPlus will calculate convection and radiation heat transfer more precisely.
-
-#### Field(s) 2-10: Layers
-
-The next fields are optional and the number of them showing up in a particular Construction definition depends solely on the number of material layers present in that particular construction. The data expected is identical to the outside layer field (see previous field description). The order of the remaining layers is important and should be listed in order of occurrence from the one just inside the outside layer until the inside layer is reached. As noted above, the inside layer should NOT be a film coefficient since EnergyPlus will calculate convection and radiation heat transfer more precisely.
-
-### Composite Wall Constructions
-
-Standard constructions in EnergyPlus are built with the materials and layers described earlier. However, some configurations will not be adequately represented by using this approach. The Reference Data Set CompositeWallConstructions.idf contains constructions and associated materials for a set of **composite** walls. These are walls—such as stud walls—that have complicated heat-flow paths so that the conduction is two- or three-dimensional. Thermal bridges are one of the common terms for these complicated heat-flow paths; this dataset will help you represent these in EnergyPlus.
-
-The materials here are **not** real materials but are “equivalent� materials obtained from finite-difference modeling. (The thickness, conductivity, density and specific heat values of the material layers for the different constructions have been taken from the ASHRAE report “Modeling Two- and Three-Dimensional Heat Transfer through Composite Wall and Roof Assemblies in Hourly Energy Simulation Programs (1145-TRP),� by Enermodal Engineering Limited, Oak Ridge National Laboratory, and the Polish Academy of Sciences, January 2001.). EnergyPlus will calculate conduction transfer functions using these materials. The heat transfer based on these conduction transfer functions will then be very close to what would be calculated with a two- or three-dimensional heat transfer calculation.
-
-For stud walls, using these composite constructions will give more accurate heat flow than you would get by manually dividing the wall into a stud section and a non-stud section.
-
-If your wall’s exterior or interior roughness or thermal, solar or visible absorptances are different from those in the data set, you can make the appropriate changes to the first material (the outside layer) or the third material (the inside layer). **None of the other values should be changed.**
-
-Complete description of the CompositeWallConstructions data set are found in the OutputDetailsAndExamples document.
-
-### Construction:ComplexFenestrationState
-
-This input object is used to describe the properties of a single state for complex fenestration.  There are two parts to the input, 1) layer-by-layer physical description of fenestration system and 2) a set of matrices that describe overall system optical performance.  Each layer also has associated with it two matrices that give the layer absorptance (for front and back incidence on the system.
-
-The optical properties are given as a two-dimensional matrix describing the basis and four two-dimensional matrices of system bidirectional optical properties.
-
-These input objects will generally be exported directly from the WINDOW program and it is expected that users usually will not develop the input themselves. However, this is an option for users who prefer to use a different method (e.g., Monte-Carlo ray-trace or measurement) of determining optical properties.
-
-Multiple instances of this object are used to define the separate operating states of complex fenestration.  For example, blinds could be deployed or redirected to create a new state, or electrochromic glazings could change transmittance.  Each separate state defines the materials present and the overall optical performance.  If the glazing system has only one state, then only one of these objects is needed.
-
-If there is more than one complex fenestration state, it will be controlled using the EMS actuator called “Surface� with the control type “Construction State� and the EMS input object called EnergyManagementSystem:ConstructionIndexVariable.
-
-#### Field: Name
-
-Unique name of this construction.  Used to identify type of window in surface objects.
-
-#### Field: Basis Type keyword
-
-Only value currently implemented is “LBNLWINDOW�. More options may be added in the future.
-
-#### Field: Basis Symmetry, keyword
-
-Only value currently implemented is “None�. More options will be added in the future.
-
-#### Field: Thermal Parameters
-
-This field gives the name of WindowThermalModel:Params object used to keep common data necessary for thermal simulation.
-
-#### Field: Basis Matrix Name
-
-This field gives the name of an 2 x N matrix object that defines the basis  For a fenestration basis, N would be the number of theta (polar angle) values, the first of the two elements for each of the i=1,..,N would be the theta value, and the second would be the number of phi (azimuthal angle) values that 360º is divided into for that theta.
-
-#### Field: Solar Optical Complex Front Transmittance Matrix Name
-
-This field contains the name of matrix object that describes the solar transmittance at different incident angles.  This is from the outside toward the inside.
-
-#### Field: Solar Optical Complex Back Reflectance Matrix Name
-
-This field contains the name of matrix object that describes the solar back reflectance at different incident angles.  This is from the inside toward the outside.
-
-#### Field: Visible Optical Complex Front Transmittance Matrix Name
-
-This field contains the name of matrix object that describes the visible transmittance at different incident angles.  This is from the outside toward the inside.
-
-#### Field: Visible Optical Complex Back Reflectance Matrix Name
-
-This field contains the name of vector object that describes the visible back reflectance at different incident angles.  This is from the inside toward the outside.
-
-#### Field: Outside Layer &lt;x=1&gt;
-
-Each construction must have at least one layer. The layer order is from outside to inside, with the first layer being either WindowMaterial:Glazing or WindowMaterial:ComplexShade. The next layer is a WindowMaterial:Gap layer, and the following layers then alternate between WindowMaterial:Glazing or WindowMaterial:ComplexShade and WindowMaterial:Gap. The last layer cannot be WindowMaterial:Gap.
-
-#### Field: Outside Layer Directional Front Absorptance Matrix Name
-
-Points to an Nbasis x 1 matrix object.
-
-#### Field: Outside Layer Directional Back Absorptance Matrix Name
-
-Points to an Nbasis x 1 matrix object.
-
-#### Above 3 fields are optionally repeated for layers 2-10
-
-These layers include gaps, which do not need to have matrix data specified.
-
-
-
-An IDF example of complex fenestration with single layer:
-
-```idf
-Construction:ComplexFenestrationState,       !- single layer example
-  CFS_Glz_1,                 !- name
-  LBNLWindow,                !- basis type
-  None,                      !- basis symmetry type
-  ThermParam_1,              !- window thermal model
-  CFS_Glz_1_Basis,           !- basis matrix name
-  CFS_Glz_1_TfSol,           !- Tfsol
-  CFS_Glz_1_RbSol,           !- Rbsol
-  CFS_Glz_1_Tfvis,           !- Tfvis
-  CFS_Glz_1_Tbvis,           !- Tbvis
-  Glass_102_Layer,           !- layer 1 name
-  CFS_Glz_1_Layer_1_fAbs,    !- fAbs
-  CFS_Glz_1_Layer_1_bAbs;    !- bAbs
-```
-
-
-
-
-An complex fenestration IDF example with double layer (first layer is shading device):
-
-```idf
-Construction:ComplexFenestrationState,       !- double layer example
-  CFS_Glz_59,                    !- name
-  LBNLWindow,                    !- basis type
-  None,                          !- basis symmetry type
-  ThermParam_59,                 !- window thermal model
-  CFS_Glz_59_Basis,              !- basis matrix name
-  CFS_Glz_59_TfSol,              !- Tfsol
-  CFS_Glz_59_RbSol,              !- Rbsol
-  CFS_Glz_59_Tfvis,              !- Tfvis
-  CFS_Glz_59_Tbvis,              !- Tbvis
-  Shade_30001_Layer,             !- layer 1 name (shading device)
-  CFS_Glz_59_Layer_1_fAbs,       !- fAbs
-  CFS_Glz_59_Layer_1_bAbs,       !- bAbs
-  Gap_1_Layer,                   !- layer 1 name
-  ,                 !- absorptance matrices for gaps should be empty for now
-  ,                              !- it is for future use
-  Glass_3110_Layer,              !- layer 2 name
-  CFS_Glz_59_Layer_3110_fAbs,    !- fAbs
-  CFS_Glz_59_Layer_3110_bAbs;    !- bAbs
-```
-
-
-### WindowThermalModel:Params
-
-This input object is used with the Construction:ComplexFenestrationState
-
-#### Field: Name
-
-Unique name of the window thermal model parameters.
-
-#### Field: Calculation Standard
-
-The type of the calculation standard.  The choices are:
-
-- ISO15099
-
-- EN673Declared
-
-- EN673Design
-
-The default is ISO15099.
-
-#### Field: Thermal Model
-
-The type of thermal model.  The choices are:
-
-- ISO15099
-
-- ScaledCavityWidth
-
-- ConvectiveScalarModel\_NoSDThickness
-
-- ConvectiveScalarModel\_withSDThickness
-
-The default is ISO15099.
-
-#### Field: SD Scalar
-
-Shading Device Scalar Factor. Only used for  Thermal Model = Convective Scalar Model.  Factor of venetian shading device layer contribution to convection. Real value between 0 (where the shading device contribution to convection is neglected) and 1 (where the shading device treated as “closed� – as if it is a glass layer with thermal properties of SD slat material). Default: 1.0
-
-#### Field: Deflection Model
-
-The type of deflection model used to model deflection in windows and glass.  The choices are:
-
-- NoDeflection
-
-- TemperatureAndPressureInput
-
-- MeasuredDeflection
-
-The default is NoDeflection.
-
-#### Field: Vacuum Pressure Limit
-
-The pressure (Pa) which will be considered to be the limit for vacuum glazing pressure.  All pressures less than or equal to this pressure will be considered to be vacuum. Default: 13.238 Pa.
-
-#### Field: Initial Temperature
-
-The temperature (<sup>o</sup>C) of the gap in the time of fabrication.  It is used only when WindowThermalModel:Params DeflectionModel =TemperatureAndPressureInput
-
-#### Field: Initial Pressure
-
-The pressure (Pa) of the gap at the time of fabrication of the sealed glazing system unitIt is used only when WindowThermalModel:Params DeflectionModel =TemperatureAndPressureInput.
-
-
-
-An IDF example for WindowThermalModel:Params (without deflection):
-
-```idf
-WindowThermalModel:Params,
-  ThermParam_59,                   !- name
-  ISO15099,                        !- standard
-  ISO15099,                        !- thermal model standard
-  1.00,                            !- SD scalar
-  NoDeflection;                    !- deflection model
-```
-
-
-
-
-An IDF example for thermal paramters (with deflection):
-
-```idf
-WindowThermalModel:Params,
-  ThermParam_59,                   !- name
-  ISO15099,                        !- standard
-  ISO15099,                        !- thermal model standard
-  1.00,                            !- SD scalar
-  TemperatureAndPressureInput,     !- deflection model
-  ,                                !- vacuum pressure limit
-  21.00,                           !- temperature at time of fabrication
-  10000.00;                        !- pressure at time of fabrication
-```
-
-
-
-
-An IDF example for WindowThermalModel:Params for modeling vacuum glazing
-
-```idf
-WindowThermalModel:Params,
-ThermParam_1006,                                    !- name
-ISO15099,                                           !- standard
-ISO15099,                                           !- thermal model
-1.0000,                                             !- SDScalar
-NoDeflection,                                       !- deflection model
-13.238;                                             !- vacuum pressure limit
-```
-
-
-### Matix:TwoDimension
-
-This is input object is only used with Construction:ComplexFenestrationState object to enter a two-dimensional matrix of values.
-
-It is used to define the Basis Matrix for BSDF input data, and is also used to define the actual BSDF matrices data for the complete fenestration definition as well as the individual layers of the system.
-
-The data are entered in row-major order: all the elements of row 1, followed by all the elements of row 2, etc.  The number of values to be entered depends on the number of rows and the number of columns.  Blank fields are treated as having been set to zero.
-
-See example IDF file “SmOff\_ CmplxGlz\_IntExtShading.idf� for the definition of two complex shading layers with matrix data defined.
-
-#### Field: Name
-
-Unique name of matrix input object.
-
-#### Field: Number of Rows
-
-This field is the number of rows in the matrix.
-
-#### Field: Number of Columns
-
-This field is the number of columns in the matrix
-
-#### &lt; Field Set: Value \# N &gt;
-
-Repeat entering value exactly the same number of times as the number of rows times the number of columns.
-
-#### Field: Value \# 1
-
-This is the value of the matrix at the first row and first column.
-
-#### Field: Value \#2
-
-This is the value of the matrix at the first row and the second column.
-
-An IDF example of matrix for defining BSDF basis:
-
-```idf
-Matrix:TwoDimension,       !- matrix for basis definition
-  CFS_Glz_1_Basis,         !- basis matrix name
-  9,                       !- number of rows
-  2,                       !- number of colums
-  0.00000, 1.00000,
-  10.00000, 8.00000,
-  20.00000, 16.00000,
-  30.00000, 20.00000,
-  40.00000, 24.00000,
-  50.00000, 24.00000,
-  60.00000, 24.00000,
-  70.00000, 16.00000,
-  82.50000, 12.00000;
-```
-
-
-### Construction:WindowEquivalentLayer
-
-This object defines the construction for equivalent layer window (ASHWAT) model. This window can model various mix of glazing and shading layers combination. Shadings are defined as an integral part of the construction. The construction is defined by listing the layers name starting with outside layer and work your way to the inside Layer. Up to six solid layers (glazing and shade) and up to five gaps, i.e., a total of up to 11 layers maximum are allowed in equivalent layer window object. The solid layer types allowed are: Glazing, Insect Screen, Roller Blinds, Venetian Blind, and Drape Fabrics. This window model requires optical data of the individual glazing and shading layers to calculate the effective optical properties of the composite fenestration construction. Venetian blinds in equivalent layer window model can be in a fixed slat angle or has the option to control the slat angle in order to maximize visibility, or maximize solar gains. An equivalent-layer concept can simulate wide range of multiple glazing and shading layers combination and provides unlimited flexibility to combine different types of shading layers in a fenestration. For the gap layer object any one of the five different Gas types can be specified: AIR, ARGON, XENON, KRYPTON, or CUSTOM.This window object is referenced by fenestration surfaces. For details of the model description refer to Equivalent Layer Fenestration Model section in Engineering Reference. The various layer objects that can be referenced in Equivalent Layer window model are:
-
-WindowMaterial:Glass:EquivalentLayer
-
-WindowMaterial:Shade:EquivalentLayer
-
-WindowMaterial:Drape:EquivalentLayer
-
-WindowMaterial:Blind:EquivalentLayer
-
-WindowMaterial:Screen:EquivalentLayer
-
-WindowMaterial:Gap:EquivalentLayer
-
-#### Field: Name
-
-This field is a user specified name that will be used as a reference by other input syntax. For example, a heat transfer surface (ref: Fenestration) requires a construction name to define what the make-up of the fenestration is. This name must be identical to one of the Window Construction Equivalent Layer definitions in the input data file.
-
-#### Field: Outside Layer
-
-Each equivalent layer window construction must have at least one layer. This field defines the material name associated with the layer on the outside of the construction—outside referring to the side that is exposed to the outdoor environment or another zone. Material layers for equivalent layer window model are defined based on their thermal properties elsewhere in the input file (ref: WindowEquivalentLayerMaterialNames)
-
-#### Field: Layer 2 - Layer11
-
-The next fields are optional and the number of them showing up in a particular equivalent layer window construction definition depends solely on the number of material layers present in that construction. The data expected is identical to the outside layer field (see previous field description). The order of the remaining layers is important and should be listed in order of occurrence from the one just inside the outside layer until the inside layer is reached. As noted above, the inside layer should NOT be a film coefficient since EnergyPlus will calculate inside convection and radiation heat transfer more precisely.
-
-An IDF example for this object, is shown below:
-
-```idf
-Construction:WindowEquivalentLayer,
-  Six Solid Layers Window,   !- Name
-  INSCRN,                    !- Outside Layer
-  Air GAP Outdoor 12.7mm,    !- Layer 2
-  GLZGRY,                    !- Layer 3
-  Argon GAP Sealed 12.7mm,   !- Layer 4
-  FEP,                       !- Layer 5
-  Xenon GAP Sealed 12.7mm,   !- Layer 6
-  LOF1436,                   !- Layer 7
-  Krypton GAP Sealed 12.7mm, !- Layer 8
-  GLZCLR,                    !- Layer 9
-  Air GAP Indoor 12.7mm,     !- Layer 10
-  ShadeTrns;                 !- Layer 11
-```
-
-
-### Construction:WindowDataFile
-
-The WINDOW program, which does a thermal and optical analysis of a window under different design conditions, writes a data file (“Window data file�) containing a description of the window that was analyzed. The Construction:WindowDataFile object allows a window to be read in from the WINDOW data file—see “Importing Windows from WINDOW.� For information on adding a shading device to the window see “WindowProperty:ShadingControl.�
-
-#### Field: Name
-
-This is the name of a window on the Window data file. An error will result if EnergyPlus cannot find a window of this name on the file, or if the file, shown in the next field, is not present. The location of the data file should be specified in the File Name field. For details on what is done with the data if a matching window is found on the file see “Importing Windows from WINDOW.�
-
-#### Field: File Name
-
-This is the file name of the Window data file that contains the Window referenced in the previous field. The field may include a full path with file name, for precise results. The field must be &lt;= 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
-
-If this field is left blank, the file name is defaulted to Window5DataFile.dat.
-
-Input Example
-
-```idf
-Construction:WindowDataFile,
-  DoubleClear;          !- Name of a Window on the Window Data File
-```
-
-**  ! Note – Window5DataFile.dat is presumed to be in the “run� folder where EnergyPlus.exe is**
-
-```idf
-FenestrationSurface:Detailed,
-  Zn001:Wall001:Win001, !- Name
-  Window,               !- Class
-  DoubleClear,          !- Construction Name
-  Zn001:Wall001,,       !- Base Surface Name, and Target (if applicable)
-  0.5,                  !- View Factor to Ground
-  ,                     !- Window Shading Control name
-  ,                     !- Frame/Divider name
-  1.0,                  !- Multiplier
-  4,                    !- Number of vertices
-  0.548, 0.0, 2.5000,   !- X,Y,Z of Vertices
-  0.548, 0.0, 0.5000,
-  5.548, 0.0, 0.5000,
-  5.548, 0.0, 2.5000;
-```
-
-
-
-
-An example showing use of specific data file name and complete path location follows:
-
-```idf
-Construction:WindowDataFile,
-  DoubleClear,            !- Name of a Window on the Window Data File
-```
-**  C:\\EnergyPlusData\\DataSets\\MyWindow.dat;**
-
-### Construction Element Outputs
-
-An optional report (contained in **eplusout.eio**) gives calculational elements for the materials and constructions used in the input. These reports are explained fully in the Output Details and Examples document.
-
-Group – Thermal Zone Description/Geometry
------------------------------------------
-
-Without thermal zones and surfaces, the building can’t be simulated. This group of objects (Zone, BuildingSurface) describes the thermal zone characteristics as well as the details of each surface to be modeled. Included here are shading surfaces.
-
-### Zone
-
-This element sets up the parameters to simulate each thermal zone of the building.
-
-#### Field: Direction of Relative North
-
-The Zone North Axis is specified **relative to the Building North Axis**. This value is specified in degrees (clockwise is positive). For more information, see the figure below as well as the description under “GlobalGeometryRules�.
-
-#### Field(s): (X,Y,Z) Origin
-
-The X,Y,Z coordinates of a zone origin can be specified, for convenience in vertice entry. Depending on the values in “GlobalGeometryRules� (see description later in this section), these will be used to completely specify the building coordinates in “world coordinate� or not. Zone Origin coordinates are specified **relative to the Building Origin (which always 0,0,0)**. The following figure illustrates the use of Zone North Axis as well as Zone Origin values.
-
-![](media/image053.svg)
-
-Figure 27. Illustration of Zone North Axis and Origins
-
-#### Field: Type
-
-Zone type is currently unused.
-
-#### Field: Multiplier
-
-Zone Multiplier is designed as a “multiplier� for floor area, zone loads, and energy consumed by internal gains. It takes the calculated load for the zone and multiplies it, sending the multiplied load to the attached HVAC system. The HVAC system size is specified to meet the entire multiplied zone load and will report the amount of the load met in the Zone Air System Sensible Heating or Cooling Energy/Rate output variable. Autosizing automatically accounts for multipliers. Metered energy consumption by internal gains objects such as Lights or Electric Equipment will be mutliplied.  The default is 1.
-
-#### Field: Ceiling Height
-
-Zone ceiling height is used in several areas within EnergyPlus (such as various room models, some convection coefficient calculations and, primarily, in calculating zone volume in the absence of other parameters). Energyplus automatically calculates the zone ceiling height (m) from the average height of the zone. If this field is 0.0, negative or **autocalculate**, then the calculated zone ceiling height will be used in subsequent calculations. If this field is positive, then the calculated zone ceiling height will not be used -- the number entered here will be used as the zone ceiling height. If this number differs significantly from the calculated ceiling height, then a warning message will be issued. If a zone ceiling height is entered, but no Volume is entered, then the floor area (if there is one) times the zone ceiling height will be used as the volume.
-
-Note that the Zone Ceiling Height is the distance from the Floor to the Ceiling in the Zone, not an absolute height from the ground.
-
-#### Field: Volume
-
-Zone volume is used in several areas within EnergyPlus (such as calculating air change rates for reporting or flow when air change rates are chosen as input, daylighting calculations, some convection coefficient calculations). EnergyPlus automatically calculates the zone volume (m<sup>3</sup>) from the zone geometry given by the surfaces that belong to the zone. If this field is 0.0, negative or **autocalculate**, then the calculated zone volume will be used in subsequent calculations. If this field is positive, then it will be used as the zone volume. If this number differs significantly from the calculated zone volume a warning message will be issued. For autocalculate to work properly, the zone must be enclosed by the entered walls. Note that indicating the volume to be calculated but entering a positive ceiling height in the previous field will cause the volume to be calculated as the floor area (if &gt; 0) times the entered ceiling height; else the volume will be calculated from the described surfaces. If this field is positive, any ceiling height positive value will not be used in volume calculations.
-
-#### Field: Floor Area
-
-Zone floor area is used in many places within EnergyPlus. EnergyPlus automatically calculates the zone floor area (m<sup>2</sup>) from the zone geometry given by the surfaces that belong to the zone. If this field is 0.0, negative or **autocalculate**, then the calculated zone floor area will be used in subsequent calculations. If this field is positive, then it will be used as the zone floor area. If this number differs significantly from the calculated zone floor area a warning message will be issued.
-
-#### Field: Zone Inside Convection Algorithm
-
-The Zone Inside Convection Algorithm field is optional. This field specifies the convection model to be used for the inside face of heat transfer surfaes associated with this zone. The choices are: **Simple** (constant natural convection - ASHRAE), **Detailed** (variable natural convection based on temperature difference - ASHRAE), **CeilingDiffuser** (ACH based forced and mixed convection correlations for ceiling diffuser configuration with simple natural convection limit), **AdaptiveConvectionAlgorithm** (complex arrangement of various models that adapt to various zone conditions and can be customized) and **TrombeWall** (variable natural convection in an enclosed rectangular cavity). See the Inside Convection Algorithm object for further descriptions of the available models.
-
-If omitted or blank, the algorithm specified in the SurfaceConvectionAlgorithm:Inside object is the default.
-
-#### Field: Zone Outside Convection Algorithm
-
-The Zone Outside Convection Algorithm field is optional. This field specifies the convection model to be used for the outside face of heat transfer surfaces associated with this zone. The choices are: **SimpleCombined**, **TARP**, **DOE-2**, **MoWiTT, and AdaptiveConvectionAlgorithm**. The simple convection model applies heat transfer coefficients depending on the roughness and windspeed. This is a combined heat transfer coefficient that includes radiation to sky, ground, and air. The correlation is based on Figure 1, Page 25.1 (Thermal and Water Vapor Transmission Data), 2001 ASHRAE Handbook of Fundamentals.
-
-The other convection models apply heat transfer coefficients depending on the roughness, windspeed, and terrain of the building’s location. These are *convection only* heat transfer coefficients; radiation heat transfer coefficients are calculated automatically by the program. The TARP algorithm was developed for the TARP software and combines natural and wind-driven convection correlations from laboratory measurements on flat plates.  The DOE-2 and MoWiTT were derived from field measurements.  The AdaptiveConvectionAlgorithm model is an dynamic algorithm that organizes a large number of different convection models and automatically selects the one that best applies.  The adaptive convection algorithm can also be customized using the SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections input object. All algorithms are described more fully in the Engineering Reference.
-
-If omitted or blank, the algorithm specified in the SurfaceConvectionAlgorithm:Outside object is the default.
-
-#### Field: Part of Total Floor Area
-
-This optional field defaults to Yes if not specified. The field is used to show when a zone is not part of the Total Floor Area as shown in the Annual Building Utility Performance Summary tables. Specifically, when No is specified, the area is excluded from both the conditioned floor area and the total floor area in the Building Area sub table and the Normalized Metrics sub tables.
-
-
-
-And, an IDF example:
-
-```idf
-  Zone,
-    DORM ROOMS AND COMMON AREAS,  !- Name
-    0.0000000E+00,           !- Direction of Relative North {deg}
-    0.0000000E+00,           !- X Origin {m}
-    6.096000,                !- Y Origin {m}
-    0.0000000E+00,           !- Z Origin {m}
-    1,                       !- Type
-    1,                       !- Multiplier
-    autocalculate,           !-Ceiling Height {m}
-    autocalculate;           !- Volume {m3}
-```
-
-
-### Zone Outputs
-
-* Zone,Average,Zone Outdoor Air Drybulb Temperature [C]
-
-* Zone,Average,Zone Outdoor Air Wetbulb Temperature [C]
-
-* Zone,Average,Zone Outdoor Air Wind Speed [m/s]
-
-
-#### Zone Outdoor Air Drybulb Temperature [C]
-
-The outdoor air dry-bulb temperature calculated at the height above ground of the zone centroid.
-
-#### Zone Outdoor Air Wetbulb Temperature [C]
-
-The outdoor air wet-bulb temperature calculated at the height above ground of the zone centroid.
-
-#### Zone Outdoor Air Wind Speed [m/s]
-
-The outdoor wind speed calculated at the height above ground of the zone centroid.
-
-### Zone Thermal Output(s)
-
-In addition to the canned Surface reports (view the Reports section later in this document) and surface variables (above), the following variables are available for all zones:
-
-* Zone,Sum,Zone Total Internal Radiant Heating Energy [J]
-
-* Zone,Average,Zone Total Internal Radiant Heating Rate [W]
-
-* Zone,Sum,Zone Total Internal Visible Radiation Heating Energy [J]
-
-* Zone,Average,Zone Total Internal Visible Radiation Heating Rate [W]
-
-* Zone,Sum,Zone Total Internal Convective Heating Energy [J]
-
-* Zone,Average,Zone Total Internal Convective Heating Rate [W]
-
-* Zone,Sum,Zone Total Internal Latent Gain Energy [J]
-
-* Zone,Average,Zone Total Internal Latent Gain Rate [W]
-
-* Zone,Sum,Zone Total Internal Total Heating Energy [J]
-
-* Zone,Average,Zone Total Internal Total Heating Rate [W]
-
-* Zone,Average,Zone Mean Air Temperature [C]
-
-* HVAC,Average,Zone Air Temperature [C]
-
-* Zone,Average,Zone Mean Air Dewpoint Temperature [C]
-
-* Zone,Average,Zone Mean Radiant Temperature [C]
-
-* Zone,Average,Zone Operative Temperature [C]
-
-* HVAC,Average,Zone Air Heat Balance Internal Convective Heat Gain Rate [W]
-
-* HVAC,Average,Zone Air Heat Balance Surface Convection Rate [W]
-
-* HVAC,Average,Zone Air Heat Balance Interzone Air Transfer Rate [W]
-
-* HVAC,Average,Zone Air Heat Balance Outdoor Air Transfer Rate [W]
-
-* HVAC,Average,Zone Air Heat Balance System Air Transfer Rate [W]
-
-* HVAC,Average,Zone Air Heat Balance System Convective Heat Gain Rate [W]
-
-* HVAC,Average,Zone Air Heat Balance Air Energy Storage Rate [W]
-
-* HVAC,Average,Zone Air Heat Balance Deviation Rate [W]
-
-* HVAC,Sum,Zone Air System Sensible Heating Energy [J]
-
-* HVAC,Sum,Zone Air System Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Air System Sensible Heating Rate [W]
-
-* HVAC,Average,Zone Air System Sensible Cooling Rate [W]
-
-* HVAC,Average,Zone Air Humidity Ratio[kgWater/kgDryAir]
-
-* HVAC,Average,Zone Air Relative Humidity[%]
-
-
-Two of these are of particular interest:
-
-Zone,Average,Zone Mean Air Temperature [C]
-
-HVAC,Average,Zone Air Temperature [C]
-
-These two variable outputs are/should be identical. However, note that they can be reported at different time intervals. “Zone Mean Air Temperature� is only available on the Zone/HB timestep (Number of Timesteps per Hour) whereas “Zone Air Temperature� can be reported at the HVAC timestep (which can vary).
-
-#### Zone Mean Air Temperature [C]
-
-From the code definition, the zone mean air temperature is the average temperature of the air temperatures at the system timestep. Remember that the zone heat balance represents a “well stirred� model for a zone, therefore there is only one mean air temperature to represent the air temperature for the zone.
-
-#### Zone Air Temperature [C]
-
-This is very similar to the mean air temperature in the last field. The “well stirred� model for the zone is the basis, but this temperature is also available at the “detailed� system timestep.
-
-#### Zone Mean Air Dewpoint Temperature [C]
-
-This is the dewpoint temperature of the zone calculated from the Zone Mean Air Temperature (above), the Zone Air Humidity Ratio (below) and the outdoor barometric pressure.
-
-#### Zone Thermostat Air Temperature [C]
-
-This is the zone air node temperature for the well-mixed room air model, which is the default room air model type (RoomAirModelType=Mixing).  But for other types of Room Air Model (the RoomAir:TemperaturePattern:\* and RoomAirSettings:\* objects) the zone thermostat air temperature may depend on the Thermostat Height and Thermostat Offset.
-
-#### Zone Mean Radiant Temperature [C]
-
-The Mean Radiant Temperature (MRT) in degrees Celsius of a space is a measure of the combined effects of temperatures of surfaces within that space. Specifically it is the surface area × emissivity weighted average of the zone inside surface temperatures (ref. Surface Inside Temperature), where emissivity is the Thermal Absorptance of the inside material layer of each surface.
-
-#### Zone Operative Temperature [C]
-
-Zone Operative Temperature (OT) is the average of the Zone Mean Air Temperature (MAT) and Zone Mean Radiant Temperature (MRT),  OT = 0.5\*MAT + 0.5\*MRT.  This output variable is not affected by the type of thermostat controls in the zone, and does not include the direct effect of high temperature radiant systems.  See also Zone Thermostat Operative Temperature.
-
-#### Zone Air Heat Balance Internal Convective Heat Gain Rate [W]
-
-The Zone Air Heat Balance Internal Convective Heat Gain Rate is the sum, in watts, of heat transferred to the zone air from all types of internal gains, including people, lights, equipment etc.  This and the following provide results on the load components of the zone air heat balance.  This field is not multiplied by zone or group multipliers.
-
-#### Zone Air Heat Balance Surface Convection Rate [W]
-
-The Zone Air Heat Balance Surface Convection Rate is the sum, in watts, of heat transferred to the zone air from all the surfaces.  This field is not multiplied by zone or group multipliers.
-
-#### Zone Air Heat Balance Interzone Air Transfer Rate [W]
-
-The Zone Air Heat Balance Interzone Air Transfer Rate is the sum, in watts, of heat transferred to the zone air from all the transfers of air from other thermal zones. This field is not multiplied by zone or group multipliers.
-
-#### Zone Air Heat Balance Outdoor Air Transfer Rate [W]
-
-The Zone Air Heat Balance Outdoor Air Transfer Rate is the sum, in watts, of heat transferred to the zone air from all the transfers of air from the out side, such as infiltration.  This field is not multiplied by zone or group multipliers.
-
-#### Zone Air Heat Balance System Air Transfer Rate [W]
-
-The Zone Air Heat Balance System Air Transfer Rate is the sum, in watts, of heat transferred to the zone air by HVAC forced-air systems and air terminal units.  Such HVAC systems are connected to the zone by an inlet node (see ZoneHVac:EquipmentConnections input field called Zone Air Inlet Node or Node List Name) This field is not multiplied by zone or group multipliers.
-
-#### Zone Air Heat Balance System Convective Heat Gain Rate [W]
-
-The Zone Air Heat Balance System Convective Heat Gain Rate is the sum, in watts, of heat transferred directly to the zone air by “non-air� HVAC systems.  Such HVAC systems are not connected to the zone by an inlet node but rather add or subtract heat directly to the zone air in a manner similar to internal gains.  These include the convective fraction of zone HVAC baseboards and high temperature radiant systems, zone HVAC refrigeration chiller set, and the extra convective cooling provided by the cooled beam air terminal unit.  This field is not multiplied by zone or group multipliers.
-
-#### Zone Air Heat Balance Air Energy Storage Rate [W]
-
-The Zone Air Heat Balance Air Energy Storage Rate is the heat stored, in watts, in the zone air as result of zone air temperature changing from one timestep to the next.  This field is not multiplied by zone or group multipliers.
-
-#### Zone Air Heat Balance Deviation Rate [W]
-
-The Zone Air Heat Balance Deviation Rate is the imbalance, in watts, in the energy balance for zone air.  The value should be near zero but will become non-zero if zone conditions are changing rapidly or erratically.  This field is not multiplied by zone or group multipliers.  (This output variable is only generated if the user has set a computer system environment variable DisplayAdvancedReportVariables equal to “yes�.)
-
-#### Zone Air System Sensible Heating Energy [J]
-
-This output variable represents the sensible heating energy in Joules that is actually supplied by the system to that zone for the timestep reported. This is the sensible heating rate multiplied by the simulation timestep. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module. . This field is not multiplied by zone or group multipliers.
-
-Zone Air System Sensible Heating (and Cooling) Energy (and Rate) all report the heating or cooling delivered by the HVAC system to a zone. These values are calculated by multiplying the supply air mass flow rate by the difference between the supply air temperature and the zone air temperature. This does not always indicate the operation of heating or cooling coils. For example, cooling will be reported if the supply air is cooled due to the introduction of outside air, even if all coils are off.
-
-Note that these variables are calculated at the system timestep. When reported at the "detailed" reporting frequency, these variable will never show heating and cooling both in the same system timestep. If reported at a frequency less than "Detailed" (for example, Hourly) values may appear in both the heating and cooling variable for the same hour if the system cooled the zone for part of the reporting period and heated the zone for another part of the reporting period.
-
-#### Zone Air System Sensible Cooling Energy [J]
-
-This output variable represents the sensible cooling energy in Joules that is actually supplied by the system to that zone for the timestep reported. This is the sensible cooling rate multiplied by the simulation timestep. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module.   This field is not multiplied by zone or group multipliers.
-
-#### Zone Air System Sensible Heating Rate [W]
-
-This output variable represents the sensible heating rate in Watts that is actually supplied by the system to that zone for the timestep reported. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module.   This field is not multiplied by zone or group multipliers.
-
-#### Zone Air System Sensible Cooling Rate [W]
-
-This output variable represents the sensible cooling rate in Watts that is actually supplied by the system to that zone for the timestep reported. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module.   This field is not multiplied by zone or group multipliers.
-
-#### Zone Air Humidity Ratio [kgWater/kgDryAir]
-
-This output variable represents the air humidity ratio after the correct step for each zone. The humidity ratio is the mass of water vapor to the mass of dry air contained in the zone in (kg water/kg air) and is unitless.
-
-#### Zone Air Relative Humidity [%]
-
-This output variable represents the air relative humidity after the correct step for each zone. The relative humidity is in percent and uses the Zone Air Temperature, the Zone Air Humidity Ratio and the Outside Barometric Pressure for calculation.
-
-#### Zone Total Internal Radiant Heating Rate [W]
-
-#### Zone Total Internal Radiant Heating Energy [J]
-
-These output variables represent the sum of radiant gains from specific internal sources  (e.g. equipment) throughout the zone in Watts (for rate) or joules. This includes radiant gain from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
-
-#### Zone Total Internal Visible Radiation Heating Rate [W]
-
-#### Zone Total Internal Visible Radiation Heating Energy [J]
-
-These output variables expresse the sum of heat gain in Watts (for rate) or joules that is the calculated short wavelength radiation gain from lights in the zones. This calculation uses the total energy from lights and the fraction visible to realize this value, summed over the zones in the simulation.
-
-#### Zone Total Internal Convective Heating Rate [W]
-
-#### Zone Total Internal Convective Heating Energy [J]
-
-These output variables represent the sum of convective gains from specific sources (e.g. equipment) throughout the zone in Watts (for rate) or joules. This includes convective gain from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
-
-#### Zone Total Internal Latent Gain Rate [W]
-
-#### Zone Total Internal Latent Gain Energy [J]
-
-These output variables represent the sum of latent gains from specific internal sources (e.g. equipment) throughout the zone in Watts (for rate) or joules. This includes latent gain from People, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
-
-#### Zone Total Internal Total Heating Rate [W]
-
-#### Zone Total Internal Total Heating Energy [J]
-
-These output variables represent the sum of all heat gains throughout the zone in Watts (for rate) or joules. This includes all heat gains from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
-
-### ZoneList
-
-The ZoneList object defines a list of Zone objects. It is primarily used with the ZoneGroup object to provide a generalized way for doing "Floor Multipliers". (See the ZoneGroup description below.) The associated ZoneList output variables also provide a way to aggregate and organize zone loads.
-
-Zone lists are not exclusive. A zone can be referenced be more than one ZoneList object.
-
-#### Field: Zone List Name
-
-The name of the ZoneList object. Must be unique across ZoneLists.
-
-#### Field: Zone 1 - Zone 20 Name
-
-Reference to a Zone object. This field is extensible; for greater than 20 zones, edit the IDD to add more *Zone Name* fields.
-
-```idf
-ZoneList,
-  Mid Floor List,  !- Name
-  Mid West Zone,   !- Zone 1 Name
-  Mid Center Zone, !- Zone 2 Name
-  Mid East Zone;   !- Zone 3 Name
-```
-
-
-### ZoneList Outputs
-
-The following output variables are reported by the ZoneList object:
-
-* HVAC,Average,Zone List Sensible Heating Rate [W]
-
-* HVAC,Average,Zone List Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone List Sensible Heating Energy [J]
-
-* HVAC,Sum,Zone List Sensible Cooling Energy [J]
-
-
-All ZoneList variables are the sum of the corresponding Zone variables. *Zone Multiplier* fields in the Zone objects are also taken into account.
-
-### ZoneGroup
-
-The ZoneGroup object adds a multiplier to a ZoneList. This can be used to reduce the amount of input necessary for simulating repetitive structures, such as the identical floors of a multi-story building. To create a "Floor Multiplier", use the ZoneList object to organize several zones into a typical floor. Then use the *Zone List Multiplier* field in the ZoneGroup object to multiply the system load for the zones in the list will also be multiplied. Zones with a *Multiplier* field greater than one in the Zone object are effectively double-multiplied.
-
-NOTE:  Although ZoneLists are not exclusive by themselves, ZoneLists used to form a ZoneGroup are exclusive; the ZoneLists used with a ZoneGroup must not have any zones in common.
-
-#### Tips for Multi-Story Simulations:
-
-- For floors that are multiplied, connect exterior boundary conditions of the floor to the ceiling and vice versa.
-
-- Since exterior convection coefficients vary with elevation, locate the typical middle floor zones midheight between the lowest and highest middle floors to be modeled.
-
-- Shading must be identical for all multiplied floors or less accurate results may be obtained by using the zone list multiplier.
-
-ZoneGroup and ZoneList can also be used to simulate other repetitive cases, such as clusters of zones on the ground.
-
-#### Field: Zone Group Name
-
-The name of the ZoneGroup object. This must be unique across ZoneGroups.
-
-#### Field: Zone List Name
-
-Reference to a ZoneList object. The zones in the list constitute the zones in the group.
-
-#### Field: Zone List Multiplier
-
-An integer multiplier. Zone List Multiplier is designed as a “multiplier� for floor area, zone loads, and energy consumed by internal gains. It takes the calculated load for the zone and multiplies it, sending the multiplied load to the attached HVAC system. The HVAC system size is specified to meet the entire multiplied zone load and will report the amount of the load met in the Zone Air System Sensible Heating or Cooling Energy/Rate output variable. Autosizing automatically accounts for multipliers. Metered energy consumption by internal gains objects such as Lights or Electric Equipment will be mutliplied. The default is 1.
-
-```idf
-ZONE GROUP,
-  Mid Floor,  !- Zone Group Name
-  Mid Floor List,  !- Zone List Name
-  8;  !- Zone List Multiplier
-```
-
-
-### ZoneGroup Outputs
-
-The following output variables are reported by the ZoneGroup object:
-
-* HVAC,Average,Zone Group Sensible Heating Rate [W]
-
-* HVAC,Average,Zone Group Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Group Sensible Heating Energy [J]
-
-* HVAC,Sum,Zone Group Sensible Cooling Energy [J]
-
-
-All ZoneGroup variables report the associated ZoneList value multiplied by the *Zone List Multiplier*.
-
-### Surface(s)
-
-What’s a building without surfaces?
-
-EnergyPlus allows for several surface types:
-
-- **BuildingSurface:Detailed**
-
-- **FenestrationSurface:Detailed**
-
-- **Shading:Site:Detailed**
-
-- **Shading:Building:Detailed**
-
-- **Shading:Zone:Detailed**
-
-Each of the preceding surfaces has “correct� geometry specifications. BuildingSurface and Fenestration surfaces (heat transfer surfaces) are used to describe the important elements of the building (walls, roofs, floors, windows, doors) that will determine the interactions of the building surfaces with the outside environment parameters and the internal space requirements. These surfaces are also used to represent “interzone� heat transfer. All surfaces are modeled as a thin plane (with no thickness) except that material thicknesses are taken into account for heat transfer calculations. 
-
-During specification of surfaces, several “outside� environments may be chosen:
-
-- **Ground** – when the surface is in touch with the ground (e.g. slab floors)
-
-- **Outdoors** – when the surface is an external surface (e.g. walls, roofs, windows directly exposed to the outdoor conditions)
-
-- **Surface** – when the surface is
-
-- An adiabatic internal zone surface
-
-- A interzone surface
-
-- **Zone –** when the surface is
-
-- A interzone surface in which the other surface is not put in the input file.
-
-- **OtherSideCoefficients** – when using a custom profile to describe the external conditions of the surface (advanced concept – covered in subject: SurfaceProperty:OtherSideCoefficients)
-
-- **OtherSideConditionsModel** – when using specially modeled components, such as active solar systems, that cover the outside surface and modify the conditions it experiences.
-
-**Surface** items must also specify an “outside face object�. This is
-
-- Current surface name – for adiabatic internal surfaces.
-
-- A surface name in another zone – for interzone heat transfer.
-
-- An “opposing� surface name (in the current zone) – for representing “middle� zones.
-
-**Zone** items must also specify an “outside face object�. This is
-
-- The zone that contains the other surface that is adjactent to this surface but is not entered in input.
-
-Note that heat transfer surfaces are fully represented with each description. As stated earlier in the Construction description, materials in the construction (outside to inside) are included but film coeffients neither inside nor outside are used in the description – these are automatically calculated during the EnergyPlus run. Interzone surfaces which do not have a symmetrical construction (such as a ceiling/floor) require two Construction objects with the layers in reverse order. For example, CEILING with carpet, concrete, ceiling tile and FLOOR with ceiling tile, concrete, carpet. If interzone surfaces have a symmetrical construction, the specification for the two surfaces can reference the same Construction. When a surface is connected as the outside boundary condition for another surface, the two surfaces may be in the same plane, or they may be separated to imply thickness.
-
-**Shading** surfaces are used to describe aspects of the site which do not directly impact the physical interactions of the environmental parameters but may significantly shade the building during specific hours of the day or time so the year (e.g. trees, bushes, mountains, nearby buildings which aren’t being simulated as part of this facility, etc.)
-
-Note that surfaces which are part of the simulated building automatically shade other parts of the building as geometry and time of day dictate – there is no need on the user’s part to include surfaces that might be in other zones for shading.
-
-Another surface type:
-
-- **InternalMass**
-
-is used to specify the construction/material parameters and area of items within the space that are important to heat transfer calculations but not necessarily important geometrically. (For example, furniture within the space – particularly for large spaces). Internal mass can also be used for internal walls that are not needed (when FullInteriorAndExterior Solar Distribution is in effect) for solar distribution or to represent many, if not all, interior walls when solar is distributed to the floors only.
-
-### Interzone Surfaces
-
-EnergyPlus can quite accurately simulate the surface heat exchange between two zones. However, this accuracy is not always required and using interzonal heat transfer does add to the complexity of the calculations – thus requiring more CPU time to simulate. More information about interzonal heat transfer calculations is contained in the Engineering Reference. Some simple guidelines are presented here – for three cases: adiabatic surfaces, surfaces in “middle� zones, and surfaces where heat transfer is “expected� (e.g. between a residence and an unheated, attached garage).
-
-- Adiabatic Surfaces – These surfaces would be represented as common surfaces (between two zones) where both zones are typically the same temperature. Thus, no transfer is expected in the surface from one zone to the next. These surfaces should be described as simply internal surfaces for the zone referencing as their Outside Boundary Condition Object (see later description in individual surface objects) their own surface names.
-
-- Surfaces in Middle Zones – Middle zones in a building can be simulated using a judicious use of surfaces and zone multipliers to effect the correct “loads� for the building. Thus, middle zone behavior can be simulated without modeling the adjacent zones. This is done by specifying a surface within the zone. For example, a middle floor zone can be modeled by making the floor the Outside Boundary Condition Object for the ceiling, and the ceiling the Outside Boundary Condition Object for the floor.
-
-- Surfaces between Zones with differing temperatures – These zones represent the true use of interzone surfaces. In a residence that has an attached garage, the garage may be unheated/uncooled or at least not conditioned to the same degree as the residence interior. In this case, EnergyPlus can be used to accurately calculate the effects of the differently conditioned space to the other spaces.
-
-### Surface View Factors
-
-EnergyPlus uses an area weighted approximation to calculate "view factors" between surfaces within a thermal zone. Each surface uses the total area that it can “see� among the other surfaces. The approximate view factor from this surface to each other surface is then the area of the receiving surface over the sum of areas that is visible to the sending surface.
-
-In order to account in some limited way for the fact that certain surfaces will not see each other, several assumptions have been built into this simple view factor approximation. First, a surface cannot see itself. Second, surfaces with approximately the same azimuth (facing direction) and tilt ("same" being within a built in limit) will not see each other. This means that a window will not see the wall that it is placed on, for example. Third, floors cannot see each other. Fourth, if the surface is a floor, ceiling, roof, or internal mass, the rule for the same azimuth and tilt eliminating radiant exchange between surface is waived when the receiving surface is floor, roof, ceiling, or internal mass as long as both surfaces are not floors.
-
-Note that this does not take into account that surfaces may be "around the corner" from each other and in reality not see each other at all. Rooms are assumed to be convex rather than concave in this method.
-
-To summarize, using the Surface “Class�, the approximate view factors have:
-
-1.     No surface sees itself.
-
-2.    No Floor sees another floor.
-
-3.    All other surface types see Internal Mass.
-
-4.    All other surface types see floors.
-
-5.    Floors always see ceilings.
-
-6.    Floors always see roofs.
-
-7.    All other surfaces whose tilt or facing angle differences are greater than 10 degrees see each other.
-
-If geometry is correct, conditions 1,3, and 7 should take care of all surfaces, but the other conditions supply common sense when the geometry is incorrect. More information about the EnergyPlus view factor calculation is contained in the Engineering Reference document.
-
-### GlobalGeometryRules
-
-Before the surface objects are explained in detail, a description of geometric parameters used in EnergyPlus will be given. Since the input of surface vertices is common to most of the surface types, it will also be given a separate discussion.
-
-Some flexibility is allowed in specifying surface vertices. This flexibility is embodied in the GlobalGeometryRules class/object in the input file. Note that the parameters specified in this statement are used for all surface vertice inputs – there is no further “flexibility� allowed.
-
-In order to perform shadowing calculations, the building surfaces must be specified. EnergyPlus uses a three dimensional (3D) Cartesian coordinate system for surface vertex specification. This Right Hand coordinate system has the X-axis pointing east, the Y-axis pointing north, and the Z-axis pointing up. See figure below.
-
-![](media/image054.svg)
-
-Figure 28. EnergyPlus Coordinate System
-
-#### Field: Starting Vertex Position
-
-The shadowing algorithms in EnergyPlus rely on surfaces having vertices in a certain order and positional structure. Thus, the surface translator needs to know the starting point for each surface entry. The choices are:  UpperLeftCorner, LowerLeftCorner , UpperRightCorner, or LowerRightCorner. Since most surfaces will be 4 sided, the convention will specify this position as though each surface were 4 sided. Extrapolate 3 sided figures to this convention. For 5 and more sided figures, again, try to extrapolate the best “corner� starting position.
-
-#### Field: Vertex Entry Direction
-
-Surfaces are always specified as being viewed from the outside of the zone to which they belong. (Shading surfaces are specified slightly differently and are discussed under the particular types). EnergyPlus needs to know whether the surfaces are being specified in counterclockwise or clockwise order (from the Starting Vertex Position). EnergyPlus uses this to determine the outward facing normal for the surface (which is the *facing angle* of the surface – very important in shading and shadowing calculations.
-
-#### Field: Coordinate System
-
-Vertices can be specified in two ways: using “Absolute�/“World� coordinates, or a **relative** coordinate specification. Relative coordinates allow flexibility of rapid change to observe changes in building results due to orientation and position. “World� coordinates will facilitate use within a CADD system structure.
-
-**Relative** coordinates make use of both Building and Zone North Axis values as well as Zone Origin values to locate the surface in 3D coordinate space. **World** coordinates do not use these values.
-
-Typically, all zone origin values for “World� coordinates will be (0,0,0) but Building and Zone North Axis values may be used in certain instances (namely the Daylighting Coordinate Location entries).
-
-#### Field: Daylighting Reference Point Coordinate System
-
-Daylighting reference points need to be specified as well.  Again, there can be two flavors; **relative** and **world**. Daylighting reference points must fit within the zone boundaries.
-
-**Relative** coordinates make use of both Building and Zone North Axis values as well as Zone Origin values to locate the reference point in 3D coordinate space. **World** coordinates do not use these values.
-
-#### Field: Rectangular Surface Coordinate System
-
-Simple, rectangular surfaces (Wall:Exterior, Wall:Adiabatic, Wall:Underground, Wall:Interzone, Roof, Ceiling:Adiabatic, Ceiling:Interzone, Floor:GroundContact, Floor:Adiabatic, Floor:Interzone) can be specified with their Lower Left Corner as **relative** or **world**.
-
-**Relative** (default) corners are specified relative to the Zone Origin for each surface. **World** corners would specify the absolute/world coordinate for this corner.
-
-### Surfaces
-
-Surfaces make up the buildings and the elements that shade buildings. There are several methods to inputting surfaces, ranging from simple rectangular surfaces to detailed descriptions that describe each vertex in the order specified in the GlobalGeometryRules object. The simple, rectangular surface objects are described first with the more detailed descriptions following.
-
-### Walls
-
-Walls are usually vertical (tilt = 90 degrees). These objects are used to describe exterior walls, interior walls (adiabatic), underground walls, and walls adjacent to other zones.
-
-### Wall:Exterior
-
-The Wall:Exterior object is used to describe walls that are exposed to the external environment. They receive sun, wind – all the characteristics of the external world.
-
-#### Field: Name
-
-This is a unique name associated with the exterior wall. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Azimuth Angle
-
-The Azimuth Angle indicates the direction that the wall faces (outward normal).  The angle is specified in degrees where East=90, South=180, West=270, North=0.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground).  Normally, walls are tilted 90 degrees and that is the default for this field.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate.  This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the wall in meters.
-
-#### Field: Height
-
-This field is the height of the wall in meters.
-
-### Wall:Adiabatic
-
-The Wall:Adiabatic object is used to describe interior walls and partitions. Adiabatic walls are used to describe walls next to zones that have the same thermal conditions (thus, no heat transfer).
-
-#### Field: Name
-
-This is a unique name associated with the interior wall. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Azimuth Angle
-
-The Azimuth Angle indicates the direction that the wall faces (outward normal).  The angle is specified in degrees where East=90, South=180, West=270, North=0.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground).  Normally, walls are tilted 90 degrees and that is the default for this field.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate.  This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the wall in meters.
-
-#### Field: Height
-
-This field is the height of the wall in meters.
-
-### Wall:Underground
-
-The Wall:Underground object is used to describe walls with ground contact. The temperature at the outside of the wall is the temperature in the GroundTemperature:BuildingSurface object.
-
-#### Field: Name
-
-This is a unique name associated with the underground wall. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones. Note that if the construction is **Construction:CfactorUndergroundWall** then the GroundFCfactoreMethod will be used for this wall.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Azimuth Angle
-
-The Azimuth Angle indicates the direction that the wall faces (outward normal).  The angle is specified in degrees where East=90, South=180, West=270, North=0.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground).  Normally, walls are tilted 90 degrees and that is the default for this field.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate.  This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the wall in meters.
-
-#### Field: Height
-
-This field is the height of the wall in meters.
-
-### Wall:Interzone
-
-The Wall:Interzone object is used to describe walls adjacent to zones that are significantly different conditions than the zone with this wall.
-
-#### Field: Name
-
-This is a unique name associated with the interzone wall. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Outside Boundary Condition Object
-
-The Outside Boundary Condition Object field is the name of a wall in an adjacent zone or the name of the adjacent zone.  If the adjacent zone option is used, the adjacent wall is automatically generated in the adjacent zone.  If the surface name is used, it must be in the adjacent zone.
-
-#### Field: Azimuth Angle
-
-The Azimuth Angle indicates the direction that the wall faces (outward normal).  The angle is specified in degrees where East=90, South=180, West=270, North=0.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground).  Normally, walls are tilted 90 degrees and that is the default for this field.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate.  This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the wall in meters.
-
-#### Field: Height
-
-This field is the height of the wall in meters.
-
-### Roofs/Ceilings
-
-Roofs and ceilings are, by default, flat (tilt = 0 degrees). These objects are used to describe roofs, interior ceilings (adiabatic) and ceilings adjacent to other zones.
-
-### Roof
-
-The Roof object is used to describe roofs that are exposed to the external environment.
-
-#### Field: Name
-
-This is a unique name associated with the roof. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Azimuth Angle
-
-The Azimuth Angle indicates the direction of the outward normal for the roof.  The angle is specified in degrees where East=90, South=180, West=270, North=0.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground).  Flat roofs are tilted 0 degrees and that is the default for this field.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate.  This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the roof in meters.
-
-#### Field: Width
-
-This field is the width of the roof in meters.
-
-### Ceiling:Adiabatic
-
-The Ceiling:Adiabatic object is used to describe interior ceilings that separate zones of like conditions.
-
-#### Field: Name
-
-This is a unique name associated with the ceiling. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Azimuth Angle
-
-The Azimuth Angle indicates the direction of the outward normal for the roof.  The angle is specified in degrees where East=90, South=180, West=270, North=0.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground).  Flat ceilings are tilted 0 degrees and that is the default for this field.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate.  This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the ceiling in meters.
-
-#### Field: Width
-
-This field is the width of the ceiling in meters.
-
-### Ceiling:Interzone
-
-The Ceiling:Interzone object is used to describe interior ceilings that separate zones of differing conditions (and expect heat transfer through the ceiling from the adjacent zone).
-
-#### Field: Name
-
-This is a unique name associated with the interzone ceiling. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Outside Boundary Condition Object
-
-The Outside Boundary Condition Object field is the name of a floor in an adjacent zone or the name of the adjacent zone.  If the adjacent zone option is used, the adjacent floor is automatically generated in the adjacent zone.  If the surface name is used, it must be in the adjacent zone.
-
-#### Field: Azimuth Angle
-
-The Azimuth Angle indicates the direction of the outward normal for the roof.  The angle is specified in degrees where East=90, South=180, West=270, North=0.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground).  Flat ceilings are tilted 0 degrees and that is the default for this field.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate.  This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the ceiling in meters.
-
-#### Field: Width
-
-This field is the width of the ceiling in meters.
-
-### Floors
-
-Floors are, by default, flat (tilt = 180 degrees). These objects are used to describe floors on the ground, interior floors (adiabatic) and floors adjacent to other zones.
-
-### Floor:GroundContact
-
-The Floor:GroundContact object is used to describe floors that have ground contact (usually called slabs). The temperature at the outside of the floor is the temperature in the GroundTemperature:BuildingSurface object.
-
-#### Field: Name
-
-This is a unique name associated with the floor.
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones. Note that if the construction is **Construction:FfactorGroundFloor,** then the GroundFCfactorMethod will be used with this floor.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Azimuth Angle
-
-The Azimuth Angle indicates the direction of the outward normal for the roof.  The angle is specified in degrees where East=90, South=180, West=270, North=0.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground).  Flat floors are tilted 180 degrees and that is the default for this field.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate.  This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the floor in meters.
-
-#### Field: Width
-
-This field is the width of the floor in meters.
-
-### Floor:Adiabatic
-
-The Floor:Adiabatict object is used to describe interior floors or floors that you wish to model with no heat transfer from the exterior to the floor.
-
-#### Field: Name
-
-This is a unique name associated with the floor.
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Azimuth Angle
-
-The Azimuth Angle indicates the direction of the outward normal for the roof.  The angle is specified in degrees where East=90, South=180, West=270, North=0.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground).  Flat floors are tilted 180 degrees and that is the default for this field.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate.  This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the floor in meters.
-
-#### Field: Width
-
-This field is the width of the floor in meters.
-
-### Floor:Interzone
-
-The Floor:Interzone object is used to describe floors that are adjacent to other zones that have differing conditions and you wish to model the heat transfer through the floor.
-
-#### Field: Name
-
-This is a unique name associated with the floor.
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Outside Boundary Condition Object
-
-The Outside Boundary Condition Object field is the name of a ceiling in an adjacent zone or the name of the adjacent zone.  If the adjacent zone option is used, the adjacent ceiling is automatically generated in the adjacent zone.  If the surface name is used, it must be in the adjacent zone.
-
-#### Field: Azimuth Angle
-
-The Azimuth Angle indicates the direction of the outward normal for the roof.  The angle is specified in degrees where East=90, South=180, West=270, North=0.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the wall is tilted from horizontal (or the ground).  Flat floors are tilted 180 degrees and that is the default for this field.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate.  This is specified with (x,y,z) and can be relative to the zone origin or in world coordinates, depending on the value for rectangular surfaces specified in the GlobalGeometryRules object.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the floor in meters.
-
-#### Field: Width
-
-This field is the width of the floor in meters.
-
-### Windows/Doors
-
-The following window and door objects can be used to specify simple, rectangular doors and windows. In each case, the lower left corner (locator coordinate) of the window or door is specified **relative** to the surface it is on.  Viewing the base surface as a planar surface, base the relative location from the lower left corner of the base surface. Vertex entry description as well as provisions for a few other surface types can be entered with the FenestrationSurface:Detailed object.
-
-### Window
-
-The Window object is used to place windows on surfaces that can have windows, including exterior walls, interior walls, interzone walls, roofs, floors that are exposed to outdoor conditions, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
-
-#### Field: Name
-
-This is a unique name associated with the window.
-
-#### Field: Construction Name
-
-This is the name of the subsurface’s construction (ref: objects: Construction, Construction:WindowDataFile, Construction:CompexFenestrationState).
-
-For windows, if Construction Name is not found among the constructions on the input (.idf) file, the Window Data File (ref. Construction:WindowDataFile object) will be searched for that Construction Name (see “Importing Windows from WINDOW�). If that file is not present or if the Construction Name does not match the name of an entry on the file, an error will result. If there is a match, a window construction and its corresponding glass and gas materials will be created from the information read from the file.
-
-#### Field: Building Surface Name
-
-This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. For example, a surface in contact with the ground (e.g., Outside Boundary Condition = Ground) cannot contain a window. The window assumes the outward facing angle as well as the tilt angle of the base surface.
-
-#### Field: Shading Control Name
-
-This field, if not blank, is the name of the window shading control (ref: WindowProperty:ShadingControl object) for this subsurface. It is used for Surface Type = Window and GlassDoor. To assign a shade to a window or glass door, see WindowMaterial: Shade. To assign a screen, see WindowMaterial:Screen. To assign a blind, see WindowMaterial:Blind. To assign switchable glazing, such as electrochromic glazing, see WindowProperty:ShadingControl.
-
-#### Field: Frame and Divider Name
-
-This field, if not blank, can be used to specify window frame, divider and reveal-surface data (ref: WindowProperty:FrameAndDivider object). It is used only for exterior GlassDoors and rectangular exterior Windows, i.e., those with OutsideFaceEnvironment = Outdoors.
-
-This field should be blank for triangular windows.
-
-#### Field: Multiplier
-
-This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
-
-Multiplier should be used with caution. Multiplier &gt; 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
-
-If Multiplier &gt; 1, you will get
-
---a *warning* if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
-
---an *error* if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
-
-#### Starting Corner for the surface
-
-The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate.  This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the window in meters.
-
-#### Field: Height
-
-This field is the height of the window in meters.
-
-### Door
-
-The Door object is used to place opaque doors on surfaces that can have doors, including exterior walls, interior walls, interzone walls, roofs, floors that are exposed to outdoor conditions, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
-
-#### Field: Name
-
-This is a unique name associated with the door.
-
-#### Field: Construction Name
-
-This is the name of the subsurface’s construction (ref: Construction object)
-
-#### Field: Building Surface Name
-
-This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. The door assumes the outward facing angle as well as the tilt angle of the base surface.
-
-#### Field: Multiplier
-
-This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
-
-Multiplier should be used with caution. Multiplier &gt; 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
-
-If Multiplier &gt; 1, you will get
-
---a *warning* if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
-
---an *error* if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
-
-#### Starting Corner for the surface
-
-The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate.  This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the door in meters.
-
-#### Field: Height
-
-This field is the height of the door in meters.
-
-### GlazedDoor
-
-The GlazedDoor object is used to place doors on surfaces that can have doors, including exterior walls, interior walls, interzone walls, roofs, floors that are exposed to outdoor conditions, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
-
-#### Field: Name
-
-This is a unique name associated with the glass door.
-
-#### Field: Construction Name
-
-This is the name of the subsurface’s construction (ref: objects: Construction, Construction:WindowDataFile, Construction:CompexFenestrationState).
-
-For windows, if Construction Name is not found among the constructions on the input (.idf) file, the Window Data File (ref. Construction:WindowDataFile object) will be searched for that Construction Name (see “Importing Windows from WINDOW�). If that file is not present or if the Construction Name does not match the name of an entry on the file, an error will result. If there is a match, a window construction and its corresponding glass and gas materials will be created from the information read from the file.
-
-#### Field: Building Surface Name
-
-This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. For example, a surface in contact with the ground (Outside Boundary Condition = Ground) cannot contain a window. The door assumes the outward facing angle as well as the tilt angle of the base surface.
-
-#### Field: Shading Control Name
-
-This field, if not blank, is the name of the window shading control (ref: WindowProperty:ShadingControl object) for this subsurface. It is used for Surface Type = Window and GlassDoor. To assign a shade to a window or glass door, see WindowMaterial: Shade. To assign a screen, see WindowMaterial:Screen. To assign a blind, see WindowMaterial:Blind. To assign switchable glazing, such as electrochromic glazing, see WindowProperty:ShadingControl.
-
-#### Field: Frame and Divider Name
-
-This field, if not blank, can be used to specify window frame, divider and reveal-surface data (ref: WindowProperty:FrameAndDivider object). It is used only for exterior GlassDoors and rectangular exterior Windows, i.e., those with OutsideFaceEnvironment = Outdoors.
-
-This field should be blank for triangular windows.
-
-#### Field: Multiplier
-
-This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
-
-Multiplier should be used with caution. Multiplier &gt; 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
-
-If Multiplier &gt; 1, you will get
-
---a *warning* if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
-
---an *error* if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
-
-#### Starting Corner for the surface
-
-The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate.  This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the door in meters.
-
-#### Field: Height
-
-This field is the height of the door in meters.
-
-### Window:Interzone
-
-The Window:Interzone object is used to place windows on surfaces that can have windows, including interzone walls, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
-
-#### Field: Name
-
-This is a unique name associated with the window.
-
-#### Field: Construction Name
-
-This is the name of the subsurface’s construction (ref: objects: Construction, Construction:WindowDataFile, Construction:CompexFenestrationState).
-
-For windows, if Construction Name is not found among the constructions on the input (.idf) file, the Window Data File (ref. Construction:WindowDataFile object) will be searched for that Construction Name (see “Importing Windows from WINDOW�). If that file is not present or if the Construction Name does not match the name of an entry on the file, an error will result. If there is a match, a window construction and its corresponding glass and gas materials will be created from the information read from the file.
-
-#### Field: Building Surface Name
-
-This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. For example, a surface in contact with the ground (Outside Boundary Condition = Ground) cannot contain a window. The window assumes the outward facing angle as well as the tilt angle of the base surface.
-
-#### Field: Outside Boundary Condition Object
-
-The Outside Boundary Condition Object field is the name of a window in an adjacent zone or the name of the adjacent zone.  If the adjacent zone option is used, the adjacent ceiling is automatically generated in the adjacent zone.  If the surface name is used, it must be in the adjacent zone.
-
-#### Field: Multiplier
-
-This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
-
-Multiplier should be used with caution. Multiplier &gt; 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
-
-If Multiplier &gt; 1, you will get
-
---a *warning* if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
-
---an *error* if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
-
-#### Starting Corner for the surface
-
-The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate.  This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the window in meters.
-
-#### Field: Height
-
-This field is the height of the window in meters.
-
-### Door:Interzone
-
-The Door:Interzone object is used to place opaque doors on surfaces that can have doors, including interzone walls, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
-
-#### Field: Name
-
-This is a unique name associated with the door.
-
-#### Field: Construction Name
-
-This is the name of the subsurface’s construction (ref: Construction object).
-
-#### Field: Building Surface Name
-
-This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. The door assumes the outward facing angle as well as the tilt angle of the base surface.
-
-#### Field: Outside Boundary Condition Object
-
-The Outside Boundary Condition Object field is the name of a door in an adjacent zone or the name of the adjacent zone.  If the adjacent zone option is used, the adjacent ceiling is automatically generated in the adjacent zone.  If the surface name is used, it must be in the adjacent zone.
-
-#### Field: Multiplier
-
-This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
-
-Multiplier should be used with caution. Multiplier &gt; 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
-
-If Multiplier &gt; 1, you will get
-
---a *warning* if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
-
---an *error* if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
-
-#### Starting Corner for the surface
-
-The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate.  This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the door in meters.
-
-#### Field: Height
-
-This field is the height of the door in meters.
-
-### GlazedDoor:Interzone
-
-The GlazedDoor:Interzone object is used to place doors on surfaces that can have doors, including interzone walls, interzone ceiling/floors. These, of course, can be entered using the simple rectangular objects or the more detailed vertex entry objects.
-
-#### Field: Name
-
-This is a unique name associated with the glass door.
-
-#### Field: Construction Name
-
-This is the name of the subsurface’s construction (ref: objects: Construction, Construction:WindowDataFile, Construction:ComplexFenestrationState).
-
-For windows, if Construction Name is not found among the constructions on the input (.idf) file, the Window Data File (ref. Construction:WindowDataFile object) will be searched for that Construction Name (see “Importing Windows from WINDOW�). If that file is not present or if the Construction Name does not match the name of an entry on the file, an error will result. If there is a match, a window construction and its corresponding glass and gas materials will be created from the information read from the file.
-
-#### Field: Building Surface Name
-
-This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. For example, a surface in contact with the ground (Outside Boundary Condition = Ground) cannot contain a window. The door assumes the outward facing angle as well as the tilt angle of the base surface.
-
-#### Field: Outside Boundary Condition Object
-
-The Outside Boundary Condition Object field is the name of a glazed (glass) door in an adjacent zone or the name of the adjacent zone.  If the adjacent zone option is used, the adjacent ceiling is automatically generated in the adjacent zone.  If the surface name is used, it must be in the adjacent zone.
-
-#### Field: Multiplier
-
-This field is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
-
-Multiplier should be used with caution. Multiplier &gt; 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
-
-If Multiplier &gt; 1, you will get
-
---a *warning* if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
-
---an *error* if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
-
-#### Starting Corner for the surface
-
-The rectangular subsurfaces specify the lower left corner of the surface for their starting coordinate.  This corner is specifed relative to the lower left corner of the base surface by specifying the X and Z values from that corner.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the door in meters.
-
-#### Field: Height
-
-This field is the height of the door in meters.
-
-Examples of the rectangular surfaces are found in the example files 4ZoneWithShading\_Simple\_1.idf and 4ZoneWithShading\_Simple\_2. Some examples:
-
-```idf
-  Wall:Exterior,
-    Zn001:Wall001,           !- Name
-    EXTERIOR,                !- Construction Name
-    ZONE 1,                  !- Zone Name
-    180,                     !- Azimuth Angle {deg}
-    90,                      !- Tilt Angle {deg}
-    0,                       !- Starting X Coordinate {m}
-    0,                       !- Starting Y Coordinate {m}
-    0,                       !- Starting Z Coordinate {m}
-    20,                      !- Length {m}
-    10;                      !- Height {m}
-
-  Window,
-    Zn001:Wall001:Win001,    !- Name
-    SINGLE PANE HW WINDOW,   !- Construction Name
-    Zn001:Wall001,           !- Building Surface Name
-    ,                        !- Shading Control Name
-    ,                        !- Frame and Divider Name
-    1,                       !- Multiplier
-    4,                       !- Starting X Coordinate {m}
-    3,                       !- Starting Z Coordinate {m}
-    3,                       !- Length {m}
-    5;                       !- Height {m}
-
-  Door,
-    Zn001:Wall001:Door001,   !- Name
-    HOLLOW WOOD DOOR,        !- Construction Name
-    Zn001:Wall001,           !- Building Surface Name
-    1,                       !- Multiplier
-    14,                      !- Starting X Coordinate {m}
-    0,                       !- Starting Z Coordinate {m}
-    3,                       !- Length {m}
-    5;                       !- Height {m}
-
-  Wall:Adiabatic,
-    Zn001:Wall004,           !- Name
-    INTERIOR,                !- Construction Name
-    ZONE 1,                  !- Zone Name
-    90,                      !- Azimuth Angle {deg}
-    90,                      !- Tilt Angle {deg}
-    20,                      !- Starting X Coordinate {m}
-    0,                       !- Starting Y Coordinate {m}
-    0,                       !- Starting Z Coordinate {m}
-    20,                      !- Length {m}
-    10;                      !- Height {m}
-
-  Floor:Adiabatic,
-    Zn001:Flr001,            !- Name
-    FLOOR,                   !- Construction Name
-    ZONE 1,                  !- Zone Name
-    90,                      !- Azimuth Angle {deg}
-    180,                     !- Tilt Angle {deg}
-    0,                       !- Starting X Coordinate {m}
-    0,                       !- Starting Y Coordinate {m}
-    0,                       !- Starting Z Coordinate {m}
-    20,                      !- Length {m}
-    20;                      !- Width {m}
-
-  Ceiling:Interzone,
-    Zn001:Roof001,           !- Name
-    CEILING34,               !- Construction Name
-    ZONE 1,                  !- Zone Name
-    Zn003:Flr001,            !- Outside Boundary Condition Object
-    180,                     !- Azimuth Angle {deg}
-    0,                       !- Tilt Angle {deg}
-    0,                       !- Starting X Coordinate {m}
-    0,                       !- Starting Y Coordinate {m}
-    10,                      !- Starting Z Coordinate {m}
-    20,                      !- Length {m}
-    20;                      !- Width {m}
-
-  Window,
-    Zn002:Wall001:Win001,    !- Name
-    SINGLE PANE HW WINDOW,   !- Construction Name
-    Zn002:Wall001,           !- Building Surface Name
-    ,                        !- Shading Control Name
-    ,                        !- Frame and Divider Name
-    1,                       !- Multiplier
-    4,                       !- Starting X Coordinate {m}
-    3,                       !- Starting Z Coordinate {m}
-    3,                       !- Length {m}
-    5;                       !- Height {m}
-```
-
-### Surface Vertices
-
-Each of the following surfaces:
-
-* BuildingSurface:Detailed
-
-* Wall:Detailed
-
-* RoofCeiling:Detailed
-
-* Floor:Detailed
-
-* FenstrationSurface:Detailed
-
-* Shading:Site:Detailed
-
-* Shading:Building:Detailed
-
-* Shading:Zone:Detailed
-
-use the same vertex input. The numeric parameters indicated below are taken from the BuildingSurface:Detailed definition;  the others may not be exactly the same but are identical in configuration. They are also “extensible� – so, if you want more vertices for these surfaces, you may add to the IDD definition as indicated in the “extensible� comment or, as EnergyPlus is “auto-extensible� just add the number of vertices into your input file.. Note that FenestrationSurface:Detailed is not extensible and is limited to 4 (max) vertices. If you leave the Number of Surface Vertex groups blank or enter **autocalculate**, EnergyPlus looks at the number of groups entered and figures out how many coordinate groups are entered.
-
-**Note that the resolution on the surface vertex input is 1 millimeter (.001 meter). Therefore, using vertices that are very close together (&lt;1 mm) may result in invalid dot product and fatal errors during shading calculations.**
-
-![](media/image055.svg)
-
-Figure 29. Illustration for Surface Vertices
-
-The figure above will help illustrate Surface Vertex entry. The convention used in “GlobalGeometryRules� dictates the order of the vertices (ref: GlobalGeometryRules). In this example, the conventions used are Starting Vertex Position = UpperLeftCorner and Vertex Entry Direction= CounterClockwise. The surfaces for this single zone are:
-
-4,0,0,H, 0,0,0, A,0,0, A,0,H; ! **(4 vertices, South Wall)**
-
-4,A,0,H,A,0,0,A,B,0,A,B,H;  ! **(4 vertices, East Wall)**
-
-     **ignore other walls that are not shown in this figure**
-
-4,C,0,J,A,0,H,A,B,H,C,B,J; ! **(4 vertices, roof)**
-
-3,C,0,J,0,0,H,A,0,H; ! **(3 vertices, gable end)**
-
-4,0,0,H, 0,0,0, A,0,0, A,0,H; ! **(4 vertices, South Wall)**
-
-Note that in this example, point 1 of the entry is the Upper Left Corner of the rectangular surfaces and the point of the triangle for the 3 sided surface. The east wall shows the order of vertex entry. For horizontal surfaces, any vertex may be chosen as the starting position, but the Vertex Entry Direction convention must be followed. The surface details report (Output: Surfaces:List, Details;) is very useful for reviewing the accuracy of surface geometry inputs (ref: Surface Output Variables/Reports and Variable Dictionary Reports).
-
-From the detailed vertices, EnergyPlus tries to determine the “height� and “width� of the surface. Obviously, this doesn’t work well for &gt;4 sided surfaces; for these, if the calculated height and width are not close to the gross area for the surface, the height and width shown will be the square root of the area (and thus a square).
-
-### Building Surfaces - Detailed
-
-A building surface is necessary for all calculations. There must be at least one building surface per zone. You can use the detailed descriptions as shown below or the simpler, rectangular surface descriptions shown earlier.
-
-### Wall:Detailed
-
-The Wall:Detailed object is used to describe walls.
-
-#### Field: Name
-
-This is a unique name associated with each building surface. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Outside Boundary Condition
-
-This value can be one of several things depending on the actual kind of surface.
-
-1)    **Surface** – if this surface is an internal surface, then this is the choice. The value will either be a surface in the base zone or a surface in another zone. The heat balance between two zones can be accurately simulated by specifying a surface in an adjacent zone. EnergyPlus will simulate a group of zones simultaneously and will include the heat transfer between zones. However, as this increases the complexity of the calculations, it is not necessary to specify the other zone unless the two zones will have a significant temperature difference. If the two zones will not be very different (temperature wise), then the surface should use itself as the outside environment or specify this field as **Adiabatic**. The surface name on the “outside� of this surface (adjacent to) is placed in the next field.
-
-2)    **Adiabatic** – an internal surface in the same Zone. This surface will not transfer heat out of the zone, but will still store heat in thermal mass. Only the inside face of the surface will exchange heat with the zone (i.e. two adiabatic surfaces are required to model internal partitions where both sides of the surface are exchanging heat with the zone). The Outside Boundary Condition Object can be left blank.
-
-3)    **Zone** – this is similar to Surface but EnergyPlus will automatically create the required surface in the adjacent zone when this is entered for the surface. If there are windows or doors on the surface, EnergyPlus automatically creates appropriate sub-surfaces as well.
-
-4)    **Outdoors** – if this surface is exposed to outside temperature conditions, then this is the choice. See Sun Exposure and Wind Exposure below for further specifications on this kind of surface.
-
-5)    **Ground** – if this surface is exposed to the ground, then this is the usual choice. The temperature on the outside of this surface will be the Site:GroundTemperature:Surface value for the month. For more information on ground contact surfaces, reference the Auxiliary Programs document section on “Ground Heat Transfer in EnergyPlus�.
-
-6)    **GroundFCfactorMethod** – if this surface is exposed to the ground and using the **Construction:CfactorUndergroundWall**, then this is the choice. The temperature on the outside of this surface will be the Site:GroundTemperature:FcfactorMethod value for the month.
-
-7)    **OtherSideCoefficients** – if this surface has a custom, user specified temperature or other parameters (See SurfaceProperty:OtherSideCoefficients specification), then this is the choice. The outside boundary condition will be the name of the SurfaceProperty:OtherSideCoefficients specification.
-
-8)    **OtherSideConditionsModel** – if this surface has a specially-modeled multi-skin component, such as a transpired collector or vented photovoltaic panel, attached to the outside (See SurfaceProperty:OtherSideConditionsModel specification), then this the choice. The outside face environment will be the name of the SurfaceProperty:OtherSideConditionsModelspecification.
-
-9)    **GroundSlabPreprocessorAverage** – uses the average results from the Slab preprocessor calculations.
-
-10) **GroundSlabPreprocessorCore** – uses the core results from the Slab preprocessor calculations.
-
-11) **GroundSlabPreprocessorPerimeter** – uses the perimeter results from the Slab preprocessor calculations.
-
-12) **GroundBasementPreprocessorAverageWall** – uses the average wall results from the Basement preprocessor calculations.
-
-13) **GroundBasementPreprocessorAverageFloor** – uses the average floor results from the Basement preprocessor calculations.
-
-14) **GroundBasementPreprocessorUpperWall** – uses the upper wall results from the Basement preprocessor calculations.
-
-15) **GroundBasementPreprocessorLowerWall** – uses the lower wall results from the Basement preprocessor calculations.
-
-#### Field: Outside Boundary Condition Object
-
-If neither Surface, OtherSideCoefficients, or OtherSideConditionsModel are specified for the Outside Boundary Condition (previous field), then this field should be left blank.
-
-As stated above, if the Outside Boundary Condition is “Surface�, then this field’s value must be the surface name whose inside face temperature will be forced on the outside face of the base surface. This permits heat exchange between adjacent zones (interzone heat transfer) when multiple zones are simulated, but can also be used to simulate middle zone behavior without modeling the adjacent zones. This is done by specifying a surface within the zone. For example, a middle floor zone can be modeled by making the floor the Outside Boundary Condition Object for the ceiling, and the ceiling the Outside Boundary Condition Object for the floor.
-
-If the Outside Boundary Condition is Zone, then this field should contain the zone name of the adjacent zone for the surface.
-
-Note: Zones with interzone heat transfer are not adiabatic and the internal surfaces contribute to gains or losses. Adiabatic surfaces are modeled by specifying the base surface itself in this field.  Also, for interzone heat transfer, both surfaces must be represented – for example, if you want interzone heat transfer to an attic space, the ceiling in the lower zone must have a surface object with the outside face environment as the floor in the attic and, likewise, there must be a floor surface object in the attic that references the ceiling surface name in the lower zone.
-
-Equally, if the Outside Boundary Condition is “OtherSideCoefficients�, then this field’s value must be the SurfaceProperty:OtherSideCoefficients name. Or if the Outside Boundary Condition is “OtherSideConditionsModel� then this field’s value must be the SurfaceProperty:OtherSideConditionsModel name.
-
-#### Field: Sun Exposure
-
-If the surface is exposed to the sun, then “SunExposed� should be entered in this field. Otherwise, “NoSun� should be entered.
-
-Note, a cantilevered floor could have “Outdoors� but “NoSun� exposure.
-
-#### Field: Wind Exposure
-
-If the surface is exposed to the Wind, then “WindExposed� should be entered in this field. Otherwise, “NoWind� should be entered.
-
-Note: When a surface is specified with “NoWind�, this has several implications. Within the heat balance code, this surface will default to using the simple ASHRAE exterior convection coefficient correlation with a zero wind speed. In addition, since the ASHRAE simple method does not have a separate value for equivalent long wavelength radiation to the sky and ground, using “NoWind� also eliminates long wavelength radiant exchange from the exterior of the surface to both the sky and the ground. Thus, only simple convection takes place at the exterior face of a surface specified with “NoWind�.
-
-#### Field: View Factor to Ground
-
-The fraction of the ground plane (assumed horizontal) that is visible from a heat-transfer surface. It is used to calculate the diffuse solar radiation from the ground that is incident on the surface.
-
-For example, if there are no obstructions, a vertical surface sees half of the ground plane and so View Factor to Ground = 0.5. A horizontal downward-facing surface sees the entire ground plane, so  View Factor to Ground = 1.0. A horizontal upward-facing surface (horizontal roof) does not see the ground at all, so View Factor to Ground = 0.0.
-
-Unused if reflections option in Solar Distribution field in Building object input unless a DaylightingDevice:Shelf or DaylightingDevice:Tubular has been specified.
-
-If you do not use the reflections option in the Solar Distribution field in your Building object input, you are responsible for entering the View Factor to Ground for each heat-transfer surface. Typical values for a surface that is not shadowed are obtained by the simple equation:
-
-View Factor to Ground = (1-cos(SurfTilt))/2
-
-For example, this gives 0.5 for a wall of tilt 90°. If the tilt of the wall changes, then the View Factor to Ground must also change.
-
-If you enter **autocalculate** in this field, EnergyPlus will automatically calculate the view factor to ground based on the tilt of the surface.
-
-If **you do use the reflections option in the Solar Distribution field** in your Building object input, you do **not** have to enter View Factor to Ground values. In this case the program will automatically calculate the value to use for each exterior surface taking into account solar shadowing (including shadowing of the ground by the building) and reflections from obstructions (ref: Building, Field: Solar Distribution).
-
-However, if you do use the reflections option AND you are modeling a DaylightingDevice:Shelf or DaylightingDevice:Tubular, then you still need to enter some values of View Factor to Ground. For DaylightingDevice:Shelf you need to enter View Factor to Ground for the window associated with the shelf. And for DaylightingDevice:Tubular you need to enter the View Factor to Ground for the FenestrationSurface:Detailed corresponding to the dome of the tubular device.
-
-Note 1: The corresponding view factor to the sky for diffuse solar radiation is not a user input; it is calculated within EnergyPlus based on surface orientation, sky solar radiance distribution, and shadowing surfaces.
-
-Note 2:  The view factors to the sky and ground for thermal infrared (long-wave) radiation are not user inputs; they are calculated within EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground IR view factor.
-
-#### Field: Number of Vertices
-
-This field specifies the number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on “Surface Vertices� above.
-
-### RoofCeiling:Detailed
-
-The RoofCeiling:Detailed object is used to describe walls.
-
-#### Field: Name
-
-This is a unique name associated with each building surface. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Outside Boundary Condition
-
-This value can be one of several things depending on the actual kind of surface.
-
-1)   **Surface** – if this surface is an internal surface, then this is the choice. The value will either be a surface in the base zone or a surface in another zone. The heat balance between two zones can be accurately simulated by specifying a surface in an adjacent zone. EnergyPlus will simulate a group of zones simultaneously and will include the heat transfer between zones. However, as this increases the complexity of the calculations, it is not necessary to specify the other zone unless the two zones will have a significant temperature difference. If the two zones will not be very different (temperature wise), then the surface should use itself as the outside environment or specify this field as **Adiabatic**. The surface name on the “outside� of this surface (adjacent to) is placed in the next field.
-
-2)   **Adiabatic** – an internal surface in the same Zone. This surface will not transfer heat out of the zone, but will still store heat in thermal mass. Only the inside face of the surface will exchange heat with the zone (i.e. two adiabatic surfaces are required to model internal partitions where both sides of the surface are exchanging heat with the zone). The Outside Boundary Condition Object can be left blank.
-
-3)   **Zone** – this is similar to Surface but EnergyPlus will automatically create the required surface in the adjacent zone when this is entered for the surface. If there are windows or doors on the surface, EnergyPlus automatically creates appropriate sub-surfaces as well.
-
-4)   **Outdoors** – if this surface is exposed to outside temperature conditions, then this is the choice. See Sun Exposure and Wind Exposure below for further specifications on this kind of surface.
-
-5)   **Ground** – if this surface is exposed to the ground, then this is the choice. The temperature on the outside of this surface will be the Ground Temperature.
-
-6)   **OtherSideCoefficients** – if this surface has a custom, user specified temperature or other parameters (See SurfaceProperty:OtherSideCoefficients specification), then this is the choice. The outside boundary condition will be the name of the SurfaceProperty:OtherSideCoefficients specification.
-
-7)   **OtherSideConditionsModel** – if this surface has a specially-modeled multi-skin component, such as a transpired collector or vented photovoltaic panel, attached to the outside (See SurfaceProperty:OtherSideConditionsModel specification), then this the choice. The outside face environment will be the name of the SurfaceProperty:OtherSideConditionsModelspecification.
-
-8)   **GroundSlabPreprocessorAverage** – uses the average results from the Slab preprocessor calculations.
-
-9)   **GroundSlabPreprocessorCore** – uses the core results from the Slab preprocessor calculations.
-
-10)**GroundSlabPreprocessorPerimeter** – uses the perimeter results from the Slab preprocessor calculations.
-
-11)**GroundBasementPreprocessorAverageWall** – uses the average wall results from the Basement preprocessor calculations.
-
-12)**GroundBasementPreprocessorAverageFloor** – uses the average floor results from the Basement preprocessor calculations.
-
-13)**GroundBasementPreprocessorUpperWall** – uses the upper wall results from the Basement preprocessor calculations.
-
-14)**GroundBasementPreprocessorLowerWall** – uses the lower wall results from the Basement preprocessor calculations.
-
-#### Field: Outside Boundary Condition Object
-
-If neither Surface, OtherSideCoefficients, or OtherSideConditionsModel are specified for the Outside Boundary Condition (previous field), then this field should be left blank.
-
-As stated above, if the Outside Boundary Condition is “Surface�, then this field’s value must be the surface name whose inside face temperature will be forced on the outside face of the base surface. This permits heat exchange between adjacent zones (interzone heat transfer) when multiple zones are simulated, but can also be used to simulate middle zone behavior without modeling the adjacent zones. This is done by specifying a surface within the zone. For example, a middle floor zone can be modeled by making the floor the Outside Boundary Condition Object for the ceiling, and the ceiling the Outside Boundary Condition Object for the floor.
-
-If the Outside Boundary Condition is Zone, then this field should contain the zone name of the adjacent zone for the surface.
-
-Note: Zones with interzone heat transfer are not adiabatic and the internal surfaces contribute to gains or losses. Adiabatic surfaces are modeled by specifying the base surface itself in this field.  Also, for interzone heat transfer, both surfaces must be represented – for example, if you want interzone heat transfer to an attic space, the ceiling in the lower zone must have a surface object with the outside face environment as the floor in the attic and, likewise, there must be a floor surface object in the attic that references the ceiling surface name in the lower zone.
-
-Equally, if the Outside Boundary Condition is “OtherSideCoefficients�, then this field’s value must be the SurfaceProperty:OtherSideCoefficients name. Or if the Outside Boundary Condition is “OtherSideConditionsModel� then this field’s value must be the SurfaceProperty:OtherSideConditionsModel name.
-
-#### Field: Sun Exposure
-
-If the surface is exposed to the sun, then “SunExposed� should be entered in this field. Otherwise, “NoSun� should be entered.
-
-Note, a cantilevered floor could have “Outdoors� but “NoSun� exposure.
-
-#### Field: Wind Exposure
-
-If the surface is exposed to the Wind, then “WindExposed� should be entered in this field. Otherwise, “NoWind� should be entered.
-
-Note: When a surface is specified with “NoWind�, this has several implications. Within the heat balance code, this surface will default to using the simple ASHRAE exterior convection coefficient correlation with a zero wind speed. In addition, since the ASHRAE simple method does not have a separate value for equivalent long wavelength radiation to the sky and ground, using “NoWind� also eliminates long wavelength radiant exchange from the exterior of the surface to both the sky and the ground. Thus, only simple convection takes place at the exterior face of a surface specified with “NoWind�.
-
-#### Field: View Factor to Ground
-
-The fraction of the ground plane (assumed horizontal) that is visible from a heat-transfer surface. It is used to calculate the diffuse solar radiation from the ground that is incident on the surface.
-
-For example, if there are no obstructions, a vertical surface sees half of the ground plane and so View Factor to Ground = 0.5. A horizontal downward-facing surface sees the entire ground plane, so  View Factor to Ground = 1.0. A horizontal upward-facing surface (horizontal roof) does not see the ground at all, so View Factor to Ground = 0.0.
-
-Unused if reflections option in Solar Distribution field in Building object input unless a DaylightingDevice:Shelf or DaylightingDevice:Tubular has been specified.
-
-If you do not use the reflections option in the Solar Distribution field in your Building object input, you are responsible for entering the View Factor to Ground for each heat-transfer surface. Typical values for a surface that is not shadowed are obtained by the simple equation:
-
-View Factor to Ground = (1-cos(SurfTilt))/2
-
-For example, this gives 0.5 for a wall of tilt 90°. If the tilt of the wall changes, then the View Factor to Ground must also change.
-
-If you enter **autocalculate** in this field, EnergyPlus will automatically calculate the view factor to ground based on the tilt of the surface.
-
-If **you do use the reflections option in the Solar Distribution field** in your Building object input, you do **not** have to enter View Factor to Ground values. In this case the program will automatically calculate the value to use for each exterior surface taking into account solar shadowing (including shadowing of the ground by the building) and reflections from obstructions (ref: Building, Field: Solar Distribution).
-
-However, if you do use the reflections option AND you are modeling a DaylightingDevice:Shelf or DaylightingDevice:Tubular, then you still need to enter some values of View Factor to Ground. For DaylightingDevice:Shelf you need to enter View Factor to Ground for the window associated with the shelf. And for DaylightingDevice:Tubular you need to enter the View Factor to Ground for the FenestrationSurface:Detailed corresponding to the dome of the tubular device.
-
-Note 1: The corresponding view factor to the sky for diffuse solar radiation is not a user input; it is calculated within EnergyPlus based on surface orientation, sky solar radiance distribution, and shadowing surfaces.
-
-Note 2:  The view factors to the sky and ground for thermal infrared (long-wave) radiation are not user inputs; they are calculated within EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground IR view factor.
-
-#### Field: Number of Vertices
-
-This field specifies the number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on “Surface Vertices� above.
-
-### Floor:Detailed
-
-The Floor:Detailed object is used to describe walls.
-
-#### Field: Name
-
-This is a unique name associated with each building surface. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Outside Boundary Condition
-
-This value can be one of several things depending on the actual kind of surface.
-
-1)   **Surface** – if this surface is an internal surface, then this is the choice. The value will either be a surface in the base zone or a surface in another zone. The heat balance between two zones can be accurately simulated by specifying a surface in an adjacent zone. EnergyPlus will simulate a group of zones simultaneously and will include the heat transfer between zones. However, as this increases the complexity of the calculations, it is not necessary to specify the other zone unless the two zones will have a significant temperature difference. If the two zones will not be very different (temperature wise), then the surface should use itself as the outside environment or specify this field as **Adiabatic**. The surface name on the “outside� of this surface (adjacent to) is placed in the next field.
-
-2)   **Adiabatic** – an internal surface in the same Zone. This surface will not transfer heat out of the zone, but will still store heat in thermal mass. Only the inside face of the surface will exchange heat with the zone (i.e. two adiabatic surfaces are required to model internal partitions where both sides of the surface are exchanging heat with the zone). The Outside Boundary Condition Object can be left blank.
-
-3)   **Zone** – this is similar to Surface but EnergyPlus will automatically create the required surface in the adjacent zone when this is entered for the surface. If there are windows or doors on the surface, EnergyPlus automatically creates appropriate sub-surfaces as well.
-
-4)   **Outdoors** – if this surface is exposed to outside temperature conditions, then this is the choice. See Sun Exposure and Wind Exposure below for further specifications on this kind of surface.
-
-5)   **Ground** – if this surface is exposed to the ground, then this is the usual choice. The temperature on the outside of this surface will be the Site:GroundTemperature:Surface value for the month. For more information on ground contact surfaces, reference the Auxiliary Programs document section on “Ground Heat Transfer in EnergyPlus�.
-
-6)   **GroundFCfactorMethod** – if this surface is exposed to the ground and using the **Construction:FfactorGroundFloor**, then this is the choice. The temperature on the outside of this surface will be the Site:GroundTemperature:FcfactorMethod value for the month.
-
-7)   **OtherSideCoefficients** – if this surface has a custom, user specified temperature or other parameters (See SurfaceProperty:OtherSideCoefficients specification), then this is the choice. The outside boundary condition will be the name of the SurfaceProperty:OtherSideCoefficients specification.
-
-8)   **OtherSideConditionsModel** – if this surface has a specially-modeled multi-skin component, such as a transpired collector or vented photovoltaic panel, attached to the outside (See SurfaceProperty:OtherSideConditionsModel specification), then this the choice. The outside face environment will be the name of the SurfaceProperty:OtherSideConditionsModelspecification.
-
-9)   **GroundSlabPreprocessorAverage** – uses the average results from the Slab preprocessor calculations.
-
-10)**GroundSlabPreprocessorCore** – uses the core results from the Slab preprocessor calculations.
-
-11)**GroundSlabPreprocessorPerimeter** – uses the perimeter results from the Slab preprocessor calculations.
-
-12)**GroundBasementPreprocessorAverageWall** – uses the average wall results from the Basement preprocessor calculations.
-
-13)**GroundBasementPreprocessorAverageFloor** – uses the average floor results from the Basement preprocessor calculations.
-
-14)**GroundBasementPreprocessorUpperWall** – uses the upper wall results from the Basement preprocessor calculations.
-
-15)**GroundBasementPreprocessorLowerWall** – uses the lower wall results from the Basement preprocessor calculations.
-
-#### Field: Outside Boundary Condition Object
-
-If neither Surface, OtherSideCoefficients, or OtherSideConditionsModel are specified for the Outside Boundary Condition (previous field), then this field should be left blank.
-
-As stated above, if the Outside Boundary Condition is “Surface�, then this field’s value must be the surface name whose inside face temperature will be forced on the outside face of the base surface. This permits heat exchange between adjacent zones (interzone heat transfer) when multiple zones are simulated, but can also be used to simulate middle zone behavior without modeling the adjacent zones. This is done by specifying a surface within the zone. For example, a middle floor zone can be modeled by making the floor the Outside Boundary Condition Object for the ceiling, and the ceiling the Outside Boundary Condition Object for the floor.
-
-If the Outside Boundary Condition is Zone, then this field should contain the zone name of the adjacent zone for the surface.
-
-Note: Zones with interzone heat transfer are not adiabatic and the internal surfaces contribute to gains or losses. Adiabatic surfaces are modeled by specifying the base surface itself in this field.  Also, for interzone heat transfer, both surfaces must be represented – for example, if you want interzone heat transfer to an attic space, the ceiling in the lower zone must have a surface object with the outside face environment as the floor in the attic and, likewise, there must be a floor surface object in the attic that references the ceiling surface name in the lower zone.
-
-Equally, if the Outside Boundary Condition is “OtherSideCoefficients�, then this field’s value must be the SurfaceProperty:OtherSideCoefficients name. Or if the Outside Boundary Condition is “OtherSideConditionsModel� then this field’s value must be the SurfaceProperty:OtherSideConditionsModel name.
-
-#### Field: Sun Exposure
-
-If the surface is exposed to the sun, then “SunExposed� should be entered in this field. Otherwise, “NoSun� should be entered.
-
-Note, a cantilevered floor could have “Outdoors� but “NoSun� exposure.
-
-#### Field: Wind Exposure
-
-If the surface is exposed to the Wind, then “WindExposed� should be entered in this field. Otherwise, “NoWind� should be entered.
-
-Note: When a surface is specified with “NoWind�, this has several implications. Within the heat balance code, this surface will default to using the simple ASHRAE exterior convection coefficient correlation with a zero wind speed. In addition, since the ASHRAE simple method does not have a separate value for equivalent long wavelength radiation to the sky and ground, using “NoWind� also eliminates long wavelength radiant exchange from the exterior of the surface to both the sky and the ground. Thus, only simple convection takes place at the exterior face of a surface specified with “NoWind�.
-
-#### Field: View Factor to Ground
-
-The fraction of the ground plane (assumed horizontal) that is visible from a heat-transfer surface. It is used to calculate the diffuse solar radiation from the ground that is incident on the surface.
-
-For example, if there are no obstructions, a vertical surface sees half of the ground plane and so View Factor to Ground = 0.5. A horizontal downward-facing surface sees the entire ground plane, so  View Factor to Ground = 1.0. A horizontal upward-facing surface (horizontal roof) does not see the ground at all, so View Factor to Ground = 0.0.
-
-Unused if reflections option in Solar Distribution field in Building object input unless a DaylightingDevice:Shelf or DaylightingDevice:Tubular has been specified.
-
-If you do not use the reflections option in the Solar Distribution field in your Building object input, you are responsible for entering the View Factor to Ground for each heat-transfer surface. Typical values for a surface that is not shadowed are obtained by the simple equation:
-
-View Factor to Ground = (1-cos(SurfTilt))/2
-
-For example, this gives 0.5 for a wall of tilt 90°. If the tilt of the wall changes, then the View Factor to Ground must also change.
-
-If you enter **autocalculate** in this field, EnergyPlus will automatically calculate the view factor to ground based on the tilt of the surface.
-
-If **you do use the reflections option in the Solar Distribution field** in your Building object input, you do **not** have to enter View Factor to Ground values. In this case the program will automatically calculate the value to use for each exterior surface taking into account solar shadowing (including shadowing of the ground by the building) and reflections from obstructions (ref: Building, Field: Solar Distribution).
-
-However, if you do use the reflections option AND you are modeling a DaylightingDevice:Shelf or DaylightingDevice:Tubular, then you still need to enter some values of View Factor to Ground. For DaylightingDevice:Shelf you need to enter View Factor to Ground for the window associated with the shelf. And for DaylightingDevice:Tubular you need to enter the View Factor to Ground for the FenestrationSurface:Detailed corresponding to the dome of the tubular device.
-
-Note 1: The corresponding view factor to the sky for diffuse solar radiation is not a user input; it is calculated within EnergyPlus based on surface orientation, sky solar radiance distribution, and shadowing surfaces.
-
-Note 2:  The view factors to the sky and ground for thermal infrared (long-wave) radiation are not user inputs; they are calculated within EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground IR view factor.
-
-#### Field: Number of Vertices
-
-This field specifies the number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on “Surface Vertices� above.
-
-Some examples of using these objects:
-
-```idf
-Floor:Detailed,
-    Floor_NorthZone_1stFloor,!- Name
-    FLOOR-SLAB-ASSEMBLY,     !- Construction Name
-    NorthZone_1stFloor,      !- Zone Name
-    Ground,                  !- Outside Boundary Condition
-    ,                        !- Outside Boundary Condition Object
-    NoSun,                   !- Sun Exposure
-    NoWind,                  !- Wind Exposure
-    0.0,                     !- View Factor to Ground
-    4,                       !- Number of Vertices
-    0, 11, 0,                           !- X,Y,Z  1 {m}
-    25, 11, 0,                          !- X,Y,Z  2 {m}
-    25, 5.5, 0,                         !- X,Y,Z  3 {m}
-   0, 5.5, 0;                          !- X,Y,Z  4 {m}
-
-RoofCeiling:Detailed,
-    Ceiling_SouthZone_1stFloor,  !- Name
-    CEILING-FLOOR-ASSEMBLY,  !- Construction Name
-    SouthZone_1stFloor,      !- Zone Name
-    Surface,                 !- Outside Boundary Condition
-    Floor_SouthZone_2ndFloor,!- Outside Boundary Condition Object
-    NoSun,                   !- Sun Exposure
-    NoWind,                  !- Wind Exposure
-    0.0,                     !- View Factor to Ground
-    4,                       !- Number of Vertices
-    0, 0, 3.4,                          !- X,Y,Z  1 {m}
-    25, 0, 3.4,                         !- X,Y,Z  2 {m}
-    25, 5.5, 3.4,                       !- X,Y,Z  3 {m}
-   0, 5.5, 3.4;                        !- X,Y,Z  4 {m}
-
-Wall:Detailed,
-    InteriorWall_SouthZone_1stFloor,  !- Name
-    INTERIOR-WALL-ASSEMBLY,  !- Construction Name
-    SouthZone_1stFloor,      !- Zone Name
-    Surface,                 !- Outside Boundary Condition
-    InteriorWall_NorthZone_1stFloor,  !- Outside Boundary Condition Object
-    NoSun,                   !- Sun Exposure
-    NoWind,                  !- Wind Exposure
-    0,                       !- View Factor to Ground
-    4,                       !- Number of Vertices
-    25, 5.5, 3.7,                       !- X,Y,Z  1 {m}
-    25, 5.5, 0,                         !- X,Y,Z  2 {m}
-    0, 5.5, 0,                          !- X,Y,Z  3 {m}
-   0, 5.5, 3.7;                        !- X,Y,Z  4 {m}
-```
-
-### BuildingSurface:Detailed
-
-The BuildingSurface:Detailed object can more generally describe each of the surfaces.
-
-#### Field: Name
-
-This is a unique name associated with each building surface. It is used in several other places as a reference (e.g. as the base surface name for a Window or Door).
-
-#### Field: Surface Type
-
-Used primarily for convenience, the surface type can be one of the choices illustrated above – Wall, Floor, Ceiling, Roof. Azimuth (facing) and Tilt are determined from the vertex coordinates. Note that “normal� floors will be tilted 180° whereas flat roofs/ceilings will be tilted 0°. EnergyPlus uses this field’s designation, along with the calculated tilt of the surface, to issue warning messages when tilts are “out of range�. Calculations in EnergyPlus use the actual calculated tilt values for the actual heat balance calculations. Note, however, that a floor tilted 0° is really facing “into� the zone and is not what you will desire for the calculations even though the coordinate may appear correct in the viewed DXF display.
-
-“Normal� tilt for walls is 90° -- here you may use the calculated Azimuth to make sure your walls are facing away from the zone’s interior.
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface. Regardless of location in the building, the “full� construction (all layers) is used. For example, for an interior wall separating two zones, zone x would have the outside layer (e.g. drywall) as the material that shows in zone y and then the layers to the inside layer – the material that shows in zone x. For symmetric constructions, the same construction can be used in the surfaces described in both zones.
-
-#### Field: Zone Name
-
-This is the zone name to which the surface belongs.
-
-#### Field: Outside Boundary Condition
-
-This value can be one of several things depending on the actual kind of surface.
-
-1)   **Surface** – if this surface is an internal surface, then this is the choice. The value will either be a surface in the base zone or a surface in another zone. The heat balance between two zones can be accurately simulated by specifying a surface in an adjacent zone. EnergyPlus will simulate a group of zones simultaneously and will include the heat transfer between zones. However, as this increases the complexity of the calculations, it is not necessary to specify the other zone unless the two zones will have a significant temperature difference. If the two zones will not be very different (temperature wise), then the surface should use itself as the outside environment or specify this field as **Adiabatic**. In either case, the surface name on the “outside� of this surface (adjacent to) is placed in the next field.
-
-2)   **Adiabatic** – an internal surface in the same Zone. This surface will not transfer heat out of the zone, but will still store heat in thermal mass. Only the inside face of the surface will exchange heat with the zone (i.e. two adiabatic surfaces are required to model internal partitions where both sides of the surface are exchanging heat with the zone). The Outside Boundary Condition Object can be left blank.
-
-3)   **Zone** – this is similar to Surface but EnergyPlus will automatically create the required surface in the adjacent zone when this is entered for the surface. If there are windows or doors on the surface, EnergyPlus automatically creates appropriate sub-surfaces as well.
-
-4)   **Outdoors** – if this surface is exposed to outside temperature conditions, then this is the choice. See Sun Exposure and Wind Exposure below for further specifications on this kind of surface.
-
-5)   **Ground** – if this surface is exposed to the ground, then this is the usual choice. The temperature on the outside of this surface will be the Site:GroundTemperature:Surface value for the month. For more information on ground contact surfaces, reference the Auxiliary Programs document section on “Ground Heat Transfer in EnergyPlus�.
-
-6)   **GroundFCfactorMethod** – if this surface is exposed to the ground and using the **Construction:CfactorUndergroundWall** or **Construction:FfactorGroundFloor** (depending on surface type), then this is the choice. The temperature on the outside of this surface will be the Site:GroundTemperature:FcfactorMethod value for the month.
-
-7)   **OtherSideCoefficients** – if this surface has a custom, user specified temperature or other parameters (See SurfaceProperty:OtherSideCoefficients specification), then this is the choice. The outside boundary condition will be the name of the SurfaceProperty:OtherSideCoefficients specification.
-
-8)   **OtherSideConditionsModel** – if this surface has a specially-modeled multi-skin component, such as a transpired collector or vented photovoltaic panel, attached to the outside (See SurfaceProperty:OtherSideConditionsModel specification), then this the choice. The outside face environment will be the name of the SurfaceProperty:OtherSideConditionsModelspecification.
-
-9)   **GroundSlabPreprocessorAverage** – uses the average results from the Slab preprocessor calculations.
-
-10)**GroundSlabPreprocessorCore** – uses the core results from the Slab preprocessor calculations.
-
-11)**GroundSlabPreprocessorPerimeter** – uses the perimeter results from the Slab preprocessor calculations.
-
-12)**GroundBasementPreprocessorAverageWall** – uses the average wall results from the Basement preprocessor calculations.
-
-13)**GroundBasementPreprocessorAverageFloor** – uses the average floor results from the Basement preprocessor calculations.
-
-14)**GroundBasementPreprocessorUpperWall** – uses the upper wall results from the Basement preprocessor calculations.
-
-15)**GroundBasementPreprocessorLowerWall** – uses the lower wall results from the Basement preprocessor calculations.
-
-#### Field: Outside Boundary Condition Object
-
-If neither Surface, OtherSideCoefficients, or OtherSideConditionsModel are specified for the Outside Boundary Condition (previous field), then this field should be left blank.
-
-As stated above, if the Outside Boundary Condition is “Surface�, then this field’s value must be the surface name whose inside face temperature will be forced on the outside face of the base surface. This permits heat exchange between adjacent zones (interzone heat transfer) when multiple zones are simulated, but can also be used to simulate middle zone behavior without modeling the adjacent zones. This is done by specifying a surface within the zone. For example, a middle floor zone can be modeled by making the floor the Outside Boundary Condition Object for the ceiling, and the ceiling the Outside Boundary Condition Object for the floor.
-
-If the Outside Boundary Condition is Zone, then this field should contain the zone name of the adjacent zone for the surface.
-
-Note: Zones with interzone heat transfer are not adiabatic and the internal surfaces contribute to gains or losses. Adiabatic surfaces are modeled by specifying the base surface itself in this field.  Also, for interzone heat transfer, both surfaces must be represented – for example, if you want interzone heat transfer to an attic space, the ceiling in the lower zone must have a surface object with the outside face environment as the floor in the attic and, likewise, there must be a floor surface object in the attic that references the ceiling surface name in the lower zone.
-
-Equally, if the Outside Boundary Condition is “OtherSideCoefficients�, then this field’s value must be the SurfaceProperty:OtherSideCoefficients name. Or if the Outside Boundary Condition is “OtherSideConditionsModel� then this field’s value must be the SurfaceProperty:OtherSideConditionsModel name.
-
-#### Field: Sun Exposure
-
-If the surface is exposed to the sun, then “SunExposed� should be entered in this field. Otherwise, “NoSun� should be entered.
-
-Note, a cantilevered floor could have “Outdoors� but “NoSun� exposure.
-
-#### Field: Wind Exposure
-
-If the surface is exposed to the Wind, then “WindExposed� should be entered in this field. Otherwise, “NoWind� should be entered.
-
-Note: When a surface is specified with “NoWind�, this has several implications. Within the heat balance code, this surface will default to using the simple ASHRAE exterior convection coefficient correlation with a zero wind speed. In addition, since the ASHRAE simple method does not have a separate value for equivalent long wavelength radiation to the sky and ground, using “NoWind� also eliminates long wavelength radiant exchange from the exterior of the surface to both the sky and the ground. Thus, only simple convection takes place at the exterior face of a surface specified with “NoWind�.
-
-#### Field: View Factor to Ground
-
-The fraction of the ground plane (assumed horizontal) that is visible from a heat-transfer surface. It is used to calculate the diffuse solar radiation from the ground that is incident on the surface.
-
-For example, if there are no obstructions, a vertical surface sees half of the ground plane and so View Factor to Ground = 0.5. A horizontal downward-facing surface sees the entire ground plane, so  View Factor to Ground = 1.0. A horizontal upward-facing surface (horizontal roof) does not see the ground at all, so View Factor to Ground = 0.0.
-
-Unused if reflections option in Solar Distribution field in Building object input unless a DaylightingDevice:Shelf or DaylightingDevice:Tubular has been specified.
-
-If you do not use the reflections option in the Solar Distribution field in your Building object input, you are responsible for entering the View Factor to Ground for each heat-transfer surface. Typical values for a surface that is not shadowed are obtained by the simple equation:
-
-View Factor to Ground = (1-cos(SurfTilt))/2
-
-For example, this gives 0.5 for a wall of tilt 90°. If the tilt of the wall changes, then the View Factor to Ground must also change.
-
-If you enter **autocalculate** in this field, EnergyPlus will automatically calculate the view factor to ground based on the tilt of the surface.
-
-If **you do use the reflections option in the Solar Distribution field** in your Building object input, you do **not** have to enter View Factor to Ground values. In this case the program will automatically calculate the value to use for each exterior surface taking into account solar shadowing (including shadowing of the ground by the building) and reflections from obstructions (ref: Building, Field: Solar Distribution).
-
-However, if you do use the reflections option AND you are modeling a DaylightingDevice:Shelf or DaylightingDevice:Tubular, then you still need to enter some values of View Factor to Ground. For DaylightingDevice:Shelf you need to enter View Factor to Ground for the window associated with the shelf. And for DaylightingDevice:Tubular you need to enter the View Factor to Ground for the FenestrationSurface:Detailed corresponding to the dome of the tubular device.
-
-Note 1: The corresponding view factor to the sky for diffuse solar radiation is not a user input; it is calculated within EnergyPlus based on surface orientation, sky solar radiance distribution, and shadowing surfaces.
-
-Note 2:  The view factors to the sky and ground for thermal infrared (long-wave) radiation are not user inputs; they are calculated within EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground IR view factor.
-
-#### Field: Number of Vertices
-
-This field specifies the number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on “Surface Vertices� above.
-
-IDF example of three walls (first is an exterior wall, second and third are interzone partitions):
-
-```idf
-BuildingSurface:Detailed,Zn001:Wall001,  !- Base Surface Name
-  Wall,EXTERIOR,  !- Class and Construction Name
-  ZONE 1 @ 200 601 0 T,  !- Zone
-  Outdoors,,  !- Outside Boundary Condition  and Target (if applicable)
-   SunExposed,  !- Solar Exposure
-   WindExposed,  !- Wind Exposure
-  0.5000000    ,  !- VF to Ground
-           4, !-Rectangle
-  0.0000000E+00,  0.0000000E+00,   3.048000    ,
-  0.0000000E+00,  0.0000000E+00,  0.0000000E+00,
-   6.096000    ,  0.0000000E+00,  0.0000000E+00,
-   6.096000    ,  0.0000000E+00,   3.048000    ;
-
-BuildingSurface:Detailed,Zn001:Wall006,  !-Base Surface Name
-  Wall,INTERIOR,  !- Class and Construction Name
-  HEARTLAND AREA,  !- Zone
-  Surface,Zn004:Wall005,  !- Outside Boundary Conditions and Target (if applicable)
-   NoSun,  !- Solar Exposure
-   NoWind,  !- Wind Exposure
-  0.5000000    ,  !- VF to Ground
-           4, !-Rectangle
-   38.01000    ,   28.25000    ,   10.00000    ,
-   38.01000    ,   28.25000    ,  0.0000000E+00,
-   38.01000    ,   18.25000    ,  0.0000000E+00,
-   38.01000    ,   18.25000    ,   10.00000    ;
-
-BuildingSurface:Detailed,Zn001:Wall007,  !- Base Surface Name
-  Wall,INTERIOR,  !- Class and Construction Name
-  HEARTLAND AREA,  !- Zone
-  Surface,Zn003:Wall006,  !- Outside Boundary Conditions and Target (if applicable)
-   NoSun,  !- Solar Exposure
-   NoWind,  !- Wind Exposure
-  0.5000000    ,  !- VF to Ground
-           4, !-Rectangle
-   58.01000    ,   18.25000    ,   10.00000    ,
-   58.01000    ,   18.25000    ,  0.0000000E+00,
-   58.01000    ,   28.25000    ,  0.0000000E+00,
-   58.01000    ,   28.25000    ,   10.00000    ;
-```
-
-### FenestrationSurface:Detailed
-
-This surface class is used for subsurfaces, which can be of five different types: Windows, Doors, GlassDoors, TubularDaylightDomes, and TubularDaylightDiffusers. A subsurface (such as a window) of a base surface (such as a wall) inherits several of the properties (such as Outside Boundary Condition, Sun Exposure, etc.) of the base surface. Windows, GlassDoors, TubularDaylightDomes, and TubularDaylightDiffusers are considered to have one or more glass layers and so transmit solar radiation. Doors are considered to be opaque.
-
-#### Field: Name
-
-This is a unique name associated with the heat transfer subsurface. It may be used in other places as a reference (e.g. as the opposing subsurface of an interzone window or door).
-
-#### Field: Surface Type
-
-The choices for Surface Type are Window, Door, GlassDoor, TubularDaylightDome, and TubularDaylightDiffuser. Doors are assumed to be opaque (do not transmit solar radiation) whereas the other surface types do transmit solar radiation. Windows and Glass Doors are treated identically in the calculation of conduction heat transfer, solar gain, daylighting, etc. A Window or GlassDoor, but not a Door, can have a movable interior, exterior or between-glass shading device, such as blinds (ref: WindowMaterial:Blind object), and can have a frame and/or a divider (ref: WindowProperty:FrameAndDivider object). TubularDaylightDomes and TubularDaylightDomes are specialized subsurfaces for use with the DaylightingDevice:Tubular object to simulate Tubular Daylighting Devices (TDDs). TubularDaylightDomes and TubularDaylightDomes cannot have shades, screens or blinds. In the following, the term “window� applies to Window, GlassDoor, TubularDaylightDome, and TubularDaylightDome, if not otherwise explicitly mentioned.
-
-As noted in the description of the BuildingSurface:Detailed, Azimuth (facing angle) and Tilt are calculated from the entered vertices. Tilts of subsurfaces will normally be the same as their base surface. If these are significantly beyond the “normals� for the base surface, warning messages may be issued. If the facing angles are not correct, you may have a window pointing “into� the zone rather than out of it – this would cause problems in the calculations.  Note, too, that a “reveal� (inset or outset) may occur if the plane of the subsurface is not coincident with the base surface; the reveal has an effect on shading of the subsurface.
-
-#### Field: Construction Name
-
-This is the name of the subsurface’s construction (ref: Construction object [for Door] and Construction, Construction:ComplexFenestrationState, Construction:WindowDataFile objects [for Window and GlassDoor]).
-
-For windows, if Construction Name is not found among the constructions on the input (.idf) file, the Window Data File (ref. Construction:WindowDataFile object) will be searched for that Construction Name (see “Importing Windows from WINDOW�). If that file is not present or if the Construction Name does not match the name of an entry on the file, an error will result. If there is a match, a window construction and its corresponding glass and gas materials will be created from the information read from the file.
-
-#### Field: Building Surface Name
-
-This is the name of a surface that contains this subsurface. Certain kinds of surfaces may not be allowed to have subsurfaces. For example, a surface in contact with the ground (Outside Boundary Condition = Ground) cannot contain a window.
-
-#### Field: Outside Boundary Condition Object
-
-If the base surface has Outside Boundary Condition = Surface or OtherSideCoefficients, then this field must also be specified for the subsurface. Otherwise, it can be left blank.
-
-If the base surface has Outside Boundary Condition = Zone, then this surface retains that characteristic and uses the same zone of the base surface. It can be entered here for clarity or it can be left blank.
-
-If Outside Boundary Condition for the base surface is Surface, this field should specify the subsurface in the opposing zone that is the counterpart to this subsurface. The constructions of the subsurface and opposing subsurface must match, except that, for multi-layer constructions, the layer order of the opposing subsurface’s construction must be the reverse of that of the subsurface.
-
-If Outside Boundary Condition for the base surface is OtherSideCoefficients, this field could specify the set of SurfaceProperty:OtherSideCoefficients for this subsurface. If this is left blank, then the Other Side Coefficients of the base surface will be used for this subsurface. *Windows and GlassDoors are not allowed to have Other Side Coefficients.*
-
-#### Field: View Factor to Ground
-
-The fraction of the ground plane (assumed horizontal) that is visible from a heat-transfer surface. It is used to calculate the diffuse solar radiation from the ground that is incident on the surface.
-
-For example, if there are no obstructions, a vertical surface sees half of the ground plane and so View Factor to Ground = 0.5. A horizontal downward-facing surface sees the entire ground plane, so  View Factor to Ground = 1.0. A horizontal upward-facing surface (horizontal roof) does not see the ground at all, so View Factor to Ground = 0.0.
-
-Unused if reflections option in Solar Distribution field in Building object input unless a Daylighting Device:Shelf or Daylighting Device:Tubular has been specified.
-
-If you do not use the reflections option in the Solar Distribution field in your Building object input, you are responsible for entering the View Factor to Ground for each heat-transfer surface. Typical values for a surface that is not shadowed are obtained by the simple equation:
-
-View Factor to Ground = (1-cos(SurfTilt))/2
-
-For example, this gives 0.5 for a wall of tilt 90°. If the tilt of the wall changes, then the View Factor to Ground must also change.
-
-If you enter **autocalculate** in this field, EnergyPlus will automatically calculate the view factor to ground based on the tilt of the surface.
-
-If **you do use the reflections option in the Solar Distribution field** in your BUILDING object input, you do **not** have to enter View Factor to Ground values. In this case the program will automatically calculate the value to use for each exterior surface taking into account solar shadowing (including shadowing of the ground by the building) and reflections from obstructions (ref: Building, Field: Solar Distribution).
-
-However, if you do use the reflections option AND you are modeling a DaylightingDevice:Shelf or DaylightingDevice:Tubular, then you still need to enter some values of View Factor to Ground. For DaylightingDevice:Shelf you need to enter View Factor to Ground for the window associated with the shelf. And for DaylightingDevice:Tubular you need to enter the View Factor to Ground for the FenestrationSurface:Detailed corresponding to the dome of the tubular device (ref: DaylightingDevice:Tubular).
-
-Note 1: The corresponding view factor to the sky for diffuse solar radiation is not a user input; it is calculated within EnergyPlus based on surface orientation, sky solar radiance distribution, and shadowing surfaces.
-
-Note 2:  The view factors to the sky and ground for thermal infrared (long-wave) radiation are not user inputs; they are calculated within EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground infrared view factor.
-
-#### Field: Shading Control Name
-
-This field, if not blank, is the name of the window shading control (ref: WindowProperty:ShadingControl object) for this subsurface. It is used for Surface Type = Window and GlassDoor. To assign a shade to a window or glass door, see WindowMaterial: Shade. To assign a screen, see WindowMaterial:Screen. To assign a blind, see WindowMaterial:Blind. To assign switchable glazing, such as electrochromic glazing, see WindowProperty:ShadingControl.
-
-#### Field: Frame and Divider Name
-
-This field, if not blank, can be used to specify window frame, divider and reveal-surface data (ref: WindowProperty:FrameAndDivider object). It is used only for exterior GlassDoors and rectangular exterior Windows, i.e., those with OutsideFaceEnvironment = Outdoors.
-
-This field should be blank for triangular windows.
-
-#### Field: Multiplier
-
-Used only for Surface Type = Window, Door or Glass Door. It is the number of identical items on the base surface. Using Multiplier can save input effort and calculation time. In the calculation the area (and area of frame and divider, if present and surface type is a window) is multiplied by Multiplier. The calculation of shadowing on the subsurfaces (and the calculation of the interior distribution of beam solar radiation transmitted by windows and glass doors) are done for the specified subsurface position and dimensions.
-
-Multiplier should be used with caution. Multiplier &gt; 1 can give inaccurate or nonsensical results in situations where the results are sensitive to window or glass door position. This includes shadowing on the window/glass door, daylighting from the window/glass door, and interior distribution of solar radiation from the window/glass door. In these cases, the results for the single input window/glass door, after multiplication, may not be representative of the results you would get if you entered each of the multiple subsurfaces separately.
-
-If Multiplier &gt; 1, you will get
-
---a *warning* if Solar Distribution = FullExterior or FullInteriorAndExterior (ref: Building - Field: Solar Distribution), indicating that the shadowing on the input window or the interior solar radiation distribution from the input window may not be representative of the actual group of windows. No warning is issued if Solar Distribution = MinimalShadowing.
-
---an *error* if the window is an exterior window/glass door in a zone that has a detailed daylighting calculation (Daylighting:Detailed specified for the zone). Since a single window with a multiplier can never give the same daylight illuminance as the actual set of windows, you are not allowed to use Multiplier in this situation.
-
-#### Field: Number of Vertices
-
-The number of sides the surface has (number of X,Y,Z vertex groups). For further information, see the discussion on “Surface Vertices� above. Door and GlassDoor subsurfaces are rectangular and therefore have four vertices. Window subsurfaces can be rectangular or triangular and therefore have four or three vertices, respectively.
-
-#### Fields: Vertex Coordinates
-
-This is a total of twelve fields giving the x,y,z coordinate values of the four vertices  of   rectangular subsurfaces [m], or a total of nine fields giving the x,y,z coordinate values of the three vertices of triangular windows.
-
-For triangular windows the first vertex listed can be any of the three vertices, but the order of the vertices should be counter-clockwise if VertexEntry is CounterClockWise and clockwise if VertexEntry is ClockWise (ref: GlobalGeometryRules).
-
-An IDF example of a rectangular subsurface (Window):
-
-```idf
-FenestrationSurface:Detailed,
- Zn001:Wall001:Win001,  !- SubSurface Name
-  Window,SINGLE PANE HW WINDOW,  !- Class and Construction Name
-  Zn001:Wall001,,         !- Base Surface Name and Target (if applicable)
-  0.5000000    ,          !- VF to Ground
-  WINDOW-CONTROL-DRAPES,  !- Window Shading Control
-  TestFrameAndDivider,    !- Frame/Divider name
-  5,                      !- Multiplier
-  4,                      !- Rectangle (number of sides)
-   1.524000    ,  0.1520000    ,   2.743000    ,
-   1.524000    ,  0.1520000    ,  0.3050000    ,
-   4.572000    ,  0.1520000    ,  0.3050000    ,
-   4.572000    ,  0.1520000    ,   2.743000    ;
-```
-
-
-### Window Modeling Options
-
-The following table shows what input objects/fields to use to model different window options. It also gives the name of an example input, if available, that demonstrates the option.
-
-
-
-Table 8. Window Modeling Options
-
-<table class="table table-striped">
-<tr>
-<th>Option</th>
-<th>Object/Field or Output Variable</th>
-<th>Input File (histributeh with install)</th>
-</tr>
-<tr>
-<td>Build up a window from layers</td>
-<td>WindowMaterial:Glazing, WindowMaterial:Gas, WindowMaterial:Shade, WindowMaterial:Screen, WindowMaterial:Blind, Construction</td>
-<td>WindowTests.idf</td>
-</tr>
-<tr>
-<td>Add an overhang</td>
-<td>Shading:Zone:Detailed</td>
-<td>5ZoneAirCooled.idf</td>
-</tr>
-<tr>
-<td>Add a shading device</td>
-<td>WindowMaterial:Shade, WindowMaterial:Screen or WindowMaterial:Blind; WindowProperty:ShadingControl</td>
-<td>WindowTests.idf, PurchAirWindowBlind.idf</td>
-</tr>
-<tr>
-<td>Control a shading device</td>
-<td>WindowProperty:ShadingControl</td>
-<td>PurchAirWindowBlind.idf</td>
-</tr>
-<tr>
-<td>Determine when a shading device is on in a particular timestep</td>
-<td>Print the variable  “Surface Shading Device Is On Time Fraction�</td>
-<td>PurchAirWindowBlind.idf</td>
-</tr>
-<tr>
-<td>Control the slat angle of a blind</td>
-<td>WindowProperty:ShadingControl</td>
-<td>PurchAirWindowBlind.idf</td>
-</tr>
-<tr>
-<td>Add a frame</td>
-<td>WindowProperty:FrameAndDivider</td>
-<td>PurchAirWithDaylighting.idf</td>
-</tr>
-<tr>
-<td>Add a divider</td>
-<td>WindowProperty:FrameAndDivider</td>
-<td>PurchAirWithDaylighting.idf</td>
-</tr>
-<tr>
-<td>Allow window to daylight a zone</td>
-<td>Daylighting:Controls, Daylighting:DELight:Controls</td>
-<td>PurchAirWithDaylighting.idf, DElight-Detailed-Comparison.idf</td>
-</tr>
-<tr>
-<td>Find solar reflected onto window from neighboring buildings</td>
-<td>Building/SolarDistribution field – uses “WithReflections�</td>
-<td>ReflectiveAdjacentBuilding.idf</td>
-</tr>
-<tr>
-<td>Model switchable glazing (e.g., electrochromic glass)</td>
-<td>WindowProperty:ShadingControl</td>
-<td>PurchAirWithDaylighting.idf</td>
-</tr>
-<tr>
-<td>Add an interior window</td>
-<td>Define two FenestrationSurface:Detailed’s, one for each associated interior wall</td>
-<td>PurchAirWithDoubleFacadeDaylighting.idf</td>
-</tr>
-<tr>
-<td>Track how beam solar falls on interior surfaces</td>
-<td>Building/Solar Distribution = FullInteriorAndExterior</td>
-<td>PurchAirWithDoubleFacadeDaylighting.idf</td>
-</tr>
-<tr>
-<td>Track beam solar transmitted through interior windows</td>
-<td>Building/Solar Distribution = FullInteriorAndExterior</td>
-<td>PurchAirWithDoubleFacadeDaylighting.idf</td>
-</tr>
-<tr>
-<td>Add a shading device on an interior window</td>
-<td>Not allowed</td>
-<td> </td>
-</tr>
-<tr>
-<td>Model an airflow window (aka, heat extract window)</td>
-<td>WindowProperty:AirflowControl</td>
-<td>AirflowWindowsAndBetweenGlassBlinds.idf</td>
-</tr>
-<tr>
-<td>Add a storm window glass layer</td>
-<td>WindowProperty:StormWindow</td>
-<td>StormWindow.idf</td>
-</tr>
-<tr>
-<td>Add natural ventilation through an open window</td>
-<td>Ventilation or AirflowNetwork objects (AirflowNetwork:Multizone:Surface, AirflowNetwork:MultiZone:Component:DetailedOpening, etc.)</td>
-<td>AirflowNetwork3zvent.idf</td>
-</tr>
-<tr>
-<td>Add diffusing glass</td>
-<td>WindowMaterial:Glazing/Solar Diffusing = Yes</td>
-<td> </td>
-</tr>
-<tr>
-<td>Add dirt on window</td>
-<td>WindowMaterial:Glazing/Dirt Correction Factor for Solar and Visible Transmittance</td>
-<td> </td>
-</tr>
-<tr>
-<td>Import window (and frame/divider if present) from WINDOW program</td>
-<td>See “Importing Windows from WINDOW program�</td>
-<td> </td>
-</tr>
-<tr>
-<td>Find daylighting through interior windows</td>
-<td>See “Double Facades: Daylighting through Interior Windows�</td>
-<td>PurchAirWithDoubleFacadeDaylighting.idf</td>
-</tr>
-<tr>
-<td>Determine when condensation occurs</td>
-<td>Print the variables “Surface Window Inside Face Glazing Condensation Status,� “Surface Window Inside Face Frame Condensation Status,� “Surface Window Inside Face Divider Condensation Status�</td>
-<td> </td>
-</tr>
-</table>
-
-
-
-### InternalMass
-
-Any surface that would logically be described as an interior wall, floor or ceiling can just as easily be described as Internal Mass. Internal Mass surface types only exchange energy with the zone in which they are described; they do not see any other zones. There are two approaches to using internal mass. The first approach is to have several pieces of internal mass with each piece having a different construction type. The other approach is to choose an average construction type and combine all of the interior surfaces into a single internal mass. Similar to internal surfaces with an adiabatic boundary condtion, the zone will only exchange energy with the inside of the Internal Mass construction. If both sides of the surface exchange energy with the zone then the user should input twice the area when defining the Internal Mass object. Note that furniture and other large objects within a zone can be described using internal mass. However, simplifying calculations using internal mass must be used with caution when the “FullInteriorAndExterior� or “FullInteriorAndExteriorWithReflections� Solar Distribution model (see Building parameters) is chosen.
-
-#### Example
-
-When zoning an office building, five west-facing offices have been combined into one zone. All of the offices have interior walls made of the same materials. As shown in the figure below, this zone may be described with 5 exterior walls and 11 internal walls or 1 exterior wall and 1 internal mass. Note that fewer surfaces will speed up the EnergyPlus calculations.
-
-![](media/image056.svg)
-
-Figure 30. Representing 11 internal walls as internal mass
-
-#### Example
-
-A five-story building has the same ceiling/floor construction separating each of the levels. Zones that are on floors 2 through 4 may be described using a single piece of internal mass to represent both the floor and ceiling. The construction for this internal mass would be identical to the ceiling/floor construction that would be used to describe separate surfaces and the area of the internal mass surface would be the total surface area of the combined ceilings/floors (i.e. twice the total floor area).
-
-#### Field: Name
-
-This is a unique character string associated with the internal mass surface. Though it must be unique from other surface names, it is used primarily for convenience with internal mass surfaces.
-
-#### Field: Construction Name
-
-This is the name of the construction (ref: Construction object) used in the surface.
-
-#### Field: Zone Name
-
-This is the name of the zone in which the internal mass is represented.
-
-#### Field: Surface Area
-
-This field is the surface area of the internal mass. The area that is specified must be the entire surface area that is exposed to the zone. If both sides of a wall are completely within the same zone, then the area of both sides must be included when describing that internal wall.
-
-IDF examples of Internal Mass surfaces:
-
-```idf
-InternalMass,Zn002:IntM001,  !- Surface Name
-  INTERIOR,  !- Construction Name
-  DORM ROOMS AND COMMON AREAS,  !- Zone
-   408.7734    ;  !- Total area exposed to Zone {m2}
-
-InternalMass,Zn002:IntM002,  !- Surface Name
-  PARTITION02,  !- Construction Name
-  DORM ROOMS AND COMMON AREAS,  !- Zone
-   371.6122    ;  !- Total area exposed to Zone {m2}
-```
-
-
-### Surface Output Variables/Reports
-
-Note that Surface Outputs from specialized algorithms (such as Effective Moisture Penetration Depth (EMPD), Combined Heat and Moisture Transport (HAMT) and Conduction Finite Difference (CondFD) are discussed under the objects that describe the specialized inputs for these algorithms). You can access them via these links:
-
-- Moisture Penetration Depth (EMPD) Outputs
-
-- Conduction Finite Difference (CondFD) Outputs
-
-- Heat and Moisture (HAMT) Outputs
-
-Additionally, the output variables applicable to all heat transfer surfaces:
-
-* Zone,Sum,Surface Inside Face Heat Balance Calculation Iteration Count []
-
-* Zone,Average,Surface Inside Face Temperature [C]
-
-* Zone,Average,Surface Outside Face Temperature [C]
-
-* Zone,Average,Surface Inside Face Adjacent Air Temperature [C]
-
-* Zone,Average,Surface Inside Face Convection Heat Transfer Coefficient [W/m2-K]
-
-* Zone,Average,Surface Inside Face Convection Heat Gain Rate [W]
-
-* Zone,Average,Surface Inside Face Convection Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Inside Face Convection Heat Gain Energy [J]
-
-* Zone,Average,Surface Inside Face Net Surface Thermal Radiation Heat Gain Rate [W]
-
-* Zone,Average,Surface Inside Face Net Surface Thermal Radiation Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Inside Face Net Surface Thermal Radiation Heat Gain Energy [J]
-
-* Zone,Average,Surface Inside Face Solar Radiation Heat Gain Rate [W]
-
-* Zone,Average,Surface Inside Face Solar Radiation Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Inside Face Solar Radiation Heat Gain Energy [J]
-
-* Zone,Average,Surface Inside Face Lights Radiation Heat Gain Rate [W]
-
-* Zone,Average,Surface Inside Face Lights Radiation Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Inside Face Lights Radiation Heat Gain Energy [J]
-
-* Zone,Average,Surface Inside Face Internal Gains Radiation Heat Gain Rate [W]
-
-* Zone,Average,Surface Inside Face Internal Gains Radiation Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Inside Face Internal Gains Radiation Heat Gain Energy [J]
-
-* Zone,Average,Surface Inside Face System Radiation Heat Gain Rate [W]
-
-* Zone,Average,Surface Inside Face System Radiation Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Inside Face System Radiation Heat Gain Energy [J]
-
-* Zone,Average,Surface Outside Face Convection Heat Transfer Coefficient [W/m2-K]
-
-* Zone,Average,Surface Outside Face Convection Heat Gain Rate [W]
-
-* Zone,Average,Surface Outside Face Convection Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Outside Face Convection Heat Gain Energy [J]
-
-* Zone,Average,Surface Outside Face Net Thermal Radiation Heat Gain Rate [W]
-
-* Zone,Average,Surface Outside Face Net Thermal Radiation Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Outside Face Net Thermal Radiation Heat Gain Energy [J]
-
-* Zone,Average,Surface Outside Face Thermal Radiation to Air Heat Transfer Coefficient [W/m2-K]
-
-* Zone,Average,Surface Outside Face Thermal Radiation to Sky Heat Transfer Coefficient [W/m2-K]
-
-* Zone,Average,Surface Outside Face Thermal Radiation to Ground Heat Transfer Coefficient [W/m2-K]
-
-* Zone,Average,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate [W]
-
-* Zone,Sum,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Energy [J]
-
-* Zone,Average,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate [W]
-
-* Zone,Average,Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate per Area[W/m2]
-
-* Zone, Sum,Surface Inside Face Interior Windows Incident Beam Solar Radiation Energy [J]
-
-* Zone,Average,Surface Inside Face Initial Transmitted Diffuse Absorbed Solar Radiation Rate [W]
-
-* Zone,Average,Surface Inside Face Initial Transmitted Diffuse Transmitted Out Window Solar Radiation Rate [W]
-
-* Zone,Average,Surface Inside Face Absorbed Shortwave Radiation Rate [W]
-
-Output variables applicable to all exterior heat transfer surfaces:
-
-* Zone,Average,Surface Outside Face Outdoor Air Drybulb Temperature [C]
-
-* Zone,Average,Surface Outside Face Outdoor Air Wetbulb Temperature [C]
-
-* Zone,Average,Surface Outside Face Outdoor Air Wind Speed [m/s]
-
-* Zone,Average,Surface Outside Face Sunlit Area [m2]
-
-* Zone,Average,Surface Outside Face Sunlit Fraction []
-
-* Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Solar Radiation Heat Gain Rate [W]
-
-* Zone,Average,Surface Outside Face Solar Radiation Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Outside Face Solar Radiation Heat Gain Energy [J]
-
-* Zone,Average,Surface Outside Face Incident Beam Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Ext Diff Sol From Bm-To-Diff Refl From Ground[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Sky Diffuse Ground Reflected Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Sky Diffuse Surface Reflected Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Beam To Beam Surface Reflected Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Beam To Diffuse Surface Reflected Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Beam Solar Incident Angle Cosine Value[]
-
-* Zone,Average,Surface Anisotropic Sky Multiplier []
-
-* Zone,Average,Surface Window BSDF Beam Direction Number []
-
-* Zone,Average,Surface Window BSDF Beam Theta Angle [rad]
-
-* Zone,Average,Surface Window BSDF Beam Phi Angle [rad]
-
-Output variables applicable to opaque heat transfer surfaces (FLOOR, WALL, ROOF, DOOR). **Note – these are advanced variables – you must read the descriptions and understand before use – then you must use the Diagnostics object to allow reporting.**
-
-* Zone,Average,Surface Inside Face Solar Radiation Heat Gain Rate [W]
-
-* Zone,Average,Surface Inside Face Solar Radiation Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Inside Face Solar Radiation Heat Gain Energy [J]
-
-* Zone,Average,Surface Inside Face Lights Radiation Heat Gain Rate [W]
-
-* Zone,Average,Surface Inside Face Lights Radiation Heat Gain Rate per Area [W/m2]
-
-* Zone,Sum,Surface Inside Face Lights Radiation Heat Gain Energy [J]
-
-* Zone,Average,Surface Inside Face Conduction Heat Transfer Rate [W]
-
-* Zone,Average,Surface Inside Face Conduction Heat Gain Rate [W]
-
-* Zone,Average,Surface Inside Face Conduction Heat Loss Rate [W]
-
-* Zone,Average,Surface Inside Face Conduction Heat Transfer Rate per Area [W/m2]
-
-* Zone,Sum,Surface Inside Face Conduction Heat Transfer Energy [J]
-
-* Zone,Average,Surface Outside Face Conduction Heat Transfer Rate [W]
-
-* Zone,Average,Surface Outside Face Conduction Heat Gain Rate [W]
-
-* Zone,Average,Surface Outside Face Conduction Heat Loss Rate [W]
-
-* Zone,Average,Surface Outside Face Conduction Heat Transfer Rate per Area [W/m2]
-
-* Zone,Sum,Surface Outside Face Conduction Heat Transfer Energy [J]
-
-* Zone,Average,Surface Average Face Conduction Heat Transfer Rate [W]
-
-* Zone,Average,Surface Average Face Conduction Heat Gain Rate [W]
-
-* Zone,Average,Surface Average Face Conduction Heat Loss Rate [W]
-
-* Zone,Average,Surface Average Face Conduction Heat Transfer Rate per Area [W/m2]
-
-* Zone,Sum,Surface Average Face Conduction Heat Transfer Energy [J]
-
-* Zone,Average,Surface Heat Storage Rate [W]
-
-* Zone,Average,Surface Heat Storage Gain Rate [W]
-
-* Zone,Average,Surface Heat Storage Loss Rate [W]
-
-* Zone,Average,Surface Heat Storage Rate per Area [W/m2]
-
-* Zone,Sum,Surface Heat Storage Energy [J]
-
-* Zone,Average,Surface Internal Source Location Temperature [C]
-
-* Zone,Average,Zone Opaque Surface Inside Face Conduction [W]
-
-* Zone,Average,Zone Opaque Surface Inside Faces Total Conduction Heat Gain Rate [W]
-
-* Zone,Average,Zone Opaque Surface Inside Faces Total Conduction Heat Loss Rate [W]
-
-* Zone,Sum,Zone Opaque Surface Inside Faces Total Conduction Heat Gain Energy [J]
-
-* Zone,Sum,Zone Opaque Surface Inside Faces Total Conduction Heat Loss Energy [J]
-
-* Zone,Average,Zone Opaque Surface Outside Face Conduction [W]
-
-* Zone,Average,Zone Opaque Surface Outside Face Conduction Gain[W]
-
-* Zone,Average,Zone Opaque Surface Outside Face Conduction Loss[W]
-
-* Zone,Average, Surface Inside Face Beam Solar Radiation Heat Gain Rate [W]
-
-### Window Output Variables
-
-Output variables applicable only to exterior windows and glass doors:
-
-* Zone,Average,Zone Windows Total Transmitted Solar Radiation Rate [W]
-
-* Zone,Sum,Zone Transmitted Solar Energy [J]
-
-* Zone,Average,Zone Windows Total Heat Gain Rate [W]
-
-* Zone,Sum,Zone Windows Total Heat Gain Energy [J]
-
-* Zone,Average,Zone Windows Total Heat Loss Rate [W]
-
-* Zone,Sum,Zone Windows Total Heat Loss Energy [J]
-
-* Zone,Average,Zone Exterior Windows Total Transmitted Beam Solar Radiation Rate [W]
-
-* Zone,Sum,Zone Exterior Windows Total Transmitted Beam Solar Radiation Energy [J]
-
-* Zone,Average,Zone Interior Windows Total Transmitted Beam Solar Radiation Rate [W]
-
-* Zone,Sum,Zone Interior Windows Total Transmitted Beam Solar Radiation Energy [J]
-
-* Zone,Average,Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Rate [W]
-
-* Zone,Sum,Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Energy [J]
-
-* Zone,Average,Zone Interior Windows Total Transmitted Diffuse Solar Radiation Rate [W]
-
-* Zone,Average,Surface Window Total Glazing Layers Absorbed Solar Radiation Rate [W]
-
-* Zone,Average,Surface Window Total Glazing Layers Absorbed Shortwave Radiation Rate [W]
-
-* Zone,Sum,Surface Window Total Glazing Layers Absorbed Solar Radiation Energy [J]
-
-* Zone,Average,Surface Window Shading Device Absorbed Solar Radiation Rate [W]
-
-* Zone,Sum,Surface Window Shading Device Absorbed Solar Radiation Energy [J]
-
-* Zone,Average, Surface Window Transmitted Solar Radiation Rate [W]
-
-* Zone,Sum,Surface Window Transmitted Solar Radiation Energy [J]
-
-* Zone,Average,Surface Window Transmitted Beam Solar Radiation Rate [W]
-
-* Zone,Average,Surface Window Transmitted Beam To Beam Solar Radiation Rate [W]
-
-* Zone,Average,Surface Window Transmitted Beam To Diffuse Solar Radiation Rate [W]
-
-* Zone,Sum,Surface Window Transmitted Beam Solar Radiation Energy [J]
-
-* Zone,Sum,Surface Window Transmitted Beam To Beam Solar Radiation Energy [J]
-
-* Zone,Sum,Surface Window Transmitted Beam To Diffuse Solar Radiation Energy [J]
-
-* Zone,Average,Surface Window Transmitted Diffuse Solar Radiation Rate [W]
-
-* Zone,Sum,Surface Window Transmitted Diffuse Solar Radiation Energy [J]
-
-* Zone,Average,Surface Window System Solar Transmittance []
-
-* Zone,Average,Surface Window System Solar Absorptance []
-
-* Zone,Average,Surface Window System Solar Reflectance []
-
-* Zone,Average,Surface Window Gap Convective Heat Transfer Rate [W]
-
-* Zone,Sum,Surface Window Gap Convective Heat Transfer Energy [J]
-
-* Zone,Average,Surface Window Heat Gain Rate [W]
-
-* Zone,Sum,Surface Window Heat Gain Energy [J]
-
-* Zone,Average,Surface Window Heat Loss Rate [W]
-
-* Zone,Sum,Surface Window Heat Loss Energy [J]
-
-* Zone,Average,Surface Window Glazing Beam to Beam Solar Transmittance[]
-
-* Zone,Average,Surface Window Glazing Beam to Diffuse Solar Transmittance []
-
-* Zone,Average,Surface Window Glazing Diffuse to Diffuse Solar Transmittance[]
-
-* Zone,Average,Surface Window Model Solver Iteration Count []
-
-* Zone,Average,Surface Window Solar Horizontal Profile Angle[deg]
-
-* Zone,Average,Surface Window Solar Vertical Profile Angle[deg]
-
-* Zone,Average,Surface Window Outside Reveal Reflected Beam Solar Radiation Rate [W]
-
-* Zone,Sum,Surface Window Outside Reveal Reflected Beam Solar Radiation Energy
-
-* Zone,Average,Surface Window Inside Reveal Reflected Beam Solar Radiation Rate [W]
-
-* Zone,Sum,Surface Window Inside Reveal Reflected Beam Solar Radiation Energy [J]
-
-* Zone,Average,Surface Window Inside Reveal Absorbed Beam Solar Radiation Rate [W]
-
-* Zone,Average,Surface Window Inside Face Glazing Condensation Status []
-
-* Zone,Average,Surface Window Inside Face Frame Condensation Status []
-
-* Zone,Average,Surface Window Inside Face Divider Condensation Status []
-
-* Zone,Average,Surface Shading Device Is On Time Fraction[]
-
-* Zone,Average,Surface Window Blind Slat Angle [deg]
-
-* Zone,Average,Surface Window Blind Beam to Beam Solar Transmittance[]
-
-* Zone,Average,Surface Window Blind Beam to Diffuse Solar Transmittance[]
-
-* Zone,Average,Surface Window Blind Diffuse to Diffuse Solar Transmittance[]
-
-* Zone,Average,Surface Window Blind and Glazing System Beam Solar Transmittance[]
-
-* Zone,Average,Surface Window Blind and Glazing System Diffuse Solar Transmittance[]
-
-* Zone,Average,Surface Window Screen Beam to Beam Solar Transmittance []
-
-* Zone,Average,Surface Window Screen Beam to Diffuse Solar Transmittance []
-
-* Zone,Average,Surface Window Screen Diffuse to Diffuse Solar Transmittance []
-
-* Zone,Average,Surface Window Screen and Glazing System Beam Solar Transmittance []
-
-* Zone,Average,Surface Window Screen and Glazing System Diffuse Solar Transmittance []
-
-* Zone,State,Surface Storm Window On Off Status []
-
-* Zone,Average,Surface Window Inside Face Frame and Divider Zone Heat Gain Rate [W]
-
-* Zone,Average,Surface Window Frame Heat Gain Rate [W]
-
-* Zone,Average,Surface Window Frame Heat Loss Rate [W]
-
-* Zone,Average,Surface Window Divider Heat Gain Rate [W]
-
-* Zone,Average,Surface Window Divider Heat Loss Rate [W]
-
-* Zone,Average,Surface Window Frame Inside Temperature [C]
-
-* Zone,Average,Surface Window Frame Outside Temperature [C]
-
-* Zone,Average,Surface Window Divider Inside Temperature [C]
-
-* Zone,Average,Surface Window Divider Outside Temperature [C]
-
-If the user requests to display advanced report/output variables (e.g. see Output:Diagnostics keyword DisplayAdvancedReportVariables) the the following additional output variables are available for exterior windows and glass doors
-
-* Zone,Average,Surface Window Inside Face Glazing Zone Convection Heat Gain Rate [W]
-
-* Zone,Average,Surface Window Inside Face Glazing Net Infrared Heat Transfer Rate [W]
-
-* Zone,Average,Surface Window Shortwave from Zone Back Out Window Heat Transfer Rate [W]
-
-* Zone,Average,Surface Window Inside Face Frame and Divider Zone Heat Gain Rate [W]
-
-* Zone,Average,Surface Window Inside Face Gap between Shade and Glazing Zone Convection Heat Gain Rate [W]
-
-* Zone,Average,Surface Window Inside Face Shade Zone Convection Heat Gain Rate [W]
-
-* Zone,Average,Surface Window Inside Face Shade Net Infrared Heat Transfer Rate [W]
-
-Output variables applicable only to interior windows and glass doors:
-
-* Zone,Average, Surface Window Transmitted Beam Solar Radiation Rate [W]
-
-* Zone,Sum,Surface Window Transmitted Beam Solar Radiation Energy [J]
-
-If the user requests to display advanced report/output variables (e.g. see Output:Diagnostics keyword DisplayAdvancedReportVariables) the the following additional output variable is available for Equivalent Layer Window;
-
-* Zone,Average, Surface Window Inside Face Other Convection Heat Gain Rate [W]
-
-* Output variables applicable to interior and exterior windows and doors are:
-
-* Zone,Average,Surface Window Total Absorbed Shortwave Radiation Rate Layer &lt;x&gt; [W]
-
-* Zone,Average,Surface Window Front Face Temperature Layer &lt;x&gt; [C]
-
-* Zone,Average,Surface Window Back Face Temperature Layer &lt;x&gt; [C]
-
-#### Surface Window Total Absorbed Shortwave Radiation Rate Layer &lt;x&gt; [W]
-
-This will output shortwave radiation absorbed in a window layer. The key values for this output variable are the surface name. Layers are numbered from the outside to the inside of the surface. The full listing will appear in the RDD file.
-
-#### Surface Window Front Face Temperature Layer &lt;x&gt; [C]
-
-This will output a temperature for the front face of the layer. The layer front face is considered to be the face closest to the outside environment. The full listing will appear in the RDD file.
-
-#### Surface Window Back Face Temperature Layer &lt;x&gt; [C]
-
-This will output a temperature for the back face of the layer. The layer back face is considered to be the face closest to the inside environment. The full listing will appear in the RDD file.
-
-### Surface Output Variables (all heat transfer surfaces)
-
-The various output variables related to surface heat transfer are organized around the inside and outside face of each surface.  The zone heat balance model draws energy balances at each side, or face, of a surface and so each surface essentially has two sets of results. The inside face is the side of a heat transfer surface that faces toward the thermal zone. The outside face is the side of a heat transfer surface that faces away from the thermal zone, typically facing outdoors.  The Key Value for these is generally the user-defined name of the surface.
-
-#### Surface Inside Face Heat Balance Calculation Iteration Count []
-
-This output is the number of iterations used in a part of the solution for surface heat transfer that accounts for thermal radiation heat transfer between zone surfaces.  This is simply a counter on the iteration loop for inside face surface modeling.  There is only one instance of this output in a given run and the Key Value is “Simulation.�
-
-#### Surface Inside Face Temperature [C]
-
-This is the temperature of the surface’s inside face, in degrees Celsius.  Former Name: Prior to version 7.1 this output was called Surface Inside Temperature.
-
-#### Surface Outside Face Temperature [C]
-
-This is the temperature of the surface’s outside face, in degrees Celsius.  Former Name: Prior to version 7.1, this output was called Surface Outside Temperature.
-
-#### Surface Inside Face Adjacent Air Temperature [C]
-
-This is the effective bulk air temperature used for modeling the inside surface convection heat transfer. This is the same as the zone mean air temperature when using the mixing model for roomair. However, if more advanced roomair models are used, this variable will report the air temperature predicted by the roomair model as it was used in the surface heat balance model calculations. Former Name: Prior to version 7.1, this output was called Surface Int Adjacent Air Temperature.
-
-#### Surface Inside Face Convection Heat Gain Rate [W]
-
-#### Surface Inside Face Convection Heat Gain Rate per Area [W/m2]
-
-#### Surface Inside Face Convection Heat Gain Energy [J]
-
-These “inside face convection heat gain� output variables describe the heat transferred by convection between the inside face and the zone air.  The values can be positive or negative with positive indicating heat is being added to the surface’s face by convection.  Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
-
-Former Name: Prior to version 7.1, these outputs were called “Surface Int Convection Heat \* � and had used the opposite sign convention.
-
-#### Surface Inside Face Convection Heat Transfer Coefficient [W/m2-K]
-
-This is the coefficient that describes the convection heat transfer. It is the value of “Hc� in the classic convection model Q = Hc\* A\* (T – T).  This is the result of the surface convection algorithm used for the inside face. Former Name: Prior to version 7.1, this output was called “Surface Int Convection Coeff.�
-
-#### Surface Inside Face Net Surface Thermal Radiation Heat Gain Rate [W]
-
-#### Surface Inside Face Net Surface Thermal Radiation Heat Gain Rate per Area [W/m2]
-
-#### Surface Inside Face Net Surface Thermal Radiation Heat Gain Energy [J]
-
-These “inside face net surface thermal radiation heat gain� output variables describe the heat transferred by longwave infrared thermal radiation exchanges between the inside faces of other surfaces in the zone. The values can be positive or negative with positive indicating heat is being added to the surface’s face by thermal radiation.  Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
-
-#### Surface Inside Face Solar Radiation Heat Gain Rate [W]
-
-#### Surface Inside Face Solar Radiation Heat Gain Rate per Area [W/m2]
-
-#### Surface Inside Face Solar Radiation Heat Gain Energy [J]
-
-These “inside face solar radiation heat gain� output variables describe the heat transferred by solar radiation onto the inside face. The values are always positive and indicate heat is being added to the surface’s face by solar radiation.  This is sunlight that has entered the zone through a window and been absorbed on the inside face of the surface.  Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
-
-#### Surface Inside Face Lights Radiation Heat Gain Rate [W]
-
-#### Surface Inside Face Lights Radiation Heat Gain Rate per Area [W/m2]
-
-#### Surface Inside Face Lights Radiation Heat Gain Energy [J]
-
-These “inside face lights radiation heat gain� output variables describe the heat transferred by shortwave radiation onto the inside face. The values are always positive and indicate heat is being added to the surface’s face by shortwave radiation that emanated from electric lighting equipment and was absorbed by the surface.  Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
-
-#### Surface Inside Face Internal Gains Radiation Heat Gain Rate [W]
-
-#### Surface Inside Face Internal Gains Radiation Heat Gain Rate per Area [W/m2]
-
-#### Surface Inside Face Internal Gains Radiation Heat Gain Energy [J]
-
-These “inside face internal gains radiation heat gain� output variables describe the heat transferred by longwave infrared thermal radiation onto the inside face that emanated from internal gains such as lights, electric equipment, and people.  The values are always positive and indicate heat is being added to the surface’s face by the absorption of longwave thermal radiation.  Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
-
-#### Surface Inside Face System Radiation Heat Gain Rate [W]
-
-#### Surface Inside Face System Radiation Heat Gain Rate per Area [W/m2]
-
-#### Surface Inside Face System Radiation Heat Gain Energy [J]
-
-These “inside face system radiation heat gain� output variables describe the heat transferred by infrared thermal radiation onto the inside face that emanated from HVAC equipment such as baseboard heaters or high-temperature radiant heating panels.  The values are always positive and indicate heat is being added to the surface’s face by the absorption of thermal radiation.  Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
-
-#### Surface Outside Face Convection Heat Gain Rate [W]
-
-#### Surface Outside Face Convection Heat Gain Rate per Area [W/m2]
-
-#### Surface Outside Face Convection Heat Gain Energy [J]
-
-These “outside face convection� output variables describe heat transferred by convection between the outside face and the surrounding air.  The values can be positive or negative with positive values indicating heat is added to the surface face by convection heat transfer. Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m<sup>2</sup>), and an energy version (J).
-
-Former Name: Prior to version 7.1, these outputs were called “Surface Ext Convection Heat \*� and used the opposite sign convention.
-
-#### Surface Outside Face Convection Heat Transfer Coefficient [W/m2-K]
-
-This is the coefficient that describes the convection heat transfer. It is the value of “Hc� in the classic convection model Q = Hc\* A\* (T – T).  This is the result of the surface convection algorithm used for the outside face. Former Name: Prior to Version 7.1, this output was called “Surface Ext Convection Coeff.�
-
-#### Surface Outside Face Net Thermal Radiation Heat Gain Rate [W]
-
-#### Surface Outside Face Net Thermal Radiation Heat Gain Rate per Area [W/m2]
-
-#### Surface Outside Face Net Thermal Radiation Heat Gain Energy [J]
-
-These “outside face net thermal radiation� output variables describe the heat transferred by longwave infrared thermal radiation exchanges between the surface and the surroundings of the outside face.  This is the net of all forms of longwave thermal infrared radiation heat transfer. The values can be positive or negative with positive indicating the net addition of heat to the outside face. Different versions of the report are available including the basic heat gain rate (W), and a per unit area flux (W/m2), and an energy version (J).
-
-Former Name: Prior to version 7.1, these outputs were called “Surface Ext Thermal Radiation Heat \*� and used the opposite sign convention.
-
-#### Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate [W]
-
-#### Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate per Area [W/m2]
-
-#### Surface Inside Face Exterior Windows Incident Beam Solar Radiation Energy [J]
-
-Beam solar radiation from the exterior windows in a zone incident on the inside face of a surface in the zone. If Solar Distribution in the BUILDING object is equal to MinimalShadowing or FullExterior, it is assumed that all beam solar from exterior windows falls on the floor. In this case the value of this output variable can be greater than zero only for floor surfaces. If Solar Distribution equals FullInteriorExterior the program tracks where beam solar from exterior windows falls inside the zone, in which case the value of this variable can be greater than zero for floor as well as wall surfaces. Different versions of the report are available including the basic incident rate (W), a per unit area flux (W/m2), and an energy version (J).
-
-#### 
-
-#### Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate [W]
-
-#### Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate per Area [W/m2]
-
-#### Surface Inside Face Interior Windows Incident Beam Solar Radiation Energy [J]
-
-Beam solar radiation from the interior (i.e., interzone) windows in a zone incident on the inside face of a surface in the zone. This value is calculated only if Solar Distribution in the BUILDING object is equal to FullInteriorExterior. However, the program does not track where this radiation falls. Instead, it is treated by the program as though it were diffuse radiation uniformly distributed over all of the zone surfaces. See **Figure 31**. Different versions of the report are available including the basic incident rate (W), a per unit area flux (W/m2), and an energy version (J).
-
-![](media/image057.svg)
-
-Figure 31. Beam solar radiation entering a zone through an interior window is distributed inside the zone as though it were diffuse radiation.
-
-#### Surface Inside Face Initial Transmitted Diffuse Absorbed Solar Radiation Rate [W]
-
-As of Version 2.1, diffuse solar transmitted through exterior and interior windows is no longer uniformly distributed.  Instead, it is distributed according to the approximate view factors between the transmitting window and all other heat transfer surfaces in the zone.  This variable is the amount of transmitted diffuse solar that is initially absorbed on the inside of each heat transfer surface.  The portion of this diffuse solar that is reflected by all surfaces in the zone is subsequently redistributed uniformly to all heat transfer surfaces in the zone, along with interior reflected beam solar and shortwave radiation from lights.  The total absorbed shortwave radiation is given by the next variable.
-
-#### Surface Inside Face Absorbed Shortwave Radiation Rate [W]
-
-As of Version 2.1, the previous variable plus absorbed shortwave radiation from uniformly distributed initially-reflected diffuse solar, reflected beam solar, and shortwave radiation from lights. This sum is the power of all sources of solar and visible radiation absorbed by the surface at the inside face.
-
-### Surface Output Variables (exterior heat transfer surfaces)
-
-#### Surface Outside Face Outdoor Air Drybulb Temperature [C]
-
-The outdoor air dry-bulb temperature calculated at the height above ground of the surface centroid. Former Name: Prior to version 7.1, this output was called “Surface Ext Outdoor Dry Bulb.�
-
-#### Surface Outside Face Outdoor Air Wetbulb Temperature [C]
-
-The outdoor air wet-bulb temperature calculated at the height above ground of the surface centroid. Former Name: Prior to version 7.1, this output was called “Surface Ext Outdoor Wet Bulb.�
-
-#### Surface Outside Face Outdoor Air Wind Speed [m/s]
-
-The outdoor wind speed calculated at the height above ground of the surface centroid. Former Name: Prior to version 7.1, this output was called “Surface Ext Wind Speed.�
-
-#### Surface Outside Face Sunlit Area [m2]
-
-The outside area of an exterior surface that is illuminated by (unreflected) beam solar radiation.
-
-#### Surface Outside Face Sunlit Fraction []
-
-The fraction of the outside area of an exterior surface that is illuminated by (unreflected) beam solar radiation. Equals Surface Outside Face Sunlit Area divided by total surface area.
-
-#### Surface Outside Face Thermal Radiation to Air Heat Transfer Coefficient [W/m2-K]
-
-This is the coefficient that describes thermal radiation heat transfer between the outside face and the air mass surrounding the surface.  It is the value of “Hr� in the classic linearized model for thermal radiation Q = Hr \* A \* (T_surf – T_surfodb) when applied to the ambient air. Where T_surf = Surface Outside Face Temperature, and T_surfodb = Surface Outside Face Outdoor Air Drybulb Temperature. Former Name: Prior to version 7.1, this output was called “Surface Ext Rad to Air Coeff.�
-
-#### Surface Outside Face Thermal Radiation to Sky Heat Transfer Coefficient [W/m2-K]
-
-This is the coefficient that describes thermal radiation heat transfer between the outside face and the sky surrounding the surface.  It is the value of “Hr� in the classic linearized model for thermal radiation Q = Hr \* A \* (T_surf – T_sky) when applied to the sky. Where T_surf = Surface Outside Face Temperature, and T_sky = Site Sky Temperature. Former Name: Prior to version 7.1, this output was called “Surface Ext Rad to Sky Coeff.�
-
-#### Surface Outside Face Thermal Radiation to Ground Heat Transfer Coefficient [W/m2-K]
-
-This is the coefficient that describes thermal radiation heat transfer between the outside face and the ground surrounding the surface.  It is the value of “Hr� in the classic linearized model for thermal radiation Q = Hr \* A \* (T_surf – T_odb) when applied to the ground. Where T_surf = Surface Outside Face Temperature, and T_odb = Site Outdoor Air Drybulb Temperature (used as an approximation for the ground surface temperature). Former Name: Prior to version 7.1, this output was called “Surface Ext Rad to Ground Coeff.�
-
-#### Surface Outside Face Solar Radiation Heat Gain Rate [W]
-
-#### Surface Outside Face Solar Radiation Heat Gain Rate per Area [W/m2]
-
-#### Surface Outside Face Solar Radiation Heat Gain Energy [J]
-
-These “outside face solar radiation� output variables describe the heat transferred by the absorption of solar radiation at the outside face.  This is the result of incident solar radiation being absorbed at the surface face.  The values are always positive.
-
-#### Surface Outside Face Incident Solar Radiation Rate per Area [W/m2]
-
-The total solar radiation incident on the outside of an exterior surface. It is the sum of:
-
-* Surface Outside Face Incident Beam Solar Radiation Rate per Area
-
-* Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area
-
-* Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area
-
-* Surface Outside Face Incident Sky Diffuse Surface Reflected Solar Radiation Rate per Area
-
-* Surface Outside Face Incident Beam To Beam Surface Reflected Solar Radiation Rate per Area
-
-* Surface Outside Face Incident Sky Diffuse Surface Reflected Solar Radiation Rate per Area
-
-#### Surface Outside Face Incident Beam Solar Radiation Rate per Area [W/m2]
-
-The solar beam radiation incident on the outside of an exterior surface, including the effects of shadowing, if present. The beam here is that directly from the sun; it excludes beam specularly reflected from obstructions.
-
-#### Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area [W/m2]
-
-The solar diffuse radiation from the sky incident on the outside of an exterior surface, including the effects of shadowing, if present.
-
-#### Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area  [W/m2]
-
-The solar diffuse radiation incident on the outside of an exterior surface that arises from reflection of beam solar and sky diffuse solar from the ground. This is the sum of the next two output variables, “Surface Outside Face Incident Beam To Diffuse Ground Reflected Solar Radiation Rate per Area� and “Surface Outside Face Incident Sky Diffuse Ground Reflected Solar Radiation Rate per Area.� The reflected solar radiation from the ground is assumed to be diffuse and isotropic (there is no specular component).
-
-If “Reflections� option is not chosen in the Solar Distribution Field in the BUILDING object, the effects of shadowing are accounted for by the user-specified value of View Factor to Ground for the surface. If “Reflections� option is chosen, the program determines the effects of shadowing, including time-varying shadowing of the ground plane by the building itself.
-
-#### Surface Outside Face Incident Beam To Diffuse Ground Reflected Solar Radiation Rate per Area [W/m2]
-
-The solar diffuse radiation incident on the outside of an exterior surface that arises from beam-to-diffuse reflection from the ground. It is assumed that there is no beam-to-beam (specular) component. The beam here is that directly from the sun; it excludes beam specularly reflected from obstructions.
-
-#### Surface Outside Face Incident Sky Diffuse Ground Reflected Solar Radiation Rate per Area [W/m2]
-
-The solar diffuse radiation incident on the outside of an exterior surface that arises from sky diffuse solar reflection from the ground. The sky diffuse here is that directly from the sky; it excludes reflection of sky diffuse from obstructions.
-
-#### Surface Outside Face Incident Sky Diffuse Surface Reflected Solar Radiation Rate per Area [W/m2]
-
-The solar diffuse radiation incident on the outside of an exterior surface that arises from sky diffuse reflection from one or more obstructions. This value will be non-zero only if “Reflections� option is chosen in the BUILDING object.
-
-#### Surface Outside Face Incident Beam To Beam Surface Reflected Solar Radiation Rate per Area [W/m2]
-
-The solar beam radiation incident on the outside of an exterior surface that arises from beam-to-beam (specular) reflection from one or more obstructions. This value will be non-zero only if “Reflections� option is chosen in the BUILDING object. For windows, the program treats this beam radiation as diffuse radiation in calculating its transmission and absorption.
-
-#### Surface Outside Face Incident Beam To Diffuse Surface Reflected Solar Radiation Rate per Area [W/m2]
-
-The solar diffuse radiation incident on the outside of an exterior surface that arises from beam-to-diffuse reflection from building shades or building surfaces. This value will be non-zero only if  “Reflections� option is chosen in the BUILDING object.
-
-#### Surface Outside Face Beam Solar Incident Angle Cosine Value []
-
-The cosine of the angle of incidence of (unreflected) beam solar radiation on the outside of an exterior surface. The value varies from 0.0 for beam parallel to the surface (incidence angle = 90<sup>O</sup>) to 1.0 for beam perpendicular to the surface (incidence angle = 0<sup>O</sup>). Negative values indicate the sun is behind the surface, i.e the surface does not see the sun.
-
-#### Surface Anisotropic Sky Multiplier []
-
-This is the view factor multiplier for diffuse sky irradiance on exterior surfaces taking into account the anisotropic radiance of the sky. The diffuse sky irradiance on a surface is given by Anisotropic Sky Multiplier \* Diffuse Solar Irradiance.
-
-#### Surface Window BSDF Beam Direction Number []
-
-#### Surface Window BSDF Beam Phi Angle [rad]
-
-#### Surface Window BSDF Beam Theta Angle [rad]
-
-### Opaque Surface Output Variables
-
-The following variables apply only to opaque surfaces, where an opaque surface is considered here to be an exterior or interzone heat transfer surface of class FLOOR, WALL, ROOF or DOOR. **Note – these are advanced variables – you must read the descriptions and understand before use – then you must use the** **Output:Diagnostics** **object to allow reporting.**
-
-#### Surface Inside Face Conduction Heat Transfer Rate [W]
-
-#### Surface Inside Face Conduction Heat Transfer Rate per Area [W/m2]
-
-#### Surface Inside Face Conduction Heat Gain Rate [W]
-
-#### Surface Inside Face Conduction Heat Loss Rate [W]
-
-These “inside face conduction� output variables describe heat flow by conduction right at the inside face of an opaque heat transfer surface. A positive value means that the conduction is from just inside the inside face toward the inside face. A negative value means that the conduction is from the inside face into the core of the heat transfer surface.
-
-Note that Inside Face Conduction, when positive, does **not** indicate the heat flow from the surface to the zone air, which is governed by the inside face convection coefficient and the difference in temperature between the inside face and the zone air.
-
-Different versions of the reports are available.  The basic heat gain rate (W) and a per unit area flux (W/m<sup>2</sup>) can have positive or negative values with the sign convention that positive indicates heat flowing toward the face itself.  There are also directed “gain� and “loss� versions that have only positive values or zero when the heat flow direction opposes.
-
-Former Name: Prior to version 7.1, these outputs were called “Opaque Surface Inside Face Conduction \*.�
-
-Former Name: For Conduction Finite Difference simulations (CondFD), CondFD Inside Surface Heat Flux is replaced with Surface Inside Face Conduction Heat Transfer Rate Per Area. Likewise for CondFD Inside Heat Flux to Surface.
-
-#### Surface Outside Face Conduction Heat Transfer Rate [W]
-
-#### Surface Outside Face Conduction Heat Transfer Rate per Area [W/m2]
-
-#### Surface Outside Face Conduction Heat Gain Rate [W]
-
-#### Surface Outside Face Conduction Heat Loss Rate [W]
-
-These “outside face conduction� output variables describe heat flow by conduction right at the outside face of an opaque heat transfer surface. A positive value means that the conduction is from just inside the outside face toward the outside face. A negative value means that the conduction is from the outside face into the core of the heat transfer surface.
-
-Note that outside face conduction, when positive, does **not** indicate the heat flow from the surface to the surrounding air, which is governed by the outside face convection coefficient and the difference in temperature between the inside face and the surrounding air.
-
-Different versions of the reports are available.  The basic heat transfer rate (W) and a per unit area flux (W/m<sup>2</sup>) can have positive or negative values with the sign convention that positive indicates heat flowing toward the face itself.  There are also directed “gain� and “loss� versions that have only positive values or zero when the heat flow direction opposes.
-
-Former Name: For Conduction Finite Difference simulations (CondFD), CondFD Outside Surface Heat Flux is replaced with Surface Outside Face Conduction Heat Transfer Rate Per Area. Likewise for CondFD Outside Heat Flux to Surface.
-
-#### Surface Average Face Conduction Heat Transfer Rate [W]
-
-#### Surface Average Face Conduction Heat Transfer Rate per Area [W/m2]
-
-#### Surface Average Face Conduction Heat Gain Rate [W]
-
-#### Surface Average Face Conduction Heat Loss Rate [W]
-
-#### Surface Average Face Conduction Heat Transfer Energy [J]
-
-These “average face conduction� output variables combine the inside face conduction and outside face conduction reports together to describe the conduction situation in a heat transfer surface in a nominal way.  This is simply the average of the inside and outside face conduction rates, but with the sign convention for the outside face switched to match the inside face so that positive values here indicate heat flowing into the thermal zone.
-
-Different versions of the reports are available.  The basic heat conduction rate (W) and a per unit area flux (W/m<sup>2</sup>) can have positive or negative values with the sign convention that positive indicates heat flowing toward the thermal zone.  There are also directed “gain� and “loss� versions that have only positive values or zero when the heat flow direction opposes (W). Finally there is a version for total energy transfer (J).
-
-#### Surface Heat Storage Rate [W]
-
-#### Surface Heat Storage Rate per Area [W/m2]
-
-#### Surface Heat Storage Gain Rate [W]
-
-#### Surface Heat Storage Loss Rate [W]
-
-#### Surface Heat Storage Energy [J]
-
-These “heat storage� output variables combine the inside face conduction and outside face conduction reports together to describe the thermal storage situation in a heat transfer surface in a nominal way.  This is simply the difference between the inside and outside face conduction, but with the sign convention arranged so that positive values indicate heat being added to the core of the surface.
-
-Different versions of the reports are available.  The basic heat storage rate (W) and a per unit area flux (W/m<sup>2</sup>) can have positive or negative values with the sign convention that positive indicates heat being added to the surface’s mass.  There are also directed “gain� and “loss� versions that have only positive values or zero when the heat storage direction opposes (W). Finally there is a version for total energy stored (J).
-
-#### Surface Internal Source Location Temperature [C]
-
-When a surface has an internal source or sink (defined using Construction:InternalSource) then this output is available for the temperature within the surface at the location of the source/sink.
-
-#### Zone Opaque Surface Inside Face Conduction [W]
-
-The sum of the Opaque Surface Inside Face Conduction values for all opaque surfaces in a zone for both positive and negative sums. For example, assume a zone has six opaque surfaces with Opaque Surface Inside Face Conduction values of 100, -200, 400, 50, 150 and –300 W. Then Zone Opaque Surface Inside Face Conduction = 700 - 500 = 200 W.  Or if a zone has six opaque surfaces with Opaque Surface Inside Face Conduction values of -100, -200, 400, -50, 150 and –300W. Then Zone Opaque Surface Inside Face Conduction = 550 – 650 = -100 W.
-
-#### Zone Opaque Surface Inside Faces Total Conduction Heat Gain Rate [W]
-
-#### Zone Opaque Surface Inside Faces Total Conduction Heat Gain Energy [J]
-
-These are the power and energy sums for the Opaque Surface Inside Face Conduction values for all opaque surfaces in a zone when that sum is positive. For example, assume a zone has six opaque surfaces with Opaque Surface Inside Face Conduction values of 100, -200, 400, 50, 150 and –300 W. Then Zone Opaque Surface Inside Faces Total Conduction Heat Gain Rate = 700 - 500 = 200 W.
-
-#### Zone Opaque Surface Inside Faces Total Conduction Heat Loss Rate [W]
-
-#### Zone Opaque Surface Inside Faces Total Conduction Heat Loss Energy [J]
-
-These are the power and energy absolute value for the sums of the Opaque Surface Inside Face Conduction values for all opaque surfaces in a zone when that sum is negative. For example, assume a zone has six opaque surfaces with Opaque Surface Inside Face Conduction values of -100, -200, 400,
-  -50, 150 and –300W. Then Zone Opaque Surface Inside Faces Total Conduction Heat Loss Rate = |550 – 650| = |-100| = 100 W.
-
-#### Zone Opaque Surface Outside Face Conduction [W]
-
-The sum of the Opaque Surface Outside Face Conduction values for all opaque surfaces in a zone for both positive and negative sums. For example, assume a zone has six opaque surfaces with Opaque Surface Outside Face Conduction values of 100, -200, 400, 50, 150 and –300 W. Then Zone Opaque Surface Outside Face Conduction = 700 - 500 = 200 W.  Or if a zone has six opaque surfaces with Opaque Surface Outside Face Conduction values of -100, -200, 400, -50, 150 and –300W. Then Zone Opaque Surface Outside Face Conduction = 550 – 650 = -100 W.
-
-#### Zone Opaque Surface Outside Face Conduction Gain [W]
-
-#### Zone Opaque Surface Outside Face Conduction Gain Energy [J]
-
-These are the power and energy sums for the Opaque Surface Outside Face Conduction values for all opaque surfaces in a zone when that sum is positive. For example, assume a zone has six opaque surfaces with Opaque Surface Outside Face Conduction values of 100, -200, 400, 50, 150 and –300 W. Then Zone Opaque Surface Outside Face Conduction Gain = 700 - 500 = 200 W.
-
-#### Zone Opaque Surface Outside Face Conduction Loss [W]
-
-#### Zone Opaque Surface Outside Face Conduction Loss Energy [J]
-
-These are the power and energy absolute value for the sums of the Opaque Surface Outside Face Conduction values for all opaque surfaces in a zone when that sum is negative. For example, assume a zone has six opaque surfaces with Opaque Surface Outside Face Conduction values of -100, -200, 400,
-  -50, 150 and –300W. Then Zone Opaque Surface Outside Face Conduction Loss = |550 – 650| = |-100| = 100 W.
-
-#### Surface Inside Face Beam Solar Radiation Heat Gain Rate [W]
-
-Beam solar radiation from exterior windows absorbed on the inside face of an opaque heat transfer surface. For Solar Distribution = FullInteriorAndExterior, this quantity can be non-zero for both floor and wall surfaces. Otherwise, for Solar Distribution = FullExterior or MinimalShadowing, it can be non-zero only for floor surfaces since in this case all entering beam solar is assumed to fall on the floor. Note that this variable will not be operational (have a real value) unless there are exterior windows in the zone.
-
-### Window Output Variables
-
-The following output variables apply to subsurfaces that are windows or glass doors. These two subsurface types are called “window� here. “Exterior window� means that the base surface of the window is an exterior wall, floor, roof or ceiling (i.e., the base surface is a BuildingSurface:Detailed with OutsideFaceEnvironment = ExteriorEnvironment). “Interior window� means that the base surface of the window is an inter-zone wall, floor or ceiling. “Glass� means a transparent solid layer, usually glass, but possibly plastic or other transparent material. “Shading device� means an interior, exterior or between-glass shade or blind, or an exterior screen (only exterior windows can have a shading device).
-
-#### Zone Windows Total Transmitted Solar Radiation Rate [W]
-
-#### Zone Windows Total Transmitted Solar Radiation Energy [J]
-
-The total Surface Window Transmitted Solar Radiation Rate of all the exterior windows in a zone.
-
-#### Zone Windows Total Heat Gain Rate [W]
-
-#### Zone Windows Total Heat Gain Energy [J]
-
-The sum of the heat flow from all of the exterior windows in a zone when that sum is positive. (See definition of “heat flow� under “Window Heat Gain,� below.)
-
-#### Zone Windows Total Heat Loss Rate [W]
-
-#### Zone Windows Total Heat Loss Energy [J]
-
-The absolute value of the sum of the heat flow from all of the exterior windows in a zone when that sum is negative.
-
-#### Surface Window Total Glazing Layers Absorbed Shortwave Radiation Rate [W]
-
-#### Surface Window Total Glazing Layers Absorbed Solar Radiation Rate [W]
-
-#### Surface Window Total Glazing Layers Absorbed Solar Radiation Energy  [J]
-
-The total exterior beam and diffuse solar radiation absorbed in all of the glass layers of an exterior window.
-
-#### Surface Window Shading Device Absorbed Solar Radiation Rate [W]
-
-Surface Window Shading Device Absorbed Solar Radiation Energy [J]
-
-The exterior beam and diffuse solar radiation absorbed in the shading device, if present, of an exterior window.
-
-#### Surface Window Transmitted Solar Radiation Rate [W]
-
-#### Surface Window Transmitted Solar Radiation Energy [J]
-
-The amount of beam and diffuse solar radiation entering a zone through an exterior window. It is the sum of the following two variables, “Surface Window Transmitted Beam Solar Radiation Rate� and “Surface Window Transmitted Diffuse Solar Radiation Rate.�
-
-#### Surface Window Transmitted Beam Solar Radiation Rate [W]
-
-#### Surface Window Transmitted Beam Solar Radiation Energy [J]
-
-The solar radiation transmitted by an exterior window whose source is beam solar incident on the outside of the window. For a bare window, this transmitted radiation consists of beam radiation passing through the glass (assumed transparent) and diffuse radiation from beam reflected from the outside window reveal, if present. For a window with a shade, this transmitted radiation is totally diffuse (shades are assumed to be perfect diffusers). For a window with a blind, this transmitted radiation consists of beam radiation that passes between the slats and diffuse radiation from beam-to-diffuse reflection from the slats. For a window with a screen, this value consists of direct beam radiation that is transmitted through the screen (gaps between the screen material) and diffuse radiation from beam-to-diffuse reflection from the screen material.
-
-For each zone time step,
-
-Surface Window Transmitted Beam Solar Radiation Rate = Surface Window Transmitted Beam To Beam Solar Radiation Rate  + Surface Window Transmitted Beam To Diffuse Solar Radiation Rate
-
-Surface Window Transmitted Beam Solar Radiation Energy = Surface Window Transmitted Beam To Beam Solar Radiation Energy + Surface Window Transmitted Beam To Diffuse Solar Radiation Energy
-
-#### Surface Window Transmitted Beam To Beam Solar Radiation Rate [W]
-
-#### Surface Window Transmitted Beam To Beam Solar Radiation Energy [J]
-
-#### For a window with a blind, this transmitted radiation consists of beam radiation that passes between the slats. For a window with a screen, this value consists of direct beam radiation that is transmitted through the screen (gaps between the screen material).
-
-#### Surface Window Transmitted Beam To Diffuse Solar Radiation Rate [W]
-
-#### Surface Window Transmitted Beam To Diffuse Solar Radiation Energy [J]
-
-#### For a window with a blind, this transmitted radiation consists of diffuse radiation reflected from beam by the slats. For a window with a screen, this value consists of diffuse radiation reflected by the screen material.
-
-#### Zone Exterior Windows Total Transmitted Beam Solar Radiation Rate [W]
-
-#### Zone Exterior Windows Total Transmitted Beam Solar Radiation Energy [J]
-
-The sum of the Surface Window Transmitted Beam Solar Radiation Rate (see definition above) from all exterior windows in a zone.
-
-#### Zone Interior Windows Total Transmitted Beam Solar Radiation Rate [W]
-
-#### Zone Interior Windows Total Transmitted Beam Solar Radiation Energy [J]
-
-The sum of the Surface Window Transmitted Beam Solar Radiation Rate (see definition above) from all interior windows in a zone.
-
-#### Surface Window Transmitted Diffuse Solar Radiation Rate [W]
-
-#### Surface Window Transmitted Diffuse Solar Radiation Energy [J]
-
-The solar radiation transmitted by an exterior window whose source is diffuse solar incident on the outside of the window. For a bare window, this transmitted radiation consists of diffuse radiation passing through the glass. For a window with a shade, this transmitted radiation is totally diffuse (shades are assumed to be perfect diffusers). For a window with a blind, this transmitted radiation consists of diffuse radiation that passes between the slats and diffuse radiation from diffuse-to-diffuse reflection from the slats. For a window with a screen, this value consists of diffuse radiation transmitted through the screen (gaps between the screen material) and diffuse radiation from diffuse-to-diffuse reflection from the screen material.
-
-#### Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Rate [W]
-
-#### Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Energy [J]
-
-The combined beam and diffuse solar that first entered adjacent zones through exterior windows in the adjacent zones, was subsequently reflected from interior surfaces in those zones (becoming diffuse through that reflection), and was then transmitted through interior windows into the current zone.
-
-#### Zone Interior Windows Total Transmitted Diffuse Solar Radiation Rate [W]
-
-#### Zone Interior Windows Total Transmitted Diffuse Solar Radiation Energy [J]
-
-The sum of the Surface Window Transmitted Diffuse Solar Radiation Rate (see definition above) from all interior windows in a zone.
-
-#### Surface Window System Solar Transmittance []
-
-Effective solar transmittance of an exterior window, including effect of shading device, if present. Equal to “Surface Window Transmitted Solar Radiation Rate� divided by total exterior beam plus diffuse solar radiation incident on the window (excluding frame, if present).
-
-#### Surface Window System Solar Absorptance []
-
-Effective solar absorptance of an exterior window, including effect of shading device, if present. Equal to “Window Solar Absorbed: All Glass Layers� plus “Window Solar Absorbed: Shading Device� divided by total exterior beam plus diffuse solar radiation incident on window (excluding frame, if present)
-
-#### Surface Window System Solar Reflectance []
-
-Effective solar reflectance of an exterior window, including effect of shading device, if present. Equal to: [1.0 – “Surface Window System Solar Transmittance� – “Surface Window System Solar Absorptance�].
-
-#### Surface Window Gap Convective Heat Transfer Rate [W]
-
-#### Surface Window Gap Convective Heat Transfer Energy [J]
-
-For an airflow window, the forced convective heat flow from the gap through which airflow occurs. This is the heat gained (or lost) by the air from the glass surfaces (and between-glass shading device surfaces, if present) that the air comes in contact with as it flows through the gap. If the gap airflow goes to the zone indoor air, the gap convective heat flow is added to the zone load. Applicable to exterior windows only.
-
-#### Surface Window Heat Gain Rate [W]
-
-#### Surface Window Heat Gain Energy [J]
-
-The total heat flow to the zone from the glazing, frame and divider of an exterior window when the total heat flow is positive.
-
-For a window *without an interior shading device*, this heat flow is equal to:
-
-[Surface Window Transmitted Solar Radiation Rate (see definition, above)]
-
-+ [Convective heat flow to the zone from the zone side of the glazing]
-
-+ [Net IR heat flow to the zone from zone side of the glazing]
-
-– [Short-wave radiation from zone transmitted back out the window]
-
-+ [Conduction to zone from window frame and divider, if present]
-
-Here, short-wave radiation is that from lights and diffuse interior solar radiation.
-
-For a window *with an interior shading device*, this heat flow is equal to:
-
-[Surface Window Transmitted Solar Radiation Rate]
-
-+ [Convective heat flow to the zone from the air flowing through the gap between glazing and shading device]
-
-+ [Convective heat flow to the zone from the zone side of the shading device]
-
-+ [Net IR heat flow to the zone from the zone side of the glazing]
-
-+ [Net IR heat flow to the zone from the zone side of the shading device]
-
-– [Short-wave radiation from zone transmitted back out the window]
-
-+ [Conduction to zone from window frame and divider, if present]
-
-The total window heat flow can also be thought of as the sum of the solar and conductive gain from the window glazing.
-
-#### Surface Window Heat Loss Rate [W]
-
-#### Surface Window Heat Loss Energy [J]
-
-The absolute value of the total heat flow through an exterior window when the total heat flow is negative. (See definition of “total heat flow� under “Surface Window Heat Gain Rate,� above.)
-
-#### Surface Window Glazing Beam to Beam Solar Transmittance []
-
-The fraction of exterior beam solar radiation incident on the glass of an exterior window that is transmitted through the glazing as beam radiation.  This is for the base  window without shading. Takes into account the angle of incidence of beam solar radiation on the glass.
-
-#### Surface Window Glazing Beam to Diffuse Solar Transmittance []
-
-The fraction of exterior beam solar radiation incident on the glazing of an exterior window that is transmitted through the glazing as diffuse radiation.
-
-#### Surface Window Glazing Diffuse to Diffuse Solar Transmittance []
-
-The fraction of exterior diffuse solar radiation incident on the glass of an exterior window that is transmitted through the glass assuming that the window has no shading device. It is assumed that incident diffuse solar is transmitted only as diffuse with no beam component.
-
-#### Surface Window Model Solver Iteration Count []
-
-The number of iterations needed by the window-layer heat balance solution to converge.
-
-#### Surface Window Solar Horizontal Profile Angle [deg]
-
-For a vertical exterior window, this is an angle appropriate for calculating beam solar quantities appropriate to horizontal window elements such as horizontal reveal surfaces, horizontal frame and divider elements and horizontal slats of window blinds. It is defined as the angle between the window outward normal and the projection of the sun’s ray on the vertical plane containing the outward normal. See Figure 32.
-
-For an exterior window of arbitrary tilt, it is defined as the angle between the window outward normal the projection of the sun’s ray on the plane that contains the outward normal and is perpendicular to the ground.
-
-If the sun is behind the window, the horizontal profile angle is not defined and is reported as 0.0.
-
-Note that in most texts what we call “horizontal profile angle� is called “vertical profile angle.�
-
-#### Surface Window Solar Vertical Profile Angle [deg]
-
-For a vertical exterior window, this is an angle appropriate for calculating beam solar quantities appropriate to vertical window elements such as vertical reveal surfaces, vertical frame and divider elements and vertical slats of window blinds. It is defined as the angle between the window outward normal and the projection of the sun’s ray on the horizontal plane containing the outward normal. See **Figure 32.**
-
-For an exterior window of arbitrary tilt, it is defined as the angle between the window outward normal the projection of the sun’s ray on the plane that contains the outward normal and is perpendicular to the plane defined above for Surface Window Solar Horizontal Profile Angle for a window of arbitrary tilt.
-
-If the sun is behind the window, the vertical profile angle is not defined and is reported as 0.0.
-
-Note that in most texts what we call “vertical profile angle� is called “horizontal profile angle.�
-
-![](media/image058.svg)
-
-Figure 32. Vertical exterior window showing solar horizontal profile angle, solar vertical profile angle and solar incidence angle.
-
-#### Surface Window Outside Reveal Reflected Beam Solar Radiation Rate [W]
-
-#### Surface Window Outside Reveal Reflected Beam Solar Radiation Energy [J]
-
-Beam solar radiation reflected from the outside reveal surfaces of a window (ref: Reveal Surfaces under WindowProperty:FrameAndDivider object). There are both rate and energy versions.
-
-#### Surface Window Inside Reveal Reflected Beam Solar Radiation Rate [W]
-
-#### Surface Window Inside Reveal Reflected Beam Solar Radiation Energy [J]
-
-Beam solar radiation reflected from the inside reveal surfaces of a  window (ref: Reveal Surfaces under WindowProperty:FrameAndDivider object). There are both rate and energy versions.
-
-#### Surface Window Inside Reveal Absorbed Beam Solar Radiation Rate [W]
-
-Beam solar radiation absorbed at the inside reveal surfaces of a window, in Watts.
-
-#### Surface Window Inside Reveal Reflected Diffuse Zone Solar Radiation Rate [W]
-
-Diffuse solar radiation reflected from inside reveal surfaces of a window into the zone, in Watts.
-
-#### Surface Window Inside Reveal Reflected Diffuse Frame Solar Radiation Rate [W]
-
-Diffuse solar radiation reflected from inside reveal surfaces onto the frame surfaces of a window, in Watts.
-
-#### Surface Window Inside Reveal Reflected Diffuse Glazing Solar Radiation Rate [W]
-
-Diffuse solar radiation reflected from inside reveal surfaces onto the glazing surfaces of a window, in Watts.
-
-#### Surface Window Inside Face Glazing Condensation Status []
-
-A value of 1 means that moisture condensation will occur on the innermost glass face of an exterior window (i.e., on the glass face in contact with the zone air). Otherwise the value is 0. The condition for condensation is glass inside face temperature &lt; zone air dewpoint temperature.
-
-For airflow exterior windows, in which forced air passes between adjacent glass faces in double- and triple-pane windows, a value of 1 means that condensation will occur on one or both of the glass faces in contact with the airflow. In this case the condition for condensation is:
-
-- *For airflow source = indoorair*, temperature of either face in contact with airflow &lt; zone air dewpoint temperature.
-
-- *For airflow source = outdoorair*, temperature of either face in contact with airflow &lt; outside air dewpoint temperature.
-
-As for regular windows, the value will also be 1 if condensation occurs on the innermost glass face.
-
-#### Surface Window Inside Face Frame Condensation Status []
-
-If an exterior window has a frame and the value of this flag is 1, condensation will occur on the inside surface of the frame. The condition for condensation is frame inside surface temperature &lt; zone air dewpoint temperature.
-
-#### Surface Window Inside Face Divider Condensation Status []
-
-If an exterior window has a divider and the value of this flag is 1, condensation will occur on the inside surface of the divider. The condition for condensation is divider inside surface temperature &lt; zone air dewpoint temperature.
-
-#### Surface Shading Device Is On Time Fraction []
-
-The fraction of time that a shading device is on an exterior window. For a particular simulation timestep, the value is 0.0 if the shading device is off (or there is no shading device) and the value is 1.0 if the shading device is on. (It is assumed that the shading device, if  present, is either on or off for the entire timestep.) If the shading device is switchable glazing, a value of 0.0 means that the glazing is in the unswitched (light colored) state, and a value of 1.0 means that the glazing is in the switched (dark colored) state.
-
-For a time interval longer a timestep, this is the fraction of the time interval that the shading device is on. For example, take the case where the time interval is one hour and the timestep is 10 minutes. Then if the shading device is on for two timesteps in the hour and off for the other four timesteps, then the fraction of time that the shading device is on = 2/6 = 0.3333.
-
-#### Surface Window Blind Slat Angle [deg]
-
-For an exterior window with a blind, this is the angle in degrees between the glazing outward normal and the blind slat angle outward normal, where the outward normal points away from the front face of the slat. The slat angle varies from 0 to 180 deg. If the slat angle is 0 deg or 180 deg, the slats are parallel to the glazing and the slats are said to be “closed�. If the slat angle is 90 deg, the slats are perpendicular to the glazing and the slats are said to be “fully open�. See illustrations under WindowMaterial:Blind. For blinds with a fixed slat angle, the value reported here will be constant.
-
-#### Surface Window Blind Beam to Beam Solar Transmittance []
-
-For an exterior window with a blind, this is the fraction of exterior beam solar radiation incident on the blind that is transmitted through the blind as beam solar radiation when the blind is isolated (i.e., as though the window glass were not present). Depends on various factors, including slat angle, width, separation, and thickness, and horizontal solar profile angle (for blinds with horizontal slats) or vertical solar profile angle (for blinds with vertical slats). The transmittance value reported here will be non-zero only when some beam solar can pass through the blind without hitting the slats.
-
-#### Surface Window Blind Beam to Diffuse Solar Transmittance []
-
-For an exterior window with a blind, the fraction of exterior beam solar radiation incident on the blind that is transmitted through the blind as diffuse solar radiation when the blind is isolated (i.e., as though the window glass were not present). Depends on various factors, including slat angle, width, separation, thickness and reflectance, and horizontal solar profile angle (for blinds with horizontal slats) or vertical solar profile angle (for blinds with vertical slats).
-
-#### Surface Window Blind Diffuse to Diffuse Solar Transmittance []
-
-For an exterior window with a blind, the fraction of exterior diffuse solar radiation incident on the blind that is transmitted through the blind as diffuse solar radiation when the blind is isolated (i.e., as though the window glass were not present). Depends on various factors, including slat angle, width, separation, thickness and reflectance. For blinds with a fixed slat angle the transmittance value reported here will be constant.
-
-#### Surface Window Blind and Glazing System Beam Solar Transmittance []
-
-The fraction of exterior beam solar radiation incident on an exterior window with a blind (excluding window frame, if present) that is transmitted through the blind/glass system as beam solar radiation. Depends on various factors, including type of glass; solar incidence angle; slat angle, width, separation, and thickness; and horizontal solar profile angle (for blinds with horizontal slats) or vertical solar profile angle (for blinds with vertical slats).
-
-#### Surface Window Blind and Glazing System Diffuse Solar Transmittance []
-
-The fraction of exterior diffuse solar radiation incident on an exterior window with a blind (excluding window frame, if present) that is transmitted through the blind/glass system as diffuse solar radiation. Depends on various factors, including type of glass and slat angle, width, separation, thickness and reflectance. For blinds with a fixed slat angle the transmittance value reported here will be constant.
-
-#### Surface Window Screen Beam to Beam Solar Transmittance []
-
-For an exterior window with a screen, this is the fraction of exterior beam solar radiation incident on the screen that is transmitted through the screen as beam solar radiation when the screen is isolated (i.e., as though the window glass were not present). Depends on various factors, including the screen reflectance and the relative angle of the incident beam with respect to the screen. This value will include the amount of inward reflection of solar beam off the screen material surface if the user specifies this modeling option (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method = Model as Direct Beam).
-
-#### Surface Window Screen Beam to Diffuse Solar Transmittance[]
-
-For an exterior window with a screen, the fraction of exterior beam solar radiation incident on the screen that is transmitted through the screen as diffuse solar radiation when the screen is isolated (i.e., as though the window glass were not present). Depends on various factors, including the screen reflectance and the relative angle of the incident beam with respect to the screen. This value is the amount of inward reflection of solar beam off the screen material surface if the user specifies this modeling option (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method = Model as Diffuse); otherwise, this value will be zero.
-
-#### Surface Window Screen Diffuse to Diffuse Solar Transmittance[]
-
-For an exterior window with a screen, the fraction of exterior diffuse solar radiation incident on the screen that is transmitted through the screen as diffuse solar radiation when the screen is isolated (i.e., as though the window glass were not present). Depends on various factors including screen material geometry and reflectance. This value is calculated as an average, constant For a window with a screen, this value consists of diffuse radiation transmitted through the screen (gaps between the screen material) and diffuse radiation from diffuse-to-diffuse reflection from the screen material. For a window with a screen, this value consists of diffuse radiation transmitted through the screen (gaps between the screen material) and diffuse radiation from diffuse-to-diffuse reflection from the screen material.
-
-#### Surface Window Screen and Glazing System Beam Solar Transmittance[]
-
-The fraction of exterior beam solar radiation incident on an exterior window with a screen (excluding window frame, if present) that is transmitted through the screen/glass system as beam solar radiation. Depends on various factors, including the screen reflectance and the relative angle of the incident beam with respect to the screen. This value will include the amount of inward reflection of solar beam off the screen material surface if the user specifies this modeling option (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method = Model as Direct Beam).
-
-#### Surface Window Screen and Glazing System Diffuse Solar Transmittance []
-
-The fraction of exterior diffuse solar radiation incident on an exterior window with a screen (excluding window frame, if present) that is transmitted through the screen/glass system as diffuse solar radiation. Depends on various factors including screen material geometry and reflectance.
-
-#### Surface Window Transmitted Beam Solar Radiation Rate [W]
-
-#### Surface Window Transmitted Beam Solar Radiation Energy [J]
-
-The beam solar radiation transmitted through an interior window. Calculated only if Solar Distribution = FullInteriorAndExterior in your Building input. The origin of this radiation is beam solar that enters through an exterior window in a zone and then passes through an interior window into the adjacent zone. The amount of this radiation depends on several factors, including sun position, intensity of beam solar incident on the exterior window (including effects of shadowing, if present),  relative position of the exterior and interior window, and the size and transmittance of the windows. Note that if there are two or more exterior windows in a zone, then beam solar from one or more of them may pass through the same interior window. Likewise, if there are more than two or more interior windows in a zone then beam solar from a single exterior window may pass through one or more of the interior windows. There are both rate and energy versions of the output.
-
-#### Surface Storm Window On Off Status [ ]
-
-Indicates whether a storm window glass layer is present (ref: StormWindow object). The value is **0** if the storm window glass layer is off, **1** if it is on, and **–1** if the window does not have an associated storm window. Applicable only to exterior windows and glass doors.
-
-#### Surface Inside Face Initial Transmitted Diffuse Transmitted Out Window Solar Radiation Rate [W]
-
-As of Version 2.1, the diffuse solar transmitted through exterior windows that is initially distributed to another window in the zone and transmitted out of the zone through that window. For exterior windows, this transmitted diffuse solar is “lost� to the exterior environment  For interior windows, this transmitted diffuse solar is distributed to heat transfer surfaces in the adjacent zone, and is part of the Surface Inside Face Initial Transmitted Diffuse Absorbed Solar Radiation Rate for these adjacent zone surfaces.
-
-#### Additional Window Outputs (Advanced)
-
-The following output variables for windows or glass doors are available when the user requests to display advanced output variables. These seven reports show the individual components that are combined to determine overall Surface Window Heat Gain Rate and/or Surface Window Heat Loss Rate (described above).
-
-#### Surface Window Inside Face Glazing Zone Convection Heat Gain Rate [W]
-
-The surface convection heat transfer from the glazing to the zone in watts. This output variable is the term called “[Convective heat flow to the zone from the zone side of the glazing]� under the description above for Surface Window Heat Gain Rate output variable. If the window has an interior shade or blind, then this is zero and the glazing’s convection is included in the report called “Surface Window Inside Face Gap between Shade and Glazing Zone Convection Heat Gain Rate�.
-
-#### Surface Window Inside Face Glazing Net Infrared Heat Transfer Rate [W]
-
-The net exchange of infrared radiation heat transfer from the glazing to the zone in watts.  This output variable is the term called “[Net IR heat flow to the zone from zone side of the glazing]� under the description above for Surface Window Heat Gain Rate output variable.
-
-#### Surface Window Shortwave from Zone Back Out Window Heat Transfer Rate [W]
-
-This is the short-wave radiation heat transfer from the zone back out the window in watts.  This is a measure of the diffuse short-wave light (from reflected solar and electric lighting) that leave the zone through the window.  This output variable is the term called “[Short-wave radiation from zone transmitted back out the window]� under the description above for Surface Window Heat Gain Rate output variable.
-
-#### Surface Window Inside Face Frame and Divider Zone Heat Gain Rate [W]
-
-This is the heat transfer from any frames and/or dividers to the zone in watts.  This output variable is the term called “[Conduction to zone from window frame and divider, if present]� under the description above for Surface Window Heat Gain Rate output variable.  (The word “conduction� here is used because the models is simplified compared to the complexities of surface convection and radiation.)
-
-#### Surface Window Frame Heat Gain Rate [W]
-
-This is the positive heat flow from window frames to the zone in watts. This is part of the Surface Window Inside Face Frame and Divider Zone Heat Gain Rate.
-
-#### Surface Window Frame Heat Loss Rate [W]
-
-This is the negative heat flow from window frames to the zone in watts. This is part of the Surface Window Inside Face Frame and Divider Zone Heat Gain Rate.
-
-#### Surface Window Frame Inside Temperature [C]
-
-This is the temperature of the inside surface of the window frames.
-
-#### Surface Window Frame Outside Temperature [C]
-
-This is the temperature of the outside surface of the window frames.
-
-#### Surface Window Divider Heat Gain Rate [W]
-
-This is the positive heat flow from window dividers to the zone in watts. This is part of the Surface Window Inside Face Frame and Divider Zone Heat Gain Rate.
-
-#### Surface Window Divider Heat Loss Rate [W]
-
-This is the negative heat flow from window dividers to the zone in watts. This is part of the Surface Window Inside Face Frame and Divider Zone Heat Gain Rate.
-
-#### Surface Window Divider Inside Temperature [C]
-
-This is the temperature of the inside surface of the window dividers.
-
-#### Surface Window Divider Outside Temperature [C]
-
-This is the temperature of the outside surface of the window dividers.
-
-#### Surface Window Inside Face Gap between Shade and Glazing Zone Convection Heat Gain Rate [W]
-
-This is the convection surface heat transfer from the both the glazing and the shade’s back face to the zone in Watts.  This output variable is the term called “[Convective heat flow to the zone from the air flowing through the gap between glazing and shading device]� under the description above for Surface Window Heat Gain Rate output variable. For Equivalent Layer window this output variable is the convection heat gain from vented interior air gap to the zone in Watts.
-
-#### Surface Window Inside Face Shade Zone Convection Heat Gain Rate [W]
-
-This is the convection surface heat transfer from the front side of any interior shade or blind to the zone in Watts.  This output variable is the term called “[Convective heat flow to the zone from the zone side of the shading device]� under the description above for Surface Window Heat Gain Rate output variable. For equivalent Layer window this output variable is the convection heat gain rate from the inside face of a glazing or a shade to the zone in Watts.
-
-#### Surface Window Inside Face Shade Net Infrared Heat Transfer Rate [W]
-
-The net exchange of infrared radiation heat transfer from the shade or blind to the zone in watts.  This output variable is the term called “[Net IR heat flow to the zone from the zone side of the shading device]� under the description above for Surface Window Heat Gain Rate output variable.
-
-***Surface Window Inside Face Other Convection Heat Gain Rate [W]***
-
-The other (extra) convection heat transfer rate from the inside face of a an equivalent layer window. This output is computed from the difference in convection flux when using equivalent inside surface temperature of a window instead of the inside surface temperature from the standard surface heat balance calculation.
-
-### Thermochomic Window Outputs
-
-#### Window Thermochromic Layer Temperature [C]
-
-The temperature of the TC glass layer of a TC window at each time step.
-
-#### Surface Window Thermochromic Layer Property Specification Temperature [C]
-
-The temperature under which the optical data of the TC glass layer are specified.
-
-The overall properties (U-factor/SHGC/VT) of the thermochromic windows at different specification temperatures are reported in the **.eio** file. These window constructions are created by EnergyPlus during run time. They have similar names with suffix “\_TC\_XX� where XX represents a specification temperature.
-
-#### Switchable Window Outputs
-
-#### Surface Window Switchable Glazing Switching Factor[]
-
-The switching factor (tint level) of the switchable window: 0 means no switching – clear state; 1 means fully switched – dark state.
-
-#### Surface Window Switchable Glazing Visible Transmittance[]
-
-The visible transmittance of the switchable window.
-
-### Other Surface Outputs/Reports
-
-Several reports can be selected for Surfaces. (See Group – Report for details on how to specify). Examples are:
-
-#### DXF
-
-This report produces a special file (**eplusout.dxf**) in the industry standard DXF (Drawing Interchange Format) for drawings. It is produced and accepted by many popular, commercial CAD programs. Detailed reference can be found on the AutoCADâ„¢ website at: http://www.autodesk.com/techpubs/autocad/acadr14/dxf/index.htm
-
-EnergyPlus produces this file from the Report command:
-
-```idf
-Output:Reports, Surfaces, DXF;
-```
-
-#### Details, Vertices, DetailsWithVertices
-
-This version of the report creates lines in the eplusout.eio file for each surface (except internal mass surfaces). Details of this reporting is shown in the Output Details and Examples document.
-
-### Shading Surfaces
-
-Shading surfaces are entities outside of the building that may cast shadows on the building’s heat transfer surfaces. These entities do not typically have enough thermal mass to be described as part of the building’s thermal makeup.
-
-The most important effect of shading surfaces is to reduce solar gain in windows that are shadowed. (However, in some cases, shading surfaces can reflect solar onto a wall or window and increase solar gain.)
-
-There are two kinds of shading surfaces in EnergyPlus: **detached** and **attached**. A **detached** shading surface, such as a tree or neighboring building, is not connected to the building. An **attached** shading surface is typically an overhang or fin that is attached to a particular base surface of the building, usually a wall; attached shading surfaces are usually designed to shade specific windows.
-
-Objects for detached shading surfaces:
-
-* Shading:Site
-
-* Shading:Building
-
-* Shading:Site:Detailed
-
-* Shading:Building:Detailed
-
-Similarly to the surfaces, the detailed objects use vertex entry whereas the other objects are limited to rectangular representation.
-
-Objects for attached shading surfaces:
-
-* Shading:Overhang
-
-* Shading:Overhang:Projection
-
-* Shading:Fin
-
-* Shading:Fin:Projection
-
-* Shading:Zone:Detailed
-
-EnergyPlus creates “bi-directional� shades from each shading surface entered. This means that the shade you input will cast a shadow no matter which side of the shade the sun is on. For example, a vertical fin will cast a shadow whether the sun is on the left side or right side of the fin.  Prior to V1.0.2, a shading surface cast a shadow only in the hemisphere toward which the surface faced. This hemisphere is the one pointed to by the shading surface’s outward normal vector, which is the cross product V23 x V21, where V23 is the vector from vertex 2 to vertex 3 of the shading surface and V21 is the vector from vertex 2 to vertex 1. Beginning with V1.0.2, the shades in EnergyPlus are “bi-directional� so that they can cast shadows in both hemispheres depending on the time-varying position of the sun relative to the shading surface.
-
-It is important to note that EnergyPlus will automatically account for “self-shading� effects—such as in L-shaped buildings—in which some of the building’s wall and roof surfaces shade other parts of the building, especially windows. This means that you only need to describe shading elements that aren’t building heat-transfer surfaces.
-
-Shading surfaces can also **reflect** solar radiation onto the building. This feature is simulated if you choose FullExteriorWithReflections or FullInteriorAndExteriorWithReflections in the Building object (ref: Building - Field: Solar Distribution). In this case, you may specify the reflectance properties of a shading surface with the ShadingProperty:Reflectance object. Note: If no ShadingProperty:Reflectance object is defined, then the shading surface reflectance values are assumed to be 0.2 and the fraction of shading surface that is glazed is assumed to be 0.0.
-
-Shading surfaces also automatically shade diffuse solar radiation (and long-wave radiation) from the sky. And they will automically shade diffuse solar radiation from the ground if Solar Distribution Field = FullExteriorWithReflections or FullInteriorAndExteriorWithReflections in the Building  object. (If the reflections option for Solar Distribution is used, the program also takes into account the reduction of solar radiation reflected from the ground due to shading of the ground by shading surfaces and by the building itself.)  Otherwise, shading surfaces will not shade diffuse radiation from the ground unless you enter a reduced value for View Factor to Ground for those building surfaces that are shaded (ref: BuildingSurface:Detailed - Field: View Factor to Ground and FenestrationSurface:Detailed - Field: View Factor to Ground).
-
-### Detached Shading Surfaces
-
-### Shading:Site, Shading:Building
-
-These objects are used to describe rectangular shading elements that are external to the building. Examples are trees, high fences, near-by hills, and neighboring buildings.
-
-If relative coordinates are used (ref: Field: Coordinate System in GlobalGeometryRules), shading surfaces entered with Shading:Site remain stationary if the building is rotated, whereas those entered with Shading:Building rotate with the building. If world coordinates are used Shading:Site and Shading:Building are equivalent.
-
-These shading elements are always opaque.
-
-#### Field: Name
-
-This is a unique character string associated with the detached shading surface. Though it must be unique from other surface names, it is used primarily for convenience with detached shading surfaces.
-
-#### Field: Azimuth Angle
-
-Theoretically, this should face to the surface it is shading (i.e. if a south wall, this should be a north facing shade) but since EnergyPlus automatically generates the mirror image, the facing angle per se’ is not so important.
-
-#### Field: Tilt Angle
-
-The tilt angle is the angle (in degrees) that the shade is tilted from horizontal (or the ground).  Default for this field is 90 degrees.
-
-#### Starting Corner for the surface
-
-The rectangular surfaces specify the lower left corner of the surface for their starting coordinate. See the introductory paragraph for rules on this entry.
-
-#### Field: Starting X Coordinate
-
-This field is the X coordinate (in meters).
-
-#### Field: Starting Y Coordinate
-
-This field is the Y coordinate (in meters).
-
-#### Field: Starting Z Coordinate
-
-This field is the Z coordinate (in meters).
-
-#### Field: Length
-
-This field is the length of the shade in meters.
-
-#### Field: Height
-
-This field is the width of the shade in meters.
-
-Examples of these (can be found in example files 4ZoneWithShading\_Simple\_1.idf and 4ZoneWithShading\_Simple\_2.idf)
-
-```idf
-  Shading:Building,
-    Bushes-East,             !- Name
-    90,                      !- Azimuth Angle {deg}
-    90,                      !- Tilt Angle {deg}
-    45,                      !- Starting X Coordinate {m}
-    0,                       !- Starting Y Coordinate {m}
-    0,                       !- Starting Z Coordinate {m}
-    50,                      !- Length {m}
-    1;                       !- Height {m}
-
-  Shading:Site,
-    Bushes-North,            !- Name
-    0,                       !- Azimuth Angle {deg}
-    90,                      !- Tilt Angle {deg}
-    45,                      !- Starting X Coordinate {m}
-    50,                      !- Starting Y Coordinate {m}
-    0,                       !- Starting Z Coordinate {m}
-    50,                      !- Length {m}
-    1;                       !- Height {m}
-```
-
-### Shading:Site:Detailed, Shading:Building:Detailed
-
-These objects are used to describe shading elements that are external to the building. Examples are trees, high fences, near-by hills, and neighboring buildings.
-
-If relative coordinates are used (ref: Field: Coordinate System in GlobalGeometryRules), shading surfaces entered with Shading:Site:Detailed remain stationary if the building is rotated, whereas those entered with Shading:Building:Detailed rotate with the building. If world coordinates are used Shading:Site:Detailed and Shading:Building:Detailed are equivalent.
-
-While "detached" implies that shading surfaces are not part of the building, the detached shading sequence can be used to describe attached shading surfaces that may shade heat transfer surfaces in more than one zone. For example, wing A of a building might shade several zones of wing B but wing A (for whatever reason) is not described in the geometry for the simulation so it is represented by a detached shade to get its shadowing effect.
-
-#### Field: Name
-
-This is a unique character string associated with the detached shading surface. Though it must be unique from other surface names, it is used primarily for convenience with detached shading surfaces.
-
-#### Field: Transmittance Schedule Name
-
-The name of a schedule of solar transmittance values from 0.0 to 1.0 for the shading surface. If a blank is entered in this field, the transmittance value defaults to 0.0, i.e., the shading surface is opaque at all times. This scheduling can be used to allow for seasonal transmittance change, such as for deciduous trees that have a higher transmittance in winter than in summer. Transmittance based on time of day can also be used—a movable awning, for example, where the transmittance is some value less than 1.0 when the awning is in place and is 1.0 when the awning is retracted.
-
-The following assumptions are made in the shading surface transmittance calculation:
-
-- Both sides of the shading surface have the same transmittance properties.
-
-- The transmittance is the same for both beam and diffuse solar radiation.
-
-- Beam solar transmittance is independent of angle of incidence on the shading surface.
-
-- Beam radiation incident on a shading surface is transmitted as beam radiation with no change in direction, i.e., there is no beam-to-diffuse component.
-
-- If two shading surfaces with non-zero transmittance overlap, the net transmittance is the product of the individual transmittances. Inter-reflection between the shading surfaces (and between the shading surfaces and the building) is ignored.
-
-- For the daylighting calculation (ref: Group – Daylighting) the shading surface’s visible transmittance is assumed to be the same as its solar transmittance.
-
-- Shading devices are assumed to be opaque to long-wave radiation no matter what the solar transmittance value is.
-
-Note that shading devices only shade solar radiation when the sun is up, which is automatically determined by EnergyPlus from latitude, time of year, etc. The user need only account for the time-varying transmittance of the shading device in the transmittance schedule, not whether the sun is up or not.
-
-#### Field: Number Vertices
-
-The number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on “Surface Vertices� above.
-
-IDF example of Detached Shading Surfaces:
-
-```idf
-Shading:Building:Detailed,
-   EAST SIDE TREE,  !- Detached Shading
-   ShadingTransmittance:0002,  !- Shadowing Transmittance & Schedule
-   3, !-Triangle
-   33.52800    ,   10.66800    ,   10.05800    ,
-   33.52800    ,   13.71600    ,  0.9140000    ,
-   33.52800    ,   4.572000    ,  0.9140000    ;
-
-Shading:Building:Detailed,
-   WEST SIDE TREE,  !- Detached Shading
-   ShadingTransmittance:0002,  !- Shadowing Transmittance & Schedule
-   3, !-Triangle
-  -3.048000    ,   7.620000    ,   10.05800    ,
-  -3.048000    ,   4.572000    ,  0.9140000    ,
-  -3.048000    ,   13.71600    ,  0.9140000    ;
-```
-
-
-### Attached Shading Surfaces
-
-Overhangs are usually horizontal devices that are used to shade windows. Fins are usually vertical devices that similarly shade windows.
-
-### Shading:Overhang
-
-An overhang typically is used to shade a window in a building.
-
-#### Field: Name
-
-This is the name of the overhang. It must be different from other surface names.
-
-#### Field: Window or Door Name
-
-The name of a window or door that this overhang shades.
-
-#### Field: Height above Window or Door
-
-This field is the height (meters) above the top of the door for the overhang.
-
-#### Field Tilt Angle from Window/Door
-
-This field is the tilt angle from the Window/Door.  For a flat overhang, this would be 90 (degrees).
-
-#### Field: Left Extension from Window/Door Width
-
-This field is the width from the left edge of the window/door to the start of the overhang (meters).
-
-#### Field: Right Extension from Window/Door Width
-
-This field is the width from the right edge of the window/door to the start of the overhang (meters).
-
-#### Field: Depth
-
-This field is the depth of the overhang (meters) projecting out from the wall.
-
-### Shading:Overhang:Projection
-
-An overhang typically is used to shade a window in a building. This object allows for specifying the depth of the overhang as a fraction of the window or door’s height.
-
-#### Field: Name
-
-This is the name of the overhang. It must be different from other surface names.
-
-#### Field: Window or Door Name
-
-The name of a window or door that this overhang shades.
-
-#### Field: Height above Window or Door
-
-This field is the height (meters) above the top of the door for the overhang.
-
-#### Field Tilt Angle from Window/Door
-
-This field is the tilt angle from the Window/Door.  For a flat overhang, this would be 90 (degrees).
-
-#### Field: Left Extension from Window/Door Width
-
-This field is the width from the left edge of the window/door to the start of the overhang (meters).
-
-#### Field: Right Extension from Window/Door Width
-
-This field is the width from the right edge of the window/door to the start of the overhang (meters).
-
-#### Field: Depth as Fraction of Window/Door Height
-
-This field is the fraction of the window/door height to specify as the depth of the overhang (meters) projecting out from the wall.
-
-### Shading:Fin
-
-Fins shade either side of windows/doors in a building. This object allows for specification of both fins for the window. Fin placement is relative to the edge of the glass and user must include the frame width when a frame is present.
-
-#### Field: Name
-
-This is the name of the overhang. It must be different from other surface names.
-
-#### Field: Window or Door Name
-
-The name of a window or door that this overhang shades.
-
-#### Field: Left Fin Extension from Window/Door
-
-This field is the width from the left edge of the window/door to the plane of the left fin (meters). The extension width is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Left Fin  Distance Above Top of Window
-
-This field is the distance from the top of the window to the top of the left fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Left Fin Distance Below Bottom of Window
-
-This field is the distance from the bottom of the window to the bottom of the left fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Left Fin Tilt Angle from Window/Door
-
-This field is the tilt angle from the window / door for the left fin.  Typically, a fin is 90 degrees (default) from its associated window/door.
-
-#### Field: Left Fin Depth
-
-This field is the depth (meters) of the left fin (projecting out from the wall).
-
-#### Field: Right Fin Extension from Window/Door
-
-This field is the width from the right edge of the window/door to the plane of the right fin (meters). The extension width is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Right Fin Distance Above Top of Window
-
-This field is the distance from the top of the window to the top of the right fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Right Fin Distance Below Bottom of Window
-
-This field is the distance from the bottom of the window to the bottom of the right fin (meters) and is relative to the edge of the glass and includes the frame width.
-
-#### Field: Right Fin Tilt Angle from Window/Door
-
-This field is the tilt angle from the window / door for the right fin..  Typically, a fin is 90 degrees (default) from its associated window/door.
-
-#### Field: Right Fin Depth
-
-This field is the depth (meters) of the right fin (projecting out from the wall).
-
-### Shading:Fin:Projection
-
-Fins shade either side of windows/doors in a building. This object allows for specification of both fins for the window. This object allows for specifying the depth of the overhang as a fraction of the window or door’s width. Fin placement is relative to the edge of the glass and user must include the frame width when a frame is present.
-
-#### Field: Name
-
-This is the name of the overhang. It must be different from other surface names.
-
-#### Field: Window or Door Name
-
-The name of a window or door that this overhang shades.
-
-#### Field: Left Fin Extension from Window/Door
-
-This field is the width from the left edge of the window/door to the plane of the left fin (meters). The extension width is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Left Fin Distance Above Top of Window
-
-This field is the distance from the top of the window to the top of the left fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Left Fin Distance Below Bottom of Window
-
-This field is the distance from the bottom of the window to the bottom of the left fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Left Fin Tilt Angle from Window/Door
-
-This field is the tilt angle from the window / door for the left fin.  Typically, a fin is 90 degrees (default) from its associated window/door.
-
-#### Field: Left Fin Depth as Fraction of Window/Door Width
-
-This field is the fraction of the window/door width to specify as the depth of the left fin (meters) projecting out from the wall.
-
-#### Field: Right Fin Extension from Window/Door
-
-This field is the width from the right edge of the window/door to the plane of the right fin (meters).. The extension width is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Right Fin Distance Above Top of Window
-
-This field is the distance from the top of the window to the top of the right fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Right Fin Distance Below Bottom of Window
-
-This field is the distance from the bottom of the window to the bottom of the right fin (meters) and is relative to the edge of the glass and includes the frame width when a frame is present.
-
-#### Field: Right Fin Tilt Angle from Window/Door
-
-This field is the tilt angle from the window / door for the right fin..  Typically, a fin is 90 degrees (default) from its associated window/door.
-
-#### Field: Right Fin Depth as Fraction of Window/Door Width
-
-This field is the fraction of the window/door width to specify as the depth of the right fin (meters) projecting out from the wall.
-
-zone.
-
-Examples of these (can be found in example files 4ZoneWithShading\_Simple\_1.idf and 4ZoneWithShading\_Simple\_2.idf)
-
-```idf
-  Shading:Overhang:Projection,
-    Zn001:Wall001:Win001:Shade001,  !- Name
-    Zn001:Wall001:Win001,    !- Window or Door Name
-    .7,                      !- Height above Window or Door {m}
-    90,                      !- Tilt Angle from Window/Door {deg}
-    .2,                      !- Left extension from Window/Door Width {m}
-    .2,                      !- Right extension from Window/Door Width {m}
-    .6;                      !- Depth as Fraction of Window/Door Height {m}
-
-  Shading:Overhang,
-    Zn001:Wall001:Door001:Shade001,  !- Name
-    Zn001:Wall001:Door001,   !- Window or Door Name
-    .6,                      !- Height above Window or Door {m}
-    90,                      !- Tilt Angle from Window/Door {deg}
-    0,                       !- Left extension from Window/Door Width {m}
-    0,                       !- Right extension from Window/Door Width {m}
-    3;                       !- Depth {m}
-
-  Shading:Fin:Projection,
-    Zn001:Wall001:Shade003,  !- Name
-    Zn001:Wall001:Win001,    !- Window or Door Name
-    .1,                      !- Left Extension from Window/Door {m}
-    .1,                   !- Left Distance Above Top of Window {m}
-    .1,                   !- Left Distance Below Bottom of Window {m}
-    90,                   !- Left Tilt Angle from Window/Door {deg}
-    .6,                   !- Left Depth as Fraction of Window/Door Width {m}
-    .1,                   !- Right Extension from Window/Door {m}
-    .1,                   !- Right Distance Above Top of Window {m}
-    .1,                   !- Right Distance Below Bottom of Window {m}
-    90,                   !- Right Tilt Angle from Window/Door {deg}
-    .6;                   !- Right Depth as Fraction of Window/Door Width {m}
-```
-
-### Shading:Zone:Detailed
-
-This object is used to describe attached “subsurfaces� such as overhangs, wings or fins that project outward from a base surface. This classification is used for convenience; actually, a device of this type can cast shadows on the surface to which it is attached as well as on adjacent surfaces. For example, a fin may shade its parent wall as well as adjacent walls.
-
-Note that a zone surface can cast shadows on other zone surfaces. However, you don’t have to worry about such effects—for example, one wall of an L-shaped building shading another wall--because EnergyPlus will automatically check for this kind of “self shadowing� and do the proper calculations.
-
-Unlike attached (or detached) shading surfaces, building surfaces can only cast shadows in the hemisphere towards which they face. This means, for example, that a roof that faces *upward* will not cast a shadow *downward*. (Thus, specifying an oversized roof in an attempt to account for the shading effects of overhangs will *not* work). Interior surfaces do not cast shadows of any kind.
-
-#### Field: Name
-
-This is the name of the attached shading surface. It must be different from other surface names.
-
-#### Field: Base Surface Name
-
-This is the name of the surface to which this shading device is attached. This surface can be a wall (or roof) but not a window or door.
-
-#### Field: Transmittance Schedule Name
-
-The name of a schedule of solar transmittance values from 0.0 to 1.0 for the shading surface. If a blank is entered in this field, the transmittance value defaults to 0.0, i.e., the shading surface is opaque at all times. This scheduling can be used to allow for seasonal transmittance change, such as for deciduous trees that have a higher transmittance in winter than in summer. Transmittance based on time of day can also be used—a movable awning, for example, where the transmittance is some value less than 1.0 when the awning is in place and is 1.0 when the awning is retracted.
-
-The following assumptions are made in the shading surface transmittance calculation:
-
-- Both sides of the shading surface have the same transmittance properties.
-
-- The transmittance is the same for both beam and diffuse solar radiation.
-
-- Beam solar transmittance is independent of angle of incidence on the shading surface.
-
-- Beam radiation incident on a shading surface is transmitted as beam radiation with no change in direction, i.e., there is no beam-to-diffuse component.
-
-- If two shading surfaces with non-zero transmittance overlap, the net transmittance is the product of the individual transmittances. Inter-reflection between the shading surfaces (and between the shading surfaces and the building) is ignored.
-
-- For the daylighting calculation (ref: Group – Daylighting) the shading surface’s visible transmittance is assumed to be the same as its solar transmittance.
-
-- Shading devices are assumed to be opaque to long-wave radiation no matter what the solar transmittance value is.
-
-Note that shading devices only shade solar radiation when the sun is up, which is automatically determined by EnergyPlus from latitude, time of year, etc. The user need only account for the time-varying transmittance of the shading device in the transmittance schedule, not whether the sun is up or not.
-
-#### Field: Number Vertices
-
-The number of sides in the surface (number of X,Y,Z vertex groups). For further information, see the discussion on “Surface Vertices� above. The example below shows the correct input for an overhang (to shade the appropriate portion of the base wall and window).
-
-![](media/image059.svg)
-
-Figure 33. Illustration for Attached Shading Surface
-
-Proper specification for this overhang (facing up) is:
-
-4,(C,0,D),(C,-B,D),(C+A,-B,D),(C+A,0,D); () used to illustrate each vertex.
-
-Note that for horizontal surfaces, any corner may be chosen as the starting corner. The order of vertices determines whether the surface is facing up or down. Shading surfaces are mirrored automatically unless the user specifies "DoNotMirrorDetachedShading", so each shading surface need only be described once.
-
-Thus, another shading surface will be created (facing down):
-
-4,(C+A,-B,D),(C+A,0,D),(C,0,D),(C,-B,D);
-
-IDF example of attached shading surfaces (overhang, fin):
-
-```idf
-Shading:Zone:Detailed,
-  Zn001:Wall001:Shade001,  !- Surface Name
-  Zn001:Wall001,  !- Base Surface Name
-  ShadingTransmittance:0001,  !- Shadowing Transmittance Schedule
-   4, !-RectangularOverhang
-   1.524000    , -0.3050000    ,   2.865000    ,
-   1.524000    ,  0.0000000E+00,   2.865000    ,
-   4.572000    ,  0.0000000E+00,   2.865000    ,
-   4.572000    , -0.3050000    ,   2.865000    ;
-Shading:Zone:Detailed,
-  Zn003:Wall001:Shade001,  !- Surface Name
-  Zn003:Wall001,  !- Base Surface Name
-  ShadingTransmittance:0001,  !- Shadowing Transmittance Schedule
-   4, !-RectangularLeftFin
-   57.97000    ,   8.450000    ,   10.00000    ,
-   57.97000    ,   8.450000    ,  0.0000000E+00,
-   57.97000    ,   6.450000    ,  0.0000000E+00,
-   57.97000    ,   6.450000    ,   10.00000    ;
- Shading:Zone:Detailed,Zn003:Wall001:Shade002,  !- Surface Name
-  Zn003:Wall001,  !- Base Surface Name
-  ShadingTransmittance:0003,  !- Shadowing Transmittance Schedule
-   4, !-RectangularRightFin
-   77.97000    ,   6.450000    ,   10.00000    ,
-   77.97000    ,   6.450000    ,  0.0000000E+00,
-   77.97000    ,   8.450000    ,  0.0000000E+00,
-   77.97000    ,   8.450000    ,   10.00000    ;
-```
-
-### ShadingProperty:Reflectance
-
-Specifies the reflectance properties of a shading surface when the solar reflection calculation has requested, i.e., when if “WithReflections� option is chosen in the Building object (ref: Building - Field: Solar Distribution). It is assumed that shading surfaces are divided into an unglazed, diffusely reflecting portion and a glazed, specularly-reflecting portion, either of which may be zero. The reflectance properties are assumed to be the same on both sides of the shading surface.
-
-Note that a shadowing transmittance schedule (ref: Shading Surfaces, Field: Transmittance Schedule Name) can be used with a reflective shading surface. However, EnergyPlus assumes that the reflectance properties of the shading surface are constant even if the transmittance varies.
-
-If no ShadingProperty:Reflectance objects are entered, the default values shown here will be used for shading surfaces. Other surfaces have their reflectance properties defined by the materials in the outer layers of the constructions.
-
-#### Field: Shading Surface Name
-
-The name of the Shading:Site, Shading:Building, Shading:Site:Detailed, Shading:Building:Detailed, Shading:Overhang, Shading:Overhang:Projection, Shading:Fin, Shading:Fin:Projection or Shading:Zone:Detailed object to which the following fields apply.
-
-If this ShadingProperty:Reflectance object is not defined for a shading surface the default values listed in each of the following fields will be used in the solar reflection calculation.
-
-#### Field: Diffuse Solar Reflectance of Unglazed Part of Shading Surface
-
-The diffuse solar reflectance of the unglazed part of the shading surface (default = 0.2). This reflectance is assumed to be the same for beam-to-diffuse and diffuse-to-diffuse reflection. Beam-to-diffuse reflection is assumed to be independent of angle of incidence of beam radiation. Diffuse-to-diffuse reflection is assumed to be independent of angular distribution of the incident of diffuse radiation. The outgoing diffuse radiation is assumed to be isotropic (hemispherically uniform).
-
-The sum of this reflectance and the shading surface transmittance should be less than or equal to 1.0.
-
-#### Field: Diffuse Visible Reflectance of Unglazed Part of Shading Surface
-
-The diffuse visible reflectance of the unglazed part of the shading surface (default = 0.2). This reflectance is assumed to be the same for beam-to-diffuse and diffuse-to-diffuse reflection. Beam-to-diffuse reflection is assumed to be independent of angle of incidence of beam radiation. Diffuse-to-diffuse reflection is assumed to be independent of angular distribution of the incident of diffuse radiation. The outgoing diffuse radiation is assumed to be isotropic (hemispherically uniform).
-
-This value if used only for the daylighting calculation (ref: Daylighting:Controls). The sum of this reflectance and the shading surface transmittance should be less than or equal to 1.0.
-
-#### Field: Fraction of Shading Surface That Is Glazed
-
-The fraction of the area of the shading surface that consists of windows (default = 0.0). It is assumed that the windows are evenly distributed over the surface and have the same glazing construction (see following “Name of Glazing Construction�). This might be the case, for example, for reflection from the façade of a neighboring, highly-glazed building. For the reflection calculation the possible presence of shades, screens or blinds on the windows of the shading surface is ignored. Beam-to-beam (specular) reflection is assumed to occur only from the glazed portion of the shading surface. This reflection depends on angle of incidence as determined by the program from the glazing construction. Beam-to-diffuse reflection from the glazed portion is assumed to be zero. The diffuse-to-diffuse reflectance of the glazed portion is determined by the program from the glazing construction.
-
-#### Field: Glazing Construction Name
-
-The name of the construction of the windows on the shading surface. Required if Fraction of Shading Surface That Is Glazed is greater than 0.0.
-
-IDF example of Shading Surface Reflectance for shading surface with specular reflection
-
-```idf
-Shading:Site:Detailed,
-Adjacent Glazed Facade,  !- User Supplied Surface Name
-,   !- Shadowing Transmittance Schedule
-4,  !- Number of Surface Vertex Groups -- Number of (X,Y,Z) groups
-0,-24,30, !- Vertex 1 X,Y,Z coordinates
-0,-24,0,  !- Vertex 2 X,Y,Z coordinates
-0,0,0,    !- Vertex 3 X,Y,Z coordinates
-0,0,30;   !-Vertex 3 X,Y,Z coordinates
-
-
-ShadingProperty:Reflectance,
-Adjacent Glazed Facade, !- Name of Surface:Shading Object
-0.3,  !- Diffuse Solar Reflectance of Unglazed Part of Shading Surface
-0.3,  !- Diffuse Visible Reflectance of Unglazed Part of Shading Surface
-0.7,  !- Fraction of Shading Surface That Is Glazed
-GlassCon-1; !- Name of Glazing Construction
-```
-
-
-
-
-IDF example of Shading Surface Reflectance for shading surface without specular reflection
-
-```idf
-Shading:Site:Detailed,
-Adjacent Blank Facade,  !- User Supplied Surface Name
-,   !- Shadowing Transmittance Schedule
-4,  !- Number of Surface Vertex Groups -- Number of (X,Y,Z) groups
-0,-24,30,
-0,-24,0,
-0,0,0,
-0,0,30;
-
-
-ShadingProperty:Reflectance,
-Adjacent Blank Facade, !- Name of Surface:Shading Object
-0.4,  !- Diffuse Solar Reflectance of Unglazed Part of Shading Surface
-0.4,  !- Diffuse Visible Reflectance of Unglazed Part of Shading Surface
-0.0,  !- Fraction of Shading Surface That Is Glazed
-;     !- Name of glazing construction
-```
-
-### WindowProperty:ShadingControl
-
-Window shading with coverings like drapes, blinds, screens or pull-down shades can be used to reduce the amount of solar radiation entering the window or reduce daylighting glare. It can also be used to reduce heat loss through the window (movable insulation). Leaving the window covering open in the winter can maximize solar heat gain and thereby reduce heating loads.
-
-With WindowProperty:ShadingControl—which is referenced by windows and glass doors (ref: FenestrationSurface:Detailed with Type = Window or GlassDoor)--you specify the type and location of the shading device, what variable or combination of variables controls deployment of the shading device, and what the control setpoint is. If the shading device is a blind, you also specify how the slat angle is controlled.
-
-NOTE: WindowProperty:ShadingControl does not work with complex fenestration systems. Controlled complex fenestration systems can be made only with Energy Management Systems objects. Inserting WindowProperty:ShadingControl in FenestrationSurface:Detailed while using complex fenestration systems will be ignored by program.
-
-As shown in Figure 34, a shading device can be inside the window (Shading Type = InteriorShade or InteriorBlind), outside the window (Shading Type = ExteriorShade or ExteriorBlind), or between panes of glass (Shading Type = BetweenGlassShade or BetweenGlassBlind). The exception is window screens which can only be outside the window (Shading Type = ExteriorScreen).
-
-![](media/image060.svg)
-
-Figure 34. Allowed locations of a window shading device.
-
-When a shading device is present it is either retracted or activated. When it is retracted it covers none of the window. When it is activated it covers the entire glazed part of the window (but not the frame). Whether the shading device is retracted or activated in a particular timestep depends on the control mechanism: see “Shading Control Type,� below. To model a case in which the shading device, when activated, covers only **part** of the window you will have to divide the window into two separate windows, one with the shading device and one without the shading device.
-
-A shading device can also be of a kind in which the optical properties of the glazing switch from one set of values to another in order to increase or decrease solar or visible transmittance (Shading Type = SwitchableGlazing).
-
-There are two ways of specifying the actual shading device:
-
-#### Specify “Name of Construction with Shading�
-
-This is the name of a window Construction that has the shading device as one of its layers. The thermal and solar-optical properties of the shading device are given by the shading material referenced in that Construction (ref: Construction, WindowMaterial:Shade, WindowMaterial:Screen and WindowMaterial:Blind). To use this method you have to define two Constructions for the window, one without the shading device and one with it. See Example 1, below.
-
-The Construction without the shading device is referenced in the FenestrationSurface:Detailed input for the window (see IDF example, below). The Construction with the shading device is referenced by the window’s WindowProperty:ShadingControl.
-
-For Shading Type = InteriorShade, InteriorBlind, ExteriorShade, ExteriorScreen and ExteriorBlind these two Constructions must be identical expect for the presence of the shading layer in the shaded Construction, otherwise you will get an error message. You will also get an error message if the Construction referenced by the window has a shading layer.
-
-#### Specify the “Material Name of the Shading Device�
-
-This is the name of a WindowMaterial:Shade, WindowMaterial:Screen or WindowMaterial:Blind. This method can be used with Shading Type = InteriorShade, InteriorBlind, ExteriorShade and ExteriorBlind. It cannot be used with Shading Type = BetweenGlassShade, BetweenGlassBlind, or SwitchableGlazing. If Shading Type = InteriorShade or ExteriorShade, then you specify the name of a WindowMaterial:Shade. If Shading Type = InteriorBlind or ExteriorBlind, then you specify the name of a WindowMaterial:Blind. If Shading Type = ExteriorScreen, then you specify the name of a WindowMaterial:Screen. See Example 2, below. This method is simpler to use since you don’t have to specify two Constructions that differ only by the shading layer.
-
-When this method is used, the program will automatically create a shaded window construction by adding a shading layer to the outside or inside of the construction corresponding to the window referencing the WindowProperty:ShadingControl. The name, created by the program, of this shaded construction is composed as follows: if the name of the window construction is CCC and the material name of the shading device is DDD, then the shaded construction name is CCC:DDD:INT for an interior shading device and CCC:DDD:EXT for an exterior shading device.
-
-This method is the required if you want to add a shading device to a construction brought in from a WINDOW Data File (ref:Construction:WindowDataFile).
-
-Note that if both “Name of Construction with Shading� and “Material Name of Shading Device� are specified, the former takes precedence.
-
-Most Shading Control Types allow you to specify a schedule that determines when the control is active. One example is a control that is active seasonally. For example, to deploy shading only in the summer when the incident solar is high enough, use Shading Control Type = OnIfHighSolarOnWindow with a schedule that is 1 during the summer months and 0 otherwise and specify Shading Control Is Scheduled = YES.
-
-In addition, most Shading Control Types also allow you to specify that glare control is active in addition to the specified Control Type. For example, you might want to deploy shading when the solar incident on a window is too high OR the glare from the window is too high. This type of joint control requires that the window be in a daylit zone, that the maximum allowed glare be specified in the Daylighting object for the zone, and that Glare Control Is Active = YES in WindowProperty:ShadingControl.
-
-If Shading Type = InteriorBlind, ExteriorBlind or BetweenGlassBlind you can use WindowProperty:ShadingControl to specify how the slat angle of the blind is controlled when the blind is in place.
-
-A special type of WindowProperty:ShadingControl is SwitchableGlazing. An example is electrochromic glazing in which the transmittance and reflectance of the glass is controlled electronically. For example, you could have electrochromic glazing switch from clear (high transmittance) to dark (low transmittance) to control solar gain. If you choose the Shading Type = SwitchableGlazing option for WindowProperty:ShadingControl, the unswitched (clear) state is specified by the Construction referenced by the window and the switched (dark) state is specified by the Construction referenced by WindowProperty:ShadingControl for that window. For example, if you specify Shading Type = SwitchableGlazing and Shading Control Type = OnIfHighSolarOnWindow, then the glazing will switch to the dark state whenever the solar radiation striking the window exceeds the Setpoint value.
-
-For Shading Type = SwitchableGlazing the state of the window is either clear (unswitched) or dark (fully switched) for all Shading Control Types except MeetDaylightIlluminanceSetpoint. In this case, the transmittance of the glazing is adjusted to just meet the daylight illuminance set point at the first daylighting reference point (see Daylighting). This type of control assures that there is just enough solar gain to meet the daylighting requirements in a zone, and no more, thus reducing the cooling load.
-
-#### Field: Name
-
-Name of the window shading control. It is referenced by a window (ref: Field: Shading Control Name).
-
-#### Field: Shading Type
-
-The type of shading device. The choices are:
-
-*InteriorShade*: A diffusing shade is on the inside of the window. (In the shaded Construction the shading layer must be a WindowMaterial:Shade.)
-
-*ExteriorShade*: A diffusing shade is on the outside of the window. (In the shaded Construction the shading layer must be a WindowMaterial:Shade.)
-
-*BetweenGlassShade*: A diffusing shade is between two glass layers. (In the shaded Construction the shading layer must be a WindowMaterial:Shade.) This shading type is allowed only for double- and triple-glazing. For triple-glazing the shade must be between the two inner glass layers.
-
-*ExteriorScreen*: An insect screen is on the outside of the window. (In the shaded Construction the shadling layer must be a WindowMaterial:Screen.)
-
-*InteriorBlind*: A slat-type shading device, such as a Venetian blind, is on the inside of the window. (In the shaded Construction the shading layer must be a WindowMaterial:Blind.)
-
-*ExteriorBlind*: A slat-type shading device is on the outside of the window. (In the shaded Construction the shading layer must be a WindowMaterial:Blind.)
-
-*BetweenGlassBlind*: A slat-type shading device is between two glass layers. (In the shaded Construction the shading layer must be a WindowMaterial:Blind.) This shading type is allowed only for double- and triple-glazing. For triple-glazing the blind must be between the two inner glass layers.
-
-*SwitchableGlazing*: Shading is achieved by changing the characteristics of the window glass, such as by darkening it.
-
-#### Field: Construction with Shading Name
-
-Name of the window Construction that has the shading in place. The properties of the shading device are given by the shading material referenced in that Construction (ref: Construction, WindowMaterial:Shade, WindowMaterial:Screen and WindowMaterial:Blind). For Shading Type = SwitchableGlazing, this is the name of the Construction that corresponds to the window in its fully-switched (darkest) state.
-
-Specifying “Name of Construction with Shading� is required if Shading Type = BetweenGlassShade, BetweenGlassBlind, or SwitchableGlazing. For other Shading Types, you may alternatively specify “Material Name of Shading Device� (see below).
-
-#### Field: Shading Control Type
-
-Specifies how the shading device is controlled, i.e., it determines whether the shading device is “on� or “off.� For blinds, screens and shades, when the device is “on� it is assumed to cover all of the window except its frame; when the device is “off� it is assumed to cover none of the window (whether “on� or “off� the shading device is assumed to cover none of the wall that the window is on).
-
-For switchable glazing, “on� means that the glazing is in the fully-switched state and “off� means that it is in the unswitched state; for example, for electrochromic glazing, “on� means the glazing is in its darkest state and “off� means it is in its lightest state.
-
-The choices for Shading Control Type are the following. If SetPoint is applicable its units are shown in parentheses.
-
-*AlwaysOn*: Shading is always on.
-
-*AlwaysOff*: Shading is always off.
-
-The following six control types are used primarily to reduce zone cooling load due to window solar gain.
-
-*OnIfScheduleAllows*: Shading is on if schedule value is non-zero. Requires that Schedule Name be specified and Shading Control Is Scheduled = Yes.
-
-Note: For exterior window screens *AlwaysOn, AlwaysOff, and OnIfScheduleAllows* are the only valid shading control types.
-
-*OnIfHighSolarOnWindow*: Shading is on if beam plus diffuse solar radiation incident on the window exceeds SetPoint (W/m<sup>2</sup>) and schedule, if specified, allows shading.
-
-*OnIfHighHorizontalSolar*: Shading is on if total (beam plus diffuse) horizontal solar irradiance exceeds SetPoint (W/m<sup>2</sup>) and schedule, if specified, allows shading.
-
-*OnIfHighOutdoorAirTemperature*: Shading is on if outside air temperature exceeds SetPoint (C) and schedule, if specified, allows shading.
-
-*OnIfHighZoneAirTemperature*: Shading is on if zone air temperature in the previous timestep exceeds SetPoint (C) and schedule, if specified, allows shading.
-
-*OnIfHighZoneCooling*: Shading is on if zone cooling rate in the previous timestep exceeds SetPoint (W) and schedule, if specified, allows shading.
-
-*OnIfHighGlare*: Shading is on if the total daylight glare index at the zone’s first daylighting reference point from all of the exterior windows in the zone exceeds the maximum glare index specified in the daylighting input for zone (ref: Group – Daylighting). Applicable only to windows in zones with daylighting.
-
-Note: Unlike other Shading Control Types, glare control is active whether or not a schedule is specified.
-
-*MeetDaylightIlluminanceSetpoint*: Used only with ShadingType = SwitchableGlazing in zones with daylighting controls. In this case the transmittance of the glazing is adjusted to just meet the daylight illuminance set point at the first daylighting reference point. Note that the daylight illuminance set point is specified in the Daylighting:Controls object for the Zone; it is not specified as a WindowProperty:ShadingControl SetPoint. When the glare control is active, if meeting the daylight illuminance set point at the first daylighting reference point results in higher discomfort glare index (DGI) than the specified zone’s maximum allowable DGI for either of the daylight reference points, the glazing will be further dimmed until the DGI equals the specified maximum allowable value.
-
-The following three control types can be used to reduce zone heating load during the winter by reducing window conductive heat loss at night and leaving the window unshaded during the day to maximize solar gain. They are applicable to any Shading Type except ExteriorScreen but are most appropriate for interior or exterior shades with high insulating value ("movable insulation"). “Night� means the sun is down and “day� means the sun is up.
-
-*OnNightIfLowOutdoorTempAndOffDay*: Shading is on at night if the outside air temperature is less than SetPoint (C) and schedule, if specified, allows shading. Shading is off during the day.
-
-*OnNightIfLowInsideTempAndOffDay*: Shading is on at night if the zone air temperature in the previous timestep is less than SetPoint (C) and schedule, if specified, allows shading. Shading is off during the day.
-
-*OnNightIfHeatingAndOffDay*: Shading is on at night if the zone heating rate in the previous timestep exceeds SetPoint (W) and schedule, if specified, allows shading. Shading is off during the day.
-
-The following two control types can be used to reduce zone heating and cooling load. They are applicable to any Shading Type except ExteriorScreen but are most appropriate for translucent interior or exterior shades with high insulating value ("translucent movable insulation").
-
-*OnNightIfLowOutdoorTempAndOnDayIfCooling*: Shading is on at night if the outside air temperature is less than SetPoint (C). Shading is on during the day if the zone cooling rate in the previous timestep is non-zero. Night and day shading is subject to schedule, if specified.
-
-*OnNightIfHeatingAndOnDayIfCooling*: Shading is on at night if the zone heating rate in the previous timestep exceeds SetPoint (W). Shading is on during the day if the zone cooling rate in the previous timestep is non-zero. Night and day shading is subject to schedule, if specified.
-
-The following control types can be used to reduce zone cooling load. They are applicable to any Shading Type except ExteriorScreen but are most appropriate for interior or exterior blinds, interior or exterior shades with low insulating value, or switchable glazing.
-
-*OffNightAndOnDayIfCoolingAndHighSolarOnWindow*: Shading is off at night. Shading is on during the day if the solar radiation incident on the window exceeds SetPoint (W/m<sup>2</sup>) and if the zone cooling rate in the previous timestep is non-zero. Daytime shading is subject to schedule, if specified.
-
-*OnNightAndOnDayIfCoolingAndHighSolarOnWindow*: Shading is on at night. Shading is on during the day if the solar radiation incident on the window exceeds SetPoint (W/m<sup>2</sup>) and if the zone cooling rate in the previous timestep is non-zero. Day and night shading is subject to schedule, if specified. (This Shading Control Type is the same as the previous one, except the shading is on at night rather than off.)
-
-*OnIfHighOutdoorAirTempAndHighSolarOnWindow:* Shading is on if the outside air temperature exceeds the Setpoint (C) and if if the solar radiation incident on the window exceeds SetPoint 2 (W/m<sup>2</sup>).
-
-*OnIfHighOutdoorAirTempAndHighHorizontalSolar:* Shading is on if the outside air temperature exceeds the Setpoint (C) and if if the horizontal solar radiation exceeds SetPoint 2 (W/m<sup>2</sup>).
-
-#### Field: Schedule Name
-
-Required if Shading Control Is Scheduled = Yes. If schedule value &gt; 0 , shading control is active, i.e., shading can be on only if the shading control test passes. If schedule value = 0, shading is off whether or not the control test passes. If Schedule Name is not specified, shading control is assumed to be active at all times.
-
-#### Field: Setpoint
-
-The setpoint for activating window shading. The units depend on the type of trigger:
-
-- W/m<sup>2</sup> for solar-based controls
-
-- W for cooling- or heating-based controls
-
-- Degrees C for temperature-based controls
-
-SetPoint is unused for Shading Control Type = OnIfScheduleAllows, OnIfHighGlare and DaylightIlluminance.
-
-#### Field: Shading Control Is Scheduled
-
-Accepts values YES and NO. The default is NO. Not applicable for Shading Control Type = OnIfHighGlare and should be blank in that case.
-
-If YES, Schedule Name is required and that schedule determines whether the shading control specified by Shading Control Type is active or inactive (see Schedule Name, above).
-
-If NO, Schedule Name is not applicable (should be blank) and the shading control is unscheduled.
-
-Shading Control Is Scheduled = YES is required if Shading Control Type = OnIfScheduleAllows.
-
-#### Field: Glare Control Is Active
-
-Accepts values YES and NO. The default is NO.
-
-If YES and the window is in a daylit zone, shading is on if the zone's discomfort glare index exceeds the maximum discomfort glare index specified in the Daylighting object referenced by the zone. For switchable windows with *MeetDaylightIlluminanceSetpoint* shading control, if Glare Control is active, the windows are always continuously dimmed as necessary to meet the zone’s maximum allowable DGI while providing appropriate amount of daylight for the zone.
-
-The glare test is OR'ed with the test specified by Shading Control Type. For example, if Glare Control Is Active = YES and Shading Control Type = OnIfHighZoneAirTemp, then shading is on if glare is too high OR if the zone air temperature is too high.
-
-Glare Control Is Active = YES is required if Shading Control Type = OnIfHighGlare.
-
-#### Field: Shading Device Material Name
-
-The name of a WindowMaterial:Shade, WindowMaterial:Screen or WindowMaterial:Blind. Required if "Name of Construction with Shading" is not specified. Not applicable if Shading Type = BetweenGlassShade, BetweenGlassBlind or SwitchableGlazing and should be blank in this case. If both "Name of Construction with Shading" and "Material Name of Shading Device" are entered the former takes precedence.
-
-#### Field: Type of Slat Angle Control for Blinds
-
-Applies only to Shading Type = InteriorBlind, ExteriorBlind or BetweenGlassBlind. Specifies how the slat angle is controlled. The choices are FixedSlatAngle, ScheduledSlatAngle and BlockBeamSolar.
-
- If FixedSlatAngle (the default), the angle of the slat is fixed at the value input for the WindowMaterial:Blind that is contained in the construction specified by Name of Construction with Shading or is specified by Material Name of Shading Device.
-
-If ScheduledSlatAngle, the slat angle varies according to the schedule specified by Slat Angle Schedule Name, below.
-
-If BlockBeamSolar, the slat angle is set each timestep to just block beam solar radiation. If there is no beam solar on the window the slat angle is set to the value input for the WindowMaterial:Blind that is contained in the construction specified by Name of Construction with Shading or is specified by Material Name of Shading Device. The BlockBeamSolar option prevents beam solar from entering the window and causing possible unwanted glare if the beam falls on work surfaces while at the same time allowing near-optimal indirect radiation for daylighting.
-
-#### Field: Slat Angle Schedule Name
-
-This is the name of a schedule of slat angles that is used when Type of Slat Angle Control for Blinds = ScheduledSlatAngle. You should be sure that the schedule values fall within the range given by the Minimum Slat Angle and Maximum Slat Angle values entered in the corresponding WindowMaterial:Blind. If not, the program will force them into this range.
-
-#### Field: Setpoint 2
-
-Used only as the second setpoint for the following two-setpoint control types: OnIfHighOutdoorAirTempAndHighSolarOnWindow,  OnIfHighOutdoorAirTempAndHighHorizontalSolar, OnIfHighZoneAirTempAndHighSolarOnWindow,
-
-and OnIfHighZoneAirTempAndHighHorizontalSolar
-
-An IDF example: window with interior roll shade that is deployed when solar incident on the window exceeds 50 W/m<sup>2</sup>.
-
- ! Example 1: Interior movable shade specified by giving name of shaded construction
-
- ! in WindowProperty:ShadingControl
-
-```idf
- WindowMaterial:Glazing, GLASS - CLEAR SHEET 1 / 8 IN,  !- Material Name
-     SpectralAverage,! Optical data type {SpectralAverage or Spectral}
-     ,               ! Name of spectral data set when Optical Data Type = Spectral
-     0.003        ,  !- Thickness {m}
-     0.837        ,  !- Solar Transmittance at Normal Incidence
-     0.075        ,  !- Solar Reflectance at Normal Incidence: Front Side
-     0.075        ,  !- Solar Reflectance at Normal Incidence: Back Side
-     0.898        ,  !- Visible Transmittance at Normal Incidence
-     0.081        ,  !- Visible Reflectance at Normal Incidence: Front Side
-     0.081        ,  !- Visible Reflectance at Normal Incidence: Back Side
-     0.0          ,  !- IR Transmittance
-     0.8400000    ,  !- IR Emissivity: Front Side
-     0.8400000    ,  !- IR Emissivity: Back Side
-     0.9000000    ;  !- Conductivity {W/m-K}
-
- WindowMaterial:Shade, ROLL SHADE,  !- Material Name
-     0.3          ,   !- Solar Transmittance at normal incidence
-     0.5000000    ,   !- Solar Reflectance (same for front and back side)
-     0.3          ,   !- Visible Transmittance at normal incidence
-     0.5000000    ,   !- Visible reflectance (same for front and back side)
-     0.9000000    ,   !- IR Emissivity (same for front and back side)
-     0.05         ,   !- IR Transmittance
-     0.003        ,   !- Thickness
-     0.1          ,   !- Conductivity {W/m-K}
-     0.0          ,   !- Top Opening Multiplier
-     0.0          ,   !- Bottom Opening Multiplier
-     0.5          ,   !- Left-Side Opening Multiplier
-     0.5          ,   !- Right-Side Opening Multiplier
-     0.0          ;   !- Air-Flow Permeability
-
- Construction, SINGLE PANE WITH NO SHADE,  ! Name of construction without shade
-     GLASS - CLEAR SHEET 1 / 8 IN;  !- First material layer
-
- Construction, SINGLE PANE WITH INT SHADE, ! Name of construction with shade
-     GLASS - CLEAR SHEET 1 / 8 IN,  !- First material layer
-     ROLL SHADE                  ;  !- Second material layer
-
- WindowProperty:ShadingControl, CONTROL ON INCIDENT SOLAR,  !- Name of Shading Control
-     InteriorShade,                !- Shading Type
-     SINGLE PANE WITH INT SHADE,   !- Name of construction with shading device
-     OnIfHighSolarOnWindow,        !- Shading Control Type
-     ,                             !- Schedule name
-     50.0,                         !- Setpoint {W/m2}
-     NO,                           !- Shading Control Is Scheduled
-     NO,                           !- Glare Control Is Active
-     ,                             !- Material Name of Shading Device
-     ,                             !- Type of Slat Angle Control for Blinds
-     ;                             !- Slat Angle Schedule Name
-
- FenestrationSurface:Detailed, Zn001:Wall001:Win001,  !- SubSurface Name
-     Window                   ,    !- Class
-     SINGLE PANE WITH NO SHADE,    !- Name of construction without shading device
-     Zn001:Wall001            ,    !- Base Surface Name
-     ,                             !- Target
-     0.5000000                ,    !- VF to Ground
-     CONTROL ON INCIDENT SOLAR,    !- Window Shading Control name
-     ,                             !- Frame/Divider name
-     1.0                      ,    !- Multiplier
-     4                        ,    !- Number of vertices (assumed rectangular)
-     0.548 ,  0.0 ,   2.5     ,    !- x,y,z of vertices {m}
-     0.548 ,  0.0 ,   0.5     ,
-     5.548 ,  0.0 ,   0.5     ,
-     5.548 ,  0.0 ,   2.5     ;
-
- ! Example 2: Interior movable shade specified by giving name of shading device in WindowProperty:ShadingControl
-
- WindowMaterial:Glazing, GLASS - CLEAR SHEET 1 / 8 IN,  !- Material Name
-     SpectralAverage,! Optical data type {SpectralAverage or Spectral}
-     ,               ! Name of spectral data set when Optical Data Type = Spectral
-     0.003        ,  !- Thickness {m}
-     0.837        ,  !- Solar Transmittance at Normal Incidence
-     0.075        ,  !- Solar Reflectance at Normal Incidence: Front Side
-     0.075        ,  !- Solar Reflectance at Normal Incidence: Back Side
-     0.898        ,  !- Visible Transmittance at Normal Incidence
-     0.081        ,  !- Visible Reflectance at Normal Incidence: Front Side
-     0.081        ,  !- Visible Reflectance at Normal Incidence: Back Side
-     0.0          ,  !- IR Transmittance
-     0.8400000    ,  !- IR Emissivity: Front Side
-     0.8400000    ,  !- IR Emissivity: Back Side
-     0.9000000    ;  !- Conductivity {W/m-K}
-
- WindowMaterial:Shade, ROLL SHADE,  !- Material Name
-     0.3          ,   !- Solar Transmittance at normal incidence
-     0.5000000    ,   !- Solar Reflectance (same for front and back side)
-     0.3          ,   !- Visible Transmittance at normal incidence
-     0.5000000    ,   !- Visible reflectance (same for front and back side)
-     0.9000000    ,   !- IR Emissivity (same for front and back side)
-     0.05         ,   !- IR Transmittance
-     0.003        ,   !- Thickness
-     0.1          ,   !- Conductivity {W/m-K}
-     0.0          ,   !- Top Opening Multiplier
-     0.0          ,   !- Bottom Opening Multiplier
-     0.5          ,   !- Left-Side Opening Multiplier
-     0.5          ,   !- Right-Side Opening Multiplier
-     0.0          ;   !- Air-Flow Permeability
-
- Construction, SINGLE PANE WITH NO SHADE,  ! Name of construction without shade
-     GLASS - CLEAR SHEET 1 / 8 IN;  !- First material layer
-
- WINDOWPROPERTY:SHADINGCONTROL, CONTROL ON INCIDENT SOLAR,  !- Name of Shading Control
-     InteriorShade,                !- Shading Type
-     ,                             !- Name of shaded construction
-     OnIfHighSolarOnWindow,        !- Shading Control Type
-     ,                             !- Schedule name
-     50.0,                         !- Setpoint {W/m2}
-     NO,                           !- Shading Control Is Scheduled
-     NO,                           !- Glare Control Is Active
-     ROLL SHADE,                   !- Material Name of Shading Device
-     ,                             !- Type of Slat Angle Control for Blinds
-     ;                             !- Slat Angle Schedule Name
-
- FenestrationSurface:Detailed, Zn001:Wall001:Win001,  !- SubSurface Name
-     Window                   ,    !- Class
-     SINGLE PANE WITH NO SHADE,    !- Name of construction without shade
-     Zn001:Wall001            ,    !- Base Surface Name
-     ,                             !- Target
-     0.5000000                ,    !- VF to Ground
-     CONTROL ON INCIDENT SOLAR,    !- Window Shading Control name
-     ,                             !- Frame/Divider name
-     1.0                      ,    !- Multiplier
-     4                        ,    !- Number of vertices (assumed rectangular)
-     0.548 ,  0.0 ,   2.5     ,    !- x,y,z of vertices {m}
-     0.548 ,  0.0 ,   0.5     ,
-     5.548 ,  0.0 ,   0.5     ,
-     5.548 ,  0.0 ,   2.5     ;
-```
-
-
-### WindowProperty:FrameAndDivider
-
-The WindowProperty:FrameAndDivider object is referenced by exterior windows that have
-
-- a frame, and/or
-
-- a divider, and/or
-
-- reveal surfaces that reflect beam solar radiation.
-
-A ***frame*** surrounds the glazing in a window (see Figure 35 and Figure 36). It is assumed that all frame characteristics—such as width, conductance and solar absorptance—are the same for the top, bottom and side elements of the frame. If the frame elements are not the same then you should enter area-weighted average values for the frame characteristics.
-
-The window vertices that you specify in the FenestrationSurface:Detailed object are those of the glazed part of the window, not the frame. EnergyPlus automatically subtracts the area of the frame—determined from the glazing dimensions and the frame width—from the area of the wall containing the window.
-
-A ***divider***, as shown in Figure 35, Figure 36 and Figure 37, divides the glazing up into separate lites. It is assumed that all divider elements have the same characteristics. If not, area-weighted average values should be used. EnergyPlus automatically subtracts the divider area from the glazed area of the window.
-
-***Reveal surfaces***, as shown in Figure 38, are associated with the setback of the glazing from the outside and/or inside surface of the parent wall. If the depth and solar absorptance of these surfaces are specified, the program will calculate the reflection of beam solar radiation from these surfaces. The program also calculates the shadowing (onto the window) of beam and diffuse solar radiation by outside reveal surfaces.
-
-In EnergyPlus, a window can have any combination of frame, divider and reveal surfaces, or none of these.
-
-The best source of frame and divider characteristics is the WINDOW program, which will calculate the values required by EnergyPlus for different frame and divider types. In particular, the THERM program within the WINDOW program will calculate the effective conductance of frames and dividers; this is the conductance taking 2-D heat transfer effects into account.
-
-Note that a window’s frame and divider characteristics, along with other window information, can be read in from the Window Data File (see “Importing Windows from the WINDOW program� and “Construction:WindowDataFile object�). In this case the WindowProperty:FrameAndDivider referenced by the window is not applicable and should be blank unless you want to specify reveal surfaces for beam solar reflection.
-
-![](media/image061.svg)
-
-Figure 35. A window with a frame and divider.
-
-In the illustration above, the divider has two horizontal elements and one vertical element.
-
-#### Field: Name
-
-The name of the frame/divider object. It is referenced by WindowProperty:FrameAndDivider Name in FenestrationSurface:Detailed.
-
-***Frame Fields***
-
-#### Field: Frame Width
-
-The width of the frame elements when projected onto the plane of the window. It is assumed that the top, bottom and side elements of the frame have the same width. If not, an average frame width should be entered such that the projected frame area calculated using the average value equals the sum of the areas of the frame elements.
-
-#### Field: Frame Outside Projection
-
-The amount by which the frame projects outward from the outside surface of the window glazing. If the outer surface of the frame is flush with the glazing, Frame Outside Projection = 0.0. Used to calculate shadowing of frame onto glass, solar absorbed by frame, IR emitted and absorbed by frame, and convection from frame.
-
-#### Field: Frame Inside Projection
-
-The amount by which the frame projects inward from the inside surface of the window glazing. If the inner surface of the frame is flush with the glazing, Frame Inside Projection = 0.0. Used to calculate solar absorbed by frame, IR emitted and absorbed by frame, and convection from frame.
-
-![](media/image062.svg)
-
-Figure 36. Illustration showing frame and divider dimensioning.
-
-#### Field: Frame Conductance
-
-The effective thermal conductance of the frame measured from inside to outside frame surface (no air films) and taking 2-D conduction effects into account. Obtained from the WINDOW program or other 2-D calculation.
-
-#### Field: Ratio of Frame-Edge Glass Conductance to Center-Of-Glass Conductance
-
-The glass conductance near the frame (excluding air films) divided by the glass conductance at the center of the glazing (excluding air films). Used only for multi-pane glazing constructions. This ratio is greater than 1.0 because of thermal bridging from the glazing across the frame and across the spacer that separates the glass panes. Values can be obtained from the WINDOW program the user-selected glazing construction and frame characteristics.
-
-#### Field: Frame Solar Absorptance
-
-The solar absorptance of the frame. The value is assumed to be the same on the inside and outside of the frame and to be independent of angle of incidence of solar radiation. If solar reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials).
-
-#### Field: Frame Visible Absorptance
-
-The visible absorptance of the frame. The value is assumed to be the same on the inside and outside of the frame and to be independent of angle of incidence of solar radiation. If visible reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials).
-
-#### Field: Frame Thermal Hemispherical Emissivity
-
-The thermal emissivity of the frame, assumed the same on the inside and outside.
-
-***Divider Fields***
-
-#### Field: Divider Type
-
-The type of divider (see figure below). Divider Type = Suspended is applicable only to multi-pane glazing. It means that the divider is suspended between the panes. (If there are more than two glass layers, the divider is assumed to be placed between the two outermost layers.)
-
-Divider Type = DividedLite means that the divider elements project out from the outside and inside surfaces of the glazing and divide the glazing into individual lites. For multi-pane glazing, this type of divider also has between-glass elements that separate the panes.
-
-![](media/image063.svg)
-
-Figure 37. Illustration showing divider types.
-
-#### Field: Divider Width
-
-The width of the divider elements when projected onto the plane of the window. It is assumed that the horizontal and vertical divider elements have the same width. If not, an average divider width should be entered such that the projected divider area calculated using the average value equals the sum of the areas of the divider elements.
-
-#### Field: Number of Horizontal Dividers
-
-The number of divider elements parallel to the top and bottom of the window.
-
-#### Field: Number of Vertical Dividers
-
-The number of divider elements parallel to the sides of the window.
-
-#### Field: Divider Outside Projection
-
-The amount by which the divider projects out from the outside surface of the window glazing. For Divider Type = Suspended, Divider Projection = 0.0. Used to calculate shadowing of divider onto glass, solar absorbed by divider, IR emitted and absorbed by divider, and convection from divider.
-
-#### Field: Divider Inside Projection
-
-The amount by which the divider projects inward from the inside surface of the window glazing. If the inner surface of the divider is flush with the glazing, Divider Inside Projection = 0.0. Used to calculate solar absorbed by divider, IR emitted and absorbed by divider, and convection from divider.
-
-#### Field: Divider Conductance
-
-The effective thermal conductance of the divider measured from inside to outside divider surface (no air films) and taking 2-D conduction effects into account. Obtained from the WINDOW program or other 2-D calculation.
-
-#### Field: Ratio of Divider-Edge Glass Conductance to Center-Of-Glass Conductance
-
-The glass conductance near the divider (excluding air films) divided by the glass conductance at the center of the glazing (excluding air films). Used only for multi-pane glazing constructions. This ratio is greater than 1.0 because of thermal bridging from the glazing across the divider and across the spacer that separates the glass panes. Values can be obtained from the WINDOW program for the user-selected glazing construction and divider characteristics.
-
-#### Field: Divider Solar Absorptance
-
-The solar absorptance of the divider. The value is assumed to be the same on the inside and outside of the divider and to be independent of angle of incidence of solar radiation. If solar reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials).
-
-#### Field: Divider Visible Absorptance
-
-The visible absorptance of the divider. The value is assumed to be the same on the inside and outside of the divider and to be independent of angle of incidence of solar radiation. If visible reflectance (or reflectivity) data is available, then absorptance is equal to 1.0 minus reflectance (for opaque materials).
-
-#### Field: Divider Thermal Hemispherical Emissivity
-
-The thermal emissivity of the divider, assumed the same on the inside and outside.
-
-***Reveal Surface Fields***
-
-The following fields specify the properties of the window reveal surfaces (reveals occur when the window is not in the same plane as the base surface). From this information and from the geometry of the window and the sun position, the program calculates beam solar radiation absorbed and reflected by the top, bottom, right and left sides of outside and inside window reveal surfaces. In doing this calculation, the shadowing on a reveal surface by other reveal surfaces is determined using the orientation of the reveal surfaces and the sun position.
-
-It is assumed that:
-
-- The window is an exterior window.
-
-- The reveal surfaces are perpendicular to the window plane.
-
-- If an exterior shade, screen or blind is in place it shades exterior and interior reveal surfaces so that in this case there is no beam solar on these surfaces.
-
-- If an interior shade or blind is in place it shades the interior reveal surfaces so that in this case there is no beam solar on these surfaces.
-
-- The possible shadowing on inside reveal surfaces by a window divider is ignored.
-
-- The outside reveal surfaces (top, bottom, left, right) have the same solar absorptance and depth. This depth is not input here but is automatically determined by the program—from window and wall vertices--as the distance between the plane of the outside face of the glazing and plane of the outside face of the parent wall.
-
-- The inside reveal surfaces are divided into two categories: (1) the bottom reveal surface, called here the "inside sill;" and (2) the other reveal surfaces (left, right and top).
-
-- The left, right and top inside reveal surfaces have the same depth and solar absorptance. The inside sill is allowed to have depth and solar absorptance values that are different from the corresponding values for the other inside reveal surfaces.
-
-- The inside sill depth is required to be greater than or equal to the depth of the other inside reveal surfaces. If the inside sill depth is greater than zero the depth of the other inside reveal surfaces is required to be greater than zero.
-
-- The reflection of beam solar radiation from all reveal surfaces is assumed to be isotropic diffuse; there is no specular component.
-
-- Half of the beam solar reflected from outside reveal surfaces is goes towards the window; the other half goes back to the exterior environment (i.e., reflection of this outward-going component from other outside reveal surfaces is not considered).
-
-- The half that goes towards the window is added to the other solar radiation incident on the window. Correspondingly, half of the beam solar reflected from inside reveal surfaces goes towards the window, with the other half going into the zone. The portion going towards the window that is not reflected is absorbed in the glazing or is transmitted back out into the exterior environment.
-
-- The beam solar that is absorbed by outside reveal surfaces is added to the solar absorbed by the outside surface of the window's parent wall; similarly, the beam solar absorbed by the inside reveal surfaces is added to the solar absorbed by the inside surface of the parent wall.
-
-The net effect of beam solar reflected from outside reveal surfaces is to increase the heat gain to the zone, whereas the effect of beam solar reflected from inside reveal surfaces is to decrease the heat gain to the zone since part of this reflected solar is transmitted back out the window.
-
- If the window has a frame, the absorption of reflected beam solar by the inside and outside surfaces of the frame is considered. The shadowing of the frame onto interior reveal surfaces is also considered.
-
-#### Field: Outside Reveal Solar Absorptance
-
-The solar absorptance of outside reveal surfaces.
-
-#### Field: Inside Sill Depth
-
-The depth of the inside sill, measured from the inside surface of the glazing to the edge of the sill (see Figure 38).
-
-#### Field: Inside Sill Solar Absorptance
-
-The solar absorptance of the inside sill.
-
-***Field: Inside Reveal Depth***
-
-The depth of the inside reveal surfaces other than the sill, measured from the inside surface of the glazing to the edge of the reveal surface (see Figure 38).
-
-#### Field: Inside Reveal Solar Absorptance
-
-The solar absorptance of the inside reveal surfaces other than the sill.
-
-![](media/image064.svg)
-
-Figure 38. (a) Vertical section through a window (with frame) showing outside and inside reveal surfaces and inside sill. (b) Perspective view looking from the outside of a window (without frame) showing reveal surfaces. Note that “Outside Reveal Depth� is not a user input; it is calculated by the program from the window and wall vertices.
-
-An IDF example:
-
-```idf
-  WindowProperty:FrameAndDivider,
-      TestFrameAndDivider, ! Frame/Divider Name
-      0.05, ! Frame Width
-      0.04, ! Frame Outside Projection
-      0.03, ! Frame Inside Projection
-      5.0,  ! Frame Conductance
-      1.3,  ! Ratio of Frame-Edge Glass Conductance to Center-Of-Glass Conductance
-      0.8,  ! Frame Solar Absorptance
-      0.8,  ! Frame Visible Absorptance
-      0.9,  ! Frame Thermal Emissivity
-      DividedLite, ! Divider Type
-      0.03, ! Divider Width
-      2,    ! Number of Horizontal Dividers
-      2,    ! Number of Vertical Dividers
-      0.03, ! Divider Outside Projection
-      0.03, ! Divider Inside Projection
-      5.0,  ! Divider Conductance
-      1.3,  ! Ratio of Divider-Edge Glass Conductance to Center-Of-Glass Conductance
-      0.8,  ! Divider Solar Absorptance
-      0.8,  ! Divider Visible Absorptance
-      0.9,  ! Divider Thermal Emissivity
-      0.7,  ! Outside Reveal Solar Absorptance
-      0.25, ! Inside Sill Depth (m)
-      0.6,  ! Inside Sill Solar Absorptance
-      0.2,  ! Inside Reveal Depth (m)
-      0.5;  ! Inside Reveal Solar Absorptance
-```
-
-
-### WindowProperty:AirflowControl
-
-This object is used to specify the control mechanism for windows in which forced air flows in the gap between adjacent layers of glass. Such windows are called “airflow windows.� They are also known as “heat-extract windows� or “climate windows.�
-
-A common application is to reduce the zone load by exhausting indoor air through the window. In the cooling season this picks up and expels some of the solar heat absorbed by the window glass (and by the between-glass shade or blind, if present). In the heating season this warms the window, reducing the heat loss from the window. A side benefit is increased thermal comfort. This is because the inside surface of the window will generally be cooler in summer and warmer in winter.
-
-The surface output variable “Surface Window Gap Convective Heat Transfer Rate� gives the heat picked up (or lost) by the gap airflow.
-
-#### Field: Name
-
-Name of the window that this WindowProperty:AirflowControl refers to. It must be a window with two or three glass layers, i.e., double- or triple-glazing. For triple-glazing the airflow is assumed to be between the two inner glass layers.
-
-An error will result if the gas in the airflow gap is other than air. If an airflow window has a between-glass shade or blind, the gas in the gap on either side of the shade or blind must be air.
-
-#### Field: Airflow Source
-
-The source of the gap airflow. The choices are:
-
-*IndoorAir*: Indoor air from the window’s zone is passed through the window.
-
-*OutdoorAir*: Outdoor air is passed through the window.
-
-#### Field: Airflow Destination
-
-This is where the gap air goes after passing through the window. The choices are:
-
-*IndoorAir*: The gap air goes to the indoor air of the window’s zone.
-
-*OutdoorAir*: The gap air goes to the outside air.
-
-*ReturnAir*. The gap air goes to the return air for the window’s zone. This choice is allowed only if Airflow Source = InsideAir. If the return air flow is zero, the gap air goes to the indoor air of the window’s zone. If the sum of the gap airflow for all of the windows in a zone with Airflow Destination = ReturnAir exceeds the return airflow, then the difference between this sum and the return airflow goes to the indoor air.
-
-Figure 39 shows the allowed combinations of Airflow Source and Airflow Destination. The allowed combinations of Airflow Source and Airflow Destination are:
-
-IndoorAir -&gt; OutdoorAir
-
-IndoorAir -&gt; IndoorAir
-
-IndoorAir -&gt; ReturnAir
-
-OutdoorAir -&gt; IndoorAir
-
-OutdoorAir -&gt; OutdoorAir
-
-#### Field: Maximum Flow Rate
-
-The maximum value of the airflow, in m<sup>3</sup>/s per m of glazing width. The value is typically 0.006 to 0.009 m<sup>3</sup>/s-m (4 to 6 cfm/ft).
-
-The airflow can be modulated by specifying Airflow Has Multiplier Schedule = Yes and giving the name of the Airflow Multiplier Schedule (see below).
-
-The fan energy used to move the air through the gap is generally very small and so is ignored.
-
-#### Field: Airflow Control Type
-
-Specifies how the airflow is controlled. The choices are:
-
-*AlwaysOnAtMaximumFlow*. The airflow is always equal to Maximum Airflow.
-
-*AlwaysOff*. The airflow is always zero.
-
-*ScheduledOnly*. The airflow in a particular timestep equals Maximum Airflow times the value of the Airflow Multiplier Schedule for that timestep.
-
-#### Field: Airflow Is Scheduled
-
-Specifies if the airflow is scheduled. The choices are:
-
-*Yes*. The airflow is scheduled.
-
-*No*. The airflow is not scheduled.
-
-If Yes, Airflow Multiplier Schedule Name is required.
-
-#### Field: Airflow Multiplier Schedule Name
-
-The name of a schedule with values between 0.0 and 1.0. The timestep value of the airflow is Maximum Airflow times the schedule value. Required if Airflow Is Scheduled = Yes. Unused if Airflow Is Scheduled = No. This schedule should have a ScheduleType with Numeric Type = Continuous and Range = 0.0 : 1.0.
-
-
-
-![](media/image065.svg)
-
-Figure 39. Gap airflow configurations for airflow windows. (a) **Air exhaust window**: Airflow Source = InsideAir, Airflow Destination = OutsideAir; (b) **Indoor air curtain window**: Airflow Source = InsideAir, Airflow Destination = InsideAir; (c) **Air supply window**: Airflow Source = OutsideAir, Airflow Destination = InsideAir; (d) **Outdoor air curtain window**: Airflow Source = OutsideAir, Airflow Destination = OutsideAir; (e) **Airflow to Return Air**: Airflow Source = InsideAir, Airflow Destination = ReturnAir. Based on “Active facades,� Version no. 1, Belgian Building Research Institute, June 2002.
-
-
-
-An IDF example: window with a constant airflow from inside to outside at 0.008 m<sup>3</sup>/s-m.
-
-```idf
- WindowProperty:AirflowControl,   !- Used to control forced airflow through a gap between glass layers
-    Zn001:Wall001:Win002,   !- Name of Associated Window
-    InsideAir,              !- Airflow Source
-    OutsideAir,             !- Airflow Destination
-    0.008,                  !- Maximum Airflow (m3/s per m of glazing width)
-    AlwaysOnAtMaxFlow,      !- Airflow Control Type
-    No,                     !- Airflow Has Multiplier Schedule?
-    ;                       !- Name of Airflow Multiplier Schedule
-```
-
-
-### WindowProperty:StormWindow
-
-This object allows you to assign a movable exterior glass layer (“storm window� or “storm glass�) that is usually applied to a window in the winter to reduce heat loss and removed in the summer. A WindowProperty:StormWindow object is required for each window that has an associated storm window. It is assumed that:
-
-- When the storm glass is in place it is the outermost layer of the window, it covers only the glazed part of the window and not the frame, and it forms a tight seal. See Figure 40.
-
-- When the storm glass is not in place it is completely removed and has no effect on window heat transfer.
-
-- The gap between the storm glass and rest of the glazing is filled with air.
-
-
-
-![](media/image066.svg)
-
-Figure 40. Section through a single-glazed window without (left) and with (right) a storm glass layer. Not to scale.
-
-With the addition of a storm window, single glazing effectively becomes double glazing, double glazing becomes triple glazing, etc.
-
-The presence of a storm window is indicated by the output variable “Surface Storm Window On Off Status� (see “Window Output Variables�). This flag is **0** if the storm window is off, **1** if it is on, and **–1** if the window does not have an associated storm window.
-
-The program automatically creates a window construction (ref: Construction) that consists of the storm window glass layer and its adjacent air layer added to the original (unshaded, or “bare�) window construction. In the eplusout.eio file this construction is called BARECONSTRUCTIONWITHSTORMWIN:*n*, where *n* is the number of the associated StormWin object. If the window has a shaded construction, the program creates a construction called SHADEDCONSTRUCTIONWITHSTORMWIN:*n* that consists of the storm window glass layer and its adjacent air layer added to the original shaded window construction.
-
-The program also creates a WindowMaterial:Gas layer corresponding to the air layer adjacent to the storm glass. In the eplusout.eio file this layer is called AIR:STORMWIN:*k*MM, where *k* is the thickness of the air layer expressed as an integer number of millimeters.
-
-#### Field: Window Name
-
-This is the name of a window (or glass door) to which the storm glass is applied. Not all windows can accept WindowProperty:StormWindow. The rules are:
-
-- The window must be an exterior window. WindowProperty:StormWindow is not applicable to interior (interzone) windows.
-
-- The window construction (without the storm glass layer) can have up to three glass layers.
-
-- If the window has an associated shaded construction (ref: WindowProperty:ShadingControl), that construction can have an interior shade or blind and up to three glass layers, or a between-glass shade or blind and two glass layers. The shaded construction cannot have an exterior shade or blind, cannot have a between-glass shade or blind and three glass layers, and cannot be switchable glazing.
-
-- The window cannot be an airflow window, i.e., a window that has an associated WindowProperty:AirflowControl.
-
-#### Field: Storm Glass Layer Name
-
-This is the name of a window glass material. Storm windows are assumed to consist of a single layer of glass. A storm window frame, if present, is ignored.
-
-#### Field: Distance Between Storm Glass Layer and Adjacent Glass
-
-The separation between the storm glass and the rest of the window (Figure 40). It is measured from the inside of the storm glass layer to the outside of the adjacent glass layer.
-
-#### Field: Month that Storm Glass Layer Is Put On
-
-The number of the month (January = 1, February = 2, etc.) during which the storm window is put in place.
-
-#### Field: Day of Month that Storm Glass Layer Is Put On
-
-The day of the month that the storm window is put in place. It is assumed that the storm window is put in place at the beginning of this day, i.e., during the first simulation timestep of the day, and remains in place until that month and day given by the following two fields.
-
-#### Field: Month that Storm Glass Layer Is Taken Off
-
-The number of the month (January = 1, February = 2, etc.) during which the storm window is removed.
-
-#### Field: Day of Month that Storm Glass Layer Is Taken Off
-
-The day of the month that the storm window is removed. It is assumed that the storm window is removed at the beginning of this day, i.e., during the first simulation timestep of the day, and stays off until the month and day given by Month that Storm Glass Layer Is Put On, Day of Month that Storm Glass Layer Is Put On.
-
-In the northern hemisphere, the month the storm window is put on is generally greater than the month it is taken off (for example put on in month 10, when it starts to get cold, and taken off in month 5, when it starts to warm up). In the southern hemisphere this is reversed: month on is less than month off.
-
-An IDF example of WindowProperty:StormWindow. The storm window is put in place on October 15 and removed on May 1.
-
-```idf
-WindowProperty:StormWindow,
- Window1, !- Name of Window to Which Storm Window Glass Layer is Applied
- GlassA,  !- Name of Material:WindowGlass or MATERIAL:WindowGlass:AltInput that is the storm window layer
- 0.060,   !- Distance from storm window to adjacent glass (m)
- 10,      !- Month that Storm Window Is Put On
- 15,      !- Day of Month that Storm Window Is Put On
- 5,       !- Month that Storm Window Is Taken Off
- 1;       !- Day of Month that Storm Window Is Taken Off
-```
-
-
-### Importing Windows from WINDOW program
-
-WINDOW v6.3 and later is capable of writing IDF excerpts for Window data. This is the preferred method as no external file is necessary. See the Tips document for details on obtaining the IDF excerpt.
-
-The WINDOW program calculates the U-value, Solar Heat Gain Coefficient, solar transmission/absorption characteristics, visible transmission characteristics and other properties of a window under standard indoor and outdoor conditions. WINDOW treats the whole window system—glazing, frame and divider. A sub-program of WINDOW called THERM uses a 2-D finite element calculation to determine the effective conductance of frame, divider and edge-of-glass elements. Another sub-program, OPTICS, determines the solar-optical properties of glazing, including laminates and coated glass.
-
-WINDOW can write a data file containing a description of the window that was analyzed. An example of this file (which is no longer the preferred method) is shown in the Tips document under WINDOW generated files. is shown below. This file, which can be named by the user, can be read by EnergyPlus. For more complete description and examples, see the object description -- Construction:WindowDataFile.
-
-In this way, the same window that was created in WINDOW can be imported into EnergyPlus for annual energy analysis without having to re-input the window data. To obtain WINDOW, THERM, or OPTICS go to http://windows.lbl.gov and choose the software link. A major advantage of using WINDOW to create window input for EnergyPlus is that you will have direct access to WINDOW’s expanding database of over 1000 different glass types; and you will be able to browse through this database according to different criteria (color, transmittance, solar heat gain coefficient, etc.) to help you select the best glass type for your application.
-
-Although WINDOW writes only one window entry on the WINDOW data file, EnergyPlus users can combine two or more of these files to end up with a single data file with multiple window entries of different types. In this way a library of windows from WINDOW can be built up if so desired. If you combine files like this you should be sure not to leave out or change any of lines from the original files.
-
-- There are four methods for inputting window constructions in EnergyPlus:
-
-1)   input full spectral data for each layer in the IDF,
-
-2)   input spectral average data for each layer in the IDF,
-
-3)   items 1 and 2 can be accomplished by reporting the IDF excerpt method from WINDOW
-
-4)   import WINDOW report containing layer-by-layer calculated values and overall glazing system angular values.
-
-**Note: When using method 4, the overall glazing system angular dependent properties, including Tsol, Abs, Rfsol, Rbsol, Tvis, Rfvis, and Rbvis, are not used by EnergyPlus. Therefore, methods 1 and 2 and preferably 3 are recommended.**
-
-- The SHGC calculations in EnergyPlus for window layers input using full spectral data use a spectral weighting data set (derived from Optics5 data file ISO-9845GlobalNorm.std) that is different from the WINDOW default spectral weighting data set (W5\_NFRC\_2003.std).  This difference accounts for most of the variation in SHGC values reported by EnergyPlus and WINDOW for full spectral data window layer input.  This variation is more pronounced for window constructions of three glass layers or more.
-
-- Users intending to select a window construction based on SHGC value for energy code compliance should base their selection on the value reported by WINDOW since this is the officially recognized value.
-
-In EnergyPlus, the Window data file is searched for each “Construction:WindowDataFile� object in the EnergyPlus input. This object has a very simple form:
-
-```idf
-Construction:WindowDataFile,
-ConstructionName,
-FileName; ! Default is Window5DataFile.dat in the “run� folder.
-```
-
-
-If there is a window called ConstructionName on the Window data file, the data for that window is read from the file and the following EnergyPlus objects and their names are created. The “W5� prefixed to these names indicates that the object originated in the Window data file.
-
-
-
-### Zone Thermal Output(s)
-
-In addition to the canned Surface reports (view the Reports section later in this document) and surface variables (above), the following variables are available for all zones:
-
-* Zone,Sum,Zone Total Internal Radiant Heating Energy [J]
-
-* Zone,Sum,Zone Total Internal Visible Radiation Heating Energy [J]
-
-* Zone,Sum,Zone Total Internal Convective Heating Energy [J]
-
-* Zone,Sum,Zone Total Internal Latent Gain Energy [J]
-
-* Zone,Sum,Zone Total Internal Total Heating Energy [J]
-
-* Zone,Average,Zone Mean Air Temperature [C]
-
-* HVAC,Average,Zone Air Temperature [C]
-
-* Zone,Average,Zone Mean Radiant Temperature [C]
-
-* Zone,Average,Zone Operative Temperature [C]
-
-* HVAC,Sum,Zone Air System Sensible Heating Energy [J]
-
-* HVAC,Sum,Zone Air System Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Air System Sensible Heating Rate [W]
-
-* HVAC,Average,Zone Air System Sensible Cooling Rate [W]
-
-* HVAC,Average,Zone Air Humidity Ratio[kgWater/kgDryAir]
-
-* HVAC,Average,Zone Air Relative Humidity[%]
-
-* Two of these are of particular interest:
-
-* Zone,Average,Zone Mean Air Temperature [C]
-
-* HVAC,Average,Zone Air Temperature [C]
-
-
-These two variable outputs are/should be identical. However, note that they can be reported at different time intervals. “Zone Mean Air Temperature� is only available on the Zone/HB timestep (Number of Timesteps per Hour) whereas “Zone Air Temperature� can be reported at the HVAC timestep (which can vary).
-
-#### Zone Mean Air Temperature [C]
-
-From the code definition, the zone mean air temperature is the average temperature of the air temperatures at the system timestep. Remember that the zone heat balance represents a “well stirred� model for a zone, therefore there is only one mean air temperature to represent the air temperature for the zone.
-
-#### Zone Air Temperature [C]
-
-This is very similar to the mean air temperature in the last field. The “well stirred� model for the zone is the basis, but this temperature is also available at the “detailed� system timestep.
-
-#### Zone  Mean Radiant Temperature [C]
-
-The Mean Radiant Temperature (MRT) in degrees Celsius of a space is really the measure of the combined effects of temperatures of surfaces within that space. The larger the surface area and the closer one is to it, the more effect the surface temperature of that surface has on each other. The MRT is the measure of all these surface areas and temperatures.
-
-#### Zone Operative Temperature [C]
-
-Zone Operative Temperature (OT) is the average of the Zone Mean Air Temperature (MAT) and Zone Mean Radiant Temperature (MRT),  OT = 0.5\*MAT + 0.5\*MRT.  This output variable is not affected by the type of thermostat controls in the zone, and does not include the direct effect of high temperature radiant systems.  See also Zone Thermostat Operative Temperature.
-
-#### Zone Air System Sensible Heating Energy [J]
-
-This field represents the sensible heating energy in Joules that is actually supplied by the system to that zone for the timestep reported. This is the sensible heating rate multiplied by the simulation timestep. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module. . This field is not multiplied by zone or group multipliers.
-
-Zone Air System Sensible Heating (and Cooling) Energy (and Rate) all report the heating or cooling delivered by the HVAC system to a zone. These values are calculated by multiplying the supply air mass flow rate by the difference between the supply air temperature and the zone air temperature. This does not always indicate the operation of heating or cooling coils. For example, cooling will be reported if the supply air is cooled due to the introduction of outside air, even if all coils are off.
-
-Note that these variables are calculated at the system timestep. When reported at the "detailed" reporting frequency, these variable will never show heating and cooling both in the same system timestep. If reported at a frequency less than "Detailed" (for example, Hourly) values may appear in both the heating and cooling variable for the same hour if the system cooled the zone for part of the reporting period and heated the zone for another part of the reporting period.
-
-#### Zone Air System Sensible Cooling Energy [J]
-
-This field represents the sensible cooling energy in Joules that is actually supplied by the system to that zone for the timestep reported. This is the sensible cooling rate multiplied by the simulation timestep. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module.   This field is not multiplied by zone or group multipliers.
-
-#### Zone Air System Sensible Heating Rate [W]
-
-This field represents the sensible heating rate in Watts that is actually supplied by the system to that zone for the timestep reported. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module.   This field is not multiplied by zone or group multipliers.
-
-#### Zone Air System Sensible Cooling Rate [W]
-
-This field represents the sensible cooling rate in Watts that is actually supplied by the system to that zone for the timestep reported. This is calculated and reported from the Correct step in the Zone Predictor-Corrector module.   This field is not multiplied by zone or group multipliers.
-
-#### Zone Air Humidity Ratio[kgWater/kgDryAir]
-
-This field represents the air humidity ratio after the correct step for each zone. The humidity ratio is the mass of water vapor to the mass of dry air contained in the zone in (kg water/kg air) and is unitless.
-
-#### Zone Air Relative Humidity[%]
-
-This field represents the air relative humidity ratio after the correct step for each zone. The relative humidity is in percent and uses the Zone Air Temperature, the Zone Air Humidity Ratio and the Outside Barometric Pressure for calculation.
-
-#### Zone Total Internal Radiant Heating Energy [J]
-
-This field represents the sum of radiant gains from specific internal sources  (e.g. equipment) throughout the zone in joules. This includes radiant gain from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
-
-#### Zone-Total Internal Visible Heat Gain [J]
-
-This field expresses the sum of heat gain in joules that is the calculated short wavelength radiation gain from lights in the zones. This calculation uses the total energy from lights and the fraction visible to realize this value, summed over the zones in the simulation.
-
-#### Zone Total Internal Convective Heating Energy [J]
-
-This field represents the sum of convective gains from specific sources (e.g. equipment) throughout the zone in joules. This includes convective gain from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
-
-#### Zone Total Internal Latent Gain Energy [J]
-
-This field represents the sum of latent gains from specific internal sources (e.g. equipment) throughout the zone in joules. This includes latent gain from People, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
-
-#### Zone Total Internal Total Heating Energy [J]
-
-This field represents the sum of all heat gains throughout the zone in joules. This includes all heat gains from People, Lights, Electric Equipment, Gas Equipment, Other Equipment, Hot Water Equipment, and Steam Equipment.
-
-Group – Advanced Surface Concepts
----------------------------------
-
-This group of objects describe concepts applied to heat transfer surfaces that are of an advanced nature. Careful consideration must be given before using these.
-
-### SurfaceProperty:HeatTransferAlgorithm
-
-This object, and three other related objects, can be used to control which surface heat transfer model is used on specific surfaces.  The separate object called HeatBalanceAlgorithm is used to control the heat transfer model in an overall way while this object can be used to revise the algorithm selections for specific surfaces.  This object allows selectively overriding the global setting in HeatBalanceAlgorithm to choose one of the following models for a particular surface:
-
-- CTF (Conduction Transfer Functions),
-
-- EMPD (Effective Moisture Penetration Depth with Conduction Transfer Functions).
-
-- CondFD (Conduction Finite Difference)
-
-- HAMT (Combined Heat And Moisture Finite Element)
-
-#### Field: Surface Name
-
-This is the name of the surface that will be assigned to use the heat transfer algorithm selected in the next field.  This should be a name of a surface defined elsewhere.
-
-#### Field: Algorithm
-
-This field is used to determine the heat transfer algorithm that is to be applied to the surface named in the previous field.  The allowable choices are:
-
-- ConductionTransferFunction
-
-- MoisturePenetrationDepthConductionTransferFunction
-
-- ConductionFiniteDifference
-
-- CombinedHeatAndMoistureFiniteElement
-
-### SurfaceProperty:HeatTransferAlgorithm:MultipleSurface
-
-This object can be used to control the surface heat transfer model used for specific types of surfaces.  The separate object called HeatBalanceAlgorithm is used to control the heat transfer model in an overall way while this object can be used to revise the algorithm selections for specific types of surfaces.  This object allows selectively overriding the global setting in HeatBalanceAlgorithm to choose one of the following models for all surfaces of a particular type:
-
-- CTF (Conduction Transfer Functions),
-
-- EMPD (Effective Moisture Penetration Depth with Conduction Transfer Functions).
-
-- CondFD (Conduction Finite Difference)
-
-- HAMT (Combined Heat And Moisture Finite Element)
-
-#### Field: Name
-
-This is a unique, user-defined name for the object.
-
-#### Field: Surface Type
-
-This field is selects the type of surfaces that are all assigned to use the heat transfer algorithm selected in the next field.  This field is used with one of the following allowable keywords:
-
-- AllExteriorSurfaces—all surfaces that have “Outdoors� outside boundary condition
-
-- AllExteriorWalls—all walls that have “Outdoors� outside boundary condition
-
-- AllExteriorRoofs—all roofs that have “Outdoors� outside boundary condition
-
-- AllExteriorFloors—all floors that have “Outdoors� outside boundary condition
-
-- AllGroundContactSurfaces—all surfaces that have “Ground� outside boundary condition
-
-- AllInteriorSurfaces—all surfaces that are internal partition-type surfaces
-
-- AllInteriorWalls—all walls that are internal surfaces
-
-- AllInteriorCeilings—all ceilings that are internal surfaces
-
-- AllInteriorFloors—all floors that are are internal surfaces
-
-#### Field: Algorithm
-
-This field is used to determine the heat transfer algorithm that is to be applied to the surface types in the previous field.  The allowable choices are:
-
-- ConductionTransferFunction
-
-- MoisturePenetrationDepthConductionTransferFunction
-
-- ConductionFiniteDifference
-
-- CombinedHeatAndMoistureFiniteElement
-
-```idf
-SurfaceProperty:HeatTransferAlgorithm:MultipleSurface,
-    my exterior wall override,
-    AllExteriorWalls,
-    ConductionFiniteDifference;
-```
-
-
-### SurfaceProperty:HeatTransferAlgorithm:SurfaceList
-
-This object can be used to control the surface heat transfer model used for a list of surfaces.  The separate object called HeatBalanceAlgorithm is used to control the heat transfer model in an overall way while this object can be used to revise the algorithm selections for a list of specific surfaces.  This object allows selectively overriding the global setting in HeatBalanceAlgorithm to choose one of the following models for listed:
-
-- CTF (Conduction Transfer Functions),
-
-- EMPD (Effective Moisture Penetration Depth with Conduction Transfer Functions).
-
-- CondFD (Conduction Finite Difference)
-
-- HAMT (Combined Heat And Moisture Finite Element)
-
-#### Field: Name
-
-This is a unique, user-defined name for the object.
-
-#### Field: Algorithm
-
-This field is used to determine the heat transfer algorithm that is to be applied to the surface listed in the remaining fields.  The allowable choices are:
-
-- ConductionTransferFunction
-
-- MoisturePenetrationDepthConductionTransferFunction
-
-- ConductionFiniteDifference
-
-- CombinedHeatAndMoistureFiniteElement
-
-#### Field: Surface Name N
-
-This is the name of the “Nth� surface that will be assigned to use the heat transfer algorithm selected in this object.  These should be the names of surfaces defined elsewhere. This object is extensible.  Additional surfaces can be added to extend the object.
-
-An example IDF object follows.
-
-```idf
-SurfaceProperty:HeatTransferAlgorithm:SurfaceList,
-    my wall construct override,   !- Name
-    ConductionFiniteDifference,   !- Algorithm
-    Zn001:Wall001,                !- Surface Name 1
-    Zn001:Wall002,                !- Surface Name 2
-    Zn001:Wall003,                !- Surface Name 3
-    Zn001:Wall004;                !- Surface Name 4
-```
-
-### SurfaceProperty:HeatTransferAlgorithm:Construction
-
-This object can be used to control the surface heat transfer model used for surfaces that have a specific type of construction.  The separate object called HeatBalanceAlgorithm is used to control the heat transfer model in an overall way while this object can be used to revise the algorithm selections for specific constructions.  This object allows selectively overriding the global setting in HeatBalanceAlgorithm to choose one of the following models for all surfaces with particular type of construction:
-
-- CTF (Conduction Transfer Functions),
-
-- EMPD (Effective Moisture Penetration Depth with Conduction Transfer Functions).
-
-- CondFD (Conduction Finite Difference)
-
-- HAMT (Combined Heat And Moisture Finite Element)
-
-#### Field: Name
-
-This is a unique, user-defined name for the object.
-
-#### Field: Algorithm
-
-This field is used to determine the heat transfer algorithm that is to be applied to the surfaces with the type of of construction listed in the next field.  The allowable choices are:
-
-- ConductionTransferFunction
-
-- MoisturePenetrationDepthConductionTransferFunction
-
-- ConductionFiniteDifference
-
-- CombinedHeatAndMoistureFiniteElement
-
-#### Field: Construction Name
-
-This field is the name of a Construction object defined elsewhere.  All the surfaces in the model that are assigned this type of construction will be assigned to use the heat transfer algorithm slected in the previous field.
-
-An example IDF object follows.
-
-```idf
-SurfaceProperty:HeatTransferAlgorithm:Construction,
-    my wall construct override,  !- Name
-    ConductionFiniteDifference,  !- Algorithm
-    R13WALL;                     !- Construction Name
-```
-
-
-### SurfaceControl:MoveableInsulation
-
-Movable insulation can be used/scheduled on any surface regular surface (such as a wall, floor, roof, etc.) but not on a subsurface (such as a window, use WindowProperty:ShadingControl instead). With movable insulation, no reference is made in the surface that is using the insulation – rather the movable insulation statement references the surface to which it is applied.
-
-Exterior and interior movable insulation have undergone some testing and appears to producing expected results. The underlying principle has been implemented in EnergyPlus for both interior and exterior movable insulation with the possibility for exterior movable insulation to be transparent (transparent insulation material or TIM).
-
-TIM exterior layers can be used with the ConductionFiniteDifference (CondFD) solution algorithm. With this addition, TIM layers can be used in conjunction with wall layers that have phase change materials (PCM) included, or any other advanced capability of the CondFD algorithm such as variable conductivity. The input requirements are exactly the same as when used with the CTF algorithm. The Solution Algorithm needs to be changed to CondFD, and as with CTF, the “SurfaceControl:MovableInsulation� object must be completed to specify the insulated surface and the “WindowMaterial:Glazing� object is needed to provide the TIM layer properties.
-
-Basically, the addition of movable insulation allows the user to schedule an extra amount of insulation on either the inside or outside surface of a wall (or both). The insulation must be a simple, homogenous material layer (linked to a material definition within the input data file). Note that EnergyPlus allows the exterior movable insulation layer to be transparent to short wavelength radiation (solar). In this case, incident solar is split between the plane between the movable insulation and the surface and the plane between the movable insulation and the surrounding air. This calculation is fairly basic and based on the solar transmittance of the insulation layer (material properties). Using transparent layers for exterior movable insulation allows solar energy to penetrate deeper into a construction where it can be stored for later use in the building (similar in concept to a Trombe Wall).
-
-#### Field: Insulation Type
-
-This field determines whether the movable insulation is applied to the inside or the outside of the surface by entering either “Inside� or “Outside�, respectively.
-
-#### Field: Surface Name
-
-This field refers the movable insulation back to a particular surface (ref: Building Surfaces) via its user assigned name so that EnergyPlus knows where to apply this extra layer of insulation. This will affect either the inside or outside surface heat balance of this surface depending on the value in the insulation type field (see previous field).
-
-#### Field: Material Name
-
-This field refers to a material layer (e.g., Material, Material:NoMass, or WindowMaterial:Glazing; transparent layers are only valid for outside movable insulation) via its user assigned name. This provides the program with a full complement of material properties so that the effect of the insulation (R-value and solar transmittance) can be correctly taken into account by EnergyPlus.
-
-#### Field: Schedule Name
-
-This field is a schedule that theoretically can be any positive real number but was originally intended to be a parameter between 0.0 and 1.0. Its purpose is to act as a fractional modifier on the resistance of the material layer. The actual thermal resistance of the movable insulation is equal to the resistance of the material layer times the current value in the movable insulation schedule. A value of 0.0 simply means that the movable insulation is not present.
-
-An example of this syntax implemented in an input file is:
-
-```idf
-SurfaceControl:MoveableInsulation,
-  Exterior,                      ! Insulation Type
-  Zone001:Wall001,               ! Surface Name
-  TransparentInsulationMaterial, ! Material Name
-  PresentInWinterSchedule;       ! Schedule Name
-```
-
-
-### SurfaceProperty:OtherSideCoefficients
-
-By referencing the Other Side Coefficients statement in the surface statements (i.e. Outside Boundary Condition), the temperature of the outer plane of a surface (see Figure 41) can be directly controlled. Other side coefficients can also be used to control the exterior convective heat transfer coefficient of a surface and the corresponding exterior air temperature. It should be noted that solar effects are not accounted for when other side coefficients are used. In addition, if other side coefficients are specified for a surface, they also hold for subsurfaces of that surface (though subsurfaces can have their own coefficient set).
-
-other side coefficients have the same effect on all types of heat transfer surfaces. In other words, an interior surface with other side coefficients specified and an exterior wall with identical other side coefficients specified are simulated exactly the same. A surface that uses other side coefficients should be thought of as a new or separate type of surface. All heat transfer surfaces are simulated in the same manner through conduction transfer functions. The only difference between the various types of heat transfer surfaces is the environment on the other side of the surface. For example, the other side environment of an exterior surface is the outdoor environment. For an interior surface, the temperature of the outer plane of the surface is set equal to the temperature of the inner plane of the surface. Similarly, a surface with other side coefficients specified will allow the user to control the other side environment.
-
-Heat transfer through a surface is an extremely important component in the calculation of zone loads. The information to calculate this heat transfer is readily available if the surface is exposed to the outdoor environment or to another zone that is being simulated. Occasionally, a user will want to model the heat transfer through a surface that is adjacent to an area that is not included in the EnergyPlus model.  For example, an office area is attached to a warehouse and the user is only interested in simulating the office area. An interior surface with other side coefficients specified could be used to control the environment on the other side of the surface, thereby accounting for the heat transfer through the adjoining surface.
-
-Other Side Coefficients affects the "other side" of a surface as described below. Each coefficient has a special meaning. You may enter a 0 or blank if you are not using a particular coefficient. Note that there are two potential ways to use other side coefficients. Either they are used to set the temperature of the exterior side surface directly (if the combined convective/radiative coefficient below is less than or equal to zero) or to set both the film coefficient (positive value for the combined convective/radiative coefficient below) and the outside air temperature.
-
-#### Field: Name
-
-This, of course, is the string referenced in the Surface statement that is using OtherSideCoefficients as the Outside Boundary Condition.
-
-#### Field: Combined Convective/Radiative Film Coefficient
-
-This is a trigger value. If the value is greater than zero, then it is taken to be the combined convective/radiative film coefficient. In this case (value &gt; 0), the remaining fields are used first to calculate the outside air temperature for the surface and then to calculate the outside surface temperature based on the outside air temperature and the film coefficient. If this field is less than or equal to zero, then the remaining fields are used to calculate the surface temperature (not the outside air temperature). The units for this field are the same as for a convective heat transfer coefficient: W/(m<sup>2</sup>\*K). This is referred to as “C1� in the reference below.
-
-#### Field: Constant Temperature
-
-This field defines a temperature term that is a constant part of the calculation either of the surface or outside air temperature. This parameter is shown as “C2� in the equation below. The units for this parameter are degrees C. If a schedule name is included as the second parameter, the value of this parameter will be overridden by the value from the schedule. The default for this field is 0.0.
-
-#### Field: Constant Temperature Coefficient
-
-This field defines a constant coefficient that is applied to the constant temperature (see previous field). This parameter is shown as “C3� in the equation below. This parameter is dimensionless. The value of this parameter is usually 1.0 if a schedule is used to set C2. This field is ignored if *Sinusoidal Variation of Constant Temperature Coefficient* = Yes. The default for this field is 1.0.
-
-#### Field: External Dry-Bulb Temperature Coefficient
-
-This field defines a constant coefficient that is applied to the outside air dry-bulb temperature. This parameter is shown as “C4� in the equation below. This parameter is dimensionless. The default for this field is 0.0.
-
-#### Field: Ground Temperature Coefficient
-
-This field defines a constant coefficient that is applied to the ground temperature (ref. Site:GroundTemperature:BuildingSurface). This parameter is shown as “C5� in the equation below. This parameter is dimensionless.
-
-#### Field: Wind Speed Coefficient
-
-This field defines a constant coefficient that is applied to the product of the outside air dry-bulb temperature and the wind speed. This parameter is shown as “C6� in the equation below. This parameter has dimensions of inverse velocity or s/m. The default for this field is 0.0.
-
-#### Field: Zone Air Temperature Coefficient
-
-This field defines a constant coefficient that is applied to the temperature of the zone to which this surface belongs. This parameter is shown as “C7� in the equation below. This parameter is dimensionless. The default for this field is 0.0.
-
-#### Field: Constant Temperature Schedule Name
-
-This field is used to supply a schedule name. That schedule will supply the “constant� temperature value C2. Note that the value of the C3 field should normally be 1.0 if a schedule is used for C2. If not blank, this field must be a valid schedule name.
-
-#### Field: Sinusoidal Variation of Constant Temperature Coefficient
-
-This field is optional and can be used to define an alternate method of prescribing the coefficient that is applied to the constant temperature (see the fields Constant Temperature and Constant Temperature Coefficient).  This parameter is shown as “C2� in the equation below.  If this field is omitted, left blank, or set to “No,� then C2 is a constant (defined in the field Constant Temperature Coefficient).  However if this is set to “Yes,� then the value of C2 varies with a unitary sine wave in the following way:
-
-<div>\[C2 = Sin\left( {2\pi \frac{{\left( {time\,of\,day} \right)}}{{\left( {period} \right)}}} \right)\]</div>
-
-The value for “period� is controlled in the following field.  The value for “time of day� is based on the zone timestep and is in units of hours.  The sine function here uses input as radians.  When using this option, the value for C2 will vary between -1.0 and 1.0 and the value put in the field Constant Temperature Coefficient is not used.  This option cannot be used at the same time as scheduling a constant temperature with the previous field.
-
-#### Field: Period of Sinusoidal Variation
-
-This field is used to define the period of the sine wave when using the Sinusodial Variation of Constant Temperature Coefficient capability selected in the previous field.  This field is the time period of the sine wave in units of hours.  The default is 24 hours and provides a diurnal sine wave.  The value entered here is “period� in the equation in the previous field.
-
-#### Field: Previous Other Side Temperature Coefficient
-
-This field defines a constant coefficient that is applied to the other side temperature computed by this object from the previous zone time step. This parameter is shown as “C8� in the equation below. This parameter is dimensionless. The default for this field is 0.0.
-
-#### Field: Minimum Other Side Temperature Limit
-
-This field specifies a lower limit for the other side temperature result in degrees C. If blank, there is no lower limit.
-
-#### Field: Maximum Other Side Temperature Limit
-
-This field specifies an upper limit for the other side temperature result in degrees C. If blank, there is no upper limit.
-
-The coefficients listed above are used in the following equation:
-
-<div>\[T = C2*C3 + C4*Toadb + C5*Tgrnd + C6*Wspd*Toadb + C7*Tzone + C8*Tpast\]</div>
-
-where:
-
-T = Outside Air Temperature when C1 (Combined convective/radiative film Coeff) &gt; 0
-
-T = Exterior Surface Temperature when C1 (Combined convective/radiative film Coeff) &lt;= 0
-
-Tzone  = Temperature of the zone being simulated (°C)
-
-Toadb  = Dry-bulb temperature of the outdoor air (°C)
-
-Tgrnd  = Temperature of the ground (°C) from Site:GroundTemperature:BuildingSurface
-
-Wspd  = Outdoor wind speed (m/sec)
-
-Tpast  = Other side temperature from previous zone timestep (°C)
-
-![](media/image069.svg)
-
-Figure 41. Illustration for Other Side Coefficients
-
-```idf
-!  Example input using temperature schedule
-SurfaceProperty:OtherSideCoefficients,
-    OSCCoef:Zn005:Wall003,   !- Name
-    0,                       !- Combined Convective/Radiative Film Coefficient {W/m2-K}
-    0.000000,                !- Constant Temperature {C}
-    1.000000,                !- Constant Temperature Coefficient
-    0.000000,                !- External Dry-Bulb Temperature Coefficient
-    0.000000,                !- Ground Temperature Coefficient
-    0.000000,                !- Wind Speed Coefficient
-    0.000000,                !- Zone Air Temperature Coefficient
-    Zn005Wall003OtherSideTempSched;  !- Constant Temperature Schedule Name
-
-
-!  Example input for outside heat transfer coefficient of 1.23, using Tosdb
-SurfaceProperty:OtherSideCoefficients,
-    OSCCoef:Zn005:Wall004,   !- Name
-    1.230000,                !- Combined Convective/Radiative Film Coefficient {W/m2-K}
-    0.000000,                !- Constant Temperature {C}
-    0.000000,                !- Constant Temperature Coefficient
-    1.000000,                !- External Dry-Bulb Temperature Coefficient
-    0.000000,                !- Ground Temperature Coefficient
-    0.000000,                !- Wind Speed Coefficient
-    0.000000,                !- Zone Air Temperature Coefficient
-    ,                        !- Constant Temperature Schedule Name
-    No,                      !- Sinusoidal Variation of Constant Temperature Coefficient
-    24,                      !- Period of Sinusoidal Variation {hr}
-    0.,                      !- Previous Other Side Temperature Coefficient
-    ,                        !- Minimum Other Side Temperature Limit {C}
-    ;                        !- Maximum Other Side Temperature Limit {C}
-```
-
-
-### SurfaceProperty:OtherSideCoefficients Outputs
-
-Zone,Average,Surface Other Side Coefficients Exterior Air Drybulb Temperature
-
-#### Surface Other Side Coefficients Exterior Air Drybulb Temperature [C]
-
-This is the air temperature applied to the other side of the surface.
-
-### SurfaceProperty:OtherSideConditionsModel
-
-By referencing the Other Side Conditions Model statement in the surface statements (i.e. Outside Boundary Condition), the boundary conditions for the outer plane of the mass wall can be connected to the appropriate model for various multi-skin components. The types of multi-skin components that use this object include systems that are mounted to the outside surface using standoffs that create a small air gap – see Figure 42. This type of modeling allows using the usual heat transfer calculations for the underlying surface with other types of multi-skin  component models that are available including: unglazed transpired solar collectors, ventilated photovoltaic panels, and naturally ventilated facades.
-
-The boundary condition values are determined dynamically by the program using internal component models. If you want to define other side surface temperatures or convection conditions, then use SurfaceProperty:OtherSideCoefficients instead of this object.
-
-It should be noted that when other side conditions models are used, solar effects are removed from the surface’s outside face heat balance, but are used in modeling the component adjacent to that surface.
-
-In addition, the other side conditions model has been modified to include underground piping system interaction.  The PipingSystem:Underground:Domain object represents a mass of ground which may include interaction with, for example, basement surfaces.  In this case, the ground model will internally use the other side condition model hook to update boundary conditions for those surfaces which use that other side condition model name reference.
-
-#### Field: Name
-
-This is the string referenced in the Surface statement that is using OtherSideModel as the Exterior Environment.
-
-#### Field: Type of Modeling
-
-This is a string key selection used to identify the type of model that will be used to determine boundary conditions. The only available choices are �GapConvectionRadiation,� “UndergroundPipingSystemSurface,� and "GroundCoupledSurface."
-
-![OtherSideConditionsFig](media/image070.png)
-
-Figure 42. Illustration for Other Side Conditions Model
-
-An example specification is:
-
-```idf
-SurfaceProperty:OtherSideConditionsModel,
-    UTSC OSCM ZN11,          ! OtherSideConditionsModel Name
-    GapConvectionRadiation; ! Type of Modeling used to determine Boundary Conditions
-```
-
-### SurfaceProperty:OtherSideConditionsModel Outputs
-
-* Zone,Average,Surface Other Side Conditions Modeled Convection Air Temperature [C]
-
-* Zone,Average,Surface Other Side Conditions Modeled Convection Heat Transfer Coefficient [W/m2-K]
-
-* Zone,Average,Surface Other Side Conditions Modeled Radiation Temperature [C]
-
-* Zone,Average,Surface Other Side Conditions Modeled Radiation Heat Transfer Coefficient [W/m2-K]
-
-#### Surface Other Side Conditions Modeled Convection Air Temperature [C]
-
-This is the air temperature exposed to the other side of the surface by the model and used in convection heat transfer calculations.
-
-#### Surface Other Side Conditions Modeled Convection Heat Transfer Coefficient [W/m2-K]
-
-This is the surface convection heat transfer coefficient applied to the other side of the surface by the model.
-
-#### Surface Other Side Conditions Modeled Radiation Temperature [C]
-
-This is the effective temperature exposed to the other side of the surface for thermal radiation heat transfer calculations.
-
-#### Surface Other Side Conditions Modeled Radiation Heat Transfer Coefficient [W/m2-K]
-
-This is the effective (Iinearized) radiation heat transfer coefficient applied to the other side of the surface by the model.
-
-### SurfaceConvectionAlgorithm:Inside:AdaptiveModelSelections
-
-This object provides options to change the individual convection model equations for dynamic selection when using AdaptiveConvectionAlgorithm. This object is only needed to make changes to the default model selections for any or all of the surface categories. This object is for the inside face, the side of the surface facing a thermal zone.
-
-#### Field: Name
-
-A unique name for the object.
-
-#### Field: Simple Buoyancy Vertical Wall Equation Source
-
-Applies to zone with no HVAC or when HVAC is off.  This is for vertical walls.  The key choice options include:  FohannoPolidoriVerticalWall, ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq3WallAwayFromHeat, KhalifaEq6NonHeatedWalls FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve
-
-#### Field: Simple Buoyancy Vertical Wall User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
-
-#### Field: Simple Buoyancy Stable Horizontal Equation Source
-
-Applies to zone with no HVAC or when HVAC is off.  This is for horizontal surfaces with heat flow directed for stable thermal stratification.  The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve
-
-#### Field: Simple Buoyancy Stable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
-
-#### Field: Simple Buoyancy Unstable Horizontal Equation Source
-
-Applies to zone with no HVAC or when HVAC is off. This is for passive horizontal surfaces with heat flow for unstable thermal stratification.  The key choice options include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
-
-#### Field: Simple Buoyancy Unstable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Simple Buoyancy Stable Tilted Equation Source
-
-Applies to zone with no HVAC or when HVAC is off.  This is for tilted surfaces with heat flow for stable thermal stratification.  The key choice options include:  WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve
-
-#### Field: Simple Buoyancy Stable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Simple Buoyancy Unstable Tilted Equation Source
-
-Applies to zone with no HVAC or when HVAC is off.  This is for tilted surfaces with heat flow for unstable thermal stratification.  The key choices include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
-
-#### Field: Simple Buoyancy Unstable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Simple Buoyancy Windows Equation Source
-
-Applies to zone with no HVAC or when HVAC is off.  This is for all window surfaces. The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, KaradagChilledCeiling, ISO15099Windows, or UserCurve.
-
-#### Field: Simple Buoyancy Windows Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Vertical Wall Equation Source
-
-Applies to zone with in-floor heating and/or in-ceiling cooling.  This is for vertical walls.  The key choice options include:  ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq3WallAwayFromHeat, FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Vertical Wall Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Stable Horizontal Equation Source
-
-Applies to zone with in-floor heating and/or in-ceiling cooling. This is for passive horizontal surfaces with heat flow for stable thermal stratification.  The key choice options include:  WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Stable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Unstable Horizontal Equation Source
-
-Applies to zone with in-floor heating and/or in-ceiling cooling. This is for passive horizontal surfaces with heat flow for unstable thermal stratification.  The key choice options include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, KhalifaEq4CeilingAwayFromHeat, or UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Unstable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Heated Floor Equation Source
-
-Applies to zone with in-floor heating and/or in-ceiling cooling.  This is for a floor with active heating elements.  The key choice options include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, AwbiHattonHeatedFloor, or UserCurve
-
-#### Field: Floor Heat Ceiling Cool Heated Floor Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Chilled Ceiling Equation Source
-
-Applies to zone with in-floor heating and/or in-ceiling cooling. This is for a ceiling with active cooling elements. The key choice options include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, KaradagChilledCeiling, or UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Chilled Ceiling Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
-
-#### Field: Floor Heat Ceiling Cool Stable Tilted Equation Source
-
-Applies to zone with in-floor heating and/or in-ceiling cooling. This is for tilted surfaces with heat flow for stable thermal stratification.  The key choice options include:  WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, ISO15099Windows, or UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Stable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Unstable Tilted Equation Source
-
-Applies to zone with in-floor heating and/or in-ceiling cooling.  This is for tilted surfaces with heat flow for unstable thermal stratification.  The key choice options include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, ISO15099Windows, or UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Unstable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Window Equation Source
-
-Applies to zone with in-floor heating and/or in-ceiling cooling. This is for all window surfaces.  The key choice options include:  ASHRAEVerticalWall, AlamdariHammondVerticalWall, ISO15099Windows, or UserCurve.
-
-#### Field: Floor Heat Ceiling Cool Window Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Wall Panel Heating Vertical Wall Equation Source
-
-Applies to zone with in-wall panel heating. This is for vertical walls that are not actively heated.  The key choice options include:  ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq6NonHeatedWalls, FohannoPolidoriVerticalWall, AlamdariHammondVerticalWall, ISO15099Windows, or UserCurve.
-
-#### Field: Wall Panel Heating Vertical Wall Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Wall Panel Heating Heated Wall Equation Source
-
-Applies to zone with in-wall panel heating. This is for vertical walls that are being actively heated.  The key choice options include:  ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq5WallNearHeat, AwbiHattonHeatedWall, FohannoPolidoriVerticalWall, AlamdariHammondVerticalWall, or UserCurve.
-
-#### Field: Wall Panel Heating Heated Wall Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Wall Panel Heating Stable Horizontal Equation Source
-
-Applies to zone with in-wall panel heating. This is for horizontal surfaces with heat flow directed for stable thermal stratification. The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
-
-#### Field: Wall Panel Heating Stable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Wall Panel Heating Unstable Horizontal Equation Source
-
-Applies to zone with in-wall panel heating. This is for horizontal surfaces with heat flow directed for unstable thermal stratification. The key choice options include: ASHRAEVerticalWall, WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, KhalifaEq7Ceiling, or UserCurve
-
-#### Field: Wall Panel Heating Unstable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Wall Panel Heating Stable Tilted Equation Source
-
-Applies to zone with in-wall panel heating. This is for tilted surfaces with heat flow for stable thermal stratification.  The key choice options include:  WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, ISO15099Windows, or UserCurve.
-
-#### Field: Wall Panel Heating Stable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
-
-#### Field: Wall Panel Heating Unstable Tilted Equation Source
-
-Applies to zone with in-wall panel heating. This is for tilted surfaces with heat flow for unstable thermal stratification. The key choice options include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, ISO15099Windows, or UserCurve.
-
-#### Field: Wall Panel Heating Unstable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Wall Panel Heating Window Equation Source
-
-Applies to zone with in-wall panel heating. This is for all window surfaces.  The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve.
-
-#### Field: Wall Panel Heating Window Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Convective Zone Heater Vertical Wall Equation Source
-
-Applies to zone with convective heater.  This is for vertical walls not directly affected by heater.  The key choice options include: ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq3WallAwayFromHeat, KhalifaEq6NonHeatedWalls, FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve
-
-#### Field: Convective Zone Heater Vertical Wall Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Convective Zone Heater Vertical Walls Near Heater Equation Source
-
-Applies to zone with convective heater. This is for vertical walls that are directly affected by heater. Walls are considered "near" when listed in field set for Fraction of Radiant Energy to Surface.  The key choice options include:  ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq5WallNearHeat, AwbiHattonHeatedWall, FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve.
-
-#### Field: Convective Zone Heater Vertical Walls Near Heater Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Convective Zone Heater Stable Horizontal Equation Source
-
-Applies to zone with convective heater.  This is for horizontal surfaces with heat flow directed for stable thermal stratification. The key choice options include:  WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
-
-#### Field: Convective Zone Heater Stable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
-
-#### Field: Convective Zone Heater Unstable Horizontal Equation Source
-
-Applies to zone with convective heater.  This is for horizontal surfaces with heat flow directed for unstable thermal stratification.  The key choice options include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, KhalifaEq4CeilingAwayFromHeat, KhalifaEq7Ceiling, or UserCurve.
-
-#### Field: Convective Zone Heater Unstable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Convective Zone Heater Stable Tilted Equation Source
-
-Applies to zone with convective heater.  This is for tilted surfaces with heat flow for stable thermal stratification. The key choice options include:  WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
-
-#### Field: Convective Zone Heater Stable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Convective Zone Heater Unstable Tilted Equation Source
-
-Applies to zone with convective heater.  This is for tilted surfaces with heat flow for unstable thermal stratification.  The key choice options include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
-
-#### Field: Convective Zone Heater Unstable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Convective Zone Heater Windows Equation Source
-
-Applies to zone with convective heater.  This is for all window surfaces. The key choice options include:  ASHRAEVerticalWall, AlamdariHammondVerticalWall, KhalifaEq3WallAwayFromHeat, FohannoPolidoriVerticalWall, ISO15099Windows, or UserCurve.
-
-#### Field: Convective Zone Heater Windows Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Central Air Diffuser Wall Equation Source
-
-Applies to zone with mechanical forced central air with diffusers. This is for all wall surfaces.  The key choice options include:  ASHRAEVerticalWall, FisherPedersenCeilingDiffuserWalls, AlamdariHammondVerticalWall, BeausoleilMorrisonMixedAssistedWall, BeausoleilMorrisonMixedOpposingWall, FohannoPolidoriVerticalWall, ISO15099Windows, GoldsteinNovoselacCeilingDiffuserWalls, or UserCurve
-
-#### Field: Central Air Diffuser Wall Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Central Air Diffuser Ceiling Equation Source
-
-Applies to zone with mechanical forced central air with diffusers.  This is for all ceiling surfaces.  The key choice options include:  FisherPedersenCeilingDiffuserCeiling, BeausoleilMorrisonMixedStableCeiling, BeausoleilMorrisonMixedUnstableCeiling, or UserCurve.
-
-#### Field: Central Air Diffuser Ceiling Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Central Air Diffuser Floor Equation Source
-
-Applies to zone with mechanical forced central air with diffusers.  This is for all floor surfaces. The key choice options include:  FisherPedersenCeilingDiffuserFloor, BeausoleilMorrisonMixedStableFloor, BeausoleilMorrisonMixedUnstableFloor, GoldsteinNovoselacCeilingDiffuserFloor, or UserCurve.
-
-#### Field: Central Air Diffuser Floor Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Central Air Diffuser Window Equation Source
-
-Applies to zone with mechanical forced central air with diffusers.  This is for all window surfaces.  The key choice options include:  ASHRAEVerticalWall, FisherPedersenCeilingDiffuserWalls, BeausoleilMorrisonMixedAssistedWall, BeausoleilMorrisonMixedOpposingWall, FohannoPolidoriVerticalWall, AlamdariHammondVerticalWall, ISO15099Windows, GoldsteinNovoselacCeilingDiffuserWindow, or UserCurve.
-
-#### Field: Central Air Diffuser Window Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
-
-#### Field: Mechanical Zone Fan Circulation Vertical Wall Equation Source
-
-The key choice options include: KhalifaEq3WallAwayFromHeat, ASHRAEVerticalWall, FisherPedersenCeilingDiffuserWalls, AlamdariHammondVerticalWall, BeausoleilMorrisonMixedAssistedWall, BeausoleilMorrisonMixedOpposingWall, FohannoPolidoriVerticalWall, ISO15099Windows, GoldsteinNovoselacCeilingDiffuserWalls, or UserCurve.
-
-#### Field: Mechanical Zone Fan Circulation Vertical Wall Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
-
-#### Field: Mechanical Zone Fan Circulation Stable Horizontal Equation Source
-
-The key choice options include: WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
-
-#### Field: Mechanical Zone Fan Circulation Stable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Mechanical Zone Fan Circulation Unstable Horizontal Equation Source
-
-The key choice options include:  KhalifaEq4CeilingAwayFromHeat, WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
-
-#### Field: Mechanical Zone Fan Circulation Unstable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Mechanical Zone Fan Circulation Stable Tilted Equation Source
-
-The key choice options include:  WaltonStableHorizontalOrTilt or UserCurve
-
-#### Field Mechanical Zone Fan Circulation Stable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Mechanical Zone Fan Circulation Unstable Tilted Equation Source
-
-The key choice options include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
-
-#### Field: Mechanical Zone Fan Circulation Unstable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Mechanical Zone Fan Circulation Window Equation Source
-
-The key choice options include:  ASHRAEVerticalWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, ISO15099Windows, GoldsteinNovoselacCeilingDiffuserWindow, or UserCurve.
-
-#### Field: Mechanical Zone Fan Circulation Unstable Tilted Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
-
-#### Field: Mixed Regime Buoyancy Assisting Flow on Walls Equation Source
-
-The key choice options include:  BeausoleilMorrisonMixedAssistedWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, ASHRAEVerticalWall, FisherPedersenCeilingDiffuserWalls, GoldsteinNovoselacCeilingDiffuserWalls, or UserCurve.
-
-#### Field: Mixed Regime Buoyancy Assisting Flow on Walls Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Mixed Regime Buoyancy Oppossing Flow on Walls Equation Source
-
-The key choice options include:  BeausoleilMorrisonMixedOpposingWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, ASHRAEVerticalWall, FisherPedersenCeilingDiffuserWalls, GoldsteinNovoselacCeilingDiffuserWalls, or UserCurve
-
-#### Field: Mixed Regime Buoyancy Oppossing Flow on Walls Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve
-
-#### Field: Mixed Regime Stable Floor Equation Source
-
-The key choice options include:  BeausoleilMorrisonMixedStableFloor, WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve
-
-#### Field: Mixed Regime Stable Floor Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Mixed Regime Unstable Floor Equation Source
-
-The key choice options include:  BeausoleilMorrisonMixedUnstableFloor, WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
-
-#### Field: Mixed Regime Unstable Floor Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Mixed Regime Stable Ceiling Equation Source
-
-The key choice options include:  BeausoleilMorrisonMixedStableCeiling, WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, or UserCurve.
-
-#### Field: Mixed Regime Stable Ceiling Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Mixed Regime Unstable Ceiling Equation Source
-
-The key choice options include:  BeausoleilMorrisonMixedUnstableCeiling, WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, or UserCurve.
-
-#### Field: Mixed Regime Unstable Ceiling Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Mixed Regime Window Equation Source
-
-The key choice options include:  GoldsteinNovoselacCeilingDiffuserWindow, ISO15099Windows, or UserCurve.
-
-#### Field: Mixed Regime Window Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-### SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections
-
-Options to change the individual convection model equations for dynamic selection when using AdaptiveConvectionAlgorithm. This object is only needed to make changes to the default model selections for any or all of the surface categories. This object is for the outside face, the side of the surface facing away from the thermal zone.
-
-#### Field: Name
-
-A unique name for the object
-
-#### Field: Wind Convection Windward Vertical Wall Equation Source
-
-This is for just the wind-driven component of the total convection coefficient. The key choice options include: SimpleCombined, TARPWindward, MoWiTTWindward, DOE2Windward, NusseltJurges, McAdams, Mitchell, Blocken, Emmel, or UserCurve.
-
-#### Field: Wind Convection Windward Equation Vertical Wall User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Wind Convection Leeward Vertical Wall Equation Source
-
-This is for just the wind-driven component of the total convection coefficient. The key choice options include:  SimpleCombined, TARPLeeward, MoWiTTLeeward, DOE2Leeward, Emmel, NusseltJurges, McAdams, Mitchell, or UserCurve.
-
-#### Field: Wind Convection Leeward Vertical Wall Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Wind Convection Horizontal Roof Equation Source
-
-This is for just the wind-driven component of the total convection coefficient. The key choice options include:  SimpleCombined, TARPWindward, MoWiTTWindward, DOE2Windward, NusseltJurges, McAdams, Mitchell, Blocken, Emmel, ClearRoof, or UserCurve.
-
-#### Field: Wind Convection Horizontal Roof User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Natural Convection Vertical Wall Equation Source
-
-This is for just the natural convection portion of the total film coefficient. This is for vertical walls. The key choice options include:  ASHRAEVerticalWall, AlamdariHammondVerticalWall, FohannoPolidoriVerticalWall, ISO15099Windows, UserCurve, or None.
-
-#### Field: Natural Convection Vertical Wall Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Natural Convection Stable Horizontal Equation Source
-
-This is for just the natural convection portion of the total film coefficient.  This is for horizontal surfaces with heat flow directed for stable thermal stratification.  The key choice options include:  WaltonStableHorizontalOrTilt, AlamdariHammondStableHorizontal, UserCurve, or None.
-
-#### Field: Natural Convection Stable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-#### Field: Natural Convection Unstable Horizontal Equation Source
-
-This is for just the natural convection portion of the total film coefficient.  This is for horizontal surfaces with heat flow directed for unstable thermal stratification. The key choice optios include:  WaltonUnstableHorizontalOrTilt, AlamdariHammondUnstableHorizontal, UserCurve, or None
-
-#### Field: Natural Convection Unstable Horizontal Equation User Curve Name
-
-The SurfaceConvectionAlgorithm:UserCurve named in this field is used when the previous field is set to UserCurve.
-
-### SurfaceConvectionAlgorithm:Inside:UserCurve
-
-This object is used to describe a custom model equation for surface convection heat transfer coefficients. If more than one curve is referenced, or non-blank, then they are all used and the result is the simple addition of all the curve results.
-
-#### Field: Name
-
-Unique name of input object.
-
-#### Field: Reference Temperature for Convection Heat Transfer
-
-This field controls the nature of the reference temperature used with convection coefficient when calculating the heat flow at the surface. Select one of the three choices:  MeanAirTemperature, AdjacentAirTemperature,  SupplyAirTemperature.  MeanAirTemperature is the typical application for the classic convection model used with the complete mixing of room air.  AdjacentAirTemperature applies when used with Roomair models that account for temperature variations within the zone air and directs the model to use the temperature near the surface rather than the average for the entire zone.  SupplyAirTemperature directs the model to use the supply air conditions for the heat transfer conditions.
-
-#### Field: Hc Function of Temperature Difference Curve Name
-
-This field contains the name of separate performance curve or table object that describes *h<sub>c</sub>*, the convection coefficient, as a function of temperature difference. The curve's "x" is absolute value of delta-T (Surface temperature minus air temperature, (C))
-
-#### Field: Hc Function of Temperature Difference Divided by Height Curve Name
-
-This field contains the name of separate performance curve or table object that describes *h<sub>c</sub>*, the convection coefficient, as a function of temperature difference divided by height. The curve's "x" is absolute value of delta-T/Height (Surface temp minus Air temp)/(vertical length scale), (C/m).  For an inside face, the vertical length scale is the zone's interior height.
-
-#### Field: Hc Function of Air Change Rate Curve Name
-
-This field contains the name of separate performance curve or table object that describes *h<sub>c</sub>*, the convection coefficient, as a function of air change rate. The curve's "x" is mechanical ACH (Air Changes per hour from mechanical air system), (1/hr)
-
-#### Field: Hc Function of Air System Volume Flow Rate Divided by Zone Perimeter Length Curve Name
-
-This field contains the name of separate performance curve or table object that describes *h<sub>c</sub>*, the convection coefficient, as a function of air change rate divided perimeter scale. Curve's "x" is mechanical system air flow rate (m<sup>3</sup>/s) divided by zone's length along exterior walls (m).
-
-### SurfaceConvectionAlgorithm:Outside:UserCurve
-
-This object is used to describe a custom model equation for surface convection heat transfer coefficients. If more than one curve is referenced, or non-blank, then they are all used and the result is the simple addition of all the curve results.
-
-#### Field: Name
-
-Unique name of input object.
-
-#### Field: Wind Speed Type for Curve
-
-This field specifies what sort of wind velocity data should be used in when evaluating the curve in the following field.  There are for key choice options. “WeatherFile� directs  using the unmodified value from the epw file or design weather data.  “HeightAdjust� uses the value from the epw file modified for height above ground, as determined by the z cooridinate, using the site terrain and weather station information.  “ParallelComponent� uses the value from the epw file modified to take just the velocity component that is parallel to the surface.  “ParallelComponentHeightAdjust� uses the height adjusted wind velocity and then computes the parallel component.
-
-#### Field: Hf Function of Wind Speed Curve Name
-
-This field contains the name of separate performance curve or table object that describes *h<sub>f</sub>*, the forced convection coefficient, as a function of wind speed. The curve's "x" is wind speed as defined by the method chosen in the previous field.
-
-#### Field: Hn Function of Temperature Difference Curve Name
-
-This field contains the name of separate performance curve or table object that describes *h<sub>n</sub>*, the natural convection coefficient, as a function of temperature difference. Curve's "x" is absolute value of delta-T (Surface temperature minus air temperature, (C))
-
-#### Field: Hc Function of Temperature Difference Divided by Height Curve Name
-
-This field contains the name of separate performance curve or table object that describes *h<sub>n</sub>*, the natural convection coefficient, as a function of temperature difference divided by height. Curve's "x" is absolute value of delta-T/Height (Surface temp minus Air temp)/(vertical length scale), (C/m).  For an outside face the vertical length scale is the exterior facade's overall height.
-
-### SurfaceProperty:ConvectionCoefficients
-
-The convection coefficients of each surface, both exterior and interior, are automatically calculated during EnergyPlus execution. These calculations are “governed� by other objects such as the SurfaceConvectionAlgorithm:Inside (overall default), the Zone object’s field called Zone Inside Convection Algorithm (Zone Default), the  and the SurfaceConvectionAlgorithm:Outside (overall default), and/or the Zone object’s field called Zone Outside Convection Algorithm (Zone Default). Usually, that will be enough flexibility for most users. However, if you need to match pre-existing convection coefficients (from another program) or are trying to match a test suite of results, you may wish to use the “override� convection coefficients in the following object. This object allows for a single surface to be given specific convection coefficients.
-
-Note that using these in conjunction, in particular, the “Simple� option on either the Outside Convection Algorithm or the Zone Outside Convection Algorithm field will result in a combined coefficient regardless of choice chosen here.
-
-Note that surfaces with “SurfaceProperty:OtherSideCoefficients� cannot use this object with the “outside� coefficient – attempting to do so will cause a severe error; SurfaceProperty:OtherSideCoefficients surfaces can apply an “inside� coefficient. And, surfaces with “Ground� exposure do not use the “outside� coefficient that might be supplied here. Note, too, that some lower boundaries are used regardless by certain surface types (i.e. Window) or certain algorithm types.
-
-#### Field: Surface Name
-
-This field is the applicable surface name for the user supplied convection coefficient.
-
-#### Fields (Convection Location, Type, Coefficient & Schedule Name)
-
-For simplicity, the descriptions of these field occur together – however, the fields are used sequentially when put into the IDF file (reference the IDF examples following the descriptions).
-
-#### Field: Convection Coefficient 1 Location
-
-#### Field: Convection Coefficient 2 Location
-
-This field contains the word “Outside� or “Inside� depending on which location is being described.
-
-#### Field: Convection Coefficient 1 Type
-
-#### Field: Convection Coefficient 2 Type
-
-The entries can be of several types: Value (simple numeric value), Schedule (name of schedule with the values), the usual key choices for overall models for Outside or Inside (Simple, SimpleCombined, TARP, AdaptiveConvectionAlgorithm etc.), the key choices for individual convection equations used for customizing the adaptive algorithm, or a custom user defined correlation. The field should contain one of the keys listed in the table below along with face they can be applied.  The definitions of the models and key choices are discussed under SurfaceConvectionAlgorithm:Inside , SurfaceConvectionAlgorithm:Outside, SurfaceConvectionAlgorithm:Inside:AdaptiveModelSelections, and SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections.
-
-<table class="table table-striped">
-<tr>
-<th>Key choice</th>
-<th>Applies to Insihe or Outsihe</th>
-</tr>
-<tr>
-<td>Value</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>Schedule</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>Simple</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>SimpleCombined</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>TARP</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>DOE-2</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>MoWitt</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>AdaptiveConvectionAlgorithm</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>ASHRAEVerticalWall   </td>
-<td>Both</td>
-</tr>
-<tr>
-<td>WaltonUnstableHorizontalOrTilt</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>WaltonStableHorizontalOrTilt</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>FisherPedersenCeilingDiffuserWalls</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>FisherPedersenCeilingDiffuserCeiling</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>FisherPedersenCeilingDiffuserFloor</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>AlamdariHammondStableHorizontal</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>AlamdariHammondUnstableHorizontal</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>AlamdariHammondVerticalWall</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>KhalifaEq3WallAwayFromHeat</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>KhalifaEq4CeilingAwayFromHeat</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>KhalifaEq5WallNearHeat</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>KhalifaEq6NonHeatedWalls</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>KhalifaEq7Ceiling</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>AwbiHattonHeatedFloor</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>AwbiHattonHeatedWall</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedAssistedWall</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedOpposingWall</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedStableFloor</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedUnstableFloor</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedStableCeiling</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedUnstableCeiling</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>FohannoPolidoriVerticalWall      </td>
-<td>Both</td>
-</tr>
-<tr>
-<td>KaradagChilledCeiling</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>ISO15099Windows</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>GoldsteinNovoselacCeilingDiffuserWindow</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>GoldsteinNovoselacCeilingDiffuserWalls</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>GoldsteinNovoselacCeilingDiffuserFloor</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>SimpleCombined     </td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>NusseltJurges</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>McAdams</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>Mitchell</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>BlockenWindard</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>Emmel</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>ClearRoof</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>UserCurve</td>
-<td>Both</td>
-</tr>
-</table>
-
-
-
-#### Field: Convection Coefficient 1
-
-#### Field: Convection Coefficient 2
-
-If the Convection type was “Value�, then this field is filled and contains the simple value to be used. Otherwise, this can be blank.
-
-#### Field: Convection Coefficient 1 Schedule Name
-
-#### Field: Convection Coefficient 2 Schedule Name
-
-If the Convection type was “Schedule�, then this field contains the name of a schedule describing the value to be used during the time intervals for the schedule.
-
-The complete IDD definition for the ConvectionCoefficients object follows:
-
-#### Field: Convection Coefficient 1 User Curve Name
-
-#### Field: Convection Coefficient 2 User Curve Name
-
-If the Convection type was “UserCurve�, then this field contains the name of a SurfaceConvectionAlgorithm:UserCurve input objct describing the model equations to be used during the time intervals for the schedule.
-
-In IDF usage:
-
-```idf
-SurfaceProperty:ConvectionCoefficients,
-Zn001:Wall001,  ! Surface Name
-Outside,        ! Convection Coefficient 1 Location
-Value,          ! Convection Coefficient 1 Type
-9.8,            ! Convection Coefficient 1
-,               ! Convection Coefficient 1 Schedule Name
-,               ! Convection Coefficient 1 User Curve Name
-Inside,         ! Convection Coefficient 2 Location
-Schedule,       ! Convection Coefficient 2 Type
-,               ! Convection Coefficient 2 {blank because using schedule}
-MyInteriorCC,   ! Convection Coefficient 2 Schedule Name
-;               ! Convection Coefficient 2 User Curve Name
-
-SurfaceProperty:ConvectionCoefficients,
-Zn001:Wall002,  ! Surface Name
-Inside,         ! Convection Coefficient 1 Location
-Value,          ! Convection Coefficient 1 Type
-.8,             ! Convection Coefficient 1
-,               ! Convection Coefficient 1 Schedule Name
-,               ! Convection Coefficient 1 User Curve Name
-Outside,        ! Convection Coefficient 2 Location
-Value,          ! Convection Coefficient 2 Type
-5.5,            ! Convection Coefficient 2
-;               ! Convection Coefficient 2 User Curve Name
-
-SurfaceProperty:ConvectionCoefficients,
-Zn001:Wall003,  ! Surface Name
-Outside,        ! Convection Coefficient 1 Location
-Value,          ! Convection Coefficient 1 Type
-9.8;            ! Convection Coefficient 1
-```
-
-
-### SurfaceProperty:ConvectionCoefficients:MultipleSurface
-
-The convection coefficients of each surface, both outside and inside, are automatically calculated during EnergyPlus execution. These calculations are “governed� by other objects such as the Inside Convection Algorithm (overall default) and the Zone Inside Convection Algorithm (Zone Default) and the Outside Convection Algorithm (overall default) and/or the Zone Outside Convection Algorithm (Zone Default). Usually, that will be enough flexibility for most users. However, if you need to match pre-existing convection coefficients (from another program) or are trying to match a test suite of results, you may wish to use the “override� convection coefficients in the following object. This object is similar to the preceding “ConvectionCoefficients� object but allows multiple surfaces to be assigned a type with one object entry.
-
-Note that using these in conjunction, in particular, the “Simple� option on either the Outside Convection Algorithm or the Zone Outside Convection Algorithm field will result in a combined coefficient regardless of choice chosen here.
-
-Note that surfaces with “SurfaceProperty:OtherSideCoefficients� cannot use this object with the “outside� coefficient – attempting to do so will ignore OSC surfaces during a multiple surface “apply�; SurfaceProperty:OtherSideCoefficients surfaces can apply an “inside� coefficient. And, surfaces with “Ground� exposure do not use the “outside� coefficient that might be supplied here. Note, too, that some lower boundaries are used regardless by certain surface types (i.e. Window) or certain algorithm types.
-
-#### Field: Surface Type
-
-This field is the applicable surface name for the user supplied convection coefficient. The allowable surface types are:
-
-- AllExteriorSurfaces  (all surfaces that are “external environment� surfaces)
-
-- AllExteriorWindows (all windows that are “external environment� surfaces)
-
-- AllExteriorWalls
-
-- AllExteriorRoofs
-
-- AllExteriorFloors
-
-- AllInteriorSurface (all surfaces that are “internal� surfaces)
-
-- AllInteriorWindows
-
-- AllInteriorCeilings
-
-- AllInteriorFloors
-
-#### Fields (Convection Location, Type, Coefficient & Schedule Name)
-
-For simplicity, the descriptions of these field occur together – however, the fields are used sequentially when put into the IDF file (reference the IDF examples following the descriptions).
-
-#### Field: Convection Coefficient 1 Location
-
-#### Field: Convection Coefficient 2 Location
-
-This field contains the word “Outside� or “Inside� depending on which location is being described.
-
-#### Field: Convection Coefficient 1 Type
-
-#### Field: Convection Coefficient 2 Type
-
-The entries can be of several types: Value (simple numeric value), Schedule (name of schedule with the values), the usual key choices for overall models for Outside or Inside (Simple, SimpleCombined, TARP, AdaptiveConvectionAlgorithm etc.), the key choices for individual convection equations used for customizing the adaptive algorithm, or a custom user defined correlation. The field should contain one of the keys listed in the table below along with face they can be applied.  The definitions of the models and key choices are discussed under SurfaceConvectionAlgorithm:Inside , SurfaceConvectionAlgorithm:Outside, SurfaceConvectionAlgorithm:Inside:AdaptiveModelSelections, and SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections.
-
-<table class="table table-striped">
-<tr>
-<th>Key choice</th>
-<th>Applies to Insihe or Outsihe</th>
-</tr>
-<tr>
-<td>Value</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>Schedule</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>Simple</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>SimpleCombined</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>TARP</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>DOE-2</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>MoWitt</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>AdaptiveConvectionAlgorithm</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>ASHRAEVerticalWall   </td>
-<td>Both</td>
-</tr>
-<tr>
-<td>WaltonUnstableHorizontalOrTilt</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>WaltonStableHorizontalOrTilt</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>FisherPedersenCeilingDiffuserWalls</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>FisherPedersenCeilingDiffuserCeiling</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>FisherPedersenCeilingDiffuserFloor</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>AlamdariHammondStableHorizontal</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>AlamdariHammondUnstableHorizontal</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>AlamdariHammondVerticalWall</td>
-<td>Both</td>
-</tr>
-<tr>
-<td>KhalifaEq3WallAwayFromHeat</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>KhalifaEq4CeilingAwayFromHeat</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>KhalifaEq5WallNearHeat</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>KhalifaEq6NonHeatedWalls</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>KhalifaEq7Ceiling</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>AwbiHattonHeatedFloor</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>AwbiHattonHeatedWall</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedAssistedWall</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedOpposingWall</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedStableFloor</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedUnstableFloor</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedStableCeiling</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>BeausoleilMorrisonMixedUnstableCeiling</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>FohannoPolidoriVerticalWall      </td>
-<td>Both</td>
-</tr>
-<tr>
-<td>KaradagChilledCeiling</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>ISO15099Windows</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>GoldsteinNovoselacCeilingDiffuserWindow</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>GoldsteinNovoselacCeilingDiffuserWalls</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>GoldsteinNovoselacCeilingDiffuserFloor</td>
-<td>Inside</td>
-</tr>
-<tr>
-<td>SimpleCombined     </td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>NusseltJurges</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>McAdams</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>Mitchell</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>BlockenWindard</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>Emmel</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>ClearRoof</td>
-<td>Outside</td>
-</tr>
-<tr>
-<td>UserCurve</td>
-<td>Both</td>
-</tr>
-</table>
-
-#### Field: Convection Coefficient 1
-
-#### Field: Convection Coefficient 2
-
-If the Convection type was “Value�, then this field is filled and contains the simple value to be used. Otherwise, this can be blank.
-
-#### Field: Convection Coefficient 1 Schedule Name
-
-#### Field: Convection Coefficient 2 Schedule Name
-
-If the Convection type was “Schedule�, then this field contains the name of a schedule describing the value to be used during the time intervals for the schedule.
-
-#### Field: Convection Coefficient 1 User Curve Name
-
-#### Field: Convection Coefficient 2 User Curve Name
-
-If the Convection type was “UserCurve�, then this field contains the name of a SurfaceConvectionAlgorithm:UserCurve input objct describing the model equations to be used during the time intervals for the schedule.
-
-In IDF usage:
-
-```idf
-SurfaceProperty:ConvectionCoefficients:MultipleSurface,
-AllExteriorWindows,  ! Surface Types
-Outside,             ! Convection Coefficient 1 Location
-MoWitt;              ! Convection Coefficient 1 Type
-```
-
-
-### Convection Coefficient Application Hierarchy
-
-Ultimate flexibility and possibly ultimate user confusion can result from the convection coefficient possibilties in EnergyPlus. The objects that control how convection models are assigned to individual surfaces  are:
-
-- SurfaceConvectionAlgorithm:Inside
-
-- SurfaceConvectionAlgorithm:Outside
-
-- Zone, Field: Zone Inside Convection Algorithm
-
-- Zone, Field: Zone Outside Convection Algorithm
-
-- SurfaceProperty:ConvectionCoefficients
-
-- SurfaceProperty:ConvectionCoefficients:MultipleSurface
-
-General to Specific, they are assigned in this order:
-
-Table 9. Convection Coefficient Assignment Hierarchy
-
-<table class="table table-striped">
-<tr>
-<th>Objects/Description</th>
-<th>Action</th>
-</tr>
-<tr>
-<td>SurfaceConvectionAlgorithm:*</td>
-<td>Assigns for all surfaces in the run.</td>
-</tr>
-<tr>
-<td>Zone, Fields: Zone * Convection Algorithm</td>
-<td>Trumps global assignment and assigns for all surfaces in Zone.</td>
-</tr>
-<tr>
-<td>SurfaceProperty:...:MultipleSurfaces</td>
-<td>Trumps above and assigns for specific types of surfaces.</td>
-</tr>
-<tr>
-<td>Two Multiple Surface Assignments overlapping (such as AllExteriorSurfaces vs AllExteriorWalls)</td>
-<td>Order in IDF is now important. Whichever is first gets the cookie and the second gets a warning.</td>
-</tr>
-<tr>
-<td>Specific Surface Assignment</td>
-<td>Trumps all Above.</td>
-</tr>
-</table>
-
-There are additional objects that provide fine control over the models that get assigned.
-
-- SurfaceConvectionAlgorithm:Inside:AdaptiveModelSelections
-
-- SurfaceConvectionAlgorithm:Outside:AdaptiveModelSelections
-
-- SurfaceConvectionAlgorithm:Inside:UserCurve
-
-- SurfaceConvectionAlgorithm:Outside:UserCurve
-
-### Convection Coefficients Outputs
-
-Outputs for the User Supplied Convection Coefficients appear as values in the Surface Output Variables (*Surface Inside Face Convection Heat Transfer Coefficient* and *Surface Outside Face Convection Heat Transfer Coefficient*). What the program expects to use is shown in the Surface Details report (*Output:Surfaces:List, Details;*)
-
-When EnergyPlus is set to Display Advanced Variables (Output:Diagnostics, DisplayAdvancedVariables;), then additional output variables are available that indicate the status of convection modeling by identifying which models are in effect at a given time.  The adaptive convection algorithms may switch between models over time and the following output variables provide a way to monitor this behavior.  These outputs are integer codes and the integer values are explained in tables.
-
-#### Surface Inside Face Convection Classification Index
-
-This variable reports how the surface was classified as part of the adaptive convection algorithm for the inside face.  The algorithm examines probable flow regimes, heat flow directions, orientations, HVAC equipment connections, and current operating status to assign each surface a category.  The numbers in this report are integer codes that correspond to surface categories as described in the following table.
-
-<table class="table table-striped">
-<tr>
-<th>Cohe</th>
-<th>Zone Airflow Regime</th>
-<th>Type of surface</th>
-<th>Heat Flow</th>
-</tr>
-<tr>
-<td>1</td>
-<td>A1 Radiant Heated Floor or Chilled Ceiling</td>
-<td>Vertical Wall</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>2</td>
-<td>A1 Radiant Heated Floor or Chilled Ceiling</td>
-<td>Horizontal</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>3</td>
-<td>A1 Radiant Heated Floor or Chilled Ceiling</td>
-<td>Horizontal</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>4</td>
-<td>A1 Radiant Heated Floor or Chilled Ceiling</td>
-<td>Heated Floor</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>5</td>
-<td>A1 Radiant Heated Floor or Chilled Ceiling</td>
-<td>Chilled Ceiling</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>6</td>
-<td>A1 Radiant Heated Floor or Chilled Ceiling</td>
-<td>Tilted</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>7</td>
-<td>A1 Radiant Heated Floor or Chilled Ceiling</td>
-<td>Tilted</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>8</td>
-<td>A1 Radiant Heated Floor or Chilled Ceiling</td>
-<td>Window</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>9</td>
-<td>A2 Radiant Wall Heat</td>
-<td>Non-heated Vertical Wall</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>10</td>
-<td>A2 Radiant Wall Heat</td>
-<td>Heated wall</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>11</td>
-<td>A2 Radiant Wall Heat</td>
-<td>Horizontal</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>12</td>
-<td>A2 Radiant Wall Heat</td>
-<td>Horizontal</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>13</td>
-<td>A2 Radiant Wall Heat</td>
-<td>Tilted</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>14</td>
-<td>A2 Radiant Wall Heat</td>
-<td>Tilted</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>15</td>
-<td>A2 Radiant Wall Heat</td>
-<td>Windows</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>16</td>
-<td>A3 Simple Buoyancy</td>
-<td>Vertical Walls</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>17</td>
-<td>A3 Simple Buoyancy</td>
-<td>Horizontal</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>18</td>
-<td>A3 Simple Buoyancy</td>
-<td>Horizontal</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>19</td>
-<td>A3 Simple Buoyancy</td>
-<td>Tilted</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>20</td>
-<td>A3 Simple Buoyancy</td>
-<td>Tilted</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>21</td>
-<td>A3 Simple Buoyancy</td>
-<td>Windows</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>22</td>
-<td>B Convective Zone Heat</td>
-<td>Vertical Walls</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>23</td>
-<td>B Convective Zone Heat</td>
-<td>Vertical Walls near heater</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>24</td>
-<td>B Convective Zone Heat</td>
-<td>Horizontal</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>25</td>
-<td>B Convective Zone Heat</td>
-<td>Horizontal</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>26</td>
-<td>B Convective Zone Heat</td>
-<td>Tilted</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>27</td>
-<td>B Convective Zone Heat</td>
-<td>Tilted</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>28</td>
-<td>B Convective Zone Heat</td>
-<td>Windows</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>29</td>
-<td>C Central Air Diffuser</td>
-<td>Walls</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>30</td>
-<td>C Central Air Diffuser</td>
-<td>Ceiling</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>31</td>
-<td>C Central Air Diffuser</td>
-<td>Floor</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>32</td>
-<td>C Central Air Diffuser</td>
-<td>Windows</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>33</td>
-<td>D Zone Fan Unit</td>
-<td>Walls</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>34</td>
-<td>D Zone Fan Unit</td>
-<td>Horizontal</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>35</td>
-<td>D Zone Fan Unit</td>
-<td>Horizontal</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>36</td>
-<td>D Zone Fan Unit</td>
-<td>Tilted</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>37</td>
-<td>D Zone Fan Unit</td>
-<td>Tilted</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>38</td>
-<td>D Zone Fan Unit</td>
-<td>Windows</td>
-<td>Any</td>
-</tr>
-<tr>
-<td>39</td>
-<td>E Mixed Forced and Buoyancy</td>
-<td>Walls</td>
-<td>Assisting</td>
-</tr>
-<tr>
-<td>40</td>
-<td>E Mixed Forced and Buoyancy</td>
-<td>Walls</td>
-<td>Opposing</td>
-</tr>
-<tr>
-<td>41</td>
-<td>E Mixed Forced and Buoyancy</td>
-<td>Floor</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>42</td>
-<td>E Mixed Forced and Buoyancy</td>
-<td>Floor</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>43</td>
-<td>E Mixed Forced and Buoyancy</td>
-<td>Ceiling</td>
-<td>Stable</td>
-</tr>
-<tr>
-<td>44</td>
-<td>E Mixed Forced and Buoyancy</td>
-<td>Ceiling</td>
-<td>Unstable</td>
-</tr>
-<tr>
-<td>45</td>
-<td>E Mixed Forced and Buoyancy</td>
-<td>Windows</td>
-<td>Any</td>
-</tr>
-</table>
-
-#### Surface Inside Face Convection Model Equation Index
-
-This variable reports the specific model equation used to calculate the inside face convection coefficient.  This can vary when using the adaptive convection algorithm and so the result of that selection algorithm is reported here.  The following table lists the models associated with specific interger codes reported here.  The models correspond to key words used in input objects.
-
-<table class="table table-striped">
-<tr>
-<th>Report Cohe</th>
-<th>Relateh key anh mohel</th>
-</tr>
-<tr>
-<td>200</td>
-<td>UserValue    </td>
-</tr>
-<tr>
-<td>201</td>
-<td>UserSchedule</td>
-</tr>
-<tr>
-<td>202</td>
-<td>UserCurve </td>
-</tr>
-<tr>
-<td>203</td>
-<td>ASHRAEVerticalWall </td>
-</tr>
-<tr>
-<td>204</td>
-<td>WaltonUnstableHorizontalOrTilt</td>
-</tr>
-<tr>
-<td>205</td>
-<td>WaltonStableHorizontalOrTilt  </td>
-</tr>
-<tr>
-<td>206</td>
-<td>FisherPedersenCeilDiffuserFloor</td>
-</tr>
-<tr>
-<td>207</td>
-<td>FisherPedersenCeilDiffuserCeiling</td>
-</tr>
-<tr>
-<td>208</td>
-<td>FisherPedersenCeilDiffuserWalls        </td>
-</tr>
-<tr>
-<td>209</td>
-<td>AlamdariHammondStableHorizontal        </td>
-</tr>
-<tr>
-<td>210</td>
-<td>AlamdariHammondVerticalWall            </td>
-</tr>
-<tr>
-<td>211</td>
-<td>AlamdariHammondUnstableHorizontal      </td>
-</tr>
-<tr>
-<td>212</td>
-<td>KhalifaEq3WallAwayFromHeat             </td>
-</tr>
-<tr>
-<td>213</td>
-<td>KhalifaEq4CeilingAwayFromHeat          </td>
-</tr>
-<tr>
-<td>214</td>
-<td>KhalifaEq5WallNearHeat                 </td>
-</tr>
-<tr>
-<td>215</td>
-<td>KhalifaEq6NonHeatedWalls </td>
-</tr>
-<tr>
-<td>216</td>
-<td>KhalifaEq7Ceiling </td>
-</tr>
-<tr>
-<td>217</td>
-<td>AwbiHattonHeatedFloor                  </td>
-</tr>
-<tr>
-<td>218</td>
-<td>AwbiHattonHeatedWall                   </td>
-</tr>
-<tr>
-<td>219</td>
-<td>BeausoleilMorrisonMixedAssistingWall   </td>
-</tr>
-<tr>
-<td>220</td>
-<td>BeausoleilMorrisonMixedOppossingWall   </td>
-</tr>
-<tr>
-<td>221</td>
-<td>BeausoleilMorrisonMixedStableCeiling   </td>
-</tr>
-<tr>
-<td>222</td>
-<td>BeausoleilMorrisonMixedUnstableCeiling </td>
-</tr>
-<tr>
-<td>223</td>
-<td>BeausoleilMorrisonMixedStableFloor     </td>
-</tr>
-<tr>
-<td>224</td>
-<td>BeausoleilMorrisonMixedUnstableFloor   </td>
-</tr>
-<tr>
-<td>225</td>
-<td>FohannoPolidoriVerticalWall            </td>
-</tr>
-<tr>
-<td>226</td>
-<td>KaradagChilledCeiling                  </td>
-</tr>
-<tr>
-<td>227</td>
-<td>ISO15099Windows                        </td>
-</tr>
-<tr>
-<td>228</td>
-<td>GoldsteinNovoselacCeilingDiffuserWindow</td>
-</tr>
-<tr>
-<td>229</td>
-<td>GoldsteinNovoselacCeilingDiffuserWalls </td>
-</tr>
-<tr>
-<td>230</td>
-<td>GoldsteinNovoselacCeilingDiffuserFloor</td>
-</tr>
-</table>
-
-#### Surface Inside Face Convection Reference Air Index
-
-The inside face convection heat transfer calculations can be based on different reference air temperatures.  This reference air temperature can vary during the simulation when the adaptive algorithm selects models that use different references.  The following table lists the meaning of the integer codes.
-
-<table class="table table-striped">
-<tr>
-<th>Report Cohe</th>
-<th>Reference Air Temperature Methoh</th>
-</tr>
-<tr>
-<td>1</td>
-<td>Zone mean air temperature</td>
-</tr>
-<tr>
-<td>2</td>
-<td>Surface adjacent air temperature</td>
-</tr>
-<tr>
-<td>3</td>
-<td>Supply air temperature</td>
-</tr>
-</table>
-
-#### Surface Outside Face Convection Classification Index
-
-This variable reports how the surface was classified as part of the adaptive convection algorithm for the outside face.  The algorithm examines the wind direction, heat flow directions and orientations to assign each surface a category.  The numbers in this report are integer codes that correspond to surface categories as described in the following table.
-
-<table class="table table-striped">
-<tr>
-<th>Report Cohe</th>
-<th>Surface Classification</th>
-</tr>
-<tr>
-<td>101</td>
-<td>Vertical Wall, Windward</td>
-</tr>
-<tr>
-<td>102</td>
-<td>Vertical Wall, Leeward</td>
-</tr>
-<tr>
-<td>103</td>
-<td>Roof, stable heat flow direction</td>
-</tr>
-<tr>
-<td>104</td>
-<td>Roof, unstable heat flow direction</td>
-</tr>
-</table>
-
-#### Surface Outside Face Forced Convection Model Equation Index
-
-#### Surface Outside Face Natural Convection Model Equation Index
-
-These variables report the specific model equation used to calculate the outside face’s convection coefficient.  They can vary when using the adaptive convection algorithm and so the results of that selection algorithm are reported in these variables.  The following table lists the models associated with specific integer codes that might be reported here.  The models correspond to key words used in input objects.
-
-<table class="table table-striped">
-<tr>
-<th>Report Cohe</th>
-<th>Relateh key anh mohel</th>
-</tr>
-<tr>
-<td>300</td>
-<td>None </td>
-</tr>
-<tr>
-<td>301</td>
-<td>UserValue</td>
-</tr>
-<tr>
-<td>302</td>
-<td>UserSchedule</td>
-</tr>
-<tr>
-<td>303</td>
-<td>UserCurve                              </td>
-</tr>
-<tr>
-<td>304</td>
-<td>ASHRAESimpleCombined                   </td>
-</tr>
-<tr>
-<td>305</td>
-<td>NaturalASHRAEVerticalWall              </td>
-</tr>
-<tr>
-<td>306</td>
-<td>NaturalWaltonUnstableHorizontalOrTilt  </td>
-</tr>
-<tr>
-<td>307</td>
-<td>NaturalWaltonStableHorizontalOrTilt    </td>
-</tr>
-<tr>
-<td>308</td>
-<td>SparrowWindward                        </td>
-</tr>
-<tr>
-<td>309</td>
-<td>SparrowLeeward                         </td>
-</tr>
-<tr>
-<td>310</td>
-<td>MoWiTTWindward                         </td>
-</tr>
-<tr>
-<td>311</td>
-<td>MoWiTTLeeward                          </td>
-</tr>
-<tr>
-<td>312</td>
-<td>DOE2Windward                           </td>
-</tr>
-<tr>
-<td>313</td>
-<td>DOE2Leeward                            </td>
-</tr>
-<tr>
-<td>314</td>
-<td>NusseltJurges                          </td>
-</tr>
-<tr>
-<td>315</td>
-<td>McAdams                                </td>
-</tr>
-<tr>
-<td>316</td>
-<td>Mitchell                               </td>
-</tr>
-<tr>
-<td>317</td>
-<td>ClearRoof                              </td>
-</tr>
-<tr>
-<td>318</td>
-<td>BlockenWindward                        </td>
-</tr>
-<tr>
-<td>319</td>
-<td>EmmelVertical                           </td>
-</tr>
-<tr>
-<td>320</td>
-<td>EmmelRoof                              </td>
-</tr>
-<tr>
-<td>321</td>
-<td>AlamdariHammondVerticalWall            </td>
-</tr>
-<tr>
-<td>322</td>
-<td>FohannoPolidoriVerticalWall            </td>
-</tr>
-<tr>
-<td>323</td>
-<td>ISO15099Windows                        </td>
-</tr>
-<tr>
-<td>324</td>
-<td>AlamdariHammondStableHorizontal        </td>
-</tr>
-<tr>
-<td>325</td>
-<td>AlamdariHammondUnstableHorizontal      </td>
-</tr>
-</table>
-
-### SurfaceProperties:VaporCoefficients
-
-Advanced/Research Usage:.The internal and external vapor transfer coefficients that are used by the CombinedHeatAndMoistureFiniteElement model are automatically calculated during EnergyPlus execution using information on the convection coefficients. However it is sometimes useful to be able to “override� the calculation and set fixed values of vapor transfer coefficient for a single surface. These coefficients are only used by the CombinedHeatAndMoistureFiniteElement model and will be ignored by other solution algorithms.
-
-#### Field: Surface Name
-
-This field is the applicable surface name for the user supplied vapor transfer coefficient.
-
-#### Field: Constant External Vapor Transfer Coefficient
-
-Select ‘yes’ to use the value supplied as the external vapor transfer coefficient
-
-#### Field: External Vapor Coefficient Value
-
-HAMT will use this value to calculate the vapour transfer into and out off the external surface of this surface. Units are kg/Pa.s.m2.
-
-#### Field: Constant Internal vapor Transfer Coefficient
-
-Select ‘yes’ to use the value supplied as the internal vapor transfer coefficient
-
-#### Field: Internal Vapor Coefficient Value
-
-The CombinedHeatAndMoistureFiniteElement algorithm will use this value to calculate the vapor transfer into and out of the internal surface of this surface. Units are kg/Pa.s.m2.
-
-Below is an example input of vapor transfer coefficients for a surface.
-
-```idf
-SurfaceProperties:VaporCoefficients,
-      South wall,     !- Surface Name
-      Yes,     !- Constant External Vapor Transfer Coefficient
-      0.0000000625,     !- External Vapor Coefficient Value
-      Yes,     !- Constant Internal vapor Transfer Coefficient
-      0.00000002;     !- Internal Vapor Coefficient Value
-```
-
-
-### SurfaceProperty:ExteriorNaturalVentedCavity
-
-This object is used to model a multi-skin exterior heat transfer surface. This is a special case where the outside face is a slightly detached layer forming a naturally ventilated cavity. The actual outer surface is referred to as the baffle. The modeling here assumes that the heat capacity in the outer baffle can be neglected since it is much lower than the underlying mass surface. This object is used with the BuildingSurface:Detailed object where the Heat Transfer surfaces are referred to as the underlying surfaces. The constructions and materials for the BuildingSurface:Detailed object should reflect the construction of just the underlying surface. The SurfaceProperty:ExteriorNaturalVentedCavity object is used to describe the decoupled layer, or baffle, and the characteristics of the cavity and openings for natural ventilation. This object is also used in conjunction with the OtherSideConditionsModel.
-
-The area and orientation are obtained from **BuildingSurface:Detailed** objects, which are referenced by name. This object can be used to model certain types of photovoltaic mounting configurations such as interlocking roof pavers. If the baffle covers only part of a surface, then that surface should be split into separate **BuildingSurface:Detailed** objects where one matches the size of the baffle. A single baffle can be associated with as many **BuildingSurface:Detailed** objects as desired (although if you need to use more than 10 surfaces, then the IDD will need to be extended). The base heat transfer surfaces need not be contiguous nor have the same orientation, but the program will issue warnings if surfaces have widely ranging tilts and azimuths.
-
-Note that the model involves predicting the rates that ambient air moves in and out of the cavity. Accurate modeling of these air flows would be extremely challenging and so the models provided through this object are simplistic engineering models based on discharge coefficients that are sensitive to wind and bouancy effects. The accuracy depends on the values for, and applicability of, the discharge coefficients and unfortunately little research is available to help characterize these. The models should be considered rudimentary and the user is encouraged to explore different values for the coefficients in attempts to bound the importance of natural ventilation for the cavities. See the Engineering Reference for more details.
-
-#### Field: Name
-
-This field contains a unique name for the ventilated cavity.
-
-#### Field: Boundary Conditions Model Name
-
-This field contains the name of an SurfaceProperty:OtherSideConditionsModel object declared elsewhere in the input file. This will connect the baffle and ventilated cavity to the exterior boundary conditions for the underlying heat transfer surface.
-
-#### Field: Area Fraction of Openings
-
-This field is used to enter an area fraction for what part of the baffle consists of openings. The area of the openings will set to the product of this field and the sum of the area of the underlying surfaces.
-
-#### Field: Thermal Emissivity of Exterior Baffle Material
-
-This field is used to enter the thermal emissivity of the baffler. This surface property is for longwave infrared radiation. The property is used for both sides of collector. Most painted materials have an emissivity of 0.9.
-
-#### Field: Solar Absorptivity of Exterior Baffle
-
-This field is used to enter the solar absorbtivity of the baffle. This surface property is for shortwave, solar radiation. The property is used for the front side of the baffle that faces the environment. Darker colors have a higher absorptivity. While black is the highest performance, other colors might be used to match the color scheme of the rest of the façade.
-
-#### Field: Height Scale for Buoyancy-Driven Ventilation
-
-This field is used to enter a nominal height scale (m) for prediction of ventilation induced by bouancy. This value (<span>\(\Delta {H_{NPL}}\)</span>) is defined as the height from the midpoint of the lower opening to the neutral pressure level. Increasing the value will increase the ventilation rate due to buoyancy.
-
-#### Field: Effective Thickness of Cavity Behind Exterior Baffle
-
-This field is used to enter a nominal gap thickness (m) for the collector. If the baffle is corrugated, use the average depth. This distance value is only used when the collector is near horizontal to determine a length scale in the vertical direction for buoyancy calculations. For example, if the collector is mounted on a flat roof, its tilt-adjusted height is zero and the program will use this gap thickness as a length scale rather than the height from the previous field.
-
-#### Field: Ratio of Actual Surface Area to Projected Surface Area
-
-This field is used to enter a factor that accounts for the extra surface area resulting from and uneven baffle surface. Corrugations may be present to help stiffen the baffle or ventilated roofing tiles may have more surface are for convection heat transfer than the underlying surface. The projected surface area is obtained by the program from the (flat) underlying surfaces. If the baffle is flat then this ratio is 1.0. If the baffle is corrugated, then this ratio will be greater than one with a typical value might be 1.165.
-
-#### Field: Roughness of Exterior Surface
-
-This field is used to describe the relative roughness of the baffle material. This field is similar to one in the **Material** object. This parameter only influences the convection coefficients, more specifically the exterior convection coefficient. A special keyword is expected in this field with the options being “VeryRough�, “Rough�, “MediumRough�, “MediumSmooth�, “Smooth�, and “VerySmooth� in order of roughest to smoothest options.
-
-#### Field: Effectiveness for Perforations with Respect to Wind
-
-This field is used to enter a value for the coefficient used to determine natural air exchanges from wind. Wind will cause exterior air to move in and out of the cavity. Cv is an arbitrary coefficient used to model the effectiveness of openings and depends on opening geometry and the orientation with respect to the wind. Cv should probably be in the range 0.05 to 0.65. Increasing Cv will increase the amount of natural ventilation. The following equation shows how Cv is used in the program to predict the volumetric flow rate due to wind:
-
-<div>\[{{\rm{\dot \rlap{--} V}}_{{\rm{wind}}}} = {C_v}{A_{in}}{U_\infty }\]</div>
-
-#### Field: Discharge Coefficient for Openings with Respect to Buoyancy Driven Flow
-
-This field is used to enter a value for the coefficient used to determine natural air exchanges from buoyancy. Stack or buoyancy effects will cause exterior air to move in and out of the cavity. Cd is an arbitrary discharge coefficient that depends on the geometry of the opening. Cd should probably be in the range 0.1 to 1.0. Increasing Cd will increase the amount of natural ventilation. The following equations show how Cd is used in the program to predict the volume flow rate due to buoyancy:
-
-<span>\({{\rm{\dot \rlap{--} V}}_{{\rm{thermal}}}} = {C_D}{A_{in}}\sqrt {2g\Delta {H_{NPL}}\left( {{T_{a,cav}} - {T_{amb}}} \right)/{T_{a,cav}}} \)</span>  (if <span>\({T_{a,cav}} > {T_{amb}}\)</span>)
-
-<span>\({{\rm{\dot \rlap{--} V}}_{{\rm{thermal}}}} = {C_D}{A_{in}}\sqrt {2g\Delta {H_{NPL}}\left( {{T_{amb}} - {T_{a,cav}}} \right)/{T_{amb}}} \)</span>  (if <span>\({T_{amb}} > {T_{a,cav}}\)</span> and baffle is vertical)
-
-where <span>\(\Delta {H_{NPL}}\)</span> is the value input into the field above for the height scale for buoyancy-driven ventilation.
-
-#### Field(s): Surface &lt;1 thru x&gt; Name
-
-The remaining fields are used to name the **BuildingSurface:Detailed** objects that are associated with the exterior naturally vented cavity. These are the underlying heat transfer surfaces and are defined elsewhere in the input file. These surfaces should all specify OtherSideConditionsModel as their exterior environment. The input object can currently accommodate up to ten surfaces, but it is extensible by modifying the Energy+.idd entry.
-
-An example IDF entry is
-
-```idf
-SurfaceProperty:ExteriorNaturalVentedCavity,
-PVRoofPaverExtVentCav1 ,   ! Name
-    PVRoofPaverSystem1,        ! OtherSideConditionsModel Object Name
-    0.02,    ! Area Fraction of Openings
-    0.9,     ! Thermal Emissivity of Exterior Baffle Material
-    0.92,    ! Solar Absorbtivity of Exterior Baffle
-    0.05,    ! Height scale for buoyancy-driven ventilation
-    0.05,    ! Effective Thickness of Cavity Behind Exterior Baffle
-    0.97,    ! Ratio of Actual surface area to projected surface area
-    Smooth , ! Roughness of collector
-    0.1 ,    ! Cv, Effectiveness for perforations with respect to Wind
-    0.5 ,    ! Cd, Discharge Coefficient for Openings with respect to buoyancy-driven flow
-    Zn001:Roof001 ;    ! Surface Name
-```
-
-### SurfaceProperty:ExteriorNaturalVentedCavity Outputs
-
-In addition to related output that can be obtained for all surfaces, these outputs are available for exterior naturally vented cavity configurations:
-
-* HVAC,Average, Surface Exterior Cavity Air Drybulb Temperature [C]
-
-* HVAC,Average, Surface Exterior Cavity Baffle Surface Temperature [C]
-
-* HVAC,Average, Surface Exterior Cavity Total Natural Ventilation Air Change Rate [ACH]
-
-* HVAC,Average, Surface Exterior Cavity Total Natural Ventilation Mass Flow Rate [kg/s]
-
-* HVAC,Average, Surface Exterior Cavity Natural Ventilation from Wind Mass Flow Rate [kg/s]
-
-* HVAC,Average, Surface Exterior Cavity Natural Ventilation from Buoyancy Mass Flow Rate [kg/s]
-
-#### Surface Exterior Cavity Air Drybulb Temperature [C]
-
-The temperature of air inside the cavity behind the baffle.
-
-#### Surface Exterior Cavity Baffle Surface Temperature [C]
-
-The surface temperature of the exterior baffle material itself.
-
-#### Surface Exterior Cavity Total Natural Ventilation Air Change Rate [ACH]
-
-The rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive in Air Changes per Hour.
-
-#### Surface Exterior Cavity Total Natural Ventilation Mass Flow Rate [kg/s]
-
-The mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive.
-
-#### Surface Exterior Cavity Natural Ventilation from Wind Mass Flow Rate [kg/s]
-
-The part of mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive due to wind-driven forces.
-
-#### Surface Exterior Cavity Natural Ventilation from Buoyancy Mass Flow Rate [kg/s]
-
-The part of mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive due to buoyancy-driven forces.
-
-### SurfaceProperty:SolarIncidentInside
-
-This object can be used as an alternative to the standard (automatic) EnergyPlus calculation of the solar radiation incident on interior surfaces of the building. Using this method, the normal EnergyPlus calculation is replaced with a schedule of solar incidence values that are calculated outside the program.
-
-#### Field: Name
-
-The name of the SurfaceProperty:SolarIncidentInside object  Must be unique between all SurfaceProperty:SolarIncidentInside objects.
-
-#### Field: Surface Name
-
-The building surface associated with this object (ref BuildingSurface:Detailed). Solar absorptance values in the schedule file will be applied to the inside of this surface.
-
-#### Field: Construction Name
-
-The building construction associated with this object (ref Construction).  It is possible that the Energy Management System will change the construction associated with the surface; if the construction is changed, a new set of data may need to be applied to the current surface.
-
-#### Field: Inside Surface Incident Sun Solar Radiation Schedule Name
-
-This field specifies the name of a schedule that contains the values for incident solar radiation.  Values from the schedule data will be used to replace the absorbed solar radiation that would normally be calculated by EnergyPlus.  Units in the external schedule file must be W/m<sup>2</sup>.
-
-Example for SurfaceProperty:SolarIncidentInside using a compact schedule:
-
-```idf
-  Schedule:Compact,
-    North Wall SSG,          !- Name
-    Positive Number,         !- Schedule Type Limits Name
-    Through: 12/31,          !- Field 1
-    For: AllDays,            !- Field 2
-    Until: 07:00,10,         !- Field 3
-    Until: 17:00,20,         !- Field 5
-    Until: 24:00,15;         !- Field 7
-
-
-  SurfaceProperty:SolarIncidentInside,
-    North Wall Solar Incident,  !- Name
-    Room102 North Wall,         !- Surface Name
-    Room Wall - North,          !- Construction Name
-    North Wall SSG;             !- Schedule Name
-```
-
-### ComplexFenestrationProperty:SolarAbsorbedLayers
-
-This object can be used as an alternative to the standard (automatic) EnergyPlus calculation of the solar radiation absorbed by fenestration systems in the building.  Using this method, the normal EnergyPlus calculation is replaced with a schedule of solar absorptance values that are calculated outside the program.
-
-#### Field: Name
-
-The name of the ComplexFenestrationProperty:SolarAbsorbedLayers object  Must be unique between all ComplexFenestrationProperty:SolarAbsorbedLayers objects.
-
-#### Field: Fenestration Surface
-
-The fenestration surface associated with this object (ref FenestrationSurface:Detailed).  Values from the schedule data will be used to replace the absorbed solar radiation in the fenestration layers that would normally be calculated by EnergyPlus.  Value units in the schedule must be W/m<sup>2</sup>.
-
-#### Field: Construction Name
-
-The building construction associated with this object (ref Construction).  It is possible that the Energy Management System will change the construction associated with the surface; if the construction is changed, a new set of data may need to be applied to the current surface.
-
-#### Field: Layer 1 Solar Radiation Absorbed Schedule Name
-
-Specifies the name of a schedule that contains the absorbed solar radiation values in units of W/m<sup>2</sup>.  Values from the schedule are used for the absorbed solar radiation of the first (outside) layer .
-
-#### Field: Layer 2 Solar Radiation Absorbed Schedule Name
-
-Specifies the name of a schedule that contains absorbed solar radiation values in units of W/m<sup>2</sup>.  Values from the schedule are used for the absorbed solar radiation of the second layer .
-
-#### Field: Layer 3 Solar Radiation Absorbed Schedule Name
-
-Specifies the name of a schedule that contains absorbed solar radiation values in units of W/m<sup>2</sup>.  Values from the schedule are used for the absorbed solar radiation for the third layer .
-
-#### Field: Layer 4 Solar Radiation Absorbed Schedule Name
-
-Specifies the name of a schedule that contains absorbed solar radiation values in units of W/m<sup>2</sup>.  Values from the schedule are used for the absorbed solar radiation of the fourth layer.
-
-#### Field: Layer 5 Solar Radiation Absorbed Schedule Name
-
-Specifies the name of a schedule that contains absorbed solar radiation values in units of W/m<sup>2</sup>.  Values from the schedule are used for the absorbed solar radiation of the fifth layer .
-
-Example for ComplexFenestrationProperty:SolarAbsorbedLayers with compact schedules:
-
-```idf
-  Schedule:Compact,
-    Layer 1,                 !- Name
-    Positive Number,         !- Schedule Type Limits Name
-    Through: 12/31,          !- Field 1
-    For: AllDays,            !- Field 2
-    Until: 07:00,1,         !- Field 3
-    Until: 17:00,2,         !- Field 5
-    Until: 24:00,1.5;         !- Field 7
-
-
-  Schedule:Compact,
-    Layer 2,                 !- Name
-    Positive Number,         !- Schedule Type Limits Name
-    Through: 12/31,          !- Field 1
-    For: AllDays,            !- Field 2
-    Until: 07:00,0.8,        !- Field 3
-    Until: 17:00,1.2,        !- Field 5
-    Until: 24:00,1.0;        !- Field 7
-
-
-  Schedule:Compact,
-    Layer 3,                 !- Name
-    Positive Number,         !- Schedule Type Limits Name
-    Through: 12/31,          !- Field 1
-    For: AllDays,            !- Field 2
-    Until: 07:00,1,          !- Field 3
-    Until: 17:00,2.1,        !- Field 5
-    Until: 24:00,1.7;        !- Field 7
-
-
-  ComplexFenestrationProperty:SolarAbsorbedLayers,
-    South Window Solar Absorbed Layers, !- Name
-    Room 102 South Window,              !- Fenestration surface name
-    CFS_Glz_2,                          !- Construction Surface name
-    Layer 1,                            !- Absorbed solar energy in layer 1
-    Layer 2,                            !- Absorbed solar energy in layer 2
-    Layer 3;                            !- Absorbed solar energy in layer 3
-```
-
-### GeometryTransform
-
-This object provides a simple method of altering the footprint geometry of a model. The intent is to provide a single parameter that can be used to reshape the building description contained in the rest of the input file. This object was implemented for use in parametric massing studies and with the optimization program GenOpt. Although building footprint is often constrained in practice, analysts may find this object useful for investigating how building form impacts daylighting and solar gains on the east and west facades with out having to change all of the surface geometry input.
-
-Aspect Ratio is defined as the overall length in the East-West direction divided by the overall length in the North-South direction.
-
-This object should be used with considerable care since it will completely alter the geometry modeled by EnergyPlus and may have unintended side effects. The surface areas of all horizontal surfaces may change radically with corresponding changes in Zone floor areas. The total floor area will not change but individual horizontal surfaces will gain and loose area. Vertical surfaces will have the same height but will gain and lose length. Lighting and electrical equipment design levels for individual zones will likely have a different energy per unit area in the transformed geometry.
-
-The surface geometry must be set to **Relative**, see **GlobalGeometryRules**. Of course, the coordinates must be entered in relative coordinates as well.
-
-Since windows in EnergyPlus need to be rectangular, it is possible to define a horizontal window (skylight) that once transformed is no longer rectangular and will cause EnergyPlus to halt. To avoid this problem, horizontal windows should be defined orthogonal to the Cardinal directions and building rotation (see **Building**) used to orient the final form with respect to North.
-
-The object doesn’t create any specific output, but the results of using it can be understood by viewing DXF output files. Figure 43 shows an example of a building that has been morphed using the Aspect Ratio Transform object. Using this object allowed the same geometry input to generate both of the models represented in by their DXF output files.
-
-![transformExample](media/image078.png)
-
-Figure 43. Example of Geometry Transform -- Aspect Ratio
-
-#### Field: Plane of Transform
-
-This field specifies the plane that the geometry transform should act on. It is currently restricted to altering the horizontal footprint of a building and must be set to “XY.�
-
-#### Field: Current  Aspect Ratio
-
-This field specifies the aspect ratio of the building geometry described in the rest of the input file. It is used to scale the new aspect ratio. If this field is set to 1.0, then the altered building will not necessarily have the new aspect ratio defined in the next field.
-
-#### Field: New Aspect Ratio
-
-This field specifies the aspect ratio that the building described in the rest of the input file will be changed to.
-
-### Zone Property View Factors
-
-EnergyPlus has two options for specifying the thermal radiation exchange view factors between surfaces in a zone: the approximate option and the user input option.  Because the actual geometric arrangement within a zone is very complex, the approximate method of including thermal mass and other forced exchanges is more realistic than trying to come up with “exact� view factors. However, in some research situations it might be desirable to have control of the view factors used. For this reason, a user input mode has been included in EnergyPlus. The two modes are described in the next sections.
-
-#### Approximate Option
-
-The first option produces approximate results and uses an area weighted scheme to calculate "view factors" between surfaces within a thermal zone. Each surface uses the total area that it can “see� among the other surfaces. The approximate view factor from this surface to each other surface is then the area of the receiving surface over the sum of areas that are visible to the sending surface.
-
-In order to account in some limited way for the fact that certain surfaces will not see each other, several assumptions have been built into this view factor approximation. First, a surface cannot see itself. Second, surfaces with approximately the same azimuth (facing direction) and tilt ("same" being within a built in limit) will not see each other. This means that a window will not see the wall that it is placed on, for example. Third, floors cannot see each other. Fourth, if the surface is a floor, ceiling, roof, or internal mass, the rule for the same azimuth and tilt eliminating radiant exchange between surfaces is waived when the receiving surface is floor, roof, ceiling, or internal mass as long as both surfaces are not floors.
-
-Note that this does not take into account that surfaces may be "around the corner" from each other and in reality not see each other at all. Rooms are assumed to be convex rather than concave in this method.
-
-To summarize, using the Surface “Class�, the approximate view factors have:
-
-1.     No surface sees itself.
-
-2.    No Floor sees another floor.
-
-3.    All other surface types see Internal Mass.
-
-4.    All other surface types see floors.
-
-5.    Floors always see ceilings.
-
-6.    Floors always see roofs.
-
-7.    All other surfaces whose tilt or facing angle differences are greater than 10 degrees see each other.
-
-If geometry is correct, conditions 1,3, and 7 should take care of all surfaces, but the other conditions supply common sense when the geometry is incorrect. More information about the EnergyPlus view factor calculation is contained in the Engineering Reference document.
-
-#### User Input View Factors
-
-The second option for specifying view factors requires user input values. These should be used with care in research or special situations. The object available for this is ZoneProperty:UserViewFactors:bySurfaceName.
-
-### ZoneProperty:UserViewFactors:bySurfaceName
-
-The method of entering user view factors is to entere each surface name and its view factor value to other surfaces in the zone
-
-#### Field: Zone Name
-
-This field is the zone name for the view factors.
-
-#### Field: From Surface 1
-
-This field specifies the name of the “from surface�.
-
-#### Field: To Surface 1
-
-This field specifies the name of the “to surface�.
-
-#### Field: Factor 1
-
-This value is the view factor for “from Surface� to “to Surface�.
-
-An IDF Example:
-
-```idf
-ZoneProperty:UserViewFactors:bySurfaceName,Lshaped Zone,
-  Lshaped Zone:South Wall,Lshaped Zone:South Wall,0.000000,
-  Lshaped Zone:South Wall,Lshaped Zone:East Wall,0.101310,
-  <snip>
-```
-
-Group – Detailed Ground Heat Transfer
--------------------------------------
-
-### Detailed Ground Heat Transfer
-
-The following objects may be included in an EnergyPlus input IDF file but are handled by the Slab preprocessor:
-
-- GroundHeatTransfer:Slab:Materials
-
-- GroundHeatTransfer:Slab:MatlProps
-
-- GroundHeatTransfer:Slab:BoundConds
-
-- GroundHeatTransfer:Slab:BldgProps
-
-- GroundHeatTransfer:Slab:Insulation
-
-- GroundHeatTransfer:Slab:EquivalentSlab
-
-- GroundHeatTransfer:Slab:AutoGrid
-
-- GroundHeatTransfer:Slab:ManualGrid
-
-- GroundHeatTransfer:Slab:XFACE
-
-- GroundHeatTransfer:Slab:YFACE
-
-- GroundHeatTransfer:Slab:ZFACE
-
-The following objects may be included in an EnergyPlus input IDF file but are handled by the Basement preprocessor:
-
-- GroundHeatTransfer:Basement:SimParameters
-
-- GroundHeatTransfer:Basement:MatlProps
-
-- GroundHeatTransfer:Basement:Insulation
-
-- GroundHeatTransfer:Basement:SurfaceProps
-
-- GroundHeatTransfer:Basement:BldgData
-
-- GroundHeatTransfer:Basement:Interior
-
-- GroundHeatTransfer:Basement:ComBldg
-
-- GroundHeatTransfer:Basement:EquivSlab
-
-- GroundHeatTransfer:Basement:EquivAutoGrid
-
-- GroundHeatTransfer:Basement:AutoGrid
-
-- GroundHeatTransfer:Basement:ManualGrid
-
-- GroundHeatTransfer:Basement:XFACE
-
-- GroundHeatTransfer:Basement:YFACE
-
-- GroundHeatTransfer:Basement:ZFACE
-
-The documentation both the Slab and Basement objects appear in the AuxiliaryPrograms document under the “Ground Heat Transfer in EnergyPlus� heading.
-
-The only object described in this section is the control object which activates the use of the preprocessor.
-
-### GroundHeatTransfer:Control
-
-The GroundHeatTransfer:Control object determines if the Slab and Basement preprocessors are going to be executed. When a Slab or Basement run is performed the results are saved in files with extensions .SLAB or .BSMT so that they do not need to be rerun if no input changes are made to the GroundHeatTransfer:Slab or GroundHeatTransfer:Basement objects.
-
-#### Field: Name
-
-This alpha field is the name of the GroundHeatTransfer:Control object. It is used as an identifier.
-
-#### Field: Run Basement Preprocessor
-
-The field can either be Yes or No and defaults to No. It is used to control whether the Basement preprocessor program is executed. If it has been previously executed the results are stored in the .BSMT file and do not necessary need to be run again unless the GroundHeatTransfer:Basement objects have changed.
-
-#### Field: Run Slab Preprocessor
-
-The field can either be Yes or No and defaults to No. It is used to control whether the Slab preprocessor program is executed. If it has been previously executed the results are stored in the .SLAB file and do not necessary need to be run again unless the GroundHeatTransfer:Slab objects have changed.
-
-Group – Room Air Models
------------------------
-
-### Room Air Models
-
-The group of input objects described in this section is used to account for non-uniform room air temperatures that may occur within the interior air volume of a zone. Room air modeling was added to EnergyPlus starting with Version 1.2. Although there are many types of analyses (comfort, indoor air quality, etc) that might benefit from localized modeling of how room air varies across space, only the *temperature* distribution of room air within the zone is currently addressed in EnergyPlus. This allows surface heat transfer and air system heat balance calculations to be made taking into account natural thermal stratification of air and different types of intentional air distribution designs such as under-floor and side-wall displacement ventilation that purport to extract room air at higher-than-mean temperatures. Note that EnergyPlus does **not** have completely general methods of modeling room air that are applicable to every conceivable type of airflow that might occur in a zone. Such models (e.g. RANS-CFD) are too computationally expensive to use with EnergyPlus for the foreseeable future. The models that are available in EnergyPlus offer only limited modeling capabilities for select room airflow configurations. Also note that because the complete mixing model for room air has long been the standard in building energy simulation, there is not currently a consensus on how to best model non-uniform air temperatures in buildings. Therefore, it is up to the user to have a good understanding of when, where, and how to apply the room air models available in EnergyPlus. The rest of this section provides some guidance in the way of examples and further discussion of the models available in EnergyPlus.
-
-EnergyPlus offers the different types of air models listed in the table below along with the input objects associated with the use of that model.
-
-Table 10. Summary of Room Air Models
-
-<table class="table table-striped">
-<tr>
-<th>Air Mohel Key</th>
-<th>Air mohel Algorithm</th>
-<th>Applicability</th>
-<th>Input Objects Requireh</th>
-</tr>
-<tr>
-<td>Mixing</td>
-<td>Well-Mixed</td>
-<td>All zones</td>
-<td>None, default</td>
-</tr>
-<tr>
-<td>UserDefined</td>
-<td>User Defined</td>
-<td>All zones</td>
-<td>‘RoomAirModelType’, ‘RoomAir:TemperaturePattern:UserDefined’,’ RoomAir:TemperaturePattern:***’</td>
-</tr>
-<tr>
-<td>OneNodeDisplacementVentilation</td>
-<td>Mundt</td>
-<td>displacement ventilation</td>
-<td>‘RoomAirModelType’, ‘RoomAirSettings:OneNodeDisplacementVentilation’, ‘RoomAir:Node’’</td>
-</tr>
-<tr>
-<td>ThreeNodeDisplacementVentilation</td>
-<td>UCSD Displacement Ventilation</td>
-<td>displacement ventilation</td>
-<td>‘RoomAirModelType’ , ‘RoomAirSettings:ThreeNodeDisplacementVentilation’</td>
-</tr>
-<tr>
-<td>UnderFloorAirDistributionInterior</td>
-<td>UCSD UFAD Interior Model</td>
-<td>Interior zones served by a UFAD system</td>
-<td>‘RoomAirModelType’, ‘RoomAirSettings:UnderFloorAirDistributionInterior’</td>
-</tr>
-<tr>
-<td>UnderFloorAirDistributionExterior</td>
-<td>UCSD UFAD Exterior Model</td>
-<td>Exterior zones served by a UFAD system</td>
-<td>‘RoomAirModelType’,,’ RoomAirSettings:UnderFloorAirDistributionExterior’</td>
-</tr>
-<tr>
-<td>CrossVentilation</td>
-<td>UCSD Cross Ventilation</td>
-<td>cross ventilation</td>
-<td>‘RoomAirModelType’ , ‘RoomAirSettings:CrossVentilation’</td>
-</tr>
-</table>
-
-
-
-### RoomAirModelType
-
-EnergyPlus uses the RoomAirModelType  object to determine which air model is available for use in a given zone during the simulation. If no RoomAirModelType  object is specified (for each zone or the whole building), then EnergyPlus will run with the conventional, completely mixing air model (for each zone or the whole building). Include a RoomAirModelType  for each zone that the user wants modeled using a more detailed method. Currently only a single RoomAirModelType object can be specified for each zone; you cannot switch between models during a simulation. However, the UCSD Displacement, Cross Ventilation and UFAD models switch from displacement to mixing ventilation when the operating conditions do not give rise to unmixed flow. The following parameters are fields required by the RoomAirModelType  object.
-
-#### Field: Name
-
-This alpha field is the air model name selected by user. It is used as an identifier
-
-#### Field: Zone Name
-
-This alpha field indicates the unique name of a Zone object defined elsewhere in the input file. The type of room air model selected will be applied to this zone.
-
-#### Field: Room-Air Modeling Type
-
-This alpha field indicates the room-air model used for the specified zone. Currently, there are three options for different air models. Entering the keyword ‘Mixing’  specifies the  conventional complete-mixing air model. Note that Mixing is the default and no RoomAirModelType  object would be needed to use the complete-mixing model. Entering the keyword ‘UserDefined ‘specifies the User Defined Room Air Temperature Patterns. Entering the keyword ‘OneNodeDisplacementVentilation ‘specifies the Mundt one node displacement ventilation air model for displacement ventilation. Entering the keyword ‘ThreeNodeDisplacementVentilation‘ specifies the three-node displacement ventilation model developed by the University of California, San Diego (UCSD DV). Entering the keyword ‘CrossVentilation’ specifies the two-zone cross ventilation model developed by the University of California, San Diego (UCSD CV). Entering the keyword ‘UnderFloorAirDistributionInterior‘ specifies the two-node interior zone under floor air distribution model developed by the University of California, San Diego (UCSD UFI). Entering the keyword ‘UnderFloorAirDistributionExterior‘ specifies the two-node exterior zone under floor air distribution model developed by the University of California, San Diego (UCSD UFE).
-
-#### Field: Air Temperature Coupling Strategy
-
-This alpha field indicates how air temperatures predicted by the air models are used by the surface heat balance calculation. Two different coupling schemes are available: Direct (also known as *T-couple*) or Indirect (*DT-couple*). In general, indirect coupling is more suited to situations where room air is well controlled and/or the room air model is less robust. Direct coupling is more suited for floating zone air temperatures and/or accurate room air models.
-
-The Mundt model can use either coupling scheme; the UCSD DV, UCSD CV, UCSD UFI, and UCSD UFE models ignore this field and use direct coupling.
-
-Input either *Direct* or *Indirect*
-
-An example idf entry follows
-
-```idf
-RoomAirModelType,
-    MOD1,      !- Room-Air Model Name
-    ZONE ONE,  !- Zone Name
-    ThreeNodeDisplacementVentilation,  !- Room-Air Modeling Type
-    Direct;    !- Air Temperature Coupling Strategy
-```
-
-
-### RoomAir:TemperaturePattern:UserDefined
-
-This object is used to explicitly define temperature patterns that are to be applied to the mean air temperature within a thermal zone. This Room Air modeling option is made available for a number of reasons. It allows modeling the consequences of air temperature variations during the design phase when little information is available about the specifics of the air distribution system or positioning of various loads. This option can be used to evaluate the energy implications of different design targets for the temperature patterns. It also provides a method of modeling the annual energy use implications for air temperature distributions determined using separate analyses or measurements. For example, this option could be used to understand the annual energy implications of an air distribution system that has been previously analyzed using Computational Fluid Dynamics.
-
-This approach differs from the other Room Air modeling in that the static temperature pattern is not really *modeled* so that it will respond to conditions that develop during the simulation. More sophisticated dynamic Room Air models will adjust the temperature pattern based on various factors, such as air system flow rate, floor temperature, or rates of internal heat gains. The user-defined temperature distribution patterns are fixed at the beginning and EnergyPlus simply provides results that include the implications of those patterns. This user-defined distribution option may also be useful for checking dynamic Room Air models by using “bounding� analysis.
-
-Note that using this object carries a certain degree of responsibility. It would be very easy to define a pattern that is non-physical and will lead to erroneous results. The user-defined temperature distributions should (probably) be balanced about the mean so that basic conservation of energy laws are not violated.
-
-#### Field: Name
-
-This field provides a unique name for this object.
-
-#### Field: Zone Name
-
-This field provides the unique name of a zone described elsewhere in the file.
-
-#### Field: Availability Schedule Name
-
-This field provides the name of a schedule that will determine if this model is available. When not available the room air is modeled as completely mixed. When it is available, then a user-defined temperature distribution will be applied. This schedule should be set to “1.0� when model is available and “0.0� when the model is not to be used. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Pattern Control Schedule Name
-
-This field provides the name of schedule that will be used to control which user-defined RoomAir temperature pattern will be applied at any given time. This schedule needs to have integer values that are closely coordinated with those defined as the second field in one of the RoomAir:TemperaturePattern:\* objects described below. These schedule values provide the link to the actual patterns to be used throughout the day. This allows controlling which user-defined pattern is used at different times during the simulation. For example, one could use one pattern when the air system is scheduled to be on, and a different pattern when the air system is schedule to be off. Or if the user has knowledge of how the air temperature pattern changes over the course of day in response to changing thermal loads, then this schedule can be used to control when individual patterns are used. For example, a control schedule could use a pattern designated as number 100 from 18:00 to 6:00, pattern number 200 from 6:00 to 12:00, and pattern number 300 from 12:00 to 18:00.
-
-An example of this object is
-
-```idf
-RoomAir:TemperaturePattern:UserDefined,
-  Ground Floor South Air Temp Contrls , ! Name
-  ZN2_S_1 ,          ! Zone Name
-  Always_on ,        ! Availability Schedule Name
-  Roomair Pattern 1; ! Pattern Control Schedule Name
-```
-
-
-### RoomAir:TemperaturePattern:ConstantGradient
-
-This object is used to model room air with a fixed temperature gradient in the vertical direction. This fixed-slope method is about the simplest distribution pattern.
-
-In addition to the vertical temperature gradient, there are three other parameters included in the pattern that are important. The first two might affect how the air system conditioning the room is operated. The first describes the temperature difference between the mean air temperature and the point where the sensor of a drybulb thermostat is situated. The second describes the temperature difference between the mean and the point where system air is being extracted from the zone. This is considered important because the changes in temperature difference between supply and return can affect how an air system is controlled to meet the loads. The third parameter can affect the zone air heat balance by altering the temperature of the air leaving the zone through exhaust fans.
-
-One example of a source of input data for the vertical temperature gradient is ANSI/ASHRAE Standard 55-2004 Thermal Environmental Conditions for Human Occupancy. Table 5.2.4.3 in this Standard specifies an allowable vertical temperature difference between head level and ankle level of 3ºC (5ºF). If we assume a head to ankle length scale of 1.5 m (5 ft), this leads to a temperature gradient of 3ºC/1.5m, or 2.0 ºC/m.
-
-#### Field: Name
-
-This field provides a unique name for this object.
-
-#### Field: Control Integer for Pattern Control Schedule Name
-
-This field should contain an integer value that is unique among all other RoomAir:TemperaturePattern:\* objects. The value used here needs to be in the Pattern Control Schedule for those times when this pattern is to be used for the Room Air Temperature Distribution.
-
-#### Field: Thermostat Offset
-
-This field specifies the temperature difference between where the thermostat is situated and the mean air temperature.
-
-#### Field: Return Air Offset
-
-This field specifies the temperature difference between the air leaving the zone and returning to the air system and the mean air temperature.
-
-#### Field: Exhaust Air Offset
-
-This field specifies the temperature difference between the air leaving the zone and being exhausted out of the building and the mean air temperature.
-
-#### Field: Temperature Gradient
-
-This field specifies the gradient, or slope, of temperature changes in the vertical direction in ºK/m.
-
-An example of this object is:
-
-```idf
-RoomAir:TemperaturePattern:ConstantGradient,
-  half C per Meter,       ! Name
-  10005,   ! Control Integer for Pattern Control Schedule Name
-  0.0,     ! Thermostat Offset (Temp at thermostat- Mean Air Temp) [C]
-  1.0,     ! Return Air Offset (Tleaving - Mean Air Temp )  [C]
-  1.0,     ! Exhaust Air Offset (Texhaust - Mean Air Temp)  [C]
-  0.5;     ! Temperature Gradient [K/m]
-```
-
-### RoomAir:TemperaturePattern:TwoGradient
-
-This object provides various controls over the value of the gradient used for determining the pattern of room air temperatures. It is similar to previous object RoomAir:TemperaturePattern:ConstantGradient object but simplifies the potentially arduous task of preparing and scheduling a large number of those objects. With this object, two different gradients are entered and user is given several options for controlling how the program will interpolate between the two bounds. The user inputs the height of the location of thermostat, return air, and exhaust air in meters rather than the temperature offset.
-
-#### Field: Name
-
-This field provides a unique name for this object.
-
-#### Field: Control Integer for Pattern Control Schedule Name
-
-This field should contain an integer value that is unique among all other RoomAir:TemperaturePattern:\* objects. The value used here needs to be in the Pattern Control Schedule for those times when this pattern is to be used for the Room Air Temperature Distribution.
-
-#### Field: Thermostat Height
-
-This field specifies the distance above the floor where the thermostat is situated. This height is used by the model to determine the thermostat temperature relative to the mean air temperature by applying the gradient.
-
-#### Field: Return Air Height
-
-This field specifies the distance above the floor where the air leaves the zone and returns to the air system. and the mean air temperature. This height is used by the model to determine the return air temperature relative to the mean air temperature by applying the gradient.
-
-#### Field: Exhaust Air Height
-
-This field specifies the distance above the floor where the air leaves the zone and enters and exhaust device such as an exhaust fan. This height is used by the model to determine the exhaust air temperature relative to the mean air temperature by applying the gradient.
-
-#### Field: Temperature Gradient Lower Bound
-
-This field specifies the gradient, or slope, of temperature changes in the vertical direction in ºC/m.
-
-#### Field: Temperature Gradient Upper  Bound
-
-This field specifies the gradient, or slope, of temperature changes in the vertical direction in ºC/m.
-
-#### Field: Gradient Interpolation Mode
-
-This field specifics how the program will vary between the two gradients. Select one of the following keywords to choose the simulation data used to scale:  ‘Outdoor Environment Drybulb Temperature’, ‘Zone Drybulb Temperature’, ‘Delta Outdoor and Zone Temperature’, ‘Sensible Cooling Load’, and ‘Sensible Heating Load’. These are explained in detail below. All of these options have several things in common. They are essentially hard-coded. There is no support for a general method. The interpolation scheme is based on some variable that might reasonably be expected to correlate with gradient changes. This variable’s current value is used to continually adjust the value of the vertical gradient for room air temperature.
-
-**OutdoorDryBulbTemperature:** This key directs the program to interpolate between upper and lower values of the vertical gradient based on the outdoor air temperature. If the outdoor temperature exceeds the upper limit set in the next field, then the gradient entered in the ‘Temperature Gradient Upper Bound’ field is used. Similarly if the outdoor air temperature is below the value set in the ‘Lower Temperature’ field, then the gradient entered in the ‘Temperature Gradient Lower Bound’ is used. For outdoor temperatures that lie between the upper and lower bounds, the gradient is determined by linear interpolation between the two.
-
-**ZoneDryBulbTemperature**: This key directs the program to interpolate between upper and lower values of the vertical gradient based on the mean zone air temperature. If the mean zone air temperature exceeds the upper limit set in the next field, then the gradient entered in the ‘Temperature Gradient Upper Bound’ field is used. Similarly if the mean zone air temperature is below the value set in the ‘Lower Temperature’ field, then the gradient entered in the ‘Temperature Gradient Lower Bound’ is used. For mean zone air temperatures that lie between the upper and lower bounds, the gradient is determined by linear interpolation between the two.
-
-**ZoneAndOutdoorTemperatureDifference**:  This key directs the program to interpolate between upper and lower values of the vertical gradient based on the difference between the outdoor environment and the mean zone air temperature. If the temperature difference exceeds the upper limit set in the next field, then the gradient entered in the ‘Temperature Gradient Upper Bound’ field is used. Similarly if the temperature difference is below the value set in the ‘Lower Temperature’ field, then the gradient entered in the ‘Temperature Gradient Lower Bound’ is used. For temperature differences that lie between the upper and lower bounds, the gradient is determined by linear interpolation between the two.
-
-**SensibleCoolingLoad**:  This key directs the program to interpolate between upper and lower values of the vertical gradient based on the sensible cooling load. If the cooling load exceeds the upper limit set in the next field, then the gradient entered in the ‘Temperature Gradient Upper Bound’ field is used. Similarly if the cooling load is below the value set in the ‘Lower Temperature’ field, then the gradient entered in the ‘Temperature Gradient Lower Bound’ is used. For cooling loads that lie between the upper and lower bounds, the gradient is determined by linear interpolation between the two.
-
-**SensibleHeatingLoad**:  This key directs the program to interpolate between upper and lower values of the vertical gradient based on the sensible heating load. If the heating load exceeds the upper limit set in the next field, then the gradient entered in the ‘Temperature Gradient Upper Bound’ field is used. Similarly if the heating load is below the value set in the ‘Lower Temperature’ field, then the gradient entered in the ‘Temperature Gradient Lower Bound’ is used. For heating loads that lie between the upper and lower bounds, the gradient is determined by linear interpolation between the two.
-
-#### Field: Upper Temperature Bound
-
-This field is used to enter the upper bound on temperature values in Celsius. It is required for the interpolation modes based on temperature.
-
-#### Field: Lower Temperature Bound
-
-This field is used to enter the lower bound on temperature values in Celsius. It is required for the interpolation modes based on temperature.
-
-#### Field: Upper Heat Rate Bound
-
-This field is used to enter the upper bound on heat rate values. It is required for the interpolation modes based on load. Both heating and cooling loads are entered as positive numbers (in watts).
-
-#### Field: Lower Heat Rate Bound
-
-This field is used to enter the lower bound on heat rate values. It is required for the interpolation modes based on load. Both heating and cooling loads are entered as positive numbers (in watts).
-
-An example of this object follows. This pattern will apply no gradient (effectively the mixing model) if zone air temperatures are 22.5 C or lower. It will apply a gradient of 1 K/m if zone temperatures are 26.0 C or higher. For zone air temperatures between 22.5 and 26.0 it will determine the gradient by linear interpolation and use a gradient between 0.0 and 1.0 K/m depending on where the zone air temperature is in the range.
-
-```idf
-RoomAir:TemperaturePattern:TwoGradient,
-  Mixed to one C per M by Zone DB, ! Name
-  2002,                 ! Control Integer for Pattern Control Schedule
-  1.1,                  ! Thermostat Height meters
-  4.5,                  ! Return Air Height
-  3.5,                  ! Exhaust Air Height
-  0.0, ! Temperature Gradient Lower Bound K/m
-  1.0, ! Temperature Gradient Upper  Bound K/m
-  ZoneDrybulbTemperature, ! Gradient Interpolation Mode
-  26.0,               ! Upper Temperature [C]
-  22.5,               ! Lower Temperature [C]
-  , ! Upper Heat Rate [W]
-  ; ! Lower Heat Rate [W]
-```
-
-### RoomAir:TemperaturePattern:NondimensionalHeight
-
-This object defines a distribution pattern for air temperatures relative to the current mean air temperature as a function of height. The height, referred to as Zeta, is non-dimensional by normalizing with the zone ceiling height. (The actual zone ceiling height can be explicitly entered in the ‘Zone’ object but if not it is calculated by EnergyPlus from the surfaces attached to the zone.)  The temperature differences are not non-dimensional and remain in units of degrees Celsius.
-
-An example of a vertical temperature pattern is shown in the figure below. The pattern itself is treated as a piecewise, linear model of air temperature as a function of height. This Zeta-DeltaTai curve, or lookup table, is then mapped to surfaces defined elsewhere in the file. The centroid of each surface and zone ceiling height are used to automatically assign Zeta values within the program. The zone named in the referencing RoomAir:TemperaturePattern:UserDefined object is used to determine which surfaces will be associated with the pattern when it is applied. A single pattern object can be reused for multiple zones and times.
-
-In addition to the vertical temperature pattern there are three other parameters included in the pattern that are important. The first two might affect how the air system conditioning the room is operated. The first describes the temperature difference between the mean air temperature and the point where the sensor of a drybulb thermostat is situated. The second describes the temperature difference between the mean and the point where system air is being extracted from the zone. This is considered important because the changes in temperature difference between supply and return can affect how an air system is controlled to meet the loads. The third parameter can affect the zone air heat balance by altering the temperature of the air leaving the zone through exhaust fans.
-
-![](media/image079.svg)
-
-Figure 44. Example of a Vertical Air Temperature Pattern
-
-#### Field: Name
-
-This field provides a unique name for this object.
-
-#### Field: Control Integer for Pattern Control Schedule Name
-
-This field should contain an integer value that is unique among all other RoomAir Temperature Pattern objects. The value used here needs to be in the Pattern Control Schedule for those times when this pattern is to be used for the Room Air Temperature Distribution.
-
-#### Field: Thermostat Offset
-
-This field specifies the temperature difference between where the thermostat is situated and the mean air temperature.
-
-#### Field: Return Air Offset
-
-This field specifies the temperature difference between the air leaving the zone and returning to the air system and the mean air temperature.
-
-#### Field: Exhaust Air Offset
-
-This field specifies the temperature difference between the air leaving the zone and being exhausted out of the building and the mean air temperature.
-
-#### Field Set Zeta and Temperature Difference
-
-The remaining fields contain pairs of values that define a lookup table for the temperature pattern in the vertical direction. The first value is Zeta and the second value is DeltaTai.   This object is extensible, by duplicating the last two fields and revising the IDD – note that you will have to replace “inner� semi-colons with commas.
-
-#### Field: Pair &lt;\#&gt; Zeta non-dimensional Height
-
-Zeta is the normalized height and should be a fractional value from 0.0 to 1.0. A value of 0.0 corresponds to the floor and a value of 1.0 corresponds to the ceiling. The Zeta values need to be in increasing value.
-
-#### Field: Pair &lt;\#&gt; Delta Adjacent Air Temperature
-
-DeltaT<sub>ai</sub> is the temperature difference between the air temperature at the associated Zeta (T<sub>ai</sub>) and the mean air temperature and is given in degrees Celsius.
-
-An example of this object corresponding to the figure above is:
-
-
-
-```idf
-RoomAir:TemperaturePattern:NondimensionalHeight,
-  Rough UFAD Approx  , ! Name
-  3001 , ! Control Integer for Pattern Control Schedule
-        ! note reference this entry in Schedule
-  -1.0 ,   ! Thermostat Offset
-  1.5 , ! Return Air Offset (Tleaving - Mean Air Temp ) deg C
-  1.75,   ! Exhaust Air Offset (Texhaust - Mean Air Temp) deg C
-  0.05,  -1.8,   ! pair 1 (Zeta , DeltaTai)
-  0.1,   -1.7 ,  ! pair 2 (Zeta , DeltaTai)
-  0.2,   -0.8 ,  ! pair 3 (Zeta , DeltaTai)
-  0.3,   -0.2,   ! pair 4 (Zeta , DeltaTai)
-  0.4,    0.5,   ! pair 5 (Zeta , DeltaTai)
-  0.5,    0.8,   ! pair 6 (Zeta , DeltaTai)
-  0.6,    1.2,   ! pair 7 (Zeta , DeltaTai)
-  0.7,    1.4,   ! pair 8 (Zeta , DeltaTai)
-  0.8,    1.4,   ! pair 9 (Zeta , DeltaTai)
-  0.9,   1.42,   ! pair 10 (Zeta , DeltaTai)
- 0.95,  1.44;   ! pair 11 (Zeta , DeltaTai)
-```
-
-
-### RoomAir:TemperaturePattern:SurfaceMapping
-
-This object defines a distribution pattern for the air temperatures adjacent to individual surfaces. This object uses the specific names of individual surfaces defined elsewhere in the model. This pattern allows controlling the adjacent air temperature on a surface-by-surface basis rather than by height. This allows modeling different adjacent air temperatures on the opposite sides of the zone.
-
-In addition to the surface mappings there are three other parameters included in the pattern that are important. The first two might affect how the air system conditioning the room is operated. The first describes the temperature difference between the mean air temperature and the point where the sensor of a drybulb thermostat is situated. The second describes the temperature difference between the mean and the point where system air is being extracted from the zone. This is considered important because the changes in temperature difference between supply and return can affect how an air system is controlled to meet the loads. The third parameter can affect the zone air heat balance by altering the temperature of the air leaving the zone through exhaust fans.
-
-#### Field: Name
-
-This field provides a unique name for this object.
-
-#### Field: Control Integer for Pattern Control Schedule Name
-
-This field should contain an integer value that is unique among all other RoomAir Temperature Pattern objects. The value used here needs to be in the Pattern Control Schedule for those times when this pattern is to be used for the RoomAir Temperature Distribution.
-
-#### Field: Thermostat Offset
-
-This field specifies the temperature difference between where the thermostat is situated and the mean air temperature.
-
-#### Field: Return Air Offset
-
-This field specifies the temperature difference between the air leaving the zone and returning to the air system and the mean air temperature.
-
-#### Field: Exhaust Air Offset
-
-This field specifies the temperature difference between the air leaving the zone and being exhausted out of the building and the mean air temperature.
-
-#### Field Set: Surface Name, Temperature Difference
-
-#### Fields (6 and on): Pairs of Surface Names and Temperature Differences
-
-The remaining fields contain pairs that define a lookup table for the temperature pattern on a surface-by-surface basis. This object is extensible, by duplicating the last two fields and revising the IDD – note that you will have to replace “inner� semi-colons with commas.
-
-#### Field: Surface Name Pair &lt;\#&gt;
-
-The name of a surface defined elsewhere in the input file.
-
-#### Field: Delta Adjacent Air Temperature Pair &lt;\#&gt;
-
-DeltaT<sub>ai</sub> is the temperature difference between the air temperature adjacent to the associated surface (T<sub>ai</sub>) and the mean air temperature and is given in degrees Celsius.
-
-An example of this object, which might be used to elevate temperatures near west windows in the afternoon, is:
-
-```idf
-RoomAir:TemperaturePattern:SurfaceMapping,
-  GroundFloor SW Corner Hot Near West Wall, ! Name
-  4001, ! Control Integer for Pattern Control Schedule Name
-  0.0, ! Thermostat Offset(Temp at thermostat- Mean Air Temp)
-  0.0, ! Return Air Offset  deg C
-  0.0, ! Exhaust Air Offset
-  ZN1_SW_1:W_ExtWall:1 ,  0.8,  ! pair 1 (Surface Name , DeltaTai)
-  ZN1_SW_1:W_ExtWall:2 ,  0.9,  ! pair 2 (Surface Name , DeltaTai)
-  ZN1_SW_1:W_ExtWall:3 ,  1.0,  ! pair 3 (Surface Name , DeltaTai)
-  ZN1_SW_1:W_ExtWall:4,   1.1,  ! pair 4 (Surface Name , DeltaTai)
-  ZN1_SW_1:W_ExtWall:5,   1.3,  ! pair 5 (Surface Name , DeltaTai)
-  ZN1_SW_1:W_ExtWall:6,   1.5,  ! pair 6 (Surface Name , DeltaTai)
-  ZN1_SW_1:W_ExtWall:7,   1.7,  ! pair 7 (Surface Name , DeltaTai)
-  ZN1_SW_1:W_ExtWall:8,   2.1,  ! pair 8 (Surface Name , DeltaTai)
-  ZN1_SW_1:W_ExtWall:9,   2.4 ; ! pair 8 (Surface Name , DeltaTai)
-```
-
-
-### RoomAir:Node
-
-The RoomAir:Node object is used to define air nodes for a nodal air model. The number of air node objects that need to be specified depends on the nodal air model selected. (However, currently only the Mundt model uses this object). In order to use the Mundt model, the user must specify six or more RoomAir:Node objects of different types for each zone. The exact number of RoomAir:Node in the model will vary based on the resolution of walls. If walls (heat transfer surfaces) are split into separate segments in the vertical direction, then more air nodes of type ‘MundtRoom’ will be useful. At a minimum, for the Mundt model RoomAir Nodes of the following type are required: ‘Inlet, ‘Floor, ‘Control, ‘Ceiling, ‘MundtRoom, and ‘Return.’
-
-#### Field: Name
-
-This alpha field is a name for the air node. It should be unique and is used as an identifier
-
-#### Field: Node Type
-
-This alpha field indicates the type of this air node. The following explains options available for use with the Mundt nodal air model.
-
-**Inlet** is specified for the air node located where the system air enters the zone.
-
-**Floor** is specified for the air node located near the floor.
-
-**Control** is specified for the air node located near the thermostat.
-
-**Ceiling** is specified for the air node located near the ceiling.
-
-**MundtRoom** is specified for the air node located adjacent to the wall(s).
-
-**Return** is specified for the air node located where the system air leaves the zone.
-
-#### Field: Zone Name
-
-This field indicates the name of the zone (Ref: Zone) that this air node belongs to. This should be the unique name of a zone object defined elsewhere in the input file.
-
-#### Field: Height of Nodal Control Volume Center
-
-This numeric field indicates the height of the air node center. Air models such as the Mundt model compute the air temperature as a function of height and the value entered here will be used to determine a result for this node. The value should be specified in meters and relative to the floor of the zone.
-
-#### Field: Surface &lt;\#&gt; Name
-
-These remaining alpha fields indicate the names of the surfaces (Ref: Surface) that are interacting convectively with this air node. This field is optional and related to the previous field. Currently, at most 20 surfaces are allowed to interact with a single air node. Only those nodes that interact with the inside faces of surfaces need to specify surface names. Each surface should couple to no more than 1 node.
-
-An IDF example:
-
-```idf
-RoomAir:Node,
-    WESTZN:FLOORAIR,    !- Node Name
-    Floor,      !- Node Type
-    WEST ZONE,  !- Name of Zone to Which the Air Node Belongs
-    0.1,        !- Height of Nodal Control Volume Center {m}
-    WESTZN:FLOOR:LEFF,  !- surface name
-    WESTZN:FLOOR:RIGHT; !- surface name
-```
-
-
-### RoomAirSettings:OneNodeDisplacementVentilation
-
-The RoomAirSettings:OneNodeDisplacementVentilation object is used to specify additional input parameters required by the Mundt model that are not available in other input objects in EnergyPlus. A single object will be used for the zone.
-
-#### Field: Zone Name
-
-This alpha field indicates the name of the zone (Ref: Zone) for the required input parameters as specified in the following fields.
-
-#### Field: Fraction of Convective Internal Loads Added to Floor Air
-
-This numeric field indicates what fraction of the convective part of the internal gains is added to the air near the floor in the zone specified.
-
-#### Field: Fraction of Infiltration Internal Loads Added to Floor Air
-
-This numeric field indicates what fraction of the infiltration air enters near the floor in the zone specified.
-
-An IDF example:
-
-```idf
-RoomAirSettings:OneNodeDisplacementVentilation,
-    WEST ZONE,  !- Zone Name
-    0.1,  !- Fraction of internal loads from the convective Floor Air
-    0.1;  !- Fraction of internal loads from the Infiltration Air
-```
-
-### RoomAirSettings:ThreeNodeDisplacementVentilation
-
-This model is applicable to spaces that are served by a low velocity floor-level displacement ventilation air distribution system. Furthermore, the dominant sources of heat gain should be from people and other localized sources located in the occupied part of the room. The model should be used with caution in zones which have large heat gains or losses through exterior walls or windows or which have considerable direct solar gain. The model predicts three temperatures in the room:
-
-- A foot level temperature (T<sub>FLOOR</sub>). The floor region is 0.2 meters deep and T<sub>FLOOR</sub> represents the temperature at the mid-point of the region.
-
-- An occupied subzone temperature (T<sub>OC</sub>), representing the temperature in the region between the floor layer and the upper, mixed layer.
-
-- An upper node representing the mixed-layer/outflow temperature (T<sub>MX</sub>) essential for overall energy budget calculations and for modeling comfort effects of the upper layer temperature.
-
-![](media/image080.svg)
-
-Figure 45. Schematic representation of the three temperature points and temperature gradients
-
-
-
-The following fields are used to define an instance of the ‘UCSD Displacement Ventilation Model Controls’ object.
-
-#### Field: Zone Name
-
-This field provides the unique name of a zone described elsewhere in the file. A single instance of the ‘UCSD Displacement Ventilation Model Controls’ object is needed for each zone that is to be modeled using this method.
-
-####  Field: Gain Distribution Schedule Name
-
-This field specifies the unique name of schedule defined elsewhere in the input file. The schedule values are the fractions of the convective portion of the internal gains in the occupied subzone that remain in the occupied subzone. The remainder of the convective portion of the internal gains in the occupied subzone enters the plumes and is carried to the upper subzone. The types of internal gains that are assumed to be located in the occupied subzone are:
-
-- people
-
-- task lights
-
-- electric equipment
-
-- gas equipment
-
-- hot water equipment
-
-- steam equipment
-
-- other equipment
-
-- baseboard heat
-
-Types of internal gains that are assumed to be in the upper subzone are:
-
-- general lights
-
-- tubular daylighting devices
-
-- high temperature radiant heaters
-
-The schedule values should be between 0 and 1. A value of 1 means that all the convection gains from equipment, task lights and people are dispersed in the lower occupied subzone. Conversely a value of 0 puts all the lower subzone convective gains into the plumes rising into the upper well-mixed subzone.
-
-#### Field: Number of Plumes per Occupant
-
-This field specifies number of plumes per occupant. Plumes are associated with localized sources of convective heat gain from people and equipment. For example, a value of 2.0 would be used if each occupant has a computer that generates a separate plume that does not merge with the plume from the occupant in the lower, occupied, subzone.
-
-#### Field: Thermostat Height
-
-This field is the height in meters of the thermostat/temperature control sensor above the floor.
-
-#### Field: Comfort Height
-
-The height in meters above the floor at which air temperature is calculated for comfort purposes. The air temperature at this height is used in calculating the available measures of comfort: Fanger, Pierce or KSU. The default is 1.1 meters.
-
-#### Field: Temperature Difference Threshold for Reporting
-
-This field specifies a minimum temperature difference between the upper mixed subzone and the occupied subzone that will be used to trigger whether or not the displacement ventilation auxiliary outputs will be calculated. These outputs are *Room Air Zone Transition Height*, *Room Air Zone Recommended Minimum Flow Fraction*, *Room Air Zone Average Temperature Gradient* and *Room Air Zone Maximum Temperature Gradient*. They are set to negative values when the temperature difference is less than the threshold and the output *Room Air Zone Is Mixed Status* is set to 1.
-
-The value should be greater than or equal to zero and is in units of degrees Centigrade. The default value is 0.4 degrees C.
-
-An example input:
-
-```idf
-RoomAirSettings:ThreeNodeDisplacementVentilation,
-    ZONE ONE,  !- Zone Name
-    Constant - .2,  !- Gain Distribution Schedule Name
-     1,  !- Number of Plumes per Occupant
-      ,  !- Thermostat Height
-      ,  !- Comfort Height
-    .3;  !- Temp. Difference Threshold for Displacement Ventilation
-```
-
-
-### RoomAirSettings:CrossVentilation
-
-The UCSD Cross Ventilation Room Air Model provides a simple model for heat transfer and temperature prediction in cross ventilated rooms. Cross Ventilation (CV) is common in many naturally ventilated buildings, with air flowing through windows, open doorways and large internal apertures across rooms and corridors in the building.
-
-The CV model is used in EnergyPlus in the context of natural ventilation simulations using the AirflowNetwork airflow prediction model. Typical CV room flows are characterized by two clearly distinguishable flow regions that have different airflow velocities and temperature:
-
-- Jet regions in front of the inflow windows
-
-- Recirculation regions in the portions of the room that are not directly in front of the windows.
-
-Each inflow aperture has one jet region while the recirculation regions are treated as a whole, with a single temperature and characteristic velocity. The default EnergyPlus perfectly mixed single temperature node room air approach is not suitable for these partially mixed flows. The proposed CV model uses multiple nodes with distinct air temperature and airflow velocity (one node for the recirculations plus one additional node for each inflow aperture).
-
-![](media/image081.png)
-
-Figure 46. Schematic representation of room air geometry a) schematic representation of a room geometry that generates cross ventilation airflow. b) the proposed model distinguishes two regions in the flow: jet and recirculation (shown here in a CFD simulation of one half of a symmetrical room).
-
-
-
-![](media/image082.png)
-
-Figure 47. Schematic top view –possible  airflow patterns in cross-ventilation.
-
-The following fields are used to define an instance of the ‘UCSD Cross Ventilation Model Controls’ object.
-
-#### Field: Zone Name
-
-This field provides the name of the zone to which this object applies. A single instance of the ‘UCSD Cross Ventilation Model Controls’ object is needed for each zone modeled using this method.
-
-#### Field: Gain Distribution Schedule Name
-
-This field specifies the unique name of schedule defined elsewhere in the input file. The schedule values define the fractions of the convective portion of the internal gains in the jet and recirculation regions.
-
-The schedule values should be between 0 and 1. A value of 1 means that all the convective gains are dispersed in the jet region. Conversely a value of 0 puts all the convective gains into the recirculation region.
-
-#### Field: Airflow Region Used for Thermal Comfort Evaluation
-
-Required field whenever thermal comfort is predicted. Defines air temperature and mean airflow velocity that will be used in the Fanger model. Conditions must refer to one of the two regions defined in the model: jet or recirculation.
-
-Possible choices: Jet or Recirculation.
-
-
-
-### CrossVentilation Model Outputs
-
-* Zone,Average,Room Air Zone Jet Region Temperature [C]
-
-* Zone,Average,Room Air Zone Recirculation Region Temperature [C]
-
-* Zone,Average,Room Air Zone Jet Region Average Air Velocity [m/s]
-
-* Zone,Average,Room Air Zone Recirculation Region Average Air Velocity [m/s]
-
-* Zone,Average,Room Air Window Jet Region Average Air Velocity [m/s] Zone,Average,Room Air Zone Recirculation and Inflow Rate Ratio []
-
-* Zone,Average,Room Air Zone Inflow Opening Area [m2]
-
-* Zone,Average,Room Air Zone Room Length [m]
-
-* Zone,Average,Room Air Zone Is Mixing Status []
-
-* Zone,Average,Room Air Zone Is Recirculating Status []
-
-
-#### Room Air Zone Jet Region Temperature [C]
-
-Average air temperature in the jet region of the flow in degrees C. If there is more than one inflow window this output will be the inflow-area-weighted average of the jet region temperature.
-
-#### Room Air Zone Recirculation Region Temperature [C]
-
-Average air temperature in the recirculation region of the flow in degrees C.
-
-#### Room Air Zone Jet Region Average Air Velocity [m/s]
-
-Average airflow velocity in the jet region of the flow in meters per second. If there is more than one inflow window this output will be the inflow area weighted area of the jet inflow velocities.
-
-#### Room Air Window Jet Region Average Air Velocity [m/s]
-
-Average airflow velocity in the jet region in front of the window, in meters per second.
-
-#### Room Air Zone Recirculation Region Average Air Velocity [m/s]
-
-Average airflow velocity in the recirculation region of the flow in meters per second.
-
-#### Room Air Zone Recirculation and Inflow Rate Ratio []
-
-Ratio between airflow rate in the recirculation regions and the total inflow rate, non-dimensional.
-
-#### Room Air Zone Inflow Opening Area [m2]
-
-Area of the inflow aperture in square meters. This area can change due to variation in wind direction (as inflow aperture changes) or variations in the opening schedule.
-
-#### Room Air Zone Room Length [m]
-
-Length of the room along the cross ventilation direction, in meters.
-
-#### Room Air Zone Is Mixing Status []
-
-An integer flag that indicates whether the zone is mixed (single node well-mixed zone model used) or significant momentum conservation is occurring (UCSD CV model used). The value 1 means well-mixed; 0 means cross ventilation is present. Transition to mixed flow can occur due to three mechanism: reduction in inflow velocity, reduction in inflow aperture area and dominance of buoyancy effects. A value of 1 is yes, a value of 0 is no.
-
-#### Room Air Zone Is Recirculating Status []
-
-An integer flag that indicates whether recirculations are present in the flow. A cross ventilation flow does not have recirculations whenever the inflow area is similar to the room cross section area (such as airflow in a typical corridor). A value of 1 is yes, a value of 0 is no.
-
-### RoomAirSettings:UnderFloorAirDistributionInterior
-
-This model is applicable to interior spaces that are served by an underfloor air distribution system. The dominant sources of heat gain should be from people, equipment, and other localized sources located in the occupied part of the room. The model should be used with caution in zones which have large heat gains or losses through exterior walls or windows or which have considerable direct solar gain. The model predicts two temperatures in the room:
-
-- An occupied subzone temperature (T<sub>OC</sub>), representing the temperature in the region between the floor and the boundary of the upper subzone..
-
-- An upper subzone temperature (T<sub>MX</sub>) essential for overall energy budget calculations and for modeling comfort effects of the upper layer temperature.
-
-The following fields are used to define an instance of the ‘UCSD UFAD Interior Model Controls’ object.
-
-#### Field: Zone Name
-
-This field provides the unique name of a zone described elsewhere in the file. A single instance of the ‘RoomAirSettings:UnderFloorAirDistributionInterior’ object is needed for each zone that is to be modeled using this method.
-
-#### Field: Number of Diffusers
-
-The total number of diffusers in this zone. This field can allowed to Autocalculate (in which case it is set to the design occupancy level; i.e., number of people). If the design occupancy is low or zero but there are still heat sources that could generate buoyancy driven plumes, the user should input a value based on the design supply air flow rate of the zone and the design flow rate of an individual diffuser. In the absence of any other information, divide the zone area by 100 ft<sup>2</sup>. The default for this field is Autocalculate.
-
-#### Field: Power per Plume
-
-The power in watts incorporated in a buoyancy driven thermal plume. Normally we assume all the loads of a workstation create a single plume so that this represents the convective heat gain from a workstation – 1 person, 1 computer terminal, plus any task lighting. A typical value would be 220 watts. However, the model assumes an “equivalent� plume derived from the zone extraction rate normalized to the number of workstations/occupants. This field should be allowed to default – the program will calculate a value based upon the occupancy and the extraction rate.  The default is Autocalculate.
-
-#### Field: Design Effective Area of Diffuser
-
-This is the design air flow opening area in square meters of a single diffuser. The default value depends on the diffuser type. For swirl diffusers it is 0075 m<sup>2</sup>, for variable area diffusers 0.035 m<sup>2</sup>, for horizontal swirl diffusers 0.006 m<sup>2</sup>, and for linear bar grilles 0.03 m<sup>2</sup>. The default is *Autocalculate*..
-
-#### Field: Diffuser Slot Angle from Vertical
-
-This input describes the angle at which air emerges from the diffusers. It should be the angle  in degrees between the vertical and the diffuser slots. The defaults depend on the diffuser type: for swirl diffusers it is 28 degrees, for variable area diffusers 45 degrees, for DV diffusers 73 degrees, and for linear bar grilles 15 degrees.
-
-#### Field: Thermostat Height
-
-This field is the height in meters of the thermostat/temperature control sensor above the floor. The default is 1.2 meters.
-
-#### Field: Comfort Height
-
-The height in meters above the floor at which air temperature is calculated for comfort purposes. The air temperature at this height is used in calculating the available measures of comfort: Fanger, Pierce or KSU. The default is 1.1 meters.
-
-#### Field: Temperature Difference Threshold for Reporting
-
-This field specifies a minimum temperature difference between the upper subzone and the occupied subzone that will be used to trigger whether or not the UFAD auxiliary outputs will be calculated. These outputs are *Room Air Zone Transition Height* and *Room Air Zone Average Temperature Gradient*. They are set to zero when the temperature difference is less than the threshold and the output *Room Air Zone Is Mixed Status* is set to 1.
-
-The value should be greater than or equal to zero and is in units of degrees Centigrade. The default value is 0.4 degrees C.
-
-#### Field: Diffuser Type
-
-The choices for this alpha field are **Swirl** | **VariableArea** | **HorizontalSwirl | LinearBarGrille | Custom.** The swirl and displacement diffusers are fixed area diffusers. The variable area diffusers maintain an approximately constant exit velocity. Linear bar grilles are normally used in exterior zonesand are fixed area diffusers. Custom is used to signify that the user intends to input the coefficients A – E (see below) rather than let the program set the coefficients based on diffuser type. The default is *Swirl*.
-
-#### Field: Transition Height
-
-An optional field to allow the user to specify the transition height (meters above floor) rather than have the program calculate it. The default is 1.7 meters.
-
-#### Field: Coefficient A
-
-The coefficient A in the formula: Kc = A\*Gamma\*\*B + C + D\*Gamma + E\*Gamma\*\*2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is *autocalculate*.
-
-#### Field: Coefficient B
-
-The coefficient B in the formula: Kc = A\*Gamma\*\*B + C + D\*Gamma + E\*Gamma\*\*2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is *autocalculate*.
-
-#### Field: Coefficient C
-
-The coefficient C in the formula: Kc = A\*Gamma\*\*B + C + D\*Gamma + E\*Gamma\*\*2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is *autocalculate*.
-
-#### Field: Coefficient D
-
-The coefficient D in the formula: Kc = A\*Gamma\*\*B + C + D\*Gamma + E\*Gamma\*\*2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is *autocalculate*.
-
-#### Field: Coefficient E
-
-The coefficient E in the formula: Kc = A\*Gamma\*\*B + C + D\*Gamma + E\*Gamma\*\*2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is *autocalculate*.
-
-An example input is:
-
-
-
-```idf
-  RoomAirModelType,
-    SPACE5-1 RoomAir Model,  !- Name
-    SPACE5-1,                !- Zone Name
-    UnderFloorAirDistributionInterior,  !- Room-Air Modeling Type
-    DIRECT;                  !- Air Temperature Coupling Strategy
-
-RoomAirSettings:UnderFloorAirDistributionInterior,
-    SPACE5-1,                !- Zone Name
-    Autocalculate,           !- Number of Diffusers
-    Autocalculate,           !- Power per Plume
-    Autocalculate,           !- Design Effective Area of Diffuser {m2}
-    Autocalculate,           !- Diffuser Slot Angle from Vertical {deg}
-    ,                        !- Thermostat Height {m}
-    ,                        !- Comfort Height {m}
-    0.001,         !- Temperature Difference Threshold for Reporting {deltaC}
-    Swirl,                   !- Diffuser Type
-    1.7,                     !- Transition Height {m}
-    Autocalculate,           !- Coefficient A
-    Autocalculate,           !- Coefficient B
-    Autocalculate,           !- Coefficient C
-    Autocalculate,           !- Coefficient D
-   Autocalculate;           !- Coefficient E
-```
-
-
-### RoomAirSettings:UnderFloorAirDistributionExterior
-
-This model is applicable to exterior spaces that are served by an underfloor air distribution system. The dominant sources of heat gain should be from people, equipment, and other localized sources located in the occupied part of the room, as well as convective gain coming from a warm window. The model predicts two temperatures in the room:
-
-- An occupied subzone temperature (T<sub>OC</sub>), representing the temperature in the region between the floor and the boundary of the upper subzone..
-
-- An upper subzone temperature (T<sub>MX</sub>) essential for overall energy budget calculations and for modeling comfort effects of the upper layer temperature.
-
-The following fields are used to define an instance of the ‘UCSD UFAD Exterior Model Controls’ object.
-
-#### Field: Zone Name
-
-This field provides the unique name of a zone described elsewhere in the file. A single instance of the ‘RoomAirSettings:UnderFloorAirDistributionExterior’ object is needed for each zone that is to be modeled using this method.
-
-#### Field: Number of Diffusers
-
-#### The total number of diffusers in this zone. This field can allowed to Autocalculate (in which case it is set to the design occupancy level; i.e., number of people). If the design occupancy is low or zero but there are still heat sources that could generate buoyancy driven plumes, the user should input a value based on the design supply air flow rate of the zone and the design flow rate of an individual diffuser. In the absence of any other information, divide the zone area by 100 ft<sup>2</sup>. The default for this field is Autocalculate.
-
-#### Field: Power per Plume
-
-#### The power in watts incorporated in a buoyancy driven thermal plume. Normally we assume all the loads of a workstation create a single plume so that this represents the convective heat gain from a workstation – 1 person, 1 computer terminal, plus any task lighting. A typical value would be 220 watts. However, the model assumes an “equivalent� plume derived from the zone extraction rate normalized to the number of workstations/occupants. This field should be allowed to default – the program will calculate a value based upon the occupancy and the extraction rate.  The default is Autocalculate.
-
-#### Field: Design Effective Area of Diffuser
-
-This is the design air flow opening area in square meters of a single diffuser. The default value depends on the diffuser type. For swirl diffusers it is 0075 m<sup>2</sup>, for variable area diffusers 0.035 m<sup>2</sup>, for horizontal swirl diffusers 0.006 m<sup>2</sup>, and for linear bar grilles 0.03 m<sup>2</sup>. The default is *Autocalculate*..
-
-#### Field: Diffuser Slot Angle from Vertical
-
-This input describes the angle at which air emerges from the diffusers. It should be the angle  in degrees between the vertical and the diffuser slots. The defaults depend on the diffuser type: for swirl diffusers it is 28 degrees, for variable area diffusers 45 degrees, for DV diffusers 73 degrees, and for linear bar grilles 15 degrees.
-
-#### Field: Thermostat Height
-
-This field is the height in meters of the thermostat/temperature control sensor above the floor. The default is 1.2 meters.
-
-#### Field: Comfort Height
-
-The height in meters above the floor at which air temperature is calculated for comfort purposes. The air temperature at this height is used in calculating the available measures of comfort: Fanger, Pierce or KSU. The default is 1.1 meters.
-
-#### Field: Temperature Difference Threshold for Reporting
-
-This field specifies a minimum temperature difference between the upper subzone and the occupied subzone that will be used to trigger whether or not the UFAD auxiliary outputs will be calculated. These outputs are *Room Air Zone Transition Height* and *Room Air Zone Average Temperature Gradient*. They are set to zero when the temperature difference is less than the threshold and the output *Room Air Zone Is Mixed Status* is set to 1.
-
-The value should be greater than or equal to zero and is in units of degrees Centigrade. The default value is 0.4 degrees C.
-
-The value should be greater than or equal to zero and is in units of degrees Centigrade. The default value is 0.4 degrees C.
-
-#### Field: Diffuser Type
-
-The choices for this alpha field are **Swirl** | **VariableArea** | **HorizontalSwirl | LinearBarGrille | Custom.** The swirl and displacement diffusers are fixed area diffusers. The variable area diffusers maintain an approximately constant exit velocity. Linear bar grilles are normally used in exterior zonesand are fixed area diffusers. Custom is used to signify that the user intends to input the coefficients A – E (see below) rather than let the program set the coefficients based on diffuser type. The default is *Swirl*.
-
-#### Field: Transition Height
-
-An optional field to allow the user to specify the transition height (meters above floor) rather than have the program calculate it. The default is 1.7 meters.
-
-#### Field: Coefficient A
-
-The coefficient A in the formula: Kc = A\*Gamma\*\*B + C + D\*Gamma + E\*Gamma\*\*2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is *autocalculate*.
-
-#### Field: Coefficient B
-
-The coefficient B in the formula: Kc = A\*Gamma\*\*B + C + D\*Gamma + E\*Gamma\*\*2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is *autocalculate*.
-
-#### Field: Coefficient C
-
-The coefficient C in the formula: Kc = A\*Gamma\*\*B + C + D\*Gamma + E\*Gamma\*\*2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is *autocalculate*.
-
-#### Field: Coefficient D
-
-The coefficient D in the formula: Kc = A\*Gamma\*\*B + C + D\*Gamma + E\*Gamma\*\*2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is *autocalculate*.
-
-#### Field: Coefficient E
-
-The coefficient E in the formula: Kc = A\*Gamma\*\*B + C + D\*Gamma + E\*Gamma\*\*2. Gamma is a variable that characterizes the amount of stratification in a UFAD zone. Kc is the fraction of the total internal convective heat gain that is assigned to the lower (occupied) subzone. The coefficients in the formula are defaulted based upon diffuser type. A user would normally allow this field to default. The default is *autocalculate*.
-
-An example input is:
-
-```idf
-  RoomAirSettings:UnderFloorAirDistributionExterior,
-    SPACE1-1,                !- Zone Name
-    Autocalculate,           !- Number of Diffusers per Zone
-    Autocalculate,           !- Power per Plume
-    Autocalculate,           !- Design Effective Area of Diffuser {m2}
-    Autocalculate,           !- Diffuser Slot Angle from Vertical {deg}
-    ,                        !- Thermostat Height {m}
-    ,                        !- Comfort Height {m}
-    0.001,                   !- Temperature Difference Threshold for Reporting {deltaC}
-    LinearBarGrille,         !- Diffuser Type
-    1.7,                     !- Transition Height {m}
-    Autocalculate,           !- Coefficient A
-    Autocalculate,           !- Coefficient B
-    Autocalculate,           !- Coefficient C
-    Autocalculate,           !- Coefficient D
-    Autocalculate;           !- Coefficient E
-```
-
-### RoomAirflowNetwork Model
-
-This model simulates a thermal zone using a network approach by assuming intra-zone nodes connected by user-defined patterns of airflows. The new model also allows users to specify a node to be connected to surfaces to have convective heat transfer between surfaces and the node, portion of internal gains and supply air and return air fractions from zone equipment. The model requires following objects to work together:
-
-    RoomAirSettings:AirflowNetwork
-    RoomAir:Node:AirflowNetwork
-    RoomAir:Node:AirflowNetwork:AdjacentSurfaceList
-    RoomAir:Node:AirflowNetwork:InternalGains
-    RoomAir:Node:AirflowNetwork:HVACEquipment
-    AirflowNetwork:Intrazone:Node
-    AirflowNetwork:Intrazone:Linkage
-
-The first *five* **objects** are described below. The last two objects are described in the Airflow Network Model section. 
-
-### RoomAirSettings:AirflowNetwork
-
-This object provides inputs in a thermal zone needed for the RoomAirflowNetwork model.  The inputs specify a thermal zone and a list of RoomAir nodes. The object gives a summary of the model configuration in a zone.
-
-#### Field: Name
-
-This is a unique character string associated with this instance of the RoomAirSettings:AirflowNetwork object.
- 
-#### Field: Zone Name
-
-The name of the EnergyPlus thermal zone corresponding to the RoomAir model zone.
-
-#### Field: Control Point RoomAir:Node Name
-
-This is the name of a RoomAir:Node:AirflowNetwork object that contains the sensor for zone HVAC controls.  The conditions at this node will be used for thermostatic, humidistatic, or comfort based control decisions. The zone node defined in a Zone object is required.  
-
-#### Field: RoomAir:Node:AirflowNetwork x Name
-
-The name of a RoomAir:Node:AirflowNetwork object defined elsewhere.  This node will receive the fraction of internal gains, and HVAC equipment, and a list of surface names exposed to this node with convective heat transfer. 
-
-An IDF example input is:
-
-```idf
-  RoomAirSettings:AirflowNetwork,
-    NORTH_ZONE,     !- Name 
-    NORTH_ZONE,              !- Zone Name
-    RoomAir Schedule,        !- Availability Schedule Name
-    NORTH_ZONE,              !- Control Point RoomAir:Node Name
-    LeftUpper,               !- RoomAir:Node:AirflowNetwork 1 Name
-    CentralUpper,            !- RoomAir:Node:AirflowNetwork 2 Name
-    NORTH_ZONE,              !- RoomAir:Node:AirflowNetwork 3 Name
-    LeftMiddle,              !- RoomAir:Node:AirflowNetwork 4 Name
-    LeftLower,               !- RoomAir:Node:AirflowNetwork 5 Name
-    CentralLower;            !- RoomAir:Node:AirflowNetwork 6 Name
-```
-
-### RoomAir:Node:AirflowNetwork
-
-This object is used to define a node in a thermal zone. The input specifies the fraction of zone volume and provides a list of names to define fraction of internal gains, surface connection and HVAC equipment.
-
-#### Field: Name
-
-This is a unique character string associated with this instance of the RoomAirSettings:AirflowNetwork object. 
-
-#### Field: Zone Name
-
-The name of the EnergyPlus thermal zone and is defined in an RoomAirSettings:AirflowNetwork object.
-
-#### Field: Fraction of Zone Air Volume
-
-The field specifies a fraction of the overall zone air volume that is assigned to this RoomAir:Node:AirflowNetwork object. The fraction will be used to calculate zone air storage term. See corresponding sections in Engineering Reference for its use in the node energy and moisture balance equations.
-
-#### Field: RoomAir:Node:AirflowNetwork:AdjacentSurfaceList Name
-
-The field specifies a name to provide a list of connected adjacent surfaces with convective heat transfer between surfaces and this particular node.  When a moisture mode is assigned to surfaces, convective moisture transfer will be calculated. See corresponding sections in Engineering Reference for its use in the node energy and moisture balance equations.
-
-#### Field: RoomAir:Node:AirflowNetwork:InternalGains Name
-
-The field specifies a name to provide a list of internal gain objects and associated fractions assigned to this particular node. See corresponding sections in Engineering Reference for its use in the node energy and moisture balance equations.
-
-#### Field: RoomAir:Node:AirflowNetwork:HVACEquipment Name
-
-The field specifies a name to provide a list of HVAC equipment, including AirLoop terminals and zone equipment. See corresponding sections in Engineering Reference for its use in the node energy and moisture balance equations.
-
-```idf
-  RoomAir:Node:AirflowNetwork,
-    LeftUpper,         !- Name
-    NORTH_ZONE,        !- Zone Name
-    0.15,              !- Fraction of Zone Air Volume
-    Surface_18_T_List, !- RoomAir:Node:AirflowNetwork:AdjacentSurfaceList Name
-    LeftUpper_Gain,    !- RoomAir:Node:AirflowNetwork:InternalGains Name
-    LeftUpper_HVAC;    !- RoomAir:Node:AirflowNetwork:HVACEquipment Name
-```
-
-### RoomAir:Node:AirflowNetwork:AdjacentSurfaceList
-
-This object is used to provide a list of connected adjacent surfaces with convective heat transfer between surfaces and this particular node. When a moisture mode is assigned to surfaces, convective moisture transfer will be calculated. It should be pointed out that a fraction of a surface exposed to this particular node is not allowed.
-
-#### Field: Name
-
-This is a unique character string associated with this instance of the RoomAir:Node:AirflowNetwork:AdjacentSurfaceList object. 
-
-#### Field: Surface x Name
-
-The field specifies a surface name based on the order from 1 to 21. The maximum number of surfaces can be extensible.
-
-```idf
-  RoomAir:Node:AirflowNetwork:AdjacentSurfaceList,
-    Surface_18_T_List, !- Name
-    Surface_18_T;      !- Surface 1 Name
-```
-### RoomAir:Node:AirflowNetwork:InternalGains
-
-This object is used to define a list of internal gains in the same zone and associated fraction assigned to this particular node. 
-
-#### Field: Name
-
-This is a unique character string associated with this instance of the RoomAir:Node:AirflowNetwork:InternalGains object. 
-
-#### Field: Internal Gain Object x Type
-
-The field specifies an internal gain object type based on the list in the Energy+. 
-
-#### Field: Internal Gain Object x Name
-
-The field specifies an internal gain object name based on the list in the Energy+.
- 
-#### Field: Fraction of Gains to Node x
-
-The field specifies a fraction of the particular internal gain object assigned to this node. 
-
-```idf
-  RoomAir:Node:AirflowNetwork:InternalGains,
-    CentralUpper_Gain,        !- Name
-    People,                !- Internal Gain Object 1 Type
-    NORTH_ZONE People,     !- Internal Gain Object 1 Name
-    0.15,                  !- Fraction of Gains to Node 1
-    Lights,                !- Internal Gain Object 2 Type
-    NORTH_ZONE Lights,     !- Internal Gain Object 2 Name
-    0.15,                  !- Fraction of Gains to Node 2
-    ElectricEquipment,     !- Internal Gain Object 3 Type
-    NORTH_ZONE Equip,     !- Internal Gain Object 3 Name
-    0.15;                  !- Fraction of Gains to Node 3
-```
-
-{Field set: 3 fields (Internal Gain Object x Type, Internal Gain Object x Name, and Fraction of Gains to Node x). are extensible.}
-
-### RoomAir:Node:AirflowNetwork:HVACEquipment
-
-This object is used to define a list of HVAC equipment objects in the same zone and associated fractions assigned to this particular node. 
-
-#### Field: Name
-
-This is a unique character string associated with this instance of the RoomAir:Node:AirflowNetwork:HVACEquipment object. 
-
-#### Field: ZoneHVAC or Air Terminal Equipment Object Type x
-
-The field specifies an object type of ZoneHVAC equipment or terminal type based on the list in the Energy+.idd.
-
-#### Field: ZoneHVAC or Air Terminal Equipment Object Name x
-
-The field specifies the object name based on the object type defined in the previous field.  
-
-#### Field: Fraction of Output or Supply Air from HVAC Equipment x 
-
-The field specifies a fraction of supply air from the particular equipment to this node. 
-
-#### Field: Fraction of Input or Return Air from HVAC Equipment x 
-
-The field specifies a fraction of return air from the particular equipment to this node. 
-
-```idf
-  RoomAir:Node:AirflowNetwork:HVACEquipment,
-    CentralUpper_HVAC,        !- Name
-    ZoneHVAC:PackagedTerminalAirConditioner, !- ZoneHVAC or Air Terminal Equipment Object Type 1
-    NORTH_ZONE PTAC,       !- ZoneHVAC or Air Terminal Equipment Object Name 1
-    0.14,                   !- Fraction of Output or Supply Air from HVAC Equipment 1 
-    0.14;                   !- Fraction of Input or Return Air to HVAC Equipment 1
-```
-
-{Field set: 4 fields (ZoneHVAC or Air Terminal Equipment Object Type x, ZoneHVAC or Air Terminal Equipment Object Name x, Fraction of Output or Supply Air from HVAC Equipment x, and Fraction of Input or Return Air from HVAC Equipment x) are extensible.}
-
-### Room Air Model Outputs
-
-Each room air model sets up outputs specific to that model. The effect of room air modeling is usually to adjust the adjacent air temperature along the inside surface of heat transfer surfaces. The output report “Surface Int Adjacent Air Temperature [C]� is provided for this and described under Surface Outputs.
-
-#### Zone Predicted Sensible Load Room Air Correction Factor
-
-This output variable provides the value of the correction factor applied to the predicted zone loads.  Predicted zone load to setpoint is (usually) used to control HVAC air systems and the presence of a room air model has an impact on the loads.  The predicited loads are multiplied by the factor in this output variable.  The value is always 1.0 when there is no Room Air model.  When there is a Room Air model, this output shows how that model is increasing or decreasing overall zone loads experienced by the air system.
-
-### RoomAir:TemperaturePattern:TwoGradient Outputs
-
-The user-defined air temperature pattern that interpolates between two gradients produces the following output variable.
-
-HVAC,Average,Room Air Zone Vertical Temperature Gradient [K/m]
-
-#### Room Air Zone Vertical Temperature Gradient [K/m]
-
-This output variable is the result of the interpolation performed by the user-defined roomair model using RoomAir:TemperaturePattern:TwoGradient.  This is the temperature gradient in the vertical direction.  The units are degrees Kelvin per meter.
-
-### Mundt Model / OneNodeDisplacementVentilation Outputs
-
-The following output is available for the Mundt model.
-
-Room Air Node Air Temperature [C]
-
-#### Room Air Node Air Temperature [C]
-
-This output variable provides the drybulb air temperature used in, or calculated by, the Mundt model. The selection key is the name of an air node defined in a ROOMAIR Node object.
-
-### ThreeNodeDisplacementVentilation Outputs
-
-* HVAC,Average,Room Air Zone Mixed Subzone Temperature [C]
-
-* HVAC,Average,Room Air Zone Occupied Subzone Temperature [C]
-
-* HVAC,Average,Room Air Zone Floor Subzone Temperature [C]
-
-* HVAC,Average,Room Air Zone Transition Height [m]
-
-* HVAC,Average,Room Air Zone Recommended Minimum Flow Fraction
-
-* HVAC,Average,Room Air Zone Is Mixed Status []
-
-* HVAC,Average,Room Air Zone Average Temperature Gradient [K/m]
-
-* HVAC,Average,Room Air Zone Maximum Temperature Gradient [K/m]
-
-* HVAC,Average,Room Air Zone Thermal Comfort Effective Air Temperature [C]
-
-* HVAC,Average,Room Air Zone Thermostat Temperature [C]
-
-
-#### Room Air Zone Mixed Subzone Temperature [C]
-
-The temperature of the upper well-mixed subzone in degrees C.
-
-#### Room Air Zone Occupied Subzone Temperature [C]
-
-The average temperature of the lower, stratified, occupied subzone in degrees C.
-
-#### Room Air Zone Floor Subzone Temperature [C]
-
-The temperature of the region near the floor in degrees C.
-
-#### Room Air Zone Transition Height  [m]
-
-The height above the floor, in meters, of the boundary between the lower occupied subzone and the upper well-mixed subzone.
-
-#### Room Air Zone Recommended Minimum Flow Fraction []
-
-The ratio of the minimum recommended flow rate to the actual flow rate. Here flow rate means the sum of infiltration, ventilation, mixing and system air flow rates. The minimum flow is the flow needed to establish the boundary between the occupied and mixed subzones at 1.5 meters.
-
-#### Room Air Zone Is Mixed Status []
-
-An integer flag that indicates whether the zone is mixed (single node well-mixed zone model used) or stratified (UCSD DV model used). The value 1 means well-mixed; 0 means stratified.
-
-#### Room Air Zone Average Temperature Gradient  [K/m]
-
-The temperature gradient between the middle of the floor region and the middle of the well-mixed upper subzone in degrees Kelvin per meter.
-
-#### Room Air Zone Maximum Temperature Gradient [K/m]
-
-The maximum of the temperature gradient between the middle of the floor region and the middle of the occupied subzone and the temperature gradient between the middle of the occupied subzone and the middle of the well-mixed subzone. The gradient is in degrees Kelvin per meter.
-
-#### Room Air Zone Thermal Comfort Effective Air Temperature [C]
-
-The temperature at the user specified comfort height in degrees C.
-
-#### Room Air Zone Thermostat Temperature [C]
-
-The temperature at the height of the thermostat (specified by user input) in degrees C.
-
-### CrossVentilation Model Outputs
-
-* Zone,Average,Room Air Zone Jet Region Temperature [C]
-
-* Zone,Average,Room Air Zone Recirculation Region Temperature [C]
-
-* Zone,Average,Room Air Zone Jet Region Average Air Velocity [m/s]
-
-* Zone,Average,Room Air Zone Recirculation Region Average Air Velocity [m/s]
-
-* Zone,Average,Room Air Zone Inflow Opening Area[m2]
-
-* Zone,Average,Room Air Zone Room Length [m]
-
-* Zone,Average,Room Air Zone Recirculation and Inflow Rate Ratio []
-
-* Zone,Average,Room Air Zone Is Mixing Status []
-
-* Zone,Average,Room Air Zone Is Recirculating Status []
-
-
-#### Room Air Zone Jet Region Temperature [C]
-
-Average air temperature in the jet region of the flow in degrees C.
-
-#### Room Air Zone Recirculation Region Temperature [C]
-
-Average air temperature in the recirculation region of the flow in degrees C.
-
-#### Room Air Zone Jet Region Average Air Velocity [m/s]
-
-Average airflow velocity in the jet region of the flow in meters per second.
-
-#### Room Air Zone Recirculation Region Average Air Velocity [m/s]
-
-Average airflow velocity in the recirculation region of the flow in meters per second.
-
-#### Room Air Zone Inflow Opening Area [m2]
-
-Area of the inflow aperture in square meters. This area can change due to variation in wind direction (as inflow aperture changes) or variations in the opening schedule.
-
-#### Room Air Zone Room Length [m]
-
-Length of the room along the cross ventilation direction, in meters.
-
-#### Room Air Zone Recirculation and Inflow Rate Ratio []
-
-Ratio between airflow rate in the recirculation region and inflow rate, non-dimensional.
-
-#### Room Air Zone Is Mixing Status []
-
-An integer flag that indicates whether the zone is mixed (single node well-mixed zone model used) or significant momentum conservation is occurring (UCSD CV model used). The value 1 means well-mixed; 0 means cross ventilation is present. Transition to mixed flow can occur due to three mechanism: reduction in inflow velocity, reduction in inflow aperture area and dominance of buoyancy effects. A value of 1 is yes, a value of 0 is no.
-
-
-
-#### Room Air Zone Is Recirculating Status []
-
-An integer flag that indicates whether recirculations are present in the flow. A cross ventilation flow does not have recirculations whenever the inflow area is similar to the room cross section area (such as airflow in a typical corridor). A value of 1 is yes, a value of 0 is no.
-
-### UnderFloorAirDistributionInterior/Exterior Model Outputs
-
-* HVAC,Average,Room Air Zone Mixed Subzone Temperature [C]
-
-* HVAC,Average,Room Air Zone Occupied Subzone Temperature [C]
-
-* HVAC,Average,Room Air Zone Transition Height [m]
-
-* HVAC,Average,Room Air Zone Is Mixed Status []
-
-* HVAC,Average,Room Air Zone Average Temperature Gradient [K/m]
-
-* HVAC,Average,Room Air Zone Effective Comfort Air Temperature [C]
-
-* HVAC,Average,Room Air Zone Thermostat Temperature [C]
-
-* HVAC,Average,Room Air Zone Transition Height Gamma Value [ ]
-
-* HVAC,Average,Room Air Zone Plume Heat Transfer Rate [W]
-
-* HVAC,Average,Room Air Zone Temperature Stratification Fraction []
-
-* HVAC,Average,Room Air Zone Window Plume Heat Transfer Rate [W]
-
-
-#### Room Air Zone Mixed Subzone Temperature [C]
-
-The temperature of the upper subzone in degrees C.
-
-#### Room Air Zone Occupied Subzone Temperature [C]
-
-The temperature of the lower, occupied subzone in degrees C.
-
-#### Room Air Zone Transition Height [m]
-
-The height above the floor, in meters, of the boundary between the lower occupied subzone and the upper subzone..
-
-#### Room Air Zone Is Mixed Status []
-
-An integer flag that indicates whether the zone is mixed (single node well-mixed zone model used) or stratified (UCSD UFI model used). The value 1 means well-mixed; 0 means stratified.
-
-#### Room Air Zone Average Temperature Gradient [K/m]
-
-The temperature gradient between the middle of the occupied subzone and the middle of the upper subzone in degrees Kelvin per meter.
-
-#### Room Air Zone Effective Comfort Air Temperature [C]
-
-The temperature at the user specified comfort height in degrees C.
-
-#### Room Air Zone Thermostat Temperature [C]
-
-The temperature at the height of the thermostat (specified by user input) in degrees C.
-
-#### Room Air Zone Transition Height Gamma Value []
-
-Value of gamma – a dimensionless “height� used in calculating the transition height. Lower values of gamma indicate increased stratification, higher values less. Generally the values should be between 2 and 30.
-
-#### Room Air Zone Plume Heat Transfer Rate [W]
-
-The heat in watts driving the plumes in the occupied subzone.
-
-#### Room Air Zone Window Plume Heat Transfer Rate [W]
-
-The convective heat gain from windows in an UnderFloorAirDistributionExterior zone.
-
-#### Room Air Zone Temperature Stratification Fraction []
-
-This output, (Phi) is a measure of temperature stratification in the space. It is the difference between the occupied subzone temperature and the supply temperature divided by difference between the return temperature and the supply temperature. Technically it is equal to Kc. As phi approaches 1, the space is fully mixed. As phi approaches 0, the space becomes fully stratified. Expressed as an equation:
-
-*(T<sub>occ</sub>* – *T<sub>sup</sub>) / (T<sub>ret</sub>* *- T<sub>sup</sub>)*
-
-### RoomAirflowNetwork Model Outputs
-
-* HVAC,Average,RoomAirflowNetwork Node Temperature [C]
-
-* HVAC,Average,RoomAirflowNetwork Node Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC,Average,RoomAirflowNetwork Node Relative Humidity [%]
-
-* HVAC,Average,RoomAirflowNetwork Node SumIntSensibleGain [W]
-
-* HVAC,Average,RoomAirflowNetwork Node SumIntLatentGain [W]
-
-* HVAC,Average,RoomAirflowNetwork Node NonAirSystemResponse [W]
-
-* HVAC,Average,RoomAirflowNetwork Node SysDepZoneLoadsLagged [W]
-
-* HVAC,Average,RoomAirflowNetwork Node HVAC Supply Fraction []
-
-* HVAC,Average,RoomAirflowNetwork Node HVAC Return Fraction []
-
-#### RoomAirflowNetwork Node Temperature [C]
-
-The temperature at a Room Air Node in a zone in degrees C.
-
-#### HVAC,Average,RoomAirflowNetwork Node Humidity Ratio [kgWater/kgDryAir]
-
-The humidity ratio at a Room Air Node in a zone in kgWater/kgDryAir.
-
-#### RoomAirflowNetwork Node Relative Humidity [%]
-
-The relative humidity ratio at a Room Air Node in a zone in percent.
-
-#### HVAC,Average,RoomAirflowNetwork Node SumIntSensibleGain [W]
-
-A sum of internal sensible gains assigned to a Room Air node in a zone.
-
-#### HVAC,Average,RoomAirflowNetwork Node SumIntLatentGain [W]
-
-A sum of internal latent gains assigned to a Room Air node in a zone.
-
-#### HVAC,Average,RoomAirflowNetwork Node NonAirSystemResponse [W]
-
-A sum of system convective gains, collected via NonAirSystemResponse, and assigned to a Room Air node in a zone. 
-
-#### HVAC,Average,RoomAirflowNetwork Node SysDepZoneLoadsLagged [W]
-
-A sum of SysDepZoneLoads saved to be added to zone heat balance at the next HVAC time step. A typical system is a zone dehumidifier.
-
-Group – Internal Gains (People, Lights, Other internal zone equipment)
-----------------------------------------------------------------------
-
-Not all the influence for energy consumption in the building is due to envelope and ambient conditions. This group of objects describes other internal gains that may come into play (People, Lights, Various Equipment Types).
-
-### People
-
-The people statement is used to model the occupant’s effect on the space conditions. The following definition addresses the basic affects as well as providing information that can be used to report the thermal comfort of a group of occupants. The Fanger, Pierce Two-Node, and Kansas State University Two-Node thermal comfort models are available in EnergyPlus. A user may select any of these models for each People statement by simply adding the appropriate choice keyword after the air velocity schedule name. Thermal comfort calculations will only be made for people statements that include specific requests for these thermal comfort models. . This object also requires input of carbon dioxide generation rate based on people activity level for zone carbon dioxide simulations.
-
-#### Field: Name
-
-The name of the People object. Must be unique across all People objects.
-
-#### Field: Zone or ZoneList Name
-
-This field is the name of the zone (ref: Zone) or ZoneList (ref: ZoneList) and links a particular people statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this people definition is applied to each of the zones in the zone list effecting a global definition for the number of people in the zone. The Zonelist option can be used effectively with the people/area and area/person options of the Number of People Calculation Method.
-
-The name of the actual people object becomes &lt;Zone Name&gt; &lt;People Object Name&gt; and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
-
-#### Field: Number of People Schedule Name
-
-This field is the name of the schedule (ref: Schedules) that modifies the number of people parameter (see Number of People Calculation Method and related fields). The schedule values can be any positive number. The actual number of people in a zone as defined by this statement is the product of the number of people field and the value of the schedule specified by name in this field.
-
-#### Field: Number of People Calculation Method
-
-This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal number of occupants (people) in the Zone. The key/choices are:
-
-- People
-
-With this choice, the method used will be a straight insertion of the number of occupants (people).  (The Number of People field should be filled.)
-
-- People/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The People per Zone Floor Area field should be filled).
-
-- Area/Person
-
-With this choice, the method used will be a factor of floor area per person. (The Zone Floor Area per Person field should be filled).
-
-#### Field: Number of People
-
-This field is used to represent the maximum number of people in a zone that is then multiplied by a schedule fraction (see schedule field). In EnergyPlus, this is slightly more flexible in that the number of people could be a “diversity factor� applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour, the number of people field is constant for all simulation environments.
-
-#### Field: People per Zone Floor Area
-
-This factor (person/m<sup>2</sup>) is used, along with the Zone Floor Area to determine the maximum number of people as described in the Number of People field. The choice from the method field should be “people/area�.
-
-#### Field: Zone Floor Area per Person
-
-This factor (m<sup>2</sup>/person) is used, along with the Zone Floor Area to determine the maximum number of people as described in the Number of People field. The choice from the method field should be “area/person�.
-
-#### Field: Fraction Radiant
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the type of heat being given off by people in a zone. The number specified in this field will be multiplied by the total sensible energy emitted by people to give the amount of long wavelength radiation gain from human beings in a zone. The remainder of the sensible load is assumed to be convective heat gain. Note that latent gains from people are not included in either the radiant or convective heat gains. See the Engineering Reference document for more details.
-
-#### Field: Sensible Heat Fraction
-
-The user can use this field to specify a fixed sensible fraction for the heat gain due to this PEOPLE object. Normally the program calculates the sensible/latent split; this field gives the user control over this split. This field is autocalculated: if the field is blank or **autocalculate**, the program will calculate the sensible/latent split; if a value is entered, it will be used as the sensible fraction of the current total heat gain.
-
-#### Field: Activity Level Schedule Name
-
-This field is the name of the schedule that determines the amount of heat gain per person in the zone under design conditions. This value is modified somewhat based on a correlation to account for variations in space temperature. The schedule values may be any positive number and the units for this parameter is Watts per person. This schedule represents the total heat gain per person including convective, radiant, and latent. An internal algorithm is used to determine what fraction of the total is sensible and what fraction is latent. Then, the sensible portion is divided into radiant and convective portions using the value specified for Fraction Radiant (above). See the Engineering Reference document for more details.
-
-Values for activity level can range anywhere from approximately 100-150 Watts per person for most office activities up to over 900 Watts per person for strenuous physical activities such as competitive wrestling. The following table (Table 11) is based on Table 4 from the 2005 ASHRAE Handbook of Fundamentals, page 8.6. In addition to the information from the ASHRAE HOF, there is an added column of values in W/Person such as necessary for the activity level schedule values. This column uses the standard adult body surface area of 1.8 m<sup>2</sup> to multiply the activity levels in W/m<sup>2</sup> that are used in the table. Warnings are produced when the activity level schedule values fall outside normal ranges. Having too low or too high values can also skew thermal comfort reporting values.
-
-#### Field: Carbon Dioxide Generation Rate
-
-This numeric input field specifies carbon dioxide generation rate per person with units of m3/s-W. The total carbon dioxide generation rate from this object is:
-
-Number of People \* People Schedule \* People Activity \* Carbon Dioxide Generation Rate. The default value is 3.82E-8 m3/s-W (obtained from ASHRAE Standard 62.1-2007 value at 0.0084 cfm/met/person over the general adult population). The maximum value can be 10 times the default value.
-
-#### Field: Enable ASHRAE 55 comfort warnings
-
-This field accepts either “Yes� or “No� as values. When “Yes� is specified, warnings are generated when the space conditions are outside of the ASHRAE 55 comfort range as discussed in the sections that follow titled “Simplified ASHRAE 55-2004 Graph Related Outputs� and “Simplified ASHRAE 55 Warnings.� The default is not to provide these warnings so if you want to know if your space is outside this comfort range you must set this field to Yes.
-
-Table 11. Metabolic Rates for Various Activities
-
-<table class="table table-striped">
-  <tr>
-    <th>Activity</th>
-    <th>Activity Level w/Person EnergyPlus Schedule Value</th>
-    <th>Activity Level W/m2</th>
-    <th>met*</th>
-  </tr>
-  <tr>
-    <td colspan="4">Resting</td>
-  </tr>
-  <tr>
-    <td>Sleeping</td>
-    <td>72</td>
-    <td>40</td>
-    <td>0.7</td>
-  </tr>
-  <tr>
-    <td>Reclining</td>
-    <td>81</td>
-    <td>45</td>
-    <td>0.8</td>
-  </tr>
-  <tr>
-    <td>Seated, quiet</td>
-    <td>108</td>
-    <td>60</td>
-    <td>1</td>
-  </tr>
-  <tr>
-    <td>Standing, relaxed</td>
-    <td>126</td>
-    <td>70</td>
-    <td>1.2</td>
-  </tr>
-  <tr>
-    <td colspan="4">Walking (on level surface)</td>
-  </tr>
-  <tr>
-    <td>3.2 km/h (0.9 m/s)</td>
-    <td>207</td>
-    <td>115</td>
-    <td>2</td>
-  </tr>
-  <tr>
-    <td>4.3 km/h (1.2 m/s)</td>
-    <td>270</td>
-    <td>150</td>
-    <td>2.6</td>
-  </tr>
-  <tr>
-    <td>6.4 km/h (1.8 m/s)</td>
-    <td>396</td>
-    <td>220</td>
-    <td>3.8</td>
-  </tr>
-  <tr>
-    <td colspan="4">Office Activities</td>
-  </tr>
-  <tr>
-    <td>Reading, seated</td>
-    <td>99</td>
-    <td>55</td>
-    <td>1</td>
-  </tr>
-  <tr>
-    <td>Writing</td>
-    <td>108</td>
-    <td>60</td>
-    <td>1</td>
-  </tr>
-  <tr>
-    <td>Typing</td>
-    <td>117</td>
-    <td>65</td>
-    <td>1.1</td>
-  </tr>
-  <tr>
-    <td>Filing, seated</td>
-    <td>126</td>
-    <td>70</td>
-    <td>1.2</td>
-  </tr>
-  <tr>
-    <td>Filing, standing</td>
-    <td>144</td>
-    <td>80</td>
-    <td>1.4</td>
-  </tr>
-  <tr>
-    <td>Walking about</td>
-    <td>180</td>
-    <td>100</td>
-    <td>1.7</td>
-  </tr>
-  <tr>
-    <td>Lifting/packing</td>
-    <td>216</td>
-    <td>120</td>
-    <td>2.1</td>
-  </tr>
-  <tr>
-    <td colspan="4">Miscellaneous Occupational Activities</td>
-  </tr>
-  <tr>
-    <td>Cooking</td>
-    <td>171 to 207</td>
-    <td>95 to 115</td>
-    <td>1.6 to 2.0</td>
-  </tr>
-  <tr>
-    <td>Housecleaning</td>
-    <td>207 to 360</td>
-    <td>115 to 200</td>
-    <td>2.0 to 3.4</td>
-  </tr>
-  <tr>
-    <td>Seated, heavy limb movement</td>
-    <td>234</td>
-    <td>130</td>
-    <td>2.2</td>
-  </tr>
-  <tr>
-    <td>Machine work</td>
-    <td>189</td>
-    <td>105</td>
-    <td>1.8</td>
-  </tr>
-  <tr>
-    <td>sawing (table saw)</td>
-    <td>207 to 252</td>
-    <td>115 to 140</td>
-    <td>2.0 to 2.4</td>
-  </tr>
-  <tr>
-    <td>light (electrical industry)</td>
-    <td>423</td>
-    <td>235</td>
-    <td>4</td>
-  </tr>
-  <tr>
-    <td>Handling 50 kg bags</td>
-    <td>423</td>
-    <td>235</td>
-    <td>4</td>
-  </tr>
-  <tr>
-    <td>Pick and shovel work</td>
-    <td>423 to 504</td>
-    <td>235 to 280</td>
-    <td>4.0 to 4.8</td>
-  </tr>
-  <tr>
-    <td colspan="4">Miscellaneous Leisure Activities</td>
-  </tr>
-  <tr>
-    <td>Dancing, social</td>
-    <td>252 to 459</td>
-    <td>140 to 255</td>
-    <td>2.4 to 4.4</td>
-  </tr>
-  <tr>
-    <td>Calisthenics/exercise</td>
-    <td>315 to 423</td>
-    <td>175 to 235</td>
-    <td>3.0 to 4.0</td>
-  </tr>
-  <tr>
-    <td>Tennis, singles</td>
-    <td>378 to 486</td>
-    <td>210 to 270</td>
-    <td>3.6 to 4.0</td>
-  </tr>
-  <tr>
-    <td>Basketball, competitive</td>
-    <td>522 to 792</td>
-    <td>290 to 440</td>
-    <td>5.0 to 7.6</td>
-  </tr>
-  <tr>
-    <td>Wrestling, competitive</td>
-    <td>738 to 909</td>
-    <td>410 to 505</td>
-    <td>7.0 to 8.7</td>
-  </tr>
-</table>
-
-**\*Note that one met = 58.1 W/m<sup>2</sup>**
-
-#### Field: Mean Radiant Temperature Calculation Type
-
-This field specifies the type of Mean Radiant Temperature (MRT) calculation the user wishes to use for the thermal comfort model. At the present time, there are two options for MRT calculation type: zone averaged and surface weighted. The default calculation is “ZoneAveraged�. In the zone averaged MRT calculation, the MRT used for the thermal comfort calculations is for an “average� point in the zone. MRT is calculated based on an area-emissivity weighted average of all of the surfaces in the zone. In cases where the emissivity of all of the surfaces are sufficiently small (near zero), the mean radiant temperature will be set to the mean air temperature of the space to avoid divide by zero errors. The other MRT calculation type is “SurfaceWeighted�. The goal of this calculation type is to estimate a person in the space close to a particular surface without having to define exact view factors for all of the surfaces and the location of the person in the space. The MRT used in the thermal comfort calculations when the “surface weighted� calculation type is selected is actually the average of the temperature of the surface to which the person is closest (defined by the next field “Surface Name�) and the zone averaged MRT (defined above). The surface temperature alone is not used because in theory the maximum view factor from a person to any flat surface is roughly 0.5. In the “surfaceweighted� calculation, the surface in question actually gets slightly more weighting than 50% since the surface selected is still a part of the zone average MRT calculation. Again, this simplification was made to avoid the specification of view factors and the exact location of the person.
-
-A third option is to use “anglefactor�. This option allows for more explicit positioning of the person within the space by defining the angle factors from the person to the various surfaces in the zone. This option requires the user to list the surfaces that the person can see from a radiation standpoint and also define the angle (or view) factor for each surface. The AngleFactorList object (see next object description) is intended to give the user this opportunity.
-
-#### Field: Surface Name/Angle Factor List Name
-
-This field is only valid when the user selects “surfaceweighted� for the MRT calculation type (see the previous input field description). In this case, the field is the name of a surface within the zone the people are residing. This surface will be used in the MRT calculation as defined above to come up with a more representative MRT for a person near a particular surface. The MRT used for thermal comfort calculations using the “surface weighted� MRT calculation method is the average of the temperature of the surface specified in this field and the “zone averaged� MRT (see the Mean Radiant Temperature calculation type field above).
-
-#### Field: Work Efficiency Schedule Name
-
-This field is the name of the schedule that determines the efficiency of energy usage within the human body that will be used for thermal comfort calculations. Note that all energy produced by the body is assumed to be converted to heat for the zone heat balance calculation. A value of zero correspondsto all of the energy produced in the body being converted to heat. A value of unity corresponds to all of the energy produced in the body being converted to mechanical energy. The values for this parameter defined in the schedule must be between 0.0 and 1.0. Any value greater than zero will result in a reduction of heat that impacts thethermal comfort energy balance of a person within the space, resulting in PMV results appearing lower than expected.  Ensure that if this value is non-zero, the base activity level is chosen to ensure that the net activity converted to heat and zone conditions are sufficient to maintain thermal comfort..
-
-#### Field: Clothing Insulation Calculation Method
-
-This field is a key/choice field that tells which of the next two fields are filled and is descriptive of the method for calculating the clothing insulation value of occupants (people) in the Zone. The key/choices are:
-
-- ClothingInsulationSchedule
-
-With this choice, the method used will be a straight insertion of the scheduled clothing insulation values of occupants (people).  (The Clothing Insulation Schedule Name field should be filled.)
-
-- DynamicClothingModelASHRAE55
-
-With this choice, the method used will be the dynamic predictive clothing insulation model developed by Schiavon and Lee (2013) based on 6,333 selected observations taken from ASHRAE RP-884 and RP-921 databases. It varies the clothing insulation as a function of outdoor air temperature measured at 6am as illustrated below.
-
-- CalculationMethodSchedule
-
-With this choice, the method used can be either the ClothingInsulationSchedule or the DynamicClothingModelASHRAE55, depending on a schedule (to be entered as the next field) that determines which method to use in different time of a day. When this option is chosen, the next field “Clothing Insulation Calculation Method Schedule Name� is a required input.
-
-![](media/image083.png)
-
-Figure 48. Graphical representation fo the dynamic predictive clothing insulation model
-
-#### Field: Clothing Insulation Calculation Method Schedule Name
-
-This field specifies which clothing insulation method (ClothingInsulationSchedule or DynamicClothingModelASHRAE55) to use at a particular time of the day. A schedule value of 1 means the ClothingInsulationSchedule method, and 2 means the DynamicClothingModelASHRAE55 method. This field is only required when the “Clothing Insulation Calculation Method� field is set to **CalculationMethodSchedule**. If this field is left blank, the specified clothing insulation calculation method will be used and not changed during the simulation.
-
-#### Field: Clothing Insulation Schedule Name
-
-This field is the name of the schedule that defines the amount of clothing being worn by a typical zone occupant during various times in the simulation period. The choice from the Clothing Insulation Calculation Method field should be “**ClothingInsulationSchedule**�. This parameter must be a positive real number and has units of Clo. Typical values for Clo can be seen in the ASHRAE 2009 HOF Table 7, page 9.8 (for clothing ensembles) and Table 8, page 9.9 (for garment values) ) or www.cbe.berkeley.edu/comforttool/.
-
-#### Field: Air Velocity Schedule Name
-
-This field is the name of the schedule that approximates the amount of air movement in the space as a function of time throughout the simulation period. The user has control over this parameter through the schedule that requires the individual numbers in the schedule to be positive real numbers having units of meters per second.
-
-#### Field: Thermal Comfort Model Type (up to 5 allowed)
-
-The final one to five fields are optional and are intended to trigger various thermal comfort models within EnergyPlus. By entering the keywords Fanger, Pierce, KSU, AdaptiveASH55,, and AdaptiveCEN15251, the user can request the Fanger, Pierce Two-Node, Kansas State UniversityTwo-Node, and the adaptive comfort models of the ASHRAE Standard 55 and CEN Standard 15251 results for this particular people statement. AdaptiveASH55 is only applicable when the running average outdoor air temperature for the past 7 days is between 10.0 and 33.5C.  AdaptiveCEN15251 is only applicable when the running average outdoor air temperature for the past 30 days is between 10.0 and 30.0C. Note that since up to five models may be specified, the user may opt to have EnergyPlus calculate the thermal comfort for people identified with this people statement using all five models if desired. Note that the KSU model is computationally intensive and may noticeably increase the execution time of the simulation. For descriptions of the thermal comfort calculations, see the Engineering Reference document.
-
-The following IDF example allows for a maximum of 31 people with scheduled occupancy of “Office Occupancy�, 60% radiant using an Activity Schedule of “Activity Sch�. The example allows for thermal comfort reporting.
-
-```idf
-People,
-  Kitchen_ZN_1_FLR_1,  !- Name
-  Kitchen_ZN_1_FLR_1,  !- Zone or ZoneList Name
-  BLDG_OCC_SCH,  !- Number of People Schedule Name
-  People,  !- Number of People Calculation Method
-  25.2000,,,  !- Number of People, People per Zone Floor Area, Zone Floor Area per Person
-  0.3000,  !- Fraction Radiant
-  AUTOCALCULATE,  !- Sensible Heat Fraction
-  ACTIVITY_SCH,  !- Activity Level Schedule Name
-  3.82E-8        !- Carbon Dioxide Generation Rate {m3/s-W}
-  No,  !- Enable ASHRAE 55 Comfort Warnings
-  ZoneAveraged,  !- Mean Radiant Temperature Calculation Type
-  ,  !- Surface Name/Angle Factor List Name
-  WORK_EFF_SCH,  !- Work Efficiency Schedule Name
-  CLOTHING_SCH,  !- Clothing Insulation Schedule Name
-  AIR_VELO_SCH,  !- Air Velocity Schedule Name
-  Fanger;  !- Thermal Comfort Model 1 Type
-```
-
-
-A simpler example, without using the thermal comfort reporting option:
-
-```idf
-People,
-    RIGHT FORK,              !- Name
-    RIGHT FORK,              !- Zone or ZoneListName
-    Dorm Occupancy,          !- Number of People Schedule Name
-    people,                  !- Number of People Calculation Method
-    8.00000,                 !- Number of People,
-   ,                         !- People per Zone Floor Area
-   ,                         !- Zone Floor Area per Person
-    0.6000000,               !- Fraction Radiant
-    Autocalculate,           !- Sensible Heat Fraction
-    Activity Sch,            !- Activity level Schedule Name
-```
-
-
-And with the sensible fraction specified:
-
-```idf
-People,
-    SPACE1-1 People 1,       !- Name
-    SPACE1-1,                !- Zone or ZoneListName
-    OCCUPY-1,                !- Number of People Schedule Name
-    people,                  !- Number of People Calculation Method
-    11,                      !- Number of People
-    ,                        !- People per Zone Floor Area
-    ,                        !- Zone Floor Area per Person
-    0.3,                     !- Fraction Radiant
-    0.55,                    !- Sensible Heat Fraction
-    ActSchd;                 !- Activity level Schedule Name
-```
-
-
-Global People Object:
-
-```idf
-  ZoneList,AllOccupiedZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
-
-
-  People,
-    AllZones with People,       !- Name
-    AllOccupiedZones,        !- Zone or ZoneList Name
-    OCCUPY-1,                !- Number of People Schedule Name
-    People/Area,             !- Number of People Calculation Method
-    ,                        !- Number of People
-    .11,                     !- People per Zone Floor Area {person/m2}
-    ,                        !- Zone Floor Area per Person {m2/person}
-    0.3,                     !- Fraction Radiant
-    ,                        !- Sensible Heat Fraction
-    ActSchd;                 !- Activity Level Schedule Name
-```
-
-
-### People Outputs
-
-People objects have output variables for individual objects and for zone totals.
-
-People specific outputs include:
-
-* Zone,Average,People Occupant Count []
-
-* Zone,Sum,People Radiant Heating Energy [J]
-
-* Zone,Average,People Radiant Heating Rate [W]
-
-* Zone,Sum,People Convective Heating Energy [J]
-
-* Zone,Average,People Convective Heating Rate [W]
-
-* Zone,Sum,People Sensible Heating Energy [J]
-
-* Zone,Average,People Sensible Heating Rate [W]
-
-* Zone,Sum,People Latent Gain Energy [J]
-
-* Zone,Average,People Latent Gain Rate [W]
-
-* Zone,Sum,People Total Heating Energy [J]
-
-* Zone,Average,People Total Heating Rate [W]
-
-* Zone,Average,Zone People Occupant Count []
-
-* Zone,Sum,Zone People Radiant Heating Energy [J]
-
-* Zone,Average,Zone People Radiant Heating Rate [W]
-
-* Zone,Sum,Zone People Convective Heating Energy [J]
-
-* Zone,Average,Zone People Convective Heating Rate [W]
-
-* Zone,Sum,Zone People Sensible Heating Energy [J]
-
-* Zone,Average,Zone People Sensible Heating Rate [W]
-
-* Zone,Sum,Zone People Latent Gain Energy [J]
-
-* Zone,Average,Zone People Latent Gain Rate [W]
-
-* Zone,Sum,Zone People Total Heating Energy [J]
-
-* Zone,Average,People Air Temperature [C]
-
-* Zone,Average,People Air Relative Humidity [%]
-
-* Zone,Average,Zone People Total Heating Rate [W]
-
-* Zone,Average,Zone Thermal Comfort Mean Radiant Temperature [C]
-
-* Zone,Average,Zone Thermal Comfort Operative Temperature [C]
-
-* Zone,Average,Zone Thermal Comfort Fanger Model PMV []
-
-* Zone,Average,Zone Thermal Comfort Fanger Model PPD [%]
-
-* Zone,Average,Zone Thermal Comfort Clothing Surface Temperature [C]
-
-* Zone,Average,Zone Thermal Comfort Pierce Model Effective Temperature PMV []
-
-* Zone,Average,Zone Thermal Comfort Pierce Model Standard Effective Temperature PMV []
-
-* Zone,Average,Zone Thermal Comfort Pierce Model Discomfort Index []
-
-* Zone,Average,Zone Thermal Comfort Pierce Model Thermal Sensation Index []
-
-* Zone,Average,Zone Thermal Comfort KSU Model Thermal Sensation Index []
-
-* Zone,Average,Zone Thermal Comfort ASHRAE 55 Adaptive Model 80% Acceptability Status []
-
-* Zone,Average,Zone Thermal Comfort ASHRAE 55 Adaptive Model 90% Acceptability Status []
-
-* Zone,Average,Zone Thermal Comfort ASHRAE 55 Adaptive Model Running Average Outdoor Air Temperature [C]
-
-* Zone,Average,Zone Thermal Comfort ASHRAE 55 Adaptive Model Temperature [C]
-
-* Zone,Average,Zone Thermal Comfort CEN 15251 Adaptive Model Category I Status []
-
-* Zone,Average,Zone Thermal Comfort CEN 15251 Adaptive Model Category II Status []
-
-* Zone,Average,Zone Thermal Comfort CEN 15251 Adaptive Model Category III Status
-
-* Zone,Average,Zone Thermal Comfort CEN 15251 Adaptive Model Running Average Outdoor Air Temperature [C]
-
-* Zone,Average,Zone Thermal Comfort CEN 15251 Adaptive Model Temperature [C]
-
-
-#### People Occupant Count []
-
-This field is the number of people for this PEOPLE object during the timestep in question.
-
-#### People Radiant Heating Rate [W]
-
-#### People Radiant Heating Energy [J]
-
-These output variables are the amount of radiant heat gain for this People object in Watts (for rate) or Joules. This is determined by the current sensible heat gain from people to the zone and the “Fraction Radiant� specified in the input. The radiant gains from people are distributed to the surfaces using an area weighting scheme.
-
-#### People Convective Heating Rate [W]
-
-#### People Convective Heating Energy [J]
-
-These output variables are the amount of convective heat gain for this People object in Watts (for rate) or Joules. This is determined by the current sensible heat gain from people to the zone and the “Fraction Radiant� specified in input. Note that the radiant and convective gains should add up to the sensible heat gain from people. The convective heat gain from people is added to the zone air heat balance directly.
-
-#### People Latent Gain Rate [W]
-
-#### People Latent Gain Energy [J]
-
-These output variables are the amount of latent heat gain for this People object in Watts (for rate) or Joules. This amount is based on the number of people in the space as well as the total amount of energy produced by a typical person defined by the activity schedule in the input. An internal algorithm is used to determine what fraction of the total is sensible and what fraction is latent. Details about this split are included in the Engineering Reference document.
-
-#### People Sensible Heating Rate [W]
-
-#### People Sensible Heating Energy [J]
-
-These output variables are the amount of sensible heat gain for this People object in Watts (for rate) or Joules. This amount is based on the number of people in the space as well as the total amount of energy produced by a typical person defined by the activity schedule in the input. An internal algorithm (described in the Engineering Reference document) is used to determine what fraction of the total is sensible and what fraction is latent. The sensible plus the latent heat gain from people equals the total gain specified in the input.
-
-#### People Total Heating Rate [W]
-
-#### People Total Heating Energy [J]
-
-These output variables are the total amount of heat gain for this People object in Watts (for rate) or Joules. This is derived from the activity level times the number of occupants.
-
-#### People Air Temperature [C]
-
-This output variable represents the zone air temperature based on the Fanger thermal comfort model.  If there is a ZoneControl:Thermostat:ThermalComfort object specified and the thermal zone is occupied, then the value of “People Air Temperature� is determined based on the thermal comfort hat satisfies the thermal comfort setpoint PMV value specified; othwesie, it is set to average zone air temperature.
-
-#### People Air Relative Humidity [%]
-
-This output variable represents the zone air relative humidity based on the Fanger thermal comfort model.  If there is a ZoneControl:Thermostat:ThermalComfort object specified and the thermal zone is occupied, then the value of “People Air Relative Humidity� is determined from the mean zone air temperature and zone air humidity ratio that satisfies the thermal comfort setpoint PMV value specified; othwesie, it is calculated from the zone air temperature and humidity ratio averaged over the time step.
-
-#### Zone People Occupant Count []
-
-This field is the total number of people within the zone during the timestep in question.
-
-#### Zone People Radiant Heating Rate [W]
-
-#### Zone People Radiant Heating Energy [J]
-
-These output variables are the amount of radiant heat gain from people within the zone in Watts (for rate) or Joules. This is determined by the current sensible heat gain from people to the zone and the “Fraction Radiant� specified in the input. The radiant gains from people are distributed to the surfaces using an area weighting scheme.
-
-#### Zone People Convective Heating Rate [W]
-
-#### Zone People Convective Heating Energy [J]
-
-These output variables are the amount of convective heat gain from people within the zone in Watts (for rate) or Joules. This is determined by the current sensible heat gain from people to the zone and the “Fraction Radiant� specified in input. Note that the radiant and convective gains should add up to the sensible heat gain from people. The convective heat gain from people is added to the zone air heat balance directly.
-
-#### Zone People Latent Gain Rate [W]
-
-#### Zone People Latent Gain Energy [J]
-
-These output variables are the amount of latent heat gain from people within the zone in Watts (for rate) or Joules. This amount is based on the number of people in the space as well as the total amount of energy produced by a typical person defined by the activity schedule in the input. An internal algorithm is used to determine what fraction of the total is sensible and what fraction is latent. Details about this split are included in the Engineering Reference document.
-
-#### Zone People Sensible Heating Rate [W]
-
-#### Zone People Sensible Heating Energy [J]
-
-These output variables are the amount of sensible heat gain from people within the zone in Watts (for rate) or Joules. This amount is based on the number of people in the space as well as the total amount of energy produced by a typical person defined by the activity schedule in the input. An internal algorithm (described in the Engineering Reference document) is used to determine what fraction of the total is sensible and what fraction is latent. The sensible plus the latent heat gain from people equals the total gain specified in the input.
-
-#### Zone People Total Heating Rate [W]
-
-#### Zone People Total Heating Energy [J]
-
-These output variables are the total amount of heat gain from people within the zone in Watts (for rate) or Joules. Derived from the activity level times the number of occupants, this is summed for each people object within a zone.
-
-#### Zone Thermal Comfort Mean Radiant Temperature [C]
-
-This output variable is the mean radiant temperature used in the thermal comfort calculations.  This value is computed according to the "MRT Calculation Type" specified in the PEOPLE object.  If a high temperature radiant system is present in the zone, this value will be adjusted according to the current heater operation and the "Fraction of radiant energy incident on people" specified in the HIGH TEMP RADIANT SYSTEM object.
-
-#### Zone Thermal Comfort Operative Temperature [C]
-
-This output variable is the operative temperature as defined by the thermal comfort operations. Specifically, it is the average of the thermal comfort mean radiant temperature and the zone air temperature.
-
-Note for all Thermal Comfort reporting:  Though the published values for thermal comfort “vote� have a discrete scale (e.g. –3 to +3 or –4 to +4), the calculations in EnergyPlus are carried out on a continuous scale and, thus, reporting may be “off the scale� with specific conditions encountered in the space. This is not necessarily an error in EnergyPlus – rather a different approach that does not take the “limits� of the discrete scale values into account.
-
-#### Zone Thermal Comfort Fanger Model PMV []
-
-This field is the “predicted mean vote� (PMV) calculated using the Fanger thermal comfort model.
-
-#### Zone Thermal Comfort Fanger Model PPD [%]
-
-This field is the “predicted percentage of dissatisfied� (PPD) calculated using the Fanger thermal comfort model.
-
-#### Zone Thermal Comfort Clothing Surface Temperature [C]
-
-This output variable is the calculation of the clothing surface temperature using the Fanger thermal comfort model.
-
-#### Zone Thermal Comfort Pierce Model Effective Temperature PMV []
-
-This field is the “predicted mean vote� (PMV) calculated using the effective temperature and the Pierce two-node thermal comfort model.
-
-#### Zone Thermal Comfort Pierce Model Standard Effective Temperature PMV []
-
-This field is the “predicted mean vote� (PMV) calculated using the “standard� effective temperature and the Pierce two-node thermal comfort model.
-
-#### Zone Thermal Comfort Pierce Model Discomfort Index []
-
-This field is the “discomfort index� calculated using the the Pierce two-node thermal comfort model.
-
-#### Zone Thermal Comfort Pierce Model Thermal Sensation Index []
-
-This field is the “thermal sensation index� (PMV) calculated using the Pierce two-node thermal comfort model.
-
-#### Zone Thermal Comfort KSU Model Thermal Sensation Vote []
-
-This field is the “thermal sensation vote� (TSV) calculated using the KSU two-node thermal comfort model.
-
-#### Zone Thermal Comfort ASHRAE 55 Adaptive Model 90% Acceptability Status []
-
-This field is to report whether the operative temperature falls into the 90% acceptability limits of the adaptive comfort in ASHRAE 55-2010. A value of 1 means within (inclusive) the limits, a value of 0 means outside the limits, and a value of -1 means not applicable (when unoccupied or running average outdoor temp is outside the range of 10.0 to 33.5C).
-
-#### Zone Thermal Comfort ASHRAE 55 Adaptive Model 80% Acceptability Status [ ]
-
-This field is to report whether the operative temperature falls into the 80% acceptability limits of the adaptive comfort in ASHRAE 55-2010. A value of 1 means within (inclusive) the limits, a value of 0 means outside the limits, and a value of -1 means not applicable (when unoccupied or running average outdoor temp is outside the range of 10.0 to 33.5C).
-
-#### Zone Thermal Comfort ASHRAE 55 Adaptive Model Running Average Outdoor Air Temperature [C]
-
-This field reports the mean monthly outdoor air temperature, an input parameter for the ASHRAE-55 adaptive comfort model. This can be computed in two ways. If the .stat file is provided for the simulation, this field will reflect the monthly daily average temperature.
-
-If the .epw file is used, the field reports the simple running average of the daily average outdoor dry-bulb temperatures of the previous 30 days.
-
-#### Zone Thermal Comfort ASHRAE 55 Adaptive Model Temperature [C]
-
-This field reports the ideal indoor operative temperature, or comfort temperature, as determined by the ASHRAE-55 adaptive comfort model. The 80% acceptability limits for indoor operative temperature are defined as no greater than 3.5 degrees C from the adaptive comfort temperature. The 90% acceptability limits are defined as no greater than 2.5 degrees C from the adaptive comfort temperature. A value of -1 means not applicable (when running average outdoor temp is outside the range of 10.0 to 33.5C).
-
-#### Zone Thermal Comfort CEN 15251 Adaptive Model Category I Status
-
-This field is to report whether the operative temperature falls into the Category I (90% acceptability) limits of the adaptive comfort in the European Standard EN15251-2007. A value of 1 means within (inclusive) the limits, a value of 0 means outside the limits, and a value of -1 means not applicable (when unoccupied or running average outdoor temp is outside the range of 10.0 to 30.0C).
-
-#### Zone Thermal Comfort CEN 15251 Adaptive Model Category II Status
-
-This field is to report whether the operative temperature falls into the Category II (80% acceptability) limits of the adaptive comfort in the European Standard EN15251-2007. A value of 1 means within (inclusive) the limits, a value of 0 means outside the limits, and a value of -1 means not applicable (when unoccupied or running average outdoor temp is outside the range of 10.0 to 30.0C).
-
-#### Zone Thermal Comfort CEN 15251 Adaptive Model Category III Status
-
-This field is to report whether the operative temperature falls into the Category III (65% acceptability) limits of the adaptive comfort in the European Standard EN15251-2007. A value of 1 means within (inclusive) the limits, a value of 0 means outside the limits, and a value of -1 means not applicable (when unoccupied or running average outdoor temp is outside the range of 10.0 to 30.0C).
-
-#### Zone Thermal Comfort CEN 15251 Adaptive Model Running Average Outdoor Air Temperature
-
-This field reports the weighted average of the outdoor air temperature of the previous seven days, an input parameter for the CEN-15251 adaptive comfort model.
-
-#### Zone Thermal Comfort CEN 15251 Adaptive Model Temperature
-
-This field reports the ideal indoor operative temperature, or comfort temperature, as determined by the CEN-15251 adaptive comfort model. Category I, II, and II limits for indoor operative temperature are defined as no greater than 2, 3, and 4 degrees C from this value respectively. A value of -1 means not applicable (when running average outdoor temp is outside the range of 10.0 to 30.0C).
-
-### Simplified ASHRAE 55-2004 Graph Related Outputs
-
-The following output variables are all based on whether the humidity ratio and the operative temperature is within the region shown in ASHRAE Standard 55-2004 in Figure 5.2.1.1. For these outputs the operative temperature is simplified to be the average of the air temperature and the mean radiant temperature. For summer, the 0.5 Clo level is used and, for winter, the 1.0 Clo level is used. The graphs below are based on the following tables which extend the ASHRAE values to zero humidity ratio.
-
-Table 12. Winter Clothes (1.0 Clo)
-
-<table class="table table-striped">
-<tr>
-<th>Operative Temperature (C)</th>
-<th>Humidity Ratio (kgWater/kgDryAir)</th>
-</tr>
-<tr>
-<td>19.6</td>
-<td>0.012</td>
-</tr>
-<tr>
-<td>23.9</td>
-<td>0.012</td>
-</tr>
-<tr>
-<td>26.3</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>21.7</td>
-<td>0.000</td>
-</tr>
-</table>
-
-
-
-![](media/image084.png)
-
-Figure 49. Winter Comfort Range
-
-
-
-Table 13. Summer Clothes (0.5 Clo)
-
-<table class="table table-striped">
-<tr>
-<th>Operative Temperature (C)</th>
-<th>Humidity Ratio (kgWater/kgDryAir)</th>
-</tr>
-<tr>
-<td>23.6</td>
-<td>0.012</td>
-</tr>
-<tr>
-<td>26.8</td>
-<td>0.012</td>
-</tr>
-<tr>
-<td>28.3</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>25.1</td>
-<td>0.000</td>
-</tr>
-</table>
-
-
-![](media/image085.png)
-
-Figure 50. Summer Comfort Range
-
-#### Zone Thermal Comfort ASHRAE 55 Simple Model Summer Clothes Not Comfortable Time[hr]
-
-The time when the zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 summer clothes region (see above)
-
-#### Zone Thermal Comfort ASHRAE 55 Simple Model Winter Clothes Not Comfortable Time[hr]
-
-The time when the zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 winter clothes region (see above)
-
-#### Zone Thermal Comfort ASHRAE 55 Simple Model Summer or Winter Clothes Not Comfortable Time[hr]
-
-The time when the zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 summer or winter clothes region (see above)
-
-#### Facility Thermal Comfort ASHRAE 55 Simple Model Summer Clothes Not Comfortable Time[hr]
-
-The time when any zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 summer clothes region (see above)
-
-#### Facility Thermal Comfort ASHRAE 55 Simple Model Winter Clothes Not Comfortable Time [hr]
-
-The time when any zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 winter clothes region (see above)
-
-#### Facility Thermal Comfort ASHRAE 55 Simple Model Summer or Winter Clothes Not Comfortable Time [hr]
-
-The time when any zone is occupied that the combination of humidity ratio and operative temperature is not in the ASHRAE 55-2004 summer or winter clothes region (see above)
-
-### Simplified ASHRAE 55 Warnings
-
-The simplified ASHRAE 55 calculations may be computed for occupied zones and, possibly, warnings are shown on the .err file at the end of each simulated environment. To enable this option set the “Enable ASHRAE 55 comfort warnings� field of the People object to Yes. These warnings will not be generated by default.
-
-If you enable the warnings, the simplified ASHRAE 55 calculations are done for occupied zones and, possibly, warnings are shown on the .err file at the end of each simulated environment.
-
-```
-   ** Warning ** More than 4% of time (350.4 hours) uncomfortable in zone ZSF1
-   **   ~~~   ** 553.0 hours were uncomfortable based on ASHRAE 55-2004 graph (Section 5.2.1.1)
-   **   ~~~   ** During Environment [10/01 - 09/30]: CHICAGO IL USA TMY2-94846 WMO\#=725300
-   ** Warning ** More than 4% of time (350.4 hours) uncomfortable in zone ZNF1
-   **   ~~~   ** 827.8 hours were uncomfortable based on ASHRAE 55-2004 graph (Section 5.2.1.1)
-   **   ~~~   ** During Environment [10/01 - 09/30]: CHICAGO IL USA TMY2-94846 WMO\#=725300
-   ** Warning ** More than 4% of time (350.4 hours) uncomfortable in zone ZSF2
-   **   ~~~   ** 593.5 hours were uncomfortable based on ASHRAE 55-2004 graph (Section 5.2.1.1)
-   **   ~~~   ** During Environment [10/01 - 09/30]: CHICAGO IL USA TMY2-94846 WMO\#=725300
-   ** Warning ** More than 4% of time (350.4 hours) uncomfortable in zone ZNF2
-   **   ~~~   ** 875.8 hours were uncomfortable based on ASHRAE 55-2004 graph (Section 5.2.1.1)
-   **   ~~~   ** During Environment [10/01 - 09/30]: CHICAGO IL USA TMY2-94846 WMO\#=725300
-```
-
-You may decide if you need to change parameters to reduce these “uncomfortable� hours. The individual output variables shown previously may help you get more details on when these are occurring.
-
-Following are some suggestions that might be applicable:
-
-- Eliminate occupancy when conditioning equipment is off.
-
-- Note that the ASHRAE graph lower limit is (19.6C to 21.7C) – heating setpoints may need to be nearer 22.2C (72F) than 21.1C (70F).
-
-- Unoccupied heating setpoint should be nearer 16.7C (62F) rather than 12.8C (55F) to reduce the start up recovery.
-
-- Start the occupied setpoint schedule, fan availability schedule, cooling pump availability schedule, reheat coil availability, one hour before occupancy. Seasonal turn on and off of equipment may cause more warnings (but potentially more energy consumption).
-
-- Unoccupied cooling setpoint should be nearer 29.4C (85F) rather than 40.0 (104F) to reduce the start up recovery.
-
-### ComfortViewFactorAngles
-
-When requesting EnergyPlus to do a thermal comfort calculation, the program user has three options for defining how the mean radiant temperature will be calculated. The user may select “zoneaveraged� which results in a mean radiant temperature that is characteristic of an “average� location near the center of the zone. The user may also elect to place the person near a particular surface by selecting “surfaceweighted� in the People statement. This takes the average of the zone mean radiant temperature and the temperature of the surface that the person is near and uses this value as the mean radiant temperature when calculating thermal comfort.
-
-The third option is for the user to more explicitly position the person within the space by defining the angle factors from the person to the various surfaces in the zone. This option requires the user to list the surfaces that the person can see from a radiation standpoint and also define the angle (or view) factor for each surface. The AngleFactorList input line is intended to give the user this opportunity.
-
-#### Field: Name
-
-This field is an unique user assigned name for the list of surfaces that can be seen radiantly by the person for whom thermal comfort is to be evaluated. Any reference to this list by a People statement will use this name.
-
-#### Field: Zone Name
-
-Zone Name for this surface list. Each of the surfaces listed must be in this zone.
-
-#### Field: Surface &lt;\#&gt; Name
-
-This field is the name of a surface in the zone seen by the person.
-
-#### Field: Angle Factor &lt;\#&gt;
-
-This field is the fraction that this surface contributes to the total mean radiant temperature. This can be thought of as a weighting factor for this surface and the actual mean radiant temperature used in the thermal comfort model is simply the sum of all angle factors multiplied by the corresponding inside surface temperature. Note that the Surface Name/Angle Factor pair can be repeated up to 20 times. The sum of all angle factors within any angle factor list must equal unity, otherwise the program will not accept the input as valid.
-
-An example IDF with an electric low temperature radiant system is shown below.
-
-```idf
-ComfortViewFactorAngles,
-    South Zone Angle Factors, !- name of angle factor list
-    Sourth Zone,              !- Zone Name
-    Zn001:Flr001,             !- Surface name 1
-    0.75,                     !- Angle factor for surface 1
-    Zn001:Wall001,            !- Surface name 2
-    0.15,                     !- Angle factor for surface 2
-    Zn001:Roof001,            !- Surface name 3
-    0.10;                     !- Angle factor for surface 3
-```
-
-
-### Lights
-
-The Lights statement allows you to specify information about a zone’s electric lighting system, including design power level and operation schedule, and how the heat from lights is distributed thermally.
-
-A zone may have multiple Lights statements. For example, one statement may describe the general lighting in the zone and another the task lighting. Or you can use multiple Lights statements for a zone that has two or more general lighting systems that differ in design level, schedule, etc.
-
-#### Field: Name
-
-The name of the Lights object.
-
-#### Field: Zone or ZoneList Name
-
-The field is the name of the thermal zone (ref: Zone) or ZoneList (ref: ZoneLIst) and links this Lights statement to a thermal zone or set of thermal zones in the buidling. When the ZoneList option is used then this lights definition is applied to each of the zones in the zone list effecting a global definition for the amount of light wattage in the zone. The Zonelist option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
-
-The name of the actual lights object becomes &lt;Zone Name&gt; &lt;Lights Object Name&gt; and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
-
-#### Field: Schedule Name
-
-The name of the schedule that modifies the lighting power design level (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The electrical input for lighting in a particular timestep is the product of the design level and the value of this schedule in that timestep. If the design level is the maximum lighting power input the schedule should contain values between 0.0 and 1.0.
-
-#### Field: Design Level Calculation Method
-
-This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal lighting level in the Zone. The key/choices are:
-
-- LightingLevel
-
-With this choice, the method used will be a straight insertion of the lighting level (Watts) for the Zone.  (The Lighting Level field should be filled.)
-
-- Watts/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The Watts per Zone Floor Area field should be filled).
-
-- Watts/Person
-
-With this choice, the method used will be a factor of lighting level (watts) per person. (The Watts per person field should be filled).
-
-#### Field: Lighting Level
-
-This is typically the maximum electrical power input (in Watts) to lighting in a zone, including ballasts, if present. This value is multiplied by a schedule fraction (see previous field) to get the lighting power in a particular timestep. In EnergyPlus, this is slightly more flexible in that the lighting design level could be a “diversity factor� applied to a schedule of real numbers.
-
-#### Field: Watts per Zone Floor Area
-
-This factor (watts/m<sup>2</sup>) is used, along with the Zone Floor Area to determine the maximum lighting level as described in the Lighting Level field. The choice from the method field should be “watts/area�.
-
-#### Field: Watts per Person
-
-This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum lighting level as described in the Lighting Level field. The choice from the method field should be “watts/person�.
-
-#### Heat Gains from Lights:
-
-The electrical input to lighting ultimately appears as heat that contributes to zone loads or to return air heat gains. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Return Air Fraction, Fraction Radiant and Fraction Visible. A fourth, defined as the fraction of the heat from lights convected to the zone air, is calculated by the program as:
-
-f<sub>convected</sub> = 1.0 – (Return Air Fraction + Fraction Radiant + Fraction Visible)
-
-You will get an error message if Return Air Fraction + Fraction Radiant + Fraction Visible exceeds 1.0.
-
-These fractions depend on the type of lamp and luminaire, whether the luminaire is vented to the return air, etc.
-
-#### Field: Return Air Fraction
-
-The fraction of the heat from lights that goes into the zone return air (i.e., into the zone outlet node). If the return air flow is zero or the zone has no return air system, the program will put this fraction into the zone air. Return Air Fraction should be non-zero only for luminaires that are return-air ducted  (see Table 14 and Figure 51). (However, see the field “Return Air Fraction Is Calculated from Plenum Temperature,� below, for an approach to modeling the case where Return Air Fraction is caused by *conduction* between a luminaire that is in contact with a return-air plenum.)
-
-#### Field: Fraction Radiant
-
-The fraction of heat from lights that goes into the zone as long-wave (thermal) radiation. The program calculates how much of this radiation is absorbed by the inside surfaces of the zone according the area times thermal absorptance product of these surfaces.
-
-#### Field: Fraction Visible
-
-The fraction of heat from lights that goes into the zone as visible (short-wave) radiation. The program calculates how much of this radiation is absorbed by the inside surfaces of the zone according the area times solar absorptance product of these surfaces.
-
-Approximate values of Return Air Fraction, Fraction Radiant and Fraction Visible are given in Table 14 for overhead fluorescent lighting for a variety of luminaire configurations. The data is based on ASHRAE 1282-RP "Lighting Heat Gain Distribution in Buildings" by Daniel E. Fisher and Chanvit Chantrasrisalai.
-
-Table 14. Approximate values of Return Air Fraction, Fraction Radiant and Fraction Visible for overhead fluorescent lighting for different luminaire configurations. 
-
-<table class="table table-striped">
-  <tr>
-    <th>Fixture No.</th>
-    <th>Luminaire Feature</th>
-    <th>Return Air Fraction</th>
-    <th>Fraction Radiant</th>
-    <th>Fraction Visible</th>
-    <th>fconvected</th>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td>Recessed, Parabolic Louver, Non-Vented, T8</td>
-    <td>0.31</td>
-    <td>0.22</td>
-    <td>0.20</td>
-    <td>0.27</td>
-  </tr>
-  <tr>
-    <td>2</td>
-    <td>Recessed, Acrylic Lens, Non-Vented, T8</td>
-    <td>0.56</td>
-    <td>0.12</td>
-    <td>0.20</td>
-    <td>0.12</td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>Recessed, Parabolic Louver, Vented, T8</td>
-    <td>0.28</td>
-    <td>0.19</td>
-    <td>0.20</td>
-    <td>0.33</td>
-  </tr>
-  <tr>
-    <td>4</td>
-    <td>Recessed, Acrylic Lens, Vented, T8</td>
-    <td>0.54</td>
-    <td>0.10</td>
-    <td>0.18</td>
-    <td>0.18</td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>Recessed, Direct/Indirect, T8</td>
-    <td>0.34</td>
-    <td>0.17</td>
-    <td>0.16</td>
-    <td>0.33</td>
-  </tr>
-  <tr>
-    <td>6</td>
-    <td>Recessed, Volumetric, T5</td>
-    <td>0.54</td>
-    <td>0.13</td>
-    <td>0.20</td>
-    <td>0.13</td>
-  </tr>
-  <tr>
-    <td>7</td>
-    <td>Downlights, Compact Fluorescent, DTT</td>
-    <td>0.86</td>
-    <td>0.04</td>
-    <td>0.10</td>
-    <td>0.00</td>
-  </tr>
-  <tr>
-    <td>8</td>
-    <td>Downlights, Compact Fluorescent, TRT</td>
-    <td>0.78</td>
-    <td>0.09</td>
-    <td>0.13</td>
-    <td>0.00</td>
-  </tr>
-  <tr>
-    <td>9a</td>
-    <td>Downlights, Incandescent, A21</td>
-    <td>0.29</td>
-    <td>0.10</td>
-    <td>0.6</td>
-    <td>0.01</td>
-  </tr>
-  <tr>
-    <td>9b</td>
-    <td>Downlights, Incandescent, BR40</td>
-    <td>0.21</td>
-    <td>0.08</td>
-    <td>0.71</td>
-    <td>0.00</td>
-  </tr>
-  <tr>
-    <td>10</td>
-    <td>Surface Mounted, T5HO</td>
-    <td>0.00</td>
-    <td>0.27</td>
-    <td>0.23</td>
-    <td>0.50</td>
-  </tr>
-  <tr>
-    <td>11</td>
-    <td>Pendant, Direct/Indirect, T8</td>
-    <td>0.00</td>
-    <td>0.32</td>
-    <td>0.23</td>
-    <td>0.45</td>
-  </tr>
-  <tr>
-    <td>12</td>
-    <td>Pendant, Indirect, T5HO</td>
-    <td>0.00</td>
-    <td>0.32</td>
-    <td>0.25</td>
-    <td>0.43</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td>Recessed, Parabolic Louver, Non-Vented, T8 - Ducted</td>
-    <td>0.27</td>
-    <td>0.27</td>
-    <td>0.21</td>
-    <td>0.25</td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>Recessed, Direct/Indirect, T8 - Ducted</td>
-    <td>0.27</td>
-    <td>0.22</td>
-    <td>0.17</td>
-    <td>0.34</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td>Recessed, Parabolic Louver, Non-Vented, T8 - Half Typical Supply Airflow Rate</td>
-    <td>0.45</td>
-    <td>0.30</td>
-    <td>0.22</td>
-    <td>0.03</td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>Recessed, Parabolic Louver, Vented, T8 - Half Typical Supply Airflow Rate</td>
-    <td>0.43</td>
-    <td>0.25</td>
-    <td>0.21</td>
-    <td>0.11</td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>Recessed, Direct/Indirect, T8 - Half Typical Supply Airflow Rate</td>
-    <td>0.43</td>
-    <td>0.27</td>
-    <td>0.18</td>
-    <td>0.12</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>1</td>
-    <td>Recessed, Parabolic Louver, Non-Vented, T8 - Half Typical Supply Airflow Rate</td>
-    <td>0.10</td>
-    <td>0.16</td>
-    <td>0.20</td>
-    <td>0.54</td>
-  </tr>
-  <tr>
-    <td>3</td>
-    <td>Recessed, Parabolic Louver, Vented, T8 - Half Typical Supply Airflow Rate</td>
-    <td>0.11</td>
-    <td>0.15</td>
-    <td>0.19</td>
-    <td>0.55</td>
-  </tr>
-  <tr>
-    <td>5</td>
-    <td>Recessed, Direct/Indirect, T8 - Half Typical Supply Airflow Rate</td>
-    <td>0.04</td>
-    <td>0.13</td>
-    <td>0.16</td>
-    <td>0.67</td>
-  </tr>
-</table>
-
-#### Field: Fraction Replaceable
-
-This field defines the daylighting control for the LIGHTS object.
-
-If **Daylighting:Controls** or **Daylighting:DELight:Controls** is specified for the zone, this field is used as an on/off flag for dimming controls. If set to 0.0, the lights are not dimmed by the daylighting controls. If set to 1.0, the lights are allowed to be dimmed by the daylighting controls.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Task Lights", "Hall Lights", etc. A new meter for reporting is created for each unique subcategory  (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the lights will be assigned to the "General" end-use subcategory.
-
-#### Field: Return Air Fraction Calculated from Plenum Temperature
-
-Accepts values Yes or No (the default). Yes is for advanced used only. In this case the program will calculate the return air fraction by assuming that it is due to conduction of some of the light heat into the zone’s return air plenum and that the amount of the conduction depends on the plenum air temperature. A Yes value should only be used for luminaires that are recessed and non-vented, as shown in Figure 52.
-
-The value you enter for the Return Air Fraction field will be ignored and you can enter, for fluorescent lighting, Fraction Radiant = 0.37 and Fraction Visible = 0.18, as indicated in Table 14.
-
-This feature requires that the coefficients described below be determined from measurements or detailed calculations since they are very sensitive to the luminaire type, lamp type, thermal resistance between fixture and plenum, etc.
-
-If “Return Air Fraction Is Calculated from Plenum Temperature� = Yes, the return air fraction is calculated *each timestep* from the following empirical correlation:
-
-(Return Air Fraction)<sub>calculated</sub> = C<sub>1</sub> – C<sub>2</sub> x T<sub>plenum</sub>
-
-where T<sub>plenum</sub> is the previous-time-step value of the return plenum air temperature (C),
-
-and C<sub>1</sub> and C<sub>2</sub>  are the values of the coefficients entered in the next two fields.
-
-To compensate for the change in the return air fraction relative to its input value, the program modifies Fraction Radiant and f<sub>convected</sub> by a scale factor such that
-
-(Return Air Fraction)<sub>calculated</sub> + (Fraction Radiant)<sub>modified</sub>+ (f<sub>convected</sub>)<sub>modified</sub> + (Fraction Visible)<sub>input</sub> = 1.0
-
-It is assumed that Fraction Visible is a constant equal to its input value.
-
-#### Field: Return Air Fraction Function of Plenum Temperature Coefficient 1
-
-The coefficient C<sub>1</sub> in the equation for (Return Air Fraction)<sub>calculated</sub>.
-
-#### Field: Return Air Fraction Function of Plenum Temperature Coefficient 2
-
-The coefficient C<sub>2</sub>  in the equation for (Return Air Fraction)<sub>calculated</sub>. Its units are 1/<sup>O</sup>C.
-
-![](media/image087.svg)
-
-Figure 52. Vertical section through a zone and its return air plenum showing recessed lighting (not to scale). The heat from lights is divided into four fractions, three of which—ReturnAirFraction, FractionRadiant and FractionConvected—depend on plenum air temperature.
-
-An IDF example:
-
-```idf
-Lights,
-    RIGHT FORK Lights 1,     !- Name
-    RIGHT FORK,              !- Zone Name
-    Office Lighting,         !- SCHEDULE Name
-    LightingLevel,          !- Design Level calculation method
-    1039.706,,,                !- Lighting Level {W}
-    0.0000000E+00,           !- Return Air Fraction
-    0.4000000,               !- Fraction Radiant
-    0.2000000,               !- Fraction Visible
-    1.0,                     !- Fraction Replaceable
-    GeneralLights;           !- End-Use Subcategory
-```
-
-Global Lights Object:
-
-```idf
-  ZoneList,AllOccupiedZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
-
-  Lights,
-    AllZones with Lights,       !- Name
-    AllOccupiedZones,        !- Zone or ZoneList Name
-    LIGHTS-1,                !- Schedule Name
-    Watts/Area,              !- Design Level Calculation Method
-    ,                        !- Lighting Level {W}
-    16,                      !- Watts per Zone Floor Area {W/m2}
-    ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
-    0.59,                    !- Fraction Radiant
-    0.2,                     !- Fraction Visible
-    0,                       !- Fraction Replaceable
-    GeneralLights;           !- End-Use Subcategory
-```
-
-### Lights Report Outputs
-
-If daylighting controls are operating in the zone, all of the Lights objects with a Fraction Replaceble  greater than zero will be reduced by a multiplicative factor that accounts for how much the electric lighting is lowered due to daylighting.
-
-Lights objects have output variables for individual objects and for zone totals.
-
-* Zone,Average,Lights Electric Power [W]
-
-* Zone,Sum,Lights Radiant Heat Gain [J]
-
-* Zone,Average,Lights Radiant Heating Rate [W]
-
-* Zone,Sum,Lights Visible Radiation Heating Energy [J]
-
-* Zone,Average,Lights Visible Radiation Heating Rate [W]
-
-* Zone,Sum,Lights Convective Heating Energy [J]
-
-* Zone,Average,Lights Convective Heating Rate [W]
-
-* Zone,Sum,Lights Return Air Heating Energy [J]
-
-* Zone,Average,Lights Return Air Heating Rate [W]
-
-* Zone,Sum,Lights Total Heating Energy [J]
-
-* Zone,Average,Lights Total Heating Rate [W]
-
-* Zone,Sum,Lights Electric Energy [J]
-
-* Zone,Average,Zone Lights Electric Power [W]
-
-* Zone,Sum,Zone Lights Radiant Heating Energy [J]
-
-* Zone,Average,Zone Lights Radiant Heating Rate [W]
-
-* Zone,Sum,Zone Lights Visible Radiation Heating Energy [J]
-
-* Zone,Average,Zone Lights Visible Radiation Heating Rate [W]
-
-* Zone,Sum,Zone Lights Convective Heating Energy [J]
-
-* Zone,Average,Zone Lights Convective Heating Rate [W]
-
-* Zone,Sum,Zone Lights Return Air Heating Energy [J]
-
-* Zone,Average,Zone Lights Return Air Heating Rate [W]
-
-* Zone,Sum,Zone Lights Total Heating Energy [J]
-
-* Zone,Average,Zone Lights Total Heating Rate [W]
-
-* Zone,Sum,Zone Lights Electric Energy [J]
-
-#### Lights Electric Power [W]
-
-The electric power input for the lights.
-
-#### Lights Radiant Heating Rate [W]
-
-#### Lights Radiant Heating Energy [J]
-
-The amount of heat gain from lights that is in the form of long-wave (thermal) radiation entering the zone. This heat is absorbed by the inside surfaces of the zone according to an area times long-wave absorptance weighting scheme.
-
-#### Lights Visible Radiation Heating Rate [W]
-
-#### Lights Visible Radiation Heating Energy [J]
-
-The amount of heat gain from lights that is in the form of visible (short-wave) radiation entering the zone. This heat is absorbed by the inside surfaces of the zone according  to an area times short-wave absorptance weighting scheme.
-
-#### Lights Convective Heating Rate [W]
-
-#### Lights Convective Heating Energy [J]
-
-The amount of heat gain from lights that is convected to the zone air.
-
-#### Lights Return Air Heating Rate [W]
-
-#### Lights Return Air Heating Energy [J]
-
-The amount of heat gain from lights that goes into the zone’s return air (and, therefore, does not directly contribute to the zone load). If the zone has no return air system or the zone’s air system is off, this heat will be added to the zone air.
-
-#### Lights Total Heating Rate [W]
-
-#### Lights Total Heating Energy [J]
-
-The total heat gain from lights. It is the sum of the following four outputs, i.e., Total Heat Gain = Return Air Heat Gain + Radiant Heat Gain + Visible Heat Gain + Convective Heat Gain. It is also equal to the electrical input to the lights.
-
-#### Lights Electric Energy [J]
-
-The lighting electrical consumption including ballasts, if present. These will have the same value as Lights Total Heating Energy (above).
-
-#### Zone Lights Electric Power [W]
-
-The electric power input for all lights in the zone.
-
-#### Zone Lights Radiant Heating Rate [W]
-
-#### Zone Lights Radiant Heating Energy [J]
-
-The amount of heat gain from all lights in the zone that is in the form of long-wave (thermal) radiation entering the zone. This heat is absorbed by the inside surfaces of the zone according to an area times long-wave absorptance weighting scheme.
-
-#### Zone Lights Visible Radiation Heating Rate [W]
-
-#### Zone Lights Visible Radiation Heating Energy [J]
-
-The amount of heat gain from all lights in the zone that is in the form of visible (short-wave) radiation entering the zone. This heat is absorbed by the inside surfaces of the zone according  to an area times short-wave absorptance weighting scheme.
-
-#### Zone Lights Convective Heating Rate [W]
-
-#### Zone Lights Convective Heating Energy [J]
-
-The amount of heat gain from all lights in the zone that is convected to the zone air.
-
-#### Zone Lights Return Air Heating Rate [W]
-
-#### Zone Lights Return Air Heating Energy [J]
-
-The amount of heat gain from all lights in the zone that goes into the zone’s return air (and, therefore, does not directly contribute to the zone load). If the zone has no return air system or the zone’s air system is off, this heat will be added to the zone air.
-
-#### Zone Lights Total Heating Rate [W]
-
-#### Zone Lights Total Heating Energy [J]
-
-The total heat gain from all lights in the zone. It is the sum of the following four outputs, i.e., Total Heat Gain = Return Air Heat Gain + Radiant Heat Gain + Visible Heat Gain + Convective Heat Gain. It is also equal to the electrical input to the lights.
-
-#### Zone Lights Electric Energy [J]
-
-The lighting electrical consumption for all lights in the zone including ballasts, if present. This will have the same value as Zone Lights Total Heating Energy (above). However, this amount is also shown in the Electricity meters that are associated with the zone:
-
-Electricity:Facility,
-
-Electricity:Building,
-
-Electricity:Zone:&lt;Zone Name&gt;.
-
-In addition, depending on use, it will be shown in:
-
-InteriorLights: Electricity and
-
-InteriorLights:Electricity:Zone :&lt;Zone Name&gt;.
-
-### Meters for Lights Outputs
-
-As described in the Lights Outputs, values for lights will show up on the following meters:
-
-Table 15. Distribution of Lights to Meters
-
-<table class="table table-striped">
-<tr>
-<th>Meter Name</th>
-<th>Scope</th>
-<th>Lights Specfics</th>
-</tr>
-<tr>
-<td>Electricity:Facility</td>
-<td>Entire Facility</td>
-<td>All</td>
-</tr>
-<tr>
-<td>Electricity:Building</td>
-<td>All Zones</td>
-<td>All</td>
-</tr>
-<tr>
-<td>Electricity:Zone:&lt;Zone Name&gt;</td>
-<td>Specific Zone</td>
-<td>All</td>
-</tr>
-<tr>
-<td>InteriorLights:Electricity</td>
-<td>All Zones</td>
-<td>Lights Use</td>
-</tr>
-<tr>
-<td>InteriorLights:Electricity:Zone:&lt;Zone Name&gt;</td>
-<td>Specific Zone</td>
-<td>Lights Use</td>
-</tr>
-<tr>
-<td>&lt;End-Use Subcategory&gt;:InteriorLights:Electricity</td>
-<td>Specific Subcategory</td>
-<td>Lights Use</td>
-</tr>
-</table>
-
-### ElectricEquipment
-
-The object models equipment in the zone which consumes electricity, such as computers, televisions, and cooking equipment, also known as “plug loads.� All of the energy consumed by the equipment becomes a heat gain in the zone or is lost (exhausted) as specified below.
-
-#### Field: Name
-
-The name of the ElectricEquipment object.
-
-#### Field: Zone or ZoneList Name
-
-This field is the name of the zone (ref: Zone) or ZoneList (ref: ZoneList) and attaches a particular electric equipment statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this electric equipment definition is applied to each of the zones in the zone list effecting a global definition for the amount of electric wattage in the zone. The Zonelist option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
-
-The name of the actual electric equipment object becomes &lt;Zone Name&gt; &lt;ElectricEquipment Object Name&gt; and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule that modifies the design level parameter for electric equipment (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The actual electrical input for equipment in a zone as defined by this statement is the product of the design level field and the value of the schedule specified by name in this field.
-
-#### Field: Design Level Calculation Method
-
-This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal electric equipment level in the Zone. The key/choices are:
-
-- EquipmentLevel
-
-With this choice, the method used will be a straight insertion of the electric equipment level (Watts) for the Zone.  (The Design Level field should be filled.)
-
-- Watts/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The Watts per Zone Floor Area field should be filled).
-
-- Watts/Person
-
-With this choice, the method used will be a factor of equipment level (watts) per person. (The Watts per Person field should be filled).
-
-#### Field: Design Level
-
-This field (in Watts) is typically used to represent the maximum electrical input to equipment in a zone that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the electric equipment design level could be a “diversity factor� applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour, the design level field is constant for all simulation environments.
-
-#### Field: Watts per Zone Floor Area
-
-This factor (watts/m<sup>2</sup>) is used, along with the Zone Area to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be “Watts/Area�.
-
-#### Field: Watts per Person
-
-This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be “Watts/Person�.
-
-#### Heat Gains from Electric Equipment:
-
-The electrical input to the equipment ultimately appears as heat that contributes to zone loads. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Fraction Latent, Fraction Radiant and Fraction Lost. A fourth, defined as the fraction of the heat from electric equipment convected to the zone air, is calculated by the program as:
-
-f<sub>convected</sub> = 1.0 – (Fraction Latent + Fraction Radiant + Fraction Lost)
-
-You will get an error message if Fraction Latent + Fraction Radiant + Fraction Lost exceeds 1.0.
-
-#### Field: Fraction Latent
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of latent heat given off by electric equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by electric equipment to give the amount of latent energy produced by the electric equipment. This energy affects the moisture balance within the zone.
-
-#### Field: Fraction Radiant
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of long-wave radiant heat being given off by electric equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by electric equipment to give the amount of long wavelength radiation gain from electric equipment in a zone.
-
-#### Field: Fraction Lost
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of “lost� heat being given off by electric equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by electric equipment to give the amount of heat which is “lost� and does not impact the zone energy balances. This might correspond to electrical energy converted to mechanical work or heat that is vented to the atmosphere.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Computers", "Copy Machines", etc. A new meter for reporting is created for each unique subcategory  (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the "General" end-use subcategory.
-
-An IDF example:
-
-```idf
-ElectricEquipment,
-    DORM ROOMS AND COMMON AREAS ElecEq 1,  !- Name
-    DORM ROOMS AND COMMON AREAS,  !- Zone Name
-    Residence Equipment,     !- SCHEDULE Name
-    EquipmentLevel,         !- Design Level calculation method
-    9210.921,                !- Design Level {W}
-    ,                        !- Watts per Zone Floor Area {watts/m2}
-    ,                        !- Watts per Person {watts/person}
-    0.0000000E+00,           !- Fraction Latent
-    0.3000000,               !- Fraction Radiant
-    0.0000000E+00,           !- Fraction Lost
-    Computers;               !- End-use Subcategory
-```
-
-Global ElectricEquipment example:
-
-```idf
-  ZoneList,AllOccupiedZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
-
-  ElectricEquipment,
-    AllZones with Electric Equipment,       !- Name
-    AllOccupiedZones,        !- Zone or ZoneList Name
-    EQUIP-1,                 !- Schedule Name
-    Watts/Person,            !- Design Level Calculation Method
-    ,                        !- Design Level {W}
-    ,                        !- Watts per Zone Floor Area {W/m2}
-    96,                      !- Watts per Person {W/person}
-    0,                       !- Fraction Latent
-    0.3,                     !- Fraction Radiant
-    0;                       !- Fraction Lost
-```
-
-### GasEquipment
-
-The object models equipment in the zone which consumes natural gas, such as cooking equipment or a gas fireplace. All of the energy consumed by the equipment becomes a heat gain in the zone or is lost (exhausted) as specified below.
-
-#### Field: Name
-
-The name of the GasEquipment object.
-
-#### Field: Zone or ZoneList Name
-
-This field is the name of the thermal zone (ref: Zone) or ZoneList (ref: ZoneList) and attaches a particular gas equipment statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this gas equipment definition is applied to each of the zones in the zone list effecting a global definition for the amount of gas in the zone. The Zonelist option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
-
-The name of the actual gas equipment object becomes &lt;Zone Name&gt; &lt;GasEquipment Object Name&gt; and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule that modifies the design level parameter for gas equipment (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The actual energy input for gas equipment in a zone as defined by this statement is the product of the design level field and the value of the schedule specified by name in this field.
-
-#### Field: Design Level Calculation Method
-
-This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal gas equipment level in the Zone. The key/choices are:
-
-- EquipmentLevel
-
-With this choice, the method used will be a straight insertion of the gas equipment level (Watts) for the Zone.  (The Design Level field should be filled.)
-
-- Watts/Area or Power/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The Power per Zone Floor Area field should be filled).
-
-- Watts/Person or Power/Person
-
-With this choice, the method used will be a factor of equipment level (watts) per person. (The Power per Person field should be filled).
-
-#### Field: Design Level
-
-This field (in Watts) is typically used to represent the maximum energy input to gas equipment in a zone that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the gas equipment design level could be a “diversity factor� applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour, the design level field is constant for all simulation environments.
-
-#### Field: Power per Zone Floor Area
-
-This factor (watts/m<sup>2</sup>) is used, along with the Zone Area to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be “**Watts/Area**� or “**Power/Area**�.
-
-#### Field: Power per Person
-
-This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be “**Watts/Person**� or “**Power/Person**�.
-
-#### Heat Gains from Gas Equipment:
-
-The fuel input to the equipment ultimately appears as heat that contributes to zone loads. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Fraction Latent, Fraction Radiant and Fraction Lost. A fourth, defined as the fraction of the heat from gas equipment convected to the zone air, is calculated by the program as:
-
-f<sub>convected</sub> = 1.0 – (Fraction Latent + Fraction Radiant + Fraction Lost)
-
-You will get an error message if Fraction Latent + Fraction Radiant + Fraction Lost exceeds 1.0.
-
-#### Field: Fraction Latent
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of latent heat given off by gas equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by gas equipment to give the amount of latent energy produced by the gas equipment. This energy affects the moisture balance within the zone.
-
-#### Field: Fraction Radiant
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of long-wave radiant heat being given off by gas equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by gas equipment to give the amount of long wavelength radiation gain from gas equipment in a zone.
-
-#### Field: Fraction Lost
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of “lost� heat being given off by gas equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by gas equipment to give the amount of heat which is “lost� and does not impact the zone energy balances. This might correspond to input energy converted to mechanical work or heat that is vented to the atmosphere.
-
-#### Field: Carbon Dioxide Generation Rate
-
-This numeric input field specifies carbon dioxide generation rate with units of m3/s-W. The default value of 0.0 assumes the equipment is fully vented to outdoors. In the absence of better information, the user might consider using a value of 3.45E-8 m3/s-W which assumes the equipment is not vented to outdoors. This value is converted from natural gas CO<sub>2</sub> emission rate at 11.7 lbs CO<sub>2</sub> per therm. The CO<sub>2</sub> emission rate is provided by U.S. Energy Information Administration, "Frequently Asked Questions - Environment, Questions About Environmental Emissions",  http://tonto.eia.doe.gov/ask/environment_faqs.asp#CO2_quantity, January 2010. The maximum value for this input field is 3.45E-7 m3/s-W.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Cooking", "Clothes Drying", etc. A new meter for reporting is created for each unique subcategory  (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the "General" end-use subcategory.
-
-An IDF example:
-
-```idf
-GasEquipment,
-    DORM ROOMS AND COMMON AREAS GasEq 1,  !- Name
-    DORM ROOMS AND COMMON AREAS,  !- Zone Name
-    Gas Eq Sch,              !-Schedule Name
-    EquipmentLevel,          !- Design Level Calculation Method
-    29287.51,                !- Design Level {W}
-    ,                        !- Power per Zone Floor Area {W/m2}
-    ,                        !- Power per Person {W/Person}
-    0,                       !- Fraction Latent
-    0.3,                     !- Fraction Radiant
-    0,                       !- Fraction Lost
-    0,                       !- Carbon Dioxide Generation Rate {m3/s-W}
-    Cooking;                 !- End-Use Subcategory
-```
-
-Global Gas Equipment example:
-
-```idf
-  ZoneList,OfficeZones,Left Fork, Middle Fork, Right Fork;
-
-  GasEquipment,
-    Office Zones with Gas Equipment,       !- Name
-    OfficeZones,               !- Zone Name
-    Gas Eq Sch,              !- Schedule Name
-    Watts/Area,              !- Design Level Calculation Method
-    ,                        !- Design Level {W}
-    197,                     !- Power per Zone Floor Area {W/m2}
-    ,                        !- Power per Person {W/Person}
-    0.0000000E+00,           !- Fraction Latent
-    0.3000000,               !- Fraction Radiant
-    0.0000000E+00;           !- Fraction Lost
-```
-
-### HotWaterEquipment
-
-The object models hot water equipment in the zone which consumes district heating, such as cooking equipment or process loads. All of the energy consumed by the equipment becomes a heat gain in the zone or is lost (exhausted) as specified below. This object consumes district heating energy directly and does not cause a load on a hot water plant loop or water heater. For domestic hot water uses, such as sinks and showers, see WaterUse:Equipment.
-
-#### Field: Name
-
-The name of the HotWaterEquipment object.
-
-#### Field: Zone or ZoneList Name
-
-This field is the name of the thermal zone (ref: Zone) or ZoneList (ref: ZoneList) and attaches a particular hot water equipment statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this hot water equipment definition is applied to each of the zones in the zone list effecting a global definition for the amount of hot water in the zone. The Zonelist option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
-
-The name of the actual hot water equipment object becomes &lt;Zone Name&gt; &lt;HotWaterEquipment Object Name&gt; and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule that modifies the design level parameter for hot water equipment (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The actual energy input for hot water equipment in a zone as defined by this statement is the product of the design level field and the value of the schedule specified by name in this field.
-
-#### Field: Design Level Calculation Method
-
-This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal hot water equipment level in the Zone. The key/choices are:
-
-- EquipmentLevel
-
-With this choice, the method used will be a straight insertion of the hot water equipment level (Watts) for the Zone.  (The Design Level field should be filled.)
-
-- Watts/Area or Power/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The Power per Zone Floor Area field should be filled).
-
-- Watts/Person or Power/Person
-
-With this choice, the method used will be a factor of equipment level (watts) per person. (The Power per Person field should be filled).
-
-#### Field: Design Level
-
-This field (in Watts) is typically used to represent the maximum energy input to hot water equipment in a zone that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the hot water equipment design level could be a “diversity factor� applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour, the design level field is constant for all simulation environments.
-
-#### Field: Power per Zone Floor Area
-
-This factor (watts/m<sup>2</sup>) is used, along with the Zone Area to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be “**Watts/Area**� or “**Power/Area**�.
-
-#### Field: Power per Person
-
-This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be “**Watts/Person**� or “**Power/Person**�.
-
-#### Heat Gains from Hot Water Equipment:
-
-The fuel input to the equipment ultimately appears as heat that contributes to zone loads. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Fraction Latent, Fraction Radiant and Fraction Lost. A fourth, defined as the fraction of the heat from hot water equipment convected to the zone air, is calculated by the program as:
-
-f<sub>convected</sub> = 1.0 – (Fraction Latent + Fraction Radiant + Fraction Lost)
-
-You will get an error message if Fraction Latent + Fraction Radiant + Fraction Lost exceeds 1.0.
-
-#### Field: Fraction Latent
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of latent heat given off by hot water equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by hot water equipment to give the amount of latent energy produced by the hot water equipment. This energy affects the moisture balance within the zone.
-
-#### Field: Fraction Radiant
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of long-wave radiant heat being given off by hot water equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by hot water equipment to give the amount of long wavelength radiation gain from hot water equipment in a zone.
-
-#### Field: Fraction Lost
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of “lost� heat being given off by hot water equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by hot water equipment to give the amount of heat which is “lost� and does not impact the zone energy balances. This might correspond to input energy converted to mechanical work or heat that is vented to the atmosphere.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Cooking", "Clothes Drying", etc. A new meter for reporting is created for each unique subcategory  (ref: Output:Meter obejct). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the "General" end-use subcategory.
-
-IDF Examples:
-
-```idf
-HotWaterEquipment,
-    SPACE2-1 HWEq 1,         !- Name
-    SPACE2-1,                !- Zone Name
-    EQUIP-1,                 !- SCHEDULE Name
-    EquipmentLevel,         !- Design Level calculation method
-    300,                     !- Design Level {W}
-    ,                        !- Power per Zone Floor Area {watts/m2}
-    ,                        !- Power per Person {watts/person}
-    0.2,                     !- Fraction Latent
-    0.1,                     !- Fraction Radiant
-    0.5,                     !- Fraction Lost
-    Dishwashing;             !- End-Use Subcategory
-```
-
-Global Hot Water Equipment example:
-
-```idf
-  ZoneList,OfficeZones,Left Fork, Middle Fork, Right Fork;
-
-  HotWaterEquipment,
-    Office Zones with Hot Water Equipment,       !- Name
-    OfficeZones,             !- Zone Name
-    HotWater Eq Sch,         !- Schedule Name
-    Watts/Area,              !- Design Level Calculation Method
-    ,                        !- Design Level {W}
-    50,                      !- Power per Zone Floor Area {W/m2}
-    ,                        !- Power per Person {W/Person}
-    0.0000000E+00,           !- Fraction Latent
-    0.3000000,               !- Fraction Radiant
-    0.0000000E+00;           !- Fraction Lost
-```
-
-### SteamEquipment
-
-The object models steam equipment in the zone which consumes district heating, such as cooking equipment or process loads. All of the energy consumed by the equipment becomes a heat gain in the zone or is lost (exhausted) as specified below. This object consumes district heating energy directly and does not cause a load on a steam plant loop.
-
-#### Field: Name
-
-The name of the SteamEquipment object.
-
-#### Field: Zone or ZoneList Name
-
-This field is the name of the thermal zone (ref: Zone) and attaches a particular steam equipment statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this steam equipment definition is applied to each of the zones in the zone list effecting a global definition for the amount of steam in the zone. This option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule that modifies the design level parameter for steam equipment (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The actual energy input for steam equipment in a zone as defined by this statement is the product of the design level field and the value of the schedule specified by name in this field.
-
-#### Field: Design Level Calculation Method
-
-This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal steam equipment level in the Zone. The key/choices are:
-
-- EquipmentLevel
-
-With this choice, the method used will be a straight insertion of the steam equipment level (Watts) for the Zone.  (The Design Level field should be filled.)
-
-- Watts/Area or Power/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The Power per Zone Floor Area field should be filled).
-
-- Watts/Person or Power/Person
-
-With this choice, the method used will be a factor of equipment level (watts) per person. (The Power per Person field should be filled).
-
-#### Field: Design Level
-
-This field (in Watts) is typically used to represent the maximum energy input to steam equipment in a zone that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the steam equipment design level could be a “diversity factor� applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour, the design level field is constant for all simulation environments.
-
-#### Field: Power per Zone Floor Area
-
-This factor (watts/m<sup>2</sup>) is used, along with the Zone Area to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be “**Watts/Area**� or “**Power/Area**�.
-
-#### Field: Power per Person
-
-This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum equipment level as described in the Design Level field. The choice from the method field should be “**Watts/Person**� or “**Power/Person**�.
-
-#### Heat Gains from Steam Equipment:
-
-The fuel input to the equipment ultimately appears as heat that contributes to zone loads. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Fraction Latent, Fraction Radiant and Fraction Lost. A fourth, defined as the fraction of the heat from steam equipment convected to the zone air, is calculated by the program as:
-
-f<sub>convected</sub> = 1.0 – (Fraction Latent + Fraction Radiant + Fraction Lost)
-
-You will get an error message if Fraction Latent + Fraction Radiant + Fraction Lost exceeds 1.0.
-
-#### Field: Fraction Latent
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of latent heat given off by steam equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by steam equipment to give the amount of latent energy produced by the steam equipment. This energy affects the moisture balance within the zone.
-
-#### Field: Fraction Radiant
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of long-wave radiant heat being given off by steam equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by steam equipment to give the amount of long wavelength radiation gain from steam equipment in a zone.
-
-#### Field: Fraction Lost
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of “lost� heat being given off by steam equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by steam equipment to give the amount of heat which is “lost� and does not impact the zone energy balances. This might correspond to input energy converted to mechanical work or heat that is vented to the atmosphere.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Cooking", "Clothes Drying", etc. A new meter for reporting is created for each unique subcategory  (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the "General" end-use subcategory.
-
-IDF Examples:
-
-```idf
-SteamEquipment,
-    SPACE4-1 ElecEq 1,       !- Name
-    SPACE4-1,                !- Zone Name
-    EQUIP-1,                 !- SCHEDULE Name
-    EquipmentLevel,          !- Design Level calculation method
-    1050,                    !- Design Level {W}
-    ,                        !- Power per Zone Floor Area {watts/m2}
-    ,                        !- Power per Person {watts/person}
-    0.5,                     !- Fraction Latent
-    0.3,                     !- Fraction Radiant
-    0,                       !- Fraction Lost
-    Laundry;                 !- End-Use Subcategory
-```
-
-### SwimmingPool:Indoor
-
-The Indoor Swimming Pool object is used to describe the indoor swimming pools that are exposed to the internal environment.  There are several rules that should be noted regarding the specification of an indoor pool in EnergyPlus.  First, the pool is linked to a surface that must be a floor.  The pool is assumed to cover the entire floor to which it is linked.  If the pool only covers part of the floor in the actual building, then the user must break the floor up into multiple sections.
-
-As pools attempt to achieve a particular water temperature and have a variety of heat losses, heating equipment is necessary to maintain the proper setpoint temperature.  In EnergyPlus, the pool itself becomes part of the demand side of a plant loop with heating equipment on the supply side providing whatever heating is needed to maintain the desired temperature.  This heating equipment as well as the loop connections must be entered separately and the input shown in this section only details what is needed to specify the pool itself.
-
-The following information is useful for defining and modeling an indoor pool in EnergyPlus.  For more information on the algorithm used for this model or details on some of the input parameters, please reference the indoor pool section of the EnergyPlus Engineering Reference document.
-
-#### Field: Name
-
-This is a unique name associated with the indoor swimming pool.
-
-#### Field: Surface Name
-
-This is the name of the surface (floor) where the pool is located. Pools are not allowed on any surfaces other than a floor.
-
-#### Field: Average Depth
-
-This field is the average depth of the pool in meters.  If the pool has variable depth, the average depth should be specified to achieve the proper volume of water in the pool.
-
-#### Field: Activity Factor Schedule Name
-
-This field references a schedule that contains values for pool activity.  This parameter can be varied using the schedule named here, and it has an impact on the amount of evaporation that will take place from the pool to the surrounding zone air.  For example values of the activity factor and what impact it will have on the evaporation of water from the pool, please refer to indoor swimming pool section of the EnergyPlus Engineering Reference document.  If left blank, the activity factor will be assumed to be unity.
-
-#### Field: Make-up Water Supply Schedule Name
-
-The scheduled named by this field establishes a cold water temperature [C] for the water that replaces the water which is lost from the pool due to evaporation.  If blank, water temperatures are calculated by the Site:WaterMainsTemperature object.  This field (even if blank) overrides the Cold Water Supply Temperature Schedule in all of the listed WaterUse:Equipment objects.
-
-#### Field: Cover Schedule Name
-
-This schedule defines when the pool water cover is available and affects the evaporation, convection, and radiation rate calculations. A schedule value of 0.0 means that the pool is not covered.  A schedule value of 1.0 means the pool is 100% covered.  The pool may be fully covered, fully open (uncovered), or partially covered (a value between 0.0 and 1.0).  The user also has the option to control the evaporation, convection, short-wavelength radiation, and long-wavelength radiation factors when the pool is covered.  These terms are discussed in the next four fields.
-
-#### Field: Cover Evaporation Factor
-
-This input field can optionally be used to modify the pool evaporation rate and is used in conjunction with the pool cover factor defined by the Pool Cover Schedule field (see above).  The value for this parameter can normally range from 0.0 to 1.0, where 1 means that the pool cover completely eliminates evaporation from the pool surface, 0 means the pool cover has no effect on evaporation, and fractions in between 0 and 1 result in a fractional reduction in evaporation by the pool cover.  So, if this parameter is 0.5 and the pool is 50% covered, the overall reduction in evaporation from a fully uncovered pool is 25% or 0.25.
-
-#### Field: Cover Convection Factor
-
-This input field can optionally be used to modify the pool convection rate and is used in conjunction with the pool cover factor defined by the Pool Cover Schedule field (see above).  The value for this parameter can normally range from 0.0 to 1.0, where 1 means that the pool cover completely eliminates convection from the pool surface, 0 means the pool cover has no effect on convection, and fractions in between 0 and 1 result in a fractional reduction in convection by the pool cover.  So, if this parameter is 0.5 and the pool is 50% covered, the overall reduction in convection from a fully uncovered pool is 25% or 0.25.
-
-#### Field: Cover Short-Wavelength Radiation Factor
-
-This input field can optionally be used to modify the pool short-wavelength radiation rate and is used in conjunction with the pool cover factor defined by the Pool Cover Schedule field (see above).  The value for this parameter can normally range from 0.0 to 1.0, where 1 means that the pool cover completely eliminates short-wavelength radiation from the pool surface, 0 means the pool cover has no effect on short-wavelength radiation, and fractions in between 0 and 1 result in a fractional reduction in short-wavelength radiation by the pool cover.  So, if this parameter is 0.5 and the pool is 50% covered, the overall reduction in short-wavelength radiation from a fully uncovered pool is 25% or 0.25.  Note that with radiation terms that whatever portion of the short-wavelength radiation is blocked by the cover is transferred via convection to the surrounding zone air.
-
-#### Field: Cover Long-Wavelength Radiation Factor
-
-This input field can optionally be used to modify the pool long-wavelength radiation rate and is used in conjunction with the pool cover factor defined by the Pool Cover Schedule field (see above).  The value for this parameter can normally range from 0.0 to 1.0, where 1 means that the pool cover completely eliminates long-wavelength radiation from the pool surface, 0 means the pool cover has no effect on long-wavelength radiation, and fractions in between 0 and 1 result in a fractional reduction in long-wavelength radiation by the pool cover.  So, if this parameter is 0.5 and the pool is 50% covered, the overall reduction in long-wavelength radiation from a fully uncovered pool is 25% or 0.25.  Note that with radiation terms that whatever portion of the long-wavelength radiation is blocked by the cover is transferred via convection to the surrounding zone air.
-
-#### Field: Pool Water Inlet Node
-
-This input is the name of the node on the demand side of a plant loop that leads into the pool.  From the standpoint of an EnergyPlus input file, the pool sits on a plant demand loop, and the pump and heater reside on the plant supply loop.  The pool heater and pump must be defined by other existing EnergyPlus input.
-
-#### Field: Pool Water Outlet Node
-
-This input is the name of the node on the demand side of a plant loop that leads out of the pool.  From the standpoint of an EnergyPlus input file, the pool sits on a plant demand loop, and the pump and heater reside on the plant supply loop.  The pool heater and pump must be defined by other existing EnergyPlus input.
-
-#### Field: Pool Water Maximum Flow Rate
-
-This input is the maximum water volumetric flow rate in m3/s going between the pool and the water heating equipment.  This along with the pool setpoint temperature and the heating plant equipment outlet temperature will establish the maximum heat addition to the pool.  This flow rate to the pool will be varied in an attempt to reach the desired pool water setpoint temperature (see Setpoint Temperature Schedule below).
-
-#### Field: Pool Miscellaneous Equipment Power
-
-This input defines the power consumption rate of miscellaneous equipment such as the filtering and chlorination technology associated with the pool.  The units for this input are in power consumption per flow rate of water through the pool from the heater or W/(kg/s). This field will be multiplied by the flow rate of water through the pool to determine the power consumption of this equipment. Any heat generated by this equipment is assumed to have no effect on the pool water itself.
-
-#### Field: Setpoint Temperature Schedule
-
-Pools attempt to maintain a particular water temperature.  In EnergyPlus, this field defines the setpoint temperature for the desired pool water temperature.  It is input as a schedule to allow the user to vary the pool setpoint temperature as desired.  The equipment defined to provide heating for the pool will deliver the necessary hot water to the pool, up to the capacity of that equipment defined by other input by the user.
-
-#### Field: Maximum Number of People
-
-This field defines the maximum occupancy of people actually in the pool and thus will be used with the next two inputs to determine how much heat people contribute to the pool heat balance.  People who are not in the pool should be modeled separately using the standard People description for zones.
-
-#### Field: People Schedule
-
-This field defines a schedule that establishes how many people are in the pool at any given time.  The current value of this schedule is multiplied by the maximum number of people in the previous field determines how many people are currently in the pool.
-
-#### Field: People Heat Gain Schedule
-
-This field defines the amount of heat given off by an average person in the pool in Watts.  This field is a schedule so that this heat gain can be allowed to vary as the type of activity in a pool can vary greatly and thus the amount of heat gain per person also varies.  This parameter times the number of people in the pool determines how much heat is added to the pool.  All heat given off by people is added to the heat balance of the pool water.
-
-An example of an indoor swimming pool definition is:
-
-```idf
-  SwimmingPool:Indoor,
-    Test Pool,             !- Name
-    F1-1,                  !- Surface Name
-    1.5,                   !- Average Depth {m}
-    PoolActivitySched,     !- Pool Activity Schedule
-    MakeUpWaterSched,      !- MakeUp Water Temperature Schedule
-    PoolCoverSched,        !- Pool Cover Schedule
-    0.0,                   !- Cover Evaporation Factor
-    0.2,                   !- Cover Convection Factor
-    0.9,                   !- Cover Short-Wavelength Radiation Factor
-    0.5,                   !- Cover Long-Wavelength Radiation Factor
-    Pool Water Inlet Node,    !- Water Inlet Node (Plant/Heater)
-    Pool Water Outlet Node,   !- Water Outlet Node (Plant/Heater)
-    0.1,                   !- Maximum flow rate from water heating system {m3/s}
-    0.6,                   !- Miscellaneous Equipment Power Factor
-    PoolSetpointTempSched, !- Pool Water Setpoint Temperature Schedule
-    15,                    !- Maximum Number of People in Pool
-    PoolOccupancySched,    !- Pool People Schedule
-    PoolOccHeatGainSched;  !- Pool People Heat Gain Schedule
-```
-
-### SwimmingPool:Indoor Outputs
-
-* HVAC, Average, Indoor Pool Makeup Water Rate [m3/s]
-* HVAC, Sum, Indoor Pool Makeup Water Volume [m3]
-* HVAC, Average, Indoor Pool Makeup Water Temperature [C]
-* HVAC, Average, Indoor Pool Water Temperature [C]
-* HVAC, Average, Indoor Pool Inlet Water Temperature [C]
-* HVAC, Average, Indoor Pool Inlet Water Mass Flow Rate [kg/s]
-* HVAC, Average, Indoor Pool Miscellaneous Equipment Power [W]
-* HVAC, Sum, Indoor Pool Miscellaneous Equipment Energy [J]
-* HVAC, Average, Indoor Pool Heating Rate [W]
-* HVAC, Sum, Indoor Pool Heating Energy [J]
-* HVAC, Average, Indoor Pool Radiant to Convection by Cover [W]
-* HVAC, Average, Indoor Pool People Heat Gain [W]
-* HVAC, Average, Indoor Pool Current Activity Factor []
-* HVAC, Average, Indoor Pool Current Cover Factor []
-* HVAC, Average, Indoor Pool Evaporative Heat Loss Rate [W]
-* HVAC, Sum, Indoor Pool Evaporative Heat Loss Energy [J]
-
-#### Indoor Pool Makeup Water Rate [m3/s]
-
-The water consumption rate for the makeup water of indoor swimming pool.
-
-#### Indoor Pool Makeup Water Volume [m3]
-
-The water consumption for the makeup water of indoor swimming pool.
-
-#### Indoor Pool Makeup Water Temperature [C]
-
-The temperature of the makeup water of indoor swimming pool.
-
-#### Indoor Pool Water Temperature [C]
-
-The average calculated pool water temperature during the simulation at the time frequency requested.
-
-#### Indoor Pool Inlet Water Temperature [C]
-
-The temperature of the water being sent to the pool from the plant heating equipment.
-
-#### Indoor Pool Inlet Water Mass Flow Rate [kg/s]
-
-The mass flow rate of water being sent to the pool from the plant heating equipment.  Typically this water is being passed through a heater and miscellaneous equipment.
-
-#### Indoor Pool Miscellaneous Equipment Power [W]
-
-The miscellaneous equipment power includes the power consumption of pool filter and chlorinator in Watts.
-
-#### Indoor Pool Miscellaneous Equipment Energy [J]
-
-The miscellaneous equipment power consumption includes the energy consumption of pool filter and chlorinator in Joules.
-
-#### Indoor Pool Heating Rate [W]
-
-This is the rate of heating provided by the plant loop to the pool in Watts.
-
-#### Indoor Pool Heating Energy [J]
-
-This is the amount of heating provided by the plant loop to the pool in Joules over the time step requested.
-
-#### Indoor Pool Radiant to Convection by Cover [W]
-
-The pool cover may block some or all of short- and long-wavelength radiation incident on the pool.  To account for this and to not have the cover result in energy that is not accounted for by the model, the radiation that is blocked by the cover is converted to a convective gain (or loss) to/from the zone air.  This output field reports this value.
-
-#### Indoor Pool Current Activity Factor []
-
-This is the current activity factor as defined by the user input schedule.
-
-#### Indoor Pool Current Cover Factor []
-
-This is the current cover factor as defined by the user input schedule.
-
-#### Indoor Pool Evaporative Heat Loss Rate [W]
-
-This is the rate of evaporative heat loss (latent) to the zone from the pool in Watts.
-
-#### Indoor Pool Evaporative Heat Loss Energy [J]
-
-This is the amount of evaporative heat loss (latent) to the zone from the pool in in Joules over the time step requested.
-
-### OtherEquipment
-
-Other Equipment object is provided as an additional source for heat gains or losses directly to the zone.  That is to say, a loss can be entered by putting a negative value into the Design Level field(s). Note, too, that this object does not have an end-use component – gains or losses do not show up in the bottom energy lines (except as influencing overall zone gains or losses).
-
-#### Field: Name
-
-The name of the OtherEquipment object.
-
-#### Field: Zone or ZoneList Name
-
-This field is the name of the thermal zone (ref: Zone) and attaches a particular other equipment statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this other equipment definition is applied to each of the zones in the zone list effecting a global definition for the amount of other in the zone. This option can be used effectively with the watts/area and watts/person options of the Design Level Calculation Method.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule that modifies the design level parameter for other equipment (see Design Level Calculation Method field and related subsequent fields). The schedule values can be any positive number. The actual energy input for other equipment in a zone as defined by this statement is the product of the design level field and the value of the schedule specified by name in this field.
-
-#### Field: Design Level Calculation Method
-
-This field is a key/choice field that tells which of the next three fields are filled and is descriptive of the method for calculating the nominal other equipment level in the Zone. The key/choices are:
-
-- EquipmentLevel
-
-With this choice, the method used will be a straight insertion of the other equipment level (Watts) for the Zone.  (The Design Level field should be filled.)
-
-- Watts/Area or Power/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The Power per Zone Floor Area field should be filled).
-
-- Watts/Person or Power/Person
-
-With this choice, the method used will be a factor of equipment level (watts) per person. (The Power per Person field should be filled).
-
-#### Field: Design Level
-
-This field (in Watts) is typically used to represent the maximum energy input to other equipment in a zone that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the other equipment design level could be a “diversity factor� applied to a schedule of real numbers. This value can be negative to denote a loss. Note that while the schedule value can vary from hour to hour, the design level field is constant for all simulation environments.
-
-#### Field: Power per Zone Floor Area
-
-This factor (watts/m<sup>2</sup>) is used, along with the Zone Area to determine the maximum equipment level as described in the Design Level field. This value can be negative to denote a loss. The choice from the method field should be “**Watts/Area**� or “**Power/Area**�.
-
-#### Field: Power per Person
-
-This factor (watts/person) is used, along with the number of occupants (people) to determine the maximum equipment level as described in the Design Level field. This value can be negative to denote a loss. The choice from the method field should be “**Watts/Person**� or “**Power/Person**�.
-
-#### Heat Gains/Losses from Other Equipment:
-
-The fuel input to the equipment ultimately appears as heat that contributes to zone loads. In EnergyPlus this heat is divided into four different fractions. Three of these are given by the input fields Fraction Latent, Fraction Radiant and Fraction Lost. A fourth, defined as the fraction of the heat from other equipment convected to the zone air, is calculated by the program as:
-
-f<sub>convected</sub> = 1.0 – (Fraction Latent + Fraction Radiant + Fraction Lost)
-
-You will get an error message if Fraction Latent + Fraction Radiant + Fraction Lost exceeds 1.0.
-
-#### Field: Fraction Latent
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of latent heat given off by other equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by other equipment to give the amount of latent energy produced by the other equipment. This energy affects the moisture balance within the zone.
-
-#### Field: Fraction Radiant
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of long-wave radiant heat being given off by other equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by other equipment to give the amount of long wavelength radiation gain from other equipment in a zone.
-
-#### Field: Fraction Lost
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the amount of “lost� heat being given off by other equipment in a zone. The number specified in this field will be multiplied by the total energy consumed by other equipment to give the amount of heat which is “lost� and does not impact the zone energy balances. This might correspond to input energy converted to mechanical work or heat that is vented to the atmosphere.
-
-IDF Examples
-
-```idf
-OtherEquipment,
-    BASE-1 OthEq 1,          !- Name
-    BASE-1,                  !- Zone Name
-    ALWAYSON,                !- SCHEDULE Name
-    EquipmentLevel,          !- Design Level calculation method
-    6766.,                   !- Design Level {W}
-    ,                        !- Power per Zone Floor Area {watts/m2}
-    ,                        !- Power per Person {watts/person}
-    0,                       !- Fraction Latent
-    0.3,                     !- Fraction Radiant
-    0;                       !- Fraction Lost
-```
-
-### Electric, Gas, Other, HotWater, Steam Equipment Outputs
-
-Each type of equipment object has output variables for individual objects and for zone totals.
-
-Electric Equipment
-
-* Zone,Average,Electric Equipment Electric Power [W]
-
-* Zone,Sum,Electric Equipment Electric Energy [J]
-
-* Zone,Sum,Electric Equipment Radiant Heating Energy [J]
-
-* Zone,Average,Electric Equipment Radiant Heating Rate [W]
-
-* Zone,Sum,Electric Equipment Convective Heating Energy [J]
-
-* Zone,Average,Electric Equipment Convective Heating Rate [W]
-
-* Zone,Sum,Electric Equipment Latent Gain Energy [J]
-
-* Zone,Average,Electric Equipment Latent Gain Rate [W]
-
-* Zone,Sum,Electric Equipment Lost Heat Energy [J]
-
-* Zone,Average,Electric Equipment Lost Heat Rate [W]
-
-* Zone,Sum,Electric Equipment Total Heating Energy [J]
-
-* Zone,Average,Electric Equipment Total Heating Rate [W]
-
-* Zone,Average,Zone Electric Equipment Electric Power [W]
-
-* Zone,Sum,Zone Electric Equipment Electric Energy [J]
-
-* Zone,Sum,Zone Electric Equipment Radiant Heating Energy [J]
-
-* Zone,Average,Zone Electric Equipment Radiant Heating Rate [W]
-
-* Zone,Sum,Zone Electric Equipment Convective Heating Energy [J]
-
-* Zone,Average,Zone Electric Equipment Convective Heating Rate [W]
-
-* Zone,Sum,Zone Electric Equipment Latent Gain Energy [J]
-
-* Zone,Average,Zone Electric Equipment Latent Gain Rate [W]
-
-* Zone,Sum,Zone Electric Equipment Lost Heat Energy [J]
-
-* Zone,Average,Zone Electric Equipment Lost Heat Rate [W]
-
-* Zone,Sum,Zone Electric Equipment Total Heating Energy [J]
-
-* Zone,Average,Zone Electric Equipment Total Heating Rate [W]
-
-
-
-
-**Gas Equipment**
-
-* Zone,Average,Gas Equipment Gas Rate [W]
-
-* Zone,Sum,Gas Equipment Gas Energy [J]
-
-* Zone,Sum,Gas Equipment Radiant Heating Energy [J]
-
-* Zone,Sum,Gas Equipment Convective Heating Energy [J]
-
-* Zone,Sum,Gas Equipment Latent Gain Energy [J]
-
-* Zone,Sum,Gas Equipment Lost Heat Energy [J]
-
-* Zone,Sum,Gas Equipment Total Heating Energy [J]
-
-* Zone,Average,Gas Equipment Radiant Heating Rate [W]
-
-* Zone,Average,Gas Equipment Convective Heating Rate [W]
-
-* Zone,Average,Gas Equipment Latent Gain Rate [W]
-
-* Zone,Average,Gas Equipment Lost Heat Rate [W]
-
-* Zone,Average,Gas Equipment Total Heating Rate [W]
-
-* Zone,Average,Zone Gas Equipment Gas Rate [W]
-
-* Zone,Sum,Zone Gas Equipment Gas Energy [J]
-
-* Zone,Sum,Zone Gas Equipment Radiant Heating Energy [J]
-
-* Zone,Average,Zone Gas Equipment Radiant Heating Rate [W]
-
-* Zone,Sum,Zone Gas Equipment Convective Heating Energy [J]
-
-* Zone,Average,Zone Gas Equipment Convective Heating Rate [W]
-
-* Zone,Sum,Zone Gas Equipment Latent Gain Energy [J]
-
-* Zone,Average,Zone Gas Equipment Latent Gain Rate [W]
-
-* Zone,Sum,Zone Gas Equipment Lost Heat Energy [J]
-
-* Zone,Average,Zone Gas Equipment Lost Heat Rate [W]
-
-* Zone,Sum,Zone Gas Equipment Total Heating Energy [J]
-
-* Zone,Average,Zone Gas Equipment Total Heating Rate [W]
-
-
-
-
-**HotWater Equipment**
-
-* Zone,Average,Hot Water Equipment District Heating Rate [W]
-
-* Zone,Sum,Hot Water Equipment District Heating Energy [J]
-
-* Zone,Sum,Hot Water Equipment Radiant Heating Energy [J]
-
-* Zone,Average,Hot Water Equipment Radiant Heating Rate [W]
-
-* Zone,Sum,Hot Water Equipment Convective Heating Energy [J]
-
-* Zone,Average,Hot Water Equipment Convective Heating Rate [W]
-
-* Zone,Sum,Hot Water Equipment Latent Gain Energy [J]
-
-* Zone,Average,Hot Water Equipment Latent Gain Rate [W]
-
-* Zone,Sum,Hot Water Equipment Lost Heat Energy [J]
-
-* Zone,Average,Hot Water Equipment Lost Heat Rate [W]
-
-* Zone,Sum,Hot Water Equipment Total Heating Energy [J]
-
-* Zone,Average,Hot Water Equipment Total Heating Rate [W]
-
-* Zone,Average,Zone Hot Water Equipment District Heating Rate [W]
-
-* Zone,Sum,Zone Hot Water Equipment District Heating Energy [J]
-
-* Zone,Sum,Zone Hot Water Equipment Radiant Heating Energy [J]
-
-* Zone,Average,Zone Hot Water Equipment Radiant Heating Rate [W]
-
-* Zone,Sum,Zone Hot Water Equipment Convective Heating Energy [J]
-
-* Zone,Average,Zone Hot Water Equipment Convective Heating Rate [W]
-
-* Zone,Sum,Zone Hot Water Equipment Latent Gain Energy [J]
-
-* Zone,Average,Zone Hot Water Equipment Latent Gain Rate [W]
-
-* Zone,Sum,Zone Hot Water Equipment Lost Heat Energy [J]
-
-* Zone,Average,Zone Hot Water Equipment Lost Heat Rate [W]
-
-* Zone,Sum,Zone Hot Water Equipment Total Heating Energy [J]
-
-* Zone,Average,Zone Hot Water Equipment Total Heating Rate [W]
-
-
-
-
-**Steam Equipment**
-
-* Zone,Average,Steam Equipment District Heating Rate [W]
-
-* Zone,Sum,Steam Equipment District Heating Energy [J]
-
-* Zone,Sum,Steam Equipment Radiant Heating Energy [J]
-
-* Zone,Average,Steam Equipment Radiant Heating Rate [W]
-
-* Zone,Sum,Steam Equipment Convective Heating Energy [J]
-
-* Zone,Average,Steam Equipment Convective Heating Rate [W]
-
-* Zone,Sum,Steam Equipment Latent Gain Energy [J]
-
-* Zone,Average,Steam Equipment Latent Gain Rate [W]
-
-* Zone,Sum,Steam Equipment Lost Heat Energy [J]
-
-* Zone,Average,Steam Equipment Lost Heat Rate [W]
-
-* Zone,Sum,Steam Equipment Total Heating Energy [J]
-
-* Zone,Average,Steam Equipment Total Heating Rate [W]
-
-* Zone,Average,Zone Steam Equipment District Heating Rate [W]
-
-* Zone,Sum,Zone Steam Equipment District Heating Energy [J]
-
-* Zone,Sum,Zone Steam Equipment Radiant Heating Energy [J]
-
-* Zone,Average,Zone Steam Equipment Radiant Heating Rate [W]
-
-* Zone,Sum,Zone Steam Equipment Convective Heating Energy [J]
-
-* Zone,Average,Zone Steam Equipment Convective Heating Rate [W]
-
-* Zone,Sum,Zone Steam Equipment Latent Gain Energy [J]
-
-* Zone,Average,Zone Steam Equipment Latent Gain Rate [W]
-
-* Zone,Sum,Zone Steam Equipment Lost Heat Energy [J]
-
-* Zone,Average,Zone Steam Equipment Lost Heat Rate [W]
-
-* Zone,Sum,Zone Steam Equipment Total Heating Energy [J]
-
-* Zone,Average,Zone Steam Equipment Total Heating Rate [W]
-
-
-
-
-**Other Equipment**
-
-* Zone,Sum,Other Equipment Radiant Heating Energy [J]
-
-* Zone,Average,Other Equipment Radiant Heating Rate [W]
-
-* Zone,Sum,Other Equipment Convective Heating Energy [J]
-
-* Zone,Average,Other Equipment Convective Heating Rate [W]
-
-* Zone,Sum,Other Equipment Latent Gain Energy [J]
-
-* Zone,Average,Other Equipment Latent Gain Rate [W]
-
-* Zone,Sum,Other Equipment Lost Heat Energy [J]
-
-* Zone,Average,Other Equipment Lost Heat Rate [W]
-
-* Zone,Sum,Other Equipment Total Heating Energy [J]
-
-* Zone,Average,Other Equipment Total Heating Rate [W]
-
-* Zone,Sum,Zone Other Equipment Radiant Heating Energy [J]
-
-* Zone,Average,Zone Other Equipment Radiant Heating Rate [W]
-
-* Zone,Sum,Zone Other Equipment Convective Heating Energy [J]
-
-* Zone,Average,Zone Other Equipment Convective Heating Rate [W]
-
-* Zone,Sum,Zone Other Equipment Latent Gain Energy [J]
-
-* Zone,Average,Zone Other Equipment Latent Gain Rate [W]
-
-* Zone,Sum,Zone Other Equipment Lost Heat Energy [J]
-
-* Zone,Average,Zone Other Equipment Lost Heat Rate [W]
-
-* Zone,Sum,Zone Other Equipment Total Heating Energy [J]
-
-* Zone,Average,Zone Other Equipment Total Heating Rate [W]
-
-
-#### Electric Equipment Electric Power [W]
-
-#### Electric Equipment Electric Energy [J]
-
-The electric equipment electric power consumption in Watts (for power) or Joules (for energy). It is the sum of the radiant, convective, latent and lost components. This energy use is added to the electricity meters that are associated with the zone – Electricity:Facility, Electricity:Buidling, Electricity:Zone:&lt;Zone Name&gt;, InteriorEquipment:Electricity: :Zone:&lt;Zone Name&gt;, and &lt;End-Use Subcategory&gt;:InteriorEquipment:Electricity.
-
-#### Gas Equipment Gas Rate [W]
-
-#### Gas Equipment Gas Energy [J]
-
-The gas equipment natural gas consumption in Watts (for power) or Joules (for energy). It is the sum of the radiant, convective, latent and lost components. This energy use is added to the electricity meters that are associated with the zone – Gas:Facility, Gas:Buidling, Gas:Zone:&lt;Zone Name&gt;, InteriorEquipment:Gas: :Zone:&lt;Zone Name&gt;, and &lt;End-Use Subcategory&gt;:InteriorEquipment:Gas.
-
-#### Hot Water Equipment District Heating Rate [W]
-
-#### Hot Water Equipment District Heating Energy [J]
-
-The hot water equipment district heating consumption in Watts (for power) or Joules (for energy). It is the sum of the radiant, convective, latent and lost components. This energy use is added to the district heating meters that are associated with the zone – DistrictHeating:Facility, DistrictHeating:Buidling, DistrictHeating:Zone:&lt;Zone Name&gt;, InteriorEquipment: DistrictHeating: :Zone:&lt;Zone Name&gt;, and &lt;End-Use Subcategory&gt;:InteriorEquipment: DistrictHeating.
-
-#### Steam Equipment District Heating Rate [W]
-
-#### Steam Equipment District Heating Energy [J]
-
-The steam equipment district heating consumption in Watts (for power) or Joules (for energy). It is the sum of the radiant, convective, latent and lost components. This energy use is added to the district heating meters that are associated with the zone – DistrictHeating:Facility, DistrictHeating:Buidling, DistrictHeating:Zone:&lt;Zone Name&gt;, InteriorEquipment: DistrictHeating: :Zone:&lt;Zone Name&gt;, and &lt;End-Use Subcategory&gt;:InteriorEquipment: DistrictHeating.
-
-Note that zone energy consumption is not reported for OTHER EQUIPMENT and does not go on any meter.
-
-### ElectricEquipment:ITE:AirCooled
-
-This object describes air-cooled electric information technology equipment (ITE) which has variable power consumption as a function of loading and temperature.
-
-#### Field: Name
-
-The name of this object.
-
-#### Field: Zone Name
-
-This field is the name of the thermal zone (ref: Zone) which contains this ElectricEquipment:ITE:AirCooled object.
-
-#### Field: Design Power Input Calculation Method
-
-This field is a key/choice field that tells which of the next two fields are filled and is descriptive of the method for calculating the nominal electric power input to the ITE. The key/choices are:
-
-Watts/Unit
-
-With this choice, the design power input will be the product of Design Level per Unit and Number of Units. (Both of these fields should be filled.) This is the default.
-
-Watts/Area
-
-With this choice, the design power input will be a factor per floor area of the zone. (The Watts per Zone Floor Area field should be filled).
-
-#### Field: Watts per Unit
-
-This field (in Watts) is typically used to represent the design electrical power input to the ITE when fully loaded and the entering air temperatures is at the specified design value. This field is used if the choice from the method field is “EquipmentLevel�.
-
-#### Field: Number of Units
-
-This field is multiplied times the Design Level per Unit to determine the design electrical power input to this ITE object when fully loaded and the entering air temperature is at the specified design value. This field is used if the choice from the method field is “EquipmentLevel�. The default is 1.
-
-#### Field: Watts per Zone Floor Area
-
-This factor (Watts/m2) is used, along with the Zone Area to determine the design electrical power input as described in the Design Level field above. This field is used if the choice from the method field is “Watts/Area�.
-
-#### Field: Design Power Input Schedule Name
-
-This field is the name of the operating schedule that modifies the design level power input for this equipment This schedule specifies the fraction (typically 0.0 to 1.0) of this equipment which is available (powered up), regardless of CPU utilization. If this field is blank, the schedule is assumed to always be 1.0.
-
-#### Field: CPU Loading Schedule Name
-
-This field is the name of the schedule that specifies the CPU loading for this equipment as a fraction from 0.0 (idle) to 1.0 (full load). If this field is blank, the schedule is assumed to always be 1.0.
-
-#### Field: CPU Power Input Function of Loading and Air Temperature Curve Name
-
-The name of a two-variable curve or table lookup object which modifies the CPU power input as a function of CPU loading (x) and air inlet node temperature (y). This curve (table) should equal 1.0 at design conditions (CPU loading = 1.0 and Design Entering Air Temperature).
-
-#### Field: Design Fan Power Input Fraction
-
-This field is a decimal number between 0.0 and 1.0 and is used to specify the fraction of the total power input at design conditions which is for the cooling fan(s). If fan power data is not available, set this fraction to 0.0. The default is 0.0.
-
-#### Field: Design Fan Air Flow Rate per Power Input
-
-Specifies the cooling fan air flow rate in m3/s per Watt of total electric power input at design conditions (CPU loading = 1.0 and Design Entering Air Temperature).
-
-This is normalized by power input to allow the design power input to be changed without needing to change this value.  
-
-#### Field: Air Flow Function of Loading and Air Temperature Curve Name
-
-The name of a two-variable curve or table lookup object which modifies the cooling air flow rate as a function of CPU loading (x) and air inlet node temperature (y). This curve (table) should equal 1.0 at design conditions (CPU loading = 1.0 and Design Entering Air Temperature).
-
-#### Field: Fan Power Input Function of Flow Curve Name
-
-The name of a single-variable curve or table lookup object which modifies the fan power input as a function of airflow fraction (x). This curve (table) should equal 1.0 at the design air flow rate (flow fraction = 1.0).
-
-#### Field: Design Entering Air Temperature
-
-Specifies the entering air temperature in deg. C at design conditions. The default is 15C.
-
-#### Field: Environmental Class
-
-Specifies the allowable operating conditions for the air inlet conditions. The available inputs are A1, A2, A3, A4, B, C, or None. This is used to report the “ITE Air Inlet Operating Range Exceeded Time� If None is specified (the default), then no reporting of time outside allowable conditions will be done.
-
-#### Field: Air Inlet Connection Type
-
-Specifies the type of connection between the zone and the ITE air inlet node. The choices are:
-
-AdjustedSupply = This option is used to apply a recirculation adjustment to the ITE inlet conditions. If this option is specified, then the Supply Air Node Name is required and the air inlet temperature to the ITE will be the current supply air node temperature adjusted by the current recirculation fraction. All heat output is added to the zone air heat balance as a convective gain. AdjustedSupply is the default.
-
-ZoneAirNode = This option is used if there is no containment and the ITE air inlet node is at the average zone condition. All heat output is added to the zone air heat balance as a convective gain. 
-
-RoomAirModel = This option connects the ITE air inlet and outlet nodes to a room air model (Ref. RoomAirModelType and RoomAir:Node). 
-
-#### Field: Air Inlet Room Air Model Node Name
-
-Specifies the name of a room air model node (ref. RoomAir:Node) which is the air inlet to this equipment.  This field is required if the Air Node Connection Type = RoomAirModel.
-
-#### Field: Air Outlet Room Air Model Node Name
-
-Specifies the node name of a room air model node (ref. RoomAir:Node) which is the air outlet from this equipment. This field is required if the Air Node Connection Type = RoomAirModel.
-
-#### Field: Supply Air Node Name
-
-Specifies the node name of the supply air inlet node service this ITE. If the Air Node Connection Type = AdjustedSupply ,then this field is required, and the conditions at this node will be used to determine the ITE air inlet conditions. This field is also required if reporting of the Supply Heat Index is desired.
-
-#### Field: Design Recirculation Fraction
-
-Specifies the recirculation fraction for this equipment at design conditions. This field is used only if the Air Node Connection Type = AdjustedSupply. The recirculation fraction is defined as the ratio of recirculated air flow to total air flow entering the ITE. Recirculation is dependent upon many factors including rack and containment configuration. The default is 0.0 (no recirculation).
-
-#### Field: Recirculation Function of Loading and Supply Temperature Curve Name
-
-The name of a two-variable curve or table lookup object which modifies the Design Recirculation Fraction as a function of CPU loading (x) and supply air node temperature (y). This curve (table) should equal 1.0 at design conditions (CPU loading = 1.0 and Design Entering Air Temperature). This field is used only if the Air Node Connection Type = AdjustedSupply. If this curve is left blank, then the curve is assumed to always equal 1.0.
-
-#### Field: Design Electric Power Supply Efficiency
-
-This field is a decimal number used to specify the efficiency of the power supply system serving this ITE. The default is 1.0.
-
-#### Field: Electric Power Supply Efficiency Function of Part Load Ratio Curve Name
-
-The name of a single-variable curve or table lookup object which modifies the electric power supply efficiency as a function of part load ratio (x). This curve (table) should equal 1.0 at the design power consumption (part load ratio = 1.0). If this curve is left blank, then the curve is assumed to always equal 1.0.
-
-#### Field: Fraction of Electric Power Supply Losses to Zone
-
-This field is a decimal number between 0.0 and 1.0 and is used to specify the fraction of the electric power supply losses which are a heat gain to the zone containing the ITE. If this value is less than 1.0, the remainder of the losses are assumed to be lost to the outdoors. The default is 1.0.
-
-#### Field: CPU End-Use Subcategory
-
-This equipment is metered on the Interior Equipment end-use category for Electricity.  This field allows you to specify a user-defined end-use subcategory for the CPU power consumption. A new meter for reporting is created for each unique subcategory (ref: Output:Meter object). Subcategories are also reported in the ABUPS table. The default is ITE-CPU.
-
-#### Field: Fan End-Use Subcategory
-
-This equipment is metered on the Interior Equipment end-use category for Electricity.  This field allows you to specify a user-defined end-use subcategory for the fan power consumption. A new meter for reporting is created for each unique subcategory (ref: Output:Meter object). Subcategories are also reported in the ABUPS table.  The default is ITE-Fans
-
-#### Field: Electric Power Supply End-Use Subcategory
-
-This equipment is metered on the Interior Equipment end-use category for Electricity.  This field allows you to specify a user-defined end-use subcategory for the electric power supply power consumption. A new meter for reporting is created for each unique subcategory (ref: Output:Meter object). Subcategories are also reported in the ABUPS table. The default is ITE-UPS
-
-An IDF example:
-
-```idf
-ElectricEquipment:ITE:AirCooled,
-    Data Center Servers,     !- Name
-    Main Zone,               !- Zone Name
-    Watts/Unit,              !- Design Power Input Calculation Method
-    500,                     !- Watts per Unit {W}
-    200,                     !- Number of Units
-    ,                        !- Watts per Zone Floor Area {W/m2}
-    Data Center Operation Schedule,  !- Design Power Input Schedule Name
-    Data Center CPU Loading Schedule,  !- CPU Loading  Schedule Name
-    Model 5250 Power fLoadTemp,  !- CPU Power Input Function of Loading and Air Temperature Curve Name
-    0.4,                     !- Design Fan Power Input Fraction
-    0.0001,                  !- Design Fan Air Flow Rate per Power Input {m3/s-W}
-    Model 5250 AifFlow fLoadTemp,  !- Air Flow Function of Loading and Air Temperature Curve Name
-    ECM FanPower fFlow,      !- Fan Power Input Function of Flow Curve Name
-    15,                      !- Design Entering Air Temperature {C}
-    A3,                      !- Environmental Class
-    AdjustedSupply,          !- Air Inlet Connection Type
-    ,                        !- Air Inlet Room Air Model Node Name
-    ,                        !- Air Outlet Room Air Model Node Name
-    Main Zone Inlet Node,    !- Supply Air Node Name
-    0.1,                     !- Design Recirculation Fraction
-    Data Center Recirculation fLoadTemp,  !- Recirculation Function of Loading and Supply Temperature Curve Name
-    0.9,                     !- Design Electric Power Supply Efficiency
-    UPS Efficiency fPLR,     !- Electric Power Supply Efficiency Function of Part Load Ratio Curve Name
-    1,                       !- Fraction of Electric Power Supply Losses to Zone
-    ITE-CPU,                 !- CPU End-Use Subcategory
-    ITE-Fans,                !- Fan End-Use Subcategory
-    ITE-UPS;                 !- Electric Power Supply End-Use Subcategory
-```
-
-ElectricEquipment:ITE:AirCooled Outputs
-
-* Zone,Average,ITE CPU Electric Power [W]
-* Zone,Average,ITE Fan Electric Power [W]
-* Zone,Average,ITE UPS Electric Power [W]
-* Zone,Average,ITE CPU Electric Power at Design Inlet Conditions [W]
-* Zone,Average,ITE Fan Electric Power at Design Inlet Conditions [W]
-* Zone,Average,ITE UPS Heat Gain to Zone Rate [W]
-* Zone,Average,ITE Total Heat Gain to Zone Rate [W]
-* Zone,Sum,ITE CPU Electric Energy [J]
-* Zone,Sum,ITE Fan Electric Energy [J]
-* Zone,Sum,ITE UPS Electric Energy [J]
-* Zone,Sum,ITE CPU Electric Energy at Design Inlet Conditions [J]
-* Zone,Sum,ITE Fan Electric Energy at Design Inlet Conditions [J]
-* Zone,Sum,ITE UPS Heat Gain to Zone Energy [J]
-* Zone,Sum,ITE Total Heat Gain to Zone Energy [J]
-* Zone,Average,ITE Standard Density Air Volume Flow Rate [m3/s]
-* Zone,Average,ITE Current Density Air Volume Flow Rate [m3/s]
-* Zone,Average,ITE Air Mass Flow Rate [kg/s]
-* Zone,Average,ITE Air Inlet Dry-Bulb Temperature [C]
-* Zone,Average,ITE Air Inlet Dewpoint Temperature [C]
-* Zone,Average,ITE Air Inlet Relative Humidity [%]
-* Zone,Average,ITE Air Outlet Dry-Bulb Temperature [C]
-* Zone,Average,ITE Supply Heat Index []
-* Zone,Sum,ITE Air Inlet Operating Range Exceeded Time [hr]
-* Zone,Sum,ITE Air Inlet Dry-Bulb Temperature Above Operating Range Time [hr]
-* Zone,Sum,ITE Air Inlet Dry-Bulb Temperature Below Operating Range Time [hr]
-* Zone,Sum,ITE Air Inlet Dewpoint Temperature Above Operating Range Time [hr]
-* Zone,Sum,ITE Air Inlet Dewpoint Temperature Below Operating Range Time [hr]
-* Zone,Sum,ITE Air Inlet Relative Humidity Above Operating Range Time [hr]
-* Zone,Sum,ITE Air Inlet Relative Humidity Below Operating Range Time [hr]
-* Zone,Average,ITE Air Inlet Dry-Bulb Temperature Difference Above Operating Range [deltaC]
-* Zone,Average,ITE Air Inlet Dry-Bulb Temperature Difference Below Operating Range [deltaC]
-* Zone,Average,ITE Air Inlet Dewpoint Temperature Difference Above Operating Range [deltaC]
-* Zone,Average,ITE Air Inlet Dewpoint Temperature Difference Below Operating Range [deltaC]
-* Zone,Average,ITE Air Inlet Relative Humidity Difference Above Operating Range [%]
-* Zone,Average,ITE Air Inlet Relative Humidity Difference Below Operating Range [%]
-* Zone,Average,Zone ITE CPU Electric Power [W]
-* Zone,Average,Zone ITE Fan Electric Power [W]
-* Zone,Average,Zone ITE UPS Electric Power [W]
-* Zone,Average,Zone ITE CPU Electric Power at Design Inlet Conditions [W]
-* Zone,Average,Zone ITE Fan Electric Power at Design Inlet Conditions [W]
-* Zone,Average,Zone ITE UPS Heat Gain to Zone Rate [W]
-* Zone,Average,Zone ITE Total Heat Gain to Zone Rate [W]
-* Zone,Sum,Zone ITE CPU Electric Energy [J]
-* Zone,Sum,Zone ITE Fan Electric Energy [J]
-* Zone,Sum,Zone ITE UPS Electric Energy [J]
-* Zone,Sum,Zone ITE CPU Electric Energy at Design Inlet Conditions [J]
-* Zone,Sum,Zone ITE Fan Electric Energy at Design Inlet Conditions [J]
-* Zone,Sum,Zone ITE UPS Heat Gain to Zone Energy [J]
-* Zone,Sum,Zone ITE Total Heat Gain to Zone Energy [J]
-* Zone,Average,Zone ITE Standard Density Air Volume Flow Rate [m3/s]
-* Zone,Average,Zone ITE Air Mass Flow Rate [kg/s]
-* Zone,Average,Zone ITE Average Supply Heat Index []
-* Zone,Sum,Zone ITE Any Air Inlet Operating Range Exceeded Time [hr]
-* Zone,Sum,Zone ITE Any Air Inlet Dry-Bulb Temperature Above Operating Range Time [hr]
-* Zone,Sum,Zone ITE Any Air Inlet Dry-Bulb Temperature Below Operating Range Time [hr]
-* Zone,Sum,Zone ITE Any Air Inlet Dewpoint Temperature Above Operating Range Time [hr]
-* Zone,Sum,Zone ITE Any Air Inlet Dewpoint Temperature Below Operating Range Time [hr]
-* Zone,Sum,Zone ITE Any Air Inlet Relative Humidity Above Operating Range Time [hr]
-* Zone,Sum,Zone ITE Any Air Inlet Relative Humidity Below Operating Range Time [hr]
-
-#### Zone ITE CPU Electric Power [W]
-
-ITE CPU Electric Power [W]
-
-#### Zone ITE CPU Electric Energy [J]
-
-#### ITE CPU Electric Energy [J]
-
-The electric power (or energy) input to the ITE equipment CPU (total power input less cooling fan power). The ITE CPU Electric Energy output is also added to a meter object with Resource Type = Electricity, End Use Key = InteriorEquipment, Group Key = Building (Ref. Output:Meter object).
-
-#### Zone ITE CPU Electric Power at Design Inlet Conditions [W]
-
-#### ITE CPU Electric Power at Design Inlet Conditions [W]
-
-#### Zone ITE CPU Electric Energy at Design Inlet Conditions [J]
-
-#### ITE CPU Electric Energy at Design Inlet Conditions [J]
-
-The electric power (or energy) input to the ITE equipment CPU (total power input less cooling fan power) if the air inlet temperature were held at the design condition. May be used to calculate “IT efficiency�, the ratio of (IT energy consumed in the facility) / (IT energy that would have been consumed in the facility if the ITE were held at the reference temperature).
-
-#### Zone ITE Fan Electric Power [W]
-
-#### ITE Fan Electric Power [W]
-
-#### Zone ITE Fan Electric Energy [J]
-
-#### ITE Fan Electric Energy [J]
-
-The electric power (or energy) input to the ITE cooling fan. The ITE Fan Electric Energy output is also added to a meter object with Resource Type = Electricity, End Use Key = InteriorEquipment, Group Key = Building (Ref. Output:Meter object).
-
-#### Zone ITE Fan Electric Power at Design Inlet Conditions [W]
-
-#### ITE Fan Electric Power at Design Inlet Conditions [W]
-
-#### Zone ITE Fan Electric Energy at Design Inlet Conditions [J]
-
-#### ITE Fan Electric Energy at Design Inlet Conditions [J]
-
-The electric power (or energy) input to the ITE cooling fan if the air inlet temperature were held at the design condition. May be used to calculate “IT efficiency�, the ratio of (IT energy consumed in the facility) / (IT energy that would have been consumed in the facility if the ITE were held at the reference temperature).
-
-#### Zone ITE UPS Electric Power [W]
-
-#### ITE UPS Electric Power [W]
-
-#### Zone ITE UPS Electric Energy [J]
-
-#### ITE UPS Electric Energy [J]
-
-The net electric power (or energy) input to the ITE equipment UPS (total power input less power delivered to ITE). The ITE UPS Electric Energy output is also added to a meter object with Resource Type = Electricity, End Use Key = InteriorEquipment, Group Key = Building (Ref. Output:Meter object).
-
-#### Zone ITE UPS Heat Gain to Zone Rate [W]
-
-#### ITE UPS Heat Gain to Zone Rate [W]
-
-#### Zone ITE UPS Heat Gain to Zone Energy [J]
-
-#### ITE UPS Heat Gain to Zone Energy [J]
-
-The heat gain rate (or energy) to the zone from the UPS.
-
-#### Zone ITE Total Heat Gain to Zone Rate [W]
-
-#### ITE Total Heat Gain to Zone Rate [W]
-
-#### Zone ITE Total Heat Gain to Zone Energy [J]
-
-#### ITE Total Heat Gain to Zone Energy [J]
-
-The heat gain rate (or energy) to the zone from the UPS and from the CPU and fans if the ITE. Air Inlet Connection Type is AdjustedSupply or ZoneAirNode.  If RoomAirModel is selected, then only the heat gain from the UPS is added directly to the zone air heat balance, the heat gain from the CPU and fans will be added to the ITE air Outlet Room Air Model Node
-
-#### Zone ITE Standard Density Air Volume Flow Rate [m3/s]
-
-#### ITE Standard Density Air Volume Flow Rate [m3/s]
-
-Reports the average air volume flow rate through the ITE over the reporting interval.  Standard density in EnergyPlus corresponds to 20ºC dry bulb, dry air, and nominally adjusted for elevation.  
-
-#### Zone ITE Current Density Air Volume Flow Rate [m3/s]
-
-#### ITE Current Density Air Volume Flow Rate [m3/s]
-
-Reports the average air volume flow rate through the ITE over the reporting interval, calculated using the current density at the air inlet node.  
-
-#### Zone ITE Air Mass Flow Rate [kg/s]
-
-#### ITE Air Mass Flow Rate [kg/s]
-
-Reports the average air mass flow rate through the ITE over the reporting interval, calculated using the current density at the air inlet node.  
-
-#### ITE Air Inlet Dry-Bulb Temperature [C]
-
-The dry-bulb temperature of the air entering the ITE.
-
-#### ITE Air Inlet Dewpoint Temperature [C]
-
-The dewpoint temperature of the air entering the ITE.
-
-#### ITE Air Inlet Relative Humidity [%]
-
-The dewpoint temperature of the air entering the ITE.
-
-#### ITE Air Outlet Dry-Bulb Temperature [C]
-
-The dry-bulb temperature of the air leaving the ITE.
-
-#### Zone ITE Average Supply Heat Index []
-
-#### ITE Supply Heat Index []
-
-The supply heat index (SHI) for this equipment. SHI is a dimensionless measure of recirculation of hot air into the cold air intake of the ITE. SHI = (Tin – Tsupply)/(Tout-Tsupply) where Tin is the dry-bulb temperature of the air entering the ITE, Tout is the dry-bulb temperature of the air leaving the ITE, and Tsupply is the dry-bulb temperature at the Supply Air Node. If a Supply Air Node Name is not specified for this object, then this output will not be reported.
-
-#### Zone ITE Any Air Inlet Operating Range Exceeded Time [hr]
-
-#### ITE Air Inlet Operating Range Exceeded Time [hr]
-
-Hours when the dry-bulb and/or dewpoint temperature of the air entering the ITE is outside the range specified by the ITE Environmental Class.
-
-#### Zone ITE Any Air Inlet Dry-Bulb Temperature Above Operating Range Time [hr]
-
-#### ITE Air Inlet Dry-Bulb Temperature Above Operating Range Time [hr]
-
-Hours when the dry-bulb temperature of the air entering the ITE is above the range specified by the ITE Environmental Class.
-
-#### ITE Air Inlet Dry-Bulb Temperature Difference Above Operating Range [deltaC]
-
-The temperature difference (in degrees DeltaC) between the air inlet dry-bulb temperature and the maximum allowable dry-bulb temperature specified by the ITE Environmental Class. Only positive values are reported. When the dry-bulb temperature of the air entering the ITE is below the maximum specified by the ITE Environmental Class, this output will be zero.
-
-#### Zone ITE Any Air Inlet Dry-Bulb Temperature Below Operating Range Time [hr]
-
-#### ITE Air Inlet Dry-Bulb Temperature Below Operating Range Time [hr]
-
-Hours when the dry-bulb temperature of the air entering the ITE is above the range specified by the ITE Environmental Class.
-
-#### ITE Air Inlet Dry-Bulb Temperature Difference Below Operating Range [deltaC]
-
-The temperature difference (in degrees DeltaC) between the air inlet dry-bulb temperature and the minimum allowable dry-bulb temperature specified by the ITE Environmental Class. Only negative values are reported. When the dry-bulb temperature of the air entering the ITE is above the minimum specified by the ITE Environmental Class, this output will be zero.
-
-#### Zone ITE Any Air Inlet Dewpoint Temperature Above Operating Range Time [hr]
-
-#### ITE Air Inlet Dewpoint Temperature Above Operating Range Time [hr]
-
-Hours when the dewpoint temperature of the air entering the ITE is above the range specified by the ITE Environmental Class.
-
-#### ITE Air Inlet Dewpoint Temperature Difference Above Operating Range [deltaC]
-
-The temperature difference (in degrees DeltaC) between the air inlet dewpoint temperature and the maximum allowable dewpoint temperature specified by the ITE Envionmental Class. Only positive values are reported. When the dewpoint temperature of the air entering the ITE is below the maximum specified by the ITE Environmental Class, this output will be zero.
-
-#### Zone ITE Any Air Inlet Dewpoint Temperature Below Operating Range Time [hr]
-
-#### ITE Air Inlet Dewpoint Temperature Below Operating Range Time [hr]
-
-Hours when the dewpoint temperature of the air entering the ITE is above the range specified by the ITE Environmental Class.
-
-#### ITE Air Inlet Dewpoint Temperature Difference Below Operating Range [deltaC]
-
-The temperature difference (in degrees DeltaC) between the air inlet dewpoint temperature and the minimum allowable dewpoint temperature specified by the ITE Envionmental Class. Only negative values are reported. When the dewpoint temperature of the air entering the ITE is above the minimum specified by the ITE Environmental Class, this output will be zero.
-
-#### Zone ITE Any Air Inlet Relative Humidity Above Operating Range Time [hr]
-
-#### ITE Air Inlet Relative Humidity Above Operating Range Time [hr]
-
-Hours when the relative humidity of the air entering the ITE is above the range specified by the ITE Environmental Class.
-
-#### ITE Air Inlet Relative Humidity Difference Above Operating Range [%]
-
-The temperature difference (in degrees DeltaC) between the air inlet relative humidity and the maximum allowable relative humidity specified by the ITE Envionmental Class. Only positive values are reported. When the relative humidity of the air entering the ITE is below the maximum specified by the ITE Environmental Class, this output will be zero.
-
-#### Zone ITE Any Air Inlet Relative Humidity Below Operating Range Time [hr]
-
-#### ITE Air Inlet Relative Humidity Below Operating Range Time [hr]
-
-Hours when the relative humidity of the air entering the ITE is above the range specified by the ITE Environmental Class.
-
-#### ITE Air Inlet Relative Humidity Difference Below Operating Range [%]
-
-The temperature difference (in degrees DeltaC) between the air inlet relative humidity and the minimum allowable relative humidity specified by the ITE Envionmental Class. Only negative values are reported. When the relative humidity of the air entering the ITE is above the minimum specified by the ITE Environmental Class, this output will be zero.
-
-### ZoneContaminantSourceAndSink:CarbonDioxide
-
-The ZoneContaminantSourceAndSink:CarbonDioxide object allows users to input carbon dioxide sources or sinks in a zone. Note that carbon dioxide generation within a zone can also be specified using People and GasEquipment objects. Multiple ZoneContaminantSourceAndSink:CarbonDioxide  objects can be specified for the same zone.
-
-#### Field: Name
-
-The name of the ZoneContaminantSourceAndSink:CarbonDioxide object. The name for each ZoneContaminantSourceAndSink:CarbonDioxide object must be unique.
-
-#### Field: Zone Name
-
-This field is the name of the zone (ref: **Zone**) and links a particular ZoneContaminantSourceAndSink:CarbonDioxide object to a thermal zone in the building.
-
-#### Field: Design Generation Rate
-
-This field denotes the design carbon dioxide generation rate (m<sup>3</sup>/s). The design value is modified by the schedule fraction (see Field: Schedule Name). The resulting volumetric generation rate is converted to mass generation rate using the current zone indoor air density at each time step. The rate can be either positive or negative. A positive value represents a source rate (CO<sub>2</sub> addition to the zone air) and a negative value represents a sink rate (CO<sub>2</sub> removal from the zone air).
-
-When the mass design generation rate is available, a conversion is required to meet input requirement with volumetric flow rate. This can be accomplished by the mass flow rate divided by the density of carbon dioxide.  
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedules) that modifies the design carbon dioxide generation rate (see previous field). The schedule values can be any positive number between 0.0 and 1.0. For each simulation time step, the actual CO<sub>2</sub> generation rate in a zone is the product of the Design Generation Rate field (above) and the value specified by this schedule.
-
-An IDF example is provided below:
-
-```idf
-ZoneContaminantSourceAndSink:CarbonDioxide,
-    NORTH_ZONE CO2,        !- Name
-    NORTH_ZONE,            !- Zone Name
-    1.e-6,                 !- Design Generation Rate {m3/s}
-    CO2 Source Schedule;   !- Schedule Name
-```
-
-
-### ZoneContaminantSourceAndSink:CarbonDioxide Outputs
-
-HVAC,Average, Contaminant Source or Sink CO2 Gain Volume Flow Rate [m3/s]
-
-HVAC,Average, Zone Contaminant Source or Sink CO2 Gain Volume Flow Rate [m3/s]
-
-#### Contaminant Source or Sink CO2 Gain Volume Flow Rate [m3/s]
-
-This output is the net carbond dioxide internal gain/loss in m3/s for an individual ZoneContaminantSourceAndSink:CarbonDioxide object.
-
-#### Zone Contaminant Source or Sink CO2 Gain Volume Flow Rate [m3/s]
-
-This output variable reports the total (net) carbon dioxide internal gains/losses in cubic meters per second for a zone, including impacts from three objects: ZoneContaminantSourceAndSink:CarbonDioxide, People, and GasEquipment. Positive values denote carbon dioxide generation (gain or source), while negative values denote carbon dioxide removal (loss or sink).
-
-### ZoneContaminantSourceAndSink:Generic:Constant
-
-The ZoneContaminantSourceAndSink:Generic:Constant object specifies the generic contaminant generation rate and removal rate coefficient in a zone. The associated fraction schedules are required for allowing users to change the magnitude of sources and sinks. The object is equivalent to the combination of the constant coefficient model and the burst source model defined in the sources and sinks element types of CONTAM 3.0. The basic equation used to calculate generic contaminant source and sink for the constant model is given below:
-
-<div>\[{S_f}(t) = {G_f}(t)*{F_G} - {R_f}(t){C_f}(t)*1.0E - 6*{F_R}\]</div>
-
-where
-
-*S<sub>f</sub>* <sub>     </sub> = Contaminant generic contaminant source strength [m<sup>3</sup>/s]
-
-*G<sub>f</sub>* <sub>    </sub> = Generic contaminant generation rate [m<sup>3</sup>/s]
-
-*F<sub>G</sub>* <sub>   </sub> = Fraction value from the source fraction schedule at a given time [dimensionless]
-
-*R<sub>f</sub>* <sub>     </sub> = Generic contaminant effective removal rate [m<sup>3</sup>/s]
-
-*F<sub>R</sub>* <sub>   </sub> = Fraction value from the sink fraction schedule at a given time [dimensionless]
-
-*C<sub>f</sub>* <sub>     </sub> = Generic contaminant concentration value at a given previous time step [ppm]
-
-#### Field: Name
-
-This field represents a unique identifying name.
-
-#### Field: Zone Name
-
-This field signifies the Name of the zone with constant generic contaminant source and sink.
-
-#### Field: Design Generation Rate
-
-This field denotes the full generic contaminant design generation rate (m<sup>3</sup>/s). The design generation rate is the maximum amount of generic contaminant expected at design conditions. The design value is modified by the schedule fraction (see Field:Generation Schedule Name).
-
-When the mass generation rate is available, the rate must be converted to a volume flow rate. Use the mass flow rate divided by the vapor density of the generic contaminant.  
-
-#### Field: Generation Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design generation rate (G<sub>f</sub>). This fraction between 0.0 and 1.0 is noted as F<sub>G</sub> in the above equation.
-
-#### Field: Design Removal Coefficient
-
-This field denotes the full generic contaminant design removal coefficient (m<sup>3</sup>/s). The design removal rate is the maximum amount of generic contaminant expected at design conditions times the generic contaminant concentration in the same zone. The design value is modified by the schedule fraction (see Field:Removal Schedule Name).
-
-#### Field: Removal Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design generation rate (R<sub>f</sub>). This fraction between 0.0 and 1.0 is noted as F<sub>R</sub> in the above equation.
-
-An IDF example is provided below:
-
-```idf
-  ZoneContaminantSourceAndSink:Generic:Constant,
-    NORTH ZONE GC,          !- Name
-    NORTH ZONE,             !- Zone Name
-    1.0E-6,                 !- Design Generation Rate {m3/s}
-    GC Source Schedule,     !- Generation Schedule Name
-    1.0E-7,                 !- Design Removal Coefficient {m3/s}
-    GC Removal Schedule;    !- Removal Schedule Name
-```
-
-### ZoneContaminantSourceAndSink:Generic:Constant Outputs
-
-When a ZoneContaminantSourceAndSink:Generic:Constant object is specified, the following output variables are available:
-
-ZONE,Average, Generic Air Contaminant Constant Source Generation Volume Flow Rate [m3/s]
-
-#### Generic Air Contaminant Constant Source Generation Volume Flow Rate [m3/s]
-
-This output is the average generic contaminant generation rate from each ZoneContaminantSourceAndSink:Generic:Constant object. The generation rate is a sum of generation and removal rates. The zone air generic contaminant level at the previous zone time step is used in the removal rate calculation.
-
-### SurfaceContaminantSourceAndSink:Generic:PressureDriven
-
-The SurfaceContaminantSourceAndSink:Generic:PressureDriven object specifies the generic contaminant generation rate coefficient, which is used to calculate the generation rate due to the pressure difference across the surface. The object is equivalent to the pressure driven model defined in the sources and sinks element types of CONTAM 3.0. This object assumes to work with the AirflowNetwork model. The surface has to be defined in the AirflowNetwork:Multizone:Surface. Although the model is designed to be applied to radon and soil gas entry, it is expanded to be applied to all contaminant transport, including generic contaminant. However, it should be used in caution. The basic equation used to calculate generic contaminant source for the pressure driven constant model is provided below:
-
-<div>\[{S_f}(t) = {H_f}(t)*{F_G}*{\left( {{P_j} - {P_i}} \right)^n}\]</div>
-
-where
-
-*S<sub>f</sub>* <sub>     </sub> = Generic contaminant source strength [m<sup>3</sup>/s]
-
-*H<sub>f</sub>* <sub>     </sub> = Generic contaminant generation rate coefficient [m<sup>3</sup>/s]
-
-*F<sub>G</sub>* <sub>   </sub> = Fraction value from the source fraction schedule at a given time [dimensionless]
-
-*n   * = Flow power exponent
-
-P*<sub>i</sub>* <sub>     </sub> = Zone pressure [Pa]
-
-P*<sub>j</sub>* <sub>     </sub> = Pressure in an adjacent zone for a interior surface or outdoor for an exterior surface [Pa]
-
-#### Field: Name
-
-The field signifies the unique identifying name.
-
-#### Field: Surface Name
-
-This field represents the name of the surface as a generic contaminant source using the pressure driven model.
-
-#### Field: Design Generation Rate Coefficient
-
-This field denotes the generic contaminant design generation coefficient (m<sup>3</sup>/s). The design generation rate is the maximum amount of generic contaminant expected at design conditions times the pressure difference with a power exponent across a surface. The design value is modified by the schedule fraction (see Field:Generation Schedule Name).
-
-#### Field: Generation Exponent
-
-This field denotes the flow power exponent,* n*, in the contaminant source equation. The valid range is 0.0 to 1.0, 
-
-An IDF example is provided below:
-
-```idf
-  SurfaceContaminantSourceAndSink:Generic:PressureDriven,
-    WEST ZONE GC BLD,       !- Name
-    Zn001:Wall001,          !- Surface Name
-    1.0E-6,                 !- Design Generation Rate Coefficient {m3/s}
-    GC Source Schedule,     !- Generation Schedule Name
-    0.5;                    !- Generation Exponent
-```
-
-
-### SurfaceContaminantSourceAndSink:Generic:PressureDriven Outputs
-
-When a SurfaceContaminantSourceAndSink:Generic:PressureDriven object is specified, the following output variables are available:
-
-ZONE,Average,Generic Air Contaminant Pressure Driven Generation Volume Flow Rate [m3/s]
-
-#### Generic Air Contaminant Pressure Driven Generation Volume Flow Rate [m3/s]
-
-This output is the average generic contaminant generation rate from each SurfaceContaminantSourceAndSink:Generic:PressureDriven object.
-
-### ZoneContaminantSourceAndSink:Generic:CutoffModel
-
-The ZoneContaminantSourceAndSink:Generic contaminant:CutoffModel object specifies the generic contaminant generation rate based on the cutoff concentration model. The basic equation used to calculate generic contaminant source for the pressure driven constant model is given below:
-
-<div>\[{S_f}(t) = \left\{ \begin{array}{l}{G_f}(t)*{F_G}*\left( {1 - \frac{{{C_f}(t)}}{{{C_{cutoff}}}}} \right)\;\;\;\;\;{C_f} &lt; {C_{cutoff}}\\0\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;{C_f} \ge {C_{cutoff}}\end{array} \right\}\]</div>
-
-where
-
-*S<sub>f</sub>* <sub>     </sub> = Generic contaminant source strength [m<sup>3</sup>/s]
-
-*G<sub>f</sub>* <sub>    </sub> = Generic contaminant generation rate [m<sup>3</sup>/s]
-
-*F<sub>G</sub>* <sub>   </sub> = Fraction value from the source fraction schedule at a given time [dimensionless]
-
-*C<sub>cutoff</sub>*           = Cutoff concentration at which emission ceases [ppm]
-
-*C<sub>f</sub>* <sub>     </sub> = Generic contaminant concentration value at a given previous time step [ppm]
-
-#### Field: Name
-
-The field signifies the unique identifying name.
-
-#### Field: Zone Name
-
-This field represents the name of the zone with generic contaminant source and sink using the cutoff model.
-
-#### Field: Design Generation Rate Coefficient
-
-This field denotes the full generic contaminant design generation rate (m<sup>3</sup>/s). The design generation rate is the maximum amount of generic contaminant expected at design conditions. The design value is modified by the schedule fraction (see Field:Generation Schedule Name).
-
-When the mass generation rate is available, the rate must be converted to a volume flow rate. Use the mass flow rate divided by the vapor density of the generic contaminant.  
-
-#### Field: Generation Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design generation rate (G<sub>f</sub>). This fraction between 0.0 and 1.0 is noted as F<sub>G</sub> in the above equation.
-
-#### Field: Cutoff Generic Contaminant at which Emission Ceases
-
-This field is the generic contaminant cutoff concentration level where the source ceases its emission. 
-
-** **
-
-An IDF example is provided below:
-
-```idf
-ZoneContaminantSourceAndSink:Generic:CutoffModel,
-    NORTH ZONE GC CutoffModel,          !- Name
-    NORTH ZONE,             !- Zone Name
-    1.0E-5,                 !- Design Generation Rate Coefficient {m3/s}
-    GC Source Schedule,     !- Schedule Name
-    100000;                 !- Cutoff Generic Contaminant at which Emission Ceases {ppm}
-```
-
-
-### ZoneContaminantSourceAndSink:Generic:CutoffModel Outputs
-
-When a ZoneContaminantSourceAndSink:Generic:CutoffModel object is specified, the following output variables are available:
-
-ZONE,Average, Generic Air Contaminant Cutoff Model Generation Volume Flow Rate [m3/s]
-
-#### Generic Air Contaminant Cutoff Model Generation Volume Flow Rate [m3/s]
-
-This output is the average generic contaminant generation rate from each SurfaceContaminantSourceAndSink:Generic:CutoffModel object.
-
-### ZoneContaminantSourceAndSink:Generic:DecaySource
-
-The ZoneContaminantSourceAndSink:Generic:DecaySource object specifies the generic contaminant generation rate based on the decay source model. The basic equation used to calculate generic contaminant source for the decay source model is given below:
-
-<div>\[{S_f}(t) = {G_f}(t){F_G}\exp ( - t/{t_c})\]</div>
-
-where
-
-*S<sub>f</sub>* <sub>     </sub> = Generic contaminant source strength [m<sup>3</sup>/s]
-
-*G<sub>f</sub>* <sub>    </sub> = Initial generic contaminant generation rate [m<sup>3</sup>/s]
-
-*F<sub>G</sub>* <sub>   </sub> = Fraction value from the source fraction schedule at a given time [dimensionless]
-
-t     = Time since the start of emission [second]
-
-*t<sub>c</sub>*    = Decay time constant [second]
-
-#### Field: Name
-
-This field is the unique identifying name.
-
-#### Field: Zone Name
-
-This field represents the name of the zone with a generic contaminant decaying source.
-
-#### Field: Initial Emission Rate
-
-This field denotes the initial generic contaminant design emission rate (m<sup>3</sup>/s). The generation is controlled by a schedule, as defined in the next field. Generic contaminant emission begins when the schedule changes from a zero to a non-zero value (between zero and one). The initial emission rate is equal to the schedule value times the initial generation rate. A single schedule may be used to initiate several emissions at different times.(see Field:Generation Schedule Name).
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design emission rate (G<sub>f</sub>). This fraction between 0.0 and 1.0 is noted as F<sub>G</sub> in the above equation. When the value is equal to 1, the generation rate is used and time is reset to zero. When the value is equal to zero, the schedule value is ignored in the equation.
-
-#### Field: Decay Time Constant
-
-This field is the time at which the generation rate reaches 0.37 of the original rate.
-
-Note: The variable t, time since the start of emission, will be reset to zero, when a new run period starts, or the generation schedule value is equal to zero.
-
-An IDF example is provided below:
-
-```idf
-ZoneContaminantSourceAndSink:Generic:DecaySource,
-    WEST ZONE GC DecaySource,           !- Name
-    WEST ZONE,              !- Zone Name
-    1.0E-5,                 !- Initial Emission Rate {m3/s}
-    GC Source Schedule,     !- Schedule Name
-    100000;                 !- Delay Time Constant {s}
-```
-
-
-### ZoneContaminantSourceAndSink:Generic:DecaySource Outputs
-
-When a ZoneContaminantSourceAndSink:Generic:DecaySource object is specified, the following output variables are available:
-
-Zone,Average,Generic Air Contaminant Decay Model Generation Volume Flow Rate [m3/s]
-
-Zone,Average,Generic Air Contaminant Decay Model Generation Emission Start Elapsed Time [s]
-
-#### Generic Air Contaminant Decay Model Generation Volume Flow Rate [m3/s]
-
-This output is the average generic contaminant decay rate from each SurfaceContaminantSourceAndSink:Generic:DecaySource object.
-
-#### Generic Air Contaminant Decay Model Generation Emission Start Elapsed Time [s]
-
-This output is the decay time since the start of emission. The start time is either at the beginning of each run period, including design day simulations, or the time when the egenration schedule value is zero.
-
-### SurfaceContaminantSourceAndSink:Generic:BoundaryLayerDiffusion
-
-The SurfaceContaminantSourceAndSink:Generic:BoundaryLayerDiffusion object specifies the generic contaminant generation rate from surface diffusion. The object is equivalent to the boundary layer diffusion model driven model defined in the sources and sinks element types of CONTAM 3.0.
-
-The boundary layer diffusion controlled reversible sink/source model with a linear sorption isotherm follows the descriptions presented in [Axley 1991]. The boundary layer refers to the region above the surface of a material through which a concentration gradient exists between the near-surface concentration and the air-phase concentration. The rate at which a contaminant is transferred onto a surface (sink) is defined as:
-
-<div>\[{S_f} = h*\rho *A\left( {{C_f} - \frac{{{C_s}}}{k}} \right)*1.0E - 6\]</div>
-
-where
-
-*h*    = Average film mass transfer coefficient over the sink [m/s]
-
-*r*    = Film density of air [kg/m<sup>3</sup>]
-
-*A*    = Surface area of the adsorbent [m<sup>2</sup>]
-
-*C<sub>f</sub>*   = Concentration in the air at the previous time step [ppm]
-
-*C<sub>s</sub>*   = Concentration in the adsorbent [ppm]
-
-*k*    = Henry adsorption constant or partition coefficient [dimensionless]
-
-#### Field: Name
-
-This field signifies a unique identifying name.
-
-#### Field: Surface Name
-
-This field denotes the name of the surface as a generic contaminant reversible source or sink using the boundary layer diffusion model.
-
-#### Field: Mass Transfer Coefficient
-
-This field specifies the average mass transfer coefficient of the contaminant generic contaminant within the boundary layer (or film) above the surface of the adsorbent.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the mass transfer coefficient with the value between 0.0 and 1.0. 
-
-#### Field: Henry Adsorption Constant or Partition Coefficient
-
-This field denotes the generic contaminant Henry partition coefficient in the units of dimensionless. The coefficient relates the concentration of the contaminant generic contaminant in the bulk-air to that at the surface of the adsorption material.
-
-An IDF example is provided below:
-
-```idf
-SurfaceContaminantSourceAndSink:Generic:BoundaryLayerDiffusion,
-    WEST ZONE GC BLD,       !- Name
-    Zn001:Wall001,          !- Surface Name
-    1.0E-2,                 !- Mass Transfer Coefficient {m/s}
-    GC Source Schedule,     !- Schedule Name
-    2.0;                    !- Henry adsorption constant or partition coefficient
-```
-
-### SurfaceContaminantSourceAndSink:Generic:BoundaryLayerDiffusion Outputs
-
-When a SurfaceContaminantSourceAndSink:Generic:BoundaryLayerDiffusion object is specified, the following output variables are available:
-
-ZONE,Average, Generic Air Contaminant Boundary Layer Diffusion Generation Volume Flow Rate [m3/s]
-
-ZONE,Average, Generic Air Contaminant Boundary Layer Diffusion Inside Face Concentration [ppm]
-
-#### Generic Air Contaminant Boundary Layer Diffusion Generation Volume Flow Rate [m3/s]
-
-This output is the average generic contaminant generation rate from each SurfaceContaminantSourceAndSink:Generic:BoundaryLayerDiffusion object.
-
-#### Generic Air Contaminant Boundary Layer Diffusion Inside Face Concentration [ppm]
-
-This output is the average generic contaminant level at the interior surface.
-
-### SurfaceContaminantSourceAndSink:Generic:DepositionVelocitySink
-
-The SurfaceContaminantSourceAndSink:Generic:DepositionVelocitySink object specifies the generic contaminant removal rate from a surface. The object is equivalent to the deposition velocity sink model defined in CONTAM 3.0 sources and sinks element types.
-
-The deposition velocity model provides for the input of a sink’s characteristic in the familiar term of deposition velocity. The removal stops when the sink concentration level is higher than the zone air concentration level. The deposition velocity model equation is:
-
-<div>\[{S_f}(t) = {\nu_d}{A_s}m*{C_f}(t)*1.0E - 6*F{}_R\]</div>
-
-where
-
-S<sub>f</sub>(*t*)            = Removal rate at time t [m<sup>3</sup>/s]
-
-*n<sub>d</sub>*    = Deposition velocity [m/s]
-
-*A<sub>s</sub>*   = Deposition surface area [m<sup>2</sup>]
-
-*m*   = Element multiplier [dimensionless]
-
-*C*<sub>f</sub>(*t*)            = Concentration of contaminant generic contaminant at the previous time step [ppm]
-
-F<sub>R</sub>   = Schedule or control signal value at time *t* [-]
-
-#### Field: Name
-
-This field denotes a unique identifying name.
-
-#### Field: Surface Name
-
-This field represents the name of the surface as a generic contaminant sink using the deposition velocity sink model.
-
-#### Field: Deposition Velocity
-
-This field specifies the deposition velocity to the surface of the adsorbent in the units of m/s.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design removal rate (S<sub>f</sub>). This fraction between 0.0 and 1.0 is noted as F<sub>R</sub> in the above equation.
-
-An IDF example is provided below:
-
-```idf
-SurfaceContaminantSourceAndSink:Generic:DepositionVelocitySink,
-    EAST ZONE GC DVS,       !- Name
-    Zn002:Wall001,          !- Surface Name
-    1.0E-3,                 !- Deposition Velocity {m/s}
-    GC Source Schedule;     !- Schedule Name
-```
-
-
-### SurfaceContaminantSourceAndSink:Generic:DepositionVelocitySink Outputs
-
-The following output variables are available when the SurfaceContaminantSourceAndSink:Generic:DepositionVelocitySink
-
-object is specified.
-
-ZONE,Average, Generic Air Contaminant Deposition Velocity Removal Volume Flow Rate [m3/s]
-
-#### Generic Air Contaminant Deposition Velocity Removal Volume Flow Rate [m3/s]
-
-This output is the average generic contaminant generation rate from each SurfaceContaminantSourceAndSink:Generic:DepositionVelocitySink object.
-
-### ZoneContaminantSourceAndSink:Generic:DepositionRateSink
-
-The ZoneContaminantSourceAndSink:Generic:DepositionRateSink object specifies the generic contaminant removal rate from a zone. The object is equivalent to the deposition rate sink model defined in CONTAM 3.0 sources and sinks element types.
-
-The deposition rate model provides for the input of a sink’s characteristic in the familiar term of deposition rate in a zone. The removal stops when the sink concentration level is higher than the zone air concentration level. The deposition rate model equation is:
-
-<div>\[{S_f}(t) = {k_d}{V_z}*{C_f}(t)*1.0E - 6*{F_R}m\]</div>
-
-Where
-
-S<sub>f</sub>(*t*)            = Removal rate at time t [m<sup>3</sup>/s]
-
-*k<sub>d</sub>*   = Deposition rate [1/T]
-
-*V<sub>z</sub>*   = Zone volume [m<sup>3</sup>]
-
-*m*   = Element multiplier [dimensionless]
-
-*C*<sub>f</sub>(*t*)            = Concentration of generic contaminant at the previous time *step* [ppm]
-
-F<sub>R</sub>   = Schedule or control signal value at time *t* [dimensionless]
-
-#### Field: Name
-
-This field denotes a unique identifying name.
-
-#### Field: Zone Name
-
-This field represents the name of the zone as a generic contaminant sink using the deposition rate sink model.
-
-#### Field: Deposition Rate
-
-This field specifies the deposition rate to the zone in the units of 1/s.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design removal rate (S<sub>f</sub>). This fraction between 0.0 and 1.0 is noted as F<sub>R</sub> in the above equation.
-
-An IDF example is provided below:
-
-```idf
-ZoneContaminantSourceAndSink:Generic:DepositionRateSink,
-    NORTH ZONE GC DRS,      !- Name
-    NORTH ZONE,             !- Zone Name
-    1.0E-5,                 !- Deposition Rate {m3/s}
-    GC Source Schedule;     !- Schedule Name
-```
-
-
-### ZoneContaminantSourceAndSink:Generic:DepositionRateSink Outputs
-
-When the ZoneContaminantSourceAndSink:Generic:DepositionRateSink object is specified, the following output variables are available:
-
-ZONE,Average, Generic Air Contaminant Deposition Rate Removal Volume Flow Rate [m3/s]
-
-#### Generic Air Contaminant Deposition Rate Removal Volume Flow Rate [m3/s]
-
-This output is the average generic contaminant generation rate from each ZoneContaminantSourceAndSink:Generic:DepositionRateSink object.
-
diff --git a/doc/src/docs/InputOutputReference/01b-InputOutputReference.md b/doc/src/docs/InputOutputReference/01b-InputOutputReference.md
deleted file mode 100644
index 248c46707f8..00000000000
--- a/doc/src/docs/InputOutputReference/01b-InputOutputReference.md
+++ /dev/null
@@ -1,21003 +0,0 @@
-### ZoneBaseboard:OutdoorTemperatureControlled
-
-This object specifies outside temperature-controlled (OTC) baseboard heating. The capacities (high and low) are specified in W at the temperatures specified. The schedule allows both capacities to change hourly on a proportional basis. This baseboard heater does not operate if the outdoor dry-bulb is above the high temperature limit. Between the high temperature and the low temperature, the capacity is interpolated (linear) between the high and the low capacity values. Below the low temperature, the capacity is set at the low capacity value. This allows the user to add baseboard heat to a perimeter zone starting at a prescribed temperature and then slowly increases this capacity to a max value.
-
-**Example:**
-
-Temperature High = 10 C     Capacity High = 100,000 W
-
-Temperature Low = 0 C        Capacity Low  = 500,000 W
-
-Table 16. Outdoor Temperature Controlled Baseboard Heat Temperature vs. Capacity
-
-<table class="table table-striped">
-<tr>
-<th>Outdoor Dry-bulb(C)</th>
-<th>Baseboard Output</th>
-</tr>
-<tr>
-<td>&gt;10</td>
-<td>0</td>
-</tr>
-<tr>
-<td>10</td>
-<td>100,000</td>
-</tr>
-<tr>
-<td>8</td>
-<td>180,000</td>
-</tr>
-<tr>
-<td>6</td>
-<td>260,000</td>
-</tr>
-<tr>
-<td>4</td>
-<td>340,000</td>
-</tr>
-<tr>
-<td>2</td>
-<td>420,000</td>
-</tr>
-<tr>
-<td>0</td>
-<td>500,000</td>
-</tr>
-<tr>
-<td>&lt; 0</td>
-<td>500,000</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-#### Field: Name
-
-The name of the ZoneBaseboard:OutdoorTemperatureControlled object.
-
-#### Field: Zone Name
-
-This field is the name of the zone and attaches the baseboard heat equipment statement to a thermal zone in the building.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule that modifies the capacities (high and low) for baseboard heat equipment (see next four fields). The schedule values can be any positive number. The actual energy input for the baseboard equipment in a zone as defined by this statement depends on the actual outdoor temperature and where that temperature is in the range of Low Temperature to High Temperature..
-
-#### Field: Capacity at Low Temperature
-
-This is the baseboard equipment capacity (Watts) at the low temperature limit. This is the maximum capacity of the baseboard equipment in full load operation. This field is autosizable.
-
-#### Field: Low Temperature
-
-If the outdoor dry-bulb temperature (degrees Celsius) is at or below the low temperature the baseboard heater operates at the low temperature capacity. This field is autosizable. The lowest design outdoor dry bulb temperature is chosen, if autosized.
-
-#### Field: Capacity at High Temperature
-
-This is the baseboard equipment capacity (Watts) at the high temperature limit. This field is autosizable. The capacity at low temperature is prorated against the reference low and high temperature fields, if autosized.
-
-#### Field: High Temperature
-
-If the outdoor dry-bulb temperature (degrees Celsius) is greater than the high temperature the baseboard heater will not operate. This field is autosizable. If autosized, this is equal to the design zone heating setpoint temperature described below, so that the capacity at high temperature is zero.
-
-#### Field: Fraction Radiant
-
-This field is a decimal number between 0.0 and 1.0 and is used to characterize the type of heat being given off by baseboard heat equipment in a zone.  The number specified in this field will be multiplied by the total energy consumed by the baseboard heat equipment to give the amount of long wavelength radiation gain to the zone.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Perimeter Baseboards", etc. A new meter for reporting is created for each unique subcategory  (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the baseboard equipment will be assigned to the "General" end-use subcategory.
-
-#### Field: Design Zone Heating Setpoint
-
-This is heating setpoint temperature in the zone where the unit serves. This is used to autosize high temperature and capacity at high temperature fields. The default value is 20°C.
-
-An IDF example:
-
-```idf
-ZoneBaseboard:OutdoorTemperatureControlled,
-    SPACE4-1 BBHeat 1,       !- Name
-    SPACE4-1,                !- Zone Name
-    EQUIP-1,                 !- SCHEDULE Name
-    1500,                    !- Capacity at low temperature {W}
-    0,                       !- Low Temperature {C}
-    500,                     !- Capacity at high temperature {W}
-    10,                      !- High Temperature {C}
-    0.5,                     !- Fraction Radiant
-    Baseboard Heat,          !- End-Use Subcategory
-    20;                      !- Design Zone Heating Setpoint
-```
-{C}
-
-
-
-### ZoneBaseboard:OutdoorTemperatureControlled Output
-
-ZoneBaseboard:OutdoorTemperatureControlled objects have output variables for individual objects and for zone totals. The following outputs are available:
-
-* Zone,Average,Baseboard Electric Power [W]
-
-* Zone,Sum,Baseboard Electric Energy [J]
-
-* Zone,Sum,Baseboard Radiant Heating Energy [J]
-
-* Zone,Average,Baseboard Radiant Heating Rate [W]
-
-* Zone,Sum,Baseboard Convective Heating Energy [J]
-
-* Zone,Average,Baseboard Convective Heating Rate [W]
-
-* Zone,Sum,Baseboard Total Heating Energy [J]
-
-* Zone,Average,Baseboard Total Heating Rate [W]
-
-* Zone,Average,Zone Baseboard Electric Power [W]
-
-* Zone,Sum,Zone Baseboard Electric Energy [J]
-
-* Zone,Sum,Zone Baseboard Radiant Heating Energy [J]
-
-* Zone,Average,Zone Baseboard Radiant Heating Rate [W]
-
-* Zone,Sum,Zone Baseboard Convective Heating Energy [J]
-
-* Zone,Average,Zone Baseboard Convective Heating Rate [W]
-
-* Zone,Sum,Zone Baseboard Total Heating Energy [J]
-
-* Zone,Average,Zone Baseboard Total Heating Rate [W]
-
-
-#### Baseboard Electric Power [W]
-
-This field is the electric power for the ZoneBaseboard:OutdoorTemperatureControlled object in Watts.
-
-#### Baseboard Electric Energy [J]
-
-The outdoor temperature controlled baseboard heat option is assumed to be fueled by electricity. This field is the same as the Baseboard Total Heating Energy (above) in joules.
-
-#### Baseboard Radiant Heating Rate [W]
-
-#### Baseboard Radiant Heating Energy [J]
-
-These output variables are the amount of radiant heat gain for the ZoneBaseboard:OutdoorTemperatureControlled object in Watts (for rate) or Joules. This is determined by the current heat gain from the heater to the zone and the “Fraction Radiant� specified in the input. The radiant gains (long wavelength) are distributed to the surfaces using an area weighting scheme.
-
-#### Baseboard Convective Heating Rate [W]
-
-#### Baseboard Convective Heating Energy [J]
-
-These output variables are the amount of convective heat gain for the ZoneBaseboard:OutdoorTemperatureControlled object in Watts (for rate) or Joules. This is determined by the current heat gain from the heater to the zone and the “Fraction Radiant� specified in input (1-FractionRadiant = FractionConvected). The convective heat gain is added to the zone air heat balance directly.
-
-#### Baseboard Total Heating Rate [W]
-
-#### Baseboard Total Heating Energy [J]
-
-These output variables are the amount of heat gain for the ZoneBaseboard:OutdoorTemperatureControlled object in Watts (for rate) or Joules. This is determined by the sum of the radiant and convective heat gains from the baseboard heat.
-
-#### Zone Baseboard Electric Power [W]
-
-This field is the electric power for all ZoneBaseboard:OutdoorTemperatureControlled objects within the zone in Watts.
-
-#### Zone Baseboard Electric Energy [J]
-
-The outdoor temperature controlled baseboard heat option is assumed to be fueled by electricity. This field is the same as the Baseboard Total Heating Energy (above) in joules. However, this amount is also shown in the Electricity meters that are associated with the zone – Electricity:Facility, Electricity:Buidling, Electricity:Zone:&lt;Zone Name&gt;, and InteriorEquipment:Electricity.
-
-#### Zone Baseboard Radiant Heating Rate [W]
-
-#### Zone Baseboard Radiant Heating Energy [J]
-
-These output variables are the amount of radiant heat gain for all ZoneBaseboard:OutdoorTemperatureControlled objects within the zone in Watts (for rate) or Joules. This is determined by the current heat gain from the heater to the zone and the “Fraction Radiant� specified in the input. The radiant gains (long wavelength) are distributed to the surfaces using an area weighting scheme.
-
-#### Zone Baseboard Convective Heating Rate [W]
-
-#### Zone Baseboard Convective Heating Energy [J]
-
-These output variables are the amount of convective heat gain for all ZoneBaseboard:OutdoorTemperatureControlled objects within the zone in Watts (for rate) or Joules. This is determined by the current heat gain from the heater to the zone and the “Fraction Radiant� specified in input (1-FractionRadiant = FractionConvected). The convective heat gain is added to the zone air heat balance directly.
-
-#### Zone Baseboard Total Heating Rate [W]
-
-#### Zone Baseboard Total Heating Energy [J]
-
-These output variables are the amount of heat gain for all ZoneBaseboard:OutdoorTemperatureControlled objects within the zone in Watts (for rate) or Joules. This is determined by the sum of the radiant and convective heat gains from the baseboard heat.
-
-### Meters for Equipment Outputs
-
-As described in each of the equipment sections, values for specific equipments will show up on the following meters:
-
-Table 17. Distribution of Equipment to Meters
-
-<table class="table table-striped">
-<tr>
-<th>Meter Name</th>
-<th>Scope</th>
-<th>Equipment Specfics</th>
-</tr>
-<tr>
-<td>Electricity:Facility</td>
-<td>Entire Facility</td>
-<td>Electric Equipment, OTC Baseboard Heat</td>
-</tr>
-<tr>
-<td>Electricity:Building</td>
-<td>All Zones</td>
-<td>Electric Equipment, OTC Baseboard Heat</td>
-</tr>
-<tr>
-<td>Electricity:Zone:&lt;Zone Name&gt;</td>
-<td>Specific Zone</td>
-<td>Electric Equipment, OTC Baseboard Heat</td>
-</tr>
-<tr>
-<td>InteriorEquipment:Electricity</td>
-<td>AllZones</td>
-<td>Electric Equipment, OTC Baseboard Heat</td>
-</tr>
-<tr>
-<td>&lt;End-Use Subcategory&gt;:InteriorEquipment:Electricity</td>
-<td>Specific Subcategory</td>
-<td>Electric Equipment, OTC Baseboard Heat</td>
-</tr>
-<tr>
-<td>Gas:Facility</td>
-<td>Entire Facility</td>
-<td>Gas Equipment</td>
-</tr>
-<tr>
-<td>Gas:Building</td>
-<td>All Zones</td>
-<td>Gas Equipment</td>
-</tr>
-<tr>
-<td>Gas:Zone:&lt;Zone Name&gt;</td>
-<td>Specific Zone</td>
-<td>Gas Equipment</td>
-</tr>
-<tr>
-<td>InteriorEquipment:Gas</td>
-<td>AllZones</td>
-<td>Gas Equipment</td>
-</tr>
-<tr>
-<td>&lt;End-Use Subcategory&gt;:InteriorEquipment:Gas</td>
-<td>Specific Subcategory</td>
-<td>Gas Equipment</td>
-</tr>
-</table>
-
-
-
-Group – Daylighting
--------------------
-
-Daylighting can be invoked in EnergyPlus by the use of two objects: **Daylighting:Controls** and **Daylighting:DELight:Controls**. These are described in the following object descriptions.
-
-Note that Daylighting:Controls and Daylighting:DELight:Controls objects may be intermixed in a single IDF but may not be used in the same zone.
-
-### Daylighting:Controls
-
-In this method daylighting illuminance levels are calculated and then used to determine how much the electric lighting can be reduced. The daylight illuminance level in a zone depends on many factors, including sky condition; sun position; calculation point; location, size, and glass transmittance of windows; window shading devices; and reflectance of interior surfaces. Reduction of electric lighting depends on daylight illuminance level, illuminance set point, fraction of zone controlled and type of lighting control.
-
-#### Field: Zone name
-
-The name of the zone to which the following daylighting-related input applies.
-
-#### Field: Total Daylighting Reference Points
-
-Allowed values are 1 or 2. This the number of reference points in the zone at which horizontal daylighting illuminance will be calculated based on input for the following fields. It is assumed that the photocells that control the overhead electric lighting respond to the light levels at the specified reference points.
-
-#### Fields: (X,Y,Z) of First Reference Point
-
-Required if Total Daylighting Reference Points = 1 or 2. These three fields are the X, Y and Z values of the First Reference point in the coordinate system you specified for daylighting reference points in the GlobalGeometryRules object. Figure 53 shows an example using the relative coordinate (to zone) system. Z is typically at desk height (0.8 m).
-
-If you want to divide a thermal zone into two independently-controlled lighting zones, then Total Daylighting Reference Points should be set to 2 and (X,Y,Z) of the Second Reference Point (see following input fields) should also be specified.
-
-#### Fields: (X,Y,Z) of Second Reference Point
-
-The X, Y, and Z coordinates, in the same coordinate system, of the second daylighting reference point. Required if Total Daylighting Reference Points = 2. See Figure 53 for an example.
-
-
-
-![](media/image095.svg)
-
-Figure 53. Example showing location of daylighting reference points in the zone coordinate system (relative) of a rectangular zone with three windows. (a) Perspective view, (b) plan view, (c) elevation view. All dimensions are in meters.
-
-#### Field: Fraction of Zone Controlled by First Reference Point
-
-The fraction of the zone’s floor-area whose electric lighting is controlled by the daylight illuminance at the First Reference Point. If there is only one reference point then a fraction equal to
-
-1.0 - (Fraction of Zone Controlled by First Reference Point)
-
- is assumed to have no lighting control.
-
-#### Field: Fraction of Zone Controlled by Second Reference Point
-
-The fraction of the zone’s floor-area whose electric lighting is controlled by the daylight illuminance at the Second Reference Point. Required if Total Daylighting Reference Points = 2. A fraction equal to
-
-1.0 – ([Fraction of Zone Controlled by First Reference Point] + [Fraction of Zone Controlled by Second Reference Point])
-
-is assumed to have no lighting control.
-
-#### Field: Illuminance SetPoint at First Reference Point
-
-The desired lighting level (in lux) at the First Reference Point. This is the lighting level that would be produced at this reference point at night if the overhead electric lighting were operating at full input power. Recommended values depend on type of activity; they may be found, for example, in the Lighting Handbook of the Illuminating Engineering Society of North America. A typical value for general office work (excluding computer terminals) is 500 lux.
-
-#### Field: Illuminance SetPoint at Second Reference Point
-
-The desired lighting level (in lux) at the Second Reference Point. Required if Total Daylighting Reference Points = 2. This is the lighting level that would be produced at this reference point at night if the overhead electric lighting were operating at full input power.
-
-#### Field: Lighting Control Type
-
-The type of overhead electric lighting control. All reference points specified are assumed to have this type of control.
-
-For Lighting Control Type = 1 (continuous), the overhead lights dim continuously and linearly from (maximum electric power, maximum light output) to (minimum electric power, minimum light output) as the daylight illuminance increases. The lights stay on at the minimum point with further increase in the daylight illuminance.
-
-For Lighting Control Type = 2 (stepped), the electric power input and light output vary in discrete, equally spaced steps. The number of steps is given by Number of Steps (Excluding Off) of Stepped Control. For example, if Number of Steps = 3 and Illuminance Setpoint = 600, then the following table shows the fraction of the lights that are on vs. daylight illuminance.
-
-Table 18. Stepped Lighting Control Example
-
-<table class="table table-striped">
- <tr>
-  <th colspan="2">Example of a Stepped Lighting Control System with Three Steps</th>
- </tr>
- <tr>
-  <th>Daylight illuminance</th>
-  <th>Fraction of lights that are on</th>
- </tr>
- <tr>
-  <td>0-200</td>
-  <td>1.0</td>
- </tr>
- <tr>
-  <td>200-400</td>
-  <td>2/3</td>
- </tr>
- <tr>
-  <td>400-600</td>
-  <td>1/3</td>
- </tr>
- <tr>
-  <td>600 and above</td>
-  <td>0.0</td>
- </tr>
-</table>
-
-Lighting Control Type = 3 (continuous/off) is the same as Lighting Control Type = 1 except that the lights switch off completely when the minimum dimming point is reached.
-
-#### Field: Glare Calculation Azimuth Angle of View Direction Clockwise from Zone y-Axis
-
-Daylight glare from a window depends on occupant view direction. It is highest when you look directly at a window and decreases as you look away from a window. This field specifies the view direction for calculating glare. It is the angle, measured clockwise in the horizontal plane, between the zone y-axis and the occupant view direction.
-
-#### Field: Maximum Allowable Discomfort Glare Index
-
-If a daylit zone has windows with shading devices (except exterior screens), the shades will be deployed if the daylight glare at the First Reference Point exceeds the value of this field. To get this type of glare control you have to specify Trigger = Glare, GlareOrSolarOnWindow, GlareOrHorizontalSolar, GlareOrOutsideAirTemp, GlareOrZoneAirTemp or GlareOrZoneLoad in WindowProperty:ShadingControl for one or more windows in the zone (see WindowProperty:ShadingControl).
-
-If a zone has two or more windows with glare control, the shading devices will be deployed one by one in the order in which the windows are input until the glare level at each reference point falls below Maximum Allowable Discomfort Glare Index or is as close as possible to it.
-
-The following table gives recommended values of Maximum Allowable Discomfort Glare Index.
-
-Table 19. Recommended Values -- Discomfort Glare Index
-
-<table class="table table-striped">
-  <tr>
-    <th colspan="2">Recommended Values of Maximum Allowable Discomfort Glare Index</th>
-  </tr>
-  <tr>
-    <th>Activity or zone type</th>
-    <th>Maximum Allowable Discomfort Glare Index</th>
-  </tr>
-  <tr>
-    <td>Art Galleries</td>
-    <td>16</td>
-  </tr>
-  <tr>
-    <td>Factories</td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>Rough work</td>
-    <td>28</td>
-  </tr>
-  <tr>
-    <td>Engine assembly</td>
-    <td>26</td>
-  </tr>
-  <tr>
-    <td>Fine assembly</td>
-    <td>24</td>
-  </tr>
-  <tr>
-    <td>Instrument assembly</td>
-    <td>22</td>
-  </tr>
-  <tr>
-    <td>Hospital wards</td>
-    <td>18</td>
-  </tr>
-  <tr>
-    <td>Laboratories</td>
-    <td>22</td>
-  </tr>
-  <tr>
-    <td>Museums</td>
-    <td>20</td>
-  </tr>
-  <tr>
-    <td>Offices</td>
-    <td>22</td>
-  </tr>
-  <tr>
-    <td>School classrooms</td>
-    <td>20</td>
-  </tr>
-</table>
-
-#### Field: Minimum Input Power Fraction for Continuous Dimming Control
-
-For Lighting Control Type = 1 (continuous), the lowest power the lighting system can dim down to, expressed as a fraction of maximum input power (see figure, below). For Lighting Control Type = 3 (continuous/off) this is the power fraction reached just before the lights switch off completely.
-
-![](media/image096.svg)
-
-Figure 54. Illustration of continuous dimming relationship
-
-The figure above shows the relationship between electric light output and electrical input.
-
-#### Field: Minimum Light Output Fraction for Continuous Dimming Control
-
-For Lighting Control Type = 1 (continuous), the lowest lighting output the lighting system can dim down to, expressed as a fraction of maximum light output (see figure, above). This is the fractional light output that the system produces at minimum input power. For Lighting Control Type = 3 (continuous/off) this is the light output fraction reached just before the lights switch off completely.
-
-#### Field: Number of Stepped Control Steps
-
-The number of steps, excluding off, in a stepped lighting control system (see figure, below). Required and must be &gt;0 if Lighting Control Type = 2. The steps are assumed to be equally spaced.
-
-![](media/image097.svg)
-
-Figure 55. Stepped lighting control with Number of Steps = 3.
-
-#### Field: Probability Lighting will be Reset When Needed in Manual Stepped Control
-
-May be specified if a stepped lighting control system (Lighting Control Type = 2) is manually operated, such as in a simple, one-step (on-off) system. Gives the probability the occupants of a daylit zone will set the electric lights to the correct level to obtain the required illuminance. The rest of the time the lights are assumed to be set one step too high. For example, consider an on-off lighting system (Number of Steps = 1) with a set point of 600 lux and 0.7 reset probability. Then, when daylighting exceeds 600 lux, the electric lights will be off 70% of the time and on 30% of the time.
-
-#### Field: Availability Schedule Name
-
-This alpha field is optional and may be used to define the name of a schedule that denotes whether or not the control is available to operate during a given time period. If the schedule value is greater than zero, then the controls will be available to operate for that time period.  If the schedule value is zero or less, then the controls will not be available. If this field is left blank, the controls will be always available. For example, this can be useful for scheduling the daylighting controls off during design days so that the daylighting controls do not affect lighting power during sizing.
-
-An IDF example:
-
-
-
-```idf
-Daylighting:Controls, ! Zone Name
-    1,                ! Total Daylighting Reference Points
-    3.048,3.048,0.9,  ! X,Y,Z coordinates of first reference point {m}
-    0.0,0.0,0.0,      ! X,Y,Z coordinates of second reference point, if present {m}
-    0.99,             ! Fraction of zone controlled by first reference point
-    0.0,              ! Fraction of zone controlled by second reference point, if present
-    500.,             ! Illuminance setpoint at first reference point {lux}
-    500.,             ! Illuminance setpoint at second reference point, if present {lux}
-    1,                ! Lighting control type {1=continuous,2=stepped,3=continuous/off}
-    180.0,            ! Azimuth angle of view direction for glare calculation {deg},
-                      !   measured clockwise from zone y-axis. Value of 180 gives view
-                      !   (from reference point) that is directly at window, maximizing glare.
-    20.0,             ! Maximum discomfort glare index for window shade control
-    0.3,              ! Minimum input power fraction for continuous dimming control
-    0.2,              ! Minimum light output fraction for continuous dimming control
-    0,                ! Number of steps, excluding off, for stepped control
-    1.0;              ! Probability electric lighting will be reset when needed (used only
-                      !   for stepped control, to simulate manual on/off control)
-```
-
-
-### Guidelines for Daylighting Modeling (Detailed Method)
-
-Following are some guidelines for preparing EnergyPlus input to model the effects of daylighting. Before studying these guidelines, however, you should read the description of each input field under Daylighting:Controls, and review the IDF example, above, and the sample daylighting input, PurchAirWithDaylighting.idf.
-
-#### Use of Window Multipliers
-
-If an exterior wall in a daylit zone has a number of identical windows, the windows should be entered separately rather than using a window multiplier (ref: FenestrationSurface:Detailed). Using a multiplier would give an incorrect illuminance calculation since individual windows would not be positioned correctly on the wall.
-
-#### Use of Zone Multipliers
-
-A zone multiplier should not be used on a daylit zone if the windows in the zone are shadowed by exterior obstructions like trees or neighboring buildings, or by obstructions caused by other parts of building. The reason for this is that the shadowing on the windows of the multiplied zone may be different from zone to zone depending on exactly how the shadows fall on the zones. However, a zone multiplier may be used on a daylit zone if the shadowing is by overhangs, fins and/or window setback.
-
-#### Thermal Zoning for Daylighting
-
-To correctly calculate both direct and inter-reflected daylight illuminance you should try to model a thermal zone consisting of several similar rooms separated by interior walls as a representative room with a zone multiplier (ref: Zone). An example of this is shown in Figure 56. Room-1 is the representative room, with a zone multiplier = 4.
-
-Interior walls IW-1, IW-2 and IW-3 should be treated as adiabatic, i.e., they should have Outside Boundary Condition = Surface and Outside Boundary Condition Object = IW-1, IW-2, or IW-3, respectively (ref: BuildingSurface:Detailed). Similarly, if the ceiling and floor of Room-1 are interior surfaces, they should be treated as adiabatic.
-
-![](media/image098.svg)
-
-Figure 56. For daylighting purposes the thermal zone enclosed by the dashed boundary line should be modeled as a typical zone (Room-1) with a zone multiplier of 4.
-
-Sometimes a representative room cannot be found. Figure 57 shows a section of a building with four rooms having different daylighting characteristics because of different floor area, orientation and/or window size. In this case lumping the rooms into a single thermal zone would give nonsensical daylighting illuminance values because of the presence of the interior walls, which EnergyPlus ignores when calculating illuminance reaching a reference point directly from a window (i.e., without reflection). The solution in this case is to describe each room as a separate thermal zone with its own daylighting reference points, and input the interior walls because these will participate in the calculation of inter-reflected illuminance.
-
-![](media/image099.svg)
-
-Figure 57. Rooms A, B, C and D have different daylighting characteristics. If lumped into a single thermal zone the daylighting calculation will be less accurate because the blockage of direct light by the interior walls between these rooms is modeled with some simplifications (see Interior Obstructions below). To get a good daylighting calculation each room should be input as a separate thermal zone.
-
-#### Multiple Lighting Zones
-
-The detailed daylighting calculation allows a thermal zone to be divided into two independently-controlled lighting zones. (See the fields: Fraction of Zone Controlled by First Reference Point, Fraction of Zone Controlled by Second Reference Point, Illuminance SetPoint at First Reference Point, and Illuminance SetPoint at Second Reference Point.) An example is shown in Figure 58, where a relatively deep thermal zone has two lighting zones of equal area.
-
-![](media/image100.svg)
-
-Figure 58. Two independently-controlled lighting zones, each with 50% of the area of the thermal zone.
-
-#### Fins, Overhangs and Other Exterior Obstructions
-
-The daylighting calculation accounts for the presence of exterior obstructions in determining the amount of light that strikes the windows. For daylighting purposes exterior obstructions fall into three categories:
-
-(1)  Fins, overhangs, trees, neighboring buildings, etc., entered with the objects Shading:Zone:Detailed,
- Shading:Site:Detailed, or
- Shading:Building:Detailed.
-
-(2)  Building surfaces like walls and roofs (in an L-shaped building, for example).
-
-(3)  Surfaces associated with window setback.
-
-Category (1) obstructions can have an associated solar transmittance schedule (see description of the field Transmittance Schedule Name for these shading surfaces). If this schedule is not specified, the surface is opaque (has zero transmittance).
-
-The daylighting calculation takes the transmittance into account in determining, for example, how much light enters a window through a translucent awning. It is assumed that the solar and visible transmittance is the same and that the surfaces are non-diffusing, i.e., they do not change the direction of transmitted light. Ref:Daylighting:Controls.
-
-Category (2) and (3) surfaces are assumed to be opaque.
-
-Surfaces in all three categories are assumed to be black, i.e., they do not reflect light, unless you set if “Reflections� option is chosen  in the Building object. Then obstructions can reflect light, such as the top of an overhang reflecting light onto the window above. Ref: Building, Field: Solar Distribution (with reflections options).
-
-#### Interior Obstructions
-
-The daylighting calculation accounts for the presence of interior obstructions that lie between a window and a reference point. Unlike exterior obstructions, which can be light transmitting, interior obstructions are assumed to be opaque. Interior obstructions can reduce or eliminate the light directly reaching the reference point through a window.
-
-However, interior obstructions that are walls, ceilings or floors are reflecting so they  contribute to the inter-reflected component of daylight illuminance as do the non-obstructing zone surfaces.
-
-Interior obstructions can belong to the Shading object series. This type of obstruction is assumed to be non-reflecting so does not contribute to the inter-reflected component of daylight illuminance.
-
-An example of an interior obstruction that is a wall in an L-shaped room is shown in Figure 59. Here, wall A (or, equivalently, Wall B) prevents light from directly getting to the Reference Point from the window.
-
-
-
-![](media/image101.svg)
-
-Figure 59. Wall A (or Wall B) is an interior obstruction that prevents light from directly reaching the daylighting reference point from the window.
-
-#### Double Façades: Daylighting through Interior Windows
-
-The Daylighting:Controls method, with no additional user input,  calculates the contribution of daylight that passes into a target zone through interior windows.[[1]](#_ftn1) The origin of this daylight is exterior windows in adjacent zones that share interior windows with the target zone. This capability is aimed at daylighting through a **double façade** (also called “double envelope� or “double skin.�)
-
-This is illustrated in Figure 60, which shows a double-façade buffer zone, Z0, with exterior windows EW1 and EW2. Z0 shares interior windows IW1, IW2 and IW3 with daylit occupied zones ZD1, ZD2 and ZD3, respectively (“daylit� here means the zone has an associated Daylighting:Controls object). The daylight illuminance at reference points RP1, RP2 and RP3 comes from the interior windows and has two main sources:
-
-1.    Daylight that passes through both an exterior window and an interior window in Z0 and reaches a reference point without reflection. This is called “direct illuminance.�
-
-2.    Daylight from Z0  that passes through an interior window and reaches a reference point by inter-reflection in the daylit zone. Because the program calculates this source from the interior solar distribution in Z0 it is recommended that the most accurate calculation of this distribution be made, which occurs if Solar Distribution = FullInteriorAndExterior in the Building object.
-
-A third possible source is neglected because it is generally small in double-façade cases. This is daylight that is reflected from the surfaces of Z0, passes through an interior window and then reaches a reference point without inter-reflection in the daylit zone.
-
-PurchAirWithDoubleFacadeDaylighting.idf is an input example of daylighting through an interior window.
-
-
-
-![](media/image102.svg)
-
-Figure 60. Vertical section through a double-façade building showing daylighting through interior windows. The dashed lines show that (1) reference point RP1 receives direct light from exterior window EW1 via interior window IW1; (2) RP2 receives direct light from EW1 and EW2 via IW2; and (3) RP3 receives direct light from EW2 via IW3.
-
-#### Interior Window Daylighting Configurations that EnergyPlus Can Calculate
-
-Figure 61 shows schematically the general configuration of daylighting through interior windows that can be calculated with EnergyPlus. Here, daylit zone ZD has one or more interior windows that are adjacent to other zones, each of which has one or more exterior windows. ZD itself may or may not have exterior windows. If it does, than the daylight illuminance from its exterior and interior windows will be additive. The zones adjacent to ZD may or may not be daylit and may or may not have other interior windows that are not adjacent to ZD. (The program does not consider the illuminance in ZD from electric lighting in adjacent zones.)
-
-![](media/image103.svg)
-
-Figure 61. General configuration of daylighting through interior windows that can be calculated with EnergyPlus. IW = interior window, EW = exterior window.
-
-#### Interior Window Daylighting Configurations that EnergyPlus Cannot Calculate
-
-Figure 62 shows schematically a configuration of daylighting through interior windows that cannot be calculated with EnergyPlus. Here, zone Z has an interior window that is adjacent to zone Z1 which in turn has an interior window adjacent to zone Z2. However, the daylight from the exterior window in Z2 that enters Z after passing through Z1 is not calculated because Z2 is not adjacent to Z.
-
-
-
-![](media/image104.svg)
-
-Figure 62. Configuration in which daylighting of zone Z through its interior window  cannot be calculated with EnergyPlus. IW = interior window, EW = exterior window.
-
-#### Restrictions on Shading Devices
-
-There are two restrictions on the use of exterior-window shading devices when a daylit zone has interior windows:
-
-1)   If two daylit zones share an interior window, neither zone can have an exterior window whose shading device does glare control (i.e., the WindowProperty:ShadingControl for the exterior window has Glare Control Is Active = Yes).
-
-2)   If two daylit zones share an interior window, neither zone can have an exterior window with a WindowProperty:ShadingControl that has Shading Control Type = MeetDaylightIlluminanceSetpoint.
-
-### DElight Daylighting Method
-
-The DElight method of analyzing daylighting in buildings is very similar to that used in the Detailed method. For each point in time, DElight calculates the interior daylighting illuminance at specified reference points and then determines how much the electric lighting can be reduced while still achieving a combined daylighting and electric lighting illuminance target. The daylight illuminance level in a zone depends on many factors, including exterior light sources; location, size, and visible light transmittance of simple and complex fenestration systems; reflectance of interior surfaces; and location of calculation reference points. The subsequent reduction of electric lighting depends on daylight illuminance level, illuminance set point, fraction of zone controlled, and type of lighting control.
-
-There are two primary differences between the Detailed and DElight methods of calculating interior illuminance levels. The first is that DElight includes the capability of analyzing complex fenestration systems that include geometrically complicated shading systems (e.g., roof monitors) and/or optically complicated glazings (e.g., prismatic or holographic glass). The second key difference is that DElight uses a radiosity method to calculate the effects of light reflection inside a zone. These methods are discussed in more detail in the engineering documentation.
-
-There are other important differences between the two methods. One is the inability of DElight to perform the type of dynamic shading controls possible using the Detailed method at each point in time during the thermal simulation (e.g., changes in electrochromic glazing transmittances and blind slat angles). Another is the DElight ability to include more than two reference points in its interior illuminance and electric lighting reduction calculations. A third is the current lack of visual quality (e.g., glare) calculations performed by DElight. Fourth, the modeling of interior obstructions is different in the two methods. In the DElight method interior obstructions block interreflections but do not block the intial direct illuminance. In the Detailed method, interior obstructions block the initial direct illuminance but do not block interreflections. See the engineering documentation for more details. Fifth, when using DElight daylighting the presence of exterior shading surfaces such as overhangs is ignored.
-
-Input for invoking the DElight method involves three object types: **Daylighting:DELight:Controls**, **Daylighting:DELight:ReferencePoint**, and **Daylighting:DELight:ComplexFenestration**. Each of these objects is described below.
-
-### Daylighting:DELight:Controls
-
-The first input object required for invoking the DElight method is the Daylighting:DELight:Controls object, which defines the parameters of each daylighting zone within a building. This object must be associated with a specific thermal zone within the building for which the reduction in electric lighting due to daylight illuminance will be accounted.
-
-#### Field: Name
-
-User name of the DElight daylighting zone to which the following input applies.
-
-#### Field: Zone Name
-
-The name of the thermal Zone hosting this DElight daylighting zone. This must be a valid name that has been associated with a thermal Zone contained in the same EnergyPlus input data file.
-
-#### Field: Lighting Control Type
-
-The type of overhead electric lighting control. All reference points specified are assumed to have this type of control.
-
-For Lighting Control Type = 1 (continuous), the overhead lights dim continuously and linearly from (maximum electric power, maximum light output) to (minimum electric power, minimum light output) as the daylight illuminance increases. The lights stay on at the minimum point with further increase in the daylight illuminance.
-
-For Lighting Control Type = 2 (stepped), the electric power input and light output vary in discrete, equally spaced steps. The number of steps is given by Number of Steps (Excluding Off) of Stepped Control. For example, if Number of Steps = 3 and Illuminance Setpoint = 600, then the following table shows the fraction of the lights that are on vs. daylight illuminance.
-
-Table 20. Stepped Lighting Control Example
-
-<table class="table table-striped">
- <tr>
-  <th colspan="2">Example of a Stepped Lighting Control System with Three Steps</th>
- </tr>
- <tr>
-  <th>Daylight illuminance</th>
-  <th>Fraction of lights that are on</th>
- </tr>
- <tr>
-  <td>0-200</td>
-  <td>1.0</td>
- </tr>
- <tr>
-  <td>200-400</td>
-  <td>2/3</td>
- </tr>
- <tr>
-  <td>400-600</td>
-  <td>1/3</td>
- </tr>
- <tr>
-  <td>600 and above</td>
-  <td>0.0</td>
- </tr>
-</table>
-
-Lighting Control Type = 3 (continuous/off) is the same as Lighting Control Type = 1 except that the lights switch off completely when the minimum dimming point is reached.
-
-#### Field: Minimum Input Power Fraction for Continuous Dimming Control
-
-For Lighting Control Type = 1 (continuous), the lowest power the lighting system can dim down to, expressed as a fraction of maximum input power (see figure, below). For Lighting Control Type = 3 (continuous/off) this is the power fraction reached just before the lights switch off completely.
-
-![](media/image105.svg)
-
-Figure 63. Illustration of continuous dimming relationship
-
-The figure above shows the relationship between electric light output and electrical input.
-
-#### Field: Minimum Light Output Fraction for Continuous Dimming Control
-
-For Lighting Control Type = 1 (continuous), the lowest lighting output the lighting system can dim down to, expressed as a fraction of maximum light output (see figure, above). This is the fractional light output that the system produces at minimum input power. For Lighting Control Type = 3 (continuous/off) this is the power fraction reached just before the lights switch off completely.
-
-#### Field: Number of Steps (Excluding Off) for Stepped Control
-
-The number of steps, excluding off, in a stepped lighting control system (see figure, below). Required and must be &gt;0 if Lighting Control Type = 2. The steps are assumed to be equally spaced.
-
-![](media/image106.svg)
-
-Figure 64. Stepped lighting control with Number of Steps = 3.
-
-#### Field: Probability Lighting Will Be Reset When Needed in Manual Stepped Control
-
-May be specified if a stepped lighting control system (Lighting Control Type = 2) is manually operated, such as in a simple, one-step (on-off) system. Gives the probability the occupants of a daylit zone will set the electric lights to the correct level to obtain the required illuminance. The rest of the time the lights are assumed to be set one step too high. For example, consider an on-off lighting system (Number of Steps = 1) with a set point of 600 lux and 0.7 reset probability. Then, when daylighting exceeds 600 lux, the electric lights will be off 70% of the time and on 30% of the time.
-
-#### Field: Gridding Resolution
-
-The maximum surface area for nodes in gridding (subdividing) all surfaces in the DElight zone. All reflective and transmitting surfaces will be subdivided into approximately square nodes that do not exceed this maximum. Higher resolution subdivisions require greater calculation times, but generally produce more accurate results. This same gridding resolution is also used to subdivide any Complex Fenestration System surfaces. It is advisable to perform at least one simulation of new input using a small gridding resolution such as 0.1m2 to compare these results against simulation runs at lower resolution (i.e., higher maximum area nodal grids) to get a sense of possible levels of error.
-
-An IDF example:
-
-
-
-```idf
-Daylighting:DELight:Controls,
-    DElight NORTH ZONE, !- DElight Zone Name
-    NORTH ZONE,         !- Zone Name
-    1,     !- Lighting control type
-    0.3,   !- Minimum input power fraction for continuous dimming control
-    0.2,   !- Minimum light output fraction for continuous dimming control
-    0,     !- Number of steps (excluding off) for stepped control
-    1.0,   !- Probability lighting will be reset when needed in manual stepped control
-    1.0;   !- Gridding Resolution {m2}
-```
-
-
-
-
-### Daylighting:DELight:ReferencePoint
-
-The second input object required for invoking the DElight method is the Daylighting:DELight:ReferencePoint object, which defines the parameters of each Reference Point within the associated DElight daylighting zone. This object must be associated with a specific Daylighting:DELight:Controls object instance. There may be up to a maximum of 100 Reference Points for each DElight daylighting zone. Each Reference Point that is input does NOT need to be included in the control of the electric lighting system within the zone. This is determined by the fraction of the zone controlled by each Reference Point, which can be input as 0. Note that the sum of all Reference Point control fractions must equal 1 to obtain correct overall results.
-
-#### Field: Name
-
-User name of the DElight daylighting Reference Point to which the following input applies.
-
-#### Field: DElight Name
-
-The name of the Daylighting:DELight:Controls object instance hosting this Reference Point. This must be a valid name that has been associated with a DElight daylighting Zone contained in the same EnergyPlus input data file.
-
-#### Fields: (X,Y,Z) of Reference Point
-
-These three fields are the X, Y and Z values of the Reference point in the coordinate system you specified for daylighting reference points in the GlobalGeometryRules object. Figure 65 shows an example using the relative coordinate (to zone) system. Z is typically at work surface height (e.g., 0.8m for a desk).
-
-
-
-![](media/image107.svg)
-
-Figure 65. Example showing location of two daylighting reference points in the zone coordinate system (relative) of a rectangular zone with three windows. (a) Perspective view, (b) plan view, (c) elevation view. All dimensions are in meters.
-
-#### Field: Fraction of Zone Controlled by Reference Point
-
-The zone floor-area fraction of the electric lighting that is controlled by the daylight illuminance at this Reference Point. If the sum of the values for this field for all Reference Points input for a given daylighting zone is less than 1.0, then the remaining fraction (i.e., 1.0 – Sum) is assumed to not have lighting control.
-
-Note that Reference Points may be input with a 0.0 value for this fraction. In this case, daylight factors and interior illuminance values will be calculated for the Reference Point, but it will play no role in controlling the electric lighting within the daylighting zone to which it belongs.
-
-#### Field: Illuminance Setpoint at Reference Point
-
-The desired lighting level (in lux) at this Reference Point. This is assumed to be the lighting level that would be produced at this reference point at night if the overhead electric lighting were operating at full input power. Recommended values depend on the type of activity and may be found, for example, in the Lighting Handbook of the Illuminating Engineering Society of North America. A typical value for general office work (excluding computer terminals) is 500 lux.
-
-An IDF example:
-
-```idf
-Daylighting:DELight:ReferencePoint,
-    RefPt 2,            !- Reference Point Name
-    DElight NORTH ZONE, !- DElight Zone Name
-    5.0,  !- X-coordinate of reference point {m}
-    3.0,  !- Y-coordinate of reference point {m}
-    0.9,  !- Z-coordinate of reference point {m}
-    0.5,  !- Fraction of zone controlled by reference point
-    500.; !- Illuminance setpoint at reference point {lux}
-```
-
-
-### Daylighting:DELight:ComplexFenestration
-
-The third input object related to the DElight method is the Daylighting:DElight: Complex Fenestration object. The DElight daylighting analysis method can be applied to daylighting zones that contain only simple fenestration systems such as windows and skylights that are standard EnergyPlus sub-surfaces. In this situation, no Daylighting:DElight: Complex Fenestration object would be input.
-
-In addition to analyzing simple fenestration systems, DElight includes the capability of analyzing complex fenestration systems such as geometrically complicated static shading systems (e.g., roof monitors) and/or optically complicated glazings (e.g., prismatic or holographic glass). This capability is based on characterizing these complex fenestration systems (CFS) using bi-directional transmittance distribution functions (BTDF). In general, BTDF data for a specific CFS must be either measured or simulated (e.g., using ray-tracing techniques) prior to employing DElight to analyze it within EnergyPlus. The current implementation of DElight CFS calculations within EnergyPlus supports two approaches to the input of BTDF, an analytical approach and a file-based approach. The details of inputting these two approaches are described below under the User Complex Fenestration Type field.
-
-Two analytical CFS BTDF types are currently supported, window and light shelf. The file-based approach requires that a user has access to a data file containing raw BTDF data that DElight reads as additional input during its analysis calculations. BTDF data files are described separately since it is anticipated that individual EnergyPlus users will not create these data files themselves.
-
-The methods related to characterizing and analyzing CFS using BTDF are still evolving. DElight is an early implementation of CFS analysis methods. These methods, and the input associated with them here, will likely change in the future.
-
-#### Field: User Name
-
-User name of the DElight daylighting Complex Fenestration to which the following input applies.
-
-#### Field: Complex Fenestration Type
-
-Type name of the DElight daylighting Complex Fenestration system to be analyzed. This type name must take one of the following two forms.
-
-BTDF^GEN^Analytical Type^Normal Visible Transmittance^Dispersion Angle
-
-BTDF^FILE^Filename
-
-The first form above is for supported analytical CFS types which currently include WINDOW and LIGHTSHELF. While these analytical types are relatively simple, they represent flexible ways to explore diffusing CFS systems and the impact of light shelves in redirecting light through an aperture. Each of these types also requires the visible transmittance of the CFS at normal incidence angle, and a dispersion angle (in degrees) that represents the “spread� of transmitted light. A small dispersion angle of 10 corresponds to clear glazing while a large angle of 90 corresponds to perfectly diffusing glazing. The “^� symbol must be used as a delimiter between sub-fields within this Complex Fenestration type name string as shown in the IDF example for WINDOW below, and in the DElight sample input data files.
-
-The second form above is for CFS types for which there is pre-measured or pre-simulated BTDF data. In this case the Filename sub-field must be a valid data file name that is associated with an existing BTDF dataset that DElight can use in its calculations.
-
-#### Field: Building Surface Name
-
-The name of the heat transfer surface object instance hosting this Complex Fenestration, analogous to the Building Surface Name field for subsurfaces such as Windows. This must be a valid name that has been associated with a heat transfer surface contained in the same EnergyPlus input data file.
-
-#### Field: Window Name
-
-The name of the Window (ref: FenestrationSurface:Detailed object) instance that will be used to account for the geometry, and the solar/thermal gains/losses, of the Complex Fenestration system surface. This must be a valid name that has been associated with a Window contained in the same EnergyPlus input data file. The geometry for the Complex Fenestration is taken from the geometry input for this standard EnergyPlus subsurface, hence the term “Doppelganger.�
-
-Note that DElight only deals with the visible spectrum of light transmitted through a Complex Fenestration. To account for the solar/thermal influences of a Complex Fenestration, a geometrically coincident subsurface that will be accounted for by methods already within EnergyPlus must be defined in the input data file. This is an interim solution to the issue of accounting for solar/thermal influences that will likely change as techniques analogous to the daylighting analysis of BTDF are developed.
-
-#### Field: Fenestration Rotation
-
-The in-plane counter-clockwise rotation angle between the Complex Fenestration optical reference direction and the base edge of the Doppelganger Surface geometry. The Complex Fenestration optical reference direction is the direction of the zero azimuth angle for the BDTF dataset. This Rotation angle will typically be zero when the Doppelganger surface is rectangular and its width edge is aligned with the Complex Fenestration optical reference direction.
-
-An IDF example for an analytical WINDOW type CFS:
-
-```idf
-Daylighting:DELight:ComplexFenestration,
-    Window CFS,       !- DElight Complex Fenestration User Name
-    BTDF^GEN^WINDOW^1.0^20.0,     !- Complex Fenestration Type
-    ZN003:WALL001,  !- Complex Fenestration Host Surface
-    Zn003:Wall001:Doppel001, !- Doppelganger Surface Name
-    0.0;            !- Fenestration Rotation {deg}
-```
-
-### DElight Output
-
-In addition to the daylighting-specific outputs for DElight listed below, two ASCII text files are created during an EnergyPlus run that includes DElight analysis.  Following completion of an EnergyPlus run, these files are given names that consist of the project name appended with DElight.in and DElight.out.  The format of these files is described in the Output Details and Examples document.
-
-Zone,Average,Daylighting Reference Point Illuminance [lux]
-
-Zone,Average,Daylighting Lighting Power Multiplier []
-
-#### Daylighting Reference Point Illuminance [lux]
-
-The total daylight illuminance at a DElight reference point from all of the exterior windows in a daylit zone.
-
-#### Daylighting Lighting Power Multiplier []
-
-The amount by which the overhead electric lighting power in a zone is multiplied due to usage of DElight calculated daylighting to dim or switch electric lights. For example, if the multiplier is M and the electric power without dimming is P, then the electric power with dimming is M\*P. The multiplier varies from 0.0, which corresponds to maximum dimming (zero electric lighting), to 1.0, which corresponds to no dimming.
-
-### Daylighting Output
-
-The following daylighting-specific outputs are available for Daylighting:Controls:
-
-* Zone,Average,Site Exterior Beam Normal Illuminance [lux]
-
-* Zone,Average,Site Exterior Horizontal Beam Illuminance [lux]
-
-* Zone,Average,Site Exterior Horizontal Sky Illuminance [lux]
-
-* Zone,Average,Site Beam Solar Radiation Luminous Efficacy [lum/W]
-
-* Zone,Average,Site Sky Diffuse Solar Radiation Luminous Efficacy [lum/W]
-
-* Zone,Average,Site Daylighting Model Sky Clearness []
-
-* Zone,Average,Site Daylighting Model Sky Brightness []
-
-* Surface,Average,Daylighting Window Reference Point 1 View Luminance [cd/m2]
-
-* Surface,Average,Daylighting Window Reference Point 1 Illuminance [lux]
-
-* Zone,Average,Daylighting Reference Point 1 Illuminance [lux]
-
-* Zone,Average,Daylighting Reference Point 1 Glare Index []
-
-* Zone,Sum,Daylighting Reference Point 1 Glare Index Setpoint Exceeded Time [hr]
-
-* Zone,Sum,Daylighting Reference Point 1 Daylight Illuminance Setpoint Exceeded Time [hr]
-
-* Surface,Average,Daylighting Window Reference Point 2 View Luminance [cd/m2]
-
-* Surface,Average,Daylighting Window Reference Point 2 Illuminance [lux]
-
-* Zone,Average,Daylighting Reference Point 2 Illuminance [lux], if applicable
-
-* Zone,Average,Daylighting Reference Point 2 Glare Index [], if applicable
-
-* Zone,Sum,Daylighting Reference Point 2 Glare Index Setpoint Exceeded Time [hr]
-
-* Zone,Sum,Daylighting Reference Point 2 Daylight Illuminance Setpoint Exceeded Time [hr]
-
-* Zone,Average,Daylighting Lighting Power Multiplier []
-
-
-#### Site Exterior Beam Normal Illuminance [lux]
-
-Beam normal illuminance of the sun at the earth’s surface, measured in lux (lumens/m<sup>2</sup>)
-
-#### Site Exterior Horizontal Beam Illuminance [lux]
-
-Beam illuminance on an unobstructed horizontal plane at the earth’s surface. Equals “Site Exterior Beam Normal Illuminance� times sine of solar altitude.
-
-#### Site Exterior Horizontal Sky Illuminance [lux]
-
-Illuminance from sky solar radiation on an unobstructed horizontal plane at the earth’s surface. The total exterior horizontal illuminance is the sum of “Site Exterior Horizontal Beam Illuminance� and “Site Exterior Horizontal Sky Illuminance.�
-
-#### Site Beam Solar Radiation Luminous Efficacy [lum/W]
-
-A measure of the visible light content of beam solar radiation; equal to the number of lumens per watt of beam solar radiation. Depends on atmospheric conditions (moisture, turbidity, cloudiness) and solar altitude.
-
-#### Site Sky Diffuse Solar Radiation Luminous Efficacy [lum/W]
-
-A measure of the visible light content of sky diffuse solar radiation; equal to the number of lumens per watt of sky diffuse solar radiation. Depends on atmospheric conditions (moisture, turbidity, cloudiness) and solar altitude.
-
-#### Site Daylighting Model Sky Clearness [ ]
-
-Clearness of sky. One of the factors used to determine sky type and luminous efficacy of solar radiation (see *EnergyPlus Engineering Document*). Sky Clearness close to 1.0 corresponds to an overcast sky. Sky Clearness &gt; 6 is a clear sky.
-
-#### Site Daylighting Model Sky Brightness [ ]
-
-Brightness of sky. One of the factors used to determine sky type and luminous efficacy of solar radiation (see *EnergyPlus Engineering Document*).
-
-#### Daylighting Window Reference Point 1 View Luminance [cd/m2]
-
-The area-averaged luminance of an exterior window as viewed from the first reference point in the daylit zone containing the window. In general, higher window luminance values are associated with higher daylight glare values. (Printed only for exterior windows in daylit zones without interior windows.)
-
-#### Daylighting Window Reference Point 1 Illuminance [lux]
-
-The contribution from a particular exterior window to the daylight illuminance at the first reference point in the daylit zone containing the window. (Not printed for exterior windows in daylit zones with interior windows.)
-
-#### Daylighting Reference Point 1 Illuminance [lux]
-
-The total daylight illuminance at the first reference point from all of the windows in a daylit zone.
-
-#### Daylighting Reference Point 1 Glare Index []
-
-The daylight glare index at the first reference point in a daylit zone.
-
-#### Daylighting Reference Point 1 Glare Index Setpoint Exceeded Time [hr]
-
-The number of hours when the calculated daylight glare index at the first reference point exceeds the glare index setpoint.
-
-#### Daylighting Reference Point 1 Daylight Illuminance Setpoint Exceeded Time [hr]
-
-The number of hours when the calculated daylight illuminance at the first reference point exceeds the daylight illuminance setpoint.
-
-#### Daylighting Reference Point 2 Illuminance [lux]
-
-The total daylight illuminance at the second reference point from all of the windows in a daylit zone.
-
-#### Daylighting Window Reference Point 2 View Luminance [cd/m2]
-
-The area-averaged luminance of an exterior window as viewed from the second reference point, if present, in the daylit zone containing the window. Note that, for a bare window, this value can be different from the corresponding value at the first reference point since different regions of the sky and ground will be visible from the two reference points, and different ranges of angles of incidence and associated glass transmittance values will be involved. (Not printed for exterior windows in daylit zones with interior windows.)
-
-#### Daylighting Window Reference Point 2 Illuminance [lux]
-
-The contribution from a particular exterior window to the daylight illuminance at the second reference point, if present, in the daylit zone containing the window. (Not printed for exterior windows in daylit zones with interior windows.)
-
-#### Daylighting Reference Point 2 Glare Index []
-
-The daylight glare index at the second reference point, if present, in a daylit zone.
-
-#### Daylighting Reference Point 2 Glare Index Setpoint Exceeded Time [hr]
-
-The number of hours when the calculated daylight glare index at the second reference point exceeds the glare index setpoint.
-
-#### Daylighting Reference Point 2 Daylight Illuminance Setpoint Exceeded Time [hr]
-
-The number of hours when the calculated daylight illuminance at the second reference point exceeds the daylight illuminance setpoint.
-
-#### Daylighting Lighting Power Multiplier []
-
-The amount by which the overhead electric lighting power in a zone is multiplied due to usage of daylighting to dim or switch electric lights. For example, if the multiplier is M and the electric power without dimming is P, then the electric power with dimming is M\*P. The multiplier varies from 0.0, which corresponds to maximum dimming (zero electric lighting), to 1.0, which corresponds to no dimming.
-
-### Output:IlluminanceMap
-
-The Output:IlluminanceMap object expands on the reporting capabilities of the daylighting simulation. For any zone simulated with Daylighting:Controls, the illuminance map can generate up to 2,500 points of additional daylighting illuminance values. The resulting map is output as a comma delimited text file that can be imported into a spreadsheet program for rapid visualization of the daylighting illuminance patterns in a zone. The values are produced on an hourly basis. The Z height of the map is constant (parallel to a flat floor). More than one illuminance map can be created for a zone.
-
-#### Field: Name
-
-The name of the map object.
-
-#### Field: Zone Name
-
-Reference to a zone with Daylighting:Controls.
-
-#### Field: Z Height
-
-The height or elevation of the grid of daylighting points.
-
-#### Field: X Minimum Coordinate
-
-The minimum X coordinate boundary for the map.
-
-#### Field: X Maximum Coordinate
-
-The maximum X coordinate boundary for the map.
-
-#### Field: Number of X Grid Points
-
-The number of daylighting reference points in the X direction from the minimum to the maximum boundaries. The maximum number of points that can be generated is 2500 (Number of X Grid Points X Number of Y Grid Points).
-
-#### Field: Y Minimum Coordinate
-
-The minimum Y coordinate boundary for the map.
-
-#### Field: Y Maximum Coordinate
-
-The maximum Y coordinate boundary for the map.
-
-#### Field: Number of Y Grid Points
-
-The number of daylighting reference points in the Y direction from the minimum to the maximum boundaries. The maximum number of points that can be generated is 2500 (Number of X Grid Points X Number of Y Grid Points).
-
-Note:  Daylighting factors cannot be accurately calculated for reference points that are very close to a wall or window (less than 0.15 m or 6 inches). An error is reported for a reference point that is too close to a window, but no error is reported for a point that is too close to a wall.
-
-```idf
-Output:IlluminanceMap,
-  Daylit Map,      ! Map Name
-  Daylit Zone,     ! Zone Name
-  0,               ! Z Height [m]
-  0.1,             ! X Minimum Coordinate [m]
-  4.9,             ! X Maximum Coordinate [m]
-  10,              ! Number of X Grid Points
-  0.1,             ! Y Minimum Coordinate [m]
-  9.9,             ! Y Maximum Coordinate [m]
-  10;              ! Number of Y grid Points
-```
-
-
-Since not all zones are rectangular, it is possible to have map points that are outside the zone. Any illuminance registered at these points is inaccurate and, additionally, a “\*� marks these values for easy observance.
-
-### OutputControl:IlluminanceMap:Style
-
-This object specifies the “style� for the illuminance map output (described in the Output Details and Examples document). As described early in the document (see: EnergyPlus Output Processing), the user may select the “style� for the daylighting illuminance map output file (eplusmap.&lt;ext&gt;).
-
-#### Field: Column Separator
-
-For this field, the desired separator for columns is entered. “Comma� creates comma separated fields/columns in the outputs (eplusmap.csv file is created). “Tab� creates tab separated fields/columns in the outputs (eplusmap.tab file is created). “Fixed� creates space separated fields/columns in the outputs (eplusmap.txt file is created) but these are not necessarily lined up for easy printing.
-
-Note that both tab and comma separated files easily import into Excel™ or other spreadsheet programs. The tab delimited files can also be viewed by text editors, word processing programs and easily converted to “tables� within those programs.
-
-### Daylighting Devices
-
-Daylighting devices work in conjunction with the Daylighting:Controls object to simulate components that can improve daylighting in a zone.
-
-Daylighting devices are also tightly integrated into the zone heat balance. The thermal effects of these devices are simulated with or without the use of a Daylighting:Controls object.
-
-There are two types of daylighting device in EnergyPlus:  tubular daylighting devices and daylighting shelves.
-
-### DaylightingDevice:Tubular
-
-Tubular daylighting devices (TDDs), also known as tubular skylights or light pipes, are used to bring natural exterior daylight into the hard-to-reach, interior spaces of a building.
-
-TDDs consist of three components: a dome, a pipe, and a diffuser.
-
-![DaylightingTubular](media/image108.png)
-
-Figure 66. Tubular daylighting device diagram.
-
-In EnergyPlus each of these components corresponds to an object in the input file.
-
-The dome and diffuser are defined in the same way as windows using the FenestrationSurface:Detailed object. The *Surface Type* field must be specified as TubularDaylightDome or TubularDaylightDiffuser accordingly.
-
-The location and orientation of the dome surface affect the total amount of daylight collected.
-
-The *Base Surface* of the diffuser object determines to which zone the daylighting is delivered. The location and orientation of the diffuser surface affect the amount of daylight received at the Daylighting:Controls reference points.
-
-Although the object definition is the same as for a window, there are several restrictions on TubularDaylightDome and TubularDaylightDiffuser objects:
-
-- Shading control devices are not allowed.
-
-- Frames and dividers are not allowed.
-
-- Multipliers must be 1.0.
-
-- Dome, diffuser, and pipe areas (as given by diameter) must be approximately equal.
-
-- Outside face environment objects are not allowed.
-
-- Dome and diffuser constructions cannot be more than one layer.
-
-Since commercial TDDs are assumed to be cylindrical in shape, it is recommended that the circular areas of the actual dome and diffuser be approximated with a square of equivalent area for the TubularDaylightDome and TubularDaylightDiffuser objects. Although it is possible to use a triangular surface instead, a square is a much better geometric approximation of a circle.
-
-Note that the TubularDaylightDome surface is allowed to have a different position and tilt from the roof base surface. If the actual TDD projects some height above the roof surface, the TubularDaylightDome coordinates should be located accordingly.
-
-![](media/image109.png)
-
-Figure 67. Tubular daylighting device DXF output.
-
-The TubularDaylightDome surface automatically casts a shadow on the roof base surface. However, since the pipe is not represented by a surface, it will not cast a shadow. If this effect must be simulated, one or more SURFACE:SHADING objects can be used.
-
-The dome and diffuser objects are connected by the DAYLIGHTING DEVICE:TUBULAR object:
-
-#### Field: Name
-
-The name of the TDD object.
-
-#### Field: Dome Name
-
-Reference to a FenestrationSurface:Detailed object with *Surface Type* TubularDaylightDome.
-
-#### Field: Diffuser Name
-
-Reference to a FenestrationSurface:Detailed object with *Surface Type* TubularDaylightDiffuser.
-
-#### Field: Construction Name
-
-The construction of the TDD pipe. The visible and solar absorptance of the inside material layer determines the reflectivity of the inner mirrored surface of the TDD. This is very important for the overall transmittance of the TDD.
-
-#### Field: Diameter
-
-The diameter [m] of the TDD pipe. The area of the pipe must match the areas of the dome and diffuser.
-
-#### Field: Total Length
-
-The total length [m] of the TDD pipe between the dome and the diffuser, including the exterior part above the roof. The exterior length is determined internally by subtracting the transition zone lengths from the total length.
-
-#### Field: Effective Thermal Resistance
-
-The effective thermal resistance [m<sup>2</sup>-K/W], i.e. R-value, of the TDD between the exterior dome surface and the interior diffuser surface.
-
-#### Field: Transition Zone&lt;\#&gt;  Name
-
-Name of zone that the TDD pipe passes through before reaching the delivery zone.
-
-#### Field: Transition Zone &lt;\#&gt; Length
-
-Length of pipe [m] in the transition zone. This is used for determining heat gains due to solar absorbed by the pipe in each transition zone. The distribution of absorbed solar gains can be customized by adjusting the length of pipe in each transition zone.   The transition zone gain is proportional to the length of pipe in the zone. If no transition zones are specified, all solar absorbed by the pipe is lost to the exterior environment.
-
-The *Transition Zone Name* and *Transition Zone Length* fields can be repeated for additional transition zones.
-
-```idf
-DaylightingDevice:Tubular,
-  Pipe1,                    !- Object Name
-  Dome1,                    !- Dome Name
-  Diffuser1,                !- Diffuser Name
-  Reflective Aluminum,      !- Construction Name
-  0.3556,                   !- Diameter [m] (approximately 14", a standard size)
-  1.4,                      !- Total Length [m] (subtract zone lengths to get outdoor exposed length)
-  0.28,                     !- Effective Thermal Resistance [m2-K/W] between TubularDaylightDome and
- !                                TubularDaylightDiffuser
-  Attic Zone,               !- Transition Zone 1 Name
-  1.1;                      !- Transition Zone 1 Length [m]
-
-
- FenestrationSurface:Detailed,
-  Dome1,  !- Subsurface Name
-  TubularDaylightDome,  !- Surface Type
-  Clear Acrylic Dome,  !- Construction Name (only 1 layer allowed in construction)
-  Attic Roof,  !- Base Surface Name
-  ,  !- Outside Face Environment (not allowed for TubularDaylightDome)
-  0.0,  !- VF to Ground
-  ,  !- Window Shading Control (not allowed for TubularDaylightDome)
-  ,  !- Frame/Divider Name (not allowed for TubularDaylightDome)
-  1.0,  !- Multiplier (must be 1.0 for TubularDaylightDome)
-  4,  !- Number of Vertices
-  2.3425,  3.1575,  3.9,
-  2.3425,  2.8425,  3.9,
-  2.6575,  2.8425,  3.9,
-  2.6575,  3.1575,  3.9;
-
-
- FenestrationSurface:Detailed,
-  Diffuser1,  !- Subsurface Name
-  TubularDaylightDiffuser,  !- Surface Type
-  Frosted Acrylic Diffuser,  !- Construction Name (only 1 layer allowed in construction)
-  Daylit Zone Ceiling,  !- Base Surface Name
-  ,  !- Outside Face Environment (not allowed for TubularDaylightDiffuser)
-  0.0,  !- VF to Ground
-  ,  !- Window Shading Control (not allowed for TubularDaylightDiffuser)
-  ,  !- Frame/Divider Name (not allowed for TubularDaylightDiffuser)
-  1.0,  !- Multiplier (must be 1.0 for TubularDaylightDiffuser)
-  4,  !- Number of Vertices
-  2.3425,  3.1575,  2.5,
-  2.3425,  2.8425,  2.5,
-  2.6575,  2.8425,  2.5,
-  2.6575,  3.1575,  2.5;
-```
-
-
-### Tubular Daylighting Device Output
-
-* Zone,Average,Tubular Daylighting Device Transmitted Solar Radiation Rate [W]
-
-* Zone,Average,Tubular Daylighting Device Pipe Absorbed Solar Radiation Rate [W]
-
-* Zone,Average,Tubular Daylighting Device Heat Gain Rate [W]
-
-* Zone,Average,Tubular Daylighting Device Heat Loss Rate [W]
-
-* Zone,Average,Tubular Daylighting Device Beam Solar Transmittance []
-
-* Zone,Average,Tubular Daylighting Device Beam Visible Transmittance []
-
-* Zone,Average,Tubular Daylighting Device Diffuse Solar Transmittance []
-
-* Zone,Average,Tubular Daylighting Device Diffuse Visible Transmittance []
-
-
-
-
-#### Tubular Daylighting Device Beam Solar Transmittance []
-
-This is the transmittance of beam solar radiation through the TDD.
-
-#### Tubular Daylighting Device Beam Visible Transmittance []
-
-This is the transmittance of beam visible radiation, or daylight, through the TDD.
-
-#### Tubular Daylighting Device Diffuse Solar Transmittance []
-
-This is the transmittance of diffuse solar radiation through the TDD.
-
-#### Tubular Daylighting Device Diffuse Visible Transmittance []
-
-This is the transmittance of diffuse visible radiation, or daylight, through the TDD.
-
-#### Tubular Daylighting Device Heat Gain Rate [W]
-
-This is the rate of heat gain to the zone by the TDD, in Watts.
-
-#### Tubular Daylighting Device Heat Loss Rate [W]
-
-This is the rate of heat loss from the zone by the TDD, in Watts.
-
-#### Tubular Daylighting Device Pipe Absorbed Solar Radiation Rate [W]
-
-This is the rate at which solar radiation is absorbed by the pipe in the TDD, in Watts.
-
-#### Tubular Daylighting Device Transmitted Solar Radiation Rate [W]
-
-This is the rate at which solar radiation is transmitted by the TDD, in Watts.
-
-
-
-In addition, several surface and window variables are also reported for the TubularDaylightDome and TubularDaylightDiffuser objects. For the TubularDaylightDome:
-
-* Zone,Average,Surface Outside Face Sunlit Area [m2]
-
-* Zone,Average,Surface Outside Face Sunlit Fraction []
-
-* Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Beam Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Beam Solar Incident Angle Cosine Value[]
-
-* Zone,Average,Surface Window Transmitted Solar Radiation Rate [W]
-
-* Zone,Average,Surface Window Total Glazing Layers Absorbed Solar Radiation Rate [W]
-
-
-
-
-For the TubularDaylightDiffuser:
-
-* Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area[W/m2] *(incident inside of pipe)*
-
-* Zone,Average,Surface Window Transmitted Solar Radiation Rate [W] *(same as Tubular Daylighting Device Transmitted Solar Radiation Rate)*
-
-* Zone,Average,Surface Window Total Glazing Layers Absorbed Solar Radiation Rate [W]
-
-
-
-### DaylightingDevice:Shelf
-
-Daylighting shelves, or simply light shelves, are another device for bringing more daylight into a building. Installed as an accessory to a window, daylighting shelves work by reflecting exterior light onto the ceiling of a room. Daylighting shelves can have an inside shelf, an outside shelf, or both.
-
-
-
-![DaylightingShelf](media/image110.png)
-
-Figure 68. Daylighting shelf diagram.
-
-
-
-The inside shelf redistributes light that would have entered the zone anyway. Instead of entering as a beam, all light is reflected onto the zone ceiling and is converted to diffuse shortwave radiation.
-
-The outside shelf changes the amount of light entering the zone. If the shelf surface is more reflective than the ground, it can increase the amount of light incident on the upper part of the window. However, the shading effect of the outside shelf on the lower part of the window must also be considered as it can easily negate any gain achieved in the upper part of the window. All light reflected from the outside shelf that enters the upper window is assumed to strike the ceiling.
-
-![](media/image111.png)
-
-Figure 69. Daylighting shelf DXF output.
-
-In EnergyPlus a daylighting shelf is simulated using a DaylightingDevice:Shelf object in combination with up to three other objects: a window, a heat transfer surface, and an attached shading surface.
-
-The window must be divided into two window surfaces: an upper window and a lower window. The upper window interacts directly with the daylighting shelf object and is not allowed to have any shading control devices or frames or dividers. The lower window does not interact with the daylighting shelf object, but does receive shading from the outside shelf. There are no restrictions on the lower window.
-
-The inside shelf is defined as a regular heat transfer surface in the zone. However, the surface must have the *Outside Boundary Condition* field set to Surface with itself as the other zone surface. Shading and thermal mass effects are taken into account.
-
-The outside shelf is defined as a Shading:Zone:Detailed object. The visible and solar absorptance of the outside material layer determines the reflectivity of the shelf.
-
-NOTE:  Unlike a regular Shading:Zone:Detailed object, the vertices of the outside shelf surface must be ordered so that the outward normal vector points *upward*, i.e. toward the upper window. This is necessary in order for the outside shelf to properly receive sunlight and shading from other surfaces. A mirror shading surface with the outward normal vector pointing in the opposite direction is automatically created by the program to shade the lower window.
-
-The inside shelf and outside shelf are both optional. However, if neither shelf is specified, the daylighting shelf object has no effect on the simulation.
-
-#### Field: Name
-
-The name of the daylighting shelf object.
-
-#### Field: Window Name
-
-Reference to a FenestrationSurface:Detailed object with *Surface Type* WINDOW.
-
-#### Field: Inside Shelf Name
-
-Reference to a BuildingSurface:Detailed object. This field is optional. If used, this surface must have OTHERZONESURFACE specified for the *Outside Face Environment* field and the referenced other zone surface must be itself. The number of vertices of this surface object must be 4.
-
-#### Field: Outside Shelf Name
-
-Reference to a Shading:Zone:Detailed object. This field is optional. If used, the number of vertices of this surface object must be 4.
-
-#### Field: Outside Shelf Construction Name
-
-Reference to a CONSTRUCTION object. This field is required if an outside shelf is specified. The visible and solar absorptance of the outside material layer determines the shelf reflectivity.
-
-#### Field: View Factor To Outside Shelf
-
-User defined value for the view factor from the window to the outside shelf. This field is optional. If not specified, an exact view factor is calculated for two perpendicular rectangles of the same width having a shared edge. If the given surfaces do not meet these geometric requirements, it is necessary to specify a value here.
-
-NOTE:  It is up to the user to adjust the view factor to ground of the upper window to account for the part of the view blocked by the outside shelf. The calculated *View Factor To Outside Shelf* is reported in the eio file for this purpose. For the typical case where the shelf is parallel to the ground and the upper window is perpendicular to the ground, the view factor to ground is simply:  0.5 – *View Factor To Outside Shelf*.
-
-```idf
-DaylightingDevice:Shelf,
-  Shelf,  !- Name
-  Daylit Upper Window,  !- Window Name
-  Inside Shelf,  !- Inside Shelf Name
-  Outside Shelf,  !- Outside Shelf Name
-  Shelf Construction;  !- Outside Shelf Construction Name (required if outside shelf specified)
-  ! 0.29;  !- View Factor To Outside Shelf (optional)
-
-
-FenestrationSurface:Detailed,
-  Daylit Upper Window,  !- Subsurface Name
-  Window,  !- Surface Type
-  Standard Window,  !- Construction Name
-  Daylit South Wall,  !- Base Surface Name
-  ,  !- Outside Face Environment
-  0.211,  !- VF to Ground (user must adjust to account for view factor to outside shelf)
-  ,  !- Window Shading Control (not allowed)
-  ,  !- Frame/Divider Name (not allowed)
-  1.0,  !- Multiplier (must be 1.0)
-  4,  !- Number of Vertices
-  1.0,  0.0,  2.8,
-  1.0,  0.0,  2.0,
-  4.0,  0.0,  2.0,
-  4.0,  0.0,  2.8;
-
-
- BuildingSurface:Detailed,
-  Inside Shelf,  !- Surface Name
-  Wall,  !- Surface Type
-  Shelf Construction,  !- Construction Name
-  Daylit Zone,  !- Zone Name
-  OtherZoneSurface,  !- Exterior Conditions (must be OtherZoneSurface)
-  Inside Shelf,  !- Target (must be itself)
-  NoSun,  !- Solar Exposure
-  NoWind,  !- Wind Exposure
-  0.0,  !- VF to Ground
-  4,  !- Number of Vertices
-  1.0,  0.0,  2.0,
-  4.0,  0.0,  2.0,
-  4.0,  1.0,  2.0,
-  1.0,  1.0,  2.0;
-
-
- Shading:Zone:Detailed,
-  Outside Shelf,  !- Surface Name
-  Daylit South Wall,  !- Base Surface Name
-  ,  !- Shading Transmittance Schedule (default is always opaque)
-  4,  !- Number of Vertices
-  1.0,  0.0,  2.0,  !- Outward normal vector must point up toward the upper window
-  1.0, -1.0,  2.0,
-  4.0, -1.0,  2.0,
-  4.0,  0.0,  2.0;
-```
-
-
-### Shelf Daylighting Device Output
-
-The view factor to outside shelf calculation shows up in the .eio file along with the associated window and window view factors to sky and ground:
-
-! &lt;Shelf Details&gt;,Name,View Factor to Outside Shelf,Window Name,Window View Factor to Sky,Window View Factor to Ground
-
-SHELF,0.29,DAYLIT UPPER WINDOW,0.50,0.21
-
-This variable reports the calculated *View Factor To Outside Shelf* so that the user can correctly adjust the view factor to ground of the upper window.
-
-The usual window and surface variables are relevant for the upper window:
-
-* Zone,Average,Surface Outside Face Sunlit Area [m2]
-
-* Zone,Average,Surface Outside Face Sunlit Fraction []
-
-* Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Beam Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Beam Solar Incident Angle Cosine Value[]
-
-* Zone,Average,Surface Window Transmitted Solar Radiation Rate [W]
-
-* Zone,Average,Surface Window Total Glazing Layers Absorbed Solar Radiation Rate [W]
-
-* Zone,Average,Surface Window Heat Gain Rate [W]
-
-* Zone,Average,Surface Window Heat Loss Rate [W]
-
-
-
-
-The following surface variables are reported for the outside shelf surface, if specified:
-
-* Zone,Average,Surface Outside Face Sunlit Area [m2]
-
-* Zone,Average,Surface Outside Face Sunlit Fraction []
-
-* Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Beam Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area[W/m2]
-
-* Zone,Average,Surface Outside Face Beam Solar Incident Angle Cosine Value[]
-
-
-### DaylightingDevice:LightWell
-
-This object is used to model the impacts on daylighting of a “light well� that might be associated with exterior windows such as skylights.  The light well model attenuates the light transmitted by the skylight. The attenuation is characterized by the **well efficiency**, which is the ratio of the amount of light leaving the well to the amount of light entering the well. The well efficiency varies from close to 1.0  to close to zero if there is high attenuation. The well efficiency is used only in the EnergyPlus detailed daylighting calculation, where it multiplies the beam and diffuse light transmitted by the skylight. (The well efficiency is not used in calculating the solar gain through the skylight.)
-
-The input object describes the light well using basic characteristics of the geometry along with the visible reflectance of the well’s side walls.  The following figure diagrams how the geometry is characterized.
-
-![](media/image112.svg)
-
-Figure 70. Skylight with light well: (a) perspective view, (b) vertical section.
- If the bottom of the light well is a rectangle of side lengths c and d, as shown in (a), then the perimeter of the bottom of the well = 2(c+d) and the area = cd (see description of field names for the Light Well object).
-
-#### Field: Exterior Window Name
-
-The name of the exterior window that this Light Well is associated with. Generally this is a skylight in a roof. However, light wells can be applied to an exterior window of any slope. Light wells can be assigned to both rectangular and triangular exterior windows, but they should not be assigned to interior windows. Note that the sides of the light well can be sloped and the bottom of the light well can be any shape, not  just rectangular.
-
-#### Field: Height of Well
-
-The distance from the bottom of the skylight to the bottom of the well. If the skylight and well bottom are not coplanar, this is the distance from the center of the bottom of the skylight to center of the bottom of the well. See Figure 70.
-
-#### Field: Perimeter of Bottom of Well
-
-The perimeter of the bottom opening of the well. See Figure 70.
-
-#### Field: Area of Bottom of Well
-
-The area of the bottom opening of the well. A warning will be issued if this area is less that the area of the skylight, including frame if present. See Figure 70.
-
-#### Field: Visible Reflectance of Well Walls
-
-The visible reflectance of the side walls of the well. If the walls do not all have the same reflectance, an area-weighted average value can be used.  This is the well-wall reflectance expressed as a fraction.
-
-
-
-An IDF example:
-
-```idf
-DaylightingDevice:LightWell,  ! The well is 60% reflecting, is 1.2m high and has a 2.5m x 5.5m bottom opening.
- Skylight-1, !- Name of Exterior Window that this Light Well Applies To
- 1.2,        !- Height of Well(m)
- 16.0,       !- Perimeter of Bottom of Well (m)
- 13.75,      !- Area of Bottom of Well (m2)
- 0.60;       !- Visible Reflectance of Well Walls
-```
-
-
-
-
-### Daylighting Modeling Options
-
-The following table shows what input objects/fields to use to model different daylighting options. It also gives the name of an example input, if available, that demonstrates the option.
-
-
-
-
-
-Table 21. Daylighting Modeling Options
-
-<table class="table table-striped">
-<tr>
-<th>Option</th>
-<th>Object/Field or Output Variable</th>
-<th>Input File</th>
-</tr>
-<tr>
-<td>Allow a thermal zone to be daylit</td>
-<td>Daylighting:Controls, Daylighting:DELight:Controls</td>
-<td>PurchAirWithDaylighting.idf, DElight-Detailed-Comparison.idf</td>
-</tr>
-<tr>
-<td>Specify visible transmittance of the glazing</td>
-<td>WindowMaterial:Glazing</td>
-<td>PurchAirWithDaylighting.idf</td>
-</tr>
-<tr>
-<td>Specify the visible transmittance of a shading device</td>
-<td>WindowMaterial:Shade, WindowMaterial:Screen or WindowMaterial:Blind</td>
-<td>PurchAirWindowBlind.idf</td>
-</tr>
-<tr>
-<td>Use a shading device to control glare</td>
-<td>WindowMaterial:Shade or WindowMaterial:Blind; WindowProperty:ShadingControl*</td>
-<td>PurchAirWindowBlind.idf</td>
-</tr>
-<tr>
-<td>Use electrochromic glazing to control glare</td>
-<td>WindowProperty:ShadingControl/Shading Type = SwitchableGlazing, Shading Control Type = On If High Glare, Glare Control Is Active = Yes*</td>
-<td>PurchAirWithDaylighting.idf</td>
-</tr>
-<tr>
-<td>Adjust electrochromic glazing to just meet daylighting illuminance setpoint</td>
-<td>WindowProperty:ShadingControl/Shading Type = SwitchableGlazing, Shading Control Type = MeetDaylightIlluminanceSetpoint*</td>
-<td> </td>
-</tr>
-<tr>
-<td>Print an illuminance map</td>
-<td>Daylighting:Illuminance Map*</td>
-<td> </td>
-</tr>
-<tr>
-<td>Control electric lighting response to daylight illuminance level</td>
-<td>Daylighting:Controls/Lighting Control Type = Continuous, Stepped or Continuous/Off, plus other fields; or ….
-Daylighting:DELight:Controls/Lighting Control Type = Continuous, Stepped or Continuous/Off, plus other fields</td>
-<td>PurchAirWithDaylighting.idf; DElight-Detailed-Comparison.idf</td>
-</tr>
-<tr>
-<td>Add a light shelf (with Daylighting:Controls)</td>
-<td>DaylightingDevice:Shelf *</td>
-<td>DaylightingDeviceShelf.idf</td>
-</tr>
-<tr>
-<td>Add a light shelf (with Daylighting:DELight:Controls)</td>
-<td>Daylighting:DELight:Controls</td>
-<td>DElightCFSLightShelf.idf</td>
-</tr>
-<tr>
-<td>Add a light pipe</td>
-<td>DaylightingDevice:Tubular *</td>
-<td>DaylightingDeviceTubular.idf</td>
-</tr>
-<tr>
-<td>Model a skylight having a light well</td>
-<td>DaylightingDevice:LightWell *</td>
-<td> </td>
-</tr>
-<tr>
-<td>Model daylighting through double facade</td>
-<td>See “Double Facades: Daylighting through Interior Windows�*</td>
-<td>PurchAirWithDoubleFacadeDaylighting.idf</td>
-</tr>
-<tr>
-<td>Add diffusing (translucent) glass</td>
-<td>WindowMaterial:Glazing/Solar Diffusing = Yes*</td>
-<td> </td>
-</tr>
-<tr>
-<td>Model complex fenestration</td>
-<td>Daylighting:DELight:Controls</td>
-<td>DElightCFSWindow.idf</td>
-</tr>
-<tr>
-<td>Get a radiosity-based interior light inter-reflection calculation</td>
-<td>Daylighting:DELight:Controls</td>
-<td>DElight-Detailed-Comparison.idf</td>
-</tr>
-<tr>
-<td>Find effect on daylighting of solar reflected from overhangs, neighboring buildings, etc.</td>
-<td>Building/SolarDistribution uses “withReflections� option</td>
-<td> </td>
-</tr>
-<tr>
-<td>Find visible transmittance effect of dirt on window</td>
-<td>WindowMaterial:Glazing/Dirt Correction Factor for Solar and Visible Transmittance*</td>
-<td> </td>
-</tr>
-</table>
-
-\*Used only with Daylighting:Controls
-
-
-
-
-
-------------------------------------------------------------------------
-
-[[1]](#_ftnref1) Formerly, only the exterior windows in a zone could provide daylight to that zone.
-
-
-
-Group – Exterior Energy Use Equipment
--------------------------------------
-
-To facilitate the reporting of exterior consumption (to the building’s heat balance/loads considerations), several objects have been included. The consumption related to these items will appear on meters specific to the items.
-
-### Exterior:Lights
-
-#### Field: Name
-
-This descriptive name allows the values of exterior lights consumption to appear in the “normal� output variable list as well as the meters. It cannot be blank nor can it be duplicated by other Exterior:Lights statements.
-
-#### Field: Schedule Name
-
-A schedule will allow the exterior lights consumption to be operationally different, hour to hour as well as seasonally. Fractional values in the basic schedule will be applied to the design level field below.
-
-#### Field: Design Level
-
-This field (in Watts) is typically used to represent the maximum electrical input to exterior lighting fixtures that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the lighting design level could be a “diversity factor� applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour and seasonally, the design level field is constant for all simulation environments.
-
-#### Field: Control Option
-
-This field is used to determine how the exterior lights are controlled. There are currently two options, ‘ScheduleNameOnly’ and ‘AstronomicalClock.’  If this field is omitted or left blank then the program will default to Schedule Name Only mode. The ‘ScheduleNameOnly’ mode dictates that the exterior lights always follow the schedule named in the field above. The ‘AstronomicalClock’ mode dictates that despite what the schedule indicates, the exterior lights will not run when the sun is up. Using the Astronomical Clock mode makes it simple to model exterior lights that are controlled by a photocell or other controller that ensures that outdoor lights will not run during the daytime. However, the Astronomical Clock control works off of the position of the sun and therefore does not operate exactly like a photocell. During the night, the schedule values are still applied in the usual way.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Grounds Lights", "Facade Lights", etc. A new meter for reporting is created for each unique subcategory  (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the lights will be assigned to the "General" end-use subcategory.
-
-An IDF Example:
-
-```idf
-Exterior:Lights,
-  OutsideLights,       !- Name
-  ON,                  !- SCHEDULE Name
-  1000,                !- Design Level
-  AstronomicalClock,  !- Control Option
-  Grounds Lights;      !- End-Use Subcategory
-```
-
-
-### Exterior Lights Outputs
-
-Output for exterior lights appears in three possible places. It will appear on two meters (Electricity:Facility and ExteriorLights:Electricity) as well as in its own designated value in the standard output file.
-
-Output for exterior lights appears in three possible places. It will appear on two meters (Electricity:Facility and ExteriorLights:Electricity) as well as in its own designated value in the standard output file.
-
-* Zone,Average,Exterior Lights Electric Power [W]
-
-* Zone,Sum,Exterior Lights Electric Energy [J]
-
-#### Exterior Lights Electric Power [W]
-
-#### Exterior Lights Electric Energy [J]
-
-These are the electric power and energy consumed by the exterior lights.
-
-### Exterior:FuelEquipment
-
-#### Field: Name
-
-This descriptive name allows the values of exterior equipment consumption to appear in the “normal� output variable list as well as the meters. It cannot be blank nor can it be duplicated by other Exterior:FuelEquipment or Exterior:WaterEquipment statements.
-
-#### Field: Fuel Use Type
-
-This field designates the appropriate meter for the exterior fuel equipment. Valid fuel types are: Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Diesel, Gasoline, Coal, Steam, DistrictHeating, DistrictCooling, OtherFuel1 and OtherFuel2. The fuel type triggers the application of consumption amounts to the appropriate energy meters.
-
-#### Field: Schedule Name
-
-A schedule will allow the exterior lights consumption to be operationally different, hour to hour as well as seasonally. Fractional values in the basic schedule will be applied to the design level field below.
-
-#### Field: Design Level
-
-This field (Watts) is typically used to represent the maximum input to exterior fixtures that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the design level could be a “diversity factor� applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour and seasonally, the design level field is constant for all simulation environments.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Fountains", etc. A new meter for reporting is created for each unique subcategory  (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the "General" end-use subcategory.
-
-
-
-IDF Examples:
-
-```idf
-Exterior:FuelEquipment,OutsideGasEq,Gas,ON,1000;
-Exterior:FuelEquipment,OutsideCoalEq,Coal,ON,1000;
-Exterior:FuelEquipment,OutsideFuelOil1Eq,FuelOil#1,ON,1000;
-Exterior:FuelEquipment,OutsideFuelOil2Eq,FuelOil#2,ON,1000;
-Exterior:FuelEquipment,OutsideLPGEq,PropaneGas,ON,1000;
-```
-
-
-### Exterior:WaterEquipment
-
-#### Field: Name
-
-This descriptive name allows the values of exterior equipment consumption to appear in the “normal� output variable list as well as the meters. It cannot be blank nor can it be duplicated by other Exterior:FuelEquipment or Exterior:WaterEquipment statements.
-
-#### Field: FuelUseType
-
-For Exterior:WaterEquipment, only “Water� is current allowed for this field.
-
-#### Field: Schedule Name
-
-A schedule will allow the exterior water consumption to be operationally different, hour to hour as well as seasonally. Fractional values in the basic schedule will be applied to the design level field below.
-
-#### Field: Design Level
-
-This field (in m3/s) is typically used to represent the maximum volumetric flow for water fixtures that is then multiplied by a schedule fraction (see previous field). In EnergyPlus, this is slightly more flexible in that the exterior water equipment design level could be a “diversity factor� applied to a schedule of real numbers. Note that while the schedule value can vary from hour to hour and seasonally, the design level field is constant for all simulation environments.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Landscaping", etc. A new meter for reporting is created for each unique subcategory  (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the equipment will be assigned to the "General" end-use subcategory.
-
-IDF Example:
-
-Exterior:WaterEquipment,OutsideWaterEq,Water,ON,10000;
-
-### Exterior Fuel Equipment, Exterior Water Equipment Outputs
-
-Output for exterior equipment consumption appears in three possible places. It will appear on two meters (&lt;Fuel Type&gt;:Facility and ExteriorEquipment:&lt;Fuel Type&gt;) as well as in its own designated value in the standard output file, Exterior Equipment &lt;Fuel Type&gt; Energy. Consumption also appears on any user-defined end-use subcategory meters, i.e., &lt;End-Use Subcategory&gt;:ExteriorEquipment:&lt;Fuel Type&gt;. All outputs are in [J] except water consumption which is in [m3]. There are also rate versions
-
-* Zone, Average, Exterior Equipment Fuel Rate [W]
-
-* Zone,Sum, Exterior Equipment Electric Energy [J]
-
-* Zone,Sum, Exterior Equipment Gas Energy [J]
-
-
-
-* Zone,Average, Exterior Equipment Water Volume Flow Rate [m3/s]
-
-* Zone,Sum, Exterior Equipment Water Volume [m3]
-
-* Zone,Sum, Exterior Equipment Mains Water Volume [m3]
-
-
-
-* Zone,Sum, Exterior Equipment Coal Energy [J]
-
-* Zone,Sum, Exterior Equipment FuelOil\#1 Energy [J]
-
-* Zone,Sum, Exterior Equipment FuelOil\#2 Energy [J]
-
-
-
-* Zone,Sum, Exterior Equipment Propane Energy [J]
-
-
-
-* Zone,Sum, Exterior Equipment Gasoline Energy [J]
-
-
-
-* Zone,Sum, Exterior Equipment Diesel Energy [J]
-
-* Zone,Sum, Exterior Equipment Steam Energy [J]
-
-* Zone,Sum, Exterior Equipment OtherFuel1 Energy [J]
-
-* Zone,Sum, Exterior Equipment OtherFuel2 Energy [J]
-
-* Zone,Sum, Exterior Equipment District Heating Energy [J]
-
-* Zone,Sum, Exterior Equipment District Cooling Energy [J]
-
-
-
-
-#### Exterior Equipment Fuel Rate [W]
-
-#### Exterior Equipment &lt;Fuel Type&gt; Energy [J]
-
-These are the fuel consumption rate and energy for the exterior equipment.
-
-#### Exterior Equipment Water Volume Flow Rate [m3/s]
-
-#### Exterior Equipment Water Volume [m3]
-
-These are the water consumption rate and volume for the exterior equipment.
-
-Exterior Equipment Mains Water Volume [m3]This is the water volume drawn for the mains water service to serve the exterior equipment.
-
-Group – Airflow
----------------
-
-An important characteristic of energy consumption in buildings is the airflow between zones and airflow due to natural ventilation (e.g., open windows) or mechanically-induced ventilation (e.g., exhaust air fans). This group of objects describes those elements.
-
-The AirflowNetwork model can also be used to model infiltration and mixing (zone-to-zone air flow) with or without the HVAC air distribution system operating (see Group – Airflow Network).
-
-### ZoneInfiltration:DesignFlowRate
-
-Infiltration is the unintended flow of air from the outdoor environment directly into a thermal zone. Infiltration is generally caused by the opening and closing of exterior doors, cracks around windows, and even in very small amounts through building elements. The basic equation used to calculate infiltration with this object is:
-
-<div>\[Infiltration = \left( {{I_{design}}} \right)\left( {{F_{schedule}}} \right)\left[ {A + B\left| {\left( {{T_{zone}} - {T_{odb}}} \right)} \right| + C\left( {WindSpeed} \right) + D\left( {Windspee{d^2}} \right)} \right]\]</div>
-
-More advanced infiltration calculations are possible using the EnergyPlus AirflowNetwork model for natural infiltration driven by wind and/or by forced air. Infiltration described by the equation shown above is entered into EnergyPlus using the following syntax. Exfiltration (the leakage of zone air to the outside) is generally handled better as zone exhaust air in the zone equipment description. The equation must always yield a non-negative results; negative values are set to 0.0.
-
-The question of typical values for these coefficients is subject to debate. Ideally, one should do a detailed analysis of the infiltration situation and then determine a custom set of coefficients using methods such as those laid out in Chapter 26 of the ASHRAE Handbook of Fundamentals. The EnergyPlus defaults are 1,0,0,0 which give a constant volume flow of infiltration under all conditions.
-
-BLAST (one of the EnergyPlus predecessors) used the following values as defaults:  0.606, 0.03636, 0.1177, 0. These coefficients produce a value of 1.0 at 0C deltaT and 3.35 m/s (7.5 mph) windspeed, which corresponds to a typical summer condition. At a winter condition of 40C deltaT and 6 m/s (13.4 mph) windspeed, these coefficients would increase the infiltration rate by a factor of 2.75.
-
-In DOE-2 (the other EnergyPlus predecessor), the air change method defaults are (adjusted to SI units) 0, 0, 0.224 (windspeed), 0. With these coefficients, the summer conditions above would give a factor of 0.75, and the winter conditions would give 1.34. A windspeed of 4.47 m/s (10 mph) gives a factor of 1.0.
-
-The source of the BLAST defaults is noted in the BLAST documentation as:
-
-"Empirical equation and the coefficient default were determined from ASHRAE journal articles and other data on the effects of outdoor weather conditions."
-
-The source of the DOE-2 defaults is based on examining the infiltration relationships described in the ASHRAE Handbook of Fundamentals.
-
-The EnergyPlus example files use all of the above, the BLAST defaults in some (e.g., GeometryTest), the DOE-2 defaults in some (e.g., 5ZoneAirCooled), and the EnergyPlus defaults in some (e.g., LgOffVAVDetCoil).
-
-The local outdoor dry-bulb temperature used in the above basic equation (T<sub>odb</sub>) is typically a function of the height of the zone centroid above ground. The corresponding zone name is given in the second field. The local outdoor dry-bulb temperature calculation procedure is given in the section of “Local Outdoor Air Temperature Calculation� in the Engineering Reference.
-
-The local outdoor wind speed used in the above basic equation (WindSpeed) is also a function of the height of the zone centroid above ground. The corresponding zone name is given in the second filed. The local outdoor wind speed calculation procedure is given in the section of “Local Wind Speed Calculation� in the Engineering Reference.
-
-Note: When the value of the Wind Speed Profile Exponent field in the Site:HeightVariation is equal to 0.0. The local wind speed is always equal to the wind speed given in the weather data and will not be dependent on zone centroid height.  Similarly, if the value of the Air Temperature Gradient Coefficient is set equal to 0 the local air dry-bulb temperature is also always equal to the air dry-bulb temperature given in the weather data and will not be dependent on zone centroid height.
-
-One or more infiltration objects can be defined for each zone, and the resulting infiltration rate for the zone will simply be the summation of the flow rates specified by the infiltration objects.
-
-#### Field: Name
-
-The name of the ZoneInfiltration:DesignFlowRate object. This needs to be unique across all different ZoneInfiltration objects.
-
-#### Field: Zone or ZoneList Name
-
-This field is the name of the zone (ref: Zone) or ZoneList (ref: ZoneLIst) and attaches a particular infiltration statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this infiltration definition is applied to each of the zones in the zone list effecting a global definition for the amount of infiltration flow rate in the zone. The Zonelist option can be used effectively with the flow/area, flow/exteriorarea, flow/exteriorwallarea, or airchanges/hour of the Design Flow Rate Calculation Method.
-
-The name of the actual infiltration object becomes &lt;Zone Name&gt; &lt;ZoneInfiltration:DesignFlowRate Object Name&gt; and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design volume flow rate (I<sub>design</sub>) (see Design Flow Rate Calculation Method field and related subsequent fields). This fraction between 0.0 and 1.0 is noted as F<sub>schedule</sub> in the above equation.
-
-#### Field: Design Flow Rate Calculation Method
-
-This field is a key/choice field that tells which of the next four fields are filled and is descriptive of the method for calculating the design volume flow rate. The key/choices are:
-
-- Flow/Zone
-
-With this choice, the method used will be a straight insertion of the design volume flow rate.  (The Design Flow Rate field should be filled.)
-
-- Flow/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The flow per Zone Area field should be filled).
-
-- Flow/ExteriorArea
-
-With this choice, the method used will be a factor per exterior surface area of the zone. (The flow per Exterior Surface Area field should be filled).
-
-- Flow/ExteriorWallArea
-
-With this choice, the method used will be a factor per exterior wall surface area of the zone. (The flow per Exterior Surface Area field should be filled).
-
-- AirChanges/Hour
-
-With this choice, the method used will be the number of air changes per hour for the infiltration amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. (The Air Changes per Hour field should be filled).
-
-#### Field: Design Flow Rate
-
-This field denotes the full design volume flow rate (m<sup>3</sup>/s). The previous field should choose “flow/zone� as the choice. The design volume flow rate (noted as I<sub>design</sub> in the above equation) is the maximum amount of infiltration expected at design conditions. The design value is modified by the schedule fraction (see Field:Schedule Name) and user specified coefficients (see �coefficient� fields below). The resulting volume flow rate is converted to mass flow using the current outdoor air density at each time step.
-
-#### Field: Flow per Zone Floor Area
-
-This factor (m<sup>3</sup>/s-m<sup>2</sup>) is used, along with the Zone Area to determine the maximum Design Flow Rate as described in the Design Flow Rate field. The choice from the method field should be “Flow/Area�.
-
-#### Field: Flow per Exterior Surface Area
-
-This factor (m<sup>3</sup>/s-m<sup>2</sup>) is used, along with the Exterior Surface Area in the Zone to determine the maximum Design Flow Rate as described in the Design Flow Rate field. The choice from the method field should be “Flow/Exteriorarea� or “Flow/ExteriorWallArea�.
-
-#### Field: Air Changes per Hour
-
-This factor is used, along with the Zone Volume to determine the maximum Design Flow Rate as described in the Design Flow Rate field. The choice from the method field should be “AirChanges/Hour�.
-
-#### Field: Constant Term Coefficient
-
-This number is the “A� parameter in the above infiltration equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter, however, is a constant under all conditions and is not modified by any environmental effect. As a result, it is dimensionless.
-
-#### Field: Temperature Term Coefficient
-
-This number is the “B� parameter in the above infiltration equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the temperature difference between the outdoor and indoor air dry-bulb temperatures. The units for this parameter are inverse Celsius.
-
-#### Field: Velocity Term Coefficient
-
-This number is the “C� parameter in the above infiltration equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the speed of wind being experienced outside the building. The units for this parameter are s/m.
-
-#### Field: Velocity Squared Term Coefficient
-
-This number is the “D� parameter in the above infiltration equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by square of the speed of wind being experienced outside the building. The units for this parameter are s<sup>2</sup>/m<sup>2</sup>.
-
-An IDF example:
-
-```idf
-ZoneInfiltration:DesignFlowRate,
-  Infiltration 1,   !- Name
-  DORM ROOMS AND COMMON AREAS, !- Zone Name
-  Infiltration Sch, !- Schedule Name
-  Flow/Zone,      !- Design Flow Rate Calculation Method
-  2.831685,       !- Design Flow Rate {m3/s}
-  ,               !- Flow per Zone Floor Area {m3/s/m2}
-  ,               !- Flow per Exterior Surface Area {m3/s/m2}
-  ,               !- Air Changes per Hour
-  0.6060000    ,  !- Constant Term Coefficient
-  3.6359996E-02,  !- Temperature Term Coefficient
-  0.1177165    ,  !- Velocity Term Coefficient
-  0.0000000E+00;  !- Velocity Squared Term Coefficient
-```
-
-
-Global Infiltration example:
-
-```idf
-  ZoneList,OfficeZones,Left Fork, Middle Fork, Right Fork;
-
-
-  ZoneInfiltration:DesignFlowRate,
-    OfficeZones Infiltration,       !- Name
-    OfficeZones,             !- Zone or ZoneList Name
-    Infiltration Sch,        !- Schedule Name
-    AirChanges/Hour,         !- Design Flow Rate Calculation Method
-    ,                        !- Design Flow Rate {m3/s}
-    ,                        !- Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Flow per Exterior Surface Area {m3/s-m2}
-    4.7,                     !- Air Changes per Hour
-    0.6060000,               !- Constant Term Coefficient
-    3.6359996E-02,           !- Temperature Term Coefficient
-    0.1177165,               !- Velocity Term Coefficient
-    0.0000000E+00;           !- Velocity Squared Term Coefficient
-```
-
-
-
-
-### ZoneInfiltration:EffectiveLeakageArea
-
-ZoneInfiltration:EffectiveLeakageArea model is similar to the other infiltration objects but uses a different equation to model the unintended flow of air from the outdoor environment directly into a thermal zone.  Infiltration is generally caused by the opening and closing of exterior doors, cracks around windows, and even in very small amounts through building elements.  This model is based on work by Sherman and Grimsrud (1980) and is appropriate for smaller, residential-type buildings.  The equation used to calculate infiltration in the effective leakage area model is:
-
-<div>\[Infiltration = \left( {{F_{Schedule}}} \right)\frac{{{A_L}}}{{1000}}\sqrt {{C_s}\Delta T + {C_w}{{\left( {WindSpeed} \right)}^2}} \]</div>
-
-where <span>\(\Delta T\)</span> is the average difference between zone air temperature and the outdoor air temperature and the other coefficients are described below.
-
-Note that the coefficients for the “EffectiveLeakageArea� model are not interchangeable with the similarly named coefficients in the “FlowCoefficient� model (see ZoneInfiltration:FlowCoefficient object).
-
-One or more infiltration objects of different types can be defined for each zone, and the resulting infiltration rate for the zone will simply be the summation of the flow rates specified by the infiltration objects.
-
-#### Field: Name
-
-The name of the ZoneInfiltration:EffectiveLeakageArea object.  This needs to be unique across all different ZoneInfiltration objects.
-
-#### Field: Zone Name
-
-This field is the name of the zone (ref: Zone) and attaches a particular infiltration statement to a thermal zone in the building.
-
-#### Field: Schedule Name
-
-This field is the name of a schedule (ref: Schedule) that modifies the volume flow rate calculated by the model. This fraction between 0.0 and 1.0 is noted as F<sub>schedule</sub> in the above equation.
-
-#### Field: Effective Air Leakage Area
-
-This field is the effective air leakage area, in cm<sup>2</sup>, at 4 Pa.  This is the value <span>\({A_L}\)</span>in the equation above.  Effective leakage area data can be obtained from a whole-building pressure test (eg. blower door test).  ASHRAE Handbook of Fundamentals also lists typical values component leakage areas for low-rise residential (e.g. Table 1 in Chapter 26 of HoF 2001).  The value should correspond to a pressure difference of 4 Pa.
-
-#### Field: Stack Coefficient
-
-This field is the value of the stack coefficient, <span>\({C_s}\)</span> in the equation above.  The coefficient has units of (L/s)<sup>2</sup>/(cm<sup>4</sup>·K).  Values for the “Basic Model Stack Coefficient� listed in the ASHRAE Handbook of Fundamentals (2005 and 2001) are:
-
-
-
-<table class="table table-striped">
-<tr>
-<th>One story house</th>
-<th>Two story house</th>
-<th>Three story house</th>
-</tr>
-<tr>
-<td>0.000145</td>
-<td>0.000290</td>
-<td>0.000435</td>
-</tr>
-</table>
-
-
-
-#### Field: Wind Coefficient
-
-This field is the value of the wind coefficient, <span>\({C_w}\)</span> in the equation above.  The coefficient has units of (L/s)<sup>2</sup>/(cm<sup>4</sup>·(m/s)<sup>2</sup>).  Values for the “Basic Model Wind Coefficient� listed in the ASHRAE Handbook of Fundamentals (2005 chapter 27; 2001, Chapter 26) depend on the type of shelter and are listed in the following tables.
-
-
-
-<table class="table table-striped">
-<tr>
-<th>Shelter class</th>
-<th>One story house</th>
-<th>Two story house</th>
-<th>Three story house</th>
-</tr>
-<tr>
-<td>1</td>
-<td>0.000319</td>
-<td>0.000420</td>
-<td>0.000494</td>
-</tr>
-<tr>
-<td>2</td>
-<td>0.000246</td>
-<td>0.000325</td>
-<td>0.000382</td>
-</tr>
-<tr>
-<td>3</td>
-<td>0.000174</td>
-<td>0.000231</td>
-<td>0.000271</td>
-</tr>
-<tr>
-<td>4</td>
-<td>0.000104</td>
-<td>0.000137</td>
-<td>0.000161</td>
-</tr>
-<tr>
-<td>5</td>
-<td>0.000032</td>
-<td>0.000042</td>
-<td>0.000049</td>
-</tr>
-</table>
-
-
-
-<table class="table table-striped">
-<tr>
-<th>Shelter class</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>1</td>
-<td>No obstructions or local shielding</td>
-</tr>
-<tr>
-<td>2</td>
-<td>Typical shelter for an isolated rural house</td>
-</tr>
-<tr>
-<td>3</td>
-<td>Typical shelter caused by other buildings across the street</td>
-</tr>
-<tr>
-<td>4</td>
-<td>Typical shelter for urban buildings on larger lots</td>
-</tr>
-<tr>
-<td>5</td>
-<td>Typical shelter produced by buildings that are immediately adjacent.</td>
-</tr>
-</table>
-
-
-
-An example IDF object is
-
-```idf
-ZoneInfiltration:EffectiveLeakageArea,
-    LIVING ZONE Infil 1,     !- Name
-    LIVING ZONE,             !- Zone Name
-    INF-SCHED,               !- Schedule Name
-    500.0,                   !- Effective Air Leakage Area
-    0.000145,                !- Stack Coefficient
-    0.000174 ;               !- Wind Coefficient
-```
-
-
-
-
-### ZoneInfiltration:FlowCoefficient
-
-ZoneInfiltration:FlowCoefficient model is similar to the other infiltration objects but uses a different equation to model the unintended flow of air from the outdoor environment directly into a thermal zone.  Infiltration is generally caused by the opening and closing of exterior doors, cracks around windows, and even in very small amounts through building elements.  This reformulated model is based on the AIM-2 model by Walker and Wilson (1998) and is appropriate for smaller, residential-type buildings.  The equation used to calculate infiltration in the flow coefficient model is:
-
-<div>\[Infiltration = \left( {{F_{Schedule}}} \right)\sqrt {{{\left( {c\,{C_s}\Delta {T^n}} \right)}^2} + {{\left( {c\,{C_w}{{\left( {s * WindSpeed} \right)}^{2n}}} \right)}^2}} \]</div>
-
-Where <span>\(\Delta T\)</span> is the average difference between zone air temperature and the outdoor air temperature and the other coefficients are described below.
-
-Note that the coefficients for the “Flow Coefficient� model are not interchangeable with the similarly named coefficients in the “Effective Leakage Area� model (see ZoneInfiltration:EffectiveLeakageArea object).
-
-One or more infiltration objects of different types can be defined for each zone, and the resulting infiltration rate for the zone will simply be the summation of the flow rates specified by the infiltration objects.
-
-#### Field: Name
-
-The name of the ZoneInfiltration:FlowCoefficient object. This needs to be unique across all different ZoneInfiltration objects.
-
-#### Field: Zone Name
-
-This field is the name of the zone (ref: Zone) and attaches a particular infiltration statement to a thermal zone in the building.
-
-#### Field: Schedule Name
-
-This field is the name of a schedule (ref: Schedule) that modifies the volume flow rate calculated by the model. This fraction between 0.0 and 1.0 is noted as F<sub>schedule</sub> in the above equation.
-
-#### Field: Flow Coefficient
-
-This field is the flow coefficient in m<sup>3</sup>/(s·Pa<sup>n</sup>).  This is the value <span>\(c\)</span> in the equation above.  The flow coefficient can be determined from the effective leakage area and whole-building pressure tests (eg. blower door test).
-
-#### Field: Stack Coefficient
-
-This field is the value of the stack coefficient, <span>\({C_s}\)</span> in the equation above.  The coefficient has units of (Pa/K)<sup>n</sup>. Values for the “Enhanced Model Stack Coefficient� listed in the ASHRAE Handbook of Fundamentals (2005 and 2001) are:
-
-
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>One story house</th>
-<th>Two story house</th>
-<th>Three story house</th>
-</tr>
-<tr>
-<td>With Flue</td>
-<td>0.069</td>
-<td>0.089</td>
-<td>0.107</td>
-</tr>
-<tr>
-<td>No Flue</td>
-<td>0.054</td>
-<td>0.078</td>
-<td>0.098</td>
-</tr>
-</table>
-
-
-
-#### Field: Pressure Exponent
-
-This field is the value of the pressure exponent, *n* in the equation above.  The pressure exponent generally lies between 0.6 and 0.7 with a typical value of *n* = 0.67 for the enhanced model.
-
-#### Field: Wind Coefficient
-
-This field is the value of the wind coefficient, <span>\({C_w}\)</span> in the equation above.  The coefficient has units of (Pa·s<sup>2</sup>/m<sup>2</sup>)<sup>n</sup> .  Values for the “Enhanced Model Wind Coefficient� listed in the ASHRAE Handbook of Fundamentals (2005 and 2001) are:
-
-
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>One story house</th>
-<th>Two story house</th>
-<th>Three story house</th>
-</tr>
-<tr>
-<td>Basement/slab; With Flue</td>
-<td>0.142</td>
-<td>0.156</td>
-<td>0.167</td>
-</tr>
-<tr>
-<td>Basement/slab; No Flue</td>
-<td>0.156</td>
-<td>0.170</td>
-<td>0.170</td>
-</tr>
-<tr>
-<td>Crawlspace; With Flue</td>
-<td>0.128</td>
-<td>0.142</td>
-<td>0.154</td>
-</tr>
-<tr>
-<td>Crawlspace;
-No Flue</td>
-<td>0.128</td>
-<td>0.142</td>
-<td>0.151</td>
-</tr>
-</table>
-
-
-
-#### Field: Shelter Factor
-
-This field is the value of the wind coefficient, <span>\(s\)</span> in the equation above.  The coefficient is dimensionless.  Values for the “Enhanced Model Shelter Factor� listed in the ASHRAE Handbook of Fundamentals (2005 and 2001) are:
-
-<table class="table table-striped">
-<tr>
-<th>Shelter class</th>
-<th>No Flue</th>
-<th>One story house with flue</th>
-<th>Two story house with flue</th>
-<th>Three story house with flue</th>
-</tr>
-<tr>
-<td>1</td>
-<td>1.00</td>
-<td>1.10</td>
-<td>1.07</td>
-<td>1.06</td>
-</tr>
-<tr>
-<td>2</td>
-<td>0.90</td>
-<td>1.02</td>
-<td>0.98</td>
-<td>0.97</td>
-</tr>
-<tr>
-<td>3</td>
-<td>0.70</td>
-<td>0.86</td>
-<td>0.81</td>
-<td>0.79</td>
-</tr>
-<tr>
-<td>4</td>
-<td>0.50</td>
-<td>0.70</td>
-<td>0.64</td>
-<td>0.61</td>
-</tr>
-<tr>
-<td>5</td>
-<td>0.30</td>
-<td>0.54</td>
-<td>0.47</td>
-<td>0.43</td>
-</tr>
-</table>
-
-
-
-<table class="table table-striped">
-<tr>
-<th>Shelter class</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>1</td>
-<td>No obstructions or local shielding</td>
-</tr>
-<tr>
-<td>2</td>
-<td>Typical shelter for an isolated rural house</td>
-</tr>
-<tr>
-<td>3</td>
-<td>Typical shelter caused by other buildings across the street</td>
-</tr>
-<tr>
-<td>4</td>
-<td>Typical shelter for urban buildings on larger lots</td>
-</tr>
-<tr>
-<td>5</td>
-<td>Typical shelter produced by buildings that are immediately adjacent.</td>
-</tr>
-</table>
-
-An Example IDF object is:
-
-```idf
-ZoneInfiltration:FlowCoefficient,
-    LIVING ZONE Infil 1,     !- Name
-    LIVING ZONE,             !- Zone Name
-    INF-SCHED,               !- Schedule Name
-    0.05,                    !- Flow Coefficient
-    0.089,                   !- Stack Coefficient
-     0.67  ,                 !- Pressure Exponent
-    0.156 ,                  !- Wind Coefficient
-    0.64;                    !- Shelter Factor
-```
-
-
-
-
-### ZoneInfiltration Outputs
-
-* HVAC,Sum,Zone Infiltration Sensible Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Infiltration Sensible Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Infiltration Latent Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Infiltration Latent Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Infiltration Total Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Infiltration Total Heat Gain Energy [J]
-
-* HVAC,Average,Zone Infiltration Current Density Volume Flow Rate [m3/s]
-
-* HVAC,Average,Zone Infiltration Standard Density Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Infiltration Current Density Volume [m3]
-
-* HVAC,Sum,Zone Infiltration Standard Density Volume [m3]
-
-* HVAC,Sum,Zone Infiltration Mass [kg]
-
-* HVAC,Sum,Zone Infiltration Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Infiltration Air Change Rate [ach]
-
-
-Note: If ZoneInfiltration:\* objects and ZoneAirBalance:OutdoorAir (with Air Balance Method = Quadrature) objects reference the same Zone Name, the above infiltration output variables will not be reported for that zone. Instead, output variables for zone outdoor air flow will be reported by the corresponding ZoneAirBalance:OutdoorAir object.
-
-#### Zone Infiltration Sensible Heat Loss Energy [J]
-
-The sensible (temperature) heat loss that occurs when the infiltration air temperature (outdoor) &lt; zone air temperature.
-
-#### Zone Infiltration Sensible Heat Gain Energy [J]
-
-The sensible (temperature) heat gain that occurs when the infiltration air temperature (outdoor) &gt;= zone air temperature.
-
-#### Zone Infiltration Latent Heat Loss Energy [J]
-
-The latent heat loss that occurs when the infiltration air humidity ratio (outdoor) &lt; zone air humidity ratio.
-
-#### Zone Infiltration Latent Heat Gain Energy [J]
-
-The latent heat gain that occurs when the infiltration air humidity ratio (outdoor) &gt;= zone air humidity ratio.
-
-#### Zone Infiltration Total Heat Loss Energy [J]
-
-The total heat loss that occurs when the sum of Zone Infiltration Sensible Heat Gain Energy and Zone Infiltration Latent Heat Gain Energy &lt; the sum of Zone Infiltration Sensible Heat Loss Energy and Zone Infiltration Latent Heat Loss Energy.
-
-#### Zone Infiltration Total Heat Gain Energy [J]
-
-The total heat gain that occurs when the sum of Zone Infiltration Sensible Heat Gain Energy and Zone Infiltration Latent Heat Gain Energy &gt;= the sum of Zone Infiltration Sensible Heat Loss Energy and Zone Infiltration Latent Heat Loss Energy.
-
-#### Zone Infiltration Current Density Volume  [m3]
-
-#### Zone Infiltration Current Density Volume Flow Rate [m3/s]
-
-These outputs are the total volume and volume flow rate of infiltration air based on the current density of zone air.
-
-#### Zone Infiltration Standard Density Volume [m3]
-
-#### Zone Infiltration Standard Density Volume Flow Rate [m3/s]
-
-These outputs are the total volume and volume flow rate of infiltration air based on the standard density of air.  Standard density in EnergyPlus corresponds to 20ºC drybulb, dry air, and nominally adjusted for elevation.
-
-#### Zone Infiltration Mass [kg]
-
-The mass flow of the Infiltration air.
-
-#### Zone Infiltration Mass Flow Rate [kg/s]
-
-The mass flow rate of the Infiltration air.
-
-#### Zone Infiltration Air Change Rate [ach]
-
-The rate of infiltration in air changes per hour.
-
-### ZoneVentilation:DesignFlowRate
-
-Ventilation is the purposeful flow of air from the outdoor environment directly into a thermal zone in order to provide some amount of non-mechanical cooling. Ventilation, as specified by the input syntax for the ZoneVentilation:DesignFlowRate object, is intended to model “simple� ventilation as opposed to the more detailed ventilation investigations that can be performed with the AirflowNetwork model or with air systems that have outdoor air mixers. Zone ventilation, as specified via this input object, can be controlled by a schedule and through the specification of minimum, maximum and delta temperatures as described below. The temperatures can be either single constant values for the entire simulation or schedules which can vary over time. As with infiltration, the actual flow rate of ventilation air can be modified by the temperature difference between the inside and outside environment and the wind speed. The basic equation used to calculate ventilation with this model is:
-
-<div>\[Ventilation = \left( {{V_{design}}} \right)\left( {{F_{schedule}}} \right)\left[ {A + B\left| {{T_{zone}} - {T_{odb}}} \right| + C\left( {WindSpeed} \right) + D\left( {WindSpee{d^2}} \right)} \right]\]</div>
-
-Similar to infiltration, the question of typical values for these coefficients is subject to debate. Ideally, one should do a detailed analysis of the ventilation situation and then determine a custom set of coefficients using methods such as those laid out in Chapter 26 of the ASHRAE Handbook of Fundamentals. The EnergyPlus defaults are 1,0,0,0 which give a constant volume flow of ventilation under all conditions. The following discussion is duplicated from the infiltration design flow rate object. The equation must always yield a non-negative results; negative values are set to 0.0.
-
-BLAST (one of the EnergyPlus predecessors) used the following values as defaults:  0.606, 0.03636, 0.1177, 0. These coefficients produce a value of 1.0 at 0C deltaT and 3.35 m/s (7.5 mph) windspeed, which corresponds to a typical summer condition. At a winter condition of 40C deltaT and 6 m/s (13.4 mph) windspeed, these coefficients would increase the infiltration rate by a factor of 2.75.
-
-In DOE-2 (the other EnergyPlus predecessor), the air change method defaults are (adjusted to SI units) 0, 0, 0.224 (windspeed), 0. With these coefficients, the summer conditions above would give a factor of 0.75, and the winter conditions would give 1.34. A windspeed of 4.47 m/s (10 mph) gives a factor of 1.0.
-
-The source of the BLAST defaults is noted in the BLAST documentation as:
-
-"Empirical equation and the coefficient default were determined from ASHRAE journal articles and other data on the effects of outdoor weather conditions."
-
-The source of the DOE-2 defaults is based on examining the *infiltration* relationships described in the ASHRAE Handbook of Fundamentals.
-
-The local outdoor dry-bulb temperature used in the above basic equation (T<sub>odb</sub>) is typically a function of the height of the zone centroid above ground. The corresponding zone name is given in the second field. The local outdoor dry-bulb temperature calculation procedure is described in the “Local Outdoor Air Temperature Calculation� section of the Engineering Reference.
-
-The local outdoor wind speed used in the above basic equation (WindSpeed) is also a function of the height of the zone centroid above ground. The corresponding zone name is given in the second field. The local outdoor wind speed calculation procedure is described in the “Local Wind Speed Calculation� section of the Engineering Reference.
-
-Note: When the value of the Wind Speed Profile Exponent field in the Site:HeightVariation object is equal to 0.0, the local wind speed is always equal to the wind speed given in the weather data and will not be dependent on zone centroid height.  Similarly, if the value of the Air Temperature Gradient Coefficient is set equal to 0, the local air dry-bulb temperature is also always equal to the air dry-bulb temperature given in the weather data and will not be dependent on zone centroid height.
-
-One or more ventilation objects (i.e., ZoneVentilation:DesignFlowRate and/or ZoneVentilation:WindandStackOpenArea) can be defined for each zone, and the resulting ventilation rate for the zone will simply be the summation of the flow rates specified by the ventilation objects.
-
-More advanced ventilation calculations are possible using the EnergyPlus AirflowNetwork model.
-
-#### Field: Name
-
-The name of the ZoneVentilation:DesignFlowRate object.
-
-#### Field: Zone or ZoneList Name
-
-This field is the name of the zone (ref: Zone) or ZoneList (ref: ZoneList) and attaches a particular ventilation statement to a thermal zone or set of thermal zones in the building. When the ZoneList option is used then this ventilation definition is applied to each of the zones in the zone list effecting a global definition for the amount of infiltration flow rate in the zone. The Zonelist option can be used effectively with the flow/area, flow/person, or airchanges/hour of the Design Flow Rate Calculation Method.
-
-The name of the actual ventilation object becomes &lt;Zone Name&gt; &lt;ZoneVentilation:DesignFlowRate Object Name&gt; and should be less than the standard length (100 characters) for a name field. If it is greater than this standard length, it may be difficult to specify in output reporting as it will be truncated. A warning will be shown if the generated name is greater than 100 characters. If it duplicates another such concatenated name, there will be a severe error and terminate the run.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design volume flow rate (V<sub>design</sub>) (see Design Flow Rate Calculation Method field and related subsequent fields). This fraction between 0.0 and 1.0 is noted as F<sub>schedule</sub> in the above equation.
-
-#### Field: Design Flow Rate Calculation Method
-
-This field is a key/choice field that tells which of the next four fields are filled and is descriptive of the method for calculating the design volume flow rate. The key/choices are:
-
-- Flow/Zone
-
-With this choice, the method used will be a straight insertion of the design volume flow rate.  (The Design Flow Rate field should be filled.)
-
-- Flow/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The Flow per Zone Floor Area field should be filled).
-
-- Flow/Person
-
-With this choice, the method used will be a factor per nominal number of people in the zone. (The Flow per Person field should be filled).
-
-- AirChanges/Hour
-
-With this choice, the method used will be the number of air changes per hour for the infiltration amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. (The Air Changes per Hour field should be filled).
-
-#### Field: Design Flow Rate
-
-This field denotes the full design volume flow rate (m<sup>3</sup>/s). The previous field should choose “flow/zone� as the choice. The design volume flow rate (noted as V<sub>design</sub> in the above equation) is the maximum amount of ventilation expected at design conditions. The design value is modified by the schedule fraction (see Field: Schedule Name) and user specified coefficients (see four “coefficient� fields below).
-
-#### Field: Flow Rate per Zone Floor Area
-
-This factor (m<sup>3</sup>/s-m<sup>2</sup>) is used, along with the Zone Area to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be “flow/area�.
-
-#### Field: Flow Rate per Person
-
-This factor (m<sup>3</sup>/s-person) is used, along with the nominal (maximum) number of occupants (people) in the Zone to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be “flow/person�.
-
-#### Field: Air Changes per Hour
-
-With this choice, the method used will be the number of air changes per hour for the ventilation amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. The choice from the method field should be “AirChanges/Hour�.
-
-#### Field: Ventilation Type
-
-This alpha character string defines the type of ventilation as one of the following options: Natural, Exhaust, Intake, or Balanced. Natural ventilation is assumed to be air movement/exchange as a result of openings in the building façade and will not consume any fan energy. Values for fan pressure and efficiency for natural ventilation are ignored. For either Exhaust or Intake, values for fan pressure and efficiency define the fan electric consumption. For Natural and Exhaust ventilation, the conditions of the air entering the space are assumed to be equivalent to outside air conditions. For Intake and Balanced ventilation, an appropriate amount of fan heat is added to the entering air stream. For Balanced ventilation, both an intake fan and an exhaust fan are assumed to co-exist, both having the same flow rate and power consumption (using the entered values for fan pressure rise and fan total efficiency). Thus, the fan electric consumption for Balanced ventilation is twice that for the Exhaust or Intake ventilation types which employ only a single fan.
-
-#### Field: Fan Pressure Rise
-
-This is the pressure rise experienced across the fan in Pascals (N/m<sup>2</sup>). This is a function of the fan and plays a role in determining the amount of energy consumed by the fan.
-
-#### Field: Fan Total Efficiency
-
-This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1."
-
-#### Field: Constant Term Coefficient
-
-This number is the “A� parameter in the above ventilation equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter, however, is a constant under all conditions and is not modified by any environmental effect. As a result, it is dimensionless.
-
-#### Field: Temperature Term Coefficient
-
-This number is the “B� parameter in the above ventilation equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the temperature difference between the outdoor and indoor air dry-bulb temperatures. The units for this parameter are inverse Celsius.
-
-#### Field: Velocity Term Coefficient
-
-This number is the “C� parameter in the above ventilation equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the speed of wind being experienced outside the building. The units for this parameter are s/m.
-
-#### Field: Velocity Squared Term Coefficient
-
-This number is the “D� parameter in the above ventilation equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by square of the speed of wind being experienced outside the building. The units for this parameter are s<sup>2</sup>/m<sup>2</sup>.
-
-#### Field: Minimum Indoor Temperature
-
-This is the indoor temperature (in Celsius) below which ventilation is shutoff. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is -100.0°C if the field is left blank. This lower temperature limit is intended to avoid overcooling a space and thus result in a heating load. For example, if the user specifies a minimum temperature of 20°C, ventilation is assumed to be available if the zone air temperature is above 20°C. If the zone air temperature drops below 20°C, then ventilation is automatically turned off.
-
-#### Field: Minimum Indoor Temperature Schedule Name
-
-This alpha field defines the name of a schedule (ref. Schedule objects) which contains the minimum indoor temperature (in Celsius) below which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Minimum Indoor Temperature field. If the user enters a valid schedule name, the minimum temperature values specified in this schedule will override the constant value specified in the Minimum Indoor Temperature field.
-
-#### Field: Maximum Indoor Temperature
-
-This is the indoor temperature (in Celsius) above which ventilation is shutoff. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is 100.0°C if the field is left blank. This upper temperature limit is intended to avoid overheating a space and thus result in a cooling load. For example, if the user specifies a maximum temperature of 28°C, ventilation is assumed to be available if the zone air temperature is below 28°C. If the zone air temperature increases to 28°C, then ventilation is automatically turned off.
-
-#### Field: Maximum Indoor Temperature Schedule Name
-
-This alpha field defines the name of a schedule (ref. Schedule objects) which contains the maximum indoor temperature (in Celsius) above which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Maximum Indoor Temperature field. If the user enters a valid schedule name, the maximum temperature values specified in this schedule will override the constant value specified in the Maximum Indoor Temperature field.
-
-#### Field: Delta Temperature
-
-This is the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which ventilation is shutoff. The minimum value for this field is -100.0°C and thedefault value is also -100.0°C if the field is left blank. This field allows ventilation to be stopped if the temperature outside is too warm and could potentially heat the space. For example, if the user specifies a delta temperature of 2°C, ventilation is assumed to be available if the outside air temperature is at least 2°C cooler than the zone air temperature. If the outside air dry-bulb temperature is less than 2°C cooler than the indoor dry-bulb temperature, then ventilation is automatically turned off.
-
-The values for this field can include negative numbers. This allows ventilation to occur even if the outdoor temperature is above the indoor temperature. The Delta Temperature is used in the code in the following way:
-
-IF ((IndoorTemp - OutdoorTemp) &lt; DeltaTemperature) Then ventilation is not allowed.
-
-Thus, if a large negative number is input for DeltaTemperature, the ventilation can be kept on even if the outdoor temperature is greater than the indoor temperature. This is useful for uncontrolled natural ventilation (open windows) or as a way to estimate the effect of required ventilation air for load calculations.
-
-#### Field: Delta Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which ventilation is shutoff as a function of time. The minimum temperature difference value in the schedule can be -100°C. This field is an optional field and has the same functionality as the Delta Temperature field. If the user enters a valid schedule name, the delta temperature values specified in this schedule will override the constant value specified in the Delta Temperature field.
-
-#### Field: Minimum Outdoor Temperature
-
-This is the outdoor temperature (in Celsius) below which ventilation is shut off. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is           -100.0°C if the field is left blank. This lower temperature limit is intended to avoid overcooling a space, which could result in a heating load.
-
-#### Field: Minimum Outdoor Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) below which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Minimum Outdoor Temperature field. If the user enters a valid schedule name, the temperature values in this schedule will override the constant value specified in the Minimum Outdoor Temperature field.
-
-#### Field: Maximum Outdoor Temperature
-
-This is the outdoor temperature (in Celsius) above which ventilation is shut off. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is 100.0°C if the field is left blank. This upper temperature limit is intended to avoid overheating a space, which could result in a cooling load.
-
-#### Field: Maximum Outdoor Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) above which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Maximum Outdoor Temperature field. If the user enters a valid schedule name, the temperature values in this schedule will override the constant value specified in the Maximum Outdoor Temperature field.
-
-#### Field: Maximum Wind Speed
-
-This is the wind speed (m/s) above which ventilation is shut off. This can help simulate conditions where one would normally close windows to avoid chaos in a space (papers blowing around, etc.).
-
-Two IDF examples are provided below:
-
-```idf
-ZoneVentilation:DesignFlowRate,
-  Ventilation 1,  !- Name
-  ZONE 2,         !- Zone Name
-  Simple Vent,    !- Schedule Name
-  Flow/Zone,      !- Design Volume Flow Rate calculation method
-  6.131944,       !- Design Volume Flow Rate {m3/s}
-  ,               !- Volume Flow Rate per area {m3/s/m2}
-  ,               !- Volume Flow Rate per person {m3/s/person}
-  ,               !- Air Changes Per Hour
-  INTAKE,         !- Ventilation Type
-  400.0,          !- Fan Pressure Rise{Pa}
-  0.9,            !- Fan Total Efficiency
-  0.6060000    ,  !- Constant Term Coefficient
-  2.0199999E-02,  !- Temperature Term Coefficient
-  5.9800001E-04,  !- Velocity Term Coefficient
-  0.0000000E+00!- Velocity Squared Term Coefficient
-  18.0,           !- Minimum Indoor Temperature {C}
-  ,               !- Minimum Indoor Temperature Schedule Name
-  ,               !- Maximum Indoor Temperature {C}
-  ,               !- Maximum Indoor Temperature Schedule Name
-  1.0;            !- Delta temperature {C}
-
-ZoneVentilation:DesignFlowRate,
-    SPACE1-1 Ventl 1,        !-Name
-    SPACE1-1,                !- Zone Name
-    NightVentSched,          !- SCHEDULE Name
-    Flow/Zone,               !- Design Volume Flow Rate calculation method
-    .05295,                  !- Design Volume Flow Rate {m3/s}
-    ,                        !- Volume Flow Rate per area {m3/s/m2}
-    ,                        !- Volume Flow Rate per person {m3/s/person}
-    ,                        !- Air Changes Per Hour
-    Intake,                  !- Ventilation Type
-    67.,                     !- Fan Pressure Rise
-    .7,                      !- Fan Total Efficiency
-    1,                       !- Constant Term Coefficient
-    0,                       !- Temperature Term Coefficient
-    0,                       !- Velocity Term Coefficient
-    0,                       !- Velocity Squared Term Coefficient
-    ,                        !- Minimum Indoor Temperature {C}
-    MinIndoorTemp,           !- Minimum Indoor Temperature Schedule Name
-    ,                        !- Maximum Indoor Temperature {C}
-    MaxIndoorTemp,           !- Maximum Indoor Temperature Schedule Name
-    ,                        !- Delta Temperature {deltaC}
-    DeltaTemp,               !- Delta Temperature Schedule Name
-   ,                        !- Minimum Outdoor Temperature {C}
-    MinOutdoorTemp,          !- Minimum Outdoor Temperature Schedule Name
-    ,                        !- Maximum Outdoor Temperature {C}
-    MaxOutdoorTemp,          !- Maximum Outdoor Temperature Schedule Name
-    40;                      !- Maximum WindSpeed {m/s}
-```
-
-
-
-
-Global Ventilation example:
-
-```idf
-  Zonelist, West-East Zones, West Zone, East Zone;
-
-
-  ZoneVentilation:DesignFlowRate,
-    West-East Zones Ventilation,         !- Name
-    West-East Zones,         !- Zone or ZoneList Name
-    VentSched,               !- Schedule Name
-    AirChanges/Hour,         !- Design Flow Rate Calculation Method
-    ,                        !- Design Flow Rate {m3/s}
-    ,                        !- Flow Rate per Zone Floor Area {m3/s-m2}
-    ,                        !- Flow Rate per Person {m3/s-person}
-    1.7,                        !- Air Changes per Hour
-    Intake,                  !- Ventilation Type
-    67.,                     !- Fan Pressure Rise {Pa}
-    0.7,                     !- Fan Total Efficiency
-    1,                       !- Constant Term Coefficient
-    0,                       !- Temperature Term Coefficient
-    0,                       !- Velocity Term Coefficient
-    0,                       !- Velocity Squared Term Coefficient
-    ,                        !- Minimum Indoor Temperature {C}
-    MinIndoorTemp,           !- Minimum Indoor Temperature Schedule Name
-    ,                        !- Maximum Indoor Temperature {C}
-    MaxIndoorTemp,           !- Maximum Indoor Temperature Schedule Name
-    ,                        !- Delta Temperature {deltaC}
-    DeltaTemp,               !- Delta Temperature Schedule Name
-    ,                        !- Minimum Outdoor Temperature {C}
-    MinOutdoorTemp,          !- Minimum Outdoor Temperature Schedule Name
-    ,                        !- Maximum Outdoor Temperature {C}
-    MaxOutdoorTemp,          !- Maximum Outdoor Temperature Schedule Name
-    40;                      !- Maximum Wind Speed {m/s}
-```
-
-
-### ZoneVentilation:WindandStackOpenArea
-
-For this model, the ventilation air flow rate is a function of wind speed and thermal stack effect, along with the area of the opening being modeled. This object can be used alone or in combination with ZoneVentilation:DesignFlowRate objects. This model is intended for simplified ventilation calculations as opposed to the more detailed ventilation investigations that can be performed with the AirflowNetwork model. Using the “Wind and Stack with Open Area� model, the natural ventilation flow rate can be controlled by a multiplier fraction schedule applied to the user-defined opening area and through the specification of minimum, maximum and delta temperatures. The temperatures can be either single constant values for the entire simulation or schedules which can vary over time. The equation used to calculate the ventilation rate driven by wind is:
-
-<div>\[{Q_w} = {C_w}{A_{opening}}{F_{schedule}}V\]</div>
-
-where,
-
-      *Q<sub>w</sub>*        = Volumetric air flow rate driven by wind [m<sup>3</sup>/s]
-
-      *C<sub>w</sub>*        = Opening effectiveness [dimensionless]
-
-      *A<sub>opening</sub>*  = Opening area [m<sup>2</sup>]
-
-      *F<sub>schedule</sub>* = Open area fraction [user-defined schedule value, dimensionless]
-
-      *V*          = Local wind speed [m/s]
-
-The equation used to calculate the ventilation rate due to stack effect is:
-
-<div>\[{Q_s} = {C_D}{A_{opening}}{F_{schedule}}\sqrt {2g\Delta {H_{NPL}}(|{T_{zone}} - {T_{odb}}|/{T_{zone}})} \]</div>
-
-where,
-
-      *Q<sub>s</sub>*        = Volumetric air flow rate due to stack effect [m<sup>3</sup>/s]
-
-      *C<sub>D</sub>*        = Discharge coefficient for opening [dimensionless]
-
-      *A<sub>opening</sub>*  = Opening area [m<sup>2</sup>]
-
-      *F<sub>schedule</sub>* = Open area fraction [user-defined schedule value, dimensionless]
-
-      *ΔH<sub>NPL</sub>*  = Height from midpoint of lower opening to the neutral pressure level [m].
-
-Estimation of this value is difficult; refer to Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals for guidance.
-
-      *T<sub>zone</sub>*      = Zone air dry-bulb temperature [K]
-
-*T<sub>odb</sub>*<sub>            </sub> = Local outdoor air dry-bulb temperature [K]
-
-The total ventilation rate calculated by this model is the quadrature sum of the wind and stack air flow components:
-
-<div>\[Ventilatio{n_{WindAndStack}} = \sqrt {{Q_s}^2 + {Q_w}^2} \]</div>
-
-The local outdoor air dry-bulb temperature used in the stack effect equation (T<sub>odb</sub>) is typically a function of the height of the zone centroid above ground. The corresponding zone name is given in the second field. The local outdoor air dry-bulb temperature calculation procedure is described in the “Local Outdoor Air Temperature Calculation� section of the Engineering Reference.
-
-The local outdoor wind speed used in the above wind-driven equation (V) is also a function of the height of the zone centroid above ground. The corresponding zone name is given in the second field. The local outdoor wind speed calculation procedure is described in the “Local Wind Speed Calculation� section of the Engineering Reference.
-
-Note: When the value of the Wind Speed Profile Exponent field in the Site:HeightVariation object is equal to 0.0, the local wind speed is always equal to the wind speed given in the weather data and will not be dependent on zone centroid height.  Similarly, if the value of the Air Temperature Gradient Coefficient is set equal to 0, the local air dry-bulb temperature is also always equal to the air dry-bulb temperature given in the weather data and will not be dependent on zone centroid height.
-
-One or more ventilation objects (i.e., ZoneVentilation:DesignFlowRate and/or ZoneVentilation:WindandStackOpenArea) can be defined for each zone, and the resulting ventilation rate for the zone will simply be the summation of the flow rates specified by the ventilation objects.
-
-More advanced ventilation calculations are possible using the EnergyPlus AirflowNetwork model.
-
-#### Field: Name
-
-The name of the ZoneVentilation:WindandStackOpenArea object.
-
-#### Field: Zone Name
-
-This field is the name of the zone (ref: Zone) and attaches a particular ventilation statement to a thermal zone in the building.
-
-#### Field: Opening Area
-
-This is the opening area exposed to outdoors (m<sup>2</sup>) in a zone.
-
-#### Field: Opening Area Fraction Schedule Name
-
-This field is the name of the schedule (ref: Schedule) which modifies the Opening Area value (see previous field). The schedule values must be any positive number between 0 and 1 as a fraction. The actual opening area in a zone for a particular simulation time step is defined as the product of the Opening Area input field and the value specified by the schedule named in this input field.
-
-#### Field: Opening Effectiveness
-
-This field is the opening effectiveness (C<sub>w</sub>). The value must be between 0.0 and 1.0 or the value can be autocalculated. If a real value is input, that constant value will be used in the calculations. Otherwise, this field can be left blank (default = Autocalculate) or the user can input **Autocalculate.** Based on recommended values provided in Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals, C<sub>w</sub> = 0.55 for perpendicular winds and C<sub>w</sub> = 0.3 for diagonal winds. For Autocalculate, any angles between perpendicular and diagonal are linearly interpolated between 0.3 and 0.55 by the model.
-
-#### Field: Effective Angle
-
-This is the angle in degrees counting from the North clockwise to the opening outward normal. The value must be between 0 and 360, with the default being 0 if this input field is left blank. The Effective Angle is 0 if the opening outward normal faces North, 90 if faces East, 180 if faces South, and 270 if faces West. The value is fixed and independent of coordinate system defined in the GlobalGeometryRules object. This input field value is used to calculate the angle between the wind direction and the opening outward normal to determine the opening effectiveness values when the input field Opening Effectiveness = Autocalculate.
-
-#### Field: Height Difference
-
-This is the height difference between the midpoint of the lower opening and the neutral pressure level in meters. This value is a required user input.
-
-Note: Estimation of the height difference is difficult for natural ventilated buildings. Chapter 16 of the 2009 ASHRAE Handbook of Fundamentals may provide guidance for estimating the height difference.
-
-#### Field: Discharge Coefficient for Opening
-
-This is the discharge coefficient for the opening (C<sub>D</sub>). The value must be between 0.0 and 1.0, or the value can be autocalculated. If a real value is input, that constant value will be used in the calculations. Otherwise, this field can be left blank (default = Autocalculate) or the user can input **Autocalculate.** For Autocalculate, the program will determine the discharge coefficient based on the following equation:
-
-<div>\[{C_D} = 0.40 + 0.0045\left| {{T_{zone}} - {T_{odb}}} \right|\]</div>
-
-#### Field: Minimum Indoor Temperature
-
-This is the indoor temperature (in Celsius) below which ventilation is shutoff. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is           -100.0°C if the field is left blank. This lower temperature limit is intended to avoid overcooling a space and thus result in a heating load. For example, if the user specifies a minimum temperature of 20°C, ventilation is assumed to be available if the zone air temperature is above 20°C. If the zone air temperature drops below 20°C, then ventilation is automatically turned off.
-
-#### Field: Minimum Indoor Temperature Schedule Name
-
-This alpha field defines the name of a schedule (ref. Schedule objects) which contains the minimum indoor temperature (in Celsius) below which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Minimum Indoor Temperature field. If the user enters a valid schedule name, the minimum temperature values specified in this schedule will override the constant value specified in the Minimum Indoor Temperature field.
-
-#### Field: Maximum Indoor Temperature
-
-This is the indoor temperature (in Celsius) above which ventilation is shutoff. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is 100.0°C if the field is left blank. This upper temperature limit is intended to avoid overheating a space and thus result in a cooling load. For example, if the user specifies a maximum temperature of 28°C, ventilation is assumed to be available if the zone air temperature is below 28°C. If the zone air temperature increases to 28°C, then ventilation is automatically turned off.
-
-#### Field: Maximum Indoor Temperature Schedule Name
-
-This alpha field defines the name of a schedule (ref. Schedule objects) which contains the maximum indoor temperature (in Celsius) above which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Maximum Indoor Temperature field. If the user enters a valid schedule name, the maximum temperature values specified in this schedule will override the constant value specified in the Maximum Indoor Temperature field.
-
-#### Field: Delta Temperature
-
-This is the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which ventilation is shutoff. The minimum value for this field is -100.0°C and the default value is also -100.0°C if the field is left blank. This field allows ventilation to be stopped if the temperature outside is too warm and could potentially heat the space. For example, if the user specifies a delta temperature of 2°C, ventilation is assumed to be available if the outside air temperature is at least 2°C cooler than the zone air temperature. If the outside air dry-bulb temperature is less than 2°C cooler than the indoor dry-bulb temperature, then ventilation is automatically turned off.
-
-The values for this field can include negative numbers. This allows ventilation to occur even if the outdoor temperature is above the indoor temperature. The Delta Temperature is used in the code in the following way:
-
-IF ((IndoorTemp - OutdoorTemp) &lt; DeltaTemperature) Then ventilation is not allowed.
-
-Thus, if a large negative number is input for DeltaTemperature, the ventilation can be kept on even if the outdoor temperature is greater than the indoor temperature. This is useful for uncontrolled natural ventilation (open windows) or as a way to estimate the effect of required ventilation air for load calculations.
-
-#### Field: Delta Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which ventilation is shutoff as a function of time. The minimum temperature difference value in the schedule can be -100°C. This field is an optional field and has the same functionality as the Delta Temperature field. If the user enters a valid schedule name, the delta temperature values specified in this schedule will override the constant value specified in the Delta Temperature field.
-
-#### Field: Minimum Outdoor Temperature
-
-This is the outdoor temperature (in Celsius) below which ventilation is shut off. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is           -100.0°C if the field is left blank. This lower temperature limit is intended to avoid overcooling a space, which could result in a heating load.
-
-#### Field: Minimum Outdoor Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) below which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Minimum Outdoor Temperature field. If the user enters a valid schedule name, the temperature values in this schedule will override the constant value specified in the Minimum Outdoor Temperature field.
-
-#### Field: Maximum Outdoor Temperature
-
-This is the outdoor temperature (in Celsius) above which ventilation is shut off. The minimum value for this field is -100.0°C and the maximum value is 100.0°C. The default value is 100.0°C if the field is left blank. This upper temperature limit is intended to avoid overheating a space, which could result in a cooling load.
-
-#### Field: Maximum Outdoor Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) above which ventilation is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field and has the same functionality as the Maximum Outdoor Temperature field. If the user enters a valid schedule name, the temperature values in this schedule will override the constant value specified in the Maximum Outdoor Temperature field.
-
-#### Field: Maximum Wind Speed
-
-This is the wind speed (m/s) above which ventilation is shut off. This can help simulate conditions where one would normally close windows to avoid chaos in a space (papers blowing around, etc.).
-
-An IDF example is provided below:
-
-
-
-```idf
-  ZoneVentilation:WindandStackOpenArea,
-    ZONE 3 Ventl 1,          !- Name
-    ZONE 3,                  !- Zone Name
-    0.5,                     !- Opening Area {m2}
-    Constant,                !- Opening Area Fraction Schedule Name
-    AutoCalculate,           !- Opening Effectiveness
-    0.0,                     !- Effective Angle {deg}
-    1.0,                     !- Height Difference {m}
-    AutoCalculate,           !- Discharge Coefficient for Opening
-    18.0,                    !- Minimum Indoor Temperature {C}
-    ,                        !- Minimum Indoor Temperature Schedule Name
-    ,                        !- Maximum Indoor Temperature {C}
-    ,                        !- Maximum Indoor Temperature Schedule Name
-    1.0;                     !- Delta Temperature {deltaC}
-```
-
-### ZoneVentilation Outputs
-
-Current ventilation output variables:
-
-* HVAC,Sum,Zone Ventilation Sensible Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Ventilation Sensible Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Ventilation Latent Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Ventilation Latent Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Ventilation Total Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Ventilation Total Heat Gain Energy [J]
-
-* HVAC,Average,Zone Ventilation Current Density Volume Flow Rate [m3/s]
-
-* HVAC,Average,Zone Ventilation Standard Density Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Ventilation Current Density Volume [m3]
-
-* HVAC,Sum,Zone Ventilation Standard Density Volume [m3]
-
-* HVAC,Sum,Zone Ventilation Mass [kg]
-
-* HVAC,Sum,Zone Ventilation Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Ventilation Air Change Rate [ach]
-
-* HVAC,Sum,Zone Ventilation Fan Electric Energy [J]
-
-* HVAC,Average,Zone Ventilation Air Inlet Temperature [C]
-
-Note: If ZoneVentilation:\* objects and ZoneAirBalance:OutdoorAir (with Air Balance Method = Quadrature) objects reference the same Zone Name, the above ventilation output variables will not be reported for that zone. Instead, output variables for zone outdoor air flow will be reported by the corresponding ZoneAirBalance:OutdoorAir object.
-
-#### Zone Ventilation Sensible Heat Loss Energy [J]
-
-The sensible (temperature) heat loss that occurs when the ventilation inlet air temperature &lt; zone air temperature. If multiple ventilation objects are specified for a particular zone, the ventilation inlet air temperature is from all ZoneVentilation:DesignFlowRate and ZoneVentilation:WindandStackOpenArea objects specified for the zone.
-
-#### Zone Ventilation Sensible Heat Gain Energy [J]
-
-The sensible (temperature) heat gain that occurs when the ventilation inlet air temperature &gt;= zone air temperature. If multiple ventilation objects are specified for a particular zone, the ventilation inlet air temperature is from all ZoneVentilation:DesignFlowRate and ZoneVentilation:WindandStackOpenArea objects specified for the zone.
-
-#### Zone Ventilation Latent Heat Loss Energy [J]
-
-The latent heat loss that occurs when the Ventilation air humidity ratio (outdoor) &lt; zone air humidity ratio from all ZoneVentilation:DesignFlowRate and ZoneVentilation:WindandStackOpenArea objects specified for the zone.
-
-#### Zone Ventilation Latent Heat Gain Energy [J]
-
-The latent heat gain that occurs when the Ventilation air humidity ratio (outdoor) &gt;= zone air humidity ratio from all ZoneVentilation:DesignFlowRate and ZoneVentilation:WindandStackOpenArea objects specified for the zone.
-
-#### Zone Ventilation Total Heat Loss Energy [J]
-
-The total heat loss that occurs when the sum of Zone Ventilation Sensible Heat Gain Energy and Zone Ventilation Latent Heat Gain Energy &lt; the sum of Zone Ventilation Sensible Heat Loss Energy and Zone Ventilation Latent Heat Loss Energy.
-
-#### Zone Ventilation Total Heat Gain Energy [J]
-
-The total heat gain that occurs when the sum of Zone Ventilation Sensible Heat Gain Energy and Zone Ventilation Latent Heat Gain Energy &gt;= the sum of Zone Ventilation Sensible Heat Loss Energy and Zone Ventilation Latent Heat Loss Energy.
-
-#### Zone Ventilation Current Density Volume [m3]
-
-#### Zone Ventilation Current Density Volume Flow Rate [m3/s]
-
-These outputs are the total volume and volume flow rate of ventilation air based on the current density of zone air.
-
-#### Zone Ventilation Standard Density Volume [m3]
-
-#### Zone Ventilation Standard Density Volume Flow Rate [m3/s]
-
-These outputs are the total volume and volume flow rate of ventilation air based on the standard density of air.  Standard density in EnergyPlus corresponds to 20ºC drybulb, dry air, and nominally adjusted for elevation.
-
-#### Zone Ventilation Mass [kg]
-
-This output is the total mass flow into a particular zone from outdoors.
-
-#### Zone Ventilation Mass Flow Rate [kg/s]
-
-This output is the total mass flow rate into a particular zone from outdoors.
-
-#### Zone Ventilation Air Change Rate [ach]
-
-The volume flow rate of the ventilation air in air changes per hour.
-
-#### Zone Ventilation Fan Electric Energy [J]
-
-The fan electrical consumption for Intake or Exhaust ventilation types (for ZoneVentilation:DesignFlowRate objects only).
-
-#### Zone Ventilation Air Inlet Temperature [C]
-
-This is equal to the outdoor air temperature except when INTAKE fan power is included (for ZoneVentilation:DesignFlowRate objects only). When intake fan power is used, then the additional heat due to the fan is added to the outdoor temperature and this will be reported as the inlet air temperature. If multiple ventilation objects are specified for a particular zone, the reported value is the mass flow weighted temperature for the multiple ventilation objects specified for this zone.
-
-### ZoneAirBalance:OutdoorAir
-
-This model calculates a combined zone outdoor airflow by including interactions between mechanical ventilation, infiltration and duct leakage. It is mainly applied to a single zone (e.g., residential) building. The model combines all outdoor airflows from ZoneInfiltration and ZoneVentilation objects in the same zone. This object also includes the induced outdoor airflows due to unbalanced duct leakage, and unbalanced outdoor airflows introduced by unbalanced airflows from ZoneHVAC:EnergyRecoveryVentilator objects when the exhaust airflow is greater than the supply outdoor airflow. This model is intended for simplified outdoor airflow calculations as opposed to the more detailed outdoor airflow investigations that can be performed with the AirflowNetwork model. The equation used to calculate the combined zone outdoor airflow is:
-
-<div>\[Q = \sqrt {{Q_n}^2 + {Q_{u,v}}^2 + {Q_{u,l}}^2}  + {Q_{b,v}}\]</div>
-
-where,
-
-*Q*    = Combined outdoor airflow with infiltration, balanced and unbalanced outdoor air flows, and unbalanced duct leakage [m<sup>3</sup>/s]
-
-*Q<sub>n</sub>*   = Natural infiltration airflow from ZoneInfiltration:\* objects [m<sup>3</sup>/s]
-
-*Q<sub>b,v</sub>* = Balanced ventilation airflow, excluding infiltration [m<sup>3</sup>/s]
-
-*Q<sub>u,v</sub>* = Unbalanced ventilation airflow, excluding infiltration [m<sup>3</sup>/s]
-
-*Q<sub>u,l</sub>*  = Unbalanced duct leakage: the difference between supply and return leaks [m<sup>3</sup>/s]
-
-This object cannot be used simultaneously with the EnergyPlus AirflowNetwork model.  If the AirflowNetwork model is active for a simulation time step, the Air Balance Method is reset to “None� for that time step. More advanced outdoor airflow calculations are possible using the EnergyPlus AirflowNetwork model.
-
-This object does not combine any airflows from Fan:ZoneExhaust objects and is independent of HVAC equipment operation.
-
-This object will not work with the AvailabilityManager:HybridVentilation object in the same zone, when the Simple Airflow Control Type Schedule Name is provided in the HybridVentilation object. For this case, the Air Balance Method is reset to “None�.
-
-#### Field: Name
-
-The name of the ZoneOutdoorAir:Combined object.
-
-#### Field: Zone Name
-
-This field is the name of the zone (ref: Zone) and attaches a combined outdoor airflow statement to a thermal zone in the building.
-
-#### Field: Air Balance Method
-
-This choice field determines the air balance method. Two choices are Quadrature and None. If Quadrature, the combined zone outdoor air flow is calculated based on the above equation. If None, no combining of outdoor air will be performed (i.e., any ZoneInfiltration:\* and ZoneVentilation:\* objects specified for this zone are simulated individually).
-
-#### Field: Induced Outdoor Air Due to Unbalanced Duct Leakage
-
-This is the induced outdoor airflow rate, in m<sup>3</sup>/s, due to unbalanced duct leakage. If left blank, the default value is 0.
-
-#### Field: Induced Outdoor Air Schedule Name
-
-This field is the name of the schedule (ref: Schedule) which modifies the induced outdoor airflow rate value (see previous field). The schedule values must be any positive number between 0 and 1 as a fraction. The actual induced outdoor airflow rate in a zone for a particular simulation time step is defined as the product of the Induced Outdoor Air Due to Unbalanced Duct Leakage input field and the value specified by the schedule named in this input field.
-
-Note: Since this object is independent of HVAC operation, the inputs for the last two fields should be carefully selected to match HVAC system operation schedules.
-
-An IDF example is provided below:
-
-```idf
-ZoneAirBalance:OutdoorAir,
-    ZONE 2 Balance 1,        !- Name
-    ZONE 2,                  !- Zone Name
-    Quadrature,              !- Air Balance Method
-    0.00,                    !- Induced Outdoor Air Due to Unbalanced Duct Leakage {m3/s}
-    Constant;                !- Induced Outdoor Air Schedule Name
-```
-
-### ZoneAirBalance:OutdoorAir Outputs
-
-ZoneAirBalance:OutdoorAir output variables will be provided when the Air Balance Method is Quadrature. Output variables from the associated ZoneVentilation:\* and ZoneInfiltration:\* objects for the same zone will not be produced when ZoneAirBalance:OutdoorAir output variables are available. If the Air Balance Method = None, then no ZoneAirBalance:OutputAir outputs will be produced and the associated ZoneVentilation:\* and ZoneInfiltration:\* objects will specify their output variables for the zone.
-
-* HVAC,Sum,Zone Combined Outdoor Air Sensible Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Combined Outdoor Air Sensible Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Combined Outdoor Air Latent Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Combined Outdoor Air Latent Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Combined Outdoor Air Total Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Combined Outdoor Air Total Heat Gain Energy [J]
-
-* HVAC,Average,Zone Combined Outdoor Air Current Density Volume Flow Rate [m3/s]
-
-* HVAC,Average,Zone Combined Outdoor Air Standard Density Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Combined Outdoor Air Current Density Volume [m3]
-
-* HVAC,Sum,Zone Combined Outdoor Air Standard Density Volume [m3]
-
-* HVAC,Sum,Zone Combined Outdoor Air Mass [kg]
-
-* HVAC,Sum,Zone Combined Outdoor Air Mass Flow Rate [kg/s]
-
-* HVAC,Average, Zone Combined Outdoor Air Changes per Hour [ach]
-
-* HVAC,Sum, Zone Combined Outdoor Air Fan Electric Energy [J]
-
-
-#### Zone Combined Outdoor Air Sensible Heat Loss Energy [J]
-
-The sensible (temperature) heat loss that occurs when the outdoor air temperature &lt; zone air temperature.
-
-#### Zone Combined Outdoor Air Sensible Heat Gain Energy [J]
-
-The sensible (temperature) heat gain that occurs when the outdoor air temperature &gt;= zone air temperature.
-
-#### Zone Combined Outdoor Air Latent Heat Loss Energy [J]
-
-The latent heat loss that occurs when the outdoor air humidity ratio &lt; zone air humidity ratio.
-
-#### Zone Combined Outdoor Air Latent Heat Gain Energy [J]
-
-The latent heat gain that occurs when the outdoor air humidity ratio &gt;= zone air humidity ratio.
-
-#### Zone Combined Outdoor Air Total Heat Loss Energy [J]
-
-The total heat loss that occurs when the sum of Zone Combined Outdoor Air Sensible Heat Gain Energy and Zone Combined Outdoor Air Latent Heat Gain Energy &lt; the sum of Zone Combined Outdoor Air Sensible Heat Loss Energy and Zone Combined Outdoor Air Latent Heat Loss Energy.
-
-#### Zone Combined Outdoor Air Total Heat Gain Energy [J]
-
-The total heat gain that occurs when the sum of Zone Combined Outdoor Air Sensible Heat Gain Energy and Zone Combined Outdoor Air Latent Heat Gain Energy &gt;= the sum of Zone Combined Outdoor Air Sensible Heat Loss Energy and Zone Combined Outdoor Air Latent Heat Loss Energy.
-
-#### Zone Combined Outdoor Air Current Density Volume [m3]
-
-#### Zone Combined Outdoor Air Current Density Volume Flow Rate [m3/s]
-
-These outputs are the total volume and volume flow rate of outdoor air based on the current density of zone air.
-
-#### Zone Combined Outdoor Air Standard Density Volume [m3]
-
-#### Zone Combined Outdoor Air Standard Density Volume Flow Rate [m3/s]
-
-These outputs are the total volume and volume flow rate of outdoor air based on the standard density of air.  Standard density in EnergyPlus corresponds to 20ºC drybulb, dry air, and nominally adjusted for elevation.
-
-#### Zone Combined Outdoor Air Mass [kg]
-
-This output is the total mass flow into a particular zone from outdoors.
-
-#### Zone Combined Outdoor Air Mass Flow Rate [kg/s]
-
-This output is the total mass flow rate into a particular zone from outdoors.
-
-#### Zone Combined Outdoor Air Changes per Hour [ach]
-
-The volume flow rate of the ventilation air in air changes per hour.
-
-#### Zone Combined Outdoor Air Fan Electric Energy [J]
-
-The fan electrical consumption for Intake, Exhaust, or Balanced ventilation types (for
-
-ZoneVentilation:DesignFlowRate objects used to calculate a combined zone outdoor airflow).
-
-### ZoneMixing
-
-In EnergyPlus, the ZoneMixing syntax is intended to allow simplified treatment of air exchange between zones. Note that this statement only affects the energy balance of the “receiving� zone and that this statement will not produce any effect on the “source� zone. Mixing statements can be complementary and include multiple zones, but the balancing of flows between zones is left to the user’s discretion. The use of the Cross Mixing syntax (ref: Cross Mixing) can allow for automatic balancing of flows and energy flow rates between zones but is hindered by the limitation of only a single cross mixing statement per zone. The use of Refrigeration Door Mixing syntax (ref: Refrigeration Door Mixing) automatically balances the flow and energy between two zones and allows multiple mixing statements per zone. More advanced mixing calculations are possible using the EnergyPlus AirflowNetwork model for multi-zone airflow with or without HVAC system operation. Mixing is entered using the following syntax.
-
-#### Field: Name
-
-The name of the ZoneMixing object.
-
-#### Field: Zone Name
-
-This field is the name of the zone (ref: Zone) receiving the amount of air being exchanged and attaches a particular mixing statement to a thermal zone in the building.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design volume flow rate parameter (see next field). This fraction between 0.0 and 1.0 modifies the design level parameter.
-
-#### Field: Design Flow Rate Calculation Method
-
-This field is a key/choice field that tells which of the next four fields are filled and is descriptive of the method for calculating the design volume flow rate. The key/choices are:
-
-- Flow/Zone
-
-With this choice, the method used will be a straight insertion of the design volume flow rate.  (The Design Flow Rate field should be filled.)
-
-- Flow/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The Flow per Zone Floor Area field should be filled).
-
-- Flow/Person
-
-With this choice, the method used will be a factor per nominal number of people in the zone. (The Flow per Person field should be filled).
-
-- AirChanges/Hour
-
-With this choice, the method used will be the number of air changes per hour for the infiltration amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. (The Air Changes per Hour field should be filled).
-
-#### Field: Design Flow Rate
-
-This field denotes the full design volume flow rate (m<sup>3</sup>/s). The previous field should choose “flow/zone� as the choice. The design volume flow rate is the maximum amount of mixing air expected. The design value is modified by the schedule fraction (see Field: Schedule Name) and user specified coefficients (see four “coefficient� fields below).
-
-#### Field: Flow Rate per Zone Floor Area
-
-This factor (m<sup>3</sup>/s-m<sup>2</sup>) is used, along with the Zone Area to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be “Flow/Area�.
-
-#### Field: Flow Rate per Person
-
-This factor (m<sup>3</sup>/s-person) is used, along with the nominal (maximum) number of occupants (people) in the Zone to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be “Flow/Person�.
-
-#### Field: Air Changes per Hour
-
-With this choice, the method used will be the number of air changes per hour for the mixing amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. The choice from the method field should be “AirChanges/Hour�.
-
-#### Field: Source Zone Name
-
-This field is the name of the “source� zone (ref: Zone) that exhausts the amount of air specified by the design level and schedule fields to the zone named in the zone name field.
-
-#### Field: Delta Temperature
-
-This number controls when mixing air from the source zone is sent to the receiving zone. This parameter is a temperature and is expressed in units of Celsius. If this field is positive, the temperature of the zone from which the air is being drawn (source zone) must be “Delta Temperature� warmer than the receiving zone air or else no mixing occurs. If this field is negative, the temperature of the source zone must be “Delta Temperature� cooler than the receiving zone air or else no mixing occurs. If this parameter is zero, mixing occurs regardless of the relative zone temperatures.
-
-#### Field: Delta Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the temperature difference (in Celsius) between the source zone and receiving zone air dry-bulb temperatures as a function of time. This field is an optional field and has the same functionality as the Delta Temperature field. If the user enters a valid schedule name, the delta temperature values specified in this schedule will supersede the constant value specified in the Delta Temperature field.
-
-#### Field: Minimum Zone Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum receiving zone temperature (in Celsius) below which mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum zone temperature control is not applied.
-
-#### Field: Maximum Zone Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum receiving zone temperature (in Celsius) above which mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum zone temperature control is not applied.
-
-**Note:** The maximum zone temperature when mixing is shutoff must be greater than or equal to the minimum zone temperature when mixing is shutoff at any given time. Otherwise, warnings will be issued and the maximum zone shutoff temperature will be set to the minimum zone shutoff temperature.
-
-#### Field: Minimum Source Zone Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum source zone temperature (in Celsius) below which mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum source zone temperature control is not applied.
-
-#### Field: Maximum Source Zone Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum source zone temperature (in Celsius) above which mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum source zone temperature control is not applied.
-
-**Note:** The maximum source zone temperature when mixing is shutoff must be greater than or equal to the minimum source zone temperature when mixing is shutoff at any given time. Otherwise, warnings will be issued and the maximum source zone shutoff temperature will be set to the minimum source zone shutoff temperature.
-
-#### Field: Minimum Outdoor Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) below which mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum outdoor temperature control is not applied.
-
-#### Field: Maximum Outdoor Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum outdoor temperature (in Celsius) above which mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum outdoor temperature control is not applied.
-
-**Note:** The maximum outdoor temperature when mixing is shutoff must be greater than or equal to the minimum outdoor temperature which mixing is shutoff at any given time. Otherwise, a warning will be issued and the maximum outdoor shutoff temperature will be set to the minimum outdoor shutoff temperature.
-
-An IDF Example:
-
-```idf
-ZoneMixing,
-  Kitchen_ZN_1_FLR_1 Exhaust Fanmixing_0,  !- Name
-  Kitchen_ZN_1_FLR_1,  !- Zone Name
-  Hours_of_operation,  !- Schedule Name
-  Flow/Zone,  !- Design Flow Rate Calculation Method
-  1.4540,  !- Design Level
-   ,  !- Volume Flow Rate per Area {m3/s/m2}
-   ,  !- Volume Flow Rate Per Person {m3/s/person}
-   ,  !- Air Changes per Hour {ACH}
-  CAFETERIA_ZN_1_FLR_1,  !- Source Zone Name
-  0.0;  !- Delta Temperature
-```
-
-### Zone Mixing Outputs
-
-* HVAC,Sum,Zone Mixing Volume [m3]
-
-* HVAC,Sum,Zone Mixing Current Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Mixing Standard Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Mixing Mass [kg]
-
-* HVAC,Sum,Zone Mixing Mass Flow Rate [kg/s]
-
-* HVAC,Sum,Zone Mixing Sensible Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Mixing Sensible Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Mixing Latent Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Mixing Latent Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Mixing Total Heat Loss [J]
-
-* HVAC,Sum,Zone Mixing Total Heat Gain Energy [J]
-
-
-#### Zone Mixing Volume [m3]
-
-The air volume in m<sup>3</sup> entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
-
-#### Zone Mixing Current Density Volumetric Flow Rate [m3/s]
-
-The air volumetric flow rate in m<sup>3</sup>/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at current zone air conditions.
-
-#### Zone Mixing Standard Density Volumetric Flow Rate [m3/s]
-
-The air volumetric flow rate in m<sup>3</sup>/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at standard conditions.
-
-#### Zone Mixing Mass [kg]
-
-The air mass in kg entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep. The air mass is calculated using the air volume flow from each “source� zone and the density of air calculated for the average conditions (temperature and humidity) between the “source� and “receiving� zones.
-
-#### Zone Mixing Mass Flow Rate [kg/s]
-
-The air mass flow rate in kg/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
-
-#### Zone Mixing Sensible Heat Loss Energy [J]
-
-#### Zone Mixing Sensible Heat Gain Energy [J]
-
-The sensible (temperature) heat transfer due to the sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the specific heat (calculated for the average conditions (temperature and humidity) between the “source� and “receiving� zones) and the temperature differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing sensible heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing sensible heat gain.
-
-#### Zone Mixing Latent Heat Loss Energy [J]
-
-#### Zone Mixing Latent Heat Gain Energy [J]
-
-The latent heat transfer due to the sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the heat of vaporization (calculated for the average conditions (temperature and humidity) between the “source� and “receiving� zones) and the humidity ratio differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing latent heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing latent heat gain.
-
-#### Zone Mixing Total Heat Loss Energy [J]
-
-The total heat loss due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy &lt; the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
-
-#### Zone Mixing Total Heat Gain Energy [J]
-
-The total heat gain due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy &gt;= the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
-
-### ZoneCrossMixing
-
-The ZoneCrossMixing syntax is ideally suited for two zones that exchange an equal amount of air between each other and do not have any air exchange with other zones. As with Mixing (ref: Mixing), this is a simplified view of interzone airflow in EnergyPlus. The main difference between Mixing and Cross Mixing is that Cross Mixing has an energy effect on both the source and the receiving zone, thus maintaining both the air mass and energy balances in the two zones.
-
-Cross Mixing can be entered once, in one of the mixing zones; or twice, once for each zone. The object should be entered once if Delta Temperature &gt; 0.0 and it is desirable to have mixing only when the source zone  is warmer than the receiving zone. This might be the case when the warmer zone is below the colder zone and the mixing is buoyancy driven. If the zones are next to each other, separated by an open doorway, it would be more suitable to input a cross mixing object for each zone. Then mixing would occur if the zone temperatures differed by Delta Temperature or greater regardless of which is the warmer zone.
-
-If Delta Temperature = 0.0, Cross Mixing can be entered either once or twice: the effect is exactly the same.
-
-Cross Mixing is entered using the following syntax.
-
-#### Field: Name
-
-The name of the ZoneCrossMixing object.
-
-#### Field: Zone Name
-
-This field is the name of the zone (ref: Zone) receiving the amount of air being exchanged and attaches a particular cross mixing statement to a thermal zone in the building.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design volume flow rate parameter (see next field). This fraction between 0.0 and 1.0 modifies the design level parameter.
-
-#### Field: Design Flow Rate Calculation Method
-
-This field is a key/choice field that tells which of the next four fields are filled and is descriptive of the method for calculating the design volume flow rate. The key/choices are:
-
-- Flow/Zone
-
-With this choice, the method used will be a straight insertion of the design volume flow rate.  (The Design Flow Rate field should be filled.)
-
-- Flow/Area
-
-With this choice, the method used will be a factor per floor area of the zone. (The Flow per Zone Floor Area field should be filled).
-
-- Flow/Person
-
-With this choice, the method used will be a factor per nominal number of people in the zone. (The flow per person field should be filled).
-
-- AirChanges/Hour
-
-With this choice, the method used will be the number of air changes per hour for the infiltration amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. (The Air Changes per Hour field should be filled).
-
-#### Field: Design Flow Rate
-
-This field denotes the full design volume flow rate (m<sup>3</sup>/s). The previous field should choose “flow/zone� as the choice. The design volume flow rate is the maximum amount of mixing air expected. The design value is modified by the schedule fraction (see Field: Schedule Name) and user specified coefficients (see four “coefficient� fields below).
-
-#### Field: Flow Rate per Zone Floor Area
-
-This factor (m<sup>3</sup>/s-m<sup>2</sup>) is used, along with the Zone Area to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be “Flow/Area�.
-
-#### Field: Flow Rate per Person
-
-This factor (m<sup>3</sup>/s-person) is used, along with the nominal (maximum) number of occupants (people) in the Zone to determine the maximum Design Volume Flow Rate as described in the Design Volume Flow Rate field. The choice from the method field should be “Flow/Person�.
-
-#### Field: Air Changes per Hour
-
-With this choice, the method used will be the number of air changes per hour for the mixing amount. This factor, along with the Zone Volume, will be used to determine the Design Flow Rate. The choice from the method field should be “AirChanges/Hour�.
-
-#### Field: Source Zone Name
-
-This field is the name of the “source� zone (ref: Zone) that exhausts the amount of air specified by the design level and schedule fields to the zone named in the zone name field. In reality, the “source� and “receiving� zones are interchangeable since the cross-mixed air affects both zones.
-
-#### Field: Delta Temperature
-
-This number controls when mixing air from the source zone is sent to the receiving zone. This parameter is a temperature and is expressed in units of Celsius. If this field is positive, the temperature of the zone from which air is being drawn (“source zone�) must be “Delta Temperature� warmer than the zone air or no mixing occurs. If this field is zero, mixing occurs regardless of the relative air temperatures. Negative values for “Delta Temperature� are not permitted.
-
-#### Field: Delta Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the temperature difference (in Celsius) between the source zone and receiving zone air dry-bulb temperatures as a function of time. This field is an optional field and has the same functionality as the Delta Temperature field. If the user enters a valid schedule name, the delta temperature values specified in this schedule will supersede the constant value specified in the Delta Temperature field.
-
-#### Field: Minimum Zone Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum receiving zone temperature (in Celsius) below which cross mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum zone temperature control is not applied.
-
-#### Field: Maximum Zone Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum receiving zone temperature (in Celsius) above which cross mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum zone temperature control is not applied.
-
-**Note:** The maximum zone temperature when cross mixing is shutoff must be greater than or equal to the minimum zone temperature when cross mixing is shutoff at any given time. Otherwise, warnings will be issued and the maximum zone shutoff temperature will be set to the minimum zone shutoff temperature.
-
-#### Field: Minimum Source Zone Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum source zone temperature (in Celsius) below which cross mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum source zone temperature control is not applied.
-
-#### Field: Maximum Source Zone Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum source zone temperature (in Celsius) above which cross mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum source zone temperature control is not applied.
-
-**Note:** The maximum source zone temperature when cross mixing is shutoff must be greater than or equal to the minimum source zone temperature when cross mixing is shutoff at any given time. Otherwise, warnings will be issued and the maximum source zone shutoff temperature will be set to the minimum source zone shutoff temperature.
-
-#### Field: Minimum Outdoor Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the minimum outdoor temperature (in Celsius) below which cross mixing is shutoff as a function of time. The minimum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the minimum outdoor temperature control is not applied.
-
-#### Field: Maximum Outdoor Temperature Schedule Name
-
-This alpha field contains the name of a schedule (ref. Schedule objects) which contains the maximum outdoor temperature (in Celsius) above which cross mixing is shutoff as a function of time. The maximum temperature value in the schedule can be -100°C and the maximum value can be 100°C. This field is an optional field. If this field is not entered, the maximum outdoor temperature control is not applied.
-
-**Note:** The maximum outdoor temperature when cross mixing is shutoff must be greater than or equal to the minimum outdoor temperature which cross mixing is shutoff at any given time. Otherwise, a warning will be issued and the maximum outdoor shutoff temperature will be set to the minimum outdoor shutoff temperature.
-
-An IDF Example:
-
-```idf
-ZoneCrossMixing,
-    1stFloor-Garage,  !- Name
-    GARAGE,      !- Zone Name
-    Always On,   !- SCHEDULE Name
-    Flow/Zone,               !- Design Flow Rate calculation method
-    0.1,                     !- Design Flow Rate {m3/s}
-    ,                        !- Flow Rate per Area {m3/s/m2}
-    ,                        !- Flow Rate per Person {m3/s/person}
-    ,                        !- Air Changes Per Hour
-    1ST-FLOOR,   !- Source Zone Name
-    1.0;         !- Delta temp
-
-ZoneCrossMixing,
-    Garage-1stFloor,  !- Name
-    1ST-FLOOR,   ! Zone Name
-    Always On,   !- SCHEDULE Name
-    flow/zone,               !- Design Flow Rate calculation method
-    0.1,                     !- Design Flow Rate {m3/s}
-    ,                        !- Flow Rate per area {m3/s/m2}
-    ,                        !- Flow Rate per person {m3/s/person}
-    ,                        !- Air Changes Per Hour
-    GARAGE,      ! Source Zone Name
-    1.0;         ! Delta temp
-```
-
-
-### Zone Cross Mixing Outputs
-
-* HVAC,Sum,Zone Mixing Volume [m3]
-
-* HVAC,Sum,Zone Mixing Current Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Mixing Standard Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Mixing Mass [kg]
-
-* HVAC,Sum,Zone Mixing Mass Flow Rate [kg/s]
-
-* HVAC,Sum,Zone Mixing Sensible Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Mixing Sensible Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Mixing Latent Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Mixing Latent Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Mixing Total Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Mixing Total Heat Gain Energy [J]
-
-#### Zone Mixing Volume [m3]
-
-The air volume in m<sup>3</sup> entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
-
-#### Zone Mixing Current Density Volumetric Flow Rate [m3/s]
-
-The air volumetric flow rate in m<sup>3</sup>/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at current zone air conditions.
-
-#### Zone Mixing Standard Density Volumetric Flow Rate [m3/s]
-
-The air volumetric flow rate in m<sup>3</sup>/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at standard conditions.
-
-#### Zone Mixing Mass [kg]
-
-The air mass in kg entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep. The air mass is calculated using the air volume flow from each “source� zone and the density of air calculated for the average conditions (temperature and humidity) between the “source� and “receiving� zones.
-
-#### Zone Mixing Mass Flow Rate [kg/s]
-
-The air mass flow rate in kg/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
-
-#### Zone Mixing Sensible Heat Loss Energy [J]
-
-#### Zone Mixing Sensible Heat Gain Energy [J]
-
-The sensible (temperature) heat transfer due to the sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the specific heat (calculated for the average conditions (temperature and humidity) between the “source� and “receiving� zones) and the temperature differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing sensible heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing sensible heat gain.
-
-#### Zone Mixing Latent Heat Loss Energy [J]
-
-#### Zone Mixing Latent Heat Gain Energy [J]
-
-The latent heat transfer due tothe sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the heat of vaporization (calculated for the average conditions (temperature and humidity) between the “source� and “receiving� zones)and the humidity ratio differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing latent heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing latent heat gain.
-
-#### Zone Mixing Total Heat Loss Energy [J]
-
-The total heat loss due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy &lt; the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
-
-#### Zone Mixing Total Heat Gain Energy [J]
-
-The total heat gain due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy &gt;= the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
-
-### ZoneRefrigerationDoorMixing
-
-The ZoneRefrigerationDoorMixing syntax is ideally suited for two zones, at least one of which is refrigerated, that exchange an equal amount of dry air. They may also have mixed air from other zones, but only one object should be entered for any one pair of zones. As with Mixing (ref: Mixing), this is a simplified view of interzone airflow in EnergyPlus. The ZoneRefrigerationDoorMixing approach shares some features of both Mixing and Cross Mixing. Like Cross Mixing, RefrigerationDoorMixing has an energy effect on both the source and the receiving zone, thus maintaining both the air mass and energy balances in the two zones. Like Mixing, the refrigerated zone can exchange air with multiple zones.  Unlike either of the other two mixing objects, the RefrigeratedDoorMixing always calculates the air exchange based on the zone temperature and relative humidity. That is, the user does not specify the air flow rate. The user can moderate the flow through a door-opening schedule.
-
-Unlike, Cross Mixing, Refrigeration Door Mixing can only be entered once for any unique pair of zones. It doesn’t matter which zone is listed first and the zones will automatically switch back and forth between source and receiving zones depending upon which zone is colder.
-
-Refrigeration Door Mixing is entered using the following syntax.
-
-#### Field: Name
-
-The name of the ZoneRefrigerationDoorMixing object.
-
-#### Field: Zone 1  Name
-
-This field is the name of one of the two zones (ref: Zone) exchanging air and attaches a particular refrigeration door  mixing statement to both thermal zones in the building.
-
-#### Field: Zone 2  Name
-
-This field is the name of the other zone (ref: Zone) exchanging air and attaches a particular refrigeration door  mixing statement to both thermal zones in the building.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the door opening between the two zones and should contain values between  0.0 and 1.0.
-
-#### Field: Door Height
-
-This field denotes the door opening height (m). The default value is 3 m.
-
-#### Field: Door  Area
-
-This field denotes the door opening area (m<sup>2</sup>). The default value is 9 m<sup>2</sup>.
-
-#### Field: Door Protection Type
-
-This field is a key/choice field that tells how the door is protected. The impact of this choice is decribed in the Engineering Reference. The key/choices are:
-
-- None
-
-None, or no door protection is the default choice
-
-- AirCurtain
-
-- StripCurtain
-
-An IDF Example:
-
-```idf
-ZoneRefrigerationDoorMixing,
-    Freezer1_Cooler1,  !- Name
-    Freezer1,          !- Zone 1 Name
-    Cooler1,           !- Zone 2 Name
-    Freezer1DoorSched, !- Schedule Name
-    1.8,               !- Door height {m}
-    2.3,               !- Door area {m2}
-    StripCurtain;      !- Door protection type
-```
-
-
-### Refrigeration Door Mixing Outputs
-
-* HVAC,Sum,Zone Mixing Volume [m3]
-
-* HVAC,Sum,Zone Mixing Current Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Mixing Standard Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Mixing Mass [kg]
-
-* HVAC,Sum,Zone Mixing Mass Flow Rate [kg/s]
-
-* HVAC,Sum,Zone Mixing Sensible Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Mixing Sensible Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Mixing Latent Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Mixing Latent Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Mixing Total Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Mixing Total Heat Gain Energy [J]
-
-
-#### Zone Mixing Volume [m3]
-
-The air volume in m<sup>3</sup> entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
-
-#### Zone Mixing Current Density Volumetric Flow Rate [m3/s]
-
-The air volumetric flow rate in m<sup>3</sup>/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at current zone air conditions.
-
-#### Zone Mixing Standard Density Volumetric Flow Rate [m3/s]
-
-The air volumetric flow rate in m<sup>3</sup>/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep using the density of air evaluated at standard conditions.
-
-#### Zone Mixing Mass [kg]
-
-The air mass in kg entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep. The air mass is calculated using the air volume flow from each “source� zone and the density of air calculated for the average conditions (temperature and humidity) between the “source� and “receiving� zones.
-
-#### Zone Mixing Mass Flow Rate [kg/s]
-
-The air mass flow rate in kg/s entering the zone due to the sum of mixing, cross-mixing, and refrigeration-door mixing during the hour or timestep.
-
-#### Zone Mixing Sensible Heat Loss Energy [J]
-
-#### Zone Mixing Sensible Heat Gain Energy [J]
-
-The sensible (temperature) heat transfer due to the sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the specific heat (calculated for the average conditions (temperature and humidity) between the “source� and “receiving� zones) and the temperature differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing sensible heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing sensible heat gain.
-
-#### Zone Mixing Latent Heat Loss Energy [J]
-
-#### Zone Mixing Latent Heat Gain Energy [J]
-
-The latent heat transfer due tothe sum of mixing, cross-mixing, and refrigeration-door mixing in the host (receiving) zone is the sum of all the incoming air mass flow rates multiplied by the elapsed time, the heat of vaporization (calculated for the average conditions (temperature and humidity) between the “source� and “receiving� zones)and the humidity ratio differences between the host zone and corresponding source zones. If the heat transfer is negative, the heat transfer is considered to be a zone mixing latent heat loss. If the heat transfer is positive, the heat transfer is considered to be a zone mixing latent heat gain.
-
-#### Zone Mixing Total Heat Loss Energy [J]
-
-The total heat loss due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy &lt; the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
-
-#### Zone Mixing Total Heat Gain Energy [J]
-
-The total heat gain due to the sum of mixing, cross-mixing, and refrigeration-door mixing that occurs when the sum of Zone Mixing Sensible Heat Gain Energy and Zone Mixing Latent Heat Gain Energy &gt;= the sum of Zone Mixing Sensible Heat Loss Energy and Zone Mixing Latent Heat Loss Energy.
-
-### ZoneEarthtube (Earth Tube)
-
-An earth tube is a long, underground metal or plastic pipe through which air is drawn. During cooling season, as air travels through the pipe, it gives up some of its heat to the surrounding soil and enters the room as cooler air. Similarly, during heating season, as air travels through the pipe, it receives some of its heat from the soil and enters the room as warmer air. Simple earth tubes in EnergyPlus can be controlled by a schedule and through the specification of minimum, maximum, and delta temperatures as described below. As with infiltration and ventilation, the actual flow rate of air through the earth tube can be modified by the temperature difference between the inside and outside environment and the wind speed. The basic equation used to calculate air flow rate of earth tube in EnergyPlus is:
-
-<div>\[EarthTubeFlowRate = \left( {{E_{design}}} \right)\left( {{F_{schedule}}} \right)\left[ {A + B\left| {{T_{zone}} - {T_{odb}}} \right| + C\left( {WindSpeed} \right) + D\left( {WindSpee{d^2}} \right)} \right]\]</div>
-
-For the simulation of the earth tube, a weather data file is required and, therefore, the earth tube cannot run without weather data file. The required input fields to simulate the earth tube include the average soil surface temperature, the amplitude of soil surface temperature, and the phase constant of soil surface temperature. These fields should be calculated in advance by using a separate stand-alone program (CalcSoilSurfTemp) and should be input into earth tube.
-
-#### CalcSoilSurfTemp – Auxiliary Programs Document
-
-The CalcSoilSurfTemp program is simple and requires only two input fields : soil condition and soil surface condition in addition to a valid weather file. For soil condition, the user should select the number corresponding to the actual condition of the soil surrounding the earth tube from the four following options: 1. HEAVY AND SATURATED, 2. HEAVY AND DAMP, 3. HEAVY AND DRY and 4. LIGHT AND DRY. This determines the thermal diffusivity and thermal conductivity of the surrounding soil. For soil surface conditions, the user should select the number corresponding to the actual condition of the ground surface above the earth tube from the eight following options: 1. BARE AND WET, 2. BARE AND MOIST, 3. BARE AND ARID, 4. BARE AND DRY, 5. COVERED AND WET, 6. COVERED AND MOIST, 7. COVERED AND ARID and 8. COVERED AND DRY. This determines the absorption coefficient and the fraction of evaporation rate of the ground surface.
-
-From this information and an analysis of the weather for the location selected, the CalcSoilSurfTemp program (ref. Auxiliary Programs document) calculates the three parameters listed above. The user must then add these parameters as input into EnergyPlus. The full input description of an earth tube in EnergyPlus is given below.
-
-#### Field: Zone Name
-
-This field is the name of the zone (ref: Zone) and attaches a particular earth tube statement to a thermal zone in the building.
-
-#### Field: Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that modifies the maximum design volume flow rate parameter (see next field). This fraction between 0.0 and 1.0 is noted as F<sub>schedule</sub> in the above equation.
-
-#### Field: Design Flow Rate
-
-This number (noted as E<sub>design</sub> in the above equation) is the maximum amount of air mass flow rate of the earth tube expected at design conditions. The flow rate is expressed in units of m<sup>3</sup>/s. The design value is modified by the schedule fraction (see previous field) and user specified coefficients (see last four fields).
-
-#### Field: Minimum Zone Temperature when Cooling
-
-This is the indoor temperature (in Celsius) below which the earth tube is shut off. This lower temperature limit is intended to avoid overcooling a space and thus result in a heating load. For example, if the user specifies a minimum temperature of 20°C, earth tube is assumed to be available if the zone air temperature is above 20°C. If the zone air temperature drops below 20°C, then earth tube is automatically turned off.
-
-#### Field: Maximum Zone Temperature when Heating
-
-This is the indoor temperature (in Celsius) above which the earth tube is shut off. This higher temperature limit is intended to avoid overheating a space and thus result in a cooling load. For example, if the user specifies a maximum temperature of 20°C, earth tube is assumed to be available if the zone air temperature is below 20°C. If the zone air temperature rises above 20°C, then earth tube is automatically turned off.
-
-#### Field: Delta Temperature
-
-This is the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which the earth tube is shut off. This is to allow the earth tube to be stopped either if the temperature outside is too warm and could potentially heat the space or if the temperature outside is too cold and could potentially cool the space. For example, if the user specifies a delta temperature of 2°C, earth tube is assumed to be available if the temperature difference between indoor and outdoor temperature is at least 2°C. If the outside air dry-bulb temperature is less than 2°C cooler or warmer than the indoor dry-bulb temperature, then the earth tube is automatically turned off.
-
-#### Field: Earthtube Type
-
-This alpha character string defines the type of earth tube as one of the following options: Natural, Exhaust, or Intake. A natural earth tube is assumed to be air movement/exchange that will not consume any fan energy or is the result of natural air flow through the tube and into the building. Values for fan pressure and efficiency for a natural flow earth tube are ignored. For either EXHAUST or Intake, values for fan pressure and efficiency define the fan electric consumption. For Natural and Exhaustearth tubes, the conditions of the air entering the space are assumed to be equivalent to the air which is cooled or heated by passing along the pipe. For Intake earth tubes, an appropriate amount of fan heat is added to the air stream.
-
-#### Field: Fan Pressure Rise
-
-This is the pressure rise experienced across the fan in Pascals (N/m<sup>2</sup>). This is a function of the fan and plays a role in determining the amount of energy consumed by the fan.
-
-#### Field: Fan Total Efficiency
-
-This is the total fan efficiency (a decimal number between 0.0 and 1.0). This is a function of the fan and plays a role in determining the amount of energy consumed by the fan.
-
-#### Field: Pipe Radius
-
-This is the radius of the earth tube/pipe (in meters). This plays a role in determining the amount of heat transferred from the surrounding soil to the air passing along the pipe. If the pipe has non-circular cross section, user can use the concept of hydraulic diameter as follows.
-
-<div>\[D = 4 \times Area/Perimeter\]</div>
-
-However, since this field requires the pipe radius, hydraulic diameter should be divided by two.
-
-#### Field: Pipe Thickness
-
-This is the thickness of the pipe wall (in meters). This plays a role in determining the amount of heat transferred from the surrounding soil to the air passing along the pipe.
-
-#### Field: Pipe Length
-
-This is the total length of the pipe (in meters). This plays a role in determining the amount of heat transferred from the surrounding soil to the air passing along the pipe. As the length of the pipe becomes longer, the amount of the heat transfer becomes larger.
-
-#### Field: Pipe Thermal Conductivity
-
-This is the thermal conductivity of the pipe (in W/m°C). This plays a role in determining the amount of heat transferred from the surrounding soil to the air passing along the pipe.
-
-#### Field: Pipe Depth Under Ground Surface
-
-This is the depth of the pipe under the ground surface (in meters). This plays a role in determining the temperature of the soil surrounding the pipe.
-
-#### Field: Soil Condition
-
-This alpha character string defines the actual condition of the soil surrounding the earth tube and can be one of any of the following options: HeavyAndSaturated, HeavyAndDamp, HeavyAndDry or LightAndDry. This determines the thermal diffusivity and thermal conductivity of the surrounding soil, which play a role in determining the amount of heat transferred from the surrounding soil to the air passing along the pipe.
-
-#### Field: Average Soil Surface Temperature
-
-This is the annual average soil surface temperature straight above the earth tube, which plays a role in determining the temperature of the soil surrounding the pipe. This field should be calculated in advance using the separate CalcSoilSurfTemp program.
-
-#### Field: Amplitude of Soil Surface Temperature
-
-This is the amplitude of soil surface temperature above the earth tube, which plays a role in determining the temperature of the soil surrounding the pipe. This is the difference between the maximum and minimum soil surface temperature for the whole year divided by two. This field should be calculated in advance using the separate CalcSoilSurfTemp program.
-
-#### Field: Phase Constant of Soil Surface Temperature
-
-This is the phase constant of the soil surface temperature straight above the earth tube, which play a role in determining the temperature of the soil surrounding the pipe at particular time. This is the time elapsed from the beginning of the year until the soil surface temperature reaches the minimum value of the year. This field should be calculated in advance using the separate CalcSoilSurfTemp program.
-
-#### Field: Constant Term Flow Coefficient
-
-This number is the “A� parameter in the above earth tube equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter, however, is a constant under all conditions and is not modified by any environmental effect. As a result, it is dimensionless.
-
-#### Field: Temperature Term Flow Coefficient
-
-This number is the “B� parameter in the above earth tube equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the temperature difference between the outdoor and indoor air dry-bulb temperatures. The units for this parameter are inverse Celsius.
-
-#### Field: Velocity Term Flow Coefficient
-
-This number is the “C� parameter in the above earth tube equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by the speed of wind being experienced outside the building. The units for this parameter are s/m.
-
-#### Field: Velocity Squared Term Flow Coefficient
-
-This number is the “D� parameter in the above earth tube equation. It is part of the user specified modifying parameters that are a function of environmental factors. This parameter is modified by square of the speed of wind being experienced outside the building. The units for this parameter are s<sup>2</sup>/m<sup>2</sup>.
-
-An IDF example:
-
-```idf
-EARTHTUBE,
-  Zone 2,           !- Zone Name
-  Simple EarthTube, !- Schedule Name
-  3.425198,         !- Design Volume Flow Rate
-  10.0,             !- Minimum Zone Temperature when Cooling
-  30.0,             !- Maximum Zone Temperature when Heating
-  1.0,              !- Delta Temperature
-  NATURAL,          !- EarthTube Type
-  350.0,            !- Fan Pressure Rise
-  0.9,              !- Fan Total Efficiency
-  0.25,             !- Pipe Radius
-  0.2,              !- Pipe Thickness
-  15.0,             !- Pipe Length
-  200.0,            !- Pipe Thermal Conductivity
-  3.5,              !- Pipe Depth Under Ground Surface
-  HeavyAndDamp,     !- Soil Condition
-  15.0,             !- Average Soil Surface Temperature
-  5.6,              !- Amplitude of Soil Surface Temperature
-  0.0,              !- Phase Constant of Soil Surface Temperature
-  0.6060000    ,    !- Constant Term Flow Coef
-  2.0199999E-02,    !- Temp Term Flow Coef
-  5.9800001E-04,    !- Velocity Term Flow Coef
-  0.0000000E+00;    !- Velocity**2 Term Flow Coef
-```
-
-
-### ZoneEarthTube Outputs
-
-Current Earth Tube output variables:
-
-* HVAC,Sum,Earth Tube Zone Sensible Cooling Energy [J]
-
-* HVAC,Average,Earth Tube Zone Sensible Cooling Rate [W]
-
-* HVAC,Sum,Earth Tube Zone Sensible Heating Energy [J]
-
-* HVAC,Average,Earth Tube Zone Sensible Heating Rate [W]
-
-* HVAC,Sum,Earth Tube Air Flow Volume [m3]
-
-* HVAC,Average,Earth Tube Air Current Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Average,Earth Tube Air Standard Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Sum,Earth Tube Air Flow Mass [kg]
-
-* HVAC,Average,Earth Tube Air Mass Flow Rate [kg/s]
-
-* HVAC,Sum,Earth Tube Fan Electric Energy [J]
-
-* HVAC,Average,Earth Tube Fan Electric Power [W]
-
-* HVAC,Average,Earth Tube Zone Inlet Air Temperature [C]
-
-* HVAC,Average,Earth Tube Ground Interface Temperature [C]
-
-* HVAC,Average,Earth Tube Outdoor Air Heat Transfer Rate [W]
-
-#### Earth Tube Zone Sensible Cooling Energy [J]
-
-#### Earth Tube Zone Sensible Cooling Rate [W]
-
-These are the energy and rate associated with the zone cooling provided by the air from the earth tube.  This occurs when the earth tube outlet air temperature is less than zone air temperature.
-
-#### Earth Tube Zone Sensible Heating Energy [J]
-
-#### Earth Tube Zone Sensible Heating Rate [W]
-
-These are the energy and rate associated with the zone heating provided by the air from the earth tube.  This occurs when the earth tube outlet air temperature is greater than the zone air temperature.
-
-#### Earth Tube Air Flow Volume [m3]
-
-The volume flow of air through the earth tube.
-
-#### Earth Tube Air Current Density Volumetric Flow Rate [m3/s]
-
-The volume flow rate of air through the earth tube evaluating density at current zone conditions.
-
-#### Earth Tube Air Standard Density Volumetric Flow Rate [m3/s]
-
-The volume flow rate of air through the earth tube evaluating density at standard conditions.
-
-#### Earth Tube Air Flow Mass [kg]
-
-The mass flow of air through the earth tube.
-
-#### Earth Tube Air Mass Flow Rate [kg/s]
-
-The mass flow rate of air through the earth tube.
-
-#### Earth Tube Fan Electric Energy [J]
-
-#### Earth Tube Fan Electric Power [W]
-
-These are the fan electricity consumption and power for intake or exhaust earth tube types.
-
-#### Earth Tube Zone Inlet Air Temperature [C]
-
-This is the temperature of the air entering the zone after passing through the earth tube [C].  This temperature includes the cooling or heating of outdoor air as it passes along the pipe.  When intake fan assist is used, then the additional heat due to the fan is included in the inlet air temperature.
-
-#### Earth Tube Ground Interface Temperature [C]
-
-This is the average temperature of the ground along the outer surface of the earth tube [C].
-
-#### Earth Tube Outdoor Air Heat Transfer Rate [W]
-
-This is the rate of heat transfer from the earth tube to the outdoor air [W].  Positive values indicate the rate at which outdoor air is preheated; negative values indicate the rate of precooling.
-
-### ZoneCoolTower:Shower
-
-A cooltower (which is sometimes referred to as a wind tower or a shower cooling tower) is a component that is intended to model a passive downdraught evaporative cooling (PDEC) that is designed to capture the wind at the top of a tower and cool the outside air using water evaporation before delivering it to a space.  The air flow in these systems is natural as the evaporation process increases the density of the air causing it to fall through the tower and into the space without the aid of a fan.  A cooltower typically consists of a water spray or an evaporative pad, a shaft, and a water tank or reservoir.  Wind catchers to improve the wind-driven performance at the top of the tower are optional.  Water is pumped over an evaporative device by water pump which is the only component consumed power for this system.  This water cools and humidifies incoming air and then the cool, dense air naturally falls down through shaft and leaves through large openings at the bottom of cooltowers.
-
-The shower cooling tower can be controlled by a schedule and the specification of maximum water flow rate and volume flow rate as well as minimum indoor temperature.  The actual flow rate of water and air can be controlled as users specify the fractions of water loss and flow schedule.  The required input fields include effective tower height and exit area to obtain the temperature and flow rate of the air exiting the tower.  A schedule and rated power for the water pump are also required to determine the power consumed. The component typically has a stand alone water system that is not added to the water consumption from mains. However, users are required to specify the water source through an optional field, the name of water supply storage tank, in case any water comes from a water main. The model is described more fully in the Engineering Reference document.
-
-This model requires weather information obtained from either design day or weather file specifications.  The control is accomplished by either specifying the water flow rate or obtaining the velocity at the outlet with inputs and weather conditions when the water flow rate is unknown.  As with infiltration, ventilation, and earth tubes, the component is treated in a similar fashion to “natural ventilation� in EnergyPlus.
-
-#### Field: Name
-
-This field is a unique user assigned name for each cooltower.  Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This field is the name of the schedule that denotes whether the cooltower can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the cooltower is available and can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the cooltower is not available and must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Zone Name
-
-This field is the name of the zone (ref: Zone) and attaches a particular cooltower statement to a thermal zone in the building.
-
-#### Field: Water Supply Storage Tank Name
-
-This field is optional.  It is used to describe where the cooltower obtains water used for evaporative cooling.  If blank or omitted, then the cooltower will obtain water directly from local water main.  If the name of a Water Storage Tank object is used here, then the cooltower will obtain its water from that tank.  If a tank is specified, the cooltower will attempt to obtain all the water it uses from the tank.  However, if the tank cannot provide all the water the cooltower needs, then the cooltower will still operate and obtain the rest of the water it needs from the mains (referred to as ‘Starved’ water).
-
-#### Field: Flow Control Type
-
-This field specifies how the user wishes to control the cooltower.  The air flow from the cooltower may be controlled by either the water flow rate along with the water pump schedule or naturally driven by wind flow.  The user must select from the following options: **WaterFlowSchedule** and **WindDrivenFlow**.  If the user either wishes to control the water flow rate or has information about the water flow rate, **WaterFlowSchedule** must be selected.  **WindDrivenFlow** for cooltower flow control must be selected when the water flow rate is unknown and the user wishes to have the flow rate of both air and water controlled by the external weather conditions (wind speed).  If the user does not select a control type, **WindDrivenFlow** is assumed as a flow control type.
-
-#### Field: Pump Flow Rate Schedule Name
-
-This field modifies the maximum flow rate of water through the cooltower in m3/sec. This input is “optional.� If the user does not enter a schedule, the flow rate through the cooltower is assumed to be constant during all hours that it is operating based on the value entered in the previous input field. Note that the values for this schedule must be between zero and one.
-
-#### Field: Maximum Water Flow Rate
-
-This field is the maximum water flow rate distributed to the tower in m3/s. This limit is intended to avoid over estimation of water flow rate, which leads higher air flow rate and exit temperature of the air. 
-
-#### Field: Effective Tower Height
-
-This field is the effective tower height for evaporative cooling, from the water spray to the top of the exit in m.
-
-#### Field: Airflow Outlet Area
-
-This field is the area at the exit of the tower in m2.  This field is used to determine the air flow rate leaving the tower with the velocity of the air flow.
-
-#### Field: Maximum Air Flow Rate
-
-This field is the maximum volumetric flow rate of the air leaving the tower in m3/s.  This airflow maximum allows the cooltower performance to be limited if the outside wind speed and the tower height are relatively high and thus result in high airflow supplied to the space.
-
-#### Field: Minimum Indoor Temperature
-
-This field is the minimum indoor temperature in Celsius below which cooltower is shutoff.  This lower temperature limit is intended to avoid overcooling a space and thus result in a heating load.  For example, if the user specifies a minimum temperature of 20°C, cooltower is assumed to be available if the zone air temperature is above 20°C.  If the zone air temperature drops below 20°C, then cooltower is automatically turned off.
-
-#### Field: Fraction of Water Loss
-
-This field specifies the fraction of the loss of water during either operation or transient operation. If the user does not enter a fraction, no loss of water is assumed and the cooltower water consumption includes only evaporation.  Note that the fraction must be between zero and one.
-
-#### Field: Fraction of Flow Schedule
-
-This field specifies the fraction of the airflow that actually goes to the outside.  The user who wishes to control the actual flow to the inside of the building must specify the value of the fraction.  If the user does not enter a fraction, the calculated flow rate is the “zone cooltower volume flow rate.�  Note that the fraction must be between zero and one.
-
-#### Field: Rated Power Consumption
-
-This field is the pump’s rated power consumption in Watts.
-
-Below is an example input for a cooltower.
-
-```idf
-ZoneCoolTower:Shower
- Cool Tower 1,         !- Name of cooltowers
- Zone 1,               !- Zone name
- Simple Vent,          !- Schedule
- ,                     !- Name of water supply storage tanks
- WindDrivenFlow,       !- Flow control type
- 0.0005,               !- Water flow rate from the spray in m3/s
- ,                     !- schedule for flow rate (optional, non-existent means constant)
- 5.0,                  !- Effective tower height in m
- 1.0,                  !- Exit area in m2
- 10.0,                 !- Maximum supply air volume flow rate in m3/s
- 18.0,                 !- Minimum indoor temperature to prevent overcooling in C
- 0.05,                 !- Fraction of Water loss
- 0.05,                 !- Fraction of flow that goes to outside
- 250.0;                !- Rated power consumption in W
-```
-
-
-### ZoneCoolTower:Shower Outputs
-
-* HVAC,Sum,Zone Cooltower Sensible Heat Loss Energy [J]
-
-* HVAC,Average,Zone Cooltower Sensible Heat Loss Rate [W]
-
-* HVAC,Sum,Zone Cooltower Latent Heat Loss Energy [J]
-
-* HVAC,Average,Zone Cooltower Latent Heat Loss Rate [W]
-
-* HVAC,Sum,Zone Cooltower Air Volume [m3]
-
-* HVAC,Average,Zone Cooltower Air Current Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Average,Zone Cooltower Air Standard Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Cooltower Air Mass [kg]
-
-* HVAC,Average,Zone Cooltower Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Cooltower Air Inlet Temperature [C]
-
-* HVAC,Average,Zone Cooltower Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC,Average,Zone Cooltower Air Outlet Temperature [C]
-
-* HVAC,Average,Zone Cooltower Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC,Average,Zone Cooltower Pump Electric Power [W]
-
-* HVAC,Sum,Zone Cooltower Pump Electric Energy [J]
-
-* HVAC,Sum,Zone Cooltower Water Volume [m3]
-
-* HVAC,Sum,Zone Cooltower Mains Water Volume [m3]
-
-* HVAC,Sum,Zone Cooltower Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Zone Cooltower Starved Mains Water Volume [m3]
-
-
-#### Zone Cooltower Sensible Heat Loss Energy [J]
-
-#### Zone Cooltower Sensible Heat Loss Rate [W]
-
-The sensible heat loss that occurs when the temperature at the exit of the cooltower is less than that of the zone.
-
-#### Zone Cooltower Latent Heat Loss Energy [J]
-
-#### Zone Cooltower Latent Heat Loss Rate [W]
-
-The latent heat loss that occurs when the humidity ratio at the exit of the cooltower is greater than that of the zone.
-
-#### Zone Cooltower Air Current Density Volumetric Flow Rate [m3/s]
-
-The volumetric flow rate of the air leaving the cooltower evaluating density at current zone conditions.
-
-#### Zone Cooltower Air Standard Density Volumetric Flow Rate [m3/s]
-
-The volumetric flow rate of the air leaving the cooltower evaluating density at standard conditions.
-
-#### Zone Cooltower Air Volume [m3]
-
-The sum of actual volumetric flow of the air leaving cooltower
-
-#### Zone Cooltower Air Mass Flow Rate [kg/s]
-
-The mass flow rate of the air leaving the cooltower
-
-#### Zone Cooltower Air Mass [kg]
-
-The sum of actual mass flow of the air leaving the cooltower
-
-#### Zone Cooltower Air Inlet Temperature [C]
-
-The dry-bulb temperature of the outdoor air the inlet of the cooltower
-
-#### Zone Cooltower Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
- The humidity ratio of the outdoorair at the inlet of the cooltower
-
-#### Zone Cooltower Air Outlet Temperature [C]
-
-The temperature at the exit of the cooltower.
-
-#### Zone Cooltower Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-The humidity ratio of the air at the exit of the cooltower.
-
-#### Zone Cooltower Water Volume  [m3]
-
-The water consumption includes not only the direct thermodynamics of water evaporation but also other sources of consumption such as drift or concentration blow down specified by users throughout all processes during the operation. 
-
-#### Zone Cooltower Mains Water Volume  [m3]
-
-This is the water consumed by the cooltower that actually be met by the mains water. This output variable appears only when the water comes from mains. 
-
-#### Zone Cooltower Storage Tank Water Volume  [m3]
-
-This is the water consumed by the cooltower that actually be met by the water storage tank.  If any amount of the water is starved from mains, this water consumption is the difference between the Zone Cooltower Water Volume and the following output.  This output variable appears only when the water comes from storage tank waters.
-
-#### Zone Cooltower Starved Mains Water Volume [m3]
-
-This is the source (mains) of water consumed by the cooltower that could not actually be met by the storage tank.  This output variable appears only when the water comes from storage tank waters.
-
-#### Zone Cooltower Pump Electric Power [W]
-
-The power consumed by the recirculating pump in Watts.
-
-#### Zone Cooltower Pump Electric Energy [J]
-
-The energy consumed by the recirculating pump in Joules.
-
-### ZoneThermalChimney (Thermal Chimney)
-
-A thermal chimney is a vertical shaft utilizing solar radiation to enhance the natural ventilation in buildings. It consists of a absorber wall, air gap and glass cover with high solar transmissivity. For the high solar absorption, it is usually south facing.
-
-The key output parameter in the thermal chimney model is the enhanced amount of natural ventilation rate caused by the presence of a thermal chimney. In order to determine the enhanced ventilation, the discharge air temperature from a thermal chimney should be calculated, which, in turn, should be computed based on the information on the absorber wall temperature, glass cover temperature and the vertical air temperature distribution within the thermal chimney. Among them, energy balances for the absorber wall and the glass cover are carried out using the existing algorithm currently available in EnergyPlus, which has the similar approach to the Trombe wall. As stated in the Trombe wall object as well, this approach allows the flexibility for users to specify the various wall parameters and to explore unusual configurations. On the other hand, the vertical air temperature distribution and the resultant discharge air temperature of the thermal chimney are computed using the separate thermal chimney algorithm described in the Engineering Reference document.
-
-Similar to the Trombe wall model, a zone is coupled to the desired surface via an interzone partition. To simulate the thermal chimney, the Solar Distribution field in the Building object should be set to FullInteriorAndExterior so that the majority of the solar flux is directed on the absorber wall. For a normal sized thermal chimney zone, the user can set the Zone Inside Convection Algorithm to “Detailed�, which takes into account natural convection effects intended for a normal zone. For a narrow cavity zone having high aspect ratios, there is no built-in algorithm for calculating the correct convection coefficients on the inside of thermal chimney zone walls. One option is to use the “Detailed� convection algorithm similar to the Trombe wall model. However, some error may be incurred when used with a narrow zone. Another option is to use the SurfaceProperty:ConvectionCoefficients object to schedule coefficients that have been determined beforehand by the user. In addition, the wall construction of the adjoining zone must be the mirror image of the wall construction in the thermal chimney zone.
-
-The full input description of a thermal chimney in EnergyPlus is given below.
-
-#### Field: Name
-
-This field is a unique user assigned name for an instance of the thermal chimney system.
-
-#### Field: Zone Name
-
-This field is the name of the thermal chimney zone (ref: Zone). Since the thermal chimney is not only a system component but also a zone itself, this field is also necessary. It should be differentiated from the *Zone name* field described later.
-
-#### Field: Availability Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that denotes whether the thermal chimney can operate during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the system is available and can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the system is not available and must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Width of the Absorber Wall
-
-This number is the width of the absorber wall in the thermal chimney.  The width is expressed in units of m. Even though this value is specified in Surface objects as well, this value is used to compute the discharge air temperature and the enhanced ventilation rate caused by the thermal chimney.
-
-#### Field: Cross Sectional Area of Air Channel Outlet
-
-This number is the cross sectional area of air channel outlet. The area is expressed in units of m<sup>2</sup>. The enhanced air flow rate by the thermal chimney is dependent on cross sectional areas of air channel inlet and outlet. Cross sectional areas of air channel inlet will be described later in conjunction with the distance from the top of thermal chimney to each inlet and relative ratios of air flow rates passing through each inlet.
-
-#### Field: Discharge Coefficient
-
-This dimensionless number is the discharge coefficient of the thermal chimney. The ventilation rate enhanced by the thermal chimney is also dependent on the discharge coefficient.
-
-#### Field: Zone &lt;\#&gt; Name
-
-This field is the name of the zone (ref: Zone) to which the thermal chimney is attached. It is used in conjunction with the next three fields. Note that up to 20 sets of zone name, distance from the top of the thermal chimney to each inlet, relative ratios of air flow rates passing through each zone and cross sectional areas of each air channel inlet may be entered for a single thermal chimney if multiple zones share the common thermal chimney.
-
-#### Field: Distance from Top of Thermal Chimney to Inlet &lt;\#&gt;
-
-This field is the distance from the top of the thermal chimney to each inlet corresponding to each zone. It is used in conjunction with the zone name, relative ratios of air flow rates passing through each zone and cross sectional areas of each air channel inlet. The distance is expressed in units of m. The air flow rate enhanced by the thermal chimney is dependent on the distance between the thermal chimney outlet and inlet.
-
-#### Field: Relative Ratios of Air Flow Rates Passing through Zone &lt;\#&gt;
-
-This dimensionless number is the relative ratio of air flow rates enhanced by the thermal chimney passing through each zone. The total air flow rate enhanced by the thermal chimney is distributed to each zone based on this number if multiple zones share the common thermal chimney. It is used in conjunction with the zone name, the distance from the top of the thermal chimney to each inlet and cross sectional areas of each air channel inlet. Note that the sum of all ratios must be equal to 1.0.
-
-#### Field: Cross Sectional Areas of Air Channel Inlet &lt;\#&gt;
-
-This field is the cross sectional areas of each air channel inlet corresponding to each zone. It is used in conjunction with the zone name, the distance from the top of the thermal chimney to each inlet and relative ratios of air flow rates passing through each zone. The area is expressed in units of m<sup>2</sup>. The air flow rate enhanced by the thermal chimney is dependent on cross sectional areas of air channel inlet and outlet.
-
-
-
-An IDF example:
-
-```idf
-ZoneThermalChimney,
-  ThermalChimney1,               !- Name of Thermal Chimney System
-  ThermalChimneyZone,            !- Name of Thermal Chimney Zone
-  ThermalChimneyAvail,           !- Availability Schedule Name
-  3.5,                           !- Width of the Absorber Wall
-  0.04,                          !- Cross Sectional Area of Air Channel Outlet
-  0.8,                           !- Discharge Coefficient
-  Zone1,                         !- Zone Name 1
-  8.0,                           !- Distance from the Top of the Thermal Chimney to Inlet 1
-  0.8,                           !- Relative Ratios of Air Flow Rates Passing through Zone 1
-  0.02,                          !- Cross Sectional Areas of Air Channel Inlet 1
-  Zone2,                         !- Zone Name 2
-  5.0,                           !- Distance from the Top of the Thermal Chimney to Inlet 2
-  0.2,                           !- Relative Ratios of Air Flow Rates Passing through Zone 2
-  0.02;                          !- Cross Sectional Areas of Air Channel Inlet 2
-```
-
-
-### ZoneThermalChimney Outputs
-
-Current ThermalChimney output variables:
-
-* HVAC,Average,Zone Thermal Chimney Current Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Average,Zone Thermal Chimney Standard Density Volumetric Flow Rate [m3/s]
-
-* HVAC,Average,Zone Thermal Chimney Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Thermal Chimney Outlet Temperature [C]
-
-* HVAC,Sum,Zone Thermal Chimney Heat Loss Energy [J]
-
-* HVAC,Sum,Zone Thermal Chimney Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Thermal Chimney Volume [m3]
-
-* HVAC,Sum,Zone Thermal Chimney Mass [kg]
-
-#### Zone Thermal Chimney Heat Loss Energy [J]
-
-The sensible (temperature) heat loss of each zone that occurs when the thermal chimney cools the zone air.
-
-#### Zone Thermal Chimney Heat Gain Energy [J]
-
-The sensible (temperature) heat gain of each zone that occurs when the thermal chimney heats the zone air.
-
-#### Zone Thermal Chimney Volume [m3]
-
-The air volumetric flow of each zone enhanced by the thermal chimney.
-
-#### Zone Thermal Chimney Mass [kg]
-
-The air mass flow of each zone enhanced by the thermal chimney.
-
-#### Zone Thermal Chimney Current Density Volumetric Flow Rate [m3/s]
-
-The total air volumetric flow rate caused by the thermal chimney evaluating density at the current zone conditions.
-
-#### Zone Thermal Chimney Standard Density Volumetric Flow Rate [m3/s]
-
-The total air volumetric flow rate caused by the thermal chimney evaluating density at standard conditions.
-
-#### Zone Thermal Chimney Mass Flow Rate [kg/s]
-
-The total air mass flow rate caused by the thermal chimney.
-
-#### Zone Thermal Chimney Outlet Temperature [C]
-
-The temperature of the air which is discharged from the thermal chimney through the outlet.
-
-### ZoneAirMassFlowConservation
-
-This global object allows users to trigger the zone air mass flow conservation calculation when desired. This object has three input fields; the first choice input field allows the user whether to adjust mixing flows to enforce the zone air mass flow conservation; and the other fields allows the user to specify how infiltration object mass flow rate is calculated for zone air mass flow balance calculation.  If adjustments for either mixing or infiltration is specified then the zone air mass balance attempts to enforce conservation. If both mixing and infiltration adjustments are off, then the zone air mass flow calculation uses the default method which does not include zone mixing objects and assumes self-balanced simple infiltration. The default method may not necessarily enforce zone air mass flow conservation unless the user has specified a balanced flow to begin with. The zone air mass flow conservation primarily accounts for the zonemixing objects air flow in the zone air flow mass balance calculation. In addition to the zonemixing object flow, the procedure accounts for zone supply, exhaust, and return flows and adjusts infiltration air flows (up or down) when required in order to balance the zone air mass flow.  Mixing and infiltration adjustments will only be made in zones which have zonemixing or infiltration objects defined in the input. For example, if a zone does not have any infiltration objects, then no infiltration adjustment will be made for that zone.
-
-First, the ZoneMixing object mass flow rate is adjusted or modified in order to balance zone air mass flow while assuming any zone infiltration objects are self-balanced. This step will always results in balanced zone air mass for receiving zones of ZoneMixing object but it may not necessarily result in a balanced air mass flow for source zones.  
-
-Second, infiltration flow rates are adjusted accoring to the options set. Infiltration flow will be increased or decreased to balance the net flow from supply, exhaust, mixing, and return air flows. If a negative infiltration rate (exfiltration) is required to balance a zone's airflow, then the infiltration rate will be set to zero. This can happen, for example, if the total supply flow exceeds the total exahust plus return flow. 
-
-This object is optional. If it is not present in the input file, the default zone air mass flow calculastion are used which do not account for zonemixing and infiltration flows.
-
-
-
-#### Field: Adjust Zone Mixing For Zone Air Mass Flow Balance
-
-This field has two choices: *Yes* or *No*.  When set to *Yes*, the zone air mass flow balance attempts to enforce conservation by adjusting zone mixing flow rates. When set to *No*, mixing flow rates are not adjusted; the mixing flows specified in ZoneMixing obects will be used.  The default is *No*.
-
-#### Field: Infiltration Balancing Method
-
-This field has three choices: *AddInfiltrationFlow*, *AdjustInfiltrationFlow*, or *None*. The default is *AddInfiltrationFlow*. With all three options, the base infiltration flow rate is the flow specified in all Infiltration:\* objects for a given zone.
-
-*AddInfiltrationFlow*: The base infiltration flow may be increased in order to balance the zone air mass flow.  This additional infiltration air mass flow is not self-balanced, i.e., it is always assumed to be incoming flow which leaves by exahust, mixing, or return. If no infiltration air is required in order to balance the zone air mass flow, then the additional infiltration air mass flow rate is set to zero. For this option, the base infiltration flow is always assumed to be self-balanced (i.e., exfiltration = infiltration) and is not included in the zone air mass flow balance.
-
-*AdjustInfiltrationFlow*: The base infiltration flow may be increased or decreased in order to balance the zone air mass flow. If no infiltration is required to balance the zone air flow, then the base infiltration flow rate is retained and assumed to be self-balanced (i.e., exfiltration = infiltration). If the required infiltration flow rate is negative (exfiltration), then the infiltration flow rate is set to zero and surplus flow in the zone is assumed to leave as exfiltration.
-
-*None*: The base infiltration flow is always assumed to be self-balanced (i.e., exfiltration = infiltration) and is not included in the zone air mass flow balance. No changes are made to the base infiltration flow rate.
-
-#### Field: Infiltration Balancing Zones
-This field allows user to choose which zones are included in infiltration balancing. There are two choices: *MixingSourceZoneOnly* or *AllZones*.
-
-*MixingSourceZonesOnly*: Infiltration balancing is active only in zones which are source zones for mixing and which have a base infiltration object defined.
-
-*AllZones*: Infiltration balance is active in any zone which has a base infiltration object defined.
- 
-
-An IDF example is shown below:
-
-```idf
-ZoneAirMassFlowConservation,
-  Yes,                       !- Adjust Zone Mixing For Zone Air Mass Flow Balance
-  AdjustInfiltrationFlow;    !- Infiltration Balancing Method
-  AllZones;                  !- Infiltration Balancing Zones
-```
-
-### ZoneAirMassFlowConservation Outputs
-
-Current ZoneAirMassFlowConservation output variables (only applicable variables will be generated):
-
-* HVAC, Average, Zone Air Mass Balance Supply Mass Flow Rate [kg/s]
-
-* HVAC, Average, Zone Air Mass Balance Exhaust Mass Flow Rate [kg/s]
-
-* HVAC, Average, Zone Air Mass Balance Return Mass Flow Rate [kg/s]
-
-* HVAC, Average, Zone Air Mass Balance Mixing Receiving Mass Flow Rate [kg/s]
-
-* HVAC, Average, Zone Air Mass Balance Mixing Source Mass Flow Rate [kg/s]
-
-* HVAC, Average, Zone Infiltration Air Mass Flow Balance Status, []
-
-* HVAC, Average, Zone Mass Balance Infiltration Air Mass Flow Rate, [kg/s]
-
-#### Zone Air Mass Balance Supply Mass Flow Rate [kg/s]
-
-This output variable represents the total supply air mass flow rate of a zone. The value is determined by summing the supply air mass flow rates contributions from all supply air inlet nodes of a zone.
-
-#### Zone Air Mass Balance Exhaust Mass Flow Rate [kg/s]
-
-This output variable represents the total exhaust air mass flow rate of a zone. The value is determined by summing the exhaust air mass flow rates contributions from all exhaust air nodes of a zone.
-
-#### Zone Air Mass Balance Return Mass Flow Rate [kg/s]
-
-This output variable represents the total return air mass flow rate of a zone. The value is determined by summing the return air mass flow rates contributions from return air nodes of a zone.
-
-#### Zone Air Mass Balance Mixing Receiving Mass Flow Rate [kg/s]
-
-This output variable represents the total zone mixing air mass flow rate of a receiving zone from one or more mixing objects. The value is determined by summing the air mass flow contributions from all zone mixing objects connected to a single receiving zone.
-
-#### Zone Air Mass Balance Mixing Source Mass Flow Rate [kg/s]
-
-This output variable represents the total zone mixing source air mass flow rate of a source zone feeding one or more mixing objects. The value is determined by summing the air mass flow contributions from all zone mixing objects connected to a single source zone.
-
-#### Zone Air Mass Balance Infiltration Status []
-
-This output variable indicates the status of the infiltration object mass flow rate use for balancing the zone mass flow at each time step. It has values of either **0** or **1**.  If the value of this report variable is **0** then the zone infiltration object mass flow rate is not used in the zone mass conservation calculation, hence the infiltration rate calculated based on the user specified inputs is manintained and the infiltration rate is assumed as self-balanced for the current timestep.  If the value is 1 then the zone infiltration object mass flow rate is included in the zone air mass flow balance calculation, hence the user specified infiltration rate is modified and it is considered as incoming flow to the zone, i.e., self-balanced assumption is not valid for this zone and current time step.
-
-#### Zone Air Mass Balance Infiltration Mass Flow Rate [kg/s]
-
-This output variable represents the zone infiltration air mass flow rate in kg/s.  This output variable is reported only for source zones and when the zone air mass flow balance is active.  Its value depends on the Infiltration Balancing Method specified.  When the infiltration method is *AddInfiltrationFlow* this output represents the additional infiltration air mass flow rate added on top of the base infiltration air flow in order to balance the zone air mass flow. In this case, the base infiltration air mass flow calculated using the user specified input is assumed self-balanced.  When the infiltration method is *AdjustInfiltrationFlow* and the value of "Zone Air Mass Balance Infiltration Status" is **1**, this output represents the infiltration air mass flow rate required to balance the zone air mass flow. This value could be negative if the zone supply exceeds all other outflows. If the value of "Zone Air Mass Balance Infiltration Status" is **0**, then this output is the self-balanced base infiltration flow rate for current timestep.
-
-Group – Design Objects
-----------------------
-
-### Input for Design Calculations and Component Autosizing
-
-#### Overview
-
-In order for EnergyPlus to successfully calculate zone design heating and cooling loads and air flow rates and for the program to use these results to automatically size the HVAC components a number of input objects must be present and certain object input fields must be entered.
-
-- The input file should contain a SimulationControl object. The 1<sup>st</sup> field *Do Zone Sizing Calculation* should be entered as *Yes*. This will cause a zone sizing simulation to be done using all the sizing periods in the input file as weather. If there are no air or water loops in the HVAC input fields 2 and 3 can be set to *No.* If there are one or more air loops (i.e., there is at least one AirLoopHVAC object in the input file) then the 2<sup>nd</sup> field *Do System Sizing Calculation* should be entered as *Yes*. If there are one or more water loops (Plant Loop objects) then the 3<sup>rd</sup> field *Do Plant Sizing Calculation* should be set to *Yes*. Finally either the 4<sup>th</sup> field (*Run Simulation for Sizing Periods*) or the 5<sup>th</sup> field (*Run Simulation for Weather File Run Periods*) should be set to *Yes* in order to autosize the components and do a real simulation using the autosized components. The component autosizing calculations are done on the first pass through the HVAC system in the real simulation.
-
-- There must be at least 2 (up to any number) SizingPeriod objects present. Normally one will be for summer conditions and one for winter. The summer day should normally have the field *Day Type* set to *SummerDesignDay*. The winter design day should normally have *Day Type* set to *WinterDesignDay*.
-
-- To apply a global sizing factor include the Sizing:Parameters object.
-
-- For each controlled zone in the input file there should be a corresponding Sizing:Zone object. Similarly for each AirLoopHVAC there should be a Sizing:System object. And for each Plant or Condenser Loop there should be a Sizing:Plant object. Note however that if a controlled zone has no corresponding Zone Sizing object the data from the first Zone Sizing object will be used. Thus if all the zone sizing information is the same only one Zone Sizing object need be entered.
-
-- Only controlled zones are included in the zone and system sizing calculations. Thus for a design air flow rate to be calculated for a zone, it must contain a thermostat *even though it might not need or have a thermostat in the full simulation*. An illustration would be a three zone building with a packaged single zone system and a thermostat in one of the zones. In order for the two slave zones to be included in the design air flow calculations they must be treated as if they have a thermostat: there must be a ZoneControl:Thermostat for each of the slave zones.
-
-- Some attention should be paid to schedules. In a weekly schedule object the 9<sup>th</sup> and 10<sup>th</sup> day schedules are for summer and winter design days respectively. This means that if a SizingPeriod object has field *Day Type* set to *SummerDesignDay*  the day schedule for summer sizing periods will be in effect. Similarly if a SizingPeriod object has field *Day Type* set to *WinterDesignDay*  the day schedule for winter sizing periods will be in effect. Some possible applications of this capability are:
-
-1)   setting internal loads (lights, equipment, occupancy) to maximum all day for cooling and to zero all day for heating;
-
-2)   setting heating and cooling thermostat set points to constant values (no set up or set back);
-
-3)   setting heating and cooling equipment to be always on.
-
-None of these applications are necessarily recommended but these and other uses of the special summer/winter design day schedules may prove useful for specific situations.
-
-- Other than zone thermostat setpoints, the sizing calculations generally know nothing about the system control inputs such as setpoints and availability schedules. The user must coordinate sizing inputs with the actual simulation control inputs.
-
-- The sizing calculations only recognize the presence of central heating and cooling coils, preheat and precool coils and reheat coils. These are assumed to deliver the various supply temperatures specified in the Sizing:System and Sizing:Zone objects. The impact of other components such as heat recovery, dehumidifiers, and pumps are not accounted for in the sizing calculations. Central supply and return fan temperature rise is taken into account in sizing the central cooling coils.
-
-#### Component Autosizing
-
-For autosizing to occur at the component level the user must enter the special value *autosize* in the numeric fields for which autosizing is available. Those fields can be found by looking at the Energy+.idd data dictionary file or under individual object details in this document. Fields that can be autosized are denoted with the comment *\\autosizable*. The components and fields that are autosizable are listed in the following table. Note that spaces may be inserted in object names to facilitate readability.
-
-
-
-Table 22. Details of Autosizable Objects/Fields
-
-
-<table class="table table-striped">
-  <tr>
-    <th>Component / Object Name</th>
-    <th>Autosizable Fields</th>
-  </tr>
-  <tr>
-    <td colspan="2">AirConditioner:VariableRefrigerantFlow</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Heating Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Resistive Defrost Heater Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Water Condenser Volume Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Evaporative Condenser Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Evaporative Condenser Pump Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirLoopHVAC</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirLoopHVAC:Unitary:Furnace:HeatCool</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Temperature</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirLoopHVAC:Unitary:Furnace:HeatOnly</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Temperature</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirLoopHVAC:UnitaryHeatCool</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Temperature</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling System Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating System Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load System Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirLoopHVAC:UnitaryHeatOnly</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Temperature</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirLoopHVAC:UnitaryHeatPump:AirToAir</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Temperature from Supplemental Heater</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Temperature from Supplemental Heater</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Speed 1 Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Speed 2 Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Speed 3 Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Speed 4 Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Speed 1 Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Speed 2 Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Speed 3 Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Speed 4 Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirLoopHVAC:UnitaryHeatPump:WaterToAir</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Temperature from Supplemental Heater</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirLoopHVAC:UnitarySystem</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Temperature</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:DualDuct:ConstantVolume</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:DualDuct:VAV</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Damper Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:DualDuct:VAV:OutdoorAir</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Terminal Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:ConstantVolume:CooledBeam</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Volumetric Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Total Chilled Water Volumetric Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Number of Beams</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Beam Length</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Total Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Hot Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Cold Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:ConstantVolume:Reheat</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Hot Water or Steam Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:ParallelPIU:Reheat</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Primary Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Secondary Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Primary Air Flow Fraction</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Fan On Flow Fraction</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Hot Water or Steam Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:SeriesPIU:Reheat</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Primary Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Primary Air Flow Fraction</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Hot Water or Steam Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:Uncontrolled</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Hot Water or Steam Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:VAV:NoReheat</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:VAV:Reheat</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Hot Water or Steam Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Cooling Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Heating Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Hot Water or Steam Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Boiler:HotWater</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Boiler:Steam</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Branch</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Chiller:Absorption</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Pumping Power</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Condenser Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Generator Fluid Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Chiller:Absorption:Indirect</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Pumping Power</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Condenser Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Generator Fluid Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Chiller:CombustionTurbine</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Condenser Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gas Turbine Engine Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Chiller:ConstantCOP</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Condenser Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Chiller:Electric</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Condenser Fluid Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Heat Recovery Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Chiller:Electric:EIR</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Reference Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Reference Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Reference Condenser Fluid Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Heat Recovery Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Chiller:Electric:ReformulatedEIR</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Reference Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Reference Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Reference Condenser Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Heat Recovery Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Chiller:EngineDriven</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Condenser Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ChillerHeater:Absorption:DirectFired</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Condenser Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Hot Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ChillerHeater:Absorption:DoubleEffect</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Condenser Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Hot Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ChillerHeaterPerformance:Electric:EIR</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Reference Cooling Mode Evaporator Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Chilled Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Condenser Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Cooling:DX:MultiSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 1 Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 1 Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 1 Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 1 Evaporative Condenser Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 1 Rated Evaporative Condenser Pump Power Consumption</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 2 Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 2 Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 2 Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 2 Evaporative Condenser Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 2 Rated Evaporative Condenser Pump Power Consumption</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 3 Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 3 Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 3 Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 3 Evaporative Condenser Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 3 Rated Evaporative Condenser Pump Power Consumption</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 4 Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 4 Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 4 Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 4 Evaporative Condenser Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 4 Rated Evaporative Condenser Pump Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Cooling:DX:SingleSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Evaporative Condenser Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Evaporative Condenser Pump Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Cooling:DX:SingleSpeed:ThermalStorage</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Evaporator Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Only Mode Rated Total Evaporator Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Evaporative Condenser Pump Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Cooling:DX:TwoSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Speed Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Speed Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Speed Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Low Speed Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Low Speed Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Low Speed Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Speed Evaporative Condenser Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Speed Evaporative Condenser Pump Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Low Speed Evaporative Condenser Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Low Speed Evaporative Condenser Pump Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Cooling:DX:VariableRefrigerantFlow</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Cooling:DX:VariableSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Total Cooling Capacity At Selected Nominal Speed Level</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate At Selected Nominal Speed Level</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Evaporative Condenser Pump Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Cooling:Water</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Inlet Water Temperature</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Inlet Air Temperature</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Outlet Air Temperature</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Inlet Air Humidity Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Outlet Air Humidity Ratio</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Cooling:Water:DetailedGeometry</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Tube Outside Surface Area</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Total Tube Inside Area</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Fin Surface Area</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Airflow Area</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Coil Depth</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Fin Diameter</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Number of Tubes per Row</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Cooling:WaterToAirHeatPump:EquationFit</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Sensible Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Total Cooling Capacity At Selected Nominal Speed Level</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate At Selected Nominal Speed Level</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Water Flow Rate At Selected Nominal Speed Level</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:DX:MultiSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Resistive Defrost Heater Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 1 Gross Rated Heating Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 1 Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 2 Gross Rated Heating Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 2 Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 3 Gross Rated Heating Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 3 Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 4 Gross Rated Heating Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Speed 4 Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:DX:SingleSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Heating Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Resistive Defrost Heater Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:DX:VariableRefrigerantFlow</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Heating Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:DX:VariableSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Heating Capacity At Selected Nominal Speed Level</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate At Selected Nominal Speed Level</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Resistive Defrost Heater Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:Electric</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:Electric:MultiStage</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Stage 1 Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Stage 2 Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Stage 3 Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Stage 4 Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:Gas</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:Gas:MultiStage</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Stage 1 Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Stage 2 Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Stage 3 Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Stage 4 Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:Steam</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Steam Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:Water</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>U-Factor Times Area Value</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:WaterToAirHeatPump:EquationFit</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Heating Capacity At Selected Nominal Speed Level</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate At Selected Nominal Speed Level</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Water Flow Rate At Selected Nominal Speed Level</td>
-  </tr>
-  <tr>
-    <td colspan="2">CoilPerformance:DX:Cooling</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Evaporative Condenser Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Evaporative Condenser Pump Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">CondenserLoop</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Loop Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Controller:OutdoorAir</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Controller:WaterCoil</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Controller Convergence Tolerance</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Actuated Flow</td>
-  </tr>
-  <tr>
-    <td colspan="2">CoolingTower:SingleSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Fan Power</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design U-Factor Times Area Value</td>
-  </tr>
-  <tr>
-    <td colspan="2">CoolingTower:TwoSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Fan Speed Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Fan Speed Fan Power</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Fan Speed U-Factor Times Area Value</td>
-  </tr>
-  <tr>
-    <td colspan="2">CoolingTower:VariableSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Fan Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">CoolingTower:VariableSpeed:Merkel</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Air Flow Rate U-Factor Times Area Value</td>
-  </tr>
-  <tr>
-    <td colspan="2">EvaporativeCooler:Indirect:ResearchSpecial</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Secondary Fan Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">EvaporativeFluidCooler:SingleSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Air Flow Rate Fan Power</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Air Flow Rate U-factor Times Area Value</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">EvaporativeFluidCooler:TwoSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Fan Speed Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Fan Speed Fan Power</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Fan Speed U-factor Times Area Value</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Fan:ComponentModel</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Motor Fan Pulley Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Belt Maximum Torque</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Motor Output Power</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum VFD Output Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">Fan:ConstantVolume</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Fan:OnOff</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">FanPerformance:NightVentilation</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Fan:VariableVolume</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">FluidCooler:SingleSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Air Flow Rate U-factor Times Area Value</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Air Flow Rate Fan Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">FluidCooler:TwoSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Fan Speed U-factor Times Area Value</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Fan Speed Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Fan Speed Fan Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">HeaderedPumps:ConstantSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Total Rated Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">HeaderedPumps:VariableSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Total Rated Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">HeatExchanger:AirToAir:SensibleAndLatent</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">HeatExchanger:FluidToFluid</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Loop Demand Side Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Loop Supply Side Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heat Exchanger U-Factor Times Area Value</td>
-  </tr>
-  <tr>
-    <td colspan="2">Humidifier:Steam:Electric</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Plant:Boiler</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Plant:Chiller</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Plant:Tower</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Speed Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>High Speed Fan Power</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Low Speed Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Low Speed Fan Power</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Free Convection Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:System:ConstantVolume</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Fan Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Coil Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Humidifier Rated Electric Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:System:DedicatedOutdoorAir</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Fan Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>DX Cooling Coil Gross Rated Total Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>DX Cooling Coil Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Humidifier Rated Electric Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:System:DualDuct</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Main Supply Fan Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cold Duct Supply Fan Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Hot Duct Supply Fan Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Coil Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Humidifier Rated Electric Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:System:PackagedVAV</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Fan Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Fan Minimum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Total Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Coil Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Humidifier Rated Electric Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:System:Unitary</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Fan Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Total Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Coil Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Humidifier Rated Electric Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:System:UnitaryHeatPump:AirToAir</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Total Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heat Pump Heating Coil Gross Rated Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supplemental Heating Coil Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Humidifier Rated Electric Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:System:UnitarySystem</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>DX Cooling Coil Gross Rated Total Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>DX Cooling Coil Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Coil Gross Rated Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supplemental Heating or Reheat Coil Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Humidifier Rated Electric Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:System:VAV</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Fan Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Fan Minimum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Humidifier Rated Electric Power</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:System:VRF</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Gross Rated Heating Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Resistive Defrost Heater Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Water Condenser Volume Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Evaporative Condenser Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Evaporative Condenser Pump Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:BaseboardHeat</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:ConstantVolume</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:DualDuct</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:FanCoil</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:IdealLoadsAirSystem</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Heating Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Sensible Heating Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Cooling Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:PTAC</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Total Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Coil Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:PTHP</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Total Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heat Pump Heating Coil Gross Rated Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supplemental Heating Coil Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:Unitary</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:VAV</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:VAV:FanPowered</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Primary Supply Air Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Primary Supply Air Minimum Flow Fraction</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Secondary Supply Air Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Parallel Fan On Flow Fraction</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:VAV:HeatAndCool</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Maximum Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:VRF</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Total Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heat Pump Heating Coil Gross Rated Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">HVACTemplate:Zone:WaterToAirHeatPump</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Total Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Coil Gross Rated Sensible Heat Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heat Pump Heating Coil Gross Rated Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supplemental Heating Coil Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Baseboard Heating Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">PlantComponent:TemperatureSource</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Volume Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">PlantEquipmentOperation:ComponentSetpoint</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Component 1 Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Component 2 Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Component 3 Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Component 4 Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Component 5 Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Component 6 Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Component 7 Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Component 8 Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Component 9 Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Component 10 Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">PlantLoop</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Loop Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">Pump:ConstantSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">Pump:VariableSpeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">Pump:VariableSpeed:Condensate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Power Consumption</td>
-  </tr>
-  <tr>
-    <td colspan="2">Sizing:System</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">SolarCollector:FlatPlate:PhotovoltaicThermal</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ThermalStorage:ChilledWater:Mixed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Use Side Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Source Side Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ThermalStorage:ChilledWater:Stratified</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Use Side Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Source Side Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">UnitarySystemPerformance:HeatPump:Multispeed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Speed 1 Supply Air Flow Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Speed 1 Supply Air Flow Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Speed 2 Supply Air Flow Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Speed 2 Supply Air Flow Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Speed 3 Supply Air Flow Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Speed 3 Supply Air Flow Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Speed 4 Supply Air Flow Ratio</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Speed 4 Supply Air Flow Ratio</td>
-  </tr>
-  <tr>
-    <td colspan="2">WaterHeater:Mixed</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Tank Volume</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heater Maximum Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Use Side Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Source Side Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">WaterHeater:Stratified</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Tank Volume</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Tank Height</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heater 1 Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Use Side Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Source Side Design Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:Baseboard:Convective:Electric</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:Baseboard:Convective:Water</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>U-Factor Times Area Value</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:Baseboard:RadiantConvective:Electric</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Nominal Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:Baseboard:RadiantConvective:Steam</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Steam Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:Baseboard:RadiantConvective:Water</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Rated Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:EnergyRecoveryVentilator</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Exhaust Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:EvaporativeCoolerUnit</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Design Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:FourPipeFanCoil</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Cold Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Hot Water Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:HighTemperatureRadiant</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Power Input</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:IdealLoadsAirSystem</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Heating Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Sensible Heating Capacity</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Cooling Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Total Cooling Capacity</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:LowTemperatureRadiant:Electric</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Electrical Power to Panel</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:LowTemperatureRadiant:VariableFlow</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Hydronic Tubing Length</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Hot Water Flow</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Cold Water Flow</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:OutdoorAirUnit</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Exhaust Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:PackagedTerminalAirConditioner</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:PackagedTerminalHeatPump</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Temperature from Supplemental Heater</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:TerminalUnit:VariableRefrigerantFlow</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:UnitHeater</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Hot Water or Steam Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:UnitVentilator</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:VentilatedSlab</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Minimum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:WaterToAirHeatPump</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Cooling Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Heating Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>No Load Outdoor Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Temperature from Supplemental Heater</td>
-  </tr>
-  <tr>
-    <td colspan="2">ZoneHVAC:WindowAirConditioner</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Supply Air Flow Rate</td>
-  </tr>
-  <tr>
-    <td></td>
-    <td>Maximum Outdoor Air Flow Rate</td>
-  </tr>
-</table>
-
-
-There are 3 places in the input where the user can impose sizing factors.
-
-1.    In Sizing Parameters (object: Sizing:Parameters), the user can specify an over-all sizing factor. This factor is applied to all the zone design loads and air flow rates resulting from the zone sizing calculations.
-
-2.    In Zone Sizing (object: Sizing:Zone), the user can specify a sizing factor for a specific zone. The factor is applied to the calculated zone design loads and air flow rates for the zone named in the Sizing:Zone object. This sizing factor overrides the global sizing factor. That is, a zone sizing factor, if specified, replaces the global sizing factor for the named zone.
-
-3.    For some plant components (basically all central chillers, boilers and cooling towers) the user can specify a sizing factor that modifies the autosized component capacity and flow rates. These factors are applied after the application of global or zone sizing factors. They are primarily used to split the design load between multiple components. These sizing factors can change the autosizing of the associated loops and pumps. The following rules are followed the effect of plant component sizing factors on loops and pumps.
-
-a.    For supply side branches, the sizing factors of all components in series on the branch are summed and the result becomes the branch sizing factor. If there is a branch pump its autosized design flow rate is multiplied by the branch sizing factor.
-
-b.   For each loop, if the average of the branch sizing factors is less than 1, the loop sizing factor is set equal to the sum of the branch sizing factors. If the average is greater than 1, the loop sizing factor is set equal to the maximum of the branch sizing factors. The loop sizing factor is applied to the loop design flow rate (if autosized) and to the loop pump flow rate (if autosized).
-
-#### Mixing User-Specified and Autosized Inputs
-
-Mixed user-specified and autosized inputs can be successfully used if the following points and suggestions are followed.
-
-1.    Each component is autosized independently. Thus user input for a flow rate in one component will have no effect on other components’ autosized flow rates. For instance, specifying the chilled water loop pump’s rated flow rate will have no effect on the autosizing of the chiller’s design evaporator flow rate or on the plant loop’s autosized maximum loop flow rate.
-
-2.    Within a component it is best to autosize all inputs are enter specified values for all inputs. For example, in a chiller, if only the nominal capaciity is user-specified, the autosized chilled water flow rate may not be consistent with the specified capacity.
-
-3.    Sizing information flows only from the sizing objects to the components. The sizing calculations have no knowledge of user-specified values in a component. The only exception to this rule is that plant loop sizing will collect all component design water flow rates whether autosized or user-specified.
-
-4.    If the user wants to specify a zone or system air flow rate it should be done using the Sizing:Zone and Sizing:System  objects rather than done in the individual components.
-
-5.    The plant loop flow rates are sized from the total design demand of the components connected to each loop. The components demanding water need not be autosized for the plant loop autosizing to work successfully. So the user could specify all the air side components and autosize all the plant loops and plant components. Or specify the chilled water loop flow rate, chilled water pump inputs and chiller inputs and let the condenser loop and tower autosize.
-
-#### Component Sizing Output
-
-The results of the component autosizing calculations are reported on the *eplusout.eio* file. For each component field that has been autosized the object type, object name, field description with unit, and value are printed out as comma separated data on a line beginning with *Component Sizing*. Examples of this are shown in the Output Details and Examples document.
-
-The complete list of objects that have autosized fields is shown in the following table. Note that spaces may be inserted in object names to facilitate readability.
-
-Table 23. Complete list of Objects with autosized Fields
-
-<table class="table table-striped">
-  <tr>
-    <th>Object Name</th>
-    <th>Object Name</th>
-  </tr>
-  <tr>
-    <td>AirConditioner:VariableRefrigerantFlow</td>
-    <td>AirLoopHVAC</td>
-  </tr>
-  <tr>
-    <td>AirLoopHVAC:Unitary:Furnace:HeatCool</td>
-    <td>AirLoopHVAC:Unitary:Furnace:HeatOnly</td>
-  </tr>
-  <tr>
-    <td>AirLoopHVAC:UnitaryHeatCool</td>
-    <td>AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass</td>
-  </tr>
-  <tr>
-    <td>AirLoopHVAC:UnitaryHeatOnly</td>
-    <td>AirLoopHVAC:UnitaryHeatPump:AirToAir</td>
-  </tr>
-  <tr>
-    <td>AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed</td>
-    <td>AirLoopHVAC:UnitaryHeatPump:WaterToAir</td>
-  </tr>
-  <tr>
-    <td>AirLoopHVAC:UnitarySystem</td>
-    <td>AirTerminal:DualDuct:ConstantVolume</td>
-  </tr>
-  <tr>
-    <td>AirTerminal:DualDuct:VAV</td>
-    <td>AirTerminal:DualDuct:VAV:OutdoorAir</td>
-  </tr>
-  <tr>
-    <td>AirTerminal:SingleDuct:ConstantVolume:CooledBeam</td>
-    <td>AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction</td>
-  </tr>
-  <tr>
-    <td>AirTerminal:SingleDuct:ConstantVolume:Reheat</td>
-    <td>AirTerminal:SingleDuct:ParallelPIU:Reheat</td>
-  </tr>
-  <tr>
-    <td>AirTerminal:SingleDuct:SeriesPIU:Reheat</td>
-    <td>AirTerminal:SingleDuct:Uncontrolled</td>
-  </tr>
-  <tr>
-    <td>AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat</td>
-    <td>AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat</td>
-  </tr>
-  <tr>
-    <td>AirTerminal:SingleDuct:VAV:NoReheat</td>
-    <td>AirTerminal:SingleDuct:VAV:Reheat</td>
-  </tr>
-  <tr>
-    <td>AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan</td>
-    <td>Boiler:HotWater</td>
-  </tr>
-  <tr>
-    <td>Boiler:Steam</td>
-    <td>Branch</td>
-  </tr>
-  <tr>
-    <td>Chiller:Absorption</td>
-    <td>Chiller:Absorption:Indirect</td>
-  </tr>
-  <tr>
-    <td>Chiller:CombustionTurbine</td>
-    <td>Chiller:ConstantCOP</td>
-  </tr>
-  <tr>
-    <td>Chiller:Electric</td>
-    <td>Chiller:Electric:EIR</td>
-  </tr>
-  <tr>
-    <td>Chiller:Electric:ReformulatedEIR</td>
-    <td>Chiller:EngineDriven</td>
-  </tr>
-  <tr>
-    <td>ChillerHeater:Absorption:DirectFired</td>
-    <td>ChillerHeater:Absorption:DoubleEffect</td>
-  </tr>
-  <tr>
-    <td>ChillerHeaterPerformance:Electric:EIR</td>
-    <td>Coil:Cooling:DX:MultiSpeed</td>
-  </tr>
-  <tr>
-    <td>Coil:Cooling:DX:SingleSpeed</td>
-    <td>Coil:Cooling:DX:SingleSpeed:ThermalStorage</td>
-  </tr>
-  <tr>
-    <td>Coil:Cooling:DX:TwoSpeed</td>
-    <td>Coil:Cooling:DX:VariableRefrigerantFlow</td>
-  </tr>
-  <tr>
-    <td>Coil:Cooling:DX:VariableSpeed</td>
-    <td>Coil:Cooling:Water</td>
-  </tr>
-  <tr>
-    <td>Coil:Cooling:Water:DetailedGeometry</td>
-    <td>Coil:Cooling:WaterToAirHeatPump:EquationFit</td>
-  </tr>
-  <tr>
-    <td>Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit</td>
-    <td>Coil:Heating:DX:MultiSpeed</td>
-  </tr>
-  <tr>
-    <td>Coil:Heating:DX:SingleSpeed</td>
-    <td>Coil:Heating:DX:VariableRefrigerantFlow</td>
-  </tr>
-  <tr>
-    <td>Coil:Heating:DX:VariableSpeed</td>
-    <td>Coil:Heating:Electric</td>
-  </tr>
-  <tr>
-    <td>Coil:Heating:Electric:MultiStage</td>
-    <td>Coil:Heating:Gas</td>
-  </tr>
-  <tr>
-    <td>Coil:Heating:Gas:MultiStage</td>
-    <td>Coil:Heating:Steam</td>
-  </tr>
-  <tr>
-    <td>Coil:Heating:Water</td>
-    <td>Coil:Heating:WaterToAirHeatPump:EquationFit</td>
-  </tr>
-  <tr>
-    <td>Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit</td>
-    <td>CoilPerformance:DX:Cooling</td>
-  </tr>
-  <tr>
-    <td>CondenserLoop</td>
-    <td>Controller:OutdoorAir</td>
-  </tr>
-  <tr>
-    <td>Controller:WaterCoil</td>
-    <td>CoolingTower:SingleSpeed</td>
-  </tr>
-  <tr>
-    <td>CoolingTower:TwoSpeed</td>
-    <td>CoolingTower:VariableSpeed</td>
-  </tr>
-  <tr>
-    <td>CoolingTower:VariableSpeed:Merkel</td>
-    <td>EvaporativeCooler:Indirect:ResearchSpecial</td>
-  </tr>
-  <tr>
-    <td>EvaporativeFluidCooler:SingleSpeed</td>
-    <td>EvaporativeFluidCooler:TwoSpeed</td>
-  </tr>
-  <tr>
-    <td>Fan:ComponentModel</td>
-    <td>Fan:ConstantVolume</td>
-  </tr>
-  <tr>
-    <td>Fan:OnOff</td>
-    <td>FanPerformance:NightVentilation</td>
-  </tr>
-  <tr>
-    <td>Fan:VariableVolume</td>
-    <td>FluidCooler:SingleSpeed</td>
-  </tr>
-  <tr>
-    <td>FluidCooler:TwoSpeed</td>
-    <td>HeaderedPumps:ConstantSpeed</td>
-  </tr>
-  <tr>
-    <td>HeaderedPumps:VariableSpeed</td>
-    <td>HeatExchanger:AirToAir:SensibleAndLatent</td>
-  </tr>
-  <tr>
-    <td>HeatExchanger:FluidToFluid</td>
-    <td>Humidifier:Steam:Electric</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:Plant:Boiler</td>
-    <td>HVACTemplate:Plant:Chiller</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:Plant:Tower</td>
-    <td>HVACTemplate:System:ConstantVolume</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:System:DedicatedOutdoorAir</td>
-    <td>HVACTemplate:System:DualDuct</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:System:PackagedVAV</td>
-    <td>HVACTemplate:System:Unitary</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:System:UnitaryHeatPump:AirToAir</td>
-    <td>HVACTemplate:System:UnitarySystem</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:System:VAV</td>
-    <td>HVACTemplate:System:VRF</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:Zone:BaseboardHeat</td>
-    <td>HVACTemplate:Zone:ConstantVolume</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:Zone:DualDuct</td>
-    <td>HVACTemplate:Zone:FanCoil</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:Zone:IdealLoadsAirSystem</td>
-    <td>HVACTemplate:Zone:PTAC</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:Zone:PTHP</td>
-    <td>HVACTemplate:Zone:Unitary</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:Zone:VAV</td>
-    <td>HVACTemplate:Zone:VAV:FanPowered</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:Zone:VAV:HeatAndCool</td>
-    <td>HVACTemplate:Zone:VRF</td>
-  </tr>
-  <tr>
-    <td>HVACTemplate:Zone:WaterToAirHeatPump</td>
-    <td>PlantComponent:TemperatureSource</td>
-  </tr>
-  <tr>
-    <td>PlantEquipmentOperation:ComponentSetpoint</td>
-    <td>PlantLoop</td>
-  </tr>
-  <tr>
-    <td>Pump:ConstantSpeed</td>
-    <td>Pump:VariableSpeed</td>
-  </tr>
-  <tr>
-    <td>Pump:VariableSpeed:Condensate</td>
-    <td>Sizing:System</td>
-  </tr>
-  <tr>
-    <td>SolarCollector:FlatPlate:PhotovoltaicThermal</td>
-    <td>ThermalStorage:ChilledWater:Mixed</td>
-  </tr>
-  <tr>
-    <td>ThermalStorage:ChilledWater:Stratified</td>
-    <td>UnitarySystemPerformance:HeatPump:Multispeed</td>
-  </tr>
-  <tr>
-    <td>WaterHeater:Mixed</td>
-    <td>WaterHeater:Stratified</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:Baseboard:Convective:Electric</td>
-    <td>ZoneHVAC:Baseboard:Convective:Water</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:Baseboard:RadiantConvective:Electric</td>
-    <td>ZoneHVAC:Baseboard:RadiantConvective:Steam</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:Baseboard:RadiantConvective:Water</td>
-    <td>ZoneHVAC:EnergyRecoveryVentilator</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:EvaporativeCoolerUnit</td>
-    <td>ZoneHVAC:FourPipeFanCoil</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:HighTemperatureRadiant</td>
-    <td>ZoneHVAC:IdealLoadsAirSystem</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:LowTemperatureRadiant:Electric</td>
-    <td>ZoneHVAC:LowTemperatureRadiant:VariableFlow</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:OutdoorAirUnit</td>
-    <td>ZoneHVAC:PackagedTerminalAirConditioner</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:PackagedTerminalHeatPump</td>
-    <td>ZoneHVAC:TerminalUnit:VariableRefrigerantFlow</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:UnitHeater</td>
-    <td>ZoneHVAC:UnitVentilator</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:VentilatedSlab</td>
-    <td>ZoneHVAC:WaterToAirHeatPump</td>
-  </tr>
-  <tr>
-    <td>ZoneHVAC:WindowAirConditioner</td>
-    <td></td>
-  </tr>
-</table>
-
-
-
-#### User or External Zone Design Flow Rate Inputs
-
-In EnergyPlus the autosizing calculations start with a calculation of the zone design air flow rates using zone by zone design day simulations. The resulting zone design air flow rates and daily air flow sequences are used in the subsequent HVAC and central plant air and fluid flow design calculations and in the component autosizing calculations. The user can override or change the calculated zone design air flow rates in several ways.
-
-1)    The user can enter a value for *Sizing Factor* in the *Sizing:Parameters* object (see description below).
-
-2)    The user can specify a zone level *Zone Sizing Factor* in each *Sizing:Zone* object.
-
-3)    For each zone the user can input a *Cooling Design Air Flow Rate* and/or a *Heating Design Air Flow Rate* (and specify *Cooling Design Air Flow Method = Flow/Zone* and *Heating Design Air Flow Method = Flow/Zone*). These user inputs override the calculated values. The program divides the user input cooling or heating design air flow rate by the calculated values and uses the result as a zone sizing factor to multiply all the elements in the design heating and cooling air flow and load sequences. From this point the design calculations proceed as usual.
-
-#### User or External System Design Flow Rate Inputs
-
-Using the results of the zone design air flow rate calculation (including any user input or altered flow rates) EnergyPlus proceeds to calculate central air system flow rates and cooling and heating loads. The results of this calculation can be overridden in the following way.
-
-For each system (AirLoopHVAC), in the corresponding Sizing:System object, specify *Cooling Design Air Flow Method* to be *Flow/System* and input a value for *Cooling Design Air Flow Rate*. Similarly for heating specify *Heating Design Air Flow Method* to be *Flow/System* and input a value for *Heating Design Air Flow Rate*.
-
-### DesignSpecification:OutdoorAir
-
-This object allows for the outdoor air requirements to be defined in a common location for use by other objects. This object may be referenced by name from other objects (e.g., VAV terminal units) as required to identify an outdoor air quantity for use by that object. Note that a zone name Is not included as an input to this zone outdoor air definition and the number of people in a zone, zone floor area, and zone volume can only be determined after this object has been referenced by another. A single zone outdoor air definition may be referenced by multiple objects to specify that the same outdoor air requirements are used by those objects *or* multiple zone outdoor air objects may be defined and referenced by other objects as needed. If multiple zone outdoor air definitions are used, each outdoor air definition must have a unique name.
-
-#### Field: Name
-
-Unique identifying name. Any reference to this name by other objects will denote that the following outdoor air requirements will be used.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Person*, *Flow/Area*, *Flow/Zone, AirChanges/Hour*, *Sum*, or *Maximum*. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the actual zone occupancy to calculate a zone outdoor air flow rate. *Flow/Area* means that the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* and the actual zone floor area as the zone outdoor air flow rate. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow per Zone* as the zone outdoor air flow rate. *AirChanges/Hour* means that the program will use the input from the field *Air Changes per Hour* and the actual zone volume (divided by 3600 seconds per hour) as the zone outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area, Outdoor Air Flow per Zone*, and *Air Changes per Hour* (using the associated conversions to m<sup>3</sup>/s for each field) will be added to obtain the zone outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area, Outdoor Air Flow per Zone,* and *Air Changes per Hour* (using the associated conversions to m<sup>3</sup>/s for each field) will be used as the zone outdoor air flow rate. The default is *Flow/Person*.
-
-#### Field: Outdoor Air Flow per Person
-
-The design outdoor air volume flow rate per person for this zone in cubic meters per second per person. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values *are not* applied during sizing calculations and *are* applied during the remainder of the simulation. This input is used if *Outdoor Air Method* is one of *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow per Zone Floor Area
-
-The design outdoor air volume flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*. The default value for this field is 0.
-
-#### Field: Outdoor Air Flow per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*. The default value for this field is 0.
-
-#### Field: Outdoor Air Flow Changes per Hour
-
-The design outdoor air volume flow rate in air changes per hour. This factor is used along with the Zone Volume and converted to cubic meters per second. This input field is used if *Outdoor Air Method* is *AirChanges/Hour, Sum* or *Maximum*. The default value for this field is 0.
-
-#### Field: Outdoor Air Flow Rate Fraction Schedule Name
-
-This field is the name of schedule that defines how outdoor air requirements change over time.  The field is optional.  If used, then the schedule values are multiplied by the outdoor air flow rate defined by the previous fields.  The schedule values must be between 0 and 1, inclusive.
-
-An IDF example:
-
-```idf
-DesignSpecification:OutdoorAir
-    ZoneOAData,            !- Name
-    Sum,                   !- Outdoor Air Method
-    0.00944,               !- Outdoor Air Flow per Person {m3/s}
-    0.00305,               !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    ,                      !- Outdoor Air Flow per Zone {m3/s}
-    ,                      !- Outdoor Air Flow Air Changes per Hour
-    OARequirements Sched;  !- Outdoor Air Flow Rate Fraction Schedule Name
-
-
-Schedule:Compact,
-    OARequirements Sched,    !- Name
-    Any Number,              !- Schedule Type Limits Name
-    Through: 12/31,          !- Field 1
-    For: Weekdays SummerDesignDay WinterDesignDay,  !- Field 2
-    Until: 24:00, 1.0,       !- Field 4
-    For: AllOtherDays,       !- Field 5
-    Until: 24:00, 0.5;       !- Field 7
-```
-
-
-### DesignSpecification:ZoneAirDistribution
-
-This object is used to describe the air distribution effectiveness and fraction of secondary recirculation air (return air not directly mixed with outdoor air) of a zone. It is referenced by the Sizing:Zone and Controller:MechanicalVentilation objects.
-
-#### Field: Name
-
-The unique user assigned name for an instance of this object. Any other object referencing this object will use this name.
-
-#### Field: Zone Air Distribution Effectiveness in Cooling Mode
-
-The positive numeric input for this field is the zone air distribution effectiveness when the zone is in cooling mode. Default value of this field is 1.0. ASHRAE Standard 62.1-2010 provides typical values.
-
-#### Field: Zone Air Distribution Effectiveness in Heating Mode
-
-The positive numeric input for this field is the zone air distribution effectiveness when the zone is in heating mode. Default value of this field is 1.0. ASHRAE Standard 62.1-2010 provides typical values as follows:
-
-![](media/image133.svg)
-
-Figure 71. Zone Air Distribution Effectiveness (Source: ASHRAE Standard 62.1-2010)
-
-#### Field: Zone Air Distribution Effectiveness Schedule Name
-
-This optional field input points to a schedule with values of zone air distribution effectiveness. It provides a more flexible way of specifying zone air distribution effectiveness if it changes with time and/or system operating status and controls. If the schedule is specified, the zone air distribution effectiveness in cooling mode and heating mode will be ignored.
-
-#### Field: Zone Secondary Recirculation Fraction
-
-The non-negative numeric input for this field is the fraction of a zone’s recirculation air that does not directly mix with the outdoor air. The zone secondary recirculation fraction Er is determined by the designer based on system configuration. For plenum return systems with secondary recirculation (e.g., fan-powered VAV with plenum return) Er is usually less than 1.0, although values may range from 0.1 to 1.2 depending upon the location of the ventilation zone relative to other zones and the air handler. For ducted return systems with secondary recirculation (e.g., fan-powered VAV with ducted return), Er is typically 0.0, while for those with system-level recirculation (e.g, dual-fan dual-duct systems with ducted return) Er is typically 1.0. For other system types, Er is typically 0.75. Minimum is 0.0, and default is 0.0 for single-path systems (also to maintain backward compatibility). For parallel fan-powered VAV systems, the secondary ventilation path only functions (Er &gt; 0.0) when the fans in the VAV boxes operate, which is during heating. The local ventilation path and the benefits of secondary recirculation disappear during cooling, when the local parallel fans are off (Er = 0.0).
-
-An example of this in an IDF context is shown:
-
-```idf
-DesignSpecification:ZoneAirDistribution,
-    CM DSZAD ZN_1_FLR_1_SEC_1,  !- Name
-    1,                       !- Zone Air Distribution Effectiveness in Cooling Mode {dimensionless}
-    1,                       !- Zone Air Distribution Effectiveness in Heating Mode {dimensionless}
-    ;                        !- Zone Air Distribution Effectiveness Schedule Name
-```
-
-### Sizing:Parameters
-
-This object allows the user to specify global heating and cooling sizing ratios. These ratios will be applied at the zone level to all of the zone heating and cooling loads and air flow rates. These new loads and air flow rates are then used to calculate the system level flow rates and capacities and are used in all component sizing calculations.
-
-The user can also specify the width (in load timesteps) of a moving average window which can be used to smooth the calculated zone design flow sequences. The use of this parameter is described below.
-
-#### Field: Heating Sizing Factor
-
-The global heating sizing ratio applied to all of the zone design heating loads and air flow rates.
-
-#### Field: Cooling Sizing Factor
-
-The global cooling sizing ratio applied to all of the zone design cooling loads and air flow rates
-
-#### Field: Timesteps in Averaging Window
-
-The number of load timesteps in the zone design flow sequence averaging window. The default is 1, in which case the calculated zone design flow rates are averaged over the load timestep.
-
-The zone design air flow rate calculation is performed assuming a potentially infinite supply of heating or cooling air at a fixed temperature. Thus the calculated design air flow rate will always be able to meet any load or change in load no matter how large or abrupt. In reality air flow rates are limited by duct sizes and fan capacities. The idealized zone design flow calculation may result in unrealistically large flow rates, especially if the user is performing the sizing calculations using thermostat schedules with night setup or setback. The calculated zone design flow rates are always averaged over the load timestep. The user may want to perform a broader average to mitigate the effect of thermostat setup and setback and prevent the warm up or cool down flow rates from dominating the design flow rate calculation.. Specifying the width of the averaging window allows the user to do this.
-
-For example, if the load calculation timestep is 15 minutes and the user specifies the *Timesteps in Averaging Window* to be 4, the zone design air flows will be averaged over a time period of 1 hour. Specifying 8 would result in averaging over a 2 hour period.
-
-### Sizing Parameters Outputs
-
-The sizing factors and the averaging window size are reported out on the *eplusout.eio* file. An example is:
-
-```
-! <Load Timesteps in Zone Design Calculation Averaging Window>, Value
- Timesteps in Averaging Window,    1
-! <Heating Sizing Factor Information>, Sizing Factor ID, Value
- Heating Sizing Factor, Global,   1.3000
- Heating Sizing Factor, Zone SPACE1-1,   1.3000
- Heating Sizing Factor, Zone SPACE2-1,   1.3000
- Heating Sizing Factor, Zone SPACE3-1,   1.3000
- Heating Sizing Factor, Zone SPACE4-1,   1.3000
- Heating Sizing Factor, Zone SPACE5-1,   1.3000
-! <Cooling Sizing Factor Information>, Sizing Factor ID, Value
- Cooling Sizing Factor, Global,   1.3000
- Cooling Sizing Factor, Zone SPACE1-1,   1.3000
- Cooling Sizing Factor, Zone SPACE2-1,   1.3000
- Cooling Sizing Factor, Zone SPACE3-1,   1.3000
- Cooling Sizing Factor, Zone SPACE4-1,   1.3000
- Cooling Sizing Factor, Zone SPACE5-1,   1.3000
-```
-
-### OutputControl:Sizing:Style
-
-As described early in the document (see: EnergyPlus Output Processing), the user may select the “style� for the sizing result files (epluszsz.&lt;ext&gt;, eplusssz.&lt;ext&gt;). This object applies to all sizing output files.
-
-```idd
-OutputControl:Sizing:Style,
-       \memo default style for the Sizing output files is comma -- this works well for
-       \memo importing into spreadsheet programs such as Excel(tm) but not so well for word
-       \memo processing progams -- there tab may be a better choice.  fixed puts spaces between
-       \memo the "columns"
-       \unique-object
-   A1; \field Column Separator
-       \required-field
-       \type choice
-       \key Comma
-       \key Tab
-       \key Fixed
-```
-
-
-#### Field: Column Separator
-
-For this field, the desired separator for columns is entered. “Comma� creates comma separated fields/columns in the outputs (eplus&lt;sizing type&gt;.csv files are created). “Tab� creates tab separated fields/columns in the outputs (eplus&lt;sizing type&gt;.tab files are created). “Fixed� creates space separated fields/columns in the outputs (eplus&lt;sizing type&gt;.txt files are created) but these are not necessarily lined up for easy printing.
-
-Note that both tab and comma separated files easily import into Excel™ or other spreadsheet programs. The tab delimited files can also be viewed by text editors, word processing programs and easily converted to “tables� within those programs.
-
-### Sizing:Zone
-
-The Sizing:Zone object provides the data needed to perform a zone design air flow calculation for a single zone. This calculation assumes a variable amount of supply air at a fixed temperature and humidity. The information needed consists of the zone inlet supply air conditions: temperature and humidity ratio for heating and cooling. The calculation is done for every design day included in the input. The maximum cooling load and air flow and the maximum heating load and air flow are then saved for the system level design calculations and for the component automatic sizing calculations.
-
-The Sizing:Zone object is also the place where the user can specify the design outdoor air flow rate by referencing the name of a design specification outdoor air object. This can be specified in a number of ways (ref. DesignSpecification:OutdoorAir).This data is saved for use in the system sizing calculation or for sizing zone components that use outdoor air.
-
-The user can also place limits on the heating and design cooling air flow rates. See * Heating Design Air Flow Method* and *Cooling Design Air Flow Method* below and the explanations of the various heating and cooling flow input fields.
-
-The user can ask the zone design calculation to take into account the effect of a Dedicated Outdoor Air System on the zone design loads and airflow rates. The design calculation will calculate the heat addition rate to the zone of an idealized SOA system and add or subtract the result from the total zone loads and flow rates. 
-
-#### Field: Zone Name
-
-The name of the Zone corresponding to this Sizing:Zone object. This is the zone for which the design air flow calculation will be made using the input data of this Sizing:Zone Object.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-The input must be either *SupplyAirTemperature* or *TemperatureDifference*. *SupplyAirTemperature* means that the user inputs from the fields of Zone Cooling Design Supply Air Temperature will be used to determine the zone cooling design air flow rates. *TemperatureDifference* means that the user inputs from the fields of Zone Cooling Design Supply Air Temperature Difference will be used to determine the zone cooling design air flow rates.
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation. Air is supplied to the zone at this temperature during the cooling design day simulation, The zone load is met by varying the zone air flow rate. The maximum zone flow rate is saved as the  zone cooling design air flow rate. This field is only used when Zone Cooling Design Supply Air Temperature Input Method = **SupplyAirTemperature**.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between cooling design supply air temperature and room air temperature in degrees Celsius for the zone cooling design air flow rate calculation. Air is supplied to the zone at this temperature during the cooling design day simulation. The zone load is met by varying the zone air flow rate. The maximum zone flow rate is saved as the zone cooling design air flow rate. This field is only used when Zone Cooling Design Supply Air Temperature Input Method = **TemperatureDifference**.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-The input must be either *SupplyAirTemperature* or *TemperatureDifference*. *SupplyAirTemperature* means that the user inputs from the fields of Zone Heating Design Supply Air Temperature will be used to determine the zone heating design air flow rates. *TemperatureDifference* means that the user inputs from the fields of Zone Heating Design Supply Air Temperature Difference will be used to determine the zone heating design air flow rates.
-
-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation. Air is supplied to the zone at this temperature during the heating design day simulation, The zone load is met by varying the zone air flow rate. The maximum zone flow rate is saved as the zone heating design air flow rate. This field is only used when Zone Heating Design Supply Air Temperature Input Method = **SupplyAirTemperature**.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and room air temperature in degrees Celsius for the zone heating design air flow rate calculation. Air is supplied to the zone at this temperature during the heating design day simulation. The zone load is met by varying the zone air flow rate. The maximum zone flow rate is saved as the zone heating design air flow rate. This field is only used when Zone Heating Design Supply Air Temperature Input Method = **TemperatureDifference**.
-
-#### Field: Zone Cooling Design Supply Air Humidity Ratio
-
-The humidity ratio in kilograms of water per kilogram of dry air of the supply air in the zone cooling design air flow rate calculation.
-
-#### Field: Zone Heating Design Supply Air Humidity Ratio
-
-The humidity ratio in kilograms of water per kilogram of dry air of the supply air in the zone heating design air flow rate calculation.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is a zone level heating sizing ratio. The zone design heating air flow rates and loads will be multiplied by the number input in this field. This input overrides the building level sizing factor input in the Sizing:Parameters object. And, of course, if this field is blank or zero, the global heating sizing factor from the Sizing:Parameters object is used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is a zone level cooling sizing ratio. The zone design cooling air flow rates and loads will be multiplied by the number input in this field. This input overrides the building level sizing factor input in the Sizing:Parameters object. And, of course, if this field is blank or zero, the global cooling sizing factor from the Sizing:Parameters object is used.
-
-#### Field: Cooling Design Air Flow Method
-
-The input must be either *Flow/Zone, DesignDay, or DesignDayWithLimit*. *Flow/Zone* means that the program will use the input of the field *Cooling Design Air Flow Rate* as the zone design cooling air flow rate. *DesignDay* means the program will calculate the zone design cooling air flow rate using the Sizing:Zone input data and a design day simulation without imposing any limits other than those set by the minimum outside air requirements. *DesignDayWithLimit* means that the maximum from *Cooling Minimum Air Flow per Zone Floor Area* and *Cooling Minimum Air Flow* will set a lower limit on the design maximum cooling air flow rate. The default method is *DesignDay*: i.e., the program uses the calculated design values subject to ventilation requirements.
-
-#### Field: Cooling Design Air Flow Rate
-
-The design zone cooling air flow rate in cubic meters per second. This input is used if *Cooling Design Air Flow Method* is specified as *Flow/Zone*. This value will be multiplied by the global or zone sizing factor and by zone multipliers.
-
-#### Field: Cooling Minimum Air Flow per Zone Floor Area
-
-The minimum zone cooling volumetric flow rate per square meter (units are m<sup>3</sup>/s-m<sup>2</sup>). This field is used when *Cooling Design Air Flow Method* is specified as *DesignDayWithLimit*. In this case it sets a lower bound on the zone design cooling air flow rate. In all cases the maximum flow derived from *Cooling Minimum Air Flow per Zone Floor Area*, *Cooling Minimum Air Flow*, and *Cooling Minimum Air Flow Fraction*  is used to set a minimum supply air flow rate for the zone for VAV systems. The default is .000762, corresponding to .15 cfm/ft<sup>2</sup>.  The applicable sizing factor is not applied to this value.
-
-#### Field: Cooling Minimum Air Flow
-
-The minimum zone cooling volumetric flow rate in m<sup>3</sup>/s. This field is used when *Cooling Design Air Flow Method* is specified as *DesignDayWithLimit*. In this case it sets a lower bound on the zone design cooling air flow rate. In all cases the maximum flow derived from *Cooling Minimum Air Flow per Zone Floor Area*, *Cooling Minimum Air Flow*, and *Cooling Minimum Air Flow Fraction*  is used to set a minimum supply air flow rate for the zone for VAV systems. The default is zero.  The applicable sizing factor is not applied to this value.
-
-#### Field: Cooling Minimum Air Flow Fraction
-
-The minimum zone design cooling volumetric flow rate expressed as a fraction of the zone design cooling volumetric flow rate. . In all cases the maximum flow derived from *Cooling Minimum Air Flow per Zone Floor Area*, *Cooling Minimum Air Flow*, and *Cooling Minimum Air Flow Fraction*  is used to set a minimum supply air flow rate for the zone for VAV systems. The default is zero. This input is currently used in sizing the fan minimum flow rate. It does not currently affect other component autosizing.
-
-#### Field: Heating Design Air Flow Method
-
-The input must be either *Flow/Zone, DesignDay, or DesignDayWithLimit*. *Flow/Zone* means that the program will use the input of the field *Heating Design Air Flow Rate* as the zone design heating air flow rate. *DesignDay* means the program will calculate the zone design heating air flow rate using the Sizing:Zone input data and a design day simulation without imposing any limits other than those set by the minimum outside air requirements. *DesignDayWithLimit* means that the maximum from *Heating Maximum Air Flow per Zone Floor Area* and *Heating Maximum Air Flow* will set a lower limit on the design maximum heating air flow rate. The default method is *DesignDay*: i.e., the program uses the calculated design values subject to ventilation requirements.
-
-#### Field: Heating Design Air Flow Rate
-
-The design zone heating air flow rate in cubic meters per second. This input is used if *Heating Design Air Flow Method* is specified as *Flow/Zone*. This value will be multiplied by the global or zone sizing factor and by zone multipliers.
-
-#### Field: Heating Maximum Air Flow per Zone Floor Area
-
-The maximum zone heating volumetric flow rate per square meter (units are m<sup>3</sup>/s-m<sup>2</sup>). This field is used when *Heating Design Air Flow Method* is specified as *DesignDayWithLimit*. In this case it sets an upper bound on the zone design heating air flow rate. For this and the next two input fields, the maximum flow derived from *Heating Maximum Air Flow per Zone Floor Area*, *Heating Maximum Air Flow*, and *Heating Maximum Air Flow Fraction*  is used to set a maximum heating supply air flow rate for the zone for VAV systems. The default is .002032, corresponding to .40 cfm/ft<sup>2</sup>. If the maximum heating design flow rate calculated using these input fields is greater than the design heating flow rate calculated during sizing, these input fields have no impact on sizing. It may be more appropriate to select only one of these three fields to calculate the maximum heating design flow rate (i.e., if one ore more of these three fields is 0, it will not be used in calculating the maximum heating design flow rate).
-
-#### Field: Heating Maximum Air Flow
-
-The maximum zone heating volumetric flow rate in m<sup>3</sup>/s. This field is used when *Heating Design Air Flow Method* is specified as *DesignDayWithLimit*. In this case it sets an upper bound on the zone design heating air flow rate. For this field and the two input fields just prior to and after this field,,the maximum flow derived from *Heating Maximum Air Flow per Zone Floor Area*, *Heating Maximum Air Flow*, and *Heating Maximum Air Flow Fraction* is used to set a maximum heating supply air flow rate for the zone for VAV systems. The default is .1415762, corresponding to 300 cfm. If the maximum heating design flow rate calculated using these input fields is greater than the design heating flow rate calculated during sizing, these input fields have no impact on sizing. It may be more appropriate to select only one of these three fields to calculate the maximum heating design flow rate (i.e., if one ore more of these three fields is 0, it will not be used in calculating the maximum heating design flow rate).
-
-#### Field: Heating Maximum Air Flow Fraction
-
-The maximum zone design heating volumetric flow rate expressed as a fraction of the zone design cooling volumetric flow rate. For this and the previous two input fields, the maximum flow derived from *Heating Maximum Air Flow per Zone Floor Area*, *Heating Maximum Air Flow*, and *Heating Maximum Air Flow Fraction*  is used to set a maximum heating supply air flow rate for the zone for VAV systems. The default is 0.3. If the maximum heating design flow rate calculated using these input fields is greater than the design heating flow rate calculated during sizing, these input fields have no impact on sizing. It may be more appropriate to select only one of these three fields to calculate the maximum heating design flow rate (i.e., if one ore more of these three fields is 0, it will not be used in calculating the maximum heating design flow rate).
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-The name of the DesignSpecification:ZoneAirDistribution object, defining the air distribution effectiveness and secondary recirculation air fraction, that applies to the zone or zone list. This object may be used for the same zone in the Controller:MechanicalVentilation object if no such DesignSpecification:ZoneAirDistribution object is specified.
-
-#### Field: Account for Dedicated Outdoor Air System
-
-This is a choice field with choices *Yes* or *No*. The default is *No*. Choosing *Yes* means that the zone sizing calculation will use the subsequent inputs to calculate the heat gain or loss (heat gains are positive, heat loss is negative) imposed on the zone by a Dedicated Outdoor Air System (DOAS). This heat gain is then added to the zone design heat gain for the zone and the zone design air flow rate is adjusted to meet the DOAS heat gain plus the zone design heat gain.
-
-#### Field: Dedicated Outdoor Air System Control Strategy
-
-This is a choice field with a choice of three ideal control strategies for the DOA system. The choices are *NeutralSupplyAir*, *NeutralDehumidifiedSupplyAir*, or *ColdSupplyAir*. The default is *NeutralSupplyAir*.
-
-*NeutralSupplyAir* implies that the ventilation air supplied to the zone will cause little heating or cooling. The air will be heated or cooled to keep it between the low and high temperature setpoints specified in the subsequent two fields. A good choice for these fields might be 21.1 and 23.9 degrees C.
-
-*NeutralDehumidifiedSupplyAir* means that the ventilation air will be cooled and dehumidified and then reheated to a neutral temperature. The ventilation air is cooled to the lower setpoint temperature (if necessary) and reheated to the upper setpoint temperature. A good choice for the setpoints would be 14.4 and 22.2 degrees C.
-
-*ColdSupplyAir* means that the ventilation air will be used to supply cooling to the zone. Cold outside air is heated to the upper setpoint; warm outside air is cooled to the lower setpoint. A good choice for the setpoints would be 12.2 and 14.4 degrees C.
-
-#### Field: Dedicated Outdoor Air Low Temperatue Setpoint for Design
-The lower setpoint temperature to be used with the DOAS design control strategy. The units are degrees C. The default is autosized to the values given above for the three design control strategies.
-
-#### Field: Dedicated Outdoor Air High Temperature Setpoint for Design
-The higher setpoint temperature to be used with the DOAS design control strategy. The units are degrees C. The default is autosized to the values given above for the three design control strategies.
-
-An IDF example:
-
-```idf
-Sizing:Zone,
-    SPACE5-1,                !- Name of a zone
-    14.,                     !- Zone cooling design supply air temperature {C}
-    50.,                     !- Zone heating design supply air temperature {C}
-    0.009,                   !- Zone cooling design supply air humidity ratio {kg-H2O/kg-air}
-    0.004,                   !- Zone heating design supply air humidity ratio {kg-H2O/kg-air}
-    DSOA1,                   !- Design Specification Outdoor Air Object Name
-    0.0,                     !- zone heating sizing factor
-    0.0,                     !- zone cooling sizing factor
-    designdaywithlimit,      !- Cooling Design Air Flow Method
-    ,                        !- cooling design air flow rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per zone area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- fraction of the cooling design air flow rate
-    designday,               !- Heating Design Air Flow Method
-    ,                        !- heating design air flow rate {m3/s}
-    ,                        !- heating max air flow per zone area {m3/s-m2}
-    ,                        !- heating max air flow {m3/s}
-    ,                        !- fraction of the cooling design air flow rate
-    DSZADO1,                 !- Design Specification Zone Air Distribution Object Name
-    Yes,                     !- Account for Dedicated Outside Air System
-    ColdSupplyAir,           !- Dedicated Outside Air System Control Strategy
-    12.2,                    !- Dedicated Outside Air Low Setpoint for Design
-    14.4;                    !- Dedicated Outside Air High Setpoint for Design
-
-DesignSpecification:OutdoorAir,
-    DSOA1,                   !- Name
-    SUM,                     !- Outdoor Air Method
-    0.00236,                 !- Outdoor Air Flow per Person
-    0.000305,                !- Outdoor Air Flow per Zone Floor Area
-    0.0,                     !- Outdoor Air Flow per Zone
-    0.0,                     !- Outdoor Air Flow Air Changes per Hour
-    ;                        !- Outdoor Air Flow Rate Fraction Schedule Name
-
-DesignSpecification:ZoneAirDistribution,
-    DSZADO1,                 !- Name
-    1.0,                     !- Zone Air Distribution Effectiveness in Cooling Mode
-    1.0,                     !- Zone Air Distribution Effectiveness in Heating Mode
-    ,                        !- Zone Air Distribution Effectiveness Schedule Name
-    0.3;                     !- Zone Secondary Recirculation Fraction
-```
-
-
-### Zone Sizing Outputs
-
-The zone design air flow rates and loads are output onto the local file “epluszsz.&lt;ext&gt;� where &lt;ext&gt; is the extension from the sizing style object (default is csv – a comma separated file *epluszsz.csv)*. The columns are clearly labeled. It will easily import into Excel or other spreadsheet program that accepts delimited files. All of these values are design air flow rates and loads *calculated by the program*. No sizing factors have been applied.
-
-The calculated zone design air flow rates and the user input or altered zone design air flow rates are also reported on the *eplusout.eio* file. The values are printed out for each zone as comma separated records beginning with *Zone Sizing*. Items output on the *eio* file are: zone name, load type (heating or cooling), design load, calculated design air flow rate, user design air flow rate, design day name, time of peak, outside temperature at peak, outside humidity ratio at peak.
-
-### DesignSpecification:ZoneHVAC:Sizing
-
-This object is used to describe general sizing and scalable sizing methods which are referenced by zone HVAC equipment objects. It is optional input field in zone HVAC objects. If a name of this optional input is not specified or is blank then the sizing method or input specified in the parent object is used.  If the name of this object is entered, then the values or method specified overrides the sizing method in the parent zone HVAC objects. This object is meant to provide scalable sizing method to users. The name of this object is an optional input field in the zoneHVAC objects. When this name in not specified in the zone HVAC object the sizing method or the value specified in the zone HVAC object will be used.
-
-List of zoneHVAC objects than can reference this object include:
-
-* ZoneHVAC:TerminalUnit:VariableRefrigerantFlow
-
-* ZoneHVAC:PackagedTerminalAirConditioner
-
-* ZoneHVAC:PackagedTerminalHeatPump
-
-* ZoneHVAC:WaterToAirHeatPump
-
-* ZoneHVAC:WindowAirConditioner
-
-* ZoneHVAC:UnitHeater
-
-* ZoneHVAC:UnitVentilator
-
-* ZoneHVAC:FourPipeFanCoil
-
-* ZoneHVAC:VentilatedSlab
-
-* ZoneHVAC:EvaporativeCoolerUnit
-
-* ZoneHVAC:IdealLoadsAirSystem
-
-The sizing methods input fields available in this objects are for supply air flow and capacity for heating and cooling operating modes. Some zone HVAC equipment has single supply air flow rate input field that serves both cooling and heating operating modes.  So entering either of the cooling or heating scalable sizing input field is sufficient.  When there are separate input fields for cooling, heating, no-cooling, and no-heating operating modes, the corresponding input fields are specified.  The child components supply air flow rate are also sized using scalable sizing methods specified in the parent objects. The methods allow users to enter a fixed or hard sized values, autosizable, or scalable sizing methods.  Methods allowed for sizing supply air flow rates include: *SupplyAirFlowRate*, *FractionOfAutosizedCoolingAirflow*, *FractionOfAutosizedHeatingAirflow*, *FlowPerFloorArea, FlowPerCoolingCapacity*, and *FlowPerHeatingCapacity*.  The different sizing options are defined as follows:
-
-* **SupplyAirFlowRate**: entered when it is intended that the user specified either hard value or the simulation engine autosize the supply air flow rates for cooling, heating, and no-cooling or no-heating operating modes.
-
-* **FlowPerFloorArea**: entered when it is intended that the simulation engine determine the supply air flow rates from the user specified *supply air flow rates per unit floor area* and the zone floor area of the zone served by the zone HVAC equipment.
-
-* **FractionOfAutosizedCoolingAirflow**: entered when it is intended that the simulation engine determines the supply air flow rates from the user specified *flow fraction* and *autosized cooling design supply air flow rate*.
-
-* **FractionOfAutosizedHeatingAirflow**: entered when it is intended that the simulation engine determines the supply air flow rates from the user specified *flow fraction* and *autosized heating design supply air flow rate*.
-
-* **FlowPerCoolingCapacity**: entered when it is intended t that he simulation engine determines the supply air flow rates from the user specified *supply air flow per cooling capacity value* and *autosized cooling design capacity*.
-
-* **FlowPerHeatingCapacity**: entered when it is intended that the simulation engine determines the supply air flow rates from the user specified *supply air flow per heating capacity value* and *autosized heating design capacity*.
-
-The  Design Specification ZoneHVAC Sizing object also has input fields for sizing or scalable sizing of cooling and heating capacity. However, most of the parent zone HVAC objects do not have input fields for sizing capacities. So, the capacity scalable sizing fields in the parent objects are used for sizing child components capacity sizings.  The scalable capacity sizing may be indirectly impacted by the scalable supply air flow rates sizing values. Moreover, the autosized cold water, hot water and steam flow rates in the parent zone HVAC objects (e.g. FanCoils, UnitHeaters, UnitVentilators, and VentilatedSlabs) and capacity in child components are determined using the scalable sizing methods.  Sizing methods allowed for cooling and heating capacity include: *CoolingDesignCapacity, HeatingDesignCapacity*, *CapacityPerFloorArea, FractionOfAutosizedCoolingCapacity*, *FractionOfAutosizedHeatingCapacity*.
-
-* **CoolingDesignCapacity**: entered when it is intended that user specifies either a hard sized cooling capacity value or the simulation engine autosizes cooling capacity value for the cooling design capacity.
-
-* **HeatingDesignCapacity**: entered when it is intended that user specifies either a hard sized heating capacity value or the simulation engine autosized heating capacity value for the heating design capacity.
-
-* **CapacityPerFloorArea**: is entered when it is intended that the simulation engine determines the cooling or heating capacity from user specified capacity per floor area value and the floor area of the zone served by the zone HVAC equipment.
-
-* **FractionOfAutosizedCoolingCapacity**: entered when it is intended that the simulation engine sizes the cooling capacity from the user specified *capacity fraction* and *autosized cooling design capacity* value.
-
-* **FractionOfAutosizedHeatingCapacity**: entered when it is intended that the simulation engine sizes the heating capacity from the user specified *capacity fraction* and *autosized heating design capacity* value.
-
-Description of the input fields of the design specification zone HVAC sizing object “DesignSpecification:ZoneHVAC:Sizing�:
-
-#### Field: Name
-
-Unique identifier name of the DesignSpecification:ZoneHVAC:Sizing object. This sizing specification object referenced by a zone HVAC equipment whose design calculation will be made using the input data of this object.
-
-#### Field: Cooling Design Air Flow Method
-
-The input of this field must be the method used to determine the cooling supply air volume flow rate. Input allowed is either *None*, *SupplyAirFlowRate*, *FlowPerFloorArea*, *FractionOfAutosizedCoolingAirflow*, or *FlowPerCoolingCapacity*.  None means cooling coil is not included in the zone HVAC equipment or this field may be left blank. *SupplyAirFlowRate* means the user specifies the magnitude of supply air flow rate or the program calculates the design cooling supply air volume flow rate if autosize is specified. *FlowPerFloorArea* means the program calculates the cooling supply air volume flow rate from zone floor area served by the zone HVAC unit and user specified *Flow Per Floor Area* value. *FractionOfAutosizedCoolingAirflow* means the program calculates the cooling supply air volume flow rate from user specified fraction and the autosized design cooling supply air volume flow rate value determined by the simulation. FlowPerCoolingCapacity means the supply air volume is calculated from user specified flow per cooling capacity and design cooling capacity determined by the simulation. The default method is *SupplyAirFlowRate*.
-
-#### Field: Cooling Design Supply Air Flow Rate {m3/s}
-
-Enter the magnitude of the cooling supply air volume flow rate in m3/s. This input is an alternative to using the program auto-calculated value. This input is a required field when the Cooling Design air Flow Method is *SupplyAirFlowRate*. This field may be left blank if a cooling coil is not included in the zone HVAC equipment. This input field is also autosizable.
-
-#### Field: Cooling Design Supply Air Flow Rate Per Floor Area {m3/s-m2}
-
-Enter the cooling supply air volume flow rate per zone conditioned floor area in m3/s-m2. This field is required field when the Cooling Design air Flow Method is *FlowPerFloorArea*. This field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design Air Flow Method is not *FlowPerFloorArea*. The program calculates the cooling supply air volume flow rate from the zone conditioned floor area served by the zone HVAC equipment and the flow per unit area value specified by the user. Zone sizing object (Sizing:Zone) is not required.
-
-#### Field: Fraction of Autosized Cooling Design Supply Air Flow Rate {-}
-
-Enter the cooling supply air volume flow rate as a fraction of the autosized cooling supply air flow rate. This input field is required when the Cooling Design air Flow Method is *FractionOfAutosizedCoolingAirflow*. This input field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design air Flow Method is not *FractionOfAutosizedCoolingAirflow*. The program calculates the cooling supply air volume flow rate from the design autosized cooling supply air flow rate and user specified fraction. Zone sizing object (Sizing:Zone) is required.
-
-#### Field: Cooling Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-
-Enter the cooling supply air volume flow rate per unit cooling capacity in m3/s-W. This input field is required when the Cooling Design air Flow Method is *FlowPerCoolingCapacity*. This field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design air Flow Method is not *FlowPerCoolingCapacity*. The program calculates the cooling supply air volume flow rate from the design autosized cooling capacity and user specified flow per cooling capacity value. Zone sizing object (Sizing:Zone) is required.
-
-#### Field: Supply Air Flow Rate Method When No Cooling or Heating is Required
-
-Enter the method used to determine the supply air volume flow rate when No Cooling or Heating is required. Inputs allowed are *None*, *SupplyAirFlowRate*, *FlowPerFloorArea*, *FractionOfAutosizedCoolingAirflow*, and *FractionOfAutosizedHeatingAirflow.* *None* is used when a cooling or heating coil is not included in the zone HVAC equipment or this field may be left blank. *SupplyAirFlowRate* means user specifies the magnitude of supply air flow rate or the program calculates the design supply air volume flow rate if autosize is specified. *FlowPerFloorArea* means the program calculates the supply air volume flow rate from the zone floor area served by the zone HVAC unit and Flow Per Floor Area value specified by user. *FractionOfAutosizedCoolingAirflow* means the program calculates the supply air volume flow rate from user specified fraction and autosized design cooling supply air volume flow rate value determined by the program. FractionOfAutosizedHeatingAirflow means the program calculates the supply air volume flow rate from user specified fraction and autosized heating supply air flow rate value determined by the program. The default method is *SupplyAirFlowRate*.
-
-#### Field: Supply Air Flow Rate When No Cooling or Heating is Required {m3/s}
-
-Enter the magnitude of the supply air volume flow rate when no cooling or heating is required in m3/s. This input is an alternative to using the program auto-calculated value. This input is a required field when the Supply Air Flow Rate Method When No Cooling or Heating is Required is *SupplyAirFlowRate*. This field may be left blank if a cooling coil is not included in the zone HVAC equipment. This input field is also autosizable.
-
-#### Field: Supply Air Flow Rate Per Floor Area When No Clg or Htg is Required  {m3/s-m2}
-
-Enter the magnitude of supply air volume flow rate per zone floor area in m3/s-m2. This input is a required field when Supply Air  Flow Rate Method When No Cooling or Heating is Required is *FlowPerFloorArea*. The program calculates the supply air flow rate when no cooling or heating is required from user specified flow per floor area and the zone area served by current zoneHVAC equipment.
-
-####  Field: Fraction of Design Cooling Supply Air Flow Rate When No Clg or Htg Required {-}
-
-Enter the fraction of supply air volume flow rate as a fraction of the autosized cooling supply air flow rate. This input field is required field when Supply Air Flow Rate Method When No Cooling or Heating is Required is *FractionOfAutosizedCoolingAirflow*.  The program calculates the supply air flow rate when no cooling or heating is required from user specified fraction and the design cooling autosized supply air flow rate.
-
-#### Field: Fraction of Design Heating Supply Air Flow Rate When No Clg or Htg Required {-}
-
-Enter the fraction of supply air volume flow rate as a fraction of the autosized cooling supply air flow rate. This input field is required field when Supply Air Flow Rate Method When No Cooling or Heating is Required is *FractionOfAutosizedHeatingAirflow*.  The program calculates the supply air flow rate when no cooling or heating is required from user specified fraction and the design heating autosized supply air flow rate.
-
-#### Field: Heating Design Air Flow Method
-
-The input of this field must be the method used to determine the heating supply air volume flow rate. Input allowed is either *None*, *SupplyAirFlowRate*, *FlowPerFloorArea*, *FractionOfAutosizedCoolingAirflow*, or *FlowPerCoolingCapacity*.  *None* means heating coil is not included in the zone HVAC equipment or this field may be left blank. *SupplyAirFlowRate* means the user specifies the magnitude of supply air flow rate or the program calculates the design heating supply air volume flow rate if autosize is specified. *FlowPerFloorArea* means the program calculates the heating supply air volume flow rate from zone floor area served by the zone HVAC unit and user specified *Flow Per Floor Area* value. *FractionOfAutosizedHeatingAirflow* means the program calculates the heating supply air volume flow rate from user specified fraction and the autosized design heating supply air volume flow rate value determined by the simulation. *FlowPerHeatingCapacity* means the supply air volume is calculated from user specified flow per heating capacity and design heating capacity determined by the simulation. The default method is *SupplyAirFlowRate*.
-
-#### Field: Heating Design Supply Air Flow Rate {m3/s}
-
-Enter the magnitude of the heating supply air volume flow rate in m3/s. This input is an alternative to using the program auto-calculated value. This input is a required field when the Heating Design air Flow Method is *SupplyAirFlowRate*. This field may be left blank if a heating coil is not included in the zone HVAC equipment. This input field is also autosizable.
-
-#### Field: Heating Design Supply Air Flow Rate Per Floor Area {m3/s-m2}
-
-Enter the heating supply air volume flow rate per zone conditioned floor area in m3/s-m2. This field is required field when the Heating Design air Flow Method is *FlowPerFloorArea*. This field may be left blank if a heating coil is not included in the zone HVAC equipment or the Heating Design Air Flow Method is not *FlowPerFloorArea*. The program calculates the heating supply air volume flow rate from the zone conditioned floor area served by the zone HVAC equipment and the flow per unit area value specified by the user.
-
-#### Field: Fraction of Autosized Heating Design Supply Air Flow Rate {-}
-
-Enter the heating supply air volume flow rate as a fraction of the autosized heating supply air flow rate. This input field is required when the Heating Design air Flow Method is *FractionOfAutosizedHeatingAirflow*. This input field may be left blank if a heating coil is not included in the zone HVAC equipment or the Heating Design air Flow Method is not *FractionOfAutosizedHeatingAirflow*. The program calculates the heating supply air volume flow rate from the design autosized heating supply air flow rate and user specified fraction.
-
-#### Field: Heating Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-
-Enter the heating supply air volume flow rate per unit heating capacity in m3/s-W. This input field is required when the Heating Design air Flow Method is *FlowPerHeatingCapacity*. This field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Heating Design air Flow Method is not *FlowPerHeatingCapacity*. The program calculates the heating supply air volume flow rate from the design autosized heating capacity and user specified flow per unit heating capacity value.
-
-#### Field Cooling Design Capacity Method
-
-Enter the method used to determine the cooling design capacity for scalable sizing. Input allowed is either *None*, *CoolingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedCoolingCapacity*. None is used when a cooling coil is not included in the Zone HVAC equipment or this field may be left blank. If this input field is left blank, then the design cooling capacity is set to zero. *CoolingDesignCapacity* means user specifies the magnitude of cooling capacity or the program calculates the design cooling capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design cooling capacity from user specified cooling capacity per floor area and floor area of the zone served by the HVAC unit. *FractionOfAutosizedCoolingCapacity* means the program calculates the design cooling capacity from user specified fraction and the auto-sized design cooling capacity. The default method is *CoolingDesignCapacity*.
-
-#### Field: Cooling Design Capacity {W}
-
-Enter the magnitude of the cooling capacity in Watts. This input is an alternative to using the program auto-calculated cooling capacity value. This input is a required field when the Cooling Design Capacity Method is *CoolingDesignCapacity*. This field may be left blank if a cooling coil is not included in the zone HVAC equipment or alternative method is specified. This input field is autosizable. Design day sizing run must be specified.
-
-#### Field: Cooling Design Capacity Per Floor Area {W/m2}
-
-Enter the cooling capacity per unit floor area in m3/s-m2. This field is required field when the Cooling Design Capacity Method is *CapacityPerFloorArea*. This field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design Capacity Method is not *CapacityPerFloorArea*. The program calculates the cooling capacity from floor area of the zone served by the zone HVAC equipment and the cooling capacity per unit floor area value specified by the user.
-
-#### Field: Fraction of Autosized Cooling Design Capacity {-}
-
-Enter the cooling capacity as a fraction of the autosized cooling capacity. This input field is required when the Cooling Design Capacity Method is *FractionOfAutosizedCoolingCapacity*. This input field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design Capacity Method is not *FractionOfAutosizedCoolingCapacity*. The program calculates the cooling capacity from the design autosized cooling capacity and user specified fraction. Design day sizing run must be specified.
-
-#### Field: Heating Design Capacity Method
-
-Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either *None*, *HeatingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedHeatingCapacity*. None is used when a heating coil is not included in the Zone HVAC equipment or this field may be left blank. If this input field is left blank, then the design heating capacity is set to zero. *HeatingDesignCapacity* means user specifies the magnitude of heating capacity or the program calculates the design heating capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the HVAC unit. *FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is *HeatingDesignCapacity*.
-
-#### Field: Heating Design Capacity {W}
-
-Enter the magnitude of the heating capacity in Watts. This input is an alternative to using the program auto-calculated heating capacity value. This input is a required field when the Heating Design Capacity Method is *HeatingDesignCapacity*. This field may be left blank if a heating coil is not included in the zone HVAC equipment or alternative method is specified. This input field is autosizable. Design day sizing run must be specified.
-
-#### Field: Heating Design Capacity Per Floor Area {W/m2}
-
-Enter the heating capacity per unit floor area in m3/s-m2. This field is required field when the Heating Design Capacity Method is *CapacityPerFloorArea*. This field may be left blank if a heating coil is not included in the zone HVAC equipment or the Heating Design Capacity Method is not *CapacityPerFloorArea*. The program calculates the heating capacity from floor area of the zone served by the zone HVAC equipment and the heating capacity per unit floor area value specified by the user.
-
-#### Field: Fraction of Autosized Heating Design Capacity {-}
-
-Enter the heating capacity as a fraction of the autosized heating capacity. This input field is required when the Heating Design Capacity Method is *FractionOfAutosizedHeatingCapacity*. This input field may be left blank if a heating coil is not included in the zone HVAC equipment or the Heating Design Capacity Method is not *FractionOfAutosizedHeatingCapacity*. The program calculates the heating capacity from the design autosized cooling capacity and user specified fraction. Design day sizing run must be specified.
-
-```idf
-  DesignSpecification:ZoneHVAC:Sizing,
-    VRFDesignSpec1,          !- Name
-    SupplyAirFlowRate,       !- Cooling Design Air Flow Method
-    autosize,                !- Cooling Design Supply Air Flow Rate
-    ,                        !- Cooling Design Supply Air Flow Rate Per Floor Area
-    ,                        !- Fraction of Autosized Cooling Design Supply Air Flow Rate
-    ,                        !- Cooling Design Supply Air Flow Rate Per Unit of Capacity {m3/s-W}
-    SupplyAirFlowRate,       !- Supply Air Flow Rate Method When No Cooling or Heating is Required
-    autosize,                !- Supply Air Flow Rate When No Cooling or Heating is Required
-    ,                        !- Supply Air Flow Rate Per Floor Area When No Clg or Htg is Required
-    ,                     !- Fraction of Autosized Design Cooling Supply Air Flow Rate When No Clg or Htg
-    ,                     !- Fraction of Autosized Design Heating Supply Air Flow Rate When No Clg or Htg
-    SupplyAirFlowRate,       !- Heating Design Air Flow Method
-    autosize,                !- Heating Design Supply Air Flow Rate
-    ,                        !- Heating Design Supply Air Flow Rate Per Floor Area
-    ,                        !- Fraction of Autosized Heating Design Supply Air Flow Rate
-    ,                        !- Heating Design Supply Air Flow Rate Per Unit of Heating Capacity
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity {-}
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ;                        !- Fraction of Autosized Cooling Design Capacity {-}
-
-  DesignSpecification:ZoneHVAC:Sizing,
-    VRFDesignSpec2,          !- Name
-    FlowPerFloorArea,        !- Cooling Design Air Flow Method
-    ,                        !- Cooling Design Supply Air Flow Rate
-    3.6311418E-03,           !- Cooling Design Supply Air Flow Rate Per Floor Area
-    ,                        !- Fraction of Autosized Cooling Design Supply Air Flow Rate
-    ,                        !- Cooling Design Supply Air Flow Rate Per Unit of Capacity {m3/s-W}
-    FlowPerFloorArea,        !- Supply Air Flow Rate Method When No Cooling or Heating is Required
-    ,                        !- Supply Air Flow Rate When No Cooling or Heating is Required
-    3.6311418E-03,           !- Supply Air Flow Rate Per Floor Area When No Clg or Htg is Required
-    ,                     !- Fraction of Autosized Design Cooling Supply Air Flow Rate When No Clg or Htg
-    ,                     !- Fraction of Autosized Design Heating Supply Air Flow Rate When No Clg or Htg
-    FlowPerFloorArea,        !- Heating Design Air Flow Method
-    ,                        !- Heating Design Supply Air Flow Rate
-    3.6311418E-03,           !- Heating Design Supply Air Flow Rate Per Floor Area
-    ,                        !- Fraction of Autosized Heating Design Supply Air Flow Rate
-    ,                        !- Heating Design Supply Air Flow Rate Per Unit of Heating Capacity
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity {-}
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ;                        !- Fraction of Autosized Cooling Design Capacity {-}
-
-DesignSpecification:ZoneHVAC:Sizing,
-    VRFDesignSpec3,          !- Name
-    FractionOfAutosizedCoolingAirflow,  !- Cooling Design Air Flow Method
-    ,                        !- Cooling Design Supply Air Flow Rate
-    ,                        !- Cooling Design Supply Air Flow Rate Per Floor Area
-    0.5,                     !- Fraction of Autosized Cooling Design Supply Air Flow Rate
-    ,                        !- Cooling Design Supply Air Flow Rate Per Unit of Capacity {m3/s-W}
-  FractionOfAutosizedCoolingAirflow, !- Supply Air Flow Rate Method When No Cooling or Heating is Required
-    ,                        !- Supply Air Flow Rate When No Cooling or Heating is Required
-    ,                        !- Supply Air Flow Rate Per Floor Area When No Clg or Htg is Required
-    0.5,                 !- Fraction of Autosized Design Cooling Supply Air Flow Rate When No Clg or Htg
-    ,                    !- Fraction of Autosized Design Heating Supply Air Flow Rate When No Clg or Htg
-    FractionOfAutosizedHeatingAirflow,  !- Heating Design Air Flow Method
-    ,                        !- Heating Design Supply Air Flow Rate
-    ,                        !- Heating Design Supply Air Flow Rate Per Floor Area
-    0.5,                     !- Fraction of Autosized Heating Design Supply Air Flow Rate
-    ,                        !- Heating Design Supply Air Flow Rate Per Unit of Heating Capacity
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity {-}
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ;                        !- Fraction of Autosized Cooling Design Capacity {-}
-
-DesignSpecification:ZoneHVAC:Sizing,
-    VRFDesignSpec4,          !- Name
-    FlowPerCoolingCapacity,  !- Cooling Design Air Flow Method
-    ,                        !- Cooling Design Supply Air Flow Rate
-    ,                        !- Cooling Design Supply Air Flow Rate Per Floor Area
-    ,                        !- Fraction of Autosized Cooling Design Supply Air Flow Rate
-    2.9541628E-05,           !- Cooling Design Supply Air Flow Rate Per Unit of Capacity {m3/s-W}
-  FractionOfAutosizedHeatingAirflow, !- Supply Air Flow Rate Method When No Cooling or Heating is Required
-    ,                        !- Supply Air Flow Rate When No Cooling or Heating is Required
-    ,                        !- Supply Air Flow Rate Per Floor Area When No Clg or Htg is Required
-    ,                    !- Fraction of Autosized Design Cooling Supply Air Flow Rate When No Clg or Htg
-    0.413231177,         !- Fraction of Autosized Design Heating Supply Air Flow Rate When No Clg or Htg
-    FlowPerHeatingCapacity,  !- Heating Design Air Flow Method
-    ,                        !- Heating Design Supply Air Flow Rate
-    ,                        !- Heating Design Supply Air Flow Rate Per Floor Area
-    ,                        !- Fraction of Autosized Heating Design Supply Air Flow Rate
-    2.9541628E-05,           !- Heating Design Supply Air Flow Rate Per Unit of Heating Capacity
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity {-}
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ;                        !- Fraction of Autosized Cooling Design Capacity {-}
-```
-
-### Sizing:System
-
-The Sizing:System object contains the input needed to perform a central forced air system design air flow, heating capacity, and cooling capacity calculation for a system serving one or more zones. The information needed consists of the outside environmental conditions and the design supply air temperatures, outdoor air flow rate, and minimum system air flow ratio.
-
-The outside conditions come from the design days in the input. A system sizing calculation is performed for every design day in the input file and the resulting maximum heating and cooling air flow rates and capacities are saved for use in the component sizing calculations.
-
-Supply air conditions are specified by inputting a supply air temperature for cooling, a supply air temperature for heating, and a preheat temperature.
-
-The system sizing calculation sums the zone design air flow rates to obtain a system supply air flow rate. The design conditions and the outdoor air flow rate are used to calculate a design mixed air temperature. The temperature plus the design supply air temperatures allows the calculation of system design heating and cooling capacities.
-
-#### Field: AirLoop Name
-
-The name of the AirLoopHVAC corresponding to this Sizing:System object. This is the air system for which the design calculation will be made using the input data of this Sizing:System Object.
-
-#### Field: Type of Load to Size On
-
-The user specified type of load on which to size the central system. The choices are *Sensible*, *Total* and *VentilationRequirement*.  *Sensible* and *Total* mean that the central system supply air flow rate will be determined by combining the zone design air flow rates, which have been calculated to meet the zone sensible loads from the design days. *VentilationRequirement* means that the central system supply air flow rate will be determined by the system ventilation requirement.  In addition *Sensible* tells the program to size the central cooling coil using entering air flow rate and air conditions at the sensible load peak; *Total* indicates that the program should size  the central cooling coil at the air flow rate and conditions at the total load peak. The central heating coil is always sized at the conditions at the peak sensible heating load.
-
-#### Field: Design Outdoor Air Flow Rate
-
-The design outdoor air flow rate in cubic meters per second. Generally this should be the minimum outdoor air flow. It is used for both heating and cooling design calculations. The assumption for cooling is that any outdoor air economizer will be closed. If *Autosize* is input the outdoor air flow rate will be taken from the sum of the zone outdoor air flow rates or calculated based on the System Outdoor Air Method selection (field below).
-
-#### Field: Central Heating Maximum System Air Flow Ratio
-
-The ratio of the maximum system air flow rate for heating to the maximum system air flow rate.  The value must be between 0 and 1. For constant volume systems the ratio should be set to 1. This ratio should be set to reflect what the user expects the system flow rate to be when maximum heating demand occurs. This ratio is used in calculating the central system heating capacity. Thus if the system is VAV with the zone VAV dampers held at minimum flow when there is a zone heating demand, this ratio should be set to the minimum flow ratio. If the zone VAV dampers are reverse action and can open to full flow to meet heating demand, this ratio should be set to 1.  The default is set to 0.5, reflecting the fact that VAV dampers are typically not allowed to fully open during heating.
-
-#### Field: Preheat Design Temperature
-
-The design air temperature exiting the preheat coil (if any) in degrees Celsius.
-
-#### Field: Preheat Design Humidity Ratio
-
-The design humidity ratio exiting the preheat coil (if any) in kilograms of water per kilogram of dry air. (kgWater/kgDryAir)
-
-#### Field: Precool Design Temperature
-
-The design air temperature exiting the precooling coil (if any) in degrees Celsius.
-
-#### Field: Precool Design Humidity Ratio
-
-The design humidity ratio exiting the precooling coil (if any) in kilograms of water per kilogram of dry air. (kgWater/kgDryAir)
-
-#### Field: Central Cooling Design Supply Air Temperature
-
-The design supply air temperature for cooling in degrees Celsius. This should be the temperature of the air exiting the central cooling coil.
-
-#### Field: Central Heating Design Supply Air Temperature
-
-The design supply air temperature for heating in degrees Celsius. This can be either the reset temperature for a single duct system or the actual hot duct supply air temperature for dual duct systems. It should be the temperature at the exit of the main heating coil. This value is also used for the sizing of zone equipment (e.g., reheat coil) for the system embedded with central heating coils, but it is not used if there is no central heating coil in the system.
-
-#### Field: Type of Zone Sum to Use
-
-If the input is *coincident* the central system air flow rate will be sized on the sum of the coincident zone air flow rates. If the input is *noncoincident* the central system air flow rate will be sized on the sum of the noncoincident zone air flow rates. The default is noncoincident.
-
-#### Field: 100% Outdoor Air in Cooling
-
-Entering *Yes* means the system will be sized for cooling using 100% outdoor air. Entering *No* means the system will be sized for cooling using minimum outside air (the default).
-
-#### Field: 100% Outdoor Air in Heating
-
-Entering *Yes* means the system will be sized for heating using 100% outdoor air. Entering *No* means the system will be sized for heating using minimum outside air (the default).
-
-#### Field: Central Cooling Design Supply Air Humidity Ratio
-
-The design humidity ratio in kilograms of water per kilogram of dry air at the exit of the central cooling coil. The default is .008 (kgWater/kgDryAir).
-
-#### Field: Central Heating Design Supply Air Humidity Ratio
-
-The design humidity ratio in kilograms of water per kilogram of dry air at the exit of the central heating coil. This value is also used for the sizing of zone equipment (e.g., reheat coil) for the system embedded with central heating coils, but it is not used if there is no central heating coil in the system. The default is .008 (kgWater/kgDryAir).
-
-#### Field: Cooling Supply Air Flow Rate Method
-
-The input of this field must be the method used to determine the airloop cooling supply air volume flow rate. The input must be either, *DesignDay*, *Flow/System,* *FlowPerFloorArea*, *FractionOfAutosizedCoolingAirflow*, or *FlowPerCoolingCapacity*. *DesignDay* means the program will calculate the system design cooling supply air volume flow rate using the System Sizing input data and a design day simulation. *Flow/System* means that the program will use the input of the field *Cooling Design Air Flow Rate* as the system design cooling supply air volume flow rate. *FlowPerFloorArea* means the program calculates the cooling supply air volume flow rate from zone floor area served by the airloop and user specified *Flow Per Floor Area* value. *FractionOfAutosizedCoolingAirflow* means the program calculates the cooling supply air volume flow rate from user specified fraction and the autosized design cooling supply air volume flow rate value determined by the simulation. *FlowPerCoolingCapacity* means the supply air volume is calculated from user specified flow per cooling capacity and design cooling capacity determined by the simulation. The default method is *DesignDay*: i.e., the program uses the calculated design values.
-
-#### Field: Cooling Supply Air Flow Rate
-
-The design system cooling air flow rate in cubic meters per second. This input is an alternative to using the program autocalculated value. This input is used if Coolingi Supply Air Flow Rate Method is Flow/System. This value will *not* be multiplied by any sizing factor or by zone multipliers. If using zone multipliers, this value must be large enough to serve the multiplied zones.
-
-#### Field: Cooling Supply Air Flow Rate Per Floor Area {m3/s-m2}
-
-Enter the cooling supply air volume flow rate per zone conditioned floor area in m3/s-m2. This field is required field when the Cooling Supply Air Flow Rate Method is *FlowPerFloorArea*. This field may be left blank if a cooling coil is not included in the airloop or the Cooling Supply Air Flow Rate Method is not *FlowPerFloorArea*. The program calculates the cooling supply air volume flow rate from the cooled floor area served by the air loop and the *Flow Per Unit Area* value specified by the user.
-
-#### Field: Cooling Fraction of Autosized Cooling Design Supply Air Flow Rate {-}
-
-Enter the cooling supply air volume flow rate as a fraction of the airloop autosized cooling supply air flow rate. This input field is required when the Cooling Supply Air Flow Rate Method is *FractionOfAutosizedCoolingAirflow*. This input field may be left blank if a cooling coil is not included in the airloop or the Cooling Supply Air Flow Rate Method is not *FractionOfAutosizedCoolingAirflow*. The program calculates the cooling supply air volume flow rate from the design autosized cooling supply air flow rate and user specified fraction.
-
-#### Field: Cooling Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-
-Enter the cooling supply air volume flow rate per unit cooling capacity in m3/s-W. This input field is required when the Cooling Supply Air Flow Rate Method is *FlowPerCoolingCapacity*. This field may be left blank if a cooling coil is not included in the airloop or the Cooling Supply Air Flow Rate Method is not *FlowPerCoolingCapacity*. The program calculates the airloop cooling supply air volume flow rate from the design autosized cooling capacity and user specified *Flow Per Cooling Capacity* value.
-
-#### Field: Heating Supply Air Flow Rate Method
-
-The input of this field must be the method used to determine the airloop heating supply air volume flow rate. The input must be either, *DesignDay*, *Flow/System,* *FlowPerFloorArea*, *FractionOfAutosizedHeatingAirflow*, *FractionOfAutosizedCoolingAirflow* or *FlowPerHeatingCapacity*. *DesignDay* means the program will calculate the system design heating supply air volume flow rate using the System Sizing input data and a design day simulation. *Flow/System* means that the program will use the input of the field *Heating Design Air Flow Rate* as the system design heating supply air volume flow rate. *FlowPerFloorArea* means the program calculates the system heating supply air volume flow rate from zone floor area served by the airloop and user specified *Flow Per Floor Area* value. *FractionOfAutosizedHeatingAirflow* means the program calculates the system heating supply air volume flow rate from user specified fraction and the autosized system design heating supply air volume flow rate value determined by the simulation. *FractionOfAutosizedCoolingAirflow* means the program calculates the system heating supply air volume flow rate from user specified fraction and the autosized system design cooling supply air volume flow rate value determined by the simulation. *FlowPerHeatingCapacity* means the system heating supply air volume is calculated from user specified flow per heating capacity and design heating capacity determined by the simulation. The default method is *DesignDay*: i.e., the program uses the calculated design values.
-
-#### Field: Heating Supply Air Flow Rate
-
-The design system heating air flow rate in cubic meters per second. This input is an alternative to using the program autocalculated value. This input is used if Heating Supply Air Flow Rate Method is Flow/System. This value will *not* be multiplied by any sizing factor or by zone multipliers. If using zone multipliers, this value must be large enough to serve the multiplied zones.
-
-#### Field: Heating Supply Air Flow Rate Per Floor Area {m3/s-m2}
-
-Enter the heating supply air volume flow rate per zone conditioned floor area in m3/s-m2. This field is required field when the Heating Supply Air Flow Rate Method is *FlowPerFloorArea*. This field may be left blank if a heating coil is not included in the airloop or the Heating Supply Air Flow Rate Method is not *FlowPerFloorArea*. The program calculates the heating supply air volume flow rate from the heated or cooled floor area served by the air loop and the *Flow Per Unit Area* value specified by the user.
-
-#### Field: Heating Fraction of Autosized Heating Supply Air Flow Rate {-}
-
-Enter the heating supply air volume flow rate as a fraction of the airloop autosized heating supply air flow rate. This input field is required when the Heating Supply Air Flow Rate Method is *FractionOfAutosizedHeatingAirflow*. This input field may be left blank if heating coil is not included in the airloop or the Heating Supply Air Flow Rate Method is not *FractionOfAutosizedHeatingAirflow*. The program calculates the heating supply air volume flow rate from the design autosized heating supply air flow rate and user specified fraction.
-
-#### Field: Heating Fraction of Autosized Cooling Supply Air Flow Rate {-}
-
-Enter the heating supply air volume flow rate as a fraction of the airloop autosized cooling supply air flow rate. This input field is required when the Heating Supply Air Flow Rate Method is *FractionOfAutosizedCoolingAirflow*. This input field may be left blank if heating coil is not included in the airloop or the Heating Supply Air Flow Rate Method is not *FractionOfAutosizedCoolingAirflow*. The program calculates the heating supply air volume flow rate from the design autosized cooling supply air flow rate and user specified fraction.
-
-#### Field: Heating Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-
-Enter the heating supply air volume flow rate per unit heating capacity in m3/s-W. This input field is required when the Heating Design air Flow Method is *FlowPerCoolingCapacity*. This field may be left blank if a heating coil is not included in the airloop or the Heating Design air Flow Method is not *FlowPerHeatingCapacity*. The program calculates the airloop heating supply air volume flow rate from the design autosized heating capacity and user specified *Flow Per Heating Capacity* value.
-
-#### Field: System Outdoor Air Method
-
-The method used to calculate the system minimum outdoor air flow. The two choices are ZoneSum and VentilationRateProcedure (VRP). ZoneSum sums the outdoor air flows across all zones served by the system. VRP uses the multi-zone equations defined in 62.1-2007 to calculate the system outdoor air flow. VRP considers zone air distribution effectiveness and zone diversification of outdoor air fractions.
-
-#### Field: Zone Maximum Outdoor Air Fraction
-
-This positive numeric input is the zone maximum outdoor air fraction. For an air loop, when a zone requires outdoor air higher than the user specified Zone Maximum Outdoor Air Fraction, the zone supply air flow will be increased to cap the outdoor air fraction at the maximum value. This allows the system level outdoor air flow to be reduced while the total supply air flow increases. Valid values are from 0 to 1.0. Default is 1.0 which indicates zones can have 100% outdoor air maintaining backward compatibility. This inputs work for constant volume air systems, single and dual duct VAV systems.
-
-#### Field Cooling Design Capacity Method
-
-Enter the method used to determine the cooling design capacity for scalable sizing. Input allowed is either *None*, *CoolingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedCoolingCapacity*. None is used when a cooling coil is not included in the airloop. If this input field is left blank, or None is specified, then the autosized design cooling capacity determined by the program is used. *CoolingDesignCapacity* means user specifies the magnitude of cooling capacity or the program calculates the design cooling capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design cooling capacity from user specified cooling capacity per floor area and floor area of the zones served by the airloop. *FractionOfAutosizedCoolingCapacity* means the program calculates the design cooling capacity from user specified fraction and the auto-sized design cooling capacity. If the value this input field is blank or specified as None, then the next three input fields are not required. The default method is *CoolingDesignCapacity*.
-
-#### Field: Cooling Design Capacity {W}
-
-Enter the magnitude of the cooling capacity in Watts. This input is an alternative to using the program auto-calculated cooling capacity value. This input is a required field when the Cooling Design Capacity Method is *CoolingDesignCapacity*. This field may be left blank if a cooling coil is not included in the air loop or alternative method is specified. This input field is autosizable.
-
-#### Field: Cooling Design Capacity Per Floor Area {W/m2}
-
-Enter the cooling capacity per unit floor area in m3/s-m2. This field is required field when the Cooling Design Capacity Method is *CapacityPerFloorArea*. This field may be left blank if a cooling coil is not included in the airloop or the Cooling Design Capacity Method is not *CapacityPerFloorArea*. The program calculates the cooling capacity from floor area of the zones served by the airloop and the cooling capacity per unit floor area value specified by the user.
-
-#### Field: Fraction of Autosized Cooling Design Capacity {-}
-
-Enter the cooling capacity as a fraction of the autosized cooling capacity. This input field is required when the Cooling Design Capacity Method is *FractionOfAutosizedCoolingCapacity*. This input field may be left blank if a cooling coil is not included in the zone HVAC equipment or the Cooling Design Capacity Method is not *FractionOfAutosizedCoolingCapacity*. The program calculates the cooling capacity from the design autosized cooling capacity and user specified fraction. Design day sizing run must be specified.
-
-#### Field: Heating Design Capacity Method
-
-Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either *None*, *HeatingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedHeatingCapacity*. *None* is used when a heating coil is not included in the airloop. If this input field is left blank, then the autosized design heating capacity determined by the program is used. *HeatingDesignCapacity* means user specifies the magnitude of heating capacity or the program calculates the design heating capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zones served by the airllop. *FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. If the value this input field is blank or specified as None, then the next three input fields are not required. The default method is *HeatingDesignCapacity*.
-
-#### Field: Heating Design Capacity {W}
-
-Enter the magnitude of the heating capacity in Watts. This input is an alternative to using the program auto-calculated heating capacity value. This input is a required field when the Heating Design Capacity Method is *HeatingDesignCapacity*. This field may be left blank if a heating coil is not included in the airloop or alternative method is specified. This input field is autosizable.
-
-#### Field: Heating Design Capacity Per Floor Area {W/m2}
-
-Enter the heating capacity per unit floor area in m3/s-m2. This field is required field when the Heating Design Capacity Method is *CapacityPerFloorArea*. This field may be left blank if a heating coil is not included in the airloop or the Heating Design Capacity Method is not *CapacityPerFloorArea*. The program calculates the heating capacity from floor area of the zones served by the airloop and the heating capacity per unit floor area value specified by the user.
-
-#### Field: Fraction of Autosized Heating Design Capacity {-}
-
-Enter the heating capacity as a fraction of the autosized heating capacity. This input field is required when the Heating Design Capacity Method is FractionOfAutosizedHeatingCapacity. This input field may be left blank if heating coil is not included in the airloop or the Heating Design Capacity Method is not FractionOfAutosizedHeatingCapacity. The program calculates the heating capacity from the design autosized cooling capacity and user specified fraction.
-
-#### Field: Central Cooling Capacity Control Method
-
-Specifies how the central cooling coil will be controlled, which affects the coil sizing calculation. There are 4 choices: VAV, Bypass, VT, and OnOff. Choose VAV  if the cooling output is controlled by varying the air flow. Bypass  should be chosen if the capacity is controlled by bypassing a variable fraction of the mixed air around the coil face. VT  indicates that cooling coil output is controlled by varying the coil exit temperature while the flow rate is constant. And OnOff means that the cooling output is controlled by cycling the air flow. 
-
-An IDF example:
-
-```IDF
-Sizing:System,
-    VAV Sys 1,               !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    autosize,                !- Design Outdoor Air Flow Rate {m3/s}
-    0.3,                     !- Minimum System Air Flow Ratio
-    4.5,                     !- Preheat Design Temperature {C}
-    .008,                    !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    .008,                    !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.8,                    !- Central Cooling Design Supply Air Temperature {C}
-    16.7,                    !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Sizing Option
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    designday,               !- Cooling Supply Air Flow Rate Method
-    0,                       !- Cooling Supply Air Flow Rate {m3/s}
-    ,                        !- Cooling Supply Air Flow Rate Per Floor Area {m3/s-m2}
-    ,                        !- Cooling Fraction of Autosized Cooling Supply Air Flow Rate {-}
-    ,                        !- Cooling Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    designday,               !- Heating Supply Air Flow Rate Method
-    0,                       !- Heating Supply Air Flow Rate {m3/s}
-    ,                        !- Heating Supply Air Flow Rate Per Floor Area {m3/s-m2}
-    ,                        !- Heating Fraction of Autosized Heating Supply Air Flow Rate {-}
-    ,                        !- Heating Fraction of Autosized Cooling Supply Air Flow Rate {-}
-    ,                        !- Heating Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ZoneSum,                 !- System Outdoor Air Method
-    0.5,                     !- Zone Maximum Outdoor Air Fraction
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity {-}
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ;                        !- Fraction of Autosized Cooling Design Capacity {-}
-
-```
-
-
-### System Sizing Outputs
-
-The system design air flow rates and heating and cooling capacities are output onto the local file “eplusssz.&lt;ext&gt;� where &lt;ext&gt; is the extension from the sizing style object (default is csv – a comma separated file *eplusssz.csv)*. The columns are clearly labeled. It will easily import into Excel or other spreadsheet program that accepts delimited files. The results are calculated values and do not include any user input system flow rates.
-
-The calculated system design air flow rates and the user input system design air flow rates are also reported on the *eplusout.eio* file. The values are printed out for each system as comma separated records beginning with *System Sizing*. An example is:
-
-```
-! <System Sizing Information>c++, System Name, Field Description, Value
- System Sizing, VAV SYS 1, Calculated Cooling Design Air Flow Rate [m3/s],   1.3194
- System Sizing, VAV SYS 1, User Cooling Design Air Flow Rate [m3/s],   1.5000
- System Sizing, VAV SYS 1, Calculated Heating Design Air Flow Rate [m3/s],  0.90363
- System Sizing, VAV SYS 1, User Heating Design Air Flow Rate [m3/s],   1.0000
-```
-
-### Sizing:Plant
-
-The Sizing:Plant object contains the input needed for the program to calculate plant loop flow rates and equipment capacities when autosizing. This information is initially used by components that use water for heating or cooling such as hot or chilled water coils to calculate their maximum water flow rates. These flow rates are then summed for use in calculating the Plant Loop flow rates.
-
-The program will size any number of chilled water, hot water, condenser water and other plant loops. There should be one Sizing:Plant object for each plant loop that is to be autosized.
-
-#### Field: Plant or Condenser Loop Name
-
-The name of a Plant Loop or Condenser Loop object corresponding to this Sizing:Plant object. This is the plant loop for which this data will be used for calculating the loop flow rate.
-
-#### Field: Loop Type
-
-The possible inputs are *Heating, Steam, Cooling,* or *Condenser*.
-
-#### Field: Design Loop Exit Temperature
-
-The water temperature in degrees Celsius at the exit of the supply side of the plant loop, Thus this is the temperature of the water supplied to the inlet of chilled or hot water coils and other equipment that places loads on a plant loop.
-
-#### Field: Loop Design Temperature Difference
-
-The design temperature rise (for cooling or condenser loops) or fall (for heating loops) in degrees Celsius across the demand side of a plant loop.  This temperature difference is used by component models to determine flow rates required to meet design capacities.  Larger values lead to smaller design flow rates.
-
-#### Field: Sizing Option
-
-This field is optional. This field controls how concurrence issues impact the plant loop design flow rate. If it is not used then the program uses noncoincident method, which is the historical behavior prior to version 8.3. There are two choices, noncoincident and coincident. The use of Coincident sizing option requires that the SimulationControl object be set to YES for the input field called Do HVAC Sizing Simulation for Sizing Periods.
-
-#### Field: Zone Timesteps in Averaging Window
-
-This field is optional and is only used if the preceding field is set to Coincident.  This is the number of zone timesteps used in a moving average to determine the design flow rate from HVAC Sizing Simulation approach.  This allows using a broader average over time when using coincident plant sizing.  This is similar in concept to the similar field in Sizing:Parameters which specifies the averaging window for zone loads.  The default is 1. 
-
-#### Field: Coincident Sizing Factor Mode
-
-This field is only used if the sizing option is set to Coincident.  This field controls the behavior of coincident sizing with respect to what, if any, sizing factor should be applied to further modify the flow rate measured while running HVAC Sizing Simulations.  There are four options.  Enter the keword None to use the raw value for flow rate without modification.  Enter the keyword GlobalHeatingSizingFactor to modify the flow by the sizing factor entered in the object called Sizing:Parameters for heating. Enter the keyword GlobalCoolingSizingFactor to modify the flow by the sizing factor entered in the object called Sizing:Parameters for cooling.  Enter the keyword LoopComponentSizingFactor to modify the flow by a sizing factor determined from the combination of component-level sizing factors in the associated plant loop. 
-
-An IDF example:
-
-```idf
-Sizing:Plant,
-   Chilled Water Loop, ! name of loop
-   Cooling,            ! type of loop
-   7.22,               ! chilled water supply temperature
-   6.67,               ! chilled water delta T
-   NonCoincident,      !- Sizing Option
-   1,                  !- Zone Timesteps in Averaging Window
-   GlobalCoolingSizingFactor; !- Coincident Sizing Factor Mode
-```
-   
-### Plant Sizing Outputs
-
-The loop flow rates are reported on the *eplusout.eio* file along with the component sizing results.
-
-When coincident plant sizing method is used, the eio file contains special summary report with various details and interim values from the calculations, under the following record header:  ! <Plant Sizing Coincident Flow Algorithm>, Plant Loop Name, Sizing Pass {#}, Measured Mass Flow{kg/s}, Measured Demand {W}, Demand Calculated Mass Flow{kg/s}, Sizes Changed {Yes/No}, Previous Volume Flow Rate {m3/s}, New Volume Flow Rate {m3/s}, Demand Check Applied {Yes/No}, Sizing Factor {}, Normalized Change {}, Specific Heat{}.
-
-HVAC: Primary and Secondary Systems
------------------------------------
-
-The HVAC and equipment section of the EnergyPlus input data dictionary and input data file are slightly more complex than the description of building geometry, internal gains, etc. because of the interconnections of the various parts of an HVAC system. In EnergyPlus, there are several portions to the HVAC simulation. All of these parts must be correctly specified in order to arrive at a valid simulation model. The goal of this section is to provide interface developers and advanced users with guidelines on what input is expected and also provide some background on basic EnergyPlus simulation methodology.
-
-An EnergyPlus HVAC simulation consists of various components that are connected physically in the actual system by ducts, piping, etc. Every component in an HVAC system must have an inlet and outlet “node�. In the actual system, a node might be a point in the system at which fluid properties can be measured. In an EnergyPlus simulation, the nodes are points at which fluid properties are evaluated and passed on to subsequent equipment.
-
-Components are linked together to form various loops within the simulation. Thus, the output node from one component also serves as the inlet node to the next component. Loops are constructed by defining these loops and also defining the components on the loops. The figure below shows a generic example of the loop-node concept.
-
-Loop nodes are a key defining feature in EnergyPlus. As a result, it is recommended that one of the first steps taken in defining an HVAC system in EnergyPlus be the definition of a node diagram or map. This is helpful for visualization of the entire system. Such a map could be created electronically within an interface or could be kept in the background out of the sight of the user.
-
-![](media/image134.svg)
-
-Figure 72. Example Node Diagram
-
-So that these loops are manageable and more clearly defined both in the input and in the simulation, four different loop sections can be defined in an EnergyPlus input file. In general, these four types are in essence two pairs of loop sections that make up  two distinct types of loops: a zone/air loop and a plant loop. As of Version 7, plant loops and condenser loops have been consolidated to be largely the same. The four loop section types are defined below.
-
-**Air Loop Supply Side:**  The air loop is defined by the section of the zone/air loop that starts after the zone return streams are combined and continues on until just before any air stream(s) are branched off to individual zones. The starting point of the air loop is fairly straightforward. The ending point is slightly more complex but can be understood with some examples. For instance, in a terminal reheat system, the end of the air loop would typically be considered the node following the cooling coil. In a dual duct system, the air loop would have two ending points that would correspond to the nodes after the cooling coil and after the heating coil/humidifier. In most cases, the air loop has a single starting point and up to two ending points (for a 2 deck system).  An outdoor air subsystem can be included in the supply side for ventilation and relief air.
-
-**Air Loop Zone Equipment:**  The zone equipment section of the input file is defined as more or less the rest of the zone/air loop (outside air is handled separately as a subset of the air loop). This includes everything from where the ducts are split to serve various zones up through where the return ducts from various zones are mixed into a single return duct. Zone equipment can include dampers and reheat coils as well as zone specific conditioning systems such as thermostatic baseboard or a window air conditioner. Most control issues are typically dealt with in the zone equipment section of the simulation.
-
-**Plant Loop Demand Side:**  One side of the plant is where energy is “demanded� by various components that make up the air loop or zone equipment. Typically, this is the water side of equipment such as coils, baseboard, radiant heating and cooling, etc. In the case of a condenser loop, energy is typically “demanded� by a chiller condenser or other water source heat pump. The demand side of this loop can also include mixers, flow splitters, and a bypass.
-
-**Plant Loop Supply Side:**  The other side of the plant loop is where energy is “supplied� by various components. The components typically found on the supply side include pumps, boilers, chillers, purchased heating and cooling, ice storage, etc. In the case of a condenser, the components would be cooling tower, fluid cooler, or ground source heat exchanger, etc.  As with the demand side, this loop can also include mixers, flow splitters, and a bypass.
-
-The section of the input file for describing the HVAC system tends to follow this structure presented above. Both plant and condenser loops are defined with a master description and then branch off into supply and demand side details. Linkage between the two sides is done using node names in the master statement. The air loop and zone equipment descriptions are slightly more complex due to the wide range of potential systems that are anticipated. Note that in every section controls become a key element and must be addressed. Each of the following sections details either a loop, a portion of a loop, or controls.
-
-Group – Node-Branch Management
-------------------------------
-
-**Nodes**, **Branch** **Lists** and **Branches** define the topography of the HVAC connections.
-
-### NodeList
-
-For convenience, the NodeList object can be used to identify all the nodes for a particular use. A node list is not always required. The advantage of listing all the nodes in this manner is that input fields in other objects that ask for a node name can refer to either a single node or a list of nodes using this object. .
-
-There are other lines of input syntax that require the use of a NodeList as part of the input. These syntax items include: OutdoorAir:NodeList and the SetpointManager objects. In these two cases, the use of a NodeList statement is mandatory if there is more than one node in this particular “list�. For example, if the outside air only has a single inlet node, then the name of that node can replace the node list name in the input syntax. As a result of this mandatory specification of node lists for certain types of input, nodes can, obviously, and may be members of more than one list.
-
-#### Field: Name
-
-This alpha designation must be unique among all the Node List Names. It is used as reference in various objects (e.g. OutdoorAir:NodeList).
-
-#### Field: Node &lt;\#&gt; Name  (up to 25 allowed)
-
-Each unique Node identifier creates a Node structure with various attributes depending on the type of node. Typical values include Temperature, Mass Flow Rate, and Temperature Set Point. The alpha designators are associated with a particular node.
-
-Though each NodeList is limited to 25 nodes, several node lists may be entered if you choose to identify all the nodes up front. For example:
-
-```
-NodeList, Nodes1-25,
-NODE_1,NODE_2,NODE_3,NODE_4,NODE_5,NODE_6,NODE_7,NODE_8,NODE_9,NODE_10,
-NODE_11,NODE_12,NODE_13,NODE_14,NODE_15,NODE_16,NODE_17,NODE_18,NODE_19,NODE_20,
-NODE_21,NODE_22,NODE_23,NODE_24,NODE_25;
-NodeList, Nodes26-49,NODE_26,NODE_27,NODE_28,NODE_29,NODE_30,
-NODE_31,NODE_32,NODE_33,NODE_34,NODE_35,NODE_36,NODE_37,NODE_38,NODE_39,NODE_40,
-NODE_41,NODE_42,NODE_43,NODE_44,NODE_45,NODE_46,NODE_47,NODE_48,NODE_49;
-```
-
-
-### Node List Outputs
-
-A simple detail of Nodes and numbers assigned appears in the **eplusout.bnd** file:
-
-```
-! <Node>,<NodeNumber>,<Node Name>,<Node Fluid Type>,<\# Times Node Referenced After Definition>
- Node,1,OUTSIDE AIR INLET NODE 1,Air,2
- Node,2,VAV SYS 1 INLET NODE,Air,3
- Node,3,MIXED AIR NODE 1,Air,5
- Node,4,MAIN COOLING COIL 1 OUTLET NODE,Air,3
- Node,5,MAIN HEATING COIL 1 OUTLET NODE,Air,4
- Node,6,VAV SYS 1 OUTLET NODE,Air,7
-```
-
-In addition, properties of each node is available during the simulation:
-
-* HVAC,Average,System Node Temperature [C]
-
-* HVAC,Average,System Node Last Timestep Temperature [C]
-
-* HVAC,Average,System Node Mass Flow Rate [kg/s]
-
-* HVAC,Average,System Node Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC,Average,System Node Setpoint Temperature [C]
-
-* HVAC,Average,System Node Setpoint High Temperature [C]
-
-* HVAC,Average,System Node Setpoint Low Temperature [C]
-
-* HVAC,Average,System Node Setpoint Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC,Average,System Node Setpoint Minimum Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC,Average,System Node Setpoint Maximum Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC,Average,System Node Relative Humidity [%]
-
-* HVAC,Average,System Node Pressure [Pa]
-
-* HVAC,Average,System Node Standard Density Volume Flow Rate [m3/s]
-
-* HVAC,Average,System Node Enthalpy [J/kg]
-
-* HVAC,Average,System Node Last Timestep Enthalpy [J/kg]
-
-* HVAC,Average,System Node Wetbulb Temperature [C]
-
-* HVAC,Average,System Node Dewpoint Temperature [C]
-
-* HVAC,Average,System Node Quality []
-
-* HVAC,Average,System Node Height [m]
-
-* HVAC,Average,System Node Specific Heat [J/kg-K]
-
-**The following node variable is also available for system nodes that are for “air�:**
-
-* HVAC, Average, System Node Current Density Volume Flow Rate [m3/s]
-
-* HVAC, Average, System Node Current Density [kg/m3]
-
-
-**The following node variables are “advanced� and normally used for debugging unusual cases:**
-
-* HVAC,Average,System Node Minimum Temperature [C]
-
-* HVAC,Average,System Node Maximum Temperature [C]
-
-* HVAC,Average,System Node Minimum Limit Mass Flow Rate [kg/s]
-
-* HVAC,Average,System Node Maximum Limit Mass Flow Rate [kg/s]
-
-* HVAC,Average,System Node Minimum Available Mass Flow Rate [kg/s]
-
-* HVAC,Average,System Node Maximum Available Mass Flow Rate [kg/s]
-
-* HVAC,Averge,System Node Requested Mass Flow Rate [kg/s]
-
-* HVAC,Average,System Node Setpoint Mass Flow Rate [kg/s]
-
-
-**The following node variable reports node carbon dioxide concentration when carbon dioxide is simulated (ref. ZoneAirContaminantBalance):**
-
-* HVAC,Average,System Node CO2 Concentration [ppm]
-
-
-**The following node variable reports node generic contaminant concentration when generic contaminant is simulated (ref. ZoneAirContaminantBalance):**
-
-* HVAC,Average,System Node Generic Air Contaminant Concentration [ppm]
-
-
-#### System Node Temperature [C]
-
-The current temperature at a system node in degrees C. For air nodes, this is the dry-bulb temperature.
-
-#### System Node Last Timestep Temperature [C]
-
-The temperature at a system node for the previous timestep.
-
-#### System Node Mass Flow Rate [kg/s]
-
-The current mass flow rate at a system node in kg/s.
-
-#### System Node Humidity Ratio [kgWater/kgDryAir]
-
-The current humidity ratio at a system node in kg-water/kg-dry-air. Not applicable for liquid nodes.
-
-#### System Node Setpoint Temperature [C]
-
-The current setpoint temperature at a system node in degrees C. Some controllers and equipment types sense this single setpoint.
-
-#### System Node Setpoint High Temperature [C]
-
-The current upper setpoint temperature at a system node in degrees C. Some controllers and equipment types use dual setpoints at a single node.
-
-#### System Node Setpoint Low Temperature [C]
-
-The current upper setpoint temperature at a system node in degrees C. Some controllers and equipment types use dual setpoints at a single node.
-
-#### System Node Setpoint Humidity Ratio [kgWater/kgDryAir]
-
-The current humidity ratio setpoint at a system node in kg-water/kg-dry-air. Some controllers and equipment types sense this single setpoint. Not applicable for liquid nodes.
-
-#### System Node Setpoint Minimum Humidity Ratio [kgWater/kgDryAir]
-
-The current minimum desired humidity ratio at a system node in kg-water/kg-dry-air. Some controllers and equipment types use the min/max values as dual setpoints at a single node. Not applicable for liquid nodes.
-
-#### System Node Setpoint Maximum Humidity Ratio [kgWater/kgDryAir]
-
-The current maximum desired humidity ratio at a system node in kg-water/kg-dry-air. Some controllers and equipment types use the min/max values as dual setpoints at a single node. Not applicable for liquid nodes.
-
-#### System Node Relative Humidity [%]
-
-The current relative humidity (calculated from the node temperature, node humidity ratio and standard barometric pressure for the location). Not applicable for liquid nodes.
-
-#### System Node Pressure [Pa]
-
-The current pressure at a system node in Pa.
-
-#### System Node Standard Density Volume Flow Rate [m<sup>3</sup>/s]
-
-The current volume flow rate at a system node in m<sup>3</sup>/s.  This is report is calculated from the mass flow using standardized values for density that do not vary over time (except for steam which varies with quality).  For water nodes this density is determined at a temperature of 5.05ºC.  For air nodes this density is determined for dry air at the standard barometric pressure for the location’s elevation, and a temperature of 20.0ºC.  For air nodes, also see the report “System Node Current Density Volume Flow Rate.�
-
-#### System Node Enthalpy [J/kg]
-
-The current enthalpy at a system node in J/kg.
-
-#### System Node Last Timestep Enthalpy [J/kg]
-
-The enthalpy at the system node for the previous timestep in Joules per kilogram.
-
-#### System Node Wetbulb Temperature [C]
-
-The current wet-bulb temperature at a system node in degrees C. Not applicable for liquid nodes.
-
-#### System Node Dewpoint Temperature [C]
-
-The current dewpoint temperature at a system node in degrees C. It is calculated from the System Node Temperature, the System Node Humidity Ratio and the Site Outdoor Air Barometric Pressure. Not applicable for liquid nodes.
-
-#### System Node Quality []
-
-The current system node vapor fraction/percent {0.0-1.0}.
-
-#### System Node Height [m]
-
-The current system node height {m}. Only applicable to outdoor air nodes.
-
-#### System Node Specific Heat [J/kg-K]
-
-The current specific heat capacity of the fluid at the node in units of J/kg-K.  Not available for steam nodes. 
-
-**Additional Node Reporting for Air Nodes**
-
-The following system node variable is available for nodes with a fluid type of air.
-
-#### System Node Current Density Volume Flow Rate [m<sup>3</sup>/s]
-
-The current volume flow rate at a system node in m<sup>3</sup>/s based on the current density.  This report differs from the one called “System Node Standard Density Volume Flow Rate� in that it uses an air density calculated for the current moist air conditions rather than a standard density.
-
-#### System Node Current Density [kg/m3]
-
-The current air density at a system node in kg/m3.  This is the density used to calculate the volume flow rate above.  The density is calculated using current outdoor air barometric pressure and the drybulb temperature and humidity ratio at the air node.
-
-**Advanced Node Reporting**
-
-The following system node variables are available when you request “Diagnostics, DisplayAdvancedReportVariable;�. They are normally used for debugging unusual system cases and may not be available for all systems. Also, their definitions may change based on the usage in the system.
-
-#### System Node Minimum Temperature [C]
-
-#### System Node Maximum Temperature [C]
-
-These node variables represent the min/max of loops or branches.
-
-#### System Node Minimum Limit Mass Flow Rate [kg/s]
-
-#### System Node Maximum Limit Mass Flow Rate [kg/s]
-
-These node variables hold the maximum possible and the minimum allowable flow rates for a particular component. As such, they represent the “hardware limit� on the flow rate for the component. By convention, these variables are stored at the component inlet node. Since components share their nodes (the outlet node of one component is the inlet node of the next component), the protocol must be strictly followed. These variables are set by each component based on the design flow limits of the equipment.
-
-#### System Node Minimum Available Mass Flow Rate [kg/s]
-
-#### System Node Maximum Available Mass Flow Rate [kg/s]
-
-These node variables represent the *loop* or *branch* maximum and minimum flow rate for the current configuration of the loop on which the component resides. The central plant routines manage these variables dynamically to resolve flow rates through branches located inside splitters and mixers.
-
-#### System Node Setpoint Mass Flow Rate [kg/s]
-
-The current mass flow rate setpoint at a system node in kg/s. Some controllers and equipment types sense this single setpoint.
-
-#### System Node Requested Mass Flow Rate [kg/s]
-
-This output is the current mass flow rate request at a system node in kg/s.  Only used for plant simulations and nodes.  This is the mass flow rate “requested� by a component.  This is a record of what the component wanted which can be useful for diagnostics when the actual simulated flow is different than expected.  This value is also used to determine overall loop flow rates.
-
-#### System Node CO2 Concentration [ppm]
-
-The average carbon dioxide concentration, in parts per million (ppm), at a system node for the timestep being reported.
-
-#### System Node Generic Air Contaminant Concentration [ppm]
-
-The average generic contaminant concentration, in parts per million (ppm), at a system node for the timestep being reported.
-
-### BranchList
-
-A branch list is intended to define the branches or portions of a particular loop that are present on an individual plant or condenser loop. Thus, the BranchList syntax simply provides a list of branch names (see Branch syntax) that then refer to more detailed syntax in another part of the input file. The syntax for describing a list of branches is given below.
-
-Branches in BranchList objects should be listed in flow order: inlet branch, then parallel branches, then outlet branch. Branches (within a splitter/mixer) are simulated in the order listed.
-
-#### Field: Name
-
-A unique name to identify the branch list.
-
-#### Field: Branch &lt;\#&gt; Name
-
-Branch name in the list.  As noted above, Branches in BranchList objects MUST be listed in flow order: inlet branch, then parallel branches, then outlet branch. Branches are simulated in the order listed.
-
-An example of this statement in an IDF is:
-
-```idf
-BranchList, Cooling Supply Side Branches,
-     CW Pump Branch,
-     Little Chiller Branch,
-     Big Chiller Branch,
-     Purchased Cooling Branch,
-     Supply Bypass Branch,
-     Cooling Supply Outlet;
-```
-
-### Branch List Output
-
-No output directly related to Branch Lists current is presented.
-
-### Branch
-
-Branches can be considered the mid-level grouping of items in the EnergyPlus HVAC loop scheme. Components are the lowest level of information. A collection of components in series forms a branch. Every branch must have at least one component, but it may have several components in series. The air loop also has “unitary� objects that are compound objects that wrap components and when they are used it is the unitary objects that appear on the Branch and not the child components.  The **Branch** defines the order that components appear on the branch. Moreover, a collection of branches and their connecting information form a loop. Therefore, a branch is a collection of components while a loop is a collection of branches. Thus, components are specified for particular HVAC loops by assigning them to branches and then connecting those branches together to form a loop.
-
-For hydronic plant systems, the Branch object is used on both the demand side and the supply side of the plant loop.  For HVAC air systems, the Branch object is only used to describe the components on the supply side of an air loop. The demand side of the air loop does not use the Branch object.  The outside air system appears on a Branch object but it does not use a Branch object itself to describe the components that included in the outside air system.  So-called “ZoneHVAC:\*� equipment, HVAC equipment directly associated with a zone, do not use the Branch object.
-
-It should be noted that each component also has at least two nodes associated with it—an inlet node and an outlet node. These nodes, by default, are also part of the branch to which their components are assigned.  Although it may appear redundant to list the node names in both the Branch and in the component object being referenced, this is needed because many components are connected to more than one loop at a time and the node names are needed here to distinguish which portion of the component is being attached to this particular branch and its loop.  It should be noted that each branch must have at least one component on it. A “null� branch such as one where the first component on the loop is in reality a splitter or mixer should be defined as a single Pipe component for plant, or a single Duct component for air systems.
-
-#### Field: Name
-
-This alpha field is the unique, user-defined name that allows the branch to be referenced by other elements such as the PlantLoop and CondenserLoop statements.
-
-#### Field: Maximum Flow Rate
-
-This field is the maximum flow rate (m<sup>3</sup>/sec) allowed on a particular branch. This number will set an absolute maximum flow rate for all components on the loop. Even if components are defined with a higher flow rate, EnergyPlus will limit the flow on this particular branch to the value entered here by the user. Currently this is used in the Air Loop and is not a required field in the Plant and Condenser Loop. The example files for the Plant and Condenser Loops leave this field blank to simplify flow input.
-
-#### Field: Pressure Drop Curve Name
-
-This is an optional field used to specify pressure drop information for this particular branch. Currently this is only available in plant/condenser fluid loops: PlantLoop and CondenserLoop. Air loops require a full airflow network, so this field is ignored if found on an air loop. The value entered for this field must match a pressure curve object also found in the input. This curve can be of the type: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Exponent, or Curve:Functional:PressureDrop. In order to then perform a pressure simulation for the loop that this branch is located on, a flag must be set in the loop object. Reference the PlantLoop and CondenserLoop field “Pressure Simulation Type� for allowable settings. See the Engineering Reference document for further information on pressure simulation in plant loops.
-
-#### Field Set (Branch Specifications)
-
-Following the two introductory items, there are groups of 5 repeated items: a type, a name, inlet and outlet node names, and a branch control type. All of these items refer to one particular component on the branch. The first component defined by these items will be the first component on this branch, etc. through the end of the list.  This object is extensible and can use as many field sets as needed.
-
-#### Field: Component &lt;\#&gt; Object Type
-
-This field is the component object type (object class name). The component type refers to other elements within the input file and specifies what kind of component this is. The objects in the  Group – Plant Equipment section are valid here when the Branch is used in Plant specifications. Fans, coils, unitary systems, and Outside Air Systems are also valid component types for the Branch object. Pipes or Ducts are also valid for this field.  No splitter or mixer type objects are allowed.
-
-#### Field: Component &lt;\#&gt; Name
-
-The component name is the unique, user-defined reference name to distinguish between potentially multiple occurrences of a particular component type in an input file. The set of component type and component name must be unique. (You can only have 1 Boiler object with name MYBOILER).
-
-#### Field: Component &lt;\#&gt; Inlet Node Name
-
-This field references an inlet node name that will be found in the actual component specification.  The inlet node, and the outlet node specified in the next field, should correspond to component model’s connections that are intended for the loop that this Branch is assigned to.  For example a water-cooled chiller will have two inlet nodes, one for chilled water return and one for condenser water return and so the chiller will appear on two Branch objects accordingly.
-
-#### Field: Component &lt;\#&gt; Outlet Node Name
-
-This field references an outlet node name that will be found in the actual component specification.
-
-#### Field: Component &lt;\#&gt; Branch Control Type
-
-This field is being deprecated and is no longer used or required. Prior to version 7 it was used by plant to resolve branch flow rates but now this is handled automatically by the program.  The field will be removed in a future version.
-
-An example of this statement in an IDF is:
-
-```idf
-Branch,
-    Air Loop Main Branch,    !- Branch Name
-    1.75,                    !- Maximum Branch Flow Rate {m3/s}
-    ,                        !- Pressure Drop Curve Name
-    AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass,  !- Comp1 Type
-    GasHeat CBVAV System,    !- Comp1 Name
-    Air Loop Inlet Node,     !- Comp1 Inlet Node Name
-    Air Loop Outlet Node,    !- Comp1 Outlet Node Name
-    ;                  !- Comp1 Branch Control Type
-```
-
-
-And a more complex one:
-
-```idf
-  BRANCH,
-    Air Loop Main Branch,    !- Branch Name
-    1.3,                     !- Maximum Branch Flow Rate {m3/s}
-    ,                        !- Pressure Drop Curve Name
-    FAN:SIMPLE:ConstVolume,  !- Comp1 Type
-    Supply Fan 1,            !- Comp1 Name
-    Air Loop Inlet Node,     !- Comp1 Inlet Node Name
-    Cooling Coil Air Inlet Node,  !- Comp1 Outlet Node Name
-    ,                  !- Comp1 Branch Control Type
-    COIL:Water:DetailedFlatCooling,  !- Comp2 Type
-    Detailed Cooling Coil,   !- Comp2 Name
-    Cooling Coil Air Inlet Node,  !- Comp2 Inlet Node Name
-    Air Loop Outlet Node,    !- Comp2 Outlet Node Name
-    ;                 !- Comp2 Branch Control Type
-```
-
-
-### Branch Output
-
-The components on a branch are in series and that list is in simulation and connection order. Each branch must obey the rules: the outlet for component 1 has to have the same node name as the inlet for component 2, and so forth.
-
-Eplusout.err contains the test for “individual branch integrity�:
-
-```
-   ************* Testing Individual Branch Integrity
-   ************* Testing Branch=AIR LOOP MAIN BRANCH
-   ************* ....passed
-   ************* Testing Branch=COOLING DEMAND INLET
-   ************* ....passed
-   ************* Testing Branch=COOLING COIL BRANCH
-   ************* ....passed
-   ************* Testing Branch=DEMAND BYPASS BRANCH
-   ************* ....passed
-   ************* Testing Branch=COOLING DEMAND OUTLET
-   ************* ....passed
-   ************* Testing Branch=COOLING SUPPLY OUTLET
-   ************* ....passed
-```
-
-The addition of pressure simulation for branches in fluid loops brings a new output at the branch level:
-
-* HVAC,Average,Plant Branch Pressure Difference [Pa]
-
-#### Plant Branch Pressure Difference [Pa]
-
-This field allows the user to output the pressure drop of a particular branch on a plant loop or condenser loop. This output is only recognized if a valid pressure simulation is being performed. To do this, the user must specify a pressure simulation type as an input in the PlantLoop or CondenserLoop object.
-
-### ConnectorList
-
-A connector list is a collection of either one or two connection devices (Connector:Mixer or Connector:Splitter). Due to the definition of a loop in EnergyPlus, there is a maximum of one mixer and one splitter allowed for each loop segment. This limitation still allows a tremendous amount of flexibility to the user and can also still be solved within a reasonable amount of time and without a complex solver routine. The connection list simply allows the specification of the types and names of these devices. This allows the main loop statements to have the flexibility to have multiple lists that can have one or more item.
-
-#### Field: Name
-
-This field is an identifying name that will be referenced to main loop statements using this connector list. The name must be unique among connector list names.
-
-#### Field-Set: Connection Object Type and Identifying Name (up to 2 allowed)
-
-Depending on the loop, either one or two of the connectors will be specified. If this particular loop only has a single connector (either Connector:Mixer or Connector:Splitter), then only the first two items (type of connection and identifying name of connector) are included. If both a mixer and splitter are present, the additional type of connection and identifying name must be included. Note that the order that the items appear is inconsequential—either the Connector:Mixer or the Connector:Splitter may appear first. This will not affect the simulation.
-
-#### Field: Connector 1 Object Type
-
-This field contains the connector type **Connector:Mixer** or **Connector:Splitter**.
-
-#### Field: Connector 1 Name
-
-This field is an identifying name for the connector. It will be used by other objects in the input file.
-
-#### Field: Connector 2 Object Type (optional)
-
-This field contains the connector type **Connector:Mixer** or **Connector:Splitter**.
-
-#### Field: Connector 2 Name (optional)
-
-This field is an identifying name for the connector. It will be used by other objects in the input file.
-
-An example of this statement in an IDF is:
-
-```idf
-ConnectorList LIST, Cooling Supply Side Connectors,
-    Connector:Splitter, CW Loop Splitter,
-    Connector:Mixer, CW Loop Mixer;
-```
-
-### Connector List Outputs
-
-No output directly related to Connector Lists is currently presented.
-
-### Pipe:Adiabatic
-
-In reality, every component is connected to its closest neighbors via a pipe or a duct. At the current time, such detail is not needed in EnergyPlus. Thus, the Pipe:Adiabatic component is currently used more as a connection device (for branches that really do not have any components associated with them) or as a bypass than anything else. As such, its input is very simple and its algorithm is equally simple. The current algorithm for a pipe is simply to pass the inlet conditions to the outlet of the pipe component.
-
-#### Field: Name
-
-This alpha field is used as an identifying field for the pipe.
-
-#### Field: Inlet Node Name
-
-This alpha field is used as an identifying field for the pipe inlet node.
-
-#### Field: Outlet Node Name
-
-This alpha field is used as an identifying field for the pipe outlet node.
-
-An example of this statement in an IDF is:
-
-```idf
-Pipe:Adiabatic,
-    Demand Side Inlet Pipe,
-    CW Demand Inlet Node,
-    CW Demand Entrance Pipe Outlet Node;
-```
-
-### Pipe Outputs
-
-There are no outputs directly related to Pipes.
-
-### Pipe:Adiabatic:Steam
-
-To connect the various components in a steam system regardless of it being the condensate or the steam side of the loop steam pipe needs to be used. In reality, every component is connected to its closest neighbors via a pipe or a duct. At the current time, such detail is not needed in EnergyPlus. Thus, the Pipe:Adiabatic:Steam component is currently used more as a connection device (for branches that really do not have any components associated with them). As such, its input is very simple and its algorithm is equally simple. The current algorithm for a pipe is simply to pass the inlet conditions to the outlet of the pipe component.
-
-#### Field: Name
-
-This alpha field is used as an identifying field for the steam pipe.
-
-#### Field: Inlet Node Name
-
-This alpha field is used as an identifying field for the steam pipe inlet node.
-
-#### Field: Outlet Node Name
-
-This alpha field is used as an identifying field for the steampipe outlet node.
-
-An example of this statement in an IDF is:
-
-```idf
-Pipe:Adiabatic:Steam,
-    Steam Demand 1 Steam Inlet Pipe,            !- PipeName
-    Steam Demand 1 Steam Demand Inlet Node,     !- Inlet Node Name
-    Steam Demand 1 Steam Demand Entrance Pipe Outlet Node;  !- Outlet Node Name
-```
-
-
-### Steam Pipe Outputs
-
-There are no outputs directly related to Steam Pipes.
-
-### Pipe:Indoor
-
-This object specifies inputs which are used to simulate the heat transfer from a plant loop pipe placed in a zone or when a user schedule is used to specify an environment.
-
-The data definition for object is shown below.
-
-#### Field: Name
-
-This alpha field is used as an identifying field for the pipe.
-
-#### Field: Construction Name
-
-This alpha field references a 'wall' construction object that gives a layer-by-layer description of the pipe wall and its insulation.  The construction object follows standard conventions, describing material properties for each layer beginning with the outermost insulation layer and ending with the pipe wall layer.
-
-#### Field: Fluid Inlet Node Name
-
-This alpha field contains the name of the pipe fluid inlet node.
-
-#### Field: Fluid Outlet Node Name
-
-This alpha field contains the name of the pipe fluid outlet node.
-
-#### Field: Environment Type
-
-Environment type is the environment in which the pipe is placed. It can be either **Zone** or **Schedule**. If specified as Zone, a zone name must be specified in the next field. If specified as Schedule, the Ambient Temperature Zone can be left blank, while a schedule must be specified for the temperature and air velocity.
-
-#### Field: Ambient Temperature Zone Name
-
-If **Zone** is specified as the environment type, this field is used to specify the name of the zone in which the pipe is located.  The zone temperature is used to calculate the heat transfer rate from the pipe.
-
-#### Field: Ambient Temperature Schedule Name
-
-If **Schedule** is specified as the environment type, this field is used to specify the name of the temperature schedule that gives the ambient air temperature surrounding the pipe.  This temperature is used as the outside boundary condition to calculate heat transfer from the pipe.
-
-#### Field: Ambient Air Velocity Schedule Name
-
-If **Schedule** is specified as the environment type, this field is used to specify the name of the velocity schedule that gives the air velocity near the pipe.  This velocity is used to calculate the convection heat transfer coefficient used in the pipe heat transfer calculation.
-
-#### Field: Pipe Inside Diameter
-
-This field is used to enter the inside diameter of the pipe in units of m. Pipe inside diameter must be a positive number.
-
-#### Field: Pipe Length
-
-This field is used to enter the length of the pipe in units of m. Pipe length must be a positive number.
-
-An example of this object in an IDF is:
-
-```idf
-Pipe:Indoor,
-    Pipe Heat Transfer Towers,    !- name of outside panel heat exchanger
-    Insulated Pipe,                      !- Construction name
-    Condenser Tower Outlet Node,  !- Comp1 Inlet Node Name
-    HTPipe Outlet Node,           !- Comp1 Outlet Node Name
-    Water,                               !- Fluid name
-    Zone,                         !- field Ambient Temperature Outside Air Node name
-    0.05,                                !- Pipe Inside Diameter (thickness in construction data)
-    100.0;                               !- pipe length
-```
-
-
-### Pipe:Indoor Outputs
-
-* HVAC,Average, Pipe Fluid Heat Transfer Rate [W]
-
-* HVAC,Average, Pipe Ambient Heat Transfer Rate [W]
-
-* HVAC,SUM, Pipe Fluid Heat Transfer Energy [J]
-
-* HVAC,SUM, Pipe Ambient Heat Transfer Energy [J]
-
-* HVAC,Average, Pipe Mass Flow Rate [kg/s]
-
-* HVAC,Average, Pipe Inlet Temperature [C]
-
-* HVAC,Average, Pipe Outlet Temperature [C]
-
-* HVAC,Average, Pipe Volume Flow Rate [m3/s]
-
-
-#### Pipe Fluid Heat Transfer Rate [W]
-
-The output provides the total amount of heat loss/gain in the fluid from pipe inlet to outlet.
-
-#### Pipe Ambient Heat Transfer Rate [W]
-
-The output provides the amount of heat loss/gain from pipe wall to the environment.
-
-#### Pipe Fluid Heat Transfer Energy [J]
-
-Total energy fluid has lost/gained between pipe inlet and outlet. It is metered on EnergyTransfer with an end use of Pipes.
-
-#### Pipe Ambient Heat Transfer Energy [J]
-
-Total energy lost from the external pipe surface.
-
-#### Pipe Mass Flow Rate [kg/s]
-
-Mass flow rate of the fluid in the pipe.
-
-#### Pipe Inlet Temperature [C]
-
-#### Pipe Outlet Temperature [C]
-
-Temperature of fluid at entering and exiting of pipe.
-
-#### Pipe Volume Flow Rate [m3/s]
-
-Fluid volumetric flow rate, (mass flow rate / density)
-
-### Pipe:Outdoor
-
-This object specifies inputs which are used to simulate the heat transfer from a plant loop pipe placed in an outdoor environment.
-
-#### Field: Name
-
-This alpha field is used as an identifying field for the pipe.
-
-#### Field: Construction Name
-
-This alpha field references a 'wall' construction object that gives a layer-by-layer description of the pipe wall and its insulation.  The construction object follows standard conventions, describing material properties for each layer beginning with the outermost insulation layer and ending with the pipe wall layer.
-
-#### Field: Fluid Inlet Node Name
-
-This alpha field contains the name of the pipe fluid inlet node.
-
-#### Field: Fluid Outlet Node Name
-
-This alpha field contains the name of the pipe fluid outlet node.
-
-#### Field: Ambient Temperature Outside Air Node Name
-
-Ambient temperature outdoor air node is a node representing outdoor air with which pipe transfers heat. The node should be included in an outdoor air node list.
-
-#### Field: Pipe Inside Diameter
-
-This field is used to enter the inside diameter of the pipe in units of m. Pipe inside diameter must be a positive quantity.
-
-#### Field: Pipe Length
-
-This field is used to enter the length of the pipe in units of m. Pipe length must be a positive   quantity.
-
-An example of this statement in an IDF is:
-
-```idf
-Pipe:Outdoor,
-    Pipe Heat Transfer Towers,    !- name of outside panel heat exchanger
-    Insulated Pipe,                      !- Construction name
-    Condenser Tower Outlet Node, !- Comp1 Inlet Node Name
-    HTPipe Outlet Node,           !- Comp1 Outlet Node Name
-    Water,                               !- Fluid name
-    PipeHeatTransfer Inlet Node,     !- field Ambient Temperature Outside Air Node name
-    0.05,                         !- Pipe Inside Diameter (thickness given in construction data)
-    100.0;                               !- pipe length
-```
-
-
-### Pipe:Outdoor Outputs
-
-* HVAC,Average, Pipe Fluid Heat Transfer Rate [W]
-
-* HVAC,SUM, Pipe Fluid Heat Transfer Energy [J]
-
-* HVAC,Average, Pipe Mass Flow Rate [kg/s]
-
-* HVAC,Average, Pipe Inlet Temperature [T]
-
-* HVAC,Average, Pipe Outlet Temperature [T]
-
-* HVAC,Average, Pipe Volume Flow Rate [m3/s]
-
-
-#### Pipe Fluid Heat Transfer Rate [W]
-
-The output provides the total amount of heat loss/gain in the fluid from pipe inlet to outlet.
-
-#### Pipe Fluid Heat Transfer Energy [J]
-
-Total energy fluid has lost/gained between pipe inlet and outlet. It is metered on EnergyTransfer with an end use of Pipes.
-
-#### Pipe Mass Flow Rate [kg/s]
-
-Mass flow rate of the fluid in the pipe.
-
-#### Pipe Inlet Temperature [C]
-
-#### Pipe Outlet Temperature [C]
-
-Temperature of fluid at entering and exiting of pipe.
-
-#### Pipe Volume Flow Rate [m3/s]
-
-Fluid volumetric flow rate, (mass flow rate / density)
-
-### Pipe:Underground
-
-This object specifies inputs which are used to simulate the heat transfer from a plant loop pipe placed underground.
-
-#### Field: Name
-
-This alpha field is used as an identifying field for the pipe.
-
-#### Field: Construction Name
-
- This alpha field references a basic construction object that gives a layer-by-layer description of the pipe wall and insulation. The construction object follows standard conventions, describing material properties for each layer beginning with the outermost layer, the insulation, if it exists, and ending with the pipe wall layer.  The construction object may have either one or two layers.  If only one, then the material must be the pipe wall.  If two, then insulation is utilized.
-
-#### Field: Fluid Inlet Node Name
-
- This alpha field contains the name of the pipe fluid inlet node.
-
-#### Field: Fluid Outlet Node Name
-
- This alpha field contains the name of the pipe fluid outlet node.
-
-#### Field: Sun Exposure
-
- This alpha field allows the user to specify one of two options: NoSun or SunExposed.  For SunExposed, the simulation includes diffuse and beam solar effects on the ground surface.  For NoSun, no solar effects are included.
-
-#### Field: Pipe Inside Diameter
-
- This field is used to enter the inside diameter of the pipe in units of m. Pipe inside diameter must be a positive quantity.
-
-#### Field: Pipe Length
-
- This field is used to enter the length of the pipe in units of {m}. Pipe length must be a positive quantity.
-
-#### Field: Soil Material Name
-
-This references a Material object that contains the soil properties and thickness.  Note that when defining the soil layer, the thickness should be the thickness of soil between the pipe wall and the ground surface.
-
-#### Field: Type of Undisturbed Ground Temperature Object
-
-This is the type of undisturbed ground temperature object that is used to determine the ground temperature.
-
-#### Field: Name of Undisturbed Ground Temperature Object
-
-This is the name of the undisturbed ground temperature object that is used to determine the ground temperature.
-
-An example of this object in an IDF is:
-
-```idf
-Pipe:Underground,
-    Pipe Heat Transfer Towers,          !- Name of Pipe
-    Insulated Buried Pipe,              !- Construction Name
-    Condenser Tower Outlet Node,        !- Inlet Node Name
-    HTPipe Outlet Node,                 !- Outlet Node Name
-    Water,                              !- Fluid Name
-    SunExposed,                         !- Sun Exposure
-    0.05,                               !- Pipe Inside Diameter    
-    20.0,                               !- Pipe Length
-    Buried Pipe Soil,                   !- Soil Material
-    Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
-    KATemps;                            !- Name of Undisturbed Ground Temperature Object
-
-  Construction,
-    Insulated Buried Pipe,              !- Name
-    Buried Pipe Insulation,             !- Layer #1
-    Buried Pipe Steel;                  !- Layer #2
-
-  Material,
-    Buried Pipe Soil,                   !- Name
-    Smooth,                             !- Roughness
-    1.5,                                !- Thickness {m}
-    0.36,                               !- Conductivity {W/m-K}
-    2000.0,                             !- Density {kg/m3}
-    1200.0,                             !- Specific Heat {J/kg-K}
-    0.9,                                !- Thermal Absorptance
-    0.5,                                !- Solar Absorptance
-    0.5;                                !- Visible Absorptance
-```
-
-### Pipe:Underground Outputs
-
-* HVAC, Average, Pipe Fluid Heat Transfer Rate [W]
-
-* HVAC, SUM, Pipe Fluid Heat Transfer Energy [J]
-
-* HVAC, Average, Pipe Mass Flow Rate [kg/s]
-
-* HVAC, Average, Pipe Volume Flow Rate [m3/s]
-
-* HVAC, Average, Pipe Inlet Temperature [C]
-
-* HVAC, Average, Pipe Outlet Temperature [C]
-
-#### Pipe Fluid Heat Transfer Rate [W]
-
-The output provides the total amount of heat loss/gain in the fluid from pipe inlet to outlet.
-
-#### Pipe Fluid Heat Transfer Energy [J]
-
-Total energy fluid has lost/gained between pipe inlet and outlet. It is metered on
-
-EnergyTransfer with an end use of Pipes.
-
-#### Pipe Mass Flow Rate [kg/s]
-
- Mass flow rate of the fluid in the pipe.
-
-#### Pipe Volume Flow Rate [m3/s]
-
-Fluid volumetric flow rate, (mass flow rate / density)
-
-#### Pipe Inlet Temperature [C]
-
-#### Pipe Outlet Temperature [C]
-
-Temperature of fluid at entrance and exit of pipe.
-
-### PipingSystem:Underground Class Objects
-
-Objects in this class are used to simulate the heat transfer processes of a piping system placed underground, which may or may not be in contact with a number of zone surfaces.  There are three related objects, all of which are prefixed with PipingSystem:Underground :
-
-- PipingSystem:Underground:Domain
-
-- PipingSystem:Underground:PipeCircuit
-
-- PipingSystem:Underground:PipeSegment
-
-### PipingSystem:Underground:Domain
-
-This section documents the domain object, which is used to specify information for the overall ground domain, including thermal properties, mesh parameters, and surface interaction.
-
-#### Field: Name
-
-This alpha field is used as an identifying field for the ground domain.
-
-#### Field: XMax, YMax, ZMax
-
-These numeric fields are used to specify the overall domain size, in each of the three Cartesian dimensions.  The domain will be meshed from {x, y, z} = {0, 0, 0} to {Xmax, Ymax, Zmax}.
-
-Note that for this object, the x-z plane lies parallel to the ground surface, such that the y-dimension can be thought of as representing the burial depth.  This is in contrast to the way building surface coordinates are defined with the x-y plane lying parallel to the ground.  Also note that any pipe segments that end up being used in a ground domain will be placed axially in the z-dimension.  Thus, pipe flow will always be in either the positive z or negative z direction.
-
-#### Field: X-Direction Mesh Density Parameter
-
-This numeric integer field represents the number of cells to be placed between any two “domain partitions� during mesh development.  A domain partition may be thought of as a basement wall/floor, or a pipe.  Once these components are laid out in the domain, this field number of cells are placed between the partitions.  Further information on this is found in the engineering reference manual.
-
-#### Field: X-Direction Mesh Type
-
-This alpha field represents the type of mesh to create when placing cells between “domain partitions.�  Two options are available: “uniform� and “symmetricgeometric.�  For uniform, the cells are placed in the region with all cells having equal size.  For symmetric-geometric, the cells are compressed toward the partitions so that there are more cells on either side of the mesh region.  This can help focus computational intensity on the boundary areas where it is likely more desired.  For symmetric-geometric mesh distribution, the mesh density parameter should be an even number to provide the symmetric condition.
-
-#### Field: X-Direction Geometric Coefficient
-
-This numeric field represents the compression of cell distribution if the x-direction mesh type is set to “symmetricgeometric.�  If the mesh type is uniform, this field is not interpreted.  For symmetric geometric, a value in this field equal to 1 would result in a uniform distribution, while a value of 2 would provide a highly skewed distribution.
-
-#### Field: Y-Direction Mesh Density Parameter
-
-See Field: X-Direction Mesh Density Parameter.
-
-#### Field: Y-Direction Mesh Type
-
-See Field: X-Direction Mesh Type.
-
-#### Field: Y-Direction Geometric Coefficient
-
-See Field: X-Direction Geometric Coefficient.
-
-#### Field: Z-Direction Mesh Density Parameter
-
-See Field: X-Direction Mesh Density Parameter.
-
-#### Field: Z-Direction Mesh Type
-
-See Field: X-Direction Mesh Type.
-
-#### Field: Z-Direction Geometric Coefficient
-
-See Field: X-Direction Geometric Coefficient.
-
-#### Field: Soil Thermal Conductivity
-
-The thermal conductivity of the soil, in W/m-K.
-
-#### Field: Soil Density
-
-The bulk density of the soil, in kg/m3.
-
-#### Field: Soil Specific Heat
-
-The specific heat of dry soil, in J/kg-K.  If moisture is defined in this object, moisture and freezing effects are accounted for by varying the specific heat value.
-
-#### Field: Soil Moisture Content Volume Fraction
-
-A nominal value of soil moisture content to be used when evaluating soil thermal properties.
-
-#### Field: Soil Moisture Content Volume Fraction at Saturation
-
-A nominal value of soil moisture content when the soil is saturated, this is used in evaluating thermal properties of freezing soil
-
-#### Field: Type of Undisturbed Ground Temperature Object
-
-The type of undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
-
-#### Field: Name of Undisturbed Ground Temperature Object
-
-The name of the undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
-
-#### Field: This Domain Includes Basement Surface Interaction
-
-A yes/no field stating whether zone surfaces should be coupled to this domain.
-
-#### Field: Width of Basement Floor in Ground Domain
-
-If this domain does include basement interaction, this represents the width of the domain cutaway to include the basement.  In essence, this is the width of basement floor to include in the ground simulation.  This width should *include* the basement wall thickness.
-
-#### Field: Width of Basement Floor in Ground Domain
-
-If this domain does include basement interaction, this represents the depth of the domain cutaway to include the basement.  In essence, this is the burial depth of the basement to include in the ground simulation.  This depth should include the basement floor thickness.
-
-#### Field: Shift Pipe X Coordinates By Basement Width
-
-If this domain does include basement interaction, this flag specifies whether the pipe segment X-values should then be shifted by the basement width.  In essence, this specifies the reference point for pipe segment x-values: if NO then the reference is domain x=0, if YES then the reference is the basement width point.
-
-#### Field: Name of Basement Wall Boundary Condition Model
-
-The name of an OtherSideConditions model defined in the input file and referenced by the surfaces which should be included as “wall surfaces� for the basement interaction part of the ground heat transfer model.
-
-#### Field: Name of Basement Wall Boundary Condition Model
-
-The name of an OtherSideConditions model defined in the input file and referenced by the surfaces which should be included as “floor surfaces� for the basement interaction part of the ground heat transfer model.
-
-#### Field: Convergence Criterion for the Outer Cartesian Domain Iteration Loop
-
-The maximum temperature deviation within any cell between one iteration and another to decide that the Cartesian domain has converged to within tolerance.  A smaller value will improve accuracy and computation time.  A smaller value should be accompanied by a higher number of iterations if maximum accuracy is desired.
-
-#### Field: Maximum Iterations in the Outer Cartesian Domain Iteration Loop
-
-The maximum number of iterations to make when performing temperature updates of the Cartesian coordinate system.  The actual number of iterations made will of course depend on transient conditions and convergence tolerance.
-
-#### Field: Evapotranspiration Ground Cover Parameter
-Numeric field specifies the ground cover effects used in the evapotranspiration model at the ground surface heat balance. The values range from 0 (solid, nonpermeable ground surface) to 1.5 (wild growth).
-
-#### Field: Number of Pipe Circuits Entered for this Domain
-
-The number of pipe circuit objects which will be defined in the following fields.
-
-#### Field: Pipe Circuit 1 {… to N; extensible}
-
-A PipingSystem:Underground:PipeCircuit to be included in this domain.  This indicates that the pipe circuit and all of the underlying pipe segments will be included during mesh development and heat transfer calculations within this domain.  Any number of pipe circuits can be added, assuming all underlying pipe segments do not cause any conflicts for the mesh development engine (overlapping pipes, etc.).
-
-### PipingSystem:Underground:PipeCircuit
-
-This section documents the pipe circuit object, which is used to specify information for the plant loop topology, such as inlet and outlet connections.  This object also groups together pipe segments to define flow paths within a given pipe circuit.
-
-#### Field: Name
-
-This alpha field is used as an identifying field for the pipe circuit.
-
-#### Field: Pipe Thermal Conductivity
-
- The thermal conductivity of the pipe, in W/m-K.
-
-#### Field: Pipe Density
-
- The bulk density of the pipe, in kg/m3.
-
-#### Field: Pipe Specific Heat
-
- The specific heat of the pipe, in J/kg-K.
-
-#### Field: Pipe Inner Diameter
-
- The inner diameter of the pipe, in m.
-
-#### Field: Pipe Outer Diameter
-
- The outer diameter of the pipe, in m.
-
-#### Field: Design Flow Rate
-
- The “design� flow in this pipe circuit, in m3/s.  This is the flow which this component will request during the simulation.  Of course, other components and overall plant management will decide the flow actually given to this component.
-
-#### Field: Circuit Inlet Node Name
-
- The inlet node name for this circuit, which is used when placing this circuit on a branch on a plant or condenser loop.
-
-#### Field: Circuit Outlet Node Name
-
- The outlet node name for this circuit, which is used when placing this circuit on a branch on a plant or condenser loop.
-
-#### Field: Convergence Criterion for the Inner Radial Iteration Loop
-
- The maximum temperature deviation within any cell between one iteration and another to decide that the radial domain has converged to within tolerance.  A smaller value will improve accuracy and computation time.  A smaller value should be accompanied by a higher number of iterations if maximum accuracy is desired.
-
-#### Field: Maximum Iterations in the Inner Radial Iteration Loop
-
- The maximum number of iterations to make when performing temperature updates of the radial coordinate system.  The actual number of iterations made will of course depend on transient conditions and convergence tolerance.
-
-#### Field: Number of Soil Nodes in the Inner Radial Near Pipe Mesh Region
-
- The number of soil nodes to discretize pipe cells.  More information on mesh development is provided in the engineering reference manual.
-
-#### Field: Radial Thickness of Inner Radial Near Pipe Mesh Region
-
- The radial distance used to discretize pipe cells.  More information on mesh development is provided in the engineering reference manual.
-
-#### Field: Number of Pipe Segments Entered for this Pipe Circuit
-
- The number of pipe segment objects which will be defined in the following fields.
-
-#### Field: Pipe Segment 1 {… to N; extensible}
-
- A PipingSystem:Underground:PipeSegment to be included in this pipe circuit.  The circuit is set up so that flow passes through the *N* segments in the order they are entered here.
-
-
-
-### PipingSystem:Underground:PipeSegment
-
-This section documents the pipe segment object, which is used to specify information for a single pipe segment placed at some x, y coordinate in the ground.  The flow direction is also defined in this object to allow for careful description of varying flow paths.  This can be useful for accounting for short circuiting effects if two pipes are placed in counterflow vs. parallel flow.
-
-#### Field: Name
-
-This alpha field is used as an identifying field for the pipe segment.
-
-#### Field: X Position
-
-This numeric field represents the x-direction placement of the pipe.  If no basement is included in the simulation, this is measured from x=0.  If a basement is included, and the domain object specifies that pipes should be shifted, this is measured from the basement wall.
-
-#### Field: Y Position
-
-This numeric field represents the burial depth of the pipe, measured from the ground surface.  This will always be a positive number.
-
-#### Field: Flow Direction
-
-This alpha field is used to define the flow direction within this pipe segment.  The choices are “increasing� or “decreasing.�  These can be chosen carefully to encapsulate specific short-circuiting effects due to varying flow configurations (circuiting).
-
-An example of this object in an IDF is offered here for a foundation heat exchanger
-
-```idf
-  PipingSystem:Underground:Domain,
-    My Piping System,        !- Name
-    12,                      !- Xmax
-    4.5,                     !- Ymax
-    36.84,                   !- Zmax
-    2,                       !- XMeshCount
-    Uniform,                 !- XMeshType
-    ,                        !- XGeometricCoeff
-    2,                       !- YMeshCount
-    Uniform,                 !- YMeshType
-    ,                        !- YGeometricCoeff
-    6,                       !- ZMeshCount
-    Uniform,                 !- ZMeshType
-    ,                        !- ZGeometricCoeff
-    1.08,                    !- GroundThermalConductivity
-    962,                     !- GroundDensity
-    2576,                    !- GroundSpecificHeat
-    30,                      !- MoistureContent
-    50,                      !- MoistureContentAtSaturation
-    Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
-    KATemps,                 !- Name of Undisturbed Ground Temperature Object
-    Yes,                     !- DomainHasBasement
-    6,                       !- BasementWidthInDomain
-    2.5,                     !- BasementDepthInDomain
-    Yes,                     !- ShiftPipeXValuesByBasementWidth
-    BasementWallOSCM,        !- BasementWallBoundaryConditionModel
-    BasementFloorOSCM,       !- BasementFloorBoundaryConditionModel
-    0.005,                   !- CartesianIterationConvergenceCriterion
-    100,                     !- CartesianMaxIterations
-    0.408,                   !- EvapotranspirationGroundCoverParameter
-    1,                       !- NumPipeCircuits
-    My Pipe Circuit;         !- PipeCircuit
-
-  PipingSystem:Underground:PipeCircuit,
-    My Pipe Circuit,         !- Name
-    0.3895,                  !- PipeThermalConductivity
-    641,                     !- PipeDensity
-    2405,                    !- PipeSpecificHeat
-    0.016,                   !- PipeInnerDiameter
-    0.02667,                 !- PipeOuterDiameter
-    0.004,                   !- DesignFlowRate
-    Piping System Inlet Node, !- InletNode
-    Piping System Outlet Node, !- OutletNode
-    0.001,                   !- RadialIterationConvergenceCriterion
-    100,                     !- RadialMaxIterations
-    2,                       !- RadialMeshCount
-    0.03,                    !- RadialMeshThickness
-    6,                       !- NumSegments
-    Segment 1,               !- Segment1
-    Segment 2,               !- Segment2
-    Segment 3,               !- Segment3
-    Segment 4,               !- Segment4
-    Segment 5,               !- Segment5
-    Segment 6;               !- Segment6
-
-  PipingSystem:Underground:PipeSegment,
-    Segment 1,               !- Name
-    0.67,                    !- X
-    2.20,                    !- Burial Depth
-    IncreasingZ;             !- Flow Direction
-
-  PipingSystem:Underground:PipeSegment,
-    Segment 2,               !- Name
-    0.95,                    !- X
-    2.20,                    !- Burial Depth
-    IncreasingZ;             !- Flow Direction
-
-  PipingSystem:Underground:PipeSegment,
-    Segment 3,               !- Name
-    1.23,                    !- X
-    2.20,                    !- Burial Depth
-    IncreasingZ;             !- Flow Direction
-
-  PipingSystem:Underground:PipeSegment,
-    Segment 4,               !- Name
-    1.40,                    !- X
-    1.94,                    !- Burial Depth
-    DecreasingZ;             !- Flow Direction
-
-  PipingSystem:Underground:PipeSegment,
-    Segment 5,               !- Name
-    1.40,                    !- X
-    1.66,                    !- Burial Depth
-    DecreasingZ;             !- Flow Direction
-
-  PipingSystem:Underground:PipeSegment,
-    Segment 6,               !- Name
-    1.40,                    !- X
-    1.39,                    !- Burial Depth
-    DecreasingZ;             !- Flow Direction
-```
-
-
-### PipingSystem:Underground Outputs
-
-* HVAC, Average, Pipe Circuit Mass Flow Rate [kg/s]
-
-* HVAC, Average, Pipe Circuit Inlet Temperature [C]
-
-* HVAC, Average, Pipe Circuit Outlet Temperature [C]
-
-* HVAC, Average, Pipe Segment Inlet Temperature [C]
-
-* HVAC, Average, Pipe Segment Outlet Temperature [C]
-
-* HVAC, Average, Pipe Circuit Fluid Heat Transfer Rate [W]
-
-* HVAC, Average, Pipe Segment Fluid Heat Transfer Rate [W]
-
-
-#### Pipe Circuit Mass Flow Rate [kg/s]
-
-The output provides the mass flow rate currently being sent through the pipe circuit.
-
-#### Pipe Circuit Inlet Temperature [C]
-
-#### Pipe Circuit Outlet Temperature [C]
-
-Temperature of fluid at the inlet and outlet of a given pipe circuit.
-
-#### Pipe Segment Inlet Temperature [C]
-
-#### Pipe Segment Outlet Temperature [C]
-
-Temperature of fluid at the inlet and outlet of a given pipe segment.
-
-#### Pipe Circuit Fluid Heat Transfer Rate [W]
-
-This is the fluid heat gain or loss in the pipe circuit, in Watts.
-
-#### Pipe Segment Fluid Heat Transfer Rate [W]
-
-This is the fluid heat gain or loss in the pipe segment, in Watts.
-
-### Duct
-
-The Duct object is a component for air systems that is a direct analogue for Pipe:Adiabatic in the fluid loops. It is used when it is necessary (due to the HVAC system configuration) to have a branch that has no functional components. This case most often arises for a bypass branch. Since every branch must have at least one component, the Duct component is used for this situation. The duct is an adiabatic, pass-through component; all of its inlet conditions are passed through unchanged to its outlet.
-
-#### Field: Name
-
-This is the unique name for this component. Any reference to this component (in a BranchList, for instance) will refer to it by this name.
-
-#### Field: Inlet Node Name
-
-The name of the component’s air inlet node.
-
-#### Field: Outlet Node Name
-
-The name of the component’s air outlet node.
-
-Below is an example input for Duct.
-
-```idf
-DUCT,
-    VAV Sys 1 Bypass Duct,            !- Name
-    VAV Sys 1 Bypass Duct Inlet Node, !- Inlet Node Name
-    VAV Sys 1 Bypass Duct Outlet Node;!- Outlet Node Name
-```
-
-
-### Duct Outputs
-
-There are no outputs for Duct.
-
-
-
-Group – Plant-Condenser Loops
------------------------------
-
-### PlantLoop
-
-The main elements of the PlantLoop syntax are described in further detail below. A map of how the input for this portion of the HVAC input fits together is provided in the following diagram.
-
-![PlantLoopSyntax (media/image135.png)
-
-Figure 73. Plant Loop Input Syntax Map
-
-#### Field: Name
-
-This alpha field is used as an identifying field for the plant loop.
-
-#### Field: Fluid Type
-
-This alpha field must be a keyword selected from the list of available fluids for an EnergyPlus plant loop. Either **Water**, **Steam** or **UserDefinedFluidType** may be used. If the UserDefinedFluidType keyword is used, the following input field i.e. User Defined Fluid Type must have a value (namely the name of a FluidProperties:GlycolConcentration object).
-
-#### Field: User Defined Fluid Type
-
-This alpha field must be specified when the previous field is set to **UserDefinedFluidType** otherwise it could be left blank. **Water**, **EthyleneGlycol**, **PropoleneGlycol** and **Steam** are all “built-in� fluids for EnergyPlus (that is, all of the appropriate properties are contained within the program). If the fluid specified here is a mixture of water and ethylene or propylene glycol, then only FluidProperties:GlycolConcentration objects need to be specified and the name of the appropriate one is used here. For another water/glycol mixture, a complete set of fluid property data (FluidProperties:Name and FluidProperties:Temperature objects plus multiple FluidProperties:Concentration objects for specific heat, density, etc.) must be specified (Ref dataset: GlycolPropertiesRefData.idf).
-
-#### Field: Plant Equipment Operation Scheme Name
-
-This alpha field is used as an identifying field for the plant operation scheme. This field ties to the PlantEquipmentOperationSchemes input structure, which must also be defined.
-
-#### Field: Loop Temperature Setpoint Node Name
-
-This alpha field is used to identify the node which the Loop Manager will access the temperature setpoint that it will try to maintain. This is typically the Plant Loop Supply Side Outlet Node so that it will not interfere with component temperature setpoints. An associated temperature setpoint manager will need to be defined.
-
-#### Field: Maximum Loop Temperature
-
-This numeric field contains the maximum allowable temperature in Celsius for this loop.
-
-#### Field: Minimum Loop Temperature
-
-This numeric field contains the minimum allowable temperature in Celsius for this loop.
-
-#### Field: Maximum Loop Flow Rate
-
-This numeric field contains the maximum loop flow rate in cubic meters per second. This parameter is also used when the user chooses to autocalculate the loop volume. See Volume of the Plant Loop below and the Engineering Manual for more details. This field is autosizable.
-
-#### Field: Minimum Loop Flow Rate
-
-This numeric field contains the minimum loop flow rate in cubic meters per second.
-
-#### Field: Plant Loop Volume
-
-Volume of the plant loop in m<sup>3</sup>. This numeric field contains the loop volume for the entire loop, i.e. both the demand side and the supply side. This is used for the loop capacitance calculation.. Loop volume (m<sup>3</sup>) could be calculated from pipe size data but this is not usually known. If zero volume is specified the loop has no fluid heat capacity. If a very large capacitance is specified unrealistic time delay may result and there may be poor response to changes in loop setpoint temperature. The loop capacitance **autocalculate** option gives reasonable values for most system sizes. This calculation is described in the Engineering Reference manual.
-
-#### Field: Plant Side Inlet Node Name
-
-This required alpha field contains the identifying name given to the Plant Side Inlet Node.  This node is the inlet to the supply side of the loop.
-
-#### Field: Plant Side Outlet Node Name
-
-This required alpha field contains the identifying name given to the Plant Side Outlet Node. This node is the outlet of the supply side of the loop.
-
-#### Field: Plant Side Branch List Name
-
-This required alpha field contains the identifying name given to the Plant Side Branch List. The list referenced here should list all the branches on the supply side of the loop.
-
-#### Field: Plant Side Connector List Name
-
-This alpha field contains the identifying name given to the Plant Side Connector List. The list referenced here should list the splitter and mixer on the supply side of the loop.
-
-#### Field: Demand Side Inlet Node Name
-
-This required alpha field contains the identifying name given to the Demand Side Inlet Node. This node is the inlet to the demand side of the loop.
-
-#### Field: Demand Side Outlet Node Name
-
-This required alpha field contains the identifying name given to the Demand Side Outlet Node. This node is the outlet of the demand side of the loop.
-
-#### Field: Demand Side Branch List Name
-
-This required alpha field contains the identifying name given to the Demand Side Branch List. The list referenced here should list all the branches on the demand side of the loop.
-
-#### Field: Demand Side Connector List Name
-
-This alpha field contains the identifying name given to the Demand Side Connector List. The list referenced here should list the splitter and mixer on the demand side of the loop.
-
-#### Field: Load Distribution Scheme
-
-This alpha field contains the Load Distribution Scheme Keyword. The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. **Optimal** operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. **SequentialLoad** loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. **UniformLoad** evenly distributes the loop demand among all available components on the equipment list for a given load range. **SequentialUniformPLR** loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. **UniformPLR** will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
-
-Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
-
-#### Field: Availability Manager List Name
-
-This alpha field contains the identifying name given to the System Availability Manager List.
-
-#### Field: Plant Loop Demand Calculation Scheme
-
-There are two plant loop demand calculations schemes in EnergyPlus. There is a SingleSetpoint and a DualSetpointDeadband; the SingleSetpoint is the default if this field is left blank. In the SingleSetpoint scheme the Plant Loop requires that a Setpoint Manager set a single setpoint value (on Node%TempSetpoint). Examples of this setpoint manager would be: SetpointManager:Scheduled, SetpointManager:OutsideAir, etc. For the DualSetPointDeadband scheme the Plant Loop requires that a Setpoint Manager set the high and low setpoint values (for Node%TempSetPointHi and Node%TempSetPointLo). Examples of this Setpoint manager would be: SetpointManager:Scheduled:DualSetpoint.
-
-The plant loop demand calculation scheme determines the amount of heating or cooling necessary to bring the temperature of the Plant Loop to its setpoint(s). When this value is determined then the load distribution scheme explained in the previous section takes this value and distributes the load to the appropriate equipment. The demand calculation scheme determines how the load is calculated. See more information in the Engineering Document.
-
-#### Field: Common Pipe Simulation
-
-This field specifies a primary-secondary plant loop simulation. When a common pipe option is specified, the plant side of the loop is the primary loop and the demand side of the loop is the secondary loop, and a pump object must be placed on the demand side inlet branch. The three options are “**None**�, “**CommonPipe**� and “**TwoWayCommonPipe**�. “**None**� means that there is no secondary loop and the plant loop is modeled as a single primary loop. “**CommonPipe**� means that the common pipe interface does not attempt any temperature control, it only satisfies secondary (demand side) flow requests. “**TwoWayCommonPipe**� allows control of the secondary (demand side) inlet temperature or the primary (plant side) inlet temperature by placing a setpoint on the corresponding node. If this field is left blank, it will default to �None�. If the field is set to “None� and the program finds a pump on the demand side it will result in a fatal error.  If the field is set to “CommonPipe� or “TwoWayCommonPipe� and the program does not find a pump on the demand side it will result in a fatal error. The common pipe simulation is currently limited to simulating loop pumps, i.e. each pump should be placed on the inlet branch of the plant side or demand side of the loop.
-
-#### Field: Pressure Simulation Type
-
-This field lets user to choose if this plant loop will be involved in a pressure drop calculation.  This requires that at least one branch on the loop have pressure drop data.  If not, an error will be thrown due to the input mismatch.  Currently there are two pressure drop simulation types: “PumpPowerCorrection� and “LoopFlowCorrection�.  In both of these methods, branch pressure drop data is used to calculate a dynamic loop pressure drop and is used to update pumping power accordingly.  The flow correction method allows the user to enter information regarding the pressure curve of a constant speed pump so that the simulation can dynamically resolve the pressure vs. flow relationship in the plant loop.  This is limited to constant speed pumps, as the variable speed pumps are expected to resolve as if it were controlled by a variable drive, so that they can inherently meet any pressure and flow demand required by the loop.  This is also limited to “loop pumps�, where there is a single pump on the plant loop. Common pipe simulations and “branch pump� simulations are not compatible with this level of pressure simulation.  See the documentation for the Pump:ConstantSpeed in order to determine required inputs for this pressure simulation method to be performed.  In the pressure drop system, parallel flow rates are not resolved (to match the pressure drop for the parallel system).  Enhancements to this calculation are planned which will allow parallel branch flow resolution.  See the Engineering Reference document for more information on how this works.
-
-An example of this statement used in an IDF is:
-
-```idf
-  PlantLoop,
-    Hot Water Loop,         !- Plant Loop Name
-    Water,                  !- Fluid Type
-    ,                       !- User Defined Fluid Type
-    Hot Loop Operation,     !- Plant Operation Scheme List Name
-    HW Loop Outlet Node,    !- Loop Temperature Setpoint Schedule Name
-    100,                    !- Maximum Loop Temperature {C}
-    10,                     !- Minimum Loop Temperature {C}
-    autosize,               !- Maximum Loop Volumetric Flow Rate {m3/s}
-    0.0,                    !- Minimum Loop Volumetric Flow Rate {m3/s}
-    autosize,               !- volume of the plant loop {m3}
-    HW Supply Inlet Node,   !- Plant Side Inlet Node Name
-    HW Supply Outlet Node,  !- Plant Side Outlet Node Name
-    Heating Supply Side Branches,    !- Plant Side Branch List Name
-    Heating Supply Side Connectors,  !- Plant Side Connector List Name
-    HW Demand Inlet Node,   !- Demand Side Inlet Node Name
-    HW Demand Outlet Node,  !- Demand Side Outlet Nodes Name
-    Heating Demand Side Branches,    !- Demand Side Branch List Name
-    Heating Demand Side Connectors,  !- Demand Side Connector List Name
-    Optimal;                !- Load Distribution Scheme
-```
-
-
-In the above example input there is no system availability manager specified and the Demand Calculation Scheme will default to SingleSetpoint using a single setpoint manager. Common pipe simulation field in the above example will default to “NONE� since it is not specified.
-
-### Plant Loop Outputs
-
-In the following output variables, “Debug� denotes variables that are used primarily by the developers and whose names and application may be cryptic to users. .
-
-* HVAC,Average,Plant Supply Side Cooling Demand Rate [W]
-
-* HVAC,Average,Plant Supply Side Heating Demand Rate [W]
-
-* HVAC,Average,Plant Supply Side Inlet Mass Flow Rate [kg/s]
-
-* HVAC,Average,Plant Supply Side Inlet Temperature [C]
-
-* HVAC,Average,Plant Supply Side Outlet Temperature [C]
-
-* HVAC,Average,Plant Supply Side Not Distributed Demand Rate [W]
-
-* HVAC,Average,Plant Supply Side Unmet Demand Rate [W]
-
-* HVAC,Sum,Plant Solver Sub Iteration Count []
-
-* HVAC,Sum,Plant Solver Half Loop Calls Count []
-
-* HVAC,Average,Debug Plant Loop Bypass Fraction
-
-* HVAC,Average,Debug Plant Last Simulated Loop Side [-]
-
-* HVAC,Average,Plant Common Pipe Mass Flow Rate [Kg/s]
-
-* HVAC,Average,Plant Common Pipe Temperature [C]
-
-* HVAC,Average,Plant Common Pipe Flow Direction Status []
-
-* HVAC,Average,Plant Common Pipe Primary Mass Flow Rate [Kg/s]
-
-* HVAC,Average,Plant Common Pipe Secondary Mass Flow Rate [Kg/s]
-
-* HVAC,Average,Primary Side Common Pipe Flow Direction []
-
-* HVAC,Average,Secondary Side Common Pipe Flow Direction []
-
-* HVAC,Average,Plant Common Pipe Primary to Secondary Mass Flow Rate [Kg/s]
-
-* HVAC,Average,Plant Common Pipe Secondary to Primary Mass Flow Rate [Kg/s]
-
-* HVAC,Average,Plant System Cycle On Off Status []
-
-* HVAC,Average,Plant Demand Side Loop Pressure Difference [Pa]
-
-* HVAC,Average,Plant Supply Side Loop Pressure Difference [Pa]
-
-* HVAC,Average,Plant Loop Pressure Difference [Pa]
-
-
-#### Plant Supply Side Cooling Demand Rate [W]
-
-This is the value of the net demand required to meet the cooling setpoint of the loop.  If the loop setpoint is met for the current HVAC timestep, Plant Supply Side Cooling Demand Rate will equal sum of the total cooling demand from the demand side coils on the loop.  It will also equal the cooling output of all chillers (or other cooling equipment) on the loop less any pump heat added to the fluid.  For example, for a chilled water loop with one chiller and one pump serving one chilled water coil:  Plant Supply Side Cooling Demand Rate will equal the chiller evaporator heat transfer less the pump heat to fluid, and it will also equal the chilled water coil total cooling output.
-
-If the plant loop setpoint is not met, Plant Supply Side Cooling Demand Rate will equal the sum of the total cooling demand from the demand side coils on the loop plus the additional cooling required to bring the loop flow to setpoint.  If the loop remains off setpoint for successive timesteps, the demand required to return to setpoint will repeat in each timestep until the loop reaches setpoint.  For this reason, Plant Supply Side Cooling Demand Rate should not be summed over time, because it will overstate the demand whenever the loop is off setpoint.
-
-#### Plant Supply Side Heating Demand Rate [W]
-
-This is the value of the net demand required to meet the heating setpoint of the loop.  If the loop setpoint is met for the current HVAC timestep, Plant Supply Side Heating Demand Rate will equal sum of the total heating demand from the demand side coils on the loop.  It will also equal the heating output of all boilers (or other cooling equipment) on the loop plus any pump heat added to the fluid.  For example, for a hot water loop with one boiler and one pump serving one hot water coil: Plant Supply Side Heating Demand Rate will equal the boiler heat transfer plus the pump heat to fluid, and it will also equal the hot water coil total heating output.
-
-If the plant loop setpoint is not met, Plant Supply Side Heating Demand Rate will equal the sum of the total heating demand from the demand side coils on the loop plus the additional heating required to bring the loop flow to setpoint.  If the loop remains off setpoint for successive timesteps, the demand required to return to setpoint will repeat in each timestep until the loop reaches setpoint.  For this reason, Plant Supply Side Heating Demand Rate should not be summed over time, because it will overstate the demand whenever the loop is off setpoint.
-
-#### Plant Supply Side Inlet Mass Flow Rate [kg/s]
-
-This is the value of the mass flow rate at the Inlet to Plant Loop on the supply side. There is not an associated Plant Loop outlet node flow rate since continuity must be maintained in the loop and the outlet must be the same.
-
-#### Plant Supply Side Inlet Temperature [C]
-
-This is the value of the temperature at the Inlet to the plant loop on the supply side.
-
-#### Plant Supply Side Outlet Temperature [C]
-
-This is the value of the temperature at the outlet to the plant loop on the supply side.
-
-#### Plant Supply Side Not Distributed Demand Rate [W]
-
-This is the value of the demand that could not be distributed to the plant equipment because of some constraint in the plant operation scheme.  This is a record of the loop operation scheme supervisory controls after attempting to distribute the load.  For example it would be  non-zero in situations where the load is larger than the upper limit of capacities set for the plant equipment controls.  This output is for *before* the equipment has actually been simulated whereas the separate output Plant Supply Side Unmet Demand Rate is for *after* the equipment has simulated.
-
-#### Plant Supply Side Unmet Demand Rate [W]
-
-This is the value of the demand NOT provided by the plant equipment to meet the heating or cooling setpoint of the loop. The value is positive when the plant equipment cannot meet the setpoint, and the value is negative when the plant equipment provides more than enough heating or cooling to meet the setpoint. A negative value can happen when the amount of demand is smaller than the minimum capacity of the equipment using the minimum part load ratio.
-
-#### Plant Solver Sub Iteration Count [ ]
-
-This is the count of iterations that the overall plant simulation used over the period of time being reported.  This high-level output is from the plant solver used for all the plant loops and condenser loops in the model.
-
-#### Plant Solver Half Loop Calls Count
-
-This is the count of calls to model individual half-loops that occurred during the overall plant simulation over the period of time being reported.  This includes all the half-loops for both plant loops and condenser loops.
-
-#### Plant Common Pipe Mass Flow Rate [Kg/s]
-
-This output gives the magnitude of the flow through common pipe. The value is averaged over the reporting interval.
-
-#### Plant Common Pipe Temperature [C]
-
-This output gives the value of the temperature of the fluid flowing through common pipe. This value is averaged over the reporting interval.
-
-#### Plant Common Pipe Flow Direction Status []
-
-This output gives the direction of flow in common pipe. The value is an integer and can be 0, 1 or 2. Since the output value is averaged over reporting interval, a non-integer value may be shown as an output when the reporting interval is not detailed. An output value of 0 means that there was no flow in common pipe. An output value of 1 means that the secondary flow is greater than primary flow, whereas a value of 2 means that primary flow is greater than secondary flow.
-
-#### Plant Common Pipe Primary Mass Flow Rate [Kg/s]
-
-This output variable gives the mass flow in the primary side common pipe leg in a Two-Way common pipe simulation. Value is averaged over the reporting interval.
-
-#### Plant Common Pipe Secondary Mass Flow Rate [Kg/s]
-
-This output variable gives the mass flow in the secondary side common pipe leg in a Two-Way common pipe simulation. Value is averaged over the reporting interval.
-
-#### Primary Side Common Pipe Flow Direction []
-
-This output variable gives the direction of flow in a primary side common pipe leg in a Two-Way Common Pipe Simulation. A value of zero means there was no flow in the pipe. A value of 1 means the flow was from top to bottom in EnergyPlus loop schematic. So for primary side, a value of 1 means the flow is from Primary side inlet to Primary side outlet and a value of 2 means flow is from Primary side outlet to Primary side inlet.
-
-#### Secondary Side Common Pipe Flow Direction []
-
-This output variable gives the direction of flow in a Secondary side common pipe leg in a Two-Way Common Pipe Simulation. A value of zero means there was no flow in the pipe. A value of 1 means the flow was from top to bottom in EnergyPlus loop schematic. So for Secondary side, a value of 1 means the flow is from Secondary side outlet to Secondary side inlet and a value of 2 means flow is from Secondary side inlet to Secondary side outlet. Note that this is opposite to the primary side common pipe.
-
-#### Plant Common Pipe Primary to Secondary Mass Flow Rate [Kg/s]
-
-This output variable gives the mass flow from primary to secondary side in a Two-Way common pipe simulation. Value is averaged over the reporting interval.
-
-#### Plant Common Pipe Secondary to Primary Mass Flow Rate [Kg/s]
-
-This output variable gives the mass flow from secondary to primary side in a Two-Way common pipe simulation. Value is averaged over the reporting interval.
-
-#### Plant System Cycle On Off Status
-
-This field is the availability status of a Plant Loop. This status flag is a result of the calculations made by the System Availability Manager(s) listed in a System Availability Manager List. When a single availability manager is used in a System Availability Manager List, this is also the availability status reported by the specific availability manager (Ref. System Availability Manager Outputs). When multiple availability managers are used in a System Availability Manager List, the loop availability status is determine by the rules associated with Plant Loops (see rules described for Group – System Availability Managers). The control status outputs are represented using integers 0 through 2.. These integers represent *NoAction* (0), *ForceOff* (1), and *CycleOn* (2). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-#### Plant Demand Side Loop Pressure Difference [Pa]
-
-This field allows the user to output the demand side pressure drop of a plant loop.  This output is only recognized if a valid pressure simulation is being performed.  To do this, the user must specify a pressure simulation type as an input in the PlantLoop object, and input at least one pressure drop curve on a branch of the plant loop.  This particular output is only relevant if the user puts that curve on the demand side of the loop.
-
-#### Plant Supply Side Loop Pressure Difference [Pa]
-
-This field allows the user to output the supply side pressure drop of a plant loop.  This output is only recognized if a valid pressure simulation is being performed.  To do this, the user must specify a pressure simulation type as an input in the PlantLoop object, and input at least one pressure drop curve on a branch of the plant loop.  This particular output is only relevant if the user puts that curve on the supply side of the loop.
-
-#### Plant Loop Pressure Difference [Pa]
-
-This output is the total pressure drop of a plant loop.  This output is only recognized if a valid pressure simulation is being performed.  To do this, the user must specify a pressure simulation type as an input in the PlantLoop object, and input at least one pressure drop curve on a branch of the plant loop.  This particular output is relevant regardless of the location of pressure drop curves: demand side, supply side, or both.
-
-
-
-The following advanced output variables are also available for plant loops (and condenser loops) when advanced output variables are requested (e.g. “Output:Diagnostics, DisplayAdvancedReportVariable;�).
-
-* HVAC,Average,Plant Demand Side Lumped Capacitance Temperature [C]
-
-* HVAC,Average,Plant Supply Side Lumped Capacitance Temperature [C]
-
-* HVAC,Average,Plant Component Distributed Demand Rate [W]
-
-#### Plant Demand Side Lumped Capacitance Temperature [C]
-
-#### Plant Supply Side Lumped Capacitance Temperature [C]
-
-These two outputs are the temperature of the plant (or condenser) loop’s working fluid where the two half-loops interface together.  The program models heat capacitance in the volume of fluid inside the plant loop itself using two simple models for “well-stirred� tanks located at each of the half-loop inlet and outlet pairs.  These tank models also receive the heat transferred to the fluid by the work done by pumping and resulting friction heating.  One output is for the point where the fluid leaves the supply side and enters the demand side.  The other output is for the point where the fluid leaves the demand side and enters the supply side.
-
-#### Plant Component Distributed Demand Rate [W]
-
-This output is available for every component on every branch in a plant (or condenser) loop and shows the outcome of the load dispatch performed by the operation schemes.  This the load in watts passed from the supervisor routines to the equipment component models.  This provides a record of what a particular component was asked to do by the supervisory routines. This can be useful for diagnosing issues in operation schemes when a component or loop is failing to meet the load.
-
-### CondenserLoop
-
-The condenser loop input is very similar to that for the plant loop. As of version 7, the two loops are modeled the same way and inside the program all condenser loops are just plant loops. (In future versions of the program, this CondenserLoop object might be deprecated and these loops will be described using the PlantLoop object.)  The main differences are the applicable components and operation schemes. This is depicted in the following diagram.
-
-![CondenserLoopSyntax (media/image136.png)
-
-Figure 74. Condenser Loop Input Syntax Map
-
-#### Field: Name
-
-This alpha field is used as an identifying field for the condenser loop.
-
-#### Field: Fluid Type
-
-This alpha field must be a keyword selected from the list of available fluids for an EnergyPlus plant loop. Either **Water** or **UserDefinedFluidType** may be used. If the UserDefinedFluidType keyword is used, the following input field i.e. User Defined Fluid Type must have a value (namely the name of a FluidProperties:GlycolConcentration object).
-
-#### Field: User Defined Fluid Type
-
-This alpha field must be specified when the previous field is set to **UserDefinedFluidType** otherwise it could be left blank. **Water**, **EthyleneGlycol**, and **PropoleneGlycol** are all “built-in� fluids for EnergyPlus (that is, all of the appropriate properties are contained within the program). If the fluid specified here is a mixture of water and ethylene or propylene glycol, then only FluidProperties:GlycolConcentration objects need to be specified and the name of the appropriate one is used here. For another water/glycol mixture, a complete set of fluid property data (FluidProperties:Name and FluidProperties:Temperature objects plus multiple FluidProperties:Concentration objects for specific heat, density, etc.) must be specified (Ref dataset: GlycolPropertiesRefData.idf).
-
-#### Field: Condenser Equipment Operation Scheme Name
-
-This alpha field is used as an identifying field for the condenser operation scheme. This field ties to the Condenser Operation Schemes input structure, which must also be defined.
-
-#### Field: Condenser Loop Temperature Setpoint Node Name
-
-This alpha field is used to identify the node which the Loop Manager will access the temperature setpoint that it will try to maintain. This is typically the Condenser Loop Supply Side Outlet Node so that it will not interfere with component temperature setpoints. An associated temperature setpoint manager will need to be defined.
-
-#### Field: Maximum Loop Temperature
-
-This numeric field contains the maximum allowable temperature in Celsius for this loop.
-
-#### Field: Minimum Loop Temperature
-
-This numeric field contains the minimum allowable temperature in Celsius for this loop. This minimum loop temperature is used by the cooling towers to make sure that the minimum is not violated to keep the equipment safe. The minimum is also used to trigger the minimum temperature warning and will notify the user if it gets too low.
-
-#### Field: Maximum Loop Flow Rate
-
-This numeric field contains the maximum loop flow rate in cubic meters per second. This field is autosizable.
-
-#### Field: Minimum Loop Flow Rate
-
-This numeric field contains the minimum loop flow rate in cubic meters per second.
-
-#### Field: Condenser Loop Volume
-
-Volume of the condenser loop in m<sup>3</sup>. This numeric field contains the loop volume for the entire loop, i.e., both the demand side and the supply side. This is used for the loop capacitance calculation. Loop volume (m<sup>3</sup>) could be calculated from pipe size data but this is not usually known. If zero volume is specified the loop has no fluid heat capacity. If a very large capacitance is specified unrealistic time delay may result and there may be poor response to changes in loop setpoint temperature. The loop capacitance **autocalculate** option gives reasonable values for most system sizes. This calculation is described in the Engineering Reference manual.
-
-#### Field: Condenser Side Inlet Node Name
-
-This required alpha field contains the identifying name given to the Condenser Side Inlet Node. This node is the inlet to the supply side of the loop.
-
-#### Field: Condenser Side Outlet Node Name
-
-This required alpha field contains the identifying name given to the Condenser Side Outlet Node. This node is the outlet of the supply side of the loop.
-
-#### Field: Condenser Side Branch List Name
-
-This required alpha field contains the identifying name given to the Condenser Side Branch List. The list referenced here should list all the branches on the supply side of the loop.
-
-#### Field: Condenser Side Connector List Name
-
-This required alpha field contains the identifying name given to the Condenser Side Connector List.  The list referenced here should list the splitter and mixer on the supply side of the loop.
-
-
-
-#### Field: Demand Side Inlet Node Name
-
-This required alpha field contains the identifying name given to the Demand Side Inlet Node.  This node is the inlet to the demand side of the loop.
-
-#### Field: Demand Side Outlet Nodes Name
-
-This required alpha field contains the identifying name given to the Demand Side Outlet Node. This node is the outlet of the demand side of the loop.
-
-#### Field: Condenser Demand Side Branch List Name
-
-This required alpha field contains the identifying name given to the Demand Side Branch List.  The list referenced here should list all the branches on the demand side of the loop.
-
-#### Field: Condenser Demand Side Connector List Name
-
-This required alpha field contains the identifying name given to the Demand Side Connector List. The list referenced here should list the splitter and mixer on the demand side of the loop.
-
-#### Field: Load Distribution Scheme
-
-This alpha field contains the Load Distribution Scheme Keyword. The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. **Optimal** operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. **SequentialLoad** loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. **UniformLoad** evenly distributes the loop demand among all available components on the equipment list for a given load range. **SequentialUniformPLR** loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. **UniformPLR** will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
-
-Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
-
-#### Field: Pressure Simulation Type
-
-This field lets user to choose if this plant loop will be involved in a pressure drop calculation.  This requires that at least one branch on the loop have pressure drop data.  If not, an error will be thrown due to the input mismatch.  Currently there are two pressure drop simulation types: “PumpPowerCorrection� and “LoopFlowCorrection�.  In both of these methods, branch pressure drop data is used to calculate a dynamic loop pressure drop and is used to update pumping power accordingly.  The flow correction method allows the user to enter information regarding the pressure curve of a constant speed pump so that the simulation can dynamically resolve the pressure vs. flow relationship in the plant loop.  This is limited to constant speed pumps, as the variable speed pumps are expected to resolve as if it were controlled by a variable drive, so that they can inherently meet any pressure and flow demand required by the loop.  This is also limited to “loop pumps�, where there is a single pump on the plant loop.  Common pipe simulations and “branch pump� simulations are not compatible with this level of pressure simulation.  See the documentation for the Pump:ConstantSpeed in order to determine required inputs for this pressure simulation method to be performed.  In the pressure drop system, parallel flow rates are not resolved (to match the pressure drop for the parallel system).  Enhancements to this calculation are planned which will allow parallel branch flow resolution.  See the Engineering Reference document for more information on how this works.
-
-An example of this statement used in an IDF is:
-
-```idf
-  CondenserLoop,
-    Condenser Water Loop,    !- Name
-    Water,                   !- Fluid Type
-    ,                        !- User Defined Fluid Type
-    Tower Loop Operation,    !- Condenser Equipment Operation Scheme Name
-    Condenser Supply Outlet Node,  !- Condenser Loop Temperature Setpoint Node Name
-    80,                      !- Maximum Loop Temperature {C}
-    10,                      !- Minimum Loop Temperature {C}
-    autosize,                !- Maximum Loop Flow Rate {m3/s}
-    0.0,                     !- Minimum Loop Flow Rate {m3/s}
-    autocalculate,           !- Condenser Loop Volume {m3}
-    Condenser Supply Inlet Node,  !- Condenser Side Inlet Node Name
-    Condenser Supply Outlet Node,  !- Condenser Side Outlet Node Name
-    Condenser Supply Side Branches,  !- Condenser Side Branch List Name
-    Condenser Supply Side Connectors,  !- Condenser Side Connector List Name
-    Condenser Demand Inlet Node,  !- Demand Side Inlet Node Name
-    Condenser Demand Outlet Node,  !- Demand Side Outlet Node Name
-    Condenser Demand Side Branches,  !- Condenser Demand Side Branch List Name
-    Condenser Demand Side Connectors,  !- Condenser Demand Side Connector List Name
-    SequentialLoad;              !- Load Distribution Scheme
-
-  SetpointManager:FollowOutdoorAirTemperature,
-    MyCondenserControl,      !- Name
-    Temperature,             !- Control Variable
-    OutdoorAirWetBulb,       !- Reference Temperature Type
-    0,                       !- Offset Temperature Difference {deltaC}
-    80,                      !- Maximum Setpoint Temperature {C}
-    10,                      !- Minimum Setpoint Temperature {C}
-    Condenser Supply Outlet Node;  !- Setpoint Node or NodeList Name
-
-  CondenserLoop,
-    Chilled Water Condenser Loop,  !- Name
-    UserDefinedFluidType,    !- Fluid Type
-    PropyleneGlycol15Percent,!- User Defined Fluid Type
-    Tower Loop Operation,    !- Condenser Equipment Operation Scheme Name
-    Condenser Supply Outlet Node,  !- Condenser Loop Temperature Setpoint Node Name
-    80,                      !- Maximum Loop Temperature {C}
-    10,                      !- Minimum Loop Temperature {C}
-    0.00330000,              !- Maximum Loop Flow Rate {m3/s}
-    0,                       !- Minimum Loop Flow Rate {m3/s}
-    autocalculate,           !- Condenser Loop Volume {m3}
-    Condenser Supply Inlet Node,  !- Condenser Side Inlet Node Name
-    Condenser Supply Outlet Node,  !- Condenser Side Outlet Node Name
-    Condenser Supply Side Branches,  !- Condenser Side Branch List Name
-    Condenser Supply Side Connectors,  !- Condenser Side Connector List Name
-    Condenser Demand Inlet Node,  !- Demand Side Inlet Node Name
-    Condenser Demand Outlet Node,  !- Demand Side Outlet Node Name
-    Condenser Demand Side Branches,  !- Condenser Demand Side Branch List Name
-    Condenser Demand Side Connectors,  !- Condenser Demand Side Connector List Name
-    SequentialLoad;              !- Load Distribution Scheme
-```
-
-
-### Condenser Loop Outputs
-
-* HVAC,Average,Plant Supply Side Cooling Demand Rate [W]
-
-* HVAC,Average,Plant Supply Side Heating Demand Rate [W]
-
-* HVAC,Average,Plant Supply Side Inlet Mass Flow Rate [kg/s]
-
-* HVAC,Average,Plant Supply Side Inlet Temperature [C]
-
-* HVAC,Average,Plant Supply Side Outlet Temperature [C]
-
-* HVAC,Average,Cond Loop Demand Not Distributed [W]
-
-* HVAC,Average,Plant Supply Side Unmet Demand Rate [W]
-
-* HVAC,Average,Plant Demand Side Loop Pressure Difference [Pa]
-
-* HVAC,Average,Plant Supply Side Loop Pressure Difference [Pa]
-
-* HVAC,Average,Plant Loop Pressure Difference [Pa]
-
-
-#### Plant Supply Side Cooling Demand Rate [W]
-
-This is the value of the net demand required to meet the cooling setpoint of the loop.  If the loop setpoint is met for the current HVAC timestep, Plant Supply Side Cooling Demand Rate will equal sum of the total cooling demand from the demand side components on the loop (typically condenser coils of chillers, etc.).  It will also equal the cooling output of all condensing equipment such as cooling towers on the loop less any pump heat added to the fluid.  For example, for a condenser loop with one tower and one pump serving one chiller, Plant Supply Side Cooling Demand Rate will equal the tower water-side heat transfer less the pump heat to fluid, and it will also equal the chiller condenser heat transfer rate.
-
-If the condenser loop setpoint is not met, Plant Supply Side Cooling Demand Rate will equal the sum of the total cooling demand from the demand side components on the loop plus the additional cooling required to bring the loop flow to setpoint.  If the loop remains off setpoint for successive timesteps, the demand required to return to setpoint will repeat in each timestep until the loop reaches setpoint.  For this reason, Plant Supply Side Cooling Demand Rate should not be summed over time, because it will overstate the demand whenever the loop is off setpoint.
-
-#### Plant Supply Side Heating Demand Rate [W]
-
-This is the value of the net demand required to meet the heating setpoint of the loop.  If the loop setpoint is met for the current HVAC timestep, Plant Supply Side Heating Demand Rate will equal sum of the total heating demand from the demand side components on the loop.  It will also equal the heating output of all heating equipment on the supply side of the loop plus any pump heat added to the fluid.  For example, for a condenser loop with one ground loop heat exchanger and one pump serving one water-to-water heat pump, Plant Supply Side Heating Demand Rate will equal the ground loop heat transfer plus the pump heat to fluid, and it will also equal the heat pump condenser side heat transfer rate.
-
-If the condenser loop setpoint is not met, Plant Supply Side Heating Demand Rate will equal the sum of the total heating demand from the demand side components on the loop plus the additional heating required to bring the loop flow to setpoint.  If the loop remains off setpoint for successive timesteps, the demand required to return to setpoint will repeat in each timestep until the loop reaches setpoint.  For this reason, Plant Supply Side Heating Demand Rate should not be summed over time, because it will overstate the demand whenever the loop is off setpoint.
-
-#### Plant Supply Side Inlet Mass Flow Rate [kg/s]
-
-This is the value of the mass flow rate at the Inlet to Condenser Loop on the supply side. There is not an associated Condenser Loop outlet node flow rate since continuity must be maintained in the loop and the outlet must be the same.
-
-#### Plant Supply Side Inlet Temperature [C]
-
-This is the value of the temperature at the Inlet to the condenser loop on the supply side.
-
-#### Cond Loop OutletNode Temperature [C]
-
-This is the value of the temperature at the outlet to the condenser loop on the supply side.
-
-#### Cond Loop Demand Not Distributed [W]
-
-This is the value of the demand that could not be distributed to the condenser equipment because of some constraint in the operation scheme.  This is a record of the loop operation scheme supervisory controls after attempting to distribute the load.  For example it would be  non-zero in situations where the load is larger than the upper limit of capacities set for the condenser equipment controls.  This output is for *before* the equipment has actually been simulated whereas the separate output Plant Supply Side Unmet Demand Rate is for *after* the equipment has simulated.
-
-#### Plant Supply Side Unmet Demand Rate [W]
-
-This is the value of the demand NOT provided by the condenser equipment to meet the heating or cooling setpoint of the loop. The value is positive when the condenser equipment cannot meet the setpoint, and the value is negative when the condenser equipment provides more than enough heating or cooling to meet the setpoint. A negative value can happen when the amount of demand is smaller than the minimum capacity of the equipment using the minimum part load ratio.
-
-#### Plant Demand Side Loop Pressure Difference [Pa]
-
-This field is the demand side pressure drop of a condenser loop.  This output is only recognized if a valid pressure simulation is being performed.  To do this, the user must specify a pressure simulation type as an input in the CondenserLoop object, and input at least one pressure drop curve on a branch of the plant/condenser loop.  This particular output is only relevant if the user puts that curve on the demand side of the loop.
-
-#### Plant Supply Side Loop Pressure Difference [Pa]
-
-This field is the supply side pressure drop of a condenser loop.  This output is only recognized if a valid pressure simulation is being performed.  To do this, the user must specify a pressure simulation type as an input in the CondenserLoop object, and input at least one pressure drop curve on a branch of the plant/condenser loop.  This particular output is only relevant if the user puts that curve on the supply side of the loop.
-
-####  Plant Loop Pressure Difference [Pa]
-
-This field is the total pressure drop of a condenser loop.  This output is only recognized if a valid pressure simulation is being performed.  To do this, the user must specify a pressure simulation type as an input in the CondenserLoop object, and input at least one pressure drop curve on a branch of the plant/condenser loop.  This particular output is relevant regardless of the location of pressure drop curves: demand side, supply side, or both.
-
-
-Group – Plant-Condenser Control
--------------------------------
-
-### Operation Schemes (Plant and Condenser)
-
-Plants and condenser loops must have some mechanism for controlling the operation of the loop and which equipment is available under what conditions. Since there may be multiple control schemes that are assigned various priorities associated with each loop, an overall operation scheme must be defined. The overall scheme consists of the object name, an identifying name that is referenced in the main plant or condenser loop statement, and a list of operation schemes. Each operation scheme must have the type of operation scheme, its identifying name, and the schedule that defines its availability. Note that the order in which the individual operation schemes appear in this list defines its priority versus the others with the same scheduled availability. The first scheme appearing in the list is given the highest priority, the second scheme has second highest priority, etc. In other words, if according to its schedule, the first operation scheme is available, then it is used by the simulation to define how the plant or condenser loop operates. If it is not available, the second operation scheme in the list is checked to see if it is available until the highest priority scheme that is also available is found.  To allow for simultaneous heating and cooling, there is one configuration where multiple operation schemes are available at a given timestep.  This is allowed if a user inputs both a heating range based operation and a cooling range based operation with overlapping schedules.  The simulation will look at the current loop demand to determine if the cooling scheme should be used or the heating scheme.  In other cases, if two schemes overlap (are available at the same time), a fatal error will be encountered.
-
-### PlantEquipmentOperationSchemes
-
-#### Field: Name
-
-This alpha field contains the identifying name given to the Plant Operation Scheme. This name is placed in the Plant Loop object to select this scheme.
-
-#### Field Set: (Component Object Type, Name, Schedule) up to 8
-
-Operation schemes are listed in "priority" order.  Note that each scheme must address the entire load and/or condition ranges for the simulation. The actual one selected for use will be the first that is "Scheduled" on.  That is, if control scheme 1 is not "on" and control scheme 2 is -- then control scheme 2 is selected. Only plant equipment should be listed on a Control Scheme for this item.
-
-#### Field: Control Scheme &lt;\#&gt; Object Type
-
-This alpha field contains the keyword for the type of control scheme used. The options for plant control schemes are:
-
-- PlantEquipmentOperation:Uncontrolled
-
-- PlantEquipmentOperation:CoolingLoad
-
-- PlantEquipmentOperation:HeatingLoad
-
-- PlantEquipmentOperation:ComponentSetpoint
-
-- PlantEquipmentOperation:ThermalEnergyStorage
-
-- PlantEquipmentOperation:UserDefined
-
-#### Field: Control Scheme &lt;\#&gt; Name
-
-This alpha field contains the identifying name given to the control scheme. These must be the named versions of the referenced Control Scheme (e.g.. a Uncontrolled Loop Operation with this name or a Cooling or Heating Load Range Based Operation with this name).
-
-#### Field: Control Scheme &lt;\#&gt; Schedule
-
-This alpha field contains the schedule name for the control scheme. This schedule consists of weeks and days, with the days containing “0 or 1� for each hour of the day. This binary schedule (0 for off, 1 for on) determines if the control scheme is operating for that hour of day or not.
-
-Examples of this statement in two different IDFs:
-
-```idf
-PlantEquipmentOperationSchemes,
-    CW Loop Operation,       !- Name
-    PlantEquipmentOperation:CoolingLoad,  ! Control Scheme 1 Object Type
-    Peak Operation,          !- Control Scheme 1 Name
-    On Peak,                 !- Control Scheme 1 Schedule
-    PlantEquipmentOperation:CoolingLoad,  ! Control Scheme 2 Object Type
-    Off Peak Operation,      !- Control Scheme 2 Name
-    Off Peak;                !- Control Scheme 2 Schedule
-
-PlantEquipmentOperationSchemes,
-    CW Loop Operation,       !- Name
-    PlantEquipmentOperation:CoolingLoad,  ! Control Scheme 1 Object Type
-    Central Chiller Only,    !- Control Scheme 1 Name
-    PlantOnSched;            !- Control Scheme 1 Schedule
-```
-
-
-In the first IDF example, “PlantEquipmentOperation:CoolingLoad� is the type of control scheme. “Peak Operation� and “Off Peak Operation� are the names of two different load range based controls defined separately (see below -- ). “On Peak� and “Off Peak� are schedules defined elsewhere in the input file.
-
-The load range based operation scheme has two statements associated with it: a main statement that defines the ranges that individual priority settings are valid and the lists of equipment that may be used for each range.
-
-### CondenserEquipmentOperationSchemes
-
-#### Field: Name
-
-This alpha field contains the identifying name given to the Condenser Operation Scheme.
-
-#### Field Set: (Component Object Type, Name, Schedule) up to 8
-
-Operation schemes are listed in "priority" order.  Note that each scheme must address the entire load and/or condition ranges for the simulation. The actual one selected for use will be the first that is "Scheduled" on.  That is, if control scheme 1 is not "on" and control scheme 2 is -- then control scheme 2 is selected. Only condenser equipment should be listed on a Control Scheme for this item.
-
-#### Field: Control Scheme &lt;\#&gt; Object Type
-
-This alpha field contains the keyword for the type of control scheme used. The options for plant control schemes are:
-
-This alpha field contains the keyword for the type of control scheme used. Currently, the available options are:
-
-- PlantEquipmentOperation:Uncontrolled
-
-- PlantEquipmentOperation:CoolingLoad
-
-- PlantEquipmentOperation:HeatingLoad
-
-- PlantEquipmentOperation:OutdoorDryBulb
-
-- PlantEquipmentOperation:OutdoorWetBulb
-
-- PlantEquipmentOperation:OutdoorDewpoint
-
-- PlantEquipmentOperation:OutdoorRelativeHumidity
-
-- PlantEquipmentOperation:OutdoorDryBulbDifference
-
-- PlantEquipmentOperation:OutdoorWetBulbDifference
-
-- PlantEquipmentOperation:OutdoorDewpointDifference
-
-- PlantEquipmentOperation:UserDefined
-
-The condenser operation schemes apply to the equipment on the ‘supply side’ of the condenser loop—pumps, cooling towers, ground coupled heat exchangers, etc. The keywords select the algorithm that will be used to determine which equipment is available for each timestep. The Load Schemes schemes select a user specified set of equipment for each user specified range of a particular simulation variable. Load schemes compare the demand on the condenser supply side with specified load ranges and associated equipment lists. Outdoor schemes compare the current value of an environmental parameter with user specified ranges of that parameter.
-
-#### Field: Control Scheme &lt;\#&gt; Name
-
-This alpha field contains the identifying name given to the control scheme.
-
-#### Field: Control Scheme &lt;\#&gt; Schedule
-
-This alpha field contains the schedule name for the control scheme. This schedule consists of weeks and days, with the days containing “0 or 1� for each hour of the day. This binary schedule (0 for off, 1 for on) determines which control scheme is operating for a particular hour. The schedule facilitates daily or seasonal changes in control schemes to meet demand side management or energy conservation goals.
-
-Scheduling conflicts are handled by selecting the first available scheme in order of appearance in the list.
-
-Examples of this statement in two IDFs:
-
-```idf
-CondenserEquipmentOperationSchemes,
-    Tower Loop Operation,    !- CondenserOperationSchemeName
-    PlantEquipmentOperation:CoolingLoad,  Control Scheme 1 Object Type
-    Year Round Tower Operation,  !- Control Scheme 1 Name
-    PlantOnSched;            !- Control Scheme 1 Schedule
-
-CondenserEquipmentOperationSchemes,Tower Loop Operation,
-    PlantEquipmentOperation:CoolingLoad, Peak Load Operation, AFTERNOONSCHEDULE,
-    PlantEquipmentOperation:CoolingLoad, OffPeak Load Operation, MORNINGSCHEDULE,
-    PlantEquipmentOperation:OutdoorWetBulb, NightOperation, NIGHTSCHEDULE;
-```
-
-
-Each schedule (AFTERNOONSCHEDULE, MORNINGSCHEDULE, NIGHTSCHEDULE) invokes its associated operation scheme (Peak Load Operation, OffPeak Load Operation, NightOperation). The type of operation scheme and its name references the input syntax associated with the range specification and the associated equipment.
-
-### PlantEquipmentOperation:Uncontrolled
-
-Uncontrolled loop operation simply specifies a group of equipment that runs ‘uncontrolled’. If the loop runs, this equipment will run also, unless turned off by the loop flow resolver to maintain continuity in the fluid loop.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the control scheme.
-
-#### Field: Equipment List Name
-
-This alpha field contains the identifying name for the Equipment List. This field ties to the Load Range Equipment List input structure, which must also be defined.
-
-#### Field: Equipment List Name
-
-This alpha field contains the identifying name for the Equipment List. This field ties to the PlantEquipmentList or CondenserEquipmentList input structure, which must also be defined.
-
-### PlantEquipmentOperation:CoolingLoad
-
-### PlantEquipmentOperation:HeatingLoad
-
-The PlantEquipmentOperation:CoolingLoad  and PlantEquipmentOperation:HeatingLoad objects define the different ranges and which equipment list is valid for each range. After the keyword and the identifying name, a series of data trios is expected. In each trio, there is a lower limit for the load range, an upper limit for the load range, and a name that links to an equipment availability list (the PlantEquipmentList or CondenserEquipmentList objects).
-
-#### Field: Name
-
-This alpha field contains the identifying name for the control scheme.
-
-#### Field Set: (Lower limit, Upper Limit, Equip List name) up to 10
-
-#### Field: Load Range &lt;\#&gt; Lower Limit
-
-This numeric field contains the lower demand range (W) for the equipment list. If demand is below this value, then this equipment list will not turn on to meet the demand.
-
-#### Field: Load Range &lt;\#&gt; Upper Limit
-
-This numeric field contains the upper demand range (W) for the equipment list. If demand is above this value, then this equipment list will not turn on to meet the demand.
-
-#### Field: Range &lt;\#&gt; Equipment List Name
-
-This alpha field contains the identifying name for the Equipment List (i.e., the name of a PlantEquipmentList or CondenserEquipmentList object).
-
-An example of these statements in an IDF is:
-
-```idf
-PlantEquipmentOperation:CoolingLoad, Peak Operation,
-        0,7000,   Chiller Plant,
-        7000,24500,   Chiller Plant and Purchased,
-        24500,500000, Purchased Only;
-```
-
-This particular load based operation scheme (above) has three different ranges. “Chiller Plant�, “Chiller Plant and Purchased�, and “Purchased Only� are names which link to various PlantEquipmentList or CondenserEquipmentList objects as described below. Gaps may be left in the load ranges specified, but to operate equipment over the entire range the upper limit of a given range must equal the lower limit of the next range as shown in the example. If gaps are left in the load ranges specified, a warning message will be issued when the load to be met falls within a load range “gap�. If the user wishes to leave a load range “gap� for a specific reason (no equipment to operate on this plant [or condenser] loop within this load range) and does not want the warning messages to be generated, then specify a lower limit, upper limit and equipment list name for the gap and do not specify any equipment in the associated equipment list, as shown below.
-
-```idf
-PlantEquipmentOperation:CoolingLoad, Peak Operation,
-    0,7000,   Chiller Plant,
-    7000,7100, NoEquipmentOperationOnThisPlantLoop,
-    7100,24500,   Chiller Plant and Purchased,
-    24500,500000, Purchased Only;
-
-PlantEquipmentList,
-    Chiller Plant,           !- Name
-    Chiller:Electric,        !- Equipment 1 Object Type
-    Big Chiller;             !- Equipment 1 Name
-
-PlantEquipmentList,
-    NoEquipmentOperationOnThisPlantLoop;    !- Name
-
-PlantEquipmentList,
-    Chiller Plant and Purchased,  !- Name
-    Chiller:Electric,        !- Equipment 1 Object Type
-    Big Chiller,             !- Equipment 1 Name
-    DistrictCooling,         !- Equipment 2 Object Type
-    Purchased Cooling;       !- Equipment 2 Name
-
-PlantEquipmentList,
-    Purchased Only,          !- Name
-    DistrictCooling,         !- Equipment 1 Object Type
-    Purchased Cooling;       !- Equipment 1 Name
-```
-
-### PlantEquipmentOperation:OutdoorDryBulb
-
-### PlantEquipmentOperation:OutdoorWetBulb
-
-### PlantEquipmentOperation:OutdoorRelativeHumidity
-
-### PlantEquipmentOperation:OutdoorDewpoint
-
-The outdoor operation objects define the different ranges of the various environmental parameters and which equipment list is valid for each range. After the keyword and the identifying name, a series of data trios is expected. In each trio, there is a lower limit for the load range, an upper limit for the load range, and a name that links to an equipment availability list (the CondenserEquipmentList).
-
-The fields for each of these are:
-
-#### Field: Name
-
-This alpha field contains the identifying name for the control scheme.
-
-#### Field Set: (Lower limit, Upper Limit, Equip List name) up to 10
-
-#### Field: &lt;specfic type&gt; Range &lt;\#&gt; Lower Limit
-
-This numeric field contains the lower limit (C for temperature operations, Percent for relative humidity operations) for the equipment list. If specific value is below this value, then this equipment list will not turn on to meet the demand.
-
-#### Field: &lt;specific type&gt; Range &lt;\#&gt; Upper Limit
-
-This numeric field contains the lower limit (C for temperature operations, Percent for relative humidity operations) for the equipment list. If specific value is above this value, then this equipment list will not turn on to meet the demand.
-
-#### Field: Range &lt;\#&gt; Equipment List Name
-
-This alpha field contains the identifying name for the Equipment List (i.e., the name of a CondenserEquipmentList object).
-
-### PlantEquipmentOperation:OutdoorDryBulbDifference
-
-### PlantEquipmentOperation:OutdoorWetBulbDifference
-
-### PlantEquipmentOperation:OutdoorDewpointDifference
-
-The Delta Temperature based control strategies help to control any condenser equipment based on the difference between a reference node temperature and any environmental temperature. For example a cooling tower can be controlled by a strategy, which looks at the difference between the tower inlet temperature and wet-bulb temperature. A difference range is specified for each equipment list. IDD excerpts are shown below:
-
-#### Field: Name
-
-This alpha value contains the identifying name of the control strategy. This name appears as ‘control scheme name’ in Condenser Operation Scheme object.
-
-#### Field: Reference Temperature Node Name
-
-This alpha value specifies the reference node for the operation scheme identified in the first field.
-
-#### Field Set: (Lower limit, Upper limit, Equipment List)
-
-#### Field: &lt;specfic type&gt; Range &lt;\#&gt; Lower Limit
-
-This numeric field specifies the minimum temperature difference required for the equipment specified in the equipment list to operate.
-
-#### Field: &lt;specfic type&gt; Range &lt;\#&gt; Upper Limit
-
-This numeric field specifies the maximum temperature difference below which the equipment specified in the equipment list is available.
-
-#### Field: Range &lt;\#&gt; Equipment List Name
-
-This alpha field contains the identifying name for the Equipment List (i.e., the name of a CondenserEquipmentList object).
-
-### PlantEquipmentOperation:ComponentSetpoint
-
-In addition to load range based control on the plant loop, sequencing the plant components based on the outlet temperature of individual equipment is allowed. This scheme is common to many present-day Energy Management Systems sequencing. In this scheme, the sequencing is done based on the order specified in the control object described below.
-
-#### Field: Name
-
-This field specifies the name of the operation scheme.
-
-#### Field Set: Equipment Object Type, Name, Demand Calculation Node, Setpoint Node, Flow Rate, Operation Type)
-
-#### Field: Equipment &lt;\#&gt; Object Type
-
-This field specifies the type of equipment controlled by scheme.
-
-#### Field: Equipment &lt;\#&gt; Name
-
-This field specifies the name of the controlled equipment.
-
-#### Field: Demand Calculation &lt;\#&gt; Node Name
-
-The component demand will be calculated using the difference between the temperature at the demand node and the component set point temperature.
-
-#### Field: Setpoint &lt;\#&gt; Node Name
-
-Each component controlled under temperature based control will have its own set point different from the loop set point. This field specifies component set point node (Generally its outlet temperatures). This node is acted upon by a SetpointManager in order to obtain the setpoint at any simulation timestep.
-
-#### Field: Component &lt;\#&gt; Flow Rate
-
-This numeric field specifies the design flow rate for the component specified in earlier fields. This flow rate is used to calculate the component demand. The field can be set to autosize, if the user wants the program to calculate the design flow. This would generally be set to autosize when the user does not know the component flow rate and does a sizing calculation for the corresponding component.
-
-#### Field: Operation&lt;\#&gt; Type
-
-This alpha field specifies the operation mode for the equipment. The equipment can be in any of the three modes viz. Cooling, Heating and Dual. Dual is used when the components both as heating and cooling equipment (for example heat pumps).
-
-
-
-
-
-And, as an example in an IDF:
-
-```idf
-PlantEquipmentOperationSchemes,
-    CW Loop Operation,       !- PlantOperationSchemeName
-    PlantEquipmentOperation:ComponentSetpoint, ! Control Scheme 1 Object Type
-    Test Scheme,                         !- Control Scheme 1 Name
-    On;                                  !- Control Scheme 1 Schedule
-
-PlantEquipmentOperation:ComponentSetpoint,
-    Test Scheme,
-    CHILLER:ELECTRIC,        !- Equipment 1 Object Type
-    Little Chiller,          !- Equipment 1 Name
-    Little Chiller Inlet Node, !- Demand Calculation 1 Node Name
-    Little Chiller Outlet Node, !- Setpoint 1 Node Name
-    0.0011,                     !- Component 1 Flow Rate
-    COOLING,                    !- Operation 1 Type
-    CHILLER:ELECTRIC,        !- Equipment 2 Object Type
-    Big Chiller,             !- Equipment 2 Name
-    Big Chiller Inlet Node,  !- Demand Calculation 2 Node Name
-    Big Chiller Outlet Node, !- Setpoint 2 Node Name
-    0.0011,                  !- Component 2 Flow Rate
-    COOLING;                 !- Operation 2 Type
-```
-
-### PlantEquipmentOperation:ThermalEnergyStorage
-
-Users of thermal energy storage, particularly ice storage systems, are often faced with a challenge of specifying input for these systems.  Essentially, they have to define various setpoint managers, temperature schedules, etc. in order to make the system functional.  This plant/condenser control type simplifies the input somewhat by eliminating both a setpoint manager and a schedule for each piece of equipment that makes up the ice storage system.  In fact, this operation scheme internally creates the setpoint managers required by the equipment listed as operated by the scheme defined by this syntax.  While the more complex definition is possible and provides more flexibility like hourly variation of setpoint temperatures at the outlet of each piece of equipment, this input provides the most convenient method for making the system to work and assumes a single charging setpoint temperature and a single discharging setpoint temperature.  For most systems, this is all that is needed.
-
-#### Field: Name
-
-This field defines the name of the thermal energy (ice) storage plant equipment operation scheme that will be referenced by the PlantEquipmentOperationSchemes list in the plant input.
-
-#### Field: On-Peak Schedule
-
-This field defines the name of an integer schedule that determines when on-peak electric pricing is in effect.  This value is used to determine whether or not the ice storage system should be charging the ice storage unit.  In the schedule, a value of 1 (or greater) corresponds to being in the on-peak period while any value of 0 or less corresponds to being in the off-peak period.
-
-#### Field: Charging Availability Schedule
-
-This field defines the name of an integer schedule that determines whether or not the system may enter charging mode off-peak.  If the current value of the on-peak schedule is “off�, then charging can take place if the charging availability schedule is “on�.  If the on-peak schedule is “off� and charging availability is “off�, then charging is not allowed and the chiller and ice storage units controlled by this statement are operating to meet the non-charging chilled water temperature defined by the next input parameter. In this schedule, a value of 1 (or greater) corresponds to “on� when charging is available during an off-peak period while any value of 0 or less corresponds to chillers not being allowed to charge even during off-peak.
-
-#### Field: Non-Charging Chilled Water Temperature
-
-This field defines the chilled water temperature when the ice storage system is NOT in charging mode.  During these times, the storage system could be discharging or dormant depending on HVAC load conditions and ice storage controls.  This value is used as the setpoint temperature for chillers associated with this plant equipment operation scheme during non-cooling season and during cooling season during the on-peak period.  The cooling season and on-peak periods are defined by schedules reference to input above.
-
-#### Field: Charging Chilled Water Temperature
-
-This field defines the chilled water temperature when the ice storage system is in charging mode.  During these times, the chiller is producing a temperature low enough to generate ice in the ice storage unit.  This value is used as the setpoint temperature for chillers associated with this plant equipment operation scheme during the cooling season during the off-peak period.  The cooling season and on-peak periods are defined by schedules reference to input above.
-
-#### Field Set: (Component Object Type, Name, Demand Calculation Node, Setpoint Node, Flow Rate, Operation Type)
-
-#### Field: Component &lt;\#&gt; Object Type
-
-This field specifies the type of equipment controlled by scheme.  This must be a thermal energy storage device (simple or detailed ice storage) or a chiller.
-
-#### Field: Component &lt;\#&gt; Name
-
-This field specifies the name of the controlled equipment.  This name must be defined in the input as a valid ice storage device or chiller.
-
-#### Field: Component &lt;\#&gt; Demand Calculation Node Name
-
-The component demand will be calculated using the difference between the temperature at the demand node and the component set point temperature.
-
-#### Field: Component &lt;\#&gt; Setpoint Node Name
-
-Each component controlled under temperature based control will have its own set point different from the loop set point. This field specifies component set point node (Generally its outlet temperatures). This node is acted upon by a SetpointManager in order to obtain the setpoint at any simulation timestep.
-
-#### Field: Component &lt;\#&gt; Flow Rate
-
-This numeric field specifies the design flow rate for the component specified in earlier fields.  This flow rate is used to calculate the component demand. The field can be set to autosize, if the user wants the program to calculate the design flow. This would generally be set to autosize when the user does not know the component flow rate and does a sizing calculation for the corresponding component.
-
-#### Field: Component &lt;\#&gt; Operation Type
-
-This alpha field specifies the operation mode for the equipment. The equipment can be in any of the three modes viz. Cooling, Heating and Dual. Dual is used when the components both as heating and cooling equipment (for example heat pumps).  Ice storage units can potentially either heat or cool the circulating fluid and thus should be defined as Dual mode.
-
-
-An example IDF is shown below:
-
-
-```idf
-  PlantEquipmentOperationSchemes,
-    CW Loop Operation,       !- Name
-    PlantEquipmentOperation:ThermalEnergyStorage,  !- Control Scheme 1 Object Type
-    Chiller and Partial Ice Storage,  !- Control Scheme 1 Name
-    PlantOnSched;            !- Control Scheme 1 Schedule Name
-
-  PlantEquipmentOperation:ThermalEnergyStorage,
-    Chiller and Partial Ice Storage,  !- Name
-    OnPeakEnergy,            !- On-Peak Schedule Name
-    ChargingAvail,           !- Charging Availability Schedule Name
-    7.22,                    !- Non-charging Chilled Water Temperature
-    -5.0,                    !- Charging Chilled Water Temperature
-    Chiller:Electric,        !- Component 1 Object Type
-    Central Chiller,         !- Component 1 Name
-    Central Chiller Inlet Node,  !- Component 1 Demand Calculation Node Name
-    Central Chiller Outlet Node,  !- Component 1 Setpoint Node Name
-    autosize,                !- Component 1 Flow Rate {m3/s}
-    COOLING,                 !- Component 1 Operation Type
-    ThermalStorage:Ice:Detailed,  !- Component 2 Object Type
-    Ice Tank,                !- Component 2 Name
-    Ice Tank Inlet Node,     !- Component 2 Demand Calculation Node Name
-    Ice Tank Outlet Node,    !- Component 2 Setpoint Node Name
-    0.13506E-02,             !- Component 2 Flow Rate {m3/s}
-    DUAL;                    !- Component 2 Operation Type
-```
-
-### PlantEquipmentList
-
-### CondenserEquipmentList
-
-The PlantEquipmentList  and CondenserEquipmentList  specify available plant and condenser loop equipment respectively for any loop operation scheme. Each statement contains the object name, an identifying name (which links the definition back to one of the operation scheme statements) and a variable length of data pairs. These pairs refer to a plant equipment type and an identifying name. The type in this list of pairs must correspond to a valid plant object as described in the next subsection.
-
-Note: If a PlantEquipmentList or CondenserEquipmentList object is specified with no equipment object types or equipment names, then the corresponding PlantEquipmentOperation:\* object will assume all available equipment on this plant (or condenser) loop should be OFF (not operate) within the specified lower/upper limit.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the Equipment List.
-
-#### Field Set: (Object Type, Name) up to 10
-
-Remember the order of equipment on this list determines operation priority. Equipment on the list first will try to meet demand first. These fields tie to the Equipment Definition input structure, which must also be defined.
-
-#### Field: Equipment &lt;\#&gt; Object Type
-
-This alpha field contains the keyword for the type of equipment in operation. Example: (Chiller:Electric, DistrictCooling). The full list of allowable plant equipment is valid plant objects as described in the next subsection.
-
-#### Field: Equipment &lt;\#&gt; Name
-
-This alpha field contains the identifying name for the equipment in operation. This distinguishes between two different pieces of equipment of the same type.
-
-An example of this statement in an IDF is:
-
-```idf
-PlantEquipmentList, Chiller Plant and Purchased,
-        Chiller:Electric, Big Chiller,
-        DistrictCooling, Purchased Cooling;
-```
-
-Note that this list is the middle range defined in the PlantEquipmentOperation:CoolingLoad statement named “Peak Operation� above. This defines the equipment available when the load encountered by the plant (chiller water demand, for example) is between 7000 W and 24500 W. EnergyPlus will run the “Big Chiller� first up to its capacity and then attempt to meet the remaining load (while in that range) with the next piece of equipment (in this case, “Purchased:Cooling�) in the list.
-
-Group – Plant Equipment
------------------------
-
-### Equipment Types
-
-In each **PlantEquipmentList** described using the above syntax, various equipment types and names must be given. Each type-name pair must then have a corresponding equipment definition. This subsection lists the various equipment types that are available and examples from an IDF. Where appropriate, notes and comments on the input structure are provided.
-
-### Generic Chiller Outputs
-
-Many output variable names are common across all chiller types. These generic chiller output names all begin with the word "Chiller". Certain chiller types have additional output variables which are specific to that type of chiller. Chiller energy use is added to the appropriate plant-level meters as a cooling end-use.
-
-* HVAC,Average,Chiller Electric Power [W]
-
-* HVAC,Sum,Chiller Electric Energy [J]
-
-* Zone,Meter,Electricity:Plant [J]
-
-* Zone,Meter,Cooling:Electricity [J]
-
-* HVAC,Average,Chiller Evaporator Cooling Rate [W]
-
-* HVAC,Sum,Chiller Evaporator Cooling Energy [J]
-
-* Zone,Meter,EnergyTransfer:Plant [J]
-
-* Zone,Meter,Chillers:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Evaporator Inlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Outlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Condenser Heat Transfer Rate [W]
-
-* HVAC,Sum,Chiller Condenser Heat Transfer Energy [J]
-
-* Zone,Meter,HeatRejection:EnergyTransfer [J]
-
-* HVAC,Average,Chiller COP [W/W]
-
-
-The following output is applicable only for air-cooled or evap-cooled chillers
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-
-The following outputs are applicable only for evap-cooled chillers
-
-* HVAC,Average,Chiller Basin Heater Electric Power [W]
-
-* HVAC,Average,Chiller Basin Heater Electric Energy [J]
-
-
-The following three outputs are only available for water-cooled chillers
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Outlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Drive Shaft Power [W]
-
-* HVAC,Sum,Chiller Drive Shaft Energy [J]
-
-* Zone,Meter,HeatRecovery:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Lube Recovered Heat Rate [W]
-
-* HVAC,Sum,Chiller Lube Recovered Heat Energy [J]
-
-* HVAC,Average,Chiller Jacket Recovered Heat Rate [W]
-
-* HVAC,Sum,Chiller Jacket Recovered Heat Energy [J]
-
-* HVAC,Average, Chiller Exhaust Recovered Heat Rate [W]
-
-* HVAC,Sum,Chiller Exhaust Recovered Heat Energy [J]
-
-* HVAC,Average,Chiller Total Recovered Heat Rate [W]
-
-* HVAC,Sum,Chiller Total Recovered Heat Energy [J]
-
-* HVAC,Average,Chiller Exhaust Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Effective Heat Rejection Temperature [C]
-
-
-The following blocks of outputs are for steam and fuel-driven chillers
-
-* HVAC,Average,Chiller Gas Rate [W]
-
-* HVAC,Sum,Chiller Gas Energy [J]
-
-* HVAC,Average,Chiller Gas Mass Flow Rate [kg/s]
-
-* HVAC,Sum,Chiller Gas Mass [kg]
-
-
-For steam absorption chillers:
-
-* HVAC,Average,Chiller Source Steam Rate [W]
-
-* HVAC,Sum, Chiller Source Steam Energy [J]
-
-* HVAC,Average,Chiller Steam Mass Flow Rate [kg/s]
-
-
-For hot water absorption chillers:
-
-* HVAC,Average,Chiller Source Hot Water Rate [W]
-
-* HVAC,Sum,Chiller Source Hot Water Energy [J]
-
-* Zone,Meter,Steam:Plant [J]
-
-* Zone,Meter,Cooling:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Hot Water Mass Flow Rate [kg/s]
-
-
-The following output is applicable only for indirect absorption chillersHVAC,Average,Chiller Part Load Ratio
-
-* HVAC,Average,Chiller Cycling Ratio []
-
-* HVAC,Average,Chiller Propane Rate [W]
-
-* HVAC,Sum,Chiller Propane Energy [J]
-
-* HVAC,Average,Chiller Propane Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Diesel Rate [W]
-
-* HVAC,Sum,Chiller Diesel Energy [J]
-
-* HVAC,Average,Chiller Diesel Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Gasoline Rate [W]
-
-* HVAC,Sum,Chiller Gasoline Energy [J]
-
-* HVAC,Average,Chiller Gasoline Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller FuelOil\#1 Rate [W]
-
-* HVAC,Sum,Chiller FuelOil\#1 Energy [J]
-
-* HVAC,Average,Chiller FuelOil\#1 Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller FuelOil\#2 Rate [W]
-
-* HVAC,Sum,Chiller FuelOil\#2 Energy [J]
-
-* HVAC,Average,Chiller FuelOil\#2 Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller OtherFuel1 Rate [W]
-
-* HVAC,Sum,Chiller OtherFuel1 Energy [J]
-
-* HVAC,Average,Chiller OtherFuel1 Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller OtherFuel2 Rate [W]
-
-* HVAC,Sum,Chiller OtherFuel2 Energy [J]
-
-* HVAC,Average,Chiller OtherFuel2 Mass Flow Rate [kg/s]
-
-
-#### Chiller Electric Power [W]
-
-#### Chiller Electric Energy [J]
-
-These outputs are the electric power input to the chiller. In the case of steam or fuel-powered chillers, this repesents the internal chiller pumps and other electric power consumption. Consumption is metered on Cooling:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Chiller Evaporator Cooling Rate [W]
-
-#### Chiller Evaporator Cooling Energy [J]
-
-These outputs are the evaporator heat transfer which is the cooling delivered by the chiller. Chiller Evaporator Cooling Energy is metered on Chillers:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Chiller Evaporator Inlet Temperature [C]
-
-#### Chiller Evaporator Outlet Temperature [C]
-
-#### Chiller Evaporator Mass Flow Rate [kg/s]
-
-These outputs are the evaporator (chilled water) inlet and outlet temperatures and flow rate.
-
-#### Chiller COP [W/W]
-
-This output is the coefficient of performance for the chiller during cooling operation. It is calculated as the evaporator heat transfer rate (Chiller Evaporator Cooling Rate) divided by the “fuel� consumption rate by the chiller. For the constant COP and electric chillers, the “fuel� is electricity so the divisor is Chiller Electric Power [W]. For the absorption chiller, the “fuel� is steam so the divisor is Steam Consumption Rate [W].
-
-*Note that this variable is reported as zero when the chiller is not operating. When reported for frequencies longer than "detailed" (such as timestep, hourly, daily, monthly or environment), this output will only be meaningful when the chiller is operating for the entire reporting period. To determine an average COP for a longer time period, compute the COP based on total evaporator heat transfer divided by total electric or fuel input over the desired period.*
-
-#### Chiller Part Load Ratio
-
-This output is the operating part-load ratio of the indirect absorption chiller. This output may fall below the minimum part-load ratio specified in the input. For this case, the Chiller Cycling Ratio is used to further define the performance of the indirect absorption chiller.
-
-#### Chiller Cycling Ratio
-
-This output is the fraction of the timestep the indirect absorption chiller operates. When the chiller operates above the minimum part-load ratio, a Chiller Cycling Ratio of 1 is reported. When the chiller operates below the minimum part-load ratio, the Chiller Cycling Ratio reports the fraction of the timestep the indirect absorption chiller operates.
-
-#### Chiller Condenser Heat Transfer Rate [W]
-
-#### Chiller Condenser Heat Transfer Energy [J]
-
-These outputs are the condenser heat transfer which is the heat rejected from the chiller to either a condenser water loop or through an air-cooled condenser. Chiller Condenser Heat Transfer Energy is metered on HeatRejection:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Chiller Condenser Inlet Temperature [C]
-
-This output is the condenser (heat rejection) inlet temperature for air-cooled or evap-cooled chillers. For an air-cooled chiller, this output would be the dry-bulb temperature of the air entering the condenser coil. For an evap-cooled chiller, this output would be the wet-bulb temperature of the air entering the evaporatively-cooled condenser coil.
-
-#### Chiller Basin Heater Electric Power [W]
-
-#### Chiller Basin Heater Electric Energy [J]
-
-These outputs are the electric power input to the chiller’s basin heater (for evaporatively-cooled condenser type). Consumption is metered on Chillers:Electricity, Electricity:Plant, and Electricity:Facility
-
-#### Chiller Condenser Inlet Temperature [C]
-
-#### Chiller Condenser Outlet Temperature [C]
-
-#### Chiller Condenser Mass Flow Rate [kg/s]
-
-These outputs are the condenser (heat rejection) inlet and outlet temperatures and flow rate for water-cooled chillers.
-
-#### Chiller Drive Shaft Power [W]
-
-#### Chiller Drive Shaft Energy [J]
-
-For engine-driven and turbine-driven chillers, these outputs are the shaft power produced by the prime mover and transferred to the chiller compressor.
-
-#### Chiller Lube Recovered Heat Rate [W]
-
-#### Chiller Lube Recovered Heat Energy [J]
-
-#### Chiller Jacket Recovered Heat Rate [W]
-
-#### Chiller Jacket Recovered Heat Energy [J]
-
-#### Chiller Exhaust Recovered Heat Rate [W]
-
-#### Chiller Exhaust Recovered Heat Energy [J]
-
-#### Chiller Total Recovered Heat Rate [W]
-
-#### Chiller Total Recovered Heat Energy [J]
-
-For chillers with heat recovery, such as engine-driven chillers, these outputs are the components of recoverable energy available. For a given chiller type, one or more of the following components may be applicable:  Lube (engine lubricant), Jacket (engine coolant), Exhaust (engine exhaust), and Total. Chiller Lube Recovered Heat Energy, Chiller Jacket Recovered Heat Energy, and Chiller Exhaust Heat Recovery Energy are metered on HeatRecovery:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Chiller Exhaust Temperature [C]
-
-This is the exhaust temperature leaving an engine chiller.
-
-#### Chiller Heat Recovery Inlet Temperature [C]
-
-#### Chiller Heat Recovery Outlet Temperature [C]
-
-#### Chiller Heat Recovery Mass Flow Rate [kg/s]
-
-These outputs are the heat recovery inlet and outlet temperatures and flow rate for chillers with heat recovery such as engine-driven and gas turbine chillers.
-
-#### Chiller Effective Heat Rejection Temperature [C]
-
-This output variable is available for heat recovery chillers that model split bundle condenser.  The condenser fluid temperatures used to characterize chiller performance are modified to account for the temperature of the heat recovery fluid.  This output is the resulting temperature used for characterizing chiller performance and is a blend of the temperatures in the condenser and heat recovery fluid streams.  For the Chiller:Electric and Chiller:Electric:EIR models, this is an effective inlet temperature while for the Chiller:Electric:ReformulatedEIR model, this is an effective outlet temperature.
-
-#### Chiller &lt;Fuel Type&gt; Rate [W]
-
-#### Chiller &lt;Fuel Type&gt; Energy  [J]
-
-#### Chiller  &lt;Fuel Type&gt; Mass Flow Rate [kg/s]
-
-#### Chiller Gas  Mass [kg] (Gas Turbine Chiller only)
-
-These outputs are the steam or fuel input for steam or fuel-fired chillers. Valid fuel types depend on the type of chiller. &lt;Fuel Type&gt; may be one of:  Gas (natural gas), Steam, Propane, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1 and OtherFuel2. Consumption is metered on Cooling:&lt;Fuel Type&gt;, &lt;Fuel Type&gt;:Plant, and &lt;Fuel Type&gt;:Facility.
-
-#### Chiller Source Hot Water Rate [W]
-
-#### Chiller Source Hot Water Energy [J]
-
-#### Chiller Source Steam Rate [W]
-
-### Chiller:Absorption
-
-#### Field: Name
-
-This alpha field contains the identifying name for the absorption chiller.
-
-#### Field: Nominal Capacity
-
-This numeric field contains the nominal cooling capability of the chiller in Watts.
-
-#### Field: Nominal Pumping Power
-
-This numeric field contains the nominal pumping power of the absorber in Watts.
-
-#### Field: Chilled Water Inlet Node Name
-
-This required alpha field contains the identifying name for the absorption chiller plant side inlet node.
-
-#### Field: Chilled Water Outlet Node Name
-
-This required alpha field contains the identifying name for the absorption chiller plant side outlet node.
-
-#### Field: Condenser Inlet Node Name
-
-This required alpha field contains the identifying name for the absorption chiller condenser side inlet node.
-
-#### Field: Condenser Outlet Node Name
-
-This required alpha field contains the identifying name given to the Heat Recovery Loop Component Outlet Node.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the absorption chiller’s minimum part load ratio. The expected range is between 0 and 1. The minimum part load is not the load where the machine shuts off, but where the amount of power remains constant to produce smaller loads than this fraction.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the absorption chiller’s maximum part load ratio. This value may exceed 1, but the normal range is between 0 and 1.1.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the absorption chiller’s optimum part load ratio. This is the part load ratio at which the chiller performs at its maximum COP.
-
-#### Field: Design Condenser Inlet Temperature
-
-This numeric field contains the absorption chiller’s condenser inlet design temperature in Celsius.
-
-#### Field: Design Chilled Water Flow Rate
-
-For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate. The units are in cubic meters per second.
-
-#### Field: Design Condenser Water Flow Rate
-
-This numeric field contains the absorption chiller’s design condenser water flow rate in cubic meters per second.
-
-#### Generator Heat Input Part Load Ratio Curve
-
-The Generator Heat Input Part Load Ratio Curve is a quadratic equation that determines the Ratio of the generator load on the absorber to the demand on the chiller. The defining equation is:
-
-<div>\[SteamInputRatio = \frac{{C1}}{{PLR}} + C2 + C3 * PLR\]</div>
-
-The following three fields contain the coefficients for the equation.
-
-#### Field: Coefficient 1 of the Steam Use Part Load Ratio Curve
-
-C1 in the Generator Heat Input Part Load Ratio Curve. This value is obtained by fitting manufacturers’ performance data to the curve.
-
-#### Field: Coefficient 2 of the Steam Use Part Load Ratio Curve
-
-C2 in the Generator Heat Input Part Load Ratio Curve. This value is obtained by fitting manufacturers’ performance data to the curve.
-
-#### Field: Coefficient 3 of the Steam Use Part Load Ratio Curve
-
-C3 in the Generator Heat Input Part Load Ratio Curve. This value is obtained by fitting manufacturers’ performance data to the curve.
-
-#### Pump Electric Use Part Load Ratio Curve
-
-The Pump Electric Use Part Load Ratio Curve is a quadratic equation that determines the Ratio of  the actual absorber pumping power to the nominal pumping power. The defining equation is:
-
-<div>\[ElectricInputRatio = C1 + C2 * PLR + C3 * PL{R^2}\]</div>
-
-The following three fields contain the coefficients for the equation.
-
-#### Field: Coefficient 1 of the Pump Electric Use Part Load Ratio Curve
-
-C1 in the Pump Electric Use Part Load Ratio Curve. This value is obtained by fitting manufacturers’ performance data to the curve.
-
-#### Field: Coefficient 2 of the Pump Electric Use Part Load Ratio Curve
-
-C2 in the Pump Electric Use Part Load Ratio Curve. This value is obtained by fitting manufacturers’ performance data to the curve.
-
-#### Field: Coefficient 3 of the Pump Electric Use Part Load Ratio Curve
-
-C3 in the Pump Electric Use Part Load Ratio Curve. This value is obtained by fitting manufacturers’ performance data to the curve.
-
-#### Field: Chilled Water Outlet Temperature Lower Limit
-
-This numeric field contains the lower limit for the evaporator outlet temperature. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn’t get too cold.
-
-#### Field: Generator Inlet Node Name
-
-This alpha field contains the identifying name given to the Generator Inlet Node. A steam or hot water loop is not required to simulate an absorption chiller. If a steam/hot water loop is used, enter the name of the generator inlet node.
-
-#### Field: Generator Outlet Node Name
-
-This alpha field contains the identifying name given to the Generator Outlet Node. A steam or hot water loop is not required to simulate an absorption chiller. If a steam/hot water loop is used, enter the name of the generator outlet node.
-
-#### Field: Chiller Flow Mode
-
-This choice field determines how the chiller operates with respect to the intended fluid flow through the device’s evaporator.  There are three different choices for specifying operating modes for the intended flow behavior:  “NotModulated,� “ConstantFlow,� and “LeavingSetpointModulated.�  NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.  ConstantFlow is useful for constant speed pumping arrangements where the chiller’s request for flow is stricter and can increase the overall loop flow.  LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint at the evaporator outlet.  For this absorption chiller, this mode also affects the flow rate on the generator connection.  In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.  The default, if not specified, is NotModulated.  This flow mode does not impact the condenser loop connection.
-
-#### Field: Generator Fluid Type
-
-This choice field specifies the type of fluid used to heat the generator solution. The valid choices are **HotWater** or **Steam**. This field should be specified as Steam or left blank if the generator inlet/outlet nodes are not specified.
-
-#### Field: Design Generator Fluid Flow Rate
-
-This numeric field contains the absorption chiller’s design condenser fluid flow rate in cubic meters per second.
-
-#### Field: Degree of Subcooling in Steam Generator
-
-Ideally, the steam trap located at the outlet of the generator should remove all the condensate immediately, however, there is a delay in this process in actual systems which causes the condensate to SubCool by a certain amount before leaving the generator. This amount of subcooling is included in the heat transferred to the solution in the generator. The minimum value is 0º Celsius and default is 5º Celsius. This field is not used when the generator inlet/outlet node are not specified or the generator is connected to a hot water loop.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Nominal Pumping Power, Design Chilled Water Flow Rate, Design Condenser Water Flow Rate and Design Generator Fluid Flow Rate. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-Following is an example input for an Absorption Chiller.
-
-```idf
-Chiller:Absorption,
-    Big Chiller,             !- Chiller Name
-    50000,                   !- Nominal Capacity {W}
-    250,                     !- Nominal Pumping Power {W}
-    Big Chiller Inlet Node,  !- Plant_Side_Inlet_Node
-    Big Chiller Outlet Node, !- Plant_Side_Outlet_Node
-    Big Chiller Condenser Inlet Node,  !- Condenser_Side_Inlet_Node
-    Big Chiller Condenser Outlet Node,  !- Condenser_Side_Outlet_Node
-    0.15,                    !- Minimum Part Load Ratio
-    1.0,                     !- Maximum Part Load Ratio
-    0.65,                    !- Opt Part Load Ratio
-    35.0,                    !- Temp Design Condenser Inlet {C}
-    0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
-    0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
-    0.03303,                 !- Coefficient1 of the steam use part load ratio curve
-    0.6852,                  !- Coefficient2 of the steam use part load ratio curve
-    0.2818,                  !- Coefficient3 of the steam use part load ratio curve
-    1.0,                     !- Coefficient1 of the pump electric use part load ratio curve
-    0,                       !- Coefficient2 of the pump electric part load ratio curve
-    0,                       !- Coefficient3 of the pump electric use part load ratio curve
-    5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
-    AbsorberSteamInletNode,  !- Generator Inlet Node Name
-    AbsorberSteamOutletNode, !- Generator Outlet Node Name
-    VariableFlow,            !- Chiller Flow Mode
-    Steam,                   !- Generator Fluid Type
-    autosize,                !- Design Generator Volumetric Fluid Flow Rate {m3/s}
-    2.0;                     !- Degree of Subcooling in Steam Generator {C}
-```
-
-
-### Absorption Chiller Outputs
-
-* HVAC,Average,Chiller Electric Power [W]
-
-* HVAC,Sum,Chiller Electric Energy [J]
-
-* Zone,Meter,Electricity:Plant [J]
-
-* Zone,Meter,Cooling:Electricity [J]
-
-* HVAC,Average,Chiller Evaporator Cooling Rate [W]
-
-* HVAC,Sum,Chiller Evaporator Cooling Energy [J]
-
-* Zone,Meter,EnergyTransfer:Plant [J]
-
-* Zone,Meter,Chillers:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Evaporator Inlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Outlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Condenser Heat Transfer Rate [W]
-
-* HVAC,Sum,Chiller Condenser Heat Transfer Energy [J]
-
-* Zone,Meter,HeatRejection:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Outlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller COP [W/W]
-
-
-For Chillers with Steam Generators:
-
-* HVAC,Average, Chiller Source Steam Rate [W]
-
-* HVAC,Sum, Chiller Source Steam Energy [J]
-
-* HVAC,Average,Chiller Steam Mass Flow Rate [kg/s]
-
-
-For Chillers with Hot Water Generators:
-
-* HVAC,Average,Chiller Source Hot Water Rate [W]
-
-* HVAC,Sum,Chiller Source Hot Water Energy [J]
-
-* HVAC,Average,Chiller Hot Water Mass Flow Rate [kg/s]
-
-These chiller output variables are defined above under "Generic Chiller Outputs."
-
-
-### Chiller:Absorption:Indirect
-
-The Chiller:Absorption:Indirect object is an enhanced version of the absorption chiller model found in the Building Loads and System Thermodynamics (BLAST) program. This enhanced model is nearly identical to the existing absorption chiller model (Ref. Chiller:Absorption) with the exceptions that: 1) the enhanced indirect absorption chiller model provides more flexible performance curves and 2) chiller performance now includes the impact of varying evaporator, condenser, and generator temperatures. Since these absorption chiller models are nearly identical (i.e., the performance curves of the enhanced model can be manipulated to produce similar results to the previous model), it is quite probable that the Chiller:Absorption model will be deprecated in a future release of EnergyPlus.
-
-#### Field: Name
-
-This required alpha field contains the identifying name for the indirect absorption chiller.
-
-#### Field: Nominal Capacity
-
-This required numeric field contains the nominal cooling capability of the chiller in Watts. This field must be greater than 0 and is autosizable.
-
-#### Field: Nominal Pumping Power
-
-This required numeric field contains the nominal pumping power of the chiller in Watts. The minimum value for this field is 0 and is autosizable.
-
-#### Field: Chilled Water Inlet Node Name
-
-This required alpha field contains the identifying name for the chiller chilled water inlet node.
-
-#### Field: Chilled Water Outlet Node Name
-
-This required alpha field contains the identifying name for the chiller chilled water outlet node.
-
-#### Field: Condenser Inlet Node Name
-
-This required alpha field contains the identifying name for the chiller condenser inlet node.
-
-#### Field: Condenser Outlet Node Name
-
-This required alpha field contains the identifying name given to the chiller outlet node.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the chiller’s minimum part-load ratio. The expected range is between 0 and 1. The minimum part load is not the load where the machine shuts off, but where the amount of power remains constant to produce smaller loads than this fraction.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the chiller’s maximum part-load ratio. This value may exceed 1, but the normal range is between 0 and 1.1.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the chiller’s optimum part-load ratio. This is the part-load ratio at which the chiller performs at its maximum COP.
-
-#### Field: Design Condenser Inlet Temperature
-
-This numeric field contains the chiller’s condenser inlet design temperature in Celsius. The default value for this field is 30º C and is only used when the Design Chilled Water Flow Rate is autosized.
-
-#### Field: Condenser Inlet Temperature Lower Limit
-
-This numeric field contains the chiller’s lower limit for the condenser entering water temperature in Celsius. The default value for this field is 15º C. If this limit is exceeded, a warning message will report the incident. No correction to chiller capacity is made for low condenser entering water temperatures.
-
-#### Field: Chilled Water Outlet Temperature Lower Limit
-
-This numeric field contains the chiller’s lower limit for the evaporator leaving water temperature in Celsius. The default value for this field is 5º C. If this limit is exceeded, a warning message will report the incident. No correction to chiller capacity is made for low evaporator leaving water temperatures.
-
-#### Field: Design Chilled Water Flow Rate
-
-This numeric input specifies the design evaporator volumetric flow rate in cubic meters per second. The value specified must be greater than 0 or this field is autosizable. For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate.
-
-#### Field: Design Condenser Water Flow Rate
-
-This numeric field specifies the chiller’s design condenser water flow rate in cubic meters per second. The value specified must be greater than 0 or this field is autosizable.
-
-#### Field: Chiller Flow Mode
-
-This choice field determines how the chiller operates with respect to the intended fluid flow through the device’s evaporator.  There are three different choices for specifying operating modes for the intended flow behavior:  “NotModulated,� “ConstantFlow,� and “LeavingSetpointModulated.�  NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.  ConstantFlow is useful for constant speed pumping arrangements where the chiller’s request for flow is stricter and can increase the overall loop flow.  LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint at the evaporator outlet.  For this absorption chiller, this mode also affects the flow rate on the generator connection.  In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.  The default, if not specified, is NotModulated.  This flow mode does not impact the condenser loop connection.
-
-#### Field: Generator Heat Input Function of Part Load Ratio Curve Name
-
-This required alpha field specifies the name of the curve used to determine the heat input to the chiller. The curve is a quadratic or cubic curve which characterizes the heat input as a function of chiller part-load ratio. The curve output is multiplied by the chiller’s nominal capacity and operating part-load ratio or minimum part-load ratio, whichever is greater, to determine the amount of heat input required for the given operating conditons.
-
-#### Field: Pump Electric Input Function of Part Load Ratio Curve Name
-
-This alpha field specifies the name of the curve used to determine the pump electrical input to the chiller. The curve is a quadratic or cubic curve which characterizes the pump electrical power as a function of chiller part-load ratio. The curve output is multiplied by the chiller’s nominal pumping power and operating part-load ratio or minimum part-load ratio, whichever is greater, to determine the amount of pumping power required for the given operating conditons.
-
-#### Field: Generator Inlet Node Name
-
-This alpha field contains the identifying name given to the Generator Inlet Node. A steam or hot water loop is not required to simulate an indirect absorption chiller. If a steam/hot water loop is used, enter the name of the generator inlet node.
-
-#### Field: Generator Outlet Node Name
-
-This alpha field contains the identifying name given to the Generator Outlet Node. A steam or hot water loop is not required to simulate an indirect absorption chiller. If a steam/hot water loop is used, enter the name of the generator outlet node.
-
-#### Field: Capacity Correction Function of Condenser Temperature Curve Name
-
-This alpha field specifies the name of a quadratic or cubic curve which correlates the chiller’s evaporator capacity as a function of condenser entering water temperature. This curve is used to correct nominal capacity at off-design condensing temperatures.
-
-#### Field: Capacity Correction Function of Chilled Water Temperature Curve Name
-
-This alpha field specifies the name of a quadratic or cubic curve which correlates the chiller’s evaporator capacity as a function of evaporator leaving water temperature. This curve is used to correct nominal capacity at off-design evaporator temperatures.
-
-#### Field: Capacity Correction Function of Generator Temperature Curve Name
-
-This alpha field specifies the name of a quadratic or cubic curve which correlates the chiller’s evaporator capacity as a function of generator entering water temperature. This curve is used to correct nominal capacity at off-design evaporator temperatures and is only used when the Generator Fluid Type is specified as Hot Water.
-
-#### Field: Generator Heat Input Correction Function of Condenser Temperature Curve Name
-
-This alpha field specifies the name of a quadratic or cubic curve which correlates the chiller’s heat input as a function of condenser entering water temperature. This curve is used to correct generator heat input at off-design condensing temperatures.
-
-#### Field: Generator Heat Input Correction Function of Chilled Water Temperature Curve Name
-
-This alpha field specifies the name of a quadratic or cubic curve which correlates the chiller’s heat input as a function of evaporator leaving water temperature. This curve is used to correct generator heat input at off-design evaporator temperatures.
-
-#### Field: Generator Heat Source Type
-
-This choice field specifies the type of fluid used to heat the generator solution. The valid choices are **HotWater** or **Steam**. This input is used to identify the method used to calculate the generator mass flow rate. This field is not used if the generator inlet/outlet nodes are not specified. The default value is Steam.
-
-#### Field: Design Generator Fluid Flow Rate
-
-This numeric field specifies the chiller’s design generator *fluid* flow rate in cubic meters per second. The value specified must be greater than 0 or this field is autosizable. For variable flow chillers this is the maximum generator flow rate, for constant flow chillers this is the flow rate.
-
-#### Field: Temperature Lower Limit Generator Inlet
-
-This numeric field specifies the lower limit of the generator’s entering water temperature. This field is not used iif the Generator Fluid Type is specified as steam.
-
-#### Field: Degree of Subcooling in Steam Generator
-
-Ideally the steam trap located at the outlet of generator should remove all the condensate immediately, however there is a delay in this process in actual systems which causes the condensate to SubCool by a certain degree before leaving the generator. This amount of subcooling is included in the heat transferred to the solution in the generator. The minimum value is 0º Celsius, the maximum value is 20º Celsius, and the default is 1º Celsius.
-
-#### Field: Degree of Subcooling in Steam Condensate Loop
-
-This essentially represents the heat loss to the atmosphere due to uninsulated condensate return piping to the boiler. Condensate return piping operates at atmospheric pressure and is not insulated. The condensate sub cools to certain degree before it is pumped back to the boiler. The minimum value is 0º Celsius and the default is 0º Celsius.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Nominal Pumping Power, Design Chilled Water Flow Rate, Design Condenser Water Flow Rate and Design Generator Fluid Flow Rate. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-Following is an example input for an Absorption Chiller.
-
-```idf
-Chiller:Absorption:Indirect,
-    Big Chiller,             !- Chiller Name
-    100000,                  !- Nominal Capacity {W}
-    250,                     !- Nominal Pumping Power {W}
-    Big Chiller Inlet Node,  !- Evaporator Inlet Node Name
-    Big Chiller Outlet Node, !- Evaporator Outlet Node Name
-    Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
-    Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
-    0.15,                    !- Minimum Part Load Ratio
-    1.0,                     !- Maximum Part Load Ratio
-    0.65,                    !- Opt Part Load Ratio
-    35.0,                    !- Temp Design Condenser Inlet {C}
-    10.0,                    !- Temp Lower Limit Condenser Inlet {C}
-    5.0,                     !- Chilled Water Outlet Temperature Lower Limit {C}
-    0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
-    0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
-    VariableFlow,            !- Chiller Flow Mode
-    SteamUseFPLR,            !- Generator Heat Input function of part-load ratio curve name
-    PumpUseFPLR,             !- Pump Electric Input function of part-load ratio curve name
-    AbsorberSteamInletNode,  !- Generator Inlet Node Name
-    AbsorberSteamOutletNode, !- Generator Outlet Node Name
-    CAPfCOND,                !- Capacity Correction function of condenser temperature curve name
-    CAPfEVAP,                !- Capacity Correction function of evaporator temperature curve name
-    ,                        !- Capacity Correction function of generator temperature curve name
-    SteamFCondTemp,       !- Generator Heat Input Correction function of condenser temperature curve name
-    SteamFEvapTemp,       !- Generator Heat Input Correction function of evaporator temperature curve name
-    Steam,                   !- Generator Heat Source Type
-    autosize,                !- Design Generator Volumetric Fluid Flow Rate {m3/s}
-    30.0,                    !- Temp Lower Limit Generator Inlet {C}
-    2.0,                     !- Degree of Subcooling in Steam Generator {C}
-    12.0;                    !- Degree of Subcooling in Steam Condensate Loop {C}
-```
-
-
-
-### Indirect Absorption Chiller Outputs
-
-* HVAC,Average,Chiller Electric Power [W]
-
-* HVAC,Sum,Chiller Electric Energy [J]
-
-* Zone,Meter,Electricity:Plant [J]
-
-* Zone,Meter,Cooling:Electricity [J]
-
-* HVAC,Average,Chiller Evaporator Cooling Rate [W]
-
-* HVAC,Sum,Chiller Evaporator Cooling Energy [J]
-
-* Zone,Meter,EnergyTransfer:Plant [J]
-
-* Zone,Meter,Chillers:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Evaporator Inlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Outlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Condenser Heat Transfer Rate [W]
-
-* HVAC,Sum,Chiller Condenser Heat Transfer Energy [J]
-
-* Zone,Meter,HeatRejection:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Outlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller COP [W/W]
-
-* HVAC,Average,Chiller Part-Load Ratio
-
-* HVAC,Average,Chiller Cycling Ratio
-
-
-
-For Chillers with Steam Generators:
-
-* HVAC,Average, Chiller Source Steam Rate [W]
-
-* HVAC,Sum, Chiller Source Steam Energy [J]
-
-* Zone,Meter,Steam:Plant [J]
-
-* Zone,Meter,Cooling:Steam [J]
-
-* HVAC,Average, Chiller Steam Mass Flow Rate [kg/s]
-
-* HVAC,Average, Chiller Steam Heat Loss Rate [W]
-
-
-
-For Chillers with Hot Water Generators:
-
-* HVAC,Average, Chiller Source Hot Water Rate [W]
-
-* HVAC,Sum, Chiller Source Hot Water Energy [J]
-
-* Zone,Meter,EnergyTransfer:Plant [J]
-
-* Zone,Meter,Cooling:EnergyTransfer [J]
-
-* HVAC,Average, Chiller Hot Water Mass Flow Rate [kg/s]
-
-These chiller output variables are defined above under "Generic Chiller Outputs."
-
-### Chiller:ConstantCOP
-
-This chiller model is based on a simple, constant COP simulation of the chiller. In this case, performance does not vary with chilled water temperature or condenser conditions.
-
-Such a model is useful when the user does not have access to detailed performance data.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the constant COP chiller.
-
-#### Field: Nominal Capacity
-
-This numeric field contains the nominal cooling capability of the chiller in Watts.
-
-#### Field: Nominal COP
-
-This numeric field contains the Chiller’s coefficient of performance.
-
-#### Field: Design Chilled Water Flow Rate
-
-For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate. The units are in cubic meters per second.
-
-#### Field: Design Condenser Water Flow Rate
-
-This numeric field contains the electric chiller’s design condenser water flow rate in cubic meters per second. This field is autosizable. This field is not used for Condenser Type = AirCooled or EvaporativelyCooled.
-
-#### Field: Chilled Water Inlet Node Name
-
-This required alpha field contains the identifying name for the constant COP chiller plant side inlet node.
-
-#### Field: Chilled Water Outlet Node Name
-
-This required alpha field contains the identifying name for the constant COP chiller plant side outlet node.
-
-#### Field: Condenser Inlet Node Name
-
-This alpha field contains the identifying name for the constant COP chiller condenser side inlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and a condenser inlet node name is specified here, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates an outdoor air node and the air temperature information on this node is taken directly from the weather file (no node height adjustment).
-
-#### Field: Condenser Outlet Node Name
-
-This alpha field contains the identifying name for the constant COP chiller condenser side outlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates a condenser side outlet air node.
-
-#### Field: Condenser Type
-
-This alpha field determines what type of condenser will be modeled with this chiller. The 3 type of condensers are AirCooled, WaterCooled, and EvaporativelyCooled with the default being AirCooled if not specified. AirCooled and EvaporativelyCooled do not require a CondenserLoop to be specified, whereas the WaterCooled option requires the full specification of the CondenserLoop and its associated equipment.
-
-#### Field: Chiller Flow Mode
-
-This choice field determines how the chiller operates with respect to the intended fluid flow through the device’s evaporator.  There are three different choices for specifying operating modes for the intended flow behavior:  “NotModulated,� “ConstantFlow,� and “LeavingSetpointModulated.�  NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.  ConstantFlow is useful for constant speed pumping arrangements where the chiller’s request for flow is stricter and can increase the overall loop flow.  LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.  In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.  The default, if not specified, is NotModulated.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Design Chilled Water Flow Rate and Design Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the chiller’s electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the chiller is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the chiller is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the chiller is off.
-
-An example of this statement in an IDF is:
-
-```idf
-Chiller:ConstantCOP, Little Chiller,
-        25000,             ! Nominal Capacity [W]
-        2.5,               ! COP
-        0.0011,            ! Design Chilled Water Flow Rate [m3/s]
-        0.0011,            ! Design Condenser Water Flow Rate [m3/s]
-        Little Chiller Inlet Node, Little Chiller Outlet Node,
-        Little Chiller Condenser Inlet Node, Little Chiller Condenser Outlet Node,
-        WaterCooled,
-        VariableFlow;
-
-
-Chiller:ConstantCOP,
-    Little Chiller,          !- Name
-    25000,                   !- Nominal Capacity {W}
-    2.5,                     !- Nominal COP {W/W}
-    0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
-    0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
-    Little Chiller Inlet Node,   !- Chilled Water Inlet Node Name
-    Little Chiller Outlet Node,  !- Chilled Water Outlet Node Name
-    Little Chiller Condenser Inlet Node,   !- Condenser Inlet Node Name
-    Little Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
-    EvaporativelyCooled,                   !- Condenser Type
-    VariableFlow,            !- Chiller Flow Mode
-    ,                        !- Sizing Factor
-    450;                     !- Basin Heater Capacity {W/K}
-```
-
-
-
-
-### Constant COP Chiller Outputs
-
-* HVAC,Average,Chiller Electric Power [W]
-
-* HVAC,Sum,Chiller Electric Energy [J]
-
-* Zone,Meter,Electricity:Plant [J]
-
-* Zone,Meter,Cooling:Electricity [J]
-
-* HVAC,Average,Chiller Evaporator Cooling Rate [W]
-
-* HVAC,Sum,Chiller Evaporator Cooling Energy [J]
-
-* Zone,Meter,EnergyTransfer:Plant [J]
-
-* Zone,Meter,Chillers:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Evaporator Inlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Outlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Condenser Heat Transfer Rate [W]
-
-* HVAC,Sum,Chiller Condenser Heat Transfer Energy [J]
-
-* Zone,Meter,HeatRejection:EnergyTransfer [J]
-
-
-Air-cooled or Evap-cooled:
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-Evap-cooled:
-
-* HVAC,Average,Chiller Basin Heater Electric Power [W]
-
-* HVAC,Average,Chiller Basin Heater Electric Energy [J]
-
-Water-cooled:
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Outlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Mass Flow Rate [kg/s]
-
-These chiller output variables are defined above under "Generic Chiller Outputs."
-
-
-
-### Chiller:Electric
-
-This chiller model is the empirical model from the Building Loads and System Thermodynamics (BLAST) program. Capacity, power, and full load are each defined by a set of performance curves (quadratics). Chiller performance curves are generated by fitting catalog data to third order polynomial equations. The nominal inputs and curves described below are combined as follows to calculate the chiller power:
-
-<div>\[{\rm{Power  =  FracFullLoadPower }}\cdot {\rm{ FullLoadPowerRat }}\cdot {\rm{ AvailToNominalCapacityRatio }}\cdot \frac{{{\rm{NominalCapacity}}}}{{{\rm{COP}}}}\]</div>
-
-where:
-
-NominalCapacity = Nominal Capacity field
-
-COP = COP field
-
-AvailToNominalCapacityRatio = the result of the Capacity Ratio Curve
-
-FullLoadPowerRat  = the result of the Power Ratio Curve
-
-FracFullLoadPower = the result of the Full Load Ratio Curve
-
-#### Field: Name
-
-This alpha field contains the identifying name for the electric chiller.
-
-#### Field: Condenser Type
-
-This alpha field determines what type of condenser will be modeled with this chiller. The 3 type of condensers are AirCooled, WaterCooled, and EvaporativelyCooled with the default being AirCooled if not specified. AirCooled and EvaporativelyCooled do not require a Condenser Loop to be specified, where the WaterCooled option requires the full specification of the Condenser Loop and its associated equipment.
-
-#### Field: Nominal Capacity
-
-This numeric field contains the nominal cooling capability of the chiller in Watts.
-
-#### Field: Nominal COP
-
-This numeric field contains the chiller’s coefficient of performance. For a water-cooled chiller, this number does not include energy use due to condenser pumps and/or fans. For an air-cooled or evap-cooled chiller, this number includes condenser fan power.
-
-#### Field: Chilled Water Inlet Node Name
-
-This required alpha field contains the identifying name for the electric chiller plant side inlet node.
-
-#### Field: Chilled Water Outlet Node Name
-
-This required alpha field contains the identifying name for the electric chiller plant side outlet node.
-
-#### Field: Condenser Inlet Node Name
-
-This alpha field contains the identifying name for the electric chiller condenser side inlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and a condenser inlet node name is specified here, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates an outdoor air node and the air temperature information on this node is taken directly from the weather file (no node height adjustment).
-
-#### Field: Condenser Outlet Node Name
-
-This alpha field contains the identifying name for the electric chiller condenser side outlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates a condenser side outlet air node.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the electric chiller’s minimum part load ratio. The expected range is between 0 and 1. The minimum part load is not the load where the machine shuts off, but where the amount of power remains constant to produce smaller loads than this fraction.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the electric chiller’s maximum part load ratio. This value may exceed 1, but the normal range is between 0 and 1.1.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the electric chiller’s optimum part load ratio. This is the part load ratio at which the chiller performs at its maximum COP.
-
-#### Field: Design Condenser Inlet Temperature
-
-This numeric field contains the electric chiller’s condenser inlet design temperature in Celsius.
-
-#### Field: Temperature Rise Coefficient
-
-This numeric field contains the electric chiller’s temperature rise coefficient which is defined as the ratio of the required change in condenser water temperature to a given change in chilled water temperature, which maintains the capacity at the nominal value. This is calculated as the following ratio:
-
-<div>\[\frac{{TCEn{t_{required}} - TCEn{t_{rated}}}}{{TEL{v_{required}} - TEL{v_{rated}}}}\]</div>
-
-where:
-
-TCEnt<sub>required</sub> = Required entering condenser air or water temperature to maintain rated capacity.
-
-TCEnt<sub>rated</sub> = Rated entering condenser air or water temperature at rated capacity.
-
-TELv<sub>required</sub> = Required leaving evaporator water outlet temperature to maintain rated capacity.
-
-TELv<sub>rated</sub> = Rated leaving evaporator water outlet temperature at rated capacity.
-
-#### Field: Design Chilled Water Outlet Temperature
-
-This numeric field contains the electric chiller’s evaporator outlet design temperature in Celsius.
-
-#### Field: Design Chilled Water Flow Rate
-
-For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate. The units are in cubic meters per second.
-
-#### Field: Design Condenser Fluid Flow Rate
-
-This numeric field contains the electric chiller’s design condenser water flow rate in cubic meters per second. This field is autosizable. This field is also used to enter the air flow rate if the Condenser Type = AirCooled or EvaporativelyCooled and Heat Recovery is specified.
-
-#### Capacity Ratio Curve
-
-The Capacity Ratio Curve is a quadratic equation that determines the Ratio of Available Capacity to Nominal Capacity. The defining equation is:
-
-<div>\[AvailToNominalCapacityRatio = {C_1} + {C_2}{\Delta_{temp}} + {C_3}\Delta_{temp}^2\]</div>
-
-Where the Delta Temperature is defined as:
-
-<div>\[{\Delta_{{\rm{Temp}}}} = \frac{{{\rm{TempCondIn  -  TempCondInDesign }}}}{{{\rm{TempRiseCoefficient}}}} - ({\rm{TempEvapOut  -  TempEvapOutDesign)}}\]</div>
-
-TempCondIn = Temperature entering the condenser (water or air temperature depending on condenser type).
-
-TempCondInDesign = Design Condenser Inlet Temperature from User input above.
-
-TempEvapOut = Temperature leaving the evaporator.
-
-TempEvapOutDesign = Design Chilled Water Outlet Temperature from User input above.
-
-TempRiseCoefficient = User Input from above.
-
-The following three fields contain the coefficients for the quadratic equation.
-
-#### Field: Coefficient 1 of Capacity Ratio Curve
-
-This numeric field contains the first coefficient for the capacity ratio curve.
-
-#### Field: Coefficient 2 of Capacity Ratio Curve
-
-This numeric field contains the second coefficient for the capacity ratio curve.
-
-#### Field: Coefficient 3 of Capacity Ratio Curve
-
-This numeric field contains the third coefficient for the capacity ratio curve.
-
-#### Power Ratio Curve
-
-The Power Ratio Curve is a quadratic equation that determines the Ratio of Full Load Power at Available Capacity to Full Load Power at Nominal Capacity. The defining equation is:
-
-<span>\(FullLoadPowerRatio = {C_1} + {C_2}AvailToNominalCapRatio + {C_3}AvailToNominalCapRati{o^2}\)</span>The following three fields contain the coefficients for the quadratic equation.
-
-#### Field: Coefficient1 of the power ratio curve
-
-This numeric field contains the first coefficient for the power ratio curve.
-
-#### Field: Coefficient 2 of Power Ratio Curve
-
-This numeric field contains the second coefficient for the power ratio curve.
-
-#### Field: Coefficient 3 of Power Ratio Curve
-
-This numeric field contains the third coefficient for the power ratio curve.
-
-#### Full Load Ratio Curve
-
-The Full Load Ratio Curve is a quadratic equation that determines the fraction of full load power. The defining equation is:
-
-<div>\[FracFullLoadPower = {C_1} + {C_2}PartLoadRatio + {C_3}PartLoadRati{o^2}\]</div>
-
-The following three fields contain the coefficients for the quadratic equation.
-
-#### Field: Coefficient 1 of Full Load Ratio Curve
-
-This numeric field contains the first coefficient for the full load ratio curve.
-
-#### Field: Coefficient 2 of Full Load Ratio Curve
-
-This numeric field contains the second coefficient for the full load ratio curve.
-
-#### Field: Coefficient 3 of Full Load Ratio Curve
-
-This numeric field contains the third coefficient for the full load ratio curve.
-
-#### Field: Chilled Water Outlet Temperature Lower Limit
-
-This numeric field contains the lower limit for the evaporator outlet temperature. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn’t get too cold.
-
-#### Field: Chiller Flow Mode
-
-This choice field determines how the chiller operates with respect to the intended fluid flow through the device’s evaporator.  There are three different choices for specifying operating modes for the intended flow behavior:  “NotModulated,� “ConstantFlow,� and “LeavingSetpointModulated.�  NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.  ConstantFlow is useful for constant speed pumping arrangements where the chiller’s request for flow is stricter and can increase the overall loop flow.  LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.  In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.  The default, if not specified, is NotModulated.
-
-#### Field: Design Heat Recovery Water Flow Rate
-
-This is the design flow rate used if the heat recovery option is being simulated. If this value is greater than 0.0 then a heat recovery loop must be specified and attached to the chiller using the next 2 node fields. To determine how the heat recovery algorithm works look at the Engineering Manual at the Chiller:Electric with Heat Recovery section. The units are in cubic meters per second. This field is autosizable.  When autosizing, the flow rate is simply the product of the design condenser flow rate and the condenser heat recovery relative capacity fraction set in the field below. Note that heat recovery is only available with Condenser Type = WaterCooled.
-
-#### Field: Heat Recovery Inlet Node Name
-
-This alpha field contains the identifying name for the electric chiller heat recovery side inlet node. A heat recovery loop must be specified.
-
-#### Field: Heat Recovery Outlet Node Name
-
-This alpha field contains the identifying name for the electric chiller heat recovery side outlet node. A heat recovery loop must be specified.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Design Chilled Water Flow Rate and Design Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the chiller’s electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the chiller is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the chiller is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the chiller is off.
-
-#### Field: Condenser Heat Recovery Relative Capacity Fraction
-
-This field is optional.  It can be used to describe the physical size of the heat recovery portion of a split bundle condenser section.  This fraction describes the relative capacity of the heat recovery bundle of a split condenser compared to the nominal, full load heat rejection rate of the chiller.  This fraction will be applied to the full heat rejection when operating at nominal capacity and nominal COP to model a capacity limit for the heat rejection.  If this field is not entered then the capacity fraction is set to 1.0.
-
-#### Field: Heat Recovery Inlet High Temperature Limit Schedule Name
-
-This field is optional.  It can be used to control heat recovery operation of the chiller.  The schedule named here should contain temperature values, in C, that describe an upper limit for the return fluid temperatures entering the chiller at the heat recovery inlet node.  If the fluid temperature is too high, then the heat recovery will not operate.  This is useful to restrict the chiller lift from becoming too high and to avoid overheating the hot water loop.  This limit can be used with or without the alternate control using leaving setpoint that is set in the next field.
-
-#### Field: Heat Recovery Leaving Temperature Setpoint Node Name
-
-This field is optional.  It can be used to refine the model and controls for heat recovery operation of the chiller.  The node named here should have a setpoint placed on it by a setpoint manager.  If the plant loop’s demand calculation scheme is set to SingleSetpoint, then a single setpoint manager should be used.  If the plant loop’s demand calculation is set to DualSetpointDeadband then a dual setpoint manager should be used and the upper setpoint is used for control.  When this field is used, a different model is used for determining the distribution of rejected heat between the two bundles that is more appropriate for series bundle arrangements and for chiller’s that are able to produce relatively higher temperature heated fluids.
-
-
-
-An example of this statement in an IDF is:
-
-```idf
-Chiller:Electric,
-    Big Chiller,             !- Chiller Name
-    WaterCooled,             !- Condenser Type
-    100000,                  !- Nominal Capacity {W}
-    2.75,                    !- COP
-    Big Chiller Inlet Node,  !- Chilled Water Inlet Node Name
-    Big Chiller Outlet Node, !- Chilled Water Outlet Node Name
-    Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
-    Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
-    .15,                     !- Minimum Part Load Ratio
-    1.0,                     !- Maximum Part Load Ratio
-    .65,                     !- Optimum Part Load Ratio
-    29.44,                   !- Design Condenser Inlet Temperature {C}
-    2.682759,                !- Temperature Rise Coefficient
-    6.667,                   !- Design Chilled Water Outlet Temperature {C}
-    0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
-    0.0005,                  !- Design Condenser Water Flow Rate {m3/s}
-    0.94483600,              !- Coefficient 1 of Capacity Ratio Curve
-    -.05700880,              !- Coefficient 2 of Capacity Ratio Curve
-    -.00185486,              !- Coefficient 3 of Capacity Ratio Curve
-    1.907846,                !- Coefficient 1 of Power Ratio Curve
-    -1.20498700,             !- Coefficient 2 of Power Ratio Curve
-    0.26346230,              !- Coefficient 3 of Power Ratio Curve
-    0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
-    0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
-    0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
-    5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
-    VariableFlow;            !- Chiller Flow Mode
-```
-
-An example of an Air-Cooled Chiller:
-
-```idf
-Chiller:Electric,
-    Big Chiller,             !- Chiller Name
-    AirCooled,              !- Condenser Type
-    100000,                  !- Nominal Capacity {W}
-    2.58,                    !- COP
-    Big Chiller Inlet Node,  !- Chilled Water Inlet Node Name
-    Big Chiller Outlet Node, !- Chilled Water Outlet Node Name
-    Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
-    Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
-    .05,                     !- Minimum Part Load Ratio
-    1.0,                     !- Maximum Part Load Ratio
-    .65,                     !- Optimum Part Load Ratio
-    35.0,                    !- Design Condenser Inlet Temperature {C}
-    2.778,                   !- Temperature Rise Coefficient
-    6.67,                    !- Design Chilled Water Outlet Temperature {C}
-    0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
-    0.002,                   !- Design Condenser Water Flow Rate {m3/s}
-    0.9949,                  !- Coefficient 1 of Capacity Ratio Curve
-    -0.045954,               !- Coefficient 2 of Capacity Ratio Curve
-    -0.0013543,              !- Coefficient 3 of Capacity Ratio Curve
-    2.333,                   !- Coefficient 1 of Power Ratio Curve
-    -1.975,                  !- Coefficient 2 of Power Ratio Curve
-    0.6121,                  !- Coefficient 3 of Power Ratio Curve
-    0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
-    0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
-    0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
-    5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
-    VariableFlow;            !- Chiller Flow Mode
-
-OutdoorAir:Node,
-    Big Chiller Condenser Inlet Node,  !- Node Name
-    -1.0;                    !- Height Above Ground {m}
-```
-
-An example of an Evaporatively-Cooled Chiller:
-
-```idf
-Chiller:Electric,
-    Big Chiller,             !- Name
-    EvaporativelyCooled,               !- Condenser Type
-    100000,                  !- Nominal Capacity {W}
-    2.58,                    !- Nominal COP
-    Big Chiller Inlet Node,  !- Chilled Water Inlet Node Name
-    Big Chiller Outlet Node, !- Chilled Water Outlet Node Name
-    Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
-    Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
-    0.05,                    !- Minimum Part Load Ratio
-    1.0,                     !- Maximum Part Load Ratio
-    0.65,                    !- Optimum Part Load Ratio
-    35.0,                    !- Design Condenser Inlet Temperature {C}
-    2.778,                   !- Temperature Rise Coefficient
-    6.67,                    !- Design Chilled Water Outlet Temperature {C}
-    0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
-    0.002,                   !- Design Condenser Water Flow Rate {m3/s}
-    0.9949,                  !- Coefficient 1 of Capacity Ratio Curve
-    -0.045954,               !- Coefficient 2 of Capacity Ratio Curve
-    -0.0013543,              !- Coefficient 3 of Capacity Ratio Curve
-    2.333,                   !- Coefficient 1 of Power Ratio Curve
-    -1.975,                  !- Coefficient 2 of Power Ratio Curve
-    0.6121,                  !- Coefficient 3 of Power Ratio Curve
-    0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
-    0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
-    0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
-    5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
-    VariableFlow,            !- Chiller Flow Mode
-    ,                        !- Design Heat Recovery Water Flow Rate {m3/s}
-    ,                        !- Heat Recovery Inlet Node Name
-    ,                        !- Heat Recovery Outlet Node Name
-    ,                        !- Sizing Factor
-    450,                     !- Basin Heater Capacity {W/K}
-    3,                       !- Basin Heater Setpoint Temperature {C}
-    Basin heater sch;        !- Basin Heater Operating Schedule Name
-
-  OutdoorAir:Node,
-    Big Chiller Condenser Inlet Node,  !- Name
-    -1.0;                    !- Height Above Ground {m}
-```
-
-
-
-
-An example of a Heat Recovery Chiller:
-
-```idf
-Chiller:Electric,
-    Big Chiller,             !- Chiller Name
-    WaterCooled,            !- Condenser Type
-    25000,                   !- Nominal Capacity {W}
-    2.75,                    !- COP
-    Big Chiller Inlet Node,  !- Chilled Water Inlet Node Name
-    Big Chiller Outlet Node, !- Chilled Water Outlet Node Name
-    Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
-    Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
-    .15,                     !- Minimum Part Load Ratio
-    1.0,                     !- Maximum Part Load Ratio
-    .65,                     !- Optimum Part Load Ratio
-    29.44,                   !- Design Condenser Inlet Temperature {C}
-    2.682759,                !- Temperature Rise Coefficient
-    6.667,                   !- Design Chilled Water Outlet Temperature {C}
-    0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
-    0.0005,                  !- Design Condenser Water Flow Rate {m3/s}
-    0.94483600,              !- Coefficient 1 of Capacity Ratio Curve
-    -.05700880,              !- Coefficient 2 of Capacity Ratio Curve
-    -.00185486,              !- Coefficient 3 of Capacity Ratio Curve
-    1.907846,                !- Coefficient 1 of Power Ratio Curve
-    -1.20498700,             !- Coefficient 2 of Power Ratio Curve
-    0.26346230,              !- Coefficient 3 of Power Ratio Curve
-    0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
-    0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
-    0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
-    5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
-    VariableFlow,            !- Chiller Flow Mode
-    0.00055,                 !- Design heat recovery water flow rate {m3/s}
-    Big Chiller Heat Rec Inlet Node,  !- Heat Recovery Inlet Node Name
-    Big Chiller Heat Rec Outlet Node;  !- Heat Recovery Outlet Node Name
-```
-
-
-### Electric Chiller Outputs
-
-* HVAC,Average,Chiller Electric Power [W]
-
-* HVAC,Sum,Chiller Electric Energy [J]
-
-* Zone,Meter,Electricity:Plant [J]
-
-* Zone,Meter,Cooling:Electricity [J]
-
-* HVAC,Average,Chiller Evaporator Cooling Rate [W]
-
-* HVAC,Sum,Chiller Evaporator Cooling Energy [J]
-
-* Zone,Meter,EnergyTransfer:Plant [J]
-
-* Zone,Meter,Chillers:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Evaporator Inlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Outlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller COP [W/W]
-
-* HVAC,Average,Chiller Condenser Heat Transfer Rate [W]
-
-* HVAC,Sum,Chiller Condenser Heat Transfer Energy [J]
-
-* Zone,Meter,HeatRejection:EnergyTransfer [J]
-
-
-Air-cooled or Evap-cooled:
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-Evap-cooled:
-
-* HVAC,Average,Chiller Basin Heater Electric Power [W]
-
-* HVAC,Average,Chiller Basin Heater Electric Energy [J]
-
-Water-cooled:
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Outlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Mass Flow Rate [kg/s]
-
-HeatRecovery:
-
-* HVAC,Average,Chiller Total Recovered Heat Rate [W]
-
-* HVAC,Sum, Chiller Total Recovered Heat Energy [J]
-
-* HVAC,Average,Chiller Heat Recovery Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Effective Heat Rejection Temperature [C]
-
-These chiller output variables are defined above under "Generic Chiller Outputs."
-
-
-
-### Chiller:Electric:EIR
-
-This chiller model is the empirical model used in the DOE-2.1 building energy simulation program. The model uses performance information at reference conditions along with three curve fits for cooling capacity and efficiency to determine chiller operation at off-reference conditions. Chiller performance curves can be generated by fitting manufacturer’s catalog data or measured data. Performance curves for more than 160 chillers, including the default DOE-2.1E reciprocating and centrifugal chillers, are provided in the EnergyPlus Reference DataSets (Chillers.idf and AllDataSets.idf).
-
-Note: Chiller:Electric:EIR objects and their associated performance curve objects are developed using performance information for a specific chiller and should normally be used together for an EnergyPlus simulation. Changing the object input values, or swapping performance curves between chillers, should be done with caution.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the electric EIR chiller.
-
-#### Field: Reference Capacity
-
-This numeric field contains the reference cooling capacity of the chiller in Watts. This should be the capacity of the chiller at the reference temperatures and water flow rates defined below. Alternately, this field can be autosized.
-
-#### Field: Reference COP
-
-This numeric field contains the chiller’s coefficient of performance. This value should **not** include energy use due to pumps or cooling tower fans. This COP should be at the reference temperatures and water flow rates defined below. This value **should** include evap-cooled or air-cooled condenser fans except when the Condenser Fan Power Ratio input field defined below is used and that input value is greater than 0. For the case when condenser fan power is modeled separately, the calculated condenser fan energy is reported on the same electric meter as compressor power. Be careful to not duplicate this energy use.
-
-#### Field: Reference Leaving Chilled Water Temperature
-
-This numeric field contains the chiller’s reference leaving chilled water temperature in Celsius. The default value is 6.67°C.
-
-#### Field: Reference Entering Condenser Fluid Temperature
-
-This numeric field contains the chiller’s reference entering condenser fluid temperature in Celsius. The default value is 29.4°C. For water-cooled chillers this is the water temperature entering the condenser (e.g., leaving the cooling tower). For air- or evap-cooled condensers this is the entering outdoor air dry-bulb or wet-bulb temperature, respectively.
-
-#### Field: Reference Chilled Water Flow Rate
-
-For a variable flow chiller this is the maximum water flow rate and for a constant flow chiller this is the operating water flow rate through the chiller’s evaporator. The units are in cubic meters per second. The minimum value for this numeric input field must be greater than zero, or this field can be autosized.
-
-#### Field: Reference Condenser Fluid Flow Rate
-
-This numeric field contains the chiller’s operating condenser water flow rate in cubic meters per second. This field can be autosized. This field is also used to enter the air flow rate if Condenser Type = AirCooled or EvaporativelyCooled and Heat Recovery is specified..
-
-#### Field: Cooling Capacity Function of Temperature Curve Name
-
-The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the cooling capacity as a function of the leaving chilled water temperature and the entering condenser fluid temperature. The output of this curve is multiplied by the reference capacity to give the cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-#### Field: Electric Input to Cooling Output Ratio Function of Temperature Curve Name
-
-The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and the entering condenser fluid temperature. The EIR is the inverse of the COP. The output of this curve is multiplied by the reference EIR (inverse of the reference COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-#### Field: Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-
-The name of a quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the part-load ratio (EIRfTPLR). The EIR is the inverse of the COP, and the part-load ratio is the actual cooling load divided by the chiller’s available cooling capacity. This curve is generated by dividing the operating electric input power by the available full-load capacity (do not divide by load) at the specific operating temperatures. The curve output should decrease from 1 towards 0 as part-load ratio decreases from 1 to 0. The output of this curve is multiplied by the reference full-load EIR (inverse of the reference COP) and the Energy Input to Cooling Output Ratio Function of Temperature Curve to give the EIR at the specific temperatures and part-load ratio at which the chiller is operating. This curve should have a value of 1.0 when the part-load ratio equals 1.0. An ideal chiller with the same efficiency at all part-load ratio’s would use a performance curve that has a value of 0 when the part-load ratio equals 0 (i.;e., a line connecting 0,0 and 1,1 when plotted as EIRfTPLR versus PLR), however, actual systems can have part-load EIR’s slightly above or below this line (i.e., part-load efficiency often differs from rated efficiency). The quadratic curve should be valid for the range of part-load ratios anticipated for the simulation.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the chiller’s minimum part-load ratio. The expected range is between 0 and 1. Below this part-load ratio, the compressor cycles on and off to meet the cooling load. The Minimum Part Load Ratio must be less than or equal to the Maximum Part Load Ratio. The default value is 0.1.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the chiller’s maximum part-load ratio. This value may exceed 1, but the normal range is between 0 and 1.0. The Maximum Part Load Ratio must be greater than or equal to the Minimum Part Load Ratio. The default value is 1.0.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the chiller’s optimum part-load ratio. This is the part-load ratio at which the chiller performs at its maximum COP. The optimum part-load ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 1.0.
-
-#### Field: Minimum Unloading Ratio
-
-This numeric field contains the chiller’s minimum unloading ratio. The expected range is between 0 and 1. The minimum unloading ratio is where the chiller capacity can no longer be reduced by unloading and must be false loaded to meet smaller cooling loads. A typical false loading strategy is hot-gas bypass. The minimum unloading ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 0.2.
-
-#### Field: Chilled Water Inlet Node Name
-
-This required alpha field contains the identifying name for the chiller plant side (chilled water) inlet node.
-
-#### Field: Chilled Water Outlet Node Name
-
-This required alpha field contains the identifying name for the chiller plant side (chilled water) outlet node.
-
-#### Field: Condenser Inlet Node Name
-
-This alpha field contains the identifying name for the chiller condenser side inlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and a condenser inlet node name is specified here, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates an outdoor air node and the air temperature information on this node is taken directly from the weather file (no node height adjustment).
-
-#### Field: Condenser Outlet Node Name
-
-This alpha field contains the identifying name for the chiller condenser side outlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates a condenser side outlet air node.
-
-#### Field: Condenser Type
-
-This alpha field determines what type of condenser will be modeled with this chiller. Valid condenser types are AirCooled, WaterCooled, and EvaporativelyCooled with the default being WaterCooled if not specified. AirCooled and EvaporativelyCooled do not require a Condenser Loop to be specified, whereas the WaterCooled option requires the full specification of the Condenser Loop and its associated equipment.
-
-#### Field: Condenser Fan Power Ratio
-
-This field is used to model condenser fan power associated with air-cooled or evaporatively-cooled condensers (for cooling towers, refer to Group - Condenser Equipment). Enter the ratio of the condenser fan power to the reference chiller cooling capacity in W/W. If this input is greater than 0, the condenser fan power is modeled seperatly from compressor power. In addition, if condenser fan power is modeled using this input, the reference COP and “Electric Input to Cooling Output Ratio Function of � performance curves should not include condenser fan power.
-
-#### Field: Fraction of Compressor Electric Power Rejected by Condenser
-
-This numeric input represents the fraction of compressor electrical energy consumption that must be rejected by the condenser. Enter a value of 1.0 when modeling hermetic chillers. For open chillers, enter the compressor motor efficiency. This value must be greater than 0.0 and less than or equal to 1.0, with a default value of 1.0.
-
-#### Field: Leaving Chilled Water Lower Temperature Limit
-
-This numeric field contains the lower limit for the leaving chilled water temperature in Celsius. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn’t get too cold. This input field is currently unused. The default value is 2°C.
-
-#### Field: Chiller Flow Mode
-
-This choice field determines how the chiller operates with respect to the intended fluid flow through the device’s evaporator.  There are three different choices for specifying operating modes for the intended flow behavior:  “NotModulated,� “ConstantFlow,� and “LeavingSetpointModulated.�  NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.  ConstantFlow is useful for constant speed pumping arrangements where the chiller’s request for flow is stricter and can increase the overall loop flow.  LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.  In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.  The default, if not specified, is NotModulated.
-
-#### Field: Design Heat Recovery Water Flow Rate
-
-This is the design heat recovery water flow rate if the heat recovery option is being simulated. If this value is greater than 0.0 (or Autosize), a heat recovery loop must be specified and attached to the chiller using the next two node fields. The units are in cubic meters per second.  This field is autosizable.  When autosizing, the flow rate is simply the product of the design condenser flow rate and the condenser heat recovery relative capacity fraction set in the field below. Note that heat recovery is only available with Condenser Type = WaterCooled.
-
-#### Field: Heat Recovery Inlet Node Name
-
-This alpha field contains the identifying name for the chiller heat recovery side inlet node. If the user wants to model chiller heat recovery, a heat recovery loop must be specified.
-
-#### Field: Heat Recovery Outlet Node Name
-
-This alpha field contains the identifying name for the chiller heat recovery side outlet node. If the user wants to model chiller heat recovery, a heat recovery loop must be specified.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Reference Capacity, Reference Chilled Water Flow Rate and Reference Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the chiller’s electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the chiller is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the chiller is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the chiller is off.
-
-#### Field: Condenser Heat Recovery Relative Capacity Fraction
-
-This field is optional.  It can be used to describe the physical size of the heat recovery portion of a split bundle condenser section.  This fraction describes the relative capacity of the heat recovery bundle of a split condenser compared to the nominal, full load heat rejection rate of the chiller.  This fraction will be applied to the full heat rejection when operating at nominal capacity and nominal COP to model a capacity limit for the heat rejection.  If this field is not entered then the capacity fraction is set to 1.0.
-
-#### Field: Heat Recovery Inlet High Temperature Limit Schedule Name
-
-This field is optional.  It can be used to control heat recovery operation of the chiller.  The schedule named here should contain temperature values, in C, that describe an upper limit for the return fluid temperatures entering the chiller at the heat recovery inlet node.  If the fluid temperature is too high, then the heat recovery will not operate.  This is useful to restrict the chiller lift from becoming too high and to avoid overheating the hot water loop.  This limit can be used with or without the alternate control using leaving setpoint that is set in the next field.
-
-#### Field: Heat Recovery Leaving Temperature Setpoint Node Name
-
-This field is optional.  It can be used to refine the model and controls for heat recovery operation of the chiller.  The node named here should have a setpoint placed on it by a setpoint manager.  If the plant loop’s demand calculation scheme is set to SingleSetpoint, then a single setpoint manager should be used.  If the plant loop’s demand calculation is set to DualSetpointDeadband then a dual setpoint manager should be used and the upper setpoint is used for control.  When this field is used, a different model is used for determining the distribution of rejected heat between the two bundles that is more appropriate for series bundle arrangements and for chiller’s that are able to produce relatively higher temperature heated fluilds.
-
-
-
-An example of this statement in an IDF is:
-
-```idf
-! ElectricEIRChiller DOE-2 Centrifugal/5.50COP
-! A generic centrifugal chiller from DOE-2.1E
-!
-Chiller:Electric:EIR,
- DOE-2 Centrifugal/5.50COP,  !- Chiller Name
- Autosize,                   !- Reference Capacity {W}
- 5.5,                        !- Reference COP {W/W}
- 6.67,                       !- Reference Leaving Chilled Water Temperature {C}
- 29.4,                       !- Reference Entering Condenser Fluid Temperature {C}
- Autosize,                   !- Reference Chilled Water Flow Rate {m3/s}
- Autosize,                   !- Reference Condenser Water Flow Rate {m3/s}
- DOE-2 Centrifugal/5.50COP CAPFT,  !- Cooling Capacity Function of Temperature Curve
- DOE-2 Centrifugal/5.50COP EIRFT,  !- Electric Input to Cooling Output Ratio Function of
-                                      Temperature Curve
- DOE-2 Centrifugal/5.50COP EIRFPLR,!- Electric Input to Cooling Output Ratio Function of Part Load
-                                      Ratio Curve
- 0.1,                        !- Minimum Part Load Ratio
- 1.0,                        !- Maximum Part Load Ratio
- 1.0,                        !- Optimum Part Load Ratio
- 0.2,                        !- Minimum Unloading Ratio
- Chilled Water Side Inlet Node,        !- Chilled Water Side Inlet Node
- Chilled Water Side Outlet Node,       !- Chilled Water Side Outlet Node
- Condenser Side Inlet Node,  !- Condenser Side Inlet Node
- Condenser Side Outlet Node, !- Condenser Side Outlet Node
- WaterCooled,               !- Condenser Type
- ,                           !- Condenser Fan Power Ratio {W/W}
- 1.0,                        !- Fraction of Compressor Electric Power Rejected by Condenser
- 2.0,                        !- Leaving Chilled Water Lower Temperature Limit {C}
- ConstantFlow;               !- Chiller Evaporator Flow Mode
-
-
-!
-! Curve set (3 Curves):
-!
-! Cooling Capacity Function of Temperature Curve for open or hermetic water-cooled centrifugal
-  chillers
-! x = Leaving Chilled Water Temperature and y = Entering Condenser Water Temperature
-! Same as DOE-2.1E HERM-CENT-CAP-FT (CCAPT3) and OPEN-CENT-CAP-FT (CCAPT1)
- Curve:Biquadratic,
- DOE-2 Centrifugal/5.50COP CAPFT,  !- Name
- 0.257896E+00,               !- Coefficient1 Constant
- 0.389016E-01,               !- Coefficient2 x
- -0.217080E-03,              !- Coefficient3 x**2
- 0.468684E-01,               !- Coefficient4 y
- -0.942840E-03,              !- Coefficient5 y**2
- -0.343440E-03,              !- Coefficient6 x*y
- 5.0,                        !- Minimum Value of x
- 10.0,                       !- Maximum Value of x
- 24.0,                       !- Minimum Value of y
- 35.0;                       !- Maximum Value of y
-!
-! Energy Input to Cooling Output Ratio Function of Temperature Curve for open or hermetic water-
-  cooled centrifugal chillers
-! x = Leaving Chilled Water Temperature and y = Entering Condenser Water Temperature
-! Same as DOE-2.1E HERM-CENT-EIR-FT (EIRT3) and OPEN-CENT-EIR-FT (EIRT1)
- Curve:Biquadratic,
- DOE-2 Centrifugal/5.50COP EIRFT,  !- Name
- 0.933884E+00,               !- Coefficient1 Constant
- -0.582120E-01,              !- Coefficient2 x
- 0.450036E-02,               !- Coefficient3 x**2
- 0.243000E-02,               !- Coefficient4 y
- 0.486000E-03,               !- Coefficient5 y**2
- -0.121500E-02,              !- Coefficient6x*y
- 5.0,                        !- Minimum Value of x
- 10.0,                       !- Maximum Value of x
- 24.0,                       !- Minimum Value of y
- 35.0;                       !- Maximum Value of y
-!
-! Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve for open or hermetic
-  water-cooled centrifugal chillers
-! x = Part Load Ratio (load/capacity)
-! Same as DOE-2.1E HERM-CENT-EIR-FPLR (EIRPLR3) and OPEN-CENT-EIR-FPLR (EIRPLR1)
- Curve:Quadratic,
- DOE-2 Centrifugal/5.50COP EIRFPLR, !- Name
- 0.222903,                   !- Coefficient1 Constant
- 0.313387,                   !- Coefficient2 x
- 0.463710,                   !- Coefficient3 x**2
- 0.0,                        !- Minimum Value of x
- 1.0;                        !- Maximum Value of x
-```
-
-
-### Electric EIR Chiller Outputs
-
-* HVAC,Average,Chiller Electric Power [W]
-
-* HVAC,Sum,Chiller Electric Energy [J]
-
-* Zone,Meter,Electricity:Plant [J]
-
-* Zone,Meter,Cooling:Electricity [J]
-
-* HVAC,Average,Chiller Evaporator Cooling Rate [W]
-
-* HVAC,Sum,Chiller Evaporator Cooling Energy [J]
-
-* Zone,Meter,EnergyTransfer:Plant [J]
-
-* Zone,Meter,Chillers:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Evaporator Inlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Outlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller COP [W/W]
-
-* HVAC,Average,Chiller Condenser Heat Transfer Rate [W]
-
-* HVAC,Sum,Chiller Condenser Heat Transfer Energy [J]
-
-* Zone,Meter,HeatRejection:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Part Load Ratio []
-
-* HVAC,Average,Chiller Cycling Ratio []
-
-* HVAC,Average,Chiller False Load Heat Transfer Rate [W]
-
-* HVAC,Sum,Chiller False Load Heat Transfer Energy [J]
-
-
-Curve object outputs:
-
-* HVAC,Average,Chiller Capacity Temperature Modifier Multiplier []
-
-* HVAC,Average,Chiller EIR Temperature Modifier Multiplier []
-
-* HVAC,Average,Chiller EIR Part Load Modifier Multiplier []
-
-
-Air-cooled or Evap-cooled:
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-
-
-Air-cooled or Evap-cooled reported only when the condenser fan power ratio input field is greater than 0:
-
-* HVAC,Average,Chiller Condenser Fan Electric Power [W]
-
-* HVAC,Average,Chiller Condenser Fan Electric Consumption [J]
-
-
-
-Evap-cooled:
-
-* HVAC,Average,Chiller Basin Heater Electric Power [W]
-
-* HVAC,Average,Chiller Basin Heater Electric Energy [J]
-
-
-
-Water-cooled:
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Outlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Mass Flow Rate [kg/s]
-
-
-
-HeatRecovery:
-
-* HVAC,Average,Chiller Total Recovered Heat Rate [W]
-
-* Zone,Meter,HeatRecovery:EnergyTransfer [J]
-
-* HVAC,Sum,Chiller Heat Recovery [J]
-
-* HVAC,Average,Chiller Heat Recovery Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Effective Heat Rejection Temperature [C]
-
-
-
-Most of these chiller output variables are defined above under "Generic Chiller Outputs."  Output variables not described above are discussed here.
-
-#### Chiller Condenser Fan Electric Power  [W]
-
-#### Chiller Condenser Fan Electric Energy  [J]
-
-These outputs are for the electric power consumption of the chiller condenser fan and are applicable to air- or evaporatively-cooled chillers. These reports are available only for the Chiller:Electric:EIR and only when the Condenser Fan Power Ratio input field is greater than 0. This output is also added to a meter object with Resource Type = Electricity, End Use Key = Chillers, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Chiller Capacity Temperature Modifier Multiplier []
-
-This is the output of the curve object Cooling Capacity Function of Temperature Curve.
-
-#### Chiller EIR Temperature Modifier Multiplier []
-
-This is the output of the curve object Electric Input to Cooling Output Ratio Function of Temperature Curve.
-
-#### Chiller EIR Part Load Modifier Multiplier []
-
-This is the output of the curve object Electric Input to Cooling Output Ratio Function of Part Load Curve.
-
-#### Chiller Part Load Ratio []
-
-This output is the ratio of the evaporator heat transfer rate plus the false load heat transfer rate (if applicable) to the available chiller capacity. This value is used to determine Chiller EIR Part Load Modifier Multiplier.
-
-#### Chiller Cycling Ratio []
-
-The cycling ratio is the amount of time the chiller operates during each simulation timestep. If the chiller part-load ratio falls below the minimum part-load ratio, the chiller cycles on and off to meet the cooling load.
-
-#### Chiller False Load Heat Transfer Rate [W]
-
-#### Chiller False Load Heat Transfer Energy [J]
-
-These outputs are the heat transfer rate and total heat transfer due to false loading of the chiller. When the chiller part-load ratio is below the minimum unloading ratio, the chiller false loads (e.g. hot-gas bypass) to further reduce capacity. The false load heat transfer output variable is not metered.
-
-### Chiller:Electric:ReformulatedEIR
-
-This chiller model, developed through the CoolTools™ project sponsored by Pacific Gas and Electric Company (PG&E), is an empirical model similar to EnergyPlus’ Chiller:Electric:EIR model. The model uses performance information at reference conditions along with three curve fits for cooling capacity and efficiency to determine chiller operation at off-reference conditions. The model has the same capabilities as the Chiller:Electric:EIR model, but can potentially provide significant accuracy improvement over the Chiller:Electric:EIR model for variable-speed compressor drive and variable condenser water flow applications. Chiller performance curves can be generated by fitting manufacturer’s catalog data or measured data. Performance curves developed from manufacturer’s performance data are provided in the EnergyPlus Reference DataSets (Chillers.idf and AllDataSets.idf). This chiller model can be used to predict the performance of various chiller types (e.g., reciprocating, screw, scroll, and centrifugal) with water-cooled condensers.
-
-The main difference between this model and the Chiller:Electric:EIR model is the condenser fluid temperature used in the associated performance curves: the Chiller:Electric:ReformulatedEIR model uses the LEAVING condenser water temperature while the Chiller:Electric:EIR model uses the ENTERING condenser water temperature.
-
-Note: Chiller:Electric:Reformulated EIR objects and their associated performance curve objects are developed using performance information for a specific chiller and should almost always be used together for an EnergyPlus simulation. Changing the object input values, or swapping performance curves between chillers, should be done with extreme caution. For example, if the user wishes to model a chiller size that is different from the reference capacity, it is highly recommended that the reference flow rates be scaled proportionately to the change in reference capacity. Although this model can provide more accurate prediction than the Chiller:Electric:EIR model, it requires more performance data to develop the associated performance curves (at least 12 points from full-load performance and 7 points from part-load performance).
-
-#### Field: Chiller Name
-
-This alpha field contains the identifying name for this chiller.
-
-#### Field: Reference Capacity
-
-This numeric field contains the reference cooling capacity of the chiller in Watts. This should be the capacity of the chiller at the reference temperatures and water flow rates defined below. Alternately, this field can be autosized.
-
-#### Field: Reference COP
-
-This numeric field contains the chiller’s coefficient of performance. This value should **not** include energy use due to pumps or cooling tower fans. This COP should be at the reference temperatures and water flow rates defined below.
-
-#### Field: Reference Leaving Chilled Water Temperature
-
-This numeric field contains the chiller’s reference leaving chilled water temperature in Celsius. The default value is 6.67°C.
-
-#### Field: Reference Leaving Condenser Water Temperature
-
-This numeric field contains the chiller’s reference leaving condenser water temperature in Celsius. The default value is 35°C.
-
-#### Field: Reference Chilled Water Flow Rate
-
-For a variable flow chiller this is the maximum water flow rate and for a constant flow chiller this is the operating water flow rate through the chiller’s evaporator. The units are in cubic meters per second. The minimum value for this numeric input field must be greater than zero, or this field can be autosized.
-
-#### Field: Reference Condenser Water Flow Rate
-
-This numeric field contains the chiller’s operating condenser water flow rate in cubic meters per second. The units are in cubic meters per second. The minimum value for this numeric input field must be greater than zero, or this field can be autosized.
-
-#### Field: Cooling Capacity Function of Temperature Curve Name
-
-The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the cooling capacity as a function of the leaving chilled water temperature and the leaving condenser water temperature. The output of this curve is multiplied by the reference capacity to give the cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation (otherwise the program issues warning messages).
-
-#### Field: Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Type
-
-This choice field determines which type of the Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve is used in the chiller modeling. Two curve types are available: (1) Type LeavingCondenserWaterTemperature is based on the leaving condenser water temperature. (2) Type Lift is based on the normalized lift, which is the temperature difference between the leaving condenser water temperature and the leaving evaporator water temperature. 
-
-#### Field: Electric Input to Cooling Output Ratio Function of Temperature Curve Name
-
-The name of the Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve. The form of this curve is based on the input for Electric Input to Cooling Output RatioFunction of Part Load Ratio Curve Type. For the type of LeavingCondenserWaterTemperature, the curve object type should be Curve:Bicubic or Table:TwoIndependentVariables that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and the leaving condenser water temperature. For the type of Lift, the curve object type should be Curve:ChillerPartLoadWithLiftCurves or Table:MultiVariableLookup that parameterizes the variation of EIR as a function of the normalized fractional Lift, normalized Tdev and the PLR. Tdev is the difference between Leaving Chilled Water Temperature and Reference Chilled Water Temperature. Lift is the Leaving Condenser Water Temperature and Leaving Chilled Water Temperature.  The EIR is the inverse of the COP. The output of this curve is multiplied by the reference EIR (inverse of the reference COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation (otherwise the program issues warning messages).
-
-#### Field: Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-
-The name of a bicubic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the leaving condenser water temperature and the part-load ratio (EIRfTPLR). The EIR is the inverse of the COP, and the part-load ratio is the actual cooling load divided by the chiller’s available cooling capacity. This curve is generated by dividing the operating electric input power by the available full-load capacity (do not divide by load) at the specific operating temperatures. The curve output should decrease from 1 towards 0 as part-load ratio decreases from 1 to 0. The output of this curve is multiplied by the reference full-load EIR (inverse of the reference COP) and the Energy Input to Cooling Output Ratio Function of Temperature Curve to give the EIR at the specific temperatures and part-load ratio at which the chiller is operating. This curve should have a value of 1.0 at the reference leaving condenser water temperature with the part-load ratio equal to 1.0. An ideal chiller with the same efficiency at all part-load ratio’s would use a performance curve that has a value of 0 when the part-load ratio equals 0 (i.;e., a line connecting 0,0 and 1,1 when plotted as EIRfTPLR versus PLR), however, actual systems can have part-load EIR’s slightly above or below this line (i.e., part-load efficiency often differs from rated efficiency). The bicubic curve should be valid for the range of condenser water temperatures and part-load ratios anticipated for the simulation (otherwise the program issues warning messages).
-
-Note: Although a bicubic curve requires 10 coefficients (ref. Curve:Bicubic), coefficients 7, 9 and 10 are typically not used in the performance curve described here and should be entered as 0 unless sufficient performance data and regression accuracy exist to justify the use of these coefficients. Additionally, coefficients 2, 3, and 6 should not be used unless sufficient temperature data is available to accurately define the performance curve (i.e., negative values may result from insufficient data).
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the chiller’s minimum part-load ratio. The expected range is between 0 and 1. Below this part-load ratio, the compressor cycles on and off to meet the cooling load. The Minimum Part Load Ratio must be less than or equal to the Maximum Part Load Ratio. The default value is 0.1.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the chiller’s maximum part-load ratio. This value may exceed 1, but the normal range is between 0 and 1.0. The Maximum Part Load Ratio must be greater than or equal to the Minimum Part Load Ratio. The default value is 1.0.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the chiller’s optimum part-load ratio. This is the part-load ratio at which the chiller performs at its maximum COP. The optimum part-load ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 1.0.
-
-#### Field: Minimum Unloading Ratio
-
-This numeric field contains the chiller’s minimum unloading ratio. The expected range is between 0 and 1. The minimum unloading ratio is where the chiller capacity can no longer be reduced by unloading and must be false loaded to meet smaller cooling loads. A typical false loading strategy is hot-gas bypass. The minimum unloading ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 0.2.
-
-#### Field: Chilled Water Side Inlet Node
-
-This required alpha field contains the identifying name for the chiller plant side (chilled water) inlet node.
-
-#### Field: Chilled Water Side Outlet Node
-
-This required alpha field contains the identifying name for the chiller plant side (chilled water) outlet node.
-
-#### Field: Condenser Side Inlet Node
-
-This required alpha field contains the identifying name for the chiller condenser side inlet node.
-
-#### Field: Condenser Side Outlet Node
-
-This required alpha field contains the identifying name for the chiller condenser side outlet node.
-
-#### Field: Fraction of Compressor Electric Power Rejected by Condenser
-
-This numeric input represents the fraction of compressor electrical energy consumption that must be rejected by the condenser. Enter a value of 1.0 when modeling hermetic chillers. For open chillers, enter the compressor motor efficiency. This value must be greater than 0.0 and less than or equal to 1.0, with a default value of 1.0.
-
-#### Field: Leaving Chilled Water Lower Temperature Limit
-
-This numeric field contains the lower limit for the leaving chilled water temperature in Celsius. This temperature acts as a cut off for heat transfer in the evaporator, so that the water doesn’t get too cold. This input field is currently unused. The default value is 2°C.
-
-#### Field: Chiller Flow Mode Type
-
-This choice field determines how the chiller operates with respect to the intended fluid flow through the device’s evaporator.  There are three different choices for specifying operating modes for the intended flow behavior:  “NotModulated,� “ConstantFlow,� and “LeavingSetpointModulated.�  NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.  ConstantFlow is useful for constant speed pumping arrangements where the chiller’s request for flow is stricter and can increase the overall loop flow.  LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.  In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.  The default, if not specified, is NotModulated.
-
-#### Field: Design Heat Recovery Water Flow Rate
-
-This is the design heat recovery water flow rate if the heat recovery option is being simulated. If this value is greater than 0.0 (or autosize), a heat recovery loop must be specified and attached to the chiller using the next two node fields. The units are in cubic meters per second.  This field is autosizable.  When autosizing, the flow rate is simply the product of the design condenser flow rate and the condenser heat recovery relative capacity fraction set in the field below.
-
-#### Field: Heat Recovery Inlet Node Name
-
-This alpha field contains the identifying name for the chiller heat recovery side inlet node. If the user wants to model chiller heat recovery, a heat recovery loop must be specified and it can only be used with a water-cooled condenser.
-
-#### Field: Heat Recovery Outlet Node Name
-
-This alpha field contains the identifying name for the chiller heat recovery side outlet node. If the user wants to model chiller heat recovery, a heat recovery loop must be specified and it can only be used with a water-cooled condenser.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Reference Capacity, Reference Chilled Water Flow Rate and Reference Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-#### Field: Condenser Heat Recovery Relative Capacity Fraction
-
-This field is optional.  It can be used to describe the physical size of the heat recovery portion of a split bundle condenser section.  This fraction describes the relative capacity of the heat recovery bundle of a split condenser compared to the nominal, full load heat rejection rate of the chiller.  This fraction will be applied to the full heat rejection when operating at nominal capacity and nominal COP to model a capacity limit for the heat rejection.  If this field is not entered then the capacity fraction is set to 1.0.
-
-#### Field: Heat Recovery Inlet High Temperature Limit Schedule Name
-
-This field is optional.  It can be used to control heat recovery operation of the chiller.  The schedule named here should contain temperature values, in C, that describe an upper limit for the return fluid temperatures entering the chiller at the heat recovery inlet node.  If the fluid temperature is too high, then the heat recovery will not operate.  This is useful to restrict the chiller lift from becoming too high and to avoid overheating the hot water loop.  This limit can be used with or without the alternate control using leaving setpoint that is set in the next field.
-
-#### Field: Heat Recovery Leaving Temperature Setpoint Node Name
-
-This field is optional.  It can be used to refine the model and controls for heat recovery operation of the chiller.  The node named here should have a setpoint placed on it by a setpoint manager.  If the plant loop’s demand calculation scheme is set to SingleSetpoint, then a single setpoint manager should be used.  If the plant loop’s demand calculation is set to DualSetpointDeadband then a dual setpoint manager should be used and the upper setpoint is used for control.  When this field is used, a different model is used for determining the distribution of rejected heat between the two bundles that is more appropriate for series bundle arrangements and for chiller’s that are able to produce relatively higher temperature heated fluilds.
-
-An example of this statement in an IDF is:
-
-```idf
-Chiller:Electric:ReformulatedEIR,
-  Main Chiller,                        !- Chiller Name
-  50000,                               !- Reference Capacity {W}
-  3.99,                                !- Reference COP
-  6.67,                                !- Reference Leaving Chilled Water Temperature {C}
-  35.0,                                !- Reference Leaving Condenser Water Temperature {C}
-  0.00898,                             !- Reference Chilled Water Flow Rate {m3/s}
-  0.01122,                             !- Reference Condenser Water Flow Rate {m3/s}
-  Main Chiller RecipCapFT,             !- Cooling Capacity Function of Temperature Curve
-  Main Chiller RecipEIRFT,             !- Electric Input to Cooling Output Ratio Function of Temperature Curve
-  LeavingCondenserWaterTemperature     !- Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Type
-  Main Chiller RecipEIRFPLR,           !- Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-  0.01,                                !- Minimum Part Load Ratio
-  1,                                   !- Maximum Part Load Ratio
-  1,                                   !- Optimum Part Load Ratio
-  0.07,                                !- Minimum Unloading Ratio
-  Main Chiller ChW Inlet,              !- Chilled Water Side Inlet Node
-  Main Chiller ChW Outlet,             !- Chilled Water Side Outlet Node
-  Main Chiller Cnd Inlet,              !- Condenser Side Inlet Node
-  Main Chiller Cnd Outlet,             !- Condenser Side Outlet Node
-  1,                                   !- Fraction of Compressor Electric Power Rejected by Condenser
-  2,                                   !- Leaving Chilled Water Lower Temperature Limit {C}
-  ConstantFlow;                        !- Chiller Flow Mode
-
-! Cooling capacity to rated capacity function of Temperature Curve
-! x = Leaving Chilled Water Temperature and y = Leaving Condenser Water Temperature
-
-  Curve:Biquadratic,
-    Main Chiller RecipCapFT,  !- Name
-    0.958546443,       !- Coefficient1 Constant
-    0.035168695,       !- Coefficient2 x
-    0.000124662,       !- Coefficient3 x\*\*2
-    -0.00274551,       !-Coefficient4y
-    -0.00005000,       !-Coefficient5y\*\*2
-    -0.00017234,       !-Coefficient6x\*y
-    5.00,              !- Minimum Value of x
-    10.0,              !- Maximum Value of x
-    20.00,             !- Minimum Value of y
-    40.94;             !- Maximum Value of y
-
-! Energy Input to Cooling Output Ratio Function of Temperature Curve
-! x = Leaving Chilled Water Temperature and y = Leaving Condenser Water Temperature
-
-  Curve:Biquadratic,
-    Main Chiller RecipEIRFT,  !- Name
-    0.732700123,       !- Coefficient1 Constant
-    -0.00834360,       !- Coefficient2 x
-    0.000638530,       !- Coefficient3 x\*\*2
-    -0.00303753,       !-Coefficient4y
-    0.000484952,       !-Coefficient5y\*\*2
-    -0.00083584,       !-Coefficient6x\*y
-    5.00,              !- Minimum Value of x
-    10.0,              !- Maximum Value of x
-    20.00,             !- Minimum Value of y
-    40.94;             !- Maximum Value of y
-
-! Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve
-! x = Leaving Condenser water Temperature and y = Part Load Ratio
-
-  Curve:Bicubic,
-    Main Chiller RecipEIRFPLR, !- Name
-    0.070862846,        !- Coefficient1 Constant
-    0.002787560,        !- Coefficient2 x
-    -0.00000891,        !- Coefficient3 x\*\*2
-    0.230973399,        !-Coefficient4y
-    1.250442176,        !-Coefficient5y\*\*2
-    -0.00216102,        !-Coefficient6x\*y
-    0.000000,           !-Coefficient7x\*\*3
-    -0.56300936,        !-Coefficient8y\*\*3
-    0.000000,           !-Coefficient9x\*\*2\*y
-    0.000000,           !-Coefficient10x\*y\*\*2
-    20.00,              !- Minimum Value of x
-    40.94,              !- Maximum Value of x
-    0.01,               !- Minimum Value of y
-    1.0;               !- Maximum Value of y
-```
-
-### Electric Reformulated EIR Chiller Outputs
-
-The output variables for Chiller:Electric:ReformulatedEIR are the same as the output variables for Chiller:Electric:EIR (ref. Electric EIR Chiller Outputs). except for the Chiller Condenser Fan Electric Power and Energy reports
-
-### Chiller:EngineDriven
-
-#### Field: Name
-
-This alpha field contains the identifying name for the engine driven chiller.
-
-#### Field: Condenser Type
-
-This alpha field determines what type of condenser will be modeled with this chiller. The 3 type of condensers are AirCooled, WaterCooled, and EvaporativelyCooled with the default being AirCooled if not specified. AirCooled and EvaporativelyCooled do not require a Condenser Loop to be specified, where the WaterCooled option requires the full specification of the Condenser Loop and its associated equipment.
-
-#### Field: Nominal Capacity
-
-This numeric field contains the nominal cooling capability of the chiller in Watts.
-
-#### Field: Nominal COP
-
-This numeric field contains the chiller’s coefficient of performance (COP).
-
-#### Field: Chilled Water Inlet Node Name
-
-This required alpha field contains the identifying name for the chiller plant side inlet node.
-
-#### Field: Chilled Water Outlet Node Name
-
-This required alpha field contains the identifying name for the chiller plant side outlet node.
-
-#### Field: Condenser Inlet Node Name
-
-This alpha field contains the identifying name for the chiller condenser side inlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and a condenser inlet node name is specified here, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates an outdoor air node and the air temperature information on this node is taken directly from the weather file (no node height adjustment).
-
-#### Field: Condenser Outlet Node Name
-
-This alpha field contains the identifying name for the chiller condenser side outlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates a condenser side outlet air node.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the chiller’s minimum part load ratio. The expected range is between 0 and 1. The minimum part load is not the load where the machine shuts off, but where the amount of power remains constant to produce smaller loads than this fraction.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the chiller’s maximum part load ratio. This value may exceed 1, but the normal range is between 0 and 1.1.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the chiller’s optimum part load ratio. This is the part load ratio at which the chiller performs at its maximum COP.
-
-#### Field: Design Condenser Inlet Temperature
-
-This numeric field contains the chiller’s condenser inlet design temperature in Celsius.
-
-#### Field: Temperature Rise Coefficient
-
-This numeric field contains the electric chiller’s temperature rise coefficient which is defined as the ratio of the required change in condenser water temperature to a given change in chilled water temperature, which maintains the capacity at the nominal value. This is calculated as the following ratio:
-
-<div>\[\frac{{TCEn{t_{required}} - TCEn{t_{rated}}}}{{TEL{v_{required}} - TEL{v_{rated}}}}\]</div>
-
-where:
-
-TCEnt<sub>required</sub> = Required entering condenser air or water temperature to maintain rated capacity.
-
-TCEnt<sub>rated</sub> = Rated entering condenser air or water temperature at rated capacity.
-
-TELv<sub>required</sub> = Required leaving evaporator water outlet temperature to maintain rated capacity.
-
-TELv<sub>rated</sub> = Rated leaving evaporator water outlet temperature at rated capacity.
-
-#### Field: Design Chilled Water Outlet Temperature
-
-This numeric field contains the chiller’s evaporator outlet design temperature in Celsius.
-
-#### Field: Design Chilled Water Flow Rate
-
-For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate. The units are in cubic meters per second.
-
-#### Field: Design Condenser Water Flow Rate
-
-This numeric field contains the chiller’s design condenser water flow rate in cubic meters per second. This field can be autosized. This field is not user for Condenser Type = AirCooled or EvaporativelyCooled.
-
-#### Capacity Ratio Curve
-
-The Capacity Ratio Curve is a quadratic equation that determines the Ratio of Available Capacity to Nominal Capacity. The defining equation is:
-
-<div>\[AvailToNominalCapacityRatio = {C_1} + {C_2}{\Delta_{temp}} + {C_3}\Delta_{temp}^2\]</div>
-
-Where the Delta Temperature is defined as:
-
-<div>\[FullLoadtoPowerRatio = {C_1} + {C_2}AvailToNominalCapRatio + {C_3}AvailToNominalCapRati{o^2}\]</div>
-
-TempCondIn = Temperature entering the condenser (water or air temperature depending on condenser type).
-
-TempCondInDesign = Design Condenser Inlet Temperature from User input above.
-
-TempEvapOut = Temperature leaving the evaporator.
-
-TempEvapOutDesign = Design Chilled Water Outlet Temperature from User input above.
-
-TempRiseCoefficient = User Input from above.
-
-The following three fields contain the coefficients for the quadratic equation.
-
-#### Field: Coefficient 1 of Capacity Ratio Curve
-
-This numeric field contains the first coefficient for the capacity ratio curve.
-
-#### Field: Coefficient 2 of Capacity Ratio Curve
-
-This numeric field contains the second coefficient for the capacity ratio curve.
-
-#### Field: Coefficient 3 of Capacity Ratio Curve
-
-This numeric field contains the third coefficient for the capacity ratio curve.
-
-#### Power Ratio Curve
-
-The Power Ratio Curve is a quadratic equation that determines the Ratio of Full Load to Power. The defining equation is:
-
-<span>\(FracFullLoadPower = {C_1} + {C_2}PartLoadRatio + {C_3}PartLoadRati{o^2}\)</span>The following three fields contain the coefficients for the quadratic equation.
-
-#### Field: Coefficient 1 of Power Ratio Curve
-
-This numeric field contains the first coefficient for the power ratio curve.
-
-#### Field: Coefficient 2 of Power Ratio Curve
-
-This numeric field contains the second coefficient for the power ratio curve.
-
-#### Field: Coefficient 3 of Power Ratio Curve
-
-This numeric field contains the third coefficient for the power ratio curve.
-
-#### Full Load Ratio Curve
-
-The Full Load Ratio Curve is a quadratic equation that determines the fraction of full load power. The defining equation is:
-
-<div>\[{\rm{CoolingLoadtoFuelCurve}} = {C_1} + {C_2} * PLR + {C_3} * PL{R^2}\]</div>
-
-The following three fields contain the coefficients for the quadratic equation.
-
-#### Field: Coefficient 1 of Full Load Ratio Curve
-
-This numeric field contains the first coefficient for the full load ratio curve.
-
-#### Field: Coefficient 2 of Full Load Ratio Curve
-
-This numeric field contains the second coefficient for the full load ratio curve.
-
-#### Field: Coefficient 3 of Full Load Ratio Curve
-
-This numeric field contains the third coefficient for the full load ratio curve.
-
-#### Field Chilled Water Outlet Temperature Lower Limit
-
-This numeric field contains the lower limit for the evaporator outlet temperature. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn’t get too cold.
-
-#### Field: Fuel Use Curve Name
-
-This alpha field contains the name of the Cooling Load to Fuel Use curve. The curve itself is specified separately using the EnergyPlus Curve Manager. The Fuel Use Curve is a quadratic equation that determines the ratio of Cooling Load to Fuel Energy. The defining equation is:
-
-<div>\[RecoveryJacketHeatToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}\]</div>
-
-where PLR is the Part Load Ratio from the Chiller. The Part Load Based Fuel Input Curve determines the ratio of fuel energy per unit time (J/s) / cooling load (W). This is illustrated by the logic block in the Engine Driven Chiller algorithm.
-
-```
-IF (PartLoadRat == 0)THEN
-   EngineDrivenFuelEnergy = 0
-ELSE
-   ClngLoadFuelRat = CurveValue(EngineDrivenChiller(ChillerNum)%ClngLoadtoFuelCurve, PartLoadRat )
-   EngineDrivenFuelEnergy = QEvaporator / ClngLoadFuelRat
-END IF
-```
-
-#### Field: Jacket Heat Recovery Curve Name
-
-This alpha field contains the name of the Recovery Jacket Heat curve. The curve itself is specified separately using the EnergyPlus Curve Manager. The Recovery Jacket Heat Curve is a quadratic equation that determines the ratio of recovery jacket heat to fuel energy. The defining equation is:
-
-<div>\[RecoveryLubeHeatToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}\]</div>
-
-where RL is the Ratio of Load to Diesel Engine Capacity
-
-#### Field: Lube Heat Recovery Curve Name
-
-This alpha field contains the name of the Recovery Lube Heat curve. The curve itself is specified separately using the EnergyPlus Curve Manager. The Recovery Lubricant Heat Curve is a quadratic equation that determines the ratio of recovery lube heat to fuel energy. The defining equation is:
-
-<div>\[TotalExhaustToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}\]</div>
-
-where RL is the Ratio of Load to Diesel Engine Capacity
-
-#### Field: Total Exhaust Energy Curve Name
-
-This alpha field contains the name of the Total Exhaust Energy curve. The curve itself is specified separately using the EnergyPlus Curve Manager. The Total Exhaust Energy Curve is a quadratic equation that determines the ratio of total exhaust energy to fuel energy. The defining equation is:
-
-<div>\[AbsoluteExhaustTemperature = {C_1} + {C_2}RL + {C_3}R{L^2}\]</div>
-
-where RL is the Ratio of Load to Diesel Engine Capacity
-
-#### Field: Exhaust Temperature Curve Name
-
-This alpha field contains the name of the Exhaust Temperature curve. The curve itself is specified separately using the EnergyPlus Curve Manager. The Exhaust Temperature Curve is a quadratic equation that determines the absolute exhaust temperature. The defining equation is:
-
-<div>\[UAToCapacityRatio = {C_1}EngineCapacit{y^{{C_2}}}\]</div>
-
-where RL is the Ratio of Load to Diesel Engine Capacity
-
-#### U-Factor Times Area Curve
-
-The U-Factor Times Area (UA) is an equation that determines the overall heat transfer coefficient for the exhaust gasses with the stack. The heat transfer coefficient ultimately helps determine the exhaust stack temperature. The defining equation is:
-
-<div>\[\frac{{TCEn{t_{required}} - TCEn{t_{rated}}}}{{TEL{v_{required}} - TEL{v_{rated}}}}\]</div>
-
-The following two fields contain the coefficients for the equation.
-
-#### Field: Coefficient 1 of U-Factor Times Area Curve
-
-This numeric field contains the first coefficient for the overall heat transfer coefficient curve.
-
-#### Field: Coefficient 2 of U-Factor Times Area Curve
-
-This numeric field contains the second (exponential) coefficient for the overall heat transfer coefficient curve.
-
-#### Field: Maximum Exhaust Flow per Unit of Power Output
-
-This numeric field contains the maximum exhaust gas mass flow rate per watt of cooling provided by the engine driven chiller
-
-#### Field: Design Minimum Exhaust Temperature
-
-This numeric field contains the steam saturation temperature in Celsius that would be used to determine the energy recovered from a water jacket heat exchanger on the engine.
-
-#### Field: Fuel Type
-
-This alpha value specifies the type of fuel used in the engine. The fuel type can be NaturalGas, PropaneGas, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1 or OtherFuel2. This field is required.
-
-#### Field: Fuel Higher Heating Value
-
-This numeric field contains the higher heating value of the fuel used in kJ/kg.
-
-#### Field: Design Heat Recovery Water Flow Rate
-
-This numeric field specifies the heat recovery volumetric flow rate through the engine in m<sup>3</sup>/sec. The heat recovery loop manager and hot water tan must also be specified if heat energy is to be recovered from the engine driven chiller.
-
-#### Field: Heat Recovery Inlet Node Name
-
-This alpha field contains the identifying name for the heat recovery side inlet. If a loop is connected, then the jacket and lubricant heat will be recovered. There is no need for an effectiveness term, since the jacket and lubricant recovered heat energies are the actual recovered energies.
-
-#### Field: Heat Recovery Outlet Node Name
-
-This alpha field contains the identifying name for the heat recovery side outlet.
-
-#### Field: Chiller Flow Mode
-
-This choice field determines how the chiller operates with respect to the intended fluid flow through the device’s evaporator.  There are three different choices for specifying operating modes for the intended flow behavior:  “NotModulated,� “ConstantFlow,� and “LeavingSetpointModulated.�  NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.  ConstantFlow is useful for constant speed pumping arrangements where the chiller’s request for flow is stricter and can increase the overall loop flow.  LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.  In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.  The default, if not specified, is NotModulated.
-
-#### Field: Maximum Temperature for Heat Recovery at Heat Recovery Outlet Node
-
-This field sets the maximum temperature that this piece of equipment can produce for heat recovery. The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit. This temperature limit puts an upper bound on the recovered heat and limits the max temperatures leaving the component.
-
-As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting. This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply. The temperature is specified in degrees C.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Design Chilled Water Flow Rate and Design Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the chiller’s electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the chiller is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the chiller is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the chiller is off.
-
-An example of this statement in an IDF is:
-```idf
-Chiller:EngineDriven,
-    Central Chiller,         !- Chiller Name
-    WaterCooled,            !- Condenser Type
-    autosize,                !- Nominal Capacity {W}
-    2.75,                    !- COP
-    Central Chiller Inlet Node,  !- Chilled Water Inlet Node Name
-    Central Chiller Outlet Node,  !- Chilled Water Outlet Node Name
-    Central Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
-    Central Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
-    0.0,                     !- Minimum Part Load Ratio
-    1.0,                     !- Maximum Part Load Ratio
-    .65,                     !- Optimum Part Load Ratio
-    35.0,                    !- Design Condenser Inlet Temperature {C}
-    2.778,                   !- Temperature Rise Coefficient
-    6.67,                    !- Design Chilled Water Outlet Temperature {C}
-    autosize,                !- Design Chilled Water Flow Rate {m3/s}
-    autosize,                !- Design Condenser Water Flow Rate {m3/s}
-    0.9949,                  !- Coefficient 1 of Capacity Ratio Curve
-    -0.045954,               !- Coefficient 2 of Capacity Ratio Curve
-    -0.0013543,              !- Coefficient 3 of Capacity Ratio Curve
-    2.333,                   !- Coefficient 1 of Power Ratio Curve
-    -1.975,                  !- Coefficient 2 of Power Ratio Curve
-    0.6121,                  !- Coefficient 3 of Power Ratio Curve
-    0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
-    0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
-    0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
-    5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
-    Fuel Use Curve,          !- the Fuel Use Curve
-    Jacket Heat Recovery Curve,  !- the Recovery Jacket Heat curve
-    Lube Heat Recovery Curve,!- the Recovery Lube Heat curve
-    Total Exhaust Energy Curve,  !- the Total Exhaust Energy curve
-    Exhaust Temperature Curve,  !- the Exhaust Temperature curve
-    0.01516,                 !- Coefficient1 of UA curve
-    0.9,                     !- Coefficient2 of UA curve
-    0.00063,                 !- Maximum Exhaust Flow per W of Power Output {(kg/s)/W}
-    150,                     !- Design Minimum Exhaust temp. (Steam Saturation Temperature) {C}
-    DIESEL,                  !- Fuel Type
-    45500,                   !- Fuel Heating Value {kJ/kg}
-    0.0,                     !- Design heat recovery water flow rate {m3/s}
-    ,                        !- Heat Recovery Inlet Node Name
-    ,                        !- Heat Recovery Outlet Node Name
-    VariableFlow,            !- Chiller Flow Mode
-    60.0;                    !- Maximum Temp for Heat Recovery. This sets max availability {C}
-```
-
-
-### Engine Driven Chiller Outputs
-
-```idf
-HVAC,Average,Chiller Electric Power [W]
-HVAC,Sum,Chiller Electric Energy [J]
-Zone,Meter,Electricity:Plant [J]
-Zone,Meter,Cooling:Electricity [J]
-HVAC,Average,Chiller Evaporator Cooling Rate [W]
-HVAC,Sum,Chiller Evaporator Cooling Energy [J]
-Zone,Meter,EnergyTransfer:Plant [J]
-Zone,Meter,Chillers:EnergyTransfer [J]
-HVAC,Average,Chiller Evaporator Inlet Temperature [C]
-HVAC,Average,Chiller Evaporator Outlet Temperature [C]
-HVAC,Average,Chiller Evaporator Mass Flow Rate [kg/s]
-HVAC,Average,Chiller COP [W/W]
-HVAC,Average,Chiller Condenser Heat Transfer Energy Rate [W]
-HVAC,Sum,Chiller Condenser Heat Transfer Energy [J]
-Zone,Meter,HeatRejection:EnergyTransfer [J]
-```
-
-
-Air-cooled or Evap-cooled:
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-Evap-cooled:
-
-* HVAC,Average,Chiller Basin Heater Electric Power [W]
-
-* HVAC,Average,Chiller Basin Heater Electric Energy [J]
-
-Water-cooled:
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Outlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Drive Shaft Power [W]
-
-* HVAC,Sum,Chiller Drive Shaft Energy [J]
-
-* HVAC,Average,Chiller Jacket Recovered Heat Rate [W]
-
-* HVAC,Sum,Chiller Jacket Recovered Heat Energy [J]
-
-* Zone,Meter,HeatRecovery:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Lube Recovered Heat Rate [W]
-
-* HVAC,Sum,Chiller Lube Recovered Heat Energy [J]
-
-* HVAC,Average,Chiller Exhaust Heat Recovery Rate [W]
-
-* HVAC,Sum,Chiller Exhaust Heat Recovery Energy [J]
-
-* HVAC,Average,Chiller Total Recovered Heat Rate [W]
-
-* HVAC,Sum,Chiller Total Recovered Heat Energy [J]
-
-* HVAC,Average,Chiller Heat Recovery Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Heat Recovery Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Outlet Temperature [C]
-
-* HVAC,Average,Chiller Exhaust Temperature [C]
-
-One of the following blocks will be applicable based on fuel type:
-
-* HVAC,Average,Chiller Gas Rate [W]
-
-* HVAC,Sum,Chiller Gas Energy [J]
-
-* HVAC,Average,Chiller Gas Mass Flow Rate [kg/s]
-
-
-* HVAC,Average,Chiller Propane Rate [W]
-
-* HVAC,Sum,Chiller Propane Energy [J]
-
-* HVAC,Average,Chiller Propane Mass Flow Rate [kg/s]
-
-
-* HVAC,Average,Chiller Diesel Rate [W]
-
-* HVAC,Sum,Chiller Diesel Energy [J]
-
-* HVAC,Average,Chiller Diesel Mass Flow Rate [kg/s]
-
-
-* HVAC,Average,Chiller Gasoline Rate [W]
-
-* HVAC,Sum,Chiller Gasoline Energy [J]
-
-* HVAC,Average,Chiller Gasoline Mass Flow Rate [kg/s]
-
-
-* HVAC,Average,Chiller FuelOil\#1 Rate [W]
-
-* HVAC,Sum,Chiller FuelOil\#1 Energy [J]
-
-* HVAC,Average,Chiller FuelOil\#1 Mass Flow Rate [kg/s]
-
-
-* HVAC,Average,Chiller FuelOil\#2 Rate [W]
-
-* HVAC,Sum,Chiller FuelOil\#2 Energy [J]
-
-* HVAC,Average,Chiller FuelOil\#2 Mass Flow Rate [kg/s
-
-
-* HVAC,Average,Chiller OtherFuel1 Rate [W]
-
-* HVAC,Sum,Chiller OtherFuel1 Energy [J]
-
-* HVAC,Average,Chiller OtherFuel1 Mass Flow Rate [kg/s]
-
-
-* HVAC,Average,Chiller OtherFuel2 Rate [W]
-
-* HVAC,Sum,Chiller OtherFuel2 Energy [J]
-
-* HVAC,Average,Chiller OtherFuel2 Mass Flow Rate [kg/s]
-
-
-These chiller output variables are defined above under "Generic Chiller Outputs."
-
-### Chiller:CombustionTurbine
-
-This chiller model is the empirical model from the Building Loads and System Thermodynamics (BLAST) program. Chiller performance curves are generated by fitting catalog data to third order polynomial equations. Three sets of coefficients are required.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the combustion turbine chiller.
-
-#### Field: Condenser Type
-
-This alpha field determines what type of condenser will be modeled with this chiller. The 3 type of condensers are AirCooled, WaterCooled, and EvaporativelyCooled with the default being AirCooled if not specified. AirCooled and EvaporativelyCooled do not require a Condenser Loop to be specified, where the WaterCooled option requires the full specification of the Condenser Loop and its associated equipment.
-
-#### Field: Nominal Capacity
-
-This numeric field contains the nominal cooling capability of the chiller in Watts.
-
-#### Field: Nominal COP
-
-This numeric field contains the chiller’s coefficient of performance (COP).
-
-#### Field: Chilled Water Inlet Node Name
-
-This alpha field contains the identifying name for the combustion turbine chiller plant side inlet node.
-
-#### Field: Chilled Water Outlet Node Name
-
-This required alpha field contains the identifying name for the combustion turbine chiller plant side inlet node.
-
-#### Field: Chilled Water Outlet Node Name
-
-This required alpha field contains the identifying name for the combustion turbine chiller plant side outlet node.
-
-#### Field: Condenser Inlet Node Name
-
-This alpha field contains the identifying name for the combustion turbine chiller condenser side inlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and a condenser inlet node name is specified here, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates an outdoor air node and the air temperature information on this node is taken directly from the weather file (no node height adjustment).
-
-#### Field: Condenser Outlet Node Name
-
-This alpha field contains the identifying name for the combustion turbine chiller condenser side outlet node. This node name is required if the chiller is WaterCooled, and optional if the chiller is AirCooled or EvaporativelyCooled. If the chiller is AirCooled or EvaporativelyCooled and this field is left blank, the program automatically creates a condenser side outlet air node.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the combustion turbine chiller’s minimum part load ratio. The expected range is between 0 and 1. The minimum part load is not the load where the machine shuts off, but where the amount of power remains constant to produce smaller loads than this fraction.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the combustion turbine chiller’s maximum part load ratio. This value may exceed 1, but the normal range is between 0 and 1.1.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the combustion turbine chiller’s optimum part load ratio. This is the part load ratio at which the chiller performs at its maximum COP.
-
-#### Field: Design Condenser Inlet Temperature
-
-This numeric field contains the combustion turbine chiller’s condenser inlet design temperature in Celsius.
-
-#### Field: Temperature Rise Coefficient
-
-This numeric field contains the electric chiller’s temperature rise coefficient which is defined as the ratio of the required change in condenser water temperature to a given change in chilled water temperature, which maintains the capacity at the nominal value. This is calculated as the following ratio:
-
-<div>\[\frac{{TCEn{t_{required}} - TCEn{t_{rated}}}}{{TEL{v_{required}} - TEL{v_{rated}}}}\]</div>
-
-where:
-
-TCEnt<sub>required</sub> = Required entering condenser air or water temperature to maintain rated capacity.
-
-TCEnt<sub>rated</sub> = Rated entering condenser air or water temperature at rated capacity.
-
-TELv<sub>required</sub> = Required leaving evaporator water outlet temperature to maintain rated capacity.
-
-TELv<sub>rated</sub> = Rated leaving evaporator water outlet temperature at rated capacity.
-
-#### Field: Design Chilled Water Outlet Temperature
-
-This numeric field contains the combustion turbine chiller’s evaporator outlet design temperature in Celsius.
-
-#### Field: Design Chilled Water Flow Rate
-
-For variable volume chiller this is the maximum flow and for constant flow chiller this is the design flow rate. The units are in cubic meters per second.
-
-#### Field: Design Condenser Water Flow Rate
-
-This numeric field contains the combustion turbine chiller’s design condenser water flow rate in cubic meters per second. This field can be autosized. This field is not used for Condenser Type = AirCooled or EvaporativelyCooled.
-
-#### Capacity Ratio Curve
-
-The Capacity Ratio Curve is a quadratic equation that determines the Ratio of Available Capacity to Nominal Capacity. The defining equation is:
-
-<div>\[AvailToNominalCapacityRatio = {C_1} + {C_2}{\Delta_{temp}} + {C_3}\Delta_{temp}^2\]</div>
-
-Where the Delta Temperature is defined as:
-
-<div>\[FullLoadtoPowerRatio = {C_1} + {C_2}AvailToNominalCapRatio + {C_3}AvailToNominalCapRati{o^2}\]</div>
-
-TempCondIn = Temperature entering the condenser (water or air temperature depending on condenser type).
-
-TempCondInDesign = Design Condenser Inlet Temperature from User input above.
-
-TempEvapOut = Temperature leaving the evaporator.
-
-TempEvapOutDesign = Design Chilled Water Outlet Temperature from User input above.
-
-TempRiseCoefficient = User Input from above.
-
-The following three fields contain the coefficients for the quadratic equation.
-
-#### Field: Coefficient 1 of Capacity Ratio Curve
-
-This numeric field contains the first coefficient for the capacity ratio curve.
-
-#### Field: Coefficient 2 of Capacity Ratio Curve
-
-This numeric field contains the second coefficient for the capacity ratio curve.
-
-#### Field: Coefficient 3 of Capacity Ratio Curve
-
-This numeric field contains the third coefficient for the capacity ratio curve.
-
-#### Power Ratio Curve
-
-The Power Ratio Curve is a quadratic equation that determines the Ratio of Full Load to Power. The defining equation is:
-
-<span>\(FracFullLoadPower = {C_1} + {C_2}PartLoadRatio + {C_3}PartLoadRati{o^2}\)</span>The following three fields contain the coefficients for the quadratic equation.
-
-#### Field: Coefficient 1 of Power Ratio Curve
-
-This numeric field contains the first coefficient for the power ratio curve.
-
-#### Field: Coefficient 2 of Power Ratio Curve
-
-This numeric field contains the second coefficient for the power ratio curve.
-
-#### Field: Coefficient 3 of Power Ratio Curve
-
-This numeric field contains the third coefficient for the power ratio curve.
-
-#### Full Load Ratio Curve
-
-The Full Load Ratio Curve is a quadratic equation that determines the fraction of full load power. The defining equation is:
-
-<div>\[FuelEnergyInput = PLoad * (FI{C_1} + FI{C_2}RLoad + FI{C_3}RLoa{d^2}) * (TBFI{C_1} + TBFI{C_2}A{T_{air}} + TBFI{C_3}AT_{air}^2)\]</div>
-
-The following three fields contain the coefficients for the quadratic equation.
-
-#### Field: Coefficient 1 of Full Load Ratio Curve
-
-This numeric field contains the first coefficient for the full load ratio curve.
-
-#### Field: Coefficient 2 of Full Load Ratio Curve
-
-This numeric field contains the second coefficient for the full load ratio curve.
-
-#### Field: Coefficient 3 of Full Load Ratio Curve
-
-This numeric field contains the third coefficient for the full load ratio curve.
-
-#### Field: Chilled Water Outlet Temperature Lower Limit
-
-This numeric field contains the lower limit for the evaporator outlet temperature. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn’t get too cold.
-
-#### Fuel Input Curve
-
-The Fuel Input Curve is a polynomial equation that determines the Ratio of Fuel Input to Energy Output. The equation combines both the Fuel Input Curve Coefficients and the Temperature Based Fuel Input Curve Coefficients. The defining equation is:
-
-<div>\[ExhaustFlowRate = GTCapacity * ({C_1} + {C_2}A{T_{air}} + {C_3}AT_{air}^2)\]</div>
-
-where FIC represents the Fuel Input Curve Coefficients, TBFIC represents the Temperature Based Fuel Input Curve Coefficients, Rload is the Ratio of Load to Combustion Turbine Engine Capacity, and AT<sub>air</sub> is the difference between the current ambient and design ambient temperatures.
-
-The following three fields contain the coefficients for the fuel input curve.
-
-#### Field: Coefficient 1 of Fuel Input Curve
-
-This numeric field contains the first coefficient for the Fuel Input Curve.
-
-#### Field: Coefficient 2 of Fuel Input Curve
-
-This numeric field contains the second coefficient for the Fuel Input Curve.
-
-#### Field: Coefficient 3 of Fuel Input Curve
-
-This numeric field contains the third coefficient for the Fuel Input Curve.
-
-The following three fields contain the coefficients for the temperature based fuel input curve.
-
-#### Field: Coefficient 1 of Temperature Based Fuel Input Curve
-
-This numeric field contains the first coefficient for the Temperature Based Fuel Input Curve.
-
-#### Field: Coefficient 2 of Temperature Based Fuel Input Curve
-
-This numeric field contains the second coefficient for the Temperature Based Fuel Input Curve.
-
-#### Field: Coefficient 3 of Temperature Based Fuel Input Curve
-
-This numeric field contains the third coefficient for the Temperature Based Fuel Input Curve.
-
-#### Exhaust Flow Curve
-
-The Exhaust Flow Curve is a quadratic equation that determines the Ratio of Exhaust Gas Flow Rate to Engine Capacity. The defining equation is:
-
-*<span>\(ExhaustTemperature = ({C_1} + {C_2}RLoad + {C_3}RLoa{d^2}) * (TB{C_1} + TB{C_2}A{T_{air}} + TB{C_3}AT_{air}^2) - 273.15\)</span> *
-
-where GTCapacity is the Combustion Turbine Engine Capacity, and AT<sub>air</sub> is the difference between the current ambient and design ambient temperatures.
-
-#### Field: Coefficient 1 of Exhaust Flow Curve
-
-This numeric field contains the first coefficient for the Exhaust Flow Curve.
-
-#### Field: Coefficient 2 of Exhaust Flow Curve
-
-This numeric field contains the second coefficient for the Exhaust Flow Curve.
-
-#### Field: Coefficient 3 of Exhaust Flow Curve
-
-This numeric field contains the third coefficient for the Exhaust Flow Curve.
-
-#### Exhaust Gas Temperature Curve
-
-The Exhaust Gas Temperature Curve is a polynomial equation that determines the Exhaust Gas Temperature. The equation combines both the Exhaust Gas Temperature Curve Coefficients (Based on the Part Load Ratio) and the (Ambient) Temperature Based Exhaust Gas Temperature Curve Coefficients. The defining equation is:
-
- <span>\(RecoveryLubeEnergy = PLoad * ({C_1} + {C_2}RL + {C_3}R{L^2})\)</span>
-
-where C represents the Exhaust Gas Temperature Curve Coefficients, TBC are the Temperature Based Exhaust Gas Temperature Curve Coefficients, RLoad is the Ratio of Load to Combustion Turbine Engine Capacity, and AT<sub>air</sub> is the difference between the actual ambient and design ambient temperatures.
-
-#### Field: Coefficient 1 of Exhaust Gas Temperature Curve
-
-This numeric field contains the first coefficient for the Exhaust Gas Temperature Curve.
-
-#### Field: Coefficient 2 of Exhaust Gas Temperature Curve
-
-This numeric field contains the second coefficient for the Exhaust Gas Temperature Curve.
-
-#### Field: Coefficient 3 of Exhaust Gas Temperature Curve
-
-This numeric field contains the third coefficient for the Exhaust Gas Temperature Curve.
-
-#### Field: Coefficient 1 of Temperature Based Exhaust Gas Temperature Curve
-
-This numeric field contains the first coefficient for the Temperature Based Exhaust Gas Temperature Curve.
-
-#### Field: Coefficient 2 of Temperature Based Exhaust Gas Temperature Curve
-
-This numeric field contains the second coefficient for the Temperature Based Exhaust Gas Temperature Curve.
-
-#### Field: Coefficient 3 of Temperature Based Exhaust Gas Temperature Curve
-
-This numeric field contains the third coefficient for the Temperature Based Exhaust Gas Temperature Curve.
-
-#### Recovery Lubricant Heat Curve
-
-The Recovery Lubricant Heat Curve is a quadratic equation that determines the recovery lube energy. The defining equation is:
-
-<div>\[UAToCapacityRatio = {C_1}GasTurbineEngineCapacit{y^{{C_2}}}\]</div>
-
-where Pload is the engine load and RL is the Ratio of Load to Combustion Turbine Engine Capacity
-
-The following three fields contain the coefficients for the quadratic equation.
-
-#### Field: Coefficient 1 of Recovery Lube Heat Curve
-
-This numeric field contains the first coefficient for the Recovery Lube Heat curve.
-
-#### Field: Coefficient 2 of Recovery Lube Heat Curve
-
-This numeric field contains the second coefficient for the Recovery Lube Heat curve.
-
-#### Field: Coefficient 3 of Recovery Lube Heat Curve
-
-This numeric field contains the third coefficient for the Recovery Lube Heat curve.
-
-#### U-Factor Times Area Curve Curve
-
-The U-Factor Times Area Curve (UA) is an equation that determines the overall heat transfer coefficient for the exhaust gasses with the stack. The heat transfer coefficient ultimately helps determine the exhaust stack temperature. The defining equation is:
-
-<div>\[AvailableCoolingCapacity = NominalCoolingCapacity*CoolCapfT\left( {{T_{cw,l}},{T_{cond}}} \right)\]</div>
-
-The following two fields contain the coefficients for the equation.
-
-#### Field: Coefficient 1 of U-Factor Times Area Curve
-
-This numeric field contains the first coefficient for the overall heat transfer coefficient curve.
-
-#### Field: Coefficient 2 of U-Factor Times Area Curve
-
-This numeric field contains the second (exponential) coefficient for the overall heat transfer coefficient curve.
-
-#### Field: Gas Turbine Engine Capacity
-
-This numeric field contains the capacity of the gas turbine engine in watts.
-
-#### Field: Maximum Exhaust Flow per Unit of Power Output
-
-This numeric field contains the maximum exhaust gas mass flow rate per kilowatt of power out.
-
-#### Field: Design Steam Saturation Temperature
-
-This numeric field contains the design steam saturation temperature in Celsius.
-
-#### Field: Fuel Higher Heating Value
-
-This numeric field contains the higher heating value of the fuel used in kJ/kg.
-
-#### Field: Design Heat Recovery Water Flow Rate
-
-This is the design heat recovery water flow rate if the heat recovery option is being simulated. If this value is greater than 0.0, a heat recovery loop must be specified and attached to the chiller using the next two node fields. The units are in cubic meters per second.
-
-#### Field: Heat Recovery Inlet Node Name
-
-This alpha field contains the identifying name for the heat recovery side inlet.  If a loop is connected, then the jacket and lubricant heat will be recovered.  There is no need for an effectiveness term, since the jacket and lubricant recovered heat energies are the actual recovered energies.
-
-#### Field: Heat Recovery Outlet Node Name
-
-This alpha field contains the identifying name for the heat recovery side outlet.
-
-#### Field: Chiller Flow Mode
-
-This choice field determines how the chiller operates with respect to the intended fluid flow through the device’s evaporator.  There are three different choices for specifying operating modes for the intended flow behavior:  “NotModulated,� “ConstantFlow,� and “LeavingSetpointModulated.�  NotModulated is useful for either variable or constant speed pumping arrangements where the chiller is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.  ConstantFlow is useful for constant speed pumping arrangements where the chiller’s request for flow is stricter and can increase the overall loop flow.  LeavingSetpointModulated changes the chiller model to internally vary the flow rate so that the temperature leaving the chiller matches a setpoint.  In all cases the operation of the external plant system can also impact the flow through the chiller -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.  The default, if not specified, is NotModulated.
-
-#### Field: Fuel Type
-
-This alpha field determines the type of fuel that the chiller uses. Valid choices are: **NaturalGas, PropaneGas, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1** or **OtherFuel2**. The default is **NaturalGas**.
-
-#### Field: Heat Recovery Maximum Temperature
-
-This field sets the maximum temperature that this piece of equipment can produce for heat recovery.  The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit.  This temperature limit puts an upper bound on the recovered heat and limits the max temperatures leaving the component.
-
-As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller.  For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field.  The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting.  This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply.
-
-The temperature is specified in degrees C.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity, Design Chilled Water Flow Rate and Design Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the chiller’s electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the chiller is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the chiller is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the chiller is off.
-
-An example of this statement in an IDF is:
-
-```idf
-Chiller:CombustionTurbine,
-    Big Chiller,             !- Chiller Name
-    WaterCooled,            !- Condenser Type
-    30000,                   !- Nominal Capacity {W}
-    2.75,                    !- COP
-    Big Chiller Inlet Node,  !- Chilled Water Inlet Node Name
-    Big Chiller Outlet Node, !- Chilled Water Outlet Node Name
-    Big Chiller Condenser Inlet Node,  !- Condenser Inlet Node Name
-    Big Chiller Condenser Outlet Node,  !- Condenser Outlet Node Name
-    .15,                     !- Minimum Part Load Ratio
-    1.0,                     !- Maximum Part Load Ratio
-    .65,                     !- Optimum Part Load Ratio
-    35.0,                    !- Design Condenser Inlet Temperature {C}
-    2.778,                   !- Temperature Rise Coefficient
-    6.67,                    !- Design Chilled Water Outlet Temperature {C}
-    0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
-    0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
-    0.9949,                  !- Coefficient 1 of Capacity Ratio Curve
-    -0.045954,               !- Coefficient 2 of Capacity Ratio Curve
-    -0.0013543,              !- Coefficient 3 of Capacity Ratio Curve
-    2.333,                   !- Coefficient 1 of Power Ratio Curve
-    -1.975,                  !- Coefficient 2 of Power Ratio Curve
-    0.6121,                  !- Coefficient 3 of Power Ratio Curve
-    0.03303,                 !- Coefficient 1 of Full Load Ratio Curve
-    0.6852,                  !- Coefficient 2 of Full Load Ratio Curve
-    0.2818,                  !- Coefficient 3 of Full Load Ratio Curve
-    5,                       !- Chilled Water Outlet Temperature Lower Limit {C}
-    9.41,                    !- Coefficient 1 of Fuel Input curve
-    -9.48,                   !- Coefficient 2 of Fuel Input curve
-    4.32,                    !- Coefficient 3 of Fuel Input curve
-    1.0044,                  !- Coefficient 1 of Temperature Based Fuel Input curve
-    -0.0008,                 !- Coefficient 2 of Temperature Based Fuel Input curve
-    0,                       !- Coefficient 3 of Temperature Based Fuel Input curve
-    15.63518363,             !- Coefficient 1 of Exhaust Flow curve
-    -0.03059999,             !- Coefficient 2 of Exhaust Flow curve
-    -0.0002,                 !- Coefficient 3 of Exhaust Flow curve
-    916.992,                 !- Coefficient 1 of Exhaust Gas Temperature curve
-    307.998,                 !- Coefficient 2 of Exhaust Gas Temperature curve
-    79.992,                  !- Coefficient 3 of Exhaust Gas Temperature curve
-    1.005,                   !- Coefficient 1 of Temperature Based Exhaust Gas Temperature c
-    0.0018,                  !- Coefficient 2 of Temperature Based Exhaust Gas Temperature c
-    0,                       !- Coefficient 3 of Temperature Based Exhaust Gas Temperature c
-    0.223,                   !- Coefficient 1 of Recovery Lube Heat curve
-    -0.4,                    !- Coefficient 2 of Recovery Lube Heat curve
-    0.2286,                  !- Coefficient 3 of Recovery Lube Heat curve
-    0.01907045,              !- Coefficient 1 of UA curve
-    0.9,                     !- Coefficient 2 of UA curve
-    50000,                   !- Gas Turbine Engine Capacity {W}
-    0.00000504,              !- Maximum Exhaust Flow per Unit of Power Output {(kg/s)/W}
-    150,                     !- Design Steam Saturation Temperature {C}
-    43500,                   !- Fuel Higher Heating Value {kJ/kg}
-    0.0,                     !- Design Heat Recovery Water Flow Rate {m3/s}
-    ,                        !- Heat Recovery Inlet Node Name
-    ,                        !- Heat Recovery Outlet Node Name
-    VariableFlow,            !- Chiller Flow Mode
-    NaturalGas,              !- Fuel Type
-    80.0;                    !- Heat Recovery Maximum Temperature {C}
-```
-
-
-### Combustion Turbine Chiller Outputs
-
-* HVAC,Average,Chiller Electric Power [W]
-
-* HVAC,Sum,Chiller Electric Energy [J]
-
-* Zone,Meter,Electricity:Plant [J]
-
-* Zone,Meter,Cooling:Electricity [J]
-
-* HVAC,Average,Chiller Evaporator Cooling Rate [W]
-
-* HVAC,Sum,Chiller Evaporator Cooling Energy [J]
-
-* Zone,Meter,EnergyTransfer:Plant [J]
-
-* Zone,Meter,Chillers:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Evaporator Inlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Outlet Temperature [C]
-
-* HVAC,Average,Chiller Evaporator Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Condenser Heat Transfer Energy Rate [W]
-
-* HVAC,Sum,Chiller Condenser Heat Transfer Energy [J]
-
-* Zone,Meter,HeatRejection:EnergyTransfer [J]
-
-* HVAC,Average,Chiller COP [W/W]
-
-
-Air-cooled or Evap-cooled:
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-
-
-Evap-cooled:
-
-* HVAC,Average,Chiller Basin Heater Electric Power [W]
-
-* HVAC,Average,Chiller Basin Heater Electric Energy [J]
-
-
-
-Water-cooled:
-
-* HVAC,Average,Chiller Condenser Inlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Outlet Temperature [C]
-
-* HVAC,Average,Chiller Condenser Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Drive Shaft Power [W]
-
-* HVAC,Sum,Chiller Drive Shaft Energy [J]
-
-* HVAC,Sum,Chiller Lube Recovered Heat Energy [J]
-
-* Zone,Meter,HeatRecovery:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Exhaust Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heat Recovery Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller &lt;Fuel Type&gt; Rate [W]
-
-* HVAC,Sum,Chiller &lt;Fuel Type&gt; Energy [J]
-
-* HVAC,Average,Chiller &lt;Fuel Type&gt; Mass Flow Rate [kg/s]
-
-* HVAC,Sum,Chiller &lt;Fuel Type&gt; Mass [kg]
-
-* HVAC,Average,Chiller COP [W/W]
-
-These chiller output variables are defined above under "Generic Chiller Outputs."  The Fuel Type input will determine which fuel type is displayed in the output. In this example with the user choice of **NaturalGas**, you will have **Gas** Consumption.
-
-
-### ChillerHeater:Absorption:DirectFired
-
-This chiller is a direct fired absorption chiller-heater which is modeled using performance curves similar to the equivalent chiller in DOE-2.1E. This type of chiller is unusual for EnergyPlus, because it may be used in the same plant on both a chilled water supply branch and a hot water supply branch. The chiller has six node connections for chilled water, condenser water, and hot water, and can provide simultaneous heating and cooling. During simultaneous operation, the heating capacity is reduced as the cooling load increases (for more details see below). Some equations are provided below to help explain the function of the various performance curves. For a detailed description of the algorithm and how the curves are used in the calculations, please see the Engineering Reference.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the chiller.
-
-#### Field: Nominal Cooling Capacity
-
-This numeric field contains the nominal cooling capability of the chiller in Watts.
-
-#### Field: Heating to Cooling Capacity Ratio
-
-A positive fraction that represents the ratio of the heating capacity divided by the cooling capacity at rated conditions. The default is 0.8.
-
-#### Field: Fuel Input to Cooling Output Ratio
-
-A positive fraction that represents the ratio of the instantaneous cooling fuel used divided by the cooling capacity at rated conditions. The default is 0.97.
-
-#### Field: Fuel Input to Heating Output Ratio
-
-A positive fraction that represents the ratio of the instantaneous heating fuel used divided by the nominal heating capacity. The default is 1.25.
-
-#### Field: Electric Input to Cooling Output Ratio
-
-A positive fraction that represents the ratio of the instantaneous electricity used divided by the cooling capacity at rated conditions. If the chiller is both heating and cooling only the greater of the computed cooling and heating electricity is used. The default is 0.01.
-
-#### Field: Electric Input to Heating Output Ratio
-
-A positive fraction that represents the ratio of the instantaneous electricity used divided by the nominal heating capacity. If the chiller is both heating and cooling, the greater of the cooling electricity and heating eletricity is used. The default is 0.0.
-
-#### Field: Chilled Water Inlet Node Name
-
-This required alpha field contains the identifying name for the chiller chilled water side inlet node. This node name must be the same as the inlet node name for the chilled water supply branch on which this chiller is placed.
-
-#### Field: Chilled Water Outlet Node Name
-
-This required alpha field contains the identifying name for the chiller chilled water side outlet node.
-
-#### Field: Condenser Inlet Node Name
-
-This required alpha field contains the identifying name for the chiller condenser side inlet node. If the Chiller is AirCooled, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air dry-bulb temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air dry-bulb temperature is taken directly from the weather data.
-
-#### Field: Condenser Outlet Node Name
-
-This required alpha field contains the identifying name for the chiller condenser side outlet node.
-
-#### Field: Hot Water Inlet Node Name
-
-This required alpha field contains the identifying name for the chiller-heater hot water side inlet node. This node name must be the same as the inlet node name for the hot water supply branch on which this chiller-heater is placed.
-
-#### Field: Hot Water Outlet Node Name
-
-This required alpha field contains the identifying name for the chiller-heater hot water side outlet node.
-
-#### Field: Minimum Part Load Ratio
-
-A positive fraction that represents the minimum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. If the load on the chiller is below this fraction, the chiller will cycle. If the chiller is simultaneously heating and cooling, the greater part load ratio will be used. The default is 0.1.
-
-#### Field: Maximum Part Load Ratio
-
-A positive fraction that represents the maximum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. If greater than 1.0, the chiller is typically thought of as capable of being overloaded. The default is 1.0.
-
-#### Field: Optimum Part Load Ratio
-
-A positive fraction that represents the optimum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. It represents the most desirable operating point for the chiller. The default is 1.0.
-
-#### Field: Design Entering Condenser Water Temperature
-
-The temperature in degrees C of the water entering the condenser of the chiller when operating at design conditions. This is usually based on the temperature delivered by the cooling tower in a water cooled application. The default is 29C.
-
-#### Field: Design Leaving Chilled Water Temperature
-
-The temperature in degrees C of the water leaving the evaporator of the chiller when operating at design conditions; also called the chilled water supply temperature or leaving chilled water temperature. The default is 7C.
-
-#### Field: Design Chilled Water Flow Rate
-
-For variable volume this is the max flow and for constant flow this is the chilled water flow rate in m<sup>3</sup>/s.
-
-#### Field: Design Condenser Water Flow Rate
-
-The water flow rate at design conditions through the condenser in m<sup>3</sup>/s. This field can be autosized. This field can be autosized. This field is not used for Condenser Type=AirCooled.
-
-#### Field: Design Hot Water Flow Rate
-
-The water flow rate at design conditions through the heater side in m<sup>3</sup>/s.
-
-#### Field: Cooling Capacity Function of Temperature Curve Name
-
-The CoolCapfT curve represents the fraction of the cooling capacity of the chiller as it varies by temperature. The curve is normalized so that at design conditions the value of the curve should be 1.0. The curve is usually a biquadratic or bilinear curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature (see *Temperature Curve Input Variable* below). The available cooling capacity is computed as follows:
-
-<div>\[\begin{array}{l}CoolFuelInput = \\AvailCoolCap \cdot RunFrac \cdot CFIR \cdot CFIRfT({T_{cw,l}},{T_{cond}}) \cdot CFIRfPLR(CPLR)\end{array}\]</div>
-
-#### Field: Fuel Input to Cooling Output Ratio Function of Temperature Curve Name
-
-The CFIRfT curve represents the fraction of the fuel input to the chiller at full load as it varies by temperature. The curve is normalized so that at design conditions the value of the curve should be 1.0. The curve is usually a biquadratic or bilinear curve with the input variables being the leaving chilled water temperature and either the entering or leaving condenser water temperature (see *Temperature Curve Input Variable* below).
-
-#### Field: Fuel Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-
-The CFIRfPLR curve represents the fraction of the fuel input to the chiller as the load the chiller varies but the operating temperatures remain at the design values. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic. The cooling fuel input to the chiller is computed as follows:
-
-<div>\[\begin{array}{l}CoolElectricPower = \\NomCoolCap \cdot RunFrac \cdot CEIR \cdot CEIRfT({T_{cw,l}},{T_{cond}}) \cdot CEIRfPLR(CPLR)\end{array}\]</div>
-
-#### Field: Electric Input to Cooling Output Ratio Function of Temperature Curve Name
-
-The ElecCoolFT curve represents the fraction of the electricity to the chiller at full load as it varies by temperature. The curve is normalized so that at design conditions the of the curve should be 1.0. The curve is usually a biquadratic or bilinear  curve with the input variables being the leaving chilled water temperature and either  the entering or leaving condenser water temperature (see *Temperature Curve Input Variable* below).
-
-#### Field: Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-
-The ElecCoolFPLR curve represents the fraction of the electricity to the chiller as the load on the chiller varies but This operating temperatures remain at the design values.  The curve is normalized so that at full load the value of the curve should be 1.0.  The curve is usually linear or quadratic. The cooling electric input to the chiller is computed as follows:
-
-<div>\[AvailHeatCap = NomCoolCap \cdot HeatCoolCapRatio \cdot HeatCapfCPLR(CPLRh)\]</div>
-
-#### Field: Heating Capacity Function of Cooling Capacity Curve Name
-
-The HeatCapFCool curve represents how the heating capacity of the chiller varies with cooling capacity when the chiller is simultaeous heating and cooling. The curve is normalized so an input of 1.0 represents the nominal cooling capacity and an output of 1.0 represents the full heating capacity (see the Heating to Cooling Capacity Ratio input)  The curve is usually linear or quadratic. The available heating capacity is computed as follows:
-
-<div>\[HeatFuelInput = AvailHeatCap \cdot HFIR \cdot HFIRfHPLR(HPLR)\]</div>
-
-#### Field: Fuel Input to Heat Output Ratio During Heating Only Operation Curve Name
-
-When the chiller is operating as only a heater, the  curve is used to represent the fraction of fuel used as the heating load varies. It is normalized so that a value of 1.0 is the full available heating capacity. The curve is usually linear or quadratic and will probably be similar to a boiler curve for most chillers.
-
-<div>\[AvailCoolCap = NomCoolCap \cdot CoolCapfT({T_{cw,l}},{T_{cond}})\]</div>
-
-#### Field: Temperature Curve Input Variable
-
-This field sets the second independent variable in the three temperature dependent performance curves  to either the leaving or entering condenser water temperature. Manufacturers express the performance of their chillers using either the leaving condenser water temperature (to  the tower) or the entering condenser water temperature (from the tower). Valid choices for this field are: LeavingCondenser or EnteringCondenser. It is important that the performance curves and this field are consistent with each other. The default is EnteringCondenser.
-
-#### Field: Condenser Type
-
-The condenser can either be air cooled or connected to a cooling tower. This alpha field contains the keyword for the type of condenser, either AirCooled, or WaterCooled. The default is WaterCooled.
-
-#### Field: Chilled Water Temperature Lower Limit
-
-The chilled water supply temperature in degrees C below which the chiller will shut off. The default is 2C.
-
-#### Field: Fuel Higher Heating Value
-
-The fuel higher heating value in kJ/kg. *This field is not currently used*.
-
-#### Field: Chiller Flow Mode
-
-This field is deprecated and is not used.
-
-#### Field: Fuel Type
-
-This alpha field determines the type of fuel that the chiller uses. The default is **NaturalGas**. Valid values are **NaturalGas**, **PropaneGas**, **Diesel**, **Gasoline**, **FuelOil\#1**, **FuelOil\#2, OtherFuel1, OtherFuel2**.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Cooling Capacity, Design Chilled Water Flow Rate, Design Condenser Water Flow Rate and Design Hot Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-An example of this statement in an IDF is:
-
-```idf
-ChillerHeater:Absorption:DirectFired,
-    Big Chiller,             !- Chiller Name
-    100000,                  !- Nominal Cooling Capacity {W}
-    0.8,                     !- Heating to Cooling capacity ratio
-    0.97,                    !- Fuel Input to Cooling Output Ratio
-    1.25,                    !- Fuel Input to Heating Output Ratio
-    0.01,                    !- Electric Input to Cooling Output Ratio
-    0.005,                   !- Electric Input to Heating Output Ratio
-    Big Chiller Inlet Node,  !- Chilled Water Side Inlet Node Name
-    Big Chiller Outlet Node, !- Chilled Water Side Outlet Node Name
-    Big Chiller Condenser Inlet Node,  !- Condenser Side Inlet Node Name
-    Big Chiller Condenser Outlet Node,  !- Condenser Side Outlet Node Name
-    Purchased Heat Inlet Node,  !- Hot Water Side Inlet Node Name
-    Purchased Heat Outlet Node,  !- Hot Water Side Outlet Node Name
-    0.000001,                !- Minimum Part Load Ratio
-    1.0,                     !- Maximum Part Load Ratio
-    0.6,                     !- Optimum Part Load Ratio
-    29,                      !- Design Entering Condenser Water Temperature {C}
-    7,                       !- Design Leaving Chilled Water Temperature {C}
-    0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
-    0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
-    0.0043,                  !- Design Hot Water Flow Rate {m3/s}
-    GasAbsFlatBiQuad,        !- Cooling Capacity Function of Temperature Curve Name
-    GasAbsFlatBiQuad,        !- Fuel Input to Cooling Output Ratio Function of Temperature Curve Name
-    GasAbsLinearQuad,        !- Fuel Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-    GasAbsFlatBiQuad,        !- Electric Input to Cooling Output Ratio Function of Temperature Curve Name
-    GasAbsFlatQuad,      !- Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-    GasAbsInvLinearQuad,     !- Heating Capacity Function of Cooling Capacity Curve Name
-    GasAbsLinearQuad,        !- Fuel Input to Heat Output Ratio During Heating Only Operation Curve Name
-    EnteringCondenser,       !- Temperature Curve Input Variable
-    WaterCooled,             !- Condenser Type
-    2,                       !- Chilled Water Temperature Lower Limit {C}
-    0,                       !- Fuel Higher Heating Value {kJ/kg}
-    VariableFlow,            !- Chiller Flow Mode
-    NaturalGas,              !- Fuel Type
-    1.0;                     !- Sizing Factor
-```
-
-
-### Direct Fired Absorption Chiller Outputs
-
-* HVAC,Average,Chiller Heater Electric Power [W]
-
-* HVAC,Sum,Chiller Heater Electric Energy [J]
-
-* Zone,Meter,Electricity:Plant [J]
-
-* Zone,Meter,Cooling:Electricity [J]
-
-* HVAC,Average,Chiller &lt;Fuel Type&gt; Consumption Rate [W]
-
-* HVAC,Sum,Chiller &lt;Fuel Type&gt; Consumption [J]
-
-* Zone,Meter,&lt;Fuel Type&gt;:Plant [J]
-
-* Zone,Meter,Cooling:&lt;Fuel Type&gt; [J]
-
-* HVAC,Average,Chiller Evaporator Cooling Rate [W]
-
-* HVAC,Sum,Chiller Heater Evaporator Cooling Energy [J]
-
-* Zone,Meter,EnergyTransfer:Plant [J]
-
-* Zone,Meter,Chillers:EnergyTransfer [J]
-
-* HVAC,Average,Chiller Heater Evaporator Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Evaporator Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Evaporator Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Heater Condenser Heat Transfer Rate [W]
-
-* HVAC,Sum,Chiller Heater Condenser Heat Transfer Energy [J]
-
-* Zone,Meter,HeatRejection:EnergyTransfer [J]
-
-
-The following output is applicable only for air-cooled chillers
-
-* HVAC,Average,Chiller Heater Condenser Inlet Temperature [C]
-
-
-
-The following three outputs are only available for water-cooled chillers
-
-* HVAC,Average,Chiller Heater Condenser Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Condenser Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Condenser Mass Flow Rate [kg/s]
-
-
-
-Outputs specific to Direct Fired Absorption Chiller
-
-* HVAC,Average,Chiller Heater Runtime Fraction []
-
-
-Outputs specific to Direct Fired Absorption Chiller during cooling operation
-
-* HVAC,Average,Chiller Heater Cooling &lt;Fuel Type&gt; Rate [W]
-
-* HVAC,Sum,Chiller Heater Cooling &lt;Fuel Type&gt; Consumption [J]
-
-* HVAC,Average,Chiller Heater Cooling Electric Power [W]
-
-* HVAC,Sum,Chiller Heater Cooling Electric Energy [J]
-
-* HVAC,Average,Chiller Heater Cooling Part Load Ratio
-
-* HVAC,Average,Chiller Heater Cooling Rate [W]
-
-* HVAC,Average,Chiller Heater Cooling COP [W/W]
-
-
-Outputs specific to Direct Fired Absorption Chiller during heating operation
-
-* HVAC,Average,Chiller Heater Heating Rate [W]
-
-* HVAC,Sum,Chiller Heater Heating Energy [J]
-
-* HVAC,Average,Chiller Heater Heating &lt;Fuel Type&gt; Rate [W]
-
-* HVAC,Sum,Chiller Heater Heating &lt;Fuel Type&gt; Energy [J]
-
-* HVAC,Average,Chiller Heater Heating Electric Power [W]
-
-* HVAC,Sum,Chiller Heater Heating Electric Energy [J]
-
-* HVAC,Average,Chiller Heater Heating Part Load Ratio []
-
-* HVAC,Average,Chiller Heater Heating Rate [W]
-
-* HVAC,Average,Chiller Heater Heating Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Heating Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Heating Mass Flow Rate [kg/s]
-
-
-The "Chiller" output variables are defined above under "Generic Chiller Outputs."  The specific "Direct Fired Absorption Chiller" output variables and exceptions to the generic outputs are defined below.
-
-#### Chiller Heater Electric Power [W]
-
-#### Chiller Heater Electric Energy [J]
-
-These outputs are the electric power input to the chiller when operating in cooling mode, heating mode, or both. This value is not metered, but the separate cooling and heating electric consumption are metered (see below).
-
-#### Chiller Heater &lt;Fuel Type&gt; Rate [W]
-
-#### Chiller Heater &lt;Fuel Type&gt; Energy [J]
-
-These outputs are the fuel input to the chiller when operating in cooling mode, heating mode, or both depending on the fuel type entered. This value is not metered, but the separate cooling and heating fuel consumption are metered (see below).
-
-#### Chiller Heater Runtime Fraction []
-
-This is the average fraction of the time period during which the direct fired absorption chiller-heater was operating in either cooling mode, heating mode, or both.
-
-#### Chiller Heater Cooling &lt;Fuel Type&gt; Rate [W]
-
-#### Chiller Heater Cooling &lt;Fuel Type&gt; Energy [J]
-
-These outputs are the fuel input to the direct fired absorption chiller to serve cooling operation. Consumption is metered on Cooling:&lt;Fuel Type&gt;, &lt;Fuel Type&gt;:Plant, and &lt;Fuel Type&gt;:Facility.
-
-#### Chiller Heater Cooling Electric Power [W]
-
-#### Chiller Heater Cooling Electric Energy [J]
-
-These outputs are the electricity input to the direct fired absorption chiller to serve cooling operation. Consumption is metered on Cooling:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Chiller Heater Cooling Rate [W]
-
-This is the average available cooling capacity for the reported time period.
-
-#### Chiller Heater Cooling Part Load Ratio
-
-This is the average cooling load (Chiller Evaporator Cooling Rate [W]) divided by the average available cooling capacity (Chiller Heater Cooling Rate [W]) for the reported time period.
-
-#### Chiller Heater Cooling COP
-
-This is the average coefficient of performance for the chiller in cooling operation, calculated as the average cooling load (Chiller Evaporator Cooling Rate [W]) divided by the average fuel consumption during cooling (Direct Fired Absorption Chiller Cooling &lt;Fuel Type&gt; Consumption Rate [W]) for the reported time period. If the chiller cooling fuel consumption rate (denominator) is zero, then this output variable is set to zero.
-
-#### Chiller Heater Heating Rate [W]
-
-#### Chiller Heater Heating Energy [J]
-
-These outputs are the heating delivered by the direct fired absorption chiller-heater to serve heating operation. Energy is metered on Boilers:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Chiller Heater Heating &lt;Fuel Type&gt; Rate [W]
-
-#### Chiller Heater Heating &lt;Fuel Type&gt; Energy [J]
-
-These outputs are the fuel input to the direct fired absorption chiller-heater to serve heating operation. Consumption is metered on Heating:&lt;Fuel Type&gt;, &lt;Fuel Type&gt;:Plant, and &lt;Fuel Type&gt;:Facility.
-
-#### Chiller Heater Heating Electric Power [W]
-
-#### Chiller Heating Heating Electric Energy [J]
-
-These outputs are the electric power input to the direct fired absorption chiller to serve heating operation. Consumption is metered on Heating:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Chiller Heater Heating Rate [W]
-
-This is the average available heating capacity for the reported time period.
-
-#### Chiller Heater Heating Part Load Ratio
-
-This is the average heating load (Chiller Heater Heating Rate [W]) divided by the average available heating capacity (Chiller Heater Heating Rate [W]) for the reported time period.
-
-#### Chiller Heater Heating Inlet Temperature [C]
-
-#### Chiller Heater Heating Outlet Temperature [C]
-
-#### Chiller Heater Heating Mass Flow Rate [kg/s]
-
-These outputs are the hot water inlet and outlet temperatures and flow rate for the direct fired absorption chiller-heater during heating mode operation.
-
-### ChillerHeater:Absorption:DoubleEffect
-
-This chiller is an exhaust fired absorption chiller-heater which is modeled using performance curves similar to the direct fired absorption chiller in DOE-2.1E. The model uses the exhaust gas output from MicroTurbine. This type of chiller is unusual for EnergyPlus, because it may be used in the same plant on both a chilled water supply branch and a hot water supply branch. The chiller has six node connections for chilled water, condenser water, and hot water, and can provide simultaneous heating and cooling. During simultaneous operation, the heating capacity is reduced as the cooling load increases (for more details see below). Some equations are provided below to help explain the function of the various performance curves. For a detailed description of the algorithm and how the curves are used in the calculations, please see the Engineering Reference.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the chiller.
-
-#### Field: Nominal Cooling Capacity
-
-This numeric field contains the nominal cooling capability of the chiller in Watts. Autosize can be used for this field.
-
-#### Field: Heating to Cooling Capacity Ratio
-
-A positive fraction that represents the ratio of the heating capacity divided by the cooling capacity at rated conditions. The default is 0.8.
-
-#### Field: Thermal Energy Input to Cooling Output Ratio
-
-A positive fraction that represents the ratio of the instantaneous cooling Thermal Energy used divided by the cooling capacity at rated conditions. The default is 0.97.
-
-#### Field: Thermal Energy Input to Heating Output Ratio
-
-A positive fraction that represents the ratio of the instantaneous heating Thermal Energy used divided by the nominal heating capacity. The default is 1.25.
-
-#### Field: Electric Input to Cooling Output Ratio
-
-A positive fraction that represents the ratio of the instantaneous electricity used divided by the cooling capacity at rated conditions. If the chiller is both heating and cooling only the greater of the computed cooling and heating electricity is used. The default is 0.01.
-
-#### Field: Electric Input to Heating Output Ratio
-
-A positive fraction that represents the ratio of the instantaneous electricity used divided by the nominal heating capacity. If the chiller is both heating and cooling, the greater of the cooling electricity and heating eletricity is used. The default is 0.0.
-
-#### Field: Chilled Water Inlet Node Name
-
-This required alpha field contains the identifying name for the chiller chilled water side inlet node. This node name must be the same as the inlet node name for the chilled water supply branch on which this chiller is placed.
-
-#### Field: Chilled Water Outlet Node Name
-
-This required alpha field contains the identifying name for the chiller chilled water side outlet node.
-
-#### Field: Condenser Inlet Node Name
-
-This required alpha field contains the identifying name for the chiller condenser side inlet node. If the Chiller is AirCooled, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air dry-bulb temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air dry-bulb temperature is taken directly from the weather data.
-
-#### Field: Condenser Outlet Node Name
-
-This required alpha field contains the identifying name for the chiller condenser side outlet node.
-
-#### Field: Hot Water Inlet Node Name
-
-This required alpha field contains the identifying name for the chiller-heater hot water side inlet node. This node name must be the same as the inlet node name for the hot water supply branch on which this chiller-heater is placed.
-
-#### Field: Hot Water Outlet Node Name
-
-This required alpha field contains the identifying name for the chiller-heater hot water side outlet node.
-
-#### Field: Minimum Part Load Ratio
-
-A positive fraction that represents the minimum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. If the load on the chiller is below this fraction, the chiller will cycle. If the chiller is simultaneously heating and cooling, the greater part load ratio will be used. The default is 0.1.
-
-#### Field: Maximum Part Load Ratio
-
-A positive fraction that represents the maximum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. If greater than 1.0, the chiller is typically thought of as capable of being overloaded. The default is 1.0.
-
-#### Field: Optimum Part Load Ratio
-
-A positive fraction that represents the optimum cooling or heating output possible when operated continually at rated temperature conditions divided by the available cooling or heating capacity at those same conditions. It represents the most desirable operating point for the chiller. The default is 1.0.
-
-#### Field: Design Entering Condenser Water Temperature
-
-The temperature in degrees C of the water entering the condenser of the chiller when operating at design conditions. This is usually based on the temperature delivered by the cooling tower in a water cooled application. The default is 29°C.
-
-#### Field: Design Leaving Chilled Water Temperature
-
-The temperature in degrees C of the water leaving the evaporator of the chiller when operating at design conditions; also called the chilled water supply temperature or leaving chilled water temperature. The default is 7°C.
-
-#### Field: Design Chilled Water Flow Rate
-
-For variable volume this is the max flow and for constant flow this is the chilled water flow rate in m<sup>3</sup>/s. This field can be autosized.
-
-#### Field: Design Condenser Water Flow Rate
-
-The water flow rate at design conditions through the condenser in m<sup>3</sup>/s. This field can be autosized. This field is not used for Condenser Type=AirCooled.
-
-#### Field: Design Hot Water Flow Rate
-
-The water flow rate at design conditions through the heater side in m<sup>3</sup>/s. This field can be autosized.
-
-#### Field: Cooling Capacity Function of Temperature Curve Name
-
-The CoolCapfT curve represents the fraction of the cooling capacity of the chiller as it varies with temperature. The curve is normalized so that at design conditions the value of the curve should be 1.0. The curve is usually a biquadratic or bilinear curve with the input variables being the leaving chilled water temperature and the entering condenser water temperature (see *Temperature Curve Input Variable* below). The available cooling capacity is computed as follows:
-
-<div>\[\begin{array}{l}CoolThermalEnergyInput = AvailCoolCap \cdot RunFrac \cdot TeFIR \cdot \\\quad \quad \quad \quad \quad \quad TeFIRfT\left( {{T_{cw,l}},{T_{cond}}} \right) \cdot TeFIRfPLR(CPLR)\end{array}\]</div>
-
-#### Field: Thermal Energy Input to Cooling Output Ratio Function of Temperature Curve Name
-
-The TeFIRfT curve represents the fraction of the Thermal Energy Input to the chiller at full load as it varies with temperature. The curve is normalized so that at design conditions the value of the curve should be 1.0. The curve is usually a biquadratic or bilinear curve with the input variables being the leaving chilled water temperature and the entering condenser water temperature (see *Temperature Curve Input Variable* below).
-
-#### Field: Thermal Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-
-The TeFIRfPLR curve represents the fraction of the Thermal Energy Input to the chiller as the load on the chiller varies but the operating temperatures remain at the design values. The curve is normalized so that at full load the value of the curve should be 1.0. The curve is usually linear or quadratic.
-
-The cooling Thermal Energy Input to the chiller is computed as follows:
-
-<div>\[CoolElectricPower = NomCoolCap \cdot RunFrac \cdot CEIR \cdot CEIRfT\left( {{T_{cw,l}},{T_{cond}}} \right) \cdot CEIRfPLR(CPLR)\]</div>
-
-#### Field: Electric Input to Cooling Output Ratio Function of Temperature Curve Name
-
-The CEIRfT curve represents the fraction of the electricity to the chiller at full load as it varies with temperature. The curve is normalized so that at design conditions the of the curve should be 1.0. The curve is usually a biquadratic or bilinear  curve with the input variables being the leaving chilled water temperature and either  the entering or leaving condenser water temperature (see *Temperature Curve Input Variable* below).
-
-#### Field: Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-
-The CEIRfPLR curve represents the fraction of the electricity to the chiller as the load on the chiller varies but This operating temperatures remain at the design values.  The curve is normalized so that at full load the value of the curve should be 1.0.  The curve is usually linear or quadratic.
-
-The cooling electric input to the chiller is computed as follows:
-
-<div>\[AvailHeatCap = NomCoolCap \cdot HeatCoolCapRatio \cdot HeatCapfCPLR(CPLRh)\]</div>
-
-#### Field: Heating Capacity Function of Cooling Capacity Curve Name
-
-The HeatCapFCPLR curve represents how the heating capacity of the chiller varies with cooling capacity when the chiller is simultaneously heating and cooling. The curve is normalized so an input of 1.0 represents the nominal cooling capacity and an output of 1.0 represents the full heating capacity (see the Heating to Cooling Capacity Ratio input)  The curve is usually linear or quadratic.
-
-The available heating capacity is computed as follows:
-
-<div>\[HeatThermalEnergyInput = AvailHeatCap \cdot HFIR \cdot HFIRfHPLR(HPLR)\]</div>
-
-#### Field: Thermal Energy Input to Heat Output Ratio During Heating Only Operation Curve Name
-
-When the chiller is operating as only a heater, the  curve is used to represent the fraction of Thermal Energy used as the heating load varies. It is normalized so that a value of 1.0 is the full available heating capacity. The curve is usually linear or quadratic and will probably be similar to a boiler curve for most chillers.
-
-The heating Thermal Energy Input to the chiller is computed as follows:
-
-<div>\[TheoreticalFuelUse = \frac{{BoilerLoad}}{{NominalThermalEfficiency}}\]</div>
-
-#### Field: Temperature Curve Input Variable
-
-This field sets the second independent variable in the three temperature dependent performance curves  to the entering condenser water temperature. Manufacturers express the performance of their chillers typically using the entering condenser water temperature (from the tower). ). This alpha field contains the keyword for the type of temperature input variable, , either **EnteringCondenserTemperature**, or **LeavingCondenserTemperature**. The default is EnteringCondenserTemperature.
-
-#### Field: Condenser Type
-
-The condenser can either be air cooled or water cooled (connected to a cooling tower). This alpha field contains the keyword for the type of condenser, either AirCooled, or WaterCooled. The default is WaterCooled.
-
-#### Field: Chilled Water Temperature Lower Limit
-
-The chilled water supply temperature in degrees C below which the chiller will shut off. The default is 2°C.
-
-#### Field: Exhaust Source
-
-This alpha field determines the type of exhaust source the chiller uses. The default is MicroTurbine. Key Generator:MicroTurbine
-
-#### Field: Exhaust Source Object
-
-This alpha field shows the name of the Exhaust source object – a Generator:MicroTurbine in this case
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. Min value should not be less than 0 and here is no max. The default is 1.  The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Cooling Capacity, Design Chilled Water Flow Rate, Design Condenser Water Flow Rate and Design Hot Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-An example of this statement in an IDF is:
-
-```idf
-ChillerHeater:Absorption:DoubleEffect,
-    Exh Chiller,             !- Chiller Name
-    100000,                  !- Nominal Cooling Capacity {W}
-    0.8,                     !- Heating to Cooling capacity ratio
-    0.97,                    !- Thermal Energy Input to Cooling Output Ratio
-    1.25,                    !- Thermal Energy Input to Heating Output Ratio
-    0.01,                    !- Electric Input to Cooling Output Ratio
-    0.005,                   !- Electric Input to Heating Output Ratio
-    Exh Chiller Inlet Node,  !- Chilled Water Side Inlet Node Name
-    Exh Chiller Outlet Node, !- Chilled Water Side Outlet Node Name
-    Exh Chiller Condenser Inlet Node,  !- Condenser Side Inlet Node Name
-    Exh Chiller Condenser Outlet Node,  !- Condenser Side Outlet Node Name
-    Exh Chiller Heating Inlet Node,  !- Hot Water Side Inlet Node Name
-    Exh Chiller Heating Outlet Node,  !- Hot Water Side Outlet Node Name
-    0.000001,                !- Minimum Part Load Ratio
-    1.0,                     !- Maximum Part Load Ratio
-    0.6,                     !- Optimum Part Load Ratio
-    29,                      !- Design Entering Condenser Water Temperature {C}
-    7,                       !- Design Leaving Chilled Water Temperature {C}
-    0.0011,                  !- Design Chilled Water Flow Rate {m3/s}
-    0.0011,                  !- Design Condenser Water Flow Rate {m3/s}
-    0.0043,                  !- Design Hot Water Flow Rate {m3/s}
-     ExhAbsorb_CapFt,        !- Cooling Capacity Function of Temperature Curve Name
-    ExhAbsorb_EIRFt,         !- Thermal Energy Input to Cooling Output Ratio Function of Temperature Curve Name
-     ExhAbsorb_PLR,        !- Thermal Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-    ExhAbsFlatBiQuad,        !- Electric Input to Cooling Output Ratio Function of Temperature Curve Name
-    ExhAbsFlatQuad,      !- Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-    ExhAbsInvLinearQuad,     !- Heating Capacity Function of Cooling Capacity Curve Name
-    ExhAbsLinearQuad,        !- Thermal Energy Input to Heat Output Ratio During Heating Only Operation Curve Name
-    EnteringCondenser,       !- Temperature Curve Input Variable
-    WaterCooled,             !- Condenser Type
-    2,                       !- Chilled Water Temperature Lower Limit {C}
-    Generator:MicroTurbine ; ! Field Exhaust Source Object Type
-    Capston500 ;                ! Field Exhaust Source name
-    1.0;                       !- Sizing Factor
-```
-
-
-### Exhaust Fired Absorption Chiller Outputs
-
-* HVAC,Average,Chiller Heater Electric Power [W]
-
-* HVAC,Sum,Chiller Heater Electric Energy [J]
-
-* HVAC,Average,Chiller Heater Evaporator Cooling Rate [W]
-
-* HVAC,Sum,Chiller Heater Evaporator Cooling Energy [J]
-
-* HVAC,Average,Chiller Heater Evaporator Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Evaporator Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Evaporator Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Heater Condenser Heat Transfer Rate [W]
-
-* HVAC,Sum,Chiller Heater Condenser Heat Transfer Energy [J]
-
-
-
-The following output is applicable only for air-cooled chillers
-
-* HVAC,Average,Chiller Heater Condenser Inlet Temperature [C]
-
-
-
-The following three outputs are only available for water-cooled chillers
-
-* HVAC,Average,Chiller Heater Condenser Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Condenser Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Condenser Mass Flow Rate [kg/s]
-
-
-
-Outputs specific to Exhaust Fired Absorption Chiller
-
-* HVAC,Average,Chiller Heater Runtime Fraction []
-
-
-
-Outputs specific to Exhaust Fired Absorption Chiller during cooling operation
-
-* HVAC,Average,Chiller Heater Cooling Electric Power [W]
-
-* HVAC,Sum,Chiller Heater Cooling Electric Energy [J]
-
-* HVAC,Average,Chiller Heater Cooling Part Load Ratio
-
-* HVAC,Average,Chiller Heater Maximum Cooling Rate [W]HVAC,Average,Chiller Heater Cooling Source Heat Transfer Rate [W]
-
-* HVAC,Average, Chiller Heater Cooling Source Heat COP [W/W]
-
-* HVAC,Average, Chiller Heater Source Exhaust Inlet Mass Flow Rate [kg/s]
-
-* HVAC,Average, Chiller Heater Source Exhaust Inlet Temperature [C]
-
-
-
-Outputs specific to Exhaust Fired Absorption Chiller during heating operation
-
-* HVAC,Average,Chiller Heater Heating Rate [W]
-
-* HVAC,Sum,Chiller Heater Heating Energy [J]
-
-* HVAC,Average,Chiller Heater Heating Electric Power [W]
-
-* HVAC,Sum,Chiller Heater Heating Electric Energy [J]
-
-* Zone,Meter,Heating:Electricity [J]
-
-* HVAC,Average,Chiller Heater Heating Part Load Ratio
-
-* HVAC,Average,Chiller Heater Maximum Heating Rate [W]
-
-* HVAC,Average,Chiller Heater Heating Source Heat Transfer Rate
-
-* HVAC,Average,Chiller Heater Heating Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Heating Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heater Heating Mass Flow Rate [kg/s]
-
-
-
-The "Chiller" output variables are defined above under "Generic Chiller Outputs."  The specific "Exhaust Fired Absorption Chiller" output variables and exceptions to the generic outputs are defined below.
-
-#### Chiller Heater Electric Power [W]
-
-#### Chiller Heater Electric Energy [J]
-
-These outputs are the electric power input to the chiller when operating in cooling mode, heating mode, or both. This value is not metered, but the separate cooling and heating electric consumption are metered (see below).
-
-#### Chiller Heater Runtime Fraction []
-
-This is the average fraction of the time period during which the Exhaust Fired absorption chiller-heater was operating in either cooling mode, heating mode, or both.
-
-These outputs are the electricity input to the Exhaust Fired absorption chiller heater to serve cooling operation. Consumption is metered on Cooling:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Chiller Heater Maximum Cooling Rate [W]
-
-This is the average available cooling capacity for the reported time period.
-
-#### Chiller Heater Cooling Part Load Ratio []
-
-This is the average cooling load (Chiller Heater Evaporator Cooling Rate [W]) divided by the average available cooling capacity (Chiller Heater Maximum Cooling Rate [W]) for the reported time period.
-
-#### Chiller Heater Cooling Source Heat COP [W/W]
-
-This is the average coefficient of performance for the chiller in cooling operation, calculated as the average cooling load (Chiller Heater Evaporator Cooling Rate [W]) divided by the average thermal energy use during cooling (Chiller Heater Cooling Source Heat Transfer Rate [W]) for the reported time period. If the chiller cooling thermal energy use rate (denominator) is zero, then this output variable is set to zero.
-
-#### Chiller Heater Heating Rate [W]
-
-#### Chiller Heater Heating Energy [J]
-
-#### Chiller Heater Heating Electric Power [W]
-
-#### Chiller Heater Heating Electric Energy [J]
-
-These outputs are the electric power input to the Exhaust Fired absorption chiller to serve heating operation. Consumption is metered on Heating:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Chiller Heater Maximum Heating Rate [W]
-
-This is the average available heating capacity for the reported time period.
-
-#### Chiller Heater Heating Part Load Ratio []
-
-This is the average heating load (Chiller Heater Heating Rate [W]) divided by the average available heating capacity (Chiller Heater Maximum Heating Rate [W]) for the reported time period.
-
-#### Chiller Heater Heating Inlet Temperature [C]
-
-#### Chiller Heater Heating Outlet Temperature [C]
-
-#### Chiller Heater Heating Mass Flow Rate [kg/s]
-
-These outputs are the hot water inlet and outlet temperatures and flow rate for the Exhaust Fired absorption chiller-heater during heating mode operation.
-
-#### Chiller Heater Heating Heat Recovery Potential Rate (W)
-
-The heat recovery potential calculated based on Microturbine exhaust temperature and flow rate during heating mode
-
-#### Chiller Heater Heating Source Heat Transfer Rate (W)
-
-The thermal energy consumption rate required  for heating.
-
-#### Chiller Heater Cooling Heat Recovery Potential Rate (W)
-
-The heat recovery potential calculated based on Microturbine exhaust temperature and flow rate during cooling mode.
-
-#### Chiller Heater Cooling Source Heat Transfer Rate (W)
-
-The thermal energy consumption rate required for cooling.
-
-#### Chiller Heater Condenser Inlet Temperature [C]
-
-The condenser (heat rejection) inlet temperature for air-cooled or water chiller heater. For an air-cooled chiller heater, this output would be the dry-bulb temperature of the air entering the condenser coil. For a water cooled chiller heater, this output would be the wet-bulb temperature of the air entering the condenser coil.
-
-#### Chiller Heater Condenser Heat Transfer Energy [J]
-
-The condenser heat transfer energy is the heat rejected from the chiller heater to either a condenser water loop or through an air-cooled condenser. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period. Chiller Heater Condenser Heat Transfer Energy is metered on HeatRejection:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Chiller Heater Condenser Heat Transfer Rate [W]
-
-The condenser heat transfer is the rate of heat rejected from the chiller heater to either a condenser water loop or through an air-cooled condenser. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Chiller Heater Condenser Mass Flow Rate [kg/s]
-
-This is the condenser coil outlet water mass flow rate in kilograms per second. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Chiller Heater Condenser Outlet Temperature [C]
-
-This is the condenser coil outlet water temperature in degrees C. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported
-
-#### Chiller Heater Evaporator Cooling Energy [J]
-
-The evaporator heat transfer is the cooling delivered by the chiller heater. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period. Chiller Heater Evaporator Cooling Energy is metered on Chillers:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Chiller Heater Evaporator Cooling Rate [W]
-
-The evaporator heat transfer rate of cooling delivered by the chiller heater. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Chiller Heater Evaporator Inlet Temperature [C]
-
-The evaporator (chilled water) inlet temperature over the time step being reported.
-
-#### Chiller Heater Evaporator Mass Flow Rate [kg/s]
-
-The evaporator (chilled water) average mass flow rate over the time step being reported
-
-#### Chiller Heater Evaporator Outlet Temperature [C]
-
-The evaporator (chilled water) outlet temperature over the time step being reported
-
-#### Chiller Heater Cooling Electric Energy [J]
-
-The electric power input to the exhaust fired absorption chiller to serve cooling operation. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period. Consumption is metered on Heating:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Chiller Heater Cooling Electric Power [W]
-
-The electric power input to the Exhaust Fired absorption chiller to serve cooling operation. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Chiller Heater Source Exhaust Inlet Mass Flow Rate [kg/s]
-
-The exhaust flow rate from the Micro Turbine
-
-#### Chiller Heater Source Exhaust Inlet Temperature [C]
-
-The exhaust temperature from  the Micro Turbine
-
-### Boiler:HotWater
-
-The boiler model calculates the performance of fuel oil, gas and electric boilers. Boiler performance is based on nominal thermal efficiency. A normailized efficiency performance curve may be used to more accurately represent the performance of non-electric boilers but is not considered a required input. When using the normalized efficiency performance curve, if all coefficients are not required simply set the unused coefficients to 0. For example, an electric boiler could be modeled by setting the nominal thermal efficiency to a value in the range of 0.96 to 1.0. Coefficient A0 in the normalized efficiency performance curve would equal 1 and all other coefficients would be set to 0. Coefficients for other types of non-electric boilers would set a combination of the available coefficents to non-zero values.
-
-#### Field: Name
-
-This required alpha field contains the identifying name for the boiler.
-
-#### Field: Fuel Type
-
-This required choice field specifies the type of fuel used by the boiler. The fuel type can be **Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1** or **OtherFuel2**.
-
-#### Field: Nominal capacity
-
-This numeric field contains the nominal operating capacity (W) of the boiler. The boiler may be autosized and would require a heating plant sizing object.
-
-#### Fuel Use Equation
-
-The model is based the following two equations:
-
-<div>\[FuelUsed = \frac{{TheoreticalFuelUse}}{{NormalizedBoilerEfficiencyCurveOutput}}\]</div>
-
-<div>\[Linear \to Eff = {A_0} + {A_1}\cdot PLR\]</div>
-
-#### Field: Nominal Thermal Efficiency
-
-This required numeric field contains the heating efficiency (as a fraction between 0 and 1) of the boiler’s burner.  This is the efficiency relative to the higher heating value (HHV) of fuel at a part load ratio of 1.0 and the temperature entered for the Design Boiler Water Outlet Temp. Manufacturers typically specify the efficiency of a boiler using the higher heating value of the fuel. For the rare occurences when a manufacturers (or particular data set) thermal efficiency is based on the lower heating value (LHV) of the fuel, multiply the thermal efficiency by the lower-to-higher heating value ratio. For example, assume a fuel’s lower and higher heating values are approximately 45,450 and 50,000 kJ/kg, respectively. For a manuracturers thermal effiency rating of 0.90 (based on the LHV), the nominal thermal efficiency entered here is 0.82 (i.e. 0.9 multiplied by 45,450/50,000).
-
-#### Field: Efficiency Curve Temperature Evaluation Variable
-
-This field is used to control which value for hot water temperature is used when evaluating the efficiency curve specified in the next field (if applicable).  There are two options,  EnteringBoiler or LeavingBoiler.  EnteringBoiler indicates that the efficiency curves will be evaluated using the temperature at boiler inlet node.  LeavingBoiler indicates that the efficiency curves will be evaluated using the temperature at the boiler outlet.  This field is only used if type of curve is one that uses temperature as a independent variable.
-
-#### Field: Normalized Boiler Efficiency Curve Name
-
-This alpha field contains the curve name which describes the normalized heating efficiency (as a fraction of nominal thermal efficiency) of the boiler’s burner. If this field is left blank, the nominal thermal efficiency is assumed to be constant (i.e., Fuel Used is equal to the Theoretical Fuel Use in the equation above). When a boiler efficiency curve is used, the curve may be any valid curve object with 1 (PLR) or 2 (PLR and boiler outlet water temperature) independent variables. A tri-quadratic curve object is not allowed since it uses 3 independent variables. The linear, quadratic, and cubic curve types may be used when the boiler efficiency is solely a function of boiler part-load ratio (PLR). When this type of curve is used, the boiler should operate at (or very near) the design boiler water outlet temperature. Other curve types may be used when the boiler efficiency is a function of both PLR and boiler water temperature. Examples of valid single and dual independent variable equations are shown below. For all curve types PLR is always the x independent variable. When using 2 independent variables, the boiler outlet water temperature (Toutlet) is always the y independent variable.
-
-<div>\[Quadratic \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2}\]</div>
-
-<div>\[Cubic \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2} + {A_3}\cdot PL{R^3}\]</div>
-
-<div>\[Cubic \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2} + {A_3}\cdot PL{R^3}\]</div>
-
-<div>\[BiQuadratic \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2} + {A_3}\cdot {T_w} + {A_4}\cdot {T_w}^2 + {A_5}\cdot PLR\cdot {T_w}\]</div>
-
-<div>\[QuadraticLinear \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2} + {A_3}\cdot {T_w} + {A_4}\cdot PLR\cdot {T_w} + {A_5}\cdot PL{R^2}\cdot {T_w}\]</div>
-
-<div>\[\begin{array}{l}Bicubic \to Eff = {A_0} + {A_1}\cdot PLR + {A_2}\cdot PL{R^2} + {A_3}\cdot {T_w} + {A_4}{T_w}^2 + {A_5}PLR\cdot {T_w} + {A_6}PL{R^3}\\\quad \quad \quad \quad \quad \quad \quad  + {A_7}\cdot {T_w}^3 + {A_8}\cdot PL{R^2}\cdot {T_w} + {A_9}\cdot PLR\cdot {T_w}^2\end{array}\]</div>
-
-where
-
-Eff = normalized boiler efficiency
-
-PLR = boiler part-load ratio
-
-T<sub>w</sub> = boiler water temperature [ºC] ], this can be either entering or leaving temperature depending on the setting in the previous field
-
-#### Field: Design Water Outlet Temperature
-
-This numeric field contains the desired boiler water outlet temperature in Celsius.
-
-#### Field: Design Water Flow Rate
-
-This numeric field contains the maximum design water volumetric flow rate in m<sup>3</sup>/sec. This should be the largest flow rate than can be heated to the design outlet temperature. This field is autosizable.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the minimum part load ratio. If the ratio of demand to boiler nominal capacity is less than the minimum part load ratio, then the Min PLR will determine the operating PLR. The expected range is between 0 and 1. If this field is left blank, the default value is 0.0.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the maximum part load ratio. If the ratio of demand to boiler nominal capacity is greater than the maximum part load ratio, then the Max PLR will determine the operating PLR. This value may exceed 1, but the normal range is between 0 and 1.1. If this field is left blank, the default value is 1.0.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the optimum part load ratio. This is the part load ratio at which the boiler performs at its maximum efficiency. If this field is left blank, the default value is 1.0.
-
-#### Field: Boiler Water Inlet Node Name
-
-This required alpha field contains the water inlet node name.
-
-#### Field: Boiler Water Outlet Node Name
-
-This required alpha field contains the water outlet node name.
-
-#### Field: Water Outlet Upper Temperature Limit
-
-This numeric field contains the outlet temperature upper limit. If this field is left blank, the default value is 99.9ºC.
-
-#### Field: Boiler Flow Mode
-
-This choice field determines how the boiler operates with respect to the intended fluid flow through the device.  There are three different choices for specifying operating modes for the intended flow behavior:  “NotModulated,� “ConstantFlow,� and “LeavingSetpointModulated.�  NotModulated is useful for either variable or constant speed pumping arrangements where the boiler is passive in the sense that although it makes a nominal request for its design flow rate it can operate at varying flow rates.  ConstantFlow is useful for constant speed pumping arrangements where the boiler’s request for flow is more strict and can increase the overall loop flow.  LeavingSetpointModulated changes the boiler model to internally vary the flow rate so that the temperature leaving the boiler matches a setpoint.  In all cases the operation of the external plant system can also impact the flow through the boiler -- for example if the relative sizes and operation are such that flow is restricted and the requests cannot be met.   The default, if not specified, is NotModulated.
-
-#### Field: Parasitic Electric Load
-
-This optional numeric field contains the parasitic electric power (W) consumed by a forced draft fan or other electrical device associated with the boiler. This parasitic electric load is consumed whenever the boiler is operating, and the model assumes that this parasitic power does not contribute to heating the water. The minimum value for this field is 0.0, and the default value is also 0.0 if the field is left blank.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity and Design Water Flow Rate. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-An example of this statement in an IDF is:
-
-```idf
-  Boiler:HotWater,
-    Condensing Boiler,   !- Boiler Name
-    NaturalGas,          !- Fuel Type
-    25000,               !- Nominal Capacity {W}
-    EnteringBoiler       !- Efficiency Curve Temperature Evaluation Variable
-    0.89,                !- Nominal Thermal Efficiency
-    CondensingBoilerEff, !- Boiler Efficiency Curve Name
-    75,                  !- Design Boiler Water Outlet Temp {C}
-    0.0021,              !- Max Design Boiler Water Flow Rate {m3/s}
-    0.10,                !- Minimum Part Load Ratio
-    1.00,                !- Maximum Part Load Ratio
-    1.00,                !- Optimum Part Load Ratio
-    Boiler Inlet Node,   !- Boiler Water Inlet Node
-    Boiler Outlet Node,  !- Boiler Water Outlet Node
-    80,                  !- Temp Upper Limit Water Outlet {C}
-    ConstantFlow,        !- Boiler Flow Mode
-    25.0;                !- Parasitic Electric Load {W}
-
-
-  Curve:Biquadratic,
-    CondensingBoilerEff,     !- Name
-    1.124970374,             !- Coefficient1 Constant
-    0.014963852,             !- Coefficient2 x
-   -0.02599835,              !- Coefficient3 x**2
-    0.0,                     !-Coefficient4y
-   -1.40464E-6,              !-Coefficient5y**2
-   -0.00153624,              !- Coefficient6x*y
-    0.1,                     !- Minimum Value of x
-    1.0,                     !- Maximum Value of x
-    30.0,                    !- Minimum Value of y
-    85.0;                    !- Maximum Value of y
-```
-
-
-### Boiler:HotWater Outputs
-
-Outputs available from the boiler:
-
-* HVAC,Average,Boiler Heating Rate [W]
-
-* HVAC,Sum,Boiler Heating Energy [J]
-
-* Zone,Meter,Boilers:EnergyTransfer [J]
-
-* HVAC,Average,Boiler Inlet Temperature [C]
-
-* HVAC,Average,Boiler Outlet Temperature [C]
-
-* HVAC,Average,Boiler Mass Flow Rate [kg/s]
-
-* HVAC,Average,Boiler Parasitic Electric Power [W]
-
-* HVAC,Sum,Boiler Ancillary Electric Energy [J]
-
-* HVAC,Average,Boiler Part Load Ratio
-
-
-  One of the following blocks will be applicable based on fuel type:
-
-Electric:
-
-* HVAC,Average,Boiler Electric Power [W]
-
-* HVAC,Sum,Boiler Electric Energy [J]
-
-Gas:
-
-* HVAC,Average,Boiler Gas Rate [W]
-
-* HVAC,Sum,Boiler Gas Energy [J]
-
-Propane:
-
-* HVAC,Average,Boiler Propane Rate [W]
-
-* HVAC,Sum,Boiler Propane Energy [J]
-
-FuelOil\#1:
-
-* HVAC,Average,Boiler FuelOil\#1 Rate [W]
-
-* HVAC,Sum,Boiler FuelOil\#1 Energy [J]
-
-FuelOil\#2:
-
-* HVAC,Average,Boiler FuelOil\#2 Rate [W]
-
-* HVAC,Sum,Boiler FuelOil\#2 Energy [J]
-
-Coal:
-
-* HVAC,Average,Boiler Coal Rate [W]
-
-* HVAC,Sum,Boiler Coal Energy [J]
-
-Diesel:
-
-* HVAC,Average,Boiler Diesel Rate [W]
-
-* HVAC,Sum,Boiler Diesel Energy [J]
-
-Gasoline:
-
-* HVAC,Average,Boiler Gasoline Rate [W]
-
-* HVAC,Sum,Boiler Gasoline Energy [J]
-
-OtherFuel1:
-
-* HVAC,Average,Boiler OtherFuel1 Rate [W]
-
-* HVAC,Sum,Boiler OtherFuel1 Energy [J]
-
-OtherFuel2:
-
-* HVAC,Average,Boiler OtherFuel2 Rate [W]
-
-* HVAC,Sum,Boiler OtherFuel2 Energy [J]
-
-
-#### Boiler Heating Rate [W]
-
-#### Boiler Heating Energy [J]
-
-These outputs are the heating output (load) of the boiler. Energy is metered on Boilers:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Boiler Inlet Temperature [C]
-
-#### Boiler Outlet Temperature [C]
-
-#### Boiler Mass Flow Rate [kg/s]
-
-These outputs are the hot water inlet and outlet temperatures and flow rate for the boiler.
-
-#### Boiler Part Load Ratio []
-
-This output is the operating part-load ratio of the boiler. The part-load ratio is calculated as the boiler load divided by the boiler nominal capacity. The part-load ratio is limited by the minimum and maximum part-load ratio inputs specified by the user.
-
-#### Boiler &lt;Fuel Type&gt; Rate [W]
-
-#### Boiler &lt;Fuel Type&gt; Energy [J] \\
-
-#### Boiler Electric Power [W]
-
-These outputs are the energy input to the boiler. Valid fuel types are:  Electric, Gas (natural gas), Propane, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1, OtherFuel2. Consumption is metered on Heating:&lt;Fuel Type&gt;, &lt;Fuel Type&gt;:Plant, and &lt;Fuel Type&gt;:Facility.
-
-#### Boiler Ancillary Electric Power [W]
-
-#### Boiler Ancillary Electric Energy [J]
-
-These outputs are the parasitic electric power and parasitic electric consumption associated with the boiler. Used when simulating a forced draft fan or other electric component. Consumption is metered on Heating:Electricity and Electricity:Plant.
-
-### Boiler:Steam
-
-The steam boiler model provides a first order approximation of performance for fuel oil, gas and electric boilers. Boiler performance is based on a “theoretical� boiler efficiency (overall efficiency at design operating conditions) and a single quadratic fuel use/ part load ratio curve. This single curve accounts for all combustion inefficiencies and stack losses.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the Steam Boiler.
-
-#### Field: Fuel Type
-
-This alpha value specifies the type of fuel used by the boiler. The fuel type can be **Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1** or **OtherFuel2.**
-
-#### Field: Maximum Operating Pressure
-
-This numeric field contains the maximum value of pressure up to which the boiler would operate, or the maximum design pressure. (Pascal)
-
-#### Field: Theoretical Efficiency
-
-This numeric field contains the heating efficiency (as a fraction between 0 and 1) of the boiler’s burner
-
-#### Field: Design Outlet Steam Temperature
-
-The maximum value of steam temperature the boiler can provide. (Celcius)
-
-#### Field: Nominal Capacity
-
-This numeric field contains the nominal operating capacity (W) of the boiler.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the minimum part load ratio. If the ratio of demand to boiler nominal capacity is less than the minimum part load ratio, then the Min PLR will determine the operating PLR. The expected range is between 0 and 1.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the maximum part load ratio. If the ratio of demand to boiler nominal capacity is greater than the maximum part load ratio, then the Max PLR will determine the operating PLR. This value may exceed 1, but the normal range is between 0 and 1.1.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the optimum part load ratio. This is the part load ratio at which the boiler performs at its maximum efficiency.
-
-#### Field: Coefficient 1 of Fuel Use Function of Part Load Ratio Curve
-
-This numeric field contains the fuel use / PLR coefficient1.
-
-#### Field: Coefficient 2 of Fuel Use Function of Part Load Ratio Curve
-
-This numeric field contains the fuel use / PLR coefficient2.
-
-#### Field: Coefficient 3 of Fuel Use Function of Part Load Ratio Curve
-
-This numeric field contains the fuel use / PLR coefficient3.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the water inlet node name.
-
-#### Field: Steam Outlet Node Name
-
-This alpha field contains the steam outlet node name.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the inputs that would be altered by the sizing factor are: Nominal Capacity. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-More information on the technical aspects of steam boiler can be found in the Engineering Reference Document.
-
-An example of a Steam Boiler input statement from an IDF is:
-
-```idf
-Boiler:Steam,
-    Steam Boiler Plant Boiler,  !- Boiler Name
-    NaturalGas,                 !- Fuel Type
-    160000,                     !-Maximum Boiler Pressure Pascal
-    0.8,                        !- Theoretical Boiler Efficiency
-    115,                        !- Max Design Outlet Steam Temp
-    300000,                     !- Nominal Capacity W
-    0.00001,                    !- Minimum Part Load Ratio
-    1.0,                        !- Maximum Part Load Ratio
-    0.2,                        !- Optimum Part Load Ratio
-    0.8,!- Coefficient 1 of the fuel use/part load ratio curve
-    0.1,!- Coefficient 2 of the fuel use/part load ratio curve
-    0.1,!- Coefficient 3 of the fuel use/part load ratio curve
-    Steam Boiler Plant Boiler Inlet Node,  !- Boiler Steam Inlet Node
-    Steam Boiler Plant Boiler Outlet Node; !- Plant Loop Outlet Node
-
-
-Boiler:Steam,
-    Steam Boiler Plant Boiler,  !- Boiler Name
-    NaturalGas,                 !- Fuel Type
-    160000,                     !-Maximum Boiler Pressure Pascal
-    0.8,                        !- Theoretical Boiler Efficiency
-    115,                        !- Max Design Outlet Steam Temp
-    autosize,                  !- Nominal Capacity W
-    0.00001,                    !- Minimum Part Load Ratio
-    1.0,                        !- Maximum Part Load Ratio
-    0.2,                        !- Optimum Part Load Ratio
-    0.8,!- Coefficient 1 of the fuel use/part load ratio curve
-    0.1,!- Coefficient 2 of the fuel use/part load ratio curve
-    0.1,!- Coefficient 3 of the fuel use/part load ratio curve
-    Steam Boiler Plant Boiler Inlet Node,  !- Boiler Steam Inlet Node
-    Steam Boiler Plant Boiler Outlet Node; !- Plant Loop Outlet Node
-```
-
-
-### Steam Boiler Outputs
-
-Outputs available from the steam boiler:
-
-* HVAC,Average,Boiler Heating Rate [W]
-
-* HVAC,Sum,Boiler Heating Energy [J]
-
-* Zone,Meter,Boilers:EnergyTransfer [J]
-
-* HVAC,Average,Boiler Steam Inlet Temperature [C]
-
-* HVAC,Average,Boiler Steam Outlet Temperature [C]
-
-* HVAC,Average,Boiler Mass Flow Rate [kg/s]
-
-
-  One of the following blocks will be applicable based on fuel type:
-
-Electric:
-
-* HVAC,Average,Boiler Electric Power [W]
-
-* HVAC,Sum,Boiler Electric Energy [J]
-
-Gas:
-
-* HVAC,Average,Boiler Gas Rate [W]
-
-* HVAC,Sum,Boiler Gas Energy [J]
-
-Propane:
-
-* HVAC,Average,Boiler Propane Rate [W]
-
-* HVAC,Sum,Boiler Propane Energy [J]
-
-FuelOil\#1:
-
-* HVAC,Average,Boiler FuelOil\#1 Rate [W]
-
-* HVAC,Sum,Boiler FuelOil\#1 Energy [J]
-
-FuelOil\#2:
-
-* HVAC,Average,Boiler FuelOil\#2 Rate [W]
-
-* HVAC,Sum,Boiler FuelOil\#2 Energy [J]
-
-Coal:
-
-* HVAC,Average,Boiler Coal Rate [W]
-
-* HVAC,Sum,Boiler Coal Energy [J]
-
-Diesel:
-
-* HVAC,Average,Boiler Diesel Rate [W]
-
-* HVAC,Sum,Boiler Diesel Energy [J]
-
-Gasoline:
-
-* HVAC,Average,Boiler Gasoline Rate [W]
-
-* HVAC,Sum,Boiler Gasoline Energy [J]
-
-OtherFuel1:
-
-* HVAC,Average,Boiler OtherFuel1 Rate [W]
-
-* HVAC,Sum,Boiler OtherFuel1 Energy [J]
-
-OtherFuel2:
-
-* HVAC,Average,Boiler OtherFuel2 Rate [W]
-
-* HVAC,Sum,Boiler OtherFuel2 Energy [J]
-
-
-#### Boiler Heating Rate [W]
-
-#### Boiler Heating Energy [J]
-
-These outputs are the heating output (load) of the boiler. Energy is metered on Boilers:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Boiler Steam Inlet Temperature [C]
-
-#### Boiler Steam Outlet Temperature [C]
-
-#### Boiler Steam Mass Flow Rate [kg/s]
-
-These outputs are the steam inlet and outlet temperatures and steam flow rate for the boiler.
-
-#### Boiler &lt;Fuel Type&gt; Rate [W]
-
-#### Boiler &lt;Fuel Type&gt; Energy [J]
-
-#### Boiler Electric Power [W]
-
-#### Boiler Electric Energy [J]
-
-These outputs are the energy input to the boiler. Valid fuel types are:  Electric, Gas (natural gas), Propane, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1, and OtherFuel2. Consumption is metered on Heating:&lt;Fuel Type&gt;, &lt;Fuel Type&gt;:Plant, and &lt;Fuel Type&gt;:Facility.
-
-### Water to Water Heat Pumps
-
-The EnergyPlus has two water-to-water heat pump models, parameter estimation and equation fit, to choose from:
-
-**HeatPump:WaterToWater:EquationFit:Cooling**
-
-**HeatPump:WaterToWater:EquationFit:Heating**
-
-This model is an equation-fit model from the catalog data which resembles a black box with no usage of heat transfer equations. The performance of the heat pump is modeled using curves fitted from the catalog data.
-
-**HeatPump:WaterToWater:ParameterEstimation:Cooling**
-
-**HeatPump:WaterToWater:ParameterEstimation:Heating**
-
-This model is a parameter estimation based model that uses physical parameters generated from the catalog data. The physical parameters are then used to predict the performance of the heat pump using thermodynamic laws and heat transfer equations. The heat pump has a reciprocating compressor that serves both the hot water and the chilled water loop. Note that this model is currently “hardwired� to fluid property R22. FluidProperties:* objects for R-22 must be included in the idf file. These may be copied from DataSets\FluidPropertiesRefData.idf.
-
-Descriptions and strength of each respective model is available in the following references:
-
-Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from [http://www.hvac.okstate.edu/](http://www.hvac.okstate.edu))
-
-Tang,C. C. 2005. Modeling Packaged Heat Pumps in Quasi-Steady State Energy Simulation Program. M.S. Thesis. Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from [http://www.hvac.okstate.edu/](http://www.hvac.okstate.edu))
-
-The Supply side of the heat pump is usually connected to a Ground Heat Exchanger. The figure below shows the layout and piping diagram of the water-to-water heat pump.
-
-![](media/image184.svg)
-
-Figure 75. Schematic of EnergyPlus Ground Loop Heat Exchanger
-
-First, the equation fit model objects are described. This model has two sets of coefficients, one for the heating mode and other for the cooling mode.
-
-### HeatPump:WaterToWater:EquationFit:Cooling
-
-#### Field: Name
-
-This alpha field contains the identifying name for the ground source heat pump.
-
-#### Field: Source Side Inlet Node Name
-
-This alpha field contains the heat pump’s source side inlet node name.
-
-#### Field: Source Side Outlet Node Name
-
-This alpha field contains the heat pump’s source side outlet node name.
-
-#### Field: Load Side Inlet Node Name
-
-This alpha field contains the heat pump’s load side inlet node name.
-
-#### Field: Load Side Outlet Node Name
-
-This alpha field contains the heat pump’s load side outlet node name.
-
-#### Field: Rated Load Side Flow Rate
-
-This numeric field contains the rated volumetric flow rate on the load side of the heat pump in m3/s. This corresponds to the highest load side heat transfer rate listed in the catalog data.
-
-#### Field: Rated Source Side Flow Rate
-
-This numeric field contains the rated volumetric flow rate on the source side of the heat pump in m3/s. This corresponds to the highest load side heat transfer rate listed in the catalog data.
-
-#### Field: Rated Cooling Capacity
-
-This numeric field contains the rated cooling capacity of the heat pump in W. This corresponds to the highest load side heat transfer rate listed in the catalog data.
-
-#### Field: Rated Cooling Power Consumption
-
-Rated cooling power consumption, in W.
-
-#### Fields: Cooling Capacity Coefficients 1-5
-
-Five fields are used to describe the coefficients for the Cooling Capacity curve. More details on how these coefficients are used are described in the Engineering Reference.
-
-#### Field: Cooling Compressor Power Coefficients 1-5
-
-Five fields are used to decribe the coefficients for the Cooling Compressor Power curve.
-
-An idf example:
-
-```idf
-  HeatPump:WaterToWater:EquationFit:Cooling,
-    GshpCLG,                 !- Name
-    GshpCLG SourceSide Inlet Node,      !- Source Side Inlet Node Name
-    GshpCLG SourceSide Outlet Node,     !- Source Side Outlet Node Name
-    GshpCLG LoadSide Inlet Node,        !- Load Side Inlet Node Name
-    GshpCLG LoadSide Outlet Node,       !- Load Side Outlet Node Name
-    1.89E-03,                !- Rated Load Side Flow Rate {m3/s}
-    1.89E-03,                !- Rated Source Side Flow Rate {m3/s}
-    39890.91,                !- Rated Cooling Capacity {W}
-    4790.00,                 !- Rated Cooling Power Consumption {W}
-    -1.52030596,             !- Cooling Capacity Coefficient 1
-    3.46625667,              !- Cooling Capacity Coefficient 2
-    -1.32267797,             !- Cooling Capacity Coefficient 3
-    0.09395678,              !- Cooling Capacity Coefficient 4
-    0.038975504,             !- Cooling Capacity Coefficient 5
-    -8.59564386,             !- Cooling Compressor Power Coefficient 1
-    0.96265085,              !- Cooling Compressor Power Coefficient 2
-    8.69489229,              !- Cooling Compressor Power Coefficient 3
-    0.02501669,              !- Cooling Compressor Power Coefficient 4
-    -0.20132665;             !- Cooling Compressor Power Coefficient 5
-```
-
-
-### Water to Water Heat Pump Equation Fit Outputs
-
-This section describes the outputs available for the water to water heat pump, equation fit model; both cooling and heating.
-
-* HVAC,Sum,Water to Water Heat Pump Electric Energy [J]
-
-* HVAC,Sum,Water to Water Heat Pump Load Side Heat Transfer Energy [J]
-
-* HVAC,Sum,Water to Water Heat Pump Source Side Heat Transfer Energy [J]
-
-* HVAC,Average,Water to Water Heat Pump Electric Power [W]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Heat Transfer Rate [W]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Heat Transfer Rate [W]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Outlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Inlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Outlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Inlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Mass Flow Rate [kg/s]
-
-
-
-
-#### Water to Water Heat Pump Electric Energy [J]
-
-This output variable represents the cumulative energy used by the compressor. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
-
-#### Water to Water Heat Pump Load Side Heat Transfer Energy [J]
-
-This output variable represents the cumulative heat transfer across the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
-
-#### Water to Water Heat Pump Source Side Heat Transfer Energy [J]
-
-This output variable represents the cumulative heat transfer across the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
-
-#### Water to Water Heat Pump Electric Power [W]
-
-This output variable represents the compressor power required to run the heat pump. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Load Side Heat Transfer Rate [W]
-
-This output variable represents the heat transfer across the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Source Side Heat Transfer Rate [W]
-
-This output variable represents the heat transfer across the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Load Side Outlet Temperature [C]
-
-This output variable represents the average fluid temperature leaving the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Load Side Inlet Temperature [C]
-
-This output variable represents the average fluid temperature entering the load side coil.  The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Source Side Outlet Temperature [C]
-
-This output variable represents the average fluid temperature leaving the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Source Side Inlet Temperature [C]
-
-This output variable represents the average fluid temperature entering the source side coil.  The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Load Side Mass Flow Rate [kg/s]
-
-This output variable represents the average fluid flow rate through the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Source Side Mass Flow Rate [kg/s]
-
-This output variable represents the average fluid flow rate through the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-
-### HeatPump:WaterToWater:EquationFit:Heating
-
-#### Field: Name
-
-This alpha field contains the identifying name for the ground source heat pump.
-
-#### Field: Source Side Inlet Node Name
-
-This alpha field contains the heat pump’s source side inlet node name.
-
-#### Field: Source Side Outlet Node Name
-
-This alpha field contains the heat pump’s source side outlet node name.
-
-#### Field: Load Side Inlet Node Name
-
-This alpha field contains the heat pump’s load side inlet node name.
-
-#### Field: Load Side Outlet Node Name
-
-This alpha field contains the heat pump’s load side outlet node name.
-
-#### Field: Rated Load Side Flow Rate
-
-This numeric field contains the rated volumetric flow rate on the load side of the heat pump in m3/s. This corresponds to the highest load side heat transfer rate listed in the catalog data.
-
-#### Field: Rated Source Side Flow Rate
-
-This numeric field contains the rated volumetric flow rate on the source side of the heat pump in m3/s. This corresponds to the highest load side heat transfer rate listed in the catalog data.
-
-#### Field: Rated Heating Capacity
-
-This numeric field contains the rated heating capacity of the heat pump in W. This corresponds to the highest load side heat transfer rate listed in the catalog data.
-
-#### Field: Rated Heating Power Consumption
-
-Rated heating power consumption, in W.
-
-#### Fields: Heating Capacity Coefficients 1-5
-
-Five fields are used to describe the coefficients for the Heating Capacity curve. More details on how these coefficients are used are described in the Engineering Reference.
-
-#### Field: Heating Compressor Power Coefficients 1-5
-
-Five fields are used to describe the coefficients for the Heating Compressor Power curve.
-
-An idf example:
-
-
-
-```idf
-  HeatPump:WaterToWater:EquationFit:Heating,
-    GshpHeating,             !- Name
-    GshpHeating SourceSide Inlet Node,      !- Source Side Inlet Node Name
-    GshpHeating SourceSide Outlet Node,     !- Source Side Outlet Node Name
-    GshpHeating LoadSide Inlet Node,        !- Load Side Inlet Node Name
-    GshpHeating LoadSide Outlet Node,       !- Load Side Outlet Node Name
-    1.89E-03,                !- Rated Load Side Flow Rate {m3/s}
-    1.89E-03,                !- Rated Source Side Flow Rate {m3/s}
-    39040.92,                !- Rated Heating Capacity {W}
-    5130.00,                 !- Rated Heating Power Consumption {W}
-    -3.33491153,             !- Heating Capacity Coefficient 1
-    -0.51451946,             !- Heating Capacity Coefficient 2
-    4.51592706,              !- Heating Capacity Coefficient 3
-    0.01797107,              !- Heating Capacity Coefficient 4
-    0.155797661,             !- Heating Capacity Coefficient 5
-    -8.93121751,             !- Heating Compressor Power Coefficient 1
-    8.57035762,              !- Heating Compressor Power Coefficient 2
-    1.29660976,              !- Heating Compressor Power Coefficient 3
-    -0.21629222,             !- Heating Compressor Power Coefficient 4
-    0.033862378;             !- Heating Compressor Power Coefficient 5
-```
-
-
-Next, the parameter estimation model objects are described. This model has two sets of parameters, one for the heating mode and other for the cooling mode.
-
-### HeatPump:WaterToWater:ParameterEstimation:Cooling
-
-#### Field: Name
-
-This alpha field contains the identifying name for the ground source heat pump.
-
-#### Field: Source Side Inlet Node Name
-
-This alpha field contains the heat pump’s source side inlet node name.
-
-#### Field: Source Side Outlet Node Name
-
-This alpha field contains the heat pump’s source side outlet node name.
-
-#### Field: Load Side Inlet Node Name
-
-This alpha field contains the heat pump’s load side inlet node name.
-
-#### Field: Load Side Outlet Node Name
-
-This alpha field contains the heat pump’s load side outlet node name.
-
-#### Field: Nominal COP
-
-This numeric field contains the nominal coefficient of performance of the heat pump.
-
-#### Field: Nominal Capacity
-
-This numeric field contains the nominal capacity of the heat pump in Watts.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the minimum part load ratio of the heat pump usually set to 0.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the maximum part load ratio of the heat pump usually set to 1.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the optimal part load ratio of the heat pump usually set to 1.
-
-#### Field: Load Side Flow Rate
-
-This numeric field contains the volumetric flow rate on the load side of the heat pump in m3/s
-
-#### Field: Source Side Flow Rate
-
-This numeric field contains the volumetric flow rate on the source side of the heat pump in m3/s
-
-#### Field: Load Side Heat Transfer Coefficient
-
-This numeric field contains Estimated parameter load side heat transfer coefficient W/K.
-
-#### Field: Source Side Heat Transfer Coefficient
-
-This numeric field contains Estimated parameter source side heat transfer coefficient W/K.
-
-#### Field: Piston Displacement
-
-This numeric field contains the Estimated parameter displacement of the reciprocating compressor in m3/s.
-
-#### Field: Compressor Clearance Factor
-
-This numeric field contains the Estimated parameter clearance factor of the reciprocating compressor.
-
-#### Field: Compressor Suction and Discharge Pressure Drop
-
-This numeric field contains the estimated parameter the pressure drop at compressor suction and discharge in Pascals (N/m2).
-
-#### Field: Superheating
-
-This numeric field contains the estimated parameter superheat at the evaporator outlet in °C.
-
-#### Field: Constant Part of Electromechanical Power Losses
-
-This numeric field contains the estimated parameter power loss, which accounts for the loss of work due mechanical and electrical losses in the compressor in Watts.
-
-#### Field: Loss Factor
-
-This numeric field contains the factor of electromechanical loss that is proportional to the theoretical power percentage.
-
-#### Field: High Pressure Cut Off
-
-This numeric field contains the design pressure limit of the compressor in Pascals (N/m2).
-
-#### Field: Low Pressure Cut Off
-
-This numeric field contains the design low-pressure limit of the compressor in Pascals (N/m2).
-
-An idf example:
-
-```idf
-HeatPump:WaterToWater:ParameterEstimation:Cooling,
-    GshpCLG,                 !- Water to Water Heat Pump Name
-    GshpCLG SourceSide Inlet Node,  !- Source Side Inlet Node
-    GshpCLG SourceSide Outlet Node,  !- Source Side Outlet Node
-    GshpCLG LoadSide Inlet Node,  !- Load Side Inlet Node
-    GshpCLG LoadSide Outlet Node,  !- Load Side Outlet Node
-    3.5,                     !- Nominal COP
-    45000,                   !- Nominal Capacity {W}
-    0.0,                     !- Min PLR
-    1,                       !- Max PLR
-    1,                       !- optimum PLR
-    .003,                    !- Load side Flow Rate {m3/s}
-    .003,                    !- Source Side Flow Rate {m3/s}
-    7761,                    !- Load side Heat Transfer Coefficient {W/K}
-    3998,                    !- Source Side Heat Transfer Coefficient {W/K}
-    .012544,                 !- Piston Displacement {m3/s}
-    .05469,                  !- Compressor Clearance Factor %
-    92156.2,                 !- Compressor Suction And Discharge Pressure Drop {Pa}
-    4.8907,                  !- Superheating {C}
-    2803.9,                  !- Constant Part of Electro Mechanical Power Losses {W}
-    .699,                    !- Loss Factor
-    0.0,                     !- High Pressure Cut off {Pa}
-    0.0;                     !- LowPressure Cut off {Pa}
-```
-
-
-
-### HeatPump:WaterToWater:ParameterEstimation:Heating
-
-#### Field: Name
-
-This alpha field contains the identifying name for the ground source heat pump.
-
-#### Field: Source Side Inlet Node Name
-
-This alpha field contains the heat pump’s source side inlet node name.
-
-#### Field: Source Side Outlet Node Name
-
-This alpha field contains the heat pump’s source side outlet node name.
-
-#### Field: Load Side Inlet Node Name
-
-This alpha field contains the heat pump’s load side inlet node name.
-
-#### Field: Load Side Outlet Node Name
-
-This alpha field contains the heat pump’s load side outlet node name.
-
-#### Field: Nominal COP
-
-This numeric field contains the nominal coefficient of performance of the heat pump.
-
-#### Field: Nominal Capacity
-
-This numeric field contains the nominal capacity of the heat pump in Watts.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the minimum part load ratio of the heat pump usually set to 0.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the maximum part load ratio of the heat pump usually set to 1.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the optimal part load ratio of the heat pump usually set to 1.
-
-#### Field: Load Side Flow Rate
-
-This numeric field contains the volumetric flow rate on the load side of the heat pump in m3/s
-
-#### Field: Source Side Flow Rate
-
-This numeric field contains the volumetric flow rate on the source side of the heat pump in m3/s
-
-#### Field: Load Side Heat Transfer Coefficient
-
-This numeric field contains Estimated parameter load side heat transfer coefficient W/K.
-
-#### Field: Source Side Heat Transfer Coefficient
-
-This numeric field contains Estimated parameter source side heat transfer coefficient W/K.
-
-#### Field: Piston Displacement
-
-This numeric field contains the Estimated parameter displacement of the reciprocating compressor in m3/s.
-
-#### Field: Compressor Clearance Factor
-
-This numeric field contains the Estimated parameter clearance factor of the reciprocating compressor.
-
-#### Field: Compressor Suction and Discharge Pressure Drop
-
-This numeric field contains the estimated parameter the pressure drop at compressor suction and discharge in Pascals (N/m2).
-
-#### Field: Superheating
-
-This numeric field contains the estimated parameter superheat at the evaporator outlet in °C.
-
-#### Field: Constant Part of Electromechanical Power Losses
-
-This numeric field contains the estimated parameter power loss, which accounts for the loss of work due mechanical and electrical losses in the compressor in Watts.
-
-#### Field: Loss Factor
-
-This numeric field contains the factor of electromechanical loss that is proportional to the theoretical power percentage.
-
-#### Field: High Pressure Cut Off
-
-This numeric field contains the design pressure limit of the compressor in Pascals (N/m2).
-
-#### Field: Low Pressure Cut Off
-
-This numeric field contains the design low-pressure limit of the compressor in Pascals (N/m2).
-
-An idf example:
-
-```idf
-HeatPump:WaterToWater:ParameterEstimation:Heating,
-    GshpHeating,             !- Water to Water Heat Pump Name
-    GshpHeating SourceSide Inlet Node,  !- Source Side Inlet Node
-    GshpHeating SourceSide Outlet Node,  !- Source Side Outlet Node
-    GshpHeating LoadSide Inlet Node,  !- Load Side Inlet Node
-    GshpHeating LoadSide Outlet Node,  !- Load Side Outlet Node
-    3.5,                     !- Nominal COP
-    50000,                   !- Nominal Capacity {W}
-    0.0,                     !- Min PLR
-    1,                       !- Max PLR
-    1,                       !- optimum PLR
-    .003,                    !- Load side Flow Rate {m3/s}
-    .003,                    !- Source Side Flow Rate {m3/s}
-    7761,                    !- Load side Heat Transfer Coefficient {W/K}
-    3998,                    !- Source Side Heat Transfer Coefficient {W/K}
-    .012544,                 !- Piston Displacement {m3/s}
-    .05469,                  !- Compressor Clearance Factor %
-    92156.2,                 !- Compressor Suction And Dischrage Pressure Drop {Pa}
-    4.8907,                  !- Superheating {C}
-    2803.9,                  !- Constant Part Of Electro Mechanical Power Losses {W}
-    .699,                    !- Loss Factor
-    0.0,                     !- High Pressure Cut off {Pa}
-    0.0;                     !- LowPressure Cut off {Pa}
-```
-
-
-
-
-Since the heat pump is defined with two separate objects (one for heating, one for cooling), the connections to the condenser has to be done carefully. The example below shows the configuration for parameter estimation objects. The same specifications and configuration also applies to the equation fit model.
-
-#### Steps to specify the Ground Source Heat Pump
-
-For the heating mode:
-
-1. Specify a branch for the Heat pump in hot water loop .
-
-2. Include the branch name in the splitter and mixer branches.
-
-3. Add a branch in condenser loop and include its name in the respective splitter and mixer.
-
-**! in hot water loop**
-
-```idf
-BRANCH, Heating GshpHeating Branch,
-      ,
-      ,
-  HeatPump:WatertoWater:ParameterEstimatinon:Heating,
-  GshpHeating,
-  GshpHeating LoadSide Inlet Node,
-  GshpHeating LoadSide Outlet Node,
-  ACTIVE;
-```
-
-
-
-
-**!in condenser loop**
-
-```idf
-BRANCH, GshpHeating SourceSide Branch,
-      ,
-      ,
-  HeatPump:WatertoWater:ParameterEstimatinon:Heating,
-  GshpHeating,
-  GshpHeating SourceSide Inlet Node,
-  GshpHeating SourceSide Outlet Node,
-  ACTIVE;
-```
-
-
-Example of Heat Pump Links
-
-For the cooling mode:
-
-1. Specify a branch for the Heat pump in chilled water loop .
-
-2. Include the branch name in the splitter and mixer branches.
-
-3. Add a branch in condenser loop and include its name in the respective splitter and mixer.
-
-**! in chilled water loop**
-
-```idf
-BRANCH,GshpCLG1 Chiller Branch,
-  ,
-  ,
-  HeatPump:WatertoWater:ParameterEstimatinon:Cooling, GshpCLG1,
-  GshpCLG LoadSide Inlet Node1,
-  GshpCLG LoadSide Outlet Node1,
-  Active;
-```
-
-**!in condenser loop**
-
-```idf
-BRANCH, GshpCLG1 Condenser Branch,
-  ,
-  ,
-  HeatPump:WatertoWater:ParameterEstimatinon:Cooling, GshpCLG1,
-  GshpCLG SourceSide Inlet Node1,
-  GshpCLG SourceSide Outlet Node1,
-  ACTIVE;
-```
-
-
-### Water to Water Heat Pump Parameter Estimation Outputs
-
-This section describes the outputs available for the water to water heat pump, parameter estimation model; both cooling and heating.
-
-* HVAC,Average,Water to Water Heat Pump Electric Power [W]
-
-* HVAC,Average,Water to Water Heat Pump Electric Power [W]
-
-* HVAC,Sum,Water to Water Heat Pump Electric Energy [J]
-
-* HVAC,Sum,Water to Water Heat Pump Electric Energy [J]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Heat Transfer Rate [W]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Heat Transfer Rate [W]
-
-* HVAC,Sum,Water to Water Heat Pump Load Side Heat Transfer Energy [J]
-
-* HVAC,Sum,Water to Water Heat Pump Load Side Heat Transfer Energy [J]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Heat Transfer Rate [W]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Heat Transfer Rate [W]
-
-* HVAC,Sum,Water to Water Heat Pump Source Side Heat Transfer Energy [J]
-
-* HVAC,Sum,Water to Water Heat Pump Source Side Heat Transfer Energy [J]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Outlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Outlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Inlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Inlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Outlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Outlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Inlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Inlet Temperature [°C]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water to Water Heat Pump Load Side Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water to Water Heat Pump Source Side Mass Flow Rate [kg/s]
-
-#### Water to Water Heat Pump Electric Power [W]
-
-#### Water to Water Heat Pump Electric Power [W]
-
-This output variable represents the compressor power required to run the heat pump. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Electric Energy [J]
-
-#### Water to Water Heat Pump Electric Energy [J]
-
-This output variable represents the cumulative energy used by the compressor. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
-
-#### Water to Water Heat Pump Load Side Heat Transfer Rate [W]
-
-#### Water to Water Heat Pump Load Side Heat Transfer Rate [W]
-
-This output variable represents the heat transfer across the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Load Side Heat Transfer Energy [J]
-
-#### Water to Water Heat Pump Load Side Heat Transfer Energy [J]
-
-This output variable represents the cumulative heat transfer across the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
-
-#### Water to Water Heat Pump Source Side Heat Transfer Rate [W]
-
-#### Water to Water Heat Pump Source Side Heat Transfer Rate [W]
-
-This output variable represents the heat transfer across the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Source Side Heat Transfer Energy [J]
-
-#### Water to Water Heat Pump Source Side Heat Transfer Energy [J]
-
-This output variable represents the cumulative heat transfer across the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are summed across the reporting period.
-
-#### Water to Water Heat Pump Load Side Outlet Temperature [C]
-
-#### Water to Water Heat Pump Load Side Outlet Temperature [C]
-
-This output variable represents the average fluid temperature leaving the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Load Side Inlet Temperature [C]
-
-#### Water to Water Heat Pump Load Side Inlet Temperature [C]
-
-This output variable represents the average fluid temperature entering the load side coil.  The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Source Side Outlet Temperature [C]
-
-#### Water to Water Heat Pump Source Side Outlet Temperature °C]
-
-This output variable represents the average fluid temperature leaving the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Source Side Inlet Temperature [C]
-
-#### Water to Water Heat Pump Source Side Inlet Temperature [C]
-
-This output variable represents the average fluid temperature entering the source side coil.  The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Load Side Mass Flow Rate [kg/s]
-
-#### Water to Water Heat Pump Load Side Mass Flow Rate [kg/s]
-
-This output variable represents the average fluid flow rate through the load side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Water to Water Heat Pump Source Side Mass Flow Rate [kg/s]
-
-#### Water to Water Heat Pump Source Side Mass Flow Rate [kg/s]
-
-This output variable represents the average fluid flow rate through the source side coil. The values are calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-### DistrictCooling
-
-When the user is not interested in a plant simulation or there is some centralized source of chilled water, the following object can be used in the input.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the district cooling (i.e., purchased chilled water).
-
-#### Field: Chilled Water Inlet Node Name
-
-This alpha field contains the identifying name for the district cooling inlet node.
-
-#### Field: Chilled Water Outlet Node Name
-
-This alpha field contains the identifying name for the district cooling outlet node.
-
-#### Field: Nominal Capacity
-
-This numeric field contains the nominal demand (W) that the district cooling will meet. This field is autosizable.
-
-#### Field: Capacity Fraction Schedule Name
-
-This alpha field contains the name of a schedule that describes how the nominal capacity varies over time.  Values must non-negative. The capacity at a given point in time is determined by the product of the previous field and the value in this schedule. If the field is omitted or left blank, then the program assumes a schedule value of 1.0 all the time.
-
-An example of this statement in an IDF is:
-
-```idf
-DistrictCooling, Purchased Cooling,
-        NODE_35,NODE_49,
-        68000;
-```
-
-
-### DistrictCooling Outputs
-
-* HVAC,Average, District Cooling Chilled Water Rate [W]
-
-* HVAC,Sum, District Cooling Chilled Water Energy [J]
-
-* Zone,Meter, DistrictCooling:Plant [J]
-
-* Zone,Meter,Cooling: DistrictCooling [J]
-
-* HVAC,Average,District Cooling Rate [W]
-
-* HVAC,Average,District Cooling Inlet Temperature [C]
-
-* HVAC,Average,District Cooling Outlet Temperature [C]
-
-* HVAC,Average,District Cooling Mass Flow Rate [kg/s]
-
-
-#### District Cooling Chilled Water Rate [W]
-
-#### District Cooling Chilled Water Energy [J]
-
-These outputs are the energy taken from purchased chilled water. Consumption is metered on Cooling:DistrictCooling, DistrictCooling:Plant, and DistrictCooling:Facility.
-
-#### District Cooling Rate [W]
-
-This is the useful rate of cooling energy from purchased chilled water. For the current algorithm, this is the same as District Cooling Chilled Water Rate.
-
-#### District Cooling Inlet Temperature [C]
-
-#### District Cooling Outlet Temperature [C]
-
-#### District Cooling Mass Flow Rate [kg/s]
-
-These outputs are the supply-side plant loop chilled water inlet and outlet temperatures and mass flow rate.
-
-### DistrictHeating
-
-When the user is not interested in a plant simulation or there is some centralized source of hot water (district heating), the following object can be used in the input.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the district heating (i.e., purchased hot water).
-
-#### Field: Hot Water Inlet Node Name
-
-This alpha field contains the identifying name for the district heating inlet node.
-
-#### Field: Hot Water Outlet Node Name
-
-This alpha field contains the identifying name for the district heating outlet node.
-
-#### Field: Nominal Capacity
-
-This numeric field contains the nominal demand (W) that the district heating will meet. This field is autosizable.
-
-#### Field: Capacity Fraction Schedule Name
-
-This alpha field contains the name of a schedule that describes how the nominal capacity varies over time.  Values must non-negative. The capacity at a given point in time is determined by the product of the previous field and the value in this schedule. If the field is omitted or left blank, then the program assumes a schedule value of 1.0 all the time.
-
-An example of this statement in an IDF is:
-
-```idf
-DistrictHeating,Purchased Heating,
-        NODE_30,NODE_29,
-        1000000;
-```
-
-### DistrictHeating Outputs
-
-* HVAC,Average,District Heating Hot Water Rate [W]
-
-* HVAC,Sum,District Heating Hot Water Energy [J]
-
-* Zone,Meter,DistrictHeating:Plant [J]
-
-* Zone,Meter,Heating:DistrictHeating [J]
-
-* HVAC,Average,District Heating Rate [W]
-
-* HVAC,Average,District Heating Inlet Temperature [C]
-
-* HVAC,Average,District Heating Outlet Temperature [C]
-
-* HVAC,Average,District Heating Mass Flow Rate [kg/s]
-
-
-#### District Heating Hot Water Rate [W]
-
-#### District Heating Hot Water Energy [J]
-
-These outputs are the energy taken from purchased hot water. Consumption is metered on Heating:DistrictHeating, DistrictHeating:Plant, and DistrictHeating:Facility.
-
-#### District Heating Rate [W]
-
-This is the useful rate of heating energy from purchased hot water. For the current algorithm, this is the same as District Heating Hot Water Rate.
-
-#### District Heating Inlet Temperature [C]
-
-#### District Heating Outlet Temperature [C]
-
-#### District Heating Mass Flow Rate [kg/s]
-
-These outputs are the supply-side plant loop hot water inlet and outlet temperatures and mass flow rate.
-
-### PlantComponent:TemperatureSource
-
-This object allows the simulation of a water (or other fluid) source at a user-specified temperature.  This could include a river, well, or seawater source, or any other configuration where the fluid temperature being supplied by the component to the plant is known.  The temperature may be a constant or scheduled.  Of course, the scheduled value may also be overwritten via EMS in cases where the specified temperature should be calculated at run-time.
-
-#### Field: Name
-
-This field is the string identifier for this component.
-
-#### Field: Inlet Node
-
-This is the name of this component’s inlet node for the plant connection.
-
-#### Field: Outlet Node
-
-This is the name of this component’s outlet node for the plant connection. The source temperature is applied to this node when the component is active.
-
-#### Field: Design Volume Flow Rate
-
-This numeric field contains the design value for component volume flow rate in m<sup>3</sup>/s.  This field may be autosized.
-
-#### Field: Temperature Specification Type
-
-This string field specifies the behavior of the source temperature.  Two inputs are allowed: Constant or Scheduled.  For a constant condition, a single input value (the next field) is used as the returning temperature (component outlet temperature) throughout the entire simulation.  For a scheduled condition, the name of a schedule (the following field) is used to allow the temperature to vary throughout the simulation.  This schedule value may be actuated via EMS to allow further flexibility on temperature specification at run-time.
-
-#### Field: Source Temperature
-
-If the Temperature Specification Type field is Constant, then the value in this field is used as the source temperature (in C) throughout the entire simulation.
-
-#### Field: Source Temperature Schedule Name
-
-If the Temperature Specification Type field is Scheduled, then this is the name of a schedule entered in the IDF which specifies the dynamic temperature of this source object. The units of this schedule should be C.
-
-And, as shown in an IDF:
-
-```idf
-PlantComponent:TemperatureSource,
-    FluidSource,             !- Name
-    FluidSource Inlet Node,  !- Inlet Node
-    FluidSource Outlet Node, !- Outlet Node
-    Autosize,                !- Design Volume Flow Rate {m3/s}
-    Constant,                !- Temperature Specification Type
-    62,                      !- Source Temperature {C}
-    ;                        !- Source Temperature Schedule Name
-```
-
-
-### PlantComponent:TemperatureSource Outputs
-
-The following output variables are available for the temperature source plant components:
-
-* HVAC,Average,Plant Temperature Source Component Mass Flow Rate [kg/s]
-
-* HVAC,Average,Plant Temperature Source Component Inlet Temperature [C]
-
-* HVAC,Average,Plant Temperature Source Component Outlet Temperature [C]
-
-* HVAC,Average,Plant Temperature Source Component Source Temperature [C]
-
-* HVAC,Average,Plant Temperature Source Component Heat Transfer Rate [W]
-
-* HVAC,Sum,Plant Temperature Source Component Heat Transfer Energy [J]
-
-#### Plant Temperature Source Component Mass Flow Rate [kg/s]
-
-The current mass flow rate of this component.
-
-#### Plant Temperature Source Component Inlet Temperature [C]
-
-The current entering fluid temperature of this component.
-
-#### Plant Temperature Source Component Outlet Temperature [C]
-
-The current outlet temperature of this component.
-
-#### Plant Temperature Source Component Source Temperature [C]
-
-The current source temperature of this component.
-
-#### Plant Temperature Source Component Heat Transfer Rate [W]
-
-The current heat transfer rate of this component, positive for outlet temperature &gt; inlet temperature, or adding heat to the loop, or absorbing heat from the source.
-
-#### Plant Temperature Source Component Heat Transfer Energy [J]
-
-The current heat transfer energy over the given reporting period of this component.
-
-### CentralHeatPumpSystem
-
-This is a central geothermal application that contains one or more chiller-heaters centrally located in the building; the available chilled and/or hot water is then piped to the individual zones. Chiller-heaters used for this particular system can be of two types: 1) standard vapor-compression, non-reversible cycle chillers designed for heat recovery or 2) reversible-cycle, water-to-water heat pump chillers. Unlike a distributed ground source heat pump configuration where individual heat pumps are located in each zone, a centralized geothermal configuration has one or more chiller-heaters. Its function is to encapsulate the extra controls needed to turn individual chiller-heater modules on/off and whether they are to operate in cooling-only, heating-only or simultaneous cooling-heating mode and whether to connect the source water to the evaporator or condenser side. A variety of control schemes can be designed by setting schedules for both zone control types and individual chiller-heaters schedules.
-
-The fluid used in this central system is usually water, and there is no sharing of condenser or evaporator water between multiple machines. However, the control logic is such that the source water can be delivered to individual chiller-heaters depending on their operating mode, e.g., modules in simultaneous cooling-heating mode receive no source water, modules in heating-only mode can have source water directed to their evaporator, or modules in cooling-only mode can have source water directed to their condenser; the decision on which module(s) receives the source water dictated by the ‘smart’ controls. The following figures illustrate node interconnections between this central geothermal application and plant and condenser loops in various situations.
-
-The order of the multiple chiller-heaters’ operation is assumed to be sequential. In other words, the very first chiller-heater will be called at first to see if it meets all loads that the central heat pump system should meet. If the chiller-heater meets all loads, the rest chiller-heaters are assumed to be turned off. If not, the following chiller-heater will be called to meet the remaining loads until all loads are met in the order as defined in the set of individual chiller-heater objects below. The order of individual chiller-heater modules needs to be carefully arranged in case users are intended to see the performance of various combinations of different sizes of chiller-heaters in a central heat pump system.
-
-
-
-![](media/image185.png)
-
-Figure 76. Diagram of a central heat pump system with three chiller-heaters in cooling-only mode (Condensers reject heat to the ground source loop)
-
-
-
-![](media/image186.png)
-
-Figure 77. Diagram of a central heat pump system with three chiller-heaters in heat recovery mode         (No heat is exchanged with the ground source loop)
-
-
-
-![](media/image187.png)
-
-Figure 78. Diagram of a central heat pump system with one chiller-heater in heat recovery mode and two chiller-heaters in cooling-only mode
-
-In the above example, the cooling load needs 3 chiller-heaters and the heating load needs 1 chiller heater. Chiller 1 is in heat recovery mode and isolated from the ground source loop while chillers 2 and 3 are in cooling-only mode, their condensers rejecting heat to the ground source loop.
-
-
-
-![](media/image188.png)
-
-Figure 79. Diagram of a central heat pump system with two chiller-heaters in heat recovery mode and one chiller-heater in heating-only mode
-
-In the above example, the heating load needs 3 chiller-heaters and the cooling load needs two chiller-heaters. Chillers 1 and 2 are in heat recovery mode and isolated from the ground source loop while chiller 3 is in heating-only mode, its evaporator extracting heat from the ground source loop.
-
-Users are required to define three different nodes such as chilled water, hot water, and source water nodes. Only this central heat pump system will be metered, and individual chiller-heaters’ energy will be available for reporting only, but not metered.
-
-#### Field: Name
-
-This alpha field contains the identifying name of the central heat pump system.
-
-#### Field: Control Method
-
-#### This field must contain a keyword defines how the central heat pump system controls the interaction between the chiller-heater modules and the water loops to meet the cooling and heating demands. Currently, the only available option isSmartMixing.
-
-#### Field: Cooling Loop Inlet Node Name
-
-This alpha field contains the identifying name of the chilled water inlet node.
-
-#### Field: Cooling Loop Outlet Node Name
-
-This alpha field contains the identifying name of the chilled water outlet node.
-
-#### Field: Source Loop Inlet Node Name
-
-This alpha field contains the identifying name of the source water inlet node.
-
-#### Field: Source Loop Outlet Node Name
-
-This alpha field contains the identifying name of the source water outlet node.
-
-#### Field: Heating Loop Inlet Node Name
-
-This alpha field contains the identifying name of the hot water inlet node.
-
-#### Field: Heating Loop Outlet Node Name
-
-This alpha field contains the identifying name of the hot water outlet node.
-
-#### Field: Ancillary Power
-
-This numeric field contains the ancillary power of the central heat pump system in watts.
-
-#### Field: Ancillary Operation Schedule Name
-
-This alpha field contains the identifying name of the ancillary power schedule.
-
-#### Field Set: Individual Chiller-Heater Module Objects
-
-The following four items are repeated up to a maximum of 20 individual chiller-heater modulesets. At least one module set must appear in an input file. In other words, a central heat pump system must include at least one chiller-heater module component. A set of the following four fields helps to define the specific type of a chiller-heater module, its operation control, and the number of identical chiller-heater module objects.
-
-#### Field: Chiller Heater Module Performance Component Object Type &lt;x&gt;
-
-This alpha field describes the type of the chiller-heater comprising this module set. Only the chiller-heater type ChillerHeaterPerformance:EIectric:EIR is currently available. Note that up to 20 sets of chiller-heater module name, schedule, and number of identical chiller-heater may be entered for a single central heat pump system.
-
-#### Field: Chiller Heater Module Performance Component Name &lt;x&gt;
-
-This alpha field is paired with the preceding chiller-heater module type to define the name of the module.
-
-#### Field: Chiller Heater Module Control Schedule Name &lt;x&gt;
-
-This alpha field is paired with the preceding chiller-heater module type and name to define its on/off control. This schedule will be used for all identical module components as defined in the next field. Currently, this schedule only controls the module set’s availability, i.e., schedule values equal to 1 indicate that the chiller-heater set is available while schedule values equal to 0 indicate that the chiller-heater set is off.
-
-#### Field: Number of Chiller Heater Modules &lt;x&gt;
-
-This numeric field is paired with the preceding three fields to define how many identical chiller-heaters define this module set.
-
-An example of this statement in an IDF is:
-
-```idf
-CentralHeatPumpSystem,
-  ChillerBank,             !- Name
-  SmartMixing,             !- Control Method
-  Chiller Inlet Node,      !- Cooling Loop Inlet Node Name
-  Chiller Outlet Node,     !- Cooling Loop Outlet Node Name
-  Condenser Inlet Node,    !- Source Loop Inlet Node Name
-  Condenser Outlet Node,   !- Source Loop Outlet Node Name
-  HWInlet,                 !- Heating Loop Inlet Node Name
-  HWOutlet,                !- Heating Loop Outlet Node Name
-  460,                     !- Ancillary Power {W}
-  ,                        !- Ancillary Operation Schedule Name
-  ChillerHeaterPerformance:Electric:EIR,  !- Chiller Heater Modules Object Type 1
-  ChillerHeaterModule 1,   !- Chiller Heater Modules Performance Component Name 1
-  ON,                      !- Chiller Heater Modules Control Schedule Name 1
-  2,                       !- Number of Chiller Heater Modules 1
-  ChillerHeaterPerformance:Electric:EIR,  !- Chiller Heater Modules Object Type 2
-  ChillerHeaterModule 2,   !- Chiller Heater Modules Performance Component Name 2
-  ON,                      !- Chiller Heater Modules Control Schedule Name 2
-  2;                       !- Number of Chiller Heater Modules 2
-```
-
-
-
-
-### Central Heat Pump System Outputs
-
-* HVAC,Average,Chiller Heater System Cooling Electric Power [W]
-
-* HVAC,Sum,Chiller Heater System Cooling Electric Energy[J]
-
-* HVAC,Average,Chiller Heater System Heating Electric Power [W]
-
-* HVAC,Sum,Chiller Heater System Heating Electric Energy[J]
-
-* HVAC,Average,Chiller Heater System Cooling Rate [W]
-
-* HVAC,Sum,Chiller Heater System Cooling Energy[J]
-
-* HVAC,Average,Chiller Heater System Heating Rate [W]
-
-* HVAC,Sum,Chiller Heater System Heating Energy[J]
-
-* HVAC,Average,Chiller Heater System Source Heat Transfer Rate [W]
-
-* HVAC,Sum,Chiller Heater System Source Heat Transfer Energy[J]
-
-* HVAC,Average,Chiller Heater System Cooling Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heater System Cooling Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heater System Cooling Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Heater System Heating Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heater System Heating Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heater System Heating Mass Flow Rate [kg/s]
-
-* HVAC,Average,Chiller Heater System Source Inlet Temperature [C]
-
-* HVAC,Average,Chiller Heater System Source Outlet Temperature [C]
-
-* HVAC,Average,Chiller Heater System Source Mass Flow Rate [kg/s]
-
-
-#### Chiller Heater System Cooling Electric Power [W]
-
-#### Chiller Heater System Cooling Electric Energy [J]
-
-These outputs are the sums of the cooling electric power consumption of the central heat pump system containing one or more child objects. Cooling Energy is metered on Cooling:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Chiller Heater System Heating Electric Power [W]
-
-#### Chiller Heater System Heating Electric Energy [J]
-
-These outputs are the sums of the heating electric power consumption of the central heat pump system. Heating Energy is metered on Heating:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Chiller Heater System Cooling Rate [W]
-
-#### Chiller Heater System Cooling Energy [J]
-
-These outputs are the evaporator heat transfer which is the cooling delivered by the central heat pump system. These are the sums of the evaporator heat transfer of individual chiller-heater modules included in the central heat pump system. Cooling Energy is metered on Chiller:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Chiller Heater System Heating Rate [W]
-
-#### Chiller Heater System Heating Energy [J]
-
-These outputs are the condenser heat transfer which is the heating delivered by the central heat pump system. These are the sums of the condenser heat transfer of individual chiller-heater modules included in the central heat pump system. Heating Energy is metered on Boiler:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Chiller Heater System Source Heat Transfer Rate [W]
-
-#### Chiller Heater System Source Heat Transfer Energy [J]
-
-These outputs are heat transfer which is the heat rejected to a ground source loop or extracted from the source loop, depending on the operating modes of the chiller-heater modules. This is the sums of evaporator heat transfer of the chiller-heater modules in heating-only mode or heating dominant simultaneous cooling-heating mode while the sums of condenser heat transfer of the chiller-heater modules in cooling-only mode or cooling dominant simultaneous cooling-heating mode. Source Heat Transfer Energy is metered on HeatRejection:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Chiller Heater System Cooling Inlet Temperature [C]
-
-#### Chiller Heater System Cooling Outlet Temperature [C]
-
-#### Chiller Heater System Cooling Mass Flow Rate [kg/s]
-
-These outputs are the chilled water inlet and outlet temperatures and flow rate.
-
-#### Chiller Heater System Heating Inlet Temperature [C]
-
-#### Chiller Heater System Heating Outlet Temperature [C]
-
-#### Chiller Heater System Heating Mass Flow Rate [kg/s]
-
-These outputs are the hot water inlet and outlet temperatures and flow rate.
-
-#### Chiller Heater System Source Inlet Temperature [C]
-
-#### Chiller Heater System Source Outlet Temperature [C]
-
-#### Chiller Heater System Source Mass Flow Rate [kg/s]
-
-These outputs are the source water inlet and outlet temperatures and flow rate.
-
-### ChillerHeaterPerformance:EIectric:EIR
-
-The performance of the chiller-heater will be defined by two sets of curves meant to describe unloading for: 1) cooling-only mode, and 2) heating-only mode or simultaneous cooling-heating mode. Reference conditions must be defined for both because each has its own set of three unloading curves based on their associated reference conditions. The cooling-mode curves are typically (but not always) based on condenser entering water temperature while the heating-only mode curves are typically based on condenser leaving water temperature. This chiller-heater object allows the user to specify whether to use condenser leaving or condenser entering as a dependent variable to differentiate, if necessary, the condenser temperature basis used to generate the cooling- and heating-only mode curves.
-
-#### Field: Name
-
-This alpha field contains the identifying name of the chiller-heater to be included in a central heat pump system.
-
-#### Field: Reference Cooling Mode Evaporator Capacity
-
-This numeric field contains the reference cooling capacity of the evaporator in cooling mode in Watts. This value should be based on the reference temperatures and design water flow rates defined below. This field can be autosized.
-
-#### Field: Reference Cooling Mode COP
-
-This numeric field contains the reference coefficient of performance of the evaporator for cooling. It must be based on the values of Reference Cooling Mode Leaving Chilled Water Temperature and Reference Cooling Mode Entering Condenser Water Temperature defined in the next two fields.
-
-#### Field: Reference Cooling Mode Leaving Chilled Water Temperature
-
-This numeric field contains the reference leaving chilled water temperature of the evaporator for cooling in Celsius. The default value is 6.67°C.
-
-#### Field: Reference Cooling Mode Entering Condenser Water Temperature
-
-This numeric field contains the reference entering condenser water temperature of the condenser in the cooling mode in Celsius. The default value is 29.4°C.
-
-#### Field: Reference Cooling Mode Leaving Condenser Water Temperature
-
-This numeric field contains the reference leaving condenser water temperature of the condenser in the cooling mode in Celsius. The default value is 35.0°C.
-
-#### Field: Reference Heating Mode Cooling Capacity Ratio
-
-This numeric field contains the evaporator’s capacity during the reference heating-only or simultaneous cooling-heating mode as a ratio of reference cooling capacity. For example, the ratio may be expressed as follows:
-
-<div>\[Ratio = \frac{{EvapCapHt{g_{@Tchw,l = 6.67C,Tcond,l = 51.67C}}}}{{EvapCapC{{\lg }_{@Tchw,l = 6.67C,Tcond,l = 35.0C}}}}\]</div>
-
-where Tchw,l is the leaving chilled water temperature and Tcond,l is the leaving condenser water temperature representing the heating-mode and cooling-mode reference temperatures defined elsewhere in this object.
-
-The default is 0.75. This field is used to determine evaporator capacity in heating-only mode or simultaneous cooling-heating mode, multiplying it by the value entered in the field of the Reference Cooling Mode Evaporator Capacity. Note that even when there is no cooling load, i.e., the machine is in heating-only mode, the evaporator must still run and extract heat from the source water. In heating-only mode, the leaving chilled water temperature (Tchw,l) may  float depending on the evaporator water flow rate and the source water temperature. In simultaneous cooling and heating mode, the leaving chilled water temperature (Tchw,l) does not float but is determined by the chilled water setpoint controls. For both heating-only and simultaneous cooling and heating mode, the leaving condenser temperature (Tcond,l) is determined by the hot water supply setpoint controls. This value of Tchw,l, combined with Tcond,l is plugged into the CAPFT and EIRFT curves to determine the off-rated heating-mode evaporator capacity and associated compressor power.
-
-#### Field: Reference Heating Mode Cooling Power Ratio
-
-This numeric field contains the compressor power during simultaneous cooling-heating mode as a ratio of reference cooling compressor power. For example, the ratio may be expressed as follows:
-
-<div>\[Ratio = \frac{{Powe{r_{@Tchw,l = 6.67C,Tcond,l = 51.67C}}}}{{Powe{r_{@Tchw,l = 6.67C,Tcond,l = 35.0C}}}}\]</div>
-
-The default value is 1.5. This field is used to determine full load compressor power at the simultaneous cooling-heating mode’s reference chilled water leaving and condenser water leaving temperatures. Note: In heating-only mode, the chilled water leaving temperature floats so the EIRFT curve is used to modify the simultaneouos cooling-heating full load compressor power value.
-
-#### Field: Reference Heating Mode Leaving Chilled Water Temperature
-
-This numeric field contains the reference leaving chilled water temperature of the evaporator in simultaneous cooling-heating mode in Celsius. This is typically the same as the reference cooling mode value and is used to create the heating-only mode and simultaneous cooling-heating mode unloading curves. The leaving chilled water temperature for the chiller-heater is not allowed to fall below this value during the heating-only mode and simultaneous cooling-heating mode. The default value is 6.67°C.
-
-#### Field: Reference Heating Mode Leaving Condenser Water Temperature
-
-This numeric field contains the reference leaving condenser water temperature of the condenser in heating mode in Celsius. This field is typically controlled to the design hot water supply temperature, and used to create the heating-only mode and simultaneous cooling-heating mode unloading curves. The default value is 60.0°C.
-
-#### Field: Reference Heating Mode Entering Condenser Water Temperature
-
-This numeric field contains the reference entering condenser water temperature of the condenser in heating mode in Celsius. This field typically represents the upper limit of the source water temperature. The default value is 29.44°C.
-
-#### Field: Heating Mode Entering Chilled Water Temperature Low Limit
-
-This numeric field contains the low limit of the entering chilled water temperature in heating-only mode or simultaneous cooling-heating mode in Celsius. This field typically represents the lower limit of the source water temperature. If necessary, auxiliary heat will be activated to prevent source water temperature falling below the chilled water entering minimum. The default value is 12.2°C.
-
-#### Field: Chilled Water Flow Mode Type
-
-This alpha field contains the chilled water flow control mode. Valid water flow mode includes constant flow and variable flow, and the default water flow mode is constant flow.
-
-#### Field: Design Chilled Water Flow Rate
-
-This numeric field contains the design chilled water flow rate in m<sup>3</sup>/s. The minimum value for this field must be greater than zero, and this field is autosizable.
-
-#### Field: Design Condenser Water Flow Rate
-
-This numeric field contains the design condenser water flow rate in m<sup>3</sup>/s. The minimum value for this field must be greater than zero, and this field is autosizable.
-
-#### Field: Design Hot Water Flow Rate
-
-This numeric field contains the design hot water flow rate in m<sup>3</sup>/s. The minimum value and default value for this field are zero, and this field is autosizable.
-
-#### Field: Compressor Motor Efficiency
-
-This numeric field contains the fraction of efficiency of the compressor electrical energy consumption that must be rejected by the condenser. This value must be between 0.0 and 1.0, and the default value is 1.0.
-
-#### Field: Condenser Type
-
-This alpha field contains the type of condenser. WaterCooled is the only valid type, and it requires the full specification of the condenser loop and its associated equipment.
-
-#### Field: Cooling Mode Temperature Curve Condenser Water Independent Variable
-
-This alpha field determines whether the entering or leaving condenser water temperature is used in the cooling mode unloading performance curves that follow. Valid variables include EnteringCondenser and LeavingCondenser, and the default variable is EnteringCondenser. The condenser temperature used for the cooling mode unloading performance curves will be dependent on this field input. For example, leaving condenser water temperature will be used when the LeavingCondenser is chosen, otherwise entering condenser water temperature.
-
-#### Field: Cooling Mode Cooling Capacity Function of Temperature Curve Name
-
-This alpha field contains the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the evaporator capacity as a function of the leaving chilled water temperature and either the entering condenser water temperature or the leaving condenser water temperature as defined in the previous field. It is then multiplied by the reference evaporator capacity to give the cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-#### Field: Cooling Mode Electric Input to Cooling Output Ratio Function of Temperature Curve Name
-
-This alpha field contains the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and either the entering condenser water temperature or the leaving condenser water temperature as defined by the user. The EIR is the inverse of the COP. It is then multiplied by the reference EIR (inverse of the reference COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-#### Field: Cooling Mode Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-
-This alpha field contains the name of a performance curve (ref: Performance Curves) that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the part-load ratio (EIRFPLR). The EIR is the inverse of the COP, and the part-load ratio is the actual cooling load divided by the available cooling capacity of the chiller-heater. This curve is generated by dividing the operating electric input power by the available full-load capacity at the specific operating temperatures. The curve output should decrease from 1 towards 0 as part-load ratio decreases from 1 to 0. Note that the bi-cubic formulation is generally only valid when LeavingCondenser variable is chosen for the field of Cooling Mode Condenser Water Temperature Curve Input Variable whereas the quadratic curve can be used both choices, i.e., LeavingCondenser and EnteringCondenser. The output of this curve is then multiplied by the reference full-load EIR and the EIRFT to give the EIR at the specific temperatures and part-load ratio at which the chiller-heater is operating. This curve should have a value of 1.0 when the part-load ratio equals 1.0. The curve should be valid for the range of part-load ratios anticipated for the simulation.
-
-#### Field: Cooling Mode Cooling Capacity Optimum Part Load Ratio
-
-This numeric field contains the chiller-heater’s optimum part-load ratio. This is the part-load ratio at which the chiller-heater performs at its maximum COP. The optimum part-load ratio must be greater than or equal to the minimum part-load ratio, and less than or equal to the maximum part-load ratio. (Note: Both the minimum part-load ratio and maximum part-load ratio are taken from the Cooling Mode EIRFPLR curve definition.) The default value is 1.0.
-
-#### Field: Heating Mode Temperature Curve Condenser Water Independent Variable
-
-This alpha field determines whether the entering or leaving condenser water temperature is used in the heating mode unloading performance curves that follow. Valid variables include EnteringCondenser and LeavingCondenser, and the default variable is EnteringCondenser. The condenser temperature used for the cooling mode unloading performance curves will be dependent on this field input. For example, leaving condenser water temperature will be used when the LeavingCondenser is chosen, otherwise entering condenser water temperature.
-
-#### Field: Heating Mode Cooling Capacity Function of Temperature Curve Name
-
-This alpha field contains the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the evaporator capacity in heating mode as a function of the leaving chilled water temperature and either the entering condenser water temperature or the leaving condenser water temperature as defined in the previous field. This curve is used to evaluate the adjusted evaporator capacity during heating-only mode or simultaneous cooling-heating mode. This adjusted capacity is used as part of the cooling part-load calculation for the EIRFPLR curve. It is then multiplied by the reference evaporator capacity to give the cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-#### Field: Heating Mode Electric Input to Cooling Output Ratio Function of Temperature Curve Name
-
-This alpha field contains the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the leaving chilled water temperature and either the entering condenser water temperature or the leaving condenser water temperature as defined by the user. The EIR is the inverse of the COP. It is then multiplied by the reference EIR (inverse of the reference COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the reference temperatures). The curve should have a value of 1.0 at the reference temperatures and flow rates specified above. The biquadratic curve should be valid for the range of water temperatures anticipated for the simulation.
-
-#### Field: Heating Mode Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve Name
-
-This alpha field contains the name of a performance curve (ref: Performance Curves) that parameterizes the variation of the energy input to cooling output ratio (EIR) as a function of the part-load ratio (EIRFPLR). The EIR is the inverse of the COP, and the part-load ratio is the actual evaporator load divided by the available evaporator capacity of the chiller-heater at the reference heating and simultaneous cooling-heating mode temperatures. This curve is generated by dividing the operating electric input power by the available full-load capacity (do not divide by load) at the specific operating temperatures. The curve output should decrease from 1 towards 0 as part-load ratio decreases from 1 to 0. Note that the bicubic formulation below can only be used when the chiller-heater uses a variable speed compressor motor drive. It is also generally valid only when LeavingCondenser variable is chosen for the field of Cooling Mode Condenser Water Temperature Curve Input Variable whereas the quadratic curve can be used both choices, i.e., LeavingCondenser and EnteringCondenser. The output of this curve is then multiplied by the reference full-load EIR (inverse of the reference COP) and the EIRFT to give the EIR at the specific temperatures and part-load ratio at which the chiller-heater is operating. This curve should have a value of 1.0 when the part-load ratio equals 1.0. The curve should be valid for the range of part-load ratios anticipated for the simulation.
-
-#### Field: Heating Mode Cooling Capacity Optimum Part Load Ratio
-
-This numeric field contains the chiller-heater’s optimum part-load ratio during heating-only mode or simultaneous cooling-heating mode. This is the part-load ratio at which the chiller-heater performs at its maximum COP. The optimum part-load ratio must be greater than or equal to the minimum part-load ratio, and less than or equal to the maximum part-load ratio. (Note: Both the minimum part-load ratio and maximum part-load ratio are taken from the Heating Mode EIRFPLR curve definition.) The default value is 1.0.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The Sizing Factor is a multiplier on the design plant chilled water loop flow rate associated with the chiller-heaters parent CentralHeatPumpSystem object. The chiller-heater's modified chilled water flow can then be used to autocalculate the Design Condenser Water Flow Rate and Reference Cooling Mode Evaporator Capacity values. In general, it is best to autosize all three fields or set fixed values for all three fields.
-
-
-
-An example of this statement in an IDF is:
-
-```idf
-ChillerHeaterPerformance:Electric:EIR,
-  ChillerHeaterModule 1,   !- Name
-  12500,                   !- Reference Cooling Mode Evaporator Capacity {W}
-  1.5,                     !- Reference Cooling Mode COP {W/W}
-  6.67,                    !- Reference Cooling Mode Leaving Chilled Water Temperature {C}
-  29.4,                    !- Reference Cooling Mode Entering Condenser Fluid Temperature {C}
-  35.0,                    !- Reference Cooling Mode Leaving Condenser Water Temperature {C}
-  0.74,                    !- Reference Heating Mode Cooling Capacity Ratio
-  1.38,                    !- Reference Heating Mode Cooling Power Input Ratio
-  6.67,                    !- Reference Heating Mode Leaving Chilled Water Temperature {C}
-  60,                      !- Reference Heating Mode Leaving Condenser Water Temperature {C}
-  29.44,                   !- Reference Heating Mode Entering Condenser Fluid Temperature {C}
-  5,                       !- Heating Mode Entering Chilled Water Temperature Low Limit {C}
-  VariableFlow,            !- Chilled Water Flow Mode Type
-  0.0003525,               !- Design Chilled Water Flow Rate {m<sup>3</sup>/s}
-  0.0005525,               !- Design Condenser Water Flow Rate {m<sup>3</sup>/s}
-  0.0003525,               !- Design Hot Water Flow Rate {m<sup>3</sup>/s}
-  1,                       !- Compressor Motor Efficiency
-  WaterCooled,             !- Condenser Type
-  EnteringCondenser,       !- Cooling Mode Temperature Curve Condenser Water Independent Variable
-  ChillerHeaterClgCapFT,   !- Cooling Mode Cooling Capacity Function of Temperature Curve Name
-  ChillerHeaterClgEIRFT,   !- Cooling Mode Electric Input to Cooling Output Ratio Function of
-                              !-   Temperature Curve Name
-  ChillerHeaterClgEIRFPLR, !- Cooling Mode Electric Input to Cooling Output Ratio Function of Part Load
-                       !-   Ratio Curve Name
-  1,                       !- Cooling Mode Cooling Capacity Optimum Part Load Ratio
-  LeavingCondenser,        !- Heating Mode Temperature Curve Condenser Water Independent Variable
-  ChillerHeaterHtgCapFT,   !- Heating Mode Cooling Capacity Function of Temperature Curve Name
-  ChillerHeaterHtgEIRFT,   !- Heating Mode Electric Input to Cooling Output Ratio Function of
-                             !-   Temperature Curve Name
-  ChillerHeaterHtgEIRFPLR, !- Heating Mode Electric Input to Cooling Output Ratio Function of Part Load
-                             !-   Ratio Curve Name
-  1,                       !- Heating Mode Cooling Capacity Optimum Part Load Ratio
-  1;                       !- Sizing Factor
-```
-
-
-### ChillerHeaterPerformance:Electric:EIR Outputs
-
-* HVAC,Average,Chiller Heater Operation Mode Unit &lt;x&gt; []
-
-* HVAC,Average,Chiller Heater Part Load Ratio Unit &lt;x&gt; []
-
-* HVAC,Average,Chiller Heater Cycling Ratio Unit &lt;x&gt; []
-
-* HVAC,Average,Chiller Heater Cooling Electric Power Unit &lt;x&gt; [W]
-
-* HVAC,Sum,Chiller Heater Cooling Electric Energy Unit &lt;x&gt; [J]
-
-* HVAC,Average,Chiller Heater Heating Electric Power Unit &lt;x&gt; [W]
-
-* HVAC,Sum,Chiller Heater Heating Electric Energy Unit &lt;x&gt; [J]
-
-* HVAC,Average,Chiller Heater Cooling Rate Unit &lt;x&gt; [W]
-
-* HVAC,Sum,Chiller Heater Cooling Energy Unit &lt;x&gt; [J]
-
-* HVAC,Average,Chiller Heater False Load Heat Transfer Rate Unit &lt;x&gt; [W]
-
-* HVAC,Sum,Chiller Heater False Load Heat Transfer Energy Unit &lt;x&gt; [J]
-
-* HVAC,Average,Chiller Heater Condenser Heat Transfer Rate Unit &lt;x&gt; [W]
-
-* HVAC,Sum,Chiller Heater Condenser Heat Transfer Energy Unit &lt;x&gt; [J]
-
-* HVAC,Average,Chiller Heater Evaporator Inlet Temperature Unit &lt;x&gt; [C]
-
-* HVAC,Average,Chiller Heater Evaporator Outlet Temperature Unit &lt;x&gt; [C]
-
-* HVAC,Average,Chiller Heater Evaporator Mass Flow Rate Unit &lt;x&gt; [kg/s]
-
-* HVAC,Average,Chiller Heater Condenser Inlet Temperature Unit &lt;x&gt; [C]
-
-* HVAC,Average,Chiller Heater Condenser Outlet Temperature Unit &lt;x&gt; [C]
-
-* HVAC,Average,Chiller Heater Condenser Mass Flow Rate Unit &lt;x&gt; [kg/s]
-
-* HVAC,Average,Chiller Heater COP Unit &lt;x&gt; []
-
-* HVAC,Average,Chiller Heater Capacity Temperature Modifier Multiplier Unit &lt;x&gt; []
-
-* HVAC,Average,Chiller Heater EIR Temperature Modifier Multiplier Unit &lt;x&gt; []
-
-* HVAC,Average,Chiller Heater EIR Part Load Modifier Multiplier Unit &lt;x&gt; []
-
-
-Note that much of these output variables are adapted from the definitions above under “Generic Chiller Outputs� and “Electric EIR Chiller Outputs.� The following outputs are repeated up to the maximum of individual chiller-heater module objects. The maximum number may be different from the number of object defined in this object when users define two or more identical chiller-heater modules for a single chiller heater object in the central heat pump system.
-
-#### Chiller Heater Operation Mode Unit &lt;x&gt; [  ]
-
-This output represents the operating mode of the chiller-heater module. Two single mode outputs and three simultaneous cooling-heating mode outputs are possible:
-
-0. off
-
-1. cooling-only mode
-
-2. heating-only mode
-
-3. heat recovery mode
-
-4. cooling dominant simultaneous cooling-heating mode
-
-5. heating dominant simultaneous cooling-heating mode.
-
-The first mode 0 is reported when the chiller-heater is turned off. The next two modes 2 and 3 are reported when the chiller-heater provides only either cooling or heating, respectively. The last three modes 3 to 5 indicate when the chiller-heater is in a simultaneous cooling-heating mode. Mode 3 indicates the chiller-heaters provides simultaneous cooling and heating ***without*** heat exchange with the ground source. Mode 4 denotes that at least one of the chiller-heater modules in the central heat pump system provides both cooling and heating, and the chiller-heater is meeting remaining cooling demand (see Figure 78. Diagram of a central heat pump system with one chiller-heater in heat recovery mode and two chiller-heaters in cooling-only mode) Similarly, mode 5 indicates that at least one of the chiller-heater modules in the central heat pump system is in the heat recovery mode, and the chiller-heater is meeting remaining heating demand (see Figure 79).
-
-Note that the decision to operate individual chiller-heater modules is solely dependent on the chiller-heater schedule and loads. A fraction may appear in case the chiller-heater mode varies within a zone time step. In this particular case, users may define a detailed reporting frequency for this output variable.
-
-#### Chiller Heater Part Load Ratio Unit &lt;x&gt; [  ]
-
-This output is the ratio of the evaporator heat transfer rate plus the false load heat transfer rate (if applicable) to the available chiller-heater capacity. This value is used to determine ChillerEIRFPLR.
-
-#### Chiller Heater Cycling Ratio Unit &lt;x&gt; [  ]
-
-The cycling ratio is the amount of time the chiller-heater operates during each simulation time step. If the chiller-heater part-load ratio falls below the minimum part-load ratio, the chiller-heater cycles on and off to meet the loads.
-
-#### Chiller Heater Cooling Electric Power Unit &lt;x&gt; [W]
-
-#### Chiller Heater Cooling Electric Energy Unit &lt;x&gt; [J]
-
-These outputs are the cooling electric power consumption of the chiller-heater.
-
-#### Chiller Heater Heating Electric Power Unit &lt;x&gt; [W]
-
-#### Chiller Heater Heating Electric Energy Unit &lt;x&gt; [J]
-
-These outputs are the heating electric power consumption of the chiller-heater.
-
-#### Chiller Heater Cooling Rate Unit &lt;x&gt; [W]
-
-#### Chiller Heater Cooling Energy Unit &lt;x&gt; [J]
-
-These outputs are the evaporator heat transfer which is the cooling delivered by the chiller-heater module.
-
-#### Chiller Heater False Load Heat Transfer Rate Unit &lt;x&gt; [W]
-
-#### Chiller Heater False Load Heat Transfer Energy Unit &lt;x&gt; [J]
-
-These outputs are the heat transfer rate and total heat transfer due to false loading of the chiller-heater. When the chiller-heater part-load ratio is below the minimum unloading ratio, the chiller-heater false loads (e.g. hot-gas bypass) to further reduce capacity.
-
-#### Chiller Heater Condenser Heat Transfer Rate Unit &lt;x&gt; [C]
-
-#### Chiller Heater Condenser Heat Transfer Energy Unit &lt;x&gt; [C]
-
-These outputs are the heat transfer which is the heating delivered by the chiller-heater module in heating mode.
-
-#### Chiller Heater Evaporator Inlet Temperature Unit &lt;x&gt; [C]
-
-#### Chiller Heater Evaporator Outlet Temperature Unit &lt;x&gt; [C]
-
-#### Chiller Heater Evaporator Mass Flow Rate Unit &lt;x&gt; [C]
-
-These outputs are the evaporator water inlet and outlet temperatures and flow rate. Note that these represent the chilled water temperatures and flow rate in cooling mode or the source water temperature and flow rate in heating mode.
-
-#### Chiller Heater Condenser Inlet Temperature Unit &lt;x&gt; [C]
-
-#### Chiller Heater Condenser Outlet Temperature Unit &lt;x&gt; [C]
-
-#### Chiller Heater Condenser Mass Flow Rate Unit &lt;x&gt; [C]
-
-These outputs are the condenser water inlet and outlet temperatures and flow rate. Note that these represent the hot water temperatures and flow rate in heating mode or the source water temperature and flow rate in cooling mode.
-
-#### Chiller Heater COP Unit &lt;x&gt; [C]
-
-This output is the coefficient of performance for the chiller-heater. It is calculated as the evaporator heat transfer rate divided by the chiller-heater electric power.
-
-#### Chiller Heater Capacity Temperature Modifier Multiplier Unit &lt;x&gt; [C]
-
-This is the output of the curve object Cooling Capacity Function of Temperature Curve.
-
-#### Chiller Heater EIR Temperature Modifier Multiplier Unit &lt;x&gt; [C]
-
-This is the output of the curve object Electric Input to Cooling Output Ratio Function of Temperature Curve.
-
-#### Chiller Heater EIR Part Load Modifier Multiplier Unit &lt;x&gt; [C]
-
-This is the output of the curve object Electric Input to Cooling Output Ratio Function of Part Load Ratio Curve.
-
-### Thermal Storage Objects
-
-There are four types of cold thermal storage objects:
-
-- ThermalStorage:Ice:Simple
-
-- ThermalStorage:Ice:Detailed
-
-- ThermalStorage:ChilledWater:Mixed
-
-- ThermalStorage:ChilledWater:Stratified
-
-These objects are typically placed on the supply side of a primary chilled water loop in series or in parallel with one or more chillers.  Using the the component set point (PlantEquipmentOperation:ComponentSetpoint) plant operation scheme type, the chiller and storage tank setpoints are used to control operation. Using a SetpointManager:Scheduled object (or other appropriate type of set point manager), the setpoints on the chiller outlet node and the ice storage outlet node can be used to control how the cooling load is shared and when charging of storage occurs.  Example setpoints to use for various modes of operation are shown in the table below:
-
-<table class="table table-striped">
-<tr>
-<th>Mode</th>
-<th>Chiller Setpoint</th>
-<th>Storage Setpoint</th>
-</tr>
-<tr>
-<td>Charging ice storage tank</td>
-<td>-5C</td>
-<td>7C</td>
-</tr>
-<tr>
-<td>Cooling with chiller only</td>
-<td>7C</td>
-<td>99C</td>
-</tr>
-<tr>
-<td>Cooling with chiller and storage (fully load chiller before using storage))</td>
-<td>7C</td>
-<td>7C</td>
-</tr>
-<tr>
-<td>Cooling with chiller and storage (chiller carries portion of load, valid if chiller is upstream of storage)</td>
-<td>10C</td>
-<td>7C</td>
-</tr>
-</table>
-
-Example files have been developed for three common storage configurations:
-
-1. Series – Chiller Upstream:  In this configuration, a chiller is placed first on the same branch as the storage unit and both use the **SeriesActive** branch control type.
-
-2. Series – Chiller Downstream:  In this configuration, a chiller is placed second on the same branch as the storage unit and both use the **SeriesActive** branch control type.
-
-3. Parallel:  In this configuration, the chiller is on a branch parallel to the storage unit branch when it is not charging.  During charging mode, valves will be changed so that the chiller is in series upstream of the storage.  To accomplish this in EnergyPlus, the chiller must be modeled using two different chiller objects to represent the same chiller.  One chiller object on a parallel branch operates only when storage is not being charged.  The other chiller object, in series upstream of the storage unit operates only during charging mode.
-
-Other considerations for applying cold thermal storage objects include:
-
-- In the PlantLoop object, the "Minimum Loop Temperature" must be set equal to or less than the lowest setpoint to be used anywhere in the loop.
-
-- To end the storage charging cycle, use a AvailabilityManager:LowTemperatureTurnOff to shut off the primary chilled water loop when the temperature leaving the storage tank nears the charging mode chiller setpoint indicating that the tank is fully charged.  For example, if the chiller is set to provide –5C chilled water during charging, then charging can be shut down when the water temperature leaving the storage unit reaches –4C.  When using a primary-secondary loop arrangement, it may be necessary to schedule this availability manager to be active only when the HVAC systems are off to avoid fighting between the demand controls and the availability manager.
-
-### ThermalStorage:Ice:Simple
-
-This thermal storage model is based on a simple simulation of an ice storage tank with a fixed capacity.  The tank is charged, or frozen, in an ice-on-coil configuration where ice builds up on the outside of the tubes carrying the brine or glycol solution from the chiller.  There are two discharge (melt) options, internal or external.  Internal melt uses the same fluid tubes for charging and discharging.  External melt uses a separate fluid path for discharge such that the outer layers of ice melt first.  The ice storage model includes an implied 3-way valve to control the amount if charge/discharge based on the incoming water temperature and the outlet node setpoint temperature.  The storage tank is assumed to be fully charged (full of ice) at the beginning of each environment.  The tank is then allowed to charge and discharge during the warmup days of the environment.  The tank is best controlled using the PlantEquipmentOperation:ComponentSetpoint plant operation scheme, and requires that a setpoint be placed by a set point manager on the ice storage Plant Outlet Node.
-
-The input fields for the object are described in detail below:
-
-#### Field: Name
-
-This alpha field contains the identifying name for the ice storage tank.
-
-#### Field: Ice Storage Type
-
-This alpha field specifies the type of ice storage tank to be modeled. There are two options:  "**IceOnCoilInternal**" models ice-on-coil, internal melt."IceOnCoilExternal" models ice-on-coil, external melt.
-
-#### Field: Capacity
-
-This numeric field contains the nominal capacity of the ice storage in GJ (Giga is 10<sup>9</sup>).
-
-#### Field: Inlet Node Name
-
-This alpha field specifies the name of the chilled water inlet node.
-
-#### Field: Outlet Node Name
-
-This alpha field specifies the name of the chilled water outlet node.
-
-Following is an example input for the THERMAL STORAGE:ICE:SIMPLE object.
-
-
-
-```idf
-ThermalStorage:Ice:Simple,
-    ITS,                     !- Ice Storage Name
-    IceOnCoilInternal,       !- Ice Storage Type
-    1.5,                     !- Ice Storage Capacity {GJ}
-    ITS Inlet Node,          !- Plant Loop Inlet Node
-    ITS Outlet Node;         !- Plant Loop Outlet Node
-```
-
-### Simple Ice Storage Outputs
-
-The following outputs are available for simple Ice Storage model:
-
-* HVAC,Average,Ice Thermal Storage Requested Load [W]
-
-* Zone,Average,Ice Thermal Storage End Fraction[]
-
-* HVAC,Average,Ice Thermal Storage Mass Flow Rate [kg/s]
-
-* HVAC,Average,Ice Thermal Storage Inlet Temperature [C]
-
-* HVAC,Average,Ice Thermal Storage Outlet Temperature [C]
-
-* HVAC,Average,Ice Thermal Storage Cooling Discharge Rate [W]
-
-* HVAC,Sum,Ice Thermal Storage Cooling Discharge Energy [J]
-
-* HVAC,Average,Ice Thermal Storage Cooling Charge Rate [W]
-
-* HVAC,Sum,Ice Thermal Storage Cooling Charge Energy [J]
-
-
-
-#### Ice Thermal Storage Requested Load [W]
-
-The load requested by the plant control scheme. A positive value indicates a cooling load or a request to discharge (melt) the tank. A negative value indicates a request to charge (freeze) the tank.
-
-#### Ice Thermal Storage End Fraction []
-
-The fraction of full ice storage which is present at the end of the current HVAC timestep. When reported at a frequency less than detailed, this value is averaged over the reporting period.
-
-#### Ice Thermal Storage Mass Flow Rate [kg/s]
-
-The total water mass flow rate through the ice storage component. Because the component includes an implied 3-way valve, this flow may be all through the tank, all bypassed through the valve, or a mixture of both.
-
-#### Ice Thermal Storage Inlet Temperature [C]
-
-The water temperature entering the ice storage component.
-
-#### Ice Thermal Storage Outlet Temperature [C]
-
-The water temperature leaving the ice storage component.
-
-#### Ice Thermal Storage Cooling Discharge Rate [W]
-
-The rate of cooling delivered by the ice storage component. A positive value indicates the ice tank is discharging (melting). A zero value indicates the tank is charging or dormant.
-
-#### Ice Thermal Storage Cooling Discharge Energy [J]
-
-The cooling energy delivered by the ice storage component. A positive value indicates the ice tank is discharging (melting). A zero value indicates the tank is charging or dormant.
-
-#### Ice Thermal Storage Cooling Charge Rate [W]
-
-The rate of charging delivered to the ice storage component. A positive value indicates the ice tank is charging (freezing). A zero value indicates the tank is discharging or dormant.
-
-#### Ice Thermal Storage Cooling Charge Energy [J]
-
-The charging energy delivered to the ice storage component. A positive value indicates the ice tank is charging (freezing). A zero value indicates the tank is discharging or dormant.
-
-### ThermalStorage:Ice:Detailed
-
-The detailed ice storage model allows the users of EnergyPlus to model more closely specific manufacturers’ ice storage units. This is possible due to the use of curve fits to simulate the performance of the ice storage unit during charging and discharging. In this implementation, both charging and discharging are a function of the fraction charged/discharged as well as the log mean temperature difference across the storage unit. More information on the model is provided in the Engineering Reference for EnergyPlus. The remainder of this section describes the input required for the detailed ice storage model and the output that it can produce.
-
-#### Field: Name
-
-This field is the name of the detailed ice storage system given to it by the user.
-
-#### Field: Availability Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that determines whether or not the ice storage system is available during a particular time period. This allows the system to be turned off during a particular season. A value of less than or equal to zero indicates that the ice storage system is not available. Any value greater than zero indicates that the system is available. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Capacity
-
-This number is the maximum amount of latent thermal storage available in the ice storage system. This model does not allow the removal or addition of sensible energy from the tank. Thus, it is always assumed to be at the freezing temperature of the storage material. The capacity is expressed in units of GJ.
-
-#### Field: Inlet Node Name
-
-This is the name of the node that connects the ice storage system to the plant loop. It is the inlet node to the ice storage component. The next field defines the outlet node. Due to presence of an internal bypass in this model, there are other “nodes� that are handled internally within the program. Users do not need to define any nodes other than the inlet and outlet nodes.
-
-#### Field: Outlet Node Name
-
-This is the name of the other node that connects the ice storage system to the plant loop. It is the outlet node to the ice storage component.
-
-#### Field: Discharging Curve Object Type
-
-The detailed ice storage model in EnergyPlus takes advantage of the Curve feature of the program. Currently, the only two allowed curve fit types for the detailed ice storage model are the QuadraticLinear and the CubicLinear curves. More information on this curve can be found in the section on Curves.
-
-#### Field: Discharging Curve Name
-
-This field specifies the name of the actual curve fit to be used to model the discharging process of the detailed ice storage system.
-
-#### Field: Charging Curve Object Type
-
-The detailed ice storage model in EnergyPlus takes advantage of the Curve feature of the program. Currently, the only two allowed curve fit types for the detailed ice storage model are the QuadraticLinear and the CubicLinear curves. More information on this curve can be found in the section on Curves.
-
-#### Field: Charging Curve Name
-
-This field specifies the name of the actual curve fit to be used to model the charging process of the detailed ice storage system.
-
-#### Field: Timestep of the Curve Data
-
-This field defines what timestep was used to produce the curve fits named in the previous inputs. This parameter is important because the curve fit is non-dimensional. Thus, the data used to develop the curve fits were based on a specific length of time. In many cases, this is probably one hour or 1.0. The units for this parameter are hours.
-
-#### Field: Parasitic Electric Load During Discharging
-
-This field defines the amount of parasitic electric consumption (for controls or other miscellaneous electric consumption associate with the ice storage unit itself) during the discharge phase. This parameter is dimensionless and gets multiplied by the current load on the tank.
-
-#### Field: Parasitic Electric Load During Charging
-
-This field defines the amount of parasitic electric consumption (for controls or other miscellaneous electric consumption associate with the ice storage unit itself) during the charge phase. This parameter is dimensionless and gets multiplied by the current load on the tank.
-
-#### Field: Tank Loss Coefficient
-
-This field defines the loss of ice stored during a particular hour. This field is dimensionless (per hour). It is not multiplied by any temperature difference between the tank and the environment in which it might be located.
-
-#### Field: Freezing Temperature of Storage Medium
-
-This parameter defines the freezing/melting temperature of the ice storage medium in degrees Celsius. For most tanks, this is simply 0.0°C (the default value). However, some tanks may use other materials or salts which would change the freezing temperature. This can be changed using this parameter.
-
-#### Field: Thaw Process Indicator
-
-This input field assists in more accurate modeling of the charging process by defining how the thawing of ice takes place. There are two options for this input: **InsideMelt** and **OutsideMelt**. Some ice storage systems, by their nature, start the charging process with a bare coil or no ice left on the charging surface even though there is still ice stored in the tank.  An example of such a system is sometimes referred to as an ice-on-coil inside melt system, and these systems would define this parameter using the “InsideMelt� option for this field.  Other systems melt the ice from the outside, leaving ice still on the charging surface when charging begins. These systems are modeled using the “OutsideMelt� option.  For systems that have a charging process that does not vary significantly with fraction charged can ignore this input by accepting the default value.  The default value for this field is “OutsideMelt�.
-
-
-
-An IDF example:
-
-```idf
-ThermalStorage:Ice:Detailed,
-    Ice Tank,                !- Ice Storage Name
-    ON,                      !- Ice Storage availability schedule
-    0.5,                     !- Ice Storage Capacity {GJ}
-    Ice Tank Inlet Node,     !- Plant Loop Inlet Node
-    Ice Tank Outlet Node,    !- Plant Loop Outlet Node
-    QuadraticLinear,         !- Discharging Curve Fit Type
-    DischargeCurve,          !- Discharging Curve Name
-    QuadraticLinear,         !- Charging Curve Fit Type
-    ChargeCurve,             !- Charging Curve Name
-    1.0,                     !- Timestep of Curve Fit Data
-    0.0001,                  !- Parasitic electric load during discharging
-    0.0002,                  !- Parasitic electric load during charging
-    0.0003,                  !- Tank loss coefficient
-    0.0;                     !- Freezing temperature [C]
-```
-
-
-
-
-### Detailed Ice Storage Outputs
-
-Current detailed ice storage output variables are:
-
-* System, Average, Ice Thermal Storage Cooling Rate [W]
-
-* System, Average, Ice Thermal Storage Change Fraction []
-
-* System, Average, Ice Thermal Storage End Fraction []
-
-* System, Average, Ice Thermal Storage Mass Flow Rate [kg/s]
-
-* System, Average, Ice Thermal Storage Bypass Mass Flow Rate [kg/s]
-
-* System, Average, Ice Thermal Storage Tank Mass Flow Rate [kg/s]
-
-* System, Average, Ice Thermal Storage Fluid Inlet Temperature [C]
-
-* System, Average, Ice Thermal Storage Blended Outlet Temperature [C]
-
-* System, Average, Ice Thermal Storage Tank Outlet Temperature [C]
-
-* System, Average, Ice Thermal Storage Cooling Discharge Rate [W]
-
-* System, Sum, Ice Thermal Storage Cooling Discharge Energy [J]
-
-* System, Average, Ice Thermal Storage Cooling Charge Rate [W]
-
-* System, Sum, Ice Thermal Storage Cooling Charge Energy [J]
-
-* System, Average, Ice Thermal Storage Ancillary Electric Power [W]
-
-* System, Sum, Ice Thermal Storage Ancillary Electric Energy [J]
-
-* System, Average, Ice Thermal Storage On Coil Fraction []
-
-
-####  Ice Thermal Storage Cooling Rate [W]
-
-The actual load (absolute value) provided by the ice storage system during the current timestep
-
-#### Ice Thermal Storage Change Fraction []
-
-The change in the ice tank’s charge fraction charged during the current timestep (positive for charging, negative for discharging).
-
-#### Ice Thermal Storage End Fraction [ ]
-
-The fraction charge of the ice storage system at the end of the timestep
-
-#### Ice Thermal Storage On Coil Fraction [ ]
-
-The fraction of ice that is actually on the freezing surface at the end of the timestep.  This can be different for an “inside melt� system than the end fraction (see previous output parameter).
-
-#### Ice Thermal Storage Mass Flow Rate [kg/s]
-
-The mass flow through the ice storage component
-
-#### Ice Thermal Storage Bypass Mass Flow Rate [kg/s]
-
-The mass flow through the ice storage component bypass (bypasses the actual unit)
-
-#### Ice Thermal Storage Tank Mass Flow Rate [kg/s]
-
-The mass flow through the ice storage unit itself
-
-#### Ice Thermal Storage Fluid Inlet Temperature [C]
-
-The inlet temperature to the ice storage component
-
-#### Ice Thermal Storage Blended Outlet Temperature [C]
-
-The outlet temperature of the component after mixing any bypass flow with flow through the ice storage unit
-
-#### Ice Thermal Storage Tank Outlet Temperature [C]
-
-The outlet temperature of the ice storage unit itself below mixing with any bypass flow
-
-#### Ice Thermal Storage Cooling Discharge Rate [W]
-
-The cooling done (as a rate) by the ice storage unit or its discharge rate
-
-#### Ice Thermal Storage Cooling Discharge Energy [J]
-
-The total cooling done by the ice storage unit or its discharge rate
-
-#### Ice Thermal Storage Cooling Charge Rate [W]
-
-The charging done (as a rate) to the ice storage unit
-
-#### Ice Thermal Storage Cooling Charge Energy [J]
-
-The total charging done to the ice storage unit
-
-#### Ice Thermal Storage Ancillary Electric Power [W]
-
-The electric power as a result of parasitic loads on the ice storage unit for things like controls or other miscellaneous parts of the ice storage unit itself
-
-#### Ice Thermal Storage Ancillary Electric Energy [J]
-
-The electric consumption as a result of parasitic loads on the ice storage unit for things like controls or other miscellaneous parts of the ice storage unit itself
-
-### ThermalStorage:ChilledWater:Mixed
-
-The ThermalStorage:ChilledWater:Mixed object analytically solves the differential equation governing the energy balance of the water tank.  The chilled water is “used� by drawing from the “Use Side� of the water tank.  The tank is indirectly charged by circulating cold water through the “Source Side� of the water tank.
-
-Control is based on cycling flow through the source side.  When the tank temperature rises above a “cut-in� temperature, source side flow is requested.  Source side flow will continue until the tank is cooled to below the tank set point or “cut-out� temperature.
-
-For heat gains from the ambient environment, the ambient air temperature can be taken from a schedule, a zone, or the exterior. When used with a zone, the skin gains are removed from the zone heat balance as negative internal heat gains.
-
-#### Field: Name
-
-The unique name of the ThermalStorage:ChilledWater:Mixed object.
-
-#### Field: Tank Volume
-
-The volume of the thermal storage tank [m<sup>3</sup>].
-
-#### Field: Setpoint Temperature Schedule Name
-
-The reference to the schedule object specifying the chilled water temperature setpoint [°C]. Also known as the "cut-out" temperature.
-
-#### Field: Deadband Temperature Difference
-
-The delta temperature difference [Δ°C] between the setpoint and the "cut-in" temperature at which the storage tank will request cooling. In other words, the "cut-in" temperature is Setpoint + Deadband.
-
-#### Field: Minimum Temperature Limit
-
-The temperature [°C] at which the tank water becomes too cold.  No source side flow is allowed when the tank temperature is below this limit.  The minimum temperature must be lower than the setpoint temperature at all times.
-
-#### Field: Nominal Cooling Capacity
-
-This field describes the typical cooling capacity that the chilled water tank will provide.  Since this is a passive device, the actual cooling capacity depends on water temperatures and flow rates.  However, this field is used to describe the chilled water tank’s nominal cooling capacity for supervisory control where plant operation schemes require a cooling capacity to model how equipment is dispatched.
-
-#### Field: Ambient Temperature Indicator
-
-The Ambient Temperature Indicator specifies how the ambient air temperature will be indicated. The field can be “Schedule�, “Zone�, or “Exterior.� If *Schedule* is used, the Ambient Temperature Schedule Name field provides the values for ambient temperature. If *Zone* is used, the zone air temperature of the zone specified in the Ambient Temperature Zone field provides the ambient temperature. If *Exterior* is used, the outdoor dry-bulb air temperature provides the ambient temperature.
-
-#### Field: Ambient Temperature Schedule Name
-
-The field contains the name of a schedule object specifying the ambient air temperature around the tank for skin gains. This field is only used if Ambient Temperature Indicator is *Schedule*.
-
-#### Field: Ambient Temperature Zone Name
-
-The reference to the zone object specifying the ambient air temperature around the tank for skin gains. This field is only used if Ambient Temperature Indicator is *Zone*.
-
-#### Field: Ambient Temperature Outdoor Air Node Name
-
-This optional alpha field specifies the outdoor air node (OutdoorAir:Node) name used to define the ambient conditions surrounding the chilled water tank. This field is applicable only when the Ambient Temperature Indicator is specified as *Exterior*, otherwise this field should be left blank. The node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-#### Field: Heat Gain Coefficient from Ambient Temperature
-
-The gain coefficient [W/K] from the ambient air temperature. This coefficient is often referred to as the "UA" for the overall tank thermal performance with respect to heat gains from the tank’s skin..
-
-#### Field: Use Side Inlet Node Name
-
-The inlet node connection to the plant loop for the use side of the chilled water storage tank. Typically the use side draws chilled water from the tank and returns warmer water.
-
-#### Field: Use Side Outlet Node Name
-
-The outlet node connection to the plant loop for the use side of the chilled water storage tank. Typically the use side chilled water from the tank and returns warmer water.
-
-#### Field: Use Side Heat Transfer Effectiveness
-
-This field specifies the heat transfer effectiveness between the use side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the use side water and the tank water. If the effectiveness is lower, then the use side outlet water temperature will not be as cold as the tank water, simulating a heat exchanger.
-
-#### Field: Use Side Availability Schedule Name
-
-This field contains the name of an availability schedule for the use side of the water tank. If the schedule’s value is 0.0, then the use side is not available and flow will not be requested.  If the schedule’s value is note equal to 0.0 (usually 1 is used), the use side is available. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Use Side Design Flow Rate
-
-This field is used to specify the design flow rate through the Use Side of the chilled water tank.  The volumetric design flow rate is specified in m<sup>3</sup>/s.  The field can be autosized.  If autosized, then the input file should include a Plant Sizing object for the plant loop connected to the Use side.  Sizing results are reported in the EIO file.
-
-#### Field: Source Side Inlet Node Name
-
-The inlet node connection to the plant loop for the source side of the chilled water storage tank. Typically the source side draws somewhat warm water from the tank and returns colder water.  The source side volume flow rate is obtained from the plant loop.  The magnitude of the flow rates through the source side can be controlled by setting the Maximum Branch Flow Rate field in the BRANCH object that connects the source inlet node.
-
-#### Field: Source Side Outlet Node Name
-
-The outlet node connection to the plant loop for the source side of the chilled water storage tank. Typically the source side draws somewhat warm water from the tank and returns colder water.
-
-#### Field: Source Side Heat Transfer Effectiveness
-
-This field specifies the heat transfer effectiveness between the source side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the source side water and the tank water. If the effectiveness is lower, then the source side outlet water temperature will not be as cold as the tank water, simulating a heat exchanger.
-
-#### Field: Source Side Availability Schedule Name
-
-This field contains the name of an availability schedule for the source side of the water tank.  If the schedule’s value is 0.0, then the source side is not available and flow will not be requested.  If the schedule’s value is not equal to 0.0 (usually 1 is used), the source side is available. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Source Side Design Flow Rate
-
-This field is used to specify the design flow rate through the Source Side of the chilled water tank.  The volumetric design flow rate is specified in m<sup>3</sup>/s.  The field can be autosized.  If autosized, then the input file should include a Plant Sizing object for the plant loop.  Sizing results are reported in the EIO file.
-
-#### Field: Tank Recovery Time
-
-This field is used to autosize the Source Side Design Flow Rate.  The field is used if the previous field is set to autosize and the water tank’s source side is on the demand side of a plant loop.  This the the time, in hours, that the chilled water tank is to be indirectly cooled from 14.4ºC to 9.0ºC using the exit temperature of in the associated Plant Sizing object.
-
-An example input object follows.
-
-```idf
-  ThermalStorage:ChilledWater:Mixed,
-    Chilled Water Storage Tank 1 ,  !- Name
-    4.0 ,                           !- Tank Volume
-    CW-Tank-Temp-Schedule,          !- Setpoint Temperature Schedule Name
-    3.5,                            !- Deadband Temperature Difference
-    1.0 ,                           !- Minimum Temperature Limit
-    25000 ,                         !- Nominal Cooling Capacity
-    Zone ,                          !- Ambient Temperature Indicator
-    ,                               !- Ambient Temperature Schedule Name
-    ZN_1_FLR_1_SEC_5 ,              !- Ambient Temperature Zone Name
-    ,                               !- Ambient Temperature Outdoor Air Node Name
-    5.0 ,                           !- Heat Gain Coefficient from Ambient Temperature
-    CW Tank Discharge Inlet node,   !- Use Side Inlet Node Name
-    CW Tank Discharge Outlet node , !- Use Side Outlet Node Name
-    1.0 ,                           !- Use Side Effectiveness
-    TES Use Schedule,               !- Use Side Availability Schedule Name
-    Autosize ,                      !- Use Side Design Flow Rate
-    CW Tank Charge Inlet Node,      !- Source Side Inlet Node Name
-    CW Tank Charge Outlet Node,     !- Source Side Outlet Node Name
-    1.0,                            !- Source Side Effectiveness
-    TES Charge Schedule,            !- Source Side Availability Schedule Name
-    Autosize ,                      !- Source Side Design Flow Rate
-    4.0;                            !- Tank Recovery Time
-```
-
-
-
-### Chilled Water Mixed Thermal Storage Outputs
-
-The following output variables are reported for chilled water thermal storage tanks.
-
-* Chilled Water Thermal Storage Tank Temperature               !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Final Tank Temperature         !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Tank Heat Gain Rate                 !- HVAC Average [W]
-
-* Chilled Water Thermal Storage Tank Heat Gain Energy               !- HVAC Sum [J]
-
-* Chilled Water Thermal Storage Use Side Mass Flow Rate             !- HVAC Average [kg/s]
-
-* Chilled Water Thermal Storage Use Side Inlet Temperature     !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Use Side Outlet Temperature    !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Use Side Heat Transfer Rate                  !- HVAC Average [W]
-
-* Chilled Water Thermal Storage Use Side Heat Transfer Energy                !- HVAC Sum [J]
-
-* Chilled Water Thermal Storage Source Side Mass Flow Rate          !- HVAC Average [kg/s]
-
-* Chilled Water Thermal Storage Source Side Inlet Temperature  !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Source Side Outlet Temperature !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Source Side Heat Transfer Rate               !- HVAC Average [W]
-
-* Chilled Water Thermal Storage Source Side Heat Transfer Energy             !- HVAC Sum [J]
-
-
-#### Chilled Water Thermal Storage Tank Temperature [C]
-
-The average water tank temperature.
-
-#### Chilled Water Thermal Storage Final Tank Temperature [C]
-
-The final water tank temperature at the end of the system timestep. If reported at the "Detailed" interval, this output variable can be used to verify an exact energy balance on the water storage tank.
-
-#### Chilled Water Thermal Storage Tank Heat Gain Rate [W]
-
-The average heat exchange rate to the storage tank from the surrounding ambient.  This is usually positive with surrounding ambient heating the storage tank.
-
-#### Chilled Water Thermal Storage Tank Heat Gain Energy [J]
-
-The energy exchange to the storage tank from the surrounding ambient.  This is usually positive with surrounding ambient heating the storage tank.
-
-#### Chilled Water Thermal Storage Use Side Mass Flow Rate [kg/s]
-
-The use side mass flow rate.
-
-#### Chilled Water Thermal Storage Use Side Inlet Temperature [C]
-
-The inlet temperature on the use side.
-
-#### Chilled Water Thermal Storage Use Side Outlet Temperature [C]
-
-The outlet temperature on the use side.
-
-#### Chilled Water Thermal Storage Use Side Heat Transfer Rate [W]
-
-The average heat transfer rate between the use side water and the tank water.
-
-#### Chilled Water Thermal Storage Use Side Heat Transfer Energy [J]
-
-The heat transfer energy between the use side water and the tank water.
-
-#### Chilled Water Thermal Storage Source Side Mass Flow Rate [kg/s]
-
-The source side mass flow rate.
-
-#### Chilled Water Thermal Storage Source Side Inlet Temperature [C]
-
-The inlet temperature on the source side.
-
-#### Chilled Water Thermal Storage Source Side Outlet Temperature [C]
-
-The outlet temperature on the source side.
-
-#### Chilled Water Thermal Storage Source Side Heat Transfer Rate [W]
-
-The average heat transfer rate between the source side water and the tank water.
-
-#### Chilled Water Thermal Storage Source Side Heat Transfer Energy [J]
-
-The heat transfer energy between the source side water and the tank water.
-
-### ThermalStorage:ChilledWater:Stratified
-
-The ThermalStorage:ChilledWater:Stratified object divides the water tank into multiple nodes of equal volume. The nodes are coupled by vertical conduction effects, internode fluid flow, and temperature inversion mixing. The object simultaneously solves the differential equations governing the energy balances on the nodes using a numerical method. The system timestep is divided into many small substeps that allow the simulation to capture events that occur on a very short time scale.  The chilled water is “used� by drawing from the “Use Side� of the water tank.  The tank is indirectly charged by circulating cold water through the “Source Side� of the water tank.
-
-Control is based on cycling flow through the source side.  When the tank temperature rises above a “cut-in� temperature, source side flow is requested.  Source side flow will continue until the tank is cooled to below the tank set point or “cut-out� temperature.
-
-For heat gains from the ambient environment, the ambient air temperature can be taken from a schedule, a zone, or the exterior. When used with a zone, the skin gains are removed from the zone heat balance as negative internal heat gains.
-
-#### Field: Name
-
-The unique name of the ThermalStorage:ChilledWater:Stratified object.
-
-#### Field: Tank Volume
-
-The volume of the thermal storage tank [m<sup>3</sup>].
-
-#### Field: Tank Height
-
-The height [m] of the tank. For the HorizontalCylinder shape (see below) the height of the tank is the measure in the axial direction, i.e., the height if you were to stand the cylinder up on its end.
-
-#### Field: Tank Shape
-
-The tank shape determines the size and skin losses of the stratified nodes. There are three options:  “VerticalCylinder,� “HorizontalCylinder,� and “Other.�
-
-*VerticalCylinder* describes most upright cylindrical water tanks.
-
-*HorizontalCylinder* describes a few specialty water tanks and some large commercial storage tanks. *HorizontalCylinder* implies that the tank is divided into nodes of equal mass, but not equal height.
-
-*Other* describes water storage tanks that have a uniform horizontal cross-section, but are not cylinders, e.g., a cuboid or other shape. The length of the perimeter is then specified by the Tank Perimeter field.
-
-If blank, the default shape is *VerticalCylinder*.
-
-#### Field: Tank Perimeter
-
-The length of the tank perimeter [m]. This field is only used if Tank Shape is *Other*.
-
-#### Field: Setpoint Temperature Schedule Name
-
-The reference to the schedule object specifying the chilled water temperature setpoint [°C]. Also known as the "cut-out" temperature.
-
-#### Field: Deadband Temperature Difference
-
-The delta temperature difference [Δ°C] between the setpoint and the "cut-in" temperature at which the storage tank will request cooling. In other words, the "cut-in" temperature is Setpoint + Deadband.
-
-#### Field: Temperature Sensor Height
-
-This field is used to describe the location in the tank where the temperature is sensed for control descisions.  The program will associate one of the nodes with this height and use that node’s temperature for control decisions.  The location is described in meters from the bottom of the tank.
-
-#### Field: Minimum Temperature Limit
-
-The temperature [°C] at which the tank water becomes too cold.  No source side flow is allowed when the tank temperature is below this limit.  The minimum temperature must be lower than the setpoint temperature at all times.
-
-#### Field: Nominal Cooling Capacity
-
-This field describes the typical cooling capacity that the chilled water tank will provide.  Since this is a passive device, the actual cooling capacity depends on water temperatures and flow rates.  However, this field is used to describe the chilled water tank’s nominal cooling capacity for supervisory control where plant operation schemes require a cooling capacity to model how equipment is dispatched.
-
-#### Field: Ambient Temperature Indicator
-
-The Ambient Temperature Indicator specifies how the ambient air temperature will be indicated. The field can be “Schedule�, “Zone�, or “Exterior.� If *Schedule* is used, the Ambient Temperature Schedule Name field provides the values for ambient temperature. If *Zone* is used, the zone air temperature of the zone specified in the Ambient Temperature Zone field provides the ambient temperature. If *Exterior* is used, the outdoor dry-bulb air temperature provides the ambient temperature.
-
-#### Field: Ambient Temperature Schedule Name
-
-The field contains the name of a schedule object specifying the ambient air temperature around the tank for skin gains. This field is only used if Ambient Temperature Indicator is *Schedule*.
-
-#### Field: Ambient Temperature Zone Name
-
-The reference to the zone object specifying the ambient air temperature around the tank for skin gains. This field is only used if Ambient Temperature Indicator is *Zone*.
-
-#### Field: Ambient Temperature Outside Air Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the ambient conditions surrounding the chilled water tank. This field is applicable only when the Ambient Temperature Indicator is specified as *Exterior*, otherwise this field should be left blank. The node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-#### Field: Uniform Skin Loss Coefficient per Unit Area to Ambient Temperature
-
-The uniform skin loss coefficient [W/m<sup>2</sup>-K] or U-Value of the tank to the ambient air temperature. The uniform skin loss accounts for the tank insulation. The overall losses at any particular tank node can be further modified using the Additional Loss Coefficient fields to account for thermal shorting due to pipe penetrations, tank feet, and any other loss effects.
-
-#### Field: Use Side Inlet Node Name
-
-The inlet node connection to the plant loop for the use side of the chilled water storage tank. Typically the use side draws chilled water from the tank and returns warmer water.
-
-#### Field: Use Side Outlet Node Name
-
-The outlet node connection to the plant loop for the use side of the chilled water storage tank. Typically the use side chilled water from the tank and returns warmer water.
-
-#### Field: Use Side Heat Transfer Effectiveness
-
-This field specifies the heat transfer effectiveness between the use side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the use side water and the tank water. If the effectiveness is lower, then the use side outlet water temperature will not be as cold as the tank water, simulating a heat exchanger.
-
-#### Field: Use Side Availability Schedule Name
-
-This field contains the name of an availability schedule for the use side of the water tank.  If the schedule’s value is 0.0, then the use side is not available and flow will not be requested.  If the schedule’s value is not equal to 0.0 (usually 1 is used), then the use side is available. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Use Side Inlet Height
-
-The height of the use side inlet to the tank. If blank, the inlet defaults to the top of the tank. The inlet height cannot be higher than the tank height.
-
-#### Field: Use Side Outlet Height
-
-The height of the use side outlet from the tank. If blank or **autocalculate**, the inlet defaults to the bottom of the tank. The outlet height cannot be higher than the tank height.
-
-#### Field: Use Side Design Flow Rate
-
-This field is used to specify the design flow rate through the Use Side of the water tank.  The volumetric design flow rate is specified in m<sup>3</sup>/s.  The field is needed when the Use Side is connected to a plant loop.  The field can be autosized.  If autosized, then the input file should include a Plant Sizing object for the plant loop.  Sizing results are reported in the EIO file.
-
-#### Field: Source Side Inlet Node Name
-
-The inlet node connection to the plant loop for the source side of the chilled water storage tank. Typically the source side draws somewhat warm water from the tank and returns colder water.  The source side volume flow rate is obtained from the plant loop.  The magnitude of the flow rates through the source side can be controlled by setting the Maximum Branch Flow Rate field in the BRANCH object that connects the source inlet node.
-
-#### Field: Source Side Outlet Node Name
-
-The outlet node connection to the plant loop for the source side of the chilled water storage tank. Typically the source side draws somewhat warm water from the tank and returns colder water.
-
-#### Field: Source Side Heat Transfer Effectiveness
-
-This field specifies the heat transfer effectiveness between the source side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the source side water and the tank water. If the effectiveness is less than 1.0, then the source side outlet water temperature will be less than the tank water at the outlet node, simulating a heat exchanger.
-
-#### Field: Source Side Availability Schedule Name
-
-This field contains the name of an availability schedule for the source side of the water tank.  If the schedule’s value is 0.0, then the source side is not available and flow will not be requested. If the schedule’s value is not equal to 0.0 (usually 1 is used), then the source side is available. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Source Side Inlet Height
-
-The height of the source side inlet to the tank. If blank or **autocalculate**, the inlet defaults to the bottom of the tank. The inlet height cannot be higher than the tank height.
-
-#### Field: Source Side Outlet Height
-
-The height of the source side outlet from the tank. If blank, the inlet defaults to the top of the tank. The outlet height cannot be higher than the tank height.
-
-#### Field: Source Side Design Flow Rate
-
-This field is optional and is used to specify the design flow rate through the Source Side of the water heater.  The volumetric design flow rate is specified in m<sup>3</sup>/s.  The field is needed when the Source Side is connected to a plant loop.  The field can be autosized.  If autosized, then the input file should include a Plant Sizing object for the plant loop.  Sizing results are reported in the EIO file.
-
-#### Field: Tank Recovery Time
-
-This field is used to autosize the Source Side Design Flow Rate.  The field is used if the previous field is set to autosize and the water tank’s source side is on the demand side of a plant loop.  This the the time, in hours, that the chilled water tank is to be indirectly cooled from 14.4C to 9.0C using the exit temperature of in the associated Plant Sizing object.
-
-#### Field: Inlet Mode
-
-The inlet mode of entering fluid from the use and source sides. There are two options:  “Fixed� or “Seeking.� In *Fixed* mode, the fluid enters at the fixed heights specified above. In *Seeking* mode, the fluid "seeks out" the stratified node that is closest to the inlet temperature and adds all flow to that node. The *Seeking* mode provides maximum stratification.
-
-#### Field: Number of Nodes
-
-The number of stratified nodes in the tank. There must be at least one node. The maximum number of nodes is 10, although this limit can be increased by editing the IDD.
-
-#### Field: Additional Destratification Conductivity
-
-An additional destratification conductivity [W/m-K] is added to the fluid conductivity of water (0.6 W/m-K) to account for vertical conduction effects along the inside of the tank wall, and perhaps other vertical components such as a dip tube pipe or anode rod.
-
-#### Field: Node 1-10 Additional Loss Coefficient
-
-An additional heat gain coefficient [W/K] added to the skin gains for a given node to account for thermal shorting due to pipe penetrations, tank feet, and any other loss effects.
-
-
-
-An example input object follows.
-
-```idf
-  ThermalStorage:ChilledWater:Stratified,
-    Chilled Water Storage Tank 1 ,  !- Name
-    4.0  ,                          !- Tank Volume
-    2.0 ,                           !- Tank Height
-    VerticalCylinder,               !- Tank Shape
-     ,                              !- Tank Perimeter
-    CW-Tank-Temp-Schedule ,         !- Setpoint Temperature Schedule Name
-    3.5 ,                           !- Deadband Temperature Difference
-    1.4 ,                           !- Temperature Sensor Height
-    1.0 ,                           !- Minimum Temperature Limit
-    2500,                           !- Nominal Cooling Capacity
-    Zone,                           !- Ambient Temperature Indicator
-     ,                              !- Ambient Temperature Schedule Name
-    ZN_1_FLR_1_SEC_5 ,              !- Ambient Temperature Zone Name
-     ,                              !- Ambient Temperature OutdoorAir:Node Name
-    4.2,                            !- Uniform Skin Loss Coefficient Per Unit Area To Ambient Temperature
-    CW Tank Discharge Inlet node,   !- Use Side Inlet Node Name
-    CW Tank Discharge Outlet node,  !- Use Side Outlet Node Name
-    1.0,                            !- Use Side Effectiveness
-    ALWAYS_ON,                      !- Use Side Availability Schedule Name
-    1.85 ,                          !- Use Side Inlet Height
-    0.15 ,                          !- Use Side Outlet Height
-    autosize,                       !- Use Side Design Flow Rate
-    CW Tank Charge Inlet Node,      !- Source Side Inlet Node Name
-    CW Tank Charge Outlet Node,     !- Source Side Outlet Node Name
-    1.0,                            !- Source Side Effectiveness
-    TES Charge Schedule,            !- Source Side Availability Schedule Name
-    0.15,                           !- Source Side Inlet Height
-    1.85,                           !- Source Side Outlet Height
-    autosize,                       !- Source Side Design Flow Rate
-    2.0,                            !- Tank Recovery Time
-    Seeking,                        !- Inlet Mode
-    6,                              !- Number Of Nodes
-    0.0;                            !- Additional Destratification Conductivity
-```
-
-
-
-
-### Chilled Water Stratified Thermal Storage Outputs
-
-The following output variables are reported for stratified chilled water thermal storage tanks.
-
-* Chilled Water Thermal Storage Tank Temperature                !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Final Tank Temperature          !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Tank Heat Gain Rate                  !- HVAC Average [W]
-
-* Chilled Water Thermal Storage Tank Heat Gain Energy                !- HVAC Sum [J]
-
-* Chilled Water Thermal Storage Use Side Mass Flow Rate              !- HVAC Average [kg/s]
-
-* Chilled Water Thermal Storage Use Side Inlet Temperature      !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Use Side Outlet Temperature     !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Use Side Heat Transfer Rate                   !- HVAC Average [W]
-
-* Chilled Water Thermal Storage Use Side Heat Transfer Energy                 !- HVAC Sum [J]
-
-* Chilled Water Thermal Storage Source Side Mass Flow Rate           !- HVAC Average [kg/s]
-
-* Chilled Water Thermal Storage Source Side Inlet Temperature   !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Source Side Outlet Temperature  !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Source Side Heat Transfer Rate                !- HVAC Average [W]
-
-* Chilled Water Thermal Storage Source Side Heat Transfer Energy              !- HVAC Sum [J]
-
-* Chilled Water Thermal Storage Temperature Node &lt;1 - 10&gt;        !- HVAC Average [C]
-
-* Chilled Water Thermal Storage Final Temperature Node &lt;1 – 10&gt; !- HVAC Average [C]
-
-
-#### Chilled Water Thermal Storage Tank Temperature [C]
-
-The average water tank temperature, i.e., the average of all of the node average temperatures.
-
-#### Chilled Water Thermal Storage Tank Final Temperature [C]
-
-The final water tank temperature at the end of the system timestep, i.e., the average of all of the final node temperatures at the end of the system timestep.  If reported at the "Detailed" interval, this output variable can be used to verify an exact energy balance on the water storage tank.
-
-#### Chilled Water Thermal Storage Tank Heat Gain Rate [W]
-
-The average heat exchange rate to the storage tank from the surrounding ambient.  This is usually positive with surrounding ambient heating the storage tank.
-
-#### Chilled Water Thermal Storage Tank Heat Gain Energy [J]
-
-The energy exchange to the storage tank from the surrounding ambient.  This is usually positive with surrounding ambient heating the storage tank.
-
-#### Chilled Water Thermal Storage Use Side Mass Flow Rate [kg/s]
-
-The use side mass flow rate.
-
-#### Chilled Water Thermal Storage Use Side Inlet Temperature [C]
-
-The inlet temperature on the use side.
-
-#### Chilled Water Thermal Storage Use Side Outlet Temperature [C]
-
-The outlet temperature on the use side.
-
-#### Chilled Water Thermal Storage Use Side Heat Transfer Rate [W]
-
-The average heat transfer rate between the use side water and the tank water.
-
-#### Chilled Water Thermal Storage Use Side Heat Transfer Energy [J]
-
-The heat transfer energy between the use side water and the tank water.
-
-#### Chilled Water Thermal Storage Source Side Mass Flow Rate [kg/s]
-
-The source side mass flow rate.
-
-#### Chilled Water Thermal Storage Source Side Inlet Temperature [C]
-
-The inlet temperature on the source side.
-
-#### Chilled Water Thermal Storage Source Side Outlet Temperature [C]
-
-The outlet temperature on the source side.
-
-#### Chilled Water Thermal Storage Source Side Heat Transfer Rate [W]
-
-The average heat transfer rate between the source side water and the tank water.
-
-#### Chilled Water Thermal Storage Source Side Heat Transfer Energy [J]
-
-The heat transfer energy between the source side water and the tank water.
-
-#### Chilled Water Thermal Storage Temperature Node  1-10 [C]
-
-The average node temperature.
-
-#### Chilled Water Thermal Storage Final Temperature Node 1-10  [C]
-
-The final node temperature at the end of the system timestep.
-
-Group – Water Heaters
----------------------
-
-Water heater objects are components for storing and heating water. They can be coupled to a plant loop simulation or used stand-alone. Typical water heater applications are for domestic hot water heating, low-temperature radiant space heating, and energy storage for solar hot water systems or waste heat recovery.
-
-When coupled to the plant loop, the water heater has an inlet node and outlet node on the "source side" and an inlet node and outlet node on the "use side". The source side typically draws cold water from the tank and returns warmer water, for instance, from solar hot water systems or waste heat recovery systems. The use side typically draws hot water from the tank and returns cooler water from the cold water supply mains or from the outlet of a heating system. The distinction between source and use sides is merely a convenience for reporting. They can actually be used interchangeably. If so desired, either source side or use side can be used by itself, without the other side being connected to the plant loop.
-
-However, for a water heater that is indirectly heated (e.g. with a separate boiler), the source side can be used to provide remotely heated water to the tank.  The source side is configured to operate as a component on the demand side of a plant loop.  The design flow rate through the source side can be set by the user or autosized.  If autosized, then a Plant Sizing object is needed elsewhere in the input file for the Plant Loop serving the source side.  The water heater input includes an additional design parameter that describes how rapidly the tank can recover.
-
-![WHFig](media/image191.png)
-
-Figure 80. Water Heater Configuration
-
-If the use side only consists of domestic hot water usage, a simple scheduled use flow rate can be specified in lieu of the full plant loop connections. The scheduled use flow rate can be used simultaneously with source side plant connections, but cannot be used with use side plant connections.
-
-For stand-alone operation, there are no node connections to the plant loop on either source or use sides. The scheduled use flow rate determines all fluid exchange with the water tank.
-
-There are currently two water heater objects in EnergyPlus:
-
-- WaterHeater:Mixed
-
-- WaterHeater:Stratified
-
-There are also compound objects that uses the WaterHeater:Mixed and/or WaterHeater:Stratified as part of their strategy:
-
-- WaterHeater:HeatPump:PumpedCondenser (WaterHeater:Mixed or WaterHeater:Stratified)
-- WaterHeater:HeatPump:WrappedCondenser (WaterHeater:Stratified only)
-
-The WaterHeater:Mixed object simulates a well-mixed, single-node water tank. The WaterHeater:Stratified object simulates a stratified, multi-node water tank. Both water heater objects can be appropriate for simulating many types of water heaters and storage tanks, including gas and electric residential water heaters, and a variety of large commercial water heaters. Both objects share similar features, such as stand-alone operation, on- and off-cycle parasitic loads, and thermal losses to the zone. However, each object has its advantages which may make one water heater object more appropriate than the other depending on the application.
-
-Advantages of **WaterHeater:Mixed**:
-
-- can simulate instantaneous/tankless water heaters
-
-- requires less input than the stratified tank
-
-- faster execution time than the stratified tank
-
-- adequate for modeling gas water heaters with no source connections.
-
-Advantages of **WaterHeater:Stratified**:
-
-- better modeling of electric water heaters with two heating elements
-
-- better modeling of thermal storage applications which rely on stratification to improve heat transfer peformance.
-
-### Standard Ratings
-
-The EIO file reports the industry standard ratings of Recovery Efficiency and Energy Factor for water heater objects. The rating method is based on the GAMA and 10CFR430 test procedures. Under certain input parameters, the rating method will not succeed and a warning message will be generated. Problems occur when inputs do not allow the tank to recover to the setpoint temperature within the test period. This can occur if the maximum heater capacity is undersized, or if the deadband temperature difference is large enough that the first draw of the test does not trigger the heater to come on. In either case, the Recovery Efficiency test will not compute properly because recovery to the setpoint was not achieved.
-
-Standard ratings for storage-only water tanks (Heater Maximum Capacity = 0) cannot be calculated and do not report anything in the EIO file.
-
-### WaterHeater:Mixed
-
-The WaterHeater:Mixed object analytically solves the differential equation governing the energy balance of the water tank. Within a timestep, conditions are solved separately for when the heater element or burner is "on" (on-cycle) and when it is "off" (off-cycle). This approach allows ambient losses and parasitic loads to be divided into on-cycle and off-cycle effects and accounted for in detail.
-
-For losses to the ambient environment, the ambient air temperature can be taken from a schedule, a zone, or the exterior. When used with a zone, a fraction of the skin losses can be added to the zone heat balance as internal heat gains.
-
-Control options allow the heater to cycle or modulate to meet the load. When cycling, the heater element or burner is either on or off. The heater remains fully on while heating the tank up to the setpoint temperature. When the setpoint is reached, the heater turns off. The heater remains off until the tank temperature falls below the "cut-in" temperature, i.e., the setpoint temperature minus the deadband temperature difference. The heater continuously cycles on and off to maintain the tank temperature within the deadband. Most storage-tank water heaters cycle.
-
-When modulating, the heater power varies between the maximum and minimum heater capacities. The heater stays on as long as the required total demand is above the minimum capacity. Below the minimum capacity, the heater will begin to cycle on and off based on the deadband temperature difference. Equipment is usually designed and rated to avoid this condition. Most tankless/instantaneous water heaters modulate.
-
-#### Field: Name
-
-The name of the WaterHeater:Mixed object.
-
-#### Field: Tank Volume
-
-The volume of the storage tank [m<sup>3</sup>].  This field is autosizable if used with a Water Heater:Sizing object.  Although this field is allowed to go down to zero, even so-called "tankless" water heaters have some volume of water that is maintained around the heating elements or in the heat exchanger, typically around 0.00379 m<sup>3</sup> (1 gallon).
-
-#### Field: Setpoint Temperature Schedule Name
-
-The reference to the schedule object specifying the hot water temperature setpoint [°C]. Also known as the "cut-out" temperature.
-
-#### Field: Deadband Temperature Difference
-
-The delta temperature difference [Δ°C] between the setpoint and the "cut-in" temperature at which the heater will turn on. In other words, the "cut-in" temperature is Setpoint – Deadband.
-
-#### Field: Maximum Temperature Limit
-
-The temperature [°C] at which the tank water becomes dangerously hot and is vented through boiling or an automatic safety. The tank temperature will never exceed the maximum. Any extra heat added to the tank is immediately vented. Note:  The maximum temperature must be greater than the setpoint temperature at all times.
-
-#### Field: Heater Control Type
-
-The control type can be **Cycle** or **Modulate**. Cycle is appropriate for most storage tank-type water heaters. Modulate is appropriate for most instantaneous/tankless water heaters.
-
-#### Field: Heater Maximum Capacity
-
-The maximum heat rate [W] that can be supplied to the water, probably the same as the "nominal" capacity.  This field is autosizable if used with a Water Heater:Sizing object.
-
-#### Field: Heater Minimum Capacity
-
-The minimum heat rate [W] that can be supplied to the water. This field is only used when the Heater Control Type is **Modulate**. If the total demand rate for heating is less than the minimum, even a modulating water heater will begin to cycle.
-
-#### Field: Heater Ignition Minimum Flow Rate
-
-NOT YET IMPLEMENTED.
-
-#### Field: Heater Ignition Delay
-
-NOT YET IMPLEMENTED.
-
-#### Field: Heater Fuel Type
-
-The type of fuel used for heating. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating.
-
-#### Field: Heater Thermal Efficiency
-
-The thermal conversion efficiency from fuel energy to heat energy for the heater element or burner. This is not the same as the overall efficiency of the water heater.
-
-#### Field: Part Load Factor Curve Name
-
-The reference to the curve object that relates the overall efficiency of the water heater to the Runtime Fraction (if Control Type **Cycle**) or Part Load Ratio (if Control Type **Modulate**). This is an additional multiplier applied to the Heater Thermal Efficiency to compute fuel energy use. The Part Load Factor Curve should not have a value less than 0.1 in the domain from 0 to 1. If the Part Load Factor Curve accounts for ambient losses and/or parasitic fuel consumption, these effects should not also be input into the related fields in this object as that would result in double-counting.
-
-#### Field: Off-Cycle Parasitic Fuel Consumption Rate
-
-Off-cycle parasitics include parts of the water heater that consume fuel when the heater is off, for example, a pilot light, or stand-by electronic control circuits. The fuel consumption rate [W] is strictly the total fuel that is consumed by all of the off-cycle parasitics.
-
-#### Field: Off-Cycle Parasitic Fuel Type
-
-The type of fuel used by the off-cycle parasitics. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating. The fuel type can be the same or different from the Heater Fuel Type.
-
-#### Field: Off-Cycle Parasitic Heat Fraction to Tank
-
-The fraction of off-cycle parasitic fuel energy that is converted to heat energy that ends up in the tank water. For example, a pilot light would deliver most of its heat to the tank water, as long as the thermal conversion efficiency must be taken into account, so perhaps 0.80 is reasonable. Electronic control circuits, on the other hand, do not add any heat to the tank and should be 0.
-
-#### Field: On-Cycle Parasitic Fuel Consumption Rate
-
-On-cycle parasitics include parts of the water heater that consume fuel when the heater is on, for example, an induction fan, or stand-by electronic control circuits. The fuel consumption rate [W] is strictly the total fuel that is consumed by all of the on-cycle parasitics.
-
-#### Field: On-Cycle Parasitic Fuel Type
-
-The type of fuel used by the on-cycle parasitics. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating. The fuel type can be the same or different from the Heater Fuel Type.
-
-#### Field: On-Cycle Parasitic Heat Fraction to Tank
-
-The fraction of on-cycle parasitic fuel energy that is converted to heat energy that ends up in the tank water. For example, an induction fan might (maybe) deliver a small fraction of its energy to the tank water for a value of 0.05. Electronic control circuits, on the other hand, do not add any heat to the tank and should be 0.
-
-#### Field: Ambient Temperature Indicator
-
-The Ambient Temperature Indicator specifies how the ambient air temperature will be indicated. The field can be **Schedule**, **Zone**, or **Outdoors**. If **Schedule** is used, the Ambient Temperature Schedule field provides the ambient temperature. If **Zone** is used, the zone air temperature of the zone specified in the Ambient Temperature Zone field provides the ambient temperature. If **Outdoors** is used, the outdoor dry-bulb air temperature provides the ambient temperature.
-
-#### Field: Ambient Temperature Schedule Name
-
-The reference to the schedule object specifying the ambient air temperature around the tank for skin losses. This field is only used if Ambient Temperature Indicator is **Schedule**.
-
-#### Field: Ambient Temperature Zone Name
-
-The reference to the zone object specifying the ambient air temperature around the tank for skin losses. This field is only used if Ambient Temperature Indicator is **Zone**.
-
-#### Field: Ambient Temperature Outdoor Air Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the ambient conditions surrounding the water heater tank. This field is applicable only when the Ambient Temperature Indicator is specified as **Outdoors**, otherwise this field should be left blank. The node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-#### Field: Off-Cycle Loss Coefficient to Ambient Temperature
-
-The loss coefficient [W/K] to the ambient air temperature. Often this coefficient is identical to the "UA" for skin losses. However, it can also be used to model the loss effects of the flue in a combustion water heater, in addition to the skin losses.
-
-#### Field: Off-Cycle Loss Fraction to Zone
-
-If the Ambient Temperature Indicator is **Zone**, this field adds the specified fraction of the off-cycle losses to the zone heat balance as an internal gain.
-
-#### Field: On-Cycle Loss Coefficient to Ambient Temperature
-
-The loss coefficient [W/K] to the ambient air temperature. Often this coefficient is identical to the "UA" for skin losses. If the loss effects of the flue are being modeled in the Off-Cycle Loss Coefficient, than this field would have a different value accounting only for the skin losses.
-
-#### Field: On-Cycle Loss Fraction to Zone
-
-If the Ambient Temperature Indicator is **Zone**, this field adds the specified fraction of the on-cycle losses to the zone heat balance as an internal gain.
-
-#### Field: Peak Use Flow Rate
-
-The peak flow rate [m<sup>3</sup>/s] of domestic hot water usage for stand-alone operation, i.e., without plant loop node connections. The peak value is multiplied by the Use Flow Rate Fraction Schedule. If there are node connections, this field is not used.
-
-#### Field: Use Flow Rate Fraction Schedule Name
-
-The reference to the schedule object specifiying the current fraction of Peak Volumetric Use Flow Rate of domestic hot water usage for stand-alone operation.
-
-#### Field: Cold Water Supply Temperature Schedule Name
-
-The reference to the schedule object specifying the cold water temperature [°C] from the supply mains that makes up for the hot water lost down the drain. If blank, water temperatures are calculated by the Site:WaterMainsTemperature object. This field is for stand-alone operation only. If there are node connections, this field is not used.
-
-#### Field: Use Side Inlet Node Name
-
-The inlet node connection to the plant loop for the use side of the water heater. Typically the use side draws hot water from the tank and returns cooler water.
-
-#### Field: Use Side Outlet Node Name
-
-The outlet node connection to the plant loop for the use side of the water heater. Typically the use side draws hot water from the tank and returns cooler water.
-
-#### Field: Use Side Effectiveness
-
-This field specifies the heat transfer effectiveness between the use side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the use side water and the tank water. If the effectiveness is lower, then the use side outlet water temperature will not be as hot as the tank water, simulating a heat exchanger.
-
-#### Field: Source Side Inlet Node Name
-
-The inlet node connection to the plant loop for the source side of the water heater. Typically the source side draws cold water from the tank and returns warmer water.  The source side volume flow rate is obtained from the plant loop.  The magnitude of the flow rates through the source side can be controlled by setting the Maximum Branch Flow Rate field in the **Branch** object that connects the source inlet node.
-
-#### Field: Source Side Outlet Node Name
-
-The outlet node connection to the plant loop for the source side of the water heater. Typically the source side draws cold water from the tank and returns warmer water.
-
-#### Field: Source Side Effectiveness
-
-This field specifies the heat transfer effectiveness between the source side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the source side water and the tank water. If the effectiveness is lower, then the source side outlet water temperature will not be as hot as the tank water, simulating a heat exchanger.
-
-#### Field: Use Side Design Flow Rate
-
-This field is optional and is used to specify the design flow rate through the Use Side of the water heater.  The volumetric design flow rate is specified in m<sup>3</sup>/s.  The field is needed when the Use Side is connected to a plant loop.  The field can be autosized.  If autosized, then the input file should include a Plant Sizing object for the plant loop.  Sizing results are reported in the EIO file.
-
-#### Field: Source Side Design Flow Rate
-
-This field is optional and is used to specify the design flow rate through the Source Side of the water heater.  The volumetric design flow rate is specified in m<sup>3</sup>/s.  The field is needed when the Source Side is connected to a plant loop.  The field can be autosized.  If autosized, then the input file should include a Plant Sizing object for the plant loop.  Sizing results are reported in the EIO file.
-
-#### Field: Indirect Water Heating Recovery Time
-
-This field is optional and is used to provide a design parameter for autosizing design flow rates when the water heater is connected to the demand side of a plant loop.  The recovery time is expressed in hours.  This is the time that the entire volume of the tank can be heated from 14.4ºC to 57.2ºC (58ºF to 135ºF) with an inlet temperature defined as the exit temperature in the associated Plant Sizing object.  The default is 1.5 hours.  The calculation is based on log-mean temperature difference (LMTD) and includes the heat transfer effectiveness factor entered above.
-
-#### Field: Source Side Flow Control Mode
-
-This field is optional and is used to provide control over the logic used by the source side of the water heater to request flow. There are three choices for different modes: IndirectHeatPrimarySetpoint, IndirectHeatAlternateSetpoint, or StorageTank.    The mode called IndirectHeatPrimarySetpoint is the historical behavior prior to version 8.1.  In this mode the water heater will request flow at the source side when the main setpoint, in the input field called Setpoint Temperature Schedule Name, and deadband call for the tank to be heated.  This mode is typical for a water heater indirectly heated by a boiler.  The mode called IndirectHeatAlternateSetpoint is similar but it bases its control decisions on an alternate setpoint given in the following field.  This mode is useful when the indirect source of heat may not satisfy the load and an internal heater is used for backup.  The mode called StorageTank is for a passive tank and it always requests flow unless the tank temperature is equal to or higher than the maximum limit given in the input field called Maximum Temperature Limit.
-
-#### Field: Indirect Alternate Setpoint Temperature Schedule Name
-
-This field is optional and is used to provide a schedule with alternate setpoints for use with the IndirectHeatAlternateSetpoint mode in the previous field.  The input field should contain a reference to a schedule object specifying the hot water temperature setpoint [°C] to use as the "cut-out" temperature for control logic at the source side.
-
-
-
-```idf
-WaterHeater:Mixed,                     ! Stand-alone electric, outdoor example
-    Outdoor Electric Tank,  !- Name
-    0.151,  !- Tank Volume {m3}
-    Hot Water Setpoint Temp Schedule,  !- Setpoint Temperature Schedule
-    2.0,  !- Deadband Temperature Difference {deltaC}
-    82.2222,  !- Maximum Temperature Limit {C}
-    Cycle,  !- Heater Control Type {Cycle | Modulate}
-    11712,  !- Heater Maximum Capacity {W}
-    ,  !- Heater Minimum Capacity {W}
-    ,  !- Heater Ignition Minimum Flow Rate {m3/s}
-    ,  !- Heater Ignition Delay {s}
-    ELECTRICITY,  !- Heater Fuel Type
-    0.95,  !- Heater Thermal Efficiency
-    ,  !- Part Load Factor Curve
-    15,  !- Off-Cycle Parasitic Fuel Consumption Rate {W}
-    ELECTRICITY,  !- Off-Cycle Parasitic Fuel Type
-    0,  !- Off-Cycle Parasitic Heat Fraction To Tank
-    15,  !- On-Cycle Parasitic Fuel Consumption Rate {W}
-    ELECTRICITY,  !- On-Cycle Parasitic Fuel Type
-    0,  !- On-Cycle Parasitic Heat Fraction To Tank
-    Outdoors,  !- Ambient Temperature Indicator {Schedule | Zone | Outdoors}
-    ,  !- Ambient Temperature Schedule
-    ,  !- Ambient Temperature Zone
-    2.36,  !- Off-Cycle Loss Coefficient To Ambient Temperature {W/K}
-    ,  !- Off-Cycle Loss Fraction To Zone
-    2.36,  !- On-Cycle Loss Coefficient To Ambient Temperature {W/K}
-    ,  !- On-Cycle Loss Fraction To Zone
-    0.000379,  !- Peak Volumetric Use Flow Rate {m3/s}
-    Hot Water Demand Schedule,  !- Use Flow Rate Fraction Schedule
-    Constant Mains Temp Schedule;  !- Cold Water Supply Temperature Schedule
-
-
-
-
-WaterHeater:Mixed,                     ! Stand-alone electric, tankless example
-    Tankless,  !- Name
-    0.003785,  !- Tank Volume {m3}
-    Hot Water Setpoint Temp Schedule,  !- Setpoint Temperature Schedule
-    ,  !- Deadband Temperature Difference {deltaC}
-    82.2222,  !- Maximum Temperature Limit {C}
-    Modulate,  !- Heater Control Type {Cycle | Modulate}
-    11712,  !- Heater Maximum Capacity {W}
-    0,  !- Heater Minimum Capacity {W}
-    ,  !- Heater Ignition Minimum Flow Rate {m3/s}
-    ,  !- Heater Ignition Delay {s}
-    ELECTRICITY,  !- Heater Fuel Type
-    0.95,  !- Heater Thermal Efficiency
-    ,  !- Part Load Factor Curve
-    10,  !- Off-Cycle Parasitic Fuel Consumption Rate {W}
-    ELECTRICITY,  !- Off-Cycle Parasitic Fuel Type
-    0,  !- Off-Cycle Parasitic Heat Fraction To Tank
-    30,  !- On-Cycle Parasitic Fuel Consumption Rate {W}
-    ELECTRICITY,  !- On-Cycle Parasitic Fuel Type
-    0,  !- On-Cycle Parasitic Heat Fraction To Tank
-    Schedule,  !- Ambient Temperature Indicator {Schedule | Zone | Outdoors}
-    Hot Water Ambient Temp Schedule,  !- Ambient Temperature Schedule
-    ,  !- Ambient Temperature Zone
-    ,  !- Off-Cycle Loss Coefficient To Ambient Temperature {W/K}
-    ,  !- Off-Cycle Loss Fraction To Zone
-    ,  !- On-Cycle Loss Coefficient To Ambient Temperature {W/K}
-    ,  !- On-Cycle Loss Fraction To Zone
-    0.000379,  !- Peak Volumetric Use Flow Rate {m3/s}
-    Hot Water Demand Schedule,  !- Use Flow Rate Fraction Schedule
-    ;  !- Cold Water Supply Temperature Schedule
-
-
-  WaterHeater:Mixed,                     ! Plant loop connected, gas example
-    Water Heater,  !- Name
-    0.454,  !- Tank Volume {m3}
-    Hot Water Setpoint Temp Schedule,  !- Setpoint Temperature Schedule
-    5.0,  !- Deadband Temperature Difference {deltaC}
-    82.2222,  !- Maximum Temperature Limit {C}
-    Cycle,  !- Heater Control Type {Cycle | Modulate}
-    2000,  !- Heater Maximum Capacity {W}
-    ,  !- Heater Minimum Capacity {W}
-    ,  !- Heater Ignition Minimum Flow Rate {m3/s}
-    ,  !- Heater Ignition Delay {s}
-    NATURALGAS,  !- Heater Fuel Type
-    0.80,  !- Heater Thermal Efficiency
-    ,  !- Part Load Factor Curve
-    ,  !- Off-Cycle Parasitic Fuel Consumption Rate {W}
-    ,  !- Off-Cycle Parasitic Fuel Type
-    ,  !- Off-Cycle Parasitic Heat Fraction To Tank
-    ,  !- On-Cycle Parasitic Fuel Consumption Rate {W}
-    ,  !- On-Cycle Parasitic Fuel Type
-    ,  !- On-Cycle Parasitic Heat Fraction To Tank
-    Schedule,  !- Ambient Temperature Indicator {Schedule | Zone | Outdoors}
-    Hot Water Ambient Temp Schedule,  !- Ambient Temperature Schedule
-    ,  !- Ambient Temperature Zone
-    5.0,  !- Off-Cycle Loss Coefficient To Ambient Temperature {W/K}
-    ,  !- Off-Cycle Loss Fraction To Zone
-    5.0,  !- On-Cycle Loss Coefficient To Ambient Temperature {W/K}
-    ,  !- On-Cycle Loss Fraction To Zone
-    ,  !- Peak Volumetric Use Flow Rate {m3/s}
-    ,  !- Use Flow Rate Fraction Schedule
-    ,  !- Cold Water Supply Temperature Schedule
-    Water Heater Use Inlet Node,  !- Use Side Inlet Node
-    Water Heater Use Outlet Node,  !- Use Side Outlet Node
-    1.0,  !- Use Side Effectiveness
-    Water Heater Source Inlet Node,  !- Source Side Inlet Node
-    Water Heater Source Outlet Node,  !- Source Side Outlet Node
-    1.0;  !- Source Side Effectiveness
-
-
-WaterHeater:Mixed,
-    Indirect Water Heater,   !- Name
-    1.00,                    !- Tank Volume {m3}
-    Hot Water Setpoint Temperature Schedule,  !- Setpoint Temperature Schedule
-    5.0,                     !- Deadband Temperature Difference {deltaC}
-    82.2222,                 !- Maximum Temperature Limit {C}
-    Cycle,                   !- Heater Control Type
-    0.0,                     !- Heater Maximum Capacity {W}
-    ,                        !- Heater Minimum Capacity {W}
-    ,                        !- Heater Ignition Minimum Flow Rate {m3/s}
-    ,                        !- Heater Ignition Delay {s}
-    ELECTRICITY,             !- Heater Fuel Type
-    0.8,                     !- Heater Thermal Efficiency
-    ,                        !- Part Load Factor Curve
-    ,                        !- Off-Cycle Parasitic Fuel Consumption Rate {W}
-    ,                        !- Off-Cycle Parasitic Fuel Type
-    ,                        !- Off-Cycle Parasitic Heat Fraction To Tank
-    ,                        !- On-Cycle Parasitic Fuel Consumption Rate {W}
-    ,                        !- On-Cycle Parasitic Fuel Type
-    ,                        !- On-Cycle Parasitic Heat Fraction To Tank
-    Zone,                    !- Ambient Temperature Indicator
-    ,                        !- Ambient Temperature Schedule
-    SPACE5-1,                !- Ambient Temperature Zone
-    ,                        !- Ambient Temperature Outside Air Node
-    5.0,                     !- Off-Cycle Loss Coefficient To Ambient Temperature {W/K}
-    ,                        !- Off-Cycle Loss Fraction To Zone
-    5.0,                     !- On-Cycle Loss Coefficient To Ambient Temperature {W/K}
-    ,                        !- On-Cycle Loss Fraction To Zone
-    ,                        !- Peak Volumetric Use Flow Rate {m3/s}
-    ,                        !- Use Flow Rate Fraction Schedule
-    ,                        !- Cold Water Supply Temperature Schedule
-    SHWSys1 Pump-SHWSys1 Water HeaterNode,  !- Use Side Inlet Node
-    SHWSys1 Supply Equipment Outlet Node,  !- Use Side Outlet Node
-    1.0,                     !- Use Side Effectiveness
-    Indirect Water Heater SrcSideInletNode,  !- Source Side Inlet Node
-    Indirect Water Heater SrcSideOutletNode,  !- Source Side Outlet Node
-    0.9,                     !- Source Side Effectiveness
-    autosize,                !- Use Side Design Flow Rate
-    autosize,                !- Source Side Design Flow Rate
-    1.0;                     !- Indirect Water Heating Recovery Time
-```
-
-
-### Mixed Water Heater Outputs
-
-The following output variables are reported for the WaterHeater:Mixed object:
-
-* HVAC,Average,Water Heater Tank Temperature [C]
-
-* HVAC,Average,Water Heater Final Tank Temperature [C]
-
-* HVAC,Average,Water Heater Heat Loss Rate [W]
-
-* HVAC,Sum,Water Heater Heat Loss Energy [J]
-
-* HVAC,Average, Water Heater Use Side Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water Heater Use Side Inlet Temperature [C]
-
-* HVAC,Average,Water Heater Use Side Outlet Temperature [C]
-
-* HVAC,Average,Water Heater Use Side Heat Transfer Rate [W]
-
-* HVAC,Sum,Water Heater Use Side Heat Transfer Energy [J]
-
-* HVAC,Average,Water Heater Source Side Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water Heater Source Side Inlet Temperature [C]
-
-* HVAC,Average,Water Heater Source Side Outlet Temperature [C]
-
-* HVAC,Average,Water Heater Source Side Heat Transfer Rate [W]
-
-* HVAC,Sum,Water Heater Source Side Heat Transfer Energy [J]
-
-* HVAC,Average,Water Heater Off Cycle Parasitic Tank Heat Transfer Rate [W]
-
-* HVAC,Sum,Water Heater Off Cycle Parasitic Tank Heat Transfer Energy [J]
-
-* HVAC,Average,Water Heater On Cycle Parasitic Tank Heat Transfer Rate [W]
-
-* HVAC,Sum,Water Heater On Cycle Parasitic Tank Heat Transfer Energy [J]
-
-* HVAC,Average,Water Heater Total Demand Heat Transfer Rate [W]
-
-* HVAC,Sum,Water Heater Total Demand Energy [J]
-
-* HVAC,Average,Water Heater Heating Rate [W]
-
-* HVAC,Sum,Water Heater Heating Energy [J]
-
-* HVAC,Average,Water Heater Unmet Demand Heat Transfer Rate [W]
-
-* HVAC,Sum,Water Heater Unmet Demand Heat Transfer Energy [J]
-
-* HVAC,Average,Water Heater Venting Heat Transfer Rate [W]
-
-* HVAC,Sum,Water Heater Venting Heat Transfer Energy [J]
-
-* HVAC,Average,Water Heater Net Heat Transfer Rate [W]
-
-* HVAC,Sum,Water Heater Net Heat Transfer Energy [J]
-
-* HVAC,Sum,Water Heater Cycle On Count []
-
-* HVAC,Average,Water Heater Runtime Fraction []
-
-* HVAC,Average,Water Heater Part Load Ratio []
-
-* HVAC,Average,Water Heater Electric Power [W]
-
-* HVAC,Average,Water Heater &lt;Fuel Type&gt; Rate [W]
-
-* HVAC,Sum,Water Heater &lt;Fuel Type&gt; Energy [J]
-
-* HVAC,Average,Water Heater Off Cycle Parasitic &lt;Fuel Type&gt; Rate [W]
-
-* HVAC,Sum,Water Heater Off Cycle Parasitic &lt;Fuel Type&gt; Energy [J]
-
-* HVAC,Average,Water Heater On Cycle Parasitic &lt;Fuel Type&gt; Rate [W]
-
-* HVAC,Sum,Water Heater On Cycle Parasitic &lt;Fuel Type&gt; Energy [J]
-
-* HVAC,Average,Water Heater Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Water Heater Water Volume [m3]
-
-
-
-#### Water Heater Tank Temperature [C]
-
-The average water tank temperature.
-
-#### Water Heater Final Tank Temperature [C]
-
-The final water tank temperature at the end of the system timestep. If reported at the "Detailed" interval, this output variable can be used to verify an exact energy balance on the water heater. Also see the output variable:  Water Heater Net Heat Transfer Energy.
-
-#### Water Heater Heat Loss Rate [W]
-
-The average heat loss rate due to the off- and on-cycle loss coefficients to the ambient temperature.
-
-#### Water Heater Heat Loss Energy [J]
-
-The heat loss energy due to the off- and on-cycle loss coefficients to the ambient temperature.
-
-#### Water Heater Use Side Mass Flow Rate [kg/s]
-
-The use side mass flow rate. If stand-alone, this is the scheduled use flow rate.
-
-#### Water Heater Use Side Inlet Temperature [C]
-
-The inlet temperature on the use side.
-
-#### Water Heater Use Side Outlet Temperature [C]
-
-The outlet temperature on the use side.
-
-#### Water Heater Use Side Heat Transfer Rate [W]
-
-The average heat transfer rate between the use side water and the tank water.
-
-#### Water Heater Use Side Heat Transfer Energy [J]
-
-The heat transfer energy between the use side water and the tank water.
-
-#### Water Heater Source Side Mass Flow Rate [kg/s]
-
-The source side mass flow rate. If in stand-alone operation, this is 0.
-
-#### Water Heater Source Side Inlet Temperature [C]
-
-The inlet temperature on the source side.
-
-#### Water Heater Source Side Outlet Temperature [C]
-
-The outlet temperature on the source side.
-
-#### Water Heater Source Side Heat Transfer Rate [W]
-
-The average heat transfer rate between the source side water and the tank water.
-
-#### Water Heater Source Side Heat Transfer Energy [J]
-
-The heat transfer energy between the source side water and the tank water.
-
-#### Water Heater Off Cycle Parasitic Tank Heat Transfer Rate [W]
-
-The average heat gain rate to the tank water due to off-cycle parasitics.
-
-#### Water Heater Off Cycle Parasitic Tank Heat Transfer Energy [J]
-
-The heat gain energy to the tank water due to off-cycle parasitics.
-
-#### Water Heater On Cycle Parasitic Tank Heat Transfer Rate [W]
-
-The average heat gain rate to the tank water due to on-cycle parasitics.
-
-#### Water Heater On Cycle Parasitic Tank Heat Transfer Energy [J]
-
-The heat gain energy to the tank water due to on-cycle parasitics.
-
-#### Water Heater Total Demand Heat Transfer Rate [W]
-
-The average heating rate demanded to maintain the setpoint temperature.
-
-#### Water Heater Total Demand Energy [J]
-
-The heating energy demanded to maintain the setpoint temperature.
-
-#### Water Heater Heating Rate [W]
-
-The average heating rate supplied by the heater element or burner.
-
-#### Water Heater Heating Energy [J]
-
-The heating energy supplied by the heater element or burner.
-
-#### Water Heater Unmet Demand Heat Transfer Rate [W]
-
-The average heating rate unmet by the heater element or burner. The difference between the Total Demand Rate and the Heating Rate.
-
-#### Water Heater Unmet Demand Heat Transfer Energy [J]
-
-The heating energy unmet by the heater element or burner. The difference between the Total Demand Energy and the Heating Energy.
-
-#### Water Heater Venting Heat Transfer Rate [W]
-
-The average venting rate to keep the tank below the Maximum Temperature Limit.
-
-#### Water Heater Venting Heat Transfer Energy [J]
-
-The venting energy to keep the tank below the Maximum Temperature Limit.
-
-#### Water Heater Net Heat Transfer Rate [W]
-
-The average net heat transfer rate when considering all losses and gains.
-
-#### Water Heater Net Heat Transfer Energy [J]
-
-The net heat transfer energy when considering all losses and gains.
-
-#### Water Heater Cycle On Count []
-
-The number of times that the heater turned on in the time period.
-
-#### Water Heater Runtime Fraction []
-
-The fraction of the time period that the heater was running.
-
-#### Water Heater Part Load Ratio []
-
-The fraction of the Heater Maximum Capacity.
-
-#### Water Heater &lt;Fuel Type&gt; Rate [W]
-
-#### Water Heater Electric Power [W]
-
-The average fuel consumption rate for the heater element or burner.
-
-#### Water Heater &lt;Fuel Type&gt; Energy [J]
-
-The fuel consumption energy for the heater element or burner.
-
-#### Water Heater Off Cycle Parasitic &lt;Fuel Type&gt; Rate [W]
-
-#### Water Heater Off Cycle Parasitic Electric Power [W]
-
-The average fuel consumption rate for the off-cycle parasitics.
-
-#### Water Heater Off Cycle Parasitic &lt;Fuel Type&gt; Energy [J]
-
-The fuel consumption energy for the off-cycle parasitics.
-
-#### Water Heater On Cycle Parasitic &lt;Fuel Type&gt; Rate [W]
-
-#### Water Heater On Cycle Parasitic Electric Power [W]
-
-The average fuel consumption rate for the on-cycle parasitics.
-
-#### Water Heater On Cycle Parasitic &lt;Fuel Type&gt; Energy [J]
-
-The fuel consumption energy for the on-cycle parasitics.
-
-#### Water Heater Water Volume Flow Rate [m<sup>3</sup>/s]
-
-The water consumption rate for the use side, if in stand-alone operation.
-
-#### Water Heater Water Volume [m<sup>3</sup>]
-
-The water consumption for the use side, if in stand-alone operation.
-
-#### Water Heater Mains Water Volume [m3]
-
-The volume of water consumption drawn from mains water service.
-
-### WaterHeater:Stratified
-
-The WaterHeater:Stratified object divides the water tank into multiple nodes of equal volume. The nodes are coupled by vertical conduction effects, internode fluid flow, and temperature inversion mixing. The object simultaneously solves the differential equations governing the energy balances on the nodes using a numerical method. The system timestep is divided into many small substeps that allow the simulation to capture events that occur on a very short time scale. This approach allows ambient losses and parasitic loads to be divided into on-cycle and off-cycle effects and accounted for in detail.
-
-For losses to the ambient environment, the ambient air temperature can be taken from a schedule, a zone, or the exterior. When used with a zone, a fraction of the skin losses can be added to the zone heat balance as internal heat gains.
-
-The WaterHeater:Stratified object allows two heating elements to be simulated. The two elements can cycle on and off to maintain the node temperature within the deadband. The Heater Priority Control field determines how the heaters work together. There are two options:  MasterSlave or Simultaneous. In the MasterSlave option, Heater 1 is the master and Heater 2 is the slave. That is, both heaters are not allowed to turn on at the same time. If the thermostats ask for heat at both Heater 1 and 2, only Heater 1 will turn on. Once Heater 1 has met the set point, it turns off and Heater 2 can turn on, if necessary. In the Simultaneousoption, Heater 1 and Heater 2 can turn on and off independently.  Autosizing is available for only Heater 1.
-
-#### Field: Name
-
-The name of the WaterHeater:Stratified object.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Laundry", "Dish Washing", etc. A new meter for reporting is created for each unique subcategory  (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table under the "Water Systems" end-use category. If this field is omitted or blank, the water use will be assigned to the "General" end-use subcategory.
-
-#### Field: Tank Volume
-
-The actual volume [m3] of fluid in the tank. This field is autosizable if used with a Water Heater:Sizing object.  The actual volume is typically not equal to the nominal volume specified by the manufacturer. Actual volume is almost always 10% lower for electric water heaters, and 5% lower for gas water heaters (Burch and Erickson 2004).
-
-Burch, J., and P. Erickson. 2004. "Using Ratings Data to Derive Simulation-Model Inputs for Storage-Tank Water Heaters". *Proceedings of the Solar 2004 Conference, 11-14 July 2004, Portland, Oregon*, American Solar Energy Society (ASES), pp. 393-398.
-
-#### Field: Tank Height
-
-The height [m] of the tank. For the **HorizontalCylinder** shape (see below) the height of the tank is the measure in the axial direction, i.e., the height if you were to stand the cylinder up on its end. This field is autosizable if used with a Water Heater:Sizing object.
-
-#### Field: Tank Shape
-
-The tank shape determines the size and skin losses of the stratified nodes. There are three options:  **VerticalCylinder**, **HorizontalCylinder**, and **Other**.
-
-**VerticalCylinder** describes most upright residential water heaters.
-
-HorizontalCylinder describes a few specialty water heaters and large commercial storage tanks. HorizontalCylinder can also be used to model an outdoor storage tank located above a solar collector in a thermosiphon configuration. HorizontalCylinder implies that the tank is divided into nodes of equal mass, but not equal height.
-
-Other describes water heaters or storage tanks that have a uniform horizontal cross-section, but are not cylinders, e.g., a cuboid or other shape. The length of the perimeter is then specified by the Tank Perimeter field.
-
-If blank, the default shape is **VerticalCylinder**.
-
-#### Field: Tank Perimeter
-
-The length of the tank perimeter [m]. This field is only used if Tank Shape is **Other**.
-
-#### Field: Maximum Temperature Limit
-
-The temperature [°C] at which the tank water becomes dangerously hot and is vented through boiling or an automatic safety. The tank temperature will never exceed the maximum. Any extra heat added to the tank is immediately vented. Note:  The maximum temperature must be greater than the setpoint temperature at all times.
-
-#### Field: Heater Priority Control
-
-The heater priority control determines how Heater 1 and Heater 2 work together. There are two options:  **MasterSlave** or **Simultaneous**. In the MasterSlave option, Heater 1 is the master and Heater 2 is the slave. In most residential electric water heaters, the heaters operate in a MasterSlave relationship. That is, both heaters are not allowed to turn on at the same time. If the thermostats ask for heat at both Heater 1 and 2, only Heater 1 will turn on. Once Heater 1 has met the set point, it turns off and Heater 2 can turn on, if necessary. In other words, only one heater can be on at any time, and Heater 1 is always has priority over Heater 2.
-
-In the Simultaneous option, Heater 1 and Heater 2 can turn on and off independently.
-
-If blank, the default is **MasterSlave**.
-
-#### Field: Heater 1 Set Point Temperature Schedule Name
-
-The reference to the schedule object specifying the hot water temperature set point [°C] for Heater 1. Also known as the "cut-out" temperature.
-
-#### Field: Heater 1 Deadband Temperature Difference
-
-The delta temperature difference [Δ°C] between the set point and the "cut-in" temperature at which Heater 1 will turn on. In other words, the "cut-in" temperature is Set Point – Deadband.
-
-#### Field: Heater 1 Capacity
-
-The heat rate [W] supplied to the water for Heater 1, probably the same as the "nominal" capacity. For residential electric water heaters, heating elements are usually 4500 W.  This field is autosizable if used with a Water Heater:Sizing object.
-
-#### Field: Heater 1 Height
-
-The height [m] of Heater 1 in the tank.
-
-#### Field: Heater 2 Set Point Temperature Schedule Name
-
-The reference to the schedule object specifying the hot water temperature set point [°C] for Heater 2. Also known as the "cut-out" temperature.
-
-#### Field: Heater 2 Deadband Temperature Difference
-
-The delta temperature difference [Δ°C] between the set point and the "cut-in" temperature at which Heater 2 will turn on. In other words, the "cut-in" temperature is Set Point – Deadband.
-
-#### Field: Heater 2 Capacity
-
-The heat rate [W] supplied to the water for Heater 1, probably the same as the "nominal" capacity. For residential electric water heaters, heating elements are usually 4500 W.
-
-#### Field: Heater 2 Height
-
-The height [m] of Heater 2 in the tank.
-
-#### Field: Heater Fuel Type
-
-The type of fuel used for both Heaters 1 and 2. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating.
-
-#### Field: Heater Thermal Efficiency
-
-The thermal conversion efficiency from fuel energy to heat energy for the heater element or burner (for both Heaters 1 and 2). This is not the same as the overall efficiency of the water heater.
-
-#### Field: Off-Cycle Parasitic Fuel Consumption Rate
-
-Off-cycle parasitics include parts of the water heater that consume fuel when the heater is off, for example, a pilot light, or stand-by electronic control circuits. The fuel consumption rate [W] is strictly the total fuel that is consumed by all of the off-cycle parasitics.
-
-#### Field: Off-Cycle Parasitic Fuel Type
-
-The type of fuel used by the off-cycle parasitics. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating. The fuel type can be the same or different from the Heater Fuel Type.
-
-#### Field: Off-Cycle Parasitic Heat Fraction to Tank
-
-The fraction of off-cycle parasitic fuel energy that is converted to heat energy that ends up in the tank water. For example, a pilot light would deliver most of its heat to the tank water, as long as the thermal conversion efficiency must be taken into account, so perhaps 0.80 is reasonable. Electronic control circuits, on the other hand, do not add any heat to the tank and should be 0.
-
-#### Field: Off-Cycle Parasitic Height
-
-The height [m] where any off-cycle parasitic heat gains are added to the tank.
-
-#### Field: On-Cycle Parasitic Fuel Consumption Rate
-
-On-cycle parasitics include parts of the water heater that consume fuel when the heater is on, for example, an induction fan, or stand-by electronic control circuits. The fuel consumption rate [W] is strictly the total fuel that is consumed by all of the on-cycle parasitics.
-
-#### Field: On-Cycle Parasitic Fuel Type
-
-The type of fuel used by the on-cycle parasitics. The fuel type can be Electricity, NaturalGas, PropaneGas, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, Steam, OtherFuel1, OtherFuel2 or DistrictHeating. The fuel type can be the same or different from the Heater Fuel Type.
-
-#### Field: On-Cycle Parasitic Heat Fraction to Tank
-
-The fraction of on-cycle parasitic fuel energy that is converted to heat energy that ends up in the tank water. For example, an induction fan might (maybe) deliver a small fraction of its energy to the tank water for a value of 0.05. Electronic control circuits, on the other hand, do not add any heat to the tank and should be 0.
-
-#### Field: On-Cycle Parasitic Height
-
-The height [m] where any on-cycle parasitic heat gains are added to the tank.
-
-#### Field: Ambient Temperature Indicator
-
-The Ambient Temperature Indicator specifies how the ambient air temperature will be indicated. The field can be **Schedule**, **Zone**, or **Outdoors**. If **Schedule** is used, the Ambient Temperature Schedule value provides the ambient temperature. If **Zone** is used, the zone air temperature of the zone specified in the Ambient Temperature Zone field provides the ambient temperature. If **Outdoors** is used, the outdoor dry-bulb air temperature of the outdoor air node specified in the Ambient Temperature OutdoorAir:Node field provides the ambient temperature.
-
-#### Field: Ambient Temperature Schedule Name
-
-The reference to the schedule object specifying the ambient air temperature around the tank for skin losses. This field is only used if Ambient Temperature Indicator is **Schedule**.
-
-#### Field: Ambient Temperature Zone
-
-The reference to the zone object specifying the ambient air temperature around the tank for skin losses. This field is only used if Ambient Temperature Indicator is **Zone**.
-
-#### Field: Ambient Temperature Outdoor Air Node
-
-The reference to the outdoor air node specifying the ambient air temperature around the tank for skin losses. An outdoor air node can be defined by an OutdoorAir:Node object or OutdoorAir:NodeList object. This field is only used if Ambient Temperature Indicator is **Outdoors**.
-
-#### Field: Uniform Skin Loss Coefficient Per Unit Area to Ambient Temperature
-
-The uniform skin loss coefficient [W/m2-K] or U-Value of the tank to the ambient air temperature. The uniform skin loss accounts for the tank insulation and applies during both off- and on-cycle operation. The overall losses at any particular node can be further modified using the Additional Loss Coefficient fields to account for thermal shorting due to pipe penetrations, water heater feet, and any other loss effects.
-
-#### Field: Skin Loss Fraction to Zone
-
-If the Ambient Temperature Indicator is **Zone**, this field adds the specified fraction of the skin losses to the zone heat balance as an internal gain.
-
-#### Field: Off-Cycle Flue Loss Coefficient to Ambient Temperature
-
-The off-cycle flue loss coefficient [W/K] to the ambient air temperature. This field mainly applies to gas water heaters that have a flue.
-
-#### Field: Off-Cycle Flue Loss Fraction to Zone
-
-If the Ambient Temperature Indicator is **Zone**, this field adds the specified fraction of the off-cycle flue losses to the zone heat balance as an internal gain.
-
-#### Field: Peak Use Flow Rate
-
-The peak flow rate [m<sup>3</sup>/s] of domestic hot water usage for stand-alone operation, i.e., without plant loop node connections. The peak value is multiplied by the Use Flow Rate Fraction Schedule. If there are node connections, this field is not used.
-
-#### Field: Use Flow Rate Fraction Schedule Name
-
-The reference to the schedule object specifiying the current fraction of Peak Volumetric Use Flow Rate of domestic hot water usage for stand-alone operation. If blank, the fraction defaults to 1.0 at all times.
-
-#### Field: Cold Water Supply Temperature Schedule Name
-
-The reference to the schedule object specifying the cold water temperature [°C] from the supply mains that makes up for the hot water lost down the drain. If blank, water temperatures are calculated by the Site:WaterMainsTemperature object. This field is for stand-alone operation only. If there are node connections, this field is not used.
-
-#### Field: Use Side Inlet Node Name
-
-The inlet node connection to the plant loop for the use side of the water heater. Typically the use side draws hot water from the tank and returns cooler water.
-
-#### Field: Use Side Outlet Node Name
-
-The outlet node connection to the plant loop for the use side of the water heater. Typically the use side draws hot water from the tank and returns cooler water.
-
-#### Field: Use Side Effectiveness
-
-This field specifies the heat transfer effectiveness between the use side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the use side water and the tank water. If the effectiveness is less than 1.0, then the use side outlet water temperature will not be as hot as the tank water at the outlet node, simulating an external heat exchanger that is indirectly coupled to the water heater tank.
-
-#### Field: Use Side Inlet Height
-
-The height of the use side inlet to the tank. If blank, the inlet defaults to the bottom of the tank. The inlet height cannot be higher than the tank height.
-
-#### Field: Use Side Outlet Height
-
-The height of the use side outlet from the tank. If blank or **autocalculate**, the inlet defaults to the top of the tank. The outlet height cannot be higher than the tank height.
-
-#### Field: Source Side Inlet Node
-
-The inlet node connection to the plant loop for the source side of the water heater. Typically the source side draws cold water from the tank and returns warmer water.
-
-#### Field: Source Side Outlet Node
-
-The outlet node connection to the plant loop for the source side of the water heater. Typically the source side draws cold water from the tank and returns warmer water.
-
-#### Field: Source Side Effectiveness
-
-This field specifies the heat transfer effectiveness between the source side water and the tank water. If the effectiveness is set to 1 then complete heat transfer occurs, simulating perfect mixing of the source side water and the tank water. If the effectiveness is less than 1.0, then the source side outlet water temperature will be higher than the tank water at the outlet node, simulating an external heat exchanger that is indirectly coupled to the water heater tank.
-
-#### Field: Source Side Inlet Height
-
-The height of the source side inlet to the tank. If blank or **autocalculate**, the inlet defaults to the top of the tank. The inlet height cannot be higher than the tank height.
-
-#### Field: Source Side Outlet Height
-
-The height of the source side outlet from the tank. If blank, the inlet defaults to the bottom of the tank. The outlet height cannot be higher than the tank height.
-
-#### Field: Inlet Mode
-
-The inlet mode of entering fluid from the use and source sides. There are two options:  **Fixed** or **Seeking**. In Fixed mode, the fluid enters at the fixed heights specified above. In Seeking mode, the fluid "seeks out" the stratified node that is closest to the inlet temperature and adds all flow to that node. The Seekingbmode provides maximum stratification. The default is **Fixed**.
-
-#### Field: Use Side Design Flow Rate
-
-This field is optional and is used to specify the design flow rate through the Use Side of the water heater.  The volumetric design flow rate is specified in m<sup>3</sup>/s.  The field is needed when the Use Side is connected to a plant loop.  The field can be autosized.  If autosized, then the input file should include a Plant Sizing object for the plant loop.  Sizing results are reported in the EIO file.
-
-#### Field: Source Side Design Flow Rate
-
-This field is optional and is used to specify the design flow rate through the Source Side of the water heater.  The volumetric design flow rate is specified in m<sup>3</sup>/s.  The field is needed when the Source Side is connected to a plant loop.  The field can be autosized.  If autosized, then the input file should include a Plant Sizing object for the plant loop.  Sizing results are reported in the EIO file.
-
-#### Field: Indirect Water Heating Recovery Time
-
-This field is optional and is used to provide a design parameter for autosizing design flow rates when the water heater is connected to the demand side of a plant loop.  The recovery time is expressed in hours.  This is the time that the entire volume of the tank can be heated from 14.4ºC to 57.2ºC (58ºF to 135ºF) with an inlet temperature defined as the exit temperature in the associated Plant Sizing object.  The default is 1.5 hours.  The calculation is based on log-mean temperature difference (LMTD) and includes the heat transfer effectiveness factor entered above.
-
-#### Field: Number Of Nodes
-
-The number of stratified nodes in the tank. There must be at least one node. The maximum number of nodes is 12, although this limit can be increased by editing the IDD.
-
-#### Field: Additional Destratification Conductivity
-
-An additional destratification conductivity [W/m-K] is added to the fluid conductivity of water (0.6 W/m-K) to account for vertical conduction effects along the inside of the tank wall, and perhaps other vertical components such as the flue, the cold water inlet pipe (dip tube), and the anode rod.
-
-#### Field: Node 1-12 Additional Loss Coefficient
-
-An additional loss coefficient [W/K] added to the skin losses for a given node to account for thermal shorting due to pipe penetrations, water heater feet, and any other loss effects.
-
-#### Field: Source Side Flow Control Mode
-
-This field is optional and is used to provide control over the logic used by the source side of the water heater to request flow. There are three choices for different modes: IndirectHeatPrimarySetpoint, IndirectHeatAlternateSetpoint, or StorageTank.    The mode called IndirectHeatPrimarySetpoint is the historical behavior prior to version 8.1.  In this mode the water heater will request flow at the source side when the main setpoint, in the input field called Setpoint Temperature Schedule Name, and deadband call for the tank to be heated.  This mode is typical for a water heater indirectly heated by a boiler.  The mode called IndirectHeatAlternateSetpoint is similar but it bases its control decisions on an alternate setpoint given in the following field.  This mode is useful when the indirect source of heat may not satisfy the load and an internal heater is used for backup.  The mode called StorageTank is for a passive tank and it always requests flow unless the tank temperature is equal to or higher than the maximum limit given in the input field called Maximum Temperature Limit.
-
-#### Field: Indirect Alternate Setpoint Temperature Schedule Name
-
-This field is optional and is used to provide a schedule with alternate setpoints for use with the IndirectHeatAlternateSetpoint mode in the previous field.  The input field should contain a reference to a schedule object specifying the hot water temperature setpoint [°C] to use as the "cut-out" temperature for control logic at the source side.
-
-
-
-```idf
-WaterHeater:Stratified,
-    Electric Water Heater,  !- Name
-    Water Heater,  !- End-Use Subcategory
-    0.1893,  !- Tank Volume {m3}
-    1.4,  !- Tank Height {m}
-    VerticalCylinder,  !- Tank Shape
-    ,  !- Tank Perimeter {m}
-    82.2222,  !- Maximum Temperature Limit {C}
-    MasterSlave,  !- Heater Priority
-    Hot Water Set Point Temp Schedule,  !- Heater 1 Set Point Temperature Schedule
-    2.0,  !- Heater 1 Deadband Temperature Difference {deltaC}
-    4500,  !- Heater 1 Capacity {W}    (Master)
-    1.0,  !- Heater 1 Height {m}
-    Hot Water Set Point Temp Schedule,  !- Heater 2 Set Point Temperature Schedule
-    5.0,  !- Heater 2 Deadband Temperature Difference {deltaC}
-    4500,  !- Heater 2 Capacity {W}    (Slave)
-    0.0,  !- Heater 2 Height {m}
-    ELECTRICITY,  !- Heater Fuel Type
-    0.98,  !- Heater Thermal Efficiency
-    10,  !- Off-Cycle Parasitic Fuel Consumption Rate {W}
-    ELECTRICITY,  !- Off-Cycle Parasitic Fuel Type
-    0,  !- Off-Cycle Parasitic Heat Fraction To Tank
-    ,  !- Off-Cycle Parasitic Height {m}
-    10,  !- On-Cycle Parasitic Fuel Consumption Rate {W}
-    ELECTRICITY,  !- On-Cycle Parasitic Fuel Type
-    0,  !- On-Cycle Parasitic Heat Fraction To Tank
-    ,  !- On-Cycle Parasitic Height {m}
-    SCHEDULE,  !- Ambient Temperature Indicator
-    Ambient Temp Schedule,  !- Ambient Temperature Schedule
-    ,  !- Ambient Temperature Zone
-    ,  !- Ambient Temperature Outdoor Air Node
-    0.846,  !- Uniform Skin Loss Coefficient Per Unit Area To Ambient Temperature {W/m2-K}
-    ,  !- Skin Loss Fraction To Zone {}
-    ,  !- Off-Cycle Flue Loss Coefficient To Ambient Temperature {W/K}
-    ,  !- Off-Cycle Flue Loss Fraction To Zone {}
-    ,  !- Peak Volumetric Use Flow Rate {m3/s}
-    ,  !- Use Flow Rate Fraction Schedule
-    ,  !- Cold Water Supply Temperature Schedule
-    Water Heater Use Inlet Node,  !- Use Side Inlet Node
-    Water Heater Use Outlet Node,  !- Use Side Outlet Node
-    1.0,  !- Use Side Effectiveness {}
-    ,  !- Use Side Inlet Height {m}
-    ,  !- Use Side Outlet Height {m}
-    ,  !- Source Side Inlet Node
-    ,  !- Source Side Outlet Node
-    ,  !- Source Side Effectiveness {}
-    ,  !- Source Side Inlet Height {m}
-    ,  !- Source Side Outlet Height {m}
-    FIXED,  !- Inlet Mode {FIXED | SEEKING}
-    6,  !- Number Of Nodes
-    0.1,  !- Destratification Conductivity {W/m-K}
-    0.15,  !- Node 1 Additional Loss Coefficient {W/K}
-    ,  !- Node 2 Additional Loss Coefficient {W/K}
-    ,  !- Node 3 Additional Loss Coefficient {W/K}
-    ,  !- Node 4 Additional Loss Coefficient {W/K}
-    ,  !- Node 5 Additional Loss Coefficient {W/K}
-    0.1;  !- Node 6 Additional Loss Coefficient {W/K}
-```
-
-
-
-
-### Stratified Water Heater Outputs
-
-All of the output variables reported for the WaterHeater:Mixed object also apply to the WaterHeater:Stratified object, with several qualifications noted below:
-
-#### Water Heater Tank Temperature [C]
-
-The average water tank temperature, i.e., the average of all of the node average temperatures.
-
-#### Water Heater Final Tank Temperature [C]
-
-The final water tank temperature at the end of the system timestep, i.e., the average of all of the final node temperatures at the end of the system timestep. If reported at the "Detailed" interval, this output variable can be used to verify an exact energy balance on the water heater.
-
-#### Water Heater Heating Rate [W]
-
-The total average heating rate supplied by Heater 1 plus Heater 2.
-
-#### Water Heater Heating Energy [J]
-
-The total heating energy supplied by Heater 1 plus Heater 2.
-
-#### Water Heater Cycle On Count []
-
-The number of times that either Heater 1 or Heater 2 turned on in the time period.
-
-#### Water Heater Runtime Fraction []
-
-The fraction of the time period that either Heater 1 or Heater 2 was running.
-
-In addition, the WaterHeater:Stratified object also reports the following output variables:
-
-* HVAC,Average,Water Heater Heater 1 Heating Rate [W]
-
-* HVAC,Average,Water Heater Heater 2 Heating Rate [W]
-
-* HVAC,Sum,Water Heater Heater 1 Heating Energy [J]
-
-* HVAC,Sum,Water Heater Heater 2 Heating Energy [J]
-
-* HVAC,Sum,Water Heater Heater 1 Cycle On Count []
-
-* HVAC,Sum,Water Heater Heater 2 Cycle On Count  []
-
-* HVAC,Average,Water Heater Heater 1 Runtime Fraction []
-
-* HVAC,Average,Water Heater Heater 2 Runtime Fraction []
-
-* HVAC,Average,Water Heater Temperature Node &lt;x&gt; [C]
-
-* HVAC,Average,Water Heater Final Temperature Node &lt;x&gt; [C]
-
-#### Water Heater Heater 1 Heating Rate [W]
-
-The average heating rate supplied by Heater 1.
-
-#### Water Heater Heater 2 Heating Rate [W]
-
-The average heating rate supplied by Heater 2.
-
-#### Water Heater Heater 1 Heating Energy [J]
-
-The heating energy supplied by Heater 1.
-
-#### Water Heater Heater 2 Heating Energy [J]
-
-The heating energy supplied by Heater 2.
-
-#### Water Heater Heater 1 Cycle On Count []
-
-The number of times that Heater 1 turned on in the time period.
-
-#### Water Heater Heater 2 Cycle On Count  []
-
-The number of times that Heater 2 turned on in the time period.
-
-#### Water Heater Heater 1 Runtime Fraction []
-
-The fraction of the time period that Heater 1 was running.
-
-#### Water Heater Heater 2 Runtime Fraction []
-
-The fraction of the time period that Heater 2 was running.
-
-#### Water Heater Temperature Node 1-12 [C]
-
-The average node temperature.
-
-#### Water Heater Final Temperature Node 1-12 [C]
-
-The final node temperature at the end of the system timestep.
-
-### WaterHeater:Sizing
-
-The WaterHeater:Sizing object is used to provide additional input data needed for designing tank volume and/or heater capacity for either the Mixed or Stratified water heaters.  This object is only needed if volume or capacity is being automatically sized.  There are no output variable associated with this object --  sizing results are reported to the EIO output file and some predefined summary reports.
-
-A source of design input data for use with this object can be found in the current ASHRAE Handbook HVAC Applications chapter on Service Water Heating.
-
-The idd entry for this object follows.
-
-#### Field: WaterHeater Name
-
-This field contains the unique name of the water heater being sized.  This name should match the name of a Water Heater:Mixed or a Water Heater:Stratified input object defined elsewhere in the input file.
-
-#### Field: Design Mode
-
-This field describes which of several methods are to be used for sizing the water heater.  There are six possible choices and one of the following should be selected:
-
-- **PeakDraw**. This design method uses the design flow rates of all the different demands placed on the water heater.  The tank size is based on how long it can meet the demand and how quickly it can recover.  The user enters the time in hours that the water heater can meet the demands.  Only the hot water uses connected to an individual water heater, or scheduled in the water heater object for stand-alone units, are included in that water heater’s peak draw.
-
-- **ResidentialHUD-FHAMinimum** This design method is based on minimum permissible water heater sizes (established by HUD-FHA in its Minimum Property Standards for One- and Two-Family Living Units, No. 4900.1-1982).  The user enters the number of bathrooms and bedrooms in this input object.  The smallest allowable water heater sizes are used.
-
-- **PerPerson** This design method scales sizes based on the total number of people in all zones in the building.  Each water heater in the model will be sized using the total (peak, design) number of people for the entire model.  The number of people is determined from People objects defined elsewhere in the input file
-
-- **PerFloorArea** This design method scales sizes based on the total floor area in all the zones in the building.  Each water heater in the model will be sized using all the floor area in the model.  The floor areas are determined from the geometry input elsewhere in the input file.
-
-- **PerUnit** This design method scales sizes based on an arbitrary number of units.  This can be used, for example, to size based on the number of rooms in a lodging building.  The user provides the number of units in an input field in this object.
-
-- **PerSolarCollectorArea** This design method scales tank volume based on the collector area for a solar hot water collector.  The collector area is summed for all the collectors in the model and each tank is sized for the total.  The collector area is determined from input for Solar Collectors defined elsewhere in the input file.
-
-#### Field: Time Storage Can Meet Peak Draw
-
-This field provides the time, in hours, that the tank’s volume can sustain a peak draw.  It is used to size the tank’s volume which is the simple product of peak draw volume flow rate and the draw time.  There is no assurance that the water will be at the desired temperature for the entire draw.  This field is only used if the Design Mode is “**PeakDraw**.� For a water heater connected to a full plant loop, it should be on the supply side and the plant loop needs a Plant Sizing object and the draw rate is the Use side design flow rate. For a stand-alone water heater, the draw rate is the maximum scheduled peak use flow rate.
-
-#### Field: Time for Tank Recovery
-
-This field provides the the time, in hours, that tank’s heater needs to recover the volume of the tank. The temperatures used to define recovery are a starting temperature of 14.4ºC (58ºF) and a final temperature of 57.2ºC (135ºF). This field is only used if the Design Mode is “**PeakDraw**.�
-
-#### Field: Nominal Tank Volume for Autosizing Plant Connections
-
-This field is used in case the water heater is indirectly heated by its source side connections and they are also autosized.  Because of the complexity of such a water heater and the timing for when sizing calculation happen inside EnergyPlus, the Source side connection flow rates need to be reported before the tank’s volume can be sized to meet Peak Draw.  This input field is used to provide a nominal tank volume to use temporarily while the flow connections are sized.  This field is only used if the Design Mode is “**PeakDraw**� and the water heater has autosized plant connections on the demand side.
-
-#### Field: Number of Bedrooms
-
-This field is used to enter the numer of bedrooms in the model.  This field is only used if the Design Mode is “**ResidentialHUD-FHAMinimum**.�
-
-#### Field: Number of Bathrooms
-
-This field is used to enter the number of bathrooms in the model.  This field is only used if the Design Mode is “**ResidentialHUD-FHAMinimum**.�
-
-#### Field: Storage Capacity per Person
-
-This field is used to enter the tank’s storage volume on per-person basis.  The units are m<sup>3</sup>/person.  This field is only used if the Design Mode is “**PerPerson**.�
-
-#### Field: Recovery Capacity per Person
-
-This field is used to enter the recovery capacity per person in units of m<sup>3</sup>/person/hr.  This is the volume of water the heater can recover in one hour per person.  Recovery is heating water from a starting temperature of 14.4ºC (58ºF) to a final temperature of 57.2ºC (135ºF).  This field is only used if the Design Mode is “**PerPerson**.�
-
-#### Field: Storage Capacity per Floor Area
-
-This field is used to enter the tank’s storage volume on a per-floor-area basis.  The units are m<sup>3</sup> /m<sup>2</sup> (water/floor area).  This field is only used if the Design Mode is “**PerFloorArea**.�
-
-#### Field: Recovery Capacity per Floor Area
-
-This field is used to enter the recovery capacity per floor area in units of m<sup>3</sup>/m<sup>2</sup>/hr.  This is the volume water the heater can recover in an hour per floor area.  Recovery is heating water from a starting temperature of 14.4ºC (58ºF) to a final temperature of 57.2ºC (135ºF).  This field is only used if the Design Mode is “**PerFloorArea**.�
-
-#### Field: Number of Units
-
-This field is used to enter the number of Units for use in sizing on per-Unit basis with the next two fields.  This field is only used if the Design Mode is “**PerUnit**.�  This can be used to account for any arbitrary item such as lodging rooms, desks, water fixtures, restrooms, etc.
-
-#### Field: Storage Capacity per Unit
-
-This field is used to enter the tanks’ storage volume on per-Unit basis.  The units are m<sup>3</sup>/Unit.  The number of Units is entered in the previous field.  This field is only used if the Design Mode is “**PerUnit**.�
-
-#### Field: Recovery Capacity per Unit
-
-This field is used to enter the recover capacity per Unit in units of m<sup>3</sup>/Unit/hr.  This is the volume of water the heater can recover in an hour per Unit.  Recovery is heating water from a starting temperature of 14.4ºC (58ºF) to a final temperature of 57.2ºC (135ºF).  This field is only used if the Design Mode is “**PerUnit**.�
-
-#### Field: Storage Capacity per Collector Area
-
-This field is used to enter the tank’s storage volume on per-solar-collector-area basis.  The units are m<sup>3</sup>/m<sup>2</sup>.  This field is only used if the Design Mode is “**PerSolarCollectorArea**.�
-
-#### Field: Height Aspect Ratio
-
-This field is used to scale the height of a stratified tank to preserve relative geometry for different size tanks. The Height Aspect Ratio is defined at the length scale in the vertical direction (height) divided by the length scale in the horizontal direction (diameter).  This field is only used if the water heater being sized is a Water Heater:Stratified, the tank height has been set to Autosize, and the tank shape is set to **VerticalCylinder**. This field can be used with any Design Mode.
-
-### WaterHeater:HeatPump:PumpedCondenser
-
-The heat pump water heater with pumped condenser (HPWH) is a compound object consisting of a water heater tank (e.g., `WaterHeater:Mixed` or `WaterHeater:Stratified`), a direct expansion (DX) “coil� (i.e., an air-to-water DX compression system which includes a water heating coil, air coil, compressor, and water pump), and a fan to provide air flow across the air coil associated with the DX compression system. These objects work together to model a system which heats water using zone air, outdoor air, or a combination of zone and outdoor air as the primary heat source. Numerous configurations of tank location, inlet air source, and DX coil compressor location can be modeled, with one common configuration shown below.
-
-![HPHotWaterHeater](media/image192.png)
-
-Figure 81. Schematic diagram for a heat pump water heater located in a zone
-
-In this model, the heat pump water heater’s DX coil is considered the primary heat source and the water tank’s heater (element or burner) provides supplemental heat as necessary. The model also assumes that the heat pump’s fan and water pump cycle on and off with the compressor.
-
-To model a heat pump water heater, the input data file must include some combination of the following objects depending on the configuration to be modeled:
-
-- `WaterHeater:HeatPump:PumpedCondenser` (required)
-
-- `WaterHeater:Mixed` or `WaterHeater:Stratified` (required)
-
-- `Coil:WaterHeating:AirToWaterHeatPump:Pumped` or `Coil:WaterHeating:AirToWaterHeatPump:VariableSpeed` (required)
-
-- `Fan:OnOff` (required)
-
-- `ZoneHVAC:EquipmentList` (when the HPWH draws some or all of its air from the zone, the heat pump water heater type and name must be in this list)
-
-- `ZoneHVAC:EquipmentConnections` (when the HPWH draws some or all of its air from the zone, the HPWH air inlet and outlet node names must be provided in this object)
-
-- `OutdoorAir:NodeList` (for HPWHs that use outdoor air as all or part of the heat source, the HPWH outdoor air node name must be provided in this list)
-
-The input fields for the compound object are described in detail below:
-
-#### Field: Name
-
-This alpha field contains a unique user-assigned name for an instance of a heat pump water heater. Any reference to this heat pump water heater by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the name of the schedule (ref: Schedule) that denotes whether the heat pump compressor is available to operate during a given time period. A schedule value equal to 0 denotes that the heat pump compressor is off for that time period. A value other than 0 denotes that the heat pump compressor is available to operate during that time period. During times when the heat pump compressor is scheduled off, the heater (element or burner) in the water tank object operates based on its tank set point temperature schedule and the heat pump’s parasitic electric power is also off for that time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Compressor Setpoint Temperature Schedule Name
-
-This alpha field contains the name of the schedule (ref: Schedule) that specifies the set point (or “cut-out�) temperature for the heat pump compressor. Temperature values used in this schedule should be in degrees Celsius. The heat pump compressor cycles off when the tank water reaches this set point temperature. Once the heat pump compressor cycles off, the tank water temperature floats downward until it falls below the set point temperature minus the dead band temperature difference defined below (i.e., the “cut-in� temperature). At this point, the heat pump compressor cycles on and remains on until the heat pump compressor set point temperature is reached.
-
-#### Field: Dead Band Temperature Difference
-
-This numeric field contains the dead band temperature difference in degrees Celsius. The heat pump compressor “cut-in� temperature is defined as the compressor set point temperature defined above minus this dead band temperature difference. The heat pump compressor cycles on when the water temperature in the tank falls below the “cut-in� temperature. The heat pump compressor remains on until the water temperature in the tank rises above the compressor set point (“cut-out�) temperature defined above. The dead band temperature difference must be greater than 0°C and less than or equal to 20°C. If this field is left blank, the default value is 5°C.
-
-In this model, the heat pump water heater’s DX compression system is considered the primary heat source and the water tank’s heater (element or burner) provides supplemental heat as necessary. Therefore, the cut-in temperature for the heat pump compressor (set point minus dead band temperature difference) is usually higher than the set point temperature for the heater (element or burner) in the associated water heater tank object. At times when the water heater tank set point temperature is greater than the cut-in temperature of the heat pump compressor, the heat pump compressor is disabled and the tank’s heater is used to heat the water.
-
-#### Field: Condenser Water Inlet Node Name
-
-This alpha field contains the name of the inlet water node for the heat pump’s water heating coil (condenser). This node name must also be specified in the water heater tank object as the source outlet node name, and in the DX coil object as the condenser water inlet node name.
-
-#### Field: Condenser Water Outlet Node Name
-
-This alpha field contains the name of the outlet water node for the heat pump’s water heating coil (condenser). This node name must also be specified in the water heater tank object as the source inlet node name, and in the DX coil object as the condenser water outlet node name.
-
-#### Field: Condenser Water Flow Rate
-
-This numeric field contains the heat pump’s condenser water flow rate in cubic meters per second. It is the actual condenser water flow rate to be simulated, which may differ from the rated condenser water volumetric flow rate specified for the heat pump’s DX coil (Ref. Coil:WaterHeating:AirToWaterHeatPump). This water flow rate must be greater than 0 or this field is autocalculatable. If autocalculated (field value = **autocalculate**), the condenser water flow rate is set equal to the rated heating capacity of the heat pump’s DX coil multiplied by 4.487E-8 m<sup>3</sup>/s/W. When this flow rate is different from the Rated Condenser Water Volumetric Flow Rate specified in the heat pump’s DX coil object (Ref. Coil:WaterHeating:AirToWaterHeatPump), the user should also specify a Total Heating Capacity Modifier Curve Name (function of water flow fraction) and a Heating COP Modifier Curve Name (function of water flow fraction) in the associated DX coil object to account for differences in capacity and power consumption at the off-rated water flow rate.
-
-#### Field: Evaporator Air Flow Rate
-
-This numeric field contains the air flow rate across the heat pump’s air coil (evaporator) in cubic meters per second. It is the actual air flow rate to be simulated, which may differ from the rated evaporator air volumetric flow rate specified for the heat pump’s DX coil (Ref. Coil:WaterHeating:AirToWaterHeatPump:Pumped). Values must be greater than 0 or this field is autocalculatable. If autocalculated (field value = **autocalculate**), the evaporator air flow rate is set equal to the rated heating capacity of the heat pump’s DX coil multiplied by 5.035E-5 m<sup>3</sup>/s/W. When this flow rate is different from the Rated Evaporator Air Volumetric Flow Rate specified in the heat pump’s DX coil object (Ref. Coil:WaterHeating:AirToWaterHeatPump:Pumped), the user should also specify a Total Heating Capacity Modifier Curve Name (function of air flow fraction) and a Heating COP Modifier Curve Name (function of air flow fraction) in the associated DX coil object to account for differences in capacity and power consumption at the off-rated air flow rate.
-
-#### Field: Inlet Air Configuration
-
-This choice field defines the configuration of the air flow path through the heat pump air coil (evaporator) and fan section. Valid entries are **Schedule**, **ZoneAirOnly**, **OutdoorAirOnly**, or **ZoneAndOutdoorAir**. If ‘Schedule’ is selected, names for an inlet air temperature schedule and an inlet air humidity schedule must be defined in the fields below. If ‘ZoneAirOnly’ is selected, the corresponding zone name must be entered in the Inlet Air Zone Name field below. If ‘ZoneAndOutdoorAir’ is selected, the corresponding Inlet Air Zone Name, Inlet Air Mixer Node Name, Outlet Air Splitter Node Name, and an Inlet Air Mixer Schedule Name must be entered in the corresponding fields below.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the name of the node from which the heat pump water heater draws its inlet air. If the Inlet Air Configuration field defined above is set to ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’, then this node name should be the name of a zone air exhaust node (Ref. ZoneHVAC:EquipmentConnections). If the Inlet Air Configuration field is set to ‘OutdoorAirOnly’, this node name should be left blank. If the Inlet Air Configuration field is set to ‘Schedule’, this node name should simply be a unique name that allows the user to receive output on conditions at this node for verification purposes.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the name of the node to which the heat pump water heater sends its outlet air. If the Inlet Air Configuration field defined above is set to ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’, then this node name should be the name of a zone air inlet node (Ref. ZoneHVAC:EquipmentConnections). If the Inlet Air Configuration field is set to ‘OutdoorAirOnly’, this node name should be left blank. If the Inlet Air Configuration field is set to ‘Schedule’, this node name should simply be a unique name that allows the user to receive output on conditions at this node for verification purposes.
-
-#### Field: Outdoor Air Node Name
-
-This alpha field contains the name of the node from which the heat pump water heater draws its outdoor air. If the Inlet Air Configuration field defined above is set to ‘ZoneAirOnly’ or ‘Schedule’, this node name should be left blank. If the Inlet Air Configuration field is set to ‘ZoneAndOutdoorAir’ or ‘OutdoorAirOnly’, this node name should be the name of an outdoor air node (Ref. OutdoorAir:NodeList).
-
-#### Field: Exhaust Air Node Name
-
-This alpha field contains the name of the node to which the heat pump water heater sends its exhaust air. If the Inlet Air Configuration field defined above is set to ‘ZoneAirOnly’ or ‘Schedule’, this node name should be left blank. If the Inlet Air Configuration field is set to ‘ZoneAndOutdoorAir’ or ‘OutdoorAirOnly’, then this node name should be a unique name that allows the user to receive output on conditions at this node for verification purposes.
-
-#### Field: Inlet Air Temperature Schedule Name
-
-This alpha field contains the name of a schedule used to define the dry-bulb temperature of the inlet air to the heat pump air coil (evaporator) and fan section. Schedule values should be in degrees Celsius. This field is only used when the Inlet Air Configuration defined above is specified as ‘Schedule’, otherwise leave this field blank.
-
-#### Field: Inlet Air Humidity Schedule Name
-
-This alpha field contains the name of a schedule used to define the humidity of the inlet air to the heat pump evaporator and fan section. Schedule values must be entered as relative humidity fraction from 0 to 1 (e.g., a schedule value of 0.5 means 50%RH). This field is only used when the Inlet Air Configuration defined above is specified as ‘Schedule’, otherwise leave this field blank.
-
-#### Field: Inlet Air Zone Name
-
-This alpha field contains the name of the zone from which the heat pump evaporator and fan section draws some or all of its inlet air. This field is only used when the Inlet Air Configuration defined above is specified as ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’.
-
-#### Field: Tank Object Type
-
-This alpha (choice) field contains the type of water heater tank used by this heat pump water heater. Currently, the only valid choices are WaterHeater:Mixed or WaterHeater:Stratified.
-
-#### Field: Tank Name
-
-This alpha field contains the name of the specific water heater tank used by this heat pump water heater. This must be a tank of type `WaterHeater:Mixed` or `WaterHeater:Stratified`.
-
-#### Field: Tank Use Side Inlet Node Name
-
-This alpha field contains the name of the use side inlet node of the water heater tank used by this heat pump water heater. This name must match the Use Side Inlet Node Name in the water heater tank object (Ref. `WaterHeater:Mixed`). This field is required if the water heater tank use side nodes are connected to a plant loop, otherwise leave this field blank. When used, the branch object should reflect that this node is part of a `WaterHeater:HeatPump:PumpedCondenser` object (see branch object example below).
-
-#### Field: Tank Use Side Outlet Node Name
-
-This alpha field contains the name of the use side outlet node of the water heater tank used by this heat pump water heater. This name must match the Use Side Outlet Node Name in the water heater tank object (Ref. `WaterHeater:Mixed`). This field is required if the water heater tank use side nodes are connected to a plant loop, otherwise leave this field blank. When used, the branch object should reflect that this node is part of a `WaterHeater:HeatPump:PumpedCondenser` object (see branch object example below).
-
-#### Field: DX Coil Object Type
-
-This alpha (choice) field contains the type of DX coil used by this heat pump water heater. Currently, the only valid choice is Coil:WaterHeating:AirToWaterHeatPump:Pumped.
-
-#### Field: DX Coil Name
-
-This alpha field contains the name of the specific DX coil (`Coil:WaterHeating:AirToWaterHeatPump:Pumped` or `Coil:WaterHeating:AirToWaterHeatPump:VariableSpeed` object) used by this heat pump water heater.
-
-#### Field: Minimum Inlet Air Temperature for Compressor Operation
-
-This numeric field contains the minimum inlet air dry-bulb temperature entering the air coil (evaporator) and fan section, in degrees Celsius, below which the heat pump compressor does not operate. The minimum inlet air dry-bulb temperature should be greater than or equal to -5°C. If this field is left blank, the default value is 10°C.
-
-#### Field: Compressor Location
-
-This alpha (choice) field contains the location of the heat pump compressor and the air temperature for this location is used to control operation of the compressor’s crankcase heater in the Coil:WaterHeating:AirToWaterHeatPump:Pumped object. Valid entries are **Schedule**, **Zone**, or **Outdoors**. If ‘Schedule’ is selected, a compressor ambient temperature schedule name must be defined in the field below; otherwise, the field below should be left blank. If ‘Zone’ is selected, the crankcase heater operation is controlled based on the air temperature in the zone defined in the field Inlet Air Zone Name, and the Inlet Air Configuration must be ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’. If ‘Outdoors’ is selected, crankcase heater operation is controlled based on the outdoor air temperature.
-
-#### Field: Compressor Ambient Temperature Schedule Name
-
-This alpha field contains the name of a schedule that defines the ambient air temperature surrounding the heat pump compressor, which is used to control the compressor’s crankcase heater operation. This field is only used when the compressor location field defined above is specified as ‘Schedule’, otherwise it should be left blank.
-
-#### Field: Fan Object Type
-
-This alpha (choice) field contains the type of fan used by this heat pump water heater. Currently, the only valid choice is Fan: OnOff.
-
-#### Field: Fan Name
-
-This alpha field contains the name of the specific fan (`Fan:OnOff` object) used by this heat pump water heater.
-
-#### Field: Fan Placement
-
-This alpha (choice) field defines the placement of the fan in the heat pump water heater. Valid choices are **BlowThrough** (fan upstream of the air coil) and **DrawThrough** (fan downstream of the air coil). If this field is left blank, the default value is DrawThrough.
-
-#### Field: On Cycle Parasitic Electric Load
-
-This numeric field contains the on-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the heat pump water heater. This parasitic electric load is consumed whenever the heat pump compressor is operating and the model assumes that this parasitic power does not contribute to heating the water. This parasitic load does, however, affect the zone air heat balance when the heat pump water heater sends some or all of its outlet air to a zone (i.e., Inlet Air Configuration field specified as ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’) and the Parasitic Heat Rejection Location field is specified as ‘Zone’. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
-
-#### Field: Off Cycle Parasitic Electric Load
-
-This numeric field contains the off-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the heat pump compressor. This parasitic electric load is consumed whenever the heat pump water heater is available but the compressor is not operating, and the model assumes that this parasitic power does not contribute to heating the water. This parasitic load does, however, affect the zone air heat balance when the heat pump water heater sends some or all of its outlet air to a zone (i.e., Inlet Air Configuration field specified as ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’) and the Parasitic Heat Rejection Location field is specified as ‘Zone’. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
-
-#### Field: Parasitic Heat Rejection Location
-
-This alpha (choice) field determines where the on-cycle and off-cycle parasitic heat is rejected. Valid choices are Zone and Exterior. If ‘Zone’ is selected, both the on-cycle and off-cycle parasitic heat is rejected to the zone defined in the field Inlet Air Zone Name, and the Inlet Air Configuration must be ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir. If ’Outdoors’ is selected, this parasitic heat is rejected outdoors (does not impact the zone air heat balance) regardless of the specified Inlet Air Configuration. If this field is left blank, the default value is ’Outdoors’.
-
-#### Field: Inlet Air Mixer Node Name
-
-This optional alpha field defines the name of the HVAC node which represents the mixture of outdoor air and zone air that enters the heat pump air coil (evaporator) and fan section. The model mixes outdoor air with zone air and places the result on this inlet air mixer node based on the Inlet Air Mixer Schedule defined below. When the schedule value is equal to 0, 100% zone air enters the evaporator coil and fan section of the heat pump water heater. When the schedule value is equal to 1, 100% outdoor air enters the evaporator coil and fan section. This node name must be provided if the Inlet Air Configuration field above is specified as ‘ZoneAndOutdoor Air’, otherwise this field should be left blank.
-
-#### Field: Outlet Air Splitter Node Name
-
-This alpha field defines the name of the air node to which the heat pump air coil (evaporator) and fan sends all of its outlet air. The supply air flow downstream of this node is split between the zone and outdoors based on the Inlet Air Mixer schedule defined below. When the schedule value is equal to 0, the entire outlet air stream is diverted to the zone. When the schedule value is equal to 1, the entire outlet air stream is exhausted to outdoors. This node name must be provided if the Inlet Air Configuration field above is specified as ‘Zone and Outdoor Air’, otherwise this field should be left blank.
-
-#### Field: Inlet Air Mixer Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump draws its inlet air from the zone, outdoors, or a combination of zone and outdoor air. A schedule value equal to 0 indicates that the heat pump draws its inlet air from the zone. A schedule value equal to 1 denotes that the heat pump draws its inlet air from outdoors. Values between 0 and 1 denote a mixture of zone and outdoor air proportional to the schedule value. The Inlet Air Mixer schedule controls both the inlet air mixer and outlet air splitter nodes in unison to ensure that the operation of the heat pump does not contribute to zone pressurization or depressurization. For example if the Inlet Air Mixer schedule value is 0.4, then the inlet air mixer node is composed of 40% outdoor air and 60% zone air. For this same case, the outlet air splitter directs 60% of the HPWH outlet air back to the zone and 40% of the outlet air flow is exhausted outdoors. This schedule name must be provided if the Inlet Air Configuration field is specified as ‘Zone and Outdoor Air’, otherwise this field should be left blank.
-
-#### Field: Tank Element Control Logic
-
-This alpha field defines settings for the control logic of when to run the tank element in relation to whether the heat pump is running. 
-
-  - **MutuallyExclusive** means that once the tank heating element(s) are active, the heat pump is shut down until the heating element setpoint is reached. 
-  - **Simultaneous** (default) means that both the tank heating element and heat pump are used at the same time to recover the tank temperature. 
-
-#### Field: Control Sensor 1 Height In Stratified Tank
-
-This alpha field defines where the tank temperature is sensed for heat pump control when the tank type is `WaterHeater:Stratified`.  The stratified tank model produces tank temperature at different nodes in the vertical direction and various options are available for how this temperature should be sensed to control the heat pump.  This is measured in height from the bottom of the tank. Internally the appropriate node is determined based on this height. If omitted, this defaults to the height of Heater1.
-
-#### Field: Control Sensor 1 Weight
-
-The model can optionally use two control sensor locations in stratified tanks. When that is the case, the temperature sensed at each location is weighted. This alpha input specifies the weight associated with Control Sensor 1. It is input as a value between 0 and 1. The weight of Control Sensor 2 is determined by subtracting this weight from 1. The default for this field is 1, indicating that only Control Sensor 1 is used. 
-
-#### Field: Control Sensor 2 Height in Stratified Tank
-
-This alpha field defines the optional second location where the tank temperature is sensed for heat pump control when the tank type is `WaterHeater:Stratified`. If omitted, this defaults to the height of Heater2.
-
-Following is an example input for the `WaterHeater:HeatPump:PumpedCondenser` compound object and the other required component objects that it references.
-
-```idf
-WaterHeater:HeatPump:PumpedCondenser,
-    PlantHeatPumpWaterHeater,!- Name
-    PlantHPWHSch,            !- Availability Schedule Name
-    PlantHPWHTempSch,        !- Compressor Setpoint Temperature Schedule Name
-    2.0,                     !- Dead Band Temperature Difference {deltaC}
-    HPPlantWaterInletNode,   !- Condenser Water Inlet Node Name
-    HPPlantWaterOutletNode,  !- Condenser Water Outlet Node Name
-    0.00115525,              !- Condenser Water Flow Rate {m3/s}
-    1.00695,                 !- Evaporator Air Flow Rate {m3/s}
-    OutdoorAirOnly,          !- Inlet Air Configuration
-    ,                        !- Air Inlet Node Name
-    ,                        !- Air Outlet Node Name
-    HPPlantAirInletNode,     !- Outdoor Air Node Name
-    HPPlantAirOutletNode,    !- Exhaust Air Node Name
-    ,                        !- Inlet Air Temperature Schedule Name
-    ,                        !- Inlet Air Humidity Schedule Name
-    ,                        !- Inlet Air Zone Name
-    WaterHeater:Mixed,       !- Tank Object Type
-    HPWHPlantTank,           !- Tank Name
-    HPWH Use Inlet Node,     !- Tank Use Side Inlet Node Name
-    HPWH Use Outlet Node,    !- Tank Use Side Outlet Node Name
-    Coil:WaterHeating:AirToWaterHeatPump:Pumped,  !- DX Coil Object Type
-    HPWHPlantDXCoil,         !- DX Coil Name
-    11.0,                    !- Minimum Inlet Air Temperature for Compressor Operation {C}
-    Outdoors,                !- Compressor Location
-    ,                        !- Compressor Ambient Temperature Schedule Name
-    Fan:OnOff,               !- Fan Object Type
-    HPWHPlantFan,            !- Fan Name
-    BlowThrough,             !- Fan Placement
-    ,                        !- On Cycle Parasitic Electric Load {W}
-    ,                        !- Off Cycle Parasitic Electric Load {W}
-    ;                        !- Parasitic Heat Rejection Location
-```
-
-
-
-
-NOTE: branch object required only when tank use inlet nodes are used.
-
-
-
-```idf
-  Branch,
-    Central HPWH Branch,     !- Name
-    0,                       !- Maximum Flow Rate {m3/s}
-    ,                        !- Pressure Drop Curve Name
-    WaterHeater:HeatPump:PumpedCondenser,    !- Component 1 Object Type
-    PlantHeatPumpWaterHeater,!- Component 1 Name
-    HPWH Use Inlet Node,     !- Component 1 Inlet Node Name
-    HPWH Use Outlet Node,    !- Component 1 Outlet Node Name
-    PASSIVE;                 !- Component 1 Branch Control Type
-
-
-
-
-  WaterHeater:Mixed,
-    HPWHPlantTank,           !- Name
-    0.757,                   !- Tank Volume {m3}
-    Plant Hot Water Setpoint Temp Schedule,  !- Setpoint Temperature Schedule Name
-    2.0,                     !- Deadband Temperature Difference {deltaC}
-    82.2222,                 !- Maximum Temperature Limit {C}
-    CYCLE,                   !- Heater Control Type
-    25000,                   !- Heater Maximum Capacity {W}
-    0,                       !- Heater Minimum Capacity {W}
-    ,                        !- Heater Ignition Minimum Flow Rate {m3/s}
-    ,                        !- Heater Ignition Delay {s}
-    ELECTRICITY,             !- Heater Fuel Type
-    0.98,                    !- Heater Thermal Efficiency
-    ,                        !- Part Load Factor Curve Name
-    10,                      !- Off Cycle Parasitic Fuel Consumption Rate {W}
-    ELECTRICITY,             !- Off Cycle Parasitic Fuel Type
-    0,                       !- Off Cycle Parasitic Heat Fraction to Tank
-    30,                      !- On Cycle Parasitic Fuel Consumption Rate {W}
-    ELECTRICITY,             !- On Cycle Parasitic Fuel Type
-    0,                       !- On Cycle Parasitic Heat Fraction to Tank
-    Outdoors,                !- Ambient Temperature Indicator
-    ,                        !- Ambient Temperature Schedule Name
-    ,                        !- Ambient Temperature Zone Name
-    HPWHPlantTank OA Node,   !- Ambient Temperature Outdoor Air Node Name
-    0.0,                     !- Off Cycle Loss Coefficient to Ambient Temperature {W/K}
-    0.0,                     !- Off Cycle Loss Fraction to Zone
-    0.0,                     !- On Cycle Loss Coefficient to Ambient Temperature {W/K}
-    0.0,                     !- On Cycle Loss Fraction to Zone
-    ,                        !- Peak Use Flow Rate {m3/s}
-    ,                        !- Use Flow Rate Fraction Schedule Name
-    ,                        !- Cold Water Supply Temperature Schedule Name
-    HPWH Use Inlet Node,     !- Use Side Inlet Node Name
-    HPWH Use Outlet Node,    !- Use Side Outlet Node Name
-    0.98,                    !- Use Side Effectiveness
-    HPPlantWaterOutletNode,  !- Source Side Inlet Node Name
-    HPPlantWaterInletNode,   !- Source Side Outlet Node Name
-    0.98,                    !- Source Side Effectiveness
-    autosize;                !- Use Side Design Flow Rate {m3/s}
-
-
-  OutdoorAir:Node,
-    HPWHPlantTank OA Node;   !- Name
-
-
-  Coil:WaterHeating:AirToWaterHeatPump:Pumped,
-    HPWHPlantDXCoil,         !- Name
-    25000.0,                 !- Rated Heating Capacity {W}
-    3.2,                     !- Rated COP {W/W}
-    0.736,                   !- Rated Sensible Heat Ratio
-    29.44,                   !- Rated Evaporator Inlet Air Dry-Bulb Temperature {C}
-    22.22,                   !- Rated Evaporator Inlet Air Wet-Bulb Temperature {C}
-    55.72,                   !- Rated Condenser Inlet Water Temperature {C}
-    1.00695,                 !- Rated Evaporator Air Flow Rate {m3/s}
-    0.00115525,              !- Rated Condenser Water Flow Rate {m3/s}
-    No,                      !- Evaporator Fan Power Included in Rated COP
-    No,                      !- Condenser Pump Power Included in Rated COP
-    No,                      !- Condenser Pump Heat Included in Rated Heating Capacity and Rated COP
-    150.0,                   !- Condenser Water Pump Power {W}
-    0.1,                     !- Fraction of Condenser Pump Heat to Water
-    HPPlantFanAirOutletNode, !- Evaporator Air Inlet Node Name
-    HPPlantAirOutletNode,    !- Evaporator Air Outlet Node Name
-    HPPlantWaterInletNode,   !- Condenser Water Inlet Node Name
-    HPPlantWaterOutletNode,  !- Condenser Water Outlet Node Name
-    100.0,                   !- Crankcase Heater Capacity {W}
-    5.0,                     !- Maximum Ambient Temperature for Crankcase Heater Operation {C}
-    WetBulbTemperature,      !- Evaporator Air Temperature Type for Curve Objects
-    HPWHHeatingCapFTemp,     !- Heating Capacity Function of Temperature Curve Name
-    ,                        !- Heating Capacity Function of Air Flow Fraction Curve Name
-    ,                        !- Heating Capacity Function of Water Flow Fraction Curve Name
-    HPWHHeatingCOPFTemp,     !- Heating COP Function of Temperature Curve Name
-    ,                        !- Heating COP Function of Air Flow Fraction Curve Name
-    ,                        !- Heating COP Function of Water Flow Fraction Curve Name
-    HPWHPLFFPLR;             !- Part Load Fraction Correlation Curve Name
-
-
-  Fan:OnOff,
-    HPWHPlantFan,            !- Name
-    PlantHPWHSch,            !- Availability Schedule Name
-    0.7,                     !- Fan Total Efficiency
-    100.0,                   !- Pressure Rise {Pa}
-    2.6852,                  !- Maximum Flow Rate {m3/s}
-    0.9,                     !- Motor Efficiency
-    1.0,                     !- Motor In Airstream Fraction
-    HPPlantAirInletNode,     !- Air Inlet Node Name
-    HPPlantFanAirOutletNode; !- Air Outlet Node Name
-```
-
-
-### Pumped Condenser Heat Pump Water Heater Outputs
-
-* **HVAC,Average,Water Heater Compressor Part Load Ratio**
-
-* **HVAC,Average,Water Heater On Cycle Ancillary Electric Power [W]**
-
-* **HVAC,Sum,Water Heater On Cycle Ancillary Electric Energy [J]**
-
-* **HVAC,Average,Water Heater Off Cycle Ancillary Electric Power [W]**
-
-* **HVAC,Sum,Water Heater Off Cycle Ancillary Electric Energy [J]**
-
-
-
-#### Water Heater Compressor Part Load Ratio
-
-This output is the average part-load ratio of the heat pump water heater’s compressor (as well as its water pump and fan) for the timestep being reported. This output is independent of the “Water Heater Part Load Ratio� (Ref. Water Heater Outputs) which represents the part-load ratio of the supplemental heater (element or burner) in the water tank. When the water tank’s (supplemental) heater set point temperature is higher than the cut-in temperature of the heat pump water heater’s compressor, the heat pump compressor is disabled and the water tank’s heater (element or burner) is used to heat the water. During these times the Water Heater Compressor Part Load Ratio is equal to 0.
-
-#### Water Heater On Cycle Ancillary Electric Power [W]
-
-#### Water Heater On Cycle Ancillary Electric Energy [J]
-
-#### Water Heater Off Cycle Ancillary Electric Power [W]
-
-#### Water Heater Off Cycle Ancillary Electric Energy [J]
-
-These outputs are the parasitic electric power and consumption associated with the heat pump water heater. Specific outputs represent parasitic electrical usage during the compressor/fan on and off cycles. These outputs represent electronic controls or other electric component. The model assumes that the parasitic power does not contribute to heating the water, but it can impact the zone air heat balance depending on user inputs. The parasitic electric consumption outputs are also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
-
-### WaterHeater:HeatPump:WrappedCondenser
-
-The heat pump water heater with wrapped condenser is a compound object very similar to the `WaterHeater:HeatPump:PumpedCondenser` object. It likewise combines a water heater tank, a direct expansion (DX) “coil�, and a fan to provide air flow across the air coil associated with the DX compression system. The primary difference is that instead of pumping water through an external condenser, the heating coils are wrapped around or submerged in the tank. This type of HPWH is most common in packaged units meant for residential applications.
-
-To model a wrapped condenser heat pump water, the input data file must include some combination of the following objects depending on the configuration to be modeled:
-
-- `WaterHeater:HeatPump:WrappedCondenser` (required)
-
-- `WaterHeater:Stratified` (required)
-
-- `Coil:WaterHeating:AirToWaterHeatPump:Wrapped` (required)
-
-- `Fan:OnOff` (required)
-
-- `ZoneHVAC:EquipmentList` (when the HPWH draws some or all of its air from the zone, the heat pump water heater type and name must be in this list)
-
-- `ZoneHVAC:EquipmentConnections` (when the HPWH draws some or all of its air from the zone, the HPWH air inlet and outlet node names must be provided in this object)
-
-- `OutdoorAir:NodeList` (for HPWHs that use outdoor air as all or part of the heat source, the HPWH outdoor air node name must be provided in this list)
-
-The input fields for the compound object are described in detail below:
-
-#### Field: Name
-
-This alpha field contains a unique user-assigned name for an instance of a heat pump water heater. Any reference to this heat pump water heater by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the name of the schedule (ref: Schedule) that denotes whether the heat pump compressor is available to operate during a given time period. A schedule value equal to 0 denotes that the heat pump compressor is off for that time period. A value other than 0 denotes that the heat pump compressor is available to operate during that time period. During times when the heat pump compressor is scheduled off, the heater (element or burner) in the water tank object operates based on its tank set point temperature schedule and the heat pump’s parasitic electric power is also off for that time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Compressor Setpoint Temperature Schedule Name
-
-This alpha field contains the name of the schedule (ref: Schedule) that specifies the set point (or “cut-out�) temperature for the heat pump compressor. Temperature values used in this schedule should be in degrees Celsius. The heat pump compressor cycles off when the tank water reaches this set point temperature. Once the heat pump compressor cycles off, the tank water temperature floats downward until it falls below the set point temperature minus the dead band temperature difference defined below (i.e., the “cut-in� temperature). At this point, the heat pump compressor cycles on and remains on until the heat pump compressor set point temperature is reached.
-
-#### Field: Dead Band Temperature Difference
-
-This numeric field contains the dead band temperature difference in degrees Celsius. The heat pump compressor “cut-in� temperature is defined as the compressor set point temperature defined above minus this dead band temperature difference. The heat pump compressor cycles on when the water temperature in the tank falls below the “cut-in� temperature. The heat pump compressor remains on until the water temperature in the tank rises above the compressor set point (“cut-out�) temperature defined above. The dead band temperature difference must be greater than 0°C and less than or equal to 20°C. If this field is left blank, the default value is 5°C.
-
-In this model, the heat pump water heater’s DX compression system is considered the primary heat source and the water tank’s heater (element or burner) provides supplemental heat as necessary. Therefore, the cut-in temperature for the heat pump compressor (set point minus dead band temperature difference) is usually higher than the set point temperature for the heater (element or burner) in the associated water heater tank object. At times when the water heater tank set point temperature is greater than the cut-in temperature of the heat pump compressor, the heat pump compressor is disabled and the tank’s heater is used to heat the water.
-
-#### Field: Condenser Bottom Location
-
-This numeric field contains the distance from the bottom of the tank to the bottom of the wrapped condenser. 
-
-#### Field: Condenser Top Location
-
-This numeric field contains the distance from the bottom of the tank to the top of the wrapped condenser.
-
-#### Field: Evaporator Air Flow Rate
-
-This numeric field contains the air flow rate across the heat pump’s air coil (evaporator) in cubic meters per second. It is the actual air flow rate to be simulated, which may differ from the rated evaporator air volumetric flow rate specified for the heat pump’s DX coil (Ref. Coil:WaterHeating:AirToWaterHeatPump:Wrapped). Values must be greater than 0 or this field is autocalculatable. If autocalculated (field value = **autocalculate**), the evaporator air flow rate is set equal to the rated heating capacity of the heat pump’s DX coil multiplied by 5.035E-5 m<sup>3</sup>/s/W. When this flow rate is different from the Rated Evaporator Air Volumetric Flow Rate specified in the heat pump’s DX coil object (Ref. Coil:WaterHeating:AirToWaterHeatPump:Wrapped), the user should also specify a Total Heating Capacity Modifier Curve Name (function of air flow fraction) and a Heating COP Modifier Curve Name (function of air flow fraction) in the associated DX coil object to account for differences in capacity and power consumption at the off-rated air flow rate.
-
-#### Field: Inlet Air Configuration
-
-This choice field defines the configuration of the air flow path through the heat pump air coil (evaporator) and fan section. Valid entries are **Schedule**, **ZoneAirOnly**, **OutdoorAirOnly**, or **ZoneAndOutdoorAir**. If ‘Schedule’ is selected, names for an inlet air temperature schedule and an inlet air humidity schedule must be defined in the fields below. If ‘ZoneAirOnly’ is selected, the corresponding zone name must be entered in the Inlet Air Zone Name field below. If ‘ZoneAndOutdoorAir’ is selected, the corresponding Inlet Air Zone Name, Inlet Air Mixer Node Name, Outlet Air Splitter Node Name, and an Inlet Air Mixer Schedule Name must be entered in the corresponding fields below.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the name of the node from which the heat pump water heater draws its inlet air. If the Inlet Air Configuration field defined above is set to ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’, then this node name should be the name of a zone air exhaust node (Ref. ZoneHVAC:EquipmentConnections). If the Inlet Air Configuration field is set to ‘OutdoorAirOnly’, this node name should be left blank. If the Inlet Air Configuration field is set to ‘Schedule’, this node name should simply be a unique name that allows the user to receive output on conditions at this node for verification purposes.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the name of the node to which the heat pump water heater sends its outlet air. If the Inlet Air Configuration field defined above is set to ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’, then this node name should be the name of a zone air inlet node (Ref. ZoneHVAC:EquipmentConnections). If the Inlet Air Configuration field is set to ‘OutdoorAirOnly’, this node name should be left blank. If the Inlet Air Configuration field is set to ‘Schedule’, this node name should simply be a unique name that allows the user to receive output on conditions at this node for verification purposes.
-
-#### Field: Outdoor Air Node Name
-
-This alpha field contains the name of the node from which the heat pump water heater draws its outdoor air. If the Inlet Air Configuration field defined above is set to ‘ZoneAirOnly’ or ‘Schedule’, this node name should be left blank. If the Inlet Air Configuration field is set to ‘ZoneAndOutdoorAir’ or ‘OutdoorAirOnly’, this node name should be the name of an outdoor air node (Ref. OutdoorAir:NodeList).
-
-#### Field: Exhaust Air Node Name
-
-This alpha field contains the name of the node to which the heat pump water heater sends its exhaust air. If the Inlet Air Configuration field defined above is set to ‘ZoneAirOnly’ or ‘Schedule’, this node name should be left blank. If the Inlet Air Configuration field is set to ‘ZoneAndOutdoorAir’ or ‘OutdoorAirOnly’, then this node name should be a unique name that allows the user to receive output on conditions at this node for verification purposes.
-
-#### Field: Inlet Air Temperature Schedule Name
-
-This alpha field contains the name of a schedule used to define the dry-bulb temperature of the inlet air to the heat pump air coil (evaporator) and fan section. Schedule values should be in degrees Celsius. This field is only used when the Inlet Air Configuration defined above is specified as ‘Schedule’, otherwise leave this field blank.
-
-#### Field: Inlet Air Humidity Schedule Name
-
-This alpha field contains the name of a schedule used to define the humidity of the inlet air to the heat pump evaporator and fan section. Schedule values must be entered as relative humidity fraction from 0 to 1 (e.g., a schedule value of 0.5 means 50%RH). This field is only used when the Inlet Air Configuration defined above is specified as ‘Schedule’, otherwise leave this field blank.
-
-#### Field: Inlet Air Zone Name
-
-This alpha field contains the name of the zone from which the heat pump evaporator and fan section draws some or all of its inlet air. This field is only used when the Inlet Air Configuration defined above is specified as ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’.
-
-#### Field: Tank Object Type
-
-This alpha (choice) field contains the type of water heater tank used by this heat pump water heater. Currently, the only valid choice is WaterHeater:Stratified.
-
-#### Field: Tank Name
-
-This alpha field contains the name of the specific water heater tank used by this heat pump water heater. This must be a tank of type `WaterHeater:Stratified`.
-
-#### Field: Tank Use Side Inlet Node Name
-
-This alpha field contains the name of the use side inlet node of the water heater tank used by this heat pump water heater. This name must match the Use Side Inlet Node Name in the water heater tank object (Ref. `WaterHeater:Stratified`). This field is required if the water heater tank use side nodes are connected to a plant loop, otherwise leave this field blank. When used, the branch object should reflect that this node is part of a `WaterHeater:HeatPump:WrappedCondenser` object (see branch object example below).
-
-#### Field: Tank Use Side Outlet Node Name
-
-This alpha field contains the name of the use side outlet node of the water heater tank used by this heat pump water heater. This name must match the Use Side Outlet Node Name in the water heater tank object (Ref. `WaterHeater:Stratified`). This field is required if the water heater tank use side nodes are connected to a plant loop, otherwise leave this field blank. When used, the branch object should reflect that this node is part of a `WaterHeater:HeatPump:WrappedCondenser` object (see branch object example below).
-
-#### Field: DX Coil Object Type
-
-This alpha (choice) field contains the type of DX coil used by this heat pump water heater. Currently, the only valid choice is Coil:WaterHeating:AirToWaterHeatPump:Wrapped.
-
-#### Field: DX Coil Name
-
-This alpha field contains the name of the specific DX coil (`Coil:WaterHeating:AirToWaterHeatPump:Wrapped`) used by this heat pump water heater.
-
-#### Field: Minimum Inlet Air Temperature for Compressor Operation
-
-This numeric field contains the minimum inlet air dry-bulb temperature entering the air coil (evaporator) and fan section, in degrees Celsius, below which the heat pump compressor does not operate. The minimum inlet air dry-bulb temperature should be greater than or equal to -5°C. If this field is left blank, the default value is 10°C.
-
-#### Field: Compressor Location
-
-This alpha (choice) field contains the location of the heat pump compressor and the air temperature for this location is used to control operation of the compressor’s crankcase heater in the Coil:WaterHeating:AirToWaterHeatPump:Wrapped object. Valid entries are **Schedule**, **Zone**, or **Outdoors**. If ‘Schedule’ is selected, a compressor ambient temperature schedule name must be defined in the field below; otherwise, the field below should be left blank. If ‘Zone’ is selected, the crankcase heater operation is controlled based on the air temperature in the zone defined in the field Inlet Air Zone Name, and the Inlet Air Configuration must be ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’. If ‘Outdoors’ is selected, crankcase heater operation is controlled based on the outdoor air temperature.
-
-#### Field: Compressor Ambient Temperature Schedule Name
-
-This alpha field contains the name of a schedule that defines the ambient air temperature surrounding the heat pump compressor, which is used to control the compressor’s crankcase heater operation. This field is only used when the compressor location field defined above is specified as ‘Schedule’, otherwise it should be left blank.
-
-#### Field: Fan Object Type
-
-This alpha (choice) field contains the type of fan used by this heat pump water heater. Currently, the only valid choice is Fan: OnOff.
-
-#### Field: Fan Name
-
-This alpha field contains the name of the specific fan (`Fan:OnOff` object) used by this heat pump water heater.
-
-#### Field: Fan Placement
-
-This alpha (choice) field defines the placement of the fan in the heat pump water heater. Valid choices are **BlowThrough** (fan upstream of the air coil) and **DrawThrough** (fan downstream of the air coil). If this field is left blank, the default value is DrawThrough.
-
-#### Field: On Cycle Parasitic Electric Load
-
-This numeric field contains the on-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the heat pump water heater. This parasitic electric load is consumed whenever the heat pump compressor is operating and the model assumes that this parasitic power does not contribute to heating the water. This parasitic load does, however, affect the zone air heat balance when the heat pump water heater sends some or all of its outlet air to a zone (i.e., Inlet Air Configuration field specified as ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’) and the Parasitic Heat Rejection Location field is specified as ‘Zone’. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
-
-#### Field: Off Cycle Parasitic Electric Load
-
-This numeric field contains the off-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the heat pump compressor. This parasitic electric load is consumed whenever the heat pump water heater is available but the compressor is not operating, and the model assumes that this parasitic power does not contribute to heating the water. This parasitic load does, however, affect the zone air heat balance when the heat pump water heater sends some or all of its outlet air to a zone (i.e., Inlet Air Configuration field specified as ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir’) and the Parasitic Heat Rejection Location field is specified as ‘Zone’. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
-
-#### Field: Parasitic Heat Rejection Location
-
-This alpha (choice) field determines where the on-cycle and off-cycle parasitic heat is rejected. Valid choices are Zone and Exterior. If ‘Zone’ is selected, both the on-cycle and off-cycle parasitic heat is rejected to the zone defined in the field Inlet Air Zone Name, and the Inlet Air Configuration must be ‘ZoneAirOnly’ or ‘ZoneAndOutdoorAir. If ’Outdoors’ is selected, this parasitic heat is rejected outdoors (does not impact the zone air heat balance) regardless of the specified Inlet Air Configuration. If this field is left blank, the default value is ’Outdoors’.
-
-#### Field: Inlet Air Mixer Node Name
-
-This optional alpha field defines the name of the HVAC node which represents the mixture of outdoor air and zone air that enters the heat pump air coil (evaporator) and fan section. The model mixes outdoor air with zone air and places the result on this inlet air mixer node based on the Inlet Air Mixer Schedule defined below. When the schedule value is equal to 0, 100% zone air enters the evaporator coil and fan section of the heat pump water heater. When the schedule value is equal to 1, 100% outdoor air enters the evaporator coil and fan section. This node name must be provided if the Inlet Air Configuration field above is specified as ‘ZoneAndOutdoor Air’, otherwise this field should be left blank.
-
-#### Field: Outlet Air Splitter Node Name
-
-This alpha field defines the name of the air node to which the heat pump air coil (evaporator) and fan sends all of its outlet air. The supply air flow downstream of this node is split between the zone and outdoors based on the Inlet Air Mixer schedule defined below. When the schedule value is equal to 0, the entire outlet air stream is diverted to the zone. When the schedule value is equal to 1, the entire outlet air stream is exhausted to outdoors. This node name must be provided if the Inlet Air Configuration field above is specified as ‘Zone and Outdoor Air’, otherwise this field should be left blank.
-
-#### Field: Inlet Air Mixer Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump draws its inlet air from the zone, outdoors, or a combination of zone and outdoor air. A schedule value equal to 0 indicates that the heat pump draws its inlet air from the zone. A schedule value equal to 1 denotes that the heat pump draws its inlet air from outdoors. Values between 0 and 1 denote a mixture of zone and outdoor air proportional to the schedule value. The Inlet Air Mixer schedule controls both the inlet air mixer and outlet air splitter nodes in unison to ensure that the operation of the heat pump does not contribute to zone pressurization or depressurization. For example if the Inlet Air Mixer schedule value is 0.4, then the inlet air mixer node is composed of 40% outdoor air and 60% zone air. For this same case, the outlet air splitter directs 60% of the HPWH outlet air back to the zone and 40% of the outlet air flow is exhausted outdoors. This schedule name must be provided if the Inlet Air Configuration field is specified as ‘Zone and Outdoor Air’, otherwise this field should be left blank.
-
-#### Field: Tank Element Control Logic
-
-This alpha field defines settings for the control logic of when to run the tank element in relation to whether the heat pump is running. 
-
-  - **MutuallyExclusive** means that once the tank heating element(s) are active, the heat pump is shut down until the heating element setpoint is reached. 
-  - **Simultaneous** (default) means that both the tank heating element and heat pump are used at the same time to recover the tank temperature. 
-
-#### Field: Control Sensor 1 Height In Stratified Tank
-
-This alpha field defines where the tank temperature is sensed for heat pump control when the tank type is `WaterHeater:Stratified`.  The stratified tank model produces tank temperature at different nodes in the vertical direction and various options are available for how this temperature should be sensed to control the heat pump.  This is measured in height from the bottom of the tank. Internally the appropriate node is determined based on this height. If omitted, this defaults to the height of Heater1.
-
-#### Field: Control Sensor 1 Weight
-
-The model can optionally use two control sensor locations in stratified tanks. When that is the case, the temperature sensed at each location is weighted. This alpha input specifies the weight associated with Control Sensor 1. It is input as a value between 0 and 1. The weight of Control Sensor 2 is determined by subtracting this weight from 1. The default for this field is 1, indicating that only Control Sensor 1 is used. 
-
-#### Field: Control Sensor 2 Height in Stratified Tank
-
-This alpha field defines the optional second location where the tank temperature is sensed for heat pump control when the tank type is `WaterHeater:Stratified`. If omitted, this defaults to the height of Heater2.
-
-Following is an example input for the `WaterHeater:HeatPump:WrappedCondenser` compound object and the other required component objects that it references.
-
-```idf
-WaterHeater:HeatPump:WrappedCondenser,
-    PlantHeatPumpWaterHeater,!- Name
-    PlantHPWHSch,            !- Availability Schedule Name
-    PlantHPWHTempSch,        !- Compressor Setpoint Temperature Schedule Name
-    3.89,                    !- Dead Band Temperature Difference {deltaC}
-    0.0664166667,            !- Condenser Bottom Location
-    0.8634166667,            !- Condenser Top Location
-    0.2279,                  !- Evaporator Air Flow Rate {m3/s}
-    OutdoorAirOnly,          !- Inlet Air Configuration
-    ,                        !- Air Inlet Node Name
-    ,                        !- Air Outlet Node Name
-    HPPlantAirInletNode,     !- Outdoor Air Node Name
-    HPPlantAirOutletNode,    !- Exhaust Air Node Name
-    ,                        !- Inlet Air Temperature Schedule Name
-    ,                        !- Inlet Air Humidity Schedule Name
-    ,                        !- Inlet Air Zone Name
-    WaterHeater:Stratified,  !- Tank Object Type
-    HPWHPlantTank,           !- Tank Name
-    HPWH Use Inlet Node,     !- Tank Use Side Inlet Node Name
-    HPWH Use Outlet Node,    !- Tank Use Side Outlet Node Name
-    Coil:WaterHeating:AirToWaterHeatPump:Wrapped,  !- DX Coil Object Type
-    HPWHPlantDXCoil,         !- DX Coil Name
-    7.2,                     !- Minimum Inlet Air Temperature for Compressor Operation {C}
-    Outdoors,                !- Compressor Location
-    ,                        !- Compressor Ambient Temperature Schedule Name
-    Fan:OnOff,               !- Fan Object Type
-    HPWHPlantFan,            !- Fan Name
-    DrawThrough,             !- Fan Placement
-    0,                       !- On Cycle Parasitic Electric Load {W}
-    0,                       !- Off Cycle Parasitic Electric Load {W}
-    ,                        !- Parasitic Heat Rejection Location
-    ,                        !- Inlet Air Mixer Node Name
-    ,                        !- Outlet Air Splitter Node Name
-    ,                        !- Inlet Air Mixer Schedule Name
-    MutuallyExclusive,       !- Tank Element Control Logic
-    1.262,                   !- Control Sensor 1 Height In Stratified Tank
-    0.75,                    !- Control Sensor 1 Weight
-    0.464;                   !- Control Sensor 2 Height In Stratified Tank
-```
-
-NOTE: branch object required only when tank use inlet nodes are used.
-
-```idf
-Branch,
-    Central HPWH Branch,     !- Name
-    0,                       !- Maximum Flow Rate {m3/s}
-    ,                        !- Pressure Drop Curve Name
-    WaterHeater:HeatPump:WrappedCondenser,    !- Component 1 Object Type
-    PlantHeatPumpWaterHeater,!- Component 1 Name
-    HPWH Use Inlet Node,     !- Component 1 Inlet Node Name
-    HPWH Use Outlet Node,    !- Component 1 Outlet Node Name
-    PASSIVE;                 !- Component 1 Branch Control Type
-
-WaterHeater:Stratified,
-    HPWHPlantTank,           !- Name
-    Water Heater,            !- End-Use Subcategory
-    0.287691,                !- Tank Volume {m3}
-    1.594,                   !- Tank Height {m}
-    VerticalCylinder,        !- Tank Shape
-    ,                        !- Tank Perimeter {m}
-    100,                     !- Maximum Temperature Limit {C}
-    MasterSlave,             !- Heater Priority Control
-    Plant Hot Water Setpoint Temp Schedule,  !- Heater 1 Setpoint Temperature Schedule Name
-    18.5,                      !- Heater 1 Deadband Temperature Difference {deltaC}
-    4500,                    !- Heater 1 Capacity {W}
-    1.129,                   !- Heater 1 Height {m}
-    Plant Hot Water Setpoint Temp Schedule,  !- Heater 2 Setpoint Temperature Schedule Name
-    18.5,                      !- Heater 2 Deadband Temperature Difference {deltaC}
-    0,                    !- Heater 2 Capacity {W}
-    0.266,                   !- Heater 2 Height {m}
-    Electricity,             !- Heater Fuel Type
-    1,                       !- Heater Thermal Efficiency
-    8.3,                     !- Off Cycle Parasitic Fuel Consumption Rate {W}
-    Electricity,             !- Off Cycle Parasitic Fuel Type
-    0,                       !- Off Cycle Parasitic Heat Fraction to Tank
-    1,                       !- Off Cycle Parasitic Height {m}
-    8.3,                     !- On Cycle Parasitic Fuel Consumption Rate {W}
-    Electricity,             !- On Cycle Parasitic Fuel Type
-    0,                       !- On Cycle Parasitic Heat Fraction to Tank
-    1,                       !- On Cycle Parasitic Height {m}
-    Outdoors,                !- Ambient Temperature Indicator
-    ,                        !- Ambient Temperature Schedule Name
-    ,                        !- Ambient Temperature Zone Name
-    ,                        !- Ambient Temperature Outdoor Air Node Name
-    0.7878,                  !- Uniform Skin Loss Coefficient per Unit Area to Ambient Temperature {W/m2-K}
-    1,                       !- Skin Loss Fraction to Zone
-    ,                        !- Off Cycle Flue Loss Coefficient to Ambient Temperature {W/K}
-    1,                       !- Off Cycle Flue Loss Fraction to Zone
-    0.001,                   !- Peak Use Flow Rate {m3/s}
-    ,                        !- Use Flow Rate Fraction Schedule Name
-    ,                        !- Cold Water Supply Temperature Schedule Name
-    HPWH Use Inlet Node,     !- Use Side Inlet Node Name
-    HPWH Use Outlet Node,    !- Use Side Outlet Node Name
-    1,                       !- Use Side Effectiveness
-    0,                       !- Use Side Inlet Height {m}
-    autocalculate,           !- Use Side Outlet Height {m}
-    HPPlantWaterOutletNode,  !- Source Side Inlet Node Name
-    HPPlantWaterInletNode,   !- Source Side Outlet Node Name
-    1,                       !- Source Side Effectiveness
-    0.7,                     !- Source Side Inlet Height {m}
-    0,                       !- Source Side Outlet Height {m}
-    Fixed,                   !- Inlet Mode
-    autosize,                !- Use Side Design Flow Rate {m3/s}
-    autosize,                !- Source Side Design Flow Rate {m3/s}
-    1.5,                     !- Indirect Water Heating Recovery Time {hr}
-    12;                      !- Number of Nodes
-
-OutdoorAir:Node,
-    HPWHPlantTank OA Node;   !- Name
-
-Coil:WaterHeating:AirToWaterHeatPump:Wrapped,
-    HPWHPlantDXCoil,               !- Name
-    2349.6,                  !- Rated Heating Capacity {W}
-    2.4,                     !- Rated COP {W/W}
-    0.981,                   !- Rated Sensible Heat Ratio
-    19.72,                   !- Rated Evaporator Inlet Air Dry-Bulb Temperature {C}
-    13.5,                    !- Rated Evaporator Inlet Air Wet-Bulb Temperature {C}
-    48.89,                   !- Rated Condenser Water Temperature {C}
-    0.189,                   !- Rated Evaporator Air Flow Rate {m3/s}
-    Yes,                     !- Evaporator Fan Power Included in Rated COP
-    HPPlantFanAirOutletNode, !- Evaporator Air Inlet Node Name
-    HPPlantAirOutletNode,    !- Evaporator Air Outlet Node Name
-    0,                       !- Crankcase Heater Capacity {W}
-    10,                      !- Maximum Ambient Temperature for Crankcase Heater Operation {C}
-    WetBulbTemperature,      !- Evaporator Air Temperature Type for Curve Objects
-    HPWH-Htg-Cap-fT,         !- Heating Capacity Function of Temperature Curve Name
-    ,                        !- Heating Capacity Function of Air Flow Fraction Curve Name
-    HPWH-Htg-COP-fT,         !- Heating COP Function of Temperature Curve Name
-    ,                        !- Heating COP Function of Air Flow Fraction Curve Name
-    HPWH-COP-fPLR;           !- Part Load Fraction Correlation Curve Name
-
-Fan:OnOff,
-    HPWHPlantFan,            !- Name
-    PlantHPWHSch,            !- Availability Schedule Name
-    0.1722,                  !- Fan Total Efficiency
-    65,                      !- Pressure Rise {Pa}
-    0.2279,                  !- Maximum Flow Rate {m3/s}
-    1,                       !- Motor Efficiency
-    0,                       !- Motor In Airstream Fraction
-    HPPlantAirInletNode,     !- Air Inlet Node Name
-    HPPlantFanAirOutletNode; !- Air Outlet Node Name
-```
-
-
-### Wrapped Condenser Heat Pump Water Heater Outputs
-
-* **HVAC,Average,Water Heater Compressor Part Load Ratio**
-
-* **HVAC,Average,Water Heater On Cycle Ancillary Electric Power [W]**
-
-* **HVAC,Sum,Water Heater On Cycle Ancillary Electric Energy [J]**
-
-* **HVAC,Average,Water Heater Off Cycle Ancillary Electric Power [W]**
-
-* **HVAC,Sum,Water Heater Off Cycle Ancillary Electric Energy [J]**
-
-
-
-#### Water Heater Compressor Part Load Ratio
-
-This output is the average part-load ratio of the heat pump water heater’s compressor (as well as its water pump and fan) for the timestep being reported. This output is independent of the “Water Heater Part Load Ratio� (Ref. Water Heater Outputs) which represents the part-load ratio of the supplemental heater (element or burner) in the water tank. When the water tank’s (supplemental) heater set point temperature is higher than the cut-in temperature of the heat pump water heater’s compressor, the heat pump compressor is disabled and the water tank’s heater (element or burner) is used to heat the water. During these times the Water Heater Compressor Part Load Ratio is equal to 0.
-
-#### Water Heater On Cycle Ancillary Electric Power [W]
-
-#### Water Heater On Cycle Ancillary Electric Energy [J]
-
-#### Water Heater Off Cycle Ancillary Electric Power [W]
-
-#### Water Heater Off Cycle Ancillary Electric Energy [J]
-
-These outputs are the parasitic electric power and consumption associated with the heat pump water heater. Specific outputs represent parasitic electrical usage during the compressor/fan on and off cycles. These outputs represent electronic controls or other electric component. The model assumes that the parasitic power does not contribute to heating the water, but it can impact the zone air heat balance depending on user inputs. The parasitic electric consumption outputs are also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
-
-
-Group – Condenser Equipment
----------------------------
-
-### Equipment Types
-
-In each CondenserEquipmentList, various equipment types and names must be given. Each type-name pair must then have a corresponding equipment definition. This subsection lists the various equipment types that are available and examples from an IDF. Where appropriate, notes and comments on the input structure are provided.
-
-### CoolingTower:SingleSpeed
-
-Cooling towers are components that may be assigned to condenser loops. The cooling tower is modeled as a counterflow heat exchanger with a single-speed fan (induced draft configuration) based on Merkel’s theory. The user must define tower performance via one of two methods: design heat transfer coefficient-area product (UA) and design water flow rate, or nominal tower capacity at a specific rating point. Regardless of which method is chosen, the design airflow rate and corresponding fan power must be specified. The model will also account for tower performance in the “free convection� regime, when the tower fan is off but the water pump remains on and heat transfer still occurs (albeit at a low level). If the user wants the model to account for “free convection�, they must specify the corresponding airflow rate and heat transfer coefficient-area product (UA), or the nominal tower capacity during this mode of operation.
-
-The cooling tower seeks to maintain the temperature of the water exiting the cooling tower at (or below) a set point. The set point schedule value is defined by the field “Condenser Loop Temperature Setpoint Node Name or Reference� for the CondenserLoop object. The model first checks to determine the impact of “free convection�, if specified by the user, on the tower exiting water temperature. If the exiting water temperature based on “free convection� is at or below the set point, then the tower fan is not turned on. If the exiting water temperature based on “free convection� is below the set point, the tower will operate in FluidBypass mode – portion of the water goes through the tower media and gets cooled while the remaining water flow gets bypassed, two water flows then mix together trying to meet the water setpoint temperature. If the exiting water temperature remains above the set point after “free convection� is modeled, then the tower fan is turned on to reduce the exiting water temperature to the set point. If the capacity control is FanCycling, the model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., tower fan on for the entire simulation timestep and tower fan off for the entire simulation timestep). Cyclic losses are not taken into account. If the capacity control is FluidBypass, the model determines the fraction of water flow to be bypassed while the remaining water goes through the tower cooling media and gets cooled, then the two water flows mix to meet the setpoint temperature. In this case, the fan runs at full speed for the entire timestep.
-
-Cooling towers here are “wet� and consume water through evaporation, drift, and blowdown. The model can be used to predict water consumed by the towers. The last six input fields are optional and provide methods of controlling details of the water consumption calculations. The user can specifiy connections to the rest of the buildings water system by providing the name of a water storage tanks (i.e. WaterUse:Storage objects).
-
-For the operation of multi-cell towers, the first step is to determine the number of cells to operate based on the cell control method – between the minimum number of cells subject to the maximum water flow rate fraction per cell, and maximum number of cells subject to the minimum water flow rate fraction per cell. If the calculated cells do not meet the loads, additional cells will be operating to help meet the loads. Inside each cell, the existing capacity controls still apply.
-
-For multi-cell towers, the following inputs are assumed to be for the entire tower including all cells:
-
-- Design Water Flow Rate; Design Air Flow Rate; Fan Power at Design Air Flow Rate;
-
-- Air Flow Rate in Free Convection Regime; Nominal Capacity; Free Convection Capacity
-
-- BASIN HEATER (we assume that there is a common basin)
-
-#### Field: Name
-
-This alpha field contains the identifying name for the cooling tower.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the identifying name for the cooling tower’s water inlet node.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the identifying name for the cooling tower’s water outlet node.
-
-#### Field: Design Water Flow Rate
-
-This numeric field contains the design water flow rate through the tower in m<sup>3</sup>/s. This value is the flow rate of the condenser loop water being cooled by the tower (not the flow rate of water being sprayed on the outside of the heat exchange coil). If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a water flow rate greater than zero must be defined or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections). If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically assumes a water flow rate of 5.382E-8 m3/s per watt (3 gpm/ton) of tower capacity specified in the field “Nominal Capacity�.
-
-#### Field: Design Air Flow Rate
-
-This numeric field contains the design air flow rate induced by the tower fan in m<sup>3</sup>/s. A value greater than zero must be defined regardless of the tower performance input method. Alternately, this field can be autosized. If autosized, the design air flow rate is calculated as follows:
-
-<div>\[Design\;Air\;Flow\;Rate = \frac{{0.5{\rho_{air}}(Fan\;power\;at\;Design\;Air\;Flow\;Rate)}}{{190.}}\]</div>
-
-where a fan pressure rise of 190 Pascals and total fan efficiency of 0.5 are assumed.
-
-***Field: Design Fan Power***
-
-This numeric field contains the fan power (in watts) at the design air flow rate specified in the previous field. A value greater than zero must be specified regardless of the tower performance input method, or this field can be autosized. If autosized, the fan power is calculated as follows:
-
-If“Performance Input Method� is specified as “*UFactorTimesAreaAndDesignWaterFlowRate*�, then
-
-<div>\[Fan\;power = 0.0105\cdot {\rho_{water}}\cdot {C_{p,water}}\cdot Design\;Water\;Flow\;Rate\cdot Design\;Loop\Delta T\]</div>
-
-is used.
-
-If“Performance Input Method� is specified as “*NominalCapacity*�, then
-
-<div>\[Fan\;power = 0.0105\cdot Tower\;Nominal\;Capacity\]</div>
-
-is used.
-
-#### Field: Design U-Factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the design air and water flow rates specified above. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design tower UA value is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), assuming a tower water inlet temperature of 35C and tower inlet air at 35C drybulb/25.6C wetbulb. If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field “Nominal Capacity�.
-
-#### Field:Free Convection Regime Air Flow Rate
-
-This numeric field contains the air flow rate (m<sup>3</sup>/s) when the tower is in the “free convection� regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field “Design Air Flow Rate�. This field may be autocalculated, in which case it is set to a fraction of the “Design Air Flow Rate� determined in the following input field. If the user does not wish to model “free convection� and is using the Performance Input Method “UFactorTimesAreaAndDesignWaterFlowRate�, then this field should be set to 0.0. If the user specifies the U-Factor Times Area Value at Free Convection Air Flow Rate or Free Convection Capacity as a value greater than zero, then the free convection air flow rate must be specified greater than 0.0.
-
-#### Field: Free Convection Regime Air Flow Rate Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the free convection regime air flow rate.  The default is 0.1.
-
-#### Field:Free Convection Regine U-Factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (W/K) when the tower is in the “free convection� regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field “U-Factor Times Area Value at Design Air Flow Rate�. This field may be autosized, in which case it is set to a fraction of the “U-Factor Times Area Value at Design Air Flow Rate� determined in the following input field. If the user does not wish to model “free convection� and is using the  Performance Input Method “UFactorTimesAreaAndDesignWaterFlowRate�, then this field should be set to 0.0. If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field “Free Convection Capacity�.\\
-
-#### Field: Free Convection U-Factor Times Area Value Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the free convection regime U-Factor times area value.  The default is 0.1.
-
-#### Field: Performance Input Method
-
-This alpha field contains the method by which the user will specify tower performance: “**UFactorTimesAreaAndDesignWaterFlowRate**� or “**NominalCapacity**�. If this field is left blank in the input data file, the default input method is assumed to be “**UFactorTimesAreaAndDesignWaterFlowRate**�. If the method “**UFactorTimesAreaAndDesignWaterFlowRate**� is selected, then the user must enter design UA values, design water flow rates and air flow rates as described for the previous input fields. If the method “NominalCapacity� is selected then the fields “Design Water Flow Rate�, “U-Factor Times Area Value at Design Air Flow Rate� and “U-Factor Times Area Value at Free Convection Air Flow Rate� must be left blank, but the fields “Nominal Capacity� and “Free Convection Capacity� must be entered as described below.
-
-#### Field: Heat Rejection Capacity and Nominal Capacity Sizing Ratio
-
-This numeric field contains the value for the ratio of actual tower heat rejection to nominal capacity.  This ratio is defined at entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. Historically this ratio has been set at 1.25 based on the assumption that the tower must dissipate 0.25 W of compressor power for every what of heat removed at the chiller evaporator.  The default is 1.25.
-
-#### Field: Nominal Capacity
-
-This numeric input field contains the “nominal� heat rejection capacity of the cooling tower in watts, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of nominal capacity (3 gpm/ton). The value in the previous field times this nominal tower capacity gives the actual tower heat rejection at these operating conditions (based on historical assumption that the tower must dissipate additional heat from the compressor heat for heat removed at the evaporator).
-
-#### Field: Free Convection Capacity
-
-This numeric input field contains the “nominal� heat rejection capacity of the cooling tower in watts when the tower is in the “free convection� regime (water flow exists but tower fan is turned off), with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of nominal tower capacity (input field above). The heat rejection capacity and nominal capacity sizing ratio is applied tof this free convection tower capacity to give the actual tower heat rejection at these operating conditions (typical value is 1.25 based on historical assumption that the tower must dissipate 0.25W of compressor heat for every watt of heat removed by the evaporator). The value specified for this field must be less than the value specified for the field “Tower Nominal Capacity�. If the user does not wish to model “free convection�, then this field should be set to 0.0. If the user specifies a value greater than zero, then the “Air Flow Rate in Free Convection Regime� field must contain a value greater than zero. This field can be automatically calculated using the sizing factor in the following field.
-
-#### Field: Free Convection Nominal Capacity Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the Free Convection Capacity. The default is 0.1.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the tower’s electric basin heater in watts per degree Kelvin. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the tower fan is off and water is not flowing through the tower, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the tower fan is off and water is not flowing through the tower. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the cooling tower fan is off and water is not flowing through the tower.
-
-#### Field: Evaporation Loss Mode
-
-This field is used to choose which method is used to model the amount of water evaporated by the cooling tower. There are two options: **LossFactor** or **SaturatedExit**. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the tower is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the cooling tower model (and does not require additional user input).
-
-#### Field: Evaporation Loss Factor
-
-This field is used to specify the rate of water evaporated from the cooling tower and lost to the outside air [percent/K]. This field is only used if the Evaporation Calculation Mode is set to **LossFactor**. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-degree Kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Typical values are from 0.15 to 0.27 [percent/K]. The default is 0.2.
-
-#### Field: Drift Loss Percent
-
-This field is used to specify the rate of water lost to the exiting air as entrained droplets [%]. The drift loss is a percent of the condenser water flow. Typical values for towers with efficient drift eliminators are between 0.002 and 0.2% of the condenser water flow rate. The default value is 0.008%.
-
-#### Field: Blowdown Calculation Mode
-
-This field specifies which method is used to determine blowdown rates. There two options **ConcentrationRatio** or **ScheduledRate**. The choice will determine which of the two models below is used. The default is ConcentrationRatio.
-
-#### Field: Blowdown Concentration Ratio
-
-This field is used to dynamically adjust the rate of blowdown in the cooling tower as a function of the rate of evaporation. Blowdown is water intentionally drained from the tower in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values for tower operation are 3 to 5. The default value is 3.
-
-#### Field: Blowdown Makeup Water Usage Schedule Name
-
-This alpha field contains the name of the schedule used to define the amount of water (m<sup>3</sup>/s) flushed from the basin on a periodic basis to purge the tower of mineral scale build-up and other contaminants. This schedule is only used if the Blowdown Calculation Mode is set to ScheduledRate. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Typical values range from 0.0002 to 0.0013 m<sup>3</sup>/s (17.3 to 112.3 m<sup>3</sup>/day). This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the cooling tower is active and water is flowing through the tower (regardless of the water usage defined by this schedule).
-
-#### Field: Supply Water Storage Tank Name
-
-This field is optional. It is used to describe where the tower obtains water used for evaporative cooling. If blank or omitted, then the tower will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the tower will obtain its water from that tank. If a tank is specified, the tower will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the tower needs, then the tower will still operate and obtain the rest of the water it needs from the mains (referred to as ‘Starved’ water).
-
-#### Field: Outdoor Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the cooling tower. If this field is left blank, the outdoor air conditions entering the cooling tower are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-#### Field:Capacity Control
-
-This alpha field contains the cooling capacity control for the cooling tower. Two choices are available: **FanCycling** and **FluidBypass**. During part-load conditions, there are two ways to maintain the exiting water temperature at the setpoint: either cycling the tower fan, or bypassing portion of the tower water with a three-way valve. For FluidBypass, the tower fan still runs at full speed for the entire timestep, but only portion of the water flow goes through the cooling tower media to get cooled while the remaining portion of the water flow gets bypassed. Two water flows then mix at the common water sump to meet the setpoint temperature.
-
-#### Field: Number of Cells
-
-This integer field contains the number of cells in the multi-cell cooling tower. If not entered, the program will assume it is a single-cell cooling tower
-
-#### Field: Cell Control
-
-This alpha field specifies the method used to control the number of cells used to meet the load, the two choices are:
-
-**MinimalCell** : the program will use minimal number of cells needed, all other cells will be shut down with no water flow. It will attempt to use as few cells as possible to cool the fluid. In no case, however, will the flow per cell be allowed to exceed its maximum value defined by the *Maximum Water Flow Rate Fraction.*
-
-**MaximalCell**: As many cells as possible will be turned on. In no case, however, will the flow per cell be allowed to drop below its minimum value specified by the *Minimum Water Flow Rate Fraction*.
-
-#### Field: Cell Minimum Water Flow Rate Fraction
-
-This numeric field specifies the allowable smallest fraction of the design water flow rate. Flows less than this value will commonly result in fluid distribution problems; the pressure at each nozzle will be too weak for the fluid to be sprayed out in the correct pattern, not all the fill would be wet. If this field is left blank, the default value is 0.33.
-
-#### Field: Cell Maximum  Water Flow Rate Fraction
-
-This numeric field specifies the allowable largest fraction of the design water flow rate. If this field is left blank, the default value is 2.5.
-
-***Field: Sizing Factor***
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature. For this component the inputs that would be altered by the sizing factor are:
-
-1.    Design Water Flow Rate;
-
-2.    Design Air Flow Rate;
-
-3.    Fan Power at Design Air Flow Rate;
-
-4.    U-Factor Times Area Value at Design Air Flow Rate;
-
-5.    Air Flow Rate in Free Convection Regime;
-
-6.    U-Factor Times Area Value at Free Convection Air Flow Rate.
-
-Note that the U-Factor Times Area Value at Design Air Flow Rate is not *multiplied* by the Sizing Factor. Instead the design tower load is multiplied by the sizing factor and the design UA then calculated as usual. The U-Factor Times Area Value at Free Convection Air Flow Rate is set to 10% of the new design Tower UA.
-
-Three examples of an IDF specification for this object are shown below:
-
-```idf
-CoolingTower:SingleSpeed,
-  My Tower,                     !- Name
-  Condenser Tower Inlet Node,   !- Water Inlet Node Name
-  Condenser Tower Outlet Node,  !- Water Outlet Node Name
-  .0011,                        !- Design Water Flow Rate (m3/s)
-  16.0,                         !- Design Air Flow Rate (m3/s)
-  10000.,                       !- Fan Power at Design Air Flow Rate (W)
-  3500.,  !- U-Factor Times Area Value at Design Air Flow Fate (W/C)
-  0.0,    !- Air Flow Rate in Free Convection Regime (m3/s)
-  0.0,    !- U-Factor Times Area Value at Free Convection Air Flow Rate (W/C)
-  UFactorTimesAreaAndDesignWaterFlowRate,!- Performance Input Method
-  ,                             !- Nominal Capacity (W)
-  ,                             !- Free Convection Capacity (W)
-  ,                             !- Basin Heater Capacity {W/K}
-  ,                             !- Basin Heater Setpoint Temperature {C}
-  ,                             !- Basin Heater Operating Schedule Name
-  ,                             !- Evaporation Loss Mode
-  ,                             !- Evaporation Loss Factor (percent/K)
-  ,                             !- Drift Loss Percent (percent)
-  ,                             !- Blowdown Calculation Mode
-  ,                             !- Blowdown Concentration Ratio
-  ,                             !- Blowdown Makeup Water Usage Schedule Name
-  ,                             !- Supply Water Storage Tank Name
-  ,                             !- Outdoor Air Inlet Node Name
-  FluidBypass,                  !- Capacity Control
-  4,                            !- Number of Cells
-  MinimalCell,                  !- Cell Control
-  0.25,                         !- Cell Minimum Water Flow Rate Fraction
-  1.50;                         !- Cell Maximum Water Flow Rate Fraction
-
-
-CoolingTower:SingleSpeed,
-  My Tower,                   !- Name
-  Condenser Tower Inlet Node, !- Water Inlet Node Name
-  Condenser Tower Outlet Node,!- Water Outlet Node Name
-  ,                           !- Design Water Flow Rate (m3/s)
-  autosize,                   !- Design Air Flow Rate (m3/s)
-  1000.,                      !- Fan Power at Design Air Flow Rate (W)
-  ,                !- U-Factor Times Area Value at Design Air Flow Fate (W/C)
-  autosize,        !- Air Flow Rate in Free Convection Regime (m3/s)
-  ,       !- U-Factor Times Area Value at Free Convection Air Flow Rate (W/C)
-  NominalCapacity,            !- Performance Input Method
-  95250.,                     !- Nominal Capacity (W)
-  9525.;                      !- Free Convection Capacity (W)
-
-
-CoolingTower:SingleSpeed,
-    TowerWaterSys CoolTower, !- Name
-    TowerWaterSys Pump-TowerWaterSys CoolTowerNode,  !- Water Inlet Node Name
-    TowerWaterSys Supply Equipment Outlet Node,  !- Water Outlet Node Name
-    AUTOSIZE,                !- Design Water Flow Rate {m3/s}
-    AUTOSIZE,                !- Design Air Flow Rate {m3/s}
-    AUTOSIZE,                !- Fan Power at Design Air Flow Rate {W}
-    AUTOSIZE,   !- U-Factor Times Area Value at Design Air Flow Rate {W/K}
-    AUTOSIZE,   !- Air Flow Rate in Free Convection Regime {m3/s}
-    AUTOSIZE,   !- U-Factor Times Area at Free Convection Air Flow Rate {W/K}
-    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
-    ,                        !- Nominal Capacity {W}
-    ,                        !- Free Convection Capacity {W}
-    ,                        !- Basin Heater Capacity {W/K}
-    ,                        !- Basin Heater Setpoint Temperature {C}
-    ,                        !- Basin Heater Operating Schedule Name
-    SaturatedExit,           !- Evaporation Loss Mode
-    ,                        !- Evaporation Loss Factor {percent/K}
-    0.0080,                  !- Drift Loss Percent {percent}
-    ConcentrationRatio,      !- Blowdown Calculation Mode
-    3.0000,                  !- Blowdown Concentration Ratio
-    ,                        !- Blowdown Makeup Water Usage Schedule Name
-    ,                        !- Supply Water Storage Tank Name
-    TowerWaterSys CoolTowerOA ref Node,  !- Outdoor Air Inlet Node Name
-    FanCycling,              !- Capacity Control
-    4,                       !- Number of Cells
-    MinimalCell,             !- Cell Control
-    0.25,                    !- Cell Minimum Water Flow Rate Fraction
-    1.50,                    !- Cell Maximum Water Flow Rate Fraction
-    1.0000;                  !- Sizing Factor
-```
-
-
-
-
-### Single Speed Cooling Tower Outputs
-
-* HVAC,Average,Cooling Tower Fan Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Fan Electric Energy [J]
-
-
-
-* HVAC,Average,Cooling Tower Heat Transfer Rate [W]
-
-* HVAC,Average,Cooling Tower Inlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Outlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Mass Flow Rate [kg/s]
-
-* HVAC,Average,Cooling Tower Bypass Fraction []
-
-* HVAC,Average,Cooling Tower Fan Cycling Ratio []
-
-* HVAC,Average,Cooling Tower Operating Cells Count []
-
-
-
-A tower uses either mains water or storage tank for make-up water.
-
-*When mains water is used:*
-
-* HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate  [m3/s]
-
-* HVAC,Sum,Cooling Tower Make Up Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Make Up Mains Water Volume [m3]
-
-
-
-*When storage tank water is used:*
-
-* HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate  [m3/s]
-
-* HVAC,Sum,Cooling Tower Make Up Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Make Up Mains Water Volume [m3]
-
-
-
-* HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Evaporation Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Drift Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Blowdown Volume [m3]
-
-
-
-
-IF specified:
-
-* HVAC,Average,Cooling Tower Basin Heater Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Basin Heater Electric Energy [J]
-
-
-
-#### Cooling Tower Fan Electric Power [W]
-
-#### Cooling Tower Fan Electric Energy [J]
-
-These outputs are the electric power input to the tower fans. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Cooling Tower Heat Transfer Rate [W]
-
-This is the rate at which heat is removed from the condenser water loop by the tower.
-
-#### Cooling Tower Inlet Temperature [C]
-
-#### Cooling Tower Outlet Temperature [C]
-
-#### Cooling Tower Mass Flow Rate [kg/s]
-
-These outputs are the tower water inlet and outlet temperatures, and mass flow rate of the circulating condenser water loop.
-
-#### Cooling Tower Basin Heater Electric Power [W]
-
-#### Cooling Tower Basin Heater Electric Energy [J]
-
-These outputs are the electric power input to the tower basin heater. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility
-
-#### Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Make Up Water Volume [m3]
-
-These outputs are the water consumed by the wet cooling tower for external water sprays used to augment heat transfer. This is the total of evaporation, drift, and blowdown.
-
-#### Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Evaporation Volume [m3]
-
-#### Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Drift Volume [m3]
-
-#### Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Blowdown Volume [m3]
-
-These outputs provide the breakdown of the different components of water use during cooling tower operation.
-
-#### Cooling Tower Make Up Mains Water Volume [m3]
-
-This is the volume of water drawn from mains service to feed the cooling tower.
-
-If a water storage tank is used to provide water to the tower, then the following output variables will also be available.
-
-#### Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Storage Tank Water Volume [m3]
-
-These are the rate and volume of water provided by the Water Storage Tank.
-
-#### Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Starved Storage Tank Water Volume [m3]
-
-These are the rate and volume of water the Storage Tank connections was not able to provide. The starved water is assumed to come from the mains. The tower’s operation is not affected by a lack of storage tank water.
-
-#### Cooling Tower Fan Cycling Ratio []
-
-This represents the fraction of a time-step when tower fan is on.
-
-#### Cooling Tower Bypass Fraction []
-
-This represents the fraction of a fluid bypassing the tower when a mixture of the tower fluid and tower return water is able to meet the set point temperature.
-
-#### Cooling Tower Operating Cells Count []
-
-This represents the number of cells operating at each time step.
-
-### CoolingTower:TwoSpeed
-
-The two-speed cooling tower is modeled in a similar fashion to the single-speed tower. The cooling tower is modeled as a counterflow heat exchanger with a two-speed fan (induced draft configuration) based on Merkel’s theory. The user must define tower performance via one of two methods: heat transfer coefficient-area product (UA) and design water flow rate, or nominal tower capacity at a specific rating point. Regardless of which method is chosen, the airflow rate and corresponding fan power at both high and low fan speed must be specified. The model will also account for tower performance in the “free convection� regime, when the tower fan is off but the water pump remains on and heat transfer still occurs (albeit at a low level). If the user wants the model to account for “free convection�, they must specify the corresponding air flow rate and heat transfer coefficient-area product (UA), or the nominal tower capacity during this mode of operation.
-
-The cooling tower seeks to maintain the temperature of the water exiting the cooling tower at (or below) a set point. The set point schedule value is defined by the field “Condenser Loop Temperature Setpoint Node Name or Reference� for the CondenserLoop object. The model first checks to determine the impact of “free convection�, if specified by the user, on the tower exiting water temperature. If the exiting water temperature based on “free convection� is at or below the set point, then the tower fan is not turned on. If the exiting water temperature remains above the set point after “free convection� is modeled, then the tower fan is turned on at low speed to reduce the exiting water temperature. If operating the tower fan at low speed does not reduce the exiting water temperature to the set point, then the tower fan is increased to its high speed.
-
-The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., tower fan at high speed for the entire simulation timestep and tower fan at low speed for the entire simulation timestep, or tower fan at low speed for the entire simulation timestep and tower fan off for the entire simulation timestep). Cyclic losses are not taken into account.
-
-Cooling towers here are “wet� and consume water through evaporation, drift, and blowdown. The model can be used to predict water consumed by the towers. The last six input fields are optional and provide methods of controlling details of the water consumption calculations. The user can specifiy connections to the rest of the buildings water system by providing the name of a WaterUse:Storage object.
-
-For the operation of multi-cell towers, the first step is to determine the number of cells to operate based on the cell control method – between the minimum number of cells subject to the maximum water flow rate fraction per cell, and maximum number of cells subject to the minimum water flow rate fraction per cell. If the calculated cells do not meet the loads, additional cells will be operating to help meet the loads. Inside each cell, the existing capacity controls still apply.
-
-For multi-cell towers, the following inputs are assumed to be for the entire tower including all cells:
-
-- Design Water Flow Rate; Design Air Flow Rate; Fan Power at Design Air Flow Rate;
-
-- Air Flow Rate in Free Convection Regime; Nominal Capacity; Free Convection Capacity
-
-- BASIN HEATER (we assume that there is a common basin)
-
-***Field: Name***
-
-This alpha field contains the identifying name for the cooling tower.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the identifying name for the cooling tower’s water inlet node.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the identifying name for the cooling tower’s water outlet node.
-
-#### Field: Design Water Flow Rate
-
-This numeric field contains the design water flow rate through the tower in m<sup>3</sup>/s. This value is the flow rate of the condenser loop water being cooled by the tower (not the flow rate of water being sprayed on the outside of the heat exchange coil). If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a water flow rate greater than zero must be defined or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections). If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically assumes a design water flow rate of 5.382E-8 m3/s per watt (3 gpm/ton) of tower capacity specified in the field “Tower High-Speed Nominal Capacity�.
-
-#### Field: High Fan Speed Air Flow Rate
-
-This numeric field contains the tower air flow rate at high fan speed in m<sup>3</sup>/s. A value greater than zero must be defined regardless of the tower performance input method. Alternately, this field can be autosized. If autosized, the design air flow rate is calculated as follows:
-
-<div>\[Air\,Flow\,Rate\,at\,High\,Fan\,Speed\, = \,\frac{{0.5{\rho_{air}}(Fan\,Power\,at\,High\,Fan\,Speed\,)}}{{190.}}\]</div>
-
-where a fan pressure rise of 190 Pascals and total fan efficiency of 0.5 are assumed.
-
-***Field: High Fan Speed Fan Power***
-
-This numeric field contains the fan power (in Watts) at the high-speed air flow rate specified in the previous field. A value greater than zero must be specified regardless of the tower performance input method, or this field can be autosized. If autosized, the fan power is calculated as follows:
-
-If“Performance Input Method� is specified as “*UFactorTimesAreaAndDesignWaterFlowRate*�, then
-
-<div>\[Fan\;powe{r_{High\;Fan\;Speed}} = 0.0105\cdot {\rho_{water}}\cdot {C_{p,water}}\cdot Design\;Water\;Flow\;Rate\cdot Design\;Loop\Delta T\]</div>
-
-is used.
-
-If“Performance Input Method� is specified as “*NominalCapacity*�, then
-
-<div>\[Fan\;powe{r_{High\;Fan\;Speed}} = 0.0105\cdot Tower\;High - Speed\;Nominal\;Capacity\]</div>
-
-is used.
-
-#### Field: High Fan Speed U-Factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (UA) in watts per degree Celsius corresponding to the high-speed air flow rate and design water flow rate specified above. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the tower UA value at high fan speed is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), assuming a tower water inlet temperature of 35C and tower inlet air at 35C drybulb/25.6C wetbulb. If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically calculates the tower UA based on the capacity specified in the field “High-Speed Nominal Capacity�.
-
-#### Field: Low Fan Speed Air Flow Rate
-
-This numeric field contains the tower air flow rate at low fan speed in m<sup>3</sup>/s. This value must be greater than zero, less than the value specified for the field “Air Flow Rate at High Fan Speed�, and greater than the value specified for the field “Air Flow Rate in Free Convection Regime�. This field may be autocalculated, in which case it is set to a fraction of the “Air Flow Rate at High Fan Speed� determined in the next field.
-
-#### Field: Low Fan Speed Air Flow Rate Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the low fan speed air flow rate.  The default is 0.5.
-
-#### Field: Low Fan Speed Fan Power
-
-This numeric field contains the fan power (in Watts) at the low-speed air flow rate specified in the previous field. This value must be specified greater than zero or the field may be autocalculated, in which case it is set to a fraction of the “Fan Power at High Fan Speed� determined in the next field.
-
-#### Field: Low Fan Speed Fan Power Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the low speed fan power.  The default is 0.16.
-
-#### Field: Low Fan Speed U-Factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (UA) in watts per degree Celsius corresponding to the design water flow rate and low-speed air flow rate specified above. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, this value must be greater than zero but less than or equal to 300,000, less than the value specified for the field “U-Factor Times Area Value at High Fan Speed�, and greater than the value specified for the field “U-Factor Times Area Value at Free Convection Air Flow Rate�. This field may be autocalculated, in which case it is set to a fraction of the “U-Factor Times Area Value at High Fan Speed� determined in the following field. If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field “Low Speed Nominal Capacity�.
-
-#### Field: Low Fan Speed U-Factor Times Area Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the low speed heat transfer coefficient-area product (UA).  The default is 0.6.
-
-#### Field: Free Convection Regime Air Flow Rate
-
-This numeric field contains the air flow rate (m<sup>3</sup>/s) when the tower is in the “free convection� regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field “Air Flow Rate at Low Fan Speed�. This field may be autocalculated, in which case it is set to a fraction of the “Air Flow Rate at High Fan Speed� determined in the following field. If the user does not wish to model “free convection� and is using the Performance Input Method “UFactorTimesAreaAndDesignWaterFlowRate�, then this field should be set to 0.0. If the user specifies the U-Factor Times Area Value at Free Convection Air Flow Rate or Free Convection Capacity as a value greater than zero, then the free convection air flow rate must be specified greater than 0.0.
-
-#### Field: Free Convection Air Flow Rate Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the free convection regime air flow rate.  The default is 0.1.
-
-#### Field: Free ConvectionU-Factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (W/°C) when the tower is in the “free convection� regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field “U-Factor Times Area Value at Low Fan Speed�. This field may be autocalculated, in which case it is set to a fraction of the “U-Factor Times Area Value at High Fan Speed� determined in the following field. If the user does not wish to model “free convection� and is using the Performance Input Method “UFactorTimesAreaAndDesignWaterFlowRate�, then this field should be set to 0.0. If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field “Free Convection Capacity�.
-
-#### Field: Free Convection U-Factor Times Area Value Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the free convection regime U-Factor times area value.  The default is 0.1.
-
-#### Field: Performance Input Method
-
-This alpha field contains the method by which the user will specify tower performance: “UFactorTimesAreaAndDesignWaterFlowRate� or “NominalCapacity�. If this field is left blank in the input data file, the default input method is assumed to be “UFactorTimesAreaAndDesignWaterFlowRate�. If the method “UFactorTimesAreaAndDesignWaterFlowRate� is selected, then the user must enter UA values, design water flow rate and air flow rates as described for the previous input fields. If the method “NominalCapacity� is selected then the fields “Design Water Flow Rate�, “U-Factor Times Area Value at High Fan Speed�, “U-Factor Times Area Value at Low Fan Speed� and “U-Factor Times Area Value at Free Convection Air Flow Rate� must be left blank, but the fields “High Speed Nominal Capacity�, “Low Speed Nominal Capacity� and “Free Convection Capacity� must be entered as described below.
-
-#### Field: Heat Rejection Capacity and Nominal Capacity Sizing Ratio
-
-This numeric field contains the value for the ratio of actual tower heat rejection to nominal capacity.  This ratio is defined at entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. Historically this ratio has been set at 1.25 based on the assumption that the tower must dissipate 0.25 W of compressor power for every what of heat removed at the chiller evaporator.  The default is 1.25.
-
-#### Field: High Speed Nominal Capacity
-
-This numeric input field contains the “nominal� heat rejection capacity of the cooling tower in watts under high-speed fan operation, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of high-speed nominal capacity (3 gpm/ton). The Heat Rejection Capacity and Nominal Capacity Sizing Ratio set in the previous field is applied to this nominal tower capacity to give the actual tower heat rejection at these operating.
-
-#### Field: Low Speed Nominal Capacity
-
-This numeric input field contains the “nominal� heat rejection capacity of the cooling tower in watts under low-speed fan operation, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of high-speed nominal tower capacity (input field above). The Heat Rejection Capacity and Nominal Capacity Sizing Ratio is applied to this nominal tower capacity to give the actual tower heat rejection at these operating conditions. The value specified for this field must be greater than zero but less than the value specified for the field “High-Speed Nominal Capacity�.  This field may be autocalculated, in which case it is set to a fraction of the High Speed Nominal Capacity determined in the following field.
-
-#### Field: Low Speed Nominal Capacity Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the Low Speed Nominal Capacity. The default is 0.5.
-
-#### Field: Free Convection Capacity
-
-This numeric input field contains the “nominal� heat rejection capacity of the cooling tower in watts when the tower is in the “free convection� regime (water flow exists but tower fan is turned off), with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of high-speed nominal tower capacity (input field above). The Heat Rejection Capacity and Nominal Capacity Sizing Ratio is applied to this free convection tower capacity to give the actual tower heat rejection at these operating conditions.The value specified for this field must be less than the value specified for the field “Tower Low-Speed Nominal Capacity�. If the user does not wish to model “free convection�, then this field should be set to 0.0. If the user specifies a value greater than zero, then the “Air Flow Rate in Free Convection Regime� field must contain a value greater than zero. This field may be autocalculated, in which case it is set to a fraction of the High Speed Nominal Capacity determined in the following field.
-
-#### Field: Free Convection Nominal Capacity Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the Free Convection Capacity. The default is 0.1.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the tower’s electric basin heater in watts per degree Kelvin. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the tower fan is off and water is not flowing through the tower, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the tower fan is off and water is not flowing through the tower. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the cooling tower fan is off and water is not flowing through the tower.
-
-#### Field: Evaporation Loss Mode
-
-This field is used to choose which method is used to model the amount of water evaporated by the cooling tower. There are two options: ‘LossFactor’ or ‘SaturatedExit’. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the tower is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the cooling tower model (and does not require additional user input).
-
-#### Field: Evaporation Loss Factor
-
-This field is used to specify the rate of water evaporated from the cooling tower and lost to the outside air [percent/K]. This field is only used if the Evaporation Calculation Mode is set to LossFactor. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-degree Kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Typical values are from 0.15 to 0.27 [percent/K]. The default is 0.2.
-
-#### Field: Drift Loss Percent
-
-This field is used to specify the rate of water lost to the exiting air as entrained droplets [%]. The drift loss is a percent of the condenser water flow. Typical values for towers with efficient drift eliminators are between 0.002 and 0.2% of the condenser water flow rate. The default value is 0.008%.
-
-#### Field: Blowdown Calculation Mode
-
-This field specifies which method is used to determine blowdown rates. There two options ConcentrationRatio or ScheduledRate. The choice will determine which of the two models below is used. The default is ConcentrationRatio
-
-#### Field: Blowdown Concentration Ratio
-
-This field is used to dynamically adjust the rate of blowdown in the cooling tower as a function of the rate of evaporation. Blowdown is water intentionally drained from the tower in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values for tower operation are 3 to 5. The default value is 3.
-
-#### Field: Blowdown Makeup Water Usage Schedule Name
-
-This alpha field contains the name of the schedule used to define the amount of water (m<sup>3</sup>/s) flushed from the basin on a periodic basis to purge the tower of mineral scale build-up and other contaminants. This schedule is only used if the Blowdown Calculation mode is set to ScheduledRate. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Typical values range from 0.0002 to 0.0013 m<sup>3</sup>/s (17.3 to 112.3 m<sup>3</sup>/day). This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the cooling tower is active and water is flowing through the tower (regardless of the water usage defined by this schedule).
-
-#### Field: Supply Water Storage Tank Name
-
-This field is optional. It is used to describe where the tower obtains water used for evaporative cooling. If blank or omitted, then the tower will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the tower will obtain its water from that tank. If a tank is specified, the tower will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the tower needs, then the tower will still operate and obtain the rest of the water it needs from the mains (referred to as ‘Starved’ water).
-
-#### Field: Outdoor Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the cooling tower. If this field is left blank, the outdoor air conditions entering the cooling tower are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-#### Field: Number of Cells
-
-This integer field contains the number of cells in the multi-cell cooling tower. If not entered, the program will assume it is a single-cell cooling tower
-
-#### Field: Cell Control
-
-This alpha field specifies the method used to control the number of cells used to meet the load, the two choices are:
-
-**MinimalCell**: the program will use minimal number of cells needed, all other cells will be shut down with no water flow. It will attempt to use as few cells as possible to cool the fluid. In no case, however, will the flow per cell be allowed to exceed its maximum value defined by the *Maximum Water Flow Rate Fraction.*
-
-**MaximalCell**: As many cells as possible will be turned on. In no case, however, will the flow per cell be allowed to drop below its minimum value specified by the *Minimum Water Flow Rate Fraction*.
-
-#### Field: Cell Minimum Water Flow Rate Fraction
-
-This numeric field specifies the allowable smallest fraction of the design water flow rate. Flows less than this value will commonly result in fluid distribution problems; the pressure at each nozzle will be too weak for the fluid to be sprayed out in the correct pattern, not all the fill would be wet. If this field is left blank, the default value is 0.33.
-
-#### Field: Cell Maximum  Water Flow Rate Fraction
-
-This numeric field specifies the allowable largest fraction of the design water flow rate. If this field is left blank, the default value is 2.5.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.For this component the inputs that would be altered by the sizing factor are:
-
-1.    Design Water Flow Rate;
-
-2.    Air Flow Rate at High Fan Speed;
-
-3.    Fan Power at High Fan Speed;
-
-4.    U-Factor Times Area Value at High Fan Speed;
-
-5.    Air Flow Rate at Low Fan Speed;
-
-6.    Fan Power at Low Fan Speed;
-
-7.    U-Factor Times Area Value at Low Fan Speed;
-
-8.    Air Flow Rate in Free Convection Regime;
-
-9.    U-Factor Times Area Value at Free Convection Air Flow Rate.
-
-Note that the U-Factor Times Area Value at High Fan Speed is not *multiplied* by the Sizing Factor. Instead the design tower load is multiplied by the sizing factor and the design UA then calculated as usual. The U-Factor Times Area Value at Low Fan Speed is set to a fraction of the full load design UA determined by the field Low Fan Speed U-Factor Times Area Sizing Factor. The U-Factor Times Area Value at Free Convection Air Flow Rate is set to a fraction of the design Tower UA determined by the field Free Convection Air U-Factor Times Area Value Sizing Factor.
-
-Four examples of an IDF specification for this object are shown below:
-
-
-
-```idf
-CoolingTower:TwoSpeed,
-   My Tower,                      !- Name
-   Condenser Tower Inlet Node,    !- Water inlet node name
-   Condenser Tower Outlet Node,   !- Water outlet node name
-   .0011,                         !- Design water flow rate, m3/s
-   16.0,                          !- Air flow rate at high fan speed, m3/s
-   10000,                         !- Fan power at high fan speed, W
-   3500.,                         !- Tower UA at high fan speed, W/C
-   8.0,                           !- Air flow rate at low fan speed, m3/s
-   1600,                          !- Fan power at low fan speed, W
-   2100.,                         !- Tower UA at low fan speed, W/C
-   1.6,                           !- Air flow rate for free convection, m3/s
-   350,                          !- Tower UA at free convection air flow, W/C
-   UFactorTimesAreaAndDesignWaterFlowRate; !- Tower performance input method
-
-
-  CoolingTower:TwoSpeed,
-    My Tower,                !- Name
-    Condenser Tower Inlet Node,   !- Water Inlet Node Name
-    Condenser Tower Outlet Node,  !- Water Outlet Node Name
-    ,                        !- Design Water Flow Rate {m3/s}
-    8.0,                     !- Air Flow Rate at High Fan Speed {m3/s}
-    500,                     !- Fan Power at High Fan Speed {W}
-    ,                   !- U-Factor Times Area Value at High Fan Speed {W/K}
-    4.0,                     !- Air Flow Rate at Low Fan Speed {m3/s}
-    125,                     !- Fan Power at Low Fan Speed {W}
-    ,                   !- U-Factor Times Area Value at Low Fan Speed {W/K}
-    0.8,                !- Air Flow Rate in Free Convection Regime {m3/s}
-    ,     !- U-Factor Times Area Value at Free Convection Air Flow Rate {W/K}
-    NominalCapacity,         !- Performance Input Method
-    20000.0,                 !- High Speed Nominal Capacity {W}
-    10000.0,                 !- Low Speed Nominal Capacity {W}
-    2000.0;                  !- Free Convection Capacity {W}
-
-
-CoolingTower:TwoSpeed,
-  Big Tower1,  !- Tower Name
-  Condenser Tower 1 Inlet Node,  !- Water Inlet Node Name
-  Condenser Tower 1 Outlet Node,  !- Water Outlet Node Name
-  ,  !- Design Water Flow Rate {m3/s}
-  8.0,  !- Design High Speed Air Flow Rate {m3/s}
-  500,  !- Fan Power at Design High Speed Air Flow Rate {W}
-  ,  !- Tower UA Value at Design High Speed Air Flow Rate {W/K}
-  4.0,  !- Design Low Speed Air Flow Rate {m3/s}
-  125,  !- Fan Power at Design Low Speed Air Flow Rate {W}
-  ,  !- Tower UA Value at Design Low Speed Air Flow Rate {W/K}
-  0.8,  !- Air Flow Rate in Free Convection Regime {m3/s}
-  ,  !- Tower UA Value at Free Convection Air Flow Rate {W/K}
-  NominalCapacity,  !- Tower Performance Input Method
-  20000.0,  !- Tower High Speed Nominal Capacity
-  10000.0,  !- Tower Low Speed Nominal Capacity
-  2000.0,  !- Tower Free Convection Nominal Capacity
-  ,        !- Basin Heater Capacity {W/K}
-  ,        !- Basin Heater Setpoint Temperature {C}
-  ,        !- Basin Heater Operating Schedule Name
-  SaturatedExit,  !- Evaporation Loss Mode
-  ,  !- Evaporation Loss Factor [%/C]
-  0.008 ,  !- Drift Loss Percent
-  ConcentrationRatio,  !- Blowdown Calculation Mode
-  3.0,  !- Blowdown Concentration Ratio
-  ,  !- Schedule Name for Makeup Water Usage due to Blowdown
-  Recovery Tank;  !- Name of Water Storage Tank for Supply
-
-
-CoolingTower:TwoSpeed,
-    TowerWaterSys CoolTower,   !- Name
-    TowerWaterSys Pump-TowerWaterSys CoolTowerNode,  !- Water Inlet Node Name
-    TowerWaterSys Supply Equipment Outlet Node,  !- Water Outlet Node Name
-    AUTOSIZE,                        !- Design Water Flow Rate {m3/s}
-    AUTOSIZE,                     !- Air Flow Rate at High Fan Speed {m3/s}
-    AUTOSIZE,                     !- Fan Power at High Fan Speed {W}
-    AUTOSIZE,           !- U-Factor Times Area Value at High Fan Speed {W/K}
-    AUTOSIZE,           !- Air Flow Rate at Low Fan Speed {m3/s}
-    AUTOSIZE,                     !- Fan Power at Low Fan Speed {W}
-    AUTOSIZE,           !- U-Factor Times Area Value at Low Fan Speed {W/K}
-    AUTOSIZE,           !- Air Flow Rate in Free Convection Regime {m3/s}
-    AUTOSIZE,   !- U-Factor Times Area at Free Convection Air Flow Rate {W/K}
-    UFactorTimesAreaAndDesignWaterFlowRate,     !- Performance Input Method
-    ,                 !- High Speed Nominal Capacity {W}
-    ,                 !- Low Speed Nominal Capacity {W}
-    ,                  !- Free Convection Capacity {W}
-    ,  !- Basin Heater Capacity {W/K}
-    ,  !- Basin Heater Setpoint Temperature {C}
-    ,  !- Basin Heater Operating Schedule Name
-    SaturatedExit,  !- Evaporation Loss Mode { LossFactor | SaturatedExit }
-    ,  !- Evaporation Loss Factor
-    0.0080,  !- Drift Loss Percent
-    ConcentrationRatio,  !- Blowdown Calculation Mode { ConcentrationRatio |
-                         !- ScheduledRate }
-    3.0000,  !- Blowdown Concentration Ratio
-    ,  !- Blowdown Makeup Water Usage Schedule Name
-    ,  !- Supply Water Storage Tank Name
-    TowerWaterSys CoolTower OA ref Node,  !- Outdoor Air Inlet Node Name
-    ,         !- Number of cells available
-    MinimalCell, !- Cell Control
-    ,        !- Cell Minimum Water Flow Rate Fraction
-    ,        !- Cell Maximum Water Flow Rate Fraction
-    1.0000;  !- Sizing Factor
-```
-
-
-### Two Speed Cooling Tower Outputs
-
-* HVAC,Average,Cooling Tower Fan Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Fan Electric Energy [J]
-
-* HVAC,Average,Cooling Tower Heat Transfer Rate [W]
-
-* HVAC,Average,Cooling Tower Inlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Outlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Mass Flow Rate [kg/s]
-
-* HVAC,Average,Cooling Tower Fan Cycling Ratio []
-
-* HVAC,Average,Cooling Tower Operating Cells Count []
-
-* HVAC,Average,Cooling Tower Fan Speed Level []
-
-* HVAC,Average,Cooling Tower Bypass Fraction []
-
-
-
-A tower uses either mains water or storage tank for make-up water.
-
-*When mains water is used:*
-
-* HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Make Up Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Make Up Mains Water Volume [m3]
-
-
-
-*When storage tank water is used:*
-
-* HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Make Up Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Make Up Mains Water Volume [m3]
-
-
-
-* HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Evaporation Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Drift Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Blowdown Volume [m3]
-
-
-
-
-IF specified:
-
-* HVAC,Average,Cooling Tower Basin Heater Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Basin Heater Electric Energy [J]
-
-
-
-#### Cooling Tower Fan Electric Power [W]
-
-#### Cooling Tower Fan Electric Energy [J]
-
-These outputs are the electric power input to the tower fans. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Cooling Tower Heat Transfer Rate [W]
-
-This is the rate at which heat is removed from the condenser water loop by the tower.
-
-#### Cooling Tower Inlet Temperature [C]
-
-#### Cooling Tower Outlet Temperature [C]
-
-#### Cooling Tower Mass Flow Rate [kg/s]
-
-These outputs are the tower water inlet and outlet temperatures, and mass flow rate.
-
-#### Cooling Tower Basin Heater Electric Power [W]
-
-#### Cooling Tower Basin Heater Electric Energy [J]
-
-These outputs are the electric power input to the tower basin heater. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility
-
-#### Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Make Up Water Volume [m3]
-
-These outputs are the water consumed by the wet cooling tower for external water sprays used to augment heat transfer. This is the total of evaporation, drift, and blowdown.
-
-#### Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Evaporation Volume [m3]
-
-#### Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Drift Volume [m3]
-
-#### Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Blowdown Volume [m3]
-
-These outputs provide the breakdown of the different components of water use during cooling tower operation.
-
-#### Cooling Tower Make Up Mains Water Volume [m3]
-
-This is the volume of water drawn from mains service to feed the cooling tower. If a water storage tank is used to provide water to the tower, then the following output variables will also be available.
-
-#### Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Storage Tank Water Volume [m3]
-
-These are the rate and volume of water provided by the Water Storage Tank.
-
-#### Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Starved Storage Tank Water Volume [m3]
-
-These are the rate and volume of water the Storage Tank connections was not able to provide. The starved water is assumed to come from the mains. The tower’s operation is not affected by a lack of storage tank water.
-
-#### Cooling Tower Fan Cycling Ratio []
-
-This represents the fraction of a time-step when tower fan is on. The fan can cycle at both speeds.
-
-#### Cooling Tower Operating Cells Count []
-
-This represents the number of cells operating at each time step.
-
-#### Cooling Tower Fan Speed Level []
-
-This represents the fan speed operating at each time step: 2 for High Speed, 1 for Low Speed, and 0 when the fan is OFF.
-
-### CoolingTower:VariableSpeed:Merkel
-
-This variable speed tower model is based on Merkel's theory and is similar to the single-speed and two-speed tower models.  The open wet cooling tower is modeled as a counter flow heat exchanger with a variable-speed fan drawing air through the tower (induced-draft configuration). The model also includes a “free convection� regime where cooling tower performance modeled with the fan off.
-
-For this model, Merkel’s theory is modified to include adjustments developed by Scheier to alter the heat transfer effectiveness based on current wetbulb, air flow rates, and water flow rates. The input requires performance curves or lookup tables to describe these three adjustment factors.
-
-For a multi-cell tower, the capacity and air/water flow rate inputs are for the entire tower.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the cooling tower.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the identifying name for the cooling tower’s water inlet node.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the identifying name for the cooling tower’s water outlet node.
-
-#### Field: Performance Input Method
-
-This alpha field contains the method by which the user will specify tower performance: “**UFactorTimesAreaAndDesignWaterFlowRate**� or “**NominalCapacity**�. If this field is left blank in the input data file, the default input method is assumed to be “**NominalCapacity**�. If the method “� is selected, then the user must enter design UA values, design water flow rates and air flow rates as described for the previous input fields. If the method “NominalCapacity� is selected then the fields “Design Water Flow Rate�, “U-Factor Times Area Value at Design Air Flow Rate� and “U-Factor Times Area Value at Free Convection Air Flow Rate� must be left blank, but the fields “Nominal Capacity� and “Free Convection Capacity� must be entered as described below.
-
-#### Field: Heat Rejection Capacity and Nominal Capacity Sizing Ratio
-
-This numeric field contains the value for the ratio of actual tower heat rejection to nominal capacity.  This ratio is defined at entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. Historically this ratio has been set at 1.25 based on the assumption that the tower must dissipate 0.25 W of compressor power for every what of heat removed at the chiller evaporator.  The default is 1.25.
-
-#### Field: Nominal Capacity
-
-This numeric input field contains the “nominal� heat rejection capacity of the cooling tower in watts under full-speed fan operation, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The Heat Rejection Capacity and Nominal Capacity Sizing Ratio set in the previous field is applied to this nominal tower capacity to give the actual tower heat rejection at these operating conditions.  This field can be autosized, in which case a Sizing:Plant object is needed for the condenser loop.
-
-#### Field: Free Convection Nominal Capacity
-
-This numeric input field contains the “nominal� heat rejection capacity of the cooling tower in watts when the tower is in the “free convection� regime (water flow exists but tower fan is turned off), with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The Heat Rejection Capacity and Nominal Capacity Sizing Ratio is applied to this free convection tower capacity to give the actual tower heat rejection at these operating conditions.The value specified for this field must be less than the value specified for the field “Tower Low-Speed Nominal Capacity�. If the user does not wish to model “free convection�, then this field should be set to 0.0. If the user specifies a value greater than zero, then the “Air Flow Rate in Free Convection Regime� field must contain a value greater than zero. This field may be autocalculated, in which case it is set to a fraction of the High Speed Nominal Capacity determined in the following field.
-
-#### Field: Free Convection Nominal Capacity Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the Free Convection Capacity. The default is 0.1.
-
-#### Field: Design Water Flow Rate
-
-This numeric field contains the design water flow rate through the tower in m<sup>3</sup>/s. This value is the flow rate of the condenser loop water being cooled by the tower. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a water flow rate greater than zero must be defined or the field can be autosized. If autosized, a Sizing:Plant object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections). If “Performance Input Method� is specified as “NominalCapacity�, then this field can be autocalculated using the sizing factor in the following field.
-
-#### Field: Design Water Flow Rate per Unit of Nominal Capacity
-
-This numeric field contains a scalable sizing factor for design water flow rate that scales with nominal capacity, in units of m<sup>3</sup>/s/W. The default value is 5.382\*10<sup>-8</sup>. This field is only used if the previous field is set to autocalculate and performance input method is NominalCapacity.  (If the performance input method is set to UFactorTimesAreaAndDesignWaterFlowRate then the design water flow rate is obtained from the plant sizing result.)
-
-#### Field: Design Air Flow Rate
-
-This numeric field contains the tower air flow rate at full fan speed, in m<sup>3</sup>/s.  The value can be autocalculated, in which case the air flow rate is based off of the scalable sizing factor in the following input field.
-
-#### Field: Design Air Flow Rate Per Unit of Nominal Capacity
-
-This numeric field contains the sizing factor to use when calculating the design air flow rate from the nominal capacity, in units of m<sup>3</sup>/s/W.  The default is 2.76316\*10<sup>-5</sup>.  When this field is left blank, then the default value is used but the flow rate is also scaled to account for elevation (with larger volume flow rates at higher altitudes).  When a hard value is entered, even if it is the same as the default, then the design air flow rate is not also adjusted for elevation and the scaling factor is used directly.
-
-#### Field: Minimum Air Flow Rate Ratio
-
-This numeric field contains the minimum air flow rate ratio. The tower fan is allowed to operate between the ratio defined here and a maximum air flow rate ratio of 1.0 (which corresponds to the design [maximum] tower air flow rate). Below this value the tower is assumed to operate in the “free convection� regime with the tower fan off. The minimum air flow rate ratio must be greater than or equal to 0.1 and less than or equal to 0.5, with a default value of 0.2 if the field is left blank.
-
-#### Field: Design Fan Power
-
-This numeric field contains the fan power in watts at the design (maximum) air flow rate through the tower. A value greater than zero must be specified or this field can be autocalculated. When the field is autocalculated the following input field is used to size the fan power based on nominal capacity.
-
-#### Field: Design Fan Power Per Unit of Nominal Capacity
-
-This numeric field contains the sizing factor to use when calculating the design fan power from the nominal capacity, in units of Watts per Watt. This field is only used if the previous is set to autocalculate. The default values is 0.0105.
-
-#### Field: Fan Power Modifier Function of Air Flow Rate Ratio Curve Name
-
-This alpha field contains the name of a curve or table object that describes fan power ratio (fan power/design fan power) as a function of air flow rate ratio (air flow rate/design air flow rate). The curve or table object must be for one independent variable, typically a cubic, and should be normalized to 1.0 at an air flow rate ratio of 1.0.  This field is required.
-
-#### Field: Free Convection Regime Air Flow Rate
-
-This numeric field contains the air flow rate (m<sup>3</sup>/s) when the tower is in the “free convection� regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field “Design Air Flow Rate�. This field may be autocalculated, in which case it is set to a fraction of the “Design Air Flow Rate� determined in the following input field. If the user does not wish to model “free convection� and is using the Performance Input Method “UFactorTimesAreaAndDesignWaterFlowRate�, then this field should be set to 0.0. If the user specifies the U-Factor Times Area Value at Free Convection Air Flow Rate or Free Convection Capacity as a value greater than zero, then the free convection air flow rate must be specified greater than 0.0.
-
-#### Field: Free Convection Regime Air Flow Rate Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the free convection regime air flow rate.  The default is 0.1.
-
-#### Field: Design Air Flow Rate U-Factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the design air and water flow rates specified above. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design tower UA value is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), assuming a tower water inlet temperature of 35C and tower inlet air at 35C drybulb/25.6C wetbulb. If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field “Nominal Capacity�.
-
-#### Field: Free Convection Regime U-Factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (W/K) when the tower is in the “free convection� regime (water flow exists but tower fan is turned off). This value must be less than the value specified for the field “U-Factor Times Area Value at Design Air Flow Rate�. This field may be autosized, in which case it is set to a fraction of the “U-Factor Times Area Value at Design Air Flow Rate� determined in the following input field. If the user does not wish to model “free convection� and is using the  Performance Input Method “UFactorTimesAreaAndDesignWaterFlowRate�, then this field should be set to 0.0. If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically calculates the tower UA based on the tower capacity specified in the field “Free Convection Capacity�.
-
-#### Field: Free Convection U-Factor Times Area Value Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the free convection regime U-Factor times area value.  The default is 0.1. This field is only used if the previous field is set to autocalculate and the performance input method is UFactorTimesAreaAndDesignWaterFlowRate.
-
-#### Field: U-Factor Times Area Modifier Function of Air Flow Ratio Curve Name
-
-This alpha field contains the name of a curve or table object that describes how the UA value varies as a function of air flow rate ratio (air flow rate/design air flow rate).  The result of this curve is multiplied by the design UA value to adjust for air flow rate, along with the two other modifiers discussed below.  The curve or table object must be for one independent variable and should be normalized to 1.0 at an air flow rate ratio of 1.0.  This field is required.
-
-#### Field: U-Factor Times Area Modifier Function of Wetbulb Temperature Difference Curve Name
-
-This alpha field contains the name of a curve or table object that describes how the UA value varies as a function of the current wetbulb temperature.  The result of this curve is multiplied by the design UA value to adjust for wetbulb temperatures that differ from design conditions at 25.56°C (78°F), along with the two other modifiers discussed in the previous and following fields.  The independe variable is the design wetbulb minus the current outdoor air wetbulb, in units of degrees Celsius.  The curve or table object must be for one independent variable and should be normalized to 1.0 at a wetbulb temperature difference of 0.0.  This field is required.
-
-#### Field: U-Factor Times Area Modifier Function of Water Flow Ratio Curve Name
-
-This alpha field contains the name of a curve or table object that describes how the UA value varies as a function of the current water flow rate ratio (water flow rate/design water flow rate). The result of this curve is multiplied by the design UA value to adjust for water flow rates that differ from design level, along with the other two modifiers discussed above. The curve or table object must be for one independent variable and should be normalized to 1.0 at a water flow ratio of 1.0.  This field is required
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the tower’s electric basin heater in watts per degree Kelvin. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the tower fan is off and water is not flowing through the tower, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the tower fan is off and water is not flowing through the tower. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the cooling tower fan is off and water is not flowing through the tower.
-
-#### Field: Evaporation Loss Mode
-
-This field is used to choose which method is used to model the amount of water evaporated by the cooling tower. There are two options: **LossFactor** or **SaturatedExit**. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the tower is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the cooling tower model (and does not require additional user input).
-
-#### Field: Evaporation Loss Factor
-
-This field is used to specify the rate of water evaporated from the cooling tower and lost to the outside air [percent/K]. This field is only used if the Evaporation Calculation Mode is set to **LossFactor**. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-degree Kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Typical values are from 0.15 to 0.27 [percent/K]. The default is 0.2.
-
-#### Field: Drift Loss Percent
-
-This field is used to specify the rate of water lost to the exiting air as entrained droplets [%]. The drift loss is a percent of the condenser water flow. Typical values for towers with efficient drift eliminators are between 0.002 and 0.2% of the condenser water flow rate. The default value is 0.008%.
-
-#### Field: Blowdown Calculation Mode
-
-This field specifies which method is used to determine blowdown rates. There two options **ConcentrationRatio** or **ScheduledRate**. The choice will determine which of the two models below is used. The default is ConcentrationRatio.
-
-#### Field: Blowdown Concentration Ratio
-
-This field is used to dynamically adjust the rate of blowdown in the cooling tower as a function of the rate of evaporation. Blowdown is water intentionally drained from the tower in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values for tower operation are 3 to 5. The default value is 3.
-
-#### Field: Blowdown Makeup Water Usage Schedule Name
-
-This alpha field contains the name of the schedule used to define the amount of water (m<sup>3</sup>/s) flushed from the basin on a periodic basis to purge the tower of mineral scale build-up and other contaminants. This schedule is only used if the Blowdown Calculation Mode is set to ScheduledRate. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Typical values range from 0.0002 to 0.0013 m<sup>3</sup>/s (17.3 to 112.3 m<sup>3</sup>/day). This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the cooling tower is active and water is flowing through the tower (regardless of the water usage defined by this schedule).
-
-#### Field: Supply Water Storage Tank Name
-
-This field is optional. It is used to describe where the tower obtains water used for evaporative cooling. If blank or omitted, then the tower will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the tower will obtain its water from that tank. If a tank is specified, the tower will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the tower needs, then the tower will still operate and obtain the rest of the water it needs from the mains (referred to as ‘Starved’ water).
-
-#### Field: Outdoor Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the cooling tower. If this field is left blank, the outdoor air conditions entering the cooling tower are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-#### Field: Number of Cells
-
-This integer field contains the number of cells in the multi-cell cooling tower. If not entered, the program will assume it is a single-cell cooling tower
-
-#### Field: Cell Control
-
-This alpha field specifies the method used to control the number of cells used to meet the load, the two choices are:
-
-**MinimalCell** : the program will use minimal number of cells needed, all other cells will be shut down with no water flow. It will attempt to use as few cells as possible to cool the fluid. In no case, however, will the flow per cell be allowed to exceed its maximum value defined by the *Maximum Water Flow Rate Fraction.*
-
-**MaximalCell**: As many cells as possible will be turned on. In no case, however, will the flow per cell be allowed to drop below its minimum value specified by the *Minimum Water Flow Rate Fraction*.
-
-#### Field: Cell Minimum  Water Flow Rate Fraction
-
-This numeric field specifies the allowable smallest fraction of the design water flow rate. Flows less than this value will commonly result in fluid distribution problems; the pressure at each nozzle will be too weak for the fluid to be sprayed out in the correct pattern, not all the fill would be wet. If this field is left blank, the default value is 0.33.
-
-#### Field: Cell Maximum Water Flow Rate Fraction
-
-This numeric field specifies the allowable largest fraction of the design water flow rate. If this field is left blank, the default value is 2.5.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-An example IDF specification follows.
-
-```idf
-  CoolingTower:VariableSpeed:Merkel,
-    Big Tower1, !- Name
-    Condenser Tower 1 Inlet Node, !- Water Inlet Node Name
-    Condenser Tower 1 Outlet Node, !- Water Outlet Node Name
-    NominalCapacity, !- Performance Input Method
-    1.25, !- Heat Rejection Capacity and Nominal Capacity Sizing Ratio
-    20000.0,  !- Nominal Capacity
-    autocalculate, !- Free Convection Nominal Capacity
-    0.1, !- Free Convection Nominal Capacity Sizing Factor
-    autocalculate, !- Design Water Flow Rate
-    5.382E-8, !- Design Water Flow Rate per Unit of Nominal Capacity
-    autocalculate, !- Design Air Flow Rate
-    2.76316E-5, !- Design Air Flow Rate Per Unit of Nominal Capacity
-    0.2, !- Minimum Air Flow Rate Ratio
-    autocalculate, !- Design Fan Power
-    0.0105, !- Design Fan Power Per Unit of Nominal Capacity
-    VS tower fan power mod func air flow ratio, !- Fan Power Modifier Function of Air Flow Rate Ratio Curve Name
-    autocalculate, !- Free Convection Regime Air Flow Rate
-    0.1, !- Free Convection Regime Air Flow Rate Sizing Factor
-    , !- Design Air Flow Rate U-Factor Times Area Value
-    , !- Free Convection Regime U-Factor Times Area Value
-    , !- Free Convection U-Factor Times Area Value Sizing Factor
-    VS tower UA mod func air flow ratio, !- U-Factor Times Area Modifier Function of Air Flow Ratio Curve Name
-    VS tower UA mod func wetbulb difference, !- U-Factor Times Area Modifier Function of Wetbulb Temperature Difference Curve Name
-    VS tower UA mod func water flow ratio; !- U-Factor Times Area Modifier Function of Water Flow Ratio Curve Name
-
-
-  Curve:Cubic,
-    VS tower fan power mod func air flow ratio, !- Name
-    0.02 , !- Coefficient1 Constant
-    0.0 ,  !- Coefficient2 x
-    0.0 ,  !- Coefficient3 x**2
-    0.98 , !- Coefficient4 x**3
-    0.2,   !- Minimum Value of x
-    1.0 ,  !- Maximum Value of x
-    0.0 ,  !- Minimum Curve Output
-    1.0 ,  !- Maximum Curve Output
-    Dimensionless,  !- Input Unit Type for X
-    Dimensionless;  !- Output Unit Type
-
-
-  Curve:Quadratic,
-    VS tower UA mod func air flow ratio, !- Name
-    0.0 , !- Coefficient1 Constant
-    1.3 , !- Coefficient2 x
-    -0.3 , !- Coefficient3 x**2
-    0.2 , !- Minimum Value of x
-    1.0 , !- Maximum Value of x
-    0.0 , !- Minimum Curve Output
-    1.0 , !- Maximum Curve Output
-    Dimensionless,  !- Input Unit Type for X
-    Dimensionless;  !- Output Unit Type
-
-
-  Curve:Linear,
-    VS tower UA mod func wetbulb difference , !- Name
-    1.0 , !- Coefficient1 Constant
-    0.0081 , !- Coefficient2 x
-    -10 , !- Minimum Value of x
-    25.0 , !- Maximum Value of x
-    0.85 , !- Minimum Curve Output
-    1.3 , !- Maximum Curve Output
-    Dimensionless,  !- Input Unit Type for X
-    Dimensionless; !- Output Unit Type
-
-
-  Curve:Quadratic,
-    VS tower UA mod func water flow ratio, !- Name
-    0.1082 , !- Coefficient1 Constant
-    1.667 , !- Coefficient2 x
-    -0.7713 , !- Coefficient3 x**2
-    0.3 , !- Minimum Value of x
-    1.0 , !- Maximum Value of x
-    0.5 , !- Minimum Curve Output
-    1.1 , !- Maximum Curve Output
-    Dimensionless,  !- Input Unit Type for X
-    Dimensionless;  !- Output Unit Type
-```
-
-
-
-### CoolingTower:VariableSpeed:Merkel Outputs
-
-* HVAC,Average,Cooling Tower Inlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Outlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Mass Flow Rate [kg/s]
-
-* HVAC,Average,Cooling Tower Heat Transfer Rate [W]
-
-* HVAC,Average,Cooling Tower Fan Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Fan Electric Energy [J]
-
-* HVAC,Average,Cooling Tower Operating Cells Count []
-
-* HVAC,Average,Cooling Tower Fan Speed Ratio []
-
-
-A tower uses either mains water or storage tank for make-up water.
-
-*When mains water is used:*
-
-* HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Make Up Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Make Up Mains Water Volume [m3]
-
-
-
-*When storage tank water is used:*
-
-* HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Make Up Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Make Up Mains Water Volume [m3]
-
-
-
-* HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Evaporation Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Drift Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Blowdown Volume [m3]
-
-
-
-IF specified:
-
-* HVAC,Average,Cooling Tower Basin Heater Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Basin Heater Electric Energy [J]
-
-
-#### Cooling Tower Fan Electric Power [W]
-
-#### Cooling Tower Fan Electric Energy [J]
-
-These outputs are the electric power input to the tower fans. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Cooling Tower Heat Transfer Rate [W]
-
-This is the rate at which heat is removed from the condenser water loop by the tower.
-
-#### Cooling Tower Inlet Temperature [C]
-
-#### Cooling Tower Outlet Temperature [C]
-
-#### Cooling Tower Mass Flow Rate [kg/s]
-
-These outputs are the tower water inlet and outlet temperatures, and mass flow rate.
-
-#### Cooling Tower Fan Speed Ratio
-
-This output is the air flow ratio.  The current air flow rate divided by the design air flow rate with values from 0.0 to 1.0.
-
-#### Cooling Tower Operating Cells Count []
-
-This represents the number of cells operating at each time step.
-
-#### Cooling Tower Basin Heater Electric Power [W]
-
-#### Cooling Tower Basin Heater Electric Energy [J]
-
-These outputs are the electric power input to the tower basin heater. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility
-
-#### Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Make Up Water Volume [m3]
-
-These outputs are the water consumed by the wet cooling tower for external water sprays used to augment heat transfer. This is the total of evaporation, drift, and blowdown.
-
-#### Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Evaporation Volume [m3]
-
-#### Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Drift Volume [m3]
-
-#### Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Blowdown Volume [m3]
-
-These outputs provide the breakdown of the different components of water use during cooling tower operation.
-
-#### Cooling Tower Make Up Mains Water Volume [m3]
-
-This is the volume of water drawn from mains service to feed the cooling tower. If a water storage tank is used to provide water to the tower, then the following output variables will also be available.
-
-#### Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Storage Tank Water Volume [m3]
-
-These are the rate and volume of water provided by the Water Storage Tank.
-
-#### Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Starved Storage Tank Water Volume [m3]
-
-These are the rate and volume of water the Storage Tank connections was not able to provide. The starved water is assumed to come from the mains. The tower’s operation is not affected by a lack of storage tank water.
-
-
-
-### CoolingTower:VariableSpeed
-
-The variable speed tower model is based on empirical curve fits of manufacturer’s performance data or field measurements. The user specifies tower performance at design conditions, and empirical curves are used to determine the approach temperature and fan power at off-design conditions. The user defines tower performance by entering the inlet air wet-bulb temperature, tower range, and tower approach temperature at the design conditions. The corresponding water flow rate (within ±25% of the tower’s rated water mass flow rate), air flow rate, and fan power must also be specified. The model will account for tower performance in the “free convection� regime, when the tower fan is off but the water pump remains on and heat transfer still occurs (albeit at a low level). Basin heater operation and makeup water usage (due to evaporation, drift, and blowdown) are also modeled.
-
-The cooling tower seeks to maintain the temperature of the water exiting the cooling tower at (or below) a set point. The set point schedule is defined by the field “Condenser Loop Temperature Setpoint Node Name or Reference� for the CondenserLoop object. The model first checks to determine the impact of “free convection� on the tower exiting water temperature. If the exiting water temperature based on “free convection� is at or below the set point, then the variable-speed tower fan is not turned on. If the exiting water temperature is above the set point after “free convection� is modeled, then the variable-speed tower fan is turned on to reduce the exiting water temperature. Tower fan power is calculated based on the tower air flow rate required to achieve the exiting water set point temperature.
-
-Cooling towers here are “wet� and consume water through evaporation, drift, and blowdown. The model can be used to predict water consumed by the towers. The last six input fields are optional and provide methods of controlling details of the water consumption calculations. The user can specifiy connections to the rest of the buildings water system by providing the name of a WaterUse:Storage object.
-
-For the operation of multi-cell towers, the first step is to determine the number of cells to operate based on the cell control method – between the minimum number of cells subject to the maximum water flow rate fraction per cell, and maximum number of cells subject to the minimum water flow rate fraction per cell. If the calculated cells do not meet the loads, additional cells will be operating to help meet the loads. Inside each cell, the existing capacity controls still apply.
-
-For multi-cell towers, the following inputs are assumed to be for the entire tower including all cells:
-
-- Design Water Flow Rate; Design Air Flow Rate; Fan Power at Design Air Flow Rate;
-
-- Air Flow Rate in Free Convection Regime; Nominal Capacity; Free Convection Capacity
-
-- BASIN HEATER (we assume that there is a common basin)
-
-#### Field: Name
-
-This alpha field contains the identifying name for the variable speed cooling tower.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the identifying name for the cooling tower’s water inlet node.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the identifying name for the cooling tower’s water outlet node.
-
-#### Field: Model Type
-
-This alpha field contains the type of empirical model used to simulate the tower’s thermal performance (approach temperature). Valid choices for this field are “CoolToolsCrossFlow�, “CoolToolsUserDefined�, “YorkCalc�, or “YorkCalcUserDefined�. “CoolToolsCrossFlow� and “YorkCalc� are empirical models with the equation form and model coefficients already defined within EnergyPlus. If “CoolToolsUserDefined� or “YorkCalcUserDefined� is selected, the user must specify a valid Model Coefficient Name in the next input field to reference an appropriate CoolingTowerPerformance:CoolTools or CoolingTowerPerformance:YorkCalc object. If a user-defined model type is selected and the specified Model Coefficient Name is not found in the input data file (idf), then a severe message is issued and the simulation will terminate.
-
-#### Field: Model Coefficient Name
-
-This alpha field contains the identifying name for the object(s) CoolingTowerPerformance:CoolTools or CoolingTowerPerformance:YorkCalc. A single model coefficient object may be used to define coefficients for multiple variable speed cooling tower objects (i.e., the same name may be used in this input field for more than one variable speed tower). This field is only used when the field Tower Model Type described above is set to “CoolToolsUserDefined� or “YorkCalcUserDefined�, and should be left blank otherwise.
-
-#### Field: Design Inlet Air Wet-Bulb Temperature
-
-This numeric field specifies the inlet air wet-bulb temperature (ËšC) at design conditions. This design temperature should correspond with the design values for range temperature, approach temperature, water flow rate, and air flow rate specified in the following fields. The minimum value for this field is 20ËšC and the default value is 25.6ËšC if this field is left blank.
-
-#### Field: Design Approach Temperature
-
-This numeric field specifies the tower approach temperature (ËšC) at design conditions. The approach temperature is the outlet water temperature minus the inlet air wet-bulb temperature. The design approach temperature should correspond with the design values for inlet air wet-bulb temperature, range temperature, water flow rate, and air flow rate specified for this tower. The value for this field must be greater than 0ËšC and the default value is 3.9ËšC if this field is left blank.
-
-#### Field: Design Range Temperature
-
-This numeric field specifies the range temperature (ËšC) at design conditions. The range temperature is defined as the inlet water temperature minus the outlet water temperature. The design range temperature should correspond with the design values for inlet air wet-bulb temperature, approach temperature, water flow rate, and air flow rate specified for this tower. The value for this field must be greater than 0ËšC and the default value is 5.6ËšC if this field is left blank.
-
-#### Field: Design Water Flow Rate
-
-This numeric field contains the design water flow rate through the tower in m<sup>3</sup>/s. The value entered should be within ±25% of the tower’s rated water mass flow rate as specified by the manufacturer if Model Type is “CoolToolsCrossFlow� or “YorkCalc�. This constraint may be different for Model Type “CoolToolsUserDefined� or “YorkCalcUserDefined� (ref. CoolingTowerPerformance:CoolTools or CoolingTowerPerformance:YorkCalc).
-
-This value is the flow rate of the condenser loop water being cooled by the tower. A value greater than zero must be specified or this field can be autosized. A Plant Sizing object must be defined if the field is autosized and the design water flow rate is then derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections). The design water flow rate should correspond with the design values specified for the inlet air wet-bulb temperature, approach temperature, range temperature, and air flow rate. When this field is not autosized, the condenser loop flow rate specified in other objects should be within ±25% of the tower’s rated water flow rate (different range is permissible if Model Type is “User Defined�).
-
-#### Field: Design Air Flow Rate
-
-This numeric field contains the design (maximum) air flow rate through the tower in m<sup>3</sup>/s. A value greater than zero must be specified or this field can be autosized. Autosizing of this field does not require a Plant Sizing object since the design air flow rate is assumed to be the design fan power multiplied by a total fan efficiency of 0.5 and divided by a fan pressure rise of 190 Pascals. A correction for altitude is also included as follows:
-
-<div>\[Design\;Air\;Flow\;Rate = \frac{{0.5(Fan\;power\;at\;Design\;Air\;Flow\;Rate)}}{{190.}}\left( {\frac{{101325.}}{{{P_{atm}}}}} \right)\]</div>
-
-#### Field: Design Fan Power
-
-This numeric field contains the fan power in watts at the design (maximum) air flow rate through the tower. A value greater than zero must be specified or this field can be autosized. If autosized, a Plant Sizing object must be defined and the fan power is calculated as follows:
-
-<div>\[Design\,fan\;power = 0.0105\cdot {\rho_{water}}\cdot {C_{p,water}}\cdot Design\;Water\;Flow\;Rate\cdot Design\;Loop\Delta T\]</div>
-
-#### Field: Fan Power Ratio Function of Air Flow Rate Ratio Curve Name
-
-This alpha field contains the curve object name for fan power ratio (fan power/design fan power) as a function of air flow rate ratio (air flow rate/design air flow rate) [ref. Performance Curves]. The curve object must be a cubic curve and should be normalized to 1.0 at an air flow rate ratio of 1.0. If this field is left blank, a theoretical fan curve is assumed where fan power ratio is directly proportional to the air flow rate ratio cubed.
-
-#### Field: Minimum Air Flow Rate Ratio
-
-This numeric field contains the minimum air flow rate ratio. The tower fan is allowed to operate between the ratio defined here and a maximum air flow rate ratio of 1.0 (which corresponds to the design [maximum] tower air flow rate). Below this value, the tower is assumed to operate either in the “free convection� regime with the tower fan off, or the tower fan is cycled on/off to maintain the exiting water set point temperature. The minimum air flow rate ratio must be greater than or equal to 0.2 and less than or equal to 0.5, with a default value of 0.2 if the field is left blank.
-
-#### Field: Fraction of Tower Capacity in Free Convection Regime
-
-This numeric field contains the fraction of tower capacity available in the free convection regime (i.e., when the tower fan is off but water continues to flow through the tower). The tower fan does not operate when the free convection tower capacity is able to meet or exceed the exiting water set point temperature. The air flow rate through the tower in the free convection regime is assumed to be this same fraction of the tower design air flow rate. The fraction of tower capacity in free convection regime must be greater than or equal to 0 and less than or equal to 0.2, with a default value of 0.125 if this field is left blank.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the tower’s electric basin heater in watts per degree Kelvin. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the tower fan is off and water is not flowing through the tower, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the tower fan is off and water is not flowing through the tower. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the cooling tower fan is off and water is not flowing through the tower.
-
-#### Field: Evaporation Loss Mode
-
-This field is used to choose which method is used to model the amount of water evaporated by the cooling tower. There are two options: ‘LossFactor’ or ‘SaturatedExit’. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the tower is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the cooling tower model (and does not require additional user input).
-
-#### Field: Evaporation Loss Factor
-
-This field is used to specify the rate of water evaporated from the cooling tower and lost to the outside air [percent/K]. This field is only used if the Evaporation Calculation Mode is set to LossFactor. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-degree Kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Typical values are from 0.15 to 0.27 [percent/K]. The default is 0.2.
-
-#### Field: Drift Loss Percent
-
-This numeric field contains the percent (%) of design water flow rate lost to the atmosphere at the design air flow rate due to drift, which is water droplets that are entrained in the airstream as it passes through the tower. Drift is assumed to vary directly with tower air flow rate ratio, and is in addition to the amount of water lost to the atmosphere due to evaporation and/or blowdown. Typical values for water usage due to drift are from 0.05 to 0.2% of the total water circulation rate with currently-available drift eliminators from tower manufacturers. The value entered in this field must be greater than or equal to zero, and the default is zero if the field is left blank.
-
-#### Field: Blowdown Calculation Mode
-
-This field specifies which method is used to determine blowdown rates. There two options ‘ConcentrationRatio’ or ‘ScheduledRate’. The choice will determine which of the two models below is used. The default is ConcentrationRatio.
-
-#### Field: Blowdown Concentration Ratio
-
-This field is used to dynamically adjust the rate of blowdown in the cooling tower as a function of the rate of evaporation. Blowdown is water intentionally drained from the tower in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Typical values for tower operation are 3 to 5. The default value is 3.
-
-#### Field: Blowdown Makeup Water Usage Schedule Name
-
-This alpha field contains the name of the schedule used to define the amount of water (m<sup>3</sup>/s) flushed from the basin on a periodic basis to purge the condenser loop of mineral scale build-up and other contaminants. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Typical values range from 0.0002 to 0.0013 m<sup>3</sup>/s (17.3 to 112.3 m<sup>3</sup>/day). This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the cooling tower is active and water is flowing through the tower (regardless of the water usage defined by this schedule).
-
-#### Field: Supply Water Storage Tank Name
-
-This field is optional. It is used to describe where the tower obtains water used for evaporative cooling. If blank or omitted, then the tower will obtain water directly from the mains. If the name of a WaterUser:Storage object is used here, then the tower will obtain its water from that tank. If a tank is specified, the tower will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the tower needs, then the tower will still operate and obtain the rest of the water it needs from the mains (referred to as ‘Starved’ water).
-
-#### Field: Outdoor Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the cooling tower. If this field is left blank, the outdoor air conditions entering the cooling tower are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-#### Field: Number of Cells
-
-This integer field contains the number of cells in the multi-cell cooling tower. If not entered, the program will assume it is a single-cell cooling tower
-
-#### Field: Cell Control
-
-This alpha field specifies the method used to control the number of cells used to meet the load, the two choices are:
-
-**MinimalCell**: the program will use minimal number of cells needed, all other cells will be shut down with no water flow. It will attempt to use as few cells as possible to cool the fluid. In no case, however, will the flow per cell be allowed to exceed its maximum value defined by the *Maximum Water Flow Rate Fraction.*
-
-**MaximalCel** : As many cells as possible will be turned on. In no case, however, will the flow per cell be allowed to drop below its minimum value specified by the *Minimum Water Flow Rate Fraction*.
-
-#### Field: Cell Minimum Water Flow Rate Fraction
-
-This numeric field specifies the allowable smallest fraction of the design water flow rate. Flows less than this value will commonly result in fluid distribution problems; the pressure at each nozzle will be too weak for the fluid to be sprayed out in the correct pattern, not all the fill would be wet. If this field is left blank, the default value is 0.33.
-
-#### Field: Cell Maximum  Water Flow Rate Fraction
-
-This numeric field specifies the allowable largest fraction of the design water flow rate. If this field is left blank, the default value is 2.5.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.For this component the inputs that would be altered by the sizing factor are:
-
-1.    Design Water Flow Rate;
-
-2.    Design Air Flow Rate;
-
-3.    Design Fan Power.
-
-An example IDF specification for this object is shown below:
-
-```idf
-CoolingTower:VariableSpeed,
-  Big Tower1,  !- Tower Name
-  Condenser 1 Inlet Node,  !- Water Inlet Node Name
-  Condenser 1 Outlet Node,  !- Water Outlet Node Name
-  YorkCalc,  !- Tower Model Type
-  ,  !- Tower Model Coefficient Name
-  25.5556,  !- Design Inlet Air Wet-Bulb Temperature {C}
-  3.8889,  !- Design Approach Temperature {C}
-  5.5556,  !- Design Range Temperature {C}
-  0.0015,  !- Design Water Flow Rate {m3/s}
-  1.6435,  !- Design Air Flow Rate {m3/s}
-  275,  !- Design Fan Power {W}
-  FanRatioCurve,  !- Fan Power Ratio - function of Air Flow Rate Curve Name
-  0.2,  !- Minimum Air Flow Rate Ratio
-  0.125,  !- Fraction of Tower Capacity in Free Convection Regime
-  450.0,  !- Basin Heater Capacity {W/K}
-  4.5,  !- Basin Heater Set Point Temperature {C}
-  BasinSchedule,  !- Basin Heater Operating Schedule Name
-  SaturatedExit,  !- Evaporation Loss Mode
-  ,  !- Evaporation Loss Factor
-  0.05,  !- Makeup Water Usage due to Drift {percent}
-  ScheduledRate,  !- Blowdown Calculation Mode
-  BlowDownSchedule,  !- Schedule Name for Makeup Water Usage due to Blowdown
-  ,  !- Name of Water Storage Tank for Supply
-  ,  !- Outdoor Air Inlet Node Name
-  4, !- Number of Cells
-  MinimalCell, !- Cell Control
-  ,  !- Cell Minimum Water Flow Rate Fraction
-  ,  !- Cell Maximum Water Flow Rate Fraction
-  1.000 ;  !- Sizing Factor
-```
-
-
-
-### Variable Speed Cooling Tower Outputs
-
-* HVAC,Average,Cooling Tower Fan Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Fan Electric Energy [J]
-
-
-
-* HVAC,Average,Cooling Tower Heat Transfer Rate [W]
-
-* HVAC,Average,Cooling Tower Inlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Outlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Mass Flow Rate [kg/s]
-
-* HVAC,Average,Cooling Tower Fan Part Load Ratio
-
-* HVAC,Average,Cooling Tower Air Flow Rate Ratio
-
-* HVAC,Average,Cooling Tower Operating Cells Count
-
-
-
-A tower uses either mains water or storage tank for make-up water.
-
-*When mains water is used:*
-
-* HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate  [m3/s]
-
-* HVAC,Sum,Cooling Tower Make Up Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Make Up Mains Water Volume [m3]
-
-
-
-*When storage tank water is used:*
-
-* HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate  [m3/s]
-
-* HVAC,Sum,Cooling Tower Make Up Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Cooling Tower Make Up Mains Water Volume [m3]
-
-
-
-* HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Evaporation Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Drift Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Blowdown Volume [m3]
-
-
-
-IF specified:
-
-* HVAC,Average,Cooling Tower Basin Heater Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Basin Heater Electric Energy [J]
-
-#### Cooling Tower Fan Electric Power [W]
-
-#### Cooling Tower Fan Electric Energy [J]
-
-These outputs are the electric power input to the tower fan. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Cooling Tower Fan Part Load Ratio []
-
-This is the on/off cycling rate of the tower fan when free convection cannot meet the set point temperature and the tower capacity at the minimum air flow rate ratio drives the tower exiting water temperature below the set point temperature. The fan part-load ratio is calculated as the ratio of the exiting water temperature in the free convection regime minus the exiting water temperature set point divided by the exiting water temperature in the free convection regime minus the exiting water temperature at the minimum air flow rate ratio. If tower air flow is at or above the minimum air flow rate ratio, then the tower fan part-load ratio is 1.0.
-
-#### Cooling Tower Heat Transfer Rate [W]
-
-This is the rate at which heat is removed from the condenser water loop by the tower.
-
-#### Cooling Tower Inlet Temperature [C]
-
-#### Cooling Tower Outlet Temperature [C]
-
-#### Cooling Tower Mass Flow Rate [kg/s]
-
-These outputs are the tower water inlet and outlet temperatures, and mass flow rate of the circulating condenser water loop.
-
-#### Cooling Tower Air Flow Rate Ratio []
-
-This is the ratio of air flow through the tower to the design air flow rate. During times when the tower can maintain the condenser loop set point temperature using free convection (when the fan in not operating), the air flow rate ratio is assumed to be equal to the field Fraction of Tower Capacity in Free Convection Regime. During times when the fan cycles on/off to maintain the outlet water set point temperature, the air flow rate ratio is calculated as the summation of Fan Part-Load Ratio multiplied by the Minimum Air Flow Rate Ratio and (1.0 - Fan Part-Load Ratio) multiplied by the fraction of Tower Capacity in Free Convection Regime.
-
-#### Cooling Tower Basin Heater Electric Power [W]
-
-#### Cooling Tower Basin Heater Electric Energy [J]
-
-These outputs are the electric power input to the tower basin heater. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Make Up Water Volume [m3]
-
-These outputs are the water consumed by the wet cooling tower for external water sprays used to augment heat transfer. This is the total of evaporation, drift, and blowdown.
-
-#### Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Evaporation Volume [m3]
-
-#### Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Drift Volume [m3]
-
-#### Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Blowdown Volume [m3]
-
-These outputs provide the breakdown of the different components of water use during cooling tower operation.
-
-#### Cooling Tower Make Up Mains Water Volume [m3]
-
-This is the volume of water drawn from mains service to feed the cooling tower.  If a water storage tank is used to provide water to the tower, then the following output variables will also be available.
-
-#### Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Storage Tank Water Volume [m3]
-
-These are the rate and volume of water provided by the Water Storage Tank.
-
-#### Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Starved Storage Tank Water Volume [m3]
-
-These are the rate and volume of water the Storage Tank connections was not able to provide. The starved water is assumed to come from the mains. The tower’s operation is not affected by a lack of storage tank water.
-
-#### Cooling Tower Operating Cells Count []
-
-This represents the number of cells operating at each time step.
-
-### CoolingTowerPerformance:CoolTools
-
-Variable speed cooling towers can be modeled by EnergyPlus with user-selectable performance based on the CoolTools correlation, YorkCalc correlation, or user-defined coefficients for either the CoolTools or YorkCalc correlations.The empirical CoolTools tower correlation uses a set of 35 coefficients to model the thermal performance (approach temperature) of a cooling tower based on four independent variables. If the user specifies Model Type = CoolToolsCrossFlow in the CoolingTower:VariableSpeed object, then the 35 coefficients derived for the CoolTools simulation model are used and these coefficients are already defined within EnergyPlus. If the user specifies Model Type = CoolToolsUserDefined, then the user must enter a CoolingTowerPerformance:CoolTools object to define the 35 coefficients that will be used by the CoolTools correlation.
-
-The user must specify a name for the model coefficient object, and this name must be used in the CoolingTower:VariableSpeed object (field Model Coefficient Name) to tell the program to use these coefficients. Next, the user enters the minimum and maximum values for inlet air wet-bulb temperature, range temperature, approach temperature, and water mass flow rate ratio to specify the valid range for which the model coefficients were derived. For all of these variables, the program issues warnings if the actual values are beyond the minimum/maximum values specified. For inlet air wet-bulb temperature and water mass flow rate ratio, the values of these variables used in the calculation of approach temperature are limited to be within the valid minimum/maximum range specified. For approach and range, the warnings are issued if the values are beyond the specified minimum/maximum range but the actual values are still used.
-
-The CoolTools correlation has four independent variables: inlet air wet-bulb temperature (Twb), tower range temperature (Tr), water flow rate ratio (FRwater), and air flow rate ratio (FRair). Temperatures are in units of ËšC and flow rate ratios are dimensionless (actual flow rate divided by design flow rate). Using these independent variables, tower approach temperature (ËšC) is calculated as follows:
-
-Approach =   Coeff(1)  +  Coeff(2)•FRair  +  Coeff(3)•(FRair)<sup>2</sup>  +
-
-Coeff(4)•(FRair)<sup>3</sup>  +  Coeff(5)•FRwater  +
-
-Coeff(6)•FRair•FRwater  +  Coeff(7)•(FRair)<sup>2</sup>•FRwater  +
-
-Coeff(8)•(FRwater)<sup>2</sup>  +  Coeff(9)•FRair•(FRwater)<sup>2</sup>  +
-
-Coeff(10)•(FRwater)<sup>3</sup>  +  Coeff(11)•Twb  +  Coeff(12)•FRair•Twb  +
-
-Coeff(13)•(FRair)<sup>2</sup>•Twb  +  Coeff(14)•FRwater•Twb  +
-
-Coeff(15)•FRair•FRwater•Twb  +  Coeff(16)•(FRwater)<sup>2</sup>•Twb  +
-
-Coeff(17)•(Twb)<sup>2</sup>  +  Coeff(18)•FRair•(Twb)<sup>2</sup>  +
-
-Coeff(19)•FRwater•(Twb)<sup>2</sup>  +  Coeff(20)•(Twb)<sup>3</sup>  +  Coeff(21)•Tr  +
-
-Coeff(22)•FRair•Tr  +  Coeff(23)•FRair•FRair•Tr  +
-
-Coeff(24)•FRwater•Tr  +  Coeff(25)•FRair•FRwater•Tr  +
-
-Coeff(26)•(FRwater)<sup>2</sup>•Tr  +  Coeff(27)•Twb•Tr  +
-
-Coeff(28)•FRair•Twb•Tr  +  Coeff(29)•FRwater•Twb•Tr  +
-
-Coeff(30)•(Twb)<sup>2</sup>•Tr  +  Coeff(31)•(Tr)<sup>2</sup> + Coeff(32)•FRair•(Tr)<sup>2 </sup> +
-
-Coeff(33)•FRwater•(Tr)<sup>2 </sup> +  Coeff(34)•Twb•(Tr)<sup>2 </sup> +  Coeff(35)•(Tr)<sup>3</sup>
-
-This object allows the user to specify model coefficients for use with the CoolTools correlation shown above. It is recommended that a broad set of cooling tower performance data be used to generate these model coefficients. The data set used to create the model coefficients should cover the entire range of water and air flow rate ratios and inlet air wet-bulb, range, and approach temperatures expected during the simulation.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the variable speed cooling tower model coefficients.
-
-#### Field: Minimum Inlet Air Wet-Bulb Temperature
-
-This numeric field contains the minimum inlet air wet-bulb temperature to be used by the model (approach temperature correlation). Inlet air wet-bulb temperatures less than this value will not be used; instead, the minimum inlet air wet-bulb temperature specified here will be used by the correlation and a warning will be issued.
-
-#### Field: Maximum Inlet Air Wet-Bulb Temperature
-
-This numeric field contains the maximum inlet air wet-bulb temperature to be used by the model (approach temperature correlation). Inlet air wet-bulb temperatures greater than this value will not be used; instead, the maximum inlet air wet-bulb temperature specified here will be used by the correlation and a warning will be issued.
-
-#### Field: Minimum Range Temperature
-
-This numeric field contains the minimum range temperature (inlet water temperature minus outlet water temperature) to be used by the empirical model. If the range temperature is less than this value the actual range temperature is still passed to the empirical model but a warning will be issued.
-
-#### Field: Maximum Range Temperature
-
-This numeric field contains the maximum range temperature (inlet water temperature minus outlet water temperature) to be used by the empirical model. If the range temperature is greater than this value the actual range temperature is still passed to the empirical model but a warning will be issued.
-
-#### Field: Minimum Approach Temperature
-
-This numeric field contains the minimum approach temperature (outlet water temperature minus inlet air wet-bulb temperature) to be used by the empirical model. If the calculated approach temperature is less than this value then the calculated value is still used but a warning will be issued.
-
-#### Field: Maximum Approach Temperature
-
-This numeric field contains the maximum approach temperature (outlet water temperature minus inlet air wet-bulb temperature) to be used by the empirical model. If the calculated approach temperature is greater than this value then the calculated value is still used but a warning will be issued.
-
-#### Field: Minimum Water Flow Rate Ratio
-
-This numeric field contains the minimum water flow rate ratio (ratio of actual water flow rate to rated water flow rate) to be used by the empirical model. Water flow rate ratios less than this value will not be used; instead, the minimum water flow rate ratio specified here will be used by the model and a warning will be issued.
-
-#### Field: Maximum Water Flow Rate Ratio
-
-This numeric field contains the maximum water flow rate ratio (ratio of actual water flow rate to rated water flow rate) to be used by the empirical model. Water flow rate ratios greater than this value will not be used; instead, the maximum water flow rate ratio specified here will be used by the model and a warning will be issued.
-
-#### Field: Coefficient 1 to 35
-
-These numeric fields contain the coefficients to be used by the CoolTools approach temperature correlation shown above.
-
-
-
-An example IDF specification for this object is shown below:
-
-```idf
-CoolingTowerPerformance:CoolTools,
- CoolTools CrossFlow Default Model, !- Tower Model Coefficient Name
-     -1.0,               !- Minimum Inlet Air Wet-Bulb Temperature {C}
-     26.6667,            !- Maximum Inlet Air Wet-Bulb Temperature {C}
-     1.1111,             !- Minimum Range Temperature {C}
-     11.1111,            !- Maximum Range Temperature {C}
-     1.1111,             !- Minimum Approach Temperature {C}
-     11.1111,            !- Maximum Approach Temperature {C}
-     0.75,               !- Minimum Water Flow Rate Ratio
-     1.25,               !- Maximum Water Flow Rate Ratio
-     0.52049709836241,                !- Coefficient 1
-   -10.617046395344,                  !- Coefficient 2
-    10.7292974722538,                 !- Coefficient 3
-    -2.74988377158227,                !- Coefficient 4
-     4.73629943913743,                !- Coefficient 5
-    -8.25759700874711,                !- Coefficient 6
-     1.57640938114136,                !- Coefficient 7
-     6.51119643791324,                !- Coefficient 8
-     1.50433525206692,                !- Coefficient 9
-    -3.2888529287801,                 !- Coefficient 10
-     0.0257786145353773,              !- Coefficient 11
-     0.182464289315254,               !- Coefficient 12
-    -0.0818947291400898,              !- Coefficient 13
-    -0.215010003996285,               !- Coefficient 14
-     0.0186741309635284,              !- Coefficient 15
-     0.0536824177590012,              !- Coefficient 16
-    -0.00270968955115031,             !- Coefficient 17
-     0.00112277498589279,             !- Coefficient 18
-    -0.00127758497497718,             !- Coefficient 19
-     0.0000760420796601607,           !- Coefficient 20
-     1.43600088336017,                !- Coefficient 21
-    -0.5198695909109,                 !- Coefficient 22
-     0.117339576910507,               !- Coefficient 23
-     1.50492810819924,                !- Coefficient 24
-    -0.135898905926974,               !- Coefficient 25
-    -0.152577581866506,               !- Coefficient 26
-    -0.0533843828114562,              !- Coefficient 27
-     0.00493294869565511,             !- Coefficient 28
-    -0.00796260394174197,             !- Coefficient 29
-     0.000222619828621544,            !- Coefficient 30
-    -0.0543952001568055,              !- Coefficient 31
-     0.00474266879161693,             !- Coefficient 32
-    -0.0185854671815598,              !- Coefficient 33
-     0.00115667701293848,             !- Coefficient 34
-     0.000807370664460284;            !- Coefficient 35
-```
-
-
-### CoolingTowerPerformance:CoolTools Outputs
-
-No additional cooling tower output variables are output when this object is used.
-
-### CoolingTowerPerformance:YorkCalc
-
-Variable speed cooling towers can be modeled by EnergyPlus with user-selectable performance based on the CoolTools correlation, YorkCalc correlation, or user-defined coefficients for either the CoolTools or YorkCalc correlations.The empirical YorkCalc tower correlation uses a set of 27 coefficients to model the thermal performance (approach temperature) of a variable speed cooling tower based on three independent variables. If the user specifies Tower Model Type = YorkCalc in the CoolingTower:VariableSpeed object, then the 27 coefficients derived for the YorkCalc simulation model are used and these coefficients are already defined within EnergyPlus. If the user specifies Tower Model Type = YorkCalcUserDefined, then the user must enter a CoolingTowerPerformance:YorkCalc object to define the 27 coefficients that will be used by the YorkCalc correlation.
-
-The user must specify a name for the model coefficient object, and this name must be used in the CoolingTower:VariableSpeed object (field Model Coefficient Name) to tell the program to use these coefficients. Next, the user enters the minimum and maximum values for inlet air wet-bulb temperature, range temperature, approach temperature, and water mass flow rate ratio to specify the valid range for which the model coefficients were derived. The user also specifies the maximum valid liquid-to-gas ratio. For all of these variables, the program issues warnings if the actual values are beyond the minimum/maximum values specified. For inlet air wet-bulb temperature and water mass flow rate ratio, the values of these variables used in the calculation of approach temperature are limited to be within the valid minimum/maximum range specified. For approach, range, and liquid-to-gas ratio the warnings are issued if the values are beyond the specified minimum/maximum range but the actual values are still used.
-
-The YorkCalc correlation has three independent variables: inlet air wet-bulb temperature (Twb), tower range temperature (Tr), and the liquid-to-gas ratio (ratio of water flow rate ratio to air flow rate ratio = LGRatio). Temperatures are in units of ËšC and liquid-to-gas ratio is dimensionless. Using these independent variables, an approach temperature (ËšC) is calculated as follows:
-
-    Approach =      Coeff(1)  +  Coeff(2)•Twb  +  Coeff(3)•Twb<sup>2 </sup> +  Coeff(4)•Tr  +
-
-Coeff(5)•Twb•Tr  +  Coeff(6)•Twb<sup>2</sup>•Tr  +  Coeff(7)•Tr<sup>2</sup>  +
-
-Coeff(8)•Twb•Tr<sup>2 </sup> +  Coeff(9)•Twb<sup>2</sup>•Tr<sup>2</sup> + Coeff(10)•LGRatio  +
-
-Coeff(11)•Twb•LGRatio  +  Coeff(12)•Twb<sup>2</sup>•LGRatio  +
-
-Coeff(13)•Tr•LGRatio  +  Coeff(14)•Twb•Tr•LGRatio  +
-
-Coeff(15)•Twb<sup>2</sup>•Tr•LGRatio  +  Coeff(16)•Tr<sup>2</sup>•LGRatio  +
-
-Coeff(17)•Twb•Tr<sup>2</sup>•LGRatio  +  Coeff(18)•Twb<sup>2</sup>•Tr<sup>2</sup>•LGRatio +
-
-Coeff(19)•LGRatio<sup>2 </sup> +  Coeff(20)•Twb•LGRatio<sup>2</sup>  +
-
-Coeff(21)• Twb<sup>2</sup>•LGRatio<sup>2 </sup> +  Coeff(22)•Tr•LGRatio<sup>2 </sup> +
-
-Coeff(23)•Twb•Tr•LGRatio<sup>2 </sup> +  Coeff(24)•Twb<sup>2</sup>•Tr•LGRatio<sup>2 </sup> +
-
-Coeff(25)•Tr<sup>2</sup>•LGRatio<sup>2 </sup> +  Coeff(26)•Twb•Tr<sup>2</sup>•LGRatio<sup>2 </sup> +
-
-Coeff(27)•Twb<sup>2</sup>•Tr<sup>2</sup>•LGRatio<sup>2</sup>
-
-This object allows the user to specify model coefficients for use with the YorkCalc correlation shown above. It is recommended that a broad set of cooling tower performance data be used to generate these model coefficients. The data set used to create the model coefficients should cover the entire range of water and air flow rate ratios and inlet air wet-bulb, range, and approach temperatures expected during the simulation.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the variable speed cooling tower model coefficients.
-
-#### Field: Minimum Inlet Air Wet-Bulb Temperature
-
-This numeric field contains the minimum inlet air wet-bulb temperature to be used by the model (approach temperature correlation). Inlet air wet-bulb temperatures less than this value will not be used; instead, the minimum inlet air wet-bulb temperature specified here will be used by the correlation and a warning will be issued.
-
-#### Field: Maximum Inlet Air Wet-Bulb Temperature
-
-This numeric field contains the maximum inlet air wet-bulb temperature to be used by the model (approach temperature correlation). Inlet air wet-bulb temperatures greater than this value will not be used; instead, the maximum inlet air wet-bulb temperature specified here will be used by the model and a warning will be issued.
-
-#### Field: Minimum Range Temperature
-
-This numeric field contains the minimum range temperature (inlet water temperature minus outlet water temperature) to be used by the empirical model. If the range temperature is less than this value the actual range temperature is still passed to the empirical model but a warning will be issued.
-
-#### Field: Maximum Range Temperature
-
-This numeric field contains the maximum range temperature (inlet water temperature minus outlet water temperature) to be used by the empirical model. If the range temperature is greater than this value the actual range temperature is still passed to the empirical model but a warning will be issued.
-
-#### Field: Minimum Approach Temperature
-
-This numeric field contains the minimum approach temperature (outlet water temperature minus inlet air wet-bulb temperature) to be used by the empirical model. If the calculated approach temperature is less than this value then the calculated value is still used but a warning will be issued.
-
-#### Field: Maximum Approach Temperature
-
-This numeric field contains the maximum approach temperature (outlet water temperature minus inlet air wet-bulb temperature) to be used by the empirical model. If the calculated approach temperature is greater than this value then the calculated value is still used but a warning will be issued.
-
-#### Field: Minimum Water Flow Rate Ratio
-
-This numeric field contains the minimum water flow rate ratio (ratio of actual water flow rate to rated water flow rate) to be used by the empirical model. Water flow rate ratios less than this value will not be used; instead, the minimum water flow rate ratio specified here will be used by the model and a warning will be issued.
-
-#### Field: Maximum Water Flow Rate Ratio
-
-This numeric field contains the maximum water flow rate ratio (ratio of actual water flow rate to rated water flow rate) to be used by the empirical model. Water flow rate ratios greater than this value will not be used; instead, the maximum water flow rate ratio specified here will be used by the model and a warning will be issued.
-
-#### Field: Maximum Liquid to Gas Ratio
-
-This numeric field contains the maximum liquid-to-gas ratio (ratio of actual water flow rate ratio [capped to be within the minimum/maximum water flow rate ratio defined above as necessary] to actual air flow rate ratio) to be used by the empirical model. If the liquid-to-gas ratio is greater than this value the actual liquid to gas ratio is still passed to the empirical model but a warning will be issued.
-
-#### Field: Coefficient 1 to 27
-
-These numeric fields contain the coefficients to be used by the YorkCalc approach temperature correlation shown above.
-
-An example IDF specification for this object is shown below:
-
-
-
-```idf
-CoolingTowerPerformance:YorkCalc
- YorkCalc Default Tower Model, !- Tower Model Coefficient Name
-     -34.4,              !- Minimum Inlet Air Wet-Bulb Temperature {C}
-     26.6667,            !- Maximum Inlet Air Wet-Bulb Temperature {C}
-     1.1111,             !- Minimum Range Temperature {C}
-     22.2222,            !- Maximum Range Temperature {C}
-     1.1111,             !- Minimum Approach Temperature {C}
-     40.0,               !- Maximum Approach Temperature {C}
-     0.75,               !- Minimum Water Flow Rate Ratio
-     1.25,               !- Maximum Water Flow Rate Ratio
-     8.0,                !- Maximum Liquid to Gas Ratio
-    -0.359741205,                     !- Coefficient 1
-    -0.055053608,                     !- Coefficient 2
-     0.0023850432,                    !- Coefficient 3
-     0.173926877,                     !- Coefficient 4
-    -0.0248473764,                    !- Coefficient 5
-     0.00048430224,                   !- Coefficient 6
-    -0.005589849456,                  !- Coefficient 7
-     0.0005770079712,                 !- Coefficient 8
-    -0.00001342427256,                !- Coefficient 9
-     2.84765801111111,                !- Coefficient 10
-    -0.121765149,                     !- Coefficient 11
-     0.0014599242,                    !- Coefficient 12
-     1.680428651,                     !- Coefficient 13
-    -0.0166920786,                    !- Coefficient 14
-    -0.0007190532,                    !- Coefficient 15
-    -0.025485194448,                  !- Coefficient 16
-     0.0000487491696,                 !- Coefficient 17
-     0.00002719234152,                !- Coefficient 18
-    -0.0653766255555556,              !- Coefficient 19
-    -0.002278167,                     !- Coefficient 20
-     0.0002500254,                    !- Coefficient 21
-    -0.0910565458,                    !- Coefficient 22
-     0.00318176316,                   !- Coefficient 23
-     0.000038621772,                  !- Coefficient 24
-    -0.0034285382352,                 !- Coefficient 25
-     0.00000856589904,                !- Coefficient 26
-    -0.000001516821552;               !- Coefficient 27
-```
-
-
-### CoolingTowerPerformance:YorkCalc Outputs
-
-No additional cooling tower output variables are output when this object is used.
-
-### EvaporativeFluidCooler:SingleSpeed
-
-Evaporative fluid coolers are components that may be assigned to condenser loops. The Evaporative fluid cooler is modeled as a counter flow heat exchanger with single-speed fans (induced draft configuration). The user must define fluid cooler performance via one of three methods: design heat transfer coefficient-area product (UA) and design water flow rate, or standard fluid cooler design capacity at a specific rating point or design capacity at non standard conditions. Regardless of which method is chosen, the design airflow rate and corresponding fan power must be specified.
-
-The evaporative fluid cooler seeks to maintain the temperature of the water exiting the evaporative fluid cooler at (or below) a set point. The set point schedule value is defined by the field “Condenser Loop Temperature Setpoint Node Name or Reference� for the CondenserLoop object. The model first checks to see whether inlet water temperature is at or below the set point. If so, then the fluid cooler fan is not turned on and all the flow goes through bypass. If the inlet water temperature is above the set point then the fluid cooler fan is turned on to reduce the exiting water temperature to the set point. If the capacity control is FanCycling, the model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., fluid cooler fan on for the entire simulation timestep and fluid cooler fan off for the entire simulation timestep). Cyclic losses are not taken into account. If the capacity control is FluidBypass, the model determines the fraction of water flow to be bypassed while the remaining water goes through the fluid cooler cooling media and gets cooled, then the two water flows mix to meet the setpoint temperature. In this case, the fan runs at full speed for the entire timestep.
-
-Evaporative fluid coolers consume water through evaporation, drift, and blowdown. The model can be used to predict water consumed by the fluid coolers. For this purpose, the last seven input fields can either be provided in the input or if nothing is specified then the default values for these fields will be used. These fields provide the methods of controlling details of the water consumption calculations. The user can specify connections to the rest of the building’s water system by providing the name of a water storage tanks (i.e. WaterUse:Storage objects). The schematic of the system is shown below:
-
-![EvaporativeFluidCooler](media/image201.svg)
-
-Figure 82. Schematic diagram for evaporative fluid cooler
-
-Where,
-
-* h = Enthalpy (j/kg-K)
-
-* m = mass flow rate (kg/s)
-
-* Subscripts
-
-* a = air
-
-* w = water
-
-* wb = wet-bulb
-
-* in = inlet
-
-* out= outlet
-
-
-#### Field: Name
-
-This alpha field contains the identifying name for the fluid cooler.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the identifying name for the fluid cooler’s water inlet node.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the identifying name for the fluid cooler’s water outlet node.
-
-#### Field: Design Air Flow Rate
-
-This numeric field contains the design air flow rate induced by the fluid cooler fan in m<sup>3</sup>/s. The field must contain a value greater than zero regardless of the fluid cooler performance input method. Alternately, this field can be autosized. See Engineering Reference document for autosizing calculations.
-
-#### Field: Design Air Flow Rate Fan Power
-
-This numeric field contains the fan power (in watts) at the design air flow rate specified in the previous field. The field must contain a value greater than zero regardless of the fluid cooler performance input method. Alternately, this field can be autosized. See Engineering Reference document for autosizing calculations.
-
-#### Field: Design Spray Water Flow Rate
-
-This numeric field contains the design spray water flow rate through the fluid cooler in m<sup>3</sup>/s. A value greater than zero must be specified regardless of the performance input method,
-
-#### Field: Performance Input Method
-
-This alpha field contains the method by which the user will specify fluid cooler performance: “UFactorTimesAreaAndDesignWaterFlowRate� or “StandardDesignCapacity� or “UserSpecifiedDesignCapacity�.
-
-#### Field: Outdoor Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the fluid cooler. If this field is left blank, the outdoor air conditions entering the fluid cooler are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-#### Field: Heat Rejection Capacity and Nominal Capacity Sizing Ratio
-
-This numeric field contains the value for the ratio of actual tower heat rejection to nominal capacity.  This ratio is defined at entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. Historically this ratio has been set at 1.25 based on the assumption that the tower must dissipate 0.25 W of compressor power for every what of heat removed at the chiller evaporator.  The default is 1.25.
-
-#### Field: Standard Design Capacity
-
-This numeric input field contains the heat rejection capacity of the fluid cooler in watts, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of nominal capacity (3 gpm/ton). 125% of this capacity gives the actual fluid cooler heat rejection at these operating conditions (based on historical assumption that the evaporative fluid cooler must dissipate 0.25W of compressor heat for every watt of heat removed by the evaporator). This field is only used for performance input method =�StandardDesignCapacity�. For other input methods this field is ignored. The standard conditions mentioned above for “standard design capacity� are already specified in the EnergyPlus. So the input fields such as design entering water temp., design entering air wet-bulb and dry-bulb temp. and design water flow rate, if provided in the input, will be ignored for the StandardDesignCapacity performance input method. Also, the standard conditions are for water as a fluid type so this performance input method can only be used with water as a fluid type (ref. CondenserLoop object).
-
-#### Field: Design Air Flow Rate U-factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the design air and water flow rates specified above. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design fluid cooler UA value is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), the fluid cooler inlet air dry-bulb and wetbulb temperature are taken from the input. This field is only used for performance input method =� UFactorTimesAreaAndDesignWaterFlowRate�. For other performance input methods, this field is ignored.
-
-#### Field: Design Water Flow Rate
-
-This numeric field contains the design water flow rate through the fluid cooler in m<sup>3</sup>/s. This value is the flow rate of the condenser loop water being cooled by the fluid cooler. This field is ignored for the “StandardDesignCapacity� performance input method. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections).
-
-#### Field: User Specified Design Capacity
-
-This numeric input field contains the heat rejection capacity of the fluid cooler in watts. Design conditions for this capacity i.e. entering air dry-bulb temperature, entering air wet-bulb temperature and entering water temperature must be provided in the input. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
-
-#### Field:Design Entering Water Temperature
-
-This numeric field contains entering water temperature at nominal conditions in degrees Celsius. The design entering water temperature must be greater than the design entering air temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
-
-#### Field:Design Entering Air Temperature
-
-This numeric field contains entering air dry-bulb temperature at nominal conditions in degrees Celsius. The design entering air temperature must be greater than the design entering air wet-bulb temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
-
-#### Field:Design Entering Air Wet-bulb Temperature
-
-This numeric field contains entering air wetbulb temperature at nominal conditions in degrees Celsius. The design entering air wet-bulb temperature must be less than the design entering air (dry-bulb) temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
-
-#### Field: Capacity Control
-
-This alpha field contains the cooling capacity control for the evaporative fluid cooler. Two choices are available: FanCycling and FluidBypass. During part-load conditions, there are two ways to maintain the exiting water temperature at the setpoint: either cycling the evaporative fluid cooler fan, or bypassing portion of the evaporative fluid cooler water with a three-way valve. For FluidBypass, the evaporative fluid cooler fan still runs at full speed for the entire timestep, but only portion of the water flow goes through the evaporative fluid cooler media to get cooled while the remaining portion of the water flow gets bypassed. Two water flows then mix at the common water sump to meet the setpoint temperature.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature. For this component the inputs that would be altered by the sizing factor are:
-
-1.   Design Water Flow Rate;
-
-2.   Design Air Flow Rate;
-
-3.   Fan Power at Design Air Flow Rate;
-
-4.   U-Factor Times Area Value at Design Air Flow Rate;
-
-Note that the U-Factor Times Area Value at Design Air Flow Rate is not multiplied by the Sizing Factor. Instead the design evaporative fluid cooler load is multiplied by the sizing factor and the design UA then calculated as usual.
-
-#### Field: Evaporation Loss Mode
-
-This field is used to choose which method is used to model the amount of water evaporated by the evaporative fluid cooler. There are two options: LossFactor or SaturatedExit. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the evaporative fluid cooler is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the evaporative fluid cooler model (and does not require additional user input).
-
-#### Field: Evaporation Loss Factor
-
-This field is used to specify the rate of water evaporated from the evaporative fluid cooler and lost to the outside air [percent/K]. This field is only used if the Evaporation Calculation Mode is set to LossFactor. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Empirical correlation is used to calculate default loss factor if it not explicitly specified in the input file.
-
-#### Field: Drift Loss Percent
-
-This field is used to specify the rate of water lost to the exiting air as entrained droplets [%]. The drift loss is a percent of the condenser water flow. Default value is under investigation for now cooling tower’s evaporation loss factor is taken as default value.
-
-#### Field: Blowdown Calculation Mode
-
-This field specifies which method is used to determine blowdown rates. There two options ConcentrationRatio or ScheduledRate. The choice will determine which of the two models below is used. The default is ConcentrationRatio.
-
-#### Field: Blowdown Concentration Ratio
-
-This field is used to dynamically adjust the rate of blowdown in the evaporative fluid cooler as a function of the rate of evaporation. Blowdown is water intentionally drained from the evaporative fluid cooler in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Default value is under investigation for now cooling tower’s evaporation loss factor is taken as default value.
-
-#### Field: Blowdown Makeup Water Usage Schedule Name
-
-This alpha field contains the name of the schedule used to define the amount of water (m3/s) flushed from the basin on a periodic basis to purge the evaporative fluid cooler of mineral scale build-up and other contaminants. This schedule is only used if the Blowdown Calculation Mode is set to ScheduledRate. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Default value is under investigation for now cooling tower’s evaporation loss factor is taken as default value.This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the evaporative fluid cooler is active and water is flowing through the evaporative fluid cooler (regardless of the water usage defined by this schedule).
-
-#### Field: Supply Water Storage Tank Name
-
-This field is optional. It is used to describe where the evaporative fluid cooler obtains water used for evaporative cooling. If blank or omitted, then the evaporative fluid cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the evaporative fluid cooler will obtain its water from that tank. If a tank is specified, the evaporative fluid cooler will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the evaporative fluid cooler needs, then the evaporative fluid cooler will still operate and obtain the rest of the water it needs from the mains (referred to as ‘Starved’ water).
-
-An IDF specification for this object is shown below:
-```idf
-EvaporativeFluidCooler:SingleSpeed,
-    Big EvaporativeFluidCooler,         !- Name
-    Condenser EvaporativeFluidcooler Inlet Node,  !- Water Inlet Node Name
-    Condenser EvaporativeFluidcooler Outlet Node,  !- Water Outlet Node Name
-    3.02,                    !- Design Air Flow Rate {m3/s}
-    2250,                    !- Design Air Flow Rate Fan Power {W}
-    0.002208,                !- Design Spray Water Flow Rate {m3/s}
-    UserSpecifiedDesignCapacity,                        !- Performance Input Method
-    ,                        !- Outdoor Air Inlet Node Name
-    1.25,                    !- Heat Rejection Capacity and Nominal Capacity Sizing Ratio
-    ,                        !- Standard Design Capacity {W}
-    ,                        !- Design Air Flow Rate U-factor Times Area Value {W/K}
-    0.001703,                !- Design Water Flow Rate {m3/s}
-    87921,                   !- User Specified Design Capacity {W}
-    46.11,                   !- Design Entering Water Temperature {C}
-    35,                      !- Design Entering Air Temperature {C}
-    25.6;                    !- Design Entering Air Wet-bulb Temperature {C}
-```
-
-### Single Speed Evaporative Fluid Cooler Outputs
-
-* HVAC,Average,Cooling Tower Fan Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Fan Electric Energy [J]
-
-* HVAC,Average,Cooling Tower Heat Transfer Rate [W]
-
-* HVAC,Average,Cooling Tower Inlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Outlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Mass Flow Rate [kg/s]
-
-* HVAC,Average,Cooling Tower Bypass Fraction []
-
-* HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Make Up Water Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Evaporation Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Evaporative Fluid Cooler Water Drift [m3]
-
-* HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Blowdown Volume [m3]
-
-* HVAC,Sum,Cooling Tower Make Up Mains Water Volume [m3]
-
-
-If Supply Water Storage Tank Name is specified:
-
-* HVAC,Average,Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Storage Tank Water Volume [m3]
-
-* HVAC,Average,Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume [m3]
-
-
-
-#### Cooling Tower Fan Electric Power [W]
-
-The average electric power consumption of the fluid cooler fan in Watts for the timestep being reported.
-
-#### Cooling Tower Fan Electric Energy [J]
-
-Fan energy use in Joules.  Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Cooling Tower Heat Transfer Rate [W]
-
-This is the average rate, in Watts, at which heat is removed from the condenser water loop by the fluid cooler for the time step being reported.
-
-#### Cooling Tower Inlet Temperature [C]
-
-The fluid temperature at the fluid cooler inlet in degrees Celsius.
-
-#### Cooling Tower Outlet Temperature [C]
-
-The fluid temperature at the fluid cooler outlet in degrees Celsius.
-
-#### Cooling Tower Mass Flow Rate [kg/s]
-
-The average fluid mass flow rate through the fluid cooler in kg/s for the time step being reported.
-
-#### Cooling Tower Bypass Fraction []
-
-This output is the average fluid bypass fraction for the time step being reported. See Capacity Control input field.
-
-#### Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Make Up Water Volume [m3]
-
-These outputs are the external spray water consumed by the evaporative fluid cooler. This is the total of evaporation, drift, and blowdown.
-
-#### Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Evaporation Volume [m3]
-
-#### Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Drift Volume  [m3]
-
-#### Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Blowdown Volume [m3]
-
-These outputs provide the breakdown of the different components of water use during fluid cooler operation.
-
-#### Cooling Tower Make Up Mains Water Volume [m3]
-
-The volume of make up water provided by the mains in cubic meters. If no Supply Water Storage Tank is specified, then all fluid cooler make up water is provided by the mains (same as Cooling Tower Make Up Water Volume). If a Supply Water Storage Tank is specified, then the make up from the mains only occurs when sufficient water supply is not available from the tank (same as Evaporative Fluid Cooler Water Starved by Storage Tank). This output variable is metered on HeatRejection:MainsWater, MainsWater:Plant and MainsWater:Facility.
-
-#### Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Storage Tank Water Volume [m3]
-
-These are the rate and volume of water provided by the Supply Water Storage Tank.
-
-#### Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Starved Storage Tank Water Volume [m3]
-
-These are the rate and volume of water the Supply Water Storage Tank was not able to provide. The starved water is assumed to come from the mains. The fluid cooler’s operation is not affected by a lack of storage tank water.
-
-### EvaporativeFluidCooler:TwoSpeed
-
-The two-speed evaporative fluid cooler is modeled in a similar fashion to the single-speed evaporative fluid cooler. The evaporative fluid cooler is modeled as a counter flow heat exchanger with two-speed fan (induced draft configuration. See schematic diagram in EvaporativeFluidCooler:SingleSpeed section). The user must define fluid cooler performance via one of the three methods: design heat transfer coefficient-area product (UA) and design water flow rate, or standard fluid cooler design capacity at a specific rating point or design capacity at non standard conditions. Regardless of which method is chosen, the design airflow rate and corresponding fan power must be specified.
-
-The evaporative fluid cooler seeks to maintain the temperature of the water exiting the evaporative fluid cooler at (or below) a set point. The set point schedule value is defined by the field “Condenser Loop Temperature Setpoint Node Name or Reference� for the CondenserLoop object. The model first checks to see whether inlet water temperature is at or below the set point. If so, then the fluid cooler fan is not turned on and all the flow goes through bypass. If the inlet water temperature is above the set point then the fluid cooler fan is turned on at low speed to reduce the exiting water temperature to the set point. If operating the fluid cooler fan at low speed does not reduce the exiting water temperature to the set point, then the fluid cooler fan is increased to its high speed.
-
-The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., fluid cooler fan at high speed for the entire simulation timestep and fluid cooler fan at low speed for the entire simulation timestep, or fluid cooler fan at low speed for the entire simulation timestep and fluid cooler fan off for the entire simulation timestep). Cyclic losses are not taken into account.
-
-Evaporative fluid coolers consume water through evaporation, drift, and blowdown. The model can be used to predict water consumed by the evaporative fluid coolers. For this purpose, the last seven input fields can either be provided in the input or if nothing is specified then the default values for these fields will be used. These fields provide methods of controlling details of the water consumption calculations. The user can specify connections to the rest of the buildings water system by providing the name of a water storage tanks (i.e. WaterUse:Storage objects).
-
-#### Field: Name
-
-This alpha field contains the identifying name for the fluid cooler.
-
-#### Field: WaterInlet Node Name
-
-This alpha field contains the identifying name for the fluid cooler’s water inlet node.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the identifying name for the fluid cooler’s water outlet node.
-
-#### Field: High Fan Speed Air Flow Rate
-
-This numeric field contains the fluid cooler air flow rate at high fan speed in m<sup>3</sup>/s. A value greater than zero must be defined regardless of fluid cooler performance input method. Alternately, this field can be autosized. See Engineering Reference document for fluid cooler autosizing.
-
-#### Field: High Fan Speed Fan Power
-
-This numeric field contains the fan power (in Watts) at the high-speed air flow rate specified in the previous field. A value greater than zero must be specified regardless of fluid cooler performance input method, or this field can be autosized. See Engineering Reference document for fluid cooler autosizing.
-
-#### Field: Low Fan Speed Air Flow Rate
-
-This numeric field contains the fluid cooler air flow rate at low fan speed in m<sup>3</sup>/s. This value must be greater than zero, less than the value specified for the field “Air Flow Rate at High Fan Speed�. This field may be autocalculated, in which case it is set to a fraction of the “Air Flow Rate at High Fan Speed� determined in the following field.
-
-#### Field: Low Fan Speed Air Flow Rate Sizing Factor
-
-This numeric field contains the sizing factor for calculating the low fan speed air flow rate as a fraction of the high fan speed air flow rate.  The default is 0.5.
-
-#### Field: Low Fan Speed Fan Power
-
-This numeric field contains the fan power (in Watts) at the low-speed air flow rate specified in the previous field. This value must be specified greater than zero or the field may be autocalculated, in which case it is set to a fraction of the “Fan Power at High Fan Speed� determined in the following field.
-
-#### Field: Low Fan Speed Fan Power Sizing Factor
-
-This numeric field contains the sizing factor for calculating the low fan speed fan power as a fraction of the high fan speed fan power.  The default is 0.16.
-
-#### Field: Design Spray Water Flow Rate
-
-This numeric field contains the design spray water flow rate through the fluid cooler in m<sup>3</sup>/s. This input field must be specified for all the performance input methods.
-
-#### Field: Performance Input Method
-
-This alpha field contains the method by which the user will specify fluid cooler performance: “UFactorTimesAreaAndDesignWaterFlowRate� or “StandardDesignCapacity� or “UserSpecifiedDesignCapacity�.
-
-#### Field: Outdoor Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the fluid cooler. If this field is left blank, the outdoor air conditions entering the fluid cooler are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-#### Field: Heat Rejection Capacity and Nominal Capacity Sizing Ratio
-
-This numeric field contains the value for the ratio of actual tower heat rejection to nominal capacity.  This ratio is defined at entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. Historically this ratio has been set at 1.25 based on the assumption that the tower must dissipate 0.25 W of compressor power for every what of heat removed at the chiller evaporator.  The default is 1.25.
-
-#### Field: High Speed Standard Design Capacity
-
-This numeric input field contains the heat rejection capacity of the fluid cooler in watts, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of nominal capacity (3 gpm/ton). The Heat Rejection Capacity and Nominal Capacity Sizing Ratio set in the previous field is applied to this capacity to give the actual fluid cooler heat rejection at these operating conditions. This field is only used for performance input method =�StandardDesignCapacity�. For other input methods this field is ignored. The standard conditions mentioned above for “standard design capacity� are already specified in the EnergyPlus. So the input fields such as design entering water temp., design entering air wet-bulb and dry-bulb temp. and design water flow rate, if provided in the input, will be ignored for the StandardDesignCapacity performance input method. Also, the standard conditions are for water as a fluid type so this performance input method can only be used with water as a fluid type (ref. CondenserLoop object).
-
-#### Field: Low Speed Standard Design Capacity
-
-This numeric input field contains the heat rejection capacity of the fluid cooler in watts, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of nominal capacity (3 gpm/ton). The Heat Rejection Capacity and Nominal Capacity Sizing Ratio is applied to this capacity to give the actual fluid cooler heat rejection at these operating conditions. This field is only used for performance input method =�StandardDesignCapacity�. For other input methods this field is ignored. The standard conditions mentioned above for “standard design capacity� are already specified in the EnergyPlus. So the input fields such as design entering water temp., design entering air wet-bulb and dry-bulb temp. and design water flow rate, if provided in the input, will be ignored for the StandardDesignCapacity performance input method. Also, the standard conditions are for water as a fluid type so this performance input method can only be used with water as a fluid type (ref. CondenserLoop object). The value specified for this field must be greater than zero but less than the value specified for the field “High-Speed Standard Design Capacity�. This field may be autocalculated, in which case it is set to a fraction of the High-Speed Standard Design Capacity determined in the following field.
-
-#### Field: Low Speed Standard Capacity Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the Low Speed Standard Design Capacity.  The default is 0.5.
-
-#### Field: High Fan Speed U-factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the high speed design air and water flow rates specified above. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a UA value greater than zero but less than or equal to 2,100,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design fluid cooler UA value is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), the fluid cooler inlet air dry-bulb and wetbulb temperature are taken from the input. This field is only used for performance input method =� UFactorTimesAreaAndDesignWaterFlowRate�. For other input methods this field is ignored.
-
-#### Field: Low Fan Speed U-factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (UA) in watts per degree Kelvin corresponding to the low speed design air and water flow rates specified above. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a UA value greater than zero but less than or equal to 300,000 and less than the value specified for the field “U-Factor Times Area Value at High Fan Speed� must be defined. This field may be autocalculated, in which case it is set to a factor of the “U-Factor Times Area Value at High Fan Speed� determined in the following field. This field is only used for performance input method =� UFactorTimesAreaAndDesignWaterFlowRate�. For other input methods this field is ignored.
-
-#### Field: Low Fan Speed U-Factor Times Area Sizing Factor
-
-This field contains the sizing factor to use when calculating the Low Fan Speed U-Factor Times Area Value.  The default is 0.6.
-
-#### Field: Design Water Flow Rate
-
-This numeric field contains the design water flow rate through the fluid cooler in m<sup>3</sup>/s. This value is the flow rate of the condenser loop water being cooled by the fluid cooler. This field is ignored for the “StandardDesignCapacity� performance input method. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections).
-
-#### Field: High Speed User Specified Design Capacity
-
-This numeric input field contains the heat rejection capacity of the fluid cooler in watts. Design conditions for this capacity i.e. entering air dry-bulb temperature, entering air wet-bulb temperature and entering water temperature must be provided in the input. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
-
-#### Field: Low Speed User Specified Design Capacity
-
-This numeric input field contains the heat rejection capacity of the fluid cooler in watts. Design conditions for this capacity i.e. entering air dry-bulb temperature, entering air wet-bulb temperature and entering water temperature must be provided in the input. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored. This field may be autocalculated, in which case it is set to a fraction of the “High Speed User Specified Design Capacity� determined in the following field.
-
-#### Field: Low Speed User Specified Design Capacity Sizing Factor
-
-This field contains the sizing factor to use when calculating the Low-Speed User Specified Design Capacity.  The default is 0.5.
-
-#### Field:Design Entering Water Temperature
-
-This numeric field contains entering water temperature at nominal conditions in degrees Celsius. The design entering water temperature must be greater than the design entering air temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
-
-#### Field:Design Entering Air Temperature
-
-This numeric field contains entering air dry-bulb temperature at nominal conditions in degrees Celsius. The design entering air temperature must be greater than the design entering air wet-bulb temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
-
-#### Field:Design Entering Air Wet-bulb Temperature
-
-This numeric field contains entering air wetbulb temperature at nominal conditions in degrees Celsius. The design entering air wet-bulb temperature must be less than the design entering air (dry-bulb) temperature. Only used for Performance Input Method = UserSpecifiedDesignCapacity; for other performance input methods this field is ignored.
-
-#### Field: High Speed Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature. For this component the inputs that would be altered by the sizing factor are:
-
-1.    Design Water Flow Rate;
-
-2.    Air Flow Rate at High Fan Speed;
-
-3.    Fan Power at High Fan Speed;
-
-4.    U-Factor Times Area Value at High Fan Speed;
-
-5.    Air Flow Rate at Low Fan Speed;
-
-6.    Fan Power at Low Fan Speed;
-
-7.    U-Factor Times Area Value at Low Fan Speed;
-
-Note that the U-Factor Times Area Value at High Fan Speed is not multiplied by the Sizing Factor. Instead the design evaporative fluid cooler load is multiplied by the sizing factor and the design UA then calculated as usual. The U-Factor Times Area Value at Low Fan Speed is set to Low Fan Speed U-Factor Times Area Sizing Factor times the full load design UA.
-
-#### Field: Evaporation Loss Mode
-
-This field is used to choose which method is used to model the amount of water evaporated by the evaporative fluid cooler. There are two options: LossFactor or SaturatedExit. The default is SaturatedExit. The user-defined loss factor is entered in the following field. By assuming that the air leaving the evaporative fluid cooler is saturated, the evaporation can be directly calculated using moist air engineering calculations with data available within the evaporative fluid cooler model (and does not require additional user input).
-
-#### Field: Evaporation Loss Factor
-
-This field is used to specify the rate of water evaporated from the evaporative fluid cooler and lost to the outside air [percent/K]. This field is only used if the Evaporation Calculation Mode is set to LossFactor. The evaporation loss is then calculated as a fraction of the circulating condenser water flow and varies with the temperature change in the condenser water. The value entered here is in units of percent-per-kelvin. The evaporation rate will equal this value times each degree Kelvin of temperature drop in the condenser water. Empirical correlation is used to calculate default loss factor if it not explicitly specified in the input file.
-
-#### Field: Drift Loss Percent
-
-This field is used to specify the rate of water lost to the exiting air as entrained droplets [%]. The drift loss is a percent of the condenser water flow. Default value is under investigation for now cooling tower’s evaporation loss factor is taken as default value.
-
-#### Field: Blowdown Calculation Mode
-
-This field specifies which method is used to determine blowdown rates. There two options ConcentrationRatio or ScheduledRate. The choice will determine which of the two models below is used. The default is ConcentrationRatio.
-
-#### Field: Blowdown Concentration Ratio
-
-This field is used to dynamically adjust the rate of blowdown in the evaporative fluid cooler as a function of the rate of evaporation. Blowdown is water intentionally drained from the evaporative fluid cooler in order to offset the build up of solids in the water that would otherwise occur because of evaporation. The value entered here is dimensionless. It can be characterized as the ratio of solids in the blowdown water to solids in the make up water. Default value is under investigation for now cooling tower’s evaporation loss factor is taken as default value.
-
-#### Field: Blowdown Makeup Water Usage Schedule Name
-
-This alpha field contains the name of the schedule used to define the amount of water (m3/s) flushed from the basin on a periodic basis to purge the evaporative fluid cooler of mineral scale build-up and other contaminants. This schedule is only used if the Blowdown Calculation Mode is set to ScheduledRate. The amount of water use due to blowdown depends on the makeup water quality and is specific to each geographical location. Default value is under investigation for now cooling tower’s evaporation loss factor is taken as default value.This water usage is in addition to the amount of water lost to the atmosphere due to evaporation and/or drift. Since blowdown occurs when the basin water contaminant concentration is high, blowdown only occurs when the evaporative fluid cooler is active and water is flowing through the evaporative fluid cooler (regardless of the water usage defined by this schedule).
-
-#### Field: Supply Water Storage Tank Name
-
-This field is optional. It is used to describe where the evaporative fluid cooler obtains water used for evaporative cooling. If blank or omitted, then the evaporative fluid cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the evaporative fluid cooler will obtain its water from that tank. If a tank is specified, the evaporative fluid cooler will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the evaporative fluid cooler needs, then the evaporative fluid cooler will still operate and obtain the rest of the water it needs from the mains (referred to as ‘Starved’ water).
-
-Examples of an IDF specification for this object are shown below:
-
-```idf
-EvaporativeFluidCooler:TwoSpeed,
-    Big EvaporativeFluidCooler,         !- Name
-    Condenser EvaporativeFluidcooler Inlet Node,  !- Water Inlet Node Name
-    Condenser EvaporativeFluidcooler Outlet Node,  !- Water Outlet Node Name
-    9.911,                   !- High Fan Speed Air Flow Rate {m3/s}
-    autosize,                !- High Fan Speed Fan Power {W}
-    4.911,                   !- Low Fan Speed Air Flow Rate {m3/s}
-    0.5,                     !- Low Fan Speed Air Flow Rate Sizing Factor
-    autosize,                !- Low Fan Speed Fan Power {W}
-    0.16,                    !- Low Fan Speed Fan Power Sizing Factor
-    0.002208,                !- Design Spray Water Flow Rate {m3/s}
-    UserSpecifiedDesignCapacity,    !- Performance Input Method
-    ,                        !- Outdoor Air Inlet Node Name
-    1.25,                    !- Heat Rejection Capacity and Nominal Capacity Sizing Ratio
-    ,                        !- High Speed Standard Design Capacity {W}
-    ,                        !- Low Speed Standard Design Capacity {W}
-    0.5,                     !- Low Speed Standard Capacity Sizing Factor
-    ,                        !- High Fan Speed U-factor Times Area Value  {W/K}
-    ,                        !- Low Fan Speed U-factor Times Area Value  {W/K}
-    0.6,                     !- Low Fan Speed U-Factor Times Area Sizing Factor
-    0.001703,                !- Design Water Flow Rate {m3/s}
-    87921,                   !- High Speed User Specified Design Capacity {W}
-    47921,                   !- Low Speed User Specified Design Capacity {W}
-    0.5,                     !- Low Speed User Specified Design Capacity Sizing Factor
-    46.11,                   !- Design Entering Water Temperature {C}
-    35,                      !- Design Entering Air Temperature {C}
-    25.6;                    !- Design Entering Air Wet-bulb Temperature {C}
-```
-
-### Two Speed Evaporative Fluid Cooler Outputs
-
-* HVAC,Average,Cooling Tower Fan Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Fan Electric Energy [J]
-
-* HVAC,Average,Cooling Tower Heat Transfer Rate [W]
-
-* HVAC,Average,Cooling Tower Inlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Outlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Mass Flow Rate [kg/s]
-
-* HVAC,Average,Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Make Up Water Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Evaporation Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Drift Volume [m3]
-
-* HVAC,Average,Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Water Blowdown Volume [m3]
-
-* HVAC,Sum,Cooling Tower Make Up Mains Water Volume [m3]
-
-If Supply Water Storage Tank Name is specified:
-
-* HVAC,Average,Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Storage Tank Water Volume [m3]
-
-* HVAC,Average,Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Tower Starved Storage Tank Water Volume [m3]
-
-
-
-#### Cooling Tower Fan Electric Power [W]
-
-The average electric power consumption of the fluid cooler fan in Watts for the timestep being reported.
-
-#### Cooling Tower Fan Electric Energy [J]
-
-Fan energy use in Joules.  Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Cooling Tower Heat Transfer Rate [W]
-
-This is the average rate, in Watts, at which heat is removed from the condenser water loop by the fluid cooler for the time step being reported.
-
-#### Cooling Tower Inlet Temperature [C]
-
-The fluid temperature at the fluid cooler inlet in degrees Celsius.
-
-#### Cooling Tower Outlet Temperature [C]
-
-The fluid temperature at the fluid cooler outlet in degrees Celsius.
-
-#### Cooling Tower Mass Flow Rate [kg/s]
-
-The average fluid mass flow rate through the fluid cooler in kg/s for the time step being reported.
-
-#### Cooling Tower Make Up Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Make Up Water Volume [m3]
-
-These outputs are the external spray water consumed by the evaporative fluid cooler. This is the total of evaporation, drift, and blowdown.
-
-#### Cooling Tower Water Evaporation Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Evaporation Volume [m3]
-
-#### Cooling Tower Water Drift Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Drift Volume [m3]
-
-#### Cooling Tower Water Blowdown Volume Flow Rate [m3/s]
-
-#### Cooling Tower Water Blowdown Volume [m3]
-
-These outputs provide the breakdown of the different components of water use during fluid cooler operation.
-
-#### Cooling Tower Make Up Mains Water Volume [m3]
-
-The volume of make up water provided by the mains in cubic meters. If no Supply Water Storage Tank is specified, then all fluid cooler make up water is provided by the mains (same as Cooling Tower Make Up Water Volume). If a Supply Water Storage Tank is specified, then the make up from the mains only occurs when sufficient water supply is not available from the tank (same as Cooling Tower Starved Storage Tank Water Volume). This output variable is metered on HeatRejection:MainsWater, MainsWater:Plant and MainsWater:Facility.
-
-#### Cooling Tower Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Storage Tank Water Volume [m3]
-
-These are the rate and volume of water provided by the Supply Water Storage Tank.
-
-#### Cooling Tower Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Cooling Tower Starved Storage Tank Water Volume [m3]
-
-These are the rate and volume of water the Supply Water Storage Tank was not able to provide. The starved water is assumed to come from the mains. The fluid cooler’s operation is not affected by a lack of storage tank water.
-
-### FluidCooler:SingleSpeed
-
-Fluid coolers are components that may be assigned to condenser loops. The Fluid cooler is modeled as a cross flow heat exchanger (both streams unmixed) with single-speed fans (induced draft configuration). The user must define fluid cooler performance via one of the two methods: design heat transfer coefficient-area product (UA) and design water flow rate, or nominal fluid cooler capacity at a specific rating point. Regardless of which method is chosen, the design airflow rate and corresponding fan power must be specified.
-
-The fluid cooler seeks to maintain the temperature of the water exiting the fluid cooler at (or below) a set point. The set point schedule value is defined by the field “Condenser Loop Temperature Setpoint Node Name or Reference� for the CondenserLoop object. The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., fluid cooler fan on for the entire simulation timestep and fluid cooler fan off for the entire simulation timestep). Cyclic losses are not taken into account.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the Fluid Cooler.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the identifying name for the Fluid Cooler’s water inlet node.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the identifying name for the Fluid Cooler’s water outlet node.
-
-#### Field: Performance Input Method
-
-This alpha field contains the method by which the user will specify fluid cooler performance: “UFactorTimesAreaAndDesignWaterFlowRate� or “NominalCapacity�.
-
-#### Field: Design Air Flow Rate U-factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the design air and water flow rates specified above. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design fluid cooler UA value is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), the fluid cooler inlet air dry-bulb and wetbulb temperature are taken from the input. If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically calculates the fluid cooler UA based on the fluid cooler capacity and nominal conditions specified in input file.
-
-#### Field: Nominal Capacity
-
-This numeric input field contains the “nominal� heat rejection capacity of the fluid cooler in watts, Nominal conditions i.e. entering air dry-bulb temperature, entering air wet-bulb temperature and Entering water temperature should be provided in the input.
-
-#### Field:Design Entering Water Temperature
-
-This numeric field contains entering water temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering water temperature must be greater than the design entering air temperature.
-
-#### Field:Design Entering Air Temperature
-
-This numeric field contains entering air dry-bulb temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering air temperature must be greater than the design entering air wet-bulb temperature.
-
-#### Field:Design Entering Air Wet-bulb Temperature
-
-This numeric field contains entering air wetbulb temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering air wet-bulb temperature must be less than the design entering air (dry-bulb) temperature.
-
-#### Field: Design Water Flow Rate
-
-This numeric field contains the design water flow rate through the fluid cooler in m<sup>3</sup>/s. This value is the flow rate of the condenser loop water being cooled by the fluid cooler. A water flow rate greater than zero must be defined or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections).
-
-#### Field: Design Air Flow Rate
-
-This numeric field contains the design air flow rate induced by the fluid cooler fan in m<sup>3</sup>/s. A value greater than zero must be defined regardless of the fluid cooler performance input method. Alternately, this field can be autosized. See Engineering Reference document for fluid cooler autosizing.
-
-#### Field: Design Air Flow Rate Fan Power
-
-This numeric field contains the fan power (in watts) at the design air flow rate specified in the previous field. A value greater than zero must be specified regardless of the performance input method, or this field can be autosized. See Engineering ref. for fluid cooler autosizing.
-
-#### Field: Outdoor Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the fluid cooler. If this field is left blank, the outdoor air conditions entering the fluid cooler are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-An IDF specification for this object is shown below:
-
-```idf
-FluidCooler:SingleSpeed,
-    Big FLUIDCOOLER1,              !- Name
-    Condenser FLUIDCOOLER 1 Inlet Node,  !- Water Inlet Node Name
-    Condenser FLUIDCOOLER 1 Outlet Node, !- Water Outlet Node Name
-    NominalCapacity,        !- Performance Input Method
-    ,                       !- Design Air Flow Rate U-factor Times Area Value {W/K}
-    58601.,                 !- Nominal Capacity {W}
-    51.67,                  !- Design Entering Water Temperature {C}
-    35,                     !- Design Entering Air Temperature {C}
-    25.6,                   !- Design Entering Air Wetbulb Temperature {C}
-    0.001388,               !- Design Water Flow Rate{m3/s}
-    9.911,                  !- Design Air Flow Rate {m3/s}
-    Autosize;               !- Design Air Flow Rate Fan Power {W}
-```
-
-### Single Speed Fluid Cooler Outputs
-
-* HVAC,Average,Cooling Tower Fan Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Fan Electric Energy [J]
-
-* Zone,Meter,HeatRejection:Electricity [J]
-
-* HVAC,Average,Cooling Tower Heat Transfer Rate [W]
-
-* HVAC,Average, Cooling Tower Inlet Temperature [C]
-
-* HVAC,Average, Cooling Tower Outlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Mass Flow Rate [kg/s]
-
-#### Cooling Tower Fan Electric Power [W]
-
-The electric power consumption of the fluid cooler fans.
-
-#### Cooling Tower Fan Electric Energy [J]
-
-Fan energy use.  Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Cooling Tower Heat Transfer Rate [W]
-
-This is the rate at which heat is removed from the condenser water loop by the fluid cooler.
-
-#### Cooling Tower Inlet Temperature [C]
-
-The loop temperature at the fluid cooler inlet.
-
-#### Cooling Tower Outlet Temperature [C]
-
-The loop temperature at the fluid cooler outlet.
-
-#### Cooling Tower Mass Flow Rate [kg/s]
-
-The loop mass flow rate of the circulating condenser water loop.
-
-### FluidCooler:TwoSpeed
-
-The two-speed fluid cooler is modeled in a similar fashion to the single-speed fluid cooler. The fluid cooler is modeled as a cross flow heat exchanger (both stream unmixed) with  two-speed fans (induced draft configuration). The user must define fluid cooler performance via one of two methods: heat transfer coefficient-area product (UA) and design water flow rate, or nominal fluid cooler capacity at a specific rating point. Regardless of which method is chosen, the airflow rate and corresponding fan power at both high and low fan speed must be specified. The Fluid Cooler seeks to maintain the temperature of the water exiting the Fluid Cooler at (or below) a set point. The set point schedule is defined by the field “Condenser Loop Temperature Setpoint Node Name or Reference� for the CondenserLoop object. The model first runs at low speed and calculates the fluid cooler exiting water temperature. If the exiting water temperature based on “low speed� is at or below the set point, then the fluid cooler fan runs at this speed or below this speed. If the exiting water temperature remains above the set point after “low speed� is modeled, then the fluid cooler fan runs at high speed to reduce the exiting water temperature.
-
-The model assumes that part-load operation is represented by a simple linear interpolation between two steady-state regimes (i.e., fluid cooler fan at high speed for the entire simulation timestep and fluid cooler fan at low speed for the entire simulation timestep,). Cyclic losses are not taken into account.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the fluid cooler.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the identifying name for the fluid cooler’s water inlet node.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the identifying name for the fluid cooler’s water outlet node.
-
-#### Field: Performance Input Method
-
-This alpha field contains the method by which the user will specify fluid cooler performance: “UFactorTimesAreaAndDesignWaterFlowRate� or “NominalCapacity�.
-
-#### Field: High Fan Speed U-factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (UA) in watts per degree Celsius corresponding to the high-speed air flow rate and design water flow rate specified above. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, then a UA value greater than zero but less than or equal to 300,000 must be defined, or the field can be autosized. If autosized, a Plant Sizing object must be defined and the fluid cooler UA value at high fan speed is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections), fluid cooler water inlet temperature, fluid cooler inlet air drybulb and wetbulb are provided in the input. If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically calculates the fluid cooler UA based on the capacity specified in the field “High Speed Nominal Capacity� and nominal conditions.
-
-#### Field: Low Fan Speed U-factor Times Area Value
-
-This numeric field contains the heat transfer coefficient-area product (UA) in watts per Kelvin corresponding to the design water flow rate and low-speed air flow rate specified above. If the input field “Performance Input Method� is specified as “UFactorTimesAreaAndDesignWaterFlowRate�, this value must be greater than zero but less than or equal to 300,000, less than the value specified for the field “U-factor Times Area Value at High Fan Speed�. This field may be autocalculated, in which case it is set to a factor of the “U-factor Times Area Value at High Fan Speed� determined in the following field. If “Performance Input Method� is specified as “NominalCapacity�, then this field must be left blank since the model automatically calculates the fluid cooler UA based on the fluid cooler capacity specified in the field “Low Speed Nominal Capacity�.
-
-#### Field: Low Fan Speed U-Factor Times Area Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the Low Fan Speed U-factor Times Area Value.  The default is 0.6.
-
-#### Field: High Speed Nominal Capacity
-
-This numeric input field contains the “nominal� heat rejection capacity of the fluid cooler in watts under high-speed fan operation, with nominal (design) inputs entering water temperature, entering air temperature and entering air wet-bulb temperature. The design water flow rate is also provided in the input.
-
-#### Field: Low Speed Nominal Capacity
-
-This numeric input field contains the “nominal� heat rejection capacity of the Fluid Cooler in watts under low-speed fan operation, with nominal (design) inputs entering water temperature, entering air temperature and entering air wet-bulb temperature. The design water flow rate is also provided in the input. The value specified for this field must be greater than zero but less than the value specified for the field “High Speed Nominal Capacity�. This field may be autocalculated, in which case it is set to a fraction of the “High Speed Nominal Capacity� determined in the following field.
-
-#### Field: Low Speed Nominal Capacity Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the Low Speed Nominal Capacity.  The default is 0.5.
-
-#### Field:Design Entering Water Temperature
-
-This numeric field contains entering water temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering water temperature must be greater than the design entering air temperature.
-
-#### Field:Design Entering Air Temperature
-
-This numeric field contains entering air dry-bulb temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering air temperature must be greater than the design entering air wet-bulb temperature.
-
-#### Field:Design Entering Air Wet-bulb Temperature
-
-This numeric field contains entering air wet-bulb temperature at nominal conditions in degrees Celsius. This field must be specified for both the performance input methods. The design entering air wet-bulb temperature must be less than the design entering air (dry-bulb) temperature.
-
-#### Field: Design Water Flow Rate
-
-This numeric field contains the design water flow rate through the fluid cooler in m<sup>3</sup>/s. This value is the flow rate of the condenser loop water being cooled by the fluid cooler. A water flow rate greater than zero must be defined or the field can be autosized. If autosized, a Plant Sizing object must be defined and the design water flow rate is derived from the design load to be rejected by the condenser loop and the design loop delta T (Ref. Sizing and Input for Design Calculations and Component Autosizing sections).
-
-#### Field: High Fan Speed Air Flow Rate
-
-This numeric field contains the fluid cooler air flow rate at high fan speed in m<sup>3</sup>/s. A value greater than zero must be defined regardless of the fluid cooler performance input method. Alternately, this field can be autosized. See Engineering ref. for fluid cooler autosizing.
-
-#### Field: High Fan Speed Fan Power
-
-This numeric field contains the fan power (in Watts) at the high-speed air flow rate specified in the previous field. A value greater than zero must be specified regardless of the fluid cooler performance input method, or this field can be autosized. See Engineering ref. for fluid cooler autosizing.
-
-#### Field: Low Fan Speed Air Flow Rate
-
-This numeric field contains the fluid cooler air flow rate at low fan speed in m<sup>3</sup>/s. This value must be greater than zero, less than the value specified for the field “Air Flow Rate at High Fan Speed�. This field may be autocalculated, in which case it is set to a fraction of the “Air Flow Rate at High Fan Speed� determined in the following field.
-
-#### Field: Low Fan Speed Air Flow Rate Sizing Factor
-
-This numeric field contains the sizing factor to use when calculating the Low Fan Speed Air Flow Rate. The default is 0.5.
-
-#### Field: Low Fan Speed Fan Power
-
-This numeric field contains the fan power (in Watts) at the low-speed air flow rate specified in the previous field. This value must be specified greater than zero or the field may be autocalculated, in which case it is set to set to a fraction of the “Fan Power at High Fan Speed� determined in the following field.
-
-#### Field: Low Fan Speed Fan Power Sizing Factor
-
-This numeric field contains the sizing factor to use whe calculating the Low Fan Speed Fan Power.  The default is 0.16.
-
-#### Field: Outdoor Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the Fluid Cooler. If this field is left blank, the outdoor air conditions entering the Fluid Cooler are taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air conditions from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air conditions are taken directly from the weather data.
-
-Examples of an IDF specification for this object are shown below:
-
-```idf
-FluidCooler:TwoSpeed,
-    Big FLUIDCOOLER1,              !- Name
-    Condenser FLUIDCOOLER 1 inlet Node,  !- Water Inlet Node Name
-    Condenser FLUIDCOOLER 1 Outlet Node,  !- Water Outlet Node Name
-    NominalCapacity,         !- Performance Input Method
-    ,                        !- High Fan Speed U-factor Times Area Value {W/K}
-    ,                        !- Low Fan Speed U-factor Times Area Value {W/K}
-    ,                        !- Low Fan Speed U-Factor Times Area Sizing Factor
-    58601.,                  !- High Speed Nominal Capacity {W}
-    28601.,                  !- Low Speed Nominal Capacity {W}
-.   0.6,                     !- Low Speed Nominal Capacity Sizing Factor
-    51.67,                   !- Design Entering Water tempereture {C}
-    35,                      !- Design Entering Air tempereture {C}
-    25.6,                    !- Design Entering Air Wet-bulb tempereture {C}
-    0.001388,                !- Design Water Flow Rate {m3/s}
-    9.911,                   !- High Fan Speed Air Flow Rate {m3/s}
-    autosize,                !- High Fan Speed Fan Power {W}
-    autosize,                !- Low Fan Speed Air Flow Rate {m3/s}
-    0.5,                     !- Low Fan Speed Air Flow Rate Sizing Factor
-    autosize,                !- Low Fan Speed Fan Power {W}
-    0.16;                    !- Low Fan Speed Fan Power Sizing Factor
-```
-
-### Two Speed Fluid Cooler Outputs
-
-* HVAC,Average,Cooling Tower Fan Electric Power [W]
-
-* HVAC,Sum,Cooling Tower Fan Electric Energy [J]
-
-* HVAC,Average,Cooling Tower Heat Transfer Rate [W]
-
-* HVAC,Average, Cooling Tower Inlet Temperature [C]
-
-* HVAC,Average, Cooling Tower Outlet Temperature [C]
-
-* HVAC,Average,Cooling Tower Mass Flow Rate [kg/s]
-
-#### Cooling Tower Fan Electric Power [W]
-
-Average fan electric power consumed.
-
-#### Cooling Tower Fan Electric Energy [J]
-
-Total energy used by the fan. Consumption is metered on HeatRejection:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Cooling Tower Heat Transfer Rate [W]
-
-This is the rate at which heat is removed from the condenser water loop by the fluid cooler.
-
-#### Cooling Tower Inlet Temperature [C]
-
-Loop temperature at the fluid cooler inlet.
-
-#### Cooling Tower Outlet Temperature [C]
-
-Loop temperature at the fluid cooler outlet.
-
-#### Cooling Tower Mass Flow Rate [kg/s]
-
-Loop mass flow rate through the fluid cooler.
diff --git a/doc/src/docs/InputOutputReference/01c-InputOutputReference.md b/doc/src/docs/InputOutputReference/01c-InputOutputReference.md
deleted file mode 100644
index 2779c3fe531..00000000000
--- a/doc/src/docs/InputOutputReference/01c-InputOutputReference.md
+++ /dev/null
@@ -1,21154 +0,0 @@
-
-### GroundHeatExchanger:Vertical
-
-The EnergyPlus Ground loop heat exchanger is a condenser component. This serves the condenser supply side in addition to the cooling towers and other condensing components. The following figure shows the Ground Heat Exchanger in the simulation environment.
-
-The heat exchanger response is defined by a G-function. This is a non-dimensional function that is used to calculate the response to square heat pulses of different duration. (This function is not the same as ‘G-factors’ referred to in the ASHRAE Applications Handbook). This continuous function is specified by a series of data pairs (LNTTS*i*, GFNC*i*) where,
-
-- LNTTS*i* is the non-dimensional time: *ln(T/T<sub>s</sub>)*
-
-- GFNC*i* is the G-function value
-
-The G-function is different for each borehole field configuration (i.e. a 4x4 field has a different response than a 80x80 field) and the borehole thermal resistance. It is also dependant on the ratio of borehole spacing to depth. G-function values, for accurate simulation, have to be calculated for each specific heat exchanger design. This can be done using some commercial ground loop heat exchanger design tool and the like. A reference data set, containing examples input data for 1x2, 4x4 and 8x8 configurations and for both standard and thermally enhanced grout, have also been provided. These data are provided as examples only. Custom G-function values may be generated using an external program such as GLHEPro. For more information about the datasets and GLHEPro, see the Auxiliary Programs document section “G-Function Spreadsheet.�
-
-Further details of the implementation of this model can be found in:
-
-Murugappan, A. *Implementing Ground Source Heat Pump and Ground Loop Heat Exchanger Models in the EnergyPlus Simulation Environment*. M.S. Thesis, Oklahoma State University, December 2002.
-
-![](media/image202.svg)
-
-Figure 83. Schematic of EnergyPlus Ground Loop Heat Exchanger
-
-The data definition for the ground loop heat exchanger from the Energy+.idd is shown below. The syntax to the specification of Borehole, U-tube and ground are illustrated in the example following.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the ground heat exchanger (GHE).
-
-#### Field: Inlet Node Name
-
-This alpha field contains the ground heat exchanger inlet node name.
-
-#### Field: Outlet Node Name
-
-This alpha field contains the ground heat exchanger outlet node name.
-
-#### Field: Design Flow Rate
-
-This numeric field contains the GHE design flow rate in cubic meters per second {m<sup>3</sup>/s}.
-
-#### Field: Number of Bore Holes
-
-This numeric field contains the number of bore holes in the GHE installation.
-
-#### Field: Bore Hole Length
-
-This numeric field contains the length of the borehole in meters {m}.
-
-#### Field: Bore Hole Radius
-
-This numeric field contains the radius of the borehole in meters.
-
-#### Field: Ground Thermal Conductivity
-
-This numeric field contains the thermal conductivity of the ground in W/m-K.
-
-#### FieldSet: Ground Thermal Heat Capacity
-
-This numeric field contains the thermal heat capacity of the ground in J/m<sup>3</sup>-K.
-
-#### Field: Ground Temperature
-
-This numeric field contains the far field temperature of the ground in °C.
-
-#### Field: Grout Thermal Conductivity
-
-This numeric field contains the thermal conductivity of the filler material in W/m-K.
-
-#### Field: Pipe Thermal Conductivity
-
-This numeric field contains the thermal conductivity of the pipe in W/m-K.
-
-#### Field: Pipe Out Diameter
-
-This numeric field contains the outer diameter of the U-tube (pipe) in meters {m}.
-
-#### Field: U-Tube Distance
-
-This numeric field contains the distance between the two legs of the U-tube in meters {m}.
-
-#### Field: Pipe Thickness
-
-This numeric field contains the outer diameter of the U-tube (pipe) in meters.
-
-#### Field: Maximum Length of Simulation
-
-This numeric field contains the maximum number of years of simulation to be carried out.
-
-#### Field: G-Function Reference Ratio
-
-The G-Functions may be formulated slightly differently based on the program which generated them. The “raw� G-Functions are based on an borehole radius to active length ratio of 0.0005. If the physical ratio is different from this, a correction must be applied. EnergyPlus will apply the correction, based on the reference ratio entered in this field. Therefore, therefore two possible input configurations.
-
-- If the G-Functions have not had a correction applied, then the G-Functions are still based on a reference of 0.0005, so use a value of 0.0005 in this field. EnergyPlus will adjust the G-Functions internally to create the properly referenced G-Function.
-
-- If the correction has already been applied, then the input G-Functions are based on a reference to the actual (physical) radius/length ratio, so enter the physical radius/length in this field. Entering the actual value will nullify any internal corrections, which will avoid re-basing the G-Function set.
-
-The software GLHEPro has been making this “pre-correction� to the data sets since version 3.1 of that software, so this input field should match the actual (physical) radius/length ratio.
-
-#### Field: Number of Data Pairs of the G Function
-
-The borehole response is defined by a non-dimensional ‘G-function’. This is specified as a series of data points giving values of non-dimensional time *vs* G-function value (LNTTS1, GFUNC1), (LNTTS2, GFUNC2), (LNTTS3, GFUNC3) …….. (LNTTS*n*, GFUNC*n*), This numeric field contains the number of data pairs to be read in (*n*).
-
-#### Field: G-Function Ln(T/Ts) Value &lt;x&gt;
-
-This numeric field contains the natural log of time/steady state time: *ln(T/T<sub>s</sub>)*
-
-#### Field: G-Function 'G' Value &lt;x&gt;
-
-This numeric field contains the G-function value of the corresponding LNTTS.
-
-The following is an example input:
-
-```idf
-GroundHeatExchanger:Vertical,
-Vertical Ground Heat Exchanger, !- Name
-GHE Inlet Node,                 !- Inlet Node Name
-GHE Outlet Node,                !- Outlet Node Name
-0.00330000,                     !- Design Flow Rate {m3/s}
-120,                            !- Number of Bore Holes
-76.2,                           !- Bore Hole Length {m}
-.635080E-01,                    !- Bore Hole Radius {m}
-.692626E+00,                    !- Ground Thermal Conductivity {W/m-K}
-.234700E+07,                    !- Ground Thermal Heat Capacity {J/m3-K}
-13.375,                         !- Ground Temperature {C}
-.692626E+00,                    !- Grout Thermal Conductivity {W/m-K}
-.391312E+00,                    !- Pipe Thermal Conductivity {W/m-K}
-2.66667E-02,                    !- Pipe Out Diameter {m}
-2.53977E-02,                    !- U-Tube Distance {m}
-2.41285E-03,                    !- Pipe Thickness {m}
-2,                              !- Maximum Length of Simulation
-0.0005,                         !- G-Function Reference Ratio
-35,                             !- Number of Data Pairs of the G Function
-! The G-function is defined by the following data pairs
--15.2996, -0.348322,            ! G-Function Ln(T/Ts) Value 1, G-Function G Value 1
--14.201,  0.022208,             ! G-Function Ln(T/Ts) Value 2, G-Function G Value 2
--13.2202, 0.412345,             ! G-Function Ln(T/Ts) Value 3, G-Function G Value 3
--12.2086, 0.867498,             ! G-Function Ln(T/Ts) Value 4, G-Function G Value 4
--11.1888, 1.357839,             ! G-Function Ln(T/Ts) Value 5, G-Function G Value 5
--10.1816, 1.852024,             ! G-Function Ln(T/Ts) Value 6, G-Function G Value 6
--9.1815,  2.345656,             ! G-Function Ln(T/Ts) Value 7, G-Function G Value 7
--8.6809,  2.593958,             ! G-Function Ln(T/Ts) Value 8, G-Function G Value 8
--8.5,     2.679,                ! etc, etc.
--7.8,     3.023,
--7.2,     3.32,
--6.5,     3.681,
--5.9,     4.071,
--5.2,     4.828,
--4.5,     6.253,
--3.963,   7.894,
--3.27,    11.82,
--2.864,   15.117,
--2.577,   18.006,
--2.171,   22.887,
--1.884,   26.924,
--1.191,   38.004,
--0.497,   49.919,
--0.274,   53.407,
--0.051,   56.632,
-0.196,    59.825,
-0.419,    62.349,
-0.642,    64.524,
-0.873,    66.412,
-1.112,    67.993,
-1.335,    69.162,
-1.679,    70.476,
-2.028,    71.361,
-2.275,    71.79,
-3.003,    72.511;               !- 35 PAIRS
-```
-
-### Vertical Ground Heat Exchanger Outputs
-
-* HVAC,Average,Ground Heat Exchanger Average Borehole Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Heat Transfer Rate [W]
-
-* HVAC,Average,Ground Heat Exchanger Inlet Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Outlet Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Mass Flow Rate [kg/s]
-
-* HVAC,Average,Ground Heat Exchanger Average Fluid Temperature [C]
-
-#### Ground Heat Exchanger Average Borehole Temperature [C]
-
-This is the model result for the average temperature of the borehole heat exchanger.
-
-#### Ground Heat Exchanger Heat Transfer Rate [W]
-
-This is the rate of heat transfer between the working fluid and the ground heat exchanger, in Watts.
-
-#### Ground Heat Exchanger Inlet Temperature [C]
-
-This is the temperature of the working fluid entering the ground heat exchanger.
-
-#### Ground Heat Exchanger Outlet Temperature [C]
-
-This is the temperature of the working fluid leaving the ground heat exchanger.
-
-#### Ground Heat Exchanger Mass Flow Rate [kg/s]
-
-This is the mass flow rate of the working fluid through the heat exchanger.
-
-#### Ground Heat Exchanger Average Fluid Temperature [C]
-
-This is the average temperature of the working fluid inside the heat exchanger.
-
-
-
-### GroundHeatExchanger:Slinky
-
-The GroundHeatExchanger:Slinky use the g-functions to calculate the GHX temperature response, similar to the GroundHeatExchanger:Vertical model, however for this model g-functions are automatically calculated by EnergyPlus without the need of external software or data.
-
-Horizontal slinky-loop ground heat exchangers (GHXs) consist of coiled tubing, with the individual rings spread out along the direction of the trench either horizontally or vertically, as shown in [Figure](#SlinkyIOFig1). A schematic of a slinky GHX can be seen in [Figure](#SlinkyIOFig2). Compared to conventional straight tube horizontal GHXs, slinky loops have a higher tube density; hence, with the same cooling/heating loads, slinky-loop GHXs require less land area and excavation work than straight tube HGHXs.
-
-![slinky heat exchanger](media/image901.png)
-
-Figure: Slinky Ground Heat Exchanger Configurations. <a name="SlinkyIOFig1"></a>
-
-![slinky heat exchanger](media/image902.png)
-
-Figure: Schematic of Slinky HX. <a name="SlinkyIOFig2"></a>
-
-An example GroundHeatExchanger:Slinky object is shown below.
-
-```idf
-GroundHeatExchanger:Slinky,
-  Slinky GHX,       !- Name
-  GHE Inlet Node,   !- Inlet Node
-  GHE Outlet Node,  !- Outlet Node
-  0.0033,           !- Design Flow Rate [m3/s]
-  1.2,              !- Soil Thermal Conductivity [W/m-K]
-  3200,             !- Soil Density [kg/m3]
-  850,              !- Soil Specific Heat [J/kg-K]
-  1.8,              !- Pipe Thermal Conductivity [W/m-K]
-  920,              !- Pipe Density [kg/m3]
-  2200,             !- Pipe Specific Heat [J/kg-K]
-  0.02667,          !- Pipe Outside Diameter [m]
-  0.002413,         !- Pipe Wall Thickness [m]
-  Vertical,         !- Heat Exchanger Configuration (Vertical, Horizontal)
-  1,                !- Coil Diameter [m]
-  0.2,              !- Coil Pitch [m]
-  2.5,              !- Trench Depth [m]
-  40,               !- Trench Length [m]
-  15,               !- Number of Parallel Trenches
-  2,                !- Trench Spacing [m]
-  Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
-  KATemps,          !- Name of Undisturbed Ground Temperature Object
-  10;               !- Maximum length of simulation [years]
-```
-
-
-#### Field: Name
-
-Alpha field used as identifying field for heat exchanger
-
-#### Field: Inlet Node
-
-This alpha field is the name of the inlet node of the component on a plant loop.
-
-#### Field: Outlet Node
-
-This alpha field is the name of the outlet node of the component on a plant loop.
-
-#### Field: Design Flow Rate
-
-This numeric field is the design flow rate in m3/s for the heat exchanger. The plant loop will attempt to meet this request based on loop and flow conditions.
-
-#### Field: Soil Thermal Conductivity
-
-This numeric field is the thermal conductivity of the soil, in W/m-K.
-
-#### Field: Soil Density
-
-This numeric field is the density of the soil, in kg/m3.
-
-#### Field: Soil Specific Heat
-
-This numeric field is the specific heat of the soil, in J/kg-K.
-
-#### Field: Pipe Thermal Conductivity
-
-This numeric field is the thermal conductivity of the heat exchanger pipe.
-
-#### Field: Pipe Density
-
-This numeric field is the density of the heat exchanger pipe, in kg/m3.
-
-#### Field: Pipe Specific Heat
-
-This numeric field is the specific heat of the heat exchanger pipe, in J/kg-K.
-
-#### Field: Pipe Outside Diameter
-
-This numeric field is the outside pipe diameter, in meters.
-
-#### Field: Pipe Wall Thickness
-
-This numeric field is the pipe wall thickness, in meters.
-
-#### Field: Heat Exchanger Configuration
-
-This alpha field is heat exchanger configuration, either Vertical or Horizontal.
-
-#### Field: Coil Diameter
-
-This numeric is the diameter of the slinky coil, in meters.
-
-#### Field: Coil Pitch
-
-This numeric field is the center-to-center distance between heat exchanger coils, in meters.
-
-#### Field: Trench Depth
-
-This numeric field is the distance from the bottom of the trench to the ground surface, in meters.
-
-#### Field: Trench Length
-
-This numeric field is the length of the heat exchanger trench, in meters. This assumes the heat exchanger runs the full length of the trench.
-
-#### Field: Number of Parallel Trenches
-
-This numeric field is the number of parallel trenches. Design flow rate will be equally divided among all parallel trenches.
-
-#### Field: Trench Spacing
-
-This numeric field is the center-to-center distance in between parallel trenches, in meters.
-
-#### Field: Type of Undisturbed Ground Temperature Object
-
-The type of undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
-
-#### Field: Name of Undisturbed Ground Temperature Object
-
-The name of the undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
-
-#### Field: Maximum Length of Simulation
-
-This numeric field contains the maximum number of years of simulation to be carried out.
-
-### GroundHeatExchanger:Slinky Outputs
-
-The following output variables are available.
-
-* HVAC,Average,Ground Heat Exchanger Average Borehole Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Heat Transfer Rate [W]
-
-* HVAC,Average,Ground Heat Exchanger Inlet Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Outlet Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Mass Flow Rate [kg/s]
-
-* HVAC,Average,Ground Heat Exchanger Average Fluid Temperature [C]
-
-#### Ground Heat Exchanger Average Borehole Temperature [C]
-
-This is the model result for the average temperature of the borehole heat exchanger.
-
-#### Ground Heat Exchanger Heat Transfer Rate [W]
-
-This is the rate of heat transfer between the working fluid and the ground heat exchanger, in Watts.
-
-#### Ground Heat Exchanger Inlet Temperature [C]
-
-This is the temperature of the working fluid entering the ground heat exchanger.
-
-#### Ground Heat Exchanger Outlet Temperature [C]
-
-This is the temperature of the working fluid leaving the ground heat exchanger.
-
-#### Ground Heat Exchanger Mass Flow Rate [kg/s]
-
-This is the mass flow rate of the working fluid through the heat exchanger.
-
-#### Ground Heat Exchanger Average Fluid Temperature [C]
-
-This is the average temperature of the working fluid inside the heat exchanger.
-
-
-
-### GroundHeatExchanger:Pond
-
-The pond heat exchanger model represents a shallow pond with submerged hydronic tubes through which the heat transfer fluid is circulated. The model represents a 'shallow' pond in that no attempt is made to model any stratification effects that may  be present in deeper ponds.
-
-This type of heat exchanger is intended to be connected to the supply side of a condenser loop, and can be used with any type of plant loop. The pond may be specified as the only heat exchanger on the condenser loop (as shown in Figure 84) or it may be connected in parallel with other condenser loop heat exchangers (such as cooling towers, ground surface heat exchangers) as shown in the second figure below.
-
-![pond heat exchanger](media/image203.svg)
-
-Figure 84. Example of Pond Ground Heat Exchanger as only heat exchanger on condenser loop
-
-![pond surface heat exchangers](media/image204.svg)
-
-Figure 85. Pond Ground Heat Exchanger with other heat exchangers on condenser loop
-
-#### Field: Name
-
-This alpha field contains the identifying name for the outside pond heat exchanger.
-
-#### Field: Fluid Inlet Node Name
-
-This alpha field contains the fluid inlet node name.
-
-#### Field: Fluid Outlet Node Name
-
-This alpha field contains the fluid outlet node name.
-
-#### Field: Pond Depth
-
-This numeric field contains the pond depth {m}.
-
-#### Field: Pond Area
-
-This numeric field contains the pond area {m<sup>2}</sup>.
-
-#### Field: Hydronic Tubing Inside Diameter
-
-This numeric field contains the hydronic tubing inside diameter {m}.
-
-#### Field: Hydronic Tubing Outside Diameter
-
-This numeric field contains the hydronic tubing outside diameter {m}.
-
-#### Field: Hydronic Tubing Thermal Conductivity
-
-This numeric field contains the hydronic tubing thermal conductivity in W/mK.
-
-#### Field: Ground Thermal Conductivity
-
-This numeric field contains the ground thermal conductivity in W/m<sup>2</sup>K.
-
-#### Field: Number of Tubing Circuits
-
-This numeric field contains the number of hydronic tubing circuits, total in parallel in this pond..
-
-#### Field: Length of Each Tubing Circuit
-
-This numeric field contains length {m} of each hydronic tubing circuit.
-
-An example of the IDF is shown below.
-
-```idf
-  GroundHeatExchanger:Pond,
-    Pond 1,                  !- Name
-    Condenser Tower 1 Inlet Node,  !- Fluid Inlet Node Name
-    Condenser Tower 1 Outlet Node,  !- Fluid Outlet Node Name
-    2.0,                     !- Pond Depth {m}
-    1000.0,                  !- Pond Area {m2}
-    0.02,                    !- Hydronic Tubing Inside Diameter {m}
-    0.025,                   !- Hydronic Tubing Outside Diameter {m}
-    0.4,                     !- Hydronic Tubing Thermal Conductivity {W/m-K}
-    1.0,                     !- Ground Thermal Conductivity {W/m2-K}
-    10,                      !- Number of Tubing Circuits
-    50.0;                    !- Length of Each Tubing Circuit {m}
-```
-
-
-### Pond Heat Exchanger Outputs
-
-* HVAC,Average,Pond Heat Exchanger Heat Transfer Rate [W]
-
-* HVAC,Sum,Pond Heat Exchanger Heat Transfer Energy [J]
-
-* HVAC,Average,Pond Heat Exchanger Mass Flow Rate [kg/s]
-
-* HVAC,Average,Pond Heat Exchanger Inlet Temperature [C]
-
-* HVAC,Average,Pond Heat Exchanger Outlet Temperature [C]
-
-* HVAC,Average,Pond Heat Exchanger Bulk Temperature [C]
-
-#### Pond Heat Exchanger Heat Transfer Rate [W]
-
-#### Pond Heat Exchanger Heat Transfer Energy [J]
-
-These outputs are the pond ground heat exchanger heat transfer rate and total energy exchange for the timestep.
-
-#### Pond Heat Exchanger Mass Flow Rate [kg/s]
-
-#### Pond Heat Exchanger Inlet Temperature [C]
-
-#### Pond Heat Exchanger Outlet Temperature [C]
-
-These outputs are the pond fluid inlet and outlet temperatures and mass flow rate.
-
-#### Pond Heat Exchanger Bulk Temperature [C]
-
-This output is the pond bulk temperature.
-
-
-
-### GroundHeatExchanger:Surface
-
-The surface heat exchanger model is to simulate hydronic surface ground heat exchangers. This includes pavement surfaces with embedded pipes for snow-melting or heat rejection from hybrid ground source heat pump systems.
-
-The heat exchanger may be ground coupled or not. In the latter case the bottom surface is exposed to the wind but not solar gains. This type of heat exchanger is intended to be connected to the supply side of a condenser loop, and can be used with any type of plant loop. The surface heat exchanger may be specified as the only heat exchanger on the condenser loop (as shown in the first figure below) or it may be connected in parallel with other condenser loop heat exchangers (such as cooling towers, ground surface heat exchangers) as shown in the second figure below.
-
-![surface heat exchanger](media/image205.svg)
-
-Figure 86. Example of Surface Ground Heat Exchanger as only heat exchanger on condenser loop
-
-
-
-![tower surface heat exchangers](media/image206.svg)
-
-Figure 87. Surface Ground Heat Exchanger with other heat exchangers on condenser loop
-
-#### Field: Name
-
-This alpha field contains the identifying name for the outside panel heat exchanger.
-
-#### Field: Construction Name
-
-This alpha field contains the construction name. It must contain a valid “Construction� name that is usual for Surfaces. (Ref: Group – Surface Construction Elements).
-
-#### Field: Fluid Inlet Node Name
-
-This alpha field contains the fluid inlet node name.
-
-#### Field: Fluid Outlet Node Name
-
-This alpha field contains the fluid outlet node name.
-
-#### Field: Hydronic Tubing Inside Diameter
-
-This numeric field contains the hydronic tubing inside diameter in m.
-
-#### Field: Number of Tubing Circuits
-
-This numeric field contains the number of hydronic tubing circuits.
-
-#### Field: Hydronic Tube Spacing
-
-This numeric field contains the hydronic tube spacing in m.
-
-#### Field: Surface Length
-
-This numeric field contains the surface length in m.
-
-#### Field: Surface Width
-
-This numeric field contains the surface width in m.
-
-#### Field: Lower Surface Environment
-
-This alpha field expresses the lower surface exposure: Exposed or Ground.
-
-An example of this statement in an IDF is shown below:
-
-```idf
-  GroundHeatExchanger:Surface,
-    SURFACE 1,               !- Name
-    Outside Surface Construction,  !- Construction Name
-    Condenser Tower 1 Inlet Node,  !- Fluid Inlet Node Name
-    Condenser Tower 1 Outlet Node,  !- Fluid Outlet Node Name
-    0.02,                    !- Hydronic Tubing Inside Diameter {m}
-    10.0,                    !- Number of Tubing Circuits
-    0.3,                     !- Hydronic Tube Spacing {m}
-    100.0,                   !- Surface Length {m}
-    100.0,                   !- Surface Width {m}
-    GROUND;                  !- Lower Surface Environment
-```
-
-
-
-### Surface Ground Heat Exchanger Outputs
-
-* HVAC,Average,Ground Heat Exchanger Heat Transfer Rate [W]
-
-* HVAC,Average,Ground Heat Exchanger Surface Heat Transfer Rate [W]
-
-* HVAC,Sum,Ground Heat Exchanger Heat Transfer Energy [J]
-
-* HVAC,Average,Ground Heat Exchanger Mass Flow Rate [kg/s]
-
-* HVAC,Average,Ground Heat Exchanger Inlet Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Outlet Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Top Surface Temperature [C]
-
-* HVAC,Average Ground Heat Exchanger Bottom Surface Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Top Surface Heat Transfer Energy per Area [J/m2]
-
-* HVAC,Average,Ground Heat Exchanger Bottom Surface Heat Transfer Energy per Area[J/m2]
-
-* HVAC,Sum,Ground Heat Exchanger Surface Heat Transfer Energy [J]
-
-* HVAC,Average,Ground Heat Exchanger Source Temperature [C]
-
-
-#### Ground Heat Exchanger Heat Transfer Rate [W]
-
-#### Ground Heat Exchanger Surface Heat Transfer Rate [W]
-
-#### Ground Heat Exchanger Heat Transfer Energy [J]
-
-These outputs are the source heat transfer rate, surface heat transfer rate and the total source energy input for the timestep.
-
-#### Ground Heat Exchanger Mass Flow Rate [kg/s]
-
-#### Ground Heat Exchanger Inlet Temperature [C]
-
-#### Ground Heat Exchanger Outlet Temperature [C]
-
-These outputs are the surface heat exchanger fluid inlet and outlet temperatures and mass flow rate.
-
-#### Ground Heat Exchanger Top Surface Temperature [C]
-
-#### Ground Heat Exchanger Bottom Surface Temperature [C]
-
-These outputs are the surface heat exchanger top and bottom surface temperatures.
-
-#### Ground Heat Exchanger Top Surface Heat Transfer Energy per Area  [J/m<sup>2</sup>]
-
-#### Ground Heat Exchanger Bottom Surface Heat Transfer Energy per Area [J/m<sup>2</sup>]
-
-These outputs are the surface heat exchanger top and bottom surface flux.
-
-#### Ground Heat Exchanger Surface Heat Transfer Energy [J]
-
-This is the total surface energy exchange for the timestep.
-
-#### Ground Heat Exchanger Source Temperature [C]
-
-This is the surface heat exchanger source temperature.
-
-
-
-### GroundHeatExchanger:HorizontalTrench
-
-The horizontal trench ground heat exchanger object provides an alternate interface to the detailed PipingSystem:Underground:\* objects.  The same underlying simulation algorithm is utilized, providing a transient numerical simulation of soil with buried pipes and a detailed surface heat balance.  The input syntax is much smaller and useful for simple applications.  For full flexibility, use the PipingSystem:Underground:\* objects to build a detailed simulation domain and piping circuit.  For information regarding the simulation algorithms, see the engineering reference document section covering the buried piping system objects.
-
-***Field: Name***
-
-This alpha field is used as an identifying field for the ground heat exchanger.
-
-***Field: Inlet Node Name***
-
-This alpha field is the name of the inlet node of this component on a plant loop, and must match other topology definitions such as branch objects.
-
-***Field: Outlet Node Name***
-
-This alpha field is the name of the outlet node of this component on a plant loop, and must match other topology definitions such as branch objects.
-
-***Field: Design Flow Rate [m3/s]***
-
-This numeric field is the designed flow rate for this heat exchanger; the plant loop solver will attempt to meet this request based on flow and loop conditions.
-
-***Field: Trench Length in Pipe Axial Direction [m]***
-
-This numeric field represents the axial length of each pipe trench.  Each pipe defined for this ground heat exchanger will have the same length.  If different pipes have different lengths, they must use separate GroundHeatExchanger:HorizontalTrench objects with different lengths.
-
-***Field: Number of Trenches***
-
-This integer field is the number of trenches for this heat exchanger.  Since each trench has a single pipe, this defines the number of “pipe segments� for this overall heat exchanger.  The total piping length is then calculated as the trench length times the number of trenches.
-
-***Field: Horizontal Spacing Between Pipes [m]***
-
-This numeric field represents the horizontal spacing (pipe centroid to pipe centroid) between pipes/trenches.
-
-***Field: Pipe Inner Diameter [m]***
-
-This numeric field is the inner diameter of the pipe.  The same pipe properties are used for all pipes in this heat exchanger.
-
-***Field: Pipe Outer Diameter [m]***
-
-This numeric field is the outer diameter of the pipe.  The same pipe properties are used for all pipes in this heat exchanger.
-
-***Field: Burial Depth [m]***
-
-This numeric field is the burial depth of each pipe, from ground surface to pipe cross section centroid. The same pipe depth is used for all pipes in this heat exchanger.
-
-***Field: Soil Thermal Conductivity [W/mK]***
-
-This numeric field is the soil thermal conductivity.
-
-***Field: Soil Density [kg/m3]***
-
-This numeric field is the soil density.
-
-***Field: Soil Specific Heat [J/kgK]***
-
-This numeric field is the nominal soil specific heat, but is corrected for moisture content and in freezing conditions.
-
-***Field: Pipe Thermal Conductivity [W/mK]***
-
-This numeric field is the pipe thermal conductivity.
-
-***Field: Pipe Density [kg/m3]***
-
-This numeric field is the pipe density.
-
-***Field: Pipe Specific Heat [J/kgK]***
-
-This numeric field is the pipe specific heat.
-
-***Field: Soil Moisture Content Percent [%]***
-
-This numeric field represents the volume fraction, in percent, of water content in the soil.
-
-***Field: Soil Moisture Content Percent at Saturation [%]***
-
-This numeric field represents the volume fraction, in percent, of water content in the soil which results in saturation.
-
-#### Field: Type of Undisturbed Ground Temperature Object
-
-The type of undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
-
-#### Field: Name of Undisturbed Ground Temperature Object
-
-The name of the undisturbed ground temperature object used to determine ground temperature for the farfield boundary conditions.
-
-***Field: Evapotranspiration Ground Cover Parameter [-]***
-
-This numeric field specifies the ground cover effects used in the evapotranspiration model at the ground surface heat balance.  The values range from 0 (solid, non-permeable ground surface) to 1.5 (wild growth).
-
-An example of this statement in an IDF is shown below:
-
-```idf
-GroundHeatExchanger:HorizontalTrench,
-   My Pipe Circuit, !- Name
-   Plant Supply Intermediate Node, !- Inlet Node Name
-   Plant Supply Outlet Node, !- Outlet Node Name
-   0.004,       !- Design Flow Rate
-   75,          !- Trench Length in Pipe Axial Direction
-   2,           !- Number of Trenches
-   2.0,         !- Horizontal Spacing Between Pipes
-   0.016,       !- Pipe Inner Diameter
-   0.02667,     !- Pipe Outer Diameter
-   1.25,        !- Burial Depth
-   1.08,        !- Soil Thermal Conductivity
-   962,         !- Soil Density
-   2576,        !- Soil Specific Heat
-   0.3895,      !- Pipe Thermal Conductivity {W/m-K}
-   641,         !- Pipe Density {kg/m3}
-   2405,        !- Pipe Specific Heat {J/kg-K}
-   30,          !- Soil Moisture Content Volume Fraction {percent}
-   50,          !- Soil Moisture Content Volume Fraction at Saturation {percent}
-   Site:GroundTemperature:Undisturbed:KusudaAchenbach, !- Type of Undisturbed Ground Temperature Object
-   KATemps,     !- Name of Undisturbed Ground Temperature Object
-   0.408;       !- Evapotranspiration Ground Cover Parameter
-```
-
-### Horizontal Trench Ground Heat Exchanger Outputs
-
-* HVAC,Average,Ground Heat Exchanger Mass Flow Rate [kg/s]
-
-* HVAC,Average,Ground Heat Exchanger Inlet Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Outlet Temperature [C]
-
-* HVAC,Average,Ground Heat Exchanger Fluid Heat Transfer Rate [W]
-
-
-#### Ground Heat Exchanger Mass Flow Rate [kg/s]
-
-The output provides the mass flow rate currently being sent through the heat exchanger.
-
-#### Ground Heat Exchanger Inlet Temperature [C]
-
-#### Ground Heat Exchanger Outlet Temperature [C]
-
-Temperature of fluid at the inlet and outlet of the heat exchanger.
-
-#### Ground Heat Exchanger Fluid Heat Transfer Rate [W]
-
-Heat transfer rate for the heat exchanger, defined as positive for ***fluid heat loss***.
-
-### HeatExchanger:FluidToFluid
-
-A fluid-to-fluid heat exchanger designed to couple the supply side of one plant or condenser loop to the demand side of another plant or condenser loop. This heat exchanger is fairly general and can be configured for use in any application where any two loops need to be connected together. The only constraints are that that one side must be connected to the supply side of one loop and the other side connected to the demand side of a different loop.  Because the heat exchanger is intended to be generic, its two sides are distinguished by the nature of loop side being connected.  One side is called “Loop Supply Side� to indicate the heat exchanger is situated on the supply side of a loop. The other side is called “Loop Demand Side� to indicate it is on the demand side of a loop.  The heat exchanger is intended to act as a supply component for the loop connected to it as the “Loop Supply Side� and as a demand component for the loop connected to it as the “Loop Demand Side.�  From the point of view of the heat exchanger model itself, the Loop Demand Side fluid serves as the source/sink to supply heating/cooling to the fluid in the Loop Supply Side.  Only hydronic “plant� fluids are allowed, no air-side connections are possible with this heat exchanger.
-
-![HX diagram draft.tif](media/image207.png)
-
-Figure 88. Plant Fluid-to-Fluid Heat Exchanger
-
-Various options are available for the heat exchanger model. The heat transfer between the two sides can be modeled using one of seven different models for different types of heat exchangers. Heat transfer is calculated and reported using a sign convention from chilled water applications where positive heat transfer indicates energy was extracted from the Loop Supply Side and added to the Loop Demand Side.
-
-There are eleven options for different ways to control the heat exchanger.  One general type of control is “OnOff� where the flow through the heat exchanger is either fully on or fully off.  Another type of control is “Modulated� where the flow through the Loop Demand Side is controlled to try and meet a target setpoint or load on the Loop Supply Side.
-
-This heat exchanger can be used for a wide variety of applications including chilled water, hot water, condenser, ground source, primary-secondary systems, etc.  As of Version 8.0, this object replaces three separate objects that were available prior to version 8.0 of EnergyPlus.  The former HeatExchanger:Hydronic object corresponds to a situation where the Loop Demand Side is the demand side of condenser loop, the Loop Supply Side is a the supply side of a chilled water loop, the control type is “CoolingSetpointOnOffWithComponentOverride,� and the remote override component is a chiller. The former HeatExchanger:WatersideEconomizer object corresponds to a situation where the Loop Demand Side is the demand side of condenser loop, the Loop Supply Side is a the supply side of a chilled water loop, and the control type is “CoolingDifferentialOnOff.�  The former HeatExchanger:Plate object corresponds to a situation where the Loop Demand Side is the demand side of a condenser loop, the Loop Supply Side is the supply side of a second condenser loop, and the control type is “UncontrolledOn.�
-
-#### Field: Name
-
-This alpha field provides the unique identifying name for this heat exchanger.
-
-#### Field: Availability Schedule Name
-
-This field specifies the name of an availability schedule that can be used for supervisory control of the device.  If blank, the default is that heat exchanger is always available.  If a scheduled is named here, then the heat exchanger is available for use whenever the schedule value is greater than zero.  The heat exchanger is not available whenever the schedule value is zero or less.
-
-#### Field: Loop Demand Side Inlet Node Name
-
-This field specifies the name of a plant system node that connects an inlet of the heat exchanger to the demand side of a loop.  This node must be on a branch located on the demand side of a plant or condenser loop.
-
-#### Field: Loop Demand Side Outlet Node Name
-
-This field specifies the name of a plant system node that connects an outlet of the heat exchanger to the demand side of a loop.  This node must be on a branch located on the demand side of a plant or condenser loop.
-
-#### Field: Loop Demand Side Design Flow Rate
-
-This field specifies the design flow rate, in m<sup>3</sup>/s, of the hydronic fluid passing through the heat exchanger on the Loop Demand Side. This field is autosizable. When autosized, this design flow rate is set to equal the design flow rate for the Loop Supply Side.
-
-#### Field: Loop Supply Side Inlet Node Name
-
-This field specifies the name of a plant system node that connects an inlet of the heat exchanger to the supply side of a loop.  This node must be on a branch located on the supply side of a plant or condenser loop.
-
-#### Field: Loop Supply Side Outlet Node Name
-
-This field specifies the name of a plant system node that connects an outlet of the heat exchanger to the supply side of a loop.  This node must be on a branch located on the supply side of a plant or condenser loop.
-
-#### Field: Loop Supply Side Design Flow Rate
-
-This field specifies the design flow rate, in m<sup>3</sup>/s, of the fluid passing through the heat exchanger on the Loop Supply Side. This field is autosizable. When autosized, this design flow rate is set equal to the overall design flow rate of the loop that is connected.  If a sizing factor is entered in the field below, then it is multiplied to modify the design flow rate.
-
-#### Field: Heat Exchange Model Type
-
-This alpha field identifies the nature of heat exchanger.  Heat exchanger model type is specified by one of the following four key word choices:
-
-- **CrossFlowBothUnMixed**.  Specifies a single-pass, cross-flow heat exchanger.  The effectiveness will be calculated using a cross-flow heat exchanger correlation for both streams unmixed.
-
-- **CrossFlowBothMixed**.  Specifies a single-pass, cross-flow heat exchanger. The effectiveness will be calculated using a cross-flow heat exchanger correlation for both streams mixed.
-
-- **CrossFlowSupplyMixedDemandUnMixed**.  Specifes a single-pass, cross-flow heat exchanger.  The effectiveness will be calculated using a cross-flow heat exchanger correlation for flow mixed on the Loop Supply side and flow unmixed on the Loop Demand Side.
-
-- **CrossFlowSupplyUnMixedDemandMixed**.   Specifes a single-pass, cross-flow heat exchanger.  The effectiveness will be calculated using a cross-flow heat exchanger correlation for flow unmixed on the Loop Supply side and flow mixed on the Loop Demand Side.
-
-- **CounterFlow**. Specifies a counter-flow shell and tube heat exchanger.  The effectiveness will be calculated using a counter-flow shell and tube heat exchanger correlation.
-
-- **ParallelFlow**. Specifies a parallel-flow shell and tube heat exchanger.  The effectiveness will be calculated using a parallel-flow shell and tube heat exchanger correlation.
-
-- **Ideal**. Specifies an ideal heat exchanger.  The effectiveness will be set to '1.0' and the specified UA will be ignored.  The heat transfer rate will be calculated as the maximum possible heat transfer rate.
-
-#### Field: Heat Exchanger U-Factor Times Area Value
-
-This numerical field is used to specify the overall U-Factor Times Area (UA) {W/K} for use in the calculation of the heat exchanger effectiveness using the appropriate D-NTU correlation.  If **Ideal** is specified as the heat exchanger type, the effectiveness will be set to 1.0. When set to autosize Heat Exchanger U-Factor Times Area Value is calculated based on an effectiveness of 1.0 where capacity is such that the temperatures in the Sizing:Plant objects for the two loops can be maintained.
-
-#### Field: Control Type
-
-This field is used to specify how the heat exchanger is to be controlled during operation.  Different applications for connecting two loops will require different control behavior and different control options are needed depending on the desired behavior.  There are the following eleven key choice options to choose from:
-
-- **UncontrolledOn**. This control mode is applicable to situations where the heat exchanger is passively running all the time and always transfers as much heat as possible between the fluid streams.  However there is one aspect of control in that it will only request flow on the Loop Demand Side when there is non-zero flow into the heat exchanger on the Loop Supply Side.  This control mode corresponds to that available in the HeatExchanger:Plate object prior to version 8.0.
-
-- **OperationSchemeModulated**.  This control mode is applicable to situations where the heat exchanger is controlled by an operation scheme (see objects called PlantEquipmentOperationScheme or CondenserEquipmentOperationSchemes).  When using this control mode the heat exchanger must be listed in PlantEquipmentList or a CondenserEquipmentList and it serves as a supply component.  The operation scheme will dispatch a load request to the heat exchanger which it will try meet by conditioning the fluid stream connected as the Loop Supply Side.  If the heat exchanger could exceed the load request, then the flow through the fluid stream connected as the Loop Demand Side will be modulated to just meet the load request.
-
-- **OperationSchemeOnOff**. This control mode is applicable to situations where the heat exchanger is controlled by an operation scheme (see objects called PlantEquipmentOperationScheme or CondenserEquipmentOperationSchemes).  When using this control mode the heat exchanger must be listed in PlantEquipmentList or a CondenserEquipmentList and it serves as a supply component.  The operation scheme will dispatch a load request to the heat exchanger which it will use as an on/off signal to decide if the heat exchange should run or not.  If it runs, it will run at full capacity and may exceed the load request.
-
-- **HeatingSetpointModulated**.  This control mode is applicable to situations where the Loop Demand Side can provide useful heating to the Loop Supply Side.  A heating setpoint is obtained from a node named in the following field.  If the setpoint and inlet temperatures are such that heat exchanger could transfer heat from the Loop Demand Side to the Loop Supply Side to meet the heating setpoint, then the heat exchanger will run.  The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate.  If the heat exchanger could overshoot the setpoint, then the flow through the fluid stream connected as the Loop Demand Side will be modulated to just meet the setpoint.
-
-- **HeatingSetpointOnOff**. This control mode is applicable to situations where the Loop Demand Side can provide useful heating to the Loop Supply Side.  A heating setpoint is obtained from a node named in the following field.  If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Demand Side to the Loop Supply Side to meet the heating setpoint, then the heat exchanger will run. The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate.  If it runs, it will run at full capacity and may overshoot the setpoint.
-
-- **CoolingSetpointModulated**.  This control mode is applicable to situations where the Loop Demand Side can provide useful cooling to the Loop Supply Side.  A cooling setpoint is obtained from a node named in the following field.  If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Supply Side to the Loop Demand Side to meet the cooling setpoint, then the heat exchanger will run. The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate. If the heat exchanger could undershoot the setpoint, then the flow through the fluid stream connected as the Loop Demand Side will be modulated to just meet the setpoint.
-
-- **CoolingSetpointOnOff**. This control mode is applicable to situations where the Loop Demand Side can provide useful cooling to the Loop Supply Side.  A cooling setpoint is obtained from a node named in the following field.  If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Supply Side to the Loop Demand Side to meet the cooling setpoint, then the heat exchanger will run. The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate. If it runs, it will run at full capacity and may undershoot the setpoint.  This control mode corresponds to that available in the HeatExchanger:WatersideEconomizer object prior to version 8.0.
-
-- **DualDeadbandSetpointModulated**. This control mode is applicable to situations where the Loop Demand Side can provide either useful cooling or heating to the Loop Supply Side.  A dual deadband setpoint is obtained from a node named in the following field.  If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Demand Side to the Loop Supply Side to meet the lower setpoint, then the heat exchanger will run. If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Supply Side to the Loop Demand Side to meet the high setpoint, then the heat exchanger will run. The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate.  If the heat exchanger could overshoot the lower setpoint, or undershoot the higher setpoint, then the flow through the fluid stream connected as the Loop Demand Side will be modulated to just meet the deadband setpoint.
-
-- **DualDeadbandSetpointOnOff**. This control mode is applicable to situations where the Loop Demand Side can provide either useful cooling or heating to the Loop Supply Side.  A dual deadband setpoint is obtained from a node named in the following field.  If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Demand Side to the Loop Supply Side to meet the lower setpoint, then the heat exchanger will run. If the setpoints and inlet temperatures are such that heat exchanger could transfer heat from the Loop Supply Side to the Loop Demand Side to meet the high setpoint, then the heat exchanger will run. The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate. If the heat exchanger runs, it will run at full capacity and may overshoot the lower setpoint or undershoot the higher setpoint.
-
-- **CoolingDifferentialOnOff**.  This control mode is applicable to situations where the Loop Demand Side can provide useful cooling to the Loop Supply Side.  This mode is similar to CoolingSetpointOnOff except that it ignores any cooling setpoint and its control is based only on the temperature difference between Loop Demand Side and the Loop Supply Side.  The inlet temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate.   This control mode corresponds to that available in the HeatExchanger:WatersideEconomizer object prior to version 8.0.
-
-- **CoolingSetpointOnOffWithComponentOverride**.  This control mode is applicable to situations where the heat exchanger operation is integrated with the operation of a specific chiller.  When conditions are favorable for the heat exchanger to provide cooling to the Loop Supply Side, the heat exchanger is run and the integrated chiller is turned off.  A cooling setpoint is obtained from a node named in the following field.   If it runs it will run at full capacity and may undershoot the setpoint.  The chiller that is integrated with the heat exchanger is identified by entering the names of the chiller’s inlet nodes in the input fields below.  The control decision can be based on one of three different temperature signals selected in the field below called Component Override Cooling Control Temperature Mode.  The setpoint and control signal temperatures must differ by more than the value set in the field called Minimum Temperature Difference to Activate Heat Exchanger for the heat exchanger to operate. This control mode corresponds to that available in the HeatExchanger:Hydronic object prior to version 8.0.
-
-#### Field: Heat Exchanger Setpoint Node Name
-
-This field specifies the name of a plant system node located on loop attached to the Loop Supply Side.  This field is used and required when the previous field is set to one of the “Setpoint� control types.  The node must have a temperature setpoint placed on it by a setpoint manager (or EMS actuator).
-
-If the previous field is set to DualDeadbandSetpointModulated or DeadbandSetpointOnOff then there must be a setpoint manager that places both a high and low setpoint on the node named in this field. (see SetpointManager:Scheduled:DualSetpoint).
-
-#### Field: Minimum Temperature Difference to Activate Heat Exchanger
-
-This field specifies the value of a temperature tolerance used in control decisions, in deg. Celsius.  Whenever the control logic needs to compare two temperatures, the value entered in this field is used as a threshold for comparisons.
-
-#### Field: Heat Transfer Metering End Use Type
-
-This field specifies how the metering for heat transfer will be accounted with respect to end uses.  Although the heat exchanger consumes no energy that needs to be metered, there are also meters for heat transfers that apply to the model. The nature of the end use may vary depending on the application that the heat exchanger is being used for.  The available choices are FreeCooling, HeatRecovery, HeatRejection, HeatRecoveryForCooling, HeatRecoveryForHeating, and LoopToLoop.
-
-#### Field: Component Override Loop Supply Side Inlet Node Name
-
-This field specifies the name of an inlet node for the remote component that will be integrated with this heat exchanger.  This inlet should be on the supply side of a loop -- typically chilled water inlet or return for a chiller.  This field and the next two are only used for the control type called CoolingSetpointOnOffWithComponentOverride.
-
-#### Field: Component Override Loop Demand Side Inlet Node Name
-
-This field specifies the name of an inlet node for the remote component that will be integrated with this heat exchanger.  This inlet should be on the demand side of a loop -- typically condenser water inlet or return for a water-cooled chiller.  This field is only used for the control type called CoolingSetpointOnOffWithComponentOverride.
-
-#### Field: Component Override Cooling Control Temperature Mode
-
-This field specifies which type of temperature is used to control a heat exchanger that uses the control type called CoolingSetpointOnOffWithComponentOverride.  There are three options: Loop, WetBulbTemperature, and DryBulbTemperature.  The option called “Loop� directs the program to use the inlet fluid temperature at the Loop Demand Side connection of  heat exchanger for the temperature used as a signal to be compared with the setpoint. The option call “WetBulbTemperature� uses the outdoor air wetbulb temperature as the signal.  The option called “DryBulbTemperature� uses the outdoor air drybulb temperature as the signal.
-
-#### Field: Sizing Factor
-
-This optional field can be used to modify the results of autosize calculations.  This sizing factor is used for this heat exchanger and modifies sizing results by multiplying them by the factor entered here.  This factor is applied to the Loop Supply Side Design Flow rate and in turn affects the heat exchanger UA and the loop demand side flow rate which are derived from that flow rate.  This allows fine control over the size of the heat exchanger when using autosize in those fields.
-
-#### Field: Operation Minimum Temperature Limit
-
-This optional field can be used to provide supervisory control of the heat exchanger. If either of the inlet temperatures are below this limit (°C), the heat exchanger will not operate.
-
-#### Field: Operation Maximum Temperature Limit
-
-This optional field can be used to provide supervisory control of the heat exchanger. If either of the inlet temperatures are above this limit  (°C), the heat exchanger will not operate.
-
-
-
-Some example IDF input objects follow.
-
-```idf
-
-  HeatExchanger:FluidToFluid,
-    CondenserLoop HX,!- Name
-    ALWAYS_ON,     !- Availability Schedule Name
-    CondenserLoop HX HX Inlet Node, !- Loop Demand Side Inlet Node Name
-    CondenserLoop HX HX Outlet Node, !- Loop Demand Side Outlet Node Name
-    autosize,                     !- Loop Demand Side Design Flow Rate
-    CondenserLoop Pump- HXNode,   !- Loop Supply Side Inlet Node Name
-    CondenserLoop HX- ChillerNode,!- Loop Supply Side Outlet Node Name
-    autosize,                !- Loop Supply Side Design Flow Rate
-    CounterFlow,             !- Heat Exchange Model Type
-    autosize,                !- Heat Exchanger U-Factor Times Area Value
-    CoolingDifferentialOnOff,    !- Control Type
-    ,   !- Heat Exchanger Setpoint Node Name
-    2.0,         !- Minimum Temperature Difference to Activate Heat Exchanger
-    FreeCooling;             !- Heat Transfer Metering End Use Type
-
-
-HeatExchanger:FluidToFluid,
-    SOURCE to TRANSFER HX , !- Name
-    AlwaysOnSchedule, !- Availability Schedule Name
-    SOURCE Demand HX Inlet Node , !- Loop Demand Side Inlet Node Name
-    SOURCE Demand HX Outlet Node , !- Loop Demand Side Outlet Node Name
-    0.003 , !- Loop Demand Side Design Flow Rate
-    TRANSFER HX Supply Inlet Node, !- Loop Supply Side Inlet Node Name
-    TRANSFER HX Supply Outlet Node, !- Loop Supply Side Outlet Node Name
-    0.003 , !- Loop Supply Side Design Flow Rate
-    CrossFlow, !- Heat Exchange Model Type
-    15000 , !- Heat Exchanger U-Factor Times Area Value
-    DualDeadbandSetpointModulated , !- Control Type
-    TRANSFER Supply Outlet Node, !- Heat Exchanger Setpoint Node Name
-    0.2 , !- Minimum Temperature Difference to Activate Heat Exchanger
-    LoopToLoop; !- Heat Transfer Metering End Use Type
-```
-
-
-### Fluid to Fluid Heat Exchanger Outputs
-
-#### Fluid Heat Exchanger Heat Transfer Rate [W]
-
-#### Fluid Heat Exchanger Heat Transfer Energy [J]
-
-These outputs are the rate and energy transferred from the Loop Supply Side to the Loop Demand Side.  The sign convention is taken from cooling or heat rejection applications such that positive values indicate cooling of the Loop Supply Side.
-
-#### Fluid Heat Exchanger Loop Supply Side Mass Flow Rate [kg/s]
-
-This is the system mass flow of fluid through the heat exchanger side connected as the Loop Supply Side, in kg/s.
-
-#### Fluid Heat Exchanger Loop Supply Side Inlet Temperature [C]
-
-This is the temperature, in degrees Celsius, of the fluid entering the heat exchanger on the side connected as the Loop Supply Side.
-
-#### Fluid Heat Exchanger Loop Supply Side Outlet Temperature [C]
-
-This is the temperature, in degrees Celsius, of the fluid leaving the heat exchanger on the side connected as the Loop Supply Side.
-
-#### Fluid Heat Exchanger Loop Demand Side Mass Flow Rate [kg/s]
-
-This is the system mass flow of fluid through the heat exchanger side connected as the Loop Demand Side, in kg/s.
-
-#### Fluid Heat Exchanger Loop Demand Side Inlet Temperature [C]
-
-This is the temperature, in degrees Celsius, of the fluid entering the heat exchanger on the side connected as the Loop Demand Side.
-
-#### Fluid Heat Exchanger Loop Demand Side Outlet Temperature [C]
-
-This is the temperature, in degrees Celsius, of the fluid leaving the heat exchanger on the side connected as the Loop Demand Side.
-
-#### Fluid Heat Exchanger Operation Status [0=off, 1= on]
-
-This output is a numeric flag that indicates whether or not the heat exchanger was operating or not.  If the value is 0, then the heat exchanger was not operating.  If the value is 1, then the heat was operating.
-
-#### Fluid Heat Exchanger Effectiveness [ ]
-
-This output is the calculated heat exchanger effectiveness (non-dimensional).  It is an intermediate value in the NTU model calculations for heat flow rate.  Values range between 0 and 1.0.  A value of 1.0 indicates ideal heat transfer.
-
-Group – Plant-Condenser Flow Control
-------------------------------------
-
-The connector list described earlier determines how the branches of a particular loop will be hooked together. These connections can be classified either as a separation of a single stream into several outlet streams (splitter) or the merging of several streams into a single outlet stream (mixer). Due to the limitation per branch of a single splitter and a single mixer, the connector list can only have two pieces of equipment as a maximum. The names defined for either/both the splitter or/and the mixer refer then to “component� definitions as described below.
-
-### Connector:Splitter, Connector:Mixer
-
-The format of both the **Connector:Splitter** and **Connector:Mixer** statements is similar. Both begin with an identifying name followed by the branch name of the “single side� of the component. In the case of the splitter, this is the inlet since the inlet stream is broken into several outlet streams. In the case of the mixer, this is the outlet since several streams are mixed together to form a single outlet. The remaining list of up to 50 names is simply the branch names of the outlet legs in the case of the splitter and inlet legs in the case of the mixer. No control logic is assume in these components—a determination of how much air to split in which direction using the splitter must be defined by other components.
-
-### Connector:Splitter
-
-#### Field: Name
-
-This alpha field contains the identifying name for the Splitter.
-
-#### Field: Inlet Branch Name
-
-This alpha field contains the identifying name for the Splitter Inlet Branch.
-
-#### Field: Outlet Branch &lt;x&gt; Name
-
-This alpha field contains the identifying names for the Splitter Outlet Branches and you enter as many outlet branches as needed.
-
-### Connector:Mixer
-
-#### Field: Name
-
-This alpha field contains the identifying name for the Mixer.
-
-#### Field: Outlet Branch Name
-
-This alpha field contains the identifying name for the Mixer Outlet Branch.
-
-#### Field: Inlet Branch &lt;x&gt; Name
-
-This alpha field contains the identifying names for the Mixer Inlet Branches and you enter as many inlet branch names as needed..
-
-An example of these statements in an IDF is:
-
-```idf
-Connector:Splitter,
-             CW Loop Splitter,
-             CW Pump Branch,
-             Little Chiller Branch,
-             Big Chiller Branch,
-             Purchased Cooling Branch,
-             Supply Bypass Branch;
-Connector:Mixer,
-             CW Loop Mixer,
-             Cooling Supply Outlet,
-             Little Chiller Branch,
-             Big Chiller Branch,
-             Purchased Cooling Branch,
-             Supply Bypass Branch;
-```
-
-
-
-### TemperingValve
-
-This object is used for special cases where plant flow control is needed to make efficient use of thermal storage. In certain solar hot water and heat recovery situations, a thermal storage tank may become warmer than is necessary or allowable for safe use of the hot water. Although real installations of a tempering, or anti-scald valve, would more commonly mix a new stream of mains water with the hot water to achieve a desired outlet temperature, this is difficult to model directly within EnergyPlus because plant loops need to be closed circuits. For many installations where the water entering the splitter is directly from the mains, such as make up water entering a water heater tank, the modeling provided with this object should be thermodynamically equivalent.
-
-The TemperingValve object models a temperature-controlled diversion valve. It models a valve on a bypass pipe that can open to divert flow around one or more plant components. It can only be used on one of two branches between a Splitter and a Mixer. The figure below shows the use of the tempering valve with a Water Heater:Mixed component on “Stream 2.�  The tempering valve acts to divert flow through the branch it is on in order to adjust the temperature at the outlet of the mixer. If the temperature at Stream 2 Source Node is warmer than the setpoint and the inlet flow is cooler than the setpoint, then a controller determines how much flow should bypass the storagew tank to achieve the desired setpoint.
-
-![Schematic](media/image208.png)
-
-Figure 89. Tempering Valve Schematic
-
-The TemperingValve is an **Active** component and the other path should have only **Passive** components. Only two paths in the splitter/mixer can be used; bypasses are not allowed. No other Connector:Splitter and Connector:Mixer pair can be used on the supply side of the plant loop.
-
-#### Field: Name
-
-This field should contain an unique name for each TemperingValve object
-
-#### Field: Inlet Node Name
-
-This field should contain the name of node which is the inlet for the valve.
-
-#### Field: Outlet Node Name
-
-This field should contain the name of node which is the outlet for the valve
-
-#### Field: Stream 2 Source Node Name
-
-This field should contain the name of node that is the inlet to the Mixer object for the second stream containing the component whose flow is being diverted.
-
-#### Field: Temperature Setpoint Node Name
-
-This field should contain the name of a node that has a temperature setpoint assigned to it. A separate set point manager object is needed to provide a set point on the node listed here.
-
-#### Field: Pump Outlet Node Name
-
-This field should contain the name of the node that is the outlet for the pump that is one the same plant loop. This is node is used to sense the total flow rate.
-
-This object is demonstrated in the example file called SolarCollectorFlatPlateWater.idf. An example of this object is:
-
-```idf
-TemperingValve,
-        DHW Anti-Scald Diverter,
-        DHW Anti-Scald Inlet Node, ! Inlet Node Name
-        DHW Anti-Scald Outlet Node, ! Outlet Node Name
-        SHW Storage Tank Use Outlet Node, ! Stream 2 Source Node Name
-        DHW Instantaneous Boost Outlet Node, ! Temperature Setpoint Node Name
-        DHW Use Side Pump Outlet;  ! pump outlet node
-```
-
-
-### Tempering Valve Outputs
-
-Use output variables for System Nodes for flow and temperature results.
-
-Group – Air Distribution
-------------------------
-
-### AirLoopHVAC
-
-Air loops along with zone equipment form the entire forced air heating and cooling system (air side). The main statement for defining an air loop is the *AirLoopHVAC* object described here. As with the main plant and condenser statements, several of the items in the AirLoopHVAC object definition are actually names that refer to other objects in the input file. After the AirLoopHVAC object name, four such list pointers are encountered: for controllers, system availability, branches, and connectors. The Controller List defines how the air loop will respond due to various inputs (control signals). The Availability Manager List refers to methods for controlling when a system is operational. This may be as simple as a schedule to define when the system is shutdown. The Branch List lists the branches that comprise the primary air system. Finally, the Connector List lists the connections between the branches. The branches and connections together define the primary air system topology.
-
-The only numeric input is the design primary air flow rate. This item is input just before the BranchList name.
-
-The next series of names refer to nodes for the various inlet and outlet points of the air loop. The air loop starts where the zone equipment ends. This is a single point consisting of the return air duct once all of the zone return air streams have been collected. While in reality, there is really only one point, for clarity within the simulation components and consistency with the other HVAC loop sections, this point in the systems is defined as two points: one that resides with the zone equipment simulation and one that is acted upon by the air loop simulation. Both node names must be entered into the input file, and both nodes must have unique names. Similarly, the end points of the air loop that also correspond to the beginning points of the zone equipment loop must also be defined. These consist of names referencing lists of up to three pairs of node names as shown below. Up to three air loop outlets are allowed to accommodate the simulation of three deck systems.
-
-#### Field: Name
-
-This field is a unique, user assigned name for a single instance of an AirLoopHVAC object. Any other object referencing this AirLoopHVAC will use this name.
-
-#### Field: Controller List Name
-
-This field is the name of a ControllerList object. A Controller List is simply a list of controllers giving both controller name and type. This Controller List specifies all the controllers that will act on this primary air loop. The order of the controllers in the list is significant: controllers are simulated sequentially in the order given in the Controller List.
-
-#### Field: Availability Manager List Name
-
-This field is the name of a AvailabilityManagerList object. A Availability Manager List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this primary air loop. That is, they determine when and if this air loop is on or off, overriding the control provided by the central fan on/off schedule.
-
-#### Field: Design Supply Air Flow Rate
-
-This is the system primary air design volumetric flow rate in cubic meters per second.
-
-#### Field: Branch List Name
-
-This field is the object name of a BranchList object (see BranchList and Branch). The BranchList named here specifies all the branches composing the primary air system. These branches, together with the Connectors listed in the ConnectorList, define the primary air system topology.
-
-#### Field: Connector List Name
-
-This field is the name of ConnectorList object. This ConnectorList object lists all the Connectors (by type and name) that are included in this primary air system. These Connectors, together with the Branches in the BranchList, define the topology of the primary air system.
-
-#### Field: Supply Side Inlet Node Name
-
-The name of the air entrance node of this primary air system. This is the inlet node for return air for this air system.
-
-#### Field: Demand Side Outlet Node Name
-
-The name of the air outlet node for the zone equipment group (ZoneHVAC:EquipmentConnections objects) attached to the primary air system. This should be the outlet node of a AirLoopHVAC:ZoneMixer in the AirLoopHVAC:ReturnPath for the zone equipment group attached to this primary air system.
-
-#### Field: Demand Side Inlet Node Names
-
-This field can be the name of a node which is the air inlet node for the zone equipment group (see ZoneHVAC:EquipmentConnections objects) attached to this primary air system. Or, this field can be the name of a node list containing one or more nodes (up to 3). These nodes should be the inlet nodes to the AirLoopHVAC:ZoneSplitter or AirLoopHVAC:SupplyPlenum in each of the AirLoopHVAC:SupplyPaths for the zone equipment groups attached to this primary air system. For single duct systems, there is only one node name in this list. For two and three duct systems, the order of the nodes in this list must correspond with the order of the nodes in the Supply Side Outlet Node Names list.
-
-#### Field: Supply Side Outlet Node Names
-
-This field can be the name of a node which is the air outlet node for each supply duct of this primary air system. Or, this field can be the name of a node list containing one or more nodes (up to 3). The list can contain the names of up to three nodes. For single duct systems, there is only one node name in this list. For two and three duct systems, the order of the nodes in this list must correspond with the order of the nodes in the Demand Side Inlet Node Names list.
-
-An example of this statement in an IDF is:
-
-```idf
-AirLoopHVAC,
-  Main Dual Duct Air Loop,           ! Primary Air Loop Name
-  Dual Duct System 1 Controllers,    ! Controller List
-  Dual Duct System 1 Schedule List , ! System Availability Manager List
-  1.3 ,                              ! Primary air design volumetric flow rate
-  Dual Duct Air Loop Branches ,      ! Air Loop Branch List Name
-  Dual Duct Connectors ,             ! Air Loop Connector List Name
-  Supply Fan Inlet Node ,            ! ReturnAir AirLoop Inlet Node
-  Return Air Mixer Outlet ,          ! ZoneEquipGroup Outlet Node
-  Zone Equipment Inlet Node List ,   ! SupplyAirPath ZoneEquipGroup Inlet Nodes
-  Air Loop Outlet Node List ;        ! AirLoop Outlet Nodes
-```
-
-
-### AirLoopHVAC Outputs
-
-* HVAC,Average,Air System Simulation Cycle On Off Status
-
-* HVAC,Sum,HVAC System Solver Iteration Count []
-
-* HVAC,Sum,Air System Solver Iteration Count []
-
-* HVAC,Sum,Air System Simulation Maximum Iteration Count []
-
-* HVAC,Sum,Air System Simulation Iteration Count []
-
-* HVAC,Sum,Air System Component Model Simulation Calls []
-
-
-#### Air System Simulation Cycle On Off Status
-
-This field is the availability status of an AirLoopHVAC. This status flag is a result of the calculations made by the System Availability Manager(s) listed in a System Availability Manager List. When a single availability manager is used in a System Availability Manager List, this is also the availability status reported by the specific availability manager (Ref. System Availability Manager Outputs). When multiple availability managers are used in a System Availability Manager List, the loop availability status is determine by the rules associated with AirLoopHVACs (see rules described for Group – System Availability Managers). The control status outputs are represented using integers 0 through 3.. These integers represent *NoAction* (0), *ForceOff* (1), *CycleOn* (2), and *CycleOnZoneFansOnly* (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-#### HVAC System Solver Iteration Count []
-
-#### Air System Solver Iteration Count []
-
-#### Air System Simulation Maximum Iteration Count []
-
-#### Air System Simulation Iteration Count []
-
-#### Air System Component Model Simulation Calls []
-
-These variables are simply counters of how many iterations were executed. The count for any given HVAC time step will be the iterations executed before convergence was achieved, or the max allowed in which case the simulation throws a warning and proceeds to the next time step.
-
-### Outdoor Air Ventilation Outputs
-
-This section provides more detailed information on the reporting available for outdoor air ventilation.  Sixteen cooling and heating load variables and eight energy summary variables are available that report the impact of system outdoor air on zone loads, system demand and total energy use. The representative air system shown in the diagram below shows outdoor air (OA), return air (RA), supply air (SA) and mixed air (MA).
-
-![VentRept](media/image209.png)
-
-Figure 90. Example System for Ventilation Loads Report
-
-The overall effect of outdoor air on the system shown above can be summarized by considering the mixing box. In this system, part or all of the return air is replaced by outdoor air. The presence of any heat recovery will already be taken into account and thus will automatically be accounted for by using the outdoor air inlet conditions to the mixing box (point OA in the diagram) rather than actual outdoor air conditions. Thus, the overall energy impact of outdoor air (ventilation) on a particular system can be evaluated by multiplying the outdoor air mass flow rate by the enthalpy difference between the outdoor air entering the mixing box (OA) and the return air entering the mixing box (RA’) as shown in the following equation.
-
-<div>\[{\dot q_{OA}} = {\dot m_{OA}}\left( {{h_{OA}} - {h_{RA'}}} \right) = {\dot m_{sys}}\left( {{h_{MA}} - {h_{RA'}}} \right)\]</div>
-
-#### Ventilation Flow Outputs
-
-The fresh air flow into each zones are reported using the ventilation flow output variables. The total outdoor air flow in a primary air system is divided to each zone based on the fraction of flow each zone is supplied. There are six variables which deals with the mechanical ventilation flow reporting. Those six variables are:
-
-#### Zone Mechanical Ventilation Mass Flow Rate [kg/s]
-
-Reports the average outdoor air mass flow rate to any zone over the reporting interval.
-
-#### Zone Mechanical Ventilation Mass [kg]
-
-Reports the total outdoor air mass that has been supplied to any zone over the reporting interval.
-
-#### Zone Mechanical Ventilation Standard Density Volume Flow Rate [m3/s]
-
-Reports the average outdoor air volume flow rate to any zone over the reporting interval, calculated using a standard density for air.  Standard density in EnergyPlus corresponds to 20ºC drybulb, dry air, and nominally adjusted for elevation.
-
-#### Zone Mechanical Ventilation Standard Density Volume [m3]
-
-Reports the total outdoor air volume that has been supplied to a zone over the reporting interval, calculated using a standard density for air.  Standard density in EnergyPlus corresponds to 20ºC drybulb, dry air, and nominally adjusted for elevation.
-
-#### Zone Mechanical Ventilation Current Density Volume Flow Rate [m3/s]
-
-Reports the average outdoor air volume flow rate to any zone over the reporting interval, calculated using the current density for zone air.
-
-#### Zone Mechanical Ventilation Current Density Volume [m3]
-
-Reports the total outdoor air volume that has been supplied to a zone over the reporting interval, calculated using the current density for zone air.
-
-#### Zone Mechanical Ventilation Air Changes per Hour [ach]
-
-Reports the air changes per hour in the zone due to the outside fresh air supplied by mechanical ventilation system.
-
-The example syntax below shows the basic ventilation flow variables reported on an hourly basis.
-
-* Output:Variable,\*,Zone Mechanical Ventilation Mass Flow Rate,Hourly;
-
-* Output:Variable,\*,Zone Mechanical Ventilation Mass,Hourly;
-
-* Output:Variable,\*,Zone Mechanical Ventilation Standard Density Volume Flow Rate,Hourly;
-
-* Output:Variable,\*,Zone Mechanical Ventilation Standard Density Volume,Hourly;
-
-* Output:Variable,\*,Zone Mechanical Ventilation Current Density Volume Flow Rate,Hourly;
-
-* Output:Variable,\*,Zone Mechanical Ventilation Current Density Volume,Hourly;
-
-* Output:Variable,\*, Zone Mechanical Ventilation Air Changes per Hour,Hourly;
-
-
-#### Ventilation Load Reports
-
-The impact of system outdoor air on a particular zone may be calculated by summing the mass flow weighted <span>\({\dot q_{OA}}\)</span> over the supply air paths (both cooling and heating) serving the zone as follows:
-
-<div>\[{\dot q_{OA,Zone\;1}} = \sum\limits_{n = 1}^{AirPathNum} {{{\dot q}_{OA}}\frac{{{{\dot m}_n}}}{{{{\dot m}_{sys}}}}} \]</div>
-
-Four output variables each for cooling and heating report the impact of the ventilation air on the zone load in the absence of ventilation air system interactions. The ventilation load output variables are:
-
-#### Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy [J]
-
-#### Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy [J]
-
-The cooling/heating load that would occur once ventilation air met the zone cooling/heating load and continued to overcool/overheat the zone. No system effects are accounted for.
-
-#### Zone Mechanical Ventilation Cooling Load Decrease Energy [J]
-
-#### Zone Mechanical Ventilation Heating  Load Decrease[J]
-
-The decrease in zone cooling/heating load that would occur as a result of ventilation air introduced directly into the zone. No system effects are accounted for.
-
-#### Zone Mechanical Ventilation No Load Heat Removal Energy [J]
-
-#### Zone Mechanical Ventilation No Load Heat Addition Energy [J]
-
-The addition or removal of heat to a zone with no load. The heat addition or removal is due to mechanical ventilation while the zone thermostat is in the deadband.
-
-To summarize:
-
-**Cooling:**
-
-***1.    Zone Mechanical Ventilation No Load Heat Removal Energy [J]***
-
-Cooling that would be provided directly to zone by ventilation air. Ventilation occurred with no zone load.
-
-***2.    Zone Mechanical Ventilation Cooling Load Increase Energy [J]***
-
-The increase in zone cooling load that would occur as a result of ventilation air introduced directly into the zone. No system effects are accounted for.
-
-***3.    Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy [J]***
-
-The cooling load that would occur once ventilation air met the zone heating load and continued to overheat the zone. No system effects are accounted for.
-
-***4.    Zone Mechanical Ventilation Cooling Load Decrease Energy [J]***
-
-The decrease in zone cooling load that would occur as a result of ventilation air introduced directly into the zone. No system effects are accounted for.
-
-**Heating:**
-
-***1.    Zone Mechanical Ventilation No Load Heat Addition Energy [J]***
-
-Heating that would be provided directly to zone by ventilation air. Ventilation occurred with no zone load.
-
-***2.    Zone Mechanical Ventilation Heating Load Increase Energy [J]***
-
-The increase in zone heating load that would occur as a result of ventilation air introduced directly into the zone. No system effects are accounted for.
-
-***3.    Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy [J]***
-
-The heating load that would occur once ventilation air met the zone cooling load and continued to overcool the zone. No system effects are accounted for.
-
-***4.    Zone Mechanical Ventilation Heating Load Decrease Energy [J]***
-
-The decrease in zone heating load that would occur as a result of ventilation air introduced directly into the zone. No system effects are accounted for.
-
-The output variables are calculated by comparing the zone ventilation load with the zone cooling or heating load.  ‘Ventilation cooling’ decreases the zone cooling load until the cooling load has been eliminated. The remaining ‘ventilation cooling’ is reported as ‘overcooling’. ‘Overheating’ is calculated in the same manner. The actual system operation, which determines whether or not an ‘overcooling’ or ‘overheating’ load actually results in increased energy consumption, is not considered in the calculation of these output variables.
-
-The ventilation zone load output variables are shown in Table 24. The variables report the maximum potential “cost� or “benefit� of ventilation air introduced directly into the zone.
-
-Table 24. Ventilation Load Output Variables
-
-<table class="table table-striped">
-  <tr>
-    <th></th>
-    <th>No Zone Load</th>
-    <th>Zone Cooling Load</th>
-    <th>Zone Heating Load</th>
-  </tr>
-  <tr>
-    <td rowspan="2">Ventilation Cooling</td>
-    <td rowspan="2">Zone Mechanical Ventilation No Load Heat Removal Energy</td>
-    <td>Zone Mechanical Ventilation Cooling Load Decrease Energy</td>
-    <td rowspan="2">Zone Mechanical Ventilation Heating Load Increase Energy</td>
-  </tr>
-  <tr>
-    <td>Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Ventilation Heating</td>
-    <td rowspan="2">Zone Mechanical Ventilation No Load Heat Addition Energy</td>
-    <td rowspan="2">Zone Mechanical Ventilation Cooling Load Increase Energy</td>
-    <td>Zone Mechanical Ventilation Heating Load Decrease Energy</td>
-  </tr>
-  <tr>
-    <td>Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy</td>
-  </tr>
-</table>
-
-The example syntax below shows the basic ventilation load variables reported on a monthly basis.
-
-*   Output:Variable,\*,Zone Mechanical Ventilation Heating Load Increase Energy,monthly;
-
-*   Output:Variable,\*,Zone Mechanical Ventilation Heating Load Decrease Energy,monthly;
-
-*   Output:Variable,\*,Zone Mechanical Ventilation No Load Heat Addition Energy,monthly;
-
-*   Output:Variable,\*,Zone Mechanical Ventilation Cooling Load Increase Energy,monthly;
-
-*   Output:Variable,\*,Zone Mechanical Ventilation Cooling Load Decrease Energy,monthly;
-
-*   Output:Variable,\*,Zone Mechanical Ventilation No Load Heat Removal Energy,monthly;
-
-Reporting on a timestep or hourly level would produce a detailed report with variables intermingled with the other output variables that might be requested in the input file.
-
-Another method will more easily encapsulate the report:
-```idf
-OutputControl:Table:Style, HTML;     !- ColumnSeparator
-
-
-Output:Table:Monthly,
-  Ventilation Loads,       !- Name
-  ,                        !- DigitsAfterDecimal
-  Zone Mechanical Ventilation No Load Heat Removal Energy,
-         SumOrAverage,
-  Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy,
-         SumOrAverage,
-  Zone Mechanical Ventilation Cooling Load Decrease Energy,
-         SumOrAverage,
-  Zone Mechanical Ventilation Cooling Load Increase Energy,
-         SumOrAverage,
-  Zone Mechanical Ventilation No Load Heat Addition Energy,
-         SumOrAverage,
-  Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy,
-         SumOrAverage,
-  Zone Mechanical Ventilation Heating Load Decrease Energy,
-         SumOrAverage,
-  Zone Mechanical Ventilation Heating Load Increase Energy,
-         SumOrAverage;
-```
-
-This combination will report the ventilation loads on a monthly basis in a HTML style report that can be easily read in a web browser. Review the Output:Table:Monthly object for other methods of display or further options on this report item.
-
-### Systems Level Reporting
-
-Most output variables are a single entity reporting. Meters are a combination of like variables – specifically for Energy Consumption. This section introduces a slightly different concept – where output variables described herein are a combination of several similar items – specifically targeted at HVAC/System level reporting. This reporting is coupled with an Air Loop (ref: AirLoopHVAC)
-
-All items shown in this section are typical “output variables� and can be reported with the Output:Variable object.
-
-Or, as is shown by example here, perhaps a more readable form is to generate them in Tabular Form with the “Output:Table:Monthly� object.
-
-
-
-![system](media/image213.svg)
-
-Figure 91. View of System Level Reporting
-
-
-
-### System Loads Outputs
-
-In this category, the total system load is reported. Two aspects are reported here: Heating and Cooling. The following two variables report the heat energy that system components (including packaged equipment, fans, main coils, reheat coils, humidifiers, desiccant dehumidifiers, evaporative coolers and heat exchangers) add or remove from the air loop. Each variable within these grouping wil
-
-#### Air System Total Heating Energy
-
-Heat Addition to the Air Loop (Sum of all components) in Joules
-
-#### Air System Total Cooling Energy
-
-Heat Removal from the Air Loop (Sum of all components) in Joules
-
-In ‘Output:Table:Monthly’ format shown below.
-
-
-
-```idf
-  OutputControl:Table:Style,HTML;
-
-  Output:Table:Monthly,
-    System Loads,       !- Name
-    ,                        !- DigitsAfterDecimal
-    Air System Total Heating Energy,  SumOrAverage,
-    Air System Total Cooling Energy,  SumOrAverage;
-```
-
-
-### System Energy Use Outputs
-
-System Energy Use consists of six output variables that report the total energy (in Joules) and water consumption (in m<sup>3</sup>) for all system components and including packaged equipment, fans, main coils, reheat coils, humidifiers, desiccant dehumidifiers, and evaporative coolers. The output variables shown below show hot and cold water, steam, electric and gas energy. Hot and cold water energy includes all ‘district cooling’ and ‘district heating’ energy.
-
-#### Air System Hot Water Energy
-
-Hot Water Consumption for the system (Joules).
-
-#### Air System Steam Energy
-
-Steam Consumption for the system (Joules).
-
-#### Air System Chilled Water Energy
-
-Chilled Water Consumption for the system (Joules).
-
-#### Air System Electric Energy
-
-Electric Consumption for the system (Joules).
-
-#### Air System Gas Energy
-
-Gas (Natural Gas and Propane) Consumption for the system (Joules).
-
-#### Air System Water Volume
-
-Water Consumption for the system (humidifiers and evaporative coolers) (m3).
-
-The Standard reports file includes these variables reporting in the Tabular report form as “Air Loop System Energy and Water Use�.
-
-```idf
-  OutputControl:Table:Style,HTML;
-
-  Output:Table:Monthly,
-    Air Loop System Energy and Water Use,       !- Name
-    ,                        !- DigitsAfterDecimal
-    Air System Hot Water Energy ,  SumOrAverage,
-    Air System Steam Energy ,  SumOrAverage,
-    Air System Chilled Water Energy,  SumOrAverage,
-    Air System Electric Energy,  SumOrAverage,
-    Air System Gas Energy,  SumOrAverage,
-    Air System Water Volume,  SumOrAverage;
-```
-
-### System Component Loads Outputs
-
-Reporting System Component Loads shows the energy transferred to or extracted from the air loop by system component type. Fans, Cooling Coils, Heating Coils, Heat exchangers, humidifiers, evaporative coolers, and desiccant dehumidifiers show heat transfer rates in Joules. The components may be located in outdoor air systems bundled with packaged equipment or specified as stand-alone components. The reporting accounts for both main branch and reheat coils.
-
-The Standard reports file includes these variables reporting in the Tabular report form as “Air Loop System Component Loads�.
-
-
-```idf
-  OutputControl:Table:Style,HTML;
-
-
-  Output:Table:Monthly,
-    Air Loop System Component Loads,       !- Name
-    ,                        !- DigitsAfterDecimal
-    Air System Fan Air Heating Energy,  SumOrAverage,
-    Air System Cooling Coil Total Cooling Energy,  SumOrAverage,
-    Air System Heating Coil Total Heating Energy,  SumOrAverage,
-    Air System Heat Exchanger Total Heating Energy,  SumOrAverage,
-    Air System Heat Exchanger Total Cooling Energy,  SumOrAverage,
-    Air System Humidifier Total Heating Energy,  SumOrAverage,
-    Air System Evaporative Cooler Total Cooling Energy,  SumOrAverage,
-    Air System Desiccant Dehumidifier Total Cooling Energy,  SumOrAverage;
-```
-
-
-#### Air System Fan Air Heating Energy
-
-Energy added to the air loop by Fans (Joules)
-
-#### Air System Cooling Coil Total Cooling Energy
-
-Energy removed from air loop by Cooling Coils (Joules)
-
-#### Air System Heating Coil Total Heating Energy
-
-Energy added to air loop by Heating Coils (Joules)
-
-#### Air System Heat Exchanger Total Heating Energy
-
-Energy added to air loop by air-to-air heat recovery heat exchangers (Joules)
-
-#### Air System Heat Exchanger Total Cooling Energy
-
-Energy removed from air loop by air-to-air heat recovery heat exchangers (Joules)
-
-#### Air System Humidifier Total Heating Energy
-
-Energy added to air loop by humidifiers (Joules)
-
-#### Air System Evaporative Cooler Total Cooling Energy
-
-Energy removed from air loop by evaporative coolers (Joules)
-
-#### Air System Desiccant Dehumidifier Total Cooling Energy
-
-Energy removed from air loop by desiccant dehumidifiers (Joules)
-
-#### Air System Solar Collector Total Heating Energy
-
-Energy added to air loop by solar collectors (Joules)
-
-#### Air System Solar Collector Total Cooling Energy
-
-Energy removed from air loop by solar collectors (Joules)
-
-#### Air System User Defined Air Terminal Total Heating Energy
-
-Energy added to air loop by user defined air terminal units (Joules)
-
-#### Air System User Defined Air Terminal Total Cooling Energy
-
-Energy removed from air loop by user defined air terminal units (Joules)
-
-### System Component Energy Use Outputs
-
-Reporting System Component Energy Use consists of eleven output variables that report the total energy consumption (in Joules) of system components by energy type and coil type. Electric energy consumption is reported for fans, heating and cooling coils in packaged (DX) systems, electric resistance heating coils, humidifiers, evaporative coolers and desiccant dehumidifiers.
-
-#### Air System Fan Electric Energy
-
-Electric consumption for fans. (Joules)
-
-#### Air System Heating Coil Hot Water Energy
-
-Consumption for heating coil hot water (both purchased and plant supplied) (Joules)
-
-#### Air System Cooling Coil Chilled Water Energy
-
-Consumption for cooling coil chilled water (both purchased and plant supplied) (Joules)
-
-#### Air System DX Heating Coil Electric Energy
-
-Compressor plus condenser fan electricity use. (Joules)
-
-#### Air System DX Cooling Coil Electric Energy
-
-Compressor plus condenser fan electricity use. (Joules)
-
-#### Air System Heating Coil Electric Energy
-
-Electricity consumption for the heating coil. (Joules)
-
-#### Air System Heating Coil Gas Energy
-
-Gas (Propane and Natural Gas) consumption for the heating coil. (Joules)
-
-#### Air System Heating Coil Steam Energy
-
-Steam consumption for the heating coil (steam coils). (Joules)
-
-#### Air System Humidifier Electric Energy
-
-Electricity consumption for the humidifiers. (Joules)
-
-#### Air System Evaporative Cooler Electric Energy
-
-Electricity consumption for the evaporative coolers. (Joules)
-
-#### Air System Desiccant Dehumidifier Electric Energy
-
-Electricity consumption for the desiccant dehumidifiers. (Joules)
-
-The Standard reports file includes these variables reporting in the Tabular report form as “Air Loop System Component Energy Use�.
-
-
-```idf
-  OutputControl:Table:Style,HTML;
-
-
-  Output:Table:Monthly,
-    Air Loop System Component Energy Use,       !- Name
-    ,                        !- DigitsAfterDecimal
-    Air System Fan Electric Energy,  SumOrAverage,
-    Air System Heating Coil Hot Water Energy,  SumOrAverage,
-    Air System Cooling Coil Chilled Water Energy,  SumOrAverage,
-    Air System DX Heating Coil Electric Energy,  SumOrAverage,
-    Air System DX Cooling Coil Electric Energy,  SumOrAverage,
-    Air System Heating Coil Electric Energy,  SumOrAverage,
-    Air System Heating Coil Gas Energy,  SumOrAverage,
-    Air System Heating Coil Steam Energy,  SumOrAverage,
-    Air System Humidifier Electric Energy,  SumOrAverage,
-    Air System Evaporative Cooler Electric Energy,  SumOrAverage,
-    Air System Desiccant Dehumidifier Electric Energy,  SumOrAverage;
-```
-
-
-### Overall Air Loop Syntax
-
-A map for Air Loop input syntax is shown in the following diagram.
-
-![](media/image214.svg)
-
-Figure 92. Air Loop Input Syntax Map
-
-### AirLoopHVAC:ControllerList
-
-The syntax for the AirLoopHVAC:ControllerList definition is shown below. As with other lists in EnergyPlus input, the object title and identifying name are followed by type-name pairs. In this case, the types are controller types. The order in which controllers appear on this list also define the priority as described below. The identifying name refers back to the name recorded in the AirLoopHVAC statement.
-
-#### Field: Name
-
-The user designated unique name of an instance of a Controller List. Any object referencing this Controller List will do so using this name.
-
-#### Field Set (Object Type, Controller Name) up to 8
-
-After the identifying name, input for the controller list consists of up to 8 pairs of data items: a controller type and a controller name. The first controller listed has the highest priority, the second the second highest priority, and so forth.
-
-#### Field: Controller &lt;x&gt; Object Type
-
-The type of  controller. This should be a key word defining a class of controllers such as Controller:WaterCoil.
-
-#### Field: Controller &lt;x&gt; Name
-
-The name of a controller object (such as a Controller:WaterCoil) defined elsewhere in the input file.
-
-An example of this statement in an IDF is:
-
-```idf
-AirLoopHVAC:ControllerList,
-           Dual Duct System 1 Controllers,
-           Controller:WaterCoil, Main Cooling Coil Controller,
-           Controller:WaterCoil, Main Heating Coil Controller;
-```
-
-
-### AvailabilityManagerAssignmentList
-
-The AvailabilityManagerAssignmentList defines the applicable managers used for an AirLoopHVAC or PlantLoop. The priority of availability managers is based on a set of rules and are specific to the type of loop. The output from each Availability Manager is an availability status flag. This flag can have the values *NoAction*, *ForceOff*, *CycleOn*, or *CycleOnZoneFansOnly* (used only for air loops). The availability status flags for the Availability Managers referenced by an air or plant loop are used to set the availability status flag for each loop. For the air loops, *ForceOff* takes precedence: if any of the loop’s availability managers are showing status *ForceOff*, the loop status will be *ForceOff*. Next in precedence is *CycleOnZoneFansOnly,* followed by *CycleOn*, and *NoAction*. For the plant loops, there is no precedence among the Availability Manager status flag values. Instead, the first availability manager giving a status flag value other than *NoAction* sets the status for the loop. The Availability Managers are executed in Availability Manager List order.
-
-Special rules also apply for which managers may be listed in a Availability Manager list. The Hybrid Ventilation Control Manager (object: AvailabilityManager:HybridVentilation) is a special type of manager and is never specified in a Availability Manager List (it is used stand-alone for a specific air loop). All other types of availability managers may be listed in the Availability Manager List used for AirLoopHVACs. For Plant Loops, the Night Cycle and Night Ventilation managers (objects: AvailabilityManager:NightCycle  and AvailabilityManager:NightVentilation) are not allowed in the Availability Manager List.
-
-#### Field: Name
-
-The name of the AvailabilityManagerAssignmentList  object. This is referenced by AirLoopHVAC and PlantLoop objects.
-
-#### Field Set (Availability Manager Object Type, Name)
-
-Managers are listed by pairs of data items:  *Availability Manager Object Type* and *Availability Manager Name*. The managers are simulated down the list and calculate a control status for use by the AirLoopHVAC or PlantLoop. The priority of each manager used for a specific loop is based on the rules described above. Availability managers are not currently used for condenser loops. The availability managers, along with the AirLoopHVAC and PlantLoop object, report the control status calculated each simulation timestep. These output variables can be used to prioritize the managers according to the required control strategy. Six managers are accomodated in the list by default, however, this IDD specification is extensible. Additional pairs may be added by directly editing the IDD.
-
-#### Field: Availability Manager &lt;x&gt; Object Type
-
-The key word defining the type of manager, e.g. AvailabilityManager:NightCycle.
-
-#### Field: Availability Manager&lt;x&gt;  Name
-
-The name of a AvailabilityManager object defined elsewhere in the input file.
-
-An example of this statement in an IDF is:
-
-```idf
-AvailabilityManagerAssignmentList,
-  Collector Loop Availability Manager List,  !- Name
-  AvailabilityManager:HighTemperatureTurnOff,    !- System Availability Manager Type 1
-  High Temperature Turn Off Availability Manager,  !- System Availability Manager Name 1
-  AvailabilityManager:LowTemperatureTurnOn ,     !- System Availability Manager Type 2
-  Low Temperature Turn On Availability Manager,  !- System Availability Manager Name 2
-  AvailabilityManager:DifferentialThermostat,    !- System Availability Manager Type 3
-  Differential Thermostat Availability Manager;  !- System Availability Manager Name 3
-```
-
-
-### AirLoopHVAC:OutdoorAirSystem
-
-The Outside Air System (object AirLoopHVAC:OutdoorAirSystem) is a subsystem of an AirLoopHVAC. It handles the mixed air portion of the primary air system: the system relief air, the outside air inlet, and any components and controllers associated with the system relief air and outside air streams. From the perspective of the primary air loop the Outside Air System is treated as a single component. As a subsystem, it can contain one or more components and controllers.
-
-The input for the Outside Air System consists of a system name, a controller list name, an equipment list name, and an availability manager list name. The controller list simply lists, by type and unique name, all the controllers in the subsystem. The controllers will be simulated in list order. The equipment list lists all the components in the subsystem, by type and name. The equipment is simulated in list order. Finally, the availability manager list gives the type and name of the availability managers used by the subsystem.
-
-The equipment inlet/outlet must be sequential with no loops - the simulation can only handle a straight-through air path, both on the primary air side and on the secondary air side, if any. Heat exchanger secondary air inlets need to be independent of the primary air stream – usually relief air is used.
-
-#### Field: Name
-
-The unique, user assigned name for a single instance of an Outside Air System. Any other object referencing this Outside Air System will use this name.
-
-#### Field: Name: Controller List Name
-
-This field is the name of a AirLoopHVAC:ControllerList object. A AirLoopHVAC:ControllerList is simply a list of controllers giving both controller name and type. This Controller List specifies all the controllers that will act on this outside air system. The order of the controllers in the list is significant: controllers are simulated sequentially in the order given in the Controller List. Typically the Controller List would contain a Controller:OutdoorAir. If there are chilled water or hot water coils in the outdoor air system, each such coil will need a Controller:WaterCoil.
-
-#### Field: Outdoor Air Equipment List Name
-
-This field is the name of an AirLoopHVAC:OutdoorAirSystem:EquipmentList object. An AirLoopHVAC:OutdoorAirSystem:EquipmentList is simply a list of components giving both component name and type. This Outdoor Air Equipment List specifies all the components that will be simulated in this outside air system. The order of the components in the list is significant: components are simulated sequentially in the order given in the Outdoor Air Equipment List. Typically the equipment list would contain at least an OutdoorAir:Mixer. If there is more than one component, the components must be listed in order from the outside air to the OutdoorAir:Mixer (the OutdoorAir:Mixer is last).
-
-#### Field: Availability Manager List Name
-
-This field is the name of a AvailabilityManagerAssignmentList object. An Availability Manager List is a list of Availability Managers giving both Availability Manager Object Type and Name. **Use of this input is optional.** This field may be omitted; it is not currently used by the program.
-
-An IDF example, including the AirLoopHVAC, and the controller and equipment lists.
-
-
-
-```idf
-AirLoopHVAC,Typical Terminal Reheat 1,
-           Reheat System 1 Controllers,
-           Reheat System 1 Avail List,
-           1.3,
-           Air Loop Branches,,
-           Air Loop Inlet Node, Return Air Mixer Outlet,
-           Zone Equipment Inlet Node, Air Loop Outlet Node;
-
-AirLoopHVAC:ControllerList,
-           Reheat System 1 Controllers,
-           Controller:WaterCoil, Main Cooling Coil Controller;
-
-BranchList, Air Loop Branches,
-           Air Loop Main Branch;
-
-Branch, Air Loop Main Branch,
-           1.3,
-           ,
-           AirLoopHVAC:OutdoorAirSystem, OA Sys 1,
-           Air Loop Inlet Node, Mixed Air Node,PASSIVE
-           Fan:ConstantVolume, Supply Fan 1,
-           Mixed Air Node, Cooling Coil Air Inlet Node, ACTIVE,
-           Coil:Cooling:Water:DetailedGeometry, Detailed Cooling Coil,
-           Cooling Coil Air Inlet Node, Air Loop Outlet Node, PASSIVE;
-
-AvailabilityManagerAssignmentList, Reheat System 1 Avail List,
-           AvailabilityManager:Scheduled, Reheat System 1 Avail;
-
-AvailabilityManager:Scheduled, Reheat System 1 Avail,
-           FanAndCoilAvailSched;
-
-AirLoopHVAC:OutdoorAirSystem,
-           OA Sys 1,
-           OA Sys 1 Controllers,
-           OA Sys 1 Equipment;
-
-AirLoopHVAC:ControllerList,
-           OA Sys 1 Controllers,
-           Controller:OutdoorAir, OA Controller 1;
-
-AirLoopHVAC:OutdoorAirSystem:EquipmentList,
-           OA Sys 1 Equipment,
-           HeatExchanger:AirToAir:FlatPlate,OA Heat Recovery 1,
-           OutdoorAir:Mixer, OA Mixing Box 1;
-```
-
-
-### Outdoor Air System Outputs
-
-The impact of using outside air/mechanical ventilation is described in the section: Outdoor Air Ventilation Outputs.
-
-### AirLoopHVAC:OutdoorAirSystem:EquipmentList
-
-Used to specify the components in the outdoor air system. The components will be simulated in the order in which they occur in the list.
-
-The following HVAC equipment types are allowed as outdoor air system equipment. The component matrix shows which coils and fans are allowed with which equipment models.
-
-![](media/OASysComponentMatrix.png)
-
-#### Field: Name
-
-The user designated unique name of an instance of an Air Loop Equipment List. Any object referencing this Air Loop Equipment List will do so using this name.
-
-#### Field Set (Component Object Type,, Component Name) up to 8
-
-After the identifying name, the list consists of up to 8 pairs of data items:
-
-#### Field: Component &lt;x&gt; Object Type
-
-This field specifies the keyword for the type of component used.
-
-#### Field: Component &lt;x&gt; Name
-
-This field is the unique name of the component specified in the previous field. This named object must appear in the IDF.
-
-An example from an IDF:
-
-```idf
-AirLoopHVAC:OutdoorAirSystem:EquipmentList,
-           OA Sys 1 Equipment,
-           HeatExchanger:AirToAir:FlatPlate,OA Heat Recovery 1,
-           OutdoorAir:Mixer, OA Mixing Box 1;
-```
-
-### OutdoorAir:Node
-
-The OutdoorAir:Node object declares an HVAC system node for outdoor air conditions. The program automatically sets the air conditions at these nodes to correspond to the ambient environmental conditions at the beginning of every timestep. The outdoor air node is typically used as the inlet air node to an HVAC component such as the OutdoorAir:Mixer object. Multiple OutdoorAir:Node objects can be used in an input file, however, duplicate node names are not allowed.
-
-The *Height Above Ground* field is used to adjust the weather file air conditions, e.g., outdoor dry-bulb and wet-bulb air temperatures, for atmospheric variation with height. This variation can become a significant factor when modeling tall buildings. See the Engineering Reference section on Atmospheric Variation for a description of the algorithm for variation of atmospheric properties with height. A blank entry or a value less than zero for this field indicates that the height will be ignored and the weather file conditions will be used.
-
-**OutdoorAir:Node** and **OutdoorAir:NodeList** both set a node to outdoor air conditions. **OutdoorAir:Node** modifies the weather file conditions if a height has been specified. **OutdoorAir:NodeList** does not have a height input and always uses the weather file conditions without modification. The same node name may not be used with both of these objects.
-
-#### Field: Name
-
-The unique name for this outdoor air node.
-
-#### Field: Height Above Ground
-
-The height [m] of the node above ground level. A value greater than zero allows the weather file conditions, e.g., outdoor dry-bulb and wet-bulb air temperatures, to be adjusted according to atmospheric variation with height.
-
-A blank entry or value less than zero indicates that the height will be ignored and the weather file conditions will be used.
-
-An example IDF:
-
-```idf
-OutdoorAir:Node,
-  OA Node 1;  !- Name
-
-OutdoorAir:Node,
-  Floor 10 Outdoor air Inlet Node,  !- Name
-  30.0;  !- Height Above Ground {m}
-```
-
-
-
-### Outdoor Air Node outputs:
-
-The ambient dry-bulb air temperature and flow rate at the outdoor air node can be monitored using the system node output variables:
-
-* HVAC,Average,System Node Temperature [C]
-
-* HVAC,Average,System Node Mass Flow Rate [kg/s]
-
-e.g.
-
-```idf
-Output:Variable,
-  Floor 10 Outdoor air Inlet Node,
-  System Node Temperature,
-  Hourly;
-```
-
-
-### OutdoorAir:NodeList
-
-The program needs to know which HVAC system nodes are inlets for outdoor air. Knowing this, the program can set the conditions at these nodes to the outdoor conditions at the start of each major timestep. The OutdoorAir:NodeList provides the means for specifying which nodes are outdoor air nodes.
-
-The input is flexible: there may be one or more OutdoorAir:NodeList in each input file. Each list contains up to 25 names. The names can be the name of a unique HVAC system node, or the name of a Node List which will contain the actual node names. Duplicate node names are ignored.
-
-**OutdoorAir:Node** and **OutdoorAir:NodeList** both set a node to outdoor air conditions. **OutdoorAir:Node** modifies the weather file conditions if a height has been specified. **OutdoorAir:NodeList** does not have a height input and always uses the weather file conditions without modification. The same node name may not be used with both of these objects.
-
-#### Field: Node or NodeList name
-
-The name of an HVAC system node or of a NodeList object. There can be up to 25 names.
-
-An example IDF:
-
-```idf
-OutdoorAir:NodeList,
-    OutsideAirInletNodes;
-
-NodeList,OutsideAirInletNodes,
-    Outdoor air Inlet Node;
-```
-
-
-### OutdoorAir:Mixer
-
-The OutdoorAir:Mixer is the most common component used in an outdoor air system. The outdoor air mixer has 2 inlet air streams: the system return air and the outdoor air. It has 2 outlet air streams: the system relief air and the mixed air. This is a passive component. It takes the inlet mass flows and conditions plus the relief air mass flow and calculates the mixed air flow rate and conditions (as well as the relief air conditions). The inlet and relief mass flow must be set outside the component – most commonly by an outdoor air controller. The OutdoorAir:Mixer can also be used in compound components such as a fan coil unit.
-
-Input for this object is very simple: a unique name plus the node names of the 2 inlet nodes and the 2 outlet nodes.
-
-#### Field: Name
-
-A unique user assigned name for a particular outdoor air mixer component. Any reference to this component by another object will use this name.
-
-#### Field: Mixed Air Node Name
-
-The name of the HVAC system node which is the outlet for the mixed air stream.
-
-#### Field: Outdoor Air Stream Node Name
-
-The name of the HVAC system node which is the inlet for the outdoor air stream.
-
-#### Field: Relief Air Stream Node Name
-
-The name of the HVAC system node which is the outlet for the system relief air.
-
-#### Field: Return Air Stream Node Name
-
-The name of the HVAC system node which is the inlet for the return air stream.
-
-An IDF example:
-
-```idf
-OutdoorAir:Mixer,
-    Zone1WindACOAMixer,           ! name
-    Zone1WindACOAMixerOutletNode, ! mixer outlet node
-    Zone1WindACOAInNode,          ! mixer OA node
-    Zone1WindACExhNode,           ! mixer relief node
-    Zone1WindACAirInletNode;      ! mixer inlet node
-```
-
-
-Group – Airflow Network
------------------------
-
-### Overview
-
-The Airflow Network model provides the ability to simulate multizone airflows driven by wind and also by a forced air distribution system. The model can also simulate the heat and moisture gains or losses from the air distribution system itself (e.g., ductwork). When modeling an air distribution system, the current version of the Airflow Network model is restricted to a single forced air system (i.e., AirLoopHVAC object) with a constant volume supply air fan (Fan:ConstantVolume or Fan:OnOff). The capabilities of the model are to:
-
-- Simulate zone pressures due to envelope leakage and forced air distribution during HVAC system fan operation
-
-- Simulate node pressures in a forced air distribution system during HVAC system fan operation
-
-- Calculate multizone airflows due to forced air, wind, and surface leakage, including adjacent zones and outdoors, during HVAC system fan operation
-
-- Simulate distribution system airflows, including supply and return air leaks, during HVAC system fan operation
-
-- Simulate air distribution system node temperatures and humidity ratios during HVAC system fan operation
-
-- Calculate duct conduction losses during HVAC system fan operation
-
-- Calculate vapor diffusion losses of ducts during HVAC system fan operation
-
-- Calculate sensible and latent loads on the surrounding zones due to supply and return air leaks in the air distribution system during HVAC system fan operation
-
-- Simulate zone pressures due to envelope leakage driven by wind when the HVAC system fan is off or if no air distribution system is specified
-
-- Calculate multizone airflows due to wind and surface leakage, including adjacent zones and outdoors when the HVAC system fan is off or if no air distribution system is specified
-
-- Allow zone exhaust fans to be included as part of the airflow network
-
-- For airflow networks with a forced air distribution system, calculate zone sensible and latent loads for two different supply air fan operation modes as required: cycling fan, cycling compressor (CyclingFanAndCompressor) and continuous fan, cycling compressor (ContinuousFanWithCyclingCompressor)
-
-### Summary of Objects
-
-Before describing the Airflow Network input objects in detail, we list all of the objects and then give a short description of what the objects do.
-
-The Airflow Network input objects are:
-
-**AirflowNetwork:SimulationControl**
-
-**AirflowNetwork:Multizone:Zone**
-
-**AirflowNetwork:Multizone:Surface**
-
-**AirflowNetwork:MultiZone:Component:SimpleOpening**
-
-**AirflowNetwork:MultiZone:Component:DetailedOpening**
-
-**AirflowNetwork:MultiZone:Component:HorizontalOpening**
-
-**AirflowNetwork:MultiZone:Surface:Crack**
-
-**AirflowNetwork:MultiZone:ReferenceCrackConditions**
-
-**AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea**
-
-**AirflowNetwork:MultiZone:Component:ZoneExhaustFan**
-
-**AirflowNetwork:MultiZone:ExternalNode**
-
-**AirflowNetwork:MultiZone:WindPressureCoefficientArray**
-
-**AirflowNetwork:MultiZone:WindPressureCoefficientValues**
-
-**AirflowNetwork:Intrazone:Node**
-
-**AirflowNetwork:Intrazone:Linkage**
-
-**AirflowNetwork:Distribution:Node**
-
-**AirflowNetwork:Distribution:Component:Leak**
-
-**AirflowNetwork:Distribution:Component:LeakageRatio**
-
-**AirflowNetwork:Distribution:Component:Duct**
-
-**AirflowNetwork:Distribution:Component:ConstantPressureDrop**
-
-**AirflowNetwork:Distribution:Component:ConstantVolumeFan**
-
-**AirflowNetwork:Distribution:Component:Coil**
-
-**AirflowNetwork:Distribution:Component:HeatExchanger**
-
-**AirflowNetwork:Distribution:Component:TerminalUnit**
-
-**AirflowNetwork:Distribution:Linkage**
-
-** **
-
-- **AirflowNetwork:SimulationControl** defines basic run parameters for the air flow calculations and specifies whether wind pressure coefficients are input by the user or, for rectangular buildings, calculated by the program.
-
-- The **AirflowNetwork:Multizone:Zone** object specifies the ventilation control that applies to all of the openable exterior and interior windows and doors in the corresponding thermal zone. Surface-level ventilation control can be used to override the zone-level ventilation control if required (see AirflowNetwork: Multizone:Surface object below).
-
-- **AirflowNetwork:Multizone:Surface** object indicates whether a heat transfer surface (wall, window, etc.) has a crack or opening and references an **AirflowNetwork:MultiZone:Surface:Crack,
- AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea,
- AirflowNetwork:MultiZone:Component:SimpleOpening,
- AirflowNetwork:MultiZone:Component:DetailedOpening,
- AirflowNetwork:MultiZone:Component:HorizontalOpening
- or AirflowNetwork:MultiZone:Component:ZoneExhaustFan** object that gives the air flow characteristics of that crack, opening, or zone exhaust fan. The AirflowNetwork:Multizone:Surface object can also be used to specify individual ventilation control for openable exterior and interior windows and doors.
-
-- **AirflowNetwork:MultiZone:ReferenceCrackConditions** is used to normalize crack information that is based on measurements of crack air flow.
-
-- **AirflowNetwork:Distribution:Node** represents air distribution system nodes for the AirflowNetwork model. A set of an AirLoopHVAC and ZoneHVAC:EquipmentList nodes is a subset of the AirflowNetwork:Distribution:Nodes.
-
-- **AirflowNetwork:Distribution:Component** objects consist of **Leak, LeakageRatio, Duct, ConstantPressureDrop, ConstantVolumeFan, Coil,** and **TerminalUnit.** The components provide a relationship between pressure and airflow. The **Leak** and **Leakage** components can be used to simulate supply and/or return leaks in an air distribution system**.** The **Duct** and **ConstantPressureDrop components** can be used to deliver forced air into conditioned spaces. The components **ConstantVolumeFan, Coil, and TerminalUnit** reference normal EnergyPlus objects. The Airflow Network model gets information from these objects to perform an airflow network simulation.
-
-- **AirflowNetwork:Distribution:Linkage** object represents a connection between two node objects and an AirflowNetwork component. The node objects can be an AirflowNetwork:Distribution:Node, AirflowNetwork:MultiZone:ExternalNode or AirflowNetwork:Multizone:Zone.
-
-If you input wind pressure coefficients, **AirflowNetwork:Multizone:Surface** also has an associated **AirflowNetwork:MultiZone:ExternalNode**, that, via the **AirflowNetwork:Multizone:WindPressureCoefficientArray** and **AirflowNetwork:MultiZone:WindPressureCoefficientValues** objects, gives the wind pressure distribution vs. wind direction for that node and, implicitly, for the cracks and openings in the exterior surfaces associated with that node.
-
-Figure 93 shows the relationships among AirflowNetwork:Multizone objects and between AirflowNetwork:Multizone objects and regular EnergyPlus objects. In this figure an arrow from object A to object B means A references B, i.e., one of the inputs in A is the name of object B. For example, one input for AirflowNetwork: Multizone:Surface is the name of a heat transfer surface, and another is the name of a crack or opening object. The arrow between AirflowNetwork:Multizone:Surface and AirflowNetwork:MultiZone:ExternalNode is shown dashed to indicate that this reference is not used when wind pressure coefficients are calculated by the program rather than being input by the user.
-
-Figure 93 also shows the relationships among AirflowNetwork:Distribution objects and between AirflowNetwork:Distribution objects and regular EnergyPlus objects. The AirflowNetwork:Distribution:Linkage objects link two nodes from AirflowNetwork:Distribution:Node and/or AirflowNetwork:Multizone:Zone objects with a component defined in the object AirflowNetwork:Distribution:Component. The solid arrows show a reference from object A to object B. The dashed arrows indicate the components which can be used in a linkage object. The red arrows pointing to the Zone object indicate the components that interact with the zone air. For example, the temperature in a zone where a supply leak terminates is used to calculate duct leakage energy loss. The temperature in a zone where a duct component is located is also used to calculate duct conduction loss.
-
-![](media/image215.png)
-
-Figure 93. Relationships among AirflowNetwork objects (right-hand side) and between AirflowNetwork objects and regular EnergyPlus objects. An arrow from object A to object B means that A references B.
-
-Much of the information needed for the air flow calculation is automatically extracted from the building description for thermal modeling. This includes things like the volume and neutral height of the zones, and the orientation and location of the building surfaces that contain cracks or openings through which air flows. From all of this information the program creates a “pressure-flow network� that is solved each timestep using iterative solution methods to obtain the unknown pressures and air flows.
-
-Figure 94 shows a plan view of a very simple air flow network that you can construct using the above AirflowNetwork objects. There are three thermal zones, Zone-1, Zone-2 and Zone-3. There are openable exterior windows—Window-1, Window-2 and Window-3—and openable interior doors—Door-12 and Door-23. Two External Nodes are indicated. ExternalNode-1 is associated with the façade that contains Window-1 and Window-2. ExternalNode-2 is associated with the façade containing Window-3.
-
-One possible air flow pattern is shown in this figure. The actual air flow pattern in a particular timestep, and the size of the flows, depends on many factors, such as (1) What is the wind pressure distribution seen by the exterior windows? (2) Are the exterior windows open or closed, and if open, how far are they open? (3) Are the interior doors open or closed? (4) What are the air temperature differences between zones and between zones and the outdoor air (which affect buoyancy flows)?
-
-
-
-![](media/image216.svg)
-
-Figure 94. Plan view of a simple air flow network showing a possible air flow pattern in which all of the windows and doors are open.
-
-Figure 94 shows a possible air flow pattern in which all of the windows and doors are open. Associated with the external nodes are wind pressure coefficient distributions as a function of wind direction that are input using two AirflowNetwork:Multizone:Wind Pressure Coefficient objects. The nature of the air flows through the windows and doors is specified using AirflowNetwork:MultiZone:Component:DetailedOpening and AirflowNetwork:MultiZone:Component:SimpleOpening objects. The Airflow Network model calculates the flows each system timestep depending on various factors, including wind direction and speed, size and vertical position of openings, outdoor air temperature, and zone air temperatures.
-
-### Airflow Network Example Files (included in the installation)
-
-* AirflowNetwork3zVent.idf
-
-* AirflowNetwork3zVentAutoWPC.idf
-
-* AirflowNetwork\_Simple\_House.idf
-
-* AirflowNetwork\_Simple\_SmallOffice.idf
-
-* AirflowNetwork\_Multizone\_House.idf
-
-* AirflowNetwork\_MultiZone\_House\_OvercoolDehumid.idf
-
-* AirflowNetwork\_Multizone\_House\_TwoSpeed.idf
-
-* AirflowNetwork\_Multizone\_SmallOffice.idf
-
-* AirflowNetwork\_Multizone\_SmallOffice\_CoilHXAssistedDX.idf
-
-* AirflowNetwork\_MultiZone\_SmallOffice\_GenericContam.idf
-
-* AirflowNetwork\_Multizone\_SmallOffice\_HeatRecoveryHXSL.idf
-
-* AirflowNetwork\_Multizone\_SmallOffice\_VAV.idf
-
-* AirflowNetwor\_Multizone\_HorizontalOpening.idf
-
-* CrossVent\_1Zone\_AirflowNetwork.idf
-
-* DisplacementVent\_Nat\_AirflowNetwork.idf
-
-* HybridVentilationControl.idf
-
-### What the Airflow Network Model Can and Cannot Do
-
-Here is a list of some of the things that the Airflow Network calculation can and cannot model.
-
-#### Can Do
-
-1)   Air flow through cracks in exterior or interzone surfaces.
-
-2)   Air flow through cracks around windows and doors when closed.
-
-3)   Natural ventilation (i.e., air flow through open or partially open exterior windows and doors).
-
-4)   Zone level control of natural ventilation (all windows/doors in a zone that are defined with a component opening object have identical controls).
-
-5)   Individual surface control of natural ventilation for a subsurface (window, door, or glassdoor).
-
-6)   Modulation of natural ventilation to prevent large zone air temperature swings.
-
-7)   Interzone air flow (i.e., air flow through open interzone windows and doors, and through cracks in interzone surfaces).
-
-8)   Dependence of air flow on buoyancy effects and wind pressure.
-
-9)   Dependence of wind pressure on wind speed, wind direction and surface orientation.
-
-10)  Supply and return air leaks in an air distribution system.
-
-11)  Account for the effect of supply-air and/or return-air leakage on zone pressure when a forced air distribution system is present and is operating.
-
-12)  When duct leakage is modeled and the HVAC system is on, interzone airflow or infiltration/exfiltration can occur due to changes in zone pressure.
-
-13)  Bi-directional flow through large openings. See discussion below under AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:Multizone:Component:HorizontalOpening, and AirflowNetwork:Multizone:Component:SimpleOpening.
-
-14)  Calculate air flows and pressures in ducts or other components of a forced air distribution system.
-
-15)  Calculate zone loads when the supply air fan cycles on and off during a system timestep using the CyclingFanAndCompressor fan operation mode (Fan:OnOff).
-
-16)  Determine the impact of zone exhaust fans on air flows, pressures, air temperatures/humidity levels and energy consumption.
-
-#### Cannot Do or Restricted
-
-1)   The model is restricted to using a constant volume fan (Fan:ConstantVolume and Fan:OnOff) and cannot model variable volume fan equipment.
-
-2)   Air circulation and/or air temperature stratification within a thermal zone. For example, you should not try to divide a high space, such as an atrium, into subzones separated by artificial horizontal surfaces that have cracks or openings with the expectation that AirflowNetwork will give you a realistic temperature in each subzone and/or a realistic air flow between subzones.
-
-3)   The model is restricted to eleven types of coils that can be in the air distribution system (Coil:Cooling:DX:SingleSpeed, Coil:Heating:Gas, Coil:Heating:Electric,  Coil:Heating:DX:SingleSpeed, Coil:Cooling:Water, Coil:Heating:Water, Coil:Cooling:Water:DetailedGeometry, Coil:Cooling:DX:TwoStageWithHumidityControlMode, Coil:Cooling:DX:MultiSpeed, Coil:Heating:DX:MultiSpeed, and Coil:Heating:Desuperheater).
-
-4)   The model is restricted to a single type of air distribution equipment terminal units (AirTerminal:SingleDuct:ConstantVolume:Reheat).
-
-5)   Pollutant transport cannot currently be modeled.
-
-6)   Supply and return leaks are not allowed in an AirLoopHVAC. They can only be modeled in the Zone Equipment portion of the air loop (i.e., return leaks may be modeled between the zone return node and the zone mixer inlet or the zone mixer outlet and the zone equipment loop outlet; and supply leaks may be modeled between the zone equipment loop inlet and the AirLoopHVAC:ZoneSplitter inlet node or the AirLoopHVAC:ZoneSplitter outlet node and the zone supply node).
-
-7)   An air distribution system must be located inside the building (i.e., the ducts must pass through zones within the building).
-
-8)   Zone exhaust fans must be defined in ZoneHVAC:EquipmentConnections objects.
-
-
-
-The input specifications consist of five main sections: **AirflowNetwork:SimulationControl object, AirflowNetwork multizone data objects, AirflowNetwork distribution node objects, AirflowNetwork distribution component objects,** and **AirflowNetwork distribution linkage objects.** Each of these object types is described in detail below.
-
-### AirflowNetwork:SimulationControl
-
-The basic run parameters for this model are defined in this unique object which has the following input specifications:
-
-#### Field: Name
-
-This is a unique character string associated with this instance of the AirflowNetwork:SimulationControl object. At this time, only one AirflowNetwork:SimulationControl object can be specified in an input data file (idf).
-
-#### Field: AirflowNetwork Control
-
-The following selections are available to control the Airflow Network simulation:
-
-**MultizoneWithDistribution:** Multizone air flow calculations are performed during all simulation timesteps, including the impacts of the air distribution system when a HVAC system fan is operating. Any **ZoneInfiltration:\***, **ZoneVentilation:\***, **ZoneMixing** and **ZoneCrossMixing** objects specified in the input data file are not simulated.
-
-**MultizoneWithoutDistribution**: Multizone air flow calculations are performed during all simulation timesteps, but the air distribution system portion of the network is not modeled even if it is specified in the input data file. Any **ZoneInfiltration:\***, **ZoneVentilation:\***, **ZoneMixing** and **ZoneCrossMixing** objects specified in the input data file are not simulated.
-
-**MultizoneWithDistributionOnlyDuringFanOperation:** Multizone air flow calculations, including the impacts of the air distribution system, are only performed when the HVAC system fan is operating. Any **ZoneInfiltration:\***, **ZoneVentilation:\***, **ZoneMixing** and **ZoneCrossMixing** objects specified in the input data file are used when the HVAC system fan is OFF (if none are specified, then no air flow calculations are performed when the fan is OFF).
-
-**NoMultizoneOrDistribution:** No multizone air flow calculations (with or without the air distribution system portion of the network) are performed during the simulation. Any **ZoneInfiltration:\***, **ZoneVentilation:\***, **ZoneMixing** and **ZoneCrossMixing** objects specified in the input data file are simulated (if none are specified, then no air flow calculations are performed). Note: Having an input data file with no AirflowNetwork:SimulationControl objects gives the same impact – no multizone air flow calculations. However, this choice is provided as a convenience to the user to easily disable the multizone air flow calculations for an input data file that already contains AirflowNetwork objects.
-
-**Note:** A **ZoneInfiltration:\*** object indicates any one of **ZoneInfiltration:DesignFlowRate**, **ZoneInfiltration:EffectiveLeakageArea**,and **ZoneInfiltration:FlowCoefficient** objects.A object of**ZoneVentilation:\*** indicates any one of **ZoneVentilation:DesignFlowRate** and **ZoneVentilation:WindandStackOpenArea** objects**.**
-
-#### Field: Wind Pressure Coefficient Type
-
-Determines whether the wind pressure coefficients are input by the user or calculated. The choices are **Input** or **SurfaceAverageCalculation**, with the default being SurfaceAverageCalculation.
-
-If INPUT, you must enter an AirflowNetwork:MultiZone:WindPressureCoefficientArray object, one or more AirflowNetwork:MultiZone:ExternalNode objects, and one or more AirflowNetwork:MultiZone:WindPressureCoefficientValues objects.
-
-The second choice, SurfaceAverageCalculation, should only be used for **rectangular** buildings. In this case surface-average wind pressure coefficients vs. wind direction are calculated by the program for the four vertical facades and the roof based on user entries for “Building Type,� “Azimuth Angle of Long Axis of Building,� and “Ratio of Building Width Along Short Axis to Width Along Long Axis� (see description of these fields below). With this choice you do **not** have to enter any of the following objects: AirflowNetwork:MultiZone: Wind Pressure Coefficient Array, AirflowNetwork:MultiZone:ExternalNode and AirflowNetwork:MultiZone:WindPressureCoefficientValues.
-
-#### Field: AirflowNetwork Wind Pressure Coefficient Array Name
-
-This is the name of the AirflowNetwork:MultiZone:WindPressureCoefficientArray object that contains wind directions corresponding to the wind pressure coefficients given in the AirflowNetwork:MultiZone:WindPressureCoefficientValues objects.
-
-A value need be entered only if Wind Pressure Coefficient Type = INPUT (see description of previous field).
-
-#### Field: Height Selection for Local Wind Pressure Calculation
-
-Determines whether the local wind pressure is calculated based on either given external node heights or surface opening heights. The choices are **ExternalNode** or **OpeningHeight**, with the default being OpeningHeight. The local outdoor wind speed calculation procedure is given in the section of “Local Wind Speed Calculation� in the Engineering Reference. The calculation procedure requires the height input.
-
-If **ExternalNode**, the heights given in the AirflowNetwork:MultiZone:ExternalNode objects are used to calculate local wind pressures based on the given height local wind speed.  Used only if Wind Pressure Coefficient Type = INPUT (see description of previous field).
-
-If **OpeningHeight**, the number of the AirflowNetwork:MultiZone:ExternalNode objects has to be equal to the number of external surfaces defined in the AirflowNetwork:MultiZone:Surface objects. The centroids in the z direction of the AirflowNetwork:MultiZone:Surface objects are the heights used in the local wind pressure calculation with the given height wind speed. The input is required if Wind Pressure Coefficient Type = INPUT (see description of previous field).
-
-If Wind Pressure Coefficient Type = **SurfaceAverageCalculation**, a value in this field is not required and a blank may be entered. The default choice is used internally to generate the AirflowNetwork:MultiZone:ExternalNode objects
-
-#### Field: Building Type
-
-Used only if Wind Pressure Coefficient Type = SurfaceAverageCalculation. The choices for Building Type are LowRise and HighRise, with the default being LowRise.
-
-LowRise corresponds to a rectangular building whose height is less than three times the width of the footprint (*w<sub>short</sub>* in Figure 95) and is less than three times the length of the footprint (*w<sub>long</sub>* in the same figure).
-
-HighRise corresponds to a rectangular building whose height is more than three times the width of the footprint (*w<sub>short</sub>* in Figure 95) or is more than three times the length of the footprint (*w<sub>long</sub>* in the same figure).
-
-#### Field: Maximum Number of Iterations
-
-The maximum number of iterations allowed in finding an AirflowNetwork solution. If the number of iterations at each simulation timestep is above the maximum number of iterations defined by this field, the program could not find the solution and a Severe error is issued and the program is aborted. The default value is 500.
-
-#### Field: Initialization Type
-
-Designates which method is used for AirflowNetwork initialization. The choices for Initialization Type are LinearInitializationMethod and ZeroNodePressures, with the default being ZeroNodePressures.
-
-#### Field: Relative Airflow Convergence Tolerance
-
-The solution is assumed to have converged when <span>\({{\left| {\,\sum\limits_{} {{{\mathop m\limits^ \bullet  }_{_i}}} } \right|} \mathord{\left/ {\vphantom {{\left| {\,\sum\limits_{} {{{\mathop m\limits^ \bullet  }_{_i}}} } \right|} {\sum\limits_{} {\left| {{{\mathop m\limits^ \bullet  }_{_i}}} \right|} }}} \right. } {\sum\limits_{} {\left| {{{\mathop m\limits^ \bullet  }_{_i}}} \right|} }}\)</span>is less than the value specified for this input field. This convergence criteria is equivalent to the ratio of the absolute value of the sum of all network airflows (<span>\(\left| {\sum {{{\mathop m\limits^ \bullet  }_{_i}}} } \right|\)</span>) to the sum of network airflow magnitudes (<span>\(\sum\limits_{}^{} {\left| {{{\mathop m\limits^ \bullet  }_{_i}}} \right|} \)</span>). The default value is 1.0x10<sup>-4</sup>.
-
-#### Field: Absolute Airflow Convergence Tolerance
-
-The solution is assumed to have converged when the summation of the absolute value of all network airflows (<span>\(\left| {\sum {{{\mathop m\limits^ \bullet  }_{_i}}} } \right|\)</span>) is less than the value specified for this input field. The default value is 1.0x10<sup>-6</sup>.
-
-#### Field: Convergence Acceleration Limit
-
-If the ratio of successive pressure corrections is less than this limit, use Steffensen acceleration algorithm (Ref. AirflowNetwork Model in the EnergyPlus Engineering Reference). The range for this field is -1 to 1, with the default value being -0.5.
-
-#### Field: Azimuth Angle of Long Axis of Building
-
-Gives the orientation of a rectangular building for calculating wind pressure coefficients. This is the smaller of the angles, measured clockwise, between North and the long axis of the building (see Figure 95). Used only if Wind Pressure Coefficient Type = SurfaceAverageCalculation. The range for this input is 0 to 180, with the default value being 0.
-
-#### Field: Ratio of Building Width Along Short Axis to Width Along Long Axis
-
-This is the aspect ratio of a rectangular footprint. It is given by the width of the footprint along its short axis divided by the width along the long axis (see Figure 95). If the footprint is square, the value of this field is 1.0. Used only if Wind Pressure Coefficient Type = SurfaceAverageCalculation. The range for this input is &gt; 0 to 1, with the default value being 1.
-
-
-
-![](media/image221.svg)
-
-Figure 95. Footprint of a rectangular building showing variables used by the program to calculate surface-average wind pressure coefficients. The angle a is the “Azimuth Angle of Long Axis of Building.�  *w<sub>short</sub>*/*w<sub>long</sub>* is the “Ratio of Building Width Along Short Axis to Width Along Long Axis.�
-
-#### Field: Height Dependence of External Node Temperature
-
-This is an optional field. Input is Yes or No. The default is No. Yes is that external node temperature is dependent on node height. No means that external node temperature is calculated with zero height.
-
-
-
-An IDF example is shown below:
-
-```idf
-AirflowNetwork:SimulationControl,
-    AirflowNetwork_All,      !- Name
-    MultiZoneWithDistribution,  !- AirflowNetwork Control
-    Input,                   !- Wind Pressure Coefficient Type
-    Every 30 Degrees,        !- AirflowNetwork Wind Pressure Coefficient Array Name
-    OpeningHeight,           !- Height Selection for Local Wind Speed Calculation
-    LowRise,                 !- Building Type
-    500,                     !- Maximum Number of Iterations {dimensionless}
-    ZeroNodePressures,       !- Initialization Type
-    1.0E-05,                 !- Relative Airflow Convergence Tolerance {dimensionless}
-    1.0E-06,                 !- Absolute Airflow Convergence Tolerance {kg/s}
-    -0.5,                    !- Convergence Acceleration Limit {dimensionless}
-    0.0,                     !- Azimuth Angle of Long Axis of Building {deg}
-    1.0;                     !- Ratio of Building Width Along Short Axis to Width Along Long Axis
-```
-
-
-AirflowNetwork:Multizone data objects are used to calculate multizone airflows. This section describes the input requirements for the following objects:
-
-- AirflowNetwork:MultiZone:Zone
-
-AirflowNetwork:Multizone data objects are used to calculate multizone airflows. This section describes the input requirements for the following objects:
-
-- AirflowNetwork:MultiZone:Zone
-
-- AirflowNetwork:MultiZone:Surface
-
-- AirflowNetwork:MultiZone:Surface:Crack
-
-- AirflowNetwork:MultiZone:ReferenceCrackConditions
-
-- AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea
-
-- AirflowNetwork:MultiZone:Component:DetailedOpening
-
-- AirflowNetwork:MultiZone:Component:SimpleOpening
-
-- AirflowNetwork:MultiZone:Component:HorizontalOpening
-
-- AirflowNetwork:MultiZone:Component:ZoneExhaustFan
-
-- AirflowNetwork:MultiZone:ExternalNode
-
-- AirflowNetwork:MultiZone:WindPressureCoefficientArray
-
-- AirflowNetwork:MultiZone:WindPressureCoefficientValues
-
-A detailed description for each of these objects is provided below.
-
-### AirflowNetwork:Multizone:Zone
-
-This object allows control of natural ventilation through exterior and interior openings in a zone, where “opening� is defined as an openable window or door. (Note that only window, door or glass door subsurfaces in a zone that are specified using AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:MultiZone:Component:HorizontalOpening or AirflowNetwork:Multizone:Component:SimpleOpening and have an associated AirflowNetwork:Multizone:Surface object are considered to be openings). The control will be applied in the same way to all of the openings in the zone.
-
-This object is required to perform Airflow Network calculations. Note that ventilation control for all openings is provided at the zone level as default and individual ventilation control of a surface opening can be used to override the zone-level control (see the AirflowNetwork:Multizone:Surface object description below).
-
-#### Field: Zone Name
-
-The name of the EnergyPlus thermal zone corresponding to the AirflowNetwork zone.
-
-#### Field: Ventilation Control Mode
-
-Specifies the type of zone-level natural ventilation control.
-
-Let T<sub>out</sub> equal the outdoor air temperature, T<sub>zone</sub> equal the previous timestep’s zone air temperature, T<sub>set</sub> equal the Vent Temperature Schedule value, H<sub>zone</sub> equal the specific enthalpy of zone air from the previous timestep, and H<sub>out</sub> equal the specific enthalpy of outdoor air. Then the four allowed choices for Ventilation Control Mode are:
-
-**NoVent**: All of the zone’s openable windows and doors are closed at all times independent of indoor or outdoor conditions. The Venting Availability Schedule is ignored in this case. This is the default value for this field.
-
-**Temperature**: All of the zone’s openable windows and doors are opened if T<sub>zone</sub> &gt; T<sub>out</sub> **and** T<sub>zone</sub> &gt; T<sub>set</sub> **and** Venting Availability Schedule (see below) allows venting.
-
-**Enthalpy:** All of the zone’s openable windows and doors are opened if H<sub>zone</sub> &gt; H<sub>out</sub> **and** T<sub>zone</sub> &gt; T<sub>set</sub> **and** Venting Availability Schedule allows venting.
-
-**Constant**: Whenever this object’s Venting Availability Schedule allows venting, all of the zone’s openable windows and doors are open, independent of indoor or outdoor conditions. Note that “Constant� here means that the size of each opening is fixed while venting; the air flow through each opening can, of course, vary from timestep to timestep.
-
-**ASHRAE55Adaptive**: All of the zone’s operable windows and doors are opened if the operative temperature is greater than the comfort temperature (central line) calculated from the ASHRAE Standard 55-2010 adaptive comfort model and Venting Availability Schedule allows venting.
-
-**CEN15251Adaptive:** All of the zone’s operable windows and doors are opened if the operative temperature is greater than the comfort temperature (central line) calculated from the CEN15251 adaptive comfort model and Venting Availability Schedule allows venting.
-
-#### Field: Ventilation Control Zone Temperature Setpoint Schedule Name
-
-The name of a schedule of zone air temperature set points that controls the opening of windows and doors in the thermal zone to provide natural ventilation. This setpoint is the temperature above which all the openable windows and doors in the zone will be opened if the conditions described in the previous field Ventilation Control Mode are met.
-
-The Ventilation Control Zone Temperature Setpoint Schedule Name applies only to windows and doors in the zone that are specified using AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:MultiZone:Component:HorizontalOpening or AirflowNetwork:MultiZone:Component:SimpleOpening and have an associated AirflowNetwork:MultiZone:Surface object.
-
-(The discussion under the field Window/Door Opening Factor in the AirflowNetwork:MultiZone:Surface object describes how the actual opening area of a window or door in a particular timestep is determined.)
-
-*Modulation of Openings*
-
-The following five fields can be used to modulate the window/door openings when Ventilation Control Mode = Temperature or Enthalpy. These fields determine a factor between 0 and 1 that multiplies the opening factor of each window and door in the zone according to the control action shown in Figure 96 for Ventilation Control Mode = Temperature and in Figure 97 for Ventilation Control Mode = Enthalpy. Modulation of the openings can reduce the large temperature swings that can occur if the windows/doors are open too far when they are venting, especially when there is a large inside-outside temperature difference.
-
-The modulation takes the following form when Ventilation Control Mode = Temperature:
-
-**if** T<sub>zone</sub> - T<sub>out</sub>  &lt;=  [Lower Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor]  **then**  Multiplication factor = 1.0
-
-**if** [Lower Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor] &lt; T<sub>zone</sub> - T<sub>out</sub> &lt; [Upper Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor]  **then** Multiplication factor varies linearly from 1.0 to [Limit Value on Multiplier for Modulating Venting Open Factor]
-
-**if** T<sub>zone</sub> - T<sub>out</sub> &gt;=  [Upper Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor]  **then**  Multiplication factor = [Limit Value on Multiplier for Modulating Venting Open Factor]
-
-One way of “tuning� the following modulation control parameters is to perform a sensitivity analysis for winter and/or summer design days to determine what combination of values causes the biggest reduction in zone air temperature fluctuations due to venting.
-
-Note that the default values for the following fields are such that, if none of the fields are specified, the default values are assigned.
-
-#### Field: Minimum Venting Open Factor
-
-See Figure 96 or Figure 97. This field applies only if Ventilation Control Mode = Temperature or Enthalpy. This value may be from zero to 1.0, with the default being 0.0.
-
-#### Field: Indoor and Outdoor Temperature Difference Lower Limit For Maximum Venting Open Factor
-
-See Figure 96. This field applies only if Ventilation Control Mode = Temperature. This value may be from zero to less than 100ËšC, with the default being 0ËšC. The value for this field must be less than the value specified for the following field.
-
-#### Field: Indoor and Outdoor Temperature Difference Upper Limit for Minimun Venting Open Factor
-
-See Figure 96. This field applies only if Ventilation Control Mode = Temperature. This value must be greater than 0ËšC, with the default being 100ËšC. The value for this field must be greater than the value specified for the previous field..
-
-#### Field: Indoor and Outdoor Enthalpy Difference Lower Limit For Maximum Venting Open Factor
-
-See Figure 97. This field applies only if Ventilation Control Mode = Enthalpy. This value may be from zero to less than 300,000 J/kg, with the default being 0 J/kg. The value for this field must be less than the value specified for the following field.
-
-#### Field: Indoor and Outdoor Enthalpy Difference Upper Limit for Minimun Venting Open Factor
-
-See Figure 97. This field applies only if Ventilation Control Mode = Enthalpy. This value must be greater than zero, with the default being 300,000 J/kg. The value for this field must be greater than the value specified for the previous field.
-
-#### Field: Venting Availability Schedule Name
-
-The name of a schedule that specifies when venting is available. A zero or negative schedule value means venting is not allowed. A value greater than zero means venting can occur if other venting control conditions (specified by Ventilation Control Mode and Vent Temperature Schedule Name) are satisfied. This schedule name should not be confused with Vent Temperature Schedule Name.
-
-If a Venting Availability Schedule Name is not specified, it is assumed that venting is always available.
-
-Using Venting Availability Schedule allows you to turn off venting at certain times of the day (at night, for example), of the week (on weekends, for example), or of the year (during the winter, for example).
-
-If used with Ventilation Control Mode = Constant, the ventilation rate is constant only when this schedule allows venting; otherwise the ventilation rate is set to zero.
-
-If Ventilation Control Mode = NoVent, this schedule has no effect.
-
-#### Field: Occupant Ventilation Control Name
-The name of an AirlowNetwork:OccupantVentilationControl object. The object is used to perform advanced window opening control based on occupant conditions. When an object name is given, advanced window opening control is performed and, the ventilation control defined in the Ventilation Control Mode field will be overridden.
-
-**Note:** The Occupant Ventilation Control object can be assigned to a zone (AirflowNetwork:MultiZone:Zone) or a surface (AirflowNetwork:MultiZone:Surface). When the object is assigned to a zone, the Occupant Ventilation Control is assigned to the surfaces belonging to the zone automatically. The surface objects must have an associated AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:MultiZone:Component:HorizontalOpening, or  AirflowNetwork:MultiZone:Component:SimpleOpening component specified in the field of Leakage Component Name. All output variables will be shown under surface names only, and not under zone names.
-
-![](media/image222.svg)
-
-Figure 96. Modulation of venting area according to inside-outside temperature difference.
-
-
-
-![](media/image223.svg)
-
-Figure 97. Modulation of venting area according to inside-outside enthalpy difference.
-
-**Note:** In order to establish an airflow network, each AirflowNetwork:Multizone:Zone object must have at least two surfaces defined with AirflowNetwork:Multizone:Surface objects, so that air can flow from one zone into other zones (or to outdoors) through the network (air mass flow conserved). In addition, for all AirflowNetwork:Multizone:Surface objects facing the same Zone (ref. BuildingSurface:Detailed), at least two different environments must be defined for the other side of these surfaces (e.g., an external node and an adjacent zone, two adjacent zones, or two external nodes).
-
-An IDF example is shown below:
-
-
-```idf
-AirflowNetwork:MultiZone:Zone,
-    RESISTIVE ZONE,          !- Name of Associated Thermal Zone
-    Temperature,             !- Ventilation Control Mode
-    WindowVentSched,         !- Vent Temperature Schedule Name
-    0.3,                     !- Limit Value on Multiplier for Modulating Venting Open Factor
-                             !- {dimensionless}
-    5.0,                     !- Lower Value on Inside/Outside Temperature Difference for
-                             !- Modulating the Venting Open Factor {deltaC}
-    10.0,                    !- Upper Value on Inside/Outside Temperature Difference for
-                             !- Modulating the Venting Open Factor {deltaC}
-    0.0,                     !- Lower Value on Inside/Outside Enthalpy Difference for Modulating
-                             !- the Venting Open Factor {J/kg}
-    300000.0,                !- Upper Value on Inside/Outside Enthalpy Difference for Modulating
-                             !- the Venting Open Factor {J/kg}
-    VentingSched;            !- Venting Availability Schedule Name
-```
-
-### AirflowNetwork:Multizone:Surface
-
-The AirflowNetwork:Multizone:Surface object specifies the properties of a surface “linkage� through which air flows. This linkage is always associated with a heat transfer surface (wall, roof, floor, or a ceiling) or subsurface (door, glass door, or window) with both faces exposed to air. The linkage specifies two connected nodes: two zone nodes defined in AirflowNetwork:Multizone:Zone objects based on inside and outside face environment for an interior surface, or a zone node defined in an AirflowNetwork:Multizone:Zone object based on inside face environment and an external node defined in an AirflowNetwork:MultiZone:ExternalNode object for an exterior surface. The associated leakage component for this surface can be a crack (or surface effective leakage area) in an exterior or interior heat transfer surface or subsurface, or an exterior or interior window, door or glass door (heat transfer subsurface) that can be opened to allow air flow. The allowed surface air leakage components are:
-
-- AirflowNetwork:MultiZone:Surface:Crack
-
-- AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea
-
-- AirflowNetwork:MultiZone:Component:DetailedOpening
-
-- AirflowNetwork:MultiZone:Component:HorizontalOpening
-
-- AirflowNetwork:MultiZone:Component:SimpleOpening
-
-- AirflowNetwork:MultiZone:Component:ZoneExhaustFan
-
-The two “opening� components are used to modulate openness based on required conditions.
-
-The AirflowNetwork:Multizone:Surface object allows a heat transfer surface or subsurface to have one crack (or one surface effective leakage area object), or a subsurface (i.e., window, door or glass door) to have one opening (detailed or simple).
-
-An interior heat transfer surface (BuildingSurface:Detailed) whose surface name is used as the input for the Outside Boundary Condition Object field represents a floor without ground contact and is not allowed as an AirflowNetwork:Multizone:Surface. A heat transfer surface defined in the BuildingSurface:Detailed:ExteriorNaturalVentedCavity is also not allowed.
-
-When a triangular subsurface is used, the model provides a warning and treats this subsurface as rectangular. The effective width and height calculated in the ProcessSurfaceVertices function of the SurfaceGeometry module are used to represent a rectangular subsurface.
-
-Effective width = 0.75 x Length between Vertex 1 and Vertex 2
-
-Effective height = 4 x Area / ( 3 x Length between Vertex 2 and Vertex 3 )   
-
-#### Field: Surface Name
-
-This is the name of the corresponding surface (wall, roof, ceiling, floor, window, door or glass door).
-
-Information on this surface is used by the program as follows:
-
-(1)  For a linkage associated with an exterior heat transfer surface: air flow through this linkage is between the outside environment and the thermal zone to which the surface belongs.
-
-(2)  For a linkage associated with an interior (i.e., interzone) heat transfer surface: air flow through this linkage is between the thermal zones separated by the surface (i.e., the thermal zone associated with the inside face environment and the thermal zone associated with the outside face environment).
-
-(3)  This heat transfer surface determines the height of the linkage, which is used in calculating buoyancy-related flow through the linkage.
-
-**Note:** It is possible to define an interzone surface twice in EnergyPlus, once in each of the zones that the surface separates. Previously this was a requirement of EnergyPlus (prior to version 2.0), but now it is optional and the user also has the option of only defining the surface once (EnergyPlus defines the second surface automatically within the program). For each interzone surface, use only one (of possible two) interzone surface names in the AirflowNetwork:Multizone:Surface object for “Surface Name.� **Do not** enter two AirflowNetwork:Multizone:Surface objects corresponding to the two possible interzone names. This would cause the air flow through the surface to be counted twice.
-
-#### Field: Leakage Component Name
-
-The name of the AirflowNetwork:MultiZone:Surface:Crack,
- AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea,
- AirflowNetwork:MultiZone:Component:SimpleOpening,
- AirflowNetwork:MultiZone:Component:HorizontalOpening,
- AirflowNetwork:MultiZone:Component:DetailedOpening
- or AirflowNetwork:MultiZone:Component:ZoneExhaustFan object associated with this air flow linkage.
-
-If the name of an opening component (i.e. AirflowNetwork:MultiZone:Component:DetailedOpening. AirflowNetwork:MultiZone:Component:HorizontalOpening,  or AirflowNetwork:MultiZone:Component:SimpleOpening is given here, then the Surface Name in the previous field must be that of a window, door or glass door heat transfer subsurface. Otherwise an error message will be reported.
-
-If the name of an AirflowNetwork:MultiZone:Surface:Crack object or AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea object is given here, the program will position the crack at the average height of the associated heat transfer surface or subsurface. The user can define multiple heat transfer surfaces (e.g., split a wall into several surfaces) to be more precise in establishing the crack location. Similarly, the user can define multiple heat transfer surfaces if a wall, for example, has multiple cracks or openings that need to be defined individually.
-
-If the name of an AirflowNetwork:MultiZone:Component:ZoneExhaustFan is given here, then the Surface Name in the previous field must be that of an exterior heat transfer surface. The zone name defined in the Zone Name field for this heat transfer surface must be the same zone name defined in the ZoneHVAC:EquipmentConnections object (which references a ZoneHVAC:EquipmentList containing the name of the corresponding zone exhaust fan).Otherwise an error message will be reported. When this zone exhaust fan is operating for a simulation timestep, all surface-level controls described below are ignored for that timestep.
-
-
-
-#### Field: External Node Name
-
-The name of the associated AirflowNetwork:MultiZone:ExternalNode object, which determines the wind pressure coefficients for the heat transfer surface. Used only if Surface Name is for an exterior surface.
-
-If Wind Pressure Coefficient Type = SurfaceAverageCalculation in the AirflowNetwork:SimulationControl object, this field is not used and a blank may be entered. If the surface is an interior (i.e., interzone) surface, leave this field blank.
-
-#### Field: Window/Door Opening Factor, or Crack Factor
-
-If this linkage is associated with an AirflowNetwork:MultiZone:Component:DetailedOpening or AirflowNetwork:MultiZone:Component:SimpleOpening object (which means it is an openable window or door), then this field is called “Window/Door Opening Factor� and represents the value of the Opening Factor that is in effect when the Vent Temperature Schedule (defined in the AirflowNetwork:Multizone:Zone object) indicates that this window or door is open.
-
-The AirflowNetwork model uses a combination of factors to determine the actual opening area for a window or door when it is venting. For example, consider a window that is 1.5m high and 2.0m wide (excluding frame). Assume that the AirflowNetwork:MultiZone:Component:DetailedOpening for this window has Type of Large Vertical Opening = 1 (non-pivoting window), Height Factor = 0.5 and Width Factor = 0.8. Then when the window is fully open, the opening area = height of opening (0.5x1.5) times width of opening (0.8x2.0) = 0.75x1.6 = 1.2 m<sup>2</sup>. If the Window/Door Opening Factor is 0.75, then the opening area = 0.75x1.2 = 0.9 m<sup>2</sup>.
-
-If, in addition, the window is in a thermal zone for which opening modulation has been specified (ref: AirflowNetwork:Multizone:Zone) and the multiplication factor due to modulation is 0.3 in a particular timestep, then the actual opening factor that timestep = 0.3x0.75 = 0.225 and the actual opening area that timestep = 0.3x0.9 = 0.27 m<sup>2</sup>.
-
-If this linkage is associated with an AirflowNetwork:MultiZone:Surface:Crack object, the following crack air flow equation is used.
-
-<sup><span>\(Q = {\rm{(Crack Factor)*}}{C_T}{\rm{*}}{C_Q}{\left( {\Delta P} \right)^n}\)</span></sup>
-
-Where
-
-*Q*   = air mass flow (kg/s)
-
-*C<sub>Q</sub>* = air mass flow coefficient (kg/s @ 1 Pa)
-
-*C<sub>T</sub>* = reference condition temperature correction factor (dimensionless). See AirflowNetwork:MultiZone:Surface:Crack object.
-
-<span>\(\Delta P\)</span>= pressure difference across crack (Pa)
-
-*n*   = air flow exponent (dimensionless)
-
-*The following fields control venting. They are used only when Name of Associated Heat Transfer Surface is that of an openable exterior or interior window, door or glass door. They only apply to openings, and do not apply to surface cracks, effective leakage area or zone exhaust fans. If none of these fields is specified, or if Ventilation Control Mode = ZoneLevel, venting is controlled by the AirflowNetwork:Multizone:Zone object for the thermal zone containing the window or door (ref: AirflowNetwork:Multizone:Zone Data).*
-
-#### Field: Ventilation Control Mode
-
-Specifies the type of surface-level natural ventilation control.
-
-Let T<sub>out</sub> equal the outdoor air temperature, T<sub>zone</sub> equal the previous timestep’s zone air temperature, T<sub>set</sub> equal the Vent Temperature Schedule value, H<sub>zone</sub> equal the specific enthalpy of zone air from the previous timestep, and H<sub>out</sub> equal the specific enthalpy of outdoor air. Then the four allowed choices for Ventilation Control Mode are:
-
-**NoVent**: The openable window or door associated with this surface is closed at all times independent of indoor or outdoor conditions. The Venting Availability Schedule is ignored in this case.
-
-**Temperature**: The openable window or door associated with this surface is opened if T<sub>zone</sub> &gt; T<sub>out</sub> **and** T<sub>zone</sub> &gt; T<sub>set</sub> **and** Venting Availability Schedule (see below) allows venting.
-
-**Enthalpy:** The openable window or door associated with this surface is opened if H<sub>zone</sub> &gt; H<sub>out</sub> **and** T<sub>zone</sub> &gt; T<sub>set</sub> **and** Venting Availability Schedule allows venting.
-
-**Constant**: Whenever this object’s Venting Availability Schedule allows venting, the openable window or door associated with this surface is open, independent of indoor or outdoor conditions. Note that “Constant� here means that the size of this opening is fixed while venting; the air flow through this opening can, of course, vary from timestep to timestep.
-
-**ASHRAE55Adaptive**: The openable window or door associated with this surface is opened if the operative temperature is greater than the comfort temperature (central line) calculated from the ASHRAE Standard 55-2010 adaptive comfort model **and** Venting Availability Schedule allows venting.
-
-**CEN15251Adaptive:** The openable window or door associated with this surface is opened if the operative temperature is greater than the comfort temperature (central line) calculated from the CEN15251 adaptive comfort model **and** Venting Availability Schedule allows venting.
-
-**ZoneLevel**: Venting of the window or door is not controlled individually, but is controlled instead at the zone level. This means that the venting is determined by the AirflowNetwork:Multizone:Zone object for the thermal zone containing the window or door (ref: AirflowNetwork:Multizone:Zone object). This is the default value for this field.
-
-**AdjacentTemperature**: This choice is used for an interior surface only. The openable interior window or door associated with this surface is opened if T<sub>zone</sub> &gt; T<sub>adjacent\\ zone</sub> **and** T<sub>zone</sub> &gt; T<sub>set</sub> **and** Venting Availability Schedule (see below) allows venting, where T<sub>adjacent\\ zone</sub>is the adjacent zone temperature.
-
-**AdjacentEnthalpy:** This choice is also used for an interior surface only. The interior openable window or door associated with this surface is opened if H<sub>zone</sub> &gt; H<sub>adjacent\\ zone</sub> **and** T<sub>zone</sub> &gt; T<sub>set</sub> **and** Venting Availability Schedule allows venting, where H<sub>adjacent\\ zone</sub>is the adjacent zone specific enthalpy.
-
-#### Field: Ventilation Control Zone Temperature Setpoint Schedule Name
-
-The name of a schedule of zone air temperature set points that controls the opening of a window or door associated with this surface to provide natural ventilation. This setpoint is the temperature above which this openable window or door will be opened if the conditions described in the previous field Ventilation Control Mode are met.
-
-The Ventilation Control Zone Temperature Setpoint Schedule applies only to a window or door attached to this surface that is specified using AirflowNetwork:MultiZone:Component:DetailedOpening or AirflowNetwork:MultiZone:Component:SimpleOpening.
-
-(The discussion under the field Window/Door Opening Factor in this object describes how the actual opening area of a window or door in a particular timestep is determined.)
-
-*Modulation of Openings*
-
-The following five fields can be used to modulate this window/door opening when Ventilation Control Mode = Temperature or Enthalpy. These fields determine a factor between 0 and 1 that multiplies the opening factor of this window or door according to the control action shown in Figure 96 for Ventilation Control Mode = Temperature and in Figure 97 for Ventilation Control Mode = Enthalpy. Modulation of this opening can reduce the large temperature swings that can occur if the window/door is open too far when it is venting, especially when there is a large inside-outside temperature difference.
-
-The modulation takes the following form when Ventilation Control Mode = Temperature:
-
-**if** T<sub>zone</sub> - T<sub>out</sub> &lt;= [Lower Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor]  **then**  Multiplication factor = 1.0
-
-**if** [Lower Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor] &lt; T<sub>zone</sub> - T<sub>out</sub> &lt; [Upper Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor]  **then**  Multiplication factor varies linearly from 1.0 to [Limit Value on Multiplier for Modulating Venting Open Factor]
-
-**if** T<sub>zone</sub> - T<sub>out</sub> &gt;=  [Upper Value on Inside/Outside Temperature Difference for Modulating the Venting Open Factor]  **then**  Multiplication factor = [Limit Value on Multiplier for Modulating Venting Open Factor]
-
-One way of “tuning� the following modulation control parameters is to perform a sensitivity analysis for winter and/or summer design days to determine what combination of values causes the biggest reduction in zone air temperature fluctuations due to venting.
-
-Note that the default values for the following fields are such that, if none of the fields are specified, modulation will not occur.
-
-#### Field: Minimum Venting Open Factor
-
-See Figure 96 or Figure 97. This field applies only if Ventilation Control Mode = Temperature or Enthalpy. This value may be from zero to 1.0, with the default being 0.0.
-
-#### Field: Indoor and Outdoor Temperature Difference Lower Limit For Maximum Venting Open Factor
-
-See Figure 96. This field applies only if Ventilation Control Mode = Temperature. This value may be from zero to less than 100°C, with the default being 0°C. The value for this field must be less than the value specified for the following field.
-
-#### Field: Indoor and Outdoor Temperature Difference Upper Limit for Minimun Venting Open Factor
-
-See Figure 96. This field applies only if Ventilation Control Mode = Temperature. This value must be greater than 0°C, with the default being 100°C. The value for this field must be greater than the value specified for the previous field.
-
-#### Field: Indoor and Outdoor Enthalpy Difference Lower Limit For Maximum Venting Open Factor
-
-See Figure 97. This field applies only if Ventilation Control Mode = Enthalpy. This value may be from zero to less than 300,000 J/kg, with the default being 0 J/kg. The value for this field must be less than the value specified for the following field.
-
-#### Field: Indoor and Outdoor Enthalpy Difference Upper Limit for Minimun Venting Open Factor
-
-See Figure 97. This field applies only if Ventilation Control Mode = Enthalpy. This value must be greater than zero, with the default being 300,000 J/kg. The value for this field must be greater than the value specified for the previous field.
-
-#### Field: Venting Availability Schedule Name
-
-The name of a schedule that specifies when venting is available. A zero or negative schedule value means venting is not allowed. A value greater than zero means venting can occur if other venting control conditions (specified by Ventilation Control Mode and Vent Temperature Schedule Name) are satisfied. This schedule name should not be confused with Vent Temperature Schedule Name.
-
-If a Venting Availability Schedule Name is not specified, it is assumed that venting is always available.
-
-Using Venting Availability Schedule allows you to turn off venting at certain times of the day (at night, for example), week (on weekends, for example), or year (during the winter, for example).
-
-If used with Ventilation Control Mode = Constant, the ventilation rate is constant only when this schedule allows venting; otherwise the ventilation rate is set to zero.
-
-If Ventilation Control Mode = NoVent, this schedule has no effect.
-
-**Note:** In order to establish an airflow network, each AirflowNetwork:Multizone:Zone object must have at least two surfaces defined with AirflowNetwork:Multizone:Surface objects, so that air can flow from one zone into other zones (or to outdoors) through the network (air mass flow conserved). In addition, for all AirflowNetwork:Multizone:Surface objects facing the same Zone Name (ref. BuildingSurface:Detailed), at least two different environments must be defined for the other side of these surfaces (e.g., an external node and an adjacent zone, two adjacent zones, or two external nodes).
-
-#### Field: Occupant Ventilation Control Name
-The name of an AirlowNetwork:OccupantVentilationControl object. The object is used to perform advanced window opening control based on occupant conditions. When an object name is given, advanced window opening control is performed and, the Ventilation Control defined in the Ventilation Control Mode field will be overridden.
-
-
-IDF examples are provided below:
-
-
-
-```idf
-AirflowNetwork:MultiZone:Surface,
-    Zn001:Wall001,           !- Name of Associated Heat Transfer Surface
-    CR-1,                    !- Leakage Component Name
-    SFacade,                 !- External Node Name
-    1.0;                     !- Window/Door Opening Factor, or Crack Factor {dimensionless}
-
-AirflowNetwork:MultiZone:Surface,
-    Zn001:Wall001:Win001,    !- Name of Associated Heat Transfer Surface
-    WiOpen1,                 !- Leakage Component Name
-    SFacade,                 !- External Node Name
-    0.5;                     !- Window/Door Opening Factor, or Crack Factor {dimensionless}
-
-AirflowNetwork:MultiZone:Surface,
-    Zn003:Wall003,           !- Name of Associated Heat Transfer Surface
-    Zone3 Exhaust Fan,       !- Leakage Component Name
-    EFacade,                 !- External Node Name
-    1.0;                     !- Window/Door Opening Factor, or Crack Factor {dimensionless}
-
-AirflowNetwork:MultiZone:Surface,
-    Zn001:Wall001:Win002,    !- Name of Associated Heat Transfer Surface
-    WiOpen2,                 !- Leakage Component Name
-    WFacade,                 !- External Node Name
-0.5;                     !- Window/Door Opening Factor, or Crack Factor {dimensionless}
-    Temperature,             !- Ventilation Control Mode
-    WindowVentSched,         !- Vent Temperature Schedule Name
-    0.3,                     !- Limit Value on Multiplier for Modulating Venting Open Factor
-                             !- {dimensionless}
-    5.0,                     !- Lower Value on Inside/Outside Temperature Difference for
-                             !- Modulating the Venting Open Factor {deltaC}
-    10.0,                    !- Upper Value on Inside/Outside Temperature Difference for
-                             !- Modulating the Venting Open Factor {deltaC}
-    0.0,                     !- Lower Value on Inside/Outside Enthalpy Difference for Modulating
-                             !- the Venting Open Factor {J/kg}
-    300000.0,                !- Upper Value on Inside/Outside Enthalpy Difference for Modulating
-                             !- the Venting Open Factor {J/kg}
-    VentingSched;            !- Venting Availability Schedule Name
-```
-
-
-
-### AirflowNetwork:MultiZone:ReferenceCrackConditions
-
-This object specifies the reference conditions for temperature, humidity, and pressure which correspond to the AirflowNetwork:MultiZone:Surface:Crack object.
-
-#### Field: Name
-
-The name of this Reference Crack Conditons object. This name is referenced by an AirflowNetwork:MultiZone:Surface:Crack object.
-
-#### Field: Reference Temperature
-
-The reference temperature in °C under which the Surface Crack Data were obtained. The default value is 20°C.
-
-#### Field: Reference Barometric Pressure
-
-The reference barometric pressure in Pa under which the Surface Crack Data were obtained. The default value is 101325 Pa.
-
-#### Field: Reference Humidity Ratio
-
-The reference humidity ratio in kgWater/kgDryAir under which the Surface Crack Data were obtained. The default value is 0 kgWater/kgDryAir.
-
-An IDF example is provided below:
-
-```idf
-AirflowNetwork:MultiZone:ReferenceCrackConditions,
-    ReferenceCrackConditions,      !- Name of Reference Crack Conditions
-    20.0,                          !- Reference Temperature for Crack Data {C}
-    101325,                        !- Reference Barometric Pressure for Crack Data {Pa}
-    0.0;                           !- Reference Humidity Ratio for Crack Data {kgWater/kgDryAir}
-```
-
-### AirflowNetwork:MultiZone:Surface:Crack
-
-This object specifies the properties of air flow through a crack and the associated measurement conditions. The following power law form is used that gives air flow through the crack as a function of the pressure difference across the crack:
-
-<sup><span>\(Q = {\rm{(Crack Factor)*}}{C_T}{\rm{*}}{C_Q}{\left( {\Delta P} \right)^n}\)</span></sup>
-
-Where
-
-*Q*   = air mass flow (kg/s)
-
-*C<sub>Q</sub>* = air mass flow coefficient (kg/s-Pa<sup>n</sup> @ 1 Pa)
-
-*C<sub>T</sub>* = reference condition temperature correction factor (dimensionless)
-
-<span>\(\Delta P\)</span>= pressure difference across crack (Pa)
-
-*n*   = air flow exponent (dimensionless)
-
-<div>\[{C_T} = {\left[ {\frac{{{\rho_o}}}{\rho }} \right]^{n - 1}}{\left[ {\frac{{{\nu_o}}}{\nu }} \right]^{2n - 1}}\]</div>
-
-where
-
-� = Air density at the specific air temperature and humidity ratio conditions [kg/m<sup>3</sup>]
-
-ν = Air kinetic viscosity at the specific air temperature condition [m<sup>2</sup>/s]
-
-�<sub>o</sub> = Air density at the reference air conditions provided by the object AirflowNetwork:MultiZone:ReferenceCrackConditions specified in the field Reference Crack Conditions [kg/m<sup>3</sup>]
-
-ν<sub>o</sub> = Air kinetic viscosity at the reference air temperature provided by the object AirflowNetwork:MultiZone:ReferenceCrackConditions specified in the field Reference Crack Conditions [m<sup>2</sup>/s]
-
-Note: The correction factor shown above is use for this particular component as specified.
-
-#### Field: Name
-
-This is a name for this AirflowNetwork:MultiZone:Surface:Crack object. It is referenced by an AirflowNetwork:Multizone:Surface object.
-
-#### Field: Air Mass Flow Coefficient at Reference Conditions
-
-The value of the air mass flow coefficient,<span>\({C_Q}\)</span>, in the crack air flow equation. It has units of kg/s at 1Pa. This value must be greater than zero.
-
-#### Field: Air Mass Flow Exponent
-
-The value of the exponent,* n*, in the crack air flow equation. The valid range is 0.5 to 1.0, with the default value being 0.65.
-
-#### Field: Reference Crack Conditions
-
-The name of the AirflowNetwork:MultiZone:ReferenceCrackConditions object which specifies the conditions under which the air mass flow coefficient was measured. If the user omits this field and only one AirflowNetwork:MultiZone:ReferenceCrackConditions object is defined in the input data file, then those reference crack conditions will be used. If the user omits this field and either zero or more than one AirflowNetwork:MultiZone:ReferenceCrackConditions objects are defined in the input data file, then the default conditions for the AirflowNetwork:Multizone: Reference Crack Conditions object will be used.
-
-An IDF example is shown below:
-
-```idf
-AirflowNetwork:MultiZone:Surface:Crack,
-    CR-1,                     !- Name of Surface Crack Component
-    0.01,                     !- Air Mass Flow Coefficient at Reference Conditions {kg/s}
-    0.667,                    !- Air Mass Flow Exponent {dimensionless}
-    ReferenceCrackConditions; !- Reference Crack Conditions
-```
-
-### AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea
-
-The effective leakage area (ELA) object is used to define surface air leakage. It has
-
-five fields. The relationship between pressure and airflow may be expressed as:
-
-<div>\[\dot m = ELA*{C_d}\sqrt {2\rho } *{\left( {\Delta {P_r}} \right)^{0.5 - n}}{\left( {\Delta P} \right)^n}\]</div>
-
-where
-
-<span>\(\dot m\)</span>     = Air mass flow rate [kg/s]
-
-*ELA*   = Effective leakage area [m<sup>2</sup>]
-
-�       = Air density [kg/m<sup>3</sup>]
-
-<span>\(\Delta {P_r}\)</span>  = Reference pressure difference [Pa]
-
-<span>\(\Delta P\)</span>   = Pressure difference across this component [Pa]
-
-C<sub>d           </sub> = Discharge coefficient [dimensionless]
-
--       = Air mass flow exponent [dimensionless]
-
-#### Field: Name
-
-This is a name for this AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea object. It is referenced by an AirflowNetwork:Multizone:Surface object.
-
-#### Field: Effective Leakage Area
-
-This numeric field is used to input the effective leakage area  in square meters. The effective leakage area is used to characterize openings for infiltration calculations (ASHRAE Handbook of Fundamentals, 1997, pp 25.18). This value must be greater than zero.
-
-#### Field: Discharge Coefficient
-
-This numeric field is used to input the discharge coefficient. This value must be greater than zero, with a default value of 1.0.
-
-#### Field: Reference Pressure Difference
-
-This numeric field is used to input the reference pressure difference [Pa]. This value must be greater than zero, with a default value of 4.0 Pa.
-
-#### Field: Air Mass Flow Exponent
-
-This numeric field is used to input the pressure difference exponent. The valid range of the exponent is from 0.5 to 1.0, with a default value of 0.65.
-
-Note: There are two common sets of reference conditions: C<sub>d</sub> = 1.0 and DP = 4 Pa, or C<sub>d</sub> = 0.6 and DP = 10 Pa
-
-An IDF example is shown below:
-
-```idf
-AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea,
-    SurfaceELR,              !- Name of surface effective leakage area component
-    0.07,                    !- Effective leakage area {dimensionless}
-    1.00,                    !- Discharge coefficient {dimensionless}
-    4.0,                     !- Reference pressure difference {Pa}
-    0.65;                    !- Air mass flow exponent {dimensionless}
-```
-
-### AirflowNetwork:MultiZone:Component:DetailedOpening
-
-This object specifies the properties of air flow through windows and doors (window, door and glass door heat transfer subsurfaces) when they are closed or open. The fields are similar to those for AirflowNetwork:Multizone:SurfaceCrack object when the window or door is closed, but additional fields are required to describe the air flow characteristics when the window or door is open. These additional fields include opening type, opening dimensions, degree of opening, and opening schedule.
-
-The AirflowNetwork model assumes that open windows or doors are vertical or close to vertical; for this reason they are called “Large Vertical Openings.� Such openings can have air flow moving simultaneously in two different directions depending on stack effects and wind conditions (for example, flow from inside to outside at the top of a window and from outside to inside at the bottom). AirflowNetwork models such two-directional flow, but only for vertical openings.
-
-It is assumed that the air flow through a window opening is unaffected by the presence of a shading device such as a shade or blind on the window. Also, the calculation of conductive heat transfer and solar gain through a window or door assumes that the window or door is closed.
-
-The AirflowNetwork model does not have a model for bi-directional flow through large horizontal openings. For this reason, **AirflowNetwork:MultiZone:Component:DetailedOpening should not be used for horizontal openings**. The best modeling technique in this case is to put an AirflowNetwork:MultiZone:Surface:Crack object in a horizontal surface and use a large air mass flow coefficient. Crack flow is assumed to be uni-directional in any given timestep (but can reverse flow direction from timestep to timestep).
-
-A subsurface multiplier may be used to represent multiple subsurfaces and calculates total air flow when the subsurface (window, glassdoor, or door) is either closed or open. The total airflow across the surface is equal to the airflow based on the surface geometry multiplied by the subsurface multiplier.
-
-#### Field: Name
-
-The name of this AirflowNetwork:MultiZone:Component:DetailedOpening object. It is referenced by an AirflowNetwork:Multizone:Surface object.
-
-#### Field: Air Mass Flow Coefficient When Opening is Closed
-
-Crack flow is assumed when the window or door is closed. The units for this air mass flow coefficient (<span>\({C_{Q,\;unit\;length}}\)</span>) are different from the units for <span>\({C_Q}\)</span>(kg/s at 1 Pa pressure difference) defined in an AirflowNetwork:MultiZone:Surface:Crack object. There is no default but the entered value must be greater than zero. The program will automatically generate four cracks around the perimeter of the window or door--one along the bottom, one along the top, and one on each side. The temperature correction factor used in the AirflowNetwork:MultiZone:Surface:Crack object is not used for this component to calculate air mass flow rate.
-
-#### Field: Air Mass Flow Exponent When Opening Is Closed
-
-Crack flow is assumed when the window or door is closed. In this case, the value of this field is the exponent,* n*, in the crack air flow equation. The valid range for this exponent is 0.5 to 1.0, with the default value being 0.65. Mass Flow Rate = Air Mass Flow Coefficient * (deltaP)^Air Mass Flow Exponent.
-
-#### Field: Type of Rectanguler Large Vertical Opening (LVO)
-
-This alpha field specifies the type of rectangular window or door. (Open windows or doors are also called Large Vertical Openings (LVOs). The choices for the opening type are **NonPivoted** (LVO Type 1) and **HorizontallyPivoted** (LVO Type 2) with the default being **NonPivoted**. The NonPivoted type represents a regular window or door. The HorizontallyPivoted type represents a window with a horizontal axis ((i.e., a horizontally-pivoting window) and cannot be used for a door.
-
-#### Field: Extra Crack Length or Height of Pivoting Axis
-
-Specifies window or door characteristics that depend on the LVO type.
-
-For LVO Type 1 (rectangular non-pivoted windows and doors) this field is the extra crack length in meters due to multiple openable parts, if present. “Extra� here means in addition to the length, calculated by the program, of the cracks on the top, bottom and sides of the window/door.
-
-For LVO Type 2 (rectangular horizontally-pivoted windows) this field gives the height of the pivoting axis measured from the bottom of the glazed part of the window (m).
-
-#### Field: Number of Sets of Opening Factor Data
-
-This is the number of the following sets of data for opening factor, discharge coefficient, width factor, height factor, and start height factor. From two to four of these sets must be defined. The first set should be for Opening Factor = 0.0 and the last set should be for Opening Factor = 1.0. For example, if only two sets are defined, the first set should be for Opening Factor = 0.0 and the second set should be for Opening Factor = 1.0, as shown below in the IDF example below.
-
-An “opening factor� refers to the amount that a window or door is opened. The program linearly interpolates each timestep between the values of discharge coefficient, width factor, etc., in these sets using the opening factor for the window or door for the timestep. (See discussion under the field Window/Door Opening Factor in the AirflowNetwork:Multizone:Zone object for a description of how the AirflowNetwork model determines the time-step value of the opening factor.)
-
-#### Field Group: Opening Factor, Discharge Coefficient, Width Factor, Height Factor, Start Height Factor
-
-Each field is described for as many groups as required in the previous field (number of sets of opening factor data). As the final field has specific requirements, this field (n) will be described.
-
-#### Field: Opening Factor 11
-
-The first opening factor of a window or door. This value must be 0.0. The default value is also 0.0.
-
-For LVO Type 1 (rectangular non-pivoted window or door), the Opening Factor corresponds to the fraction of window or door that is opened.
-
-For LVO Type 2 (rectangular horizontally-pivoted windows), the Opening Factor is determined by the window opening angle. For example, an opening angle of 45° corresponds to an Opening Factor of 0.50 since the maximum opening angle is 90°.
-
-#### Field: Discharge Coefficient for Opening Factor 1
-
-The discharge coefficient of the window or door for Opening Factor 1. The range is greater than 0.0 to less than or equal to 1.0. The default value is 0.001. The Discharge Coefficient indicates the fractional effectiveness for air flow through a window or door at that Opening Factor.
-
-**Note:** In the following, “window width� and “window height� are glazing dimensions; they do not include the frame, if present.
-
-#### Field: Width Factor for Opening Factor 1
-
-The Width Factor of the rectangular window or door for Opening Factor 1. The Width Factor is the opening width divided by the window or door width (see Figure 98). The range is 0.0 to 1.0. The default value is 0.0. Note that the width factor applies to rectangular windows or doors where the width is assumed constant along the entire height of the opening.
-
-#### Field: Height Factor for Opening Factor 1
-
-The Height Factor of the rectangular window or door for Opening Factor 1. The Height Factor is the opening height divided by the window or door height (see Figure 98). The range is 0.0 to 1.0. The default value is 0.0. Note that the height factor applies to rectangular windows or doors where the height is assumed constant along the entire width of the opening.
-
-#### Field: Start Height Factor for Opening Factor 1
-
-The Start Height Factor of the window or door for Opening Factor 1. The Start Height Factor is the Start Height divided by the window or door height (see Figure 98). The range is 0.0 to 1.0. The default is 0. Start Height is the distance between the bottom of the window or door and the bottom of the window or door opening. The sum of the Height Factor and the Start Height Factor must be less than 1.0 in order to have the opening within the window or door dimensions.
-
-
-
-![](media/image236.svg)
-
-Figure 98. Window (or door) showing geometrical factors associated with an opening through which air flows.
-
-#### Field: Opening Factor &lt;n&gt;
-
-When Number of Sets of Opening Factor Data = n, the value of Opening Factor n must be set to 1.0.
-
-#### Field: Discharge Coefficient for Opening Factor &lt;n&gt;
-
-The discharge coefficient of the window or door for Opening Factor n. The range is greater than 0.0 to less than or equal to 1.0. The default value is 1.0.
-
-#### Field: Width Factor for Opening Factor &lt;n&gt;
-
-The Width Factor of the rectangular window or door for Opening Factor n. The Width Factor is the opening width divided by the window or door width (see Figure 98). The range is 0.0 to 1.0. The default value is 1.0.
-
-#### Field: Height Factor for Opening Factor &lt;n&gt;
-
-The Height Factor of the rectangular window or door for Opening Factor n. The Height Factor is the opening height divided by the window or door height (see Figure 98). The range is 0.0 to 1.0. The default value is 1.0.
-
-#### Field: Start Height Factor for Opening Factor &lt;n&gt;
-
-The Start Height Factor of the window or door for Opening Factor n. The Start Height Factor is the Start Height divided by the window or door height (see Figure 98). The range is 0.0 to 1.0. The default is 0.
-
-When the opening factor value (as described under the field Window/Door Opening Factor in the AirflowNetwork:Multizone:Surface object) is between two Opening Factor field values, the values of Discharge Coefficient, Width Factor, Height Factor, and Start Height Factor are linearly interpolated.
-
-An IDF example is shown below:
-
-```idf
-AirflowNetwork:MultiZone:Component:DetailedOpening,
-    WiOpen1,                 !- Detailed Opening Name
-    0.001,                   !- Air Mass Flow Coefficient When Opening is Closed {kg/s-m}
-    0.667,                   !- Air Mass Flow Exponent When Opening is Closed {dimensionless}
-    NonPivoted,             !- Type of Large Vertical Opening (LVO)
-    0.0,                     !- Extra crack length for LVO type 1 with multiple openable parts,
-                             !- or Height of pivoting axis for LVO type 2 {m}
-    2,                       !- Number of Sets of Opening Factor Data
-    0.0,                     !- Opening factor 1 {dimensionless}
-    0.5,                     !- Discharge coefficient for opening factor 1 {dimensionless}
-    0.0,                     !- Width factor for opening factor 1 {dimensionless}
-    1.0,                     !- Height factor for opening factor 1 {dimensionless}
-    0.0,                     !- Start height factor for opening factor 1 {dimensionless}
-    1.0,  0.6,  1.0,  1.0,  0.0;  !-  Set of values for opening factor 2
-```
-
-
-### AirflowNetwork:MultiZone:Component:HorizontalOpening
-
-This object specifies the properties of air flow through windows, doors and glass doors (heat transfer subsurfaces defined as a subset of FenestrationSurface:Detailed objects) when they are closed or open. This AirflowNetwork model assumes that these openings are horizontal or close to horizontal and are interzone surfaces. The second and third input fields are similar to those for AirflowNetwork:MultiZone:Surface:Crack, when the window or door is closed, but additional information is required to describe the air flow characteristics when the window or door is open. This additional information is specified in the last two input fields. The airflow across the opening consists of two types of flows: forced and buoyancy. The forced flow is caused by the pressure difference between two zones, while the buoyancy flow only occurs when the air density in the upper zone is greater than the air density in the lower zone. This opening also allows for the possibility of two-way flow when forced and buoyancy flows co-exist. This object’s openness can also be modulated based on the same opening factor control as an AirflowNetwork:MultiZone:Component:DetailedOpening object. However, the opening factor is only applied to the subsurface width. The opening width is equal to opening factor multiplied by the subsurface width.
-
-A subsurface multiplier may be used to represent multiple subsurfaces and calculates total air flow when the subsurface (window, glassdoor, or door) is either closed or open. The total airflow across the surface is equal to the airflow based on the surface geometry multiplied by the subsurface multiplier.
-
-#### Field: Name
-
-This is a name for this AirflowNetwork:MultiZone:Component:HorizontalOpening object. It is referenced by an AirflowNetwork:Multizone:Surface object.
-
-#### Field: Air Mass Flow Coefficient When Opening is Closed
-
-The value of the air mass flow coefficient, <span>\({C_{Q,\;unit\;length}}\)</span>, in the horizontal opening air flow equation. It has units of kg/s-m at 1Pa. The temperature correction factor is not applied to the mass flow calculation. This is a required input field and the entered value must be greater than zero.
-
-#### Field: Air Mass Flow Exponent When Opening is Closed
-
-The value of the exponent,* n*, in the crack air flow equation. The valid range is 0.5 to 1.0, with the default value being 0.65.
-
-#### Field: Sloping Plane Angle
-
-This numeric field is used to represent the angle between the horizontal plane and a sloped plane under the horizontal opening. Sloping plane angle = 90 is equivalent to fully open. The valid range is &gt;0 to 90, with the default value being 90.
-
-#### Field: Discharge Coefficient
-
-This numeric field is used to input the discharge coefficient. This is a required field and the entered value must be greater than zero.
-
-An IDF example is shown below:
-
-```idf
-AirflowNetwork:MultiZone:Component:HorizontalOpening,
-    HrOpen,                  !- Name
-    0.001,                   !- Air Mass Flow Coefficient When Opening is Closed {kg/s-m}
-    0.667,                   !- Air Mass Flow Exponent When Opening is Closed {dimensionless}
-    90.0,                    !- Sloping Plane Angle
-    0.2;                     !- Discharge Coefficient
-```
-
-### AirflowNetwork:MultiZone:Component:SimpleOpening
-
-This object specifies the properties of air flow through windows, doors and glass doors (heat transfer subsurfaces) when they are closed or open. The AirflowNetwork model assumes that open windows or doors are vertical or close to vertical. The second and third fields are similar to those for AirflowNetwork:MultiZone:Surface:Crack, when the window or door is closed, but additional information is required to describe the air flow characteristics when the window or door is open. This additional information is specified in the last two fields. Compared to the object AirflowNetwork:MultiZone:Component:DetailedOpening, which requires more inputs at different opening factors, this object needs comparatively less inputs. For this reason it is called a simple opening. This opening also allows for the possibility of two-way flow due to temperature and resulting density differences. Therefore, it is possible to have a positive pressure difference at the top of the opening, and a negative pressure difference at the bottom (or vice versa) when the neutral height is between the bottom and top heights of the associated surface. This object’s openness can also be modulated based on the same opening factor control as an AirflowNetwork:MultiZone:Component:DetailedOpening object. However, the opening factor is only applied to the subsurface width. The opening width is equal to opening factor multiplied by the subsurface width.
-
-A subsurface multiplier may be used to represent multiple subsurfaces and calculates total air flow when the subsurface (window, glassdoor, or door) is either closed or open. The total airflow across the surface is equal to the airflow based on the surface geometry multiplied by the subsurface multiplier.
-
-#### Field: Name
-
-This is a name for this AirflowNetwork:MultiZone:Component:SimpleOpening object. It is referenced by an AirflowNetwork:Multizone:Surface object.
-
-#### Field: Air Mass Flow Coefficient When Opening is Closed
-
-The value of the air mass flow coefficient, <span>\({C_{Q,\;unit\;length}}\)</span>, in the simple opening air flow equation. It has units of kg/s-m at 1Pa. The temperature correction factor is not applied for mass flow calculation.
-
-#### Field: Air Mass Flow Exponent When Opening is Closed
-
-The value of the exponent,* n*, in the crack air flow equation. The valid range is 0.5 to 1.0, with the default value being 0.65. Mass Flow Rate = Air Mass Flow Coefficient * (deltaP)^Air Mass Flow Exponent.
-
-#### Field: Minimum Density Difference for Two-Way Flow
-
-This numeric field is used to input the minimum density difference above which two-way or one way flow may occur due to stack effect with the window being open. Two-way flow occurs only when the neutral plane is within the opening. Density differences less than this value result in one-way flow only with the window being closed. The minimum value for this field is greater than zero.
-
-#### Field: Discharge Coefficient
-
-This numeric field is used to input the discharge coefficient. This value must be greater than zero.
-
-An IDF example is shown below:
-
-```idf
- AirflowNetwork:MultiZone:Component:SimpleOpening,
-    WiOpen2,                 !- Simple Opening Name
-    0.001,                   !- Air Mass Flow Coefficient When Opening Is Closed {kg/s-m}
-    0.650,                   !- Air Mass Flow Exponent When Opening Is Closed {dimensionless}
-    0.0001,                  !- Minimum density difference for two-way flow (kg/m3)
-    1.0;                     !- Discharge coefficient (dimensionless)
-```
-
-### AirflowNetwork:MultiZone:Component:ZoneExhaustFan
-
-This object specifies the properties of air flow through an exterior heat transfer surface with a zone exhaust fan. The zone exhaust fan turns on or off based on the availability schedule defined in the corresponding Fan:ZoneExhaust object. When the exhaust fan mass flow rate is greater than zero, the airflow network model treats this object as a constant volume fan. When the fan is off based on the availability schedule, the model treats this object as a crack.
-
-When the fan is on, the air mass flow rate modeled for the airflow network is based on the value defined in the MaximumFlow Rate field of the Fan:ZoneExhaust object. The airflow direction is from the corresponding zone to outdoors.
-
-When the fan is off, the following power law form is used that gives air flow through the crack as a function of the pressure difference across the crack:
-
-<sup><span>\(Q = {\rm{(Crack Factor)*}}{C_T}{\rm{*}}{C_Q}{\left( {\Delta P} \right)^n}\)</span></sup>
-
-Where
-
-*Q*   = air mass flow (kg/s)
-
-*C<sub>Q</sub>* = air mass flow coefficient (kg/s-Pa<sup>n</sup> @ 1 Pa)
-
-*C<sub>T</sub>* = reference condition temperature correction factor (dimensionless)
-
-<span>\(\Delta P\)</span>= pressure difference across crack (Pa)
-
-*n*   = air flow exponent (dimensionless)
-
-<div>\[{C_T} = {\left[ {\frac{{{\rho_o}}}{\rho }} \right]^{n - 1}}{\left[ {\frac{{{\nu_o}}}{\nu }} \right]^{2n - 1}}\]</div>
-
-where
-
-� = Air density at the specific air temperature and humidity ratio conditions [kg/m<sup>3</sup>]
-
-ν = Air kinetic viscosity at the specific air temperature condition [m<sup>2</sup>/s]
-
-�<sub>o</sub> = Air density at the reference air conditions provided by the object AirflowNetwork:MultiZone:ReferenceCrackConditions specified in the field Reference Crack Conditions [kg/m<sup>3</sup>]
-
-ν<sub>o</sub> = Air kinetic viscosity at the reference air temperature provided by the object AirflowNetwork:MultiZone:ReferenceCrackConditions specified in the field Reference Crack Conditions [m<sup>2</sup>/s]
-
-Note: The correction factor shown above is used when the exhaust fan is off. The airflow direction is based on the pressure difference between the zone and outdoors.
-
-#### Field: Name
-
-This is the name for this instance of the AirflowNetwork:MultiZone:Component:ZoneExhaustFan object. This name must be the same name defined in the Fan:ZoneExhaust object. It is referenced by an AirflowNetwork:Multizone:Surface object.
-
-#### Field: Air Mass Flow Coefficient When the Zone Exhaust Fan is Off at Reference Conditions
-
-The value of the air mass flow coefficient,<span>\({C_Q}\)</span>, in the crack air flow equation. It has units of kg/s at 1Pa. This value must be greater than zero. The value is used when the fan is off.
-
-#### Field: Air Mass Flow Exponent When the Zone Exhaust Fan is Off
-
-The value of the exponent,* n*, in the crack air flow equation. The valid range is 0.5 to 1.0, with the default value being 0.65. The value is used when the fan is off.
-
-#### Field: Reference Crack Conditions
-
-The name of the AirflowNetwork:MultiZone:ReferenceCrackConditions object which specifies the conditions under which the air mass flow coefficient was measured. If the user omits this field and only one AirflowNetwork:MultiZone:ReferenceCrackConditions object is defined in the input data file, then those reference crack conditions will be used. If the user omits this field and either zero or more than one AirflowNetwork:MultiZone:ReferenceCrackConditions objects are defined in the input data file, then the default conditions for the AirflowNetwork:Multizone: Reference Crack Conditions object will be used.
-
-An IDF example is shown below:
-
-```idf
-AirflowNetwork:MultiZone:Component:ZoneExhaustFan,
-   Zone3 Exhaust Fan,       !- Name
-   0.01,     !- Air Mass Flow Coefficient When the Zone Exhaust Fan is Off at Reference Conditions {kg/s}
-    0.667;    !- Air Mass Flow Exponent When the Zone Exhaust Fan is Off{dimensionless}
-    ReferenceCrackConditions; !- Reference Crack Conditions
-```
-
-### AirflowNetwork:MultiZone:ExternalNode
-
-External nodes in the AirflowNetwork model define environmental conditions outside of the building. These conditions include wind pressure coefficients that vary from façade to façade and can be highly dependent on the building geometry.
-
-AirflowNetwork:MultiZone:ExternalNode objects do **not** have to be entered if Wind Pressure Coefficient Type = SurfaceAverageCalculation in the AirflowNetwork:SimulationControl object.
-
-#### Field: Name
-
-The external node name is associated with a particular building façade. This name is referenced by the External Node Name field of an AirflowNetwork:MultiZone:WindPressureCoefficientValues object (which gives wind pressure coefficients for the façade as a function of angle of wind incident on the façade) and by the External Node Name field of an AirflowNetwork:MultiZone:Surface object.
-
-#### Field: External Node Height
-
-Designates the reference height, in meters, used to calculate relative pressure. The default value is 0 meters.
-
-#### Field: Wind Pressure Coefficient Values Object Name
-
-The name of a specific AirflowNetwork:MultiZone:WindPressureCoefficientValues object (which gives wind pressure coefficients for the façade as a function of angle of wind incident on the façade).
-
-IDF examples are provided below:
-
-
-
-```idf
-AirflowNetwork:MultiZone:ExternalNode,
-    NFacade,                 !- Name
-    1.524,                   !- External Node Height {m}
-    NFacade_WPCValue;        !- Wind Pressure Coefficient Values Object Name
-
-AirflowNetwork:MultiZone:ExternalNode,
-    EFacade,                 !- Name
-    1.524,                   !- External Node Height {m}
-    EFacade_WPCValue;        !- Wind Pressure Coefficient Values Object Name
-
-AirflowNetwork:MultiZone:ExternalNode,
-    SFacade,                 !- Name
-    1.524,                   !- External Node Height {m}
-    SFacade_WPCValue;        !- Wind Pressure Coefficient Values Object Name
-
-AirflowNetwork:MultiZone:ExternalNode,
-    WFacade,                 !- Name
-    1.524,                   !- External Node Height {m}
-    WFacade_WPCValue;        !- Wind Pressure Coefficient Values Object Name
-
-AirflowNetwork:MultiZone:ExternalNode,
-    Horizontal,              !- Name
-    3.028,                   !- External Node Height {m}
-    Horizontal_WPCValue;     !- Wind Pressure Coefficient Values Object Name
-```
-
-
-### AirflowNetwork:MultiZone:WindPressureCoefficientArray
-
-The reference height and wind directions are first specified under the AirflowNetwork:MultiZone:WindPressureCoefficientArray object. The user may specify up to 36 different wind directions in ascending order. These are then referenced by AirflowNetwork:MultiZone:WindPressureCoefficientValues objects defined for each AirflowNetwork:MultiZone:ExternalNode.
-
-The AirflowNetwork:MultiZone:WindPressureCoefficientArray object is unique and needs to be entered only if Wind Pressure Coefficient Type = INPUT in the AirflowNetwork:SimulationControl object. If Wind Pressure Coefficient Type = SurfaceAverageCalculation, this object is not required.
-
-#### Field: Name
-
-The name of this AirflowNetwork:MultiZone:WindPressureCoefficientArray object. This name is referenced by each AirflowNetwork:MultiZone:WindPressureCoefficientValues object which, for each AirflowNetwork:MultiZone:ExternalNode, gives the wind pressure coefficients at each of the wind directions listed in the AirflowNetwork:MultiZone:WindPressureCoefficientArray. This name is also referenced by the AirflowNetwork:SimulationControl object, indicating that this AirflowNetwork:MultiZone:WindPressureCoefficientArray and the pressure coefficients in the associated AirflowNetwork:MultiZone:WindPressureCoefficientValues objects will be used in the air flow simulation.
-
-#### Field: Wind Direction 1-Wind Direction N
-
-Each field references the wind direction corresponding to the first through the Nth WPC value in each of the AirflowNetwork:MultiZone:WindPressureCoefficientValues objects. *N* can be as high as 36.
-
-An IDF example is provided below:
-
-
-
-```idf
-AirflowNetwork:MultiZone:WindPressureCoefficientArray,
-    Every 30 Degrees,        !- WPC Array Name
-    0,                       !- Wind Direction #1 {deg}
-    30,                      !- Wind Direction #2 {deg}
-    60,                      !- Wind Direction #3 {deg}
-    90,                      !- Wind Direction #4 {deg}
-    120,                     !- Wind Direction #5 {deg}
-    150,                     !- Wind Direction #6 {deg}
-    180,                     !- Wind Direction #7 {deg}
-    210,                     !- Wind Direction #8 {deg}
-    240,                     !- Wind Direction #9 {deg}
-    270,                     !- Wind Direction #10 {deg}
-    300,                     !- Wind Direction #11 {deg}
-    330;                     !- Wind Direction #12 {deg}
-```
-
-
-### AirflowNetwork:MultiZone:WindPressureCoefficientValues
-
-This object specifies up to 36 wind pressure coefficients (WPCs) for an AirflowNetwork:MultiZone:ExternalNode. These coefficients are defined for each of the wind directions defined in the unique AirflowNetwork:MultiZone:WindPressureCoefficientArray object. In the air flow calculation, interpolation of the specified WPC values is done for time-step values of wind direction.
-
-AirflowNetwork:MultiZone:WindPressureCoefficientValues objects need to be entered only if the Wind Pressure Coefficient Type = INPUT in the AirflowNetwork:SimulationControl object. If Wind Pressure Coefficient Type = SurfaceAverageCalculation, this object is not required and is not used.
-
-#### Field: Name
-
-The name of this WindPressureCoefficientValues object. This name can be referenced by multiple AirflowNetwork:MultiZone:ExternalNode objects.
-
-#### Field: WindPressureCoefficientArray Name
-
-Name of the associated AirflowNetwork:MultiZone:WindPressureCoefficientArray, which lists the wind direction corresponding to each wind pressure coefficient value in this AirflowNetwork:MultiZone:WindPressureCoefficientValues object.
-
-#### Field: Wind Pressure Coefficient Value 1 to Wind Pressure Coefficient Value N
-
-The WPC (wind pressure coefficient) value for the building façade indicated by the External Node Name field above. This WPC value corresponds to the first wind direction in the AirflowNetwork:MultiZone:WindPressureCoefficientArray. Note that WPC values can be positive, negative or zero.
-
-#### Obtaining WPC values
-
-WPC values can be obtained from wind tunnel measurements, CFD calculations, or from published values for different building shapes.
-
-For **rectangular buildings** EnergyPlus will automatically calculate surface-averaged Cp values for the walls and roof of the building if you specify Wind Pressure Coefficient Type = SurfaceAverageCalculation in the AirflowNetwork:SimulationControl object. In this case you do not have to enter any AirflowNetwork:MultiZone:WindPressureCoefficientValues objects.
-
-Wind pressure coefficients are reported in the eplusout.eio either from inputs using “INPUT� as the choice for the Wind Pressure Coefficient Type field defined in the AirflowNetwork:SimulationControl object, or from internal calculation using SurfaceAverageCalculation as the choice for the Wind Pressure Coefficient Type field defined in the same object. Below is an output example from the eplusout.eio file:
-
-```
-AirflowNetwork Model:Wind Direction, 0.0,30.0,60.0,90.0,120.0,150.0,180.0,210.0,240.0,270.0,300.0,330.0
-! <AirflowNetwork Model:Wind Pressure Coefficients, WPC Name, Wind Pressure Coefficients #1 to n (dimensionless)>
-AirflowNetwork Model:Wind Pressure Coefficients, NFACADE, 0.60,0.48,4.00E-002,-0.56,-0.56,-0.42,-0.37,-0.42,-0.56,-0.56,4.00E-002,0.48
-AirflowNetwork Model:Wind Pressure Coefficients, EFACADE, -0.56,4.00E-002,0.48,0.60,0.48,4.00E-002,-0.56,-0.56,-0.42,-0.37,-0.42,-0.56
-AirflowNetwork Model:Wind Pressure Coefficients, SFACADE, -0.37,-0.42,-0.56,-0.56,4.00E-002,0.48,0.60,0.48,4.00E-002,-0.56,-0.56,-0.42
-AirflowNetwork Model:Wind Pressure Coefficients, WFACADE, -0.56,-0.56,-0.42,-0.37,-0.42,-0.56,-0.56,4.00E-002,0.48,0.60,0.48,4.00E-002
-```
-
-
-An IDF example is provided below:
-
-
-```idf
-AirflowNetwork:MultiZone:WindPressureCoefficientValues,
-    NFacade_WPCValue,        !- Name
-    Every 30 Degrees,        !- AirflowNetwork:MultiZone:WindPressureCoefficientArray Name
-    0.60,                    !- Wind Pressure Coefficient Value 1 {dimensionless}
-    0.48,                    !- Wind Pressure Coefficient Value 2 {dimensionless}
-    0.04,                    !- Wind Pressure Coefficient Value 3 {dimensionless}
-    -0.56,                   !- Wind Pressure Coefficient Value 4 {dimensionless}
-    -0.56,                   !- Wind Pressure Coefficient Value 5 {dimensionless}
-    -0.42,                   !- Wind Pressure Coefficient Value 6 {dimensionless}
-    -0.37,                   !- Wind Pressure Coefficient Value 7 {dimensionless}
-    -0.42,                   !- Wind Pressure Coefficient Value 8 {dimensionless}
-    -0.56,                   !- Wind Pressure Coefficient Value 9 {dimensionless}
-    -0.56,                   !- Wind Pressure Coefficient Value 10 {dimensionless}
-    0.04,                    !- Wind Pressure Coefficient Value 11 {dimensionless}
-    0.48;                    !- Wind Pressure Coefficient Value 12 {dimensionless}
-```
-
-###AirflowNetwork:OccupantVentilationControl
-
-The AirflowNetwork:OccupantVentilationControl object provides control options with minimum opening and closing time checks and opening and closing probability values. In general, the probability values could be a constant or a specific function. Due to lack of real data, two schedules are selected to represent probability values. If real data are available, this object may be modified to adopt new data.
-
-#### Field: Name
-This is the name of the object.
-
-#### Field: Minimum Opening Time
-The field represents the minimum time that windows will remain open. If a window has been open for a time less than this value, the window will remain open.
-
-#### Field: Minimum Closing Time
-The field represents the minimum time that windows will remain closed. If a window has been closed for a time less than this value, the window will remain closed.
-
-#### Field: Thermal Comfort Low Temperature Curve Name
-This alpha field defines the name of a curve to be used for thermal comfort temperature calculation at low outdoor dry-bulb temperature. This curve is a linear or quadratic equation using outdoor dry-bulb temperatures as an independent variable. This performance curve can be used to describe the thermal comfort temperature at low outdoor dry-bulb temperature. It allows maximum two curves to describe the thermal comfort temperature in two different outdoor dry-bulb temperature regions. If a single curve is used, blanks are entered in the following two fields.
-
-#### Field: Thermal Comfort Temperature Boundary Point
-When there are two piecewise curves to represent thermal comfort temperature calculation, this field represents a boundary point of outdoor dry-bulb temperature. The low temperature curve and the high temperature curve should have the same values at the boundary point. If a single curve is used, this field may be left blank.
-
-#### Field: Thermal Comfort High Temperature Curve Name
-This alpha field defines the name of a curve to be used for thermal comfort temperature calculation at high outdoor dry-bulb temperature. This curve is a linear or quadratic equation using outdoor dry-bulb temperatures as an independent variable. This performance curve can be used to describe the thermal comfort temperature at high outdoor dry-bulb temperature. It allows maximum two curves to describe the thermal comfort temperature in two different outdoor dry-bulb temperature regions. If a single curve is used, blanks are entered in this field.
-
-#### Field: Maximum Threshold for Persons Dissatisfied PPD
-This field is used to calculate the comfort band as a function of predicted percentage of dissatisfied (PPD). The default value is 10%. The equation is based on curve fit and is valid between 0% and 35%.
-
-<div>\[\Theta = -0.0028 (100-PPD)^2 + 0.3419 (100-PPD) - 6.6275\]</div>
-
-where
-
-* <span>\(\Theta\)</span> is the comfort band (degC)
-* PPD is predicted percentage person of dissatisfied (%)
-
-#### Field: Occupancy Check
-Input is Yes or No. The default is No. If Yes, an occupancy check is performed used in the opening probability check. If No, the occupancy check is bypassed.
-
-#### Field: Opening Probability Schedule Name
-The name of a schedule of opening probability that controls the opening of windows and doors in the thermal zone to provide natural ventilation. If the probability value is greater a random number, windows are allowed to open. Otherwise, the output will be false. This control will occur when minimum time checks for both opening and closing are satisfied.
-
-#### Field: Closing Probability Schedule Name
-The name of a schedule of closing probability that controls the closing of windows and doors in the thermal zone to reduce natural ventilation. If the probability value is greater a random number, windows are allowed to be closed. Otherwise, the output will be false. This control will occur when minimum time checks for both opening and closing are satisfied.
-
-An IDF example is provided below:
-
-```idf
-AirlowNetwork:OccupantVentilationControl,
- VentilationControl,      !- Name
- 5.0,                     !- Minimum Opening Time
- 5.0,                     !- Minimum Opening Time
- ComfortLowTempCurve,     !- Thermal Comfort Low Temperature Curve Name
- 10.0,                    !- Thermal Comfort Temperature Boundary Point
- ComfortHighTempCurve,    !- Thermal Comfort High Temperature Curve Name
- 10.0,                    !- Maximum Threshold for Persons Dissatisfied PPD
- Yes,                     !- Occupancy Check
- OpeningProbabilitySch,   !- Opening Probability Schedule Name
- ClosingProbabilitySch;   !- Closing Probability Schedule Name
-```
-
-The next two objects of AirflowNetwork:Intrazone:Node and AirflowNetwork:Intrazone:Linkage are used with RoomAir:Node:AirflowNetwork objects together to simulate multiple internal airflows via multiple intrazone nodes and linkages in a thermal zone. The mixed-air assumption for zone air conditions is not always appropriate.  EnergyPlus includes several RoomAir models that can model the implications for different flow patterns on variations in temperature within the zone.  However none of them are generalized enough for different types of air flow situations and none are coupled tightly with AirflowNetwork.  A general RoomAir model based on pressure network solver will allow modeling a variety of spaces types not currently covered by existing models such as tall spaces.
-
-Recent advancements have been made to AirflowNetwork to model large horizontal openings.  This new development makes AirflowNetwork useful for not only modeling air movement between zones (and outdoors), but also within individual thermal zones.
-
-The possible combination will allow the EnergyPlus to simulate a thermal zone using a network approach by assuming internal nodes connected by user-defined patterns of temperatures and airflows.
-It should be pointed out that the new model works when the MultizoneWithoutDistribution is selected in the field of AirflowNetwork Control of the AirflowNetwork:SimulationCOntrol object. The model cannot work with other choices.
-
-### AirflowNetwork:Intrazone:Node
-
-This object allows users to input multiple nodes in a zone. A single object represent a node. If there is only one node per zone, then use the AirflowNetwork:Multizone:Zone input object. The zone node is not defined in this object.
-
-#### Field: Name
-The name identifies the node for later reference and in the output listing. Each node should have a unique name. This name can be referenced as AirflowNetworkNodeNames.
-
-#### Field: RoomAir:Node:AirflowNetwork Name
-
-The name of a RoomAir:Node:AirflowNetwork object, which is also defined in a RoomAirSettings:AirflowNetwork object (zone based).
-
-#### Field: Zone Name
-
-The name of a zone object, which is also defined in a AirflowNetwork:MultiZone:Zone object (zone based).
-
-#### Field: Node Height
-
-This field requires input of node height in meters.
-
-An IDF example is provided below:
-
- VentilationControl,      !- Name
-
-```idf
-AirflowNetwork:IntraZone:Node,
- LeftUpper,               !- Name
- LeftUpper,               !- RoomAir:Node:AirflowNetwork Name
- NORTH_ZONE,              !- Zone Name
- 4.572;                   !- Node Height {m}
-```
-
-### AirflowNetwork:Intrazone:Linkage
-
-The input object specifies a connection between two AirflowNetwork:Intrazone:Node objects and an AiflowNetwork component defined elsewhere. The object also allow users to specify a connection between an AirflowNetwork:Intrazone:Node and an adjacent zone defined in an AirflowNetwork:MultiZone:Zone object. This object provides flexibility to define a linkage either in the same zone or in two different zones.
-
-#### Field: Name
-
-The name identifies the linkage for later reference and in the output listing. Each linkage should have a unique name.
-
-#### Field: Node 1 Name
-
-The input designates a node name where airflow starts. The node name should be defined in an AirflowNetwork:Intrazone:Node object or an AirflowNetwork:MultiZone:Zone object.
-
-#### Field: Node 2 Name
-
-The input designates a node name where airflow ends. The node name should be defined in an AirflowNetwork:Intrazone:Node object or an AirflowNetwork:MultiZone:Zone object.
-
-Note: One of Node 1 and Node 2 should be defined as an AirflowNetwork:Intrazone:Node object. In other words, both nodes cannot be defined as AirflowNetwork:MultiZone:Zone object. This type of connection should be defined as an AirflowNetwork:MultiZone:Surface object.
-
-#### Field: Component Name
-
-The input designates an AirflowNetwork component name associated with the two nodes. The component name should be one of the AirflowNetwork:Multizone:Component object names. The component is used for intrazone node connection only. If the next field is specified, the input of this field could be a blank.
-
-It should be pointed out that an AirflowNetwork:Multizone:Surface object allows following five AirflowNetwork:Multizone:Component objects:
-
-- AirflowNetwork:MultiZone:Component:DetailedOpening,
-- AirflowNetwork:MultiZone:Component:SimpleOpening,
-- AirflowNetwork:MultiZone:Surface:Crack,
-- AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea,
-- AirflowNetwork:MultiZone:Component:HorizontalOpening
-
-However, an AirflowNetwork:Intrazone:Linkage object without a surface connection has connection with two intrazone nodes in the same zone and allows two AirflowNetwork:Multizone:Component objects due to lack of geometry inputs.
-
-- AirflowNetwork:MultiZone:Surface:Crack,
-- AirflowNetwork:MultiZone:Surface:EffectiveLeakageArea,
-
-
-#### Field: Connection Surface
-
-The input specifies an AirflowNetwork:Multizone:Surface object name, when the nodes defined above are not located in the same zone. The surface linkage will be connected by the above two nodes, instead of zone nodes in normal definition. In other words, the connection defined in an AirflowNetwork:Multizone:Surface is removed. Instead, this new connection replaces the the connection specified before. A warning message is issued to let users be aware of the changes. Since each AirflowNetwork:Multizone:Surface object has its own component defined in the Leakage Component Name field, the input of the Component Name field in this object will be ignored.
-
-An IDF example is provided below:
-
-```idf
-AirflowNetwork:IntraZone:Linkage,
- IntraZoneMiddleUpperLink, !- Name
- LeftUpper,               !- Node 1 Name
- CentralUpper,            !- Node 2 Name
- CR-1;                    !- Component Name
-
-AirflowNetwork:IntraZone:Linkage,
- IntraZoneLeftUpperLink,
- LeftUpper,               !- Node 1 Name
- EAST_ZONE_T,             !- Node 2 Name
- CR-1,                    !- Component Name
- Surface_11_T;            !- Surface Name
-
-```
-
-The previous sections of this AirflowNetwork model discussion describe input objects used for multizone airflow calculations. The following sections describe input objects used for air distribution system simulations. These objects work when control option “MultiZone with Distribution� or “MultiZone with Distribution Only During Fan Operation� is defined in the AirflowNetwork Control field in the AirflowNetwork:SimulationControl object.
-
-The first section presents the input object for distribution system nodes. Although thermal zones are required to perform air distribution system simulations, the thermal zones are already defined in the multizone input section (described previously), so that there is no need to repeat the inputs for thermal zones when modeling an air distribution system. The same is also true for surface air leakage. This section has only one object: AirflowNetwork:Distribution:Node.
-
-### AirflowNetwork:Distribution:Node
-
-The AirflowNetwork:Distribution:Node object is used to represent air distribution system nodes for the AirflowNetwork model. The EnergyPlus nodes defined in an AirLoopHVAC are a subset of the nodes used to simulate the distribution system using the AirflowNetwork model. For example, the inlet node of a fan and the outlet node of a coil defined in an AirLoopHVAC must be defined as nodes using the AirflowNetwork:Distribution:Node object. A set of EnergyPlus Zone Equipment nodes is also a subset of the AirflowNetwork:Distribution:Nodes. For example, zone inlet and outlet nodes must be defined as nodes using the AirflowNetwork:Distribution: Node object. In addition, although mixers and splitters are defined as objects with inlet and outlet nodes within EnergyPlus, the AirflowNetwork:Distribution:Node object treats mixers and splitters as single nodes. The node objects are referenced by AirflowNetwork:Distribution:Linkage objects.
-
-In summary, all nodes used to define an AirLoopHVAC (except splitters, mixers, and outdoor air systems which are treated as single nodes) and its connections to a thermal zone must be specified as AirflowNetwork:Distribution:Nodes. If distribution system air leaks are to be modeled, additional AirflowNetwork:Distribution:Nodes may be defined along with AirflowNetwork:Distribution:Components (e.g., leak or leak ratio) to define the air leakage characteristics.
-
-Note: Supply and return leaks are not allowed in an AirLoopHVAC. They can only be modeled in the Zone Equipment Loop (i.e., return leaks may be modeled between the zone return node and the zone mixer inlet or the zone mixer outlet and the zone equipment loop outlet; and supply leaks may be modeled between the zone equipment loop inlet and the AirLoopHVAC:ZoneSplitter inlet node or the AirLoopHVAC:ZoneSplitter outlet node and the zone supply node).
-
-#### Field: Name
-
-The name of an air distribution system node. This node name is referenced by an AirflowNetwork:Distribution:Linkage and in the output listing. Each node should have a unique name within the AirflowNetwork:Distribution:Node objects (however, the node name may be used elsewhere as regular EnergyPlus node names such as the fan inlet node or coil outlet node).
-
-#### Field:Component Name or Node Name
-
-Designates node names defined in another EnergyPlus object, so that the AirflowNetwork:Distribution:Node object is able to get input parameters and node conditions from the associated EnergyPlus node or object. The actual node name is entered here and represents a node already defined in an AirLoopHVAC or zone equipment loop. This field is left blank if the EnergyPlus Node Type field below is entered as Mixer, Splitter, Outdoor air System, or Other.
-
-#### Field: Component Object Type or Node Type
-
-This choice field distinguishes the node type for the EnergyPlus node or object name defined above. Five node types are available:
-
-- **AirLoopHVAC:ZoneMixer**: Represents an AirLoopHVAC:ZoneMixer object defined in EnergyPlus
-
-- **AirLoopHVAC:ZoneSplitter**: Represents an AirLoopHVAC:ZoneSplitter object defined in EnergyPlus
-
-- **AirLoopHVAC:OutdoorAirSystem**: Represents an AirLoopHVAC:OutdoorAirSystem object used in EnergyPlus
-
-- **OAMixerOutdoorAirStreamNode**: Represents an external node name specified as an Outdoor Air Stream Node Name in the OutdoorAir:Mixer object when the AirLoopHVAC:OutdoorAirSystem object is used.
-
-- **OutdoorAir:NodeList**: Represents an external node name defined in the OutdoorAir:NodeList object when the AirLoopHVAC:OutdoorAirSystem object and an exhaust energy recovery system (air-to-air heat exchanger) are used.
-
-- **OutdoorAir**: Represents an external node name defined in the OutdoorAir:Node object when the AirLoopHVAC:OutdoorAirSystem and an exhaust energy recovery system (air-to-air heat exchanger) are used.
-
-- **Other**: Represents a type not already defined above.
-
-Note: Both the OutdoorAir:NodeList and OutdoorAir:Node node types represent a node to outdoor air conditions. Either one of these node types can be used to represent an external node when an air-to-air heat exchanger is used to recover energy from the exhaust air stream as part of an AirLoopHVAC:OutdoorAirSystem object. Node type OAMixerOutdoorAirStreamNode does not represent an external node when an OutdoorAir:NodeList or OutdoorAir:Node object is specified. If no exhaust heat recovery system (i.e., air-to-air heat exchanger) is specified in the AirLoopHVAC:OutdoorAirSystem, the node type OAMixerOutdoorAirStreamNode represents an external node.
-
-#### Field: Node Height
-
-Designates the reference height in meters used to calculate relative pressure. The default value is 0 meters.
-
-IDF examples are provided below:
-
-```idf
-AirflowNetwork:Distribution:Node,
-    EquipmentInletNode,      !- Name
-    Zone Equipment Inlet Node,  !- Component Name or Node Name
-    Other,                   !- Component Object Type or Node Type
-    3.0;                     !- Node Height {m}
-
-
-AirflowNetwork:Distribution:Node,
-    SupplyMainNode,          !- Name
-    ,                        !- Component Name or Node Name
-    Other,                   !- Component Object Type or Node Type
-    3.0;                     !- Node Height {m}
-
-
-AirflowNetwork:Distribution:Node,
-    MainSplitterNode,        !- Name
-    ,                        !- Component Name or Node Name
-    AirLoopHVAC:ZoneSplitter,  !- Component Object Type or Node Type
-    3.0;                     !- Node Height {m}
-
-
-AirflowNetwork:Distribution:Node,
-    MainSplitterNode,        !- Name of Node
-    ,                        !- Name of Associated EnergyPlus Node or Object
-    AirLoopHVAC:ZoneSplitter,  !- EnergyPlus Object or Node Type
-    3.0;                     !- Node Height {m}
-```
-
-
-The next section describes AirflowNetwork Distribution Components, with 7 available types listed below. All required fields for each component represent a relationship between pressure difference and airflow. The components are referenced in AirflowNetwork:Distribution:Linkage objects.
-
-- AirflowNetwork:Distribution:Component:Leak
-
-- AirflowNetwork:Distribution:Component:LeakageRatio
-
-- AirflowNetwork:Distribution:Component:Duct
-
-- AirflowNetwork:Distribution:Component:ConstantVolumeFan
-
-- AirflowNetwork:Distribution:Component:Coil
-
-- AirflowNetwork:Distribution:Component:HeatExchanger
-
-- AirflowNetwork:Distribution:Component:TerminalUnit
-
-- AirflowNetwork:Distribution:Component:ConstantPressureDrop
-
-### AirflowNetwork:Distribution:Component:Leak
-
-This component may be also called a power law component and is used to represent a supply or return air leak in an air distribution system. Its relationship between pressure difference and airflow may be expressed as:
-
-<div>\[\dot m = {C_T}C{\left( {\Delta P} \right)^n}\]</div>
-
-where
-
-<span>\(\dot m\)</span> = Air mass flow rate through the component [kg/s]
-
-C = Air mass flow coefficient (kg/s at 1 Pa pressure difference)
-
-<span>\(\Delta P\)</span> = Total pressure loss across the element [Pa]
-
-n = Air mass flow exponent
-
-C<sub>T</sub> = Temperature correction factor
-
-<div>\[{C_T} = {\left[ {\frac{{{\rho_o}}}{\rho }} \right]^{n - 1}}{\left[ {\frac{{{\nu_o}}}{\nu }} \right]^{2n - 1}}\]</div>
-
-where
-
-� = Air density at the specific air temperature and humidity ratio conditions [kg/m<sup>3</sup>]
-
-ν = Air kinetic viscosity at the specific air temperature condition [m<sup>2</sup>/s]
-
-�<sub>o</sub> = Air density at air conditions of 20°C, 0 kg/kg and 101325 Pa [kg/m<sup>3</sup>]
-
-ν<sub>o</sub> = Air kinetic viscosity at an air temperature of 20°C [m<sup>2</sup>/s]
-
-Note: The correction factor shown above is use for this particular component as specified.
-
-#### Field: Name
-
-A unique name identifying a supply or return air leak in an air distribution system. This unique name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component leak.
-
-#### Field: Air Mass Flow Coefficient
-
-This numeric field is defined as the air mass flow coefficient at 1 Pa pressure difference across this component. Valid entries must be greater than zero.
-
-#### Field: Air Mass Flow Exponent
-
-This numeric field is defined as the pressure difference exponent across the component. Valid entries are from 0.5 to 1.0, with the default value being 0.65.
-
-An IDF example is provided below:
-
-
-```idf
-AirflowNetwork:Distribution:Component:Leak,
-    MainSupplyLeak,          !- Name of Supply or Return Leak
-    0.0001,                  !- Air Mass Flow Coefficient {kg/s}
-    0.65;                    !- Air Mass Flow Exponent {dimensionless}
-
-
-AirflowNetwork:Distribution:Component:Leak,
-    ZoneSupplyLeak,          !- Name of Supply or Return Leak
-    0.01,                    !- Air Mass Flow Coefficient {kg/s}
-    0.65;                    !- Air Mass Flow Exponent {dimensionless}
-```
-
-
-### AirflowNetwork:Distribution:Component:LeakageRatio
-
-The leakage ratio component is generally used to define supply and return leaks with respect to a constant fan flow. This object requires 5 inputs. The relationship between pressure and airflow may be expressed as a power law element:
-
-<div>\[\dot m = {C_{equ}}{\left( {\Delta P} \right)^n}\]</div>
-
-where
-
-r = Air density [kg/m<sup>3</sup>]
-
-<span>\(\Delta P\)</span> = Total pressure loss across the element [Pa]
-
-n = Air mass flow exponent
-
-C<sub>equ</sub> = Equivalent air mass flow coefficient
-
-<div>\[{C_{equ}}\,\,\,\,\,\, = r*{Q_r}*\rho *{\left( {\Delta {P_r}} \right)^{ - n}}\]</div>
-
-where
-
-r = Effective leakage ratio [dimensionless]
-
-Q<sub>r</sub> = Maximum airflow rate [m<sup>3</sup>/s]
-
-<span>\(\Delta {P_r}\)</span> = Reference pressure difference [Pa]
-
-n = Air mass flow exponent [dimensionless]
-
-The above calculation is valid only for a HVAC system using a constant volume supply fan: Fan:ConstantVolume or Fan:OnOff.
-
-#### Field: Name
-
-A unique name identifying a supply or return air leak (ratio with respect to the constant volume fan flow rate) in an air distribution system. This unique name will be referenced in an AirflowNetwork:Distribution:Linkage object to represent a component.
-
-#### Field: Effective Leakage Ratio
-
-This numeric field is used to input the effective leakage ratio. This value must be greater than zero and less than or equal to 1. The effective leakage ratio is used to characterize supply and return leaks with respect to the constant fan flow (supply or return air leak flow rate divided by the maximum air flow rate for the fan). When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, the ratio for a supply leak is defined as the value of supply air leak flow rate divided by the supply fan air flow rate at the current time step. The inputs of the rest of 3 fields are not used.
-
-#### Field: Maximum Flow Rate
-
-This numeric field is used to input the maximum flow rate for a constant volume fan [m<sup>3</sup>/s]. This value must be greater than 0 m<sup>3</sup>/s. When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, this input is not used, because the real supply fan flow rate at the current time step is used to calculate the amount of a supply leak.
-
-#### Field: Reference Pressure Difference
-
-This numeric field is used to input the reference pressure difference [Pa]. This value must be greater than 0 Pa. When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, this input is not used, because the real supply fan flow rate at the current time step is used to calculate the amount of a supply leak.
-
-#### Field: Air Mass Flow Exponent
-
-This numeric field is used to input the pressure difference exponent. The value of the exponent can be from 0.5 to 1.0, with the default value being 0.65. When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, this input is not used, because the real supply fan flow rate at the current time step is used to calculate the amount of a supply leak.
-
-Note: The reference pressure difference is defined as the difference between pressures of originate and terminate nodes for supply and return leaks. In general, it may require that a simulation be performed with an initial guess for reference pressure difference using design day conditions. After obtaining pressures at the leakage nodes, more realistic reference pressure differences can be entered. It should be pointed out that since pressures at the nodes vary with temperature and other conditions, the effective leakage ratio is only an estimate. In other words, the exact leakage ratio may not be available.
-
-When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, the AirflowNetwork:Distribution:Component:LeakageRatio object has to be used to define a supply leak. The other components cannot be used. In addition, the first node in a AirflowNetwork:Distribution:Linkage to define a supply leak has to be the node in the duct to originate a supply leak, and the second node has to be the node of a zone to terminate a supply leak. In other words, the supply leak has to flow from node 1 to node 2.  When this object is used to define a return leak, the first node in a AirflowNetwork:Distribution:Linkage has to be a thermal zone to originate a leak, and the second node has to be the node of a duct to terminate a leak.
-
-An IDF example is provided below:
-
-
-```idf
-AirflowNetwork:Distribution:Component:LeakageRatio,
-    Zone1SupplyLeakELA,      !- Name of Effective Leakage Ratio
-    0.043527,                !- Effective Leakage Ratio {dimensionless}
-    1.0,                     !- Maximum Flow Rate {m3/s}
-    20.0,                    !- Reference Pressure Difference {Pa}
-    0.65;                    !- Air Mass Flow Exponent {dimensionless}
-```
-
-### AirflowNetwork:Distribution:Component:Duct
-
-This object represents a duct component and requires 9 input fields, one alpha field and 8 numeric fields. The relationship between pressure and airflow across the component may be expressed as (2001 ASHRAE Handbook of Fundamentals, Chapter 34):
-
-<div>\[\dot m = \sqrt {\frac{{2\rho {A^2}\Delta P}}{{fL/D + \sum {C_d}}}} \]</div>
-
-where
-
-<span>\(\dot m\)</span> = Mass flow rate of air through the component [kg/s]
-
-r= Air density [kg/m<sup>3</sup>]
-
-A = Cross sectional area [m<sup>2</sup>]
-
-<span>\(\Delta P\)</span> = Total pressure loss across the component [Pa]
-
-L = Duct length [m]
-
-D = Hydraulic diameter [m]
-
-C<sub>d</sub> = Dynamic loss coefficient due to fitting [dimensionless]
-
-f = Friction factor
-
-The friction factor can be calculated using the nonlinear Colebrook equation (ASHRAE Handbook of Fundamentals, 1997. p. 2.9, Eq. 29b)
-
-<div>\[\frac{1}{{\sqrt f }} = 1.44 + 2*\log \left( {\frac{D}{\varepsilon }} \right) - 2*\log \left( {1 + \frac{{9.3}}{{{\mathop{\rm Re}\nolimits} *\varepsilon /D*\sqrt f }}} \right)\]</div>
-
-where
-
-e= Surface roughness [m]
-
-Re = Reynolds number = <span>\({\raise0.7ex\hbox{${\rho VD}$} \!\mathord{\left/ {\vphantom {{\rho VD} \mu }}\right.}\!\lower0.7ex\hbox{$\mu $}}\)</span>
-
-#### Field: Name
-
-A unique name for an AirflowNetwork duct component in an air distribution system. This unique name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component.
-
-#### Field: Duct Length
-
-This numeric field is used to input duct length [m]. This value must be greater than zero.
-
-#### Field: Hydraulic Diameter
-
-This numeric field is used to input hydraulic diameter, which is defined as:
-
-<div>\[{D_h} = \frac{{4A}}{P}\]</div>
-
-where
-
-D<sub>h</sub> = Hydraulic diameter [m]
-
-A = Duct cross sectional area [m<sup>2</sup>]
-
-P = Perimeter of cross section [m]
-
-#### Field: Cross Section Area
-
-This numeric field is used to input cross section area [m<sup>2</sup>]. The model assumes that this element has no area change along its length. Otherwise, effective cross sectional area is required.
-
-#### Field: Surface Roughness
-
-This numeric field is used to input surface roughness [m]. This value must be greater than zero, and the default value is 0.0009 m.
-
-#### Field: Coefficient for Local Dynamic Loss Due to fitting
-
-This numeric field is defined as a coefficient for dynamic loss [dimensionless]. It represents dynamic loss due to fittings (such as an elbow).
-
-#### Field: Overall Heat Transmittance Coefficient (U-Factor) from Air to Air
-
-This numeric field is defined as the overall heat transmittance coefficient (U value, W/m<sup>2</sup>-K) from air to air, including film coefficients at both surfaces.
-
-#### Field: Overall Moisture Transmittance Coefficient from Air to Air
-
-This numeric field is defined as the overall moisture transmittance coefficient (kg/m<sup>2</sup>) from air to air, including film coefficients at both surfaces.
-
-An IDF example is provided below:
-
-```idf
-AirflowNetwork:Distribution:Component:Duct,
-    MainTruck1,              !- Name of Duct Component
-    3.0,                     !- Duct Length {m}
-    0.6,                     !- Hydraulic Diameter {m}
-    0.2827,                  !- Cross Section Area {m2}
-    0.0009,                  !- Surface Roughness {m}
-    0.01,                    !- Coefficient for local dynamic loss due to fitting {dimensionless}
-    0.772,                   !- Overall heat transmittance coefficient (U value) from air to air
-                             !- {W/m2-K}
-    0.0001;                  !- Overall moisture transmittance coefficient from air to air {kg/m2}
-```
-
-
-### AirflowNetwork:Distribution:Component:Fan
-
-This component represents a constant volume fan in the air distribution system (AirLoopHVAC). The air flow rate and air conditions (temperature and humidity) are obtained from the associated Fan:ConstantVolume, Fan:OnOff, or Fan:VariableVolume object.
-
-#### Field: Fan Name
-
-The name identifying an AirflowNetwork constant volume fan in an air distribution system. This name must be the same as the name of the associated Fan:ConstantVolume,  Fan:OnOff or Fan:VariableVolume object. This name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component.
-
-#### Field: Supply Fan Object Type
-
-This choice field defines the type of fan. The only valid choices are Fan:OnOff,  Fan:ConstantVolume, and Fan:VariableVolume, with the default being Fan:ConstantVolume. Both cycling and continuous fan operating modes are allowed for Fan:OnOff. Only the continuous fan operating mode is allowed for Fan:ConstantVolume. The variable airflow rate is allowed for Fan:VariableVolume.
-
-Note: Make sure that the volumetric air flow rates for the fan, coils, and parent components (e.g., unitary system or furnace) are the same so that fan energy and air distribution system losses/gains are properly calculated.
-
-
-
-An IDF example is provided below:
-
-```idf
-AirflowNetwork:Distribution:Component:Fan,
-    Supply Fan 1,            !- Name of Constant Volume Fan
-    Fan:ConstantVolume;  !- Supply fan type
-```
-
-
-### AirflowNetwork:Distribution:Component:Coil
-
-This component represents a cooling or heating coil. The main purpose for this object is to get calculated values (air flow and temperature/humidity conditions) from the associated coil models.
-
-#### Field: Coil Name
-
-The name identifying an AirflowNetwork cooling coil or heating coil defined in an air loop. This name must be the same name as the associated coil object. This unique name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component.
-
-#### Field: Coil Object Type
-
-This field requires input of the coil type used in the AirflowNetwork model. The available choices are:
-
-- Coil:Cooling:DX:SingleSpeed
-
-- Coil:Heating:Gas
-
-- Coil:Heating:Electric
-
-- Coil:Heating:DX:SingleSpeed
-
-- Coil:Cooling:Water
-
-- Coil:Heating:Water
-
-- Coil:Cooling:Water:DetailedGeometry
-
-- Coil:Cooling:DX:TwoStageWithHumidityControlMode
-
-- Coil:Cooling:DX:MultiSpeed
-
-- Coil:Heating:DX:MultiSpeed
-
-- Coil:Heating:Desuperheater
-
-#### Field: Air Path Length
-
-This numeric field is used to input air path length for the coil [m]. This value must be greater than 0 meters.
-
-#### Field: Air Path Hydraulic Diameter
-
-This numeric field is used to input hydraulic diameter of a coil’s air path, which is defined as:
-
-<div>\[{D_h} = \frac{{4A}}{P}\]</div>
-
-where
-
-D<sub>h</sub> = Hydraulic diameter [m]
-
-A = Duct cross section area [m<sup>2</sup>]
-
-P = Perimeter of cross section [m]
-
-For this component, the relationship between airflow and pressure is similar to the component AirflowNetwork:Distribution:Component:Duct. However, the model assumes very small surface roughness (10<sup>-4</sup>) and no local dynamic loss due to fittings for this component. Therefore, this component only requires two numerical fields. Heat and moisture exchange from surroundings is ignored.
-
-Note: Make sure that the volumetric air flow rates for the fan, coils, and parent components (e.g., unitary system or furnace) are the same so that fan energy and air distribution system losses/gains are properly calculated.
-
-An IDF example is provided below:
-
-```idf
-AirflowNetwork:Distribution:Component:Coil,
-    ACDXCoil 1,                            !- Name of Associated EnergyPlus Coil
-    Coil:Cooling:DX:SingleSpeed,           !- EnergyPlus Coil Type
-    0.1,                                   !- Air Path Length {m}
-1.00;                                  !- Air Path Hydraulic Diameter {m}
-
-
-AirflowNetwork:Distribution:Component:Coil,
-    HP Heating Coil 1,                     !- Name of Associated EnergyPlus Coil
-    Coil:Heating:DX:SingleSpeed,           !- EnergyPlus Coil Type
-    0.1,                                   !- Air Path Length {m}
-    1.00;                                  !- Air Path Hydraulic Diameter {m}
-```
-
-
-### AirflowNetwork:Distribution:Component:HeatExchanger
-
-This component represents an air-to-air heat exchanger typically used in combination with a cooling coil to enhance dehumidification or in an outside air system to recover energy from exhaust air to pretreat incoming outdoor ventilation air. The cooling coils with enhanced dehumidification are defined in the two objects CoilSystem:Cooling:DX:HeatExchangerAssisted and CoilSystem:Cooling:Water:HeatExchangerAssisted using one of three heat exchanger objects specified below. The exhaust air energy recovery system also has the same restriction using the one of three heat exchanger objects. The main purpose for this object is to obtain calculated values (air flow and temperature/humidity conditions) from the associated heat exchanger models for the airflow network calculations.
-
-#### Field: Heat Exchanger Name
-
-The name identifying an AirflowNetwork heat exchanger defined in an air loop. This name must be the same name that is used in the associated heat exchanger object. This unique name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component.
-
-#### Field: Heat Exchanger Object Type
-
-This field requires input of the heat exchanger type. The available choices are:
-
--    HeatExchanger:AirToAir:FlatPlate
-
--    HeatExchanger:AirToAir:SensibleAndLatent
-
--    HeatExchanger:Desiccant:BalancedFlow
-
-#### Field: Air Path Length
-
-This numeric field is used to input air path length for the heat exchanger coil [m]. This value must be greater than 0 meters.
-
-#### Field: Air Path Hydraulic Diameter
-
-This numeric field is used to input hydraulic diameter of a heat exchanger coil’s air path, which is defined as:
-
-<div>\[{D_h} = \frac{{4A}}{P}\]</div>
-
-where
-
-D<sub>h</sub> = Hydraulic diameter [m]
-
-A = Duct cross section area [m<sup>2</sup>]
-
-P = Perimeter of cross section [m]
-
-For this component, the relationship between airflow and pressure is similar to the component AirflowNetwork:Distribution:Component:Duct. However, the model assumes very small surface roughness (10<sup>-4</sup>) and no local dynamic loss due to fittings for this component. Therefore, this component only requires two numerical fields. Heat and moisture exchange from surroundings are ignored.
-
-Note: When a heat exchanger is used as a component of either CoilSystem:Cooling:DX:HeatExchangerAssisted or CoilSystem:Cooling:Water:HeatExchangerAssisted, the heat exchanger acts as two components in an air primary loop. For example, an air-to-air heat exchanger has a component connected to the supply air side (equivalent to a supply coil) and a component connected to exhaust air side (equivalent to an exhaust coil). The desiccant heat exchanger has a component connected to regeneration air side (equivalent to a regeneration air coil) and a component connected to process air side (equivalent to a process air coil). Therefore, each air-to-air heat exchanger used in this configuration requires two linkage objects (instead of only one linkage object as required for other AirflowNetwork components).
-
-When a heat exchanger is used in an exhaust air energy recovery system (i.e., in an AirLoopHVAC:OutdoorAirSystem object to recover waste heat from exhaust air to pretreat incoming outdoor ventilation air), the heat exchanger is treated as a single component. The AirflowNetwork model only connects the two nodes associated with the incoming outdoor ventilation air, while the two exhaust nodes are not defined as part of the AirflowNetwork model. Therefore, each heat exchanger component used in an exhaust air energy recovery system has only one linkage object, similar to AirflowNetwork coil components.
-
-An IDF example is provided below:
-
-```idf
-AirflowNetwork:Distribution:Component:HeatExchanger,
-    OA Heat Recovery 1,      !- HeatExchanger Name
-    HeatExchanger:AirToAir:SensibleAndLatent,  !- HeatExchanger Object Type
-    0.1,                     !- Air Path Length {m}
-    1.00;                    !- Air Path Hydraulic Diameter {m}
-
-
-AirflowNetwork:Distribution:Component:HeatExchanger,
-    Desiccant Heat Exchanger 1, !- HeatExchanger Name
-    HeatExchanger:Desiccant:BalancedFlow,  !- HeatExchanger Object Type
-    0.1,                     !- Air Path Length {m}
-    1.00;                    !- Air Path Hydraulic Diameter {m}
-```
-
-
-
-
-### AirflowNetwork:Distribution:Component:TerminalUnit
-
-This component represents a terminal unit for reheating the incoming supply air. The main purpose is to get calculated values from the terminal unit models.
-
-#### Field: Terminal Unit Name
-
-A name identifying an AirflowNetwork terminal unit defined in a zone equipment list. This name must be the same as the associated terminal unit object. This unique name will be referenced by an AirflowNetwork:Distribution:Linkage object to represent a component.
-
-#### Field: Terminal Unit Object Type
-
-This field requires input of the terminal unit type used in the AirflowNetwork model. The available types are AirTerminal:SingleDuct:ConstantVolume:Reheat and AirTerminal:SingleDuct:VAV:Reheat. The AirTerminal:SingleDuct:ConstantVolume:Reheat type is used when the Supply Fan Object Type in the AirflowNetwork:Distribution:Component:Fan is either Fan:ConstantVolume or Fan:OnOff. The AirTerminal:SingleDuct:VAV:Reheat type is used when the Supply Fan Object Type in the AirflowNetwork:Distribution:Component:Fan is Fan:VariableVolume only.
-
-#### Field: Air Path Length
-
-This numeric field is used to input the air path length for the terminal unit [m]. This value must be greater than 0 meters.
-
-#### Field: Air Path Hydraulic Diameter
-
-This numeric field is used to input hydraulic diameter for the terminal unit’s air path, which is defined as:
-
-<div>\[{D_h} = \frac{{4A}}{P}\]</div>
-
-where
-
-D<sub>h</sub> = Hydraulic diameter [m]
-
-A = Duct cross section area [m<sup>2</sup>]
-
-P = Perimeter of cross section [m]
-
-It should be noted that the relationship for this component between airflow and pressure is similar to the component AirflowNetwork:Distribution:Component:Duct. However, the model assumes very small surface roughness (10<sup>-4</sup>) and no local dynamic loss due to fittings for this component. Therefore, this component only requires two numerical fields. Heat and moisture exchange from surroundings is ignored.
-
-Note: The AirflowNetwork:Distribution:Component:TerminalUnit object is used to represent an AirTerminal:SingleDuct:ConstantVolume:Reheat or an AirTerminal:SingleDuct:VAV:Reheat object in an AirflowNetwork simulation. The AirflowNetwork:Distribution:Component:TerminalUnit should not be used to represent any other air terminal unit types. When the ZoneHVAC:EquipmentList object specifies an Air:Terminal:SingleDuct:Uncontrolled object, the AirflowNetwork:Distribution:Component:Duct object should be used instead.
-
-The AirTerminal:SingleDuct:VAV:Reheat object has two components: a damper and a reheat coil. When the AirTerminal:SingleDuct:VAV:Reheat type is used, two objects of AirflowNetwork:Distribution:Linkage have to be used to make two links, one of which is a link to connect two nodes for a damper, and the other is a link to connect two nodes for a reheat coil.
-
-When a VAV system is used with Supply Fan Object Type = Fan:VariableVolume in the AirflowNetwork:Distribution:Component:Fan object, the type of all terminals has to be AirTerminal:SingleDuct:VAV:Reheat. The object of Air:Terminal:SingleDuct:Uncontrolled is not allowed.
-
-An IDF example is provided below:
-
-```idf
-AirflowNetwork:Distribution:Component:TerminalUnit,
-    Reheat Zone 1,                    !- Name of Associated Energyplus Terminal Unit
-    AirTerminal:SingleDuct:ConstantVolume:Reheat,  !- EnergyPlus Terminal Unit Type
-    0.1,                              !- Air Path Length {m}
-    0.44;                             !- Air Path Hydraulic Diameter {m}
-```
-
-
-
-### AirflowNetwork:Distribution:Component:ConstantPressureDrop
-
-This component represents a constant pressure drop component. It is generally used to simulate a constant pressure drop filter. The mathematical equation may be written as:
-
-<div>\[\Delta P = const\]</div>
-
-#### Field: Name
-
-A unique name identifying an AirflowNetwork constant pressure drop component in an air distribution system. This unique name will be referenced by an AirflowNetwork: Distribution:Linkage object to represent a component.
-
-#### Field: Pressure Difference across the Component
-
-This numeric field is used to input the pressure difference across the element [Pa].
-
-Note: This object should be used with caution. Each node connected to this object cannot be a node for a mixer or splitter, a node in an AirLoopHVAC, or a node in a zone configuration loop. It is recommended that duct components be specified at both ends of this object.
-
-An IDF example is provided below:
-
-```idf
-AirflowNetwork:Distribution:Component:ConstantPressureDrop,
- SupplyCPDComp, ! Name of Constant Pressure Drop Component
- 1.0;           ! Pressure Difference Across the Component [Pa]
-```
-
-### AirflowNetwork:Distribution:Linkage
-
-The AirflowNetwork:Distribution:Linkage represents a connection between two AirflowNetwork:Distribution:Node objects and an AirflowNetwork component defined above. In addition, the relative height from node height to linkage height for each node is required.
-
-#### Field: Name
-
-The name identifies the linkage for later reference and in the output listing. Each linkage should have a unique name.
-
-#### Field: Node 1 Name
-
-Designates a node name where airflow starts. The node name should be defined in an AirflowNetwork:Distribution:Node object.
-
-#### Field: Node 2 Name
-
-Designates a node name where airflow ends. The node name should be defined in an AirflowNetwork:Distribution:Node object.
-
-#### Field: Component Name
-
-Designates an AirflowNetwork component name associated with the two nodes. The component name should be one of the AirflowNetwork:Distribution:Component… object names.
-
-#### Field: Thermal Zone Name
-
-Designates a thermal zone where the linkage is located. The information provides the ambient conditions for duct elements to calculate duct conduction losses (only used if component is AirflowNetwork:Distribution:Component:Duct).
-
-An IDF example is provided below:
-
-```idf
-AirflowNetwork:Distribution:Linkage,
-    Main Link 1,             !- Name of Linkage
-    EquipmentInletNode,      !- Node 1 Name
-    SupplyMainNode,          !- Node 2 Name
-    MainTruck1,              !- Component Name
-    Attic Zone;              !- Thermal Zone Name
-```
-
-### Airflow Network Outputs
-
-The AirflowNetwork nodes in the following output variables includes zones defined in AirflowNetwork:Multizone:Zone objects, external nodes defined in AirflowNetwork:MultiZone:ExternalNode objects, and nodes defined in AirflowNetwork:Distribution:Node objects.
-
-The AirflowNetwork linkage used in following output variables includes surfaces defined in AirflowNetwork:Multizone:Surface objects, and linkages defined in AirflowNetwork:Distribution:Linkage objects. The surface linkages represent airflows through surface cracks or openings between two zones or between a zone and outdoors. The distribution linkages represent airflows in an air distribution system.
-
-
-
-* HVAC,Average,AFN Node Temperature [C]
-
-* HVAC,Average,AFN Node Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC,Average,AFN Node Total Pressure [Pa]
-
-* HVAC,Average,AFN Node Wind Pressure [Pa]
-
-* HVAC,Average,AFN Node CO2 Concentration [ppm]
-
-* HVAC,Average,AFN Node Generic Air Contaminant Concentration [ppm]
-
-* HVAC,Average,AFN Linkage Node 1 to Node 2 Mass Flow Rate [kg/s]
-
-* HVAC,Average,AFN Linkage Node 2 to Node 1 Mass Flow Rate [kg/s]
-
-* HVAC,Average,AFN Linkage Node 1 to Node 2 Volume Flow Rate [m3/s]
-
-* HVAC,Average,AFN Linkage Node 2 to Node 1 Volume Flow Rate [m3/s]
-
-* HVAC,Average,AFN Linkage Node 1 to Node 2 Pressure Difference [Pa]
-
-* HVAC,Average,AFN Surface Venting Window or Door Opening Factor []
-
-* HVAC,Average,AFN Surface Venting Window or Door Opening Modulation Multiplier []
-
-* HVAC,Average,AFN Surface Venting Inside Setpoint Temperature [C]
-
-* HVAC,Average,AFN Surface Venting Availability Status []
-
-* HVAC,Average,AFN Zone Infiltration Sensible Heat Gain Rate [W]
-
-* HVAC,Sum,AFN Zone Infiltration Sensible Heat Gain Energy [J]
-
-* HVAC,Average,AFN Zone Mixing Sensible Heat Gain Rate [W]
-
-* HVAC,Sum,AFN Zone Mixing Sensible Heat Gain Energy [J]
-
-* HVAC,Average,AFN Zone Infiltration Sensible Heat Loss Rate [W]
-
-* HVAC,Sum,AFN Zone Infiltration Sensible Heat Loss Energy [J]
-
-* HVAC,Average,AFN Zone Mixing Sensible Heat Loss Rate [W]
-
-* HVAC,Sum,AFN Zone Mixing Sensible Heat Loss Energy [J]
-
-* HVAC,Average,AFN Zone Infiltration Latent Heat Gain Rate [W]
-
-* HVAC,Sum,AFN Zone Infiltration Latent Heat Gain Energy [J]
-
-* HVAC,Average,AFN Zone Infiltration Latent Heat Loss Rate [W]
-
-* HVAC,Sum,AFN Zone Infiltration Latent Heat Loss Energy [J]
-
-* HVAC,Average,AFN Zone Mixing Latent Heat Gain Rate [W]
-
-* HVAC,Sum,AFN Zone Mixing Latent Heat Gain Energy [J]
-
-* HVAC,Average,AFN Zone Mixing Latent Heat Loss Rate [W]
-
-* HVAC,Sum,AFN Zone Mixing Latent Heat Loss Energy [J]
-
-* HVAC,Average,AFN Zone Duct Leaked Air Sensible Heat Gain Rate [W]
-
-* HVAC,Sum,AFN Zone Duct Leaked Air Sensible Heat Gain Energy [J]
-
-* HVAC,Average,AFN Zone Duct Leaked Air Sensible Heat Loss Rate [W]
-
-* HVAC,Sum,AFN Zone Duct Leaked Air Sensible Heat Loss Energy [J]
-
-* HVAC,Average,AFN Zone Duct Leaked Air Latent Heat Gain Rate [W]
-
-* HVAC,Sum,AFN Zone Duct Leaked Air Latent Heat Gain Energy [J]
-
-* HVAC,Average,AFN Zone Duct Leaked Air Latent Heat Loss Rate [W]
-
-* HVAC,Sum,AFN Zone Duct Leaked Air Latent Heat Loss Energy [J]
-
-* HVAC,Average,AFN Zone Duct Conduction Sensible Heat Gain Rate [W]
-
-* HVAC,Sum,AFN Zone Duct Conduction Sensible Heat Gain Energy [J]
-
-* HVAC,Average,AFN Zone Duct Conduction Sensible Heat Loss Rate [W]
-
-* HVAC,Sum,AFN Zone Duct Conduction Sensible Heat Loss Energy [J]
-
-* HVAC,Average,AFN Zone Duct Diffusion Latent Heat Gain Rate [W]
-
-* HVAC,Sum,AFN Zone Duct Diffusion Latent Heat Gain Energy [J]
-
-* HVAC,Average,AFN Zone Duct Diffusion Latent Heat Loss Rate [W]
-
-* HVAC,Sum,AFN Zone Duct Diffusion Latent Heat Loss Energy [J]
-
-* HVAC,Average,AFN Distribution Sensible Heat Gain Rate [W]
-
-* HVAC,Sum,AFN Distribution Sensible Heat Gain Energy [J]
-
-* HVAC,Average,AFN Distribution Sensible Heat Loss Rate [W]
-
-* HVAC,Sum,AFN Distribution Sensible Heat Loss Energy [J]
-
-* HVAC,Average,AFN Distribution Latent Heat Gain Rate [W]
-
-* HVAC,Sum,AFN Distribution Latent Heat Gain Energy [J]
-
-* HVAC,Average,AFN Distribution Latent Heat Loss Rate [W]
-
-* HVAC,Sum,AFN Distribution Latent Heat Loss Energy [J]
-
-* HVAC,Sum,AFN Zone Infiltration Volume [m3]
-
-* HVAC,Sum,AFN Zone Infiltration Mass [kg]
-
-* HVAC,Average,AFN Zone Infiltration Air Change Rate [ach]
-
-* HVAC,Sum,AFN Zone Mixing Volume [m3]
-
-* HVAC,Sum,AFN Zone Mixing Mass [kg]
-
-
-
-**The following output variables are reported only when a Fan:OnOff object is used:**
-
-* HVAC,Average,AFN Zone Average Pressure [Pa]
-
-* HVAC,Average,AFN Zone On Cycle Pressure [Pa]
-
-* HVAC,Average,AFN Zone Off Cycle Pressure [Pa]
-
-* HVAC,Average,AFN Linkage Node 1 to 2 Average Mass Flow Rate [kg/s]
-
-* HVAC,Average,AFN Linkage Node 2 to 1 Average Mass Flow Rate [kg/s]
-
-* HVAC,Average,AFN Linkage Node 1 to 2 Average Volume Flow Rate [m3/s]
-
-* HVAC,Average,AFN Linkage Node 2 to 1 Average Volume Flow Rate [m3/s]
-
-* HVAC,Average,AFN Surface Average Pressure Difference [Pa]
-
-* HVAC,Average,AFN Surface On Cycle Pressure Difference [Pa]
-
-* HVAC,Average,AFN Surface Off Cycle Pressure Difference [Pa]
-
-
-**The following output variables are reported only when an AirflowNetwork:OccupantVentilationControl object is used:**
-
-* HVAC,Average,AFN Surface Venting Window or Door Opening Factor at Previous Time Step []
-
-* HVAC,Average,AFN Surface Opening Elapsed Time [min]
-
-* HVAC,Average,AFN Surface Closing Elapsed Time [min]
-
-* HVAC,Average,AFN Surface Opening Status at Previous Time Step []
-
-* HVAC,Average,AFN Surface Opening Status []
-
-* HVAC,Average,AFN Surface Opening Probability Status []
-
-* HVAC,Average,AFN Surface Closing Probability Status []
-
-
-**The following are reported only when an integrated model of RoomAir and AirflowNetwork is used:**
-
-* HVAC,Average, RoomAirflowNetwork Node Total Pressure [Pa]
-
-* HVAC,Average, RoomAirflowNetwork Node Temperature [C]
-
-* HVAC,Average, RoomAirflowNetwork Node Humidity Ratio [kgWater/kgDryAir]
-
-
-#### AFN Node Temperature [C]
-
-This is the AirflowNetwork node temperature output in degrees C. When a Fan:OnOff object is used and is scheduled to operate in the cycling fan operation mode, this value for AirflowNetwork:Distribution:Node objects reflects the temperature when the fan is operating (ON).
-
-#### AFN Node Humidity Ratio [kgWater/kgDryAir]
-
-This is the AirflowNetwork node humidity ratio output in kgWater/kgDryAir. When a Fan:OnOff object is used and is scheduled to operate in the cycling fan operation mode, this value for AirflowNetwork:Distribution:Node objects reflects the humidity ratio when the fan is operating (ON).
-
-#### AFN Node Total Pressure [Pa]
-
-This is the AirflowNetwork node total pressure in Pa with respect to outdoor barometric pressure. The total pressure is the sum of static pressure, dynamic pressure, and elevation impact at the node’s relative height. When a Fan:OnOff object is used and is scheduled to operate in the cycling fan operation mode, the value for AirflowNetwork:Distribution:Node objects reflects the total pressure when the fan is operating (ON). The total pressures for nodes associate with AirflowNetwork:Multizone:Zone objects are reported in different output variables (below).
-
-#### AFN Node CO2 Concentration [ ppm]
-
-This is the AirflowNetwork node carbon dioxide concentration level in parts per million (ppm). When a Fan:OnOff object is used and is scheduled to operate in the cycling fan operation mode, this value for AirflowNetwork:Distribution:Node objects reflects the carbon dioxide when the fan is operating (ON).
-
-#### AFN Node Generic Air Contaminant Concentration [ppm]
-
-This is the AirflowNetwork node generic contaminant concentration level in parts per million (ppm). When a Fan:OnOff object is used and is scheduled to operate in the cycling fan operation mode, this value for AirflowNetwork:Distribution:Node objects reflects the carbon dioxide when the fan is operating (ON).
-
-#### AFN Zone Average Pressure [Pa]
-
-This is the AirflowNetwork average zone total pressure in Pa with respect to outdoor barometric pressure. This output is only available when a Fan:OnOff object is used in the air distribution system. The average zone pressure is weighted by the system fan part-load ratio using the calculated zone pressures during the fan on and off periods for the system timestep. The system fan part-load ratio is defined as the ratio of the air distribution system mass flow rate (average for the simulation timestep) to the system design mass flow rate.
-
-Average zone pressure = (Zone pressure during on cycle \* Part-load ratio) + Zone pressure during off cycle \* (1.0 – Part-load ratio)
-
-#### AFN Zone On Cycle Pressure [Pa]
-
-This is the AirflowNetwork zone total pressure in Pa with respect to outdoor barometric pressure when the air distribution system fan is operating (ON). This output is only available when a Fan:OnOff object is used in the air distribution system. When the fan part-load ratio is equal to 0.0, this pressure value will be zero because the air distribution system is not simulated when the fan is off for the entire timestep.
-
-#### AFN Zone Off Cycle Pressure [Pa]
-
-This is the AirflowNetwork zone total pressure in Pa with respect to outdoor barometric pressure when the air distribution system fan is not operating (OFF). This output is only available when a Fan:OnOff object is used in the air distribution system. Even if the fan part-load ratio is equal to 1.0, the pressure calculated as if the fan were not operating (OFF) is reported.
-
-#### AFN Node Wind Pressure [Pa]
-
-This is the AirflowNetwork wind pressure output in Pa. The wind pressure depends on several factors, including wind speed, wind direction, the wind-pressure coefficient (Cp) values for the AirflowNetwork:MultiZone:ExternalNode associated with the heat transfer surface and the site wind conditions.
-
-When Wind Pressure Coefficient Type = “Input� in the AirflowNetwork:SimulationControl object, the output represents external node pressures driven by wind defined in an AirflowNetwork:MultiZone:ExternalNode object. When Wind Pressure Coefficient Type = “SurfaceAverageCalculation� in AirflowNetwork:SimulationControl, the program assumes five external nodes:
-
-- FACADE1         Representing north orientation
-
-- FACADE2         Representing east orientation
-
-- FACADE3         Representing south orientation
-
-- FACADE4         Representing west orientation
-
-- ROOF               Representing horizontal orientation
-
-In this case, the output represents the wind pressures for the five external nodes defined above.
-
-#### AFN Linkage Node 1 to Node 2 Mass Flow Rate [kg/s]
-
-This is the AirflowNetwork linkage mass flow rate output in kg/s in the direction from Node 1 to Node 2. It reports surface airflows through a crack or opening, and through linkages defined in an AirflowNetwork:Distribution:Linkage object. The surface linkage is divided into two types of surfaces, exterior surface and interior surface. Node 1 for an exterior surface linkage is a thermal zone and Node 2 is an external node. The value of AFN Linkage Node 1 to Node 2 Mass Flow Rate represents the flow rate from a thermal zone to outdoors. The flow direction through an interior surface crack or opening is defined from a thermal zone defined by a surface’s Zone Name (Node 1) to an adjacent thermal zone defined by a surface’s OutsideFaceEnvironment (Node 2). For an AirflowNetwork:Distribution:Linkage object, the value represents the air mass flow rate flowing from Node 1 to Node 2.
-
-It should be pointed out that in general, each linkage has one directional flow at any given time, either from Node 1 to 2 or from Node 2 to 1. However, there are three components which may have flows in both directions simultaneously: AirflowNetwork:MultiZone:Component:DetailedOpening, AirflowNetwork:MultiZone:Component:SimpleOpening, and AirflowNetwork:MultiZone:Component:HorizontalOpening.
-
-When a Fan:OnOff object is used, the air mass flow rates reported for the AirflowNetwork:Distribution:Linkage objects are the values when the fan is operating (ON). It is assumed that the air mass flow rates when the fan is off are zero for the distribution system air linkage objects. The air mass flow rates for the AirflowNetwork:Multizone:Surface object are reported in different output variables (below).
-
-#### AFN Linkage Node 2 to Node 1 Mass Flow Rate [kg/s]
-
-This is the AirflowNetwork linkage mass flow rate output in kg/s in the direction from Node 2 to Node 1. It reports airflows from surfaces through a crack or opening, and from linkages defined in an AirflowNetwork:Distribution:Linkage object. Node 1 and Node 2 for a surface or subsurface are defined in the same manner as AFN Linkage Node 1 to Node 2 Mass Flow Rate.
-
-When a Fan:OnOff object is used, the air mass flow rates reported for the AirflowNetwork:Distribution:Linkage objects are the values when the fan is operating (ON). It is assumed that the air mass flow rates when the fan is off are zero for the distribution system air linkage objects. The air mass flow rates for the AirflowNetwork:Multizone:Surface object are reported in different output variables (below).
-
-#### AFN Linkage Node 1 to 2 Average Mass Flow Rate [kg/s]
-
-This is the AirflowNetwork linkage average mass flow rate in kg/s in the direction from Node 1 to Node 2 defined in the AirflowNetwork:Multizone:Surface objects. This output is only available when a Fan:OnOff object is used in the air distribution system. The average mass flow rate is weighted by the system fan part-load ratio using the calculated air mass flow rates during the fan on and off periods for the system timestep. The system fan part-load ratio is defined as the ratio of the air distribution system mass flow rate (average for the simulation timestep) to the system design mass flow rate.
-
-Average surface mass flow rate = (Surface mass flow rate during on cycle \* Part-load ratio) + Surface mass flow rate during off cycle \* (1.0 – Part-load ratio)
-
-#### AFN Linkage Node 2 to 1 Average Mass Flow Rate [kg/s]
-
-This is the AirflowNetwork linkage average mass flow rate in kg/s in the direction from Node 2 to Node 1 defined in the AirflowNetwork:Multizone:Surface objects. This output is only available when a Fan:OnOff object is used in the air distribution system. The average mass flow rate is weighted by the system fan part-load ratio using the calculated air mass flow rates during the fan on and off periods for the system timestep. The system fan part-load ratio is defined as the ratio of the air distribution system mass flow rate (average for the simulation timestep) to the system design mass flow rate.
-
-#### AFN Linkage Node 1 to Node 2 Volume Flow Rate [m<sup>3</sup>/s]
-
-This is the AirflowNetwork linkage volume flow rate output in m<sup>3</sup>/s in the direction from the Node 1 to Node 2. It is defined in the same manner as AFN Linkage Node 1 to Node 2 Mass Flow Rate.
-
-When a Fan:OnOff object is used, the air volume flow rates reported for the AirflowNetwork:Distribution:Linkage objects are the values when the fan is operating (ON). It is assumed that the air volume flow rates when the fan is off are zero for the distribution system air linkage objects. The air volume flow rates for the AirflowNetwork:Multizone:Surface object are reported in different output variables (below).
-
-#### AFN Linkage Node 2 to Node 1 Volume Flow Rate [m<sup>3</sup>/s]
-
-This is the AirflowNetwork linkage volume flow rate output in m<sup>3</sup>/s in the direction from Node 2 to Node 1. It is defined in the same manner as AFN Linkage Node 2 to Node 1 Mass Flow Rate.
-
-When a Fan:OnOff object is used, the air volume flow rates reported for the AirflowNetwork:Distribution:Linkage objects are the values when the fan is operating (ON). It is assumed that the air volume flow rates when the fan is off are zero for the distribution system air linkage objects. The air volume flow rates for the AirflowNetwork:Multizone:Surface object are reported in different output variables (below).
-
-#### AFN Linkage Node 1 to 2 Average Volume Flow Rate [m<sup>3</sup>/s]
-
-This is the AirflowNetwork linkage average volume flow rate in m<sup>3</sup>/s in the direction from Node 1 to Node 2 defined in the AirflowNetwork:Multizone:Surface objects. This output is only available when a Fan:OnOff object is used. The average volume flow rate is weighted by the system fan part-load ratio using the calculated air volume flow rates during the fan on and off periods for the system timestep.
-
-Average surface volume flow rate = (Surface volume flow rate during on cycle \* Part-load ratio) + Surface volume flow rate during off cycle \* (1.0 – Part-load ratio)
-
-#### AFN Linkage Node 2 to 1 Average Volume Flow Rate [m<sup>3</sup>/s]
-
-This is the AirflowNetwork linkage average volume flow rate in m<sup>3</sup>/s in the direction from Node 2 to Node 1 defined in the AirflowNetwork:Multizone:Surface objects. This output is only available when a Fan:OnOff object is used. The average volume flow rate is weighted by the system fan part-load ratio using the calculated air volume flow rates during the fan on and off periods for the system timestep.
-
-#### AFN Linkage Node 1 to Node 2 Pressure Difference [Pa]
-
-This is the pressure difference across a linkage in Pa. The linkage includes both objects: AirflowNetwork:Multizone:Surface and AirflowNetwork: Distribution:Linkage.
-
-When a Fan:OnOff object is used, the pressure differences reported for the AirflowNetwork:Distribution:Linkage objects are the values calculated when the fan is operating (ON). It is assumed that the pressure differences when the fan is off are zero for the distribution system air linkage objects. The pressure differences defined in the AirflowNetwork:Multizone:Surface are reported in different output variables (below).
-
-#### AFN Surface Average Pressure Difference [Pa]
-
-This is the average pressure difference across a linkage in Pa for the AirflowNetwork:Multizone:Surface objects only when a Fan:OnOff object is used. The average pressure difference is weighted by the system fan part-load ratio using the calculated pressure differences during the fan on and off periods for the system timestep. The system fan part-load ratio is defined as the ratio of the air distribution system mass flow rate (average for the simulation timestep) to the system design mass flow rate.
-
-Surface Average Pressure Difference = (Surface Average Pressure Difference during on cycle \* Part-load ratio) + Surface Average Pressure Difference during off cycle \* (1.0 - Part-load ratio)
-
-#### AFN Surface On Cycle Pressure Difference [Pa]
-
-This is the pressure difference across a linkage in Pa for the AirflowNetwork:Multizone:Surface objects only when the air distribution system fan is operating (ON). This output is only available when a Fan:OnOff object is used. When the fan part-load ratio is equal to 0.0, this pressure difference value will be zero because the air distribution system is not simulated when the fan is off for the entire timestep.
-
-#### AFN Surface Off Cycle Pressure Difference [Pa]
-
-This is the pressure difference across a linkage in Pa for the AirflowNetwork:Multizone:Surface objects only when the air distribution system fan is not operating (OFF). This output is only available when a Fan:OnOff object is used. Even if the fan part-load ratio is equal to 1.0, the pressure difference calculated as if the fan were not operating (OFF) is reported.
-
-#### AFN Surface Venting Window or Door Opening Factor []
-
-The current time-step value of the venting opening factor for a particular window or door. When the window or door is venting, this is the input value of the opening factor (see AirflowNetwork:Multizone:Surface, Window/Door Opening Factor) times the multiplier for venting modulation (see description of next output variable, “Opening Factor Multiplier for AirflowNetwork Venting Modulation�). For example, if  the input Window/Door opening factor is 0.5 and the modulation multiplier is 0.7, then the value of this output variable will be 0.5x0.7 = 0.35.
-
-#### AFN Surface Venting Window or Door Opening Modulation Multiplier  []
-
-This is the multiplier on a window or door opening factor when venting modulation is in effect. See “Modulation of Openings� under AirflowNetwork:Multizone:Zone for a description of how the multiplier is determined.
-
-When modulation is in effect the value of the multiplier is between 0.0 and 1.0. When modulation does not apply the value of the multiplier may be –1.0. When modulation applies but the surface is not venting, the value is –1.0. This is summarized in the following table. In this table, “Zone� means a thermal zone for which AirflowNetwork:Multizone:Zone has been specified. See object AirflowNetwork: Multizone:Zone for definition of “Ventilation Control Mode.�
-
-
-
-Table 25. Value of opening factor multiplier for different venting conditions.
-
-<table class="table table-striped">
-  <tr>
-    <th>Is surface in a Zone?</th>
-    <th>Ventilation Control Mode</th>
-    <th>Is surface venting?</th>
-    <th>Value of opening factor multiplier</th>
-  </tr>
-  <tr>
-    <td rowspan="6">Yes</td>
-    <td rowspan="2">Temperature</td>
-    <td>Yes</td>
-    <td>0.0 to 1.0</td>
-  </tr>
-  <tr>
-    <td>No</td>
-    <td>-1.0</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Enthalpy</td>
-    <td>Yes</td>
-    <td>0.0 to 1.0</td>
-  </tr>
-  <tr>
-    <td>No</td>
-    <td>-1.0</td>
-  </tr>
-  <tr>
-    <td>Constant</td>
-    <td>Yes</td>
-    <td>1.0</td>
-  </tr>
-  <tr>
-    <td>NoVent</td>
-    <td>No</td>
-    <td>-1.0</td>
-  </tr>
-</table>
-
-#### AFN Surface Venting Inside Setpoint Temperature [C]
-
-The time-step value of the venting setpoint temperature for the zone to which the surface belongs. This setpoint is determined from the Vent Temperature Schedule input (ref: AirflowNetwork:Multizone:Zone).
-
-#### AFN Surface Venting Availability Status [ ]
-
-A value of 1.0 means venting through the surface can occur if venting control conditions are satisfied. A value of 0.0 means venting through the surface cannot occur under any circumstances. This value is determined by the Venting Availability Schedule input (ref: AirflowNetwork:Multizone:Zone or AirflowNetwork:Multizone:Surface).
-
-#### AFN Zone Infiltration Sensible Heat Gain Rate [W]
-
-The average convective sensible heat gain rate, in Watts, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period. This value is calculated for each timestep when the outdoor dry-bulb temperature is higher than the zone temperature; otherwise, the sensible gain rate is set to 0.
-
-When a Fan:OnOff object is used, this reported value is weighted by the system run time fraction using the calculated infiltration sensible gain rate during the system on and off cycles for the reporting period:
-
-Infiltration Sensible Gain Rate = (Infiltration Sensible Gain Rate during on cycle \* Run time fraction) + Infiltration Sensible Gain Rate during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Infiltration Sensible Heat Gain Energy [J]
-
-The average convective sensible heat gain, in Joules, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period. This value is calculated for each timestep when the outdoor dry-bulb temperature is higher than the zone temperature; otherwise, the sensible gain rate is set to 0.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration sensible gain during the system on and off cycles for the reporting period:
-
-Infiltration Sensible Gain = (Infiltration Sensible Gain during on cycle \* Run time fraction) + Infiltration Sensible Gain during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Infiltration Sensible Heat Loss Rate [W]
-
-The average convective sensible heat loss rate, in Watts, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration sensible loss rate during the system on and off cycles for the reporting period:
-
-Infiltration Sensible Loss Rate = (Infiltration Sensible Loss Rate during on cycle \* Run time fraction) + Infiltration Sensible Loss Rate during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Infiltration Sensible Heat Loss Energy [J]
-
-The average convective sensible heat loss, in Joules, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration sensible loss rate during the system on and off cycles for the reporting period:
-
-Infiltration Sensible Loss = (Infiltration Sensible Loss during on cycle \* Run time fraction) + Infiltration Sensible Loss during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Infiltration Latent Heat Gain Rate [W]
-
-The average convective latent heat gain rate, in Watts, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period, when the outdoor humidity ratio is higher than the zone air humidity ratio.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration latent gain rate during the system on and off cycles for the reporting period:
-
-Infiltration Latent Gain Rate = (Infiltration Latent Gain Rate during on cycle \* Run time fraction) + Infiltration Latent Gain Rate during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Infiltration Latent Heat Gain Energy [J]
-
-The total convective latent heat gain, in Joules, to the zone air corresponding to the Zone Infiltration Volume summed over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration latent gain during the system on and off cycles for the reporting period:
-
-Infiltration Latent Gain = (Infiltration Latent Gain during on cycle \* Run time fraction) + Infiltration Latent Gain during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Infiltration Latent Heat Loss Rate [W]
-
-The average convective latent heat loss rate, in Watts, to the zone air corresponding to the Zone Infiltration Volume averaged over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration latent loss rate during the system on and off cycles for the reporting period:
-
-Infiltration Latent Loss Rate = (Infiltration Latent Gain Loss Rate during on cycle \* Run time fraction) + Infiltration Latent Loss Rate during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Infiltration Latent Heat Loss Energy [J]
-
-The total convective latent heat loss, in Joules, to the zone air corresponding to the Zone Infiltration Volume summed over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated infiltration latent loss during the system on and off cycles for the reporting period:
-
-Infiltration Latent Loss = (Infiltration Latent Gain Loss during on cycle \* Run time fraction) + Infiltration Latent Loss during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Mixing Sensible Heat Gain Rate [W]
-
-The average convective sensible heat gain rate, in Watts, to the zone air corresponding to the Zone Mixing Volume averaged over the reporting period. The mixing-volume is defined as incoming volume flow from other adjacent zones where the air temperature is higher than the temperature in this zone. For example, there are two zones (Zone 2 and Zone 3) adjacent to this zone (Zone 1). Zone 1 receives airflows from both Zone 2 and Zone 3. The air temperature is 21°C in Zone 1. The air temperatures are 20°C in Zone 2 and 22°C in Zone 3. The sensible gain rate only includes heat gain from Zone 3 with respect to Zone 1. The energy received from Zone 2 is considered as a sensible loss, instead of a gain, because the air temperature in Zone 2 is lower than in Zone 1.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing sensible gain rate during the system on and off cycles for the reporting period:
-
-Mixing Sensible Gain Rate = (Mixing Sensible Gain Rate during on cycle \* Run time fraction) + Mixing Sensible Gain Rate during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Mixing Sensible Heat Loss Rate [W]
-
-The average convective sensible heat loss rate, in Watts, to the zone air corresponding to the Zone Mixing Volume averaged over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing sensible loss rate during the on and off cycles for the reporting period:
-
-Mixing Sensible Loss Rate = (Mixing Sensible Loss Rate during on cycle \* Run time fraction) + Mixing Sensible Loss Rate during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Mixing Sensible Heat Gain Energy [J]
-
-The total convective sensible heat gain, in Joules, to the zone air corresponding to the Zone Mixing Volume summed over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing sensible gain during the on and off cycles for the reporting period:
-
-Mixing Sensible Gain = (Mixing Sensible Gain during on cycle \* Run time fraction) + Mixing Sensible Gain during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Mixing Sensible Heat Loss Energy [J]
-
-The total convective sensible heat loss, in Joules, to the zone air corresponding to the Zone Mixing Volume summed over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing sensible loss during the on and off cycles for the reporting period:
-
-Mixing Sensible Loss = (Mixing Sensible Loss during on cycle \* Run time fraction) + Mixing Sensible Loss during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Mixing Latent Heat Gain Rate [W]
-
-The average convective latent heat gain rate, in Watts, to the zone air corresponding to the Zone Mixing Volume averaged over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing latent gain rate during the on and off cycles for the reporting period:
-
-Mixing Latent Gain Rate = (Mixing Latent Gain Rate during on cycle \* Run time fraction) + Mixing Latent Gain Rate during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Mixing Latent Heat Gain Energy [J]
-
-The total convective latent heat gain, in Joules, to the zone air corresponding to the Zone Mixing Volume summed over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing latent gain during the on and off cycles for the reporting period:
-
-Mixing Latent Gain = (Mixing Latent Gain during on cycle \* Run time fraction) + Mixing Latent Gain during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Mixing Latent Heat Loss Rate [W]
-
-The average convective latent heat loss rate, in Watts, to the zone air corresponding to the Zone Mixing Volume averaged over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing latent loss rate during the on and off cycles for the reporting period:
-
-Mixing Latent Loss Rate = (Mixing Latent Loss Rate during on cycle \* Run time fraction) + Mixing Latent Loss Rate during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Mixing Latent Heat Loss Energy [J]
-
-The total convective latent heat loss, in Joules, to the zone air corresponding to the Zone Mixing Volume summed over the reporting period.
-
-When a Fan:OnOff object is used, the reported value is weighted by the system run time fraction using the calculated mixing latent loss during the on and off cycles for the reporting period:
-
-Mixing Latent Loss = (Mixing Latent Loss during on cycle \* Run time fraction) + Mixing Latent Loss during off cycle \* (1.0 – Run time fraction)
-
-#### AFN Zone Mixing CO2 Mass Flow Rate [kg/s]
-
-This is a sum of mass flow rates from adjacent zones multiplied by the corresponding zone carbon dioxide concentration level to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the mixing mass flow rate calculated during the fan on and off periods for the simulation timestep.
-
-#### AFN Zone Mixing Generic Air Contaminant Mass Flow Rate [kg/s]
-
-This is a sum of mass flow rates from adjacent zones multiplied by the corresponding zone generic contaminant concentration level to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the mixing mass flow rate calculated during the fan on and off periods for the simulation timestep.
-
-#### AFN Zone Duct Leaked Air Sensible Heat Gain Rate [W]
-
-This is the average sensible heat gain rate, in Watts, to a specific zone due to supply air leaks from the forced air distribution system. This value is averaged over the reporting period. A sensible heat gain occurs when duct air is warmer than zone air. It should be pointed out that when multiple supply air leaks are present in a single zone, the output value is the summation of all the supply air leak gains in this zone. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Leaked Air Sensible Heat Gain Energy [J]
-
-This is the total sensible heat gain, in Joules, to a specific zone due to supply air leaks summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Leaked Air Sensible Heat Loss Rate [W]
-
-This is the average sensible heat loss rate, in Watts, to a specific zone due to supply air leaks from the forced air distribution system. This value is averaged over the reporting period. A sensible heat loss occurs when duct air is cooler than zone air. It should be pointed out that when multiple supply air leaks are present in this zone, the output value is the summation of all the supply air leak losses in this zone. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Leaked Air Sensible Heat Loss Energy [J]
-
-This is the total sensible heat loss, in Joules, to a specific zone due to supply air leaks summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Leaked Air Latent Heat Gain Rate [W]
-
-This is the average latent heat gain rate, in Watts, to a specific zone due to supply air leaks from the forced air distribution system for the reported time period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Leaked Air Latent Heat Gain Energy [J]
-
-This is the total latent heat gain, in Joules, to a specific zone due to supply air leaks summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Leaked Air Latent Heat Loss Rate [W]
-
-This is the average latent heat loss rate, in Watts, to a specific zone due to supply air leaks from the forced air distribution system for the reported time period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Leaked Air Latent Heat Loss Energy [J]
-
-This is the total latent heat loss, in Joules, to a specific zone due to supply air leaks summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Conduction Sensible Heat Gain Rate [W]
-
-This is the average sensible heat gain rate, in Watts, of duct conduction to a specific zone where the ducts are located. This value is averaged over the reporting period. A sensible heat gain occurs when duct air is warmer than the zone air. It should be pointed out that when ducts are located in different zones, the total duct conduction loss should be the summation of the duct conduction losses in these zones. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Conduction Sensible Heat Gain Energy [J]
-
-This is the total sensible heat gain, in Joules, to a specific zone due to duct conduction summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Conduction Sensible Heat Loss Rate [W]
-
-This is the average sensible heat loss rate, in Watts, of duct conduction to a specific zone where the ducts are located. This value is averaged over the reporting period. A sensible heat loss occurs when duct air is cooler than the zone air. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Conduction Sensible Heat Loss Energy [J]
-
-This is the total sensible heat loss, in Joules, to a specific zone due to duct conduction summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Diffusion Latent Heat Gain Rate [W]
-
-This is the average latent heat gain rate, in Watts, of vapor diffusion through the walls of the air distribution system to a specific zone where the ducts are located. This value is averaged over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Diffusion Latent Heat Gain Energy [J]
-
-This is the total latent heat gain, in Joules, to a specific zone due to duct vapor diffusion summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Diffusion Latent Heat Loss Rate [W]
-
-This is the average latent heat loss rate, in Watts, of duct vapor diffusion to a specific zone where the ducts are located. This value is averaged over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Duct Diffusion Latent Heat Loss Energy [J]
-
-This is the total latent heat loss, in Joules, to a specific zone due to duct vapor diffusion summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Distribution Sensible Heat Gain Rate [W]
-
-This is the average total sensible heat gain rate, in Watts, in a specific zone caused by the forced air distribution system. The total sensible gain rate is the sum of duct leakage sensible gain rate and duct conduction sensible gain rate. This value is averaged over the reporting period. The multizone airflow sensible gain rate is excluded in this output variable. The output of multizone airflow sensible gain is reported in the previously-described output variables AFN Zone Infiltration Sensible Heat Gain Rate and AFN Zone Mixing Sensible Heat Gain Rate. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Distribution Sensible Heat Gain Energy [J]
-
-This is the total sensible heat gain, in Joules, in a specific zone caused by the forced air distribution system. The total sensible gain is the sum of duct leakage sensible gain and duct conduction sensible gain. This value is summed over the reporting period. The multizone airflow sensible gain is excluded in this output variable. The output of multizone airflow sensible gain is reported in the previously-described output variables AFN Zone Infiltration Sensible Heat Gain Energy and AFN Zone Mixing Sensible Heat Gain Energy. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Distribution Sensible Heat Loss Rate [W]
-
-This is the average total sensible heat loss rate, in Watts, in a specific zone caused by the forced air distribution system. The total sensible loss rate is the sum of duct leakage sensible loss rate and duct conduction sensible loss rate. This value is averaged over the reporting period. The multizone airflow sensible loss rate is excluded in this output variable. The output of multizone airflow sensible loss rate is reported in the previously-described output variables AFN Zone Infiltration Sensible Heat Loss Rate and AFN Zone Mixing Sensible Heat Loss Rate. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Distribution Sensible Heat Loss Energy [J]
-
-This is the total sensible heat loss, in Joules, in a specific zone caused by the forced air distribution system. The total sensible loss is the sum of duct leakage sensible loss and duct conduction sensible loss. This value is summed over the reporting period. The multizone airflow sensible loss is excluded in this output variable. The output of multizone airflow sensible loss is reported in the previously-described output variables AFN Zone Infiltration Sensible Heat Loss Energy and AFN Zone Mixing Sensible Heat Loss Energy. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Distribution Latent Heat Gain Rate [W]
-
-This is the average total latent heat gain rate, in Watts, in a specific zone caused by the forced air distribution system. The total latent gain rate is the sum of duct leakage latent gain rate and duct conduction latent gain rate. This value is averaged over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Distribution Latent Heat Gain Energy [J]
-
-This is the total latent heat gain, in Joules, in a specific zone caused by the forced air distribution system. The total latent gain is the sum of duct leakage latent gain and duct diffusion latent gain. This value is summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Distribution Latent Heat Loss Rate [W]
-
-This is the average total latent heat loss rate, in Watts, in a specific zone caused by the forced air distribution system. The total latent loss rate is a sum of duct leakage latent loss rate and duct diffusion latent loss rate. This value is averaged over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Distribution Latent Heat Loss Energy [J]
-
-This is the total latent heat loss, in Joules, in a specific zone caused by the forced air distribution system. The total latent loss is the sum of duct leakage latent loss and duct diffusion latent loss. This value is summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-**NOTE:** The following output variables should not be confused with similar output variables for the infiltration, mixing, and cross mixing objects (Ref. Infiltration Output, Mixing Output, or Cross Mixing Output). The output variables described below refer to infiltration, mixing, and cross-mixing when an Airflow Network Simulation is performed. The following output variables are always used to describe infiltration, mixing, and cross mixing when the AirflowNetwork Control field in the AirflowNetwork:SimulationControl object is set to “MultizoneWithoutDistribution� or “MultizoneWithDistribution�. In this case the output variables for the infiltration, mixing, and cross mixing objects will always be 0.
-
-In contrast, the following output variables are only used to describe infiltration, mixing, and cross mixing when the AirflowNetwork Control field in the AirflowNetwork:SimulationControl object is set to “MultizoneAirflowWithDistributionOnlyDuringFanOperation� and the fan is operating. When the fan is not operating, the output variables for the infiltration, mixing, and cross mixing objects are used.
-
-In the case where the AirflowNetwork Control field in the AirflowNetwork:SimulationControl object is set to “NoMultizoneOrDistribution�, the following output variables are not used and the output variables for the infiltration, mixing, and cross mixing objects are used instead.
-
-#### AFN Zone Infiltration Sensible Heat Gain Energy [J]
-
-The total convective sensible heat gain, in Joules, to the zone air corresponding to the Zone Infiltration Volume summed over the reporting period. This value is calculated for each timestep when the outdoor dry-bulb temperature is higher than the zone temperature, otherwise the sensible gain is set to 0. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Infiltration Sensible Heat Loss Energy [J]
-
-The total convective sensible heat loss, in Joules to the zone air corresponding to the Zone Infiltration Volume summed over the reporting period. When a Fan:OnOff object is used, the reported value is for the system on cycle.
-
-#### AFN Zone Infiltration Volume [m3]
-
-The volume of outdoor air flow into the zone from window/door openings and cracks in the exterior surfaces of the zone (i.e., the sum of ventilation and crack flows from the exterior into the zone). The zone air density is used to calculate the zone infiltration volume based on the mass flow rate. Note that AirflowNetwork Zone Infiltration Volume will be zero if all of the flows through the zone’s exterior surfaces are out of the zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the infiltration volume calculated during the fan on and off periods for the simulation timestep.
-
-#### AFN Zone Infiltration Mass [kg]
-
-The mass of air corresponding to the AirflowNetwork Zone Infiltration Volume. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the infiltration mass calculated during the fan on and off periods for the simulation timestep.
-
-#### AFN Zone Infiltration Air Change Rate [ach]
-
-The number of air changes per hour produced by outdoor air flow into the zone from window/door openings and cracks in the exterior surfaces of the zone (i.e. the sum of ventilation and crack flows from the exterior into the zone). The target zone air density is used to calculate the zone infiltration air change rate based on the mass flow rate Note that, like Zone Infiltration Volume, Zone Infiltration Air Change Rate will be zero if all flows through the zone’s exterior surfaces are out of the zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the infiltration air change rate calculated during the fan on and off periods for the simulation timestep.
-
-#### AFN Zone Mixing Volume [m3]
-
-This is a measure of interzone air flow for each thermal zone. It is the volume of air flow into the zone from adjacent zones through window/door openings and cracks in the interior heat transfer surfaces of the zone. The target zone air density is used to calculate the zone mixing volume based on the mass flow rate. This variable does not include flows that are from the zone to adjacent zones. Note that Zone Mixing Volume will be zero if all flows through the zone’s interior surfaces are out of the zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the mixing volume calculated during the fan on and off periods for the simulation timestep.
-
-#### AFN Zone Mixing Mass [kg]
-
-The mass of air corresponding to the AFN Zone Mixing Volume. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the mixing mass calculated during the fan on and off periods for the simulation timestep.
-
-#### AFN Zone Mixing Mass Flow Rate [kg/s]
-
-This is a sum of mass flow rates from adjacent zones to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the mixing mass flow rate calculated during the fan on and off periods for the simulation timestep.
-
-#### AFN Zone Outdoor Air CO2 Mass Flow Rate [kg/s]
-
-This is a sum of mass flow rates from outdoors multiplied by the outdoor carbon dioxide concentration level to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the outdoor mass flow rate calculated during the fan on and off periods for the simulation timestep.
-
-#### AFN Zone Outdoor Air Generic Air Contaminant Mass Flow Rate [kg/s]
-
-This is a sum of mass flow rates from outdoors multiplied by the outdoor generic air contaminant concentration level to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the outdoor mass flow rate calculated during the fan on and off periods for the simulation timestep
-
-#### AFN Zone Outdoor Air Mass Flow Rate [kg/s]
-
-This is a sum of mass flow rates from outdoors to the receiving zone. When a Fan:OnOff object is used, the reported value is weighted by the system fan part-load ratio using the outdoor mass flow rate calculated during the fan on and off periods for the simulation timestep.
-
-#### AFN Zone Total CO2 Mass Flow Rate [kg/s]
-
-This is a sum of mass flow rates from adjacent zones or outdoors multiplied by the carbon dioxide concentration differences between the corresponding zone and the receiving zone.
-
-#### AFN Zone Total Generic Air Contaminant Mass Flow Rate [kg/s]
-
-This is a sum of mass flow rates from adjacent zones or outdoors multiplied by the generic contaminant concentration differences between the corresponding zone and the receiving zone.
-
-The following output variables are reported only when an AirflowNetwork:OccupantVentilationControl object is used:
-
-#### AFN Surface Venting Window or Door Opening Factor at Previous Time Step []
-
-The value of the venting opening factor for a particular window or door at the previous time step. When the window or door is venting, this is the input value of the opening factor (see AirflowNetwork:Multizone:Surface, Window/Door Opening Factor) times the multiplier for venting modulation (see description of next output variable, "Opening Factor Multiplier for AirflowNetwork Venting Modulation"). For example, if  the input Window/Door opening factor is 0.5 and the modulation multiplier is 0.7, then the value of this output variable will be 0.5*0.7 = 0.35.
-
-#### AFN Surface Opening Elapsed Time [min]
-
-This output is the opening elapsed time in the units of minutes since the window opened.
-
-#### AFN Surface Closing Elapsed Time [min]
-
-This output is the opening elapsed time in the units of minutes since the windows closed.
-
-#### AFN Surface Opening Status at Previous Time Step []
-
-This is the window or door opening factor control status at the previous time step using an AirflowNetwork:OccupantVentilationControl object, which can have three integer values: 0, 1, and 2. A 0 value indicates no occupant ventilation control. The opening factor is determined by the Ventilation Control Mode field. A value of 1 indicates that a window or door is allowed to open. The value of 1 is determined when the opening elapsed time is less than the minimum opening time. A value of 2 denotes that a window or door is forced to close. The value of 2 is determined when the closing elapsed time is less than the minimum closing time.
-
-#### AFN Surface Opening Status []
-
-This is the window or door opening factor control status at the current time step using an AirflowNetwork:OccupantVentilationControl object, which can have three integer values: 0, 1, and 2. A 0 value indicates no occupant ventilation control. The opening factor is determined by the Ventilation Control Mode field. A value of 1 indicates that a window or door is allowed to open. The value of 1 is determined when the opening elapsed time is less than the minimum opening time. A value of 2 denotes that a window or door is forced to close. The value of 2 is determined when the closing elapsed time is less than the minimum closing time.
-
-#### AFN Surface Opening Probability Status []
-
-This is the opening probability status at the current time step using an AirflowNetwork:OccupantVentilationControl object, which can have three integer values: 0, 1, and 2. A 0 value indicates no opening probability control action. A value of 1 indicates that a window or door is forced to open when the opening status is 0. A value of 2 denotes that the status at the previous time step will be kept.
-
-#### AFN Surface Closing Probability Status []
-
-This is the closing probability status at the current time step using an AirflowNetwork:OccupantVentilationControl object, which can have three integer values: 0, 1, and 2. A 0 value indicates no closing probability control action. A value of 1 indicates that a window or door is forced to close when the opening status is 0. A value of 2 denotes that the status at the previous time step will be kept.
-
-#### RoomAirflowNetwork Node Temperature [C]
-
-This is the RoomAirflowNetwork node temperature output in degrees C.
-
-#### RoomAirflowNetwork Node Humidity Ratio [kgWater/kgDryAir]
-
-This is the RoomAirflowNetwork node humidity ratio output in kgWater/kgDryAir.
-
-#### RoomAirflowNetwork Node Total Pressure [Pa]
-
-This is the RoomAirflowNetwork node total pressure in Pa with respect to outdoor barometric pressure. The total pressure is the sum of static pressure, dynamic pressure, and elevation impact at the node’s relative height.
-
-Group - Zone Equipment
-----------------------
-
-There are five main zone equipment statements that must be used to describe a block of zone equipment as shown in the below figure “Zone Equipment Input Syntax Map�.
-
-Types of Zone equipment are listed below and shown below in figure “Zone Equipment�.
-
-Table 26. Available Zone Equipment Types
-
-<table class="table table-striped">
-<tr>
-<th>Air Distribution Equipment</th>
-<td>AirTerminal:SingleDuct:Uncontrolled <BR>
-AirTerminal:SingleDuct:ConstantVolume:Reheat <BR>
-AirTerminal:SingleDuct:VAV:Reheat <BR>
-AirTerminal:SingleDuct:VAV:NoReheat <BR>
-AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan <BR>
-AirTerminal:DualDuct:ConstantVolume <BR>
-AirTerminal:DualDuct:VAV <BR>
-Powered Induction Units (Series and Parallel)</td>
-</tr>
-<tr>
-<th>Zone Forced Air Units
- </td>
-<td>ZoneHVAC:IdealLoadsAirSystem <BR>
-ZoneHVAC:FourPipeFanCoil <BR>
-ZoneHVAC:WindowAirConditioner <BR>
-ZoneHVAC:RefrigerationChillerSet <BR>
-Unit Ventilator/Heater <BR>
-Air-to-Air Heat Pumps <BR>
-Unitary Systems (heat only and heat/cool) <BR>
-Furnaces (heat only and heat/cool) <BR>
-Energy Recovery Ventilator:Stand Alone <BR>
-CoilSystem:Cooling:DX</td>
-</tr>
-<tr>
-<th>Radiative/Convective Units</th>
-<td>Baseboard Heaters <BR>
-Low Temp Radiant Systems <BR>
-High Temp Radiant System</td>
-</tr>
-</table>
-
-![ZoneEquipmentSyntax (media/image261.png)
-
-Figure 99. Zone Equipment Input Syntax Map
-
-![](media/image262.svg)
-
-Figure 100. Representative Zone Equipment
-
-The following figure (Air Loop/Zone Equipment Node Diagram) illustrates the connection between the zone equipment and the air loop systems.
-
-![](media/image263.svg)
-
-Figure 101. Air Loop/Zone Equipment Node Diagram
-
-Each zone served by an HVAC system must have three additional statements to complete the zone equipment specification. An ZoneHVAC:AirDistributionUnit allows equipment typically found within the zone inlet ductwork (such as dampers, reheat coils, etc.) to be attached to the supply air stream for a particular zone. A ZoneControl statement will allow the conditions in the zone to be managed. Finally, a ZoneHVAC:EquipmentConnections statement describes all of the pertinent information about the zone from an HVAC perspective. Each of these statements is described in more detail below.
-
-### ZoneHVAC:AirDistributionUnit
-
-The ZoneHVAC:AirDistributionUnit object gives further information on what air loop equipment (air terminal units) will be serving a particular zone. The ZoneHVAC:AirDistributionUnit is the part of the system that is supplied from a common main air handler simulated in the Air Loop Simulation and includes the equipment that controls or tempers the air going to each individual zone according to the desired thermostatic control. The current options for ZoneHVAC:AirDistributionUnit terminal unit types are:
-
-* AirTerminal:DualDuct:ConstantVolume
-
-* AirTerminal:DualDuct:VAV
-
-* AirTerminal:DualDuct:VAV:OutdoorAir
-
-* AirTerminal:SingleDuct:ConstantVolume:Reheat
-
-* AirTerminal:SingleDuct:VAV:Reheat
-
-* AirTerminal:SingleDuct:VAV:NoReheat
-
-* AirTerminal:SingleDuct:SeriesPIU:Reheat
-
-* AirTerminal:SingleDuct:ParallelPIU:Reheat
-
-* AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction
-
-* AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan
-
-* AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat
-
-* AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat
-
-
-Connections between the air distribution unit, the supply air duct, and the zone are specified in the input syntax for the air distribution unit and the AirLoopHVAC:ZoneSplitter. The input syntax also explicitly defines an outlet identifier. This implies a connection to a zone through a NodeList for zone inlets (see the ZoneHVAC:EquipmentConnections statement). The air distribution unit is limited to one combined component-controller unit; because controls are normally based on the zone thermostat and can work in parallel or series in complex fashion. Since the control and the flow resolution can be complex, each air distribution unit is unique in addressing these combinations and therefore only one is allowed per zone.
-
-The Air Distribution unit also allows the user to specify leaks in the supply air duct system. These inputs are used in the EnergyPlus Simplified Duct Leakage Model (SDLM). This model simulates a specific configuration: supply leaks to a return plenum in a commercial VAV or CV system. The system must have a constant static pressure setpoint. Within these limitations SDLM allows the user to easily evaluate the energy penalty due to duct leakage.
-
-#### Field: Name
-
-Unique identifying name of the air distribution unit.
-
-#### Field: Air Distribution Unit Outlet Node Name
-
-Outlet node name for the air distribution unit to the attached zone.
-
-#### Field: Air Terminal Object Type
-
-Single combined component/controller unit for that attached zone. Selection of components as listed above.
-
-#### Field: Air Terminal Name
-
-The unique identifying component name.
-
-#### Field: Nominal Upstream Leakage Fraction
-
-This is the leakage upstream of the terminal unit as a fraction of the design flow rate through the unit. It is the leakage fraction at the design flow rate. It is used to calculate a leakage flow rate which is then held constant while the system air flow varies. This input is optional; the default is zero.
-
-#### Field: Constant Downstream Leakage Fraction
-
-This is the leakage downstream of the terminal unit as a fraction of the current flow rate through the terminal unit. This fraction is held constant, so the leakage flow rate will vary proportinally with the supply air flow rate. This input is optional; the default is zero.
-
-Two example IDF excerpts (one with duct leakage, one without):
-
-```idf
-ZoneHVAC:AirDistributionUnit,
-    SPACE1-1 ATU,            !- Air Distribution Unit Name
-    SPACE1-1 In Node,        !- Air Dist Unit Outlet Node Name
-    AIRTERMINAL:SINGLEDUCT:VAV:REHEAT,  !- KEY--System Component Type 1
-    SPACE1-1 VAV Reheat;     !- Component Name 1
-
-ZoneHVAC:AirDistributionUnit,
-    SPACE4-1 ATU,            !- Air Distribution Unit Name
-    SPACE4-1 In Node,        !- Air Dist Unit Outlet Node Name
-    AIRTERMINAL:SINGLEDUCT:VAV:REHEAT,  !- KEY--System Component Type 1
-    SPACE4-1 VAV Reheat,     !- Component Name 1
-    0.05,                    !- upstream nominal leakage fraction
-    0.07;                    !- downstream constant leakage fraction
-```
-
-
-### ZoneHVAC:EquipmentConnections
-
-Finally, the ZoneHVAC:EquipmentConnections statement defines the remaining details about each thermal zone from an HVAC perspective (besides the controls which were defined above). As with other statements, the first two items in this object are the keyword and an identifying name which links the zone back to its geometrical input, internal gains, etc. and other statements in the HVAC section of the input. The next three items are names of lists (equipment, air inlet nodes, and air exhaust nodes) that are described in more detail below. Note that if there are no air exhaust nodes from the zone that field is left blank. And if there are no air inlet nodes, that field is left blank. Finally, two node names are necessary to complete the zone-HVAC description. The first node is the main air node for the zone upon which the air heat balance is performed. The other node begins the return air path from the zone.
-
-Note that all nodes mentioned in the ZoneHVAC:EquipmentConnections input must be unique.  That is, all nodes in all the ZoneHVAC:EquipmentConnections statements referenced by the “Zone Air Inlet Nodes�, “Zone Air Exhaust Nodes�, “Zone Air Node Name� and “Zone Return Air Node Name� cannot have any node name appearing more than once.
-
-#### Field: Zone Name
-
-Name links this equipment list back to the heat balance for the zone.
-
-#### Field: Zone Conditioning Equipment List Name
-
-List of zone equipment for this zone in a ZoneHVAC:EquipmentList object. This list will consist of air distribution units or other direct convection or radiant equipment, i.e. window air conditioner, baseboard, fan coils, etc.
-
-#### Field: Zone Air Inlet Node or NodeList Name
-
-There can be more than one air inlet node depending on how many pieces of equipment are in the ZoneHVAC:EquipmentList. Generally there will be one air inlet node for each piece of zone equipment that delivers conditioned air to the zone. Components such as electric or hot water baseboards and radiant systems do not require zone air inlet nodes. If there is only one node – its name can be put in this field. If there is more than one node, this must be the name of a node list object (a node list object can also contain only one node name). If this field is not required (as in the baseboard system), it should be blank.
-
-#### Field: Zone Air Exhaust Node or NodeList Name
-
-List of exhaust nodes leaving the zone for exhaust fans, zone energy recovery, etc. However these nodes are also used as sources of zone air for zone components such as fan coil units, unit heaters and ventilators, and window air conditioners. For each such component attached to a zone there should be a unique zone exhaust node acting as the inlet node to the component. If there is only one node – its name can be put in this field. If there is more than one node, this must be the name of a node list object (a node list object can also contain only one node name). If there are no air exhaust nodes, this field should be blank.
-
-#### Field: Zone Air Node Name
-
-The conditions at this node represent the average state of the air in the zone. For zones modeled as fully mixed the conditions at this node are assumed to represent the air in the entire zone. This field is required for all ZoneHVAC:EquipmentConnections statements.
-
-#### Field: Zone Return Air Node Name
-
-The name of the return air node which attaches the zone to the return air path described above. Even if there is no return air or no return air path a unique name must be entered in this field. The conditions at this node represent the state of the air leaving the zone including any heat gain from light-heat-to-return.
-
-#### Field: Zone Return Air Flow Rate Fraction Schedule Name
-
-The name of a schedule to specify the return air flow rate as a fraction of the base return air. If the next field is blank, then the return air flow rate is the total supply inlet flow rate to the zone less the total exhaust node flow rate from the zone multiplied by this schedule name. If this field is left blank, the schedule defaults to 1.0 at all times.
-
-#### Field: Zone Return Air Flow Rate Basis Node or NodeList Name
-
-The name of a node or list of nodes (NodeList) that is used to calculate the return air flow rate for this zone. The sum of the current flow rates for this node(s) multiplied by the Zone Return Air Flow Rate Fraction Schedule determines the return air flow rate. If this field is blank, then the base return air flow rate is the total supply inlet flow rate to the zone less the total exhaust node flow rate from the zone.
-
-An example of this statement in an IDF is:
-
-```idf
-ZoneHVAC:EquipmentConnections,
-    SPACE3-1,              !- Zone Name
-    SPACE3-1 Eq,           !- List Name: Zone Equipment
-    SPACE3-1 In Nodes,     !- List Name: Zone Air Inlet Nodes
-    ,                      !- List Name: Zone Air Exhaust Nodes
-    SPACE3-1 Node,         !- Zone Air Node Name
-    SPACE3-1 Out Node;     !- Zone Return Air Node Name
-```
-
-The following HVAC equipment types are allowed as zone equipment. The component matrix shows which coils and fans are allowed with which equipment models.
-
-![](media/ZoneComponentMatrix.png)
-
-### ZoneHVAC:EquipmentList
-
-The first list encountered in the ZoneHVAC:EquipmentConnections statement is the ZoneHVAC:EquipmentList. This object lists all HVAC equipment serving the zone. Each item in the list has four fields associated with it: Object Type, Name, Cooling Sequence and Heating or No-Load Sequence The Object Type and Name identify the specific equipment object. Cooling Sequence and Heating or No-Load Sequence specify the order of simulation for zones with more than one type of HVAC equipment.
-
-Note that a ZoneHVAC:AirDistributionUnit or AirTerminal:SingleDuct:Uncontrolled must be listed in this statement if there is a forced air system serving the zone from an air loop.
-
-#### Field: Name
-
-Unique identifying name.
-
-#### Field Set (Zone Equipment: Object Type, Name, Cooling Sequence, Heating or No-Load Sequence)
-
-This set is used together in order to sequence the equipment for heating and cooling. The \#1 sequence equipment will try to meet the entire demand with its capacity and then pass the results on to the \#2 and so on for both heating and cooling. This field set is extensible by duplicating the last four fields.
-
-Equipment is simulated in the order specified by Zone Equipment Cooling Sequence and Zone Equipment Heating or No-Load Sequence, depending on the current thermostat request. For equipment of similar type, assign sequence 1 to the first system intended to serve that type of load, assign sequence 2 to the next system, and so on. For situations where one or more equipment types has limited capacity or limited control capability, order the sequence so that the most controllable piece of equipment runs last. For example, with a dedicated outdoor air system (DOAS), the air terminal for the DOAS should be assigned Heating Sequence = 1 and Cooling Sequence = 1. Any other equipment should be assigned sequence 2 or higher so that it will see the net load after the DOAS air is added to the zone.
-
-#### Field: Zone Equipment &lt;x&gt; Object Type
-
-Type of zone equipment such as air distribution unit, baseboard, window air conditioner, etc. The current legal types are listed in the following table:
-
-Table 27. Legal Zone Equipment Types (ZoneHVAC:EquipmentList)
-
-<table class="table table-striped">
-<tr>
-<th>Legal Zone Equipment Types</th>
-</tr>
-<tr>
-<td>AirTerminal:SingleDuct:Uncontrolled</td>
-</tr>
-<tr>
-<td>Fan:ZoneExhaust</td>
-</tr>
-<tr>
-<td>WaterHeater:HeatPump:PumpedCondenser</td>
-</tr>
-<tr>
-<td>WaterHeater:HeatPump:WrappedCondenser</td>
-</tr>
-<tr>
-<td>ZoneHVAC:AirDistributionUnit</td>
-</tr>
-<tr>
-<td>ZoneHVAC:Baseboard:Convective:Electric</td>
-</tr>
-<tr>
-<td>ZoneHVAC:Baseboard:Convective:Water</td>
-</tr>
-<tr>
-<td>ZoneHVAC:Baseboard:RadiantConvective:Electric</td>
-</tr>
-<tr>
-<td>ZoneHVAC:Baseboard:RadiantConvective:Water</td>
-</tr>
-<tr>
-<td>ZoneHVAC:Baseboard:RadiantConvective:Steam</td>
-</tr>
-<tr>
-<td>ZoneHVAC:Dehumidifier:DX</td>
-</tr>
-<tr>
-<td>ZoneHVAC:EnergyRecoveryVentilator</td>
-</tr>
-<tr>
-<td>ZoneHVAC:FourPipeFanCoil</td>
-</tr>
-<tr>
-<td>ZoneHVAC:HighTemperatureRadiant</td>
-</tr>
-<tr>
-<td>ZoneHVAC:IdealLoadsAirSystem</td>
-</tr>
-<tr>
-<td>ZoneHVAC:LowTemperatureRadiant:ConstantFlow</td>
-</tr>
-<tr>
-<td>ZoneHVAC:LowTemperatureRadiant:Electric</td>
-</tr>
-<tr>
-<td>ZoneHVAC:LowTemperatureRadiant:VariableFlow</td>
-</tr>
-<tr>
-<td>ZoneHVAC:OutdoorAirUnit</td>
-</tr>
-<tr>
-<td>ZoneHVAC:PackagedTerminalAirConditioner</td>
-</tr>
-<tr>
-<td>ZoneHVAC:PackagedTerminalHeatPump</td>
-</tr>
-<tr>
-<td>ZoneHVAC:RefrigerationChillerSet</td>
-</tr>
-<tr>
-<td>ZoneHVAC:UnitHeater</td>
-</tr>
-<tr>
-<td>ZoneHVAC:UnitVentilator</td>
-</tr>
-<tr>
-<td>ZoneHVAC:WindowAirConditioner</td>
-</tr>
-<tr>
-<td>ZoneHVAC:WaterToAirHeatPump</td>
-</tr>
-<tr>
-<td>ZoneHVAC:VentilatedSlab</td>
-</tr>
-</table>
-
-#### Field: Zone Equipment &lt;x&gt; Name
-
-Name of the zone equipment used in the object definition of its type.
-
-#### Field: Zone Equipment &lt;x&gt; Cooling Sequence
-
-Specifies the zone equipment simulation order when the zone thermostat requests cooling.
-
-#### Field: Zone Equipment &lt;x&gt; Heating or No-Load Sequence
-
-
-
-Specifies the zone equipment simulation order when the zone thermostat requests heating or no load.
-
-
-
-Examples of this statement in an IDF are:
-
-```idf
-  ZoneHVAC:EquipmentList,
-    Zone1Equipment,          !- Name
-    ZoneHVAC:AirDistributionUnit,  !- Zone Equipment 1 Object Type
-    Zone1TermReheat,         !- Zone Equipment 1 Name
-    1,                       !- Zone Equipment 1 Cooling Sequence
-    1;                       !- Zone Equipment 1 Heating or No-Load Sequence
-
-
-  ZoneHVAC:EquipmentList,
-    Zone1Equipment,          !- Name
-    AirTerminal:SingleDuct:Uncontrolled,  !- Zone Equipment 1 Object Type
-    Zone1DirectAir,          !- Zone Equipment 1 Name
-    1,                       !- Zone Equipment 1 Cooling Sequence
-    1,                       !- Zone Equipment 1 Heating or No-Load Sequence
-    ZoneHVAC:WaterToAirHeatPump,  !- Zone Equipment 2 Object Type
-    Zone1WTAHP,              !- Zone Equipment 2 Name
-    2,                       !- Zone Equipment 2 Cooling Sequence
-    2;                       !- Zone Equipment 2 Heating or No-Load Sequence
-```
-
-Group – Air Distribution Equipment
-----------------------------------
-
-The systems described in the Air Distribution Units (ADU’s) are shown below. A variety of air terminal units are available for connecting air systems to thermal zones. These single description ADU’s contain the reference to the components and the actual controls in one block of input. The idea is that the control volume is drawn tightly around the controls and loosely around the components. This allows complex interactions to take place between all of the components that respond to the Zone Thermostatic Control output. The coils that are referenced in the ADU’s are explained fully in the “Coils� section of this manual.
-
-### AirTerminal:SingleDuct:Uncontrolled
-
-Central system air is usually supplied to a zone through a terminal unit such as a single duct VAV reheat box. Sometimes, however, it is desirable to supply central system air directly to a zone without any zone level control or tempering. An example would be a single zone reheat system.
-
-The control zone receives supply air directly from the central system since the supply air temperature has been adjusted to control the temperature in the control zone. The slave zones then have baseboards or reheat coils to allow some temperature adjustment. The AirTerminal:SingleDuct:Uncontrolled object creates the capability of supplying central system air directly to a zone. Its input consists of the object name, an availability (on/off) schedule, and a node name. This node is both a zone inlet node and an outlet node of the AirLoopHVAC:ZoneSplitter.
-
-For the objects to work correctly, it is important in any systems including Direct Air objects for the sum of the maximum zone air flow rates to be equal to the maximum central system flow rate. The zone maximum flow rates are specified in the zone terminal unit or direct air inputs. The central air system flow rate is specified in the AirLoopHVAC input and also in the air loop branch and central fan inputs.
-
-#### Field: Name
-
-A unique user assigned name for each AirTerminal:SingleDuct:Uncontrolled component. Any other component that needs to use this direct air component will refer to it by this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the component can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Zone Supply Air Node Name
-
-The name of the node to which the component is supplying air. This should be one of the supply air nodes for the zone the component is serving. This node should also be an outlet node of a AirLoopHVAC:ZoneSplitter component.
-
-#### Field: Maximum Air Flow Rate
-
-The design maximum volume flow rate  (m<sup>3</sup>/sec) specified for the AirTerminal:SingleDuct:Uncontrolled object.  This field is autosizable.
-
-An example input follows.
-
-```idf
-AirTerminal:SingleDuct:Uncontrolled,
-    Zone1DirectAir,
-    FanAndCoilAvailSched,
-    Zone 1 Inlet Node,
-    0.47;
-AirTerminal:SingleDuct:Uncontrolled,
-    Zone2DirectAir,
-    FanAndCoilAvailSched,
-    Zone 2 Inlet Node,
-    0.36;
-AirTerminal:SingleDuct:Uncontrolled,
-    Zone3DirectAir,
-    FanAndCoilAvailSched,
-    Zone 3 Inlet Node,
-    0.47;
-```
-
-
-### Single Duct Uncontrolled AirTerminal Outputs
-
-* HVAC,Sum,Zone Air Terminal Sensible Heating Energy [J]
-
-* HVAC,Sum,Zone Air Terminal Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Air Terminal Sensible Heating Rate [W]
-
-* HVAC,Average,Zone Air Terminal Sensible Cooling Rate [W]
-
-#### Zone Air Terminal Sensible Heating Energy  [J]
-
-#### Zone Air Terminal Sensible Heating Rate [W]
-
-These outputs are the sensible heating power and energy provided to the zone by the uncontrolled air terminal unit.
-
-#### Zone Air Terminal Sensible Cooling Energy [J]
-
-#### Zone Air Terminal Sensible Cooling Rate [W]
-
-These outputs are the sensible cooling power and energy provided to the zone by the uncontrolled air terminal unit.
-
-### AirTerminal:SingleDuct:ConstantVolume:Reheat
-
-The AirTerminal:SingleDuct:ConstantVolume:Reheat or terminal reheat system is a constant volume reheat system. The systems cooling capabilities are provided by way of cooling coil that supplies cooling to the entire supply air volume. The cooling coil is controlled by a controller setpoint specified for the cooling coil. Zone control is accomplished by heating (reheating) the airflow into each zone as determined by the zone thermostat. Currently the reheat can be supplied by a electric, gas, or hot water coil that tries to meet the zone demand.
-
-#### Field: Name
-
-Unique name for the terminal reheat Air Distribution Unit (ADU).
-
-#### Field: Availability Schedule Name
-
-Schedule that this component will operate or is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Outlet Node Name
-
-The outlet node from the ADU to the zone. This is the same node as the reheat component air outlet node.
-
-#### Field: Air Inlet Node Name
-
-The air-inlet node name that connects the air splitter to the individual zone ADU. This is the same node as the reheat component air inlet node.
-
-#### Field: Maximum Air Flow Rate
-
-The design constant volume flow rate (m<sup>3</sup>/sec) specified for the terminal reheat ADU.
-
-#### Field: Reheat Coil Object Type
-
-The valid reheat component objects currently available are:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Steam
-
-#### Field: Reheat Coil Name
-
-Reheat Coil Object name being simulated with this ADU. Applicable for all coils.
-
-#### Field: Maximum Hot Water or Steam Flow Rate
-
-This field is zero for gas and electric coils. Set to the maximum design hot water or steam volumetric flow rate in m<sup>3</sup>/s for the hot water or steam heating coil. The steam volumetric  flow rate is calculated at 100C and 101325 Pa.
-
-#### Field: Minimum Hot Water or Steam Flow Rate
-
-This field is zero for gas and electric coils. Set to the minimum design hot water or steam volumetric flow rate in m<sup>3</sup>/s for the hot water or steam coil, normally set to be a shut off valve that is set to zero. The steam volumetric  flow rate is calculated at 100C and 101325 Pa.
-
-#### Field: Convergence Tolerance
-
-The coil is controlled by knowing the zone demand determined by the zone thermostat and setting the outlet conditions to meet this demand. For the electric and gas coils, this is set exactly since the coil model solution can be inverted. With the hot water coil that uses an effectiveness-NTU method, the solution cannot be inverted directly. Therefore, to determine the correct mass flow rate for the hot water the solution is solved for by iteration. The iterative solution uses an interval halving routine and needs a termination criteria that is set with the Convergence Tolerance parameter. This control offset is set to a decimal fraction of the zone demand as the criteria, i.e. 0.001. The default for the field is 0.001.
-
-#### Field: Maximum Reheat Air Temperature
-
-This is the upper limit on the temperature in degrees C of the air leaving the terminal unit – reheat coil (and being delivered to the zone). If the user leaves this field blank, no maximum reheat air temperature is enforced.
-
-An IDF example:
-
-```idf
-AirTerminal:SingleDuct:ConstantVolume:Reheat,
-    Reheat Zone 1,  !- Name of System
-    FanAndCoilAvailSched,  !- Availability schedule for VAV System
-    Zone 1 Reheat Air Outlet Node,  !- Unit Air Outlet Node
-    Zone 1 Reheat Air Inlet Node,  !- Unit Air Inlet Node
-    0.59,  !- Maximum air flow rate {m3/s}
-    COIL:Gas:Heating,  !- Reheat Component Object
-    Reheat Coil Zone 1,  !- Name of Reheat Component
-    0.0,  !- Max Reheat Water Flow {m3/s}
-    0.0,  !- Min Reheat Water Flow {m3/s}
-    0.001;  !- Convergence Tolerance
-```
-
-### Single Duct Constant Volume Reheat AirTerminal Outputs
-
-There are no outputs for the constant volume reheat air terminal.
-
-### AirTerminal:SingleDuct:VAV:Reheat
-
-AirTerminal:SingleDuct:VAV:Reheat - Variable air volume (VAV) systems control the dry-bulb temperature inside a zone by varying the supply air volume instead of the air temperature. At full cooling the VAV damper is fully open supplying the specified maximum air flow rate. As the cooling load decreases, the damper closes until it reaches the minimum stop specified by the zone minimum air flow fraction.
-
-VAV systems can be used for interior or perimeter zones with a common fan system, air temperature control, and reheating devices. The VAV concept may vary according to the VAV box locations, air temperature controls and types of heating elements. Heating can usually be provided by use of reheat coils or thermostatic baseboard.
-
-#### Field: Name
-
-Unique name for the AirTerminal:SingleDuct:VAV:Reheat Air Distribution Unit (ADU).
-
-#### Field: Availability Schedule Name
-
-Schedule that this component will operate or is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Damper Air Outlet Node Name
-
-The VAV damper outlet node. This is the outlet node of the damper and the inlet node of the reheat coil.
-
-#### Field: Air Inlet Node Name
-
-The air inlet node name that connects the air splitter to the individual zone ADU. This is *not* the same as the air inlet node of the reheat component: it is upstream of that node. This is the inlet node to the terminal unit and the damper
-
-#### Field: Maximum Air Flow Rate
-
-The design maximum volume flow rate (m<sup>3</sup>/sec) specified for VAV ADU.
-
-#### Field: Zone Minimum Air Flow Method
-
-This field is used to select how the program will determine the minimum flow rate to the zone while the system is operating.  There are three choices for selecting how the minimum flow rate is specified:  Constant, FixedFlowRate, and Scheduled.  If Constant is entered, then the program will use the value for the constant minimum air flow fraction entered in the following field.  If FixedFlowRate is entered, then the program will use the value entered in the field below called Fixed Minimum Air Flow Rate.If Scheduled is entered, then the program will obtain the value for minimum flow fraction from the schedule named in the field below called Minimum Air Flow Fraction Schedule Name.
-
-#### Field: Constant Minimum Air Flow Fraction
-
-The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default).  This field is used if the previous field is set to Constant.  If the previous field is set to Scheduled (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then this field is optional and can be used to separately control the air flow rate used for sizing normal-action reheat coils. If this field and the following field have values, the greater of the two is used for sizing.
-
-#### Field: Fixed Minimum Air Flow Rate
-
-The minimum flow rate to the zone while the system is operating, specified as a fixed minimum air flow rate in meters cubed per second. The minimum air flow rate is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default).  This field is used if the Zone Minimum Air Flow Method field is set to FixedFlowRate. If the Zone Minimum Air Flow Method field is set to Scheduled (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then this field is optional and can be used to separately control the air flow rate used for sizing normal-action reheat coils. Only one of these two minimum air flow fields (i.e., this field and the previous field) should be used at any time. If this field and the previous field have values, the greater of the two is used for sizing.
-
-#### Field: Minimum Air Flow Fraction Schedule Name
-
-The name of a schedule that determines the value of the minimum air flow fraction.  The schedule should contain fractions from 0.0 to 1.0.  These values will define the minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate.  The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default).  This field is used if the previous field is set to Scheduled.  If the previous field is left blank (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then the air flow rate usedfor sizing normal-action reheat coils is the average of the minimum and maximum values in this schedule.  The air flow rate used for reheat coil sizing is reported with other component sizing information as “Reheat Coil Sizing Air Volume Flow Rate.�
-
-#### Field: Reheat Coil Object Type
-
-The valid reheat component objects currently available are:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Steam
-
-If there is no reheat coil,use AirTerminal:SingleDuct:VAV:NoReheat instead of this object.
-
-#### Field: Reheat Coil Name
-
-Reheat Coil Object name being simulated with this ADU. Applicable for all coils. If there is no reheat coil,use object AirTerminal:SingleDuct:VAV:NoReheat instead of this object.
-
-#### Field: Maximum Hot Water or Steam Flow Rate
-
-This field is zero for gas and electric coils. Set to the maximum design hot water or steam volumetric flow rate in m<sup>3</sup>/s for the hot water or steam heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. This field is autosizable. If there is no reheat coil,  this is left blank.
-
-#### Field: Minimum Hot Water or Steam Flow Rate
-
-This field is zero for gas and electric coils. Set to the minimum design hot water or steam volumetric flow rate in m<sup>3</sup>/s for the hot water or steam heating coil, normally set to be a shut off valve that is set to zero. The steam volumetric flow rate is calculated at 100C and 101325 Pa. If there is no reheat coil,  this is left blank.
-
-#### Field: Air Outlet Node Name
-
-The terminal unit outlet node. This is the outlet node of the reheat coil and the zone inlet node.
-
-#### Field: Convergence Tolerance
-
-The coil is controlled by knowing the zone demand determined by the zone thermostat and setting the outlet conditions to meet this demand. For the electric and gas coils, this is set exactly since the coil model solution can be inverted. With the hot water coil that uses an effectiveness-NTU method, the solution cannot be inverted directly. Therefore, to determine the correct mass flow rate for the hot water the solution is solved for by iteration. The iterative solution uses an interval halving routine and needs a termination criteria that is set with the Convergence Tolerance parameter. This control offset is set to a decimal fraction of the zone demand as the criteria, i.e. 0.001. The default for the field is 0.001.
-
-#### Field: Damper Heating Action
-
-During heating operation, there are two control options for the damper controlling the air flow in the VAV terminal unit as the zone moves above or below the zone setpoint. With both control options, the damper is at the minimum air flow rate whenever the zone temperature is between the cooling and heating setpoints (deadband condition).
-
-With **Normal** (the default) action, the damper will remain at the minimum air flow rate during heating operation. As the heating load increases, the water flow rate in the reheat coil will be increased to maintain temperature in the zone until the maximum water flow rate is reached or the user-specified maximum reheat air temperature is reached..  This is sometimes called the single maximum control logic as illustrated below.
-
-![](media/image264.svg)
-
-Figure 102. The Single Maximum Control Logic
-
-With **Reverse** action, as the heating load increases, the unit starts at minimum air flow and minimum hot water flow. The hot water flow is increased until it reaches maximum flow or the user-specified maximum reheat air temperature is reached, then the air damper starts to open to meet the load. This option is used if the minimum air flow rate is not adequate to serve the peak heating load. This is sometimes called the dual maximum control logic as illustrated in following figure. For heating coil types other than the hot-water coil, e.g. electric, steam, and gas, the reverse action works the same as the normal action – always keeping the air flow at the minimum during heating.
-
-The dual-max control currently applies to the AirTerminal:SingleDuct:VAV:Reheat objects with reverse acting dampers and hot-water coils.
-
-![](media/image265.svg)
-
-Figure 103.  The Dual Maximum Control Logic
-
-#### Control Fields for Maximum Flow During Reheat:
-
-The following two fields are used only when Reheat Coil Object Type = Coil:Heating:Water and Damper Heating Action = Reverse. Maximum Flow per Zone Floor Area During Reheat and Maximum Flow Fraction During Reheat are two optional methods to calculate the maximum allowable air flow rate during reheat operation. If both are entered, the greater resulting flow rate is used. If Design Specification Outdoor Air Object Name is also specified, it may increase this limit to meet the outdoor air flow rate requirement. At no time will the maximum flow rate calculated here exceed the value for Maximum Air Flow Rate.
-
-This limit is active only when the zone thermostat requests heating and the VAV box damper is reverse acting.
-
-#### Field: Maximum Flow per Zone Floor Area During Reheat
-
-This factor (m<sup>3</sup>/s-m<sup>2</sup>) is multiplied by the zone area, to determine the maximum volume flow rate (m<sup>3</sup>/s) allowed during reheat operation (see detailed explanation above). This field is autocalculatable. If autocalculate is selected, the value is set to 0.002032 m<sup>3</sup>/s-m<sup>2</sup> (0.4 cfm/ft<sup>2</sup>). If this field and the following field are entered, the greater of the two inputs is used. If this field and the following field are left blank, the maximum flow will not be limited.
-
-#### Field: Maximum Flow Fraction During Reheat
-
-This fraction is multiplied by the Maximum Air Flow Rate to determine the maximum volume flow rate (m<sup>3</sup>/s) allowed during reheat operation (see detailed explanation above). This field is autocalculatable. If autocalculate is selected, the value is set to 0.002032 m<sup>3</sup>/s-m<sup>2</sup> (0.4 cfm/ft<sup>2</sup>) multiplied by the zone floor area divided by the Maximum Air Flow Rate. If this field and the previous field are entered, the greater of the two inputs is used. If this field and the previous field are left blank, the maximum flow will not be limited.
-
-#### Field: Maximum Reheat Air Temperature
-
-This field specifies a maximum supply air temperature (°C) leaving the reheat coil in a VAV terminal unit during heating operation. If leaving blank, the temperature of the supply air to the space in heating operation may get unrealistic high.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object. When this field is used, the terminal unit will increase flow as needed to meet this outdoor air requirement. If Outdoor Air Flow per Person is non-zero, then the outdoor air requirement will be computed based on the current number of occupants in the zone. At no time will the supply air flow rate exceed the value for Maximum Air Flow Rate. If this field is blank, then the terminal unit will not be controlled for outdoor air flow. See documentation for the zone HVAC outdoor air object for further information (Ref DesignSpecification:OutdoorAir).
-
-An IDF example:
-
-```idf
-AirTerminal:SingleDuct:VAV:Reheat,
-    SPACE2-1 VAV Reheat,  !- Name of System
-    ReheatCoilAvailSched,  !- Availability schedule for VAV System
-    SPACE2-1 Zone Coil Air In Node,  !- Damper Air Outlet Node
-    SPACE2-1 ATU In Node,  !- Unit Air Inlet Node
-    autosize,  !- Maximum air flow rate {m3/s}
-    Constant,  !- Zone Minimum Air Flow Input Method
-    0.3,  !- Constant Minimum Air Flow Fraction
-    ,  !- Fixed Minimum Air Flow Rate
-    ,  !- Minimum Air Flow Fraction Schedule Name
-    COIL:Gas:Heating,  !- Reheat Component Object
-    SPACE2-1 Zone Coil,  !- Name of Reheat Component
-    0.0,  !- Max Reheat Water Flow {m3/s}
-    0.0,  !- Min Reheat Water Flow {m3/s}
-    SPACE2-1 In Node,  !- Unit Air Outlet Node
-    0.001,  !- Convergence Tolerance
-    Reverse,  !- Damper Heating Action
-    ,         !- Maximum Flow per Zone Floor Area During Reheat
-    ,         !- Maximum Flow Fraction During Reheat
-    35.0,     !- Maximum Reheat Air Temperature {C}
-    ;         !- Design Specification Outdoor Air Object Name
-
-  DesignSpecification:OutdoorAir,
-    ZoneMinOARequirements,    !- Name
-    Sum,                      !- Outdoor Air Method
-    0.00472,                  !- Outdoor Air Flow per Person {m3/s}
-    0.000508,                 !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    ,                         !- Outdoor Air Flow per Zone
-    ,                         !- Outdoor Air Flow Air Changes per Hour
-    Min OARequirements Sched; !- Outdoor Air Flow Rate Fraction Schedule Name
-
-
-  Schedule:Compact,
-    Min OARequirements Sched,  !- Name
-    Any Number,                !- Schedule Type Limits Name
-    Through: 12/31,            !- Field 1
-    For: Weekdays SummerDesignDay WinterDesignDay, !- Field 2
-    Until: 24:00,1.0,          !- Field 7
-    For: AllOtherDays,         !- Field 9
-    Until: 24:00,0.25;         !- Field 10
-    COIL:Heating:Gas,
-    SPACE1-1 Zone Coil,  !- Coil Name
-    ReheatCoilAvailSched,  !- Availability Schedule Name
-    0.8,  !- Gas Burner Efficiency of the Coil
-    autosize,  !- Nominal Capacity of the Coil {W}
-    SPACE1-1 Zone Coil Air In Node,  !- Coil_Air_Inlet_Node
-    SPACE1-1 In Node;  !- Coil_Air_Outlet_Node
-```
-
-
-### Single Duct VAV Reheat AirTerminal Outputs
-
-* HVAC,Average,Zone Air Terminal VAV Damper Position []
-
-* HVAC,Average,Zone Air Terminal Minimum Air Flow Fraction []
-
-* HVAC,Average,Zone Air Terminal Outdoor Air Volume Flow Rate [m3/s]
-
-#### Zone Air Terminal VAV Damper Position []
-
-This output is the variable air volume damper position required to meet the zone load. This is the average value over the frequency being reported. The damper position is defined as the terminal unit air mass flow rate divided by the terminal unit’s maximum air mass flow rate.
-
-#### Zone Air Terminal Minimum Air Flow Fraction []
-
-This output is the value for the minimum air flow fraction setting on a VAV terminal.   This is the average value over the frequency being reported.  The minimum air flow fraction is defined as the lower limit on the terminal unit air mass flow rate divided by the terminal units maximum air mass flow rate.
-
-#### Zone Air Terminal Outdoor Air Volume Flow Rate [m3/s]
-
-This output is the amount of outdoor air entering the zone. This is the average value over the frequency being reported.  The amount of outdoor air is defined as the terminal unit air volume flow rate multiplied by the fraction of outdoor air entering the air loop’s outside air system.
-
-### AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan
-
-The VAV terminal unit with variable-speed fan and reheat coil is an air system terminal unit consisting of a variable speed fan in series with a heating coil. These units are usually employed in underfloor air distribution (UFAD) systems where the air is supplied at low static pressure through an underfloor plenum. The fan is used to control the flow of conditioned air that enters the space. When the fan is off the plenum pressure drives the minimum air flow through the terminal unit. At maximum cooling the fan runs at its maximum speed. At full heating the fan runs at its heating maximum – usually less than the cooling maximum flow rate. Thus this unit has two separate maximum flow rates – one for heating and one for cooling.
-
-For cooling, control is maintained simply by varying the fan speed. For heating, the unit first tries to meet the heating load by varying the heating coil output while keeping the air flow at minimum (fan off). If this is not adequate the fan turns on and operates in variable flow mode up to the heating maximum flow rate.
-
-This unit is modeled in EnergyPlus as a compound component – a variable speed fan and a heating coil in series in the air stream. The unit is blow through – the fan is upstream of the heating coil.
-
-#### Field: Name
-
-A unique user assigned name for a particular VS fan VAV reheat terminal unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Maximum Cooling Air Flow Rate
-
-The maximum volumetric air flow rate through the unit in cubic meters per second when the thermostat is calling for cooling. Normally this is the same as the unit’s fan maximum volumetric flow rate.
-
-#### Field: Maximum Heating Air Flow Rate
-
-The maximum volumetric air flow rate through the unit in cubic meters per second when the thermostat is calling for heating.
-
-#### Field: Zone Minimum Air Flow Fraction
-
-The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. For this unit this is the flow rate when the fan is off.
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node that is the air inlet node for the terminal unit. This is also the air inlet node for the unit’s fan.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node that is the air outlet node of the unit. This same node will be the unit heating coil’s air outlet node. This node is also a zone inlet node.
-
-#### Field: Fan Object Type
-
-The type of fan in the terminal unit. At this time the only type of fan allowed is *Fan:VariableVolume*.
-
-#### Field: Fan Name
-
-The name of the particular fan object in this terminal unit.
-
-#### Field: Heating Coil Object Type
-
-The type of heating coil in the terminal unit. The valid choices are:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Steam
-
-#### Field: Heating Coil Name
-
-The name of the heating coil object contained in this terminal unit.
-
-#### Field: Maximum Hot Water or Steam Flow Rate
-
-The maximum hot water or steam volumetric flow rate in m<sup>3</sup>/s through the unit’s heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. If the heating coil is not a hot water or steam coil this field should be left blank.
-
-#### Field: Minimum Hot Water or Steam Flow Rate
-
-The minimum hot water or steam volumetric flow rate in m<sup>3</sup>/s through the unit’s heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. If the heating coil is not a hot water or steam  coil this field should be left blank.
-
-The control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. The model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {{Q_{unit,out}} - {Q_{zone\;load}}} \right|}}{{{Q_{zone\;load}}}} \le ConvergenceTolerance\)\(\frac{{\left| {{Q_{PIU,out}} - {Q_{zone\;load}}} \right|}}{{{Q_{zone\;load}}}} \le ConvergenceTolerance\]</div>
-
-The default is 0.001.
-
-An IDF example:
-
-```idf
-AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan,
-    SPACE2-1 VAV Reheat,     !- Name of System
-    ReheatCoilAvailSched,    !- System Availability schedule
-    autosize,                !- Maximum cooling air volume flow rate
-    autosize,                !- Maximum heating air volume flow rate
-    0.05,                    !- Zone Minimum Air Flow Fraction
-    SPACE2-1 ATU In Node,    !- Air Inlet Node Name
-    SPACE2-1 In Node,        !- Air Outlet Node Name
-    FAN:SIMPLE:VariableVolume,       !- Fan object
-    SPACE2-1 Zone Fan,       !- Fan name
-    COIL:Water:SimpleHeating,!- Heating coil object
-    SPACE2-1 Zone Coil,      !- Heating coil name
-    autosize,                !- Max hot water flow
-    0.0,                     !- Min hot water flow
-    0.001;                   !- Heating Convergence Tolerance
-
-Coil:Heating:Water,
-    SPACE2-1 Zone Coil,      !- Coil Name
-    ReheatCoilAvailSched,    !- Availability Schedule Name
-    autosize,                !- UA of the Coil {W/K}
-    autosize,                !- Max Water Flow Rate of Coil {m3/s}
-    SPACE2-1 Zone Coil Water In Node,  !- Coil_Water_Inlet_Node
-    SPACE2-1 Zone Coil Water Out Node,  !- Coil_Water_Outlet_Node
-    SPACE2-1 Zone Coil Air In Node,  !- Coil_Air_Inlet_Node
-    SPACE2-1 In Node;        !- Coil_Air_Outlet_Node
-
-Fan:VariableVolume,
-    SPACE2-1 Zone Fan,       !- Fan Name
-    FanAvailSched,           !- Availability Schedule Name
-    0.7,                     !- Fan Total Efficiency
-    125.0,                   !- Delta Pressure {Pa}
-    autosize,                !- Max Flow Rate {m3/s}
-    0.0,                     !- Min Flow Rate {m3/s}
-    0.9,                     !- Motor Efficiency
-    1.0,                     !- Motor In Airstream Fraction
-    0.00153028,              !- FanCoefficient 1
-    0.00520806,              !- FanCoefficient 2
-    1.1086242,               !- FanCoefficient 3
-    -.11635563,              !- FanCoefficient 4
-    0.000,                   !- FanCoefficient 5
-    SPACE2-1 ATU In Node,    !- Fan_Inlet_Node
-    SPACE2-1 Zone Coil Air In Node;   !- Fan_Outlet_Node
-```
-
-
-### Single Duct VAV Reheat Variable Speed Fan AirTerminal Outputs
-
-HVAC,Average,Zone Air Terminal VAV Damper Position []
-
-#### Zone Air Terminal VAV Damper Position
-
-This output is the variable air volume flow fraction required to meet the zone load. This is the average value over the frequency being reported. The flow fraction is defined as the terminal unit air mass flow rate divided by the terminal unit’s maximum air mass flow rate.
-
-### AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat
-
-Variable air volume (VAV) systems typically control the dry-bulb temperature inside a zone by varying the supply air volume instead of the supply air temperature (ref: AirTerminal:SingleDuct:VAV:NoReheat). Reheat coils may be required to avoid overcooling (ref: AirTerminal:SingleDuct:VAV:Reheat).
-
-This terminal unit is slightly different from the AirTerminal:SingleDuct:VAV:Reheat terminal unit. Both operate the same in cooling mode: the damper opens as needed to provide additional sensible cooling to the zone. The difference between the two is in heating mode.  For the Single Duct VAV Reheat terminal unit, the air flow rate is reduced to the minimum value (max air flow rate x zone minimum air flow fraction) when zone heating is required and the reheat coil output is modulated to meet the zone heating load.  For the AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat terminal unit, the air flow rate in heating mode is increased to meet higher zone heating loads (similar to what is done in cooling mode). If additional heat is required (beyond what the terminal unit can provide with its damper fully open), then the reheat coil is modulated as needed to meet the additional heating load.
-
-This terminal unit model was originally developed and tested for use with the changeover-bypass VAV unitary system.
-
-![Damper](media/image267.png)
-
-Figure 104. Single Duct VAV Heat and Cool Reheat Schematic
-
-#### Field: Name
-
-Unique user-defined name for this Air Distribution Unit (ADU).
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether or not this component is available to operate during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Damper Air Outlet Node Name
-
-This alpha field defines the name of the VAV damper air outlet node. This is the outlet node of the damper and the inlet node of the reheat coil.
-
-#### Field: Air Inlet Node Name
-
-This alpha field defines the name of the air inlet node that connects the air splitter to the individual zone ADU. This is *not* the same as the air inlet node of the reheat component: it is upstream of that node. This is the inlet node to the terminal unit and the damper.
-
-#### Field: Maximum Air Flow Rate
-
-This numeric field defines the design maximum volumetric flow rate (m<sup>3</sup>/sec) specified for this VAV ADU. This flow rate must be greater than 0 or can be autosized.
-
-#### Field: Zone Minimum Air Flow Fraction
-
-This numeric field defines the minimum air volumetric flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates as needed to maintain the heating set point specified in the Zone Control:Thermostatic object. This value must be between 0 and 1.
-
-#### Field: Reheat Coil Object Type
-
-The valid reheat component objects currently available are:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Steam
-
-If no reheat coil is required, use AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat instead of this object.
-
-#### Field: Reheat Coil Name
-
-Unique coil name being simulated with this ADU. Applicable for all coils. If there is no reheat coil, use AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat instead of this object.
-
-#### Field: Maximum Hot Water or Steam Flow Rate
-
-This field is ignored for gas or electric reheat coils. If using a hot water or steam reheat coil, set to the maximum design water or steam volumetric flow rate in m<sup>3</sup>/s for the hot water or steam heating coil. The steam volume flow rate is calculated at 100C and 101325 Pa. This volumetric flow rate can be autosized.
-
-#### Field: Minimum Hot Water or Steam Flow Rate
-
-This field is ignored for gas and electric coils. Set to the minimum design water or steam volumetric flow rate in m<sup>3</sup>/s for the hot water or steam heating coil, normally set to be a shut-off valve that is set to zero. The steam volume flow rate is calculated at 100C and 101325 Pa.
-
-#### Field: Air Outlet Node Name
-
-This is the air outlet node for the ADU and is then connected to the zone. This is the same node as the air outlet node of the reheat component.
-
-#### Field: Convergence Tolerance
-
-The coil is controlled by knowing the zone demand determined by the zone thermostat and setting the outlet conditions to meet this demand. For the electric and gas coils, this is set exactly since the coil model solution can be inverted and this field is not used. With the hot water coil that uses an effectiveness-NTU method, the solution cannot be inverted directly. Therefore, to determine the correct mass flow rate for the hot water the solution is solved by iteration. The iterative solution uses an interval-halving routine and needs a termination criteria that is set with this Convergence Tolerance parameter. This control offset is set to a decimal fraction of the zone demand. The default value for this field is 0.001.
-
-#### Field: Maximum Reheat Air Temperature
-
-This is the upper limit on the temperature in degrees C of the air leaving the terminal unit – reheat coil (and being delivered to the zone). If the user leaves this field blank, no maximum reheat air temperature is enforced.
-
-An IDF example is provided below:
-
-```idf
-AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat,
-    Zone 1 VAV System,             !- Name of System
-    FanAndCoilAvailSched,          !- System Availability schedule
-    Zone 1 Reheat Air Inlet Node,  !- DAMPER Air Outlet Node
-    Zone 1 VAV Inlet Node,         !- UNIT Air Inlet Node
-    0.583,                         !- Maximum air flow rate {m3/s}
-    0.25,                          !- Zone Minimum Air Flow Fraction
-    Coil:Heating:Electric,         !- Reheat Component Object
-    Reheat Coil Zone 1,            !- Name of Reheat Component
-    0.0,                           !- Max Reheat Water Flow {m3/s}
-    0.0,                           !- Min Reheat Water Flow {m3/s}
-    Zone 1 Reheat Air Outlet Node, !- UNIT Air Outlet Node
-    0.001;                         !- Convergence Tolerance
-
-Coil:Heating:Electric,
-    Reheat Coil Zone 1,            !- Coil Name
-    FanAndCoilAvailSched,          !- Availability Schedule Name
-    1.0,                           !- Efficiency of the Coil
-    3000.0,                        !- Nominal Capacity of the Coil {W}
-    Zone 1 Reheat Air Inlet Node,  !- Coil_Air_Inlet_Node
-    Zone 1 Reheat Air Outlet Node; !- Coil_Air_Outlet_Node
-```
-
-
-### Single Duct VAV Heat and Cool Reheat AirTerminal Outputs
-
-HVAC,Average,Zone Air Terminal VAV Damper Position []
-
-#### Zone Air Terminal VAV Damper Position []
-
-This output is the damper position required to meet the zone load. This is the average value over the simulation timestep being reported. The damper position is defined as the terminal unit air mass flow rate divided by the terminal unit’s maximum air mass flow rate.
-
-### AirTerminal:SingleDuct:VAV:NoReheat
-
-Variable air volume (VAV) systems control the dry-bulb temperature inside a zone by varying the supply air volume instead of the air temperature. At full cooling the VAV damper is fully open supplying the specified maximum air flow rate. As the cooling load decreases, the damper closes until it reaches the minimum stop specified by the zone minimum air flow fraction.
-
-VAV systems can be used for interior or perimeter zones with a common fan system and air temperature control. The VAV concept may vary according to the VAV box locations and air temperature controls. Heating can be provided if necessary by use of baseboard.
-
-#### Field: Name
-
-Unique name for the VAV Air Distribution Unit (ADU).
-
-#### Field: Availability Schedule Name
-
-Schedule that this component will operate or is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Outlet Node Name
-
-The VAV damper and Unit outlet node.
-
-#### Field: Air Inlet Node Name
-
-The air inlet node name that connects the air splitter to the individual zone ADU.
-
-#### Field: Maximum Air Flow Rate
-
-The design maximum volume flow rate (m<sup>3</sup>/sec) specified for VAV ADU. This is autosizable.
-
-#### Field: Zone Minimum Air Flow Method
-
-This field is used to select how the program will determine the minimum flow rate to the zone while the system is operating.  The minimum flow rate is modeled as a fraction of the maximum flow rate.  There are five choices:  Constant, FixedFlowRate, Scheduled, Sum and Maximum.  If Constant is entered, then the program will use the value for minimum flow fraction entered in the following field.  If FixedFlowRate is entered, then the program will use the value for minimum flow rate entered in the field below called Fixed Minimum Air Flow Rate.If Scheduled is entered, then the program will obtain the value for minimum flow fraction from the schedule named in the field below called Minimum Air Flow Fraction Schedule Name. Sum and Maximum are used to either provide the summation of all “entered� inputs or the maximum of all “entered� inputs.
-
-#### Field: Constant Minimum Air Flow Fraction
-
-The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. This field is only used if the Zone Minimum Air Flow Method field is set to Constant.
-
-#### Field: Fixed Minimum Air Flow Rate
-
-The minimum flow rate to the zone while the system is operating, specified as a fixed minimum air flow rate in meters cubed per second. The minimum air flow rate is normally specified to meet the minimum ventilation requirement for the occupants. This field is only used if the Zone Minimum Air Flow Method field is set to FixedFlowRate.
-
-#### Field: Minimum Air Flow Fraction Schedule Name
-
-The name of a schedule that determines the value of the minimum air flow fraction.  The schedule should contain fractions from 0.0 to 1.0.  These values will define the minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. This field is only used if the Zone Minimum Air Flow Method field is set to Scheduled.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object. When this field is used, the terminal unit will increase flow as needed to meet this outdoor air requirement. If Outdoor Air Flow per Person is non-zero, then the outdoor air requirement will be computed based on the current number of occupants in the zone. At no time will the supply air flow rate exceed the value for Maximum Air Flow Rate. If this field is blank, then the terminal unit will not be controlled for outdoor air flow. See documentation for the zone HVAC outdoor air object for further information (Ref DesignSpecification:OutdoorAir).
-
-An IDF example:
-
-```idf
-  AirTerminal:SingleDuct:VAV:NoReheat,
-    Zone 1 VAV System,       !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    Zone 1 Reheat Air Outlet Node,  !- Air Outlet Node Name
-    Zone 1 Damper Inlet Node,!- Air Inlet Node Name
-    0.47,                    !- Maximum Air Flow Rate {m3/s}
-    Constant,                !- Zone Minimum Air Flow Input Method
-    0.3,                     !- Constant Minimum Air Flow Fraction
-    ,                        !- Fixed Minimum Air Flow Rate
-    ,                        !- Minimum Air Flow Fraction Schedule Name
-    ZoneOAData;              !- Design Specification Outdoor Air Object Name
-
-  DesignSpecification:OutdoorAir,
-    ZoneOAData,            !- Name
-    Sum,                   !- Outdoor Air Method
-    0.00236,               !- Outdoor Air Flow per Person {m3/s}
-    0.00305,               !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    ,                      !- Outdoor Air Flow per Zone {m3/s}
-    ,                      !- Outdoor Air Flow Air Changes per Hour
-    OARequirements Sched;  !- Outdoor Air Flow Rate Fraction Schedule Name
-
-Schedule:Compact,
-    OARequirements Sched,    !- Name
-    Any Number,              !- Schedule Type Limits Name
-    Through: 12/31,          !- Field 1
-    For: Weekdays SummerDesignDay WinterDesignDay,  !- Field 2
-    Until: 24:00, 1.0,       !- Field 4
-    For: AllOtherDays,       !- Field 5
-    Until: 24:00, 0.5;       !- Field 7
-```
-
-
-### Single Duct VAV NoReheat AirTerminal Outputs
-
-* HVAC,Average,Zone Air Terminal VAV Damper Position []
-
-* HVAC,Average,Zone Air Terminal Outdoor Air Volume Flow Rate [m3/s]
-
-#### Zone Air Terminal VAV Damper Position []
-
-This output is the damper position required to meet the zone load. This is the average value over the simulation timestep being reported. The damper position is defined as the terminal unit air mass flow rate divided by the terminal unit’s maximum air mass flow rate.
-
-#### Zone Air Terminal Outdoor Air Volume Flow Rate [m3/s]
-
-This output is the amount of outdoor air entering the zone. This is the average value over the frequency being reported.  The amount of outdoor air is defined as the terminal unit air volume flow rate multiplied by the fraction of outdoor air entering the air loop’s outside air system.
-
-### AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat
-
-Variable air volume (VAV) systems typically control the dry-bulb temperature inside a zone by varying the supply air volume instead of the supply air temperature (ref: AirTerminal:SingleDuct:VAV:NoReheat). Reheat coils may be required to avoid overcooling (ref: AirTerminal:SingleDuct:VAV:Reheat).
-
-This terminal unit is slightly different from the AirTerminal:SingleDuct:VAV:NoReheat terminal unit. Both operate the same in cooling mode: the damper opens as needed to provide additional sensible cooling to the zone. The difference between the two is in heating mode. For the Single Duct VAV NoReheat terminal unit, the air flow rate is reduced to the minimum value (max air flow rate x zone minimum air flow fraction) when zone heating is required. For the AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat terminal unit, the air flow rate in heating mode is increased to meet higher zone heating loads (similar to what is done in cooling mode).
-
-This terminal unit model was originally developed and tested for use with the changeover-bypass VAV unitary system..This object may be used when the central heating coil is sufficient to maintain the heating set point temperature. Additional heating may be provided, if necessary, by use of AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat or ZoneHVAC:Baseboard:\* objects.
-
-![Damper\_NoHeat](media/image268.png)
-
-Figure 105. Single Duct VAV Heat and Cool NoReheat Schematic
-
-#### Field: Name
-
-Unique user-defined name for this Air Distribution Unit (ADU).
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether or not this component is available to operate during a given time period. If a schedule value is greater than zero then the system is available to operate; otherwise, the system is unavailable for that time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Outlet Node Name
-
-This alpha field defines the name of the VAV damper air outlet node.
-
-#### Field: Air Inlet Node Name
-
-This alpha field defines the name of the air inlet node that connects the air splitter to the individual zone ADU.
-
-#### Field: Maximum Air Flow Rate
-
-This numeric field defines the design maximum volume flow rate (m<sup>3</sup>/sec) specified for this VAV ADU. This flow rate must be greater than 0 or can be autosized.
-
-#### Field: Zone Minimum Air Flow Fraction
-
-This numeric field defines the minimum air volume flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. This value must be between 0 and 1.
-
-An IDF example is provided below:
-
-```idf
-AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat,
-    Zone 3 VAV System,       !- Name of System
-    FanAndCoilAvailSched,    !- System Availability schedule
-    Zone 3 Reheat Air Outlet Node,  !- UNIT Air Outlet Node
-    Zone 3 VAV Inlet Node,   !- UNIT Air Inlet Node
-    0.584,                   !- Maximum air flow rate {m3/s}
-    0.25;                    !- Zone Minimum Air Flow Fraction
-```
-
-### Single Duct VAV Heat and Cool NoReheat AirTerminal Outputs
-
-HVAC,Average,Zone Air Terminal VAV Damper Position []
-
-#### Zone Air Terminal VAV Damper Position []
-
-This output is the damper position required to meet the zone load. This is the average value over the simulation timestep being reported. The damper position is defined as the terminal unit air mass flow rate divided by the terminal unit’s maximum air mass flow rate.
-
-### AirTerminal:SingleDuct:SeriesPIU:Reheat
-
-The series powered induction unit is an air system terminal unit that mixes varying amounts of secondary (recirculated) air and primary (conditioned supply) air to produce a fixed flow of air to a zone. The unit contains a small fan that acts to induce the secondary air and a heating coil for heating the mixed secondary and primary air. The fan runs at a constant volume flow rate whenever the unit is on (and the fan’s availability schedule is on or it is activated by an availability manager). The fan is downstream of the primary and secondary air inlets. The variable mixing is accomplished by a damper in the unit’s primary air supply inlet duct. This damper can move from fully open (100% primary air. 0% secondary air) to a minimum stop that is specified in the input description. At full cooling the damper will be fully open. At minimum cooling and for heating the damper will be at the minimum stop and the secondary air flow will be at its maximum.
-
-The EnergyPlus model of the series PIU terminal unit is composed of three components: a zone mixer, a constant volume fan, and a heating coil (hot water, electric, or gas).
-
-![SeriesPIUPicture.png](media/image269.png)
-
-Figure 106. Series PIU Terminal Unit
-
-#### Field: Name
-
-A unique user assigned name for a particular series powered induction terminal unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Maximum Air Flow Rate
-
-The maximum volumetric air flow rate through the unit in cubic meters per second. Since this is a constant air volume unit, this is also the design, rated air flow rate of the unit.
-
-#### Field: Maximum Primary Air Flow Rate
-
-The maximum volumetric air flow rate of primary air through the unit in cubic meters per second. This is the primary air flow rate at full cooling load when the primary air damper is fully open. Usually this quantity is the same as the total unit flow rate, but it can be less.
-
-#### Field: Minimum Primary Air Flow Fraction
-
-The minimum volumetric air flow rate of primary air through the unit expressed as a fraction of the maximum volumetric air flow rate of primary air. This input can be 0.0.
-
-#### Field: Supply Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its primary or supply air
-
-#### Field: Secondary Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its secondary or recirculated air. The unit can draw secondary air from its conditioned zone directly or from a return air plenum. Thus this node should be one of the zones exhaust air nodes (see *Zone Air Exhaust Node* in **ZoneHVAC:EquipmentConnections**) or an induced air node outlet of a return plenum (see *Induced Air Outlet Node* in **AirLoopHVAC:ReturnPlenum**).
-
-#### Field: Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its outlet air. This should be one of the inlet air nodes of the zone which is being served.
-
-#### Field: Reheat Coil Air Inlet Node Name
-
-The name of the HVAC system node which is the inlet node of the unit’s heating coil. This is also the outlet node of the unit’s fan.
-
-#### Field: Zone Mixer Name
-
-The name of an zone mixer component (object: AirLoopHVAC:ZoneMixer) which composes part of the unit. Note that some of the input for the mixer will duplicate input fields of the powered induction unit. One of the zone mixer inlet nodes should be the same as the supply air inlet node of the PIU; the other inlet node of the zone mixer should be the same as the secondary air inlet node of the PIU. The outlet node of the zone mixer should be the same as the inlet node of the PIU fan.
-
-#### Field: Fan Name
-
-The name of a fan component which composes part of the unit. Note that the fan’s maximum flow rate should be the same as the maximum air flow rate of the PIU and the type of fan object must be Fan:ConstantVolume. The fan’s inlet node should be the same as the zone mixer’s outlet node. The fan’s outlet node should be the same as the heating coil’s air inlet node. The secondary fan will run according to the Availability Schedule specified in the Fan:ConstantVolume object, unless it is overridden by an availability manager (ref. AvailabilityManager:NightCycle and others).
-
-#### Field: Reheat Coil Object Type
-
-The type of coil in the PIU. The valid choices are:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Steam
-
-In other words the PIU may have a hot water, gas, electric or steam reheat coil.
-
-#### Field: Reheat Coil Name
-
-The name of the heating coil component which composes part of the unit. Note that the heating coil’s air inlet node is the same as the fan outlet node and the heating coil’s air outlet node is the same as the PIU outlet node.
-
-#### Field: Maximum Hot Water or Steam Flow Rate
-
-The maximum hot water volumetric flow rate in m<sup>3</sup>/sec through the unit’s heating coil. If the heating coil is gas or electric this field should be blank.
-
-#### Field: Minimum Hot Water or Steam Flow Rate
-
-The minimum hot water volumetric flow rate in m<sup>3</sup>/sec through the unit’s heating coil. If the heating coil is gas or electric this field should be blank.
-
-#### Field: Convergence Tolerance
-
-The control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {{Q_{PIU,out}} - {Q_{zone\;load}}} \right|}}{{{Q_{zone\;load}}}} \le ConvergenceTolerance\]</div>
-
-For gas or electric heating coils, this input should be left blank. The default is 0.001.
-
-An IDF example:
-
-```idf
-AirTerminal:SingleDuct:SeriesPIU:Reheat,
-          Zone 1 SPIU ATU,          ! Name of air terminal unit
-          FanAndCoilAvailSched,     ! Availability schedule for series PIU ATU
-          0.47,                     ! Total volume flow rate through ATU
-          0.47,                     ! Maximum primary air flow rate through terminal unit
-          0.3,                      ! Minimum primary air flow rate (fraction of max)
-          Zone 1 PIU Pri Air Inlet Node,   ! Air Terminal unit supply air inlet node
-          Zone 1 PIU Sec Air Inlet Node,   ! Air Terminal unit secondary air inlet node
-          Zone 1 PIU Air Outlet Node,      ! Air Terminal unit outlet node
-          Zone 1 Reheat Air Inlet Node,    ! Reheat coil air inlet node (fan outlet node)
-          Zone 1 PIU Mixer,                ! Air terminal unit mixer name
-          Zone 1 PIU Fan,                  ! Air terminal unit fan name
-          COIL:Heating:Water,              ! type of air terminal unit reheat coil
-          Reheat Coil Zone 1,              ! name of air terminal unit reheat coil
-          0.0013,                          ! Max Reheat Water Flow {Flow: m3/sec}
-          0.0,                             ! Min Reheat Water Flow {Flow: m3/sec}
-          0.001;                           ! Convergence tolerance
-```
-
-
-### Single Duct Series PIU Reheat AirTerminal Outputs
-
-* HVAC,Average,Zone Air Terminal Heating Rate [W]
-
-* HVAC,Sum,Zone Air Terminal Heating Energy [J]
-
-* HVAC,Average,Zone Air Terminal Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Air Terminal Sensible Cooling Energy [J]
-
-#### Zone Air Terminal Heating Rate [W]
-
-This field reports the dry air heating addition rate of the series PIU terminal unit to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the terminal unit.
-
-#### Zone Air Terminal Heating Energy [J]
-
-This field reports the dry air heat addition of the series PIU terminal unit  to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the terminal unit, and the timestep.
-
-#### Zone Air Terminal Sensible Cooling Rate [W]
-
-This field reports the dry air sensible heat extraction rate of the series PIU terminal unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the terminal unit.
-
-#### Zone Air Terminal Sensible Cooling Energy [J]
-
-This field reports the dry air sensible heat extraction of the series PIU terminal unit from the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the terminal unit, and the timestep.
-
-### AirTerminal:SingleDuct:ParallelPIU:Reheat
-
-The parallel powered induction unit is an air system terminal unit that mixes varying amounts of secondary (recirculated) air and primary (conditioned supply) air to produce a variable total flow of air to a zone. The unit contains a small fan that acts to induce the secondary air and a heating coil for heating the mixed secondary and primary air. The secondary and primary air streams enter the unit in parallel. The fan sits in the secondary air stream and runs only when the primary air flow is below the Fan On Flow Fraction and the fan’s availability schedule is on or it is activated by an availability manager. The primary air inlet contains a damper that can move from fully open (maximum primary air) to a minimum stop (minimum primary air).
-
-At full cooling load the primary air damper is fully open and the fan is off. The primary air flow is at maximum and there is little or no secondary air flow. As the cooling load decreases, the primary air damper gradually closes and the secondary air flow remains close to zero. At some point, usually when the primary air flow has reached the minimum, the fan switches on and secondary air is induced. The heating coil will switch on as needed to meet any heating demand.
-
-The EnergyPlus model of the parallel PIU terminal unit is composed of three components: a constant volume fan, a zone mixer, and a heating coil (hot water, electric, or gas).
-
-![ParallelPIUPicture.png](media/image271.png)
-
-Figure 107. Parallel PIU Terminal Unit
-
-#### Field: Name
-
-A unique user assigned name for a particular  parallel powered induction terminal unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Maximum Primary Air Flow Rate
-
-The maximum volumetric air flow rate of primary air through the unit in cubic meters per second. This is the primary air flow rate at full cooling load when the primary air damper is fully open.
-
-#### Field: Maximum Secondary Air Flow Rate
-
-The maximum volumetric air flow rate of secondary air through the unit in cubic meters per second. This flow rate can be any amount but is commonly less than the maximum primary air flow rate.
-
-#### Field: Minimum Primary Air Flow Fraction
-
-The minimum volumetric air flow rate of primary air through the unit expressed as a fraction of the maximum volumetric air flow rate of primary air. This input can be 0.0.
-
-#### Field: Fan On Flow Fraction
-
-The fraction of the primary air flow at which fan turns on. In the parallel PIU the fan operation is intermittent. If the primary air flow is above this fraction of the maximum, the fan is off. Otherwise the secondary fan will run according to the Availability Schedule specified in the Fan:ConstantVolume object (see Fan Name below), unless it is overridden by an availability manager (ref. AvailabilityManager:NightCycle and others).
-
-#### Field: Supply Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its primary or supply air
-
-#### Field: Secondary Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its secondary or recirculated air. The unit can draw secondary air from its conditioned zone directly or from a return air plenum. Thus this node should be one of the zones exhaust air nodes (see *Zone Air Exhaust Node* in **ZoneHVAC:EquipmentConnections**) or an induced air node outlet of a return plenum (see *Induced Air Outlet Node* in **AirLoopHVAC:ReturnPlenum**).
-
-#### Field: Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its outlet air. This should be one of the inlet air nodes of the zone which is being served.
-
-#### Field: Reheat Coil Air Inlet Node Name
-
-The name of the HVAC system node which is the inlet node of the unit’s heating coil. This is also the outlet node of the unit’s zone mixer.
-
-#### Field: Zone Mixer Name
-
-The name of an zone mixer component (object: AirLoopHVAC:ZoneMixer) which composes part of the unit. Note that some of the input for the mixer will duplicate input fields of the powered induction unit. One of the zone mixer inlet nodes should be the same as the supply air inlet node of the PIU; the other inlet node of the zone mixer should be the same as the air outlet node of the fan. The outlet node of the zone mixer should be the same as the inlet node of the heating coil.
-
-#### Field: Fan Name
-
-The name of a fan component which composes part of the unit. Note that the fan’s maximum flow rate should be the same as the maximum secondary air flow rate of the PIU and the type of fan object must be Fan:ConstantVolume. The fan’s inlet node should be the same as the PIU secondary air inlet node. The fan’s outlet node should be the same as one of the zone mixer’s inlet nodes. When the primary air flow is below the Fan On Flow Fraction (above), the secondary fan will run according to the Availability Schedule specified in the Fan:ConstantVolume object, unless it is overridden by an availability manager (ref. AvailabilityManager:NightCycle and others).
-
-#### Field: Reheat Coil Object Type
-
-The type of coil in the PIU. The valid choices are:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Steam
-
-In other words the PIU may have a hot water, gas, electric or steam reheat coil.
-
-#### Field: Reheat Coil Name
-
-The name of the heating coil component which composes part of the unit. Note that the heating coil’s air inlet node is the same as the zone mixer’s outlet node and the heating coil’s air outlet node is the same as the PIU outlet node.
-
-#### Field: Maximum Hot Water or Steam Flow Rate
-
-The maximum hot water or steam volumetric flow rate in m<sup>3</sup>/s through the unit’s heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. If the heating coil is gas or electric this field should be blank.
-
-#### Field: Minimum Hot Water or Steam Flow Rate
-
-The minimum hot water or steam volumetric flow rate in m<sup>3</sup>/s through the unit’s heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. If the heating coil is gas or electric this field should be blank.
-
-#### Field: Convergence Tolerance
-
-The control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {{Q_{PIU,out}} - {Q_{zone\;load}}} \right|}}{{{Q_{zone\;load}}}} \le ConvergenceTolerance\]</div>
-
-For gas or electric heating coils, this input should be left blank. The default is 0.001.
-
-An IDF example:
-
-```idf
-AirTerminal:SingleDuct:ParallelPIU:Reheat,
-          Zone 3 PPIU ATU,          ! Name of air terminal unit
-          FanAndCoilAvailSched,     ! Availability schedule for series PIU ATU
-          0.47,                     ! Maximum primary air flow rate through terminal unit
-          0.375,                    ! Maximum secondary air flow rate through the terminal unit
-          0.1,                      ! Minimum primary air flow rate (fraction of max)
-          0.1,                      ! fan on flow fraction
-          Zone 3 PIU Pri Air Inlet Node,   ! Air Terminal unit supply air inlet node
-          Zone 3 PIU Sec Air Inlet Node,   ! Air Terminal unit secondary air inlet node
-          Zone 3 PIU Air Outlet Node,      ! Air Terminal unit outlet node
-          Zone 3 Reheat Air Inlet Node,    ! Reheat coil air inlet node (fan outlet node)
-          Zone 3 PIU Mixer,                ! Air terminal unit mixer name
-          Zone 3 PIU Fan,                  ! Air terminal unit fan name
-          Coil:Heating:Water,              ! type of air terminal unit reheat coil
-          Reheat Coil Zone 3,              ! name of air terminal unit reheat coil
-          0.0013,                          ! Max Reheat Water Flow {Flow: m3/sec}
-          0.0,                             ! Min Reheat Water Flow {Flow: m3/sec}
-          0.001;                           ! Convergence tolerance
-```
-
-
-### Single Duct Parallel PIU Reheat AirTerminal Outputs
-
-* HVAC,Average,Zone Air Terminal Heating Rate [W]
-
-* HVAC,Sum,Zone Air Terminal Heating Energy [J]
-
-* HVAC,Average,Zone Air Terminal Sensible Cooling Rate [W]
-
-* HVAC,Sum, Zone Air Terminal Sensible Cooling Energy [J]
-
-#### Zone Air Terminal Heating Rate [W]
-
-This field reports the dry air heating addition rate of the parallel PIU terminal unit to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the terminal unit.
-
-#### Zone Air Terminal Heating Energy [J]
-
-This field reports the dry air heat addition of the parallel PIU terminal unit  to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the terminal unit, and the timestep.
-
-#### Zone Air Terminal Sensible Cooling Rate [W]
-
-This field reports the sensible heat extraction rate of the parallel PIU terminal unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the terminal unit.
-
-#### Zone Air Terminal Sensible Cooling Energy [J]
-
-This field reports the dry air sensible heat extraction of the parallel PIU terminal unit from the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the terminal unit, and the timestep.
-
-### AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction
-
-The four pipe induction terminal unit provides local hot water heating or chilled water cooling of induced zone air which then mixes with centrally conditioned supply air. An air conditioning system consisting of these terminal units is effectively a mixed cental air / local hydronic system. The centrally conditioned air supplied to the induction terminal units is constant volume at quite high pressure. The central air is discharged through a nozzle in the terminal unit, inducing a flow of room air over a hydronic heating/cooling coil. The coil is connected either to a single inlet and outlet pipe (2 pipe unit) or to 2 inlets and 2 outlets (4 pipe unit). The heated or cooled induced air mixes with the centrally conditioned air before being discharged into the zone. The terminal units are usually expected to do only sensible cooling – any dehumidification is done by the central air conditioning system.
-
-The EnergyPlus model of the four pipe induction terminal unit is a compound component consisting of a hot water heating coil, a chilled water cooling coil, and an air mixer. The unit has two inlet air streams: the centrally conditioned supply air and the induced air from the zone. The induced air passes first through the heating coil, then through the cooling coil and finally through the mixer. The central supply air goes directly into the mixer. The water flow through the hot or cold water coil is varied to meet the zone air conditioning requirement. Note that EnergyPlus models the four pipe induction terminal unit as having separate heating and cooling coils whereas real units have only a single coil used for both heating and cooling. Note also that the four pipe induction unit model can be used to model a two pipe unit by simply adjusting the heating and cooling coil schedules so that the heating coil is off when the cooling coil is on and vice versa.
-
-#### Field: Name
-
-A unique user assigned name for a particular  four pipe induction terminal unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Maximum Total Air Flow Rate
-
-The maximum volumetric air flow rate discharged from the unit in cubic meters per second. Since this is a constant air volume unit, this is also the design, rated air flow rate of the unit. Note that this is the total discharge flow rate – including both central supply and induced air.
-
-#### Field: Induction Ratio
-
-The ratio of induced air flow rate to primary supply air flow rate. The default is 2.5 the supply air induces zone air flow at 2.5 times the primary supply air flow rate.
-
-#### Field: Supply Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its primary or supply air
-
-#### Field: Induced Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its secondary or recirculated air. This should be the same node as one of the zone exhaust nodes.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its outlet air. This should be one of the inlet air nodes of the zone which is being served.
-
-#### Field: Heating Coil Object Type
-
-The type of heating coil in the terminal unit. The choices are:
-
-* Coil:Heating:Water
-
-In other words the unit may have a hot water coil only.
-
-#### Field: Heating Coil Name
-
-The name of the heating coil component which composes part of the unit. Note that the heating coil’s air inlet node is the same as the terminal unit’s induced air inlet node. The heating coil’s air outlet node is the same as the cooling coil’s air inlet node.
-
-#### Field: Maximum Hot Water Flow Rate
-
-The maximum hot water volumetric flow rate in m<sup>3</sup>/sec through the unit’s heating coil.
-
-#### Field: Minimum Hot Water Flow Rate
-
-The minimum hot water volumetric flow rate in m<sup>3</sup>/sec through the unit’s heating coil.
-
-#### Field: Heating Convergence Tolerance
-
-The control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. The model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {{Q_{unit,out}} - {Q_{zone\;load}}} \right|}}{{{Q_{zone\;load}}}} \le ConvergenceTolerance\]</div>
-
-The default is 0.001.
-
-#### Field: Cooling Coil Object Type
-
-The type of cooling coil in the terminal unit. The choices are:
-
-* Coil:Cooling:Water
-
-* Coil:Cooling:Water:DetailedGeometry
-
-In other words the unit must use only the water cooling coils.
-
-#### Field: Cooling Coil Name
-
-The name of the cooling coil component which composes part of the unit. Note that the cooling coil’s air inlet node is the same as the heating coil’s air outlet node. The cooling coil’s air outlet node is the same as one of the zone mixer’s inlets.
-
-#### Field: Maximum Cold Water Flow Rate
-
-The maximum cold water volumetric flow rate in m<sup>3</sup>/sec through the unit’s cooling coil.
-
-#### Field: Minimum Cold Water Flow Rate
-
-The minimum cold water volumetric flow rate in m<sup>3</sup>/sec through the unit’s cooling coil.
-
-#### Field: Cooling Convergence Tolerance
-
-The control tolerance for the unit cooling output. The unit is controlled by matching the unit output to the zone demand. The model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {{Q_{unit,out}} - {Q_{zone\;load}}} \right|}}{{{Q_{zone\;load}}}} \le ConvergenceTolerance\]</div>
-
-The default is 0.001.
-
-#### Field: Zone Mixer Name
-
-The name of an zone mixer component (object: AirLoopHVAC:ZoneMixer) which composes part of the terminal unit. Note that some of the zone mixer’s inputs will duplicate some of the terminal units’s inputs. One of the zone mixer inlet nodes should be the same as the supply air inlet node of the terminal unit; the other inlet node of the zone mixer should be the same as the cooling coil air outlet node. The outlet node of the zone mixer should be the same as the outlet node of the terminal unit.
-
-An IDF example:
-
-```idf
-AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction,
-    SPACE2-1 FPIU,            !- Name of System
-    ReheatCoilAvailSched,     !- System Availability schedule
-    autosize,                 !- Maximum total air volume flow rate
-    1.0,                      !- Induction ratio
-    SPACE2-1 ATU Supply Node, !- Terminal unit supply air inlet node
-    SPACE2-1 ATU Induc Node,  !- Terminal unit induced air inlet node
-    SPACE2-1 In Node,         !- Terminal unit air outlet node
-    COIL:Heating:Water,       !- Heating coil object
-    SPACE2-1 HW Coil,         !- Heating coil name
-    autosize,                 !- Max hot water flow
-    0.0,                      !- Min hot water flow
-    0.001,                    !- Heating Convergence Tolerance
-    COIL:Cooling:Water,       !- Cooling coil object
-    SPACE2-1 CW Coil,         !- Cooling coil name
-    autosize,                 !- Max cold water flow
-    0.0,                      !- Min cold water flow
-    0.001,                    !- Cooling Convergence Tolerance
-    SPACE2-1 ATU Mixer;       !- Zone mixer component name
-
-COIL:Heating:Water,
-    SPACE2-1 HW Coil,        !- Coil Name
-    ReheatCoilAvailSched,    !- Availability Schedule Name
-    autosize,                !- UA of the Coil {W/K}
-    autosize,                !- Max Water Flow Rate of Coil {m3/s}
-    SPACE2-1 HW Coil Water In Node,  !- Coil_Water_Inlet_Node
-    SPACE2-1 HW Coil Water Out Node, !- Coil_Water_Outlet_Node
-    SPACE2-1 ATU Induc Node, !- Coil_Air_Inlet_Node
-    SPACE2-1 HW Coil Air Out Node;   !- Coil_Air_Outlet_Node
-
-COIL:Cooling:Water,
-    SPACE2-1 CW Coil,        !- Coil Name
-    CWCoilAvailSched,        !- Availability Schedule
-    autosize,                !- UA of the Coil
-    autosize,                !- Max Water Flow Rate of Coil
-    ,                        !- Leaving Relative Humidity of Coil
-    SPACE2-1 CW Coil Water In Node,  !- Coil_Water_Inlet_Node
-    SPACE2-1 CW Coil Water Out Node, !- Coil_Water_Outlet_Node
-    SPACE2-1 HW Coil Air Out Node,   !- Coil_Air_Inlet_Node
-    SPACE2-1 CW Coil Air Out Node;   !- Coil_Air_Outlet_Node
-
-AirLoopHVAC:ZoneMixer,
-    SPACE2-1 ATU Mixer,              !- Mixer Name
-    SPACE2-1 In Node,                !- Outlet_Node
-    SPACE2-1 ATU Supply Node,        !- Inlet_Node_1
-    SPACE2-1 CW Coil Air Out Node;   !- Inlet_Node_2
-```
-
-### Single Duct Constant Volume Four Pipe Induction AirTerminal Outputs
-
-There are no specific outputs for the four pipe induction terminal units.
-
-### AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam
-
-The four-pipe beam air terminal system is a mixed air-hydronic system. A central, single-duct forced-air system that supplies conditioned air to the zones. Chilled water circulates through ceiling-mounted fin-tube convector units to provide sensible cooling. Hot water circulates through the same convectors to provide heating.  Water flow rate through the beam unit is varied to meet the zone sensible cooling or heating load. Any dehumidification is done by the central forced-air system. Thermodynamically, the cooled beam system resembles the four-pipe induction unit (**AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction**).
-
-To model a typical four-pipe beam system the user will need to define a conventional central constant volume forced air system in order to deliver primary air to the beam. This central system (usually) provides outside air for ventilation.  Primary air is normally delivered at a fixed temperature but could be reset by a schedule or using an outdoor air reset setpoint manager. On the supply side of this air loop there will be the usual central conditioning equipment: outside air mixer, fan, heating and cooling coil. On the zone equipment (demand) side of the loop, the four-pipe beams will be represented as air terminal units. Because the four-pipe beam can provide heating the system can avoid over-cooling zones during times of low load with cool primary air temperatures, similar to the action of a reheat coil in a VAV terminal.  Therefore it is not necessary to have additional zone equipment (such as baseboard heaters) to handle heating (or reheating) loads.
-
-Although the four-pipe beam equipment in a zone is treated by the program as a single terminal unit, the actual installation will often have multiple beam units in each zone. In this model, it is only the total length of all the beams and the total air flow of all the units that are described, not the number of individual beam units.
-
-If needed, the program (in its sizing calculation for the system) determines the total length of beams and primary supply air flow that is needed to meet the zone design loads. The four pipe beam air terminal sizing differs from other air terminals in that the primary supply air flow rate is sized using the entire performance model and the flow rate is not the direct result from the Sizing:Zone and Sizing:System calculations. The flow rates will be somewhere between what an air terminal would size out using *VentilationRequirement* or *Sensible* in the Sizing:System object (either setting can be used).
-
-The model includes two different types of inputs for flow rates, “design� and “rated … per-meter.�  The design values are the actual sizes of the flow rates as viewed from the zone and central air handler (but before zone multipliers).  The design values include all the individual beam units and their lengths.  The rated per-meter values are used to characterize product performance at nominal rating conditions in such a way that it can be scaled to match the size of a zone.  The performance characteristics at the rating point are not fixed in the program and can be entered by the user when they differ from default values.  The rated per meter values are normalized by the linear dimensions of the beam and are generally obtained from product catalog data by dividing by the length of the beam.  The rated primary air flow rate is assumed to be for sea level conditions while the design primary air flow rate is modeled for the location elevation above sea level.
-
-#### Field: Name
-A unique user-assigned name for a particular beam unit. Any reference to this unit by another object will use this name.
-
-#### Field: Primary Air Availability Schedule Name
-The name of the schedule that denotes whether the terminal unit is operating to provide primary air during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit is on and requesting primary air flow during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Cooling Availability Schedule Name
-The name of the schedule that denotes whether the terminal unit is operating to provide cooling during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit is on and available for beam cooling during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods. The primary air availability schedule named in the previous input field must have a value that is “on� during times that cooling is available.
-
-#### Field: Heating Availability Schedule Name
-The name of the schedule that denotes whether the terminal unit can operate to provide heating during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit is on and available for beam heating during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods. The primary air availability schedule named in the input field above must have a value that is “on� during times that heating is available.
-
-#### Field: Primary Air Inlet Node Name
-The name of the HVAC system air node from which the unit draws its primary air.
-
-#### Field: Primary Air Outlet Node Name
-The name of the HVAC system air node that connects this terminal unit to the zone. The will be the same as one of the zone inlet nodes.
-
-#### Field: Chilled Water Inlet Node Name
-The name of the chilled water inlet node.  If desired, the chilled water node connections can be omitted and the model will assume the intent is to model a two-pipe heating only beam.
-
-#### Field: Chilled Water Outlet Node Name
-The name of the chilled water outlet node.
-
-#### Field: Design Primary Air Volume Flow Rate
-This is the air flow rate (m3/s) of the primary air entering the air terminal unit from the central air handling unit. This input can be autosized.
-
-#### Field: Design Chilled Water Volume Flow Rate
-The maximum chilled water flow rate (m3/s) for the unit(s) serving the entire zone. This input can be autosized based on the zone design load.
-
-#### Field: Design Hot Water Volume Flow Rate
-The maximum hot water flow rate (m3/s) for the unit(s) serving the entire zone. This input can be autosized based on the zone design load.
-
-#### Field: Zone Total Beam Length (m)
-The total length of all the beams in the zone (m). The real spaces may actually have a number of individual beam units of a specific length and this is the length of individual beams times the total number of beams in the thermal zone. It need not be an even multiple of actual unit’s beam length but it can be if desired. This field is autosizable.
-
-#### Field: Rated Primary Air Flow Rate per Beam Length (m3/s-m)
-This is the primary air volume flow rate at rating conditions divided by the length of the beam, in m3/s-m.  This "catalog" value for volume flow rate input is converted to a mass flow rate using standard air density at sea level. This value will be used for sizing the design primary air volume flow rate if the total beam length is not also autosized. The default is 0.035 m3/s-m.
-
-#### Field: Beam Rated Cooling Capacity per Beam Length (W/m)
-This is the beam cooling capacity at rating conditions divided by the length of the beam, in W/m.  This is only the cooling contributed by the chilled water circulating through the convector and is separate from any cooling (or heating) that may also be provided by the primary air. The default is 600 W/m.
-
-#### Field: Beam Rated Cooling Room Air Chilled Water Temperature Difference (Delta C)
-This input defines the value of the temperature difference between the room air and entering chilled water at the rating point, in delta Celsius.  This "catalog" input helps to define the operating conditions that correspond with Rated Beam Cooling Capacity per Meter. It is used to normalize the independent variable in the input field called Beam Cooling Capacity Temperature Difference Modification Factor Curve or Table Name. The default is 10.0 delta C.
-
-#### Field: Beam Rated Chilled Water Volume Flow Rate per Beam Length (m3/s-m)
-This input defines the value of the chilled water flow rate per meter length of beam at the rating point, in m3/s-m.  This input helps to define the operating conditions that correspond with Rated Beam Cooling Capacity per Meter. It is used to normalize the independent variable in the input field called Beam Cooling Capacity Chilled Water Flow Modification Factor Curve or Table Name.  The default is 0.00005 m3/s-m.
-
-#### Field: Beam Cooling Capacity Temperature Difference Modification Factor Curve Name
-This field is the name of a curve or table object that describes how the beam convector’s cooling capacity varies as a function of the temperature difference between the zone air and the entering chilled water.  The single independent variable is the ratio of the current simulation results for the difference between the air and entering water and the difference at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the cooling capacity.
-
-#### Field: Beam Cooling Capacity Air Flow Modification Factor Curve Name
-This field is the name of a curve or table object that describes how the beam convector's cooling capacity varies as a function of the primary air flow rate.  The single independent variable is the ratio of the current primary air flow rate and the primary air flow rate at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the cooling capacity.  The factor is useful to adjust for a range of primary air flow rates that a given product can accommodate.  However since this is a constant volume air terminal, the modification does not typically vary during the simulation and the range of independent variable does not need to be all that broad in practice.
-
-#### Field: Beam Cooling Capacity Chilled Water Flow Modification Factor Curve Name
-This field is the name of a curve or table object that describes how the beam convector’s cooling capacity varies as a function of the water flow rate.  The single independent variable is the ratio of the current fluid flow rate to the fluid flow rate at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the cooling capacity.  The model will adjust the chilled water flow rate to vary cooling power to meet the zone load, so for control purposes, the range of the independent variable must include all the way down to zero flow, with zero capacity at zero flow.
-
-#### Field: Beam Rated Heating Capacity per Beam Length (W/m)
-This is the beam heating capacity at rating conditions divided by the length of the beam, in W/m.  This is only the heating contributed by the hot water circulating through the convector and is separate from any heating (or cooling) that may also be provided by the primary air.  The default is 1.200 W/m.
-
-#### Field: Beam Rated Heating Room Air Hot Water Temperature Difference (Delta C)
-This input defines the value of the temperature difference between the entering hot water and the room air at the rating point, in delta Celsius.  This input helps to define the operating conditions that correspond with Rated Beam Heating Capacity per Meter. It is used to normalize the independent variable in the input field called Beam Heating Capacity Temperature Difference Modification Factor Curve or Table Name. The default is 27.8 delta C.
-
-#### Field: Beam Rated Hot Water Volume Flow Rate per Beam Length (m3/s-m)
-This input defines the value of the hot water flow rate per meter length of beam at the rating point, in m3/s/m, or more strictly m3/s-m.  This input helps to define the operating conditions that correspond with Rated Beam Heating Capacity per Meter.   It is used to normalize the independent variable in the input field called Beam Heating Capacity Hot Water Flow Modification Factor Curve or Table Name.  The default is 0.00005 m3/s-m.
-
-#### Field: Beam Heating Capacity Temperature Difference Modification Factor Curve Name
-This field is the name of a curve or table object that describes how the beam convector’s heating capacity varies as a function of the temperature difference between the entering hot water and the zone air.  The single independent variable is the ratio of the current simulation results for the difference between the water and air and the difference at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the heating capacity.
-
-#### Field: Beam Heating Capacity Air Flow Modification Factor Curve Name
-This field is the name of a curve or table object that describes how the beam convectors heating capacity varies as a function of the primary air flow rate.  The single independent variable is the ratio of the current primary air flow rate and the primary air flow rate at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the heating capacity.  The factor is useful to adjust for a range of primary air rates that a given product can accommodate.  However since this is a constant volume air terminal, the modification does not typically vary during the simulation and the range of independent variable does not need to be all that broad in practice.
-
-#### Field: Beam Heating Capacity Hot Water Flow Modification Factor Curve Name
-This field is the name of a curve or table object that describes how the beam convector’s heating capacity varies as a function of the water flow rate.  The single independent variable is the ratio of the current fluid flow rate to the fluid flow rate at the rating point. The result of the curve or table is multiplied by the rated capacity to adjust the heating capacity.  The model will adjust the hot water flow rate to vary heating power to meet the zone load, so for control purposes, the range of the independent variable must include all the way down to zero flow, with zero capacity at zero flow.
-
-
-An example input follows:
-
-      AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam,
-        Zone One 4pipe Beam, !- Name
-        ALWAYS_ON , !- Primary Air Availability Schedule Name
-        ALWAYS_ON , !- Cooling Availability Schedule Name
-        ALWAYS_ON , !- Heating Availability Schedule Name
-        Zone One 4pipe Beam Inlet Node Name , !- Primary Air Inlet Node Name
-        Zone One 4pipe Beam Outlet Node Name , !- Primary Air Outlet Node Name
-        Zone One 4pipe Beam CW Inlet Node , !- Chilled Water Inlet Node Name
-        Zone One 4pipe Beam CW Outlet Node , !- Chilled Water Outlet Node Name
-        AUTOSIZE , !- Design Primary Air Volume Flow Rate
-        AUTOSIZE , !- Design Chilled Water Volume Flow Rate
-        AUTOSIZE , !- Design Hot Water Volume Flow Rate
-        AUTOSIZE , !- Zone Total Beam Length
-        0.036 , !- Rated Primary Air Flow Rate per Beam Length
-        597 , !- Rated Beam Cooling Capacity per Beam Length
-        10.0 , !- Rated Cooling Room Air Chilled Water Temperature Difference
-        5.2E-5 , !- Rated Chilled Water Volume Flow Rate per Beam Length
-        CapModFuncOfTempDiff, !- Beam Cooling Capacity Temperature Difference Modification Factor Curve or Table Name
-        CoolCapModFuncOfSAFlow, !- Beam Cooling Capacity Air Flow Modification Factor Curve or Table Name
-        CapModFuncOfWaterFlow, !- Beam Cooling Capacity Chilled Water Flow Modification Factor Curve or Table Name
-        1548 , !- Rated Beam Heating Capacity per Beam Length
-        27.8, !- Rated Heating Room Air Hot Water Temperature Difference
-        5.2E-5, !- Rated Hot Water Volume Flow Rate per Beam Length
-        CapModFuncOfTempDiff, !- Beam Heating Capacity Temperature Difference Modification Factor Curve or Table Name
-        HeatCapModFuncOfSAFlow, !- Beam Heating Capacity Air Flow Modification Factor Curve or Table Name
-        CapModFuncOfWaterFlow; !- Beam Heating Capacity Hot Water Flow Modification Factor Curve or Table Name
-
-      Curve:Linear,  ! y = x
-        CapModFuncOfTempDiff, !-Name
-        0, !_ Coef Const
-        1, !- Coef x
-        0,  !- min x
-        1.5, !- max x
-        0.0 , !- min y
-        1.5; ! max y
-
-      Table:OneIndependentVariable,
-        CoolCapModFuncOfSAFlow, !- Name
-        quadratic,!- Curve Type
-        EvaluateCurveToLimits,!- Interpolation Method
-        0.714,!- min x
-        1.2857,!- max x
-        0.8234,!- min y
-        1.1256,!- max y
-        dimensionless, !-
-        dimensionless, !-
-        , !- normalization ref
-        0.714286, 0.823403,
-        1.0,      1.0,
-        1.2857,   1.1256;
-
-      Table:OneIndependentVariable,
-        CapModFuncOfWaterFlow, !- Name
-        quadratic,!- Curve Type
-        EvaluateCurveToLimits,!- Interpolation Method
-        0.0,!- min x
-        1.333333,!- max x
-        0.0,!- min y
-        1.04,!- max y
-        dimensionless, !-
-        dimensionless, !-
-         , !- normalization ref
-        0.0,      0.0,
-        0.05,     0.001,
-        0.33333,  0.71,
-        0.5,      0.85,
-        0.666667, 0.92,
-        0.833333, 0.97,
-        1.0,      1.0,
-        1.333333, 1.04;
-
-      Table:OneIndependentVariable,
-        HeatCapModFuncOfSAFlow, !- Name
-        quadratic,!- Curve Type
-        EvaluateCurveToLimits,!- Interpolation Method
-        0.714,!- min x
-        1.2857,!- max x
-        0.8554,!- min y
-        1.0778,!- max y
-        dimensionless, !-
-        dimensionless, !-
-        , !- normalization ref
-        0.714286, 0.8554,
-        1.0,      1.0,
-        1.2857,   1.0778;
-
-
-### AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam Outputs
-
-#### Zone Air Terminal Beam Sensible Cooling Rate [W]
-#### Zone Air Terminal Beam Sensible Cooling Energy [J]
-These are the sensible cooling power and energy delivered by the beams to the zone, exclusive of any cooling or heating done by the primary air.
-
-#### Zone Air Terminal Beam Sensible Heating Rate [W]
-#### Zone Air Terminal Beam Sensible Heating Energy [J]
-These are the sensible heating power and energy delivered by the beams to the zone, exclusive of any cooling or heating done by the primary air.
-
-#### Zone Air Terminal Primary Air Sensible Cooling Rate [W]
-Sensible cooling by the primary air to the zone, exclusive of any cooling or heating done by the beams.
-
-#### Zone Air Terminal Primary Air Sensible Cooling Energy [J]
-Sensible cooling by the primary air to the zone, exclusive of any cooling or heating done by the beams.
-
-#### Zone Air Terminal Primary Air Sensible Heating Rate [W]
-Heating by the primary air to the zone, exclusive of any cooling or heating done by the beams.
-
-#### Zone Air Terminal Primary Air Sensible Heating Energy [J]
-Heating by the primary air to the zone, exclusive of any cooling or heating done by the beams.
-
-#### Zone Air Terminal Primary Air Flow Rate [m3/s]
-Air flow rate from the central air handler into the zone in m3/s.  Note that this does not include any of the secondary air flow that is induced by the convector and nozzle action (the model does not resolve secondary air flow rate and the result are not available).
-
-
-### AirTerminal:SingleDuct:ConstantVolume:CooledBeam
-
-The Cooled Beam system is a mixed air-hydronic system. A central, single-duct forced-air system supplies conditioned ventilation air to the zones. Sensible cooling is done by chilled water circulating through ceiling mounted cooled beam units. Chilled water flow rate through the cooled beam units is varied to meet the zone sensible cooling load. Any dehumidification is done by the central ventilation air system. Heating is usually accomplished with hot water radiators. Thermodynamically, the cooled beam system resembles the four-pipe induction unit.
-
-To model a typical cooled beam system the user will need to define a conventional central constant volume forced air system. This system will normally be 100% outside air delivered at a fixed supply temperature (which could be reset by schedule or by outside air temperature). On the supply side of this air loop there will be the usual central AC equipment: outside air mixer, fan, heating and cooling coil. On the zone equipment (demand) side of the loop, the chilled beams will be represented as terminal units. Additional zone equipment (such as baseboard heaters) will be needed to handle heating loads.
-
-Although the cooled beam equipment in a zone is treated by the program as a single terminal unit, the actual installation will have multiple beams in each zone. The program (in its sizing calculation for the system) figures out how many beams of what length are needed to meet the zone design load.
-
-#### Field: Name
-
-A unique user assigned name for a particular chilled beam unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Cooled Beam Type
-
-Two types of units are modeled: *Active* or *Passive*. In the active unit, primary air is supplied through the beam, inducing some secondary zone air into contact with the coil. This unit acts as an active convector. The passive unit is simply a passive, finned convector. Primary air is supplied through a normal diffuser.
-
-#### Field: Supply Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its primary or supply air. Note that this field should be specified for both types of unit, even though supply air does not pass through the passive unit.
-
-#### Field: Supply Air Outlet Node Name
-
-The name of the air node that connects this terminal unit to the zone. The will be the same as one of the zone inlet nodes. The name of this node must be entered even if the actual beams are passive and is not actually supplying air to the zone.
-
-#### Field: Chilled Water Inlet Node Name
-
-The name of the chilled water inlet node.
-
-#### Field: Chilled Water Outlet Node Name
-
-The name of the chilled water outlet node.
-
-#### Field: Supply Air Volumetric Flow Rate
-
-This is the air flow rate in cubic meters per second of the supply air entering the zone. This input would normally be autosized based on the ventilation requirement (see Zone Sizing).
-
-#### Field: Maximum Total Chilled Water Volumetric Flow Rate
-
-The maximum chilled water flow rate (in cubic meters per second) for the unit. This input would normally be autosized based on the zone design load.
-
-#### Field: Number of Beams
-
-The number of individual cooled beam units in the zone. Normally this unit would be autocalculated by the program based upon the previous field and the nominal flow rate for a single beam unit (set by the program to 0.07 kg/s).
-
-#### Field: Beam Length
-
-The length of an individual beam in meters. Normally this will be autocalculated by the program based upon the number of beam units and the zone design sensible cooling load. 1 to 4 meters is a typical length range.
-
-#### Field: Design Inlet Water Temperature
-
-The nominal or design inlet water temperature in degrees Celsius. The default is 15°C.
-
-#### Field: Design Outlet Water Temperature
-
-The nominal or design outlet water temperature in degrees Celsius. The default is 17°C.
-
-*The following inputs are parameters used to characterize the performance of the chilled beam units. Values for a given unit can be obtained from the manufacturer. The parameters are used in the following equations.     *
-
-*P<sub>beam</sub>* = *A·K·DT       *                         beam cooling output per unit length W/m
-
-*K=a·DT<sup>n1</sup>·vr<sup>n2</sup>·w<sup>n3</sup>*                            coil heat transfer coefficient W/(m<sup>2</sup>K)
-
-*vr=(q<sub>in</sub>*/a*<sub>0</sub>)·r<sub>air</sub>*                                  room air mass flow rate across coil kg/(m<sup>2</sup>s)
-
-*q<sub>in</sub>=K<sub>1</sub>·DT<sup>n</sup>+K<sub>in</sub>·q<sub>pr</sub>*                 room air volumetric flow rate across coil per
-
-unit length m<sup>3</sup>/(s-m)
-
-DT is the room air –water temperature difference (average water temperature is used) in degrees C.
-
-w is the water velocity in m/s.
-
-q<sub>pr</sub> is the supply air flow rate per unit length m<sup>3</sup>/(s-m)
-
-#### Field: Coil Surface Area per Coil Length
-
-Surface area on the air side of the beam per unit beam length. The units are square meters per meter. The default is 5.422. This is *A* in the above equations.
-
-#### Field: Model Parameter a (a)
-
-This is ain the above equations. The default is 15.3
-
-#### Field: Model Parameter n1
-
-This is n1 in the above equations. The default is 0.
-
-#### Field: Model Parameter n2
-
-This is n2 in the above equations. The default is 0.84.
-
-#### Field: Model Parameter n3
-
-This is n3 in the above equations. The default is 0.12.
-
-#### Field: Model Parameter a<sub>0</sub> (a)
-
-This is a<sub>0</sub> in the above equations. It is the free area of the coil in plan view (for the air flow) per unit beam length. The units are square meters per meter. The default is 0.171.
-
-#### Field: Model Parameter K<sub>1</sub> (K1)
-
-This is K<sub>1</sub> in the above equations. The default is 0.005.
-
-#### Field: Model Parameter n
-
-This is n in the above equations. The default is 0.4.
-
-#### Field: Coefficient of Induction K<sub>in</sub> (Kin)
-
-The coefficient of induction K<sub>in</sub> in the above equations. The default is 2.0 for active beams and 0.0 for passive beams.
-
-#### Field: Pipe Inside Diameter
-
-The water pipe inside diameter in meters. The default is 0.0145.
-
-An example input is:
-
-```idf
-  AirTerminal:SingleDuct:ConstantVolume:CooledBeam,
-    SPACE2-1 CB,             !- Name
-    CWCoilAvailSched,        !- Availability Schedule Name
-    Active,                  !- Cooled Beam Type
-    SPACE2-1 ATU Supply Node,!- Supply Air Inlet Node Name
-    SPACE2-1 In Node,        !- Supply Air Outlet Node Name
-    SPACE2-1 CW Coil Water In Node,  !- Chilled Water Inlet Node Name
-    SPACE2-1 CW Coil Water Out Node, !- Chilled Water Outlet Node Name
-    ,                        !- Supply Air Volumetric Flow Rate
-    ,                   !- Maximum Total Chilled Water Volumetric Flow Rate
-    ,                        !- Number of Beams
-    ,                        !- Beam Length
-    ,                        !- Design Inlet Water Temperature
-    ,                        !- Design Outlet Water temperature
-    ,                        !- Coil Surface Area per Coil Length
-    ,                        !- Model Parameter a
-    ,                        !- Model Parameter n1
-    ,                        !- Model Parameter n2
-   ,                        !- Model Parameter n3
-    ,                        !- Model Parameter a0
-    ,                        !- Model Parameter K1
-    ,                        !- Model Parameter n
-    ,                        !- Coefficient of Induction Kin
-    ;                        !- Leaving Pipe Inside Diameter
-```
-
-
-### Singled Duct Constant Volume Cooled Beam AirTerminal Outputs
-
-* HVAC,Sum,Zone Air Terminal Beam Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Air Terminal Beam Sensible Cooling Rate [W]
-
-* HVAC,Sum, Zone Air Terminal Supply Air Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Air Terminal Supply Air Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Air Terminal Supply Air Sensible Heating Energy [J]
-
-* HVAC,Average,Zone Air Terminal Supply Air Sensible Heating Rate [W]
-
-* HVAC,Sum,Zone Air Terminal Beam Chilled Water Energy [J]
-
-#### Zone Air Terminal Beam Sensible Cooling Rate [W]
-
-Sensible cooling by the beams in the zone, exclusive of any cooling or heating done by the supply air.
-
-#### Zone Air Terminal Beam Sensible Cooling Energy [J]
-
-Sensible cooling by the beams in the zone, exclusive of any cooling or heating done by the supply air.
-
-#### Zone Air Terminal Supply Air Sensible Cooling Rate [W]
-
-Sensible cooling by the supply air to the zone, exclusive of any cooling done by the beams.
-
-#### Zone Air Terminal Supply Air Sensible Cooling Energy [J]
-
-Sensible cooling by the supply air to the zone, exclusive of any cooling done by the beams.
-
-#### Zone Air Terminal Supply Air Sensible Heating Rate [W]
-
-Heating by the supply air to the zone, exclusive of any cooling done by the beams.
-
-#### Zone Air Terminal Supply Air Sensible Heating Energy [J]
-
-Heating by the supply air to the zone, exclusive of any cooling done by the beams.
-
-#### Zone Air Terminal Beam Chilled Water Energy [J]
-
-The heat transfer energy for the chilled water serving the beams, in Joules.
-
-### AirTerminal:SingleDuct:InletSideMixer
-
-The inlet side mixer air terminal unit provides a means of supplying central system air to the air inlet of a zone AC unit such as a four pipe fan coil. Normally the central air would be ventilation air from a dedicated outside air system (DOAS).
-
-The AirTerminal:SingleDuct:InletSideMixer simply mixes two inlet air streams into a single outlet stream. One inlet - designated the primary air stream - is from the DOAS. The other inlet - designated the secondary air stream - is recirculated air from the zone. The outlet air stream of the inlet side mixer is then the inlet to the zone AC unit.
-
-![](media/image275.svg)
-
-Figure 108. Inlet Side Mixer Air Terminal Unit with Fan Coil
-
-#### Field: Name
-
-A unique user assigned name for a particular inlet side mixer terminal unit. Any reference to this unit by another object will use this name.
-
-#### Field: ZoneHVAC Terminal Unit Object Type
-
-The type of zone AC unit to which this terminal unit will be connected. This is a choice field. The choices are ZoneHVAC:FourPipeFanCoil or ZoneHVAC:WaterToAirHeatPump.
-
-#### Field: ZoneHVAC Terminal Unit Name
-
-The name of the zone AC unit to which this terminal will be connected.
-
-#### Field: Terminal Unit Outlet Node Name
-
-The name of the air outlet node of the inlet side mixer. This will be the inlet air node of the zone AC unit.
-
-#### Field: Terminal Unit Primary Air Inlet Node Name
-
-The name of the primary air inlet node of the inlet side mixer. This will be an outlet node of an AirLoopHVAC:ZoneSplitter, providing the connection to the DOAS system.
-
-#### Field: Terminal Unit Secondary Air Inlet Node Name
-
-The name of the secondary air inlet node of the inlet side mixer. This will be an exhaust node of the zone that is being conditioned.
-
-An IDF example:
-
-```idf
-AirTerminal:SingleDuct:InletSideMixer,
-    SPACE2-1 DOAS Air Terminal,  !- Name
-    ZoneHVAC:FourPipeFanCoil,!- ZoneHVAC Terminal Unit Object Type
-    SPACE2-1 Fan Coil,       !- ZoneHVAC Terminal Unit Name
-    SPACE2-1 Fan Coil Inlet, !- Terminal Unit Outlet Node Name
-    SPACE2-1 Air Terminal Mixer Primary Inlet,  !- Terminal Unit Primary Air Inlet Node Name
-    SPACE2-1 Air Terminal Mixer Secondary Inlet;  !- Terminal Unit Secondary Air Inlet Node Name
-```
-
-### AirTerminal:SingleDuct:SupplySideMixer
-
-The supply side mixer air terminal unit provides a means of supplying central system air to the air outlet of a zone AC unit such as a four pipe fan coil. Normally the central air would be ventilation air from a dedicated outside air system (DOAS).
-
-The AirTerminal:SingleDuct:SupplySideMixer simply mixes two inlet air streams into a single outlet stream. One inlet - designated the primary air stream - is from the DOAS. The other inlet - designated the secondary air stream - is outlet air from the zone AC unit. The outlet air stream from the supply side mixer is then the inlet to the conditioned zone.
-
-![](media/image276.svg)
-
-Figure 109. Supply Side Mixer Air Terminal Unit with Fan Coil
-
-#### Field: Name
-
-A unique user assigned name for a particular supply side mixer terminal unit. Any reference to this unit by another object will use this name.
-
-#### Field: ZoneHVAC Terminal Unit Object Type
-
-The type of zone AC unit to which this terminal unit will be connected. This is a choice field. The choices are ZoneHVAC:FourPipeFanCoil or ZoneHVAC:WaterToAirHeatPump.
-
-#### Field: ZoneHVAC Terminal Unit Name
-
-The name of the zone AC unit to which this terminal will be connected.
-
-#### Field: Terminal Unit Outlet Node Name
-
-The name of the air outlet node of the supply side mixer. This will be an inlet air node of the conditioned zone.
-
-#### Field: Terminal Unit Primary Air Inlet Node Name
-
-The name of the primary air inlet node of the supply side mixer. This will be an outlet node of an AirLoopHVAC:ZoneSplitter, providing the connection to the DOAS system.
-
-#### Field: Terminal Unit Secondary Air Inlet Node Name
-
-The name of the secondary air inlet node of the supply side mixer. This will be the outlet air node of the zone AC unit.
-
-An IDF example:
-
-```idf
-AirTerminal:SingleDuct:SupplySideMixer,
-    SPACE1-1 DOAS Air Terminal,  !- Name
-    ZoneHVAC:FourPipeFanCoil,!- ZoneHVAC Terminal Unit Object Type
-    SPACE1-1 Fan Coil,       !- ZoneHVAC Terminal Unit Name
-    SPACE1-1 Supply Inlet,   !- Terminal Unit Outlet Node Name
-    SPACE1-1 Air Terminal Mixer Primary Inlet,  !- Terminal Unit Primary Air Inlet Node Name
-    SPACE1-1 Fan Coil Outlet;!- Terminal Unit Secondary Air Inlet Node Name
-```
-
-### AirTerminal:DualDuct:ConstantVolume
-
-The AirTerminal:DualDuct:ConstantVolume simulation or the typical Multizone is described by this Air Distribution Unit (ADU). Multizone systems condition all the air in a central apparatus and distribute it to the conditioned zones through two parallel ducts. One duct carries cold air and the other warm air, providing air sources for both heating and cooling at all times. In each conditioned zone, a mixing valve responsive to a room thermostat mixes the warm and cold air in proper proportions to satisfy the prevailing heating or cooling load of the space. The Multizone ADU is the specific component that leads to the zone containing the mixer and the mixing damper and then connecting to the zone. The total airflow to each room is kept constant while the proportion of hot air to cold air is adjusted to maintain the temperature in each zone at the desired level.
-
-#### Field: Name
-
-Unique name for the Multizone ADU.
-
-#### Field: Availability Schedule Name
-
-Schedule that this component will operate or is available to operate for a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Outlet Node Name
-
-The outlet node from the ADU to the zone.
-
-#### Field: Hot Air Inlet Node Name
-
-The air-inlet node name that connects the hot air splitter to the individual zone ADU.
-
-#### Field: Cold Air Inlet Node Name
-
-The air-inlet node name that connects the cold air splitter to the individual zone ADU.
-
-#### Field: Maximum Air Flow Rate
-
-The design constant volume flow rate  (m<sup>3</sup>/sec) specified for that Multizone ADU.
-
-An IDF example:
-
-```idf
-AirTerminal:DualDuct:ConstantVolume,
-    Zone2MixDamp,  !- Name
-    FanAndCoilAvailSched,  !- Availability Schedule
-    Zone 2 Dual Duct Outlet,  !- Unit Air Outlet Node
-    Zone 2 Dual Duct Hot Inlet,  !- Unit Hot Air Inlet Node
-    Zone 2 Dual Duct Cold Inlet,  !- Unit Cold Air Inlet Node
-    0.36;  !- Max Air Flow Rate {m3/s}
-```
-
-### Dual Duct Constant Volume AirTerminal Outputs
-
-* HVAC,Average,Zone Air Terminal Cold Supply Duct Damper Position []
-
-* HVAC,Average,Zone Air Terminal Hot Supply Duct Damper Position []
-
-#### Zone Air Terminal Cold Supply Duct Damper Position
-
-This output is the damper position of the cold air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit cold air mass flow rate divided by the terminal unit’s maximum cold air mass flow rate. This output is dimensionless and ranges from 0.0 to 1.0.
-
-#### Zone Air Terminal Hot Supply Duct Damper Position
-
-This output is the damper position of the hot air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit hot air mass flow rate divided by the terminal unit’s maximum hot air mass flow rate. This output is dimensionless and ranges from 0.0 to 1.0.
-
-### AirTerminal:DualDuct:VAV
-
-AirTerminal:DualDuct:VAV (i.e., Dual duct variable air volume (DDVAV)) systems are used to obtain zone temperature control by mixing the cold and warm air in various volume combinations. The fan is sized for the anticipated maximum coincident hot or cold volume, not the sum of the instantaneous peaks. This system has an advantage of a true single path VAV system, except for warm port leakage. When cold air is modulated for control before mixing, it operates similar to the VAV induction when mixing occurs without hot deck reheat. It is similar to a reheat system when mixing occurs while the hot deck is using the reheat coil. It uses more energy than a true VAV system, but less than a constant volume dual duct system.
-
-#### Field: Name
-
-Unique name for the AirTerminal:DualDuct:VAV Air Distribution Unit (ADU).
-
-#### Field: Availability Schedule Name
-
-Schedule that this component will operate or is available to operate for a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Outlet Node Name
-
-The outlet node from the ADU to the zone.
-
-#### Field: Hot Air Inlet Node Name
-
-The air-inlet node name that connects the hot air splitter to the individual zone ADU.
-
-#### Field: Cold Air Inlet Node Name
-
-The air-inlet node name that connects the cold air splitter to the individual zone ADU.
-
-#### Field: Maximum Damper Air Flow Rate
-
-The design maximum volume flow rate  (m<sup>3</sup>/sec) specified for DDVAV ADU.
-
-#### Field: Zone Minimum Air Flow Fraction
-
-The minimum flow rate to the zone while the system is operating, specified as a fraction of the Max Damper Air Flow Rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object. When this field is used, the terminal unit will increase flow as needed to meet this outdoor air requirement. If Outdoor Air Flow per Person is non-zero, then the outdoor air requirement will be computed based on the current number of occupants in the zone. At no time will the supply air flow rate exceed the value for Maximum Air Flow Rate. If this field is blank, then the terminal unit will not be controlled for outdoor air flow. See documentation for the zone HVAC outdoor air object for further information (Ref DesignSpecification:OutdoorAir).
-
-An IDF example:
-
-```idf
-  AirTerminal:DualDuct:VAV,
-    Zone1MixDamp,            !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    Zone 1 Dual Duct Outlet, !- Air Outlet Node Name
-    Zone 1 Dual Duct Hot Inlet,  !- Hot Air Inlet Node Name
-    Zone 1 Dual Duct Cold Inlet,  !- Cold Air Inlet Node Name
-    autosize,                !- Maximum Air Flow Rate {m3/s}
-    0.1,                     !- Zone Minimum Air Flow Fraction
-    ZoneMinOARequirements;   !- Design Specification Outdoor Air Object Name
-
-! Outdoor air specification should be consistent with Sizing:Zone object inputs.
-  DesignSpecification:OutdoorAir,
-    ZoneMinOARequirements,    !- Name
-    Sum,                      !- Outdoor Air Method
-    0.00944,                  !- Outdoor Air Flow per Person {m3/s}
-    0.000508,                 !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    ,                         !- Outdoor Air Flow per Zone
-    ,                         !- Outdoor Air Flow Air Changes per Hour
-    Min OARequirements Sched; !- Outdoor Air Flow Rate Fraction Schedule Name
-
-  Schedule:Compact,
-    Min OARequirements Sched,  !- Name
-    Any Number,                !- Schedule Type Limits Name
-    Through: 12/31,            !- Field 1
-    For: Weekdays SummerDesignDay WinterDesignDay, !- Field 2
-    Until: 24:00,1.0,          !- Field 7
-    For: AllOtherDays,         !- Field 9
-    Until: 24:00,0.25;         !- Field 10
-```
-
-### Dual Duct VAV AirTerminal Outputs
-
-* HVAC,Average,Zone Air Terminal Cold Supply Duct Damper Position []
-
-* HVAC,Average,Zone Air Terminal Hot Supply Duct Damper Position []
-
-* HVAC,Average,Zone Air Terminal Outdoor Air Volume Flow Rate [m3/s]
-
-
-#### Zone Air Terminal Cold Supply Duct Damper Position []
-
-This output is the damper position of the cold air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit cold air mass flow rate divided by the terminal unit’s maximum cold air mass flow rate.
-
-#### Zone Air Terminal Hot Supply Duct Damper Position []
-
-This output is the damper position of the hot air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit hot air mass flow rate divided by the terminal unit’s maximum hot air mass flow rate.
-
-#### Zone Air Terminal Outdoor Air Volume Flow Rate [m3/s]
-
-This output is the amount of outdoor air entering the zone. This is the average value over the frequency being reported.  The amount of outdoor air is defined as the terminal unit air volume flow rate multiplied by the fraction of outdoor air entering the air loop’s outdoor air system.
-
-### AirTerminal:DualDuct:VAV:OutdoorAir
-
-AirTerminal:DualDuct:VAV:OutdoorAir provides a model for a type of dual duct air system in which one duct provides outdoor air ventilation and the other provides VAV cooling.  The Outdoor Air stream and the Recirculated Air stream are conditioned and supplied through separate air streams as part of a centralized dedicated outdoor air  (DOAS) distribution system. The dual duct arrangement allows the ventilation air to be controlled separately using schedules or occupancy demand while the recirculated air is controlled to meet the dry-bulb zone temperature setpoint. The two airstreams remain decoupled until the terminal box where they are mixed. The terminal unit is meant for systems regulating outdoor air based only on demand control or code minimum settings and not on economizer operation.
-
-This air terminal does not have heating coils and is not configured for conditions zones that need heat. Additional ZoneHVAC equipment, such as baseboards or fan coil units, are needed to provide heating to the zone when using this air terminal.
-
-Although this air terminal is primarily for dual duct system, it is allowed to use just the outdoor air side in a single duct system. This can be useful for modeling single duct DOAS when the required volume of outdoor air varies over time.
-
-#### Field: Name
-
-Unique name for the AirTerminal:DualDuct:VAV:OutdoorAir Air Distribution Unit (ADU).
-
-#### Field: Availability Schedule Name
-
-Schedule that this component will operate or is available to operate for a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Outlet Node Name
-
-The outlet node of the terminal unit.  This is the node leaving the unit and serving as the inlet to the zone. It is for the mixed flow leaving from both of the inlet node.
-
-#### Field: Outdoor Air Inlet Node Name
-
-The inlet node of the Outdoor Air (OA) stream deck of the Dual Duct system.
-
-#### Field: Recirculated Air Inlet Node Name
-
-The inlet node of the Recirculated Air (RA) stream deck of the Dual Duct system.  This input is optional.  If no node name is entered here, then the recirulation duct is disabled and the model functions as a single duct terminal and no second cooling deck is needed.
-
-#### Field: Maximum Zone Total Airflow Rate
-
-Max total airflow rate (in m3/s) at the terminal unit outlet including both the Outdoor Air stream and the Recirculated stream.  Can be autosized based on the Design Outdoor Airflow Rate and the zone thermal cooling load.  The autosized flow rate will be the sum of the maximum outdoor air requirement and the flow for cooling.  When autosizing, this maximum and the individual inlet flow rate sizes are reported to the eio file.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This field specifies the name of a DesignSpecification:OutdoorAir object.  This field is required for this object.  The terminal unit will modulate the Outdoor Air stream to meet this outdoor air requirement.  If Outdoor Air Flow per Person is applied, then the outdoor air required will be based on either the current number of occupants in the zone, as for demand controlled ventilation, or the design level of occupants depending on the setting in the next field.
-
-#### Field: Per Person Ventilation Rate Mode
-
-This field specifies how the outdoor air ventilation rates are calculated when based on a rate per person.  It can be either based on the current number of people as affected by time-varying occupancy schedules, or on the constant value for the maximum number of people.   Enter the key CurrentOccupancy for the former and DesignOccupancy for the later.
-
-
-
-An example input object follows.
-
-```idf
-  AirTerminal:DualDuct:VAV:OutdoorAir,
-    Media_Center Dual Duct Box Component,          !- Name
-    ALWAYS_ON,                                     !- Availability Schedule Name
-    Media_Center Dual Duct Box Outlet Node Name,   !- Air Outlet Node Name
-    Media_Center Dual Duct Box Inlet Node Name,    !- Outdoor Air Inlet Node Name
-    RC Media_Center Dual Duct Box Inlet Node Name, !- Recirculated Air Inlet Node Name
-    AUTOSIZE,                                      !- Maximum Terminal Air Flow Rate {m3/s}
-    Media_Center Dual Duct Box OA Design Spec,     !- Design Specification Outdoor Air Object Name
-    CurrentOccupancy;                              !- Per Person Ventilation Rate Mode
-
-
-  DesignSpecification:OutdoorAir,
-    Media_Center Dual Duct Box OA Design Spec,  !- Name
-    Sum,                     !- Outdoor Air Method
-    0.004719,                !- Outdoor Air Flow per Person {m3/s-person}
-    0.00061,                 !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0,                     !- Outdoor Air Flow per Zone {m3/s}
-    0.0,                     !- Outdoor Air Flow Air Changes per Hour
-    MinOA_Sched;             !- Outdoor Air Flow Rate Fraction Schedule Name
-```
-
-
-
-### Dual Duct VAV Outdoor Air AirTerminal Outputs
-
-* Output:Variable,\*,Zone Air Terminal Outdoor Air Duct Damper Position,hourly; !- HVAC Average []
-
-* Output:Variable,\*,Zone Air Terminal Recirculated Air Duct Damper Position,hourly; !- HVAC Average []
-
-* Output:Variable,\*,Zone Air Terminal Outdoor Air Fraction,hourly; !- HVAC Average []
-
-#### Zone Air Terminal Outdoor Air Duct Damper Position []
-
-This output is the damper position of the outdoor air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit outdoor air mass flow rate divided by the terminal unit’s maximum outdoor air mass flow rate.  This output is dimensionless and ranges from 0.0 to 1.0.
-
-#### Zone Air Terminal Recirculated Air Duct Damper Position []
-
-This output is the damper position of the recirculated cool air stream in a dual duct air terminal. This is the average value over the frequency being reported. The damper position is defined as the terminal unit cool air mass flow rate divided by the terminal unit’s maximum cool air mass flow rate.  This output is dimensionless and ranges from 0.0 to 1.0.
-
-#### Zone Air Terminal Outdoor Air Fraction []
-
-This output is the current fraction of outdoor air contained in the combined flow of aire entering the zone from the terminal unit. This is the average value over the frequency being reported. The outdoor air fraction is defined as the terminal unit outdoor air mass flow rate divided by the total air mass flow rate.  This output is dimensionless and ranges from 0.0 to 1.0.
-
-Group – Zone Forced Air Units
------------------------------
-
-### ZoneHVAC:IdealLoadsAirSystem
-
-The simplest piece of zone equipment is the ZoneHVAC:IdealLoadsAirSystem component. ZoneHVAC:IdealLoadsAirSystem is used in situations where the user wishes to study the performance of a building without modeling a full HVAC system. In such a case, the Ideal Loads Air System is usually the sole conditioning component: the user does not need to specify air loops, water loops, etc. All that is needed for the ideal system are zone controls, zone equipment configurations, and the ideal loads system component.
-
-This component can be operated with infinite or finite heating and cooling capacity. For either mode – infinite or limited capacity – the user can also specify on/off schedules for heating and cooling and outdoor air controls. There are also optional controls for dehumidification, humidification, economizer, and heat recovery. This component may be used in combination with other HVAC equipment serving the same zone.
-
-This component can be thought of as an ideal unit that mixes air at the zone exhaust condition with the specified amount of outdoor air and then adds or removes heat and moisture at 100% efficiency in order to produce a supply air stream at the specified conditions. The energy required to condition the supply air is metered and reported as DistrictHeating and DistrictCooling.
-
-**Notes:** The ideal loads system uses the zone return node or an optional zone exhaust node to extract air from the zone. Every zone served by an HVAC component must have a return air node, even though this node may not be connected to anything.
-
-The ideal loads system was significantly expanded in version 7.0 (October 2011). As part of this upgrade, any change in the moisture content of the supply air stream results in a latent cooling (dehumidification) or latent heating (humidification) load which is metered as DistrictCooling and DistrictHeating energy consumption. Prior to version 7.0, when the ideal loads system was in heating mode, only the energy for sensible heating was metered. This results in significant changes in reported energy use compared to earlier versions, especially when using the ***ConstantSupplyHumidityRatio*** option for Humidification Control Type.
-
-Older idf files which are transitioned to version 7.0 will automatically be set to use the ***ConstantSupplyHumidityRatio*** option for both dehumidification and humidification controls, because this is equivalent to the controls used in the older version of this system. However, the user should review all of the humidity control options and select the one which best reflects the goal of the simulation.
-
-#### Field: Name
-
-A unique user assigned name for each ideal loads air system component.  This name is referenced in a ZoneHVAC:EquipmentList object.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether or not this component is available to operate during a given time period. If the schedule value is greater than zero then the system is available to operate; otherwise, the system is unavailable for that time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Zone Supply Air Node Name
-
-The name of the outlet air node of the ideal loads object. This should be the same as one of the zone air inlet nodes for the zone the ideal loads component is serving.
-
-#### Field: Zone Exhaust Air Node Name
-
-The name of the zone exhaust air node of the ideal loads object. This should be the same as one of the zone air exhaust nodes for the zone this component is serving. This node name is required if ZoneHVAC:IdealLoadsAirSystem is used in a zone which also has other forced air HVAC equipment. Otherwise this node name is optional but recommended.
-
-#### Field: Maximum Heating Supply Air Temperature
-
-The maximum air temperature (degrees C) of the air used for heating the zone. The default is 50C (122F).
-
-#### Field: Minimum Cooling Supply Air Temperature
-
-The minimum air temperature (degrees C) of the air used for cooling the zone. The default is 13C (55.4F).
-
-#### Field: Maximum Heating Supply Air Humidity Ratio
-
-The maximum humidity ratio (kg of water per kg of dry air) of the hot supply air. The default is 0.0156 kgWater/kgDryAir which corresponds to a 20%RH at 50C (122F) dry bulb.
-
-#### Field: Minimum Cooling Supply Air Humidity Ratio
-
-The minimum humidity ratio (kg of water per kg of dry air) of the cool supply air. The default is 0.0077 kgWater/kgDryAir which corresponds to a 10C (50F) dew point.
-
-#### Field: Heating Limit
-
-The input must be either ***LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity*** or ***NoLimit***. ***LimitFlowRate*** means that the heating supply air flow rate will be limited to the value specified in the next input field. ***LimitCapacity*** means that the sensible heating capacity will be limited to the value specified in the Maximum Sensible Heating Capacity field. ***LimitFlowRateAndCapacity*** means that both flow rate and capacity will be limited. ***NoLimit*** (the default) means that there will not be any limit on the heating supply air flow rate or capacity and the subsequent two fields will be ignored.
-
-#### Field: Maximum Heating Air Flow Rate
-
-The maximum heating supply air flow rate in cubic meters per second if heating limit is set to ***LimitFlowRate or LimitFlowRateAndCapacity*** *.* This field may be autosized. This field is ignored if heating limit is set to ***NoLimit*** or ***LimitCapacity***.  If blank, there is no limit.
-
-#### Field: Maximum Sensible Heating Capacity
-
-The maximum allowed sensible heating capacity in Watts if Heating Limit is set to ***LimitCapacity*** or ***LimitFlowRateAndCapacity***. This field may be autosized. If blank, there is no limit. If Heating Limit *is set to **NoLimit*** or ***LimitFlowRate***, this field is ignored.
-
-#### Field: Cooling Limit
-
-The input must be either ***LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity*** or ***NoLimit***. ***LimitFlowrate*** means that the cooling supply air flow rate will be limited to the value specified in the next input field. ***LimitCapacity*** means that the total cooling capacity will be limited to the value specified in the Maximum Total Cooling Capacity field. ***LimitFlowRateAndCapacity*** means that both flow rate and capacity will be limited. ***NoLimit*** (the default) means that there will not be any limit on the cooling supply air flow rate or capacity and the subsequent two fields will be ignored.
-
-#### Field: Maximum Cooling Air Flow Rate
-
-The maximum cooling supply air flow rate in cubic meters per second if Cooling Limit is set to ***LimitFlowRate*** or ***LimitFlowRateAndCapacity****.* This field may be autosized. This field is ignored if cooling limit is set to ***NoLimit*** or ***LimitCapacity***. If blank, there is no limit. If *Cooling Limit is set to **NoLimit**,* this field is ignored*.* This field is required if Outdoor Air Control Type is ***TemperatureEconomizer*** in order to establish an upper limit on outdoor air flow when the economizer is active***.***
-
-#### Field: Maximum Total Cooling Capacity
-
-The maximum allowed total (sensible plus latent) cooling capacity in Watts if Cooling Limit is set to ***LimitCapacity*** or ***LimitFlowRateAndCapacity***. This field may be autosized. If blank, there is no limit. If Cooling Limit *is set to **NoLimit*** or ***LimitFlowRate****,* this field is ignored*.*
-
-#### Field: Heating Availability Schedule Name
-
-The name of a schedule (ref: Schedule) that denotes whether heating is available. A schedule value greater than 0 (usually 1 is used) indicates that heating and humidification are available. A value less than or equal to 0 (usually 0 is used) denotes that heating and humidification are not available. If blank, heating and humidification are always available.
-
-#### Field: Cooling Availability Schedule Name
-
-The name of a schedule (ref: Schedule) that denotes whether cooling is available. A schedule value greater than 0 (usually 1 is used) indicates that cooling and dehumidification are available. A value less than or equal to 0 (usually 0 is used) denotes that cooling and dehumidification is not available. If blank, cooling and dehumidification are always available.
-
-#### Field: Dehumidification Control Type
-
-Select from ***ConstantSensibleHeatRatio***, ***Humidistat, None, or ConstantSupplyHumidityRatio***. ***ConstantSensibleHeatRatio*** (the default) means that the ideal loads system will be controlled to meet the sensible cooling load, and the latent cooling rate will be computed using a constant sensible heat ratio (SHR) (see next field). ***Humidistat*** means that there is a ZoneControl:Humidistat for this zone and the ideal loads system will attempt to meet the humidistat request (i.e. will dehumidify according to the Dehumidifying Relative Humidity Schedule in the ZoneControl:Humidistat object). ***None*** means that there is no dehumidification. ***ConstantSupplyHumidityRatio*** means that during cooling the supply air will always be at the Minimum Cooling Supply Humidity Ratio. For ***ConstantSensibleHeatRatio*** and ***Humidistat***, if the mixed air humidity ratio is less than the target humidity ratio, then the mixed air humidity ratio will be used. For all options, the supply air humidity ratio will never be allowed to exceed saturation at the supply dry bulb temperature.
-
-The selected dehumidification control type is always applied when the unit is in cooling mode. If the unit is in deadband mode (not actively heating the supply air) control type ***Humidistat*** will be active. If the unit is in heating mode, control type ***Humidistat*** will be active if the Humidification Control Type field below is set to *Humidistat* or *None*.
-
-This allows the ideal loads system to heat and dehumidify at the same time.
-
-#### Field: Cooling Sensible Heat Ratio
-
-When the Dehumidification Control Type is set to ***ConstantSensibleHeatRatio*** the ideal loads system will be controlled to meet the sensible cooling load, and the latent cooling rate will be computed using the value of Cooling Sensible Heat Ratio (SHR), where SHR = Sensible Cooling divided by Total Cooling (sensible plus latent). The default is 0.7. If Dehumidification Control Type is set to something other than ***ConstantSensibleHeatRatio*** then this field will be ignored.
-
-#### Field: Humidification Control Type
-
-Select from ***None***, ***Humidistat, or ConstantSupplyHumidityRatio***. ***None*** means that there is no humidification. ***Humidistat*** means that there is a ZoneControl:Humidistat for this zone and the ideal loads system will attempt to meet the humidistat request (i.e., humidify according to the Humidifying Relative Humidity Setpoint Schedule in the ZoneControl:Humidistat object). ***ConstantSupplyHumidityRatio*** means that during heating the supply air will always be at the Maximum Heating Supply Humidity Ratio. The default is ***None***. For ***Humidistat***, if the mixed air humidity ratio is greater than the target humidity ratio, then the mixed air humidity ratio will be used. For all options, the supply air humidity ratio will never be allowed to exceed saturation at the supply dry bulb temperature.
-
-The selected humidification control type is always applied when the unit is in heating mode. If the unit is in deadband mode (not actively heating the supply air) control type ***Humidistat*** will be active. If the unit is in cooling mode, control type ***Humidistat*** will be active if the Dehumidification Control Type field above is set to *Humidistat* or *None*.
-
-This allows the ideal loads system to cool and humidify at the same time.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the outdoor air requirements and schedule for this system. The outdoor air flow rate may also be affected by the next two fields, Demand Controlled Ventilation Type and Outdoor Air Economizer Type. If this field is blank, this system will have no outdoor air, and all outdoor air control and heat recovery options will be ignored..
-
-#### Field: Outdoor Air Inlet Node Name
-
-This alpha field specifies the node name of the outdoor air inlet node. This node name is also specified in an OutdoorAir:Node or OutdoorAir:NodeList object. If this field is blank, a node name will be created internally.
-
-#### Field: Demand Controlled Ventilation Type
-
-This field, along with the Design Specification Outdoor Air Object (if used) specifies how the minimum outdoor air flow rate is calculated. The choices are: ***None, OccupancySchedule or CO2Setpoint***. The default is ***None***.
-
-- ***None*** means that the design occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field).
-
-- ***OccupancySchedule*** means that the current occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field).
-
-- ***CO2Setpoint*** means that the design occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field). In addition, the minimum outdoor air flow rate may be increased if necessary to maintain the level of indoor air carbon dioxide at or below the setpoint defined in a ZoneControl:ContaminantController object.
-
-#### Field: Outdoor Air Economizer Type
-
-This field specifies if there is an outdoor air economizer. The choices are: ***NoEconomizer, DifferentialDryBulb,*** or ***DifferentialEnthalpy***. The default is ***NoEconomizer***. ***DifferentialDryBulb*** and ***DifferentialEnthalpy*** mean that the economizer will increase the outdoor air flow rate above the minimum outdoor air flow (see fields Design Specification Outdoor Air Object Name and Demand Controlled Ventilation Type) when there is a cooling load and the outdoor air temperature or enthalpy is below the zone exhaust air temperature or enthalpy. The ***DifferentialDryBulb*** and ***DifferentialEnthalpy*** options require that the Maximum Cooling Air Flow Rate be specified which will be used as the limit for maximum outdoor air flow rate.
-
-#### Field: Heat Recovery Type
-
-Select from ***None***, **Sensible**, or ***Enthalpy***. ***None*** means that there is no heat recovery. ***Sensible*** means that there is sensible heat recovery whenever the zone exhaust air temperature is more favorable than the outdoor air temperature. ***Enthalpy*** means that there is latent and sensible heat recovery whenever the zone exhaust air enthalpy is more favorable than the outdoor air enthalpy. The default is ***None***.
-
-#### Field: Sensible Heat Recovery Effectiveness
-
-The sensible heat recovery effectiveness, where effectiveness is defined as the change in supply temperature divided by the difference in entering supply and relief air temperatures. The default is 0.70.
-
-#### Field: Latent Heat Recovery Effectiveness
-
-The latent heat recovery effectiveness, where effectiveness is defined as the change in supply humidity ratio divided by the difference in entering supply and relief air humidity ratios. The default is 0.65.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Maximum Heating Air Flow Rate and Maximum Cooling Air Flow Rate in a Ideal Load Air System zone HVAC object. The scaled maximum heating and cooling air flow rates are used to size the heating and cooling capacities.
-
-
-
-An example of this object in an IDF is:
-
-
-
-```idf
-  ZoneHVAC:IdealLoadsAirSystem,
-    Zone1 Ideal Loads System, !- Name
-    AlwaysOn,                !- Availability Schedule Name
-    Zone1 Ideal Loads Supply Node, !- Zone Supply Air Node Name
-    Zone1 Ideal Loads Return Node, ! Zone Exhaust Air Node Name
-    50,                      !- Maximum Heating Supply Air Temperature {C}
-    13,                      !- Minimum Cooling Supply Air Temperature {C}
-    0.0156,                  !- Maximum Heating Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.0077,                  !- Minimum Cooling Supply Air Humidity Ratio {kgWater/kgDryAir}
-    NoLimit,                 !- Heating Limit
-    ,                        !- Maximum Heating Air Flow Rate {m3/s}
-    ,                        !- Maximum Sensible Heating Capacity {W}
-    NoLimit,                 !- Cooling Limit
-    ,                        !- Maximum Cooling Air Flow Rate {m3/s}
-    ,                        !- Maximum Total Cooling Capacity {W}
-    ,                        !- Heating Availability Schedule Name
-    ,                        !- Cooling Availability Schedule Name
-    ConstantSensibleHeatRatio,  !- Dehumidification Control Type
-    0.7,                     !- Cooling Sensible Heat Ratio
-    None,                    !- Humidification Control Type
-    Office OA Specification, !- Design Specification Outdoor Air Object Name
-    Zone1 Ideal Loads OA Inlet Node, !- Outdoor Air Inlet Node Name
-    None,                    !- Demand Controlled Ventilation Type
-    NoEconomizer,            !- Outdoor Air Economizer Type
-    Enthalpy,                !- Heat Recovery Type
-    0.70,                    !- Sensible Heat Recovery Effectiveness
-    0.65;                    !- Latent Heat Recovery Effectiveness
-```
-
-### ZoneHVAC:IdealLoadsAirSystem Outputs
-
-* HVAC,Sum,Zone Ideal Loads Supply Air Sensible Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Supply Air Total Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Supply Air Sensible Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Supply Air Latent Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Supply Air Total Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Supply Air Latent Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Zone Sensible Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Zone Latent Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Zone Total Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Zone Sensible Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Zone Latent Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Zone Total Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Outdoor Air Sensible Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Outdoor Air Latent Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Outdoor Air Total Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Outdoor Air Sensible Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Outdoor Air Latent Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Outdoor Air Total Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Heat Recovery Sensible Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Heat Recovery Latent Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Heat Recovery Total Heating Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Heat Recovery Sensible Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Heat Recovery Latent Cooling Energy [J]
-
-* HVAC,Sum,Zone Ideal Loads Heat Recovery Total Cooling Energy [J]
-
-* HVAC,Average,Zone Ideal Loads Supply Air Sensible Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Supply Air Latent Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Supply Air Total Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Supply Air Sensible Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Supply Air Latent Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Supply Air Total Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Zone Sensible Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Zone Latent Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Zone Total Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Zone Sensible Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Zone Latent Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Zone Total Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Outdoor Air Sensible Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Outdoor Air Latent Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Outdoor Air Total Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Outdoor Air Sensible Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Outdoor Air Latent Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Outdoor Air Total Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Heat Recovery Sensible Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Heat Recovery Latent Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Heat Recovery Total Heating Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Heat Recovery Sensible Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Heat Recovery Latent Cooling Rate [W]
-
-* HVAC,Average,Zone Ideal Loads Heat Recovery Total Cooling Rate [W]
-
-* HVAC,Sum,Zone Ideal Loads Economizer Active Time [hr]
-
-* HVAC,Sum,Zone Ideal Loads Heat Recovery Active Time [hr]
-
-* HVAC,Average,Zone Ideal Loads Hybrid Ventilation Available Status []
-
-* HVAC,Average,Zone Ideal Loads Outdoor Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Ideal Loads Outdoor Air Standard Density Volume Flow Rate [m3/s]
-
-* HVAC,Average,Zone Ideal Loads Supply Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Ideal Loads Supply Air Standard Density Volume Flow Rate [m3/s]
-
-
-
-#### Ideal Loads Output Variable Overview
-
-All of the ZoneHVAC:IdealLoadsAirSystem loads and energy use are reported for Sensible Heating, Latent Heating, Total Heating, Sensible Cooling, Latent Cooling, and Total Cooling. To explain the relationship between the various outputs, Total Cooling Energy will be used.
-
-*Zone Ideal Loads Supply Air Total Cooling Energy* is the district cooling energy consumed by the ideal loads system “cooling coil� to cool and dehumidify the supply air.
-
-*Zone Ideal Loads Zone Total Cooling Energy* is the total (sensible plus latent) cooling energy delivered to the zone. If there is no outdoor air, then *Zone Ideal Loads Supply Air Total Cooling Energy = Zone Ideal Loads Zone Total Cooling Energy.*
-
-*Zone Ideal Loads Outdoor Air Total Cooling Energy* is the total (sensible plus latent) cooling energy required to cool the outdoor air to the zone exhaust air temperature and humidity ratio.
-
-*Zone Ideal Loads Heat Recovery Total Cooling Energy* is the total (sensible plus latent) cooling energy supplied by heat recovery. This offsets a portion of the *Zone Ideal Loads Outdoor Air Total Cooling Energy*.
-
-
-
-When the economizer is not active, these values are related by the following equation:
-
-*Zone Ideal Loads Supply Air Total Cooling Energy + Zone Ideal Loads Heat Recovery Total Cooling Energy =
- Zone Ideal Loads Zone Total Cooling Energy+ Zone Ideal Loads Outdoor Air Total Cooling Energy*
-
-#### Zone Ideal Loads Supply Air Sensible Heating Energy [J]
-
-#### Zone Ideal Loads Supply Air Sensible Heating Rate [W]
-
-The sensible heating energy (or rate) added to raise the temperature of the mixed air stream to the temperature of the supply air stream. This is the ideal “heating coil� load.
-
-#### Zone Ideal Loads Supply Air Latent Heating Energy [J]
-
-#### Zone Ideal Loads Supply Air Latent Heating Rate [W]
-
-The latent heating energy (or rate) added to raise the humidity ratio of the mixed air stream to the temperature of the supply air stream. This is the ideal “humidifier� load.
-
-#### Zone Ideal Loads Supply Air Total Heating Energy [J]
-
-#### Zone Ideal Loads Supply Air Total Heating Rate [W]
-
-The total (sensible and latent) heating energy (or rate) added to raise the mixed air stream to the temperature and humidity ratio of the supply air stream. *Zone Ideal Loads Supply Air Total Heating Energy* is metered as DistrictHeating energy.
-
-#### Zone Ideal Loads Supply Air Sensible Cooling Energy [J]
-
-#### Zone Ideal Loads Supply Air Sensible Cooling Rate [W]
-
-The sensible cooling energy (or rate) removed to lower the temperature of the mixed air stream to the temperature of the supply air stream. This is the ideal “cooling coil� sensible load.
-
-#### Zone Ideal Loads Supply Air Latent Cooling Energy [J]
-
-#### Zone Ideal Loads Supply Air Latent Cooling Rate [W]
-
-The latent cooling energy (or rate) removed to lower the humidity ratio of the mixed air stream to the temperature of the supply air stream. This is the ideal “cooling coil� latent load.
-
-#### Zone Ideal Loads Supply Air Total Cooling Energy [J]
-
-#### Zone Ideal Loads Supply Air Total Cooling Rate [W]
-
-The total (sensible and latent) cooling energy (or rate) removed to lower the mixed air stream to the temperature and humidity ratio of the supply air stream. *Zone Ideal Loads Supply Air Total Cooling Energy* is metered as DistrictCooling energy. This is the ideal “cooling coil� total load.
-
-#### Zone Ideal Loads Zone Sensible Heating Energy [J]
-
-#### Zone Ideal Loads Zone Sensible Heating Rate [W]
-
-The sensible heating energy (or rate) added to the zone.
-
-#### Zone Ideal Loads Zone Latent Heating Energy [J]
-
-#### Zone Ideal Loads Zone Latent Heating Rate [W]
-
-The latent heating energy (or rate) added to the zone.
-
-#### Zone Ideal Loads Zone Total Heating Energy [J]
-
-#### Zone Ideal Loads Zone Total Heating Rate [W]
-
-The total (sensible and latent) heating energy (or rate) added to the zone.
-
-#### Zone Ideal Loads Zone Sensible Cooling Energy [J]
-
-#### Zone Ideal Loads Zone Sensible Cooling Rate [W]
-
-The sensible cooling energy (or rate) removed from the zone.
-
-#### Zone Ideal Loads Zone Latent Cooling Energy [J]
-
-#### Zone Ideal Loads Zone Latent Cooling Rate [W]
-
-The latent cooling energy (or rate) removed from the zone.
-
-#### Zone Ideal Loads Zone Total Cooling Energy [J]
-
-#### Zone Ideal Loads Zone Total Cooling Rate [W]
-
-The total (sensible and latent) cooling energy (or rate) removed from the zone.
-
-#### Zone Ideal Loads Outdoor Air Sensible Heating Energy [J]
-
-#### Zone Ideal Loads Outdoor Air Sensible Heating Rate [W]
-
-The sensible heating energy (or rate) required to raise the temperature of the outdoor air to the zone exhaust air temperature. This value will be calculated only when heating is active.
-
-#### Zone Ideal Loads Outdoor Air Latent Heating Energy [J]
-
-#### Zone Ideal Loads Outdoor Air Latent Heating Rate [W]
-
-The latent heating energy (or rate) required to raise the humidity ratio of the outdoor air to the zone exhaust air humidity ratio. This value will be calculated only when humidification is active.
-
-#### Zone Ideal Loads Outdoor Air Total Heating Energy [J]
-
-#### Zone Ideal Loads Outdoor Air Total Heating Rate [W]
-
-The total (sensible and latent) heating energy (or rate) required to raise the temperature and humidity ratio of the outdoor air to the zone exhaust air humidity ratio. This value will be calculated only when heating or humidification is active.
-
-#### Zone Ideal Loads Outdoor Air Sensible Cooling Energy [J]
-
-#### Zone Ideal Loads Outdoor Air Sensible Cooling Rate [W]
-
-The sensible cooling energy (or rate) required to lower (or raise) the temperature of the outdoor air to the zone exhaust air temperature. This value will be calculated only when cooling is active.
-
-#### Zone Ideal Loads Outdoor Air Latent Cooling Energy [J]
-
-#### Zone Ideal Loads Outdoor Air Latent Cooling Rate [W]
-
-The latent cooling energy (or rate) required to lower (or raise) the humidity ratio of the outdoor air to the zone exhaust air humidity ratio. This will be calculated only when dehumidification is active.
-
-#### Zone Ideal Loads Outdoor Air Total Cooling Energy [J]
-
-#### Zone Ideal Loads Outdoor Air Total Cooling Rate [W]
-
-The total (sensible and latent) cooling energy (or rate) required to lower the temperature and humidity ratio of the outdoor air to the zone exhaust air temperature and humidity ratio. This value will be calculated only when cooling or dehumidification is active.
-
-#### Zone Ideal Loads Heat Recovery Sensible Heating Energy [J]
-
-#### Zone Ideal Loads Heat Recovery Sensible Heating Rate [W]
-
-The sensible heating energy (or rate) added to the outdoor air stream from heat recovery.
-
-#### Zone Ideal Loads Heat Recovery Latent Heating Energy [J]
-
-#### Zone Ideal Loads Heat Recovery Latent Heating Rate [W]
-
-The latent heating energy (or rate) added to the outdoor air stream from heat recovery.
-
-#### Zone Ideal Loads Heat Recovery Total Heating Energy [J]
-
-#### Zone Ideal Loads Heat Recovery Total Heating Rate [W]
-
-The total (sensible and latent) heating energy (or rate) added to the outdoor air stream from heat recovery.
-
-#### Zone Ideal Loads Heat Recovery Sensible Cooling Energy [J]
-
-#### Zone Ideal Loads Heat Recovery Sensible Cooling Rate [W]
-
-The sensible cooling energy (or rate) removed from the outdoor air stream from heat recovery.
-
-#### Zone Ideal Loads Heat Recovery Latent Cooling Energy [J]
-
-#### Zone Ideal Loads Heat Recovery Latent Cooling Rate [W]
-
-The latent cooling energy (or rate) removed from the outdoor air stream from heat recovery.
-
-#### Zone Ideal Loads Heat Recovery Total Cooling Energy [J]
-
-#### Zone Ideal Loads Heat Recovery Total Cooling Rate [W]
-
-The total (sensible and latent) cooling energy (or rate) removed from the outdoor air stream from heat recovery.
-
-#### Zone Ideal Loads Economizer Active Time [hr]
-
-Hours when the Ideal Loads economizer increased the outdoor air flow rate above the minimum.
-
-#### Zone Ideal Loads Heat Recovery Active Time [hr]
-
-Hours when the Ideal Loads heat recovery was actively heating or cooling the outdoor air stream.
-
-#### Zone Ideal Loads Hybrid Ventilation Available Status []
-
-This is the availability status of the ideal loads object as set by the hybrid ventilation manager. Rules to determine the availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 and 1. These integers represent NoAction (0) and ForceOff (1). When the availability status is ForceOff, the unit is turned off regardless of its availability schedule. The other status flag i.e. NoAction does not control the unit and the controls of the unit turn it back on. Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-#### Zone Ideal Loads Outdoor Air Mass Flow Rate [kg/s]
-
-The mass flow rate of the outdoor air stream in kg/s.
-
-#### Zone Ideal Loads Outdoor Air Standard Density Volume Flow Rate [m3/s]
-
-The volume flow rate of the outdoor air stream in m3/s using the standard density. The standard density is determined for dry air at the standard barometric pressure for the location’s elevation and a temperature of 20.0ºC. The standard density does not vary over time.
-
-#### Zone Ideal Loads Supply Air Mass Flow Rate [kg/s]
-
-The mass flow rate of the supply air stream in kg/s.
-
-#### Zone Ideal Loads Supply Air Standard Density Volume Flow Rate [m3/s]
-
-The volume flow rate of the supply air stream in m3/s using the standard density. The standard density is determined for dry air at the standard barometric pressure for the location’s elevation and a temperature of 20.0ºC. The standard density does not vary over time.
-
-### ZoneHVAC:FourPipeFanCoil
-
-What is a fan coil unit? Like many HVAC terms, “fan coil unit� is used rather loosely. Sometimes it is used for terminal units that would be better described as powered induction units. Carrier and others use the term for the room side of refrigerant-based split systems. Here we are modeling in-room forced-convection hydronic units. The hydronic heating coil may be replaced with an electric heating coil. Typically these units are small (200 – 1200 cfm) and self-contained. They are mostly used in exterior zones, usually in hotels, apartments, or offices. They may be connected to ducted outside air, or have a direct outside air vent, but they do not have outside air economizers. Units with outside air economizers are marketed (in the United States) as unit ventilators. Unit ventilators are typically bigger than fan coils and are widely used in classrooms or other applications where ventilation is a priority. If a zonal unit with an outside economizer is desired, *ZoneHVAC:UnitVentilator* should be used.
-
-The heating or cooling output of the unit ventilator is controlled by varying the air flow rate, the water flow rate, or both. Air flow rate can be controlled by cycling the fan on/off or with a variable speed fan drive. The most common setup is a two or three speed fan with the speed selected by hand. The fan then cycles on/off to control heating / cooling output. The controls are often a wall mounted thermostat with hand selection of heating/cooling and fan speed (off/low/medium/high). These controls may also be mounted on the unit.
-
-Carrier offers a retrofit VSD motor for fan coil units. It claims up to 45% energy savings from such a retrofit, as well as increased comfort and less noise compared to a cycling fan (fan coil fans are typically noisy and inefficient). Some other manufacturers are also offering units with VSD fans. Variable speed fans appear to offer an easy way to significantly increase the efficiency of what have typically been very inefficient units.
-
-EnergyPlus provides 6 capacity control methods for this unit:
-
-  1. multi-speed cycling fan with constant water flow rate
-
-  2. constant speed continuous fan with variable water flow rate
-
-  3. variable-speed fan with constant water flow rate
-
-  4. variable-speed fan with variable water flow rate
-
-  5. multi-speed fan with cycling between speeds and  constant water flow.
-
-  6. fan speed control based on ASHRAE 90.1
-
-In EnergyPlus the fan coil units are modeled as compound components. That is, they are assembled from other components. Fan coils contain an outdoor air mixer, a fan, a heating coil and a cooling coil. These components are described elsewhere in this document. The fan coil input simply requires the names of these four components, which have to be described elsewhere in the input. The input also requires the name of an availability schedule, maximum airflow rate, outdoor airflow rate, and maximum and minimum hot (for hydronic heating coil only) and cold water volumetric flow rates. The unit is connected to the zone inlet and exhaust nodes and the outdoor air by specifying unit inlet, and outlet air node names and the outdoor air mixer object name. The outdoor air mixer child object provides the outdoor air and relief air nodes names. Note that the unit air inlet node should be the same as a zone exhaust node and the unit outlet node should be the same as a zone inlet node. The fan coil unit is connected to a hot water loop through its hot water coil or with no hot water loop when using an electric coil (demand side) and to a chilled water loop (demand side) through its cooling coil.
-
-Note that the type of fan component associated with the fan coil unit depends on the type of capacity control method chosen. For *ConstantFanVariableFlow * a *Fan:OnOff* or *Fan:ConstantVolume* should be used. For *CyclingFan*, a *Fan:OnOff* should be used, for *VariableFanVariableFlow* or *VariableFanConstantFlow* a *Fan:VariableVolume*, for *MultiSpeedFan* a *Fan:OnOff* should be used, and for *ASHRAE90VariableFan*, a *Fan:OnOff* or *Fan:VariableVolume* should be chosen.
-
-Fan coil units can be 4-pipe or 2-pipe. For 4-pipe units there are 2 supply pipes and 2 return pipes. For 2-pipe units there is a single supply pipe and a single return pipe and the supply is switched between hot and chilled water depending on the season. EnergyPlus models 4-pipe units, but the 4-pipe model can be used to model 2-pipe units by using the coil availability schedules to make sure that either hot or chilled water is exclusively available. Fan coil units with hydronic heat can instead be modeled using an electric heating coil if desired (i.e., replace the hydronic heating coil with an electric heating coil).
-
-#### Field: Name
-
-A unique user assigned name for an instance of a Fan Coil unit. Any reference to this Fan Coil unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the fan coil unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-***Field: Capacity Control Method***
-
-This input denotes how the unit’s output is controlled in order to meet zone heating or cooling requirement. The choices are ***ConstantFanVariableFlow***, ***CyclingFan***, ***VariableFanVariableFlow***, ***VariableFanConstantFlow***, ***MultiSpeedFan***, or ***ASHRAE90VariableFan***. For *ConstantFanVariableFlow*, the fan speed is held constant to produce a fixed air flow rate whenever the unit is scheduled on. The hot water or chilled flow rate is varied so that the unit output matches the zone heating or cooling requirement. For *CyclingFan*, the fan speed is chosen so that the unit capacity is greater than or equal to the heating / cooling load and the fan is cycled to match unit output with the load. For *VariableFanVariableFlow*  both air and water flow rates are varied to match the load. For *VariableFanConstantFlow,* the water flow rate is at full flow and the fan speed varies to meet the load. For *MultiSpeedFan* the water flow rate is at full flow when there is load or fully closed when there is no load and the supply air flow rate is varied by varying the fan speed in order to match the load. For *ASHRAE90VariableFan*, the fan air flow rate is reduced according to the low speed supply air flow ratio when the zone sensible load is less than the zone sensible load multiplied by the low speed supply air flow ratio. The water coil water flow rate, or the electric heating coil part-load ratio, is modulated to meet the zone load. If the zone sensible load is greater than the zone sensible load multiplied by the low speed supply air flow ratio, then the air and water flow rate is increased to meet the load. If the zone load is greater than the design sensible load, the fan air flow rate is maintained at the maximum value while the water flow rate is further increased to the maximum available while electric heating coils are maintained at the maximum output.
-
-***Note: when ASHRAE90VariableFan is selected, if the the Minimum Supply Air Temperature in Cooling/Heating Mode inputs are not specified, the simulation must include zone sizing to calculate the zone design sensible cooling and heating load used to modulate the fan speed and, for water coils, the water flow rate or for electric heating coils, the part load ratio.***
-
-***MultiSpeedFan:*** for a given load, the fan cycles between speeds when fan speed selected is higher than the minimum speed or the fan cycles on-off when the fan speed selected is the minimum and the fan operating schedule is cycling fan. When the fan is operating as a continuous fan, then the fan runs at minimum speed even when there is no load to meet. When the speed selected is higher than the minimum speed, then the fan cycles between consecutive speed regardless of the fan operating schedule type. The model selects at what fan speed to run depending on cooling or heating load.
-
-#### Field: Maximum Supply Air Flow Rate
-
-The maximum volumetric airflow rate (m<sup>3</sup>/sec) through the fan coil unit. This is also the design, rated airflow rate of the unit.
-
-#### Field: Low Speed Supply Air Flow Ratio
-
-This numerical field specifies the ratio of the low speed flow rate to the maximum supply air flow rate. This value should be less than the *Medium Speed Supply Air Flow Ratio.* If left blank, the default value is 0.33. Leave this field blank if the capacity control method selected is not *CyclingFan* or *ASHRAE90VariableFan*. The suggested value is 0.5 when using the ASHRAE90VariableFan capacity control method.
-
-#### Field: Medium Speed Supply Air  Flow Ratio
-
-This numerical field specifies the ratio of the medium speed flow rate to the maximum supply air flow rate. Its value should be greater than the *Low Speed Supply Air Flow Ratio* but less than 1. If left blank, the default value is 0.66. Leave this field blank if the capacity control method selected is not *CyclingFan* or *MultiSpeedFan*.
-
-#### Field: Maximum Outdoor Air Flow Rate
-
-If the fan coil unit uses outdoor air, this field specifies the outdoor air volumetric flow rate (m<sup>3</sup>/sec). This flow rate should be less than or equal to the maximum airflow rate. A value of zero specifies no outdoor air.
-
-#### Field: Outdoor Air Schedule Name
-
-The name of a schedule whose values (0.0 to 1.0) are used as multipliers to alter the outdoor air flow rate. If this field is left blank, the values will default to 1.0.
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node from which the fan coil unit draws its indoor air. This should be one of zone exhaust nodes for the zone which the fan coil unit is serving.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node to which the fan coil unit sends its outlet air. This should be one of the inlet air nodes of the zone which is being served.
-
-#### Field: Outdoor Air Mixer Object Type
-
-This field specifies the type of outdoor air mixer used by this fan coil unit. The outdoor air mixer component is part of the fan coil compound object. The only available outdoor air mixer type is:
-
-OutdoorAir:Mixer
-
-#### Field: Outdoor Air Mixer Name
-
-The name of an outdoor air mixer component (object:OutdoorAir:Mixer) which composes part of the fan coil unit. Note that the return air node of the outdoor air mixer should be the same node as the air inlet node of the fan coil unit. In addition, the outdoor air mixer’s mixed air node should be the same as the inlet air node of the fan coil unit’s fan.
-
-#### Field: Supply Air Fan Object Type
-
-This field specifies the type of supply air fan object used by this fan coil. The supply air fan is part of the fan coil compound object. The only valid supply air fan types are:
-
-* Fan:OnOff
-
-* Fan:ConstantVolume
-
-* Fan:VariableVolume
-
-#### Field: Supply Air Fan Name
-
-The name of a fan component that composes part of the fan coil unit. Note that the fan’s maximum flow rate should be the same as the maximum airflow rate of the fan coil unit and the type of fan object should correspond to the capacity control method. Namely, for *ConstantFanVariableFlow * a *Fan:OnOff* or *Fan:ConstantVolume* should be used. For *CyclingFan*, a *Fan:OnOff* should be used. For *VariableFanVariableFlow* or *VariableFanConstantFlow* a *Fan:VariableVolume* should be chosen. For *MultiSpeedFan* a *Fan:OnOff* should be used. And for *ASHRAE90VariableFan*, a *Fan:OnOff* or *Fan:VariableVolume* should be chosen. 
-
-    The fan’s inlet node should be the same as the outdoor air mixer’s mixed air node.
-    The fan’s outlet node should be the same as the cooling coil’s air inlet node.
-
-#### Field: Cooling Coil Object Type
-
-This field specifies the type of chilled water cooling coil to be modeled for this fan coil unit. Only the following coil types can be used:
-
-* Coil:Cooling:Water
-
-* Coil:Cooling:Water:DetailedGeometry
-
-* CoilSystem:Cooling:Water:HeatExchangerAssisted
-
-The input requirements for these chilled water coil objects are described elsewhere in this document.
-
-#### Field: Cooling Coil Name
-
-The name of the cooling coil component that composes part of the fan coil unit. The cooling coil air inlet node should be the same as the fan outlet node. The cooling coil air outlet node should be the same as the heating coil air inlet node.
-
-Only the following coil types can be used:
-
-* Coil:Cooling:Water
-
-* Coil:Cooling:Water:DetailedGeometry
-
-* CoilSystem:Cooling:Water:HeatExchangerAssisted
-
-#### Field: Maximum Cold Water Flow Rate
-
-The maximum cold water volumetric flow rate (m<sup>3</sup>/sec) through the fan coil unit’s cooling coil.
-
-#### Field: Minimum Cold Water Flow Rate
-
-The minimum cold water volumetric flow rate (m<sup>3</sup>/sec) through the fan coil unit’s cooling coil.
-
-#### Field: Cooling Convergence Tolerance
-
-The convergence tolerance for the control of the unit cooling output. The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The cooling convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {{Q_{fancoil,out}} - {Q_{zoneload}}} \right|}}{{{Q_{zoneload}}}} \le CoolingConvergenceTolerance\]</div>
-
-#### Field: Heating Coil Object Type
-
-This field is the type of coil that is used for heating in the fan coil system. It is used in conjunction with the heating coil name (see next field) to specify the heating coil present within the system. The only allowable heating coil types are:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-#### Field: Heating Coil Name
-
-The name of the heating coil component that composes part of the fan coil unit. The heating coil air inlet node should be the same as the cooling coil outlet node. The heating coil air outlet node should be the same as the fan coil air outlet node.
-
-Only the following coil types can be used:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-#### Field: Maximum Hot Water Flow Rate
-
-The maximum hot water volumetric flow rate (m<sup>3</sup>/sec) through the fan coil unit’s heating coil. This field is not used with an electric heating coil.
-
-#### Field: Minimum Hot Water Flow Rate
-
-The minimum hot water volumetric flow rate (m<sup>3</sup>/sec) through the fan coil unit’s heating coil. This field is not used with an electric heating coil.
-
-#### Field: Heating Convergence Tolerance
-
-The convergence tolerance for the control of the unit heating output. The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The heating convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {{Q_{fancoil,out}} - {Q_{zoneload}}} \right|}}{{{Q_{zoneload}}}} \le HeatingConvergenceTolerance\]</div>
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this object’s fan. If the fan coil is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this object should be on or off.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Maximum Air Flow Rate in this Four Pipe FanCoil zone HVAC object. The scaled Maximum Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-This input field is the name of a schedule that controls fan operation. Schedule Name values of 0
-denote cycling fan operation (fan cycles with heating or cooling coil). Schedule values greater than 0 denote constant fan operation (fan runs continually regardless of coil operation). The fan operating mode defaults to cycling fan operation if this field is left blank. This input field is currently used with *MultiSpeedFan* capacity control method only.
-
-#### Field: Minimum Supply Air Temperature in Cooling Mode
-This optional input is used only when *Capacity Control Method = ASHRAE90VariableFan*. Specify the minimum supply air temperature in cooling mode. When the fan coil capacity is greater than the zone load, the fan speed will modulate down to the minimum fan speed, based on the Low Speed Supply Air Flow Ratio input field, and the water flow rate will also be reduced to maintain the zone thermostat set point temperature. When the zone load is one-half the fan coil capacity, the fan will operate at the minimum speed. When these fields are not entered, a zone sizing simulation must be performed. Both the cooling and heating supply air temperature must be entered or blank in unison. Values must be greater than 0 or this field is autosizable. A value of 0 (in both fields) will disregard these fields.
-
-#### Field: Maximum Supply Air Temperature in Heating Mode
-This optional input is used only when *Capacity Control Method = ASHRAE90VariableFan*. Specify the maximum supply air temperature in heating mode. When the fan coil capacity is greater than the zone load, the fan speed will modulate down to the minimum fan speed, based on the Low Speed Supply Air Flow Ratio input field, and the water flow rate will also be reduced to maintain the zone thermostat set point temperature. When the zone load is one-half the fan coil capacity, the fan will operate at the minimum speed. When these fields are not entered, a zone sizing simulation must be performed. Both the cooling and heating supply air temperature must be entered or blank in unison. Values must be greater than 0 or this field is autosizable. A value of 0 (in both fields) will disregard these fields.
-
-
-An example input for a fan coil unit, including its constituent components, is shown below.
-
-```idf
-  ZoneHVAC:FourPipeFanCoil,
-    Zone1FanCoil,            !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    ConstantFanVariableFlow, !- Capacity Control Method
-    autosize,                !- Maximum Supply Air Flow Rate {m3/s}
-    ,                        !- Low Speed Supply Air Flow Ratio
-    ,                        !- Medium Speed Supply Air Flow Ratio
-    autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
-    OUTAIRFANCOILSCHEDULE,   !- Outdoor Air Schedule Name
-    Zone1FanCoilAirInletNode,!- Air Inlet Node Name
-    Zone1FanCoilAirOutletNode,  !- Air Outlet Node Name
-    OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type
-    Zone1FanCoilOAMixer,     !- Outdoor Air Mixer Name
-    Fan:ConstantVolume,      !- Supply Air Fan Object Type
-    Zone1FanCoilFan,         !- Supply Air Fan Name
-    Coil:Cooling:Water,      !- Cooling Coil Object Type
-    Zone1FanCoilCoolingCoil, !- Cooling Coil Name
-    autosize,                !- Maximum Cold Water Flow Rate {m3/s}
-    0.0,                     !- Minimum Cold Water Flow Rate {m3/s}
-    0.001,                   !- Cooling Convergence Tolerance
-    Coil:Heating:Water,      !- Heating Coil Object Type
-    Zone1FanCoilHeatingCoil, !- Heating Coil Name
-    autosize,                !- Maximum Hot Water Flow Rate {m3/s}
-    0.0,                     !- Minimum Hot Water Flow Rate {m3/s}
-    0.001;                   !- Heating Convergence Tolerance
-
-OutdoorAir:Mixer,
-    Zone1FanCoilOAMixer, ! name
-    Zone1FanCoilOAMixerOutletNode, !Mixed Air Node Name
-    Zone1FanCoilOAInNode, !Outdoor Air Stream Node Name
-    Zone1FanCoilExhNode, !Relief Air Stream Node Name
-    Zone1FanCoilAirInletNode; !Return Air Stream Node Name
-
-Fan:OnOff,
-   Zone1FanCoilFan,         !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    0.5,                     !- Fan Total Efficiency
-    75.0,                    !- Pressure Rise {Pa}
-    autosize,                !- Maximum Flow Rate {m3/s}
-    0.9,                     !- Motor Efficiency
-    1.0,                     !- Motor In Airstream Fraction
-    Zone1FanCoilOAMixerOutletNode,  !- Air Inlet Node Name
-    Zone1FanCoilFanOutletNode,  !-Air Outlet Node Name
-    FanPowerRatioCurve,      !- Fan Power Ratio Function of Speed Ratio Curve Name
-    FanEffRatioCurve;        !- Fan Efficiency Ratio Function of Speed Ratio Curve Name
-
-Coil:Cooling:Water,
-    Zone1FanCoilCoolingCoil, !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    autosize,                !- Design Water Flow Rate {m3/s}
-    autosize,                !- Design Air Flow Rate {m3/s}
-    autosize,                !- Design Inlet Water Temperature {C}
-    autosize,                !- Design Inlet Air Temperature {C}
-    autosize,                !- Design Outlet Air Temperature {C}
-    autosize,                !- Design Inlet Air Humidity Ratio {kgWater/kgDryAir}
-    autosize,                !- Design Outlet Air Humidity Ratio {kgWater/kgDryAir}
-    Zone1FanCoilChWInletNode,!- Water Inlet Node Name
-    Zone1FanCoilChWOutletNode,  !- Water Outlet Node Name
-    Zone1FanCoilFanOutletNode,  !- Air Inlet Node Name
-    Zone1FanCoilCCOutletNode,!-Air Outlet Node Name
-    SimpleAnalysis,          !- Type of Analysis
-    CrossFlow;               !- Heat Exchanger Configuration
-
-Coil:Heating:Water,
-    Zone1FanCoilHeatingCoil, !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    autosize,                !- U-Factor Times Area Value {W/K}
-    autosize,                !- Maximum Water Flow Rate {m3/s}
-    Zone1FanCoilHWInletNode, !- Water Inlet Node Name
-    Zone1FanCoilHWOutletNode,!- Water Outlet Node Name
-    Zone1FanCoilCCOutletNode,!- Air Inlet Node Name
-    Zone1FanCoilAirOutletNode,  !-Air Outlet Node Name
-    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
-    autosize,                !- Nominal Capacity {W}
-    82.2,                    !- Design Inlet Water Temperature {C}
-    16.6,                    !- Design Inlet Air Temperature {C}
-    71.1,                    !- Design Outlet Water Temperature {C}
-    32.2;                    !- Design Outlet Air Temperature {C}
-
-Curve:Exponent,
-    FanPowerRatioCurve,      !- Name
-    0.0,                     !- Coefficient1 Constant
-    1.0,                     !- Coefficient2 Constant
-    3.0,                     !- Coefficient3 Constant
-    0.0,                     !- Minimum Value of x
-    1.5,                     !- Maximum Value of x
-    0.01,                    !- Minimum Curve Output
-    1.5;                     !- Maximum Curve Output
-
-Curve:Cubic,
-   FanEffRatioCurve,        !- Name
-   0.33856828,              !- Coefficient1 Constant
-   1.72644131,              !- Coefficient2 x
-   -1.49280132,             !- Coefficient3 x**2
-   0.42776208,              !- Coefficient4 x**3
-   0.5,                     !- Minimum Value of x
-   1.5,                     !- Maximum Value of x
-   0.3,                     !- Minimum Curve Output
-   1.0;                     !- Maximum Curve Output
-```
-
-### Fan Coil Outputs
-
-* HVAC,Average,Fan Coil Heating Rate [W]
-
-* HVAC,Sum,Fan Coil Heating Energy [J]
-
-* HVAC,Average,Fan Coil Total Cooling Rate [W]
-
-* HVAC,Sum,Fan Coil Total Cooling Energy [J]
-
-* HVAC,Average,Fan Coil Sensible Cooling Rate [W]
-
-* HVAC,Sum,Fan Coil Sensible Cooling Energy [J]
-
-* HVAC,Average,Fan Coil Fan Electric Power[W]
-
-* HVAC,Sum,Fan Coil Fan Electric Energy [J]
-
-* HVAC,Average,Fan Coil Runtime Fraction []
-
-* HVAC,Average, Fan Coil Fan Speed Level []
-
-* HVAC,Average, Fan Coil Part Load Ratio []
-
-* HVAC,Average, Fan Coil Availability Status []
-
-* HVAC,Average, Fan Coil Part Load Ratio []
-
-* HVAC,Average, Fan Coil Speed Ratio []
-
-
-#### Fan Coil Heating Rate [W]
-
-This field reports the dry air heating addition rate of the fan coil unit to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the unit.
-
-#### Fan Coil Heating Energy [J]
-
-This field is the dry air heat addition of the fan coil unit to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit, and the timestep.
-
-#### Fan Coil Total Cooling Rate [W]
-
-This field is the total (sensible and latent) heat extraction rate of the fan coil unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
-
-#### Fan Coil Total Cooling Energy [J]
-
-This field is the total (sensible and latent)  heat extraction of the fan coil unit from the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit, and the timestep.
-
-#### Fan Coil Sensible Cooling Rate [W]
-
-This field reports the dry air sensible heat extraction rate of the fan coil unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
-
-#### Fan Coil Sensible Cooling Energy [J]
-
-This field is the dry air sensible heat extraction of the fan coil unit from the zone it is serving in Joules over the timestep being reported. This is determined by the outlet and zone conditions, the mass flow rate through the unit, and the timestep.
-
-#### Fan Coil Fan Electric Power [W]
-
-This field reports the electricity consumption rate of the fan coil unit in Watts.
-
-#### Fan Coil Fan Electric Energy [J]
-
-This field is the electricity consumption of the fan coil unit in Joules over the timestep being reported.
-
-#### Fan Coil Runtime Fraction[]
-
-This field is the fraction of the system timestep the fan coil unit is running for the *CyclingFan* capacity control method.  This variable is defined only for the *CyclingFan* capacity control method.
-
-#### Fan Coil Fan Speed Level []
-
-This field is indicates the speed chosen for the fan in the *CyclingFan* and *MultiSpeedFan* capacity control methods.  A value of '0' means that the unit is off, '1' the fan is running at its low speed, '2' medium speed, and '3' high speed (maximum). This variable is defined only for the *CyclingFan* and *MultiSpeedFan* capacity control methods.
-
-#### Fan Coil Part Load Ratio []
-
-When the capacity control method is *VariableFanVariableFlow* or *VariableFanConstantFlow,* this output variable reports the unit part load ratio (ratio of unit heating / cooling output to the maximum heating / cooling output). This variable is defined only for *VariableFanVariableFlow*, *VariableFanConstantFlow* or *MultiSpeedFan* capacity control methods. The unit part load ratio is applicable to *MultiSpeedFan* only when the fan speed level selected is the minimum (Speed 1).
-
-#### Fan Coil Availability Status []
-
-This is the availability status of the fan coil unit fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the fan coil unit  object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-#### Fan Coil Speed Ratio []
-This output variable is the ratio of time in a system timestep that the fan coil unit is at rated speed between two consecutive speed levels ( [load – Capacity at Fan Speed i-1] / [Capacity at Fan Speed i – Capacity at Fan Speed i-1]). The fan speed ratio has minimum value of 0.0, and a maximum value of 1.0 and any value in between as it is averaged over the timestep. The value is 0.0 during Speed Level 1 operation.  Hydronic FanCoil units speed ratio depends on the fan speed and current load. The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the lower speed runs in the rest of the system timestep.
-
-
-### ZoneHVAC:UnitVentilator
-
-Unit ventilators are zone equipment units which are assembled from other components. They contain a built-in outdoor air mixer, a fan, a heating coil, and a cooling coil. These components are described elsewhere in this document, except the built-in outdoor air mixer which is contained within the unit ventilator statement. The unit ventilator input simply requires the names of these other three components, which have to be described elsewhere in the input. The input also requires the name of an availability schedule, maximum airflow rate, outdoor air control information (control type and schedules), an outdoor airflow rate, and maximum and minimum hot and cold water mass flow rates. The unit is connected to the zone inlet and exhaust nodes and the outdoor air by specifying unit inlet, outlet, outdoor air and exhaust (relief) air node names. Note that the unit air inlet node should be the same as a zone exhaust node and the unit outlet node should be the same as a zone inlet node. In general, the unit ventilator input is very similar to the fan coil unit input, and the unit is connected to a hot water loop (demand side) through its hot water coil and to a chilled water loop (demand side) through its cooling coil.
-
-The main difference between the fan coil and unit ventilator input is that the unit ventilator has a built-in outdoor air mixer with its own specialized controls. The outdoor air control type can be selected from one of the following options: “variable percent�, “fixed temperature� or “fixed amount�. In fixed temperature control, the amount of outdoor air is varied between the minimum outdoor air fraction (specified by a schedule) and 100% outdoor air to obtain a mixed air temperature as close as possible to the temperature schedule defined in the input. Variable percent control will also vary the amount of outdoor air between the minimum and maximum fractions (both specified in input by the user) to meet the load without the use of a coil if possible. In fixed amount control, the outdoor air flow rate is fixed to the specified value by the user. In this control strategy, the maximum outdoor air flow rate and schedule are automatically set to be equal to the minimum outdoor air flow rate and schedule. These control types are based on the 2004 ASHRAE Systems and Equipment Handbook (pp. 31.1-31.3) description of unit ventilator systems.
-
-The unit is controlled to meet the zone (remaining) heating or cooling demand. If there is a heating demand, the cooling coil is off and the hot water flow through the heating coil is throttled to meet the demand. The hot water control node must be specified (same as the hot water coil inlet node). If there is a cooling demand from the zone, the hot water coil is off and the chilled water flow through the cooling coil is throttled to meet the load. The cooling coil control node must be specified (same as the cooling coil inlet node). Finally both heating and cooling require a convergence tolerance, which is the tolerance denoting how closely the fan coil unit will meet the heating or cooling load. The tolerance is always relative to the zone load.
-
-Overall, control of the unit must consider the outdoor air. Here is a more detailed description of the overall unit control:
-
-**Off:** Unit is schedule off or there is no load on it. All flow rates are set to zero and the temperatures are set to zone conditions (except for the outdoor air inlet). Outdoor air requirements will not override this condition.
-
-**Heating/No Coil/VariablePercent:** The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and variable percent outdoor air control type has been specified. In this case, the variable percent outdoor air controls what happens with the outdoor air. If the outside temperature is greater than the return temperature, then the outdoor air is set to the maximum as defined by the user input. If the outdoor air temperature is less than the return temperature from the zone, then the outdoor air is set to the minimum outdoor air flow rate as defined by the user. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
-
-**Heating/No Coil/FixedTemperature:** The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate.
-
-**Heating/No Coil/FixedAmount:** The unit is on, there is a heating load, no heating coil is present or it has been scheduled off, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
-
-**Heating /With Coil/VariablePercent:** The unit is on, there is a heating load, and variable percent control is specified. The outdoor air fraction is set to the minimum outdoor air fraction (schedule based), and the heating coil is activated. The heating coil attempts to meet the remaining load on the zone being served by the unit ventilator.
-
-**Heating /With Coil/FixedAmount:** The unit is on, there is a heating load, a heating coil is present and is scheduled on, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. The heating coil then attempts to meet any remaining zone heating load.
-
-**Cooling/No Coil/VariablePercent:** The unit is on, there is a cooling load, no coil is present or it has been scheduled off, and variable percent outdoor air control type has been specified. In this case, the variable percent outdoor air controls what happens with the outdoor air. If the outside temperature is greater than the return temperature, then the outdoor air is set to the minimum as defined by the user input. If the outdoor air temperature is less than the return temperature from the zone, then the outdoor air is set to the maximum outdoor air flow rate as defined by the user. This may be somewhat simplistic in that it could result in overcooling of the space. However, since a temperature goal was not established, this is the best that can be done by the simulation. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outdoor air controls.
-
-**Cooling/No Coil/FixedTemperature:** The unit is on, there is a cooling load, no cooling coil is present or it has been scheduled off, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate in the same fashion as the variable percent outdoor air control.
-
-**Cooling/No Coil/FixedAmount:** The unit is on, there is a cooling load, no cooling coil is present or it has been scheduled off, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. Since a coil is not present to further condition the supply air, the zone simply receives whatever temperature air results from the outside air controls.
-
-**Cooling/With Coil/VariablePercent:** The unit is on, there is a cooling load, a coil is present and is scheduled on, and variable percent outdoor air control type has been specified. In this case, the percentage of outdoor air is set to the minimum flow outdoor air flow rate. The coil then attempts to meet any remaining zone load.
-
-**Cooling/With Coil/FixedTemperature:** The unit is on, there is a cooling load, a cooling coil is present and is scheduled on, and fixed temperature has been specified. The unit ventilator tries to use outdoor air as best as possible to meet the temperature goal. If it cannot meet this goal because the temperature goal is not between the zone return temperature and the outdoor air temperature, then the unit ventilator will either use the maximum or minimum outdoor air flow rate in the same fashion as the fixed temperature outdoor air control for the “no coil� conditions. The cooling coil then attempts to meet any remaining zone load.
-
-**Cooling/With Coil/FixedAmount:** The unit is on, there is a cooling load, a cooling coil is present and is scheduled on, and fixed amount control has been specified. The unit ventilator fixes the outdoor air flow rate as defined by the user and sets the maximum and minimum outdoor air flow rate to be equal in order to avoid the variation of outdoor air flow rate between the maximum and minimum values. The cooling coil then attempts to meet any remaining zone cooling load.
-
-Note: the unit ventilator controls are strictly temperature based and do not factor humidity into the equation (not an enthalpy economy cycle but rather a simple return air economy cycle). In addition, temperature predictions are not strict energy balances here in the control routine though in the mixing routine an energy balance is preserved.
-
-#### Field: Name
-
-This field is simply the identifying name that distinguishes one particular unit ventilator from another in the input data file. Like all other names in EnergyPlus, it is assumed that this is a unique character string and that no other unit ventilators use this same name.
-
-#### Field: Availability Schedule Name
-
-This field is a schedule name (ref: Schedule) that determines whether the unit ventilator is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Maximum Supply Air Flow Rate
-
-This field allows the user to enter the maximum volumetric flow rate of air through the unit ventilator system in m<sup>3</sup>/sec. This parameter should be some real number greater than zero.
-
-#### Field: Outdoor Air Control Type
-
-This field allows the user to control how outdoor air is used in the unit ventilator system. The unit ventilator system described by this syntax has its own outdoor air handler. The three options for outdoor air control are “**VariablePercent**�, “**FixedTemperature**� and “**FixedAmount**�. Those keys are the only allowed choices for this parameter. In general, the variable percent control will attempt to vary the amount of outdoor air between some minimum and maximum schedules of fractions (see next two fields) to best meet the current heating or cooling load. The fixed temperature control will vary the amount of outdoor air between the minimum schedule (fraction of maximum, see next field) and 100% available outdoor air to come as close as possible to a desired mixed air temperature (see 2 fields down) that can be scheduled. The fixed amount control will fix the outdoor air flow rate as minimum outdoor air flow rate and schedule specified by the user and automatically set the maximum and minimum outside flow rate to be equal by ignoring the maximum outdoor air flow rate. More information on the controls and operation of the unit ventilator are given in the introductory section above. For cycling fan operating mode, the outdoor air mass rate is capped by the actual supply air flow rate if the former is greater than the latter; otherwise, uses the amount calculated by the outdoor air control.
-
-#### Field: Minimum Outdoor Air Flow Rate
-
-This field allows the user to enter the minimum volumetric flow rate of outdoor air (in m<sup>3</sup>/sec) that will be brought in to the unit ventilator. The actual minimum outdoor air flow rate will be this number multiplied by the schedule value from the minimum outdoor air schedule. If “**FixedAmount**� type is selected as the outdoor air control strategy, the outdoor air flow rate will be fixed as this field and the unit ventilator will automatically set the maximum and minimum outside flow rate to be equal by ignoring the maximum outdoor air flow rate.
-
-#### Field: Minimum Outdoor Air Schedule Name
-
-This field contains a schedule name (ref: Schedule) that should contain values for the minimum outdoor air used by the unit ventilator system for IAQ or other reasons. Note that if the unit ventilator is scheduled off or if there is no load sensed in the zone that the system will not operate even to achieve the minimum air fraction. However, if the system is operating, it will always bring in this fraction of the minimum air flow rate (see minimum air flow rate field above). If “FixedAmount� type is selected as the outdoor air control strategy, the actual outdoor air flow rate will be this number multiplied by the minimum outdoor air flow rate in the field above. The unit ventilator will automatically set the maximum and minimum outdoor air schedule to be equal by ignoring the maximum outdoor air schedule.
-
-#### Field: Maximum Outdoor Air Flow Rate
-
-This field allows the user to enter the maximum volumetric flow rate of outdoor air that can be brought into the unit ventilator system in m<sup>3</sup>/sec. This parameter should be some real number greater than zero. Note that the value for this parameter may be less than the maximum air flow rate of the unit ventilator and this may affect the maximum fraction of outdoor air within the control strategy defined above. This parameter is an absolute maximum and will supercede any scheduled fraction of the unit ventilator maximum airflow rate. If “FixedAmount� type is selected as the outdoor air control strategy, this field will be ignored and be automatically set to be equal to the minimum outdoor air flow rate specified in the field above.
-
-#### Field: Maximum Outdoor Air Fraction or Temperature Schedule Name
-
-This field can have one of two meanings depending the type of control selected in the outdoor air control type parameter above. If “VariablePercent� or “FixedAmount� was selected, then this field is a schedule name (ref: Schedule) corresponding to a maximum air fraction schedule. Furthermore, if “FixedAmount� type is selected as the outdoor air control strategy, this field will be ignored and be automatically set to be equal to the minimum outdoor air fraction specified in the field below. Note that this is a fraction of the maximum airflow rate field (see parameter above) for the unit ventilator. If “FixedTemperature� control was selected, then this field is still a schedule name (ref: Schedule), but it corresponds to a schedule of mixed air temperatures that the outdoor air control will try to attain.
-
-#### Field: Air Inlet Node Name
-
-This field is a node name used to identify the node that serves as the inlet (air side) to the unit ventilator. In EnergyPlus, nodes represent points between components or at various points in the loops. In a unit ventilator, the air inlet node to the system will typically be the same node as a zone outlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
-
-#### Field: Air Outlet Node Name
-
-This field is a node name used to identify the node that serves as the outlet (air side) to the unit ventilator. In EnergyPlus, nodes represent points between components or at various points in the loops. In a unit ventilator, the air outlet node from the system will typically be the same node as a zone inlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
-
-#### Field: Outdoor Air Node Name
-
-This field is a node name used to identify the node associated with fresh air brought into the unit ventilator from the outdoor environment. You should also have defined an OutdoorAir:Node object with the same name and assign it an optional height (above ground).
-
-#### Field: Exhaust Air Node Name
-
-This field is a node name used to identify the node associated with air exhausted out of the unit ventilator to the outdoor environment. While from a simulation standpoint this name is arbitrary and not a “necessity�, assigning a name to this node allows the user to receive output on conditions at this node to verify the correct operation of the unit ventilator.
-
-#### Field: Mixed Air Node Name
-
-This field is a node name used to identify the node associated with the “mixed� air of the unit ventilator. These conditions are post-“mixing box� since they are the conditions of the fraction of return air combined with the outdoor air. Since this is a simple system, this can also be viewed as the conditions of the air being sent to the coils. While from a simulation standpoint this name is arbitrary and not a “necessity�, assigning a name to this node allows the user to receive output on conditions at this node to verify the correct operation of the unit ventilator.
-
-#### Field: Supply Air Fan Object Type
-
-This field specifies the type of supply air fan used by this unit ventilator. The supply air fan is part of the unit ventilator compound object. The only valid supply air fan types are:
-
-* Fan:OnOff
-
-* Fan:ConstantVolume
-
-* Fan:VariableVolume
-
-#### Field: Supply Air Fan Name
-
-This field is the name of a fan (ref: Fan:OnOff, Fan:ConstantVolume, Fan: VariableVolume) that is part of the unit ventilator system. This name links the unit ventilator to particular fan data entered elsewhere in the input data file. A fan name is required since it is the prime mover of air in the unit ventilator system.
-
-#### Field: Coil Option
-
-This field allows the user to specify the coil operating options as one of the following options: **None**, **Heating**, **Cooling** or **HeatingAndCooling**. If **None** is selected, the unit ventilator does not have any coils, and any other input will be ignored. If either **Heating** or **Cooling** is selected, only a heating or cooling coil, respectively, is present. Thus, only four more inputs will be expected. If **HeatingAndCooling** is selected, both heating and cooling coil input must be entered, and the unit ventilator will have both a heating and a cooling coil.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This field is a schedule name (ref: Schedule) that determines the operating modes of the unit ventilator’s On:Off fan. A schedule value of 0 indicates cycling fan operation (fan cycles with cooling/heating coil). A schedule value greater than 0 (usually 1 is used) indicates constant fan operation (fan runs continually regardless of the coils operation). If this input field is left blank, then the operating mode of the On:Off fan type defaults to cycling operation.
-
-#### Field: Heating Coil Object Type
-
-This field is the type of coil that is used for heating in the unit ventilator system. It is used in conjunction with the heating coil name (see next field) to specify the heating coil present within the system. Allowable heating coil types are:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Steam
-
-#### Field: Heating Coil Name
-
-This field is the name of the heating coil that is part of the unit ventilator system. It is assumed that there is always some sort of heating coil associated with a unit ventilator system. This name links the unit ventilator to particular heating coil data entered elsewhere in the input data file.
-
-#### Field: Heating Convergence Tolerance
-
-The control tolerance for the unit heating output. This field allows the user some control over how closely the heating coil will control the air side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in supply conditions (that could in turn result in excessive iterations). Initial experience with this parameter lends to the recommendation of using 0.001 as a starting point. This field is ignored for gas and electric heating coils.
-
-The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The heating convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {{Q_{UnitVentilator,Out}} - {Q_{ZoneLoad}}} \right|}}{{{Q_{ZoneLoad}}}} \le HeatingConvergenceTolerance\]</div>
-
-#### Field: Cooling Coil Object Type
-
-This field is the type of coil that is used for cooling in the unit ventilator system. It is used in conjunction with the cooling coil name (see next field) to specify the cooling coil present within the system.
-
-Only the following coil types can be used:
-
-* Coil:Cooling:Water
-
-* Coil:Cooling:Water:DetailedGeometry
-
-* CoilSystem:Cooling:Water:HeatExchangerAssisted
-
-#### Field: Cooling Coil Name
-
-This field is the name of the cooling coil that is part of the unit ventilator system. This name links the unit ventilator to particular cooling coil data entered elsewhere in the input data file. Note that a cooling coil is not a required part of a unit ventilator system. If no cooling coil is present, the previous field may be followed by a semi-colon and the remaining parameters in this statement may be ignored.
-
-#### Field: Cooling Convergence Tolerance
-
-The convergence tolerance for the unit cooling output. This field allows the user some control over how closely the cooling coil will control the air side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in supply conditions (that could in turn result in excessive iterations). Initial experience with this parameter lends to the recommendation of using 0.001 as a starting point.
-
-The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The cooling convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {{Q_{UnitVentilator,Out}} - {Q_{ZoneLoad}}} \right|}}{{{Q_{ZoneLoad}}}} \le CoolingConvergenceTolerance\]</div>
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this unit ventilator object’s fan. If the unit ventilator is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this unit ventilator object should be on or off.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Maximum Air Flow Rate in this Unit Ventilator zone HVAC object. The scaled Maximum Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
-
-
-
-An example input for a unit ventilator, including its constituent components, is shown below.
-
-```idf
-ZoneHVAC:UnitVentilator,
-    Zone1UnitVent,           !- Name
-    UnitVentAvailability,    !- Availability Schedule Name
-    0.84,                    !- Maximum Supply Air Flow Rate {m3/s}
-    VariablePercent,         !- Outdoor Air Control Type
-    0.168,                   !- Minimum Outdoor Air Flow Rate {m3/s}
-    UnitVentMinOA,           !- Minimum Outdoor Air Schedule Name
-    0.84,                    !- Maximum Outdoor Air Flow Rate {m3/s}
-    UnitVentMaxOA,           !- Maximum Outdoor Air Fraction or Temperature Schedule Name
-    Zone1UnitVentAirInletNode,  !- Air Inlet Node Name
-    Zone1UnitVentAirOutletNode,  !- Air Outlet Node Name
-    Zone1UnitVentOAInNode,   !- Outdoor Air Node Name
-    Zone1UnitVentExhNode,    !- Exhaust Air Node Name
-    Zone1UnitVentOAMixerOutletNode,  !- Mixed Air Node Name
-    Fan: ConstantVolume,     !- Supply Air Fan Object Type
-    Zone1UnitVentFan,        !- Fan Name
-    HeatingAndCooling,       !- Coil Option
-    Coil:Heating:Water,      !- Heating Coil Object Type
-    Zone1UnitVentHeatingCoil,!- Heating Coil Name
-    0.001,                   !- Heating Convergence Tolerance
-    Coil:Cooling:Water,      !- Cooling Coil Object Type
-    Zone1UnitVentCoolingCoil,!- Cooling Coil Name
-    0.001;                   !- Cooling Convergence Tolerance
-
-OutdoorAir:Node,
-    Zone1UnitVentOAInNode,   !- Name
-    -1.0;                    !- Height Above Ground {m}
-
-Fan:ConstantVolume,
-    Zone1UnitVentFan,        !- Name
-    UnitVentAvailability,    !- Availability Schedule Name
-    0.5,                     !- Fan Total Efficiency
-    75.0,                    !- Pressure Rise {Pa}
-    0.84,                    !- Maximum Flow Rate {m3/s}
-    0.9,                     !- Motor Efficiency
-    1.0,                     !- Motor In Airstream Fraction
-    Zone1UnitVentOAMixerOutletNode,  !- Fan Inlet Node Name
-    Zone1UnitVentFanOutletNode;  !- Fan Outlet Node Name
-
-Coil:Cooling:Water,
-    Zone1UnitVentCoolingCoil,!- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    0.0010,                  !- Design Water Flow Rate {m3/s}
-    0.84,                    !- Design Air Flow Rate {m3/s}
-    6.67,                    !- Design Inlet Water Temperature {C}
-    30,                      !- Design Inlet Air Temperature {C}
-    12,                      !- Design Outlet Air Temperature {C}
-    0.013,                   !- Design Inlet Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Design Outlet Air Humidity Ratio {kgWater/kgDryAir}
-    Zone1UnitVentChWInletNode,  !- Water Inlet Node Name
-    Zone1UnitVentChWOutletNode,  !- Water Outlet Node Name
-    Zone1UnitVentFanOutletNode,  !- Air Inlet Node Name
-    Zone1UnitVentCCOutletNode,  !- Air Outlet Node Name
-    SimpleAnalysis,          !- Type of Analysis
-    CrossFlow;               !- Heat Exchanger Configuration
-
-Coil:Heating:Water,
-    Zone1UnitVentHeatingCoil,!- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    400.,                    !- U-Factor Times Area Value {W/K}
-    0.0005,                  !- Maximum Water Flow Rate {m3/s}
-    Zone1UnitVentHWInletNode,!- Water Inlet Node Name
-    Zone1UnitVentHWOutletNode,  !- Water Outlet Node Name
-    Zone1UnitVentCCOutletNode,  !- Air Inlet Node Name
-    Zone1UnitVentAirOutletNode,  !- Air Outlet Node Name
-    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
-    autosize,                !- Nominal Capacity {W}
-    82.2,                    !- Design Inlet Water Temperature {C}
-    16.6,                    !- Design Inlet Air Temperature {C}
-    71.1,                    !- Design Outlet Water Temperature {C}
-    32.2;                    !- Design Outlet Air Temperature {C}
-```
-
-
-### Unit Ventilator Outputs
-
-* HVAC,Average,Zone Unit Ventilator Heating Rate [W]
-
-* HVAC,Sum,Zone Unit Ventilator Heating Energy [J]
-
-* HVAC,Average,Zone Unit Ventilator Total Cooling Rate [W]
-
-* HVAC,Sum,Zone Unit Ventilator Total Cooling Energy [J]
-
-* HVAC,Average,Zone Unit Ventilator Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Unit Ventilator Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Unit Ventilator Fan Electric Power[W]
-
-* HVAC,Sum,Zone Unit Ventilator Fan Electric Energy [J]
-
-* HVAC,Average,Zone Unit Ventilator Fan Availability Status []
-
-* HVAC,Average, Zone Unit Ventilator Fan Part Load Ratio []
-
-#### Zone Unit Ventilator Heating Rate [W]
-
-This field reports the heating output rate of the unit ventilator system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the unit ventilator.
-
-#### Zone Unit Ventilator Heating Energy [J]
-
-This field is the heating output of the unit ventilator system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit ventilator, and the timestep.
-
-#### Zone Unit Ventilator Total Cooling Rate [W]
-
-This field reports the total cooling (sensible plus latent) output rate of the unit ventilator system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the unit ventilator.
-
-#### Zone Unit Ventilator Total Cooling Energy [J]
-
-This field is the total cooling (sensible plus latent) output of the unit ventilator system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit ventilator, and the timestep.
-
-#### Zone Unit Ventilator Sensible Cooling Rate [W]
-
-This field reports the sensible cooling output rate of the unit ventilator system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the unit ventilator.
-
-#### Zone Unit Ventilator Sensible Cooling Energy [J]
-
-This field is the sensible cooling output of the unit ventilator system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit ventilator, and the timestep.
-
-#### Zone Unit Ventilator Fan Electric Power [W]
-
-This field reports the electric power consumption rate of the fan of the unit ventilator in Watts.
-
-#### Zone Unit Ventilator Fan Electric Energy [J]
-
-This field reports the electric power consumed by the fan of the unit ventilator over the timestep in Joules.
-
-#### Zone Unit Ventilator Fan Availability Status []
-
-This is the availability status of the unit ventilator fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the unit ventilator  object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-#### Zone Unit Ventilator Fan Part Load Ratio []
-
-This is the fan’s part load ratio for the report timestep during which the fan had operated. This variable is available for OnOff supply air fan type only.
-
-### ZoneHVAC:UnitHeater
-
-Unit heaters are zone equipment units which are assembled from other components and are a simplification of unit ventilators. They contain only a fan and a heating coil. These components are described elsewhere in this document. The unit heater input simply requires the names of these components, which have to be described elsewhere in the input. The input also requires the name of an availability schedule, maximum airflow rate, and maximum and minimum hot water volumetric flow rates. The unit is connected to the zone inlet and exhaust nodes by specifying unit inlet and outlet node names. Note that the unit air inlet node should be the same as a zone exhaust node and the unit outlet node should be the same as a zone inlet node.
-
-While the control of the heating coil is similar to the fan coil units and the unit ventilator, the overall control of the unit heater is much different. There are four different modes in which a unit heat can operate based on the user input:
-
-**Off:** Unit is schedule off. All flow rates are set to zero and the temperatures are set to zone conditions.
-
-**NoLoad OR Cooling/�No�** is specified in input field “Supply Air Fan Operation During No Heating�**:** Unit is available, but there is no heating load. With “No� specified for “Supply Air Fan Operation During No Heating� and the supply fan operating mode set to 0, the fan will be off since there is no heating load. All flow rates are set to zero and the temperatures are set to zone conditions.
-
-**NoLoad OR Cooling/�Yes�** is specified in input field “Supply Air Fan Operation During No Heating�**:** Unit is available, the supply fan operating mode schedule value is greater than 0 (for OnOff Fan) and the fan is running (if it is scheduled to be available also). No heating is provided, only air circulation via the fan running. However, any heat added by the fan is introduced into the space with the circulation of the air.
-
-**Heating:** The unit is on/available and there is a heating load. The heating coil is modulated (constant fan speed) to meet the heating load. When the fan type is not an OnOff fan then the  control of the heating coil and its flow rate is identical to the fan coil unit. In the case of OnOff fan, the fan cycles with heating coil if the current timestep supply fan operating mode is schedule value is 0, or else if the current timestep supply fan operating mode schedule value is greater than 0, then the supply fan runs continuously for the entire timestep.
-
-#### Field: Name
-
-This field is simply the identifying name that distinguishes one particular unit heater from another in the input data file. Like all other names in EnergyPlus, it is assumed that this is a unique character string and that no other unit heaters use this same name.
-
-#### Field: Availability Schedule Name
-
-This field is a schedule name (ref: Schedule) that determines whether the unit heater is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the component can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the component must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Inlet Node Name
-
-This field is a node name used to identify the node that serves as the inlet (air side) to the unit heater. In EnergyPlus, nodes represent points between components or at various points in the loops. In a unit heater, the air inlet node to the system will typically be the same node as a zone outlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
-
-#### Field: Air Outlet Node Name
-
-This field is a node name used to identify the node that serves as the outlet (air side) to the unit heater. In EnergyPlus, nodes represent points between components or at various points in the loops. In a unit heater, the air outlet node from the system will typically be the same node as a zone inlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
-
-#### Field: Supply Air Fan Object Type
-
-This field specifies the type of supply air fan used by this unit heater. The supply air fan is part of the unit heater compound object. The only valid supply air fan types are:
-
-* Fan:OnOff
-
-* Fan:ConstantVolume
-
-* Fan:VariableVolume
-
-#### Field: Supply Air Fan Name
-
-This field is the name of a fan (ref: Fan:ConstantVolume, Fan:VariableVolume) that is part of the unit heater system. This name links the unit heater to particular fan data entered elsewhere in the input data file. A fan name is required since it is the prime mover of air in the unit heater system.
-
-#### Field: Maximum Supply Air Flow Rate
-
-This field allows the user to enter the maximum volumetric flow rate of air through the unit heater system in m<sup>3</sup>/s. This parameter should be some real number greater than zero.
-
-#### Field: Heating Coil Object Type
-
-This field is the type of coil that is used for heating in the unit heater system. It is used in conjunction with the heating coil name (see next field) to specify the heating coil present within the system. Allowable heating coil types are:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Steam
-
-#### Field: Heating Coil Name
-
-This field is the name of the heating coil that is part of the unit heater system. It is assumed that there is always some sort of heating coil associated with a unit heater system. This name links the unit ventilator to particular heating coil data entered elsewhere in the input data file.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This field is a schedule name (ref: Schedule) that determines the operating modes of the unit heater’s On:Off fan. A schedule value of 0 indicates cycling fan operation (fan cycles with cooling/heating coil). A schedule value greater than 0 (usually 1 is used) indicates constant fan operation (fan runs continually regardless of the coils operation). If this input field is left blank, then the operating mode of the On:Off fan type defaults to cycling operation.
-
-#### Field: Supply Air Fan Operation During No Heating
-
-This choice field allows the user to define how the unit heater will operate under “no heating load� or cooling conditions. The user may select from two options (“Yes�, “No�). If the “**No**� control is selected, then the fan will not run unless there is a heating load. If the fan does not run, this effectively shuts the unit heater system off. If the “**Yes**� control is selected, the unit heater is available, and the fan is continuous, then the fan will always run. This will produce air movement in the zone but also add some amount of heat to the energy balance since the fan generates some heat. But if the “**Yes**� control is selected and the “Supply Air Fan Operating Mode Schedule� values is 0 (for OnOff fan), then the fan will NOT run.  This allows the user to schedule the operation of the fan when there is no load.
-
-#### Field: Maximum Hot Water or Steam Flow Rate
-
-This field allows the user to enter a maximum hot water or steam volumetric flow rate through the heating coil in m<sup>3</sup>/s. The steam volume flow rate is calculated at 100C and 101325 Pa. This number should be some number greater than zero and greater than the minimum hot water or steam volumetric flow rate (see next field). Note that this parameter has no meaning for either an electric or a gas heating coil.
-
-#### Field: Minimum Hot Water or Steam Flow Rate
-
-This field allows the user to enter a minimum hot water or steam volumetric flow rate through the heating coil in m<sup>3</sup>/s. The steam volume flow rate is calculated at 100C and 101325 Pa. This number should be some number greater than zero and less than the maximum hot water or steam volumetric flow rate (see previous field). Note that this parameter has no meaning for either an electric or a gas heating coil.
-
-#### Field: Heating Convergence Tolerance
-
-The convergence tolerance for the unit heating output. This field allows the user some control over how closely the heating coil will control the air side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in supply conditions (that could in turn result in excessive iterations). Initial experience with this parameter lends to the recommendation of using 0.001 as a starting point. This field is ignored for gas and electric heating coils.
-
-The unit is controlled by matching the unit output to the zone demand. For units with water coils, the model must be numerically inverted to obtain a specified output. The heating convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {{Q_{unit{\kern 1pt} heater,out}} - {Q_{zoneload}}} \right|}}{{{Q_{zoneload}}}} \le HeatingConvergenceTolerance\]</div>
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this unit heater object’s fan. If the unit heater is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this unit heater object should be on or off.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields *Maximum Supply Air Flow Rate* in this Unit Heater zone HVAC object. The scaled maximum supply air flow rates is used to size Maximum Hot Water or Steam Flow Rate if specified as autosize. The scaled Maximum Air Flow Rate in turn is used to size heating capacity of the unit.
-
-
-
-An example input for a unit heater, including its constituent components, is shown below.
-
-```idf
-ZoneHVAC:UnitHeater,
-    Zone1UnitHeat,           !- Name
-    UnitHeatAvailability,    !- Availability Schedule Name
-    Zone1UnitHeatAirInletNode,  !- Air Inlet Node Name
-    Zone1UnitHeatAirOutletNode,  !- Air Outlet Node Name
-    Fan: ConstantVolume,     !- Supply Air Fan Object Type
-    Zone1UnitHeatFan,        !- Fan Name
-    0.84,                    !- Maximum Supply Air Flow Rate {m3/s}
-    Continuous,              !- Fan Control Type
-    Coil:Heating:Water,      !- Heating Coil Object Type
-    Zone1UnitHeatHeatingCoil,!- Heating Coil Name
-    0.0005,                  !- Maximum Hot Water or Steam Flow Rate {m3/s}
-    0.0,                     !- Minimum Hot Water or Steam Flow Rate {m3/s}
-    0.001;                   !- Heating Convergence Tolerance
-
-
-Fan:ConstantVolume,
-    Zone1UnitHeatFan,        !- Name
-    UnitHeatAvailability,    !- Availability Schedule Name
-    0.5,                     !- Fan Total Efficiency
-    75.0,                    !- Pressure Rise {Pa}
-    0.84,                    !- Maximum Flow Rate {m3/s}
-    0.9,                     !- Motor Efficiency
-    1.0,                     !- Motor In Airstream Fraction
-    Zone1UnitHeatAirInletNode,  !- Fan Inlet Node Name
-    Zone1UnitHeatFanOutletNode;  !- Fan Outlet Node Name
-
-
-Coil:Heating:Water,
-    Zone1UnitHeatHeatingCoil,!- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    400.,                    !- U-Factor Times Area Value {W/K}
-    0.0005,                  !- Maximum Water Flow Rate {m3/s}
-    Zone1UnitHeatHWInletNode,!- Water Inlet Node Name
-    Zone1UnitHeatHWOutletNode,  !- Water Outlet Node Name
-    Zone1UnitHeatFanOutletNode,  !- Air Inlet Node Name
-    Zone1UnitHeatAirOutletNode,  !- Air Outlet Node Name
-    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
-    autosize,                !- Nominal Capacity {W}
-    82.2,                    !- Design Inlet Water Temperature {C}
-    16.6,                    !- Design Inlet Air Temperature {C}
-    71.1,                    !- Design Outlet Water Temperature {C}
-    32.2;                    !- Design Outlet Air Temperature {C}
-```
-
-
-
-
-### Unit Heater Outputs
-
-* HVAC,Average,Zone Unit Heater Heating Rate [W]
-
-* HVAC,Sum,Zone Unit Heater Heating Energy [J]
-
-* HVAC,Average,Zone Unit Heater Fan Electric Power[W]
-
-* HVAC,Sum,Zone Unit Heater Fan Electric Energy [J]
-
-* HVAC,Average, Zone Unit Heater Fan Availability Status []
-
-* HVAC,Average, Zone Unit Heater Fan Part Load Ratio []
-
-#### Zone Unit Heater Heating Rate [W]
-
-This field reports the heating output rate of the unit heater system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the unit heater.
-
-#### Zone Unit Heater Heating Energy [J]
-
-This field is the heating output of the unit heater system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit heater, and the timestep.
-
-#### Zone Unit Heater Fan Electric Power [W]
-
-This field reports the electric power consumption rate of the fan of the unit heater in Watts.
-
-#### Zone Unit Heater Fan Electric Energy [J]
-
-This field reports the electric power consumed by the fan of the unit heater over the timestep in Joules.
-
-#### Zone Unit Heater Fan Availability Status []
-
-This is the availability status of the unit heater fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the unit heater  object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-#### Zone Unit Heater Fan Part Load Ratio []
-
-This is the fan’s part load ratio for the report timestep during which the fan had operated. This variable is available for OnOff supply air fan type only.
-
-### ZoneHVAC:EvaporativeCoolerUnit
-
-The zone evaporative cooler unit is a compound object made up of a fan and one or two evaporative cooler components.  This unit serves a single thermal zone as a forced-convection, cooling-only unit with supply fan.  It always draws 100% of its supply air from the outside, passes the air through a supply fan and evaporative cooler(s) and then into the zone.  The fan can be positioned upstream of the cooler(s) for a blow through placement.  Or it can be positioned downstream of the cooler(s) for a draw through placement.  If there is more than one evaporative cooler, then should be in series with the first cooler immediately upstream of the second cooler. There is an option to include a relief zone exhaust node to balance the air in the zone.
-
-The unit can have either constant or variable speed fans.  This zone unit differs from other constant speed forced-air zone units in that its controls are not based on a part-load formulation with averaged air flow rates. Instead the unit is completely on or off during the entire timestep.  This means that it is beneficial to use relatively short timesteps. However for variable speed fans, the unit can modulate fan speed to just meet cooling loads and therefore operates similar to other zone HVAC units.
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a zone evaporative cooler unit.  References to this unit by other objects will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of a schedule that denotes whether the unit operates during a given time period. A schedule value equal to 0.0 denotes that the cooler unit must be off for that time period. A schedule value greater than 0.0 denotes that the cooler is available to operate during that time period. If this field is left blank, then the program assumes that the unit is always available as if the schedule was always set to 1.0.
-
-#### Field: Availability Manager List Name
-
-This optional alpha input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name.  The availability managers in the list apply to this evaporative cooler unit’s operation. If this field is used and the cooler unit is scheduled to be available, based on the previous input field, then the unit will operate based on the result of the availability managers in the list.
-
-#### Field: Outdoor Air Inlet Node Name
-
-This alpha input field defines the name of the HVAC system node from which the evaporative cooler unit draws its supply air.  This node is usually declared to be an outdoor air node using OutdoorAir:Node or OutdoorAir:NodeList.
-
-#### Field: Cooler Outlet Node Name
-
-This alpha input field defines the name of the HVAC system node to which the evaporative cooler sends its outlet air.  This node name must be the name of a zone air inlet node (Ref. ZoneHVAC:EquipmentConnections).
-
-#### Field: Zone Relief Air Node Name
-
-This optional alpha input field defines the name of an HVAC system node which can extract air from the zone to balance the air supplied to the zone by the cooler outlet node.  This node name would match the name of a zone exhaust air node.
-
-#### Field: Supply Air Fan Object Type
-
-This alpha input field defines the type of fan used by the zone evaporative cooler unit.  There are four valid choices: Fan:ConstantVolume, Fan:OnOff, Fan:VariableVolume, or Fan:ComponentModel.  However the type of fan must be consistent with the control method defined below and a variable speed fan is needed with ZoneCoolingLoadVariableSpeedFan.
-
-#### Field: Supply Air Fan Name
-
-This alpha input field defines the user-defined name of the fan used by this cooler unit. The fan itself is defined elsewhere.  Note that the fan’s maximum flow rate should be greater than or equal to the Design Supply Air Flow Rate defined in the following field.  For a blow-through fan placement, the fan’s inlet node should be the same as the Outlet Air Inlet Node Name. For a draw-through fan placement, the fan’s outlet node should be the same as the Cooler Outlet Node Name.
-
-#### Field: Design Supply Air Flow Rate [m<sup>3</sup>/s]
-
-This numeric input field defines the evaporative cooler unit’s design supply air flow rate, in cubic meters per second.  This value is typically consistent with the maximum air flow rate of the fan, but it can be less if desired.
-
-#### Field: Fan Placement
-
-This alpha input field defines how the supply fan is arranged.  There are two choices, BlowThrough or DrawThrough.  The BlowThrough choice indicates that the fan is located upstream of the evaporative cooler(s). The DrawThrough choice indicates that the fan is located downstream of the evaporative cooler(s). These are the only configurations that are available and the HVAC system nodes used as inlets and outlet in the components must be arranged consistent with the flow path.
-
-#### Field: Cooler Unit Control Method
-
-This alpha field is used to determine how the unit is to be controlled.  There are three possible choices:
-
-- **ZoneTemperatureDeadbandOnOffCycling**. This control method determines whether or not to operate the cooler based on the thermostat setpoint and the zone air temperature.  This thermostatic control method uses a throttling temperature range, determined in the following input field, to model hysteresis-type control to avoid excessive short-cycling.  If the zone air temperature is warmer than the cooling setpoint temperature plus one-half of the throttling range, then the unit is operated for the entire timestep at the design air mass flow rate.  If the zone air temperature is cooler than the cooling setpoint temperature minus one-half of the throttling range, then the unit is off for the entire timestep.  When the zone air temperatures are within the throttling range, then the unit will stay off if it was not running during the previous timestep and will stay on if it was already running. This control method does not usually behave in a smooth manner and zone conditions will tend to oscillate considerably during periods of low load.
-
-- **ZoneCoolingLoadOnOffCycling**. This control method determines whether or not to operate the cooler based on the predicted zone load to cooling setpoint.  If there is a cooling load (and the unit is available), then the unit is operated for the entire timestep at the design air mass flow rate. If there is no cooling load, then the unit is not operated at all.  The magnitude of the cooling load that will trigger the unit to operate can be controlled using the field below called Cooling Load Control Threshold Heat Transfer Rate. This control method does not usually behave in a smooth manner and zone conditions will tend to oscillate considerably during periods of low load.
-
-- **ZoneCoolingLoadVariableSpeedFan**.  This control method determines whether or not to operate the cooler based on the predicted zone load to cooling setpoint.  If there is a cooling load (and the unit is available), then the unit is operated for the entire timestep at a fan speed that is controlled to meet the sensible cooling load (if possible). The magnitude of the cooling load that will trigger the unit to operate can be controlled using the field below called Cooling Load Control Threshold Heat Transfer Rate.  This control method requires a variable speed fan and cannot be used with Fan:ConstantVolume or Fan:OnOff.
-
-#### Field: Throttling Range Temperature Difference [DeltaC]
-
-This numeric input field defines the throttling range to use for zone-temperature based control, in degrees Celsius. This value is used when the unit’s control method is ZoneTemperatureDeadbandOnOffCycling.  This temperature range is used for hysteresis thermostatic control.  It is modeled as symmetric about the cooling setpoint. The default is 1.0°C.
-
-#### Field: Cooling Load Control Threshold Heat Transfer Rate [W]
-
-This numeric input field defines the magnitude, in Watts, of a significant zone cooling load to use with zone-load-to-setpoint based control.  This value is used when the unit’s control method is ZoneCoolingLoadOnOffCycling or ZoneCoolingLoadVariableSpeedFan.  This is a sensible cooling load that is used as a threshold to determine when the cooling load is significant.  When the predicted zone load to cooling setpoint is less than this threshold, the cooler unit’s control will consider the load to be too small to trigger operation. The default is 100W.
-
-#### Field: First Evaporative Cooler Object Type
-
-This alpha input field defines the type of evaporative cooler used in the unit. The zone evaporative cooler unit can have one or two separate cooler components and this field is for the first cooler. There are five types of evaporative cooler component models to choose from: EvaporativeCooler:Direct:CelDekPad, EvaporativeCooler:Direct:ResearchSpecial, EvaporativeCooler:Indirect:CelDekPad, EvaporativeCooler:Indirect:WetCoil, or EvaporativeCooler:Indirect:ResearchSpecial.
-
-#### Field: First Evaporative Cooler Object Name
-
-This alpha input field defines the user-defined name of the first evaporative cooler component used by this zone unit.  The cooler component itself is defined elsewhere. For a blow through fan placement, the inlet node for the evaporative cooler should be the same as the fan’s outlet node.  For a draw through fan placement, the inlet node for the evaporative cooler should be the same as the unit’s Outdoor Air Inlet Node Name.
-
-#### Field: Second Evaporative Cooler Object Type
-
-This optional alpha input field defines the type of evaporative cooler used in the unit. This field is used when the zone evaporative cooler unit has two separate evaporative cooler sections arranged in series. For example, some coolers are arranged with both direct and indirect evaporative coolers. If the unit has only one type of cooler, this field should be left blank. There are five types of evaporative cooler component models to choose from: EvaporativeCooler:Direct:CelDekPad, EvaporativeCooler:Direct:ResearchSpecial, EvaporativeCooler:Indirect:CelDekPad, EvaporativeCooler:Indirect:WetCoil, or EvaporativeCooler:Indirect:ResearchSpecial
-
-#### Field: Second Evaporative Cooler Name
-
-This optional alpha input field defines the user-defined name of the second evaporative cooler component used by this zone unit.  The cooler component itself is defined elsewhere. The inlet node for the second evaporative cooler should be the same as the outlet node for the first evaporative cooler.  For a draw through fan placement, the outlet node for the second evaporative cooler should be the same as the unit’s fan inlet node.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object defined elsewhere. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input field *Design Supply Air Flow Rate* in Evaportaive Cooler zone HVAC object. The scaled design supply air flow rates in turn is used to size capacity of the unit.
-
-
-
-An example input object follows.
-
-```idf
-ZoneHVAC:EvaporativeCoolerUnit,
-   Zone Evap Unit, !- Name
-   System Availability Schedule , !- Availability Schedule Name
-   , !- Availability Manager List Name
-   Cooler Unit OA inlet , !- Outdoor Air Inlet Node Name
-   Main Zone Inlet Node, !- Cooler Outlet Node Name
-   Main Zone Relief Node , !- Zone Relief Air Node Name
-   Fan:ConstantVolume , !- Supply Air Fan Object Type
-   Supply Fan , !- Supply Air Fan Name
-   2.0, !- Design Supply Air Flow Rate
-   DrawThrough , !- Fan Placement
-   ZoneCoolingLoadOnOffCycling, !- Cooler Unit Control Method
-   1.1, !- Throttling Range Temperature Difference
-   100.0, !- Cooling Load Control Threshold Heat Transfer Rate
-   EvaporativeCooler:Direct:CelDekPad, !- First Evaporative Cooler Object Type
-   Evaporative Cooler, !- First Evaporative Cooler Object Name
-    , !- Second Evaporative Cooler Object Type
-    ; !- Second Evaporative Cooler Name
-```
-
-
-### ZoneHVAC:EvaporativeCoolerUnit Outputs
-
-* HVAC,Average,Zone Evaporative Cooler Unit Total Cooling Rate [W]
-
-* HVAC,Sum,Zone Evaporative Cooler Unit Total Cooling Energy [J]
-
-* HVAC,Average,Zone Evaporative Cooler Unit Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Evaporative Cooler Unit Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Evaporative Cooler Unit Latent Heating Rate [W]
-
-* HVAC,Sum,Zone Evaporative Cooler Unit Latent Heating Energy [J]
-
-* HVAC,Average,Zone Evaporative Cooler Unit Latent Cooling Rate [W]
-
-* HVAC,Sum,Zone Evaporative Cooler Unit Latent Cooling Energy [J]
-
-* HVAC,Average,Zone Evaporative Cooler Unit Fan Speed Ratio []
-
-* HVAC,Average,Zone Evaporative Cooler Unit Fan Availability Status []
-
-
-#### Zone Evaporative Cooler Unit Total Cooling Rate [W]
-
-This output is the total (enthalpy) heat extraction rate of the zone evaporative cooler unit from the zone it is serving, in Watts.  This value is calculated using the enthalpy difference of the unit outlet air node and the zone air node and the air mass flow rate entering the zone.
-
-#### Zone Evaporative Cooler Unit Total Cooling Energy [J]
-
-This output is the total (enthalpy) heat extraction of the zone evaporative cooler unit from the zone it is serving, in Joules.  This value is calculated using the enthalpy difference of the unit outlet air node and the zone air node and the air mass flow rate entering the zone.
-
-#### Zone Evaporative Cooler Unit Sensible Cooling Rate [W]
-
-This output is the moist air sensible-only heat extraction rate of the zone evaporative cooler unit from the zone it is serving, in Watts. This value is calculated using the enthalpy difference of the unit outlet air node and the zone air node based on a single, minimum humidity ratio along with the air mass flow rate entering the zone.
-
-#### Zone Evaporative Cooler Unit Sensible Cooling Energy [J]
-
-This output is the moist air sensible-only heat extraction of the zone evaporative cooler unit from the zone it is serving, in Joules. This value is calculated using the enthalpy difference of the unit outlet air node and the zone air node based on a single, minimum humidity ratio along with the air mass flow rate entering the zone.
-
-#### Zone Evaporative Cooler Unit Latent Heating Rate [W]
-
-This output is the latent heat addition (humidification) rate of the zone evaporative cooler unit to the zone it is serving in Watts.  This value is calculated as the difference between the total cooling rate and the sensible cooling rate.  Because an evaporative cooler can provide sensible cooling while adding moisture the zone air, a unit can operate with both a positive sensible cooling load and a positive latent heating rate.
-
-#### Zone Evaporative Cooler Unit Latent Heating Energy [J]
-
-This output is the latent heat addition (humidification) of the zone evaporative cooler unit to the zone it is serving in Joules.  This value is calculated as the difference between the total cooling energy and the sensible cooling energy.
-
-#### Zone Evaporative Cooler Unit Latent Cooling Rate [W]
-
-This output is the latent heat extraction (dehumidification) rate of the zone evaporative cooler unit to the zone it is serving in Watts.  This value is calculated as the difference between the total cooling rate and the sensible cooling rate.
-
-#### Zone Evaporative Cooler Unit Latent Cooling Energy [J]
-
-This output is the latent heat extraction (dehumidification) of the zone evaporative cooler unit to the zone it is serving in Joules.  This value is calculated as the difference between the total cooling energy and the sensible cooling energy.
-
-#### Zone Evaporative Cooler Unit Fan Speed Ratio [ ]
-
-This output is the speed ratio of the fan for the zone evaporative cooler unit.  The speed ratio is defined as the current supply air mass flow rate divided by the design air mass flow rate.
-
-#### Zone Evaporative Cooler Unit Fan Availability Status [ ]
-
-This output is the availability status of the zone evaporative cooler unit’s fan.  This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object.  The AvailabilityManagerAssignmentList is an optional input in the zone evaporative cooler object.  When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific manager.  For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager)), rules to determine fan availability status are described in the section on system availability managers.  The control status outputs are represented using integers 0 through 3.  These integers represent NoAction (0), ForceOff (1), CycleOn(2), and CycleOneZoneFansOnly (3).  It is recommend to report this output at the “Detailed� frequency because the integer status flags do not average out to meaningful values.
-
-### ZoneHVAC:OutdoorAirUnit
-
-The zone outdoor air unit (ZoneHVAC:OutdoorAirUnit) in EnergyPlus is intended to model dedicated outdoor air systems (DOAS) and other similar systems which aim to provide either additional outside air or some limited amount of sensible and/or latent conditioning.  The zone outdoor air unit is a piece of zone equipment that can consist of a supply fan, an exhaust fan (optional), heating and cooling coils, and heat recovery.  The outdoor air unit input simply requires information about flow rates, schedules, node names, and a list of component that are part of the unit.  These components require additional input as per the requirements for these components.  In addition, the input includes information about controls for the unit.  It should be noted that the components that make up the zone outdoor air unit do not require additional controls or setpoints.  The unit input defines how the unit outlet temperature is controlled as described below.
-
-![](media/image282.png)
-
-Figure 110. Zone Outdoor Air Unit Schematic
-
-Zones may contain one or more zone outdoor air units.  The user can choose to have each unit have its own exhaust fan or may choose to have only one unit have a exhaust fan that will handle the flow of all of the zone outdoor air units.  Note that the user will need to account for any flow balance among the zone outdoor air units on the supply and exhaust sides.
-
-The full input for zone outdoor air units is described below using a variety of fields.
-
-#### Field: Name
-
-This field is simply the identifying name that distinguishes one particular outdoor air unit from another in the input data file. Like all other names in EnergyPlus, it is assumed that this is a unique character string and that no other zone outdoor air units use this same name.
-
-#### Field: Availability Schedule Name
-
-This field is a schedule name (ref: Schedule) that determines whether the zone outdoor air unit is available to operate. A schedule value greater than 0 (usually 1 is used) indicates that the outdoor air unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the outdoor air unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods. For any schedule value greater than zero, the outdoor air unit is considered available and will operate at the supply and exhaust flow rates defined by input field described below.
-
-#### Field: Zone Name
-
-This field is the name of the zone (Ref: Zone) in which the outdoor air unit is located and intended to affect.  Zone outdoor air units impact only a single zone.
-
-#### Field: Outdoor Air Flow Rate
-
-This field allows the user to enter the volumetric flow rate of outdoor air (in m<sup>3</sup>/sec) that will be brought in through the outdoor air unit. The actual outdoor air flow rate will be this number multiplied by the schedule value from the outdoor air schedule. This field is autosizable.  When autosized, the unit’s outdoor air flow rate will match the minimum outdoor air requirements specified through the Sizing:Zone object.
-
-#### Field: Outdoor Air Schedule Name
-
-This field contains a schedule name (ref: Schedule) that contains values for modifying the outdoor air flow rate.  The supply air flow rate is the product of the outdoor air flow rate and the outdoor air schedule value for the time of interest.  Note that if the outdoor air unit is scheduled off that the system will not operate regardless of the outdoor air schedule value. However, if the system is operating, it will always bring in this fraction of the outdoor air flow rate.
-
-#### Field: Supply Fan Name
-
-This field is the name of a fan (ref: Fan:ConstantVolume, Fan: VariableVolume) that is part of the zone outdoor air unit. This name links the outdoor air unit to particular fan data entered elsewhere in the input data file. A fan name is required since it is the prime mover of air in the outdoor air control unit.
-
-#### Field: Fan Placement
-
-This field has two choices: **BlowThrough** or **DrawThrough**. The first choice stands for “blow through fan�. It means that the unit consists of outdoor air node followed by a supply fan followed by the equipment that are part of the system. The second choice stands for “draw through fan�. It means that the supply fan placed at the end of supply air stream and supply fan outlet node is identified with the air outlet node. The fan “draws air through� the equipment system.
-
-* BlowThrough
-
-* DrawThrough
-
-If the user does not select a fan placement type, **DrawThrough** is assumed as default by EnergyPlus.
-
-#### Field: Exhaust Fan Name
-
-This field is the name of a fan (ref: Fan:ConstantVolume, Fan: VariableVolume) that is part of the outdoor air unit. This name links the outdoor air unit to particular fan data entered elsewhere in the input data file. This field is optional.
-
-#### Field: Exhaust Air Flow Rate
-
-This field allows the user to enter the volumetric flow rate of air (in m<sup>3</sup>/sec) that will be exhausted to the outdoors. The actual exhaust air flow rate will be this number multiplied by the schedule value from the exhaust air schedule. If the exhaust fan name is left blank, this field will be ignored and automatically set to be equal to zero.
-
-#### Field: Exhaust Air Schedule Name
-
-This field contains a schedule name (ref: Schedule) that should contain values for modifying the exhaust air flow rate.  The actual exhaust air flow rate equals the exhaust air flow rate input (previous field) multiplied by the exhaust air schedule value. If the exhaust fan name is left blank, this field will be ignored and automatically set to be equal to zero.
-
-#### Field: Unit Control Type
-
-The unit control type field determines with conditions in the zone being served what the response of the zone outdoor air system will be. It is important to note that this only controls the temperature of the air being delivered to the space not whether or not the system will operate.  There are two options for this field: Neutral or Temperature. Neutral control tries to have no energy impact on the zone by delivering air at the temperature of the zone. This allows air to be delivered to the zone without affecting the zone air heat balance and thus provides outside air without impacting any other system providing conditioning to this zone. The temperature control option will supply air to the zone based on the high and low air control temperature schedules (see next two fields). For temperature control, when the outside air temperature is less than the low air control temperature, the zone outdoor air unit will provide whatever heating is available from its components to achieve the low air temperature value.  When the outside air temperature is above the high air control temperature, the zone outdoor air unit will provide whatever cooling is available from its components to achieve the high air temperature value.  When the outdoor air temperature is between the high and low air control temperatures, the unit will simply provide air at whatever the outdoor air conditions are, modified by any fan heat added by the supply fan. In summary, the user must select from the following two options:
-
-* NeutralControl
-
-* TemperatureControl
-
-If the user does not select a unit control type, **NeutralControl** is assumed as the default by EnergyPlus.
-
-#### Field: High Air Control Temperature Schedule Name
-
-This field specifies the dry-bulb air temperature in degrees Celsius for the supply air temperature to the zone. When the outdoor air temperature or post-supply fan outlet temperature in the case of blow through is above the high air control temperature, a cooling coil, if available and specified by the user, is tuned on to conditioning the outdoor air to the high control temperature. This field only applies to zone outdoor air units that use Temperature Control (see previous field).
-
-#### Field: Low Air Control Temperature Schedule Name
-
-This field specifies the dry-bulb air temperature in degrees Celsius for the supply air temperature to the zone. When the outdoor air temperature or post-supply fan outlet temperature is below the low air control temperature, a heating coil, if available and specified by the user, is tuned on to conditioning the outdoor air to the low control temperature. This field only applies to zone outdoor air units that use Temperature Control (see two previous fields).
-
-#### Field: Outdoor Air Node Name
-
-This field is a node name used to identify the node associated with fresh air brought into the outdoor air unit from the outdoor environment. It should also be defined in an OutdoorAir:Node object with the same name and assigned an optional height (above ground).
-
-#### Field: Air Outlet Node Name
-
-This field is a node name used to identify the node that serves as the outlet (air side) from the zone outdoor air unit. In EnergyPlus, nodes represent points between components or at various points in the loops. In an outdoor air unit, the air outlet node from the system will typically be the same node as a zone inlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
-
-#### Field: Air Inlet Node Name
-
-This field is a node name used to identify the node that serves as the inlet (air side) to the exhaust side of the outdoor air unit. In EnergyPlus, nodes represent points between components or at various points in the loops. In an outdoor air unit, the air inlet node of the system will typically be the same node as a zone outlet node. While a node name may be referenced more than once in an input data file, each node must have a unique name.
-
-#### Field: Supply Fan Outlet Node Name
-
-This field is a node name used to identify the node that serves as the outlet (air side) of the supply fan for the zone outdoor air unit. In EnergyPlus, nodes represent points between components or at various points in the loops. While a node name may be referenced more than once in an input data file, each node must have a unique name.
-
-#### Field: Outdoor Air Unit List Name
-
-This field is the name of an ZoneHVAC:OutdoorAirUnit:EquipmentList object. An ZoneHVAC:OutdoorAirUnit:EquipmentList  is simply a list of components giving both component name and type. This equipment list specifies all the components that will be simulated in this unit. The order of the components in the list is significant: components are simulated sequentially in the order given in the Equipment List.
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this outdoor air unit  object’s fan. If the outdoor air unit is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this outdoor air unit  object should be on or off.
-
-An example of this object defined in an input data file is shown below**:**
-
-```idf
-ZoneHVAC:OutdoorAirUnit,
-    Zone5DXOutAir,           !- Name
-    OAUnitOASched,           !- Availability Schedule Name
-    SPACE5-1,                !- Zone Name
-    0.42,                    !- Outdoor Air Flow Rate {m3/s}
-    OAUnitOASched,           !- Outdoor Air Schedule Name
-    Zone5OAUFan1,            !- Supply Fan Name
-    BlowThrough,             !- Supply Fan Placement
-    ,                        !- Exhaust Fan Name
-    ,                        !- Exhaust Air Flow Rate {m3/s}
-    ,                        !- Exhaust Air Schedule Name
-    TemperatureControl,      !- Unit Control Type
-    OAUHitemp2,              !- High Air Control Temperature Schedule Name
-    OAULotemp2,              !- Low Air Control Temperature Schedule Name
-    Zone5OAUOANode,          !- Outdoor Air Node Name
-    Zone5OAUZoneInletNode,   !- AirOutlet Node Name
-    Zone5OAUZoneOutletNode,  !- AirInlet Node Name
-    Zone5OAUFanOutletNode,   !- Supply FanOutlet Node Name
-    Zone5OAUEquip1;          !- Outdoor Air Unit List Name
-```
-
-
-### Outdoor Air Unit Outputs
-
-* HVAC,Average, Zone Outdoor Air Unit Total Heating Rate [W]
-
-* HVAC,Sum, Zone Outdoor Air Unit Total Heating Energy [J]
-
-* HVAC,Average, Zone Outdoor Air Unit Total Cooling Rate [W]
-
-* HVAC,Sum, Zone Outdoor Air Unit Total Cooling Energy [J]
-
-* HVAC,Average, Zone Outdoor Air Unit Sensible Cooling Rate [W]
-
-* HVAC,Sum, Zone Outdoor Air Unit Sensible Heating Energy [J]
-
-* HVAC,Average, Zone Outdoor Air Unit Fan Electric Power [W]
-
-* HVAC,Sum, Zone Outdoor Air Unit Fan Electric Energy [J]
-
-* HVAC,Average, Zone Outdoor Air Unit Air Mass Flow Rate [kg/s]
-
-* HVAC,Average, Zone Outdoor Air Unit Fan Availability Status []
-
-* Zone Outdoor Air Unit Latent Cooling Energy
-
-#### Zone Outdoor Air Unit Total Heating Rate [W]
-
-This field reports the heating output rate of the outdoor air unit system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the zone outdoor air unit.
-
-#### Zone Outdoor Air Unit Total Heating Energy [J]
-
-This field is the heating output of the outdoor air unit system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the zone outdoor air unit, and the time step.
-
-#### Zone Outdoor Air Unit Total Cooling Rate [W]
-
-This field reports the total cooling (sensible plus latent) output rate of the outdoor air unit system to the zone it is serving in Watts. This is determined by outlet and zone air conditions and the mass flow rate through the zone outdoor air unit.
-
-#### Zone Outdoor Air Unit Total Cooling Energy [J]
-
-This field is the total cooling (sensible plus latent) output of the outdoor air unit system to the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the zone outdoor air unit, and the time step.
-
-#### Zone Outdoor Air Unit Sensible Cooling Energy [J]
-
-#### Zone Outdoor Air Unit Sensible Cooling Rate [W]
-
-These reports are the sensible cooling output rate of the outdoor air unit system to the zone it is serving in Joules or Watts. This is determined by outlet and zone air conditions and the mass flow rate through the zone outdoor air unit.
-
-#### Zone Outdoor Air Unit Sensible Heating Energy [J]
-
-#### Zone Outdoor Air Unit Sensible Heating Rate [W]
-
-These are the sensible heating output of the outdoor air unit system to the zone it is serving in Joules or Watts over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the zone outdoor air unit, and the time step.
-
-#### Zone Outdoor Air Unit Latent Cooling Energy [J]
-
-#### Zone Outdoor Air Unit Latent Cooling Rate [W]
-
-These are the latent cooling output of the outdoor air unit system to the zone it is serving, in Joules and Watts. This is determined by outlet and zone air conditions, the mass flow rate through the zone outdoor air unit, and the time step.
-
-#### Zone Outdoor Air Unit Latent Heating Energy [J]
-
-#### Zone Outdoor Air Unit Latent Heating Rate [W]
-
-These are the latent heating output of the outdoor air unit system to the zone it is serving, in Joules and Watts. This is determined by outlet and zone air conditions, the mass flow rate through the zone outdoor air unit, and the time step.
-
-#### Zone Outdoor Air Unit Fan Electric Power [W]
-
-This field reports the electric power consumption rate of the fan of the outdoor air unit in Watts.
-
-#### Zone Outdoor Air Unit Fan Electric Energy [J]
-
-This field reports the electric power consumed by the fan of the outdoor air unit over the time step in Joules.
-
-#### Zone Outdoor Air Unit Air Mass Flow Rate [kg/s]
-
-This field reports the air mass flow rate of the zone outdoor air unit Outdoor Air Unit  in kilograms per second.
-
-#### Zone Outdoor Air Unit Fan Availability Status []
-
-This is the availability status of the outdoor air unit fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the outdoor air unit  object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-### ZoneHVAC:OutdoorAirUnit:EquipmentList
-
-This input syntax is used to specify the components in a zone outdoor air unit. The components will be simulated in the order in which they occur in this list.
-
-#### Field: Name
-
-The user designated unique name of an instance of a zone outdoor air unit equipment list.
-
-#### Field Set (Component Object Type, Component Name, Control Node Name) up to 8
-
-After the identifying name, the list consists of up to 8 pairs of data items.
-
-#### Field: Component &lt;x&gt; Object Type
-
-This field specifies the keyword for the type of component used.
-
-#### Field: Component &lt;x&gt; Name
-
-This field is the unique name of the component specified in the previous field. This named object must appear in the IDF.
-
-Note: If any of the components use the autosized option at the component level, input data for zone sizing purposes are required for the proper sizing of the components. Please refer to the Sizing:Zone object for more information.
-
-An example from an IDF:
-
-```idf
-ZoneHVAC:OutdoorAirUnit:EquipmentList,
-    Zone5OAUEquip1,          !- Name
-    Dehumidifier:Desiccant:NoFans,  !- Component 1 Object Type
-    Z5Dessicant,             !- Component 1 Name
-    HeatExchanger:AirToAir:FlatPlate,  !- Component 2 Object Type
-    Zone5A2AHeat Recovery,   !- Component 2 Name
-    CoilSystem:Cooling:DX,  !- Component 3 Object Type
-    DX Cooling Coil System 5,!- Component 3 Name
-    Coil:Heating:Electric,   !- Component 4 Object Type
-    Zone5DESHCoil;           !- Component 4 Name
-```
-
-
-### ZoneHVAC:WindowAirConditioner
-
-The Window Air Conditioner is a unit of zone equipment made up of other components. Each window air conditioner consists of an outdoor air mixer, a fan, and a direct expansion (DX) cooling coil. These components are described elsewhere in this document. The input for a window air conditioner requires the names of these three pieces of equipment, which are then specified individually elsewhere in the input. The input for a window air conditioner also requires the name of an availability schedule, the maximum unit airflow rate, and the maximum outdoor airflow rate for the unit. The unit is connected to a zone by specifying an air inlet node, which must be the same as a zone exhaust node; and an air outlet node, which must be the same as a zone inlet node (ref. ZoneHVAC:EquipmentConnections).
-
-A supply air fan operating mode schedule must also be specified. The supply air fan operating mode schedule value determines if the supply air fan can run continuously with the DX coil cycling on/off to match the zone cooling demand or the fan and DX coil can cycle on/off together to meet the cooling demand. The placement of the supply air fan, in relation to the DX coil, must also be specified (blow through or draw through). The cooling convergence tolerance is required, which is the tolerance denoting how closely the window air conditioner will meet the cooling load. The tolerance is always relative to the zone load (i.e., the unit will operate to meet the zone load to within the tolerance value times the zone load for each simulation timestep). Finally, the DX cooling coil type must be specified.
-
-#### Field: Name
-
-A unique user assigned name for an instance of a window air conditioner unit. Any reference to this window air conditioner by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the window air conditioner unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Maximum Supply Air Flow Rate
-
-The maximum volumetric airflow rate through the window air conditioner in cubic meters per second. Since the unit operates by cycling on/off, this is also the design, rated airflow rate of the unit.
-
-#### Field: Maximum Outdoor Air Flow Rate
-
-If the window air conditioner uses outdoor air, this field specifies the outdoor air volumetric flow rate in cubic meters per second. This flow rate should be less than or equal to the maximum airflow rate. A value of zero specifies no outdoor air. Note that the outdoor airflow rate is fixed: it cannot change during the simulation
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node (see Node) from which the window air conditioner draws its indoor air. This should be one of the zone exhaust nodes for the zone which the window air conditioner is cooling.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node (see Node) to which the window air conditioner sends its outlet air. This should be one of the inlet air nodes for the zone which is being cooled.
-
-#### Field: Outdoor Air Mixer Object Type
-
-This field specifies the type of outdoor air mixer used by this window air conditioner unit. The outdoor air mixer component is part of the window air conditioner compound object. The only available outdoor air mixer type is:
-
-OutdoorAir:Mixer
-
-#### Field: Outdoor Air Mixer Name
-
-The name of an outdoor air mixer component which composes part of the window air conditioner unit. Note that the return air node of the outdoor air mixer should be the same node as the air inlet node of the window air conditioner. In addition, the outdoor air mixer’s mixed air node should be the same as the window air conditioner’s fan inlet air node (for blow through) or the air conditioner’s DX coil inlet node (for draw through)
-
-#### Field: Supply Air Fan Object Type
-
-This field specifies the type of supply air fan used by window air conditioner. The supply air fan is part of the window air conditioner compound object. The only valid supply air fan types are:
-
-* Fan:OnOff
-
-* Fan:ConstantVolume
-
-#### Field:Supply Air Fan Name
-
-The name of a constant volume fan component that composes part of the window air conditioner. Note that the fan’s maximum flow rate should be the same as the maximum airflow rate of the window air conditioner. A fan of type Fan:OnOff may be used with either cycling or continuous fan, and a fan of type Fan:ConstantVolume is used only with continuous fan (see Supply Air Fan Operating Mode Schedule field below). The fan’s inlet node should be the same as the outdoor air mixer’s mixed air node (for blow through) or the DX coil’s outlet node (for draw through). The fan’s outlet node should be the same as the DX coil’s air inlet node (for blow through) or the window air conditioner’s air outlet node (for draw through).
-
-#### Field: Cooling Coil Object Type
-
-This field specifies the type of cooling coil to be modeled for this window air conditioner. The input requirements for these cooling coil objects are described elsewhere in this document. If the user wants to control the enhanced dehumidification performance of the Heat Exchanger Assisted coil type based on zone air humidity level, then the input file must include a humidistat object (ref. ZoneControl:Humidistat) for the zone being served by this air conditioner and a high humidity set point manager (ref. SetpointManager:SingleZone:Humidity:Maximum) with the high humidity set point placed on the outlet node of the heat exchanger assisted cooling coil. Only allowable coil types are:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* CoilSystem:Cooling:DX:HeatExchangerAssisted
-
-#### Field: DX Cooling Coil Name
-
-The name of a DX cooling coil component that composes part of the window air conditioner unit. The DX coil air inlet node should be the same as the fan outlet node (for blow through) or the outdoor air mixer’s mixed air node (for draw through). The DX coil air outlet node should be the same as the window air conditioner’s air outlet node (for blow through) or the fan’s inlet node (for draw through).
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply air fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, the model assumes the supply air fan cycles with the heating or cooling coil throughout the simulation.
-
-#### Field: Fan Placement
-
-This input field has two choices: **BlowThrough** or **DrawThrough**. The first choice stands for “blow through fan�. This means that the unit consists of an outdoor air mixer followed by a fan followed by a DX coil. The fan “blows through� the DX coil. The second choice stands for “draw through fan�. This means that the unit consists of an outdoor air mixer followed by a DX coil followed by a fan. The fan “draws air through� the coil.
-
-#### Field: Cooling Convergence Tolerance
-
-This input field defines the convergence tolerance for the unit’s cooling output. This field allows the user some control over how closely the air conditioner will control the air-side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in zone air temperature. Initial experience with this parameter lends to the recommendation of using 0.001 as the starting point.
-
-The window air conditioner is controlled by matching its sensible (temperature) cooling output to the zone sensible load (demand). Because the performance of the DX coil is frequently non-linear, the air conditioner model must call the DX coil model several times (iterate) to determine the proper run time fraction to meet the zone load. The cooling convergence tolerance is the error tolerance used to terminate the iteration procedure when the following equation is satisfied:
-
-<div>\[\frac{{\left| {{Q_{ZoneLoad}} - {Q_{WindowAirConditioner,out}})} \right|}}{{{Q_{ZoneLoad}}}} \le Cooling{\kern 1pt} Convergence{\kern 1pt} Tolerance\]</div>
-
-The maximum number of iterations is limited, with a warning message generated if the above equation is not satisfied within the maximum number of iterations.
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this window air conditioner or object’s fan. If the window air conditioner is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this window air conditioner object should be on or off.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Maximum Air Flow Rate in this Window Air Conditioner zone HVAC object. The scaled Maximum Air Flow Rate in turn is used to size cooling capacity of the unit.
-
-
-
-Following is an example input for the cycling window air conditioner, along with its constituent components.
-
-```idf
-ZoneHVAC:WindowAirConditioner,
-       Zone3WindAC,                  ! name of window AC unit
-       FanAndCoilAvailSched,         ! Availability Schedule Name
-       0.6,                          ! Maximum Supply Air Flow Rate {m3/s}
-       0.05,                         ! Maximum Outdoor Air Flow Rate {m3/s}
-       Zone3WindACAirInletNode,      ! Air Inlet Node Name
-       Zone3WindACAirOutletNode,     ! Air Outlet Node Name
-       OutdoorAir:Mixer,             ! Outdoor Air Mixer Object Type
-       Zone3WindACOAMixer,           ! Outdoor Air Mixer Name
-       Fan:ConstantVolume,           ! Supply Air Fan Object Type
-       Zone3WindACFan,               ! Fan Name
-       Zone3WindACDXCoil,            ! DX Cooling Coil Name
-       CyclingFanSch,                ! Supply Air Fan Operation Mode Schedule Name
-       DrawThrough,                  ! Fan Placement
-       0.001,                        ! Cooling Convergence Tolerance
-       Coil:Cooling:DX:SingleSpeed;  ! Cooling Coil Object Type
-
-
-Schedule:Compact,
-       CyclingFanSch,                !- Name
-       Fraction,                     !- ScheduleType
-       Through: 12/31,               !- Complex Field \#1
-       For: AllDays,                 !- Complex Field \#2
-       Until: 24:00,                 !- Complex Field \#7
-       0.0;                          !- Complex Field \#8
-
-
-OutdoorAir:Mixer,
-       Zone3WindACOAMixer,           ! Name
-       Zone3WindACOAMixerOutletNode, ! Mixed Air Node Name
-       Zone3WindACOAInNode,          ! Outdoor Air Stream Node Name
-       Zone3WindACExhNode,           ! Relief Air Stream Node Name
-       Zone3WindACAirInletNode;      ! Return Air Stream Node Name
-
-
-Fan:ConstantVolume,
-       Zone3WindACFan,               ! Name
-       FanAndCoilAvailSched,         ! Availability Schedule Name
-       0.5,                          ! Fan Total Efficiency
-       75.0,                         ! Pressure Rise {Pa}
-       0.6,                          ! Maximum Flow Rate {m3/s}
-       0.9,                          ! Motor Efficiency
-       1.0,                          ! Motor In Airstream Fraction
-       Zone3WindACDXOutletNode,      ! Air Inlet Node Name
-       Zone3WindACAirOutletNode;     ! Air Outlet Node Name
-
-
-Coil:Cooling:DX:SingleSpeed,
-    Zone3WindACDXCoil,       !- Name
-    CoolingCoilAvailSched,   !- Availability Schedule Name
-    autosize,                !- Rated Total Cooling Capacity {W}
-    autosize,                !- Rated Sensible Heat Ratio
-    3.0,                     !- Rated COP
-    autosize,                !- Rated Air Flow Rate {m3/s}
-    Zone3WindACOAMixerOutletNode,  !- Air Inlet Node Name
-    Zone3WindACDXOutletNode, !- Air Outlet Node Name
-    WindACCoolCapFT,         !- Total Cooling Capacity Function of Temperature Curve Name
-    WindACCoolCapFFF,        !- Total Cooling Capacity Function of Flow Fraction Curve Name
-    WindACEIRFT,             !- Energy Input Ratio Function of Temperature Curve Name
-    WindACEIRFFF,            !- Energy Input Ratio Function of Flow Fraction Curve Name
-    WindACPLFFPLR;           !- Part Load Fraction Correlation Curve Name
-```
-
-
-### Window Air Conditioner Outputs
-
-* HVAC,Average,Zone Window Air Conditioner Total Cooling Rate [W]
-
-* HVAC,Sum,Zone Window Air Conditioner Total Cooling Energy [J]
-
-* HVAC,Average,Zone Window Air Conditioner Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Window Air Conditioner Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Window Air Conditioner Latent Cooling Rate [W]
-
-* HVAC,Sum,Zone Window Air Conditioner Latent Cooling Energy [J]
-
-* HVAC,Average,Zone Window Air Conditioner Electric Power[W]
-
-* HVAC,Sum,Zone Window Air Conditioner Electric Energy [J]
-
-* HVAC,Average, Zone Window Air Conditioner Fan Part Load Ratio []
-
-* HVAC,Average, Zone Window Air Conditioner Compressor Part Load Ratio []
-
-* HVAC,Average,Zone Window Air Conditioner Fan Availability Status []
-
-#### Zone Window Air Conditioner Total Cooling Rate [W]
-
-This field is the total (sensible and latent) heat extraction rate of the window air conditioner unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
-
-#### Zone Window Air Conditioner Total Cooling Energy [J]
-
-This is the total (sensible and latent) heat extraction of the window air conditioner unit from the zone it is serving in Joules over the timestep being reported. This is determined by outlet and zone air conditions, the mass flow rate through the unit, and the timestep.
-
-#### Zone Window Air Conditioner Sensible Cooling Rate [W]
-
-This field reports the moist air sensible heat extraction rate of the window air conditioner unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
-
-#### Zone Window Air Conditioner Sensible Cooling Energy [J]
-
-This field reports the moist air sensible heat extraction of the window air conditioner unit from the zone it is serving in Joules over the timestep being reported. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
-
-#### Zone Window Air Conditioner Latent Cooling Rate [W]
-
-This output is the latent heat extraction rate of the window air conditioner unit from the zone it is serving in Watts. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
-
-#### Zone Window Air Conditioner Latent Cooling Energy [J]
-
-This is the latent heat extraction of the window air conditioner unit from the zone it is serving in Joules over the timestep being reported. This is determined by the outlet and zone conditions and the mass flow rate through the unit.
-
-#### Zone Window Air Conditioner Electric Power[W]
-
-This output is the electricity consumption rate of the window air conditioner unit in Watts. The consumption includes electricity used by the compressor and the fans (indoor supply air fan and the condenser fan).
-
-#### Zone Window Air Conditioner Electric Energy [J]
-
-This output is the electricity consumption of the window air conditioner unit in Joules for the time period being reported. The consumption includes electricity used by the compressor and the fans (indoor supply air fan and the condenser fan).
-
-#### Zone Window Air Conditioner Fan Part Load Ratio []
-
-This is the fan’s part load ratio for the report timestep during which the fan had operated.
-
-#### Zone Window Air Conditioner Compressor Part Load Ratio []
-
-This is the part load ratio of the report timestep during which the DX unit compressor had operated.
-
-***Zone Window Air Conditioner Fan Availability Status []***
-
-This is the availability status of the window air conditioner fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the window air conditioner object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-### ZoneHVAC:PackagedTerminalAirConditioner
-
-The packaged terminal air conditioner (PTAC) is a compound object made up of other components. Each PTAC consists of an outdoor air mixer, direct expansion (DX) cooling coil, heating coil (gas, electric, hot water, or steam) and a supply air fan. While the figure below shows the PTAC with draw through fan placement, blow through fan placement can also be modeled by positioning the supply air fan between the outdoor air mixer and the DX cooling coil. The packaged terminal air conditioner coordinates the operation of these components and is modeled as a type of zone equipment (Ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
-
-![PTAC\_Drawthrough](media/image284.png)
-
-Figure 111.  Schematic of a packaged terminal air conditioner with draw through fan placement
-
-Links to the PTAC’s supply air fan, DX cooling coil, heating coil, and outdoor air mixer specifications are provided in the air conditioner’s input syntax. Additional inputs include supply and outdoor air flow rates during cooling operation, heating operation, and when neither cooling or heating is required. A description of each input field for the packaged terminal air conditioner compound object is provided below.
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a packaged terminal air conditioner. Any reference to this air conditioner by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the air conditioner operates during a given time period. A schedule value equal to 0 denotes that the air conditioner must be off for that time period. A value greater than 0 denotes that the air conditioner is available to operate during that time period. This schedule may be used to completely disable the air conditioner (all of its coils and the supply air fan) as required. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Inlet Node Name
-
-This alpha field defines the name of the HVAC system node from which the air conditioner draws its inlet air. This node name must be the name of a zone air exhaust node (Ref. ZoneHVAC:EquipmentConnections).
-
-#### Field: Air Outlet Node Name
-
-This alpha field defines the name of the HVAC system node to which the air conditioner sends its outlet air. This node name must be the name of a zone air inlet node (Ref. ZoneHVAC:EquipmentConnections).
-
-#### Field: Outdoor Air Mixer Object Type
-
-This field specifies the type of outdoor air mixer used by this PTAC. The outdoor air mixer component is part of the PTAC unit. The only available outdoor air mixer type is:
-
-* OutdoorAir:Mixer
-
-#### Field: Outdoor Air Mixer Name
-
-This alpha field defines the name of an outdoor air mixer component which composes part of the PTAC. The return air node of the outdoor air mixer should also be the same node as the air inlet node of the PTAC. Furthermore, the outdoor air mixer’s mixed air node should be the same as the PTAC’s fan inlet air node (for blow through fan placement) or the PTAC’s DX cooling coil inlet node (for draw through fan placement).
-
-#### Field: Cooling Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the air conditioner in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the air conditioner in cubic meters per second when the heating coil is operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: No Load Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the air conditioner in cubic meters per second when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the air conditioner’s supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner’s supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).
-
-#### Field: Cooling Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air flow rate through the air conditioner in cubic meters per second when the DX cooling coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Cooling Outdoor Air Flow Rate is fixed; it cannot change during the simulation. In addition, the Cooling Outdoor Air Flow Rate cannot be greater than the air conditioner’s supply air volumetric flow rate during cooling operation.
-
-#### Field: Heating Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air flow rate through the air conditioner in cubic meters per second when the heating coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Heating Outdoor Air Flow Rate is fixed; it cannot change during the simulation. In addition, the Heating Outdoor Air Flow Rate cannot be greater than the air conditioner’s supply air volumetric flow rate during heating operation.
-
-#### Field: No Load Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air flow rate through the air conditioner in cubic meters per second when neither cooling nor heating is required (i.e., cooling and heating coils are off but the supply air fan operates). Values must be greater than or equal to 0, or this field is autosizable. Note that the outdoor air flow rate when no cooling/heating is needed is fixed; it cannot change during the simulation. In addition, the outdoor air flow rate when no cooling/heating is needed cannot be greater than the air conditioner’s supply air volumetric flow rate when no cooling/heating is needed. This field is only used when the air conditioner’s supply air fan operating mode schedule specifies continuous fan operation. If the air conditioner’s supply air fan operating mode schedule specifies continuous fan operation and the field ‘Supply air volumetric flow rate when no cooling or heating is needed’ is set to zero or is left blank, then the model assumes that the outdoor air flow rate when no cooling/heating is needed is equal to the outdoor air flow rate when the cooling or heating coil was last operating (for cooling operation [i.e., Cooling Outdoor Air Flow Rate] or heating operation [i.e., Heating Outdoor Air Flow Rate]) and this field is not used.
-
-#### Field: Supply Air Fan Object Type
-
-This alpha field defines the type of fan used by this PTAC. The only valid choices are **Fan:OnOff** and **Fan:ConstantVolume**. A fan of type Fan:OnOff is used with cycling fan operating mode, and a fan of type Fan:ConstantVolume is used with continuous fan operating mode (see Supply Air Fan Operating Mode Schedule field below). The input requirements for these fan objects are described elsewhere in this document.
-
-#### Field: Supply Air Fan Name
-
-The name of a constant volume fan component that composes part of the PTAC. Note that the fan’s maximum flow rate should be greater than or equal to the maximum supply air flow rate for the PTAC. The fan’s inlet node should be the same as the outdoor air mixer’s mixed air node (for blow through fan placement) or the heating coil’s outlet node (for draw through fan placement). The fan’s outlet node should be the same as the DX cooling coil’s air inlet node (for blow through fan placement) or the PTAC’s air outlet node (for draw through fan placement).
-
-#### Field: Heating Coil Object Type
-
-This alpha field defines the type of heating coil to be used by this PTAC. The input requirements for this heating coil object are described elsewhere in this document. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (PTAC) itself provides the "controller" function of modulating water flow. Allowable heating coil types are:
-
-* Coil:Heating:Water
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Steam
-
-#### Field: Heating Coil Name
-
-This alpha field defines the name of the heating coil used by this PTAC, and this name should match the name specified in the corresponding heating coil object.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field defines the type of DX cooling coil used by this PTAC. The input requirements for these DX cooling coil objects are described elsewhere in this document. Only allowable coil types are:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* CoilSystem:Cooling:DX:HeatExchangerAssisted
-
-* Coil:Cooling:DX:VariableSpeed
-
-#### Field: Cooling Coil Name
-
-This alpha field defines the name of the cooling coil used by this PTAC, and this name should match the name specified in the corresponding DX cooling coil object.
-
-#### Field: Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. The first choice stands for “blow through fan�. This means that the unit consists of an outdoor air mixer followed by a fan followed by the DX cooling coil and heating coil. The fan “blows through� the DX cooling coil and the heating coil. The second choice stands for “draw through fan�. This means that the unit consists of an outdoor air mixer followed by the DX cooling coil and heating coil with the fan located at the outlet of the PTAC. The fan “draws air through� the DX cooling coil and the heating coil. If this field is left blank, the default is draw through.
-
-Note: the packaged terminal air conditioner’s supply air fan, cooling coil and heating coil must be connected according to the configuration shown above (Figure 111) for the draw through fan configuration. The only other valid configuration is with a blow through fan placement, where the fan is located between the outdoor air mixer and the DX cooling coil.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this packaged terminal air conditioner or object’s fan. If the packaged terminal air conditioner is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this packaged terminal air conditioner object should be on or off.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Cooling Supply Air Flow Rate in this Packaged Terminal Air Conditioner  zone HVAC object. The scaled Supply Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
-
-As shown in the example below, correct specification of the packaged terminal air conditioner requires the following objects in addition to the compound object itself:
-
-1) Fan (Fan:OnOff or Fan:ConstantVolume)
-
-2) DX cooling coil (Coil:Cooling:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted)
-
-3) Heating coil (Coil:Heating:Gas, Coil:Heating:Electric, Coil:Heating:Water, or Coil:Heating:Steam)
-
-4) OutdoorAir:Mixer
-
-
-```idf
-ZoneHVAC:PackagedTerminalAirConditioner,
-    Zone2PTAC,               !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    Zone2PTACAirInletNode,   !- Air Inlet Node Name
-    Zone2PTACAirOutletNode,  !- Air Outlet Node Name
-    OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type
-    Zone2PTACOAMixer,        !- Outdoor Air Mixer Name
-    autosize,              !- Cooling Supply Air Flow Rate {m3/s}
-    autosize,              !- Heating Supply Air Flow Rate operation {m3/s}
-    autosize,              !- No Load Supply Air Flow Rate {m3/s}
-    autosize,              !- Cooling Outdoor Air Flow Rate {m3/s}
-    autosize,              !- Heating Outdoor Air Flow Rate {m3/s}
-    autosize,              !- No Load Outdoor Air Flow Rate  {m3/s}
-    Fan:OnOff,                      !- Supply Air Fan Object Type
-    Zone2PTACFan,                          !- Supply Air Fan Name
-    Coil:Heating:Electric,                 !- Heating Coil Object Type
-    Zone2PTACHeatCoil,                     !- Heating Coil Name
-    Coil:Cooling:DX:SingleSpeed,  !- Cooling Coil Object Type
-    Zone2PTACDXCoolCoil,                   !- Cooling Coil Name
-    BlowThrough,                           !- Fan Placement
-    SupplyFanSch;                          !- Supply Air Fan Operating Mode Schedule Name
-
-
-Schedule:Compact,
-    SupplyFanSch,            !- Name
-    Fraction,                !- ScheduleType
-    Through: 12/31,          !- Complex Field \#1
-    For: AllDays,            !- Complex Field \#2
-    Until:  7:00,            !- Complex Field \#3
-    0.0,                     !- Complex Field \#4
-    Until: 18:00,            !- Complex Field \#5
-    1.0,                     !- Complex Field \#6
-    Until: 24:00,            !- Complex Field \#7
-    0.0;                     !- Complex Field \#8
-
-OutdoorAir:Mixer,
-    Zone2PTACOAMixer,            !- Name
-    Zone2PTACOAMixerOutletNode,  !-Mixed Air Node Name
-    Zone2PTACOAInNode,           !-Outdoor Air Stream Node Name
-    Zone2PTACExhNode,            !- Relief Air Stream Node Name
-    Zone2PTACAirInletNode;       !- Return Air Stream Node Name
-
-  Fan:OnOff,
-    Zone2PTACFan,                !- Name
-    FanAndCoilAvailSched,        !- Availability Schedule Name
-    0.5,                         !- Fan Total Efficiency
-    75.0,                        !- Pressure Rise {Pa}
-    autosize,                    !- Maximum Flow Rate{m3/s}
-    0.9,                         !- Motor Efficiency
-    1.0,                         !- Motor In Airstream Fraction
-    Zone2PTACOAMixerOutletNode,  !- Air Inlet Node Name
-    Zone2PTACFanOutletNode;      !- Air Outlet Node Name
-
-Coil:Cooling:DX:SingleSpeed,
-    Zone2PTACDXCoolCoil,         !- Coil Name
-    CoolingCoilAvailSched,       !- Availability Schedule Name
-    autosize,                    !- Rated Total Cooling Capacity (gross) {W}
-    autosize,                    !- Rated SHR
-    3.0,                         !- Rated COP
-    autosize,                    !- Rated Air Volume Flow Rate {m3/s}
-    Zone2PTACFanOutletNode,      !- Coil Air Inlet Node
-    Zone2PTACCoolCoilOutletNode, !-Coil Air Outlet Node
-    HPACCoolCapFT,               !- Total Cooling Capacity Modifier Curve (function of temperature)
-    HPACCoolCapFFF,              !- Total Cooling Capacity Modifier Curve (function of flow fraction)
-    HPACEIRFT,                   !- Energy Input Ratio Modifier Curve (function of temperature)
-    HPACEIRFFF,                  !- Energy Input Ratio Modifier Curve (function of flow fraction)
-    HPACPLFFPLR;                 !- Part Load Fraction Correlation (function of part load ratio)
-
-Coil:Heating:Electric,
-    Zone2PTACHeatCoil,           !- Coil Name
-    HeatingCoilAvailSched,       !- Availability Schedule Name
-    1.0,                         !- Efficiency
-    autosize,                    !- Nominal Capacity {W}
-    Zone2PTACCoolCoilOutletNode, !- Air Inlet Node Name
-    Zone2PTACAirOutletNode;      !- Air Outlet Node Name
-```
-
-### Packaged Terminal Air Conditioner (PTAC) Outputs
-
-* HVAC,Average,Zone Packaged Terminal Air Conditioner Total Heating Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Air Conditioner Total Heating Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Air Conditioner Total Cooling Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Air Conditioner Total Cooling Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Air Conditioner Sensible Heating Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Air Conditioner Sensible Heating Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Air Conditioner Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Air Conditioner Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Air Conditioner Latent Heating Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Air Conditioner Latent Heating Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Air Conditioner Latent Cooling Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Air Conditioner Latent Cooling Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Air Conditioner Electric Power [W]
-
-* HVAC,Sum,Zone Packaged Terminal Air Conditioner Electric Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Air Conditioner Fan Part Load Ratio []
-
-* HVAC,Average,Zone Packaged Terminal Air Conditioner Compressor Part Load Ratio []
-
-* HVAC,Average,Zone Packaged Terminal Air Conditioner Fan Availability Status []
-
-
-#### Zone Packaged Terminal Air Conditioner Total Heating Rate [W]
-
-This output field is the total (enthalpy) heat addition rate of the packaged terminal air conditioner to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams, and the air mass flow rate through the air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Total Heating Energy [J]
-
-This output field is the total (enthalpy) heat addition of the packaged terminal air conditioner to the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams, the air mass flow rate through the air conditioner, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Total Cooling Rate [W]
-
-This output field is the total (enthalpy) heat extraction rate of the packaged terminal air conditioner from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams, and the air mass flow rate through the air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Total Cooling Energy [J]
-
-This output field is the total (enthalpy) heat extraction of the packaged terminal air conditioner from the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams, the air mass flow rate through the air conditioner, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Sensible Heating Rate [W]
-
-This output field is the sensible heat addition rate of the packaged terminal air conditioner to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Sensible Heating Energy [J]
-
-This output field is the sensible heat addition of the packaged terminal air conditioner to the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the air conditioner, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Sensible Cooling Rate [W]
-
-This output field reports the moist air sensible heat extraction rate of the packaged terminal air conditioner from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Sensible Cooling Energy [J]
-
-This output field reports the moist air sensible heat extraction of the packaged terminal air conditioner from the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the air conditioner outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the air conditioner, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Latent Heating Rate [W]
-
-This output field is the latent heat addition (humidification) rate of the packaged terminal air conditioner to the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the packaged terminal air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Latent Heating Energy [J]
-
-This output field is the latent heat addition (humidification) of the packaged terminal air conditioner to the zone it is serving in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the packaged terminal air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Latent Cooling Rate [W]
-
-This output field is the latent heat extraction (dehumidification) rate of the packaged terminal air conditioner from the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the packaged terminal air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Latent Cooling Energy [J]
-
-This output field is the latent heat extraction (dehumidification) of the packaged terminal air conditioner from the zone it is serving in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the packaged terminal air conditioner. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Electric Power [W]
-
-This output field is the electricity consumption rate of the packaged terminal air conditioner in Watts. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the heating coil (includes electricity consumption rate for electric heating coil or parasitic electricity consumption rate for non-electric coils). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Electric Energy [J]
-
-This output field is the electricity consumption of the packaged terminal air conditioner in Joules for the time period being reported. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the heating coil (includes electricity consumption for electric heating coil or parasitic electricity consumption for non-electric coils). This value is calculated for each HVAC system timestep being simulated, and the results are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Fan Part Load Ratio []
-
-This output field is the part-load ratio of the fan. The fan part-load ratio is defined as the average supply air mass flow rate divided by the maximum supply air mass flow rate. The maximum supply air mass flow rate depends on whether heating, cooling, or no heating or cooling is required during the timestep. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Compressor Part Load Ratio []
-
-This output field is the part-load ratio used by the coils (cooling and heating). Part-load ratio is defined as the total coil load divided by the coil steady-state capacity. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Air Conditioner Fan Availability Status []
-
-This is the availability status of the packaged terminal air conditioner fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the packaged terminal air conditioner  object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-### ZoneHVAC:PackagedTerminalHeatPump
-
-The packaged terminal heat pump (PTHP) is a compound object made up of other components. Each PTHP consists of an outdoor air mixer, direct expansion (DX) cooling coil, DX heating coil, supply air fan, and a supplemental heating coil as shown in the figure below. These individual components are described elsewhere in this document. The packaged terminal heat pump coordinates the operation of these components and is modeled as a type of zone equipment (Ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
-
-![PTPFigure](media/image285.png)
-
-Figure 112. Schematic of a packaged terminal heat pump (draw through fan placement)
-
-Links to the PTHP’s supply air fan, DX coils, supplemental heating coil, and outdoor air mixer specifications are provided in the heat pump’s input syntax. Additional inputs include supply and outdoor air flow rates during cooling operation, heating operation, and when neither cooling or heating is required. A description of each input field for the packaged terminal heat pump compound object is provided below.
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a packaged terminal heat pump. Any reference to this heat pump by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump operates during a given time period. A schedule value equal to 0 denotes that the heat pump must be off for that time period. A value greater than 0 denotes that the heat pump is available to operate during that time period. This schedule may be used to completely disable the heat pump (all of its coils and the supply air fan) as required. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Inlet Node Name
-
-This alpha field defines the name of the HVAC system node from which the heat pump draws its inlet air. This node name must be the name of a zone air exhaust node (Ref. ZoneHVAC:EquipmentConnections).
-
-#### Field: Air Outlet Node Name
-
-This alpha field defines the name of the HVAC system node to which the heat pump sends its outlet air. This node name must be the name of a zone air inlet node (Ref. ZoneHVAC:EquipmentConnections).
-
-#### Field: Outdoor Air Mixer Object Type
-
-This field specifies the type of outdoor air mixer used by this PTHP. The outdoor air mixer component is part of the PTHP compound object. The only available outdoor air mixer type is:
-
-* OutdoorAir:Mixer
-
-#### Field: Outdoor Air Mixer Name
-
-This alpha field defines the name of an outdoor air mixer component which composes part of the PTHP. Note that the return air node of the outdoor air mixer should also be the same node as the air inlet node of the PTHP. Furthermore, the outdoor air mixer’s mixed air node should be the same as the PTHP’s fan inlet air node (for blow through fan placement) or the PTHP’s DX cooling coil inlet node (for draw through fan placement).
-
-#### Field: Cooling Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: No Load Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the heat pump’s supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the heat pump’s supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).
-
-#### Field: Cooling Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when the DX cooling coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Cooling Outdoor Air Flow Rate is fixed; it cannot change during the simulation. In addition, the Cooling Outdoor Air Flow Rate cannot be greater than the heat pump’s supply air volumetric flow rate during cooling operation.
-
-#### Field: Heating Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Heating Outdoor Air Flow Rate is fixed; it cannot change during the simulation. In addition, the Heating Outdoor Air Flow Rate cannot be greater than the heat pump’s supply air volumetric flow rate during heating operation.
-
-#### Field: No Load Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). Values must be greater than or equal to 0, or this field is autosizable. Note that the outdoor air flow rate when no cooling/heating is needed is fixed; it cannot change during the simulation. In addition, the outdoor air flow rate when no cooling/heating is needed cannot be greater than the heat pump’s supply air volumetric flow rate when no cooling/heating is needed. This field is only used when the heat pump’s supply air fan operating mode schedule specifies continuous fan operation. If the heat pump’s supply air fan operating mode schedule specifies continuous fan operation and the field ‘Supply air volumetric flow rate when no cooling or heating is needed’ is set to zero or is left blank, then the model assumes that the outdoor air flow rate when no cooling/heating is needed is equal to the outdoor air flow rate when the cooling or heating coil was last operating (for cooling operation [i.e., Cooling Outdoor Air Flow Rate] or heating operation [i.e., Heating Outdoor Air Flow Rate]) and this field is not used.
-
-#### Field: Supply Air Fan Object Type
-
-This alpha field defines the type of fan used by this PTHP. The only valid choices are Fan:OnOff and Fan:ConstantVolume. A fan of type Fan:OnOff may be used with either cycling or continuous fan operating mode, and a fan of type Fan:ConstantVolume is used only with continuous fan operating mode (see Supply Air Fan Operating Mode Schedule field below). The input requirements for these fan objects are described elsewhere in this document.
-
-#### Field: Supply Air Fan Name
-
-The name of a constant volume fan component that composes part of the PTHP. Note that the fan’s maximum flow rate should be greater than or equal to the maximum supply air flow rate for the PTHP. The fan’s inlet node should be the same as the outdoor air mixer’s mixed air node (for blow through fan placement) or the DX heating coil’s outlet node (for draw through fan placement). The fan’s outlet node should be the same as the DX cooling coil’s air inlet node (for blow through fan placement) or the supplemental heater’s air inlet node (for draw through fan placement).
-
-#### Field: Heating Coil Object Type
-
-This alpha field defines the type of DX heating coil to be used by this PTHP. The only valid choice are **Coil:Heating:DX:SingleSpeed** and **Coil:Heating:DX:VariableSpeed**. The input requirements for this DX heating coil object are described elsewhere in this document.
-
-#### Field: Heating Coil Name
-
-This alpha field defines the name of the DX heating coil used by this PTHP, and this name should match the name specified in the corresponding DX heating coil object.
-
-#### Field: Heating Convergence Tolerance
-
-This numeric field defines the convergence tolerance for the unit’s heating output. This field allows the user some control over how closely the heat pump will control the air-side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in zone air temperature. Initial experience with this parameter lends to the recommendation of using 0.001 as the starting point.
-
-The heat pump is controlled by matching its sensible (temperature) heating output to the zone sensible load (demand). Because the performance of the DX heating coil is frequently non-linear, the heat pump model must call the DX heating coil model several times (iterate) to determine the proper run time fraction to meet the zone load. The heating convergence tolerance is the error tolerance used to terminate the iteration procedure when the following equation is satisfied:
-
-<div>\[\frac{{\left| {({Q_{ZoneLoad}} - {Q_{HeatPump,out}})} \right|}}{{{Q_{ZoneLoad}}}}\,\, \le \,\,Heating{\kern 1pt} Convergence{\kern 1pt} Tolerance\]</div>
-
-The maximum number of iterations is limited, with a warning message generated if the above equation is not satisfied within the maximum number of iterations.
-
-#### Field: Minimum Outdoor Dry-Bulb Temperature for Compressor Operation
-
-This numeric field defines the minimum outdoor dry-bulb temperature in degrees Celsius for PTHP compressor operation. The compressor will not operate (for DX heating or DX cooling) when outdoor dry-bulb temperatures fall below this value. The minimum value must be greater than or equal to -20 °C. If this field is left blank, the default value is -8°C. This temperature should match the minimum compressor operating temperature specified for the heat pump’s DX heating coil (if they don’t match, the highest of the two temperatures will be the cut-off temperature for compressor operation).
-
-#### Field: Cooling Coil Object Type
-
-This alpha field defines the type of DX cooling coil used by this PTHP. The input requirements for these DX cooling coil objects are described elsewhere in this document. Only allowable coil types are:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* CoilSystem:Cooling:DX:HeatExchangerAssisted
-
-* Coil:Cooling:DX:VariableSpeed
-
-#### Field: Cooling Coil Name
-
-This alpha field defines the name of the cooling coil used by this PTHP, and this name should match the name specified in the corresponding DX cooling coil object.
-
-#### Field: Cooling Convergence Tolerance
-
-This numeric field defines the convergence tolerance for the unit’s cooling output. This field allows the user some control over how closely the heat pump will control the air-side conditions. The relative size of this parameter relates directly to the closeness of the control. A very small value in this field will result in tight control and will probably result in larger numbers of iterations. A large value in this field will result in looser controls and could result in unsatisfactory fluctuations in zone air temperature. Initial experience with this parameter lends to the recommendation of using 0.001 as the starting point.
-
-The heat pump is controlled by matching its sensible (temperature) cooling output to the zone sensible load (demand). Because the performance of the DX cooling coil is frequently non-linear, the heat pump model must call the DX cooling coil model several times (iterate) to determine the proper run time fraction to meet the zone load. The cooling convergence tolerance is the error tolerance used to terminate the iteration procedure when the following equation is satisfied:
-
-<div>\[\frac{{\left| {({Q_{ZoneLoad}} - {Q_{HeatPump,out}})} \right|}}{{{Q_{ZoneLoad}}}}\,\, \le \,\,Cooling{\kern 1pt} Convergence{\kern 1pt} Tolerance\]</div>
-
-The maximum number of iterations is limited, with a warning message generated if the above equation is not satisfied within the maximum number of iterations.
-
-#### Field: Supplemental Heating Coil Object Type
-
-This alpha field defines the type of supplemental heating coil to be used by this PTHP. The input requirements for these heating coil objects are described elsewhere in this document. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the supplemental heating coil does not require additional controller or Controller:WaterCoil object. The parent object (PTHP) itself provides the "controller" function of modulating water flow. Allowable coil types are:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Supplemental Heating Coil Name
-
-This alpha field defines the name of the supplemental heating coil used by this PTHP, and this name should match the name specified in the corresponding heating coil object.
-
-#### Field: Maximum Supply Air Temperature from Supplemental Heater
-
-This numeric field defines the maximum supply air temperature in degrees Celsius exiting the heat pump supplemental heater coil. The supplemental heater will be controlled so that its supply air temperature does not exceed this value. This field is autosizable.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation
-
-This numeric field defines the maximum outdoor dry-bulb temperature in degrees Celsius for PTHP supplemental heater operation. The supplemental heater will not operate when the outdoor dry-bulb temperature is above this value. The maximum value must be less than or equal to 21°C. If this field is left blank, the default value is 21°C.
-
-#### Field: Fan Placement
-
-This alpha field has two choices: **BlowThough** or **DrawThrough**. The first choice stands for “blow through fan�. This means that the unit consists of an outdoor air mixer followed by a fan followed by the DX coils and supplemental heating coil. The fan “blows through� the cooling and heating coils. The second choice stands for “draw through fan�. This means that the unit consists of an outdoor air mixer followed by the DX coil(s) followed by a fan, with the supplemental heater located at the outlet of the fan. The fan “draws air through� the DX coil(s). If this field is left blank, the default is draw through.
-
-Note: the packaged terminal heat pump’s supply air fan, cooling coil, heating coil and supplementary heating coil must be connected according to the configuration shown above (Figure 112) for the draw through fan configuration. The only other valid configuration is with a blow through fan placement, where the fan is located between the outdoor air mixer and the DX cooling coil.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply air fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, the model assumes the supply air fan cycles with the heating or cooling coil throughout the simulation.
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this packaged terminal heat pump or object’s fan. If the packaged terminal heat pump is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this packaged terminal heat pump object should be on or off.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Cooling Supply Air Flow Rate in this PTHP zone HVAC object. The scaled Supply Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
-
-As shown in the example below, correct specification of the packaged terminal heat pump requires the following objects in addition to the compound object itself:
-
-1) Fan (Fan:OnOff or Fan:ConstantVolume)
-
-2) DX cooling coil (Coil:Cooling:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted)
-
-3) DX heating coil (Coil:Heating:DX:SingleSpeed)
-
-4) Supplemental heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
-
-5) OutdoorAir:Mixer
-
-```idf
-ZoneHVAC:PackagedTerminalHeatPump,
-    Zone2PTHP,               !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    Zone2PTHPAirInletNode,   !- Air Inlet Node Name
-    Zone2PTHPAirOutletNode,  !- Air Outlet Node Name
-    OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type
-    Zone2PTHPOAMixer,        !- Outdoor Air Mixer Name
-    autosize,                !- Cooling Supply Air Flow Rate {m3/s}
-    autosize,                !- Heating Supply Air Flow Rate {m3/s}
-    autosize,                !- No Load Supply Air Flow Rate {m3/s}
-    autosize,                !- Cooling Outdoor Air Flow Rate {m3/s}
-    autosize,                !- Heating Outdoor Air Flow Rate {m3/s}
-    autosize,                !- No Load Outdoor Air Flow Rate {m3/s}
-    Fan:OnOff,               !- Supply Air Fan Object Type
-    Zone2PTHPFan,            !- Supply Air Fan Name
-    Coil:Heating:DX:SingleSpeed,  !- Heating Coil Object Type
-    Zone2PTHPDXHeatCoil,     !- Heating Coil Name
-    0.001,                   !- Heating Convergence Tolerance {dimensionless}
-    2.0,                     !- Minimum Outdoor Dry-Bulb Temperature for Compressor Operation {C}
-    Coil:Cooling:DX:SingleSpeed,  !- Cooling Coil Object Type
-    Zone2PTHPDXCoolCoil,     !- Cooling Coil Name
-    0.001,                   !- Cooling Convergence Tolerance {dimensionless}
-    Coil:Heating:Electric,   !- Supplemental Heating Coil Object Type
-    Zone2PTHPSupHeater,      !- Supplemental Heating Coil Name
-    autosize,                !- Maximum Supply Air Temperature from Supplemental Heater {C}
-    10.0,                    !- Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation {C}
-    BlowThrough,             !- Fan Placement
-    CyclingFanSch;           !- Supply Air Fan Operating Mode Schedule Name
-
-
-Schedule:Compact,
-    CyclingFanSch,               !- Name
-    Fraction,                    !- ScheduleType
-    Through: 12/31,              !- Complex Field \#1
-    For: AllDays,                !- Complex Field \#2
-    Until: 24:00,                !- Complex Field \#7
-    0.0;                         !- Complex Field \#8
-
-OutdoorAir:Mixer,
-    Zone2PTHPOAMixer,            !- Name
-    Zone2PTHPOAMixerOutletNode,  !-Mixed Air Node Name
-    Zone2PTHPOAInNode,           !-Outdoor Air Stream Node Name
-    Zone2PTHPExhNode,            !- Relief Air Stream Node Name
-    Zone2PTHPAirInletNode;       !- Return Air Stream Node Name
-
-Fan:OnOff,
-    Zone2PTHPFan,                !- Name
-    FanAndCoilAvailSched,        !- Availability Schedule Name
-    0.5,                         !- Fan Total Efficiency
-    75.0,                        !- Pressure Rise {Pa}
-    autosize,                    !- Maximum Flow Rate {m3/s}
-    0.9,                         !- Motor Efficiency
-    1.0,                         !- Motor In Airstream Fraction
-    Zone2PTHPOAMixerOutletNode,  !- Air Inlet Node Name
-    Zone2PTHPFanOutletNode;      !- Air Outlet Node Name
-
-Coil:Cooling:DX:SingleSpeed,
-    Zone2PTHPDXCoolCoil,         !- Coil Name
-    CoolingCoilAvailSched,       !- Availability Schedule
-    autosize,                    !- Rated Total Cooling Capacity (gross) {W}
-    autosize,                    !- Rated SHR
-    3.0,                         !- Rated COP
-    autosize,                    !- Rated Air Volume Flow Rate {m3/s}
-    Zone2PTHPFanOutletNode,      !- Coil Air Inlet Node
-    Zone2PTHPCoolCoilOutletNode, !- Coil Air Outlet Node
-    HPACCoolCapFT,               !- Total Cooling Capacity Modifier Curve (function of temperature)
-    HPACCoolCapFFF,              !- Total Cooling Capacity Modifier Curve (function of flow fraction)
-    HPACEIRFT,                   !- Energy Input Ratio Modifier Curve (function of temperature)
-    HPACEIRFFF,                  !- Energy Input Ratio Modifier Curve (function of flow fraction)
-    HPACPLFFPLR;                 !- Part Load Fraction Correlation (function of part load ratio)
-
-COIL:Heating:DX:SingleSpeed,
-    Zone2PTHPDXHeatCoil,         !- Coil Name
-    HeatingCoilAvailSched,       !- Availability Schedule
-    autosize,                    !- Rated Total Heating Capacity {W}
-    2.75,                        !- Rated COP
-    autosize,                    !- Rated Air Volume Flow Rate {m3/s}
-    Zone2PTHPCoolCoilOutletNode, !- Coil Air Inlet Node
-    Zone2PTHPDXHeatCoilOutletNode, !- Coil Air Outlet Node
-    HPACHeatCapFT,              !- Total heating capacity modifier curve (function of temperature)
-    HPACHeatCapFFF,             !- Total heating capacity modifier curve (function of flow fraction)
-    HPACHeatEIRFT,              !- Energy input ratio modifier curve (function of temperature)
-    HPACHeatEIRFFF,             !- Energy input ratio modifier curve (function of flow fraction)
-    HPACCOOLPLFFPLR,            !- Part load fraction correlation (function of part load ratio)
-    ,                           !- Defrost energy input ratio modifier curve (function of temperature)
-    2.0,                        !- Minimum Outdoor Dry-bulb Temperature for Compressor Operation {C}
-    5.0,                        !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation {C}
-    200.0,                      !- Crankcase Heater Capacity {W}
-    10.0,                       !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
-    Resistive,                  !- Defrost Strategy
-    TIMED,                      !- Defrost Control
-    0.166667,                   !- Defrost Time Period Fraction
-    20000;                      !- Resistive Defrost Heater Capacity {W}
-
-Coil:Heating:Electric,
-    Zone2PTHPSupHeater,          !- Name
-    HeatingCoilAvailSched,       !- Availability Schedule Name
-    1.0,                         !- Efficiency
-    autosize,                    !- Nominal Capacity {W}
-    Zone2PTHPDXHeatCoilOutletNode, !- Air Inlet Node Name
-    Zone2PTHPAirOutletNode;      !- Air Outlet Node Name
-```
-
-
-### Packaged Terminal Heat Pump (PTHP) Outputs
-
-* HVAC,Average,Zone Packaged Terminal Heat Pump Total Heating Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Heat Pump Total Heating Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Heat Pump Total Cooling Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Heat Pump Total Cooling Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Heat Pump Sensible Heating Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Heat Pump Sensible Heating Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Heat Pump Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Heat Pump Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Heat Pump Latent Heating Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Heat Pump Latent Heating Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Heat Pump Latent Cooling Rate [W]
-
-* HVAC,Sum,Zone Packaged Terminal Heat Pump Latent Cooling Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Heat Pump Electric Power [W]
-
-* HVAC,Sum,Zone Packaged Terminal Heat Pump Electric Energy [J]
-
-* HVAC,Average,Zone Packaged Terminal Heat Pump Fan Part Load Ratio []
-
-* HVAC,Average,Zone Packaged Terminal Heat Pump Compressor Part Load Ratio []
-
-* HVAC,Average,Zone Packaged Terminal Heat Pump Fan Availability Status []
-
-#### Zone Packaged Terminal Heat Pump Total Heating Rate [W]
-
-This output field is the total (enthalpy) heat addition rate of the packaged terminal heat pump to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Total Heating Energy [J]
-
-This output field is the total (enthalpy) heat addition of the packaged terminal heat pump to the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, the air mass flow rate through the heat pump, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Total Cooling Rate [W]
-
-This output field is the total (enthalpy) heat extraction rate of the packaged terminal heat pump from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Total Cooling Energy [J]
-
-This output field is the total (enthalpy) heat extraction of the packaged terminal heat pump from the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, the air mass flow rate through the heat pump, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Sensible Heating Rate [W]
-
-This output field is the sensible heat addition rate of the packaged terminal heat pump to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Sensible Heating Energy [J]
-
-This output field is the sensible heat addition of the packaged terminal heat pump to the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the heat pump, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Sensible Cooling Rate [W]
-
-This output field reports the moist air sensible heat extraction rate of the packaged terminal heat pump from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Sensible Cooling Energy [J]
-
-This output field reports the moist air sensible heat extraction of the packaged terminal heat pump from the zone it is serving in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the heat pump, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Latent Heating Rate [W]
-
-This output field is the latent heat addition (humidification) rate of the packaged terminal heat pump to the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the packaged terminal heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Latent Heating Energy [J]
-
-This output field is the latent heat addition (humidification) of the packaged terminal heat pump to the zone it is serving in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the packaged terminal heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Latent Cooling Rate [W]
-
-This output field is the latent heat extraction (dehumidification) rate of the packaged terminal heat pump from the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the packaged terminal heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Latent Cooling Energy [J]
-
-This output field is the latent heat extraction (dehumidification) of the packaged terminal heat pump from the zone it is serving in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the packaged terminal heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Electric Power [W]
-
-This output field is the electricity consumption rate of the packaged terminal heat pump in Watts. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Electric Energy [J]
-
-This output field is the electricity consumption of the packaged terminal heat pump in Joules for the time period being reported. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are summed for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Fan Part Load Ratio []
-
-This output field is the part-load ratio of the fan. The fan part-load ratio is defined as the average supply air mass flow rate divided by the maximum supply air mass flow rate. The maximum supply air mass flow rate depends on whether heating, cooling, or no heating or cooling is required during the timestep. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Compressor Part Load Ratio []
-
-This output field is the part-load ratio of the compressor used by the DX coils (cooling and heating). Compressor part-load ratio is defined as the total coil load divided by the coil steady-state capacity. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Zone Packaged Terminal Heat Pump Fan Availability Status []
-
-This is the availability status of the packaged terminal heat pump  fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the packaged terminal heat pump  object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-### ZoneHVAC:RefrigerationChillerSet
-
-The ZoneHVAC:RefrigerationChillerSet object works in conjunction with one or multiple air chillers, compressor racks, refrigeration systems, or refrigeration secondary system objects (Ref. Refrigeration:AirChiller Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem) to simulate the performance of a group of air chillers cooling a single zone. The chiller set model passes information about the zone conditions to determine the performance of individual chiller coils within the set, thus providing the sensible and latent heat exchange with the zone environment.
-
-The refrigeration chiller set object inputs include a name, an availability schedule name, the name of the zone cooled by the chiller set, the air inlet node name, the air outlet node name, and an extensible list of air chiller names (Ref. Refrigeration:AirChiller).
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a refrigeration chiller. Any reference to this refrigeration chiller by another object (may be listed in a Refrigeration:CaseAndWalkInList, Refrigeration:System, Refrigeration:SecondarySystem, or Refrigeration:CompressorRack) will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the refrigeration chiller can operate during a given time period. A schedule value greater than 0 (maximum schedule value of 1.0 is typically used) indicates that the refrigeration chiller will operate during a given time period. A value equal to 0 denotes that the case does not operate (everything is OFF: refrigeration, fans, lights, anti-sweat, etc.). Typically the refrigeration chiller will operate throughout the day (i.e., the schedule will contain 1 for all time periods); however, refrigeration chillers require maintenance and/or cleaning and this can be modeled accordingly using this schedule if desired. If this field is left blank, the default schedule has a value of 1 for all time periods.
-
-#### Field: Zone Name
-
-A unique user-assigned name for the zone cooled by this refrigeration chiller. This zone must represent a conditioned space, that is, it must appear in a ZoneHVAC:EquipmentConnections object.
-
-#### Field: Air Inlet Node Name
-
-Not used, reserved for future use.  Current version exchanges energy directly with the zone, external of any air system. (Future: The name of the zone exhaust node (see Node) from which the refrigeration chiller draws its indoor air. This should be one of the zone exhaust nodes for the zone cooled by the chiller set.)
-
-#### Field: Air Outlet Node Name
-
-Not used, reserved for future use.  Current version exchanges energy directly with the zone, external of any air system. (Future: The name of the node where the chiller coil sends its outlet air, which must be one of the inlet air nodes for the zone which is being cooled.)
-
-#### Field: Air Chiller \#1  Name
-
-The name of the first air chiller that will be used to meet the zone cooling load.
-
-#### Field: Air Chiller \#2  Name
-
-The name of the second air chiller that will be used to meet the zone cooling load.
-
-#### Field: Air Chiller \#3  Name
-
-The name of the third air chiller that will be used to meet the zone cooling load.
-
-#### Field: Air Chiller \#n  Name (Extensible list, 20 provided in the IDD)
-
-The name of the nth air chiller that will be used to meet the zone cooling load.
-
-
-
-The following is an example input for a refrigeration chiller set.
-
-```idf
-   ZoneHVAC:RefrigerationChillerSet,
-    SubFreezerChillerSet ,     !- Name
-    ,                         !- Availability Schedule Name
-    SubFreezer,                !- Zone Name
-    NODE_142,                   !- Air Inlet Node Name
-    NODE_141,                   !- Air Outlet Node Name
-    SubFreezerAirChiller_1,    !- Air Chiller \#1 Name
-    SubFreezerAirChiller_2,    !- Air Chiller \#2 Name
-    SubFreezerAirChiller_3;    !- Air Chiller \#3 Name
-```
-
-
-There are no outputs variables for a ZoneHVAC:RefrigerationChillerSet. Outputs for the refrigeration impact on any zone are listed in the Group:Refrigeration.
-
-### ZoneHVAC:WaterToAirHeatPump
-
-The zone water-to-air heat pump is a compound component consisting of a fan, water-to-air cooling and heating coils, and a supplemental heating coil. Links to the fan, WaterToAirHeatPump cooling coil, WaterToAirHeatPump heating coil, and supplementary heating coil specifications are provided in the heat pump’s input data syntax. The heat pump switches between cooling and heating depending on the zone’s demand. The load side (air) of the zone water-to-air heat pump consists of an On/Off fan component, a WaterToAirHeatPump cooling coil component, a WaterToAirHeatPump heating coil component, and a Gas or Electric supplemental heating coil component. The source side (water) of the heat pump is connected to a condenser loop with a heat exchanger (ground heat exchanger or other type) or a plant loop with a heating source such as a boiler and a cooling source such as a chiller or cooling tower.  The diagram below shows the setup and connection of the heat pump for the source side and load side for a ground heat exchanger configuration. Note that on the load side, the WaterToAirHeatPump cooling coil must always be placed before the WaterToAirHeatPump heating coil.
-
-For this zone heat pump,there are two types of WaterToAirHeatPump coil model allowed:
-
-* Coil:Cooling:WaterToAirHeatPump:EquationFit
-
-* Coil:Heating:WaterToAirHeatPump:EquationFit
-
-* Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit
-
-* Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit
-
-![Schematic\_ZoneWSHP](media/image288.png)
-
-Figure 113. Zone Water to Air Heat Pump Schematic for a DrawThrough Configuration with Ground Heat Exchanger
-
-#### Field: Name
-
-This alpha field contains the identifying name for the zone system heat pump.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump operates during a given time period. A schedule value equal to 0 denotes that the heat pump must be off for that time period. A value greater than 0 denotes that the heat pump is available to operate during that time period. This schedule may be used to completely disable the heat pump (all of its coils and the supply air fan) as required. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the name of the HVAC system node from which the heat pump draws its inlet air. This node must be a zone exhaust node as specified in a ZoneHVAC:EquipmentConnections object.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the name of the HVAC system node to which the heat pump sends its outlet air. This node must be a zone inlet node as specified in a ZoneHVAC:EquipmentConnections object.
-
-#### Field: Outdoor Air Mixer Object Type
-
-This field specifies the type of outdoor air mixer used by this WaterToAirHeatPump unit. The outdoor air mixer component is part of the WaterToAirHeatPump compound object. The only available outdoor air mixer type is:
-
-* OutdoorAir:Mixer
-
-#### Field: Outdoor Air Mixer Name
-
-This alpha field defines the name of an outdoor air mixer component which composes part of the zone WaterToAirHeatPump. The return air stream node of the outdoor air mixer should also be the same node as the air inlet node of the WaterToAirHeatPump. Furthermore, the outdoor air mixer’s mixed air node should be the same as the WaterToAirHeatPump’s fan inlet air node (for blow through fan placement) or the WaterToAirHeatPump’s cooling coil inlet node (for draw through fan placement).
-
-#### Field: Cooling Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: No Load Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the heat pump’s supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the heat pump’s supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).
-
-#### Field: Cooling Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when the DX cooling coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the outside air flow rate during cooling operation is fixed; it cannot change during the simulation. In addition, the outside air flow rate during cooling operation cannot be greater than the heat pump’s supply air flow rate during cooling operation.
-
-#### Field: Heating Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the outside air flow rate during heating operation is fixed; it cannot change during the simulation. In addition, the outside air flow rate during heating operation cannot be greater than the heat pump’s supply air flow rate during heating operation.
-
-#### Field: No Load Outdoor Air Flow Rate When No Cooling or Heating is Needed
-
-This numeric field defines the outdoor air flow rate through the heat pump in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). Values must be greater than or equal to 0, or this field is autosizable. Note that the no load outdoor air flow rate cannot change during the simulation. In addition, the no load outdoor air flow rate cannot be greater than the heat pump's no load supply air flow rate. This field is only used when the heat pump's supply air fan operating mode schedule specifies continuous fan operation. If the heat pump's supply air fan operating mode schedule specifies continuous fan operation and the field "No Load Supply Air Flow Rate" is set to zero or is left blank, then the model assumes that the no load outdoor air flow rate is equal to the outdoor air flow rate when the cooling or heating coil was last operating (for cooling operation [i.e., Cooling outdoor air flow rate] or heating operation [i.e., Heating outdoor air flow rate]) and this field is not used.
-
-#### Field: Supply Air Fan Object Type
-
-This alpha field contains the identifying type of supply air fan specified in the heat pump. Fan type must be Fan:OnOff.
-
-#### Field: Supply Air Fan Name
-
-This alpha field contains the identifying name given to the heat pump supply air fan, and should match the name specified in the corresponding fan object.
-
-#### Field: Heating Coil Object Type
-
-This alpha field contains the identifying type of heating coil specified in the heat pump. The only valid types are Coil:Heating:WaterToAirHeatPump:EquationFit Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit..
-
-#### Field: Heating Coil Name
-
-This alpha field contains the identifying name given to the WaterToAirHeatPump heating coil, and should match the name specified in the corresponding WaterToAirHeatPump heating coil object.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field contains the identifying type of cooling coil specified in the heat pump. The only valid types are Coil:Cooling:WaterToAirHeatPump:EquationFit and Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit.
-
-#### Field: Cooling Coil Name
-
-This alpha field contains the identifying name given to the WaterToAirHeatPump cooling coil, and should match the name specified in the corresponding WaterToAirHeatPump cooling coil object.
-
-#### Field: Maximum Cycling Rate
-
-This numeric field contains the maximum on-off cycling rate for the compressor, which occurs at 50% run time fraction. Suggested values are shown below (Henderson et al. 1999):
-
-![](media/image289.svg)
-
-#### Field: Heat Pump Time Constant
-
-This numeric field contains the time constant for the cooling coil's capacity to reach steady state after startup. Suggested values are shown below (Henderson et al. 1999):
-
-![](media/image290.svg)
-
-#### Field: Fraction of On-Cycle Power Use
-
-This numeric field contains the fraction of on-cycle power use to adjust the part load fraction based on the off-cycle power consumption due to crankcase heaters, controls, fans, and etc. Suggested value values are below (Henderson et al. 1999):
-
-![](media/image291.svg)
-
-#### Field: Heat Pump Fan Delay Time
-
-This numeric field contains the time delay in seconds for the heat pump supply air fan to shut off after compressor cycle off. This value can be obtained from the manufacturer or the heat pump catalog. Suggested value is 60 seconds. This value is disregared at times when the WaterToAirHeatPump’s fan operating mode schedule value is greater than 0 (i.e., continuous fan mode).
-
-#### Field: Supplemental Heating Coil Object Type
-
-This is the object type of the supplemental heating coil. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the supplemental heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Zone Water to Air Heat Pump) itself provides the "controller" function of modulating water flow. The valid choices are:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Supplemental Heating Coil Name
-
-This alpha field contains the identifying name given to the supplemental heating coil, and should match the name specified in the corresponding supplemental heating coil object.
-
-#### Field: Maximum Supply Air Temperature from Supplemental Heater
-
-This numeric field defines the maximum allowed supply air temperature exiting the heat pump supplemental heating coil in degrees Celsius.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation
-
-This numeric field defines the outdoor air dry-bulb temperature in degrees Celsius above which the heat pump supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21°C. If this input field is left blank, the default value is 21°C.
-
-#### Field: Outdoor Dry-Bulb Temperature Sensor Node Name
-
-This alpha field specifies the name of the outdoor node which controls the operation of the supplemental heating coil. If this field is left blank, the outdoor temperature is based solely on the weather data. If this field is not blank, the node name specified must also be listed in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor temperature from the weather data. Alternately, the node name must be specified in an OutdoorAir:NodeList object where the outdoor temperature is taken directly from the weather data.
-
-#### Field: Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. The first choice represents a blow through system where the supply air fan is before the WaterToAirHeatPump cooling/heating coil and the supplementary heating coil. The second choice represents a draw through system where the supply fan is between the WaterToAirHeatPump cooling/heating coil and the supplementary heating coil. If this input field is left blank, the default is blow through.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply air fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, the model assumes the supply air fan cycles with the heating or cooling coil throughout the simulation.
-
-As shown in the example below, correct specifications of the WatertoAirHeatPump requires specification of the following objects in addition to the ZoneHVAC:WaterToAirHeatPump object:
-
-- On/Off fan
-
-- WatertoAirHeatPump cooling coil (EquationFit only)
-
-- WatertoAirHeatPump heating coil (EquationFit only)
-
-- Supplementary heating coil
-
-- Outdoor air mixer
-
-- Condenser loop or plant loop demand branches
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this WatertoAirHeatPump or object’s fan. If the WatertoAirHeatPump is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this WatertoAirHeatPump object should be on or off.
-
-#### Field: Heat Pump Coil Water Flow Mode
-
-This field specifies the way in which water flow through the heat pump coils will be modeled.  This field is only used when WatertoAirHeatPump:EquationFit coils are used. There are three options:
-
-- Cycling
-
-- Constant
-
-- CyclingOnDemand
-
-**Cycling** varies water flow through the coil based on the heat pump Part Load Ratio.  This control method is appropriate for modeling heat pumps that are outfitted with a soleniod valve which allows water to flow through the coil only when the compressor is active. This is the default for EnergyPlus V8 and later.
-
-**Constant** provides a constant water flow regardless of heat pump operation.  Remember that EnergyPlus has two coils (a heating coil and a cooling coil) to approximate the operation of one coil that can operate in either heating mode or cooling mode.  Therefore, when the water flow mode is constant, there will be full flow through either the heating coil or the cooling coil, but not both at the same time.
-
-**ConstantOnDemand** provides full flow through the coil whenever there is a load.  When there is no load, there is zero flow through the coil.  This control strategy represents the way EnergyPlus modeled heat pump water flow prior to Version 8.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object.  A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Cooling Supply Air Flow Rate in this Water To Air Heat Pump zone HVAC object.  The scaled Supply Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
-
-
-
-Examples of IDF use:
-
-```idf
-ZoneHVAC:WaterToAirHeatPump,
-    Zone1WTAHP,               !- Name
-    FanAndCoilAvailSched,     !- Availability Schedule Name
-    Zone 1 Outlet Node,       !- Air Inlet Node Name
-    Zone 1 Inlet Node,        !- Air Outlet Node Name
-    OutdoorAir:Mixer,         !- Outdoor air mixer object type
-    Zone 1 Mixer,             !- Outdoor Air Mixer Name
-    Autosize,                 !- Cooling Supply Air Flow Rate {m3/s}
-    Autosize,                 !- Heating Supply Air Flow Rate {m3/s}
-    ,                         !- No Load Supply Air Flow Rate {m3/s}
-    0.0,                      !- Cooling Outdoor Air Flow Rate {m3/s}
-    0.0,                      !- Heating Outdoor Air Flow Rate {m3/s}
-    ,                         !- No Load Outdoor Air Flow Rate {m3/s}
-    Fan:OnOff,                !- Supply Air Fan Object Type
-    Zone 1 Fan,               !- Supply Air Fan Name
-    Coil:Heating:WaterToAirHeatPump:EquationFit,  !- Heating Coil Object Type
-    Sys 1 Heat Pump Heating Mode,  !- Heating Coil Name
-    Coil:Cooling:WaterToAirHeatPump:EquationFit, !- Cooling Coil Object Type
-    Sys 1 Heat Pump Cooling Mode, !- Cooling Coil Name
-    2.5,                      !- Maximum Cycling Rate
-    60.0,                     !- Heat Pump Time Constant
-    0.01,                     !- Fraction of On-Cycle Power Use
-    60,                       !- Heat Pump Fan Delay Time
-    Coil:Heating:Gas,         !- Supplemental Heating Coil Object Type
-    Heat Pump DX Supp Heating Coil 1, !- Supplemental Heating Coil Name
-    60.0,                  !- Maximum Supply Air Temperature from Supplemental Heater {C}
-    20.0,                  !- Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation {C}
-    Sys 1 Outside Air Inlet Node, !- Outdoor Dry-Bulb Temperature Sensor Node Name
-    BlowThrough,              !- Fan Placement
-    CyclingFanSch;            !- Supply Air Fan Operating Mode Schedule Name
-
-Schedule:Compact,
-    CyclingFanSch,           !- Name
-    Fraction,                !- Schedule Type Limits Name
-    Through: 12/31,          !- Field 1
-    For: AllDays,            !- Field 2
-    Until: 24:00,            !- Field 3
-    0.0;                     !- Field 4
-
-  Coil:Heating:WaterToAirHeatPump:EquationFit,
-    Sys 1 Heat Pump Heating Mode,  !- Name
-    Sys 1 Water to Air Heat Pump Source Side2 Inlet Node,   !- Water Inlet Node Name
-    Sys 1 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
-    Sys 1 Heating Coil Air Inlet Node,      !- Air Inlet Node Name
-    Sys 1 SuppHeating Coil Air Inlet Node,  !- Air Outlet Node Name
-    Autosize,                !- Rated Air Flow Rate {m3/s}
-    Autosize,                !- Rated Water Flow Rate {m3/s}
-    Autosize,                !- Rated Heating Capacity {W}
-    4.75,                    !- Rated Heating Coefficient of Performance
-    -1.361311959,            !- Heating Capacity Coefficient 1
-    -2.471798046,            !- Heating Capacity Coefficient 2
-    4.173164514,             !- Heating Capacity Coefficient 3
-    0.640757401,             !- Heating Capacity Coefficient 4
-    0.0,                     !- Heating Capacity Coefficient 5
-    -2.176941116,            !- Heating Power Consumption Coefficient 1
-    0.832114286,             !- Heating Power Consumption Coefficient 2
-    1.570743399,             !- Heating Power Consumption Coefficient 3
-    0.690793651,             !- Heating Power Consumption Coefficient 4
-    0.0;                     !- Heating Power Consumption Coefficient 5
-
-  OutdoorAir:Mixer,
-    Zone 1 Mixer,          !- Name
-    Sys 1 Mixed Air Node,  !- Mixed Air Node Name
-    Sys 1 Outside Air Inlet Node,  !- Outdoor Air Stream Node Name
-    Sys 1 Relief Air Outlet Node,  !- Relief Air Stream Node Name
-    Zone 1 Outlet Node;  !- Return Air Stream Node Name
-
-  Fan:OnOff,
-    Zone 1 Fan,              !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    0.7,                     !- Fan Total Efficiency
-    300.0,                   !- Pressure Rise {Pa}
-    Autosize,                !- Maximum Flow Rate {m3/s}
-    0.9,                     !- Motor Efficiency
-    1.0,                     !- Motor In Airstream Fraction
-    Sys 1 Mixed Air Node,    !- Air Inlet Node Name
-    Sys 1 Cooling Coil Air Inlet Node;  !- Air Outlet Node Name
-
-  Coil:Heating:Gas,
-    Heat Pump DX Supp Heating Coil 1,  !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    0.8,                     !- Gas Burner Efficiency
-    32000,                   !- Nominal Capacity {W}
-    Sys 1 SuppHeating Coil Air Inlet Node,  !- Air Inlet Node Name
-    Zone 1 Inlet Node;  !-Air Outlet Node Name
-
-  BRANCH,
-    Gshp Cooling Condenser Branch,  !- Name
-    0,  !- Maximum Flow Rate {m3/s}
-     ,  !- Pressure Drop Curve Name
-    Coil:Cooling:WaterToAirHeatPump:ParameterEstimation,  !- Component 1 Object Type
-    Heat Pump Cooling Mode,  !- Component 1 Name
-    Water to Air Heat Pump Source Side1 Inlet Node,  !- Component 1 Inlet Node Name
-    Water to Air Heat Pump Source Side1 Outlet Node, !- Component 1 Outlet Node Name
-    ACTIVE;  !- Component 1 Branch Control Type
-
-  BRANCH,
-    Gshp Heating Condenser Branch,  !- Name
-    0,  !- Maximum Flow Rate {m3/s}
-     ,  !- Pressure Drop Curve Name
-    Coil:Heating:WaterToAirHeatPump:ParameterEstimation,  !- Component 1 Object Type
-    Heat Pump Heating Mode,  !- Component 1 Name
-    Water to Air Heat Pump Source Side2 Inlet Node,   !- Component 1 Inlet Node Name
-    Water to Air Heat Pump Source Side2 Outlet Node,  !- Component 1 Outlet Node Name
-    ACTIVE;  !- Component 1 Branch Control Type
-```
-
-
-### Water to Air Heat Pump (ZoneHVAC) Outputs
-
-* HVAC,Average,Zone Water to Air Heat Pump Total Heating Rate [W]
-
-* HVAC,Sum,Zone Water to Air Heat Pump Total Heating Energy [J]
-
-* HVAC,Average,Zone Water to Air Heat Pump Total Cooling Rate [W]
-
-* HVAC,Sum,Zone Water to Air Heat Pump Total Cooling Energy [J]
-
-* HVAC,Average,Zone Water to Air Heat Pump Sensible Heating Rate [W]
-
-* HVAC,Sum,Zone Water to Air Heat Pump Sensible Heating Energy [J]
-
-* HVAC,Average,Zone Water to Air Heat Pump Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Water to Air Heat Pump Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Water to Air Heat Pump Latent Heating Rate [W]
-
-* HVAC,Sum,Zone Water to Air Heat Pump Latent Heating Energy [J]
-
-* HVAC,Average,Zone Water to Air Heat Pump Latent Cooling Rate [W]
-
-* HVAC,Sum,Zone Water to Air Heat Pump Latent Cooling Energy [J]
-
-* HVAC,Average,Zone Water to Air Heat Pump Electric Power [W]
-
-* HVAC,Sum,Zone Water to Air Heat Pump Electric Energy [J]
-
-* HVAC,Average,Zone Water to Air Heat Pump Fan Part Load Ratio []
-
-* HVAC,Average,Zone Water to Air Heat Pump Compressor Part Load Ratio []
-
-* HVAC,Average,Zone Water to Air Heat Pump Fan Availability Status []
-
-#### Zone Water to Air Heat Pump Total Heating Rate [W]
-
-This output field is the total (enthalpy) heat addition rate of the Water to Air Heat Pump to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system time step being simulated, and the results (enthalpy addition only) are averaged for the time step being reported.
-
-#### Zone Water to Air Heat Pump Total Heating Energy [J]
-
-This output field is the total (enthalpy) heat addition of the Water to Air Heat Pump to the zone it is serving in Joules over the time step being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, the air mass flow rate through the heat pump, and the HVAC simulation time step. This value is calculated for each HVAC system time step being simulated, and the results (enthalpy addition only) are summed for the time step being reported.
-
-#### Zone Water to Air Heat Pump Total Cooling Rate [W]
-
-This output field is the total (enthalpy) heat extraction rate of the Water to Air Heat Pump from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system time step being simulated, and the results (enthalpy extraction only) are averaged for the time step being reported.
-
-#### Zone Water to Air Heat Pump Total Cooling Energy [J]
-
-This output field is the total (enthalpy) heat extraction of the Water to Air Heat Pump from the zone it is serving in Joules over the time step being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, the air mass flow rate through the heat pump, and the HVAC simulation time step. This value is calculated for each HVAC system time step being simulated, and the results (enthalpy extraction only) are summed for the time step being reported.
-
-#### Zone Water to Air Heat Pump Sensible Heating Rate [W]
-
-This output field is the sensible heat addition rate of the Water to Air Heat Pump to the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system time step being simulated, and the results (heating only) are averaged for the time step being reported.
-
-#### Zone Water to Air Heat Pump Sensible Heating Energy [J]
-
-This output field is the sensible heat addition of the Water to Air Heat Pump to the zone it is serving in Joules over the time step being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the heat pump, and the HVAC simulation time step. This value is calculated for each HVAC system time step being simulated, and the results (heating only) are summed for the time step being reported.
-
-#### Zone Water to Air Heat Pump Sensible Cooling Rate [W]
-
-This output field reports the moist air sensible heat extraction rate of the Water to Air Heat Pump from the zone it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system time step being simulated, and the results (cooling only) are averaged for the time step being reported.
-
-#### Zone Water to Air Heat Pump Sensible Cooling Energy [J]
-
-This output field reports the moist air sensible heat extraction of the Water to Air Heat Pump from the zone it is serving in Joules over the time step being reported. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, the air mass flow rate through the heat pump, and the HVAC simulation time step. This value is calculated for each HVAC system time step being simulated, and the results (cooling only) are summed for the time step being reported.
-
-#### Zone Water to Air Heat Pump Latent Heating Rate [W]
-
-This output field is the latent heat addition (humidification) rate of the Water to Air Heat Pump to the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the WaterToAirHP heat pump. This value is calculated for each HVAC system time step being simulated, and the results (latent heat addition only) are averaged for the time step being reported.
-
-#### Zone Water to Air Heat Pump Latent Heating Energy [J]
-
-This output field is the latent heat addition (humidification) of the Water to Air Heat Pump to the zone it is serving in Joules over the time step being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the WaterToAirHP heat pump. This value is calculated for each HVAC system time step being simulated, and the results (latent heat addition only) are summed for the time step being reported.
-
-#### Zone Water to Air Heat Pump Latent Cooling Rate [W]
-
-This output field is the latent heat extraction (dehumidification) rate of the Water to Air Heat Pump from the zone it is serving in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the WaterToAirHP heat pump. This value is calculated for each HVAC system time step being simulated, and the results (latent heat extraction only) are averaged for the time step being reported.
-
-#### Zone Water to Air Heat Pump Latent Cooling Energy [J]
-
-This output field is the latent heat extraction (dehumidification) of the Water to Air Heat Pump from the zone it is serving in Joules over the time step being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the WaterToAirHP heat pump. This value is calculated for each HVAC system time step being simulated, and the results (latent heat extraction only) are summed for the time step being reported.
-
-#### Zone Water to Air Heat Pump Electric Power [W]
-
-This output field is the electricity consumption rate of the Water to Air Heat Pump in Watts. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the supplemental heating coil (if electric). This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Zone Water to Air Heat Pump Electric Energy [J]
-
-This output field is the electricity consumption of the Water to Air Heat Pump in Joules for the time period being reported. The consumption includes electricity used by the compressor (including crankcase heater), fans (indoor supply air fan and the condenser fan), and the supplemental heating coil (if electric). This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported.
-
-#### Zone Water to Air Heat Pump Fan Part Load Ratio []
-
-This output field is the part-load ratio of the fan. The fan part-load ratio is defined as the average supply air mass flow rate divided by the maximum supply air mass flow rate. The maximum supply air mass flow rate depends on whether heating, cooling, or no heating or cooling is required during the time step. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Zone Water to Air Heat Pump Compressor Part Load Ratio []
-
-This output field is the part-load ratio of the compressor used by the DX coils (cooling and heating). Compressor part-load ratio is defined as the total coil load divided by the coil steady-state capacity. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### Zone Water to Air Heat Pump Fan Availability Status []
-
-This is the availability status of the zone water source heat pump  fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the zone water source heat pump  object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-### ZoneHVAC:Dehumidifier:DX
-
-This object can be used for modeling conventional mechanical dehumidifiers. These systems use a direct expansion (DX) cooling coil to cool and dehumidify an airstream. Heat from the DX system’s condenser section is rejected into the cool/dehumidified airstream, resulting in warm dry air being supplied from the unit. In EnergyPlus, this object is modeled as a type of zone equipment (ref. ZoneHVAC:EquipmentList and ZoneHVAC:EquipmentConnections).
-
-![Dehumidifier\_Schematic](media/image292.png)
-
-Figure 114. Schematic of a mechanical dehumidifier
-
-The model has inputs for water removal, energy factor and air flow rate at rated conditions (26.7°C, 60% RH). Curve objects must be specified to describe performance at off-rated conditions. A part-load cycling curve input must also be specified to account for inefficiencies due to cycling. Other inputs including minimum and maximum operating temperatures for dehumidifier operation, off-cycle parasitic load, and an input to direct the removed water to a storage tank.
-
-The model assumes that this equipment dehumidifies and heats the air. If used in tandem with another system that cools and dehumidifies the zone air, then the zone dehumidifier should be specified as the lowest cooling priority in the ZoneHVAC:EquipmentList object for best control of zone temperature and humidity levels (e.g., if there are 3 pieces of equipment in ZoneHVAC:EquipmentList, then the zone dehumidifier should have Cooling Priority = 3). With this zone equipment prioritization, the other cooling and dehumidification system would operate first to meet the temperature setpoint (and possibly meet the high humidity setpoint as well). If additional dehumidification is needed, then the zone dehumidifier would operate. The sensible heat generated by the dehumidifier is carried over to the zone air heat balance for the next HVAC time step.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a zone DX dehumidifier unit. Any reference to this dehumidifier by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the dehumidifier operates during a given time period. A schedule value equal to 0 denotes that the dehumidifier will not operate for that time period. A value greater than 0 denotes that the dehumidifier is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Air Inlet Node Name
-
-This alpha field defines the name of the HVAC system node from which the dehumidifier draws its inlet air. This node name must be the name of a zone air exhaust node (ref. ZoneHVAC:EquipmentConnections).
-
-#### Field: Air Outlet Node Name
-
-This alpha field defines the name of the HVAC system node to which the dehumidifier sends its outlet air. This node name must be the name of a zone air inlet node (ref. ZoneHVAC:EquipmentConnections).
-
-#### Field: Rated Water Removal
-
-This numeric input is the full load water removal rate, in liters per day, at rated conditions (air entering the dehumidifier at 26.7°C [80°F] dry-bulb and 60% relative humidity, and air flow rate as defined by field “Rated Air Flow Rate� below). This is a required input field and the entered value must be greater than zero.
-
-#### Field: Rated Energy Factor
-
-This numeric input is the energy factor (liters of water removed per kWh of electricity consumed) at rated conditions (air entering the dehumidifier at 26.7°C [80°F] dry-bulb and 60% relative humidity, and air flow rate as defined by field “Rated Air Flow Rate� below). This is a required input field and the entered value must be greater than zero.
-
-#### Field: Rated Air Flow Rate
-
-This numeric input is the volumetric air flow rate through the dehumidifier, in m<sup>3</sup> per second, at rated conditions (air entering the dehumidifier at 26.7°C [80°F] dry-bulb and 60% relative humidity). This is a required input field and the entered value must be greater than zero.
-
-#### Field: Water Removal Curve Name
-
-This alpha field defines the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of water removal as a function of the dry-bulb temperature (°C) and relative humidity (%) of the air entering the dehumidifier. The output of this curve is multiplied by the Rated Water Removal to give the water removal of the dehumidifier at specific operating conditions (i.e., at temperatures and relative humidity levels different from the rating point conditions). The curve should be normalized to have the value of 1.0 at the rating point (air entering the dehumidifier at 26.7°C [80°F] dry-bulb and 60% relative humidity, and air flow rate as defined by field “Rated Air Flow Rate� above).
-
-#### Field: Energy Factor Curve Name
-
-This alpha field defines the name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy factor as a function of the dry-bulb temperature (°C) and relative humidity (%) of the air entering the dehumidifier. The output of this curve is multiplied by the Rated Energy Factor to give the energy factor of the dehumidifier at specific operating conditions (i.e., at temperatures and relative humidity levels different from the rating point conditions). The curve should be normalized to have the value of 1.0 at the rating point (air entering the dehumidifier at 26.7°C [80°F] dry-bulb and 60% relative humidity, and air flow rate as defined by field “Rated Air Flow Rate� above).
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of electrical power input to the dehumidifier as a function of the part load ratio (PLR, defined as the water removal load to be met (kg/s) divided by the dehumidifier’s water removal rate (kg/s) at the current operating conditions). The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
-
-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the dehumidifier runs continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-0.7 &lt;= PLF &lt;= 1.0   and   PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the dehumidifier is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the dehumidifier is set to 1.0.
-
-Mechanical dehumidifier typically have long runtimes with minimal compressor cycling. So, a typical part load fraction correlation might be:
-
-      PLF = 0.95 + 0.05(PLR)
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-      PLF = 1.0 + 0.0(PLR)
-
-#### Field: Minimum Dry-Bulb Temperature for Dehumidifier Operation
-
-This numeric field defines the minimum inlet air dry-bulb temperature for dehumidifier operation. The dehumidifier will not operate if the inlet air temperature is below this value. This input value must be less than the Maximum Dry-Bulb Temperature for Dehumidifier Operation, and the default value is 10°C.
-
-#### Field: Maximum Dry-Bulb Temperature for Dehumidifier Operation
-
-This numeric field defines the maximum inlet air dry-bulb temperature for dehumidifier operation. The dehumidifier will not operate if the inlet air temperature is above this value. This input value must be greater than the Minimum Dry-Bulb Temperature for Dehumidifier Operation, and the default value is 35°C.
-
-#### Field: Off-Cycle Parasitic Electric Load
-
-This numeric field contains the off-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the dehumidifier. This parasitic electric load is consumed whenever the dehumidifier is available to operate, but is not operating. The model assumed that this parasitic power contributes to heating the zone air (i.e., affects the zone air heat balance). The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
-
-#### Field: Condensate Collection Water Storage Tank Name
-
-This field is optional. It is used to specify where condensate from the dehumidifier is collected. If blank or omitted, then any water (condensate) removed is discarded. Enter the name of a Water Storage Tank (ref. WaterUse:Storage) object defined elsewhere and the condensate will then be collected in that tank.
-
-Following is an example input for a zone DX dehumidifier object. A ZoneControl:Humidistat object must also be specified for the zone to which the dehumidifier is connected (connect via a zone air exhaust node and a zone air inlet node, ref. ZoneHVAC:EquipmentConnections).
-
-
-
-```idf
-  ZoneHVAC:Dehumidifier:DX,
-    North Zone Dehumidifier,  !- Name
-    ON,                       !- Availability Schedule Name
-    Zone3DehumidifierInlet,   !- Air Inlet Node Name
-    Dehumidifier Outlet Node, !- Air Outlet Node Name
-    50.16,                    !- Rated Water Removal {L/day} (106 pints/day)
-    3.412,                    !- Rated Energy Factor {L/kWh} (7.21 pints/kWh)
-    0.12036,                  !- Rated Air Flow Rate {m3/s} (255 cfm)
-    ZoneDehumidWaterRemoval,  !- Water Removal Curve Name
-    ZoneDehumidEnergyFactor,  !- Energy Factor Curve Name
-    ZoneDehumidPLFFPLR,        !- Part Load Fraction Correlation Curve Name
-    10.0,  !- Minimum Dry-Bulb Temperature for Compressor Operation {C}
-    32.0,  !- Maximum Dry-Bulb Temperature for Compressor Operation {C}
-    0.0;   !- Off Cycle Parasitic Electric Load {W}
-
-
-  ZoneControl:Humidistat,
-    Zone 3 Humidistat,       !- Name
-    NORTH ZONE,              !- Zone Name
-    Seasonal Relative Humidity Sch;  !- Relative Humidity Setpoint Schedule Name
-```
-
-
-
-### DX Dehumidifier (ZoneHVAC) Outputs
-
-* HVAC,Average,Zone Dehumidifier Sensible Heating Rate [W]
-
-* HVAC,Sum,Zone Dehumidifier Sensible Heating Energy [J]
-
-* HVAC,Average,Zone Dehumidifier Removed Water Mass Flow Rate [kg/s]
-
-* HVAC,Sum,Zone Dehumidifier Removed Water Mass [kg]
-
-* HVAC,Average,Zone Dehumidifier Electric Power [W]
-
-* HVAC,Sum,Zone Dehumidifier Electric Energy [J]
-
-* HVAC,Average,Zone Dehumidifier Off Cycle Parasitic Electric Power [W]
-
-* HVAC,Sum,Zone Dehumidifier Off Cycle Parasitic Electric Energy [J]
-
-* HVAC,Average,Zone Dehumidifier Part Load Ratio []
-
-* HVAC,Average,Zone Dehumidifier Runtime Fraction []
-
-* HVAC,Average,Zone Dehumidifier Outlet Air Temperature [C]
-
-
-
-If Condensate Collection Water Storage Tank Name is specified:
-
-* HVAC,Average,Zone Dehumidifier Condensate Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Zone Dehumidifier Condensate Volume [m3]
-
-
-
-#### Zone Dehumidifier Sensible Heating Rate [W]
-
-This output field is the sensible heating rate output of the dehumidifier in Watts. This is determined by the water removal rate, enthalpy of water evaporation, and the zone dehumidifier electric power. To reduce simulation time, this heating is carried over to the zone air heat balance for the next HVAC time step (i.e., it is reported here for the current time step but actually impacts the zone air heat balance on the following HVAC time step). This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
-
-#### Zone Dehumidifier Sensible Heating Energy [J]
-
-This output field is the sensible heating output of the dehumidifier in Joules over the timestep being reported. This is determined by the water removal rate, enthalpy of water evaporation, and the zone dehumidifier electric power. To reduce simulation time, this heating is carried over to the zone air heat balance for the next HVAC time step (i.e., it is reported here for the current time step but actually impacts the zone air heat balance on the following HVAC time step). This value is calculated for each HVAC system timestep, and the results are summed for the timestep being reported.
-
-#### Zone Dehumidifier Removed Water Mass Flow Rate [kg/s]
-
-This output field is the water removal rate by the dehumidifier in kg/s. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
-
-#### Zone Dehumidifier Removed Water Mass [kg]
-
-This output field is the water removed by the dehumidifier in kg. This value is calculated for each HVAC system timestep, and the results are summed for the timestep being reported.
-
-#### Zone Dehumidifier Electric Power [W]
-
-#### Zone Dehumidifier Electric Energy [J]
-
-These outputs are the electric power and electric consumption of the dehumidifier for the time period being reported. They include all electricity used by the dehumidifier (including off-cycle electric parasitics). These values are calculated for each HVAC system timestep, and the results are averaged (power) or summed (consumption) for the timestep being reported. The electric consumption output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
-
-#### Zone Dehumidifier Off Cycle Parasitic Electric Power [W]
-
-#### Zone Dehumidifier Off Cycle Parasitic Electric Energy [J]
-
-These outputs are the parasitic electric power and electric consumption for controls or other electrical devices associated with the dehumidifier. This parasitic electric load is consumed whenever the dehumidifier is available to operate, but is not operating. The model assumes that this parasitic power contributes to heating the zone air (i.e., affects the zone air heat balance). These outputs values are included in the Zone Dehumidifier Electric Power and Zone Dehumidifier Electric Energy output variables.
-
-#### Zone Dehumidifier Part Load Ratio []
-
-This output field is the part-load ratio for the dehumidifier. Part-load ratio is defined as the water removal load to be met (kg/s) divided by the dehumidifier’s water removal rate (kg/s) at the current operating conditions. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
-
-#### Zone Dehumidifier Runtime Fraction []
-
-This output field is the runtime fraction for the dehumidifier. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
-
-#### Zone Dehumidifier Outlet Air Temperature [C]
-
-This output field is dry-bulb temperature of the air leaving the dehumidifier in Celsius. This value represents the dry-bulb temperature of the air leaving the dehumidifier when it is operating. For periods when the dehumidifier is not operating, the outlet air temperature is set equal to the inlet air temperature. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
-
-#### Zone Dehumidifier Condensate Volume Flow Rate [m3/s]
-
-#### Zone Dehumidifier Condensate Volume [m3]
-
-These outputs are the rate and volume of water removed as condensate by the dehumidifier. These reports only appear if a water storage tank is named in the input object. The condensate volume output is also added to a meter with Resource Type = OnSiteWater, End Use Key = Condensate, Group Key = System (ref. Output:Meter objects).
-
-### ZoneHVAC:EnergyRecoveryVentilator
-
-The ZoneHVAC:EnergyRecoveryVentilator - stand alone energy recovery ventilator (ERV) is a single-zone HVAC component used for exhaust air heat recovery (Figure 115). This compound object consists of 3 required components: a generic air-to-air heat exchanger (see object Heat Exchanger:Air to Air:Generic), a supply air fan, and an exhaust air fan (see object Fan:OnOff).
-
-An optional controller (see object ZoneHVAC:EnergyRecoveryVentilator:Controller) may be used to simulate economizer (free cooling) operation, modify air flow rates based on high indoor humidity, or simulate a “push-button� type economizer controller.
-
-![Schematic\_StandAloneERV](media/image293.png)
-
-Figure 115. ZoneHVAC:EnergyRecoveryVentilator compound object Schematic
-
-This compound object models the basic operation of supply and exhaust air fans and an air-to-air heat exchanger. The stand alone ERV operates whenever the unit is scheduled to be available (Availability schedule). The stand alone ERV object can be used in conjunction with an economizer feature whereby heat exchange is suspended whenever free cooling is available (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped). The economizer feature may also be activated based on a time-of-day schedule. Heat exchange is also suspended when air flow rates through the heat exchanger are modified in response to a zone humidistat. When an economizer is used in conjunction with high humidity control, high humidity control has the priority.
-
-To model a stand alone ERV connected to a single zone, the input data file should include the following objects:
-
-- ZoneHVAC:EnergyRecoveryVentilator
-
-- HeatExchanger:AirToAir:SensibleAndLatent
-
-- Fan:OnOff (supply air)
-
-- Fan:OnOff (exhaust air)
-
-- ZoneHVAC:EnergyRecoveryVentilator:Controller (if economizer [free cooling] mode or high humidity control operation is desired)
-
-- ZoneControl:Humidistat (required for high humidity control option)
-
-- SetpointManager:Scheduled (if supply air outlet temperature control is used, Ref. Heat Exchanger:Air to Air:Generic for additional guidance)
-
-- ZoneHVAC:EquipmentConnections
-
-- ZoneHVAC:EquipmentList
-
-- OutdoorAir:NodeList
-
-A description of each input field for this compound object is provided below.
-
-#### Field: Name
-
-A unique user-assigned name for the stand alone ERV unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the unit can operate during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can operate during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit will not operate. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Heat Exchanger Name
-
-The user-assigned name corresponding to the air-to-air heat exchanger used in this compound object. The only allowable type is:.
-
-HeatExchanger:AirToAir:SensibleAndLatent
-
-#### Field: Supply Air Flow Rate
-
-The supply air flow rate through the ERV unit in cubic meters per second at standard temperature and pressure (dry air at 20<sup>o</sup> C drybulb). The program uses local barometric pressure to account for altitude using the equation for "standard atmospheric" pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
-
-p=101325\*(1-2.25577E-05\*Z)\*\*5.2559
-
-where p=pressure in Pa and Z=altitude in m
-
-Note that this flow rate must be within the valid air flow range for the heat exchanger (ref: HeatExchanger:AirToAir:SensibleAndLatent in the Engineering Document). In addition, this flow rate must be less than or equal to the supply fan air flow rate (Fan:OnOff). If the supply air flow rate is less than the exhaust air flow rate, the zone infiltration (ref: ZoneInfiltration) should be specified accordingly (the infiltration induced by imbalanced air flows is not accounted for automatically). The ERV supply air flow rate may also be autosized using the ventilation rate per floor area and/or ventilation rate per occupant fields below. When autosizing, the heat exchanger and fan air flow rates should also be autosized.
-
-Note: The supply air inlet node specified in the generic heat exchanger object must be an outdoor air node (ref: OutdoorAir:Node and OutdoorAir:NodeList). The supply air outlet node specified in the generic heat exchanger object must be a zone air inlet node (ref: ZoneHVAC:EquipmentConnections).
-
-#### Field: Exhaust Air Flow Rate
-
-The exhaust air flow rate through the ERV unit in cubic meters per second at standard temperature and pressure (dry air at 20<sup>o</sup> C drybulb). The program uses local barometric pressure to account for altitude using the equation for "standard atmospheric" pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
-
-p=101325\*(1-2.25577E-05\*Z)\*\*5.2559
-
-where p=pressure in Pa and Z=altitude in m
-
-Note that this flow rate must be within the valid air flow range for the heat exchanger (ref: HeatExchanger:AirToAir:SensibleAndLatent in the Engineering Document). In addition, this flow rate must be less than or equal to the exhaust fan air flow rate (Fan:OnOff). If the exhaust air flow rate is greater than the supply air flow rate, the zone infiltration (ref: ZoneInfiltration) should be specified accordingly (the infiltration induced by imbalanced air flows is not accounted for automatically). The ERV exhaust air flow rate may also be autosized using the ventilation rate per floor area and/or ventilation rate per occupant fields below. When autosizing, the heat exchanger and fan air flow rates should also be autosized.
-
-Note: The exhaust air inlet node specified in the generic heat exchanger object must be a zone air exhaust node (ref: ZoneHVAC:EquipmentConnections).
-
-#### Field: Supply Air Fan Name
-
-The name of the supply air fan used in this object. Fan type must be Fan:OnOff.
-
-#### Field: Exhaust Air Fan Name
-
-The name of the exhaust air fan used in this object. Fan type must be Fan:OnOff.
-
-#### Field: Controller Name
-
-This optional field specifies the name of the controller used by this compound component if economizer (free cooling) mode or high humidity control operation is desired. Controller type must be ZoneHVAC:EnergyRecoveryVentilator:Controller.
-
-#### Field: Ventilation Rate per Unit Floor Area
-
-This optional numeric field defines the ventilation rate per unit floor area in cubic meters per second per square meter. This field is only used when the supply and exhaust air flow rates are autosized.
-
-#### Field: Ventilation Rate per Occupant
-
-This optional numeric field defines the ventilation rate per occupant in cubic meters per second per occupant. This field is only used when the supply and exhaust air flow rates are autosized.
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this Stand Alone ERV  object’s fan. If the Stand Alone ERV is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this Stand Alone ERV  object should be on or off.
-
-
-
-Following is an example input for this compound object and associated objects that may be defined:
-
-
-```idf
-ZoneHVAC:EnergyRecoveryVentilator,
-    Stand Alone ERV 1,                        !- Stand alone ERV name
-    FanAndCoilAvailSched,                     !- Availability schedule name
-    OA Heat Recovery 1,                       !- Heat exchanger name
-    0.05,                                     !- Supply air flow rate {m3/s}
-    0.05,                                     !- Exhaust air flow rate {m3/s}
-    Stand Alone ERV Supply Fan,               !- Supply air fan name
-    Stand Alone ERV Exhaust Fan,              !- Exhaust air fan name
-    ERV OA Controller 1;                      !- ERV controller name
-
-
-OutdoorAir:NodeLine,
-    OutsideAirInletNodes;       !- 1st Node name or node list name
-
-
-NodeList,
-    OutsideAirInletNodes,       !- Node List Name
-    ERV Outdoor air Inlet Node; !- Node_ID_1
-
-
-
-
-ZoneHVAC:EquipmentConnections,
-    RESISTIVE ZONE,      !- Zone Name
-    Zone1Equipment,      !- List Name: Zone Equipment
-    Zone1Inlets,         !- List Name: Zone Inlet Nodes
-    Zone1Exhausts,       !- List Name: Zone Exhaust Nodes
-    Zone 1 Node,         !- Zone Air Node Name
-    Zone 1 Outlet Node;  !- Zone Return Air Node Name
-
-
-ZoneHVAC:EquipmentList,
-    Zone1Equipment,                          !-Name
-ZoneHVAC:EnergyRecoveryVentilator,  !- KEY--Zone Equipment Type 1
-    Stand Alone ERV 1,                       !- Type Name 1
-    1,                                       !- Cooling Priority
-    1;                                       !- Heating Priority
-
-
-NodeList,
-    Zone1Inlets,                             !- Node List Name
-    Stand Alone ERV Supply Fan Outlet Node;  !- Node_ID_1
-
-
-NodeList,
-    Zone1Exhausts,         !- Node List Name
-    Zone 1 Exhaust Node;   !- Node_ID_1
-
-
-ZoneHVAC:EnergyRecoveryVentilator:Controller,
-    ERV OA Controller 1,           !- ERV controller name
-    0.05,                          !- Outdoor air flow rate {m3/s}
-    19.,                           !- Temperature high limit {C}
-    14.,                           !- Temperature low limit {C}
-    0.0,                           !- Enthalpy high limit {J/kg}
-    NoExhaustAirTemperatureLimit,     !- Exhaust air temperature limit
-    NoExhaustAirEnthalpyLimit; !- Exhaust air enthalpy limit
-
-
-
-
-HeatExchanger:AirToAir:SensibleAndLatent,
-    OA Heat Recovery 1,            !- Heat exchanger name
-    FanAndCoilAvailSched,          !- Availability schedule name
-    0.05,                          !- Nominal supply air flow rate {m3/s}
-    .76,                           !- Sensible effectiveness at 100% airflow heating condition
-    .68,                           !- Latent effectiveness at 100% airflow heating condition
-    .81,                           !- Sensible effectiveness at 75% airflow heating condition
-    .73,                           !- Latent effectiveness at 75% airflow heating condition
-    .76,                           !- Sensible effectiveness at 100% airflow cooling condition
-    .68,                           !- Latent effectiveness at 100% airflow cooling condition
-    .81,                           !- Sensible effectiveness at 75% airflow cooling condition
-    .73,                           !- Latent effectiveness at 75% airflow cooling condition
-    ERV Outdoor air Inlet Node,    !- Supply air inlet node name
-    Heat Recovery Outlet Node,     !- Supply air outlet node name
-    Zone 1 Exhaust Node,           !- Exhaust air inlet node name
-    Heat Recovery Secondary Outlet Node,  !- Exhaust air outlet node name
-    50.0,                          !- Nominal electric power {W}
-    Yes,                           !- Supply air outlet temperature control
-    Rotary,                        !- Heat exchanger type
-    MinimumExhaustTemperature,   !- Frost control type
-    1.7;                           !- Threshold temperature
-
-
-
-
-Fan:OnOff,
-    Stand Alone ERV Supply Fan,               !- Fan Name
-    FanAndCoilAvailSched,                     !- Availability Schedule Name
-    0.5,                                      !- Fan Total Efficiency
-    75.0,                                     !- Delta Pressure {Pa}
-    0.05,                                     !- Max Flow Rate {m3/s}
-    0.9,                                      !- Motor Efficiency
-    1.0,                                      !- Motor In Airstream Fraction
-    Heat Recovery Outlet Node,                !- Fan_Inlet_Node
-    Stand Alone ERV Supply Fan Outlet Node;   !- Fan_Outlet_Node
-
-
-Fan:OnOff,
-    Stand Alone ERV Exhaust Fan,              !- Fan Name
-    FanAndCoilAvailSched,                     !- Availability Schedule Name
-    0.5,                                      !- Fan Total Efficiency
-    75.0,                                     !- Delta Pressure {Pa}
-    0.05,                                     !- Max Flow Rate {m3/s}
-    0.9,                                      !- Motor Efficiency
-    1.0,                                      !- Motor In Airstream Fraction
-    Heat Recovery Secondary Outlet Node,      !- Fan_Inlet_Node
-    Stand Alone ERV Exhaust Fan Outlet Node;  !- Fan_Outlet_Node
-
-
-SetpointManager:Scheduled,
-    Heat Exhchanger Supply Air Temp Manager,  !- Name
-    Temperature,  !- Control variable
-    Heat Exchanger Supply Air Temp Sch,  !- Schedule Name
-    Heat Exchanger Supply Air Nodes;     !- Name of the set point Node List
-
-
-NodeList,
-    Heat Exchanger Supply Air Nodes,  !- Node List Name
-    Heat Recovery Outlet Node;        !- Node_ID_1
-```
-
-
-### Energy Recovery Ventilator (ERV) (ZoneHVAC) Outputs
-
-* HVAC,Average,Zone Ventilator Electric Power[W]
-
-* HVAC,Sum,Zone Ventilator Electric Energy [J]
-
-* HVAC,Average,Zone Ventilator Total Cooling Rate [W]
-
-* HVAC,Sum,Zone Ventilator Total Cooling Energy [J]
-
-* HVAC,Average,Zone Ventilator Total Heating Rate [W]
-
-* HVAC,Sum,Zone Ventilator Total Heating Energy [J]
-
-* HVAC,Average,Zone Ventilator Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Ventilator Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Ventilator Sensible Heating Rate [W]
-
-* HVAC,Sum,Zone Ventilator Sensible Heating Energy [J]
-
-* HVAC,Average,Zone Ventilator Latent Cooling Rate [W]
-
-* HVAC,Sum,Zone Ventilator Latent Cooling Energy [J]
-
-* HVAC,Average,Zone Ventilator Latent Heating Rate [W]
-
-* HVAC,Sum,Zone Ventilator Latent Heating Energy [J]
-
-* HVAC,Average,Zone Ventilator Supply Fan Availability Status []
-
-#### Zone Ventilator Electric Power [W]
-
-This output field is the electric consumption rate of the stand alone energy recovery ventilator in Watts. This rate includes the electric consumption by the supply air fan, exhaust air fan and the generic air-to-air heat exchanger.
-
-#### Zone Ventilator Electric Energy [J]
-
-This output field is the electric consumption of the stand alone energy recovery ventilator in Joules for the timestep being reported. This value includes the electric consumption by the supply air fan, exhaust air fan and the generic air-to-air heat exchanger.
-
-#### Zone Ventilator Total Cooling Rate [W]
-
-This output field is the total (enthalpy) heat extraction rate of the stand alone energy recovery ventilator from the zone in Watts. This value is calculated using the supply air outlet mass flow rate, and the enthalpy difference of the supply outlet and exhaust inlet air streams. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
-
-#### Zone Ventilator Total Cooling Energy [J]
-
-This output field is the total (enthalpy) heat extraction of the stand alone energy recovery ventilator from the zone in Joules over the timestep being reported. This value is calculated using the supply air outlet mass flow rate, the enthalpy difference of the supply outlet and exhaust inlet air streams, and the HVAC system timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are summed for the timestep being reported.
-
-#### Zone Ventilator Total Heating Rate [W]
-
-This output field is the total (enthalpy) heat addition rate of the stand alone energy recovery ventilator to the zone in Watts. This value is calculated using the supply air outlet mass flow rate, and the enthalpy difference of the supply outlet and exhaust inlet air streams. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
-
-#### Zone Ventilator Total Heating Energy [J]
-
-This output field is the total (enthalpy) heat addition of the stand alone energy recovery ventilator to the zone in Joules over the timestep being reported. This value is calculated using the supply air outlet mass flow rate, the enthalpy difference of the supply outlet and exhaust inlet air streams, and the HVAC system timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are summed for the timestep being reported.
-
-#### Zone Ventilator Sensible Cooling Rate [W]
-
-This output is the moist air sensible heat extraction rate of the stand alone energy recovery ventilator from the zone in Watts. This value is calculated using the supply air outlet mass flow rate, and the enthalpy difference of the supply outlet and exhaust inlet air streams at a constant humidity ratio. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
-
-#### Zone Ventilator Sensible Cooling Energy [J]
-
-This output is the moist air sensible heat extraction of the stand alone energy recovery ventilator from the zone in Joules over the timestep being reported. This value is calculated using the supply air outlet mass flow rate, the enthalpy difference of the supply outlet and exhaust inlet air streams at a constant humidity ratio, and the HVAC system timestep. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are summed for the timestep being reported.
-
-#### Zone Ventilator Sensible Heating Rate [W]
-
-This output is the sensible heat addition rate of the stand alone energy recovery ventilator to the zone in Watts. This value is calculated using the supply air outlet mass flow rate, and the enthalpy difference of the supply outlet and exhaust inlet air streams at a constant humidity ratio. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
-
-#### Zone Ventilator Sensible Heating Energy [J]
-
-This output is the sensible heat addition of the stand alone energy recovery ventilator to the zone in Joules over the timestep being reported. This value is calculated using the supply air outlet mass flow rate, the enthalpy difference of the supply outlet and exhaust inlet air streams at a constant humidity ratio, and the HVAC system timestep. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are summed for the timestep being reported.
-
-#### Zone Ventilator Latent Cooling Rate [W]
-
-This output is the latent heat extraction (dehumidification) rate of the stand alone energy recovery ventilator from the zone in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the stand alone ERV. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
-
-#### Zone Ventilator Latent Cooling Energy [J]
-
-This output is the latent heat extraction (dehumidification) of the stand alone energy recovery ventilator from the zone in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the stand alone ERV. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are summed for the timestep being reported.
-
-#### Zone Ventilator Latent Heating Rate [W]
-
-This output is the latent heat addition (humidification) rate of the stand alone energy recovery ventilator to the zone in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the stand alone ERV. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
-
-#### Zone Ventilator Latent Heating Energy [J]
-
-This output is the latent heat addition (humidification) of the stand alone energy recovery ventilator to the zone in Joules over the timestep being reported. This value is calculated as the difference between the total energy delivered to the zone and the sensible energy delivered to the zone by the stand alone ERV. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are summed for the timestep being reported.
-
-#### Zone Ventilator Supply Fan Availability Status []
-
-This is the availability status of the Stand Alone ERV  fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the Stand Alone ERV  object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List (with or without Hybrid Ventilation Manager), rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-### ZoneHVAC:TerminalUnit:VariableRefrigerantFlow
-
-Zone terminal units with variable refrigerant flow DX coils are used exclusively with variable refrigerant flow (VRF) air conditioning systems (Ref. AirConditioner:VariableRefrigerantFlow object). The zone terminal units are connected to a zone using the inlet and exhaust node names specified in a ZoneHVAC:EquipmentConnections object. The zone exhaust node has the same name as the terminal unit air inlet node. The zone inlet node has the same name as the terminal unit air outlet node. The zone terminal unit is also listed in a zone’s equipment list and will typically be the first equipment operating for both cooling and heating (i.e., Sequence = 1 in the ZoneHVAC:EquipmentList). Other ZoneHVAC equipment may be used in the same zone and should be sequenced to operate after the zone terminal units (i.e., sequence = 2 or higher)
-
-The terminal units operate to satisfy a heating or cooling load in a zone based on a zone thermostat temperature set point. A direct-expansion (DX) cooling and/or DX heating coil is specified depending on the operating mode required. Both a DX cooling and DX heating coil will typically be installed in the terminal unit, however only one may be used if desired. Outdoor ventilation air is modeled with the use of an optional outside air mixer object. Outside air may be provided to the zone only when the coil is operating or can be supplied continuously even when the coil is not operating. A supply air fan is also required and can be modeled as either draw through or blow through.
-
-#### Field: Zone Terminal Unit Name
-
-This alpha field defines a unique user-assigned name for an instance of a variable refrigerant flow zone terminal unit. Any reference to this terminal unit by another object will use this name. The zone terminal unit name must be specified in a ZoneTerminalUnitList object to connect this terminal unit to an AirConditioner:VariableRefrigerantFlow object.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the terminal unit operates during a given time period. A schedule value equal to 0 denotes that the terminal unit must be off for that time period. A value greater than 0 denotes that the terminal unit is available to operate during that time period. This schedule may be used to completely disable the terminal unit as required. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Terminal Unit Air Inlet Node Name
-
-This alpha field defines the name of the terminal unit air inlet node. This node name should be the same as a zone exhaust node (ref: ZoneHVAC:EquipmentConnections).
-
-#### Field: Terminal Unit Air Outlet Node Name
-
-This alpha field defines the name of the terminal unit air outlet node. This node name should be the same as a zone inlet node (ref: ZoneHVAC:EquipmentConnections).
-
-#### Field: Cooling Supply Air Flow Rate
-
-This numeric field defines the terminal unit’s operating volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in cooling mode.
-
-#### Field: No Cooling Supply Air Flow Rate
-
-This numeric field defines the terminal unit’s operating volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit’s cooling coil is not operating and the previous mode was cooling.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field defines the terminal unit’s operating volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in heating mode.
-
-#### Field: No Heating Supply Air Flow Rate
-
-This numeric field defines the terminal unit’s operating volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit’s heating coil is not operating and the previous mode was heating.
-
-#### Field: Cooling Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in cooling mode.
-
-#### Field: Heating Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in heating mode.
-
-#### Field: No Load Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is not operating in cooling or heating mode.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This alpha field defines the name of the supply air fan operating mode schedule. Schedule values equal to 0 denote cycling fan/cycling coil operation. All other schedule values denote constant fan/cycling coil operation.
-
-#### Field: Supply Air Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. If this field is left blank, the default is blow through.
-
-The first choice stands for “blow through fan�. This means that the unit consists of a fan followed by the DX coils. The fan “blows through� the cooling and heating coils. If an outside air mixer is used, the fan inlet connects to the outside air mixer’s mixed air node. If an outside air mixer is not used, the fan inlet connects to the zone exhaust node. For this configuration, the fan outlet always connects to the DX cooling coil inlet node (or if a DX cooling coil is not used, the DX heating coil inlet node).
-
-The second choice stands for “draw through fan�. This means that the unit consists of the DX coil(s) followed by a fan. The fan “draws air through� the DX coil(s). In this case the fan inlet always connects to the DX heating coil outlet node (or if a DX heating coil is not use, the DX cooling coil outlet node) and the fan outlet node always connects to the zone inlet node.
-
-#### Field: Supply Air Fan Object Type
-
-This choice field contains the identifying type of supply air fan specified for the furnace. Fan type must be **Fan:OnOff** or **Fan:ConstantVolume**. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e. Supply Air Fan Operating Mode Schedule values are at times 0).
-
-#### Field: Supply Air Fan Object Name
-
-This alpha field defines the name of the terminal unit’s supply air fan.
-
-#### Field: Outside Air Mixer Object Type
-
-This alpha field contains the identifying type of outside air mixer specified for the terminal unit. Outside air mixer type must be **OutsideAir:Mixer**. This field should be left blank when an outside air mixer is not simulated.
-
-#### Field: Outside Air Mixer Object Name
-
-This alpha field defines the name of the terminal unit’s outside air mixer. If this field is left blank, an outside air mixer is not simulated.
-
-#### Field: DX Cooling Coil Object Type
-
-This choice field contains the identifying type of the terminal unit’s DX cooling coil. The only valid DX cooling coil type is **Coil:Cooling:DX:VariableRefrigerantFlow**. This field should be left blank when a DX cooling coil is not simulated.
-
-#### Field: DX Cooling Coil Name
-
-This alpha field defines the name of the terminal unit’s DX cooling coil. If this field is left blank, a DX cooling coil is not simulated.
-
-#### Field: DX Heating Coil Object Type
-
-This choice field contains the identifying type of the terminal unit’s DX heating coil. The only valid DX heating coil type is **Coil:Heating:DX:VariableRefrigerantFlow**. This field should be left blank when a DX heating coil is not simulated.
-
-#### Field: DX Heating Coil Object Name
-
-This alpha field defines the name of the terminal unit’s DX heating coil. This field should be left blank when a DX heating coil is not simulated.
-
-#### Field: Zone Terminal Unit On Parasitic Electric Energy Use
-
-This numeric field defines the parasitic electrical energy use of the zone terminal unit when either terminal unit coil is operating. When in cooling mode, this electric energy use is reported in a zone terminal unit cooling electric consumption output variable. When in heating mode, this electric energy use is reported in a zone terminal unit heating electric consumption output variable.
-
-#### Field: Zone Terminal Unit Off Parasitic Electric Energy Use
-
-This numeric field defines the parasitic electrical energy use of the zone terminal unit when the terminal unit coil(s) is not operating. When the previous mode was cooling, this electric energy use is reported in a zone terminal unit cooling electric consumption output variable. When the previous mode was heating, this electric energy use is reported in a zone terminal unit heating electric consumption output variable.
-
-#### Field: Rated Total Heating Capacity Sizing Ratio
-
-This numeric field defines the ratio of the heating coil to cooling coil size when autosizing is used. The model assumes that when used, this value will be greater than 1. This field supersedes the Rated Total Heating Capacity Sizing Ratio entered in the AirConditioner:VariableRefrigerantFlow object. If this field is left blank, the value entered in the parent object is used for sizing. If neither field is used, the sizing ratio is assumed to be 1.
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this Zone Terminal Unit object’s fan. If the Zone Terminal Unit is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this Zone Terminal Unit object should be on or off.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Cooling Supply Air Flow Rate in this VRF terminal unit zone HVAC object. The scaled Supply Air Flow Rate in turn is used to size cooling and heating capacity of the unit.
-
-
-
-Following is an example input for a ZoneHVAC:TerminalUnit:VariableRefrigerantFlow object.
-
-```idf
-ZoneHVAC:TerminalUnit:VariableRefrigerantFlow,
-    Zone 1 TU,               !- Zone Terminal Unit Name
-    TU Availability Schedule,!- Terminal Unit Availability schedule
-    TU1 Inlet Node,          !- Terminal Unit Air Inlet Node Name
-    TU1 Outlet Node,         !- Terminal Unit Air Outlet Node Name
-    0.005,                   !- Cooling Supply Air Flow Rate {m3/s}
-    0,                       !- No Cooling Supply Air Flow Rate {m3/s}
-    0.005,                   !- Heating Supply Air Flow Rate {m3/s}
-    0,                       !- No Heating Supply Air Flow Rate {m3/s}
-    0.001,                   !- Cooling Outdoor Air Flow Rate
-    0.001,                   !- Heating Outdoor Air Flow Rate
-    0,                       !- No Load Outdoor Air Flow Rate
-    TU1 Fan Op Schedule,     !- Supply Air Fan Operating Mode Schedule Name
-    drawthrough,             !- Supply Air Fan placement
-    Fan:ConstantVolume,      !- Supply Air Fan Object Type
-    TU1 SA Fan,              !- Supply Air Fan Object Name
-    OutdoorAir:Mixer,        !- Outside Air Mixer Object Type
-    TU1 OA Mixer,            !- Outside Air Mixer Object Name
-    COIL:Cooling:DX:VariableRefrigerantFlow,  !- Cooling Coil Object Type
-    TU1 VRF DX Cooling Coil, !- Cooling Coil Object Name
-    COIL:Heating:DX:VariableRefrigerantFlow,  !- Heating Coil Object Type
-    TU1 VRF DX Heating Coil, !- Heating Coil Object Name
-    30,                      !- Zone Terminal Unit On Parasitic Electric Energy Use {W}
-    20,                      !- Zone Terminal Unit Off Parasitic Electric Energy Use {W}
-    ,                        !- Rated Total Heating Capacity Sizing Ratio {W/W}
-    ;                        !- Availability Manager List Name
-```
-
-### Variable Refrigerant Flow (VRF) Terminal Unit (ZoneHVAC) Outputs
-
-* HVAC,Average,Zone VRF Air Terminal Total Cooling Rate [W]
-
-* HVAC,Sum, Zone VRF Air Terminal Total Cooling Energy [J]
-
-* HVAC,Average, Zone VRF Air Terminal Sensible Cooling Rate [W]
-
-* HVAC,Sum, Zone VRF Air Terminal Sensible Cooling Energy [J]
-
-* HVAC,Average, Zone VRF Air Terminal Latent Cooling Rate [W]
-
-* HVAC,Sum, Zone VRF Air Terminal Latent Cooling Energy [J]
-
-* HVAC,Average,Zone VRF Air Terminal Total Heating Rate [W]
-
-* HVAC,Sum, Zone VRF Air Terminal Total Heating Energy [J]
-
-* HVAC,Average, Zone VRF Air Terminal Sensible Heating Rate [W]
-
-* HVAC,Sum, Zone VRF Air Terminal Sensible Heating Energy [J]
-
-* HVAC,Average, Zone VRF Air Terminal Latent Heating Rate [W]
-
-* HVAC,Sum, Zone VRF Air Terminal Latent Heating Energy [J]
-
-* HVAC,Average, Zone VRF Air Terminal Cooling Electric Power [W]
-
-* HVAC,Sum, Zone VRF Air Terminal Cooling Electric Energy [J]
-
-* HVAC,Average,Zone VRF Air Terminal Heating Electric Power [W]
-
-* HVAC,Sum,Zone VRF Air Terminal Heating Electric Energy [J]
-
-* HVAC,Average, Zone VRF Air Terminal Fan Availability Status []
-
-
-#### Zone VRF Air Terminal Total Cooling Rate [W]
-
-This field is the total (sensible and latent) cooling rate output of the terminal unit in Watts. This is determined by terminal unit inlet and outlet air conditions and the air mass flow rate through the unit. This value describes the total energy rate delivered to the zone.
-
-#### Zone VRF Air Terminal Total Cooling Energy [J]
-
-This is the total (sensible plus latent) cooling output of the terminal unit in Joules over the time step being reported. This is determined by the terminal unit inlet and outlet air conditions and the air mass flow rate through the unit. This value describes the total cooling energy delivered to the zone.
-
-#### Zone VRF Air Terminal Sensible Cooling Rate [W]
-
-This output is the moist air sensible cooling rate output of the terminal unit in Watts. This is determined by enthalpy difference between the inlet and outlet air temperature at a constant humidity ratio, using the minimum of the inlet and outlet air node humidity ratios, and the air mass flow rate through the unit. This value describes the sensible cooling energy rate delivered to the zone.
-
-#### Zone VRF Air Terminal Sensible Cooling Energy [J]
-
-This is the moist air sensible cooling output of the terminal unit in Joules for the time step being reported. This is determined by enthalpy difference between the inlet and outlet air temperature at a constant humidity ratio, using the minimum of the inlet and outlet air node humidity ratios, and the air mass flow rate through the unit. This value describes the sensible cooling energy delivered to the zone.
-
-#### Zone VRF Air Terminal Latent Cooling Rate [W]
-
-This is the latent cooling rate output of the terminal unit in Watts. This is determined by the inlet and outlet air humidity ratios and the air mass flow rate through the unit. This value describes the latent cooling energy rate delivered to the zone.
-
-#### Zone VRF Air Terminal Latent Cooling Energy [J]
-
-This is the latent cooling output of the terminal unit in Joules for the time step being reported. This is determined by the inlet and outlet air humidity ratios and the air mass flow rate through the unit. This value describes the latent cooling energy delivered to the zone.
-
-#### Zone VRF Air Terminal Total Heating Rate [W]
-
-This field is the total enthalpic heating rate output of the terminal unit in Watts. This is determined by the terminal unit inlet and outlet air conditions and the air mass flow rate through the unit. This value describes the total heating energy rate delivered to the zone.
-
-#### Zone VRF Air Terminal Total Heating Energy [J]
-
-This is the total enthalpic heating output of the terminal unit in Joules over the time step being reported. This is determined by the terminal unit inlet and outlet air conditions and the air mass flow rate through the unit. This value describes the total heating energy delivered to the zone.
-
-#### Zone VRF Air Terminal Sensible Heating Rate [W]
-
-This output is the moist air sensible heating rate output of the terminal unit in Watts. This is determined by enthalpy difference between the inlet and outlet air temperature at a constant humidity ratio, using the minimum of the inlet and outlet air node humidity ratios, and the air mass flow rate through the unit. This value describes the sensible heating energy rate delivered to the zone.
-
-#### Zone VRF Air Terminal Sensible Heating Energy [J]
-
-This is the moist air sensible heating output of the terminal unit in Joules for the time step being reported. This is determined by enthalpy difference between the inlet and outlet air temperature at a constant humidity ratio, using the minimum of the inlet and outlet air node humidity ratios, and the air mass flow rate through the unit. This value describes the sensible heating energy delivered to the zone.
-
-#### Zone VRF Air Terminal Latent Heating Rate [W]
-
-This is the latent heating rate output of the terminal unit in Watts. This is determined by the inlet and outlet air specific humidity ratios and the air mass flow rate through the unit. This value describes the latent heating energy rate delivered to the zone.
-
-#### Zone VRF Air Terminal Latent Heating Energy [J]
-
-This is the latent heating output of the terminal unit in Joules for the time step being reported. This is determined by the inlet and outlet air specific humidity ratios and the air mass flow rate through the unit. This value describes the latent heating energy delivered to the zone.
-
-#### Zone VRF Air Terminal Cooling Electric Power[W]
-
-This output field is the parasitic electricity consumption rate of the zone terminal unit in Watts. The consumption rate includes parasitic electricity used by the zone terminal unit’s transformers, controls, or other electricity consuming devices. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. The terminal unit parasitic on and off electricity is reported in this cooling output variable when the unit operates in cooling mode or the most recent operation was for cooling.
-
-#### Zone VRF Air Terminal Cooling Electric Energy [J]
-
-This output field is the electricity consumption of the zone terminal unit in Joules for the time period being reported. The consumption includes parasitic electricity used by the zone terminal unit’s transformers, controls, or other electricity consuming devices. This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported. The terminal unit parasitic on and off electricity consumption is reported in this cooling output variable when the unit operates in cooling mode or the most recent operation was for cooling. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
-
-#### Zone VRF Air Terminal Heating Electric Power[W]
-
-This output field is the parasitic electricity consumption rate of the zone terminal unit in Watts. The consumption rate includes parasitic electricity used by the zone terminal unit’s transformers, controls, or other electricity consuming devices. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. The terminal unit parasitic on and off electricity is reported in this heating output variable when the unit operates in heating mode or the most recent operation was for heating.
-
-#### Zone VRF Air Terminal Heating Electric Energy [J]
-
-This output field is the electricity consumption of the zone terminal unit in Joules for the time period being reported. The consumption includes parasitic electricity used by the zone terminal unit’s transformers, controls, or other electricity consuming devices. This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported. The terminal unit parasitic on and off electricity consumption is reported in this heating output variable when the unit operates in heating mode or the most recent operation was for heating. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Zone VRF Air Terminal Fan Availability Status []
-
-This is the availability status of the Zone Terminal Unit fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the Zone Terminal Unit object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List along with Hybrid Ventilation Manager, rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-Group – Unitary Equipment
--------------------------
-
-### Furnace and Unitary Systems
-
-The components
-
-* AirLoopHVAC:UnitarySystem
-
-* AirLoopHVAC:Unitary:Furnace:HeatOnly
-
-* AirLoopHVAC:Unitary:Furnace:HeatCool
-
-* AirLoopHVAC:UnitaryHeatOnly
-
-* AirLoopHVAC:UnitaryHeatCool
-
-* AirLoopHVAC:UnitaryHeatPump:AirToAir
-
-* AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed
-
-are compound components usually placed in the primary air loop as the sole component. On the zone equipment side they are usually connected to one or more zones through uncontrolled terminal units (i.e., AirTerminal:SingleDuct:Uncontrolled objects). The maximum or design air flow rate through the furnace or unitary system should usually be set equal to the sum of the maximum air flow rates through the terminal unit objects. However, the simulation program can usually account for unequal air flows if the user wishes to model this scenario.
-
-The following HVAC equipment types are allowed in the air loop. The component matrix shows which coils and fans are allowed with which equipment models.
-
-![](media/AirLoopComponentMatrix.png)
-
-### AirLoopHVAC:UnitarySystem
-
-The AirloopHVAC:UnitarySystem object is intended to replace all other air loop equipment, although other system types are still available. This system is unique in that it can accommodate all fan and coil types whereas other system types are specific to the type of fan and coil available for simulation. Additionally, although the AirloopHVAC:UnitarySystem is intended for use in the primary airloop, this object can be modeled as zone equipment (i.e., listed in a ZoneHVAC:EquipmentList) or as an outside air system component (i.e., listed in a AirLoopHVAC:OutdoorAirSystem:EquipmentList).
-
-The AirLoopHVAC:UnitarySystem object is a “virtual� component that consists of a fan component (OnOff, ConstantVolume, VariableVolume, or ComponentModel), a cooling coil component, a heating coil component, and a reheat coil as shown in Figure 117. When a draw through configuration is desired, the fan is placed directly after the heating coil. If dehumidification control is selected, a reheat coil component is also required. If the reheat coil is present and the dehumidification control type input is not specified as CoolReheat, the reheat coil will not be active.  All of the fan and coil components are optional which allows the AirLoopHVAC:UnitarySystem object to be configured for fan-only, heating-only, cooling-only, or both heating and cooling.  It may also be applied without a fan, controlling one or more coils, similar to the function of CoilSystem:Cooling:DX.
-
-![](media/image294.png)
-
-Figure 1. Schematic of the EnergyPlus Unitary System
-
-Links to the fan, cooling coil, heating coil and reheat coil specifications are provided in the unitary system input data syntax. In addition, the control zone name and the system design operating conditions are specified by the unitary system inputs.
-
-#### Multi-Speed Fan and Water Coils In Unitary System
-Multi-speed fan chilled and hot water coils Air Handling Unit (AHU) can be modeled using Airloop Unitary System HVAC object (AirloopHVAC:UnitarySystem). AHU with chilled and hot water coils is setup by specifying Fan:OnOff and DesignSpecificationPerformance:MultiSpeed objects in Unitary System. The design specification performance object allows running the chilled and hot water coils capacity control using a multi-speed supply air fan. The multi-speed fan capacity control for chilled and hot water coil AHU is performed by modulating the supply air flow rate while maintaining a constant water flow rate. The chilled or hot water flow rates is set at maximum fixed flow rate when there is cooling or heating load and the water flow rate is set to zero when there is no load. Such control strategy is called two-position cooling or heating coil control. The fan speed selection depends on the current load, at lower load the fan is operated at minimum speed (Speed = 1) and the fan speed level increases progressively as the load increases until it reaches the maximum speed level specified. The multi-speed fan operation is modulated between the speeds to meet the current load. When the supply air fan is cycling between consecutive speeds levels, the speed ratio is calculated that indicates what fraction of the time step that the system run at the higher of the two speeds. At lower load, the fan may cycle on-off or run continuously depending the fan operating schedule specified.  When the fan is cycling a part-load ratio is calculated to reflect the proportion of the system timestep the fan and coils were operating. In continuous fan operating mode only the coil cycles on-off and the part-load ratio applies to the coil only. Multi-speed fan capacity control is allowed with load based control type only.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the unitary system.
-
-#### Field: Control Type
-
-This alpha field contains control type i.e. load based or setpoint based for the unitary system. Valid choices are Load and SetPoint. Load control requires a Controlling Zone name and SetPoint control requires set points at each coil outlet node. A single set point at the outlet of the system is allowed but not recommended.
-
-#### Field: Controlling Zone or Thermostat Location
-
-This alpha field contains the identifying zone name where the thermostat controlling the unitary system is located.
-
-#### Field: Dehumidification Control Type
-
-This alpha field contains the type of dehumidification control. The following options are valid for this field:
-
-**None** - meet sensible load only, no active dehumidification control
-
-**Multimode** - activate enhanced dehumidification mode as needed and meet sensible load. This option is used to model DX equipment with a controllable heat exchanger assisting the DX cooling coil for improved dehumidification. It is valid only with cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted.
-
-**CoolReheat** - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. If cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted, then the heat exchanger is assumed to always transfer energy between the cooling coil’s inlet and outlet airstreams when the cooling coil is operating.
-
-The default is **None**. For the other dehumidification control modes, the maximum humidity setpoint is used. This must be set using a **ZoneControl:Humidistat** object. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate. If the dehumidification control type is specified as **CoolReheat**, then two additional inputs (reheat coil type and name) are also required as shown below. Although the reheat coil is required only when **CoolReheat** is selected, the optional reheat coil may be present for any of the allowed Dehumidification Control Types. If the reheat coil is present and the dehumidification control type is not specified as **CoolReheat**, the reheat coil will not be active,
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name which contains information on the availability of the unitary system to operate. A schedule value equal to 0 denotes that the unitary system must be off for that time period. A value greater than 0 denotes that the unitary system is available to operate during that time period. This schedule may be used to completely disable the unitary system as required. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Unitary System Air Inlet Node Name
-
-This alpha field contains the unitary system inlet node name.
-
-#### Field: Unitary System Air Outlet Node Name
-
-This alpha field contains the unitary system outlet node name.
-
-#### Field: Supply Fan Object Type
-
-This alpha field contains the identifying type of supply air fan specified for the unitary system. Fan type must be **Fan:OnOff,** **Fan:ConstantVolume, Fan:VariableVolume, or Fan:ComponentModel**. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e. Supply Air Fan Operating Mode Schedule values are at times 0). Fan:VariableVolume is used for variable air volume systems or multi- or variable-speed coils. The Fan:ComponentModel may be used in place of the ConstantVolume or VariableVolume fan types to more accurately represent fan performance.
-
-#### Field: Supply Fan Name
-
-This alpha field contains the identifying name given to the unitary system fan.
-
-#### Field: Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. The first choice stands for “blow through fan�. This means that the unit consists of a fan followed by the main cooling and heating coils and supplemental heating coil. The fan “blows through� the cooling and heating coils. The second choice stands for “draw through fan�. This means that the unit consists of the main cooling/heating coil(s) followed by a fan, with the supplemental heater located at the outlet of the fan. The fan “draws air through� the cooling/heating coil(s). If this field is left blank, the default is blow through.
-
-***Field: Supply Air Fan Operating Mode Schedule Name***
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the unitary system supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.
-
-#### Field: Heating Coil Object Type
-
-This alpha field contains the identifying type of heating coil specified in the unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. Allowable coil types are:
-
-* Coil:Heating:DX:SingleSpeed
-
-* Coil:Heating:DX:TwoSpeed
-
-* Coil:Heating:DX:MultiSpeed
-
-* Coil:Heating:DX:VariableSpeed
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-* Coil:Heating:WaterToAirHeatPump:ParameterEstimation
-
-* Coil:Heating:WaterToAirHeatPump:EquationFit
-
-* Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Gas:MultiStage
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Electric:MultiStage
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-* Coil:Heating:Desuperheater
-
-* Coil:UserDefined
-
-#### Field: Heating Coil Name
-
-This alpha field contains the identifying name given to the unitary system heating coil.
-
-#### Field: DX Heating Coil Sizing Ratio
-
-This numeric field is used to adjust heat pump heating capacity with respect to DX cooling capacity. It is used only for DX heat pump configurations (i.e., a DX cooling and heating coil is used).
-
-#### Field: Cooling Coil Object Type
-
-This alpha field contains the identifying type of cooling coil specified in the unitary system. Allowable coil types are:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* Coil:Cooling:DX:SingleSpeed:ThermalStorage
-
-* Coil:Cooling:DX:TwoSpeed
-
-* Coil:Cooling:DX:MultiSpeed
-
-* Coil:Cooling:DX:VariableSpeed
-
-* Coil:Cooling:DX:TwoStageWithHumidityControlMode
-
-* CoilSystem:Cooling:DX:HeatExchangerAssisted
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-* Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
-
-* Coil:Cooling:WaterToAirHeatPump:EquationFit
-
-* Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit
-
-* Coil:Cooling:Water
-
-* Coil:Cooling:Water:DetailedGeometry
-
-* CoilSystem:Cooling:Water:HeatExchangerAssisted
-
-* Coil:UserDefined
-
-#### Field: Cooling Coil Name
-
-This alpha field contains the identifying name given to the unitary system cooling coil.
-
-#### Field: Use DOAS DX Cooling Coil
-
-This input field eanbles DX Cooling coils to be used for 100% outdoor air dedicated outdor air system applications. There are two choices Yes or No. If Yes, the DX coil is used as 100% outdoor DX coil. If No, the DX coil is used as regular DX coil. This input file d is optional and the default is No.
-
-#### Field: DOAS DX Cooling Coil Leaving Minimum Air Temperature
-
-This input field is DX Cooling coils leaving minimum air temperature for frost control. The DX cooling coil leaving air temperature is not allowed to exceed this minimum air temperature. The DX cooling coil frost controller adjusts or limits the desired coil outlet air setpoint temperature when the coil outlet temperature exceeds this minimum temperature limit specified. This input field is optional and only used along with in the input field above. The minimum and maximum values of this input field are 0.0C and 7.2C, and the default value is 2.0°C.
-
-#### Field: Latent Load Control
-
-This alpha field defines the latent load control method. Available choices are SensibleOnlyLoadControl, LatentOnlyLoadControl, LatentWithSensibleLoadControl, or LatentOrSensibleLoadControl. The default choice is SensibleOnlyLoadControl. The SensibleOnlyLoadControl choice will operate to meet only a sensible load, and the LatentOnlyLoadConrol will operate to meet only a latent load. The LatentWithSensibleLoadControl will operate to meet the latent load only if there is a sensible load. The LatentOrSensibleLoadControl will operate to meet either a latent or sensible load.
-
-#### Field: Supplemental Heating Coil Object Type
-
-This alpha field contains the identifying type of supplemental heating coil specified in the unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The Coil:UserDefined object must be configured as a heating coil. Supplemental heating type must be one of:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Desuperheater
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-* Coil:UserDefined
-
-#### Field: Supplemental Heating Coil Name
-
-This alpha field contains the identifying name given to the unitary system reheat coil.
-
-#### Field: Cooling Supply Air Flow Rate Method
-
-This alpha field defines the supply air flow method during cooling operation. Available choices are SupplyAirFlowRate, FlowPerFloorArea, FractionOfAutosizedCoolingValue, FlowPerCoolingCapacity. For each of the choices, a corresponding air flow rate for cooling must be specified.
-
-#### Field: Cooling Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when the cooling coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Cooling Supply Air Flow Rate Method is **SupplyAirFlowRate**.
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-#### Field: Cooling Supply Air Flow Rate Per Floor Area
-
-This numeric field defines the supply air flow rate per floor area leaving the unitary system in meters per second when the cooling coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Cooling Supply Air Flow Rate Method is **FlowPerFloorArea**.
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-#### Field: Cooling Fraction of Autosized Design Cooling Supply Air Flow Rate
-
-This numeric field defines the fraction of autosized supply air flow rate leaving the unitary system when the cooling coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Cooling Supply Air Flow Rate Method is **FractionOfAutosizedCoolingValue**.
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-#### Field: Cooling Supply Air Flow Rate Per Unit of Capacity
-
-This numeric field defines the supply air flow rate per unit of capacity leaving the unitary system when the cooling coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Cooling Supply Air Flow Rate Method is **FlowPerCoolingCapacity**.
-
-#### Field: Heating Supply Air Flow Rate Method
-
-This alpha field defines the supply air flow method during heating operation. Available choices are SupplyAirFlowRate, FlowPerFloorArea, FractionOfAutosizedHeatingValue, FlowPerHeatingCapacity. For each of the choices, a corresponding air flow rate for heating must be specified.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when the heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Heating Supply Air Flow Rate Method is **SupplyAirFlowRate**.
-
-#### Field: Heating Supply Air Flow Rate Per Floor Area
-
-This numeric field defines the supply air flow rate per floor area leaving the unitary system in meters per second when the heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Heating Supply Air Flow Rate Method is **FlowPerFloorArea**.
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-#### Field: Heating Fraction of Autosized Design Heating Supply Air Flow Rate
-
-This numeric field defines the fraction of autosized supply air flow rate leaving the unitary system when the heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Heating Supply Air Flow Rate Method is **FractionOfAutosizedHeatingValue**.
-
-#### Field: Heating Supply Air Flow Rate Per Unit of Capacity
-
-This numeric field defines the supply air flow rate per unit of capacity leaving the unitary system when the heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when Heating Supply Air Flow Rate Method is **FlowPerHeatingCapacity**.
-
-#### Field: No Load Supply Air Flow Rate Method
-
-This alpha field defines the supply air flow method when neither cooling or heating is required. Available choices are SupplyAirFlowRate, FlowPerFloorArea, FractionOfAutosizedCoolingValue, FractionOfAutosizedHeatingValue, FlowPerCoolingCapacity, FlowPerHeatingCapacity. For each of the choices, a corresponding air flow rate must be specified.
-
-#### Field: No Load Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when neither cooling or heating is required (i.e., main cooling/heating coils and supplemental heater are off but the supply air fan operates). This field is only used when the unitary system operating mode is specified as continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the unitary system operating mode is specified as continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the compressor was last operating (for cooling operation or heating operation).
-
-#### Field: No Load Supply Air Flow Rate Per Floor Area
-
-This numeric field defines the supply air flow rate per floor area leaving the unitary system in meters per second when neither cooling or heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when No Load Supply Air Flow Rate Method During is **FlowPerFloorArea**.
-
-#### Field: No Load Fraction of Autosized Cooling Supply Air Flow Rate
-
-This numeric field defines the fraction of autosized supply air flow rate leaving the unitary system when neither cooling or heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when No Load Supply Air Flow Rate Method is **FractionOfAutosizedCoolingValue**.
-
-#### Field: No Load Fraction of Autosized Heating Supply Air Flow Rate
-
-This numeric field defines the fraction of autosized supply air flow rate leaving the unitary system when the neither cooling or heating coil is operating. Values must be greater than 0 or this field is autosizable. Required field when No Load Supply Air Flow Rate Method is **FractionOfAutosizedHeatingValue**.
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-#### Field: No Load Supply Air Flow Rate Per Unit of Capacity During Cooling Operation
-
-This numeric field defines the supply air flow rate per unit of capacity leaving the unitary system when neither cooling or heating is operating. Values must be greater than 0 or this field is autosizable. Required field when No Load Supply Air Flow Rate Method is **FlowPerCoolingCapacity**.
-
-#### Field: No Load Supply Air Flow Rate Per Unit of Capacity During Heating Operation
-
-This numeric field defines the supply air flow rate per unit of capacity leaving the unitary system when neither cooling or heating is operating. Values must be greater than 0 or this field is autosizable. Required field when No Load Supply Air Flow Rate Method is **FlowPerHeatingCapacity**.
-
-#### Field: Maximum Supply Air Temperature
-
-This numeric field contains the design operating air outlet temperature in degrees C when the unitary system is heating. If this input field is left blank, the default value is 80 C.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which the heat pump supplemental heating coil is disabled.  The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
-
-#### Field: Outdoor Dry-Bulb Temperature Sensor Node Name
-
-This alpha field specifies the name of the outdoor node which controls the operation of the supplemental heating coil. If this field is left blank, the outdoor temperature is based solely on the weather data. If this field is not blank, the node name specified must also be listed in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor temperature from the weather data. Alternately, the node name must be specified in an OutdoorAir:NodeList object where the outdoor temperature is taken directly from the weather data.
-
-#### Field: Maximum Cycling Rate
-
-This numeric field contains the maximum on-off cycling rate for the compressor, which occurs at 50% run time fraction. Suggested values are shown below (Henderson et al. 1999):
-
-![](media/image295.svg)
-
-#### Field: Heat Pump Time Constant
-
-This numeric field contains the time constant for the cooling coil's capacity to reach steady state after startup. Suggested values are shown below (Henderson et al. 1999):
-
-![](media/image296.svg)
-
-#### Field: Fraction of On-Cycle Power Use
-
-This numeric field contains the fraction of on-cycle power use to adjust the part load fraction based on the off-cycle power consumption due to crankcase heaters, controls, fans, and etc. Suggested value values are below (Henderson et al. 1999):
-
-![](media/image297.svg)
-
-#### Field: Heat Pump Fan Delay Time
-
-This numeric field contains the time delay for the heat pump supply air fan to shut off after the compressor cycles off in seconds. This value can be obtained from the manufacturer or the heat pump catalog. Enter a value of zero when the heat pump’s fan operating mode is continuous. Suggested value is 60 seconds.
-
-#### Field: Ancillary On-Cycle Electric Power
-
-This field defines ancillary electrical power (W) consumed during the on-cycle period (i.e., when the cooling or heating coil is operating). The model assumes that this ancillary power does not contribute to heating the supply air. The minimum value for this field is 0.0, and the default value is also 0.0 if the field is left blank.
-
-#### Field: Ancillary Off-Cycle Electric Power
-
-This field defines ancillary electrical power (W) consumed during the off-cycle period (i.e., when the cooling and heating coil are not operating). The model assumes that this ancillary power does not contribute to heating the supply air. The minimum value for this field is 0.0, and the default value is also 0.0 if the field is left blank.
-
-#### Field: Design Heat Recovery Water Flow Rate
-
-This optional input field defines the design water flow rate used if the heat recovery option is being simulated. If this value is greater than 0.0 then a heat recovery loop must be specified and attached to the multispeed heat pump using the next 2 node fields. To determine how the heat recovery algorithm works, refer to the EnergyPlus Engineering Reference in the AirLoopHVAC:UnitarySystem with Heat Recovery section. The units for this input value are cubic meters per second.
-
-#### Field: Maximum Temperature for Heat Recovery
-
-This field sets the maximum temperature (in degrees C) that this heat pump can produce for heat recovery. The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit. This temperature limit puts an upper bound on the recovered heat and limits the max temperature leaving the component.
-
-As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting. This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply.
-
-#### Field: Heat Recovery Water Inlet Node Name
-
-This alpha field contains the identifying name for the heat recovery side inlet node.
-
-#### Field: Heat Recovery Water Outlet Node Name
-
-This alpha field contains the identifying name for the heat recovery side outlet node.
-
-#### Field: Design Specification Multispeed Object Type
-
-This alpha field contains the identifying type for the design specification multispeed object. This field is only needed when multispeed cooling or heating coil is specified.
-
-#### Field: Design Specification Multispeed Object Name
-
-This alpha field contains the identifying name for the design specification multispeed object. This field is only needed when multispeed cooling or heating coil is specified.
-
-As shown in the example below, correct specification of the heat/cool unitary system requires specification of the following objects in addition to the unitary system object:
-
-1) Fan (Fan:OnOff or Fan:ConstantVolume)
-
-2) Cooling coil
-
-3) Heating coil
-
-4) Reheat coil
-
-5) Direct air unit (AirTerminal:SingleDuct:Uncontrolled) for each zone served by the unitary system
-
-```idf
-AirLoopHVAC:UnitarySystem,
-   DXAC Heat Pump 1,        !- Name
-   Load,                    !- Control Type
-   East Zone,               !- Controlling Zone or Thermostat Location
-   ,                        !- Dehumidification Control Type
-   FanAndCoilAvailSched,    !- Availability Schedule Name
-   Mixed Air Node,          !- Air Inlet Node Name
-   Air Loop Outlet Node,    !- Air Outlet Node Name
-   Fan:OnOff,               !- Supply Air Fan Object Type
-   Supply Fan 1,            !- Supply Air Fan Name
-   BlowThrough,             !- Fan Placement
-   FanModeSchedule,         !- Supply Air Fan Operating Mode Schedule Name
-   Coil:Heating:DX:MultiSpeed,  !- Heating Coil Object Type
-   Heat Pump DX Heating Coil 1, !- Heating Coil Name
-   ,                            !- DX Heating Coil Sizing Ratio
-   Coil:Cooling:DX:MultiSpeed,  !- Cooling Coil Object Type
-   Heat Pump ACDXCoil 1,    !- Cooling Coil Name
-   ,                        !- Use DOAS DX Cooling Coil
-   ,                        !- DOAS DX Cooling Coil Leaving Minimum Air Temperature
-   ,                        !- Latent Load Control
-   Coil:Heating:Gas,        !- Supplemental Heating Coil Object Type
-   Supp Gas Heating Coil 1, !- Supplemental Heating Coil Name
-   SupplyAirFlowRate,       !- Cooling Supply Air Flow Rate Method
-   1.7,                     !- Cooling Supply Air Flow Rate {m3/s}
-   ,                        !- Cooling Supply Air Flow Rate Per Floor Area
-   ,                        !- Cooling Fraction of Autosized Cooling Supply Air Flow Rate
-   ,                        !- Cooling Supply Air Flow Rate Per Unit of Cooling Capacity
-   SupplyAirFlowRate,       !- Heating Supply Air Flow Rate Method
-   1.7,                     !- Heating Supply Air Flow Rate {m3/s}
-   ,                        !- Heating Supply Air Flow Rate Per Floor Area
-   ,                        !- Heating Fraction of Autosized Heating Supply Air Flow Rate
-   ,                        !- Heating Supply Air Flow Rate Per Unit of Heating Capacity
-   SupplyAirFlowRate,       !- No Load Supply Air Flow Rate Method
-   0.2,                     !- No Load Supply Air Flow Rate {m3/s}
-   ,                        !- No Load Supply Air Flow Rate Per Floor Area
-   ,                        !- No Load Fraction of Autosized Cooling Supply Air Flow Rate
-   ,                        !- No Load Fraction of Autosized Heating Supply Air Flow Rate
-   ,                        !- No Load Supply Air Flow Rate Per Unit of Cooling Capacity
-   ,                        !- No Load Supply Air Flow Rate Per Unit of Heating Capacity
-   50,                      !- Maximum Supply Air Temperature {C}
-   21,  !- Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation
-   ,  !- Outdoor Dry-Bulb Temperature Sensor Node Name
-   ,  !- Maximum Cycling Rate
-   ,  !- Heat Pump Time Constant
-   ,  !- Fraction of On-Cycle Power Use
-   ,  !- Heat Pump Fan Delay Time
-   ,  !- Ancillary On-Cycle Electric Power
-   ,  !- Ancillary Off-Cycle Electric Power
-   ,  !- Design Heat Recovery Water Flow Rate
-   ,  !- Maximum Temperature for Heat Recovery (Maximum Heat Recovery Outlet Temperature?)
-   ,  !- Heat Recovery Water Inlet Node Name
-   ,  !- Heat Recovery Water Outlet Node Name
-   UnitarySystemPerformance:Multispeed,  !- Design Specification Multispeed Heat Pump Object Type
-   MyMultispeedHPSpec;  !- Design Specification Multispeed Heat Pump Object Name
-
-UnitarySystemPerformance:Multispeed,
-   MyMultispeedHPSpec,      !- Name
-   4,                       !- Number of Speeds for Heating
-   4,                       !- Number of Speeds for Cooling
-   No,                      !- Single Mode Operation
-   0.235294118,             !- Heating Speed 1 Supply Air Flow Rate {m3/s}
-   0.235294118,             !- Cooling Speed 1 Supply Air Flow Rate {m3/s}
-   0.470588235,             !- Heating Speed 2 Supply Air Flow Rate {m3/s}
-   0.470588235,             !- Cooling Speed 2 Supply Air Flow Rate {m3/s}
-   0.705882353,             !- Heating Speed 3 Supply Air Flow Rate {m3/s}
-   0.705882353,             !- Cooling Speed 3 Supply Air Flow Rate {m3/s}
-   1.0,                     !- Heating Speed 4 Supply Air Flow Rate {m3/s}
-   1.0;                     !- Cooling Speed 4 Supply Air Flow Rate {m3/s}
-```
-
-
-### Unitary System (AirLoopHVAC) Outputs
-
-* HVAC,Average, Unitary System Fan Part Load Ratio []
-
-* HVAC,Average, Unitary System Compressor Part Load Ratio
-
-* HVAC,Average,Unitary System Total Cooling Rate [W]
-
-* HVAC,Average,Unitary System Total Heating Rate [W]
-
-* HVAC,Average,Unitary System Sensible Cooling Rate [W]
-
-* HVAC,Average,Unitary System Sensible Heating Rate [W]
-
-* HVAC,Average,Unitary System Latent Cooling Rate [W]
-
-* HVAC,Average,Unitary System Latent Heating Rate [W]
-
-* HVAC,Average,Unitary System Ancillary Electric Power[W]
-
-Two speed coil outputs
-
-* HVAC,Average,Unitary System Cycling Ratio []
-
-Multi speed coil outputs
-
-* HVAC,Average,Unitary System DX Coil Cycling Ratio []
-
-* HVAC,Average,Unitary System DX Coil Speed Ratio []
-
-* HVAC,Average,Unitary System DX Coil Speed Level []
-
-* HVAC,Average,Unitary System Electric Power[W]
-
-* HVAC,Sum,Unitary System Electric Energy [J]
-
-* HVAC,Sum,Unitary System Cooling Ancillary Electric Energy [J]
-
-* HVAC,Sum,Unitary System Heating Ancillary Electric Energy [J]
-
-Multi speed coil outputs(If heat recovery is specified)
-
-* HVAC,Average, Unitary System Heat Recovery Rate [W]
-
-* HVAC,Average, Unitary System Heat Recovery Inlet Temperature [C]
-
-* HVAC,Average, Unitary System Heat Recovery Outlet Temperature [C]
-
-* HVAC,Average, Unitary System Heat Recovery Fluid Mass Flow Rate [kg/s]
-
-* HVAC,Sum, Unitary System Heat Recovery Energy [J]
-
-Water to air heat pump outputs
-
-* HVAC,Average, Unitary System Requested Sensible Cooling Rate [W]
-
-* HVAC,Average, Unitary System Requested Latent Cooling Rate [W]
-
-* HVAC,Average, Unitary System Requested Heating Rate [W]
-
-* HVAC,Average, Unitary System Water Coil Cycling Ratio []
-
-* HVAC,Average, Unitary System Water Coil Speed Ratio []
-
-* HVAC,Average, Unitary System Water Coil Speed Level []
-
-
-#### Unitary System Fan Part Load Ratio []
-
-This output variable is the ratio of actual air mass flow rate through the unitary system to the unitary system’s design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the unitary system is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating (or cooling) load to the steady-state unitary system heating (or cooling) capacity. For the cycling fan mode, the runtime fraction for the unitary system fan may be different from the fan part-load ratio reported here due the part-load performance of the unitary system’s heating (or cooling) coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff). When the speed number is greater than 1, the value is 1.0.
-
-#### Unitary System Compressor Part Load Ratio []
-
-This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the unitary system’s DX heating or cooling coil at Speed 1. The runtime fraction for the unitary system compressor may be different from the compressor part-load ratio reported here due the part-load performance of the heating/cooling coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate. When the speed number is greater than 1, the value is 1.0.
-
-#### Unitary System DX Coil Cycling Ratio []
-
-This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the unitary system’s DX heating or cooling coil (Speed 1) for the entire system timestep. The value is between 0.0 and 1.0 when the unitary system is cycling on and off its lowest speed (Speed 1) and 1.0 when the unitary system operates at speeds above 1.
-
-When Single Mode Operation is specified, the value is between 0.0 and 1.0 when the heat pump is cycling on at any given speed. 
-
-#### Unitary System DX Coil Speed Ratio []
-
-This output variable is the ratio of time in a system timestep that the compressor is at rated speed between two consecutive speed numbers ( [Compressor Speed - Compressor speed at Speed i-1] / [Compressor speed at Speed i - Compressor speed at Speed i-1]). The compressor speed ratio reports (1.0 is max, 0.0 is min) and any value in between as it is averaged over the timestep. The value is 0.0 during Speed 1 operation.
-
-The physical meaning of the speed ratio is dependent on the compressor configuration defined in the field of child coil object: Apply Part Load Fraction to Speeds greater than 1. The allowed choice is either Yes or No. When No is entered, one compressor is assumed for all speeds.  The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the lower speed runs in the rest of the system timestep. When Yes is entered, multiple compressors are assumed, and each compressor has associated speed. The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the low speed runs in a whole system timestep.
-
-When Single Mode Operation is specified, the speed ratio is set to 0 at Speed 1 and 1 at Speed > 1.
-
-#### Unitary System DX Coil Speed Level []
-
-This output variable reports the maximum speed needed when the unitary system operates to meet the sensible load (heating or cooling) in a system timestep. When the value is 1, the unitary system operates at Speed 1 (lowest speed). For this case the cycling ratio is between 0.0 and 1.0, while the speed ratio is 0.0. When the speed number output variable is above one, such as i, the unitary system operation is determined by the speed ratio through linear interpolation. For example, when the speed ratio is 0.4 and the speed number is 3, the unitary system operates at Speed 3 for 40% of a system timestep and at Speed 2 for 60% of a system timestep for a single compressor. For multiple compressors, the unitary system operates at Speed 3 in the 40% of a system timestep and at Speed 2 in the whole system timestep.
-
-#### Unitary System Total Heating Rate [W]
-
-This output field is the total (enthalpy) heat addition rate of the unitary system to the zones it is serving in Watts. This value is calculated using the enthalpy difference of the unitary system outlet air and inlet air streams, and the air mass flow rate through the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
-
-#### Unitary System Total Cooling Rate [W]
-
-This output field is the total (enthalpy) heat extraction rate of the unitary system from the zones it is serving in Watts. This value is calculated using the enthalpy difference of the unitary system outlet air and inlet air streams, and the air mass flow rate through the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
-
-#### Unitary System Sensible Heating Rate [W]
-
-This output field reports the sensible heat addition rate of the unitary system to the zones it is serving in Watts. This value is calculated using the enthalpy difference of the unitary system outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
-
-#### Unitary System Sensible Cooling Rate [W]
-
-This output field reports the moist air sensible heat extraction rate of the unitary system from the zones it is serving in Watts. This value is calculated using the enthalpy difference of the unitary system outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
-
-#### Unitary System Latent Heating Rate [W]
-
-This output field is the latent heat addition (humidification) rate of the unitary system in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
-
-#### Unitary System Latent Cooling Rate [W]
-
-This output field is the latent heat extraction (dehumidification) rate of the unitary system in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the unitary system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
-
-#### Unitary System Electric Power [W]
-
-This output field is the electricity consumption rate of the unitary system in Watts. The consumption includes electricity used by the DX coils (including crankcase heater if the fuel type is electricity), fans (indoor supply air fan and the condenser fans associated with the DX coil[s]), auxiliary power during on and off period, and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported. Any non-electric energy use is not reported by the unitary system object but is reported in the associated coil objects as appropriate.
-
-#### Unitary System Electric Energy [J]
-
-This output field is the electricity consumption of the unitary system in Joules for the timestep being reported. The consumption includes electricity used by the DX compressor (including crankcase heater if the fuel type is electricity), fans (indoor supply air fan and the condenser fans associated with the DX coil[s]), auxiliary power during on and off period, and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are summed for the timestep being reported. Any non-electric energy use is not reported by the unitary system object but is reported in the associated coil objects as appropriate.
-
-#### Unitary System Ancillary Electric Power [W]
-
-This output field is the average auxiliary electricity consumption rate (including both on-cycle and off-cycle) in Watts for the timestep being reported.
-
-#### Unitary System Cooling Ancillary Electric Energy [J]
-
-This is the auxiliary electricity consumption in Joules for the timestep being reported. This is the auxiliary electricity consumption during periods when the unitary system is providing cooling (DX cooling coil is operating). This output is also added to a meter with Resource Type = Electricity, End Use Key =Cooling, Group Key = System (ref. Output:Meter objects).
-
-#### Unitary System Heating Ancillary Electric Energy [J]
-
-This is the auxiliary electricity consumption in Joules for the timestep being reported. This is the auxiliary electricity consumption during periods when the unitary system is providing heating (DX heating coil is operating). This output is also added to a meter with Resource Type = Electricity, End Use Key =Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Unitary System Heat Recovery Inlet Temperature [C]
-
-#### Unitary System Heat Recovery Outlet Temperature [C]
-
-#### Unitary System Heat Recovery Fluid Mass Flow Rate [kg/s]
-
-These outputs are the heat recovery inlet and outlet temperatures and water mass flow rate for unitary systems with heat recovery.
-
-#### Unitary System Heat Recovery Rate [W]
-
-#### Unitary System Heat Recovery Energy [J]
-
-For multispeed unitary systems with heat recovery, these outputs are the recoverable energy rate (in Watts) and energy (in Joules).
-
-#### Unitary System Requested Sensible Cooling Rate [W]
-
-This output variable is the sensible cooling requested from the zone thermostat in watts. This value is calculated using the unitary system outlet air and zone conditions, the specific heat of the zone air, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Unitary System Requested Latent Cooling Rate [W]
-
-This output variable is the latent cooling requested from the zone humidistat in watts. This value is calculated using the unitary system outlet air and zone conditions, the heat of vaporization of water at the current zone conditions, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Unitary System Requested Heating Rate [W]
-
-This output variable is the sensible heating requested from the zone thermostat in watts. This value is calculated using the unitary system outlet air and zone conditions, the specific heat of the zone air, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Unitary System Water Coil Cycling Ratio []
-This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the multispeed fan chilled water or hot water coil for the entire system timestep. The value is between 0.0 and 1.0 when the AHU is cycling on and off its lowest speed (fan speed 1) and 1.0 when the multispeed fan chilled water or hot water AHU operates at speed levels above 1.
-
-#### Unitary System Water Coil Speed Ratio []
-This output variable is the ratio of time in a system timestep that the AHU fan is at rated speed between two consecutive speed levels ( [System Load – Capacity at Fan Speed i-1] / [Capacity at Fan Speed i – Capacity at Fan Speed i-1]). The fan speed ratio reports (1.0 is max, 0.0 is min) and any value in between as it is averaged over the timestep. The value is 0.0 during Speed 1 operation. AHU speed ratio depends on the system load and the supply air fan speed. The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the lower speed runs in the rest of the system timestep.
-
-#### Unitary System Water Coil Speed Level []
-This output variable reports the maximum speed needed when the system operates to meet the sensible load (heating or cooling) in a system timestep. When the value is 1, the AHU operates at Speed 1 (lowest speed). For this case the cycling ratio is between 0.0 and 1.0, while the speed ratio is 0.0. When the speed level is above the minimum (speed =1), the system operation is determined by the speed ratio. For example, when the speed ratio is 0.4 and the speed lever is 3, then the supply air fan and water coil operate at Speed 3 for 40% of a system timestep and at Speed 2 for 60% of a system timestep.
-
-### UnitarySystemPerformance:Multispeed
-
-#### Field: Name
-
-This alpha field contains the identifying name for the multispeed performance specification.
-
-#### Field: Number of Speeds for Heating
-
-This field defines the number of heating speeds for the heat pump, and must match the number of heating speeds defined in the associated heating coil. The value for this input field defines the number of airflow rate ratios that must be defined for heating in the fields below. The minimum value for this field is one and the maximum value is the number specified in the coil object. If the heating coil type used in the unitary system object is not a multispeed coil type, then this field should be 1.
-
-#### Field: Number of Speeds for Cooling
-
-This field defines the number of cooling speeds for the heat pump, and must match the number of cooling speeds defined in the associated DX cooling coil. The value for this input field defines the number of airflow rate ratios that must be defined for cooling in the fields below. The minimum value for this field is one and the maximum value is the number specified in the coil object. If the cooling coil type used in the unitary system object is not a multispeed coil type, then this field should be 1.
-
-#### Field: Single Mode Operation
-
-This field specifies the coil operation mode for multiple speed DX cooling and heating coils during each HVAC timestep. The allowed choice is Yes or No. The No choice allows a coil works between two adjacent speeds when a system load is greater than the coil capacity at speed 1. The Yes choice allows a coil works with a single capacity at a different speed. The speed number is determined by a system load.  
-
-#### Field: Heating Speed 1 Supply Air Flow Ratio
-
-This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the heating coil and/or supplemental heater are operating at Speed 1 (lowest speed). Values must be greater than 0.
-
-#### Field: Cooling Speed 1 Supply Air Flow Ratio
-
-This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the DX cooling coil is operating at Speed 1 (lowest speed). Values must be greater than 0.
-
-#### Field: Heating Speed 2 Supply Air Flow Ratio
-
-This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the heating coil and/or supplemental heater are operating at Speed 2. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for heating speed 1.
-
-#### Field: Cooling Speed 2 Supply Air Flow Ratio
-
-This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the DX cooling coil is operating at Speed 2. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for cooling speed 1.
-
-#### Field: Heating Speed 3 Supply Air Flow Ratio
-
-This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the heating coil and/or supplemental heater are operating at Speed 3. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for heating speed 2.If the ‘Number of Speeds for Heating’ is less than 3, then this field can be left blank.
-
-#### Field: Cooling Speed 3 Supply Air Flow Ratio
-
-This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the DX cooling coil is operating at Speed 3. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for cooling speed 2.If the ‘Number of Speeds for Cooling’ is less than 3, then this field can be left blank.
-
-#### Field: Heating Speed 4 Supply Air Flow Ratio
-
-This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the DX heating coil and/or supplemental heater are operating at Speed 3. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for heating Speed 3.If the ‘Number of Speeds for Heating’ is less than 4, then this field can be left blank.
-
-#### Field: Cooling Speed 4 Supply Air Flow Ratio
-
-This numeric field defines the ratio of supply air flow rate leaving the unitary system to the maximum air flow rate specified in the coil object at maximum speed when the DX cooling coil is operating at Speed 4. Values must be greater than 0. The entered value must be greater or equal to the flow rate ratio specified for cooling Speed 3.If the ‘Number of Speeds for Cooling’ is less than 4, then this field can be left blank.
-
-### AirLoopHVAC:Unitary:Furnace:HeatCool
-
-The heat/cool furnace is a “virtual� component that consists of a fan component (OnOff or ConstantVolume), a DX cooling coil component, and a Gas or Electric heating coil component. The blow through furnace configuration is shown in Figure 116 below. When a draw through furnace configuration is desired, the fan is placed directly after the heating coil. If the dehumidification control type is specified as CoolReheat, a reheat coil component is also required. If the reheat coil is present and the dehumidification control type input is not specified as CoolReheat, the reheat coil will not be active,
-
-![FurnaceSchematic\_BlowThru](media/image298.png)
-
-Figure 116. Schematic of EnergyPlus Heat/Cool Furnace
-
-Note: the coil order shown here has been revised from previous versions (prior to V4.0) of Energyplus to configure the cooling coil upstream of the heating coil. This configuration provides uniformity with all unitary equipment. However, for unitary HeatCool systems that do not use a reheat coil, the heating coil can also be placed upstream of the cooling coil. This optional coil placement is retained to allow compatibility with previous versions of Energyplus. For input files developed using previous versions of Energyplus, it is recommended that the coil order be revised according to the figure above.
-
-Links to the fan, heating coil, DX cooling coil and optional reheat coil specifications are provided in the furnace input data syntax. In addition, the control zone name and the furnace design operating conditions are specified by the furnace inputs.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the unit.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name which contains information on the availability of the furnace to operate. A schedule value equal to 0 denotes that the furnace must be off for that time period. A value greater than 0 denotes that the furnace is available to operate during that time period. This schedule may be used to completely disable the furnace as required. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Furnace Air Inlet Node Name
-
-This alpha field contains the furnace inlet node name.
-
-#### Field: Furnace Air Outlet Node Name
-
-This alpha field contains the furnace outlet node name.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the furnace supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.
-
-#### Field: Maximum Supply Air Temperature
-
-This numeric field contains the design operating furnace air outlet temperature in degrees C when the furnace is heating. If this input field is left blank, the default value is 80 C.
-
-#### Field: Cooling Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the furnace in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the furnace in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: No Load Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the furnace in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the furnace operating mode is specified as continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the furnace operating mode is specified as continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the compressor was last operating (for cooling operation or heating operation).
-
-#### Field: Controlling Zone or Thermostat Location
-
-This alpha field contains the identifying zone name where the thermostat controlling the furnace is located.
-
-#### Field: Supply Fan Object Type
-
-This alpha field contains the identifying type of supply air fan specified for the furnace. Fan type must be **Fan:OnOff** or **Fan:ConstantVolume**. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e. Supply Air Fan Operating Mode Schedule values are at times 0).
-
-#### Field: Supply Fan Name
-
-This alpha field contains the identifying name given to the furnace fan.
-
-#### Field: Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. The first choice stands for “blow through fan�. This means that the unit consists of a fan followed by the DX coils and supplemental heating coil. The fan “blows through� the cooling and heating coils. The second choice stands for “draw through fan�. This means that the unit consists of the DX coil(s) followed by a fan, with the supplemental heater located at the outlet of the fan. The fan “draws air through� the DX coil(s). If this field is left blank, the default is blow through.
-
-#### Field: Heating Coil Object Type
-
-This alpha field contains the identifying type of heating coil specified in the furnace. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat and Cool Furnace) itself provides the "controller" function of modulating water flow. Allowable coil types are:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Heating Coil Name
-
-This alpha field contains the identifying name given to the furnace heating coil.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field contains the identifying type of cooling coil specified in the furnace. Only allowable coil types are:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* CoilSystem:Cooling:DX:HeatExchangerAssisted
-
-* Coil:Cooling:DX:VariableSpeed
-
-#### Field: Cooling Coil Name
-
-This alpha field contains the identifying name given to the furnace cooling coil.
-
-#### Field: Dehumidification Control Type
-
-This alpha field contains the type of dehumidification control. The following options are valid for this field:
-
-* **None** - meet sensible load only, no active dehumidification control
-
-* **Multimode** - activate enhanced dehumidification mode as needed and meet sensible load. This option is used to model DX equipment with a controllable heat exchanger assisting the DX cooling coil for improved dehumidification. It is valid only with cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted.
-
-* **CoolReheat** - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. If cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted, then the heat exchanger is assumed to always transfer energy between the cooling coil’s inlet and outlet airstreams when the cooling coil is operating.
-
-The default is **None**. For the other dehumidification control modes, the maximum humidity setpoint is used. This must be set using a **ZoneControl:Humidistat** object. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate. If the dehumidification control type is specified as **CoolReheat**, then two additional inputs (reheat coil type and name) are also required as shown below. Although the reheat coil is required only when **CoolRheat** is selected, the optional reheat coil may be present for any of the allowed Dehumidification Control Types. If the reheat coil is present and the dehumidification control type is not specified as **CoolReheat**, the reheat coil will not be active,
-
-#### Field: Reheat Coil Object Type
-
-This alpha field contains the identifying type of reheat coil specified in the furnace. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the reheat coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat and Cool Furnace) itself provides the "controller" function of modulating water flow. Reheat coil type must be one of:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Desuperheater
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Reheat Coil Name
-
-This alpha field contains the identifying name given to the furnace reheat coil.
-
-As shown in the example below, correct specification of the heat/cool furnace requires specification of the following objects in addition to the furnace object:
-
-1) fan (Fan:OnOff or Fan:ConstantVolume)
-
-2) cooling coil (Coil:Cooling:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted)
-
-3) heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
-
-4) reheat coil (optional, Coil:Heating:Gas, Coil:Heating:Electric, or Coil:Heating:Desuperheater)
-
-5) terminal unit (AirTerminal:SingleDuct:Uncontrolled) for each zone served by the furnace
-
-Note: the furnace's fan, cooling coil, heating coil and optional reheat coil must be connected in the air loop according to the configuration shown above (Figure 116) when CoolReheat is selected as the dehujmidificaiton control type. In addition, the volumetric air flow rate specified in the terminal air unit for the controlling zone should properly reflect the fractional volumetric air flow rate specified in the furnace object.
-
-```idf
-AirLoopHVAC:Unitary:Furnace:HeatCool,
-    GasHeat DXAC Furnace 1, !- Name of furnace
-    FanAndCoilAvailSched,   !- Availability schedule
-    Air Loop Inlet Node,    !- Furnace inlet node name
-    Air Loop Outlet Node,   !- Furnace outlet node name
-    CycFanSchedule,         !- Supply Air Fan Operating Mode Schedule Name
-    80,                     !- Maximum supply air temperature from furnace heater {C}
-    1.3,                    !- Cooling Supply Air Flow Rate {m3/s}
-    1.3,                    !- Heating Supply Air Flow Rate {m3/s}
-    0.0,                    !- No Load Supply Air Flow Rate {m3/s}
-    East Zone,              !- Controlling zone or thermostat location
-    Fan:OnOff,              !- Supply fan type
-    Supply Fan 1,           !- Supply fan name
-    BlowThrough,            !- Fan Placement
-    Coil:Heating:Gas,       !- Heating coil type
-    Furnace Heating Coil 1, !- Heating coil name
-    Coil:Cooling:DX:SingleSpeed,  !- Cooling coil type
-    Furnace ACDXCoil 1,     !- Cooling coil name
-    None;                   !- Dehumidificatioin Control Type
-
-
-Coil:Heating:Gas,
-    Furnace Heating Coil 1,         !- Coil Name
-    FanAndCoilAvailSched,           !- Availability Schedule Name
-    0.8,    !- Gas Burner Efficiency of the Coil
-    25000,  !- Nominal Capacity of the Coil {W}
-    Heating Coil Air Inlet Node,    !- Coil\_Air\_Inlet\_Node
-    Air Loop Outlet Node;           !- Coil\_Air\_Outlet\_Node
-
-  Coil:Cooling:DX:SingleSpeed,
-    Furnace ACDXCoil 1,    !- Coil Name
-    FanAndCoilAvailSched,  !- Availability Schedule
-    25000,  !- Rated Total Cooling Capacity (gross) {W}
-    0.75,   !- Rated SHR
-    3.0,    !- Rated COP
-    1.3,    !- Rated Air Volume Flow Rate {m3/s}
-    DX Cooling Coil Air Inlet Node, !- Coil Air Inlet Node
-    Heating Coil Air Inlet Node,    !- Coil Air Outlet Node
-    WindACCoolCapFT,  !- Total Cooling Capacity Modifier Curve (function of temperature)
-    WindACCoolCapFFF, !- Total Cooling Capacity Modifier Curve (function of flow fraction)
-    WindACEIRFT,      !- Energy Input Ratio Modifier Curve (function of temperature)
-    WindACEIRFFF,     !- Energy Input Ratio Modifier Curve (function of flow fraction)
-    WindACPLFFPLR,    !- Part Load Fraction Correlation (function of part load ratio)
-    CyclingFanAndCompressor;    !- Supply Air Fan Operation Mode
-
-  Fan:OnOff,
-    Supply Fan 1,                !- Fan Name
-    FanAndCoilAvailSched,        !- Availability Schedule Name
-    0.7,    !- Fan Total Efficiency
-    600.0,  !- Delta Pressure {Pa}
-    1.3,    !- Max Flow Rate {m3/s}
-    0.9,    !- Motor Efficiency
-    1.0,    !- Motor In Airstream Fraction
-    Air Loop Inlet Node,         !- Fan\_Inlet\_Node
-    DX Cooling Coil Air Inlet Node; !- Fan\_Outlet\_Node
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone1DirectAir,        !- Direct Air Name
-    FanAndCoilAvailSched,  !- Schedule name for on/off schedule
-    Zone 1 Inlet Node,     !- Zone Supply Air Node Name
-    0.47;  !- Maximum air flow rate {m3/s}
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone2DirectAir,        !- Direct Air Name
-    FanAndCoilAvailSched,  !- Schedule name for on/off schedule
-    Zone 2 Inlet Node,     !- Zone Supply Air Node Name
-    0.36;  !- Maximum air flow rate {m3/s}
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone3DirectAir,        !- Direct Air Name
-    FanAndCoilAvailSched,  !- Schedule name for on/off schedule
-    Zone 3 Inlet Node,     !- Zone Supply Air Node Name
-    0.47;  !- Maximum air flow rate {m3/s}
-```
-
- Example of Heat/Cool Furnace Specification
-
-### Unitary System/Furnace Heat and Cool (AirLoopHVAC) Outputs
-
-HVAC,Average,Unitary System Fan Part Load Ratio []
-
-HVAC,Average,Unitary System Compressor Part Load Ratio []
-
-#### Unitary System Fan Part Load Ratio
-
-This output variable is the ratio of actual air mass flow rate through the furnace to the furnace’s design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the furnace is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating (or cooling) load to the steady-state furnace heating (or cooling) capacity. For the cycling fan mode, the runtime fraction for the furnace fan may be different from the fan part-load ratio reported here due the part-load performance of the furnace’s heating (or cooling) coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff).
-
-Unitary System Compressor Part Load Ratio []
-
-###  AirLoopHVAC:UnitaryHeatCool
-
-The AirLoopHVAC:UnitaryHeatCool object is the identical model to the AirLoopHAVC:Unitary:Furnace:HeatCool object. The heat/cool unitary system is a “virtual� component that consists of a fan component (OnOff or ConstantVolume), a DX cooling coil component and a Gas or Electric heating coil component as shown in Figure 117. When a draw through configuration is desired, the fan is placed directly after the heating coil. If dehumidification control is selected, a reheat coil component is also required. If the reheat coil is present and the dehumidification control type input is not specified as CoolReheat, the reheat coil will not be active,
-
-![FurnaceSchematic\_Unitary\_BlowThru](media/image299.png)
-
-Figure 117. Schematic of Blow Through Heat/Cool Unitary System
-
-Note: the coil order shown here has been revised from previous versions (prior to V4.0) of Energyplus to configure the cooling coil upstream of the heating coil. This configuration provides uniformity with all unitary equipment. However, for unitary HeatCool systems that do not use a reheat coil, the heating coil can also be placed upstream of the cooling coil. This optional coil placement is retained to allow compatibility with previous versions of Energyplus. For input files developed using previous versions of Energyplus, it is recommended that the coil order be revised according to the figure above.
-
-Links to the fan, DX cooling coil, heating coil and optional reheat coil specifications are provided in the unitary system input data syntax. In addition, the control zone name and the system design operating conditions are specified by the unitary system inputs.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the unitary system.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name which contains information on the availability of the unitary system to operate. A schedule value equal to 0 denotes that the unitary system must be off for that time period. A value greater than 0 denotes that the unitary system is available to operate during that time period. This schedule may be used to completely disable the unitary system as required. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Unitary System Air Inlet Node Name
-
-This alpha field contains the unitary system inlet node name.
-
-#### Field: Unitary System Air Outlet Node Name
-
-This alpha field contains the unitary system outlet node name.
-
-***Field: Supply Air Fan Operating Mode Schedule Name***
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the unitary system supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.
-
-#### Field: Maximum Supply Air Temperature
-
-This numeric field contains the design operating air outlet temperature in degrees C when the unitary system is heating. If this input field is left blank, the default value is 80 C.
-
-#### Field: Cooling Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: No Load Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the unitary system in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the unitary system operating mode is specified as continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the unitary system operating mode is specified as continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the compressor was last operating (for cooling operation or heating operation).
-
-#### Field: Controlling Zone or Thermostat Location
-
-This alpha field contains the identifying zone name where the thermostat controlling the unitary system is located.
-
-#### Field: Supply Fan Object Type
-
-This alpha field contains the identifying type of supply air fan specified for the unitary system. Fan type must be **Fan:OnOff** or **Fan:ConstantVolume**. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e. Supply Air Fan Operating Mode Schedule values are at times 0).
-
-#### Field: Supply Fan Name
-
-This alpha field contains the identifying name given to the unitary system fan.
-
-#### Field: Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. The first choice stands for “blow through fan�. This means that the unit consists of a fan followed by the DX coils and supplemental heating coil. The fan “blows through� the cooling and heating coils. The second choice stands for “draw through fan�. This means that the unit consists of the DX coil(s) followed by a fan, with the supplemental heater located at the outlet of the fan. The fan “draws air through� the DX coil(s). If this field is left blank, the default is blow through.
-
-#### Field: Heating Coil Object Type
-
-This alpha field contains the identifying type of heating coil specified in the unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat and Cool System) itself provides the "controller" function of modulating water flow. Allowable coil types are:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Heating Coil Name
-
-This alpha field contains the identifying name given to the unitary system heating coil.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field contains the identifying type of cooling coil specified in the unitary system. Only allowable coil types are:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* CoilSystem:Cooling:DX:HeatExchangerAssisted
-
-* Coil:Cooling:DX:VariableSpeed
-
-#### Field: Cooling Coil Name
-
-This alpha field contains the identifying name given to the unitary system cooling coil.
-
-#### Field: Dehumidification Control Type
-
-This alpha field contains the type of dehumidification control. The following options are valid for this field:
-
-* **None** - meet sensible load only, no active dehumidification control
-
-* **Multimode** - activate enhanced dehumidification mode as needed and meet sensible load. This option is used to model DX equipment with a controllable heat exchanger assisting the DX cooling coil for improved dehumidification. It is valid only with cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted.
-
-* **CoolReheat** - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. If cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted, then the heat exchanger is assumed to always transfer energy between the cooling coil’s inlet and outlet airstreams when the cooling coil is operating.
-
-The default is **None**. For the other dehumidification control modes, the maximum humidity setpoint is used. This must be set using a **ZoneControl:Humidistat** object. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate. If the dehumidification control type is specified as **CoolReheat**, then two additional inputs (reheat coil type and name) are also required as shown below. Although the reheat coil is required only when **CoolReheat** is selected, the optional reheat coil may be present for any of the allowed Dehumidification Control Types. If the reheat coil is present and the dehumidification control type is not specified as **CoolReheat**, the reheat coil will not be active,
-
-#### Field: Reheat Coil Object Type
-
-This alpha field contains the identifying type of reheat coil specified in the unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the reheat coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat and Cool System) itself provides the "controller" function of modulating water flow. Reheat coil type must be one of:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Desuperheater
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Reheat Coil Name
-
-This alpha field contains the identifying name given to the unitary system reheat coil.
-
-As shown in the example below, correct specification of the heat/cool unitary system requires specification of the following objects in addition to the unitary system object:
-
-1)   Fan (Fan:OnOff or Fan:ConstantVolume)
-
-2)   Cooling coil (Coil:Cooling:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted)
-
-3)   Heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
-
-4)   Reheat coil (optional, Coil:Heating:Gas, Coil:Heating:Electric, or Coil:Heating:Desuperheater)
-
-5)   Direct air unit (AirTerminal:SingleDuct:Uncontrolled) for each zone served by the unitary system
-
-Note: the unitary system’s fan, cooling coil, heating coil and optional reheat coil must be connected in the air loop according to the configuration shown above (Figure 117). In addition, the volumetric air flow rate specified in the direct air unit for the controlling zone should properly reflect the fractional volumetric air flow rate specified in the unitary system object.
-
-
-```idf
-AirLoopHVAC:Unitary:Furnace:HeatCool,
-    GasHeat DXAC Unitary System 1, !- Name of unitary system
-    FanAndCoilAvailSched,   !- Availability schedule
-    Air Loop Inlet Node,    !- Unitary system inlet node name
-    Air Loop Outlet Node,   !- Unitary system outlet node name
-    CycFanSchedule,         !- Supply Air Fan Operating Mode Schedule Name
-    80,                     !- Maximum supply air temperature from unitary system heater {C}
-    1.3,                    !- Cooling Supply Air Flow Rate {m3/s}
-    1.3,                    !- Heating Supply Air Flow Rate {m3/s}
-    0.0,                    !- No Load Supply Air Flow Rate {m3/s}
-    East Zone,              !- Controlling zone or thermostat location
-    Fan:OnOff,              !- Supply fan type
-    Supply Fan 1,           !- Supply fan name
-    BlowThrough,            !- Fan Placement
-    Coil:Heating:Gas,       !- Heating coil type
-    Unitary System Heating Coil 1,   !- Heating coil name
-    Coil:Cooling:DX:SingleSpeed,  !- Cooling coil type
-    Unitary System ACDXCoil 1,       !- Cooling coil name
-    None;        !- High humidity control
-
-  Coil:Heating:Gas,
-    Unitary System Heating Coil 1,  !- Coil Name
-    FanAndCoilAvailSched,           !- Availability Schedule Name
-    0.8,    !- Gas Burner Efficiency of the Coil
-    25000,  !- Nominal Capacity of the Coil {W}
-    Heating Coil Air Inlet Node,    !- Coil\_Air\_Inlet\_Node
-    Air Loop Outlet Node;           !- Coil\_Air\_Outlet\_Node
-
-
-  Coil:Cooling:DX:SingleSpeed,
-    Unitary System ACDXCoil 1,      !- Coil Name
-    FanAndCoilAvailSched,  !- Availability Schedule
-    25000,  !- Rated Total Cooling Capacity (gross) {W}
-    0.75,   !- Rated SHR
-    3.0,    !- Rated COP
-    1.3,    !- Rated Air Volume Flow Rate {m3/s}
-    DX Cooling Coil Air Inlet Node, !- Coil Air Inlet Node
-    Heating Coil Air Inlet Node,    !- Coil Air Outlet Node
-    WindACCoolCapFT,  !- Total Cooling Capacity Modifier Curve (function of temperature)
-    WindACCoolCapFFF, !- Total Cooling Capacity Modifier Curve (function of flow fraction)
-    WindACEIRFT,      !- Energy Input Ratio Modifier Curve (function of temperature)
-    WindACEIRFFF,     !- Energy Input Ratio Modifier Curve (function of flow fraction)
-    WindACPLFFPLR,    !- Part Load Fraction Correlation (function of part load ratio)
-    CyclingFanAndCompressor;    !- Supply Air Fan Operation Mode
-
-
-  Fan:OnOff,
-    Supply Fan 1,                !- Fan Name
-    FanAndCoilAvailSched,        !- Availability Schedule Name
-    0.7,    !- Fan Total Efficiency
-    600.0,  !- Delta Pressure {Pa}
-    1.3,    !- Max Flow Rate {m3/s}
-    0.9,    !- Motor Efficiency
-    1.0,    !- Motor In Airstream Fraction
-    Air Loop Inlet Node,         !- Fan\_Inlet\_Node
-    DX Cooling Coil Air Inlet Node; !- Fan\_Outlet\_Node
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone1DirectAir,        !- Direct Air Name
-    FanAndCoilAvailSched,  !- Schedule name for on/off schedule
-    Zone 1 Inlet Node,     !- Zone Supply Air Node Name
-   0.47;  !- Maximum air flow rate {m3/s}
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone2DirectAir,        !- Direct Air Name
-    FanAndCoilAvailSched,  !- Schedule name for on/off schedule
-    Zone 2 Inlet Node,     !- Zone Supply Air Node Name
-   0.36;  !- Maximum air flow rate {m3/s}
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone3DirectAir,        !- Direct Air Name
-    FanAndCoilAvailSched,  !- Schedule name for on/off schedule
-    Zone 3 Inlet Node,     !- Zone Supply Air Node Name
-   0.47;  !- Maximum air flow rate {m3/s}
-```
-
-
-Example of Heat/Cool Unitary System Specification
-
-### Unitary System Heat and Cool (AirLoopHVAC) Outputs
-
-* HVAC,Average, Unitary System Fan Part Load Ratio []
-
-* HVAC,Average, Unitary System Compressor Part Load Ratio
-
-#### Unitary System Fan Part Load Ratio []
-
-This output variable is the ratio of actual air mass flow rate through the unitary system to the system’s design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the unitary system is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating (or cooling) load to the steady-state unitary system heating (or cooling) capacity. For the cycling fan mode, the runtime fraction for the unitary system fan may be different from the fan part-load ratio reported here due the part-load performance of the system’s heating (or cooling) coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff).
-
-#### Unitary System Compressor Part Load Ratio []
-
-This output variable is the ratio of the sensible cooling load to the steady-state cooling capacity of the unitary system’s DX cooling coil. The runtime fraction for the DX cooling coil compressor may be different from the compressor part-load ratio reported here due the part-load performance of the cooling coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
-
-### AirLoopHVAC:UnitaryHeatPump:AirToAir
-
-The unitary air-to-air heat pump is a “virtual� component that consists of a fan component (OnOff or ConstantVolume), a DX cooling coil component, a DX heating coil component, and a Gas or Electric supplementary heating coil component as shown in the Figure below.
-
- ![FurnaceSchematic\_HeatPump](media/image300.png)
-
-Figure 118. Schematic of EnergyPlus Unitary Air-to-Air Heat Pump (Blow Through Configuration)
-
-Links to the fan, DX cooling coil, DX heating coil, and supplementary heating coil specifications are provided in the heat pump’s input data syntax. In addition the control zone name and the system design operating conditions are specified by the heat pump inputs.
-
-####  Field: Name
-
-This alpha field contains the identifying name for the unitary system heat pump.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name (ref. Schedule objects) that contains information on the availability of the heat pump to operate. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the hour. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the hour. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the  name of the HVAC system node from which the heat pump draws its inlet air.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the  name of the HVAC system node to which the heat pump sends its outlet air.
-
-#### Field: Cooling Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating. Values must be greater than 0 or this field is autosizable.
-
-#### Field: No Load Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when neither cooling or heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the heat pump operating mode is specified as continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the heat pump operating mode is specified as continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the compressor was last operating (for cooling operation or heating operation).
-
-#### Field: Controlling Zone or Thermostat Location
-
-This alpha field contains the identifying zone name where the thermostat controlling the heat pump is located.
-
-#### Field: Supply Air Fan Object Type
-
-This alpha field contains the identifying type of supply air fan specified for the heat pump. Fan type must be **Fan:OnOff** or **Fan:ConstantVolume**. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e. Supply Air Fan Operating Mode Schedule values are at times 0).
-
-#### Field: Supply Air Fan Name
-
-This alpha field contains the identifying name given to the heat pump supply air fan, and should match the name specified in the corresponding fan object.
-
-#### Field: Heating Coil Object Type
-
-This alpha field contains the identifying type of heating coil specified in the heat pump. Heating coil type must be either Coil:Heating:DX:SingleSpeed or Coil:Heating:DX:VariableSpeed.
-
-#### Field: Heating Coil Name
-
-This alpha field contains the identifying name given to the heat pump DX heating coil, and should match the name specified in the corresponding DX heating coil object.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field contains the identifying type of cooling coil specified in the heat pump. There are three valid choices for this field:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* CoilSystem:Cooling:DX:HeatExchangerAssisted
-
-* Coil:Cooling:DX:VariableSpeed
-
-#### Field: Cooling Coil Name
-
-This alpha field contains the identifying name given to the heat pump cooling coil, and should match the name specified in the corresponding DX cooling coil object.
-
-#### Field: Supplemental Heating Coil Object Type
-
-This alpha field contains the identifying type of supplemental heating coil specified in the heat pump. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the supplemental heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Airloop Air to Air Heat Pump) itself provides the "controller" function of modulating water flow. Heating coil type must be:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Supplemental Heating Coil Name
-
-This alpha field contains the identifying name given to the heat pump supplemental heating coil, and should match the name specified in the corresponding heating coil object.
-
-#### Field: Maximum Supply Air Temperature from Supplemental Heater
-
-This numeric field defines the maximum allowed supply air temperature exiting the heat pump supplemental heating coil.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which the heat pump supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
-
-#### Field: Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. The first choice represents a blow through system where the supply air fan is before the DX cooling/heating coil and the supplementary heating coil. The second choice represents a draw through system where the supply air fan is between the DX cooling/heating coil and the supplementary heating coil. If this input field is left blank, the default is blow through.
-
-***Field: Supply Air Fan Operating Mode Schedule Name***
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the unitary system supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.
-
-As shown in the example below, correct specification of the air-to-air heat pump requires specification of the following objects in addition to the heat pump object:
-
-1)   Fan (Fan:OnOff or Fan:ConstantVolume)
-
-2)   Heating coil (Coil:Heating:DX:SingleSpeed)
-
-3)   Cooling coil (Coil:Cooling:DX:SingleSpeed or CoilSystem:Cooling:DX:HeatExchangerAssisted)
-
-4)   Supplemental heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
-
-5)   Direct air unit (AirTerminal:SingleDuct:Uncontrolled)for each zone served by the unitary system
-
-#### Field: Dehumidification Control Type
-
-This alpha input field contains the type of dehumidification control. The following options are valid for this field:
-
-* **None** - meet sensible load only, no active dehumidification control
-
-* **Multimode** - activate enhanced dehumidification mode as needed and meet sensible cooling load. This option is used to model DX equipment with a controllable heat exchanger assisting the DX cooling coil for improved dehumidification. It is valid only with cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted.
-
-* **CoolReheat** - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. The excess cooling beyond the cooling set point temperature is offset by the supplemental heating coil. If cooling coil type = CoilSystem:Cooling:DX:HeatExchangerAssisted, then the heat exchanger is assumed to always transfer energy between the cooling coil’s inlet and outlet airstreams when the cooling coil is operating.
-
-The default is **None**. For the other dehumidification control modes, the maximum humidity setpoint is required. This must be set using a **ZoneControl:Humidistat** object. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate. Supplemental heating coil (supplemental heating coil type and name) is a required input in AirToAir HeatPumps. The supplemental heating coil capacity must be adequate enough to meet the heating coil load and offset the excess cooling load due to extra dehumidification required to meet the high relative humidity setpoint.
-
-Note: the air-to-air heat pump’s fan, cooling coil, heating coil and supplementary heating coil must be connected in the air loop according to the configuration shown above (Figure 118) for the blow-through fan configuration. The only other valid configuration is with a draw-through fan placement, where the fan is located between the DX heating coil and the supplementary heating coil.
-
-#### AirLoopHVAC:UnitaryHeatPump:AirToAir Example Specification
-
-```idf
-AirLoopHVAC:UnitaryHeatPump:AirToAir,
-      DXAC Heat Pump 1,            ! Heat Pump name
-      FanAndCoilAvailSched,        ! Heat Pump availability schedule
-      Mixed Air Node,              ! Heat Pump air inlet  node
-      Air Loop Outlet Node,        ! Heat Pump air outlet  node
-      1.3,                  !- Cooling Supply Air Flow Rate {m3/s}
-      1.3,                  !- Heating Supply Air Flow Rate {m3/s}
-      0.0,                  !- No Load Suuply Air Flow Rate {m3/s}
-      East Zone,                   ! Controlling zone or thermostat location
-      Fan:OnOff,            ! Supply air fan type
-      Supply Fan 1,                ! Supply air fan name –- same name used in fan object
-      Coil:Heating:DX:SingleSpeed,    ! Heating coil type
-      Heat Pump DX Heating Coil 1, ! Heating coil name –- same name used in DX heating coil object
-      Coil:Cooling:DX:SingleSpeed, !  Cooling coil type
-      Heat Pump ACDXCoil 1,        ! Cooling coil name –- same name used in DX cooling coil object
-      Coil:Heating:Gas,            ! Supplemental heating coil type
-      Heat Pump DX Supp Heating Coil 1, ! Supplemental heating coil name–- same as in heating coil object
-      50,                          ! Maximum supply air temperature from supplemental heater [C]
-      21,                      ! Maximum outdoor dry-bulb temp for supplemental heating coil operation [C]
-      BlowThrough,                ! Fan  placement
-      CycFanSchedule,              ! Supply air fan operating mode schedule name
-      CoolReheat;                  !- Dehumidification Control Type
-
-   Coil:Heating:DX:SingleSpeed,
-      Heat Pump DX Heating Coil 1,     ! Name of heating coil
-      FanAndCoilAvailSched,            ! Heating coil schedule
-      35000,                           ! Rated total heating capacity [W] (at 21.11C/8.33C)
-      2.75,                            ! Rated heating COP
-      1.7,                             ! Rated air flow rate [m3/s]
-      Heating Coil Air Inlet Node,     ! Coil air inlet node
-      SuppHeating Coil Air Inlet Node, ! Coil air outlet node
-      HPACHeatCapFT,                   ! Heating capacity modifier curve (temperature,C)
-      HPACHeatCapFFF,                  ! Heating capacity modifier curve (flow fraction)
-      HPACHeatEIRFT,                   ! Energy input ratio modifier curve (temperature,C)
-      HPACHeatEIRFFF,                  ! Energy input ratio modifier curve (flow fraction)
-      HPACCoolPLFFPLR,                 ! Part load fraction modifier curve (function of part-load ratio)
-      ,                         ! defrost EIR modifier curve (temp, C) not required for resistive defrost
-      CyclingFanAndCompressor,                   ! Operation mode (cycling fan, cycling compressor)
-      -5.0,                            ! Minimum OAT for heat pump compressor operation [C]
-      5.0,                             ! Maximum outdoor dry-bulb temp for defrost operation [C]
-      200.0,                           ! Crankcase heater capacity[W]
-      10.0,                            ! Maximum OAT for crankcase heater operation [C]
-      resistive,                       ! Defrost strategy (resistive or reverse-cycle)
-      timed,                           ! Defrost control (timed or on-demand)
-      0.166667,                        !Defrost time period fraction (used for timed defrost control only)
-      20000;                           ! Resistive defrost heater capacity [W]
-
-   Coil:Cooling:DX:SingleSpeed,
-      Heat Pump ACDXCoil 1,            ! Name of cooling coil
-      FanAndCoilAvailSched,            ! Availability schedule
-      32000,                           ! Rated total cooling capacity [W]
-      0.75,                            ! Rated sensible heat ratio
-      3.0,                             ! Rated COP
-      1.7,                             ! Rated air flow rate [m3/s]
-      DX Cooling Coil Air Inlet Node,  ! Coil air inlet node
-      Heating Coil Air Inlet Node,     ! Coil air outlet node
-      HPACCoolCapFT,                   ! Cooling capacity modifier curve (temperature,C)
-      HPACCoolCapFFF,                  ! Cooling capacity modifier curve (flow fraction)
-      HPACCoolEIRFT,                   ! Energy input ratio modifier curve (temperature,C)
-      HPACCoolEIRFFF,                  ! Energy input ratio modifier curve (flow fraction)
-      HPACCoolPLFFPLR,                 ! Part load factor modifier curve (function of part-load ratio)
-      CyclingFanAndCompressor;                   ! Operation mode (cycling fan, cycling compressor)
-
-   Coil:Heating:Gas,
-      Heat Pump DX Supp Heating Coil 1, ! Name of heating coil
-      FanAndCoilAvailSched,             ! Availability schedule
-      0.8 ,                             ! Gas Burner Efficiency of the Coil
-      32000,                            ! Nominal Capacity of the Coil [W]
-      SuppHeating Coil Air Inlet Node,  ! Supplementary heating coil air side inlet node
-      Air Loop Outlet Node;             ! Supplementary heating coil air side outlet node
-
-   Fan:OnOff,
-      Supply Fan 1,                    ! Fan Name
-      FanAndCoilAvailSched,            ! Fan Schedule
-      0.7,                             ! Fan Total Efficiency
-      300.0,                           ! Delta Pressure [N/M^2]
-      1.7,                             ! Max Vol Flow Rate  [m^3/Sec]
-      0.9,                             ! motor efficiency
-      1.0,                             ! motor in air stream fraction
-      Mixed Air Node,                  ! fan inlet node
-      DX Cooling Coil Air Inlet Node;  ! fan outlet node
-
-   AirTerminal:SingleDuct:Uncontrolled,
-      Zone1DirectAir,                  ! direct air unit name
-     FanAndCoilAvailSched,            ! schedule name for on/off schedule
-      Zone 1 Inlet Node,               ! zone supply air node name
-     0.612;                           ! maximum air flow rate, m3/s
-
-   AirTerminal:SingleDuct:Uncontrolled,
-      Zone2DirectAir,                  ! direct air unit name
-     FanAndCoilAvailSched,            ! schedule name for on/off schedule
-      Zone 2 Inlet Node,               ! zone supply air node name
-     0.476;                           ! maximum air flow rate, m3/s
-
-   AirTerminal:SingleDuct:Uncontrolled,
-      Zone3DirectAir,                  ! direct air unit name
-     FanAndCoilAvailSched,            ! schedule name for on/off schedule
-      Zone 3 Inlet Node,               ! zone supply air node name
-     0.612;                           ! maximum air flow rate, m3/s
-```
-
-
-### Unitary Air to Air Heat Pump (AirLoopHVAC) Outputs
-
-* HVAC, Average, Unitary System Fan Part Load Ratio []
-
-* HVAC, Average, Unitary System Compressor Part Load Ratio []
-
-* HVAC, Average, Unitary System Dehumidification Induced Heating Demand Rate [W]
-
-#### Unitary System Fan Part Load Ratio []
-
-This output variable is the ratio of actual air mass flow rate through the heat pump to the heat pump’s design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the furnace is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating (or cooling) load to the steady-state heat pump heating (or cooling) capacity. For the cycling fan mode, the runtime fraction for the heat pump fan may be different from the fan part-load ratio reported here due the part-load performance of the heat pump’s heating (or cooling) coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff).
-
-#### Unitary System Compressor Part Load Ratio []
-
-This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the heat pump’s DX heating or cooling coil. The runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due the part-load performance of the heating/cooling coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
-
-#### Unitary System Dehumidification Induced Heating Demand Rate [W]
-
-This output variable is the additional heating demand rate of the supplemental heating coil of an Air-to-Air heat pumps in Watts.  This additional heating demand is induced when zone air overshoots the heating setpoint due to extra dehumidification requirement to meet the high humidity setpoint. This value is always positive. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
-
-### AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed
-
-The multispeed air-to-air heat pump is a “virtual� component that consists of a fan component (On/Off or ConstVolume), a DX multispeed cooling coil component, a DX multispeed heating coil component, and a Gas or Electric supplemental heating coil component. This system also includes the option to use available waste energy to heat water. A schematic diagram of the air-to-air multispeed heat pump is shown below. The component connection sequence for the blow through option (shown below) from inlet to outlet is fan, cooling coil, heating coil, and supplemental heater. The connection sequence for the draw through option is cooling coil, heating coil, fan, and supplemental heater.
-
-The main difference between this heat pump object and other EnergyPlus heat pump objects is that this object allows from two to four discrete compressor speeds for heating and cooling operation (instead of a single speed for each mode). The lowest speed is called Speed 1, and the highest speed is called Speed n (2, 3 or 4 as specified in the input syntax). This object allows a different number of speeds for cooling and heating, and each speed has an associated airflow rate. The airflow rates for the various heating speeds can be different from the airflow rates for the cooling speeds. In addition, the airflow rate when no cooling or heating is needed can also be defined. The number of cooling and heating speeds defined by the user in this heat pump object must equal the number of speeds defined in the associated coils (child objects). For example, the number of speeds for cooling defined in this heat pump object must be equal to the number of speeds defined in the associated cooling coil object.
-
-Links to the fan, DX multispeed cooling coil, DX multispeed heating coil, and supplementary heating coil specifications are provided in the heat pump’s input data syntax. In addition, the control zone name and airflow rates at the corresponding compressor speeds are specified by the heat pump syntax.
-
-If the ZoneControl:Thermostat:StagedDualSetpoint object and other zone control thermostat and humidistat are assigned to the same controlled zone in the Controlling Zone or Thermostat Location field, the ZoneControl:Thermostat:StagedDualSetpoint object takes precedence and the stage number provided by the the ZoneControl:Thermostat:StagedDualSetpoint object is used to set the speed number.
-
-![FurnaceSchematic\_BlowThru\_Multispeed](media/image301.png)
-
-Figure 119. Schematic of EnergyPlus Unitary Air-to-Air Multi Speed Heat Pump
-
-#### Field: Name
-
-This alpha field contains the identifying name for the multispeed heat pump.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name (ref. Schedule objects) that contains information on the availability of the heat pump to operate. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the name of the HVAC system node from which the heat pump draws its inlet air.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the name of the HVAC system node to which the heat pump sends its outlet air.
-
-#### Field: Controlling Zone or Thermostat Location
-
-This alpha field contains the identifying zone name where the thermostat controlling the multispeed heat pump is located.
-
-#### Field: Supply Air Fan Object Type
-
-This alpha field contains the identifying type of supply air fan specified for the heat pump. Fan type must be Fan:OnOff or Fan:ConstantVolume. Fan:ConstantVolume can only be used when the supply air fan operating mode is continuous (see field ‘Supply air fan operating mode schedule name).
-
-#### Field: Supply Air Fan Name
-
-This alpha field contains the identifying name given to the heat pump supply air fan, and should match the name specified in the corresponding fan object.
-
-#### Field: Supply Air Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. The first choice stands for “blow through fan�. This means that the unit consists of a fan followed by a DX multispeed cooling coil, DX multispeed heating coil, and a supplemental heating coil. The fan “blows through� the cooling and heating coils. The second choice stands for “draw through fan�. This means that the unit consists of the DX cooling and heating coils followed by a fan, with the supplemental heater located at the outlet of the fan.  The fan “draws� air through the DX coils.
-
-**Note**: the multispeed heat pump’s supply air fan, cooling coil, heating coil and supplemental heating coil must be connected according to the configuration shown above (Figure 119) for the ‘blow through’ fan configuration. For the ‘draw through’ fan configuration the fan must be located between the DX heating coil and the supplemental heater, whose outlet node is the system outlet node. In addition, the DX cooling coil and DX heating coil operation mode must be specified consistently with the heat pump’s supply air fan operating mode (e.g., with the heat pump’s supply air fan set to cycle on and off with the cooling/heating load, the DX cooling and heating coil operation mode must be CyclingFanAndCompressor). If the operation modes in the parent (heat pump) and child (coil) objects are specified differently, the operation mode in the parent object prevails.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This alpha field contains the schedule name (ref. Schedule objects) that contains information to control the supply air fan. Schedule values of zero mean that the supply air fan will cycle off if there is no cooling or heating load in the control zone. Non-zero schedule values mean that the supply air fan will operate continuously even if there is no cooling or heating load in the control zone. If this field is left blank, the supply air fan will operate continuously for the entire simulation period.
-
-#### Field: Heating Coil Object Type
-
-This alpha field contains the identifying type of heating coil specified in the heat pump.  Allowable choices for Heating coil type  are **Coil:Heating:DX:MultiSpeed**, **Coil:Heating:Electric:MultiStage**, **Coil:Heating:Gas:MultiStage**, **Coil:Heating:Water**, and  **Coil:Heating:Steam**.
-
-#### Field: Heating Coil Name
-
-This alpha field contains the identifying name given to the DX heating coil, and should match the name specified in the corresponding DX heating coil object.
-
-#### Field: Minimum Outdoor Dry-Bulb Temperature for Compressor Operation
-
-This numeric field defines the outdoor air dry-bulb temperature below which the DX heating coil turns off.  The temperature for this input field must be greater than or equal to –20 C.  If this input field is left blank, the default value is -8 C. This temperature should match the minimum compressor operating temperature specified for the multispeed heat pump’s DX heating coil. This field is only needed when Heating Coil Object Type above is **Coil:Heating:DX:MultiSpeed**.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field contains the identifying type of cooling coil specified in the heat pump.  Cooling coil type must be Coil:Cooling:DX:MultiSpeed.
-
-#### Field: Cooling Coil Name
-
-This alpha field contains the identifying name given to the heat pump cooling coil, and should match the name specified in the corresponding DX cooling coil object.
-
-#### Field: Supplemental Heating Coil Object Type
-
-This alpha field contains the identifying type of supplemental heating coil specified in the heat pump. The hot water and steam heating coils require specifying plant loop, branches, and connectors objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the supplemental heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary MultiSpeed Air to Air Heat Pump) itself provides the "controller" function of modulating water flow. Heating coil type must be:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Supplemental Heating Coil Name
-
-This alpha field contains the identifying name given to the heat pump supplemental heating coil, and should match the name specified in the corresponding heating coil object.
-
-#### Field: Maximum Supply Air Temperature from Supplemental Heater
-
-This numeric field defines the maximum allowed supply air temperature (in degrees C) exiting the heat pump supplemental heating coil. If the calculated supply air temperature exiting the supplemental heater exceeds this value, then it is reset to this maximum temperature. This field is autosizable.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which the heat pump supplemental heating coil is disabled.  The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
-
-#### Field: Auxiliary On-Cycle Electric Power
-
-This field defines auxiliary electrical power (W) consumed during the on-cycle period (i.e., when the cooling or heating coil is operating). The model assumes that this auxiliary power does not contribute to heating the supply air. The minimum value for this field is 0.0, and the default value is also 0.0 if the field is left blank.
-
-#### Field: Auxiliary Off-Cycle Electric Power
-
-This field defines auxiliary electrical power (W) consumed during the off-cycle period (i.e., when the cooling and heating coil are not operating). The model assumes that this auxiliary power does not contribute to heating the supply air. The minimum value for this field is 0.0, and the default value is also 0.0 if the field is left blank.
-
-#### Field: Design Heat Recovery Water Flow Rate
-
-This optional input field defines the design water flow rate used if the heat recovery option is being simulated. If this value is greater than 0.0 then a heat recovery loop must be specified and attached to the multispeed heat pump using the next 2 node fields. To determine how the heat recovery algorithm works, refer to the EnergyPlus Engineering Reference in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed with Heat Recovery section. The units for this input value are cubic meters per second.
-
-#### Field: Maximum Temperature for Heat Recovery
-
-This field sets the maximum temperature (in degrees C) that this heat pump can produce for heat recovery. The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit. This temperature limit puts an upper bound on the recovered heat and limits the max temperature leaving the component.
-
-As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting. This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply.
-
-#### Field: Heat Recovery Water Inlet Node Name
-
-This alpha field contains the identifying name for the heat recovery side inlet node.
-
-#### Field: Heat Recovery Water Outlet Node Name
-
-This alpha field contains the identifying name for the heat recovery side outlet node.
-
-#### Field: No Load Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when neither cooling nor heating is required (i.e., DX coils and supplemental heater are off but the supply air fan operates). This field is only used when the heat pump supply air fan is scheduled to operate continuously regardless of DX coil operation (ref. field “Supply Air Fan Operating Mode Schedule). Values must be greater than or equal to zero, or this field is autosizable. If the heat pump supply air fan is scheduled to operate continuously and the input value for this field is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the compressor was last operating (for cooling operation or heating operation).
-
-#### Field: Number of Speeds for Heating
-
-This field defines the number of heating speeds for the heat pump, and must match the number of heating speeds defined in the associated heating coil. The value for this input field defines the number of airflow rates that must be defined for heating in the field below. The minimum value for this field is one and the maximum value is four. If the Heating Coil Object Type above are **Coil:Heating:Water** or **Coil:Heating:Steam**, then this field should be 1.
-
-#### Field: Number of Speeds for Cooling
-
-This field defines the number of cooling speeds for the heat pump, and must match the number of cooling speeds defined in the associated DX cooling coil. The value for this input field defines the number of airflow rates that must be defined for cooling in the field below. The minimum value for this field is two and the maximum value is four.
-
-#### Field: Heating Speed 1 Supply Air Flow Rate
-
-This required numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating at Speed 1 (lowest speed). Values must be greater than 0 or this field is autosizable.
-
-#### Field: Heating Speed 2 Supply Air Flow Rate
-
-This required numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating at Speed 2. Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for heating Speed 1.
-
-#### Field: Heating Speed 3 Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating at Speed 3. Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for heating Speed 2. If the ‘Number of Speeds for Heating’ is less than 3, then this field can be left blank.
-
-#### Field: Heating Speed 4 Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX heating coil and/or supplemental heater are operating at Speed 4 (high speed). Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for heating Speed 3. If the ‘Number of Speeds for Heating’ is less than 4, then this field can be left blank.
-
-**Note**: When autosizable is selected for any of the supply air volumetric flow rate fields, all supply air flow fields at the different speeds must be specified as autosizable. Otherwise, a fatal error will be issued and the simulation will terminate.
-
-#### Field: Cooling Speed 1 Supply Air Flow Rate
-
-This required numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating at Speed 1 (lowest speed). Values must be greater than 0 or this field is autosizable.
-
-#### Field: Cooling Speed 2 Supply Air Flow Rate
-
-This required numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating at Speed 2. Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for cooling Speed 1.
-
-#### Field: Cooling Speed 3 Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating at Speed 3. Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for cooling Speed 2. If the ‘Number of Speeds for Cooling’ is less than 3, then this field can be left blank.
-
-#### Field: Cooling Speed 4 Supply Air Flow Rate
-
-This numeric field defines the supply air flow rate leaving the heat pump in cubic meters per second when the DX cooling coil is operating at Speed 4 (highest speed). Values must be greater than 0 or this field is autosizable. If not autosized, the entered value must be greater or equal to the flow rate specified for cooling Speed 3. If the ‘Number of Speeds for Cooling’ is less than 4, then this field can be left blank.
-
-Following is an example input for the object and its associated components.
-
-```idf
-AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed,
-    DXAC Heat Pump 1,        !- Name of multispeed heat pump
-    FanAndCoilAvailSched,    !- Availability schedule
-    Mixed Air Node,          !- Heat pump air inlet node name
-    Air Loop Outlet Node,    !- Heat pump air outlet node name
-    East Zone,               !- Controlling zone or thermostat location
-    Fan:OnOff,               !- Supply air fan type
-    Supply Fan 1,            !- Supply air fan name
-    BlowThrough,             !- Supply air fan placement
-    FanModeSchedule,         !- Supply air fan operating mode schedule name
-    Coil:Heating:DX:MultiSpeed, Heat Pump DX Heating Coil 1,  !- Heating coil type & name
-    -8.0,                    !- Minimum outdoor dry-bulb temperature for compressor operation
-    Coil:Cooling:DX:MultiSpeed, Heat Pump ACDXCoil 1,    !- Cooling coil type & name
-    Coil:Heating:Gas,        !- Supplemental heating coil type
-    Supp Gas Heating Coil 1, !- Supplemental heating coil name
-    50.0,                    !- Maximum supply air temperature from supplemental heater
-    21,                      !- Maximum outdoor dry-bulb temperature for supplemental heater operation
-    0,                       !- Auxiliary On-Cycle Electric Power {W}
-    0,                       !- Auxiliary Off-Cycle Electric Power {W}
-    0.00,                    !- Design Heat Recovery Water Flow Rate {m3/s}
-    80.0,,,                    !- Maximum Temp for Heat Recovery {C} & Node names (none)
-    0.2,                     !- Supply air volumetric flow rate when no cooling or heating is needed
-    4,                       !- Number of speeds for heating
-    4,                       !- Number of speeds for cooling
-    0.4,                     !- Heating Speed 1 Supply Air Flow Rate
-    0.8,                     !- Heating Speed 2 Supply Air Flow Rate
-    1.2,                     !- Heating Speed 3 Supply Air Flow Rate
-    1.7,                     !- Heating Speed 4 Supply Air Flow Rate
-    0.4,                     !- Cooling Speed 1 Supply Air Flow Rate
-    0.8,                     !- Cooling Speed 2 Supply Air Flow Rate
-    1.2,                     !- Cooling Speed 3 Supply Air Flow Rate
-    1.7;                     !- Cooling Speed 4 Supply Air Flow Rate
-
-Coil:Heating:DX:MultiSpeed,
-    Heat Pump DX Heating Coil 1,  !- Name of heat pump heating coil
-    FanAndCoilAvailSched,    !- Availability Schedule
-    Heating Coil Air Inlet Node,  !- Coil Air Inlet Node
-    SuppHeating Coil Air Inlet Node,  !- Coil Air Outlet Node
-    CyclingFanAndCompressor,           !- Supply Air Fan Operation Mode
-    -8.0,                    !- Minimum Outdoor Dry-bulb Temperature for Compressor Operation {C}
-    200.0,                   !- Crankcase Heater Capacity {W}
-    10.0,                    !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater
-                         !- Operation {C}
-    HPACDefrostCAPFT,        !- Defrost energy input ratio modifier curve (temperature)
-    7.22,                    !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation
-    reverse-cycle,           !- Defrost Strategy
-    timed,                   !- Defrost Control
-    0.058333,                !- Defrost Time Period Fraction
-    2000.0,                  !- Resistive Defrost Heater Capacity {W}
-    No,                      !- Apply Part Load Fraction to Speeds greater than 1
-    NaturalGas,              !- Fuel type
-    4,                       !- Number of speeds
-    7500,                    !- Rated Total Heating Capacity, Speed 1 {W}
-    2.75,                    !- Rated COP, Speed 1
-    0.45,                    !- Rated Air Volume Flow Rate, Speed 1 {m3/s}
-    HPACHeatCapFT Speed 1,   !- Total Heating Capacity Modifier Curve, Speed 1 (temperature)
-    HPACHeatCapFF Speed 1,   !- Total Heating capacity modifier curve, Speed 1 (flow fraction)
-    HPACHeatEIRFT Speed 1,   !- Energy input ratio modifier curve, Speed 1 (temperature)
-    HPACHeatEIRFF Speed 1,   !- Energy input ratio modifier curve, Speed 1 (flow fraction)
-    HPACHeatPLFFPLR Speed 1, !- Part load fraction correlation, Speed 1 (part load ratio)
-    0.2,                     !- Rated waste heat fraction of power input, Speed 1
-    HAPCHeatWHFT Speed 1,    !- Waste heat modifier curve, Speed 1 (temperature)
-    17500,                   !- Rated Total Heating Capacity, Speed 2 {W}
-    2.75,                    !- Rated COP, Speed 2
-    0.85,                    !- Rated Air Volume Flow Rate, Speed 2 {m3/s}
-    HPACHeatCapFT Speed 2,   !- Total Heating Capacity Modifier Curve, Speed 2 (temperature)
-    HPACHeatCapFF Speed 2,   !- Total Heating capacity modifier curve, Speed 2 (flow fraction)
-    HPACHeatEIRFT Speed 2,   !- Energy input ratio modifier curve, Speed 2 (temperature)
-    HPACHeatEIRFF Speed 2,   !- Energy input ratio modifier curve, Speed 2 (flow fraction)
-    HPACHeatPLFFPLR Speed 2, !- Part load fraction correlation, Speed 2 (part load ratio)
-    0.2,                     !- Rated waste heat fraction of power input, Speed 2
-    HAPCHeatWHFT Speed 2,    !- Waste heat modifier curve, Speed 2 (temperature)
-    25500,                   !- Rated Total Heating Capacity, Speed 3 {W}
-    2.75,                    !- Rated COP, Speed 3
-    1.25,                    !- Rated Air Volume Flow Rate, Speed 3 {m3/s}
-    HPACHeatCapFT Speed 3,   !- Total Heating Capacity Modifier Curve, Speed 3 (temperature)
-    HPACHeatCapFF Speed 3,   !- Total Heating capacity modifier curve, Speed 3 (flow fraction)
-    HPACHeatEIRFT Speed 3,   !- Energy input ratio modifier curve, Speed 3 (temperature)
-    HPACHeatEIRFF Speed 3,   !- Energy input ratio modifier curve, Speed 3 (flow fraction)
-    HPACHeatPLFFPLR Speed 3, !- Part load fraction correlation, Speed 3 (part load ratio)
-    0.2,                     !- Rated waste heat fraction of power input, Speed 3
-    HAPCHeatWHFT Speed 3,    !- Waste heat modifier curve, Speed 3 (temperature)
-    35500,                   !- Rated Total Heating Capacity, Speed 4 {W}
-    2.75,                    !- Rated COP, Speed 4
-    1.75,                    !- Rated Air Volume Flow Rate, Speed 4 {m3/s}
-    HPACHeatCapFT Speed 4,   !- Total Heating Capacity Modifier Curve, Speed 4 (temperature)
-    HPACHeatCapFF Speed 4,   !- Total Heating capacity modifier curve, Speed 4 (flow fraction)
-    HPACHeatEIRFT Speed 4,   !- Energy input ratio modifier curve, Speed 4 (temperature)
-    HPACHeatEIRFF Speed 4,   !- Energy input ratio modifier curve, Speed 4 (flow fraction)
-    HPACHeatPLFFPLR Speed 4, !- Part load fraction correlation, Speed 4 (part load ratio)
-    0.2,                     !- Rated waste heat fraction of power input, Speed 4
-    HAPCHeatWHFT Speed 4;    !- Waste heat modifier curve, Speed 4 (temperature)
-
-
-  COIL:Cooling:DX:MultiSpeed,
-    Heat Pump ACDXCoil 1,    !- Coil Name
-    FanAndCoilAvailSched,    !- Availability Schedule
-    DX Cooling Coil Air Inlet Node,  !- Coil Air Inlet Node
-    Heating Coil Air Inlet Node,  !- Coil Air Outlet Node
-    CyclingFanAndCompressor,           !- Supply Air Fan Operation Mode
-    Outdoor Condenser Air Node, !- Condenser Air Inlet Node Name
-    AirCooled,              !- Condenser Type
-    ,                        !- Name of Water Storage Tank for Supply
-    ,                        !- Name of Water Storage Tank for Condensate Collection
-    No,                      !- Apply Part Load Fraction to Speeds greater than 1
-    No,                      !- Apply Latent Degradation to Speeds greater than 1
-    200.0,                   !- Crankcase Heater Capacity {W}
-10.0,                    !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater
-                         !- Operation {C}
-    NaturalGas,              !- Fuel type
-    4,                       !- Number of speeds
-    7500,                    !- Rated Total Cooling Capacity, Speed 1 (gross) {W}
-    0.75,                    !- Rated SHR, Speed 1
-    3.0,                     !- Rated COP, Speed 1
-    0.40,                    !- Rated Air Volume Flow Rate, Speed 1 {m3/s}
-    HPACCoolCapFT Speed 1,   !- Total Cooling Capacity Modifier Curve, Speed 1 (temperature)
-    HPACCoolCapFF Speed 1,   !- Total Cooling Capacity Modifier Curve, Speed 1 (flow fraction)
-    HPACCOOLEIRFT Speed 1,   !- Energy Input Ratio Modifier Curve, Speed 1 (temperature)
-    HPACCOOLEIRFF Speed 1,   !- Energy Input Ratio Modifier Curve, Speed 1 (flow fraction)
-    HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 1 (part load ratio)
-    1000.0,                  !- Nominal Time for Condensate Removal to Begin, Speed 1 {s}
-1.5,                     !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent
-                         !- Capacity, Speed 1 {dimensionless}
-    3.0,                     !- Maximum ON/OFF Cycling Rate, Speed 1 {cycles/hr}
-    45.0,                    !- Latent Capacity Time Constant, Speed 1 {s}
-    0.2,                     !- Rated waste heat fraction of power input, Speed 1 {dimensionless}
-    HAPCCoolWHFT Speed 1,    !- Waste heat modifier curve, Speed 1 (temperature)
-    0.9,                     !- Evaporative Condenser Effectiveness, Speed 1 {dimensionless}
-    0.05,                    !- Evaporative Condenser Air Volume Flow Rate, Speed 1 {m3/s}
-    50,                      !- Evaporative Condenser Pump Rated Power Consumption, Speed 1 {W}
-    17500,                   !- Rated Total Cooling Capacity, Speed 2 (gross) {W}
-    0.75,                    !- Rated SHR, Speed 2
-    3.0,                     !- Rated COP, Speed 2
-    0.85,                    !- Rated Air Volume Flow Rate, Speed 2 {m3/s}
-    HPACCoolCapFT Speed 2,   !- Total Cooling Capacity Modifier Curve, Speed 2 (temperature)
-    HPACCoolCapFF Speed 2,   !- Total Cooling Capacity Modifier Curve, Speed 2 (flow fraction)
-    HPACCOOLEIRFT Speed 2,   !- Energy Input Ratio Modifier Curve, Speed 2 (temperature)
-    HPACCOOLEIRFF Speed 2,   !- Energy Input Ratio Modifier Curve, Speed 2 (flow fraction)
-    HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 2 (part load ratio)
-    1000.0,                  !- Nominal Time for Condensate Removal to Begin, Speed 2 {s}
-1.5,                     !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent
-                         !- Capacity, Speed 2 {dimensionless}
-    3.0,                     !- Maximum ON/OFF Cycling Rate, Speed 2 {cycles/hr}
-    45.0,                    !- Latent Capacity Time Constant, Speed 2 {s}
-    0.2,                     !- Rated waste heat fraction of power input, Speed 2 {dimensionless}
-    HAPCCoolWHFT Speed 2,    !- Waste heat modifier curve, Speed 2 (temperature)
-    0.9,                     !- Evaporative Condenser Effectiveness, Speed 2 {dimensionless}
-    0.1,                     !- Evaporative Condenser Air Volume Flow Rate, Speed 2 {m3/s}
-    60,                      !- Evaporative Condenser Pump Rated Power Consumption, Speed 2 {W}
-    25500,                   !- Rated Total Cooling Capacity, Speed 3 (gross) {W}
-    0.75,                    !- Rated SHR, Speed 3
-    3.0,                     !- Rated COP, Speed 3
-    1.25,                    !- Rated Air Volume Flow Rate, Speed 3 {m3/s}
-    HPACCoolCapFT Speed 3,   !- Total Cooling Capacity Modifier Curve, Speed 3 (temperature)
-    HPACCoolCapFF Speed 3,   !- Total Cooling Capacity Modifier Curve, Speed 3 (flow fraction)
-    HPACCOOLEIRFT Speed 3,   !- Energy Input Ratio Modifier Curve, Speed 3 (temperature)
-    HPACCOOLEIRFF Speed 3,   !- Energy Input Ratio Modifier Curve, Speed 3 (flow fraction)
-    HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 3 (part load ratio)
-    1000.0,                  !- Nominal Time for Condensate Removal to Begin, Speed 3 {s}
-1.5,                     !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent
-                         !- Capacity, Speed 3 {dimensionless}
-    3.0,                     !- Maximum ON/OFF Cycling Rate, Speed 3 {cycles/hr}
-    45.0,                    !- Latent Capacity Time Constant, Speed 3 {s}
-    0.2,                     !- Rated waste heat fraction of power input, Speed 3 {dimensionless}
-    HAPCCoolWHFT Speed 3,    !- Waste heat modifier curve, Speed 3 (temperature)
-    0.9,                     !- Evaporative Condenser Effectiveness, Speed 3 {dimensionless}
-    0.2,                     !- Evaporative Condenser Air Volume Flow Rate, Speed 3 {m3/s}
-    80,                      !- Evaporative Condenser Pump Rated Power Consumption, Speed 3 {W}
-    35500,                   !- Rated Total Cooling Capacity, Speed 4 (gross) {W}
-    0.75,                    !- Rated SHR, Speed 4
-    3.0,                     !- Rated COP, Speed 4
-    1.75,                    !- Rated Air Volume Flow Rate, Speed 4 {m3/s}
-    HPACCoolCapFT Speed 4,   !- Total Cooling Capacity Modifier Curve, Speed 4 (temperature)
-    HPACCoolCapFF Speed 4,   !- Total Cooling Capacity Modifier Curve, Speed 4 (flow fraction)
-    HPACCOOLEIRFT Speed 4,   !- Energy Input Ratio Modifier Curve, Speed 4 (temperature)
-    HPACCOOLEIRFF Speed 4,   !- Energy Input Ratio Modifier Curve, Speed 4 (flow fraction)
-    HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 4 (part load ratio)
-    1000.0,                  !- Nominal Time for Condensate Removal to Begin, Speed 4 {s}
-1.5,                     !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent
-                         !- Capacity, Speed 4 {dimensionless}
-    3.0,                     !- Maximum ON/OFF Cycling Rate, Speed 4 {cycles/hr}
-    45.0,                    !- Latent Capacity Time Constant, Speed 4 {s}
-    0.2,                     !- Rated waste heat fraction of power input, Speed 4 {dimensionless}
-    HAPCCoolWHFT Speed 4,    !- Waste heat modifier curve, Speed 4 (temperature)
-    0.9,                     !- Evaporative Condenser Effectiveness, Speed 4 {dimensionless}
-    0.3,                     !- Evaporative Condenser Air Volume Flow Rate, Speed 4 {m3/s}
-    100;                     !- Evaporative Condenser Pump Rated Power Consumption, Speed 4 {W}
-
-Coil:Heating:Gas,
-    Supp Gas Heating Coil 1,  !- Coil Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    0.8,                     !- Gas Burner Efficiency of the Coil
-    45000,                   !- Nominal Capacity of the Coil {W}
-    SuppHeating Coil Air Inlet Node,  !- Coil\_Air\_Inlet\_Node
-    Air Loop Outlet Node;    !- Coil\_Air\_Outlet\_Node
-
-Fan:OnOff,
-    Supply Fan 1,            !- Fan Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    0.7,                     !- Fan Total Efficiency
-    300.0,                   !- Delta Pressure {Pa}
-    1.7,                     !- Max Flow Rate {m3/s}
-    0.9,                     !- Motor Efficiency
-    1.0,                     !- Motor In Airstream Fraction
-    Mixed Air Node,          !- Fan\_Inlet\_Node
-    DX Cooling Coil Air Inlet Node;  !- Fan\_Outlet\_Node
-
-AirTerminal:SingleDuct:Uncontrolled,
-      Zone1DirectAir,                  ! direct air unit name
-     FanAndCoilAvailSched,            ! schedule name for on/off schedule
-      Zone 1 Inlet Node,               ! zone supply air node name
-     0.612;                           ! maximum air flow rate, m3/s
-
-AirTerminal:SingleDuct:Uncontrolled,
-      Zone2DirectAir,                  ! direct air unit name
-     FanAndCoilAvailSched,            ! schedule name for on/off schedule
-      Zone 2 Inlet Node,               ! zone supply air node name
-     0.476;                           ! maximum air flow rate, m3/s
-
-AirTerminal:SingleDuct:Uncontrolled,
-      Zone3DirectAir,                  ! direct air unit name
-     FanAndCoilAvailSched,            ! schedule name for on/off schedule
-      Zone 3 Inlet Node,               ! zone supply air node name
-     0.612;                           ! maximum air flow rate, m3/s
-```
-
-### Unitary Air to Air MultiSpeed Heat Pump (AirLoopHVAC) Outputs
-
-* HVAC,Average,Unitary System Fan Part Load Ratio []
-
-* HVAC,Average,Unitary System Compressor Part Load Ratio []
-
-* HVAC,Average,Unitary System DX Coil Cycling Ratio []
-
-* HVAC,Average,Unitary System DX Coil Speed Ratio []
-
-* HVAC,Average,Unitary System DX Coil Speed Level []
-
-* HVAC,Average,Unitary System Electric Power[W]
-
-* HVAC,Sum,Unitary System Electric Energy [J]
-
-* HVAC,Average,Unitary System Total Cooling Rate [W]
-
-* HVAC,Average,Unitary System Total Heating Rate [W]
-
-* HVAC,Average,Unitary System Sensible Cooling Rate [W]
-
-* HVAC,Average,Unitary System Sensible Heating Rate [W]
-
-* HVAC,Average,Unitary System Latent Cooling Rate [W]
-
-* HVAC,Average,Unitary System Latent Heating Rate [W]
-
-* HVAC,Average,Unitary System Ancillary Electric Power[W]
-
-* HVAC,Sum,Unitary System Cooling Ancillary Electric Energy [J]
-
-* HVAC,Sum,Unitary System Heating Ancillary Electric Energy [J]
-
-If heat recovery is specified:
-
-* HVAC,Average, Unitary System Heat Recovery Rate [W]
-
-* HVAC,Average, Unitary System Heat Recovery Inlet Temperature [C]
-
-* HVAC,Average, Unitary System Heat Recovery Outlet Temperature [C]
-
-* HVAC,Average, Unitary System Heat Recovery Fluid Mass Flow Rate [kg/s]
-
-* HVAC,Sum, Unitary System Heat Recovery Energy [J]
-
-#### Unitary System Fan Part Load Ratio []
-
-This output variable is the ratio of actual air mass flow rate through the multispeed heat pump to the heat pump’s design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate) at Speed 1. For continuous fan operation mode, this variable is always 1.0 when the heat pump is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating (or cooling) load to the steady-state heat pump heating (or cooling) capacity. For the cycling fan mode, the runtime fraction for the heat pump fan may be different from the fan part-load ratio reported here due the part-load performance of the heat pump’s heating (or cooling) coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff). When the speed number is greater than 1, the value is 1.0.
-
-#### Unitary System Compressor Part Load Ratio []
-
-This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the multispeed heat pump’s DX heating or cooling coil at Speed 1. The runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due the part-load performance of the heating/cooling coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate. When the speed number is greater than 1, the value is 1.0.
-
-#### Unitary System DX Coil Cycling Ratio []
-
-This output variable is the ratio of the sensible load (heating or cooling) to the steady-state capacity of the multispeed heat pump’s DX heating or cooling coil (Speed 1) for the entire system timestep. The value is between 0.0 and 1.0 when the heat pump is cycling on and off its lowest speed (Speed 1) and 1.0 when the multispeed heat pump operates at speeds above 1.
-
-When Single Mode Operation is specified, the value is between 0.0 and 1.0 when the heat pump is cycling on at any given speed. 
-
-#### Unitary System DX Coil Speed Ratio []
-
-This output variable is the ratio of time in a system timestep that the compressor is at rated speed between two consecutive speed numbers ( [Compressor Speed - Compressor speed at Speed i-1] / [Compressor speed at Speed i - Compressor speed at Speed i-1]). The compressor speed ratio reports (1.0 is max, 0.0 is min) and any value in between as it is averaged over the timestep. The value is 0.0 during Speed 1 operation.
-
-The physical meaning of the speed ratio is dependent on the compressor configuration defined in the field of child coil object: Apply Part Load Fraction to Speeds greater than 1. The allowed choice is either Yes or No. When No is entered, one compressor is assumed for all speeds.  The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the lower speed runs in the rest of the system timestep. When Yes is entered, multiple compressors are assumed, and each compressor has associated speed. The speed ratio represents how long the higher speed runs as a fraction of the system timestep, and the low speed runs in a whole system timestep.
-
-When Single Mode Operation is specified, the speed ratio is set to 0 at Speed 1, and 1 at Speed > 1
-
-#### Unitary System DX Coil Speed Level []
-
-This output variable reports the maximum speed needed when the heat pump operates to meet the sensible load (heating or cooling) in a system timestep. When the value is 1, the heat pump operates at Speed 1 (lowest speed). For this case the cycling ratio is between 0.0 and 1.0, while the speed ratio is 0.0. When the speed number output variable is above one, such as i, the heat pump operation is determined by the speed ratio through linear interpolation. For example, when the speed ratio is 0.4 and the speed number is 3, the heat pump operates at Speed 3 for 40% of a system timestep and at Speed 2 for 60% of a system timestep for a single compressor. For multiple compressors, the heat pump operates at Speed 3 in the 40% of a system timestep and at Speed 2 in the whole system timestep.
-
-#### Unitary System Total Heating Rate [W]
-
-This output field is the total (enthalpy) heat addition rate of the multispeed heat pump to the zones it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
-
-#### Unitary System Total Cooling Rate [W]
-
-This output field is the total (enthalpy) heat extraction rate of the multispeed heat pump from the zones it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
-
-#### Unitary System Sensible Heating Rate [W]
-
-This output field reports the sensible heat addition rate of the multispeed heat pump to the zones it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
-
-#### Unitary System Sensible Cooling Rate [W]
-
-This output field reports the moist air sensible heat extraction rate of the multispeed heat pump from the zones it is serving in Watts. This value is calculated using the enthalpy difference of the heat pump outlet air and inlet air streams at a constant humidity ratio, and the air mass flow rate through the heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
-
-#### Unitary System Latent Heating Rate [W]
-
-This output field is the latent heat addition (humidification) rate of the multispeed heat pump in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the multispeed heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
-
-#### Unitary System Latent Cooling Rate [W]
-
-This output field is the latent heat extraction (dehumidification) rate of the multispeed heat pump in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the multispeed heat pump. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
-
-#### Unitary System Electric Power [W]
-
-This output field is the electricity consumption rate of the multispeed heat pump in Watts. The consumption includes electricity used by the DX coils (including crankcase heater if the fuel type is electricity), fans (indoor supply air fan and the condenser fans associated with the DX coil[s]), auxiliary power during on and off period, and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported. Any non-electric energy use is not reported by the heat pump object but is reported in the associated coil objects as appropriate.
-
-#### Unitary System Electric Energy [J]
-
-This output field is the electricity consumption of the multispeed heat pump in Joules for the timestep being reported. The consumption includes electricity used by the DX compressor (including crankcase heater if the fuel type is electricity), fans (indoor supply air fan and the condenser fans associated with the DX coil[s]), auxiliary power during on and off period, and the supplemental heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are summed for the timestep being reported. Any non-electric energy use is not reported by the heat pump object but is reported in the associated coil objects as appropriate.
-
-#### Unitary System Ancillary Electric Power [W]
-
-This output field is the average auxiliary electricity consumption rate (including both on-cycle and off-cycle) in Watts for the timestep being reported.
-
-#### Unitary System Cooling Ancillary Electric Energy [J]
-
-This is the auxiliary electricity consumption in Joules for the timestep being reported. This is the auxiliary electricity consumption during periods when the heat pump is providing cooling (DX cooling coil is operating). This output is also added to a meter with Resource Type = Electricity, End Use Key =Cooling, Group Key = System (ref. Output:Meter objects).
-
-#### Unitary System Heating Ancillary Electric Energy [J]
-
-This is the auxiliary electricity consumption in Joules for the timestep being reported. This is the auxiliary electricity consumption during periods when the heat pump is providing heating (DX heating coil is operating). This output is also added to a meter with Resource Type = Electricity, End Use Key =Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Unitary System Heat Recovery Inlet Temperature [C]
-
-#### Unitary System Heat Recovery Outlet Temperature [C]
-
-#### Unitary System Heat Recovery Fluid Mass Flow Rate [kg/s]
-
-These outputs are the heat recovery inlet and outlet temperatures and water mass flow rate for multispeed heat pumps with heat recovery.
-
-#### Unitary System Heat Recovery Rate [W]
-
-#### Unitary System Heat Recovery Energy [J]
-
-For multispeed heat pumps with heat recovery, these outputs are the recoverable energy rate (in Watts) and energy (in Joules).
-
-### AirLoopHVAC:Unitary:Furnace:HeatOnly
-
-The EnergyPlus furnace is a “virtual� component that consists of a fan component  (OnOff or ConstantVolume) and a Gas or Electric heating coil component. The blow through furnace configuration is shown in the Figure below.
-
-![](media/image302.svg)
-
-Figure 120. Schematic of Blow Through Furnace Model
-
-Links to the fan and heating coil specifications are provided in the furnace input data syntax. In addition the control zone name and the furnace design operating conditions are specified by the furnace inputs.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the furnace.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name which contains information on the availability of the furnace to operate. A schedule value equal to 0 denotes that the furnace must be off for that time period. A value greater than 0 denotes that the furnace is available to operate during that time period. This schedule may be used to completely disable the unitary system as required. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Furnace Inlet Node Name
-
-This alpha field contains the furnace inlet node name.
-
-#### Field: Furnace Outlet Node Name
-
-This alpha field contains the furnace outlet node name.
-
-***Field: Supply Air Fan Operating Mode Schedule Name***
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the furnace supply air fan and the heating coil cycle on and off together to meet the heating load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating coil cycles to meet the load.
-
-#### Field: Maximum Supply Air Temperature
-
-This numeric field contains the design operating furnace air outlet temperature in degrees C when the furnace is heating. If this input field is left blank, the default value is 80 C.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field contains the design volumetric flow rate of the furnace in cubic meters per second. This volumetric flow rate should match the flow rate specified for the furnace fan.
-
-#### Field: Controlling Zone or Thermostat Location
-
-This alpha field contains the identifying zone name where the thermostat controlling the furnace is located.
-
-#### Field: Supply Fan Object Type
-
-This alpha field contains the identifying type of supply air fan specified for the furnace. Fan type must be **Fan:OnOff** or **Fan:ConstantVolume**. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e. Supply Air Fan Operating Mode Schedule values are at times 0).
-
-#### Field: Supply Fan Name
-
-This alpha field contains the identifying name given to the furnace fan.
-
-#### Field: Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. The first choice stands for “blow through fan�. This means that the unit consists of a fan followed by the heating coil. The fan “blows through� the heating coil. The second choice stands for “draw through fan�. This means that the unit consists of the heating coil followed by a fan. The fan “draws air through� the heating coil. If this field is left blank, the default is blow through.
-
-#### Field: Heating Coil Object Type
-
-This alpha field contains the identifying type of heating coil specified in the furnace. The hot water and steam heating coils require specifying plant loop, branches, and connectors objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat Only Furnace) itself provides the "controller" function of modulating water flow. Heating coil type must be:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Heating Coil Name
-
-This alpha field contains the identifying name given to the furnace heating coil.
-
-As shown in the example below, correct specification of the furnace requires specification of the following objects in addition to the furnace object:
-
-1)   fan (Fan:OnOff or Fan:ConstantVolume)
-
-2)   heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
-
-3)   direct air unit (AirTerminal:SingleDuct:Uncontrolled) for each zone served by the furnace
-
-Note: the furnace’s fan and heating coil must be connected in the air loop according to the configuration shown above (Figure 120) when a blow through fan configuration is specified. If a draw through fan is used, the fan is located down stream of the heating coil. In addition, the volumetric air flow rate specified in the direct air unit for the controlling zone should properly reflect the fractional volumetric air flow rate specified in the furnace object.
-```idf
-AirLoopHVAC:Unitary:Furnace:HeatOnly,
-    Gas Furnace 1,        !- Name
-    FanAndCoilAvailSched, !- Availability Schedule Name
-    Air Loop Inlet Node,  !- Furnace Air Inlet Node Name
-    Air Loop Outlet Node, !- Furnace Air Outlet Node Name
-    CycFanSchedule,       !- Supply Air Fan Operating Mode Schedule Name
-    80,                   !- Maximum Supply Air Temperature {C}
-    1.3,                  !- Heating Supply Air Flow Rate {m3/s}
-    East Zone,            !- Controlling Zone or Thermostat Location
-    Fan:OnOff,            !- Supply Fan Object Type
-    Supply Fan 1,         !- Supply Fan Fame
-    BlowThrough,          !- Fan Placement
-    Coil:Heating:Gas,     !- Heating Coil Object Type
-    Furnace Coil;         !- Heating Coil Name
-
-
-  Coil:Heating:Gas,
-    Furnace Coil,          !- Coil Name
-    FanAndCoilAvailSched,  !- Availability Schedule Name
-    0.8,                   !- Gas Burner Efficiency of the Coil
-    20000,                 !- Nominal Capacity of the Coil {W}
-    Heating Coil Air Inlet Node,  !- Coil_Air_Inlet_Node
-    Air Loop Outlet Node,         !- Coil_Air_Outlet_Node
-    ,                      !- Coil_Temp_Setpoint_Node
-    100,                   !- Parasitic Electric Load {W}
-    PLFCurveforGasFurnace, !- Part load fraction correlation (function of part load ratio)
-    10;                    !- Parasitic Gas Load {W}
-
-
-Curve:Cubic,
-    PLFCurveforGasFurnace, !- Name
-    0.8,  !- Coefficient1 Constant
-    0.2,  !- Coefficient2 x
-    0.0,  !- Coefficient3 x**2
-    0.0,  !- Coefficient4 x**3
-    0,  !- Minimum Value of x
-    1;  !- Maximum Value of x
-
-
-  Fan:OnOff,
-    Supply Fan 1,          !- Fan Name
-    FanAndCoilAvailSched,  !- Availability Schedule Name
-    0.7,    !- Fan Total Efficiency
-    600.0,  !- Delta Pressure {Pa}
-    1.3,    !- Max Flow Rate {m3/s}
-    0.9,    !- Motor Efficiency
-    1.0,    !- Motor In Airstream Fraction
-    Air Loop Inlet Node,          !- Fan_Inlet_Node
-    Heating Coil Air Inlet Node;  !- Fan_Outlet_Node
-
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone1DirectAir,       !-Direct Air Name
-    FanAndCoilAvailSched, !- Schedule name for on/off schedule
-    Zone 1 Inlet Node,    !- Zone Supply Air Node Name
-   0.47;   !- Maximum air flow rate {m3/s}
-
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone2DirectAir,       !- Direct Air Name
-   FanAndCoilAvailSched, !- Schedule name for on/off schedule
-    Zone 2 Inlet Node,    !- Zone Supply Air Node Name
-   0.36;   !- Maximum air flow rate {m3/s}
-
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone3DirectAir,       !- Direct Air Name
-   FanAndCoilAvailSched, !- Schedule name for on/off schedule
-    Zone 3 Inlet Node,    !- Zone Supply Air Node Name
-   0.47;   !- Maximum air flow rate {m3/s}
-```
-
-
-
-Example of Heat-Only Furnace Specification
-
-### Unitary/Furnace Heat Only (AirLoopHVAC) Outputs
-
-* HVAC,Average,Unitary System Fan Part Load Ratio []
-
-#### Unitary System Fan Part Load Ratio []
-
-This output variable is the ratio of actual air mass flow rate through the furnace to the furnace’s design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the furnace is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating load to the furnace heating capacity. For the cycling fan mode, the runtime fraction for the furnace fan may be different from the fan part-load ratio reported here due the part-load performance of the furnace’s heating coil (delay at start-up to reach steady-state heating output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff).
-
-### AirLoopHVAC:UnitaryHeatOnly
-
-The AirLoopHVAC:UnitaryHeatOnly is identical to the AirLoopHVAC:Unitary:Furnace:HeatOnly model. The heat-only unitary system is a “virtual� component that consists of a fan component (OnOff or ConstantVolume) and a Gas or Electric heating coil component. The blow through unitary system configuraion is shown in the Figure below.
-
-![](media/image303.svg)
-
-Figure 121. Schematic of Blow Through Heat-Only Unitary System
-
-Links to the fan and heating coil specifications are provided in the unitary system input data syntax. In addition, the control zone name and the unitary system design operating conditions are specified by the unitary system syntax.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the unitary system.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name which contains information on the availability of the unitary system to operate. A schedule value equal to 0 denotes that the unitary system must be off for that time period. A value greater than 0 denotes that the unitary system is available to operate during that time period. This schedule may be used to completely disable the unitary system as required. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Unitary System Air Inlet Node Name
-
-This alpha field contains the unitary system inlet node name.
-
-#### Field: Unitary System Air Outlet Node Name
-
-This alpha field contains the unitary system outlet node name.
-
-***Field: Supply Air Fan Operating Mode Schedule Name***
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the furnace supply air fan and the heating coil cycle on and off together to meet the heating load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating coil cycles to meet the load.
-
-#### Field: Maximum Supply Air Temperature
-
-This numeric field contains the design  air outlet temperature in degrees C when the unitary system is heating. If this input field is left blank, the default value is 80 C.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field contains the design volumetric flow rate of the unitary system in cubic meters per second. This volumetric flow rate should match the flow rate specified for the unitary system fan.
-
-#### Field: Controlling Zone or Thermostat Location
-
-This alpha field contains the identifying zone name where the thermostat controlling the unitary system is located.
-
-#### Field: Supply Fan Object Type
-
-This alpha field contains the identifying type of supply air fan specified for the unitary system. Fan type must be **Fan:OnOff** or **Fan:ConstantVolume**. Fan:ConstantVolume is used when the Supply Air Fan Operating Mode Schedule values are never 0 and the fan operates continuously. Fan:OnOff is used when the fan cycles on and off with the cooling or heating coil (i.e. Supply Air Fan Operating Mode Schedule values are at times 0).
-
-#### Field: Supply Fan Name
-
-This alpha field contains the identifying name given to the unitary system fan.
-
-#### Field: Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. The first choice stands for “blow through fan�. This means that the unit consists of a fan followed by the heating coil. The fan “blows through� the heating coil. The second choice stands for “draw through fan�. This means that the unit consists of the heating coil followed by a fan. The fan “draws air through� the heating coil. If this field is left blank, the default is blow through.
-
-#### Field: Heating Coil Object Type
-
-This alpha field contains the identifying type of heating coil specified in the unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connectors objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Unitary Heat Only) itself provides the "controller" function of modulating water flow. Heating coil type must be:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Heating Coil Name
-
-This alpha field contains the identifying name given to the unitary system heating coil.
-
-As shown in the example below, correct specification of the heat-only unitary system requires specification of the following objects in addition to the unitary system object:
-
-1)   fan (Fan:OnOff or Fan:ConstantVolume)
-
-2)   heating coil (Coil:Heating:Gas or Coil:Heating:Electric)
-
-3)   direct air unit (AirTerminal:SingleDuct:Uncontrolled) for each zone served by the furnace
-
-Note: the unitary system’s fan and heating coil must be connected in the air loop according to the configuration shown above (Figure 121) when a blow through fan configuration is specified. If a draw through fan is used, the fan is located down stream of the heating coil. In addition, the volumetric air flow rate specified in the direct air unit for the controlling zone should properly reflect the fractional volumetric air flow rate specified in the unitary system object.
-
-```idf
-AirLoopHVAC:UnitaryHeatOnly,
-    Gas Unitary System 1, !- Name
-    FanAndCoilAvailSched, !- Availability Schedule Name
-    Air Loop Inlet Node,  !- Unitary System Air Inlet Node Name
-    Air Loop Outlet Node, !- Unitary System Air Outlet Node Name
-    CycFanSchedule,       !- Supply Air Fan Operating Mode Schedule Name
-    80,                   !- Maximum Supply Air Temperature {C}
-    1.3,                  !- Heating Supply Air Flow Rate {m3/s}
-    East Zone,            !- Controlling Zone or Thermostat Location
-    Fan:OnOff,            !- Supply Fan Object Type
-    Supply Fan 1,         !- Supply Fan Name
-    BlowThrough,          !- Fan Placement
-    Coil:Heating:Gas,     !- Heating Coil Object Type
-    Unitary System Heating Coil; !- Heating Coil Name
-
-
-  Coil:Heating:Gas,
-    Unitary System Heating Coil, !- Coil Name
-    FanAndCoilAvailSched,        !- Availability Schedule Name
-    0.8,                         !- Gas Burner Efficiency of the Coil
-    20000,                       !- Nominal Capacity of the Coil {W}
-    Heating Coil Air Inlet Node, !- Coil_Air_Inlet_Node
-    Air Loop Outlet Node,        !- Coil_Air_Outlet_Node
-    ,                            !- Coil_Temp_Setpoint_Node
-    100,                         !- Parasitic Electric Load {W}
-    PLFCurveforUnitarySystem,    !- Part load fraction correlation (function of part load ratio)
-    10;                          !- Parasitic Gas Load {W}
-
-
-Curve:Cubic,
-    PLFCurveforUnitarySystem,  !- Name
-    0.8,  !- Coefficient1 Constant
-    0.2,  !- Coefficient2 x
-    0.0,  !- Coefficient3 x**2
-    0.0,  !- Coefficient4 x**3
-    0,  !- Minimum Value of x
-    1;  !- Maximum Value of x
-
-
-Fan:OnOff,
-    Supply Fan 1,          !- Fan Name
-    FanAndCoilAvailSched,  !- Availability Schedule Name
-    0.7,    !- Fan Total Efficiency
-    600.0,  !- Delta Pressure {Pa}
-    1.3,    !- Max Flow Rate {m3/s}
-    0.9,    !- Motor Efficiency
-    1.0,    !- Motor In Airstream Fraction
-    Air Loop Inlet Node,          !- Fan_Inlet_Node
-    Heating Coil Air Inlet Node;  !- Fan_Outlet_Node
-
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone1DirectAir,       !-Direct Air Name
-    FanAndCoilAvailSched, !- Schedule name for on/off schedule
-    Zone 1 Inlet Node,    !- Zone Supply Air Node Name
-   0.47;   !- Maximum air flow rate {m3/s}
-
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone2DirectAir,       !- Direct Air Name
-   FanAndCoilAvailSched, !- Schedule name for on/off schedule
-    Zone 2 Inlet Node,    !- Zone Supply Air Node Name
-   0.36;   !- Maximum air flow rate {m3/s}
-
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone3DirectAir,       !- Direct Air Name
-   FanAndCoilAvailSched, !- Schedule name for on/off schedule
-    Zone 3 Inlet Node,    !- Zone Supply Air Node Name
-   0.47;   !- Maximum air flow rate {m3/s}
-```
-
-Example of Heat-Only Unitary System Specification
-
-### Unitary Heat Only (AirLoopHVAC) Outputs
-
-* HVAC,Average,Unitary System Fan Part Load Ratio []
-
-#### Unitary System Fan Part Load Ratio []
-
-This output variable is the ratio of actual air mass flow rate through the unitary system to the unitary system’s design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the unitary system is available (based on the availability schedule). For cycling fan/cycling coil operation mode, the actual air mass flow rate is calculated based on the ratio of the sensible heating load to the unitary system heating capacity. For the cycling fan mode, the runtime fraction for the unitary system fan may be different from the fan part-load ratio reported here due the part-load performance of the unitary system’s heating coil (delay at start-up to reach steady-state heating output). In general, runtime fractions are reported by individual components where appropriate (e.g., Fan:OnOff).
-
-### AirLoopHVAC:UnitaryHeatPump:WaterToAir
-
-The unitary water-to-air heat pump is similar to the unitary air-to-air heat pump except water is used on the source side. Links to the fan, WaterToAirHeatPump cooling coil, WaterToAirHeatPump heating coil, and supplementary heating coil specifications are provided in the heat pump’s input data syntax. The heat pump switches between cooling and heating depending on the zone’s demand. The load side (air) of the unitary water-to-air heat pump consists of an On/Off fan component, a WaterToAirHeatPump cooling coil component, a WaterToAirHeatPump heating coil component, and a Gas, Electric, Steam, or Hot Water supplemental heating coil component. The source side (water) of the heat pump is connected to a condenser loop with a heat exchanger (ground heat exchanger or other type) or a plant loop with a heating source such as a boiler and a cooling source such as a chiller or cooling tower. The diagram below shows the setup and connection of the heat pump for the source side and load side for a ground heat exchanger configuration. Note that on the load side, the WaterToAirHeatPump cooling coil must always be placed before the WaterToAirHeatPump heating coil.
-
-There are three type of WaterToAirHeatPump coil models available:
-
-* Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
-
-* Coil:Heating:WaterToAirHeatPump:ParameterEstimation
-
-* Coil:Cooling:WaterToAirHeatPump:EquationFit
-
-* Coil:Heating:WaterToAirHeatPump:EquationFit
-
-* Coil:Cooling:WatertoAirHeatPump:VariableSpeedEquationFit
-
-* Coil:Heating:WatertoAirHeatPump:VariableSpeedEquationFit
-
-![FurnaceSchematic\_WSHP](media/image304.png)
-
-Figure 122. Water to Air Heat Pump Schematic for a BlowThrough Configuration with Ground Heat Exchanger
-
-In addition, the control zone name and the system design operating conditions are specified by the heat pump inputs.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the unitary system heat pump.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name (ref. Schedule objects) that contains information on the availability of the heat pump to operate. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the name of the HVAC system node from which the heat pump draws its inlet air.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the name of the HVAC system node to which the heat pump sends its outlet air.
-
-#### Field: Supply Air Flow Rate
-
-This numeric field contains the design volumetric flow rate through the heat pump in cubic meters per second. This volume flow rate is only used when the cooling and heating coil object type is Coil:\*:WaterToAirHeatPump:ParameterEstimation. Although a value greater than 0 is required (input cannot be blank or 0), this input is not used for the EquationFit model. Instead, the supply air flow rate is determined by the input in the corresponding Coil:\*:WaterToAirHeatPump:EquationFit objects.
-
-#### Field: Controlling Zone or Thermostat Location
-
-This alpha field contains the identifying zone name where the thermostat controlling the heat pump is located.
-
-#### Field: Supply Air Fan Object Type
-
-This alpha field contains the identifying type of supply air fan specified in the heat pump. Fan type must be Fan:OnOff.
-
-#### Field: Supply Air Fan Name
-
-This alpha field contains the identifying name given to the heat pump supply air fan, and should match the name specified in the corresponding fan object.
-
-#### Field: Heating Coil Object Type
-
-This alpha field contains the identifying type of heating coil specified in the heat pump. Heating coil types are:
-
-* Coil:Heating:WaterToAirHeatPump:ParameterEstimation
-
-* Coil:Heating:WaterToAirHeatPump:EquationFit
-
-* Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit
-
-#### Field: Heating Coil Name
-
-This alpha field contains the identifying name given to the WaterToAirHeatPump heating coil, and should match the name specified in the corresponding WaterToAirHeatPump heating coil object.
-
-#### Field: Heating Convergence
-
-This numeric value allows the user to determine how close the air side has to be controlled. Lower the value of convergence better the control of air side conditions and less the zone temperature fluctuations. However in a poorly designed system, a lower convergence might result in warning errors which are caused due to the iteration limit for run time fraction calculation is limited to 20.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field contains the identifying type of cooling coil specified in the heat pump. Cooling coil types are:
-
-* Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
-
-* Coil:Cooling:WaterToAirHeatPump:EquationFit
-
-* Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit
-
-#### Field: Cooling Coil Name
-
-This alpha field contains the identifying name given to the WaterToAirHeatPump cooling coil, and should match the name specified in the corresponding WaterToAirHeatPump cooling coil object.
-
-#### Field: Cooling Convergence
-
-This numeric value allows the user to determine how close the air side has to be controlled. Lower the value of convergence better the control of air side conditions and less the zone temperature fluctuations. However in a poorly designed system, a lower convergence might result in warning errors which are caused due to the iteration limit for run time fraction calculation is limited to 20.
-
-#### Field: Maximum Cycling Rate
-
-This numeric field contains the maximum on-off cycling rate for the compressor, which occurs at 50% run time fraction. Suggested values are shown below (Henderson et al. 1999):
-
-![](media/image305.svg)
-
-#### Field: Heat Pump Time Constant
-
-This numeric field contains the time constant for the cooling coil's capacity to reach steady state after startup. Suggested values are shown below (Henderson et al. 1999):
-
-![](media/image306.svg)
-
-#### Field: Fraction of On-Cycle Power Use
-
-This numeric field contains the fraction of on-cycle power use to adjust the part load fraction based on the off-cycle power consumption due to crankcase heaters, controls, fans, and etc. Suggested value values are below (Henderson et al. 1999):
-
-![](media/image307.svg)
-
-#### Field: Heat Pump Fan Delay Time
-
-This numeric field contains the time delay for the heat pump supply air fan to shut off after the compressor cycles off in seconds. This value can be obtained from the manufacturer or the heat pump catalog. Enter a value of zero when the heat pump’s fan operating mode is continuous. Suggested value is 60 seconds.
-
-#### Field: Supplemental Heating Coil Object Type
-
-This is the object type of the supplemental heating coil. The hot water and steam heating coils require specifying plant loop, branches, and connectors objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the supplemental heating coil does not require additional controller or Controller:WaterCoil object. The parent object (AirLoop Unitary Water to Air Heat Pump) itself provides the "controller" function of modulating water flow. The valid choices are:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Supplemental Heating Coil Name
-
-This alpha field contains the identifying name given to the supplemental heating coil, and should match the name specified in the corresponding supplemental heating coil object.
-
-#### Field: Maximum Supply Air Temperature from Supplemental Heater
-
-This numeric field defines the maximum allowed supply air temperature exiting the heat pump supplemental heating coil in degrees Celsius.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation
-
-This numeric field defines the outdoor air dry-bulb temperature in degrees Celsius above which the heat pump supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21°C. If this input field is left blank, the default value is 21°C.
-
-#### Field: Outdoor Dry-Bulb Temperature Sensor Node Name
-
-This alpha field specifies the name of the outdoor node which controls the operation of the supplemental heating coil. If this field is left blank, the outdoor temperature is based solely on the weather data. If this field is not blank, the node name specified must also be listed in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor temperature from the weather data. Alternately, the node name must be specified in an OutdoorAir:NodeList object where the outdoor temperature is taken directly from the weather data.
-
-#### Field: Fan Placement
-
-This alpha field has two choices: **BlowThrough** or **DrawThrough**. The first choice represents a blow through system where the supply air fan is before the WaterToAirHeatPump cooling/heating coil and the supplementary heating coil. The second choice represents a draw through system where the supply fan is between the WaterToAirHeatPump cooling/heating coil and the supplementary heating coil. If this input field is left blank, the default is blow through.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This alpha field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating/cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply air fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, the model assumes the supply air fan cycles with the heating or cooling coil throughout the simulation period.
-
-As shown in the example below, correct specification of the water-to-air heat pump requires specification of the following objects in addition to the AirLoopHVAC:UnitaryHeatPump:WaterToAir object:
-
-- On/Off fan
-
-- WaterToAirHeatPump cooling coil
-
-- WaterToAirHeatPump heating coil
-
-- Supplementary heating coil
-
-- Direct air unit for each zone served by the heat pump
-
-- Condenser demand branches
-
-It should be noted that the volumetric air flow rate specified in the direct air unit for the controlling zone should properly reflect the fractional volumetric air flow rate specified in the heat pump object.
-
-#### Field: Dehumidification Control Type
-
-This alpha input field contains the type of dehumidification control. The following options are valid for this field:
-
-**None** - meet sensible load only, no active dehumidification control
-
-**CoolReheat** - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. The excess cooling beyond the cooling set point temperature is offset by the supplemental heating coil.
-
-The default is **None**. For **CoolReheat** dehumidification control modes, the maximum humidity setpoint is required. This must be set using a **ZoneControl:Humidistat** object. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate. Supplemental heating coil (supplemental heating coil type and name) is a required input in WaterToAir HeatPumps. When dehumidification control is active the heating and the reheat load due to extra dehumidification are met with supplemetal heating coil. The supplemental heating coil capacity must be adequate enough to meet the heating coil load and offset the excess cooling load due to  extra dehumidification. The dehumidification control type CoolReheat works only with Coil:Cooling:WaterToAirHeatPump:EquationFit cooling coil type.
-
-#### Field: Heat Pump Coil Water Flow Mode
-
-This field specifies the way in which water flow through the heat pump coils will be modeled.  This field is only used when WatertoAirHeatPump:EquationFit coils are used. There are three options:
-
-- Cycling
-
-- Constant
-
-- CyclingOnDemand
-
-**Cycling** varies water flow through the coil based on the heat pump Part Load Ratio.  This control method is appropriate for modeling heat pumps that are outfitted with a soleniod valve which allows water to flow through the coil only when the compressor is active. This is the default for EnergyPlus V8 and later.
-
-**Constant** provides a constant water flow regardless of heat pump operation.  Remember that EnergyPlus has two coils (a heating coil and a cooling coil) to approximate the operation of one coil that can operate in either heating mode or cooling mode.  Therefore, when the water flow mode is constant, there will be full flow through either the heating coil or the cooling coil, but not both at the same time.
-
-**ConstantOnDemand** provides full flow through the coil whenever there is a load.  When there is no load, there is zero flow through the coil.  This control strategy represents the way EnergyPlus modeled heat pump water flow prior to Version 8.
-
-
-
-Following is an example of IDF usage:
-```idf
-AirLoopHVAC:UnitaryHeatPump:WaterToAir,
-    DXAC Heat Pump 1,        !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    Mixed Air Node,          !- Air Inlet Node Name
-    Air Loop Outlet Node,    !- Air Outlet Node Name
-    2,                       !- Supply Air Flow Fate {m3/s}
-    East Zone,               !- Controlling Zone or Thermostat Location
-    Fan:OnOff,        !- Supply Air Fan Object Type
-    Supply Fan 1,            !- Supply Air Fan Name
-    Coil:Heating:WaterToAirHeatPump:ParameterEstimation,  !- Heating Coil Object Type
-    Heat Pump Heating Mode,  !- Heating Coil Name
-    0.001,                   !- Heating Convergence
-    Coil:Cooling:WaterToAirHeatPump:ParameterEstimation,  !- Cooling Coil Object Type
-    Heat Pump Cooling Mode,  !- Cooling Coil Name
-    0.001,                   !- Cooling Convergence
-    2.5, !- Maximum Cycling Rate {cycles/hr}
-    60, !- Heat Pump Time Constant {s}
-    0.01, !- Fraction of On-Cycle Power Use
-    60,    !- Heat Pump Fan Delay Time {s}
-    Coil:Heating:Gas,        !- Supplemental Heating Coil Object Type
-    Heat Pump DX Supp Heating Coil 1,  !- Supplemental Heating Coil Name
-    50,                      !- Maximum Supply Air Temperature from Supplemental Heater {C}
-    21,                      !- Maximum Outdoor Dry-Bulb Temperature for Supplemental Heater Operation {C}
-    Outside Air Inlet Node, !- Outdoor Dry-Bulb Temperature Sensor Node Name
-    BlowThrough,             !- Fan Placement
-    CyclingFanSch,           !- Supply Air Fan Operating Mode Schedule Name
-    CoolReheat;              !- Dehumidification Control Type
-
-
-Schedule:Compact,
-    CyclingFanSch,           !- Name
-    Fraction,                !- Schedule Type Limits Name
-    Through: 12/31,          !- Field 1
-    For: AllDays,            !- Field 2
-    Until: 24:00,            !- Field 3
-    0.0;                     !- Field 4
-
-
-
-
-  Coil:Cooling:WaterToAirHeatPump:ParameterEstimation,
-    Heat Pump Cooling Mode,  !- Name
-    Scroll,                !- Compressor Type
-    R22,                   !- Refrigerant Type
-    0.0015,                  !- Design Source Side Flow Rate {m3/s}
-    38000,  !- Nominal Cooling Coil Capacity {W)
-    0,            !- Nominal Time for Condensate Removal to Begin {s}
-    0,      !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity
-    3000000,                 !- High Pressure CutOff {Pa}
-    0,                       !- Low Pressure CutOff {Pa}
-    Water to Air Heat Pump Source Side1 Inlet Node,  !- Water Inlet Node Name
-    Water to Air Heat Pump Source Side1 Outlet Node,  !- Water Outlet Node Name
-    Cooling Coil Air Inlet Node,  !- Air Inlet Node Name
-    Heating Coil Air Inlet Node,  !- Air Outlet Node Name
-    3.78019E+03,!-Parameter 1 {W/K}
-    2.80303E+03,!- Parameter 2 {W/K}
-   7.93591E-01,!- Parameter 3 {C}
-    1.91029E+03,!- Parameter 4 {W}
-    2.66127E+00,!- Parameter 5
-    1.06009E-02,!- Parameter 6
-    1.65103E+00,!- Parameter 7
-    9.73887E-03,!- Parameter 8
-    1.04563E+03;!- Parameter 9
-
-
-
-
- Coil:Heating:WaterToAirHeatPump:ParameterEstimation,
-    Heat Pump HEATING Mode,  !- Name
-    Scroll,                !- Compressor Type
-    R22,                   !- Refrigerant Type
-    0.0015,                  !- Design Source Side Flow Rate {m3/s}
-    38000,                   !- Nominal Heating Coil Capacity {W}
-    3000000,                 !- High Pressure CutOff
-    0,                       !- Low Pressure CutOff {Pa}
-    Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
-    Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
-    Heating Coil Air Inlet Node,  !- Air Inlet Node Name
-    SuppHeating Coil Air Inlet Node,  !- Air Outlet Node Name
-    3.91379E+03,  !-Parameter 1 {W/K}
-   5.94753E-01,  !- Parameter 2 {C}
-    2.49945E+03,  !- Parameter 3 {W}
-    8.68734E-01,  !- Parameter 4
-    7.23595E-03,  !- Parameter 5
-    3.69126E+00,  !- Parameter 6
-    1.75701E-05,  !- Parameter 7
-   3.65348E+03;  !-Parameter 8
-
-
-
-
-  Coil:Heating:Gas,
-    Heat Pump DX Supp Heating Coil 1,  !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    0.8,                     !- Gas Burner Efficiency
-    32000,                   !- Nominal Capacity {W}
-    SuppHeating Coil Air Inlet Node,  !- Air Inlet Node Name
-    Air Loop Outlet Node;    !- Air Outlet Node Name
-
-
-
-
-  BRANCH,
-    Gshp Cooling Condenser Branch,  !- Name
-    0,  !- Maximum Flow Rate {m3/s}
-     , !- Pressure Drop Curve Name
-    Coil:Cooling:WaterToAirHeatPump:ParameterEstimation,  !- Component 1 Object Type
-    Heat Pump Cooling Mode,  !- Component 1 Name
-    Water to Air Heat Pump Source Side1 Inlet Node, !- Component 1 Inlet Node Name
-    Water to Air Heat Pump Source Side1 Outlet Node, !- Component 1 Outlet Node Name
-    ACTIVE;  !- Component 1 Branch Control Type
-
-
-  BRANCH,
-    Gshp Heating Condenser Branch,  !- Name
-    0,  !- Maximum Flow Rate {m3/s}
-     , !- Pressure Drop Curve Name
-    Coil:Heating:WaterToAirHeatPump:ParameterEstimation,  !- Component 1 Object Type
-    Heat Pump Heating Mode,  !- Component 1 Name
-    Water to Air Heat Pump Source Side2 Inlet Node,  !- Component 1 Inlet Node Name
-    Water to Air Heat Pump Source Side2 Outlet Node,  !- Component 1 Outlet Node Name
-    ACTIVE;  !- Component 1 Branch Control Type
-
-
-
-
-  Fan:OnOff,
-    Supply Fan 1,          !- Name
-    FanAndCoilAvailSched,  !- Availability Schedule Name
-    0.7,                   !- FanTotal Efficiency
-    300.0,                 !– Pressure Rise {Pa}
-    2.0,                   !- Maximum Flow Rate {m3/s}
-    0.9,                   !- Motor Efficiency
-    1.0,                   !- Motor In Airstream Fraction
-    Mixed Air Node,        !- Air Inlet_Node Name
-    Cooling Coil Air Inlet Node;  !- Air Outlet Node Name
-
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone1DirectAir,        !- Name
-    FanAndCoilAvailSched,  !- Availability Schedule Name
-   Zone 1 Inlet Node,     !- Zone Supply Air Node Name
-   0.7;                   !- Maximum Air Flow Rate {m3/s}
-
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone2DirectAir,        !- Name
-    FanAndCoilAvailSched,  !- Availability Schedule Name
-   Zone 2 Inlet Node,     !- Zone Supply Air Node Name
-   0.6;                   !- Maximum Air Flow Rate {m3/s}
-
-
-  AirTerminal:SingleDuct:Uncontrolled,
-    Zone3DirectAir,        !- Name
-    FanAndCoilAvailSched,  !- Availability Schedule Name
-   Zone 3 Inlet Node,     !- Zone Supply Air Node Name
-   0.7;                   !- Maximum Air Flow Rate {m3/s}
-```
-
-
-
-### Unitary Water to Air Heat Pump (AirLoopHVAC) Outputs
-
-Energy use reporting for the water-to-air heat pump is documented under the heat pump coil object types:
-
-* Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
-
-* Coil:Heating:WaterToAirHeatPump:ParameterEstimation
-
-* Coil:Cooling:WaterToAirHeatPump:EquationFit
-
-* Coil:Heating:WaterToAirHeatPump:EquationFit
-
-
-
-The heat pump *demand* as well as the compressor and fan part-load ratios may be obtained with the output variables shown below.
-
-* HVAC,Average, Unitary System Requested Sensible Cooling Rate [W]
-
-* HVAC,Average, Unitary System Requested Latent Cooling Rate [W]
-
-* HVAC,Average, Unitary System Requested Heating Rate [W]
-
-* HVAC,Average, Unitary System Compressor Part Load Ratio []
-
-* HVAC,Average, Unitary System Fan Part Load Ratio
-
-* HVAC,Average, Unitary System Dehumidification Induced Heating Demand Rate [W]
-
-
-
-#### Unitary System Requested Sensible Cooling Rate [W]
-
-This output variable is the sensible cooling requested from the zone thermostat in watts. This value is calculated using the unitary heat pump outlet air and zone conditions, the specific heat of the zone air, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Unitary System Requested Latent Cooling Rate [W]
-
-This output variable is the latent cooling requested from the zone humidistat in watts. This value is calculated using the unitary heat pump outlet air and zone conditions, the heat of vaporization of water at the current zone conditions, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Unitary System Requested Heating Rate [W]
-
-This output variable is the sensible heating requested from the zone thermostat in watts. This value is calculated using the unitary heat pump outlet air and zone conditions, the specific heat of the zone air, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Unitary System Compressor Part Load Ratio []
-
-This output variable is the ratio of actual load on the unitary system to the unitary system’s steady state output.  This ratio is based on the nominal capacity of the unit.
-
-#### Unitary System Fan Part Load Ratio []
-
-This output variable is the ratio of actual air mass flow rate through the unitary system to the unitary system’s design air mass flow rate (i.e., design volumetric flow rate converted to dry air mass flow rate). For continuous fan operation mode, this variable is always 1.0 when the unitary system is available (based on the availability schedule).
-
-#### Unitary System Dehumidification Induced Heating Demand Rate [W]
-
-This output variable is the additional heating demand rate of the supplemental heating coil of a Water-to-Air heat pumps in Watts.  This additional heating demand is induced when zone air overshoots the heating setpoint due to extra dehumidification requirement to meet the high humidity setpoint. This value is always positive. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
-
-### AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass
-
-The changeover-bypass variable air volume (CBVAV) unitary system is a compound object made up of other components. Each CBVAV system consists of an outdoor air mixer, direct expansion (DX) cooling coil, heating coil, and a supply air fan as shown in the figures below. Zone thermostats and terminal units are required in each zone served by this system. The terminal units are specific to this system type and are either AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat or AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat. A zone humidistat and single zone max humidity set point manager may also be specified to help control high humidity levels. These individual components are described elsewhere in this document. The CBVAV unitary system object coordinates the operation of these components and is modeled as a type of air loop equipment (Ref. AirLoopHVAC).
-
-![DrawthruCBVAV](media/image308.png)
-
-Figure 123. Schematic of a CBVAV unitary system (draw through fan placement)
-
-![BlowthruCBVAV](media/image309.png)
-
-Figure 124. Schematic of a CBVAV unitary system (blow through fan placement)
-
-Links to the CBVAV system’s supply air fan, coils, and outdoor air mixer specifications are provided in the object’s input syntax. Additional inputs include system and outdoor air flow rates during heating and cooling operation, the priority control mode, and dehumidification control type. A description of each input field for the CBVAV unitary system compound object is provided below.
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a changeover-bypass VAV system. Any reference to this system by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the system operates during a given time period. A schedule value equal to 0 denotes that the system must be off for that time period, and a schedule value greater than 0 denotes that the system is available to operate during that time period. This schedule may be used to completely disable the system (all of its coils and the supply air fan) as required. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Cooling Supply Air Flow Rate
-
-This numeric field defines the air flow rate through the system (i.e., through the fan and heating/cooling coils) in cubic meters per second when the DX cooling coil is operating. Values must be greater than 0, or this field is autosizable.
-
-#### Field: Heating Supply Air Flow Rate
-
-This numeric field defines the air flow rate through the system (i.e., through the fan and heating/cooling coils) in cubic meters per second when the heating coil is operating. Values must be greater than 0, or this field is autosizable.
-
-#### Field: No Load Supply Air Flow Rate
-
-This numeric field defines the air flow rate through the system (i.e., through the fan and heating/cooling coils) in cubic meters per second when neither cooling nor heating is required (i.e., the DX cooling coil and heating coil are off but the supply air fan operates). Values must be greater than or equal to zero, or this field is autosizable. This field is only used when the unitary system’s supply air fan operating mode is specified as continuous fan operation (Ref. Field: Supply air fan operating mode schedule name). If the system’s supply air fan operating mode is specified as continuous fan operation and this value is set to zero or the field is left blank, then the model assumes that the system air flow rate when no heating/cooling is needed is equal to the system air flow rate when the coils were last operating (for cooling operation or heating operation).
-
-#### Field: Cooling Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air flow rate through the system (i.e., through the Outdoor air Mixer’s Outside\_Air\_Stream\_Node) in cubic meters per second when the DX cooling coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Cooling Outdoor Air Flow Rate can be changed during the simulation using a multiplier schedule (Ref. Field: Outdoor air volumetric flow rate multiplier schedule name). For any simulation timestep, the Cooling Outdoor Air Flow Rate cannot exceed the system air volumetric flow rate during cooling operation.
-
-#### Field: Heating Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air flow rate through the system (i.e., through the Outdoor air Mixer’s Outside\_Air\_Stream\_Node) in cubic meters per second when the heating coil is operating. Values must be greater than or equal to 0, or this field is autosizable. Note that the Heating Outdoor Air Flow Rate can be changed during the simulation using a multiplier schedule (Ref. Field: Outdoor air volumetric flow rate multiplier schedule name). For any simulation timestep, the Heating Outdoor Air Flow Rate cannot exceed the system air volumetric flow rate during heating operation.
-
-#### Field: No Load Outdoor Air Flow Rate When No Cooling or Heating is Needed
-
-This numeric field defines the outdoor air flow rate through the system (i.e., through the Outdoor air Mixer's Outside_Air_Stream_Node) in cubic meters per second when neither cooling nor heating is required (i.e., the DX cooling coil and heating coil are off but the supply air fan operates). Values must be greater than or equal to 0, or this field is autosizable. Note that the no load outdoor air flow rate can be changed during the simulation using a multiplier schedule (Ref. Field: Outdoor air volumetric flow rate multiplier schedule name). For any simulation timestep, the no load outdoor air flow rate cannot exceed the no load supply air flow rate. This field is only used when the unitary system's supply air fan operating mode is specified as continuous fan operation (Ref. Field: Supply air fan operating mode schedule name). If the system's supply air fan operating mode is specified as continuous fan operation and this value is set to zero or the field is left blank, then the model assumes that the no load outdoor air flow rate is equal to the outdoor air flow rate when the coils were last operating (for cooling operation [i.e. Cooling outdoor air flow rate] or heating operation [i.e. Heating outdoor air flow rate]) and this field is not used.
-
-#### Field: Outdoor Air Flow Rate Multiplier Schedule Name
-
-This alpha field defines the name of a schedule (ref: Schedule) that contains multipliers for the outdoor air volume flow rates (heating, cooling, no heating/cooling). Schedule values must be from zero to 1. If this field is left blank, then the model assumes that the outdoor air multiplier is 1 for the entire simulation period.
-
-#### Field: Air Inlet Node Name
-
-This alpha field defines the name of the HVAC system node from which the system draws its inlet air.
-
-#### Field: Bypass Duct Mixer Node Name
-
-This alpha field defines the name of the HVAC system node where the bypass air mixes with the unitary system's inlet air. This name should match the name of the Return Air Stream Node Name for the OutdoorAir:Mixer associated with this system. This node name must be different from the system’s air inlet node name.
-
-#### Field: Bypass Duct Splitter Node Name
-
-This alpha field defines the name of the HVAC system node where the conditioned air is split into bypass air and supply air leaving the system (e.g., delivered to the terminal units). This splitter air node name should match the outlet node name for the last component (furthest downstream) in this unitary system. For blow through fan placement, the splitter air node is the outlet node of the heating coil. For draw through fan placement, the splitter node is the outlet node of the supply air fan.
-
-#### Field: Air Outlet Node Name
-
-This alpha field defines the name of the HVAC system node to which the system sends its outlet air.
-
-#### Field: Outdoor Air Mixer Object Type
-
-This field specifies the type of outdoor air mixer used by this CBVAV unitary system. The outdoor air mixer component is part of the CBVAV unitary compound object. The only available outdoor air mixer type is:
-
-* OutdoorAir:Mixer
-
-#### Field: Outdoor Air Mixer Name
-
-This alpha field defines the name of an outdoor air mixer component that composes part of the CBVAV system. The name of the outdoor air mixer’s Return\_Air\_Stream\_Node should match the bypass duct mixer node name, and be different from the CBVAV system’s air inlet node name. The Mixed Air Node Name of the outdoor air mixer should be the same as the CBVAV system’s supply fan inlet air node (for blow through fan placement) or the system’s DX cooling coil inlet node (for draw through fan placement).
-
-#### Field: Supply Air Fan Object Type
-
-This alpha field defines the type of fan used by this unitary system. The only valid choices are **Fan:OnOff** and **Fan:ConstantVolume**. The input requirements for these fan objects are described elsewhere in this document.
-
-#### Field: Supply Air Fan Name
-
-This alpha field defines the name of the fan component that composes part of this unitary system. Note that the fan component’s maximum flow rate should be greater than or equal to the largest system air volumetric flow rate specified for this unitary system (heating, cooling, and no heating/cooling). In addition, the fan’s inlet air node should be the same as the outdoor air mixer’s Mixed Air Node (for blow through fan placement) or the heating coil’s outlet node (for draw through fan placement). The fan outlet air node should be the same as the DX cooling coil’s air inlet node (for blow through fan placement) or the system’s bypass duct splitter node (for draw through fan placement).
-
-#### Field: Supply Air Fan Placement
-
-This alpha field defines the placement of the supply air fan within this unitary system. The only valid choices are **BlowThrough** and **DrawThrough**. With blow through placement, the supply air fan is located immediately upstream of the system’s cooling coil. With draw through placement, the supply air fan is located immediately downstream of the heating coil.
-
-#### Field: Supply Air Fan Operating Mode Schedule Name
-
-This alpha field defines the name of a schedule that specifies the supply air fan operating mode during the simulation. A schedule value of 0 denotes the fan cycles off when no cooling or heating is required, and any other value denotes that the fan runs continuously regardless of the need for heating or cooling. If this field is left blank, the model assumes continuous supply air fan operation for the entire simulation period.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field defines the type of cooling coil used by this unitary system. There are three valid choices for this field:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* CoilSystem:Cooling:DX:HeatExchangerAssisted
-
-* Coil:Cooling:DX:TwoStageWithHumidityControlMode
-
-The input requirements for these cooling coil objects are described elsewhere in this document.
-
-#### Field: Cooling Coil Name
-
-This alpha field defines the name of the cooling coil used by this unitary system, and this name should match the name specified in the corresponding cooling coil object.
-
-#### Field: Heating Coil Object Type
-
-This alpha field defines the type of heating coil used by this unitary system. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the heating coil does not require additional controller or Controller:WaterCoil object. The parent object (CBVAV Unitary System) itself provides the "controller" function of modulating water flow. The valid choices are:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:DX:SingleSpeed
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-The input requirements for these heating coil objects are described elsewhere in this document.
-
-#### Field: Heating Coil Name
-
-This alpha field defines the name of the heating coil used by this unitary system, and this name should match the name specified in the corresponding heating coil object.
-
-#### Field: Priority Control Mode
-
-This choice field defines the cooling or heating priority control mode for the unitary system. Valid choices are:
-
-* CoolingPriority
-
-* HeatingPriority
-
-* ZonePriority
-
-If CoolingPriority is selected, the system operates to meet the cooling load if any zone served by this system (air loop) requires cooling. If no zones require cooling, then the system operates in heating mode if needed. If HeatingPriority is selected, the system operates to meet the heating load if any zone requires heating. If no zones require heating, then the system operates in cooling mode if needed. If ZonePriority is selected, the system operates based on the maximum number of zones requiring either heating or cooling. If the number of zones requiring cooling is greater than the number of zones requiring heating, then the system operates in cooling mode. If the number of zones requiring heating is greater than the number of zones requiring cooling, then the system operates in heating mode. If the number of zones requiring cooling equals the number of zones requiring heating, then the largest combined load (i.e., the sum of the cooling loads for zones requiring cooling compared to the sum of the heating loads for zones that require heating) sets the cooling or heating operating mode for the system during that simulation timestep.
-
-#### Field: Minimum Outlet Air Temperature During Cooling Operation
-
-This numeric field defines the minimum outlet air temperature leaving the system when the unit is operating to provide cooling. Values are specified in degrees Celsius and must be greater than 0. The default value is 8°C. This value must be less than or equal to the maximum outlet air temperature during heating operation.
-
-#### Field: Maximum Outlet Air Temperature During Heating Operation
-
-This numeric field defines the maximum outlet air temperature leaving the system when the unit is operating to provide heating. Values are specified in degrees Celsius and must be greater than 0. The default value is 50°C. This value must be greater than or equal to the minimum outlet air temperature during cooing operation.
-
-#### Field: Dehumidification Control Type
-
-This alpha field contains the type of dehumidification control. The following options are valid for this field:
-
-**None** - meet sensible load only, no active dehumidification control
-
-**Multimode** - activate enhanced dehumidification mode as needed and meet sensible load. This option is used to model DX equipment with a controllable heat exchanger assisting the DX cooling coil for improved dehumidification. It is valid only with cooling coil type = Coil:Cooling:DX:TwoStageWithHumidityControlMode.
-
-**CoolReheat** - cool beyond the dry-bulb temperature set point as required to meet the high humidity setpoint. It is valid only with cooling coil type = Coil:Cooling:DX:TwoStageWithHumidityControlMode.
-
-The default is **None**. For the other dehumidification control modes, the maximum humidity setpoint on the CBVAV system’s air outlet node is used. This must be set using a **ZoneControl:Humidistat** and one of:
-
-- **SetpointManager:SingleZone:Humidity:Maximum**
-
-- **SetpointManager:MultiZone:Humidity:Maximum**
-
-- **SetpointManager:MultiZone:MaximumHumidity:Average**
-
-objects. When extra dehumidification is required, the system may not be able to meet the humidity setpoint if its full capacity is not adequate.
-
-As shown in the example below, correct specification of the CBVAV unitary system requires specification of the following objects in addition to the AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass object:
-
-1)   outdoor air mixer (OutdoorAir:Mixer)
-
-2)   fan (Fan:OnOff or Fan:ConstantVolume)
-
-3)   cooling coil (Coil:Cooling:DX:SingleSpeed, CoilSystem:Cooling:DX:HeatExchangerAssisted, or Coil:Cooling:DX:TwoStageWithHumidityControlMode)
-
-4)   heating coil (Coil:Heating:Gas, Coil:Heating:Electric, or Coil:Heating:DX:SingleSpeed)
-
-5)   terminal unit for each zone being served by this system (AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat or AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat)
-
-Note: The fan, heating coil, cooling coil, and outdoor air mixer must be connected in the air loop according to the configurations shown above (Figure 123 and Figure 124).
-
-```idf
-AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass,
-    GasHeat CBVAV System,  !- Name of unitary system
-    FanAndCoilAvailSched,  !- Availability schedule name
-    1.8,                   !- Cooling Supply Air Flow Rate {m3/s}
-    1.7,                   !- Heating Supply Air Flow Rate {m3/s}
-    1.6,                   !- No Load Supply Air Flow Rate {m3/s}
-    0.32,                  !- Cooling Outdoor Air Flow Rate {m3/s}
-    0.3,                   !- Heating Outdoor Air Flow Rate {m3/s}
-    0.27,                  !- No Load Outdoor Air Flow Rate {m3/s}
-    Outdoor Air Multiplier Schedule, !- Outdoor air volumetric flow rate multiplier schedule name
-    Air Loop Inlet Node,     !- Air inlet node name
-    Mixer Inlet Node,        !- Bypass duct mixer node name
-    Heating Coil Air Outlet Node,    !- Bypass duct splitter node name
-    Air Loop Outlet Node,    !- Air outlet node name
-    OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type
-    Outdoor air Mixer,       !- Outdoor air mixer name
-    Fan:OnOff,        !- Supply air fan type
-    Supply Fan 1,            !- Supply air fan name
-    BlowThrough,            !- Supply air fan placement
-    Fan OpMode Schedule,     !- Supply air fan operating mode schedule name
-    Coil:Cooling:DX:TwoStageWithHumidityControlMode,  !- Cooling coil type
-    ACDXCoil 2,              !- Cooling coil name
-    Coil:Heating:Gas,        !- Heating coil type
-    Furnace Heating Coil 1,  !- Heating coil name
-    CoolingPriority,        !- Priority control mode
-    10.0,                    !- Minimum outlet air temperature during cooling operation {C}
-    50.0,                    !- Maximum outlet air temperature during heating operation {C}
-    None;                    !- Dehumidification control type
-
-OutdoorAir:Mixer,
-    Outdoor air Mixer,       !- Name
-    Mixed Air Node,          !- Mixed Air Node Name
-    Outdoor air Inlet Node,  !- Outdoor Air Stream Node
-    Relief Air Outlet Node,  !- Relief Air Stream Node Name
-    Mixer Inlet Node;        !- Return Air Stream Node Name
-
-Fan:OnOff,
-    Supply Fan 1,            !- Fan Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    0.7,                     !- Fan Total Efficiency
-    600.0,                   !- Delta Pressure {Pa}
-    1.8,                     !- Max Flow Rate {m3/s}
-    0.9,                     !- Motor Efficiency
-    1.0,                     !- Motor In Airstream Fraction
-    Mixed Air Node,          !- Fan\_Inlet\_Node
-    DX Cooling Coil Air Inlet Node;  !- Fan\_Outlet\_Node
-
-Coil:Cooling:DX:TwoStageWithHumidityControlMode,
-    ACDXCoil 2,              !- Coil Name
-    FanAndCoilAvailSched,    !- Availability Schedule
-    DX Cooling Coil Air Inlet Node, !- Coil Air Inlet Node
-    Heating Coil Air Inlet Node,    !- Coil Air Outlet Node
-    ,                        !- Crankcase Heater Capacity {W}
-    ,                        !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
-    2,                       !- Number of Capacity Stages
-    0,                       !- Number of Enhanced Dehumidification Modes
-    CoilPerformance:DX:Cooling,  !- Normal Mode Stage 1 Coil Performance Object Type
-    ACDXCoil 2 Standard Mode-Stage 1,  !- Normal Mode Stage 1 Coil Performance Object Name
-    CoilPerformance:DX:Cooling,  !- Normal Mode Stage 1+2 Coil Performance Object Type
-    ACDXCoil 2 Standard Mode-Stage 1&2;  !- Normal Mode Stage 1+2 Coil Performance Object Name
-
-Coil:Heating:Gas,
-    Furnace Heating Coil 1,  !- Coil Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    0.8,                     !- Gas Burner Efficiency of the Coil
-    35000,                   !- Nominal Capacity of the Coil {W}
-    Heating Coil Air Inlet Node,  !- Coil\_Air\_Inlet\_Node
-    Heating Coil Air Outlet Node; !- Coil\_Air\_Outlet\_Node
-
-AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat,
-    Zone 1 VAV System,       !- Name of System
-    FanAndCoilAvailSched,    !- System Availability schedule
-    Zone 1 Reheat Air Inlet Node,  !- DAMPER Air Outlet Node
-    Zone 1 VAV Inlet Node,   !-UNIT Air Inlet Node
-    0.583,                   !- Maximum air flow rate {m3/s}
-    0.25,                    !- Zone Minimum Air Flow Fraction
-    ,                        !- Control node
-    Coil:Heating:Electric,   !- Reheat Component Object
-    Reheat Coil Zone 1,      !- Name of Reheat Component
-    0.0,                     !- Max Reheat Water Flow {m3/s}
-    0.0,                     !- Min Reheat Water Flow {m3/s}
-    Zone 1 Reheat Air Outlet Node,  !- UNIT Air Outlet Node
-    0.001;                   !- Convergence Tolerance
-
-AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat,
-    Zone 2 VAV System,       !- Name of System
-    FanAndCoilAvailSched,    !- System Availability schedule
-    Zone 2 Reheat Air Inlet Node,  !- DAMPER Air Outlet Node
-    Zone 2 VAV Inlet Node,   !-UNIT Air Inlet Node
-    0.583,                   !- Maximum air flow rate {m3/s}
-    0.25,                    !- Zone Minimum Air Flow Fraction
-    ,                        !- Control node
-    Coil:Heating:Electric,   !- Reheat Component Object
-    Reheat Coil Zone 2,      !- Name of Reheat Component
-    0.0,                     !- Max Reheat Water Flow {m3/s}
-    0.0,                     !- Min Reheat Water Flow {m3/s}
-    Zone 2 Reheat Air Outlet Node,  !- UNIT Air Outlet Node
-    0.001;                   !- Convergence Tolerance
-
-AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat,
-    Zone 3 VAV System,       !- Name of System
-    FanAndCoilAvailSched,    !- System Availability schedule
-    Zone 3 Reheat Air Outlet Node,  !- UNIT Air Outlet Node
-    Zone 3 VAV Inlet Node,   !-UNIT Air Inlet Node
-    0.584,                   !- Maximum air flow rate {m3/s}
-    0.25;                    !- Zone Minimum Air Flow Fraction
-```
-
-### Unitary VAV Changeover Bypass Heat and Cool (AirLoopHVAC) Outputs
-
-* HVAC,Average,Unitary System Total Heating Rate [W]
-
-* HVAC,Sum,Unitary System Total Heating Energy [J]
-
-* HVAC,Average,Unitary System Total Cooling Rate [W]
-
-* HVAC,Sum,Unitary System Total Cooling Energy [J]
-
-* HVAC,Average,Unitary System Sensible Heating Rate [W]
-
-* HVAC,Sum,Unitary System Sensible Heating Energy [J]
-
-* HVAC,Average,Unitary System Sensible Cooling Rate [W]
-
-* HVAC,Sum,Unitary System Sensible Cooling Energy [J]
-
-* HVAC,Average,Unitary System Latent Heating Rate [W]
-
-* HVAC,Sum,Unitary System Latent Heating Energy [J]
-
-* HVAC,Average,Unitary System Latent Cooling Rate [W]
-
-* HVAC,Sum,Unitary System Latent Cooling Energy [J]
-
-* HVAC,Average,Unitary System Electric Power [W]
-
-* HVAC,Sum,Unitary System Electric Energy [J]
-
-* HVAC,Average,Unitary System Fan Part Load Ratio []
-
-* HVAC,Average,Unitary System Compressor Part Load Ratio []
-
-* HVAC,Average,Unitary System Bypass Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Unitary System Air Outlet Setpoint Temperature [C]
-
-#### Unitary System Total Heating Rate [W]
-
-This output field is the total (enthalpy) heat addition rate of the CBVAV system in Watts. This value is calculated using the enthalpy difference of the outlet air and inlet air streams, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are averaged for the timestep being reported.
-
-#### Unitary System Total Heating Energy [J]
-
-This output field is the total (enthalpy) heat addition of the CBVAV system in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the outlet air and inlet air streams, the supply air mass flow rate entering/leaving the system, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy addition only) are summed for the timestep being reported.
-
-#### Unitary System Total Cooling Rate [W]
-
-This output field is the total (enthalpy) heat extraction rate of the CBVAV system in Watts. This value is calculated using the enthalpy difference of the outlet air and inlet air streams, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are averaged for the timestep being reported.
-
-#### Unitary System Total Cooling Energy [J]
-
-This output field is the total (enthalpy) heat extraction of the CBVAV system in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the outlet air and inlet air streams, the supply air mass flow rate entering/leaving the system, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (enthalpy extraction only) are summed for the timestep being reported.
-
-#### Unitary System Sensible Heating Rate [W]
-
-This output field is the sensible heat addition rate of the CBVAV system in Watts. This value is calculated using the enthalpy difference of the outlet air and inlet air streams at a constant humidity ratio, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are averaged for the timestep being reported.
-
-#### Unitary System Sensible Heating Energy [J]
-
-This output field is the sensible heat addition of the CBVAV system in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the outlet air and inlet air streams at a constant humidity ratio, the supply air mass flow rate entering/leaving the system, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (heating only) are summed for the timestep being reported.
-
-#### Unitary System Sensible Cooling Rate [W]
-
-This output field reports the moist air sensible heat extraction rate of the CBVAV system in Watts. This value is calculated using the enthalpy difference of the outlet air and inlet air streams at a constant humidity ratio, and the supply air mass flow rate entering/leaving the system. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are averaged for the timestep being reported.
-
-#### Unitary System Sensible Cooling Energy [J]
-
-This output field reports the moist air sensible heat extraction of the CBVAV system in Joules over the timestep being reported. This value is calculated using the enthalpy difference of the outlet air and inlet air streams at a constant humidity ratio, the supply air mass flow rate entering/leaving the system, and the HVAC simulation timestep. This value is calculated for each HVAC system timestep being simulated, and the results (cooling only) are summed for the timestep being reported.
-
-#### Unitary System Latent Heating Rate [W]
-
-This output field is the latent heat addition (humidification) rate of the CBVAV system in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are averaged for the timestep being reported.
-
-#### Unitary System Latent Heating Energy [J]
-
-This output field is the latent heat addition (humidification) of the CBVAV system in Joules over the timestep being reported. This value is calculated as the difference between the total energy and the sensible energy delivered by the system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat addition only) are summed for the timestep being reported.
-
-#### Unitary System Latent Cooling Rate [W]
-
-This output field is the latent heat extraction (dehumidification) rate of the CBVAV system in Watts. This value is calculated as the difference between the total energy rate and the sensible energy rate provided by the system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are averaged for the timestep being reported.
-
-#### Unitary System Latent Cooling Energy [J]
-
-This output field is the latent heat extraction (dehumidification) of the CBVAV system in Joules over the timestep being reported. This value is calculated as the difference between the total energy and the sensible energy delivered by the system. This value is calculated for each HVAC system timestep being simulated, and the results (latent heat extraction only) are summed for the timestep being reported.
-
-#### Unitary System Electric Power [W]
-
-This output field is the electricity consumption rate of the CBVAV system in Watts. The consumption includes electricity used by the DX compressor (including crankcase heater), fans (indoor supply air fan and the condenser fans associated with the DX coil[s]), and the heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Unitary System Electric Energy [J]
-
-This output field is the electricity consumption of the CBVAV system in Joules for the time period being reported. The consumption includes electricity used by the DX compressor (including crankcase heater), fans (indoor supply air fan and the condenser fans associated with the DX coil[s]), and the heating coil (if electric). This value is calculated for each HVAC system timestep being simulated, and the results are summed for the timestep being reported.
-
-#### Unitary System Fan Part Load Ratio []
-
-This output field is the part-load ratio of the supply air fan, which will be either zero or 1 for each simulation timestep. For this system, the fan will operate continuously for the simulation timestep if the system is available (ref. Field: Availability schedule name) and there is a cooling or heating load to be met (i.e., fan part-load ratio will equal 1). When the system is available but there is no cooling or heating load to be met, the fan will either be off for the entire timestep or on for the entire timestep depending on the supply air fan operating mode schedule (ref. Field: Supply Air Fan Operating Mode Schedule Name). This value is set for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Unitary System Compressor Part Load Ratio []
-
-This output field is the part-load ratio of the compressor used by the DX coils (cooling and heating). The compressor part-load ratio is defined as the total coil load divided by the coil steady-state capacity (steady-state capacity of first stage for multi-mode coils). This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Unitary System Bypass Air Mass Flow Rate [kg/s]
-
-This output field is the mass flow rate of air, in kg/s, being bypassed from the supply air path and blended with the air entering the CBVAV system. This value is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Unitary System Air Outlet Setpoint Temperature [C]
-
-This output field is the dry-bulb set point temperature in degrees Celsius. This set point temperature is calculated by the model based on the zone cooling/heating loads calculated by EnergyPlus, and the priority control mode and the dehumidification control type specified for this unitary system. The CBVAV system attempts to achieve the outlet air set point temperature to the extent possible.
-
-
-
-Group – Variable Refrigerant Flow Equipment
--------------------------------------------
-
-This group of EnergyPlus input objects describes the configurations of Variable Refrigerant Flow (VRF, or Variable Refrigerant Volume) air-conditioning systems.
-
-A VRF system is an air-conditioning system that varies the refrigerant flow rate using variable speed compressor(s) in the outdoor unit, and the electronic expansion valves (EEVs) located in each indoor unit. The system meets the space cooling or heating load requirements by maintaining the zone air temperature at the setpoint. The ability to control the refrigerant mass flow rate according to the cooling and/or heating load enables the use of as many as 60 or more indoor units with differing capacities in conjunction with one single outdoor unit. This unlocks the possibility of having individualized comfort control, simultaneous heating and cooling in different zones, and heat recovery from one zone to another. It may also lead to more efficient operations during part-load conditions.
-
-There are two alternative VRF models in EnergyPlus:
-
- 1. **System curve based model (VRF-SysCurve)**. In this model, a number of system level curves are used to describe the VRF system performance. This model corresponds to the *AirConditioner:VariableRefrigerantFlow* object.
-
- 2. **Physics based model (VRF-FluidTCtrl)**. This model is able to consider the dynamics of more operational parameters and is applicable for fluid temperature control. This model corresponds to the *AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl* object.
-
-( Please refer to the engineering reference for more technical details of the two models).
-
-In the VRF system model, direct-expansion cooling and/or heating coils are configured in a zone terminal unit, which is connected to a zone via the zone inlet and exhaust nodes. The zone terminal units are identified in a *ZoneTerminalUnitList* object, the name of which is entered as an input to the *AirConditioner:VariableRefrigerantFlow* or *AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl* object.
-
-The Energyplus connection methodology is shown as dashed and greyed arrows in the figure below according to the following rules:
-
-  * The zone inlet and zone exhaust node names are defined in a *ZoneHVAC:EquipmentConnections* object (bottom of figure).
-
-  * A *ZoneHVAC:TerminalUnit:VariableRefrigerantFlow* object will identify these zone exhaust and zone inlet node names as the terminal unit’s air inlet and air outlet nodes, respectively.
-
-  * All zone terminal units that are connected to the same *AirConditioner:VariableRefrigerantFlow* or *AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl* object are listed in a *ZoneTerminalUnitList* object.
-
-  * The name of the *ZoneTerminalUnitList* object is an input to the *AirConditioner:VariableRefrigerantFlow* or *AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl* object.
-
-  * The *AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl* or *AirConditioner:VariableRefrigerantFlow* object is not listed in an AirloopHVAC object, and therefore, can only be simulated if the terminal units are connected to the *AirConditioner:VariableRefrigerantFlow* or *AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl* object using the ZoneTerminalUnitList.
-
-  * Secondary ZoneHVAC equipment objects may be used in the same zones as the terminal units for other purposes (e.g., code compliance)
-
-The following schematic demonstrates these connection rules.
-
-![VRFSchematic](media/image310.png)
-
-Figure 125. Variable Refrigerant Flow Schematic
-
-Energyplus object type and object name, and node name relationships are also shown in the following figure to aid in the assembly of this HVAC system type.
-
-![VRFObjects](media/image311.png)
-*(a) VRF model based on system curves (VRF-SysCurve)*
-
-![VRFObjects](media/image312.png)
-*(b) VRF model based on physics (VRF-FluidTCtrl)*
-
-Figure 126. Variable Refrigerant Flow Object Links
-
-
-### AirConditioner:VariableRefrigerantFlow
-
-#### Field: Heat Pump Name
-
-This alpha field defines a unique user-assigned name for an instance of a variable refrigerant flow heat pump. Any reference to this heat pump will use this name. Since this object is not listed in an AirloopHVAC object, the most likely use of this name would be for reporting purposes.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump operates during a given time period. A schedule value equal to 0 denotes that the heat pump must be off for that time period. A value other than 0 denotes that the heat pump is available to operate during that time period. This schedule may be used to completely disable the heat pump (and all of its terminal units) as required. If this field is blank, the unit is enabled the entire simulation.
-
-#### Field: Gross Rated Total Cooling Capacity
-
-This numeric field defines the total cooling capacity (sensible + latent) of the heat pump at rated conditions in watts. The cooling capacity must be greater than 0 or set to autosize.
-
-#### Field: Gross Rated Cooling COP
-
-This numeric field defines the cooling coefficient of performance at rated conditions. The cooling coefficient of performance includes compressor power and condenser fan power. This COP value does not account for impacts due to the supply air fan. The nominal heat pump cooling COP must be greater than 0. If this field is left blank, a default coefficient of performance of 3.3 is assumed.
-
-#### Field: Minimum Outdoor Temperature in Cooling Mode
-
-This numeric field defines the minimum outdoor dry-bulb temperature allowed for cooling operation. Below this temperature, cooling is disabled. If this field is left blank, the default value is -6ºC.
-
-#### Field: Maximum Outdoor Temperature in Cooling Mode
-
-This numeric field defines the maximum outdoor dry-bulb temperature allowed for cooling operation. Above this temperature, cooling is disabled. If this field is left blank, the default value is 43ºC.
-
-#### Field: Cooling Capacity Ratio Modifier Function of Low Temperature Curve Name
-
-This alpha field defines the cooling capacity ratio modifier at low outdoor dry-bulb temperatures. This curve is a bi-quadratic equation using weighted average indoor wet-bulb temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air dry-bulb temperature as the independent variables. This performance curve can be used to describe the cooling capacity ratio at low outdoor temperatures (i.e., the following two curves are used) or can be used to describe the performance for all outdoor temperatures (i.e., the following two curves are not used). For this system type it is likely that all three of these performance curves will be required. See the Engineering Reference for more discussion on using this input field.
-
-#### Field: Cooling Capacity Ratio Boundary Curve Name
-
-This alpha field defines the cooling capacity ratio boundary curve name. This curve is a linear, quadratic or cubic curve that defines a change in cooling capacity at a specific condenser entering air dry-bulb temperature as a function of indoor air wet-bulb temperature. This curve is used when the trend in cooling capacity changes dramatically as outdoor temperature changes. If the cooling capacity does not change dramatically with changes in outdoor conditions, this field may be left blank. See the Engineering Reference for more discussion on using this input field.
-
-#### Field: Cooling Capacity Ratio Modifier Function of High Temperature Curve Name
-
-This alpha field defines the cooling capacity ratio modifier at high outdoor temperatures. This curve is a bi-quadratic equation using weighted average indoor wet-bulb temperature and condenser entering air dry-bulb temperature as the independent variables. This curve is used when the trend in cooling capacity changes dramatically as outdoor temperature changes. If the cooling capacity does not change dramatically with changes in outdoor conditions, this field may be left blank. See the Engineering Reference for more discussion on using this input field.
-
-#### Field: Cooling Energy Input Ratio Modifier Function of Low Temperature Curve Name
-
-This alpha field defines the cooling energy input ratio modifier at low outdoor temperatures. This curve is a bi-quadratic equation with a weighted average indoor wet-bulb temperature and condenser entering air dry-bulb temperature as the independent variables. This performance curve can be used to describe the cooling energy input ratio at low outdoor temperatures (i.e., the following two curves are used) or can be used to describe the performance for all outdoor temperatures (i.e., the following two curves are not used). For this system type it is likely that all three of these performance curves will be required. See the Engineering Reference for more discussion on using this input field.
-
-#### Field: Cooling Energy Input Ratio Boundary Name
-
-This alpha field defines the cooling energy input ratio boundary curve name. This curve is a linear, quadratic or cubic curve that defines a change in cooling energy at a specific condenser entering air dry-bulb temperature as a function of indoor air wet-bulb temperature. This curve is used when the trend in cooling energy changes dramatically as outdoor temperature changes. If the cooling energy does not change dramatically with changes in outdoor conditions, this field may be left blank. See the Engineering Reference for more discussion on using this input field.
-
-#### Field: Cooling Energy Input Ratio Modifier Function of High Temperature Curve Name
-
-This alpha field defines the cooling energy input ratio modifier at high outdoor temperatures. This curve is a bi-quadratic equation with weighted average indoor wet-bulb temperature and condenser entering air dry-bulb temperature as the independent variables. This curve is used when the trend in cooling energy changes dramatically as outdoor temperature changes. If the cooling energy does not change dramatically with changes in outdoor conditions, this field may be left blank. See the Engineering Reference for more discussion on using this input field.
-
-#### Field: Cooling Energy Input Ratio Modifier Function of Low Part-Load Ratio Curve Name
-
-This alpha field defines the cooling energy input ratio modifier (function of part-load ratio when PLR is less than or equal to 1) curve name. This curve is a linear, quadratic or cubic equation with cooling part-load ratio used as the independent variable. The cooling energy input ratio modifier curve is normalized to 1 at a part-load ratio of 1 and is used only when the operating part-load ratio is less than or equal to 1.
-
-#### Field: Cooling Energy Input Ratio Modifier Function of HIgh Part-Load Ratio Curve Name
-
-This alpha field defines the cooling energy input ratio modifier (function of part-load ratio when PLR is greater than 1) curve name. This curve is a linear, quadratic or cubic equation with cooling part-load ratio used as the independent variable. The cooling energy input ratio modifier curve is normalized to 1 at a part-load ratio of 1 and is used only when the operating part-load ratio is greater than 1.
-
-#### Field: Cooling Combination Ratio Correction Factor Curve Name
-
-This alpha field defines the cooling combination ratio (CR) correction factor curve name for combination ratios greater than or equal to 1. The combination ratio is defined as the total rated indoor terminal unit cooling capacity divided by this heat pump’s gross rated total cooling capacity. The curve is a linear, quadratic or cubic equation and uses the minimum value of x in the curve object to determine the maximum part-load ratio which is linearly proportional to capacity (i.e., the minimum value of x [CR] in the curve object must be ≥1). The output of this curve provides a multiplier (&gt;1) which is applied to this heat pump’s Gross Rated Total Cooling Capacity. Between a combination ratio of 1 and the curve’s minimum value of x, the multiplier is linearly interpolated. For combination ratio’s less than 1 (i.e., the total indoor terminal unit capacity is less than this heat pump’s rated total capacity), capacity is directly proportional to part-load ratio and this curve will not be used.
-
-#### Field: Cooling Part-Load Fraction Correlation Curve Name
-
-This alpha field defines the cooling part-load fraction correlation curve name. This curve is used to define the cycling losses when the condenser’s compressors cycle on and off. The compressor cycles when the cooling part-load ratio is less than the Minimum Heat Pump Part-Load Ratio specified later in this object’s inputs.
-
-#### Field: Gross Rated Heating Capacity
-
-This numeric field defines the gross total heat pump heating capacity at rated conditions in watts. The nominal heat pump heating capacity must be greater than 0 or set to autosize.
-
-#### Field: Rated Heating Capacity Sizing Ratio
-
-This numeric field defines the ratio of gross heating to gross cooling capacity. The model assumes that when used, this value will be greater than 1. A similar input is available in the ZoneHVAC:TerminalUnit:VariableRefrigerantFlow object. When the heating capacity is autosized, if this field is non-blank, this ratio is used to scale the heating capacity to the gross rated total cooling capacity regardless of the value entered in the terminal unit objects. When the heating capacity is not autosized, the gross rated heating capacity will be equal to the value specified in the Gross Rated Heating Capacity input field and this value will be compared to the sum of the terminal unit heating coil size. If these values are more than 10% different, a warning will be issued when Output:Diagnostics, DisplayExtraWarnings; is included in the input file. If this field is blank and the terminal unit sizing ratio input is also blank, then the heating capacity sizing ratio is assumed to be 1. If this field is not blank and the heating capacity sizing ratio in the terminal unit object(s) is blank, then this ratio also applies to each heating coil. If this field is not blank and the heating capacity sizing ratio in the terminal units is also not blank, then the terminal unit heating coil capacity sizing ratio input applies to each heating coil.
-
-#### Field: Gross Rated Heating COP
-
-This numeric field defines the heating coefficient of performance at rated conditions. The heating coefficient of performance includes compressor power and condenser fan power. This gross COP value does NOT account for  the supply air fan. The nominal heat pump heating COP must be greater than 0. If this field is left blank, a coefficient of performance of 3.4 is assumed.
-
-#### Field: Minimum Outdoor Temperature in Heating Mode
-
-This numeric field defines the minimum outdoor temperature allowed for heating operation. Below this temperature, heating is disabled. If this field is left blank, the default value is -20ºC.
-
-#### Field: Maximum Outdoor Temperature in Heating Mode
-
-This numeric field defines the maximum outdoor temperature allowed for heating operation. Above this temperature, heating is disabled. If this field is left blank, the default value is 16ºC.
-
-#### Field: Heating Capacity Ratio Modifier Function of Low Temperature Curve Name
-
-This alpha field defines the heating capacity ratio modifier at low temperature curve name. This curve is a bi-quadratic equation with a weighted average indoor dry-bulb temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air dry-bulb or wet-bulb temperature as the independent variables. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This performance curve can be used to describe the heating capacity ratio at low outdoor temperatures (i.e., the following two curves are used) or can be used to describe the performance for all outdoor temperatures (i.e., the following two curves are not used). For this system type it is likely that all three of these performance curves will be required. See the Engineering Reference for more discussion on using this input field.
-
-#### Field: Heating Capacity Ratio Boundary Curve Name
-
-This alpha field defines the heating capacity ratio boundary curve name. This curve is a quadratic or cubic curve that defines a change in heating capacity at a specific condenser entering air dry-bulb or wet-bulb temperature as a function of indoor air dry-bulb temperature. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This curve is used when the trend in heating capacity changes dramatically as outdoor temperature changes. If the heating capacity does not change dramatically with changes in outdoor conditions, this field may be left blank.
-
-#### Field: Heating Capacity Ratio Modifier Function of High Temperature Curve Name
-
-This alpha field defines the heating capacity ratio modifier at high temperature curve name. This curve is a bi-quadratic equation with a weighted average indoor dry-bulb temperature and condenser entering air dry-bulb or wet-bulb temperature as the independent variables. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This curve is used when the trend in heating capacity changes dramatically as outdoor temperature changes. If the heating capacity does not change dramatically with changes in outdoor conditions, this field may be left blank.
-
-#### Field: Heating Energy Input Ratio Modifier Function of Low Temperature Curve Name
-
-This alpha field defines the heating energy input ratio modifier at low temperature curve name. This curve is a bi-quadratic equation with a weighted average indoor dry-bulb temperature and condenser entering air dry-bulb or wet-bulb temperature as the independent variables. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This performance curve can be used to describe the heating energy input ratio at low outdoor temperatures (i.e., the following two curves are used) or can be used to describe the performance for all outdoor temperatures (i.e., the following two curves are not used).
-
-#### Field: Heating Energy Input Ratio Boundary Curve Name
-
-This alpha field defines the heating energy input ratio boundary curve name. This curve is a quadratic or cubic curve that defines a change in heating energy at a specific condenser entering air dry-bulb or wet-bulb temperature as a function of indoor air dry-bulb temperature. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This curve is used when the trend in heating energy changes dramatically as outdoor temperature changes. If the heating energy does not change dramatically with changes in outdoor conditions, this field may be left blank.
-
-#### Field: Heating Energy Input Ratio Modifier Function of High Temperature Curve Name
-
-This alpha field defines the heating energy input ratio modifier at high temperature curve name. This curve is a bi-quadratic equation with a weighted average indoor dry-bulb temperature and condenser entering air dry-bulb or wet-bulb temperature as the independent variables. Since manufacturers may provide performance data using either outdoor dry-bulb or wet-bulb temperatures, either of these temperature types may be used for heating performance curves as specified in the Heating Performance Curve Outdoor Temperature Type input field below. This curve is used when the trend in heating energy changes dramatically as outdoor temperature changes. If the heating energy does not change dramatically with changes in outdoor conditions, this field may be left blank.
-
-#### Field: Heating Performance Curve Outdoor Temperature Type
-
-This choice field defines the outdoor temperature type used for all performance curves. The valid choices are DryBulbTemperature and WetBulbTemperature. The default value is WetBulbTemperature. Manufacturers will typically provide heating performance data as a function of outdoor air wet-bulb temperatures. This means that the performance (e.g., capacity and energy input ratio) curves will use outdoor wet-bulb temperature as one of the independent variables. At times, manufacturers will only provide performance data as a function of outdoor dry-bulb temperatures. In this case, all performance curves shall be developed using outdoor dry-bulb temperature and this field shall be selected as DryBulbTemperature.
-
-#### Field: Heating Energy Input Ratio Modifier Function of Low Part-Load Ratio Curve Name
-
-This alpha field defines the heating energy input ratio modifier (function of part-load ratio when PLR is less than or equal to 1) curve name. This curve is a linear, quadratic, or cubic equation with heating part-load ratio used as the independent variable. The heating energy input ratio modifier curve is normalized to 1 at a part-load ratio of 1 and is used only when the part-load ratio is less than or equal to 1.
-
-#### Field: Heating Energy Input Ratio Modifier Function of High Part-Load Ratio Curve Name
-
-This alpha field defines the heating energy input ratio modifier (function of part-load ratio when PLR is greater than 1) curve name. This curve is a linear, quadratic, or cubic equation with heating part-load ratio used as the independent variable. The heating energy input ratio modifier curve is normalized to 1 at a part-load ratio of 1 and is used only when the part-load ratio is greater than 1.
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-#### Field: Heating Combination Ratio Correction Factor Curve Name
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-This alpha field defines the heating combination ratio (CR) correction factor curve name for combination ratios greater than or equal to 1. The combination ratio is defined as the total rated indoor heating capacity divided by the rated heat pump heating capacity. The curve is either quadratic or cubic and uses the minimum value of x in the curve object to determine the maximum part-load ratio which is linearly proportional to capacity (i.e., the minimum value of x in the curve object must be ≥1). The output of this curve provides a multiplier (&gt;1) which is applied to the Nominal Heat Pump Heating Capacity. Between a combination ratio of 1 and the curve’s minimum value of x, the multiplier is linearly interpolated. For combination ratio’s less than 1, capacity is directly proportional to part-load ratio and this curve will not be used. If this field is left blank, the Cooling Combination Ratio Correction factor will be used.
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-#### Field: Heating Part-Load Fraction Correlation Curve Name
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-This alpha field defines the heating part-load fraction correlation curve name. This curve is used to define the cycling losses when the condenser’s compressors cycle on and off. The compressor cycles when the indoor to outdoor heating capacity ratio is less than the Minimum Heat Pump Part-Load Ratio specified in the following field.
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-#### Field: Minimum Heat Pump Part-Load Ratio
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-This numeric field specifies the minimum operating part-load ratio (PLR) of the heat pump. When the heat pump operates at a PLR below this value, the heat pump’s compressor will cycle to meet the cooling or heating demand. Above this value, the heat pump’s compressor operates the entire time step to meet the cooling or heating demand. The minimum value for this field is 0. If this field is left blank, the default value is 0.15. When the heat pump compressor cycles, the previous field is used to determine cycling losses.
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-#### Field: Zone Name for Master Thermostat Location
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-This alpha field defines the name of the zone where the “master� thermostat is located. When the heat pump is connected to multiple zone terminal units, one terminal unit must be selected as the master thermostat. The remaining thermostats are slaves and can operate only in the same mode as the master thermostat.
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-#### Field: Master Thermostat Priority Control Type
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-This choice field determines the logic used to simulate the “master� thermostat. Valid choices are LoadPriority, ZonePriority, ThermostatOffsetPriority, MasterThermostatPriority, and Scheduled. The default value is MasterThermostatPriority. When LoadPriority is selected, the total zone load is used to choose the operating mode as either cooling or heating. When ZonePriority is selected, the number of zones requiring cooling or heating determines the operating mode. When ThermostatOffsetPriority is selected, the zone farthest from the thermostat set point determines the operating mode. The MasterThermostatPriority choice operates the system according the zone load where the master thermostat is located. The heat pump can also be scheduled to operate in either cooling or heating mode. For scheduled operation, a schedule name is entered in the following field.
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-#### Field: Thermostat Priority Schedule Name
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-This alpha field identifies the schedule used when the previous field is set to Scheduled. Schedule values of 0 denote heating mode while values of 1 denote cooling mode. Any other values will force the system off.
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-#### Field: Zone Terminal Unit List Name
-
-This alpha field defines the name of the zone terminal unit list. The name specified here should match the name of a valid ZoneTerminalUnitList object. In addition, each name specified in this list should match the name of a valid ZoneHVAC:TerminalUnit: VariableRefrigerantFlow object. All terminal units connected to this heat pump must be listed in this ZoneTerminalUnitList object.
-
-Note: the previous field is designated at the last field necessary to simulate the variable refrigerant flow heat pump. The following fields do not have to be entered, however, piping loses, defrost operation, crankcase heater operation, and basin heater operation will not be modeled. Defaults for fields not entered may also not apply. These remaining fields must be entered if that portion of the model is to be simulated.
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-#### Field: Heat Pump Waste Heat Recovery
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-This choice field defines the configuration of the heat pump refrigeration system. Valid choices are **Yes** and **No**. If Yes is selected, heat recovery is enabled and the heat pump can independently cool and heat different zones. If No is selected, the heat pump is only able to cool or heat for any given time step.
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-#### Field: Equivalent Piping Length used for Piping Correction Factor in Cooling Mode
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-This numeric field defines the equivalent pipe length in meters between the farthest terminal unit and the heat pump condenser. This value includes the gas refrigerant line length (for both horizontal and vertical distances), fitting losses, pipe bends, and other connections that contribute to piping losses. This field is used to calculate the piping correction factor in cooling mode. This value defines the head losses due to the pipe length between the farthest terminal unit and the heat pump condenser and impacts the maximum available capacity in cooling mode.
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-#### Field: Vertical Height used for Piping Correction Factor
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-This numeric field defines the vertical pipe height in meters between the highest or lowest terminal unit and the heat pump condenser. This value defines the gravitational losses due to a change in height between the highest (positive value), or lowest (negative value) terminal unit and the heat pump condenser. The distance specified here is applied to the piping correction factor calculation for both cooling and heating. If the distance between the highest terminal unit above the heat pump condenser is greater than the distance between the lowest terminal unit below the condenser enter the difference between the highest and lowest terminal units as a positive distance, otherwise enter this difference as a negative distance. Example: if the distance from the heat pump condenser to the highest terminal unit above the condenser is 10 m and the distance from the heat pump condenser to the lowest terminal unit below the condenser is -15 m, then enter a value of -5 m in this field. This head loss impacts the maximum available capacity in cooling mode.
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-#### Field: Piping Correction Factor for Length in Cooling Mode Curve Name
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-This alpha field defines the linear, quadratic, or cubic curve name used to calculate the piping correction factor for length in cooling mode. Piping losses are a function of piping length. If sufficient piping loss information is available where piping losses are also a function of combination ratio (i.e., in addition to length), a biquadratic performance curve may be used.
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-#### Field: Piping Correction Factor for Height in Cooling Mode Coefficient
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-This numeric field defines the coefficient used to calculate the piping correction factor for height in cooling mode.
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-#### Field: Equivalent Piping Length used for Piping Correction Factor in Heating Mode
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-This numeric field defines the equivalent pipe length in meters between the farthest terminal unit and the heat pump condenser. This value includes the liquid refrigerant line length (for both horizontal and vertical distances), fitting losses, pipe bends, and other connections that contribute to piping losses. This field is used to calculate the piping correction factor in heating mode. This value defines the head losses due to the pipe length between the farthest terminal unit and the heat pump condenser and impacts the maximum available capacity in heating mode.
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-#### Field: Piping Correction Factor for Length in Heating Mode Curve Name
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-This alpha field defines the linear, quadratic, or cubic curve name used to calculate the piping correction factor for length in heating mode. Piping losses are a function of piping length. If sufficient piping loss information is available where piping losses are also a function of combination ratio (i.e., in addition to length), a biquadratic performance curve may be used.
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-#### Field: Piping Correction Factor for Height in Heating Mode Coefficient
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-This numeric field defines the coefficient used to calculate the piping correction factor for height in heating mode.
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-#### Field: Crankcase Heater Power per Compressor
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-This numeric field defines the electrical power consumed by the crankcase heater in watts for *each* compressor. This crankcase heater power is consumed when the outdoor temperature is below the maximum outdoor dry-bulb temperature for crankcase heater operation. The minimum value for this field is 0. If this field is left blank, the default value is 33 watts. Crankcase heater electrical consumption is applied only when the compressor is off or is applied during the off cycle when the compressor is cycling below the Minimum Heat Pump Part-Load Ratio. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
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-#### Field: Number of Compressors
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-This numeric field defines the number of compressors in the heat pump condensing unit and is used exclusively to determine the operating characteristics of the crankcase heater. For example, if the number of compressors is 3, one crankcase heater will operate when the heat pump condensing unit’s part-load ratio is less than or equal to 0.67 (when the ratio of compressor size to total compressor capacity input is 0.33) and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. Similarly, two crankcase heaters will operate when the heat pump condensing unit’s PLR is less than or equal to 0.33 and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. If the heat pump condensing unit is off, all 3 crankcase heaters will operate if the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. The minimum value for this field is 1. If this field is left blank, the default value is 2. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
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-#### Field: Ratio of Compressor Size to Total Compressor Capacity
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-This numeric field defines the size of the first stage compressor to the total compressor capacity and is used exclusively for calculating crankcase heater energy. If this field and the previous field are left blank, the default value is 0.5.  If this field is left blank and the previous field is not blank, the compressors are assumed to be equally sized. When the number of compressors is greater than 2, the 2<sup>nd</sup> stage compressor and all additional compressors are assumed to be equally sized. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
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-#### Field: Maximum Outdoor Dry-bulb Temperature for Crankcase Heater
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-This numeric field defines the maximum outdoor temperature, in degrees Celsius, below which the crankcase heater will operate. If this field is left blank, the default value is 0°C. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
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-#### Field: Defrost Strategy
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-This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse-cycle. Defrost can be disabled by entering a resistive defrost strategy using a timed defrost control, a 0 defrost time period fraction and a 0 resistive defrost heater capacity in the following inputs fields. This method is used when the Maximum Outdoor Dry-Bulb Temperature for Defrost Operation field value is greater than the expected minimum outdoor dry-bulb temperature simulated in the weather file.
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-#### Field: Defrost Control
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-This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value of compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field “Defrost Time Period Fraction� described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field “Maximum Outdoor Dry-bulb Temperature for Defrost Operation� described above. If this input field is left blank, the default defrost control is timed.
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-#### Field: Defrost Energy Input Ratio Modifier Function of Temperature Curve Name
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-This alpha field defines the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) during reverse-cycle defrost periods as a function of the outdoor air dry-bulb temperature and the weighted average wet-bulb temperature of the air entering the indoor terminal units. The output of this curve is multiplied by the coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the indoor and outdoor coils are operating. The curve is normalized to a value of 1.0 at the rating point conditions.
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-#### Field: Defrost Time Period Fraction
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-This numeric field defines the fraction of compressor runtime when the defrost cycle is active. For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
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-#### Field: Resistive Defrost Heater Capacity
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-This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is ‘resistive’ (see input field “Defrost Strategy� above). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.
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-#### Field: Maximum Outdoor Dry-bulb Temperature for Defrost Operation
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-This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. If this input field is left blank, the default value is 5 C. Defrost can be completely eliminated by selecting a temperature lower than the minimum expected outdoor temperature found in the weather file.
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-#### Field: Condenser Type
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-This choice field defines the configuration of the heat pump condenser. Valid choices are **AirCooled**, **EvaporativelyCooled**, and **WaterCooled**.
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-#### Field: Condenser Inlet Node Name
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-This alpha field defines the name of the condenser inlet air or water node. For Condenser type = AirCooled, this node name should also be listed in an OutdoorAir:Node or OutdoorAir:NodeList object. If this field is blank, the model assumes an air-cooled condenser and the weather file is used to define the outdoor conditions entering the condenser. If this field is not blank, the node conditions are used to define the outdoor air or inlet water conditions entering the condenser. A node name is typically entered here for air-cooled systems when conditions other than those found in the weather file should be used (ref. OutdoorAir:Node related to height above ground).
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-#### Field: Condenser Outlet Node Name
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-This alpha field defines the name of the condenser outlet water node. This field is only used for water-cooled systems.
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-#### Field: Water Condenser Volume Flow Rate
-
-This numeric field defines the condenser water volume flow rate in cubic meters per second. This field is autosizable and only used for water-cooled systems.
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-#### Field: Evaporative Condenser Effectiveness
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-The effectiveness of the evaporative condenser, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
-
-<div>\[Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectiveness} \right)\left( {Tdb,o\,\, - Twb,o} \right)\]</div>
-
-where
-
-*T<sub>cond\\ inlet</sub>* = the temperature of the air entering the condenser coil (C)
-
-*T<sub>wb,o</sub>* = the wet-bulb temperature of the outdoor air (C)
-
-*T<sub>db,o</sub>* = the dry-bulb temperature of the outdoor air (C)
-
-The resulting condenser inlet air temperature is used by the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled and the simulation is calculating heating performance.
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-If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
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-If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = EvapCooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
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-If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = EvapCooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Cooling Capacity and Cooling EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
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-#### Field: Evaporative Condenser Air Flow Rate
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-The air volume flow rate, in m<sup>3</sup> per second, entering the evaporative condenser. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000144 m<sup>3</sup>/s per watt of rated total cooling capacity [850 cfm/ton]). This field is not used when Condenser Type = AirCooled.
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-#### Field: Evaporative Condenser Pump Rated Power Consumption
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-The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt [15 W/ton] of rated total cooling capacity). This field is not used when Condenser Type = AirCooled.
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-#### Field: Supply Water Storage Tank Name
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-This alpha field defines the name of the water storage tank when an evaporatively-cooled condenser is used.
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-#### Field: Basin Heater Capacity
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-This numeric field contains the capacity of the heat pump’s electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the heat pump compressor(s) is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
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-#### Field: Basin Heater Setpoint Temperature
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-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the heat pump is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
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-#### Field: Basin Heater Operating Schedule Name
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-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the heat pump is off.
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-#### Field: Fuel Type
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-This alpha field determines the type of fuel that this variable refrigerant flow system uses.  This field has seven choices: Electricity, NaturalGas, PropaneGas, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1, and OtherFuel2. The default is Electricity. The use of alternate fuel types assumes an engine drives the variable speed compression system and also accounts for condenser air flow (i.e., a fan attached to the engine provides air flow through the outdoor condenser.
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-#### Field: Minimum Outdoor Temperature in Heat Recovery Mode
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-This numeric field defines the minimum outdoor dry-bulb temperature allowed for heat recovery operation. Below this temperature, heat recovery is disabled. This input must be greater than the larger of the minimum outdoor temperature in cooling or heating mode. If this field is left blank, the default value is the higher of the Minimum Outdoor Temperature in Cooling Mode or Minimum Outdoor Temperature in Heating Mode inputs. This system may still operate in cooling or heating only mode when outdoor temperatures are below the minimum outdoor temperature in heat recovery mode. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes.
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-#### Field: Maximum Outdoor Temperature in Heat Recovery Mode
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-This numeric field defines the maximum outdoor dry-bulb temperature allowed for heat recovery operation. Above this temperature, heat recovery is disabled. This input must be less than the smaller of the maximum outdoor temperature in cooling or heating mode. If this field is left blank, the default value is the lower of the Maximum Outdoor Temperature in Cooling Mode or Maximum Outdoor Temperature in Heating Mode inputs.. This system may still operate in cooling or heating only mode when outdoor temperatures are above the maximum outdoor temperature in heat recovery mode. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes.
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-#### Field: Heat Recovery Cooling Capacity Modifier Curve Name
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-This alpha field defines the cooling capacity modifier when heat recovery mode is active. This modifier is used as a multiplier for available cooling capacity, and when in heat recovery mode, this modifier is usually less than 1. This curve is either a bi-quadratic equation using weighted average indoor temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air temperature as the independent variables or a cubic curve based on part-load ratio. This performance curve can be used to describe the cooling capacity modifier as either a constant (e.g., temperature or part-load ratio term coefficients are 0), a cooling modifier that varies with either indoor temperature and/or outdoor temperature, or part-load ratio (e.g., one or more temperature or part-load ratio term coefficients are 0), or varies with both indoor and outdoor temperatures or part-load ratio (e.g., all temperature or part-load ratio term coefficients are non-zero). If this field is left blank, and heat recovery operating mode is selected, the default constant modifier is 0.9. This modifier is applied only when heat recovery mode is active. To model a heat recovery system which has no degradation in cooling performance when heat recovery mode is active, or if the degradation is not constant at different operating conditions, a performance curve object must be used. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode.
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-#### Field: Initial Heat Recovery Cooling Capacity Fraction
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-This numeric field defines the fraction of cooling capacity available when the system transitions from cooling only operation to simultaneous cooling and heating. It is common for the cooling capacity to decrease before the system recovers. If this field is left blank, a default value of 0.5 is used (50% reduction in cooling capacity at the start of heat recovery mode). The system will recovery according to the time constant entered in Heat Recovery Cooling Capacity Time Constant input field. If the transition period will not be modeled, this input field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
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-#### Field: Heat Recovery Cooling Capacity Time Constant
-
-This numeric field defines the cooling capacity time constant, in hours, used to model the time it takes for the system to change from cooling only operation to simultaneous cooling and heating. Total response time is defined as 5 time constants. If this field is left blank, a default value of 0.083 is used. If the transition period will not be modeled, the Initial Heat Recovery Cooling Capacity Fraction field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
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-#### Field: Heat Recovery Cooling Energy Modifier Curve Name
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-This alpha field defines the cooling energy modifier when heat recovery mode is active. This modifier is used as a multiplier for operating cooling energy, and when in heat recovery mode, this modifier is usually greater than 1. This curve is a bi-quadratic equation using weighted average indoor temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air temperature as the independent variables. This performance curve can be used to describe the cooling energy modifier as either a constant (e.g., temperature term coefficients are 0), a cooling energy modifier that varies with indoor and/or outdoor temperatures (e.g., one or more temperature term coefficients are 0), or varies with both indoor and outdoor temperatures (e.g., temperature term coefficients are non-zero). If this field is left blank, and heat recovery operating mode is selected, the default constant modifier is 1.1. This modifier is applied only when heat recovery mode is active. To model a heat recovery system which has no degradation in cooling performance when heat recovery mode is active, or if the degradation is not constant at different operating conditions, a performance curve object must be used. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode.
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-#### Field: Initial Heat Recovery Cooling Energy Fraction
-
-This numeric field defines the fraction of cooling energy consumed when the system transitions from cooling only operation to simultaneous cooling and heating. It is common for the cooling energy to drop before the system recovers. If this field is left blank, a default value of 1 is used (no change in energy at the start of heat recovery mode). If the transition period will not be modeled, this input field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
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-#### Field: Heat Recovery Cooling Energy Time Constant
-
-This numeric field defines the cooling energy time constant, in hours, used to model the time it takes for the system to transition from cooling only operation to simultaneous cooling and heating. Total response time is defined as 5 time constants. If this field is left blank, a default value of 0.0 is used. If the transition period will not be modeled, the Initial Heat Recovery Cooling Energy Fraction field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from cooling only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
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-#### Field: Heat Recovery Heating Capacity Modifier Curve Name
-
-This alpha field defines the heating capacity modifier when heat recovery mode is active. This modifier is used as a multiplier for available heating capacity, and when in heat recovery mode, this modifier is usually less than 1. This curve is a bi-quadratic equation using weighted average indoor temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air temperature as the independent variables. This performance curve can be used to describe the heating capacity modifier as either a constant (e.g., temperature term coefficients are 0), a heating modifier that varies with indoor and/or outdoor temperatures (e.g., one or more temperature term coefficients are 0), or varies with both indoor and outdoor temperatures (e.g., temperature term coefficients are non-zero). If this field is left blank, and heat recovery operating mode is selected, the default constant modifier is 0.9. This modifier is applied only when heat recovery mode is active. To model a heat recovery system which has no degradation in heating performance when heat recovery mode is active, or if the degradation is not constant at different operating conditions, a performance curve object must be used. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode.
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-#### Field: Initial Heat Recovery Heating Capacity Fraction
-
-This numeric field defines the fraction of heating capacity available when the system changes from heating only operation to simultaneous heating and cooling. It is common for the heating capacity to decrease before the system recovers. If this field is left blank, a default value of 0.5 is used (50% reduction in heating capacity at the start of heat recovery mode). The system will recovery according to the time constant entered in Heat Recovery Heating Capacity Time Constant input field. If the transition period will not be modeled, this input field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
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-#### Field: Heat Recovery Heating Capacity Time Constant
-
-This numeric field defines the heating capacity time constant, in hours, used to model the time it takes for the system to transition from cooling only operation to simultaneous cooling and heating. Total response time is defined as 5 time constants. If this field is left blank, a default value of 0.083 is used. If the transition period will not be modeled, the Initial Heat Recovery Heating Capacity Fraction field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
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-#### Field: Heat Recovery Heating Energy Modifier Curve Name
-
-This alpha field defines the heating energy modifier when heat recovery mode is active. This modifier is used as a multiplier for operating heating energy, and when in heat recovery mode, this modifier is usually greater than 1. This curve is a bi-quadratic equation using weighted average indoor temperature (i.e., the indoor terminal units weighted average inlet temperatures) and condenser entering air temperature as the independent variables. This performance curve can be used to describe the heating energy modifier as either a constant (e.g., temperature term coefficients are 0), a heating energy modifier that varies with indoor and/or outdoor temperatures (e.g., one or more temperature term coefficients are 0), or varies with both indoor and outdoor temperatures (e.g., temperature term coefficients are non-zero). If this field is left blank, and heat recovery operating mode is selected, the default constant modifier is 1.1. This modifier is applied only when heat recovery mode is active. To model a heat recovery system which has no degradation in heating performance when heat recovery mode is active, or if the degradation is not constant at different operating conditions, a performance curve object must be used. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode.
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-#### Field: Initial Heat Recovery Heating Energy Fraction
-
-This numeric field defines the fraction of heating energy consumed when the system changes from heating only operation to simultaneous heating and cooling. It is common for the heating energy to decrease before the system recovers. If this field is left blank, a default value of 0.5 is used (50% reduction in heating energy at the start of heat recovery mode). The system will recovery according to the time constant entered in Heat Recovery Heating Energy Time Constant input field. If the transition period will not be modeled, this input field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
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-#### Field: Heat Recovery Heating Energy Time Constant
-
-This numeric field defines the heating energy time constant, in hours, used to model the time it takes for the system to change from cooling only operation to simultaneous cooling and heating. Total response time is defined as 5 time constants. If this field is left blank, a default value of 0.0 is used. If the transition period will not be modeled, the Initial Heat Recovery Heating Energy Fraction field must be set to 1. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes and the system changes from heating only mode to heat recovery mode. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
-
-Following is an example input for a AirConditioner:VariableRefrigerantFlow system.
-
-
-
-```idf
-AirConditioner:VariableRefrigerantFlow,
-  VRF Heat Pump,        !- Heat Pump Name
-  VRFCondAvailSched,    !- Availability Schedule Name
-  autosize,             !- Gross Rated Total Cooling Capacity {W}
-  3.16038,              !- Gross Rated Cooling COP {W}
-  -5,                   !- Minimum Outdoor Temperature in Cooling Mode {C}
-  43,                   !- Maximum Outdoor Temperature in Cooling Mode {C}
-  VRFCoolCapFT,         !- Cooling Capacity Ratio Modifier Function of Low Temperature Curve Name
-  VRFCoolCapFTBoundary, !- Cooling Capacity Ratio Boundary Curve Name
-  VRFCoolCapFTHi,       !- Cooling Capacity Ratio Modifier Function of High Temperature Curve Name
-  VRFCoolEIRFT,         !- Cooling Energy Input Ratio Modifier Function of Low Temperature Curve Name
-  VRFCoolEIRFTBoundary, !- Cooling Energy Input Ratio Boundary Curve Name
-  VRFCoolEIRFTHi,       !- Cooling Energy Input Ratio Modifier Function of High Temperature Curve Name
-  CoolingEIRLowPLR,     !- Cooling Energy Input Ratio Modifier Function of Low Part-Load Ratio Curve Name
-  CoolingEIRHiPLR,      !- Cooling Energy Input Ratio Modifier Function of High Part-Load Ratio Curve Name
-  CoolingCombRatio,     !- Cooling Combination Ratio Correction Factor Curve Name
-  VRFCPLFFPLR,          !- Cooling Part-Load Fraction Correlation Curve Name
-  autosize,             !- Gross Rated Heating Capacity {W}
-  ,                     !- Rated Heating Capacity Sizing Ratio (W/W)
-  3.40909,              !- Gross Rated Heating COP
-  -20,                  !- Minimum Outdoor Temperature in Heating Mode {C}
-  15.5,                 !- Maximum Outdoor Temperature in Heating Mode {C}
-  VRFHeatCapFT,         !- Heating Capacity Ratio Modifier Function of Low Temperature Curve Name
-  VRFHeatCapFTBoundary, !- Heating Capacity Ratio Boundary Curve Name
-  VRFHeatCapFTHi,       !- Heating Capacity Ratio Modifier Function of High Temperature Curve Name
-  VRFHeatEIRFT,         !- Heating Energy Input Ratio Modifier Function of Low Temperature Curve Name
-  VRFHeatEIRFTBoundary, !- Heating Energy Input Ratio Boundary Curve Name
-  VRFHeatEIRFTHi,       !- Heating Energy Input Ratio Modifier Function of High Temperature Curve Name
-  WetBulbTemperature,   !- Heating Performance Curve Outdoor Temperature Type
-  HeatingEIRLowPLR,     !- Heating Energy Input Ratio Modifier Function of Low Part-Load Ratio Curve Name
-  HeatingEIRHiPLR,      !- Heating Energy Input Ratio Modifier Function of High Part-Load Ratio Curve Name
-  HeatingCombRatio,     !- Heating Combination Ratio Correction Factor Curve Name
-  VRFCPLFFPLR,          !- Heating Part-Load Fraction Correlation Curve Name
-  0.25,                 !- Minimum Heat Pump Part-Load Ratio
-  SPACE1-1,             !- Zone Name for Master Thermostat Location
-  LoadPriority,         !- Master Thermostat Priority Control Type
-  ,                     !- Thermostat Priority Schedule Name
-  VRF Heat Pump TU List, !- Zone Terminal Unit List Name
-  No,                   !- Heat Pump Waste Heat Recovery
-  30,                   !- Equivalent Piping Length used for Piping Correction Factor in Cooling Mode {m}
-  10,                   !- Vertical Height used for Piping Correction Factor {m}
-  CoolingLengthCorrectionFactor,  !- Piping Correction Factor for Length in Cooling Mode Curve Name
-  -0.000386,            !- Piping Correction Factor for Height in Cooling Mode Coefficient
-  30,                   !- Equivalent Piping Length used for Piping Correction Factor in Heating Mode {m}
-  ,                     !- Piping Correction Factor for Length in Heating Mode Curve Name
-  ,                     !- Piping Correction Factor for Height in Heating Mode Coefficient
-  15,                   !- Crankcase Heater Power per Compressor {W}
-  3,                    !- Number of Compressors
-  0.33,                 !- Ratio of Compressor Size to Total Compressor Capacity
-  7,                    !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater {C}
-  Resistive,            !- Defrost Strategy
-  Timed,                !- Defrost Control
-  ,                     !- Defrost Energy Input Ratio Modifier Function of Temperature Curve Name
-  ,                     !- Defrost Time Period Fraction
-  autosize,             !- Resistive Defrost Heater Capacity {W}
-  7,                    !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation {C}
-  EvaporativelyCooled,  !- Condenser Type
-  MyVRFOANode,          !- Condenser Inlet Node Name
-  ,                     !- Condenser Outlet Node Name
-  ,                     !- Water Condenser Volume Flow Rate
-  ,                     !- Evaporative Condenser Effectiveness {dimensionless}
-  autosize,             !- Evaporative Condenser Air Flow Rate {m3/s}
-  autosize,             !- Evaporative Condenser Pump Rated Power Consumption {W}
-  ,                     !- Supply Water Storage Tank Name
-  200,                  !- Basin Heater Capacity {W/K}
-  ,                     !- Basin Heater Set Point Temperature (C)
-  ,                     !- Basin Heater Operating Schedule Name
-  ,                     !- Fuel Type
-  ,                     !- Minimum Outdoor Temperature in Heat Recovery Mode (C)
-  ,                     !- Maximum Outdoor Temperature in Heat Recovery Mode (C)
-  ,                     !- Heat Recovery Cooling Capacity Modifier Function of Temperature Curve Name
-  ,                     !- Initial Heat Recovery Cooling Capacity Fraction
-  ,                     !- Heat Recovery Cooling Capacity Time Constant (hr)
-  ,                     !- Heat Recovery Cooling Energy Modifier Function of Temperature Curve Name
-  ,                     !- Initial Heat Recovery Cooling Energy Fraction
-  ,                     !- Heat Recovery Cooling Energy Time Constant (hr)
-  ,                     !- Heat Recovery Heating Capacity Modifier Function of Temperature Curve Name
-  ,                     !- Initial Heat Recovery Heating Capacity Fraction
-  ,                     !- Heat Recovery Heating Capacity Time Constant (hr)
-  ,                     !- Heat Recovery Heating Energy Modifier Function of Temperature Curve Name
-  ,                     !- Initial Heat Recovery Heating Energy Fraction
-  ;                     !- Heat Recovery Heating Energy Time Constant (hr)
-```
-
-
-
-### AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl
-
-#### Field: Heat Pump Name
-
-This alpha field defines a unique user-assigned name for an instance of a variable refrigerant flow heat pump. Any reference to this heat pump will use this name. Since this object is not listed in an AirloopHVAC object, the most likely use of this name would be for reporting purposes.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump operates during a given time period. A schedule value equal to 0 denotes that the heat pump must be off for that time period. A value other than 0 denotes that the heat pump is available to operate during that time period. This schedule may be used to completely disable the heat pump (and all of its terminal units) as required. If this field is blank, the unit is enabled the entire simulation.
-
-#### Field: Zone Terminal Unit List Name
-
-This alpha field defines the name of the zone terminal unit list. The name specified here should match the name of a valid ZoneTerminalUnitList object. In addition, each name specified in this list should match the name of a valid ZoneHVAC:TerminalUnit:VariableRefrigerantFlow object. All terminal units connected to this heat pump must be listed in this ZoneTerminalUnitList object.
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-#### Field: Refrigerant Type
-
-This alpha field defines the name of the refrigerant used in the VRF system. The name specified here should match the name of a valid FluidProperties:Name object.
-
-####Field: Rated Evaporative Capacity
-
-This numeric field defines the total evaporative capacity in watts at rated conditions. This is the capacity corresponding to the max compressor speed at rated conditions. The actual evaporative capacity is obtained by multiplying the rated capacity with the modification factor calculated by Evaporative Capacity Multiplier Function of Temperature Curve. The value must be greater than 0. If this field is left blank, a default value of 40,000 W is assumed.
-
-####Field: Rated Compressor Power Per Unit of Rated Evaporative Capacity
-
-This numeric field defines the rated compressor power per Watt of rated evaporative capacity. Rated compressor power corresponds to the max compressor speed at rated conditions. The actual compressor power is obtained by multiplying the rated power with the modification factor calculated by Compressor Power Multiplier Function of Temperature Curve. The value must be greater than 0. If this field is left blank, a default value of 0.35 W/W is assumed.
-
-####Field: Minimum Outdoor Air Temperature in Cooling Mode
-
-This numeric field defines the minimum outdoor dry-bulb temperature allowed for cooling operation. Below this temperature, cooling is disabled. If this field is left blank, the default value is -6ºC.
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-####Field: Maximum Outdoor Air Temperature in Cooling Mode
-
-This numeric field defines the maximum outdoor dry-bulb temperature allowed for cooling operation. Above this temperature, cooling is disabled. If this field is left blank, the default value is 43ºC.
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-####Field: Minimum Outdoor Air Temperature in Heating Mode
-
-This numeric field defines the minimum outdoor temperature allowed for heating operation. Below this temperature, heating is disabled. If this field is left blank, the default value is -20ºC.
-
-####Field: Maximum Outdoor Air Temperature in Heating Mode
-
-This numeric field defines the maximum outdoor temperature allowed for heating operation. Above this temperature, heating is disabled. If this field is left blank, the default value is 16ºC.
-
-#### Field: Outdoor Unit Reference Superheating
-
-This numeric field defines the reference superheating degrees of the outdoor unit. If this field is blank, the default value of 3.0ºC is used.
-
-#### Field: Outdoor Unit Reference Subcooling
-
-This numeric field defines the reference subcooling degrees of the outdoor unit. If this field is blank, the default value of 3.0ºC is used.
-
-#### Field: Refrigerant Temperature Control Algorithm for Indoor Unit
-
-This alpha field specifies the algorithm for the refrigerant temperature control. Two choices are available: ConstantTemp or VariableTemp. The indoor unit evaporating temperature at cooling mode or condensing temperature at heating are fixed in the ConstantTemp algorithm, while in VariableTemp algorithm they can be varied.
-
-#### Field: Reference Evaporating Temperature for Indoor Unit
-
-This numeric field defines the reference evaporating temperature for the indoor unit when VRF runs at cooling mode. This field is required if Refrigerant Temperature Control Algorithm is ConstantTemp. If this field is blank, the default value of 6.0ºC is used.
-
-#### Field: Reference Condensing Temperature for Indoor Unit
-
-This numeric field defines the reference condensing temperature for the indoor unit when VRF runs at heating mode. This field is required if Refrigerant Temperature Control Algorithm is ConstantTemp. If this field is blank, the default value of 44.0ºC is used.
-
-#### Field: Variable Evaporating Temperature Minimum for Indoor Unit
-
-This numeric field defines the minimum evaporating temperature for the indoor unit when VRF runs at cooling mode. This field is required if Refrigerant Temperature Control Algorithm is VariableTemp. If this field is blank, the default value of 4.0ºC is used.
-
-#### Field: Variable Evaporating Temperature Maximum for Indoor Unit
-
-This numeric field defines the maximum evaporating temperature for the indoor unit when VRF runs at cooling mode. This field is required if Refrigerant Temperature Control Algorithm is VariableTemp. If this field is blank, the default value of 13.0ºC is used.
-
-#### Field: Variable Condensing Temperature Minimum for Indoor Unit
-
-This numeric field defines the minimum condensing temperature for the indoor unit when VRF runs at heating mode. This field is required if Refrigerant Temperature Control Algorithm is VariableTemp. If this field is blank, the default value of 42.0ºC is used.
-
-#### Field: Variable Condensing Temperature Maximum for Indoor Unit
-
-This numeric field defines the maximum condensing temperature for the indoor unit when VRF runs at heating mode. This field is required if Refrigerant Temperature Control Algorithm is VariableTemp. If this field is blank, the default value of 46.0ºC is used.
-
-#### Field: Outdoor Unit Fan Power Per Unit of Rated Evaporative Capacity
-
-This numeric field defines the outdoor unit fan power per watt of rated evaporative capacity. If this field is blank, the default value of 4.25E-3 W/W is used.
-
-#### Field: Outdoor Unit Fan Flow Rate Per Unit of Rated Evaporative Capacity
-
-This numeric field defines the outdoor unit fan volumetric flow rate per watt of rated evaporative capacity. If this field is blank, the default value of 7.50E-5 m<sup>3</sup>/s-W is used.
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-#### Field: Outdoor Unit Evaporating Temperature Function of Superheating Curve Name
-
-This alpha field defines the name of a quadratic performance curve that parameterizes the variation of outdoor unit evaporating temperature as a function of superheating degrees. The output of this curve is the temperature difference between the coil surface air temperature and the evaporating temperature.
-
-#### Field: Outdoor Unit Condensing Temperature Function of Subcooling Curve Name
-
-This alpha field defines the name of a quadratic performance curve that parameterizes the variation of outdoor unit condensing temperature as a function of subcooling degrees. The output of this curve is the temperature difference between the condensing temperature and the coil surface air temperature.
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-#### Field: Diameter of Main Pipe Connecting Outdoor Unit to Indoor Units
-
-This numeric field defines the diameter of main pipe connecting outdoor unit to indoor units. This value is used to calculate the piping loss of the refrigerant when going through the main pipe, including the heat loss and pressure drop. If this field is blank, the default value of 0.0254m is used.
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-#### Field: Length of Main Pipe Connecting Outdoor Unit to Indoor Units
-
-This numeric field defines the length of main pipe connecting outdoor unit to indoor units. This value is used to calculate the heat loss of the refrigerant when going through the main pipe. The value should be greater than 0. If this field is blank, the default value of 30m is used.
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-#### Field: Equivalent Length of Main Pipe Connecting Outdoor Unit to Indoor Units
-
-This numeric field defines the equivalent length of main pipe connecting outdoor unit to indoor units. This value is used to calculate the pressure drop of the refrigerant when going through the main pipe. The value should be greater than the real pipe length specified in the above field. If this field is blank, the default value of 36m is used.
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-#### Field: Height Difference Between Outdoor Unit and Indoor Units
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-This numeric field defines the height difference between the outdoor unit node and indoor unit node of the main pipe. This value is used to calculate the piping loss of the refrigerant when going through the main pipe. The value can be positive, zero, or negative. Positive means outdoor unit is higher than indoor unit, while negative means outdoor unit is lower than indoor unit.
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-#### Field: Main Pipe Insulation Thickness
-
-This numeric field defines the insulation thickness of the main pipe. This value is used to calculate the heat loss of the refrigerant when going through the main pipe. The value should be greater than 0. If this field is blank, the default value of 0.02m is used.
-
-#### Field: Main Pipe Insulation Thermal Conductivity
-
-This numeric field defines the thermal conductivity of the main pipe insulation material. This value is used to calculate the heat loss of the refrigerant when going through the main pipe. The value should be greater than 0. If this field is blank, the default value of 0.032 W/m-K is used.
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-#### Field: Crankcase Heater Power per Compressor
-
-This numeric field defines the electrical power consumed by the crankcase heater in watts for each compressor. This crankcase heater power is consumed to warm the refrigerant and oil when the compressor is off when the outdoor temperature is below the maximum outdoor dry-bulb temperature for crankcase heater operation. The minimum value for this field is 0. If this field is left blank, the default value is 33 watts. Crankcase heater electrical consumption is applied only when the compressor is off or is applied during the off cycle when the compressor is cycling below the Minimum Heat Pump Part-Load Ratio. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
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-#### Field: Number of Compressors
-
-This numeric field defines the number of compressors in the heat pump condensing unit and is used exclusively to determine the operating characteristics of the crankcase heater. For example, if the number of compressors is 3, one crankcase heater will operate when the heat pump condensing unit’s part-load ratio is less than or equal to 0.67 (when the ratio of compressor size to total compressor capacity input is 0.33) and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. Similarly, two crankcase heaters will operate when the heat pump condensing unit’s PLR is less than or equal to 0.33 and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. If the heat pump condensing unit is off, all 3 crankcase heaters will operate if the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. The minimum value for this field is 1. If this field is left blank, the default value is 2. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
-
-#### Field: Ratio of Compressor Size to Total Compressor Capacity
-
-This numeric field defines the size of the first stage compressor to the total compressor capacity and is used exclusively for calculating crankcase heater energy. If this field and the previous field are left blank, the default value is 0.5.  If this field is left blank and the previous field is not blank, the compressors are assumed to be equally sized. When the number of compressors is greater than 2, the 2<sup>nd</sup> stage compressor and all additional compressors are assumed to be equally sized. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
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-#### Field: Maximum Outdoor Dry-bulb Temperature for Crankcase Heater
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-This numeric field defines the maximum outdoor temperature, in degrees Celsius, below which the crankcase heater will operate. If this field is left blank, the default value is 5°C. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
-
-#### Field: Defrost Strategy
-
-This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse-cycle. Defrost can be disabled by entering a resistive defrost strategy using a timed defrost control, a 0 defrost time period fraction and a 0 resistive defrost heater capacity in the following inputs fields. This method is used when the Maximum Outdoor Dry-Bulb Temperature for Defrost Operation field value is greater than the expected minimum outdoor dry-bulb temperature simulated in the weather file.
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-#### Field: Defrost Control
-
-This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value of compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field “Defrost Time Period Fraction� described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field “Maximum Outdoor Dry-bulb Temperature for Defrost Operation� described above. If this input field is left blank, the default defrost control is timed.
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-#### Field: Defrost Energy Input Ratio Modifier Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) during reverse-cycle defrost periods as a function of the outdoor air dry-bulb temperature and the weighted average wet-bulb temperature of the air entering the indoor terminal units. The output of this curve is multiplied by the coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the indoor and outdoor coils are operating. The curve is normalized to a value of 1.0 at the rating point conditions.
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-#### Field: Defrost Time Period Fraction
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-This numeric field defines the fraction of compressor runtime when the defrost cycle is active. For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
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-#### Field: Resistive Defrost Heater Capacity
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-This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is ‘resistive’ (see input field “Defrost Strategy� above). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.
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-#### Field: Maximum Outdoor Dry-bulb Temperature for Defrost Operation
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-This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. If this input field is left blank, the default value is 5°C. Defrost can be completely eliminated by selecting a temperature lower than the minimum expected outdoor temperature found in the weather file.
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-#### Field: Compressor maximum delta Pressure
-
-This numeric field defines the maximum pressure increase that the compressor can provide. The value should be greater than 0. If this field is blank, the default value of 4,500,000 Pa is used.
-
-#### Field: Number of Compressor Loading Index Entries
-
-This numeric field defines the number of compressor loading index entries. Loading index specifies the VRF operational modes at various load conditions. In a single compressor system, loading index reflects the compressor speed. The model requires at least two loading indices. The first index represents the minimal capacity operation, while the last index represents full capacity operation.
-
-#### Field: Compressor Speed at Loading Index i
-
-This numeric field defines the compressor speed at the i-th loading index. The value must be greater than 0.
-
-#### Field: Loading Index i Evaporative Capacity Multiplier Function of Temperature Curve Name
-
-This alpha field defines the name of a BiQuadratic curve for the VRF operational mode corresponding to the i-th loading index. It parameterizes the variation of VRF evaporating capacity as a function of operating conditions, i.e., evaporating and condensing temperatures. The output of this curve is a dimensionless multiplier to be applied on the rated evaporative capacity to calculate the actual capacity.
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-#### Field: Loading Index i Compressor Power Multiplier Function of Temperature Curve Name
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-This alpha field defines the name of a BiQuadratic curve for the VRF operational mode corresponding to the i-th loading index. It parameterizes the variation of compressor power as a function of operating conditions, i.e., evaporating and condensing temperatures. The output of this curve is a dimensionless multiplier to be applied on the rated compressor power to calculate the actual compressor power.
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-Following is an example input for a AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl system.
-
-
-```idf
-
-  AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl,
-    VRF Heat Pump,           !- Heat Pump Name
-    VRFCondAvailSched,       !- Availability Schedule Name
-    VRF Heat Pump TU List,   !- Zone Terminal Unit List Name
-    R410A,                   !- Refrigerant Type
-    41300,                   !- Rated Evaporative Capacity {W}
-    0.344,                   !- Rated Compressor Power Per Unit of Rated Evaporative Capacity {W/W}
-    ,                        !- Minimum Outdoor Air Temperature in Cooling Mode {C}
-    ,                        !- Maximum Outdoor Air Temperature in Cooling Mode {C}
-    ,                        !- Minimum Outdoor Air Temperature in Heating Mode {C}
-    ,                        !- Maximum Outdoor Air Temperature in Heating Mode {C}
-    3,                       !- Reference Outdoor Unit Superheating Degrees {C}
-    3,                       !- Reference Outdoor Unit Subcooling Degrees {C}
-    VariableTemp,            !- Refrigerant Temperature Control Algorithm for Indoor Unit
-    ,                        !- Reference Evaporating Temperature for Indoor Unit {C}
-    ,                        !- Reference Condensing Temperature for Indoor Unit {C}
-    6,                       !- Variable Evaporating Temperature Minimum for Indoor Unit {C}
-    13,                      !- Variable Evaporating Temperature Maximum for Indoor Unit {C}
-    42,                      !- Variable Condensing Temperature Minimum for Indoor Unit {C}
-    46,                      !- Variable Evaporating Temperature Maximum for Indoor Unit {C}
-    4.12E-3,                 !- Outdoor Unit Fan Power Per Unit of Rated Evaporative Capacity {W/W}
-    7.26E-5,                 !- Outdoor Unit Fan Flow Rate Per Unit of Rated Evaporative Capacity {m3/s-W}
-    OUEvapTempCurve,         !- Outdoor Unit Evaporating Temperature Function of Superheating Curve Name
-    OUCondTempCurve,         !- Outdoor Unit Condensing Temperature Function of Subcooling Curve Name
-    0.0508,                  !- Diameter of main pipe connecting outdoor unit to indoor units {m}
-    30,                      !- Length of main pipe connecting outdoor unit to indoor units {m}
-    36,                      !- Equivalent length of main pipe connecting outdoor unit to indoor units {m}
-    5,                       !- Height difference between the outdoor unit node and indoor unit node of the main pipe {m}
-    0.02,                    !- Insulation thickness of the main pipe {m}
-    0.032,                   !- Thermal conductivity of the main pipe insulation material {W/m-K}
-    33,                      !- Crankcase Heater Power per Compressor {W}
-    1,                       !- Number of Compressors
-    0.33,                    !- Ratio of Compressor Size to Total Compressor Capacity
-    7,                       !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater {C}
-    ,                        !- Defrost Strategy
-    ,                        !- Defrost Control
-    ,                        !- Defrost Energy Input Ratio Modifier Function of Temperature Curve Name
-    ,                        !- Defrost Time Period Fraction
-    ,                        !- Resistive Defrost Heater Capacity {W}
-    ,                        !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation {C}
-    4500000,                 !- Compressor maximum delta Pressure {Pa}
-    3,                       !- Number of Compressor Loading Index Entries
-    1500,                    !- Compressor Speed at Loading Index 1 {rev/min}
-    MinSpdCooling,           !- Loading Index 1 Evaporative Capacity Multiplier Function of Temperature Curve Name
-    MinSpdPower,             !- Loading Index 1 Compressor Power Multiplier Function of Temperature Curve Name
-    3600,                    !- Compressor Speed at Loading Index 2 {rev/min}
-    Spd1Cooling,             !- Loading Index 2 Evaporative Capacity Multiplier Function of Temperature Curve Name
-    Spd1Power,               !- Loading Index 2 Compressor Power Multiplier Function of Temperature Curve Name
-    6000,                    !- Compressor Speed at Loading Index 3 {rev/min}
-    Spd2Cooling,             !- Loading Index 3 Evaporative Capacity Multiplier Function of Temperature Curve Name
-    Spd2Power;               !- Loading Index 3 Compressor Power Multiplier Function of Temperature Curve Name
-
-  Curve:Quadratic,
-    OUEvapTempCurve,         !- Name
-    0,                       !- Coefficient1 Constant
-    6.05E-1,                 !- Coefficient2 x
-    2.50E-2,                 !- Coefficient3 x**2
-    0,                       !- Minimum Value of x
-    15,                      !- Maximum Value of x
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature;             !- Output Unit Type
-
-  Curve:Quadratic,
-    OUCondTempCurve,         !- Name
-    0,                       !- Coefficient1 Constant
-    -2.91,                   !- Coefficient2 x
-    1.180,                   !- Coefficient3 x**2
-    0,                       !- Minimum Value of x
-    20,                      !- Maximum Value of x
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature;             !- Output Unit Type
-
-  Curve:Biquadratic,
-    MinSpdCooling,           !- Name
-    3.19E-01,                !- Coefficient1 Constant
-    -1.26E-03,               !- Coefficient2 x
-    -2.15E-05,               !- Coefficient3 x**2
-    1.20E-02,                !- Coefficient4 y
-    1.05E-04,                !- Coefficient5 y**2
-    -8.66E-05,               !- Coefficient6 x*y
-    15,                      !- Minimum Value of x
-    65,                      !- Maximum Value of x
-    -30,                     !- Minimum Value of y
-    15,                      !- Maximum Value of y
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature,             !- Input Unit Type for Y
-    Dimensionless;           !- Output Unit Type
-
-  Curve:Biquadratic,
-    MinSpdPower,             !- Name
-    8.79E-02 ,               !- Coefficient1 Constant
-    -1.72E-04,               !- Coefficient2 x
-    6.93E-05 ,               !- Coefficient3 x**2
-    -3.38E-05,               !- Coefficient4 y
-    -8.10E-06,               !- Coefficient5 y**2
-    -1.04E-05,               !- Coefficient6 x*y
-    15,                      !- Minimum Value of x
-    65,                      !- Maximum Value of x
-    -30,                     !- Minimum Value of y
-    15,                      !- Maximum Value of y
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature,             !- Input Unit Type for Y
-    Dimensionless;           !- Output Unit Type
-
-  Curve:Biquadratic,
-    Spd1Cooling,             !- Name
-    8.12E-01 ,               !- Coefficient1 Constant
-    -4.23E-03,               !- Coefficient2 x
-    -4.11E-05,               !- Coefficient3 x**2
-    2.97E-02 ,               !- Coefficient4 y
-    2.67E-04 ,               !- Coefficient5 y**2
-    -2.23E-04,               !- Coefficient6 x*y
-    15,                      !- Minimum Value of x
-    65,                      !- Maximum Value of x
-    -30,                     !- Minimum Value of y
-    15,                      !- Maximum Value of y
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature,             !- Input Unit Type for Y
-    Dimensionless;           !- Output Unit Type
-
-  Curve:Biquadratic,
-    Spd1Power,               !- Name
-    3.26E-01 ,               !- Coefficient1 Constant
-    -2.20E-03,               !- Coefficient2 x
-    1.42E-04 ,               !- Coefficient3 x**2
-    2.82E-03 ,               !- Coefficient4 y
-    2.86E-05 ,               !- Coefficient5 y**2
-    -3.50E-05,               !- Coefficient6 x*y
-    15,                      !- Minimum Value of x
-    65,                      !- Maximum Value of x
-    -30,                     !- Minimum Value of y
-    15,                      !- Maximum Value of y
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature,             !- Input Unit Type for Y
-    Dimensionless;           !- Output Unit Type
-
-  Curve:Biquadratic,
-    Spd2Cooling,             !- Name
-    1.32E+00 ,               !- Coefficient1 Constant
-    -6.20E-03,               !- Coefficient2 x
-    -7.10E-05,               !- Coefficient3 x**2
-    4.89E-02 ,               !- Coefficient4 y
-    4.59E-04 ,               !- Coefficient5 y**2
-    -3.67E-04,               !- Coefficient6 x*y
-    15,                      !- Minimum Value of x
-    65,                      !- Maximum Value of x
-    -30,                     !- Minimum Value of y
-    15,                      !- Maximum Value of y
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature,             !- Input Unit Type for Y
-    Dimensionless;           !- Output Unit Type
-
-  Curve:Biquadratic,
-    Spd2Power,               !- Name
-    6.56E-01 ,               !- Coefficient1 Constant
-    -3.71E-03,               !- Coefficient2 x
-    2.07E-04 ,               !- Coefficient3 x**2
-    1.05E-02 ,               !- Coefficient4 y
-    7.36E-05 ,               !- Coefficient5 y**2
-    -1.57E-04,               !- Coefficient6 x*y
-    15,                      !- Minimum Value of x
-    65,                      !- Maximum Value of x
-    -30,                     !- Minimum Value of y
-    15,                      !- Maximum Value of y
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature,             !- Input Unit Type for Y
-    Dimensionless;           !- Output Unit Type
-
-```
-
-
-### Variable Refrigerant Flow (VRF) Air Conditioner Outputs
-
-* HVAC,Average,VRF Heat Pump Total Cooling Rate [W]
-
-* HVAC,Average,VRF Heat Pump Total Heating Rate [W]
-
-* HVAC,Average,VRF Heat Pump Cooling COP []
-
-* HVAC,Average,VRF Heat Pump Heating COP []
-
-* HVAC,Average,VRF Heat Pump COP []
-
-* HVAC,Average,VRF Heat Pump Part Load Ratio []
-
-* HVAC,Average,VRF Heat Pump Runtime Fraction []
-
-* HVAC,Average,VRF Heat Pump Cycling Ratio []
-
-* HVAC,Average,VRF Heat Pump Operating Mode []
-
-* HVAC,Average,VRF Heat Pump Condenser Inlet Temperature [C]
-
-* HVAC,Average,VRF Heat Pump Maximum Capacity Cooling Rate [W]
-
-* HVAC,Average,VRF Heat Pump Maximum Capacity Heating Rate [W]
-
-* HVAC,Average,VRF Heat Pump Crankcase Heater Electric Power [W]
-
-* HVAC,Sum,VRF Heat Pump Crankcase Heater Electric Energy [J]
-
-* HVAC,Average,VRF Heat Pump Terminal Unit Heating Load Rate [W]
-
-* HVAC,Average,VRF Heat Pump Terminal Unit Cooling Load Rate [W]
-
-
-
-Heat Recovery:
-
-* HVAC,Average,VRF Heat Pump Heat Recovery Status Change Multiplier []
-
-
-
-Evap-cooled:
-
-* HVAC,Sum,VRF Heat Pump Evaporative Condenser Water Use Volume [m3]
-
-* HVAC,Average,VRF Heat Pump Evaporative Condenser Pump Electric Power [W]
-
-* HVAC,Sum,VRF Heat Pump Evaporative Condenser Pump Electric Energy [J]
-
-* HVAC,Average,VRF Heat Pump Basin Heater Electric Power [W]
-
-* HVAC,Average,VRF Heat Pump Basin Heater Electric Energy [J]
-
-* HVAC,Average,VRF Heat Pump Heat Recovery Status Change Multiplier []
-
-
-
-Water-cooled:
-
-* HVAC,Average,VRF Heat Pump Condenser Outlet Temperature [C]
-
-* HVAC,Average,VRF Heat Pump Condenser Mass Flow Rate [kg/s]
-
-* HVAC,Sum,VRF Heat Pump Condenser Heat Transfer Energy [J]
-
-* HVAC,Average, VRF Heat Pump Condenser Heat Transfer Rate [W]
-
-
-
-Electric Fuel type (default):
-
-* HVAC,Average,VRF Heat Pump Cooling Electric Power [W]
-
-* HVAC,Sum,VRF Heat Pump Cooling Electric Energy [J]
-
-* HVAC,Average,VRF Heat Pump Heating Electric Power [W]
-
-* HVAC,Sum,VRF Heat Pump Heating Electric Energy [J]
-
-
-
-Electric defrost always used for Defrost Strategy = Resistive regardless of fuel type
-
-* HVAC,Average,VRF Heat Pump Defrost Electric Power [W]
-
-* HVAC,Sum,VRF Heat Pump Defrost Electric Energy [J]
-
-
-
-Alternate Fuel types (e.g., FuelType = NaturalGas):
-
-* HVAC,Average,VRF Heat Pump Cooling &lt;FuelType&gt; Rate [W]
-
-* HVAC,Sum,VRF Heat Pump Cooling &lt;FuelType&gt; Energy [J]
-
-* HVAC,Average,VRF Heat Pump Heating &lt;FuelType&gt; Rate [W]
-
-* HVAC,Sum,VRF Heat Pump Heating &lt;FuelType&gt; Energy [J]
-
-* HVAC,Average,VRF Heat Pump Defrost &lt;FuelType&gt; Rate [W]
-
-* HVAC,Sum,VRF Heat Pump Defrost &lt;FuelType&gt; Energy [J]
-
-
-
-For the pysics based VRF model (VRF-FluidTCtrl) only:
-
-* VRF Heat Pump Indoor Unit Evaporating Temperature at Cooling Mode [C]
-
-* VRF Heat Pump Outdoor Unit Condensing Temperature at Cooling Mode [C]
-
-* VRF Heat Pump Indoor Unit Condensing Temperature at Heating Mode [C]
-
-* VRF Heat Pump Outdoor Unit Evaporating Temperature at Heating Mode [C]
-
-* VRF Heat Pump Compressor Electric Power at Cooling Mode [W]
-
-* VRF Heat Pump Compressor Electric Power at Heating Mode [W]
-
-* VRF Heat Pump Compressor Rotating Speed [rev/min]
-
-* VRF Heat Pump Outdoor Unit Fan Power [W]
-
-
-Note: refer to the rdd file after a simulation for exact output variable names
-
-
-
-#### VRF Heat Pump Total Cooling Rate  [W]
-
-This output field is the operating total cooling capacity of the variable refrigerant flow heat pump in Watts. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. This value should match the sum of the individual zone terminal unit output variables for Zone VRF Air Terminal Total Cooling Rate.
-
-#### VRF Heat Pump Total Heating Rate [W]
-
-This output field is the operating total heating capacity of the variable refrigerant flow heat pump in Watts. The capacity includes any degradation due to defrost mode. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. This value should match the sum of the individual zone terminal unit output variables for Zone VRF Air Terminal Total Heating Rate.
-
-#### VRF Heat Pump Cooling Electric Power [W]
-
-This output field is the cooling mode electricity consumption rate of the variable refrigerant flow heat pump in Watts. The consumption includes electricity used by the compressor and the condenser fan. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump Cooling NaturalGas Consumption Rate).
-
-#### VRF Heat Pump Cooling Electric Energy [J]
-
-This output field is the cooling mode electricity consumption of the variable refrigerant flow heat pump in Joules for the time period being reported. The consumption includes electricity used by the compressor and the condenser fan. This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (Ref. Output:Meter objects). The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump Cooling NaturalGas Consumption). The resource type meter will also be modified to reflect the chosen fuel type (e.g., Resource Type = NaturalGas).
-
-#### VRF Heat Pump Heating Electric Power [W]
-
-This output field is the heating mode electricity consumption rate of the variable refrigerant flow heat pump in Watts. The consumption includes electricity used by the compressor (including crankcase heater), additional energy required for defrost, and the condenser fan. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump Heating NaturalGas Consumption Rate).
-
-#### VRF Heat Pump Heating Electric Energy [J]
-
-This output field is the heating mode electricity consumption of the variable refrigerant flow heat pump in Joules for the time period being reported. The consumption includes electricity used by the compressor (including crankcase heater), additional energy required for defrost, and the condenser fan. This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (Ref. Output:Meter objects). The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump Heating NaturalGas Consumption). The resource type meter will also be modified to reflect the chosen fuel type (e.g., Resource Type = NaturalGas).
-
-#### VRF Heat Pump Cooling COP[]
-
-This is the operating cooling coefficient of performance for the heat pump. This value is calculated using the ratio of VRF Heat Pump Total Cooling Rate and Variable Refrigerant Flow Heat Pump Cooling Electric Consumption Rate output variables. Crankcase heater (usually 0 in cooling mode), evaporative condenser water pump, and defrost (usually 0 in cooling mode) consumption rate output variables are included in this calculation. This value is specific to outdoor unit performance in cooling mode, is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### VRF Heat Pump Heating COP[]
-
-This is the operating heating coefficient of performance for the heat pump. This value is calculated using the ratio of VRF Heat Pump Total Heating Rate and Variable Refrigerant Flow Heat Pump Heating Electric Consumption Rate output variables. Crankcase heater, evaporative condenser water pump (usually 0 in heating mode), and defrost consumption rate output variables are included in this calculation. This value is specific to outdoor unit performance in heating mode, is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### VRF Heat Pump COP[]
-
-This is the operating coefficient of performance for the heat pump. This value is calculated using the ratio of the total terminal unit coil capacity (cooling plus heating and accounts for piping losses) and total system electric consumption rate (compressor, crankcase heater, evaporative condenser water pump, defrost, and terminal unit parasitic electric consumption rate). This output variable does not include pump power for a water-cooled system. This value is specific to overall system performance, is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### VRF Heat Pump Defrost Electric Power [W]
-
-This is the electricity consumption rate of the heat pump defrost in Watts when the unit is in defrost mode (timed, reverse-cycle). . The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump NaturalGas Defrost Consumption Rate).
-
-#### VRF Heat Pump Defrost Electric Energy [J]
-
-This is the electricity consumption of the heat pump in Joules for the time step being reported. This consumption is applicable when the unit is in defrost mode (reverse-cycle or resistive). This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (Ref. Output:Meter objects). The choice of an alternate fuel type (see Fuel Type input) will result in a change in the output variable name (e.g., Variable Refrigerant Flow Heat Pump NaturalGas Defrost Consumption). The resource type meter will also be modified to reflect the chosen fuel type (e.g., Resource Type = NaturalGas).
-
-#### VRF Heat Pump Part Load Ratio
-
-This output field is the part-load ratio of the heat pump condenser. Heat pump part-load ratio is defined as the total coil load divided by the heat pump’s maximum available capacity at the current operating conditions. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### VRF Heat Pump Runtime Fraction []
-
-This output field is the runtime fraction of the heat pump condenser’s first stage compressor. Heat pump runtime fraction is defined as the fraction of time the first stage compressor is on during a given time period and includes cycling losses. This value is calculated as the ratio of the VRF Heat Pump Cycling Ratio and the output of the Cooling Part-Load Fraction Correlation Curve object as the specific cycling ratio. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### VRF Heat Pump Cycling Ratio []
-
-This output field is the cycling ratio of the heat pump condenser’s first stage compressor. Heat pump cycling ratio is defined as the fraction of time the first stage compressor is on during a given time period. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### VRF Heat Pump Operating Mode []
-
-This output field is an integer representation of the operating mode of the variable refrigerant flow heat pump. The operating mode for cooling mode is indicated by a 1 and heating mode is indicated by a 2. A value of 0 is reported if the heat pump is off. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported.
-
-#### VRF Heat Pump Condenser Inlet Temperature [C]
-
-This is the inlet air temperature entering the condenser coil in degrees C. This value can represent the outdoor air dry-bulb temperature, wet-bulb temperature, or somewhere in between from the weather data being used, depending on the value used in the input field “Evaporative Condenser Effectiveness�. The temperature reported here is used in the various modifier curves related to temperature (e.g., Total Cooling Capacity Modifier Curve [function of temperature]). (The use of the word *Condenser* here is taken from cooling operation -- the same device can also be an evaporator during heating operation.)
-
-#### VRF Heat Pump Condenser Outlet Temperature [C]
-
-This is the condenser coil outlet water temperature in degrees C. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. This value is only reported for water-cooled systems.  (The use of the word *Condenser* here is taken from cooling operation -- the same device can also be an evaporator during heating operation.)
-
-#### VRF Heat Pump Condenser Mass Flow Rate [kg/s]
-
-This is the condenser coil outlet water mass flow rate in kilograms per second. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. This value is only reported for water-cooled systems. (The use of the word *Condenser* here is taken from cooling operation -- the same device can also be an evaporator during heating operation.)
-
-#### VRF Heat Pump Condenser Heat Transfer Rate [W]
-
-This is the condenser coil heat transfer rate in Watts. This value is calculated for each HVAC system time step being simulated, and the results are averaged for the time step being reported. This value is only reported for water-cooled systems. (The use of the word *Condenser* here is taken from cooling operation -- the same device can also be an evaporator during heating operation.)
-
-#### VRF Heat Pump Condenser Heat Transfer Energy [J]
-
-This is the condenser coil heat transfer in Joules. This value is calculated for each HVAC system time step being simulated, and the results are summed for the time step being reported. This value is only reported for water-cooled systems. (The use of the word *Condenser* here is taken from cooling operation -- the same device can also be an evaporator during heating operation.)
-
-#### VRF Heat Pump Maximum Capacity Cooling Rate [W]
-
-This output field is the maximum available terminal unit cooling capacity in Watts allowed for the current time step being reported. If the terminal units request more capacity than is actually available from the variable refrigerant flow heat pump, the individual terminal units will be limited to this value. A maximum limit of 1E+20 is reported when there is sufficient capacity available to meet all requests from the terminal units. This output variable easily identifies times when the total terminal unit cooling load exceeds the heat pump’s available cooling capacity.
-
-#### VRF Heat Pump Maximum Capacity Heating Rate [W]
-
-This output field is the maximum available terminal unit heating capacity in Watts allowed for the current time step being reported. If the terminal units request more capacity than is actually available from the variable refrigerant flow heat pump, the individual terminal units will be limited to this value. A maximum limit of 1E+20 is reported when there is sufficient capacity available to meet all requests from the terminal units. This output variable easily identifies times when the total terminal unit heating load exceeds the heat pump’s available heating capacity.
-
-#### VRF Heat Pump Terminal Unit Cooling Load Rate [W]
-
-This output field is the sum of the terminal unit cooling coil loads in Watts for the current time step being reported. This value is derived directly from the cooling coils and represents the total cooling load on the VRF system after piping losses have been accounted for. The total cooling load will be less than the variable refrigerant flow total cooling capacity reported when piping losses are modeled (i.e., when piping losses are &lt; 1).
-
-#### VRF Heat Pump Terminal Unit Heating Load Rate [W]
-
-This output field is the sum of the terminal unit heating coil loads in Watts for the current time step being reported. This value is derived directly from the heating coils and represents the total heating load on the VRF system after piping losses have been accounted for. The total heating load will be less than the variable refrigerant flow total heating capacity reported when piping losses are modeled (i.e., when piping losses are &lt; 1).
-
-#### VRF Heat Pump Crankcase Heater Electric Power [W]
-
-This output field is the average electricity consumption rate of the heat pump’s crankcase heaters in Watts for the time step being reported.
-
-#### VRF Heat Pump Crankcase Heater Electric Energy [J]
-
-This output field is the electricity consumption rate of the heat pump’s crankcase heaters in Joules for the time step being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
-
-#### VRF Heat Pump Evaporative Condenser Water Use Volume [m3]
-
-This output is the amount of water used to evaporatively cool the condenser coil inlet air, in cubic meters. This output is also added to a meter with Resource Type = Water, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
-
-#### VRF Heat Pump Evaporative Condenser Pump Electric Power [W]
-
-This is the average electricity consumption rate of the evaporative condenser water pump in Watts for the time step being reported.
-
-#### VRF Heat Pump Evaporative Condenser Pump Electric Energy [J]
-
-This is the electricity consumption rate of the evaporative condenser water pump in Joules for the time step being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
-
-#### VRF Heat Pump Basin Heater Electric Power [W]
-
-This output is the electric consumption rate of the heat pump’s basin heater (for evaporatively-cooled condenser type) in Watts. This basin heater only operates when the variable refrigerant flow heat pump’s compressor(s) is off and therefore is reported as 0 anytime the compressor operates. If the compressor is cycling (see VRF Heat Pump Cycling Ratio output variable above), the basin heater electric power is proportional to one minus the cycling ratio of the compressor (i.e., the basin heater is on when the compressor is off).
-
-#### VRF Heat Pump Basin Heater Electric Energy [J]
-
-This output is the electric consumption of the heat pump’s basin heater (for evaporatively-cooled condenser type) in Joules. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (Ref. Output:Meter objects).
-
-#### VRF Heat Pump Heat Recovery Status Change Multiplier []
-
-This output applies only when heat recovery is used and represents the multiplier used to derate the capacity of the system when transitioning from cooling or heating mode to heat recovery mode. This value is 1 when derating does not apply (i.e., the system has not recently changed modes to provide heat recovery). Derating during a transition period is applied according to the inputs for Heat Recovery Fraction and Heat Recovery Time Constant. To turn transition derating off, set Heat Recovery Fraction to 1. Refer to the engineering reference document discussion on the variable refrigerant flow heat pump model section for transition from cooling only mode to heat recovery mode for a more detailed description.
-
-
-#### VRF Heat Pump Indoor Unit Evaporating Temperature at Cooling Mode [C]
-
-This output only applies for the VRF-FluidTCtrl model. This is the evaporating temperature of the VRF system operating at cooling mode. This value is manipulated by the VRF system considering the load conditions of all the zones it serves. It affects the indoor unit cooling coil surface temperature and thus the cooling capacity of the indoor unit. It also affects the compressor operating conditions and thus the compressor energy consumption.
-
-#### VRF Heat Pump Outdoor Unit Condensing Temperature at Cooling Mode [C]
-
-This output only applies for the VRF-FluidTCtrl model. This is the condensing temperature of the VRF system operating at cooling mode. This value is related with the outdoor air conditions as well as the system operational mode. It affects the condensing capacity of the outdoor unit. It also affects the compressor operating conditions and thus the compressor energy consumption.
-
-#### VRF Heat Pump Indoor Unit Condensing Temperature at Heating Mode [C]
-
-This output only applies for the VRF-FluidTCtrl model. This is the condensing temperature of the VRF system operating at heating mode. This value is manipulated by the VRF system considering the load conditions of all the zones it serves. It affects the indoor unit heating coil surface temperature and thus the heating capacity of the indoor unit. It also affects the compressor operating conditions and thus the compressor energy consumption.
-
-#### VRF Heat Pump Outdoor Unit Evaporating Temperature at Heating Mode [C]
-
-This output only applies for the VRF-FluidTCtrl model. This is the evaporating temperature of the VRF system operating at heating mode. This value is related with the outdoor air conditions as well as the system operational mode. It affects the evaporating capacity of the outdoor unit. It also affects the compressor operating conditions and thus the compressor energy consumption.
-
-#### VRF Heat Pump Compressor Electric Power at Cooling Mode [W]
-
-This output only applies for the VRF-FluidTCtrl model. This is the electric power of the compressor running at the cooling mode. This value is related with the compressor speed as well as the operational conditions, i.e., evaporating and condensing temperatures of the system.
-
-#### VRF Heat Pump Compressor Electric Power at Heating Mode [W]
-
-This output only applies for the VRF-FluidTCtrl model. This is the electric power of the compressor running at the heating mode. This value is related with the compressor speed as well as the operational conditions, i.e., evaporating and condensing temperatures of the system.
-
-#### VRF Heat Pump Compressor Rotating Speed [rev/min]
-
-This output only applies for the VRF-FluidTCtrl model. This is the rotating speed of the compressor, which indicates the loading index.
-
-#### VRF Heat Pump Outdoor Unit Fan Power [W]
-
-This output only applies for the VRF-FluidTCtrl model. This is the power consumed by the fan located in the VRF outdoor unit.
-
-
-
-### ZoneTerminalUnitList
-
-The zone terminal unit list defines the names of the terminal units connected to a single variable refrigerant flow air-conditioning system. The zone terminal unit list is used exclusively in the variable refrigerant flow (VRF) air conditioner object (ref: AirConditioner:VariableRefrigerantFlow). Up to 20 terminal units may be connected to a single VRF outdoor condensing unit. This list is extensible if additional indoor terminal units are required. The name of this zone terminal unit list object is then input into the corresponding variable refrigerant flow air conditioner object. The following figure demonstrates this concept.
-
-![ZoneTUObjectSchematic](media/image313.png)
-
-Figure 127. Zone Terminal Unit List Diagram
-
-#### Field: Zone Terminal List Name
-
-This alpha field specifies the name of the zone terminal unit list. This name must be specified in the AirConditioner:VariableRefrigerantFlow object.
-
-#### Field: Zone Terminal Unit Name &lt;x&gt;
-
-This alpha field defines the name of the zone terminal unit used in a variable refrigerant air conditioner. The zone terminal unit must be connected to a zone using the ZoneHVAC:EquipmentConnections object. The terminal unit air inlet node is the same name as a zone exhaust node. The terminal unit air outlet node is the same name as a zone inlet node. The IDD is supplied with 20 fields for this.  The object is extensible and you can change the IDD by adding more fields or, if you are using text editor for your input file, just add to the list of names.
-
-Following is an example input for a ZoneTerminalUnitList object.
-
-```idf
-ZoneTerminalUnitList,
-   VRF Heat Pump TU List, !- Zone Terminal Unit List Name
-   TU3,                   !- Zone Terminal Unit Name 1
-   TU4,                   !- Zone Terminal Unit Name 2
-   TU1,                   !- Zone Terminal Unit Name 3
-   TU2,                   !- Zone Terminal Unit Name 4
-   TU5;                   !- Zone Terminal Unit Name 5
-```
-
-
-Group – Radiative **/** Convective Units
-----------------------------------------
-
-This section describes the radiative/convective zone equipment units.  The following units are included in this section:
-
-- ZoneHVAC:Baseboard:Convective:Electric
-
-- ZoneHVAC:Baseboard:RadiantConvective:Water
-
-- ZoneHVAC:Baseboard:RadiantConvective:Steam
-
-- ZoneHVAC:Baseboard:RadiantConvective:Electric
-
-- ZoneHVAC:Baseboard:Convective:Water
-
-- ZoneHVAC:HighTemperatureRadiant
-
-- ZoneHVAC:LowTemperatureRadiant:ConstantFlow
-
-- ZoneHVAC:LowTemperatureRadiant:Electric
-
-- ZoneHVAC:LowTemperatureRadiant:VariableFlow
-
-### ZoneHVAC:Baseboard:RadiantConvective:Water
-
-The objective of this model is to calculate the convective and radiant heat transfer from water baseboard heaters to the people and the surfaces within a zone so that surface heat balances can take into account the radiant heat transfer to the surfaces and thus enhance the accuracy of thermal comfort predictions within the space. The radiant heat gains are distributed to the surfaces by fractions defined by user input.
-
-#### Field: Name
-
-A unique user assigned name for an instance of a hot water baseboard heater unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the hot water baseboard heater unit can run during a given time period. A schedule value equal to 0 denotes that the unit must be off for that time period. A value greater than 0 denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Inlet Node Name
-
-This field is the name of the hot water inlet node for the baseboard heater.
-
-#### Field: Outlet Node Name
-
-This field is the name of the hot water outlet node for the baseboard heater.
-
-#### Field: Rated AverageWaterTemperature
-
-This field is the rated average water temperature for the baseboard heater which is published in the manufacturer’s literature in degree Celsius. It typically ranges from 65.56°C to 115.36°C in the I=B=R rating document while the lowest allowable temperature is 32.22°C. The default value is 87.78°C. If the user does not enter this field, the default value is assumed.
-
-#### Field: Rated Water Mass Flow Rate
-
-This field is the rated standard water flow rate in kg/s which is published as part of the manufacturer’s literature. It is used by the manufacturers when determining the rated capacity (see next field). The default value is 0.063kg/s. If it is blank or zero, the default values is assumed.
-
-#### Field: Heating Design Capacity Method
-
-Enter the method used to determine the heating design capacity or the method for scalable sizing. Input allowed is either *HeatingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedHeatingCapacity*. If this input field is left blank or zero, then autosizing is assumed. *HeatingDesignCapacity* means user specifies the magnitude of heating capacity or the program calculates the design heating capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the radiant baseboard unit. *FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is *HeatingDesignCapacity*.
-
-#### Field: Heating Design Capacity {W}
-
-This field is the radiant-convective water baseboard rated capacity in watts at a rated water mass flow rate (see input field Rated Mass Flow Rate). Almost all publications from manufacturers indicate it as W/m (Btuh per linear foot). The user thus must multiply it by the active length of the unit. The active length is available in the literature. Manufacturers are required to publish the difference between active and total length of the unit (I=B=R rating for boilers baseboard radiation, 2009).If it is blank or zero, autosizing is assumed. Design day sizing run must be specified for autosizing.
-
-#### Field: Heating Design Capacity Per Floor Area {W/m2}
-
-Enter the rated heating capacity per unit floor area of radiant-convective water baseboard unit in m3/s-m2. This field is required field when the Heating Design Capacity Method is *CapacityPerFloorArea*. The program calculates the heating capacity from floor area of the zone served by the radiant baseboard unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
-
-#### Field: Fraction of Autosized Heating Design Capacity {-}
-
-Enter the heating capacity as a fraction of the autosized heating capacity of radiant-convective water baseboard. This input field is required when the Heating Design Capacity Method is *FractionOfAutosizedHeatingCapacity*. The program calculates the heating capacity from the design autosized heating capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
-
-#### Field: Maximum Water Flow Rate
-
-This field is the maximum water volumetric flow rate in m<sup>3</sup>/sec.  It can be autosized by EnergyPlus.
-
-#### Field: Convergence Tolerance
-
-This field is the control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. For hot water baseboards, the model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {({Q_{bb,out}} - {Q_{ZoneLoad}})} \right|}}{{{Q_{ZoneLoad}}}} \le Convergence{\kern 1pt} Tolerance\]</div>
-
-The default is 0.001.
-
-#### Field: Fraction Radiant
-
-This field specifies what fraction of the power input to the baseboard heater is actually transferred to the space as radiant heat. The fraction should be between 0 and 1. This is the portion of the total power that is modeled as radiation. The portion that is radiant heat transfer from the baseboard heater is distributed to people and specific surfaces using the remaining fields. Note that the sum of the fractions in the remaining fields (people and surfaces) must equal 1.0 so that all the radiant power is distributed properly. For more information on the specification of this parameter, please see the Engineering Reference for EnergyPlus.
-
-#### Field: Fraction of Radiant Energy Incident on People
-
-This field specifies the fraction of radiant portion of heat transfer to the zone from the baseboard heater that is incident directly on people within the space. This has an impact on the predicted thermal comfort of the zone occupants. Note that although this energy is “radiant� it is actually modeled in the zone heat balance as convective energy (like an internal gain). The basic assumption here is that most radiant energy falling on people will most likely be rereleased to the zone air by convection. This is a simplification of reality, but it maintains the overall energy balance.
-
-#### Field Set: Surface Name, Fraction of Radiant Energy to Surface
-
-The following two items are repeated up to a maximum of 20 surface/fraction pairs. At least one surface/fraction pair must appear in an input file. In other words, at least one surface must be identified as a recipient of radiant energy from the baseboard heater.
-
-#### Field: Surface &lt;x&gt; Name
-
-This field is the name of the first surface to which radiant heat transfer from the baseboard heater is distributed. Used in conjunction with the next field, it helps to define the distribution of the radiant energy on the surfaces within the zone. Note that up to 20 pairs of surface names and corresponding fractions may be entered for a single radiant heater system.
-
-#### Field: Fraction of Radiant Energy to Surface &lt;x&gt;
-
-This field is paired with the preceding surface name (previous field) to define the fraction of radiant heat transfer leaving the baseboard heater that is incident on a particular surface. Users should take into account the directionality of baseboard heaters and their location when defining the value for this input field.
-
-***Note on Fraction of Radiant Energy Incident on People and to Surfaces***
-
-The radiant energy from the baseboard heater is defined by the total energy input to the baseboard heater from the water loop times the fraction radiant field shown above. This radiant energy is distributed to surfaces and people using the surface and fraction pairs and the fraction to people input by the user. These fractions to people and surfaces must add up to 1.0. In other words, in an input file, the following relation should be maintained by the user input:
-
-<div>\[FractionIndicentOnPeople + \sum {FractionToSurfaces = 1} \]</div>
-
-An example IDF for the water baseboard is shown below.
-
-```idf
-ZoneHVAC:Baseboard:RadiantConvective:Water,
-    SPACE2-1 Baseboard,      !- Baseboard Name
-    ReheatCoilAvailSched,    !- Availability Schedule Name
-    SPACE2-1 Zone Coil Water In Node,  !- Inlet\_Node
-    SPACE2-1 Zone Coil Water Out Node,  !- Outlet\_Node
-    76.67,                   !- Average Water Temperature {C}
-    0.063,                   !- Standard Water Mass Flow Rate {Kg/s}
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    3000.0,                  !- Heating Design Capacity{ W }
-    ,                        !- Heating Design Capacity Per Floor Area{ W / m2 }
-    ,                        !- Fraction of Autosized Heating Design Capacity{ -}
-    0.0013,                  !- Max Water Volumetric Flow Rate {m3/s}
-    0.001,                   !- Convergence Tolerance
-    0.3,                     !- Fraction radiant
-    0.3,                     !- Fraction of radiant energy incident on people
-    C2-1,                    !- Surface 1 Name
-    0.1,                     !- Fraction of radiant energy from heater distributed to surface 1
-    F2-1,                    !- Surface 2 Name
-    0.2,                     !- Fraction of radiant energy from heater distributed to surface 2
-    SB21,                    !- surface 3 Name
-    0.1,                     !- fraction of radiant energy from heater distributed to surface 3
-    SB23,                    !- surface 4 Name
-    0.1,                     !- fraction of radiant energy from heater distributed to surface 4
-    SB25,                    !- surface 5 Name
-    0.1,                     !- fraction of radiant energy from heater distributed to surface 5
-    WR-1,                    !- surface 6 Name
-    0.1;                     !- fraction of radiant energy from heater distributed to surface 6
-```
-
-### Baseboard (Water) Radiant Convective (ZoneHVAC) Outputs
-
-* HVAC,Average,Baseboard Total Heating Rate [W]
-
-* HVAC,Average,Baseboard Convective Heating Rate [W]
-
-* HVAC,Average,Baseboard Radiant Heating Rate [W]
-
-* HVAC,Sum,Baseboard Total Heating Energy [J]
-
-* HVAC,Sum,Baseboard Total Heating Energy [J]
-
-* HVAC,Sum,Baseboard Convective Heating Energy [J]
-
-* HVAC,Sum,Baseboard Radiant Heating Energy [J]
-
-* HVAC,Meter,Baseboard:EnergyTransfer [J]
-
-#### Baseboard Total Heating Rate [W]
-
-This is the actual convective heat addition rate of the baseboard to the zone in Watts.  This value includes the heat convected to the zone air from the baseboard unit, the heat radiated to people in the zone from the baseboard unit, and the additional convection from surfaces within the zone that have been heated by radiation from the baseboard unit.  This value will be different from (and almost always less than) the next field.
-
-#### Baseboard Convective Heating Rate [W]
-
-This field reports the rate at which convective heat addition is transferred from the baseboard to the zone in Watts.
-
-#### Baseboard Radiant Heating Rate [W]
-
-This field reports the rate at which radiant heat addition is transferred from the baseboard to the people and the surfaces within the zone in Watts.
-
-#### Baseboard Total Heating Energy  [J]
-
-This is the actual, total convective energy transferred directly and indirectly from the baseboard to the zone it is serving in Joules.  Direct convective heat transfer includes the convective portion of the baseboard unit.  Indirect convective heat transfer includes heat radiated to people that is then convected to the zone air and heat that is radiated to the surfaces and then convected to the zone air.
-
-#### Baseboard Convective Heating Energy [J]
-
-This field reports the amount of convective energy transferred from the baseboard directly to the zone air in Joules.
-
-#### Baseboard Radiant Heating Energy [J]
-
-This field reports the amount of radiant energy transferred from the baseboard to the zone in Joules.
-
-#### Baseboard Hot Water Mass Flow Rate [kg/s]
-
-This field reports the water mass flow rate at the inlet node of a baseboard unit.
-
-#### Baseboard Air Mass Flow Rate [kg/s]
-
-This field reports the air mass flow rate at the inlet node of a baseboard unit.
-
-#### Baseboard Water Inlet Temperature [C]
-
-This field reports the water temperatures at the inlet node of a baseboard unit.
-
-#### Baseboard Water Outlet Temperature [C]
-
-This field reports the water temperatures at the outlet node of a baseboard unit.
-
-#### Baseboard Air Inlet Temperature [C]
-
-This field reports the air temperatures at the inlet node of a baseboard unit.
-
-#### Baseboard Air Outlet Temperature [C]
-
-This field reports the air temperatures at the outlet node of a baseboard unit.
-
-### ZoneHVAC:Baseboard:RadiantConvective:Steam
-
-The objective of this model is to calculate the convective and radiant heat transfer from steam baseboard heaters to the people and the surfaces within a zone so that surface heat balances can take into account the radiant heat transfer to the surfaces and thus enhance the accuracy of thermal comfort predictions within the space. The radiant heat gains are distributed to the surfaces by fractions defined by the user. Users are requested to provide degree of sub cooling to estimate the outlet conditions of the condensate.
-
-#### Field: Name
-
-A unique user assigned name for an instance of a steam baseboard heater unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the steam baseboard heater unit can run during a given time period. A schedule value equal to 0 denotes that the unit must be off for that time period. A value greater than 0 denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Inlet Node Name
-
-This field is the name of the steam inlet node for the baseboard heater.
-
-#### Field: Outlet Node Name
-
-This field is the name of the steam outlet node for the baseboard heater.
-
-#### Field: Heating Design Capacity Method
-
-Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either *HeatingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedHeatingCapacity*. If this input field is left blank or zero, then autosizing is assumed. *HeatingDesignCapacity* means user specifies the magnitude of maximum heating capacity or the program calculates the maximum design heating capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the radiant baseboard unit. *FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is *HeatingDesignCapacity*.
-
-#### Field: Heating Design Capacity {W}
-
-This field is for the a radiant/convective steam baseboard unit heating capacity in watts. This field can be autosized by EnergyPlus. When the Heating Design Capacity Method is *HeatingDesignCapacity*  and this input is is blank, autosizing is assumed. Design day sizing run must be specified.
-
-#### Field: Heating Design Capacity Per Floor Area {W/m2}
-
-Enter the heating capacity per unit floor area in m3/s-m2 of radiant/convective steam baseboard. This field is required field when the Heating Design Capacity Method is *CapacityPerFloorArea*. The program calculates the heating capacity from floor area of the zone served by the steam baseboard unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
-
-#### Field: Fraction of Autosized Heating Design Capacity {-}
-
-Enter the heating capacity as a fraction of the autosized heating capacity of a radiant/convective steam baseboard unit. This input field is required when the Heating Design Capacity Method is *FractionOfAutosizedHeatingCapacity*. The program calculates the heating capacity from the design autosized heat capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
-
-#### Field: Degree of SubCooling
-
-This field is the temperature drop of the condensate in the coil of the baseboard heater. The steam condensates in the coil and changes the phase to the water, giving up the latent heat of steam to the air in the steam to air heat exchanger. The condensate due to the phase change then cools by certain degree in the coil, so that this amount of heat is added to the zone. The minimum value is 1.0° Celsius and default is 5.0° Celsius.
-
-#### Field: Maximum Steam Flow Rate
-
-This field is the maximum steam volumetric flow rate in m<sup>3</sup>/s through the steam baseboard heater.  The steam volumetric flow rate is calculated at 100C and 101325 Pa. It can be autosized by EnergyPlus.
-
-#### Field: Convergence Tolerance
-
-This field is the control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. For steam baseboards, the model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {({Q_{bb,out}} - {Q_{ZoneLoad}})} \right|}}{{{Q_{ZoneLoad}}}} \le Convergence{\kern 1pt} Tolerance\]</div>
-
-The default is 0.001.
-
-#### Field: Fraction Radiant
-
-This field specifies what fraction of the power input to the baseboard heater is actually transferred to the space as radiant heat. The fraction should be between 0 and 1. This is the portion of the total power that is modeled as radiation. The portion that is radiant heat transfer from the baseboard heater is distributed to people and specific surfaces using the remaining fields. Note that the sum of the fractions in the remaining fields (people and surfaces) must equal 1.0 so that all the radiant power is distributed properly.
-
-#### Field: Fraction of Radiant Energy Incident on People
-
-This field specifies the fraction of radiant portion of heat transfer to the zone from the baseboard heater that is incident directly on people within the space. This has an impact on the predicted thermal comfort of the zone occupants. Note that although this energy is “radiant� it is actually modeled in the zone heat balance as convective energy (like an internal gain). The basic assumption here is that most radiant energy falling on people will most likely be rereleased to the zone air by convection. This is a simplification of reality, but it maintains the overall energy balance.
-
-#### Field Set: Surface Name, Fraction of Radiant Energy to Surface
-
-The following two items are repeated up to a maximum of 20 surface/fraction pairs. At least one surface/fraction pair must appear in an input file. In other words, at least one surface must be identified as a recipient of radiant energy from the baseboard heater.
-
-#### Field: Surface &lt;x&gt; Name
-
-This field is the name of the first surface to which radiant heat transfer from the baseboard heater is distributed. Used in conjunction with the next field, it helps to define the distribution of the radiant energy on the surfaces within the zone. Note that up to 20 pairs of surface names and corresponding fractions may be entered for a single radiant heater system.
-
-#### Field: Fraction of Radiant Energy to Surface &lt;x&gt;
-
-This field is paired with the preceding surface name (previous field) to define the fraction of radiant heat transfer leaving the baseboard heater that is incident on a particular surface. Users should take into account the directionality of baseboard heaters and their location when defining the value for this input field.
-
-#### Note on Fraction of Radiant Energy Incident on People and to Surfaces
-
-The radiant energy from the baseboard heater is defined by the total energy input to the baseboard heater from the steam loop times the fraction radiant field shown above. This radiant energy is distributed to surfaces and people using the surface and fraction pairs and the fraction to people input by the user. These fractions to people and surfaces must add up to 1.0. In other words, in an input file, the following relation should be maintained by the user input:
-
-<div>\[FractionIndicentOnPeople + \sum {FractionToSurfaces = 1} \]</div>
-
-An example IDF for the steam baseboard is shown below.
-
-```idf
-ZoneHVAC:Baseboard:RadiantConvective:Steam,
-    Zone1Baseboard,       !- Baseboard name
-    FanAndCoilAvailSched, !- On/off schedule
-    Steam Inlet Node,     !- Steam inlet node
-    Steam Outlet Node,    !- Steam outlet node
-    HeatingDesignCapacity,!- Heating Design Capacity Method
-    autosize,             !- Heating Design Capacity{ W }
-    ,                     !- Heating Design Capacity Per Floor Area{ W / m2 }
-    ,                     !- Fraction of Autosized Heating Design Capacity{ -}
-    5.0,                  !- Degree of sub cooling in the coil {C}
-    autosize,             !- Maximum steam volumetric flow rate {m3/s}
-    0.001,                !- Tolerance
-    0.3,                  !- Fraction radiant
-    0.3,                  !- Fraction of radiant energy that is incident directly on people
-    OuterWall,            !- Surface 1 Name
-    0.4,                  !- Fraction of radiant energy from heater distributed to surface 1
-    Ceiling,              !- Surface 2 Name
-    0.1,                  !- Fraction of radiant energy from heater distributed to surface 2
-    InnerWall,            !- Surface 3 Name
-    0.1,                  !- Fraction of radiant energy from heater distributed to surface 3
-    Floor,                !- Surface 4 Name
-    0.1;                  !- Fraction of radiant energy from heater distributed to surface 4
-```
-
-### Baseboard (Steam) Radiant Convective (ZoneHVAC) Outputs
-
-* HVAC,Average,Baseboard Total Heating Rate [W]
-
-* HVAC,Average,Baseboard Convective Heating Rate [W]
-
-* HVAC,Average,Baseboard Radiant Heating Rate [W]
-
-* HVAC,Sum,Baseboard Total Heating Energy [J]
-
-* HVAC,Sum,Baseboard Convective Heating Energy [J]
-
-* HVAC,Sum,Baseboard Radiant Heating Energy [J]
-
-* HVAC,Meter,Baseboard:EnergyTransfer [J]
-
-* HVAC,Average,Baseboard Steam Mass Flow Rate [kg/s]
-
-* HVAC,Average,Baseboard Steam Inlet temperature [C]
-
-* HVAC,Average,Baseboard Steam Outlet temperature [C]
-
-#### Baseboard Total Heating Rate [W]
-
-This is the actual convective heat addition rate of the baseboard to the zone in Watts.  This value includes the heat convected to the zone air from the baseboard unit, the heat radiated to people in the zone from the baseboard unit, and the additional convection from surfaces within the zone that have been heated by radiation from the baseboard unit. This value will be different from (and almost always less than) the next field.
-
-#### Baseboard Convective Heating Rate [W]
-
-This field reports the rate at which convective heat addition is transferred from the baseboard to the zone in Watts.
-
-#### Baseboard Radiant Heating Rate [W]
-
-This field reports the rate at which radiant heat addition is transferred from the baseboard to the people and the surfaces within the zone in Watts.
-
-#### Baseboard Total Heating Energy [J]
-
-This is the actual, total convective energy transferred directly and indirectly from the baseboard to the zone it is serving in Joules. Direct convective heat transfer includes the convective portion of the baseboard unit. Indirect convective heat transfer includes heat radiated to people that is then convected to the zone air and heat that is radiated to the surfaces and then convected to the zone air.
-
-#### Baseboard Convective Heating Energy [J]
-
-This field reports the amount of convective energy transferred from the baseboard directly to the zone air in Joules.
-
-#### Baseboard Radiant Heating Energy [J]
-
-This field reports the amount of radiant energy transferred from the baseboard to the zone in Joules.
-
-#### Baseboard Steam Energy [J]
-
-#### Baseboard Steam Rate [W]
-
-These are the total heat addition energy and rate of steam used by the baseboard to heat the zone it is serving in Joules and Watts.
-
-#### Baseboard Steam Mass Flow Rate [kg/s]
-
-This field reports the steam mass flow rate at the inlet node of a baseboard unit.
-
-#### Baseboard Steam Inlet Temperature [C]
-
-This field reports the steam temperatures at the inlet node of a baseboard unit.
-
-#### Baseboard Steam Outlet Temperature [C]
-
-This field reports the steam temperatures at the outlet node of a baseboard unit.
-
-### ZoneHVAC:Baseboard:RadiantConvective:Electric
-
-The electric baseboard heater is a component in the zone equipment simulation. Heat from this device is radiated to people and surfaces and also convected to the surrounding air. The electric baseboard model includes the impact of the radiant heat addition to people and surfaces so that the thermal comfort and surface heat balances are impacted. The component is controlled to meet any remaining zone load not met by other equipment baseboard operates to meet the remaining zone load and the total electric consumption is calculated by dividing by the efficiency of the baseboard.
-
-#### Field: Name
-
-A unique user assigned name for an instance of an electric baseboard heater unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the electric baseboard heater unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit will be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Heating Design Capacity Method
-
-Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either *HeatingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedHeatingCapacity*. If this input field is left blank or zero, then autosizing is assumed. *HeatingDesignCapacity* means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the maximum or nominal design heating capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the radiant baseboard unit. *FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is *HeatingDesignCapacity*.
-
-#### Field: Heating Design Capacity {W}
-
-This field is for the radiant-convective electric baseboard unit nominal heating capacity in watts. This field can be autosized by EnergyPlus. This input field is autosizable. When the Heating Design Capacity Method is *HeatingDesignCapacity*  and this input is is blank, autosizing is assumed. Design day sizing run must be specified.
-
-#### Field: Heating Design Capacity Per Floor Area {W/m2}
-
-Enter the heating capacity per unit floor area in m3/s-m2 of radiant/convective electric baseboard. This field is required field when the Heating Design Capacity Method is *CapacityPerFloorArea*. The program calculates the heating capacity from floor area of the zone served by the radiant baseboard unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
-
-#### Field: Fraction of Autosized Heating Design Capacity {-}
-
-Enter the heating capacity as a fraction of the autosized heating capacity for radiant/convective electric baseboard. This input field is required when the Heating Design Capacity Method is *FractionOfAutosizedHeatingCapacity*. The program calculates the heating capacity from the design autosized heat capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
-
-#### Field: Efficiency
-
-This is the overall electrical efficiency of the electric baseboard unit. The zone load met by this unit is divided by the electrical efficiency to obtain the total electric energy used.
-
-#### Field: Fraction Radiant
-
-This field specifies what fraction of the power input to the baseboard heater is actually transferred to the space as radiant heat. The fraction should be between 0 and 1. This is the portion of the total power that is modeled as radiation. The portion that is radiant heat transfer from the baseboard heater is distributed to people and specific surfaces using the remaining fields. Note that the sum of the fractions in the remaining fields (people and surfaces) must equal 1.0 so that all the radiant power is distributed properly.
-
-#### Field: Fraction of Radiant Energy Incident on People
-
-This field specifies the fraction of the radiant portion of heat transfer to the zone from the baseboard heater that is incident directly on people within the space. This has an impact on the predicted thermal comfort of the zone occupants. Note that although this energy is “radiant� it is actually modeled in the zone heat balance as a convective energy (like an internal gain). The basic assumption here is that radiant energy falling on people will most likely be rereleased to the zone air by convection. This is a simplification of reality, but it maintains the overall energy balance.
-
-#### Field Set: Surface Name, Fraction of Radiant Energy to Surface
-
-The following two items are repeated up to a maximum of 20 surface/fraction pairs. At least one surface/fraction pair must appear in an input file. In other words, at least one surface must be identified as a recipient of radiant energy from the baseboard heater.
-
-#### Field Set: Surface &lt;x&gt; Name
-
-This field is the name of the first surface to which radiant heat transfer from the baseboard heater is distributed. Used in conjunction with the next field, it helps to define the distribution of the radiant energy on the surfaces within the zone. Note that up to 20 pairs of surface names and corresponding fractions may be entered for a single radiant heater system.
-
-#### Field Set: Fraction of Radiant Energy to Surface &lt;x&gt;
-
-This field is paired with the preceding surface name (previous field) to define the fraction of radiant heat transfer leaving the baseboard heater that is incident on a particular surface. Users should take into account the directionality of baseboard heaters and their location when defining the value for this input field.
-
-#### Note on Fraction of Radiant Energy Incident on People and to Surfaces
-
-The radiant energy from the baseboard heater is defined by the total energy input to the baseboard heater times the fraction radiant field shown above. This radiant energy is distributed to surfaces and people using the surface and fraction pairs and the fraction to people input by the user. These fractions to people and surfaces must add up to 1.0. In other words, in an input file, the following relation should be maintained by the user input:
-
-<div>\[FractionIndicentOnPeople + \sum {FractionToSurfaces = 1} \]</div>
-
-Below is an example input for an Electric Baseboard Heater.
-
-```idf
-ZoneHVAC:Baseboard:RadiantConvective:Electric,
-    Baseboard 1,   !- Name
-    BB Schedule,   !- Availability Schedule Name
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    5000,          !- Heating Design Capacity{ W }
-    ,              !- Heating Design Capacity Per Floor Area{ W / m2 }
-    ,              !- Fraction of Autosized Heating Design Capacity{ -}
-    0.97,          !- Efficiency of the baseboard
-    0.3,           !- Fraction radiant
-    0.3,           !- Fraction of radiant energy that is incident directly on people
-    EastWall,      !- Surface 1 name
-    0.3,           !- Fraction of radiant energy from heater distributed to surface 1
-    WestWall,      !- Surface 2 name
-    0.1,           !- Fraction of radiant energy from heater distributed to surface 2
-    NorthWall,     !- Surface 3 name
-    0.1,           !- Fraction of radiant energy from heater distributed to surface 3
-    SouthWall,     !- Surface 4 name
-    0.1,           !- Fraction of radiant energy from heater distributed to surface 4
-    Ceiling,       !- Surface 5 name
-    0.1;           !- Fraction of radiant energy from heater distributed to surface 5
-```
-
-### Baseboard (Electric) Radiant Convective (ZoneHVAC) Outputs
-
-* HVAC,Average,Baseboard Total Heating Rate [W]
-
-* HVAC,Average,Baseboard Radiant Heating Rate [W]
-
-* HVAC,Average,Baseboard Convective Heating Rate [W]
-
-* HVAC,Average,Baseboard Electric Power[W]
-
-* HVAC,Sum,Baseboard Total Heating Energy [J]
-
-* HVAC,Sum,Baseboard Radiant Heating Energy [J]
-
-* HVAC,Sum,Baseboard Convective Heating Energy [J]
-
-* HVAC,Sum,Baseboard Electric Energy [J]
-
-* HVAC,Meter,Baseboard:EnergyTransfer [J]
-
-* HVAC,Meter,Heating:Electricity[J]
-
-#### Baseboard Total Heating Rate [W]
-
-This is the actual convective heat addition rate of the baseboard to the zone in Watts. This value includes the heat convected to the zone air from the baseboard unit, the heat radiated to people in the zone from the baseboard unit, and the additional convection from surfaces within the zone that have been heated by radiation from the baseboard unit. This value will be different from (and almost always less than) the next field.
-
-#### Baseboard Radiant Heating Rate [W]
-
-This field reports the rate at which radiant heat addition is transferred from the baseboard to the people and the surfaces within the zone in Watts.
-
-#### Baseboard Convective Heating Rate [W]
-
-This field reports the rate at which convective heat addition is transferred from the baseboard to the zone in Watts.
-
-#### Baseboard Electric Energy [J]
-
-This is the electric energy used by the baseboard in Joules.
-
-#### Baseboard Electric Power [J]
-
-This is the electric power required by the baseboard to heat the zone it is serving in Watts
-
-#### Baseboard Total Heating Energy [J]
-
-This is the actual convective energy transferred directly and indirectly from the baseboard heater to the zone it is serving in Joules. Direct convective heat transfer includes the convective portion of the baseboard unit. Indirect convective heat transfer includes heat radiated to people that is then convected to the zone air and heat that is radiated to the surfaces and then convected to the zone air.
-
-#### Baseboard Radiant Heating Energy [J]
-
-This field reports the amount of radiant energy transferred from the baseboard to the zone in Joules.
-
-#### Baseboard Convective Heating Energy [J]
-
-This field reports the amount of convective energy transferred from the baseboard directly to the zone air in Joules.
-
-### ZoneHVAC:Baseboard:Convective:Water
-
-The hot water baseboard heater is a component of zone equipment. The component is controlled to meet any remaining zone load not met by other equipment in the zone that have higher heating priority. The control is accomplished by throttling the hot water flow. Input resembles that for the simple heating coil: there is an availability schedule, an overall UA, and a maximum hot water mass flow rate. The unit is connected to a hot water loop (demand side) with an inlet and outlet node. Finally, there is the convergence tolerance, which is the tolerance on how closely the baseboard outlet will meet the zone load. Of course, this tolerance is relative to the zone load.
-
-#### Field: Name
-
-A unique user assigned name for an instance of a hot water baseboard heater unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the hot water baseboard heater unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Inlet Node Name
-
-The name of the hot water inlet node for the baseboard heater.
-
-#### Field: Outlet Node Name
-
-The name of the hot water outlet node for the baseboard heater.
-
-#### Field: Heating Design Capacity Method
-
-Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either *HeatingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedHeatingCapacity*. If this input field is left blank or zero, then autosizing is assumed. *HeatingDesignCapacity* means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the maximum or nominal design heating capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the hot water baseboard heater. *FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is *HeatingDesignCapacity*.
-
-#### Field: Heating Design Capacity {W}
-
-This field is for the hot water baseboard heater design heating capacity in watts. This field can be autosized by EnergyPlus. This input field is autosizable. When the Heating Design Capacity Method is *HeatingDesignCapacity*  and this input is is blank, autosizing is assumed. Design day sizing run must be specified id autosize is specified.
-
-#### Field: Heating Design Capacity Per Floor Area {W/m2}
-
-Enter the heating capacity per unit floor area in m3/s-m2 of hot water baseboard heater. This field is required field when the Heating Design Capacity Method is *CapacityPerFloorArea*. The program calculates the heating capacity from floor area of the zone served by hot water baseboard heater and the heating capacity per unit floor area value specified by the user. This field may be left blank.
-
-#### Field: Fraction of Autosized Heating Design Capacity {-}
-
-Enter the heating capacity as a fraction of the autosized heating capacity for the hot water baseboard heater. This input field is required when the Heating Design Capacity Method is *FractionOfAutosizedHeatingCapacity*. The program calculates the heating capacity from the design autosized heat capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
-
-#### Field: U-Factor Times Area Value
-
-The overall heat transfer coefficient for the baseboard heater in watts per degree Celsius at design conditions. The U-Factor Times Area Value (UA) is used in an NTU - effectiveness calculation. An estimate of the UA can be obtained from:
-
-<div>\[q = UA \times ({T_{water,avg}} - {T_{air,avg}})\]</div>
-
-where q is the heat transferred from water to the air in watts; T<sub>water,\\ avg</sub> is the average water temperature in degrees C; and T<sub>air,\\ avg</sub> is the average air temperature in degrees C. Or the LMTD temperature difference can be used.
-
-#### Field: Maximum Water Flow Rate
-
-The maximum hot water volumetric flow rate in m<sup>3</sup>/sec.
-
-#### Field Convergence Tolerance
-
-The control tolerance for the unit heating output. The unit is controlled by matching the unit output to the zone demand. For hot water baseboards, the model must be numerically inverted to obtain a specified output. The convergence tolerance is the error tolerance used to terminate the numerical inversion procedure. Basically this is the fraction:
-
-<div>\[\frac{{\left| {({Q_{bb,out}} - {Q_{ZoneLoad}})} \right|}}{{{Q_{ZoneLoad}}}} \le Convergence{\kern 1pt} Tolerance\]</div>
-
-The default is 0.001.
-
-An example IDF for the hot water convective baseboard is shown below.
-
-```idf
-ZoneHVAC:Baseboard:Convective:Water,
-        Zone3Baseboard, ! name
-        FanAndCoilAvailSched, ! on/off schedule
-        Zone 3 Reheat Water Inlet Node, ! water inlet node
-        Zone 3 Reheat Water Outlet Node, ! water outlet node
-        HeatingDesignCapacity, !- Heating Design Capacity Method
-        autosize,!- Heating Design Capacity{ W }
-        ,        !- Heating Design Capacity Per Floor Area{ W / m2 }
-        ,        !- Fraction of Autosized Heating Design Capacity{ -}
-        500.,    ! UA
-        0.0013,  ! maximum water flow rate m3/s
-        0.001;   ! tolerance
-```
-
-### Baseboard (Water) Convective (ZoneHVAC) Outputs
-
-* HVAC,Average,Baseboard Total Heating Rate [W]
-
-* HVAC,Sum,Baseboard Total Heating Energy [J]
-
-* HVAC,Sum,Baseboard Hot Water Energy [J]
-
-* HVAC,Average,Baseboard Hot Water Mass Flow Rate [kg/s]
-
-* HVAC,Average,Baseboard Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Baseboard Air Inlet Temperature [C]
-
-* HVAC,Average,Baseboard Air Outlet Temperature [C]
-
-* HVAC,Average,Baseboard Water Inlet Temperature [C]
-
-* HVAC,Average,Baseboard Water Outlet Temperature [C]
-
-#### Baseboard Total Heating Rate [W]
-
-This is the heat addition rate of the convective baseboard to the zone it is serving in Watts.
-
-#### Baseboard Total Heating Energy [J]
-
-This is the heat addition of the convective baseboard to the zone it is serving in Joules over the timestep being reported.
-
-#### Baseboard Hot Water Energy [J]
-
-This is the energy in the hot water used by the baseboard to heat the zone, in Joules.
-
-#### Baseboard Hot Water Mass Flow Rate [kg/s]
-
-This field reports the water mass flow rate at the inlet node of a baseboard unit.
-
-#### Baseboard Air Mass Flow Rate [kg/s]
-
-This field reports the air mass flow rate at the inlet node of a baseboard unit.
-
-#### Baseboard Water Inlet Temperature [C]
-
-This field reports the water temperatures at the inlet node of a baseboard unit.
-
-#### Baseboard Water Outlet Temperature [C]
-
-This field reports the water temperatures at the outlet node of a baseboard unit.
-
-#### Baseboard Air Inlet Temperature [C]
-
-This field reports the air temperatures at the inlet node of a baseboard unit.
-
-#### Baseboard Air Outlet Temperature [C]
-
-This field reports the air temperatures at the outlet node of a baseboard unit.
-
-### ZoneHVAC:Baseboard:Convective:Electric
-
-The electric baseboard heater is a component in the zone equipment simulation. The component is controlled to meet any remaining zone load not met by other equipment in the zone that have higher heating priority. The control is accomplished by taking the remaining zone load and dividing by the efficiency of the baseboard.
-
-#### Field: Name
-
-A unique user assigned name for an instance of a electric baseboard heater unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the electric baseboard heater unit can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Heating Design Capacity Method
-
-Enter the method used to determine the heating design capacity or enter the method for scalable sizing of heating capacity of electric baseboard unit. Input allowed is either *HeatingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedHeatingCapacity*. If this input field is left blank or zero, then autosizing is assumed. *HeatingDesignCapacity* means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the maximum or nominal design heating capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the electric convective baseboard unit. *FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is *HeatingDesignCapacity*.
-
-#### Field: Heating Design Capacity {W}
-
-This field is for the convective electric baseboard nominal heating capacity in watts. This field can be autosized by EnergyPlus. This input field is autosizable. Design day sizing run must be specified. This input field may be left blank.
-
-#### Field: Heating Design Capacity Per Floor Area {W/m2}
-
-Enter the heating capacity per unit floor area in m3/s-m2 of electric convective baseboard unit. This field is required field when the Heating Design Capacity Method is *CapacityPerFloorArea*. The program calculates the heating capacity from floor area of the zone served by the electric convective baseboard unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
-
-#### Field: Fraction of Autosized Heating Design Capacity {-}
-
-Enter the heating capacity as a fraction of the autosized heating capacity for convective electric baseboard unit. This input field is required when the Heating Design Capacity Method is *FractionOfAutosizedHeatingCapacity*. The program calculates the heating capacity from the design autosized heating capacity and user specified fraction. Design day sizing must be specified. This field may be left blank.  Default value is 1.0.
-
-#### Field: Efficiency
-
-This is the overall electrical efficiency of the electric baseboard. The zone load met by this unit is divided by the electrical efficiency to obtain the total electric energy used.
-
-An example IDF for the electric convective baseboard is shown below.
-
-```idf
-ZoneHVAC:Baseboard:Convective:Electric,
-    Zone1Baseboard,  !- Baseboard Name
-    FanAndCoilAvailSched,  !- Availability Schedule Name
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    5000,                    !- Heating Design Capacity{ W }
-    ,                        !- Heating Design Capacity Per Floor Area{ W / m2 }
-    ,                        !- Fraction of Autosized Heating Design Capacity{ -}
-    0.97;  !- Efficiency of the BaseBoard
-```
-
-### Baseboard (Electric) Convective (ZoneHVAC) Outputs
-
-* HVAC,Average,Baseboard Total Heating Rate [W]
-
-* HVAC,Sum,Baseboard Total Heating Energy [J]
-
-* HVAC,Meter,Baseboard:EnergyTransfer [J]
-
-* HVAC,Sum,Baseboard Electric Energy [J]
-
-* HVAC,Average,Baseboard Electric Power[W]
-
-* HVAC,Meter,Heating:Electricity[J]
-
-#### Baseboard Total Heating Rate [W]
-
-This is the heat addition rate of the electric convective baseboard to the zone it is serving in Watts.
-
-#### Baseboard Total Heating Energy [J]
-
-This is the heat addition of the convective baseboard to the zone it is serving in Joules over the timestep being reported.
-
-#### Baseboard Electric Energy [J]
-
-This is the total electric consumption of the baseboard for the zone it is serving in Joules over the timestep being reported.
-
-#### Baseboard Electric Power [W]
-
-This is the electric power required by the baseboard to the zone it is serving in Watts.
-
-### ZoneHVAC:LowTemperatureRadiant:VariableFlow
-
-This low temperature radiant system (hydronic) is a component of zone equipment that is intended to model any “radiant system� where water is used to supply/remove energy to/from a building surface (wall, ceiling, or floor). The component is controlled to meet any remaining zone load not met by other equipment in the zone that have higher priority. The control is accomplished by throttling the hot or chilled water flow to the unit. Note that this system will only control based on the radiant system controls defined by this input syntax and not via a zone thermostat such as is used for forced air systems. Note also that because this unit does not require a thermostat that in cases where no other systems are serving the zone in which this system resides that it will use the heating equipment priority to determine which system will run first.  If the radiant system is serving a zone with forced air equipment, the radiant system will follow the priority order established by the zone thermostat but will still base its response on the controls defined by the user for the radiant system.
-
-This model covers a wide range of low temperature radiant systems: heating and/or cooling, panel or embedded pipes, etc. It is not intended to simulate high temperature electric or gas radiant heaters. Those devices will be handled by a separate model and different input syntax. Low temperature radiant systems that use electric resistance heating should also be defined using separate input syntax (ref: ZoneHVAC:LowTemperatureRadiant:Electric).
-
-#### Field: Name
-
-This field is an unique user assigned name for an instance of a hydronic low temperature radiant system. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that denotes whether the hydronic low temperature radiant system can run during a given time period. A schedule value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for that time period. A value greater than 0 (usually 1 is used) denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Zone Name
-
-This field is the name of the zone (Ref: Zone) in which the hydronic low temperature radiant system is principally located and intended to affect. A system that is between two zones will still act upon each zone; however, the zone name referenced here should be the zone that controls the radiant system response.
-
-#### Field: Surface Name or Radiant Surface Group Name
-
-This field is the name of the surface (Ref: BuildingSurface) or surface list (Ref: ZoneHVAC:LowTemperatureRadiant:SurfaceGroup) in which the hydronic tubing is embedded/contained. This specification attaches the source or sink from the radiant system to a particular surface and the contribution of the system to the heat balances of that surface. If this field is a surface list, then the source or sink is attached to all of the surfaces in the list with the radiant system surface group defining the breakdown of how flow rate is split between the various surfaces. Base surfaces (e.g., BuildingSurface:Detailed), door surfaces and internal mass are valid. Window surfaces are not valid surface types for embedded radiant systems.
-
-#### Field: Hydronic Tubing Inside Diameter
-
-This field is the inside diameter of the tubes through which water is circulated for the system being defined by this statement. The inside diameter should be recorded in meters and is used to determine the convective heat transfer from the water to the inside surface of the hydronic tubing.
-
-#### Field: Hydronic Tubing Length
-
-This field is the total length of pipe embedded in the surface named above in the surface name field. The length of the tube should be entered in meters and is used to determine the effectiveness of heat transfer from the fluid being circulated through the tubes and the tube/surface. Longer tubing lengths result in more heat will be transferred to/from the radiant surface to the circulating fluid. Note that if the user elects to autosize this field that a standard zone thermostat such as would be used for a forced air system must be defined as autosizing calculations are based on the zone thermostat value and not on the radiant system control values.
-
-#### Field: Temperature Control Type
-
-This field specifies along with the throttling range and setpoint schedules how the user wishes to control the hydronic radiant system. The temperature denoted in the setpoint schedule can refer to one of five different temperatures: the zone mean air temperature, the zone mean radiant temperature, the zone operative temperature, the outdoor dry-bulb temperature, or the outdoor wet-bulb temperature. The choice of temperature is controlled by the current field—temperature control type. The user must select from the following options:
-
-* MeanAirTemperature
-
-* MeanRadiantTemperature
-
-* OperativeTemperature
-
-* OutdoorDryBulbTemperature
-
-* OutdoorWetBulbTemperature
-
-Operative temperature for radiant system controls is the average of Mean Air Temperature and Mean Radiant Temperature. If the user does not select a control type, **MeanAirTemperature** control is assumed by EnergyPlus. See the throttling range and control temperature schedule fields below for more information.
-
-#### Field: Heating Design Capacity Method
-
-Enter the method used to determine the heating design capacity for scalable sizing. Input allowed is either *HeatingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedHeatingCapacity*. If this input field is left blank or zero, then autosizing is assumed. *HeatingDesignCapacity* means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the design heating capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the low temperature radiant variable flow unit. *FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is *HeatingDesignCapacity*.
-
-#### Field: Heating Design Capacity {W}
-
-This field is for the low temperature radiant variable flow unit design heating capacity in watts. This field can be autosized by EnergyPlus. This input field is autosizable. When the Heating Design Capacity Method is *HeatingDesignCapacity*  and this input is is blank, autosizing is assumed. Design day sizing run must be specified if autosized.
-
-#### Field: Heating Design Capacity Per Floor Area {W/m2}
-
-Enter the heating capacity per unit floor area in m3/s-m2 of low temperature radiant variable flow unit. This field is required field when the Heating Design Capacity Method is *CapacityPerFloorArea*. The program calculates the heating capacity from floor area of the zone served by the low temperature radiant variable flow unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
-
-#### Field: Fraction of Autosized Heating Design Capacity {-}
-
-Enter the heating capacity as a fraction of the autosized heating capacity for low temperature radiant variable flow unit. This input field is required when the Heating Design Capacity Method is *FractionOfAutosizedHeatingCapacity*. The program calculates the heating capacity from the design autosized heat capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
-
-#### Field: Maximum Hot Water Flow
-
-This field is the maximum flow rate of hot water through the radiant system in m<sup>3</sup>/sec. The controls for the radiant system will vary the flow rate of hot water through the surface using zero flow and the maximum flow rate specified in this field as the lower and upper bounds, respectively. Note that if the user elects to autosize this field that a standard zone thermostat such as would be used for a forced air system must be defined as autosizing calculations are based on the zone thermostat value and not on the radiant system control values.
-
-#### Field: Heating Water Inlet Node Name
-
-This field contains the name of the hot water inlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a heating coil.
-
-#### Field: Heating Water Outlet Node Name
-
-This field contains the name of the hot water oulet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a heating coil.
-
-#### Field: Heating Control Throttling Range
-
-This field specifies the range of temperature in degrees Celsuis over which the radiant system throttles from zero flow rate up to the maximum defined by the maximum hot water flow rate field described above. The throttling range parameter is used in conjunction with the control temperature to define the response of the system to various zone conditions. The heating control temperature schedule specifies the “setpoint� temperature where the flow rate to the system is at half of the maximum flow rate. For example, if the heating control temperature setpoint is currently 15°C and the heating throttling range is 2°C, the water flow rate to the radiant system will be zero when the controlling temperature (MAT, MRT, Operative Temperature, ODB, or OWB; see control type field above) is at or above 16°C and the maximum flow rate when the controlling temperature is at or below 14°C. This represents a throttling range of 2°C around the setpoint of 15°C. In between 14°C and 16°C, the flow rate to the radiant system is varied linearly.
-
-#### Field: Heating Control Temperature Schedule Name
-
-This field specifies the heating setpoint or control temperature for the radiant system in degrees Celsius. Used in conjunction with the previous field (heating control throttling range), it will define whether or not the system is running and the current flow rate. Water flow rate to the system is varied linearly around the setpoint temperature based on the throttling range and the maximum heating flow rate parameters (see above). It should be noted that this control schedule will allow different setpoint temperatures throughout the year for heating. The control of the radiant system is based solely on the heating control temperature schedule, the cooling control temperature schedule (see below), and the control temperature type listed above. The radiant system will not use any zone thermostat that might be used by other systems serving the zone in which the radiant system resides.
-
-#### Field: Cooling Design Capacity Method
-
-Enter the method used to determine the cooling design capacity for scalable sizing. Input allowed is either *CoolingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedCoolingCapacity*. If this input field is left blank or zero, then autosizing is assumed. *CoolingDesignCapacity* means user specifies the design cooling capacity or the program calculates the design cooling capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design cooling capacity from user specified heating capacity per floor area and floor area of the zone served by the low temperature radiant variable flow unit. *FractionOfAutosizedCoolingCapacity* means the program calculates the design cooling capacity from user specified fraction and the auto-sized design cooling capacity. The default method is *CoolingDesignCapacity*.
-
-#### Field: Cooling Design Capacity {W}
-
-This field is for the low temperature radiant variable flow unit design cooling capacity in watts. This field can be autosized by EnergyPlus. This input field is autosizable. When the Cooling Design Capacity Method is *CoolingDesignCapacity* and this input is is blank, autosizing is assumed. Design day sizing run must be specified if autosized.
-
-#### Field: Cooling Design Capacity Per Floor Area {W/m2}
-
-Enter the cooling capacity per unit floor area in m3/s-m2 of low temperature radiant variable flow unit. This field is required field when the Cooling Design Capacity Method is *CapacityPerFloorArea*. The program calculates the cooling capacity from floor area of the zone served by the low temperature radiant variable flow unit and the cooling capacity per unit floor area value specified by the user. This field may be left blank.
-
-#### Field: Fraction of Autosized Cooling Design Capacity {-}
-
-Enter the cooling capacity as a fraction of the autosized cooling capacity for low temperature radiant variable flow unit. This input field is required when the Cooling Design Capacity Method is *FractionOfAutosizedCoolingCapacity*. The program calculates the cooling capacity from the design autosized cooling capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. Default value is 1.0.
-
-#### Field: Maximum Cold Water Flow
-
-This field is the maximum flow rate of cold water through the radiant system in m<sup>3</sup>/sec. The controls for the radiant system will vary the flow rate of cold water through the surface using zero flow and the maximum flow rate specified in this field as the lower and upper bounds, respectively. Note that this field is optional and not required for a heating only system. Note also that if the user elects to autosize this field that a standard zone thermostat such as would be used for a forced air system must be defined as autosizing calculations are based on the zone thermostat value and not on the radiant system control values.
-
-#### Field: Cooling Water Inlet Node Name
-
-This field contains the name of the cold water inlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a cooling coil. As with the maximum cold water flow rate, this field is optional and not required for a heating only system.
-
-#### Field: Cooling Water Outlet Node Name
-
-This field contains the name of the cold water oulet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a cooling coil. As with the maximum cold water flow rate, this field is optional and not required for a heating only system.
-
-#### Field: Cooling Control Throttling Range
-
-This field specifies the range of temperature in degrees Celsuis over which the radiant system throttles from zero flow rate up to the maximum defined by the maximum cold water flow rate field described above. The throttling range parameter is used in conjunction with the control temperature to define the response of the system to various zone conditions. The cooling control temperature schedule specifies the “setpoint� temperature where the flow rate to the system is at half of the maximum flow rate. For example, if the cooling control temperature setpoint is currently 25°C and the cooling throttling range is 2°C, the water flow rate to the radiant system will be zero when the controlling temperature (MAT, MRT, Operative Temperature, ODB, or OWB; see control type field above) is at or below 24°C and the maximum flow rate when the controlling temperature is at or above 26°C. This represents a throttling range of 2°C around the setpoint of 25°C. In between 24°C and 26°C, the flow rate to the radiant system is varied linearly.
-
-#### Field: Cooling Control Temperature Schedule Name
-
-This field specifies the cooling setpoint or control temperature for the radiant system in degrees Celsius. Used in conjunction with the previous field (cooling control throttling range), it will define whether or not the system is running and the current flow rate. Water flow rate to the system is varied linearly around the setpoint temperature based on the throttling range and the maximum cooling flow rate parameters (see above). It should be noted that this control schedule will allow different setpoint temperatures throughout the year for cooling. The control of the radiant system is based solely on the heating control temperature schedule listed above, the cooling control temperature schedule, and the control temperature type listed above. The radiant system will not use any zone thermostat that might be used by other systems serving the zone in which the radiant system resides.
-
-#### Field: Condensation Control Type
-
-When radiant systems do cooling, there is the possibility that condensation will occur on the surface that is being cooled.  This is due to the fact that the surface temperature may drop below the dew-point temperature of the space.  When this occurs, condensation on the surface will occur.  In EnergyPlus, users have several options for handling this situation including: Off and SimpleOff.  When the user chooses the Off option, EnergyPlus will not do anything other than produce a warning message when condensation is predicted to occur.  The program will simply continue on; no moisture will be removed from the zone air and there will be no adjustment of the surface temperature as a result of the condensation.  When the user chooses the SimpleOff option, the program will predict cases where condensation will occur and shut-off the radiant system to avoid this situation.  With this option, the users also have the opportunity to adjust when the system will shut down.  This is specified with the next parameter (field: condensation differential parameter). This parameter is optional and EnergyPlus will use the SimpleOff strategy when this parameter is not specified.
-
-#### Field: Condensation Control Dewpoint Offset
-
-This optional parameter is only valid with the SimpleOff condensation handling algorithm (see previous input parameter).  It establishes the difference between the calculated dew-point temperature of the space and the allowed surface temperature to which the surface can drop before the radiant system shuts down in degrees Celsius.  This parameter can be any positive, negative, or zero value.  When this parameter is zero, the radiant system will shut down when the surface temperature drops to the dew-point temperature or below.  When this parameter is positive, the radiant system will shut down when the surface is the number of degrees Celsius above the dew-point temperature.  This allows some extra safety to avoid condensation.  When this parameter is negative, the radiant system will shut down when the surface temperature is the number of degrees Celsius below the dew-point temperature.  While not recommended, this strategy allows the user to simulate a situation where small amounts of condensation are tolerable.
-
-#### Field: Number of Circuits
-
-This optional input allows the user to choose between modeling each surface in the radiant system as a single hydronic circuit or to allow the program to divide the surface into multiple parallel hydronic circuits based on the next input field *Circuit Length*. To model as a single circuit choose *OnePerSurface*. To model as multiple circuits choose *CalculateFromCircuitLength*. It is recommended that *CalculateFromCircuitLength* be chosen. The default is *OnePerSurface* for backward compatibility with older versions of EnergyPlus.
-
-#### Field: Circuit Length
-
-The length in meters of each parallel hydronic circuit in a surface. Used when the previous input field is set to *CalculateFromCircuitLength*. The default is 106.7 meters (350 feet), which is the maximum circuit length allowed in Title 24.
-
-An example IDF with a hydronic low temperature radiant system is shown below.
-
-```idf
-  ZoneHVAC:LowTemperatureRadiant:VariableFlow,
-    SPACE1-1 Zone Radiant Floor,  !- Name
-    RADIANTSYSAVAILSCHED,    !- Availability Schedule Name
-    SPACE1-1,                !- Zone Name
-    C1-1,                    !- Surface Name or Radiant Surface Group Name
-    0.013,                   !- Hydronic Tubing Inside Diameter {m}
-    autosize,                !- Hydronic Tubing Length {m}
-    OperativeTemperature,    !- Temperature Control Type
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity{ W }
-    ,                        !- Heating Design Capacity Per Floor Area{ W / m2 }
-    ,                        !- Fraction of Autosized Heating Design Capacity{ -}
-    0.0004,                  !- Maximum Hot Water Flow {m3/s}
-    SPACE1-1 Zone Radiant Water Inlet Node,  !- Heating Water Inlet Node Name
-    SPACE1-1 Zone Radiant Water Outlet Node,  !- Heating Water Outlet Node Name
-    2.0,                     !- Heating Control Throttling Range {deltaC}
-    RADIANT HEATING SETPOINTS,  !- Heating Control Temperature Schedule Name
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity{ W }
-    ,                        !- Cooling Design Capacity Per Floor Area{ W / m2 }
-    ,                        !- Fraction of Autosized Cooling Design Capacity{ -}
-    autosize,                !- Maximum Cold Water Flow {m3/s}
-    SPACE1-1 Cooling Water Inlet Node,  !- Cooling Water Inlet Node Name
-    SPACE1-1 Cooling Water Outlet Node,  !- Cooling Water Outlet Node Name
-    2.0,                     !- Cooling Control Throttling Range {deltaC}
-    RADIANT COOLING SETPOINTS,  !- Cooling Control Temperature Schedule Name
-    Off,                     !- Condensation Control Type
-    1.0,                     !- Condensation Control Dewpoint Offset
-    CalculateFromCircuitLength,   !- Number of Circuits
-    106.7;                   !- Circuit Length
-```
-
-### Low Temperature Radiant Variable Flow (ZoneHVAC) Outputs
-
-* HVAC,Average,Zone Radiant HVAC Heating Rate [W]
-
-* HVAC,Sum,Zone Radiant HVAC Heating Energy [J]
-
-* HVAC,Average,Zone Radiant HVAC Cooling Rate [W]
-
-* HVAC,Sum,Zone Radiant HVAC Cooling Energy [J]
-
-* HVAC,Average,Zone Radiant HVAC Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Radiant HVAC Inlet Temperature [C]
-
-* HVAC,Average,Zone Radiant HVAC Outlet Temperature [C]
-
-* HVAC,Sum,Zone Radiant HVAC Moisture Condensation Time[s]
-
-* HVAC,Sum,Zone Radiant HVAC Heating Fluid Energy [J]
-
-* HVAC,Sum,Zone Radiant HVAC Cooling Fluid Energy [J]
-
-#### Zone Radiant HVAC Heating Rate [W]
-
-This field reports the heating input rate to the low temperature radiant system in Watts. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions and the control scheme defined in the user input.
-
-#### Zone Radiant HVAC Heating Energy [J]
-
-This field reports the heating input to the low temperature radiant system in Joules. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
-
-#### Zone Radiant HVAC Cooling Rate [W]
-
-This field reports the cooling input rate to the low temperature radiant system in Watts. This is the heat sink to the surface that is defined as the radiant system. The cooling rate is determined by the zone conditions and the control scheme defined in the user input.
-
-#### Zone Radiant HVAC Cooling Energy [J]
-
-This field reports the cooling input to the low temperature radiant system in Joules. This is the heat sink to the surface that is defined as the radiant system. The cooling rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
-
-#### Zone Radiant HVAC Mass Flow Rate Rate [kg/s]
-
-This field reports the mass flow rate of water through the low temperature radiant system in kilograms per second.
-
-#### Zone Radiant HVAC Inlet Temperature [C]
-
-This field reports the temperature of water entering the low temperature radiant system in Celsius.
-
-#### Zone Radiant HVAC Outlet Temperature [C]
-
-This field reports the temperature of water leaving the low temperature radiant system in Celsius.
-
-#### Zone Radiant HVAC Moisture Condensation Time[s]
-
-This field reports the amount of time when condensation is occurring.  When using the Off condensation control, this simply reports the amount of time when condensation occurs.  When using the SimpleOff condensation control, this indicates the amount of time when the system has been shut off because of the potential danger of condensation.
-
-#### Zone Radiant HVAC Heating Fluid Energy [J]
-
-This is the demand placed on the hot fluid plant loop connection serving the low temperature radiant system, in Joules.
-
-#### Zone Radiant HVAC Cooling Fluid Energy [J]
-
-This is the demand placed on the cooling fluid plant loop connection serving the low temperature radiant system, in Joules.
-
-### ZoneHVAC:LowTemperatureRadiant:ConstantFlow
-
-This low temperature radiant system (hydronic) is a component of zone equipment that is intended to model any “radiant system� where water is used to supply/remove energy to/from a building surface (wall, ceiling, or floor). The component is controlled via control schedules as described in the syntax below and does not require a zone thermostat. Note that because this unit does not require a thermostat that in cases where no other systems are serving the zone in which this system resides that it will use the heating equipment priority to determine which system will run first.  If the radiant system is serving a zone with forced air equipment, the radiant system will follow the priority order established by the zone thermostat but will still base its response on the controls defined by the user for the radiant system.
-
-The constant flow system differs from the hydronic system describe above in what it controls. The hydronic system varies the flow rate through the radiant system based on some control temperature. The constant flow system keeps flow rate constant via a local circulation pump and varies the water temperature that is sent to the radiant system. This is accomplished with a mixing valve that is controlled by a sensor. This model covers a wide range of low temperature radiant systems: heating and/or cooling, panel or embedded pipes, etc. It is not intended to simulate high temperature electric or gas radiant heaters. Those devices will be handled by a separate model and different input syntax. Low temperature radiant systems that use electric resistance heating should also be defined using separate input syntax (ref: ZoneHVAC:LowTemperatureRadiant:Electric). Low temperature radiant systems that vary the flow rate through the radiant system should also be defined using separate input syntax (ref: ZoneHVAC:LowTemperatureRadiant:VariableFlow)
-
-One of the other differences between this model and the variable flow hydronic radiant system is that the constant flow radiant system has a built-in local secondary loop. It will recirculate flow coming out of the system and mix this with flow from the loop to arrive at the desired inlet temperature to the radiant system (note that this model has the temperature sensor AFTER the pump to insure proper inlet temperature to the radiant system). The local loop also contains a pump which is assumed to be upstream of the radiant system and after the mixing valve. So, the local loop can have some recirculation. The flow from the main loop may also bypass the radiant system if more than enough flow is available and the main loop is also a constant flow system.
-
-#### Field: Name
-
-This field is an unique user assigned name for an instance of a constant flow low temperature radiant system. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This field is the name of the schedule (ref: Schedule) that denotes whether the constant flow low temperature radiant system can run during a given time period. A schedule value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for that time period. A value greater than 0 (usually 1 is used) denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Zone Name
-
-This field is the name of the zone (Ref: Zone) in which the constant flow low temperature radiant system is principally located and intended to affect. A system that is between two zones will still act upon each zone; however, the zone name referenced here should be the zone that controls the radiant system response.
-
-#### Field: Surface Name or Radiant Surface Group Name
-
-This field is the name of the surface (Ref: BuildingSurface:Detailed) or surface list (Ref: ZoneHVAC:LowTemperatureRadiant:SurfaceGroup) in which the hydronic tubing is embedded/contained. This specification attaches the source or sink from the radiant system to a particular surface and the contribution of the system to the heat balances of that surface. If this field is a surface list, then the source or sink is attached to all of the surfaces in the list with the radiant system surface group defining the breakdown of how flow rate is split between the various surfaces. Base surfaces (e.g., BuildingSurface:Detailed), door surfaces and internal mass are valid. Window surfaces are not valid surface types for embedded radiant systems.
-
-#### Field: Hydronic Tubing Inside Diameter
-
-This field is the inside diameter of the tubes through which water is circulated for the system being defined by this statement. The inside diameter should be recorded in meters and is used to determine the convective heat transfer from the water to the inside surface of the hydronic tubing.
-
-#### Field: Hydronic Tubing Length
-
-This field is the total length of pipe embedded in the surface named above in the surface name field. The length of the tube should be entered in meters and is used to determine the effectiveness of heat transfer from the fluid being circulated through the tubes and the tube/surface. Longer tubing lengths result in more heat being transferred to/from the radiant surface to the circulating fluid. This field is autosizable.
-
-#### Field: Temperature Control Type
-
-This field specifies along with setpoint (control) and water schedules how the user wishes to control the constant flow radiant system. The temperature denoted in the setpoint schedule can refer to one of five different temperatures: the zone mean air temperature, the zone mean radiant temperature, the zone operative temperature, the outdoor dry-bulb temperature, or the outdoor wet-bulb temperature. The choice of temperature is controlled by the current field—temperature control type. The user must select from the following options:
-
-* MeanAirTemperature
-
-* MeanRadiantTemperature
-
-* OperativeTemperature
-
-* OutdoorDryBulbTemperature
-
-* OutdoorWetBulbTemperature
-
-Operative temperature for radiant system controls is the average of Mean Air Temperature and Mean Radiant Temperature. If the user does not select a control type, **MeanAirTemperature** control is assumed by EnergyPlus. See the throttling range and control temperature schedule fields below for more information.
-
-#### Field: Rated Flow Rate
-
-This field is the maximum flow rate of water through the radiant system in m<sup>3</sup>/sec. This flow rate is held constant by the local component pump, but the user has the option of varying this flow rate via a schedule (see next input field). The constant flow system will accept this flow rate and control the inlet temperature based on the control and water temperature schedules defined below. This field is autosizable.
-
-#### Field: Pump Flow Rate Schedule Name
-
-This field modifies the maximum flow rate of water through the radiant system in m<sup>3</sup>/sec. This input is “optional�. If the user does not enter a schedule, the flow rate through the radiant system is assumed to be constant during all hours that it is operating based on the value entered in the previous input field. Note that the values for this schedule must be between zero and one. The values in this schedule are multipliers on the previous field – Rated Flow Rate.
-
-#### Field: Rated Pump Head
-
-This numeric field contains the pump’s rated head in Pascals.
-
-#### Field: Rated Power Consumption
-
-This numeric field contains the pump’s rated power consumption in Watts.
-
-#### Field: Motor Efficiency
-
-This numeric field contains the pump’s efficiency in decimal form (0 = 0%, 1 = 100%).
-
-#### Field: Fraction of Motor Inefficiencies to Fluid Stream
-
-This numeric field contains the pump’s fraction of power loss to the fluid.
-
-#### Field: Heating Water Inlet Node Name
-
-This field contains the name of the hot water inlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a heating coil.
-
-#### Field: Heating Water Outlet Node Name
-
-This field contains the name of the hot water outlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a heating coil.
-
-#### Field: Heating High Water Temperature Schedule Name
-
-This field specifies the high water temperature in degrees Celsius for the temperature control of a constant flow radiant heating system. Water and control temperatures for heating work together to provide a linear function that determines the water temperature sent to the radiant system. The current control temperature (see Temperature Control Type above) is compared to the high and low control temperatures at the current time. If the control temperature is above the high temperature, then the system will be turned off and the water mass flow rate will be zero. If the control temperature is below the low temperature, then the inlet water temperature is set to the high water temperature. If the control temperature is between the high and low value, then the inlet water temperature is linearly interpolated between the low and high water temperature values.  For more information and a graph of how the water and control schedules affect the system operation, please consult the Engineering Reference document.
-
-#### Field: Heating Low Water Temperature Schedule Name
-
-This field specifies the low water temperature in degrees Celsius for the temperature control of a constant flow heating radiant system. For more information on its interpretation, see Heating High Water Temperature Schedule above.
-
-#### Field: Heating High Control Temperature Schedule Name
-
-This field specifies the high control temperature in degrees Celsius for the temperature control of a constant flow heating radiant system. For more information on its interpretation, see Heating High Water Temperature Schedule above.
-
-#### Field: Heating Low Control Temperature Schedule Name
-
-This field specifies the low control temperature in degrees Celsius for the temperature control of a constant flow heating radiant system. For more information on its interpretation, see Heating High Water Temperature Schedule above.
-
-#### Field: Cooling Water Inlet Node Name
-
-This field contains the name of the cold water inlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a cooling coil. As with the maximum cold water flow rate, this field is optional and not required for a heating only system.
-
-#### Field: Cooling Water Outlet Node Name
-
-This field contains the name of the cold water outlet node to the radiant system. Note that this node name must also show up in the branch description when defining the plant demand side network in a manner identical to defining a cooling coil. As with the maximum cold water flow rate, this field is optional and not required for a heating only system.
-
-#### Field: Cooling High Water Temperature Schedule Name
-
-This field specifies the high water temperature in degrees Celsius for the temperature control of a constant flow radiant cooling system. Water and control temperatures for heating work together to provide a linear function that determines the water temperature sent to the radiant system. The current control temperature (see Temperature Control Type above) is compared to the high and low control temperatures at the current time. If the control temperature is above the high temperature, then the inlet water temperature is set to the low water temperature. If the control temperature is below the low temperature, then system will be turned off and the water mass flow rate will be zero. If the control temperature is between the high and low value, then the inlet water temperature is linearly interpolated between the low and high water temperature values.  For more information and a graph of how the water and control schedules affect the system operation, please consult the Engineering Reference document.
-
-#### Field: Cooling Low Water Temperature Schedule Name
-
-This field specifies the low water temperature in degrees Celsius for the temperature control of a constant flow cooling radiant system. For more information on its interpretation, see Cooling High Water Temperature Schedule above.
-
-#### Field: Cooling High Control Temperature Schedule Name
-
-This field specifies the high control temperature in degrees Celsius for the temperature control of a constant flow cooling radiant system. For more information on its interpretation, see Cooling High Water Temperature Schedule above.
-
-#### Field: Cooling Low Control Temperature Schedule Name
-
-This field specifies the low control temperature in degrees Celsius for the temperature control of a constant flow cooling radiant system. For more information on its interpretation, see Cooling High Water Temperature Schedule above.
-
-#### Field: Condensation Control Type
-
-When radiant systems do cooling, there is the possibility that condensation will occur on the surface that is being cooled.  This is due to the fact that the surface temperature may drop below the dew-point temperature of the space.  When this occurs, condensation on the surface will occur.  In EnergyPlus, users have several options for handling this situation including: Off and SimpleOff.  When the user chooses the Off option, EnergyPlus will not do anything other than produce a warning message when condensation is predicted to occur.  The program will simply continue on; no moisture will be removed from the zone air and there will be no adjustment of the surface temperature as a result of the condensation.  When the user chooses the SimpleOff option, the program will predict cases where condensation will occur and shut-off the radiant system to avoid this situation.  With this option, the users also have the opportunity to adjust when the system will shut down.  This is specified with the next parameter (field: condensation differential parameter). This parameter is optional and EnergyPlus will use the SimpleOff strategy when this parameter is not specified.
-
-#### Field: Condensation Control Dewpoint Offset
-
-This optional parameter is only valid with the SimpleOff condensation handling algorithm (see previous input parameter).  It establishes the difference between the calculated dew-point temperature of the space and the allowed surface temperature to which the surface can drop before the radiant system shuts down in degrees Celsius.  This parameter can be any positive, negative, or zero value.  When this parameter is zero, the radiant system will shut down when the surface temperature drops to the dew-point temperature or below.  When this parameter is positive, the radiant system will shut down when the surface is the number of degrees Celsius above the dew-point temperature.  This allows some extra safety to avoid condensation.  When this parameter is negative, the radiant system will shut down when the surface temperature is the number of degrees Celsius below the dew-point temperature.  While not recommended, this strategy allows the user to simulate a situation where small amounts of condensation are tolerable.
-
-#### Field: Number of Circuits
-
-This optional input allows the user to choose between modeling each surface in the radiant system as a single hydronic circuit or to allow the program to divide the surface into multiple parallel hydronic circuits based on the next input field *Circuit Length*. To model as a single circuit choose *OnePerSurface*. To model as multiple circuits choose *CalculateFromCircuitLength*. It is recommended that *CalculateFromCircuitLength* be chosen. The default is *OnePerSurface* for backward compatibility with older versions of EnergyPlus.
-
-#### Field: Circuit Length
-
-The length in meters of each parallel hydronic circuit in a surface. Used when the previous input field is set to *CalculateFromCircuitLength*. The default is 106.7 meters (350 feet), which is the maximum circuit length allowed in Title 24.
-
-
-
-An example IDF with a constant flow low temperature radiant system is shown below.
-
-```idf
-ZoneHVAC:LowTemperatureRadiant:ConstantFlow,
-    Resistive Zone Radiant Floor,  !- name of CONSTANT FLOW low temperature radiant system
-    RadiantSysAvailSched,  !- availability schedule
-    Resistive Zone,  !- Zone name
-    Zn001:Flr001,  !- Surface name or group
-    0.012,  !- Hydronic tubing inside diameter {m}
-    400.0,  !- Hydronic tubing length {m}
-    MeanAirTemperature,  !- temperature control type
-    0.0004,  !- maximum water volumetric flow rate {m3/s}
-    ,  !-schedule for flow rate (optional, non-existent means constant)
-    30000, !-Rated Pump Head in Pa
-    50,  !-Rated Power Consumption in W
-    0.87,  !-Motor Efficiency
-    0.1,  !-Fraction of Motor Inefficiencies to Fluid Stream
-    Resistive Zone Radiant Water Inlet Node,  !- heating water inlet node
-    Resistive Zone Radiant Water Outlet Node,  !- heating water outlet node
-    RadHeatHighWaterTemp,  !-high water temperature schedule
-    RadHeatLowWaterTemp,   !-low water temperature schedule
-    RadHeatHighControlTemp, !-high control temperature schedule
-    RadHeatLowControlTemp,  !-low control temperature schedule
-    Zone 1 Cooling Water Inlet Node,  !- cooling water inlet node
-    Zone 1 Cooling Water Outlet Node,  !- cooling water outlet node
-    RadCoolHighWaterTemp, !-cooling high water temperature schedule
-    RadCoolLowWaterTemp,  !-cooling low water temperature schedule
-    RadCoolHighControlTemp, !- cooling high control temperature schedule
-    RadCoolLowControlTemp,  !- cooling low control temperature schedule
-    SimpleOff,              !- condensation control type
-    0.5,                    !- condensation control dewpoint offset
-    CalculateFromCircuitLength,   !- Number of Circuits
-    106.7;                   !- Circuit Length
-```
-
-### Low Temperature Radiant Constant Flow (ZoneHVAC) Outputs
-
-* HVAC,Average,Zone Radiant HVAC Heating Rate [W]
-
-* HVAC,Sum,Zone Radiant HVAC Heating Energy [J]
-
-* HVAC,Average,Zone Radiant HVAC Cooling Rate [W]
-
-* HVAC,Sum,Zone Radiant HVAC Cooling Energy [J]
-
-* HVAC,Average,Zone Radiant HVAC Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Radiant HVAC Injection Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Radiant HVAC Recirculation Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Radiant HVAC Inlet Temperature [C]
-
-* HVAC,Average,Zone Radiant HVAC Outlet Temperature [C]
-
-* HVAC,Average,Zone Radiant HVAC Pump Inlet Temperature [C]
-
-* HVAC,Average,Zone Radiant HVAC Pump Electric Power[W]
-
-* HVAC,Sum,Zone Radiant HVAC Pump Electric Energy [J]
-
-* HVAC,Average,Zone Radiant HVAC Pump Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Radiant HVAC Pump Fluid Heat Gain Rate [W]
-
-* HVAC,Sum,Zone Radiant HVAC Pump Fluid Heat Gain Energy [J]
-
-* HVAC,Sum,Zone Radiant HVAC Moisture Condensation Time [s]
-
-* HVAC,Sum,Zone Radiant HVAC Cooling Fluid Heat Transfer Energy [J]
-
-* HVAC,Sum,Zone Radiant HVAC Heating Fluid Heat Transfer Energy [J]
-
-
-
-#### Zone Radiant HVAC Heating Rate [W]
-
-This field reports the heating input rate to the low temperature radiant system in Watts. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions and the control scheme defined in the user input.
-
-#### Zone Radiant HVAC Heating Energy [J]
-
-This field reports the heating input to the low temperature radiant system in Joules. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
-
-#### Zone Radiant HVAC Cooling Rate [W]
-
-This field reports the cooling input rate to the low temperature radiant system in Watts. This is the heat sink to the surface that is defined as the radiant system. The cooling rate is determined by the zone conditions and the control scheme defined in the user input.
-
-#### Zone Radiant HVAC Cooling Energy [J]
-
-This field reports the cooling input to the low temperature radiant system in Joules. This is the heat sink to the surface that is defined as the radiant system. The cooling rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
-
-#### Zone Radiant HVAC Mass Flow Rate [kg/s]
-
-This field reports the mass flow rate of water through the low temperature radiant system in kilograms per second. This should be identical to the pump flow rate for the system.
-
-#### Zone Radiant HVAC Injection Mass Flow Rate [kg/s]
-
-This field reports the mass flow rate of water that is injected into the radiant system from the main loop. A valve will control the injection and recirculation mass flow rates (see next field) to match the temperature controls specified by the user and dictated by the current simulation conditions.
-
-#### Zone Radiant HVAC Recirculation Mass Flow Rate [kg/s]
-
-This field reports the mass flow rate of water that is recirculated from the radiant system outlet and mixed with the injection flow from the main loop. A valve will control the injection and recirculation mass flow rates (see next field) to match the temperature controls specified by the user and dictated by the current simulation conditions.
-
-#### Zone Radiant HVAC Inlet Temperature [C]
-
-This field reports the temperature of water entering the low temperature radiant system in Celsius. This may differ from the inlet node temperature for the component since this component has its own local secondary loop.
-
-#### Zone Radiant HVAC Outlet Temperature [C]
-
-This field reports the temperature of water leaving the low temperature radiant system in Celsius. This may differ from the outlet node temperature for the component since this component has its own local secondary loop.
-
-#### Zone Radiant HVAC Pump Inlet Temperature [C]
-
-This field reports the temperature of water entering the low temperature radiant system pump in Celsius. This may differ from the inlet node temperature for the component since this component has its own local secondary loop. It is assumed that the pump is upstream of the radiant system.
-
-#### Zone Radiant HVAC Pump Electric Power [W]
-
-This field reports the rate of electric power consumption for the pump which supplies flow to the constant flow radiant system in Watts.
-
-#### Zone Radiant HVAC Pump Electric Energy [J]
-
-This field reports the electric power consumption for the pump which supplies flow to the constant flow radiant system in Joules.
-
-#### Zone Radiant HVAC Pump Mass Flow Rate [kg/s]
-
-This field reports the mass flow rate of water through the low temperature radiant system pump in kilograms per second. This should be identical to the flow rate for the system.
-
-#### Zone Radiant HVAC Pump Fluid Heat Gain Rate [W]
-
-This field reports the rate at which heat is added to the fluid stream as it passes through the pump in Watts. This heat is reflected in the radiant system inlet temperature which will be different from the pump inlet temperature if this field has a non-zero value.
-
-#### Zone Radiant HVAC Pump Fluid Heat Gain Energy [J]
-
-This field reports the amount of heat energy added to the fluid stream as it passes through the pump in Joules. This heat is reflected in the radiant system inlet temperature which will be different from the pump inlet temperature if this field has a non-zero value.
-
-#### Zone Radiant HVAC Moisture Condensation Time [s]
-
-This field reports the amount of time when condensation is occurring.  When using the Off condensation control, this simply reports the amount of time when condensation occurs.  When using the SimpleOff condensation control, this indicates the amount of time when the system has been shut off because of the potential danger of condensation.
-
-#### Zone Radiant HVAC Cooling Fluid Heat Transfer Energy [J]
-
-The heat transfer energy for the cooling fluid connection, in Joules.
-
-#### Zone Radiant HVAC Heating Fluid Heat Transfer Energy [J]
-
-The heat transfer energy for the heating fluid connection, in Joules.
-
-### ZoneHVAC:LowTemperatureRadiant:Electric
-
-This low temperature radiant system (electric) is a component of zone equipment that is intended to model any “radiant system� where electric resistance heating is used to supply energy (heat) to a building surface (wall, ceiling, or floor). The component is controlled by the radiant system controls that are defined in the syntax below and this control does not require the use of a zone thermostat unless the unit is being autosized. Note also that because this unit does not require a thermostat that in cases where no other systems are serving the zone in which this system resides that it will use the heating equipment priority to determine which system will run first.  If the radiant system is serving a zone with forced air equipment, the radiant system will follow the priority order established by the zone thermostat but will still base its response on the controls defined by the user for the radiant system.
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-The control is accomplished by varying the electrical power supplied to the unit. This model covers either a radiant panel system or wires embedded in entire walls, floors, or ceilings. It is not intended to simulate high temperature electric or gas radiant heaters. Those devices will be handled by a separate model and different input syntax. Low temperature radiant systems that use water flowing through tubes to provide heat to the system should also be defined using separate input syntax (ref: Low Temp Radiant System:Hydronic).
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-#### Field: Name
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-This field is an unique user assigned name for an instance of an electric low temperature radiant system. Any reference to this unit by another object will use this name.
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-#### Field: Availability Schedule Name
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-This field is the name of the schedule (ref: Schedule) that denotes whether the electric low temperature radiant system can operate during a given time period. A schedule value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for that time period. A value greater than 0 (usually 1 is used) denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
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-#### Field: Zone Name
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-This field is the name of the zone (Ref: Zone) in which the electric low temperature radiant system is principally located and intended to affect. A system that is between two zones will still act upon each zone; however, the zone name referenced here should be the zone that controls the radiant system response.
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-#### Field: Surface Name or Radiant Surface Group Name
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-This field is the name of the surface (Ref: BuildingSurface) or surface list (Ref: ZoneHVAC:LowTemperatureRadiant:SurfaceGroup) in which the hydronic tubing is embedded/contained. This specification attaches the source or sink from the radiant system to a particular surface and the contribution of the system to the heat balances of that surface. If this field is a surface list, then the source or sink is attached to all of the surfaces in the list with the radiant system surface group defining the breakdown of how flow rate is split between the various surfaces. Base surfaces (e.g., BuildingSurface:Detailed), door surfaces and internal mass are valid. Window surfaces are not valid surface types for embedded radiant systems.
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-#### Field: Heating Design Capacity Method
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-Enter the method used to determine the maximum electrical power (heating design capacity ) or enter the method for scalable sizing the maximum electrical power of low temperature radiant electric unit. Input allowed is either *HeatingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedHeatingCapacity*. If this input field is left blank or zero, then autosizing is assumed. *HeatingDesignCapacity* means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the maximum or nominal design heating capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the low temperature radiant electric unit. *FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is *HeatingDesignCapacity*.
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-#### Field: Heating Design Capacity {W}
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-This field is for the maximum amount of electric energy rate (electric power) converted into heat in low temperature radiant electric unit in watts. This input field is autosizable. The controls for the radiant system will vary the amount of power supplied to the surface between zero input and the maximum power specified in this field as the lower and upper bounds, respectively. Note that if the user elects to autosize this field that a standard zone thermostat such as would be used for a forced air system must be defined as autosizing calculations are based on the zone thermostat value and not on the low temperature radiant electric unit control values. The default input for this input field is autosize.
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-#### Field: Heating Design Capacity Per Floor Area {W/m2}
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-Enter the heating capacity per unit floor area in m3/s-m2 of low temperature radiant electric system. This field is required field when the Heating Design Capacity Method is *CapacityPerFloorArea*. The program calculates the heating capacity from floor area of the zone served by the low temperature radiant electric unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
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-#### Field: Fraction of Autosized Heating Design Capacity {-}
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-Enter the heating capacity as a fraction of the autosized heating capacity of low temperature radiant electric unit. This input field is required when the Heating Design Capacity Method is *FractionOfAutosizedHeatingCapacity*. The program calculates the heating capacity from the design autosized heating capacity and user specified fraction. Design day sizing must be specified. This field may be left blank. The default value is 1.0.
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-#### Field: Temperature Control Type
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-This field specifies along with the throttling range and setpoint schedules how the user wishes to control the low temperature electric radiant system. The temperature denoted in the setpoint schedule can refer to one of three different temperatures: the zone mean air temperature, the zone mean radiant temperature, the zone operative temperature, the outdoor dry-bulb temperature, or the outdoor wet-bulb temperature. The choice of temperature is controlled by the current field—temperature control type. The user must select from the following options:
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-* MeanAirTemperature
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-* MeanRadiantTemperature
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-* OperativeTemperature
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-* OutdoorDryBulbTemperature
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-* OutdoorWetBulbTemperature
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-Operative temperature for radiant system controls is the average of Mean Air Temperature and Mean Radiant Temperature. If the user does not select a control type, **MeanAirTemperature** control is assumed by EnergyPlus. See the throttling range and control temperature schedule fields below for more information.
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-#### Field: Heating Throttling Range
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-This field specifies the range of temperature in degrees Celsuis over which the radiant system throttles from zero heat input via the electric resistance wires up to the maximum defined by the maximum electrical power field described above. The throttling range parameter is used in conjunction with the control temperature (see below) to define the response of the system to various zone conditions. The heating control temperature schedule specifies the “setpoint� temperature where the power input to the system is at half of the maximum power input. For example, if the heating control temperature setpoint is currently 15°C and the heating throttling range is 2°C, the electrical power supplied to the radiant system will be zero when the controlling temperature (MAT, MRT, Operative Temperature, ODB, or OWB; see control type field above) is at or above 16°C and the maximum power input when the controlling temperature is at or below 14°C. This represents a throttling range of 2°C around the setpoint of 15°C. In between 14°C and 16°C, the power input to the radiant system is varied linearly.
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-#### Field: Heating Setpoint Temperature Schedule Name
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-This field specifies the heating setpoint or control temperature for the radiant system in degrees Celsius. Used in conjunction with the previous field (heating throttling range), it will define whether or not the system is running and the current power input to the radiant surface. Power input to the system is varied linearly around the setpoint temperature based on the throttling range and the maximum electrical power parameters (see above). It should be noted that this control schedule will allow different setpoint temperatures throughout the year for heating. In addition, this schedule may be different that the thermostatic control schedule defined for overall operation of components serving the zone in which the radiant system is located. The thermostatic control determines whether or not there is a heating or cooling load in the space and thus whether the systems should be operating. This field simply controls the flow rate to the radiant system.
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-An example IDF with an electric low temperature radiant system is shown below.
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-```idf
-ZoneHVAC:LowTemperatureRadiant:Electric, Zone 2 Radiant Floor,
-         RadiantPanelAvailSched ,    ! Availability schedule
-         EAST ZONE ,                 ! Zone name (name of zone system is serving)
-         Zn002:Flr001 ,              ! Surface name (name of surface system is embedded in)
-         HeatingDesignCapacity,      !- Heating Design Capacity Method
-         10000,                      !- Heating Design Capacity{ W }
-         ,                           !- Heating Design Capacity Per Floor Area{ W / m2 }
-         ,                           !- Fraction of Autosized Heating Design Capacity{ -}
-         MeanAirTemperature,         ! control type (control on mean air temperature)
-         2.0 ,                       ! heating throttling range (in C)
-         Radiant Heating Setpoints ; ! heating setpoint temperatures
-```
-
-### Low Temperature Radiant Electric (ZoneHVAC) Outputs
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-* HVAC,Average, Zone Radiant HVAC Electric Power[W]
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-* HVAC,Sum, Zone Radiant HVAC Electric Energy [J]
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-* HVAC,Sum,Zone Radiant HVAC Heating Energy [J]
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-* HVAC,Average, Zone Radiant HVAC Heating Rate [W]
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-#### Zone Radiant HVAC Electric Power [W]
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-This field reports the rate at which electric energy is “burned� in the low temperature radiant system in Watts. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions and the control scheme defined in the user input.
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-#### Zone Radiant HVAC Electric Energy [J]
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-This field reports the amount of electric energy “burned� in the low temperature radiant system in Joules. This is the heat source to the surface that is defined as the radiant system. The heating rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
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-#### Zone Radiant HVAC Heating Energy [J]
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-#### Zone Radiant HVAC Heating Rate [W]
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-These outputs are the heating provided by the low temperature radiant system to the zone, in Watts or Joules.
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-### ZoneHVAC:LowTemperatureRadiant:SurfaceGroup
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-A low temperature radiant system (hydronic or electric) may consist of multiple active surfaces that are serving to condition the space. Surfaces that act serially can be specified as multiple radiant systems using the standard radiant system input described above. However, if the multiple surfaces act in parallet, the Radiant System Surface Group input line is used to specify which surfaces are acting in a coordinated fashion and how flow rate is split between the surfaces. This list of surfaces (the name it is assigned) replaces the name of a single surface in the radiant system input described above. Note that all of the surfaces within a single list must be a part of the same zone and that the zone of these surfaces must also match the zone the radiant system is attempting to condition.
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-#### Field: Name
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-This field is an unique user assigned name for the list of surfaces that are acting in coordination with one another. Any reference to this list by a radiant system will use this name.
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-#### Field Set: Surface Name, Flow Fraction to Surface
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-The pairs of Surface Name, Flow Fraction to Surface are used in several objects. There can be up to 10 specified. The object is extensible so more can be added.
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-#### Field: Surface &lt;x&gt; Name
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-This field is the name of a surface in the zone being conditioned by the radiant system. Base surfaces (e.g., BuildingSurface:Detailed), door surfaces and internal mass are valid. Window surfaces are not valid surface types for embedded radiant systems.
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-#### Field: Flow Fraction for Surface &lt;x&gt;
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-This field is the fraction of the total radiant system flow rate that is being sent to this particular surface. Note that the Surface Name/Surface Flow Fraction pair can be repeated up to 10 times. Flow rate fractions must sum to unity, otherwise the program will not accept the input as valid.
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-An example IDF with an electric low temperature radiant system is shown below.
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-```idf
-ZoneHVAC:LowTemperatureRadiant:SurfaceGroup,
-    Zone 1 Radiant Surfaces, !- name of surface list
-    Zn001:Flr001,            !- Surface name 1
-    0.75,                    !- Flow fraction for surface 1
-    Zn001:Roof001,           !- Surface name 2
-    0.25;                    !- Flow fraction for surface 2
-```
-
-### ZoneHVAC:HighTemperatureRadiant
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-The high temperature radiant system (gas-fired or electric) is a component of zone equipment that is intended to model any “high temperature� or “high intensity� radiant system where electric resistance or gas-fired combustion heating is used to supply energy (heat) to a building occupants directly as well as the building surfaces (wall, ceiling, or floor). The component is controlled by the radiant system controls defined in the syntax below and this control does not require the use of a zone thermostat unless the unit is being autosized. Note also that because this unit does not require a thermostat that in cases where no other systems are serving the zone in which this system resides that it will use the heating equipment priority to determine which system will run first.  If the radiant system is serving a zone with forced air equipment, the radiant system will follow the priority order established by the zone thermostat but will still base its response on the controls defined by the user for the radiant system.
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-The control is accomplished by varying the electrical power supplied to or gas consumed by the unit. It is not intended to simulate low temperature electric or hydronic radiant systems. Those devices will be handled by a separate model and different input syntax (ref: the low temperature systems described elsewhere).
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-#### Field: Name
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-This field is an unique user assigned name for an instance of the high temperature radiant system. Any reference to this unit by another object will use this name.
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-#### Field: Availability Schedule Name
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-This field is the name of the schedule (ref: Schedule) that denotes whether the high temperature radiant system can operate during a given time period. A schedule value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for that time period. A value greater than 0 (usually 1 is used) denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
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-#### Field: Zone Name
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-This field is the name of the zone (Ref: Zone) in which the high temperature radiant system is principally located and intended to affect.
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-#### Field: Heating Design Capacity Method
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-Enter the method used to determine the maximum electrical power (heating design capacity ) or enter the method for scalable sizing the maximum electrical power of high temperature radiant system unit. Input allowed is either *HeatingDesignCapacity*, *CapacityPerFloorArea*, and *FractionOfAutosizedHeatingCapacity*. If this input field is left blank or zero, then autosizing is assumed. *HeatingDesignCapacity* means user specifies the magnitude of maximum or nominal heating capacity or the program calculates the maximum or nominal design heating capacity if autosize is specified. *CapacityPerFloorArea* means the program calculates the design heating capacity from user specified heating capacity per floor area and floor area of the zone served by the high temperature radiant electric unit. *FractionOfAutosizedHeatingCapacity* means the program calculates the design heating capacity from user specified fraction and the auto-sized design heating capacity. The default method is *HeatingDesignCapacity*.
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-#### Field: Heating Design Capacity {W}
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-This field is for the maximum amount of electric energy rate (electric power) converted into heat in high temperature radiant electric unit in watts. This input field is autosizable. The controls for the radiant system will vary the amount of power supplied to the surface between zero input and the maximum power specified in this field as the lower and upper bounds, respectively. Note that if the user elects to autosize this field that a standard zone thermostat such as would be used for a forced air system must be defined as autosizing calculations are based on the zone thermostat value and not on the radiant system control values. The default input for this field is autosize.
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-#### Field: Heating Design Capacity Per Floor Area {W/m2}
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-Enter the heating capacity per unit floor area in m3/s-m2 of high temperature radiant electric unit. This field is required field when the Heating Design Capacity Method is *CapacityPerFloorArea*. The program calculates the heating capacity from floor area of the zone served by the high temperature radiant electric unit and the heating capacity per unit floor area value specified by the user. This field may be left blank.
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-#### Field: Fraction of Autosized Heating Design Capacity {-}
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-Enter the heating capacity as a fraction of the autosized heating capacity for high temperature radiant electric unit. This input field is required when the Heating Design Capacity Method is *FractionOfAutosizedHeatingCapacity*. The program calculates the heating capacity from the design autosized heating capacity and user specified fraction. Design day sizing run must be specified. This field may be left blank. The default value is 1.0.
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-#### Field: Fuel Type
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-This field denotes the type of high temperature radiant heater: gas or electric. The user must specify this by inputting either the keyword “**NaturalGas**� or “**Electricity**� for this field.
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-#### Field: Combustion Efficiency
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-This field is the combustion efficiency for a gas high temperature radiant heater. This value should be greater than 0 and less than or equal to 1. It is intended to take into account any potential inefficiencies in the combustion process inside the radiant heater. The heater gas consumption is the ratio of heater output over the combustion efficiency. This parameter has no meaning for an electric high temperature radiant heater and is ignored when the previous field is equal to “Electric�.
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-#### Field: Fraction of Input Converted to Radiant Energy
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-This field specifies what fraction of the power input to the high temperature radiant heater is actually radiant heat transfer. The fraction should be between 0 and 1. In conjunction with the next two parameters, it defines the breakdown of how the power input to the heater is distributed to the rest of the zone. The sum of these fractions must be less than or equal to 1. If the fractions are less than one, the remaining energy is added to the zone as convective heat transfer. The radiant heat transfer from the heat is distributed to people and surfaces using the distribution fractions listed below.
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-#### Field: Fraction of Input Converted to Latent Energy
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-This field specifies the fraction of the power input to the high temperature radiant heater that is converted to a latent heat gain within the space. This may be appropriate when a combustion process produces moisture that is transferred into the space. The latent heat addition from a high temperature radiant heater is handled as any other latent heat gain within the space, affecting the moisture balance on the zone air.
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-#### Field: Fraction of Input that Is Lost
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-This field specifies the fraction of power input to the high temperature radiant heater that is “lost�. This energy is a loss term, and this fraction of the input power has no effect on the zone heat balances.
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-#### Field: Temperature control type
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-This field specifies along with the throttling range and setpoint schedules how the user wishes to control the high temperature radiant system. The temperature denoted in the setpoint schedule can refer to one of three different temperatures: a mean air temperature, a mean radiant temperature, or an operative temperature. The choice of temperature is controlled by the current field—temperature control type. The user must select from the following options:
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-* MeanAirTemperature
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-* MeanRadiantTemperature
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-* OperativeTemperature
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-* MeanAirTemperatureSetpoint
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-* MeanRadiantTemperatureSetpoint
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-* OperativeTemperatureSetpoint
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-If the user does not select a control type, OperativeTemperature control is assumed by EnergyPlus. For the setpoint control strategies (those ending in Setpoint above), EnergyPlus will attempt to find the correct heater output to meet the heating setpoint temperature (see below) through iteration and interpolation. This will more closely match the operation of an actual thermostat, but it will require significantly longer execution times.  For more information on the standard piecewise linear control algorithm used by the Mean Air Temperature, Mean Radiant Temperature, and Operative Temperature control types (the “non-Setpoint� controls), see the throttling range and control temperature schedule fields below for more information.
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-#### Field: Heating Throttling Range
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-This field specifies the range of temperature in degrees Celsuis over which the radiant system throttles from zero heat input via the electric resistance wires up to the maximum defined by the maximum electrical power field described above. The throttling range parameter is used in conjunction with the control temperature (see below) to define the response of the system to various zone conditions. The heating control temperature schedule specifies the “setpoint� temperature where the power input to the system is at half of the maximum power input. For example, if the heating control temperature setpoint is currently 15°C and the heating throttling range is 2°C, the electrical power supplied to the radiant system will be zero when the controlling temperature (Mean Air Temperature, Mean Radiant Temperature, and Operative Temperature; see control type field above) is at or above 16°C and the maximum power input when the controlling temperature is at or below 14°C. This represents a throttling range of 2°C around the setpoint of 15°C. In between 14°C and 16°C, the power input to the radiant system is varied linearly.
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-#### Field: Heating Setpoint Temperature Schedule Name
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-This field specifies the heating setpoint or control temperature for the radiant system in degrees Celsius. Used in conjunction with the previous field (heating throttling range), it will define whether or not the system is running and the current power input to the radiant surface. Power input to the system is varied linearly around the setpoint temperature based on the throttling range and the maximum electrical power parameters (see above). It should be noted that this control schedule will allow different setpoint temperatures throughout the year for heating. In addition, this schedule may be different that the thermostatic control schedule defined for overall operation of components serving the zone in which the radiant system is located. The thermostatic control determines whether or not there is a heating or cooling load in the space and thus whether the systems should be operating. This field simply controls the flow rate to the radiant system.
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-#### Field: Fraction of Radiant Energy Incident on People
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-This field specifies the fraction of radiant heat transfer to the zone from the radiant heater that is incident directly on people within the space. This has an impact on the predicted thermal comfort of the zone occupants. Note that since the thermal comfort models only use the results of the zone heat balances this energy is accounted for within the heat balance as convective energy, directly affecting the zone air heat balance. The basic assumption here is that most radiant energy falling on people will most likely be convected to the surroundings. This is a simplification of reality, but it maintains the overall energy balance.
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-#### Field Set: Surface Name, Fraction of radiant energy to Surface
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-The pairs of Surface Name, Fraction of Radiant Energy to Surface are used in several objects. There can be up to 20 specified.
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-#### Field: Surface &lt;x&gt; Name
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-This field is the name of the first surface to which radiant heat transfer from the high temperature radiant heater is distributed. Used in conjunction with the next field, it helps to define the distribution of the radiant energy on the surfaces within the zone. Note that up to 20 pairs of surface names and corresponding fractions may be entered for a single radiant heater system.
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-#### Field: Fraction of Radiant Energy to Surface &lt;x&gt;
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-This field is paired with the preceding surface name (previous field) to define the fraction of radiant heat transfer leaving the high temperature radiant system that is incident on a particular surface. Users should take into account the directionality of high temperature radiant heaters and their location when defining the value for this input field. Note that the sum of all fractions plus the fraction of radiant energy incident on people must add up to less than or equal to 1.
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-An example IDF with a high temperature radiant system is shown below.
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-```idf
-ZoneHVAC:HighTemperatureRadiant, Zone 2 Radiant Heater,
-         RadiantPanelAvailSched ,   ! Availability schedule
-         EAST ZONE ,                ! Zone name (name of zone system is serving)
-         10000,                     !- Heating Design Capacity{ W }
-         ,                          !- Heating Design Capacity Per Floor Area{ W / m2 }
-         ,                          !- Fraction of Autosized Heating Design Capacity{ -}
-         Gas,                       ! type of heater (either gas or electric)
-         0.8,                       ! combustion efficiency (ignored for electric radiant heaters)
-         0.80,                      ! fraction radiant
-         0.00,                      ! fraction latent
-         0.00,                      ! fraction lost
-         OperativeTemperature,      ! temperature control type (controls on operative temperature)
-         2.0 ,                      ! heating throttling range (in C)
-         Radiant Heating Setpoints, ! heating setpoint temperatures
-         0.04,                      ! fraction of radiant energy that is incident directly on people
-         Zn002:Flr001, 0.80,        ! fraction of radiant energy that is incident on the surface indicated
-         Zn002:Wall001, 0.04,       ! fraction of radiant energy that is incident on the surface indicated
-         Zn002:Wall002, 0.04,       ! fraction of radiant energy that is incident on the surface indicated
-         Zn002:Wall003, 0.04,       ! fraction of radiant energy that is incident on the surface indicated
-         Zn002:Wall004, 0.04;       ! fraction of radiant energy that is incident on the surface indicated
-```
-
-### High Temperature Radiant (ZoneHVAC) Outputs
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-* HVAC,Average, Zone Radiant HVAC Heating Rate [W]
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-* HVAC,Sum, Zone Radiant HVAC Heating Energy [J]
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-* HVAC,Average, Zone Radiant HVAC Gas Rate [W]
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-* HVAC,Sum, Zone Radiant HVAC Gas Energy [J]
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-* HVAC,Average, Zone Radiant HVAC Electric Power[W]
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-* HVAC,Sum, Zone Radiant HVAC Electric Energy [J]
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-#### Zone Radiant HVAC Heating Rate [W]
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-This field reports the rate at which energy is transferred from the high temperature radiant system to the zone in Watts. This rate is determined by the zone conditions and the control scheme defined in the user input. Note that this amount takes into account any combustion inefficiency and thus could be different that the gas consumption rate in a high temperature gas radiant system.
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-#### Zone Radiant HVAC Heating Energy [J]
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-This field reports the amount of energy transferred from the high temperature gas radiant system to the zone in Joules. This amount is determined by the zone conditions, the control scheme defined in the user input, and the timestep. Note that this amount takes into account any combustion inefficiency and thus could be different that the gas consumption in a high temperature gas radiant system.
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-#### Zone Radiant HVAC Gas Rate [W]
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-This field reports the rate at which gas is “burned� in a high temperature gas radiant system in Watts. This rate is determined by the zone conditions and the control scheme defined in the user input.
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-#### Zone Radiant HVAC Gas Energy [J]
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-This field reports the amount of gas “burned� in a high temperature gas radiant system in Joules. This amount is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
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-#### Zone Radiant HVAC Electric Power[W]
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-This field reports the rate at which electric energy is “burned� in a high temperature electric radiant system in Watts. This rate is determined by the zone conditions and the control scheme defined in the user input.
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-#### Zone Radiant HVAC Electric Energy [J]
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-This field reports the amount of electric energy “burned� in a high temperature electric radiant system in Joules. This amount is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
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-### ZoneHVAC:VentilatedSlab
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-Ventilated slab systems in general use outdoor air to “precool� slabs with colder nighttime air.  This method of precooling the thermal mass of a space can be very effective when nighttime temperatures are low and the mass of the system is high enough to provide a significant amount of cooling potential during the day to counteract internal heat gains within a zone.  Nearly all ventilated slabs are simple systems such as that shown in the right side of Figure 128.  The fan is shown in a blow through position, but the model will allow either a blow or draw through configuration.
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-![f102\_jpeg](media/image321.png)
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-Figure 128. Ventilated Slab model - basic system
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-#### Field: Name
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-This field is a unique user assigned name for an instance of a ventilated slab system. Any reference to this unit by another object will use this name. Other objects that use this ventilated slab system will reference it by this name.
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-#### Field: Availability Schedule Name
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-This field is the name of the schedule (ref: Schedule) that denotes whether the ventilated slab system can run during a given time period. A schedule value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for that time period. A value greater than 0 (usually 1 is used) denotes that the unit is available to operate during that time period. If this field is left blank, the schedule has a value of 1 for all time periods.
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-![Presentation1](media/image322.png)
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-Figure 129. Example operating schedule for Ventilated Slab
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-#### Field: Zone Name
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-This field is the name of the zone (Ref: Zone) in which the ventilated slab system is principally located and intended to affect. A system that is between two zones will still act upon each zone; however, the zone name referenced here should be the zone that controls the system response.
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-#### Field: Surface Name or Radiant Surface Group Name
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-This field is the name of the surface (Ref: Surface) or surface list (Ref: ZoneHVAC:VentilatedSlab:SlabGroup) in which the hollow cores are embedded/contained. This specification attaches the source or sinks from the radiant system to a particular surface and the contribution of the system to the heat balances of that surface. If this field is a surface list, then the source or sink is attached to all of the surfaces in the list with the radiant system surface group defining the breakdown of how flow rate is split between the various surfaces. Only base surfaces (Walls, Roofs, Floors) are valid. Window/Door surfaces and Internal Mass are not valid surface types for embedded radiant systems.
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-#### Field: Maximum Air Flow Rate
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-This field allows the user to enter the maximum volumetric flow rate of air through the ventilated slab system in m<sup>3</sup>/sec.  This parameter should be some real number greater than zero.
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-#### Field: Outdoor Air Control Type
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-This field allows the user to control how outdoor air is used in the ventilated slab system.  The ventilated slab system described by this syntax has its own outdoor air handler.  The three options for outdoor air control are “**VariablePercent**�, “**FixedTemperature**� and “**FixedAmount**�. Those keywords are the only allowed choices for this parameter.  In general, the variable percent control will attempt to vary the amount of outdoor air between some minimum and maximum schedules of fractions (see next two fields) to best meet the current heating or cooling load. The fixed temperature control will vary the amount of outdoor air between the minimum schedule (fraction of maximum, see next field) and 100% available outdoor air to come as close as possible to a desired mixed air temperature (see two fields down) that can be scheduled. The fixed amount control will fix the outdoor air flow rate as minimum outdoor air flow rate and schedule specified by the user and automatically set the maximum and minimum outside flow rate to be equal by ignoring the maximum outdoor air flow rate. More information on the controls and operation of the ventilated slab are given in the section above (preceding the IDF description).
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-#### Field: Minimum Outdoor Air Flow Rate
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-This field allows the user to enter the minimum volumetric flow rate of outdoor air (in m<sup>3</sup>/sec) that will be brought in to the ventilated slab. The actual minimum outdoor air flow rate will be this number multiplied by the schedule value from the minimum outdoor air schedule. If “FixedAmount� type is selected as the outdoor air control strategy, the outdoor air flow rate will be fixed at the value of this field and the ventilated slab will automatically set the maximum and minimum outside flow rate to be equal by ignoring the maximum outdoor air flow rate.
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-#### Field: Minimum Outdoor Air Schedule Name
-
-This field contains a schedule name (ref: Schedule) that should contain values for the minimum outdoor air used by the ventilated slab system for IAQ or other reasons.  Note that if the ventilated slab is scheduled off or if there is no load sensed in the zone that the system will not operate even to achieve the minimum air fraction.  However, if the system is operating, it will always bring in at least this fraction of the minimum air flow rate (see minimum air flow rate field above). If “FixedAmount� type is selected as the outdoor air control strategy, the actual outdoor air flow rate will be this number multiplied by the minimum outdoor air flow rate in the field above. The ventilated slab will automatically set the maximum and minimum outdoor air schedule to be equal by ignoring the maximum outdoor air schedule.
-
-#### Field: Maximum Outdoor Air Flow Rate
-
-This field allows the user to enter the maximum volumetric flow rate of outdoor air that can be brought into the ventilated slab in m<sup>3</sup>/sec.  This parameter should be some real number greater than zero.  Note that the value for this parameter may be less than the maximum air flow rate of the ventilated slab and this may affect the maximum fraction of outdoor air within the control strategy defined above. This parameter is an absolute maximum and will supercede any scheduled fraction of the ventilated slab maximum airflow rate. If “FixedAmount� type is selected as the outdoor air control strategy, this field will be ignored and be automatically set to be equal to the minimum outdoor air flow rate specified in the field above.
-
-#### Field: Maximum Outdoor Air Fraction or Temperature Schedule Name
-
-This field can have one of two meanings depending the type of control selected in the outdoor air control type parameter above.  If “VariablePercent� or “FixedAmount� was selected, then this field is a schedule name (ref: Schedule) corresponding to a maximum air fraction schedule. Furthermore, if “FixedAmount� type is selected as the outdoor air control strategy, this field will be ignored and be automatically set to be equal to the minimum outdoor air fraction specified in the field below. Note that this is a fraction of the maximum airflow rate field (see parameter above) for the ventilated slab. If “FixedTemperature� control was selected, then this field is still a schedule name (ref: Schedule), but it corresponds to a schedule of mixed air temperatures that the outdoor air control will try to attain.
-
-#### Field: System Configuration Type
-
-This field allows the user to control how the air is circulated using the ventilated slab system.  The options for system configuration are
-
-* SlabOnly
-
-* SlabAndZone
-
-* SeriesSlabs
-
-In the **SlabOnly**, the ventilation air is sent to the slab only and does not enter the zone.  In the **SlabAndZone**, the air first enters the slab and then is delivered to the zone before returning to the system. With the **SeriesSlabs** option, the user specifies a list of slabs (ZoneHVAC:VentilatedSlab:SlabGroup). This list determines the order of slabs through which the air passes.  In this option, air is not delivered to any zone.
-
-#### Field: Hollow Core Inside Diameter
-
-This field is the inside diameter of the cores through which air is circulated for the system being defined by this statement.  The inside diameter should be recorded in meters and is used to determine the convective heat transfer from the circulated air to the inside surface of the ventilated slab.
-
-#### Field: Hollow Core Length
-
-This field is the length of core embedded in the surface named above in the surface name field.  In other words, this should be the distance that air travels as it through the slab.  The length of the hollow core in the slab should be entered in meters and is used to determine the effectiveness of heat transfer from the air being circulated through the cores and the core inside surface.  Longer core lengths result in more heat transferred to/from the radiant surface to the circulating fluid.
-
-#### Field: Number of Cores
-
-This field allows the user to specify how many cores there are in the ventilated slab.  Air flow will be divided equally among the different cores.
-
-#### Field: Temperature Control Type
-
-This field specifies along with the throttling range and setpoint schedules how the user wishes to control the ventilated slab system.  The temperature denoted in the set temperature schedule can refer to one of seven different temperatures: the zone mean air temperature, the zone mean radiant temperature, the zone operative temperature, the surface temperature of the ventilated slab, the outdoor dry-bulb temperature, the outdoor wet-bulb temperature, or the dewpoint temperature of zone mean air temperature.  The choice of temperature is controlled by the current field—temperature control type.  The user must select from the following options:
-
-* MeanAirTemperature
-
-* MeanRadiantTemperature
-
-* OperativeTemperature
-
-* OutdoorDryBulbTemperature
-
-* OutdoorWetBulbTemperature
-
-* SurfaceTemperature
-
-* ZoneAirDewPointTemperature
-
-If the user does not select a control type, **MeanAirTemperature** control is assumed by EnergyPlus. See the control temperature schedule fields below for more information.
-
-#### Field: Heating High Air Temperature Schedule Name
-
-This field specifies the high air temperature in degrees Celsius for the temperature control of a ventilated slab system. Air and control temperatures for heating work together to provide a linear function that determines the air temperature sent to the ventilated slab. The current control temperature (see Temperature Control Type above) is compared to the high and low control temperatures at the current time.      If the control temperature is above the high temperature, then the inlet air temperature is set to the low air temperature. If the control temperature is below the low temperature, then the inlet air temperature is set to the high air temperature. If the control temperature is between the high and low value, then the inlet air temperature is linearly interpolated between the low and high air temperature values.
-
-#### Field: Heating Low Air Temperature Schedule Name
-
-This field specifies the low air temperature in degrees Celsius for the temperature control of a ventilated slab. For more information on its interpretation, see Heating High Air Temperature Schedule above.
-
-#### Field: Heating High Control Temperature Schedule Name
-
-This field specifies the high control temperature in degrees Celsius for the temperature control of a ventilated slab. For more information on its interpretation, see Heating High Air Temperature Schedule above.
-
-#### Field: Heating Low Control Temperature Schedule Name
-
-This field specifies the low control temperature in degrees Celsius for the temperature control of a ventilated slab. For more information on its interpretation, see Heating High Air Temperature Schedule above.
-
-#### Field: Cooling High Air Temperature Schedule Name
-
-This field specifies the high air temperature in degrees Celsius for the temperature control of a ventilated slab system. Air and control temperatures for cooling work together to provide a linear function that determines the air temperature sent to the ventilated slab system. The current control temperature (see Temperature Control Type above) is compared to the high and low control temperatures at the current time. If the control temperature is above the high temperature, then the inlet air temperature is set to the low air temperature. If the control temperature is below the low temperature, then the inlet air temperature is set to the high air temperature. If the control temperature is between the high and low value, then the inlet air temperature is linearly interpolated between the low and high air temperature values.
-
-#### Field: Cooling Low Air Temperature Schedule Name
-
-This field specifies the low air temperature in degrees Celsius for the temperature control of a constant flow cooling radiant system. For more information on its interpretation, see Cooling High Air Temperature Schedule above.
-
-#### Field: Cooling High Control Temperature Schedule Name
-
-This field specifies the high control temperature in degrees Celsius for the temperature control of a constant flow cooling radiant system. For more information on its interpretation, see Cooling High Air Temperature Schedule above.
-
-#### Field: Cooling Low Control Temperature Schedule Name
-
-This field specifies the low control temperature in degrees Celsius for the temperature control of a ventilated slab system. For more information on its interpretation, see Cooling High Air Temperature Schedule above.
-
-#### Field: Return Air Node Name
-
-This field is a node name used to identify the node that serves as the zone return air inlet to the ventilated slab system. This node is one of the inlets to the outdoor air mixer which is implicit in the ventilated slab system model. For “SlabAndZone� configuration, the Return Air Node will typically be the same node as a zone exhaust node. For “SlabOnly� or “SeriesSlabs� configuration, this node name is required but will have zero flow.
-
-#### Field: Slab In Node Name
-
-This field is a node name used to identify the node that serves as the inlet of the ventilated slab or series of slabs, after the outdoor air mixer, fan, and optional coils.
-
-#### Field: Zone Supply Air Node Name
-
-This field is a node name used to identify the node that serves as the outlet from the ventilated slab system to the zone when using the “SlabAndZone� configuration. It is the node exiting the slab section of the system. This node will typically be the same node as a zone inlet node. In the case of “SlabOnly� or “SeriesSlabs� configuration, this field will be ignored and it should be left BLANK.
-
-#### Field: Outdoor Air Node Name
-
-This field is a node name used to identify the node associated with fresh outdoor air brought into the ventilated slab system outdoor air mixer.  This node should also be specified in an OutdoorAir:Node or OutdoorAir:NodeList object.
-
-#### Field: Relief Air Node Name
-
-This field is a node name used to identify the node associated with air exhausted out of the ventilated slab system to the outdoor environment.
-
-#### Field: Outdoor Air Mixer Outlet Node Name
-
-This field is a node name used to identify the node associated with the “mixed� air of the ventilated slab.  These conditions are post-“mixing box� since they are the conditions of the fraction of return air combined with the outdoor air.  Since this is a simple system, this can also be viewed as the conditions of the air being sent to the coils.
-
-#### Field: Fan Outlet Node Name
-
-This field is a node name used to identify the node that serves as the air outlet from the fan.
-
-#### Field: Fan Name
-
-This field is the name of a fan (ref: Fan:ConstantVolume) that is part of the ventilated slab system.  This name links the ventilated slab to particular fan data entered elsewhere in the input data file.  A fan name is required since it is the prime mover of air in the ventilated slab system.
-
-#### Field: Coil Option Type
-
-This field allows the user to specify the coil operating options as one of the following options:
-
-* None
-
-* Heating
-
-* Cooling
-
-* HeatingAndCooling
-
-If **None** is selected, the ventilated slab does not have any coils, and any other input will be ignored. If either **Heating** or **Cooling** is selected, only a heating or cooling coil, respectively, is present.  Thus, only four more inputs will be expected. If **HeatingAndCooling** is selected, both heating and cooling coil input must be entered, and the ventilated slab will have both a heating and a cooling coil.
-
-#### Field: Heating Coil Object Type
-
-This field is the type of coil (ref: Coil:Heating:Water, Coil:Heating:Electric, Coil:Heating:Gas, Coil:Heating:Steam) that is used for heating in the ventilated slab system. This field must be one of the following keywords: Coil:Heating:Water, Coil:Heating:Electric, Coil:Heating:Gas, Coil:Heating:Steam.  It is used in conjunction with the heating coil name (see next field) to specify the heating coil present within the system.
-
-#### Field: Heating Coil Name
-
-This field is the name of the heating coil that is part of the ventilated slab system.  It is assumed that there is always some sort of heating coil associated with a ventilated slab system.  This name links the ventilated slab to particular heating coil data entered elsewhere in the input data file.
-
-#### Field: Hot Water or Steam Inlet Node Name
-
-This field corresponds to the water inlet node to the heating coil for a water coil.  The water inlet node controls how a water heating coil operates.  This field is ignored/not needed for gas and electric heating coils.
-
-#### Field: Cooling Coil Object Type
-
-This field is the name of the cooling coil (ref: Coil:Cooling:Water, Coil:Cooling:Water:DetailedGeometry, CoilSystem:Cooling:Water:HeatExchangerAssisted) that is part of the ventilated slab system.  This name links the ventilated slab system to particular cooling coil data entered elsewhere in the input data file. If no cooling coil is present, the previous field may be followed by a semi-colon and the remaining parameters in this statement may be ignored.
-
-#### Field: Cooling Coil Name
-
-This field is the name of the cooling coil that is part of the ventilated slab system.  It is assumed that there is always some sort of cooling coil associated with a ventilated slab system.  This name links the ventilated slab to particular cooling coil data entered elsewhere in the input data file.
-
-#### Field: Cold Water Inlet Node Name
-
-This field corresponds to the water inlet node to the cooling coil.  The water inlet node controls how a water cooling coil operates and is required for the ventilated slab system that has a cooling coil associated with it to function properly.
-
-#### Field: Availability Manager List Name
-
-This optional input field is the name of an AvailabilityManagerAssignmentList object. An Availability Manager Assignment List is a list of Availability Managers giving both Availability Manager type and name. The availability managers in the list apply to this ventilated slab object’s fan. If the ventilated slab is available (per the Availability Schedule Name input field above) and this input field has a valid availability manager assignment list name, then the availability managers in the list determine when and if the fan of this ventilated slab object should be on or off.
-
-#### Field: Design Specification ZoneHVAC Sizing Object Name
-
-This optional input field is the name of a DesignSpecification:ZoneHVAC:Sizing object. The name must correspond to unique name of a DesignSpecification:ZoneHVAC:Sizing object. A Design Sepcification Zone HVAC Sizing object defines scalable sizing methods for sizing input fields such as Maximum Air Flow Rate in this Ventilated Slab zone HVAC object. The scaled Maximum Air Flow Rate in turn is used to size cooling and heating capacity of the coils.
-
-An example IDF with a ventilated slab is shown below.
-```idf
-  ZoneHVAC:VentilatedSlab,
-    Zone4VentSlab,           !- Name
-    VentSlabAvailability,    !- Availability Schedule Name
-    SPACE4-1,                !- Zone Name
-    F4-1,                    !- Surface Name or Radiant Surface Group Name
-    0.84,                    !- Maximum Air Flow Rate {m3/s}
-    VariablePercent,         !- Outdoor Air Control Type
-    0.168,                   !- Minimum Outdoor Air Flow Rate {m3/s}
-    U2MinOASched,            !- Minimum Outdoor Air Schedule Name
-    0.84,                    !- Maximum Outdoor Air Flow Rate {m3/s}
-    VentSlabMaxOA,           !- Maximum Outdoor Air Fraction or Temperature Schedule Name
-    SlabAndZone,             !- System Configuration Type
-    0.050,                   !- Hollow Core Inside Diameter {m}
-    15.0,                    !- Hollow Core Length {m}
-    50.0,                    !- Number of Cores
-    MeanRadiantTemperature,  !- Temperature Control Type
-    VentSlabHotHighAir,      !- Heating High Air Temperature Schedule Name
-    VentSlabHotLowAir,       !- Heating Low Air Temperature Schedule Name
-    VentSlabHotHighControl,  !- Heating High Control Temperature Schedule Name
-    VentSlabHotLowControl,   !- Heating Low Control Temperature Schedule Name
-    VentSlabCoolHighAir,     !- Cooling High Air Temperature Schedule Name
-    VentSlabCoolLowAir,      !- Cooling Low Air Temperature Schedule Name
-    VentSlabCoolHighControl, !- Cooling High Control Temperature Schedule Name
-    VentSlabCoolLowControl,  !- Cooling Low Control Temperature Schedule Name
-    Zone4VentSlabReturnAirNode,  !- Return Air Node Name
-    Zone4VentslabSlabInNode, !- Slab In Node Name
-    Zone4Inlets,             !-Zone Supply Air Node Name
-    Zone4VentSlabOAInNode,   !- Outdoor Air Node Name
-    Zone4VentSlabExhNode,    !- Relief Air Node Name
-    Zone4VentSlabOAMixerOutletNode,  !-Outdoor Air Mixer Outlet Node Name
-    Zone4VentSlabFanOutletNode,  !- Fan Outlet Node Name
-    Zone4VentSlabFan,        !- Fan Name
-    HeatingAndCooling,       !- Coil Option Type
-    Coil:Heating:Electric,   !- Heating Coil Object Type
-    Zone4VentSlabHeatingCoil,!- Heating Coil Name
-    ,                        !- Hot Water or Steam Inlet Node Name
-    Coil:Cooling:Water,      !- Cooling Coil Object Type
-    Zone4VentSlabCoolingCoil,!- Cooling Coil Name
-    Zone4VentSlabChWInletNode;  !- Cold Water Inlet Node Name
-```
-
-
-### Ventilated Slab (ZoneHVAC) Outputs
-
-* HVAC,Average,Zone Ventilated Slab Radiant Heating Rate [W]
-
-* HVAC,Sum,Zone Ventilated Slab Radiant Heating Energy [J]
-
-* HVAC,Average,Zone Ventilated Slab Radiant Cooling Rate [W]
-
-* HVAC,Sum,Zone Ventilated Slab Radiant Cooling Energy [J]
-
-* HVAC,Average,Zone Ventilated Slab Coil Heating Rate [W]
-
-* HVAC,Sum,Zone Ventilated Slab Coil Heating Energy [J]
-
-* HVAC,Average,Zone Ventilated Slab Coil Total Cooling Rate [W]
-
-* HVAC,Sum,Zone Ventilated Slab Coil Total Cooling Energy [J]
-
-* HVAC,Average,Zone Ventilated Slab Coil Sensible Cooling Rate [W]
-
-* HVAC,Sum,Zone Ventilated Slab Coil Sensible Cooling Energy [J]
-
-* HVAC,Average,Zone Ventilated Slab Coil Latent Cooling Rate [W]
-
-* HVAC,Sum,Zone Ventilated Slab Coil Latent Cooling Energy [J]
-
-* HVAC,Average, Zone Ventilated Slab Air Mass Flow Rate [kg/s]
-
-* HVAC,Average, Zone Ventilated Slab Fan Electric Power [W]
-
-* HVAC,Sum,Zone Ventilated Slab Fan Electric Energy [J]
-
-* HVAC,Average,Zone Ventilated Slab Inlet Air Temperature [C]
-
-* HVAC,Average,Zone Ventilated Slab Outlet Air Temperature [C]
-
-* HVAC,Average,Zone Ventilated Slab Zone Inlet Air Temperature [C]
-
-* HVAC,Average,Zone Ventilated Slab Return Air Temperature [C]
-
-* HVAC,Average,Zone Ventilated Slab Fan Outlet Air Temperature [C]
-
-* HVAC,Average,Zone Ventilated Slab Fan Availability Status []
-
-#### Zone Ventilated Slab Radiant Heating Rate  [W]
-
-This field reports the radiant heating input rate of the ventilated slab system to the zone it is serving in Watts.  This is determined by outlet and zone air conditions and the mass flow rate through the ventilated slab system.
-
-#### Zone Ventilated Slab Radiant Heating Energy [J]
-
-This field is the heating radiant input of the ventilated slab system to the zone it is serving in Joules over the timestep being reported.  This is determined by outlet and zone air conditions, the mass flow rate through the ventilated slab system, and the timestep.
-
-#### Zone Ventilated Slab Radiant Cooling Rate [W]
-
-This field reports the radiant cooling input rate to the ventilated slab system in Watts. This is the heat sink to the surface that is defined as the ventilated slab system. The cooling rate is determined by the zone conditions and the control scheme defined in the user input.
-
-#### Zone Ventilated Slab Radiant Cooling Energy [J]
-
-This field reports the radiant cooling input to the ventilated slab system in Joules. This is the heat sink to the surface that is defined as the radiant system. The cooling rate is determined by the zone conditions, the control scheme defined in the user input, and the timestep.
-
-#### Zone Ventilated Slab Coil Heating Rate [W]
-
-This field reports the heating input rate of the heating coil of ventilated slab system the zone it is serving in Watts.  This is determined by return air and zone air conditions and the mass flow rate through the ventilation slab system.
-
-#### Zone Ventilated Slab Coil Heating Energy [J]
-
-This field is the heating output of the heating coil of the ventilated slab system the zone it is serving in Joules over the timestep being reported.  This is determined by return air and zone air conditions, the mass flow rate through the ventilation slab system, and the timestep.
-
-#### Zone Ventilated Slab Coil Total Cooling Rate [W]
-
-This field reports the total cooling (sensible plus latent) output rate of the cooling coil of the ventilated slab system to the zone it is serving in Watts.  This is determined by outlet and zone air conditions and the mass flow rate through the ventilation slab system.
-
-#### Zone Ventilated Slab Coil Total Cooling Energy [J]
-
-This field is the total cooling (sensible plus latent) output of the cooling coil of the ventilated slab system to the zone it is serving in Joules over the timestep being reported.  This is determined by outlet and zone air conditions, the mass flow rate through the ventilation slab system, and the timestep.
-
-#### Zone Ventilated Slab Coil Sensible Cooling Rate [W]
-
-This field reports the sensible cooling output rate of the cooling coil of the ventilated slab system to the zone it is serving in Watts.  This is determined by outlet and zone air conditions and the mass flow rate through the ventilation slab system.
-
-#### Zone Ventilated Slab Coil Sensible Cooling Energy [J]
-
-This field is the sensible cooling output of the cooling coli of the ventilated slab system to the zone it is serving in Joules over the timestep being reported.  This is determined by outlet and zone air conditions, the mass flow rate through the ventilation slab system, and the timestep.
-
-#### Zone Ventilated Slab Coil Latent Cooling Rate [W]
-
-This field reports the latent cooling output rate of the cooling coil of the ventilated slab system to the zone it is serving in Watts.  This is determined by outlet and zone air conditions and the mass flow rate through the ventilation slab system.
-
-#### Zone Ventilated Slab Coil Latent Cooling Energy [J]
-
-This field is the latent cooling output of the cooling coli of the ventilated slab system to the zone it is serving in Joules over the timestep being reported.  This is determined by outlet and zone air conditions, the mass flow rate through the ventilation slab system, and the timestep.
-
-#### Zone Ventilated Slab Air Mass Flow Rate [kg/s]
-
-This field reports the mass flow rate of air through the ventilated slab system in kilograms per second.
-
-#### Zone Ventilated Slab Fan Electric Power [W]
-
-This field reports the electric power consumption rate of the fan of the ventilated slab system in Watts.
-
-#### Zone Ventilated Slab Fan Electric Energy [J]
-
-This field reports the electric power consumed by the fan of the ventilated slab system over the timestep in Joules.
-
-#### Zone Ventilated Slab Inlet Air Temperature [C]
-
-This field reports the temperature of air entering the ventilated slab system in Celsius.
-
-#### Zone Ventilated Slab Outlet Air Temperature [C]
-
-This field reports the temperature of air leaving the ventilated slab system in Celsius.
-
-#### Zone Ventilated Slab Zone Inlet Air Temperature [C]
-
-This field reports the temperature of air entering the zone in Celsius.
-
-#### Zone Ventilated Slab Return Air Temperature [C]
-
-This field reports the temperature of air leaving the zone in Celsius. When system does not circulate air to zone(“SlabOnly� Configuration), the slab outlet temperature and return air temperature will be the same.
-
-#### Zone Ventilated Slab Fan Outlet Air Temperature [C]
-
-This field reports the fan outlet air temperature for the ventilated slab system in Celsius.
-
-#### Zone Ventilated Slab Fan Availability Status []
-
-This is the availability status of the ventilated slab fan. This status flag is a result of the calculations made by the Availability Manager(s) listed in an AvailabilityManagerAssignmentList object and/or calculations made by Hybrid Ventilation Manager object. The AvailabilityManagerAssignmentList is an optional input in the ventilated slab object. When a single availability manager is used in an Availability Manager Assignment List, this is also the availability status reported by the specific availability manager (Ref. AvailabilityManager:\* Outputs). For multiple availability managers in an Availability Manager Assignment List along with Hybrid Ventilation Manager, rules to determine fan availability status are described in the section ‘Group – System Availability Managers’. The control status outputs are represented using integers 0 through 3. These integers represent NoAction (0), ForceOff (1), CycleOn (2), and CycleOnZoneFansOnly (3). Since the status output is averaged, the output result may not correspond to the values described here when output variable frequencies other than detailed are used. Use the “detailed� reporting frequency (Ref. Output:Variable object) to view the availability status at each simulation timestep.
-
-### ZoneHVAC:VentilatedSlab:SlabGroup
-
-A ventilated slab system may consist of multiple active slabs that are serving to condition the zone. Slabs that act serially can be specified as multiple radiant systems using the standard ventilated slab input described above. This list of surfaces (the name it is assigned) replcaces the name of a single surface in the ventilated slab system input described above.
-
-#### Field : Name of Ventilated Slab Surface Group
-
-This field is a unique user assigned name for the list of surfaces that are acting in coordination with one another. Any reference to this list by a ventilated slab system will use this name.
-
-#### Field: Zone Name
-
-This field is the name of the zone in which the surface is principally located and intended to affect.
-
-#### Field: Surface Name
-
-This field is the name of a surface in the zone being conditioned by the ventilated slab system. Only base surfaces like walls, floors and roofs are valid. Door/Window Surface and Internal Mass are not valid surface types for the ventilated slab system.
-
-#### Field: Core Diameter
-
-This field is the inside diameter of the cores through which air is circulated for the surface being defined by this statement.  The inside diameter should be recorded in meters and is used to determine the convective heat transfer from the circulated air to the inside surface of the ventilated slab.
-
-#### Field: Core length
-
-This field is the length of core embedded in the surface named above in the surface name field.  In other words, this should be the distance that air travels as it through the slab.  The length of the hollow core in the surface should be entered in meters and is used to determine the effectiveness of heat transfer from the air being circulated through the cores and the core inside surface.  Longer core lengths result in more heat transferred to/from the radiant surface to the circulating fluid.
-
-#### Field: Number of Cores
-
-This field allows the user to specify how many cores there are in the ventilated slab.  Air flow will be divided equally among the different cores.
-
-#### Field: Slab Inlet Node Name
-
-This field is a node name (character string) used to identify the node that serves as the inlet (air side) to the surface.  In EnergyPlus, nodes represent points between components or at various points in the loops.  While a node name may be referenced more than once in an input data file, each node must have a unique name.
-
-#### Field: Slab Outlet Node Name
-
-This field is a node name (character string) used to identify the node that serves as the outlet (air side) of the surface.  In EnergyPlus, nodes represent points between components or at various points in the loops.  While a node name may be referenced more than once in an input data file, each node must have a unique name.
-
-An Example IDF with a ventilated slab system is shown below
-
-```idf
-ZoneHVAC:VentilatedSlab:SlabGroup,
-    Z125,                    !- Name
-    SPACE1-1,                !- Zone 1 Name
-    C1-1,                    !- Surface 1 Name
-    0.05,                    !- Core Diameter for Surface 1
-    30,                      !- Core Length for Surface 1
-    20,                      !- Core Numbers for Surface 1
-    Z1VentslabIn,            !- Slab In Node Name for Surface 1
-    Z1VentSlabout,           !- Slab Outlet Node Name for Surface 1
-    SPACE2-1,                !- Zone 2 Name
-    C2-1,                    !- Surface 2 Name
-    0.05,                    !- Core Diameter for Surface 2
-    15,                      !- Core Length for Surface 2
-    20,                      !- Core Numbers for Surface 2
-    Z2VentSlabIn,            !- Slab In Node Name for Surface 2
-    Z2VentSlabOut,           !- Slab Outlet Node Name for Surface 2
-    SPACE5-1,                !- Zone 3 Name
-    C5-1,                    !- Surface 3 Name
-    0.05,                    !- Core Diameter for Surface 3
-    30,                      !- Core Length for Surface 3
-    20,                      !- Core Numbers for Surface 3
-    Z5VentSlabIn,            !- Slab In Node Name for Surface 3
-    Z5VentSlabOut;           !- Slab Outlet Node Name for Surface 3
-```
-
-
-
-
-
-Group – Refrigeration
----------------------
-
-There are two ways to model a supermarket refrigeration system.  The first, and simplest, approach models the combination of compressor(s) and condenser as a single refrigeration compressor rack object. (A list is used to enter multiple case or walk-in names.)
-
-For the first approach, the input objects needed are:
-
-- One Refrigeration:CompressorRack object
-
-- At least one refrigeration load, which may be any combination of:
-
-- Refrigeration:Case or
-
-- Refrigeration:WalkIn or
-
-- Refrigeration:CaseAndWalkInList objects .
-
-The second approach requires more input objects but also allows the user to model more complex systems.  This detailed approach must be used whenever loads are transferred from one system to another, such as with secondary loops, cascade condensers, or mechanical subcoolers. Again lists are used to enter multiple load or compressor names.
-
-For the detailed approach, the input objects needed are:
-
-- One Refrigeration:System object
-
-- At least one refrigeration load object which may include any combination of:
-
-- Refrigeration:Case,
-
-- Refrigeration:WalkIn,
-
-- Refrigeration:CaseAndWalkInList (may include any combination of cases and walk in cooler names, OR, a list of air chiller names)
-
-- Refrigeration:SecondarySystem,
-
-- Refrigeration:Condenser:Cascade (as a load, cooling a lower-temperature system) objects,
-
-- Refrigeration:TransferLoadList (may include cascade condenser loads and/or secondary loop loads)
-
-- Refrigeration:AirChiller
-
-- At least one Refrigeration:Compressor object (multiple compressors are entered using a Refrigeration:CompressorList),
-
-- One condenser object which may be either:
-
-- Refrigeration:Condenser:AirCooled,
-
-- Refrigeration:Condenser:EvaporativeCooled,
-
-- Refrigeration:Condenser:WaterCooled, or
-
-- Refrigeration:Condenser:Cascade (rejecting heat from this system)
-
-- The object Refrigeration:Subcooler may optionally be included to describe either a liquid suction or mechanical subcooler.
-
-Output variables are also available to describe the total heat exchange between all refrigeration objects and the zones containing these objects. These variables are described at the end of this section after all the refrigeration objects.
-
-### Refrigeration:CompressorRack
-
-The refrigeration compressor rack object works in conjunction with the refrigeration case and walkin objects (Ref. Refrigeration:Case and Refrigeration:WalkIn) to simulate the performance of a refrigerated case system. This object models the electric consumption of the rack compressors and the condenser fans. Heat removed from the refrigerated cases, walkins, and compressor/condenser fan heat can be rejected either outdoors or to a zone. Compressor rack waste heat can also be reclaimed for use by an optional air- or water-heating coil (Ref. Coil:Heating:Desuperheater and Coil:WaterHeating:Desuperheater).
-
-If heat is rejected outdoors, condenser cooling can either be accomplished by direct air flow, evaporative water cooling, or a by water-cooled condenser with appropriate plant loop piping. With evaporative cooling, water is sprayed through the air stream to effectively lower the air temperature experienced by the condenser coil as a result of water evaporation. The use of a water-cooled condenser requires the definition of a plant loop to supply cooling to the condenser.  Waste heat can be reclaimed and stored using a water storage device.
-
-The inputs for the compressor rack object include a name, the heat rejection location, the compressor rack coefficient of performance (COP) at design conditions, the design condenser fan power, and the type of condenser cooling. The model requires two curve objects to describe performance at off-design conditions. If the condenser is water-cooled, the inlet and outlet node names as well as the water outlet temperature schedule name are required.  If the condenser has evaporative cooling, additional inputs for evaporative condenser effectiveness, condenser air flow rate, basin heater parameters, water pump power, water source, and an evaporative cooling availability schedule are available. The names of refrigerated cases and walkins connected to the compressor rack are the final inputs to the model.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a refrigeration compressor rack. Any reference to this compressor rack by another object will use this name.
-
-#### Field: Heat Rejection Location
-
-The location of the compressor rack’s condenser. The compressor rack condenser heat can be directed “Outdoors� to model an outdoor air or water-cooled condenser or “Zone� to model a condenser located in a zone (e.g., a stand-alone packaged refrigerated case with integral condenser located in a conditioned zone). The default for this field is “Outdoors�. If the heat rejection location is “Zone� and no walk-in coolers are served by this compressor rack, then all refrigerated cases connected to this compressor rack must be located in the same zone. If however, walk-in coolers are also served by this compressor rack, then the heat rejection zone name must be specified (see Heat Rejection Zone Name field below) and cases and walk-ins can be located in multiple zones.
-
-NOTE: When modeling a heat reclaim coil, the heat rejection location must be “Outdoors�. If the heat rejection location is “Zone�, the total amount of waste heat available for reclaim (e.g., by a desuperheater heating coil) is set to zero by this compressor rack object and the simulation proceeds.
-
-#### Field: Design Compressor Rack COP
-
-The coefficient of performance (COP) for the compressor rack at design conditions (compressors only, excluding condenser fan power). This value must be greater than zero, with a default value of 2.0 if this field is left blank. This value should represent the compressor rack COP corresponding to the lowest evaporating temperature of any case or walkin served by the rack.
-
-#### Field: Compressor Rack COP Function of Temperature Curve Name
-
-The name of the curve object defining the change in compressor rack COP as a function of the temperature of air entering the condenser. The curve object will be evaluated using the zone air dry-bulb temperature when rack heat rejection location equals “Zone� and the outdoor air dry-bulb temperature when rack heat rejection location equals “Outdoors� and the condenser type is air-cooled. As explained below, if the condenser is cooled by evaporative or water loop cooling, the curve object is evaluated using an effective temperature. The output from this curve is multiplied by the design compressor rack COP to yield the actual COP at the specific air temperature entering the condenser. This curve must be cubic or quadratic (Curve:Cubic or Curve:Quadratic), and should be normalized to 1.0 at the condenser entering air temperature at which the design compressor rack COP occurs. This curve should represent the compressor rack COP corresponding to the lowest evaporating temperature of any case served by the rack.
-
-#### Field: Design Condenser Fan Power
-
-This field defines the design power for the condenser fan(s) in Watts. This field is applicable for air or evaporative cooling only.  If the condenser is water-cooled, the fan power is captured in the cooling object (e.g., cooling tower).  If applicable, this value must be greater than 0.0, with a default value of 250 Watts if this field is left blank.
-
-#### Field: Condenser Fan Power Function of Temperature Curve Name
-
-This field is the name of the curve object defining the change in condenser fan power as a function of the temperature of air entering the condenser. This curve is used to simulate the modulation of air flow by the condenser fans (e.g., staging, multi-speed, or variable speed) as a function of temperature.  The curve object will be evaluated using the zone air dry-bulb temperature when rack heat rejection location equals “Zone� and the outdoor air dry-bulb temperature when rack heat rejection location equals “Outdoors� and the condenser type is air-cooled. As explained below, if the condenser is cooled by evaporative cooling, the curve object is evaluated using an effective temperature. The output from this curve is multiplied by the design condenser fan power to yield the actual fan power at the specific air temperature entering the condenser. This curve must be cubic or quadratic (Curve:Cubic or Curve:Quadratic), and should be normalized to 1.0 at the condenser entering air temperature at which the design condenser fan power occurs. The actual condenser fan power is not allowed to exceed the design condenser fan power defined in the previous input field or go below zero (i.e., the output of the curve object is limited to values from 0.0 to 1.0). If this field is left blank, then the model assumes the condenser fan power is at the design power level when any of the refrigerated cases connected to this rack are operating.
-
-#### Field: Condenser Type
-
-When the heat rejection location is “Outdoors�, the condenser may be either cooled by dry air by specifying “AirCooled�, by wet evaporative cooling by specifying “EvaporativelyCooled�, or by a water loop by specifying “WaterCooled�.  If the condenser type is “WaterCooled�, then a plant cooling loop will need to be defined using other EnergyPlus objects, e.g., plant loop, pump, cooling tower, etc.  The default value is “AirCooled�.
-
-#### Field: Water-cooled Condenser Inlet Node Name
-
-When the condenser type is “WaterCooled�, a node name for the water-side condenser inlet must be provided.
-
-#### Field: Water-cooled Condenser Outlet Node Name
-
-When the condenser type is “WaterCooled�, a node name for the water-side condenser outlet must be provided.
-
-#### Field: Water-cooled Loop Flow Type
-
-When the condenser type is “WaterCooled�, the type of flow loop should be specified.  The two choices are **VariableFlow**, in which a Pump:VariableSpeed needs to  be included in the plant loop, or **ConstantFlow**, in which the loop circuit has a constant flow rate, typically associated with a Pump:ConstantSpeed object.  If the flow type is VariableFlow, the flow needed to remove the condenser heat energy will be calculated and requested of the pump.  If the flow type is Constant Flow, the outlet water temperature will be determined based on the fixed loop flow rate and heat energy to be removed.  The default type is **VariableFlow**. Refer to additional discussion in the Engineering Reference.
-
-#### Field: Water-cooled Condenser Outlet Temperature Schedule Name
-
-When the condenser type is “WaterCooled�, and when the water-cooled loop flow type is “Variable Flow�, the name of a schedule (Ref: Schedule) that defines the desired condenser water outlet temperature must be provided.  The schedule may define an outlet temperature that varies through time.
-
-#### Field: Water-cooled Condenser Design  Flow Rate
-
-When the condenser type is “WaterCooled�, and when the water-cooled loop flow type is “Constant Flow�, this is the design water flow rate in m<sup>3</sup>/s that will be requested initially.  This requested flow will be passed to the loop simulation, and resulting actual flow will be dependent upon supply system capabilities (e.g., pump capability).  The design flow rate must always be less than the maximum flow rate, defined below.
-
-#### Field: Water-cooled Condenser Maximum  Flow Rate
-
-When the condenser type is “Water Cooled�, this is the maximum water flow rate in m<sup>3</sup>/s that will be allowed through the condenser.  When the loop flow type is Variable Flow, if the calculated flow rate is higher than the maximum flow rate, an error message will be generated, and the flow rate will be reset to the maximum flow rate.
-
-#### Field: Water-cooled Condenser Maximum Water Outlet Temperature
-
-When the condenser type is “WaterCooled�, this field specifies the maximum allowed water temperature in degrees C leaving the compressor rack condenser. The default value is 55 degrees C.
-
-#### Field: Water-cooled Condenser Minimum Water Inlet Temperature
-
-When the condenser type is “WaterCooled�, this field specifies the minimum allowed water temperature in degrees C entering the compressor rack condenser. The default value is 10 degrees C.  Refer to additional discussion in the Engineering Reference.
-
-#### Field: Evaporative Condenser Availability Schedule Name
-
-When the condenser type is “EvaporativelyCooled�, the name of the optional schedule (Ref: Schedule) that specifies the time periods that evaporative cooling is available/unavailable. In some colder climates, evaporative cooling is periodically discontinued and the basin sumps drained to avoid freezing. In these times, the condenser runs as a typical dry air cooled condenser, and related evaporative cooling systems (e.g., water pump, basin heaters) do not operate. Use of this optional schedule permits modeling of planned, seasonal interruptions of evaporative cooling. All schedule values must be greater than or equal to zero. Typically, an ON/OFF schedule type is used with values being either 0 or 1. A schedule value of 1 indicates that evaporative cooling is available during the defined time period, and a value of 0 denotes that evaporative cooling is not available during the defined time period. If the schedule name is omitted (blank) and Condenser Type = “Evap Cooled�, then the model assumes that evaporative cooling of the condenser is available for the entire simulation period.
-
-#### Field: Evaporative Condenser Effectiveness
-
-When the condenser type is “EvaporativelyCooled�, this field specifies the effectiveness of the evaporative system in modifying the temperature of the air entering the condenser coil. The resulting effective temperature is determined as
-
-<div>\[{T_{effective}} = {T_{owb}} + (1 - \varepsilon )*[{T_{odb}} - {T_{owb}}]\]</div>
-
-where:
-
-<span>\({T_{effective}}\)</span>       = effective dry-bulb temperature of air entering the condenser cooling coil (°C)
-
-<span>\({T_{owb}}\)</span>           = outdoor air wet-bulb temperature (°C)
-
-<span>\({T_{odb}}\)</span>           = outdoor air dry-bulb temperature (°C)
-
-<span>\(\varepsilon \)</span>               = evaporative condenser effectiveness.
-
-The resulting condenser inlet air temperature is used by the Compressor Rack COP as a Function of Temperature Curve and the Condenser Fan Power as a Function of Temperature Curve. The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0.
-
-If the two function-of-temperature curves (i.e., Compressor Rack COP as a Function of Temperature Curve and Condenser Fan Power as a Function of Temperature Curve) are based on wet-bulb temperature rather than dry-bulb temperature, the evaporative condenser effectiveness should be set to 1.0 for consistency.
-
-#### Field: Evaporative Condenser Air Flow Rate
-
-When the condenser type is “EvaporativelyCooled�, the air volume flow rate, in m<sup>3</sup>per second, entering the evaporative condenser. This value is used to calculate the amount of water evaporated when evaporatively cooling the condenser inlet air. The value for this field must be greater than zero. This input field is also autocalculatable, equivalent to 0.000144 m<sup>3</sup>/s per watt of total cooling capacity [850 cfm/ton] where the total cooling capacity is the sum of the rated total cooling capacities for the refrigerated cases connected to this compressor rack (Ref. Refrigeration:Case).
-
-#### Field: Basin Heater Capacity
-
-When the condenser type is “EvaporativelyCooled�, this field defines the power level of the basin heater, if applicable, used to avoid water freezing in an outdoor evaporative cooler basin. This numeric field contains the capacity of the electric basin heater in Watts per degree Kelvin. This field is used in conjunction with the Basin Heater Set Point Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the dry-bulb temperature of the condenser coil inlet air. The basin heater only operates when the condenser fan is off (i.e., no compressor heat rejection). The basin heater capacity must be greater than or equal to zero, with a default value of 200 W/K if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-When the condenser type is “EvaporativelyCooled�, this numeric field contains the set point temperature (°C) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this set point temperature, as long as the condenser fan is off. The default value is 2°C if this field is left blank.
-
-#### Field: Design Evaporative Condenser Water Pump Power
-
-When the condenser type is “EvaporativelyCooled�, the rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The value for this field must be greater than or equal to 0, with a default value of 1000 Watts if this field is left blank. This input field is also autocalculatable, equivalent to 0.004266 W per watt [15 W/ton] of total cooling capacity where the total cooling capacity is the sum of the rated total cooling capacities for the refrigerated cases and walk-ins connected to this compressor rack (Ref. Refrigeration:Case and Refrigeration:WalkIn)).
-
-#### Field: Evaporative Water Supply Tank Name
-
-When the condenser type is “EvaporativelyCooled�, this field is used to define where the compressor rack obtains water used for evaporative cooling of its condenser. If this field is left blank, the unit will obtain water directly from the mains (Ref. Water Mains Temperatures). If the name of a Water Storage Tank object is used here, then the unit will obtain its water from that tank.
-
-#### Field: Condenser Air Inlet Node Name
-
-This optional alpha field contains the name of the node from which the outdoor compressor rack condenser draws its outdoor air. This field is applicable only when the heat rejection location is “Outdoors� (if the heat rejection location is “Zone�, this field is disregarded). If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, this node name must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
-
-#### Field: End-Use Subcategory
-
-This field allows the specification of a user-defined end-use subcategory (e.g., "Low Temperature Rack"). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the "General" end-use subcategory.
-
-#### Field: Refrigeration Case Name or WalkIn Name or CaseAndWalkInList Name
-
-This alpha field is the name of a single refrigerated case, a single walk in cooler,  the name of a CaseAndWalkInList for multiple refrigerated cases and/or walk-ins, the name of a refrigeration chiller, or the name of a CaseAndWalkInList for multiple refrigeration chillers connected to this compressor rack. Note that if a CaseAndWalkInList contains the name(s) of refrigeration chillers, it CANNOT have the name(s) or any refrigerated cases or walkins . This field is required.
-
-#### Field: Heat Rejection Zone Name
-
-If the Heat Rejection Location is “Zone� and any walk-in coolers are connected to this compressor rack, then this field is required. The compressor rack heat rejection will impact the air heat balance in this zone.
-
-
-
-The following is an example input for a  Refrigeration Compressor Rack with water cooled condenser.
-
-```idf
-Refrigeration:CompressorRack,
-    MediumTempRack,          !- Name
-    Outdoors,                !- Heat Rejection Location
-    1.7,                     !- Design Compressor Rack COP {W/W}
-    RackCOPfTCurve,          !- Compressor Rack COP as a Function of Temperature Curve Name
-    1025.0,                  !- Design Condenser Fan Power {W}
-    RackCondFanCurve,        !- Condenser Fan Power as a Function of Temperature Curve Name
-    WaterCooled,             !- Condenser Type
-    Condenser Inlet Node,    !- Water-cooled Condenser Inlet Node Name
-    Condenser Outlet Node,   !- Water-cooled Condenser Outlet Node Name
-    VariableFlow,            !- Water-cooled Loop Flow Type
-    Cond Outlet Temp Sch,    !- Water-cooled Condenser Outlet Temperature Schedule Name
-    ,                        !- Water-cooled Condenser Design Flow Rate {m3/s}
-    0.003,                   !- Water-cooled Condenser Maximum Flow Rate {m3/s}
-    55,                      !- Water-cooled Condenser Maximum Water Outlet Temperature {C}
-    ,                        !- Water-cooled Condenser Minimum Water Inlet Temperature {C}
-    ,                        !- Evaporative Condenser Availability Schedule Name
-    ,                        !- Evaporative Condenser Effectiveness {dimensionless}
-    ,                        !- Evaporative Condenser Air Volume Flow Rate {m3/s}
-    ,                        !- Basin Heater Capacity {W/K}
-    ,                        !- Basin Heater Set Point Temperature {C}
-    ,                        !- Design Evaporative Condenser Water Pump Power {W}
-    ,                        !- Evaporative Water Supply Tank Name
-    ,                        !- Condenser Air Inlet Node Name
-    ,                        !- End-Use Subcategory
-    MediumTempCaseList;      !- Refrigeration Case Name or WalkIn Name or CaseAndWalkInList Name
-```
-
-
-### Refrigeration Compressor Rack Outputs
-
-If Condenser Type = Water Cooled:
-
-* System,Average, Refrigeration Compressor Rack Condenser Refrigerant Mass Flow Rate [kg/s]
-
-* System,Average, Refrigeration Compressor Rack Condenser Heat Transfer Rate [W]
-
-* System,Sum, Refrigeration Compressor Rack Condenser Heat Transfer Energy [J]
-
-
-
-IF THE RACK SERVES CASES AND/OR WALKINS:
-
-* Zone,Average, Refrigeration Compressor Rack Electric Power [W]
-
-* Zone,Sum, Refrigeration Compressor Rack Electric Energy [J]
-
-* Zone,Average, Refrigeration Compressor Rack Condenser Fan Electric Power [W]
-
-* Zone,Sum, Refrigeration Compressor Rack Condenser Fan Electric Energy [J]
-
-* Zone,Average, Refrigeration Compressor Rack Total Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Compressor Rack Total Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration Compressor Rack COP [W/W]
-
-
-If Condenser Type = Evap Cooled:
-
-* Zone,Average, Refrigeration Compressor Rack Evaporative Condenser Pump Electric Power [W]
-
-* Zone,Sum, Refrigeration Compressor Rack Evaporative Condenser Pump Electric Energy [J]
-
-* Zone,Average, Refrigeration Compressor Rack Evaporative Condenser Basin Heater Electric Power [W]
-
-* Zone,Sum, Refrigeration Compressor Rack Evaporative Condenser Basin Heater Electric Energy [J]
-
-* Zone,Average, Refrigeration Compressor Rack Evaporative Condenser Water Volume Flow Rate [m<sup>3</sup>/s]
-
-* Zone,Sum, Refrigeration Compressor Rack Evaporative Condenser Water Volume [m<sup>3</sup>]
-
-
-
-If Heat Rejection Location = Zone:
-
-* Zone,Average, Refrigeration Compressor Rack Zone Sensible Heating Rate [W]
-
-* Zone,Sum,Refrigeration Compressor Rack Zone Sensible Heating Energy [J]
-
-* Zone,Average, Refrigeration Compressor Rack Return Air Sensible Heating Rate [W]
-
-* Zone,Sum,Refrigeration Compressor Rack Return Air Sensible Heating Energy [J]
-
-
-
-IF THE RACK SERVES REFRIGERATION CHILLERS
-
-* HVAC,Average, Refrigeration Air Chiller Compressor Rack Electric Power [W]
-
-* HVAC,Sum, Refrigeration Air Chiller Compressor Rack Electric Energy [J]
-
-* HVAC,Average,Refrigeration Air Chiller System Compressor Runtime Fraction []
-
-* HVAC,Average, Refrigeration Air Chiller Compressor Rack Condenser Fan Electric Power [W]
-
-* HVAC,Sum, Refrigeration Air Chiller Compressor Rack Condenser Fan Electric Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller Compressor Rack Total Heat Transfer Rate [W]
-
-* HVAC,Sum, Refrigeration Air Chiller Compressor Rack Total Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller Compressor Rack COP [W/W]
-
-
-
-
-
-
-
-
-If Condenser Type = Evap Cooled:
-
-* HVAC,Average, Refrigeration Air Chiller Compressor Rack Evaporative Condenser Pump Electric Power [W]
-
-* HVAC,Sum, Refrigeration Air Chiller Compressor Rack Evaporative Condenser Pump Electric Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller Compressor Rack Evaporative Condenser Basin Heater Electric Power [W]
-
-* HVAC,Sum, Refrigeration Air Chiller Compressor Rack Electric PowerRefrigeration Air Chiller Compressor Rack Evaporative Condenser Basin Heater Electric Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller Compressor Rack Evaporative Condenser Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum, Refrigeration Air Chiller Compressor Rack Evaporative Condenser Water Volume [m3]
-
-
-If Heat Rejection Location = Zone:
-
-* HVAC,Average, Refrigeration Air Chiller Compressor Rack Zone Sensible Heating Rate [W]
-
-* HVAC,Sum,Refrigeration Air Chiller Compressor Rack Zone Sensible Heating Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller Compressor Rack Return Air Sensible Heating Rate [W]
-
-* HVAC,Sum,Refrigeration Air Chiller Compressor Rack Return Air Sensible Heating Energy [J]
-
-#### Refrigeration Compressor Rack Condenser Mass Flow Rate [kg/s]
-
-When condenser type is Water Cooled, this is the mass flow rate of water flowing through the water cooled condenser.
-
-#### Refrigeration Compressor Rack Condenser Heat Transfer Rate [W]
-
-When condenser type is Water Cooled, this is the total heat transfer across the condenser (i.e., compressor energy and case cooling).
-
-#### Refrigeration Compressor Rack Condenser Heat Transfer Energy [J]
-
-When condenser type is Water Cooled, this is the total heat energy flowing across the condenser for the timestep being reported.
-
-#### IF THE RACK SERVES CASES AND OR WALKINS:
-
-#### Refrigeration Compressor Rack Electric Power [W]
-
-This output is the electric power input to the rack compressor(s) in Watts.
-
-#### Refrigeration Compressor Rack Electric Energy [J]
-
-This is the electricity consumption of the rack compressor(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Compressor Runtime Fraction []
-
-This is the runtime operating ratio for the compressor.
-
-#### Refrigeration Compressor Rack Condenser Fan Electric Power [W]
-
-This output is the electric input to the rack condenser fan(s) in Watts.
-
-#### Refrigeration Compressor Rack Condenser Fan Electric Energy [J]
-
-This is the electricity consumption of the rack condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Compressor Rack Total Heat Transfer Rate [W]
-
-This output is the total heat transfer rate of the  refrigeration compressor rack in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases and walk-ins that are connected to this rack. This value does not include compressor or condenser fan heat.
-
-#### Refrigeration Compressor Rack Total Heat Transfer Energy [J]
-
-This is the total heat transfer of the  refrigeration compressor rack in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Compressor Rack COP [W/W]
-
-This field is the  refrigeration compressor rack coefficient of performance. It is the actual compressor rack COP for the timestep being reported, accounting for the COP variation as a function of temperature. It is calculated as the Design Compressor Rack COP times the Compressor Rack COP as a Function of Temperature Curve evaluated at the effective condenser entering air temperature for the timestep being reported.
-
-#### Refrigeration Compressor Rack Evaporative Condenser Pump Electric Power [W]
-
-This is the electrical power requirement in Watts for the timestep being reported for the water pump used with evaporative cooling of the compressor rack condenser.
-
-#### Refrigeration Compressor Rack Evaporative Condenser Pump Electric Energy [J]
-
-This is the electricity consumption in Joules of the water pump used with evaporative cooling of the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### Refrigeration Compressor Rack Evaporative Condenser Basin Heater Electric Power [W]
-
-This is the electrical power requirement in Watts for the timestep being reported for the water heater in the basin of the evaporative system used to cool the compressor rack condenser.
-
-#### Refrigeration Compressor Rack Evaporative Condenser Basin Heater Electric Energy [J]
-
-This is the electricity consumption in Joules of the water heater used to prevent freezing of the evaporative cooling system for the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### Refrigeration Compressor Rack Evaporative Condenser Water Volume Flow Rate [m3/s]
-
-The volumetric flow rate in m<sup>3</sup>/s of water consumed while providing evaporative cooling of the compressor rack condenser.
-
-#### Refrigeration Compressor Rack Evaporative Condenser Water Volume [m3]
-
-This is the water consumed by evaporation in m<sup>3</sup> while providing evaporative cooling of the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Water, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### Refrigeration Compressor Rack Zone Sensible Heating Rate [W]
-
-This field is the rate of sensible heating in Watts provided to the zone by condenser waste heat rejection, which impacts the zone air heat balance.
-
-#### Refrigeration Compressor Rack Zone Sensible Heating Energy [J]
-
-This field is the sensible heating energy in Joules provided to the zone by condenser waste heat rejection for the timestep being reported.
-
-#### Refrigeration Compressor Rack Return Air Sensible Heating Rate [W]
-
-This field is the rate of sensible heating in Watts provided by condenser waste heat rejection to the HVAC return air (zone return air path outlet node), which impacts the HVAC return air temperature. If the HVAC system is off for a simulation timestep (no return air mass flow), then this sensible heating is actually provided to the zone air instead (even though a non-zero value is reported here).
-
-#### Refrigeration Compressor Rack Return Air Sensible Heating Energy [J]
-
-This field is the sensible heating energy in Joules provided by condenser waste heat rejection to the HVAC return air (zone return air path outlet node) for the timestep being reported. If the HVAC system is off for a simulation timestep (no return air mass flow), then this sensible heating is actually provided to the zone air instead (even though a non-zero value is reported here).
-
-#### IF THE RACK SERVES CHILLERS
-
-#### Refrigeration Air Chiller Compressor Rack Electric Power [W]
-
-This output is the electric power input to the rack compressor(s) in Watts.
-
-#### Refrigeration Air Chiller Compressor Rack Electric Energy [J]
-
-This is the electricity consumption of the rack compressor(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller System Compressor Runtime Fraction []
-
-This is the runtime fraction for the compressor serving air chillers.
-
-#### Refrigeration Air Chiller Compressor Rack Condenser Fan Electric Power [W]
-
-This output is the electric input to the rack condenser fan(s) in Watts.
-
-#### Refrigeration Air Chiller Compressor Rack Condenser Fan Electric Energy [J]
-
-This is the electricity consumption of the rack condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller Compressor Rack Total Heat Transfer Rate [W]
-
-This output is the total heat transfer rate of the  refrigeration compressor rack in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases and walk-ins that are connected to this rack. This value does not include compressor or condenser fan heat.
-
-#### Refrigeration Air Chiller Compressor Rack Total Heat Transfer Energy [J]
-
-This is the total heat transfer of the  refrigeration compressor rack in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller Compressor Rack COP [W/W]
-
-This field is the  refrigeration compressor rack coefficient of performance. It is the actual compressor rack COP for the timestep being reported, accounting for the COP variation as a function of temperature. It is calculated as the Design Compressor Rack COP times the Compressor Rack COP as a Function of Temperature Curve evaluated at the effective condenser entering air temperature for the timestep being reported.
-
-#### Refrigeration Air Chiller Compressor Rack Evaporative Condenser Pump Electric Power [W]
-
-This is the electrical power requirement in Watts for the timestep being reported for the water pump used with evaporative cooling of the compressor rack condenser.
-
-#### Refrigeration Air Chiller Compressor Rack Evaporative Condenser Pump Electric Energy [J]
-
-This is the electricity consumption in Joules of the water pump used with evaporative cooling of the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller Compressor Rack Evaporative Condenser Basin Heater Electric Power [W]
-
-This is the electrical power requirement in Watts for the timestep being reported for the water heater in the basin of the evaporative system used to cool the compressor rack condenser.
-
-#### Refrigeration Air Chiller Compressor Rack Evaporative Condenser Basin Heater Electric Energy [J]
-
-This is the electricity consumption in Joules of the water heater used to prevent freezing of the evaporative cooling system for the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller Compressor Rack Evaporative Condenser Water Volume Flow Rate [m<sup>3</sup>/s]
-
-The volumetric flow rate in m<sup>3</sup>/s of water consumed while providing evaporative cooling of the compressor rack condenser.
-
-#### Refrigeration Air Chiller Compressor Rack Evaporative Condenser Water Volume [m<sup>3</sup>]
-
-This is the water consumed by evaporation in m<sup>3</sup> while providing evaporative cooling of the compressor rack condenser for the timestep being reported. This output is also added to a meter with Resource Type = Water, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller Compressor Rack Zone Sensible Heating Rate [W]
-
-This field is the rate of sensible heating in Watts provided to the zone by condenser waste heat rejection, which impacts the zone air heat balance.
-
-#### Refrigeration Air Chiller Compressor Rack Zone Sensible Heating Energy [J]
-
-This field is the sensible heating energy in Joules provided to the zone by condenser waste heat rejection for the timestep being reported.
-
-#### Refrigeration Air Chiller Compressor Rack Return Air Sensible Heating Energy [J]
-
-#### Refrigeration Air Chiller Compressor Rack Return Air Sensible Heating Rate [W]
-
-These are the sensible heating energy, in Joules or Watts, provided to the HVAC system return air node by condenser heat rejection at the compressor rack.
-
-### Refrigeration:Case
-
-The Refrigeration Case object works in conjunction with a compressor rack, a refrigeration system, or a secondary loop object (Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem) to simulate the performance of a refrigerated case system. The refrigerated case model uses performance information at rated conditions along with performance curves for latent case credits and defrost heat load to determine performance at off-rated conditions. Energy use for lights, fans and anti-sweat heaters is modeled based on inputs for nominal power, schedules, and control type. The refrigerated case model accounts for the sensible and latent heat exchange with the surrounding environment (termed "case credits") which impacts the temperature and humidity in the zone where the case is located.
-
-***A dataset has been provided containing refrigerated case input data for a large number of refrigerated cases from multiple manufacturers. See RefrigerationCases.idf.***
-
-The Refrigeration Case object inputs include a case name, an availability schedule name, the zone name for the location of the case, and the temperature and relative humidity of the ambient (zone) air surrounding the refrigerated case at the rating conditions for case performance. Additional inputs include the total cooling capacity, latent heat ratio, and run time fraction of the refrigerated case at rated conditions. The case length and operating temperature (average temperature of air/products within the case) must also be specified.
-
-The refrigerated case model requires two curves to describe performance at off-rated conditions (i.e., at different zone temperature and humidity levels): the latent case credit curve and the defrost energy correction curve. The user must enter cubic performance curves with the independent variable being user selectable (case temperature, zone relative humidity, or zone dewpoint temperature).
-
-The user can select from eight case defrost types, with additional inputs being required depending on the type selected. The user must enter a defrost schedule (unless Case Defrost Type = None), and an optional defrost drip-down schedule can be specified to allow additional time for melted frost to drain from the cooling coil following the regular defrost period.
-
-Inputs are required for case fans, lights, and anti-sweat heaters. Case lighting can be controlled by the user through entering a schedule. The case fans operate whenever the cooling coil is operating and during defrost periods for certain case defrost types. Anti-sweat heater power can be controlled by several methods which are user selectable. The model assumes that the fans are contained within the thermal envelope of the case and provide a direct heat load on the case cooling coil. For lighting and anti-sweat heaters, the user can specify the fraction of their respective heat loads that directly impact the case cooling coil (with the remainder of their heat load impacting the surrounding zone air).
-
-The user has the option of specifying a case restocking schedule and a schedule for modifying the case credits if needed. Finally, the user can specify the under case HVAC return air fraction which determines the portion of the case credits that directly impact the HVAC return air conditions (with the remainder of the case credits impacting the zone sensible and latent loads).
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a refrigerated case. Any reference to this case by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the refrigerated case can operate during a given time period. A schedule value greater than 0 (maximum schedule value of 1.0 is typically used) indicates that the case will operate during a given time period. A value equal to 0 denotes that the case does not operate (everything is OFF: refrigeration, fans, lights, anti-sweat, etc.). Typically the refrigerated case will operate throughout the day (i.e., the schedule will contain 1 for all time periods); however, cases require maintenance and/or cleaning and this can be modeled accordingly using this schedule if desired. If this field is left blank, the case is assumed to be available at all time periods.
-
-#### Field: Zone Name
-
-The name of the zone where the refrigerated case is located. The refrigerated case will impact the air heat balance in this zone. When modeling multiple refrigerated cases connected to a single compressor rack where the condenser heat is rejected to the zone (ref: Refrigeration:CompressorRack), **all** of the refrigerated cases connected to that compressor rack must be located in the same zone.
-
-#### Field: Rated Ambient Temperature
-
-Dry-bulb temperature of the ambient (zone) air surrounding the refrigerated case at the rating conditions for refrigerated case performance. The default value for this field is 23.9ËšC (75ËšF). This temperature must be greater than 0ËšC and greater than the case operating temperature.
-
-#### Field: Rated Ambient Relative Humidity
-
-Relative humidity of the ambient (zone) air surrounding the refrigerated case at the rating conditions for refrigerated case performance. The default value for this field is 55% RH.
-
-#### Field: Rated Total Cooling Capacity per Unit Length
-
-The total, full load cooling capacity (sensible plus latent) in watts per unit length of refrigerated case (W/m) at rated conditions (i.e., at the Rated Ambient Temperature, Rated Ambient Relative Humidity, Case Operating Temperature, and with the Standard Case Fan Power per Unit Length and the Standard Case Lighting Power per Unit Length). The value entered for this field must be greater than zero, with a default value of 1900 W/m if the field is blank.
-
-#### Field: Rated Latent Heat Ratio
-
-The latent heat ratio (LHR=latent capacity divided by total cooling capacity) of the refrigerated case at rated conditions (i.e., at the Rated Ambient Temperature, Rated Ambient Relative Humidity, Case Operating Temperature, and with the Standard Case Fan Power per Unit Length and the Standard Case Lighting Power per Unit Length). The value for this field can range from zero to 1.0, with a default value of 0.3 if the field is blank.
-
-#### Field: Rated Runtime Fraction
-
-The runtime fraction of the refrigerated case at rated conditions (i.e., at the Rated Ambient Temperature, Rated Ambient Relative Humidity, and Case Operating Temperature). Even at rated conditions, refrigerated cases typically include additional cooling capacity to account for product stocking and recovery from defrost. The rated runtime fraction for refrigerated cases typically ranges from 0.8 to 0.9. The entered value for this field must be greater than 0.0 and less than or equal to 1.0, and the default value is 0.85 if the field is blank.
-
-#### Field: Case Length
-
-The length of the refrigerated case in meters. The entered value for this field must be greater than 0.0, and the default value is 3 meters if the field is blank.
-
-#### Field: Case Operating Temperature
-
-The average temperature of the air and products within the refrigerated case in ˚C. The refrigerated case manufacturer typically provides this information in the product literature. Typical operating temperatures for medium temperature cases are 1.6˚C to 7.2˚C (35˚F to 45˚F). Typical operating temperatures for low temperatures cases are -28.9˚C to -17.8˚C        (-20˚F to 0˚F). The entered value for this field must be less than 20˚C and lower than the Rated Ambient Temperature. The default value is 1.1˚C if the field is blank.
-
-#### Field: Latent Case Credit Curve Type
-
-This alpha field defines the form of the curve used to modify the latent case credits (latent heat removed from the zone where the refrigerated case is located) at off-rated conditions. The valid choices for this field are:
-
-- CaseTemperatureMethod
-
-This method defines the variation in latent case credits as a cubic function of Case Operating Temperature. The result from the cubic curve is multiplied by the difference between the rated ambient relative humidity and the actual zone relative humidity, and one minus this value is multiplied by the Rated LHR to give the operating LHR at the actual zone humidity condition. (Representative cooefficient values for single-shelf horizontal and multi-shelf vertical display cases are given in the EnergyPlus Engineering Reference.)
-
-- RelativeHumidityMethod
-
-This method defines the variation in latent case credits as a cubic function of ambient (zone) air relative humidity.
-
-- DewpointMethod
-
-This method defines the variation in latent case credits as a cubic function of ambient (zone) air dewpoint temperature.
-
-The default curve type is the Case Temperature Method. Refer to the Engineering Reference for further information on how latent case credits are modeled.
-
-#### Field: Latent Case Credit Curve Name
-
-The name of a **cubic** performance curve (ref: Performance Curves) that parameterizes the variation of the latent case credits at off-rated conditions. The curve should be normalized to have a value of 1.0 at the rated ambient air conditions defined above.
-
-#### Field: Standard Case Fan Power per Unit Length
-
-The total standard fan power in Watts per unit length of refrigerated case (W/m). This value represents the fan power included in the field Rated Total Cooling Capacity per Unit Length, and is used to determine the sensible case credits. The entered value for this field must be greater than or equal to zero, and the default value is 75.0 W/m if the field is blank.
-
-#### Field: Operating Case Fan Power per Unit Length
-
-The total operating fan power in Watts per unit length of refrigerated case (W/m). Enter the actual power for the installed fans. The entered value for this field must be greater than or equal to zero, and the value is set equal to the standard case fan powers if the field is blank.
-
-#### Field: Standard Case Lighting Power per Unit Length
-
-The total standard lighting power in Watts per unit length of refrigerated case (W/m). This value should represent the lighting power provided by the case manufacturer and included in the “Rated Total Cooling Capacity per Unit Length� field and is used to determine the sensible case credits. For cases where the manufacturer does not include the lights in the Rated Total Cooling Capacity, this value should be zero (0.0). The entered value for this field must be greater than or equal to zero, and the default value is 90.0 W/m if the field is blank.
-
-#### Field: Installed Case Lighting Power per Unit Length
-
-The total installed lighting power in Watts per unit length of refrigerated case (W/m). Enter the actual power for the installed lights. This number may be greater or less than the standard lighting power value, depending upon the manufacturer’s practice in specifying the case rated cooling capacity and whether or not energy-efficient lights are being modeled.  The next field (i.e. Case Lighting Schedule Name) may be used to specify the name of a schedule that contains the fraction of the Installed Case Lighting Power per Unit Length to be modeled for each timestep of the simulation period. The entered value for this field must be greater than or equal to zero, and the value is set equal to the standard case lighting power if the field is blank.
-
-#### Field: Case Lighting Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes the fraction of installed refrigerated case lights that operate during a given time period. A schedule value greater than 0 indicates that the lights will operate during that time period (maximum schedule value of 1.0 means lights are fully on at the Installed Case Lighting Power per Unit Length level). A schedule value of zero denotes that the lights are off. The refrigerated case lights will typically operate only when the store is open for business and can be scheduled off as desired via this schedule. If this field is left blank, the default schedule has a value of 1 for all time periods.
-
-#### Field: Fraction of Lighting Energy To Case
-
-The fraction of the lighting energy that directly contributes to the case heat load. The remainder of the lighting energy (1 – fraction) is a heating load to the zone where the case is located. This field can be used to model lighting ballasts and bulbs located outside the air curtain of the refrigerated case. The value for this field can range from zero to 1.0, with a default value of 1.0 if the field is blank.
-
-#### Field: Case Anti-Sweat Heater Power per Unit Length
-
-The electric anti-sweat heater power in watts per unit length of refrigerated case (W/m). The entered value for this field must be greater than or equal to zero, and the default value is 0 W/m if the field is blank.
-
-#### Field: Minimum Anti-Sweat Heater Power per Unit Length
-
-The minimum electric anti-sweat heater power in watts per unit length of refrigerated case (W/m). Anti-sweat heater power will remain at or above this value for anti-sweat heater control types linear, dewpoint method, or heat balance method. Other anti-sweat heater control types disregard this field. The entered value for this field must be greater than or equal to zero, and the default value is 0 W/m if the field is blank.
-
-#### Field: Anti-Sweat Heater Control Type
-
-The type of anti-sweat heater control used for this refrigerated case. Valid choices are None, Constant, Linear, DewpointMethod, or HeatBalanceMethod. The default is None if the field is blank. Refer to the Engineering Reference for further information on how the different anti-sweat heater controls are modeled.
-
-#### Field: Humidity at Zero Anti-Sweat Heater Energy
-
-The value of this numeric field is only used when the Linear anti-sweat heater control type is selected. Enter the zone relative humidity where anti-sweat heater energy use is zero. Negative values for relative humidity may be entered. Other anti-sweat heater control types disregard this field. The value entered for this field must be less than the Rated Ambient Relative Humidity specified above. The default for this field is -10.0.
-
-#### Field: Case Height
-
-The value of this numeric field is used when Heat Balance Method anti-sweat heater control is selected. Enter the case height in meters. Other anti-sweat heater control types disregard this field. The entered value for this field must be greater than zero when Heat Balance Method anti-sweat heater control is selected, and the default value is 1.5 meters if the field is blank.
-
-#### Field: Fraction of Anti-Sweat Heater Energy To Case
-
-This value denotes the fraction of anti-sweat heater energy that results in a direct heat load to the refrigerated case. The remainder of the anti-sweat heater energy (1-fraction) is a heating load to the zone where the refrigerated case is located. The value for this field can range from zero to 1.0, with a default value of 1.0 if the field is blank.
-
-#### Field: Case Defrost Power per Unit Length
-
-The defrost power in watts per unit length of refrigerated case (W/m). This input is required for hot-gas, hot-fluid, or electric defrost types and is used to evaluate the load on the case as well as power or heat consumption. Refrigerated case manufacturers do not typically provide information on the heat input for hot-gas and hot-fluid defrost. Information provided for electric defrost power can be substituted here for refrigerated cases using hot-gas or hot-fluid defrost if other information is not available. Only electric Case Defrost Types consume electricity during the defrost period. The entered value for this field must be greater than or equal to zero, and the default value is 0 W/m if the field is blank.
-
-#### Field: Case Defrost Type
-
-The type of defrost used for this refrigerated case. Valid choices are None, OffCycle, HotGas, HotGaswithTemperatureTermination, Electric, ElectricwithTemperatureTermination, HotFluid, and HotFluidwithTemperatureTermination. The default defrost type is OffCycle if the field is blank. Refer to the Engineering Reference for further information on how the different case defrost types are modeled. In particular, hot-fluid defrost systems may be effective with much shorter defrost times than other systems, which should be reflected in the defrost and drip-down schedules.
-
-#### Field: Case Defrost Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the refrigerated case requires defrosting. A schedule value of 1.0 indicates that defrost will be on during a given time period. A value equal to 0 denotes that the defrost is off. Defrost schedules normally repeat the duration and number of defrost cycles for each day of the year. The refrigerated case manufacturer typically provides this information with the product literature. The use of Compact Schedules (ref. Schedules) are ideal for this purpose. In a typical supermarket with many cases, it is important to diversify the defrost schedules in order to avoid large swings in the load placed upon the remainder of the refrigeration system.
-
-#### Field: Case Defrost Drip-Down Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the refrigerated case requires additional time for draining condensate after the defrost period. A schedule value of 1.0 indicates that the defrost drip-down period is on during a given time period. A value equal to 0 denotes that the defrost drip-down period is over. The refrigerated case manufacturer typically provides this information with the product literature.
-
-Each defrost drip-down period specified in this schedule should start at the same time as the corresponding defrost period specified in the schedule for Case Defrost Schedule, and the drip-down schedule defrost period should always be longer than or equal to the length of the defrost schedule time period. For example, if the case defrost schedule contains a defrost period from 7:00 to 7:15, you would specify a case defrost drip-down period from 7:00 to 7:20 if you wanted to model a 5 minute condensate drip-down period after the regular defrost period. If no drip-down schedule is entered, then the case defrost schedule (specified for the previous input field) will be used. The use of Compact Schedules (ref. Schedules) are ideal for this purpose.
-
-#### Field: Defrost Energy Correction Curve Type
-
-This alpha field defines the form of the correction curve used to modify the defrost energy use (and the associated load on the case cooling coil) at off-rated conditions. The valid choices for this field are:
-
-- None
-
-This choice specifies that a defrost energy correction curve will not be used.
-
-- CaseTemperatureMethod
-
-This method defines the variation in defrost energy as a cubic function of Case Operating Temperature. The result from the cubic curve is multiplied by the difference between the rated ambient relative humidity and the actual zone relative humidity, and one minus this value is multiplied by the Case Defrost Power to give the (average) operating defrost power at the actual zone humidity condition. (Representative cooefficient values for single-shelf horizontal and multi-shelf vertical display cases are given in the EnergyPlus Engineering Reference.)
-
-- RelativeHumidityMethod
-
-This method defines the variation in defrost energy as a cubic function of ambient (zone) air relative humidity.
-
-- DewpointMethod
-
-This method defines the variation in defrost energy as a cubic function of ambient (zone) air dewpoint temperature.
-
-The default curve type is None. The methods described here (e.g. Case Temperature, Relative Humidity, and Dewpoint) are applicable only to Electric with Temperature Termination, Hot-Gas with Temperature Termination, and Hot-Brine with Temperature Termination case defrost types. Refer to the Engineering Reference for further information on how the defrost energy correction types are modeled.
-
-#### Field: Defrost Energy Correction Curve Name
-
-The name of a **cubic** performance curve (ref: Performance Curves) that parameterizes the variation of the defrost energy (and the associated load on the case cooling coil) at off-rated conditions. The curve should be normalized to have the value of 1.0 at the rated ambient air conditions defined above. The defrost energy correction curve name is used only for the Electric with Temperature Termination, Hot-Gas with Temperature Termination, and Hot-Brine with Temperature Termination case defrost types.
-
-#### Field: Under Case HVAC Return Air Fraction
-
-This field denotes the fraction of HVAC system (air loop) return air that passes beneath the refrigerated case, if any. At times it is necessary to design HVAC systems with under case returns to avoid overcooling the area around the refrigerated case, thus providing a more comfortable environment for the zone occupants. This return air fraction affects the portion of the case credits (sensible and latent) that are applied to the air returning to the HVAC system, while the remainder of the case credits directly impacts the zone air heat balance. Refer to the Engineering Reference for further information on how this is modeled. The sum of the Under Case HVAC Return Air Fractions for all refrigerated cases located in a single zone must be less than or equal to 1.0. The value for this field can range from zero to 1.0, with a default value of 0 if the field is blank.
-
-#### Field: Refrigerated Case Restocking Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the refrigerated case is being restocked with product. The schedule should contain values in units of Watts per unit length of refrigerated case (W/m). This field can be used to denote the additional load imposed on the refrigerated case from stocking the case with product that is warmer than the refrigerated case temperature. This information is difficult to find and may require additional research for proper modeling; however, this schedule is available for this purpose if desired. If restocking of the refrigerated case will not be simulated, enter a schedule with values of zero for all time periods or leave this field blank.
-
-#### Field: Case Credit Fraction Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes a fraction of both the sensible and latent case credits to be applied to the zone and/or the HVAC system return air. Schedule values must be from 0 to 1. This allows correction of the case credits for various refrigerated case types. For instance, if glass door refrigerated display cases are installed in a store that is operated 12 hours per day, then the doors will remain closed during the unoccupied times and would therefore reduce the sensible and latent case credits during the unoccupied time. Leaving this field blank will result in no case credit fraction being applied during the simulation.
-
-#### Field: Design Evaporator Temperature or Brine Inlet Temperature
-
-The value of this numeric field is used only with the detailed refrigeration system and is not read for the compressor-rack system. For the refrigeration system, it is used to evaluate compressor performance and is also used when the evaporator pressure and temperature are allowed to float at loads less than the design load. If the case is cooled by a secondary system (ref: Refrigeration:SecondarySystem), this value is the brine inlet temperature. The minimum value is -70C and the maximum value is 40C.  The default value is 5C less than the case temperature.
-
-#### Field: Average Refrigerant Charge Inventory
-
-The value of this optional field is the refrigerant inventory present in the refrigerated case during ordinary operation. The value is used to produce an estimate of the total refrigerant present in the refrigeration system. The value is entered in kg/m.
-
-
-
-The following is an example input for a refrigerated case.
-
-```idf
- Refrigeration:Case,
-  Multi-Deck Dairy/Deli Merchandiser with Synergy-E,  !- Name [Based on Hill Phoenix 6DMLH-NRG]
-  ,   !- Availability Schedule [Used to turn case on/off including all power draws (ie fans, lights, etc)]
-  UserProvideZoneName,    !- Zone Name [Location of Fixture]
-  23.89,                  !- Rated Ambient Temperature {C}  [75øF]
-  55,                     !- Rated Ambient Relative Humidity {percent}
-  1394,         !- Rated Total Cooling Capacity per Unit length {W/m}  [1,450 Btu/hr/ft = 11,600 Btu/hr]
-  0.30,                   !- Rated Latent Heat Ratio  [ Rated Latent Capacity]
-  0.85,                   !- Rated Runtime Fraction
-  2.4,                    !- Case Length {m}  [8 ft]
-  3.33,                   !- Case Operating Temperature {C}  [38øF]
-  CaseTemperatureMethod,  !- Latent Case Credit Curve Type
-  Multi_Shelf_Vertical_Latent_Case_Credit_Curve,            !- Latent Case Credit Curve Name
-  27.3,                   !- Standard Case Fan Power per Unit Length {W/m}  [8.3 W/ft]
-  27.3,                   !- Operating Case Fan Power per Unit Length {W/m}  [8.3 W/ft = 67 W]
-  0.0,                    !- Standard Case Lighting Power per Unit Length {W/m}  [0.0 W/ft]
-  114.8,                  !- Installed Case Lighting Power per Unit Length {W/m}  [35.0 W/ft = 280 W]
-  ,                       !- Case Lighting Schedule Name
-  1.0,                    !- Fraction Of Lighting Energy To Case
-  0.0,                    !- Case Anti-Sweat Heater Power per Unit Length {W/m}  [0.0 W/ft = 0 W]
-  ,                       !- Minimum Anti-Sweat Heater Power per Unit Length {W/m}  []
-  None,                   !- Anti-Sweat Heater Control Type
-  ,                       !- Humidity At Zero Anti-Sweat Heater Energy {%}
-  ,                       !- Case Height {m}  []
-  1.0,                    !- Fraction of Anti-Sweat Heater Energy To Case
-  0.0,                    !- Case Defrost Power per Unit Length {W/m}  [0.0 W/ft  0 W]
-  Off Cycle,              !- Case Defrost Type
-  UserProvideDefSched6PerDay45MinEa,                        !- Case Defrost Schedule Name
-  UserProvideDefSched4PerDay42MinEa,                        !- Case Defrost Drip-Down Schedule
-  CaseTemperatureMethod,  !- Defrost Energy Correction Curve Type
-  Multi Shelf Vertical,   !- Defrost Energy Correction Curve Name
-  0.00,                   !- Under Case HVAC Return Air Fraction
-  ,                       !- Refrigerated Case Restocking Schedule Name  [Not modeling any restocking]
-  ,                       !- Case Credit Fraction Schedule Name
-  -3.33,                  !- Design Evaporator Temperature or Brine Inlet Temperature {C}  [26øF]
-  ;                       !- Average Refrigerant Charge Inventory {kg/m}  [ = ]
-```
-
-
-
-### Refrigeration:Case Outputs
-
-* Zone,Average,Refrigeration Case Evaporator Total Cooling Rate [W]
-
-* Zone,Sum,Refrigeration Case Evaporator Total Cooling Energy [J]
-
-* Zone,Average,Refrigeration Case Evaporator Sensible Cooling Rate [W]
-
-* Zone,Sum,Refrigeration Case Evaporator Sensible Cooling Energy [J]
-
-* Zone,Average, Refrigeration Case Evaporator Latent Cooling Rate [W]
-
-* Zone,Sum, Refrigeration Case Evaporator Latent Cooling Energy [J]
-
-* Zone,Average,Refrigeration Case Zone Sensible Cooling Rate [W]
-
-* Zone,Sum,Refrigeration Case Zone Sensible Cooling Energy [J]
-
-* Zone,Average,Refrigeration Case Zone Sensible Heating Rate [W]
-
-* Zone,Sum,Refrigeration Case Zone Sensible Heating Energy [J]
-
-* Zone,Average,Refrigeration Case Zone Latent Rate [W]
-
-* Zone,Sum,Refrigeration Case Zone Latent Energy [J]
-
-* Zone,Average,Refrigeration Case Return Air Sensible Cooling Rate [W]
-
-* Zone,Sum,Refrigeration Case Return Air Sensible Cooling Energy [J]
-
-* Zone,Average,Refrigeration Case Return Air Sensible Heating Rate [W]
-
-* Zone,Sum,Refrigeration Case Return Air Sensible Heating Energy [J]
-
-* Zone,Average,Refrigeration Case Return Air Latent Rate [W]
-
-* Zone,Sum,Refrigeration Case Return Air Latent Energy [J]
-
-* Zone,Average,Refrigeration Case Evaporator Fan Electric Power [W]
-
-* Zone,Sum,Refrigeration Case Evaporator Fan Electric Energy [J]
-
-* Zone,Average,Refrigeration Case Lighting Electric Power [W]
-
-* Zone,Sum,Refrigeration Case Lighting Electric Energy [J]
-
-* Zone,Average,Refrigeration Case Latent Credit Curve Value []
-
-If case defrost type is Electric, Hot-Gas, or Hot-Brine with Temperature Termination
-
-* Zone,Average,Refrigeration Case Defrost Energy Correction Curve Value
-
-If anti-sweat heater control type is not equal to None:
-
-* Zone,Average,Refrigeration Case Anti Sweat Electric Power [W]
-
-* Zone,Sum,Refrigeration Case Anti Sweat Electric Energy [J]
-
-If case defrost type is Electric or Electric with Temperature Termination:
-
-* Zone,Average,Refrigeration Case Defrost Electric Power [W]
-
-* Zone,Sum,Refrigeration Case Defrost Electric Energy [J]
-
-#### Refrigeration Case Evaporator Total Cooling Rate [W]
-
-This field is the total (sensible plus latent) cooling rate of the refrigerated case evaporator coil in Watts.
-
-#### Refrigeration Case Evaporator Total Cooling Energy [J]
-
-This field is the total (sensible plus latent) cooling of the refrigerated case evaporator coil in Joules over the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
-
-#### Refrigeration Case Evaporator Sensible Cooling Rate [W]
-
-This field is the sensible cooling rate of the refrigerated case evaporator coil in Watts.
-
-#### Refrigeration Case Evaporator Sensible Cooling Energy [J]
-
-This field is the sensible cooling of the refrigerated case evaporator coil in Joules over the timestep being reported.
-
-#### Refrigeration Case Evaporator Latent Cooling Rate [W]
-
-This field is the latent cooling (dehumidification) rate of the refrigerated case evaporator coil in Watts.
-
-#### Refrigeration Case Evaporator Latent Cooling Energy [J]
-
-This field is the latent cooling (dehumidification) of the refrigerated case evaporator coil in Joules over the timestep being reported.
-
-#### Refrigeration Case Zone Sensible Cooling Rate [W]
-
-This field is the rate of sensible cooling case credits delivered to the zone in Watts. If an under case return duct is simulated, only a portion of the sensible case credits are applied to the zone. A positive value is reported when the zone is cooled by sensible case credits, otherwise a zero is reported.
-
-#### Refrigeration Case Zone Sensible Cooling Energy [J]
-
-This field is the amount of sensible cooling case credit energy delivered to the zone in Joules. If an under case return duct is simulated, only a portion of the sensible case credits are applied to the zone. A positive value is reported when the zone is cooled by sensible case credits, otherwise a zero is reported.
-
-#### Refrigeration Case Zone Sensible Heating Rate [W]
-
-This field is the rate of sensible heating case credits delivered to the zone in Watts. If an under case return duct is simulated, only a portion of the sensible case credits are applied to the zone. A positive value is reported when the zone is heated by sensible case credits, otherwise a zero is reported.
-
-#### Refrigeration Case Zone Sensible Heating Energy [J]
-
-This field is the amount of sensible heating case credit energy delivered to the zone in Joules. If an under case return duct is simulated, only a portion of the sensible case credits are applied to the zone. A positive value is reported when the zone is heated by sensible case credits, otherwise a zero is reported.
-
-#### Refrigeration Case Zone Latent Rate [W]
-
-This field is the rate of latent cooling (dehumidification) case credits delivered to the zone in Watts. If an under case return duct is simulated, only a portion of the latent case credits are applied to the zone. A negative value (or zero) will be reported when the refrigerated case provides dehumidification (thereby reducing the zone latent load).
-
-#### Refrigeration Case Zone Latent Energy [J]
-
-This field is the amount of latent cooling (dehumidification) case credit energy delivered to the zone in Joules. If an under case return duct is simulated, only a portion of the latent case credits are applied to the zone. A negative value (or zero) will be reported when the refrigerated case provides dehumidification (thereby reducing the zone latent load).
-
-#### Refrigeration Case Return Air Sensible Cooling Rate [W]
-
-This field is the rate of sensible cooling case credits delivered to the return air duct (zone return air node) in Watts. If an under case return duct is simulated, a portion of the sensible case credits are applied to the HVAC (zone) return air. A positive value is reported when the return air is cooled by sensible case credits, otherwise a zero is reported. If the HVAC system is off for a simulation timestep (no return air mass flow), then this sensible cooling is actually provided to the zone air instead (even though a non-zero value is reported here).
-
-#### Refrigeration Case Return Air Sensible Cooling Energy [J]
-
-This field is the amount of sensible cooling case credit energy delivered to the return air duct (zone return air node) in Joules. If an under case return duct is simulated, a portion of the sensible case credits are applied to the HVAC (zone) return air. A positive value is reported when the return air is cooled by sensible case credits, otherwise a zero is reported. If the HVAC system is off for a simulation timestep (no return air mass flow), then this sensible cooling is actually provided to the zone air instead (even though a non-zero value is reported here).
-
-#### Refrigeration Case Return Air Sensible Heating Rate [W]
-
-This field is the rate of sensible heating case credits delivered to the return air duct (zone return air node) in Watts. If an under case return duct is simulated, a portion of the sensible case credits are applied to the HVAC (zone) return air. A positive value is reported when the return air is heated by sensible case credits, otherwise a zero is reported. If the HVAC system is off for a simulation timestep (no return air mass flow), then this sensible heating is actually provided to the zone air instead (even though a non-zero value is reported here).
-
-#### Refrigeration Case Return Air Sensible Heating Energy [J]
-
-This field is the amount of sensible heating case credit energy delivered to the return air duct (thereby reducing the zone latent load). If the HVAC system is off for a simulation timestep (no return air mass flow), then this latent energy is actually provided to the zone air instead (even though a non-zero value is reported here).
-
-#### Refrigeration Case Return Air Latent Energy [J]
-
-#### Refrigeration Case Return Air Latent Rate [W]
-
-These are the amount of latent cooling (dehumidification) case credit energy delivered to the return air duct (zone return air node) in Joules or Watts. If an under case return duct is simulated, only a portion of the latent case credits are applied to the HVAC (zone) return air. A negative value (or zero) will be reported since the refrigerated case provides dehumidification (thereby reducing the zone latent load). If the HVAC system is off for a simulation timestep (no return air mass flow), then this latent energy is actually provided to the zone air instead (even though a non-zero value is reported here).
-
-#### Refrigeration Case Evaporator Fan Electric Power [W]
-
-This field is the electric power input to the refrigerated case fan(s) in Watts.
-
-#### Refrigeration Case Evaporator Fan Electric Energy [J]
-
-This field is the electricity consumption of the refrigerated case fan(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
-
-#### Refrigeration Case Lighting Electric Power [W]
-
-This field is the electric power input to the refrigerated case lights in Watts.
-
-#### Refrigeration Case Lighting Electric Energy [J]
-
-This field is the electricity consumption of the refrigerated case lights in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
-
-#### Refrigeration Case Defrost Energy Correction Curve Value
-
-This field is the output of the Defrost Energy Correction Curve which denotes the variation in defrost energy at off-rated conditions. The output of the defrost energy correction curve directly impacts the energy used during the defrost time period. It does not, however, impact the duration of the defrost period. This output is available only for Electric with Temperature Termination, Hot-Gas with Temperature Termination, or Hot-Brine with Temperature Termination case defrost types.
-
-#### Refrigeration Case Latent Credit Curve Value []
-
-This field is the output of the Latent Case Credit Curve which denotes the variation in latent case credits at off-rated conditions. The output of the latent case credit curve directly impacts the amount of frost formation on the refrigerated case evaporator coil and the requirement for defrost.
-
-#### Refrigeration Case Anti Sweat Electric Power [W]
-
-This field is the electric power input to the refrigerated case anti-sweat heater in Watts. This output is available unless anti-sweat heater control type is specified as NONE.
-
-#### Refrigeration Case Anti Sweat Electric Energy [J]
-
-This field is the total electricity consumption of the refrigerated case anti-sweat heater in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects). This output is available unless anti-sweat heater control type is specified as NONE.
-
-#### Refrigeration Case Defrost Electric Power [W]
-
-This field is the electric power input to the refrigerated case electric defrost heater(s) in Watts. This output is available if case defrost type is Electric or Electric with Temperature Termination.
-
-#### Refrigeration Case Defrost Electric Energy [J]
-
-This field is the total electricity consumption of the refrigerated case electric defrost heater(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects). This output is available if case defrost type is Electric or Electric with Temperature Termination.
-
-### Refrigeration:CaseAndWalkInList
-
-This object provides a list of all the refrigerated cases and/or walk in coolers cooled by a single refrigeration system (ref: Refrigeraion:CompressorRack and Refrigeration:System). This list is extensible. Note that the names of all cases, walk-ins,air chillers, and caseandwalkinlists must be unique.  That is, you cannot give a list the same name as one of the cases.  Similarly, a walkin cannot have the same name as a case.This list may contain a combination of case and walk-in names OR a list of air chiller names.  Air chillers may not be included in any list that also includes cases or walk-ins.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a CaseAndWalkInList. Any reference to this list by another object will use this name.
-
-#### Field: Case or WalkIn or Air Chiller &lt;x&gt; Name
-
-Identifies a particular refrigerated case or walk-in. The name will be validated against the  Refrigeration Case, Refrigeration WalkIn, and Air Chiller names (ref: Refrigeration:Case,  Refrigeration:WalkIn, and Refrigeration:AirChiller) in the input file. Up to 20 are provided in the IDD; this object is extensible.
-
-The following is an example input for a CaseAndWalkInList.
-
-```idf
-Refrigeration:CaseAndWalkInList,
-    MediumTempCaselist,      !- Name
-    UprightDairyCase,        !- Refrigeration Case or WalkIn Name \#1
-    LunchmeatCase,           !- Refrigeration Case or WalkIn Name \#2
-    MeatWalkIn,              !- Refrigeration Case or WalkIn Name \#3
-    DeliCaseOne;             !- Refrigeration Case or WalkIn Name \#4
-```
-
-
-
-### Refrigeration:WalkIn
-
-The Refrigeration WalkIn object works in conjunction with a compressor rack, a refrigeration system, or a refrigeration secondary system object (Ref. Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem) to simulate the performance of a walk-in cooler. The walk-in cooler model uses information at rated conditions along with input descriptions for heat transfer surfaces facing multiple zones to determine performance. Energy use for lights, fans, and floor and anti-sweat heaters is modeled based on inputs for nominal power, schedules, and control type. The walk-in cooler model accounts for the sensible and latent heat exchange with the surrounding environment (termed "case credits") which impacts the temperature and humidity in each zone adjacent to the walk-in.
-
-The walk-in cooler object inputs include a name, an availability schedule name, the rated cooling capacity, the rated operating temperature, the rated cooling source temperature, the rated total heating power and heating power schedule, the rated fan and lighting power and schedules, defrost type, defrost control type, defrost schedule name, drip-down schedule name, defrost power, the portion of the defrost energy used to melt ice (only for temperature termination control type), restocking schedule, refrigerant inventory, and the floor area and U-value.
-
-For each zone adjacent to the walk-in, the user must input the zone name and the insulated surface area and U-value facing that zone. The user must also specify, for two types of doors, the door area, height, U-value, door opening schedule name, and any door opening protection.
-
-Under case HVAC return air fraction, available for refrigerated cases, is not available for walk-in coolers.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a refrigerated walk-in. Any reference to this walk-in by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the walk in can operate during a given time period. A schedule value greater than 0 (maximum schedule value of 1.0 is typically used) indicates that the walkin will operate during a given time period. A value equal to 0 denotes that the case does not operate (everything is OFF: refrigeration, fans, lights, anti-sweat, etc.). Typically the walkin will operate throughout the day (i.e., the schedule will contain 1 for all time periods); however, walkins require maintenance and/or cleaning and this can be modeled accordingly using this schedule if desired. If this field is left blank, the default schedule has a value of 1 for all time periods.
-
-#### Field: Rated Coil Cooling Capacity
-
-The total, full load cooling capacity (sensible plus latent) in watts (W) at rated conditions The value entered for this field must be greater than zero, with no default value.
-
-#### Field: Operating Temperature
-
-The rated average temperature of the air and products within the walk-in cooler in ËšC. The entered value for this field must be less than 20ËšC. There is no default value.
-
-#### Field: Rated Cooling Source Temperature
-
-For a DX evaporator coil, enter the saturated evaporating temperature in ˚C.  For a fluid coil, enter the fluid coil entrance temperature in ˚C. There is no default value. This number is used, with temperatures for other refrigeration loads on any one system, to set that system’s minimum suction pressure or minimum circulating fluid temperature. (This value is not used if the walkin is cooled by a compressor rack object.)
-
-#### Field: Rated Total Heating Power
-
-The total heating power in watts including all anti-sweat, door, drip-pan, and floor heaters (W). This value is required and has no default value.
-
-#### Field: Heating Power Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes the fraction of heater power that operates during a given time period. A schedule value of zero denotes that all heaters are off. A schedule value greater than 0 indicates that some portion of the total heater power will operate during that time period (maximum schedule value of 1.0 means all heaters are fully on). For example, if door and floor heaters represent 50% of the total heater power and are on all the time, the minimum schedule value would be 0.5. If anti-sweat heaters represent 40% of the total heater power and are only on during certain hours, the schedule value during those hours would be increased by 0.4. If this field is left blank, the default schedule has a value of 1 for all time periods.
-
-#### Field: Rated Cooling Coil Fan Power
-
-The cooling coil fan power in watts (W). This value has a default value of 375W. This fan is assumed to run continuously except during electric, hot brine, or hot gas defrost periods.
-
-#### Field: Rated Circulation Fan Power
-
-The circulation fan power in watts (W). This value has a default value of 0 W. This fan is assumed to run continuously.
-
-#### Field: Rated Total Lighting Power
-
-The total lighting power in watts including both display and task lighting (W). This value is required and has no default value.
-
-#### Field: Lighting Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes the fraction of walk-in lights that operate during a given time period. A schedule value greater than 0 indicates that the lights will operate during that time period (maximum schedule value of 1.0 means lights are fully on). A schedule value of zero denotes that the lights are off. If this field is left blank, the default schedule has a value of 1 for all time periods.
-
-#### Field: Defrost Type
-
-The type of defrost used for this walk-in. Valid choices are None, Off-Cycle, HotFluid, and Electric. The default defrost type is Electric if the field is blank. HotFluid includes both hot gas and hot brine defrost systems. Refer to the Engineering Reference for further information on how the different defrost types are modeled.
-
-#### Field: Defrost Control Type
-
-The type of defrost control used for this walkin. Valid choices are TimeSchedule and TemperatureTermination. The default is TimeSchedule if the field is blank. Refer to the Engineering Reference for further information on how the different defrost controls are modeled.
-
-#### Field: Defrost Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes when the walkin requires defrosting. A schedule value of 1.0 indicates that defrost will be on during a given time period if the defrost control type is “TimeSchedule�. For the TemperatureTermination defrost control type, the defrost will start with the schedule value changes from 0 to 1, but will end when the ice is melted. A value equal to 0 denotes that the defrost is off. Defrost schedules normally repeat the duration and number of defrost cycles for each day of the year. The walkin manufacturer typically provides this information with the product literature. If TemperatureTermination control type is used, the defrost schedule is used for the defrost cycle start time and the defrost cycle end time is not allowed to extend beyond the scheduled off time. The use of Compact Schedules (ref. Schedules) are ideal for this purpose.
-
-#### Field: Defrost Drip-Down Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the walkin requires additional time for draining condensate after the defrost period. A schedule value of 1.0 indicates that the defrost drip-down period is on during a given time period. A value equal to 0 denotes that the defrost drip-down period is over. The walkin manufacturer typically provides this information with the product literature.
-
-Each defrost drip-down period specified in this schedule should start at the same time as the corresponding defrost period specified in the schedule for Defrost Schedule, and the drip-down schedule defrost period should always be longer than or equal to the length of the defrost schedule time period. For example, if the defrost schedule contains a defrost period from 7:00 to 7:15, you would specify a case defrost drip-down period from 7:00 to 7:20 if you wanted to model a 5 minute condensate drip-down period after the regular defrost period. If no drip-down schedule is entered, then the defrost schedule (specified for the previous input field) will be used. The use of Compact Schedules (ref. Schedules) are ideal for this purpose.
-
-#### Field: Defrost Power
-
-The defrost power in watts. This input is required for hot-fluid (hot gas or hot brine), or electric defrost types. Walkin manufacturers do not typically provide information on the heat input for hot gas and hot brine defrost. Information provided for electric defrost power can be substituted here for walkins using hot-gas or hot-brine defrost if other information is not available. Only electric Defrost Types consume electricity during the defrost period. The entered value for this field must be greater than or equal to zero.
-
-#### Field: Temperature Termination Defrost Fraction to Ice
-
-When cooling coils go through a defrost cycle, only a portion of the defrost energy is actually used to melt the ice.  The rest of the defrost energy goes to increasing the temperature of the coils themselves and to the walkin environment. The Temperature Termination defrost control type calculates the end of the defrost cycle that corresponds to melting all the ice. Therefore, the user must input this fractional value. The default value is 0.7 for electric defrost and 0.3 for hot fluid defrost. Refer to the Engineering Reference for further information on how the defrost energy control types are modeled.
-
-#### Field: Restocking Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the walkin is being restocked with product. The schedule should contain values in units of Watts (note this is different from the restocking schedule values for cases that are entered per unit length). This field can be used to denote the additional load imposed on the walkin from stocking the walkin with product that is warmer than the walkin temperature. This information is difficult to find and may required additional research for proper modeling; however, this schedule is available for this purpose if desired. If restocking of the refrigerated walkin will not be simulated, enter a schedule with values of zero for all time periods or leave this field blank.
-
-#### Field: Average Refrigerant Charge Inventory
-
-The value of this optional field is the refrigerant inventory present in the walkin during ordinary operation. The value is used to produce an estimate of the total refrigerant present in the refrigeration system. The value is entered in kg.
-
-#### Field: Insulated Floor Surface Area
-
-The floor area in square meters. This value is required and has no default value.
-
-#### Field: Insulated Floor U-Value
-
-The floor themal transmittance (in W/m<sup>2</sup>-K). This value has a default value of 0.3154. (This corresponds to R18 in Archaic American Insulation Units.  To convert other R-values to thermal transmittance, divide 5.678 by the R-value.  For example, R15 is 0.3785 W/m<sup>2</sup>-K and R5 is 1.136 W/m<sup>2</sup>-K.)
-
-***THE REMAINING 12 FIELDS FOR THE WALK-IN COOLER MUST BE REPEATED FOR EACH ZONE WHICH IS IN CONTACT WITH A WALK-IN WALL, CEILING, OR DOOR. The IDD includes fields for 3 zones, but can be extended by repeating the last 12 values in the object.***
-
-#### Field: Zone &lt;x&gt; Name
-
-The name of a zone adjoining the walkin. The walkin will impact the air heat balance in this zone. This zone must represent a conditioned space, that is, it must appear in a ZoneHVAC:EquipmentConnections object.
-
-#### Field: Total Insulated Surface Area Facing  Zone &lt;x&gt;
-
-The total surface area (walls and ceilings) facing this particular zone in square meters. This value is required and has no default value.
-
-#### Field: Insulated Surface U-Value Facing Zone &lt;x&gt;
-
-The surface (walls and ceilings) themal transmittance (in W/m<sup>2</sup>-K). This value has a default value of 0.3154. (This corresponds to R18 in Archaic American Insulation Units.  To convert other R-values to thermal transmittance, divide 5.678 by the R-value.  For example, R15 is 0.3785 W/m<sup>2</sup>-K and R5 is 1.136 W/m<sup>2</sup>-K.)
-
-#### Field: Area of Glass Reach In Doors Facing Zone &lt;x&gt;
-
-The total area of glass doors facing this particular zone in square meters. The default is 0.0.
-
-#### Field: Height of Glass Reach In Doors Facing Zone &lt;x&gt;
-
-The glass reach in door height in meters. The default is 1.5.
-
-#### Field: Glass Reach In Door U-Value Facing Zone &lt;x&gt;
-
-The glass door themal transmittance (in W/m<sup>2</sup>-K). This field has a default value of 1.136. (This corresponds to R5 in Archaic American Insulation Units.)
-
-#### Field: Glass Reach In Door Opening Schedule Name Facing Zone &lt;x&gt;
-
-The name of the schedule (ref: Schedule) that denotes the fraction of time glass doors are open during a given time period. The schedule values should be between 0 and 1.0. If no schedule is specified, the doors are assumed to be open 5% of the time (corresponding to a schedule value of 0.05).
-
-#### Field: Area of Stocking Doors Facing Zone &lt;x&gt;
-
-The total area of stock doors facing this particular zone in square meters. The default is 0.0.
-
-#### Field: Height of Stocking Doors Facing Zone &lt;x&gt;
-
-The stocking door height in meters. The default is 2.0.
-
-#### Field: Stocking Door U-Value Facing Zone &lt;x&gt;
-
-The stocking door themal transmittance (in W/m<sup>2</sup>-K). This value has a default value of 0.3785. (This corresponds to R15 in Archaic American Insulation Units.)
-
-#### Field: Stocking Door Opening Schedule Name Facing Zone &lt;x&gt;
-
-The name of the schedule (ref: Schedule) that denotes the fraction of time stocking doors are open during a given time period. The schedule values should be between 0 and 1.0. If no schedule is specified, the doors are assumed to be open 5% of the time (corresponding to a schedule value of 0.05).
-
-#### Field: Stocking Door Opening Protection Type Facing Zone &lt;x&gt;
-
-The type of stocking door opening protection used for this walkin. Valid choices are None, AirCurtain, and StripCurtain. The default is AirCurtain if the field is blank. Use the type, StripCurtain, for both hanging strips and airlock vestibules. Refer to the Engineering Reference for further information on how the door protection types are modeled.
-
-The following is an example input for a refrigeration walkin.
-
-```idf
-   Refrigeration:WalkIn,
-    WalkInFreezer,           !- Name
-    CaseOperatingSched,      !- Availability Schedule Name
-    4690.,                   !- Rated Coil Cooling Capacity {W}
-    -2.22,                   !- Operating Temperature {C}
-    -6.67,                   !- Rated Cooling Source Temperature {C}
-    0.0,                     !- Rated Total Heating Power {W}
-    CaseOperatingSched,      !- Heating Power Schedule Name
-    735.,                    !- Rated Cooling Coil Fan Power {W}
-    0.0,                     !- Rated Circulation Fan Power {W}
-    120.,                    !- Rated Total Lighting Power {W}
-    CaseLightingSched2,      !- Lighting Schedule Name
-    Electric,                !- Defrost Type
-    TimeSchedule,            !- Defrost Control Type
-    CaseDefrostSched3,       !- Defrost Schedule Name
-    CaseDripDownSched3,      !- Defrost Drip-Down Schedule Name
-    5512.,                   !- Defrost Power {W}
-    ,                        !- Temperature Termination Defrost Fraction to Ice {dimensionless}
-    WalkInStockingSched,     !- Restocking Schedule Name
-    ,                        !- Average Refrigerant Charge Inventory {kg}
-    13.0,                    !- Insulated Floor Surface Area {m2}
-    0.207,                   !- Insulated Floor U-Value {W/m2-C}
-    BackRoom,                !- Zone Name
-    43.4,                    !- Total Insulated Surface Area Facing this Zone {m2}
-    .235,                    !- Insulated Surface U-Value Facing this Zone {W/m2-C}
-    ,                        !- Area of Glass Reach In Doors Facing this Zone {m2}
-    ,                        !- Height of Glass Reach In Doors Facing this Zone {m}
-    ,                        !- Glass Reach In Door U Value Facing this Zone {W/m2-C}
-    ,                        !- Glass Reach In Door Opening Schedule Name Facing this Zone
-    2.0,                     !- Area of Stocking Doors Facing this Zone {m2}
-    2.0,                     !- Height of Stocking Doors Facing this Zone {m}
-    ,                        !- Stocking Door U Value Facing this Zone {W/m2-C}
-    WIStockDoorOpenSch,      !- Stocking Door Opening Schedule Name Facing this Zone
-    StripCurtain;            !- Stocking Door Opening Protection Type Facing this Zone
-```
-
-
-
-
-### Refrigeration Case and WalkIn Outputs
-
-* Zone,Average,Refrigeration Walk In Evaporator Total Cooling Rate [W]
-
-* Zone,Sum,Refrigeration Walk In Evaporator Total Cooling Energy [J]
-
-* Zone,Average,Refrigeration Walk In Evaporator Sensible Cooling Rate [W]
-
-* Zone,Sum,Refrigeration Walk In Evaporator Sensible Cooling Energy [J]
-
-* Zone,Average,Refrigeration Walk In Evaporator Latent Cooling Rate [W]
-
-* Zone,Sum,Refrigeration Walk In Evaporator Latent Cooling Energy [J]
-
-* Zone,Average,Refrigeration Walk In Ancillary Electric Power [W]
-
-* Zone,Sum,Refrigeration Walk In Ancillary Electric Energy [J]
-
-* Zone,Average,Refrigeration Walk In Fan Electric Power [W]
-
-* Zone,Sum,Refrigeration Walk In Fan Electric Energy [J]
-
-* Zone,Average,Refrigeration Walk In Lighting Electric Power [W]
-
-* Zone,Sum,Refrigeration Walk In Lighting Electric Energy [J]
-
-* Zone,Average,Refrigeration Walk In Heater Electric Power [W]
-
-* Zone,Sum,Refrigeration Walk In Heater Electric Energy [J]
-
-
-
-*Report only for WalkIns using electric defrost*
-
-* Zone,Average,Refrigeration Walk In Defrost Electric Power [W]
-
-* Zone,Sum,Refrigeration Walk In Defrost Electric Energy [J]
-
-
-
-***Report for each Zone exchanging energy with the WalkIn***
-
-* Zone,Average,Refrigeration Walk In Zone Sensible Cooling Rate [W]
-
-* Zone,Sum,Refrigeration Walk In Zone Sensible Cooling Energy [J]
-
-* Zone,Average, Zone,Average,Refrigeration Walk In Zone Sensible Heating Rate [W]
-
-* Zone,Sum,Refrigeration Walk In Zone Sensible Heating Energy [J]
-
-* Zone,Average,Zone,Average,Refrigeration Walk In Zone Latent Rate [W]
-
-* Zone,Sum,Refrigeration Walk In Zone Latent Energy [J]
-
-#### Refrigeration Walk In Evaporator Total Cooling Rate [W]
-
-This field is the total (sensible plus latent) cooling rate of the WalkIn evaporator coil in Watts.
-
-#### Refrigeration Walk In Evaporator Total Cooling Energy [J]
-
-This field is the total (sensible plus latent) cooling of the WalkIn evaporator coil in Joules over the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
-
-#### Refrigeration Walk In Evaporator Sensible Cooling Rate [W]
-
-This field is the sensible cooling rate of the WalkIn evaporator coil in Watts.
-
-#### Refrigeration Walk In Evaporator Sensible Cooling Energy [J]
-
-This field is the sensible cooling of the WalkIn evaporator coil in Joules over the timestep being reported.
-
-#### Refrigeration Walk In Evaporator Latent Cooling Rate [W]
-
-This field is the latent cooling (dehumidification) rate of the WalkIn evaporator coil in Watts.
-
-#### Refrigeration Walk In Evaporator Latent Cooling Energy [J]
-
-This field is the latent cooling (dehumidification) of the WalkIn evaporator coil in Joules over the timestep being reported.
-
-#### Refrigeration Walk In Ancillary Electric Power [W]
-
-This field is the total electricity (fan, heaters, lights, and electric defrost) used by the walkin in Watts.
-
-#### Refrigeration Walk In Ancillary Electric Energy [J]
-
-This field is the electricity (fan, heaters, lights, and electric defrost)used by the WalkIn in Joules over the timestep being reported.
-
-#### Refrigeration Walk In Fan Electric Power [W]
-
-This field is the electric power input to the WalkIn fan(s) in Watts.
-
-#### Refrigeration Walk In Fan Electric Energy [J]
-
-This field is the electricity consumption of the WalkIn fan(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
-
-#### Refrigeration Walk In Lighting Electric Power [W]
-
-This field is the electric power input to the WalkIn lights in Watts.
-
-#### Refrigeration Walk In Lighting Electric Energy [J]
-
-This field is the electricity consumption of the WalkIn lights in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
-
-#### Refrigeration Walk In Heater Electric Power [W]
-
-This field is the electric power input to the WalkIn heaters in Watts.
-
-#### Refrigeration Walk In Heater Electric Energy [J]
-
-This field is the total electricity consumption of the WalkIn heaters in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
-
-#### Refrigeration Walk In Defrost Electric Power [W]
-
-This field is the electric power input to the WalkIn electric defrost heater(s) in Watts. This output is available if case defrost type is Electric.
-
-#### Refrigeration Walk In Defrost Electric Energy [J]
-
-This field is the total electricity consumption of the WalkIn electric defrost heater(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects). This output is available if case defrost type is Electric.
-
-*The following output variables are available for each zone adjacent to the walkin. An output variable identification is created for each zone exchanging energy with the walkin.  For example if the walkin, “DairyWalkIn�, were exchanging energy with the zone, “SalesArea�, the output variable identification would be “DairyWalkInInZoneSalesArea�.*
-
-#### Refrigeration Walk In Zone Sensible Cooling Rate [W]
-
-This field is the rate of sensible cooling case credits delivered to the zone in Watts. A positive value is reported when the zone is cooled by sensible case credits, otherwise a zero is reported.
-
-#### Refrigeration Walk In Zone Sensible Cooling Energy [J]
-
-This field is the amount of sensible cooling case credit energy delivered to the zone in Joules. A positive value is reported when the zone is cooled by sensible case credits, otherwise a zero is reported.
-
-#### Refrigeration Walk In Zone Sensible Heating Rate [W]
-
-This field is the rate of sensible heating case credits delivered to the zone in Watts. A positive value is reported when the zone is heated by sensible case credits, otherwise a zero is reported.
-
-#### Refrigeration Walk In Zone Sensible Heating Energy [J]
-
-This field is the amount of sensible heating case credit energy delivered to the zone in Joules. A positive value is reported when the zone is heated by sensible case credits, otherwise a zero is reported.
-
-#### Refrigeration Walk In Zone Latent Rate [W]
-
-This field is the rate of latent cooling (dehumidification) case credits delivered to the zone in Watts. A negative value (or zero) will be reported when the WalkIn provides dehumidification (thereby reducing the zone latent load).
-
-#### Refrigeration Walk In Zone Latent Energy [J]
-
-This field is the amount of latent cooling (dehumidification) case credit energy delivered to the zone in Joules. A negative value (or zero) will be reported when the WalkIn provides dehumidification (thereby reducing the zone latent load).
-
-### Refrigeration:System
-
-The refrigeration system object simulates the performance of a supermarket refrigeration system when used along with other objects to define the refrigeration load(s), the compressor(s), and the condenser.
-
-At least one refrigeration load object must be defined which may be one of four types of load, a refrigerated case, a walk-in cooler, a chiller providing refrigeration to a secondary loop, or a cascade condenser which absorbs heat rejected by a lower-temperature system (Ref. Refrigeration:Case, Refrigeration:WalkIn, Refrigeration:SecondarySystem,  and Refrigeration:Condenser:Cascade) If multiple loads are served by the same system , the user should use one or both of the list objects available to assign loads to the system. The first list includes all cases and walkins cooled directly by this system (Ref. Refrigeration:CaseAndWalkInList). The second list includes any ‘transfer’ loads, that is refrigeration loads borne by this system that are transferred from another refrigeration system via either a secondary loop chiller or a cascade condenser (Ref. Refrigeration:TransferLoadList, see the Engineering Reference for more information about these types of systems).
-
-The refrigeration system object is capable of modeling both single-stage and two-stage compression refrigeration systems.  The name of at least one compressor must be defined and a list object is available if the system is served by more than one compressor (Ref. Refrigeration:Compressor and Refrigeration:CompressorList).
-
-Heat is rejected outdoors in a condenser by direct air flow, evaporative water cooling, by a water-cooled condenser with appropriate plant loop piping, or to a cascade condenser cooled by another refrigeration system(ref: Refrigeration:Condenser:AirCooled, Refrigeration:Condenser:EvaporativeCooled, Refrigeration:Condenser:WaterCooled, Refrigeration:Condenser:Cascade). With evaporative cooling, water is sprayed through the air stream to effectively lower the air temperature experienced by the condenser coil as a result of water evaporation. The use of a water-cooled condenser requires the definition of a plant loop to supply cooling to the condenser.  If a cascade condenser is specified, the refrigeration system absorbing the rejected heat must also be defined.
-
-The refrigeration system may also include a liquid suction and/or mechanical subcooler (Ref. Refrigeration:Subcooler).
-
-The system object coordinates the energy flows between the other refrigeration objects and is used to set system parameters. Compressor waste heat can also be reclaimed for use by an optional air- or water-heating coil (Ref. Coil:Heating:Desuperheater and Coil:WaterHeating:Desuperheater).
-
-The inputs for the refrigeration system object, in addition to the names of the other refrigeration objects described above, include a name for this system, the minimum condensing temperature, the refrigeration system working fluid, and the type of saturated suction temperature control. Optional input fields are also provided for users seeking to keep track of refrigerant inventory and suction pipe heat gains.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a refrigeration system. Any reference to this refrigeration system by another object will use this name.
-
-#### Field: Refrigerated Case or WalkIn or CaseAndWalkInList Name
-
-Identifies a single case, a single walkin, single air chiller, or a particular list of refrigerated cases and walkins or air chillers, that is cooled by this refrigeration system. The name will be validated against the case, walkin, air chiller and CaseAndWalkInList names  (ref: Refrigeration:Case, Refrigeration:WalkIn, Refrigeration:AirChiller, and Refrigeration:CaseAndWalkInList) in the input file. Only cases and walkins or air chillers served directly by the system should be included in this list.  Any cases, walkins, or air chillers served indirectly via a secondary loop should NOT be included in this list. Note that any system that serves an air chiller cannot also serve a case or walkin.
-
-#### Field: Refrigeration Transfer Load or TransferLoad List Name
-
-Identifies a single SecondarySystem, a single Cascade Condenser, OR or a list of Transfer Loads (where the list is comprised of SecondarySystems and/or Cascade Condensers) that are cooled by this refrigeration system. The name will be validated against the secondary system, cascade condenser, and TransferLoad list names (ref: Refrigeration:SecondarySystem, Refrigeration:Condenser:Cascade, and Refrigeration:TransferLoadList) in the input file. Only secondary systems and cascade condensers served directly by the system should be included in this list. (NOTE – this entry is for a cascade condenser *cooled by* this system, not a condenser *absorbing heat rejected by* this system.)
-
-#### Field: Condenser Name
-
-The name of the condenser that is used to *reject heat from* this refrigeration system. The name will be validated against the condenser names (ref: Refrigeration:Condenser:AirCooled, Refrigeration:Condenser:WaterCooled, Refrigeration:Condenser:EvaporativeCooled, and Refrigeration:Condenser:Cascade) in the input file.
-
-#### Field:Compressor or  Compressor List Name
-
-Identifies a single compressor, or a particular list of compressors, that provide cooling energy to this refrigeration system. The name will be validated against the compressor list names (ref: List:Refrigeration:Compressors) in the input file.  If the refrigeration systems contains two stages of compression, this field identifies the low-stage compressors connected to the two-stage system.
-
-#### Field: Minimum Condensing Temperature
-
-This numeric field specifies the minimum condensing temperature (C), which is usually determined by the temperature required to maintain acceptable thermal expansion valve performance.
-
-#### Field: Refrigeration System Working Fluid Type
-
-The type of refrigerant used by the system.  Valid choices are R11, R123, R134A, R12, R22, R404A, R507A, or R410A. This name will be validated against Fluid Names (ref: Fluid Properties section) in the input file. Note that the corresponding property data, available in FluidPropertiesRefData.idf, must by supplied in the input file.
-
-#### Field: Suction Temperature Control Type
-
-The type of saturated suction temperature control used by the system. Valid choices are **FloatSuctionTemperature** and **ConstantSuctionTemperature**.  If the field is blank, the default will be **ConstantSuctionTemperature**. See the Engineering Reference section, Variable Evaporator Temperature, for a discussion of this option.
-
-#### Field: Mechanical Subcooler Name
-
-This optional field identifies a mechanical subcooler that absorbs heat from this refrigeration system. This field should not be used for a mechanical subcooler that absorbs heat from another system. The name will be validated against the subcooler names (ref: Refrigeration:Subcooler) in the input file.
-
-#### Field: Liquid Suction Heat Exchanger Subcooler Name
-
-This optional field Identifies a particular liquid suction heat exchanger (LSHX) subcooler present in this refrigeration system. The name will be validated against the subcooler names (ref: Refrigeration:Subcooler) in the input file.
-
-#### Field: Sum UA Suction Piping
-
-This optional field is typically used when trying to determine the impact of pipe heat gains on system performance and zone heat balance, particularly in comparing a DX system to a secondary system. Enter the value for suction piping heat gain (in W/C).  That is, sum up the product of the pipe wall insulation conductance times the outer surface area of the pipe insulation. Please see the Engineering Reference for guidance in calculating this value. If the Sum UA Suction Piping is entered, the Suction Piping Zone Name is also required.
-
-#### Field: Suction Piping Zone Name
-
-This optional field is typically used when trying to determine the impact of pipe heat gains on system performance, particularly in comparing a DX system to a secondary system. (If the previous field, Sum UA Suction Piping, is blank, this field will not be used.) Enter the name of the zone where the suction piping is located. The suction piping heat gains will be calculated based upon the air temperature within this zone. The heat balance of this zone will also be affected by the piping heat exchange. Additional output variables are described at the end of this “Group-Refrigeration� section for the total impact of refrigeration on zones, including suction pipe heat exchange.
-
-#### Field: End-Use Subcategory
-
-This field allows the specification of a user-defined end-use subcategory (e.g., "Low Temperature Rack"). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the "General" end-use subcategory.
-
-#### Field: Number of Compressor Stages
-
-This field determines whether the refrigeration system contains one or two stages of compression.  In this field, enter either “1� for single-stage compression systems or “2� for two-stage compression systems.  If two stages of compression are selected, then an intercooler will be used between the compressor stages to cool the discharge of the low-stage compressors.  The default value is “1�.
-
-#### Field: Intercooler Type
-
-This field determines the type of intercooler which is used for two-stage compression systems.  Valid choices for this field include “None�, “Flash Intercooler� or “Shell-and-Coil Intercooler�.  Single-stage systems require “None� while two-stage systems require either “Flash Intercooler� or “Shell-and-Coil Intercooler�.  The default selection is “None�, corresponding to a single-stage compression system.
-
-#### Field: Shell-and-Coil Intercooler Effectiveness
-
-When a shell-and-coil intercooler is selected for two-stage compression systems, this field allows the specification of the shell-and-coil intercooler effectiveness.  Values in this field will only be valid if “Shell-and-Coil Intercooler� is selected in the “Intercooler Type� field above.  The valid range of values for this field is between 0.0 and 1.0.  A default value of 0.80 will be used if none is specified.
-
-#### Field: High-Stage Compressor or CompressorList Name
-
-Identifies a single compressor, or a particular list of compressors, that comprise the high-stage compression of a two-stage compression refrigeration system. The name will be validated against the compressor list names (ref: List:Refrigeration:Compressors) in the input file.  Names in this field are only valid if two compressor stages have been specified in the “Number of Compressor Stages� field above.
-
-The following is an example input for a single-stage compression refrigeration system.
-
-```idf
- Refrigeration:System,
-    MediumTempSystem,        !- Refrigeration System Name
-   MediumTempCaselist,      !-  Refrigeration Case or Walkin or CaseAndWalkInList Name
-    ,                        !- Refrigeration Transfer Load or TransferLoad List Name
-    AirCooledCondenserA,     !- Refrigeration Condenser Name
-    MediumTempCompressorlist, !- Refrigeration Compressor or CompressorList Name
-    25.0,                    !- Minimum Condensing Temperture {C}
-    R134a,                   !- Refrigeration System Working Fluid
-    ConstantSuctionTemperature,  !- Suction Temperature Control Type
-    ,                        !- Optional mechanical subcooler name
-    ,                        !- Optional LSHX subcooler name
-    ,                        !- Sum UA Distribution Piping {W/K}
-    ,                        !- Distribution Piping Zone Name
-    MedTempRefrig;           !- End-Use Subcategory
-```
-
-
-
-The following is an example input for a two-stage compression refrigeration system.
-
-```idf
- Refrigeration:System,
-    LowTempSystem,           !- Refrigeration System Name
-   LowTempCaselist,         !-  Refrigeration Case or Walkin or CaseAndWalkInList Name
-    ,                        !- Refrigeration Transfer Load or TransferLoad List Name
-    AirCooledCondenserB,     !- Refrigeration Condenser Name
-    LowStageCompressorList,  !- Refrigeration Compressor or CompressorList Name
-    25.0,                    !- Minimum Condensing Temperture {C}
-    R404A,                   !- Refrigeration System Working Fluid
-    ConstantSuctionTemperature,  !- Suction Temperature Control
-    ,                        !- Optional mechanical subcooler name
-    ,                        !- Optional LSHX subcooler name
-    ,                        !- Sum UA Distribution Piping {W/K}
-    ,                        !- Distribution Piping Zone Name
-    LowTempRefrig,           !- End-Use Subcategory
-    2,                       !- Number of Compressor Stages
-    Shell-and-Coil Intercooler,  !- Intercooler Type
-    0.7,                     !- Shell-and-Coil Intercooler Effectiveness
-    HiStageCompressorList    !- High-Stage Compressor or CompressorList Name
-```
-
-
-
-### Refrigeration System Outputs
-
-THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE CASES AND/OR WALKINS:
-
-* Zone,Average, Refrigeration System Total Compressor Electric Power [W]
-
-* Zone,Sum, Refrigeration System Total Compressor Electric Energy [J]
-
-* Zone,Average, Refrigeration System Average Compressor COP [W/W]
-
-* Zone,Average, Refrigeration System Total Compressor Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration System Total Compressor Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Total Cases and Walk Ins Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration System Total Cases and Walk Ins Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Total Transferred Load Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration System Total Transferred Load Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Total Suction Pipe Heat Gain Rate [W]
-
-* Zone,Sum, Refrigeration System Total Suction Pipe Heat Gain Energy [J]
-
-* Zone,Average, Refrigeration System Net Rejected Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration System Net Rejected Heat Transfer Energy [J]
-
-* Zone,Average,Refrigeration System Estimated Refrigerant Inventory Mass [kg]
-
-* Zone,Average, Refrigeration System Liquid Suction Subcooler Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Liquid Suction Subcooler Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Estimated Refrigerant Inventory [kg]
-
-* Zone,Average, Refrigeration System Estimated Refrigerant Mass Flow Rate [kg/s]
-
-* Zone,Average, Refrigeration System Condensing Temperature [C]'
-
-* Zone,Average, Refrigeration System Evaporating Temperature [C]
-
-* Zone,Average, Refrigeration System Suction Pipe Suction Temperature [C]
-
-* Zone,Average, Refrigeration System Thermostatic Expansion Valve Liquid Temperature [C]
-
-* Zone,Average, Refrigeration System Estimated High Stage Refrigerant Mass Flow Rate [kg/s]
-
-* Zone,Sum,Refrigeration System Total High Stage Compressor Electric Energy [J]
-
-* Zone,Average,Refrigeration System Total High Stage Compressor Electric Power [W]
-
-* Zone,Sum,Refrigeration System Total High Stage Compressor Heat Transfer Energy [J]
-
-* Zone,Average,Refrigeration System Total High Stage Compressor Heat Transfer Rate [W]
-
-* Zone,Sum,Refrigeration System Total Low and High Stage Compressor Electric Energy [J]
-
-* Zone,Sum,Refrigeration System Total Low Stage Compressor Electric Energy [J]
-
-* Zone,Average,Refrigeration System Total Low Stage Compressor Electric Power [W]
-
-* Zone,Sum,Refrigeration System Total Low Stage Compressor Heat Transfer Energy [J]
-
-* Zone,Average,Refrigeration System Total Low Stage Compressor Heat Transfer Rate [W]
-
-* Zone,Average,Refrigeration System Estimated Low Stage Refrigerant Mass Flow Rate [kg/s]
-
-
-
-THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE AIR CHILLERS:
-
-
-
-* HVAC,Average, Refrigeration Air Chiller System Total Compressor Electric Power [W]
-
-* HVAC,Sum, Refrigeration Air Chiller System Total Compressor Electric Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Average Compressor COP [W/W]
-
-* HVAC,Average, Refrigeration Air Chiller System Total Compressor Heat Transfer Rate [W]
-
-* HVAC,Sum, Refrigeration Air Chiller System Total Compressor Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Total Air Chiller Heat Transfer Rate [W]
-
-* HVAC,Sum, Refrigeration Air Chiller System Total Case and Walk In Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Total Transferred Load Heat Transfer Rate [W]
-
-* HVAC,Sum, Refrigeration Air Chiller System Total Transferred Load Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Total Suction Pipe Heat Gain Rate [W]
-
-* HVAC,Sum, Refrigeration Air Chiller System Total Suction Pipe Heat Gain Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Net Rejected Heat Transfer Rate [W]
-
-* HVAC,Sum, Refrigeration Air Chiller System Net Rejected Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Liquid Suction Subcooler Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Liquid Suction Subcooler Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Estimated Refrigerant Inventory Mass [kg]
-
-* HVAC,Average, Refrigeration Air Chiller System Estimated Refrigerant Mass Flow Rate [kg/s]
-
-* HVAC,Average,Refrigeration Air Chiller System Intercooler Temperature [C]
-
-* HVAC,Average,Refrigeration Air Chiller System Intercooler Pressure [Pa]
-
-* HVAC,Average, Refrigeration Air Chiller System Condensing Temperature [C]'
-
-* HVAC,Average, Refrigeration Air Chiller System Evaporating Temperature [C]
-
-* HVAC,Average, Refrigeration Air Chiller System Suction Temperature [C]
-
-* HVAC,Average, Refrigeration Air Chiller System TXV Liquid Temperature [C]
-
-* HVAC,Average,Refrigeration Air Chiller System Estimated High Stage Refrigerant Mass Flow Rate [kg/s]
-
-* HVAC,Sum,Refrigeration Air Chiller System Total High Stage Compressor Electric Energy [J]
-
-* HVAC,Average,Refrigeration Air Chiller System Total High Stage Compressor Electric Power [W]
-
-* HVAC,Sum,Refrigeration Air Chiller System Total High Stage Compressor Heat Transfer Energy [J]
-
-* HVAC,Average,Refrigeration Air Chiller System Total High Stage Compressor Heat Transfer Rate [W]
-
-* HVAC,Sum, Refrigeration Air Chiller System Total Low and High Stage Compressor Electric Energy [J]
-
-* HVAC,Sum,Refrigeration Air Chiller System Total Low Stage Compressor Electric Energy [J]
-
-* HVAC,Average,Refrigeration Air Chiller System Total Low Stage Compressor Electric Power [W]
-
-* HVAC,Sum, Refrigeration Air Chiller System Total Low Stage Compressor Heat Transfer Energy [J]
-
-* HVAC,Average,Refrigeration Air Chiller System Total Low Stage Compressor Heat Transfer Rate [W]
-
-* HVAC,Average,Refrigeration Air Chiller System Estimated Low Stage Refrigerant Mass Flow Rate [kg/s]
-
-
-
-#### THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE CASES AND/OR WALKINS
-
-#### Refrigeration System Total Compressor Electric Power [W]
-
-This output is the total electric power input to the system compressor(s) in Watts.
-
-#### Refrigeration System Total Compressor Electric Energy [J]
-
-This is the electricity consumption of the system’s compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration System Total Low Stage Compressor Electric Power [W]
-
-This output is the total electric power input to the system’s low-stage compressor(s) in Watts.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Total Low Stage Compressor Electric Energy [J]
-
-This is the electricity consumption of the system’s low-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Total High Stage Compressor Electric Power [W]
-
-This output is the total electric power input to the system’s high-stage compressor(s) in Watts.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Total High Stage Compressor Electric Energy [J]
-
-This is the electricity consumption of the system’s high-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Total Low and High Stage Compressor Electric Energy  [J]
-
-This is the total electricity consumption of the system’s low- and high-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Average Compressor COP [W/W]
-
-This output is the system average compressor COP, the total refrigeration effect divided by the total power to the compressors.
-
-#### Refrigeration System Total Compressor Heat Transfer Rate [W]
-
-This output is the total heat transfer rate of the Refrigeration Compressor rack in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.
-
-#### Refrigeration System Total Compressor Heat Transfer Energy [J]
-
-This is the total heat transfer of the Refrigeration Compressor rack in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration System Total Low Stage Compressor Heat Transfer Rate [W]
-
-This output is the total heat transfer rate of the low-stage compressors in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Total Low Stage Compressor Heat Transfer Energy [J]
-
-This is the total heat transfer of the low-stage compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Total High Stage Compressor Heat Transfer Rate [W]
-
-This output is the total heat transfer rate of the high-stage compressors in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Total High Stage Compressor Heat Transfer Energy [J]
-
-This is the total heat transfer of the high-stage compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Total Cases and Walk Ins Heat Transfer Rate [W]
-
-This output is the total heat transfer rate from the refrigerated cases and walk-ins served directly by this system in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases and walk-ins that are connected directly to this system. This value does not include compressor or condenser fan heat or the heat transfer for cases and walk-ins served by any connected secondary systems.
-
-#### Refrigeration System Total Cases and Walk Ins Heat Transfer Energy [J]
-
-This output is the total heat transfer energy from the refrigerated cases and walk-ins served directly by this system in Joules. It is the sum of all of the heat transfered for the refrigerated cases and walk-ins that are connected directly to this system. This value does not include compressor or condenser fan heat or the heat transfer for cases and walk-ins served by any connected secondary systems.
-
-#### Refrigeration System Total Transferred Load Heat Transfer Rate [W]
-
-This output is the sum of the heat transfer rates for any secondary loops, cascade condensers, and mechanical subcoolers cooled by this system, minus the benefit of any mechanical subcooler providing cooling to this system in Watts. Therefore, if the only transfer load between two systems is a mechanical subcooler, the same amount will show as a negative value for the system receiving the cooling effect and as a positive number for the system serving that cooling load. It also includes the pump energy for any secondary loops and the compressor energy for any cascade condenser systems that are cooled by this system. (See the Engineering Reference for more details about the loads placed by secondary systems upon the primary system.)
-
-#### Refrigeration System Total Transferred Load Heat Transfer Energy [J]
-
-This output is the sum of the heat transfered for any secondary loops, cascade condensers, and mechanical subcoolers cooled by this system, minus the benefit of any mechanical subcooler providing cooling to this system in Joules. Therefore, if the only transfer load between two systems is a mechanical subcooler, the same amount will show as a negative value for the system receiving the cooling effect and as a positive number for the system serving that cooling load. It also includes the pump energy for any secondary loops and the compressor energy for any cascade condenser systems that are cooled by this system. (See the Engineering Reference for more details about the loads placed by secondary systems upon the primary system.)
-
-#### Refrigeration System Total Suction Pipe Heat Gain Rate [W]
-
-This output is the total heat transfer rate for suction piping served by this system in Watts. Note this is an optional input, and is only available if the user has described the suction piping heat gain characteristics in the input.
-
-#### Refrigeration System Total Suction Pipe Heat Gain Energy [J]
-
-This output is the total heat transfer rate for suction piping served by this system in Watts. Note this is an optional input, and is only available if the user has described the suction piping heat gain characteristics in the input.
-
-#### Refrigeration System Net Rejected Heat Transfer Rate [W]
-
-This output is the total heat rejected by this system to the system condenser in Watts. It does not include system heat rejection that has been recovered for useful purposes. However, if a water-cooled condenser was used to provide heat to a separate water loop, the energy transferred to that loop is included here.
-
-#### Refrigeration System Net Rejected Heat Transfer Energy [J]
-
-This output is the total heat rejected by this system to the system condenser in Joules for the timestep being reported. It does not include system heat rejection that has been recovered for useful purposes. However, if a water-cooled condenser was used to provide heat to a separate water loop, the energy transferred to that loop is included here.
-
-#### Refrigeration System Liquid Suction Subcooler Heat Transfer Rate [W]
-
-This output is the total heat transferred from the liquid condensate before the thermal expansion valve to the suction gas.
-
-#### Refrigeration System Liquid Suction Subcooler Heat Transfer Energy [J]
-
-This output is the total heat transferred from the liquid condensate before the thermal expansion valve to the suction gas.
-
-#### Refrigeration System Estimated Refrigerant Inventory Mass [kg]
-
-This output is the sum of the input inventory values for the condenser, receiver, cases, and liquid pipes that are a part of this system.
-
-#### Refrigeration System Estimated Refrigerant Mass Flow Rate [kg/s]
-
-This output is the calculated refrigerant mass flow through the compressors for this system.
-
-#### Refrigeration System Estimated Low Stage Refrigerant Mass Flow Rate [kg/s]
-
-This output is the calculated refrigerant mass flow through the low-stage compressors for this system.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Estimated High Stage Refrigerant Mass Flow Rate [kg/s]
-
-This output is the calculated refrigerant mass flow through the high-stage compressors for this system.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Intercooler Temperature [C]
-
-This is the saturation temperature in the intercooler.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Intercooler Pressure [Pa]
-
-This is the saturation pressure in the intercooler.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration System Condensing Temperature [C]
-
-This is the saturated condensing temperature.
-
-#### Refrigeration System Evaporating Temperature [C]
-
-This is the saturated evaporating temperature.
-
-#### Refrigeration System Suction Pipe Suction Temperature [C]
-
-This is the temperature at the compressor inlet including superheat after the cases and superheat from any liquid suction heat exchangers.
-
-#### Refrigeration System Thermostatic Expansion Valve Liquid Temperature [C]
-
-This is the temperature entering the thermal expansion valve before the cases, equal to the condensing temperature minus any subcooling included in the condenser or provided by mechanical and/or liquid suction heat exchanger subcoolers.
-
-#### THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE AIR CHILLERS
-
-#### Refrigeration Air Chiller System Total Compressor Electric Power [W]
-
-This output is the total electric power input to the system compressor(s) in Watts.
-
-#### Refrigeration Chiller System Total Compressor Electric Energy [J]
-
-This is the electricity consumption of the system’s compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller System Total Low Stage Compressor Electric Power [W]
-
-This output is the total electric power input to the system’s low-stage compressor(s) in Watts.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Total Low Stage Compressor Electric Energy [J]
-
-This is the electricity consumption of the system’s low-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Total High Stage Compressor Electric Power [W]
-
-This output is the total electric power input to the system’s high-stage compressor(s) in Watts.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Total High Stage Compressor Electric Energy [J]
-
-This is the electricity consumption of the system’s high-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Total Low and High Stage Compressor Electric Energy [J]
-
-This is the total electricity consumption of the system’s low- and high-stage compressor(s) in Joules for the timestep being reported. The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Average Compressor COP [W/W]
-
-This output is the system average compressor COP, the total refrigeration effect divided by the total power to the compressors
-
-#### Refrigeration Air Chiller System Total Compressor Heat Transfer Rate [W]
-
-This output is the total heat transfer rate of the Refrigeration Compressor rack in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.
-
-#### Refrigeration Air Chiller System Total Compressor Heat Transfer Energy [J]
-
-This is the total heat transfer of the Refrigeration Compressor rack in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller System Total Low Stage Compressor Heat Transfer Rate [W]
-
-This output is the total heat transfer rate of the low-stage compressors in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Total Low Stage Compressor Heat Transfer Energy [J]
-
-This is the total heat transfer of the low-stage compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Total High Stage Compressor Heat Transfer Rate [W]
-
-This output is the total heat transfer rate of the high-stage compressors in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases, walk-ins, secondary loops, cascade condensers, and mechanical subcoolers that are cooled by this system. This value does not include compressor or condenser fan heat. If specified as in input value, the suction pipe heat gains are included in this value.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Total High Stage Compressor Heat Transfer Energy [J]
-
-This is the total heat transfer of the high-stage compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Total Air Chiller Heat Transfer Rate [W]
-
-This output is the total heat transfer rate from the refrigerated cases and walk-ins served directly by this system in Watts. It is the sum of all of the heat transfer rates for the refrigerated cases and walk-ins that are connected directly to this system. This value does not include compressor or condenser fan heat or the heat transfer for cases and walk-ins served by any connected secondary systems.
-
-#### Refrigeration Air Chiller System Total Case and Walk In Heat Transfer Energy [J]
-
-This output is the total heat transfer energy from the refrigerated cases and walk-ins served directly by this system in Joules. It is the sum of all of the heat transfered for the refrigerated cases and walk-ins that are connected directly to this system. This value does not include compressor or condenser fan heat or the heat transfer for cases and walk-ins served by any connected secondary systems.
-
-#### Refrigeration Air Chiller System Total Transferred Load Heat Transfer Rate [W]
-
-This output is the sum of the heat transfer rates for any secondary loops, cascade condensers, and mechanical subcoolers cooled by this system, minus the benefit of any mechanical subcooler providing cooling to this system in Watts. Therefore, if the only transfer load between two systems is a mechanical subcooler, the same amount will show as a negative value for the system receiving the cooling effect and as a positive number for the system serving that cooling load. It also includes the pump energy for any secondary loops and the compressor energy for any cascade condenser systems that are cooled by this system. (See the Engineering Reference for more details about the loads placed by secondary systems upon the primary system.)
-
-#### Refrigeration Air Chiller System Total Transferred Load Heat Transfer Energy [J]
-
-This output is the sum of the heat transfered for any secondary loops, cascade condensers, and mechanical subcoolers cooled by this system, minus the benefit of any mechanical subcooler providing cooling to this system in Joules. Therefore, if the only transfer load between two systems is a mechanical subcooler, the same amount will show as a negative value for the system receiving the cooling effect and as a positive number for the system serving that cooling load. It also includes the pump energy for any secondary loops and the compressor energy for any cascade condenser systems that are cooled by this system. (See the Engineering Reference for more details about the loads placed by secondary systems upon the primary system.)
-
-#### Refrigeration Air Chiller System Total Suction Pipe Heat Gain Rate [W]
-
-This output is the total heat transfer rate for suction piping served by this system in Watts. Note this is an optional input, and is only available if the user has described the suction piping heat gain characteristics in the input.
-
-#### Refrigeration Air Chiller System Total Suction Pipe Heat Gain Energy [J]
-
-This output is the total heat transfer rate for suction piping served by this system in Watts. Note this is an optional input, and is only available if the user has described the suction piping heat gain characteristics in the input.
-
-#### Refrigeration Air Chiller System Net Rejected Heat Transfer Rate [W]
-
-This output is the total heat rejected by this system to the system condenser in Watts. It does not include system heat rejection that has been recovered for useful purposes. However, if a water-cooled condenser was used to provide heat to a separate water loop, the energy transferred to that loop is included here.
-
-#### Refrigeration Air Chiller System Net Rejected Heat Transfer Energy [J]
-
-This output is the total heat rejected by this system to the system condenser in Joules for the timestep being reported. It does not include system heat rejection that has been recovered for useful purposes. However, if a water-cooled condenser was used to provide heat to a separate water loop, the energy transferred to that loop is included here.
-
-#### Refrigeration Air Chiller System Liquid Suction Subcooler Heat Transfer Rate [W]
-
-This output is the total heat transferred from the liquid condensate before the thermal expansion valve to the suction gas.
-
-#### Refrigeration Air Chiller System Liquid Suction Subcooler Heat Transfer Energy [J]
-
-This output is the total heat transferred from the liquid condensate before the thermal expansion valve to the suction gas.
-
-#### Refrigeration Air Chiller System Mechanical Subcooler Heat Transfer Energy [J]
-
-#### Refrigeration Air Chiller System Estimated Refrigerant Inventory Mass [kg]
-
-This output is the sum of the input inventory values for the condenser, receiver, cases, and liquid pipes that are a part of this system.
-
-#### Refrigeration Air Chiller System Estimated Refrigerant Mass Flow Rate [kg/s]
-
-This output is the calculated refrigerant mass flow through the compressors for this system.
-
-#### Refrigeration Air Chiller System Estimated Low Stage Refrigerant Mass Flow Rate [kg/s]
-
-This output is the calculated refrigerant mass flow through the low-stage compressors for this system.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Estimated High Stage Refrigerant Mass Flow Rate [kg/s]
-
-This output is the calculated refrigerant mass flow through the high-stage compressors for this system.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Intercooler Temperature [C]
-
-This is the saturation temperature in the intercooler.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Intercooler Pressure [Pa]
-
-This is the saturation pressure in the intercooler.  This output is valid only for two-stage compression systems.
-
-#### Refrigeration Air Chiller System Condensing Temperature [C]
-
-This is the saturated condensing temperature.
-
-#### Refrigeration Air Chiller System Evaporating Temperature [C]
-
-This is the saturated evaporating temperature.
-
-#### Refrigeration Air Chiller System Suction Temperature [C]
-
-This is the temperature at the compressor inlet including superheat after the cases and superheat from any liquid suction heat exchangers.
-
-#### Refrigeration Air Chiller System TXV Liquid Temperature [C]
-
-This is the temperature entering the thermal expansion valve before the cases, equal to the condensing temperature minus any subcooling included in the condenser or provided by mechanical and/or liquid suction heat exchanger subcoolers.
-
-### Refrigeration:TranscriticalSystem
-
-The Refrigeration:TranscriticalSystem object allows users to model detailed transcritical carbon dioxide (CO<sub>2</sub>) booster refrigeration systems used in supermarkets.  The object allows for modeling either a single stage system with medium-temperature loads or a two stage system with both medium- and low-temperature loads.
-
-The input objects required to model a detailed transcritical CO<sub>2</sub> refrigeration system include the following:
-
-- One Refrigeration:TranscriticalSystem object,
-
-- At least one refrigeration load object which may include any combination of the following:
-
-- Refrigeration:Case,
-
-- Refrigeration:WalkIn,
-
-- Refrigeration:CaseAndWalkInList (may include both cases and/or walk-in cooler names),
-
-- At least one Refrigeration:Compressor object (multiple compressors are entered using a Refrigeration:CompressorList),
-
-- One Refrigeration:GasCooler:AirCooled object,
-
-Output variables are available to describe the total heat exchange between all the refrigeration objects and the zones containing these objects.  These variables are described at the end of this section.
-
-At least one refrigeration load object must be defined which may be one of two types of loads, including a refrigerated display case and a walk-in cooler, (Ref. Refrigeration:Case, and Refrigeration:WalkIn).  If multiple loads are served by the same system, the user should use the refrigerated case and walk-in list object available to assign all cases and walk-ins cooled directly by this system (Ref. Refrigeration:CaseAndWalkInList).
-
-The name of at least one compressor must be defined and a list object is available if the system is served by more than one compressor (Ref. Refrigeration:Compressor and Refrigeration:CompressorList).
-
-Heat is rejected to the outdoors via an air-cooled gas cooler (Ref. Refrigeration:GasCooler:AirCooled).
-
-The Refrigeration:TranscriticalSystem object coordinates the energy flows between the other refrigeration objects and is used to set system parameters.
-
-The inputs for the refrigeration system object, in addition to the names of the other refrigeration objects described above, include a name for this system, the receiver pressure, the subcooler effectiveness, and the refrigeration system working fluid.  Optional input fields are also provided for users seeking to keep track of suction pipe heat gains.
-
-A detailed description of the transcritical CO<sub>2</sub> booster refrigeration system may be found in the Refrigeration section of the Engineering Reference.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a transcritical CO<sub>2</sub> refrigeration system.  Any reference to this refrigeration system by another object will use this name.
-
-#### Field: System Type
-
-Identifies the transcritical CO<sub>2</sub> refrigeration system as either a single-stage system with only medium-temperature loads, or a two-stage system with both medium- and low-temperature loads.  Valid choices are:  SingleStage for single stage systems or TwoStage for two stage systems.
-
-#### Field: Medium Temperature Refrigerated Case or WalkIn or CaseAndWalkInList Name
-
-Identifies a single case, a single walk-in, or a particular list of refrigerated cases and walk-ins, that is cooled by the medium-temperature stage of the refrigeration system.  The name will be validated against the case, walk-in, and CaseAndWalkInList names (Ref. Refrigeration:Case, Refrigeration:WalkIn, and Refrigeration:CaseAndWalkInList) in the input file.  Only medium temperature cases and walk-ins served directly by the system should be included in this list.  Note that this entry is required for both single-stage and two-stage systems.
-
-#### Field: Low Temperature Refrigerated Case or WalkIn or CaseAndWalkInList Name
-
-Identifies a single case, a single walk-in, or a particular list of refrigerated cases and walk-ins, that is cooled by the low-temperature stage of the refrigeration system.  The name will be validated against the case, walk-in, and CaseAndWalkInList names (Ref. Refrigeration:Case, Refrigeration:WalkIn, and Refrigeration:CaseAndWalkInList) in the input file.  Only low temperature cases and walk-ins served directly by the system should be included in this list.  Note that this entry is valid only for two-stage systems.
-
-#### Field: Refrigeration Gas Cooler Name
-
-The name of the gas cooler that is used to reject heat from the transcritical refrigeration system.  The name will be validated against the gas cooler names (Ref. Refrigeration:GasCooler:AirCooled) in the input file.
-
-#### Field: High Pressure Compressor or Compressor List Name
-
-Identifies a single compressor, or a particular list of compressors, that provides compression for a single-stage system or the high pressure stage of a two-stage system.  The name will be validated against the compressor list names (Ref. List:Refrigeration:Compressors) in the input file.  Note that this entry is required for both single-stage and two-stage systems.
-
-#### Field: Low Pressure Compressor or Compressor List Name
-
-Identifies a single compressor, or a particular list of compressors, that provides compression for the low pressure stage of a two-stage system.  The name will be validated against the compressor list names (Ref. List:Refrigeration:Compressors) in the input file.  Note that this entry is valid only for two-stage systems.
-
-#### Field: Receiver Pressure
-
-This numeric field specifies the refrigerant pressure (Pa) in the receiver.  The default value for the receiver pressure is 4.0 × 10<sup>6</sup> Pa.
-
-#### Field: Subcooler Effectiveness
-
-This numeric field specifies the heat exchanger effectiveness of the subcooler.  The default value for the subcooler effectiveness is 0.4.
-
-#### Field: Refrigeration System Working Fluid Type
-
-The type of refrigerant used by the system.  It is assumed that carbon dioxide will be the refrigerant used in the transcritical CO<sub>2</sub> refrigeration system.  However, the user must specify the name used in the input file which refers to carbon dioxide.  This name will be validated against Fluid Names (Ref. Fluid Properties section) in the input file.  Note that the corresponding property data for carbon dioxide (R744), available in FluidPropertiesRefData.idf, must be supplied in the input file.
-
-#### Field: Sum UA Suction Piping for Medium Temperature Loads
-
-This optional field is typically used to determine the impact of pipe heat gains on system performance and zone heat balance.  Enter the value for suction piping heat gain (in W/C) for the medium-temperature suction line, i.e., sum up the product of the pipe wall insulation conductance times the outer surface area of the pipe insulation.  Please see the Engineering Reference for guidance in calculating this value.  If the Sum UA Suction Piping for Medium Temperature Loads is entered, the Medium Temperature Suction Piping Zone Name is also required.
-
-#### Field: Medium Temperature Suction Piping Zone Name
-
-This optional field is typically used to determine the impact of pipe heat gains on system performance.  If the previous field, Sum UA Suction Piping for Medium Temperature Loads, is blank, this field will not be used.  Enter the name of the zone where the medium-temperature suction piping is located.  The suction piping heat gains will be calculated based upon the air temperature within this zone.  The heat balance of this zone will also be affected by the piping heat exchange.  Additional output variables are described at the end of this section for the total impact of refrigeration on zones, including suction pipe heat exchange.
-
-#### Field: Sum UA Suction Piping for Low Temperature Loads
-
-This optional field is typically used to determine the impact of pipe heat gains on system performance and zone heat balance.  Enter the value for suction piping heat gain (in W/C) for the low-temperature suction line, i.e., sum up the product of the pipe wall insulation conductance times the outer surface area of the pipe insulation.  Please see the Engineering Reference for guidance in calculating this value.  If the Sum UA Suction Piping for Low Temperature Loads is entered, the Low Temperature Suction Piping Zone Name is also required.  Note that this entry is valid only for two-stage systems.
-
-#### Field: Low Temperature Suction Piping Zone Name
-
-This optional field is typically used to determine the impact of pipe heat gains on system performance.  If the previous field, Sum UA Suction Piping for Low Temperature Loads, is blank, this field will not be used.  Enter the name of the zone where the low-temperature suction piping is located. The suction piping heat gains will be calculated based upon the air temperature within this zone.  The heat balance of this zone will also be affected by the piping heat exchange.  Additional output variables are described at the end of this section for the total impact of refrigeration on zones, including suction pipe heat exchange.  Note that this entry is valid only for two-stage systems.
-
-#### Field: End-Use Subcategory
-
-This field allows the specification of a user-defined end-use subcategory (e.g., "Medium Temperature System").  A new meter for reporting is created for each unique subcategory (Ref. Output:Meter objects).  Subcategories are also reported in the ABUPS table.  If this field is left blank, the equipment will be assigned to the "General" end-use subcategory.
-
-The following is an example input for a transcritical CO<sub>2</sub> refrigeration system.
-
-```idf
-Refrigeration:TranscriticalSystem,
-    TransRefrigSys,          !- Name
-    TwoStage,                !- System Type
-    MTLoads,                 !- Medium Temperature Refrigerated Case or Walkin or CaseAndWalkInList Name
-    LTLoads,                 !- Low Temperature Refrigerated Case or Walkin or CaseAndWalkInList Name
-    RefrigGasCooler,         !- Refrigeration Gas Cooler Name
-    HPCompressors,           !- High Pressure Compressor or CompressorList Name
-    LPCompressors,           !- Low Pressure Compressor or CompressorList Name
-    4000000,                 !- Receiver Pressure
-    0.4,                     !- Subcooler Effectiveness
-    R744,                    !- Refrigeration System Working Fluid Type
-    ,                        !- Sum UA Suction Piping for Medium Temperature Loads
-    ,                        !- Medium Temperature Suction Piping Zone Name
-    ,                        !- Sum UA Suction Piping for Low Temperature Loads
-    ,                        !- Low Temperature Suction Piping Zone Name
-    TransRefrigSys;          !- End-Use Subcategory
-```
-
-
-
-### Refrigeration Transcritical System Outputs
-
-* Zone,Average, Refrigeration Transcritical System Total High Pressure Compressor Electric Power [W]
-
-* Zone,Sum, Refrigeration Transcritical System Total High Pressure Compressor Electric Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System Low Pressure Compressor Electric Power [W]
-
-* Zone,Sum, Refrigeration Transcritical System Low Pressure Compressor Electric Energy [J]
-
-* Zone,Sum, Refrigeration Transcritical System Total Compressor Electric Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System Average COP [W/W]
-
-* Zone,Average, Refrigeration Transcritical System Medium Temperature Cases and Walk Ins Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Transcritical System Medium Temperature Cases and Walk Ins Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System Low Temperature Cases and Walk Ins Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Transcritical System Low Temperature Cases and Walk Ins Heat Transfer Energy [J]
-
-* Zone,Sum, Refrigeration Transcritical System Total Cases and Walk Ins Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System Medium Temperature Suction Pipe Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Transcritical System Medium Temperature Suction Pipe Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System Low Temperature Suction Pipe Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Transcritical System Low Temperature Suction Pipe Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System High Pressure Compressor Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Transcritical System High Pressure Compressor Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System Low Pressure Compressor Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Transcritical System Low Pressure Compressor Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System Net Rejected Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Transcritical System Net Rejected Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System Estimated Refrigerant Inventory Mass [kg]
-
-* Zone,Average, Refrigeration Transcritical System Refrigerant Mass Flow Rate [kg/s]
-
-* Zone,Average, Refrigeration Transcritical System Medium Temperature Evaporating Temperature [C]
-
-* Zone,Average, Refrigeration Transcritical System Medium Temperature Suction Temperature [C]
-
-* Zone,Average, Refrigeration Transcritical System Low Temperature Evaporating Temperature [C]
-
-* Zone,Average, Refrigeration Transcritical System Low Temperature Suction Temperature [C]
-
-
-
-#### Refrigeration Transcritical System Total High Pressure Compressor Electric Power [W]
-
-This output is the total electric power input to the system’s high pressure compressor(s) in Watts.
-
-#### Refrigeration Transcritical System Total High Pressure Compressor Electric Energy [J]
-
-This is the electricity consumption of the system’s high pressure compressor(s) in Joules for the timestep being reported.  The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Transcritical System Low Pressure Compressor Electric Power [W]
-
-This output is the total electric power input to the system’s low pressure compressor(s) in Watts.
-
-#### Refrigeration Transcritical System Low Pressure Compressor Electric Energy [J]
-
-This is the electricity consumption of the system’s low pressure compressor(s) in Joules for the timestep being reported.  The individual consumption for each compressor is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Transcritical System Total Compressor Electric Energy [J]
-
-This output is the total electric power input to all of the system’s compressor(s) in Watts.
-
-#### Refrigeration Transcritical System Average COP [W/W]
-
-This output is the system average compressor COP, which is the total refrigeration effect divided by the total power to all of the compressors.
-
-#### Refrigeration Transcritical System Medium Temperature Cases and Walk Ins Heat Transfer Rate [W]
-
-This output is the total heat transfer rate from the medium temperature refrigerated cases and walk-ins served directly by this system in Watts.  It is the sum of all of the heat transfer rates for the medium temperature refrigerated cases and walk-ins that are connected directly to this system.
-
-#### Refrigeration Transcritical System Medium Temperature Cases and Walk Ins Heat Transfer Energy [J]
-
-This output is the total heat transfer energy from the medium temperature refrigerated cases and walk-ins served directly by this system in Joules. It is the sum of all of the heat transferred for the medium temperature refrigerated cases and walk-ins that are connected directly to this system.
-
-#### Refrigeration Transcritical System Low Temperature Cases and Walk Ins Heat Transfer Rate [W]
-
-This output is the total heat transfer rate from the low temperature refrigerated cases and walk-ins served directly by this system in Watts.  It is the sum of all of the heat transfer rates for the low temperature refrigerated cases and walk-ins that are connected directly to this system.
-
-#### Refrigeration Transcritical System Low Temperature Cases and Walk Ins Heat Transfer Energy [J]
-
-This output is the total heat transfer energy from the low temperature refrigerated cases and walk-ins served directly by this system in Joules. It is the sum of all of the heat transferred for the low temperature refrigerated cases and walk-ins that are connected directly to this system.
-
-#### Refrigeration Transcritical System Total Cases and Walk Ins Heat Transfer Energy [J]
-
-This output is the total heat transfer energy from all the low- and medium-temperature refrigerated cases and walk-ins served directly by this system in Joules. It is the sum of all of the heat transferred for all the refrigerated cases and walk-ins that are connected directly to this system.
-
-#### Refrigeration Transcritical System Medium Temperature Suction Pipe Heat Transfer Rate [W]
-
-This output is the total heat transfer rate for the medium-temperature suction piping served by this system in Watts.  Note this is an optional input, and is only available if the user has described the medium-temperature suction piping heat gain characteristics in the input.
-
-#### Refrigeration Transcritical System Medium Temperature Suction Pipe Heat Transfer Energy [J]
-
-This output is the total heat transfer rate for the medium-temperature suction piping served by this system in Watts.  Note this is an optional input, and is only available if the user has described the medium-temperature suction piping heat gain characteristics in the input.
-
-#### Refrigeration Transcritical System Low Temperature Suction Pipe Heat Transfer Rate [W]
-
-This output is the total heat transfer rate for the low-temperature suction piping served by this system in Watts.  Note this is an optional input, and is only available if the user has described the low-temperature suction piping heat gain characteristics in the input.
-
-#### Refrigeration Transcritical System Low Temperature Suction Pipe Heat Transfer Energy [J]
-
-This output is the total heat transfer rate for the low-temperature suction piping served by this system in Watts.  Note this is an optional input, and is only available if the user has described the low-temperature suction piping heat gain characteristics in the input.
-
-#### Refrigeration Transcritical System High Pressure Compressor Heat Transfer Rate [W]
-
-This output is the total heat transfer rate of the high pressure Compressors in Watts.  It is the sum of all of the heat transfer rates for the low- and medium-temperature refrigerated cases and walk-ins as well as the low pressure compressors that are cooled by this system.  This value does not include compressor or condenser fan heat.  If specified as in input value, the suction pipe heat gains are included in this value.
-
-#### Refrigeration Transcritical System High Pressure Compressor Heat Transfer Energy [J]
-
-This is the total heat transfer of the high pressure compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Transcritical System Low Pressure Compressor Heat Transfer Rate [W]
-
-This output is the total heat transfer rate of the low pressure Compressors in Watts.  It is the sum of all of the heat transfer rates for the low temperature refrigerated cases and walk-ins that are cooled by this system.  This value does not include compressor or condenser fan heat.  If specified as in input value, the suction pipe heat gains are included in this value.
-
-#### Refrigeration Transcritical System Low Pressure Compressor Heat Transfer Energy [J]
-
-This is the total heat transfer of the low pressure compressors in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Transcritical System Net Rejected Heat Transfer Rate [W]
-
-This output is the total heat rejected by this system to the system gas cooler in Watts.  It does not include system heat rejection that has been recovered for useful purposes.
-
-#### Refrigeration Transcritical System Net Rejected Heat Transfer Energy [J]
-
-This output is the total heat rejected by this system to the system gas cooler in Joules for the timestep being reported.  It does not include system heat rejection that has been recovered for useful purposes.
-
-#### Refrigeration Transcritical System Estimated Refrigerant Inventory Mass [kg]
-
-This output is the sum of the input refrigerant inventory values for the gas cooler, receiver, cases, and liquid pipes that are a part of this system.
-
-#### Refrigeration Transcritical System Refrigerant Mass Flow Rate [kg/s]
-
-This output is the calculated refrigerant mass flow rate through the high pressure compressors for this system.
-
-#### Refrigeration Transcritical System Medium Temperature Evaporating Temperature [C]
-
-This is the saturated evaporating temperature for the medium temperature loads.
-
-#### Refrigeration Transcritical System Medium Temperature Suction Temperature [C]
-
-This is the temperature at the high pressure compressor inlet including superheat after the display cases and superheat from the suction line heat exchanger.
-
-#### Refrigeration Transcritical System Low Temperature Evaporating Temperature [C]
-
-This is the saturated evaporating temperature for the low-temperature loads.
-
-#### Refrigeration Transcritical System Low Temperature Suction Temperature [C]
-
-This is the temperature at the low pressure compressor inlet including superheat after the display cases.
-
-### Refrigeration:Compressor
-
-The compressors are described here using manufacturer’s data for curves that provide the efficiency, cooling capacity, and power consumption.  The corresponding rated values for cycle superheat and subcooling are also required.
-
-**A dataset has been provided containing the compressor rating data, including the performance curve inputs, for a large number of compressors.  See RefrigerationCompressorCurves.idf.**
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a compressor. Any reference to this compressor by another object will use this name.
-
-#### Field: Refrigeration Compressor Power Curve Name
-
-This required field provides the name of the curve object that describes the compressor power as a function of the evaporating and condensing temperatures, as specified in ARI 540. The curve is of the bicubic form(ref: Curve:Bicubic).  However, the input order for the Energy Plus bicubic curve does not match the ARI 540 standard order. When this curve is entered, the user should use the following assignments:
-
-N1 is ARI C1 and N2 is ARI C2.
-
-N3 is ARI C4 and N4 is ARI C3.
-
-N5 is ARI C6 and N6 is ARI C5,
-
-N7 is ARI C7.
-
-N8 is ARI C10, N9 is ARI C8, and N10 is ARI C9.
-
-N11 is the Minimum evaporating temperature and N12 is the Maximum evaporating temperature.
-
-N13 is the the Minimum condensing temperature and N14 is the Maximum condensing temperature
-
-#### Field: Refrigeration Compressor Capacity Curve Name
-
-This required field provides the name of the curve object that describes the compressor cooling capacity as a function of the evaporating and condensing temperatures, as specified in ARI 540. The curve is of the bicubic form(ref: Curve:Bicubic).  However, the input order for the Energy Plus bicubic curve does not match the ARI 540 standard order. When this curve is entered, the user should use the following assignments:
-
-N1 is ARI C1 and N2 is ARI C2.
-
-N3 is ARI C4 and N4 is ARI C3.
-
-N5 is ARI C6 and N6 is ARI C5,
-
-N7 is ARI C7.
-
-N8 is ARI C10, N9 is ARI C8, and N10 is ARI C9.
-
-N11 is the Minimum evaporating temperature and N12 is Maximum evaporating temperature.
-
-N13 is the Minimum condensing temperature and N14 is the Maximum condensing temperature
-
-#### Field: Rated Superheat
-
-Some manufacturers specify a constant return gas temperature while others specify a constant superheat (the difference between the saturated evaporating temperature and the actual return gas temperature). Use this field for compressors that provide their rated superheat. (Do NOT use both this field and the Rated Return Gas Temperature field.) The rated superheat is specified in units of delta C.
-
-#### Field: Rated Return Gas Temperature
-
-Some manufacturers specify a constant return gas temperature ( which may also be called the Rated Suction Temperature) while others specify a constant superheat.  Use this field for compressors that provide their rated return gas temperature. (Do NOT use both this field and the Rated Superheat field.) The rated return gas temperature is specified in units of C.
-
-#### Field: Rated Liquid Temperature
-
-Some compressor manufactures rate their equipment according to a constant subcooling (the difference between the saturated condensing temperature and the actual liquid temperature entering the thermal expansion valve before the refrigeration load). Other manufacturers specify a constant liquid temperature.Use this field if the manufacturer specifies the rated liquid temperature.  (Do NOT use both this field and the Rated Subcooling field.) The units for this field are degrees C.
-
-#### Field: Rated Subcooling
-
-Some compressor manufactures rate their equipment according to a constant subcooling (the difference between the saturated condensing temperature and the actual liquid temperature entering the thermal expansion valve before the refrigeration load). Other manufacturers specify a constant liquid temperature.Use this field if the manufacturer specifies the rated subcooling.  (Do NOT use both this field and the Rated Liquid Temperature field.) The units for this field are delta C.
-
-#### Field: End-Use Subcategory
-
-This field allows the specification of a user-defined end-use subcategory (e.g., "Low Temperature System"). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the "General" end-use subcategory.
-
-
-
-
-The following is an example input for a refrigeration compressor.
-
-```idf
-Refrigeration:Compressor,
-    CompressorA,             !- Name
-    PowerCurveCompA,         !- Refrigeration Compressor Power Curve Name
-    CapCurveCompA,           !- Refrigeration Compressor Capacity Curve Name
-    10.0,                    ! – Rated Superheat {delta C}
-    ,                        !- Rated Return Gas Temperature {C}
-    ,                        ! – Rated Liquid Temperature{C}
-    15.0,                    !- Rated Subcooling {delta C}
-    MedTempRefrig;           !- End-Use Subcategory
-```
-
-### Refrigeration Compressor Outputs
-
-THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE CASES AND/OR WALKINS:
-
-* Zone,Average,Refrigeration Compressor Electric Power [W]
-
-* Zone,Sum,Refrigeration Compressor Electric Energy [J]
-
-* Zone,Average,Refrigeration Compressor Heat Transfer Rate [W]
-
-* Zone,Sum,Refrigeration Compressor Heat Transfer Energy [J]
-
-* Zone,Sum,Refrigeration Compressor Run Time Fraction []
-
-THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE AIR CHILLERS:
-
-* HVAC,Average,Refrigeration Air Chiller System Compressor Electric Power [W]
-
-* HVAC,Sum,Refrigeration Air Chiller System Compressor Electric Energy [J]
-
-* HVAC,Average,Refrigeration Air Chiller System Compressor Heat Transfer Rate [W]
-
-* HVAC,Sum,Refrigeration Air Chiller System Compressor Heat Transfer Energy [J]
-
-* HVAC,Average,Refrigeration Chiller Compressor Run TimeFraction []
-
-#### THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE CASES AND/OR WALKINS
-
-#### Refrigeration Compressor Electric Power [W]
-
-This output is the electric power input to the compressor in Watts.
-
-#### Refrigeration Compressor Electric Energy [J]
-
-This is the electric energy consumed by the compressor in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Compressor Heat Transfer Rate [W]
-
-This output is the heat removed from the refrigerated cases by the compressor in Watts.
-
-#### Refrigeration Compressor  Heat Transfer Energy [J]
-
-This is the heat removed from the refrigerated cases by the compressor in Joules for the timestep being reported.
-
-#### Refrigeration Compressor Run Time  Fraction []
-
-This is the fraction of the time step when the compressor ran to meet the load.  It is a value between 0.0 and 1.0.
-
-#### THE FOLLOWING OUTPUTS ARE AVAILABLE FOR SYSTEMS THAT SERVE AIR CHILLERS
-
-#### Refrigeration Air Chiller System Compressor Electric Power [W]
-
-This output is the electric power input to the compressor in Watts.
-
-#### Refrigeration Air Chiller System Compressor Electric Energy [J]
-
-This is the electric energy consumed by the compressor in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller System Compressor Heat Transfer Rate [W]
-
-This output is the heat removed from the refrigerated cases by the compressor in Watts.
-
-#### Refrigeration Air Chiller System Compressor Heat Transfer Energy [J]
-
-This is the heat removed from the refrigerated cases by the compressor in Joules for the timestep being reported.
-
-#### Refrigeration Chiller Compressor Run Time  Fraction []
-
-This is the fraction of the time step when the compressor ran to meet the load.  It is a value between 0.0 and 1.0.
-
-### Refrigeration:CompressorList
-
-This object provides a list of all the compressors included within a single refrigeration system (Ref: Refrigeration:System). Each list must contain at least one compressor. The order in which the individual compressors are listed here will be the order in which the compressors are dispatched to meet the system load.  That is, at very low loads, only compressor \#1 will be operating.  As the load increases, the first two compressors will be operating, and so on. This list is extensible.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a compressor list. Any reference to this compressor list by another object will use this name. The compressor list cannot have the same name as any individual compressor.
-
-#### Field: Refrigeration Compressor &lt;x&gt; Name
-
-Identifies a particular compressor that works in conjunction with the other compressors on this list to provides cooling to a single refrigeration system. The name will be validated against the compressor names (ref: Refrigeration:Compressor) in the input file. Up to 20 are available in the IDD; this object is extensible.
-
-
-
-The following is an example input for a compressor list.
-
-```idf
-Refrigeration:CompressorList,
-    MediumTempCompressorlist, !- Refrigeration Compressor List Name
-    CompressorA,             !- Refrigeration Compressor Name \#1
-    CompressorB,             !- Refrigeration Compressor Name \#2
-    CompressorC;             !- Refrigeration Compressor Name \#3
-```
-
-
-### Refrigeration:Subcooler
-
-Two types of subcoolers are modeled by the detailed refrigeration system.  As described in the Engineering Reference, the liquid suction heat exchanger uses cool suction gas to subcool the hot condensate after it leaves the condenser and before it reaches the thermal expansion valve.  For the liquid suction heat exchanger, both the source and sink of energy are located within the same refrigeration system.  In contrast, a mechanical subcooler is used to transfer cooling capacity from one refrigeration system to another. The mechanical subcooler is listed as a part of the system for which the condensate is cooled.  However, the input data for the mechanical subcooler includes a field that identifies the system that provides the cooling capacity.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a subcooler. Any reference to this subcooler by another object will use this name.
-
-#### Field: Subcooler Type
-
-The type of subcooler. Valid choices are Mechanical and LiquidSuction.  If the field is blank, the default will be LiquidSuction.
-
-#### Field: Liquid Suction Design Subcooling Temperature Difference
-
-This numeric field is the design subcooling temperature difference (DeltaC) for a liquid suction heat exchanger and should be blank for a mechanical subcooler.
-
-#### Field: Design Liquid Inlet Temperature
-
-This numeric field is the design inlet temperature (C) for the hot liquid entering a liquid suction heat exchanger and should be blank for a mechanical subcooler.
-
-#### Field: Design Vapor Inlet Temperature
-
-This numeric field is the design inlet temperature (C) for the cool vapor entering a liquid suction heat exchanger and should be blank for a mechanical subcooler.
-
-#### Field: Capacity-Providing System
-
-This field is the name of the refrigeration system object that provides the cooling capacity for the mechanical subcooler (ref: Refrigeration:System Name). This field should be blank for a liquid suction heat exchanger.
-
-#### Field: Outlet Control Temperature
-
-This numeric field is the controlled outlet temperature (C) for subcooled liquid exiting a mechanical subcooler. This field should be blank for a liquid suction heat exchanger.
-
-The following is example input for both liquid suction and mechanical subcoolers.
-
-```idf
-REFRIGERATION:SUBCOOLER,
-       SampleLSHx,          !Subcooler Name
-       LiquidSuction,             !subcooler type
-       6,                   !design liquid suction subcooling {deltaC}
-       16,                  !design inlet temperature on liquid side {C}
-       0,                   !design inlet temperature on vapor side {C}
-       ,                    !Refrigeration System Detailed Name providing cooling capacity
-       ;                    !Control Temperature Out for subcooled liquid {C}
-```
-
-
-
-! Mechanical Subcooler (uses Med Temp System to cool low temp liquid to 10C)
-
-```idf
-  REFRIGERATION:SUBCOOLER,
-       SampleMSC,           !Subcooler Name
-       Mechanical,          !subcooler type
-       ,                    !design liquid suction subcooling {C}
-       ,                    !design inlet temperature on liquid side {C}
-       ,                    !design inlet temperature on vapor side {C}
-       MediumTempSystem,    !Refrigeration System Detailed Name providing cooling capacity
-       10;                  !Control Temperature Out for subcooled liquid {C}
-```
-
-
-### Refrigeration Subcooler Outputs
-
-FOR SUBCOOLERS ON SYSTEMS SERVING CASES AND/OR WALKINS:
-
-* Zone,Average, Refrigeration System Mechanical Subcooler Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration System Mechanical Subcooler Heat Transfer Energy [J]
-
-FOR SUBCOOLERS ON SYSTEMS SERVING AIR CHILLERS:
-
-* Zone,Average, Refrigeration Air Chiller System Mechanical Subcooler Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Air Chiller System Mechanical Subcooler Heat Transfer Energy [J]
-
-#### FOR SUBCOOLERS ON SYSTEMS SERVING CASES AND/OR WALKINS:
-
-#### Refrigeration System Mechanical Subcooler Heat Transfer Rate [W]
-
-This output is the cooling energy transferred from one system’s compressor group to the refrigerant leaving the condenser for another refrigeration system in Watts.
-
-#### Refrigeration System Mechanical Subcooler Heat Transfer Energy [J]
-
-This output is the cooling energy transferred from one system’s compressor group to the refrigerant leaving the condenser for another refrigeration system in Joules.
-
-#### FOR SUBCOOLERS ON SYSTEMS SERVING AIR CHILLERS
-
-#### Refrigeration Air Chiller System Mechanical Subcooler Heat Transfer Rate [W]
-
-This output is the cooling energy transferred from one system’s compressor group to the refrigerant leaving the condenser for another refrigeration system in Watts.
-
-#### Refrigeration Air Chiller System Mechanical Subcooler Heat Transfer Energy [J]
-
-This output is the cooling energy transferred from one system’s compressor group to the refrigerant leaving the condenser for another refrigeration system in Joules.
-
-
-
-### Refrigeration:Condenser:AirCooled
-
-The refrigeration system requires a single condenser to reject the system heat.  The air cooled condenser object is one of four options for this condenser. In an air-cooled condenser, the total heat of rejection is characterized by a linear relationship between the difference between the inlet air (usually the outside drybulb) and condensing temperatures. This curve is commonly found in the condenser manufacturers’ literature. This rating curve, which corresponds to ARI 460 standards, also has an associated rated value for subcooling that should be entered. The rated condenser fan power and fan speed control type must be specified. If the condenser is not at ground level, the user may specify an air inlet node name (ref: OutdoorAir:Node name). If the condenser is located inside a conditioned zone, the zone name may be specified(ref: bbbZoneNamebbb). Optional input is provided to help the user compare refrigerant inventories for different systems.  These inputs represent the design values for the refrigerant inventory within the condenser, within a receiver beneath the condenser, and in the liquid pipes between the condenser and the refrigerated cases.
-
-#### Field: Name
-
-Identifies a particular condenser that rejects heat for a one or more refrigeration system(s). The name must be unique and will be validated against all the condenser names (ref: Refrigeration:Condenser:\*) in the input file, including names used for evaporative-cooled, water-cooled, and cascade-cooled condensers.
-
-#### Field: Rated Effective Total Heat Rejection Rate Curve Name
-
-This field is the name of a curve object defining the condenser heat rejection as a function of the difference between the condensing and entering air temperatures. The curve should be linear (Curve:Linear). See the Engineering Reference for more discussion on the curve coefficients.
-
-#### Field: Rated Subcooling Temperature Difference
-
-This numeric field specifies the rated subcooling (DeltaC) specified by the manufacturer, consistent with the heat rejection curve rating data.
-
-#### Field: Condenser Fan Speed Control Type
-
-The type of fan speed control used by the condenser fan. Valid choices are **Fixed**, **FixedLinear,** **VariableSpeed**, and **TwoSpeed**.  If the field is blank, **Fixed** will be used. See the Engineering Reference for a discussion of this option’s effect on fan energy consumption.
-
-#### Field: Rated Fan Power
-
-This numeric field specifies the rated fan power (W) specified by the manufacturer, under standard rating conditions.
-
-#### Field: Minimum Fan Air Flow Ratio
-
-Fan controls often include a minimum air flow ratio to avoid overheating the fan motor or for other reasons. This numeric field should be between 0. and 1. and has a default value of 0.2**.**
-
-#### Field: Air Inlet Node Name or Zone Name
-
-This optional alpha field contains the name of the node from which the condenser draws its outdoor air or the name of the conditioned zone where the condenser is located. If this field is left blank, the outdoor air drybulb temperature entering the condenser is taken directly from the weather data. If this field is not blank and an outdoor air node name is entered, this node name must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data. If a zone name is entered, the temperature of that zone is used.
-
-#### Field: End-Use Subcategory
-
-This field allows the specification of a user-defined end-use subcategory (e.g., "Low Temperature Rack"). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the "General" end-use subcategory.
-
-#### Field: Condenser Refrigerant Operating Charge Inventory
-
-This numeric field specifies the amount of refrigerant present within the condenser (kg) specified by the manufacturer, under standard rating conditions.
-
-#### Field: Condensate Receiver Refrigerant Inventory
-
-This numeric field specifies the amount of refrigerant present within the condensate receiver (kg) specified by the manufacturer or system designer, under standard rating conditions.
-
-#### Field: Condensate Piping Refrigerant Inventory
-
-This numeric field specifies the amount of refrigerant present within the condensate piping (kg) specified by the system designer, under standard rating conditions.
-
-The following is an example input for an air-cooled condenser.
-
-```idf
-Refrigeration:Condenser:AirCooled,
-    MediumTempCondenser,     !- Name of condenser
-    MediumTempCondenserHRCurve, !-name of condenser heat of rejection curve, linear
-    0.,                      ! Rated subcooling {deltaC}
-    VariableSpeed,           ! Fan speed control type
-    4000.,                   ! Design condenser fan power {W}
-    0.25,                    !Minimum air flow fraction through condenser fan {dimensionless}
-    Refrigeration MediumTempSystem CondenserNode,  !- Condenser Air Inlet Node Name or Zone Name
-    MediumTempRefrig;        !- End-Use Subcategory
-```
-
-### Refrigeration Condenser (AirCooled) Outputs
-
-FOR CONDENSERS COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
-
-* Zone,Average, Refrigeration System Condenser Fan Electric Power [W]
-
-* Zone, Sum, Refrigeration System Condenser Fan Electric Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Total Recovered Heat Transfer Rate [W] Zone, Sum, Refrigeration System Condenser Total Recovered Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Heat Recovered for Non-Refrigeration Purposes Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Defrost Recovered Heat Transfer Energy [J]
-
-FOR CONDENSERS COOLING SYSTEMS SERVING AIR CHILLERS:
-
-* HVAC,Average, Refrigeration System Condenser Fan Electric Power [W]
-
-* HVAC, Sum, Refrigeration System Condenser Fan Electric Consumption [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate [W] HVAC, Sum, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Energy [J]
-
-#### FOR CONDENSERS ON SYSTEMS SERVING CASES AND/OR WALKINS:
-
-#### Refrigeration System Condenser Fan Electric Power [W]
-
-This output is the electric input to the system’s condenser fan(s) in Watts.
-
-#### Refrigeration System Condenser Fan Electric Consumption [J]
-
-This is the electricity consumption of the system’s condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration System Condenser Heat Transfer Rate [W]
-
-This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration load minus any heat recovered for defrost or other purposes).
-
-#### Refrigeration System Condenser Heat Transfer Energy [J]
-
-This is the total heat energy flowing across the condenser for the timestep being reported  (i.e., compressor energy and refrigeration load minus any heat recovered for defrost or other purposes).
-
-#### Refrigeration System Condenser Total Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the condenser inlet flow for all purposes including defrost and water or air heating.
-
-#### Refrigeration System Condenser Total Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser inlet flow for all purposes including defrost and water or air heating for the timestep being reported.
-
-#### Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate  [W]
-
-This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating.
-
-#### Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating for the timestep being reported.
-
-#### Refrigeration System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system.
-
-#### Refrigeration System Condenser Defrost Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
-
-#### FOR CONDENSERS ON SYSTEMS SERVING AIR CHILLERS:
-
-#### Refrigeration Air Chiller System Condenser Fan Electric Power [W]
-
-This output is the electric input to the system’s condenser fan(s) in Watts.
-
-#### Refrigeration Air Chiller System Condenser Fan Electric Energy [J]
-
-This is the electricity consumption of the system’s condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller System Condenser Heat Transfer Rate [W]
-
-This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration load minus any heat recovered for defrost or other purposes).
-
-#### Refrigeration Air Chiller System Condenser Heat Transfer Energy [J]
-
-This is the total heat energy flowing across the condenser for the timestep being reported  (i.e., compressor energy and refrigeration load minus any heat recovered for defrost or other purposes).
-
-#### Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the condenser inlet flow for all purposes including defrost and water or air heating.
-
-#### Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser inlet flow for all purposes including defrost and water or air heating for the timestep being reported.
-
-#### Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate  [W]
-
-This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating.
-
-#### Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating for the timestep being reported.
-
-#### Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system.
-
-#### Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
-
-### Refrigeration:Condenser:EvaporativeCooled
-
-Each refrigeration system requires a single condenser.  The evaporative cooled condenser object is one of four options for this condenser. In an evaporative-cooled condenser, the total heat of rejection is characterized by a four-factor relationship between the condensing temperature and the difference between the outside wetbulb and condensing temperatures. This curve must be developed by regression from the condenser manufacturers’ literature. This rating curve, which is based upon rated data taken according to ARI 460 standards, also has an associated rated value for subcooling that should be entered. The rated condenser fan power and fan speed control type must be specified. If the condenser is not at ground level, the user may specify an air inlet node name (ref: OutdoorAir:Node name). Optional input is provided to help the user compare refrigerant inventories for different systems.  These input represent the design values for the refrigerant inventory within the condenser, within a receiver beneath the condenser, and in the liquid pipes between the condenser and the refrigerated cases.
-
-Additional inputs are needed for basin heater parameters, water pump power, and water source. An evaporative cooling availability schedule is available.
-
-#### Field: Name
-
-Identifies a particular condenser that rejects heat for a one or more refrigeration system(s). The name must be unique and will be validated against all the condenser names (ref: Refrigeration:Condenser:\*) in the input file, including names used for air-cooled, water-cooled and cascade-cooled condensers.
-
-#### Field: Rated Effective Total Heat Rejection Rate
-
-This numeric field should be the rated heat rejection effect (W) at standard rating conditions per ARI 490.  Be sure the rating corresponds to the correct refrigerant.
-
-#### Field: Rated Subcooling Temperature Difference
-
-This numeric field specifies the rated subcooling (DeltaC) specified by the manufacturer, consistent with the rated value for total heat rejection.
-
-#### Field: Fan Speed Control Type
-
-The type of fan speed control used by the condenser fan. Valid choices are **Fixed**, **FixedLinear**, **VariableSpeed**, and **TwoSpeed**.  If the field is blank, **Fixed** will be used. See the Engineering Reference for a discussion of this option’s effect on fan energy consumption.
-
-#### Field: Rated Fan Power
-
-This numeric field specifies the rated fan power (W) specified by the manufacturer, under standard rating conditions.
-
-#### Field: Minimum Fan Air Flow Ratio
-
-Fan controls often include a minimum air flow ratio to avoid overheating the fan motor or for other reasons. This numeric field has a minimum value of 0. and a default value of 0.2.
-
-#### Field: Approach Temperature Constant Term
-
-As described in the Engineering Reference (ref Refrigeration:Condenser:Evaporative), the heat rejection capacity factor is specified according to the form (where Twetbulb and Tcondense are in C):
-
-Tcondense=A1 + A2(hrcf) + A3/(hrcf) + (1 + A4)(Twb)
-
-This numeric field is the value for A1 and has a default value of 6.63, a minimum of 0. and a maximum of 20. (C)
-
-#### Field: Approach Temperature Coefficient 2
-
-As described in the Engineering Reference (ref Refrigeration:Condenser:Evaporative), the heat rejection capacity factor is specified according to the form (where Twetbulb and Tcondense are in C):
-
-Tcondense=A1 + A2(hrcf) + A3/(hrcf) + (1 + A4)(Twb)
-
-This numeric field is the value for A2 and has a default value of 0.468, a minimum of 0, and a maximum of 20 (C).
-
-#### Field: Approach Temperature Coefficient 3
-
-As described in the Engineering Reference (ref Refrigeration:Condenser:Evaporative), the heat rejection capacity factor is specified according to the form (where Twetbulb and Tcondense are in C):
-
-Tcondense =A1 + A2(hrcf) + A3/(hrcf) +(1 + A4)(Twb)
-
-This numeric field is the value for A3 and has a default value of 17.93, a minimum of 0, and a maximum of 30 (C).
-
-#### Field: Approach Temperature Coefficient 4
-
-As described in the Engineering Reference (ref Refrigeration:Condenser:Evaporative), the heat rejection capacity factor is specified according to the form (where Twetbulb and Tcondense are in C):
-
-Tcondense =A1 + A2(hrcf) + A3/(hrcf) + (1 + A4)(Twb)
-
-This numeric field is the value for A4 and has a default value of -0.322, a minimum of -20., and a maximum of 20 (dimensionless).
-
-#### Field: Minimum Capacity Factor
-
-This numeric field is the minimum heat rejection capacity factor in the manufacturer’s data used to develop the equation described in the preceding four fields. The default value is 0.5.
-
-#### Field: Maximum Capacity Factor
-
-This numeric field is the maximum heat rejection capacity factor in the manufacturer’s data used to develop the equation described in the preceding four fields. The default value is 5.0.
-
-#### Field: Air Inlet Node Name
-
-This optional alpha field contains the name of the node from which the condenser draws its outdoor air. If this field is left blank, the outdoor air drybulb temperature entering the condenser is taken directly from the weather data. If this field is not blank, this node name must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
-
-#### Field: Rated Air Flow Rate
-
-The air volume flow rate, in m<sup>3</sup>per second, entering the evaporative condenser. This value is used to calculate the amount of water evaporated when evaporatively cooling the condenser inlet air. The value for this field must be greater than zero. This input field is also autocalculatable, equivalent to 0.000144 m<sup>3</sup>/s per watt of total cooling capacity [850 cfm/ton] where the total cooling capacity is the total heat of rejection.
-
-#### Field: Basin Heater Capacity
-
-This field defines the power level of the basin heater, if applicable, used to avoid water freezing in an outdoor evaporative cooler basin. This numeric field contains the capacity of the electric basin heater in Watts per degree C. This field is used in conjunction with the Basin Heater Set Point Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the dry-bulb temperature of the condenser coil inlet air. The basin heater only operates when the condenser fan is off (i.e., no compressor heat rejection). The basin heater capacity must be greater than or equal to zero, with a default value of 200 W/C if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (°C) for the basin heater described in the previous field. The basin heater is active when the outdoor air dry-bulb temperature falls below this set point temperature, as long as the condenser fan is off. The default value is 2°C if this field is left blank.
-
-#### Field: Rated Water Pump Power
-
-The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The value for this field must be greater than or equal to 0, with a default value of 1000 Watts if this field is left blank. This input field is also autocalculatable, equivalent to 0.004266 W per Watt [15 W/ton] of total cooling capacity.
-
-#### Field: Evaporative Water Supply Tank Name
-
-This field is used to define where the condenser obtains water used for evaporative cooling. If this field is left blank, the unit will obtain water directly from the mains (Ref. Water Mains Temperatures). If the name of a Water Storage Tank object is used here, then the unit will obtain its water from that tank.
-
-#### Field: Evaporative Condenser Availability Schedule Name
-
-For evaporative cooled condensers, the name of the optional schedule (Ref: Schedule) that specifies the time periods that evaporative cooling is available/unavailable. In some colder climates, evaporative cooling is periodically discontinued and the basin sumps drained to avoid freezing and to avoid ice formation on the condenser. In these times, the condenser runs as a typical dry air cooled condenser, and related evaporative cooling systems (e.g., water pump, basin heaters) do not operate. Use of this optional schedule permits modeling of planned, seasonal interruptions of evaporative cooling. All schedule values must be greater than or equal to zero. Typically, an ON/OFF schedule type is used with values being either 0 or 1. A schedule value of 1 indicates that evaporative cooling is available during the defined time period, and a value of 0 denotes that evaporative cooling is not available during the defined time period. If the schedule name is omitted (blank), then the model assumes that evaporative cooling of the condenser is available for the entire simulation period. Note: the use of this schedule is the correct way to model an evaporative condenser in a climate subject to freezing weather.  However, because some users will take a single model description and run it for a multiple climates, the code also includes an automatic switch from wet to dry operation, as described in the Engineering Reference.
-
-#### Field: End-Use Subcategory
-
-This field allows the specification of a user-defined end-use subcategory (e.g., "Low Temperature Rack"). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the "General" end-use subcategory.
-
-#### Field: Condenser Refrigerant Operating Charge Inventory
-
-This numeric field specifies the amount of refrigerant present within the condenser (kg) specified by the manufacturer, under standard rating conditions.
-
-#### Field: Condensate Receiver Refrigerant Inventory
-
-This numeric field specifies the amount of refrigerant present within the condensate receiver (kg) specified by the manufacturer or system designer, under standard rating conditions.
-
-#### Field: Condensate Piping Refrigerant Inventory
-
-This numeric field specifies the amount of refrigerant present within the condensate piping (kg) specified by the system designer, under standard rating conditions.
-
-
-
-The following is an example input for an evaporative condenser
-
-```idf
-Refrigeration:Condenser:EvaporativeCooled,
-    MedTempEvapCooledCondenser ,  !- Refrigeration Condenser Name
-    64800. ,                    !- Rated Total Heat Rejection Effect, {W}
-    0. ,                        !- Rated Subcooling
-    VariableSpeed ,             !- Condenser Fan Speed Control
-    746.,                       !- Rated Condenser Fan Power
-    0.25,                       !- Minimum air flow fraction through condenser fan {dimensionless}
-    6.63  ,                     !- Evaporative Condenser Approach Temp Const, {C}
-    0.468 ,                     !- Evaporative Condenser Approach Temp HRCF Cooefficient
-    17.93 ,                     !- Evaporative Condenser Approach Temp 1/hrcf coefficient
-    -0.322,                     !- Evaporative Condenser Approach Temp Twb coefficient {1/C}
-    0.6  ,                      !- Minimum Condenser Capacity Factor
-    4.8  ,                      !- Maximum Condenser Capacity Factor
-    Outside Air Inlet Node,     !- Condenser Air Inlet Node Name
-    1.79 ,                      !- Rated Air Flow Rate {m3/s}
-    66.7 ,                      !- Basin Heater Capacity {W/C}
-    1.0  ,                      !- Basin Heater Set Point Temperature {C}
-    250. ,                      !- Rated Water Pump Power {W}
-    EvapWaterStorageTank,       !- Evaporative Water Supply Tank Name
-    EvapCondAvail,              !- Evaporative Condenser Availability Schedule Name
-    ,                           !- End-UseSubcategory
-    21.9 ,                      !- Condenser Refrigerant Operating Charge {kg}
-    10.  ,                      !- Condensate Receiver Refrigerant Inventory
-    25. ;                       !- Condensate Piping Refrigerant Inventory
-```
-
-
-
-
-### Refrigeration Condenser (EvaporativeCooled) Outputs
-
-* Zone,Average, Refrigeration System Condenser Fan Electric Power [W]
-
-* Zone, Sum, Refrigeration System Condenser Fan Electric Consumption [J]
-
-FOR CONDENSERS COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
-
-* Zone,Average, Refrigeration System Condenser Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Total Recovered Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Total Recovered Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Defrost Recovered Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Pump Electric Power [W]
-
-* Zone, Sum, Refrigeration System Condenser Pump Electric Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Basin Heater Electric Power [W]
-
-* Zone, Sum, Refrigeration System Condenser Basin Heater Electric Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Evaporated Water Volume Flow Rate  [m3/s]
-
-* Zone, Sum, Refrigeration System Condenser Evaporated Water Volume [m3]
-
-FOR CONDENSERS COOLING SYSTEMS SERVING AIR CHILLERS:
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Pump Electric Power [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Pump Electric Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Basin Heater Electric Power [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Basin Heater Electric Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Evaporated Water Volume Flow Rate [m3/s]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Evaporated Water Volume [m3]
-
-#### FOR CONDENSERS ON SYSTEMS SERVING CASES AND/OR WALKINS:
-
-#### Refrigeration System Condenser Fan Electric Power [W]
-
-This output is the electric input to the system’s condenser fan(s) in Watts.
-
-#### Refrigeration System Condenser Fan Electric Energy [J]
-
-This is the electricity consumption of the system’s condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration System Condenser Heat Transfer Rate [W]
-
-This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
-
-#### Refrigeration System Condenser Heat Transfer Energy [J]
-
-This is the total heat energy flowing across the condenser for the timestep being reported.
-
-#### Refrigeration System Condenser Total Recovered Heat Transfer Rate  [W]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for any purpose.
-
-#### Refrigeration System Condenser Total Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for any purpose for the timestep being reported.
-
-#### Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate  [W]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for purposes such as water or air heating.
-
-#### Refrigeration System Condenser Heat Recovered for Non-Refrigeration Purposes Energy [J]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for purposes such as water or air heating for the timestep being reported.
-
-#### Refrigeration System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for defrost purposes within the refrigeration system..
-
-#### Refrigeration System Condenser Defrost Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
-
-#### Refrigeration System Condenser Pump Electric Power [W]
-
-This is the electrical power requirement in Watts for the timestep being reported for the water pump used with evaporative cooling of the condenser.
-
-#### Refrigeration System Condenser Pump Electric Energy [J]
-
-This is the electricity consumption in Joules of the water pump used with evaporative cooling of the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### Refrigeration System Condenser Basin Heater Electric Power [W]
-
-This is the electrical power requirement in Watts for the timestep being reported for the water heater in the basin of the evaporative system used to cool the condenser.
-
-#### Refrigeration System Condenser Basin Heater Electric Energy [J]
-
-This is the electricity consumption in Joules of the water heater used to prevent freezing of the evaporative cooling system for the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### Refrigeration System Condenser Evaporated Water Volume Flow Rate [m<sup>3</sup>/s]
-
-The volumetric flow rate in m<sup>3</sup>/s of water consumed while providing evaporative cooling of the condenser.
-
-#### Refrigeration System Condenser Evaporated Water Volume [m<sup>3</sup>]
-
-This is the water consumed by evaporation in m<sup>3</sup> while providing evaporative cooling of the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Water, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### FOR CONDENSERS ON SYSTEMS SERVING AIR CHILLERS:
-
-#### Refrigeration Air Chiller System Condenser Fan Electric Power [W]
-
-This output is the electric input to the system’s condenser fan(s) in Watts.
-
-#### Refrigeration Air Chiller System Condenser Fan Electric Energy [J]
-
-This is the electricity consumption of the system’s condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller System Condenser Heat Transfer Rate [W]
-
-This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
-
-#### Refrigeration Air Chiller System Condenser Heat Transfer Energy [J]
-
-This is the total heat energy flowing across the condenser for the timestep being reported.
-
-#### Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate  [W]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for any purpose.
-
-#### Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for any purpose for the timestep being reported.
-
-#### Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate  [W]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for purposes such as water or air heating.
-
-#### Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for purposes such as water or air heating for the timestep being reported.
-
-#### Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for defrost purposes within the refrigeration system.
-
-#### Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
-
-#### Refrigeration Air Chiller System Condenser Pump Electric Power [W]
-
-This is the electrical power requirement in Watts for the timestep being reported for the water pump used with evaporative cooling of the condenser.
-
-#### Refrigeration Air Chiller System Condenser Pump Electric Energy [J]
-
-This is the electricity consumption in Joules of the water pump used with evaporative cooling of the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller System Condenser Basin Heater Electric Power [W]
-
-This is the electrical power requirement in Watts for the timestep being reported for the water heater in the basin of the evaporative system used to cool the condenser.
-
-#### Refrigeration Air Chiller System Condenser Basin Heater Electric Energy [J]
-
-This is the electricity consumption in Joules of the water heater used to prevent freezing of the evaporative cooling system for the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller System Condenser Evaporated Water Volume Flow Rate [m3/s]
-
-The volumetric flow rate in m<sup>3</sup>/s of water consumed while providing evaporative cooling of the condenser.
-
-#### Refrigeration Air Chiller System Condenser Evaporated Water Volume [m3]
-
-This is the water consumed by evaporation in m<sup>3</sup> while providing evaporative cooling of the condenser for the timestep being reported. This output is also added to a meter with Resource Type = Water, End Use Key = Refrigeration, Group Key = Plant. Use of an optional subkey category is also available, with default to the General end-use subcategory (Ref. Output:Meter objects).
-
-
-
-### Refrigeration:Condenser:WaterCooled
-
-The refrigeration system requires a single condenser.  The water cooled condenser object is one of four options for this condenser. Manufacturer’s data is required for the rated total heat rejection, the rated condensing temperature, and the rated leaving liquid refrigerant temperature, all per ARI 450.  These values are used to calculate the subcooling included in the rated capacity. The inlet and outlet node names as well as the water outlet temperature schedule name are required.  Optional input is provided to help the user compare refrigerant inventories for different systems.  These input represent the design values for the refrigerant inventory within the condenser, within a receiver beneath the condenser, and in the liquid pipes between the condenser and the refrigerated cases.
-
-#### Field: Name
-
-Identifies a particular condenser that rejects heat for one or more refrigeration system(s). The name must be unique and will be validated against all the condenser names (ref: Refrigeration:Condenser) in the input file, including names used for air-cooled, evaporative-cooled, and cascade-cooled condensers.
-
-#### Field: Rated Effective Total Heat Rejection Rate
-
-This numeric field should be the rated heat rejection effect (W) at standard rating conditions per ARI 450.  Be sure the rating corresponds to the correct refrigerant.
-
-#### Field: Rated Condensing Temperature
-
-This numeric field provides the rated condensing temperature (C) corresponding to the rated heat rejection capacity.
-
-#### Field: Rated Subcooling Temperature Difference
-
-This numeric field provides the rated liquid refrigerant subcooling (DeltaC) corresponding to the rated heat rejection capacity. Note this is equal to the difference between the saturated condensing temperature and the leaving liquid refrigerant temperature.
-
-#### Field: Rated Water Inlet Temperature
-
-This numeric field provides the rated water inlet temperature (C) corresponding to the rated heat rejection capacity at the rated condensing temperature.
-
-#### Field: Water Inlet Node Name
-
-A node name for the water-side condenser inlet must be provided.
-
-#### Field: Water Outlet Node Name
-
-A node name for the water-side condenser outlet must be provided.
-
-#### Field: Water-Cooled Loop Flow Type
-
-The type of flow loop should be specified.  The two choices are **VariableFlow**, in which a Pump:VariableSpeed must be included in the plant loop, or **ConstantFlow**, in which the loop circuit has a constant flow rate, typically associated with a Pump:ConstandSpeed object.  If the flow type is VariableFlow, the flow needed to remove the condenser heat energy will be calculated and requested of the pump.  If the flow type is ConstantFlow, the outlet water temperature will be determined based on the fixed loop flow rate and heat energy to be removed.  The default type is VariableFlow. Refer to additional discussion in the Engineering Reference.
-
-#### Field: Water Outlet Temperature Schedule Name
-
-When the water-cooled loop flow type is “VariableFlow�, the name of a schedule (Ref: Schedule) that defines the desired condenser water outlet temperature must be provided.  The schedule may define an outlet temperature that varies through time.
-
-#### Field: Water Design Flow Rate
-
-When the water-cooled loop flow type is “ConstantFlow�, this is the design water flow rate in m<sup>3</sup>/s that will be requested initially.  This requested flow will be passed to the loop simulation, and resulting actual flow will be dependent upon supply system capabilities (e.g., pump capability).  The design flow rate must always be less than the maximum flow rate, defined below.
-
-#### Field: Water Maximum Flow Rate
-
-This numeric field is the maximum water flow rate in m<sup>3</sup>/s that will be allowed through the condenser.  When the loop flow type is Variable Flow, if the calculated flow rate is higher than the maximum flow rate, an error message will be generated, and the flow rate will be reset to the maximum flow rate.
-
-#### Field: Maximum Water Outlet Temperature
-
-This numeric field specifies the maximum allowed water temperature in degrees C leaving the condenser. The default value is 55 degrees C.
-
-#### Field: Minimum Water Inlet Temperature
-
-This numeric field specifies the minimum allowed water temperature in degrees C entering the compressor rack condenser. The default value is 10 degrees C.  Refer to additional discussion in the Engineering Reference.
-
-#### Field: End-Use Subcategory
-
-This field allows the specification of a user-defined end-use subcategory (e.g., "Low Temperature System"). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the "General" end-use subcategory.
-
-#### Field: Condenser Refrigerant Operating Charge Inventory
-
-This numeric field specifies the amount of refrigerant present within the condenser (kg) specified by the manufacturer, under standard rating conditions.
-
-#### Field: Condensate Receiver Refrigerant Inventory
-
-This numeric field specifies the amount of refrigerant present within the condensate receiver (kg) specified by the manufacturer or system designer, under standard rating conditions.
-
-#### Field: Condensate Piping Refrigerant Inventory
-
-This numeric field specifies the amount of refrigerant present within the condensate piping (kg) specified by the system designer, under standard rating conditions.
-
-
-
-The following is an example input for a water cooled condenser.
-
-```idf
-Refrigeration:Condenser:WaterCooled,
-    MediumTempCondenser ,    !- Name
-    58000. ,                 !- Rated Effective Total Heat Rejection Rate {W}
-    29.4 ,                   !- Rated Condensing Temperature {C}
-    0.0 ,                    !- Rated Subcooling Temperature Difference{deltaC}
-    10.0,                    !- Rated Water Inlet Temperature {C}
-    Condenser Inlet Node,    !- Water Inlet Node Name
-    Condenser Outlet Node,   !- Water- Outlet Node Name
-    Variable Flow,           !- Water-cooled Loop Flow Type
-    Cond Outlet Temp Sch,    !- Water Outlet Temperature Schedule Name
-    ,                        !- Water Design Flow Rate {m3/s}
-    0.003,                   !- Water Maximum Flow Rate {m3/s}
-    55.,                     !- Maximum Water Outlet Temperature {C}
-    ,                        !- Minimum Water Inlet Temperature {C}
-    ,                        !- End-Use Subcategory
-    30. ,                    !- Condenser Refrigerant Operating Charge {kg}
-    65. ,                    !- Condensate Receiver Refrigerant Inventory {kg}
-    20. ;                    !- Condensate Piping Refrigerant Inventory {kg}
-```
-
-### Refrigeration Condenser (WaterCooled) Outputs
-
-FOR CONDENSERS COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
-
-* Zone,Average, Refrigeration System Condenser Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Total Recovered Heat Transfer Rate [W] Zone, Sum, Refrigeration System Condenser Total Recovered Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Heat Recovered for Non-Refrigeration Purposes Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Defrost Recovered Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration System Condenser Water Mass Flow Rate [kg/s]
-
-FOR CONDENSERS COOLING SYSTEMS SERVING AIR CHILLERS:
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate [W] HVAC, Sum, Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Energy [J]
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Fluid Mass Flow Rate [kg/s]
-
-
-
-#### FOR CONDENSERS ON SYSTEMS SERVING CASES AND/OR WALKINS:
-
-#### Refrigeration System Condenser Heat Transfer Rate [W]
-
-This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
-
-#### Refrigeration System Condenser Heat Transfer Energy [J]
-
-This is the total heat energy flowing across the condenser for the timestep being reported.
-
-#### Refrigeration System Condenser Total Recovered Heat Transfer Rate  [W]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for any purpose.
-
-#### Refrigeration System Condenser Total Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for any purpose for the timestep being reported.
-
-#### Refrigeration System Condenser Non Refrigeration Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating.
-
-#### Refrigeration System Condenser Heat Recovered for Non-Refrigeration Purposes Energy  [J]
-
-This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating for the timestep being reported.
-
-#### Refrigeration System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system..
-
-#### Refrigeration System Condenser Heat Energy Recovered for Refrigeration Defrost Energy [J]
-
-This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
-
-#### Refrigeration System Condenser Water Mass Flow Rate [kg/s]
-
-This is the mass flow rate of the water used to cool the condenser in kg/s.
-
-#### FOR CONDENSERS ON SYSTEMS SERVING AIR CHILLERS:
-
-#### Refrigeration Air Chiller System Condenser Heat Transfer Rate [W]
-
-This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
-
-#### Refrigeration Air Chiller System Condenser Heat Transfer Energy [J]
-
-This is the total heat energy flowing across the condenser for the timestep being reported.
-
-#### Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Rate  [W]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for any purpose.
-
-#### Refrigeration Air Chiller System Condenser Total Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the condenser refrigerant inlet flow for any purpose for the timestep being reported.
-
-#### Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating.
-
-#### Refrigeration Air Chiller System Condenser Non Refrigeration Recovered Heat Transfer Energy  [J]
-
-This is the total heat recovered from the condenser inlet flow for purposes such as water or air heating for the timestep being reported.
-
-#### Refrigeration Air Chiller System Condenser Defrost Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system.
-
-#### Refrigeration Chiller System Condenser Heat Energy Recovered for Refrigeration Defrost Energy [J]
-
-This is the total heat recovered from the condenser inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
-
-#### Refrigeration Air Chiller System Condenser Fluid Mass Flow Rate [kg/s]
-
-This is the mass flow rate of the water used to cool the condenser in kg/s.
-
-### Refrigeration:Condenser:Cascade
-
-The refrigeration system requires a single condenser.  The cascade condenser object is one of four options for this condenser. The cascade condenser is unlike the other condenser options because it rejects heat to another, higher-temperature, refrigeration system. That is, the cascade condenser acts as a heat rejection object for one system, but acts as a refrigeration load for another system.  Therefore, this object will be referenced twice: first for the system rejecting heat (see the field Refrigeration Condenser Name for the object Refrigeration:System), and second for the system absorbing the heat (see the input for the field Refrigeration Transfer Load or TransferLoad List Name for the object Refrigeration:System or the field Cascade Condenser Name or Secondary System Name for the object Refrigeration:TransferLoadList).
-
-Manufacturer’s data is required for the rated condensing temperature and the rated approach temperature difference. The user must also specify the condensing temperature control type.  There are two choices. The user can specify “Fixed� and the condensing temperature will be held constant at the input value.  The user can specify “Float� if they want the condensing temperature to be set by other refrigeration loads served by the higher-temperature system.
-
-The rated heat rejection capacity is not used except as a rough input value check on the overall system sizing. Optional input is provided to help the user compare refrigerant inventories for different systems.  These inputs represent the design values for the refrigerant inventory within the condenser, within a receiver beneath the condenser, and in the liquid pipes between the condenser and the refrigerated cases.
-
-#### Field: Name
-
-Identifies a particular condenser that rejects heat for a single refrigeration system. The name must be unique and will be validated against all the condenser names (ref: Refrigeration:Condenser:\*) in the input file, including names used for air-cooled, evaporative-cooled, and water-cooled condensers.
-
-#### Field: Rated Condensing Temperature
-
-This numeric field provides the rated condensing temperature (C).
-
-#### Field: Rated Approach Temperature Difference
-
-This numeric field provides the rated difference (Delta C) between the saturated condensing temperature for the system rejecting heat and the saturated evaporating refrigerant temperature for the system absorbing heat. The default value is 3.0 C.
-
-#### Field: Rated Effective Total Heat Rejection Rate
-
-This numeric field should be the rated heat rejection effect (W).  Be sure the rating corresponds to the correct refrigerant(s). This value is used for system sizing error checking.
-
-#### Field: Condensing Temperature Control Type
-
-The type of control used to set the saturated condensing temperature. Valid choices are **Fixed** and **Float**.  If the field is blank, **Fixed** will be used. Fixed will hold the condensing temperature constant at the value specified.  **Float** will consider the specified input as a minimum condensing temperature.  This value will be compared to the evaporating temperatures required by other loads on the higher-temperature refrigeration system, and will use the lowest temperature required to meet those loads, along with the Approach Temperature Difference, to set the condensing temperature.
-
-#### Field: Condenser Refrigerant Operating Charge Inventory
-
-This numeric field specifies the amount of refrigerant present within the condenser (kg) specified by the manufacturer, under standard rating conditions. This refrigerant is on the side of the condenser rejecting heat, not on the side of the condenser absorbing the heat.
-
-#### Field: Condensate Receiver Refrigerant Inventory
-
-This numeric field specifies the amount of refrigerant present within the condensate receiver (kg) specified by the manufacturer or system designer, under standard rating conditions.
-
-#### Field: Condensate Piping Refrigerant Inventory
-
-This numeric field specifies the amount of refrigerant present within the condensate piping (kg) specified by the system designer, under standard rating conditions.
-
-
-
-The following is an example input for a cascade condenser.
-
-```idf
-Refrigeration:Condenser:Cascade,
-    CascadeCondenser1 ,      !- Name
-    -4. ,                    !- Rated Condensing Temperature {C}
-    3. ,                     !- Rated Approach Temperature Difference {DeltaC}
-    20000.0 ,                !- Rated Effective Total Heat Rejection Rate {W}
-    Fixed;                   !- Condensing Temperature Control Type
-```
-
-### Refrigeration Condenser (Cascade) Outputs
-
-FOR CONDENSERS COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
-
-* Zone,Average, Refrigeration System Condenser Heat Transfer Rate [W]
-
-* Zone, Sum, Refrigeration System Condenser Heat Transfer Energy [J]
-
-FOR CONDENSERS COOLING SYSTEMS SERVING AIR CHILLERS:
-
-* HVAC,Average, Refrigeration Air Chiller System Condenser Heat Transfer Rate [W]
-
-* HVAC, Sum, Refrigeration Air Chiller System Condenser Heat Transfer Energy [J]
-
-
-
-#### FOR CONDENSERS ON SYSTEMS SERVING CASES AND/OR WALKINS:
-
-#### Refrigeration System Condenser Heat Transfer Rate [W]
-
-This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
-
-#### Refrigeration System Condenser Heat Transfer Energy [J]
-
-This is the total heat energy flowing across the condenser for the timestep being reported.
-
-#### FOR CONDENSERS ON SYSTEMS SERVING AIR CHILLERS:
-
-#### Refrigeration Air Chiller System Condenser Heat Transfer Rate [W]
-
-This is the total heat transfer across the condenser (i.e., compressor energy and refrigeration loads) in Watts.
-
-#### Refrigeration Air Chiller System Condenser Heat Transfer Energy [J]
-
-This is the total heat energy flowing across the condenser for the timestep being reported.
-
-
-
-### Refrigeration:GasCooler:AirCooled
-
-The transcritical refrigeration system requires a single gas cooler to reject the system heat.  The total heat of rejection is characterized by a linear relationship between the difference between the outside dry-bulb and gas cooler outlet temperatures.  The rated gas cooler fan power and fan speed control type must be specified.  If the gas cooler is not at ground level, the user may specify an air inlet node name (Ref. OutdoorAir:Node name).  Optional input is provided to help the user track refrigerant inventories.  These inputs represent the design values for the refrigerant inventory within the gas cooler, within a receiver, and in the liquid pipes between the gas cooler and the refrigerated cases.
-
-#### Field: Name
-
-Identifies a particular gas cooler that rejects heat for a single refrigeration system.  The name must be unique and will be validated against all the gas cooler names (Ref. Refrigeration:GasCooler:AirCooled) in the input file.
-
-#### Field: Rated Total Heat Rejection Rate Curve Name
-
-This field is the name of a curve object defining the gas cooler heat rejection as a function of the difference between the gas cooler outlet and entering air temperatures. The curve should be linear (Curve:Linear). See the Engineering Reference for more discussion on the curve coefficients.
-
-#### Field: Gas Cooler Fan Speed Control Type
-
-The type of fan speed control used by the gas cooler fan.  Valid choices are Fixed, FixedLinear, VariableSpeed, and TwoSpeed.  If the field is blank, Fixed will be used.  Note that fan energy consumption for the air-cooled gas cooler is computed in the same way as that of the air-cooled condenser.  For further information on fan energy calculations, see the discussion regarding air-cooled condenser fan energy in the Engineering Reference.
-
-#### Field: Rated Fan Power
-
-This numeric field specifies the rated fan power (W) specified by the manufacturer, under standard rating conditions.  If this field is blank, the default value of 5000 W will be used
-
-#### Field: Minimum Fan Air Flow Ratio
-
-Fan controls often include a minimum air flow ratio to avoid overheating the fan motor or for other reasons.  This numeric field should be between 0. and 1. and has a default value of 0.2.
-
-#### Field: Transition Temperature
-
-This is the temperature (C) at which the gas cooler and the refrigeration system transitions between subcritical and transcritical operation.  If this field is blank, the default value of 27.0°C will be used.
-
-#### Field: Transcritical Approach Temperature
-
-This is the temperature difference (C) between the refrigerant (CO<sub>2</sub>) exiting the gas cooler and the air entering the gas cooler during transcritical operation.  If this field is blank, the default value of 3.0°C will be used.
-
-#### Field: Subcritical Temperature Difference
-
-This is the temperature difference (C) between the condensing temperature and the ambient air temperature during subcritical operation.  If this field is blank, the default value of 10.0°C will be used.
-
-***Field: Minimum Condensing Temperature***
-
-This numeric field specifies the minimum condensing temperature (C) required to maintain stable subcritical operation.  If this field is blank, the default value of 10.0°C will be used.
-
-***Field: Air Inlet Node Name***
-
-This optional alpha field contains the name of the node from which the gas cooler draws its outdoor air.  If this field is left blank, the outdoor air dry-bulb temperature entering the gas cooler is taken directly from the weather data.  If this field is not blank, this node name must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data.  Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
-
-#### Field: End-Use Subcategory
-
-This field allows the specification of a user-defined end-use subcategory (e.g., "Low Temperature Rack").  A new meter for reporting is created for each unique subcategory (Ref. Output:Meter objects). Subcategories are also reported in the ABUPS table.  If this field is left blank, the equipment will be assigned to the "General" end-use subcategory.
-
-#### Field: Gas Cooler Refrigerant Operating Charge Inventory
-
-This numeric field specifies the amount of refrigerant present within the gas cooler (kg) specified by the manufacturer, under standard rating conditions.  If this field is blank, the default value of 0.0 kg will be used.
-
-#### Field: Gas Cooler Receiver Refrigerant Inventory
-
-This numeric field specifies the amount of refrigerant present within the gas cooler receiver (kg) specified by the manufacturer or system designer, under standard rating conditions.  If this field is blank, the default value of 0.0 kg will be used.
-
-#### Field: Gas Cooler Outlet Piping Refrigerant Inventory
-
-This numeric field specifies the amount of refrigerant present within the gas cooling outlet piping (kg) specified by the system designer, under standard rating conditions.  If this field is blank, the default value of 0.0 kg will be used.
-
-
-
-The following is an example input for an air-cooled gas cooler.
-
-```idf
-Refrigeration:GasCooler:AirCooled,
-    RefrigGasCooler,         !- Name
-    GasCoolerHRCurve,        !- Rated Total Heat Rejection Rate Curve Name
-    Fixed,                   !- Gas Cooler Fan Speed Control Type
-    6400,                    !- Rated Fan Power
-    0.2,                     !- Minimum Fan Air Flow Ratio
-    27.0,                    !- Transition Temperature
-    3.0,                     !- Transcritical Approach Temperature
-    10.0,                    !- Subcritical Temperature Difference
-    10.0,                    !- Minimum Condensing Temperature
-    ,                        !- Air Inlet Node Name
-    RefrigGasCooler,         !- End-Use Subcategory
-    ,                        !- Gas Cooler Refrigerant Operating Charge Inventory
-    ,                        !- Gas Cooler Receiver Refrigerant Inventory
-    ;                        !- Gas Cooler Outlet Piping Refrigerant Inventory
-```
-
-
-
-### Refrigeration GasCooler (AirCooled) Outputs
-
-* Zone,Average, Refrigeration Transcritical System Gas Cooler Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Transcritical System Gas Cooler Heat Transfer Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System Gas Cooler Fan Electric Power [W]
-
-* Zone,Sum, Refrigeration Transcritical System Gas Cooler Fan Electric Energy [J]
-
-* Zone,Average, Refrigeration Transcritical System Gas Cooler Outlet Temperature [C]
-
-* Zone,Average, Refrigeration Transcritical System Gas Cooler Outlet Pressure [Pa]
-
-* Zone,Average, Refrigeration Transcritical System Gas Cooler Defrost Recovered Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Transcritical System Gas Cooler Defrost Recovered Heat Transfer Energy [J]
-
-
-
-#### Refrigeration Transcritical System Gas Cooler Heat Transfer Rate [W]
-
-This output is the total heat transfer rate from the gas cooler in Watts, and includes compressor energy and the refrigeration load.
-
-#### Refrigeration Transcritical System Gas Cooler Heat Transfer Energy [J]
-
-This output is the total heat transferred from the gas cooler to the surroundings, in Joules, for the timestep being reported.
-
-#### Refrigeration Transcritical System Gas Cooler Fan Electric Power [W]
-
-This output is the electric input to the system’s gas cooler fan(s) in Watts.
-
-#### Refrigeration Transcritical System Gas Cooler Fan Electric Energy [J]
-
-This is the electricity consumption of the system’s gas cooler fan(s) in Joules for the timestep being reported.  This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Transcritical System Gas Cooler Outlet Temperature [C]
-
-This output is the temperature (in C) of the refrigerant exiting the gas cooler.
-
-#### Refrigeration Transcritical System Gas Cooler Outlet Pressure [Pa]
-
-This output is the pressure (in Pa) of the refrigerant exiting the gas cooler.
-
-#### Refrigeration Transcritical System Gas Cooler Defrost Recovered Heat Transfer Rate [W]
-
-This is the total heat recovered from the gas cooler inlet flow for defrost purposes within the refrigeration system.
-
-#### Refrigeration Transcritical System Gas Cooler Defrost Recovered Heat Transfer Energy [J]
-
-This is the total heat recovered from the gas cooler inlet flow for defrost purposes within the refrigeration system for the timestep being reported.
-
-### Refrigeration:TransferLoadList
-
-A refrigeration system may provide cooling to other, secondary, systems through either a secondary loop or a cascade condenser (Ref. Refrigeration:SecondarySystem and Refrigeration:Condenser:Cascade). If multiple transfer loads are served by a single primary system, use this list to group them together for reference by the primary system (see the field “Refrigeration Transfer Load or TransferLoad List Name� in the Refrigeration:System object).
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a refrigeration transfer load list. Any reference to this list by another object will use this name. In particular, the primary refrigeration system absorbing the heat from all the loads listed here will use this name to reference those loads.
-
-#### Field: Cascade Condenser Name or Secondary System Name
-
-Identifies a cascade condenser or secondary loop that is cooled, along with the other transfer loads listed here, by a single system. The name will be validated against the Refrigeration:SecondarySystem and Refrigeration:Condenser:Cascade names in the input file (the name will also be compared against all the other condenser names, but an error will be issued if it refers to any type of condenser other than a cascade condenser).
-
-
-
-The list is extensible; ten fields are provided in the IDD.
-
-
-
-The following is an example input for a transfer load list.
-
-```idf
-Refrigeration:TransferLoadList,
-    MedTempTransferLoads ,   !- Name
-    CascadeCondFrozen,       !- Cascade Condenser Name or Secondary System Name
-    SecondLoopDairy;         !- Cascade Condenser Name or Secondary System Name
-```
-
-### Refrigeration:SecondarySystem
-
-A refrigeration secondary system works in conjunction with refrigerated cases and walkins (Ref. Refrigeration:SecondarySystem, Refrigeration:CaseAndWalkInList, Refrigeration:Case, and Refrigeration:WalkIn) to simulate the performance of a secondary loop supermarket refrigeration system. Heat from the refrigeration loads served by the secondary loop is absorbed by a primary refrigeration system (ref: Refrigeration:System). The SecondarySystem object simulates a heat exchanger that is an evaporator, or refrigeration load, on the primary refrigeration system.
-
-The inputs for the refrigeration secondary system object include a name, which is also referenced to identify the load placed upon the primary refrigeration system. The inputs that describe the loads placed upon the secondary loop include the name of a single refrigerated case, the name of a single walk-in cooler, or a list of cases and walkin coolers.  The circulating fluid type specifies whether or not the secondary fluid remains in the liquid state throughout the loop (e.g., a glycol or brine solution) or undergoes a partial phase change while serving the refrigeration loads (e.g., a CO<sub>2</sub> liquid overfeed system). The circulating fluid name must also be specified and must correspond to a name used to provide the fluid properties.
-
-If the secondary fluid remains a liquid, the heat exchanger between the primary and secondary systems functions as an evaporator on the primary side and chills the circulating fluid on the secondary side. Inputs that describe the evaporator performance at rated conditions are used to calculate the heat exchanger effectiveness. These values include the rated evaporator capacity (which can be specified in terms of energy or fluid flow rate), the rated evaporating temperature, the rated approach temperature difference, and the rated range temperature difference.
-
-If the secondary fluid undergoes a partial phase change, the heat exchanger between the primary and secondary systems functions as an evaporator on the primary side and as a condenser on the secondary side. The evaporator capacity, evaporating temperature, and approach temperature difference, all at full-load design conditions, are input.
-
-The balance of the secondary system object describes the pumping system. The pumping options include a single constant speed pump, multiple constant speed pumps, or a variable frequency-drive pump.  The user can also keep track of distribution piping and receiver shell heat gains.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a refrigeration secondary system. Any reference to this refrigeration secondary system by another object will use this name. In particular, the primary refrigeration system absorbing the heat from this system will use this name to define that load.
-
-#### Field: Refrigerated Case or WalkIn or CaseAndWalkInList Name
-
-Identifies a single case, or walkin, or a particular list of refrigerated cases and walkins, that are cooled by this refrigeration secondary system. The name will be validated against the case, walkin, and CaseAndWalkInList names (ref. Refrigeration:Case, Refrigeration:WalkIn and Refrigeration:CaseAndWalkInList) in the input file.
-
-#### Field: Circulating Fluid Type
-
-Specifies whether the fluid is always liquid (e.g., glycol solution), or undergoes a partial phase change (e.g., CO<sub>2</sub> liquid overfeed system).  The options are “FluidAlwaysLiquid� and “FluidPhaseChange�.
-
-#### Field: Circulating Fluid Name
-
-The name of the secondary circulating fluid.
-
-For “FluidAlwaysLiquid�, this name must correspond to either an ethylene or propylene glycol (ref: FluidProperties:GlycolConcentration) or to a user-defined glycol (ref: FluidProperties:Name and FluidProperties: GlycolConcentration) in the input file. Note that the corresponding property data, including FluidProperties:Concentration, FluidProperties:Temperatures, and FluidProperties:GlycolConcentration must also be included in the input file and are provided in GlycolPropertiesRefData.idf for typical ethylene and propylene glycols.
-
-For “FluidPhaseChange�, the refrigerant used by the secondary system must be listed in the FluidProperties:Name object.  The corresponding property data must also be supplied in the input file. Property data for many refrigererants, including R11, R123, R134A, R12, R22, R404A, R507A, R410A, and R744, are available in FluidPropertiesRefData.idf.
-
-#### Field: Evaporator Capacity
-
-For “FluidAlwaysLiquid�, this numeric field should be the rated heat evaporator capacity (W).  Be sure the rating corresponds to the correct refrigerant and secondary circulating fluid. If this variable is specified and the rated evaporator flow rate for secondary fluid is not, then the flow rate will be calculated.  At least one of these two input variables is required.
-
-For “FluidPhaseChange�, this numeric field should be the evaporator capacity (W) at full-load design conditions. If this input is left blank, the capacity will be set to the sum of the capacities of the cases and walk-ins served by the secondary loop plus the pump motor load at full-load design conditions.
-
-#### Field: Evaporator Flow Rate for Secondary Fluid
-
-For “FluidAlwaysLiquid� systems, this is the rated evaporator secondary fluid flow rate in m<sup>3</sup>/s.  If this variable is specified and the rated evaporator capacity in watts is not, then the rated capacity will be calculated. At least one of these two input variables is required.
-
-For “FluidPhaseChange�, this field is not used (see “Phase Cange Circulating Rate�).
-
-#### Field:Evaporator Evaporating Temperature
-
-This numeric field provides the evaporating temperature (C) corresponding to the evaporator capacity. This is the evaporating temperature on the primary side of the heat exchanger used to chill or condense the secondary loop circulating fluid.  It is NOT the temperature in any cases or walkins served by the secondary loop.
-
-#### Field: Evaporator Approach Temperature Difference
-
-For “FluidAlwaysLiquid�, this numeric field is the rated temperature difference (DeltaC) between the circulating secondary fluid leaving the heat exchanger and the heat exchanger’s evaporating temperature.
-
-For “FluidPhaseChange�, this is the temperature difference (DeltaC) between the primary refrigerant evaporating and secondary refrigerant condensing temperatures at full-load design conditions.
-
-#### Field: Evaporator  Range Temperature Difference
-
-For “FluidAlwaysLiquid�, this numeric field is the rated temperature difference (DeltaC) between the circulating secondary fluid entering and leaving the heat exchanger. This value is not used for “FluidPhaseChange�.
-
-#### Field: Number of Pumps in Loop
-
-This numeric field provides the integer number of pumps used to circulate the secondary heat transfer fluid. The default value is 1. Unless a variable speed pump is specified, pump energy will be calculated in linear steps to achieve the necessary flow rate.
-
-#### Field: Total Pump Flow Rate
-
-This is the secondary fluid circulating flow rate in m<sup>3</sup>/s at full-load design conditions.  For “FluidAlwaysLiquid�, if no value is input, the Evaporator Flow Rate for Secondary Fluid will be used. For “FluidPhaseChange�, if no value is input, the flow rate will be calculated using the Evaporator Capacity and the PhaseChange Circulating Rate.
-
-#### Field: Total Pump Power
-
-This numeric field should be the pump power (W) at full-load design conditions.  Be sure the rating corresponds to the correct secondary circulating fluid at the design fluid temperature. EITHER the Total Pump Power OR the Total Pump Head is required.
-
-#### Field: Total Pump Head
-
-This numeric field should be the design pressure drop, or head, across the secondary loop (Pa) at full load design conditions.  Be sure the rating corresponds to the correct secondary circulating fluid at the design fluid temperature. EITHER the Total Pump Power OR the Total Head is required.
-
-#### Field: PhaseChange Circulating Rate
-
-This field is not used for “FluidAlwaysLiquid�.
-
-For “FluidPhaseChange�, the Circulating Rate is defined as the total mass flow at the pump divided by the mass flow rate of vapor returning to the separator. Values between 2.1 and 3 are common for CO<sub>2</sub> systems and the default is 2.5. If Total Pump Flow Rate is also defined, the PhaseChange Circulating Rate will only be used to check whether the two values are consistent.
-
-#### Field: Pump Drive Type
-
-Specifies whether the pump(s) is constant speed or variable speed.  The options are “Constant� and “Variable�. The default is “Constant�.
-
-#### Field: Variable Speed Pump Cubic Curve Name
-
-The name of a **cubic** performance curve (ref: Performance Curves) that parameterizes the variation of the variable speed pump power (and the associated load on the secondary refrigeration load) at off-rated conditions. The curve should be normalized to have the value of 1.0 at full-load design conditions. The variable speed pump cubic curve name is used only for the a pump drive type of “Variable�.
-
-#### Field: Pump Motor Heat to Fluid
-
-This choice field determines how much of the pump motor heat will be added to the circulating secondary fluid. This represents the motor efficiency for a non-hermetic motor. The default is 0.85.  For a semi-hermetic motor, enter 1.0. The value entered must be between 0.5 and 1.0.
-
-#### Field: Sum UA Distribution Piping
-
-This optional field is typically used when trying to compare the impact of pipe heat gains on system performance, particularly in comparing a DX system to a secondary system. Enter the value for secondary loop distribution piping heat gain (in W/C).  That is, sum up the product of the pipe insulation conductance times the outer piping insulation surface area. Please see the Engineering Reference for guidance in calculating this value.
-
-#### Field: Distribution Piping Zone Name
-
-This optional field is used when trying to determine the impact of pipe heat gains on system performance, particularly in comparing a DX system to a secondary system. (If the previous field, Sum UA Distribution Piping, is blank, this field will not be used.) Enter the name of the zone where the Distribution piping is located. The distribution piping heat gains will be calculated based upon the air temperature within this zone and will count as a cooling credit for this zone.
-
-#### Field: Sum UA Receiver/Separator Shell
-
-This optional field is typically used when trying to compare the impact of refrigeration component heat gains on system performance, particularly in comparing a conventional primary DX system to a secondary system. Enter the value for receiver/separator heat gain (in W/C).  That is, sum up the product of the tank insulaton conductance times the outer tank insulation surface area. Please see the Engineering Reference for guidance in calculating this value.
-
-#### Field: Receiver/Separator Zone Name
-
-This optional field is used when trying to determine the impact of refrigeration component heat gains on system performance, particularly in comparing a conventional primary DX system to a secondary system. (If the previous field, Sum UA Receiver/Separator, is blank, this field will not be used.) Enter the name of the zone where the receiver/separator is located. The heat gains will be calculated based upon the air temperature within this zone and will count as a cooling credit for this zone.
-
-#### Field: Evaporator Refrigerant Inventory
-
-The secondary loop is chilled by a primary system via a heat exchanger.  This field is the refrigerant inventory on the cold (primary) side of that heat exchanger, in kg. The default value is zero.
-
-#### Field: End-Use Subcategory
-
-This field allows the specification of a user-defined end-use subcategory (e.g., "Low Temperature Rack"). A new meter for reporting is created for each unique subcategory (Ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is left blank, the equipment will be assigned to the "General" end-use subcategory.
-
-
-
-
-
-The following is an example input for a brine-type (“FluidAlwaysLiquid�)refrigeration secondary system.
-
-```idf
-  Refrigeration:SecondarySystem,
-    SecondaryMedLoop,        !- Name
-    MedTempCaseList,         !- Refrigerated Case or Walkin or CaseAndWalkInList Name
-    FluidAlwaysLiquid,       !- Circulating Fluid Type
-    ProGly30Percent,         !- Circulating Fluid Name
-    3.5E4,                   !- Evaporator Capacity {W}
-    0.0021,                  !- Evaporator Flow Rate for Secondary Fluid {M3/s}
-    -12.6,                   !- Evaporator Evaporating Temperature {C}
-    2.7,                     !- Evaporator Approach Temperature Difference {DeltaC}
-    4.,                      !- Evaporator Range Temperature Difference {DeltaC}
-    3,                       !- Number of Pumps in Loop
-    .0023,                   !- Total Pump Flow Rate {M3/s}
-    ,                        !- Total Pump Power {W}
-    2.09E5,                  !- Total Pump Head {Pa}
-    ,                        !- PhaseChange Circulating Rate
-    ,                        !- Pump Drive Type
-    ,                        !- Variable Speed Pump Cubic Curve Name
-    1.0,                     !- Pump Motor Heat to Fluid
-    21.,                     !- Sum UA Distribution Piping {W/C}
-    SalesFloor,              !- Distribution Piping Zone Name
-    ,                        !- Sum UA Receiver/Separator Shell
-    ,                        !- Receiver/Separator Zone Name
-    ,                        !- Evaporator Refrigerant Inventory {kg}
-    ;                        !- End-Use Subcategory
-```
-
-
-The following is an example input for a liquid-overfeed-type (“FluidPhaseChange�) refrigeration secondary system.
-
-```idf
-  Refrigeration:SecondarySystem,
-    SecondaryLowLoop,        !- Name
-    LowTempCaseList,         !- Refrigerated Case or Walkin or CaseAndWalkInList Name
-    FluidPhaseChange,        !- Circulating Fluid Type
-    R744,                    !- Circulating Fluid Name
-    ,                        !- Evaporator Capacity {W}
-    ,                        !- Evaporator Flow Rate for Secondary Fluid {M3/s}
-    -39.2,                   !- Evaporator Evaporating Temperature {C}
-    2.,                      !- Evaporator Approach Temperature Difference {DeltaC}
-    ,                        !- Evaporator Range Temperature Difference {DeltaC}
-    3,                       !- Number of Pumps in Loop
-    ,                        !- Total Pump Flow Rate {M3/s}
-    ,                        !- Total Pump Power {W}
-    2.09E5,                  !- Total Pump Head {Pa}
-    2.5,                     !- PhaseChange Circulating Rate
-    Variable,                !- Pump Drive Type
-    SecondaryVarSpeedPump,   !- Variable Speed Pump Cubic Curve Name
-    1.0,                     !- Pump Motor Heat to Fluid
-    10.4,                    !- Sum UA Distribution Piping {W/C}
-    SalesFloor,              !- Distribution Piping Zone Name
-    1.4,                     !- Sum UA Receiver/Separator Shell
-    BackRoom,                !- Receiver/Separator Zone Name
-    ,                        !- Evaporator Refrigerant Inventory {kg}
-    ;                        !- End-Use Subcategory
-```
-
-### Refrigeration Secondary System Outputs
-
-FOR SECONDARY SYSTEMS SERVING CASES AND/OR WALKINS:
-
-* Zone,Average,Refrigeration Secondary Loop Pump Electric Power [W]
-
-* Zone,Sum,Refrigeration Secondary Loop Pump Electric Energy [J]
-
-* Zone,Average,Refrigeration Secondary Loop Load Heat Transfer Rate [W]
-
-* Zone,Sum,Refrigeration Secondary Loop Load Heat Transfer Energy [J]
-
-* Zone,Average,Refrigeration Secondary Loop Total Heat Transfer Rate [W]
-
-* Zone,Sum,Refrigeration Secondary Loop Total Heat Transfer Energy [J]
-
-* Zone,Average,Refrigeration Secondary Loop Estimated Refrigerant Inventory Mass[kg] Zone,Average,Refrigeration Secondary Loop Volume Flow Rate [m3/s]
-
-* Zone,Average,Refrigeration Secondary Loop Pipe Heat Gain Rate [W]
-
-* Zone,Average,Refrigeration Secondary Loop Pipe Heat Gain Energy [J]
-
-* Zone,Average,Refrigeration Secondary Loop Receiver Heat Gain Rate [W]
-
-* Zone,Average,Refrigeration Secondary Loop Receiver Heat Gain Energy [J]
-
-FOR SECONDARY SYSTEMS SERVING AIR CHILLERS:
-
-* HVAC,Average,Refrigeration Air Chiller Secondary Loop Pump Electric Power [W]
-
-* HVAC,Sum,Refrigeration Air Chiller Secondary Loop Pump Electric Energy [J]
-
-* HVAC,Average,Refrigeration Air Chiller Secondary Loop Load Heat Transfer Rate [W]
-
-* HVAC,Sum,Refrigeration Air Chiller Secondary Loop Load Heat Transfer Energy [J]
-
-* HVAC,Average,Refrigeration Air Chiller Secondary Loop Total Heat Transfer Rate [W]
-
-* HVAC,Sum,Refrigeration Air Chiller Secondary Loop Total Heat Transfer Energy [J]
-
-* HVAC,Average,Refrigeration Air Chiller Secondary Loop Estimated Refrigerant Inventory Mass[kg]
-
-* HVAC,Average,Refrigeration Air Chiller Secondary Loop Volume Flow Rate [m3/s]
-
-* HVAC,Average,Refrigeration Air Chiller Secondary Loop Pipe Heat Gain Rate [W]
-
-* HVAC,Average,Refrigeration Air Chiller Secondary Loop Pipe Heat Gain Energy [J]
-
-* HVAC,Average,Refrigeration Air Chiller Secondary Loop Receiver Heat Gain Rate [W]
-
-* HVAC,Average,Refrigeration Air Chiller Secondary Loop Receiver Heat Gain Energy [J]
-
-
-
-#### FOR SECONDARY SYSTEMS SERVING CASES AND/OR WALKINS:
-
-#### Refrigeration Secondary Loop Pump Electric Power [W]
-
-This output is the total electric power input to the pump(s) in Watts.
-
-#### Refrigeration Secondary Loop Pump Electric Energy [J]
-
-This is the electricity consumption of the system’s pump(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Secondary Loop Load Heat Transfer Rate [W]
-
-This is the amount of refrigeration provided to the cases and walkins served by the secondary loop in W.
-
-#### Refrigeration Secondary Loop Load Heat Transfer Energy [J]
-
-This is the amount of refrigeration provided to the cases and walkins served by the secondary loop in Joules for the timestep being reported.
-
-#### Refrigeration Secondary Loop Total Heat Transfer Rate [W]
-
-This is the total amount of refrigeration load placed upon the primary refrigeration system (including loads due to the cases and walkins plus the loads from the secondary loop pumps and any energy absorbed by the loop via pipe heat gains) in W.
-
-#### Refrigeration Secondary Loop Total Heat Transfer Energy [J]
-
-This is the total amount of energy placed upon the primary refrigeration system by the secondary loop in Joules for the timestep being reported.
-
-#### Refrigeration Secondary Loop Estimated Refrigerant Inventory Mass [kg]
-
-This output is the sum of the input inventory values for the cases and walkins and the refrigerant circulating through the loop.
-
-#### Refrigeration Secondary Loop Volume Flow Rate [m3/]s
-
-This output is the calculated volume flow through the pumps for this secondary loop.
-
-#### Refrigeration Secondary Loop Pipe Heat Gain Rate  [W]
-
-This output is the total heat transferred to the pipes in Watts.
-
-#### Refrigeration Secondary Loop Pipe Heat Gain Energy [J]
-
-This is the total heat transferred to the pipes in Joules for the timestep being reported.
-
-#### Refrigeration Secondary Loop Receiver Heat Gain Rate  [W]
-
-This output is the total heat transferred to the receiver in Watts.
-
-#### Refrigeration Secondary Loop Receiver Heat Gain Energy [J]
-
-This is the total heat transferred to the receiver in Joules for the timestep being reported.
-
-#### FOR SECONDARY SYSTEMS SERVING AIR CHILLERS:
-
-#### Refrigeration Air Chiller Secondary Loop Pump Electric Power [W]
-
-This output is the total electric power input to the pump(s) in Watts.
-
-#### Refrigeration Air Chiller Secondary Loop Pump Electric Energy [J]
-
-This is the electricity consumption of the system’s pump(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Refrigeration Air Chiller Secondary Loop Load Heat Transfer Rate [W]
-
-This is the amount of refrigeration provided to the air chillers served by the secondary loop in W.
-
-#### Refrigeration Air Chiller Secondary Loop Load Heat Transfer Energy [J]
-
-This is the amount of refrigeration provided to the air chillers served by the secondary loop in Joules for the timestep being reported.
-
-#### Refrigeration Air Chiller Secondary Loop Total Heat Transfer Rate [W]
-
-This is the total amount of refrigeration load placed upon the primary refrigeration system (including loads due to the air chillers plus the loads from the secondary loop pumps and any energy absorbed by the loop via pipe heat gains) in W.
-
-#### Refrigeration Air Chiller Secondary Loop Total Heat Transfer Energy [J]
-
-This is the total amount of energy placed upon the primary refrigeration system by the secondary loop in Joules for the timestep being reported.
-
-#### Refrigeration Air Chiller Secondary Loop Estimated Refrigerant Inventory Mass [kg]
-
-This output is the sum of the input inventory values for the air chillers  and the refrigerant circulating through the loop.
-
-#### Refrigeration Air Chiller Secondary Loop Volume Flow Rate [m3/]s
-
-This output is the calculated volume flow of coolant through the pumps for this secondary loop.
-
-#### Refrigeration Air Chiller Secondary Loop Pipe Heat Gain Rate  [W]
-
-This output is the total heat transferred to the pipes in Watts.
-
-#### Refrigeration Air Chiller Secondary Loop Pipe Heat Gain Energy [J]
-
-This is the total heat transferred to the pipes in Joules for the timestep being reported.
-
-#### Refrigeration Air Chiller Secondary Loop Receiver Heat Gain Rate  [W]
-
-This output is the total heat transferred to the receiver in Watts.
-
-#### Refrigeration Air Chiller Secondary Loop Receiver Heat Gain Energy [J]
-
-This is the total heat transferred to the receiver in Joules for the timestep being reported.
-
-### Additional Refrigeration Outputs Available for Each Zone
-
-Multiple refrigeration cases and walkins may be located within a single zone.  Each zone may also exchange heat with refrigeration system suction piping, secondary loop distribution piping, and secondary loop receivers. Output variables have been prepared to sum up the total heat exchange due to all refrigeration objects within a single zone.  The output variables that start with “Zone Refrigeration� do not account for refrigeration provided by refrigeration chiller sets or any piping from systems serving air chillers.  The output variables that start with “Zone Chillers� account for all the refrigeration system elements serving air chillers.
-
-### Additional Refrigeration Outputs for Each Zone
-
-FOR THE SUM OF ALL COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
-
-* Zone,Average, Refrigeration Zone Case and Walk In Sensible Cooling Rate [W]
-
-* Zone,Sum, Refrigeration Zone Case and Walk In Sensible Cooling Energy [J]
-
-* Zone,Average, Refrigeration Zone Case and Walk In Heating Rate [W]
-
-* Zone,Sum, Refrigeration Zone Case and Walk In Heating Energy [J]
-
-* Zone,Average, Refrigeration Zone Case and Walk In Total Sensible Cooling Rate [W]
-
-* Zone,Sum, Refrigeration Zone Case and Walk In Total Sensible Cooling Energy [J]
-
-* Zone,Average, Refrigeration Zone Case and Walk In Total Latent Cooling Rate [W]
-
-* Zone,Sum, Refrigeration Zone Case and Walk In Total Latent Cooling Energy [J]
-
-* Zone,Sum, Refrigeration Zone Case and Walk In Total Cooling Energy [J]
-
-* Zone,Average,Refrigeration Zone Case and Walk In Total Cooling Rate [W]
-
-* Zone,Average, Refrigeration Zone Case and Walk In Total Heat Transfer Rate [W]
-
-* Zone,Sum, Refrigeration Zone Case and Walk In Total Heat Transfer Energy [J]
-
-
-
-FOR THE SUM OF ALL COOLING SYSTEMS SERVING CHILLERS:
-
-* HVAC,Average, Refrigeration Zone Air Chiller Sensible Heat Transfer Rate [W]
-
-* HVAC,Sum, Refrigeration Zone Air Chiller Sensible Heat Transfer Energy  [J]
-
-* HVAC,Average, Refrigeration Zone Air Chiller Latent Cooling Rate [W]
-
-* HVAC,Sum, Refrigeration Zone Air Chiller Latent Cooling Energy [J]
-
-* HVAC,Average, Refrigeration Zone Air Chiller Total Cooling Rate [W]
-
-* HVAC,Sum, Refrigeration Zone Air Chiller Total Cooling Energy [J]
-
-#### FOR THE SUM OF ALL COOLING SYSTEMS SERVING CASES AND/OR WALKINS:
-
-#### Refrigeration Zone Case and Walk In Total Sensible Cooling Rate [W]
-
-This output is the total sensible heat transfer between all refrigeration objects located in the zone in Watts. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
-
-***Refrigeration Zone Case and Walk In Total Sensible Cooling Energy [J]***
-
-This is the total sensible heat transfer between all refrigeration objects located in the zone in Joules for for the timestep being reported. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
-
-#### Refrigeration Zone Case and Walk In Total Latent Cooling Rate [W]
-
-This output is the total latent heat transfer between all refrigeration objects located in the zone in Watts. A negative value will be reported when the refrigeration equipment provides dehumidification (thereby reducing the zone latent load).
-
-***Refrigeration Zone Case and Walk In Total Latent Cooling Energy [J]***
-
-This is the total latent heat transfer between all refrigeration objects located in the zone in Joules for for the timestep being reported. A negative value will be reported when the refrigeration equipment provides dehumidification (thereby reducing the zone latent load).
-
-#### Refrigeration Zone Case and Walk In Total Heat Transfer Rate [W]
-
-This output is the total heat transfer (sensible plus latent) between all refrigeration objects located in the zone in Watts. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
-
-***Refrigeration Zone Case and Walk In Total Heat Transfer Energy [J]***
-
-This is the total heat transfer (sensible plus latent) between all refrigeration objects located in the zone in Joules for for the timestep being reported. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
-
-#### Refrigeration Zone Case and Walk In Sensible Cooling Rate [W]
-
-This output is the total sensible cooling from all refrigeration objects located in the zone in Watts.
-
-***Refrigeration Zone Case and Walk In Sensible Cooling Energy [J]***
-
-This is the total sensible cooling from all refrigeration objects located in the zone in Joules for for the timestep being reported.
-
-#### Refrigeration Zone Case and Walk In Heating Rate [W]
-
-This output is the total heating from all refrigeration objects located in the zone in Watts.
-
-***Refrigeration Zone Case and Walk In Heating Energy [J]***
-
-This is the total heating from all refrigeration objects located in the zone in Joules for for the timestep being reported.
-
-#### Refrigeration Zone Case and Walk In Total Cooling Rate [W]
-
-This output is the total cooling (sensible plus latent) from all refrigeration objects located in the zone in Watts.
-
-***Refrigeration Zone Case and Walk In Total Cooling Energy [J]***
-
-This is the total cooling (sensible plus latent) from all refrigeration objects located in the zone in Joules for for the timestep being reported.
-
-#### FOR THE SUM OF ALL COOLING SYSTEMS SERVING AIR CHILLERS:
-
-#### Refrigeration Zone Air Chiller Heating Rate  [W]
-
-This output is the total heating from all air chillers located in the zone in Watts.
-
-***Refrigeration Zone Air Chiller Heating Energy [J]***
-
-This is the total heating from all air chillers located in the zone in Joules for for the timestep being reported.
-
-#### Refrigeration Zone Air Chiller Sensible Cooling Rate   [W]
-
-This output is the total sensible cooling from all air chillers located in the zone in Watts.
-
-***Refrigeration Zone Air Chiller Sensible Cooling Energy [J]***
-
-This is the total sensible cooling from all air chillers located in the zone in Joules for for the timestep being reported.
-
-#### Refrigeration Zone Air Chiller Sensible Heat Transfer Rate  [W]
-
-This output is the total sensible heat transfer from all air chillers located in the zone in Watts. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
-
-#### Refrigeration Zone Air Chiller Sensible Heat Transfer Energy  [J]
-
-This is the total sensible heat transfer from all air chillers located in the zone in Joules for for the timestep being reported. A negative value will be reported when the refrigeration objects cool (that is, remove heat from) the zone.
-
-#### Refrigeration Zone Air Chiller Latent Cooling Rate  [W]
-
-This output is the total latent cooling from all air chillers located in the zone in Watts.
-
-***Refrigeration Zone Air Chiller Latent Cooling Energy [J]***
-
-This is the total latent cooling from all air chillers located in the zone in Joules for for the timestep being reported.
-
-#### Refrigeration Zone Air Chiller Water Removed Mass Flow Rate  [kg/s]
-
-This is the total amount of water removed by all air chillers located in the zone in kg/s for for the timestep being reported.
-
-#### Refrigeration Zone Air Chiller Total Cooling Rate  [W]
-
-This output is the total cooling (sensible plus latent) from all air chillers located in the zone in Watts.
-
-***Refrigeration Zone Air Chiller Total Cooling Energy [J]***
-
-This is the total cooling (sensible plus latent) from all air chillers located in the zone in Joules for for the timestep being reported.
-
-### Refrigeration:AirChiller
-
-The Refrigeration:AirChiller object works in conjunction with a refrigeration chiller set, compressor rack, a refrigeration system, or a refrigeration secondary system object (Ref. ZoneHvac:RefrigerationChillerSet, and a Refrigeration:CompressorRack, Refrigeration:System, or Refrigeration:SecondarySystem) to simulate the performance of an air chiller, similar to one found in a refrigerated warehouse. The air chiller model uses information at rated conditions along with the zone conditions to determine performance. Energy use for fans and heaters is modeled based on inputs for nominal power, schedules, and control type. The refrigeration chiller model accounts for the sensible and latent heat exchange with the surrounding environment.
-
-The refrigeration chiller cooler object inputs include a name, an availability schedule name, the rated cooling capacity, the rated operating temperature, the rated cooling source temperature, the rated total heating power and heating power schedule, the rated fan power and schedules, defrost type, defrost control type, defrost schedule name, drip-down schedule name, defrost power, the portion of the defrost energy used to melt ice (only for temperature termination control type), and refrigerant inventory.
-
-Chiller coils are rated under multiple conventions. Each rating is typically based upon a selected fin material and refrigerant cycle, with correction factors for other materials or refrigerants. Fields are provided here for those correction factors. The performance of all chiller coils depends upon the inlet air temperature, relative humidity, and flow rate. Multiple methods of expressing this relationship are provided here to accommodate the way information is provided by different manufacturers.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a refrigeration chiller. Any reference to this refrigeration chiller by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the refrigeration chiller can operate during a given time period. A schedule value greater than 0 (maximum schedule value of 1.0 is typically used) indicates that the refrigeration chiller will operate during a given time period. A value equal to 0 denotes that the case does not operate (everything is OFF: refrigeration, fans, lights, anti-sweat, etc.). Typically the refrigeration chiller will operate throughout the day (i.e., the schedule will contain 1 for all time periods); however, refrigeration chillers require maintenance and/or cleaning and this can be modeled accordingly using this schedule if desired. If this field is left blank, the default schedule has a value of 1 for all time periods.
-
-#### Field: Capacity Rating Type
-
-The type of capacity rating used for this refrigeration chiller. Valid choices are UnitLoadFactorSensibleOnly, CapacityTotalSpecificConditions, EuropeanSC1Standard, EuropeanSC1NominalWet, EuropeanSC2Standard, EuropeanSC2NominalWet, EuropeanSC3Standard, EuropeanSC3NominalWet, EuropeanSC4Standard, EuropeanSC4NominalWet, EuropeanSC5Standard, and EuropeanSC5NominalWet. In each case, select the rating option that corresponds to the expected service conditions.  For example, U.S. manufacturers quote a separate Unit Load Factor for wet or frosted coils.  If the evaporating temperature is less than 0C, input the frosted coil value. Within the European convention, select SC1, 2, 3, 4, or 5 depending upon the expected evaporating temperature. This field is required and there is no default value. Refer to the Engineering Reference for further information on these rating types. NOTE: If the CapacityTotalSpecificConditions rating type is specified, the input file must include the manufacturer’s coil capacity correction curve in tabular form using the Table:MultiVariableLookup object. An example of this may be found in the RefrigeratedWarehouse.idf example file.
-
-#### NOTE – ONLY ONE OF THE FOLLOWING TWO FIELDS IS USED
-
-#### Field: Rated Unit Load Factor
-
-The sensible cooling capacity in watts (W/C) at rated conditions. The value entered for this field must be greater than zero, with no default value. This value is only used if the Capacity Rating Type is UnitLoadFactorSensibleOnly. The value given must be based upon the difference between the chiller inlet and outlet air temperatures, not on the difference between the zone mean temperature and the outlet air temperature.
-
-#### Field: Rated Capacity
-
-The cooling capacity in watts (W) at rated conditions. The value entered for this field must be greater than zero, with no default value. This field is only used if the Capacity Rating Type is CapacityTotalSpecificConditions, EuropeanSC1Standard, EuropeanSC1NominalWet, EuropeanSC2Standard, EuropeanSC2NominalWet, EuropeanSC3Standard, EuropeanSC3NominalWet, EuropeanSC4Standard, EuropeanSC4NominalWet, EuropeanSC5Standard, or EuropeanSC5NominalWet. For CapacityTotalSpecificConditions, this capacity includes both sensible and latent at the conditions given in the next two fields.  Note that the European Standard ratings are sensible only and the European Nominal ratings include latent capacity as well. The value given here must correspond to the capacity rating type given previously.
-
-#### Field: Rated Relative Humidity
-
-This field is ONLY used if the Capacity Rating Type is CapacityTotalSpecificConditions and represents the relative humidity at rated conditions, expressed as a percent. The default is 85.
-
-#### Field: Rated Cooling Source Temperature
-
-For a DX evaporator coil, enter the saturated evaporating temperature in ˚C.  For a fluid coil, enter the fluid coil entrance temperature in ˚C. There is no default value. This number is used, with temperatures for other refrigeration loads on any one system, to set that system’s minimum suction pressure or minimum circulating fluid temperature.
-
-#### Field: Rated Temperature Difference DT1
-
-The rated difference between the air entering the refrigeration chiller and the cooling source temperature in ËšC. The entered value for this field must be less than 20ËšC. There is no default value.
-
-#### Field: Maximum Difference Between Inlet Air and Evaporating Temperature
-
-The maximum difference between the air entering the refrigeration chiller and the cooling source temperature in °C used to limit capacity during pull-down. The default is 1.3 times the Rated Temperature Difference DT1.
-
-#### Field: Coil  Material Correction Factor
-
-This field is used to enter the manufacturer’s correction factor for coil material corresponding to the rating previously input. The default is 1.0 (dimensionless).
-
-#### Field: Refrigerant Correction Factor
-
-This field is used to enter the manufacturer’s correction factor for refrigerant corresponding to the rating previously input. The default is 1.0 (dimensionless). (Note, the refrigerant itself is specified for the detailed system or secondary loop providing the refrigerant to this coil.)
-
-#### Field: Capacity Correction Curve Type
-
-The type of capacity correction curve used to account for the impact of the room air conditions on the chiller capacity. Valid choices are LinearSHR60, QuadraticSHR, European, and TabularRHxDT1xTRoom. This field will default to LinearSHR60, unless the CapacityTotalSpecificConditions rating type is specified, in which case, the TabularRHxDT1xTRoom correction curve type must be used. Refer to the Engineering Reference for further information on these curve types. The resulting correction factor for LinearSHR60, QuadraticSHR, and European types will be applied to the sensible capacity and must have output values between 1 and 2. The resulting correction factor for TabularRHxDT1xTRoom will be applied to the CapacityTotalSpecificConditions capacity and can have values between 0.2 and 2. If TabularRHxDT1xTRoom is used, the curve type within the table must be specified as “Quadratic�.
-
-#### Field: Capacity Correction Curve Name
-
-The name of the curve object defining the total refrigerating capacity. For correction curve types LinearSHR60 and QuadraticSHR, the independent variable is the Sensible Heat Ratio and the output values are between 1.0 and 2.0. For correction curve type European, EnergyPlus contains built-in capacity correction curves and specification of a capacity correction curve name is not required. For correction curve type TabularRHxDT1xTRoom, enter the name of a Table:MultiVariableLookup object that gives the total capacity (in W) as a function of RH, DT1, and Room Temperature; IN THAT ORDER. An example of a TabularRHxDT1xTRoom correction curve using the Table:MultiVariableLoopkup object may be found in the RefrigeratedWarehouse.idf example file.
-
-#### Field: SHR60 Correction Factor
-
-This field is only used when the capacity correction curve type is LinearSHR60. It should correspond to the capacity factor, that is, the total capacity divided by the sensible capacity corresponding to a Sensible Heat Ratio of 0.6. The default is 1.48 (dimensionless).
-
-#### Field: Rated Total Heating Power
-
-The total heating power in watts including drip-pan and any other heaters (W). This value is required and has no default value.
-
-#### Field: Heating Power Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes the fraction of heater power that operates during a given time period. A schedule value of zero denotes that all heaters are off. A schedule value greater than 0 indicates that some portion of the total heater power will operate during that time period (maximum schedule value of 1.0 means all heaters are fully on). If this field is left blank, the default schedule has a value of 1 for all time periods.
-
-#### Field: Fan Speed Control Type
-
-The type of fan speed control used by the cooling coil’s fan(s). Valid choices are **Fixed**, **FixedLinear**, **VariableSpeed**, and **TwoSpeed**.  If the field is blank, **Fixed** will be used. See the Engineering Reference for a discussion of this option’s effect on fan energy consumption.
-
-#### Field: Rated Fan Power
-
-The cooling coil fan power in watts (W). This value has a default value of 375W. This fan is assumed to run continuously except during electric, hot brine, or hot gas defrost periods.
-
-#### Field: Rated Air Flow
-
-The cooling coil fan rated air flow in cubic meters per second (m<sup>3</sup>/s). This value has no default value and must be input.
-
-#### Field: Minimum Fan Air Flow Ratio
-
-The minimum fraction of the rated air flow for part-load fan operation, must be between 0. and 1.0. The default value is 0.2.
-
-#### Field: Defrost Type
-
-The type of defrost used for this refrigeration chiller. Valid choices are None, Off-Cycle, HotFluid, and Electric. The default defrost type is Electric if the field is blank. HotFluid includes both hot gas and hot brine defrost systems. Refer to the Engineering Reference for further information on how the different defrost types are modeled.
-
-#### Field: Defrost Control Type
-
-The type of defrost control used for this refrigeration chiller. Valid choices are TimeSchedule and TemperatureTermination. The default is TimeSchedule if the field is blank. Refer to the Engineering Reference for further information on how the different defrost controls are modeled.
-
-#### Field: Defrost Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes when the refrigeration chiller requires defrosting. A schedule value of 1.0 indicates that defrost can be on during a given time period. A value equal to 0 denotes that the defrost is off. Defrost schedules normally repeat the duration and number of defrost cycles for each day of the year. The refrigeration chiller manufacturer typically provides this information with the product literature. If TemperatureTermination control type is used, the defrost schedule is used for the defrost cycle start time and the defrost cycle end time is not allowed to extend beyond the scheduled off time. The use of Compact Schedules (ref. Schedules) are ideal for this purpose.
-
-#### Field: Defrost Drip-Down Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the refrigeration chiller requires additional time for draining condensate after the defrost period. A schedule value of 1.0 indicates that the defrost drip-down period is on during a given time period. A value equal to 0 denotes that the defrost drip-down period is over. The refrigeration chiller manufacturer typically provides this information with the product literature.
-
-Each defrost drip-down period specified in this schedule should start at the same time as the corresponding defrost period specified in the schedule for Defrost Schedule, and the drip-down schedule defrost period should always be longer than or equal to the length of the defrost schedule time period. For example, if the defrost schedule contains a defrost period from 7:00 to 7:15, you would specify a case defrost drip-down period from 7:00 to 7:20 if you wanted to model a 5 minute condensate drip-down period after the regular defrost period. If no drip-down schedule is entered, then the defrost schedule (specified for the previous input field) will be used. The use of Compact Schedules (ref. Schedules) are ideal for this purpose.
-
-#### Field: Defrost Power
-
-The defrost power in watts. This input is required for hot-fluid (hot gas or hot brine), or electric defrost types. Refrigeration chiller manufacturers do not typically provide information on the heat input for hot gas and hot brine defrost. Information provided for electric defrost power can be substituted here for refrigeration chillers using hot-gas or hot-brine defrost if other information is not available. Only electric Defrost Types consume electricity during the defrost period. The entered value for this field must be greater than or equal to zero.
-
-#### Field: Temperature Termination Defrost Fraction to Ice
-
-When cooling coils go through a defrost cycle, only a portion of the defrost energy is actually used to melt the ice.  The rest of the defrost energy goes to increasing the temperature of the coils themselves and to the refrigeration chiller environment. The Temperature Termination defrost control type calculates the end of the defrost cycle that corresponds to melting all the ice. Therefore, the user must input this fractional value. The default value is 0.7 for electric defrost and 0.3 for hot fluid defrost. Refer to the Engineering Reference for further information on how the defrost energy control types are modeled.
-
-#### Field: Vertical Location
-
-The vertical location for this refrigeration chiller. Valid choices are Floor, Middle, and Ceiling. The default is Middle if the field is blank. The vertical location is used to transform the mixed zone air temperature to the coil inlet air temperature. Refer to the Engineering Reference for further information on how the different vertical locations are modeled.
-
-#### Field: Average Refrigerant Charge Inventory
-
-The value of this optional field is the refrigerant inventory present in the refrigeration chiller during ordinary operation. The value is used to produce an estimate of the total refrigerant present in the refrigeration system. The value is entered in kg.
-
-
-
-The following is an example input for a refrigeration air chiller.
-
-```idf
-   Refrigeration:AirChiller,
-    Freezer_1AirChiller_1,    !- Name
-    AvailAllYear,             !- Availability Schedule Name
-    UnitLoadFactorSensibleOnly, !- Capacity Rating Type
-    10900.,                   !- Rated Unit Load Factor {W/deltaC}
-    ,                         !- Rated Capacity {W}
-    ,                         !- Rated Relative Humidity
-    -26.,                     !- Rated Cooling Source Temperature {C}
-    8.,                       !- Rated Temperature Difference DT1 {DeltaC}
-    11.,                      !- Maximum Temperature Difference DT1 {DeltaC}
-    ,                         !- Material Correction Factor
-    ,                         !- Refrigerant Correction Factor
-    LinearSHR60,              !- Capacity Correction Curve Type
-    ,                         !- Capacity Correction Curve Name
-    1.5,                      !- SHR60 Correction Factor {dimensionless}
-    200.,                     !- Rated Total Heating Power {W}
-    AirChillerDripDownSched1,    !- Heating Power Schedule Name
-    ,                         !- Fan Speed Control Type
-    375.,                     !- Rated Fan Power {W}
-    12.4,                     !- Rated Air Flow {m3/s}
-    ,                         !- Minimum Fan Air Flow Ratio
-    Electric,                 !- Defrost Type
-    TimeSchedule,             !- Defrost Control Type
-    AirChillerDefrostSched1,  !- Defrost Schedule Name
-    AirChillerDripDownSched1, !- Defrost Drip-Down Schedule Name
-    55066.,                  !- Defrost Power {W}
-    ,                         !- Temperature Termination Defrost Fraction to Ice
-    ,                         !- Vertical Location
-    ;                         !- Average Refrigerant Charge Inventory {kg}
-```
-
-
-
-The following is an example input for a refrigeration air chiller.
-
-```idf
-   Refrigeration:AirChiller,
-    Freezer_1AirChiller_1,    !- Name
-    AvailAllYear,             !- Availability Schedule Name
-    UnitLoadFactorSensibleOnly, !- Capacity Rating Type
-    10900.,                   !- Rated Unit Load Factor {W/deltaC}
-    ,                         !- Rated Capacity {W}
-    ,                         !- Rated Relative Humidity
-    -26.,                     !- Rated Cooling Source Temperature {C}
-    8.,                       !- Rated Temperature Difference DT1 {DeltaC}
-    11.,                      !- Maximum Temperature Difference DT1 {DeltaC}
-    ,                         !- Material Correction Factor
-    ,                         !- Refrigerant Correction Factor
-    LinearSHR60,              !- Capacity Correction Curve Type
-    ,                         !- Capacity Correction Curve Name
-    1.5,                      !- SHR60 Correction Factor {dimensionless}
-    200.,                     !- Rated Total Heating Power {W}
-    AirChillerDripDownSched1,    !- Heating Power Schedule Name
-    ,                         !- Fan Speed Control Type
-    375.,                     !- Rated Fan Power {W}
-    12.4,                     !- Rated Air Flow {m3/s}
-    ,                         !- Minimum Fan Air Flow Ratio
-    Electric,                 !- Defrost Type
-    TimeSchedule,             !- Defrost Control Type
-    AirChillerDefrostSched1,  !- Defrost Schedule Name
-    AirChillerDripDownSched1, !- Defrost Drip-Down Schedule Name
-    55066.,                  !- Defrost Power {W}
-    ,                         !- Temperature Termination Defrost Fraction to Ice
-    ,                         !- Vertical Location
-    ;                         !- Average Refrigerant Charge Inventory {kg}
-```
-
-
-
-
-### Refrigeration Air Chiller Outputs
-
-* HVAC,Average,Refrigeration Zone Air Chiller Total Cooling Rate [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Total Cooling Energy [J]
-
-* HVAC,Average,Refrigeration Zone Air Chiller Sensible Cooling Rate [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Sensible Cooling Energy [J]
-
-* HVAC,Average,Refrigeration Zone Air Chiller Latent Cooling Rate [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Latent Cooling Energy [J]
-
-* HVAC,Average, Refrigeration Zone Air Chiller Water Removed Mass Flow Rate [kg/s]
-
-* HVAC,Average,Refrigeration Zone Air Chiller Total Electric Power [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Total Electric Energy [J]
-
-* HVAC,Average,Refrigeration Zone Air Chiller Fan Electric Power [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Fan Electric Energy [J]
-
-* HVAC,Average,Refrigeration Zone Air Chiller Heater Electric Power [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Heater Electric Energy [J]
-
-* HVAC,Average,Refrigeration Zone Air Chiller Sensible Heat Ratio []
-
-* HVAC,Average,Refrigeration Zone Air Chiller Frost Accumulation Mass [kg]
-
-* HVAC,Average,Refrigeration Zone Air Chiller Zone Total Cooling Rate [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Zone Total Cooling Energy [J]
-
-* HVAC,Average,Refrigeration Zone Air Chiller Zone Sensible Cooling Rate [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Zone Sensible Cooling Energy [J]
-
-* HVAC,Average,Refrigeration Zone Air Chiller Zone Heating Rate [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Zone Heating Energy [J]
-
-
-
-*Report only for Air Chillers using electric defrost*
-
-* HVAC,Average,Refrigeration Zone Air Chiller Defrost Electric Power [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Defrost Electric Energy [J]
-
-
-
-***Report for each Zone exchanging energy with the Air Chiller***
-
-* HVAC,Average,Refrigeration Zone Air Chiller Sensible Cooling Rate [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Sensible Cooling Energy [J]
-
-* HVAC,Average, Refrigeration Zone Air Chiller Heating Rate [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Heating Energy [J]
-
-* HVAC,Average, Refrigeration Zone Air Chiller Latent Cooling Rate [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Latent Cooling Energy [J
-
-* HVAC,Average,Refrigeration Zone Air Chiller Total Cooling Rate [W]
-
-* HVAC,Sum,Refrigeration Zone Air Chiller Total Cooling Energy [J]
-
-* HVAC,Average,Refrigeration Zone Air Chiller Water Removed Mass Flow Rate [kg/s]
-
-#### Refrigeration Zone Air Chiller Total Cooling Rate [W]
-
-This field is the total (sensible plus latent) cooling rate of the Air Chiller evaporator coil in Watts.
-
-#### Refrigeration Zone Air Chiller Total Cooling Energy [J]
-
-This field is the total (sensible plus latent) cooling of the Air Chiller evaporator coil in Joules over the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
-
-#### Refrigeration Zone Air Chiller Sensible Cooling Rate [W]
-
-#### Refrigeration Zone Air Chiller Sensible Heat Transfer Rate [W]
-
-This field is the sensible cooling rate of the Air Chiller evaporator coil in Watts.
-
-#### Refrigeration Zone Air Chiller Sensible Cooling Energy  [J]
-
-#### Refrigeration Zone Air Chiller Sensible Heat Transfer Energy [J]
-
-This field is the sensible cooling of the Air Chiller evaporator coil in Joules over the timestep being reported.
-
-#### Refrigeration Zone Air Chiller Latent Cooling Rate  [W]
-
-This field is the latent cooling (dehumidification) rate of the Air Chiller evaporator coil in Watts.
-
-#### Refrigeration Zone Air Chiller Latent Cooling Energy  [J]
-
-This field is the latent cooling (dehumidification) of the Air Chiller evaporator coil in Joules over the timestep being reported.
-
-#### Refrigeration Zone Air Chiller Water Removed Mass Flow Rate  [kg/s]
-
-This field is the latent cooling (dehumidification) of the Air Chiller evaporator coil in kilograms per second over the timestep being reported.
-
-#### Refrigeration Zone Air Chiller Total Electric Power [W]
-
-This field is the total electricity (fan, heaters, lights, and electric defrost) used by the Air Chiller in Watts.
-
-#### Refrigeration Zone Air Chiller Total Electric Energy [J]
-
-This field is the electricity (fan, heaters, lights, and electric defrost)used by the Refrigeration chiller in Joules over the timestep being reported.
-
-#### Refrigeration Zone Air Chiller Fan Electric Power [W]
-
-This field is the electric power input to the Air Chiller fan(s) in Watts.
-
-#### Refrigeration Zone Air Chiller Fan Electric Energy  [J]
-
-This field is the electricity consumption of the Air Chiller fan(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
-
-#### Refrigeration Zone Air Chiller Heater Electric Power  [W]
-
-This field is the electric power input to the Air Chiller heaters in Watts.
-
-#### Refrigeration Zone Air Chiller Heater Electric Energy [J]
-
-This field is the total electricity consumption of the Air Chiller heaters in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects).
-
-#### Refrigeration Zone Air Chiller Defrost Electric Power  [W]
-
-This field is the electric power input to the Air Chiller electric defrost heater(s) in Watts. This output is available if case defrost type is Electric.
-
-#### Refrigeration Zone Air Chiller Defrost Electric Energy [J]
-
-This field is the total electricity consumption of the Air Chiller electric defrost heater(s) in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Refrigeration, Group Key = Building (Ref. Output:Meter objects). This output is available if case defrost type is Electric.
-
-#### Refrigeration Zone Air Chiller Sensible Heat Ratio
-
-This field is the Sensible Cooling Energy  Rate divided by the Total Cooling Energy Rate.
-
-#### Refrigeration Zone Air Chiller Frost Accumulation Mass [kg]
-
-This field is the total amount of frost present on the coil during the timestep being reported.
-
-#### Refrigeration Zone Air Chiller Zone Total Cooling Rate [W]
-
-This field is the rate of total cooling delivered to the zone in Watts. A positive value is reported when the zone is cooled by the air chiller, otherwise a zero is reported.
-
-#### Refrigeration Zone Air Chiller Zone Total Cooling Energy  [J]
-
-This field is the amount of total cooling energy delivered to the zone in Joules. A positive value is reported when the zone is cooled by the air chiller, otherwise a zero is reported.
-
-#### Refrigeration Zone Air Chiller Zone Sensible Cooling Rate [W]
-
-This field is the rate of sensible cooling delivered to the zone in Watts. A positive value is reported when the zone is cooled by the air chiller, otherwise a zero is reported.
-
-#### Refrigeration Zone Air Chiller Zone Sensible Cooling Energy [J]
-
-This field is the amount of sensible cooling energy delivered to the zone in Joules. A positive value is reported when the zone is cooled by the air chiller, otherwise a zero is reported.
-
-#### Refrigeration Zone Air Chiller Zone Heating Rate [W]
-
-This field is the rate of sensible heating delivered to the zone in Watts. A positive value is reported when the zone is heated by the air chiller (typically only occurs during defrost), otherwise a zero is reported.
-
-#### Refrigeration Zone Air Chiller Zone Heating Energy [J]
-
-This field is the amount of sensible heating energy delivered to the zone in Joules. A positive value is reported when the zone is heated by the air chiller (typically only occurs during defrost), otherwise a zero is reported.
-
-*The following output variables are available for each zone served by any Air Chiller. An output variable identification is created for each zone exchanging energy with the Air Chiller.  For example if the Air Chiller, “DairyRefrigeration chiller�, were exchanging energy with the zone, “SalesArea�, the output variable identification would be “DairyRefrigeration chillerInZoneSalesArea�.*
-
-#### Refrigeration Zone Air Chiller Sensible Cooling Rate  [W]
-
-This field is the rate of sensible cooling delivered to the zone, net of any auxiliary heat input,  in Watts..
-
-#### Refrigeration Zone Air Chiller Sensible Cooling Energy [J]
-
-This field is the amount of sensible cooling energy, net of any auxiliary heat input, delivered to the zone in Joules.
-
-#### Refrigeration Zone Air Chiller Latent Cooling Rate [W]
-
-This field is the rate of latent cooling (dehumidification) delivered to the zone in Watts. A negative value will be reported when the Air Chiller provides dehumidification (thereby reducing the zone latent load).
-
-#### Refrigeration Zone Air Chiller Water Removed Mass Flow Rate  [kg/s]
-
-This field is the rate of latent cooling (dehumidification) delivered to the zone in kg/s. A negative value (or zero) will be reported when the Air Chiller provides dehumidification (thereby reducing the zone latent load).
-
-#### Refrigeration Zone Air Chiller Latent Cooling Energy [J]
-
-This field is the amount of latent cooling (dehumidification) energy delivered to the zone in Joules. A negative value (or zero) will be reported when the Air Chiller provides dehumidification (thereby reducing the zone latent load).
-
-#### Refrigeration Zone Air Chiller Total Cooling Rate [W]
-
-This field is the total rate of cooling, sensible plus latent, delivered to the zone in Watts.
-
-#### Refrigeration Zone Air Chiller Total Cooling Energy [J]
-
-This field is the total amount of cooling, sensible plus latent, energy delivered to the zone in Joules.
-
-#### Refrigeration Zone Air Chiller Heating Rate  [W]
-
-This field is the rate of net heating due to any auxiliary or defrost heat input delivered to the zone,  in Watts.
-
-#### Refrigeration Zone Air Chiller Heating Energy [J]
-
-This field is the amount of net heating energy due to any auxiliary heat input, delivered to the zone in Joules.
-
diff --git a/doc/src/docs/InputOutputReference/01d-InputOutputReference.md b/doc/src/docs/InputOutputReference/01d-InputOutputReference.md
deleted file mode 100644
index 51a4983ab33..00000000000
--- a/doc/src/docs/InputOutputReference/01d-InputOutputReference.md
+++ /dev/null
@@ -1,29279 +0,0 @@
-Group - Zone Controls - Thermostats and Humidistats
----------------------------------------------------
-
-Zone Control objects are used to control zone conditions to a specific setpoint. The six types of zone control are described in this section. They are, by name, ZoneControl:**&lt;name&gt;.**. These types are:
-
-**Thermostat** - The object provides the traditional approach to space control using air temperatures. Each controlled zone contains a thermostat object.
-
-**Humidistat** - The object is used to control a zone to a specified relative humidity.
-
-**Thermostat:ThermalComfort** - The object provides a method to control a zone to a dry-bulb temperature setpoint based on a thermal comfort model (e.g. Fanger) and a user-specified thermal comfort setpoint schedule.
-
-**Thermostat:OperativeTemperature** - The operative temperature control is formulated to reuse all of the traditional thermostat objects. One input object will be used for each thermal zone to indicate if that zone   s thermostat control mode should be overridden to effect operative temperature control rather than traditional air temperature control. The user will still have to input all the traditional ZoneControl:Thermostat and setpoint objects.
-
-**Thermostat:TemperatureAndHumidity** - This thermostat control works together with the traditional ZoneControl:Thermostat object to modify temperature control based on zone air humidity conditions. Currently, this object resets the thermostat   s cooling setpoint temperature downward based on elevated zone air humidity levels, typically yielding additional cooling coil operation and associated dehumidification. A ZoneControl:Thermostat:TemperatureAndHumidity object should be specified to indicate if a zone   s traditional thermostat control mode should be overridden to provide enhanced dehumidification. The user must still input the traditional ZoneControl:Thermostat and setpoint objects.
-
-**Thermostat**:**StagedDualSetpoint** - This thermostat control works alone with "Dual Setpoint" type only. The object provides heating and cooling setpoints, throttling range and offsets, so that zone temperature setpoint used for system load calculation is adjusted by the setpoint and throttling range based on the zone temperature at the previous time step. The stage number is determined by the temperature difference between the setpoint and zone temperature at the previous time step, and offset values. If this object and other zone control thermostat and humidistat are assigned to the same controlled zone, this object takes precedence when the controlled zone is specified in the Controlling Zone or Thermostat Location field of the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object.
-
-
-
-### ZoneControl:Thermostat
-
-The thermostatic zone control object is used to control a zone to a specified temperature. ZoneControl:Thermostat references a control type schedule and one or more control type objects which in turn reference one or more setpoint schedules. The example at the end of this section illustrates a complete zone thermostat specification including the control type and setpoint schedules.
-
-The control type schedule and the list of control type/name pairs are directly related. The schedule defines the type of control that is to be used throughout the simulation. Valid Control Types are:
-
-0 - Uncontrolled (No specification or default)
-
-1 - Single Heating Setpoint
-
-2 - Single Cooling SetPoint
-
-3 - Single Heating/Cooling Setpoint
-
-4 - Dual Setpoint (Heating and Cooling) with deadband
-
-Thus, if the schedule referenced in the ZoneControl:Thermostat statement has a control type of 4 for a particular time period, this indicates that during that time period "Dual Setpoint with deadband" control is to be used. The specific "Dual Setpoint (Heating and Cooling) with deadband" control object to be used is specified in the list of control type/name pairs. Then the specific control type objects reference the thermostat setpoint temperature schedule to be used. Because only one control can be specified for each control type in a ZoneControl:Thermostat statement, there are only four pairs possible in a particular ZoneControl:Thermostat type/name list. This is because individual controls can be defined throughout the simulation, thus giving the user a full range of flexibility. Since putting in the name of the control type directly in the schedule would be very cumbersome, the control types are assigned a number which is used in the schedule profile.
-
-#### Field: Name
-
-Unique identifying name for the thermostat.
-
-#### Field: Zone or ZoneList Name
-
-Name of the zone or set of zones that is being controlled. When the ZoneList option is used then this thermostat definition is applied to each of the zones in the zone list effecting a global definition for thermostatic control in the zone.
-
-#### Field: Control Type Schedule Name
-
-Schedule which defines what type of control is active during the simulation. Valid Control Types are:
-
-0 - Uncontrolled (No specification or default)
-
-1 - Single Heating Setpoint
-
-2 - Single Cooling SetPoint
-
-3 - Single Heating Cooling Setpoint
-
-4 - Dual Setpoint with Deadband (Heating and Cooling)
-
-Each non-zero control type which is used in this schedule must appear in the following fields which list the specific thermostat control objects to be used for this zone.
-
-#### Field Set (Control Object Type, Control Name)
-
-Up to four pairs of Control Object Type and Control Name may be listed to specify which control objects are used for this zone. This list is not order-dependent, and the position in this list has no impact on the control type schedule. In the control type schedule, a value of 1 always means "Single Heating Setpoint", even if that control type is not first in this list.
-
-#### Field: Control Object &lt;x&gt;Type
-
-This field specifies the control type to be used for this zone. Available control types are:
-
-ThermostatSetpoint:SingleHeating
-
-ThermostatSetpoint:SingleCooling
-
-ThermostatSetpoint:SingleHeatingOrCooling
-
-ThermostatSetpoint:DualSetpoint
-
-#### Field: Control &lt;x&gt; Name
-
-The corresponding control type name. The name is used in an object with the name of the control type and specifies the schedule.
-
-An example of this statement in an IDF is:
-
-```idf
-ZoneControl:Thermostat, Zone 3 Thermostat, NORTH ZONE,
-               Zone Control Type Sched,
-               DUAL SETPOINT WITH DEADBAND, VAV Setpoints;
-```
-
-An example of a global thermostat:
-
-```idf
-   ZoneList,AllControlledZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
-
-   ZoneControl:Thermostat,
-       AllControlledZones Thermostat,               !- Name
-       AllControlledZones,                               !- Zone Name
-       Zone Control Type Sched, !- Control Type Schedule Name
-       ThermostatSetpoint:SingleCooling,   !- Control 1 Object Type
-       CoolingSetPoint,                 !- Control 1 Name
-       ThermostatSetpoint:SingleHeating,   !- Control 2 Object Type
-       HeatingSetpoint,                 !- Control 2 Name
-       ThermostatSetpoint:DualSetpoint,   !- Control 3 Object Type
-       DualSetPoint;                       !- Control 3 Name
-```
-
-A complete zone thermostat example showing this statement and all of the objects it must reference is:
-
-```idf
-! Zone control object which links thermostats to a particular zone
-       ZoneControl:Thermostat, Zone 2 Thermostat, EAST ZONE,
-               Zone Control Type Sched,
-               ThermostatSetpoint:SingleCooling, Cooling Setpoint with SB,
-               ThermostatSetpoint:SingleHeating; Heating Setpoint with SB;
-
-! Control type objects     these may be used in more than one zone
-       ThermostatSetpoint:SingleCooling,
-               Cooling Setpoint with SB,
-               Cooling Setpoints;
-
-       ThermostatSetpoint:SingleHeating,
-               Heating Setpoint with SB,
-               Heating Setpoints;
-
-! Schedule type definitions
-       ScheduleTypeLimits,Temperature,-60:200,CONTINUOUS;
-       ScheduleTypeLimits,Control Type,0:4,DISCRETE;
-
-! Control type schedule definition
-       Schedule:Compact, Zone Control Type Sched, Control Type,
-               Through: 3/31,
-               For: AllDays,
-               Until: 24:00, 1,   !- Single Heating
-               Through: 9/30,
-               For: AllDays,
-               Until: 24:00, 2,   !- Single Cooling
-               Through: 12/31,
-               For: AllDays,
-               Until: 24:00, 1;   !- Single Heating
-
-! Heating setpoint schedule definition
-       Schedule:Compact, Heating Setpoints, Temperature,
-               Through: 12/31,
-               For: AllDays,
-               Until: 7:00, 15.,
-               Until: 17:00,20.,
-               Until: 24:00,15.;
-
-! Cooling setpoint schedule definition
-       Schedule:Compact, Cooling Setpoints, Temperature,
-               Through: 12/31,
-               For: AllDays,
-               Until: 7:00, 30.,
-               Until: 20:00,23.,
-               Until: 24:00,30.;
-```
-
-### ZoneControl Thermostat Outputs
-
-Outputs available from controlled zones. The "key" in the below is the Zone Name.
-
-* HVAC,Average,Zone Predicted Sensible Load to Setpoint Heat Transfer Rate [W]
-
-* HVAC,Average,Zone Predicted Sensible Load to Heating Setpoint Heat Transfer Rate [W]
-
-* HVAC,Average,Zone Predicted Sensible Load to Cooling Setpoint Heat Transfer Rate [W]
-
-* Zone,Average,Zone Thermostat Control Type []
-
-* Zone,Average,Zone Thermostat Heating Setpoint Temperature [C]
-
-* Zone,Average,Zone Thermostat Cooling Setpoint Temperature [C]
-
-* HVAC,Sum,Facility Any Zone Oscillating Temperatures Time [hr]
-
-* Zone,Sum,Zone Heating Setpoint Not Met Time [hr]
-
-* Zone,Sum,Zone Heating Setpoint Not Met While Occupied Time [hr]
-
-* Zone,Sum,Zone Cooling Setpoint Not Met Time [hr]
-
-* Zone,Sum,Zone Cooling Setpoint Not Met While Occupied Time [hr]
-
-* Zone,Sum,Facility Heating Setpoint Not Met Time [hr]
-
-* Zone,Sum,Facility Cooling Setpoint Not Met Time [hr]
-
-* Zone,Sum,Facility Heating Setpoint Not Met While Occupied Time [hr]
-
-* Zone,Sum,Facility Cooling Setpoint Not Met While Occupied Time [hr]
-
-
-
-#### Zone Predicted Sensible Load to Setpoint Heat Transfer Rate [W]
-
-This is the predicted sensible load in W required to meet the current zone thermostat setpoint. A positive value indicates a heating load, a negative value indicates a cooling load. This is calculated and reported from the Predict step in the Zone Predictor-Corrector module. For nearly all equipment types, the Predictor-Corrector evaluates the active heating and/or cooling setpoints, determines if the zone requires heating or cooling or is in the deadband, and then passes this single load to the equipment. This value is not multiplied by zone or group multipliers.
-
-#### Zone Predicted Sensible Load to Heating Setpoint Heat Transfer Rate [W]
-
-This is the predicted sensible load in W required to meet the current zone thermostat heating setpoint. A positive value indicates a heating load, a negative value indicates a cooling load. This is calculated and reported from the Predict step in the Zone Predictor-Corrector module. This value is not multiplied by zone or group multipliers.
-
-#### Zone Predicted Sensible Load to Cooling Setpoint Heat Transfer Rate [W]
-
-This is the predicted sensible load in W required to meet the current zone thermostat cooling setpoint. A positive value indicates a heating load, a negative value indicates a cooling load. This is calculated and reported from the Predict step in the Zone Predictor-Corrector module. This value is not multiplied by zone or group multipliers.
-
-#### Zone Thermostat Control Type []
-
-This is the current zone thermostat control type (0 through 4). This value is set at each zone timestep. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
-
-#### Zone Thermostat Heating Setpoint Temperature [C]
-
-This is the current zone thermostat heating setpoint in degrees C. If there is no heating thermostat active, then the value will be 0. This value is set at each zone timestep. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
-
-When the Thermostat:StagedDualSetpoint object is applied to the current zone, this output variable reports staged zone heating setpoint. When the staged number is not equal to zero, both staged heating and cooling setpoints are the same. When no cooling or heating is required, the staged heating setpoint is equal to the scheduled heating setpoint     0.5 \* heating throttling range, and the staged cooling setpoint is equal to the scheduled cooling setpoint + 0.5 \* cooling throttling range.
-
-#### Zone Thermostat Cooling Setpoint Temperature [C]
-
-This is the current zone thermostat cooling setpoint in degrees C. If there is no cooling thermostat active, then the value will be 0. This value is set at each zone timestep. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
-
-When the Thermostat:StagedDualSetpoint object is applied to the current zone, this output variable reports staged zone cooling setpoint. When the staged number is not equal to zero, both staged heating and cooling setpoints are the same. When no cooling or heating is required, the staged heating setpoint is equal to the scheduled heating setpoint     0.5 \* heating throttling range, and the staged cooling setpoint is equal to the scheduled cooling setpoint + 0.5 \* cooling throttling range.
-
-#### Zone Thermostat Stage Number []
-
-This is the current zone thermostat stage number when the ZoneControl:Thermostat:StagedDualSetpoint object is specified in this zone. When no heating or cooling is required, the stage number is set to 0. When heating is required, the stage number is positive. When cooling is required, the stage number is negative. The absolute number is sent to the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object to specify the speed number accordingly.
-
-#### Zone Heating Setpoint Not Met Time [hr]
-
-Hours when the zone temperature is lower than 0.2 (default) degrees C below the heating setpoint. See the OutputControl:ReportingTolerances object to change the reporting range from 0.2 degrees C.
-
-#### Zone Heating Setpoint Not Met While Occupied Time [hr]
-
-Hours when the zone temperature is lower than 0.2 (default) degrees C below the heating setpoint and when people are present in the zone. To change the reporting range from 0.2 degrees C, see the OutputControl:ReportingTolerances object.
-
-#### Zone Cooling Setpoint Not Met Time [hr]
-
-Hours when the zone temperature is greater than 0.2 (default) degrees C above the cooling setpoint. See the OutputControl:ReportingTolerances object to change the reporting range from 0.2 degrees C.
-
-#### Zone Cooling Setpoint Not Met While Occupied Time [hr]
-
-Hours when the zone temperature is greater than 0.2 (default) degrees C above the cooling setpoint and when people are present in the zone. To change the reporting range from 0.2 degrees C, see the OutputControl:ReportingTolerances object.
-
-#### Facility Heating Setpoint Not Met Time [hr]
-
-Hours when the zone temperature is lower than 0.2 (default) degrees C below the heating setpoint in any one or more zones. See the OutputControl:ReportingTolerances object to change the reporting range from 0.2 degrees C.
-
-#### Facility Heating Setpoint Not Met While Occupied Time [hr]
-
-Hours when the zone temperature is lower than 0.2 (default) degrees C below the heating setpoint and when people are present in any one or more zones. To change the reporting range from 0.2 degrees C, see the OutputControl:ReportingTolerances object.
-
-#### Facility Cooling Setpoint Not Met Time [hr]
-
-Hours when the zone temperature is greater than 0.2 (default) degrees C above the cooling setpoint in any one or more zones. See the OutputControl:ReportingTolerances object to change the reporting range from 0.2 degrees C.
-
-#### Facility Cooling Setpoint Not Met While Occupied Time [hr]
-
-Hours when the zone temperature is greater than 0.2 (default) degrees C above the cooling setpoint and when people are present in any one or more zones. To change the reporting range from 0.2 degrees C, see the OutputControl:ReportingTolerances object.
-
-#### Zone Oscillating Temperatures Time[hr]
-
-Hours when the temperature in the zone is oscillating back and forth. Oscillation is defined as times when the three differences between zone temperatures during successive timesteps are greater in magnitude than 0.15 degrees C and the sign of the differences changes from positive to negative to positive or from negative to positive to negative.
-
-This may indicate a simulation with reduced reliability during the oscillation. Some oscillating hours should be expected in all simulations but excessive oscillations call into question the overall validity of the results. If excessive oscillations are occurring, try reducing the minimum system timestep (see ConvergenceLimits object) and the zone timestep (see the TimeStep object). Reducing these timestep lengths does increase the total computer time needed to complete the simulation. Having the zone timestep and the minimum system timestep the same length of time can also cause more oscillations. What amount of oscillations is considered    excessive    is difficult to quantify. One approach is comparing the number of oscillations to the case with 15 minute zone timesteps (4 per hour) and 1 minute minimum system timesteps. Often this variable is used as an indicator of the validity of the results when trying to decrease the time needed to perform the simulation.
-
-#### Facility Any Zone Oscillating Temperatures Time[hr]
-
-Hours when any zone in the building has oscillations. See Zone Oscillating Temperatures Time definition above.
-
-### Zone Thermostat Setpoints
-
-The syntax for the current set of four zone thermostat setpoint objects is given below. In each case, the keyword is accompanied by an identifying name and either one or two schedule names (depending on whether the control is a single or dual setpoint control). The schedule defines a temperature setpoint for the control type. The schedule would be defined through the standard schedule syntax described earlier in this document. For an uncontrolled zone no thermostat is specified or necessary.
-
-### ThermostatSetpoint:SingleHeating
-
-This would be for a heating only thermostat. The setpoint can be scheduled and varied throughout the simulation but only heating is allowed with this control type.
-
-#### Field: Name
-
-Unique name for this control type.
-
-#### Field: Setpoint Temperature Schedule Name
-
-The name of the associated schedule. Values in the schedule are temperatures {C}.
-
-### ThermostatSetpoint:SingleCooling
-
-This would be for a cooling only thermostat. The setpoint can be scheduled and varied throughout the simulation but only cooling is allowed.
-
-#### Field: Name
-
-Unique name for this control type.
-
-#### Field: Setpoint Temperature Schedule Name
-
-The name of the associated schedule. Values in the schedule are temperatures {C}.
-
-### ThermostatSetpoint:SingleHeatingOrCooling
-
-This would be for heating and cooling thermostat but only heating or cooling can be scheduled at any given time period. The setpoint can be scheduled and varied throughout the simulation for both heating and cooling.
-
-#### Field: Name
-
-Unique name for this control type.
-
-#### Field: Setpoint Temperature Schedule Name
-
-The name of the associated schedule. Values in the schedule are temperatures {C}.
-
-### ThermostatSetpoint:DualSetpoint
-
-This would be for heating and cooling thermostat where both a heating and cooling setpoint can be scheduled for any given time period. The setpoint can be scheduled and varied throughout the simulation for both heating and cooling.
-
-#### Field: Name
-
-Unique name for this control type.
-
-#### Field: Heating Setpoint Temperature Schedule Name
-
-The heating temperature schedule. Values in the schedule are temperatures {C}.
-
-#### Field: Cooling Setpoint Temperature Schedule Name
-
-The cooling temperature schedule. Values in the schedule are temperatures {C}.
-
-Examples of these statements in an IDF are:
-
-```idf
-ThermostatSetpoint:SingleHeating, Heating Setpoint with SB, Heating Setpoints;
-ThermostatSetpoint:SingleCooling, Cooling Setpoint with SB, Cooling Setpoints;
-ThermostatSetpoint:SingleHeatingOrCooling, Heating Cooling Setpoint Sched, Heating Cooling Setpoints;
-ThermostatSetpoint:DualSetpoint, VAV Setpoints, Heating Setpoints, Cooling Setpoints;
-```
-
-### ZoneControl:Thermostat:OperativeTemperature
-
-This object is used to modify the program   s behavior for ZoneControl:Thermostat objects. One input object is used for each thermal zone to indicate if that zone   s thermostat control mode should be overridden to effect operative temperature control rather than traditional air temperature control. Zone Control:Thermostatic and related set point objects also need to be included in the input file. When this object is used, the zone can be controlled by a weighted mixture of radiant and air temperatures (rather than just air temperatures).
-
-This thermostatic operative temperature, <span>\({T_{OP}}\)</span>, is defined as:
-
-<div>\[{T_{OP}} = \gamma {T_{MRT}} + (1 - \gamma ){T_{drybulb}}\]</div>
-
-where,
-
-<span>\(\gamma \)</span>   is the radiative fraction,
-
-<span>\({T_{MRT}}\)</span>  is the mean radiant temperature for the thermal zone, and
-
-<span>\({T_{drybulb}}\)</span>is the mean zone air temperature.
-
-The radiative fraction <span>\(\gamma \)</span>  is selected by the user and can be scheduled to vary during the simulation. A typical value is 0.5. The maximum value needs to be less than 0.9 and the minimum is 0.0. A value of 0.0 is the same as controlling on only zone air temperature. If air velocities are higher than 0.2 m/s, then lower values for radiative fraction might apply. Niu and Burnett (1998) cite International Standard ISO 77300 in recommending the values for this fraction listed in the following table.
-
-Table 28. Radiative Fraction vs Air Velocity (Operative Temperature Control)
-
-<table class="table table-striped">
-<tr>
-<th>Air Velocity (m/s)</th>
-<th>&lt; 0.2</th>
-<th>0.2 to 0.6</th>
-<th>0.6 to 1.0</th>
-</tr>
-<tr>
-<td><span>\(\gamma \)</span></td>
-<td>0.5</td>
-<td>0.4</td>
-<td>0.3</td>
-</tr>
-</table>
-
-
-
-Reference: J. Niu and J. Burnett. 1998. Integrating Radiant/Operative Temperature Controls into Building Energy Simulations. ASHRAE Transactions Vol. 104. Part 2. page 210. ASHRAE. Atlanta, GA.
-
-#### Field: Thermostat Name
-
-Name of ZoneControl:Thermostat object defined elsewhere in the input file whose operation is to be modified to effect control based on operative temperature. If the ZoneControl:Thermostat references a ZoneList (set of zones) then, this operative temperature thermostat will be applied to each of those zones. If only a single thermostat/zone is desired, then the name to be put here is &lt;zone name&gt; &lt;Thermostat Name&gt; where the Thermostat name is the thermostat that referenced the set of zones.
-
-#### Field: Radiative Fraction Input Mode
-
-This field controls whether the input for radiative fraction is a constant value or if it is entered using a schedule. Enter    **Constant**    here to use a fixed radiative fraction defined in the following field. Enter    **Scheduled**    to vary the radiative fraction according to the schedule named in the second field below.
-
-#### Field: Fixed Radiative Fraction
-
-This is the fraction, <span>\(\gamma \)</span>, of the operative temperature that is due to the mean radiant temperature in the zone. This field is used by the program if the previous field is set to **Constant**.
-
-#### Field: Radiative Fraction Schedule Name
-
-This field contains the name of a schedule, defined elsewhere, that determines the value for radiative fraction <span>\(\gamma \)</span>  during the simulation period. This schedule should have fractional values from 0.0 to 0.9. When the value of this schedule is 0.0, the controlling will be equivalent to control based only on zone air temperature. This field is used by the program if the Input Mode field is set to **Scheduled**.
-
-Note that by setting the values in this schedule separately for design days, the user can control how operative temperature control is applied during autosizing. (Operative temperature control tends to increase the equipment capacities calculated during sizing.)
-
-An example of this object follows.
-
-```idf
-ZoneControl:Thermostat:OperativeTemperature,
-Zone 1 Thermostat,   !- ZoneControl:Thermostat Name
-Constant,                     !- Radiative Fraction Input Mode
-0.5,                               !- Fixed Radiative Fraction
-;   !- Radiative Fraction Schedule
-```
-
-
-Global operative temperature applied to all zones for a global thermostat:
-
-```idf
-ZoneList,AllControlledZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
-
-
-ZoneControl:Thermostat,
- AllControlledZones Thermostat,               !- Name
- AllControlledZones,                               !- Zone Name
- Zone Control Type Sched, !- Control Type Schedule Name
- ThermostatSetpoint:SingleCooling,   !- Control 1 Object Type
- CoolingSetPoint,                 !- Control 1 Name
- ThermostatSetpoint:SingleHeating,   !- Control 2 Object Type
- HeatingSetpoint,                 !- Control 2 Name
- ThermostatSetpoint:DualSetpoint,   !- Control 3 Object Type
- DualSetPoint;                       !- Control 3 Name
-
-
-ZoneControl:Thermostat:OperativeTemperature,
- AllControlledZones Thermostat,               !- Thermostat Name
- CONSTANT,                               !- Radiative Fraction Input Mode
- 0.4;                                         !- Fixed Radiative Fraction
-```
-
-
-Global operative temperature referencing a single zone from the list:
-
-```idf
-ZoneList,AllControlledZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
-```
-
-```idf
-
-ZoneControl:Thermostat,
- AllControlledZones Thermostat,               !- Name
- AllControlledZones,                               !- Zone Name
- Zone Control Type Sched, !- Control Type Schedule Name
- ThermostatSetpoint:SingleCooling,   !- Control 1 Object Type
- CoolingSetPoint,                 !- Control 1 Name
- ThermostatSetpoint:SingleHeating,   !- Control 2 Object Type
- HeatingSetpoint,                 !- Control 2 Name
- ThermostatSetpoint:DualSetpoint,   !- Control 3 Object Type
- DualSetPoint;                       !- Control 3 Name
-
-
-ZoneControl:Thermostat:OperativeTemperature,
- SPACE3-1 AllControlledZones Thermostat,               !- Thermostat Name
- CONSTANT,                               !- Radiative Fraction Input Mode
- 0.4;                                         !- Fixed Radiative Fraction
-```
-
-
-
-### Zone Control Themostatic Operative Temperature Outputs
-
-* Zone,Average,Zone Thermostat Operative Temperature [C]
-
-#### Zone Thermostat Operative Temperature [C]
-
-Operative temperature (OT) is a weighted mixture of Zone Mean Air Temperature (MAT) and Zone Mean Radiant Temperature (MRT), using the current value of Radiative Fraction (RF):   OT = (1-RF)\*MAT + RF\*MAT.   This output variable does not include the direct effect of high temperature radiant systems.   See also Zone Operative Temperature.
-
-### ZoneControl:Thermostat:TemperatureAndHumidity
-
-This object is used to modify the behavior of ZoneControl:Thermostat objects (control types ThermostatSetpoint:SingleCooling and ThermostatSetpoint:DualSetpoint only) based on zone air humidity conditions. Specifically, this TemperatureAndHumidity zone control resets the ZoneControl:Thermostat   s cooling setpoint temperature downward when the zone air relative humidity exceeds the Dehumidifying Relative Humidity Setpoint defined in this object. The reduced cooling setpoint temperature typically results in longer cooling coil runtimes and additional dehumidification. The rate at which the cooling setpoint temperature is reduced is dictated by the user-specified Overcool Control Ratio. The maximum reduction in cooling setpoint temperature is defined by the user-entered OverCool Range (user choice of a constant value for the entire simulation or a schedule that can define how the overcool range varies over time). For details regarding the calculations, see the EnergyPlus Engineering Reference.
-
-Note: As described above, this ZoneControl:Thermostat:TemperatureAndHumidity control object modifies the cooling setpoint temperature of ZoneControl:Thermostat objects. The ZoneControl:Thermostat:TemperatureAndHumidity   object works independently of the ZoneControl:Humidistat object; that is, it does not replace the need for, or coordinate its input fields with, ZoneControl:Humidistat objects that are required for other types of high humidity control (e.g., ZoneControl:Humidstat objects are required for ZoneHVAC:Dehumidifier:DX objects, AirLoopHVAC:Unitary\* objects with    CoolReheat    or    MultiMode    dehumidification control types, etc.)
-
-#### Field: Thermostat Name
-
-Name of ZoneControl:Thermostat object defined elsewhere in the input file whose operation is to be modified to effect temperature control based on zone air humidity conditions. If the ZoneControl:Thermostat references a ZoneList (set of zones), then simply enter the name of the ZoneControl:Thermostat object and this TemperatureAndHumidity thermostat control will be applied to all zones in the ZoneList. If the ZoneControl:Thermostat references a ZoneList but it is desired that only a single zone within the ZoneList be controlled based on TemperatureAndHumidity control, then the name to be put here is &lt;zone name&gt; &lt;Thermostat Name&gt; where the Thermostat Name is the name of the ZoneControl:Thermostat object.
-
-#### Field: Dehumidifying Relative Humidity Setpoint Schedule Name
-
-Name of a schedule that defines the dehumidifying relative humidity setpoint, expressed as a percentage (0-100), for each timestep of the simulation. This input field is required.   This input field has absolutely no relationship or influence on the Dehumidifying Relative Humidity Setpoint Schedule Name optional input field in the ZoneControl:Humidistat object.
-
-#### Field:Dehumidification Control Type
-
-This input field defines what type of dehumidification control is active during the simulation. Valid control types are None and Overcool. The default is Overcool if this field is left blank.   Overcool resets the thermostat   s cooling setpoint temperature lower based on the zone air relative humidity level. None means no overcooling (i.e., traditional zone air temperature control based on the associated ZoneControl:Thermostat object [Thermostat Name input field above] will be in effect).
-
-#### Field: Overcool Range Input Method
-
-This field controls whether the input for the overcool (temperature) range is a constant value or if it is entered using a schedule. Enter    **Constant**    here to use a constant overcool range defined in the    Overcool Constant Range    input field below. Enter    **Scheduled**    to vary the overcool range according to the schedule named in the    Overcool Range Schedule Name    input field below. The default is    **Constant**    if this field is left blank.
-
-#### Field: Overcool Constant Range
-
-This field specifies a fixed maximum overcool temperature range for cooling setpoint temperature reduction for zone overcool dehumidification in units of deltaC.   This field is used if the Overcool Range Input Method is specified as **Constant**. The Overcool dehumidification control type only works with ZoneControl:Thermostat control types    ThermostatSetpoint:SingleCooling    and    ThermostatSetpoint:DualSetpoint   .   For    ThermostatSetpoint:DualSetpoint   ,   the model will use the **smaller** of the Overcool Constant Range input value or the difference between the cooling and heating setpoint temperatures specified in the    ThermostatSetpoint:DualSetpoint    object. The Overcool Constant Range must be greater than or equal to zero with a maximum value of 3 &deg;C.   A value of 0.0 indicates no zone air overcooling. The default value is 1.7 &deg;C (3 &deg;F) if this input field is left blank.
-
-#### Field: Overcool Range Schedule Name
-
-This field contains the name of a schedule, defined elsewhere, that determines the value for the overcool range during the simulation period. This schedule should contain values from 0.0 to &lt;=3.0 (deltaC). When the value of this schedule is 0.0, the zone air temperature control will be based only on zone air dry-bulb temperature (i.e., no zone overcooling). This field is used by the program if the Overcool Range Input Method field is set to **Scheduled**. Overcool dehumidification control type only works with ZoneControl:Thermostat control types    ThermostatSetpoint:SingleCooling    and    ThermostatSetpoint:DualSetpoint   .   For    ThermostatSetpoint:DualSetpoint   ,   the model will use the **smaller** of the Overcool Range values specified in this schedule or the difference between the cooling and heating setpoint temperatures specified in the    ThermostatSetpoint:DualSetpoint    object.
-
-Note that by setting the values in this schedule separately for design days, the user can control how Overcool Dehumidification Control is applied during autosizing. (Overcool dehumidification control tends to increase the cooling equipment capacities calculated during sizing.)
-
-#### Field:Overcool Control Ratio
-
-The value of this input field is used to adjust the cooling setpoint temperature (established by the associated ZoneControl:Thermostat object) downward based on the difference between the zone air relative humidity level and the Dehumidifying Relative Humidity Setpoint. This input field is only used with Dehumidification Control Type = Overcool.   Input values must be greater than or equal to 0.0 %RH/K. The default value is 3.6 if this field is left blank.
-
-An example of this object follows.
-
-```idf
-ZoneControl:Thermostat:TemperatureAndHumidity,
-       Zone Thermostat,                                 !- Thermostat Name
-       Seasonal Relative Humidity Sch,   !- Dehumidifying Relative Humidity Setpoint Schedule Name
-       Overcool,                                               !- Dehumidification Control Type
-       Constant,                                               !- Overcool Range Input Method
-       1.7,                                         !- Overcool Constant Range {deltaC}
-       ,                                               !- Overcool Range Schedule Name
-       3.0;                                         !- Overcool Control Ratio {percent/K}
-```
-
-
-### ZoneControl:Thermostat:StagedDualSetpoint
-
-The thermostatic zone control staged dual setpoint object is used to control a zone to a specified temperature based on multiple stages. The other types of ZoneControl:Thermostat objects reference a control type schedule and one or more control type objects which in turn reference one or more setpoint schedules. This control object does not require a control type schedule and associated one or more control type objects. Instead, the object is defined as a    Dual Setpoint    type only and has two fields to provide heating and cooling setpoints. The object also provides two fields to specify heating and cooling throttling temperature ranges, so that predicted zone loads may be varied within the throttling ranges for both heating and cooling. The number of stages for both heating and cooling varies from 1 to 4 for the time being to match the number of speeds used in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. The number of stages may be expanded later to accommodate other objects with the number of speeds higher than 4. The object requires inputs temperature offsets for both heating and cooling based on the number of stages. The stage number is determined by the temperature difference between the setpoint and zone temperature at the previous time step, and offset values. The staged number will be assigned to the speed number for the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed system type.
-
-It should be pointed out that If this object and other zone control thermostat and humidistat are assigned to the same controlled zone, this object takes precedence when the controlled zone is specified in the Controlling Zone or Thermostat Location field of the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object.
-
-#### Field: Name
-
-Unique identifying name for the staged dual-setpoint thermostat.
-
-#### Field: Zone or ZoneList Name
-
-Name of the zone or set of zones that is being controlled. When the ZoneList option is used then this thermostat definition is applied to each of the zones in the zone list effecting a global definition for thermostatic control in the zone.
-
-#### Field: Number of Heating Stages
-
-This numerical field defines the number of heating stages, and must be less than or equal to the number of heating speeds defined in the associated heating coil, such as Coil:Heating:DX:MultiSpeed. The value for this input field defines the number of heating temperature offsets that must be defined for heating in the fields below. The minimum value for this field is one (1) and the maximum value is four (4).
-
-#### Field:Heating Temperature Setpoint Schedule Name
-
-The name of the associated schedule to specify heating temperature setpoint. Values in the schedule are temperatures {C}.
-
-#### Field:Heating Throttling Temperature Range
-
-This numeric field defines the heating throttling temperature range in the units of deltaC. When the zone temperature at the previous time step is below the heating temperature setpoint, the zone heating setpoint will be set to the heating temperature setpoint + 0.5 \* heating throttling temperature range. Otherwise, the zone heating setpoint will be set to the heating temperature setpoint - 0.5 \* heating throttling temperature range. The zone heating setpoint is used in the predictor to calculate how much the heating system load is needed to maintain the zone at the heating setpoint.
-
-#### Field: Stage 1 Heating Temperature Offset
-
-This numeric field defines the heating temperature offset in the units of deltaC for Stage 1. The value entered here must be equal to or less than 0. The heating temperature offset fields are used to determine the heating stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference between the heating setpoint and the controlled zone temperature at previous time step is less than Stage 1 offset value and greater than Stage 2 offset value, the heating stage number is 1. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 1 is specified.
-
-#### Field: Stage 2 Heating Temperature Offset
-
-This numeric field defines the heating temperature offset in the units of deltaC for Stage 2. The value entered here must be less than the value at the previous field: Stage 1 Heating Temperature Offset. The heating temperature offset fields are used to determine the heating stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference between the heating setpoint and the controlled zone temperature at previous time step is less than Stage 2 offset value and greater than Stage 3 offset value, the heating stage number is 2. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 2 is specified.
-
-#### Field: Stage 3 Heating Temperature Offset
-
-This numeric field defines the heating temperature offset in the units of deltaC for Stage 3. The value entered here must be less than the value at the previous field: Stage 3 Heating Temperature Offset. The heating temperature offset fields are used to determine the heating stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference between the heating setpoint and the controlled zone temperature at previous time step is less than Stage 3 offset value and greater than Stage 4 offset value, the heating stage number is 3. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 3 is specified.
-
-Note: If the stage number is not equal to the number of heating speed in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object, the minimum value is set to the speed number for the heat pump object.
-
-#### Field: Stage 4 Heating Temperature Offset
-
-This numeric field defines the heating temperature offset in the units of deltaC for Stage 4. The value entered here must be less than the value at the previous field: Stage 4 Heating Temperature Offset. The heating temperature offset fields are used to determine the heating stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference between the heating setpoint and the controlled zone temperature at previous time step is less than Stage 4 offset value, the heating stage number is 4. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 4 is specified.
-
-Note: If the stage number is not equal to the number of heating speed in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object, the minimum value is set to the speed number for the heat pump object.
-
-#### Field: Number of Cooling Stages
-
-This field defines the number of cooling stages, and must be less than or equal to the number of cooling speeds defined in the associated cooling coil, such as Coil:Cooling:DX:MultiSpeed. The value for this input field defines the number of cooling temperature offsets that must be defined for cooling in the fields below. The minimum value for this field is one (1) and the maximum value is four (4).
-
-#### Field:Cooling Temperature Setpoint Base Schedule Name
-
-The name of the associated schedule to specify cooling temperature base setpoint. Values in the schedule are temperatures {C}.
-
-#### Field:Cooling Throttling Temperature Range
-
-This numeric field defines the cooling throttling temperature range in the units of deltaC. When the zone temperature at the previous time step is above the cooling temperature setpoint, the zone cooling setpoint will be set to the cooling temperature setpoint - 0.5 \* cooling throttling temperature range. Otherwise, the zone cooling setpoint will be set to the cooling temperature setpoint + 0.5 \* cooling throttling temperature range. The zone cooling setpoint is used in the predictor to calculate how much the cooling system load is needed to maintain the zone at the cooling setpoint.
-
-#### Field: Stage 1 Cooling Temperature Offset
-
-This numeric field defines the cooling temperature offset in the units of deltaC for Stage 1. The value entered here must be equal to or greater than 0. The cooling temperature offset fields are used to determine the cooling stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference of the cooling setpoint and the controlled zone temperature at previous time step is greater than Stage 1 offset value and less than Stage 2 offset value, the cooling stage number is 1. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 1 is specified.
-
-#### Field: Stage 2 Cooling Temperature Offset
-
-This numeric field defines the cooling temperature offset in the units of deltaC for Stage 2. The value entered here must be greater than the value at the previous field: Stage 1 Cooling Temperature Offset. When the number of cooling stage is equal to 1, this filed is not used in the program. The cooling temperature offset fields are used to determine the cooling stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference of the cooling setpoint and the controlled zone temperature at previous time step is greater than Stage 2 offset value and less than Stage 3 offset value, the cooling stage number is 2. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 2 is specified.
-
-#### Field: Stage 3 Cooling Temperature Offset
-
-This numeric field defines the cooling temperature offset in the units of deltaC for Stage 3. The value entered here must be greater than the value at the previous field: Stage 3 Cooling Temperature Offset. When the number of cooling stage is less than 3, this filed is not used in the program. The cooling temperature offset fields are used to determine the cooling stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference of the cooling setpoint and the controlled zone temperature at previous time step is greater than Stage 3 offset value and less than Stage 4 offset value, the cooling stage number is 3. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 3 is specified.
-
-Note: If the stage number is not equal to the number of cooling speed in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object, the minimum value is set to the speed number for the heat pump object.
-
-#### Field: Stage 4 Cooling Temperature Offset
-
-This numeric field defines the cooling temperature offset in the units of deltaC for Stage 4. The value entered here must be greater than the value at the previous field: Stage 4 Cooling Temperature Offset. When the number of cooling stage is less than 4, this filed is not used in the program. The cooling temperature offset fields are used to determine the cooling stage number for AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object. When the temperature difference of the cooling setpoint and the controlled zone temperature at previous time step is greater than Stage 4 offset value, the cooling stage number is 4. When the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object is called, Speed 4 is specified.
-
-Note: If the stage number is not equal to the number of cooling speed in the AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed object, the minimum value is set to the speed number for the heat pump object.
-
-An example of this statement in an IDF is:
-
-```idf
-ZoneControl:Thermostat:StagedDualSetpoint,
-       ZoneThermostat,                   !- Name
-       AllZones,                               !- Zone or ZoneList Name
-       2,                                             !- Number of Heating Stages
-       Heating Setpoints,             !- Heating Temperature Setpoint Schedule Name
-       1.1,                                         !- Heating Throttling Temperature Range {deltaC}
-       0.0,                                         !- Stage 1 Heating Temperature Offset {deltaC}
-       -0.5,                                       !- Stage 2 Heating Temperature Offset {deltaC}
-       -1.0,                                       !- Stage 3 Heating Temperature Offset {deltaC}
-       -1.5,                                       !- Stage 4 Heating Temperature Offset {deltaC}
-       4,                                             !- Number of Cooling Stages
-       Cooling Setpoints,             !- Cooling Setpoint Temperature Schedule Name
-       1.1,                                         !- Cooling Throttling Temperature Range {deltaC}
-       0.0,                                         !- Stage 1 Cooling Temperature Offset {deltaC}
-       1.0,                                         !- Stage 2 Cooling Temperature Offset {deltaC}
-       2.0,                                         !- Stage 3 Cooling Temperature Offset {deltaC}
-       3.0;                                         !- Stage 4 Cooling Temperature Offset {deltaC}
-```
-
-
-### ZoneControl:Humidistat
-
-The humidistat zone control object is used to control a zone to a single relative humidity setpoint schedule, or to dual humidity setpoint schedules (humidifying/ dehumidifying setpoints with deadband). The single setpoint humidistat requires single setpoint input only, and the dual-setpoint humidistat requires inputs of both humidifying and dehumidifying setpoints. The schedules consist of relative humidities, expressed as a percentage (0-100), to be used during the simulation for that zone   s moisture prediction calculation. Only one humidistat control statement can be specified for each zone. For a single setpoint humidistat, if the zone relative humidity is below the control relative humidity setpoint and the equipment specified can humidify then that equipment will try and meet the zone   s humidification load. The opposite is true if the zone relative humidity is above the control relative humidity setpoint and the equipment can dehumidify. For a dual setpoint humidistat, if the zone relative humidity is below the **humidifying** relative humidity setpoint and the equipment specified can humidify then that equipment will try and meet the zone   s humidification load. The opposite is true if the zone relative humidity is above the **dehumidifying** relative humidity setpoint and the equipment can dehumidify.
-
-If the ZoneControl:Humidistat is used by a furnace or unitary system (Ref. Furnace and Unitary Systems) no other objects are required. The signal from the humidistat is used directly by that component. If the Zone Control:Humidistat object is used to control a Humidifier or used in conjunction with a Controller:WaterCoil object with control variable **TemperatureAndHumidityRatio** or **HumidityRatio**, the following objects are required to determine a setpoint for those components for a single setpoint humidistat:
-
-- SetpointManager:SingleZone:Humidity:Minimum
-
-- SetpointManager:MultiZone:MinimumHumidity:Average
-
-- SetpointManager:MultiZone:MaximumHumidity:Average
-
-- SetpointManager:MultiZone:Humidity:Minimum
-
-- SetpointManager:MultiZone:Humidity:Maximum
-
-- SetpointManager:SingleZone:Humidity:Minimum
-
-For a dual setpoint humidistat, both a maximum humidity setpoint manager object:
-
-- SetpointManager:SingleZone:Humidity:Maximum
-
-- SetpointManager:MultiZone:MaximumHumidity:Average
-
-- SetpointManager:MultiZone:Humidity:Maximum
-
-and a minimum humidity setpoint manager object:
-
-- SetpointManager:SingleZone:Humidity:Minimum
-
-- SetpointManager:MultiZone:MinimumHumidity:Average
-
-- SetpointManager:MultiZone:Humidity:Minimum
-
-are required to determine the setpoints for the corresponding humidification and dehumidification components.
-
-#### Field: Name
-
-Unique identifying name for the humidistat.
-
-#### Field: Zone Name
-
-Name of the zone that is being controlled.
-
-#### Field: Humidifying Relative Humidity Setpoint Schedule Name
-
-Name of a schedule that defines the humidifying relative humidity setpoint, expressed as a percentage (0-100), for each timestep of the simulation.
-
-**Note**: If only a single setpoint humidistat is desired, then input the single schedule name in the Humidifying Setpoint Schedule Name field (and leave the Dehumidifying Setpoint Schedule Name blank).
-
-#### Field: Dehumidifying Relative Humidity Setpoint Schedule Name
-
-Name of a schedule that defines the dehumidifying relative humidity setpoint, expressed as a percentage (0-100), for each timestep of the simulation. This field is optional, only used if a dual setpoint humidistat is to be modeled.
-
-An example of this statement in an IDF is:
-
-```idf
-ZoneControl:Humidistat,
-       Zone 2 Humidistat,             !- Humidistat Name
-      EAST ZONE,                             !- Zone Name
-       Min Rel Hum Set Sch,       !- Humidifying Relative Humidity Setpoint SCHEDULE Name
-       Max Rel Hum Set Sch;       !- Dehumidifying Relative Humidity Setpoint SCHEDULE Name
-```
-
-
-An example schedule for the Zone Control:Humidistat
-
-```idf
-   ScheduleTypeLimits,Humidity,0:100,CONTINUOUS;
-
-
-   Schedule:Compact,
-       Min Rel Hum Set Sch,       !- Name
-       Humidity,                               !- ScheduleType
-       Through: 12/31,                   !- Complex Field \#1
-       For: AllDays,                       !- Complex Field \#2
-       Until: 24:00,                       !- Complex Field \#3
-       30.0;                                       !- Complex Field \#4
-   Schedule:Compact,,
-       Max Rel Hum Set Sch,       !- Name
-       Humidity,                               !- ScheduleType
-       Through: 12/31,                   !- Complex Field \#1
-       For: AllDays,                       !- Complex Field \#2
-       Until: 24:00,                       !- Complex Field \#3
-       55.0;                                       !- Complex Field \#4
-```
-
-
-
-
-### ZoneControl Humidistat Outputs
-
-Outputs available from the ZoneControl:Humidistat:
-
-* HVAC,Average,Zone Predicted Moisture Load Moisture Transfer Rate [kgWater/s]
-
-* HVAC,Average,Zone Predicted Moisture Load to Humidifying Setpoint Moisture Transfer Rate [kgWater/s]
-
-* HVAC,Average,Zone Predicted Moisture Load to Dehumidifying Setpoint Moisture Transfer Rate [kgWater/s]
-
-#### Zone Predicted Moisture Load Moisture Transfer Rate [kgWater/s]
-
-This is the predicted latent (moisture) load in kg<sub>water</sub>/s required to meet the current zone humidistat setpoint. A positive value indicates a humidification load, a negative value indicates a dehumidification load. For a dual setpoint humidistat, the value is zero when the controlled zone   s relative humidity is between the defined humidifying and dehumidifying setpoints. This moisture load rate is calculated and reported from the Predict step in the Zone Predictor-Corrector module. For nearly all equipment types, the Predictor-Corrector evaluates the active humidistat setpoints, determines if the zone requires humidification or dehumidification, and then passes this single load to the equipment for the single setpoint humidistat case. This value is not multiplied by zone or group multipliers.
-
-#### Zone Predicted Moisture Load to Humidifying Setpoint Moisture Transfer Rate [kgWater/s]
-
-This is the predicted latent (moisture) load in kg<sub>water</sub>/s required to meet the current zone humidistat **humidifying** setpoint. This is calculated and reported from the Predict step in the Zone Predictor-Corrector module. For nearly all equipment types, the Predictor-Corrector evaluates the active humidistat humidifying setpoints, determines if the zone requires humidification or not, and then passes this load to the equipment for the case of a dual setpoint humidistat (see Zone Predicted Moisture Load Moisture Transfer Rate, above, for single setpoint humidistat case). This value is multiplied by zone or group multipliers.
-
-#### Zone Predicted Moisture Load to Dehumidifying Setpoint Moisture Transfer Rate [kgWater/s]
-
-This is the predicted latent (moisture) load in kg<sub>water</sub>/s required to meet the current zone humidistat **dehumidifying** setpoint. This is calculated and reported from the Predict step in the Zone Predictor-Corrector module. For nearly all equipment types, the Predictor-Corrector evaluates the active humidistat humidifying setpoints, determines if the zone requires dehumidification or not, and then passes this load to the equipment for a dual setpoint humidistat (see Zone Predicted Moisture Load Moisture Transfer Rate, above, for single setpoint humidistat case). This value is multiplied by zone or group multipliers.
-
-### ZoneControl:Thermostat:ThermalComfort
-
-The thermal comfort zone control provides a method to control a zone to a dry-bulb temperature setpoint based on a thermal comfort model (e.g. Fanger) and a user-specified thermal comfort setpoint schedule.
-
-This object references a control type schedule and one or more thermal comfort control type objects which in turn reference one or more setpoint schedules. The example at the end of this section illustrates a complete zone thermal comfort control specification including the control type and setpoint schedules. The control type schedule and the list of control type/name pairs are directly related. The schedule defines the type of control that is to be used during for each hour. Valid Control Types are
-
-0 - Uncontrolled (No thermal comfort control)
-
-1 - Single Thermal Comfort Heating Setpoint:Fanger
-
-2 - Single Thermal Comfort Cooling Setpoint:Fanger
-
-3 - Single Thermal Comfort Heating Cooling Setpoint:Fanger
-
-4 - Dual Thermal Comfort Setpoint with Deadband:Fanger
-
-Thus, if the schedule referenced in the ZoneControl:Thermostat:ThermalComfort statement has a value of 4 for a particular hour, this indicates that during that hour "Dual Thermal Comfort Setpoint with Deadband:Fanger" is to be used. The specific "Dual Thermal Comfort Setpoint with Deadband:Fanger " control object to be used is specified in the list of control type/name pairs. Then the specific control type objects reference the thermal comfort control setpoint schedule to be used. Because only one control can be specified for each control type in a ZoneControl:Thermostat:ThermalComfort statement, there are only four pairs possible in a particular ZoneControl:Thermostat:ThermalComfort type/name list. This is because individual controls can be defined hourly, thus giving the user a full range of flexibility. Since putting in the name of the control type directly in the schedule would be very cumbersome, the control types are assigned a number which is used in the hourly schedule profile.
-
-The ZoneControl:Thermostat:ThermalComfort object can be used alone, or with a ZoneControl:Thermostat object. When both control objects co-exist for a specific zone and the thermal comfort control type value in the thermal comfort control type schedule is non-zero the thermal comfort object will override the value from the zone thermostat object. If the thermal comfort control is specified as    Uncontrolled    (thermal comfort control type value of 0) for a particular period, then control will revert to thermostat control if specified. If the thermal comfort control is specified as    Uncontrolled    for a particular period and thermostat control is not specified in the input, then conditions will float.
-
-This object currently allows only Fanger comfort control (Ref. Thermal Comfort in Engineering Reference). It requires one or more people objects in a specific zone. It also requires inputs of Fields *Activity Level Schedule Name, Work Efficiency Schedule Name, Clothing Insulation Schedule Name* and *Air Velocity Schedule Name* in the people object(s). When thermal comfort control is used in a zone, the air velocity entered in the Air Velocity Schedule (Ref. People) should be greater than or equal to 0.1 and less than or equal to 0.5 m/s. A warning message will be issued if thermal comfort control is active and the air velocity is outside this range.
-
-This object reads input PMV values from a given PMV setpoint schedule to calculate a dry-bulb temperature setpoint based on the selected thermal comfort model. The dry-bulb temperature setpoint calculation uses zone air humidity ratio at the previous system timestep and surface temperatures at the previous zone timestep, along with other conditions at the current timestep (e.g., activity level, clothing level and air velocity from the PEOPLE object).
-
-#### Field: Name
-
-Unique identifying name for this thermal comfort control object.
-
-#### Field: Zone or ZoneList Name
-
-Name of the zone or set of zones that is being controlled. When the ZoneList option is used then this thermostat definition is applied to each of the zones in the zone list effecting a global definition for thermostatic control in the zone.
-
-#### Field: Averaging Method
-
-This choice field specifies the method for calculating the thermal comfort dry-bulb temperature setpoint for a zone with multiple People objects defined. The available choices are: **SpecificObject**, **ObjectAverage**, and **PeopleAverage**. This field is only used when multiple people objects are defined for this zone. If this field is specified as **PeopleAverage** and the total number of people for all people objects is zero for a particular timestep, the PeopleAverage method cannot be applied and the program automatically uses the ObjectAverage method for this timestep. The default input is **PeopleAverage**.
-
-#### Field: Object Name for Specific Object Averaging Method
-
-This choice field specifies the name of the specific People object to be used for calculating comfort control when multiple People objects are defined. Only used if the Averaging Method is specified as    SpecificObject.   
-
-#### Field: Minimum Dry-Bulb Temperature Setpoint
-
-This field specifies the minimum dry-bulb temperature setpoint allowed for this zone. If the dry-bulb temperature calculated by the thermal comfort setpoint model is below this value, then the temperature setpoint will be set to this value. The default value is 0 ËšC.
-
-#### Field: Maximum Dry-Bulb Temperature Setpoint
-
-This field specifies the maximum dry-bulb temperature setpoint allowed for this zone. If the dry-bulb temperature calculated by the thermal comfort setpoint model exceeds this value, then the temperature setpoint will be set to this value. The default value is 50 ËšC.
-
-Note the minimum and maximum temperature setpoint fields are provided to allow the user to bound the temperature control In a specific zone if necessary. These fields are used to provide boundaries for the dry-bulb temperature setpoint calculated at each system timestep when unrealistic inputs have been specified.
-
-#### Field: Thermal Comfort Control Type Schedule Name
-
-Schedule which defines what type of thermal comfort control is active during each simulation timestep.
-
-Valid Control Types are
-
-0 - No thermal comfort control
-
-1 - Single Thermal Comfort Heating Setpoint:Fanger
-
-2 - Single Thermal Comfort Cooling Setpoint:Fanger
-
-3 - Single Thermal Comfort Heating Cooling Setpoint:Fanger
-
-4 - Dual Thermal Comfort Setpoint with Deadband:Fanger
-
-Each non-zero control type used in this schedule must appear in the following fields which list the specific thermal comfort control objects to be used for this zone.
-
-#### Field Set (Thermal Comfort Control Object Type, Thermal Comfort Control Name)
-
-Up to four pairs of Thermal Comfort Control Type and Thermal Comfort Control Type Name fields may be listed to specify which thermal comfort control type objects are used for this zone. This list is not order-dependent, and the position in this list has no impact on the control type schedule. In the control type schedule, a value of 1 always means "Single Thermal Comfort Heating Setpoint:Fanger", even if that control type is not first in this list.
-
-#### Field: Thermal Comfort Control &lt;x&gt; Object Type
-
-This field specifies the first control type name to be used for this zone. Available control types are:
-
-ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating
-
-ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling
-
-ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling
-
-ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint
-
-#### Field: Thermal Comfort Control &lt;x&gt; Name
-
-The unique name for the corresponding thermal comfort control type.
-
-An example of this statement in an IDF is:
-
-```idf
-ZoneControl:Thermostat:ThermalComfort,
-       Zone 2 Comfort Control,                   !- Thermal Comfort Control Name
-       EAST ZONE,                                             !- Zone Name
-       SpecificObject,                                   !- Averaging Method for Zones with Multiple People Objects
-       EAST ZONE,                                             !- Object Name for Specific Object Averaging Method
-       12.8,                                                       !- Minimum dry-bulb temperature setpoint
-       40.0,                                                       !- Maximum dry-bulb temperature setpoint
-       Zone Comfort Control Type Sched, !- Thermal Comfort Control Type SCHEDULE Name
-       Dual Thermal Comfort Setpoint WITH DEADBAND:Fanger, !- Control Type #1
-       Dual Comfort Setpoint;                     !- Thermal Comfort Control Type Name #1
-```
-
-
-Global thermal comfort thermostat example:
-
-```idf
-   ZoneList,AllControlledZones,SPACE1-1,SPACE2-1,SPACE3-1,SPACE4-1,SPACE5-1;
-
-
-   ZoneControl:Thermostat:ThermalComfort,
-       ControlledZones Comfort Control,   !- Name
-       AllControlledZones,                             !- Zone Name
-       PeopleAverage,                     !- Averaging Method
-       ,                                               !- Specific People Name
-       12.8,                                       !- Minimum Dry-Bulb Temperature Setpoint {C}
-       40.0,                                       !- Maximum Dry-Bulb Temperature Setpoint {C}
-       Zone Comfort Control Type Sched,   !- Thermal Comfort Control Type Schedule Name
-       ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating,   !- Thermal Comfort Control 1 Object Type
-       Single Heating Comfort Setpoint,   !- Thermal Comfort Control 1 Name
-       ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling,   !- Thermal Comfort Control 2 Object Type
-       Single Cooling Comfort Setpoint,   !- Thermal Comfort Control 2 Name
-       ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling,   !- Thermal Comfort Control 3 Object Type
-       Single Heating Cooling Comfort Setpoint,   !- Thermal Comfort Control 3 Name
-       ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint,   !- Thermal Comfort Control 4 Object Type
-       Dual Comfort Setpoint;     !- Thermal Comfort Control 4 Name
-```
-
-
-### ZoneControl Thermostat ThermalComfort Outputs
-
-Three outputs are available from the ZoneControl:Thermostat:ThermalComfort object. Two output variables used primarily for the ZoneControl:Thermost object are also described here to explain their meaning when using thermal comfort control.
-
-
-
-**ZoneControl:ThermalComfort**
-
-* Zone,Average,Zone Thermal Comfort Control Type []
-
-* Zone,Average,Zone Thermal Comfort Control Fanger Low Setpoint PMV []
-
-* Zone,Average,Zone Thermal Comfort Control Fanger High Setpoint PMV []
-
-
-
-**ZoneControl:Thermostat**
-
-* Zone,Average,Zone Thermostat Heating Setpoint Temperature [C]
-
-* Zone,Average,Zone Thermostat Cooling Setpoint Temperature [C]
-
-
-#### Zone Thermal Comfort Control Type []
-
-This is the current zone thermal comfort control type (0 through 4). This value is set at each system timestep and averaged over the reporting interval. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
-
-#### Zone Thermal Comfort Control Fanger Low Setpoint PMV []
-
-This is the current zone thermal comfort low Predicted Mean Vote value. Values range between -3 and +3. If there is no heating thermal comfort active, then the value reported will be -999. This value is set at each system timestep and averaged over the reporting interval. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
-
-#### Zone Thermal Comfort Control Fanger High Setpoint PMV []
-
-This is the current zone thermal comfort high Predicted Mean Vote value. Values range between -3 and +3. If there is no cooling thermal comfort active, then the value reported will be 999. This value is set at each system timestep and averaged over the reporting interval. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
-
-#### Zone Thermostat Heating Setpoint Temperature [C]
-
-The Zone Control:Thermal Comfort object shares the same output variable and overwrites the thermal setpoints defined in object Zone Control:Thermostatic when both objects of Zone Control:Thermostatic and Zone Control:Thermal Comfort co-exist. It outputs the current zone thermal comfort heating setpoint in degrees C when thermal comfort control is active, otherwise this output variable will report the thermostat heating setpoint (Ref. Zone Control:Thermostatic Outputs). If there is no heating thermal comfort active and no thermostat heating setpoint is defined for this zone, this value will be 0. This value is set at each system timestep and averaged over the reporting interval. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
-
-#### Zone Thermostat Cooling Setpoint Temperature   [C]
-
-This output variable defined in object Zone Control:Thermostatic. The Thermal Comfort object shares the same output variable and overwrites the thermal setpoints defined in object Zone Control:Thermostatic when both objects of Zone Control:Thermostatic and Zone Control:Thermal Comfort co-exist. It outputs the current zone thermal comfort cooling setpoint in degrees C when thermal comfort control is active, otherwise this output variable will report the thermostat cooling setpoint (Ref. Zone Control:Thermostatic Outputs). If there is no cooling thermal comfort active and no thermostat cooling setpoint is defined for this zone, this value will be 0. This value is set at each system timestep and averaged over the reporting interval. Using the averaged value for longer reporting frequencies (hourly, for example) may not be meaningful in some applications.
-
-### Thermal Comfort Setpoints
-
-The syntax for the current set (4) of zone thermal comfort control types is given below. In each case, the keyword is accompanied by an identifying name and either one or two schedule names (depending on whether the control type is a single or dual setpoint control). The schedule defines a Predicted Mean Vote (PMV) setpoint for the control type. The schedule would be defined through the standard schedule syntax described earlier in this document. For an uncontrolled thermal comfort zone, no Fanger thermal comfort object is specified or necessary.   However, the `Fanger thermal comfort output variables, Zone Thermal Comfort Fanger Model PMV and Zone Thermal Comfort Fanger Model PPD, are reported for thermal comfort uncontrolled conditions as well (e.i., free floating thermal comfort condition) just like a free floating temperature and humidity ratio.   These are indicative of the actual thermal comfort level in uncontrolled thermal comfort zone, and are outputs variables under `People objects`.`
-
-### ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating
-
-This would be used for heating only thermal comfort control. The PMV setpoint can be scheduled and varied throughout the simulation but only heating is allowed with this control type.
-
-#### Field: Name
-
-Unique name for this control type.
-
-#### Field: Fanger Thermal Comfort Schedule Name
-
-The name of the associated schedule containing `Zone Thermal Comfort Fanger Model PMV` values.
-
-### ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling
-
-This would be used for cooling only thermal comfort control. The PMV setpoint can be scheduled and varied throughout the simulation but only cooling is allowed with this control type.
-
-#### Field: Name
-
-Unique name for this control type.
-
-#### Field: Fanger Thermal Comfort Schedule Name
-
-The name of the associated schedule, containing `Zone Thermal Comfort Fanger Model PMV` values.
-
-### ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling
-
-This would be used for heating and cooling thermal comfort control but only heating or cooling can be scheduled at any given time period. The PMV setpoint can be scheduled and varied throughout the simulation for both heating and cooling.
-
-#### Field: Name
-
-Unique name for this control type.
-
-#### Field: Fanger Thermal Comfort Schedule Name
-
-The name of the associated schedule containing `Zone Thermal Comfort Fanger Model PMV` values.
-
-### ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint
-
-This would be used for heating and cooling thermal comfort control where both a heating and cooling PMV setpoint can be scheduled for any given time period. The PMV setpoint can be scheduled and varied throughout the simulation for both heating and cooling.
-
-#### Field: Name
-
-Unique name for this control type.
-
-#### Field: Fanger Thermal Comfort Heating Schedule Name
-
-The name of the associated schedule containing heating setpoint `Zone Thermal Comfort Fanger Model PMV` values.
-
-#### Field: Fanger Thermal Comfort Cooling Schedule Name
-
-The name of the associated schedule containing cooling setpoint `Zone Thermal Comfort Fanger Model PMV` values.
-
-An example of this statement in an IDF is:
-
-```idf
-ThermostatSetpoint:ThermalComfort:Fanger:SingleHeating,
-       Heating Comfort Setpoint,!- Name
-       Heating PMV Setpoints;     !- Setpoint Temperature SCHEDULE Name
-
-
-ThermostatSetpoint:ThermalComfort:Fanger:SingleCooling,
-       Cooling Comfort Setpoint,!- Name
-       Cooling PMV Setpoints;     !- Setpoint Temperature SCHEDULE Name
-
-
-ThermostatSetpoint:ThermalComfort:Fanger:SingleHeatingOrCooling,
-       Heating Cooling Comfort Setpoint,!- Name
-       Heating Cooling PMV Setpoints;     !- Setpoint Temperature SCHEDULE Name
-
-
-ThermostatSetpoint:ThermalComfort:Fanger:DualSetpoint,
-       Dual Comfort Setpoint,     !- Name
-       Heating PMV Setpoints,     !- Fanger Thermal Comfort Heating Setpoint PMV SCHEDULE Name
-       Cooling PMV Setpoints;     !- Fanger Thermal Comfort Cooling Setpoint PMV SCHEDULE Name
-```
-
-
-### ZoneControl:ContaminantController
-
-The ZoneControl:ContaminantController object is used for any of the following two purposes based on the system outdoor air method specified in the Controller:MechanicalVentilation.
-
-1)      To control a zone to a specified indoor level of contaminants. When this zone is served by an AirLoopHVAC, the other zones served by the same AirLoopHVAC will have the same specified indoor level, if no objects in the other zones served by the same AirLoop are specified. Currently, the available contaminant controls are carbon dioxide and generic contaminant controls. The specified carbon dioxide setpoint is used to calculate the required outdoor airflow rate through the HVAC system to reach the setpoint. The AirLoopHVAC system outdoor flow rate is realized by the Controller:MechanicalVentilation object with System Outdoor Air Method = IndoorAirQualityProcedure.The specified generic contaminant setpoint is used to calculate the required outdoor airflow rate through the HVAC system to reach the setpoint. The AirLoopHVAC system outdoor flow rate is realized by the Controller:MechanicalVentilation object with System Outdoor Air Method = IndoorAirQualityProcedure-GenericContaminant.
-
-2)      To specify minimum CO2 concentration schedule name for a zone. The AirLoopHVAC system outdoor flow rate is realized by the Controller:MechanicalVentilation object with System Outdoor Air Method = ProportionalControlBasedonOccupancySchedule or ProportionalControlBasedOnDesignOccupancy.    Carbon Dioxide Control Availability Schedule Name determines the availability of    ProportionalControl   .
-
-For the first purpose above, when multiple zones are served by an AirLoop, those zones that do not have a contaminant controller object specified in the input data file are automatically assigned a carbon dioxide setpoint. Zone objects entered in the input data file are internally assigned an index number from 1 to n (first defined Zone object = 1, next Zone object defined in the input file = 2, etc.). For zones served by an AirLoop that do not have a contaminant controller specified, the zone   s carbon dioxide setpoint will be the same as the zone with the next highest zone index number that has a contaminant controller specified. If a zone with a higher index number and contaminant controller specified does not exist, then the zone with the next lowest zone   index number that has a contaminant controller specified will be used. For example, assume an AirLoop serves zones 1 through 5, but one ZoneControl:ContaminantController object is specified for zone 2, a second ZoneControl:ContaminantController object is specified for zone 4, and no ZoneControl:ContaminantController objects are specified for zones 1, 3 and 5. In this case, zone 1 will be assigned the carbon dioxide setpoint schedule that was specified for zone 2, and zones 3 and 5 will be assigned the carbon dioxide setpoint schedule that was specified for zone 4.
-
-#### Field: Name
-
-Unique identifying name for the ZoneControl:ContaminantController.
-
-#### Field: Controlled Zone Name
-
-Name of the zone that is being controlled.
-
-#### Field:Carbon Dioxide Control Availability Schedule Name
-
-This field contains the name of a schedule that determines whether or not the ZoneControl:ContaminantController is available. When the schedule value is zero, the ZoneControl:ContaminantController is bypassed (not available to operate). When the schedule value is greater than zero, the ZoneControl:ContaminantController is available and will be used to calculate the required outdoor airflow rate to reach the carbon dioxide setpoint. If this field is left blank, the schedule has a value of 1 for all time periods. Schedule values must be between 0 and 1.
-
-#### Field:Carbon Dioxide Setpoint Schedule Name
-
-This field contains the name of a schedule that contains the zone carbon dioxide concentration setpoint as a function of time. The units for carbon dioxide setpoint are ppm. The setpoint values in the schedule must be between 0 and 2000 ppm. . This field is used when the field    System Outdoor Air Method    = IndoorAirQualityProcedure in the Controller:MechanicalVentilation object.
-
-#### Field:Minimum Carbon Dioxide Concentration Schedule Name
-
-This field contains the name of a schedule that contains the minimum zone carbon dioxide concentration setpoint as a function of time. The units for carbon dioxide setpoint are ppm. This field is used when the field    System Outdoor Air Method    = ProportionalControlBasedonOccupancySchedule or ProportionalControlBasedOnDesignOccupancy in the Controller:MechanicalVentilation object.
-
-#### Field: Generic Contaminant Control Availability Schedule Name
-
-This field contains the name of a schedule that determines whether or not the ZoneControl:ContaminantController is available. When the schedule value is zero, the generic contaminant control will not be performed. When the schedule value is greater than zero, the ZoneControl:ContaminantController is available and will be used to calculate the required outdoor airflow rate to reach the generic contaminant setpoint. If this field is left blank, the schedule has a value of 1 for all time periods. Schedule values must be between 0 and 1.
-
-#### Field: Generic Contaminant Setpoint Schedule Name
-
-This field contains the name of a schedule that contains the zone generic contaminant concentration setpoint as a function of time. The units for generic contaminant setpoint are ppm. The setpoint values in the schedule must be&gt;=0.
-
-
-
-An IDF example is provided below:
-
-```idf
-   ZoneControl:ContaminantController,
-       CO2 Controller1,                 !- Name
-       EAST ZONE,                             !- Controlled Zone Name
-       CO2AvailSchedule,               !- Carbon Dioxide Control Availability Schedule Name
-       CO2SetpointSchedule,         !- Carbon Dioxide Setpoint Schedule Name
-       ,                                               !- Minimum Carbon Dioxide Concentration Schedule Name
-       GCAvailSchedule,                 !- Generic Contaminant Control Availability Schedule Name
-       GCSetpointSchedule;           !- Generic Contaminant Setpoint Schedule Name
-```
-
-
-### ZoneControl Contaminant Controller Outputs
-
-The following output variables are available when the ZoneControl:ContaminantController object is specified.
-
-* HVAC,Average,Zone Air CO2 Predicted Load to Setpoint Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Air CO2 Setpoint Concentration [ppm]
-
-* HVAC,Average,Zone Generic Air Contaminant Predicted Load to Setpoint Mass Flow Rate [kg/s]
-
-* HVAC,Average,Zone Generic Air Contaminant Setpoint Concentration [ppm]
-
-
-
-#### Zone Air CO2 Predicted Load to Setpoint Mass Flow Rate [kg/s]
-
-This output is the average predicted outdoor airflow rate in kg/s required to meet the current zone carbon dioxide setpoint for the time step being reported. This value is calculated and reported from the Predict step in the Zone Contaminant Predictor-Corrector module. The calculated outdoor airflow rate will be specified in the Controller:MechanicalVentilation object with System Outdoor Air Method = IndoorAirQualityProcedureto provide enough outdoor ventilation air to keep the zone air carbon dioxide concentration level at or below the setpoint.
-
-#### Zone Air CO2 Setpoint Concentration [ppm]
-
-This output variable is the average carbon dioxide setpoint value, in parts per million, for the time step being reported.
-
-#### Zone Generic Air Contaminant Predicted Load to Setpoint Mass Flow Rate [kg/s]
-
-This output is the average predicted outdoor airflow rate in kg/s required to meet the current zone generic contaminant setpoint for the time step being reported. This value is calculated and reported from the Predict step in the Zone Contaminant Predictor-Corrector module. The calculated outdoor airflow rate will be specified in the Controller:MechanicalVentilation object with System Outdoor Air Method = IndoorAirQualityProcedure-GenericContaminant****to provide enough outdoor ventilation air to keep the zone air generic contaminant concentration level at or below the setpoint.
-
-#### Zone Generic Air Contaminant Setpoint Concentration [ppm]
-
-This output variable is the averagegeneric contaminant setpoint value, in parts per million, for the time step being reported.
-
-Group -- Air Path
------------------
-
-### AirLoopHVAC:SupplyPath, AirLoopHVAC:ReturnPath
-
-The zone supply and return air paths are used to describe the configuration of the flow path that the supply air takes in moving from the main air handler to the zone terminal units and that the return air takes on leaving the zones and returning to the central return air duct. The air paths consist of a group of components     AirLoopHVAC:ZoneSplitters and AirLoopHVAC:SupplyPlenums for the supply path and AirLoopHVAC:ReturnPlenums and AirLoopHVAC:ZoneMixers for the return path. The connectivity of the paths is established by the components    node connections. There are no branches defined in the zone air path constructs.
-
-For a typical single duct air system there will be one AirLoopHVAC:SupplyPath and one AirLoopHVAC:ReturnPath. A typical dual duct system would have 2 AirLoopHVAC:SupplyPaths     one for the hot air and one for the cold air     and 1 AirLoopHVAC:ReturnPath.
-
-The AirLoopHVAC:SupplyPlenum component provides the capability to have supply air distributed to the conditioned zones through one or more plenum zones such as would occur in an underfloor air distribution system (UFAD). The AirLoopHVAC:ReturnPlenum component allows the program to model return air plenums. Of course plenums are always optional. The simplest AirLoopHVAC:SupplyPath would consist of only an AirLoopHVAC:ZoneSplitter; similarly the simplest return air path consists of a single AirLoopHVAC:ZoneMixer. A UFAD system supply air path might consist of a single AirLoopHVAC:ZoneSplitter connecting to multiple AirLoopHVAC:SupplyPlenums which in turn could each supply one or more conditioned zones. A system with return plenums would have an AirLoopHVAC:ReturnPath in which the conditioned zones connect to the return plenum inlets and the return plenum   s outlets connect to a single AirLoopHVAC:ZoneMixer.
-
-Both the zone supply and return plenums are solved in the heat balance as thermal zones which couple through heat conduction with adjacent zones. Since they are solved as thermal zones the solution scheme involves the zone predictor-corrector technique which will lag the temperature at the system timestep in every zone. See Summary of Predictor-Corrector Procedure in the EnergyPlus Engineering Reference.
-
-Below are the descriptions of the zone supply and return path statements. Note that each statement type has an identifying name, a single inlet/outlet node name, and a list of component type/name pairs. For a single zone being served by an air loop, the inlet to its air distribution unit and the zone return air outlet can be the zone equipment inlet and outlet nodes directly, thus eliminating the need to specify an AirLoopHVAC:SupplyPath and an AirLoopHVAC:ReturnPath.
-
-### AirLoopHVAC:SupplyPath
-
-The AirLoopHVAC:SupplyPath lists one or more AirLoopHVAC:ZoneSplitter and AirLoopHVAC:SupplyPlenum components comprising the path. The components are listed in flow order: upstream to downstream and may be in series, parallel, or both. Connectivity is established by means of the individual component inlet and outlet nodes.
-
-#### Field: Name
-
-Unique name to identify the supply air path..
-
-#### Field: Supply Air Path Inlet Node Name
-
-The name of an inlet node for the zone equipment half of the air loop. This should be one of the nodes named in the AirLoopHVAC field: Demand Side Inlet Node Names.
-
-#### Field Set Component Type and Name
-
-The remaining fields are sets of two repeated times: a component type and a name.   These pairs of fields define the components on the supply air path.
-
-#### Field: Component &lt;\#&gt; Object Type
-
-Start of the component list for the AirLoopHVAC:SupplyPath. This field should contain either *AirLoopHVAC:SupplyPlenum* or *AirLoopHVAC:ZoneSplitter*.
-
-#### Field: Component &lt;\#&gt; Name
-
-Unique name of the AirLoopHVAC:SupplyPlenum or AirLoopHVAC:ZoneSplitter component.
-
-### AirLoopHVAC:ReturnPath
-
-The AirLoopHVAC:ReturnPath lists one or more AirLoopHVAC:ZoneMixer and AirLoopHVAC:ReturnPlenum components comprising the path. The components are listed in flow order: upstream to downstream and may be in series, parallel, or both. Connectivity is established by means of the individual component inlet and outlet nodes. At this time there can only be 1 AirLoopHVAC:ZoneMixer in an AirLoopHVAC:ReturnPath.
-
-#### Field: Name
-
-Unique name to identify the return air path.
-
-#### Field: Return Air Path Outlet Node Name
-
-The name of the node that is the outlet to the air loop from the AirLoopHVAC:ReturnPath. This should be the same node named in the AirLoopHVAC field: Demand Side Outlet Node Name.
-
-#### Field Set Component Type and Name
-
-The remaining fields are sets of two repeated times: a component type and a name.   These pairs of fields define the components on the return air path.
-
-#### Field: Component &lt;\#&gt; Object Type
-
-Start of the component list for the AirLoopHVAC:ReturnPath. This field should contain either *AirLoopHVAC:ReturnPlenum* or *AirLoopHVAC:ZoneMixer*.
-
-#### Field: Component &lt;\#&gt; Name
-
-Unique name of the AirLoopHVAC:ReturnPlenum or AirLoopHVAC:ZoneMixer.
-
-Example inputs are shown below
-
-```idf
-  AirLoopHVAC:SupplyPath,
-       SupplyAirPath 1,              !- Name
-       Zone Equip In Node,           !- Supply Air Path Inlet Node Name
-       AirLoopHVAC:SupplyPlenum,     !- Component 1 Object Type
-       Supply-Plenum-1,              !- Component 1 Name
-       AirLoopHVAC:ZoneSplitter,     !- Component 2 Object Type
-       Zone Supply Air Splitter 1;   !- Component 2 Name
-
-
-AirLoopHVAC:ReturnPath,
-       ReturnAirPath1,               !- Name
-       PLENUM-1 Out Node,            !- Return Air Path Outlet Node Name
-       Zone Return Plenum,           !- Component 1 Object Type
-       Return-Plenum-1;              !- Component 1 Name
-```
-
-
-### AirLoopHVAC:ReturnPlenum
-
-The simple building shown in the figure below consists of a controlled zone and a return plenum zone that is used for the return air. This simple configuration contains a ground floor controlled zone with a window and a return plenum zone which handles the roof load. The return air plenum is a special type of component since there is both a heat balance connection and building description and a system airflow connection that transfers the airflow directly from the controlled zone to the return plenum zone in the system air simulation. The input described in this section is mainly just for the system airflow connections in the HVAC algorithms. In addition the return plenum zone must be fully input as a zone object for the heat balance calculation. The zone description needs to contain the wall descriptions - the interzone ceiling and floor, and for this simple case the roof. All the other attributes of a zone that can be specified in the building description can be used with a return plenum zone if necessary: scheduled loads, windows, etc.
-
-![](media/image337.svg)
-
-Figure 130. Illustration of Zone Return Plenum
-
-After all the building zone attributes are specified, the AirLoopHVAC:ReturnPlenum object is specified and included as one of the named components in an AirLoopHVAC:ReturnPath.
-
-#### Field: Name
-
-A unique identifying name identifying the AirLoopHVAC:ReturnPlenum system component.
-
-#### Field: Zone Name
-
-The zone name specified in the heat balance portion of the input. This piece of input connects the zone return plenum system component to the heat balance data structure.
-
-#### Field: Zone Node Name
-
-The name of the zone node. The zone node name connects the heat balance data structure to the system airflow data structure through this node. This node name must be unique otherwise a warning is reported. Do not use the Zone Air Node Name specified in any ZoneHVAC:EquipmentConnections object, and since this zone is a plenum a ZoneHVAC:EquipmentConnections object is not required for the zone named in the previous field.
-
-#### Field: Outlet Node Name
-
-The name of the return plenum outlet node. For the zone return plenum there is only one outlet node that can be specified.
-
-#### Field: Induced Air Outlet Node or NodeList Name
-
-The name of an induced air outlet node or the name of a NodeList of such nodes. These nodes are to be used as the secondary inlet air nodes of powered induction terminal units (See **AirTerminal:SingleDuct:SeriesPIU:Reheat** and **AirTerminal:SingleDuct:ParallelPIU:Reheat**).
-
-#### Field: Inlet &lt;\#&gt; Node Name
-
-The name of a plenum inlet node. There is no limit to the number of inlet nodes, and there may be no duplicate inlet node names. (Note that some EnergyPlus editing tools may allow only 500 inlet node names, but this may be increased by extending the object in the Energy+.idd file.)
-
-
-
-An IDF example of a zone return plenum component specification:
-
-```idf
-   AirLoopHVAC:ReturnPlenum,
-       Return-Plenum-1,            !- Name
-       PLENUM-1,                   !- Zone Name
-       PLENUM-1 Node,              !- Zone Node Name
-       PLENUM-1 Out Node,          !- Outlet Node Name
-       PLENUM-1 Induced Air Nodes, !- Induced Air Outlet Node or NodeList Name
-       SPACE1-1 Out Node,          !- Inlet 1 Node Name
-       SPACE2-1 Out Node,          !- Inlet 2 Node Name
-       SPACE3-1 Out Node,          !- Inlet 3 Node Name
-       SPACE4-1 Out Node,          !- Inlet 4 Node Name
-       SPACE5-1 Out Node;          !- Inlet 5 Node Name
-
-
-   NodeList,
-       PLENUM-1 Induced Air Nodes, !- Name
-       SPACE1-1 ATU Sec Node,      !- Node 1 Name
-       SPACE2-1 ATU Sec Node,      !- Node 2 Name
-       SPACE3-1 ATU Sec Node,      !- Node 3 Name
-       SPACE4-1 ATU Sec Node;      !- Node 4 Name
-```
-
-
-Below is an example of the AirLoopHVAC:ReturnPath for the simple case shown above.
-
-```idf
-   AirLoopHVAC:ReturnPath,
-       ReturnAirPath1,              !- Name
-       PLENUM-1 Out Node,           !- Return Air Path Outlet Node Name
-       AirLoopHVAC:ReturnPlenum,    !- Component 1 Object Type
-       Return-Plenum-1;             !- Component 1 Name
-```
-
-
-
-
-
-### AirLoopHVAC:SupplyPlenum
-
-The building shown in the figure below consists of three controlled zones served by an AirLoopHVAC:SupplyPlenum beneath the floor.
-
-![](media/image338.png)
-
-Figure 131. Illustration of AirLoopHVAC:SupplyPlenum
-
-The AirLoopHVAC:SupplyPlenum has a heat balance connection and building description, and a system airflow connection which transfers the airflow from the supply plenum zone to the controlled zones in the system simulation. The input described in this section is mainly just for the system airflow connections in the HVAC algorithms. In addition the supply plenum zone must be fully input in the building zone description. The supply plenum zone description needs to contain the wall descriptions, the interzone ceiling and floor, and the ground connection. All the other attributes of a zone that can be specified in the building description can be utilized with a supply plenum zone if necessary, i.e. scheduled loads, windows, etc.
-
-After all the building zone attributes are specified, the AirLoopHVAC:SupplyPlenum object is specified and included as one of the named components in an AirLoopHVAC:SupplyPath.
-
-#### Field: Name
-
-A unique identifying name identifying the AirLoopHVAC:SupplyPlenum system component.
-
-#### Field: Zone Name
-
-The zone name specified in the heat balance portion of the input. This piece of input connects the AirLoopHVAC:SupplyPlenum system component to the heat balance data structure.
-
-#### Field: Zone Node Name
-
-The name of the zone node. The zone node name connects the heat balance data structure to the system airflow data structure through this node.   This node name is defined by the user in the field    Zone Air Node Name    in the ZoneHVAC:EquipmentConnections object for the zone named in the previous field.
-
-#### Field: Inlet Node Name
-
-The name of the inlet node to the supply plenum. The AirLoopHVAC:SupplyPlenum component can send air to many outlets, but there is only one inlet.
-
-#### Field: Outlet &lt;\#&gt; Node Name
-
-The name of a plenum outlet node. There is no limit to the number of outlet nodes, and there may be no duplicate outlet node names. (Note that some EnergyPlus editing tools may allow only 500 outlet node names, but this may be increased by extending the object in the Energy+.idd file.)
-
-An IDF example of an AirLoopHVAC:SupplyPlenum component specification:
-
-```idf
-  AirLoopHVAC:SupplyPlenum,
-       Supply Plenum 1,                         ! Name
-       SUPPLY PLENUM ZONE,                   ! Zone Name
-       Supply Plenum 1 Zone Node,     ! Zone Node Name
-       Zone Equipment Inlet Node,     ! Inlet Node Name
-       Supply Plenum 1 Outlet Node; ! Outlet 1 Node Name
-```
-
-
-Below is an example of the AirLoopHVAC:SupplyPath for the building shown above.
-
-```idf
-  AirLoopHVAC:SupplyPath,
-       TermReheatSupplyPath,               ! Name
-       Zone Equipment Inlet Node,     ! Supply Air Path Inlet Node Name
-       AirLoopHVAC:SupplyPlenum,       ! Component 1 Object Type
-       Supply Plenum 1,                         ! Component 1 Name
-       AirLoopHVAC:ZoneSplitter,       ! Component 2 Object Type
-       Zone Supply Air Splitter;       ! Component 2 Name
-```
-
-
-### AirLoopHVAC:ZoneSplitter
-
-The AirLoopHVAC:ZoneSplitter is a component that splits airflow from a single inlet to multiple outlets. This component must be referenced in an AirLoopHVAC:SupplyPath object. The input contains only node connection information.
-
-#### Field: Name
-
-Unique name for this zone splitter.
-
-#### Field: Inlet Node Name
-
-The name of the single inlet node going into the splitter.
-
-#### Field: Outlet &lt;\#&gt; Node Name
-
-The name of a splitter outlet node. There is no limit to the number of outlet nodes, and there may be no duplicate outlet node names. (Note that some EnergyPlus editing tools may allow only 500 outlet node names, but this may be increased by extending the object in the Energy+.idd file.)
-
-An example is shown below.
-
-```idf
-AirLoopHVAC:ZoneSplitter,
-           Zone Supply Air Splitter,     ! Name
-           Zone Equipment Inlet Node,   ! Inlet Node Name
-           Zone 1 Damper Inlet Node,     ! Outlet 1 Node Name
-          Zone 2 Damper Inlet Node,     ! Outlet 2 Node Name
-           Zone 3 Damper Inlet Node;     ! Outlet 3 Node Name
-```
-
-### AirLoopHVAC:ZoneMixer
-
-The AirLoopHVAC:ZoneMixer takes the air from multiple inlets and mixes the streams together to be sent out of a single outlet node. This is a simple process of summing flows and averaging the air properties. This compoment may be part of an air loop return path or part of an induction terminal unit. When used as a return air mixer, this component must be listed in an AirLoopHVAC:ReturnPath object, and the inlets may be zone return air nodes or AirLoopHVAC:ReturnPlenum outlet nodes. When used in an induction terminal unit (ref. AirTerminal:SingleDuct:SeriesPIU:Reheat, AirTerminal:SingleDuct:ParallelPIU:Reheat, and AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction), one inlet node is the supply (primary) air inlet from the central air handler, and the second inlet node is the induced (secondary) air inlet. These node names should match equivalent node names in the terminal unit.
-
-#### Field: Name
-
-Unique name for this zone mixer.
-
-#### Field: Outlet Node Name
-
-The name of the single outlet node leaving the mixer.
-
-#### Field: Inlet &lt;\#&gt; Node Name
-
-The name of a mixer inlet node. There is no limit to the number of inlet nodes, and there may be no duplicate inlet node names. (Note that some EnergyPlus editing tools may allow only 500 inlet node names, but this may be increased by extending the object in the Energy+.idd file.)
-
-An input example is shown below.
-
-```idf
-AirLoopHVAC:ZoneMixer,
-                 Zone Return Air Mixer,               ! Name
-                 Return Air Mixer Outlet Node, ! Outlet Node Name
-                 Zone 1 Outlet Node,                     ! Inlet 1 Node Name
-                 Zone 2 Outlet Node,                     ! Inlet 2 Node Name
-                 Zone 3 Outlet Node;                     ! Inlet 3 Node Name
-```
-
-Group -- Non-Zone Equipment
----------------------------
-
-The non-zone equipment group consists of plant objects that connect to the demand side of the plant loop but are not associated with a a specific Zone (and do not have their own group). There is currently one non-zone equipment object called   LoadProfile:Plant. This object places a scheduled demand load on the plant.
-
-Non-zone equipment allows the option of performing a plant-only EnergyPlus simulation, i.e. without any zones. This can be useful for comparing the performance of various plant configurations or components without the added complexity of a full building description.
-
-### LoadProfile:Plant
-
-The LoadProfile:Plant object is used to simulate a scheduled demand profile. This can be useful when the building loads are already known. Demanded load and flow rate are schedules specified in the object definition. The load profile can specify heating and cooling loads. Cooling loads are entered as negative numbers. The actual load met is dependent on the performance of the supply loop components.
-
-The LoadProfile:Plant object must be connected on the demand side of the plant loop. It should be located on a Branch with its control type set to    Active.    If desired, multiple LoadProfile:Plant objects can be combined in series and/or parallel.
-
-#### Field: Name
-
-The unique name of the LoadProfile:Plant object.
-
-#### Field: Inlet Node Name
-
-The name of the inlet node connection to the plant loop.
-
-  This node should be on the demand side.
-
-#### Field: Outlet Node Name
-
-The name of the outlet node connection to the plant loop.
-
-#### Field: Load Schedule Name
-
-Reference to the schedule object specifying the load profile [W].
-
-#### Field: Peak Flow Rate
-
-The peak demanded water flow rate [m<sup>3</sup>/s]. This value is multiplied by the flow rate fraction schedule values (below) to determine the actual volumetric flow rate.
-
-#### Field: Flow Rate Fraction Schedule Name
-
-Reference to the schedule object specifying the flow rate fraction relative to the value in the field Peak Flow Rate (above).
-
-An example of this object follows.
-
-```idf
-LoadProfile:Plant,
-   Load Profile 1,                                         !- Name
-   Demand Load Profile 1 Inlet Node,     !- Inlet Node Name
-   Demand Load Profile 1 Outlet Node,   !- Outlet Node Name
-   Load Profile 1 Load Schedule,             !- Load Schedule Name {W}
-   0.003,                                                           !- Peak Flow Rate {m3/s}
-   Load Profile 1 Flow Frac Schedule;   !- Flow Rate Fraction Schedule Name
-```
-
-
-
-### LoadProfile Plant Outputs
-
-The following output variables and meters are reported for the LoadProfile:Plant object:
-
-* HVAC,Average,Plant Load Profile Mass Flow Rate [kg/s]
-
-* HVAC,Average,Plant Load Profile Heat Transfer Rate [W]
-
-* HVAC,Sum,Plant Load Profile Heat Transfer Energy [J]
-
-* HVAC,Sum,Plant Load Profile Heating Energy [J]
-
-* HVAC,Sum,Plant Load Profile Cooling Energy [J]
-
-#### Plant Load Profile Mass Flow Rate [kg/s]
-
-This is the mass flow of the fluid passing through the load profile object, in kg/s.
-
-#### Plant Load Profile Heat Transfer Rate [W]
-
-#### Plant Load Profile Heat Transfer Energy [J]
-
-These report the overall heat transfer rate and energy for the load profile object, in Watts or Joules.
-
-#### Plant Load Profile Cooling Energy [J]Plant Load Profile Heating Energy [J]
-
-These report the overall cooling or heating energy that the load profile object places on the plant loop, in Joules.
-
-
-
-The inlet and outlet node temperatures and mass flow rates can be monitored using the system node output variables:
-
-* HVAC,Average,System Node Temperature [C]
-
-* HVAC,Average,System Node Mass Flow Rate [kg/s]
-
-
-
-Group     Solar Collectors
-------------------------
-
-Solar collectors are thermal devices that convert solar energy into thermal energy by raising the temperature of a circulating heat transfer fluid. The fluid can then be used to heat water for domestic hot water usage or space heating.
-
-In EnergyPlus solar collectors are components that are connected to the plant loop. A solar heating system can be constructed with a combination of solar collectors, pumps, and hot water tanks.
-
-Flate plate solar collectors are defined using two objects:   SolarCollector:FlatPlate:Water and SolarCollectorPerformance:FlatPlate. Similarly, Integral-Collector-Storage (ICS) solar collectors are defined using two objects: SolarCollector:IntegralCollectorStorage, and SolarCollectorPerformance:IntegralCollectorStorage.   The SolarCollector:FlatPlate:Water and SolarCollector:IntegralCollectorStorage objects describe the plant component connections. These object also reference   SolarCollectorPerformance:FlatPlate and SolarCollectorPerformance:IntegralCollectorStorage performance objects which contains the thermal and optical performance test data for a specific make and model of collector. Parameters are defined separately so that these values can be organized into a reference data set and need only be entered once if for an array of the same type of collectors.
-
-### SolarCollector:FlatPlate:Water
-
-The flat-plate solar collector model simulates glazed, unglazed, and tubular (i.e. evacuated tube) collectors. The SolarCollector:FlatPlate:Water object represents a single collector module connected to the plant loop. The thermal and optical properties of the collector module are taken from the referenced SolarCollectorPerformance:FlatPlate object. A surface or shading object defines the collector tilt, azimuth, and gross area. The collector surface participates normally in all shading calculations if the "FullExterior," "FullInteriorAndExterior,"    FullExteriorWithReflections    , or    FullInteriorAndExteriorWithReflections    flags are set in the Solar Distribution field of the Building object. Inlet and outlet nodes are specified for plant connections on the demand side of the plant loop.
-
-#### Field: Name
-
-The unique name of the SolarCollector:FlatPlate:Water object.
-
-#### Field: Solar Collector Performance Name
-
-Reference name of a SolarCollectorPerformance:FlatPlate object that defines the thermal and optical properties of the collector.
-
-#### Field: Surface Name
-
-Reference to one of the many different types of surfaces such as the BuildingSurface:Detailed or the Shading:Zone:Detailed objects. The surface named here is used to define the solar collector tilt, azimuth, and gross area.
-
-#### Field: Inlet Node Name
-
-The name of the inlet node connection to the plant loop.
-
-#### Field: Outlet Node Name
-
-The name of the outlet node connection to the plant loop.
-
-#### Field: Maximum Flow Rate
-
-The maximum flow rate [m<sup>3</sup>/s] allowed through the collector. This field is optional. If not specified, the collector will allow as much flow as the rest of the plant can deliver.
-
-An example follows.
-
-```idf
-  SolarCollector:FlatPlate:Water,
-   Collector 1,                                                       !- Name
-   ACR Solar International Fireball 2001,   !- Solar Collector Performance Name
-   Collector Surface,                                           !- Surface Name
-   Collector Inlet Node,                                     !- Inlet Node Name
-   Collector Outlet Node,                                   !- Outlet Node Name
-   0.00005;                                                               !- Maximum Flow Rate (m3/s)
-```
-
-
-### Solar Collector FlatPlate Water Output
-
-The following output variables are reported for the SolarCollector:FlatPlate:Water object:
-
-* HVAC,Average,Solar Collector Incident Angle Modifier []
-
-* HVAC,Average,Solar Collector Efficiency []
-
-* HVAC,Average,Solar Collector Heat Transfer Rate [W]
-
-* HVAC,Average,Solar Collector Heat Gain Rate [W]
-
-* HVAC,Average,Solar Collector Heat Loss Rate [W]
-
-* HVAC,Sum,Solar Collector Heat Transfer Energy [J]
-
-#### Solar Collector Incident Angle Modifier [ ]
-
-The incident angle modifier is an important intermediate value used in the SRCC calculation of solar collector performance.   The value reported here is the combined result for the current time that includes incident angles of beam solar, diffuse solar from sky, and diffuse solar from ground.
-
-#### Solar Collector Efficiency [ ]
-
-The overall collector efficiency.   This is the ratio of collected energy and the incident solar energy.   The efficiency can be greater than 1 at times when the outdoor air temperature is warm enough.
-
-#### Solar Collector Heat Transfer Rate [W]
-
-#### Solar Collector Heat Transfer Energy [J]
-
-These are the overall rate (in W) and amount of energy ( in J) transferred to the collector   s circulating fluid.   Positive values indicate heating of the fluid while negative values indicate cooling of the fluid.
-
-#### Solar Collector Heat Gain Rate [W]
-
-This is the overall rate of heat addition to the collector   s circulating fluid in Watts.   Values are always positive or zero.   If the fluid is actually cooled then the value is zero.
-
-#### Solar Collector Heat Loss Rate [W]
-
-This is the overall rate of heat loss from the collector   s circulating fluid in Watts.   Values are always positive or zero.   If the fluid is actually heated then the value is zero.
-
-In addition, several surface variables are also relevant for the collector   s surface object (BuildingSurface:Detailed or Shading:Zone:Detailed):
-
-* Zone,Average,Surface Outside Face Sunlit Area [m2]
-
-* Zone,Average,Surface Outside Face Sunlit Fraction []
-
-* Zone,Average,Surface Outside Face Incident Solar Radiation Rate per Area [W/m2]
-
-* Zone,Average,Surface Outside Face Incident Beam Solar Radiation Rate per Area [W/m2]
-
-* Zone,Average,Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area [W/m2]
-
-* Zone,Average,Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area [W/m2]
-
-* Zone,Average,Surface Outside Face Beam Solar Incident Angle Cosine Value []
-
-
-
-The temperatures at the inlet and outlet nodes and the collector mass flow rate can be monitored using the system node output variables:
-
-* HVAC,Average,System Node Temperature [C]
-
-* HVAC,Average,System Node Mass Flow Rate [kg/s]
-
-
-
-### SolarCollectorPerformance:FlatPlate
-
-The SolarCollectorPerformance:FlatPlate object contains the thermal and optical performance parameters for a single collector module. These parameters are based on the testing methodologies described in ASHRAE Standards 93 and 96. The Solar Rating and Certification Corporation (SRCC) applies these standards in their rating procedures of solar collectors. The ratings for commercially available collectors in North America are published in the *Directory of SRCC Certified Solar Collector Ratings*. The SRCC database has also been converted into an EnergyPlus data set of SolarCollectorPerformance:FlatPlate objects that is included with the program (see SolarCollectors.idf in the DataSets folder).
-
-The coefficients for the energy conversion efficiency and incident angle modifier allow first order (linear) or second order (quadratic) correlations. To use a first order correlation, the second order coefficient must be left blank or set to zero.
-
-In order for the model to work correctly, the test conditions for which the performance coefficients were measured must be specified in the fields:   *Test Fluid*, *Test Volumetric Flow Rate*, and *Test Correlation Type*. Currently, only water is allowed as the *Test Fluid*.
-
-For more detailed information about the performance coefficients, see the *EnergyPlus Engineering Reference Document*.
-
-#### Field: Name
-
-The unique name of the SolarCollectorPerformance:FlatPlate object.
-
-#### Field: Gross Area
-
-The gross area of the collector module [m<sup>2</sup>]. This value is mainly for reference. The area of the associated collector surface object is used in all calculations.
-
-#### Field: Test Fluid
-
-The fluid that was used in the testing procedure that resulted in the thermal and optical performance coefficients below. Currently only    Water    is allowed.   This the fluid during the collector testing, not the fluid used during a particular EnergyPlus run.
-
-#### Field: Test Flow Rate
-
-The volumetric flow rate during testing [m<sup>3</sup>/s]. If the value is available as flow rate per unit area, it is recommended to multiply by the *Gross Area* of the collector module, not the net aperture area.
-
-#### Field: Test Correlation Type
-
-This field specifies type of temperature used to develop the correlation equations.   The testing procedure is based on an experimental correlation using either    Inlet,       Average,    or    Outlet    temperature.   Enter one of these choices. The ASHRAE Standards 93 and 96 always use Inlet temperature.
-
-#### Field: Coefficient 1 of Efficiency Equation
-
-First coefficient of efficiency equation for energy conversion [dimensionless].   This is the Y-intercept term.
-
-#### Field: Coefficient 2 of Efficiency Equation
-
-Second coefficient of efficiency equation for energy conversion [W/m<sup>2</sup>-K].   This is the first-order term.
-
-#### Field: Coefficient 3 of Efficiency Equation
-
-Third coefficient of efficiency equation for energy conversion [W/m<sup>2</sup>-K<sup>2</sup>]. This field is optional. This is the second-order term. If left blank or set to zero, a first-order linear correlation is used.
-
-#### Field: Coefficient 2 of Incident Angle Modifier
-
-Second coefficient of the incident angle modifier equation. This the first-order term. (There is no *Coefficient 1 of Incident Angle Modifier* because that number is always 1.0.)
-
-#### Field: Coefficient 3 of Incident Angle Modifier
-
-Third coefficient of the incident angle modifier equation. This is the second-order term. This field is optional. If left blank or set to zero, a first order linear correlation is used.
-
-An example of this object follows.
-
-```idf
-   SolarCollectorPerformance:FlatPlate,
-       Alternate Energy Technologies AE-32,   !- Name
-       2.9646,                                   !- Gross Area {m2}
-       WATER,                                     !- Test Fluid
-       0.0000388,                             !- Test Flow Rate {m3/s}
-       INLET,                                     !- Test Correlation Type
-       0.691,                                     !- Coefficient 1 of Efficiency Equation {dimensionless}
-       -3.396,                                   !- Coefficient 2 of Efficiency Equation {W/m2-K}
-       -0.00193,                               !- Coefficient 3 of Efficiency Equation {W/m2-K2}
-       -0.1939,                                 !- Coefficient 2 of Incident Angle Modifier
-       -0.0055;                                 !- Coefficient 3 of Incident Angle Modifier
-```
-
-
-
-### SolarCollectorPerformance:FlatPlate Output
-
-This object does not generate any output; see SolarCollector:FlatPlate:Water Output
-
-### SolarCollector:IntegralCollectorStorage
-
-The Integral-Collector-Storage (ICS) solar collector model simulates glazed collectors with integral storage unit. The SolarCollector:IntegralCollectorStorage object represents a single collector module connected to the plant loop. The thermal and optical properties of the collector module are calculated from inputs in SolarCollectorPerformance:IntegralCollectorStorage object. A surface or shading object defines the collector tilt, and azimuth. The collector surface participates normally in all shading calculations if the "FullExterior," "FullInteriorAndExterior,"    FullExteriorWithReflections    , or    FullInteriorAndExteriorWithReflections    flags are set in the Solar Distribution field of the Building object. Inlet and outlet nodes are specified for plant connections on the demand side of the plant loop.   The SurfaceProperty:ExteriorNaturalVentedCavity, object is required to describe the surface properties, the characteristics of the cavity and opening for natural ventilation if OtherSideConditionsModel is specified as the collector bottom surface outside boundary condition type.
-
-#### Field: Name
-
-The unique name of the SolarCollector:IntegralCollectorStorage object.
-
-#### Field: Solar Collector Performance Name
-
-Reference name of a SolarCollectorPerformance:IntegralCollectorStorage object that defines the thermal and optical properties of the collector.
-
-#### Field: Surface Name
-
-Reference to one of the many different types of surfaces such as the BuildingSurface:Detailed or the Shading:Zone:Detailed objects. The surface named here is used to define the solar collector tilt, and azimuth. The collector shades the surface it is mounted on and hence impacts the surface heat balance.
-
-#### Field: Bottom surface Boundary Conditions Type
-
-This field contains the type of boundary conditions applicable to the ICS collector bottom surface. Allowed boundary condition types are: AmbientAir and OtherSideConditionsModel.   If the other side conditions model is selected, specify the name of the SurfaceProperty:OtherSideConditionsModel object in the next input field, otherwise, leave the next input field blank.   The AmbientAir boundary condition uses outdoor air temperature as boundary condition, hence the subsurface is assumed to be exposed to the sun and wind.
-
-#### Field: Other Side Conditions Model Name
-
-This field contains the name of a SurfaceProperty:OtherSideConditionsModel object declared elsewhere in the input file. This will connect the collector to the exterior boundary conditions for the underlying heat transfer surface specified above..
-
-#### Field: Inlet Node Name
-
-The name of the inlet node connection to the plant loop.
-
-#### Field: Outlet Node Name
-
-The name of the outlet node connection to the plant loop.
-
-#### Field: Maximum Flow Rate
-
-The maximum flow rate [m3/s] allowed through the collector. This field is optional. If not specified, the collector will allow as much flow as the rest of the plant can deliver.
-
-
-
-An example follows.
-
-```idf
-SolarCollector:IntegralCollectorStorage,
-   Collector 1,                                                       !- Name
-   ICS Solar Collector,                                       !- Solar Collector Performance Name
-   ICS Collector Surface,                                   !- Surface Name
-   OtherSideConditionsModel,                             !- Bottom Surface Boundary Conditions Type
-   ICS OSCM,                                                             !- Boundary Condition Model Name
-   Collector Inlet Node,                                     !- Inlet Node Name
-   Collector Outlet Node,                                   !- Outlet Node Name
-   0.00005;                                                               !- Maximum Flow Rate (m3/s)
-```
-
-### SolarCollectorPerformance:IntegralCollectorStorage
-
-The SolarCollectorPerformance:IntegralCollectorStorage object contains the thermal and optical performance parameters for a single collector module. The transmittance-absorptance product of the absorber and cover system is determined from optical properties specified. For more detailed information about the calculation procedure, see the *EnergyPlus Engineering Reference* Document.
-
-#### Field: Name
-
-The unique name of the SolarCollectorPerformance:IntegralCollectorStorage object.
-
-#### Field: ICS Collector Type
-
-This input field is the ICS collector type.     Currently only RectangularTank type is allowed.
-
-#### Field: Gross Area
-
-This input field is the gross area of the collector module in m2.   This gross area is used in the energy balance equations.
-
-#### Field: Collector Water Volume
-
-This input field is the volume of water in the solar collector in m3.
-
-#### Field: Bottom Heat Loss Conductance
-
-This input field is the collector bottom heat loss conductance in W/m2K.   This value is calculated from thermal conductivity and thickness of the bottom insulation.
-
-#### Field: Side Heat Loss Conductance
-
-This input field is the collector side heat loss conductance in W/m2K.   This value is calculated from thermal conductivity and thickness of the side insulation.
-
-#### Field: Collector Aspect Ratio
-
-This input field is the ratio of the short side (width) of the collector to the long side (length) of the collector.   This value is used only for calculating the collector side area along with the collector side height specified in the next input filed.   This ratio is less or equal to 1.0.
-
-#### Field: Collector Side Height
-
-This input field is height of collector side in m.   This height is used to estimate the collector side area for heat loss calculations along with heat loss coefficient specified in the input field above.
-
-#### Field: Thermal Mass of Absorber Plate
-
-This input field is thermal-mass of the absorber plate per unit area of the collector in [J/m2×K].   This input value multiplied by the absorber gross area determines the thermal mass of the absorber plate. It is estimated from the specific heat, density and average thickness of the absorber plate. If zero is specified then the absorber plate energy balance reduces to steady state form.
-
-#### Field: Number of Covers
-
-Number of transparent collector covers.   Common practice is to use two covers: glass as the outer cover and Teflon as the inner cover. If single cover is specified leave the inner cover optical and thermal properties input fields blank.
-
-#### Field: Cover Spacing
-
-This input field provides the spacing between the two transparent covers, and the spacing between the inner cover and the absorber plate in m.   Default value is 0.05m.
-
-#### Field: Refractive Index of Outer Cover
-
-This is the average Refractive index for solar spectrum range of the outer transparent cover material.   Glass is used as the outer cover.   Average refractive index value for non-absorbing glass used in solar collectors over solar spectrum range is 1.526.
-
-#### Field: Extinction Coefficient Times Thickness of Outer Cover
-
-This input field is the product of the extinction coefficient and the thickness of the out cover material.   The extinction coefficient for glass types approximately varies from 4m<sup>-1</sup> to 32 m<sup>-1</sup>.   The extinction coefficient for low-iron glass, which is the default outer cover material, is 15 m<sup>-1</sup>. The default value for extinction coefficient times thickness (KL) is 0.045 (=15.0 x0.003), which is the product of the default extinction coefficient of 15m<sup>-1</sup> and 3.0mm thick glass.
-
-#### Field: Emissivity of Outer Cover
-
-This input field value is thermal emissivity of the outer collector cover.   The default value assumes low-iron glass with thermal emissivity of 0.88.
-
-#### Field: Refractive Index of Inner Cover
-
-This input field is the average Refractive index of the inner transparent cover of the collector.   Commonly Teflon (PolytetraFluoroethylene) is used as the inner cover.   The average refractive index value over the solar spectrum range for Teflon is 1.37.
-
-#### Field: Extinction Coefficient Times Thickness of Inner Cover
-
-This input field is the product of the extinction coefficient (K) and the thickness (L) of the inner cover material.   The inner cover material is more transparent than the out cover, very thin and hence their thickness can be assumed to be negligible. The default value for extinction coefficient times thickness (KL) is 0.008 (=40.0x0.0002), which is the product of extinction coefficient of 40m<sup>-1</sup> and a thickness of 0.2mm.
-
-#### Field: Emissivity of Inner Cover
-
-This input field value is thermal emissivity of the inner transparent collector cover.   The default value assumes plastic sheet with thermal emissivity of 0.30.   This value is used in the thermal analysis only.
-
-#### Field: Absorptance of Absorber Plate
-
-This input field is shortwave or solar absorptance of the absorber plate.   The default value is 0.96.
-
-#### Field: Emissivity of Absorber Plate
-
-This input field value is thermal emissivity of the absorber plate.   Default value is 0.30.   This input value is used in the thermal analysis only.
-
-
-
-An example follows.
-
-```idf
-     SolarCollectorPerformance:IntegralCollectorStorage,
-       ICS Experimental,               !- Name
-       RectangularTank,                 !- ICS Collector Type
-       0.37275,                                 !- Gross Area {m2}
-       0.0195875,                             !- Collector Water Volume {m3}
-       0.10,                                       !- Bottom Heat Loss Conductance
-       1.00,                                       !- Side Heat Loss Conductance
-       0.8,                                         !- Collector Aspect Ratio {dimensionless}
-       0.08,                                       !- Collector Side Height {m}
-       5800.0,                                         !- Thermal Mass of Absorber Plate {J/m2K}
-       1,                                             !- Number of Covers {dimensionless}
-       0.05,                                       !- Cover Spacing {m}
-       1.526,                                     !- Refractive Index of Outer Cover {dimensionless}
-       0.0125,           !- Extinction Coefficient Times Thickness of Outer Cover {dimensionless}
-       0.88,                                       !- Emissivity of Outer Cover
-       1.126,                                     !- Refractive Index of Inner Cover {dimensionless}
-       0.0126,           !- Extinction Coefficient Times Thickness of Inner Cover {dimensionless}
-       0.88,                                       !- Emissivity of Inner Cover {dimensionless}
-       0.96,                                       !- Absorptance of Absorber Plate {dimensionless}
-       0.60;                                       !- Emissivity of Absorber Plate {dimensionless}
-```
-
-
-
-### Solar Collector Integral Collector Storage Outputs
-
-The following output variables are reported for the SolarCollector:IntegralCollectorStorage object:
-
-* HVAC,Average,Solar Collector Storage Water Temperature [C]
-
-* HVAC,Average,Solar Collector Absorber Plate Temperature [C]
-
-* HVAC,Average,Solar Collector Overall Top Heat Loss Coefficient [W/m2-C]
-
-* HVAC,Average,Solar Collector Thermal Efficiency []
-
-* HVAC,Average,Solar Collector Storage Heat Transfer Rate [W]
-
-* HVAC,Sum,Solar Collector Storage Heat Transfer Energy [J]
-
-* HVAC,Average,Solar Collector Heat Transfer Rate [W]
-
-* HVAC,Sum,Solar Collector Heat Transfer Energy [J]
-
-* HVAC,Average,Solar Collector Skin Heat Transfer Rate [W]
-
-* HVAC,Sum, Solar Collector Skin Heat Transfer Energy [J]
-
-* HVAC,Average,Solar Collector Transmittance Absorptance Product []
-
-#### Solar Collector Storage Water Temperature [C]
-
-This output variable is the ICS collector stored water average temperature at a given time steps in degree Celsius. This temperature is the same as the collector ICS collector leaving water temperature.
-
-#### Solar Collector Absorber Plate Temperature [C]
-
-This output variable is the ICS collector absorber plate average temperature at a given time steps in degree Celsius.
-
-#### Solar Collector Thermal Efficiency [ ]
-
-This output variable is the instantaneous thermal efficiency of the ICS solar collector in per cent.   This value is determined from net useful energy collected and the total incident solar radiation for each time step. The net useful energy collected is the sum of the energy stored in the collector and net useful energy delivered.
-
-#### Solar Collector Storage Heat Transfer Rate [W]
-
-#### Solar Collector Storage Heat Transfer Energy [J]
-
-These output variables are the instantaneous rate of change of the energy and the change in energy of the water in the ICS solar collector in Watts, and Joules, respectively.
-
-#### Solar Collector Skin Heat Transfer Rate [W]
-
-#### Solar Collector Skin Heat Transfer Energy [J]
-
-These output variables are the instantaneous skin heat loss rate and the heat loss energy of the ICS solar collector for each time steps in Watts, and Joules respectively.   The skin heat loss rate is the sum of the heat losses through the top, bottom and sides of the collector surfaces.   This value is mostly negative, but can have a positive value (heat gain) when the outdoor air temperature is warmer than the collector.
-
-#### Solar Collector Heat Transfer Rate [W]
-
-#### Solar Collector Heat Transfer Energy [J]
-
-This output variable is the heat rate and Energy transferred from the ICS collector to the collector loop fluid (water) in Watts and Joule, respectively.   This value is determined from the collector water mass flow rate, specific heat of water and the temperature difference between the collector water outlet and inlet nodes at each time step. The value is positive when the fluid is heated or negative when cooled.
-
-#### Solar Collector Transmittance Absorptance Product [ ]
-
-This output variable is the transmittance-absorptance product of the covers and absorber system of the ICS solar collector.   This value ranges from 0.0 to less than 1.0.
-
-#### Solar Collector Overall Top Heat Loss Coefficient [W/m2-C]
-
-This output variable is the overall heat loss coefficient from the absorber plate to the ambient air calculated for each time step.
-
-### SolarCollector:FlatPlate:PhotovoltaicThermal
-
-This object is used to model hybrid photovoltaic-thermal (PVT) solar collectors that convert incident solar energy into both electricity and useful thermal energy.   This object describes the PVT solar collector by referencing other objects that provide more detail or connections to other parts of the EnergyPlus model.
-
-The PVT solar collectors need to be connected to either an HVAC air system or a plant loop for collected thermal energy to be utilized.   The input field for the type of thermal working fluid informs the program how the PVT collector is expected to be connected.   If the the working fluid is air, then the PVT collectors are modeled as a ventilation air pretreatment component and connected to an outdoor air system.   If the working fluid is water, then the PVT collectors are modeled as a hot water solar collector and are connected to a plant loop with a water thermal storage tank.
-
-#### Field: Name
-
-This field should contain a unique name chosen by the user to identify a specific PVT collector in the building model.
-
-#### Field: Surface Name
-
-This field is the user-defined name of a surface object (defined elsewhere) to which the PVT module is attached.   These can be any type of building surface that is exposed to the exterior environment.   The model uses the named surface   s geometry for the PVT solar collector.
-
-#### Field: Photovoltaic-Thermal Model Performance Name
-
-This field is the user-defined name of an object (defined elsewhere) that provides the performance details of the PVT module.   This should be the name of a SolarCollectorPerformance:PhotovoltaicThermal:Simple object.   Multiple different SolarCollector:FlatPlate:PhotovoltaicThermal objects can reference the same object that provides performance details.
-
-#### Field: Photovoltaic Generator Name
-
-This field is the user-defined name of a Generator:Photovoltaic object (defined elsewhere) that will be used to model the solar electric portion of the PVT solar collector.   The PVT models make any adjustments needed to model PV performance in the context of the PVT collector.
-
-#### Field: Thermal Working Fluid Type
-
-This field is the user   s choice for the type of fluid used to collect thermal energy.   PVT solar collectors can capture thermal energy in either air or water streams.   The choices available for this field are    Water    or    Air.      If the choice is    Air    then the PVT collector needs to be connected to an HVAC air system loop.   The PVT collector should be situated as the first component on an outdoor air inlet stream.   If the choice is    Water    then the PVT collector needs to be connected to a Plant water system loop.   The connections are made via node names which are defined in the following fields, depending on the working fluid type.
-
-#### Field: Water Inlet Node Name
-
-This field is the name of Plant loop node that serves as the inlet to the PVT collector.   This field is only used if the Thermal Working Fluid Type is set to    Plant/Water.   
-
-#### Field: Water Outlet Node Name
-
-This field is the name of a plant loop node that seves as the outlet from the PVT collector.   This field is only used if the Thermal Working Fluid Type is set to    Plant/Water.   
-
-#### Field: Air Inlet Node Name
-
-This field is the name of HVAC air loop node that serves as the inlet to the PVT collector.   This field is only used if the Thermal Working Fluid Type is set to    HVAC/Air.   
-
-#### Field: Air Outlet Node Name
-
-This field is the name of HVAC air loop node that serves as the outlet from the PVT collector.   This field is only used if the Thermal Working Fluid Type is set to    HVAC/Air.   
-
-#### Field: Design Flow Rate
-
-This field is used to describe the nominal volume flow rate of the thermal working fluid.   The units are m3/s.   The volume flow rate is autosizable.
-
-An example of this object follows.
-
-```idf
-   SolarCollector:FlatPlate:PhotovoltaicThermal,
-       PVT: 1_Ceiling ,                                             !- Name
-       1_Ceiling ,                                                       !- Surface Name
-       30percentPVThalfArea ,                                 !- Photovoltaic-Thermal Model Performance Name
-       PV:ZN_1_FLR_1_SEC_1_Ceiling ,                   !- Photovoltaic Name
-       Air ,                                                                   !- Thermal Working Fluid Type
-       ,                                                                           !- Water Inlet Node Name
-       ,                                                                           !- Water Outlet Node Name
-       ZN_1_FLR_1_SEC_1:Sys_OAInlet Node ,       !- Air Inlet Node Name
-       PVT:ZN_1_FLR_1_SEC_1_Ceiling Outlet ,   !- Air Outlet Node Name
-       Autosize ;                                                         !- Design Flow Rate
-```
-
-
-
-### Solar Collector FlatPlate PhotovoltaicThermal Outputs
-
-The output variables that are available for flat plate PVT include the following.
-
-* HVAC,Average,Generator Produced Thermal Rate [W]
-
-* HVAC,Sum,Generator Produced Thermal Energy [J]
-
-* HVAC,Average,Generator PVT Fluid Bypass Status [ ]
-
-* HVAC,Average,Generator PVT Fluid Inlet Temperature [C]
-
-* HVAC,Average,Generator PVT Fluid Outlet Temperature [C]
-
-* HVAC,Average,Generator PVT Fluid Mass Flow Rate [kg/s]
-
-#### Generator Produced Thermal Rate [W]
-
-#### Generator Produced Thermal Energy [J]
-
-These outputs are the thermal energy and power produced by the PVT collector.   PVT collectors are a type of cogenerator, producing both electrical and thermal power and these variables report the thermal portion in the same manner as other fuel-based cogenerators.   The thermal energy is placed on    HeatProduced    meter and is attributed to    SolarWater    or    SolarAir    depending on the type of working fluid.   The generator thermal production is also reported at the load center level.
-
-#### Generator PVT Fluid Bypass Status [ ]
-
-This output variable indicates the status a bypass damper.   It is only available for air-based PVT.   There are no dimensions and the range is between 0.0 and 1.0.   If the value is 0.0, then there is no bypassing and all the working fluid goes through the collector.   If the value is 1.0, then there is complete bypassing and all the working fluid goes around the collector.   If the value is between 0.0 and 1.0, then the model is effectively mixing bypass and collector streams to target a temperature setpoint placed on the outlet node.
-
-#### Generator PVT Fluid Inlet Temperature [C]
-
-This report is the inlet temperature of the working fluid that enters the PVT collector
-
-#### Generator PVT Fluid Outlet Temperature [C]
-
-This report is the outlet temperature of the working fluid that leaves the PVT collector
-
-#### Generator PVT Fluid Mass Flow Rate [kg/s]
-
-This report is the mass flow rate of the working fluid through the PVT collector.   This is the overall mass flow rate, portions of the flow may be internally bypassed around the collector itself for control modulation.
-
-### SolarCollectorPerformance:PhotovoltaicThermal:Simple
-
-This object is used to provide performance details for the simple PVT model.   This is a simple user-defined efficiency model.   Thermal conversion efficiency is a constant or scheduled value.   There are no output variable for this object, reporting is done by the parent PVT object.
-
-#### Field: Name
-
-This field is the unique name for this object.
-
-#### Field: Fraction of Surface Area with Active Thermal Collector
-
-This field is the fraction of the surface area that is active.   It should be a decimal fraction between 0.0 and 1.0.   The area of the PVT   s surface will be multiplied by this fraction to determine the active area of the PVT collector(s).
-
-#### Field: Thermal Conversion Efficiency Input Mode Type
-
-This field is used to determine how the thermal efficiency is input.   There are two choices,    Fixed    or    Scheduled.      If this field is set to Fixed, then a constant value for thermal efficiency will be used (set in next field).   If this field is set to Scheduled, then the thermal efficiency values are defined in a schedule.
-
-#### Field: Value for Thermal Conversion Efficiency if Fixed
-
-This field is used to provide a value for the efficiency with which solar energy is collected in the working fluid.   This field is only used if the input mode is set to    Fixed    in the previous field.   Efficiency is defined as the thermal energy collected divided by the incident solar radiation.   The value should be between 0.0 and 1.0.   The user should be careful that the thermal efficiency and the electrical efficiency be consistent with each other because the overall efficiency of the PVT collector is the combination of both thermal and electrical.
-
-#### Field: Name of Schedule for Thermal Conversion Efficiency
-
-This field is used for the name of a schedule that provides values for the efficiency with which solar energy is collected in the working fluid.   This field is only used if the input mode is set to    Scheduled    in the field above.   Efficiency is defined as the thermal energy collected divided by the incident solar radiation.   The values in the named schedule should be between 0.0 and 1.0.   The user should be careful that the thermal efficiency and the electrical efficiency be consistent with each other because the overall efficiency of the PVT collector is the combination of both thermal and electrical.
-
-#### Field: Front Surface Emittance
-
-This field is used to describe an average value for the total hemispherical emittance of the collector   s front face exposed to the sky.   This is used to model cooling applications where the PVT collectors are operated at night to cool the working fluid.
-
-An example input object follows.
-
-```idf
-   SolarCollectorPerformance:PhotovoltaicThermal:Simple,
-       20percentEffPVhalfArea ,                 !- Name
-       0.5 ,                                                       !- Fraction of Surface Area with Active Thermal Collector
-       Fixed ,                                                   !- Thermal Conversion Efficiency Input Mode Type
-       0.2 ,                                                       !- Value for Thermal Conversion Efficiency if Fixed
-         ,                                                             !- Name of Schedule for Thermal Conversion Efficiency
-       0.84 ;                                                     !- Front Surface Emittance
-```
-
-### Solar Collector Heating System Plant Connections
-
-This section provides an overview of how to model solar heating systems.   A solar heating system can be constructed using a combination of solar collectors, pumps, water tanks and water heaters. The solar collector must be connected on the demand side of the plant loop. Multiple collector modules can be combined in series and parallel using the normal plant connection rules. The supply side of the plant loop should contain a water heater with the solar collector loop connecting to the *Source Side Inlet* and *Source Side Outlet* nodes. As usual, the pump must be the first component on the supply side.
-
-If the solar heating system is for domestic hot water (or service water heating) usage only, the field *Use Flow Rate Fraction Schedule Name* of the WaterHeater:Mixed object can be used to avoid additional plant connections. If the system has more complicated hot water requirements or if the system is for space heating, the *Use Side Inlet* and *Use Side Outlet* nodes must be connected to another plant loop to serve zone and non-zone equipment. (See the WaterHeater:Mixed object documentation for more information.)
-
-![](media/image339.png)
-
-Figure 132. Solar Collector Plant Loop Connection Diagram
-
-NOTE:   The EnergyPlus plant simulation requires the pump to be the first component on the supply side. This may be different from the way the solar heating system is actually configured. This should not affect the validity of the simulation results.
-
-In order to realize energy savings with a solar heating system, it is best to use a two-tank system with a storage tank and auxiliary water heater. The storage tank gathers heat directly from the solar collectors and stores it for later use. The storage tank is modeled using a WaterHeater:Mixed object with the *Heater Maximum Capacity* set to zero. The auxiliary water heater is positioned downstream of the storage tank on the supply side of the main plant loop. The auxiliary water heater, or booster water heater, provides additional heat if the storage tank water is not hot enough. The auxiliary water heater can be modeled as an instantaneous/tankless water heater or as a standard tanked water heater with heating source (see WaterHeater:Mixed).
-
-![](media/image340.png)
-
-Figure 133. Two-Tank Solar Heating System Connection Diagram
-
-Another strategy to consider for solar heating systems is to allow the storage tank to reach a much higher temperature than necessary for the end use. This allows the tank to store more energy from the solar collectors, when it is available. However, for applications such as domestic hot water, it is undesirable and unsafe to supply excessive hot water temperatures at the point of demand. To take advantage of higher storage temperatures, yet still avoid scalding temperatures at the faucet, the hot water leaving the storage tank can be tempered with cold water using a three-way valve to achieve the target temperature. See the TemperingValve object documentation for more details.
-
-A complete two-tank solar heating system with tempering valve is shown below.
-
-![](media/image341.png)
-
-Figure 134. Two-Tank Solar Heating System with Tempering Valve
-
-### Solar Heating System Control
-
-There are several options for controlling a solar heating system in EnergyPlus. Since the solar collectors request a constant flow demand based on their *Maximum Flow Rate*, the limiting factor is actually the flow rate determined by the loop pump. Therefore the entire system can be controlled using the *Pump Flow Rate Schedule* of the pump. If the schedule is omitted, the pump and system will run all the time (without any other controls specified). This is usually not the best way to operate a solar heating system.
-
-To better control the collector loop, a differential thermostat can be used to compare the temperature in the water heater to the temperature in the collector so that the pump is only turned on when there is a useful heat gain. The differential thermostat is simulated using the AvailabilityManager:DifferentialThermostat object. For a typical system, the *Hot Node Name* field refers to an outlet node of one of the collector modules. The *Cold Node Name* field refers to the *Source Side Outlet* node, i.e. the cold storage water leaving the water heater. The fields *Temperature Difference On Limit* and *Temperature Difference Off Limit* are usually 8    12 C and 1     3 C respectively. If the two temperature differences are too close, it is possible for the system to turn on and off rapidly without much useful heat gain. This can also occur if the flow rate through the collector is too high. Without flow the fluid in the collector heats up more quickly; when high flow is turned on, all of the hot fluid is removed and the temperature drops, forcing the system off again.
-
-Another control method is to use a photovoltaic panel to power the pump. The system begins pumping when there is enough solar radiation to operate the pump. This is not yet implemented in EnergyPlus.
-
-#### Freeze Prevention
-
-In climates with a cold season, the solar heating system must be designed to avoid the risk of fluid freezing in the solar collector or exposed pipes and causing damage. This is not a problem if air is the heat transfer fluid. With water, however, there are several strategies that can minimize the risk.
-
-*Seasonal schedule*. The simplest strategy is to not use the system during the cold season. This is a hassle because it requires the collector to be manually drained of all fluid. The benefits of the solar heating system are also lost during this time. This can be simulated in EnergyPlus with the appropriate pump schedule for the collector system.
-
-*Antifreeze*. The freezing point of the liquid is decreased by adding antifreeze to the water or using a different heat transfer liquid with a lower freezing point. This cannot yet be simulated in EnergyPlus because only pure water is currently allowed in plant loops.
-
-*Drain-back system*. This strategy automatically empties the collector when the pump is not running. This scenario is modeled by default in EnergyPlus, although the extra pump energy required to start the system is not taken into account.
-
-*Recirculation system*. This strategy automatically recirculates warm liquid from the storage tank back through the collector to maintain the system above the freezing point. There are system losses using this method. This can be simulated in EnergyPlus by using AvailabilityManager:LowTemperatureTurnOn to force the system to turn on when the outdoor air temperature or collector outlet temperature falls below a specified minimum.
-
-#### Additional Controls
-
-In addition to freeze prevention, it is also necessary to prevent the system from becoming too hot. This is usually a safety issue for the water heater. For this case it is important to have a high temperature cutoff to stop the pump before damaging the water heater. This is accomplished with a AvailabilityManager:HighTemperatureTurnOff.
-
-#### System Availability Manager List Example
-
-To use the availability managers for the control cases described above, a AvailabilityManagerAssignmentList must be defined and referenced in the PlantLoop object of the collector loop. An example of a differential thermostat, recirculation for freeze prevention, and high temperature cutoff is shown below:
-
-
-
-```idf
-AvailabilityManagerAssignmentList,
-   Collector Loop Availability Manager List,             !- Name
-   AvailabilityManager:HighTemperatureTurnOff,         !- Availability Manager 1 Object Type
-   High Temperature Turn Off Availability Manager, !- Availability Manager 1 Name
-   AvailabilityManager:HighTemperatureTurnOn,           !- Availability Manager 2 Object Type
-    Low Temperature Turn On Availability Manager,     !- Availability Manager 2 Name
-   AvailabilityManager:DifferentialThermostat,         !- Availability Manager 3 Object Type
-   Differential Thermostat Availability Manager;     !- Availability Manager 3 Name
-
-
-  AvailabilityManager:HighTemperatureTurnOff,           ! For water heater safety
-   High Temperature Turn Off Availability Manager, !- Name
-   Water Heater Use Outlet Node,                                     !- Sensor Node Name
-   60.0;                                                                                     !- Temperature (C)
-
-
-  AvailabilityManager:HighTemperatureTurnOn,             ! For freeze prevention by recirculation
-   Low Temperature Turn On Availability Manager,     !- Name
-   Collector Outlet Node,                                                   !- Sensor Node Name
-   0.0;                                                                                       !- Temperature (C)
-
-
-  AvailabilityManager:DifferentialThermostat,           ! For useful heat gain from collector to tank
-   Differential Thermostat Availability Manager,     !- Name
-   Collector Outlet Node,                                                   !- Hot Node Name
-   Water Heater Source Outlet Node,                               !- Cold Node Name
-   10.0,                                                                                     !- Temperature Difference On Limit (delta C)
-   2.0;                                                                                       !- Temperature Difference Off Limit (delta C)
-```
-
-
-The AvailabilityManager:DifferentialThermostat object must always be the last manager in the availability manager list. See the AvailabilityManagerAssignmentList object documentation for more information.
-
-### SolarCollector:UnglazedTranspired
-
-This object is used to model unglazed transpired solar collectors (UTSC) used to condition outdoor air. These collectors are generally used to heat air drawn through perforated absorbers that are heated by the sun and also recover heat conducted out through the underlying wall. The SolarCollector:UnglazedTranspired****object represents a single collector attached to one or more BuildingSurface:Detailed objects and to one or more outdoor air systems. Therefore the transpired collector is part of both the thermal envelope and the HVAC system. An example file is provided called TranspiredCollectors.idf.
-
-The area and orientation of the collector is obtained from BuildingSurface:Detailed objects, which are referenced by name. Although the collector surface itself is slightly detached from the underlying building wall (or roof), no additional surface object is needed to represent the collector itself. When modeling transpired collectors, it is important to consider the size of the collector when developing the building model   s BuildingSurface:Detailed objects because the underlying surfaces must match the collector. For example, if the collector covers only part of the wall, then that wall should be split into separate surfaces where one matches the size of the collector. A single collector can be associated with as many BuildingSurface:Detailed objects as desired (although if you need to use more than 10 surfaces, then the IDD will need to be extended). The collector can be arranged at any tilt angle by describing the surfaces appropriately. The surfaces need not be contiguous nor have the same orientation, but the program will issue warnings if surfaces have widely ranging tilts and azimuths.
-
-The collector conditions outdoor air and is connected to the outdoor air system using the usual method of specifying node names. Using the UTSC model requires specifying a relatively complete HVAC air system that includes an outdoor air path. This will typically require using a set of objects that, at a minimum, will include:   AirLoopHVAC:ControllerList, AirLoopHVAC:OutdoorAirSystem:EquipmentList, AirLoopHVAC:OutdoorAirSystem, OutdoorAir:NodeList, OutdoorAir:Mixer, SetpointManager:MixedAir, and Controller:OutdoorAir. A single UTSC can serve more than one outdoor air system but requires also using a separate object, called SolarCollector:UnglazedTranspired:MultiSystem to specify node connections.
-
-Controls for the UTSC involve setting the rate of air flow and the status of a bypass damper. If the bypass damper is open, then all the ventilation air goes straight into the outdoor air mixer; if it closed, then all the air first passes through the UTSC. The bypass damper is modeled as completely open or completely closed. The UTSC bypass damper control is determined by an availability manager, the airflow set by the outdoor air mixer controls, and thermostatic type controls that decide if heating is useful. An availability schedule is used to bypass the collector for certain times of the year, eg. summer cooling season. The air flow rates are set by controls associated with the outdoor air mixer (see SetpointManager:MixedAir, and Controller:OutdoorAir). Thermostatic type control decides if the collector will provide useful heating based on either of two types of setpoints. The first type of temperature setpoint is managed by SetpointManager:MixedAir, where the UTSC model looks at a control node, usually the mixed air node. The second type is an extra setpoint especially for free heating that is managed within this object where the UTSC model looks at the zone air node.
-
-#### Field: Name
-
-This field contains a unique name for the unglazed transpired solar collector.
-
-#### Field: Boundary Conditions Model Name
-
-This field contains the name of a SurfaceProperty:OtherSideConditionsModel object declared elsewhere in the input file. This will connect the collector to the exterior boundary conditions for the underlying heat transfer surface.
-
-#### Field: Availability Schedule Name
-
-This field contains the name of a schedule that determines whether or not the UTSC is available. When the schedule value is less than or equal to zero, the UTSC is always bypassed. When the schedule value is greater than zero, the UTSC is available and will be used when other conditions are met, such as outdoor air requested by mixer and preheating has been determined to be beneficial based on thermostatic control. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Inlet Node Name
-
-This field contains the name of an air node that provides air into the UTSC. This node name should also be assigned to be an outdoor air node using the OutdoorAir:NodeList or OutdoorAir:Node objects. This node should also be named as the actuated node in a Controller:OutdoorAir object. If the UTSC is connected to more than one air system, then this field can be left blank and the SolarCollector:UnglazedTranspired:MultiSystem object should be used to define the nodes.
-
-#### Field: Outlet Node Name
-
-This field contains the name of an air node that is the outlet of the UTSC. This node name will typically be the inlet to the OutdoorAir:Mixer (if there is no other equipment on the outdoor air path). If the UTSC is connected to more than one air system, then this field can be left blank and the SolarCollector:UnglazedTranspired:MultiSystem object should be used to define the nodes.
-
-#### Field: Setpoint Node Name
-
-This field contains the name of an air node that has a setpoint manager controlling its temperature setpoint. This node name will typically be named as the control node in a a Controller:OutdoorAir object. If the UTSC is connected to more than one air system, then this field can be left blank and the SolarCollector:UnglazedTranspired:MultiSystem object should be used to define the nodes.
-
-#### Field: Zone Node Name
-
-This field contains the name of an air node for a thermal zone that is ultimately connected to the air system. This node is used with the setpoint schedule, defined in the following field, to provide an added layer of thermostatic control for the UTSC without affecting the control of auxiliary heating. If there is a single air system that is connected to more than one zone, then a single zone should be selected based on where the thermostat might be located. If the UTSC is connected to more than one air system, then this field can be left blank and the SolarCollector:UnglazedTranspired:MultiSystem object should be used to define the nodes.
-
-#### Field: Free Heating Setpoint Schedule Name
-
-This field contains the name of a temperature schedule defined elsewhere in the input file. This schedule should define temperatures *desired* in the zone, but not necessarily *required*. This secondary setpoint schedule is used to allow the UTSC to operate as if it has its own thermostat that is separate from the primary control mechanism. When the UTSC is used with auxiliary heating, the usual setpoint managers and temperature controllers will determine how the auxiliary heaters are controlled. This allows using a higher zone air temperature setpoint for controlling UTSC bypass than for the auxiliary heating system.
-
-#### Field: Diameter of Perforations in Collector
-
-This field is used to enter the effective diameter of the perforations in the collector surface. The diameter should be entered in meters. For perforations other than round, use an equivalent diameter for a round hole that would have the same area.
-
-#### Field: Distance Between Perforations in Collector
-
-This field is used to enter the pitch, or average, shortest distance between perforations.
-
-#### Field: Thermal Emissivity of Collector Surface
-
-This field is used to enter the thermal emissivity of the collector. This surface property is for longwave infrared radiation. The property is used for both sides of collector. Most painted materials have an emissivity of 0.9.
-
-#### Field: Solar Absorbtivity of Collector Surface
-
-This field is used to enter the solar absorbtivity of the collector. This surface property is for shortwave, solar radiation. The property is used for the front side of the collector that faces the environment. Darker colors have a higher absorbtivity. While black is the highest performance, other colors might be used to match the color scheme of the rest of the facade. The following table provides sample solar absorbtivities for different colors (source:   Conserval Engineering Inc., Toronto, Ontario, Canada).
-
-
-
-<table class="table table-striped">
-  <tr>
-    <th>Color Name of Kynar(R) [[1]](#_ftn1) Paint</th>
-    <th>Solar Absorptivity</th>
-  </tr>
-  <tr>
-    <td>Black</td>
-    <td>0.94</td>
-  </tr>
-  <tr>
-    <td>Classic Bronze</td>
-    <td>0.91</td>
-  </tr>
-  <tr>
-    <td>Chocolate Brown</td>
-    <td>0.9</td>
-  </tr>
-  <tr>
-    <td>Hartford Green</td>
-    <td>0.9</td>
-  </tr>
-  <tr>
-    <td>Med. Bronze</td>
-    <td>0.89</td>
-  </tr>
-  <tr>
-    <td>Boysenberry</td>
-    <td>0.86</td>
-  </tr>
-  <tr>
-    <td>Rocky Grey</td>
-    <td>0.85</td>
-  </tr>
-  <tr>
-    <td>Regal Blue</td>
-    <td>0.85</td>
-  </tr>
-  <tr>
-    <td>Forest Green</td>
-    <td>0.84</td>
-  </tr>
-  <tr>
-    <td>Hemlock Green</td>
-    <td>0.82</td>
-  </tr>
-  <tr>
-    <td>Slate Blue</td>
-    <td>0.8</td>
-  </tr>
-  <tr>
-    <td>Redwood</td>
-    <td>0.79</td>
-  </tr>
-  <tr>
-    <td>Teal</td>
-    <td>0.79</td>
-  </tr>
-  <tr>
-    <td>Slate Grey</td>
-    <td>0.79</td>
-  </tr>
-  <tr>
-    <td>Patina Green</td>
-    <td>0.77</td>
-  </tr>
-  <tr>
-    <td>Mint Green</td>
-    <td>0.71</td>
-  </tr>
-  <tr>
-    <td>Dove Grey</td>
-    <td>0.69</td>
-  </tr>
-  <tr>
-    <td>Mission Red</td>
-    <td>0.69</td>
-  </tr>
-  <tr>
-    <td>Sierra Tan</td>
-    <td>0.65</td>
-  </tr>
-  <tr>
-    <td>Brite Red</td>
-    <td>0.59</td>
-  </tr>
-  <tr>
-    <td>Rawhide</td>
-    <td>0.57</td>
-  </tr>
-  <tr>
-    <td>Sandstone</td>
-    <td>0.54</td>
-  </tr>
-  <tr>
-    <td>Silversmith</td>
-    <td>0.53</td>
-  </tr>
-  <tr>
-    <td>Coppertone</td>
-    <td>0.51</td>
-  </tr>
-  <tr>
-    <td>Concord Cream</td>
-    <td>0.45</td>
-  </tr>
-  <tr>
-    <td>Ascot White</td>
-    <td>0.4</td>
-  </tr>
-  <tr>
-    <td>Bone White</td>
-    <td>0.3</td>
-  </tr>
-</table>
-
-([[1]](#_ftnref1) Kynar is a registered trademark of Elf Atochem North America, Inc.)
-
-
-
-#### Field: Effective Overall Height of Collector
-
-This field is used to enter a nominal height for the collector. This value is used in the program to determine a length scale in the vertical direction for the buoyancy-driven portion of natural ventilation that occurs when the collector is inactive. (Note that most of the geometry information is obtained from the underlying surfaces.)   The value entered here is adjusted inside the program to account for tilt of the collector. While the value here would generally correspond to the actual distance/height, its value is not critical and it can be used to adjust modeling the air exchange rates in passive mode. If the collector is horizontal, then the length scale is obtained from the following field.
-
-#### Field: Effective Gap Thickness of Plenum Behind Collector
-
-This field is used to enter a nominal gap thickness for the collector. This distance value is only used when the collector is near horizontal to determine a length scale in the vertical direction for buoyancy calculations. For example, if the collector is mounted on a flat roof, its tilt-adjusted height is zero and the program will use this gap thickness as a length scale rather than the height from the previous field.
-
-#### Field: Effective Cross Section Area of Plenum Behind Collector
-
-This field is used to enter the nominal cross sectional area of the gap behind the collector. This area is used to determine a velocity scale for surface convection heat transfer correlations when the collector is active. This value is generally the average gap thickness times the average width of the collector.
-
-#### Field: Hole Layout Pattern for Pitch
-
-This field is used to describe the pattern of perforations in the collector surface. There are currently two choices available:   Square and Triangle. Note that the hole layout pattern should be consistent with how the value for pitch was determined.
-
-#### Field: Heat Exchange Effectiveness Correlation
-
-This field is used to select which correlation is used to model heat transfer from the collector surface to the incoming air when the collector is active. There are two choices available:   Kutscher1994, and VanDeckerHollandsBrunger2001. See the Engineering Reference for details and references.
-
-#### Field: Ratio of Actual Collector Surface Area to Projected Surface Area
-
-This field is used to enter a factor that accounts for the extra surface area resulting from corrugations in the collector surface. Corrugations help stiffen the collector. The projected surface area is obtained by the program from the (flat) underlying surfaces. If the collector is flat then this ratio is 1.0. If the collector is corrugated, then this ratio will be greater than one. A typical value might be 1.165.
-
-#### Field: Roughness of Collector
-
-This field is used to describe the relative roughness of the collector material. This field is similar to one in the Material object. This parameter only influences the convection coefficients, more specifically the outside convection coefficient. A special keyword is expected in this field with the options being    VeryRough   ,    Rough   ,    MediumRough   ,    MediumSmooth   ,    Smooth   , and    VerySmooth    in order of roughest to smoothest options.
-
-#### Field: Collector Thickness
-
-This field is used to enter the thickness of the collector material. This value is only needed for the Van Decker Hollands Brunger 2001 correlation. The material thickness should be entered in meters.
-
-#### Field: Effectiveness for Perforations with Respect to Wind
-
-This field is used to enter a value for the coefficient used to determine natural air exchanges from wind, or Cv. When the collector is inactive, wind will cause exterior air to move in and out of the collector. Cv is an arbitrary coefficient used to model the effectiveness of openings and depends on opening geometry and the orientation with respect to the wind. Cv should probably be in the range 0.25 to 0.65. Increasing Cv will increase the amount of natural ventilation.
-
-#### Field: Discharge Coefficient for Openings with Respect to Buoyancy Driven Flow
-
-This field is used to enter a value for the coefficient used to determine natural air exchanges from buoyancy, or Cd. When the collector is inactive, stack or buoyancy effects will cause exterior air to move in and out of the collector. Cd is an arbitrary discharge coefficient that depends on the geometry of the opening. Cd should probably be in the range 0.4 to 1.0. Increasing Cd will increase the amount of natural ventilation.
-
-#### Field: Surface &lt;\#&gt; Name
-
-The remaining fields are used to name the BuildingSurface:Detailed objects that are associated with the UTSC. These are the underlying heat transfer surfaces and are defined elsewhere in the input file. These other surfaces should all specify OtherSideConditionsModel as their exterior environment. The input object can currently accommodate up to ten surfaces, but it is extensible.
-
-An example of this object follows.
-
-```idf
-SolarCollector:UnglazedTranspired,
-       Shop OA UTSC ZN11,                               ! Name
-       UTSC OSCM ZN11,                                     ! Boundary Conditions Model Name
-       HeatingAvailSched ,                             ! Availability Schedule Name
-       Outside Air Inlet Node ZN11 ,         ! Inlet Node Name
-       UTSC Outlet Node ZN11 ,                     ! Outlet Node Name
-       Mixed Air Node ZN11 ,                         ! Setpoint Node Name
-       ZN11 Node,                                               ! Zone Node Name
-       ShopFreeHeatingSetpoints,                 ! Free Heating Setpoint Schedule Name
-       0.0016,                                                     ! Diameter of Perforations in Collector
-       0.01689,                                                   ! Distance Between Perforations in Collector
-       0.9,                                                           ! Thermal Emissivity of Collector Surface
-       0.9,                                                           ! Solar Absorbtivity of Collector Surface
-       4.0,                                                           ! Effective Overall Height of Collector
-       0.1,                                                           ! Effective Gap Thickness of Plenum Behind Collector
-       2.0,                                                           ! Effective Cross Section Area of Plenum Behind Collector
-       Triangle,                                                 ! Hole Layout Pattern for Pitch
-       Kutscher1994,                                         ! Heat Exchange Effectiveness Correlation
-       1.165,                                           ! Ratio of Actual Collector Surface Area to Projected Surface Area
-       MediumRough ,                                         ! Roughness of Collector
-       0.00086,                                                   ! Collector Thickness
-       0.25,                                                         ! Effectiveness for Perforations with Respect to Wind
-       0.5,                                 ! Discharge Coefficient for Openings with Respect to Buoyancy Driven Flow
-       ZN11_Shop_1:ExtWall:South;               ! Surface 1 Name
-```
-
-
-
-### Solar Collector Unglazed Transpired Outputs
-
-In addition to related output that can be obtained for air nodes and surfaces, these outputs are available for UTSC systems:
-
-* HVAC,Average,Solar Collector Heat Exchanger Effectiveness []
-
-* HVAC,Average,Solar Collector Leaving Air Temperature [C]
-
-* HVAC,Average,Solar Collector Outside Face Suction Velocity [m/s]
-
-* HVAC,Average,Solar Collector Surface Temperature [C]
-
-* HVAC,Average,Solar Collector Plenum Air Temperature [C]
-
-* HVAC,Average,Solar Collector Sensible Heating Rate [W]
-
-* Zone,Meter,SolarAir:Facility [J]
-
-* Zone,Meter,SolarAir:HVAC [J]
-
-* Zone,Meter,HeatProduced:SolarAir [J]
-
-* HVAC,Sum,Solar Collector Sensible Heating Energy [J]
-
-* HVAC,Average,Solar Collector Natural Ventilation Air Change Rate [ACH]
-
-* HVAC,Average,Solar Collector Natural Ventilation Mass Flow Rate [kg/s]
-
-* HVAC,Average,Solar Collector Wind Natural Ventilation Mass Flow Rate [kg/s]
-
-* HVAC,Average,Solar Collector Buoyancy Natural Ventilation Mass Flow Rate [kg/s]
-
-* HVAC,Average,Solar Collector Incident Solar Radiation [W/m2]
-
-* HVAC,Average,Solar Collector System Efficiency []
-
-* HVAC,Average,Solar Collector Surface Efficiency []
-
-
-
-#### Solar Collector Heat Exchanger Effectiveness []
-
-The results from UTSC correlations defined by <span>\({\varepsilon_{HX}} = \frac{{{T_{a,HX}} - {T_{amb}}}}{{{T_{s,coll}} - {T_{amb}}}}\)</span>.
-
-#### Solar Collector Leaving Air Temperature [C]
-
-The temperature of air entering the plenum after being heated by the collector.
-
-#### Solar Collector Outside Face Suction Velocity [m/s]
-
-The bulk velocity of air approaching the collector.
-
-#### Solar Collector Surface Temperature [C]
-
-The surface temperature of the collector itself.
-
-#### Solar Collector Plenum Air Temperature [C]
-
-The temperature of air inside, and leaving, the plenum behind the collector.
-
-#### Solar Collector Sensible Heating Rate [W]
-
-The overall rate at which heat is being added to the outdoor air stream.
-
-#### SolarAir:Facility [J]
-
-A meter that includes the heating energy provided by the UTSC.
-
-#### SolarAir:HVAC [J]
-
-A meter that includes the heating energy provided by the UTSC.
-
-#### HeatProduced:SolarAir [J]
-
-A meter that includes the heating energy provided by the UTSC.
-
-#### Solar Collector Sensible Heating Energy [J]
-
-The overall sum of energy added to the outdoor air stream.
-
-#### Solar Collector Natural Ventilation Air Change Rate [ACH]
-
-The rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive in Air Changes per Hour.
-
-#### Solar Collector Natural Ventilation Mass Flow Rate [kg/s]
-
-The mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive.
-
-#### Solar Collector Wind Natural Ventilation Mass Flow Rate [kg/s]
-
-The part of mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive due to wind-driven forces.
-
-#### Solar Collector Buoyancy Natural Ventilation Mass Flow Rate [kg/s]
-
-The part of mass flow rate of natural ventilation air exchange between the plenum and ambient when the collector is inactive due to buoyancy-driven forces.
-
-#### Solar Collector Incident Solar Radiation [W/m2]
-
-The intensity of solar radiation incident on the UTSC collector from all sources.
-
-#### Solar Collector System Efficiency []
-
-The overall efficiency of the UTSC system including collected solar energy and heat recovered from the underlying surface.
-
-#### Solar Collector Surface Efficiency []
-
-The efficiency of the UTSC solar collector.
-
-
-
-### SolarCollector:UnglazedTranspired:MultiSystem
-
-This object is used to model unglazed transpired solar collectors (UTSC) that are connected to multiple outdoor air systems. This object supplements the SolarCollector:UnglazedTranspired object and is only necessary if more than one air system is connected to a single transpired collector. After the name field, there are sets of four node names used to define the connections of each air system. Each set contains node names for inlet, outlet, control, and zone. If more than five air systems are needed, this object is extensible.
-
-#### Field: Solar Collector Name
-
-This field is used to identify the name of the SolarCollector:UnglazedTranspired object that needs to be connected to more than one air system. This field must match the name.
-
-#### Field Set: Inlet Node, Outlet Node, Mixed Air Node, Zone Node
-
-The following four fields form a repeating set of four fields.   One set is used for each outdoor air system that is connected to the collector.
-
-#### Field: Outdoor Air System &lt;\#&gt; Collector Inlet Node
-
-This field contains the name of an air node that provides air into the UTSC. This node name should also be assigned to be an outdoor air node using the OutdoorAir:NodeList and OutdoorAir:Node objects. This node is also be named as the actuator node in a Controller:OutdoorAir object.
-
-#### Field: Outdoor Air System &lt;\#&gt; Collector Outlet Node
-
-This field contains the name of an air node that is the outlet of the UTSC. This node name will typically be the Outdoor Air Stream Node Name in the OutdoorAir:Mixer (if there is no other equipment on the outdoor air path).
-
-#### Field: Outdoor Air System &lt;\#&gt; Mixed Air Node
-
-This field contains the name of an air node that has a setpoint manager controlling its temperature setpoint. This node name will typically be named as the mixed air node in a Controller:OutdoorAir object.
-
-#### Field: Outdoor Air System &lt;\#&gt; Zone Node
-
-This field contains the name of an air node for a thermal zone that is ultimately connected to the air system. This node is used with the setpoint schedule, defined in the following field, to provide an added layer of thermostatic control for the UTSC without affecting the control of auxiliary heating. If there is a single air system that is connected to more than one zone, then a single zone should be selected based on where the thermostat might be located.
-
-An example of this object follows.
-
-```idf
-   SolarCollector:UnglazedTranspired:Multisystem,
-       OFFICE MultiSystem OA UTSC ,   ! Solar Collector Name
-       Outside Air Inlet Node ZN1,     ! Outdoor Air System 1 Collector Inlet Node
-       UTSC Outlet Node ZN1,                 ! Outdoor Air System 1 Collector Outlet Node
-       Mixed Air Node ZN1,                     ! Outdoor Air System 1 Mixed Air Node
-       ZN1 Node,                                         ! Outdoor Air System 1 Zone Node
-       Outside Air Inlet Node ZN2,     ! Outdoor Air System 2 Collector Inlet Node
-       UTSC Outlet Node ZN2,                 ! Outdoor Air System 2 Collector Outlet Node
-       Mixed Air Node ZN2,                     ! Outdoor Air System 2 Mixed Air Node
-       ZN2 Node,                                         ! Outdoor Air System 2 Zone Node
-       Outside Air Inlet Node ZN3,     ! Outdoor Air System 3 Collector Inlet Node
-       UTSC Outlet Node ZN3,                 ! Outdoor Air System 3 Collector Outlet Node
-       Mixed Air Node ZN3,                     ! Outdoor Air System 3 Mixed Air Node
-       ZN3 Node,                                         ! Outdoor Air System 3 Zone Node
-       Outside Air Inlet Node ZN4,     ! Outdoor Air System 4 Collector Inlet Node
-       UTSC Outlet Node ZN4,                 ! Outdoor Air System 4 Collector Outlet Node
-       Mixed Air Node ZN4,                     ! Outdoor Air System 4 Mixed Air Node
-       ZN4 Node,                                         ! Outdoor Air System 4 Zone Node
-       Outside Air Inlet Node ZN5,     ! Outdoor Air System 5 Collector Inlet Node
-       UTSC Outlet Node ZN5,                 ! Outdoor Air System 5 Collector Outlet Node
-       Mixed Air Node ZN5,                     ! Outdoor Air System 5 Mixed Air Node
-       ZN5 Node;                                         ! Outdoor Air System 5 Zone Node
-```
-
-
-
-Group     Pumps
--------------
-
-EnergyPlus plant and condenser loops need pump components to drive liquid flow around the loop.   There are various types of pump models available.
-
-### Pump:VariableSpeed
-
-Pumps are needed in both plant and condenser loops. The syntax for a variable speed pump is given below.
-
-#### Field: Name
-
-This alpha field contains the identifying a unique name for the pump.
-
-#### Field: Inlet Node Name
-
-This alpha field contains the identifying name for the pump inlet node.
-
-#### Field: Outlet Node Name
-
-This alpha field contains the identifying name for the pump outlet node.
-
-#### Field: Design Maximum Flow Rate
-
-This numeric field contains the pump's design maximum volume flow rate in cubic meters per second. This field can be autosized.
-
-#### Field: Design Pump Head
-
-This numeric field contains the pump's rated head pressure in Pascals. The default is 179352 Pa, or 60 ftH20, and is for a fairly large building.
-
-#### Field: Design Power Consumption
-
-This numeric field contains the pump's design power consumption in Watts.   If the user is performing a pressure simulation on the loop in which this pump is found, this value would only be used to estimate pump efficiency.   During reported calculations, the pump would use the loop pressure drop and current flow conditions along with efficiency to calculate pump power dynamically. This field can be autosized.  When set to autosize the type of scaling factor is chosen in the input field Design Power Sizing Method.
-
-#### Field: Motor Efficiency
-
-This numeric field contains the pump's efficiency in decimal form (0 = 0%, 1 = 100%).
-
-#### Field: Fraction of Motor Inefficiencies to Fluid Stream
-
-This numeric field contains the pump's fraction of power loss to the fluid.
-
-#### Field: Coefficient 1 of the Part Load Performance Curve
-
-This numeric field contains the first coefficient in the part load ratio curve. The fraction of full load power is determined by the cubic equation:
-
-<div>\[FractionFullLoadPower = {C_1} + {C_2}PLR + {C_3}PL{R^2} + {C_4}PL{R^3}\]</div>
-
-where C<sub>1</sub>,C<sub>2</sub>,C<sub>3</sub>,and C<sub>4</sub> are Coefficients 1     4 (below) and PLR is the Part Load Ratio.
-
-#### Field: Coefficient 2 of the Part Load Performance Curve
-
-This numeric field contains the second coefficient in the part load ratio curve.
-
-#### Field: Coefficient 3 of the Part Load Performance Curve
-
-This numeric field contains the third coefficient in the part load ratio curve.
-
-#### Field: Coefficient 4 of the Part Load Performance Curve
-
-This numeric field contains the fourth coefficient in the part load ratio curve.
-
-#### Field: Design Minimum Flow Rate
-
-This field contains the minimum volume flow rate while operating in variable flow capacity rate in cubic meters per second.  This field is autosizable. When set to autosize the value in the input field Design Minimum Flow Rate Sizing Factor is used to scale the minimum flow rate as a fraction of the Design Maximum Flow Rate.
-
-#### Field: Pump Control Type
-
-This is a choice field of Continuous or Intermittent. A variable speed pump is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump is operating intermittently, then the pump can shutdown. For any other condition such as the loop having a load and the pump is operating intermittently or the pump is continuously operating (regardless of the loading condition), the pump will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump is running, it will try to meet the flow request made by demand side components. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this control by forcing the pump to be on or off.
-
-#### Field: Pump Flow Rate Schedule Name
-
-The schedule values modify the value for Rated Flow Rate of the pump on a time basis. This essentially sets the maximum value available for the pump at a given time, **not the actual flow rate at that time**.  The default is that the pump is ON and runs according to its other operational requirements specified above. This schedule is for special, not typical pump operations.  For additional control over pump flow, EMS actuators can be employed.
-
-#### Field: Pump Curve Name
-
-This references a pump curve to be used during pump flow-loop head resolution.   This is only applicable for loop simulations which include pressure components on at least a single branch.   More information regarding pressure system simulation is available in the engineering reference.
-
-#### Field: Impeller Diameter
-
-For pressure simulation cases, this is the impeller diameter used during calculations which is used in non-dimensionalizing the pump curve described in the previous field.   The units of this value are meters.
-
-#### Field: VFD Control Type
-
-This string defines which type of VFD control type to perform.   PressureSetPointControl is a realistic approach which requires inputs of pressure range schedules to control the pump rpm to maintain a certain pressure drop (head).   ManualControl is an idealized control strategy in which the pump RPM is maintained at a scheduled value throughout the simulation, abiding by other flow restrictions in the loop.
-
-#### Field: Pump RPM Schedule Name
-
-For VFD Control Type = ManualControl, this defines the pump RPM schedule to use during the simulation.   For VFD Control Type = PressureSetPointControl, this field is not interpreted.   The value of the schedule is RPM.
-
-#### Field: Minimum Pressure Schedule
-
-For VFD Control Type = PressureSetPointControl, this field defines the minimum pressure range setpoint value, or the lower bound of pressure drop (head) to use when determining the required pump speed.   For VFD Control Type = ManualControl, this field is not interpreted.   The value of the schedule is Pascals.
-
-#### Field: Maximum Pressure Schedule
-
-For VFD Control Type = PressureSetPointControl, this field defines the maximum pressure range setpoint value, or the upper bound of pressure drop (head) to use when determining the required pump speed.   For VFD Control Type = ManualControl, this field is not interpreted.   The value of the schedule is Pascals.
-
-#### Field: Minimum RPM Schedule
-
-For VFD Control Type = PressureSetPointControl, this field defines the minimum allowable RPM, or the lower bound of pump speed to use when determining the required pump speed.   For VFD Control Type = ManualControl, this field is not interpreted.   The value of the schedule is RPM.
-
-#### Field: Maximum RPM Schedule
-
-For VFD Control Type = PressureSetPointControl, this field defines the maximum allowable RPM, or the upper bound of pump speed to use when determining the required pump speed.   For VFD Control Type = ManualControl, this field is not interpreted.   The value of the schedule is RPM.
-
-#### Field: Zone Name
-
-This field is optional. It can be used to input the name of the Zone in which the pump is located in the model.   If the pump is outdoors, or skin losses are not to be modeled, then leave this field blank.   If a valid Zone name is entered, then the portion of electrical power consumed by the pump that is not added to the working fluid is added to the surrounding Zone.
-
-#### Field: Skin Loss Radiative Fraction
-
-This field is optional.  If a Zone is named in the previous field and pump losses are to be added to a surrounding thermal zone, then this input determines the split between thermal radiation and thermal convection for the heat losses from the pump.   If it is left blank then all the losses will be convective.  
-
-#### Field: Design Power Sizing Method
-
-This field is optional.   There are two choices PowerPerFlow and PowerPerFlowPerPressure.  If PowerPerFlow is used the pump's Design Power Consumption will be calculated using the sizing factor from the input field Design Electric Power per Unit Flow Rate -- with Design Power Consumption = Design Maximum Flow Rate * scaling factor.  If PowerPerFlowPerPressure is used the pump's Design Power Consumption will use the sizing factor from the input field Design Shaft Power per Unit Flow Rate Per Unit Head -- with Design Power Consumption = Design Maximum Flow Rate * Design Pump Head * scaling factor / Motor Efficiency. If omitted the default method of PowerPerFlowPerPressure will be used.
-
-#### Field: Design Electric Power per Unit Flow Rate
-
-This field is optional.   This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlow.  It allows setting the efficiency the pumping system's power consumption using only the design flow rate. If omitted the default value of 348701.1 W/(m<sup>3</sup>/s) ( 22 W/gpm) will be used.
-
-#### Field: Design Shaft Power per Unit Flow Rate Per Unit Head
-
-This field is optional.  This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlowPerPressure.  It allows setting the efficiency of the impeller and drive assembly when calculating the pump power consumption for the design flow rate, motor efficiency, and pump head. If omitted the default value of 1.282051 W/((m<sup>3</sup>/s)-Pa) will be used. 
-
-#### Field: Design Minimum Flow Rate Sizing Factor
-
-This field is optional.  If omitted the default value of 0.0 will be used. This input is used when the input field Design Minimum Flow Rate is set to autosize. The minimum flow rate will be set to the product of this sizing factor and the Design Maximum Flow Rate. 
-
-Examples of this object in the IDF follow.
-
-```idf
-   Pump:VariableSpeed,
-       HW Circ Pump,                          !- Name
-       HW Supply Inlet Node,                  !- Inlet Node Name
-       HW Pump Outlet Node,                   !- Outlet Node Name
-       autosize,                              !- Design Maximum Flow Rate {m3/s}
-       179352,                                !- Design Pump Head {Pa}
-       autosize,                              !- Design Power Consumption {W}
-       0.9,                                   !- Motor Efficiency
-       0.0,                                   !- Fraction of Motor Inefficiencies to Fluid Stream
-       0,                                     !- Coefficient 1 of the Part Load Performance Curve
-       1,                                     !- Coefficient 2 of the Part Load Performance Curve
-       0,                                     !- Coefficient 3 of the Part Load Performance Curve
-       0,                                     !- Coefficient 4 of the Part Load Performance Curve
-       0,                                     !- Minimum Flow Rate {m3/s}
-       Intermittent;                          !- Pump Control Type
-
-
-   Pump:VariableSpeed,
-       Circ Pump,                             !- Name
-       CW Supply Inlet Node,                  !- Inlet Node Name
-       CW Pump Outlet Node,                   !- Outlet Node Name
-       .0011,                                 !- Design Maximum Flow Rate {m3/s}
-       300000,                                !- Design Pump Head {Pa}
-       500,                                   !- Design Power Consumption {W}
-       .87,                                   !- Motor Efficiency
-       0.0,                                   !- Fraction of Motor Inefficiencies to Fluid Stream
-       0,                                     !- Coefficient 1 of the Part Load Performance Curve
-       1,                                     !- Coefficient 2 of the Part Load Performance Curve
-       0,                                     !- Coefficient 3 of the Part Load Performance Curve
-       0,                                     !- Coefficient 4 of the Part Load Performance Curve
-       0,                                     !- Minimum Flow Rate {m3/s}
-       Intermittent;                          !- Pump Control Type
-```
-
-
-### Variable Speed Pump Outputs
-
-* HVAC,Average,Pump Electric Power [W]
-
-* HVAC,Sum,Pump Electric Energy [J]
-
-* HVAC,Average,Pump Shaft Power [W]
-
-* HVAC,Average,Pump Fluid Heat Gain Rate [W]
-
-* HVAC,Sum,Pump Fluid Heat Gain Energy [J]
-
-* HVAC,Average,Pump Outlet Temperature [C]
-
-* HVAC,Average,Pump Mass Flow Rate [kg/s]
-
-* HVAC,Average,Pump Zone Total Heating Rate [W]
-
-* HVAC,Sum,Pump Zone Total Heating Energy [J]
-
-* HVAC,Average,Pump Zone Convective Heating Rate [W]
-
-* HVAC,Average,Pump Zone Radiative Heating Rate [W]
-
-#### Pump Electric Power [W]
-
-#### Pump Electric Energy [J]
-
-These outputs are the electric power input to the pump motor. Consumption is metered on Pumps:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Pump Shaft Power [W]
-
-This is the shaft power delivered from the motor to the pump.
-
-#### Pump Fluid Heat Gain Rate [W]
-
-#### Pump Fluid Heat Gain Energy [J]
-
-These outputs are the energy added to the fluid as heat. For the current algorithm, this is equal to Pump Shaft Power, because the loops are closed and all energy added to the fluid will ultimately become heat due to friction.
-
-#### Pump Outlet Temperature [C]
-
-#### Pump Mass Flow Rate [kg/s]
-
-These outputs are the water outlet temperature and mass flow rate.
-
-#### Pump Zone Total Heating Rate [W]
-
-#### Pump Zone Total Heating Energy [J]
-
-These outputs are the thermal losses from the pump to the surrounding Zone.   They are only available if a Zone was named in the pump   s input.   These indicate the amount of heat added to the zone from the pump   s inefficiencies. They are the total heat loss including both convection and radiation.
-
-#### Pump Zone Convective Heating Rate [W]
-
-This output is the thermal loss from the pump to the surrounding Zone in the form of convective gains directly to the zone air. It is only available if a Zone was named in the pump input.
-
-#### Pump Zone Radiative Heating Rate [W]
-
-This output is the thermal loss from the pump to the surrounding Zone in the form of thermal radiation gains directly to the inside face of the zone   s surfaces. It is only available if a Zone was named in the pump input.
-
-### Pump:ConstantSpeed
-
-Pumps may be found in both plant and condenser loops. The syntax for a constant speed pump is given below.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the pump.
-
-#### Field: Inlet Node Name
-
-This alpha field contains the identifying name for the pump inlet node.
-
-#### Field: Outlet Node Name
-
-This alpha field contains the identifying name for the pump outlet node.
-
-#### Field: Design Flow Rate
-
-This numeric field contains the pump's design volume flow rate in cubic meters per second. This field is autosizable.
-
-#### Field: Design Pump Head
-
-This numeric field contains the pump's design head pressure in Pascals. The default is 179352 Pa, or 60 ftH20, and is for a fairly large building.
-
-#### Field: Design Power Consumption
-
-This numeric field contains the pump's rated power consumption in Watts.  If the user is performing a pressure simulation on the loop in which this pump is found, this value would only be used to estimate pump efficiency.  During reported calculations, the pump would use the loop pressure drop and current flow conditions along with efficiency to calculate pump power dynamically.  This field can be autosized.  When set to autosize the type of scaling factor is chosen in the input field Design Power Sizing Method.
-
-#### Field: Motor Efficiency
-
-This numeric field contains the pump's efficiency in decimal form (0 = 0%, 1 = 100%).
-
-#### Field: Fraction of Motor Inefficiencies to Fluid Stream
-
-This numeric field contains the pump's fraction of power loss to the fluid.
-
-#### Field: Pump Control Type
-
-This is a choice field of Continuous or Intermittent. The operation of a constant speed pump is fairly straightforward. If the user designates a constant speed pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump is constant speed and operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this control by forcing the pump to be on or off.
-
-#### Field: Pump Flow Rate Schedule Name
-
-The schedule values modify the value for Rated Flow Rate of the pump on a time basis. This essentially sets the maximum value available for the pump at a given time, **not the actual flow rate at that time**.  The default is that the pump is ON and runs according to its other operational requirements specified above. This schedule is for special, not typical pump operations.  For additional control over pump flow, EMS actuators can be employed.
-
-#### Field:Pump Curve Name
-
-This field is only used if the user is performing a pressure-based simulation in the plant loop of the LoopFlowCorrection type (see PlantLoop section for how to enable this).
-
-This field references a separate pressure head curve that the user has input separately in the input file.   The pressure curve represents a non-dimensional regression of pressure-flow rate data.   The equation should be of the following form:
-
-<div>\[\psi  = {C_4} \times {\varphi ^4} + {C_3} \times {\varphi ^3} + {C_2} \times {\varphi ^2} + {C_1} \times \varphi  + {C_0}.\]</div>
-
-In this equation, the two dimensionless parameters, X and X are defined in terms of physical pump and flow parameters as:
-
-<div>\[\psi  = \frac{{\Delta P}}{{\rho {N^2}{D^2}}}\]</div>
-
-<div>\[\varphi  = \frac{{\dot m}}{{\rho N{D^3}}}\]</div>
-
-Where    Delta P    is the pressure drop, mdot is the fluid mass flow rate, rho is a representative fluid density, N is the rotational speed of the pump, and D is the pump impeller diameter.
-
-Since the user may not need a full fourth order expansion of this, the user may use linear (first order), quadratic (second order), cubic (third order), or full quartic (fourth order).   These are available in the objects Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic.
-
-Once this curve is input properly (along with the following two fields), the pump will respond to the plant loop pressure drop when resolving the flow rate.   Note that this simulation method will likely result in a plant loop that does not exactly hit the setpoint as the current simulation method does.   This is due to the loop flow rate now being    pressure-based    and not    decision-based   .
-
-#### Field:Impeller Diameter
-
-This field is only used if the user is performing a pressure-based simulation in the plant loop of the LoopFlowCorrection type (see PlantLoop section for how to enable this).
-
-To re-dimensionalize the dimensionless pump curve, the impeller diameter must be known.   This value is entered in meters.
-
-#### Field:Rotational Speed
-
-This field is only used if the user is performing a pressure-based simulation in the plant loop of the LoopFlowCorrection  type (see PlantLoop section for how to enable this).
-
-To re-dimensionalize  the dimensionless pump curve, the rotational speed must be known.   This value is entered in RPM (revolutions per minute).
-
-#### Field: Zone Name
-
-This field is optional. It can be used to input the name of the Zone in which the pump is located in the model.   If the pump is outdoors, or skin losses are not to be modeled, then leave this field blank.   If a valid Zone name is entered, then the portion of electrical power consumed by the pump that is not added to the working fluid is added to the surrounding Zone.
-
-#### Field: Skin Loss Radiative Fraction
-
-This field is optional.   If a Zone is named in the previous field and pump losses are to be added to a surrounding thermal zone, then this input determines the split between thermal radiation and thermal convection for the heat losses from the pump.   If it is left blank then all the losses will be convective.  
-
-#### Field: Design Power Sizing Method
-
-This field is optional.   There are two choices PowerPerFlow and PowerPerFlowPerPressure. If omitted the default method of PowerPerFlowPerPressure will be used.  
-
-If PowerPerFlow is used the pump's Design Power Consumption will be calculated using the sizing factor from the input field Design Electrical Power per Unit Flow Rate -- with Design Power Consumption = Design Maximum Flow Rate * scaling factor.
-
-If PowerPerFlowPerPressure is used the pump's Design Power Consumption will use the sizing factor from the input field Design Shaft Power per Unit Flow Rate Per Unit Head -- with Design Power Consumption = Design Maximum Flow Rate * Design Pump Head * scaling factor / Motor Efficiency. 
-
-#### Field: Design Electrical Power per Unit Flow Rate
-
-This field is optional.   This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlow.  It allows setting the efficiency the pumping system's power consumption using only the design flow rate. If omitted the default value of 348701.1 W/(m<sup>3</sup>/s) (22 W/gpm) will be used.  
-
-#### Field: Design Shaft Power per Unit Flow Rate Per Unit Head
-
-This field is optional.  This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlowPerPressure.  It allows controlling the efficiency of the impeller and drive assembly when calculating the pump power consumption for the design flow rate, motor efficiency, and pump head. If omitted the default value of 1.282051 W/((m<sup>3</sup>/s)-Pa) will be used. 
-
-
-An example of this object follows.
-
-```idf
-Pump:ConstantSpeed,
-             Circ Pump,                         !- Name
-             CW Supply Inlet Node,              !- Inlet Node Name
-             PumpChiller Node,                  !- Outlet Node Name
-             0.0011,                            !- Design Flow Rate
-             300000,                            !- Design Pump Head
-             700,                               !- Design Power Consumption
-             0.87,                              !- Motor Efficiency
-             0.0,                               !- Fraction of Motor Inefficiencies to Fluid Stream
-             Intermittent;                      !- Pump Control Type
-```
-
-
-
-### Constant Speed Pump Outputs
-
-* HVAC,Average,Pump Electric Power [W]
-
-* HVAC,Sum,Pump Electric Energy [J]
-
-* HVAC,Average,Pump Shaft Power [W]
-
-* HVAC,Average,Pump Fluid Heat Gain Rate [W]
-
-* HVAC,Sum,Pump Fluid Heat Gain Energy [J]
-
-* HVAC,Average,Pump Outlet Temperature [C]
-
-* HVAC,Average,Pump Mass Flow Rate [kg/s]
-
-* HVAC,Average,Pump Zone Total Heating Rate [W]
-
-* HVAC,Sum,Pump Zone Total Heating Energy [J]
-
-* HVAC,Average,Pump Zone Convective Heating Rate [W]
-
-* HVAC,Average,Pump Zone Radiative Heating Rate [W]
-
-
-
-#### Pump Electric Power [W]
-
-#### Pump Electric Energy [J]
-
-These outputs are the electric power input to the pump motor. Consumption is metered on Pumps:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Pump Shaft Power [W]
-
-This is the shaft power delivered from the motor to the pump.
-
-#### Pump Fluid Heat Gain Rate [W]
-
-#### Pump Fluid Heat Gain Energy [J]
-
-These outputs are the energy added to the fluid as heat. For the current algorithm, this is equal to Pump Shaft Power, because the loops are closed and all energy added to the fluid will ultimately become heat due to friction.
-
-#### Pump Outlet Temperature [C]
-
-#### Pump Mass Flow Rate [kg/s]
-
-These outputs are the water outlet temperature and mass flow rate.
-
-#### Pump Zone Convective Heating Rate [W]
-
-This output is the thermal loss from the pump to the surrounding Zone in the form of convective gains directly to the zone air. It is only available if a Zone was named in the pump input.
-
-#### Pump Zone Radiative Heating Rate [W]
-
-This output is the thermal loss from the pump to the surrounding Zone in the form of thermal radiation gains directly to the inside face of the zone   s surfaces. It is only available if a Zone was named in the pump input.
-
-#### Pump Zone Total Heating Energy [J]
-
-#### Pump Zone Total Heating Rate [W]
-
-These outputs are the thermal losses from the pump to the surrounding Zone.   They are only available if a Zone was named in the pump   s input.   These indicate the amount of heat added to the zone from the pump   s inefficiencies. They are the total heat loss including both convection and radiation.
-
-### Pump:VariableSpeed:Condensate
-
-The Pump:VariableSpeed:Condensate object can only be used in steam system simulation for the condensate side of the loop. This is a variable speed pump, which pumps the condensate back to the steam boiler. The syntax for condensate pump is given below.
-
-#### Field: Name
-
-This alpha field contains the identifying unique name for the pump.
-
-#### Field: Inlet Node Name
-
-This alpha field contains the identifying name for the pump inlet node.
-
-#### Field: Outlet Node Name
-
-This alpha field contains the identifying name for the pump outlet node.
-
-#### Field: Design Steam Volume Flow Rate
-
-This numeric field contains the pump's design volume flow rate in cubic meters per second. This field is autosizable. This is the volume flow rate of steam in expanded stated.  The volume of condensate is calculated by the software from the steam density and is much lower. 
-
-#### Field: Design Pump Head
-
-This numeric field contains the pump's design head in Pascals.  The default is 179352 Pa, or 60 ftH20, and is for a fairly large building.
-
-#### Field: Design Power Consumption
-
-This numeric field contains the pump's rated power consumption in Watts.  If the user is performing a pressure simulation on the loop in which this pump is found, this value would only be used to estimate pump efficiency.  During reported calculations, the pump would use the loop pressure drop and current flow conditions along with efficiency to calculate pump power dynamically. This field can be autosized.  When set to autosize the type of scaling factor is chosen in the input field Design Power Sizing Method.
-
-#### Field: Motor Efficiency
-
-This numeric field contains the pump's efficiency in decimal form (0 = 0%, 1 = 100%).
-
-#### Field: Fraction of Motor Inefficiencies to Fluid Stream
-
-This numeric field contains the pump's fraction of power loss to the fluid.
-
-#### Field: Coefficient 1 of the Part Load Performance Curve
-
-This numeric field contains the first coefficient in the part load ratio curve. The fraction of full load power is determined by the cubic equation:
-
-<div>\[FractionFullLoadPower = {C_1} + {C_2}PLR + {C_3}PL{R^2} + {C_4}PL{R^3}\]</div>
-
-where C<sub>1</sub>,C<sub>2</sub>,C<sub>3</sub>,and C<sub>4</sub> are Coefficients 1     4 (below) and PLR is the Part Load Ratio.
-
-#### Field: Coefficient 2 of the Part Load Performance Curve
-
-This numeric field contains the second coefficient in the part load ratio curve.
-
-#### Field: Coefficient 3 of the Part Load Performance Curve
-
-This numeric field contains the third coefficient in the part load ratio curve.
-
-#### Field: Coefficient 4 of the Part Load Performance Curve
-
-This numeric field contains the fourth coefficient in the part load ratio curve.
-
-#### Field: Pump Flow Rate Schedule Name
-
-The schedule values modify the value for Rated Flow Rate of the pump on a time basis. This essentially sets the maximum value available for the pump at a given time, **not the actual flow rate at that time**.  The default is that the pump is ON and runs according to its other operational requirements specified above. This schedule is for special, not typical pump operations.  For additional control over pump flow, EMS actuators can be employed.
-
-#### Field: Zone Name
-
-This field is optional. It can be used to input the name of the Zone in which the pump is located in the model.   If the pump is outdoors, or skin losses are not to be modeled, then leave this field blank.   If a valid Zone name is entered, then the portion of electrical power consumed by the pump that is not added to the working fluid is added to the surrounding Zone.
-
-#### Field: Skin Loss Radiative Fraction
-
-This field is optional.   If a Zone is named in the previous field and pump losses are to be added to a surrounding thermal zone, then this input determines the split between thermal radiation and thermal convection for the heat losses from the pump.   If it is left blank then all the losses will be convective.  
-
-#### Field: Design Power Sizing Method
-
-This field is optional.   There are two choices PowerPerFlow and PowerPerFlowPerPressure.  If PowerPerFlow is used the pump's Design Power Consumption will be calculated using the sizing factor from the input field Design Electric Power per Unit Flow Rate -- with Design Power Consumption = Design Maximum Flow Rate * scaling factor.  If PowerPerFlowPerPressure is used the pump's Design Power Consumption will use the sizing factor from the input field Design Shaft Power per Unit Flow Rate Per Unit Head -- with Design Power Consumption = Design Maximum Flow Rate * Design Pump Head * scaling factor / Motor Efficiency. If omitted the default method of PowerPerFlowPerPressure will be used.
-
-#### Field: Design Electric Power per Unit Flow Rate
-
-This field is optional.   This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlow.  It allows setting the efficiency the pumping system's power consumption using only the design flow rate. If omitted the default value of 348701.1 W/(m<sup>3</sup>/s) ( 22 W/gpm) will be used.
-
-#### Field: Design Shaft Power per Unit Flow Rate Per Unit Head
-
-This field is optional.  This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlowPerPressure.  It allows setting the efficiency of the impeller and drive assembly when calculating the pump power consumption for the design flow rate, motor efficiency, and pump head. If omitted the default value of 1.282051 W/((m<sup>3</sup>/s)-Pa) will be used. 
-
-
-
-Examples of this object in the IDF follow.
-
-```idf
-Pump:VariableSpeed:Condensate,
-       Steam Boiler Plant Steam Circ Pump,         !- Name
-       Steam Boiler Plant Steam Supply Inlet Node, !- Inlet Node Name
-       Steam Boiler Plant Steam Pump Outlet Node,  !- Outlet Node Name
-       0.36,                                  !- Design Steam Volume Flow Rate {m3/s}
-       179352,                                !- Design Pump Head {Pa}
-       400,                                   !- Design Power Consumption {W}
-       0.9,                                   !- Motor Efficiency
-       0.0,                                   !- Fraction of Motor Inefficiencies to Fluid Stream
-       0,                                     !- Coefficient 1 of the Part Load Performance Curve
-       1,                                     !- Coefficient 2 of the Part Load Performance Curve
-       0,                                     !- Coefficient 3 of the Part Load Performance Curve
-       0;                                     !- Coefficient 4 of the Part Load Performance Curve
-
-
-Pump:VariableSpeed:Condensate,
-       Steam Boiler Plant Steam Circ Pump,         !- Name
-       Steam Boiler Plant Steam Supply Inlet Node, !- Inlet Node Name
-       Steam Boiler Plant Steam Pump Outlet Node,  !- Outlet Node Name
-       0.36,                                  !- Design Steam Volume Flow Rate {m3/s}
-       179352,                                !- Design Pump Head {Pa}
-       autosize,                              !- Design Power Consumption {W}
-       0.9,                                   !- Motor Efficiency
-       0.0,                                   !- Fraction of Motor Inefficiencies to Fluid Stream
-       0,                                     !- Coefficient 1 of the Part Load Performance Curve
-       1,                                     !- Coefficient 2 of the Part Load Performance Curve
-       0,                                     !- Coefficient 3 of the Part Load Performance Curve
-       0;                                     !- Coefficient 4 of the Part Load Performance Curve
-```
-
-
-
-### Variable Speed Condensate Pump Outputs
-
-* HVAC,Average,Pump Electric Power [W]
-
-* HVAC,Sum,Pump Electric Energy [J]
-
-* HVAC,Average,Pump Shaft Power [W]
-
-* HVAC,Average,Pump Fluid Heat Gain Rate [W]
-
-* HVAC,Sum,Pump Fluid Heat Gain Energy [J]
-
-* HVAC,Average,Pump Outlet Temperature [C]
-
-* HVAC,Average,Pump Mass Flow Rate [kg/s]
-
-* HVAC,Average, Pump Zone Total Heating Rate [W]
-
-* HVAC, Sum, Pump Zone Total Heating Energy [J]
-
-* HVAC, Average, Pump Zone Convective Heating Rate [W]
-
-* HVAC, Average, Pump Zone Radiative Heating Rate [W]
-
-
-
-#### Pump Electric Power [W]
-
-#### Pump Electric Energy [J]
-
-These outputs are the electric power input to the pump motor. Consumption is metered on Pumps:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Pump Shaft Power [W]
-
-This is the shaft power delivered from the motor to the pump.
-
-#### Pump Fluid Heat Gain Rate [W]
-
-#### Pump Fluid Heat Gain Energy [J]
-
-These outputs are the energy added to the fluid as heat. For the current algorithm, this is equal to Pump Shaft Power, because the loops are closed and all energy added to the fluid will ultimately become heat due to friction.
-
-#### Pump Outlet Temperature [C]
-
-#### Pump Mass Flow Rate [kg/s]
-
-These outputs are the water outlet temperature and mass flow rate.
-
-#### Pump Zone Total Heating Rate [W]
-
-#### Pump Zone Total Heating Energy [J]
-
-These outputs are the thermal losses from the pump to the surrounding Zone.   They are only available if a Zone was named in the pump   s input.   These indicate the amount of heat added to the zone from the pump   s inefficiencies. They are the total heat loss including both convection and radiation.
-
-#### Pump Zone Convective Heating Rate [W]
-
-This output is the thermal loss from the pump to the surrounding Zone in the form of convective gains directly to the zone air. It is only available if a Zone was named in the pump input.
-
-#### Pump Zone Radiative Heating Rate [W]
-
-This output is the thermal loss from the pump to the surrounding Zone in the form of thermal radiation gains directly to the inside face of the zone   s surfaces. It is only available if a Zone was named in the pump input.
-
-
-
-### HeaderedPumps:ConstantSpeed
-
-Headered pumps are components with more than one identical pumps connected in parallel. The syntax for HeaderedPumps:ConstantSpeed is as follows.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the pump bank.
-
-#### Field: Inlet Node Name
-
-This alpha field contains the identifying name for the pump bank inlet node.
-
-#### Field: Outlet Node Name
-
-This alpha field contains the identifying name for the pump bank outlet node.
-
-#### Field: Total Design Flow Rate
-
-This numeric field contains the pump bank   s rated volumetric flow rate in cubic meters per second. This is equal to the product of number of pumps and the flow rate of each individual pump. The field can be autosized.
-
-#### Field: Number of Pumps in Bank
-
-The numeric field specifies the number of pumps present in the pump bank. All these pumps are connected in parallel internally.
-
-#### Field: Flow Sequencing Control Scheme
-
-The alpha field specifies the scheme for sequencing flow. Currently the only choice is Sequential, where a pump in the pump bank will be turned ON only after fully loading the previous pump.
-
-#### Field: Design Pump Head
-
-This numeric field contains the pump   s rated head pressure in Pascals.
-
-#### Field: Design Power Consumption
-
-This numeric field contains the pump bank   s total power consumption in Watts. This field is equal to the product of number of pumps and the rated power consumption of each individual pump.   If the user is performing a pressure simulation on the loop in which this pump bank is found, this value would only be used to estimate pump efficiency.   During reported calculations, the pump would use the loop pressure drop and current flow conditions along with efficiency to calculate pump power dynamically. This field can be autosized.  When set to autosize the type of scaling factor is chosen in the input field Design Power Sizing Method.
-
-#### Field: Motor Efficiency
-
-This numeric field contains the pump   s efficiency in decimal form (0 = 0%, 1 = 100%).
-
-#### Field: Fraction of Motor Inefficiencies to Fluid Stream
-
-This numeric field contains the pump   s fraction of power loss to the fluid.
-
-#### Field: Pump Control Type
-
-This is a choice field of Continuous or Intermittent. The operation of a constant speed pump bank is fairly straightforward. If the user designates a constant speed pump bank that is operating continuously, the pump bank will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump bank is constant speed and operates intermittently, the pump bank will run at its capacity if a load is sensed and will shut off if there is no load on the loop. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this control by forcing the pump to be on or off.
-
-#### Field: Pump Flow Rate Schedule Name
-
-The schedule values modify the value for Rated Flow Rate of the pump on a time basis. This essentially sets the maximum value available for the pump at a given time, **not the actual flow rate at that time**.  The default is that the pump is ON and runs according to its other operational requirements specified above. This schedule is for special, not typical pump operations.  For additional control over pump flow, EMS actuators can be employed.
-
-#### Field: Zone Name
-
-This field is optional. It can be used to input the name of the Zone in which the pump is located in the model.   If the pump is outdoors, or skin losses are not to be modeled, then leave this field blank.   If a valid Zone name is entered, then the portion of electrical power consumed by the pump that is not added to the working fluid is added to the surrounding Zone.
-
-#### Field: Skin Loss Radiative Fraction
-
-This field is optional.   If a Zone is named in the previous field and pump losses are to be added to a surrounding thermal zone, then this input determines the split between thermal radiation and thermal convection for the heat losses from the pump.   If it is left blank then all the losses will be convective.  
-
-#### Field: Design Power Sizing Method
-
-This field is optional.   There are two choices PowerPerFlow and PowerPerFlowPerPressure.  If PowerPerFlow is used the pump's Design Power Consumption will be calculated using the sizing factor from the input field Design Electric Power per Unit Flow Rate -- with Design Power Consumption = Design Maximum Flow Rate * scaling factor.  If PowerPerFlowPerPressure is used the pump's Design Power Consumption will use the sizing factor from the input field Design Shaft Power per Unit Flow Rate Per Unit Head -- with Design Power Consumption = Design Maximum Flow Rate * Design Pump Head * scaling factor / Motor Efficiency. If omitted the default method of PowerPerFlowPerPressure will be used.
-
-#### Field: Design Electric Power per Unit Flow Rate
-
-This field is optional.   This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlow.  It allows setting the efficiency the pumping system's power consumption using only the design flow rate. If omitted the default value of 348701.1 W/(m<sup>3</sup>/s) ( 22 W/gpm) will be used.
-
-#### Field: Design Shaft Power per Unit Flow Rate Per Unit Head
-
-This field is optional.  This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlowPerPressure.  It allows setting the efficiency of the impeller and drive assembly when calculating the pump power consumption for the design flow rate, motor efficiency, and pump head. If omitted the default value of 1.282051 W/((m<sup>3</sup>/s)-Pa) will be used. 
-
-
-
-An example for constant speed pump bank follows.
-
-```idf
-   HeaderedPumps:ConstantSpeed,
-       Chilled Water Headered Pumps,           !- Name
-       CW Supply Inlet Node,                   !- Inlet Node Name
-       CW Pumps Outlet Node,                   !- Outlet Node Name
-       autosize,                               !- Total Design Flow Rate
-       2,                                      !- Number of Pumps in Bank
-       SEQUENTIAL,                             !- Flow Sequencing Control Scheme
-       179352,                                 !- Design Pump Head
-       autosize,                               !- Design Power Consumption
-       0.9,                                    !- Motor Efficiency
-       0.0,                                    !- Fraction of Motor Inefficiencies to Fluid Stream
-       INTERMITTENT,                           !- Pump Control Type
-       CoolingPumpAvailSched;                  !- Pump Flow Rate Schedule Name
-```
-
-
-### Constant Speed Headered Pumps Outputs
-
-* HVAC,Average,Pump Electric Power [W]
-
-* HVAC,Sum, Pump Electric Energy [J]
-
-* HVAC,Average,Pump Shaft Power [W]
-
-* HVAC,Average, Pump Fluid Heat Gain Rate [W]
-
-* HVAC,Sum, Pump Fluid Heat Gain Energy [J]
-
-* HVAC,Average, Pump Outlet Temperature [C]
-
-* HVAC,Average,Pump Mass Flow Rate [kg/s]
-
-* HVAC,Average,Number of Pumps Operating []
-
-* HVAC, Average, Pump Zone Total Heating Rate [W]
-
-* HVAC, Sum, Pump Zone Total Heating Energy [J]
-
-* HVAC, Average, Pump Zone Convective Heating Rate [W]
-
-* HVAC, Average, Pump Zone Radiative Heating Rate [W]
-
-
-
-#### Pump Electric Power [W]
-
-#### Pump Electric Energy [J]
-
-These outputs are the electric power input to the pump motor. Consumption is metered on Pumps:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Pump Shaft Power [W]
-
-This is the shaft power delivered from the motor to the pump.
-
-#### Pump Fluid Heat Gain Rate [W]
-
-#### Pump Fluid Heat Gain Energy [J]
-
-These outputs are the energy added to the fluid as heat. For the current algorithm, this is equal to Pump Shaft Power, because the loops are closed and all energy added to the fluid will ultimately become heat due to friction.
-
-#### Pump Outlet Temperature [C]
-
-#### Pump Mass Flow Rate [kg/s]
-
-These outputs are the water outlet temperature and mass flow rate.
-
-#### Pump Operating Pumps Count []
-
-This output tells the number of pumps in the pump bank operating at any reporting frequency.
-
-#### Pump Zone Total Heating Rate [W]
-
-#### Pump Zone Total Heating Energy [J]
-
-These outputs are the thermal losses from the pump to the surrounding Zone.   They are only available if a Zone was named in the pump   s input.   These indicate the amount of heat added to the zone from the pump   s inefficiencies. They are the total heat loss including both convection and radiation.
-
-#### Pump Zone Convective Heating Rate [W]
-
-This output is the thermal loss from the pump to the surrounding Zone in the form of convective gains directly to the zone air. It is only available if a Zone was named in the pump input.
-
-#### Pump Zone Radiative Heating Rate [W]
-
-This output is the thermal loss from the pump to the surrounding Zone in the form of thermal radiation gains directly to the inside face of the zone   s surfaces. It is only available if a Zone was named in the pump input.
-
-
-
-### HeaderedPumps:VariableSpeed
-
-Headered pumps are components with more than one identical pumps connected in parallel. Currently this object may be found only in plant loops. The syntax for a HeaderedPumps:VariableSpeed pump is given below.
-
-#### Field: Name
-
-This alpha field contains the identifying unique name for the pump bank.
-
-#### Field: Inlet Node Name
-
-This alpha field contains the identifying name for the pump bank inlet node.
-
-#### Field: Outlet Node Name
-
-This alpha field contains the identifying name for the pump bank outlet node.
-
-#### Field: Total Design Flow Rate
-
-This numeric field contains the pump bank's rated volume flow rate in cubic meters per second. This is equal to the product of number of pumps and the flow rate of each individual pump. The field can be autosized.
-
-#### Field: Number of Pumps in Bank
-
-The numeric field specifies the number of pumps present in the pump bank. All these pumps are connected in parallel internally.
-
-#### Field: Flow Sequencing Control Scheme
-
-The alpha field specifies the scheme for sequencing flow. Currently the only choice is Sequential, where a pump in the pump bank will be turned ON only after fully loading the previous pump.
-
-#### Field: Design Pump Head
-
-This numeric field contains the pump   s rated head in Pascals.
-
-#### Field: Design Power Consumption
-
-This numeric field contains the pump bank's total power consumption in Watts. This field is equal to the product of number of pumps and the design power consumption of each individual pump.   If the user is performing a pressure simulation on the loop in which this pump bank is found, this value would only be used to estimate pump efficiency.   During reported calculations, the pump would use the loop pressure drop and current flow conditions along with efficiency to calculate pump power dynamically.  This field can be autosized.  When set to autosize the type of scaling factor is chosen in the input field Design Power Sizing Method.
-
-#### Field: Motor Efficiency
-
-This numeric field contains the efficiency of the individual pump (which will be equivalent to pump bank efficiency) in decimal form (0 = 0%, 1 = 100%).
-
-#### Field: Fraction of Motor Inefficiencies to Fluid Stream
-
-This numeric field contains the individual pump   s fraction of power loss to the fluid.
-
-#### Field: Coefficient 1 of the Part Load Performance Curve
-
-This numeric field contains the first coefficient (*C<sub>1</sub>*) in the part load ratio curve. The fraction of full load power is determined by the cubic equation:
-
-<div>\[FractionFullLoadPower = {C_1} + {C_2}PLR + {C_3}PL{R^2} + {C_4}PL{R^3}\]</div>
-
-where C<sub>1</sub>,C<sub>2</sub>,C<sub>3</sub>,and C<sub>4</sub> are Coefficients 1     4 (below) and PLR is the Part Load Ratio.
-
-#### Field: Coefficient 2 of the Part Load Performance Curve
-
-This numeric field contains the second coefficient (*C<sub>2</sub>*) in the part load ratio curve.
-
-#### Field: Coefficient 3 of the Part Load Performance Curve
-
-This numeric field contains the third coefficient (*C<sub>3</sub>*) in the part load ratio curve.
-
-#### Field: Coefficient 4 of the Part Load Performance Curve
-
-This numeric field contains the fourth coefficient (*C<sub>4</sub>*) in the part load ratio curve.
-
-#### Field: Minimum Flow Rate Fraction
-
-The numeric field specifies the minimum flow allowed for the pump bank as a fraction of the nominal flow. If the requested flow is less than minimum flow pump bank runs at minimum flow.
-
-#### Field: Pump Control Type
-
-This is a choice field of Continuous or Intermittent. A variable speed pump bank is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump bank is operating intermittently, then the bank can shutdown. For any other condition such as the loop having a load and the pump bank is operating intermittently or the pump bank is continuously operating (regardless of the loading condition), the bank will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump bank is running, it will try to meet the flow request made by demand side components. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this control by forcing the pump to be on or off.
-
-#### Field: Pump Flow Rate Schedule Name
-
-The schedule values modify the value for Rated Flow Rate of the pump on a time basis. This essentially sets the maximum value available for the pump at a given time, **not the actual flow rate at that time**.  The default is that the pump is ON and runs according to its other operational requirements specified above. This schedule is for special, not typical pump operations.  For additional control over pump flow, EMS actuators can be employed.
-
-#### Field: Zone Name
-
-This field is optional. It can be used to input the name of the Zone in which the pump is located in the model.   If the pump is outdoors, or skin losses are not to be modeled, then leave this field blank.   If a valid Zone name is entered, then the portion of electrical power consumed by the pump that is not added to the working fluid is added to the surrounding Zone.
-
-#### Field: Skin Loss Radiative Fraction
-
-This field is optional.   If a Zone is named in the previous field and pump losses are to be added to a surrounding thermal zone, then this input determines the split between thermal radiation and thermal convection for the heat losses from the pump.   If it is left blank then all the losses will be convective.  
-
-#### Field: Design Power Sizing Method
-
-This field is optional.   There are two choices PowerPerFlow and PowerPerFlowPerPressure.  If PowerPerFlow is used the pump's Design Power Consumption will be calculated using the sizing factor from the input field Design Electric Power per Unit Flow Rate -- with Design Power Consumption = Design Maximum Flow Rate * scaling factor.  If PowerPerFlowPerPressure is used the pump's Design Power Consumption will use the sizing factor from the input field Design Shaft Power per Unit Flow Rate Per Unit Head -- with Design Power Consumption = Design Maximum Flow Rate * Design Pump Head * scaling factor / Motor Efficiency. If omitted the default method of PowerPerFlowPerPressure will be used.
-
-#### Field: Design Electric Power per Unit Flow Rate
-
-This field is optional.   This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlow.  It allows setting the efficiency the pumping system's power consumption using only the design flow rate. If omitted the default value of 348701.1 W/(m<sup>3</sup>/s) ( 22 W/gpm) will be used.
-
-#### Field: Design Shaft Power per Unit Flow Rate Per Unit Head
-
-This field is optional.  This input is used when the input field Design Power Consumption is set to autosize and the Design Power Sizing Method is set to PowerPerFlowPerPressure.  It allows setting the efficiency of the impeller and drive assembly when calculating the pump power consumption for the design flow rate, motor efficiency, and pump head. If omitted the default value of 1.282051 W/((m<sup>3</sup>/s)-Pa) will be used. 
-
-
-
-
-An example of this object follows.
-
-```idf
-   HeaderedPumps:VariableSpeed,
-       Chilled Water Headered Pumps, !- Name
-       CW Supply Inlet Node,       !- Inlet Node Name
-       CW Pumps Outlet Node,       !- Outlet Node Name
-       autosize,                   !- Total Design Flow Rate {m3/s}
-       2,                          !- Number of Pumps in Bank
-       SEQUENTIAL,                 !- Flow Sequencing Control Scheme
-       179352,                     !- Design Pump Head {Pa}
-       autosize,                   !- Design Power Consumption {W}
-       0.9,                        !- Motor Efficiency
-       0.0,                        !- Fraction of Motor Inefficiencies to Fluid Stream
-       0,                          !- Coefficient 1 of the Part Load Performance Curve
-       1,                          !- Coefficient 2 of the Part Load Performance Curve
-       0,                          !- Coefficient 3 of the Part Load Performance Curve
-       0,                          !- Coefficient 4 of the Part Load Performance Curve
-       0.1,                        !- Minimum Flow Rate {m3/s}
-       INTERMITTENT,               !- Pump Control Type
-       CoolingPumpAvailSched;      !- Pump Flow Rate Schedule Name
-```
-
-
-### Variable Speed Headered Pumps Outputs
-
-* HVAC,Average,Pump Electric Power [W]
-
-* HVAC,Sum, Pump Electric Energy [J]
-
-* HVAC,Average,Pump Shaft Power [W]
-
-* HVAC,Average, Pump Fluid Heat Gain Rate [W]
-
-* HVAC,Sum, Pump Fluid Heat Gain Energy [J]
-
-* HVAC,Average, Pump Outlet Temperature [C]
-
-* HVAC,Average,Pump Mass Flow Rate [kg/s]
-
-* HVAC,Average,Number of pumps operating []
-
-* HVAC, Average, Pump Zone Total Heating Rate [W]
-
-* HVAC, Sum, Pump Zone Total Heating Energy [J]
-
-* HVAC, Average, Pump Zone Convective Heating Rate [W]
-
-* HVAC, Average, Pump Zone Radiative Heating Rate [W]
-
-
-
-#### Pump Electric Power [W]
-
-#### Pump Electric Energy [J]
-
-These outputs are the electric power input to the pump motor. Consumption is metered on Pumps:Electricity, Electricity:Plant, and Electricity:Facility.
-
-#### Pump Shaft Power [W]
-
-This is the shaft power delivered from the motor to the pump.
-
-#### Pump Fluid Heat Gain Rate [W]
-
-#### Pump Fluid Heat Gain Energy [J]
-
-These outputs are the energy added to the fluid as heat. For the current algorithm, this is equal to Pump Shaft Power, because the loops are closed and all energy added to the fluid will ultimately become heat due to friction.
-
-#### Pump Outlet Temperature [C]
-
-#### Pump Mass Flow Rate [kg/s]
-
-These outputs are the water outlet temperature and mass flow rate.
-
-#### Pump Operating Pumps Count []
-
-This output tells the number of pumps in the pump bank operating at any reporting frequency.
-
-#### Pump Zone Total Heating Rate [W]
-
-#### Pump Zone Total Heating Energy [J]
-
-These outputs are the thermal losses from the pump to the surrounding Zone.   They are only available if a Zone was named in the pump   s input.   These indicate the amount of heat added to the zone from the pump   s inefficiencies. They are the total heat loss including both convection and radiation.
-
-#### Pump Zone Convective Heating Rate [W]
-
-This output is the thermal loss from the pump to the surrounding Zone in the form of convective gains directly to the zone air. It is only available if a Zone was named in the pump input.
-
-#### Pump Zone Radiative Heating Rate [W]
-
-This output is the thermal loss from the pump to the surrounding Zone in the form of thermal radiation gains directly to the inside face of the zone   s surfaces. It is only available if a Zone was named in the pump input.
-
-
-
-
-
-Group     Heating and Cooling Coils
----------------------------------
-
-Several different coils may be added to zone equipment and air loops. This includes simple heating (gas, electric, and hot water) and a simple water-cooling coil as well as a more detailed flat fin water-cooling coil model. In general, the heating coil description can be used for a heating coil, a reheat coil, or a preheat coil in the air loop simulation or for zone equipment. Figure 135 is an example of a heating and cooling coil in the air loop simulation in a dual duct system. This does show the basic node structure that will be referenced in the input description. The figure does show water coils since they are the most complex to input in the simulation compared to the Electric and Gas coils which only have air connections.
-
-![Figure103\_ExampleAirLoopHeatingandCoolingCoil](media/image349.png)
-
-Figure 135. Example Air Loop Heating & Cooling Coil
-
-### Coil:Cooling:Water
-
-The water cooling coil (Coil:Cooling:Water) has the ability to give detailed output with simplified inputs, inputting complicated coil geometry is not required by the user for this model instead the coil is sized in terms of auto-sizeable thermodynamic inputs. The coil requires thermodynamic inputs such as temperatures, mass flow rates and humidity ratios.
-
-The coil is sized using auto-sized/user design input conditions and the UA values are calculated from the design conditions. A rough estimate of the coil area is provided along with percentage of surface wet and/or dry. This model uses the NTU-effectiveness approach to model heat transfer and has two types of flow arrangements cross-flow or counter-flow.
-
-The basic underlying idea is - use auto sizable thermodynamic design inputs, calculate the coil UA   s, use these UA values and operating conditions from the nodes connections, calculate the outlet stream conditions, and calculate the heat transfer rates.
-
-See section    Cooling Coil Model    in the EnergyPlus Engineering Document for further details regarding this model.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a cooling coil. Any reference to this cooling coil by another object will use this name.
-
-#### Field:Availability Schedule Name
-
-Schedule that defines when the coil is available. The name of the schedule (ref: Schedule) that denotes whether the cooling coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during a given time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit is off. If this field is blank, the schedule has a value of 1 for all time periods.
-
-#### Field: Design Water Flow Rate
-
-The maximum possible water volume flow rate (m<sup>3</sup>/sec) through the coil. This is an auto sizable design input.
-
-#### Field: Design Air Flow Rate
-
-The maximum possible air volume flow rate (m<sup>3</sup>/sec) through the coil. This is an auto sizable design input.
-
-#### Field: Design Inlet Water Temperature
-
-The inlet water temperature for the design flow (C). This is an auto sizable design input.
-
-#### Field: Design Inlet Air Temperature
-
-The inlet air temperature for the design flow (C). This is an auto sizable design input.
-
-#### Field: Design Outlet Air Temperature
-
-The outlet air condition desired for design flow (C). This is an auto sizable design input.
-
-#### Field: Design Inlet Air Humidity Ratio
-
-The highest value of humidity ratio possible for the Design inlet air stream (kgWater/kgDryAir). This is an auto sizable input.
-
-#### Field: Design Outlet Air Humidity Ratio
-
-The value of humidity ratio for the Design outlet air stream (kgWater/kgDryAir), it is an auto sizable input.
-
-#### Field: Water Inlet Node Name
-
-The name of the water coil inlet from the chilled water loop, i.e. Cooling Coil Water Inlet Node. It is from this node the operating inputs for water are transferred to the coil.
-
-#### Field: Water Outlet Node Name
-
-The name of the water coil outlet from the chilled water loop, i.e. Cooling Coil Water Outlet Node. It is from this node the operating output for water are reported to the coil.
-
-#### Field: Air Inlet Node Name
-
-The name of the air inlet to the water coil, i.e. Cooling Coil Air Inlet Node. It is from this node the operating inputs for air are transferred to the coil.
-
-#### Field: Air Outlet Node Name
-
-The name of the air outlet from the water coil, i.e. Cooling Coil Air Outlet Node. It is from this node the operating output for airside is reported to the coil.
-
-#### Field: Type of Analysis
-
-The coil has two modes of operation, termed as **SimpleAnalysis** and **DetailedAnalysis**. The difference between the two modes being, the simple mode reports the value of surface area fraction wet of the coil as dry or wet. The detailed mode give the exact value, however the execution time in detailed mode is noticeably higher.
-
-#### Field: Heat Exchanger Configuration
-
-The coil is operable in two modes, Cross Flow for general A/C applications and Counter flow mode. Air-conditioning systems generally use cross flow heat exchangers, hence the default is set to cross flow.
-
-#### Field: Condensate Collection Water Storage Tank Name
-
-This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
-
-Examples when auto sized in an IDF are as below:
-
-```idf
-Coil:Cooling:Water,
-       Main Cooling Coil 1,       !- Coil Name
-       CoolingCoilAvailSched,   !-Availability Schedule Name
-       autosize,         !- Design Water Volume Flow Rate of Coil {m3/s}
-       autosize,         !- Design Air Flow Rate of Coil {m3/s}
-       autosize,         !- Design Inlet Water Temperature {C}
-       autosize,         !- Design Inlet Air Temperature {C}
-       autosize,         !- Design Outlet Air Temperature {C}
-       autosize,         !- Design Inlet Air Humidity Ratio(kgWater/kgDryAir)
-       autosize,         !- Design Outlet Air Humidity Ratio(kgWater/kgDryAir)
-       Main Cooling Coil 1 Water Inlet Node,     !- Coil_Water_Inlet_Node
-       Main Cooling Coil 1 Water Outlet Node,   !- Coil_Water_Outlet_Node
-       Mixed Air Node 1,                                             !- Coil_Air_Inlet_Node
-       Main Cooling Coil 1 Outlet Node;               !- Coil_Air_Outlet_Node
-```
-
-Examples when values (hard-sized) are input in an IDF are as below:
-
-
-
-```idf
-Coil:Cooling:Water,
-       Main Cooling Coil 1,       !- Coil Name
-       CoolingCoilAvailSched,   !-Availability Schedule Name
-       0.0022,       !- Design Water Volume Flow Rate of Coil {m3/s}
-       1.45,           !- Design Air Flow Rate of Coil {m3/s}
-       6.1,             !- Design Inlet Water Temperature {C}
-       25,               !- Design Inlet Air Temperature {C}
-       10,               !- Design Outlet Air Temperature {C}
-       0.012,         !- Design Inlet Air Humidity Ratio
-       0.008,         !- Design Outlet Air Humidity Ratio
-       Main Cooling Coil 1 Water Inlet Node,     !- Coil_Water_Inlet_Node
-       Main Cooling Coil 1 Water Outlet Node,   !- Coil_Water_Outlet_Node
-       Mixed Air Node 1,                                             !- Coil_Air_Inlet_Node
-       Main Cooling Coil 1 Outlet Node;               !- Coil_Air_Outlet_Node
-```
-
-
-### Cooling Coil (Water) Outputs
-
-Following are the list of possible output output variables from this coil model:
-
-* HVAC,Sum,Cooling Coil Total Cooling Energy [J]
-
-* HVAC,Sum,Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Total Cooling Rate [W]
-
-* HVAC,Average,Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC,Average,Cooling Coil Wetted Area Fraction []
-
-* HVAC,Average,Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Coil Source Side Heat Transfer Energy [J]
-
-* HVAC,Sum,Cooling Coil Condensate Volume [m3]
-
-#### Cooling Coil Total Cooling Energy (J)
-
-Cooling Coil Total Cooling Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
-
-#### Cooling Coil Sensible Cooling Energy (J)
-
-Cooling Coil Sensible Cooling Energy is the total amount of Sensible heat transfer taking place in the coil at the operating conditions. It only takes into account temperature difference in the inlet and outlet air streams at operating conditions.
-
-#### Cooling Coil Total Cooling Rate (W)
-
-Cooling Coil Total Cooling Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
-
-#### Cooling Coil Sensible Cooling Rate (W)
-
-Cooling Coil Sensible Cooling Rate is the Rate of Sensible heat transfer taking place in the coil at the operating conditions.
-
-#### Cooling Coil Wetted Area Fraction []
-
-It defines the fraction of total surface area of coil which is wet due to moisture condensation on the surface of the coil. Value varies between 0.0 and 1.0.
-
-In addition, if a Water Storage Tank is used to collect coil condensate, then the following outputs will be available.
-
-#### Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-#### Cooling Coil Condensate Volume [m3]
-
-These reports provide the rate and amount of condensate from the coil. Condensate is water condensed out of the air as a result of cooling. The condensate volume is also reported on the meter for    OnSiteWater.   
-
-#### Cooling Coil Source Side Heat Transfer Energy [J]
-
-This is the energy extracted from the chilled water serving the coil, in Joules.
-
-### Coil:Heating:Water
-
-This simple heating coil model only does sensible heating of the air.   The simple heating coil uses the Effectiveness-NTU algorithm and assumes a cross-flow heat exchanger.
-
-#### Field: Name
-
-A unique identifying name for each coil.
-
-#### Field:Availability Schedule Name
-
-Schedule that defines when the coil is available. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during a given time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit is off. If this field is blank, the schedule has a value of 1 for all time periods.
-
-#### Field: U-Factor Times Area Value
-
-The UA value for the coil needed for the Effectiveness-NTU heat exchanger model.   An estimate of the UA can be obtained from:
-
-<div>\[q = UA \times ({T_{water,avg}} - {T_{air,avg}})\]</div>
-
-where q is the heat transferred from water to the air in watts; T<sub>water,\\ avg</sub> is the average water temperature in degrees C; and T<sub>air,\\ avg</sub> is the average air temperature in degrees C. Or the LMTD temperature difference can be used. This field is used when *Performance Input Method* = *UFactorTimesAreaAndDesignWaterFlowRate*.This field is autosizable.
-
-#### Field: Maximum Water Flow Rate
-
-The maximum possible water flow rate (m<sup>3</sup>/sec) through the coil. This field is used when *Coil Performance Input Method* = *UFactorTimesAreaAndDesignWaterFlowRate*. This field is autosizable.
-
-#### Field: Water Inlet Node Name
-
-The name of the coil   s water inlet node from the hot water loop.
-
-#### Field: Water Outlet Node Name
-
-The name of the coil   s water outlet node from the hot water loop.
-
-#### Field: Air Inlet Node Name
-
-The name of the air inlet node to the water coil.
-
-#### Field: Air Outlet Node Name
-
-The name of the air outlet node from the water coil.
-
-#### Field: Performance Input Method
-
-The user can choose either *UFactorTimesAreaAndDesignWaterFlowRate* or *NominalCapacity*. If *UFactorTimesAreaAndDesignWaterFlowRate* is selected, the user must input values for UA of the Coil and Max Water FlowRate of the Coil (and Rated Capacity is ignored). If *NominalCapacity* is chosen, the user must input a Rated Capacity for the coil; UA of the Coil and Max Water FlowRate of the Coil will be ignored. Rated capacity is defined as the heating capacity in watts of the coil at the rating points (i.e., the rated inlet and outlet water/air temperatures defined in the input fields below). The rated capacity is used to calculate a water mass flow rate and a UA for the coil. The default is *NominalCapacity*.
-
-To autosize the capacity, choose *UfactorTimesAreaAndDesignWaterFlowRate* and put autosize as the inputs for *U-Factor Times Area Value, Maximum Water Flow Rate,* and *Rated Capacity*. The program will use the Sizing inputs to size the coil. The rated temperatures (see below) are ignored in autosizing. These are used only when the user is specifying coil performance using the *NominalCapacity* input method.
-
-#### Field: Gross Rated Heating Capacity
-
-The heating capacity of the coil in watts at the rated inlet and outlet air and water temperatures.   The gross rated heating capacity does not account for the effect of supply air fan heat. This field is used when the *Performance Input Method* = *Nominal Capacity*. This field is autosizable. The rating points are given in the four subsequent input fields.
-
-#### Field: Rated Inlet Water Temperature
-
-The inlet water temperature (degrees C) corresponding to the rated heating capacity. The default is 82.2 degrees C (180 degrees F).
-
-#### Field: Rated Inlet Air Temperature
-
-The inlet air temperature (degrees C) corresponding to the rated heating capacity. The default is 16.6 degrees C (60 degrees F).
-
-#### Field: Rated Outlet Water Temperature
-
-The outlet water temperature (degrees C) corresponding to the rated heating capacity. The default is 71.1 degrees C (160 degrees F).
-
-#### Field: Rated Outlet Air Temperature
-
-The outlet air temperature (degrees C) corresponding to the nominal heating capacity. The default is 32.2 degrees C (90 degrees F).
-
-#### Field: Rated Ratio for Air and Water Convection
-
-This is the ratio of convective heat transfers between air side and water side of the heating coil at the rated operating conditions.   The default is .5.   This ratio describes the geometry and the design of the coil and is defined by:
-
-<div>\[ratio = \frac{{{\eta_f}{{\left( {hA} \right)}_{air}}}}{{{{\left( {hA} \right)}_{water}}}}\]</div>
-
-where,
-
-<span>\({\eta_f}\)</span>  is the fin efficiency, (dimensionless)
-
-*h* is the surface convection heat transfer coefficient
-
-*A* is the surface area
-
-An example input of the object is:
-
-```idf
-Coil:Heating:Water,
-       SPACE3-1 Zone Coil,           !- Coil Name
-       ReheatCoilAvailSched,       !- Availability Schedule Name
-       ,                                               !- UA of the Coil {W/K}
-       ,                                               !- Max Water Flow Rate of Coil {m3/s}
-       SPACE3-1 Zone Coil Water In Node,   !- Coil_Water_Inlet_Node
-       SPACE3-1 Zone Coil Water Out Node,   !- Coil_Water_Outlet_Node
-       SPACE3-1 Zone Coil Air In Node,   !- Coil_Air_Inlet_Node
-       SPACE3-1 In Node,               !- Coil_Air_Outlet_Node
-       NominalCapacity,                 !- Coil Performance Input Method
-       10000.,                                   !- Gross Rated Heating Capacity
-       0.55;                                       !- Rated Ratio for Air and Water Convection
-```
-
-
-
-### Heating Coil (Water) Outputs
-
-* HVAC,Sum, Heating Coil Heating Energy [J]
-
-* HVAC,Sum,Heating Coil Source Side Heat Transfer Energy [J]
-
-* HVAC,Average,Heating Coil Heating Rate [W]
-
-* HVAC,Average, Heating Coil U Factor Times Area Value [W/K]
-
-#### Heating Coil Heating Energy [J]
-
-Heating Coil Heating Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
-
-#### Heating Coil Heating Rate [W]
-
-Heating Coil Heating Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
-
-#### Heating Coil U Factor Times Area Value [W/K]
-
-This characterizes the overall heat transfer    UA    value, or U-factor times Area.   The simple heating coil model adjusts UA value based on inlet temperatures and flow rates and this output contains the results from that adjustment.
-
-#### Heating Coil Source Side Heat Transfer Energy [J]
-
-This is the same has the Heating Coil Heating Energy but it is also metered as a plant loop heating demand. This represents the heat in Joules extracted from the hot water serving the coil.
-
-### Coil:Heating:Steam
-
-The simple steam to air heating coil model only does sensible heating of the air. The steam to air coils condenses the steam and sub cools steam at loop pressure and discharges the condensate through steam traps at low pressure condensate line.
-
-#### Field: Name
-
-A unique identifying name for each steam coil.
-
-#### Field:Availability Schedule Name
-
-Schedule that defines when the coil is available. If the schedule   s value is less than or equal to   0.0, then the coil is not available and flow will not be requested. If the schedule   s value is &gt; 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Maximum Steam Flow Rate
-
-The maximum possible steam volumetric flow rate in m<sup>3</sup>/s through the steam heating coil. The steam volumetric flow rate is calculated at 100C and 101325 Pa. This field is autosizable.
-
-#### Field: Degree of SubCooling
-
-Ideally the steam trap located at the outlet of steam coil should remove all the condensate immediately, however there is a delay in this process in actual systems which causes the condensate to SubCool by certain degree in the coil before leaving the coil, this SubCool occurs in the steam coil and this SubCool-heat is added to the zone. The minimum value is 2 &deg; Celsius and default is 5 &deg; Celsius.
-
-#### Field: Degree of Loop SubCooling
-
-This essentially represents the heat loss to the atmosphere due to uninsulated condensate return piping to the boiler. Condensate return piping operates at atmospheric pressure and is not insulated. The condensate sub cools to certain degree before it is pumped back to the boiler. The minimum value is 10 &deg; Celsius and default is 20 &deg; Celsius.
-
-#### Field: Water Inlet Node Name
-
-The name of the steam coil inlet from the steam loop, i.e. Steam Coil steam inlet node.
-
-#### Field: Water Outlet Node Name
-
-The name of the steam coil outlet to the condensate loop, i.e. Steam Coil condensate outlet node.
-
-#### Field: Air Inlet Node Name
-
-The name of the air inlet to the steam coil, i.e. Steam Coil Air Inlet Node.
-
-#### Field: Air Outlet Node Name
-
-The name of the air outlet from the steam coil, i.e. Steam Coil Air Outlet Node.
-
-#### Field:Coil Control Type
-
-Choice of either **ZoneLoadControl** steam coil or **TemperatureSetpointControl** steam coil. A zone coil is load controlled and an air loop steam coil is temperature controlled.
-
-#### Field: Temperature Setpoint Node Name
-
-If the coil is used in the air loop simulation and is temperature controlled using a Set Point Manager (i.e., the previous file is TemperatureSetpointConrtol), then the node that is the control node needs to be specified here. If the coil is used in an air terminal unit, the coil is load controlled and a control node set point is not required (i.e., the previous field is ZoneLoadControl).
-
-An example of a Steam Coil input statement (one each for Temperature Controlled and Load Controlled) from an IDF is given below:
-
-```idf
-Coil:Heating:Steam,
-       VAV SYS 1 Heating Coil,                   !- Coil Name
-       ReheatCoilAvailSched,                       !- Availability Schedule Name
-       0.06,                                                       !- Max Steam volume Flow rate
-       5.0,                                                         !- Deg of Subcooling Desired
-       15.0,                                                        !- Loop Subcooling Desired
-       VAV SYS 1 Heating Coil Steam Inlet,   !- Coil Steam Inlet Node
-       VAV SYS 1 Heating Coil Steam Outlet, !- Coil Water Outlet Node
-       VAV SYS 1 Cooling Coil Outlet,       !- Coil Air Inlet Node
-       VAV SYS 1 Heating Coil Outlet,       !- Coil Air Outlet Node
-       TemperatureSetPointControl,             !- field Coil Control Type
-       VAV SYS 1 Heating Coil Outlet;       !- field Coil Temp Setpoint Node
-
-
-Coil:Heating:Steam,
-       SPACE1-1 Reheat Coil,                             !- Coil Name
-       ReheatCoilAvailSched,                             !- Availability Schedule Name
-       autosize,                                                      !- Max Steam volume Flow rate
-       5.0,                                                                !- Deg of Subcooling Desired
-       15.0,                                                              !- Loop Subcooling Desired
-       SPACE1-1 Reheat Coil Steam Inlet,     !- Coil Steam Inlet Node
-       SPACE1-1 Reheat Coil Steam Outlet,   !- Coil Water Outlet Node
-       SPACE1-1 Damper Outlet,                         !- Coil Air Inlet Node
-       SPACE1-1 Supply Inlet,   !- Coil Air Outlet Node
-       ZoneLoadControl;         !- field Coil Control Type
-```
-
-### Heating Coil (Steam) Outputs:
-
-* HVAC,Sum, Heating Coil Heating Energy [J]
-
-* HVAC,Average,Total Steam Coil Heating Rate [W]
-
-* HVAC,Average,Heating Coil Steam Trap Loss Rate [W]
-
-* HVAC, Average, Heating Coil Steam Inlet Temperature [C]
-
-* HVAC, Average, Heating Coil Steam Outlet Temperature [C]
-
-* HVAC, Average, Heating Coil Steam Mass Flow Rate [kg/s]
-
-#### Heating Coil Heating Energy [J]
-
-Heating Coil Heating Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
-
-#### Heating Coil Heating Rate [W]
-
-Heating Coil Heating Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
-
-#### Heating Coil Steam Trap Loss Rate [W]
-
-Loop losses represent the unavoidable loss due to degree of sub cooling in the condensate return piping back to the boiler and the loss occurring due to flashing of steam across the steam trap due to pressure differential between the steam and the condensate side.
-
-#### Heating Coil Steam Inlet Temperature [C]
-
-#### Heating Coil Steam Outlet Temperature [C]
-
-#### Heating Coil Steam Mass Flow Rate [kg/s]
-
-These outputs are the Steam inlet and condensate outlet temperatures and steam flow rate for the boiler.
-
-### Coil:Heating:Electric
-
-The electric heating coil is a simple capacity model with a user-inputted efficiency. In many cases, this efficiency for the electric coil will be 100%. This coil will be simpler than shown in Figure 135 since it will only have air nodes to connect it in the system. The coil can be used in the air loop simulation or in the zone equipment as a reheat coil. Depending on where it is used determines if this coil is temperature or capacity controlled. If used in the air loop simulation it will be controlled to a specified temperature scheduled from the SetPoint Manager. If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand.
-
-#### Field: Name
-
-A unique identifying name for each coil.
-
-#### Field:Availability Schedule Name
-
-Schedule that defines when the coil is available. If the schedule   s value is 0.0, then the coil is not available and flow will not be requested. If the schedule   s value is &gt; 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods. Schedule values must be &gt;= 0 and &lt;= 1.
-
-#### Field: Efficiency
-
-This is user-inputted efficiency (decimal units, not percent) and can account for any loss. In most cases for the electric coil, this will be 100%.
-
-#### Field: Nominal Capacity
-
-This is the maximum capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
-
-#### Field: Air Inlet Node Name
-
-The name of the air inlet to the electric coil, i.e. Heating Coil Air Inlet Node.
-
-#### Field: Air Outlet Node Name
-
-The name of the air outlet from the electric coil, i.e. Heating Coil Air Outlet Node.
-
-#### Field: Temperature Setpoint Node Name
-
-If the coil is used in the air loop simulation and is temperature controlled using a Set Point Manager, then the node that is the control node needs to be specified here. If the coil is used in an air terminal unit, the coil is load controlled and a control node set point is not required.
-
-An example of IDF usage:
-
-```idf
-Coil:Heating:Electric,
-   AHU Reheater,                     !- Name
-   2,                                           !- Availability Schedule Name
-   0.99,                                     !- Efficiency
-   600000,                                 !- Nominal Capacity {W}
-   DOAS Supply Fan Outlet, !- Air Inlet Node Name
-   AHU Reheater Outlet,       !- Air Outlet Node Name
-   AHU Reheater Outlet;       !- Temperature Setpoint Node Name
-```
-
-### Heating Coil (Electric) Outputs
-
-* HVAC,Sum,Heating Coil Air Heating Energy [J]
-
-* HVAC,Average,Heating Coil Air Heating Rate [W]
-
-* HVAC,Sum,Heating Coil Electric Energy [J]
-
-* HVAC,Average,Heating Coil Electric Power [W]
-
-#### Heating Coil Air Heating Energy (J)
-
-Heating Coil Air Heating Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
-
-#### Heating Coil Air Heating Rate [W]
-
-Heating Coil Air Heating Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
-
-#### Heating Coil Electric Energy [J]
-
-Heating Coil electric consumption after the efficiency of the coil has been taken into account in Joules for the timestep reported.
-
-#### Heating Coil Electric Power [W]
-
-This field is the average Heating Coil electric power after the efficiency of the coil has been taken into account in Watts for the timestep reported.
-
-### Coil:Heating:Electric:MultiStage
-
-The multi stage electric heating coil is a simple capacity model with a user-inputted efficiencies at different stages. In many cases, the efficiencies for the electric coil will be 100%. This coil will only have air nodes to connect it in the system. The coil can be used in the air loop simulation or in the zone equipment as a reheat coil. Depending on where it is used determines if this coil is temperature or capacity controlled. If used in the air loop simulation it will be controlled to a specified temperature scheduled from the SetPoint Manager. If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand. For the time being, this coil model can only be called by the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
-
-#### Field: Name
-
-A unique identifying name for each coil.
-
-#### Field:Availability Schedule Name
-
-Schedule that defines when the coil is available. If the schedule   s value is 0.0, then the coil is not available and flow will not be requested. If the schedule   s value is &gt; 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods. Schedule values must be &gt;= 0 and &lt;= 1.
-
-#### Field: Air Inlet Node Name
-
-The name of the air inlet to the electric coil, i.e. Heating Coil Air Inlet Node.
-
-#### Field: Air Outlet Node Name
-
-The name of the air outlet from the electric coil, i.e. Heating Coil Air Outlet Node.
-
-#### Field: Temperature Setpoint Node Name
-
-If the coil is used in the air loop simulation and is temperature controlled using a Set Point Manager, then the node that is the control node needs to be specified here. If the coil is used in an air terminal unit, the coil is load controlled and a control node set point is not required. At present, the multistage electric heating coil does not model temperature setoint control.
-
-#### Field: Stage 1 Efficiency
-
-This is stage 1 user-inputted efficiency (decimal units, not percent) and can account for any loss. In most cases for the electric coil, this will be 100%.
-
-#### Field: Stage 1 Nominal Capacity
-
-This is stage 1 capacity of the coil (W). This field is autosizable.
-
-#### Field: Stage 2 Efficiency
-
-This is stage 2 user-inputted efficiency (decimal units, not percent) and can account for any loss. In most cases for the electric coil, this will be 100%.
-
-#### Field: Stage 2 Nominal Capacity
-
-This is stage 2 capacity of the coil (W). This field is autosizable.
-
-#### Field: Stage 3 Efficiency
-
-This is stage 3 user-inputted efficiency (decimal units, not percent) and can account for any loss. In most cases for the electric coil, this will be 100%.
-
-#### Field: Stage 3 Nominal Capacity
-
-This is stage 3 capacity of the coil (W). This field is autosizable.
-
-#### Field: Stage 4 Efficiency
-
-This is stage 4 user-inputted efficiency (decimal units, not percent) and can account for any loss. In most cases for the electric coil, this will be 100%.
-
-#### Field: Stage 4 Nominal Capacity
-
-This is stage 4 capacity of the coil (W). This field is autosizable.
-
-An example in IDF form:
-
-```idf
-   Coil:Heating:Electric:MultiStage,
-       Heat Pump Heating Coil 1,                 !- Name
-       FanAndCoilAvailSched,                         !- Availability Schedule Name
-       Heating Coil Air Inlet Node,           !- Air Inlet Node Name
-       SuppHeating Coil Air Inlet Node,   !- Air Outlet Node Name
-       ,                                               !- Temp Setpoint node name
-       3,                                             !- Number of Stages
-       1,                                             !- Stage 1 Efficiency
-       Autosize,                               !- Stage 1 Nominal Capacity {W}
-       1,                                             !- Stage 2 Efficiency
-       Autosize,                               !- Stage 2 Nominal Capacity {W}
-       1,                                             !- Stage 3 Efficiency
-       Autosize;                               !- Stage 3 Nominal Capacity {W}
-```
-
-### Heating Coil (Electric Multistage) Outputs
-
-* HVAC,Sum,Heating Coil Energy[J]
-
-* HVAC,Average,Heating Coil Rate[W]
-
-* HVAC,Sum,Heating Coil Electric Consumption [J]
-
-* HVAC,Average,Heating Coil Electric Power [W]
-
-#### Heating Coil Energy (J)
-
-Heating Coil Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
-
-#### Heating Coil Rate[W]
-
-Heating Coil Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
-
-#### Heating Coil Electric Consumption [J]
-
-Heating Coil electric consumption after the efficiency of the coil has been taken into account in Joules for the timestep reported.
-
-#### Heating Coil Electric Power [W]
-
-This field is the average Heating Coil electric power after the efficiency of the coil has been taken into account in Watts for the timestep reported.
-
-### Coil:Heating:Desuperheater
-
-A simplified approach is used to determine the performance of this air heating coil. The model assumes that the heating energy provided by this coil is reclaimed from the superheated refrigerant gas leaving a compressor (i.e., a desuperheating refrigerant-to-air heating coil) and does not impact the performance of the compressor. This coil can be used in air loop simulations but can   t be used by certain compound objects (e.g., AirLoopHVAC:UnitaryHeatPump:AirToAir, AirLoopHVAC:UnitaryHeatPump:WaterToAir, or Dehumidifier:Desiccant:NoFans) or any air distribution equipment (e.g., AirTerminal:SingleDuct:ConstantVolume:Reheat, AirTerminal:SingleDuct:VAV:Reheat, or AirTerminal:SingleDuct:SeriesPIU:Reheat).
-
-The desuperheater heating coil input requires a coil name, an availability schedule, and a heat reclaim recovery efficiency. The reclaim recovery efficiency determines the amount of heat available for use by this heating coil. Approximately 25-30% of the energy rejected by typical refrigeration system condensers is to reduce the superheated refrigerant vapor temperature to the condensing temperature. Recovery efficiencies higher than 30% may cause the refrigerant gas to condense which in turn impacts the performance of the refrigeration system. For this reason, the maximum heat reclaim recovery efficiency for this coil is 30% for most sources of waste heat, including refrigeration compressor racks. The one exception to this 30% limit is a condenser that is part of a detailed refrigeration system. In a detailed refrigeration system, the portion of the rejected heat that lies within the superheated region is explicitly calculated. Therefore, the desuperheater coils supplied by a condenser attached to a detailed refrigeration system are subject to a maximum reclaim recovery efficiency of 90% of the heat within the superheated region.
-
-The next two input items for the desuperheater heating coil are the node names for the inlet and outlet air streams. The following two input fields define the source of heating energy for the coil. This desuperheater heating coil may only be used with direct expansion (DX) cooling or refrigeration equipment. The first of these two inputs is the heating source object type while the second defines the name of the heating source. For proper modeling, the desuperheater heating coil must be placed downstream of a DX cooling coil when reclaiming heat from that cooling coil. Desuperheating heating coil placement is unrestricted when reclaiming heat from a   Refrigeration:CompressorRack   or Refrigeration:Condenser.
-
-The next input field is optional and defines the set point node name if the desuperheater heating coil is to be controlled based on temperature. When a load-based control scheme is used, this field is left blank. A final optional input is used to model parasitic electric energy use of auxiliary equipment associated with the desuperheater heating coil (e.g., solenoid valve).
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a desuperheater heating coil. Any reference to this desuperheater heating coil by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the desuperheater heating coil can run during a given time period. Schedule values must range from 0 to 1. A schedule value greater than 0 indicates that the coil can operate during the time period. A value equal to 0 denotes that the coil must be off for that time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Heat Reclaim Recovery Efficiency
-
-This numeric field defines the ratio of recovered waste heat from the superheated refrigerant gas to the total rejected waste heat from the heating source (as if no heat reclaim occurred). Values can range from 0.0 up to a maximum of 0.9 if the source is a refrigeration condenser and 0.3 for all other waste heat sources. If this input field is left blank, the default value is 0.8 for a refrigeration condenser source type and 0.25 for all other sources.
-
-#### Field: Air Inlet Node Name
-
-This alpha field defines the name of the HVAC system node from which the desuperheater heating coil draws its inlet air.
-
-#### Field: Air Outlet Node Name
-
-This alpha field defines the name of the HVAC system node to which the desuperheater heating coil sends its outlet air.
-
-#### Field: Heating Source Object Type
-
-This alpha field defines the source of superheated refrigerant gas from which the desuperheater heating coil recovers energy. Valid choices are:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* Coil:Cooling:DX:TwoSpeed
-
-* Coil:Cooling:DX:TwoStageWithHumidityControlMode
-
-* Refrigeration:CompressorRack
-
-* Refrigeration:Condenser:AirCooled
-
-* Refrigeration:Condenser:EvaporativeCooled
-
-* Refrigeration:Condenser:WaterCooled
-
-When the heating coil source is a DX Coil, the air loop   s supply air fan control mode may be auto fan (cycling fan cycling coil), constant fan, or variable volume. When the heating source is a compressor rack for refrigerated cases or a refrigeration condenser, the supply air fan control mode should be either variable volume or constant fan.
-
-NOTE: Use of the desuperheater heating coil in variable air volume systems should be done with caution since the model assumption of a fixed heat reclaim recovery efficiency may not be valid if the air flow rate over the coil varies significantly.
-
-#### Field: Heating Source Name
-
-This alpha field defines the name of the desuperheater heating coil source (e.g., the name of a specific valid coil (as mentioned in the previous field) which provides waste heat to this desuperheater heating coil).
-
-NOTE: When the heating source is a   Refrigeration Compressor rack, the heat rejection location in the Refrigeration:CompressorRack object must be    Outdoors   . If the compressor rack heat rejection location is    Zone   , the total amount of heat rejection available for reclaim (e.g., by this desuperheater heating coil) is set to zero by the compressor rack object and the simulation proceeds.
-
-#### Field: Temperature Setpoint Node Name
-
-This optional alpha field defines the name of the HVAC system node used for temperature-based control (e.g., controlling the heating coil   s outlet air dry-bulb temperature to a setpoint). If the desuperheater heating coil is temperature controlled through the use of a Set Point Manager, then the control node specified in the Set Point Manager will be entered here. If the desuperheater heating coil is controlled based on a certain heating load to be met (e.g., using this heating coil as part of AirLoopHVAC:Unitary:Furnace:HeatCool for high humidity control), this field should be left blank.
-
-#### Field: Parasitic Electric Load
-
-This optional numeric field defines the parasitic electric load (in Watts) due to control valves or other devices specific to the desuperheater heating coil. The load is applied whenever the coil is heating the air. The model assumes that this electric load is small and does not contribute to heating the air.
-
-Following is an example input for a desuperheater heating coil.
-
-```idf
-Coil:Heating:Desuperheater,
-   DesuperheaterCoil,                                   !- Coil Name
-   FanAndCoilAvailSched,                             !- Availability Schedule
-   0.3,                                                               !- Heat Reclaim Recovery Efficiency
-   Cooling Coil Air Outlet Node,             !- Coil Air Inlet Node Name
-   Air Loop Outlet Node,                             !- Coil Air Outlet Node Name
-   Coil:Cooling:DX:SingleSpeed, !- Heating Source Type
-   Furnace ACDXCoil 1,                                 !- Heating Source Name
-   ,                                                                     !- Coil Temperature Setpoint Node Name
-   0.1;                                                               !- Parasitic Electric Load {W}
-```
-
-### Heating Coil (Desuperheater) Outputs
-
-* HVAC,Average,Heating Coil Rate [W]
-
-* HVAC,Sum,Heating Coil Energy [J]
-
-* HVAC,Average,Heating Coil Electric Power [W]
-
-* HVAC,Sum,Heating Coil Electric Consumption [J]
-
-* HVAC,Average,Heating Coil Runtime Fraction []
-
-* HVAC,Average,Heating Coil Air Heating Rate [W]
-
-* HVAC,Sum,Heating Coil Air Heating Energy [J]
-
-* HVAC,Average,Heating Coil Electric Power [W]
-
-* HVAC,Sum,Heating Coil Electric Energy [J]
-
-* HVAC,Average,Heating Coil Runtime Fraction
-
-#### Heating Coil Air Heating Rate [W]
-
-This output is the average heating rate of the desuperheater heating coil in Watts over the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Heating Coil Air Heating Energy [J]
-
-This output is the total heating output of the desuperheater heating coil in Joules over the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Electric Power [W]
-
-This output is the average electric consumption rate for the parasitic load associated with the desuperheater heating coil in Watts.
-
-#### Heating Coil Electric Energy [J]
-
-This output is the electric consumption of the desuperheater heating coil parasitic load in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Runtime Fraction []
-
-This is the runtime fraction of the desuperheater heating coil for the timestep being reported. Since the desuperheater heating coil can only provide heat when the heat source object is active, the runtime fraction of the desuperheater heating coil will always be less than or equal to the runtime fraction of the heat source object.
-
-### Coil:Cooling:DX:VariableRefrigerantFlow
-
-The variable refrigerant flow (VRF) DX cooling coil model is nearly identical to the single-speed DX cooling coil model (Ref. Coil:Cooling:DX:SingleSpeed). For this reason, an adaptation of the single-speed DX cooling coil model is used to model the variable-speed compression system used in VRF AC systems. The model inputs are quite similar to the input requirements for the single-speed DX cooling coil model, however, the location of a majority of the inputs have been moved to the variable refrigerant flow air conditioner object since multiple DX cooling coils will use the same DX compression system (Ref. AirConditioner:VariableRefrigerantFlow).
-
-#### Field: Coil Name
-
-This alpha field defines a unique user-assigned name for an instance of a VRF DX cooling coil. Any reference to this DX cooling coil by another object will use this name. This cooling coil name must be entered in the AirConditioner:VariableRefrigerantFlow object. No other sytem type uses this specific coil.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the DX cooling coil availabiltiy schedule. Schedule values of 0 denote the DX cooling coil is off. A schedule value greater than 0 indicates that the coil can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Gross Rated Total Cooling Capacity
-
-This numeric field defines the gross rated total cooling capacity of the DX cooling coil in watts. The total cooling capacity should be a    gross   , i.e., the effect of supply air fan heat NOT accounted for.
-
-#### Field: Gross Ratio Sensible Heat Ratio
-
-This numeric field defines the gross sensible heat ratio (sensible capacity divided by total cooling capacity) of the DX cooling coil at rated conditions. Both the sensible and total cooling capacities used to define the Rated SHR should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for)
-
-#### Field: Rated Air Flow Rate
-
-The air volume flow rate, in m<sup>3</sup> per second, across the DX cooling coil at rated conditions. The rated air volume flow rate should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of rated total cooling capacity (300 to 450 cfm/ton). The gross rated total cooling capacity and gross rated SHR should be performance information for the unit with at this rated air volume flow rate.
-
-#### Field: Cooling Capacity Ratio Modifier Function of Temperature Curve Name
-
-This alpha field defines the cooling capacity ratio modifier as a function of indoor wet-bulb temperature or indoor wet-bulb and outdoor dry-bulb temperatures. This curve is a linear, quadratic, or cubic curve if the cooling capacity is solely a function of indoor wet-bulb temperature (i.e., the indoor terminal units weighted average inlet air wet-bulb temperatures). Without specific manufacturers data indicating otherwise, the use of a single independent variable is recommended for this coil type. If, however, the user has reason to believe the cooling capacity is both a function of indoor wet-bulb temperature and outdoor dry-bulb temperature (and has manufacturers data to create the performance curve), a bi-quadratic equation using weighted average indoor wet-bulb temperature and condenser entering air dry-bulb temperature as the independent variables may be used. See the Engineering Reference for more discussion on using this input field.
-
-#### Field: Cooling Capacity Modifier Curve Function of Flow Fraction Name
-
-This alpha field defines the name of a linear, quadratic or cubic performance curve (ref:   Performance Curves) that parameterizes the variation of total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
-
-#### Field: Coil Air Inlet Node Name
-
-This alpha field defines the name of the air inlet node entering the DX cooling coil.
-
-#### Field: Coil Air Outlet Node Name
-
-This alpha field defines the name of the air outlet node exiting the DX cooling coil.
-
-#### Field: Name of Water Storage Tank for Condensate Collection
-
-This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
-
-Following is an example input for a Coil:Cooling:DX:VariableRefrigerantFlow object.
-
-
-
-```idf
-COIL:Cooling:DX:VariableRefrigerantFlow,
-       TU1 VRF DX Cooling Coil, !- Coil Name
-       VRFAvailSched,                     !- Availability Schedule Name
-       autosize,                               !- Gross Rated Total Cooling Capacity {W}
-       autosize,                               !- Gross Rated Sensible Heat Ratio
-       autosize,                               !- Rated Air Flow Rate {m3/s}
-       VRFTUCoolCapFT,                   !- Cooling Capacity Ratio Modifier Function of Temperature Curve Name
-       VRFACCoolCapFFF,                 !- Cooling Capacity Modifier Curve Function of Flow Fraction Name
-       TU1 VRF DX CCoil Inlet Node,   !- Coil Air Inlet Node
-       TU1 VRF DX CCoil Outlet Node;   !- Coil Air Outlet Node
-```
-
-
-
-### Cooling DX Coil (VariableRefrigerantFlow) Outputs
-
-* HVAC,Average, Cooling Coil Total Cooling Rate [W]
-
-* HVAC,Sum, Cooling Coil Total Cooling Energy [J]
-
-* HVAC,Average, Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC,Sum, Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC,Average, Cooling Coil Latent Cooling Rate [W]
-
-* HVAC,Sum, Cooling Coil Latent Cooling Energy [J]
-
-* HVAC,Average, Cooling Coil Runtime Fraction []
-
-
-
-Evaporative-cooled condenser:
-
-* HVAC,Average,Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-* Zone,Meter,Condensate:OnSiteWater [m3]
-
-* HVAC,Sum,Cooling Coil Condensate Volume [m3]
-
-#### Cooling Coil Total Cooling Rate [W]
-
-This field is the total (sensible and latent) cooling rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Total Cooling Energy [J]
-
-This is the total (sensible plus latent) cooling output of the DX coil in Joules over the time step being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = CoolingCoils, Group Key = System (Ref. Output:Meter objects).
-
-#### Cooling Coil Sensible Cooling Rate [W]
-
-This output is the moist air sensible cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Sensible Cooling Energy [J]
-
-This is the moist air sensible cooling output of the DX coil in Joules for the time step being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Latent Cooling Rate [W]
-
-This is the latent cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Latent Cooling Energy [J]
-
-This is the latent cooling output of the DX coil in Joules for the time step being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Runtime Fraction []
-
-This is the runtime fraction of the DX coil compressor and condenser fan(s) for the time step being reported.
-
-#### Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-#### Cooling Coil Condensate Volume [m3]
-
-These outputs are the rate and volume of water collected as condensate from the coil. These reports only appear if a water storage tank is named in the input object.
-
-### Coil:Heating:DX:VariableRefrigerantFlow
-
-The variable refrigerant flow (VRF) DX heating coil model uses performance information at rated conditions along with performance curves for variations in total capacity, energy input ratio and part load fraction to determine performance at part-load conditions. The impacts of defrost operation is modeled based a combination of user inputs and empirical models taken from the air-to-air heat pump algorithms in DOE-2.1E.
-
-The VRF DX heating coil input requires an availability schedule, the gross rated heating capacity and the rated air volume flow rate. The rated air volume flow rate should be between 0.00008056 m<sup>3</sup>/s and 0.00002684 m<sup>3</sup>/s per watt of gross rated heating capacity.
-
-Two performance curves are required. The first performance curve defines the heating capacity as a function of indoor air dry-bulb and outdoor condenser entering air wet-bulb temperature. This curve object is specified in the variable refrigerant flow air-to-air heat pump object. The second performance curve is specific the each VRF DX heating coil and defines the change in heating capacity as a function of air flow fraction. Each of these performance curves are further discussed here.
-
-1)      Heating capacity modifier curve (function of temperature, specified in Heat Pump)
-
-The heating capacity modifier curve (function of temperature) can be a function of both the outdoor wet-bulb temperature and indoor air dry-bulb temperature. Users have the choice of a bi-quadratic curve with two independent variables or a tri-quadratic curve with three independent variable. The tri-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the combined total capacity of all indoor units connected to the heat pump condenser and a more realistic output. The output of this curve is multiplied by the gross rated heating capacity to give the gross heating capacity at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature) and the combination ratio of the installed system.
-
-2)      Heating capacity modifier curve (function of flow fraction, specified in DX coil)
-
-The heating capacity modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating.
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a VRF DX heating coil. Any reference to this DX heating coil by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the DX heating coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Gross Rated Heating Capacity
-
-This numeric field defines the total, full load gross heating capacity in watts of the DX coil unit at rated conditions (outside air dry-bulb temperature of 8.33 C, outside air wet-bulb temperature of 6.11 C, heating coil entering air dry-bulb temperature of 21.11 C, heating coil entering air wet-bulb temperature of 15.55 C, and a heating coil air flow rate defined by field    rated air flow volume    below). The value entered here must be greater than 0. The gross total heating capacity should not account for the effect of supply air fan heat.
-
-#### Field: Rated Air Flow Rate
-
-This numeric field defines the volume air flow rate, in m<sup>3</sup> per second, across the DX heating coil at rated conditions. The value entered here must be greater than 0. The rated air volume flow rate should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of gross rated heating capacity. The gross rated heating capacity and the gross rated COP should be performance information for the unit with outside air dry-bulb temperature of 8.33 C, outside air wet-bulb temperature of 6.11 C, heating coil entering air dry-bulb temperature of 21.11 C, heating coil entering air wet-bulb temperature of 15.55 C, and the rated air volume flow rate defined here.
-
-#### Field: Coil Air Inlet Node
-
-This alpha field defines the name of the HVAC system node from which the DX heating coil draws its inlet air.
-
-#### Field: Coil Air Outlet Node
-
-This alpha field defines the name of the HVAC system node to which the DX heating coil sends its outlet air.
-
-#### Field: Heating Capacity Ratio Modifier Function of Temperature Curve Name
-
-This alpha field defines the heating capacity ratio modifier as a function of indoor dry-bulb temperature or indoor dry-bulb and outdoor wet-bulb temperatures. This curve is a linear, quadratic, or cubic curve if the heating capacity is solely a function of indoor dry-bulb temperature (i.e., the indoor terminal units weighted average inlet air dry-bulb temperatures). Without specific manufacturers data indicating otherwise, the use of a single independent variable is recommended for this coil type. If, however, the user has reason to believe the heating capacity is both a function of indoor dry-bulb temperature and outdoor wet-bulb temperature (and has manufacturers data to create the performance curve), a bi-quadratic equation using weighted average indoor dry-bulb temperature and condenser entering air wet-bulb temperature as the independent variables may be used. See the Engineering Reference for more discussion on using this input field.
-
-Note: The choice of using either outdoor dry-bulb temperature or outdoor wet-bulb temperature as the independent variable in this performance curve is set in the parent object AirConditioner: VariableRefrigerantFlow.
-
-#### Field: Heating Capacity Ratio Modifier Function of Flow Fraction Curve Name
-
-This alpha field defines the name of a linear, quadratic or cubic performance curve (ref:   Performance Curves) that parameterizes the variation of heating capacity as a function of the ratio of actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
-
-Following is an example input for the object.
-
-
-
-```idf
-COIL:Heating:DX:VariableRefrigerantFlow,
-       TU1 VRF DX Heating Coil, !- Coil Name
-       VRFAvailSched,                     !- Availability Schedule
-       autosize,                               !- Gross Rated Heating Capacity {W}
-       autosize,                               !- Rated Air Flow Rate {m3/s}
-       TU1 VRF DX CCoil Outlet Node,   !- Coil Air Inlet Node
-       TU1 VRF DX HCoil Outlet Node,   !- Coil Air Outlet Node
-       VRFTUHeatCapFT,                   !- Heating Capacity Ratio Modifier Function of Temperature Curve Name
-       VRFACCoolCapFFF;                 !- Total heating capacity modifier curve Function of Flow Fraction
-```
-
-
-### Heating DX Coil (VariableRefrigerantFlow) Outputs
-
-* HVAC,Average, Heating Coil Total Heating Rate [W]
-
-* HVAC,Sum, Heating Coil Total Heating Energy [J]
-
-* HVAC,Average, Heating Coil Runtime Fraction []
-
-#### Heating Coil Total Heating Rate [W]
-
-This field is the total heating rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Heating Coil Total Heating Energy [J]
-
-This is the total heating output of the DX coil in Joules over the time step being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Runtime Fraction []
-
-This is the runtime fraction of the DX coil compressor and condenser fan(s) for the time step being reported.
-
-### Coil:Cooling:DX:VariableRefrigerantFlow:FluidTemperatureControl
-
-This coil object is specifically designed for the physics based VRF model applicable for Fluid Temperature Control (VRF-FluidTCtrl). It describes the performance of the indoor unit coil of the VRF system operating at cooling mode. The name of this object is entered as an input to the object *ZoneHVAC:TerminalUnit:VariableRefrigerantFlow*. The outdoor unit part of the VRF system is modeled separately (refer to *AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl* object).
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a VRF DX cooling coil. Any reference to this DX cooling coil by another object will use this name. This cooling coil name must be entered in the AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl object. No other system type uses this specific coil.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the coil availability schedule. A name should be entered to define the availability of the coil. Schedule values of 0 denote the DX cooling coil is off. A schedule value greater than 0 indicates that the coil can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Coil Air Inlet Node
-
-This alpha field defines the name of the air inlet node entering the DX cooling coil.
-
-#### Field: Coil Air Outlet Node
-
-This alpha field defines the name of the air outlet node exiting the DX cooling coil.
-
-#### Field: Rated Total Cooling Capacity
-
-This numeric field defines the gross rated total cooling capacity of the DX cooling coil in watts. The total cooling capacity should be a gross , i.e., the effect of supply air fan heat NOT accounted for.
- 
-#### Field: Rated Sensible Heat Ratio
-
-This numeric field defines the gross sensible heat ratio (sensible capacity divided by total cooling capacity) of the DX cooling coil at rated conditions. Both the sensible and total cooling capacities used to define the Rated SHR should be gross (i.e., the effect of supply air fan heat is NOT accounted for)
-	   
-#### Field: Indoor Unit Reference Superheating 
-
-This numeric field defines the reference superheating degrees of the indoor unit. If this field is blank, the default value of 5.0 C is used. 
-	   
-#### Field: Indoor Unit Evaporating Temperature Function of Superheating Curve Name    
-
-This alpha field defines the name of a quadratic performance curve that parameterizes the variation of indoor unit evaporating temperature as a function of superheating degrees. The output of this curve is the temperature difference between the coil surface air temperature and the evaporating temperature.
-   
-#### Field: Name of Water Storage Tank for Condensate Collection
-
-This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
-
-Following is an example input for a Coil:Cooling:DX:VariableRefrigerantFlow:FluidTemperatureControl object.
-
-```idf
-  Coil:Cooling:DX:VariableRefrigerantFlow:FluidTemperatureControl,
-    TU1 VRF DX Cooling Coil, !- Name
-    VRFAvailSched,           !- Availability Schedule Name
-    TU1 VRF DX CCoil Inlet Node,  !- Coil Air Inlet Node
-    TU1 VRF DX CCoil Outlet Node,  !- Coil Air Outlet Node
-    autosize,                !- Rated Total Cooling Capacity {W}
-    autosize,                !- Rated Sensible Heat Ratio
-    3,                       !- Indoor Unit Reference Superheating Degrees {C}    
-    IUEvapTempCurve,         !- Indoor Unit Evaporating Temperature Function of Superheating Curve Name    
-    ;                        !- Name of Water Storage Tank for Condensate Collection
-
-  Curve:Quadratic,
-    IUEvapTempCurve,         !- Name
-    0,                       !- Coefficient1 Constant
-    0.843,                   !- Coefficient2 x
-    0,                       !- Coefficient3 x**2
-    0,                       !- Minimum Value of x    
-    15,                      !- Maximum Value of x    
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature;             !- Output Unit Type
-
-```
-
-### Cooling DX Coil (VariableRefrigerantFlow:FluidTemperatureControl) Outputs
-
-* HVAC,Average, Cooling Coil Total Cooling Rate [W]
-
-* HVAC,Sum, Cooling Coil Total Cooling Energy [J]
-
-* HVAC,Average, Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC,Sum, Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC,Average, Cooling Coil Latent Cooling Rate [W]
-
-* HVAC,Sum, Cooling Coil Latent Cooling Energy [J]
-
-* HVAC,Average, Cooling Coil Runtime Fraction []
-
-* HVAC,Average, Cooling Coil VRF Evaporating Temperature [C]
-
-* HVAC,Average, Cooling Coil VRF Super Heating Degrees [C]
-
-Evaporative-cooled condenser:
-
-* HVAC,Average,Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-* Zone,Meter,Condensate:OnSiteWater [m3]
-
-* HVAC,Sum,Cooling Coil Condensate Volume [m3]
-
-#### Cooling Coil Total Cooling Rate [W]
-
-This field is the total (sensible and latent) cooling rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Total Cooling Energy [J]
-
-This is the total (sensible plus latent) cooling output of the DX coil in Joules over the time step being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = CoolingCoils, Group Key = System (Ref. Output:Meter objects).
-
-#### Cooling Coil Sensible Cooling Rate [W]
-
-This output is the moist air sensible cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Sensible Cooling Energy [J]
-
-This is the moist air sensible cooling output of the DX coil in Joules for the time step being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Latent Cooling Rate [W]
-
-This is the latent cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Latent Cooling Energy [J]
-
-This is the latent cooling output of the DX coil in Joules for the time step being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Runtime Fraction []
-
-This is the runtime fraction of the DX coil compressor and condenser fan(s) for the time step being reported.
-
-#### Cooling Coil VRF Evaporating Temperature [C]
-
-This is the evaporating temperature of the VRF system operating at cooling mode. This value is manipulated by the VRF system considering the load conditions of all the zones it serves. It affects the cooling coil surface temperature and thus the cooling capacity of the coil.
-
-#### Cooling Coil VRF Super Heating Degrees [C]
-
-This is the super heating degrees of the VRF system operating at cooling mode. This value is manipulated by each VRF terminal unit to adjust the cooling capacity of the coil considering the load conditions of the zone. It affects the cooling coil surface temperature and thus the cooling capacity of the coil.
-
-#### Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-This is the volumetric rate of water collected as condensate from the coil. This report only appears if a water storage tank is named in the input object.
-
-#### Cooling Coil Condensate Volume [m3]
-
-This is the volume of water collected as condensate from the coil. This report only appears if a water storage tank is named in the input object.
-
-
-### Coil:Heating:DX:VariableRefrigerantFlow:FluidTemperatureControl
-
-This coil object is specifically designed for the physics based VRF model applicable for Fluid Temperature Control (VRF-FluidTCtrl). It describes the performance of the indoor unit coil of the VRF system operating at heating mode. The name of this object is entered as an input to the object *ZoneHVAC:TerminalUnit:VariableRefrigerantFlow*. The outdoor unit part of the VRF system is modeled separately (refer to *AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl* object).
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a VRF DX heating coil. Any reference to this DX heating coil by another object will use this name. This heating coil name must be entered in the AirConditioner:VariableRefrigerantFlow:FluidTemperatureControl object. No other system type uses this specific coil.
-
-#### Field: Availability Schedule
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the DX heating coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank the unit is always available.
-
-#### Field: Coil Air Inlet Node
-
-This alpha field defines the name of the HVAC system node from which the DX heating coil draws its inlet air.
-
-#### Field: Coil Air Outlet Node
-
-This alpha field defines the name of the HVAC system node to which the DX heating coil sends its outlet air.
-
-#### Field: Rated Total Heating Capacity
-
-This numeric field defines the total, full load gross heating capacity in watts of the DX coil unit at rated conditions. The value entered here must be greater than 0. The gross total heating capacity should not account for the effect of supply air fan heat.
-
-#### Field: Indoor Unit Reference Subcooling 
-
-This numeric field defines the reference subcooling degrees of the indoor unit. If this field is blank, the default value of 5.0 C is used. 
-       
-#### Field: Indoor Unit Condensing Temperature Function of Subcooling Curve Name 
-
-This alpha field defines the name of a quadratic performance curve that parameterizes the variation of indoor unit condensing temperature as a function of subcooling degrees. The output of this curve is the temperature difference between the condensing temperature and the coil surface air temperature.
-
-Following is an example input for a Coil:Heating:DX:VariableRefrigerantFlow:FluidTemperatureControl object.
-
-```idf
-  Coil:Heating:DX:VariableRefrigerantFlow:FluidTemperatureControl,
-    TU1 VRF DX Heating Coil, !- Name
-    VRFAvailSched,           !- Availability Schedule
-    TU1 VRF DX CCoil Outlet Node,  !- Coil Air Inlet Node
-    TU1 VRF DX HCoil Outlet Node,  !- Coil Air Outlet Node
-    autosize,                !- Rated Total Heating Capacity {W}
-    5,                       !- Indoor Unit Reference Subcooling Degrees {C}    
-    IUCondTempCurve;         !- Indoor Unit Condensing Temperature Function of Subcooling Curve Name
-
-  Curve:Quadratic,
-    IUCondTempCurve,         !- Name
-    -1.85,                   !- Coefficient1 Constant
-    0.411,                   !- Coefficient2 x
-    0.0196,                  !- Coefficient3 x**2
-    0,                       !- Minimum Value of x    
-    20,                      !- Maximum Value of x    
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature;             !- Output Unit Type
-
-```
-
-### Heating DX Coil (VariableRefrigerantFlow) Outputs
-
-* HVAC,Average, Heating Coil Total Heating Rate [W]
-
-* HVAC,Sum, Heating Coil Total Heating Energy [J]
-
-* HVAC,Average, Heating Coil Runtime Fraction []
-
-* Heating Coil VRF Condensing Temperature [C]
-
-* Heating Coil VRF Subcooling Degrees [C]
-
-#### Heating Coil Total Heating Rate [W]
-
-This field is the total heating rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Heating Coil Total Heating Energy [J]
-
-This is the total heating output of the DX coil in Joules over the time step being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Runtime Fraction []
-
-This is the runtime fraction of the DX coil compressor and condenser fan(s) for the time step being reported.
-
-#### Cooling Coil VRF Condensing Temperature [C]
-
-This is the condensing temperature of the VRF system operating at heating mode. This value is manipulated by the VRF system considering the load conditions of all the zones it serves. It affects the heating coil surface temperature and thus the heating capacity of the coil.
-
-#### Cooling Coil VRF Subcooling Degrees [C]
-
-This is the subcooling degrees of the VRF system operating at heating mode. This value is manipulated by each VRF terminal unit to adjust the heating capacity of the coil considering the load conditions of the zone. It affects the heating coil surface temperature and thus the heating capacity of the coil.
-
-
-
-### Coil:Heating:Gas
-
-The gas heating coil is a simple capacity model with a user inputted gas burner efficiency. The default for the gas burner efficiency is 80%. This coil will be simpler than shown in Figure 135 since it will only have air nodes to connect it in the system. The coil can be used in the air loop simulation or in the zone equipment as a reheat coil. Depending on where it is used determines if this coil is temperature or capacity controlled. If used in the air loop simulation it will be controlled to a specified temperature scheduled from the Setpoint Manager. If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand.
-
-#### Field: Name
-
-A unique identifying name for each coil.
-
-#### Field: Availability Schedule Name
-
-Schedule that defines when the coil is available. If the schedule   s value is 0.0, then the coil is not available and flow will not be requested. If the schedule   s value is &gt; 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods. Schedule values must be &gt;= 0 and &lt;= 1.
-
-#### Field: Gas Burner Efficiency
-
-This is user inputted gas burner efficiency (decimal, not percent) and is defaulted to 80%.
-
-#### Field: Nominal Capacity
-
-This is the maximum capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
-
-#### Field: Air Inlet Node Name
-
-The name of the air inlet to the gas coil, i.e. Heating Coil Air Inlet Node.
-
-#### Field: Air Outlet Node Name
-
-The name of the air outlet from the gas coil, i.e. Heating Coil Air Outlet Node.
-
-#### Field: Temperature Setpoint Node Name
-
-If the coil is used in the air loop simulation and is temperature controlled using a Set Point Manager, then the node that is the control node needs to be specified here. If the coil is used in an air terminal unit, the coil is load controlled and a control node set point is not required.
-
-#### Field: Parasitic Electric Load
-
-This is the parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.. This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation timestep.
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of gas consumption rate by the heating coil as a function of the part load ratio (PLR, sensible heating load/nominal capacity of the heating coil). For any simulation timestep, the nominal gas consumption rate (heating load/burner efficiency) is divided by the part-load fraction (PLF) if a part-load curve has been defined. The part-load curve accounts for efficiency losses due to transient coil operation.
-
-The part-load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the heating coil runs continuously for the simulation timestep). For PLR values between 0 and 1 ( 0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7     and     PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the heating coil is defined a PLR/PLF. If PLF &lt; PLR, then a warning message is issues and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional gas heating coil (e.g., residential furnace) would be:
-
-           PLF = 0.8 + 0.2(PLR)
-
-#### Field: Parasitic Gas Load
-
-This numeric field is the parasitic gas load associated with the gas coil   s operation (Watts), such as a standing pilot light. The model assumes that this parasitic load is consumed only for the portion of the simulation timestep where the gas heating coil is not operating.
-
-### Heating Coil (Gas) Outputs
-
-* HVAC,Sum,Heating Coil Air Heating Energy [J]
-
-* HVAC,Average,Heating Coil Air Heating Rate [W]
-
-* HVAC,Sum,Heating Coil Gas Energy [J]
-
-* HVAC,Average,Heating Coil Gas Rate [W]
-
-* HVAC,Sum,Heating Coil Electric Energy [J]
-
-* HVAC,Average,Heating Coil Electric Power [W]
-
-* HVAC,Average,Heating Coil Runtime Fraction []
-
-* HVAC,Sum,Heating Coil Ancillary Gas Energy [J]
-
-* HVAC,Average,Heating Coil Ancillary Gas Rate [W]
-
-#### Heating Coil Air Heating Energy [J]
-
-This field is the total heating output of the coil in Joules over the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Air Heating Rate [W]
-
-This field is the average heating rate output of the coil in Watts over the timestep being reported.
-
-#### Heating Coil Gas Energy [J]
-
-This field is the gas consumption of the heating coil in Joules over the timestep being reported, including the impacts of part-load performance if a part load fraction correlation is specified. This output is also added to a meter with Resource Type = Gas, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Gas Rate [W]
-
-This field is the average gas consumption rate of the coil in Watts over the timestep being reported, including the impacts of part-load performance if a part load fraction correlation is specified.
-
-#### Heating Coil Electric Energy [J]
-
-This field is the electric consumption of the heating coil auxiliaries in Joules over the timestep being reported (e.g., inducer fan). This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Electric Power [W]
-
-This field is the average electric consumption rate of the heating coil auxiliaries (e.g., inducer fan) in Watts over the timestep being reported.
-
-#### Heating Coil Runtime Fraction []
-
-This field is the runtime fraction of the coil over the timestep being reported.
-
-#### Heating Coil Ancillary Gas Energy [J]
-
-This field is the parasitic gas consumption of the heating coil in Joules over the timestep being reported (e.g., standing pilot light). The model assumes that the parasitic load is accumulated only for the portion of the simulation timestep where the gas heating coil is not operating. This output is also added to a meter with Resource Type = Gas, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Ancillary Gas Rate [W]
-
-This field is the average parasitic gas consumption rate of the heating coil (e.g., standing pilot light) in Watts over the timestep being reported. The model assumes that the parasitic load is present only for the portion of the simulation timestep where the gas heating coil is not operating.
-
-### Coil:Heating:Gas:MultiStage
-
-The multi stage gas heating coil is a simple capacity model with a user inputted gas burner efficiencies at different stages. This coil will only have air nodes to connect it in the system. The coil can be used in the air loop simulation or in the zone equipment as a reheat coil. Depending on where it is used determines if this coil is temperature or capacity controlled. If used in the air loop simulation it will be controlled to a specified temperature scheduled from the Setpoint Manager. If it is used in zone equipment, it will be controlled from the zone thermostat by meeting the zone demand. For the time being, this coil model can only be called by the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
-
-#### Field: Name
-
-A unique identifying name for each coil.
-
-#### Field: Availability Schedule Name
-
-Schedule that defines when the coil is available. If the schedule   s value is 0.0, then the coil is not available and flow will not be requested. If the schedule   s value is &gt; 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods. Schedule values must be &gt;= 0 and &lt;= 1.
-
-#### Field: Air Inlet Node Name
-
-The name of the air inlet to the gas coil, i.e. Heating Coil Air Inlet Node.
-
-#### Field: Air Outlet Node Name
-
-The name of the air outlet from the gas coil, i.e. Heating Coil Air Outlet Node.
-
-#### Field: Temperature Setpoint Node Name
-
-If the coil is used in the air loop simulation and is temperature controlled using a Set Point Manager, then the node that is the control node needs to be specified here. If the coil is used in an air terminal unit, the coil is load controlled and a control node set point is not required. At present, the multistage gas heating coil does not model temperature setoint control.
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of gas consumption rate by the heating coil as a function of the part load ratio (PLR, sensible heating load/nominal capacity of the heating coil). For any simulation timestep, the nominal gas consumption rate (heating load/burner efficiency) is divided by the part-load fraction (PLF) if a part-load curve has been defined. The part-load curve accounts for efficiency losses due to transient coil operation.
-
-The part-load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the heating coil runs continuously for the simulation timestep). For PLR values between 0 and 1 ( 0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7     and     PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the heating coil is defined a PLR/PLF. If PLF &lt; PLR, then a warning message is issues and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional gas heating coil (e.g., residential furnace) would be:
-
-           PLF = 0.8 + 0.2(PLR)
-
-#### Field: Parasitic Gas Load
-
-This numeric field is the parasitic gas load associated with the gas coil   s operation (Watts), such as a standing pilot light. The model assumes that this parasitic load is consumed only for the portion of the simulation timestep where the gas heating coil is not operating.
-
-#### Field: Stage 1 Gas Burner Efficiency
-
-This is user inputted stage 1 gas burner efficiency (decimal, not percent) and is defaulted to 80%.
-
-#### Field: Stage 1 Nominal Capacity
-
-This is the stage 1 capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
-
-#### Field: Stage 1 Parasitic Electric Load
-
-This is the stage 1 parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.. This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation timestep.
-
-#### Field: Stage 2 Gas Burner Efficiency
-
-This is user inputted stage 2 gas burner efficiency (decimal, not percent) and is defaulted to 80%.
-
-#### Field: Stage 2 Nominal Capacity
-
-This is the stage 2 capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
-
-#### Field: Stage 2 Parasitic Electric Load
-
-This is the stage 2 parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.. This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation timestep.
-
-#### Field: Stage 3 Gas Burner Efficiency
-
-This is user inputted stage 3 gas burner efficiency (decimal, not percent) and is defaulted to 80%.
-
-#### Field: Stage 3 Nominal Capacity
-
-This is the stage 3 capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
-
-#### Field: Stage 3 Parasitic Electric Load
-
-This is the stage 3 parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.. This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation timestep.
-
-#### Field: Stage 4 Gas Burner Efficiency
-
-This is user inputted stage 4 gas burner efficiency (decimal, not percent) and is defaulted to 80%.
-
-#### Field: Stage 4 Nominal Capacity
-
-This is the stage 4 capacity of the coil (W). This controlled coil will only provide the needed capacity to meet the control criteria whether it is temperature or capacity controlled. This field is autosizable.
-
-#### Field: Stage 4 Parasitic Electric Load
-
-This is the stage 4 parasitic electric load associated with the gas coil operation, such as an inducer fan, etc.. This will be modified by the PLR (or coil runtime fraction if a part-load fraction correlation is provided in the next input field) to reflect the time of operation in a simulation timestep.
-
-
-
-An example in IDF form:
-
-```idf
-   Coil:Heating:Gas:MultiStage,
-       Heat Pump Heating Coil 1,                 !- Name
-       FanAndCoilAvailSched,                         !- Availability Schedule Name
-       Heating Coil Air Inlet Node,           !- Air Inlet Node Name
-       SuppHeating Coil Air Inlet Node,   !- Air Outlet Node Name
-       ,                                               !- Temp Setpoint node name
-       ,                                               !- Part Load Fraction Correlation Curve Name
-       ,                                               !- Parasitic Gas Load
-       3,                                             !- Number of Speeds
-       0.92,                                       !- Speed 1 Gas burner Efficiency
-       Autosize,                               !- Speed 1 Nominal Capacity {W}
-       ,                                               !- Stage 1 Parasitic Electric Load {W}
-       0.88,                                       !- Speed 2 Gas burner Efficiency
-       Autosize,                               !- Speed 2 Nominal Capacity {W}
-       ,                                               !- Stage 2 Parasitic Electric Load {W}
-       0.84,                                       !- Speed 3 Gas burner Efficiency
-       Autosize,                               !- Speed 3 Nominal Capacity {W}
-       ;                                               !- Stage 3 Parasitic Electric Load {W}
-```
-
-
-### Heating Coil (Gas Multistage) Outputs
-
-* HVAC,Sum,Heating Coil Energy[J]
-
-* HVAC,Average,Heating Coil Rate[W]
-
-* HVAC,Sum,Heating Coil Gas Consumption [J]
-
-* HVAC,Average,Heating Coil Gas Consumption Rate [W]
-
-* HVAC,Sum,Heating Coil Electric Consumption [J]
-
-* HVAC,Average,Heating Coil Electric Power [W]
-
-* HVAC,Average,Heating Coil Runtime Fraction
-
-* HVAC,Sum,Heating Coil Parasitic Gas Consumption [J]
-
-* HVAC,Average,Heating Coil Parasitic Gas Consumption Rate [W]
-
-#### Heating Coil Energy [J]
-
-This field is the total heating output of the coil in Joules over the timestep being reported. This output is also added to an output meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Rate [W]
-
-This field is the average heating rate output of the coil in Watts over the timestep being reported.
-
-#### Heating Coil Gas Consumption [J]
-
-This field is the gas consumption of the heating coil in Joules over the timestep being reported, including the impacts of part-load performance if a part load fraction correlation is specified. This output is also added to an output meter with Resource Type = Gas, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Gas Consumption Rate [W]
-
-This field is the average gas consumption rate of the coil in Watts over the timestep being reported, including the impacts of part-load performance if a part load fraction correlation is specified.
-
-#### Heating Coil Electric Consumption [J]
-
-This field is the electric consumption of the heating coil auxiliaries in Joules over the timestep being reported (e.g., inducer fan). This output is also added to an output meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Electric Power [W]
-
-This field is the average electric consumption rate of the heating coil auxiliaries (e.g., inducer fan) in Watts over the timestep being reported.
-
-#### Heating Coil Parasitic Gas Consumption [J]
-
-This field is the parasitic gas consumption of the heating coil in Joules over the timestep being reported (e.g., standing pilot light). The model assumes that the parasitic load is accumulated only for the portion of the simulation timestep where the gas heating coil is not operating. This output is also added to an output meter with Resource Type = Gas, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Parasitic Gas Consumption Rate [W]
-
-This field is the average parasitic gas consumption rate of the heating coil (e.g., standing pilot light) in Watts over the timestep being reported. The model assumes that the parasitic load is present only for the portion of the simulation timestep where the gas heating coil is not operating.
-
-### Coil:Cooling:Water:DetailedGeometry
-
-This detailed flat fin coil model is for continuous plate fins. First, found in Type 12 from MODSIM, but now programmed directly from Elmahdy, A.H. and Mitalas, G.P. Then there was a discontinuity in their original model that was fixed in the EnergyPlus implementation. Now this model can be used in an interval halving solution technique for controlling this coil without the problems of non-convergence.
-
-"A Model for Cooling and Dehumidifying Coils for Use in Energy Requirements for Buildings"   ASHRAE Transactions, Vol. 83, Part 2, pp. 103-117 (1977). For fin efficiency see K.A. Gardner, "Efficiency of Extended   ," Transactions ASME, Vol. 67, pp. 621-631, 1945.
-
-The following figures illustrate the geometry and circuits in a cooling coil.
-
-![Figure104\_GeometryofaCoolingCoilCC](media/image353.png)
-
-Figure 136. Geometry of a Cooling Coil (CC)
-
-
-
-![Figure105\_NumberofCoolantCircuiteCCNCC](media/image354.png)
-
-Figure 137. Number of Coolant Circuits (CCNCC)
-
-#### Field: Name
-
-A unique identifying name for each coil.
-
-#### Field:Availability Schedule Name
-
-Schedule that defines when the coil is available. If the schedule   s value is 0.0, then the coil is not available and flow will not be requested. If the schedule   s value is &gt; 0.0 (usually 1 is used), the coil is available. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Maximum Water Flow Rate
-
-The maximum possible water flow rate (m<sup>3</sup>/sec) through the coil.
-
-#### Field: Tube Outside Surface Area
-
-The outside surface area (m<sup>2</sup>) of the tubes that is exposed to air (i.e. the outside area of the unfinned tubes minus the area of tubes covered by the fins).
-
-#### Field: Total Tube Inside Area
-
-The total surface area (m<sup>2</sup>) inside the tubes (water side).
-
-#### Field: Fin Surface Area
-
-The total surface area (m<sup>2</sup>) of the fins attached to the coil.
-
-#### Field: Minimum Air Flow Area
-
-The minimum cross sectional area (m<sup>2</sup>) available for air passage. Frequently calculated as
-
-           Amin  = (Amin/Afr)\*Afr
-
-where Afr  is the frontal area of the heat exchanger, and (Amin/Afr) is the ratio of the minimum airflow area to frontal area.
-
-#### Field: Coil Depth
-
-The distance (m) from the front of the coil to the back of the coil in the airflow direction. Also called the fin depth. Illustrated in the figure (Figure 136. Geometry of a Cooling Coil (CC)).
-
-#### Field: Fin Diameter
-
-The outside diameter (m) of the fins. Used instead of COIL HEIGHT
-
-#### Field: Fin Thickness
-
-Thickness (m) of the air side fins.
-
-#### Field: Tube Inside Diameter
-
-The inside diameter (m) of the tubes.
-
-#### Field: Tube Outside Diameter
-
-The outside diameter (m) of the tubes.
-
-#### Field: Tube Thermal Conductivity
-
-The thermal conductivity (W/m-K) of the tube material.
-
-#### Field: Fin Thermal Conductivity
-
-The thermal conductivity (W/m-K) of the fin material.
-
-#### Field: Fin Spacing
-
-The spacing (m) of the fins, centerline to centerline.
-
-#### Field: Tube Depth Spacing
-
-The spacing (m) of the tube rows, centerline to centerline. Also called tube longitudinal spacing.
-
-#### Field: Number of Tube Rows
-
-The number of tube rows in the direction of the airflow.
-
-#### Field: Number of Tubes per Row
-
-The number of tubes per row. (NTPR in the above diagram)
-
-#### Field: Water Inlet Node Name
-
-The name of the water coil inlet from the chilled water loop, i.e. Cooling Coil Water Inlet Node.
-
-#### Field: Water Outlet Node Name
-
-The name of the water coil outlet from the chilled water loop, i.e. Cooling Coil Water Outlet Node.
-
-#### Field: Air Inlet Node Name
-
-The name of the air inlet to the water coil, i.e. Cooling Coil Air Inlet Node.
-
-#### Field: Air Outlet Node Name
-
-The name of the air outlet from the water coil, i.e. Cooling Coil Air Outlet Node.
-
-#### Field: Condensate Collection Water Storage Tank Name
-
-This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
-
-Examples of these statements in an IDF are:
-
-```idf
-Coil:Cooling:Water:DetailedGeometry,
-           Detailed Cooling Coil,   !Name of cooling coil
-           CoolingCoilAvailSched,   !Cooling Coil Schedule
-           0.0011,                   !Max Water Flow Rate of Coil m3/sec
-           6.23816,                 !Tube Outside Surf Area
-           6.20007018,           !Tube Inside Surf Area
-           101.7158224,         !Fin Surf Area
-           0.300606367,         !Min Air Flow Area
-           0.165097968,         !Coil Depth
-           0.43507152,           !Coil Height
-           0.001499982,         !Fin Thickness
-           0.014449958,         !Tube Inside Diameter
-           0.015879775,         !Tube Outside Diameter
-           386.0,                     !Tube Thermal Conductivity
-           204.0,                     !Fin Thermal Conductivity
-           0.001814292,         !Fin Spacing
-           0.02589977,           !Tube Depth
-           6,                             !Number of Tube Rows
-           16,                           !Number of Tubes per Row
-           NODE_32,NODE_33, !Coil Water Side Inlet & Outlet Node
-           NODE_5, NODE_6;   !Coil Air Side Inlet & Outlet Node
-```
-
-
-### Detailed Geometry Cooling Coil (Water) Outputs
-
-* HVAC,Sum,Cooling Coil Total Cooling Energy [J]
-
-* HVAC,Sum,Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Total Cooling Rate [W]
-
-* HVAC,Average,Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC,Average,Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Coil Source Side Heat Transfer Energy [J]
-
-* HVAC,Sum,Cooling Coil Condensate Volume [m3]
-
-#### Cooling Coil Total Cooling Energy (J)
-
-Cooling Coil Total Cooling Energy is the total amount of heat transfer taking place in the coil at the operating conditions.
-
-#### Cooling Coil Sensible Cooling Energy (J)
-
-Cooling Coil Sensible Cooling Energy is the total amount of Sensible heat transfer taking place in the coil at the operating conditions. It only takes into account temperature difference in the inlet and outlet air streams at operating conditions.
-
-#### Cooling Coil Total Cooling Rate (W)
-
-Cooling Coil Total Cooling Rate is the Rate of heat transfer taking place in the coil at the operating conditions. The units are (J/sec) or Watts.
-
-#### Cooling Coil Sensible Cooling Rate (W)
-
-Cooling Coil Sensible Cooling Rate is the Rate of Sensible heat transfer taking place in the coil at the operating conditions.
-
-In addition, if a Water Storage Tank is used to collect coil condensate, then the following outputs will be available.
-
-#### Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-#### Cooling Coil Condensate Volume [m3]
-
-These reports provide the rate and amount of condensate from the coil. Condensate is water condensed out of the air as a result of cooling. The condensate volume is also reported on the   meter for    OnSiteWater.   
-
-#### Cooling Coil Source Side Heat Transfer Energy [J]
-
-This is the energy extracted from the chilled water serving the cooling coil, in Joules.
-
-### Coil:Cooling:DX:SingleSpeed
-
-This DX cooling coil input requires an availability schedule, the gross rated total cooling capacity, the gross rated SHR, the gross rated COP, and the rated air volume flow rate. The latter 4 inputs determine the coil performance at the rating point (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb and air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb). The rated air volume flow rate should be between .00004027 m<sup>3</sup>/s and .00006041 m<sup>3</sup>/s per watt of gross rated total cooling capacity (300 to 450 cfm/ton).
-
-The rated volumetric air flow to total cooling capacity ratio for 100% dedicated outdoor air (DOAS) application DX cooling coils should be between 0.00001677 (m3/s)/W (125 cfm/ton) and 0.00003355 (m3/s)/W (250 cfm/ton).
-
-Pumped refrigerant economizer integrated with the single speed DX cooling coil model will use exactly the same model except that performance curves use lookup table to cover the pumped refrigerant economizer and the compressor operating ranges. One or two independent variables may used to represent the performance data.
-
-This model requires 5 curves as follows:
-
-1.        The total cooling capacity modifier curve (function of temperature) is a curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures).  This curve is typically a biquadratic but any curve or table with two independent variables can be used.
-
-2.        The total cooling capacity modifier curve (function of flow fraction) is a curve or lookup table with the independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating.  This curve is typically a quadratic or cubic but any curve or table with one independent variables can be used.
-
-3.        The energy input ratio (EIR) modifier curve (function of temperature) is a curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures).  This curve is typically a biquadratic but any curve or table with two independent variables can be used.
-
-4.        The energy input ratio (EIR) modifier curve (function of flow fraction) is a curve or lookup table with the independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating.  This curve is typically a quadratic or cubic but any curve or table with one independent variables can be used.
-
-5.        The part load fraction correlation (function of part load ratio) is a curve or a lookup table with the independent variable being part load ratio (sensible cooling load / steady-state sensible cooling capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the    effective    EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The curve should be normalized to a value of 1.0 when the part-load ratio equals 1.0 (i.e., the compressor(s) run continuously for the simulation timestep).  This curve is typically a quadratic or cubic but any curve or table with one independent variables can be used.
-
-The curves are simply specified by name. Curve inputs are described in the curve manager section of this document (see Performance Curves in this document).
-
-The next four input fields are optional and relate to the degradation of latent cooling capacity when the supply air fan operates continuously while the cooling coil/compressor cycle on and off to meet the cooling load. The fan operating mode is determined in the partent object and is considered to either be constant (e.g. CoilSystem:Cooling:DX) or can be scheduled (e.g. AirLoopHVAC:UnitaryHeatCool). When scheduled, the schedule value must be greater than 0 to calculate degradation of latent cooling capacity. At times when the parent object   s supply air fan operating mode schedule is 0, latent degradation will be ignored. When modeling latent capacity degradation, these next four input fields must all have positive values.
-
-The next input specifies the outdoor air node used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor temperature entering the condenser is taken directly from the weather data. If this field is not blank, the node name specified must be listed in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor temperature from the weather data. Alternately, the node name must be specified in an OutdoorAir:NodeList object where the outdoor temperature entering the condenser is taken directly from the weather data.
-
-The next input describes the type of outdoor condenser coil used with the DX cooling coil (Air Cooled or Evap Cooled). The following three inputs are required when modeling an evaporative-cooled condenser: evaporative condenser effectiveness, evaporative condenser air volume flow rate, and the power consumed by the evaporative condenser pump. Crankcase heater capacity and cutout temperature are entered in the next two input fields. These two fields for this object define the name of the water storage tank for supply and condensate collection. See section    DX Cooling Coil Model    in the EnergyPlus Engineering Document for further details regarding this model.
-
-The last two input fields following the Basin Heater Operating Schedule Name are the Sensible Heat Ratio (SHR) modifier cruve names for temperature and flow fraction.   These two input fields   are optional and used only when a user intends to override SHR calculated using the apparatus dew point (ADP) and bypass factor (BF) method.   See section    SHR Calculation Using User Specified SHR Modifier Curves    in the EnergyPlus Engineering Document for further details.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a DX cooling coil. Any reference to this DX coil by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the DX cooling coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during a given time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Gross Rated Total Cooling Capacity
-
-The total, full load gross cooling capacity (sensible plus latent) in watts of the DX coil unit at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb[[1]](#_ftn1), and a cooling coil air flow rate defined by field    rated air flow rate    below). Capacity should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for). When used in a heat pump, the gross rated total cooling capacity should be within 20% of the gross rated heating capacity, otherwise a warning message is issued.
-
-#### Field: Gross Rated Sensible Heat Ratio
-
-The sensible heat ratio (SHR= gross sensible cooling capacity divided by gross total cooling capacity) of the DX cooling coil at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb), and a cooling coil air flow rate defined by field    rated air flow rate    below). Both the sensible and total cooling capacities used to define the Rated SHR should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for).
-
-#### Field: Gross Rated Cooling COP
-
-The coefficient of performance is the ratio of the gross total cooling capacity in watts to electrical power input in watts of the DX cooling coil unit at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/ 23.9 &deg;C wetbulb, and a cooling coil air flow rate defined by field    rated air flow rate    below). The input power includes electric power for the compressor(s) and condenser fan(s) but does not include the power consumption of the supply air fan. The gross COP should NOT account for the supply air fan. If this input field is left blank, the default value is 3.0.
-
-#### Field: Rated Air Flow Rate
-
-The air volume flow rate, in m<sup>3</sup> per second, across the DX cooling coil at rated conditions. The rated air volume flow rate should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of gross rated total cooling capacity (300 to 450 cfm/ton). For DOAS applications the rated air volume flow rate should be between 0.00001677 m<sup>3</sup>/s and 0.00003355 m<sup>3</sup>/s per watt of gross rated total cooling capacity (125 to 250 cfm/ton).   The gross rated total cooling capacity, gross rated SHR and gross rated COP should be performance information for the unit with air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and the rated air volume flow rate defined here.
-
-#### Field: Rated Evaporator Fan Power Per Volume Flow Rate
-
-This field is the electric power for the evaporator (cooling coil) fan per air volume flow rate through the coil at the rated conditions in W/(m<sup>3</sup>/s). The default value is 773.3 W/(m<sup>3</sup>/s) (365 W/1000 cfm) if this field is left blank. If a value is entered, it must be &gt;= 0.0 and &lt;= 1250 W/(m<sup>3</sup>/s). This value is only used to calculate Seasonal Energy Efficiency Ratio (SEER), Energy Efficiency Ratio (EER), Integrated Energy Efficiency Ratio (IEER) and the Standard Rating (Net) Cooling Capacity which will be outputs in the EnergyPlus eio file (ref. EnergyPlus Engineering Reference, Single Speed DX Cooling Coil, Standard Ratings). This value is not used for modeling the evaporator (cooling coil) fan during simulations; instead, it is used for calculating SEER, EER, IEER and Standard Rating Cooling Capacity to assist the user in verifying their inputs for modeling this type of equipment.
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node from which the DX cooling coil draws its inlet air.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node to which the DX cooling coil sends its outlet air.
-
-#### Field: Total Cooling Capacity Function of Temperature Curve Name
-
-The name of a performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to have the value of 1.0 at the rating point.  This curve is typically a biquadratic but any curve or table with two independent variables can be used.
-
-#### Field: Total Cooling Capacity Function of Flow Fraction Curve Name
-
-The name of a quadratic or cubic performance curve (ref:   Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
-
-#### Field: Energy Input Ratio Function of Temperature Curve Name
-
-The name of a performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to a value of 1.0 at the rating point.  This curve is typically a biquadratic but any curve or table with two independent variables can be used.
-
-#### Field: Energy Input Ratio Function of Flow Fraction Curve Name
-
-The name of a performance curve (Ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate.  This curve is typically a quadratic or cubic but any curve or table with one independent variables can be used.
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the    effective    EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.  This curve is typically a quadratic or cubic but any curve or table with one independent variables can be used.
-
-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7     and     PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
-
-           PLF = 0.85 + 0.15(PLR)
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-           PLF = 1.0 + 0.0(PLR)
-
-#### Field: Nominal Time for Condensate Removal to Begin
-
-The nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]), and this field as well as the next three input fields for this object must have positive values in order to model latent capacity degradation.
-
-#### Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity
-
-Ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]); and this field, the previous field and the next two fields must have positive values in order to model latent capacity degradation.
-
-#### Field: Maximum Cycling Rate
-
-The maximum on-off cycling rate for the compressor (cycles per hour), which occurs at 50% run time fraction. Suggested value is 3; zero value means latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]); and this field, the previous two fields and the next field must have positive values in order to model latent capacity degradation.
-
-#### Field: Latent Capacity Time Constant
-
-Time constant (in seconds) for the cooling coil's latent capacity to reach steady state after startup. Suggested value is 45: supply air fan operating mode must be continuous. That is, the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects (e.g., AirloopHVAC:UnitaryHeatCool), and this field as well as the previous three input fields for this object must have positive values in order to model latent capacity degradation.
-
-#### Field: Condenser Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
-
-#### Field: Condenser Type
-
-The type of condenser used by the DX cooling coil. Valid choices for this input field are **AirCooled** or **EvaporativelyCooled**. The default for this field is **AirCooled**.
-
-#### Field: Evaporative Condenser Effectiveness
-
-The effectiveness of the evaporative condenser, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
-
-<div>\[Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectiveness} \right)\left( {Tdb,o\,\, - Twb,o} \right)\]</div>
-
-where
-
-*T<sub>cond\\ inlet</sub>* = the temperature of the air entering the condenser coil (C)
-
-*T<sub>wb,o</sub>* = the wet-bulb temperature of the outdoor air (C)
-
-*T<sub>db,o</sub>* = the dry-bulb temperature of the outdoor air (C)
-
-The resulting condenser inlet air temperature is used by the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled.
-
-If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
-
-If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
-
-If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
-
-#### Field: Evaporative Condenser Air Flow Rate
-
-The air volume flow rate, in m<sup>3</sup> per second, entering the evaporative condenser. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000144 m<sup>3</sup>/s per watt of rated total cooling capacity [850 cfm/ton]). This field is not used when Condenser Type = Air Cooled.
-
-#### Field: Evaporative Condenser Pump Rated Power Consumption
-
-The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt [15 W/ton] of rated total cooling capacity). This field is not used when Condenser Type = Air Cooled.
-
-#### Field: Crankcase Heater Capacity
-
-This numeric field defines the crankcase heater capacity in Watts. When the outdoor air dry-bulb temperature is below the value specified in the input field    Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation    (described below), the crankcase heater is enabled during the time that the compressor is not running. If this cooling coil is used as part of an air-to-air heat pump (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir or PackageTerminal: HeatPump:AirToAir), the crankcase heater defined for this DX cooling coil is ignored and the crankcase heater power defined for the DX heating coil (Ref. Coil:Heating:DX:SingleSpeed) is enabled during the time that the compressor is not running for either heating or cooling. The value for this input field must be greater than or equal to 0, and the default value is 0. To simulate a DX cooling coil without a crankcase heater, enter a value of 0.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which the compressor   s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 &deg;C, and the default value is 10 &deg;C.
-
-#### Field: Supply Water Storage Tank Name
-
-This field is optional. It is used to describe where the coil obtains water used for evaporative cooling of its condenser. If blank or omitted, then the unit will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, then the unit will obtain its water from that tank. If a tank is specified, the unit will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the condenser needs, then the unit will still operate and obtain the rest of the water it needs from the mains (referred to as StarvedWater).
-
-#### Field: Condensate Collection Water Storage Tank Name
-
-This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the DX coil   s electric evaporative cooler basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the DX coil is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the DX coil is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the DX coil is off.
-
-#### Field: Sensible Heat Ratio Function of Temperature Curve Name
-
-The name of a biquadratic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of DX cooling coil entering air wet-bulb and dry-bulb temperatures. The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of flow fraction) to give the SHR at the specific coil entering air temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 at the rated condition. This input field is optional.
-
-#### Field: Sensible Heat Ratio Function of Flow Fraction Curve Name
-
-The name of a quadratic or cubic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of temperature) to give the SHR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This input field is optional.
-
-#### Field: Zone Name for Condenser Placement
-
-This input field is name of a conditioned or unconditioned zone where the secondary coil (condenser) of DX system or a heat pump is to be placed.  This is an optional input field specified only when user desires to reject the condenser heat into a zone.  The heat rejected is modeled as sensible internal gain of a secondary zone. 
-
-Following is an example input for a Coil:Cooling:DX:SingleSpeed coil.
-
-```idf
-Coil:Cooling:DX:SingleSpeed,
-             Zone1WindACDXCoil,               ! Coil Name
-             FanAndCoilAvailSched,         ! Availability Schedule
-             10548,           ! Gross Rated Total Cooling Capacity
-             0.75,             ! Gross Rated Sensible Heat Ratio
-             3.0,               ! Gross Rated Cooling COP
-             0.637,           ! Rated Air Flow Rate (m3/s)
-             773.3,           ! Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
-             Zone1WindACFanOutletNode, ! Coil Air Inlet Node
-             Zone1WindACAirOutletNode, ! Coil Air Outlet Node
-             WindACCoolCapFT,                   ! Total Cooling Capacity Modifier Curve (function of temperature)
-             WindACCoolCapFFF,                 ! Total Cooling Capacity Modifier Curve (function of flow fraction)
-             WindACEIRFT,                           ! Energy Input Ratio Modifier Curve (function of temperature)
-             WindACEIRFFF,                         ! Energy Input Ratio Modifier Curve (function of flow fraction)
-             WindACPLFFPLR,                       ! Part Load Fraction Correlation (function of part load ratio)
-             1000.,                         ! Nominal Time for Condensate Removal to Begin {s}
-             1.5,                             ! Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity
-             3.0,                             ! Maximum ON/OFF Cycling Rate {cycles/hr}
-             45.0,                           ! Latent Capacity Time Constant {s}
-             ,                                   ! Condenser Air Inlet Node Name
-             AirCooled,               ! Condenser Type
-             ,                                   ! Evaporative Condenser Effectiveness
-             ,                                   ! Evaporative Condenser Air Volume Flow Rate {m3/s}
-             ,                                   ! Evaporative Condenser Pump Rated Power Consumption {W}
-             30.,                             ! Crankcase Heater Capacity {W}
-             10.;                             ! Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
-```
-
-
-### Coil:Cooling:DX:TwoSpeed
-
-This component models a two-speed (or variable speed) DX compressor and fan. The method is based on the model used for the cycling, single speed DX unit. The single speed unit is described by single full load capacity, SHR, COP, and air flow rate at rated conditions. Off rated full load performance is obtained by the use of 4 modifier curves. At partial load the unit cycles on/off and the cycling losses are described by a part load fraction curve.
-
-The multispeed unit is described by specifying the performance at two states: high speed compressor, high speed fan; and low speed compressor, low speed fan. When the unit load is above the high speed capacity, the unit runs with high speed compressor and fan. When the load on the unit is below the high speed capacity but above the low speed capacity, the unit will run with performance intermediate between high speed and low speed. When the load is less than the low speed capacity, the unit will cycle on/off just like the single speed unit.
-
-The multispeed unit model requires 2 full sets of performance data. There must be a high and low speed capacity, SHR, COP, and evaporator air flow rate; as well as high and low speed performance curves     total cooling capacity modifier curve (function of temperature) and energy input ratio modifier curve (function of temperature).
-
-The multispeed DX component should be used for all cases in which a DX VAV system is being simulated. Obviously this model     in which performance is obtained by interpolating between 2 specified states - is an oversimplification of how real multi-speed and variable speed DX cooling units are controlled. But detailed descriptions of how actual units perform and are controlled are not available. This model should give a good average prediction of multispeed and variable speed DX cooling unit performance. The last four input fields following the Basin Heater Operating Schedule Name are the Sensible Heat Ratio (SHR) modifier cruve names for temperature and flow fraction for high and low speed DX cooling coils.   These four input fields   are optional and used only when a user intends to override SHR calculated using the apparatus dew point (ADP) and bypass factor (BF) method.   See section    SHR Calculation Using User Specified SHR Modifier Curves    in the EnergyPlus Engineering Document for further details..
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a multispeed DX cooling coil. Any reference to this DX coil by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the DX cooling coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: High Speed Gross Rated Total Cooling Capacity
-
-The total, full load gross cooling capacity (sensible plus latent) in watts of the DX coil unit for high speed compressor and high speed fan at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and a cooling coil air flow rate defined by field    rated air flow rate    below). Capacity should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for).
-
-#### Field: High Speed Gross Rated Sensible Heat Ratio
-
-The sensible heat ratio (gross sensible capacity divided by gross total cooling capacity) of the DX cooling coil   for high speed compressor and high speed fan at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb[[2]](#_ftn2), and a cooling coil air flow rate defined by field    rated air flow rate    below). Both the sensible and total cooling capacities used to define the Rated SHR should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for).
-
-#### Field: High Speed Gross Rated Cooling COP
-
-The coefficient of performance is the ratio of the gross total cooling capacity in watts to electrical power input in watts) of the DX cooling coil unit for high speed compressor and high speed fan at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and a cooling coil air flow rate defined by field    rated air flow rate    below). The input power includes electric power for the compressor(s) and condenser fan(s) but does not include the power consumption of the supply air fan. The gross COP should NOT account for the supply air fan. If this input field is left blank, the default value is 3.0.
-
-#### Field: High Speed Rated Air Flow Rate
-
-The high speed air volume flow rate, in m<sup>3</sup> per second, across the DX cooling coil at rated conditions. The rated air volume flow rate should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of gross rated total cooling capacity. For DOAS applications the rated air volume flow rate should be between 0.00001677 m<sup>3</sup>/s and 0.00003355 m<sup>3</sup>/s per watt of gross rated total cooling capacity (125 to 250 cfm/ton).   The gross rated total cooling capacity, gross rated SHR and gross rated COP should be performance information for the unit with air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and the rated air volume flow rate defined here.
-
-#### Field: Unit Internal Static Air Pressure
-
-If this coil is used with a Fan:VariableVolume to model a packaged variable-air-volume unit, then ratings for standard rated net capacity, EER, and IEER will be calculated per ANSI/AHRI Standard 340/360-2007 with Addenda 1 and 2.   This field is to specify the internal static air pressure, in units of Pascals, associated with the unit   s supply air flow for rating purposes.   This field does not affect the performance during operation.   This field is optional. If this field is used, then the internal static air pressure is used with the associated fan characteristics when calculating standard rated net capacity, EER, and IEER.   If this field is not used, then the standard ratings are still performed but use a default for specific fan power of 773.3 (W/(m<sup>3</sup>/s)).   The air pressure drop/rise input here should be    internal    in the sense that it is for the entire package of unitary equipment as it would be tested in a laboratory (including other non-cooling sections inside the package for filters, dampers, and.or heating coils) but none of the    external    pressure drop for distributing supply air throughout the building.   This is different from the input field called Pressure Rise in the fan object which includes both the external static pressure and the internal static pressure.   The results of standard rating calculations are reported to the EIO file and to predefined output tables called    DX Cooling Coils    and    VAV DX Cooling Standard Rating Details.   
-
-#### Field: Air Inlet Node
-
-The name of the HVAC system node from which the DX cooling coil   draws its inlet air.
-
-#### Field: Air Outlet Node
-
-The name of the HVAC system node to which the DX cooling coil   sends its outlet air.
-
-#### Field: Total Cooling Capacity Function of Temperature Curve Name
-
-The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to have the value of 1.0 at the rating point. This curve is used for performance at the high speed compressor, high speed fan operating point.
-
-#### Field: Total Cooling Capacity Function of Flow Fraction Curve Name
-
-The name of a quadratic performance curve (ref:   Performance Curves) that parameterizes the variation of gross total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate. This curve is applied only at the high speed compressor, high speed fan operating point. There is no corresponding curve for the low speed operating point.
-
-#### Field: Energy Input Ratio Function of Temperature Curve Name
-
-The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the wet-bulb temperature of the air entering the cooling coil and the dry-bulb temperature of the air entering the air-cooled condenser (wet-bulb temperature if modeling an evaporative-cooled condenser). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to a value of 1.0 at the rating point. This curve is used for performance at the high speed compressor, high speed fan operating point.
-
-#### Field: Energy Input Ratio Function of Flow Fraction Curve Name
-
-The name of a quadratic performance curve (Ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This curve is applied only at the high speed compressor, high speed fan operating point. There is no corresponding curve for the low speed operating point.
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the    effective    EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
-
-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7     and     PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
-
-           PLF = 0.85 + 0.15(PLR)
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-           PLF = 1.0 + 0.0(PLR)
-
-#### Field: Low Speed Gross Rated Total Cooling Capacity
-
-The total, full load gross total cooling capacity (sensible plus latent) in watts of the DX coil unit for low speed compressor and low speed fan at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and a cooling coil air flow rate defined by field    rated air flow rate, low speed    below). Capacity should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for).
-
-#### Field: Low Speed Gross Rated Sensible Heat Ratio
-
-The sensible heat ratio (SHR= gross sensible capacity divided by gross total cooling capacity) of the DX cooling coil   for low speed compressor and low speed fan at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and a cooling coil air flow rate defined by field    rated air flow rate, low speed    below). Both the sensible and total cooling capacities used to define the Rated SHR should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for).
-
-#### Field: Low Speed Gross Rated Cooling COP
-
-The coefficient of performance is the ratio of   gross total cooling capacity in watts to electrical power input in watts) of the DX cooling coil unit for low speed compressor and low speed fan at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and a cooling coil air flow rate defined by field    rated air volume flow rate, low speed    below). The input power includes power for the compressor(s) and condenser fan(s) but does not include the power consumption of the supply air fan. The gross COP should NOT account for the supply air fan. If this input field is left blank, the default value is 3.0.
-
-#### Field: Low Speed Rated Air Flow Rate
-
-The low speed volume air flow rate, in m<sup>3</sup> per second, across the DX cooling coil at rated conditions. The rated air volume flow rate should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of the gross rated total cooling capacity. For DOAS applications the rated air volume flow rate should be between 0.00001677 m<sup>3</sup>/s and 0.00003355 m<sup>3</sup>/s per watt of gross rated total cooling capacity (125 to 250 cfm/ton).   The gross rated total cooling capacity, gross rated SHR and gross rated COP should be performance information for the unit with air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and the rated air volume flow rate defined here.
-
-#### Field: Low Speed Total Cooling Capacity Function of Temperature Curve Name
-
-The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to have the value of 1.0 at the rating point. This curve is used for performance at the low speed compressor, low speed fan operating point.
-
-#### Field: Low Speed Energy Input Ratio Function of Temperature Curve Name
-
-The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the wetbulb temperature of the air entering the cooling coil and the drybulb temperature of the air entering the air-cooled condenser (wetbulb temperature if modeling an evaporative-cooled condenser). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to a value of 1.0 at the rating point. This curve is used for performance at the low speed compressor, low speed fan operating point.
-
-#### Field: Condenser Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
-
-#### Field: Condenser Type
-
-The type of condenser used by the multi-speed DX cooling coil. Valid choices for this input field are **AirCooled** or **EvaporativelyCooled**. The default for this field is **AirCooled**.
-
-#### Field: High Speed Evaporative Condenser Effectiveness
-
-The effectiveness of the evaporative condenser at high compressor/fan speed, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
-
-<div>\[Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectivenes{s_{HighSpeed}}} \right)\left( {Tdb,o\,\, - Twb,o} \right)\]</div>
-
-where
-
-*T<sub>cond\\ inlet</sub>* = the temperature of the air entering the condenser coil (C)
-
-*T<sub>wb,o</sub>* = the wet-bulb temperature of the outdoor air (C)
-
-*T<sub>db,o</sub>* = the dry-bulb temperature of the outdoor air (C)
-
-The resulting condenser inlet air temperature is used by the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled.
-
-If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
-
-If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
-
-If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
-
-#### Field: High Speed Evaporative Condenser Air Flow Rate
-
-The air volume flow rate, in m<sup>3</sup> per second, entering the evaporative condenser at high compressor/fan speed. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000144 m<sup>3</sup>/s per watt of rated high-speed total cooling capacity [850 cfm/ton]). This field is not used when Condenser Type = Air Cooled.
-
-#### Field: High Speed Evaporative Condenser Pump Rated Power Consumption
-
-The rated power of the evaporative condenser water pump in Watts at high compressor/fan speed. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt [15 W/ton] of rated high-speed total cooling capacity). This field is not used when Condenser Type = Air Cooled.
-
-#### Field: Low Speed Evaporative Condenser Effectiveness
-
-The effectiveness of the evaporative condenser at low compressor/fan speed, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
-
-<div>\[Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectivenes{s_{LowSpeed}}} \right)\left( {Tdb,o\,\, - Twb,o} \right)\]</div>
-
-where
-
-*T<sub>cond\\ inlet</sub>* = the temperature of the air entering the condenser coil (C)
-
-*T<sub>wb,o</sub>* = the wet-bulb temperature of the outdoor air (C)
-
-*T<sub>db,o</sub>* = the dry-bulb temperature of the outdoor air (C)
-
-The resulting condenser inlet air temperature is used by the Total Cooling Capacity Modifier Curve, low speed (function of temperature) and the Energy Input Ratio Modifier Curve, low speed (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled. See field    Evaporative Condenser Effectiveness, High Speed    above for further information.
-
-#### Field: Low Speed Evaporative Condenser Air Flow Rate
-
-The air volume flow rate, in m<sup>3</sup> per second, entering the evaporative condenser at low compressor/fan speed. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000048 m<sup>3</sup>/s per watt of rated high-speed total cooling capacity [280 cfm/ton]). This field is not used when Condenser Type = Air Cooled.
-
-#### Field: Low Speed Evaporative Condenser Pump Rated Power Consumption
-
-The rated power of the evaporative condenser water pump in Watts at low compressor/fan speed. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.001422 W per watt [5 W/ton] of rated high-speed total capacity). This field is not used when Condenser Type = Air Cooled.
-
-#### Field: Supply Water Storage Tank Name
-
-This field is optional. It is used to describe where the coil obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the coil will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains (referred to as StarvedWater).
-
-#### Field: Condensate Collection Water Storage Tank Name
-
-This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the DX coil   s electric evaporative cooler basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the DX coil is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the DX coil is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the DX coil is off.
-
-#### Field: Sensible Heat Ratio Function of Temperature Curve Name
-
-The name of a biquadratic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of DX cooling coil entering air wet-bulb and dry-bulb temperatures. The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of flow fraction) to give the SHR at the specific coil entering air temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 at the rated condition. This input field is optional.
-
-#### Field: Sensible Heat Ratio Function of Flow Fraction Curve Name
-
-The name of a quadratic or cubic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of temperature) to give the SHR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This input field is optional.
-
-#### Field: Low Sensible Heat Ratio Function of Temperature Curve Name
-
-The name of a biquadratic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of DX cooling coil entering air wet-bulb and dry-bulb temperatures. The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of flow fraction) to give the SHR at the specific coil entering air temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 at the rated condition. This input field is optional.
-
-#### Field: Low Sensible Heat Ratio Function of Flow Fraction Curve Name
-
-The name of a quadratic or cubic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of temperature) to give the SHR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This input field is optional.
-
-#### Field: Zone Name for Condenser Placement
-
-This input field is name of a conditioned or unconditioned zone where the secondary coil (condenser) of DX system or a heat pump is to be placed.  This is an optional input field specified only when user desires to reject the condenser heat into a zone.  The heat rejected is modeled as sensible internal gain of a secondary zone.
-
-Following are example inputs for the object.
-
-```idf
-   Coil:Cooling:DX:TwoSpeed,
-       Main Cooling Coil 1,         !- Name
-       CoolingCoilAvailSched,     !- Availability Schedule Name
-       autosize,                               !- Gross Rated High Speed Total Cooling Capacity {W}
-       0.68,                                       !- Gross Rated High Speed Sensible Heat Ratio
-       3.0,                                         !- Gross Rated High Speed Cooling COP
-       autosize,                               !- Rated High Speed Air Flow Rate {m3/s}
-       ,                                               !- Unit Internal Static Air Pressure Drop {Pa}
-       Mixed Air Node 1,               !- Air Inlet Node Name
-       Main Cooling Coil 1 Outlet Node,   !- Air Outlet Node Name
-       VarSpeedCoolCapFT,             !- Total Cooling Capacity Function of Temperature Curve Name
-       PackagedRatedCoolCapFFlow,   !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       VarSpeedCoolEIRFT,             !- Energy Input Ratio Function of Temperature Curve Name
-       PackagedRatedCoolEIRFFlow,   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       VarSpeedCyclingPLFFPLR,   !- Part Load Fraction Correlation Curve Name
-       autosize,                               !- Rated Low Speed Total Cooling Capacity {W}
-       0.69,                                       !- Rated Low Speed Sensible Heat Ratio
-       4.2,                                         !- Rated Low Speed COP
-       autosize,                               !- Rated Low Speed Air Flow Rate {m3/s}
-       VarSpeedCoolCapLSFT,         !- Low Speed Total Cooling Capacity Function of Temperature Curve Name
-       VarSpeedCoolEIRLSFT,         !- Low Speed Energy Input Ratio Function of Temperature Curve Name
-       Main Cooling Coil 1 Condenser Node;   !- Condenser Air Inlet Node Name
-
-
-   Coil:Cooling:DX:TwoSpeed,
-       Main Cooling Coil 1,         !- Name
-       CoolingCoilAvailSched,     !- Availability Schedule Name
-       autosize,                               !- High Speed Rated Total Cooling Capacity {W}
-       0.68,                                       !- High Speed Rated Sensible Heat Ratio
-       3.0,                                         !- High Speed Rated Cooling COP
-       autosize,                               !- High Speed Rated Air Flow Rate {m3/s}
-       ,                                               !- Unit Internal Static Air Pressure Drop {Pa}
-       Mixed Air Node 1,               !- Air Inlet Node Name
-       Main Cooling Coil 1 Outlet Node,   !- Air Outlet Node Name
-       VarSpeedCoolCapFT,             !- Total Cooling Capacity Function of Temperature Curve Name
-       PackagedRatedCoolCapFFlow,   !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       VarSpeedCoolEIRFT,             !- Energy Input Ratio Function of Temperature Curve Name
-       PackagedRatedCoolEIRFFlow,   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       VarSpeedCyclingPLFFPLR,   !- Part Load Fraction Correlation Curve Name
-       autosize,                               !- Low Speed Rated Total Cooling Capacity {W}
-       0.69,                                       !- Low Speed Rated Sensible Heat Ratio
-       4.2,                                         !- Low Speed Rated Cooling COP
-       autosize,                               !- Low Speed Rated Air Flow Rate {m3/s}
-       VarSpeedCoolCapLSFT,         !- Low Speed Total Cooling Capacity Function of Temperature Curve Name
-       VarSpeedCoolEIRLSFT,         !- Low Speed Energy Input Ratio Function of Temperature Curve Name
-       Main Cooling Coil 1 Condenser Node;   !- Condenser Air Inlet Node Name
-       ,                                               !- Condenser Type
-       ,                                               !- High Speed Evaporative Condenser Effectiveness {dimensionless}
-       ,                                               !- High Speed Evaporative Condenser Air Flow Rate {m3/s}
-       ,                                               !- High Speed Evaporative Condenser Pump Rated Power Consumption {W}
-       ,                                               !- Low Speed Evaporative Condenser Effectiveness {dimensionless}
-       ,                                               !- Low Speed Evaporative Condenser Air Flow Rate {m3/s}
-       ,                                               !- Low Speed Evaporative Condenser Pump Rated Power Consumption {W}
-       ,                                               !- Supply Water Storage Tank Name
-       ,                                               !- Condensate Collection Water Storage Tank Name
-       ,                                               !- Basin Heater Capacity {W/K}
-       ,                                               !- Basin Heater Setpoint Temperature {C}
-       ,                                               !- Basin Heater Operating Schedule Name
-       DOAS DX Coil SHR-FT,         !- High Speed Sensible Heat Ratio Function of Temperature Curve Name
-       DOAS DX Coil SHR-FF,         !- High Speed Sensible Heat Ratio Function of Flow Fraction Curve Name
-       DOAS DX Coil SHR-FT,         !- Low Speed Sensible Heat Ratio Function of Temperature Curve Name
-       DOAS DX Coil SHR-FF;         !- Low Speed Sensible Heat Ratio Function of Flow Fraction Curve Name
-
-
-Curve:Quadratic,
-   DOAS DX Coil SHR-FF,                                                                         !- Name
-   0.9317,                                                                                                   !- Coefficient1 Constant
-  -0.0077,                                                                                                   !- Coefficient2 x
-   0.0760,                                                                                                   !- Coefficient3 x**2
-   0.69,                                                                                                       !- Minimum Value of x
-   1.30;                                                                                                       !- Maximum Value of x
-
-
-Curve:Biquadratic,
-   DOAS DX Coil SHR-FT,                                                                         !- Name
-   1.3294540786,                                                                                       !- Coefficient1 Constant
-   -0.0990649255,                                                                                     !- Coefficient2 x
-   0.0008310043,                                                                                       !- Coefficient3 x**2
-   0.0652277735,                                                                                       !- Coefficient4 y
-   -0.0000793358,                                                                                     !- Coefficient5 y**2
-   -0.0005874422,                                                                                     !- Coefficient6 x*y
-   24.44,                                                                                                     !- Minimum Value of x
-   26.67,                                                                                                     !- Maximum Value of x
-   29.44,                                                                                                     !- Minimum Value of y
-   46.1,                                                                                                       !- Maximum Value of y
-   0.6661,                                                                                                   !- Minimum Curve Output
-   1.6009,                                                                                                   !- Maximum Curve Output
-   Temperature,                                                                                         !- Input Unit Type for X
-   Temperature,                                                                                         !- Input Unit Type for Y
-   Dimensionless;                                                                                     !- Output Unit Type
-```
-
-
-
-### Coil:Cooling:DX:TwoStageWithHumidityControlMode
-
-The multimode DX coil is functionally equivalent to Coil:Cooling:DX:SingleSpeed but with multiple performance modes. It is capable of modeling two-stage DX units and units with an enhanced dehumidification mode such as coil bypass or subcool reheat. This object contains one-time specifications for the DX unit such as node names and crankcase heater specifications. It references one or more CoilPerformance:DX:Cooling objects which define the performance for each mode of operation. It can have up to 4 performance modes to accommodate a 2-stage 2-mode unit.
-
-The multimode DX coil can be used only as a component of CoilSystem:Cooling:DX or AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass (parent object). These parent objects pass a load and dehumidification mode to this coil. If the coil has 2 capacity stages, the multimode coil model determines the stage sequencing.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a DX cooling coil. Any reference to this DX coil by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the DX cooling coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during a given time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node from which the DX cooling coil draws its inlet air.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node to which the DX cooling coil sends its outlet air.
-
-#### Field: Crankcase Heater Capacity
-
-This numeric field defines the crankcase heater capacity in Watts. When the outdoor air dry-bulb temperature is below the value specified in the input field    Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation    (described below), the crankcase heater is enabled during the time that the compressor is not running. If this cooling coil is used as part of an air-to-air heat pump (Ref. AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass), the crankcase heater defined for this DX cooling coil is ignored and the crankcase heater power defined for the DX heating coil (Ref. Coil:Heating:DX:SingleSpeed) is enabled during the time that the compressor is not running for either heating or cooling. The value for this input field must be greater than or equal to 0, and the default value is 0. To simulate a DX cooling coil without a crankcase heater, enter a value of 0.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which the compressor   s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 &deg;C, and the default value is 10 &deg;C.
-
-#### Field: Number of Capacity Stages
-
-This integer field defines the number of capacity stages. The value for this input field must be either 1 or 2, and the default value is 1. Larger DX units often have two capacity stages, which are often two completely independent compressor/coil circuits with the evaporator coils arranged in parallel in the supply air stream. 2-stage operation affects cycling losses and latent degradation due to re-evaporation of moisture with continuous fan operation.
-
-#### Field: Number of Enhanced Dehumidification Modes
-
-This integer field defines the number of enhanced dehumidification modes available. The value for this input field must be 0 or 1, and the default value is 0. If the DX unit can switch operating modes to increase dehumidification based on a humidistat signal, then set this to 1. This field just specified the availability of enhanced dehumidification. Actual control of the operating mode is handled by the coil's parent component.
-
-#### Field: Normal Mode Stage 1 Coil Performance Object Type
-
-#### Field: Normal Mode Stage 1 Coil Performance Object Name
-
-This pair of fields specifies the object type and name for the coil performance object which specifies the DX coil performance for stage 1 operation without enhanced dehumidification (normal mode). The only valid performance object type is CoilPerformance:DX:Cooling.
-
-#### Field: Normal Mode Stage 1+2 Coil Performance Object Type
-
-#### Field: Normal Mode Stage 1+2 Coil Performance Object Name
-
-This pair of fields specifies the object type and name for the coil performance object which specifies the DX coil performance for stage 1+2 operation (both stages active) without enhanced dehumidification (normal mode). The only valid performance object type is CoilPerformance:DX:Cooling.
-
-#### Field: Dehumidification Mode 1 Stage 1 Coil Performance Object Type
-
-#### Field: Dehumidification Mode 1 Stage 1 Coil Performance Object Name
-
-This pair of fields specifies the object type and name for the coil performance object which specifies the DX coil performance for stage 1 operation with enhanced dehumidification active. The only valid performance object type is CoilPerformance:DX:Cooling.
-
-#### Field: Dehumidification Mode 1 Stage 1+2 Coil Performance Object Type
-
-#### Field: Dehumidification Mode 1 Stage 1+2 Coil Performance Object Name
-
-This pair of fields specifies the object type and name for the coil performance object which specifies the DX coil performance for stage 1+2 operation (both stages active) with enhanced dehumidification active. The only valid performance object type is CoilPerformance:DX:Cooling.
-
-#### Field: Supply Water Storage Tank Name
-
-This field is optional. It is used to describe where the coil obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the coil will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains (referred to as StarvedWater).
-
-#### Field: Condensate Collection Water Storage Tank Name
-
-This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the DX coil   s electric evaporative cooler basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the DX coil is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the DX coil is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the DX coil is off.
-
-Following is an example IDF use of the object:
-
-```idf
-Coil:Cooling:DX:TwoStageWithHumidityControlMode,
-   DOAS Cooling Coil,                          !- Name
-   HVACTemplate-Always 1,                      !- Availability Schedule Name
-   DOAS Supply Fan Outlet,                     !- Air Inlet Node Name
-   DOAS Cooling Coil Outlet,                   !- Air Outlet Node Name
-   ,                                           !- Crankcase Heater Capacity
-   ,                                           !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater
-   2,                                          !- Number of Capacity Stages
-   1,                                          !- Number of Enhanced Dehumidification Modes
-   CoilPerformance:DX:Cooling,                 !- Normal Mode Stage 1 Coil Performance Object Type
-   DOAS Standard Perf 1,                       !- Normal Mode Stage 1 Coil Performance Name
-   CoilPerformance:DX:Cooling,                 !- Normal Mode Stage 1+2 Coil Performance Object Type
-   DOAS Standard Perf 1+2,                     !- Normal Mode Stage 1+2 Coil Performance Name
-   CoilPerformance:DX:Cooling,                 !- Dehumidification Mode 1 Stage 1 Coil Performance Object Type
-   DOAS Dehumid Perf 1,                        !- Dehumidification Mode 1 Stage 1 Coil Performance Name
-   CoilPerformance:DX:Cooling,                 !- Dehumidification Mode 1 Stage 1+2 Coil Performance Object Type
-   DOAS Dehumid Perf 1+2;                      !- Dehumidification Mode 1 Stage 1+2 Coil Performance Name
-```
-
-### Coil:Cooling:DX:MultiSpeed
-
-This component models a DX cooling unit with multiple discrete levels of cooling capacity. Depending on input choices, the user can model a single compressor with multiple operating speeds, or a unit with a single cooling coil fed by multiple compressors (e.g., row split or intertwined coil circuiting). Currently, this cooling coil can only be referenced by a AirLoopHVAC:UnitaryHeatPump:AirToAir:Multispeed object. Refer to Coil:Cooling:DX:TwoStageWithHumidityControlMode if the user wishes to model a cooling coil with discrete levels of cooling and the possibility of air bypass during low speed operation (e.g. face-split coil circuiting), or if cooling coil operation based on dehumidification requirements is desired.
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-The multispeed DX cooling coil can have from two to four operating speeds. When the coil operates at Speed 1 (the lowest speed), its performance is very similar to the single speed DX coil where the impacts of part-load ratio and latent capacity degradation can be included. When the coil operates at higher speeds (above Speed 1), the linear approximation methodology is applied. The coil outputs at two consecutive speeds are linearly interpolated to meet the required cooling capacity during an HVAC system timestep. When the coil performs above the lowest speed, the user can chose if they want to include part-load ratio and latent capacity degradation impacts at the higher speeds.
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-The multispeed unit is described by specifying the performance at different operating speeds. Each speed has its own set of input specifications: full load capacity, SHR, COP and air flow rate at rated conditions, along with modifier curves to determine performance when actual operating conditions are different from the rated conditions.
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-The coil operates to meet the sensible capacity being requested. When this requested capacity is above the sensible capacity of the highest operating speed, the coil runs continuously at the highest speed. When the requested capacity is between the sensible capacities of two consecutive speeds, the unit will operate a portion of the time at each speed to meet the request. When the requested capacity is less than the low speed (Speed 1) capacity, the unit will cycle on/off as needed.
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-#### Field: Name
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-A unique user-assigned name for an instance of a multispeed DX cooling coil. Any reference to this DX coil by another object will use this name.
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-#### Field: Availability Schedule Name
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-The name of the schedule (ref: Schedule) that denotes whether the DX cooling coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
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-#### Field: Air Inlet Node Name
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-The name of the HVAC system node from which the DX cooling coil draws its inlet air.
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-#### Field: Air Outlet Node Name
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-The name of the HVAC system node to which the DX cooling coil sends its outlet air.
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-#### Field: Condenser Air Inlet Node Name
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-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
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-#### Field: Condenser Type
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-The type of condenser used by the multispeed DX cooling coil. Valid choices for this input field are AirCooled or EvaporativelyCooled. The default for this field is AirCooled.
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-#### Field: Supply Water Storage Tank Name
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-This field is optional. It is used to describe where the coil obtains water used for evaporative cooling. If blank or omitted, then the evaporative cooler will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the coil will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains (referred to as StarvedWater).
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-#### Field: Condensate Collection Water Storage Tank Name
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-This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
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-#### Field: Apply Part Load Fraction to Speeds Greater than 1
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-This field determines whether part-load impacts on coil energy use are applied when the coil is operating at speeds greater than speed 1. The allowed choices are Yes or No, with the default being No if this field is left blank. Other input fields in this object allow the user to specify a part-load fraction correlation for each speed to account for compressor start up losses (cycle on/off). For the case of a single multi-speed compressor, the part load losses may only be significant when the compressor cycles between speed 1 and off, but the losses may be extremely small when the compressor operates between speed 1 and speed 2 (or between speeds 2 and 3, etc.). In this case, the user may chose to specify NO for this input field to neglect part-load impacts on energy use at higher operating speeds. If part-load impacts on coil energy use are thought to be significant (e.g., interwined cooling coil with multiple compressors feeding individual refrigerant circuits), then the user may chose to specify YES and the part-load fraction correlations specified for speeds 2 through 4 will be applied as appropriate. The selection for this input field does not affect part-load impacts when the compressor cycles between speed 1 and off   (i.e., the part-load fraction correlation for speed 1 is always applied).
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-#### Field: Apply Latent Degradation to Speeds Greater than 1
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-This field determines whether latent capacity degradation is applied when the coil is operating at speeds greater than speed 1. The allowed choices are Yes or No, with the default being No if this field is left blank. Other input fields in this object allow the user to specify latent capacity degradation at each speed.
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-The latent capacity degradation model only applies when the ContinuousFanWithCyclingCompressor supply air fan operating mode is specified, to account for moisture evaporation from the wet cooling coil when the compressor cycles off but the supply air fan continues to operate. For the case of a single multi-speed compressor, latent capacity degradation may only be significant when the compressor cycles between speed 1 and off, but the losses may be extremely small when the compressor operates between speed 1 and speed 2 (or between speeds 2 and 3, etc.). In this case, the user may chose to specify NO for this input field to neglect latent capacity degradation impacts at higher operating speeds. If latent capacity degradation is thought to be significant (e.g., interwined or row-split cooling coil with multiple compressors feeding individual refrigerant circuits), then the user may chose to specify YES and the latent capacity degradation model will be applied for speeds 2 through 4 as appropriate. The selection for this input field does not affect latent capacity degradation between speed 1 and off.
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-#### Field: Crankcase Heater Capacity
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-This numeric field defines the crankcase heater capacity in Watts. When the outdoor air dry-bulb temperature is below the value specified in the input field    Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation    (described below), the crankcase heater is enabled during the time that the compressor is not running. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0. To simulate a unit without a crankcase heater, enter a value of 0.
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-#### Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation
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-This numeric field defines the outdoor air dry-bulb temperature above which the compressor   s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 &deg;C. If this input field is left blank, the default value is 10 &deg;C.
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-#### Field: Basin Heater Capacity
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-This numeric field contains the capacity of the DX coil   s electric evaporative cooler basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the DX coil is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
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-#### Field: Basin Heater Setpoint Temperature
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-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the DX coil is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
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-#### Field: Basin Heater Operating Schedule Name
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-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the DX coil is off.
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-#### Field: Fuel Type
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-This alpha field determines the type of fuel that this cooling coil uses.   This field has seven choices: Electricity, NaturalGas, PropaneGas, Coal, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1 and OtherFuel2. The default is NaturalGas.
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-#### Field: Number of Speeds
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-This field specifies the number of sets of data being entered for rated specifications, performance curves, evaporative condenser data, latent degradation data, and waste heat specifications for each cooling speed. The rated specifications consist of gross rated capacity, gross rated SHR, gross rated COP, and rated air flow rate. The performance curves consist of a total capacity modifier curve as a function of temperature, total capacity modifier curve as a function of flow fraction, energy input ratio modifier curve as a function of temperature, energy input ratio modifier curve as a function of flow fraction, and part load fraction correlation as a function of part load ratio. The evaporative condenser data consists of effectiveness, condenser air volume flow rate, and rated pump power consumption. The latent degradation data consists of nominal time for condensate removal to begin, ratio of initial moisture evaporation rate and steady-state latent capacity, maximum On/Off cycling rate, and latent capacity time constant. The latent degradation data are only applied if the supply air fan operation mode is specified as ContinuousFanWithCyclingCompressor. The waste heat specifications include the fraction of energy input to the cooling coil at the fully loaded and rated conditions, and a temperature modifier. The minimum number of speeds for cooling is 2 and the maximum number is 4. The number of speeds should be the same as the number of speeds for cooling defined in its parent object (AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed). The first set of performance inputs is for Speed 1 and should be for low speed, and the last set of performance inputs should be for high speed. For example, if only three cooling speeds are defined, the first set should be for low speed (Speed 1), the second set should be for medium speed (Speed 2), and the third set should be for high speed (Speed 3). In this example, any performance inputs for Speed 4 would be neglected (since this input field specifies that the coil only has three cooling speeds).
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-#### Field Group: Rated Specification, Performance Curves, Latent Capacity Degradation Inputs, and Evaporative Cooled Condenser Data
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-The performance for each cooling speed must be specified as shown below. All inputs for Speed 1 are required first, followed by the inputs for Speed 2, Speed 3 and Speed 4.
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-#### Field: Speed &lt;x&gt; Gross Rated Total Cooling Capacity
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-The total, full load gross cooling capacity (sensible plus latent) in watts of the DX coil unit for Speed &lt;x&gt; operation at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb[[3]](#_ftn3), and a cooling coil air flow rate defined by field    Rated Air Flow Rate, Speed &lt;x&gt;    below). Capacity should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for).
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-#### Field: Speed &lt;x&gt; Gross Rated Sensible Heat Ratio
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-The sensible heat ratio (SHR= gross sensible capacity divided by gross total cooling capacity) of the DX cooling coil for Speed &lt;x&gt; operation at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and a cooling coil air flow rate defined by field    Rated Air Flow Rate, Speed &lt;x&gt;    below). Both the sensible and total cooling capacities used to define the Rated SHR should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for).
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-#### Field: Speed &lt;x&gt; Gross Rated Cooling COP
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-The coefficient of performance is the ratio of the gross total cooling capacity in watts to electrical power input in watts) of the DX cooling coil unit for Speed &lt;x&gt; operation at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and a cooling coil air flow rate defined by field    Rated Air Flow Rate, Speed &lt;x&gt;    below). The input power includes power for the compressor(s) and condenser fan(s) but does not include the power consumption of the supply air fan. The gross COP should NOT account for the supply air fan. If this input field is left blank, the default value is 3.0.
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-#### Field: Speed &lt;x&gt; Rated Air Flow Rate
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-The volumetric air flow rate for Speed &lt;x&gt;, in m<sup>3</sup> per second, across the DX cooling coil at rated conditions. The rated air volume flow rate for Speed &lt;x&gt; should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of the gross rated total cooling capacity for Speed &lt;x&gt;. The gross rated total cooling capacity, gross rated SHR and gross rated COP for Speed &lt;x&gt; should be performance information for the unit with air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and the rated air volume flow rate defined here.
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-#### Field: Speed &lt;X&gt; Rated Evaporator Fan Power Per Volume Flow Rate
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-This field is the electric power for the evaporator (cooling coil) fan per air volume flow rate through the coil at the rated conditions for Speed &lt;x&gt; in W/(m3/s). The default value is 773.3 W/(m3/s) (365 W/1000 cfm) if this field is left blank. If a value is entered, it must be &gt;= 0.0 and &lt;= 1250 W/(m3/s). This value is only used to calculate Seasonal Energy Efficiency Ratio (SEER), and the Standard Rating (Net) Cooling Capacity which will be outputs in the EnergyPlus eio file (ref. EnergyPlus Engineering Reference, Multi-Speed DX Cooling Coil, Standard Ratings). This value is not used for modeling the evaporator (cooling coil) fan during simulations; instead, it is used for calculating SEER and Standard Rating Cooling Capacity to assist the user in verifying their inputs for modeling this type of equipment.
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-#### Field: Speed &lt;x&gt; Total Cooling Capacity Function of Temperature Curve Name
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-The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity for Speed &lt;x&gt; as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity for Speed &lt;x&gt; to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to have the value of 1.0 at the rating point.
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-#### Field: Speed &lt;x&gt; Total Cooling Capacity Function of Flow Fraction Curve Name
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-The name of a quadratic performance curve (ref:   Performance Curves) that parameterizes the variation of the gross total cooling capacity for Speed &lt;x&gt; as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate for Speed &lt;x&gt; (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity for Speed &lt;x&gt; at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate for Speed &lt;x&gt;.
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-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Temperature Curve Name
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-The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) for Speed &lt;x&gt; as a function of the wetbulb temperature of the air entering the cooling coil and the drybulb temperature of the air entering the air-cooled condenser (wetbulb temperature if modeling an evaporative-cooled condenser). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR for Speed &lt;x&gt; (inverse of rated COP for Speed &lt;x&gt;) to give the EIR for Speed &lt;x&gt; at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to a value of 1.0 at the rating point.
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-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Flow Fraction Curve Name
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-The name of a quadratic performance curve (Ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) for Speed &lt;x&gt; as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate for Speed &lt;x&gt; (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR for Speed &lt;x&gt; at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate for Speed &lt;x&gt;.
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-#### Field: Speed &lt;x&gt; Part Load Fraction Correlation Curve Name
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-This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity for Speed &lt;x&gt;). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the    effective    EIR for a given simulation timestep for Speed &lt;x&gt;. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
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-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
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-           PLF &gt;= 0.7     and     PLF &gt;= PLR
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-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
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-A typical part load fraction correlation for a conventional DX cooling coil (Speed &lt;x&gt;) would be:
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-           PLF = 0.85 + 0.15(PLR)
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-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
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-           PLF = 1.0 + 0.0(PLR)
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-#### Field: Speed &lt;x&gt; Nominal Time for Condensate Removal to Begin
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-For Speed &lt;x&gt;, the nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]), and this field as well as the next three input fields for this object must have positive values in order to model latent capacity degradation for Speed &lt;x&gt;.
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-#### Field: Speed &lt;x&gt; Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity
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-For Speed &lt;x&gt;, the ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) for Speed &lt;x&gt; at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]); and this field, the previous field and the next two fields must have positive values in order to model latent capacity degradation for Speed &lt;x&gt;.
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-#### Field: Speed &lt;x&gt; Maximum Cycling Rate
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-For Speed &lt;x&gt;, the maximum on-off cycling rate for the compressor (cycles per hour), which occurs at 50% run time fraction. Suggested value is 3; zero value means latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]); and this field, the previous two fields and the next field must have positive values in order to model latent capacity degradation for Speed &lt;x&gt;.
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-#### Field: Speed &lt;x&gt; Latent Capacity Time Constant
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-For Speed &lt;x&gt;, the time constant (in seconds) for the cooling coil's latent capacity to reach steady state after startup. Suggested value is 45; zero value means latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]), and this field as well as the previous three input fields for this object must have positive values in order to model latent capacity degradation for Speed &lt;x&gt;.
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-#### Field: Speed &lt;x&gt; Rated Waste Heat Fraction of Power Input
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-The fraction of energy input to the cooling coil that is available as recoverable waste heat at full load and rated conditions for Speed &lt;x&gt;.
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-#### Field: Speed &lt;x&gt; Waste Heat Function of Temperature Curve Name
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-The name of a biquadratic performance curve (ref: Performance Curves) that parameterizes the variation of the waste heat recovery as a function of outdoor dry-bulb temperature and the entering coil dry-bulb temperature at Speed &lt;x&gt;. The output of this curve is multiplied by the rated waste heat fraction at specific temperature operating conditions (i.e., at temperatures different from the rating point). The curve is normalized to a value of 1.0 at the rating point. When the fuel type is electricity, this field can remain blank since it is ignored by the program in this instance. When the fuel type is not electricity and the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed does not require waste heat calculations, this field is ignored. If the field is blank, a warning will be issued and simulation continues. When the fuel type is not electricity and the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed requires waste heat calculations, if this field is left blank, the program assumes a constant value of 1 to make simulation continue and a warning will be issued.   
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-#### Field: Speed &lt;x&gt; Evaporative Condenser Effectiveness
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-The effectiveness of the evaporative condenser at Speed &lt;x&gt;, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
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-<div>\[Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectivenes{s_{Speed1}}} \right)\left( {Tdb,o\,\, - Twb,o} \right)\]</div>
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-where
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-*T<sub>cond\\ inlet</sub>* = the temperature of the air entering the condenser coil (C)
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-*T<sub>wb,o</sub>* = the wet-bulb temperature of the outdoor air (C)
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-*T<sub>db,o</sub>* = the dry-bulb temperature of the outdoor air (C)
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-The resulting condenser inlet air temperature is used by the Total Cooling Capacity Modifier Curve, Speed &lt;x&gt; (function of temperature) and the Energy Input Ratio Modifier Curve, Speed &lt;x&gt; (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled.
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-If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve, Speed &lt;x&gt; (function of temperature) and the Energy Input Ratio Modifier Curve, Speed &lt;x&gt; (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
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-If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve, Speed &lt;x&gt; (function of temperature) and the Energy Input Ratio Modifier Curve, Speed &lt;x&gt; (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
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-If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve, Speed &lt;x&gt; (function of temperature) and the Energy Input Ratio Modifier Curve, Speed &lt;x&gt; (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves for Speed &lt;x&gt; must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
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-#### Field: Speed &lt;x&gt; Evaporative Condenser Air Flow Rate
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-The air volume flow rate, in m<sup>3</sup> per second, entering the evaporative condenser at Speed &lt;x&gt;. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000114 m<sup>3</sup>/s per watt of rated total cooling capacity for Speed &lt;x&gt; [850 cfm/ton]). This field is not used when Condenser Type = Air Cooled.
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-#### Field: Speed &lt;x&gt; Rated Evaporative Condenser Pump Power Consumption
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-The rated power of the evaporative condenser water pump in Watts at Speed &lt;x&gt;. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt [15 W/ton] of rated total capacity for Speed &lt;x&gt;). This field is not used when Condenser Type = Air Cooled.
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-#### Field: Zone Name for Condenser Placement
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-This input field is name of a conditioned or unconditioned zone where the secondary coil (condenser) of DX system or a heat pump is to be placed.  This is an optional input field specified only when user desires to reject the condenser heat into a zone.  The heat rejected is modeled as sensible internal gain of a secondary zone.
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-Following is an example input for this multispeed DX cooling coil.
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-```idf
-Coil:Cooling:DX:MultiSpeed,
-       Heat Pump ACDXCoil 1,       !- Coil Name
-       FanAndCoilAvailSched,       !- Availability Schedule
-       DX Cooling Coil Air Inlet Node,   !- Coil Air Inlet Node
-       Heating Coil Air Inlet Node,         !- Coil Air Outlet Node
-       Outdoor Condenser Air Node,           !- Condenser Air Inlet Node Name
-       AirCooled,                           !- Condenser Type
-       ,                                               !- Name of Water Storage Tank for Supply
-       ,                                               !- Name of Water Storage Tank for Condensate Collection
-       No,                                           !- Apply Part Load Fraction to Speeds greater than 1
-       No,                                           !- Apply latent degradation to Speeds greater than 1
-       200.0,                                     !- Crankcase Heater Capacity {W}
-       10.0,                                       !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation
-       ,                                               !- Basin Heater Capacity {W/K}
-       ,                                               !- Basin Heater Setpoint Temperature {C}
-       ,                                               !- Basin Heater Operating Schedule Name
-       NaturalGas,                           !- Fuel Type
-       4,                                             !- Number of speeds
-       7500,                                       !- Gross Rated Total Cooling Capacity, Speed 1 {W}
-       0.75,                                       !- Gross Rated Sensible Heat Ratio, Speed 1 {dimensionless}
-       3.0,                                         !- Gross Rated Cooling COP, Speed 1 {dimensionless}
-       0.40,                                       !- Rated Air Flow Rate, Speed 1 {m3/s}
-       ,                                               !- Rated Evaporator Fan Power Per Volume Flow Rate, Speed 1 {W/(m3/s)}
-       HPACCoolCapFT Speed 1,     !- Total Cooling Capacity Modifier Curve, Speed 1 (temperature)
-       HPACCoolCapFF Speed 1,     !- Total Cooling Capacity Modifier Curve, Speed 1 (flow fraction)
-       HPACCOOLEIRFT Speed 1,     !- Energy Input Ratio Modifier Curve, Speed 1 (temperature)
-       HPACCOOLEIRFF Speed 1,     !- Energy Input Ratio Modifier Curve, Speed 1 (flow fraction)
-       HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 1 (part load ratio)
-       1000.0,                                   !- Nominal Time for Condensate Removal to Begin, Speed 1 {s}
-       1.5,                                         !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent
-       3.0,                                         !- Maximum ON/OFF Cycling Rate, Speed 1 {cycles/hr}
-       45.0,                                       !- Latent Capacity Time Constant, Speed 1 {s}
-       0.2,                                         !- Rated waste heat fraction of power input, Speed 1 {dimensionless}
-       HAPCCoolWHFT Speed 1,       !- Waste heat modifier curve, Speed 1 (temperature)
-       0.9,                                         !- Evaporative Condenser Effectiveness, Speed 1 {dimensionless}
-       0.05,                                       !- Evaporative Condenser Air Volume Flow Rate, Speed 1 {m3/s}
-       50,                                           !- Evaporative Condenser Pump Rated Power Consumption, Speed 1 {W}
-       17500,                                     !- Gross Rated Total Cooling Capacity, Speed 2 {W}
-       0.75,                                       !- Gross Rated Sensible Heat Ratio, Speed 2 {dimensionless}
-       3.0,                                         !- Gross Rated Cooling COP, Speed 2 {dimensionless}
-       0.85,                                       !- Rated Air Flow Rate, Speed 2 {m3/s}
-       ,                                               !- Rated Evaporator Fan Power Per Volume Flow Rate, Speed 2 {W/(m3/s)}
-       HPACCoolCapFT Speed 2,     !- Total Cooling Capacity Modifier Curve, Speed 2 (temperature)
-       HPACCoolCapFF Speed 2,     !- Total Cooling Capacity Modifier Curve, Speed 2 (flow fraction)
-       HPACCOOLEIRFT Speed 2,     !- Energy Input Ratio Modifier Curve, Speed 2 (temperature)
-       HPACCOOLEIRFF Speed 2,     !- Energy Input Ratio Modifier Curve, Speed 2 (flow fraction)
-       HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 2 (part load ratio)
-       1000.0,                                   !- Nominal Time for Condensate Removal to Begin, Speed 2
-       1.5,                                         !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent
-       3.0,                                         !- Maximum ON/OFF Cycling Rate, Speed 2
-       45.0,                                       !- Latent Capacity Time Constant, Speed 2
-       0.2,                                         !- Rated waste heat fraction of power input, Speed 2 {dimensionless}
-       HAPCCoolWHFT Speed 2,       !- Waste heat modifier curve, Speed 2 (temperature)
-       0.9,                                         !- Evaporative Condenser Effectiveness, Speed 2 {dimensionless}
-       0.1,                                         !- Evaporative Condenser Air Volume Flow Rate, Speed 2 {m3/s}
-       60,                                           !- Evaporative Condenser Pump Rated Power Consumption, Speed 2 {W}
-       25500,                                     !- Gross Rated Total Cooling Capacity, Speed 3 {W}
-       0.75,                                       !- Gross Rated Sensible Heat Ratio, Speed 3 {dimensionless}
-       3.0,                                         !- Gross Rated Cooling COP, Speed 3 {dimensionless}
-       1.25,                                       !- Rated Air Flow Rate, Speed 3 {m3/s}
-       ,                                               !- Rated Evaporator Fan Power Per Volume Flow Rate, Speed 3 {W/(m3/s)}
-       HPACCoolCapFT Speed 3,     !- Total Cooling Capacity Modifier Curve, Speed 3 (temperature)
-       HPACCoolCapFF Speed 3,     !- Total Cooling Capacity Modifier Curve, Speed 3 (flow fraction)
-       HPACCOOLEIRFT Speed 3,     !- Energy Input Ratio Modifier Curve, Speed 3 (temperature)
-       HPACCOOLEIRFF Speed 3,     !- Energy Input Ratio Modifier Curve, Speed 3 (flow fraction)
-       HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 3 (part load ratio)
-       1000.0,                                   !- Nominal Time for Condensate Removal to Begin, Speed 3 {s}
-       1.5,                                         !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent
-       3.0,                                         !- Maximum ON/OFF Cycling Rate, Speed 3 {cycles/hr}
-       45.0,                                       !- Latent Capacity Time Constant, Speed 3 {s}
-       0.2,                                         !- Rated waste heat fraction of power input, Speed 3 {dimensionless}
-       HAPCCoolWHFT Speed 3,       !- Waste heat modifier curve, Speed 3 (temperature)
-       0.9,                                         !- Evaporative Condenser Effectiveness, Speed 3 {dimensionless}
-       0.2,                                         !- Evaporative Condenser Air Volume Flow Rate, Speed 3 {m3/s}
-       80,                                           !- Evaporative Condenser Pump Rated Power Consumption, Speed 3 {W}
-       35500,                                     !- Gross Rated Total Cooling Capacity, Speed 4 {W}
-       0.75,                                       !- Gross Rated Sensible Heat Ratio, Speed 4 {dimensionless}
-       3.0,                                         !- Gross Rated Cooling COP, Speed 4 {dimensionless}
-       1.75,                                       !- Rated Air Flow Rate, Speed 4 {m3/s}
-       ,                                               !- Rated Evaporator Fan Power Per Volume Flow Rate, Speed 4 {W/(m3/s)}
-       HPACCoolCapFT Speed 4,     !- Total Cooling Capacity Modifier Curve, Speed 4 (temperature)
-       HPACCoolCapFF Speed 4,     !- Total Cooling Capacity Modifier Curve, Speed 4 (flow fraction)
-       HPACCOOLEIRFT Speed 4,     !- Energy Input Ratio Modifier Curve, Speed 4 (temperature)
-       HPACCOOLEIRFF Speed 4,     !- Energy Input Ratio Modifier Curve, Speed 4 (flow fraction)
-       HPACCOOLPLFFPLR Speed 1, !- Part Load Fraction Correlation, Speed 4 (part load ratio)
-       1000.0,                                   !- Nominal Time for Condensate Removal to Begin, Speed 4 {s}
-       1.5,                                         !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent                                                     !- Capacity, Speed 4 {dimensionless}
-       3.0,                                         !- Maximum ON/OFF Cycling Rate, Speed 4 {cycles/hr}
-       45.0,                                       !- Latent Capacity Time Constant, Speed 4 {s}
-       0.2,                                         !- Rated waste heat fraction of power input, Speed 4 {dimensionless}
-       HAPCCoolWHFT Speed 4,       !- Waste heat modifier curve, Speed 4 (temperature)
-       0.9,                                         !- Evaporative Condenser Effectiveness, Speed 4 {dimensionless}
-       0.3,                                         !- Evaporative Condenser Air Volume Flow Rate, Speed 4 {m3/s}
-       100;                                         !- Evaporative Condenser Pump Rated Power Consumption, Speed 4 {W}
-```
-
-### DX Cooling Coil Outputs
-
-* HVAC,Average,Cooling Coil Total Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Total Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Latent Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Latent Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Electric Power[W]
-
-* HVAC,Sum,Cooling Coil Electric Energy [J]
-
-* HVAC,Average,Cooling Coil Runtime Fraction []
-
-
-
-If not part of AirLoopHVAC:UnitaryHeatPump:AirToAir (if part of a heat pump, crankcase heater is reported only for the heating coil):
-
-* HVAC,Average,Cooling Coil Crankcase Heater Electric Power[W]
-
-* HVAC,Sum,Cooling Coil Crankcase Heater Electric Energy [J]
-
-
-
-Evaporative-cooled condenser:
-
-* HVAC,Average,Cooling Coil Condenser Inlet Temperature [C]
-
-* HVAC,Sum,Cooling Coil Evaporative Condenser Water Volume[m3]
-
-* HVAC,Average,Cooling Coil Evaporative Condenser Pump Electric Power[W]
-
-* HVAC,Sum,Cooling Coil Evaporative Condenser Pump Electric Energy [J]
-
-* HVAC,Average,Cooling Coil Basin Heater Electric Power[W]
-
-* HVAC,Sum,Cooling Coil Basin Heater Electric Energy [J]
-
-* HVAC,Sum,Cooling Coil Evaporative Condenser Mains Supply Water Volume [m3]
-
-
-
-Additional variables for Coil:Cooling:DX:TwoStageWithHumidityControlMode only:
-
-* HVAC,Average,Cooling Coil Stage 2 Runtime Fraction []
-
-* HVAC,Average,Cooling Coil Dehumidification Mode []
-
-
-
-Additional variables when condensate is collected using a storage tank:
-
-* HVAC,Average,Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-* Zone,Meter,Condensate:OnSiteWater [m3]
-
-* HVAC,Sum,Cooling Coil Condensate Volume [m3]
-
-
-
-Additional variables for Coil:Cooling:DX:Multispeed:
-
-If Fuel Type is not Electricity:
-
-* HVAC,Average,DX Cooling Coil &lt;Fuel Type&gt; Power[W]
-
-* HVAC,Sum,DX Cooling Coil &lt;Fuel Type&gt; Consumption[J]
-
-#### 
-
-#### Cooling Coil Total Cooling Rate [W]
-
-This field is the total (sensible and latent) cooling rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Total Cooling Energy [J]
-
-This is the total (sensible plus latent) cooling output of the DX coil in Joules over the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = CoolingCoils, Group Key = System (Ref. Output:Meter objects).
-
-#### Cooling Coil Sensible Cooling Rate [W]
-
-This output is the moist air sensible cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Sensible Cooling Energy [J]
-
-This is the moist air sensible cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Latent Cooling Rate [W]
-
-This is the latent cooling rate output of the DX coil in Watts. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Latent Cooling Energy [J]
-
-This is the latent cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Electric Power [W]
-
-This output is the electricity consumption rate of the DX coil compressor and condenser fan(s) in Watts. This value is calculated for each HVAC system timestep, and the results are averaged for the timestep being reported.
-
-#### Cooling Coil Electric Energy [J]
-
-This is the electricity consumption of the DX coil compressor and condenser fan(s) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (Ref. Output:Meter objects).
-
-#### Cooling Coil Runtime Fraction []
-
-This is the runtime fraction of the DX coil compressor and condenser fan(s) for the timestep being reported.
-
-#### Cooling Coil Crankcase Heater Electric Power[W]
-
-This is the average electricity consumption rate of the DX coil compressor   s crankcase heater in Watts for the timestep being reported. If the DX Cooling Coil is used in a heat pump, the crankcase heater is reported only for the heating coil.
-
-#### Cooling Coil Crankcase Heater Electric Energy [J]
-
-This is the electricity consumption of the DX coil compressor   s crankcase heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects). This output variable appears only when the DX Cooling Coil is not used as part of a heat pump, otherwise the crankcase heater is reported only for the heating coil.
-
-#### Cooling Coil Condenser Inlet Temperature [C]
-
-This is the inlet air temperature to the condenser coil in degrees C. This value can represent the outdoor air dry-bulb temperature, wet-bulb temperature, or somewhere in between from the weather data being used, depending on the value used in the input field    Evaporative Condenser Effectiveness   . The temperature reported here is used in the various modifier curves related to temperature (e.g., Total Cooling Capacity Modifier Curve [function of temperature]). This output variable appears only when the DX Cooling Coil is not used as part of a heat pump, otherwise the crankcase heater is reported only for the heating coil.
-
-#### Cooling Coil Evaporative Condenser Water Volume [m3]
-
-This output is the amount of water used to evaporatively cool the condenser coil inlet air, in cubic meters. This output is also added to a meter with Resource Type = Water, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects). This output variable appears only when the DX Cooling Coil is evaporatively cooled. 
-
-#### Cooling Coil Evaporative Condenser Mains Supply Water Volume [m3]
-
-This is the volume of water drawn from mains water service for the evaporatively cooled condenser.
-
-#### Cooling Coil Evaporative Condenser Pump Electric Power [W]
-
-This is the average electricity consumption rate of the evaporative condenser water pump in Watts for the timestep being reported. This output variable appears only when the DX Cooling Coil is evaporatively cooled. 
-
-#### Cooling Coil Evaporative Condenser Pump Electric Energy [J]
-
-This is the electricity consumption rate of the evaporative condenser water pump in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects). This output variable appears only when the DX Cooling Coil is evaporatively cooled. 
-
-#### Cooling Coil Stage 2 Runtime Fraction []
-
-This is the runtime fraction of the stage 2 DX coil compressor and condenser fan(s) for the timestep being reported. Applicable only for COIL Coil:Cooling:DX:TwoStageWithHumidityControlMode when 2 capacity stages are specified. For 2-stage systems, Cooling Coil Runtime Fraction is the stage 1 runtime fraction. These runtime fractions overlap, because stage 2 will not run unless stage 1 is already running. For example, a system where stage 1 is 60% of total capacity is passed a load of 70%. The Cooling Coil Runtime Fraction (stage 1) will be 1.0, and the Cooling Coil Stage 2 Runtime Fraction will be 0.25 [(70%-60%)/(100%-60%)].
-
-#### Cooling Coil Dehumidification Mode []
-
-This is the dehumidification mode for the timestep being reported. Applicable only for Coil:Cooling:DX:TwoStageWithHumidityControlMode when enhanced dehumidification mode is available. A value of 0 indicates normal mode (extra dehumidification not active). A value of 1 indicates dehumidification mode 1 is active. Note that this is an averaged variable, so fractional values are likely to be reported for reporting frequencies longer than "detailed".
-
-#### Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-#### Cooling Coil Condensate Volume [m3]
-
-These outputs are the rate and volume of water collected as condensate from the coil. These reports only appear if a water storage tank is named in the input object.
-
-#### Cooling Coil Evaporative Condenser Mains Supply Water Volume   [m3]
-
-This is the water consumed by the DX Cooling Coil evaporatively cooled condenser that is met by the mains water. This output variable appears only when the DX Cooling Coil is evaporatively cooled. 
-
-#### Cooling Coil Basin Heater Electric Power [W]
-
-This is the average electricity consumption rate of the basin heater in Watts for the timestep being reported. This output variable appears only when the DX Cooling Coil is evaporatively cooled and the Basin Heater Capacity is greater than 0.
-
-#### Cooling Coil Basin Heater Electric Energy [J]
-
-This is the electricity consumption rate of the basin heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects). This output variable appears only when the DX Cooling Coil is evaporatively cooled and the Basin Heater Capacity is greater than 0.
-
-#### Cooling Coil &lt;Fuel Type&gt; Power [W]
-
-This output variable appears only when using the Coil:Cooling:DX:Multispeed object and a fuel type other than electricity is used. This variable describes the input fuel type power for the cooling coil in Watts, averaged during the timestep being reported.
-
-#### Cooling Coil &lt;Fuel Type&gt; Energy [J]
-
-This output variable appears only when using the Coil:Cooling:DX:Multispeed object and a fuel type other than electricity is used. This variable describes the input fuel type consumption for the multispeed cooling coil in the unit of Joules, summed for the timestep being reported. The electric consumption is excluded..This output is added to a meter with Resource Type = &lt;Fuel Type&gt;, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
-
-Note: &lt;Fuel Type&gt; in the above two output variables depends on the user specified input for the Fuel Type field. In addition to Electricity, valid fuel types are NaturalGas, Propane, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1 and OtherFuel2.
-
-### Coil:Cooling:DX:VariableSpeed
-
-The Variable-Speed DX Cooling Coil is a collection of performance curves that represent the cooling coil at various speed levels. The performance curves should be generated from a Reference Unit data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. On the other hand, the model uses the bypass factor approach to calculate sensible heat transfer rate, similar to the one used in the single-speed DX coil. The number of speed levels can range from 1 to 10. The cooling coil has two indoor air side connections, and one optional condenser air node connection. The user needs to specify a nominal speed level, at which the gross rated total cooling capacity, and rated volumetric air rate are sized. The rated capacity and rated volumetric flow rate represent the real situation in the air loop, and are used to determine and flow rates at various speed levels in the parent objects, e.g. of AirLoopHVAC:UnitaryHeatCool, ZoneHVAC:PackagedTerminalAirConditioner, AirLoopHVAC:UnitaryHeatPump:AirToAir and ZoneHVAC:PackagedTerminalHeatPump. It shall be mentioned that the performance correction curves, i.e. the temperature and flow fraction correction curves, should be normalized to the capacity and flow rate at each individual speed and at the rated conditions, similar to the performance curves used in the single-speed DX coil. However, the performance values, e.g. capacities, COPs, SHRs and flow rates at individual speed levels, should be given regarding a specific unit from the Reference Unit catalog data. In the following content, the statement started with    Reference Unit    means the actual Reference Unit catalog data. The rated conditions for obtaining the capacities, COPs and SHRs   are at indoor dry-bulb temperature of 26.67 ËšC (80 ËšF), wet bulb temperature of 19.44 ËšC (67 ËšF),   and the condenser entering air temperature of 35 ËšC (95 ËšF). Some equations are provided below to help explain the function of the various performance curves and data fields.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the variable-speed cooling coil.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the cooling coil load side inlet node name.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the cooling coil load side outlet node name.
-
-#### Field: Number of Speeds
-
-This numeric field contains the maximum number of speed levels that the module uses. The number of speeds, for which the user input the performance data and curves, should be equal or higher than the maximum number. The performance inputs at higher speed levels are ignored.
-
-#### Field: Nominal Speed Level
-
-This numeric field defines the nominal speed level, at which the rated capacity and rated air rate are correlated.
-
-#### Field: Gross Rated Total Cooling Capacity at Selected Nominal Speed Level
-
-This numeric field contains the gross rated total cooling capacity at the nominal speed level.   This field is autosizable. The gross rated total cooling capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
-
-<div>\[{\rm{CapacityScaleFactor}} = \frac{{{\rm{Gross RatedTotalCoolingCapacity}}}}{{{\rm{ReferenceUnitCapacity}}@{\rm{NominalSpeedLevel}}}}\]</div>
-
-And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below,
-
-<div>\[\begin{array}{l}{\rm{Gross RatedCapacity}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = \\\quad \quad \quad {\rm{CapacityScaleFactor}} \times \\\quad \quad \quad {\rm{ReferenceUnitCapacity}}@{\rm{SpeedLevel}}({\rm{x}})\end{array}\]</div>
-
-#### Field: Rated Air Flow Rate at Selected Nominal Speed Level
-
-This numeric field contains the rated volumetric air flow rate on the load side of the DX unit, corresponding to the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects.   It is recommended that the ratio of the rated volumetric air flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
-
-<div>\[{\rm{AirFlowScaleFactor}} = \frac{{{\rm{RatedVolumetricAirFlowRate}}}}{{{\rm{ReferenceUnitVolAirFlowRate}}@{\rm{NominalSpeedLevel}} \times {\rm{CapacityScaleFactor}}}}\]</div>
-
-And the volumetric air flow rates in the parent objects are calculated as below,
-
-<div>\[\begin{array}{l}{\rm{LoopVolumetricAirFlowRate}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = \\\quad \quad \quad {\rm{AirFlowScaleFactor}} \times \\\quad \quad \quad {\rm{ReferenceUnitVolAirFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) \times \\\quad \quad \quad {\rm{CapacityScaleFactor}}\end{array}\]</div>
-
-#### Field: Nominal Time for Condensate Removal to Begin
-
-This numeric field defines the nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero.
-
-#### Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity
-
-This numeric field defines ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero.
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, sensible or latent load/steady-state sensible or latent cooling capacity for Speed 1), in the case that the unit operates under the lowest speed, i.e. on/off. The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the    effective    EIR for a given simulation timestep for Speed 1. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep).
-
-#### Field: Condenser Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
-
-#### Field: Condenser Type
-
-The type of condenser used by the DX cooling coil. Valid choices for this input field are AirCooled or EvaporativelyCooled. The default for this field is AirCooled.
-
-#### Field: Evaporative Condenser Pump Rated Power Consumption
-
-The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt [15 W/ton] of rated total cooling capacity). This field is not used when Condenser Type = Air Cooled.
-
-#### Field: Crankcase Heater Capacity
-
-This numeric field defines the crankcase heater capacity in Watts. When the outdoor air drybulb temperature is below the value specified in the input field    Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation    (described below), the crankcase heater is enabled during the time that the compressor is not running. If this cooling coil is used as part of an air-to-air heat pump, the crankcase heater defined for this DX cooling coil is ignored and the crankcase heater power defined for the DX heating coil (Ref. Coil:Heating:DX:SingleSpeed) is enabled during the time that the compressor is not running for either heating or cooling. The value for this input field must be greater than or equal to 0, and the default value is 0. To simulate a DX cooling coil without a crankcase heater, enter a value of 0.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which the compressor   s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 &deg;C, and the default value is 10 &deg;C.
-
-#### Field: Supply Water Storage Tank Name
-
-This field is optional. It is used to describe where the coil obtains water used for evaporative cooling of its condenser. If blank or omitted, then the unit will obtain water directly from the mains. If the name of a Water Storage Tank object is used here, the unit will obtain its water from that tank. If a tank is specified, the unit will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the condenser needs, then the unit will still operate and obtain the rest of the water it needs from the mains (referred to as StarvedWater).
-
-#### Field: Condensate Collection Water Storage Tank Name
-
-This field is optional. It is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded. Enter the name of Water Storage Tank object defined elsewhere and the condensate will then be collected in that tank.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the DX coil   s electric evaporative cooler basin
-
-heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the DX coil is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the DX coil is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the DX coil is off.
-
-#### Field Group: Rated specification, performance curves
-
-The performance for each cooling speed must be specified as shown below. They should be directly given from the Reference Unit catalog data. All inputs for Speed 1 are required, followed by the optional inputs for other speeds.
-
-#### Field: Speed &lt;x&gt; Reference Unit Gross Rated Total Cooling Capacity
-
-This numeric field defines the total, full load gross cooling capacity in watts of the air-to-air cooling coil unit at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0. Capacity should not account for supply air fan heat.
-
-#### Field: Speed &lt;x&gt; Reference Unit Gross Rated Sensible Heat Ratio
-
-This numeric field defines sensible heat transfer ratio (SHR = gross sensible cooling capacity divided by gross total cooling capacity) of the cooling coil unit at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0.0 and less than 1.0. This value should be obtained from the Reference Unit data.
-
-#### Field: Speed &lt;x&gt; Reference Unit Gross Rated Cooling COP
-
-This numeric field defines the coefficient of performance (COP= the gross total cooling capacity in watts divided by electrical power input in watts) of the cooling coil unit at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0. The input power includes power for the compressor(s), condenser fan and accessories, but does not include the supply air fan. The gross COP should Not account for the supply air fan.
-
-#### Field: Speed &lt;x&gt; Reference Unit Rated Air Flow Rate
-
-This numeric field defines the volumetric air flow rate, in m<sup>3</sup> per second, across the cooling coil at rated conditions for Speed &lt;x&gt; operation. The value entered here should be directly from the Reference Unit data, corresponding to the given cooling capacity and COP at the speed, as above.
-
-#### Field: Speed &lt;x&gt; Reference Unit Rated Condenser Air Flow Rate
-
-This numeric field defines the condenser volumetric air flow rate, in m<sup>3</sup> per second, across the condenser coil at rated conditions for Speed &lt;x&gt; operation. The value entered here should be directly from the Reference Unit data. This field is used to calculate water evaporation rate for an evaporatively-cooled condenser. For an air-cooled condenser, this input is not used.
-
-#### Field: Speed &lt;x&gt; Reference Unit Rated Pad Effectiveness of Evap Precooling
-
-This numeric field defines the effectiveness of condenser evaporative precooling pad at rated condition. The values of effectiveness are given at individual speed levels, since varied condenser air flow rates impact the effectiveness.
-
-#### Field: Speed &lt;x&gt; Total Cooling Capacity Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the both the indoor wet-bulb and source side entering air temperature, from the Reference Unit. The output of this curve is multiplied by the gross rated total cooling capacity at the speed to give the gross total cooling capacity at specific temperature operating conditions (i.e., at an indoor air wet-bulb temperature or outdoor entering air temperature different from the rating point temperature). It should be noted that the curve is normalized to the cooling capacity at Speed&lt;x&gt; from the Reference Unit data, and have the value of 1.0 at the rating point.
-
-#### Field: Speed &lt;x&gt; Total Cooling Capacity Function of Air Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of full load flow at Speed &lt;x&gt;, from the Reference Unit data). The curve is normalized to have the value of 1.0 when the actual air flow rate equals the design air flow rate, at Speed &lt;x&gt;.
-
-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor air wet-bulb and condenser entering air temperatures The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP at Speed &lt;x&gt; from the Reference Unit data) to give the EIR at specific temperature operating conditions (i.e., at an indoor air wet-bulb temperature or condenser entering air temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
-
-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Air Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of full load flow, at Speed &lt;x&gt; from the Reference Unit data). The EIR is the inverse of the COP. This curve is normalized to a value of 1.0 when the actual air flow rate equals the design air flow rate.
-
-
-
-An example of this statement in an IDF is:
-
-```idf
-  Coil:Cooling:DX:VariableSpeed,
-       Heat Pump ACDXCoil 1,                       !- Name
-       DX Cooling Coil Air Inlet Node,   !- Air Inlet Node Name
-       Heating Coil Air Inlet Node,         !- Air Outlet Node Name
-       10.0,                                     !- Number of Speeds {dimensionless}
-       10.0,                                     !- Nominal Speed Level {dimensionless}
-       32000,                                   !- Gross Rated Total Cooling Capacity {W}
-       1.7,                                       !- Rated Air Flow Rate {m3/s}
-       0.0,                                       !- Nominal Time for Condensate to Begin Leaving the Coil {s}
-       0.0,   !- Initial Moisture Evaporation Rate Divided by Steady-State AC Latent Capacity {dimensionless}
-       HPACCOOLPLFFPLR,                     !- Part Load Fraction Correlation Curve Name
-       ,                                      ! - Condenser Air Inlet Node Name
-       AirCooled,                                ! - Condenser Type
-       ,                                      ! - Evaporative Condenser Pump Rated Power Consumption
-       200.0,                                      ! - Crankcase Heater Capacity, {w}
-       10.0,                                     !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
-       ,                               ! - Supply Water Storage Tank Name
-       ,                                ! - Condensate Collection Water Storage Tank Name
-       ,                                             ! - Basin Heater Capacity
-       ,                               ! - Basin Heater Setpoint Temperature
-       ,                                             ! - Basin Heater Operating Schedule Name
-       1524.1,                                 !- Speed 1 Gross Rated Total Cooling Capacity {w}
-       0.75,                                     !- Speed 1 Gross Rated Sensible Heat Ratio {dimensionless}
-       4.0,                                       !- Speed 1 Gross Rated Cooling COP {dimensionless}
-       0.1359072,                           !- Speed 1 Rated Air Flow Rate {m3/s}
-       0.26,                                     ! - Speed 1 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
-       ,                                             ! - Evaporative precooling effectiveness
-       HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
-       HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
-       HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
-       1877.9,                                 !- Speed 2 Gross Rated Total Cooling Capacity {w}
-       0.75,                                     !- Speed 2 Gross Rated Sensible Heat Ratio {dimensionless}
-       4.0,                                       !- Speed 2 Gross Rated Cooling COP {dimensionless}
-       0.151008,                             !- Speed 2 Rated Air Flow Rate {m3/s}
-       0.30,                                     ! - Speed 2 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
-       ,                                             ! - Evaporative precooling effectiveness
-       HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
-       HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
-       HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
-       2226.6,                                 !- Speed 3 Gross Rated Total Cooling Capacity {w}
-       0.75,                                     !- Speed 3 Gross Rated Sensible Heat Ratio {dimensionless}
-       4.0,                                       !- Speed 3 Gross Rated Cooling COP {dimensionless}
-       0.1661088,                           !- Speed 3 Rated Air Flow Rate {m3/s}
-       0.33,                                     !- Speed 3 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
-       ,                                             !- Evaporative precooling effectiveness
-       HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
-       HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
-       HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
-       2911.3,                                 !- Speed 4 Gross Rated Total Cooling Capacity {w}
-       0.75,                                     !- Speed 4 Gross Rated Sensible Heat Ratio {dimensionless}
-       4.0,                                       !- Speed 4 Gross Rated Cooling COP {dimensionless}
-       0.1963104,                           !- Speed 4 Rated Air Flow Rate {m3/s}
-       0.38,                                     !- Speed 4 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
-       ,                                             !- Evaporative precooling effectiveness
-       HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
-       HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
-       HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
-       3581.7,                                 !- Speed 5 Gross Rated Total Cooling Capacity {w}
-       0.75,                                     !- Speed 5 Gross Rated Sensible Heat Ratio {dimensionless}
-       4.0,                                       !- Speed 5 Gross Rated Cooling COP {dimensionless}
-       0.226512,                             !- Speed 5 Rated Air Flow Rate {m3/s}
-       0.44,                                     !- Speed 5 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
-       ,                                             !- Evaporative precooling effectiveness
-       HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
-       HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
-       HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
-       4239.5,                                 !- Speed 6 Gross Rated Total Cooling Capacity {w}
-       0.75,                                     !- Speed 6 Gross Rated Sensible Heat Ratio {dimensionless}
-       4.0,                                       !- Speed 6 Gross Rated Cooling COP {dimensionless}
-       0.2567136,                           !- Speed 6 Rated Air Flow Rate {m3/s}
-       0.50,                                     ! - Speed 6 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
-       ,                                             ! - Evaporative precooling effectiveness
-       HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
-       HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
-       HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
-       4885.7,                                 !- Speed 7 Gross Rated Total Cooling Capacity {w}
-       0.75,                                     !- Speed 7 Gross Rated Sensible Heat Ratio {dimensionless}
-       4.0,                                       !- Speed 7 Gross Rated Cooling COP {dimensionless}
-       0.2869152,                           !- Speed 7 Rated Air Flow Rate {m3/s}
-       0.57,                                     ! - Speed 7 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
-       ,                                             ! - Evaporative precooling effectiveness
-       HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
-       HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
-       HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
-       5520.7,                                 !- Speed 8 Gross Rated Total Cooling Capacity {w}
-       0.75,                                     !- Speed 8 Gross Rated Sensible Heat Ratio {dimensionless}
-       4.0,                                       !- Speed 8 Gross Rated Cooling COP {dimensionless}
-       0.3171168,                           !- Speed 8 Rated Air Flow Rate {m3/s}
-       0.63,                                     ! - Speed 8 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
-       ,                                             ! - Evaporative precooling effectiveness
-       HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
-       HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
-       HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
-       6144.8,                                 !- Speed 9 Gross Rated Total Cooling Capacity {w}
-       0.75,                                     !- Speed 9 Gross Rated Sensible Heat Ratio {dimensionless}
-       4.0,                                       !- Speed 9 Rated Cooling COP {dimensionless}
-       0.3473184,                           !- Speed 9 Rated Air Flow Rate {m3/s}
-       0.69,                                     ! - Speed 9 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
-       ,                                             ! - Evaporative precooling effectiveness
-       HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
-       HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
-       HPACCOOLEIRFFF,                 !- Energy Input Ratio Function of Flow Fraction Curve Name
-       6758.0,                                 !- Speed 10 Gross Rated Total Cooling Capacity {w}
-       0.75,                                     !- Speed 10 Gross Rated Sensible Heat Ratio {dimensionless}
-       4.0,                                       !- Speed 10 Gross Rated Cooling COP {dimensionless}
-       0.37752,                               !- Speed 10 Rated Air Flow Rate {m3/s}
-       0.74,                                     ! - Speed 10 Rated Condenser Air Flow Rate {m3/s}, for evaporatively cooled
-       ,                                             ! - Evaporative precooling effectiveness
-       HPACCoolCapFT,                   !- Total Cooling Capacity Function of Temperature Curve Name
-       HPACCoolCapFFF,                 !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       HPACCOOLEIRFT,                   !- Energy Input Ratio Function of Temperature Curve Name
-       HPACCOOLEIRFFF;                 !- Energy Input Ratio Function of Flow Fraction Curve Name
-```
-
-### Variable Speed DX Cooling Coil Outputs
-
-* HVAC,Average,Cooling Coil Electric Power [W]
-
-* HVAC,Average,Cooling Coil Total Cooling Rate [W]
-
-* HVAC,Average,Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC,Average,Cooling Coil Source Side Heat Transfer Rate [W]
-
-* HVAC,Average,Cooling Coil Part Load Ratio []
-
-* HVAC,Average, Cooling Coil Runtime Fraction []
-
-* HVAC,Average, Cooling Coil Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Cooling Coil Air Inlet Temperature [C]
-
-* HVAC,Average,Cooling Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC,Average,Cooling Coil Air Outlet Temperature [C]
-
-* HVAC,Average,Cooling Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC,Average,Cooling Coil Upper Speed Level []
-
-* HVAC,Average,Cooling Coil Neighboring Speed Levels Ratio []
-
-* HVAC,Average,VSAirtoAirHP Recoverable Waste Heat [W]
-
-* HVAC,Sum,Cooling Coil Electric Energy [J]
-
-* HVAC,Sum,Cooling Coil Total Cooling Energy [J]
-
-* HVAC,Sum,Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC,Sum,Cooling Coil Latent Cooling Energy [J]
-
-* HVAC,Sum,Cooling Coil Source Side Heat Transfer Energy [J]
-
-* HVAC,Average,Cooling Coil Crankcase Heater Electric Power [W]
-
-* HVAC,Sum,Cooling Coil Crankcase Heater Electric Energy [J]
-
-* HVAC,Average,Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Cooling Coil Condensate Volume [m3]
-
-* HVAC,Average,Cooling Coil Condenser Inlet Temperature [C]
-
-* HVAC,Sum,Cooling Coil Evaporative Condenser Water Volume [m3]
-
-* HVAC,Sum,Cooling Coil Evaporative Condenser Mains Water Volume [m3]
-
-* HVAC,Average,Cooling Coil Evaporative Condenser Pump Electric Power[W]
-
-* HVAC,Sum,Cooling Coil Evaporative Condenser Pump Electric Energy [J]
-
-* HVAC,Average,Cooling Coil Basin Heater Electric Power [W]
-
-* HVAC,Sum,Cooling Coil Basin Heater Electric Energy [J]
-
-#### Cooling Coil Electric Power [W]
-
-This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
-
-#### Cooling Coil Total Cooling Rate [W]
-
-The output variable is the average total cooling load provide by the heat pump which includes the sensible and latent load in Watts over the timestep being reported.
-
-#### Cooling Coil Sensible Cooling Rate [W]
-
-The output variable is the average sensible cooling load provide by the heat pump in Watts over the timestep being reported.
-
-#### Cooling Coil Source Side Heat Transfer Rate [W]
-
-The output variable is the average heat rejected to the water at the heat pump condenser in Watts over the timestep being reported.
-
-#### Cooling Coil Part Load Ratio []
-
-This output variable is the ratio of the part-load capacity to the steady state capacity of the VSAirtoAirHP coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the VSAirtoAirHP coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
-
-#### Cooling Coil Runtime Fraction []
-
-This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The runtime fraction, or duty factor, accounts for efficiency losses due to compressor cycling.
-
-#### Cooling Coil Air Mass Flow Rate [kg/s]
-
-The output variable is the average air mass flow rate on the load side going through the heat pump over the timestep being reported.
-
-#### Cooling Coil Air Inlet Temperature [C]
-
-The output variable is the average entering air dry-bulb temperature over the timestep being reported.
-
-#### Cooling Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average entering air dry humidity ratio over the timestep being reported.
-
-#### Cooling Coil Air Outlet Temperature [C]
-
-The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
-
-#### Cooling Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average leaving air dry humidity ratio over the timestep being reported.
-
-#### Cooling Coil Upper Speed Level []
-
-The output variable is the average upper speed level, for interpolating performances between two neighboring speed levels.
-
-#### Cooling Coil Neighboring Speed Levels Ratio []
-
-The output variable is the average speed ratio, for interpolating performances between two neighboring speed levels.
-
-#### Cooling Coil Electric Energy [J]
-
-The output variable is the electric consumption of the heat pump in Joules over the timestep being reported.
-
-#### Cooling Coil Total Cooling Energy [J]
-
-The output variable is the total cooling output of the coil in Joules over the timestep being reported.
-
-#### Cooling Coil Sensible Cooling Energy [J]
-
-The output variable is the total sensible cooling output of the coil in Joules over the timestep being reported
-
-#### Cooling Coil Latent Cooling Energy [J]
-
-#### Cooling Coil Latent Cooling Rate [W]
-
-These output variables are the total latent cooling output of the coil in Joules or Watts over the timestep being reported.
-
-#### Cooling Coil Source Side Heat Transfer Energy [J]
-
-The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported.
-
-#### Cooling Coil Crankcase Heater Electric Power [W]
-
-The output variable is the average power used for crankcase heater, in Watts over the timestep being reported.
-
-#### Cooling Coil Crankcase Heater Electric Energy [J]
-
-The output variable is the total electric energy usage of the coil for crankcase heater, in Joules over the timestep being reported.
-
-#### Cooling Coil Condensate Volume Flow Rate [m3/s]
-
-The output variable is the average water condensate volumetric flow rate from the cooling coil, in m<sup>3</sup>/s over the timestep being reported, if choosing to use CondensatetoTank.
-
-#### Cooling Coil Condensate Volume [m3]
-
-The output variable is the total water condensate volume from the cooling coil, in m<sup>3</sup> over the timestep being reported.
-
-#### Cooling Coil Condenser Inlet Temperature [C]
-
-The output variable is the average air temperature entering the condenser coil, in  &deg;C over the timestep being reported.
-
-#### Cooling Coil Evaporative Condenser Water Volume [m3]
-
-The output variable is the total water volume consumed for condenser evaporative pre-cooling, in m<sup>3</sup> over the timestep being reported.
-
-#### Cooling Coil Evaporative Condenser Mains Water Volume [m3]
-
-The output variable is the total water volume for condenser evaporative pre-cooling, obtained from the Mains Water supply, in m<sup>3</sup> over the timestep being reported.
-
-#### Cooling Coil Evaporative Condenser Pump Electric Power[W]
-
-The output variable is the average power consumption rate of the evaporative condenser pump, in Watts over the timestep being reported.
-
-#### Cooling Coil Evaporative Condenser Pump Electric Energy [J]
-
-The output variable is the total power consumption of the evaporative condenser pump, in Joules over the timestep being reported.
-
-#### Cooling Coil Basin Heater Electric Power [W]
-
-The output variable is the average power consumption rate by the basin heater, in Watts over the timestep being reported.
-
-#### Cooling Coil Basin Heater Electric Energy [J]
-
-The output variable is the total power consumption by the basin heater, in Joules over the timestep being reported.
-
-### CoilPerformance:DX:Cooling
-
-This coil performance object is used to specify DX coil performance for one mode of operation for a Coil:Cooling:DX:TwoStageWithHumidityControlMode. A single Coil:Cooling:DX:TwoStageWithHumidityControlMode object will reference one to four CoilPerformance:DX:Cooling objects depending on the number of available stages and dehumidification modes as specified in the two stage DX object. For example, a standard 2-stage DX system will use two of these performance objects, one to defined the capacity and performance for stage 1 operation, and a second one for stage 1+2 (both stages active) operation. In nearly all cases, the Rated Air Volume Flow Rate will be the same for all performance objects associated with a given multimode DX coil. If bypass is specified, the Rated Air Volume Flow Rate includes both the bypassed flow and the flow through the active coil.
-
-This DX coil model is identical to Coil:Cooling:DX:SingleSpeed   with addition of bypass and multi-stage capabilities. This DX cooling coil model and input are quite different from that for the heating and cooling water coils. The simple water coils use an NTU-effectiveness heat exchanger model. The single speed DX coil model uses performance information at rated conditions along with curve fits for variations in total capacity, energy input ratio and part-load fraction to determine performance at part-load conditions. Sensible/latent capacity splits are determined by the rated sensible heat ratio (SHR) and the apparatus dewpoint/bypass factor (ADP/BF) approach. This approach is analogous to the NTU-effectiveness calculations used for sensible-only heat exchanger calculations, extended to a cooling and dehumidifying coil.
-
-An alternative to ADP/BF method for sensible/latent capacity split is to use SHR modifier curves for temperature and flow fraction.   These two optional input fields are used only when a user specified SHR calculation method desired over the (ADP/BF) method.   Sensible heat ratio calculated using these two SHR modifier curves override the value calculated by ADP/BF method. See section    SHR Calculation Using User Specified SHR Modifier Curves    in the EnergyPlus Engineering Document for further details.
-
-The DX cooling coil input requires the gross rated total cooling capacity, the gross rated SHR, the gross rated COP, the rated air volume flow rate, and the fraction of air flow which is bypassed around the coil. The first 4 inputs determine the coil performance at the rating point (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb and air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb). The rated air volume flow rate (less any bypassed fraction) should be between .00004027 m<sup>3</sup>/s and .00006041 m<sup>3</sup>/s per watt of gross rated total cooling capacity (300 to 450 cfm/ton). The rated volumetric air flow to gross total cooling capacity ratio for 100% dedicated outdoor air (DOAS) application DX cooling coils should be between 0.00001677 (m3/s)/W (125 cfm/ton) and 0.00003355 (m3/s)/W (250 cfm/ton).
-
-This model requires 5 curves as follows:
-
-1.        The total cooling capacity modifier curve (function of temperature) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures).
-
-2.        The total cooling capacity modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating.
-
-3.        The energy input ratio (EIR) modifier curve (function of temperature) is a biquadratic curve with two independent variables: wet-bulb temperature of the air entering the cooling coil, and dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures).
-
-4.        The energy input ratio (EIR) modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating.
-
-5.        The part load fraction correlation (function of part load ratio) is a quadratic or cubic curve with the independent variable being part load ratio (sensible cooling load / steady-state sensible cooling capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the    effective    EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The curve should be normalized to a value of 1.0 when the part-load ratio equals 1.0 (i.e., the compressor(s) run continuously for the simulation timestep).
-
-The curves are simply specified by name. Curve inputs are described in the curve manager section of this document (see Performance Curves in this document).
-
-The next four input fields are optional and relate to the degradation of latent cooling capacity when the supply air fan operates continuously while the cooling coil/compressor cycle on and off to meet the cooling load. The fan operating mode is either considered to be constant (e.g. CoilSystem:Cooling:DX) or can be scheduled in the parent object (e.g. AirLoopHVAC:UnitaryHeatCool). When scheduled, the schedule value must be greater than 0 to calculate degradation of latent cooling capacity. At times when the parent object   s supply air fan operating mode schedule is 0, latent degradation will be ignored. When used, these next four input fields must all have positive values in order to model latent capacity degradation.
-
-The next input specifies the outdoor air node used to define the conditions of the air entering the outdoor condenser. If this field is not blank, the node name specified must be listed in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor temperature from the weather data. Alternately, the node name must be specified in an OutdoorAir:NodeList object where the outdoor temperature entering the condenser is taken directly from the weather data. This field may also be left blank, if this is the case then the outdoor temperature entering the condenser is taken directly from the weather data.
-
-The next input describes the type of outdoor condenser coil used with the DX cooling coil (Air Cooled or Evap Cooled). The following three inputs are required when modeling an evaporative-cooled condenser: evaporative condenser effectiveness, evaporative condenser air volume flow rate, and the power consumed by the evaporative condenser pump. See section    DX Cooling Coil Model    in the EnergyPlus Engineering Document for further details regarding this model.
-
-#### Field: Name
-
-This alpha field is a unique user-assigned name for an instance of DX cooling coil performance. Any reference to this DX coil performance object by another object will use this name.
-
-#### Field: Gross Rated Total Cooling Capacity
-
-The total, full load gross cooling capacity (sensible plus latent) in watts of the DX coil unit at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb[[4]](#_ftn4), and a cooling coil air flow rate defined by field    rated air flow rate    below). Capacity should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for).
-
-#### Field: Gross Rated Sensible Heat Ratio
-
-The sensible heat ratio (SHR=gross sensible capacity divided by gross total cooling capacity) of the DX cooling coil at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and a cooling coil air flow rate defined by field    rated air flow rate    below). Both the sensible and total cooling capacities used to define the Rated SHR should be    gross    (i.e., the effect of supply air fan heat is NOT accounted for).
-
-#### Field: Gross Rated Cooling COP
-
-The coefficient of performance is the ratio of the gross total cooling capacity in watts to electrical power input in watts) of the DX cooling coil unit at rated conditions (air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/ 23.9 &deg;C wetbulb, and a cooling coil air flow rate defined by field    rated air flow rate    below). The input power includes electric power for the compressor(s) and condenser fan(s) but does not include the power consumption of the supply air fan. If this input field is left blank, the default value is 3.0.
-
-#### Field: Rated Air Flow Rate
-
-The air volume flow rate, in m<sup>3</sup> per second, across the DX cooling coil at rated conditions. The gross rated total cooling capacity, gross rated SHR and gross rated COP should be performance information for the unit with air entering the cooling coil at 26.7 &deg;C drybulb/19.4 &deg;C wetbulb, air entering the outdoor condenser coil at 35 &deg;C drybulb/23.9 &deg;C wetbulb, and the rated air volume flow rate defined here.
-
-#### Field: Fraction of Air Flow Bypassed Around Coil
-
-This numeric field specifies the fraction of the Rated Air Volume Flow Rate which bypasses the active cooling coil for this performance mode. The remaining portion of the flow should be between 0.00004027 m3/s and .00006041 m3/s per watt of gross rated total cooling capacity (300 to 450 cfm/ton) for this performance mode. For DOAS applications the remaining portion of rated air volume flow rate should be between 0.00001677 m<sup>3</sup>/s and 0.00003355 m<sup>3</sup>/s per watt of gross rated total cooling capacity (125 to 250 cfm/ton).   This is used to model face-split coils on multi-stage units or bypass dampers. If total flow rate varies during simulation, the same fraction is bypassed. This input may range from 0.0 to &lt;1.0. The default is 0.0. For a multi-stage face-split coil in which stage 1 is 60% of total capacity, this field would be set to 0.4 for the Stage 1 performance and set to 0.0 for the Stage 1+2 performance. For a DX system which activates a bypass damper for improved dehumidification, this field would be set to 0.0 for normal mode performance and set to something greater than zero for enhanced dehumidification mode performance.
-
-#### Field: Total Cooling Capacity Function of Temperature Curve Name
-
-The name of a **biquadratic** performance curve (ref: Performance Curves) that parameterizes the variation of the total gross cooling capacity as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The output of this curve is multiplied by the gross rated total cooling capacity to give the gross total cooling capacity at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to have the value of 1.0 at the rating point.
-
-#### Field: Total Cooling Capacity Function of Flow Fraction Curve Name
-
-The name of a **quadratic** or **cubic** performance curve (ref:   Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated total cooling capacity and the total cooling capacity modifier curve (function of temperature) to give the gross total cooling capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
-
-#### Field: Energy Input Ratio Function of Temperature Curve Name
-
-The name of a **biquadratic** performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the wet-bulb temperature of the air entering the cooling coil, and the dry-bulb temperature of the air entering the air-cooled condenser coil (wet-bulb temperature if modeling an evaporative-cooled condenser). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at temperatures different from the rating point temperatures). The curve is normalized to a value of 1.0 at the rating point.
-
-#### Field: Energy Input Ratio Function of Flow Fraction Curve Name
-
-The name of a **quadratic** or **cubic** performance curve (Ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate.
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a **quadratic** or **cubic** performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the    effective    EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
-
-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7     and     PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
-
-           PLF = 0.85 + 0.15(PLR)
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-           PLF = 1.0 + 0.0(PLR)
-
-#### Field: Nominal Time for Condensate Removal to Begin
-
-The nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]), and this field as well as the next three input fields for this object must have positive values in order to model latent capacity degradation.
-
-#### Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity
-
-Ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]); and this field, the previous field and the next two fields must have positive values in order to model latent capacity degradation.
-
-#### Field: Maximum Cycling Rate
-
-The maximum on-off cycling rate for the compressor (cycles per hour), which occurs at 50% run time fraction. Suggested value is 3; zero value means latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]); and this field, the previous two fields and the next field must have positive values in order to model latent capacity degradation.
-
-#### Field: Latent Capacity Time Constant
-
-Time constant (in seconds) for the cooling coil's latent capacity to reach steady state after startup. Suggested value is 45; zero value means latent degradation model is disabled. The default value for this field is zero. The supply air fan operating mode must be continuous (i.e., the supply air fan operating mode may be specified in other    parent    objects and is assumed continuous in some objects (e.g., CoilSystem:Cooling:DX) or can be scheduled in other objects [e.g., AirloopHVAC:UnitaryHeatCool]), and this field as well as the previous three input fields for this object must have positive values in order to model latent capacity degradation.
-
-#### Field: Condenser Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor condenser. If this field is left blank, the outdoor air temperature entering the condenser (dry-bulb or wet-bulb) is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
-
-#### Field: Condenser Type
-
-The type of condenser used by the DX cooling coil. Valid choices for this input field are **AirCooled** or **EvaporativelyCooled**. The default for this field is **AirCooled**.
-
-#### Field: Evaporative Condenser Effectiveness
-
-The effectiveness of the evaporative condenser, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
-
-<div>\[Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectiveness} \right)\left( {Tdb,o\,\, - Twb,o} \right)\]</div>
-
-where
-
-*T<sub>cond\\ inlet</sub>* = the temperature of the air entering the condenser coil (C)
-
-*T<sub>wb,o</sub>* = the wet-bulb temperature of the outdoor air (C)
-
-*T<sub>db,o</sub>* = the dry-bulb temperature of the outdoor air (C)
-
-The resulting condenser inlet air temperature is used by the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled.
-
-If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
-
-If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
-
-If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = Evap Cooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Total Cooling Capacity Modifier Curve (function of temperature) and the Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Total Cooling Capacity and EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
-
-#### Field: Evaporative Condenser Air Flow Rate
-
-The air volume flow rate, in m<sup>3</sup> per second, entering the evaporative condenser. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000144 m<sup>3</sup>/s per watt of rated total cooling capacity [850 cfm/ton]). This field is not used when Condenser Type = Air Cooled.
-
-#### Field: Evaporative Condenser Pump Rated Power Consumption
-
-The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt [15 W/ton] of rated total cooling capacity). This field is not used when Condenser Type = AirCooled.
-
-#### Field: Sensible Heat Ratio Function of Temperature Curve Name
-
-The name of a biquadratic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of DX cooling coil entering air wet-bulb and dry-bulb temperatures. The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of flow fraction) to give the SHR at the specific coil entering air temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 at the rated condition. This input field is optional.
-
-#### Field: Sensible Heat Ratio Function of Flow Fraction Curve Name
-
-The name of a quadratic or cubic normalized curve (Ref: Performance Curves) that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated SHR and the SHR modifier curve (function of temperature) to give the SHR at the specific temperature and air flow conditions at which the cooling coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate. This input field is optional.
-
-Following is an example input for a Coil:Cooling:DX:TwoStageWithHumidityControlMode with 2 capacity stages and one enhanced dehumidification mode so it requires four   CoilPerformance:DX:Cooling objects.
-
-```idf
-Coil:Cooling:DX:TwoStageWithHumidityControlMode,
-       DXSystem 1 Cooling Coil, !- Coil Name
-       OfficeHeatCoolAvail,         !- Availability Schedule
-       DXSystem 1 Mixed Air Node,   !- Coil Air Inlet Node
-       DXSystem 1 Fan Air Inlet Node,   !- Coil Air Outlet Node
-       ,                                               !- Crankcase Heater Capacity {W}
-       ,                                               !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
-       2,                                             !- Number of Capacity Stages
-       1,                                             !- Number of Enhanced Dehumidification Modes
-       CoilPerformance:DX:Cooling,   !- Normal Mode Stage 1 Coil Performance Object Type
-       DXSystem 1 DX Coil Standard Mode-Stage 1,   !- Normal Mode Stage 1 Coil Performance Object Name
-       CoilPerformance:DX:Cooling,   !- Normal Mode Stage 1+2 Coil Perf Object Type
-       DXSystem 1 DX Coil Standard Mode-Stage 1&2,   !- Normal Mode Stage 1+2 Coil Perf Object Name
-       CoilPerformance:DX:Cooling,   !- Dehumid Mode 1 Stage 1 Coil Perf Object Type
-       DXSystem 1 DX Coil SubCoolReheat Mode-Stage 1,   !- Dehumid Mode 1 Stage 1 Coil Perf Object Name
-       CoilPerformance:DX:Cooling,   !- Dehumid Mode 1 Stage 1+2 Coil Perf Object Type
-       DXSystem 1 DX Coil SubCoolReheat Mode-Stage 1&2;   !- Dehumid Mode 1 Stage 1+2 Coil Perf Object Name
-
-
-CoilPerformance:DX:Cooling,
-       DXSystem 1 DX Coil Standard Mode-Stage 1,   !- Coil Performance Specification Name
-       21327.57812,                         !- Gross Rated Total Cooling Capacity {W}
-       0.68,                                       !- Gross Rated Sensible Heat Ratio
-       3.56,                                       !- Gross Rated Cooling COP
-       1.695372105,                         !- Rated Air Flow Rate {m3/s}
-       0.4,                                         !- Fraction of Air Flow Bypassed Around Coil
-       HPACCoolCapFT,                     !- Total Cooling Capacity Modifier Curve (function of temperature)
-       HPACCoolCapFFF,                   !- Total Cooling Capacity Modifier Curve (function of flow fraction)
-       HPACCOOLEIRFT,                     !- Energy Input Ratio Modifier Curve (function of temperature)
-       HPACCOOLEIRFFF,                   !- Energy Input Ratio Modifier Curve (function of flow fraction)
-       HPACCOOLPLFFPLR,                 !- Part Load Fraction Correlation (function of part load ratio)
-       1000,                                       !- Nominal Time for Condensate Removal to Begin {s}
-       1.5, !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity {dimensionless}
-       3,                                             !- Maximum ON/OFF Cycling Rate {cycles/hr}
-       45,                                           !- Latent Capacity Time Constant {s}
-       ,                                               !- Condenser Air Inlet Node Name
-       ,                                               !- Condenser Type
-       ,                                               !- Evaporative Condenser Effectiveness
-       ,                                               !- Evaporative Condenser Air Flow Rate
-       ,                                               !- Evaporative Condenser Pump Rated Power Consumption
-       DOAS DX Coil SHR-FT,         !- Sensible Heat Ratio Function of Temperature Curve Name
-       DOAS DX Coil SHR-FF;         !- Sensible Heat Ratio Function of Flow Fraction Curve Name
-
-
-CoilPerformance:DX:Cooling,
-       DXSystem 1 DX Coil Standard Mode-Stage 1&2,   !- Coil Performance Specification Name
-       35545.96484,                         !- Gross Rated Total Cooling Capacity {W}
-       0.68,                                       !- Gross Rated Sensible Heat Ratio
-       3.56,                                       !- Gross Rated Cooling COP
-       1.695372105,                         !- Rated Air Flow Rate {m3/s}
-       0.0,                                         !- Fraction of Air Flow Bypassed Around Coil
-       HPACCoolCapFT,                     !- Total Cooling Capacity Modifier Curve (function of temperature)
-       HPACCoolCapFFF,                   !- Total Cooling Capacity Modifier Curve (function of flow fraction)
-       HPACCOOLEIRFT,                     !- Energy Input Ratio Modifier Curve (function of temperature)
-       HPACCOOLEIRFFF,                   !- Energy Input Ratio Modifier Curve (function of flow fraction)
-       HPACCOOLPLFFPLR,                 !- Part Load Fraction Correlation (function of part load ratio)
-       1000,                                       !- Nominal Time for Condensate Removal to Begin {s}
-       1.5, !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity {dimensionless}
-       3,                                             !- Maximum ON/OFF Cycling Rate {cycles/hr}
-       45,                                           !- Latent Capacity Time Constant {s}
-       ,                                               !- Condenser Air Inlet Node Name
-       ,                                               !- Condenser Type
-       ,                                               !- Evaporative Condenser Effectiveness
-       ,                                               !- Evaporative Condenser Air Flow Rate
-       ,                                               !- Evaporative Condenser Pump Rated Power Consumption
-       DOAS DX Coil SHR-FT,         !- Sensible Heat Ratio Function of Temperature Curve Name
-       DOAS DX Coil SHR-FF;         !- Sensible Heat Ratio Function of Flow Fraction Curve Name
-
-
-CoilPerformance:DX:Cooling,
-       DXSystem 1 DX Coil SubCoolReheat Mode-Stage 1,   !- Coil Performance Specification Name
-       19962.61328,                         !- Gross Rated Total Cooling Capacity (gross) {W}
-       0.60,                                       !- Gross Rated SHR
-       3.31,                                       !- Gross Rated Cooling COP
-       1.695372105,                         !- Rated Air Flow Rate {m3/s}
-       0.4,                                         !- Fraction of Air Flow Bypassed Around Coil
-       SubCoolReheatCoolCapFT,   !- Total Cooling Capacity Modifier Curve (function of temperature)
-       SubCoolReheatCoolCapFFF, !- Total Cooling Capacity Modifier Curve (function of flow fraction)
-       SubCoolReheatCOOLEIRFT,   !- Energy Input Ratio Modifier Curve (function of temperature)
-       SubCoolReheatCoolEIRFFF, !- Energy Input Ratio Modifier Curve (function of flow fraction)
-       SubCoolReheatCoolPLFFPLR, !- Part Load Fraction Correlation (function of part load ratio)
-       1000,                                       !- Nominal Time for Condensate Removal to Begin {s}
-       1.5, !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity {dimensionless}
-       3,                                             !- Maximum ON/OFF Cycling Rate {cycles/hr}
-       45,                                           !- Latent Capacity Time Constant {s}
-       ,                                               !- Condenser Air Inlet Node Name
-       ,                                               !- Condenser Type
-       ,                                               !- Evaporative Condenser Effectiveness
-       ,                                               !- Evaporative Condenser Air Flow Rate
-       ,                                               !- Evaporative Condenser Pump Rated Power Consumption
-       DOAS DX Coil SHR-FT,         !- Sensible Heat Ratio Function of Temperature Curve Name
-       DOAS DX Coil SHR-FF;         !- Sensible Heat Ratio Function of Flow Fraction Curve Name
-
-
-CoilPerformance:DX:Cooling,
-       DXSystem 1 DX Coil SubCoolReheat Mode-Stage 1&2,   !- Coil Performance Specification Name
-       33271.01953,                         !- Gross Rated Total Cooling Capacity (gross) {W}
-       0.60,                                       !- Gross Rated SHR
-       3.31,                                       !- Gross Rated Cooling COP
-       1.695372105,                         !- Rated Air Flow Rate {m3/s}
-       0.0,                                         !- Fraction of Air Flow Bypassed Around Coil
-       SubCoolReheatCoolCapFT,   !- Total Cooling Capacity Modifier Curve (function of temperature)
-       SubCoolReheatCoolCapFFF, !- Total Cooling Capacity Modifier Curve (function of flow fraction)
-       SubCoolReheatCOOLEIRFT,   !- Energy Input Ratio Modifier Curve (function of temperature)
-       SubCoolReheatCoolEIRFFF, !- Energy Input Ratio Modifier Curve (function of flow fraction)
-       SubCoolReheatCoolPLFFPLR, !- Part Load Fraction Correlation (function of part load ratio)
-       1000,                                       !- Nominal Time for Condensate Removal to Begin {s}
-       1.5, !- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity {dimensionless}
-       3,                                             !- Maximum ON/OFF Cycling Rate {cycles/hr}
-       45,                                           !- Latent Capacity Time Constant {s}
-       ,                                               !- Condenser Air Inlet Node Name
-       ,                                               !- Condenser Type
-       ,                                               !- Evaporative Condenser Effectiveness
-       ,                                               !- Evaporative Condenser Air Flow Rate
-       ,                                               !- Evaporative Condenser Pump Rated Power Consumption
-       DOAS DX Coil SHR-FT,         !- Sensible Heat Ratio Function of Temperature Curve Name
-       DOAS DX Coil SHR-FF;         !- Sensible Heat Ratio Function of Flow Fraction Curve Name
-```
-
-### Coil Performance DX Cooling Outputs
-
-The CoilPerformance:DX:Cooling object does not have specific output variables. To request reports, use the parent object Coil:Cooling:DX:TwoStageWithHumidityControlMode output variable options (ref. DX Cooling Coil Outputs). When requesting specific output variables by name, use the name of the parent object as the Key Value for Output:Variable reporting objects (ref. Output:Variable object). The name of the CoilPerformance:DX:Cooling object cannot be used as a Key Value in the Output:Variable object.
-
-### Coil:Heating:DX:SingleSpeed
-
-The single speed heating DX coil model uses performance information at rated conditions along with curve fits for variations in total capacity, energy input ratio and part load fraction to determine performance at part-load conditions. The impacts of various defrost strategies (reverse cycle, resistive, timed or on-demand) are modeled based on a combination of user inputs and empirical models taken from the air-to-air heat pump algorithms in DOE-2.1E.
-
-The single speed heating DX coil input requires an availability schedule, the gross rated heating capacity, the gross rated COP and the rated air volume flow rate. The latter 3 inputs determine the coil performance at the rating point (outdoor air dry-bulb temperature of 8.33 C, outdoor air wet-bulb temperature of 6.11 C, coil entering air dry-bulb temperature of 21.11 C, coil entering air wet-bulb temperature of 15.55 C). The rated air volume flow rate should be between .00004027 m<sup>3</sup>/s and .00006041 m<sup>3</sup>/s per watt of gross rated heating capacity.
-
-Up to 6 curves are required depending on the defrost strategy selected.
-
-1)        The heating capacity modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the gross rated heating capacity to give the gross heating capacity at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
-
-2)        The heating capacity modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating.
-
-3)        The energy input ratio (EIR) modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
-
-4)        The energy input ratio (EIR) modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating.
-
-5)        The part load fraction correlation (function of part load ratio) is a quadratic or cubic curve with the independent variable being part load ratio (sensible heating load / steady-state heating capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the    effective    EIR for a given simulation timestep. The part load fraction correlation accounts for efficiency losses due to compressor cycling.
-
-6)        The defrost energy input ratio (EIR) modifier curve (function of temperature) is a bi-quadratic curve with two independent variables: outdoor air dry-bulb temperature and the heating coil entering air wet-bulb temperature. The output of this curve is multiplied by the heating coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the coil is operating. This curve is only required when a reverse-cycle defrost strategy is specified.
-
-The curves are simply specified by name. Curve inputs are described in the curve manager section of this document (ref. Performance Curves).
-
-The next input item for the coil is the supply air fan operation mode. Either the supply air fan runs continuously while the DX coil cycles on/off, or the fan and coil cycle on/off together. The next two inputs define the minimum outdoor dry-bulb temperature that the heat pump compressor will operate and the maximum outdoor dry-bulb temperature for defrost operation. Crankcase heater capacity and cutout temperature are entered in the following two inputs. The final four inputs cover the type of defrost strategy (reverse-cycle or resistive), defrost control (timed or on-demand), the fractional defrost time period (timed defrost control only), and the resistive defrost heater capacity if a resistive defrost strategy is selected.
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a DX heating coil. Any reference to this DX heating coil by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the DX heating coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Gross Rated Heating Capacity
-
-This numeric field defines the total, full load gross heating capacity in watts of the DX coil unit at rated conditions (outdoor air dry-bulb temperature of 8.33 C, outdoor air wet-bulb temperature of 6.11 C, heating coil entering air dry-bulb temperature of 21.11 C, heating coil entering air wet-bulb temperature of 15.55 C, and a heating coil air flow rate defined by field    rated air flow volume    below). The value entered here must be greater than 0. Capacity should not account for supply air fan heat. The gross rated heating capacity should be within 20% of the gross rated total cooling capacity, otherwise a warning message is issued. The gross heating capacity should NOT include the effect of supply air fan heat.
-
-#### Field: Gross Rated Heating COP
-
-This numeric field defines the coefficient of performance (COP= the gross heating capacity in watts divided by electrical power input in watts) of the DX heating coil unit at rated conditions (outdoor air dry-bulb temperature of 8.33 C, outdoor air wet-bulb temperature of 6.11 C, coil entering air dry-bulb temperature of 21.11 C, coil entering air wet-bulb temperature of 15.55 C, and a heating coil air flow rate defined by field    rated air flow volume rate    below). The value entered here must be greater than 0. The input power includes power for the compressor(s) and outdoor fan(s) but does not include the power consumption of the indoor supply air fan. The gross COP should NOT account for the supply air fan.
-
-#### Field: Rated Air Flow Rate
-
-This numeric field defines the volume air flow rate, in m<sup>3</sup> per second, across the DX heating coil at rated conditions. The value entered here must be greater than 0. The rated air volume flow rate should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of the gross rated heating capacity. The gross rated heating capacity and gross rated COP should be performance information for the unit with outdoor air dry-bulb temperature of 8.33 C, outdoor air wet-bulb temperature of 6.11 C, heating coil entering air dry-bulb temperature of 21.11 C, heating coil entering air wet-bulb temperature of 15.55 C, and the rated air volume flow rate defined here.
-
-#### Field: Rated Evaporator Fan Power Per Volume Flow Rate
-
-This field is the electric power for the evaporator (heating coil) fan per air volume flow rate through the coil at the rated conditions in W/(m<sup>3</sup>/s). The default value is 773.3 W/(m<sup>3</sup>/s) (365 W/1000 cfm) if this field is left blank. If a value is entered, it must be &gt;= 0.0 and &lt;= 1250 W/(m<sup>3</sup>/s). This value is only used to calculate High Temperature Heating Standard (Net) Rating Capacity, Low Temperature Heating Standard (Net) Rating Capacity and Heating Seasonal Performance Factor (HSPF) which will be outputs in the EnergyPlus eio file (ref. EnergyPlus Engineering Reference, Single Speed DX Heating Coil, Standard Ratings). This value is not used for modeling the evaporator (heating coil) fan during simulations; instead, it is used for calculating the above standard ratings to assist the user in verifying their inputs for modeling this type of equipment.
-
-#### Field: Air Inlet Node Name
-
-This alpha field defines the name of the HVAC system node from which the DX heating coil draws its inlet air.
-
-#### Field: Air Outlet Node Name
-
-This alpha field defines the name of the HVAC system node to which the DX heating coil sends its outlet air.
-
-#### Field: Heating Capacity Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of the total heating capacity as a function of the both the indoor and outdoor air dry-bulb temperature or just the outdoor air dry-bulb temperature depending on the type of curve selected. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the gross rated heating capacity to give the gross total heating capacity at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or outdoor air dry-bulb temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
-
-#### Field: Heating Capacity Function of Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve (ref:   Performance Curves) that parameterizes the variation of total heating capacity as a function of the ratio of actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
-
-#### Field: Energy Input Ratio Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor and outdoor air dry-bulb temperature or just the outdoor air dry-bulb temperature depending on the type of curve selected. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or outdoor air dry-bulb temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
-
-#### Field: Energy Input Ratio Function of Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate.
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the    effective    EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
-
-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7     and     PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
-
-           PLF = 0.85 + 0.15(PLR)
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-           PLF = 1.0 + 0.0(PLR)
-
-#### Field: Defrost Energy Input Ratio Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) during reverse-cycle defrost periods as a function of the outdoor air dry-bulb temperature and the wet-bulb temperature of the air entering the indoor coil. The EIR is the inverse of the COP. The output of this curve is multiplied by the coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the indoor and outdoor coils are operating. This curve is only required when a reverse-cycle defrost strategy is selected. The curve is normalized to a value of 1.0 at the rating point conditions.
-
-#### Field: Minimum Outdoor Dry-Bulb Temperature for Compressor Operation
-
-This numeric field defines the minimum outdoor air dry-bulb temperature where the heating coil compressor turns off. The temperature for this input field must be greater than or equal to    20 C. If this input field is left blank, the default value is -8 C.
-
-#### Field: Outdoor Dry-Bulb Temperature to Turn On Compressor
-
-This numeric field defines the outdoor air dry-bulb temperature when the compressor is automatically turned back on following an automatic shut off because of low outdoor temperature. This field is only used for the calculation heating seasonal performance factor (HSPF) of heating coil. If this field is not provided, outdoor bin temperature is always considered to be greater than this temperature and    Minimum Outdoor dry-bulb Temperature for Compressor Operation    field described above.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Defrost Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 C and less than or equal to 7.22 C. If this input field is left blank, the default value is 5 C.
-
-#### Field: Crankcase Heater Capacity
-
-This numeric field defines the crankcase heater capacity in Watts. When the outdoor air dry-bulb temperature is below the value specified in the input field    Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation    (described below), the crankcase heater is enabled during the time that the compressor is not running. If this heating coil is used as part of an air-to-air heat pump (Ref. AirLoopHVAC:UnitaryHeatPump:AirToAir or ZoneHVAC:PackagedTerminalHeatPump), the crankcase heater defined for this DX heating coil is enabled during the time that the compressor is not running for either heating or cooling (and the crankcase heater power defined in the DX cooling coil object is disregarded in this case). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0. To simulate a unit without a crankcase heater, enter a value of 0.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which the compressor   s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 C. If this input field is left blank, the default value is 10 C.
-
-#### Field: Defrost Strategy
-
-This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse-cycle.
-
-#### Field: Defrost Control
-
-This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field    Defrost Time Period Fraction    described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field    Maximum Outdoor Dry-bulb Temperature for Defrost Operation    described above. If this input field is left blank, the default defrost control is timed.
-
-#### Field: Defrost Time Period Fraction
-
-This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to    timed    defrost (see Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
-
-#### Field: Resistive Defrost Heater Capacity
-
-This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is    resistive    (see input field    Defrost Strategy    above). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.
-
-#### Field: Region Number
-
-This optional numeric field defines the region number which is used to calculate HSPF of heating coil. The value for this input field must be between 1 and 6. If this input field is left blank, the default value is 4.
-
-#### Field: Evaporator Air Inlet Node Name
-
-This optional alpha field specifies the outdoor air node name used to define the conditions of the air entering the outdoor evaporator. If this field is left blank, the outdoor air temperature entering the evaporator is taken directly from the weather data. If this field is not blank, the node name specified must also be specified in an OutdoorAir:Node object where the height of the node is taken into consideration when calculating outdoor air temperature from the weather data. Alternately, the node name may be specified in an OutdoorAir:NodeList object where the outdoor air temperature is taken directly from the weather data.
-
-#### Field: Zone Name for Evaporator Placement
-
-This input field is name of a conditioned or unconditioned zone where the secondary coil (evaporator) of a heat pump is installed.  This is an optional input field specified only when user desires to extract heat from the zone via secondary coil. Heat extracted is modeled as internal gain. If the primary DX system is a heat pump, then the zone name should be the same as the zone name specified for placing the secondary cooling DX coil.
-
-#### Field: Secondary Coil Air Flow Rate
-
-This input value is the secondary coil (evaporator) air flow rate when the heat pump is working in heating mode or the secondary coil (condenser) air flow rate when the heat pump is working in cooling mode. This input field is auto-sizable.  
-
-#### Field: Secondary Coil Fan Flow Scaling Factor
-
-This input field is scaling factor for autosizing the secondary DX coil fan flow rate.  The secondary air flow rate is determined by multiplying the primary DX coil rated air flow rate by the fan flow scaling factor.  Default value is 1.25. If the secondary coil fan flow rate is not autosized, then the secondary coil fan flow scaling factor is set to 1.0.
-
-#### Field: Nominal Sensible Heat Ratio of Secondary Coil
-
-This input value is the nominal sensible heat ratio used to split the heat extracted by a secondary DX coil (evaporator) of a heat pump into sensible and latent components.  This is an optional input field.  If this input field is left blank, then pure sensible internal heat gain is assumed, i.e., sensible heat ratio of 1.0. 
-
-#### Field: Sensible Heat Ratio Modifier Function of Temperature Curve Name
-
-This input field is name of sensible heat ratio modifier biquadratic curve.  The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary zone air node wet-bulb temperature and the heating DX coil entering air dry-bulb temperature.  This is an optional input field.  If this input field is left blank, then the nominal sensible heat ratio modifier curve value for temperature is set to 1.0.
-
-#### Field: Sensible Heat Ratio Modifier Function of Flow Fraction Curve Name
-
-This input field is name of sensible heat ratio modifier curve as function of secondary air flow fraction. The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary coil air flow fraction. This is an optional input field.  If this input field is left blank, then the sensible heat ratio modifier curve value for flow fraction is set to 1.0.
-
-Following is an example input for the object.
-
-```idf
-Coil:Heating:DX:SingleSpeed,
-   Heat Pump DX Heating Coil 1,     ! Name of heating coil
-   FanAndCoilAvailSched,                   ! Heating coil schedule
-   35000,                                                 ! Gross Rated Heating Capacity
-   2.75,                                                   ! Gross Rated Heating COP
-   1.7,                                                     !rated air flow rate (m3/s)
-   ,                                                       !rated evaporator fan power per volume flow rate (m3/s)
-   Heating Coil Air Inlet Node,     !heating coil air side inlet node
-   SuppHeating Coil Air Inlet Node, !Heating coil air side outlet node
-   HPACHeatCapFT,     ! heating cap modifier curve (temperature, C)
-   HPACHeatCapFFF,   ! heating cap modifier curve (flow fraction)
-   HPACHeatEIRFT,     ! energy input ratio modifier curve (temperature, C)
-   HPACHeatEIRFFF,   ! energy input ratio modifier curve (flow fraction)
-   HPACCOOLPLFFPLR, ! part load fraction modifier curve (function of part load ratio)
-   ,                 ! defrost EIR modifier curve (temp, C) not required for resistive defrost
-   -5.0,                       ! minimum OAT for compressor operation   (C)
-   ,                               ! outdoor dry-bulb temperature to turn on compressor   (C)
-   5.0,                         ! maximum outdoor dry-bulb temp for defrost operation (C)
-   200.0,                     ! Crankcase heater capacity (W)
-   10.0,                       ! Maximum outdoor temp for crankcase heater operation (C)
-   Resistive,             ! Defrost strategy (resistive or reverse-cycle)
-   Timed,                     ! Defrost control (timed or on-demand)
-   0.166667,             ! Defrost time period fraction (used for timed defrost control only)
-   20000;! Resistive defrost heater capacity (used for resistive defrost strategy only)
-```
-
-### DX Heating Coil Outputs
-
-* HVAC,Average,Heating Coil Total Heating Rate [W]
-
-* HVAC,Sum,Heating Coil Total Heating Energy [J]
-
-* HVAC,Average,Heating Coil Electric Power[W]
-
-* HVAC,Sum,Heating Coil Electric Energy [J]
-
-* HVAC,Average,Heating Coil Defrost Electric Power[W]
-
-* HVAC,Sum,Heating Coil Defrost Electric Energy [J]
-
-* HVAC,Average,Heating Coil Crankcase Heater Electric Power[W]
-
-* HVAC,Sum,Heating Coil Crankcase Heater Electric Energy [J]
-
-* HVAC,Average,Heating Coil Runtime Fraction []
-
-
-
-#### Heating Coil Total Heating Rate [W]
-
-This field is the total heating rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Heating Coil Total Heating Energy [J]
-
-This is the total heating output of the DX coil in Joules over the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = CoolingCoils, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Electric Power [W]
-
-This output is the electricity consumption rate of the DX coil compressor and outdoor fan(s) in Watts. This rate is applicable when the unit is providing heating to the conditioned zone(s), and excludes periods when the unit is in reverse-cycle defrost mode.
-
-#### Heating Coil Electric Energy [J]
-
-This is the electricity consumption of the DX coil compressor and condenser fan(s) in Joules for the timestep being reported. This consumption is applicable when the unit is providing heating to the conditioned zone(s), and excludes periods when the unit is in reverse-cycle defrost mode. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Defrost Electric Power [W]
-
-This is the electricity consumption rate of the DX coil unit in Watts when the unit is in defrost mode (reverse-cycle or resistive).
-
-#### Heating Coil Defrost Electric Energy [J]
-
-This is the electricity consumption of the DX coil unit in Joules for the timestep being reported. This consumption is applicable when the unit is in defrost mode (reverse-cycle or resistive).
-
-#### Heating Coil Crankcase Heater Electric Power [W]
-
-This is the average electricity consumption rate of the DX coil compressor   s crankcase heater in Watts for the timestep being reported.
-
-#### Heating Coil Crankcase Heater Electric Energy [J]
-
-This is the electricity consumption of the DX coil compressor   s crankcase heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Miscellaneous, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Runtime Fraction []
-
-This is the runtime fraction of the DX heating coil compressor and outdoor fan(s) for the timestep being reported.
-
-### Coil:Heating:DX:MultiSpeed
-
-This component models a DX heating unit with multiple discrete levels of heating capacity. Currently, this heating coil can only be referenced by a AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed compound object. The multispeed DX heating coil can have from two to four operating speeds. When the coil operates at Speed 1 (the lowest speed), its performance is very similar to the Coil:Heating:DX:SingleSpeed object where the impacts of part-load ratio can be included. When the coil operates at higher speeds (above Speed 1), the linear approximation methodology is applied. The coil outputs at two consecutive speeds are linearly interpolated to meet the required heating capacity during an HVAC system timestep. When the coil performs above the lowest speed, the user can choose if they want to include part-load ratio impacts at the higher speeds.
-
-The multispeed unit is described by specifying the performance at different operating speeds. Each speed has its own set of input specifications: full load capacity, COP and air flow rate at rated conditions, along with modifier curves to determine performance when actual operating conditions are different from the rated conditions.
-
-The coil operates to meet the sensible capacity being requested. When this requested capacity is above the sensible capacity of the highest operating speed, the coil runs continuously at the highest speed. When the requested capacity is between the sensible capacities of two consecutive speeds, the unit will operate a portion of the time at each speed to meet the request. When the requested capacity is less than the low speed (Speed 1) capacity, the unit will cycle on/off as needed.
-
-The next input defines the minimum outdoor dry-bulb temperature where the compressor will operate. The followed two inputs are related to crankcase heater operation: capacity and maximum outdoor dry-bulb temperature for crankcase heater operation. The next six inputs cover defrost operation: defrost EIR modifier curve, the maximum outdoor dry-bulb temperature for defrost operation, the type of defrost strategy (reverse-cycle or resistive), defrost control (timed or on-demand), the fractional defrost time period (timed defrost control only), and the resistive defrost heater capacity if a resistive defrost strategy is selected. The activation of defrost is dependent on outdoor conditions. The capacity reduction and energy use modification are independent of speed. The defrost EIR modifier is described below:
-
-The defrost energy input ratio (EIR) modifier curve (function of temperature) is a bi-quadratic curve with two independent variables: outdoor air dry-bulb temperature and the heating coil entering air wet-bulb temperature. The output of this curve is multiplied by the heating coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the coil is operating. This curve is only required when a reverse-cycle defrost strategy is specified.
-
-The next input allows the user to choose whether to apply the part load fraction correlation to speeds greater than 1 or not. The following input is the type of fuel.
-
-Then the number of speed for heating is entered. The rest of inputs are speed dependent. Each set of data consists of gross rated heating capacity, gross rated COP, and the rated air volume flow rate. These three inputs determine the coil performance at the rating point (outdoor air dry-bulb temperature of 8.33 &deg;C, outdoor air wet-bulb temperature of 6.11 &deg;C, coil entering air dry-bulb temperature of 21.11 &deg;C, coil entering air wet-bulb temperature of 15.55 &deg;C). The rated air volume flow rate should be between .00004027 m<sup>3</sup>/s and .00006041 m<sup>3</sup>/s per watt of gross rated heating capacity. The rated waste heat fraction is needed to calculate how much waste heat is available at the rated conditions. In addition, up to 6 modifier curves are required per speed.
-
-1)        The heating capacity modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the gross rated heating capacity to give the gross total heating capacity at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
-
-2)        The heating capacity modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating.
-
-3)        The energy input ratio (EIR) modifier curve (function of temperature) can be a function of both the outdoor and indoor air dry-bulb temperature or only the outdoor air dry-bulb temperature. User has the choice of a bi-quadratic curve with two independent variables or a quadratic curve as well as a cubic curve with a single independent variable. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the rated EIR (inverse of the rated COP) to give the EIR at specific temperature operating conditions (i.e., at an outdoor or indoor air temperature different from the rating point temperature).
-
-4)        The energy input ratio (EIR) modifier curve (function of flow fraction) is a quadratic or cubic curve with the independent variable being the ratio of the actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the rated EIR (inverse of the rated COP) and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating.
-
-5)        The part load fraction correlation (function of part load ratio) is a quadratic or cubic curve with the independent variable being part load ratio (sensible heating load / steady-state heating capacity). The output of this curve is used in combination with the rated EIR and EIR modifier curves to give the    effective    EIR for a given simulation timestep. The part load fraction correlation accounts for efficiency losses due to compressor cycling.
-
-6)        The waste heat modifier curve (function of temperature) is a bi-quadratic curve with two independent variables: outdoor air dry-bulb temperature and the heating coil entering air dry-bulb temperature. The output of this curve is multiplied by the heating input energy, the waste heat fraction of heat input to give the recoverable waste heat.
-
-The curves are simply specified by name. Curve inputs are described in the curve manager section of this document (ref. Performance Curves).
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a multispeed DX heating coil. Any reference to this DX heating coil by another object will use this name. The only allowed parent is AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed.
-
-#### Field: Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the multispeed DX heating coil can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit must be off for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Air Inlet Node name
-
-This alpha field defines the name of the HVAC system node from which the DX heating coil draws its inlet air.
-
-#### Field: Air Outlet Node Name
-
-This alpha field defines the name of the HVAC system node to which the DX heating coil sends its outlet air.
-
-#### Field: Minimum Outdoor Dry-Bulb Temperature for Compressor Operation
-
-This numeric field defines the minimum outdoor air dry-bulb temperature where the heating coil compressor turns off. The temperature for this input field must be greater than or equal to    20 &deg;C. If this input field is left blank, the default value is -8 &deg;C.
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-#### Field: Crankcase Heater Capacity
-
-This numeric field defines the crankcase heater capacity in Watts. When the outdoor air dry-bulb temperature is below the value specified in the input field    Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation    (described below), the crankcase heater is enabled during the time that the compressor is not running. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0. To simulate a unit without a crankcase heater, enter a value of 0.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which the compressor   s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0 &deg;C. If this input field is left blank, the default value is 10 &deg;C.
-
-#### Field: Defrost Energy Input Ratio Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) during reverse-cycle defrost periods as a function of the outdoor air dry-bulb temperature and the wet-bulb temperature of the air entering the indoor coil. The EIR is the inverse of the COP. The output of this curve is multiplied by the coil capacity, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the indoor and outdoor coils are operating. This curve is only required when a reverse-cycle defrost strategy is selected. The curve is normalized to a value of 1.0 at the rating point conditions.
-
-#### Field: Maximum Outdoor Dry-Bulb Temperature for Defrost Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 &deg;C and less than or equal to 7.22 &deg;C. If this input field is left blank, the default value is 5 &deg;C.
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-#### Field: Defrost Strategy
-
-This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse-cycle.
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-#### Field: Defrost Control
-
-This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field    Defrost Time Period Fraction    described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field    Maximum Outdoor Dry-bulb Temperature for Defrost Operation    described above. If this input field is left blank, the default defrost control is timed.
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-#### Field: Defrost Time Period Fraction
-
-This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to    timed    defrost (see Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
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-#### Field: Resistive Defrost Heater Capacity
-
-This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is    resistive    (see input field    Defrost Strategy    above). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.
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-#### Field: Apply Part Load Fraction to Speeds Greater than 1
-
-This field determines whether part-load impacts on coil energy use are applied when the coil is operating at speeds greater than speed 1. The allowed choices are Yes or No, with the default being No if this field is left blank. Other input fields in this object allow the user to specify a part-load fraction correlation for each speed to account for compressor start up losses (cycle on/off). For the case of a single multi-speed compressor, the part load losses may only be significant when the compressor cycles between speed 1 and off, but the losses may be extremely small when the compressor operates between speed 1 and speed 2 (or between speeds 2 and 3, etc.). In this case, the user may chose to specify **No** for this input field to neglect part-load impacts on energy use at higher operating speeds. If part-load impacts on coil energy use are thought to be significant (e.g., interwined cooling coil with multiple compressors feeding individual refrigerant circuits), then the user may chose to specify **Yes** and the part-load fraction correlations specified for speeds 2 through 4 will be applied as appropriate. The selection for this input field does not affect part-load impacts when the compressor cycles between speed 1 and off   (i.e., the part-load fraction correlation for speed 1 is always applied).
-
-#### Field: Fuel Type
-
-This alpha field determines the type of fuel that the chiller uses.   This field has seven choices: Electricity, NaturalGas, PropaneGas, Coal, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1 and OtherFuel2. The default is NaturalGas.
-
-#### Field: Number of Speeds
-
-This field specifies the number of sets of data being entered for rated specifications, performance curves, and waste heat specifications for each cooling speed. The rated specifications consist of gross rated capacity, gross rated COP, and rated air flow rate. The performance curves consist of a total capacity modifier curve as a function of temperature, total capacity modifier curve as a function of flow fraction, energy input ratio modifier curve as a function of temperature, energy input ratio modifier curve as a function of flow fraction, and part load fraction correlation as a function of part load ratio. The waste heat specifications include the fraction of energy input to the heating coil at the fully loaded and rated conditions, and a temperature modifier. The minimum number of speeds for heating is 2 and the maximum number is 4. The number of speeds should be the same as the number of speeds for heating defined in its parent object (AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed). The first set of performance inputs is for Speed 1 and should be for low speed, and the last set of performance inputs should be for high speed. For example, if only three heating speeds are defined, the first set should be for low speed (Speed 1), the second set should be for medium speed (Speed 2), and the third set should be for high speed (Speed 3). In this example, any performance inputs for Speed 4 would be neglected (since this input field specifies that the coil only has three heating speeds).
-
-#### Field Group: Rated Specification, Performance Curves, and Waste Heat Data
-
-The performance for each heating speed must be specified as shown below. All inputs for Speed 1 are required first, followed by the inputs for Speed 2, Speed 3 and Speed 4.
-
-#### Field: Speed &lt;x&gt; Gross Rated Heating Capacity
-
-This numeric field defines the total, full load gross heating capacity in watts of the DX coil unit at rated conditions for Speed &lt;x&gt; operation (outdoor air dry-bulb temperature of 8.33 &deg;C, outdoor air wet-bulb temperature of 6.11 &deg;C, heating coil entering air dry-bulb temperature of 21.11 &deg;C, heating coil entering air wet-bulb temperature of 15.55 &deg;C, and a heating coil air flow rate defined by field    Rated Air Flow Rate, Speed &lt;x&gt;    below). The value entered here must be greater than 0. The gross heating capacity should not account for the effect of supply air fan heat.
-
-#### Field: Speed &lt;x&gt; Gross Rated Heating COP
-
-This numeric field defines the coefficient of performance (COP=gross heating capacity in watts divided by electrical power input in watts) of the DX heating coil unit at rated conditions for Speed &lt;x&gt; operation (outdoor air dry-bulb temperature of 8.33 &deg;C, outdoor air wet-bulb temperature of 6.11 &deg;C, coil entering air dry-bulb temperature of 21.11 &deg;C, coil entering air wet-bulb temperature of 15.55 &deg;C, and a heating coil air flow rate defined by field    Speed &lt;x&gt; Rated Air Flow Rate    below). The value entered here must be greater than 0. The input power includes power for the compressor(s) and outdoor fan(s) but does not include the power consumption of the indoor supply air fan. The gross heating capacity is the value entered above in the field    Gross Rated Heating Capacity   . The gross COP should NOT account for the supply air fan.
-
-#### Field: Speed &lt;x&gt; Rated Air Flow Rate
-
-This numeric field defines the volume air flow rate, in m<sup>3</sup> per second, across the DX heating coil at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0. The rated air volume flow rate should be between 0.00004027 m<sup>3</sup>/s and 0.00006041 m<sup>3</sup>/s per watt of gross rated heating capacity. The gross rated heating capacity and gross rated COP should be performance information for the unit with outdoor air dry-bulb temperature of 8.33 &deg;C, outdoor air wet-bulb temperature of 6.11 &deg;C, heating coil entering air dry-bulb temperature of 21.11 &deg;C, heating coil entering air wet-bulb temperature of 15.55 &deg;C, and the rated air volume flow rate defined here.
-
-#### Field: Speed &lt;x&gt; Heating Capacity Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the total heating capacity as a function of the both the indoor and outdoor air dry-bulb temperature or just the outdoor air dry-bulb temperature depending on the type of curve selected. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The output of this curve is multiplied by the gross rated heating capacity to give the gross total heating capacity at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or outdoor air dry-bulb temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
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-#### Field: Speed &lt;x&gt; Heating Capacity Function of Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref:   Performance Curves) that parameterizes the variation of heating capacity as a function of the ratio of actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The output of this curve is multiplied by the gross rated heating capacity and the gross heating capacity modifier curve (function of temperature) to give the gross heating capacity at the specific temperature and air flow conditions at which the coil is operating. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the rated air flow rate.
-
-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor and outdoor air dry-bulb temperature or just the outdoor air dry-bulb temperature depending on the type of curve selected. The bi-quadratic curve is recommended if sufficient manufacturer data is available as it provides sensitivity to the indoor air dry-bulb temperature and a more realistic output. The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP) to give the EIR at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or outdoor air dry-bulb temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
-
-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the heating coil to the rated air flow rate (i.e., fraction of full load flow). The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR and the EIR modifier curve (function of temperature) to give the EIR at the specific temperature and air flow conditions at which the coil is operating. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate.
-
-#### Field: Speed &lt;x&gt;Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the    effective    EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
-
-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-           PLF &gt;= 0.7     and     PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional DX heating coil (Speed &lt;x&gt;) would be:
-
-           PLF = 0.85 + 0.15(PLR)
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-           PLF = 1.0 + 0.0(PLR)
-
-####   Field: Speed &lt;x&gt; Rated Waste Heat Fraction of Power Input
-
-The fraction of heat input to heating that is available as recoverable waste heat at full load and rated conditions for Speed &lt;x&gt; operation.
-
-#### Field: Speed &lt;x&gt; Waste Heat Function of Temperature Curve Name
-
-The name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the waste heat recovery as a function of outdoor dry-bulb temperature and the entering coil dry-bulb temperature for Speed &lt;x&gt;. The output of this curve is multiplied by the rated recoverable waste heat at specific temperature operating conditions (i.e., at temperatures different from the rating point). The curve is normalized to a value of 1.0 at the rating point. When the fuel type is electricity, the field is either left blank or ignored by the program. When the fuel type is not electricity and the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed does not require waste heat calculations, this field is ignored. If the field is blank, a warning will be issued and simulation continues. When the fuel type is not electricity and the parent object AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed requires waste heat calculations, if this field is left blank, the program assumes a constant value of 1 to make simulation continue and a warning will be issued. 
-
-#### Field: Zone Name for Evaporator Placement
-
-This input field is name of a conditioned or unconditioned zone where the secondary coil (evaporator) of a heat pump is installed.  This is an optional input field specified only when user desires to extract heat from the zone via secondary coil. Heat extracted is modeled as internal gain. If the primary DX system is a heat pump, then the zone name should be the same as the zone name specified for placing the secondary cooling DX coil.
-
-#### Field: Speed &lt;x&gt; Secondary Coil Air Flow Rate
-
-This input value is the secondary coil (evaporator) air flow rate when the heat pump is working in heating mode or the secondary coil (condenser) air flow rate when the heat pump is working in cooling mode. This input field is auto-sizable.  
-
-#### Field: Speed &lt;x&gt; Secondary Coil Fan Flow Scaling Factor
-
-This input field is scaling factor for autosizing the secondary DX coil fan flow rate.  The secondary air flow rate is determined by multiplying the primary DX coil rated air flow rate by the fan flow scaling factor.  Default value is 1.25. If the secondary coil fan flow rate is not autosized, then the secondary coil fan flow scaling factor is set to 1.0.
-
-#### Field: Speed &lt;x&gt; Nominal Sensible Heat Ratio of Secondary Coil
-
-This input value is the nominal sensible heat ratio used to split the heat extracted by a secondary DX coil (evaporator) of a heat pump into sensible and latent components.  This is an optional input field.  If this input field is left blank, then pure sensible internal heat gain is assumed, i.e., sensible heat ratio of 1.0. 
-
-#### Field: Speed &lt;x&gt; Sensible Heat Ratio Modifier Function of Temperature Curve Name
-
-This input field is name of sensible heat ratio modifier biquadratic curve.  The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary zone air node wet-bulb temperature and the heating DX coil entering air dry-bulb temperature.  This is an optional input field.  If this input field is left blank, then the nominal sensible heat ratio modifier curve value for temperature is set to 1.0.
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-#### Field: Speed &lt;x&gt; Sensible Heat Ratio Modifier Function of Flow Fraction Curve Name
-
-This input field is name of sensible heat ratio modifier curve as function of secondary air flow fraction. The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary coil air flow fraction. This is an optional input field.  If this input field is left blank, then the sensible heat ratio modifier curve value for flow fraction is set to 1.0.
-
-Following is an example input for a multi-speed heating DX coil.
-
-
-
-```idf
-   COIL:Heating:DX:MultiSpeed,
-       Heat Pump DX Heating Coil 1,   !- Name of heat pump heating coil
-       FanAndCoilAvailSched,       !- Availability Schedule
-       Heating Coil Air Inlet Node,   !- Coil Air Inlet Node
-       SuppHeating Coil Air Inlet Node,   !- Coil Air Outlet Node
-       -8.0,                                       !- Minimum Outdoor Dry-bulb Temperature for Compressor Operation {C}
-       200.0,                                     !- Crankcase Heater Capacity {W}
-       10.0,                                       !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation {C}
-       HPACDefrostCAPFT,               !- Defrost energy input ratio modifier curve (temperature)
-       7.22,                                       !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation
-       reverse-cycle,                     !- Defrost Strategy
-       timed,                                     !- Defrost Control
-       0.058333,                               !- Defrost Time Period Fraction
-       2000.0,                                   !- Resistive Defrost Heater Capacity {W}
-       No,                                           !- Apply Part Load Fraction to Speeds greater than 1
-       NaturalGas,                           !- Fuel type
-       4,                                             !- Number of speeds
-       7500,                                       !- Gross Rated Heating Capacity, Speed 1 {W}
-       2.75,                                       !- Gross Rated Heating COP, Speed 1
-       0.45,                                       !- Rated Air Flow Rate, Speed 1 {m3/s}
-       HPACHeatCapFT Speed 1,     !- Heating Capacity Modifier Curve, Speed 1 (temperature)
-       HPACHeatCapFF Speed 1,     !- Heating capacity modifier curve, Speed 1 (flow fraction)
-       HPACHeatEIRFT Speed 1,     !- Energy input ratio modifier curve, Speed 1 (temperature)
-       HPACHeatEIRFF Speed 1,     !- Energy input ratio modifier curve, Speed 1 (flow fraction)
-       HPACHeatPLFFPLR Speed 1, !- Part load fraction correlation, Speed 1 (part load ratio)
-       0.2,                                         !- Rated waste heat fraction of power input, Speed 1
-       HAPCHeatWHFT Speed 1,       !- Waste heat modifier curve, Speed 1 (temperature)
-       17500,                                     !- Gross Rated Heating Capacity, Speed 2 {W}
-       2.75,                                       !- Gross Rated Heating COP, Speed 2
-       0.85,                                       !- Rated Air Flow Rate, Speed 2 {m3/s}
-       HPACHeatCapFT Speed 2,     !- Heating Capacity Modifier Curve, Speed 2 (temperature)
-       HPACHeatCapFF Speed 2,     !- Heating capacity modifier curve, Speed 2 (flow fraction)
-       HPACHeatEIRFT Speed 2,     !- Energy input ratio modifier curve, Speed 2 (temperature)
-       HPACHeatEIRFF Speed 2,     !- Energy input ratio modifier curve, Speed 2 (flow fraction)
-       HPACHeatPLFFPLR Speed 2, !- Part load fraction correlation, Speed 2 (part load ratio)
-       0.2,                                         !- Rated waste heat fraction of power input, Speed 2
-       HAPCHeatWHFT Speed 2,       !- Waste heat modifier curve, Speed 2 (temperature)
-       25500,                                     !- Gross Rated Heating Capacity, Speed 3 {W}
-       2.75,                                       !- Gross Rated Heating COP, Speed 3
-       1.25,                                       !- Rated Air Flow Rate, Speed 3 {m3/s}
-       HPACHeatCapFT Speed 3,     !- Heating Capacity Modifier Curve, Speed 3 (temperature)
-       HPACHeatCapFF Speed 3,     !- Heating capacity modifier curve, Speed 3 (flow fraction)
-       HPACHeatEIRFT Speed 3,     !- Energy input ratio modifier curve, Speed 3 (temperature)
-       HPACHeatEIRFF Speed 3,     !- Energy input ratio modifier curve, Speed 3 (flow fraction)
-       HPACHeatPLFFPLR Speed 3, !- Part load fraction correlation, Speed 3 (part load ratio)
-       0.2,                                         !- Rated waste heat fraction of power input, Speed 3
-       HAPCHeatWHFT Speed 3,       !- Waste heat modifier curve, Speed 3 (temperature)
-       35500,                                     !- Gross Rated Heating Capacity, Speed 4 {W}
-       2.75,                                       !- Gross Rated Heating COP, Speed 4
-       1.75,                                       !- Rated Air Flow Rate, Speed 4 {m3/s}
-       HPACHeatCapFT Speed 4,     !- Heating Capacity Modifier Curve, Speed 4 (temperature)
-       HPACHeatCapFF Speed 4,     !- Heating capacity modifier curve, Speed 4 (flow fraction)
-       HPACHeatEIRFT Speed 4,     !- Energy input ratio modifier curve, Speed 4 (temperature)
-       HPACHeatEIRFF Speed 4,     !- Energy input ratio modifier curve, Speed 4 (flow fraction)
-       HPACHeatPLFFPLR Speed 4, !- Part load fraction correlation, Speed 4 (part load ratio)
-       0.2,                                         !- Rated waste heat fraction of power input, Speed 4
-       HAPCHeatWHFT Speed 4;       !- Waste heat modifier curve, Speed 4 (temperature)
-```
-
-
-
-### MultiSpeed DX Heating Coil Outputs
-
-* HVAC,Average,Heating Coil Total Heating Rate [W]
-
-* HVAC,Sum,Heating Coil Total Heating Energy [J]
-
-* HVAC,Average,Heating Coil Electric Power[W]
-
-* HVAC,Sum,Heating Coil Electric Energy [J]
-
-* HVAC,Average,Heating Coil Defrost Electric Power[W]
-
-* HVAC,Sum,Heating Coil Defrost Electric Energy [J]
-
-* HVAC,Average,Heating Coil Defrost Gas Rate [W]
-
-* HVAC,Sum,Heating Coil Defrost Gas Energy [J]
-
-* HVAC,Average,Heating Coil Crankcase Heater Electric Power[W]
-
-* HVAC,Sum,Heating Coil Crankcase Heater Electric Energy [J]
-
-* HVAC,Average,Heating Coil Runtime Fraction []
-
-If Fuel Type is not Electricity:
-
-* HVAC,Average, Heating Coil &lt;Fuel Type&gt; Rate [W]
-
-* HVAC,Sum, Heating Coil &lt;Fuel Type&gt; Energy [J]
-
-
-
-#### Heating Coil Total Heating Rate [W]
-
-This field is the total heating rate output of the DX coil in Watts. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Heating Coil Total Heating Energy [J]
-
-This is the total heating output of the DX coil in Joules over the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatingCoil, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Electric Power [W]
-
-This output variable is the input fuel type power for the heating coil in the unit of Watts, averaged during the report period. If Fuel Type is not Electricity, the value is zero.
-
-#### Cooling Coil Electric Energy [J]
-
-This output variable is the input fuel type consumption for the multispeed heating coil in the unit of Joules, summed during the report period. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects). If Fuel Type is not Electricity, the value is zero.
-
-#### Heating Coil Defrost Electric Power [W]
-
-This is the electricity consumption rate of the DX coil unit in Watts when the unit is in defrost mode (reverse-cycle or resistive). The variable is available when the defrost mode is resistive or the fuel type is electricity.
-
-#### Heating Coil Defrost Electric Energy [J]
-
-This is the electricity consumption of the DX coil unit in Joules for the timestep being reported. This consumption is applicable when the unit is in defrost mode (reverse-cycle or resistive). The variable is available when the defrost mode is resistive or the fuel type is electricity.
-
-#### Heating Coil Defrost &lt;Fuel Type&gt; Rate [W]
-
-This is the fuel consumption rate of the DX coil unit in Watts when the unit is in defrost mode (reverse-cycle). The variable is available when the defrost mode is reverse-cycle and the fuel type is non-electricity.
-
-#### Heating Coil Defrost &lt;Fuel Type&gt; Energy [J]
-
-This is the fuel consumption of the DX coil unit in Joules for the timestep being reported. This consumption is applicable when the unit is in defrost mode (reverse-cycle). The variable is available when the defrost mode is reverse-cycle and the fuel type is non-electricity.
-
-#### Heating Coil Crankcase Heater Electric Power [W]
-
-This is the average electricity consumption rate of the DX coil compressor   s crankcase heater in Watts for the timestep being reported. When a companion cooling coil exits, the crankcase heater power of the companion cool coil is alos reported in this variable.
-
-#### Heating Coil Crankcase Heater Electric Energy [J]
-
-This is the electricity consumption of the DX coil compressor   s crankcase heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects). When a companion cooling coil exits, the crankcase heater power of the companion cool coil is alos reported in this variable.
-
-#### Heating Coil Runtime Fraction []
-
-This is the runtime fraction of the DX heating coil compressor and outdoor fan(s) for the timestep being reported. When the heating speed is above 1, this output is the run time fraction for the higher speed.
-
-#### Heating Coil &lt;Fuel Type&gt; Rate [W]
-
-This output variable is the input fuel type power for the heating coil in the unit of Watts, averaged during the report period. The electric power is excluded. If Fuel Type is Electricity, this output variable is not reported.
-
-#### Cooling Coil &lt;Fuel Type&gt; Energy [J]
-
-This output variable is the input fuel type consumption for the multispeed heating coil in the unit of Joules, summed during the report period. The electric consumption is excluded. This output is also added to a meter with Resource Type = &lt;Fuel Type&gt;, End Use Key = Heating, Group Key = System (ref. Output:Meter objects). If Fuel Type is Electricity, this output variable is not reported.
-
-Note: The Fuel Type defined in the above two output variables depends on the input in the fuel type filed. In addition to Electricity, Valid fuel types are NaturalGas, Propane, FuelOil\#1, FuelOil\#2, Coal, Diesel, Gasoline, OtherFuel1 and OtherFuel2.
-
-### Coil:Heating:DX:VariableSpeed
-
-The Variable-Speed Air-to-Air Heating DX Coil is a collection of performance curves that represent the heating coil at various speed levels. The performance curves should be generated from the heat pump Reference Unit catalog data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. The number of speed levels can range from 1 to 10. The heating coil has two air side node connections. The user needs to specify a nominal speed level, at which the gross rated capacity and rated volumetric air flow rate are sized. The gross rated capacity and rated volumetric flow rate represent the real situation in the air loop, and are used to determine the flow rates at various speed levels in the parent objects, e.g. AirLoopHVAC:UnitaryHeatPump:AirToAir, ZoneHVAC:PackagedTerminalHeatPump, etc. It shall be mentioned that the performance correction curves, i.e. the temperature and flow fraction correction curves, should be normalized to the capacity and flow rate at each individual speed and at the rated operating conditions, similar to the performance curves used in the single-speed DX coil. On the other hand, the performance values at individual speed levels, e.g. capacities, COPs and flow rates, should be given regarding a specific unit from the Reference Unit catalog data. In the following content, the statement started with    Reference Unit    means the actual Reference Unit catalog data. The rated conditions for obtaining the capacities and COPs   are at indoor dry-bulb temperature of 21.1 ËšC (70 ËšF) and the source side entering air temperature of 8.3 ËšC (47 ËšF). Some equations are provided below to help explain the function of the various performance curves and data fields.
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-#### Field: Name
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-This alpha field contains the identifying name for the variable speed heating coil.
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-#### Field: Air Inlet Node Name
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-This alpha field contains the heating coil load side inlet node name.
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-#### Field: Air Outlet Node Name
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-This alpha field contains the heating coil load side outlet node name.
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-#### Field: Number of Speeds
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-This numeric field contains the maximum number of speed levels that the module uses. The number of speeds, for which the user input the performance data and curves, has to be equal to or higher than the maximum number. The performance inputs at higher speeds are ignored.
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-#### Field: Nominal Speed Level
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-This numeric field defines the nominal speed level, at which the rated capacity, rated air and volumetric flow rate are correlated.
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-#### Field: Gross Rated Heating Capacity at Selected Nominal Speed Level
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-This numeric field contains the rated capacity at the nominal speed level.   This field is autosizable. The gross rated heating capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
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-<div>\[{\rm{CapacityScaleFactor}} = \frac{{{\rm{Gross RatedTotalHeatingCapacity}}}}{{{\rm{ReferenceUnitCapacity}}@{\rm{NominalSpeedLevel}}}}\]</div>
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-And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below,
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-<div>\[\begin{array}{l}{\rm{Gross RatedCapacity}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = \\\quad \quad \quad {\rm{CapacityScaleFactor}} \times \\\quad \quad \quad {\rm{ReferenceUnitCapacity}}@{\rm{SpeedLevel}}({\rm{x}})\end{array}\]</div>
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-#### Field: Rated Volumetric Air Flow Rate
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-This numeric field contains the rated volumetric air flow rate on the load side of the heat pump corresponding to the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects.   It is recommended that the ratio of the rated volumetric air flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
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-<div>\[{\rm{AirFlowScaleFactor}} = \frac{{{\rm{RatedVolumetricAirFlowRate}}}}{{{\rm{ReferenceUnitVolAirFlowRate}}@{\rm{NominalSpeedLevel}} \times {\rm{CapacityScaleFactor}}}}\]</div>
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-And the volumetric air flow rates in the parent objects are calculated as below,
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-#### <span>\(\begin{array}{l}{\rm{LoopVolumetricAirFlowRate}}@{\rm{SpeedLevel}}\left( {\rm{x}} \right) = \\\quad \quad \quad {\rm{AirFlowScaleFactor}} \times \\\quad \quad \quad {\rm{ReferenceUnitVolAirFlowRate}}@{\rm{SpeedLevel}}({\rm{x}}) \times \\\quad {\kern 1pt} {\kern 1pt} \quad \quad {\rm{CapacityScaleFactor}}\end{array}\)</span>
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-#### Field: Part Load Fraction Correlation Curve Name
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-This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, heating load/steady-state heating capacity for Speed 1), in the case that the unit operates under the lowest speed, i.e. on/off. The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the    effective    EIR for a given simulation timestep for Speed 1. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep).
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-#### Field: Defrost Energy Input Ratio Function of Temperature Curve Name
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-This alpha field defines the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) during reverse-cycle defrost periods as a function of the outdoor air dry-bulb temperature and the wet-bulb temperature of the air entering the indoor coil. The EIR is the inverse of the COP. The output of this curve is multiplied by the coil capacity at the maximum speed level, the fractional defrost time period and the runtime fraction of the heating coil to give the defrost power at the specific temperatures at which the indoor and outdoor coils are operating. This curve is only required when a reverse cycle defrost strategy is selected. The curve is normalized to a value of 1.0 at the rating point conditions.
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-#### Field: Minimum Outdoor Dry-Bulb Temperature for Compressor Operation
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-This numeric field defines the minimum outdoor air dry-bulb temperature where the heating coil compressor turns off. If this input field is left blank, the default value is -8  &deg;C.
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-#### Field: Outdoor Dry-Bulb Temperature to Turn On Compressor
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-This numeric field defines the outdoor temperature when the compressor is automatically turned back on following an automatic shut off because of low outdoor dry-bulb temperature. This field is only used for the calculation of HSPF. If this field is not provided, then outdoor bin temperature used in the HSPF calculation is always considered to be greater than this temperature and 'Minimum Outdoor Dry-Bulb Temperature for Compressor Operation' field described above. This assumption is based on AHRI standard 210/240 (2008) and can introduce significant error in the final value of HSPF.
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-#### Field: Maximum Outdoor Dry-Bulb Temperature for Defrost Operation
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-This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0  &deg;C and less than or equal to 7.22  &deg;C. If this input field is left blank, the default value is 5  &deg;C.
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-#### Field: Crankcase Heater Capacity
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-This numeric field defines the crankcase heater capacity in Watts. When the outdoor air drybulb temperature is below the value specified in the input field    Maximum Outdoor Dry-bulb Temperature for Crankcase Heater Operation    (described below), the crankcase heater is enabled during the time that the compressor is not running. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0. To simulate a unit without a crankcase heater, enter a value of 0.
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-#### Field: Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation
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-This numeric field defines the outdoor air dry-bulb temperature above which the compressor   s crankcase heater is disabled. The value for this input field must be greater than or equal to 0.0  &deg;C. If this input field is left blank, the default value is 10  &deg;C.
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-#### Field: Defrost Strategy
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-This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse cycle.
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-#### Field: Defrost Control
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-This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field    Defrost Time Period Fraction    described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field    Maximum Outdoor Dry-bulb Temperature for Defrost Operation    described above. If this input field is left blank, the default defrost control is timed.
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-#### Field: Defrost Time Period Fraction
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-This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to    timed    defrost (see Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
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-#### Field: Resistive Defrost Heater Capacity
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-This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is    resistive    (see input field    Defrost Strategy    above). The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.
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-#### Field Group: Rated specification and performance curves
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-The performance for each heating speed must be specified as shown below. They should be directly given from the Reference Unit data. All inputs for Speed 1 are required, followed by the optional inputs for other speeds.
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-#### Field: Speed &lt;x&gt; Reference Unit Gross Rated Heating Capacity
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-This numeric field defines the total, full load gross heating capacity in watts of the air-to-air heating coil unit at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0. The gross heating capacity should not account for the effects of supply air fan heat.
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-#### Field: Speed &lt;x&gt; Reference Unit Gross Rated Heating COP
-
-This numeric field defines the coefficient of performance (COP=gross heating capacityin watts divided by electrical power input in watts) of the heating coil unit at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0. The input power includes   power for the compressor(s), the outdoor coil fan and accessories, but does not include the power consumption of the indoor supply air fan. The gross COP should NOT account for the supply air fan.
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-#### Field: Speed &lt;x&gt; Reference Unit Rated Air Flow Rate
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-This numeric field defines the volume air flow rate, in m<sup>3</sup> per second, across the heating coil at rated conditions for Speed &lt;x&gt; operation. The value entered here should be directly from the Reference Unit data, corresponding to the given gross rated heating capacity and gross rated heating COP at the speed, as above.
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-#### Field: Speed &lt;x&gt; Heating Capacity Function of Temperature Curve Name
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-This alpha field defines the name of a bi-quadratic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the total heating capacity as a function of the indoor dry-bulb and source side entering air temperature, from the Reference Unit. The output of this curve is multiplied by the gross rated heating capacity at the speed to give the gross heating capacity at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or entering air temperature different from the rating point temperature). It should be noted that the curve is normalized to the heating capacity at Speed&lt;x&gt; from the Reference Unit data, and have the value of 1.0 at the rating point.
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-#### Field: Speed &lt;x&gt; Heating Capacity Function of Air Flow Fraction Curve Name
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-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the gross heating capacity as a function of the ratio of actual air flow rate across the heating coil to the design air flow rate (i.e., fraction of full load flow), at Speed &lt;x&gt; from the Reference Unit data. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the design air flow rate at Speed &lt;x&gt;.
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-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Temperature Curve Name
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-This alpha field defines the name of a bi-quadratic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor air dry-bulb and entering air temperatures. The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP at Speed &lt;x&gt; from the Reference Unit data) to give the EIR at specific temperature operating conditions (i.e., at an indoor air dry bulb temperature or entering air temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
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-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Air Flow Fraction Curve Name
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-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the heating coil to the design air flow rate (i.e., fraction of full load flow, at Speed &lt;x&gt; from the Reference Unit data). The EIR is the inverse of the COP. This curve is normalized to a value of 1.0 when the actual air flow rate equals the design air flow rate.
-
-
-
-An example of this statement in an IDF is:
-
-```idf
-Coil:Heating:DX:VariableSpeed,
-       Heat Pump DX Heating Coil 1,         !- Name
-       Heating Coil Air Inlet Node,         !- Air Inlet Node Name
-       SuppHeating Coil Air Inlet Node,   !- Air Outlet Node Name
-       10.0,                                     !- Number of Speeds {dimensionless}
-       10.0,                                     !- Nominal Speed Level {dimensionless}
-       35000,                                   !- Gross Rated Heating Capacity {W}
-       1.7,                                         !- Rated Air Flow Rate {m3/s}
-       HPACCOOLPLFFPLR,                 !- Part Load Fraction Correlation Curve Name
-       ,                                               !- Defrost Energy Input Ratio Function of Temperature Curve Name
-       -5.0,                                       !- Minimum Outdoor Dry-Bulb Temperature for Compressor Operation {C}
-       ,                                               !- Outdoor Dry-Bulb Temperature to Turn Back On Compressor{C}
-       5.0,                                         !- Maximum Outdoor Dry-Bulb Temperature for Defrost Operation {C}
-       200.0,                                     !- Crankcase Heater Capacity {W}
-       10.0,                                       !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
-       Resistive,                             !- Defrost Strategy
-       TIMED,                                     !- Defrost Control
-       0.166667,                               !- Defrost Time Period Fraction
-       20000,                                     !- Resistive Defrost Heater Capacity {W}
-       1838.7,                                   !- Speed 1 Gross Rated Heating Capacity {w}
-       5.0,                                         !- Speed 1 Gross Rated Heating COP {dimensionless}
-       0.1661088,                             !- Speed 1 Rated Air Flow Rate {m3/s}
-       HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       2295.5,                                   !- Speed 2 Gross Rated Heating Capacity {w}
-       5.0,                                         !- Speed 2 Gross Rated Heating COP {dimensionless}
-       0.179322,                               !- Speed 2 Rated Air Flow Rate {m3/s}
-       HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       2751.3,                                   !- Speed 3 Gross Rated Heating Capacity {w}
-       5.0,                                         !- Speed 3 Gross Rated Heating COP {dimensionless}
-       0.1925352,                             !- Speed 3 Rated Air Flow Rate {m3/s}
-       HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       3659.6,                                   !- Speed 4 Gross Rated Heating Capacity {w}
-       5.0,                                         !- Speed 4 Gross Rated Heating COP {dimensionless}
-       0.2189616,                             !- Speed 4 Rated Air Flow Rate {m3/s}
-       HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       4563.7,                                   !- Speed 5 Gross Rated Heating Capacity {w}
-       5.0,                                         !- Speed 5 Gross Rated Heating COP {dimensionless}
-       0.245388,                               !- Speed 5 Rated Air Flow Rate {m3/s}
-       HPACHeatCapFT,                     !- Total Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Total Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       5463.3,                                   !- Speed 6 Gross Rated Heating Capacity {w}
-       5.0,                                         !- Speed 6 Gross Rated Heating COP {dimensionless}
-       0.2718144,                             !- Speed 6 Rated Air Flow Rate {m3/s}
-       HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       6358.4,                                   !- Speed 7 Gross Rated Heating Capacity {w}
-       5.0,                                         !- Speed 7 Gross Rated Heating COP {dimensionless}
-       0.2982408,                             !- Speed 7 Rated Air Flow Rate {m3/s}
-       HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       7248.5,                                   !- Speed 8 Gross Rated Heating Capacity {w}
-       5.0,                                         !- Speed 8 Gross Rated Heating COP {dimensionless}
-       0.3246672,                             !- Speed 8 Rated Air Flow Rate {m3/s}
-       HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       8133.6,                                   !- Speed 9 Gross Rated Heating Capacity {w}
-       5.0,                                         !- Speed 9 Gross Rated Heating COP {dimensionless}
-       0.3510936,                             !- Speed 9 Rated Air Flow Rate {m3/s}
-       HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       9013.2,                                   !- Speed 10 Gross Rated Heating Capacity {w}
-       5.0,                                         !- Speed 10 Gross Rated Heating COP {dimensionless}
-       0.37752,                                 !- Speed 10 Rated Air Flow Rate {m3/s}
-       HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF;                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-```
-
-### Variable Speed DX Heating Coil Outputs
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-* HVAC,Average,Heating Coil Electric Power [W]
-
-* HVAC,Average,Heating Coil Heating Rate [W]
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-* HVAC,Average,Heating Coil Sensible Heating Rate [W]
-
-* HVAC,Average,Heating Coil Source Side Heat Transfer Rate [W]
-
-* HVAC,Average,Heating Coil Part Load Ratio []
-
-* HVAC,Average, Heating Coil Runtime Fraction []
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-* HVAC,Average, Heating Coil Air Mass Flow Rate [kg/s]
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-* HVAC,Average,Heating Coil Air Inlet Temperature [C]
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-* HVAC,Average,Heating Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
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-* HVAC,Average,Heating Coil Air Outlet Temperature [C]
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-* HVAC,Average,Heating Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
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-* HVAC,Average,Heating Coil Upper Speed Level []
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-* HVAC,Average,Heating Coil Neighboring Speed Levels Ratio []
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-* HVAC,Average,VSAirtoAirHP Recoverable Waste Heat [W]
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-* HVAC,Sum,Heating Coil Electric Energy [J]
-
-* HVAC,Sum,Heating Coil Heating Energy [J]
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-* HVAC,Sum,Heating Coil Source Side Heat Transfer Energy [J]
-
-* HVAC,Average,Heating Coil Defrost Electric Power [W]
-
-* HVAC,Sum,Heating Coil Defrost Electric Energy [J]
-
-* HVAC,Average,Heating Coil Crankcase Heater Electric Power[W]
-
-* HVAC,Sum,Heating Coil Crankcase Heater Electric Energy [J]
-
-#### Heating Coil Electric Power [W]
-
-This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
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-#### Heating Coil Heating Rate [W]
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-The output variable is the average total heating capacity provide by the heat pump in Watts over the timestep being reported.
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-#### Heating Coil Sensible Heating Rate [W]
-
-The output variable is the average sensible heating capacity provide by the heat pump in Watts over the timestep being reported. For heating mode, the sensible capacity is equal to the total capacity.
-
-#### Heating Coil Source Side Heat Transfer Rate [W]
-
-The output variable is the average heat absorbed at the heat pump evaporator in Watts over the timestep being reported.
-
-#### Heating Coil Part Load Ratio   []
-
-This output variable is the ratio of the part-load capacity to the steady state capacity of the heating coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the heating coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
-
-#### Heating Coil Runtime Fraction []
-
-This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The duty factor or part load fraction accounts for efficiency losses due to compressor cycling.
-
-#### Heating Coil Air Mass Flow Rate [kg/s]
-
-The output variable is the average air mass flow rate on the load side going through the heat pump over the timestep being reported.
-
-#### Heating Coil Air Inlet Temperature [C]
-
-The output variable is the average entering air dry-bulb temperature over the timestep being reported.
-
-#### Heating Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average entering air dry humidity ratio over the timestep being reported.
-
-#### Heating Coil Air Outlet Temperature [C]
-
-The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
-
-#### Heating Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average leaving air dry humidity ratio over the timestep being reported.
-
-#### Heating Coil Upper Speed Level []
-
-The output variable is the average upper speed level, for interpolating performances between two neighboring speed levels.
-
-#### Heating Coil Neighboring Speed Levels Ratio []
-
-The output variable is the average speed ratio, for interpolating performances between two neighboring speed levels.
-
-#### Heating Coil Electric Energy [J]
-
-The output variable is the total electric consumption of the heat pump in Joules over the timestep being reported.
-
-#### Heating Coil Heating Energy [J]
-
-The output variable is the total cooling output of the coil in Joules over the timestep being reported.
-
-#### Heating Coil Source Side Heat Transfer Energy [J]
-
-The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported.
-
-#### Heating Coil Defrost Electric Power[W]
-
-The output variable is the average electric power used for defrosting, in Watts over the timestep being reported.
-
-#### Heating Coil Defrost Electric Energy [J]
-
-The output variable is the total electric defrosting energy usage of the coil in Joules over the timestep being reported.
-
-#### Heating Coil Crankcase Heater Electric Power [W]
-
-The output variable is the average power used for crankcase heater, in Watts over the timestep being reported.
-
-#### Heating Coil Crankcase Heater Electric Energy [J]
-
-The output variable is the total electric energy usage of the coil for crankcase heater, in Joules over the timestep being reported.
-
-### Coil:WaterHeating:Desuperheater
-
-A simplified approach is used to determine the performance of this water heating coil. The model assumes that the heating energy provided by this coil is reclaimed from the superheated refrigerant gas leaving a compressor (i.e., a desuperheating refrigerant-to-water heating coil) and does not impact the performance of the compressor. This coil must be used with a water heater tank (e.g., WaterHeater:Mixed) which can supply heated potable water and/or hot water for use in a plant loop (e.g., hydronic air reheat coils).
-
-Except for detailed refrigeration system models, the amount of available superheat is simply a percentage of the total heat being rejected by the DX system   s condenser. Approximately 25-30% of the energy rejected by typical refrigeration system condensers is to reduce the superheated refrigerant vapor temperature to the condensing temperature. Recovery efficiencies higher than 30% may cause the refrigerant gas to condense which in turn impacts the performance of the refrigeration system. For this reason, the maximum heat reclaim recovery efficiency for this coil is 30% for most sources of waste heat, including refrigeration compressor racks. The one exception to this 30% limit is a condenser that is part of a detailed refrigeration system. In a detailed refrigeration system, the portion of the rejected heat that lies within the superheated region is explicitly calculated. Therefore, the desuperheater coils supplied by a condenser attached to a detailed refrigeration system are subject to a maximum reclaim recovery efficiency of 90% of the heat within the superheated region.
-
-The model includes the ability to modify the heat reclaim recovery efficiency based on variations in inlet water temperature and outdoor air dry-bulb temperature.
-
-This coil model performs the following major functions:
-
-- calculates the amount of heat delivered to the water tank
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-- calculates the electricity consumption of the integral water pump and on/off-cycle parasitic loads
-
-The input fields for this object are described below in detail:
-
-#### Field: Name
-
-This alpha field contains a unique user-assigned name for an instance of a desuperheater water heating coil. Any reference to this desuperheater coil by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the name of the schedule (ref: Schedule) that denotes whether the desuperheater coil is available to operate during a given time period. A schedule value equal to 0 denotes that the desuperheater coil is off for that time period. A value other than 0 denotes that the desuperheater coil is available to operate during that time period. During times when the desuperheater coil is scheduled off, the heater (element or burner) in the water tank object operates based on its tank set point temperature schedule and the desuperheater coil   s parasitic electric power is also off for that time period. If this field is blank, the schedule has values of 1 for all time periods.
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-#### Field: Setpoint Temperature Schedule Name
-
-This alpha field contains the name of the schedule (ref: Schedule) that specifies the set point (or    cut-out   ) temperature for the desuperheater coil. Temperature values used in this schedule should be in degrees Celsius. The desuperheater coil turns off when the tank water reaches this set point temperature. Once the desuperheater coil is off, the tank water temperature floats downward until it falls below the set point temperature minus the dead band temperature difference defined below (i.e., the    cut-in    temperature). At this point, the desuperheater coil turns on and remains on until the desuperheater coil set point temperature is reached.
-
-#### Field: Dead Band Temperature Difference
-
-This numeric field contains the dead band temperature difference in degrees Celsius. The desuperheater coil    cut-in    temperature is defined as the desuperheater coil set point temperature defined above minus this dead band temperature difference. The desuperheater coil turns on when the water temperature in the tank falls below the    cut-in    temperature. The desuperheater coil remains on until the water temperature in the tank rises above the desuperheater coil set point (   cut-out   ) temperature defined above. The dead band temperature difference must be greater than 0 &deg;C and less than or equal to 20 &deg;C. If this field is left blank, the default value is 5 &deg;C.
-
-Desuperheater water heating coils are typically used to offset energy consumption by the water tank   s heater (element or burner). Therefore, the cut-in temperature for the desuperheater coil (set point minus dead band temperature difference) is usually higher than the set point temperature for the heater (element or burner) in the associated water heater tank object. At times when the water heater tank set point temperature is greater than the cut-in temperature of the desuperheater coil, the model disables the desuperheater coil and the tank   s heater is used to heat the water.
-
-#### Field: Rated Heat Reclaim Recovery Efficiency
-
-This numeric field defines the ratio of recovered waste heat from the superheated refrigerant gas to the total rejected waste heat from the heating source (as if no heat reclaim occurred). Input values must be greater than 0 up to a   maximum value is 0.3 (with a defaults of 0.25) for most sources of waste heat, including refrigeration compressor racks. The one exception to this 0.3 limit is a source that is a condenser that is part of a detailed refrigeration system. In a detailed refrigeration system, the portion of the rejected heat that lies within the superheated region is explicitly calculated. Therefore, the desuperheater coils supplied by a condenser attached to a detailed refrigeration system are subject to a maximum reclaim recovery efficiency of 0.9. with a   default value is 0.8.
-
-#### Field: Rated Inlet Water Temperature
-
-This numeric field defines the coil inlet water temperature, in degrees Celsius, that corresponds to the rated heat reclaim recovery efficiency. Also see field    Heat Reclaim Efficiency Modifier Curve Name (function of temperature)    below.
-
-#### Field: Rated Outdoor Air Temperature
-
-This numeric field defines the outdoor air dry-bulb temperature, in degrees Celsius, that corresponds to the rated heat reclaim recovery efficiency. The outdoor air dry-bulb temperature impacts the desuperheater coil refrigerant temperature and the amount of heat available for reclaim. Also see field    Heat Reclaim Efficiency Modifier Curve Name(function of temperature)    below.
-
-#### Field: Maximum Inlet Water Temperature for Heat Reclaim
-
-This numeric field defines the maximum coil inlet water temperature in degrees Celsius. Any time the inlet water temperature to the desuperheater coil is above this maximum allowed temperature, heat reclaim is restricted so that the tank water does not exceed this temperature.
-
-#### Field: Heat Reclaim Efficiency Function of Temperature Curve Name
-
-This alpha field specifies the name of a bi-quadratic curve object (ref: Performance Curves) that defines the variation in heat reclaim efficiency as a function of inlet fluid (air and water) temperatures. The bi-quadratic curve uses the coil inlet water temperature and outdoor air dry-bulb temperature (entering the DX coil condenser) as the independent variables. The output of this curve is multiplied by the rated heat reclaim recovery efficiency to give the heat reclaim efficiency at specific operating conditions (i.e., at temperatures different from the rating point temperatures). The curve should be normalized to have the value of 1.0 at the rating point temperatures. If this field is left blank, the heat reclaim efficiency remains constant (curve value assumed to be 1.0 for all conditions). The model restricts the product of the output of this curve and the rated heat reclaim recovery efficiency to a maximum of 0.9 for refrigeration condenser sources and 0.3 for all other sources..
-
-#### Field: Water Inlet Node Name
-
-This alpha field defines the name of the water node from which the desuperheater heating coil draws its inlet water. This node name must also match the source side outlet node name for the water heater tank used with this coil (ref. Water Heaters).
-
-#### Field: Water Outlet Node Name
-
-This alpha field defines the name of the water node to which the desuperheater heating coil sends its outlet water. This node name must also match the source side inlet node name for the water heater tank used with this coil (ref. Water Heaters).
-
-#### Field: Tank Object Type
-
-This alpha (choice) field contains the type of water heater tank used by this desuperheater heating coil. Currently, the only valid choice is WaterHeater:Mixed.
-
-#### Field: Tank Name
-
-This alpha field contains the name of the specific water heater tank (WaterHeater:Mixed object) used by this desuperheater heating coil.
-
-#### Field: Heating Source Object Type
-
-This alpha (choice) field defines the source of superheated refrigerant gas from which the desuperheater water heating coil recovers energy through heat reclaim. Valid choices are:
-
-This alpha (choice) field defines the source of superheated refrigerant gas from which the desuperheater water heating coil recovers energy through heat reclaim. Valid choices are:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* Coil:Cooling:DX:TwoSpeed
-
-* Coil:Cooling:DX:TwoStageWithHumidityControlMode
-
-* Refrigeration:CompressorRack
-
-* Refrigeration:Condenser:AirCooled
-
-* Refrigeration:Condenser:EvaporativeCooled
-
-* Refrigeration:Condenser:WaterCooled
-
-#### Field: Heating Source Name
-
-This alpha field defines the name of the desuperheater coil   s heat source (e.g., the name of a specific coil of the type mentioned in the previous field which provides waste heat to this desuperheater water heating coil).
-
-#### Field: Water Flow Rate
-
-This numeric field defines the desuperheater coil   s water flow rate in cubic meters per second. The model assumes that this flow rate is constant (throughout the simulation period) when the desuperheater coil operates, and that it corresponds to the heat reclaim recovery efficiency performance specified by the user. This water flow rate must be greater than zero.
-
-#### Field: Water Pump Power
-
-This numeric field defines the coil   s water circulation pump power in Watts. This is the operating pump power as installed. Values must be greater than or equal to 0. If this field is left blank, the default value is 0. A warning message will be issued if the ratio of water pump power to desuperheater water volumetric flow rate exceeds 7.9264E6 W/m<sup>3</sup>/s, but the simulation will continue using the user-defined values. The model assumes that this integral pump (i.e., no need to define a separate pump object) cycles on and off with the desuperheater heating coil.
-
-#### Field: Fraction of Pump Heat to Water
-
-This numeric field defines the fraction of water circulation pump heat that is transferred to the water. The pump is assumed to be downstream of the desuperheater water heating coil, and this field is used to determine the desuperheater water outlet temperature. Values must be greater than or equal to 0 and less than or equal to 1. If this field is left blank, the default value is 0.2.
-
-#### Field: On-Cycle Parasitic Electric Load
-
-This optional numeric field contains the on-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the desuperheater water heating coil. This parasitic electric load is consumed whenever the desuperheater coil is operating, and the model assumes that this parasitic power does not contribute to heating the water nor does it affect the zone air heat balance. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
-
-#### Field: Off-Cycle Parasitic Electric Load
-
-This optional numeric field contains the off-cycle parasitic electric power in Watts. This is the parasitic electric power consumed by controls or other electrical devices associated with the desuperheater water heating coil. This parasitic electric load is consumed whenever the desuperheater coil is available but is not operating, and the model assumes that this parasitic power does not contribute to heating the water nor does it affect the zone air heat balance. The minimum value for this field is 0.0, and the default value is also 0.0 if this field is left blank.
-
-
-
-Following is an example input for a desuperheater water heating coil.
-
-```idf
-Coil:WaterHeating:Desuperheater,
-       WaterHeatingCoil,               !- Coil Name
-       DesuperheaterSched,           !- Availability Schedule Name
-       DesuperheaterTempSch,       !- Desuperheater Coil Set Point Temperature Schedule Name
-       5.0,                                         !- Dead Band Temperature Difference {deltaC}
-       0.25,                                       !- Rated Heat Reclaim Recovery Efficiency
-       50.0,                                       !- Rated Inlet Water Temperature {C}
-       35.0,                                       !- Rated Outdoor Air Temperature {C}
-       60.0,                                       !- Maximum Inlet Water Temperature for Heat Reclaim {C}
-       HEffFTemp,                             !- Heat Reclaim Efficiency Modifier Curve Name (function of temperature)
-       WaterHeatingCoilInletNode,     !- Desuperheater Water Inlet Node Name
-       WaterHeatingCoilOutletNode,   !- Desuperheater Water Outlet Node Name
-       WaterHeater:Mixed,           !- Water Heater Tank Type
-       WaterHeatingCoilTank,       !- Water Heater Tank Name
-       Coil:Cooling:DX:SingleSpeed,   !- Heating Source Type
-       Furnace ACDXCoil 1,           !- Heating Source Name
-       0.0001,                                   !- Desuperheater Water Volumetric Flow Rate {m3/s}
-       100.0,                                     !- Water Pump Power {W}
-       0.2,                                         !- Fraction of Pump Heat to Water
-       10.0,                                       !- On-Cycle Parasitic Electric Load {W}
-       10.0;                                       !- Off-Cycle Parasitic Electric Load {W}
-```
-
-
-
-### WaterHeating Coil (Desuperheater) Outputs
-
-* HVAC,Average,Water Heater Part Load Ratio
-
-* HVAC,Average,Water Heater Heating Rate [W]
-
-* HVAC,Sum,Water Heater Heating Energy [J]
-
-* HVAC,Average,Water Heater Pump Electric Power [W]
-
-* HVAC,Sum,Water Heater Pump Electric Energy [J]
-
-* HVAC,Average,Water Heater Heat Reclaim Efficiency Modifier Multiplier []
-
-* HVAC,Average,Water Heater On Cycle Parasitic Electric Power [W]
-
-* HVAC,Sum,Water Heater On Cycle Parasitic Electric Energy [J]
-
-* HVAC,Average,Water Heater Off Cycle Parasitic Electric Power [W]
-
-* HVAC,Sum,Water Heater Off Cycle Parasitic Electric Energy [J]
-
-Water Heater Part Load Ratio []This output field contains the part load ratio of the desuperheater heating coil for the timestep being reported. This ratio represents the fraction of the timestep that the desuperheater heating coil is operating.
-
-#### Water Heater Heating Rate [W]
-
-This output field contains the average heating rate output of the desuperheater heating coil in Watts for the timestep being reported. This value includes the portion of circulation pump heat attributed to heating the water.
-
-#### Water Heater Heating Energy [J]
-
-This output field contains the total heating output of the desuperheater heating coil in Joules for the timestep being reported. This value includes the portion of circulation pump heat attributed to heating the water.
-
-#### Water Heater Pump Electric Power [W]
-
-This output field contains the average electricity consumption rate for the water circulation pump in Watts for the timestep being reported.
-
-#### Water Heater Pump Electric Energy [J]
-
-This output field contains the electricity consumption of the water circulation pump in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key= DHW, Group Key= Plant (ref. Output:Meter objects).
-
-#### Water Heater Heat Reclaim Efficiency Modifier Multiplier []
-
-This output field contains the average output of the Heat Reclaim Efficiency Modifier Curve (function of temperature) for the timestep being reported.
-
-#### Water Heater On Cycle Parasitic Electric Power [W]
-
-#### Water Heater On Cycle Parasitic Electric Energy [J]
-
-#### Water Heater Off Cycle Parasitic Electric Power [W]
-
-#### Water Heater Off Cycle Parasitic Electric Energy [J]
-
-These outputs are the parasitic electric power and consumption associated with the desuperheater water heating coil. Specific outputs represent parasitic electrical usage during the coil on and off cycles. These outputs represent electronic controls or other electric component. The model assumes that the parasitic power does not contribute to heating the water nor does it impact the zone air heat balance. The parasitic electric consumption outputs are also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
-
-### CoilSystem:Cooling:DX
-
-The CoilSystem:Cooling:DX object is a virtual container component that consists of a DX cooling coil component and its associated controls, as shown in the Figure below. This control object supports several different types of DX cooling coils (see field Cooling Coil Object Type).
-
-This component may be used as a cooling coil in constant volume or variable volume systems, as blow through or draw through, with or without humidity controls. Unlike AirLoopHVAC:Unitary system types, this component controls only the DX coil, not the supply fan.   CoilSystem:Cooling:DX is added to a system by placing it in an air loop branch (see Branch object) or in an AirLoopHVAC:OutdoorAirSystem:EquipmentList or in a ZoneHVAC:OutdoorAirUnit:EquipmentList . It requires one or more setpoint manager (see SetpointManager:\*) objects to specify temperature and/or humidity setpoints (unless it is used in a ZoneHVAC:OutdoorAirUnit which has its own temperature setpoints).   This object is the one that is listed in the Branch or equipment list object rather than the coil itself.   A constant volume or variable volume fan is modeled separately from this cooling system. These are the only fan types allowed for this system type (ref. Fan:ConstantVolume and Fan:VariableVolume).   Cycling fan operation is not available with this model. The CoilSystem:Cooling:DX object can also be placed on dedicated outdoor air system (DOAS) airloop branches or in arloop branches where the air flow to capacity ratio range is between 100     300 cfm/ton. 100% DOAS DX cooling coils operate in lower flow to capacity ratio range compared to regular DX cooling coils. The CoilSystem:Cooling:DX is selected to operate in DOAS application or in low flow to capacity ratio range by specifying    YES    to the input field    Use Outdoor Air DX Cooling Coil   . If this optional input field is left blank or specified as    NO   , then the coil is modeled as regular DX cooling coil. If the CoilSystem:Cooling:DX object is in an AirLoopHVAC:OutdoorAirSystem:EquipmentList or in a ZoneHVAC:OutdoorAirUnit:EquipmentList then it is treated as 100% DOAS DX cooling coil only if the choice input field    Use Outdoor Air DX Cooling Coil    is set too    YES   . All the control options of the regular DX cooling coils are available to DOAS DX coils as well. Heating DX coils in DOAS airloop operate at the same flow to capacity ratio limits as the DOAS DX cooling coils.
-
-![DXAirLoop](media/image368.svg)
-
-Figure 138. Schematic of CoilSystem:Cooling:DX Object in an Air Loop for a Blow Through Application
-
-#### Field: Name
-
-This alpha field contains the identifying name for this component.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name that contains information on the availability of the DX coil to operate. A schedule value of 0 indicates that the coil is off for that time period. A schedule value greater than 0 indicates that the coil can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: DX Cooling Coil System Inlet Node Name
-
-This alpha field contains the identifying name given to the DX cooling coil inlet node, as specified in the DX cooling coil object.
-
-#### Field: DX Cooling Coil System Outlet Node Name
-
-This alpha field contains the identifying name given to the DX cooling coil outlet node, as specified in the cooling coil object.
-
-#### Field: DX Cooling Coil System Sensor Node Name
-
-This alpha field contains the identifying name given to the DX cooling coil control node, this is the node at which the temperature set point is specified by the set point manager.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field specifies the type of DX cooling coil. The valid choices for this field are:
-
-* Coil:Cooling:DX:SingleSpeed
-
-* CoilSystem:Cooling:DX:HeatExchangerAssisted
-
-* Coil:Cooling:DX:TwoSpeed
-
-* Coil:Cooling:DX:TwoStageWithHumidityControlMode
-
-* Coil:Cooling:DX:VariableSpeed
-
-#### Field: Cooling Coil Name
-
-This alpha field contains the identifying name of the DX cooling coil.
-
-As shown in the example below, correct specification of this system requires specification of the DX Cooling Coil object in addition to the CoilSystem:Cooling:DX object.
-
-#### Field: Dehumidification Control Type
-
-This alpha field contains the type of dehumidification control. The following options are valid for this field:
-
-**None** - meet sensible load only, no active dehumidification control
-
-**MultiMode** - activate enhanced dehumidification mode as needed and operate to meet the sensible load. If a sensible load exists, the system will operate to meet that sensible load and may not meet the latent load. If no sensible load exists, and Run on Latent Load = Yes, the system will operate to meet the entire latent load. This option is used to model DX equipment with a switchable option such as subcool reheat. It is valid only with Cooling coil type= Coil:Cooling:DX:TwoStageWithHumidityControlMode or CoilSystem:Cooling:DX:HeatExchangerAssisted. If the Run on Latent Load option below is set to Yes, this option may require the use of a heating coil and heating coil outlet air temperature set point manager downstream of this cooling coil to maintain the temperature set point.
-
-**CoolReheat** - cool beyond the dry-bulb setpoint as required to meet the humidity setpoint. It is valid only with Cooling coil type=Coil:Cooling:DX:TwoStageWithHumidityControlMode. This option requires the use of a heating coil and heating coil outlet air temperature set point manager downstream of this cooling coil to maintain the temperature set point.
-
-The default is **None**. For all dehumidification controls, the max humidity setpoint on the control node is used. This must be set using a **ZoneControl:Humidistat** **ZoneControl:Humidistat** and one of:
-
-- **SetpointManager:SingleZone:Humidity:Maximum**
-
-- **SetpointManager:MultiZone:Humidity:Maximum**
-
-- **SetpointManager:MultiZone:MaximumHumidity:Average**
-
-objects and **SetpointManager:OutdoorAirPretreat** (optional) objects. When extra dehumidification is required, the equipment may not be able to meet the humidity setpoint if its full capacity is not adequate.
-
-#### Field: Run on Sensible Load
-
-This alpha field specifies if the unit will operate to meet a sensible load as determined by the inlet node dry-bulb temperature and the dry-bulb temperature setpoint on the control node. There are two valid choices, **Yes** or **No**. If **Yes**, unit will run if there is a sensible load. If **No**, unit will not run if there is only a sensible load. The default is **Yes**.
-
-#### Field: Run on Latent Load
-
-This alpha field specifies if the unit will operate to meet a latent load as determined by the inlet node humidity ratio and the max humidity setpoint on the control node. There are two valid choices, **Yes** or **No**. If **Yes**, unit will run if there is a latent load. If both a sensible and latent load exist, the system will operate to maintain the temperature set point. When only a latent load exists, the system will operate to meet the humidity ratio set point and requires the use of a heating coil and heating coil outlet air temperature set point manager downstream of this cooling coil to maintain the temperature set point. If **No**, unit will not run if there is only a latent load. The default is **No**.
-
-#### Field: Use Outdoor Air DX Cooling Coil
-
-This input field enables the Coil System DX Coil to be used for low air flow to capacity ratio range ( 100     300 cfm/ton).   This flow to capacity ratio range is common in 100% dedicated outdoor air system (DOAS) applications. Other airloop or zone HVAC systems may use this input filed if they operate at such a low flow to capacity ratio range. There are two valid choices, **Yes** or **No**. If **Yes**, the DX cooling coil is forced to operate in this flow to capacity ratio range or runs as 100% DOAS DX coil. If **No**, DX coil is used as regular DX coil. This input field is optional.
-
-#### Field: Outdoor Air DX Cooling Coil Leaving Minimum Air Temperature
-
-This input field is the DX cooling coil leaving supply air minimum temperature specified for frost control.   The DX cooling coil leaving air temperature is not allowed to exceed this minimum coil leaving air temperature.   The DX cooling coil frost controller adjusts or limits the desired coil outlet air setpoint temperature when the coil outlet temperature exceeds this minimum temperature limit specified.   This input field is optional and only used along with in the input field above. The minimum and maximum values of this input field are 0.0 &deg;C and 7.2 &deg;C, and the default value is 2.0 &deg;C.
-
-
-
-An example IDF specification:
-
-```idf
-CoilSystem:Cooling:DX,
-       DX Cooling Coil System 1,!- Name
-       CoolingCoilAvailSched,     !- Availability Schedule Name
-       Cooling Coil Air Inlet Node,   !- DX Cooling Coil System Inlet Node Name
-       Air Loop Outlet Node,       !- DX Cooling Coil System Outlet Node Name
-       Air Loop Outlet Node,       !- DX Cooling Coil System Sensor Node Name
-       Coil:Cooling:DX:SingleSpeed,   !- Cooling Coil Object Type
-       ACDXCoil 1,                           !- Cooling Coil Name
-       None,                                       !- Dehumidification Control Type
-       Yes,                                         !- Run on Sensible Load
-       No,                                           !- Run on Latent Load
-       Yes,                                         !- Use DOAS DX Cooling Coil
-       2.0;                                         !- DOAS DX Cooling Coil Leaving Minimum Air Temperature
-
-
-Coil:Cooling:DX:SingleSpeed,
-       ACDXCoil 1,                           !- Name
-       CoolingCoilAvailSched,     !- Availability Schedule Name
-       25000,                                     !- Gross Rated Total Cooling Capacity {W}
-       0.75,                                       !- Gross Rated Sensible Heat Ratio
-       3.0,                                         !- Gross Rated Cooling COP
-       1.3,                                         !- Rated Air Flow Rate {m3/s}
-       Cooling Coil Air Inlet Node,   !- Air Inlet Node Name
-       Air Loop Outlet Node,       !- Air Outlet Node Name
-       WindACCoolCapFT,                 !- Total Cooling Capacity Function of Temperature Curve Name
-       WindACCoolCapFFF,               !- Total Cooling Capacity Function of Flow Fraction Curve Name
-       WindACEIRFT,                         !- Energy Input Ratio Function of Temperature Curve Name
-       WindACEIRFFF,                       !- Energy Input Ratio Function of Flow Fraction Curve Name
-       WindACPLFFPLR;                     !- Part Load Fraction Correlation Curve Name
-```
-
-
-
-### DX Cooling Coil System Outputs
-
-***All DX Coils:***
-
-* HVAC,Average,Coil System Frost Control Status
-
-
-
-***Coil Type= Coil:Cooling:DX:TwoStageWithHumidityControlMode***
-
-* HVAC,Average,Coil System Cycling Ratio
-
-* HVAC,Average,Coil System Compressor Speed Ratio
-
-
-
-***Coil types=Coil:Cooling:DX:SingleSpeed & CoilSystem:Cooling:DX:HeatExchangerAssisted***
-
-* HVAC,Average,Coil System Part Load Ratio
-
-#### Coil System Cycling Ratio
-
-The system may operate for the entire system timestep, but to meet the load the compressor can cycle on and off. This reports the fraction of the system timestep that the compressor is operating. (1.0 is continuous, 0.0 is off).
-
-#### Coil System Compressor Speed Ratio
-
-This is the ratio of time in a system timestep that the compressor is at rated speed. The compressor speed ratio reports (1.0 is max, 0.0 is min) and any value in between as it is averaged over the timestep.
-
-#### Coil System Part Load Ratio
-
-The DX system can operate with a cycling compressor or a varying speed compressor, This variable reports the fraction of the Full Load that is met during the system timestep. This can differ from the cycling part load ratio or the compressor speed ratio. (1.0 is Full Load and 0.0 is no load)
-
-#### Coil System Frost Control Status
-
-This is a flag indicating whether frost control is active at current time step or not.   Frost control is activated or enforced when the sensible load control requires DX cooling coil outlet air temperature below the user specified minimum temperature or when the dehumidification load control requires DX cooling coil outlet air humidity ratio below the saturation humidity ratio corresponding to the user specified minimum temperature for frost control. Frost control status of zero means no active frost control, a value of 1 or 2 indicates that frost control is active.   If frost control status is 1, then the frost control was enforced when the cooling coil is run to meet sensible load.   If the frost control status value is 2, then the control was enforced when the cooling coil is run to meet latent load. When frost control is active the DX cooling coil setpoint value is modified based on user specified limit.
-
-### CoilSystem:Heating:DX
-
-The CoilSystem:Heating:DX object is a virtual container component for a DX heating coil that provides the controls needed to operate the coil.   Only single speed DX air-to-air heating coils are supported.
-
-
-
-This component may be used as a heating coil in constant volume or variable volume air handlers.   It can also be used in an outside air system (by including it in an AirLoopHVAC:OutdoorAirSystem:EquipmentList object)or in a zone outdoor air unit (by including it in an ZoneHVAC:OutdoorAirUnit:EquipmentList object).   This object is the one that is listed in the Branch or equipment list object rather than the coil itself.
-
-The inlet and outlet nodes for the DX heat pump system are defined in the heating coil object.   The control node is always the outlet node of the coil.   This DX heat pump heating system requires that a (drybulb) temperature setpoint be placed on the outlet node using either a setpoint manager or the energy management system.   The coil is controlled to attempt to meet that setpoint using a part load ratio modeling approach.
-
-This model only supports continuous fan and cycling compressor operation -- cycling fan modeling is not available with this model.
-
-#### Field: Name
-
-This alpha field contains the identifying name for this component.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name that contains information on the availability of the DX coil to operate. A schedule value of 0 indicates that the coil is off for that time period. A schedule value greater than 0 indicates that the coil can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Heating Coil Object Type
-
-This alpha field specifies the type of DX heating coil.   This model currently supports only single speed DX heat pump heating coils and the only options for this field are Coil:Heating:DX:SingleSpeed and Coil:Heating:DX:VariableSpeed.
-
-#### Field: Heating Coil Name
-
-This alpha field specifies the unique name of the DX heating coil.   This field references the name of a Coil:Heating:DX:SingleSpeed that needs to be defined elsewhere in the input file.
-
-
-
-An example of a DX heating coil system follows.
-
-```idf
-CoilSystem:Heating:DX,
-       HeatPump DX Coil 1, !- Name
-       FanAndCoilAvailSched , !- Availability Schedule Name
-       Coil:Heating:DX:SingleSpeed,   !- Heating Coil Object Type
-       Heat Pump DX Heating Coil 1;   !- Heating Coil Name
-
-
-   Coil:Heating:DX:SingleSpeed,
-       Heat Pump DX Heating Coil 1,   !- Name
-       FanAndCoilAvailSched,       !- Availability Schedule Name
-       autosize,                               !- Gross Rated Heating Capacity {W}
-       2.75,                                       !- Gross Rated Heating COP {W/W}
-       autosize,                               !- Rated Air Flow Rate {m3/s}
-       Heating Coil Air Inlet Node,   !- Air Inlet Node Name
-       SuppHeating Coil Air Inlet Node,   !- Air Outlet Node Name
-       HPACHeatCapFT,                     !- Heating Capacity Function of Temperature Curve Name
-       HPACHeatCapFFF,                   !- Heating Capacity Function of Flow Fraction Curve Name
-       HPACHeatEIRFT,                     !- Energy Input Ratio Function of Temperature Curve Name
-       HPACHeatEIRFFF,                   !- Energy Input Ratio Function of Flow Fraction Curve Name
-       HPACCOOLPLFFPLR,                 !- Part Load Fraction Correlation Curve Name
-       ,                                               !- Defrost Energy Input Ratio Function of Temperature Curve Name
-       -8.0,                                       !- Minimum Outdoor Dry-Bulb Temperature for Compressor Operation {C}
-       5.0,                                         !- Maximum Outdoor Dry-Bulb Temperature for Defrost Operation {C}
-       200.0,                                     !- Crankcase Heater Capacity {W}
-       10.0,                                       !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
-       Resistive,                             !- Defrost Strategy
-       TIMED,                                     !- Defrost Control
-       0.166667,                               !- Defrost Time Period Fraction
-       autosize,                               !- Resistive Defrost Heater Capacity {W}
-       Heat Pump 1 Evaporator Node;
-```
-
-
-### DX Heating Coil System Outputs
-
-#### Coil System Part Load Ratio
-
-The DX system can operate with a cycling compressor or a varying speed compressor, This variable reports the fraction of the Full Load that is met during the system timestep. This can differ from the cycling part load ratio or the compressor speed ratio. (1.0 is Full Load and 0.0 is no load)
-
-### CoilSystem:Cooling:DX:HeatExchangerAssisted
-
-The heat exchanger-assisted DX cooling coil is a    virtual    component consisting of a direct expansion (DX) cooling coil and an air-to-air heat exchanger as shown in Figure 139 below. The air-to-air heat exchanger pre-conditions the air entering the cooling coil, and reuses this energy to post-condition the supply air leaving the cooling coil. This heat exchange process improves the latent removal performance of the cooling coil by allowing it to dedicate more of its cooling capacity toward dehumidification (lower sensible heat ratio).
-
-This compound object models the basic operation of an air-to-air heat exchanger in conjunction with a cooling coil. The heat exchanger-assisted DX cooling coil does not have an operating schedule of its own; its operating schedule is governed by the availability schedules for the DX cooling coil and the air-to-air heat exchanger. This compound object is used in place of where a DX cooling coil object would normally be used by itself.
-
-To model a heat exchanger-assisted DX cooling coil, the input data file should include the following objects:
-
-- CoilSystem:Cooling:DX:HeatExchangerAssisted object
-
-- Air-to-air heat exchanger object (HeatExchanger:AirToAir:FlatPlate, HeatExchanger:AirToAir:SensibleAndLatent, or HeatExchanger:Desiccant:BalancedFlow)
-
-- DX cooling coil object (Coil:Cooling:DX:SingleSpeed)
-
-In terms of controlling the operation of the heat exchanger, the heat exchanger is assumed to always provide its heat transfer when the associated DX cooling coil is operating and no high humidity control mechanism is specified. However, the heat exchanger   s energy transfer may be controlled (i.e., turned on and off) based on a zone air humidity level using either a humidistat (ref. AirLoopHVAC:Unitary:Furnace:HeatCool or AirLoopHVAC:UnitaryHeatCool) or a humidistat and a maximum humidity set point manager to place a humidity ratio set point on the appropriate control node (ref. CoilSystem:Cooling:DX). This model may also be used with the unitary changeover bypass system and the unitary air-to-air heat pump system (ref. AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass and AirLoopHVAC:UnitaryHeatPump:AirToAir); however, the heat exchanger is assumed to always provide its heat transfer when the cooling coil operates and cannot be turned on and off based on a zone air humidity set point. Two zone air conditioners may also use this model for improved dehumidification. The first type is the packaged terminal heat pump (ref. ZoneHVAC:PackagedTerminalHeatPump) where the heat exchanger   s heat transfer is always active whenever the cooling coil operates. The second type is the window air conditioner (ref. ZoneHVAC:WindowAirConditioner) where the heat exchanger   s heat transfer is always active when the cooling coil operates and no high humidity control mechanism is specified, OR the heat exchanger   s heat transfer may be controlled based on zone air humidity level if a humidistat and high humidity set point manager are specified (maximum humidity ratio set point placed on the heat exchanger   s exhaust air outlet node, ref. Figure 139).
-
-Links to the cooling coil and air-to-air heat exchanger specifications are provided in the input data syntax for this compound object. A description of each input field for this compound object is provided below.
-
-![GenericHXAssisted](media/image369.png)
-
-Figure 139. Schematic of the CoilSystem:Cooling:DX:HeatExchangerAssisted compound object
-
-NOTE: Node naming shown in Figure 139 is representative for HeatExchanger:AirToAir:SensibleAndLatent. For HeatExchanger:AirToAir:FlatPlate, the exhaust air nodes are referred to as    secondary air    nodes. For HeatExchanger:Desiccant:BalancedFlow, the supply air nodes are referred to as    regeneration air    nodes and the exhaust air nodes as    process air    nodes.
-
-#### Field: Name
-
-A unique user-assigned name for the heat exchanger-assisted DX cooling coil. Any reference to this compound component by another object will use this name.
-
-#### Field: Heat Exchanger Object Type
-
-This alpha field denotes the type of heat exchanger being modeled. Valid choices are:
-
-* HeatExchanger:AirToAir:FlatPlate
-
-* HeatExchanger:AirToAir:SensibleAndLatent
-
-* HeatExchanger:Desiccant:BalancedFlow
-
-#### Field: Heat Exchanger Name
-
-This alpha field denotes the name of the air-to-air heat exchanger being modeled.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field denotes the type of DX cooling coil being modeled. The only valid choice is Coil:Cooling:DX:SingleSpeed.
-
-#### Field: Cooling Coil Name
-
-This alpha field denotes the name of the DX cooling coil being modeled.
-
-Following is an example input for this compound object:
-
-```idf
-CoilSystem:Cooling:DX:HeatExchangerAssisted,
-       HeatExchangerAssistedCoolingCoil,               ! Name of the heat exchanger assisted cooling coil
-       HeatExchanger:AirToAir:SensibleAndLatent,       ! Heat exchanger type
-       Air to Air Heat Exchanger 1,                    ! Heat exchanger name
-       Coil:Cooling:DX:SingleSpeed,                    ! Cooling coil type
-       DX Cooling Coil 1;                              ! Cooling coil name
-
-
-   HeatExchanger:AirToAir:SensibleAndLatent,
-       Air to Air Heat Exchanger 1,        !- Heat exchanger name
-       FanAndCoilAvailSched,               !- Availability schedule name
-       1.3,                                !- Nominal supply air flow rate {m3/s}
-       .2,                                 !- Sensible effectiveness at 100% airflow heating condition
-       .0,                                 !- Latent effectiveness at 100% airflow heating condition
-       .23,                                !- Sensible effectiveness at 75% airflow heating condition
-       .0,                                 !- Latent effectiveness at 75% airflow heating condition
-       .2,                                 !- Sensible effectiveness at 100% airflow cooling condition
-       .0,                                 !- Latent effectiveness at 100% airflow cooling condition
-       .23,                                !- Sensible effectiveness at 75% airflow cooling condition
-       .0,                                 !- Latent effectiveness at 75% airflow cooling condition
-       HeatExchangerSupplyAirInletNode,    !- Supply air inlet node name
-       DX Cooling Coil Air Inlet Node,     !- Supply air outlet node name
-       HeatExchangerExhaustAirInletNode,   !- Exhaust air inlet node name
-       HeatExchangerExhaustAirOutletNode,  !- Exhaust air outlet node name
-       50.0,                               !- Nominal electric power {W}
-       No,                                 !- Supply air outlet temperature control
-       Rotary,                             !- Heat exchanger type
-       None;                               !- Frost control type
-
-
-   Coil:Cooling:DX:SingleSpeed,
-       DX Cooling Coil 1,                  !- Coil Name
-       FanAndCoilAvailSched,               !- Availability Schedule
-       25000,                              !- Gross Rated Total Cooling Capacity {W}
-       0.75,                               !- Gross Rated Sensible Heat Ratio
-       3.0,                                !- Gross Rated Cooling COP
-       1.3,                                !- Rated Air Flow Rate {m3/s}
-       DX Cooling Coil Air Inlet Node,     !- Coil Air Inlet Node
-       HeatExchangerExhaustAirInletNode,   !- Coil Air Outlet Node
-       ACCoolCapFT,                  !- Total Cooling Capacity Modifier Curve (function of temperature)
-       ACCoolCapFFF,                 !- Total Cooling Capacity Modifier Curve (function of flow fraction)
-       ACEIRFT,                      !- Energy Input Ratio Modifier Curve (function of temperature)
-       ACEIRFFF,                     !- Energy Input Ratio Modifier Curve (function of flow fraction)
-       ACPLFFPLR;                    !- Part Load Fraction Correlation (function of part load ratio)
-```
-
-
-### CoilSystem:Cooling:DX:HeatExchangerAssisted Outputs
-
-No variables are reported for this compound object. However, outputs are provided by the cooling coil and heat exchanger that are specified.
-
-### CoilSystem:Cooling:Water:HeatExchangerAssisted
-
-The heat exchanger-assisted water cooling coil is a    virtual    component consisting of a chilled-water cooling coil and an air-to-air heat exchanger as shown in Figure 140 below. The air-to-air heat exchanger precools the air entering the cooling coil, and reuses this energy to reheat the supply air leaving the cooling coil. This heat exchange process improves the latent removal performance of the cooling coil by allowing it to dedicate more of its cooling capacity toward dehumidification (lower sensible heat ratio).
-
-![GenericHXAssisted](media/image370.png)
-
-Figure 140. Schematic of the CoilSystem:Cooling:Water:HeatExchangerAssisted compound object
-
-Note: Node naming shown in Figure 140 is representative for HeatExchanger:AirToAir:SensibleAndLatent. For HeatExchanger:AirToAir:FlatPlate, the exhaust air nodes are referred to as    secondary air    nodes.
-
-This compound object models the basic operation of an air-to-air heat exchanger in conjunction with a chilled-water cooling coil. The heat exchanger-assisted water cooling coil does not have an operating schedule of its own; its operating schedule is governed by the availability schedules for the chilled-water cooling coil and the air-to-air heat exchanger. Heat exchange will occur whenever the heat exchanger is available to operate (via its availability schedule) and a temperature difference exists between the two air streams -- there is currently no method to enable or disable heat exchange based on zone air humidity level. This compound object is used in place of where a chilled-water cooling coil object would normally be used by itself.
-
-To model a heat exchanger-assisted water cooling coil, the input data file should include the following objects:
-
-- CoilSystem:Cooling:Water:HeatExchangerAssisted compound object
-
-- Air-to-air heat exchanger object (HeatExchanger:AirToAir:FlatPlate or HeatExchanger:AirToAir:SensibleAndLatent)
-
-- Chilled-water cooling coil object (Coil:Cooling:Water or Coil:Cooling:Water:DetailedGeometry)
-
-Links to the cooling coil and air-to-air heat exchanger specifications are provided in the input data syntax for this compound object. A description of each input field for this compound object is provided below.
-
-#### Field: Name
-
-A unique user-assigned name for the heat exchanger-assisted water cooling coil. Any reference to this compound component by another object (e.g., ZoneHVAC:UnitVentilator, ZoneHVAC:FourPipeFanCoil, component in an air loop Branch object) will use this name.
-
-#### Field: Heat Exchanger Object Type
-
-This alpha field denotes the type of heat exchanger being modeled. Valid choices are:
-
-HeatExchanger:AirToAir:FlatPlate
-
-HeatExchanger:AirToAir:SensibleAndLatent
-
-#### Field: Heat Exchanger Name
-
-This alpha field denotes the name of the air-to-air heat exchanger being modeled.
-
-#### Field: Cooling Coil Object Type
-
-This alpha field denotes the type of chilled-water cooling coil being modeled. Valid choices are:
-
-Coil:Cooling:Water
-
-Coil:Cooling:Water:DetailedGeometry
-
-#### Field: Cooling Coil Name
-
-This alpha field denotes the name of the chilled-water cooling coil being modeled.
-
-Following is an example input for this compound object:
-
-```idf
-CoilSystem:Cooling:Water:HeatExchangerAssisted,
-       Heat Exchanger Assisted Cooling Coil 1, !- Name of the heat exchanger assisted cooling coil
-       HeatExchanger:AirToAir:FlatPlate,     !- Heat exchanger type
-       Heat Exchanger Assisting Cooling Coil,   !- Heat exchanger name
-       Coil:Cooling:Water:DetailedGeometry,                 !- Cooling coil type
-       Main Cooling Coil 1;                                       !- Cooling coil name
-
-
-HeatExchanger:AirToAir:FlatPlate,
-       Heat Exchanger Assisting Cooling Coil,   !- Name
-       CoolingCoilAvailSched,     !- Availability Schedule Name
-       Counter Flow,                       !- flow arrangement
-       Yes,                                         !- Economizer lockout
-       1.0,                                         !- hA ratio
-       1.32,                                       !- Nominal supply air flow rate {m3/s}
-       24.0,                                       !- Nominal supply air inlet temperature {C}
-       21.0,                                       !- Nominal supply air outlet temperature {C}
-       1.32,                                       !- Nominal secondary air flow rate {m3/s}
-       12.0,                                       !- Nominal secondary air inlet temperature {C}
-       100.0,                                     !- Nominal electric power {W}
-       Mixed Air Node 1,               !- Supply air inlet node
-       Main Cooling Coil 1 Inlet Node,   !- Supply air outlet node
-       Main Cooling Coil 1 Outlet Node, !- Secondary air inlet node
-       Main Heating Coil 1 Inlet Node;   !- Secondary air outlet node
-
-
-
-
-Coil:Cooling:Water:DetailedGeometry,
-       Main Cooling Coil 1,         !- Coil Name
-       CoolingCoilAvailSched,     !- Availability Schedule Name
-       autosize,                               !- Max Water Flow Rate of Coil {m3/s}
-       autosize,                               !- Tube Outside Surf Area {m2}
-       autosize,                               !- Total Tube Inside Area {m2}
-       autosize,                               !- Fin Surface Area {m2}
-       autosize,                               !- Minimum Air Flow Area {m2}
-       autosize,                               !- Coil Depth {m}
-       autosize,                               !- Fin Diameter {m}
-       ,                                               !- Fin Thickness {m}
-      ,                                               !- Tube Inside Diameter {m}
-       ,                                               !- Tube Outside Diameter {m}
-       ,                                               !- Tube Thermal Conductivity {W/m-K}
-       ,                                               !- Fin Thermal Conductivity {W/m-K}
-       ,                                               !- Fin Spacing {m}
-       ,                                               !- Tube Depth Spacing {m}
-       ,                                               !- Number of Tube Rows
-       autosize,                               !- Number of Tubes per Row
-       Main Cooling Coil 1 Water Inlet Node,   !- Coil_Water_Inlet_Node
-       Main Cooling Coil 1 Water Outlet Node, !- Coil_Water_Outlet_Node
-       Main Cooling Coil 1 Inlet Node,     !- Coil_Air_Inlet_Node
-       Main Cooling Coil 1 Outlet Node;   !- Coil_Air_Outlet_Node
-```
-
-### CoilSystem:Cooling:Water:HeatExchangerAssisted Outputs
-
-No variables are reported for this compound object. However, outputs are provided by the cooling coil and heat exchanger that are specified.
-
-### Coil:WaterHeating:AirToWaterHeatPump:Pumped
-
-EnergyPlus can model a heat pump water heater (HPWH) consisting of a water heater tank (e.g., `WaterHeater:Mixed`), a direct expansion (DX) coil (i.e., an air-to-water DX compression system which includes a water heating coil, air coil, compressor, and water pump), and a fan to provide air flow across the air coil associated with the DX compression system. These objects work together to model a system which heats water using zone air, outdoor air, or a combination of zone and outdoor air as the primary heat source.
-
-The `WaterHeater:HeatPump:PumpedCondenser` compound object, water heater tank object (e.g., `WaterHeater:Mixed`), and fan object (e.g., `Fan:OnOff`) are defined elsewhere in this reference document. `Coil:WaterHeating:AirToWaterHeatPump:Pumped` object described here models an air-to-water DX compression system to determine its air-side and water-side performance. This DX coil object calculates the air-side sensible and latent cooling capacity at the specific operating conditions for each simulation timestep, as well as the condenser's water-side temperature difference at a given condenser water flow rate.
-
-The heat pump water heater DX coil model performs the following major functions:
-
-- calculates the electric consumption of the DX compressor and water pump
-
-- calculates the amount of heat delivered to the water tank
-
-- calculates the electric consumption of the compressor's crankcase heater
-
-- calculates the air-side performance of the DX coil
-
-The input fields for this object are described below in detail:
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a heat pump water heater DX coil. Any reference to this coil by another object (e.g., `WaterHeater:HeatPump:PumpedCondenser`) will use this name.
-
-#### Field: Rated Heating Capacity
-
-This numeric field defines the DX coil heating capacity in Watts at the rated evaporator inlet air temperatures, rated condenser inlet water temperature, rated evaporator air flow rate, and rated condenser water flow rate specified below. Values must be greater than 0. This value represents water heating capacity, and it may or may not include the impact of condenser pump heat (see field Condenser Pump Heat Included in Rated Heating Capacity below).
-
-#### Field: Rated COP
-
-This numeric field defines the DX coil's water heating coefficient of performance (COP=water heating capacity in watts divided by electrical power input in watts) at rated conditions (rated inlet temperatures and flow rates specified below). This input not only determines the electric energy use of the heat pump DX coil, but also the amount of total air cooling provided by the evaporator. The rated COP includes compressor power, and may or may not include condenser pump power or evaporator fan power (see field Evaporator Fan Power Included in Rated COP and field Condenser Pump Power Included in Rated COP). Values must be greater than 0. If this field is left blank, the default value is 3.2.
-
-#### Field: Rated Sensible Heat Ratio
-
-This numeric field defines the air-side sensible heat ratio (SHR=sensible cooling capacity divided by total cooling capacity) of the DX coil at rated conditions (rated inlet temperatures and flow rates specified below). This value should not include the effect of evaporator fan heat. Values must be greater than or equal to 0.5, and less than or equal to 1.0. The default value is 0.85.
-
-#### Field: Rated Evaporator Inlet Air Dry-Bulb Temperature
-
-This numeric field defines the evaporator inlet air dry-bulb temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 5 &deg;C. If this field is left blank, the default value is 19.7 &deg;C.
-
-#### Field: Rated Evaporator Inlet Air Wet-Bulb Temperature
-
-This numeric field defines the evaporator inlet air wet-bulb temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 5 &deg;C. If this field is left blank, the default value is 13.5 &deg;C.
-
-#### Field: Rated Condenser Inlet Water Temperature
-
-This numeric field defines the condenser inlet water temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 25 &deg;C. If this field is left blank, the default value is 57.5 &deg;C.
-
-#### Field: Rated Evaporator Air Flow Rate
-
-This numeric field defines the evaporator air volume flow rate in cubic meters per second at rated conditions. Values must be greater than 0. If this field is left blank or autocalculated (field value = **autocalculate**), the default value is 5.035E-5 m<sup>3</sup>/s/W (31.25 cfm/MBH) multiplied by the Rated Heating Capacity specified above. When autocalculating the rated evaporator air volumetric flow rate, a zone sizing object is not required.
-
-#### Field: Rated Condenser Water Flow Rate
-
-This numeric field defines the condenser water volumetric flow rate in cubic meters per second at rated conditions. Values must be greater than 0. If this field is left blank or autocalculated (field value = **autocalculate**), the default value is 4.487E-8 m<sup>3</sup>/s/W (0.208 gpm/MBH) multiplied by the Rated Heating Capacity specified above. When autocalculating the rated condenser water volumetric flow rate, a zone sizing object is not required. A warning message will be issued if the ratio of Rated Condenser Water Volumetric Flow Rate to Rated Heating Capacity is less than 1.79405E-8 m<sup>3</sup>/s/W (0.083 gpm/MBH) or greater than 8.97024E-8 m<sup>3</sup>/s/W (0.417 gpm/MBH), but the simulation will continue.
-
-#### Field: Evaporator Fan Power Included in Rated COP
-
-This choice field specifies if evaporator fan power is included in the rated COP defined above. This input impacts the calculation of compressor electric power and total air cooling provided by the evaporator for each simulation timestep. If Yes is selected, the evaporator fan power is subtracted from the total electric heating power when calculating total evaporator cooling capacity. If No is selected, it is assumed that the total heating power does not include evaporator fan power. If this field is left blank, the default is Yes. See the Engineering Reference section for `Coil:WaterHeating:AirToWaterHeatPump:\*` for further details.
-
-#### Field: Condenser Pump Power Included in Rated COP
-
-This choice field specifies if condenser pump power is included in the rated COP defined above. This input impacts the calculation of compressor electric power which then impacts the total air cooling provided by the evaporator for each simulation timestep. If Yes is selected, the condenser pump power is subtracted from the total electric heating power when calculating total evaporator cooling capacity. If No is selected, it is assumed that the total heating power does not include the condenser pump. If this field is left blank, the default is No. See Engineering Reference section for `Coil:WaterHeating:AirToWaterHeatPump:\*` for further details.
-
-#### Field: Condenser Pump Heat Included in Rated Heating Capacity and Rated COP
-
-This choice field specifies if condenser pump heat is included in the rated heating capacity and rated COP defined above. This input impacts the calculation of compressor electric power and total air cooling provided by the evaporator for each simulation timestep. If Yes is selected, the condenser pump heat is already included in the rated heating capacity and rated COP. If No is selected, it is assumed that the rated heating capacity and rated COP do not include the condenser pump heat, and pump heat is added to the total water heating capacity based on the Condenser Water Pump Power and Fraction of Condenser Pump Heat to Water fields below. If this field is left blank, the default is No. See Engineering Reference section for `Coil:WaterHeating:AirToWaterHeatPump:\*` for further details.
-
-#### Field: Condenser Water Pump Power
-
-This numeric field defines the DX coil's condenser pump power in Watts. This is the operating pump power as installed. Values must be greater than or equal to 0. If this field is left blank, the default value is 0. A warning message will be issued if the ratio of Condenser Water Pump Power to Rated Heating Capacity exceeds 0.1422 W/W (41.67 Watts/MBH), but the simulation will continue.
-
-#### Field: Fraction of Condenser Pump Heat to Water
-
-This numeric field defines the fraction of condenser pump heat that is transferred to the condenser water. The pump is assumed to be downstream of the condenser water coil, and this field is used to determine the water temperature at the condenser outlet node when the field Condenser Pump Power Included in Rated Heating Capacity is set to No. Values must be greater than or equal to 0 and less than or equal to 1. If this field is left blank, the default value is 0.2.
-
-#### Field: Evaporator Air Inlet Node Name
-
-This alpha field defines the name of the air node from which the evaporator coil draws its inlet air.
-
-#### Field: Evaporator Air Outlet Node Name
-
-This alpha field defines the name of the air node to which the evaporator coil sends its outlet air.
-
-#### Field: Condenser Water Inlet Node Name
-
-This alpha field defines the name of the node from which the DX coil condenser draws its inlet water. This node name must also match the source side outlet node name for the water heater tank connected to this DX coil (ref: Water Heaters).
-
-#### Field: Condenser Water Outlet Node Name
-
-This alpha field defines the name of the node to which the heat pump condenser sends it outlet water. This node name must also match the source side inlet node name for the water heater tank connected to this DX coil (ref: Water Heaters).
-
-#### Field: Crankcase Heater Capacity
-
-This numeric field defines the compressor's crankcase heater capacity in Watts. The crankcase heater only operates when the compressor is off and the air surrounding the compressor is below the Maximum Ambient Temperature for Crankcase Heater Operation specified below.
-
-#### Field: Maximum Ambient Temperature for Crankcase Heater Operation
-
-This numeric field defines the maximum ambient temperature for crankcase heater operation in degree Celsius. The crankcase heater only operates when the air surrounding the compressor is below this maximum temperature value and the compressor is off. The ambient temperature surrounding the compressor is set by the Heat Pump:Water Heater parent object (field Compressor Location).
-
-#### Field: Evaporator Air Temperature Type for Curve Objects
-
-This choice field specifies the air temperature type used for the heating capacity and COP modifier curve objects below. The valid selections are Dry-bulb Temperature and Wet-bulb Temperature. If dry-bulb temperature is selected, the inlet air dry-bulb temperature entering the heat pump DX coil and fan section is used to evaluate the curve objects. If wet-bulb temperature is selected, the inlet air wet-bulb temperature entering the heat pump DX coil and fan section is used to evaluate the curve objects. If this field is left blank and the following curve names are defined, the default value is wet-bulb temperature. If the following curve names are not defined, this field is not used.
-
-#### Field: Heating Capacity Function of Temperature Curve Name
-
-This alpha field specifies the name of a **biquadratic** or **cubic** performance curve object (ref: Performance Curves) that defines the variation in DX coil heating capacity as a function of inlet fluid (air and water) temperatures. The biquadratic curve uses evaporator inlet air temperature (dry-bulb or wet-bulb temperature based on the field Evaporator Air Temperature Type for Curve Objects defined above) and condenser inlet water temperature as the independent variables. The cubic curve uses evaporator inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The output of this curve is multiplied by the rated heating capacity to give the heating capacity at specific operating conditions (i.e., at temperatures different from the rating point temperatures). The curve should be normalized to have the value of 1.0 at the rating point temperatures. If this field is left blank, the heating capacity remains constant (curve value assumed to be 1.0 for all conditions).
-
-#### Field: Heating Capacity Function of Air Flow Fraction Curve Name
-
-This alpha field specifies the name of a **quadratic** or **cubic** performance curve object (ref: Performance Curves) that defines the variation in DX coil heating capacity as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate. The output of this curve is multiplied by the rated heating capacity and the heating capacity modifier curve (function of temperature) to give the DX coil heating capacity at the specific inlet fluid temperatures and air flow rate at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated evaporator air flow rate (air flow fraction of 1.0). If this field is left blank, the heating capacity remains constant (curve value assumed to be 1.0 for all air flow rates).
-
-#### Field: Heating Capacity Function of Water Flow Fraction Curve Name
-
-This alpha field specifies the name of a **quadratic** or **cubic** performance curve object (ref: Performance Curves) that defines the variation in DX coil heating capacity as a function of the ratio of actual water flow rate through the condenser to the rated condenser water flow rate. The output of this curve is multiplied by the rated heating capacity and the output from the two other heating capacity modifier curves (function of temperature and function of air flow fraction) to give the DX coil heating capacity at the specific inlet fluid temperatures and flow rates at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated condenser water flow rate (water flow fraction of 1.0). If this field is left blank, the heating capacity remains constant (curve value assumed to be 1.0 for all water flow rates).
-
-#### Field: Heating COP Function of Temperature Curve Name
-
-This alpha field specifies the name of a **biquadratic** or **cubic** performance curve object (ref: Performance Curves) that defines the variation in DX coil heating COP as a function of inlet fluid (air and water) temperatures. The biquadratic curve uses evaporator inlet air temperature (dry-bulb or wet-bulb temperature based on the field Evaporator Air Temperature Type for Curve Objects defined above) and condenser inlet water temperature as the independent variables. The cubic curve uses evaporator inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The output of this curve is multiplied by the rated COP to give the heating COP at specific operating conditions (i.e., at temperatures different from the rating point temperatures). The curve should be normalized to have the value of 1.0 at the rating point temperatures. If this field is left blank, the COP remains constant (curve value assumed to be 1.0 for all conditions).
-
-#### Field: Heating COP Function of Air Flow Fraction Curve Name
-
-This alpha field specifies the name of a **quadratic** or **cubic** performance curve object (ref: Performance Curves) that defines the variation in DX coil heating COP as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate. The output of this curve is multiplied by the rated COP and the heating COP modifier curve (function of temperature) to give the heating COP at the specific inlet fluid temperatures and air flow rate at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated evaporator air flow rate (air flow fraction of 1.0). If this field is left blank, the heating COP remains constant (curve value assumed to be 1.0 for all air flow rates).
-
-#### Field: Heating COP Function of Water Flow Fraction Curve Name
-
-This alpha field specifies the name of a **quadratic** or **cubic** performance curve object (ref: Performance Curves) that defines the variation in DX coil heating COP as a function of the ratio of actual water flow rate through the condenser to the rated condenser water flow rate.. The output of this curve is multiplied by the rated COP and the output from the two other heating COP modifier curves (function of temperature and function of air flow fraction) to give the DX coil heating COP at the specific inlet fluid temperatures and flow rates at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated condenser water flow rate (water flow fraction of 1.0). If this field is left blank, the heating COP remains constant (curve value assumed to be 1.0 for all water flow rates).
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a **quadratic** or **cubic** performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
-
-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7     and     PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
-
-           PLF = 0.85 + 0.15(PLR)
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-           PLF = 1.0 + 0.0(PLR)
-
-Following is an example input for the `Coil:WaterHeating:AirToWaterHeatPump:Pumped` object:
-
-```idf
-Coil:WaterHeating:AirToWaterHeatPump:Pumped,
-       Zone4HPWHDXCoil,           !- Coil Name
-       4000.0,                    !- Heating Capacity {W}
-       3.2,                       !- Rated COP {W/W}
-       0.6956,                    !- Rated SHR (gross)
-       19.7,                      !- Rated Evaporator Inlet Air Dry-Bulb Temperature {C}
-       13.5,                      !- Rated Evaporator Inlet Air Wet-Bulb Temperature {C}
-       57.5,                      !- Rated Condenser Inlet Water Temperature {C}
-       autocalculate,             !- Rated Evaporator Air Volumetric Flow Rate {m3/s}
-       autocalculate,             !- Rated Condenser Water Volumetric Flow Rate {m3/s}
-       No,                        !- Evaporator Fan Power Included in Rated COP
-       No,                        !- Condenser Pump Power Included in Rated COP
-       No,                        !- Condenser Pump Heat Included in Rated Heating Capacity and Rated COP
-       150.0,                     !- Condenser Water Pump Power {W}
-       0.1,                       !- Fraction of Condenser Pump Heat to Water
-       Zone4AirOutletNode,        !- Evaporator Air Inlet Node Name
-       Zone4DXCoilAirOutletNode,  !- Evaporator Air Outlet Node Name
-       Zone4WaterInletNode,       !- Condenser Water Inlet Node Name
-       Zone4WaterOutletNode,      !- Condenser Water Outlet Node Name
-       100.0,                     !- Crankcase Heater Capacity {W}
-       5.0,                       !- Maximum Ambient Temperature for Crankcase Heater Operation {C}
-       wet-bulb temperature,      !- Evaporator Air Temperature Type for Curve Objects
-       HPWHHeatingCapFTemp,       !- Heating Capacity Modifier Curve Name (function of temperature)
-       ,                          !- Heating Capacity Modifier Curve Name (function of air flow fraction)
-       ,                          !- Heating Capacity Modifier Curve Name (function of water flow fraction)
-       HPWHHeatingCOPFTemp,       !- Heating COP Modifier Curve Name (function of temperature)
-       ,                          !- Heating COP Modifier Curve Name (function of air flow fraction)
-       ,                          !- Heating COP Modifier Curve Name (function of water flow fraction)
-       HPWHPLFFPLR;               !- Part Load Fraction Correlation Name (function of part load ratio)
-```
-
-### Coil:WaterHeating:AirToWaterHeatPump:Pumped Outputs
-
-* HVAC,Average,Cooling Coil Total Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Total Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Latent Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Latent Cooling Energy [J]
-
-* HVAC,Average, Cooling Coil Runtime Fraction []
-
-* HVAC,Average,DX Cooling Coil Crankcase Heater Electric Power [W]
-
-* HVAC,Sum, Cooling Coil Crankcase Heater Electric Energy [J]
-
-* HVAC,Average,Cooling Coil Total Water Heating Rate [W]
-
-* HVAC,Sum,Cooling Coil Total Water Heating Energy [J]
-
-* HVAC,Average,Cooling Coil Water Heating Electric Power[W]
-
-* HVAC,Sum,Cooling Coil Water Heating Electric Energy [J]
-
-#### Cooling Coil Total Cooling Rate [W]
-
-This output field is the average total (sensible and latent) cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Total Cooling Energy [J]
-
-This output field is the total (sensible plus latent) cooling output of the DX coil in Joules for the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Sensible Cooling Rate [W]
-
-This output field is the average moist air sensible cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Sensible Cooling Energy [J]
-
-This output field is the moist air sensible cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### DX Coil Latent Cooling Rate [W]
-
-This output field is the average latent cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Latent Cooling Energy [J]
-
-This output field is the latent cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Runtime Fraction   []
-
-This output field is the average runtime fraction of the DX coil compressor for the timestep being reported. This also represents the runtime fraction of the condenser water pump.
-
-#### Cooling Coil Crankcase Heater Electric Power[W]
-
-This output field is the average electricity consumption rate of the DX coil compressor's crankcase heater in Watts for the timestep being reported. The crankcase heater operates only when the compressor is off and the air surrounding the compressor is below the Maximum Ambient Temperature for Crankcase Heater Operation, otherwise this output variable is set equal to 0.
-
-#### Cooling Coil Crankcase Heater Electric Energy [J]
-
-This output field is the total electricity consumption of the DX coil compressor's crankcase heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
-
-#### Cooling Coil Total Water Heating Rate [W]
-
-This output field is the average water heating rate output of the DX coil (condenser coil plus condenser water pump) in Watts for the timestep being reported. This is determined using the inlet and outlet water temperatures and the water mass flow rate through the condenser coil.
-
-#### Cooling Coil Total Water Heating Energy [J]
-
-This output field is the total water heating output of the DX coil (condenser coil plus condenser water pump) in Joules for the timestep being reported. This is determined using the inlet and outlet water temperatures and the water mass flow rate through the condenser coil.
-
-#### Cooling Coil Water Heating Electric Power[W]
-
-This output field is the average electricity consumption rate of the DX coil compressor and condenser pump in Watts for the timestep being reported.
-
-#### Cooling Coil Water Heating Electric Energy [J]
-
-This output field is the electricity consumption of the DX coil compressor and condenser pump in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
-
-### Coil:WaterHeating:AirToWaterHeatPump:Wrapped
-
-EnergyPlus can model a heat pump water heater (HPWH) consisting of a water heater tank (e.g., `WaterHeater:Stratified`), a direct expansion (DX) coil (i.e., an air-to-water DX compression system which includes a water heating coil, air coil, compressor, and water pump), and a fan to provide air flow across the air coil associated with the DX compression system. These objects work together to model a system which heats water using zone air, outdoor air, or a combination of zone and outdoor air as the primary heat source.
-
-The `WaterHeater:HeatPump:WrappedCondenser` compound object, water heater tank object (e.g., `WaterHeater:Mixed`), and fan object (e.g., `Fan:OnOff`) are defined elsewhere in this reference document. `Coil:WaterHeating:AirToWaterHeatPump:Wrapped` object described here models an air-to-water DX compression system to determine its air-side and water-side performance. This DX coil object calculates the air-side sensible and latent cooling capacity at the specific operating conditions for each simulation timestep, as well as the condenser's water-side temperature difference at a given condenser water flow rate.
-
-The heat pump water heater DX coil model performs the following major functions:
-
-- calculates the electric consumption of the DX compressor
-
-- calculates the amount of heat delivered to the water tank
-
-- calculates the electric consumption of the compressor's crankcase heater
-
-- calculates the air-side performance of the DX coil
-
-#### Field: Name
-
-This alpha field defines a unique user-assigned name for an instance of a heat pump water heater DX coil. Any reference to this coil by another object (e.g., `WaterHeater:HeatPump:WrappedCondenser`) will use this name.
-
-#### Field: Rated Heating Capacity
-
-This numeric field defines the DX coil heating capacity in Watts at the rated evaporator inlet air temperatures, rated condenser inlet water temperature, rated evaporator air flow rate, and rated condenser water flow rate specified below. Values must be greater than 0. This value represents water heating capacity, and it may or may not include the impact of condenser pump heat (see field Condenser Pump Heat Included in Rated Heating Capacity below).
-
-#### Field: Rated COP
-
-This numeric field defines the DX coil's water heating coefficient of performance (COP=water heating capacity in watts divided by electrical power input in watts) at rated conditions (rated inlet temperatures and flow rates specified below). This input not only determines the electric energy use of the heat pump DX coil, but also the amount of total air cooling provided by the evaporator. The rated COP includes compressor power, and may or may not include condenser pump power or evaporator fan power (see field Evaporator Fan Power Included in Rated COP and field Condenser Pump Power Included in Rated COP). Values must be greater than 0. If this field is left blank, the default value is 3.2.
-
-#### Field: Rated Sensible Heat Ratio
-
-This numeric field defines the air-side sensible heat ratio (SHR=sensible cooling capacity divided by total cooling capacity) of the DX coil at rated conditions (rated inlet temperatures and flow rates specified below). This value should not include the effect of evaporator fan heat. Values must be greater than or equal to 0.5, and less than or equal to 1.0. The default value is 0.85.
-
-#### Field: Rated Evaporator Inlet Air Dry-Bulb Temperature
-
-This numeric field defines the evaporator inlet air dry-bulb temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 5 &deg;C. If this field is left blank, the default value is 19.7 &deg;C.
-
-#### Field: Rated Evaporator Inlet Air Wet-Bulb Temperature
-
-This numeric field defines the evaporator inlet air wet-bulb temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 5 &deg;C. If this field is left blank, the default value is 13.5 &deg;C.
-
-#### Field: Rated Condenser Water Temperature
-
-This numeric field defines the condenser inlet water temperature, in degrees Celsius, that corresponds to rated coil performance (heating capacity, COP and SHR). Values must be greater than 25 &deg;C. If this field is left blank, the default value is 57.5 &deg;C.
-
-#### Field: Rated Evaporator Air Flow Rate
-
-This numeric field defines the evaporator air volume flow rate in cubic meters per second at rated conditions. Values must be greater than 0. If this field is left blank or autocalculated (field value = **autocalculate**), the default value is 5.035E-5 m<sup>3</sup>/s/W (31.25 cfm/MBH) multiplied by the Rated Heating Capacity specified above. When autocalculating the rated evaporator air volumetric flow rate, a zone sizing object is not required.
-
-#### Field: Evaporator Fan Power Included in Rated COP
-
-This choice field specifies if evaporator fan power is included in the rated COP defined above. This input impacts the calculation of compressor electric power and total air cooling provided by the evaporator for each simulation timestep. If Yes is selected, the evaporator fan power is subtracted from the total electric heating power when calculating total evaporator cooling capacity. If No is selected, it is assumed that the total heating power does not include evaporator fan power. If this field is left blank, the default is Yes. See the Engineering Reference section for `Coil:WaterHeating:AirToWaterHeatPump:\*` for further details.
-
-#### Field: Evaporator Air Inlet Node Name
-
-This alpha field defines the name of the air node from which the evaporator coil draws its inlet air.
-
-#### Field: Evaporator Air Outlet Node Name
-
-This alpha field defines the name of the air node to which the evaporator coil sends its outlet air.
-
-#### Field: Crankcase Heater Capacity
-
-This numeric field defines the compressor's crankcase heater capacity in Watts. The crankcase heater only operates when the compressor is off and the air surrounding the compressor is below the Maximum Ambient Temperature for Crankcase Heater Operation specified below.
-
-#### Field: Maximum Ambient Temperature for Crankcase Heater Operation
-
-This numeric field defines the maximum ambient temperature for crankcase heater operation in degree Celsius. The crankcase heater only operates when the air surrounding the compressor is below this maximum temperature value and the compressor is off. The ambient temperature surrounding the compressor is set by the Heat Pump:Water Heater parent object (field Compressor Location).
-
-#### Field: Evaporator Air Temperature Type for Curve Objects
-
-This choice field specifies the air temperature type used for the heating capacity and COP modifier curve objects below. The valid selections are Dry-bulb Temperature and Wet-bulb Temperature. If dry-bulb temperature is selected, the inlet air dry-bulb temperature entering the heat pump DX coil and fan section is used to evaluate the curve objects. If wet-bulb temperature is selected, the inlet air wet-bulb temperature entering the heat pump DX coil and fan section is used to evaluate the curve objects. If this field is left blank and the following curve names are defined, the default value is wet-bulb temperature. If the following curve names are not defined, this field is not used.
-
-#### Field: Heating Capacity Function of Temperature Curve Name
-
-This alpha field specifies the name of a **biquadratic** or **cubic** performance curve object (ref: Performance Curves) that defines the variation in DX coil heating capacity as a function of inlet fluid (air and water) temperatures. The biquadratic curve uses evaporator inlet air temperature (dry-bulb or wet-bulb temperature based on the field Evaporator Air Temperature Type for Curve Objects defined above) and condenser inlet water temperature as the independent variables. The cubic curve uses evaporator inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The output of this curve is multiplied by the rated heating capacity to give the heating capacity at specific operating conditions (i.e., at temperatures different from the rating point temperatures). The curve should be normalized to have the value of 1.0 at the rating point temperatures. If this field is left blank, the heating capacity remains constant (curve value assumed to be 1.0 for all conditions).
-
-#### Field: Heating Capacity Function of Air Flow Fraction Curve Name
-
-This alpha field specifies the name of a **quadratic** or **cubic** performance curve object (ref: Performance Curves) that defines the variation in DX coil heating capacity as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate. The output of this curve is multiplied by the rated heating capacity and the heating capacity modifier curve (function of temperature) to give the DX coil heating capacity at the specific inlet fluid temperatures and air flow rate at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated evaporator air flow rate (air flow fraction of 1.0). If this field is left blank, the heating capacity remains constant (curve value assumed to be 1.0 for all air flow rates).
-
-#### Field: Heating COP Function of Temperature Curve Name
-
-This alpha field specifies the name of a **biquadratic** or **cubic** performance curve object (ref: Performance Curves) that defines the variation in DX coil heating COP as a function of inlet fluid (air and water) temperatures. The biquadratic curve uses evaporator inlet air temperature (dry-bulb or wet-bulb temperature based on the field Evaporator Air Temperature Type for Curve Objects defined above) and condenser inlet water temperature as the independent variables. The cubic curve uses evaporator inlet air (dry-bulb or wet-bulb) temperature as the independent variable. The output of this curve is multiplied by the rated COP to give the heating COP at specific operating conditions (i.e., at temperatures different from the rating point temperatures). The curve should be normalized to have the value of 1.0 at the rating point temperatures. If this field is left blank, the COP remains constant (curve value assumed to be 1.0 for all conditions).
-
-#### Field: Heating COP Function of Air Flow Fraction Curve Name
-
-This alpha field specifies the name of a **quadratic** or **cubic** performance curve object (ref: Performance Curves) that defines the variation in DX coil heating COP as a function of the ratio of actual air flow rate across the evaporator coil to the rated evaporator air flow rate. The output of this curve is multiplied by the rated COP and the heating COP modifier curve (function of temperature) to give the heating COP at the specific inlet fluid temperatures and air flow rate at which the coil is operating. The curve should be normalized to have the value of 1.0 at the rated evaporator air flow rate (air flow fraction of 1.0). If this field is left blank, the heating COP remains constant (curve value assumed to be 1.0 for all air flow rates).
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a **quadratic** or **cubic** performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the DX unit as a function of the part load ratio (PLR, sensible cooling load/steady-state sensible cooling capacity). The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the effective EIR for a given simulation timestep. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling.
-
-The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7     and     PLF &gt;= PLR
-
-If PLF &lt; 0.7 a warning message is issued, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, then a warning message is issued and the runtime fraction of the coil is limited to 1.0.
-
-A typical part load fraction correlation for a conventional, single-speed DX cooling coil (e.g., residential unit) would be:
-
-           PLF = 0.85 + 0.15(PLR)
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-           PLF = 1.0 + 0.0(PLR)
-
-Following is an example input for the `Coil:WaterHeating:AirToWaterHeatPump:Wrapped` object:
-
-```idf
-Coil:WaterHeating:AirToWaterHeatPump:Wrapped,
-    HPWH Coil,               !- Name
-    2349.6,                  !- Rated Heating Capacity {W}
-    2.4,                     !- Rated COP {W/W}
-    0.981,                   !- Rated Sensible Heat Ratio
-    19.72,                   !- Rated Evaporator Inlet Air Dry-Bulb Temperature {C}
-    13.5,                    !- Rated Evaporator Inlet Air Wet-Bulb Temperature {C}
-    48.89,                   !- Rated Condenser Water Temperature {C}
-    0.189,                   !- Rated Evaporator Air Flow Rate {m3/s}
-    Yes,                     !- Evaporator Fan Power Included in Rated COP
-    HPWH Air Inlet,          !- Evaporator Air Inlet Node Name
-    HPWH Coil Outlet Fan Inlet,  !- Evaporator Air Outlet Node Name
-    0,                       !- Crankcase Heater Capacity {W}
-    10,                      !- Maximum Ambient Temperature for Crankcase Heater Operation {C}
-    WetBulbTemperature,      !- Evaporator Air Temperature Type for Curve Objects
-    HPWH-Htg-Cap-fT,         !- Heating Capacity Function of Temperature Curve Name
-    ,                        !- Heating Capacity Function of Air Flow Fraction Curve Name
-    HPWH-Htg-COP-fT,         !- Heating COP Function of Temperature Curve Name
-    ,                        !- Heating COP Function of Air Flow Fraction Curve Name
-    HPWH-COP-fPLR;           !- Part Load Fraction Correlation Curve Name
-```
-
-### Coil:WaterHeating:AirToWaterHeatPump:Wrapped Outputs
-
-* HVAC,Average,Cooling Coil Total Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Total Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Latent Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Latent Cooling Energy [J]
-
-* HVAC,Average, Cooling Coil Runtime Fraction []
-
-* HVAC,Average,DX Cooling Coil Crankcase Heater Electric Power [W]
-
-* HVAC,Sum, Cooling Coil Crankcase Heater Electric Energy [J]
-
-* HVAC,Average,Cooling Coil Total Water Heating Rate [W]
-
-* HVAC,Sum,Cooling Coil Total Water Heating Energy [J]
-
-* HVAC,Average,Cooling Coil Water Heating Electric Power[W]
-
-* HVAC,Sum,Cooling Coil Water Heating Electric Energy [J]
-
-#### Cooling Coil Total Cooling Rate [W]
-
-This output field is the average total (sensible and latent) cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Total Cooling Energy [J]
-
-This output field is the total (sensible plus latent) cooling output of the DX coil in Joules for the timestep being reported. This is determined by the coil inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Sensible Cooling Rate [W]
-
-This output field is the average moist air sensible cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Sensible Cooling Energy [J]
-
-This output field is the moist air sensible cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### DX Coil Latent Cooling Rate [W]
-
-This output field is the average latent cooling rate output of the DX coil in Watts for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Latent Cooling Energy [J]
-
-This output field is the latent cooling output of the DX coil in Joules for the timestep being reported. This is determined by the inlet and outlet air conditions and the air mass flow rate through the coil.
-
-#### Cooling Coil Runtime Fraction   []
-
-This output field is the average runtime fraction of the DX coil compressor for the timestep being reported. This also represents the runtime fraction of the condenser water pump.
-
-#### Cooling Coil Crankcase Heater Electric Power[W]
-
-This output field is the average electricity consumption rate of the DX coil compressor's crankcase heater in Watts for the timestep being reported. The crankcase heater operates only when the compressor is off and the air surrounding the compressor is below the Maximum Ambient Temperature for Crankcase Heater Operation, otherwise this output variable is set equal to 0.
-
-#### Cooling Coil Crankcase Heater Electric Energy [J]
-
-This output field is the total electricity consumption of the DX coil compressor's crankcase heater in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
-
-#### Cooling Coil Total Water Heating Rate [W]
-
-This output field is the average water heating rate output of the DX coil (condenser coil plus condenser water pump) in Watts for the timestep being reported.
-
-#### Cooling Coil Total Water Heating Energy [J]
-
-This output field is the total water heating output of the DX coil (condenser coil plus condenser water pump) in Joules for the timestep being reported.
-
-#### Cooling Coil Water Heating Electric Power[W]
-
-This output field is the average electricity consumption rate of the DX coil compressor in Watts for the timestep being reported.
-
-#### Cooling Coil Water Heating Electric Energy [J]
-
-This output field is the electricity consumption of the DX coil compressor in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = DHW, Group Key = Plant (ref. Output:Meter objects).
-
-
-### Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
-
-The **Coil:Cooling:WaterToAirHeatPump:ParameterEstimation** coil is a deterministic model that requires parameters to describe the operating conditions of the heat pump's components. The parameters are generated from the manufacturer catalog data using multi-variable optimization method. In addition, the cooling coil model can be used for 3 type of compressors: **reciprocating**, **rotary** and **scroll**. Descriptions and strength of each respective model is available in the following references:
-
-Jin, Hui. 2002. Parameter Estimation Based Models of Water Source Heat Pumps. Phd. Thesis, Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from [http://www.hvac.okstate.edu/](http://www.hvac.okstate.edu))
-
-Tang,C. C. 2005. Modeling Packaged Heat Pumps in Quasi-Steady State Energy Simulation Program. M.S. Thesis. Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from [http://www.hvac.okstate.edu/](http://www.hvac.okstate.edu))
-
-#### Field: Name
-
-This alpha field contains the identifying name for the coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
-
-#### Field: Compressor Type
-
-Type of compressor mode used for the heat pump. Choices available are reciprocating, rotary and scroll compressor. Note that the parameters vary for different compressor.
-
-#### Field: Refrigerant Type
-
-This alpha field contains the type of refrigerant used by the heat pump.
-
-#### Field: Design Source Side Flow Rate
-
-This numeric field defines the water flow rate though the coil in m3/sec
-
-#### Field: Nominal Cooling Coil Capacity
-
-This numeric field defines the nominal cooling capacity for the WatertoAirHP cooling coil in Watts.
-
-#### Field: Nominal Time for Condensate Removal to Begin
-
-This numeric field defines the nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero.
-
-#### Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity
-
-This numeric field defines ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero.
-
-#### Field: High Pressure Cutoff
-
-This numeric field defines the compressor   s maximum allowable pressure in Pascal (N/m2)
-
-#### Field: Low Pressure Cutoff
-
-This numeric field defines the compressor   s minimum allowable pressure in Pascal (N/m2)
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the cooling coil source side inlet node name.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the cooling coil source side outlet node name.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the cooling coil air inlet node name.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the cooling coil air outlet node name.
-
-#### Cooling Coil Parameters
-
-Depending on the type of compressor and the source side fluid specified, the type of parameters and values also differs. An Excel Spreadsheet is developed to estimate the parameters based on the manufacturer data. The general parameters are listed first followed by specific parameters required by the respective compressor model. Lastly, parameters are listed based on the type of source side fluid used.
-
-#### Field: Load Side Total Heat Transfer Coefficient
-
-This numeric field defines the estimated parameter **load side total heat transfer coefficient** in W/K. This field was previously known as Parameter 1.
-
-#### Field: Load Side Outside Surface Heat Transfer Coefficient
-
-This numeric field defines the estimated parameter **load side outside surface heat transfer coefficient** in W/K. This field was previously known as Parameter 2.
-
-#### Field: Superheat Temperature at the Evaporator Outlet
-
-This numeric field defines the estimated parameter **superheat temperature** at the evaporator outlet in ËšC. This field was previously known as Parameter 3.
-
-#### Field: Compressor Power Losses
-
-This numeric field defines the estimated parameter **compressor power losses**, which accounts for the loss of work due to mechanical and electrical losses in the compressor in Watts. This field was previously known as Parameter 4.
-
-#### Field: Compressor Efficiency
-
-This numeric field defines the estimated parameter of the **compressor   s efficiency**. The compressor efficiency is formulated as the equation below:
-
-<div>\[\eta  = \frac{{{{\dot W}_{Theoritical}}}}{{{{\dot W}_{CompInput}} - {{\dot W}_{Loss}}}}\]</div>
-
-This field was previously know as Parameter 5.
-
-#### Field: Compressor Piston Displacement
-
-This numeric field defines the estimated parameter **piston displacement of the compressor** in m3/s. This field was part of what was previously known as Parameter 6. It should be used when the Compressor type is either Reciprocating and Rotary. The field should be left blank when Compressor type is Scroll.
-
-#### Field: Compressor Suction/Discharge Pressure Drop
-
-This numeric field defines the estimated parameter **pressure drop** at the compressor suction and discharge in Pascals (N/m2). This field was part of what was previously known as Parameter 7. It should be used when the Compressor type is either Reciprocating and Rotary. The field should be left blank when Compressor type is Scroll.
-
-#### Field: Compressor Clearance Factor
-
-This numeric field defines the estimated parameter **clearance factor of the compressor**. This parameter is dimensionless. This field was part of what was previously known as Parameter 8. It should only be used when the Compressor type is Reciprocating. The field should be left blank when Compressor type is Scroll or Rotary.
-
-#### Field: Refrigerant Volume Flow Rate
-
-This numeric field defines the **refrigerant volume flow rate** at the beginning of the compression [m3/s]. This field was part of what was previously known as Parameter 6. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
-
-#### Field: Volume Ratio
-
-This numeric field defines the built-in-**volume ratio**. This field was part of what was previously known as Parameter 7. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
-
-#### Field: Leak Rate Coefficient
-
-This numeric field defines the **leak rate coefficient** for the relationship between pressure ratio and leakage rate. This field was part of what was previously known as Parameter 8. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
-
-#### Field: Source Side Heat Transfer Coefficient
-
-This numeric field defines the estimated parameter **source side heat transfer coefficient** in W/K. This field was part of what was previously known as Parameter 9. It should only be used when the Source Side Fluid Name is Water.
-
-#### Field: Source Side Heat Transfer Resistance1
-
-This numeric field defines the estimated parameter **source side heat transfer resistance** 1. Unit is dimensionless. This field was part of what was previously known as Parameter 9. It should only be used when the Source Side Fluid Name is an antifreeze.
-
-#### Field: Source Side Heat Transfer Resistance2
-
-This numeric field defines the estimated parameter **source side heat transfer resistance** 2. Unit is W/K. This field was previously known as Parameter 10. It should only be used when the Source Side Fluid Name is an antifreeze.
-
-Following is an example for COIL:WaterToAirHP:ParameterEstimation:Cooling coil input
-
-```idf
-   Coil:Cooling:WaterToAirHeatPump:ParameterEstimation,
-       Heat Pump Cooling Mode AHU1,   !- Name
-       Scroll,                                   !- Compressor Type
-       R22,                                         !- Refrigerant Type
-       0.0015,                                   !- Design Source Side Flow Rate {m3/s}
-       38000,                                     !- Nominal Cooling Coil Capacity {W}
-       0,                                             !- Nominal Time for Condensate Removal to Begin {s}
-       0,         !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
-       3000000,                                 !- High Pressure Cutoff {Pa}
-       0,                                             !- Low Pressure Cutoff {Pa}
-       AHU1 Water to Air Heat Pump Source Side1 Inlet Node,   !- Water Inlet Node Name
-       AHU1 Water to Air Heat Pump Source Side1 Outlet Node,   !- Water Outlet Node Name
-       AHU 1 Supply Fan Outlet, !- Air Inlet Node Name
-       Cooling Coil Air Outlet Node AHU1,   !- Air Outlet Node Name
-       3.78019E+03,                         !- Load Side Total Heat Transfer Coefficient {W/K}
-       3.41103E+03,                         !- Load Side Outside Surface Heat Transfer Coefficient {W/K}
-       1.57066E+00,                         !- Superheat Temperature at the Evaporator Outlet {C}
-       2.23529E+03,                         !- Compressor Power Losses {W}
-       1.34624E+00,                         !- Compressor Efficiency
-       ,                                               !- Compressor Piston Displacement {m3/s}
-       ,                                               !- Compressor Suction/Discharge Pressure Drop {Pa}
-       ,                                               !- Compressor Clearance Factor {dimensionless}
-       9.74424E-03,                         !- Refrigerant Volume Flow Rate {m3/s}
-       2.30803E+00,                         !- Volume Ratio {dimensionless}
-       2.06530E-02,                         !-Leak Rate Coefficient
-       1.92757E+03,                         !- Source Side Heat Transfer Coefficient {W/K}
-       ,                                               !- Source Side Heat Transfer Resistance1 {dimensionless}
-       ;                                               !- Source Side Heat Transfer Resistance2 {W/K}
-```
-
-### Coil:Cooling:WaterToAirHeatPump:EquationFit
-
-The Coil:Cooling:WaterToAirHeatPump:EquationFit is a simple curve-fit model that requires coefficients generated from the heat pump catalog data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. The performance of the heat pump is modeled using curves fitted from the catalog data. Description of the equation-fit model is available in the following reference:
-
-Tang,C. C. 2005. Modeling Packaged Heat Pumps in Quasi-Steady State Energy Simulation Program. M.S. Thesis. Department of Mechanical and Aerospace Engineering, Oklahoma State University. (downloadable from [http://www.hvac.okstate.edu/](http://www.hvac.okstate.edu))
-
-#### Field: Name
-
-This alpha field contains the identifying name for the coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the cooling coil source side inlet node name.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the cooling coil source side outlet node name.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the cooling coil air inlet node name.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the cooling coil air outlet node name.
-
-#### Field: Rated Air Flow Rate
-
-This numeric field contains the rated volumetric air flow rate on the load side of the heat pump in m3/s. This field is autosizable.
-
-#### Field: Rated Water Flow Rate
-
-This numeric field contains the rated volumetric water flow rate on the source side of the heat pump in m3/s. This field is autosizable.
-
-#### Field: Gross Rated Total Cooling Capacity
-
-This numeric field contains the gross rated total cooling capacity of the heat pump in W. This field is autosizable.The gross rated total cooling capacity should be within 20% of the gross rated heating capacity, otherwise a warning message is issued. The gross rated total cooling capacity shouldnot account for the effect of supply air fan heat.
-
-#### Field: Gross Rated Sensible Cooling Capacity
-
-This numeric field contains the gross rated sensible capacity of the heat pump in W. This field is autosizable. The gross rated sensible cooling capacity shouldnot account for the effect of supply air fan heat.
-
-#### Field: Rated Cooling Coefficient of Performance
-
-This numeric field contains the rated cooling coefficient of performance of the heat pump.
-
-#### Field: Total Cooling Capacity Coefficient 1 to 5
-
-These numeric fields contain the first to fifth coefficient for the heat pump total cooling capacity.
-
-#### Field: Sensible Cooling Capacity Coefficient 1 to 6
-
-These numeric fields contain the first to sixth coefficient for the heat pump sensible cooling capacity.
-
-#### Field: Cooling Power Consumption Coefficient 1 to 5
-
-These numeric fields contain the first to fifth coefficient for the heat pump power consumption.
-
-#### Field: Nominal Time for Condensate Removal to Begin
-
-This numeric field defines the nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero.
-
-#### Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity
-
-This numeric field defines ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero.
-
-Following is an example of the input for Coil:WaterToAirHP:EquationFit:Cooling coil
-
-```idf
-Coil:Cooling:WaterToAirHeatPump:EquationFit,
-       Heat Pump Cooling Mode,!- Name of Coil
-       Water to Air Heat Pump Source Side1 Inlet Node,!- Coil Water Inlet Node Name
-       Water to Air Heat Pump Source Side1 Outlet Node,!- Coil Water Outlet Node Name
-       Cooling Coil Air Inlet Node,!- Coil Air Inlet Node Name
-       Heating Coil Air Inlet Node,!- Coil Air Outlet Node Name
-       4.6015E-01,!- Rated Air Volumetric Flow Rate
-       2.8391E-04,!- Rated Water Volumetric Flow Rate
-       23125.59,!- Gross Rated Total Cooling Capacity
-       16267.05,!- Gross Rated Sensible Cooling Capacity
-       4.7,!- Rated Cooling Coefficient of Performance
-       -0.68126221,!- Total Cooling Capacity Coefficient 1
-       1.99529297,!- Total Cooling Capacity Coefficient 2
-       -0.93611888,!- Total Cooling Capacity Coefficient 3
-       0.02081177,!- Total Cooling Capacity Coefficient 4
-       0.008438868,!- Total Cooling Capacity Coefficient 5
-       2.24209455,!- Sensible Cooling Capacity Coefficient 1
-       7.28913391,!- Sensible Cooling Capacity Coefficient 2
-       -9.06079896,!- Sensible Cooling Capacity Coefficient 3
-       -0.36729404,!- Sensible Cooling Capacity Coefficient 4
-       0.218826161,!- Sensible Cooling Capacity Coefficient 5
-       0.00901534,!- Sensible Cooling Capacity Coefficient 6
-       -3.20456384,!- Cooling Power Consumption Coefficient 1
-       0.47656454,!- Cooling Power Consumption Coefficient 2
-       3.16734236,!- Cooling Power Consumption Coefficient 3
-       0.10244637,!- Cooling Power Consumption Coefficient 4
-       -0.038132556,!- Cooling Power Consumption Coefficient 5
-       0,!- Nominal Time for Condensate Removal to Begin
-       0;!- Ratio of Initial Moisture Evaporation Rate and Steady-state Latent Capacity
-```
-
-### Water to Air Heat Pump Cooling Coil (Parameter Estimation and Equation Fit) Outputs
-
-Coil:Cooling:WaterToAirHeatPump:ParameterEstimation and Coil:Cooling:WaterToAirHeatPump:EquationFit have the same output variables listed as follows;
-
-* HVAC, Average, Cooling Coil Electric Power [W]
-
-* HVAC, Average, Cooling Coil Total Cooling Rate [W]
-
-* HVAC, Average, Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC, Average, Cooling Coil Source Side Heat Transfer Rate [W]
-
-* HVAC, Average, Cooling Coil Part Load Ratio []
-
-* HVAC, Average, Cooling Coil Runtime Fraction []
-
-* HVAC, Average, Cooling Coil Air Mass Flow Rate [kg/s]
-
-* HVAC, Average, Cooling Coil Air Inlet Temperature [C]
-
-* HVAC, Average, Cooling Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC, Average, Cooling Coil Air Outlet Temperature [C]
-
-* HVAC, Average, Cooling Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC, Average, Cooling Coil Source Side Mass Flow Rate [kg/s]
-
-* HVAC, Average, Cooling Coil Source Side Inlet Temperature [C]
-
-* HVAC, Average, Cooling Coil Source Side Outlet Temperature [C]
-
-* HVAC, Sum, Cooling Coil Electric Energy [J]
-
-* HVAC, Sum, Cooling Coil Total Cooling Energy [J]
-
-* HVAC, Sum, Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC, Sum, Cooling Coil Latent Cooling Energy [J]
-
-* HVAC, Average, Cooling Coil Latent Cooling Rate [W]
-
-* HVAC, Sum, Cooling Coil Source Side Heat Transfer Energy [J]
-
-#### Cooling Coil Electric Power [W]
-
-This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
-
-#### Cooling Coil Total Cooling Rate [W]
-
-The output variable is the average total cooling load provide by the heat pump which includes the sensible and latent load in Watts over the timestep being reported.
-
-#### Cooling Coil Sensible Cooling Rate [W]
-
-The output variable is the average sensible cooling load provide by the heat pump in Watts over the timestep being reported.
-
-#### Cooling Coil Source Side Heat Transfer Rate [W]
-
-The output variable is the average heat rejected to the water at the heat pump condenser in Watts over the timestep being reported.
-
-#### Cooling Coil Part Load Ratio []
-
-This output variable is the ratio of the part-load capacity to the steady state capacity of the WatertoAirHP coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the WatertoAirHP coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
-
-#### Cooling Coil Runtime Fraction []
-
-This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The duty factor or part load fraction accounts for efficiency losses due to compressor cycling.
-
-#### Cooling Coil Air Mass Flow Rate [kg/s]
-
-The output variable is the average air mass flow rate going through the heat pump over the timestep being reported.
-
-#### Cooling Coil Air Inlet Temperature [C]
-
-The output variable is the average entering air dry-bulb temperature over the timestep being reported.
-
-#### Cooling Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average entering air dry humidity ratio over the timestep being reported.
-
-#### Cooling Coil Air Outlet Temperature [C]
-
-The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
-
-#### Cooling Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average leaving air dry humidity ratio over the timestep being reported.
-
-#### Cooling Coil Source Side Mass Flow Rate [kg/s]
-
-The output variable is the average water mass flow rate going through the heat pump over the timestep being reported.
-
-#### Cooling Coil Source Side Inlet Temperature [C]
-
-The output variable is the average entering water temperature over the timestep being reported.
-
-#### Cooling Coil Source Side Outlet Temperature [C]
-
-The output variable is the average leaving water temperature over the timestep being reported.
-
-#### Cooling Coil Electric Energy [J]
-
-The output variable is the electric consumption of the heat pump in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cooling, Group Key = System (ref. Output:Meter objects).
-
-#### Cooling Coil Total Cooling Energy [J]
-
-The output variable is the total cooling output of the coil in Joules over the timestep being reported. Resource Type = EnergyTransfer, End Use Key = CoolingCoils, Group Key = System (ref. Output:Meter objects).
-
-#### Cooling Coil Sensible Cooling Energy [J]
-
-The output variable is the total sensible cooling output of the coil in Joules over the timestep being reported
-
-#### Cooling Coil Latent Cooling Energy [J]
-
-#### Cooling Coil Latent Cooling Rate [W]
-
-These output variables are the total latent cooling output of the coil in Joules or Watts over the timestep being reported.
-
-#### Cooling Coil Source Side Heat Transfer Energy [J]
-
-The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported
-
-------------------------------------------------------------------------
-
-[[1]](#_ftnref1) The 23.9 &deg;C wet-bulb temperature condition is not applicable for air-cooled condensers which do not evaporate condensate.
-
-[[2]](#_ftnref2) The 23.9 &deg;C wet-bulb temperature condition is not applicable for air-cooled condensers which do not evaporate condensate.
-
-[[3]](#_ftnref3) The 23.9 &deg;C wet-bulb temperature condition is not applicable for air-cooled condensers which do not evaporate condensate.
-
-[[4]](#_ftnref4) The 23.9 &deg;C wet-bulb temperature condition is not applicable for air-cooled condensers which do not evaporate condensate.
-
-### Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit
-
-The Variable-Speed Water-to-Air Cooling Equation Fit Coil is a collection of performance curves that represent the cooling coil at various speed levels. The performance curves should be generated from the heat pump Reference Unit data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. On the other hand, the model uses the bypass factor approach to calculate sensible heat transfer rate, similar to the one used in the single-speed DX coil. The number of speed levels can range from 2 to 10. The cooling coil has four node connections, i.e. two air sides and two water sides. The user needs to specify a nominal speed level, at which the gross rated total cooling capacity, rated volumetric air and water flow rates are sized. The rated capacity, rated volumetric flow rates represent the real situation in the air and water loops, and are used to determine and flow rates at various speed levels in the parent objects, e.g. AirLoopHVAC:UnitaryHeatPump:WaterToAir and ZoneHVAC:WaterToAirHeatPump. It shall be mentioned that the performance correction curves, i.e. the temperature and flow fraction correction curves, should be normalized to the capacity and flow rates at each individual speed and at the rated conditions, similar to the performance curves used in the DX coils. However, the performance values, e.g. gross capacities, gross COPs, gross SHRs and flow rates at individual speed levels, should be given regarding a specific unit from the Reference Unit catalog data. In the following content, the statement started with    Reference Unit    means the actual Reference Unit catalog data. The rated conditions for obtaining the capacities, COPs and SHRs   are at indoor dry-bulb temperature of 26.67 ËšC (80 ËšF), wet bulb temperature of 19.44 ËšC (67 ËšF),   and the source side entering water temperature of 29.4 ËšC (85 ËšF). Some equations are provided below to help explain the function of the various performance curves and data fields. For a detailed description of the algorithm and how the curves are used in the calculations, please see the Engineering Reference.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the variable speed cooling coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the cooling coil source side inlet node name.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the cooling coil source side outlet node name.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the cooling coil load side inlet node name.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the cooling coil load side outlet node name.
-
-#### Field: Number of Speeds
-
-This numeric field contains the maximum number of speed levels that the module uses. The number of speeds, for which the user input the performance data and curves, should be equal or higher than the maximum number. The performance inputs at higher speed levels are ignored.
-
-#### Field: Nominal Speed Level
-
-This numeric field defines the nominal speed level, at which the rated capacity, rated air and water volumetric flow rates are correlated.
-
-#### Field: Gross Rated Total Cooling Capacity at Selected Nominal Speed Level
-
-This numeric field contains the gross rated total cooling capacity at the nominal speed level.   This field is autosizable. The gross rated total cooling capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
-
-<div>\[CapacityScaleFactor = \frac{{GrossRatedTotalCoolingCapacity}}{{ReferenceUnitCapacity@NominalSpeedLevel}}\]</div>
-
-And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below,
-
-<div>\[\begin{array}{l}GrossRatedCapacity@SpeedLevel\left( x \right) = CapacityScaleFactor\\\quad \quad \quad \quad  \times ReferenceUnitCapacity@SpeedLevel(x)\end{array}\]</div>
-
-#### Field: Rated Volumetric Air Flow Rate
-
-This numeric field contains the rated volumetric air flow rate on the load side of the heat pump corresponding to the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects.   It is recommended that the ratio of the rated volumetric air flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
-
-<div>\[\begin{array}{l}AirFlowScaleFactor = \\\quad \quad \quad \quad \quad \frac{{RatedVolumetricAirFlowRate}}{{ReferenceUnitVolAirFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}\end{array}\]</div>
-
-And the volumetric air flow rates in the parent objects are calculated as below,
-
-<div>\[\begin{array}{l}LoopVolumetricAirFlowRate@SpeedLevel\left( x \right) = AirFlowScaleFactor\\\quad \quad \quad  \times ReferenceUnitVolAirFlowRate@SpeedLevel(x)\\\quad \quad \quad  \times CapacityScaleFactor\end{array}\]</div>
-
-#### Field: Rated Volumetric Water Flow Rate
-
-This numeric field contains the rated volumetric water flow rate on the source side of the heat pump at the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the water flow rates in the water loop.   It is recommended that the ratio of the rated volumetric water flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
-
-<div>\[\begin{array}{l}WaterFlowScaleFactor = \\\quad \quad \quad \frac{{RatedVolumetricWaterFlowRate}}{{ReferenceUnitVolWaterFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}\end{array}\)image5\(\begin{array}{l}WaterFlowScaleFactor = \\\quad \quad \quad \frac{{RatedVolumetricWaterFlowRate}}{{ReferenceUnitVolWaterFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}\end{array}\]</div>
-
-And the required volumetric water flow rates at the speed levels in the parent objects, other than the nominal speed, are calculated as below,
-
-<div>\[\begin{array}{l}LoopVolumetricWaterFlowRate@SpeedLevel\left( x \right) = WaterFlowScaleFactor\\\quad \quad \quad  \times ReferenceUnitVolWaterFlowRate@SpeedLevel(x)\\\quad \quad \quad  \times CapacityScaleFactor\end{array}\]</div>
-
-#### Field: Nominal Time for Condensate Removal to Begin
-
-This numeric field defines the nominal time (in seconds) after startup for condensate to begin leaving the coil's condensate drain line at the coil's rated airflow and temperature conditions, starting with a dry coil. Nominal time is equal to the ratio of the energy of the coil's maximum condensate holding capacity (J) to the coil's steady-state latent capacity (W). Suggested value is 1000; zero value means the latent degradation model is disabled. The default value for this field is zero.
-
-#### Field: Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity
-
-This numeric field defines ratio of the initial moisture evaporation rate from the cooling coil (when the compressor first turns off, in Watts) and the coil's steady-state latent capacity (Watts) at rated airflow and temperature conditions. Suggested value is 1.5; zero value means the latent degradation model is disabled. The default value for this field is zero.
-
-#### Field: Flag for Using Hot Gas Reheat, 0 or 1
-
-This numeric field dictates whether to use the recoverable waste heat for reheating the supply air, downstream of the coil. The value    1    means using the hot gas reheating, and    0    means not using. If the hot gas reheating is turned on, the recoverable waste heat is subtracted from both the total cooling capacity and the sensible cooling capacity. The default value for this field is zero.
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, sensible or latent load/steady-state sensible or latent cooling capacity for Speed 1), in the case that the unit operates under the lowest speed, i.e. on/off. The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the    effective    EIR for a given simulation timestep for Speed 1. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7 and PLF &gt;= PLR
-
-If PLF &lt; 0.7, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, the runtime fraction of the coil is limited to 1.0. A typical part load fraction correlation would be:
-
-<div>\[PLF = 0.85 + 0.15 \times PLR\]</div>
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-<div>\[PLF = 0.85 + 0.0 \times PLR\]</div>
-
-#### Field Group: rated specification, performance curves, and waste heat data
-
-The performance for each cooling speed must be specified as shown below. They should be directly given from the Reference Unit catalog data. All inputs for Speed 1 are required, followed by the optional inputs for other speeds.
-
-#### Field: Speed &lt;x&gt; Reference Unit Gross Rated Total Cooling Capacity
-
-This numeric field defines the total, full load cooling capacity in watts of the water-to-air cooling coil unit at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0. The gross rated total capacity should not account for the effect of supply air fan heat.
-
-#### Field: Speed &lt;x&gt; Reference Unit Gross Rated Sensible Heat Ratio
-
-This numeric field defines sensible heat transfer ratio (SHR = gross sensible cooling capacity divided by gross total cooling capacity) of the cooling coil unit at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0.0 and less than 1.0. This value should be obtained from the Reference Unit data. The gross rated SHR should not account for the effect of supply air fan heat.
-
-#### Field: Speed &lt;x&gt; Reference Unit Gross Rated Cooling COP
-
-This numeric field defines the coefficient of performance (COP=gross total cooling capacity in watts divided by electrical power input in watts) of the cooling coil unit at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0. The input power includes power for the compressor(s) and accessories, but does not include the power consumptions of the indoor supply air fan and water pump. The gross COP should not account for the supply air fan.
-
-#### Field: Speed &lt;x&gt; Reference Unit Rated Air Flow Rate
-
-This numeric field defines the volumetric air flow rate, in m<sup>3</sup>per second, across the cooling coil at rated conditions for Speed &lt;x&gt; operation. The value entered here should be directly from the Reference Unit data, corresponding to the given gross rated total cooling capacity and gross rated cooling COP at the speed, as above.
-
-#### Field: Speed &lt;x&gt; Reference Unit Rated Water Flow Rate
-
-This numeric field defines the volumetric water flow rate, in m<sup>3</sup>per second, flowing at the source side of the cooling coil at rated conditions for Speed &lt;x&gt; operation. The value entered here should be directly from the Reference Unit data, corresponding to the given gross rated total cooling capacity and gross rated cooling COP at the speed, as above.
-
-#### Field: Speed &lt;x&gt; Total Cooling Capacity Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the both the indoor wet-bulb and source side entering water temperature, from the Reference Unit. The output of this curve is multiplied by the gross rated total cooling capacity at the speed to give the gross total cooling capacity at specific temperature operating conditions (i.e., at an indoor air wet-bulb temperature or entering water temperature different from the rating point temperature). It should be noted that the curve is normalized to the cooling capacity at Speed&lt;x&gt; from the Reference Unit data, and have the value of 1.0 at the rating point.
-
-#### Field: Speed &lt;x&gt; Total Cooling Capacity Function of Air Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of full load flow at Speed &lt;x&gt;, from the Reference Unit data). The curve is normalized to have the value of 1.0 when the actual air flow rate equals the design air flow rate, at Speed &lt;x&gt;.
-
-#### Field: Speed &lt;x&gt; Total Cooling Capacity Function of Water Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the gross total cooling capacity as a function of the ratio of actual water flow rate across the cooling coil to the design water flow rate (i.e., fraction of full load flow), at Speed &lt;x&gt;, from the Reference Unit data. The curve is normalized to have the value of 1.0 when the actual water flow rate equals the design air flow rate, at Speed &lt;x&gt;.
-
-The actual total cooling capacity at Speed &lt;x&gt;, considering variations in temperatures, air and water flow rates is calculated as below:
-
-<div>\[\begin{array}{l}ActualCapacity@SpeedLevel\left( x \right) = CapacityScaleFactor\\\quad \quad \quad  \times ReferenceUnitCapacity@SpeedLevel(x)\\\quad \quad \quad  \times TotCapTempModFac@SpeedLevel(x)\\\quad \quad \quad  \times TotCapAirFlowModFac@SpeedLevel(x)\\\quad \quad \quad  \times TotCapWaterFlowModFac@SpeedLevel(x)\end{array}\]</div>
-
-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve for
-
-Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor air wet-bulb and entering water temperatures The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP at Speed &lt;x&gt; from the Reference Unit data) to give the EIR at specific temperature operating conditions (i.e., at an indoor air wet-bulb temperature or entering water temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
-
-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Air Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the design air flow rate (i.e., fraction of full load flow, at Speed &lt;x&gt; from the Reference Unit data). The EIR is the inverse of the COP. This curve is normalized to a value of 1.0 when the actual air flow rate equals the design air flow rate.
-
-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Water Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual water flow rate across the cooling coil to the design water flow rate (i.e., fraction of full load flow, at Speed &lt;x&gt; from the Reference Unit data). This curve is normalized to a value of 1.0 when the actual air flow rate equals the design air flow rate.
-
-The actual EIR at Speed &lt;x&gt;, considering variations in temperatures, air and water flow rates is calculated as below:
-
-<div>\[\begin{array}{l}ActualEIR@SpeedLevel\left( x \right) = \frac{{1.0}}{{ReferenceUnitCOP@SpeedLevel(x)}}\\\quad \quad \quad  \times EIRTempModFac@SpeedLevel(x)\\\quad \quad \quad  \times EIRAirFlowModFac@SpeedLevel(x)\\\quad \quad \quad  \times EIRWaterFlowModFac@SpeedLevel(x)\end{array}\]</div>
-
-And, the actual power consumption is calculated:
-
-<div>\[\begin{array}{l}ActualPower@SpeedLevel\left( x \right) = ActualCapacity@SpeedLevel\left( x \right)\\\quad \quad \quad \quad  \times ActualEIR@SpeedLevel\left( x \right)\end{array}\]</div>
-
-#### Field: Speed &lt;x&gt; Reference Unit Waste Heat Fraction of Power Input
-
-The fraction of heat input to cooling that is available as recoverable waste heat at full load and rated conditions for Speed &lt;x&gt; operation. The part of heat is not discharged to the water loop. And it can be used for hot gas reheating during dehumidification operation, by setting 1 to Flag for Using Hot Gas Reheat.
-
-#### Field: Speed &lt;x&gt; Waste Heat Function of Temperature Curve Name
-
-The name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the waste heat recovery as a function of indoor wet-bulb temperature and the entering water temperature for Speed &lt;x&gt; from the Reference Unit data. The output of this curve is multiplied by the design recoverable waste heat at specific temperature operating conditions (i.e., at temperatures different from the rating point). The curve is normalized to a value of 1.0 at the rating point.
-
-The actual recoverable waste heat at Speed &lt;x&gt; is calculated as below:
-
-<div>\[\begin{array}{l}ActualWasteHeat@SpeedLevel\left( x \right) = ActualPower@SpeedLevel\left( x \right)\\\quad \quad \quad \quad  \times WasteHeatFrac@SpeedLevel(x)\\\quad \quad \quad \quad  \times WasteHeatTempModFac@SpeedLevel(x)\end{array}\]</div>
-
-An example of this statement in an IDF is:
-
-```idf
-Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit,
-       Sys 1 Heat Pump Cooling Mode,                                              !- Name
-       Sys 1 Water to Air Heat Pump Source Side1 Inlet Node,   !- Water Inlet Node Name
-       Sys 1 Water to Air Heat Pump Source Side1 Outlet Node, !- Water Outlet Node Name
-       Sys 1 Cooling Coil Air Inlet Node,                                    !- Air Inlet Node Name
-       Sys 1 Heating Coil Air Inlet Node,                                    !- Air Outlet Node Name
-       10.0,                                                                                                !- Number of Speeds
-       10.0,                                                                                                !- Nominal Speed Level
-       Autosize,                                                                                      !- Gross Rated Total Cooling Capacity {W}
-       Autosize,                                                                                      !- Rated Air Flow Rate {m3/s}
-       Autosize,                                                                                      !- Rated Water Flow Rate {m3/s}
-       0.0,                                     !Nominal time for Condensate to Begin Leaving the Coil
-       0.0,                                     !Initial Moisture Evaporation Rate Divided by Steady-State AC Latent Capacity
-       1,                                !Flag for Using Hot Gas Reheat or Not, 0 = false; 1 = true
-       VS Energy Part Load Fraction 1,   !Energy Part Load Fraction Curve
-       1524.1,                                    !-Speed 1 Reference Unit Gross Rated Total Cooling Capacity
-       0.75,                                     !-Speed 1 Reference Unit Gross Sensible Heat Ratio
-       4.0,                                       !-Speed 1 Reference Unit Gross Cooling COP
-       0.1359072,                           !-Speed 1 Reference Unit Rated air flow rate
-       0.000381695,                       !-Speed 1 Reference Unit Rated water flow rate
-       TC VS Temp1 Test,             !-Speed 1 Total Cooling Capacity Function of Temperature Curve Name
-       TC VS AirFrac Test,          !-Speed 1 Total Cooling Capacity Function of Air Flow Fraction Curve Name
-       TC VS WaterFrac Test,     !-Speed 1 Total Cooling Capacity Function of Water Flow Fraction Curve Name
-       EIR VS Temp1 Test,             !-Speed 1 Energy Input Ratio Function of Temperature Curve Name
-       EIR VS AirFrac Test,        !-Speed 1 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIR VS WaterFrac Test,     !-Speed 1 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                        !-Speed 1 Waste Heat fraction to power input
-       wasteHeat VS Temp1 Test, !-Speed 1 Waste Heat Function of Temperature Curve Name
-       1877.9,                                      !-Speed 2 Reference Unit Gross Rated Total Cooling Capacity
-       0.75,                                       !-Speed 2 Reference Unit Gross Sensible Heat Ratio
-       4.0,                                         !-Speed 2 Reference Unit Gross Cooling COP
-       0.151008,                               !-Speed 2 Reference Unit Rated air flow rate
-       0.000381695,                         !-Speed 2 Reference Unit Rated water flow rate
-       TC VS Temp1 Test,               !-Speed 2 Total Cooling Capacity Function of Temperature Curve Name
-       TC VS AirFrac Test,          !-Speed 2   Total Cooling Capacity Function of Air Flow Fraction Curve Name
-       TC VS WaterFrac Test,     !-Speed 2   Total Cooling Capacity Function of Water Flow Fraction Curve Name
-       EIR VS Temp1 Test,             !-Speed 2   Energy Input Ratio Function of Temperature Curve Name
-       EIR VS AirFrac Test,        !-Speed 2   Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIR VS WaterFrac Test,     !-Speed 2   Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                        !-Speed 2   Waste Heat fraction to power input
-       wasteHeat VS Temp1 Test, !-Speed 2   Waste Heat Function of Temperature Curve Name
-       2226.6,                                      !-Speed 3 Reference Unit Gross Rated Total Cooling Capacity
-       0.75,                                       !-Speed 3 Reference Unit Gross Sensible Heat Ratio
-       4.0,                                         !-Speed 3 Reference Unit Gross Cooling COP
-       0.1661088,                               !-Speed 3 Reference Unit Rated air flow rate
-       0.000381695,                           !-Speed 3 Reference Unit Rated water flow rate
-       TC VS Temp1 Test,                 !-Speed 3 Total Cooling Capacity Function of Temperature Curve Name
-       TC VS AirFrac Test,      !-Speed 3 Total Cooling Capacity Function of Air Flow Fraction Curve Name
-       TC VS WaterFrac Test,   !-Speed 3 Total Cooling Capacity Function of Water Flow Fraction Curve Name
-       EIR VS Temp1 Test,        !-Speed 3 Energy Input Ratio Function of Temperature Curve Name
-       EIR VS AirFrac Test,     !-Speed 3 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIR VS WaterFrac Test, !-Speed 3 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                        !-Speed 3 Waste Heat fraction to power input
-       wasteHeat VS Temp1 Test,!-Speed 3 Waste Heat Function of Temperature Curve Name
-       2911.3,                                  !-Speed 4 Reference Unit Gross Rated Total Cooling Capacity
-       0.75,                                   !-Speed 4 Reference Unit Gross Sensible Heat Ratio
-       4.0,                                     !-Speed 4 Reference Unit Gross Cooling COP
-       0.1963104,                         !-Speed 4 Reference Unit Rated air flow rate
-       0.000381695,                     !-Speed 4 Reference Unit Rated water flow rate
-       TC VS Temp1 Test,           !-Speed 4 Total Cooling Capacity Function of Temperature Curve Name
-       TC VS AirFrac Test,      !-Speed 4 Total Cooling Capacity Function of Air Flow Fraction Curve Name
-       TC VS WaterFrac Test, !-Speed 4 Total Cooling Capacity Function of Water Flow Fraction Curve Name
-       EIR VS Temp1 Test,        !-Speed 4 Energy Input Ratio Function of Temperature Curve Name
-       EIR VS AirFrac Test,    !-Speed 4 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIR VS WaterFrac Test, !-Speed 4 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                    !-Speed 4 Waste Heat fraction to power input
-       wasteHeat VS Temp1 Test, !-Speed 4 Waste Heat Function of Temperature Curve Name
-       3581.7,                                  !- Speed 5 Reference Unit Gross Rated Total Cooling Capacity
-       0.75,                                   !- Speed 5 Reference Unit Gross Sensible Heat Ratio
-       4.0,                                     !- Speed 5 Reference Unit Gross Cooling COP
-       0.226512,                           !- Speed 5 Reference Unit Rated air flow rate
-       0.000381695,                     !- Speed 5 Reference Unit Rated water flow rate
-       TC VS Temp1 Test,           !- Speed 5 Total Cooling Capacity Function of Temperature Curve Name
-       TC VS AirFrac Test,      !- Speed 5 Total Cooling Capacity Function of Air Flow Fraction Curve Name
-       TC VS WaterFrac Test, !- Speed 5 Total Cooling Capacity Function of Water Flow Fraction Curve Name
-       EIR VS Temp1 Test,        !- Speed 5 Energy Input Ratio Function of Temperature Curve Name
-       EIR VS AirFrac Test,    !- Speed 5 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIR VS WaterFrac Test, !- Speed 5 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                    !- Speed 5 Waste Heat fraction to power input
-       wasteHeat VS Temp1 Test, !- Speed 5 Waste Heat Function of Temperature Curve Name
-       4239.5,                                !-Speed 6 Reference Unit Gross Total Cooling Capacity
-       0.75,                                   !-Speed 6 Reference Unit Gross Sensible Heat Ratio
-       4.0,                                     !-Speed 6 Reference Unit Gross Cooling COP
-       0.2567136,                         !-Speed 6 Reference Unit Rated air flow rate
-       0.000381695,                     !-Speed 6 Reference Unit Rated water flow rate
-       TC VS Temp1 Test,           !-Speed 6 Total Cooling Capacity Function of Temperature Curve Name
-       TC VS AirFrac Test,      !-Speed 6 Total Cooling Capacity Function of Air Flow Fraction Curve Name
-       TC VS WaterFrac Test, !-Speed 6 Total Cooling Capacity Function of Water Flow Fraction Curve Name
-       EIR VS Temp1 Test,        !-Speed 6 Energy Input Ratio Function of Temperature Curve Name
-       EIR VS AirFrac Test,    !-Speed 6 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIR VS WaterFrac Test, !-Speed 6 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                    !-Speed 6 Waste Heat fraction to power input
-       wasteHeat VS Temp1 Test, !-Speed 6 Waste Heat Function of Temperature Curve Name
-       4885.7,                                  !-Speed 7 Reference Unit Gross Rated Total Cooling Capacity
-       0.75,                                   !-Speed 7 Reference Unit Gross Sensible Heat Ratio
-       4.0,                                     !-Speed 7 Reference Unit Gross Cooling COP
-       0.2869152,                         !-Speed 7 Reference Unit Rated air flow rate
-       0.000381695,                     !-Speed 7 Reference Unit Rated water flow rate
-       TC VS Temp1 Test,           !-Speed 7 Total Cooling Capacity Function of Temperature Curve Name
-       TC VS AirFrac Test,      !-Speed 7 Total Cooling Capacity Function of Air Flow Fraction Curve Name
-       TC VS WaterFrac Test, !-Speed 7 Total Cooling Capacity Function of Water Flow Fraction Curve Name
-       EIR VS Temp1 Test,        !-Speed 7 Energy Input Ratio Function of Temperature Curve Name
-       EIR VS AirFrac Test,    !-Speed 7 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIR VS WaterFrac Test, !-Speed 7 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                    !-Speed 7 Waste Heat fraction to power input
-       wasteHeat VS Temp1 Test, !-Speed 7 Waste Heat Function of Temperature Curve Name
-       5520.7,                                  !-Speed 8 Reference Unit Gross Rated Total Cooling Capacity
-       0.75,                                     !-Speed 8 Reference Unit Gross Sensible Heat Ratio
-       4.0,                                       !-Speed 8 Reference Unit Gross Cooling COP
-       0.3171168,                           !-Speed 8 Reference Unit Rated air flow rate
-       0.000381695,                       !-Speed 8 Reference Unit Rated water flow rate
-       TC VS Temp1 Test,             !-Speed 8 Total Cooling Capacity Function of Temperature Curve Name
-       TC VS AirFrac Test,        !-Speed 8 Total Cooling Capacity Function of Air Flow Fraction Curve Name
-       TC VS WaterFrac Test, !-Speed 8 Total Cooling Capacity Function of Water Flow Fraction Curve Name
-       EIR VS Temp1 Test,        !-Speed 8 Energy Input Ratio Function of Temperature Curve Name
-       EIR VS AirFrac Test,    !-Speed 8 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIR VS WaterFrac Test, !-Speed 8 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                    !-Speed 8 Waste Heat fraction to power input
-       wasteHeat VS Temp1 Test, !-Speed 8 Waste Heat Function of Temperature Curve Name
-       6144.8,                                      !-Speed 9 Reference Unit Gross Rated Total Cooling Capacity
-       0.75,                                       !-Speed 9 Reference Unit Gross Sensible Heat Ratio
-       4.0,                                         !-Speed 9 Reference Unit Gross Cooling COP
-       0.3473184,                             !-Speed 9 Reference Unit Rated air flow rate
-       0.000381695,                         !-Speed 9 Reference Unit Rated water flow rate
-       TC VS Temp1 Test,               !-Speed 9 Total Cooling Capacity Function of Temperature Curve Name
-       TC VS AirFrac Test,        !-Speed 9 Total Cooling Capacity Function of Air Flow Fraction Curve Name
-       TC VS WaterFrac Test,   !-Speed 9 Total Cooling Capacity Function of Water Flow Fraction Curve Name
-       EIR VS Temp1 Test,          !-Speed 9 Energy Input Ratio Function of Temperature Curve Name
-       EIR VS AirFrac Test,      !-Speed 9 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIR VS WaterFrac Test,   !-Speed 9 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                      !-Speed 9 Waste Heat fraction to power input
-       wasteHeat VS Temp1 Test, !-Speed 9 Waste Heat Function of Temperature Curve Name
-       6758.0,                                    !-Speed 10 Reference Unit Gross Rated Total Cooling Capacity
-       0.75,                                       !-Speed 10 Reference Unit Gross Sensible Heat Ratio
-       4.0,                                         !-Speed 10 Reference Unit Gross Cooling COP
-       0.37752,                                 !-Speed 10 Reference Unit Rated air flow rate
-       0.000381695,                         !-Speed 10 Reference Unit Rated water flow rate
-       TC VS Temp1 Test,               !-Speed 10 Total Cooling Capacity Function of Temperature Curve Name
-       TC VS AirFrac Test,          !-Speed 10 Total Cooling Capacity Function of Air Flow Fraction Curve Name
-       TC VS WaterFrac Test,     !-Speed 10 Total Cooling Capacity Function of Water Flow Fraction Curve Name
-       EIR VS Temp1 Test,            !-Speed 10 Energy Input Ratio Function of Temperature Curve Name
-       EIR VS AirFrac Test,        !-Speed 10 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIR VS WaterFrac Test, !-Speed 10 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                    !-Speed 10 Waste Heat fraction to power input
-       wasteHeat VS Temp1 Test; !-Speed 10 Waste Heat Function of Temperature Curve Name
-```
-
-### Variable Speed Water to Air Heat Pump Cooling Coil Outputs
-
-* HVAC, Average, Cooling Coil Electric Power [W]
-
-* HVAC, Average, Cooling Coil Total Cooling Rate [W]
-
-* HVAC, Average, Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC, Average, Cooling Coil Source Side Heat Transfer Rate [W]
-
-* HVAC, Average, Cooling Coil Part Load Ratio []
-
-* HVAC, Average, Cooling Coil Runtime Fraction []
-
-* HVAC, Average, Cooling Coil Air Mass Flow Rate [kg/s]
-
-* HVAC, Average, Cooling Coil Air Inlet Temperature [C]
-
-* HVAC, Average, Cooling Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC, Average, Cooling Coil Air Outlet Temperature [C]
-
-* HVAC, Average, Cooling Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC, Average, Cooling Coil Source Side Mass Flow Rate [kg/s]
-
-* HVAC, Average, Cooling Coil Source Side Inlet Temperature [C]
-
-* HVAC, Average, Cooling Coil Source Side Outlet Temperature [C]
-
-* HVAC, Average, Cooling Coil Upper Speed Level []
-
-* HVAC, Average, Cooling Coil Neighboring Speed Levels Ratio []
-
-* HVAC, Average, Cooling Coil Recoverable Heat Transfer Rate [W]
-
-* HVAC, Sum, Cooling Coil Electric Energy [J]
-
-* HVAC, Sum, Cooling Coil Total Cooling Energy [J]
-
-* HVAC, Sum, Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC, Sum, Cooling Coil Latent Cooling Energy [J]
-
-* HVAC, Average, Cooling Coil Latent Cooling Rate [W]
-
-* HVAC, Sum, Cooling Coil Source Side Heat Transfer Energy [J]
-
-#### Cooling Coil Electric Power [W]
-
-This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
-
-#### Cooling Coil Total Cooling Rate [W]
-
-The output variable is the average total cooling load provide by the heat pump which includes the sensible and latent load in Watts over the timestep being reported.
-
-#### Cooling Coil Sensible Cooling Rate [W]
-
-The output variable is the average sensible cooling load provide by the heat pump in Watts over the timestep being reported.
-
-#### Cooling Coil Source Side Heat Transfer Rate [W]
-
-The output variable is the average heat rejected to the water at the heat pump condenser in Watts over the timestep being reported.
-
-#### Cooling Coil Part Load Ratio []
-
-This output variable is the ratio of the part-load capacity to the steady state capacity of the VSWatertoAirHP coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the VSWatertoAirHP coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
-
-#### Cooling Coil Runtime Fraction []
-
-This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The duty factor or runtime fraction accounts for efficiency losses due to compressor cycling.
-
-#### Cooling Coil Air Mass Flow Rate [kg/s]
-
-The output variable is the average air mass flow rate going through the heat pump over the timestep being reported.
-
-#### Cooling Coil Air Inlet Temperature [C]
-
-The output variable is the average entering air dry-bulb temperature over the timestep being reported.
-
-#### Cooling Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average entering air dry humidity ratio over the timestep being reported.
-
-#### Cooling Coil Air Outlet Temperature [C]
-
-The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
-
-#### Cooling Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average leaving air dry humidity ratio over the timestep being reported.
-
-#### Cooling Coil Source Side Mass Flow Rate [kg/s]
-
-The output variable is the average water mass flow rate going through the heat pump over the timestep being reported.
-
-#### Cooling Coil Source Side Inlet Temperature [C]
-
-The output variable is the average entering water temperature over the timestep being reported.
-
-#### Cooling Coil Source Side Outlet Temperature [C]
-
-The output variable is the average leaving water temperature over the timestep being reported.
-
-#### Cooling Coil Upper Speed Level []
-
-The output variable is the average upper speed level, for interpolating performances between two neighboring speed levels.
-
-#### Cooling Coil Neighboring Speed Levels Ratio []
-
-The output variable is the average speed ratio, for interpolating performances between two neighboring speed levels.
-
-#### Cooling Coil Recoverable Heat Transfer Rate [W]
-
-This output variable is the average recoverable waste heat rate of the heat pump in Watts over the timestep being reported.
-
-#### Cooling Coil Electric Energy [J]
-
-The output variable is the electric consumption of the heat pump in Joules over the timestep being reported.
-
-#### Cooling Coil Total Cooling Energy [J]
-
-The output variable is the total cooling output of the coil in Joules over the timestep being reported.
-
-#### Cooling Coil Sensible Cooling Energy [J]
-
-The output variable is the total sensible cooling output of the coil in Joules over the timestep being reported
-
-#### Cooling Coil Latent Cooling Energy [J]
-
-#### Cooling Coil Latent Cooling Rate [W]
-
-These output variables are the total latent cooling output of the coil in Joules or Watts over the timestep being reported.
-
-#### Cooling Coil Source Side Heat Transfer Energy [J]
-
-The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported.
-
-### Coil:Heating:WaterToAirHeatPump:ParameterEstimation
-
-The Water to Air heat pump heating coil is a deterministic model that requires parameters to describe the operating conditions of the heat pump   s components. The parameters are generated from the manufacturer catalog data using multi-variable optimization method. However, the parameters required for WatertoAirHP heating coil is similar to WatertoAirHP cooling except (source side outside heat transfer coefficient) parameter is not required for heating. In addition, the heating coil model can be used for 3 type of compressors which are **reciprocating**, **rotary** and **scroll**.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
-
-#### Field: Compressor Type
-
-Type of compressor mode used for the heat pump. Choices available are reciprocating, rotary and scroll compressor. Note that the parameters vary for different compressor.
-
-#### Field: Refrigerant Type
-
-This alpha field contains the type of refrigerant used by the heat pump.
-
-#### Field: Design Source Side Flow Rate
-
-This numeric field defines the water flow rate though the coil in m3/sec
-
-#### Field: Gross Rated Heating Capacity
-
-This numeric field defines the gross heating capacity for the WatertoAirHP heating coil at the rated condition in Watts. The gross heating capacity should Not inlcude the ffect of supply air fan heat.
-
-#### Field: High Pressure Cutoff
-
-This numeric field defines the compressor   s maximum allowable pressure in Pascal (N/m2)
-
-#### Field: Low Pressure Cutoff
-
-This numeric field defines the compressor   s minimum allowable pressure in Pascal (N/m2)
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the heating coil source side inlet node name.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the heating coil source side outlet node name.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the heating coil air inlet node name.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the heating coil air outlet node name.
-
-#### Heating Coil Parameters
-
-Depending on the type of compressor specified, the type of parameters and values also differs. An Excel Spreadsheet is in the final stage of development that is capable of estimating the parameters based on the manufacturer data. The general parameters are listed first followed by specific parameters required by the respective compressor model. Lastly, parameters are listed based on the type of source side fluid used.
-
-#### Field: Load Side Total Heat Transfer Coefficient
-
-This numeric field defines the estimated parameter **load side total heat transfer coefficient** in W/K. This field was previously known as Parameter 1.
-
-#### Field: Superheat Temperature at the Evaporator Outlet
-
-This numeric field defines the estimated parameter **superheat temperature** at the evaporator outlet in ËšC. This field was previously known as Parameter 2.
-
-#### Field: Compressor Power Losses
-
-This numeric field defines the estimated parameter **compressor power losses**, which accounts for the loss of work due to mechanical and electrical losses in the compressor in Watts. This field was previously known as Parameter 3.
-
-#### Field: Compressor Efficiency
-
-This numeric field defines the estimated parameter of the **compressor   s efficiency**. The compressor efficiency is formulated as the equation below:
-
-<div>\[\eta  = \frac{{{{\dot W}_{Theoritical}}}}{{{{\dot W}_{CompInput}} - {{\dot W}_{Loss}}}}\]</div>
-
-This field was previously know as Parameter 4.
-
-#### Field: Compressor Piston Displacement
-
-This numeric field defines the estimated parameter **piston displacement of the compressor** in m3/s. This field was part of what was previously known as Parameter 5. It should be used when the Compressor type is either Reciprocating and Rotary. The field should be left blank when Compressor type is Scroll.
-
-#### Field: Compressor Suction/Discharge Pressure Drop
-
-This numeric field defines the estimated parameter **pressure drop at the compressor suction** and discharge in Pascals (N/m2). This field was part of what was previously known as Parameter 6. It should be used when the Compressor type is either Reciprocating and Rotary. The field should be left blank when Compressor type is Scroll.
-
-#### Field: Compressor Clearance Factor
-
-This numeric field defines the estimated parameter **clearance factor of the compressor**. This parameter is dimensionless. This field was part of what was previously known as Parameter 7. It should only be used when the Compressor type is Reciprocating. The field should be left blank when Compressor type is Scroll or Rotary.
-
-#### Field: Refrigerant Volume Flow Rate
-
-This numeric field defines the **refrigerant volume flow rate** at the beginning of the compression [m3/s]. This field was part of what was previously known as Parameter 6. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
-
-#### Field: Volume Ratio
-
-This numeric field defines the **built-in-volume ratio**. This field was part of what was previously known as Parameter 6. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
-
-#### Field: Leak Rate Coefficient
-
-This numeric field defines the coefficient for the relationship between **pressure ratio and leakage rate**. This field was part of what was previously known as Parameter 7. It should only be used when the Compressor type is Scroll. The field should be left blank when Compressor type is Reciprocating or Rotary.
-
-#### Field: Source Side Heat Transfer Coefficient
-
-This numeric field defines the estimated parameter **source side heat transfer coefficient** in W/K. This field was part of what was previously known as Parameter 8. It should only be used when the Source Side Fluid Name is Water.
-
-#### Field: Source Side Heat Transfer Resistance1
-
-This numeric field defines the estimated parameter **source side heat transfer resistance 1**. Unit is dimensionless. This field was part of what was previously known as Parameter 8. It should only be used when the Source Side Fluid Name is an antifreeze.
-
-#### Field: Source Side Heat Transfer Resistance2
-
-This numeric field defines the estimated **parameter source side heat transfer resistance 2**. Unit is W/K. This field was previously known as Parameter 9. It should only be used when the Source Side Fluid Name is an antifreeze.
-
-Following is an example input for Coil:WatertoAirHP:ParameterEstimation:Heating
-
-```idf
-   Coil:Heating:WaterToAirHeatPump:ParameterEstimation,
-       Heat Pump HEATING Mode AHU1,   !- Name
-       Scroll,                                   !- Compressor Type
-       R22,                                         !- Refrigerant Type
-       0.0015,                                   !- Design Source Side Flow Rate {m3/s}
-       38000,                                     !- Gross Rated Heating Capacity {W}
-       3000000,                                 !- High Pressure Cutoff
-       0,                                             !- Low Pressure Cutoff {Pa}
-       AHU1 Water to Air Heat Pump Source Side2 Inlet Node,   !- Water Inlet Node Name
-       AHU1 Water to Air Heat Pump Source Side2 Outlet Node,   !- Water Outlet Node Name
-       Cooling Coil Air Outlet Node AHU1,   !- Air Inlet Node Name
-       Heating Coil Air Outlet Node AHU1,   !- Air Outlet Node Name
-       5.79505E+03,                         !- Load Side Total Heat Transfer Coefficient {W/K}
-       1.56696E+00,                         !- Superheat Temperature at the Evaporator Outlet {C}
-       3.91338E+03,                         !- Compressor Power Losses {W}
-       1.26356E+00,                         !- Compressor Efficiency
-       ,                                               !- Compressor Piston Displacement {m3/s}
-       ,                                               !- Compressor Suction/Discharge Pressure Drop {Pa}
-       ,                                               !- Compressor Clearance Factor {dimensionless}
-       6.99573E-03,                         !- Refrigerant Volume Flow Rate {m3/s}
-       4.96167E+00,                         !- Volume Ratio {dimensionless}
-       2.07750E-06,                         !-Leak Rate Coefficient {dimensionless}
-       4.00322E+03,                         !- Source Side Heat Transfer Coefficient {W/K}
-       ,                                               !- Source Side Heat Transfer Resistance1 {dimensionless}
-       ;                                               !- Source Side Heat Transfer Resistance2 {W/K}
-```
-
-### Coil:Heating:WaterToAirHeatPump:EquationFit
-
-The Water to Air Heating Equation Fit Coil is a simple curve-fit model that requires coefficients generated from the heat pump catalog data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. The performance of the heat pump is modeled using curves fitted from the catalog data.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the heating coil source side inlet node name.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the heating coil source side outlet node name.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the heating coil air inlet node name.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the heating coil air outlet node name.
-
-#### Field: Rated Air Flow Rate
-
-This numeric field contains the rated volumetric air flow rate on the load side of the heat pump in m3/s. This field is autosizable.
-
-#### Field: Rated Water Flow Rate
-
-This numeric field contains the rated volumetric water flow rate on the source side of the heat pump in m3/s. This field is autosizable.
-
-#### Field: Gross Rated Heating Capacity
-
-This numeric field contains the gross heating capacity of the heat pump at the rated condition in W. The gross heating capacity should not account for the effect of supply air fan heat. This field is autosizable.
-
-#### Field: Gross Rated Heating COP
-
-This numeric field contains the gross rated heating coefficient of performance of the heat pump. The gross rated COP of the heat pump should not account for the effect of supply air fan heat.
-
-#### Field: Heating Capacity Coefficient 1-5
-
-These numeric fields contain the first to fifth coefficient for the heat pump capacity.
-
-#### Field: Heating Power Consumption Coefficient 1-5
-
-These numeric fields contain the first to fifth coefficient for the heat pump power consumption.
-
-### Water to Air Heat Pump Heating Coil (parameter Estimation and Equation Fit) Outputs
-
-Coil:Heating:WaterToAirHeatPump:ParameterEstimation and Coil:Heating:WaterToAirHeatPump:EquationFit have the same output variables listed as follows;
-
-* HVAC, Average, Heating Coil Electric Power [W]
-
-* HVAC, Average, Heating Coil Heating Rate [W]
-
-* HVAC, Average, Heating Coil Sensible Heating Rate [W]
-
-* HVAC, Average, Heating Coil Source Side Heat Transfer Rate [W]
-
-* HVAC, Average, Heating Coil Part Load Ratio
-
-* HVAC, Average, Heating Coil Runtime Fraction []
-
-* HVAC, Average, Heating Coil Air Mass Flow Rate [kg/s]
-
-* HVAC, Average, Heating Coil Air Inlet Temperature [C]
-
-* HVAC, Average, Heating Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC, Average, Heating Coil Air Outlet Temperature [C]
-
-* HVAC, Average, Heating Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC, Average, Heating Coil Source Side Mass Flow Rate [kg/s]
-
-* HVAC, Average, Heating Coil Source Side Inlet Temperature [C]
-
-* HVAC, Average, Heating Coil Source Side Outlet Temperature [C]
-
-* HVAC, Sum, Heating Coil Electric Energy [J]
-
-* HVAC, Sum, Heating Coil Heating Energy [J]
-
-* HVAC, Sum, Heating Coil Source Side Heat Transfer Energy [J]
-
-#### Heating Coil Electric Power [W]
-
-This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
-
-#### Heating Coil Heating Rate [W]
-
-The output variable is the average total heating capacity provide by the heat pump which includes the sensible and latent capacity in Watts over the timestep being reported.
-
-#### Heating Coil Sensible Heating Rate [W]
-
-The output variable is the average sensible heating capacity provide by the heat pump in Watts over the timestep being reported. For heating mode, the sensible capacity is equal to the total capacity.
-
-#### Heating Coil Source Side Heat Transfer Rate [W]
-
-The output variable is the average heat absorbed at the heat pump evaporator in Watts over the timestep being reported.
-
-#### Heating Coil Part Load Ratio []
-
-This output variable is the ratio of the part-load capacity to the steady state capacity of the WatertoAirHP coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the WatertoAirHP coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
-
-#### Heating Coil Runtime Fraction []
-
-This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The duty factor or part load fraction accounts for efficiency losses due to compressor cycling.
-
-#### Heating Coil Air Mass Flow Rate [kg/s]
-
-The output variable is the average air mass flow rate going through the heat pump over the timestep being reported.
-
-#### Heating Coil Air Inlet Temperature [C]
-
-The output variable is the average entering air dry-bulb temperature over the timestep being reported.
-
-#### Heating Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average entering air dry humidity ratio over the timestep being reported.
-
-#### Heating Coil Air Outlet Temperature [C]
-
-The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
-
-#### Heating Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average leaving air dry humidity ratio over the timestep being reported.
-
-#### Heating Coil Source Side Mass Flow Rate [kg/s]
-
-The output variable is the average water mass flow rate going through the heat pump over the timestep being reported.
-
-#### Heating Coil Source Side Inlet Temperature [C]
-
-The output variable is the average entering water temperature over the timestep being reported.
-
-#### Heating Coil Source Side Outlet Temperature [C]
-
-The output variable is the average leaving water temperature over the timestep being reported.
-
-#### Heating Coil Electric Energy [J]
-
-The output variable is the total electric consumption of the heat pump in Joules over the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Heating, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Heating Energy [J]
-
-The output variable is the total cooling output of the coil in Joules over the timestep being reported. Resource Type = EnergyTransfer, End Use Key = HeatingCoils, Group Key = System (ref. Output:Meter objects).
-
-#### Heating Coil Source Side Heat Transfer Energy [J]
-
-The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported.
-
-### Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit
-
-The Variable-Speed Water-to-Air Heating Equation Fit Coil is a collection of performance curves that represent the heating coil at various speed levels. The performance curves should be generated from the heat pump Reference Unit catalog data. This is an equation-fit model that resembles a black box with no usage of heat transfer equations. The number of speed levels can range from 2 to 10. The heating coil has four node connections, i.e. two air sides and two water sides. The user needs to specify a nominal speed level, at which the rated capacity, rated volumetric air and water flow rates are sized. The rated capacity, rated volumetric flow rates represent the real situation in the air and water loops, and are used to determine the flow rates at various speed levels in the parent objects, e.g. AirLoopHVAC:UnitaryHeatPump:WaterToAir and ZoneHVAC:WaterToAirHeatPump. It shall be mentioned that the performance correction curves, i.e. the temperature and flow fraction correction curves, should be normalized to the capacity and flow rates at each individual speed and at the rated operating conditions, similar to the performance curves used in the DX coils. On the other hand, the performance values at individual speed levels, e.g. capacities, COPs and flow rates, should be given regarding a specific unit from the Reference Unit catalog data. In the following content, the statement started with    Reference Unit    means the actual Reference Unit catalog data. The rated conditions for obtaining the capacities and COPs   are at indoor dry-bulb temperature of 21.1 ËšC (70 ËšF) and the source side entering water temperature of 21.1 ËšC (70 ËšF). Some equations are provided below to help explain the function of the various performance curves and data fields. For a detailed description of the algorithm and how the curves are used in the calculations, please see the Engineering Reference.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the variable speed heating coil. Any reference to this coil by another object (e.g., AirLoopHVAC:UnitaryHeatPump:WaterToAir) will use this name.
-
-#### Field: Water Inlet Node Name
-
-This alpha field contains the heating coil source side inlet node name.
-
-#### Field: Water Outlet Node Name
-
-This alpha field contains the heating coil source side outlet node name.
-
-#### Field: Air Inlet Node Name
-
-This alpha field contains the heating coil load side inlet node name.
-
-#### Field: Air Outlet Node Name
-
-This alpha field contains the heating coil load side outlet node name.
-
-#### Field: Number of Speeds
-
-This numeric field contains the maximum number of speed levels that the module uses. The number of speeds, for which the user input the performance data and curves, has to be equal to or higher than the maximum number. The performance inputs at higher speeds are ignored.
-
-#### Field: Nominal Speed Level
-
-This numeric field defines the nominal speed level, at which the rated capacity, rated air and water volumetric flow rates are correlated.
-
-#### Field: Gross Rated Heating Capacity at Selected Nominal Speed Level
-
-This numeric field contains the gross rated capacity at the nominal speed level.   This field is autosizable. The gross rated heating capacity is used to determine a capacity scaling factor, as compared to the Reference Unit capacity at the nominal speed level.
-
-<div>\[CapacityScaleFactor = \frac{{GrossRatedHeatingCapacity}}{{ReferenceUnitCapacity@NominalSpeedLevel}}\]</div>
-
-And then, this scaling factor is used to determine capacities at rated conditions for other speed levels, as below,
-
-<div>\[\begin{array}{l}GrossRatedCapacity@SpeedLevel\left( x \right) = \\\quad \quad \quad \quad CapacityScaleFactor \times ReferenceUnitCapacity@SpeedLevel(x)\end{array}\]</div>
-
-#### Field: Rated Volumetric Air Flow Rate
-
-This numeric field contains the rated volumetric air flow rate on the load side of the heat pump corresponding to the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the air flow rates in the parent objects.   It is recommended that the ratio of the rated volumetric air flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
-
-<div>\[\begin{array}{l}AirFlowScaleFactor = \\\quad \quad \quad \quad \frac{{RatedVolumetricAirFlowRate}}{{ReferenceUnitVolAirFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}\end{array}\]</div>
-
-And the volumetric air flow rates in the parent objects are calculated as below,
-
-<div>\[\begin{array}{l}LoopVolumetricAirFlowRate@SpeedLevel\left( x \right) = \\\quad \quad \quad \quad AirFlowScaleFactor\\\quad \quad \quad \quad  \times ReferenceUnitVolAirFlowRate@SpeedLevel(x)\\\quad \quad \quad \quad  \times CapacityScaleFactor\end{array}\]</div>
-
-#### Field: Rated Volumetric Water Flow Rate
-
-This numeric field contains the rated volumetric water flow rate on the source side of the heat pump at the nominal speed level. This field is autosizable. The value is used to determine an internal scaling factor, and calculate the water flow rates at other speed levels.   It is recommended that the ratio of the rated volumetric water flow rate to the rated capacity is the same as the unit performance from the Reference Unit data.
-
-<div>\[WaterFlowScaleFactor = \frac{{RatedVolumetricWaterFlowRate}}{{ReferenceUnitVolWaterFlowRate@NominalSpeedLevel \times CapacityScaleFactor}}\]</div>
-
-And the required volumetric water flow rates in the water loop are calculated as below,
-
-<div>\[LoopVolumetricWaterFlowRate@SpeedLevel\left( x \right) = WaterFlowScaleFactor \times ReferenceUnitVolWaterFlowRate@SpeedLevel(x) \times CapacityScaleFactor\]</div>
-
-#### Field: Part Load Fraction Correlation Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve (Ref: Performance Curves) that parameterizes the variation of electrical power input to the unit as a function of the part load ratio (PLR, heating load/steady-state heating capacity for Speed 1), in the case that the unit operates under the lowest speed, i.e. on/off. The product of the rated EIR and EIR modifier curves is divided by the output of this curve to give the    effective    EIR for a given simulation timestep for Speed 1. The part load fraction (PLF) correlation accounts for efficiency losses due to compressor cycling. The part load fraction correlation should be normalized to a value of 1.0 when the part load ratio equals 1.0 (i.e., no efficiency losses when the compressor(s) run continuously for the simulation timestep). For PLR values between 0 and 1 (0 &lt;= PLR &lt; 1), the following rules apply:
-
-PLF &gt;= 0.7 and PLF &gt;= PLR
-
-If PLF &lt; 0.7, the program resets the PLF value to 0.7, and the simulation proceeds. The runtime fraction of the coil is defined as PLR/PLF. If PLF &lt; PLR, the runtime fraction of the coil is limited to 1.0. A typical part load fraction correlation would be:
-
-<div>\[PLF = 0.85 + 0.15 \times PLR\]</div>
-
-If the user wishes to model no efficiency degradation due to compressor cycling, the part load fraction correlation should be defined as follows:
-
-<div>\[PLF = 0.85 + 0.0 \times PLR\]</div>
-
-#### Field Group: Rated Specification, Performance Curves, and Waste Heat Data
-
-The performance for each heating speed must be specified as shown below. They should be directly given from the Reference Unit data. All inputs for Speed 1 are required, followed by the optional inputs for other speeds.
-
-#### Field: Speed &lt;x&gt; Reference Unit Gross Rated Heating Capacity
-
-This numeric field defines the total, full load gross heating capacity in watts of the water-to-air heating coil unit at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0. Capacity should not account for the effect of supply air fan heat.
-
-#### Field: Speed &lt;x&gt; Reference Unit Gross Rated Heating COP
-
-This numeric field defines the coefficient of performance (COP= gross heating capacity in watts divided by electrical power input in watts) of the heating coil unit at rated conditions for Speed &lt;x&gt; operation. The value entered here must be greater than 0. The input power includes   power for the compressor(s) and accessories, but does not include the power consumption of the indoor supply air fan and water pump. The gross COP should not account for the supply air fan.
-
-#### Field: Speed &lt;x&gt; Reference Unit Rated Air Flow Rate
-
-This numeric field defines the volume air flow rate, in m<sup>3</sup>per second, across the heating coil at rated conditions for Speed &lt;x&gt; operation. The value entered here should be directly from the Reference Unit data, corresponding to the given gross rated heating capacity and gross rated heating COP at the speed, as above.
-
-#### Field: Speed &lt;x&gt; Reference Unit Rated Water Flow Rate
-
-This numeric field defines the volume water flow rate, in m<sup>3</sup>per second, flowing at the source side of the heating coil at rated conditions for Speed &lt;x&gt; operation. The value entered here should be directly from the Reference Unit data, corresponding to the given gross rated heating capacity and gross rated heating COP at the speed, as above.
-
-#### Field: Speed &lt;x&gt; Heating Capacity Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the total heating capacity as a function of the indoor dry-bulb and source side entering water temperature, from the Reference Unit. The output of this curve is multiplied by the gross rated heating capacity at the speed to give the gross total heating capacity at specific temperature operating conditions (i.e., at an indoor air dry-bulb temperature or entering water temperature different from the rating point temperature). It should be noted that the curve is normalized to the heating capacity at Speed&lt;x&gt; from the Reference Unit data, and have the value of 1.0 at the rating point.
-
-#### Field: Speed &lt;x&gt; Heating Capacity Function of Air Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the gross total heating capacity as a function of the ratio of actual air flow rate across the heating coil to the design air flow rate (i.e., fraction of full load flow), at Speed &lt;x&gt; from the Reference Unit data. The curve is normalized to have the value of 1.0 when the actual air flow rate equals the design air flow rate at Speed &lt;x&gt;.
-
-#### Field: Speed &lt;x&gt; Heating Capacity Function of Water Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of total heating capacity as a function of the ratio of actual water flow rate across the heating coil to the design water flow rate (i.e., fraction of full load flow), at Speed &lt;x&gt; from the Reference Unit data. The curve is normalized to have the value of 1.0 when the actual water flow rate equals the design air flow rate at Speed &lt;x&gt;.
-
-The actual total heating capacity at Speed &lt;x&gt;, considering variations in temperatures, air and water flow rates is calculated as below:
-
-<div>\[\begin{array}{l}ActualCapacity@SpeedLevel\left( x \right) = CapacityScaleFactor\\\quad \quad \quad \quad \quad  \times ReferenceUnitCapacity@SpeedLevel(x)\\\quad \quad \quad \quad \quad  \times TotCapTempModFac@SpeedLevel(x)\\\quad \quad \quad \quad \quad  \times TotCapAirFlowModFac@SpeedLevel(x)\\\quad \quad \quad \quad \quad  \times TotCapWaterFlowModFac@SpeedLevel(x)\end{array}\]</div>
-
-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Temperature Curve Name
-
-This alpha field defines the name of a bi-quadratic, quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the both the indoor air dry-bulb and entering water temperatures The EIR is the inverse of the COP. The output of this curve is multiplied by the rated EIR (inverse of rated COP at Speed &lt;x&gt; from the Reference Unit data) to give the EIR at specific temperature operating conditions (i.e., at an indoor air dry bulb temperature or entering water temperature different from the rating point temperature). The curve is normalized to have the value of 1.0 at the rating point.
-
-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Air Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the heating coil to the design air flow rate (i.e., fraction of full load flow, at Speed &lt;x&gt; from the Reference Unit data). The EIR is the inverse of the COP. This curve is normalized to a value of 1.0 when the actual air flow rate equals the rated air flow rate.
-
-#### Field: Speed &lt;x&gt; Energy Input Ratio Function of Water Flow Fraction Curve Name
-
-This alpha field defines the name of a quadratic or cubic performance curve for Speed &lt;x&gt; (ref: Performance Curves) that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual water flow rate across the heating coil to the rated water flow rate (i.e., fraction of full load flow, at Speed &lt;x&gt; from the Reference Unit data). This curve is normalized to a value of 1.0 when the actual air flow rate equals the design air flow rate.
-
-The actual EIR at Speed &lt;x&gt;, considering variations in temperatures, air and water flow rates is calculated as below:
-
-<div>\[\begin{array}{l}ActualEIR@SpeedLevel\left( x \right) = \frac{{1.0}}{{ReferenceUnitCOP@SpeedLevel(x)}}\\\quad \quad \quad \quad \quad \quad \quad \quad \quad  \times EIRTempModFac@SpeedLevel(x)\\\quad \quad \quad \quad \quad \quad \quad \quad \quad  \times EIRAirFlowModFac@SpeedLevel(x)\\\quad \quad \quad \quad \quad \quad \quad \quad \quad  \times EIRWaterFlowModFac@SpeedLevel(x)\end{array}\]</div>
-
-And, the actual power consumption is calculated:
-
-<div>\[\begin{array}{l}ActualPower@SpeedLevel\left( x \right) = ActualCapacity@SpeedLevel\left( x \right)\\\quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \quad  \times ActualEIR@SpeedLevel\left( x \right)\end{array}\]</div>
-
-#### Field: Speed &lt;x&gt; Rated Waste Heat Fraction of Power Input
-
-The fraction of heat input to heating that is available as recoverable waste heat at full load and rated conditions for Speed &lt;x&gt; operation. The part of heat is not delivered to the indoor side.
-
-#### Field: Speed &lt;x&gt; Waste Heat Function of Temperature Curve Name
-
-The name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of the waste heat recovery as a function of indoor dry-bulb temperature and the entering water temperature for Speed &lt;x&gt; from the Reference Unit data. The output of this curve is multiplied by the rated recoverable waste heat at specific temperature operating conditions (i.e., at temperatures different from the rating point). The curve is normalized to a value of 1.0 at the rating point.
-
-The actual recoverable waste heat at Speed &lt;x&gt; is calculated as below:
-
-<div>\[\begin{array}{l}ActualWasteHeat@SpeedLevel\left( x \right) = ActualPower@SpeedLevel\left( x \right)\\\quad \quad \quad \quad \quad \quad  \times WasteHeatFrac@SpeedLevel(x)\\\quad \quad \quad \quad \quad \quad  \times WasteHeatTempModFac@SpeedLevel(x)\end{array}\]</div>
-
-An example of this statement in an IDF is:
-
-```idf
-Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit,
-       Sys 1 Heat Pump Heating Mode,                                                        !- Name
-       Sys 1 Water to Air Heat Pump Source Side2 Inlet Node,        !- Water Inlet Node Name
-       Sys 1 Water to Air Heat Pump Source Side2 Outlet Node,      !- Water Outlet Node Name
-       Sys 1 Heating Coil Air Inlet Node,                                              !- Air Inlet Node Name
-       Sys 1 SuppHeating Coil Air Inlet Node,                                      !- Air Outlet Node Name
-       10.0,                                                                                                         !- Number of Speeds
-       10.0,                                                                                                         !- Nominal Speed Level
-       Autosize,                                                                                                !- Rated Heating Capacity {W}
-       Autosize,                                                                                                !- Rated Air Flow Rate {m3/s}
-       Autosize,                                                                                                !- Rated Water Flow Rate {m3/s}
-       VS Energy Part Load Fraction 1,                                                    !- Energy part load fraction curve
-       1838.7,                                                                       !- Speed 1 Reference Unit Gross Rated Heating Capacity
-       5.0,                                                                              !- Speed 1 Reference Unit Gross Rated Heating COP
-       0.1661088,                                                                                !- Speed 1 Reference Unit Rated Air Flow Rate
-       0.000381695,                                                                            !- Speed 1 Reference Unit Rated Water Flow Rate
-       Heating VS Temp1 Test,       !- Speed 1 Heating Capacity Function of Temperature Curve Name
-       Heating VS AirFrac Test,   !- Speed 1 Heating Capacity Function of Air Flow Fraction Curve Name
-       Heating VS WaterFrac Test,!- Speed 1 Heating Capacity Function of Water Flow Fraction Curve Name
-       EIRH VS Temp1 Test,             !- Speed 1 Energy Input Ratio Function of Temperature Curve Name
-       EIRH VS AirFrac Test,         !- Speed 1 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIRH VS WaterFrac Test,     !- Speed 1 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                           !- Speed 1 Waste Heat Fraction to Power Input
-       Heating wasteHeat VS Temp1 Test,     !- Speed 1 Waste Heat Function of Temperature Curve Name
-       2295.5,                                        !- Speed 2 Reference Unit Gross Rated Heating Capacity
-       5.0,                                           !- Speed 2 Reference Unit Gross Rated Heating COP
-       0.179322,                                 !- Speed 2 Reference Unit Rated air flow rate
-       0.000381695,                           !- Speed 2 Reference Unit Rated water flow rate
-       Heating VS Temp1 Test,       !- Speed 2 Heating Capacity Function of Temperature Curve Name
-       Heating VS AirFrac Test,   !- Speed 2 Heating Capacity Function of Air Flow Fraction Curve Name
-       Heating VS WaterFrac Test,!- Speed 2 Heating Capacity Function of Water Flow Fraction Curve Name
-       EIRH VS Temp1 Test,            !- Speed 2 Energy Input Ratio Function of Temperature Curve Name
-       EIRH VS AirFrac Test,       !- Speed 2 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIRH VS WaterFrac Test,     !- Speed 2 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                          !- Speed 2 Waste Heat Fraction to Power Input
-       Heating wasteHeat VS Temp1 Test,   !- Speed 2 Waste Heat Function of Temperature Curve Name
-       2751.3,                                        !- Speed 3 Reference Unit Gross Rated Heating Capacity
-       5.0*,*                                             !- Speed 3 Reference Unit Gross COP
-       0.1925352,                                 !- Speed 3 Reference Unit Rated Air Flow Rate
-       0.000381695,                             !- Speed 3 Reference Unit Rated Water Flow Rate
-       Heating VS Temp1 Test,         !- Speed 3 Heating Capacity Function of Temperature Curve Name
-       Heating VS AirFrac Test,     !- Speed 3 Heating Capacity Function of Air Flow Fraction Curve Name
-       Heating VS WaterFrac Test,!- Speed 3 Heating Capacity Function of Water Flow Fraction Curve Name
-       EIRH VS Temp1 Test,             !- Speed 3 Energy Input Ratio Function of Temperature Curve Name
-       EIRH VS AirFrac Test,         !- Speed 3 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIRH VS WaterFrac Test,     !- Speed 3 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                          !- Speed 3 Waste Heat fraction to power input
-       Heating wasteHeat VS Temp1 Test, !- Speed 3 Waste Heat Function of Temperature Curve Name
-       3659.6,                                          !- Speed 4 Reference Unit Gross Rated Heating Capacity
-       5.0,                                               !- Speed 4 Reference Unit Gross Rated Heating COP
-       0.2189616,                                   !- Speed 4 Reference Unit Rated air flow rate
-       0.000381695,                               !- Speed 4 Reference Unit Rated water flow rate
-       Heating VS Temp1 Test,           !- Speed 4 Heating Capacity Function of Temperature Curve Name
-       Heating VS AirFrac Test,       !- Speed 4 Heating Capacity Function of Air Flow Fraction Curve Name
-       Heating VS WaterFrac Test,!- Speed 4 Heating Capacity Function of Water Flow Fraction Curve Name
-       EIRH VS Temp1 Test,            !- Speed 4 Energy Input Ratio Function of Temperature Curve Name
-       EIRH VS AirFrac Test,       !- Speed 4 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIRH VS WaterFrac Test,     !- Speed 4 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                          !- Speed 4 Waste Heat fraction to power input
-       Heating wasteHeat VS Temp1 Test, !- Speed 4 Waste Heat Function of Temperature Curve Name
-
-
-       4563.7,                                        !- Speed 5 Reference Unit Gross Rated Heating Capacity
-       5.0,                                             !- Speed 5 Reference Unit Gross Rated Heating COP
-       0.245388,                                   !- Speed 5 Reference Unit Rated air flow rate
-       0.000381695,                             !- Speed 5 Reference Unit Rated water flow rate
-       Heating VS Temp1 Test,         !- Speed 5 Heating Capacity Function of Temperature Curve Name
-       Heating VS AirFrac Test,     !- Speed 5 Heating Capacity Function of Air Flow Fraction Curve Name
-       Heating VS WaterFrac Test,!- Speed 5 Heating Capacity Function of Water Flow Fraction Curve Name
-       EIRH VS Temp1 Test,            !- Speed 5 Energy Input Ratio Function of Temperature Curve Name
-       EIRH VS AirFrac Test,       !- Speed 5 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIRH VS WaterFrac Test,     !- Speed 5 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                          !- Speed 5 Waste Heat fraction to power input
-       Heating wasteHeat VS Temp1 Test,   !- Speed 5 Waste Heat Function of Temperature Curve Name
-       5463.3,                                                  !- Speed 6 Reference Unit Gross Rated Heating Capacity
-       5.0,                                                           !- Speed 6 Reference Unit Gross Rated Heating COP
-       0.2718144,                                               !- Speed 6 Reference Unit Rated air flow rate
-       0.000381695,                                           !- Speed 6 Reference Unit Rated water flow rate
-       Heating VS Temp1 Test,                       !- Speed 6 Heating Capacity Function of Temperature Curve Name
-       Heating VS AirFrac Test, !- Speed 6 Heating Capacity Function of Air Flow Fraction Curve Name
-       Heating VS WaterFrac Test,!- Speed 6 Heating Capacity Function of Water Flow Fraction Curve Name
-       EIRH VS Temp1 Test,             !- Speed 6 Energy Input Ratio Function of Temperature Curve Name
-       EIRH VS AirFrac Test,       !- Speed 6 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIRH VS WaterFrac Test,     !- Speed 6 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                          !- Speed 6 Waste Heat fraction to power input
-       Heating wasteHeat VS Temp1 Test, !- Speed 6 Waste Heat Function of Temperature Curve Name
-       6358.4,                                      !- Speed 7 Reference Unit Gross Rated Heating Capacity
-       5.0,                                           !- Speed 7 Reference Unit Gross Rated Heating COP
-       0.2982408,                               !- Speed 7 Reference Unit Rated air flow rate
-       0.000381695,                           !- Speed 7 Reference Unit Rated water flow rate
-       Heating VS Temp1 Test,       !- Speed 7 Heating Capacity Function of Temperature Curve Name
-       Heating VS AirFrac Test,   !- Speed 7 Heating Capacity Function of Air Flow Fraction Curve Name
-       Heating VS WaterFrac Test,!- Speed 7 Heating Capacity Function of Water Flow Fraction Curve Name
-       EIRH VS Temp1 Test,             !- Speed 7 Energy Input Ratio Function of Temperature Curve Name
-       EIRH VS AirFrac Test,         !- Speed 7 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIRH VS WaterFrac Test,     !- Speed 7 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                          !- Speed 7 Waste Heat fraction to power input
-       Heating wasteHeat VS Temp1 Test,!- Speed 7 Waste Heat Function of Temperature Curve Name
-       7248.5,                                      !- Speed 8 Reference Unit Gross Rated Heating Capacity
-       5.0,                                           !- Speed 8 Reference Unit Gross Rated Heating COP
-       0.3246672,                               !- Speed 8 Reference Unit Rated air flow rate
-       0.000381695,                           !- Speed 8 Reference Unit Rated water flow rate
-       Heating VS Temp1 Test,       !- Speed 8 Heating Capacity Function of Temperature Curve Name
-       Heating VS AirFrac Test,   !- Speed 8 Heating Capacity Function of Air Flow Fraction Curve Name
-       Heating VS WaterFrac Test,!- Speed 8 Heating Capacity Function of Water Flow Fraction Curve Name
-       EIRH VS Temp1 Test,            !- Speed 8 Energy Input Ratio Function of Temperature Curve Name
-       EIRH VS AirFrac Test,       !- Speed 8 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIRH VS WaterFrac Test,     !- Speed 8 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                          !- Speed 8 Waste Heat fraction to power input
-       Heating wasteHeat VS Temp1 Test,   !- Speed 8 Waste Heat Function of Temperature Curve Name
-       8133.6,                                      !- Speed 9 Reference Unit Gross Heating Capacity
-       5.0,                                           !- Speed 9 Reference Unit Gross Rated Heating COP
-       0.3510936,                               !- Speed 9 Reference Unit Rated air flow rate
-       0.000381695,                           !- Speed 9 Reference Unit Rated water flow rate
-       Heating VS Temp1 Test,       !- Speed 9 Heating Capacity Function of Temperature Curve Name
-       Heating VS AirFrac Test,   !- Speed 9 Heating Capacity Function of Air Flow Fraction Curve Name
-       Heating VS WaterFrac Test,!- Speed 9 Heating Capacity Function of Water Flow Fraction Curve Name
-       EIRH VS Temp1 Test,            !- Speed 9 Energy Input Ratio Function of Temperature Curve Name
-       EIRH VS AirFrac Test,       !- Speed 9 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIRH VS WaterFrac Test,     !- Speed 9 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                          !- Speed 9 Waste Heat fraction to power input
-       Heating wasteHeat VS Temp1 Test, !- Speed 9 Waste Heat Function of Temperature Curve Name
-
-
-       9013.2,                                !- Speed 10 Reference Unit Gross Rated Heating Capacity
-       5.0,                                     !- Speed 10 Reference Unit Gross Rated Heating COP
-       0.37752,                             !- Speed 10 Reference Unit Rated air flow rate
-       0.000381695,                     !- Speed 10 Reference Unit Rated water flow rate
-       Heating VS Temp1 Test, !- Speed 10 Heating Capacity Function of Temperature Curve Name
-       Heating VS AirFrac Test, !- Speed 10 Heating Capacity Function of Air Flow Fraction Curve Name
-       Heating VS WaterFrac Test,!- Speed 10 Heating Capacity Function of Water Flow Fraction Curve
-       EIRH VS Temp1 Test,      !- Speed 10 Energy Input Ratio Function of Temperature Curve Name
-       EIRH VS AirFrac Test, !- Speed 10 Energy Input Ratio Function of Air Flow Fraction Curve Name
-       EIRH VS WaterFrac Test, !- Speed 10 Energy Input Ratio Function of Water Flow Fraction Curve Name
-       0.1,                                    !- Speed 10 Waste Heat fraction to power input
-       Heating wasteHeat VS Temp1 Test; !- Speed 10 Waste Heat Function of Temperature Curve Name
-```
-
-### Variable Speed Water to Air Heat Pump Heating Coil Outputs
-
-* HVAC, Average, Heating Coil Electric Power [W]
-
-* HVAC, Average, Heating Coil Heating Rate [W]
-
-* HVAC, Average, Heating Coil Sensible Heating Rate [W]
-
-* HVAC, Average, Heating Coil Source Side Heat Transfer Rate [W]
-
-* HVAC, Average, Heating Coil Part Load Ratio
-
-* HVAC, Average, Heating Coil Runtime Fraction []
-
-* HVAC, Average, Heating Coil Air Mass Flow Rate [kg/s]
-
-* HVAC, Average, Heating Coil Air Inlet Temperature [C]
-
-* HVAC, Average, Heating Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC, Average, Heating Coil Air Outlet Temperature [C]
-
-* HVAC, Average, Heating Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-* HVAC, Average, Heating Coil Source Side Mass Flow Rate [kg/s]
-
-* HVAC, Average, Heating Coil Source Side Inlet Temperature [C]
-
-* HVAC, Average, Heating Coil Source Side Outlet Temperature [C]
-
-* HVAC, Average, Heating Coil Upper Speed Level []
-
-* HVAC, Average, Heating Coil Neighboring Speed Levels Ratio []
-
-* HVAC, Average, Heating Coil Recoverable Heat Transfer Rate [W]
-
-* HVAC, Sum, Heating Coil Electric Energy [J]
-
-* HVAC, Sum, Heating Coil Heating Energy [J]
-
-* HVAC, Sum, Heating Coil Source Side Heat Transfer Energy [J]
-
-#### Heating Coil Electric Power [W]
-
-This output variable is the average electric consumption rate of the heat pump in Watts over the timestep being reported.
-
-#### Heating Coil Heating Rate [W]
-
-The output variable is the average total heating capacity provide by the heat pump in Watts over the timestep being reported.
-
-#### Heating Coil Sensible Heating Rate [W]
-
-The output variable is the average sensible heating capacity provide by the heat pump in Watts over the timestep being reported. For heating mode, the sensible capacity is equal to the total capacity.
-
-#### Heating Coil Source Side Heat Transfer Rate [W]
-
-The output variable is the average heat absorbed at the heat pump evaporator in Watts over the timestep being reported.
-
-#### Heating Coil Part Load Ratio []
-
-This output variable is the ratio of the part-load capacity to the steady state capacity of the VSWatertoAirHP coil. For the cycling fan mode, the runtime fraction for the heat pump compressor may be different from the compressor part-load ratio reported here due to the part-load performance of the VSWatertoAirHP coil (delay at start-up to reach steady-state output). In general, runtime fractions are reported by individual components where appropriate.
-
-#### Heating Coil Runtime Fraction []
-
-This output variable is the function of the part load ratio (PLR, part-load capacity/ steady state capacity). The duty factor or part load fraction accounts for efficiency losses due to compressor cycling.
-
-#### Heating Coil Air Mass Flow Rate [kg/s]
-
-The output variable is the average air mass flow rate going through the heat pump over the timestep being reported.
-
-#### Heating Coil Air Inlet Temperature [C]
-
-The output variable is the average entering air dry-bulb temperature over the timestep being reported.
-
-#### Heating Coil Air Inlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average entering air dry humidity ratio over the timestep being reported.
-
-#### Heating Coil Air Outlet Temperature [C]
-
-The output variable is the average leaving air dry-bulb temperature over the timestep being reported.
-
-#### Heating Coil Air Outlet Humidity Ratio [kgWater/kgDryAir]
-
-The output variable is the average leaving air dry humidity ratio over the timestep being reported.
-
-#### Heating Coil Source Side Mass Flow Rate [kg/s]
-
-The output variable is the average water mass flow rate going through the heat pump over the timestep being reported.
-
-#### Heating Coil Source Side Inlet Temperature [C]
-
-The output variable is the average entering water temperature over the timestep being reported.
-
-#### Heating Coil Source Side Outlet Temperature [C]
-
-The output variable is the average leaving water temperature over the timestep being reported.
-
-#### Heating Coil Upper Speed Level []
-
-The output variable is the average upper speed level, for interpolating performances between two neighboring speed levels.
-
-#### Heating Coil Neighboring Speed Levels Ratio []
-
-The output variable is the average speed ratio, for interpolating performances between two neighboring speed levels.
-
-#### Heating Coil Recoverable Heat Transfer Rate [W]
-
-This output variable is the average recoverable waste heat rate of the heat pump in Watts over the timestep being reported.
-
-#### Heating Coil Electric Energy [J]
-
-The output variable is the total electric consumption of the heat pump in Joules over the timestep being reported.
-
-#### Heating Coil Heating Energy [J]
-
-The output variable is the total cooling output of the coil in Joules over the timestep being reported.
-
-#### Heating Coil Source Side Heat Transfer Energy [J]
-
-The output variable is the total source side heat transfer of the coil in Joules over the timestep being reported.
-
-### Coil:Cooling:DX:SingleSpeed:ThermalStorage
-
-This object models a special direct expansion (DX) cooling coil that includes methods of storing thermal energy within the cooling coil package.   This packaged thermal storage cooling coil model includes all of the equipment needed to charge and discharge and the Thermal Energy Storage (TES) tank itself.   This coil object is used with CoilSystem:Cooling:DX object and a constant volume supply fan, but all other subcomponents are contained within the package.
-
-Some types of devices may have a process air cooling section that actually has two coils, one an evaporator and the second some other kind of coil that cools by discharging the TES tank.   There may also be two separate heat engines inside the package with two compressors.   The model wraps these complexities inside of the model which considers just one process air cooling section that combines both types of coils and one heat rejection condenser section that rejects heat from both engines.   The operating modes that are likely to have two heat engines offer dual sets of rating points and performance curves to model the energy and capacity implications separately.
-
-The model offers various modes of operation that can be controlled over time using either a schedule or EMS actuators.   The user can choose which of the five operating modes are present in the device.   Each of the modes has its own separate set of performance characteristics and curves and the model can change abruptly from one mode to the next.   For example when using the schedule control, the TES coil can be put into Charge Only Mode for some number of hours at night, operated in Cooling Only Mode during the mild morning hours, and run in Discharge Only Mode during the hottest part of the day.   Custom control routines can be programmed using EMS to obtain a dynamic, supervisory control algorithm.
-
-- Off Mode.   This mode is always present.   Although the coil will not do any cooling, the state of the TES tank is still modeled since it can continue to exchange heat with the surrounding ambient air.
-
-- Cooling Only Mode.   This mode is where the coil cools air at the evaporator using a model that is very similar to the regular, single speed DX cooling coil.   The same five performance curves are used to describe cooling capacity and electric power use.   The sensible heat ratio is described using two performance curves in the same as is available for 100% outdoor air coils. The TES tank is neither charged or discharged but it continues to exchange heat with the surrounding ambient air.
-
-- Cooling And Charge Mode.   This mode is where the coil both cools air at the evaporator and cools the TES tank at the same time.   The model supports separate performance characteristics when there two separate heat engines, one for evaporator cooling and one for charging the TES tank.
-
-- Cooling and Discharge Mode.   This mode is where the coil cools process air and heat is rejected to both the condenser section and the TES tank at the same time. The model supports separate performance characteristics when there two separate heat engines, one for evaporator cooling and one for TES cooling.
-
-- Charge Only Mode.   This mode is where the coil charges the TES tank but does not provide any cooling at the process air cooling section.
-
-- Discharge Only Mode.   This mode is where the coil cools process air by discharging the TES tank.
-
-This cooling coil can be autosized.   The cooling capacity for the cooling only mode is sized to meet the air system   s final design cooling capacity.   The cooling capacity for the other modes, and the storage capacity, can all be scaled relative to that one capacity using sizing factors that can be input by the user.
-
-#### Field:   Name
-
-A unique name for this TES coil object, assigned by user.
-
-#### Field:   Availability Schedule Name
-
-The name of a schedule that determines whether the TES coil is available for cooling during a given time period.   A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during a given time period.   A value less than or equal to 0 (usually 0 is used) denotes that unit must be in    off    mode.   If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field:   Operating Mode Control Method
-
-This field determines how the TES coil is to be controlled in terms of which operating mode is in effect for a given time period.   There are two choices,    ScheduledModes    or    EMSControlled.      Choosing ScheduledModes indicates that the operating mode is determined by the values in a schedule that is named in the following input field.   Choosing EMSControlled indicates that the operating mode is determined by the state of an EMS actuator called    Coil:Cooling:DX:SingleSpeed:ThermalStorage    with the control type    Operating Mode.   
-
-#### Field:   Operation Mode Control Schedule Name
-
-This field is used (and required) if the operating model control method is set to ScheduledModes in the previous input field.   The control schedule consists of a series of integer values that indicate what mode the TES coil should operate in for a given time period. The values for various operating modes have been programmed to be as follows:
-
-0.        Off Mode
-
-1.        Cooling Only Mode
-
-2.        Cooling And Charge Mode
-
-3.        Cooling And Discharge Mode
-
-4.        Charge Only Mode
-
-5.        Discharge Only Mode
-
-#### Field:   Storage Type
-
-This field is used to determine what type of material is used for thermal storage.   There are two basic types of thermal storage material, fluid or ice.   For fluid tanks, the material can be water or a user-defined fluid such as a glycol and the storage of thermal energy accompanies changes in the temperature of the fluid in the tank.   For ice tanks, the material is water ice and the storage of thermal energy accompanies changes in the fraction of ice.   This input field has three possible choices:   **Water**, **UserDefinedFluidType**, Or **Ice**.   Choose **Water** for a fluid tank TES based on water.   Choose **UserDefinedFluidType** for a fluid tank TES based on custom or glycol type fluid.   Choose **Ice** for ice-based TES tank.
-
-#### Field:   User Defined Fluid Type
-
-This field is used to declare what type of user defined fluid is contained in the TES tank.   This input field is only used (and required) if the previous field is set to    UserDefinedFluidType.    Water, EthyleneGlycol, and PropoleneGlycol have fluid properties built-in to EnergyPlus.   Using a FluidProperties:GlycolConcentration object allows specifying a mixture of water and a glycol and the name of one can be entered here.   For other types of fluids, a complete set of fluid property data is needed, see FluidProperties:Name, FluidProperties:Temperature, etc.
-
-#### Field:   Fluid Storage Volume [m<sup>3</sup>]
-
-This field is used to describe the size of fluid-based TES tank, in m<sup>3</sup>.   The storage volume can be automatically calculated based on the cooling capacity and sizing factor.
-
-#### Field:   Ice Storage Capacity [GJ]
-
-This field is used to describe the size of ice-based TES tank, in GJ.   The storage capacity can be automatically calculated based on the cooling capacity and a sizing factor.
-
-#### Field:   Storage Capacity Sizing Factor [hr]
-
-This field is used if one of the previous two fields is set to autocalculate.   The value entered here is a time duration, in hours.   This time period is used for calculating a storage capacity.   The basic idea is that storage be sized such that the TES can provide cooling at rated capacity for this amount of time.   The rated capacity used in the sizing calculation is the Discharge Only Mode Rated Storage Discharging Capacity unless the Discharge Only mode is not available in which case it is the Cooling Only Mode Rated Total Evaporator Cooling Capacity.   This sizing factor approach allows scaling the storage size relative to the TES coil   s capacity.   The sizing factor is applied for an ice-based TES by simply multiplying the rated capacity by the time duration (converted to seconds).   For fluid-based TES, a change in fluid temperature of 10 &deg;C is assumed to calculate the tank volume.
-
-#### Field:   Storage Tank Ambient Temperature Node Name
-
-This field is used to assign the environmental conditions surrounding the TES coil.   The thermal storage tank exchanges heat with its surroundings and the boundary conditions for those surrounding are taken from this node named in this field. Typically this is the name of a node declared to be an outdoor air node.   This field is required.
-
-#### Field:   Storage Tank to Ambient U-value Times Area Heat Transfer Coefficient [W/K]
-
-This field is used to characterize the rate at which heat is exchanged between the TES tank and the surrounding ambient conditions, in W/K.   This is an overall    UA    value for the tank where the U-factor and surface area are combined into one coefficient.   Heat loss or gain to the TES tank is modeled using <span>\(\dot Q = {\left( {UA} \right)_{Tank}}\left( {{T_{TES}} - {T_{Amb}}} \right)\)</span>. This field is required.
-
-#### Field:   Fluid Storage Tank Rating Temperature [C]
-
-This field is used to define what temperature is used for rating conditions when using a fluid storage tank.   This field is only used for Storage Type of Water or UserDefinedFluidType.   The temperature here is used for declaring the state of the TES fluid tank that corresponds to    Rated    conditions.   The temperature entered here is used to define fluid properties and to characterize the performance curves that depend on the state of the TES.
-
-#### Field:   Rated Evaporator Air Flow Rate [m<sup>3</sup>/s]
-
-This field is the air volume flow rate through the coil, in m<sup>3</sup>/s, at rating conditions.   This is the rated air flow rate through the evaporator (and any other air cooling devices that are in series with the main evaporator).   The coil can be operated with a different flow rate than this rated flow rate and the performance of the unit scales accordingly using the curves that are of the type    Function of Flow Fraction Curve.      All of the other    rated    values for capacity, COP, and SHR values, for all the various modes, should be determined at the same air flow rate used here.   This field can be autosized.
-
-#### Field:   Evaporator Air Inlet Node Name
-
-This field is the name of an HVAC system node that the coil draws in as its inlet air.   This for the evaporator   s connection to air system but it may include other air cooling devices that are in series with the evaporator and contained within the packaged TES coil. This node must be unique across the model. This field is required.
-
-#### Field:   Evaporator Air Outlet Node Name
-
-This field is the name of an HVAC system node that the coils sends its outlet air.   This for the evaporator   s connection to air system but it may include other air cooling devices that are in series with the evaporator and contained within the packaged TES coil.   This node must be unique across the model. This field is required.
-
-#### Field:   Cooling Only Mode Available
-
-This field is used to indicate if the packaged TES coil includes a mode with only cooling and no equipment is interacting with TES tank to charge or discharge it.   The choices are    Yes    or    No.    This field is required.
-
-#### Field:   Cooling Only Mode Rated Total Evaporator Cooling Capacity [W]
-
-This field is used to specify the total, full load cooling capacity (sensible plus latent), in Watts, of the TES coil at rated conditions, while operating in Cooling Only Mode.   The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb and air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, and the air flow rate specified in Rated Evaporator Air Flow Rate.   Capacity should be    gross    (i.e. supply air fan heat is NOT included).   This total cooling capacity is a central value for TES coil in the sense that it is the basis for various autocalculated sizes for the rest of the model which can be scaled off of this one value. This field is required if Cooling Only Mode is available or if another operating mode   s capacity, or storage capacity, will be autocalculated from this value.   This field is autosizable.
-
-#### Field:   Cooling Only Mode Rated Sensible Heat Ratio
-
-This field is used to specify the sensible heat ratio (SHR) at rating conditions while operating in Cooling Only Mode.   SHR is the sensible cooling capacity divided by the total (sensible plus latent) cooling capacity and is dimensionless.   The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, and cooling coil air flow rate specified in Rated Evaporator Air Flow Rate.   Both the sensible and total cooling capacities used to define the rated SHR should be gross and not include supply fan heat.   The packaged TES coil model uses SHR curves to modify the rated SHR as conditions move away from the rating conditions. This field is only used if Cooling Only Mode is available. If this input is left blank, the default is 0.7.
-
-#### Field:   Cooling Only Mode Rated COP
-
-This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Cooling Only Mode.   COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, and cooling coil air flow rate specified in Rated Evaporator Air Flow Rate.   The electric input power includes power for the compressor(s), condenser fan(s), and internal controls but does not include the electric power for the supply fan (which is modeled separately in EnergyPlus).   The total cooling power output is the same as the value for the Cooling Only Mode Rated Total Evaporator Cooling Capacity and is gross cooling without the fan heat.   This field is only used if Cooling Only Mode is available. If this input is left blank, the default is 3.0.
-
-#### Field:   Cooling Only Mode Total Evaporator Cooling Capacity Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the condenser section.   The performance curve can be any curve or table based on two independent variables, x and y, including:   Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness). The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C and y= 35.0 &deg;C. The result of the curve is multiplied by Cooling Only Mode Rated Total Evaporator Cooling Capacity to model capacity at temperatures away from the rating point.   This field is required if Cooling Only Mode is available.
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-#### Field:   Cooling Only Mode Total Evaporator Cooling Capacity Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to model capacity at air flow rates away from the rating point.   This field is required if Cooling Only Mode is available.
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-#### Field:   Cooling Only Mode Energy Input Ratio Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the condenser section.   The performance curve can be any curve or table based on two independent variables, x and y, including:   Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C and y= 35.0 &deg;C. The result of this curve is multiplied by the inverse of the Cooling Only Mode Rated COP to model electric energy consumption at temperatures away from the rating point.   This field is required if Cooling Only Mode is available.
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-#### Field:   Cooling Only Mode Energy Input Ratio Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Cooling Only Mode Rated COP to model electric energy consumption at air flow rates away from the rating point.   This field is required if Cooling Only Mode is available.
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-#### Field:   Cooling Only Mode Part Load Fraction Correlation Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) as a function of the part load ratio (PLR).   PLR is the ratio of current cooling load to the current cooling capacity.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is the part load fraction (PLF) and the runtime fraction of the coil is defined as PLR divided by PLF.   The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling.   This field is required if Cooling Only Mode is available.
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-#### Field:   Cooling Only Mode Sensible Heat Ratio Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the evaporator section. The performance curve can be any curve or table based on two independent variables, x and y, including:   Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the evaporator section.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C and y= 26.7 &deg;C.   The result of the curve is multiplied by the Cooling Only Mode Rated Sensible Heat Ratio to model the SHR at coil entering temperatures that differ from the rating point.   This field is required if Cooling Only Mode is available.
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-#### Field:   Cooling Only Mode Sensible Heat Ratio Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0.   The result of the curve is multiplied by the Cooling Only Mode Rated Sensible Heat Ratio to model the SHR at coil air flow rates that differ from the rating point. This field is required if Cooling Only Mode is available.
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-#### Field:   Cooling And Charge Mode Available
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-This field is used to indicate if the packaged TES coil includes a mode with both cooling at the coil and charging of the TES tank at the same time. The choices are    Yes    or    No.      This field is required.
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-#### Field:   Cooling And Charge Mode Rated Total Evaporator Cooling Capacity [W]
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-This field is used to specify the total, full load cooling capacity (sensible plus latent), in Watts, of the TES coil at rated conditions, while operating in Cooling And Charge Mode.   The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb and air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, the air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   Capacity should be    gross    (i.e. supply air fan heat is NOT included).   The Cooling and Charge Mode has two capacities, this first one is for    cooling    and would typically be for a heat engine operating between the condenser and the evaporator.   This field is required if Cooling And Charge Mode is available.
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-This field is autocalculatable.   When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
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-#### Field:   Cooling And Charge Mode Capacity Sizing Factor
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-This field is used if the previous input field is set to    autocalculate.      This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Cooling and Charge Mode Rated Total Evaporator Cooling Capacity, in Watts. If this field is left blank the default values is 0.5.
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-#### Field:   Cooling And Charge Mode Rated Storage Charging Capacity [W]
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-This field is used to specify the total, full load charging capacity, in Watts, of the TES coil at rated conditions, while operating in Cooling And Charge Mode.   The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb and air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, the air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   Capacity should be    net    (i.e. any ancillary equipment inside the package needed for charging is included).   The Cooling and Charge Mode has two capacities, this second one is for    charging    and would typically be for a heat engine operating between the condenser and the TES tank.   This field is required if Cooling And Charge Mode is available.
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-This field is autocalculatable.   When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
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-#### Field:   Cooling And Charge Mode Storage Capacity Sizing Factor
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-This field is used if the previous input field is set to    autocalculate.      This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Cooling and Charge Mode Rated Storage Charging Capacity, in Watts. If this field is left blank the default values is 0.5.
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-#### Field:   Cooling And Charge Mode Rated Sensible Heat Ratio
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-This field is used to specify the sensible heat ratio (SHR) at rating conditions while operating in Cooling And Charge Mode.   SHR is the sensible cooling capacity divided by the total (sensible plus latent) cooling capacity and is dimensionless.   The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, and cooling coil air flow rate specified in Rated Evaporator Air Flow Rate.   Both the sensible and total cooling capacities used to define the rated SHR should be gross and not include supply fan heat.   The packaged TES coil model uses SHR curves to modify the rated SHR as conditions move away from the rating conditions.   This field is only used if Cooling And Charge Mode is available. If this input is left blank, the default is 0.7.
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-#### Field:   Cooling And Charge Mode Cooling Rated COP
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-This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Cooling And Charge Mode to cool air at the evaporator.   COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   The electric input power includes power for the compressor(s), condenser fan(s), and internal controls but does not include the electric power for the supply fan (which is modeled separately in EnergyPlus).   The total cooling power output is the same as the value for the Cooling And Charge Mode Rated Total Evaporator Cooling Capacity and is gross cooling without the fan heat.   The Cooling And Charge Mode has two COP values and this first COP is for    cooling    and would typically be for a heat engine operating between the condenser and the evaporator.   This field is only used if Cooling And Charge Mode is available. If this input is left blank, the default is 3.0.
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-#### Field:   Cooling And Charge Mode Charging Rated COP
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-This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Cooling And Charge Mode to charge the TES.   COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   The electric input power includes power for the compressor(s), condenser fan(s), and internal controls.   The charging power output is the same as the value for the Cooling And Charge Mode Rated Storage Charging Capacity and is net charging including any internal equipment.   The Cooling And Charge Mode has two COP values and this second COP is for    charging    and would typically be for a heat engine operating between the condenser and the TES tank.   This field is only used if Cooling And Charge Mode is available. If this input is left blank, the default is 3.0.
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-#### Field:   Cooling And Charge Mode Total Evaporator Cooling Capacity Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.   The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y=35.0 &deg;C, and z=0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by Cooling And Charge Mode Rated Total Evaporator Cooling Capacity to model capacity at temperatures away from the rating point.   This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Total Evaporator Cooling Capacity Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0.   The result of the curve is multiplied by the Cooling And Charge Mode Rated Total Evaporator Cooling Capacity to model capacity at air flow rates away from the rating point.   This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Evaporator Energy Input Ratio Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for evaporator cooling as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y=35.0 &deg;C, and z=0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType.   The performance curve is normalized to have the value of 1.0 at the rating point. The result of this curve is multiplied by the inverse of the Cooling And Charge Mode Cooling Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Evaporator Energy Input Ratio Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for evaporator cooling as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0.   The result of the curve is multiplied by the inverse of the Cooling And Charge Mode Cooling Rated COP to model electric energy consumption at air flow rates away from the rating point.   This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Evaporator Part Load Fraction Correlation Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) (for evaporator cooling) as a function of the part load ratio (PLR).   PLR is the ratio of current cooling load to the current cooling capacity.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0.   The result of the curve is the part load fraction (PLF) and the runtime fraction of the coil is defined as PLR divided by PLF.   The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling.   This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Storage Charge Capacity Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the storage charging capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.   The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y=35.0 &deg;C, and z=0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType.   The result of the curve is multiplied by Cooling And Charge Mode Rated Storage Charging Capacity to model capacity at temperatures away from the rating point.   This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Storage Charge Capacity Function of Total Evaporator PLR Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the storage charging capacity as a function of part load ratio (PLR) at the evaporator.   PLR is the ratio of current evaporator cooling load to the current evaporator cooling capacity.   This curve allows increasing the storage charging capacity when loads at the evaporator are low.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0.   The result of the curve is multiplied by Cooling And Charge Mode Rated Storage Charging Capacity to model capacity at evaporator PLR less than 1.0.   This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Storage Energy Input Ratio Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for charging as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y = 35.0 &deg;C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of this curve is multiplied by the inverse of the Cooling And Charge Mode Charging Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Storage Energy Input Ratio Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for charging as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Cooling And Charge Mode Charging Rated COP to model electric energy consumption at air flow rates away from the rating point.   This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Storage Energy Part Load Fraction Correlation Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) (for storage charging) as a function of the part load ratio (PLR).   PLR is the ratio of current cooling load to the current cooling capacity (at the evaporator).   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0.   The result of the curve is the part load fraction (PLF) and the runtime fraction is defined as PLR divided by PLF.   The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling.   This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Sensible Heat Ratio Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of temperature and optionally state of TES tank.   The user can enter the name of a curve or table object that has either two or three independent variables.
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-For a curve or table with two independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the evaporator section. The performance curve can be any curve or table based on two independent variables, x and y, including:   Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the evaporator section.
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-For a curve or table with three independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the evaporator section and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    and    y    values for the curve are the same as for two independent variables while the    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.
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-The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y = 26.7 &deg;C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType.   The result of the curve is multiplied by the Cooling And Charge Mode Rated Sensible Heat Ratio to model the SHR at coil entering temperatures that differ from the rating point.   This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Charge Mode Sensible Heat Ratio Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling And Charge Mode Rated Sensible Heat Ratio to model the SHR at coil air flow rates that differ from the rating point. This field is required if Cooling And Charge Mode is available.
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-#### Field:   Cooling And Discharge Mode Available
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-This field is used to indicate if the packaged TES coil includes a mode with both cooling at the coil and discharging of the TES tank at the same time. The choices are    Yes    or    No.      This field is required.
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-#### Field:   Cooling And Discharge Mode Rated Total Evaporator Cooling Capacity [W]
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-This field is used to specify the total, full load cooling capacity (sensible plus latent), in Watts, of the TES evaporator coil at rated conditions, while operating in Cooling And Discharge Mode.   The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb and air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, the air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   Capacity should be    gross    (i.e. supply air fan heat is NOT included).   The Cooling and Discharge Mode has two capacities (and may have two separate cooling coils contained within), this first one is for    Evaporator cooling    and would typically be for a heat engine operating between the condenser and the evaporator.   This field is required if Cooling And Discharge Mode is available.
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-This field is autocalculatable.   When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
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-#### Field:   Cooling And Discharge Mode Evaporator Capacity Sizing Factor
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-This field is used if the previous input field is set to    autocalculate.      This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Cooling and Discharge Mode Rated Total Evaporator Cooling Capacity, in Watts. If this field is left blank the default values is 1.0.
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-#### Field:   Cooling And Discharge Mode Rated Storage Discharging Capacity
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-This field is used to specify the total, full load discharging capacity, in Watts, of the TES coil at rated conditions, while operating in Cooling And Discharge Mode.   The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb and air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, the air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   Capacity should be    net    (i.e. any ancillary equipment inside the package needed for discharging is included).   The Cooling and Discharge Mode has two capacities, this second one is for    discharging    and would typically be for a heat transfer loop operating between the TES tank and a coil in series with the evaporator.   This field is required if Cooling And Discharge Mode is available.
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-This field is autocalculatable.   When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
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-#### Field:   Cooling And Discharge Mode Storage Discharge Capacity Sizing Factor
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-This field is used if the previous input field is set to    autocalculate.      This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Cooling and Discharge Mode Rated Storage Discharging Capacity, in Watts. If this field is left blank the default value is 1.0.
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-#### Field:   Cooling And Discharge Mode Rated Sensible Heat Ratio
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-This field is used to specify the sensible heat ratio (SHR) at rating conditions while operating in Cooling And Discharge Mode.   SHR is the sensible cooling capacity divided by the total (sensible plus latent) cooling capacity and is dimensionless.   The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   Both the sensible and total cooling capacities used to define the rated SHR should be gross and not include supply fan heat.   The packaged TES coil model uses SHR curves to modify the rated SHR as conditions move away from the rating conditions.   Cooling and discharge mode may have two separate coils in series all contained within the package and this SHR should be for the combined performance of the entire package. This field is only used if Cooling And Discharge Mode is available. If this input is left blank, the default is 0.7.
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-#### Field:   Cooling And Discharge Mode Cooling Rated COP
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-This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Cooling And Discharge Mode to cool air at the evaporator.   COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   The electric input power includes power for the compressor(s), condenser fan(s), and internal controls but does not include the electric power for the supply fan (which is modeled separately in EnergyPlus).   The total cooling power output is the same as the value for the Cooling And Discharge Mode Rated Total Evaporator Cooling Capacity and is gross cooling without the fan heat.   The Cooling And Discharge Mode has two COP values and this first COP is for    evaporator cooling    and would typically be for a heat engine operating between the condenser and the evaporator.   This field is only used if Cooling And Discharge Mode is available. If this input is left blank, the default is 3.0.
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-#### Field:   Cooling And Discharge Mode Discharging Rated COP
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-This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Cooling And Discharge Mode to discharge the TES.   COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   The electric input power includes power for the compressor or circulation pumps and internal controls.   The discharging power output is the same as the value for the Cooling And Discharge Mode Rated Storage Discharging Capacity and is net discharging including any internal equipment.   The Cooling And Discharge Mode has two COP values and this second COP is for    discharging    and would typically be for a heat transfer loop operating between the TES tank and a coil in series with the evaporator.   This field is only used if Cooling And Discharge Mode is available. If this input is left blank, the default is 3.0.
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-#### Field:   Cooling And Discharge Mode Total Evaporator Cooling Capacity Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.   The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y = 35.0 &deg;C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by Cooling And Discharge Mode Rated Total Evaporator Cooling Capacity to model capacity at temperatures away from the rating point.   This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Total Evaporator Cooling Capacity Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the total cooling capacity as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling And Discharge Mode Rated Total Evaporator Cooling Capacity to model capacity at air flow rates away from the rating point.   This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Evaporator Energy Input Ratio Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for evaporator cooling as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y = 35.0 &deg;C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of this curve is multiplied by the inverse of the Cooling And Discharge Mode Cooling Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Evaporator Energy Input Ratio Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for evaporator cooling as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Cooling And Discharge Mode Cooling Rated COP to model electric energy consumption at air flow rates away from the rating point.   This field is required if Cooling And discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Evaporator Part Load Fraction Correlation Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) (for evaporator cooling) as a function of the part load ratio (PLR).   PLR is the ratio of current cooling load to the current cooling capacity.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is the part load fraction (PLF) and the runtime fraction of the coil is defined as PLR divided by PLF.   The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling.   This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Storage Discharge Capacity Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the storage discharging capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.   The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y = 35.0 &deg;C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by Cooling And Discharge Mode Rated Storage Discharging Capacity to model capacity at temperatures away from the rating point.   This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Storage Discharge Capacity Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the storage discharge capacity as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling And Discharge Mode Rated Storage Discharging Capacity to model capacity at air flow rates away from the rating point.   This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Storage Discharge Capacity Function of Total Evaporator PLR Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the storage discharging capacity as a function of part load ratio (PLR) at the evaporator.   PLR is the ratio of current evaporator cooling load to the current evaporator cooling capacity.   This curve allows varying the storage discharging capacity based on loads at the evaporator.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by Cooling And Discharge Mode Rated Storage Discharging Capacity to model capacity at different evaporator PLR values.   This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Storage Energy Input Ratio Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for discharging as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the condenser section, and (3) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types. The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y = 35.0 &deg;C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of this curve is multiplied by the inverse of the Cooling And Discharge Mode Discharging Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Storage Energy Input Ratio Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for discharging as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Cooling And Discharge Mode Discharging Rated COP to model electric energy consumption at air flow rates away from the rating point.   This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Storage Energy Part Load Fraction Correlation Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) (for storage discharging) as a function of the part load ratio (PLR).   PLR is the ratio of current cooling load to the current cooling capacity (at the evaporator).   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is the part load fraction (PLF) and the runtime fraction is defined as PLR divided by PLF.   The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling.   This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Sensible Heat Ratio Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of temperature and optionally state of TES tank.   The user can enter the name of a curve or table object that has either two or three independent variables.
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-For a curve or table with two independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the evaporator section. The performance curve can be any curve or table based on two independent variables, x and y, including:   Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the evaporator section.
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-For a curve or table with three independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the evaporator section and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    and    y    values for the curve are the same as for two independent variables while the    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.
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-The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y = 26.7 &deg;C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType.   The result of the curve is multiplied by the Cooling And Discharge Mode Rated Sensible Heat Ratio to model the SHR at coil entering temperatures that differ from the rating point.   This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Cooling And Discharge Mode Sensible Heat Ratio Function of Flow Fraction Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling And Discharge Mode Rated Sensible Heat Ratio to model the SHR at coil air flow rates that differ from the rating point. This field is required if Cooling And Discharge Mode is available.
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-#### Field:   Charge Only Mode Available
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-This field is used to indicate if the packaged TES coil includes a mode with only charging of the TES tank. The choices are    Yes    or    No.      This field is required.
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-#### Field:   Charge Only Mode Rated Storage Charging Capacity [W]
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-This field is used to specify the total, full load charging capacity, in Watts, of the TES coil at rated conditions, while operating in Charge Only Mode.   The rating conditions are air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   Capacity should be    net    (i.e. any ancillary equipment inside the package needed for charging is included).   The Charge Only Mode capacity would typically be for a heat engine operating between the condenser and the TES tank.   This field is required if Charge Only Mode is available.
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-This field is autocalculatable.   When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
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-#### Field:   Charge Only Mode Capacity Sizing Factor
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-This field is used if the previous input field is set to    autocalculate.      This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Charge Only Mode Rated Storage Charging Capacity, in Watts. If this field is left blank the default values is 1.0.
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-#### Field:   Charge Only Mode Charging Rated COP
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-This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Charge Only Mode to charge the TES.   COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the outdoor condenser section at 35 &deg;C drybulb and 23.9 &deg;C wetbulb and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   The electric input power includes power for the compressor(s), condenser fan(s), and internal controls.   The charging power output is the same as the value for the Charge Only Mode Rated Storage Charging Capacity and is net charging including any internal equipment.   This field is only used if Charge Only Mode is available. If this input is left blank, the default is 3.0.
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-#### Field:   Charge Only Mode Storage Charge Capacity Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the storage charging capacity as a function of (1) the drybulb temperature of the air entering the condenser section, and (2) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on two independent variables, x and y, including:   Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear.   The    x    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The    y    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.   The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 35.0 &deg;C, and y = 0.5 for Ice storage type or y = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType.   The result of the curve is multiplied by Charge Only Mode Rated Storage Charging Capacity to model capacity at temperatures away from the rating point.   This field is required if Charge Only Mode is available.
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-#### Field:   Charge Only Mode Storage Energy Input Ratio Function of Temperature Curve Name
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-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for charging as a function of (1) the drybulb temperature of the air entering the condenser section, and (2) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on two independent variables, x and y, including:   Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear.   The    x    values for the performance curve are the drybulb temperature of air entering the condenser section (which if using evaporatively-cooled condenser the temperature will be adjusted to approach the wetbulb temperature depending on effectiveness).   The    y    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.   The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 35.0 &deg;C, and y = 0.5 for Ice storage type or y = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of this curve is multiplied by the inverse of the Charge Only Mode Charging Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Charge Only Mode is available.
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-#### Field:   Discharge Only Mode Available
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-This field is used to indicate if the packaged TES coil includes a mode with only discharging of the TES tank. The choices are    Yes    or    No.      This field is required.
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-#### Field:   Discharge Only Mode Rated Storage Discharging Capacity [W]
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-This field is used to specify the total, full load discharging capacity, in Watts, of the TES coil at rated conditions, while operating in Discharge Only Mode.   The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, the air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   Capacity should be    net    (i.e. any ancillary equipment inside the package needed for discharging is included) with regard to TES discharge, and    gross    with regard to supply fan heat.   Discharge Only Mode would typically be for a heat transfer loop operating between the TES tank and a coil in series with the evaporator.   This field is required if Discharge Only Mode is available.
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-This field is autocalculatable.   When autocalculating the capacity, the following sizing factor field is used to scale this capacity relative to the Cooling Only Mode Rated Total Evaporator Cooling Capacity.
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-#### Field:   Discharge Only Mode Capacity Sizing Factor
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-This field is used if the previous input field is set to    autocalculate.      This sizing factor is multiplied by the Cooling Only Mode Rated Total Evaporator Cooling Capacity to obtain a scaled value for Discharge Only Mode Rated Storage Discharging Capacity, in Watts. If this field is left blank the default value is 1.0.
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-#### Field:   Discharge Only Mode Rated Sensible Heat Ratio
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-This field is used to specify the sensible heat ratio (SHR) at rating conditions while operating in Discharge Only Mode.   SHR is the sensible cooling capacity divided by the total (sensible plus latent) cooling capacity and is dimensionless.   The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   Both the sensible and total cooling capacities used to define the rated SHR should be gross and not include supply fan heat.   The packaged TES coil model uses SHR curves to modify the rated SHR as conditions move away from the rating conditions.   This field is only used if Discharge Only Mode is available. If this input is left blank, the default is 0.7.
-
-#### Field:   Discharge Only Mode Rated COP
-
-This field is used to specify the coefficient of performance (COP) at rating conditions while operating in Discharge Only Mode to discharge the TES.   COP is the total cooling power output in watts divided by the electric power input in watts and is dimensionless. The rating conditions are air entering the cooling coil at 26.7 &deg;C drybulb, 19.4 &deg;C wetbulb, cooling coil air flow rate specified in Rated Evaporator Air Flow Rate, and the state of TES at either the Fluid Storage Tank Rating Temperature (for water or fluid storage type) or an ice fraction of 0.5 (for ice storage type).   The electric input power includes power for the compressor or circulation pumps and internal controls.   The discharging power output is the same as the value for the Discharge Only Mode Rated Storage Discharging Capacity and is net discharging including any internal equipment.   This field is only used if Discharge Only Mode is available. If this input is left blank, the default is 3.0.
-
-#### Field:   Discharge Only Mode Storage Discharge Capacity Function of Temperature Curve Name
-
-This field is the name of a separate performance curve object that parameterizes the variation of the storage discharging capacity as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, and (2) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on two independent variables, x and y, including:   Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.   The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C and y = 0.5 for Ice storage type or y = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by Discharge Only Mode Rated Storage Discharging Capacity to model capacity at temperatures away from the rating point.   This field is required if Discharge Only Mode is available.
-
-#### Field:   Discharge Only Mode Storage Discharge Capacity Function of Flow Fraction Curve Name
-
-This field is the name of a separate performance curve object that parameterizes the variation of the storage discharge capacity as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Cooling Discharge Only Mode Rated Storage Discharging Capacity to model capacity at air flow rates away from the rating point.   This field is required if Discharge Only Mode is available.
-
-#### Field:   Discharge Only Mode Energy Input Ratio Function of Temperature Curve Name
-
-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for discharging as a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, and (2) the state of TES tank (in C or fraction).   The performance curve can be any curve or table based on two independent variables, x and y, including:   Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.   The performance curve is normalized to have the value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C and y = 0.5 for Ice storage type or y = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of this curve is multiplied by the inverse of the Discharge Only Mode Rated COP to model electric energy consumption at temperatures away from the rating point. This field is required if Discharge Only Mode is available.
-
-#### Field:   Discharge Only Mode Energy Input Ratio Function of Flow Fraction Curve Name
-
-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) for discharging as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the inverse of the Discharge Only Mode Rated COP to model electric energy consumption at air flow rates away from the rating point.   This field is required if Discharge Only Mode is available.
-
-#### Field:   Discharge Only Mode Part Load Fraction Correlation Curve Name
-
-This field is the name of a separate performance curve object that parameterizes the variation of the energy input ratio (EIR) (for storage discharging) as a function of the part load ratio (PLR).   PLR is the ratio of current cooling load to the current cooling capacity.   The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.   The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is the part load fraction (PLF) and the runtime fraction is defined as PLR divided by PLF.   The runtime fraction is then multiplied by the energy input ratio to model electric energy consumption at part load to account for inefficiencies because of compressor cycling.   This field is required if Discharge Only Mode is available.
-
-#### Field:   Discharge Only Mode Sensible Heat Ratio Function of Temperature Curve Name
-
-This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of temperature and optionally state of TES tank.   The user can enter the name of a curve or table object that has either two or three independent variables.
-
-For a curve or table with two independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil and (2) the drybulb temperature of the air entering the evaporator section. The performance curve can be any curve or table based on two independent variables, x and y, including:   Curve:Biquadratic, Table:TwoIndependentVariables, Curve:Bicubic, and Curve:QuadraticLinear.   The    x    values for the performance curve are the wetbulb temperature of air entering the evaporator section.   The    y    values for the performance curve are the drybulb temperature of air entering the evaporator section.
-
-For a curve or table with three independent variables the SHR is a function of (1) the wetbulb temperature of air entering the evaporator section of the TES coil, (2) the drybulb temperature of the air entering the evaporator section and (3) the state of TES tank (in C or fraction). The performance curve can be any curve or table based on three independent variables, x, y, and z, including:   Curve:Triquadratic and Table:MultiVariableLookup.   The    x    and    y    values for the curve are the same as for two independent variables while the    z    values are the state of the TES tank which are the tank   s temperature for water or fluid storage type or the storage fraction for ice storage types.
-
-The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 19.4 &deg;C, y = 26.7 &deg;C, and z = 0.5 for Ice storage type or z = Fluid Storage Tank Rating Temperature when storage type is Water or UserDefinedFluidType. The result of the curve is multiplied by the Discharge Only Mode Rated Sensible Heat Ratio to model the SHR at coil entering temperatures that differ from the rating point.   This field is required if Discharge Only Mode is available.
-
-#### Field:   Discharge Only Mode Sensible Heat Ratio Function of Flow Fraction Curve Name
-
-This field is the name of a separate performance curve object that parameterizes the variation of the sensible heat ratio (SHR) as a function of the ratio of actual air flow rate across the cooling coil to the value of the Rated Evaporator Air Flow Rate. The performance curve can be any curve or table based on one independent variable, x, including:   Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable. The performance curve is normalized to have a value of 1.0 at the rating point which is defined to be x = 1.0. The result of the curve is multiplied by the Discharge Only Mode Rated Sensible Heat Ratio to model the SHR at coil air flow rates that differ from the rating point. This field is required if Discharge Only Mode is available.
-
-#### Field:   Ancillary Electric Power [W]
-
-This field is the electric power level for miscellaneous ancillary controls and standby draws, in Watts.   This power is not linked to any particular operating mode and will always be    on,    except when the device is scheduled to not be available by the Availability Schedule.   This field is optional.
-
-#### Field:   Cold Weather Operation Minimum Outdoor Air Temperature [C]
-
-This field is the outdoor temperature at which the device operates additional electric components to protect from cold weather, in Degrees Celsius.   When the outdoor temperature is below this value, the power draw specified in the next field will be turned on.   The    outdoor    temperature is obtained from the node specified in the input field called Storage Tank Ambient Temperature Node Name.
-
-#### Field:   Cold Weather Operation Ancillary Power [W]
-
-This field is the electric power level for cold weather protection.   Cold weather protection is in effect whenever the outdoor temperature is lower than the limit set in the previous field, except when the device is scheduled to not be available by the Availability Schedule.
-
-#### Field:   Condenser Air Inlet Node Name
-
-This field is the name of system node that serves as the inlet to the condenser section of the packaged TES coil.   This node is typically specified to be an outdoor air node.   The conditions exposed to the condenser are obtained from this system node.   This field is required.
-
-#### Field:   Condenser Air Outlet Node Name
-
-This field is the name of system node that serves as the outlet to the condenser section of the packaged TES coil.   This node is typically not connected to anything else.   The conditions leaving the condenser are applied to this system node.   This field is required.
-
-#### Field:   Condenser Design Air Flow Rate [m<sup>3</sup>/s]
-
-This field is the rate of air flow through the condenser section, in m<sup>3</sup>/s.   The model assumes constant, single-speed condenser fans.   The flow rate is not used to determine coil operation but is used to determine the conditions leaving the condenser section.   This field is required, for both air-cooled and evaporatively-cooled condenser types.
-
-This field is autocalulatable. When autocalculated, the design flow rate is determined using the sizing factor in the following input field.
-
-#### Field:   Condenser Air Flow Sizing Factor
-
-This field is used if the previous input field is set to    autocalculate.      This sizing factor is multiplied by the Rated Evaporator Air Flow Rate to obtain a scaled value for Condenser Design Air Flow Rate, in m<sup>3</sup>/s. If this field is left blank the default value is 1.0.
-
-#### Field:   Condenser Type
-
-This field is the type of condenser used by the TES coil. There are two options, **AirCooled** or **EvaporativelyCooled**.   The default is AirCooled. The next six put fields are used when the condenser section is evaporatively cooled.
-
-#### Field:   Evaporative Condenser Effectiveness
-
-This field is the wetbulb effectiveness for the evaporatively-cooled condenser. The effectiveness is used to model the temperature of air exposed to the condenser section as follows:
-
-<div>\[{T_{Cond\,\;inlet}} = \left( {{T_{wb,o}}} \right) + \left( {1 - EvapCondEffectiveness} \right)\left( {{T_{db,o}} - {T_{wb,o}}} \right)\]</div>
-
-where
-
-           <span>\({T_{cond\;inlet}}\)</span>= the temperature of air entering the condenser section, in  &deg;C. This value will be used when evaluating performance curves that depend on the drybulb entering the condenser section.
-
-           <span>\({T_{wb,o}}\)</span>= the wetbulb temperature of outdoor air, in  &deg;C
-
-           <span>\({T_{db,o}}\)</span>= the drybulb temperature of outdoor air, in  &deg;C.
-
-This field is required if the condenser type is set to EvaporativelyCooled. If the field is left blank then a default of 0.7 is used.
-
-#### Field:   Evaporative Condenser Pump Rated Power Consumption [W]
-
-This field is the rated power of the evaporative condenser water pump, in Watts.   This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default is zero, but this field is autosizable using a sizing factor of 0.004266 W of electricity per W of cooling. This field is only used when the condenser type is set to EvaporativelyCooled.
-
-#### Field:   Basin Heater Capacity [W/K]
-
-This input field is the capacity of the evaporative cooler water basin heater for freeze protection in Watts per Kelvin. This field is only used when the condenser type is set to EvaporativelyCooled. This field is used with the following field to determine the electricity consumption rate for freeze protection of the water in a basin needed for evaporative cooling. The basin heater electric power is equal to this field multiplied by the difference between the Basin Heater Setpoint Temperature and the outdoor drybulb temperature.   The default is zero.
-
-#### Field:   Basin Heater Setpoint Temperature [C]
-
-This input field contains the setpoint temperature for basin heater operation, in  &deg;C. This field is only used when the condenser type is set to EvaporativelyCooled. The basin heater is active when the outdoor drybulb temperatures falls below this setpoint temperature. The default is 2.0 &deg;C.
-
-#### Field:   Basin Heater Availability Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field is only used when the condenser type is set to EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0.   The basin heater operates whenever the schedule is on and the outdoor air drybulb is lower than the setpoint temperature in the previous field. If the field is left blank, the basin heater is available to operate throughout the simulation.
-
-#### Field:   Supply Water Storage Tank Name
-
-This optional field is used to describe where the TES coil obtains water used for evaporative cooling of its condenser.   If blank or omitted, then the unit will obtain water directly from the mains.   If the name of a Water Storage Tank object is used here, then the unit will attempt to obtain all its water from that tank.   However, if the tank cannot provide all the water the condenser needs, then the unit will still operate and obtains the rest of the water it needs form the mains (referred to as Starved Water).
-
-#### Field:   Condensate Collection Water Storage Tank Name
-
-This optional field is used to describe where condensate from the coil is collected. If blank or omitted, then any coil condensate is discarded.   Enter the name of a Water Storage Tank defined elsewhere and the condensate will be collected in that tank.
-
-#### Field:   Storage Tank Plant Connection Inlet Node Name
-
-This is the name of a system node that is the inlet to the TES tank.   This field is optional and is only used if the TES tank is directly connected to a plant loop.
-
-#### Field:   Storage Tank Plant Connection Outlet Node Name
-
-This is the name of a system node that is the inlet to the TES tank.   This field is optional and is only used if the TES tank is directly connected to a plant loop.
-
-#### Field:   Storage Tank Plant Connection Design Flow Rate
-
-This field is the design flow rate for the plant connection to the TES tank, in m<sup>3</sup>/s.   The TES tank will make a passive request for this amount of flow.   This field is required if the storage tank is connected to plant.
-
-#### Field:   Storage Tank Plant Connection Heat Transfer Effectiveness
-
-This field specifies the heat transfer effectiveness between the plant connection and the TES tank. If the effectiveness is set to 1 then ideal heat transfer occurs, as if the fluids were completely mixed and the fluid leaving the tank is the same temperature as the tank.   If the effectiveness is less than 1.0, then the leaving fluid temperature approaches that of the tank as would be the case with a heat exchanger.   If left blank, the default is 0.7.
-
-#### Field:   Storage Tank Minimum Operating Limit Fluid Temperature [C]
-
-This field is used for fluid-based TES tank (Storage Type of Water or UserDefinedFluidType) to set the a lower limit on the operating temperatures, in Degrees Celsius.   This value represents the temperature of the fluid-based TES tank when fully charged.   This field is optional.   When left blank, the model uses the lowest temperature for which fluid properties are defined.
-
-#### Field:: Storage Tank Maximum Operating Limit Fluid Temperature [C]
-
-This field is used for fluid-based TES tank (Storage Type of Water or UserDefinedFluidType) to set the an upper limit on the operating temperatures, in Degrees Celsius.   This value represents the temperature of the fluid-based TES tank when fully discharged.   This field is optional.   When left blank, the model uses the highest temperature for which fluid properties are defined.
-
-### Coil:Cooling:DX:SingleSpeed:ThermalStorage Outputs
-
-* HVAC,Average,Cooling Coil Operating Mode Index []
-
-* HVAC,Average,Cooling Coil Total Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Total Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Sensible Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Sensible Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Latent Cooling Rate [W]
-
-* HVAC,Sum,Cooling Coil Latent Cooling Energy [J]
-
-* HVAC,Average,Cooling Coil Electric Power [W]
-
-* HVAC,Sum,Cooling Coil Electric Energy [J]
-
-* HVAC,Average,Cooling Coil Runtime Fraction []
-
-* HVAC,Sum,Cooling Coil Cold Weather Protection Electric Energy [J]
-
-* HVAC,Average,Cooling Coil Cold Weather Protection Electric Power [W]
-
-* HVAC,Average,Cooling Coil Thermal Storage Mechanical Heat Transfer Rate [W]
-
-* HVAC,Sum,Cooling Coil Thermal Storage Mechanical Heat Transfer Energy [J]
-
-* HVAC,Average,Cooling Coil Thermal Storage Ambient Heat Transfer Rate [W]
-
-* HVAC,Sum,Cooling Coil Thermal Storage Ambient Heat Transfer Energy [J]
-
-* HVAC,Average,Cooling Coil Ice Thermal Storage End Fraction []
-
-* HVAC,Average,Cooling Coil Condenser Inlet Temperature [C]
-
-* HVAC,Sum,Cooling Coil Evaporative Condenser Water Volume [m3]
-
-* HVAC,Sum,Cooling Coil Evaporative Condenser Mains Supply Water Volume [m3]
-
-* HVAC,Average,Cooling Coil Evaporative Condenser Pump Electric Power [W]
-
-* HVAC,Sum,Cooling Coil Evaporative Condenser Pump Electric Energy [J]
-
-* HVAC,Average,Cooling Coil Basin Heater Electric Power [W]
-
-* HVAC,Sum,Cooling Coil Basin Heater Electric Energy [J]
-
-* HVAC,Average,Cooling Coil Thermal Storage Plant Heat Transfer Rate [W]
-
-* HVAC,Sum,Cooling Coil Thermal Storage Plant Heat Transfer Energy [J]
-
-* HVAC,Average,Cooling Coil Fluid Thermal Storage End Temperature [C]
-
-#### Cooling Coil Operating Mode Index [ ]
-
-This output variable reports the operating mode for the cooling coil.   The numbers in this output are integer codes that correspond to the operating modes as described in the following table.   These codes match the values used for input in schedules and EMS actuators to control operation.
-
-<table class="table table-striped">
-<tr>
-<th>Code</th>
-<th>Operating Mode</th>
-</tr>
-<tr>
-<td>0</td>
-<td>Off</td>
-</tr>
-<tr>
-<td>1</td>
-<td>Cooling Only</td>
-</tr>
-<tr>
-<td>2</td>
-<td>Cooling and Charge</td>
-</tr>
-<tr>
-<td>3</td>
-<td>Cooling and Discharge</td>
-</tr>
-<tr>
-<td>4</td>
-<td>Charge Only</td>
-</tr>
-<tr>
-<td>5</td>
-<td>Discharge Only</td>
-</tr>
-</table>
-
-
-
-#### Cooling Coil Total Cooling Rate [W]
-
-This output is the total (sensible and latent) cooling rate of the coil in Watts.
-
-#### Cooling Coil Total Cooling Energy [J]
-
-This output is the total (sensible and latent) cooling energy transfer by the coil in Joules.   This output is metered as EnergyTransfer for CoolingCoils.
-
-#### Cooling Coil Sensible Cooling Rate [W]
-
-This output is the moist air sensible cooling rate of the coil in Watts.
-
-#### Cooling Coil Sensible Cooling Energy [J]
-
-This output is the moist air sensible cooling energy transfer by the coil in Joules.
-
-#### Cooling Coil Latent Cooling Rate [W]
-
-This output is the latent cooling rate of the coil in Watts.
-
-#### Cooling Coil Latent Cooling Energy [J]
-
-This output is the latent cooling energy transfer by the coil in Joules.
-
-#### Cooling Coil Electric Power [W]
-
-This output is the electricity consumption rate, in Watts, of the compressor(s), pump(s), condenser fan(s) that are inside the package to drive heat transfer for the cooling coil.   This does not include ancillary electrical consumption for such things as cold weather protection, off cycle ancillary power, or supply fans.
-
-#### Cooling Coil Electric Energy [J]
-
-This output is the electricity consumption, in Joules, of the compressor(s), pump(s), condenser fan(s) that are inside the package to drive heat transfer for the cooling coil.   This does not include ancillary electrical consumption for such things as cold weather protection, off cycle ancillary power, or supply fans.
-
-#### Cooling Coil Runtime Fraction []
-
-This output is the runtime fraction of cooling coil.
-
-#### Cooling Coil Cold Weather Protection Electric Power [W]
-
-#### Cooling Coil Cold Weather Protection Electric Energy [J]
-
-These are the power and energy outputs associated with Cold Weather Operation Ancillary Power, in Watts and Joules respectively.
-
-#### Cooling Coil Thermal Storage Mechanical Heat Transfer Rate [W]
-
-#### Cooling Coil Thermal Storage Mechanical Heat Transfer Energy [J]
-
-These are the power and energy outputs for the coil   s heat exchange with the TES tank, in Watts and Joules respectively.   The sign convection is that negative values are cooling the TES tank, or charging it, and positive values are heating the TES tank, or discharging.   This heat transfer is driven by the mechanical systems used inside the package to charge or discharge the TES tank.
-
-#### Cooling Coil Thermal Storage Ambient Heat Transfer Rate [W]
-
-#### Cooling Coil Thermal Storage Ambient Heat Transfer Energy [J]
-
-These are the power and energy outputs for the TES tank   s heat exchange with the surrounding ambient conditions, in Watts and Joules respectively.   The sign convection is that negative values are cooling the TES tank, or charging it, and positive values are heating the TES tank, or discharging.   This heat transfer is driven by the temperature difference between the media in the tank and the surrounding ambient and is governed by the UA factor.
-
-#### Cooling Coil Ice Thermal Storage End Fraction []
-
-This output is the state of the TES tank as fraction of the storage capacity.   Because the tank storage model is dynamic, this value corresponds to the point in time right at the end of the timestep.   This output variable is only available for a storage type of    Ice.   
-
-#### Cooling Coil Fluid Thermal Storage End Temperature [C]
-
-This output is the state of the TES tank as the temperature of the fluid in the tank, in  &deg;C.   Because the tank storage model is dynamic, this value corresponds to the point in time right at the end of the timestep.   This output variable is only available for a storage type of    Water    or    UserDefinedFluidType.   
-
-#### Cooling Coil Condenser Inlet Temperature [C]
-
-This output is the inlet temperature entering the condenser section of an evaporatively cooled condenser, in  &deg;C. This temperature is for the air stream after the evaporative assist and before entering the condenser.   This is the temperature used for condenser entering drybulb conditions when evaluating performance curves for evaporatively cooled condensers. This output is only available for evaporatively cooled condensers.
-
-#### Cooling Coil Evaporative Condenser Water Volume [m<sup>3</sup>]
-
-This output is the amount of water used to evaporatively cool the condenser inlet air, in cubic meters.   This output is only available for evaporatively cooled condensers.
-
-#### Cooling Coil Evaporative Condenser Mains Supply Water Volume [m<sup>3</sup>]
-
-This output is the volume of water drawn from mains water service for the evaporatively cooled condenser. This output is only available for evaporatively cooled condensers.
-
-#### Cooling Coil Evaporative Condenser Pump Electric Power [W]
-
-This output is the average electricity consumption rate of the evaporative condenser water pump, in Watts. This output is only available for evaporatively cooled condensers.
-
-#### Cooling Coil Evaporative Condenser Pump Electric Energy [J]
-
-This output is the electricity consumption of the evaporative condenser water pump, in Joules. This output is only available for evaporatively cooled condensers.
-
-#### Cooling Coil Basin Heater Electric Power [W]
-
-This output is the average electricity consumption rate of the basin heater, in Watts. This output is only available for evaporatively cooled condensers.
-
-#### Cooling Coil Basin Heater Electric Energy [J]
-
-This output is the electricity consumption of the basin heater, in Joules. This output is only available for evaporatively cooled condensers.
-
-#### Cooling Coil Thermal Storage Plant Heat Transfer Rate [W]
-
-#### Cooling Coil Thermal Storage Plant Heat Transfer Energy [J]
-
-These are the power and energy outputs for the TES tank   s heat exchange with the plant loop, in Watts and Joules respectively.   This output is only available if the plant connection to the tank is used.   The sign convection is that negative values are cooling the TES tank, or charging it, and positive values are heating the TES tank, or discharging.   This heat transfer is driven by the temperature difference between the media in the tank and the plant loop fluid and is governed by the effectiveness and plant fluid mass flow rate.
-
-### Secondary Coils of DX System and Heat Pump
-
-Secondary Coils reject to or remove heat from a secondary zone as part of a DX system or an air-to-air heat pump. Secondary coil refers to a condenser of a DX system or a heat pump in cooling operating mode or an evaporator of a heat pump in heating mode. The secondary coil (e.g. condenser) of DX system or heat pumps is commonly installed outdoor but when installed inside a zone either heat is dumped to or extracted from a secondary zone. A secondary zone is a conditioned or unconditioned zone where the secondary coil is installed. Secondary coils are not standalone DX coils but they are add-on features on existing DX coil objects. A secondary DX coil is modeled by specifying additional inputs in one of the following DX coil objects: Coil:Cooling:DX:SingleSpeed, Coil:Heating:DX:SingleSpeed, Coil:Cooling:DX:TwoSpeed, Coil:Cooling:DX:MultiSpeed, and Coil:Heating:DX:MultiSpeed. These additional inputs allow us to model the heat rejected or extracted by the secondary coil while the primary (active) coil is serving another controlled zone as shown in [Figure](#SecondaryCoilsFigure1).  A secondary coil is not controlled directly but responds to the requirements of the primary DX coil. Heat is rejected or extracted depending on the primary DX coil operating modes.  For instance, heat rejected to a secondary zone by a condenser of a DX system or a heat pump is considered as sensible only whereas the energy extracted from a secondary zone may contain sensible and latent components.
-
-![](media/image903.png)
-
-Figure: Schematic of DX System and heat pump in cooling operating mode <a name="SecondaryCoilsFigure1"></a>
-
-Applications of this technology include: inter-zone heat pump in NTED (Dixon, 2010), and PTAC or PTHP serving Offices attached to a Warehouse, where the office partially or fully enclosed by the warehouse and the condenser is inside the Warehouse. Heat rejected or extracted by the secondary DX coil installed in a secondary zone is estimated from the DX coil models and it is considered as internal gains of the secondary zone. The capacity and electric power input of the DX system and heat pumps are determined from the operating modes of the primary cooling or heating DX coils. Calculation of a secondary coil tracks the operating modes of the primary DX coil serving the primary conditioned zone(s). Currently allowed DX coil models are single speed, two speed and multi speed DX Systems and Heat Pumps.  To model secondary DX coils the condenser type should be AirCooled.  There is no need to specify the condenser air inlet node. The model uses zone air node as the secondary coil air inlet node. And the fuel type in multispeed DX coils should Electricity.
-
-**Cooling Operating Mode**: the primary DX cooling coil of a DX system serving a primary zone is active and heat is rejected by the secondary coil (condenser) into a secondary zone. The secondary zone name is specified in DX cooling coil objects.  This operating mode applies to a DX cooling system and cooling operating mode of air-to-air single and multi-speed heat pumps. Heat rejected by a secondary coil (condenser) calculated at each time step becomes internal gain of the secondary zone as shown in [Figure](#SecondaryCoilsFigure2). Whenever a secondary zone name is specified in DX cooling coil objects, the secondary DX coil model calculation is invoked. The only input field required to invoke the secondary DX coil in cooling operating model is to add a zone name in the input field  _Zone Name for Condenser Placement_ in the DX cooling coil object. 
-
-#### Field: Zone Name for Condenser Placement
-
-This input field is name of a conditioned or unconditioned zone where the secondary coil (condenser) of DX system or a heat pump is to be placed.  This is an optional input field specified only when user desires to reject the condenser heat into this zone.  The heat rejected is modeled as sensible internal gain of a secondary zone. 
-
-![](media/image904.png)
-
-Figure: Schematic of DX system and secondary coil in cooling mode <a name="SecondaryCoilsFigure2"></a>
-
-Following is an example input for a single-speed cooling DX coil with secondary DX coil run option.
-
-```idf
-Coil:Cooling:DX:SingleSpeed,
-    Heat Pump ACDXCoil 1,    !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    autosize,                !- Gross Rated Total Cooling Capacity {W}
-    autosize,                !- Gross Rated Sensible Heat Ratio
-    3.0,                     !- Gross Rated Cooling COP {W/W}
-    autosize,                !- Rated Air Flow Rate {m3/s}
-    ,                        !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
-    DX Cooling Coil Air Inlet Node,  !- Air Inlet Node Name
-    Heating Coil Air Inlet Node,  !- Air Outlet Node Name
-    HPACCoolCapFT,           !- Total Cooling Capacity Function of Temperature Curve Name
-    HPACCoolCapFFF,          !- Total Cooling Capacity Function of Flow Fraction Curve Name
-    HPACCOOLEIRFT,           !- Energy Input Ratio Function of Temperature Curve Name
-    HPACCOOLEIRFFF,          !- Energy Input Ratio Function of Flow Fraction Curve Name
-    HPACCOOLPLFFPLR,         !- Part Load Fraction Correlation Curve Name
-    ,                        !- Nominal Time for Condensate Removal to Begin {s}
-    ,   !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
-    ,                        !- Maximum Cycling Rate {cycles/hr}
-    ,                        !- Latent Capacity Time Constant {s}
-    ,                        !- Condenser Air Inlet Node Name
-    AirCooled,               !- Condenser Type
-    ,                        !- Evaporative Condenser Effectiveness {dimensionless}
-    ,                        !- Evaporative Condenser Air Flow Rate {m3/s}
-    ,                        !- Evaporative Condenser Pump Rated Power Consumption {W}
-    ,                        !- Crankcase Heater Capacity {W}
-    ,                 !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
-    ,                        !- Supply Water Storage Tank Name
-    ,                        !- Condensate Collection Water Storage Tank Name
-    200,                     !- Basin Heater Capacity {W/K}
-    ,                        !- Basin Heater Setpoint Temperature
-    ,                        !- Basin Heater Operating Schedule Name
-    ,                        !- Sensible Heat Ratio Function of Temperature Curve Name
-    ,                        !- Sensible Heat Ratio Function of Flow Fraction Curve Name
-    NORTH ZONE;              !- Zone Name for Condenser Placement
-```
-
-Following is an example input for a two-speed cooling DX coil with secondary DX coil run option.
-
-```idf
-Coil:Cooling:DX:TwoSpeed,
-    PSZ-AC_1:1_CoolC DXCoil, !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    AUTOSIZE,                !- High Speed Gross Rated Total Cooling Capacity {W}
-    AUTOSIZE,                !- High Speed Rated Sensible Heat Ratio
-    3.5,                     !- High Speed Gross Rated Cooling COP {W/W}
-    AUTOSIZE,                !- High Speed Rated Air Flow Rate {m3/s}
-    ,                        !- Unit Internal Static Air Pressure {Pa}
-    DX Cooling Coil Air Inlet Node,     !- Air Inlet Node Name
-    Heating Coil Air Inlet Node,        !- Air Outlet Node Name
-    Measured_CoolCStandard10Ton_CapFT,!- Total Cooling Capacity Function of Temperature Curve Name
-    Measured_CoolCStandard10Ton_CapFF,!- Total Cooling Capacity Function of Flow Fraction Curve Name
-    Measured_CoolCStandard10Ton_EIRFT,  !- Energy Input Ratio Function of Temperature Curve Name
-    Measured_CoolCStandard10Ton_EIRFFF, !- Energy Input Ratio Function of Flow Fraction Curve Name
-    No_PLR_Degredation,      !- Part Load Fraction Correlation Curve Name
-    AUTOSIZE,                !- Low Speed Gross Rated Total Cooling Capacity {W}
-    AUTOSIZE,                !- Low Speed Gross Rated Sensible Heat Ratio
-    3.3,                     !- Low Speed Gross Rated Cooling COP {W/W}
-    AUTOSIZE,                !- Low Speed Rated Air Flow Rate {m3/s}
-    MeasuredLowSpeedCoolCapLSFT,!- Low Speed Total Cooling Capacity Function of Temperature Curve Name
-    MeasuredLowSpeedCoolEIRLSFT,!- Low Speed Energy Input Ratio Function of Temperature Curve Name
-    ,                              !- Condenser Air Inlet Node Name
-    AirCooled,               !- Condenser Type
-    ,                        !- High Speed Evaporative Condenser Effectiveness {dimensionless}
-    ,                        !- High Speed Evaporative Condenser Air Flow Rate {m3/s}
-    ,                        !- High Speed Evaporative Condenser Pump Rated Power Consumption {W}
-    ,                        !- Low Speed Evaporative Condenser Effectiveness {dimensionless}
-    ,                        !- Low Speed Evaporative Condenser Air Flow Rate {m3/s}
-    ,                        !- Low Speed Evaporative Condenser Pump Rated Power Consumption {W}
-    ,                        !- Supply Water Storage Tank Name
-    ,                        !- Condensate Collection Water Storage Tank Name
-    ,                        !- Basin Heater Capacity {W/K}
-    ,                        !- Basin Heater Setpoint Temperature {C}
-    ,                        !- Basin Heater Operating Schedule Name
-    ,     !- Sensible Heat Ratio Function of Temperature Curve Name
-    ,     !- Sensible Heat Ratio Function of Flow Fraction Curve Name
-    ,     !- Low Speed Sensible Heat Ratio Function of Temperature Curve Name
-    ,     !- Low Speed Sensible Heat Ratio Function of Flow Fraction Curve Name
-    NORTH ZONE;              !- Zone Name for Condenser Placement
-```
-
-Following is an example input for a multi-speed cooling DX coil with secondary DX coil run option.
-
-```idf
-Coil:Cooling:DX:MultiSpeed,
-    Heat Pump ACDXCoil 1,    !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    DX Cooling Coil Air Inlet Node,  !- Air Inlet Node Name
-    Heating Coil Air Inlet Node,  !- Air Outlet Node Name
-    Outdoor Condenser Air Node,  !- Condenser Air Inlet Node Name
-    AirCooled,               !- Condenser Type
-    ,                        !- Supply Water Storage Tank Name
-    ,                        !- Condensate Collection Water Storage Tank Name
-    No,                      !- Apply Part Load Fraction to Speeds Greater than 1
-    No,                      !- Apply Latent Degradation to Speeds Greater than 1
-    200.0,                   !- Crankcase Heater Capacity {W}
-    10.0,           !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
-    ,                        !- Basin Heater Capacity {W/K}
-    ,                        !- Basin Heater Setpoint Temperature {C}
-    ,                        !- Basin Heater Operating Schedule Name
-    Electricity,             !- Fuel Type
-    4,                       !- Number of Speeds
-    autosize,                !- Speed 1 Gross Rated Total Cooling Capacity {W}
-    autosize,                !- Speed 1 Gross Rated Sensible Heat Ratio
-    3.0,                     !- Speed 1 Gross Rated Cooling COP {W/W}
-    autosize,                !- Speed 1 Rated Air Flow Rate {m3/s}
-    453.3,                   !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
-    HPACCoolCapFT Speed 1,   !- Speed 1 Total Cooling Capacity Function of Temperature Curve Name
-    HPACCoolCapFF Speed 1, !- Speed 1 Total Cooling Capacity Function of Flow Fraction Curve Name
-    HPACCOOLEIRFT Speed 1,   !- Speed 1 Energy Input Ratio Function of Temperature Curve Name
-    HPACCOOLEIRFF Speed 1,   !- Speed 1 Energy Input Ratio Function of Flow Fraction Curve Name
-    HPACCOOLPLFFPLR Speed 1, !- Speed 1 Part Load Fraction Correlation Curve Name
-    1000.0,                  !- Speed 1 Nominal Time for Condensate Removal to Begin {s}
-    1.5,  !- Speed 1 Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
-    3.0,                     !- Speed 1 Maximum Cycling Rate {cycles/hr}
-    45.0,                    !- Speed 1 Latent Capacity Time Constant {s}
-    0.2,                     !- Speed 1 Rated Waste Heat Fraction of Power Input {dimensionless}
-    HAPCCoolWHFT Speed 1,    !- Speed 1 Waste Heat Function of Temperature Curve Name
-    0.9,                     !- Speed 1 Evaporative Condenser Effectiveness {dimensionless}
-    autosize,                !- Speed 1 Evaporative Condenser Air Flow Rate {m3/s}
-    50,                      !- Speed 1 Rated Evaporative Condenser Pump Power Consumption {W}
-    autosize,                !- Speed 2 Gross Rated Total Cooling Capacity {W}
-    autosize,                !- Speed 2 Gross Rated Sensible Heat Ratio
-    3.0,                     !- Speed 2 Gross Rated Cooling COP {W/W}
-    autosize,                !- Speed 2 Rated Air Flow Rate {m3/s}
-    523.3,                   !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
-    HPACCoolCapFT Speed 2,   !- Speed 2 Total Cooling Capacity Function of Temperature Curve Name
-    HPACCoolCapFF Speed 2, !- Speed 2 Total Cooling Capacity Function of Flow Fraction Curve Name
-    HPACCOOLEIRFT Speed 2,   !- Speed 2 Energy Input Ratio Function of Temperature Curve Name
-    HPACCOOLEIRFF Speed 2,   !- Speed 2 Energy Input Ratio Function of Flow Fraction Curve Name
-    HPACCOOLPLFFPLR Speed 1, !- Speed 2 Part Load Fraction Correlation Curve Name
-    1000.0,                  !- Speed 2 Nominal Time for Condensate Removal to Begin {s}
-    1.5,  !- Speed 2 Ratio of Initial Moisture Evaporation Rate and steady state Latent Capacity {dimensionless}
-    3.0,                     !- Speed 2 Maximum Cycling Rate {cycles/hr}
-    45.0,                    !- Speed 2 Latent Capacity Time Constant {s}
-    0.2,                     !- Speed 2 Rated Waste Heat Fraction of Power Input {dimensionless}
-    HAPCCoolWHFT Speed 2,    !- Speed 2 Waste Heat Function of Temperature Curve Name
-    0.9,                     !- Speed 2 Evaporative Condenser Effectiveness {dimensionless}
-    autosize,                !- Speed 2 Evaporative Condenser Air Flow Rate {m3/s}
-    60,                      !- Speed 2 Rated Evaporative Condenser Pump Power Consumption {W}
-    autosize,                !- Speed 3 Gross Rated Total Cooling Capacity {W}
-    autosize,                !- Speed 3 Gross Rated Sensible Heat Ratio
-    3.0,                     !- Speed 3 Gross Rated Cooling COP {W/W}
-    autosize,                !- Speed 3 Rated Air Flow Rate {m3/s}
-    573.3,                   !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
-    HPACCoolCapFT Speed 3,   !- Speed 3 Total Cooling Capacity Function of Temperature Curve Name
-    HPACCoolCapFF Speed 3, !- Speed 3 Total Cooling Capacity Function of Flow Fraction Curve Name
-    HPACCOOLEIRFT Speed 3,   !- Speed 3 Energy Input Ratio Function of Temperature Curve Name
-    HPACCOOLEIRFF Speed 3,   !- Speed 3 Energy Input Ratio Function of Flow Fraction Curve Name
-    HPACCOOLPLFFPLR Speed 1, !- Speed 3 Part Load Fraction Correlation Curve Name
-    1000.0,                  !- Speed 3 Nominal Time for Condensate Removal to Begin {s}
-    1.5, !- Speed 3 Ratio of Initial Moisture Evaporation Rate and steady state Latent Capacity {dimensionless}
-    3.0,                     !- Speed 3 Maximum Cycling Rate {cycles/hr}
-    45.0,                    !- Speed 3 Latent Capacity Time Constant {s}
-    0.2,                     !- Speed 3 Rated Waste Heat Fraction of Power Input {dimensionless}
-    HAPCCoolWHFT Speed 3,    !- Speed 3 Waste Heat Function of Temperature Curve Name
-    0.9,                     !- Speed 3 Evaporative Condenser Effectiveness {dimensionless}
-    autosize,                !- Speed 3 Evaporative Condenser Air Flow Rate {m3/s}
-    80,                      !- Speed 3 Rated Evaporative Condenser Pump Power Consumption {W}
-    autosize,                !- Speed 4 Gross Rated Total Cooling Capacity {W}
-    autosize,                !- Speed 4 Gross Rated Sensible Heat Ratio
-    3.0,                     !- Speed 4 Gross Rated Cooling COP {W/W}
-    autosize,                !- Speed 4 Rated Air Flow Rate {m3/s}
-    673.3,                   !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
-    HPACCoolCapFT Speed 4,   !- Speed 4 Total Cooling Capacity Function of Temperature Curve Name
-    HPACCoolCapFF Speed 4, !- Speed 4 Total Cooling Capacity Function of Flow Fraction Curve Name
-    HPACCOOLEIRFT Speed 4,   !- Speed 4 Energy Input Ratio Function of Temperature Curve Name
-    HPACCOOLEIRFF Speed 4,   !- Speed 4 Energy Input Ratio Function of Flow Fraction Curve Name
-    HPACCOOLPLFFPLR Speed 1, !- Speed 4 Part Load Fraction Correlation Curve Name
-    1000.0,                  !- Speed 4 Nominal Time for Condensate Removal to Begin {s}
-    1.5, !- Speed 4 Ratio of Initial Moisture Evaporation Rate and steady state Latent Capacity {dimensionless}
-    3.0,                     !- Speed 4 Maximum Cycling Rate {cycles/hr}
-    45.0,                    !- Speed 4 Latent Capacity Time Constant {s}
-    0.2,                     !- Speed 4 Rated Waste Heat Fraction of Power Input {dimensionless}
-    HAPCCoolWHFT Speed 4,    !- Speed 4 Waste Heat Function of Temperature Curve Name
-    0.9,                     !- Speed 4 Evaporative Condenser Effectiveness {dimensionless}
-    autosize,                !- Speed 4 Evaporative Condenser Air Flow Rate {m3/s}
-    100,                     !- Speed 4 Rated Evaporative Condenser Pump Power Consumption {W}
-    NORTH ZONE;              !- Zone Name for Condenser Placement
-```
-
-**Heating Operating Mode**: When a heat pump operates in heating mode then energy is extracted from the secondary zone.  Total energy extracted from a secondary zone may contain sensible and latent components.  The secondary coil (evaporator) model checks for the coil inlet and outlet air condition to determine if dehumidification has occurred. The sensible and latent split of the energy extracted is done using a user specified rated sensible heat ratio (SHR) and SHR modifier curves for temperature and secondary air flow fraction.  If the coil operation is dry, then the SHR is set to 1.0.  In addition, the model assumes that condensed water is drained to the outside. If defrosting operation is on, then the defrosting melts the frost and the liquid water from the collecting pan is drained to the outside.  Thus, defrosting energy is not included in the zone energy balance. The six optioal input fields required in the DX heating coils are the following. The last five input fields are extensible depending on the speed of the heating DX coil:
-
-#### Field: Zone Name for Evaporator Placement
-
-This input field is name of a conditioned or unconditioned zone where the secondary coil (evaporator) of a heat pump is installed.  This is an optional input field specified only when user desires to extract heat from the zone via secondary coil. Heat extracted is modeled as internal gain. If the primary DX system is a heat pump, then the zone name should be the same as the zone name specified for placing the secondary cooling DX coil.
-
-#### Field: Speed <x> Secondary Coil Air Flow Rate
-
-This input value is the secondary coil (evaporator) air flow rate when the heat pump is working in heating mode or the secondary coil (condenser) air flow rate when the heat pump is working in cooling mode. This input field is auto-sizable.  
-
-#### Field: Speed <x> Secondary Coil Fan Flow Scaling Factor
-
-This input field is scaling factor for autosizing the secondary DX coil fan flow rate.  The secondary air flow rate is determined by multiplying the primary DX coil rated air flow rate by the fan flow scaling factor.  Default value is 1.25. If the secondary coil fan flow rate is not autosized, then the secondary coil fan flow scaling factor is set to 1.0.
-
-#### Field: Speed <x> Nominal Sensible Heat Ratio of Secondary Coil
-
-This input value is the nominal sensible heat ratio used to split the heat extracted by a secondary DX coil (evaporator) of a heat pump into sensible and latent components.  This is an optional input field.  If this input field is left blank, then pure sensible internal heat gain is assumed, i.e., sensible heat ratio of 1.0. 
-
-#### Field: Speed <x> Sensible Heat Ratio Modifier Function of Temperature Curve Name
-
-This input field is name of sensible heat ratio modifier biquadratic curve.  The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary zone air node wet-bulb temperature and the heating DX coil entering air dry-bulb temperature.  This is an optional input field.  If this input field is left blank, then the nominal sensible heat ratio modifier curve value for temperature is set to 1.0.
-
-#### Field: Speed <x> Sensible Heat Ratio Modifier Function of Flow Fraction Curve Name
-
-This input field is name of sensible heat ratio modifier curve as function of secondary air flow fraction. The value of this curve modifies the nominal sensible heat ratio for current time step depending on the secondary coil air flow fraction. This is an optional input field.  If this input field is left blank, then the sensible heat ratio modifier curve value for flow fraction is set to 1.0.
-
-Following is an example input for a single-speed heating DX coil with secondary DX coil run option.
-
-```idf
-Coil:Heating:DX:SingleSpeed,
-    Heat Pump DX Heating Coil 1,  !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    autosize,                !- Gross Rated Heating Capacity {W}
-    2.75,                    !- Gross Rated Heating COP {W/W}
-    autosize,                !- Rated Air Flow Rate {m3/s}
-    ,                        !- Rated Supply Fan Power Per Volume Flow Rate {W/(m3/s)}
-    Heating Coil Air Inlet Node,  !- Air Inlet Node Name
-    SuppHeating Coil Air Inlet Node,  !- Air Outlet Node Name
-    HPACHeatCapFT,           !- Heating Capacity Function of Temperature Curve Name
-    HPACHeatCapFFF,          !- Heating Capacity Function of Flow Fraction Curve Name
-    HPACHeatEIRFT,           !- Energy Input Ratio Function of Temperature Curve Name
-    HPACHeatEIRFFF,          !- Energy Input Ratio Function of Flow Fraction Curve Name
-    HPACCOOLPLFFPLR,         !- Part Load Fraction Correlation Curve Name
-    ,                        !- Defrost Energy Input Ratio Function of Temperature Curve Name
-   -5.0,                     !- Minimum Outdoor Dry-Bulb Temperature for Compressor Operation {C}
-    ,                        !- Outdoor Dry-Bulb Temperature to Turn On Compressor {C}
-    5.0,                     !- Maximum Outdoor Dry-Bulb Temperature for Defrost Operation {C}
-    200.0,                   !- Crankcase Heater Capacity {W}
-    10.0,             !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
-    Resistive,               !- Defrost Strategy
-    TIMED,                   !- Defrost Control
-    0.166667,                !- Defrost Time Period Fraction
-    autosize,                !- Resistive Defrost Heater Capacity {W}
-    4,                       !- Region number for calculating HSPF
-    ,                        !- Evaporator Air Inlet Node Name
-    NORTH ZONE,              !- Zone Name for Evaporator Placement
-    autosize,                !- Secondary Coil Air Flow Rate
-    1.5,                     !- Secondary Coil Fan Flow Scaling Factor
-    0.9,                     !- Nominal Sensible Heat Ratio of Secondary Coil
-    DXSecondaryCoilSHRFT,    !- Sensible Heat Ratio Modifier Function of Temperature Curve Name
-    DXSecondaryCoilSHRFFF;   !- Sensible Heat Ratio Function of Flow Fraction Curve Name
-```
-
-Following is an example input for a multi-speed heating DX coil with secondary DX coil run option.
-
-```idf
-Coil:Heating:DX:MultiSpeed,
-    Heat Pump DX Heating Coil 1,  !- Name
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-    Heating Coil Air Inlet Node,  !- Air Inlet Node Name
-    SuppHeating Coil Air Inlet Node,  !- Air Outlet Node Name
-    -8.0,                    !- Minimum Outdoor Dry-Bulb Temperature for Compressor Operation {C}
-    -5.0,                    !- Outdoor Dry-Bulb Temperature to Turn On Compressor {C}
-    200.0,                   !- Crankcase Heater Capacity {W}
-    10.0,              !- Maximum Outdoor Dry-Bulb Temperature for Crankcase Heater Operation {C}
-    HPACDefrostCAPFT,        !- Defrost Energy Input Ratio Function of Temperature Curve Name
-    7.22,                    !- Maximum Outdoor Dry-Bulb Temperature for Defrost Operation {C}
-    ReverseCycle,            !- Defrost Strategy
-    timed,                   !- Defrost Control
-    0.058333,                !- Defrost Time Period Fraction
-    autosize,                !- Resistive Defrost Heater Capacity {W}
-    No,                      !- Apply Part Load Fraction to Speeds Greater than 1
-    Electricity,             !- Fuel Type
-    4,                       !- Region number for Calculating HSPF
-    4,                       !- Number of Speeds
-    autosize,                !- Speed 1 Gross Rated Heating Capacity {W}
-    2.75,                    !- Speed 1 Gross Rated Heating COP {W/W}
-    autosize,                !- Speed 1 Rated Air Flow Rate {m3/s}
-    345.0,                   !- Speed 1 Rated Supply Air Fan Power Per Volume Flow Rate {W/(m3/s)}
-    HPACHeatCapFT Speed 1,   !- Speed 1 Heating Capacity Function of Temperature Curve Name
-    HPACHeatCapFF Speed 1,   !- Speed 1 Heating Capacity Function of Flow Fraction Curve Name
-    HPACHeatEIRFT Speed 1,   !- Speed 1 Energy Input Ratio Function of Temperature Curve Name
-    HPACHeatEIRFF Speed 1,   !- Speed 1 Energy Input Ratio Function of Flow Fraction Curve Name
-    HPACHeatPLFFPLR Speed 1, !- Speed 1 Part Load Fraction Correlation Curve Name
-    0.2,                     !- Speed 1 Rated Waste Heat Fraction of Power Input {dimensionless}
-    HAPCHeatWHFT Speed 1,    !- Speed 1 Waste Heat Function of Temperature Curve Name
-    autosize,                !- Speed 2 Gross Rated Heating Capacity {W}
-    2.75,                    !- Speed 2 Gross Rated Heating COP {W/W}
-    autosize,                !- Speed 2 Rated Air Flow Rate {m3/s}
-    425.0,                   !- Speed 2 Rated Supply Air Fan Power Per Volume Flow Rate {W/(m3/s)}
-    HPACHeatCapFT Speed 2,   !- Speed 2 Heating Capacity Function of Temperature Curve Name
-    HPACHeatCapFF Speed 2,   !- Speed 2 Heating Capacity Function of Flow Fraction Curve Name
-    HPACHeatEIRFT Speed 2,   !- Speed 2 Energy Input Ratio Function of Temperature Curve Name
-    HPACHeatEIRFF Speed 2,   !- Speed 2 Energy Input Ratio Function of Flow Fraction Curve Name
-    HPACHeatPLFFPLR Speed 2, !- Speed 2 Part Load Fraction Correlation Curve Name
-    0.2,                     !- Speed 2 Rated Waste Heat Fraction of Power Input {dimensionless}
-    HAPCHeatWHFT Speed 2,    !- Speed 2 Waste Heat Function of Temperature Curve Name
-    autosize,                !- Speed 3 Gross Rated Heating Capacity {W}
-    2.75,                    !- Speed 3 Gross Rated Heating COP {W/W}
-    autosize,                !- Speed 3 Rated Air Flow Rate {m3/s}
-    525.0,                   !- Speed 3 Rated Supply Air Fan Power Per Volume Flow Rate {W/(m3/s)}
-    HPACHeatCapFT Speed 3,   !- Speed 3 Heating Capacity Function of Temperature Curve Name
-    HPACHeatCapFF Speed 3,   !- Speed 3 Heating Capacity Function of Flow Fraction Curve Name
-    HPACHeatEIRFT Speed 3,   !- Speed 3 Energy Input Ratio Function of Temperature Curve Name
-    HPACHeatEIRFF Speed 3,   !- Speed 3 Energy Input Ratio Function of Flow Fraction Curve Name
-    HPACHeatPLFFPLR Speed 3, !- Speed 3 Part Load Fraction Correlation Curve Name
-    0.2,                     !- Speed 3 Rated Waste Heat Fraction of Power Input {dimensionless}
-    HAPCHeatWHFT Speed 3,    !- Speed 3 Waste Heat Function of Temperature Curve Name
-    autosize,                !- Speed 4 Gross Rated Heating Capacity {W}
-    2.75,                    !- Speed 4 Gross Rated Heating COP {W/W}
-    autosize,                !- Speed 4 Rated Air Flow Rate {m3/s}
-    673.0,                   !- Speed 4 Rated Supply Air Fan Power Per Volume Flow Rate {W/(m3/s)}
-    HPACHeatCapFT Speed 4,   !- Speed 4 Heating Capacity Function of Temperature Curve Name
-    HPACHeatCapFF Speed 4,   !- Speed 4 Heating Capacity Function of Flow Fraction Curve Name
-    HPACHeatEIRFT Speed 4,   !- Speed 4 Energy Input Ratio Function of Temperature Curve Name
-    HPACHeatEIRFF Speed 4,   !- Speed 4 Energy Input Ratio Function of Flow Fraction Curve Name
-    HPACHeatPLFFPLR Speed 4, !- Speed 4 Part Load Fraction Correlation Curve Name
-    0.2,                     !- Speed 4 Rated Waste Heat Fraction of Power Input {dimensionless}
-    HAPCHeatWHFT Speed 4,    !- Speed 4 Waste Heat Function of Temperature Curve Name
-    NORTH ZONE,              !- Zone Name for Evaporator Placement
-    autosize,                !- Speed 1 Secondary Coil Air Flow Rate
-    1.5,                     !- Speed 1 Secondary Coil Fan Flow Scaling Factor
-    0.9,                     !- Speed 1 Nominal Sensible Heat Ratio of Secondary Coil
-    DXSecondaryCoilSHRFT,!- Speed 1 Sensible Heat Ratio Modifier Function of Temperature Curve Name
-    DXSecondaryCoilSHRFFF,   !- Speed 1 Sensible Heat Ratio Function of Flow Fraction Curve Name
-    autosize,                !- Speed 2 Secondary Coil Air Flow Rate
-    1.5,                     !- Speed 2 Secondary Coil Fan Flow Scaling Factor
-    0.9,                     !- Speed 2 Nominal Sensible Heat Ratio of Secondary Coil
-    DXSecondaryCoilSHRFT,!- Speed 2 Sensible Heat Ratio Modifier Function of Temperature Curve Name
-    DXSecondaryCoilSHRFFF,   !- Speed 2 Sensible Heat Ratio Function of Flow Fraction Curve Name
-    autosize,                !- Speed 3 Secondary Coil Air Flow Rate
-    1.5,                     !- Speed 3 Secondary Coil Fan Flow Scaling Factor
-    0.9,                     !- Speed 3 Nominal Sensible Heat Ratio of Secondary Coil
-    DXSecondaryCoilSHRFT,!- Speed 3 Sensible Heat Ratio Modifier Function of Temperature Curve Name
-    DXSecondaryCoilSHRFFF,   !- Speed 3 Sensible Heat Ratio Function of Flow Fraction Curve Name
-    autosize,                !- Speed 4 Secondary Coil Air Flow Rate
-    1.5,                     !- Speed 4 Secondary Coil Fan Flow Scaling Factor
-    0.9,                     !- Speed 4 Nominal Sensible Heat Ratio of Secondary Coil
-    DXSecondaryCoilSHRFT,!- Speed 4 Sensible Heat Ratio Modifier Function of Temperature Curve Name
-    DXSecondaryCoilSHRFFF;   !- Speed 4 Sensible Heat Ratio Function of Flow Fraction Curve Name
-```
-
-### Secondary DX Coil Output
-
-* HVAC, Average, Secondary Coil Heat Rejection Rate [W] 
-
-* HVAC, Average, Secondary Coil Total Heat Removal Rate [W]
-
-* HVAC, Average, Secondary Coil Sensible Heat Removal Rate [W]
-
-* HVAC, Average, Secondary Coil Latent Heat Removal Rate [W]
-
-* HVAC, Average, Secondary Coil Sensible Heat Ratio []
-
-* HVAC, Average, Secondary Coil Compressor Part Load Ratio []
-
-
-#### Secondary Coil Heat Rejection Rate [W]
-
-This is the sensible heat rejected to a zone by a secondary DX coil (condenser) in Watts. This is sum of the total cooling rate of a DX cooling coil and cooling electric power of the primary DX coil.  This heat is applied as an internal gain to the secondary zone where the condenser is installed.
-
-#### Secondary Coil Total Heat  Removal Rate [W]
-
-This is the total energy removed from a a zone by a secondary DX coil (evaporator) in Watts. This is the total heating rate of the primary DX cooling coil minus the heating electric power of the primary DX coil.  This heat is extracted from the secondary zone when the heat pump is operating in heating mode. The negative sign indicate that heat is removed from the zone.
-
-#### Secondary Coil Sensible Heat Removal Rate [W]
-
-This is the sensible heat removed from a a zone by a secondary DX coil (evaporator) in Watts. This is determined by multiplying the total heat removed with sensible heat ratio of the secondary coil. This heat is extracted from the secondary zone when the heat pump is operating in heating mode. The negative sign indicate that sensible heat is removed from the zone.
-
-#### Secondary Coil Latent Heat  Removal Rate [W]
-
-This is the latent heat removed from a a zone by a secondary DX coil (evaporator) in Watts. This is the difference between the total heat removal rate and the sensible heat remobal rate of the secondary coil. This heat is extracted from the secondary zone when the heat pump is operating in heating mode. The negative sign indicate that moisture is removed from the zone.
-
-#### Secondary Coil Sensible Heat Ratio []
-
-This is the operating sensible heat ratio the secondary DX coil (condenser) when the heat pump is operating in heating mode. 
-
-#### Secondary Coil Compressor Part Load Ratio []
-
-This is the compressor part load ratio when the heat pump is operating in heating mode and the secondary coil is extracting heat from a zone where the coil is installed. The secondary coil DX coil compressor part load ratio can be different from the primary DX coil compressor part load ratio in that the later may include the defrosting load.
-
-Reference: Dixon, Erin Elizabeth, "Energy Model Development and Heating Energy Investigation of the Nested Thermal Envelope Design (NTED (tm))" (2010). Theses and dissertations. Paper 974.
-
-Group     Fans
-------------
-
-The following fans may be defined either in the air loop or as a zone equipment component: Fan:ConstantVolume, Fan:OnOff, Fan:VariableVolume, Fan:ZoneExhaust, and FanPerformance:NightVentilation. The data that are common to these fan types include an identifying name, an availability schedule name, a total efficiency rating, a rated pressure rise, and inlet and outlet air node names. In the case of a variable volume fan, additional input includes parameters for modeling fan performance over a range of fan speeds. See the engineering documentation for the variable speed fan for a further description of what these coefficients represent. Commonly-used values for different variable volume systems are shown in the following table.
-
-Table 29. Fan Coefficient Values
-
-<table class="table table-striped">
-<tr>
-<th>Type of Fan</th>
-<th>Fan Coeff. 1</th>
-<th>Fan Coeff. 2</th>
-<th>Fan Coeff. 3</th>
-<th>Fan Coeff. 4</th>
-<th>Fan Coeff. 5</th>
-</tr>
-<tr>
-<td>Inlet Vane Dampers</td>
-<td>0.35071223</td>
-<td>0.30850535</td>
-<td>-0.54137364</td>
-<td>0.87198823</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>Discharge Dampers</td>
-<td>0.37073425</td>
-<td>0.97250253</td>
-<td>-0.34240761</td>
-<td>0.000</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>Var. Speed Motor</td>
-<td>0.0015302446</td>
-<td>0.0052080574</td>
-<td>1.1086242</td>
-<td>-0.11635563</td>
-<td>0.000</td>
-</tr>
-</table>
-
-### Fan:ConstantVolume
-
-This object models a constant air volume fan that is intended to operate continuously based on a time schedule. This fan will not cycle on and off based on cooling/heating load or other control signals (Ref: Fan:OnOff).
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a Fan:ConstantVolume. Any reference to this fan by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the fan can run during a given time period. A schedule value of 0 indicates that the fan is off for that time period. A schedule value greater than 0 indicates that the fan can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this schedule by forcing the fan to be on or off.
-
-#### Field: Fan Total Efficiency
-
-This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1.The default is 0.7.
-
-#### Field: Pressure Rise
-
-The pressure rise in Pascals at full flow and standard (sea level) conditions (20 &deg;C and 101325 Pa).
-
-#### Field: Maximum Flow Rate
-
-The full load air volumetric flow rate (m<sup>3</sup>/sec) at standard temperature and pressure (dry air at 20 &deg;C drybulb). The program does use local barometric pressure to account for altitude using equation for "standard atmospheric" pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
-
-p=101325\*(1-2.25577E-05\*Z)\*\*5.2559
-
-where p=pressure in Pa and Z=altitude in m
-
-#### Field: Motor Efficiency
-
-The shaft power divided by the electrical power consumed. Must be between 0 and 1. The default is 0.9.
-
-#### Field: Motor In Airstream Fraction
-
-The fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat loss will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node which supplies the inlet air conditions to the fan.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node to which the fan sends its outlet air.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Central System", etc. A new meter for reporting is created for each unique subcategory   (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the fan will be assigned to the "General" end-use subcategory.
-
-### Constant Volume Fan Outputs
-
-* HVAC,Average,Fan Electric Power[W]
-
-* HVAC,Average,Fan Rise in Air Temperature [deltaC]
-
-* HVAC,Sum,Fan Electric Energy [J]
-
-#### Fan Electric Power [W]
-
-This output field contains the average electricity consumption rate for the fan in Watts for the timestep being reported.
-
-#### Fan Rise in Air Temperature [deltaC]
-
-This output field contains the average rise in air temperature across the fan (outlet air temperature minus inlet air temperature) in degrees Celsius for the timestep being reported.
-
-#### Fan Electric Energy [J]
-
-This output field contains the electricity consumption of the fan in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key= Fans, Group Key= System (ref. Output:Meter objects).
-
-### Fan:OnOff
-
-This object models a constant air volume fan that is intended to cycle on and off in tandem with a cooling or heating system (i.e., AUTO fan control mode). The fan can also operate continuously like Fan:ConstantVolume. If modeling continuous operation and this object is used as part of a system that utilizes Coil:Heating:Gas, Coil:Cooling:DX:SingleSpeed or Coil:Heating:DX:SingleSpeed, the user should confirm proper air flow rates (coil and fan max flows are equal) and that the coil part-load fraction correlation(s) are appropriate (e.g., part-load fraction is less than or equal to 1 for all values of coil part-load ratio). If modeling multi-speed fan operation, this object must be used as part of a compound object that allows multiple fan speeds (e.g., AirLoopHVAC:Unitary:Furnace:HeatCool, ZoneHVAC:PackagedTerminalAirConditioner, etc.). In this case, the ratio of the compound object air flow rate to the fan   s maximum air flow rate is used to determine the power at alternate fan speeds. The optional input for Fan Power Ratio Function of Speed Ratio Curve Name must be entered to model multi-speed fan operation. An optional fan total efficiency ratio curve is also available to model efficiency differences at alternate fan speeds.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a Fan:OnOff. Any reference to this fan by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the fan can run during a given time period. A schedule value of 0 indicates that the fan is off for that time period. A schedule value greater than 0 indicates that the fan can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this schedule by forcing the fan to be on or off.
-
-#### Field: Fan Total Efficiency
-
-This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1.The default is 0.6.
-
-#### Field: Pressure Rise
-
-The pressure rise in Pascals at full flow and standard (sea level) conditions (20 &deg;C and 101325 Pa).
-
-#### Field: Maximum Flow Rate
-
-The full load air volumetric flow rate (m<sup>3</sup>/sec) at standard temperature and pressure (dry air at 20 &deg;C drybulb). The program does use local barometric pressure to account for altitude using equation for "standard atmospheric" pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
-
-p=101325\*(1-2.25577E-05\*Z)\*\*5.2559
-
-where p=pressure in Pa and Z=altitude in m
-
-#### Field: Motor Efficiency
-
-The shaft power divided by the electrical power consumed. Must be between 0 and 1. The default is 0.8.
-
-#### Field: Motor In Airstream Fraction
-
-The fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat loss will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node which supplies the inlet air conditions to the fan.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node to which the fan sends its outlet air.
-
-#### Field: Fan Power Ratio Function of Speed Ratio Curve Name
-
-Enter the name of an exponent performance curve. This optional alpha field must be used to simulate multi-speed fan motors. This curve represents the ratio of actual fan power to rated fan power when a change in fan speed occurs. Leave this field blank when simulating constant-speed fan motors.
-
-#### Field: Fan Efficiency Ratio Function of Speed Ratio Curve Name
-
-Enter the name of a quadratic or cubic performance curve. This optional alpha field is used to simulate multi-speed fan motors. This curve represents the ratio of actual fan total efficiency to rated fan total efficiency when a change in fan speed occurs. Leave this field blank when simulating constant-speed fan motors.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Main Fans", etc. A new meter for reporting is created for each unique subcategory   (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the fan will be assigned to the "General" end-use subcategory.
-
-Following is an example input for an OnOff Fan.
-
-```idf
-Fan:OnOff,
-           Supply Fan 1,                   ! Fan Name
-           FanAndCoilAvailSched,   ! Fan Schedule
-           0.7,                                     ! Fan Total Efficiency
-           600.0,                                 ! Delta Pressure [N/M^2]
-           1.3,                                     ! Max Flow Rate   [m^3/Sec]
-           0.9,                                     ! Motor Efficiency
-           1.0,                                     ! Motor in Airstream Fraction (1.0 means motor in air stream)
-           Air Loop Inlet Node, Cooling Coil Air Inlet Node;   !Inlet Node, Outlet Node
-```
-
-### On Off Fan Outputs
-
-HVAC,Average,Fan Electric Power[W]
-
-HVAC,Average,Fan Rise in Air Temperature [deltaC]
-
-HVAC,Sum,Fan Electric Energy [J]
-
-HVAC,Average,Fan Runtime Fraction []
-
-#### Fan Electric Power [W]
-
-This output field contains the average electricity consumption rate for the fan in Watts for the timestep being reported.
-
-#### Fan Rise in Air Temperature [deltaC]
-
-This output field contains the average rise in air temperature across the fan (outlet air temperature minus inlet air temperature) in degrees Celsius for the timestep being reported.
-
-#### Fan Electric Energy [J]
-
-This output field contains the electricity consumption of the fan in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key= Fans, Group Key= System (ref. Output:Meter objects).
-
-#### Fan Runtime Fraction []
-
-This output field contains the fraction of time that this fan operated for the timestep being reported.
-
-### Fan:VariableVolume
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a Fan:VariableVolume. Any reference to this fan by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the fan can run during a given time period. A schedule value of 0 indicates that the fan is off for that time period. A schedule value greater than 0 indicates that the fan can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this schedule by forcing the fan to be on or off.
-
-#### Field: Fan Total Efficiency
-
-This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
-
-#### Field: Pressure Rise
-
-The pressure rise in Pascals at full flow and standard (sea level) conditions (20 &deg;C and 101325 Pa).
-
-#### Field: Maximum Flow Rate
-
-The full load air volumetric flow rate (m<sup>3</sup>/sec) at standard temperature and pressure (dry air at 20 &deg;C drybulb). The program does use local barometric pressure to account for altitude using equation for "standard atmospheric" pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
-
-p=101325\*(1-2.25577E-05\*Z)\*\*5.2559
-
-where p=pressure in Pa and Z=altitude in m
-
-#### Field: Fan Power Minimum Flow Rate Input Method
-
-This field is a key/choice field that tells which of the next two fields is filled and is descriptive of how the minimum flow rate is specified for calculating the fan power.   The key/choices are:
-
-- Fraction
-
-With this choice, the fan power will be calculated using the value specified in the Fan Power Minimum Flow Fraction field.   (The Fan Power Minimum Flow Fraction field should be filled.)
-
-- FixedFlowRate
-
-With this choice, the fan power will be calculated using the value specified in the Fan Power Minimum Air Flow Rate field.   (The Fan Power Minimum Air Flow Rate field should be filled.)
-
-The default is Fraction.
-
-#### Field: Fan Power Minimum Flow Fraction
-
-The minimum air volumetric flow rate for fan power, specified as a fraction of maximum system air flow rate. Must be between 0 and 1. Note that this field is only used to calculate the fan power. This field does not enforce the system air flow rate during simulation. The default is 0.25.
-
-#### Field: Fan Power Minimum Air Flow Rate
-
-The minimum air volumetric flow rate for fan power, specified as a constant minimum air flow rate (m3/sec). Note that this field is only used to calculate the fan power. This field does not enforce the system air flow rate during simulation.
-
-#### Field: Motor Efficiency
-
-The shaft power divided by the electrical power consumed. Must be between 0 and 1. The default is 0.9.
-
-#### Field: Motor In Airstream Fraction
-
-The fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat loss will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
-
-#### Field: Fan Power Coefficient 1
-
-The constant coefficient (C<sub>1</sub>) in a fourth order polynomial curve giving the fraction of full load power (PLF) as a function of flow fraction (FF). Flow fraction is the air mass flow rate divided by the maximum air mass flow rate. The curve is:
-
-PLF = C<sub>1</sub> + C<sub>2</sub><sup>.</sup> FF + C<sub>3</sub><sup>.</sup> FF<sup>2\\ +</sup> C<sub>4</sub><sup>.</sup> FF<sup>3</sup> + C<sub>5</sub><sup>.</sup> FF<sup>4</sup>
-
-#### Field: Fan Power Coefficient 2
-
-The linear coefficient (C<sub>2</sub>) in a fourth order polynomial curve giving the fraction of full load power (PLF) as a function of flow fraction (FF). Flow fraction is the air mass flow rate divided by the maximum air mass flow rate. The curve is:
-
-PLF = C<sub>1</sub> + C<sub>2</sub><sup>.</sup> FF + C<sub>3</sub><sup>.</sup> FF<sup>2\\ +</sup> C<sub>4</sub><sup>.</sup> FF<sup>3</sup> + C<sub>5</sub><sup>.</sup> FF<sup>4</sup>
-
-#### Field: Fan Power Coefficient 3
-
-The quadratic coefficient (C<sub>3</sub>) in a fourth order polynomial curve giving the fraction of full load power (PLF) as a function of flow fraction (FF). Flow fraction is the air mass flow rate divided by the maximum air mass flow rate. The curve is:
-
-PLF = C<sub>1</sub> + C<sub>2</sub><sup>.</sup> FF + C<sub>3</sub><sup>.</sup> FF<sup>2\\ +</sup> C<sub>4</sub><sup>.</sup> FF<sup>3</sup> + C<sub>5</sub><sup>.</sup> FF<sup>4</sup>
-
-#### Field: Fan Power Coefficient 4
-
-The cubic coefficient (C<sub>1</sub>) in a fourth order polynomial curve giving the fraction of full load power (PLF) as a function of flow fraction (FF). Flow fraction is the air mass flow rate divided by the maximum air mass flow rate. The curve is:
-
-           PLF = C<sub>1</sub> + C<sub>2</sub><sup>.</sup> FF + C<sub>3</sub><sup>.</sup> FF<sup>2\\ +</sup> C<sub>4</sub><sup>.</sup> FF<sup>3</sup> + C<sub>5</sub><sup>.</sup> FF<sup>4</sup>
-
-#### Field: Fan Power Coefficient 5
-
-The coefficient C<sub>5</sub> in a fourth order polynomial curve giving the fraction of full load power (PLF) as a function of flow fraction (FF). Flow fraction is the air mass flow rate divided by the maximum air mass flow rate. The curve is:
-
-           PLF = C<sub>1</sub> + C<sub>2</sub><sup>.</sup> FF + C<sub>3</sub><sup>.</sup> FF<sup>2\\ +</sup> C<sub>4</sub><sup>.</sup> FF<sup>3</sup> + C<sub>5</sub><sup>.</sup> FF<sup>4</sup>
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node which supplies the inlet air conditions to the fan.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node to which the fan sends its outlet air.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Central System", etc. A new meter for reporting is created for each unique subcategory   (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the fan will be assigned to the "General" end-use subcategory.
-
-### Variable Volume Fan Outputs
-
-* HVAC,Average,Fan Electric Power[W]
-
-* HVAC,Average,Fan Rise in Air Temperature [deltaC]
-
-* HVAC,Sum,Fan Electric Energy [J]
-
-#### Fan Electric Power [W]
-
-This output field contains the average electricity consumption rate for the fan in Watts for the timestep being reported.
-
-#### Fan Rise in Air Temperature [deltaC]
-
-This output field contains the average rise in air temperature across the fan (outlet air temperature minus inlet air temperature) in degrees Celsius for the timestep being reported.
-
-#### Fan Electric Energy [J]
-
-This output field contains the electricity consumption of the fan in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key= Fans, Group Key= System (ref. Output:Meter objects).
-
-### Fan:ZoneExhaust
-
-This fan object differs from the other fans in that it stands on its own in a zone rather than serving as one part of an HVAC air system.   This object appears directly in a ZoneHVAC:EquipmentList object and all the controls are contained within the fan object.   The zone exhaust fan model provides a way to include the electrical power used by the fan.   It can also impact air flows in central air handlers by decreasing the flow of return air and sometimes increasing the outdoor air flow rate.
-
-There are several control options available for the exhaust fan including:   an on/off availability schedule, interaction with system availability managers, minimum zone air temperature control limits and a variable flow fraction schedule.
-
-The way in which the exhaust fan impacts central air system can be controlled by declaring what portion of the flow has been    balanced    by simple airflow from infiltration, ventilation, or mixing.   However it is important to note that presence of an exhaust fan does not by itself drive any simple airflow such as infiltration, ventilation, or zone mixing.   There is no comprehensive automatic mass balancing between air system flows, exhaust flows, and the separate simple airflows.   For balancing, the simple airflows need to have their own input objects that need to be coordinated with the exhaust fan.
-
-#### Field: Name
-
-A unique user-assigned name for an instance of a Fan:ZoneExhaust. Any reference to this fan by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the fan can run during a given time period. A schedule value of 0 indicates that the fan is off for that time period. A schedule value greater than 0 indicates that the fan can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this schedule by forcing the fan to be on or off.
-
-#### Field: Fan Total Efficiency
-
-This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.6.
-
-#### Field: Pressure Rise
-
-The pressure rise in Pascals at full flow and standard (sea level) conditions (20 &deg;C and 101325 Pa).
-
-#### Field: Maximum Flow Rate
-
-The full load air volumetric flow rate (m<sup>3</sup>/sec) at standard temperature and pressure (dry air at 20 &deg;C drybulb). The program does use local barometric pressure to account for altitude using equation for "standard atmospheric" pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
-
-p=101325\*(1-2.25577E-05\*Z)\*\*5.2559
-
-where p=pressure in Pa and Z=altitude in m
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node which supplies the inlet air conditions to the fan.   This node should be listed as a zone exhaust node in an associated ZoneHVAC:EquipmentConnections object.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node to which the fan sends its outlet air.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Kitchen Exhaust", "Fume Hoods", etc. A new meter for reporting is created for each unique subcategory   (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the fan will be assigned to the "General" end-use subcategory.
-
-#### Field: Flow Fraction Schedule Name
-
-This field is optional.   If it is not used then the fan operates at the maximum flow rate.   If a schedule is input here, then it should contain fractional values between 0.0 and 1.0, inclusive.   The flow rate that the fan operates will be this fraction times the maximum flow rate.   This allows a variable speed exhaust fan to be modeled according to a schedule.
-
-#### Field: System Availability Manager Coupling Mode
-
-This field is optional. If if is not used then the exhaust fan is assumed to be integrated with the central air handler   s system availability manager.   This field can be used to control if the exhaust fan should operate independently or not.   For example, when a night cycle availability manager turns on the central air system for freeze protection, this field can be used to control if the zone exhaust fans should also run at the same time or not.   The key choice    Coupled    indicates that the exhaust fan should be integrated with the system availability manager so that the fan runs when the air system is forced to run.     The key choice    Decoupled    indicates that the exhaust fan should operate on its own and ignore the system availability manager   s requests so that the exhaust fan can remain off when the air system runs.   The default is Coupled.
-
-#### Field: Minimum Zone Temperature Limit Schedule Name
-
-This field is optional. If it is not used then there will be no temperature-related control over the operation of the exhaust fan.   If the field is used, then enter the name of a schedule with values for zone temperature values ( &deg;C).   The fan   s control will be based on a comparison between the current zone air temperature and the schedule values.   If the zone is warmer than the scheduled limit, then the fan will operate.   When balancing with simple ventilation, this feature can be used to coordinate exhaust fan operation with ZoneVentilation:\* controls for minimum indoor temperature.
-
-#### Field: Balanced Exhaust Fraction Schedule Name
-
-This field is optional.   If it is not used, then all the exhaust air flow is assumed to be unbalanced by any simple airflows, such as infiltration, ventilation, or zone mixing.   Unbalanced exhaust is then modeled as being provided by the outdoor air system in the central air system. The modeling of unbalanced will reduce the flow rates at the zone   s return air node by the flow rate that is being exhausted and will insure that the outdoor air flow rate is sufficient to serve the exhaust.   If this field is used, then enter the name of a schedule with fractional values between 0.0 and 1.0, inclusive.   This fraction is applied to the exhaust fan flow rate and the model tracks the portion of the exhaust that is    balanced.      Balanced exhaust is then modeled as being provided by simple airflows and does not impact the central air system return air or outdoor air flow rates.   For example, if a kitchen zone with an exhaust fan is designed to draw half of its make up air from a neighboring dining room and the other half from the outdoor air system, then a schedule value of 0.5 could be used here.
-
-### Zone Exhaust Fan Outputs
-
-* HVAC,Average,Fan Electric Power [W]
-
-* HVAC,Average,Fan Rise in Air Temperature[deltaC]
-
-* HVAC,Sum,Fan Electric Energy [J]
-
-* HVAC,Average,Fan Unbalanced Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Fan Balanced Air Mass Flow Rate [kg/s]
-
-#### Fan Electric Power [W]
-
-This output field contains the average electricity consumption rate for the fan in Watts for the timestep being reported.
-
-#### Fan Rise in Air Temperature [deltaC]
-
-This output field contains the average rise in air temperature across the fan (outlet air temperature minus inlet air temperature) in degrees Celsius for the timestep being reported.
-
-#### Fan Electric Energy [J]
-
-This output field contains the electricity consumption of the fan in Joules for the timestep being reported. This output is also added to an output meter with Resource Type = Electricity, End Use Key= Fans, Group Key= System (ref. Output:Meter objects).
-
-#### Fan Unbalanced Air Mass Flow Rate [kg/s]
-
-#### Fan Balanced Air Mass Flow Rate [kg/s]
-
-These two output variables are available when the exhaust fan uses the input field called Balanced Exhaust Fraction Schedule Name.   The balanced air flow is the result of the current flow rate times the balance fraction.   The unbalanced air flow is the difference between the current flow rate and the balanced flow rate.   These outputs are the resulting flow rates in kg/s.
-
-
-
-Examples of Fan:ConstantVolume, Fan:VariableVolume, Fan:ZoneExhaust, and , Fan:OnOff,   fans in an IDF are:
-
-```idf
-Fan:ConstantVolume,
-           Supply Fan 1,   !- Name
-           FanAndCoilAvailSched,               !- Availability Schedule Name
-           0.7,                     !- Fan Total Efficiency
-           600.0,                 !- Pressure Rise {Pa}
-           1.3,                     !- Maximum Flow Rate {m3/sec}
-           0.9,                     !- Motor Efficiency
-           1.0,                     !- Motor in Airstream Fraction
-           Air Loop Inlet Node, Cooling Coil Air Inlet Node;   !- Air Inlet Node Name, Air Outlet Node Name
-
-
-Fan:VariableVolume,
-           Var Vol Supply Fan 1,   !- Name
-           FanAndCoilAvailSched,   !-Availability Schedule Name
-           0.7,                    !- Fan Total Efficiency
-           600.0,                !- Pressure Rise {Pa}
-           1.3,                    !- Maximum Flow Rate {m3/s}
-           0.20,                   !- Minimum Flow Rate {m3/s}
-           0.9,                    !- Motor Efficiency
-           1.0,                     !- Motor in Airstream Fraction
-           0.35071223,       !- Fan Coefficient 1
-           0.30850535,       !- Fan Coefficient 2
-         -0.54137364,       !- Fan Coefficient 3
-           0.87198823,       !- Fan Coefficient 4
-           0.000,                 !- Fan Coefficient 5
-           Air Loop Inlet Node, Cooling Coil Air Inlet Node;  !- Air Inlet Node Name,Air Outlet Node Name
-
-
-Fan:ZoneExhaust,
-   Zone 2 Exhaust Fan,                           !-Name
-   FanAndCoilAvailSched,                       !-Availability Schedule Name
-   0.6,                                                         !-Fan Total Efficiency
-   125,                                                         !-Pressure Rise {Pa}
-   0.1,                                                         !-Maximum Flow Rate {m3/s}
-   Zone 2 Exhaust Node,                         !-Air Inlet Node Name
-   Zone 2 Exhaust Fan Outlet Node,   !-Air Outlet Node Name
-   Kitchen Exhaust;                                 !- End-Use Subcategory
-
-
-   Fan:OnOff,
-       AHU 1 Supply Fan,               !- Name
-       FanAvailSched,                     !- Availability Schedule Name
-       0.7,                                         !- Fan Total Efficiency
-       600.0,                                     !- Pressure Rise {Pa}
-       2.0,                                         !- Maximum Flow Rate {m3/s}
-       0.9,                                         !- Motor Efficiency
-       1.0,                                         !- Motor in Airstream Fraction
-       AHU 1 Air Loop Inlet,       !- Air Inlet Node Name
-       AHU 1 Supply Fan Outlet; !- Air Outlet Node Name
-```
-
-
-### FanPerformance:NightVentilation
-
-This object is used for specifying an alternate set of performance parameters for a fan. These alternate parameters are used when a system manager (such as *AvailabilityManager:NightVentilation*) sets a specified flow rate for a central forced air system. At this time, it can be used with Fan:ConstantVolume, Fan:VariableVolume, Fan:ZoneExhaust, and , Fan:OnOff fans, but not with Fan:ComponentModel fans. The fan model checks whether a fixed flow rate has been set; if it has the fan model will use these alternate performance parameters. Note that it is assumed that the fan will run at a fixed speed in the alternate mode. The inputs needed by this object are the fan name, fan total efficiency, pressure rise, flow rate, motor efficiency, and motor in airstream fraction.
-
-#### Field: Fan Name
-
-This is the name of a fan defined elsewhere in the input file. The night vent performance parameters will be applied to the named fan when a system manager has set the air system flow rate.
-
-#### Field: Fan Total Efficiency
-
-This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. This is a required field with no default.
-
-#### Field: Pressure Rise
-
-The pressure rise in Pascals at full flow and standard (sea level) conditions (20 &deg;C and 101325 Pa).
-
-#### Field: Maximum Flow Rate
-
-The design volumetric flow rate of the fan (m<sup>3</sup>/sec) at standard conditions. This input is not currently used by the night ventilation manager. The flow rate during night ventilation is specified using the SystemAvailabilityManager:NightVentilation "Night Venting Flow Fraction" field. This fraction is multiplied times the fan object's design flow rate.
-
-#### Field: Motor Efficiency
-
-The shaft power divided by the electrical power consumed. Must be between 0 and 1. This is a required field with no default.
-
-#### Field: Motor in Airstream Fraction
-
-The fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat loss will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
-
-An example of use in an IDF:
-
-```idf
-   Fan:VariableVolume,
-       Supply Fan 1,                       !- Name
-       FanAvailSched,                     !- Availability Schedule Name
-       0.7,                                         !- Fan Efficiency
-       600.0,                                     !- Pressure Rise {Pa}
-       autosize,                               !- Maximum Flow Rate {m3/s}
-       autosize,                               !- Minimum Flow Rate {m3/s}
-       0.9,                                         !- Motor Efficiency
-       1.0,                                         !- Motor In Airstream Fraction
-       0.35071223,                           !- Fan Coefficient 1
-       0.30850535,                           !- Fan Coefficient 2
-       -0.54137364,                         !- Fan Coefficient 3
-       0.87198823,                           !- Fan Coefficient 4
-       0.000,                                     !- Fan Coefficient 5
-       Main Heating Coil 1 Outlet Node,   !- Air Inlet Node Name
-       VAV Sys 1 Outlet Node;     !- Air Outlet Node Name
-
-
-   FanPerformance:NightVentilation,
-       Supply Fan 1,                       !- Fan Name
-       0.7,                                         !- Fan Total Efficiency
-       67.0,                                       !- Pressure Rise {Pa}
-       autosize,                               !- Maximum Flow Rate {m3/s}
-       0.9,                                         !- Motor Efficiency
-       1.0;                                         !- Motor in Airstream Fraction
-```
-
-### Fan:ComponentModel
-
-The Fan:ComponentModel fan is a more detailed fan type that can be defined in the air loop for central constant-air-volume (CAV) and variable-air-volume (VAV) systems. It includes inputs that describe the air-distribution system as well as the fan, its drive belt (if used), its motor, and its variable-frequency-drive (if used). See the engineering documentation for further descriptions about the inputs for this fan type.
-
-#### Field: Name
-
-The required unique user-assigned alpha name for an instance of a Fan:ComponentModel. Any reference to this fan by another object will use this name.
-
-#### Field: Air Inlet Node Name
-
-The required alpha name of the HVAC system node which supplies the inlet air conditions to the fan.
-
-#### Field: Air Outlet Node Name
-
-The required alpha name of the HVAC system node to which the fan sends its outlet air.
-
-#### Field: Availability Schedule Name
-
-The required alpha name of the schedule (ref: Schedule) that denotes whether the fan can run during a given time period. A schedule value of 0 indicates that the fan is off for that time period. A schedule value greater than 0 indicates that the fan can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods. Applicable availability managers (ref. AvailabilityManagerAssignmentList) may override this schedule by forcing the fan to be on or off.
-
-#### Field: Maximum Flow Rate
-
-The full-load volumetric airflow (m<sup>3</sup>/sec) through the fan at standard temperature and pressure (dry air at 20 &deg;C dry-bulb). To initialize the air systems being simulated, the program uses local barometric pressure adjusted for altitude, based on the equation for "standard atmospheric" pressure on p.6.1 of the 1997 ASHRAE Handbook of Fundamentals (SI edition):
-
-p=101325 \* (1 - 2.25577E-05 \* Z)\*\*5.2559
-
-where p = pressure in Pa and Z = altitude in m. Can be autosized.
-
-Specified or autosized maximum airflow rate (including effects of scaling by Field: Fan Sizing Factor) along with corresponding fan static pressure rise and fan shaft power are reported in the .eio file as, respectively, Design Fan Airflow [m3/s], Design Fan Static Pressure Rise [Pa], and Design Fan Shaft Power [W].
-
-#### Field: Minimum Flow Rate
-
-The minimum volumetric airflow (m<sup>3</sup>/sec) through the fan at standard temperature and pressure (see Maximum Flow Rate field above for condition details). Can be autosized.
-
-#### Field: Fan Sizing Factor
-
-The numeric dimensionless factor (*F<sub>fan</sub>*) used to multiply the specified or autosized full-load volumetric airflow (see Maximum Flow Rate field above for details) for fan sizing. If specified, minimum value is 1.0. Default is 1.0 if field is blank.
-
-#### Field: Fan Wheel Diameter
-
-The required numeric outer diameter of the fan wheel (*D<sub>fan</sub>*, m). This value is determined from manufacturer   s data. In general, larger diameter fans have higher maximum efficiency than smaller diameter fans of the same type (Ref: AMCA Standard 205-10: Energy Efficiency Classification for Fans). Must be greater than zero.
-
-#### Field: Fan Outlet Area
-
-The required numeric outlet area of the fan (*A<sub>fan,out</sub>*, m<sup>2</sup>). This value is determined from manufacturer   s data. It is used to convert fan total pressure rise to fan static pressure rise. Fan static pressure rise is the fan total pressure rise minus the fan outlet velocity pressure; it is not the difference between fan outlet and inlet static pressures (Ref: ANSI/AMCA Standard 210-07, ANSI/ASHRAE Standard 51-07: Laboratory Methods of Testing Fans for Certified Aerodynamic Performance Rating). Must be greater than zero.
-
-#### Field: Maximum Fan Static Efficiency
-
-The required numeric maximum ratio (<span>\(\eta_{fan,max}\)</span>) between the power delivered to the air (*H<sub>air</sub>*, W) and the fan shaft input power (*H<sub>fan</sub>*, W). For this parameter, *H<sub>air</sub>* is the volumetric airflow through the fan multiplied by the fan static pressure rise. Maximum fan static efficiency is determined from analyses of manufacturers data using:
-
-<div>\[{\eta_{fan,\max }} = \max \left[ {\frac{{\left( {\Delta {P_{fan}} * {Q_{fan}}} \right)}}{{{H_{fan}}}}} \right]\]</div>
-
-where *P<sub>fan</sub>* is fan static pressure rise (Pa) and *Q<sub>fan</sub>* is airflow through the fan (m<sup>3</sup>/sec). Typically,    do not select    curves on fan performance maps of pressure rise versus flow correspond to or are near maximum efficiency. Must be greater than zero and less than or equal to 1.0.
-
-Calculated fan static efficiency at design flow condition (including part-load effects of oversized fan) is reported in the .eio file as Design Fan Efficiency [-].
-
-#### Field: Euler Number at Maximum Fan Static Efficiency
-
-The required numeric Euler number (*Eu<sub>max</sub>*), which is also called the throttling or pressure coefficient, and is the ratio of pressure forces to inertial forces. The Euler number is determined from analyses of manufacturer   s data using:
-
-<div>\[Eu = \frac{{\left( {\Delta {P_{fan}} * D_{fan}^4} \right)}}{{\left( {\rho  * Q_{fan}^2} \right)}}\]</div>
-
-where *P<sub>fan</sub>* is fan static pressure rise (Pa; see *Fan Pressure Rise Curve Name* field), *D<sub>fan</sub>* is wheel diameter (m), *�* is the manufacturer   s reference air density (kg/m<sup>3</sup>), and *Q<sub>fan</sub>* is airflow through the fan (m<sup>3</sup>/sec). *Eu<sub>max</sub>* is calculated using any pair of pressure rise and airflow values that correspond with maximum fan static efficiency for the specified fan. Must be greater than zero.
-
-#### Field: Maximum Dimensionless Fan Airflow
-
-The required numeric maximum dimensionless airflow (<span>\(\psi_{max}\)</span>) through the fan, which corresponds to the maximum ratio between the airflow through the fan (*Q<sub>fan</sub>*, m<sup>3</sup>/sec) and the fan shaft rotational speed (<span>\(\omega\)</span><sub>fan</sub>*, rpm) for the specified fan wheel diameter (*D<sub>fan</sub>*, m). *φ<sub>max</sub>* is determined from manufacturers data using:
-
-<div>\[{\varphi_{\max }} = \frac{{30}}{{\pi D_{fan}^3}}*\max \left( {\frac{{{Q_{fan}}}}{{{\omega_{fan}}}}} \right)\]</div>
-
-<sub>max</sub>* occurs at minimum *Eu*, which corresponds to maximum speed (high flow) with zero pressure rise. The factor (<span>\(30/\pi\)</span>) converts revolutions per minute (rpm) to rad/s. Must be greater than zero.
-
-#### Field: Motor Fan Pulley Ratio
-
-The numeric dimensionless ratio of the motor pulley diameter to the fan pulley diameter (*D<sub>motor,pulley</sub> / D<sub>fan,pulley</sub>*). If specified, must be greater than zero. This ratio can be adjusted to account for belt slip if the fractional slip is known (multiply the drive ratio with no slip by 1+s, where s is the belt fractional slip). Default is 1.0 if field is blank (leave blank if no belt; i.e., direct drive). Can be autosized (assumes no slip).
-
-Specified or autosized motor/fan pulley diameter ratio is reported in the .eio file as Drive Ratio [-]. Autosized ratio is based on fan speed in revolutions per minute (rpm), calculated at design flow condition, divided by Field: Motor Maximum Speed.
-
-#### Field: Belt Maximum Torque
-
-The required numeric maximum output torque capacity of the fan drive belt (<span>\(\tau_{belt,max}\)</span> [N-m]). If specified, must be greater than zero. Can be autosized. Use autosize if no belt (i.e., direct drive).
-
-Specified or autosized belt maximum output torque (including effects of scaling by Field: Belt Sizing Factor) is reported in the .eio file as Design Belt Output Torque [N -m]. Also, calculated maximum belt efficiency corresponding to Design Fan Shaft Power, along with belt efficiency at design flow condition (including part-load effects of oversized belt), are reported in the .eio file as, respectively, Maximum Belt Efficiency [-] and Design Belt Efficiency [-].
-
-#### Field: Belt Sizing Factor
-
-The numeric dimensionless factor (*F<sub>belt</sub>*) used to multiply the specified or autosized fan shaft maximum output torque (<sub>belt,max</sub>*). If specified, minimum value is 1.0. Default is 1.0 if field is blank.
-
-#### Field: Belt Fractional Torque Transition
-
-The numeric transition point (*x<sub>belt,trans</sub>*) between performance curves for Regions 1 and 2 for the drive belt normalized part-load efficiency. Must be between 0.0 and 1.0. Default is 0.167 (corresponds to generic V-belt) if field is blank.
-
-#### Field: Motor Maximum Speed
-
-The required numeric maximum rotational speed of the fan motor shaft (*ω<sub>motor,max</sub>*) in revolutions per minute (rpm). Typical values for motors supplied by 60 Hz power are near 900, 1200, 1800, and 3600 rpm. Must be greater than zero.
-
-#### Field: Maximum Motor Output Power
-
-The required numeric maximum output power (input power to the fan drive belt) by the motor (*H<sub>belt,max</sub>*, W). If specified, must be greater than zero. Can be autosized. In the case of direct drive, *H<sub>belt,max</sub>* corresponds to the maximum fan shaft power (*H<sub>fan,max</sub>*).
-
-Specified or autosized maximum motor output power (including effects of scaling by Field: Motor Sizing Factor) is reported in the .eio file as Design Motor Output Power [W]. Also, calculated maximum motor efficiency corresponding to Design Motor Output Power, along with motor efficiency at design flow condition (including part-load effects of oversized motor), are reported in the .eio file as, respectively, Maximum Motor Efficiency [-] and Design Motor Efficiency [-]. Note that maximum motor efficiency often occurs at less than full load.
-
-#### Field: Motor Sizing Factor
-
-The numeric dimensionless sizing factor (*F<sub>motor</sub>*) used to multiply the specified or autosized fan motor output power (*H<sub>belt,max</sub>*). If specified, minimum value is 1.0. Default is 1.0.
-
-#### Field: Motor In Airstream Fraction
-
-The numeric fraction of the combined motor and belt heat that is added to the air stream. A value of 0.0 means that the motor and belt are completely outside the air stream. A value of 1.0 means that all of the motor and belt heat loss will go into the air stream and act to cause an air enthalpy rise. Must be between 0.0 and 1.0. Default is 1.0.
-
-#### Field: VFD Efficiency Type
-
-The alpha basis for calculating fan variable-frequency-drive (VFD) efficiency:    Power   , which corresponds to a function of the fraction of full-load motor input power (*H<sub>motor</sub>* / *H<sub>motor,max</sub>*), or    Speed   , which corresponds to a function of the fraction of full-load speed (*ω<sub>motor</sub> / ω<sub>motor,max</sub>*). If this field is blank, then it is assumed that the VFD efficiency is 0.97. If no VFD is used, then specify    Power    and also specify a VFD efficiency curve with a constant value of 1.0 (see VFD Efficiency Curve Name field for details).
-
-#### Field: Maximum VFD Output Power
-
-The required numeric maximum output power (input power to the fan motor) by the variable frequency drive (*H<sub>motor,max</sub>*, W). If specified, must be greater than zero. Can be autosized.
-
-Specified or autosized maximum VFD output power (including effects of scaling by Field: VFD Sizing Factor) and corresponding VFD input power are reported in the .eio file as, respectively, Design VFD Output Power [W] and Rated Power [W]. Also, calculated VFD efficiency corresponding to Design VFD Output Power (including part-load effects of oversized VFD) along with corresponding combined system efficiency (fan, belt, motor, and VFD efficiencies multiplied together) at design flow condition are reported in the .eio file as, respectively, Design VFD Efficiency [-] and Design Combined Efficiency [-].
-
-#### Field: VFD Sizing Factor
-
-The numeric dimensionless factor (*F<sub>VFD</sub>*) used to multiply the specified or autosized motor maximum input power (*H<sub>motor,max</sub>*). If specified, minimum value is 1.0. Default is 1.0 if field is blank.
-
-#### Field: Fan Pressure Rise Curve Name
-
-The required alpha name of the fan total pressure rise performance curve (ref: Curve:FanPressureRise in Performance Curves) that parameterizes the variation of fan total pressure rise (*P<sub>fan,tot</sub>*, Pa) as a function of volumetric flow through the fan (*Q<sub>fan</sub>*, m<sup>3</sup>/s) and duct static pressure set point (*P<sub>sm</sub>*, Pa). The fan outlet velocity pressure is subtracted from the output of this curve to determine fan static pressure rise, which is then used to calculate a dimensionless Euler number at each time step. The Euler number is in turn used to determine fan efficiency, speed, and torque (the Euler number is defined in the *Euler Number at Maximum Fan Static Efficiency* field). This curve should be valid for the range of volumetric flows, distribution system leakage, duct static pressures, and static pressures surrounding the ducts anticipated for the simulation period.
-
-#### Field: Duct Static Pressure Reset Curve Name
-
-The required alpha name of the performance curve that parameterizes the variation of the duct static pressure set point (*P<sub>sm</sub>*, Pa) as a function of volumetric flow through the fan (*Q<sub>fan</sub>*, m<sup>3</sup>/s), which is used so that the resistance associated with VAV box damper operation is reduced.
-
-The output of this curve is used to calculate the duct static pressure set point at each time step. This curve should be valid for the range of duct static pressure set points and volumetric flows, anticipated for the simulation period.
-
-For an ad hoc linear duct static pressure reset scheme, the relation (ref: Curve:Linear in Performance Curves) between duct static pressure (*P<sub>sm</sub>*, Pa) and flow through the fan (*Q<sub>fan</sub>*, m<sup>3</sup>/s) for *Q<sub>fan,min</sub>*  &le; *Q<sub>fan</sub>*  &le; *Q<sub>fan,max</sub>* is:
-
-<div>\[{P_{sm}} = {P_{sm,\min }} + \left( {{P_{sm,\max }} - {P_{sm,\min }}} \right)*\frac{{\left( {{Q_{fan}} - {Q_{fan,\min }}} \right)}}{{\left( {{Q_{fan,\max }} - {Q_{fan,\min }}} \right)}} = {C_1} + {C_2}*{Q_{fan}}\]</div>
-
-where <span>\({C_1} = {P_{sm,\min }} - {C_2}*{Q_{fan,\min }}\)</span>  and <span>\({C_2} = \frac{{\left( {{P_{sm,\max }} - {P_{sm,\min }}} \right)}}{{\left( {{Q_{fan,\max }} - {Q_{fan,\min }}} \right)}}\)</span>
-
-
-
-For *Q<sub>fan</sub>* &lt; *Q<sub>fan,min</sub>*, *P<sub>sm</sub>* = *P<sub>sm,min</sub>*;for *Q<sub>fan</sub>* &gt; *Q<sub>fan,max</sub>*, *P<sub>sm</sub>* = *P<sub>sm,max</sub>*
-
-
-
-The minimum and maximum fan airflows (*Q<sub>fan,min</sub>* and *Q<sub>fan,max</sub>*) correspond respectively to the minimum and maximum duct static pressure set points (*P<sub>sm,min</sub>* and *P<sub>sm,max</sub>*).
-
-If no duct static pressure reset scheme is used and the duct static pressure set point is constant, then parameter *C<sub>2</sub>* is set to zero and *C<sub>1</sub>* represents the constant duct static pressure set point.
-
-#### Field: Normalized Fan Static Efficiency Curve Name    Non-Stall Region
-
-The required alpha name of the exponential-modified skew normal performance curve (ref: Curve:ExponentialSkewNormal in Performance Curves) that parameterizes the normalized fan static efficiency (*-<sub>fan</sub>* (*x<sub>fan</sub>*) */ -<sub>fan,max</sub>*) at each time step for the normal operating (non-stall) region of the fan performance map as a function of *x<sub>fan</sub>*, which is defined as log-base-10 of Eu at the fan flow and pressure rise operating point divided by Eu at maximum fan static efficiency [*log<sub>10</sub>*(*Eu / Eu<sub>max</sub>*)]. In this region, *x<sub>fan</sub>*&lt;=0.
-
-The output of this curve is used to calculate the fan efficiency *-<sub>fan</sub>* (*x<sub>fan</sub>*) at each time step by modifying *-<sub>fan,max</sub>* (see *Maximum Fan Static Efficiency* field). This curve should have a maximum of 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
-
-#### Field: Normalized Fan Static Efficiency Curve Name    Stall Region
-
-The required alpha name of the exponential-modified skew normal performance curve (ref: Curve:ExponentialSkewNormal in Performance Curves) that parameterizes the normalized fan static efficiency (*-<sub>fan</sub>* (*x<sub>fan</sub>*) */ -<sub>fan,max</sub>*) at each time step for the stall region of the fan performance map as a function of *x<sub>fan</sub>* (see *Normalized Fan Static Efficiency Curve Name    Non-Stall Region* field). In this region, *x<sub>fan</sub>*&gt;0.
-
-The output of this curve is used to calculate the fan efficiency *-<sub>fan</sub>* (*x<sub>fan</sub>*) at each time step by modifying *-<sub>fan,max</sub>* (see *Maximum Fan Static Efficiency* field). This curve should have a maximum of 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
-
-#### Field: Normalized Dimensionless Airflow Curve Name     Non-Stall Region
-
-The required alpha name of the sigmoid performance curve (ref: Curve:Sigmoid in Performance Curves) that parameterizes the normalized dimensionless airflow through the fan (*φ* (*x<sub>fan</sub>*) */ φ<sub>max</sub>*) at each time step for the normal operating (non-stall) region of the fan performance map as a function of *x<sub>fan</sub>*, which is defined as log-base-10 of Eu at the fan flow and pressure rise operating point divided by Eu at maximum fan static efficiency [*log<sub>10</sub>*(*Eu / Eu<sub>max</sub>*)]. In this region, *x<sub>fan</sub>* &lt;=0.
-
-The output of this curve is used to calculate the dimensionless airflow *φ* (*x<sub>fan</sub>*) at each time step by modifying *φ<sub>max</sub>* (see *Maximum Dimensionless Fan Airflow* field). This curve should have a maximum of 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
-
-#### Field: Normalized Dimensionless Airflow Curve Name     Stall Region
-
-The required alpha name of the sigmoid performance curve (ref: Curve:Sigmoid in Performance Curves) that parameterizes the normalized dimensionless airflow through the fan (*φ* (*x<sub>fan</sub>*) */ φ<sub>max</sub>*) at each time step for the stall region of the fan performance map as a function of *x<sub>fan</sub>* (see *Normalized Dimensionless Airflow Curve Name     Non-Stall Region* field). In this region, *x<sub>fan</sub>* &gt;0.
-
-The output of this curve is used to calculate the dimensionless airflow *φ* (*x<sub>fan</sub>*) at each time step by modifying *φ<sub>max</sub>* (see *Maximum Dimensionless Fan Airflow* field). This curve should have a maximum of 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
-
-#### Field: Maximum Belt Efficiency Curve Name
-
-The alpha name of the quartic polynomial performance curve (ref: Curve:Quartic in Performance Curves) that determines the maximum fan drive belt efficiency in logarithmic space (*-<sub>belt,max,ln</sub>*) as a function of *x<sub>belt,max</sub>*. The curve is:
-
-*<span>\({\eta_{belt,\max ,\ln }} = {C_1} + {C_2} \cdot {x_{belt,\max }} + {C_3} \cdot x_{_{belt,\max }}^2 + {C_4} \cdot x_{_{belt,\max }}^3 + {C_5} \cdot x_{_{belt,\max }}^4\)</span>*
-
-where *x<sub>belt,max</sub>* *= ln*(*F<sub>belt</sub>\*H<sub>fan,max</sub>*) with *H<sub>fan,max</sub>* expressed in terms of hp.
-
-*Note that -<sub>belt,max</sub> = exp*(*-<sub>belt,max,ln</sub>*).
-
-The output of this curve must be greater than zero and less than or equal to 1.0. If *-<sub>belt,max</sub>* is known, it is represented by coefficient *C<sub>1</sub>* (*=ln*(*-<sub>belt,max</sub>*)). In this case, coefficients *C<sub>2</sub>* through *C<sub>5</sub>* are set to zero. If this field is left blank (e.g., there is no belt), the model assumes that the output of the modifier curve is 1.0 for the entire simulation (maximum belt efficiency = 1.0).
-
-#### Field: Normalized Belt Efficiency Curve Name     Region 1
-
-The alpha name of the single rectangular hyperbola type 2 performance curve (ref: Curve:RectangularHyperbola2 in Performance Curves) that determines the normalized (par-load) fan drive belt efficiency (*-<sub>belt</sub>* (*x*<sub>belt</sub>) / *-<sub>belt,max</sub>*) as a function of *x<sub>belt</sub>*. Normalized belt efficiency is represented by a segmented curve with three different regions. The curve for Region 1 (0 &lt;= *x<sub>belt</sub>* &lt; *x<sub>belt,trans</sub>*) is:
-
-*-<sub>belt</sub>*(*x*<sub>belt</sub>)/* -<sub>belt,max</sub> =*(*C<sub>1</sub> -\* x<sub>belt</sub>*) */* (*C<sub>2</sub>+x<sub>belt</sub>*) *+ C<sub>3</sub> -\* x<sub>belt</sub>*
-
-where *x<sub>belt</sub>* *=* <sub>belt</sub>* / <sub>belt,max</sub>;* <sub>belt</sub>*   is the belt output torque that corresponds to the calculated power input to the fan shaft (*H<sub>fan</sub>*, W) by the drive belt and the calculated fan shaft speed (*ω<sub>fan</sub>*, rpm).
-
-The output of this curve is used to calculate the belt efficiency *-<sub>belt</sub>* (*x<sub>belt</sub>*) in Region 1 at each time step by modifying *-<sub>belt,max</sub>* (see *Maximum Belt Efficiency* *Curve Name* field). The output of this curve must be greater than zero and less than or equal to 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
-
-If this field is left blank, the model assumes that the output of the modifier curve is 1.0 for the entire simulation (i.e., constant belt efficiency at *-<sub>belt,max</sub>* in Region 1).
-
-#### Field: Normalized Belt Efficiency Curve Name     Region 2
-
-The alpha name of the exponential decay performance curve (ref: Curve:ExponentialDecay in Performance Curves) that determines the normalized (part-load) fan drive belt efficiency (*-<sub>belt</sub>* (*x*<sub>belt</sub>) / *-<sub>belt,max</sub>*) as a function of *x<sub>belt</sub>*. Normalized belt efficiency is represented by a segmented curve with three different regions. The curve for Region 2 (*x<sub>belt,trans</sub>* &lt;= *x<sub>belt</sub>* &lt;= 1) is:
-
-*-<sub>belt</sub>* (*x*<sub>belt</sub>) / *-<sub>belt,max</sub> = C<sub>1</sub> + C<sub>2</sub> \* exp*<sup>(*C*</sup>*3<sup>\*x</sup>belt*<sup>)</sup>
-
-where *x<sub>belt</sub>* *=* <sub>belt</sub>* / <sub>belt,max</sub>;* <sub>belt</sub>*   is the belt output torque that corresponds to the calculated power input to the fan shaft (*H<sub>fan</sub>*, W) by the drive belt and the calculated fan shaft speed (*ω<sub>fan</sub>*, rpm).
-
-The output of this curve is used to calculate the belt efficiency *-<sub>belt</sub>* (*x<sub>belt</sub>*) in Region 2 at each time step by modifying *-<sub>belt,max</sub>* (see *Maximum Belt Efficiency* *Curve Name* field). The output of this curve must be greater than zero and less than or equal to 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
-
-If this field is left blank, the model assumes that the output of the modifier curve is 1.0 for the entire simulation (i.e., constant belt efficiency at *-<sub>belt,max</sub>* in Region 2).
-
-#### Field: Normalized Belt Efficiency Curve Name     Region 3
-
-The alpha name of the single rectangular hyperbola type 2 performance curve (ref: Curve:RectangularHyperbola2 in Performance Curves) that determines the normalized (part-load) fan drive belt efficiency (*-<sub>belt</sub>* (*x*<sub>belt</sub>) / *-<sub>belt,max</sub>*) as a function of *x<sub>belt</sub>*. Normalized belt efficiency is represented by a segmented curve with three different regions. The curve for Region 3 (*x<sub>belt</sub>* &gt; 1) is:
-
-*-<sub>belt</sub>* (*x*<sub>belt</sub>) / *-<sub>belt,max</sub> =*(*C<sub>1</sub> -\* x<sub>belt</sub>*) */* (*C<sub>2</sub>+x<sub>belt</sub>*) *+ C<sub>3</sub> -\* x<sub>belt</sub>*
-
-where *x<sub>belt</sub>* *=* <sub>belt</sub>* / <sub>belt,max</sub>;* <sub>belt</sub>*   is the belt output torque that corresponds to the calculated power input to the fan shaft (*H<sub>fan</sub>*, W) by the drive belt and the calculated fan shaft speed (*ω<sub>fan</sub>*, rpm).
-
-The output of this curve is used to calculate the belt efficiency *-<sub>belt</sub>* (*x<sub>belt</sub>*) in Region 3 at each time step by modifying *-<sub>belt,max</sub>* (see *Maximum Belt Efficiency* *Curve Name* field). The output of this curve must be greater than zero and less than or equal to 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
-
-If this field is left blank, the model assumes that the output of the modifier curve is 1.0 for the entire simulation (i.e., constant belt efficiency at *-<sub>belt,max</sub>* in Region 3).
-
-#### Field: Maximum Motor Efficiency Curve Name
-
-The alpha name of the single rectangular hyperbola type 1 performance curve (ref: Curve: RectangularHyperbola1 in Performance Curves) that determines the maximum fan motor efficiency (*-<sub>motor,max</sub>*) as a function of *x<sub>motor,max</sub>*. The curve is:
-
-*-<sub>motor,max</sub> =*(*C<sub>1</sub> \* x<sub>motor,max</sub>*) */* (*C<sub>2</sub> + x<sub>motor,max</sub>*) *+ C<sub>3</sub>*
-
-where *x<sub>motor,max</sub>=ln*(*F<sub>motor</sub> \* H<sub>belt,max</sub>*) with *H<sub>belt,max</sub>* expressed in terms of hp.*H<sub>belt,max</sub>* is the maximum output power from the motor to the belt, which corresponds to the calculated maximum power input to the fan shaft (*H<sub>fan,max</sub>*, W).
-
-The output of this curve must be greater than zero and less than or equal to 1.0. If *-<sub>motor,max</sub>* is known, it is represented by coefficient *C<sub>3</sub>*. In this case, coefficients *C<sub>1</sub>* and *C<sub>2</sub>* are set to zero.
-
-If this field is left blank, the model assumes that the output of the modifier curve is 1.0 for the entire simulation (maximum motor efficiency = 1.0).
-
-#### Field: Normalized Motor Efficiency Curve Name
-
-The name of the HVAC system node to which the fan sends its outlet air.
-
-The alpha name of the single rectangular hyperbola type 2 performance curve (ref: Curve:RectangularHyperbola2 in Performance Curves) that determines the normalized (part-load) fan motor efficiency (*-<sub>motor</sub>* (*x*<sub>motor</sub>) / *-<sub>motor,max</sub>*) as a function of the motor load fraction *x<sub>motor</sub>*. The curve is:
-
-*-<sub>motor</sub>* (*x<sub>motor</sub>*) */* *-<sub>motor,max</sub> =*(*C<sub>1</sub> \* x**<sub>motor</sub>*) */* (*C<sub>2</sub> + x**<sub>motor</sub>*) *+* (*C<sub>3</sub> -\* x**<sub>motor</sub>*)
-
-where *x<sub>motor</sub> =H<sub>belt</sub>* / *H<sub>belt,max</sub>. H<sub>belt</sub>* is the calculated output power from the motor to the belt (W), which corresponds to the calculated power input to the fan shaft (*H<sub>fan</sub>*, W).
-
-The output of this curve is used to calculate the motor efficiency (*-<sub>motor</sub>* (*x<sub>motor</sub>*)) at each time step by modifying *-<sub>motor,max</sub>* (see *Maximum Motor Efficiency Curve Name* field). The output of this curve must be greater than zero and less than or equal to 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
-
-If this field is left blank, the model assumes that the output of the modifier curve is 1.0 for the entire simulation (i.e., constant motor efficiency at *-<sub>motor,max</sub>*).
-
-#### Field: VFD Efficiency Curve Name
-
-The alpha name of the single rectangular hyperbola type 2 performance curve (e.g., Curve:RectangularHyperbola2 in Performance Curves) that determines the VFD efficiency (*-<sub>VFD</sub>* (*x*<sub>VFD</sub>)) as a function of the fractional input power of the motor or fractional motor speed (*x<sub>VFD</sub>*). An example of the curve is:
-
-*-<sub>VFD</sub>* (*x<sub>VFD</sub>*) *=*(*C<sub>1</sub> \* x**<sub>VFD</sub>*) */* (*C<sub>2</sub>+x**<sub>VFD</sub>*) *+ C<sub>3</sub> \* x**<sub>VFD</sub>*
-
-where *x<sub>VFD</sub> =H<sub>motor</sub>* / *H<sub>motor,max</sub>* or *ω<sub>motor</sub> / ω<sub>motor,max</sub>*
-
-The output of this curve is used to calculate the VFD efficiency *-<sub>VFD</sub>* (*x<sub>VFD</sub>*) at each time step. The output of this curve must be greater than zero and less than or equal to 1.0 and should be valid for the range of volumetric flows and fan pressure rises anticipated for the simulation period.
-
-If this field is left blank, the model assumes that the output of the modifier curve is 0.97 for the entire simulation (i.e., constant VFD efficiency of 0.97).
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Central System". A new meter for reporting is created for each unique subcategory   (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table. If this field is omitted or blank, the fan will be assigned to the "General" end-use subcategory.
-
-An example of use in an IDF:
-
-```idf
-Fan:ComponentModel,
-       Supply Fan 1,                                       ! Fan Name
-       Main Heating Coil 1 Outlet Node, ! Inlet Node Name
-       VAV Sys 1 Outlet Node,                     ! Outlet Node Name
-       FanAvailSched,                                     ! Fan Schedule
-       autosize,                                               ! Maximum Flow Rate [m3/s]
-       autosize,                                               ! Minimum Flow Rate [m3/s]
-       1.0,                                                         ! Fan Sizing Factor [-]
-       0.3048,                                                   ! Fan Wheel Diameter [m]
-       0.0873288576,                                       ! Fan Outlet Area [m2]
-       0.514,                                                     ! Maximum Fan Static Efficiency [-]
-       9.76,                                                       ! Euler Number at Maximum Fan Static Efficiency [-]
-       0.160331811647483,                             ! Maximum Dimensionless Fan Airflow [-]
-       autosize,                                               ! Motor/Fan Pulley Ratio [-]
-       autosize,                                               ! Belt Maximum Torque [N m]
-       1.0,                                                         ! Belt Sizing Factor [-]
-       0.167,                                                     ! Belt Fractional Torque Transition [-]
-       1800,                                                       ! Motor Maximum Speed [rpm]
-       autosize,                                               ! Maximum Motor Output Power [W]
-       1.0,                                                         ! Motor Sizing Factor [-]
-       1.0,                                                         ! Motor In Airstream Fraction [-]
-       Power,                                                     ! VFD Efficiency Type
-       autosize,                                               ! Maximum VFD Output Power [W]
-       1.0,                                                         ! VFD Sizing Factor [-]
-       VSD Example,                                         ! Fan Pressure Rise Curve Name
-       DiagnosticSPR,                                     ! Duct Static Pressure Reset Curve Name
-       FanEff120CPLANormal,                         ! Fan Efficiency Curve Name     Non-Stall
-       FanEff120CPLAStall,                           ! Fan Efficiency Curve Name - Stall
-       FanDimFlowNormal,                               ! Dimensionless Airflow Curve Name-Non-Stall
-       FanDimFlowStall,                                 ! Dimensionless Airflow Curve Name-Stall
-       BeltMaxEffMedium,                               ! Maximum Belt Efficiency Curve Name
-       BeltPartLoadRegion1,                         ! Normalized Belt Efficiency Curve Name
-       BeltPartLoadRegion2,                         ! Normalized Belt Efficiency Curve Name
-       BeltPartLoadRegion3,                         ! Normalized Belt Efficiency Curve Name
-       MotorMaxEffAvg,                                   ! Maximum Motor Efficiency Curve Name
-       MotorPartLoad,                                     ! Normalized Motor Efficiency Curve Name
-       VFDPartLoad;                                         ! VFD Efficiency Curve Name
-```
-
-
-### Component Model Fan Outputs
-
-* HVAC,Average,Fan Electric Power[W]
-
-* HVAC,Average,Fan Rise in Air Temperature [deltaC]
-
-* HVAC,Sum,Fan Electric Energy [J]
-
-#### Fan Electric Power [W]
-
-This output field contains the average electricity consumption rate for the fan in Watts for the timestep being reported.
-
-#### Fan Rise in Air Temperature [deltaC]
-
-This output field contains the average rise in air temperature across the fan (outlet air temperature minus inlet air temperature) in degrees Celsius for the timestep being reported.
-
-#### Fan Electric Energy [J]
-
-This output field contains the electricity consumption of the fan in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key= Fans, Group Key= System (ref. Output:Meter objects).
-
-#### Other Outputs
-
-Several parameters input by the user or calculated during component sizing for the design condition (maximum system airflow) are reported separately in the &lt;filename&gt;.eio file. These parameters include fan airflow and pressure rise; fan shaft input, motor output, VFD output, and VFD input (rated) power; pulley drive ratio; belt output torque; and fan, belt, motor, VFD, and combined system efficiencies. They can be identified by lines in the .eio file beginning with    Component Sizing Information, Fan:ComponentModel   . The same values are also reported under the ComponentSizingSummary heading in the &lt;filename&gt;Table.html file.
-
-Group -- Humidifiers
---------------------
-
-### Humidifier:Steam:Electric
-
-The electric steam humidifier is a component that represents an electrically heated, self contained steam humidifier. The component uses electrical energy to convert ordinary tap water to steam which it then injects into the supply air stream by means of a blower fan. The actual unit might be an electrode-type humidifier or a resistance-type humidifier.
-
-The humidifier model includes local control of the humidifier unit to meet a humidity ratio setpoint on its air outlet node. A set point manager is needed to put a setpoint on the exit node but no other local controllers are needed. The humidifier will add moisture to meet the humidity ratio setpoint.
-
-#### Field: Name
-
-A unique user assigned name for a particular humidifier unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Rated Capacity
-
-The nominal full output water addition rate of the unit in m<sup>3</sup>/sec of water at 5.05 C. This field is autosizable.
-
-#### Field: Rated Power
-
-The nominal full output power consumption of the unit in watts, exclusive of the blower fan power consumption and any standby power. This field can be autosized. When it is autosized, its calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from the a reference temperature of liquid water at 20 &deg;C to a saturated steam at 100 &deg;C.
-
-#### Field: Rated Fan Power
-
-The nominal full output power consumption of the blower fan in watts.
-
-#### Field: Standby Power
-
-The standby power consumption in watts. This amount of power will be consumed whenever the unit is available (as defined by the availability schedule).
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws inlet air.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its outlet air.
-
-#### Field: Water Storage Tank Name
-
-This field is optional. If left blank or omitted, then the humidifier obtains its water directly from the mains water. If the name of a Water Storage Tank is specified, then the humidifier will try to obtain its water from that tank. If the tank can   t provide all the water then the rest will be drawn from the mains and the humidifier will still operate.
-
-An IDF example:
-
-```idf
-Humidifier:Steam:Electric,
-           Humidifier 1,                   !- Name
-           FanAndCoilAvailSched,   !- Availability Schedule Name
-           0.00000379,                       !- Rated Capacity {m3/s}
-           10200.,                               !- Rated Power {W}
-           27.,                                     !- Rated Fan Power {W}
-           2.,                                       !- Standby Power {W}
-           Cooling Coil Air Outlet Node, !- Air Inlet Node Name
-           Air Loop Outlet Node;   !- Air Outlet Node Name
-```
-
-
-### Steam Electric Humidfier Outputs
-
-* HVAC,Average,Humidifier Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Humidifier Water Volume[m3]
-
-* HVAC,Average,Humidifier Electric Power[W]
-
-* HVAC,Sum,Humidifier Electric Energy [J]
-
-* Zone,Meter,Humidifier:Water [m3]
-
-* Zone,Meter,Humidifier:Electricity [J]
-
-* HVAC,Average,Humidifier Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Humidifier Storage Tank Water Volume [m3]
-
-* HVAC,Average,Humidifier Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Humidifier Starved Storage Tank Water Volume [m3]
-
-* Zone,Meter,Humidifier:MainsWater [m3]
-
-* HVAC,Sum,Humidifier Mains Water Volume [m3]
-
-#### Humidifier Water Volume Flow Rate [m3/s]
-
-This field reports the water consumption rate of the steam humidifier in cubic meters of water per second.
-
-#### Humidifier Water Volume[m3]
-
-This ouput is the cubic meters of water consumed by the steam humidifier over the timestep being reported.
-
-#### Humidifier Electric Power[W]
-
-This output is the electricity consumption rate in Watts of the steam humidifier.
-
-#### Humidifier Electric Energy [J]
-
-This is the electricity consumption in Joules of the steam humidifier over the timestep being reported.
-
-#### Humidifier:Water [m3]
-
-This meter output contains the sum of the water consumed (in cubic neters of water during the report timestep) by all the steam humidifiers at the HVAC level in the simulation.
-
-#### Humidifier:Electricity [J]
-
-This meter output contains the sum of the electricity consumed (in Joules during the report timestep) by all the steam humidifiers at the HVAC level in the simulation.
-
-#### Humidifier Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Humidifier Storage Tank Water Volume [m3]
-
-These outputs contain the rate and volume of water obtained from water storage tank. These are only present if the humidifier is connected to a Water Storage Tank for its water supply.
-
-#### Humidifier Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Humidifier Starved Storage Tank Water Volume [m3]
-
-These outputs contain the rate and volume of water that could not be obtained from the water storage tank. The component will still operate as if it did get all the water with the balance obtained directly from the mains
-
-#### Humidifier Mains Water Volume [m3]
-
-This output contains the volume of water obtained from the mains.
-
-### Humidifier:Steam:Gas
-
-The gas fired steam humidifier is a component that represents a gas fired self-contained steam humidifier. The component uses gas fired energy to convert ordinary tap water to steam which it then blows or injects into the supply air stream. Blower fan may not be required depending on how the dry steam is delivered into the supply air stream. The humidifier model includes local control of the humidifier unit to meet a humidity ratio setpoint on its air outlet node of the unit. A humidity set point manager is needed to put a setpoint on the outlet node but no other local controllers are needed. The humidifier either blows or injects dry steam to meet the humidity ratio setpoint requirement. If the Rated Gas Use Rate input field is not autosized, the thermal efficiency input specified will be ignored and ovverriden by a thermal efficiency  value determined from user specified Rated Gas Use Rate, rated capacity (m3/s) and design conditions for sizing calculation.    
-
-#### Field: Name
-
-A unique user assigned name for a particular humidifier unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Rated Capacity
-
-The nominal full capacity water addition rate in m3/s of water at 5.05 C.
-
-#### Field: Rated Gas Use Rate {W}
-
-The nominal gas use rate in Watts. This input field can be autosized. When this input field is autosized, it is calculated from the rated capacity in kg/s, the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20 &deg;C to a saturated steam at 100 &deg;C and user specified thermal efficiency. If this input field is hardsized and the Inlet Water Temperature Option input field is selected as FixedInletWaterTemperature, then the thermal efficiency input field will not be used in the calculation or else if the Inlet Water Temperature Option input selected is VariableInletWaterTemperature, then the user specified thermal efficiency value will be overridden using internally calculated efficiency from the capacity, rated gas use rate and design condition.
-
-#### Field: Thermal Efficiency
-
-The thermal efficiency of the gas fired humidifier. The thermal efficiency is based on the higher heating value of the fuel. The default value is 0.8. If    Rated Gas Use Rate    in the field above is not autosized and the Inlet Water Temperature Option input field selected is FixedInletWaterTemperature, then the thermal efficiency specified will be ignored in the calculation, or else if the Inlet Water Temperature Option input field is specified as VariableInletWaterTemperature, then the user specified thermal efficiency value will be overridden using internally calculated matching the capacity, rated gas use rate specified and design condition defined for sizing calculation.
-
-#### Field: Thermal Efficiency Modifier Curve Name
-
-This is thermal efficiency modifier curve name of unit. This curve is normalized, i.e., the curve output value at rated condition is 1.0. If this input field is blank, then constant efficiency value specified in the input field above will be used.  Allowed thermal efficiency modifier curve types are linear, quadratic, or cubic.  These curves are solely a function of part load ratio.
-
-#### Field: Rated Fan Power
-
-The nominal full capacity electric power input to the blower fan in Watts. If no blower fan is required to inject the dry steam to the supply air stream, then this input field is set to zero.
-
-#### Field: Auxiliary Electric Power
-
-The auxiliary electric power input in watts. This amount of power will be consumed whenever the unit is available (as defined by the availability schedule). This electric power is used for control purpose only.
-
-#### Field: Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws inlet air.
-
-#### Field: Air Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its outlet air.
-
-#### Field: Water Storage Tank Name
-
-This field is optional. If left blank or omitted, then the humidifier obtains its water directly from the mains water. If the name of a Water Storage Tank is specified, then the humidifier will try to obtain its water from that tank. If the tank can   t provide all the water then the rest will be drawn from the mains and the humidifier will still operate.
-
-#### Field: Inlet Water Temperature Option
-
-This field is a key/choice field that tells which humidifier water inlet temperature to use: fixed inlet temperature or variable water inlet temperature that depends on the source. Currently allowed water sources are main water or water storage tank in water use objects. The key/choice are: FixedInletWaterTemperature, with this choice, the gas fired humidifier will use a fixed 20C water inlet temperature. VariableInletWaterTemperature, with this choice, the gas fired humidifier will use water inlet temperature that depends on the source temperature. If a water use storage tank name is specified, then the gas humidifier water inlet temperature will be the storage water temperature, or else it uses water main temperature. The default main water temperature is 10 &deg;C. If left blank or omitted, then the humidifier assumes fixed inlet water temperature of 20 &deg;C.
-
-An IDF example:
-
-```idf
-  Humidifier:Steam:Gas,
-    Main Gas Humidifier,!- Name
-    ALWAYS_ON,          !- Availability Schedule Name
-    4.00E-5,            !- Rated Capacity {m3/s}
-    104000,             !- Rated Gas Use Rate {W}
-    1.0,                !- Thermal Efficiency {-} 
-    ,                   !- Thermal Efficiency Modifier Curve Name
-    0,                  !- Rated Fan Power {W}
-    0,                  !- Auxiliary Electric Power {W}
-    Mixed Air Node 1,   !- Air Inlet Node Name
-    Main Humidifier Outlet Node,  !- Air Outlet Node Name
-    ;                   !- Water Storage Tank Name
-```
-
-Steam Gas Humidifier Outputs
-
-* HVAC,Average,Humidifier Water Volume Flow Rate [m3/s]
-* HVAC,Sum,Humidifier Water Volume[m3]
-* HVAC,Average,Humidifier Gas Use Rate[W]
-* HVAC,Sum,Humidifier Gas Use Energy [J]
-* HVAC,Average,Humidifier Auxiliary Electric Power[W]
-* HVAC,Sum,Humidifier Auxiliary Electric Energy [J]
-* HVAC,Meter,Humidifier:Water [m3]
-* HVAC,Meter,Humidifier:Gas [J]
-* HVAC,Meter,Humidifier:Electricity [J]
-* HVAC,Average,Humidifier Storage Tank Water Volume Flow Rate [m3/s]
-* HVAC,Sum,Humidifier Storage Tank Water Volume [m3]
-* HVAC,Average,Humidifier Starved Storage Tank Water Volume Flow Rate [m3/s]
-* HVAC,Sum,Humidifier Starved Storage Tank Water Volume [m3]
-* Zone,Meter,Humidifier:MainsWater [m3]
-* HVAC,Sum,Humidifier Mains Water Volume [m3]
-
-#### Humidifier Water Volume Flow Rate [m3/s]
-
-This field reports the water consumption rate of the steam humidifier in cubic meters of water per second.
-
-#### Humidifier Water Volume [m3]
-
-This output is the cubic meters of water consumed by the steam humidifier over the timestep being reported.
-
-#### Humidifier Gas Use Rate [W]
-
-This output is the gas use rate of the gas fired steam humidifier in Watts.  
-
-#### Humidifier Gas Use Energy [J]
-
-This output is the gas consumption of the gas fired steam humidifier in Joules.  
-
-#### Humidifier Auxiliary Electric Power [W]
-
-This output is the auxiliary electricity consumption rate in Watts of the gas fired steam humidifier.  This is the auxiliary electric power input to the blower fan and control unit.
-
-#### Humidifier Auxiliary Electric Energy [J]
-
-This is the auxiliary electricity consumption in Joules of the gas fired steam humidifier over the timestep being reported. This is the auxiliary electric energy consumed by the blower fan and control unit.  This auxiliary electric energy is reported meter output Humidifier:Electricity.
-
-#### Humidifier:Water [m3]
-
-This meter output contains the sum of the water consumed (in cubic meters of water during the report timestep) by all the steam humidifiers at the HVAC level in the simulation.
-
-#### Humidifier:Gas [J]
-
-This meter output contains the sum of the gas consumed (in Joules during the report timestep) by all the steam humidifiers at the HVAC level in the simulation.
-
-#### Humidifier Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Humidifier Storage Tank Water Volume [m3]
-
-These outputs contain the rate and volume of water obtained from water storage tank. These are only present if the humidifier is connected to a Water Storage Tank for its water supply.
-
-#### Humidifier Starved Storage Tank Water Volume Flow Rate [m3/s]
-
-#### Humidifier Starved Storage Tank Water Volume [m3]
-
-These outputs contain the rate and volume of water that could not be obtained from the water storage tank. The component will still operate as if it did get all the water with the balance obtained directly from the mains
-
-#### Humidifier Mains Water Volume [m3]
-
-This output contains the volume of water obtained from the mains.
-
-
-Group     Desiccant Dehumidifiers
--------------------------------
-
-### Dehumidifier:Desiccant:NoFans
-
-This object models a solid desiccant dehumidifier (excluding associated fans). The process air stream is the air which is dehumidified. The regen air stream is the air which is heated to regenerate the desiccant. This object determines the process air outlet conditions, the load on the regeneration heating coil, the electric power consumption for the wheel rotor motor, and the regeneration air fan mass flow rate. All other heat exchangers are modeled as separate objects connected to the inlet and outlet nodes of the dehumidifier. The solid desiccant dehumidifier is typically used in an AirLoopHVAC:OutdoorAirSystem object, but can also be specified in any AirLoopHVAC. The regeneration heating coil can be Gas, Electric, Steam , or Hot Water coil.   When hot water coil is selected as regeneration heating coil user-defined curves designed for lower temperature operation must be specified in the input field Performance Model Type along with the Nominal Regeneration Temperature input field. The default performance model type is valid for higher nominal regeneration temperature (e.g. 121C).
-
-#### Field: Name
-
-This alpha field contains the identifying name for the desiccant dehumidifier.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the desiccant unit can run during a given time period. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Process Air Inlet Node Name
-
-The name of the node entering the process side of the desiccant wheel.
-
-#### Field: Process Air Outlet Node Name
-
-The name of the node leaving the process side of the desiccant wheel.
-
-#### Field: Regeneration Air inlet Node Name
-
-The name of the node entering the regeneration side of the desiccant wheel after the regeneration coil.
-
-#### Field: Regeneration Fan Inlet Node Name
-
-Node name for air entering the regeneration fan, mass flow is set by this desiccant dehumidifier model.
-
-#### Field: Control Type
-
-Type of setpoint control. Options are
-
-- LeavingMaximumHumidityRatioSetpoint
-
-- SystemNodeMaximumHumidityRatioSetpoint
-
-**LeavingMaximumHumidityRatioSetpoint** means that the unit is controlled to deliver air at the *Leaving Maximum Humidity Ratio Setpoint*, using bypass dampers to prevent overdrying.
-
-**SystemNodeMaximumHumidityRatioSetpoint** means that the unit is controlled to deliver air at the maximum humidity ratio setpoint (System Node Humidity Ratio Max) on the *Process Air outlet node*, using bypass dampers to prevent overdrying. This setpoint must be established using a set point manager which sets the MaximumHumidityRatio control variable:
-
-- SetpointManager:SingleZone:Humidity:Maximum
-
-- SetpointManager:MultiZone:MaximumHumidity:Average
-
-- SetpointManager:MultiZone:Humidity:Maximum
-
-This will also require the use of a **ZoneControl:Humidistat** object. If the dehumidifer is located in the outdoor air stream, it may also be necessary to use **SetpointManager:OutdoorAirPretreat**.
-
-#### Field: Leaving Maximum Humidity Ratio Setpoint
-
-Fixed setpoint for maximum process air leaving humidity ratio. Applicable only when Control Type = LeavingMaximumHumidityRatioSetpoint.
-
-#### Field: Nominal Process Air Flow Rate
-
-  Process air flow rate in m<sup>3</sup>/s at nominal conditions. This field is autosizable.
-
-#### Field: Nominal Process Air Velocity
-
-Process air velocity in m/s at nominal flow. The default value is 3m/s.
-
-#### Field: Rotor Power
-
-Power input to wheel rotor motor in W. If this field is unknown, electricity consumption of the unit can be obtained from nominal power per unit air flow rate below.
-
-#### Field: Regeneration Coil Object Type
-
-Type of heating coil object for regeneration air. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the regeneration air heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Dehumidifier:Desiccant:NoFans) itself provides the "controller" function of modulating water flow. The valid choices are:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Regeneration Coil Name
-
-Name of heating coil object for regeneration air.
-
-#### Field: Regeneration Fan Object Type
-
-Type of fan object for regeneration air. For UserCurves performance (see below) Fan:VariableVolume and Fan:ConstantVolume are valid. For Default performance (see below) only Fan:VariableVolume is valid.
-
-#### Field: Regeneration Fan Name
-
-Name of fan object for regeneration air.
-
-#### Field: Performance Model Type
-
-Specifies whether the Default performance model or UserCurves curves should be used to model the performance. The default model is a generic solid desiccant wheel using performance curves of the form:
-
-curve = C1 + C2\*edb + C3\*edb\*\*2 + C4\*ew + C5\*ew\*\*2 +
- C6\*vel + C7\*vel\*\*2 + C8\*edb\*ew + C9\*edb\*\*2\*ew\*\*2 +
- C10\*edb\*vel + C11\*edb\*\*2\*vel\*\*2 + C12\*ew\*vel + C13\*ew\*\*2\*vel\*\*2 +
- C14\*ALOG(edb) + C15\*ALOG(ew) + C16\*ALOG(vel)
-
- edb = process entering drybulb temperature [C]    
- ew   = process entering humidity ratio [kgWater/kgDryAir]    
- vel = process air velocity [m/s]
-
-The Default curves are valid for the following range of process inlet conditions:   dry-bulb temperatures of 1.67C (35F) to 48.9C (120F) and humidity ratios of 0.002857 kgWater/kgDryAir (20 gr/lb) to 0.02857 kgWater/kgDryAir (200 gr/lb). If the process inlet conditions are outside this range, the dehumidifier will not operate.
-
-If UserCurves are specified, then performance is calculated as follows:
-
-Leaving Dry-bulb = (Leaving Dry-Bulb Function of Entering Dry-Bulb and Humidity Ratio Curve) \* (Leaving Dry-Bulb Function of Air Velocity Curve)
-
-Leaving Humidity Ratio = (Leaving Humidity Ratio Function of Entering Dry-Bulb and Humidity Ratio Curve) \* (Leaving Humidity Ratio Function of Air Velocity Curve)
-
-Regeneration Energy = (Regeneration Energy Function of Entering Dry-Bulb and Humidity Ratio Curve) \* (Regeneration Energy Function of Air Velocity Curve)
-
-Regeneration Velocity = (Regeneration Velocity Function of Entering Dry-Bulb and Humidity Ratio Curve) \* (Regeneration Velocity Function of Air Velocity Curve)
-
-The UserCurves are limited to the following range of process inlet conditions (essentially not limited):   dry-bulb temperatures of    73.3C (-100F) to 65.6C (150F) and humidity ratios of 0.0 kgWater/kgDryAir (0 gr/lb) to 0.21273 kgWater/kgDryAir (1490 gr/lb). If the process inlet conditions are outside this range, the dehumidifier will not operate.
-
-
-
-When the Default performance model is selected, the remaining fields are ignored.
-
-#### Field: Leaving Dry-Bulb Function of Entering Dry-Bulb and Humidity Ratio Curve Name
-
-*This field is applicable only when* UserCurves *performance model type is specified.*
-
-Leaving dry-bulb of process air as a function of entering dry-bulb and entering humidity ratio, biquadratic curve.
-
-curve = C1 + C2\*edb + C3\*edb\*\*2 + C4\*ew + C5\*ew\*\*2 + C6\*edb\*ew
-
-edb = process entering drybulb temperature [C]
-
-ew   = process entering humidity ratio [kgWater/kgDryAir]
-
-#### Field: Leaving Dry-Bulb Function of Air Velocity Curve Name
-
-*This field is applicable only when* UserCurves *performance model type is specified.*
-
-Leaving dry-bulb of process air as a function of air velocity,   quadratic curve.
-
-curve = C1 + C2\*v + C3\*v\*\*2
-
-v = process air velocity [m/s]
-
-#### Field: Leaving Humidity Ratio Function of Entering Dry-Bulb and Humidity Ratio Curve Name
-
-*This field is applicable only when* UserCurves *performance model type is specified.*
-
-Leaving humidity ratio of process air as a function of entering dry-bulb and entering humidity ratio, biquadratic curve
-
-curve = C1 + C2\*edb + C3\*edb\*\*2 + C4\*ew + C5\*ew\*\*2 + C6\*edb\*ew
-
-edb = process entering drybulb temperature [C]
-
-ew   = process entering humidity ratio [kgWater/kgDryAir]
-
-#### Field: Leaving Humidity Ratio Function of Air Velocity Curve Name
-
-*This field is applicable only when* UserCurves *performance model type is specified.*
-
-Leaving humidity ratio of process air as a function of process air velocity, quadratic curve.
-
-curve = C1 + C2\*v + C3\*v\*\*2
-
-v = process air velocity [m/s]
-
-#### Field: Regeneration Energy Function of Entering Dry-Bulb and Humidity Ratio Curve Name
-
-*This field is applicable only when* UserCurves *performance model type is specified.*
-
-Regeneration energy [J/kg of water removed] as a function of entering dry-bulb and entering humidity ratio, biquadratic curve
-
-curve = C1 + C2\*edb + C3\*edb\*\*2 + C4\*ew + C5\*ew\*\*2 + C6\*edb\*ew
-
-edb = process entering drybulb temperature [C]
-
-ew   = process entering humidity ratio [kgWater/kgDryAir]
-
-#### Field: Regeneration Energy Function of Air Velocity Curve Name
-
-*This field is applicable only when* UserCurves *performance model type is specified.*
-
-Regeneration energy [J/kg of water removed] as a function of process air velocity, quadratic curve.
-
-curve = C1 + C2\*v + C3\*v\*\*2
-
-v = process air velocity [m/s]
-
-#### Field: Regeneration Velocity Function of Entering Dry-Bulb and Humidity Ratio Curve Name
-
-*This field is applicable only when* UserCurves *performance model type is specified.*
-
-Regeneration velocity [m/s] as a function of entering dry-bulb and entering humidity ratio, biquadratic curve
-
-curve = C1 + C2\*edb + C3\*edb\*\*2 + C4\*ew + C5\*ew\*\*2 + C6\*edb\*ew
-
-edb = process entering drybulb temperature [C]
-
-ew   = process entering humidity ratio [kgWater/kgDryAir]
-
-#### Field: Regeneration Velocity Function of Air Velocity Curve Name
-
-*This field is applicable only when* UserCurves *performance model type is specified.*
-
-Regeneration velocity [m/s] as a function of process air velocity, quadratic curve.
-
-curve = C1 + C2\*v + C3\*v\*\*2
-
-v = process air velocity [m/s]
-
-#### Field: Nominal Regeneration Temperature
-
-*This field is applicable only when* UserCurves *performance model type is specified.*
-
-Nominal regeneration temperature upon which the regeneration energy modifier curve is based. This input is ignored when Performance Model Type = Default, which assume a regeneration temperature of 121C.
-
-#### Field: Nominal Power Per Unit Air Flow Rate
-
-This field is nominal power consumption per unit air flow rate. It is used to calculate electricity consumption of the unit when no rotor power is entered.
-
-
-
-An example of this statement in an IDF is:
-
-```idf
-   Dehumidifier:Desiccant:NoFans,
-       Desiccant 1,                         !- Name
-       FanAndCoilAvailSched,       !- Availability Schedule Name
-       Outside Air Inlet Node,   !- Process Air Inlet Node Name
-       Desiccant Process Outlet Node,   !- Process Air Outlet Node Name
-       Regen Coil Out Node,         !- Regeneration Air Inlet Node Name
-       Outside Air Inlet Node 2,!- Regeneration Fan Inlet Node Name
-       SystemNodeMaximumHumidityRatioSetpoint,   !- Control Type
-       0.007,                                     !- Leaving Maximum Humidity Ratio Setpoint {kgWater/kgDryAir}
-       1,                                             !- Nominal Process Air Flow Rate {m3/s}
-       2.5,                                         !- Nominal Process Air Velocity {m/s}
-       10,                                           !- Rotor Power {W}
-       Coil:Heating:Gas,               !- Regeneration Coil Object Type
-       Desiccant Regen Coil,       !- Regeneration Coil Name
-       Fan:VariableVolume,           !- Regeneration Fan Object Type
-       Desiccant Regen Fan,         !- Regeneration Fan Name
-       UserCurves,                           !- Performance Model Type
-       Desiccant DryBulb fTW Curve, !- Leaving Dry-Bulb Function of Entering Dry-Bulb and Humidity Ratio
-                         !                                                 Curve Name
-       Desiccant DryBulb fV Curve,   !- Leaving Dry-Bulb Function of Air Velocity Curve Name
-       Desiccant HumRat fTW Curve,   !- Leaving Humidity Ratio Function of Entering Dry-Bulb and Humidity Ratio Curve Name
-       Desiccant HumRat fV Curve,     !- Leaving Humidity Ratio Function of Air Velocity Curve Name
-       Desiccant RegenEnergy fTW Curve, !- Regeneration Energy Function of Entering Dry-Bulb and Humidity Ratio Curve Name
-       Desiccant RegenEnergy fV Curve,   !- Regeneration Energy Function of Air Velocity Curve Name
-       Desiccant RegenVel fTW Curve,       !- Regeneration Velocity Function of Entering Dry-Bulb and Humidity Ratio Curve Name
-       Desiccant RegenVel fV Curve,         !- Regeneration Velocity Function of Air Velocity Curve Name
-       121,                                         !- Nominal Regeneration Temperature {C}
-       ;                                  !- Nominal Power Per Unit Air Flow Rate {W/m3/s}
-```
-
-### Desiccant Dehumidifier (NoFans) Outputs
-
-* HVAC,Sum,Dehumidifier Removed Water Mass [kg]
-
-* HVAC,Average,Dehumidifier Removed Water Mass Flow Rate [kg/s]
-
-* HVAC,Average,Dehumidifier Part Load Ratio []
-
-* HVAC,Average,Dehumidifier Electric Power [W]
-
-* HVAC,Sum,Dehumidifier Electric Energy [J]
-
-* HVAC,Average,Dehumidifier Regeneration Specific Energy [J/kgWater]
-
-* HVAC,Average,Dehumidifier Regeneration Rate [W]
-
-* HVAC,Sum,Dehumidifier Regeneration Energy [J]
-
-* HVAC,Average,Dehumidifier Regeneration Air Speed [m/s]
-
-* HVAC,Average,Dehumidifier Regeneration Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Dehumidifier Process Air Mass Flow Rate [kg/s]
-
-#### Dehumidifier Removed Water Mass   [kg]
-
-Mass of water removed from process air stream.
-
-#### Dehumidifier Removed Water Mass Flow Rate [kg/s]
-
-Rate of water removal from process air stream.
-
-#### Dehumidifier Part Load Ratio []
-
-Dehumidifier water removal rate divided by full-load water removal rate.
-
-#### Dehumidifier Electric Power [W]
-
-Dehumidifier rotor electric power.
-
-#### Dehumidifier Electric Energy [J]
-
-Dehumidifier rotor electric energy.
-
-#### Dehumidifier Regeneration Specific Energy [J/kgWater]
-
-Regeneration heating coil energy divided by water removed.
-
-#### Dehumidifier Regeneration Rate [W]
-
-Regeneration heating coil output rate.
-
-#### Dehumidifier Regeneration Energy [J]
-
-Regeneration heating coil output energy.
-
-#### Dehumidifier Regeneration Air Speed[m/s]
-
-Regeneration air velocity.
-
-#### Dehumidifier Regeneration Air Mass Flow Rate [kg/s]
-
-Regeneration air mass flow rate.
-
-#### Dehumidifier Process Air Mass Flow Rate [kg/s]
-
-Process air mass flow rate.
-
-### Dehumidifier:Desiccant:System
-
-The Dehumidifier:Desiccant:System object models the dehumidification of an air stream, normally called the process air stream. A second heated air stream, called the regeneration air stream, is used to remove the collected moisture from the desiccant heat exchanger and this moisture-laden air is then usually exhausted from the building. This Dehumidifier:Desiccant:System object is similar to the Dehumidifier:Desiccant:NoFans object but has some additional modeling capabilities.
-
-The Dehumidifier:Desiccant:System object in EnergyPlus is a compound object that can be placed anywhere in an air loop (AirLoopHVAC). Common locations for this object are in an AirLoopHVAC:OutdoorAirSystem or in the main air loop (AirLoopHVAC) downstream of a cooling coil (postcooling desiccant dehumidifier). This compound object coordinates the operation of several    children    objects: a desiccant heat exchanger, a regeneration air fan, and an optional regeneration air heater. Gas, Electric, Steam, or Hot Water heating coils can be used for regenerator air heaters. If this dehumidifier is placed in the main air loop immediately downstream of a direct expansion (DX) cooling coil, then the dehumidifier   s operation can be coordinated with the operation of the companion DX coil and it is also possible to specify that the DX system   s condenser waste heat can be used to help regenerate the desiccant heat exchanger. For the case of condenser waste heat regeneration, an optional exhaust fan can also be modeled by this desiccant dehumidifier compound object to help maintain a set point temperature for air entering the regeneration side of the desiccant heat exchanger.
-
-It is important to note that the optional exhaust air fan is modeled internal to the Dehumidifier:Desiccant:System and a separate fan object should *not* be added to the input data file (idf) for this fan. On the other hand, a separate fan object *is* required in the input data file for the regeneration air fan.
-
-![DesiccantDehumidifier\_DrawThrough](media/image409.png)
-
-Figure 141. Schematic of Dehumidifier:Desiccant:System with Draw Through Regeneration Fan Placement
-
-
-
-A schematic of the compound object Dehumidifier:Desiccant:Systemis shown in Figure 141 with the draw through regeneration air fan placement. Figure 142 shows the Dehumidifier:Desiccant:System object configured with the blow through regeneration air fan placement.
-
-
-
-NOTE: As with any air loop compound object, the Dehumidifier:Desiccant:System object itself is specified on the AirLoopHVAC Branch or in the AirLoopHVAC:OutdoorAirSystem:EquipmentList for an AirLoopHVAC:OutdoorAirSystem. The children objects (e.g., desiccant heat exchanger, regeneration air fan, and optional regeneration air heater) must be specified separately in the input data file and their inlet/outlet connections must be as shown in Figure 141 or Figure 142.
-
-
-
-![DesiccantDehumidifier\_BlowThrough](media/image410.png)
-
-Figure 142. Schematic of Dehumidifier:Desiccant:System with Blow Through Regeneration Fan Placement
-
-Currently the only heat exchanger choice for this object is HeatExchanger:Desiccant: BalancedFlow. So to model a Dehumidifier:Desiccant:System located in an air loop, the input data file should include the following objects:
-
-- Dehumidifier:Desiccant:System (in an air loop (AirLoopHVAC) Branch or AirLoopHVAC:OutdoorAirSystem:EquipmentList for an AirLoopHVAC:OutdoorAirSystem)
-
-- HeatExchanger:Desiccant:BalancedFlow (desiccant heat exchanger child object)
-
-- HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 (desiccant heat exchanger data object)
-
-- ZoneControl:Humidistat, and one of:
-
-- SetpointManager:SingleZone:Humidity:Maximum
-
-- SetpointManager:MultiZone:Humidity:Maximum
-
-- SetpointManager:MultiZone:MaximumHumidity:Average
-
--   (when in an air loop (AirLoopHVAC) Branch), and   SetpointManager:OutdoorAirPretreat (when in an AirLoopHVAC:OutdoorAirSystem) to place a maximum humidity ratio set point on the sensor node, typically the process air outlet node
-
-- Fan:OnOff or Fan:ConstantVolume (regeneration air fan)
-
-- Coil:Heating:Electric or Coil:Heating:Gas (optional regeneration air heater)
-
-- Coil:Cooling:DX:SingleSpeed or Coil:Cooling:DX:TwoStageWithHumidityControlMode (optional companion cooling coil)
-
-
-
-If the user wants to model the Dehumidifier:Desiccant:System in an AirLoopHVAC:OutdoorAirSystem, then the process air path of the dehumidifier should be located in the outdoor air stream and the regeneration air path may be placed in the relief air stream or modeled by the desiccant dehumidifier itself where the first node for the regeneration inlet air stream must be an outdoor air node. If the user wants to model the Dehumidifier:Desiccant:System in an air loop (AirLoopHVAC) Branch, then the process air path of the dehumidifier should be located in the air loop Branch object. For this case, the regeneration air stream is modeled by the desiccant dehumidifier object itself (i.e., not part of an air loop Branch statement) and the first node for the regeneration inlet air stream must be an outdoor air node (ref. Figure 141 or Figure 142).
-
-A description of each input field for this object is provided below:
-
-#### Field: Name
-
-A unique, user-assigned name for a particular Dehumidifier:Desiccant:System. Any reference to this dehumidifier by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the dehumidifier can operate during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the dehumidifier can operate. A value less than or equal to 0 (usually 0 is used) denotes that the dehumidifier will not operate (i.e., no heat exchange will take place and the regeneration air fan does not operate). If the field is blank, the schedule has a value of 1 for all time periods. For the case where companion cooling coil regeneration air heating has been specified, the desiccant dehumidifier   s exhaust fan serves as the condenser air fan for the cooling coil system so this availability schedule will not disable exhaust fan operation.
-
-#### Field: Desiccant Heat Exchanger Object Type
-
-This alpha field contains the type of desiccant heat exchanger used with this dehumidifier. Currently, the only valid choice is HeatExchanger:Desiccant:BalancedFlow.
-
-#### Field: Desiccant Heat Exchanger Name
-
-This alpha field contains the name of the desiccant heat exchanger used with this dehumidifier.
-
-#### Field: Sensor Node Name
-
-This alpha field specifies the name of the air loop node used to control desiccant heat exchanger operation. A set point manager must be used to place a maximum humidity ratio set point on this node (e.g., SetpointManager:SingleZone:Humidity:Maximum or SetpointManager:OutdoorAirPretreat).
-
-#### Field: Regeneration Air Fan Object Type
-
-This alpha field contains the type of regeneration air fan used. Available fan types are Fan:OnOff and Fan:ConstantVolume.
-
-#### Field: Regeneration Air Fan Name
-
-This alpha field contains the name of the regeneration air fan used with this dehumidifier.
-
-#### Field: Regeneration Air Fan Placement
-
-This alpha field specifies the fan configuration used in the desiccant dehumidifier. Valid choices are    BlowThrough    and    DrawThrough   , with a default of    DrawThrough    if this field is left blank.
-
-#### Field: Regeneration Air Heater Object Type
-
-This alpha field contains the type of heating coil used to heat the regeneration air stream. This field may be left blank when no regeneration air heater is required. The hot water and steam heating coils require specifying plant loop, branches, and connector objects to support the heating coils, and are placed on the demand side of the plantloop. The hot water flow modulation through the regeneration air heating coil does not require additional controller or Controller:WaterCoil object. The parent object (Dehumidifier:Desiccant:System) itself provides the "controller" function of modulating water flow. For autosizing regeneration air heating coil the *Design Coil Inlet Air Condition* used is the outdoor air condition if the desiccant system is on the primary air loop, or else if the desiccant system is on outdoor air system then it is the return air condition. The *Design Coil Outlet Air Temperature* is the *Regeneration Inlet Air Setpoint Temperature* specified in the input field below. Valid heating coil choices are:
-
-* Coil:Heating:Electric
-
-* Coil:Heating:Gas
-
-* Coil:Heating:Water
-
-* Coil:Heating:Steam
-
-#### Field: Regeneration Air Heater Name
-
-This alpha field contains the name of the heating coil used to heat the regeneration air stream. This field may be left blank when no regeneration air heater is required.
-
-#### Field: Regeneration Inlet Air Setpoint Temperature
-
-This optional numeric field specifies the regeneration air inlet temperature setpoint in Celsius. The regeneration air heater and/or the companion coil regeneration air heating will be controlled to this temperature to the extent possible. This field may be left blank when no regeneration air heater is required or when control of the exhaust fan used with the companion coil regeneration air heating option is not required. If regeneration air heating coils is autosized, then the value of this input field is used as the *Regeneration Air Heater Design Outlet Air Temperature* for the coil sizing calculation. The default value is 46.0 degrees.
-
-#### Field: Companion Cooling Coil Object Type
-
-This optional alpha field contains the type of companion cooling coil used with this desiccant dehumidifier. The only valid choices are Coil:Cooling:DX:SingleSpeed and Coil:Cooling:DX:TwoStageWithHumidityControlMode.
-
-#### Field: Companion Cooling Coil Name
-
-This optional alpha field contains the name of the companion cooling coil used with this desiccant dehumidifier. This field may be left blank when no companion cooling coil is being modeled.
-
-#### Field: Companion Cooling Coil Upstream of Dehumidifier Process Inlet
-
-This choice field specifies if the companion cooling coil is located immediately upstream of the dehumidifiers process inlet. Valid choices are Yes and No. If Yes is selected, then the outlet air node for the companion cooling coil must be the same as the dehumidifier   s process air inlet node (i.e., the process air inlet node name for the desiccant heat exchanger specified for this desiccant dehumidifier). For this case, the companion cooling coil and the desiccant dehumidifier are assumed to operate    in tandem   ; that is, if the simulation determines that the companion cooling coil is unable to meet the humidity set point specified on the sensor node based on its own operation, then the desiccant dehumidifier operates at the same time and for the same duration as the cooling coil to provide improved dehumidification. If No is selected, then the dehumidifier will control to the humidity set point specified on the sensor node to the extent possible. The default value is No if this field is left blank.
-
-#### Field: Companion Coil Regeneration Air Heating
-
-This choice field determines if the companion cooling coil   s condenser waste heat is used to heat the regeneration inlet air. Valid choices are Yes and No. The default value is No if this field is left blank.
-
-#### Field: Exhaust Fan Maximum Flow Rate
-
-This optional numeric field contains the maximum fan volumetric flow rate for the exhaust fan in cubic meters per second. As noted previously, this exhaust fan is modeled internally by the Dehumidifier:Desiccant:System object and a separate fan object should NOT be specified in the input data file for this fan. This field is used only when a companion cooling coil is specified and the    Companion Coil Regeneration Air Heating    field is set to    Yes   . This field must be used in conjunction with the    Exhaust Fan Maximum Power    and the    Exhaust Fan Power Curve Name    input fields. The model assumes that the exhaust fan will operate as needed to maintain the    Regeneration Inlet Air Setpoint Temperature   , up to the maximum flow rate specified in this input field. If the desiccant dehumidifier is OFF for a simulation timestep but its companion cooling coil is operating and is specified to provide regeneration air heating, then the exhaust fan operates at this maximum air flow rate (i.e., this fan serves as the condenser fan for the companion cooling coil system when regeneration air heating is specified, so the inputs to the companion cooling coil object should not include the condenser fan energy since the condenser fan energy is modeled by the Dehumidifier:Desiccant:System object).
-
-#### Field: Exhaust Fan Maximum Power
-
-This optional numeric field contains the maximum power for the exhaust fan in Watts (i.e., at the Exhaust Fan Maximum Flow Rate). This field is used only when a companion cooling coil is used and the    Companion Coil Regeneration Air Heating    field is set to    Yes   . This field must be used in conjunction with the    Exhaust Fan Maximum Flow Rate    and the    Exhaust Fan Power Curve Name    input fields.
-
-#### Field: Exhaust Fan Power Curve Name
-
-This optional alpha field contains the name of the exhaust fan power modifier curve. This field is used only when a companion cooling coil is used and the    Companion Coil Regeneration Air Heating    field is set to    Yes   . This field must be used in conjunction with the    Exhaust Fan Maximum Flow Rate    and the    Exhaust Fan Maximum Power    input fields. If this field is blank, the exhaust fan operates (when required) at the maximum power specified in the field above. The curve object type for this Exhaust Fan Power Curve Name must be Curve:Cubic or Curve:Quadratic. The curve object (Curve:Cubic or Curve:Quadratic) defines the change in exhaust fan power as a function of the ratio of the actual exhaust air flow rate divided by the maximum flow rate.
-
-Following is an example input for this object:
-
-```idf
-   Dehumidifier:Desiccant:System,
-       Desiccant 1,                         !- Name
-       FanAvailSched,                     !- Availability Schedule Name
-       HeatExchanger:Desiccant:BalancedFlow,   !- Desiccant Heat Exchanger Object Type
-       Desiccant Heat Exchanger 1,   !- Desiccant Heat Exchanger Name
-       HX Process Outlet Node,   !- Sensor Node Name
-       Fan:ConstantVolume,           !- Regeneration Air Fan Object Type
-       Desiccant Regen Fan,         !- Regeneration Air Fan Name
-       DrawThrough,                         !- Regeneration Air Fan Placement
-       Coil:Heating:Gas,               !- Regeneration Air Heater Object Type
-       Desiccant Regen Coil,       !- Regeneration Air Heater Name
-       46.111111,                             !- Regeneration Inlet Air Setpoint Temperature {C}
-       Coil:Cooling:DX:SingleSpeed,   !- Companion Cooling Coil Object Type
-       Desiccant DXSystem Cooling Coil,   !- Companion Cooling Coil Name
-       Yes,                           !- Companion Cooling Coil Upstream of Dehumidifier Process Inlet
-       Yes,                                         !- Companion Coil Regeneration Air Heating
-       1.05,                                       !- Exhaust Fan Maximum Flow Rate {m3/s}
-       50,                                           !- Exhaust Fan Maximum Power {W}
-       EXHAUSTFANPLF;                     !- Exhaust Fan Power Curve Name
-```
-
-
-
-### Desiccant Dehumidifier Outputs
-
-* HVAC,Sum,Dehumidifier Removed Water Mass [kg]
-
-* HVAC,Average,Dehumidifier Removed Water Mass Flow Rate [kg/s]
-
-* HVAC,Average,Dehumidifier Part Load Ratio []
-
-* HVAC,Average,Dehumidifier Exhaust Fan Electric Power [W]
-
-* HVAC,Sum,Dehumidifier Exhaust Fan Electric Energy [J]
-
-#### Dehumidifier Removed Water Mass   [kg]
-
-This output is the mass of water removed from the process air stream in kilograms for the timestep being reported.
-
-#### Dehumidifier Removed Water Mass Flow Rate [kg/s]
-
-This output is the average rate of water removal from the process air stream in kilograms per second for the timestep being reported.
-
-#### Dehumidifier Part Load Ratio [ ]
-
-This output is the fraction of time that the desiccant heat exchanger (and associated regeneration air heater and fans, if appropriate) operate for the timestep being reported.
-
-#### Dehumidifier Exhaust Fan Electric Power [W]
-
-This output is the average electric consumption rate for the exhaust fan in Watts for the timestep being reported.
-
-#### Dehumidifier Exhaust Fan Electric Energy [J]
-
-This output is the electric consumption for the exhaust fan in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, EndUseKey = Cooling, GroupKey = System (ref. Output:Meter objects).
-
-Group     Energy Management System (EMS)
---------------------------------------
-
-The Energy Management System (EMS) is one of the high-level control methods available in EnergyPlus. An EMS is able to access a wide variety of    sensor    data and use this data to direct various types of control actions. The concept is to emulate, inside EnergyPlus, the types of controls possible with the digital energy management systems used in real buildings.
-
-In the hierarchy of EnergyPlus controls, the EMS module is a high-level, generalized, supervisory control for building systems. The EMS replicates the functionality of many of the existing high-level control objects in EnergyPlus. Similar to the AvailabilityManager objects, the EMS can turn on and off pumps and fans. Similar to the DemandManager objects, the EMS can turn on and off lights and electric equipment, change the set points on zone thermostats, and dispatch on-site generation. Similar to the SetpointManager objects, the EMS can change the set points on system nodes. Similar to the PlantEquipmentOperation objects, the EMS can turn on and off supply-side heating, cooling, and heat rejection equipment, i.e., boilers, chillers, cooling towers, etc. Similar to the ElectricLoadCenter:Distribution, the EMS can turn on and off on-site generation equipment.
-
-A separate document called *Application Guide for EMS* contains much more information on how to use the EMS. The EMS uses the EnergyPlus Runtime Language (Erl) for custom programming of control routines.
-
-### EnergyManagementSystem:Sensor
-
-The EnergyManagmentSystem:Sensor object is used to declare an Erl variable that is linked to EnergyPlus output variables or meters. EMS sensors are used to get information from elsewhere in the model for use in control calculations.   The separate output files called eplusout.rdd and eplusout.mdd provide a listing of the output variables and meters that can be used as sensors.
-
-#### Field: Name
-
-This field contains a unique name for the sensor that becomes the name of a variable for use in Erl programs. No spaces are allowed in the object name. This name will be a global variable in Erl programs and cannot duplicate any other global scope Erl variable.
-
-#### Field: Output:Variable or Output:Meter Index Key Name
-
-The key reference for the specified output variable. For example, if System Node Temperature is the output variable, the unique node name is the key. The *Key Name* field should be omitted for weather variables and meters because they do not have a key.
-
-#### Field: Output:Variable or Output:Meter Name
-
-The name of the output variable or meter that is to be mapped to the Erl variable for the sensor. The names that can be used in a specific model are included in the .RDD output file.
-
-Examples of this object follow.
-
-```idf
-EnergyManagementSystem:Sensor,
-     T1, !Name
-     Perimeter_ZN_1 , ! Output:Variable or Output:Meter Index Key Name
-     Zone Mean Air Temperature ; ! Output:Variable or Output:Meter Name
-
-EnergyManagementSystem:Sensor,
-     PMV5, !Name
-     Core_ZN , ! Output:Variable Index Key Name
-     Zone Thermal Comfort Fanger Model PMV ; ! Output:Variable Name
-
-EnergyManagementSystem:Sensor,
-     T_VAV5FanIn, !Name
-     VAV_5_HeatC-VAV_5_FanNode , ! Output:Variable Index Key Name
-     System Node Temperature ; ! Output:Variable Name
-
-EnergyManagementSystem:Sensor,
-     cooling_setpoint,                                   ! Name
-     CLGSETP_SCH ,                 ! Output:Variable Index Key Name
-     Schedule Value ; ! Output:Variable Name
-```
-
-
-### EnergyManagementSystem:Actuator
-
-This object maps an Erl variable to a control actuator elsewhere in EnergyPlus. The EMS then initiates control actions by changing the value of this variable inside an Erl program. The Application Guide for EMS contains much more information on EMS actuators. The eplusout.EDD file can contain a listing of the actuators available for a specific model.
-
-#### Field: Name
-
-The field contains a unique name for the actuator that becomes the name of a variable for use in Erl programs. No spaces are allowed in the object name. This name will be a global variable in Erl programs and cannot duplicate any other global scope Erl variable.
-
-#### Field: Actuated Component Unique Name
-
-This field defines a unique name for the specific entity that is to be controlled. The names for each individual component are listed in the EDD output file when Verbose mode is used     see the input object Output:EnergyManagementSystem for more on the EDD file. These will often be user-defined names of input objects or system nodes, but some actuators are automatically setup by the program and will not be completely user-defined.
-
-#### Field: Actuated Component Type
-
-The field defines the type of the entity that is to be controlled by the actuator. The component types available vary with the specifics of individual models. The types of components that can be used as actuators in a specific model are listed in the EDD output file     see the input object Output:EnergyManagementSystem for more on the EDD file. Components can be object types defined elsewhere in the IDD but there are other types of entities such as nodes and system-level actuators that do not directly correspond to IDF objects.
-
-#### Field: Actuated Component Control Type
-
-This field defines the type of control to be done on the specific entity being controlled. The control types available are listed in the EDD output. Specific components may have more than one type of control available, such as flow rate or temperature, and this field is used to distinguish between them.
-
-Example input objects.
-
-```idf
-  EnergyManagementSystem:Actuator,
-      VAV_5_NightCycleStatus,     ! Name
-      VAV_5,                                       ! Actuated Component Unique Name
-      AirLoopHVAC,                           ! Actuated Component Type
-      Availability Status;           ! Actuated Component Control Type
-
-  EnergyManagementSystem:Actuator,
-      VAV_1_SAT_setpoint,                                       ! Name
-      VAV_1 Supply Equipment Outlet Node ,     ! Actuated Component Unique Name
-      System Node Setpoint,                                   ! Actuated Component Type
-      Temperature Setpoint;                                   ! Actuated Component Control Type
-
-  EnergyManagementSystem:Actuator,
-      myCLGSETP_SCH_Override,                             ! Name
-      CLGSETP_SCH,                                                   !- Actuated Component Unique Name
-      Schedule:Constant,                                       ! Actuated Component Type
-      Schedule Value;                                             ! Actuated Component Control Type
-```
-
-### EnergyManagementSystem:ProgramCallingManager
-
-The EnergyManagementSystem:ProgramCallingManager object is used to specify when individual Erl programs are run. This object manages two temporal aspects of running Erl programs. The first is when they are run relative to the rest of EnergyPlus, and the second is when they are run relative to each other. EMS applications can use multiple EnergyManagementSystem:ProgramCallingManager objects. For example, one manager may execute an initialization program once at the beginning of the run period while additional managers call various sets of programs from different EMS Calling Points.
-
-Control schemes can be organized using a multiple Erl programs and this object this specifies the order in which they are executed. *Program Name 1* is run first, *Program Name 2* is run second, etc. The run order can be important if there are interactions or dependencies between two or more programs. Within each program there may be calls to execute subroutine programs but only calling managers are used to execute main-level programs.
-
-#### Field: Name
-
-This is a unique name for this particular program manager.
-
-#### Field: EnergyPlus Model Calling Point
-
-This field describes when the Erl programs managed under this object are called during an EnergyPlus simulation. All of the programs listed are called at this same calling point. There are 15 possible calling points summarized below. For more information see the section on EMS Calling Points in the Application Guide for EMS.
-
-- BeginNewEnvironment. This calling point occurs near the beginning of each environment period. Environment periods include sizing periods such as design days and run periods. This calling point will not be useful for control actions but is useful for initialization of Erl program variables and other one-time set up actions for EMS.
-
-- AfterNewEnvironmentWarmUpIsComplete. This calling point occurs at the beginning of each environment period but after warm up days are complete. Warm up days are used to condition the transient aspects of the model with the first day before proceeding. This calling point will not be useful for control actions but is useful for re-initializing Erl programs with fresh values after warm up is complete. Programs called from this point might be used to reset counters or summed variables that would change during warmup.
-
-- BeginTimestepBeforePredictor. This calling point happens near the beginning of each timestep but before predictor executes.    Predictor    refers to the step in EnergyPlus modeling where the zone   s thermal loads are calculated. This calling point is useful for controlling components that affect the thermal loads that the systems will be attempting to meet. Programs called from this point might actuate the building envelope or internal gains based on current weather and the results from the previous timestep.
-
-- AfterPredictorBeforeHVACManagers. This calling point happens each timestep just after predictor executes but before the traditional supervisory control models for SetpointManager and AvailabilityManager are called. This calling point is useful for a variety of control actions. However, if there are conflicts, the EMS control actions may be overwritten by the actions of any traditional SetpointManagers or AvailabilityManagers in the model.
-
-- AfterPredictorAfterHVACManagers. This calling point happens each timestep after predictor executes and after the SetpointManager and AvailabilityManager models are called. This calling point is useful for a variety of control actions. However, if there are conflicts, SetpointManager or AvailabilityManager actions may be overwritten by EMS control actions.
-
-- InsideHVACSystemIterationLoop. This calling point happens each HVAC iteration. The HVAC systems solvers iterate to convergence within each timestep and this calling point is inside this iteration loop. This calling point is useful for a variety of control actions. Being inside the interation loop, this calling point has the advantage that input data need not necessarily be lagged from prior timestep results and can, in some cases, improve the accuracy of controls. The disadvantage is that programs may run an excessive number of times slowing down the execution of the program.
-
-- EndOfZoneTimestepBeforeZoneReporting. This calling point happens each zone timestep just before the output reports are updated for zone-timestep variables and meters. This calling point is useful for custom output variables with    Zone    frequency because they will be in sync with the rest of the zone output variables.
-
-- EndOfZoneTimestepAfterZoneReporting. This calling point happens each zone timestep just after the output reports are updated for zone-timestep variables and meters. This calling point is the last one of a timestep and is useful for making control decisions for the next zone timestep using the final meter values for the current zone timestep.
-
-- EndOfSystemTimestepBeforeHVACReporting. This calling point happens each system timestep just before the output reports are updated for HVAC-timestep variables and meters. This calling point is useful for custom output variables with    HVAC    frequency because they will be in sync with the rest of the system output variables.
-
-- EndOfSystemTimestepAfterHVACReporting. This calling point happens each system timestep just after the output reports are updated for HVAC-timestep variables and meters. This calling point is useful for making control decisions for the next system timestep using the final meter values for the current system timestep.
-
-- EndOfZoneSizing. This calling point happens once during each simulation and only if the run is set to do zone sizing. The calling point occurs just after the native zone sizing calculations are completed but before the sizing results are finalized. This calling point is useful for taking the intermediate results of zone sizing calculations and modifying them based on custom calculations.
-
-- EndOfSystemSizing. This calling pont happens once during each simulation and only if the run is set to do system sizing. The calling point occurs just after the native air system sizing calculations are completed but before the sizing results are finalized. This calling point is useful for taking the intermediate results of zone and system sizing calculations and modifying them based on custom calculations.
-
-- AfterComponentInputReadIn. This calling point occurs early in the simulation when   HVAC component   s input data has been processed but before any component-level calculations for automatic sizing. This calling point occurs once for each of the types of HVAC components that have EMS actuators for autosize overrides. This calling point is not directly useful for control actions but is useful for overriding the results of sizing at the component level.
-
-- UserDefinedComponentModel. This calling point occurs when user-defined HVAC and plant component models are called to be simulated.   This calling point is only used for the programs that model custom components.   This calling point differs from the others in that when it is being used the calls to trigger include a reference to a specific EnergyManagementSystem:ProgramCallingManager and only the one manger is executed.
-
-- UnitarySystemSizing.   This calling point occurs when Unitary systems begin their calculations for determining the size values for autosized input fields.   This calling point is used for overriding the autosizing outcomes for unitary systems.   Each unitary system in the simulation will call this point one time.   This calling point is used to override sizing in the following input objects:   AirLoopHVAC:UnitarySystem, AirLoopHVAC:Unitary:Furnace:HeatOnly, AirLoopHVAC:UnitaryHeatOnly, AirLoopHVAC:UnitaryHeatCool,AirLoopHVAC:Unitary:Furnace:HeatCool, AirLoopHVAC:UnitaryHeatPump:AirToAir, and AirLoopHVAC:UnitaryHeatPump:WaterToAir.
-
-#### Field: Program Name 1
-
-The name of the EnergyManagementSystem:Program object that will be the first to run for the calling point.
-
-#### Field: Program Name 2 .. N
-
-The name of the EnergyManagementSystem:Program object that will be the second to run. Additional programs can be listed. The object is automatically extensible to accommodate as many programs as needed.
-
-
-
-IDF examples:
-
-```idf
-EnergyManagementSystem:ProgramCallingManager,
-     Initialize EMS for Run , ! Name
-     BeginNewEnvironment ,       ! EnergyPlus Model Calling Point
-     InitializeMyEMS;                 ! Program Name 1
-
-
-EnergyManagementSystem:ProgramCallingManager,
-     EMS-based Setpoint Managers , ! Name
-     AfterPredictorAfterHVACManagers , ! EnergyPlus Model Calling Point
-     VAV_5_SchedSetpoint , !Program Name 2
-     VAV5MixedAirManagers,
-     VAV_1_SchedSetpoint,
-     VAV1MixedAirManagers,
-     VAV_3_SchedSetpoint,
-     VAV3MixedAirManagers,
-     VAV_2_SchedSetpoint,
-     VAV2MixedAirManagers,
-     CoolSys1_SchedSetpoint,
-     HeatSys1_SchedSetpoint,
-     SHWSys1_SchedSetpoint,
-     VAV_5_NightCycleMGR,
-     VAV_1_NightCycleMGR,
-     VAV_2_NightCycleMGR,
-     VAV_3_NightCycleMGR;
-```
-
-
-### EnergyManagementSystem:Program
-
-The EnergyManagementSystem:Program object is the central processor of the EMS and the primary container for the *EnergyPlus Runtime Language*, or Erl. The EnergyManagementSystem:Program objects are run in the order and point during an EnergyPlus simulation that is specified in an EnergyManagementSystem:ProgramCallingManager object. Multiple EnergyManagementSystem:Program objects are allowed and may interact (or interfere) with each other. The *Application Guide for EMS* provides a comprehensive overview of Erl programming.
-
-The object definition is very simple. There is a name followed by lines of Erl program code.
-
-#### Field: Name
-
-This field is the unique name of the Erl program. The name can be used to call the program to run from another program or subroutine. No spaces are allowed in the name.
-
-#### Field Set:   Program lines 1 to N
-
-Each remaining field contains a single line of code for the *EnergyPlus Runtime Language*, or Erl. Erl is a little programming language with its own syntax. The commas separating fields can be thought of as end of line characters. The *Application Guide for EMS* provides a the details on Erl program code.
-
-Example IDF input objects follow.
-
-```idf
-EnergyManagementSystem:Program,
-   RH_OpeningController ,         ! Name
-   IF ZoneRH &lt; 25,
-       SET MyOpenFactor = 0.0 ,
-   ELSEIF ZoneRH > 60,
-       SET MyOpenFactor = 1.0 ,
-   ELSE,
-       SET MyOpenFactor = (ZoneRH - 25) / (60 - 25),
-   ENDIF;
-
-EnergyManagementSystem:Program,
-     AverageZoneTemps , ! Name
-     SET Zn1vol = 346.0225, ! zone air volume
-     SET Zn2vol = 205.2650, ! zone air volume
-     SET Zn3vol = 346.0225, ! zone air volume
-     SET Zn4vol = 205.2650, ! zone air volume
-     SET Zn5vol = 456.4551, ! zone air volume
-     SET SumNumerator = T1*Zn1vol + T2*Zn2vol + T3*Zn3vol + T4*Zn4vol + T5*Zn5vol,
-     SET SumDenominator = Zn1vol + Zn2vol + Zn3vol + Zn4vol + Zn5vol,
-     SET AverageBuildingTemp = SumNumerator / SumDenominator;
-
-
-EnergyManagementSystem:Program,
-     VAV2MixedAirManagers , ! Name
-     SET VAV_2_CoolC_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV2FanOut - T_VAV2FanIn),
-     SET VAV_2_HeatC_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV2FanOut - T_VAV2FanIn),
-     SET VAV_2_OA_Setpoint = Seasonal_Reset_SAT_Sched - ( T_VAV2FanOut - T_VAV2FanIn);
-```
-
-### EnergyManagementSystem:Subroutine
-
-The EnergyManagementSystem:Subroutine object contains a block of code written in the *EnergyPlus Runtime Language* that can be run from another Erl program. If the subroutine is never called, it will never run by itself. Subroutines are useful for encapsulating code that is called in multiple places. It is also helpful for organizing and structuring code. When the subroutine finishes running, control is returned to the object that called it. See the *Application Guide for EMS* for information on writing Erl programs.
-
-#### Field: Name
-
-The name uniquely identifying the subroutine. The name can be used to call the subroutine to run from a program or another subroutine or even itself. No spaces are allowed in the name.
-
-#### Field set:   Lines 1 to N
-
-Each remaining field contains a single line of code for the *EnergyPlus Runtime Language*, or Erl. Erl is a little programming language with its own special syntax. The commas separating fields can be thought of as end of line characters. The *Application Guide for EMS* contains the details on the rules for Erl program code.
-
-IDF examples:
-
-```idf
-EnergyManagementSystem:Subroutine,
-   Add4ToN,                                                           !- Name
-   SET N = N + 4;                                               !- EnergyPlus Runtime Language
-
-EnergyManagementSystem:Subroutine,
-   manage_ext_lights,                                       !- Name
-   IF inc_solar > 0,                                         !- EnergyPlus Runtime Language
-       SET ext_lights_pwr = Off,
-   ELSE,
-       SET ext_lights_pwr = On,
-   ENDIF;
-
-EnergyManagementSystem:Subroutine,
-   manage_solar_collector,                             !- Name
-   IF Tout_F &lt; 32,                                             !- EnergyPlus Runtime Language
-       SET pump_pwr = On,
-       EXIT,
-   ENDIF,
-   SET delta_T = Tcollector     Ttank,
-   IF delta_T > 0,
-       SET pump_pwr = On,
-   ELSE,
-       SET pump_pwr = Off,
-   ENDIF;
-```
-
-
-### EnergyManagementSystem:GlobalVariable
-
-The EnergyManagementSystem:GlobalVariable object declares one or more global variables that can be accessed by all Erl programs in the EMS. Erl variables declared by the user as sensor and actuators objects are already global variables. Global scope variables are needed to move date in and out of subroutines because Erl does not support passing arguments within such calls. Global scope variables are also needed to pass an Erl variable result to an output variable. Each field in this object names a new global Erl variable.
-
-#### Field: Erl Variable (1..N) Name
-
-The name becomes the global Erl variable name that can be referenced in the *EnergyPlus Runtime Language*. No spaces are allowed in the object name. The name must be unique across all global scope variables including those declared as sensor and actuators and the built-in variables.
-
-IDF examples using this object follow:
-
-```idf
-EnergyManagementSystem:GlobalVariable,
-   global_var;                                                                   !- Name
-
-EnergyManagementSystem:GlobalVariable, Temp_C;
-
-EnergyManagementSystem:GlobalVariable, Temp_F;
-
-EnergyManagementSystem:Subroutine,
-   CalcFahrenheit,                                                           !- Name
-   SET Temp_F = Temp_C * (9/5) + 32;
-
-EnergyManagementSystem:Program,
-    DummyProgram,                                                               !- Name
-   SET Temp_C = Tout,
-   RUN CalcFahrenheit,
-   SET Tout_F = Temp_F,
-   IF Tout_F > 32,
-       RUN FreezeProtect,
-   ENDIF;
-```
-
-
-### EnergyManagementSystem:OutputVariable
-
-The **EnergyManagementSystem:OutputVariable** object creates a custom output variable that is mapped to an EMS variable. These can be declared by an **EnergyManagementSystem:Sensor** object, an **EnergyManagementSystem:Actuator** object, or an **EnergyManagementSystem:GlobalVariable** object, or any local variable in an Erl program. The custom output variable can then be reported to the output file using the standard EnergyPlus output mechanisms such as with the Output:Variable object.
-
-The EnergyManagementSystem:OutputVariable object is a primary way to obtain data from an Erl program and is likely to be essential for developing and debugging programs. This object also provides a powerful mechanism to create custom output variables. See the *Application Guide for EMS* for more information.
-
-#### Field: Name
-
-This field contains the user-defined name for the new output variable. This is the name that will appear in the RDD output file and can be referenced in other input for output such as an Output:Variable object. By convention, the name is in title case for capitalization. Units are provided in the Units field.
-
-#### Field: EMS Variable Name
-
-This field contains the EMS variable name that is to be mapped to the custom output variable. This must be used elsewhere in Erl programs and cannot have spaces.
-
-#### Field: Type of Data in Variable
-
-This field describes the nature of the variable. There are two choices, Averaged or Summed. Averaged variables are state variables such as temperature, power, or flow rate. Summed variables are quantities such as energy that accumulate across time.
-
-#### Field: Update Frequency
-
-This field describes which timestep the variable is associated with. There are two choices, ZoneTimestep or SystemTimestep. Variables that are related to the building or zone loads are generally associated with the zone timestep. Variables that are related to HVAC system operation are generally associated with the system timestep.
-
-#### Field: EMS Program or Subroutine Name
-
-If the EMS variables is a local scope variable, i.e., not declared as a global scope variable, then this field identifies which program uses the variable. The field references the object name of the Erl program or subroutine object. For global variables, this field should be omitted.
-
-#### Field: Units
-
-This field should contain the units for the output variable in standard EnergyPlus units. It does not need to be enclosed in square brackets.
-
-Examples of this object follow.
-
-```idf
-EnergyManagementSystem:OutputVariable,
-     Weighted Average Building Zone Air Temperature, ! Name
-     AverageBuildingTemp, ! EMS Variable Name
-     Averaged, ! Type of Data in Variable
-     ZoneTimeStep , ! Update Frequency
-     ,           ! EMS Program or Subroutine Name
-     C;
-
-
-   EnergyManagementSystem:OutputVariable,
-       Main CW Coil Total Cooling Rate,   !- Name
-       CWcoil1_tot_cool_Power,   !- EMS Variable Name
-       Averaged,                               !- Type of Data in Variable
-       SystemTimestep,                   !- Update Frequency
-       MainCWCoil1_ModelOuput,   !- EMS Program or Subroutine Name
-       W;                                             !- Units
-```
-
-### EnergyManagementSystem:MeteredOutputVariable,
-
-The EnergyManagementSystem:MeteredOutputVariable object creates a custom output variable that is mapped to an EMS variable and is also included in the metering system that EnergyPlus has for aggregating results for different resources across the model.   This object is very similar to EnergyManagementSystem:OutputVariable with the main differences being that only    summed    types of data in the Erl variable and the quantity is to be added to a meter.   This allows for custom output variables that also impact the results for the amount of electricity or gas consumed.
-
-#### Field: Name
-
-This field contains the user-defined name for the new output variable. This is the name that will appear in the RDD and MTD output files and can be referenced in other input for output such as an Output:Variable object. Units are provided in the Units field.
-
-#### Field: EMS Variable Name
-
-This field contains the EMS variable name that is to be mapped to the custom output variable. This must be used elsewhere in Erl programs and cannot have spaces.
-
-#### Field: Update Frequency
-
-This field describes which timestep the variable is associated with. There are two choices, ZoneTimestep or SystemTimestep. Variables that are related to the building or zone loads are generally associated with the zone timestep. Variables that are related to HVAC system operation are generally associated with the system timestep.
-
-#### Field: EMS Program or Subroutine Name
-
-If the EMS variables is a local scope variable, i.e., not declared as a global scope variable, then this field identifies which program uses the variable. The field references the object name of the Erl program or subroutine object. For global variables, this field should be omitted.
-
-#### Field: Resource Type
-
-This field is used to specify the type of resource that the output variable consumes or produces.   The choice here will determine which of the meters the output should be added to when EnergyPlus aggregates results for overall consumption.   The following keywords can be used to choose the type of resource that should be metered:
-
-- **Electricity**, this selects the main meter for electricity consumption, in units of Joules [J],
-
-- **NaturalGas**, this selects the meter for natural gas consumption, in units of Joules [J],
-
-- **Gasoline**, this selects the meter for gasoline consumption, in units of Joules [J],
-
-- **Diesel**, this selects the meter for diesel consumption, in units of Joules [J],
-
-- **Coal**, this selects the meter for coal consumption, in units of Joules [J],
-
-- **FuelOil\#1**, this selects the meter for \#1 Fuel Oil consumption, in units of Joules [J],
-
-- **FuelOil\#2**, this selects the meter for \#2 Fuel Oil consumption, in units of Joules [J],
-
-- **Propane**, this selects the meter for propane consumption, in units of Joules [J],
-
-- **WaterUse**, this selects the meter for overall water consumption, in units of cubic meters [m<sup>3</sup>],
-
-- **OnSiteWaterProduced**, this selects the meter for overall on-site water collection, in units of cubic meters [m<sup>3</sup>],
-
-- **MainsWaterSupply**, this selects the meter for water supplied by utility mains, in units of cubic meters [m<sup>3</sup>],
-
-- **RainWaterCollected**, this selects the meter for water collected from rain, in units of cubic meters [m<sup>3</sup>],
-
-- **WellWaterDrawn**, this selects the meter for water drawn from a local well, in units of cubic meters [m<sup>3</sup>],
-
-- **CondensateWaterCollected**, this selects the meter for water collected from cooling coils as condensate, in units of cubic meters [m<sup>3</sup>],
-
-- **EnergyTransfer**, this selects the general meter for energy transfers, in units of Joules [J],
-
-- **Steam**, this selects the meter for steam energy consumption, in units of Joules [J],
-
-- **DistrictCooling**, this selects the meter for district chilled water energy consumption, in units of Joules [J],
-
-- **DistrictHeating**, this selects the meter for district hot water energy consumption, in units of Joules [J],
-
-- **ElectricityProducedOnSite**, this selects the meter for electricity produced on the site, in units of Joules [J],
-
-- **SolarWaterHeating**, this selects the meter for hot water heating energy from solar collectors, in units of Joules [J], and,
-
-- **SolarAirHeating**, this selects the meter for air heating energy from solar collectors in units of Joules [J],.
-
-#### Field: Group Type
-
-This field is used to specify how the output variable fits into the categorization scheme used by the metering system in EnergyPlus to identify what part of the model is involved.   Metered output variables are classified as being in one of the following general groups:
-
-- **Building**, this category includes all the meters associated with parts of the building that are not related to HVAC or Plant.   This includes internal and exterior services such as lights, electric equipment, exterior lights, etc.
-
-- **HVAC**, this category includes all the meters associated with parts of the HVAC system that are related to air and zone thermal conditioning and ventilation (but not hydronic plant systems). This includes things like fans, air conditioners, furnaces etc.
-
-- **Plant**, this category includes all the meters associated with parts of the hydronic plant system that are related to heating, cooling, service water heating, and heat rejection.   This includes things like boilers, chillers, water heaters, towers, etc.
-
-#### Field: End-Use Category
-
-This field is used to specify the end use category that should be assigned to the resource associated with the output variable.   EnergyPlus reporting includes the breakdown of how resources are used across different end uses.   Metered output variables must be classified as being in one of the following end use categories:
-
-- Heating
-
-- Cooling
-
-- InteriorLights
-
-- ExteriorLights
-
-- InteriorEquipment
-
-- ExteriorEquipment
-
-- Fans
-
-- Pumps
-
-- HeatRejection
-
-- Humidifier
-
-- HeatRecovery
-
-- WaterSystems
-
-- Refrigeration
-
-- OnSiteGeneration
-
-#### Field: End-Use Subcategory
-
-This field is used to specify the end use subcategory that will be assigned to the output variable.   EnergyPlus reporting includes the breakdown of how resources are used across different end uses with added breakdown for the different subcategories within a particular end use.   This user can define his or her own subcategories and enter them in this field.   If left blank, then no subcategory classification is made and the output is included in the general subcategory for the end use category determined in the previous field.
-
-#### Field: Units
-
-This field should contain the units for the output variable in standard EnergyPlus units. It does not need to be enclosed in square brackets.
-
-Examples of this object follow.
-
-```idf
-   EnergyManagementSystem:MeteredOutputVariable,
-       Zone 1 WinAC Electricity Consumption,   !- Name
-       Zone1WinAC_ElectEnergy,   !- EMS Variable Name
-       SystemTimestep,                   !- Update Frequency
-       Zone1_WinAC_ModelOuput,   !- EMS Program or Subroutine Name
-       Electricity,                         !- Resource Type
-       HVAC,                                       !- Group Type
-       Cooling,                                 !- End-Use Category
-       Window Air Conditioners, !- End-Use Subcategory
-       J;                                             !- Units
-```
-
-### EnergyManagementSystem:TrendVariable
-
-The EnergyManagementSystem:TrendVariable object declares a global trend EMS variable that can be accessed by all Erl programs in the EMS. Trend variables store the recent history of the Erl variable they are associated with. The trend data are useful for examining the progression of time series data. The user declares a new trend variable using this object and associates it with another global Erl variable that will be logged. Trend data are pushed into a stack so that the most recent data are always at the beginning of the stack. Once the stack is full, the oldest data are lost from the trend log. Each value in the trend log is for a zone timestep into the past. The first value in the trend is the one from the previous zone time step.
-
-#### Field: Name
-
-The object name becomes the global EMS trend variable name that can be referenced in the *EnergyPlus Runtime Language*. No spaces are allowed in the name. Then name must be unique across all global scope variables including those declared as sensor and actuators and the built-in variables.
-
-#### Field: EMS Variable Name
-
-This field contains the EMS variable name that is to be mapped to the trend variable. This must be a global EMS variable defined elsewhere and cannot have spaces.
-
-#### Field: Number of Timesteps to be Logged
-
-This field describes how much data are to be held in the trend variable. The trended data are held in an array with one value for each data point going back in time. This field determines how many elements are in that array. If there are six timesteps per hour and this field is set to 144, then the trend will contain data for the most recent 24 hours period.
-
-Examples of this object follow.
-
-```idf
-EnergyManagementSystem:TrendVariable,
-     AvgTemptrendLog1,                   !- Name
-     AverageBuildingTemp,             !- EMS Variable Name
-     300;                                             !- Number of Timesteps to be Logged
-
-
-EnergyManagementSystem:TrendVariable,
-     PMVtrendLog1, ,                       !- Name
-     PMV5,                                           !- EMS Variable Name
-     144;                                             !- Number of Timesteps to be Logged
-```
-
-### EnergyManagementSystem:InternalVariable
-
-The EMS also provides a method to obtain static data from elsewhere in the model. Whereas EMS sensors are used for time-varying data, there are also data that describe certain design parameters for the building which may be useful for EMS calculations. A method for accessing internal data is provided as a time saver and means of better generalizing Erl programs for wider applicability. Information needed for this input object is output by EnergyPlus to the eplusout.edd file     see the Output:EnergyManagementSystem input object. The EDD file can list the internal data index keys and types that are available for use with this object. The Application Guide for EMS discusse internal variables in more depth.
-
-#### Field: Name
-
-This field contains a unique name for the internal variable that becomes the name of a variable for use in Erl programs. No spaces are allowed in the name. This name will be a global variable in Erl programs and cannot duplicate any other global scope EMS variable.
-
-#### Field: Internal Data Index Key Name
-
-This field contains the unique identifier for the internal variable. This is usually a name defined by the user elsewhere in an IDF input object. For example, for an internal variable for the floor area of a zone, this would be the name of the zone.
-
-#### Field: Internal Data Type
-
-This field defines the type of internal data source that is to be mapped to the EMS variable. The types of internal source data that can be used as internal variables are listed in the EIO output file whan an input file has any EMS-related objects.
-
-An example of this object follows.
-
-```idf
-EnergyManagementSystem:InternalVariable,
-     Zn1vol,                   !- Name
-     Perimeter_ZN_1,   !- Internal Data Index Key Name
-     Zone Air Volume; !- Internal Data Type
-```
-
-### EnergyManagementSystem:CurveOrTableIndexVariable
-
-The EMS provides a method for reusing curve and table input objects from elsewhere in the model.   Input objects, such as Curve:Cubic, Curve:Biquadratic, or Table:TwoIndependetVariables, are used by various component models to describe performance relationships in a generic way.   By using an EnergyManagementSystem:CurveOrTableIndexVariable input object, these curves and tables can be used in your own Erl programs.   This object sets up an Erl variable that contains an index that points to specific curve or table.   This index variable is then used as the first argument in a call to the built-in function called @CurveValue so that the correct curve or table is evaluated.
-
-#### Field: Name
-
-This field contains a unique name for the index variable that becomes the name of a variable for use in Erl programs. No spaces are allowed in the name. This name will be a global variable in Erl programs and cannot duplicate any other global scope EMS variable.   The variable will be filled by the EMS system to have a value that    points    to the curve or table object named in the following field.
-
-#### Field: Curve or Table Object Name
-
-This field contains the unique name of a Curve:\* or Table:\* object defined elsewhere in the input file.   The Erl variable in the previous field will be filled with the index for the curve or table named here.   The value of this index tracks the order that Curve: and Table: input objects are listed in the input file.
-
-An example IDF object is:
-
-```idf
-   EnergyManagementSystem:CurveOrTableIndexVariable,
-       Curve_Quadratic_Ptr,             !- Name
-       HPACCOOLPLFFPLR_curve;         !- Curve or Table Object Name
-```
-
-### EnergyManagementSystem:ConstructionIndexVariable
-
-The EMS provides actuators for overriding the type of construction used by a surface.   The EnergyManagementSystem:ConstructionIndexVariable input object is used to setup an Erl variable that contains an index that points to specific Construction.   This index variable is then used with a special actuator called    Surface    with the control type    Construction State.   See the Application Guide for EMS for more information on how to use this index variable and the associated actuator.
-
-#### Field: Name
-
-This field contains a unique name for the index variable that becomes the name of a variable for use in Erl programs. No spaces are allowed in the name. This name will be a global variable in Erl programs and cannot duplicate any other global scope EMS variable.   The variable will be filled by the EMS system to have a value that    points    to the Construction object named in the following field.
-
-#### Field: Construction Object Name
-
-This field contains the unique name of a Construction object defined elsewhere in the input file.   The Erl variable in the previous field will be filled with the index for the Construction named here.   The value of this index tracks the order that Construction input objects are listed in the input file.
-
-An example IDF object is:
-
-```idf
-   Construction,
-       TCwindow_25,                               !- Name
-       Clear3PPG,                             !- Outside Layer
-       AIR 3MM,                                 !- Layer 2
-       WO18RT25,                           !- Layer 3
-       AIR 8MM,                                 !- Layer 4
-       SB60Clear3PPG;                     !- Layer 5
-
-
-   EnergyManagementSystem:ConstructionIndexVariable,
-       TCwindow_25,
-       TCwindow_25;
-```
-
-
-Group     ExternalInterface
--------------------------
-
-The ExternalInterface allows coupling EnergyPlus to the Building Controls Virtual Test Bed (BCVTB). It supports the import of Functional Mock-up Units (FMUs) for co-simulation as well as the export of EnergyPlus as a FMU for co-simulation. BCVTB is a software environment that allows expert users to couple different simulation programs for distributed simulation or for a real-time simulation that is connected to a building control system. For example, the BCVTB allows simulation of the building envelope and HVAC system in EnergyPlus and the control logic in MATLAB/Simulink, while exchanging data between the two programs as they simulate. The BCVTB can be downloaded from http://simulationresearch.lbl.gov/bcvtb. A FMU is a component which implements the Functional Mock-up Interface (FMI) standard (http://www.modelisar.com).
-
-### ExternalInterface
-
-This object activates the external interface of EnergyPlus. If the object ExternalInterface is present, then the external interface objects listed below will receive their values from the BCVTB interface or from FMUs at each zone time step. If this object is not present, then the values of these objects will be fixed at the value declared in the    initial value    field of the corresponding object, and a warning will be written to the EnergyPlus error file.
-
-#### Field: Name
-
-The name of the external interface. The only valid entries are **PtolemyServer**, **FunctionalMockupUnitImport**, and **FunctionalMockupUnitExport**.
-
-An example IDF object is:
-
-```idf
-ExternalInterface,                     !- Object to activate the external interface
-  PtolemyServer;                           !- Name of external interface
-```
-
-### Building Controls Virtual Test Bed (BCVTB)
-
-The following objects are designed to couple EnergyPlus with the BCVTB.
-
-### ExternalInterface:Schedule
-
-This input object is similar to Schedule:Compact. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field    initial value.   
-
-#### Field: Name
-
-This field should contain a unique (within all DaySchedules) designation for this schedule. It is referenced by WeekSchedules to define the appropriate schedule values.
-
-#### Field: Schedule Type Limits Name
-
-This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see above), then the restrictions from the referenced object will be used to validate the current field values.
-
-#### Field: Initial Value
-
-This field contains the schedule value that is used during the warm-up period and during the system sizing.
-
-! Cooling schedule. This schedule is set directly by the external interface.
-
-! During warm-up and system-sizing, it is fixed at 24 degC.
-
-```idf
-   ExternalInterface:Schedule,
-       TSetCoo,                                 !- Name
-       Temperature,                         !- ScheduleType
-       24;                                           !- Initial value, used during warm-up
-```
-
-
-
-! Heating schedule. This schedule is set directly by the external interface.
-
-! During warm-up and system-sizing, it is fixed at 20 degC.
-
-```idf
-   ExternalInterface:Schedule,
-       TSetHea,                                 !- Name
-       Temperature,                         !- ScheduleType
-       20;                                           !- Initial value, used during warm-up
-```
-
-### ExternalInterface:Actuator
-
-This object maps a value received from the external interface to an actuator of the Energy Management System. The object is similar to EnergyManagementSystem:Actuator. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field    initial value.   
-
-#### Field: Name
-
-This field contains a unique name for the actuator. No spaces are allowed in the object name. This name will be a global read-only variable in Erl programs and cannot duplicate any other global scope Erl variable.
-
-#### Field: Actuated Component Unique Name
-
-This field defines a unique name for the specific entity that is to be controlled. The names for each individual component are listed in the EDD output file when Verbose mode is used     see the input object **Output:EnergyManagementSystem** for more on the EDD file. These will often be user-defined names of input objects or system nodes, but some actuators are automatically setup by the program and will not be completely user-defined.
-
-#### Field: Actuated Component Type
-
-The field defines the type of the entity that is to be controlled by the actuator. The component types available vary with the specifics of individual models. The types of components that can be used as actuators in a specific model are listed in the EDD output file     see the input object **Output:EnergyManagementSystem** for more on the EDD file. Components can be object types defined elsewhere in the IDD but there are other types of entities such as nodes and system-level actuators that do not directly correspond to IDF objects.
-
-#### Field: Actuated Component Control Type
-
-This field defines the type of control to be done on the specific entity being controlled. The control types available are listed in the EDD output. Specific components may have more than one type of control available, such as flow rate or temperature, and this field is used to distinguish between them.
-
-#### Field: Initial Value
-
-This field contains the initial value. If a value is specified, then this value is used during the warm-up period and the system sizing. If no value is specified, then the actuated component will only be updated once the time stepping starts, i.e., after the warm-up and the system-sizing. This allows, for example, to schedule a setpoint with a Schedule:Compact during warm-up and system-sizing, and then overwrite the value of this schedule during each zone time step based on a feedback control loop that is implemented in the BCVTB.
-
-```idf
-ExternalInterface:Actuator,
-       Zn001_Wall001_Win001_Shading_Deploy_Status,   !- Name
-       Zn001:Wall001:Win001,       !- Actuated Component Unique Name
-       Window Shading Control,   !- Actuated Component Type
-       Control Status,                   !- Actuated Component Control Type
-         ;                                             ! initial value
-```
-
-### ExternalInterface:Variable
-
-This input object is similar to EnergyManagementSystem:GlobalVariable. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field    initial value.    This object can be used to move data into Erl subroutines.
-
-#### Field: Name
-
-This field becomes the global Erl variable name that can be referenced in the EnergyPlus Runtime Language. No spaces are allowed in the object name. The name must be unique across all global scope variables including those declared as sensor and actuators and the built-in variables.
-
-#### Field: Initial Value
-
-This field contains the initial value that is used during the warm-up period and during the system sizing.
-
-```idf
-ExternalInterface:Variable,
-       yShade,                                   !- Name of Erl variable
-       1;                                             !- Initial value
-```
-
-### Functional Mock-up Unit (FMU) Import
-
-The following objects are designed to couple EnergyPlus with FMUs for co-simulation.
-
-### ExternalInterface:FunctionalMockupUnitImport
-
-This object defines the FMU that will be linked to EnergyPlus.
-
-#### Field: FMU File Name
-
-This field contains the name of the FMU file including the extension. The field should include a full path with file name, for best results. The field must be &lt;= 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
-
-#### Field: FMU Timeout
-
-This field contains the communication timeout value in milli-seconds to allow interprocess communication to take place.
-
-#### Field: FMU LoggingOn
-
-This field contains the loggingOn value to enable or disable debug in FMU. If loggingOn=1, debug logging is enabled. If loggingOn=0, debug logging is disabled.
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport,
-       MoistAir.fmu,                       !- FMU File Name
-       15,                                           !- FMU Timeout
-       0;                                             !- FMU LoggingOn
-```
-
-### ExternalInterface:FunctionalMockupUnitImport:From:Variable
-
-This input object maps the names of the output variables of EnergyPlus to the input variables of the FMU.
-
-#### Field: EnergyPlus Key Value
-
-This input object maps the names of the EnergyPlus output variables (**Output:Variable** or **EnergyManagementSystem:OutputVariable**) to the input variables of the FMU.
-
-#### Field: EnergyPlus Variable Name
-
-This field contains the output variable name as defined in the InputOutput Reference. For an **EnergyManagementSystem:OutputVariable**, the EnergyPlus Variable Name is the name of the **EnergyManagementSystem:OutputVariable**   s object.
-
-#### Field: FMU File Name
-
-This field contains the name of the FMU file including the extension. The field should include a full path with file name, for best results. The field must be &lt;= 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
-
-#### Field: FMU Instance Name
-
-This field contains the EnergyPlus instance name of the FMU. See External Interface Application guide for more details.
-
-#### Field: FMU Variable Name
-
-This field contains the name of the variable in the FMU that will be mapped to the corresponding variable in EnergyPlus.
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-       Environment,                         !- EnergyPlus Key Value
-       Site Outdoor Air Drybulb Temperature,       !- EnergyPlus Variable Name
-       MoistAir.fmu,                       !- FMU File Name
-       Model1,                                   !- FMU Instance Name
-       TDryBul;                                 !- FMU Variable Name
-
-
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-       ZONE ONE,                               !- EnergyPlus Key Value
-       Zone Mean Air Temperature, !- EnergyPlus Variable Name
-       MoistAir.fmu,                       !- FMU File Name
-       Model1,                                   !- FMU Instance Name
-       TRooMea;                                 !- FMU Variable Name
-
-
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-       Environment,                         !- EnergyPlus Key Value
-       Site Outdoor Air Relative Humidity,   !- EnergyPlus Variable Name
-       MoistAir.fmu,                       !- FMU File Name
-       Model1,                                   !- FMU Instance Name
-       outRelHum;                             !- FMU Variable Name
-
-
-ExternalInterface:FunctionalMockupUnitImport:From:Variable,
-       ZONE ONE,                               !- EnergyPlus Key Value
-       Zone Air Relative Humidity,   !- EnergyPlus Variable Name
-       MoistAir.fmu,                       !-FMU File Name
-       Model1,                                   !- FMU Instance Name
-       rooRelHum;                             !- FMU Variable Name
-```
-
-### ExternalInterface:FunctionalMockupUnitImport:To:Schedule
-
-This input object is similar to Schedule:Compact. However, during the time stepping, its value is set to the value received from the external interface. During the system sizing, its value is set to the value specified by the field    initial value.   
-
-#### Field: EnergyPlus Variable Name
-
-This field contains a unique (within all Schedules) designation for this schedule in EnergyPlus.
-
-#### Field: Schedule Type Limits Name
-
-This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see above), then the restrictions from the referenced object will be used to validate the current field values.
-
-#### Field: FMU File Name
-
-This field contains the name of the FMU file including the extension. The field should include a full path with file name, for best results. The field must be &lt;= 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
-
-#### Field: FMU Instance Name
-
-This field contains the EnergyPlus instance name of the FMU. See External Interface Application guide for more details.
-
-#### Field: FMU Variable Name
-
-This field contains the name of the variable in the FMU that will be mapped to the schedule in EnergyPlus.
-
-#### Field: Initial Value
-
-This field contains the schedule value that is used during the system sizing.
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport:To:Schedule,
-       FMU_OthEquSen_ZoneOne,     !- EnergyPlus Variable Name
-       Any Number,                           !- Schedule Type Limits Names
-       MoistAir.fmu,                       !- FMU File Name
-       Model1,                                   !- FMU Instance Name
-       QSensible,                             !- FMU Variable Name
-       0;                                             !- Initial Value
-
-
-ExternalInterface:FunctionalMockupUnitImport:To:Schedule,
-       FMU_OthEquLat_ZoneOne,     !- EnergyPlus Variable Name
-       Any Number,                           !- Schedule Type Limits Names
-       MoistAir.fmu,                       !- FMU File Name
-       Model1,                                   !- FMU Instance Name
-       QLatent,                                 !- FMU Variable Name
-       0;                                             !- Initial Value
-```
-
-### ExternalInterface:FunctionalMockupUnitImport:To:Actuator
-
-This object maps a value received from the external interface to an actuator of the Energy Management System. The object is similar to EnergyManagementSystem:Actuator. However, during the warm-up and time stepping, its value is set to the value received from the external interface. During the system sizing, its value is set to the value specified by the field    initial value.   
-
-#### Field: EnergyPlus Variable Name
-
-This field contains a unique name for the actuator. No spaces are allowed in the object name. This name will be a global read-only variable in Erl programs and cannot duplicate any other global scope Erl variable.
-
-#### Field: Actuated Component Unique Name
-
-This field defines a unique name for the specific entity that is to be controlled. The names for each individual component are listed in the EDD output file when Verbose mode is used     see the input object **Output:EnergyManagementSystem** for more on the EDD file. These will often be user-defined names of input objects or system nodes, but some actuators are automatically setup by the program and will not be completely user-defined.
-
-#### Field: Actuated Component Type
-
-The field defines the type of the entity that is to be controlled by the actuator. The component types available vary with the specifics of individual models. The types of components that can be used as actuators in a specific model are listed in the EDD output file     see the input object **Output:EnergyManagementSystem** for more on the EDD file. Components can be object types defined elsewhere in the IDD but there are other types of entities such as nodes and system-level actuators that do not directly correspond to IDF objects.
-
-#### Field: Actuated Component Control Type
-
-This field defines the type of control to be done on the specific entity being controlled. The control types available are listed in the EDD output. Specific components may have more than one type of control available, such as flow rate or temperature, and this field is used to distinguish between them.
-
-#### Field: FMU File Name
-
-This field contains the name of the FMU file including the extension. The field should include a full path with file name, for best results. The field must be &lt;= 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
-
-#### Field: FMU Instance Name
-
-This field contains the EnergyPlus instance name of the FMU. See External Interface Application guide for more details.
-
-#### Field: FMU Variable Name
-
-This field contains the name of the variable in the FMU that will be mapped to the actuator in EnergyPlus.
-
-#### Field: Initial Value
-
-This field contains the value that is used during the system sizing.
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport:To:Actuator,
-Zn001_Wall001_Win001_Shading_Deploy_Status,   !- EnergyPlus Variable Name
-       Zn001:Wall001:Win001,                                 !- Actuated Component Unique Name
-       Window Shading Control,                                   !- Actuated Component Type
-       Control Status,                                             !- Actuated Component Control Type
-       ShadingController.fmu,                                     !- FMU File Name
-       Model1,                                                                   !- FMU Instance Name
-       yShade,                                                                   !- FMU Variable Name
-       6;                                                                             !- Initial Value
-```
-
-### ExternalInterface:FunctionalMockupUnitImport:To:Variable
-
-This input object is similar to EnergyManagementSystem:GlobalVariable. However, during the warm-up and time stepping, its value is set to the value received from the external interface. During the system sizing its value is set to the value specified by the field    initial value.    This object can be used to move data into Erl subroutines.
-
-#### Field: EnergyPlus Variable Name
-
-This field becomes the global Erl variable name that can be referenced in the EnergyPlus Runtime Language. No spaces are allowed in the object name. The name must be unique across all global scope variables including those declared as sensor and actuators and the built-in variables.
-
-#### Field: FMU File Name
-
-This field contains the name of the FMU file including the extension. The field should include a full path with file name, for best results. The field must be &lt;= 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
-
-#### Field: FMU Instance Name
-
-This field contains the EnergyPlus instance name of the FMU. See External Interface Application guide for more details.
-
-#### Field: FMU Variable Name
-
-This field contains the name of the variable in the FMU that will be mapped to the corresponding variable in EnergyPlus.
-
-#### Field: Initial Value
-
-This field contains the initial value that is used during the system sizing.
-
-```idf
-ExternalInterface:FunctionalMockupUnitImport:To:Variable,
-       Shade_Signal,                       !- EnergyPlus Variable Name
-       ShadingController.fmu,     !- FMU File Name
-       Model1,                                   !- FMU Instance Name
-       yShade,                                   !- FMU Variable Name
-       1;                                             !- Initial Value
-```
-
-### Functional Mock-up Unit (FMU) Export
-
-The following objects are designed to support the export of EnergyPlus as a FMU for co-simulation.
-
-### ExternalInterface:FunctionalMockupUnitExport:From:Variable
-
-This object exposes the EnergyPlus output variables (**Output:Variable** or **EnergyManagementSystem:OutputVariable**) to the outside simulation program.
-
-#### Field: EnergyPlus Key Value
-
-This field contains a Key Value for an EnergyPlus output variable (ref Output:Variable/.rdd file). For an **EnergyManagementSystem:OutputVariable**, the EnergyPlus Key Value needs to be set to    **EMS**   .
-
-#### Field: EnergyPlus Variable Name
-
-This field contains the Variable Name as defined in the InputOutput Reference. For an **EnergyManagementSystem:OutputVariable**, the EnergyPlus Variable Name is the name of the **EnergyManagementSystem:OutputVariable**   s object.
-
-#### Field: FMU Variable Name
-
-This field contains the name of the variable in the model description file of the FMU that will be mapped to the corresponding variable in EnergyPlus.
-
-```idf
-ExternalInterface:FunctionalMockupUnitExport:From:Variable,
-       Environment,                         !- EnergyPlus Key Value
-       Site Outdoor Air Drybulb Temperature,   !- EnergyPlus Variable Name
-       TDryBul;                                 !- FMU Variable Name
-
-ExternalInterface: FunctionalMockupUnitExport:From:Variable,
-       ZONE ONE,                                   !- EnergyPlus Key Value
-       Zone Mean Air Temperature, !- EnergyPlus Variable Name
-       TRooMea;                                     !- FMU Variable Name
-
-ExternalInterface: FunctionalMockupUnitExport:From:Variable,
-       Environment,                               !- EnergyPlus Key Value
-       Site Outdoor Air Relative Humidity,   !- EnergyPlus Variable Name
-       outRelHum;                                   !- FMU Variable Name
-
-ExternalInterface:FunctionalMockupUnitExport:From:Variable,
-       ZONE ONE,                                       !- EnergyPlus Key Value
-       Zone Air Relative Humidity,   !- EnergyPlus Variable Name
-       rooRelHum;                                     !- FMU Variable Name
-```
-
-### ExternalInterface:FunctionalMockupUnitExport:To:Schedule
-
-This object is similar to Schedule:Compact. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field    initial value.   
-
-#### Field: EnergyPlus Variable Name
-
-This field contains a unique (within all Schedules) designation for this schedule in EnergyPlus.
-
-#### Field: Schedule Type Limits Name
-
-This field contains a reference to the Schedule Type Limits object. If found in a list of Schedule Type Limits (see above), then the restrictions from the referenced object will be used to validate the current field values.
-
-#### Field: FMU Variable Name
-
-This field contains the name of the variable in the model description file of the FMU that will be mapped to the schedule in EnergyPlus.
-
-#### Field: Initial Value
-
-This field contains the schedule value that is used during the warm-up period and during the system sizing.
-
-```idf
-ExternalInterface:FunctionalMockupUnitExport:To:Schedule,
-       FMU_OthEquSen_ZoneOne,     !- EnergyPlus Variable Name
-       Any Number,                           !- Schedule Type Limits Names
-       QSensible,                             !- FMU Variable Name
-       0;                                             !- Initial Value
-```
-
-### ExternalInterface:FunctionalMockupUnitExport:To:Actuator
-
-This object maps a value received from the external interface to an actuator of the Energy Management System. The object is similar to EnergyManagementSystem:Actuator. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field    initial value.   
-
-#### Field: EnergyPlus Variable Name
-
-This field contains a unique name for the actuator. No spaces are allowed in the object name. This name will be a global read-only variable in Erl programs and cannot duplicate any other global scope Erl variable.
-
-#### Field: Actuated Component Unique Name
-
-This field defines a unique name for the specific entity that is to be controlled. The names for each individual component are listed in the EDD output file when Verbose mode is used     see the input object **Output:EnergyManagementSystem** for more on the EDD file. These will often be user-defined names of input objects or system nodes, but some actuators are automatically setup by the program and will not be completely user-defined.
-
-#### Field: Actuated Component Type
-
-The field defines the type of the entity that is to be controlled by the actuator. The component types available vary with the specifics of individual models. The types of components that can be used as actuators in a specific model are listed in the EDD output file     see the input object **Output:EnergyManagementSystem** for more on the EDD file. Components can be object types defined elsewhere in the IDD but there are other types of entities such as nodes and system-level actuators that do not directly correspond to IDF objects.
-
-#### Field: Actuated Component Control Type
-
-This field defines the type of control to be done on the specific entity being controlled. The control types available are listed in the EDD output. Specific components may have more than one type of control available, such as flow rate or temperature, and this field is used to distinguish between them.
-
-#### Field: FMU Variable Name
-
-This field contains the name of the variable in the model description file of the FMU that will be mapped to the actuator in EnergyPlus.
-
-#### Field: Initial Value
-
-This field contains the initial value. If a value is specified, then this value is used during the warm-up period and the system sizing. If no value is specified, then the actuated component will only be updated once the time stepping starts, i.e., after the warm-up and the system-sizing.
-
-```idf
-ExternalInterface:FunctionalMockupUnitExport:To:Actuator,
-Zn001_Wall001_Win001_Shading_Deploy_Status,   !- EnergyPlus Variable Name
-       Zn001:Wall001:Win001,                                   !- Actuated Component Unique Name
-       Window Shading Control,                               !- Actuated Component Type
-       Control Status,                                               !- Actuated Component Control Type
-       yShade,                                                               !- FMU Variable Name
-       6;                                                                         !- Initial Value
-```
-
-### ExternalInterface:FunctionalMockupUnitExport:To:Variable
-
-This input object is similar to EnergyManagementSystem:GlobalVariable. However, during the time stepping, its value is set to the value received from the external interface. During the warm-up period and the system sizing, its value is set to the value specified by the field    initial value.    This object can be used to move data into Erl subroutines.
-
-#### Field: EnergyPlus Variable Name
-
-This field becomes the global Erl variable name that can be referenced in the EnergyPlus Runtime Language. No spaces are allowed in the object name. The name must be unique across all global scope variables including those declared as sensor and actuators and the built-in variables.
-
-#### Field: FMU Variable Name
-
-This field contains the name of the variable in the model description file of the FMU that will be mapped to the corresponding variable in EnergyPlus.
-
-#### Field: Initial Value
-
-This field contains the initial value that is used during the warm-up period and during the system sizing.
-
-```idf
-ExternalInterface:FunctionalMockupUnitExport:To:Variable,
-       Shade_Signal,                       !- EnergyPlus Variable Name
-       yShade,                                   !- FMU Variable Name
-       1;                                             !- Initial Value
-```
-
-
-Group     User Defined HVAC and Plant Component Models
-----------------------------------------------------
-
-This group of EnergyPlus input objects provides methods for users to include their own custom models for HVAC and plant components as well as plant equipment operation. This is helpful because not every conceivable type of HVAC equipment or system configuration has already had models implemented in EnergyPlus.   HVAC or plant components, or even entire system configurations, might be so new, unusual, or proprietary that no model has yet been implemented in the software.   An analyst faced with project that needs to model such a device or system could do so using one or more of the user defined components described in this section.
-
-Some building energy performance rating systems allow analysts to option of using    exceptional calculation methods    when a simulation program cannot perform the function required to be modeled. These user defined component models are intended to provide a means for including such exceptional calculations within the context of a full EnergyPlus model.   This allows using EnergyPlus for everything it can model and extending it yourself to include a new type of HVAC or Plant component.
-
-These objects are advanced.   Making good use of them requires the user to have a detailed understanding of EnergyPlus HVAC and Plant models as well as the Energy Management System (EMS).   The EnergyPlus Runtime Language (Erl) is used to program the component model.   The Application Guide for EMS provides more discussion of how to use the objects in this group     see the chapter called User-Defined Component Models.
-
-### ZoneHVAC:ForcedAir:UserDefined
-
-This object is used to define a generic zone air unit for custom component models.   This object has a primary air connection that connects to a zone through exhaust and inlet nodes.   There is an optional secondary air connection that can be used as an air-based source or heat rejection connection.   As many has three different plant connections can be made to the zone unit.   Water storage tanks can be connected for supply or collection.   An ambient zone can be connected for skin losses to be treated as separate internal gains.
-
-#### Field: Name
-
-This field defines a unique user-assigned name for an instance of a custom, forced-air zone conditioning unit.   Any reference to this zone unit by another object will use this name.
-
-#### Field: Overall Model Simulation Program Calling Manager Name
-
-This field specifies the Erl programs that are used to model the custom zone unit.   This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere.   The program manager referenced here should include all the Erl programs that are to be run each time the component is simulated and use the calling point called UserDefinedComponentModel.
-
-#### Field: Model Setup and Sizing Program Calling Manager Name
-
-This field specifies the Erl programs that are used to initialize and size the custom zone unit.   This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere and uses the calling point called UserDefinedComponentModel.   The program manager referenced here should include all the Erl programs that are needed to do any initial setup that should occur before the main modeling programs are run.   These include calculating and setting values for things that do not vary over time such as component sizes, control parameters, modeling constants etc.   The user defined component will trigger this calling manager at the beginning of each new environment period.
-
-#### Field: Primary Air Inlet Node Name
-
-This field defines the name of the HVAC system node from which the zone unit draws its inlet air from the zone. This node must be the name of a zone air exhaust node (ref. ZoneHVAC:EquipmentConnection). This field is required.
-
-#### Field: Primary Air Outlet Node Name
-
-This field defines the name of the HVAC system node to which the zone unit sends its outlet air to the zone.   This node must be the name of a zone air inlet node (ref. ZoneHVAC:EquipmentConnection). This field is required.
-
-#### Field: Secondary Air Inlet Node Name
-
-This field defines the name of a HVAC system node from which the zone unit can draw additional air.   This air inlet stream has a variety of possible uses including outdoor air supply for ventilation or a condenser inlet for heat rejection.   This field is optional.
-
-#### Field: Secondary Air Outlet Node Name
-
-This field defines the name of a HVAC system node to which the zone unit can send additional air.   This air outlet stream has a variety of possible uses including outdoor air relief for exhaust or a condenser outlet for heat rejection.   This field is optional.
-
-#### Field: Number of Plant Loop Connections
-
-This fields defines the number of different plant loop connections that the zone unit will use.   Up to three separate loops can be connected if desired.   This field is required.   Enter a 0 if the unit does not use plant at all.
-
-#### Field: Plant Connection 1 Inlet Node Name
-
-This field defines the name of a plant system node from which the zone unit can draw fluid.   This is the inlet to the component model from the first plant loop that is connected to the zone unit.
-
-#### Field: Plant Connection 1 Outlet Node Name
-
-This field defines the name of a plant system node to which the zone unit can send fluid.   This is the outlet from the component model to the first plant loop that is connected to the zone unit.
-
-#### Field: Plant Connection 2 Inlet Node Name
-
-This field defines the name of a plant system node from which the zone unit can draw fluid.   This is the inlet to the component model from the second plant loop that is connected to the zone unit.
-
-#### Field: Plant Connection 2 Outlet Node Name
-
-This field defines the name of a plant system node to which the zone unit can send fluid.   This is the outlet from the component model to the second plant loop that is connected to the zone unit.
-
-#### Field: Plant Connection 3 Inlet Node Name
-
-This field defines the name of a plant system node from which the zone unit can draw fluid.   This is the inlet to the component model from the third plant loop that is connected to the zone unit.
-
-#### Field: Plant Connection 3 Outlet Node Name
-
-This field defines the name of a plant system node to which the zone unit can send fluid.   This is the outlet from the component model to the third plant loop that is connected to the zone unit.
-
-#### Field: Supply Inlet Water Storage Tank Name
-
-This field is used to describe where the zone unit obtains water if it is to be connected to a water storage tank.   This water could be used for evaporative cooling. If a name of a WaterUse:Storage object is used here, then the unit can obtain its water from that tank.   This field is optional.
-
-#### Field: Collection Outlet Water Storage Tank Name
-
-This field is used to describe where the zone unit sends water it has collected if is to be stored in a tank.   This water could be collected from coil condensate.   If a name of a WaterUse:Storage object is used here, then the unit can send water to that tank.   This field is optional.
-
-#### Field: Ambient Zone Name
-
-This field is used to connect ancillary losses from the zone unit to a thermal zone.   The unit may have inefficiencies, leaks, or other non-ideal operation that results in some untended impact on the space surrounding the unit.   These    skin losses    can be assigned to a thermal zone and appear as internal gains for the zone named here.   This does not need to be the same thermal zone as the zone that unit is intended to condition.
-
-An example of this input object follows.
-
-```idf
-ZoneHVAC:ForcedAir:UserDefined,
-     Zone1WindAC,   !- Name
-     Zone 1 Window AC Model Program Manager , !- Overall Model Simulation Program Calling Manager Name
-     Zone 1 Window AC Init Program Manager , !- Model Setup and Sizing Program Calling Manager Name
-     Zone1WindACAirInletNode , !- Primary Air Inlet Node Name
-     Zone1WindACAirOutletNode, !- Primary Air Outlet Node Name
-     Zone1WindACOAInNode,   !- Secondary Air Inlet Node Name
-     Zone1WindACExhNode,   !- Secondary Air Outlet Node Name
-     0 ; !- Number of Plant Loop Connections
-```
-
-### AirTerminal:SingleDuct:UserDefined
-
-This object is used to define a generic single duct air terminal unit for custom component models.   This object has a primary air connection that connects a multi-zone air handler to a zone.   There is an optional secondary air connection that can be used and an air-based source or heat rejection connection.   As many as two different plant connections can be made to the air terminal unit.   Water storage tanks can be connected for supply or collection.   An ambient zone can be connected for skin losses to be treated as separate internal gains.
-
-#### Field: Name
-
-This field defines a unique user-assigned name for an instance of a custom, air terminal unit.   Any reference to this air terminal by another object will use this name.
-
-#### Field: Overall Model Simulation Program Calling Manager Name
-
-This field specifies the Erl programs that are used to model the custom air terminal unit.   This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere.   The program manager referenced here should include all the Erl programs that are to be run each time the component is simulated and use the calling point called UserDefinedComponentModel.
-
-#### Field: Model Setup and Sizing Program Calling Manager Name
-
-This field specifies the Erl programs that are used to initialize and size the custom air terminal unit.   This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere and uses the calling point called UserDefinedComponentModel.   The program manager referenced here should include all the Erl programs that are needed to do any initial setup that should occur before the main modeling programs are run.   These include calculating and setting values for things that do not vary over time such as component sizes, control parameters, modeling constants etc.   The user defined component will trigger this calling manager at the beginning of each new environment period.
-
-#### Field: Primary Air Inlet Node Name
-
-This field defines the name of the HVAC system node from which the air terminal unit draws its inlet air.   This node must be the name of a HVAC system node that is listed in a zone splitter (ref. AirLoopHVAC:ZoneSplitter). This field is required.
-
-#### Field: Primary Air Outlet Node Name
-
-This field defines the name of the HVAC system node to which the air terminal unit sends its outlet air to the zone.   This node must be the name of a zone air inlet node (ref. ZoneHVAC:EquipmentConnection). This field is required.
-
-#### Field: Secondary Air Inlet Node Name
-
-This field defines the name of a HVAC system node from which the air terminal unit can draw additional air.   This air inlet stream has a variety of possible uses including outdoor air supply for ventilation or a condenser inlet for heat rejection.   This field is optional.
-
-#### Field: Secondary Air Outlet Node Name
-
-This field defines the name of a HVAC system node to which the air terminal unit can send additional air.   This air outlet stream has a variety of possible uses including outdoor air relief for exhaust or a condenser outlet for heat rejection.   This field is optional.
-
-#### Field: Number of Plant Loop Connections
-
-This fields defines the number of different plant loop connections that the air terminal unit will use.   Up to two separate loop can be connected if desired.   This field is required.   Enter a 0 if the unit does not use plant at all.
-
-#### Field: Plant Connection 1 Inlet Node Name
-
-This field defines the name of a plant system node from which the air terminal unit can draw fluid.   This is the inlet to the component model from the first plant loop that is connected to the air terminal unit.
-
-#### Field: Plant Connection 1 Outlet Node Name
-
-This field defines the name of a plant system node to which the air terminal unit can send fluid.   This is the outlet from the component model to the first plant loop that is connected to the air terminal unit.
-
-#### Field: Plant Connection 2 Inlet Node Name
-
-This field defines the name of a plant system node from which the air terminal unit can draw fluid.   This is the inlet to the component model from the second plant loop that is connected to the air terminal unit.
-
-#### Field: Plant Connection 2 Outlet Node Name
-
-This field defines the name of a plant system node to which the air terminal unit can send fluid.   This is the outlet from the component model to the second plant loop that is connected to the air terminal unit.
-
-#### Field: Supply Inlet Water Storage Tank Name
-
-This field is used to describe where the air terminal unit obtains water if it is to be connected to a water storage tank.   This water could be used for evaporative cooling. If a name of a WaterUse:Storage object is used here, then the unit can obtain its water from that tank.   This field is optional.
-
-#### Field: Collection Outlet Water Storage Tank Name
-
-This field is used to describe where the air terminal unit sends water it has collected if is to be stored in a tank.   This water could be collected from coil condensate.   If a name of a WaterUse:Storage object is used here, then the unit can send water to that tank.   This field is optional.
-
-#### Field: Ambient Zone Name
-
-This field is used to connect ancillary losses from the air terminal unit to a thermal zone.   The unit may have inefficiencies, leaks, or other non-ideal operation that results in some untended impact on the space surrounding the unit.   These    skin losses    can be assigned to a thermal zone and appear as internal gains for the zone named here.   This does not need to be the same thermal zone as the zone that terminal unit is intended to condition.
-
-An example of this input object follows.
-
-```idf
-AirTerminal:SingleDuct:UserDefined,
-     SPACE1-1 VAV Reheat,   !- Name
-     Space1 ATU Sim Programs , !- Overall Model Simulation Program Calling Manager Name
-     Space1 ATU Init Programs , !- Model Setup and Sizing Program Calling Manager Name
-     SPACE1-1 ATU In Node , !- Primary Air Inlet Node Name
-     SPACE1-1 In Node , !- Primary Air Outlet Node Name
-     ,   !- Secondary Air Inlet Node Name
-     ,   !- Secondary Air Outlet Node Name
-     1,   !- Number of Plant Loop Connections
-     SPACE1-1 Zone Coil Water In Node , !- Plant Connection 1 Inlet Node Name
-     SPACE1-1 Zone Coil Water Out Node; !- Plant Connection 1 Outlet Node Name
-```
-
-### Coil:UserDefined
-
-This object is used to define a generic coil for custom component modeling of a device that processes air as part of an air handeler.   The Coil:UserDefined object appears directly on a Branch object used to define the supply side of an air handler, or in the AirLoopHVAC:OutdoorAirSystem:EquipmentList object used to define outdoor air systems.   This object has one or two air connections and an optional plant connection.   Water storage tanks can be connected for supply or collection.   An ambient zone can be connected for skin losses to be treated as separate internal gains.
-
-#### Field: Name
-
-This field defines a unique user-assigned name for an instance of a custom air coil.   Any reference to this coil by another object will use this name.
-
-#### Field: Overall Model Simulation Program Calling Manager Name
-
-This field specifies the Erl programs that are used to model the custom coil.   This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere.   The program manager referenced here should include all the Erl programs that are to be run each time the component is simulated and use the calling point called UserDefinedComponentModel.
-
-#### Field: Model Setup and Sizing Program Calling Manager Name
-
-This field specifies the Erl programs that are used to initialize and size the custom coil.   This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere and uses the calling point called UserDefinedComponentModel.   The program manager referenced here should include all the Erl programs that are needed to do any initial setup that should occur before the main modeling programs are run.   These include calculating and setting values for things that do not vary over time such as component sizes, control parameters, modeling constants etc.   The user defined component will trigger this calling manager at the beginning of each new environment period.
-
-#### Field: Number of Air Connections
-
-This field defines the number of air loop connections that the coil will use.   The coil must have at least one connection but a second can be used by entering a 2.
-
-#### Field: Air Connection 1 Inlet Node Name
-
-This field defines the name of the HVAC system node from which the coil draws its inlet air for its first air loop connection. This node must be the outlet of the HVAC system component located upstream, if there is one.   This field is required.
-
-#### Field: Air Connection 1 Outlet Node Name
-
-This field defines the name of the HVAC system node to which the coil sends its outlet air for its first air loop connection. This node must be the inlet of the HVAC system component located downstream, if there is one.   This field is required.
-
-#### Field: Air Connection 2 Inlet Node Name
-
-This field defines the name of the HVAC system node from which the coil draws its inlet air for its second air loop connection. This node must be the outlet of the HVAC system component located upstream, if there is one.   This field is optional.
-
-#### Field: Air Connection 2 Outlet Node Name
-
-This field defines the name of the HVAC system node to which the coil sends its outlet air for its second air loop connection. This node must be the inlet of the HVAC system component located downstream, if there is one.   This field is optional.
-
-#### Field: Plant Connection is Used
-
-This field defines whether or not the plant loop connection is going to be used.   Enter a Yes if the coil will use plant, enter No if not.   This field is required.
-
-#### Field: Plant Connection Inlet Node Name
-
-This field defines the name of a plant system node from which the coil can draw fluid.   This is the inlet to the component model from the plant loop that is connected to the coil.
-
-#### Field: Plant Connection Outlet Node Name
-
-This field defines the name of a plant system node to which the coil can send fluid.   This is the outlet from the component model to the plant loop that is connected to the coil.
-
-#### Field: Supply Inlet Water Storage Tank Name
-
-This field is used to describe where the coil obtains water if it is to be connected to a water storage tank.   This water could be used for evaporative cooling. If a name of a WaterUse:Storage object is used here, then the unit can obtain its water from that tank.   This field is optional.
-
-#### Field: Collection Outlet Water Storage Tank Name
-
-This field is used to describe where the coil sends water it has collected if is to be stored in a tank.   This water could be collected from coil condensate.   If a name of a WaterUse:Storage object is used here, then the unit can send water to that tank.   This field is optional.
-
-#### Field: Ambient Zone Name
-
-This field is used to connect ancillary losses from the coil to a thermal zone.   The coil may have inefficiencies, leaks, or other non-ideal operation that results in some untended impact on the space surrounding the unit.   These    skin losses    can be assigned to a thermal zone and appear as internal gains for the zone named here.   For example, this would be the mechanical room where the coil is located, not necessarily one of the zone served by the air handler.
-
-An example of this input object follows.
-
-```idf
-Coil:UserDefined,
-     Main Cooling Coil 1, !- Name
-     Main Cooling Coil Model Program Manager , !- Overall Model Simulation Program Calling Manager Name
-     Main Cooling Coil Init Program Manager , !- Model Setup and Sizing Program Calling Manager Name
-     1 , !- Number of Air Connections
-     Mixed Air Node 1 , !- Air Connection 1 Inlet Node Name
-     Main Cooling Coil 1 Outlet Node , !- Air Connection 1 Outlet Node Name
-     , !- Air Connection 2 Inlet Node Name
-     , !- Air Connection 2 Outlet Node Name
-     Yes , !- Plant Connection is Used
-     Main Cooling Coil 1 Water Inlet Node, !- Plant Connection Inlet Node Name
-     Main Cooling Coil 1 Water Outlet Node; !- Plant Connection Outlet Node Name
-```
-
-Note that the Coil:UserDefined needs to be specifically configured in EnergyManagementSystem:MeteredOutputVariable, in order to be included in the meters such as HeatingCoils:EnergyTransfer.
-
-An example of this input object follows.
-
-```idf
-  EnergyManagementSystem:Program,
-    MainHWCoil1_ModelOuput,  !- Name
-    Set HWcoil1_Water_MdotRequest = Water_MdotRequest,  !- Program Line 1
-    Set HWcoil1_Air_Tout          = Air_Tout,  !- Program Line 2
-    Set HWcoil1_Air_Wout          = Air_Wout,  !- <none>
-    Set HWcoil1_tot_heat_Power    = Tot_heat_Power,  !- <none>
-    Set HWcoil1_tot_heat_Energy   = Tot_heat_Power * SystemTimestep * 3600,  !- <none>
-    Set HWcoil1_Air_MdotOut       = Air_Mdot,  !- <none>
-    Set HWcoil1_Water_Tout        = Water_Tout;!- <none>
-
-  EnergyManagementSystem:MeteredOutputVariable,
-    HWcoil1 tot heat Energy, !- Name
-    HWcoil1_tot_heat_Energy, !- EMS Variable Name
-    SystemTimestep,          !- Update Frequency
-    MainHWCoil1_ModelOuput,  !- EMS Program or Subroutine Name
-    ENERGYTRANSFER,          !- Resource Type
-    System,                  !- Group Type
-    HEATINGCOILS,            !- End-Use Category
-    ,                        !- End-Use Subcategory
-    J;                       !- Units
-```
-
-### PlantComponent:UserDefined
-
-This object is used to define a generic plant component for custom component models.   This object can connect to up to four different plant loops.   There is an optional air connection that can be used as an air-based source or heat rejection connection.   Water storage tanks can be connected for supply or collection.   An ambient zone can be connected for skin losses to be treated as separate internal gains.
-
-The PlantComponent:UserDefined object appears directly on the Branch object used to describe the plant.
-
-#### Field: Name
-
-This field defines a unique user-assigned name for an instance of a custom plant component.   Any reference to this component by another object will use this name.
-
-#### Field: Main Model Program Calling Manager Name
-
-This field specifies the Erl programs that are used to model the plant component any time that the device is called to simulate.   This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere.   The program manager referenced here should include all the Erl programs that are to be run each time the component is simulated and use the calling point called UserDefinedComponentModel.
-
-#### Field: Number of Plant Loop Connections
-
-This fields defines the number of different plant loop connections that the component will use.   Up to four separate loops can be connected if desired.   This field is required.
-
-#### FeildSet: {inlet node name, outlet node name, loading mode, flow request mode, initialization program calling manager, simulation program calling manager.}
-
-Each of the plant loop connections used is defined by a set of 6 input fields that contain and inlet node, and outlet node, a loading mode, a flow request mode, a program calling manager for setup and sizing, and a program calling manager for model calculations that should run when this loop is being simulated.
-
-#### Field: Plant Connection X Inlet Node Name
-
-This field defines the name of a plant system node from which the component can draw fluid.   This is the inlet to the component model from the    x    plant loop that is connected to the component.
-
-#### Field: Plant Connection X Outlet Node Name
-
-This field defines the name of a plant system node to which the component can send fluid.   This is the outlet from the component model to the first plant loop that is connected to the component.
-
-#### Field: Plant Connection X Loading Mode
-
-This field defines the nature of the plant component with respect to how it affects the loads experienced by the    X    plant loop connection. One of the following choices must be selected depending on the purpose of the component model and this particular plant loop connection.
-
-- **DemandsLoad**. This type of loading is used for plant connections that place a load on the loop.
-
-- **MeetsLoadWithPassiveCapacity**.   This type of loading is used for plant connections where the component has some capacity to meet loads but it is not really of the type that could be actively controlled.
-
-- **MeetsLoadWithNominalCapacity**.   This type of loading is used for plant connections where the component has controllable capacity to meet loads and no outlet temperature restrictions.
-
-- **MeetsLoadWithNominalCapacityLowOutLimit**.   This type of loading is used for plant connections where the component has controllable capacity to meet loads but with a lower limit on the fluid temperature at the outlet node.
-
-- **MeetsLoadWithNominalCapacityHiOutLimit**.   This type of loading is used for plant connections where the component has controllable capacity to meet loads but with an upper limit on the fluid temperature at the outlet node.
-
-#### Field: Plant Connection X Loop Flow Request Mode
-
-This field defines the nature of the plant component with respect to how it affects the overall flow rate for the loop. One of the following three choices must be made depending on the nature of the plant component and this particular loop connection.
-
-- **NeedsFlowIfLoopOn**.   Devices with this flow request mode will contribute to the overall loop flow rate but will not initiate flow themselves.
-
-- **NeedsFlowAndTurnsLoopOn**.   Devices with this flow request mode will contribute to the overall loop flow rate and initiate flow.
-
-- **ReceivesWhateverFlowAvailable**.   Devices with this flow request mode will not contribute to the overall loop flow rate and do not initiate flow themselves.
-
-#### Field: Plant Connection X Initialization Program Calling Manager Name
-
-This field specifies the Erl programs that are used to model the plant component and should execute when the component is called to simulate by this particular loop connection.   This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere.   The program manager referenced here should include all the Erl programs that are to be run for this    X    plant loop connection and use the calling point called UserDefinedComponentModel.
-
-#### Field: Plant Connection X Simulation Program Calling Manager Name
-
-This field specifies the Erl programs that are used to initialize and size the plant component with regard to this particular plant connection.   This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere and uses the calling point called UserDefinedComponentModel.   The program manager referenced here should include all the Erl programs that are needed to do any initial setup that should occur before the main modeling programs are run.   These include calculating and setting values for things that do not vary over time such as component sizes, control parameters, modeling constants etc.   The user defined component will trigger this calling manager during the intitial setup routines for plant systems.
-
-#### Field: Air Connection Inlet Node Name
-
-This field defines the name of the HVAC system node from which the plant component draws its inlet air for its air loop connection.   This field is optional.
-
-#### Field: Air Connection Outlet Node Name
-
-This field defines the name of the HVAC system node to which the plant component sends its outlet air for its air loop connection.   This field is optional.
-
-#### Field: Supply Inlet Water Storage Tank Name
-
-This field is used to describe where the plant component obtains water if it is to be connected to a water storage tank.   This water could be used for evaporative cooling. If a name of a WaterUse:Storage object is used here, then the component can obtain its water from that tank.   This field is optional.
-
-#### Field: Collection Outlet Water Storage Tank Name
-
-This field is used to describe where the plant component sends water it has collected if is to be stored in a tank.   This water could be collected from coil condensate.   If a name of a WaterUse:Storage object is used here, then the unit can send water to that tank.   This field is optional.
-
-#### Field: Ambient Zone Name
-
-This field is used to connect ancillary losses from the plant component to a thermal zone.   The component may have inefficiencies, leaks, or other non-ideal operation that results in some untended impact on the space surrounding the device.   These    skin losses    can be assigned to a thermal zone and appear as internal gains for the zone named here.   For example, this would be the mechanical room where the plant component is located.
-
-An example of this input object follows:
-
-```idf
-PlantComponent:UserDefined,
-     Central Chiller,   !- Name
-     , !- Main Model Program Calling Manager Name
-     1 ,   !- Number of Plant Loop Connections
-     Central Chiller Inlet Node,     !- Plant Connection 1 Inlet Node Name
-     Central Chiller Outlet Node , !- Plant Connection 1 Outlet Node Name
-     MeetsLoadWithNominalCapacityLowOutLimit, !- Plant Connection 1 Loading Mode
-     NeedsFlowIfLoopOn , !- Plant Connection 1 Loop Flow Request Mode
-     Chiller model init programs, !- Plant Connection 1 Initialization Program Calling Manager Name
-     Chiller model simulation programs ,!- Plant Connection 1 Simulation Program Calling Manager Name
-     , !- Plant Connection 2 Inlet Node Name
-     , !- Plant Connection 2 Outlet Node Name
-     , !- Plant Connection 2 Loading Mode
-     , !- Plant Connection 2 Loop Flow Request Mode
-     , !- Plant Connection 2 Initialization Program Calling Manager Names
-     , !- Plant Connection 2 Simulation Program Calling Manager Name
-     , !- Plant Connection 3 Inlet Node Name
-     , !- Plant Connection 3 Outlet Node Name
-     , !- Plant Connection 3 Loading Mode
-     , !- Plant Connection 3 Loop Flow Request Mode
-     , !- Plant Connection 3 Initialization Program Calling Manager Name
-     , !- Plant Connection 3 Simulation Program Calling Manager Name
-     , !- Plant Connection 4 Inlet Node Name
-     , !- Plant Connection 4 Outlet Node Name
-     , !- Plant Connection 4 Loading Mode
-     , !- Plant Connection 4 Loop Flow Request Mode
-     , !- Plant Connection 4 Initialization Program Calling Manager Name
-     , !- Plant Connection 4 Simulation Program Calling Manager Name
-     Central Chiller Condenser Inlet Node, !- Air Connection Inlet Node Name
-     Central Chiller Condenser Outlet Node, !- Air Connection Outlet Node Name
-     , !- Supply Inlet Water Storage Tank Name
-     , !- Collection Outlet Water Storage Tank Name
-     ; !- Ambient Zone Name
-```
-
-
-### PlantEquipmentOperation:UserDefined
-
-This object is used to define a generic plant equipment operation scheme.   The PlantEquipmentOperation:UserDefined object appears directly in either a PlantEquipmentOperationSchemes or a CondenserEquipmentOperationSchemes object.   The user can configure exactly how supply side equipment is dispatched to meet loads by writing EnergyPlus Runtime Language programs and using the EMS features.   There are no output variables specifically associated with this object but the outcome of load distribution actuators can be examined using the output variable called Plant Component Distributed Demand Rate.
-
-#### Field: Name
-
-This field specifies the unique user-assigned name of the custom operation scheme.
-
-#### Field: Main Model Program Calling Manager Name
-
-This field specifies the Erl programs that are used to model the custom plant operation scheme.   The field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere.   The program manager referenced here should include all the Erl programs that are to be run each time the operation scheme is simulated and use the calling point called UserDefinedComponentModel.
-
-#### Field: Initialization Program Calling Manager Name
-
-This field specifies the Erl programs that are used to initialize and do an one-time setup needed for the custom operation scheme. This field should contain the name of an EnergyManagementSystem:ProgramCallingManager that is defined elsewhere and uses the calling point called UserDefinedComponentModel. The program manager referenced here should include all the Erl programs that are needed to do any initial setup that should occur before the main programs are run. These include calculating and setting values for things that do not vary over time such as component capacities, control range parameters, various constants etc.   The user defined operation scheme will trigger this calling manager at the beginning of each new environment period.
-
-#### Field Set: (Equipment Object Type, Equipment Name)
-
-Up to ten pairs of fields can be used to define the equipment governed by this custom operation scheme.
-
-#### Field: Equipment &lt;\#&gt; Object Type
-
-This field specifies the type of equipment, or object name, for each machine to be controlled by the scheme.
-
-#### Field: Equipment &lt;\#&gt; Name
-
-This field specifies the user selected name of the equipment to be controlled by the scheme.
-
-The following example shows control of a chilled water plant with two chillers that have different sizes and load dispatch is scaled so that each chiller runs at the same part load ratio.
-
-```idf
-PlantEquipmentOperation:UserDefined,
-  CoolSys1 Operation Scheme,  !- Name
-  Cooling_dispatch , !- Main Model Program Calling Manager Name
-  Init_Chiller_Capacity, !- Initialization Program Calling Manager Name
-  Chiller:Electric:ReformulatedEIR, !- Equipment 1 Object Type
-  CoolSys1 Chiller 1,    !- Equipment 1 Name
-  Chiller:Electric:ReformulatedEIR,* !- Equipment 2 Object Type
-  CoolSys1 Chiller 2;    !- Equipment 2 Name
-
-EnergyManagementSystem:ProgramCallingManager,
-  Init_Chiller_Capacity,
-  UserDefinedComponentModel,
-  Init_Chiller_Capacity_Values;
-
-EnergyManagementSystem:Program,
-  Init_Chiller_Capacity_Values,
-  Set totChilCap = Chil1_Cap + Chil2_Cap;
-
-EnergyManagementSystem:GlobalVariable,
-  totChilCap;
-
-EnergyManagementSystem:ProgramCallingManager,
-  Cooling_dispatch,
-  UserDefinedComponentModel,
-  Cooling_dispatch_Values;
-
-EnergyManagementSystem:Program,
-  Cooling_dispatch_Values,
-  IF CoolSys1_LoopDmnd &lt; 0.0,
-    Set UniformPLR* = CoolSys1_LoopDmnd / totChilCap,
-    Set UniformPLR* =* @min UniformPLR 1.0,
-    SET Chil1_Disptch = UniformPLR\*Chil1_Cap,
-    SET Chil2_Disptch = UniformPLR\*Chil2_Cap,
-  ELSE,
-    SET Chil1_Disptch = 0.0 ,
-    SET Chil2_Disptch = 0.0 ,
-  ENDIF;
-
-EnergyManagementSystem:InternalVariable, CoolSys1_LoopDmnd,CoolSys1 Operation Scheme,Supply Side Current Demand Rate; !,[W]
-
-EnergyManagementSystem:InternalVariable, Chil1_Cap, CoolSys1 Chiller 1, Chiller Nominal Capacity;
-
-EnergyManagementSystem:InternalVariable, Chil2_Cap, CoolSys1 Chiller 2, Chiller Nominal Capacity;
-
-EnergyManagementSystem:Actuator, Chil1_Disptch,CoolSys1 Operation Scheme:CoolSys1 Chiller 1,Plant Equipment Operation,Distributed Load Rate; ! [W]
-
-EnergyManagementSystem:Actuator, Chil2_Disptch,CoolSys1 Operation Scheme:CoolSys1 Chiller 2,Plant Equipment Operation,Distributed Load Rate; ! [W]
-```
-
-
-Group     System   Availability Managers
--------------------------------------
-
-System Availability Managers are one of the high-level control constructs in EnergyPlus. A System Availability Manager is able to access data from any of the HVAC system nodes and use this data to to make a decision on whether an entire AirLoopHVAC or PlantLoop should be on or off. Some of the zone component objects   (e.g. unit heater, unit ventilator, packaged terminal air conditioner, packaged terminal heat pump, zone water source heat pump,window air conditioner, zone terminal unit (variable refrigerant flow), energy recovery ventilator, outdoor air unit, fan coil unit, and ventilated slab) can also individually use availability managers to make a decision regarding whether their fan should be on or off.
-
-System Availability Managers are executed at the start of each HVAC timestep. They reside outside the HVAC system iteration loops. Thus, the System Availability Managers are executed once per HVAC timestep, and they use previous timestep information (except for zone load) to calculate their set points.
-
-Some of the managers monitor the temperature at an air or plant node to determine whether the system should be on or off. If the system is to be controlled on the outdoor dry-bulb temperature, an OutdoorAir:NodeList object can be used to define a node which will have the current outdoor air conditions.
-
-The output from each System Availability Manager is an availability status flag. This flag can have the values *NoAction*, *ForceOff*, *CycleOn*, or *CycleOnZoneFansOnly*. The availability status flags for the System Availability Managers referenced by an air or plant loop are used to set the availability status flag for each loop. For the air loops and zone components, *ForceOff* takes precedence: if any of the loop   s (or zone component   s) availability managers are showing status *ForceOff*, the loop (or zone component fan) status will be *ForceOff*. Next in precedence is *CycleOnZoneFansOnly* (only for air loop), followed by *CycleOn,* and *NoAction*. For the plant loops, there is no precedence among the System Availability Manager status flag values. Instead, the first availability manager giving a status flag value other than *NoAction* sets the status for the loop. The System Availability Managers are executed in AvailabilityManagerAssignmentList order.
-
-The actual action of turning on or off a loop is taken by the loop prime movers: fans for AirLoopHVACs and zone components, and pumps for plant loops. For instance when a fan is deciding whether it is on or off, it checks its on/off schedule and whether the loop availability status flag is *CycleOn* or *ForceOff*. If the schedule is on and the status flag is *ForceOff*, the fan will be off. If the fan schedule says off and the status flag is *CycleOn*, the fan will be on. Thus the availability managers overrule the fan on/off schedule. The availability managers, air loops, and plant loops all have output variables which may be used to verify the action of the loop.
-
-Availability managers for AirLoopHVAC systems also control the availability of zone exhaust fans (Ref. Fan:ZoneExhaust) and terminal unit fans (Ref. AirTerminal:SingleDuct:SeriesPIU: Reheat, AirTerminal:SingleDuct:ParallelPIU:Reheat, and AirTerminal:SingleDuct:VAV: Reheat:VariableSpeedFan) in the zones served by the AirLoopHVAC system.
-
-### AvailabilityManager:Scheduled
-
-The simplest System Availability Manager is when the availability is determined by an on/off schedule.The syntax for implementing such an availability manager is shown below. The identifying name refers back to the name recorded in the AvailabilityManagerAssignmentList statement described in the **Group     Air Distribution** section. The schedule must be the name of a schedule defined elsewhere in the input.
-
-#### Field: Name
-
-The unique, user-assigned name of an instance of a scheduled availability manager. Other objects that use this scheduled availability manager will reference it by this name.
-
-#### Field: Schedule Name
-
-The name of a schedule defined elsewhere in the input. Schedule values greater than zero (usually 1 is used) indicate that the system is on. Schedule values less than or equal to zero (usually 0 is used) denote that the system is off. This schedule overides the central fan schedule for determining whether the fan is on.
-
-An example of this statement in an IDF is:
-
-```idf
-AvailabilityManager:Scheduled,
-       VAV Sys 1 Avail, !- Name
-       FanAvailSched;     !- Schedule Name
-```
-
-AvailabilityManager:Scheduled Outputs
-
-The scheduled availability manager has one output variable.
-
-* HVAC,Average,Availability Manager Scheduled Control Status
-
-#### Availability Manager Scheduled Control Status
-
-A value of 1 indicates the manager is signaling *ForceOff*. A value of 2 means the manager is signaling *CycleOn*.
-
-### AvailabilityManager:ScheduledOn
-
-The Schedule On Availability Manager is used when equipment must be turned on during a given time period. This availability manager will not turn the equipment off, a separate availability manager must be used to disable the equipment as necessary. The scheduled on availability is determined by an on schedule. Schedule values other than 0 set a *CycleOn* availability status. Schedule values equal to 0 set a *NoAction* availability status. The syntax for implementing such an availability manager is shown below. The identifying name refers back to the name recorded in the AvailabilityManagerAssignmentList statement described in the **Group     Air Distribution** section. The schedule must be the name of a schedule defined elsewhere in the input.
-
-#### Field: Name
-
-The unique, user-assigned name of an instance of a scheduled on availability manager. Other objects that use this scheduled on availability manager will reference it by this name.
-
-#### Field: Schedule Name
-
-The name of a schedule defined elsewhere in the input. Schedule values greater than zero (usually 1 is used) indicate that the system is on. Schedule values less than or equal to zero (usually 0 is used) denote that *NoAction* is desired. This schedule overides the central fan schedule for determining whether the fan is on.
-
-An example of this statement in an IDF is:
-
-```idf
-AvailabilityManager:ScheduledOn,
-       VAV Sys 1 Avail On,   !- Name
-       FanAvailSched;             !- Schedule Name
-```
-
-### AvailabilityManager:ScheduledOn Outputs
-
-The scheduled on availability manager has one output variable.
-
-* HVAC,Average,Availability Manager Scheduled On Control Status
-
-#### Availability Manager Scheduled On Control Status []
-
-A value of 0 indicates the manager is signaling *NoAction*. A value of 2 means the manager is signaling *CycleOn*.
-
-### AvailabilityManager:ScheduledOff
-
-The Schedule Off Availability Manager is used when equipment must be turned off during a given time period. This availability manager will not turn the equipment on, a separate availability manager must be used to enable the equipment as necessary. The scheduled off availability is determined by an off schedule. Schedule values equal to 0 set a *ForceOff* availability status. Schedule values other than 0 (usually a 1 is used) set a *NoAction* availability status. The syntax for mplementing such an availability manager is shown below. The identifying name refers back to the name recorded in the AvailabilityManagerAssignmentList statement described in the **Group     Air Distribution** section. The schedule must be the name of a schedule defined elsewhere in the input.
-
-#### Field: Name
-
-The unique, user-assigned name of an instance of a scheduled off availability manager. Other objects that use this scheduled off availability manager will reference it by this name.
-
-#### Field: Schedule Name
-
-The name of a schedule defined elsewhere in the input. Schedule values equal to zero indicate that the system is off. Schedule values other than (usually 0 is used) denote that *NoAction* is desired.
-
-An example of this statement in an IDF is:
-```idf
-AvailabilityManager:ScheduledOff,
-       VAV Sys 1 Avail Off,     !- Name
-       FanAvailSched;                 !- Schedule Name
-```
-
-### AvailabilityManager:ScheduledOff Outputs
-
-The scheduled off availability manager has one output variable.
-
-* HVAC,Average,Availability Manager Scheduled Off Control Status
-
-#### Availability Manager Scheduled Off Control Status []
-
-A value of 0 indicates the manager is signaling *NoAction*. A value of 1 means the manager is signaling *ForceOff*.
-
-### AvailabilityManager:NightCycle
-
-This manager is used for cycling on an air system when one or more zones become too hot or too cold. The usual situation is that the central air handler is turned off at night. However if the building gets too cold there might be condensation on the walls and other damage. Thus the control system is usually programmed to turn the system on if 1 control thermostat or any thermostat shows a zone temperature of less than a night time set point. Similarly there might be a concern about a building getting too hot. Again the control system is programmed to turn the air handler back on if one or any zone temperature exceeds a night time cooling set point.
-
-This object gives the user considerable flexibility in determining how the night time on/off decision will be made. The manager can look at the temperature in 1 zone or it can sample all the zones connected to the air handler. The user can specify a temperature tolerance and a run time for the system once it switches on. There is also an applicability schedule     the user can schedule whether or not this availability manager itself is being applied.
-
-***Field: Name***
-
-A unique, user-assigned name for an instance of a night cycle availability manager. Other objects that use this availability manager will reference it by this name.
-
-***Field: Applicability Schedule Name***
-
-The name of a schedule defined elsewhere in the input file. This schedule determines whether or not for a given time period this availability manager is to be applied. Schedule values greater than zero (usually 1 is used) indicate the availability manager is to be applied. Schedule values less than or equal to zero (usually 0 is used) denote that the availability manager is not used for this time period.
-
-***Field: Fan Schedule Name***
-
-The name of the central fan on/off schedule for the air system that this availability manager will affect.
-
-***Field: Control Type***
-
-The possible inputs are *StayOff*, *CycleOnAny*, *CycleOnControlZone*, *CycleOnAnyZoneFansOnly*. *StayOff* means the availability manager will have no effect     air handler on/off will be determined by the fan schedule. *CycleOnAny* means that if any zone served by a system whose AvailabilityManagerAssignmentList references this system availability manager has an air temperature outside the cooling or heating set points the central fan will turn on even though the fan schedule indicates the fan is off. *CycleOnControlZone* means the same thing except the availability manager looks at the temperature in only one zone. *CycleOnAnyZoneFansOnly* is the same as *CycleOnAny* except that only the zone fans are cycled on and the central air handler fan is left off. The default is *StayOff*.
-
-***Field: Thermostat Tolerance***
-
-The Thermostat Tolerance defines the amount by which the zone temperature must fall outside the current zone heating and cooling setpoints for the Night Cycle manager to turn the system on. The zone temperature must exceed the cooling set point or fall below the heating set point by 1/2 the Thermostat Tolerance in order for the availability manager to signal that the system should turn on. The Thermostat Tolerance is specified in degrees Celsius. The default is 1 degree C.
-
-***Field: Cycling Run Time***
-
-The time in seconds for which the system will run after it has cycled on. The default is 3600 seconds (1 hour).
-
-***Field: Control Zone Name***
-
-For the option *CycleOnControlZone* this is the name of the control zone.
-
-An example of this statement in an IDF is:
-
-```idf
-AvailabilityManager:NightCycle,
-      VAV Sys 1 Avail,         ! Name
-       SysAvailApplicSch,     !Applicability Schedule Name
-       FanAvailSched,             ! Fan Schedule Name
-       CycleOnAny,                   ! Control Type
-       4.0,                                 ! Temperature Tolerance {delta C}
-       7200.;                             ! Cycle Run Time {s}
-```
-
-### AvailabilityManager:NightCycle Outputs
-
-The night cycle availability manager has one output variable.
-
-* HVAC,Average,Availability Manager Night Cycle Control Status
-
-#### Availability Manager Night Cycle Control Status
-
-A value of 0 indicates the manager is signaling *NoAction*. A value of 2 means the manager is signaling *CycleOn*. A value of 3 says that the manager is signaling *CycleOnZoneFansOnly*.
-
-### AvailabilityManager:DifferentialThermostat
-
-The differential thermostat compares the temperatures at two different system nodes. If the temperature difference (DT) is above the *Temperature Difference On Limit*, the system is turned on. If the DT is below the *Temperature Difference Off Limit*, the system is turned off. Between the *On Limit* and *Off Limit* the system is either on or off depending on the previous state of the thermostat. Unlike other availability managers, the differential thermostat is always either "On" or "Off"; it does not use the "No Action" state. Therefore, the differential thermostat must be the last manager in the AvailabilityManagerAssignmentList. Any availability managers after the differential thermostat manager will never be simulated.
-
-One application of the differential thermostat is to ensure a useful heat gain for solar heating systems, i.e. the system is only turned on when there is a significant temperature difference between the solar collector outlet node and the storage tank outlet node.
-
-#### Field: Name
-
-The name of the object. This is referenced in the AvailabilityManagerAssignmentList.
-
-#### Field: Hot Node Name
-
-The sensor node with the higher temperature.
-
-#### Field: Cold Node Name
-
-The sensor node with the colder temperature.
-
-#### Field: Temperature Difference On Limit
-
-Temperature difference [deltaC] between hot and cold nodes necessary to turn the system on.
-
-#### Field: Temperature Difference Off Limit
-
-Temperature difference [deltaC] between hot and cold nodes necessary to turn the system off. This field defaults to the *Temperature Difference On Limit*.
-
-An example of this object in an IDF is:
-
-```idf
-AvailabilityManager:DifferentialThermostat,
-   Differential Thermostat Availability Manager,   !- Name
-   Collector Outlet Node,                       !- Hot Node Name
-   Water Heater Source Outlet Node,   !- Cold Node Name
-   10.0,   !- Temperature Difference On Limit {delta C}
-   2.0;     !- Temperature Difference Off Limit {delta C}
-```
-
-
-### AvailabilityManager:DifferentialThermostat Outputs
-
-The differential thermostat availability manager has one output variable.
-
-* HVAC,Average,Availability Manager Differential Thermostat Control Status
-
-#### Availability Manager Differential Thermostat Control Status
-
-A value of 1 indicates the manager is signaling *ForceOff*. A value of 2 means the manager is signaling *CycleOn*.
-
-### AvailabilityManager:HighTemperatureTurnOff
-
-This manager turns the system off if the temperature at the sensor node is above the specified setpoint temperature.
-
-#### Field: Name
-
-The name of the object. This is referenced in the AvailabilityManagerAssignmentList.
-
-#### Field: Sensor Node Name
-
-The air or plant node where the temperature is monitored.
-
-#### Field: Temperature
-
-The setpoint temperature [C] at which the system is turned off.
-
-An example of this object in an IDF is:
-
-```idf
-AvailabilityManager:HighTemperatureTurnOff,
-   High Temperature Turn Off Availability Manager,   !- Name
-   Water Heater Use Outlet Node,   !- Sensor Node Name
-   60.0;   !- Temperature {C}
-```
-
-### AvailabilityManager:HighTemperatureTurnOff Outputs
-
-The high temperature turn off availability manager has one output variable.
-
-* HVAC,Average,Availability Manager High Temperature Turn Off Control Status
-
-#### Availability Manager High Temperature Turn Off Control Status []
-
-A value of 0 indicates the manager is signaling *NoAction*. A value of 1 means the manager is signaling *ForceOff.*
-
-### AvailabilityManager:HighTemperatureTurnOn
-
-This manager turns the system on if the temperature at the sensor node is above the specified setpoint temperature.
-
-#### Field: Name
-
-The name of the object. This is referenced in the AvailabilityManagerAssignmentList.
-
-#### Field: Sensor Node Name
-
-The air or plant node where the temperature is monitored.
-
-#### Field: Temperature
-
-The setpoint temperature [C] at which the system is turned on.
-
-An example of this object in an IDF is:
-
-```idf
-AvailabilityManager:HighTemperatureTurnOn,
-   High Temperature Turn On Availability Manager,   !- Name
-   Outside Air Inlet Node,   !- Sensor Node
-   30.0;   !- Temperature {C}
-```
-
-### AvailabilityManager:HighTemperatureTurnOn Outputs
-
-The high temperature turn on availability manager has one output variable.
-
-* HVAC,Average,Availability Manager High Temperature Turn On Control Status
-
-#### Availability Manager High Temperature Turn On Control Status []
-
-A value of 0 indicates the manager is signaling *NoAction*. A value of 2 means the manager is signaling *CycleOn.*
-
-### AvailabilityManager:LowTemperatureTurnOff
-
-This manager turns the system off if the temperature at the sensor node is below the specified setpoint temperature.
-
-#### Field: Name
-
-The name of the object. This is referenced in the AvailabilityManagerAssignmentList.
-
-#### Field: Sensor Node Name
-
-The air or plant node where the temperature is monitored.
-
-#### Field: Temperature
-
-The setpoint temperature [C] at which the system is turned off.
-
-#### Field: Applicability Schedule Name
-
-The name of a schedule defined elsewhere in the input file. This schedule determines whether or not for a given time period this availability manager is to be applied. Schedule values greater than zero (usually 1 is used) indicate the availability manager is to be applied. Schedule values less than or equal to zero (usually 0 is used) denote that the availability manager is not used for this time period. If this field is left blank, this availability manager is always active.
-
-An example of this object in an IDF is:
-```idf
-AvailabilityManager:LowTemperatureTurnOff,
-   Low Temperature Turn Off Availability Manager,   !- Name
-   Outside Air Inlet Node,   !- Sensor Node Name
-   0.0,   !- Temperature {C}
-   Low Temp Control Schedule;   !- Applicability Schedule Name
-```
-
-### AvailabilityManager:LowTemperatureTurnOff Outputs
-
-The low temperature turn off availability manager has one output variable.
-
-* HVAC,Average,Availability Manager Low Temperature Turn Off Control Status
-
-Availability Manager Low Temperature Turn Off Control Status []
-
-A value of 0 indicates the manager is signaling NoAction. A value of 1 means the manager is signaling ForceOff.
-
-### AvailabilityManager:LowTemperatureTurnOn
-
-This manager turns the system on if the temperature at the sensor node is below the specified setpoint temperature.
-
-#### Field: Name
-
-The name of the object. This is referenced in the AvailabilityManagerAssignmentList.
-
-#### Field: Sensor Node Name
-
-The air or plant node where the temperature is monitored.
-
-#### Field: Temperature
-
-The setpoint temperature [C] at which the system is turned on.
-
-An example of this object in an IDF is:
-```idf
-AvailabilityManager:LowTemperatureTurnOn,
-   Low Temperature Turn On Availability Manager,   !- Name
-   Collector Outlet Node,   !- Sensor Node Name
-   0.0;   !- Temperature {C}
-```
-
-### AvailabilityManager:LowTemperatureTurnOn Outputs
-
-The low temperature turn on availability manager has one output variable.
-
-* HVAC,Average,Availability Manager Low Temperature Turn On Control Status []
-
-#### Availability Manager Low Temperature Turn On Control Status []
-
-A value of 0 indicates the manager is signaling NoAction. A value of 2 means the manager is signaling CycleOn.
-
-### AvailabilityManager:NightVentilation
-
-This manager allows the user to implement a strategy for precooling a building at night using outdoor air. This strategy can consist of running the system fans with the outdoor air dampers open when outdoor conditions are favorable for a precooling strategy. The zone terminal unit air dampers may also be held at their fully open position to minimize fan energy consumption while precooling. Fan energy consumption is the critical parameter in deciding whether a precooling strategy will save energy.
-
-The inputs for the night ventilation manager consist of an applicability schedule name (determining when the manager is active), a fan schedule name (for the fan(s) that the manager can switch on), a ventilation temperature schedule name (one zone must be above this temperature for night venting to be active), a ventilation temperature difference (indoor     outdoor temperature difference for night venting), a low limit temperature (no conditioned zone may fall below this temperature during night venting),   a night venting flow fraction (fraction of the design flow rate at which the fans run during night venting), and the zone name of a control zone.
-
-The night ventilation manager is used in conjunction with another object: FanPerformance:NightVentilation. The performance of the fan during night venting may be very different than during normal operation (a different fan might even be used). The FanPerformance:NightVentilation object allows the user to specify alternate fan performance parameters for use during night ventilation.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a night ventilation availability manager. Other objects that use this availability manager will reference it by this name.
-
-#### Field: Applicability Schedule Name
-
-The name of a schedule defined elsewhere in the input file. This schedule determines whether or not for a given time period this availability manager is to be applied. Schedule values greater than zero (usually 1 is used) indicate the availability manager is to be applied. Schedule values less than or equal to zero (usually 0 is used) denote that the availability manager is not used for this time period.
-
-#### Field: Fan Schedule Name
-
-The name of the central fan on/off schedule for the air system that this availability manager will affect.
-
-#### Field: Ventilation Temperature Schedule Name
-
-The name of a temperature schedule defined elsewhere in the input file. At least one conditioned zone in the forced air system using this availability manager must be above the current temperature specified in this schedule for night ventilation to occur or to continue occurring.
-
-#### Field: Ventilation Temperature Difference
-
-This field specifies an indoor / outdoor temperature difference (in degrees C). The control zone temperature minus the outdoor air temperature must be greater than the Ventilation Temperature Difference for night ventilation to occur or to continue occurring. The default is 2 degrees C.
-
-#### Field: Ventilation Temperature Low Limit
-
-This field specifies a lower limit (in degrees C) on zone temperatures for night ventilation. If any conditioned zone served by the air system using this availability manager is below the ventilation temperature low limit, night ventilation will not occur or will switch off. The default is 15 degrees C.
-
-#### Field: Night Venting Flow Fraction
-
-The fraction (could be greater than 1) of the design flow rate at which the night ventilation will be done. The default is 1.
-
-#### Field: Control Zone Name
-
-The name of the control zone used in the ventilation temperature difference check.
-
-An example of this object in an input file:
-```idf
-AvailabilityManager:NightVentilation,
-       VAV Sys 1 Avail,                 !- Name
-       NightVentSched,                   !- Applicability Schedule Name
-       FanAvailSched,                     !- Fan Schedule Name
-       VentTempSched,                     !- Ventilation Temperature Schedule Name
-       2.0,                                         !- Ventilation Temperature Difference   {C}
-       15.,                                         !- Ventilation Temperature Low Limit
-       0.3333,                                   !- Night Venting Flow Fraction
-       SPACE3-1;                               !- Control Zone Name
-```
-
-### System Availability Manager Night Ventilation Outputs
-
-The night ventilation availability manager has one output variable.
-
-* HVAC,Average,Availability Manager Night Ventilation Control Status []
-
-#### Availability Manager Night Ventilation Control Status []
-
-A value of 0 indicates the manager is signaling NoAction. A value of 2 means the manager is signaling CycleOn.
-
-### AvailabilityManager:HybridVentilation
-
-This availability manager is executed at the start of each HVAC system timestep, before EnergyPlus calculates airflows defined in the objects ZoneInfiltration:\*, ZoneVentilation:\*, ZoneMixing, and ZoneCrossMixing, and before the AirflowNetwork model calculates multizone airflows. It serves two purposes: 1) prevents simultaneous natural ventilation and HVAC system operation, and 2) allows users to examine various ventilation strategies to maximize natural ventilation in order to reduce heating/cooling loads. The natural ventilation objects controlled by this availability manager have two groups: simple airflow group and AirflowNetwork group. The simple airflow group consists of the ZoneVentilation;\* and ZoneMixing objects. The AirflowNetwork group consists of AirflowNetwork:MultiZone:Component:DetailedOpening and AirflowNetwork:MultiZone:Component:SimpleOpening objects used in the AirflowNetwork model. These two groups are not allowed to work simultaneously (see restrictions in the Airflow Network model section). Basically, this object overrides the controls for these opening objects or ZoneVentilation:\* and ZoneMixing objects, closing the    openings    or shutting off ventilation/mixing airflows under certain conditions and allowing the HVAC system (AirLoopHVAC) to operate. If the availability manager determines that conditions are favorable for natural ventilation, then the HVAC system (AirLoopHVAC) is disabled and the    opening    objects or ventilation/mixing objects are able to operate based on the controls specified for those objects.
-
-Each AirLoopHVAC can have a corresponding hybrid ventilation availability manager. Each hybrid ventilation manager can control natural ventilation in the zones served by the AirLoopHVAC. The hybrid ventilation availability manager is triggered by zone air conditions for the controlled zone specified in an object input field. If there is no air loop, hybrid ventilation manager can still be applied to controlled zone specified in the object. To apply hybrid ventilation manager to the controlled zone not served by any air loop, the HVAC air loop name input field must be left blank. Currently, zone component objects such as unit heater, unit ventilator, packaged terminal air conditioner, packaged terminal heat pump, zone water source heat pump, window air conditioner, variable refrigerant flow, energy recovery ventilator, outdoor air unit, fan coil unit, and ventilated slab can individually use hybrid ventilation managers to make a decision regarding whether their fan should be on or off. Also, hybrid ventilation managers can be applied to zones served by ideal load zone components to turn them off when natural ventilation is active. Currently, hybrid ventilation manager is restricted to one per zone. It can either be applied through the air loop or directly to the zone. If hybrid ventilation manager is applied to an air loop and one of the zones served by the air loop also has hybrid ventilation manager, then zone hybrid ventilation manager is disabled. Presently, this availability manager must be used either with the ZoneVentilation:\* and ZoneMixing objects or with the AirflowNetwork model.
-
-The inputs for this availability manager consist of the name for the air loop (AirLoopHVAC) being controlled, the controlled zone name to determine which zone air conditions are used to determine system availability, a ventilation control mode schedule, maximum wind speed and rain indicator to determine whether natural ventilation is allowed or not, a low limit and high limit for dry-bulb temperature, enthalpy and dewpoint temperature to determine the hybrid ventilation control, and a minimum outdoor air ventilation schedule. The last control allows user to use a wind speed modifier to adjust openness when the AirflowNetwork opening objects are selected. The other inputs include how to control simple airflow objects and AirflowNetwork opening objects.
-
-The hybrid ventilation availability manager works independently of all other system availability manager objects, so this manager is not a valid system availability manager type in the AvailabilityManagerAssignmentList object.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a hybrid ventilation availability manager. Other objects that use this availability manager will reference it by this name.
-
-#### Field: HVAC Air Loop Name
-
-The name of the air loop (AirLoopHVAC object) to be controlled by this system availability manager. If this field is left blank, hybrid ventilation manager will be applied to the controlled zone specified in the field below.
-
-#### Field: Controlled Zone Name
-
-The name of a controlled zone served by the air loop defined in the previous field. The air conditions in this zone are used to determine if natural ventilation should be provided.
-
-#### Field: Ventilation Control Mode Schedule Name
-
-The name of a schedule defined elsewhere in the input file. This schedule determines whether or not for a given time the hybrid ventilation control mode is to be applied. Schedule values equal to zero indicate no ventilation control, resulting in natural ventilation and HVAC system operation being performed based on their own controls. Schedule values equal to one denote temperature control for either cooling or heating, which is determined internally based on thermostat set point and temperature control type. The temperature control is restricted between the minimum and maximum outdoor temperatures provided in two additional input fields (below). Schedule values equal to two denote enthalpy control, which is restricted between minimum and maximum outdoor enthalpy values given in two additional input fields (below). Schedule values equal to three denote dewpoint control for either dehumidification or humidification. Schedule values equal to four represent outdoor ventilation air control. The outdoor ventilation air control works with AirflowNetwork opening objects only, and is not allowed to work with ZoneVentilation:\* and ZoneMixing objects.
-
-The detailed control logic is given in the EnergyPlus Engineering Reference.
-
-#### Field: Use Weather File Rain Indicators
-
-This logical alpha field indicates whether or not the rain indicator is used to shut off natural ventilation or not. The valid choices for Rain Indicator are Yes and No, with the default being Yes. This can help simulate conditions where one would normally close windows to avoid rain penetration in a space. Any possible rain getting into a space will not be counted as a zone load.
-
-#### Field: Maximum Wind Speed
-
-This is the wind speed (m/s) above which hybrid ventilation is shut off.   This can help simulate conditions where one would normally close windows to avoid wind problems in a space (papers blowing around, etc).
-
-#### Field: Minimum Outdoor Temperature
-
-This is the outdoor temperature (in Celsius) below which hybrid ventilation is shut off when the ventilation control mode = 1 (Temperature). This lower temperature limit is intended to avoid overcooling a space, which could result in a heating load.
-
-#### Field: Maximum Outdoor Temperature
-
-This is the outdoor temperature (in Celsius) above which hybrid ventilation is shut off when the ventilation control mode = 1 (Temperature). This upper temperature limit is intended to avoid overheating a space, which could result in a cooling load.
-
-#### Field: Minimum Outdoor Enthalpy
-
-This is the outdoor enthalpy (in J/kg) below which hybrid ventilation is shut off when the ventilation control mode = 2 (Enthalpy).
-
-#### Field: Maximum Outdoor Enthalpy
-
-This is the outdoor enthalpy (in J/kg) above which hybrid ventilation is shut off when the ventilation control mode = 2 (Enthalpy).
-
-#### Field: Minimum Outdoor Dewpoint
-
-This is the outdoor dewpoint (in Celsius) below which hybrid ventilation is shut off when the ventilation control mode = 3 (Dewpoint). This lower dewpoint temperature limit is intended to avoid dehumidifying a space.
-
-#### Field: Maximum Outdoor Dewpoint
-
-This is the outdoor dewpoint temperature (in Celsius) above which hybrid ventilation is shut off when the ventilation control mode = 3 (Dewpoint). This upper dewpoint temperature limit is intended to avoid humidifying a space.
-
-#### Field: Minimum Outdoor Ventilation Air Schedule Name
-
-The name of a schedule defined elsewhere in the input file. This field applies only if Ventilation Control Mode = 4 (Outdoor Ventilation Air Control). This schedule determines the minimum outdoor ventilation air for a given time in the units of air change per hour (ACH). The program calculates the natural (outdoor) ventilation in the controlled zone first and compares the amount of outdoor air introduced by opening windows or doors and other small openings to this minimum value. If the amount of outdoor air from natural ventilation is less than the minimum value, the natural ventilation is shut off (i.e., the window or door openings are closed) and the HVAC system may operate if needed. Otherwise, the natural ventilation is on and the HVAC system is shut off. The amount of outdoor ventilation air entering the controlled zone is determined as air from outdoors and not from other adjacent zones. Therefore, this option is only applied to a zone having a window or door exposed to outdoors.
-
-#### Field: Opening Factor Function of Wind Speed Curve Name
-
-The name of a linear or quadratic performance curve (ref: Performance Curves) that parameterizes the variation of opening factor as a function of outdoor wind speed. The output of this curve is multiplied by the opening factor of opening objects to give the final openness. This field only works with the AirflowNetwork opening objects.
-
-#### Field: AirflowNetwork Control Type Schedule Name
-
-The name of a schedule defined elsewhere in the input file. This field works with the AirflowNetwork opening objects only. This schedule determines for a given simulation timestep how the opening objects respond to the hybrid ventilation control when the hybrid ventilation control allows the objects to operate.
-
-Schedule values equal to zero indicate individual ventilation control based on the control requirements specified for each individual AirflowNetwork opening object. Schedule values equal to one denote    group    control. The opening objects exposed to outdoors in the controlled zone served by the primary air loop (Ref. Field    HVAC Air Loop Name   ) will be considered as a master to provide group control.
-
-#### Field: Simple Airflow Control Type Schedule Name
-
-The name of a schedule defined elsewhere in the input file. This field works with ZoneVentilation:\* and ZoneMixing objects only. This schedule determines for a given simulation timestep how the ZoneVentilation:\* and ZoneMixing objects respond to the hybrid ventilation control when the hybrid ventilation control allows the objects to operate.
-
-Schedule values equal to zero indicate the individual ventilation control based on the control requirements from their own objects. Schedule values equal to one denote group control. The ZoneVentilation:\* and ZoneMixing objects in the zones served by the primary air loop defined in a previous input field (Ref. Field    HVAC Air Loop Name   ) are controlled by a single object, whose name is provided in the following input field.
-
-#### Field: ZoneVentilation Object Name
-
-The name of a ZoneVentilation:\* object whose zone name is the controlled zone name defined in a previous input field for this availability manager object (Ref. Field    Controlled Zone Name   ). The controls defined for this specific ZoneVentilation:\* object to enable ventilation air will be applied to other ZoneVentilation:\* and ZoneMixing objects served by the air loop controlled by this availability manager, regardless of the controls defined for the other ZoneVentilation:\* and ZoneMixing objects. In other words, when ventilation is enabled by this specific ZoneVentilation:\* object, the other ZoneVentilation:\* and ZoneMixing objects in the zones served by the primary air loop are also enabled.
-
-**Note:** A **ZoneInfiltration:\*** object indicates any one of **ZoneInfiltration:DesignFlowRate**, **ZoneInfiltration:EffectiveLeakageArea**,and **ZoneInfiltration:FlowCoefficient** objects.A object of**ZoneVentilation:\*** indicates any one of **ZoneVentilation:DesignFlowRate** and **ZoneVentilation:WindandStackOpenArea** objects.
-
-### AvailabilityManager:HybridVentilation Outputs
-
-The hybrid ventilation availability manager has two output variables.
-
-HVAC,Average,Availability Manager Hybrid Ventilation Control Mode []
-
-HVAC,Average,Availability Manager Hybrid Ventilation Control Status []
-
-#### Availability Manager Hybrid Ventilation Control Mode []
-
-This is the hybrid ventilation control mode given in the Ventilation Control Mode Schedule.
-
-#### Availability Manager Hybrid Ventilation Control Status []
-
-This is the hybrid ventilation control status, which can have three integer values: 0, 1, and 2. A zero value indicates no hybrid ventilation control, corresponding to zero value defined in the previous output variable. A value of one indicates that natural ventilation is allowed. A value of two denotes that the natural ventilation is not allowed, so all window/door openings are closed.
-
-### AvailabilityManager:OptimumStart
-
-When night time temperature setback and/or setup are employed, the optimum start availability manager is used to start the HVAC system prior to occupancy to ensure that the space is comfortable when people appear in the building.
-
-#### Field: Name
-
-A unique, user-defined name for an instance of this availability manager.
-
-#### Field: Applicability Schedule Name
-
-This schedule decides whether for a given time period this availability manager is to be applied. Schedule value of 1 specifies the availability manager is to be applied. Schedule value of 0 indicates that the availability manager is not used for this time period
-
-#### Field: Fan Schedule Name
-
-The name of the central fan schedule for the air system that this availability manager will govern.
-
-#### Field: Control Type
-
-The possible inputs are StayOff, MaximumofZoneList, and ControlZone. StayOff means the availability manager will have no effect     air handler on/off will be determined by the fan schedule. ControlZone means a specific zone mentioned in the field will govern the start time. The default is ControlZone. MaximumofZoneList means that from all zones mentioned in the zone list field in this availability manager maximum value of start time will be used to start the fan.
-
-#### Field: Control Zone Name
-
-For Control type ControlZone the name of zone is added here. Start time for this zone will be used for the air loop.
-
-#### Field: Zone List Name
-
-Zones mentioned in this list will be used to determine the start time. Maximum value of start time for the zones mentioned in this list will be used for the air loop.
-
-#### Field: Maximum Value for Optimum Start Time
-
-To limit too early start of the system maximum value for the start time can be entered here. Optional input, defaults to 6 hours. This is the maximum number of hours that a system can start before occupancy.
-
-#### Field: Control Algorithm
-
-The four possible inputs are **ConstantTemperatureGradient, AdaptiveTemperatureGradient, AdaptiveASHRAE,** and **ConstantStartTime**. In ConstantTemperatureGradient algorithm the temperature gradient entered by the user will be constant throughout the simulation. The response to heating and cooling operation can be non-linear thus two separate fields for temperature gradients are used.   AdaptiveTemperatureGradient algorithm will modify the temperature gradients based on the arithmetic average of the actual temperature gradients calculated for the specified number of previous days. For this algorithm user should enter two initial start values. AdaptiveASHRAE algorithm implements equations suggested in ASHRAE Handbook     HVAC Applications (2007). This algorithm will calculate the coefficients of the equation within the code and users need not provide temperature response related inputs. ConstantStartTime method calculates the start time based on specified number of hours before occupancy for each day. **The AdaptiveASHRAE algorithm has not been implemented yet.**
-
-#### Field: Constant Temperature Gradient during Cooling
-
-This input is required if ConstantTemperatureGradient algorithm is selected in the above field. Temperature gradient ( &deg;C/hour) for cooling operation is entered here. Such gradient may be obtained for existing buildings from EMCS or pre-calculated by other programs. This gradient remains constant throughout the simulation.
-
-#### Field: Constant Temperature Gradient during Heating
-
-This input is required if ConstantTemperatureGradient algorithm is selected in the Control Algorithm field. Temperature gradient ( &deg;C/hour) for heating operation is entered here. This gradient remains constant throughout the simulation.
-
-#### Field: Initial Temperature Gradient during Cooling
-
-This input is required if AdaptiveTemperatureGradient algorithm is selected in Control Algorithm field. Initial value of temperature gradient ( &deg;C/hour) for cooling operation is entered here. This value is used as initial guess value to start the adaptive method. Depending on performance, this value is modified and used in the simulation.
-
-#### Field: Initial Temperature Gradient during Heating
-
-This input is required if AdaptiveTemperatureGradient algorithm is selected in Control Algorithm field. Initial value of temperature gradient ( &deg;C/hour) for heating operation is entered here. This value is used as initial guess value to start the adaptive method. Depending on performance, this value is modified and used in the simulation.
-
-#### Field: Constant Start Time
-
-This input is required if ConstantStartTime algorithm is selected in the Control Algorithm field. Start time, the number of hours before occupancy occurs for a system, for heating and cooling operation is entered here. Irrespective of thermal response, the heating or cooling operation starts before the occupancy at this fixed time. This start time value remains constant throughout the simulation.
-
-#### Field: Number of Previous Days
-
-This input is required if AdaptiveTemperatureGradient algorithm is selected in the Control Algorithm field. The values of optimal start time for number of days entered here will be used to determine the adaptive gradients.
-
-Sample IDFs:
-
-```idf
-AvailabilityManager:OptimumStart,
-   AdaptiveSetbackRecovery, !- Name
-   AppliSch,                                             !- Applicability Schedule Name
-   FanSch,                                                 !- Fan Schedule Name
-   ControlZone,                                       !- Control Type
-   MainZone,                                             !- Control Zone Name
-   ,                                                             !- Zone List Name
-   4,                                                           !- Maximum Value for Optimum Start Time
-   AdaptiveTemperatureGradient,       !- Control Algorithm
-   ,                                                             !- Constant Temperature Gradient during Cooling
-   ,                                                             !- Constant Temperature Gradient during Heating
-   5,                                                           !- Initial Temperature Gradient during Cooling
-   5;                                                           !- Initial Temperature Gradient during Heating
-
-AvailabilityManager:OptimumStart,
-   SetbackRecovery,                               !- Name
-   AppliSch,                                             !- Applicability Schedule Name
-   FanSch,                                                 !- Fan Schedule Name
-   MaximumofZoneList,             !- Control Type
-   ,                                                            !- Control Zone Name
-   ZoneList,                                             !- Zone List Name
-   ,                                                             !- Maximum Value for Optimum Start Time
-   AdaptiveASHRAE;                                 !- Control Algorithm
-```
-
-### AvailabilityManager:OptimumStart Outputs
-
-The optimum start availability manager has two output variables.
-
-#### Availability Manager Night Ventilation Control Status
-A value of 0 indicates the manager is signaling NoAction. A value of 2 means the manager is signaling CycleOn.
-
-#### Availability Manager Optimum Start Time Before Occupancy
-
-The current time before occupancy.  Occupancy is the first zone timestep after midnight when the Fan Schedule is > 0.0.  The units are hours.
-
-Group     Setpoint Managers
--------------------------
-
-Setpoint Managers are one of the high-level control constructs in EnergyPlus. A Setpoint Manager is able to access data from any of the HVAC system nodes and use this data to calculate a setpoint (usually a temperature setpoint) for one or more other HVAC system nodes. Setpoints are then used by Controllers or Plant or Condenser Loops as a goal for their control actions.
-
-Setpoint Managers are executed at the start of each HVAC timestep, and they reside outside the HVAC system iteration loops. Thus, the Setpoint Managers are executed once per HVAC timestep, and they use previous timestep information (except for zone load) to calculate their setpoints.
-
-The following situations require the use of a Setpoint Manager:
-
-1)        any use of Controller:WaterCoil; either in    Temperature    control only or 2 Setpoint Managers for the " TemperatureAndHumidityRatio " control variable option.
-
-2)        use of Controller:OutdoorAir with *Economizer Control Type* set to anything but *NoEconomizer*;
-
-3)        use of Coil:Heating:Gas or Coil: Heating: Electric with the field *Temperature Setpoint Node Name* set to a node name;
-
-4)        any use of CoilSystem:Cooling:DX;
-
-5)        any use of Humidifier:Steam:Electric.
-
-6)        Any use of PlantLoop or CondenserLoop which doesn't use an environment reference such as AIR or GROUND as a set point
-
-Setpoint managers will place a calculated or scheduled setpoint value on the setpoint node and overwrite any previous value. This value may represent one of several control types (e.g., Temperature, HumidityRatio, MassFlowRate, etc.). No two setpoint managers should use the same setpoint node for like control types.
-
-For the case when two setpoint managers place a setpoint on the same setpoint node (e.g., a temperature setpoint placed on the same node by two different setpoint managers), the setpoint value on the node is calculated by the last setpoint manager simulated. Within a specific type of setpoint manager (e.g., Scheduled), the setpoint managers are simulated in the order found in the input data file (idf) when viewed using a text editor. It is also possible for two different types of setpoint managers to place setpoints of like control variable on the same node. In this case, the order of simulation for the type of setpoint manager determines which setpoint manager is the last to write a setpoint value to the node. This conflict in setpoint node data is most likely to cause inaccurate simulation results. For this reason, a conflicting setpoint node name warning message is issued so that the conflict can be resolved.   Duplicate setpoint node names found within a specific node list will not typically cause problems with the simulation (the same value is written twice to the same node). In this case a duplicate setpoint node name warning is issued, however, this could be an error in the spelling of the node name and should be corrected.
-
-Simulation order for setpoint managers:
-
-- SetpointManager:Scheduled
-
-- SetpointManager:Scheduled:DualSetpoint
-
-- SetpointManager:OutdoorAirReset
-
-- SetpointManager:SingleZone:Reheat
-
-- SetpointManager: SingleZone:Heating
-
-- SetpointManager: SingleZone:Cooling
-
-- SetpointManager: SingleZone:Humidity:Minimum
-
-- SetpointManager: SingleZone:Humidity:Maximum
-
-- SetpointManager:Warmest
-
-- SetpointManager:Coldest
-
-- SetpointManager:WarmestTemperatureFlow
-
-- SetpointManager:ReturnAirBypassFlow
-
-- SetpointManager:MultiZone:Cooling:Average
-
-- SetpointManager:MultiZone:Heating:Average
-
-- SetpointManager:MultiZone:MinimumHumidity:Average
-
-- SetpointManager:MultiZone:MaximumHumidity:Average
-
-- SetpointManager:MultiZone:Humidity:Minimum
-
-- SetpointManager:MultiZone:Humidity:Maximum
-
-- SetpointManager:FollowOutdoorAirTemperature
-
-- SetpointManager:FollowSystemNodeTemperature
-
-- SetpointManager:FollowGroundTemperature
-
-- SetpointManager:CondenserEnteringReset
-
-- SetpointManager:CondenserEnteringReset:Ideal
-
-- SetpointManager:MixedAir
-
-- SetpointManager:OutdoorAirPretreat
-
-- SetpointManager:ReturnTemperature:ChilledWater,
-
-- SetpointManager:ReturnTemperature:HotWater
-
-### SetpointManager:Scheduled
-
-The simplest Setpoint Manager simply uses a schedule to determine one or more setpoints. No node data is used as input. The input consists of the Setpoint Manager name, the control variable, the schedule name, and the name of a node list. The node list contains the name of those nodes at which the setpoint is to be applied. Of course, a node list name can always be simply the name of a single node.
-
-Note that although this object provides a very general method of setting the values of many different control variables on nodes, the component models and system solvers may or may not be able to use them. Therefore, it is important to understand that simply setting a control variable using this object will not necessarily always produce the desired behavior.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a scheduled setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. There are several choices for this type of set point manager. The most common control variable is Temperature but other major choices include: HumidityRatio and MassFlowRate. The versatility of control variables available here (probably) exceeds what is actually available in the component and systems models. However, a large number of possible control variables are made available here for maximum flexibility and because some (but not all) component models will be able to use them. The complete list of key words and the units required in the associated schedules follow.
-
-- Temperature                                               Temperture of fluid at node ( &deg;C)
-
-- MaximumTemperature                   Maximum temperature of fluid at node   ( &deg;C)
-
-- MinimumTemperature                     Minimum temperature of fluid at node   ( &deg;C)
-
-- HumidityRatio                                         Humidity ratio of fluid at node (kgWater/kgDryAir)
-
-- MaximumHumidityRatio   Maximum humidity ratio of fluid at node (kgWater/kgDryAir)
-
-- MinimumHumidityRatio     Minimum humidity ratio of fluid at node (kgWater/kgDryAir)
-
-- MassFlowRate                                       Mass flow rate of fluid at node (kg/s)
-
-- MaximumMassFlowRate           Maximum mass flow rate of fluid at node (kg/s)
-
-- MinimumMassFlowRate            Minimum mass flow rate of fluid at node (kg/s)
-
-#### Field: Schedule Name
-
-The name of a schedule whose values are to be used as setpoints on the node or node list. The schedule value for each time period is the setpoint for this type of setpoint manager. The schedule must have values that are in the appropriate units as defined in the previous field.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which setpoints will be established by this setpoint manager.
-
-Following is an example of the input for a Scheduled Setpoint Manager.
-
-```idf
-SetpointManager:Scheduled,
-       Supply Air Temp Manager 1,   !- Name
-       Temperature,                               !- Control Variable
-       Seasonal Reset Supply Air Temp Sch,   !- Schedule Name
-       VAV Sys 1 Outlet Node;           !- Setpoint Node or NodeList Name
-```
-
-### SetpointManager:Scheduled:DualSetpoint
-
-This setpoint manager places a high and low schedule value on one or more nodes. The input consists of the Setpoint Manager name, the control variable, the high and low set point schedule names, and the name of a node list. The node list contains the name of those nodes at which the setpoint is to be applied. Of course, a node list name can simply be the name of a single node. Currently the DualSetpoint Manager will be used with PlantLoop when the Plant Loop Demand Calculation Scheme is set to    DualSetpointDeadband   .
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of this scheduled setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
-
-#### Field: High Setpoint Schedule Name
-
-The name of a schedule that contains the high setpoint values. The schedule value for each time period is the high setpoint for this type of setpoint manager.
-
-#### Field: Low Setpoint Schedule Name
-
-The name of a schedule that contains the low setpoint values. The schedule value for each time period is the low setpoint for this type of setpoint manager.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
-
-Following is an example of the input for a SetpointManager:Scheduled:DualSetpoint object.
-
-```idf
-SetpointManager:Scheduled:DualSetpoint,
-       Water Loop Setpoint Manager,       !- Name
-       Temperature,                                       !- Control Variable
-       Plant Loop High Temp Schedule,   !- High Setpoint Schedule Name
-       Plant Loop Low Temp Schedule,     !- Low Setpoint Schedule Name
-       Plant Supply Outlet Node;             !- Setpoint Node or NodeList Name
-```
-
-### SetpointManager:OutdoorAirReset
-
-The Outdoor Air Reset Setpoint Manager sets the supply air temperature according to the outdoor air temperature using a reset rule. The reset rule is determined by 2 points: the supply air setpoint temperature at the outdoor high temperature (SATOH) and the supply air setpoint temperature at the outdoor low temperature (SATOL). If the outdoor temperature is above the outdoor high temperature, the supply air temperature is set to SATOH. If the outdoor temperature is below the outdoor low temperature, the supply air temperature is set to SATOL. If the outdoor temperature is between the outdoor high and outdoor low temperatures, the supply air temperature is linearly interpolated between SATOH and SATOL.
-
-The input consists of the setpoint manager name, the type of control variable, a node list name of the nodes affected by the setpoint, and the data for the reset rule: the supply air setpoint temperature at the outdoor low temperature, the outdoor low temperature, the supply air setpoint temperature at the outdoor high temperature, and the outdoor high temperature.
-
-There are optional inputs for a second reset rule. First there is the name of a schedule that indicates which rule to use: a schedule value of 1 means use the first rule; a schedule value of 2 means use the second rule. Next, there are the 4 inputs specifying the second reset rule.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of an outdoor air reset setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
-
-#### Field: Setpoint at Outdoor Low Temperature
-
-The supply air temperature setpoint in   <sup>o</sup>C at the outdoor low temperature for the first reset rule.
-
-#### Field: Outdoor Low Temperature
-
-The outdoor air low temperature in   <sup>o</sup>C for the first supply air temperature reset rule. Generally, at this outdoor air temperature the supply temperature is at its maximum.
-
-#### Field: Setpoint at Outdoor High Temperature
-
-The supply air temperature setpoint in   <sup>o</sup>C at the outdoor high temperature for the first reset rule.
-
-#### Field: Outdoor High Temperature
-
-The outdoor air high temperature in <sup>o</sup>C for the first supply air temperature reset rule. Generally, at this outdoor air temperature the supply temperature is at its minimum.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
-
-#### Field: Schedule Name
-
-The name of a schedule whose values indicate which reset rule to use. Schedule values of 1 indicate that the first reset rule will be used. Schedule values of 2 select the second reset rule.
-
-#### Field: Setpoint at Outdoor Low Temperature 2
-
-The supply air temperature setpoint in <sup>o</sup>C at the outdoor low temperature for the second reset rule.
-
-#### Field: Outdoor Low Temperature 2
-
-The outdoor air low temperature in <sup>o</sup>C for the second supply air temperature reset rule. Generally, at this outdoor air temperature the supply temperature is at its maximum.
-
-#### Field: Setpoint at Outdoor High Temperature 2
-
-The supply air temperature setpoint in <sup>o</sup>C at the outdoor high temperature for the second reset rule.
-
-#### Field: Outdoor High Temperature 2
-
-The outdoor air high temperature in <sup>o</sup>C for the second supply air temperature reset rule. Generally, at this outdoor air temperature the supply temperature is at its minimum.
-
-Below is an example of the input for an Outdoor Air Reset Setpoint Manager:
-
-```idf
-SetpointManager:OutdoorAirReset,
-           Supply Air Temp Manager 1,   !- Name
-           Temperature,   !- Control Variable
-           16.7,   !- Setpoint at Outdoor Low Temperature {C}
-           0.0,     !- Outdoor Low Temperature {C}
-           12.8,   !- Setpoint at Outdoor High Temperature {C}
-           32.0,   !- Outdoor High Temperature {C}
-           Supply Air Temp Nodes;   !- Setpoint Node or NodeList Name
-
-NodeList,
-           Supply Air Temp Nodes, !- Name
-           Air Loop Outlet Node;   !- Node 1 Name
-```
-
-
-### SetpointManager:SingleZone:Reheat
-
-The Single Zone Reheat Setpoint Manager allows the simulation of a single zone reheat system. This setpoint manager detects the control zone load, zone inlet node flow rate, and zone node temperature and calculates a setpoint temperature for the supply air that will satisfy the zone load for the control zone. This setpoint manager creates a variable temperature system. The input consists of the setpoint manager name, the control variable type, the minimum and maximum supply air temperatures, the name of the control zone, the name of the control zone node, the name of the control zone inlet node, and the name of a node or node list containing the nodes whose setpoint temperatures are to be set by this manager.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of this setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
-
-#### Field: Minimum Supply Air Temperature
-
-The minimum supply air temperature (in <sup>o</sup>C) that is allowed for this system (as set by this setpoint manager).
-
-#### Field: Maximum Supply Air Temperature
-
-The maximum supply air temperature (in <sup>o</sup>C) that is allowed for this system (as set by this setpoint manager)
-
-#### Field: Control Zone Name
-
-The name of the control zone for this single zone reheat system. The heating or cooling load for this zone determines the supply air temperature setpoint.
-
-#### Field: Zone Node Name
-
-The name of the zone node for the control zone.
-
-#### Field: Zone Inlet Node Name
-
-The name of the zone inlet node that is supplying air to the control zone.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
-
-Below is an example input for a SetpointManager:SingleZone:Reheat object.
-
-```idf
-SetpointManager:SingleZone:Reheat,
-           Supply Air Temp Manager,   !- Name
-           Temperature,  !- Control Variable
-           13.,  !- Minimum Supply Air Temperature {C}
-           45.,  !- Maximum Supply Air Temperature {C}
-           NORTH ZONE,     !- Control Zone Name
-           Zone 3 Node,   !- Zone Node Name
-           Zone 3 Inlet Node,  !- Zone Inlet Node Name
-           Supply Air Temp Nodes;  !- Setpoint Node or NodeList Name
-
-
-NodeList,
-           Supply Air Temp Nodes, !- Name
-           Heating Coil Air Inlet Node,   !- Node 1 Name
-           Air Loop Outlet Node; !- Node 2 Name
-```
-
-
-### SetpointManager:SingleZone:Heating
-
-The Single Zone Heating Setpoint Manager allows a component to be controlled based on the load required to meet the zone heating setpoint. Ths setpoint manager detects the control zone load to meet the current heating setpoint, zone inlet node flow rate, and zone node temperature, and calculates a setpoint temperature for the supply air that will satisfy the zone heating load for the control zone. This setpoint manager creates a variable temperature system. The input consists of the setpoint manager name, the controlled variable type, the minimum and maximum supply air temperatures, the name of the control zone, the name of the control zone node, the name of the control zone inlet node, and the name of a node or node list containing the nodes whose setpoint temperatures are to be set by this manager.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a single zone heating setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
-
-#### Field: Minimum Supply Air Temperature
-
-The minimum supply air temperature (in <sup>o</sup>C) that is allowed for this system (as set by this setpoint manager).
-
-#### Field: Maximum Supply Air Temperature
-
-The maximum supply air temperature (in <sup>o</sup>C) that is allowed for this system (as set by this setpoint manager)
-
-#### Field: Control Zone Name
-
-The name of the control zone for this setpoint manager. The heating load for this zone (to meet the zone heating setpoint) determines the supply air temperature setpoint.
-
-#### Field: Zone Node Name
-
-The name of the zone node for the control zone.
-
-#### Field: Zone Inlet Node Name
-
-The name of the zone inlet node that is supplying air to the control zone.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
-
-Below is an example input for a SetpointManager:SingleZone:Heating object.
-
-```idf
-SetpointManager:SingleZone:Heating,
-       Zone 1 Heating Supply Air Temp Manager,   !- Name
-       Temperature,                         !- Control Variable
-       7.22,                                       !- Minimum Supply Air Temperature {C}
-       45.,                                         !- Maximum Supply Air Temperature {C}
-       Zone 1,                                   !- Control Zone Name
-      Zone 1 Zone Node,               !- Zone Node Name
-      Zone 1 Supply Inlet,         !- Zone Inlet Node Name
-       Zone 1 Heating Coil Outlet;   !- Setpoint Node or NodeList Name
-```
-
-
-### SetpointManager:SingleZone:Cooling
-
-The Single Zone Cooling Setpoint Manager allows a component to be controlled based on the load required to meet the zone cooling setpoint. This setpoint manager detects the control zone load to meet the current cooling setpoint, zone inlet node flow rate, and zone node temperature, and calculates a setpoint temperature for the supply air that will satisfy the zone cooling load for the control zone. This setpoint manager creates a variable temperature system. The input consists of the setpoint manager name, the controlled variable type, the minimum and maximum supply air temperatures, the name of the control zone, the name of the control zone node, the name of the control zone inlet node, and the name of a node or node list containing the nodes whose setpoint temperatures are to be set by this manager.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a single zone cooling setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
-
-#### Field: Minimum Supply Air Temperature
-
-The minimum supply air temperature (in <sup>o</sup>C) that is allowed for this system (as set by this setpoint manager).
-
-#### Field: Maximum Supply Air Temperature
-
-The maximum supply air temperature (in <sup>o</sup>C) that is allowed for this system (as set by this setpoint manager)
-
-#### Field: Control Zone Name
-
-The name of the control zone for this setpoint manager. The cooling load of this zone (to meet the zone cooling set point) determines the supply air temperature setpoint.
-
-#### Field: Zone Node Name
-
-The name of the zone node for the control zone.
-
-#### Field: Zone Inlet Node Name
-
-The name of the zone inlet node that is supplying air to the control zone.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a Node List object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
-
-Below is an example input for a SetpointManager:SingleZone:Cooling object.
-
-```idf
-SetpointManager:SingleZone:Cooling,
-       Zone 1 Cooling Supply Air Temp Manager,   !- Name
-       Temperature,                         !- Control Variable
-       7.22,                                       !- Minimum Supply Air Temperature {C}
-       45.,                                         !- Maximum Supply Air Temperature {C}
-       Zone 1,                                   !- Control Zone Name
-      Zone 1 Zone Node,               !- Zone Node Name
-      Zone 1 Supply Inlet,         !- Zone Inlet Node Name
-       Zone 1 Cooling Coil Outlet;   !- Setpoint Node or NodeList Name
-```
-
-
-
-
-### SetpointManager:SingleZone:Humidity:Minimum
-
-The Single Zone Minimum Humidity Setpoint Manager allows the control of a single zone minimum humidity level. This setpoint manager detects the humidity level in a control zone and, using air and moisture mass balance, calculates the supply air humidity ratio needed to maintain the zone relative humidity at or above a given setpoint. The calculated supply air humidity ratio is then used as the setpoint for the designated setpoint node. A humidifier component placed upstream of the setpoint node can then use the humidity ratio setpoint to control its moisture addition rate.
-
-The use of this object requires that a    ZoneControl:Humidistat    object be specified with a humidifying relative humidity schedule for the controlling zone. The humidistat   s controlling zone must correspond with the control zone air node name specified in this setpoint manager.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a single zone minimum humidity setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-Deprecated Field. This field is not used and will be deleted in a future release.
-
-#### Field: Schedule Name
-
-Deprecated Field. This field is not used and will be deleted in a future release.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of the HVAC system node where the calculated humidity ratio setpoint is set. If the setpoint is being placed on more than one node, this input should be the name of a NodeList.
-
-#### Field: Control Zone Air Node Name
-
-The name of the zone node for the humidity control zone (as specified in the object ZoneHVAC:EquipmentConnections).
-
-An IDF example for this setpoint manager is shown below with the required humidistat:
-
-```idf
-SetpointManager:SingleZone:Humidity:Minimum,
-       Zone Min Set Point Manager,   !- Name
-       ,   !- Control Variable
-       ,   !- Schedule Name
-       Air Loop Outlet Node,   !- Setpoint Node or NodeList Name
-       Zone 2 Node;                     !- Control Zone Air Node Name
-
-
-ZoneControl:Humidistat,
-       Zone 2 Humidistat,             !- Name
-       ZONE 2,                                   !-Zone Name
-       Min rel Hum Set Sch2;       !- Humidifying Relative Humidity Setpoint Schedule Name
-```
-
-
-
-
-### SetpointManager:SingleZone:Humidity:Maximum
-
-The Single Zone Maximum Humidity Setpoint Manager allows the control of a single zone maximum humidity level. This setpoint manager, used in conjunction with object ZoneControl:Humidistat, detects the air humidity level in a single control zone and uses air/moisture mass balances to calculate the supply air humidity ratio needed to maintain the zone relative humidity at or below a given setpoint. The calculated supply air humidity ratio is then used as the setpoint for the designated setpoint node. A dehumidification component placed upstream of this node can then use the humidity ratio setpoint to control its moisture removal rate (e.g., desiccant dehumidifiers).
-
-In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determine the minimum supply air temperature required to meet both the temperature (sensible) and humidity (latent) load in the control zone. See object Controller:WaterCoil in the EnergyPlus Engineering Reference for a detailed discussion of how this is achieved.
-
-The use of this object requires that a    ZoneControl:Humidistat    object be specified with a relative humidity setpoint schedule for the controlling zone. The humidistat   s controlling zone must correspond with the control zone air node name specified in this setpoint manager..
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a single zone maximum humidity setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-Deprecated Field. This field is not used and will be deleted in a future release.
-
-#### Field: Schedule Name
-
-Deprecated Field. This field is not used and will be deleted in a future release.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of the HVAC system node where the calculated humidity ratio setpoint is set. If the setpoint is being placed on more than one node, this input should be the name of a NodeList.
-
-#### Field: Control Zone Air Node Name
-
-The name of the zone air node for the humidity control zone (as specified in the object ZoneHVAC:EquipmentConnections).
-
-An example of this object in an input data file (IDF), along with a temperature set point manager, humidistat, and a simple controller, is shown below:
-
-```idf
-   SetpointManager:SingleZone:Humidity:Maximum,
-       Zone Max Set Point Manager,                     !- Name
-       ,                                                                         !- Control Variable
-       ,                                                                         !- Schedule Name
-       VAV Sys 1 Outlet Node,                               !- Setpoint Node or NodeList Name
-       Zone 2 Node;                                                   !-Control Zone Air Node Name
-
-
-   SetpointManager:Scheduled,
-       Scheduled Set Point Manager 1,               !- Name
-       Temperature,                                                   !- Control Variable
-       Seasonal Reset Supply Air Temp Sch,     !- Schedule Name
-       VAV Sys 1 Outlet Node;                               !- Setpoint Node or NodeList Name
-
-
-   ZoneControl:Humidistat,
-       Zone 2 Humidistat,             !-Name
-       ZONE 2,                                   !- Zone Name
-       Min rel Hum Set Sch2;       !- Humidifying Relative Humidity Setpoint Schedule Name
-
-
-   Controller:WaterCoil,
-       Central Cooling Coil Contoller 1,         !- Name
-       TEMPandHUMRAT,                                               !- Control Variable
-       Reverse,                                                           !- Action
-       FLOW,                                                                 !- Actuator Variable
-       VAV Sys 1 Outlet Node,                               !- Sensor Node Name
-       Main Cooling Coil 1 Water Inlet Node, !- Actuator Node Name
-       0.002,                                                               !- Controller Convergence Tolerance {deltaC}
-       0.025,                                                               !- Maximum Actuated Flow {m3/s}
-       0.0;                                                                   !- Minimum Actuated Flow {m3/s}
-```
-
-
-
-
-### SetpointManager:MixedAir
-
-The Mixed Air Setpoint Manager is meant to be used in conjunction with a Controller:OutdoorAir object. This setpoint manager is used to establish a temperature setpoint at the mixed air node. The Controller:OutdoorAir then operates the outdoor air damper to attempt to meet this setpoint.
-
-In EnergyPlus the relief and outdoor air dampers, the economizer, and any outdoor air conditioning equipment form a separate subsystem of an air loop system (ref. AirLoopHVAC). The outdoor air controller operates within the subsystem. Consequently the mixed air temperature setpoint must take into account any downstream system fan heat if it is to meet a desired system supply air leaving temperature. The Mixed Air Setpoint Manager accomplishes this by referencing a supply air setpoint set by another setpoint manager (most likely at the AirLoopHVAC outlet node). The supply fan inlet and outlet nodes are also inputs to the Mixed Air Setpoint Manager. From this information the Mixed Air Setpoint Manager calculates the supply fan air temperature rise, subtracts it from the reference setpoint temperature, and sets the result as the mixed air node setpoint temperature.
-
-Of course any type of setpoint manager can be used to establish a temperature setpoint at the mixed air node. But the Mixed Air Setpoint Manager is likely to be the most useful.
-
-When optional inputs of Cooling Coil Inlet Node Name, Cooling coil Outlet Node Name, and Minimum Temperature at Cooling Coil Outlet Node are provided, the setpoint temperature at the mixed air node is calculated based on the maximum of both the reference setpoint temperature and minimum cooling coil outlet temperature, minus the cooling coil air temperature reduction and the supply fan air temperature rise if the supply fan placement is blow through. The setpoin temperature at the mixed air node is used to calculate the maximum outdoor air flow fraction in the corresponding Controller:OutdoorAir object. The outdoor air flow fraction is capped at the maximum outdoor air flow fraction to prevent the cooling coil from freezing, even though the fraction is below the minimum outdoor air flow fraction.  
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a mixed air setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. There is only one choice for this type of setpoint manager: Temperature.
-
-#### Field: Reference Setpoint Node Name
-
-The name of an HVAC system node where the system supply air temperature is set. Normally this would be the AirLoopHVAC outlet node. The temperature setpoint at this reference node is set by a different setpoint manager.
-
-#### Field: Fan Inlet Node Name
-
-The name of the supply fan inlet node.
-
-#### Field: Fan Outlet Node Name
-
-The name of the supply fan outlet node.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name where temperature setpoints will be established by this setpoint manager.
-
-#### Field: Cooling Coil Inlet Node Name
-
-The name of the cooling coil inlet node.
-
-#### Field: Cooling Coil Outlet Node Name
-
-The name of the cooling coil outlet node.
-
-#### Field: Minimum Temperature at Cooling Coil Outlet Node
-
-In order to prevent cooling coil freezing during economizer operation, the minimum temperature at the cooling coil outlet is required based on requirement of ASHRAE Standard 90.1. The default value is 7.2C.
-
-Below is an example input for a Mixed Air Setpoint Manager.
-
-```idf
-SetpointManager:SingleZone:Reheat, ! establishes the setpoint at the system outlet node
-           Supply Air Temp Manager,   !- Name
-           Temperature,   !- Control Variable
-           13.,  !- Minimum Supply Air Temperature
-           45.,  !- Maximum Supply Air Temperature
-           NORTH ZONE,  !- Control Zone Name
-           Zone 3 Node,  !- Zone Node Name
-           Zone 3 Inlet Node,  !- Zone Inlet Node Name
-          Supply Air Temp Nodes;   !- Setpoint Node or NodeList Name
-
-
-SetpointManager:MixedAir, ! uses the system outlet setpoint to establish the mixed air setpoint
-           Mixed Air Temp Manager 1,   !- Name
-           Temperature,   !- Control Variable
-           Air Loop Outlet Node,                   !- Reference Setpoint Node Name
-           Heating Coil Air Outlet Node,   !- Fan Inlet Node Name
-           Air Loop Outlet Node,                   !- Fan Outlet Node Name
-           Mixed Air Nodes;                             !- Setpoint Node or NodeList Name
-
-
-NodeList, Supply Air Temp Nodes,
-           Air Loop Outlet Node; ! Setpoint Nodes
-NodeList, Mixed Air Nodes,
-           Mixed Air Node; ! Setpoint Nodes
-```
-
-### SetpointManager:OutdoorAirPretreat
-
-The OutdoorAir Pretreat Setpoint Manager is meant to be used in conjunction with an OutdoorAir:Mixer object. The Outdoor air Pretreat Setpoint Manager is used to establish a temperature or humidity ratio setpoint in the outdoor air stream flowing into the "Outdoor Air Stream Node" of an OutdoorAir:Mixer object. This setpoint manager determines the required setpoint in the outdoor air stream to produce the reference setpoint in the mixed air stream after mixing with return air. For example, if the temperature setpoint at the mixed air node is 15 &deg;C, the return air temperature is 20 &deg;C, and the outdoor air flow fraction is 0.5, the Outdoor Air Pretreat setpoint would be set to 10 &deg;C.
-
-Of course any type of setpoint manager can be used to establish setpoints in the outdoor air stream, but this setpoint manager is likely to be the most useful for systems which precondition outdoor air with equipment such as a DX cooling coil or desiccant dehumidifier.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of an outdoor air pretreat setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. The choices are:
-
-- Temperature     references and sets the "System Node Setpoint Temperature" property. This single temperature setpoint is set and used by all temperature setpoint managers and equipment controls except dual-setpoint equipment.
-
-- MaximumHumidityRatio     references and sets the "System Node Humidity Ratio Max" property. This type of reference setpoint may be set using SetpointManager:SingleZone:Humidity:Maximum, SetpointManager:MultiZone:MaximumHumidity:Average, or SetpointManager:MultiZone:Humidity:Maximum and is used by equipment such as Controller:WaterCoil (with control variable    TemperatureAndHumidityRatio   ) and Dehumidifier:Desiccant:NoFans.
-
-- MinimumHumidityRatio     references and sets the "System Node Humidity Ratio Min" property. This type of reference setpoint may be set using SetpointManager:SingleZone:Humidity:Minimum, SetpointManager:Multizone:MinimumHumidity:Average or SetpointManager:MultiZone:Humidity:Minimum and is used by equipment such as Humidifier:Steam:Electric.
-
-- HumidityRatio     references and sets the "System Node Setpoint Humidity Ratio" property. This type of reference setpoint may be set using (no applicable setpoint managers at this time) and is used by equipment such as Controller:WaterCoil (with control variable    HumidityRatio   ).
-
-The system node properties listed above are all available as an Output:Variable to facilitate tracking these setpoints both at the reference node and the setpoint nodes.
-
-#### Field: Minimum Setpoint Temperature
-
-The minimum temperature (in <sup>o</sup>C) that is allowed by this setpoint manager. Applicable only if Control variable is Temperature.
-
-#### Field: Maximum Setpoint Temperature
-
-The maximum temperature (in <sup>o</sup>C) that is allowed by this setpoint manager. Applicable only if Control variable is Temperature.
-
-#### Field: Minimum Setpoint Humidity Ratio
-
-The minimum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager. Applicable only if Control variable is MaximumHumidityRatio, MinimumHumidityRatio, or HumidityRatio. Note that zero is not allowed as the computed setpoint humidity ratio, because zero is used as a special value to indicate that no humidification or dehumidification is needed. If the reference humidity ratio setpoint value is zero, the zero value will be passed directly to the Set Point Node(s).
-
-#### Field: Maximum Setpoint Humidity Ratio
-
-The maximum humidity ratio (kgWater/kgDryAir) that is allowed by this set point manager. Applicable only if Control variable is MaximumHumidityRatio, MinimumHumidityRatio, or HumidityRatio.
-
-#### Field: Reference Setpoint Node Name
-
-The name of an HVAC system node where the desired mixed air condition has been set. Normally this would be the mixed air node leaving the OutdoorAir:Mixer. The temperature or humidity setpoint at this reference node must be set by a different setpoint manager of the appropriate type (see Control Variable above).
-
-#### Field: Mixed Air Stream Node Name
-
-The name of the mixed air node. This node is used to obtain the flow rate of the combined air stream. This node is usually the same node at the Reference Setpoint Node Name, but does not have to be.
-
-#### Field: Outdoor Air Stream Node Name
-
-The name of a node in the outdoor air stream. This node is used to obtain the flow rate of the outdoor air stream.
-
-#### Field: Return Air Stream Node Name
-
-The name of a node in the return air stream. This node is used to obtain the flow rate of the return air stream.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature or humidity ratio setpoints will be established by this setpoint manager.
-
-Below is an example input for an Outdoor Air Pretreat Setpoint Manager.
-
-```idf
-SetpointManager:OutdoorAirPretreat,
-       DXSystem 1 Desiccant Set Point Manager,   !- Name
-       MaximumHumidityRatio,       !- Control Variable
-       -99,                                         !- Minimum Setpoint Temperature {C}
-       99,                                           !- Maximum Setpoint Temperature {C}
-       0.00001,                                 !- Minimum Setpoint Humidity Ratio (kgWater/kgDryAir)
-       1.0,                                         !- Maximum Setpoint Humidity Ratio (kgWater/kgDryAir)
-       DXSystem 1 Fan Air Inlet Node,   !- Reference Setpoint Node Name
-       DXSystem 1 Mixed Air Node,           !- Mixed Air Stream Node Name
-       Heat Recovery Outlet Node,           !- Outdoor Air Stream Node Name
-       DXSystem 1 Air Loop Inlet Node, !- Return Air Stream Node Name
-       Desiccant Process Outlet Node;   !- Setpoint Node or NodeList Name
-```
-
-
-### SetpointManager:Warmest
-
-The Warmest Setpoint Manager resets the cooling supply air temperature of a central forced air HVAC system according to the cooling demand of the warmest zone. For each zone in the system at each system timestep, the manager calculates a supply air temperature that will meet the zone cooling load at the maximum zone supply air flow rate. The lowest of the possible supply air temperatures becomes the new supply air temperature setpoint, subject to minimum and maximum supply air temperature constraints. The resulting temperature setpoint is the highest supply air temperature that will meet the cooling requirements of all the zones. When compared to a fixed cooling supply air temperature setpoint, this strategy minimizes zone reheat coil energy (or overcooling) and central chiller energy consumption (if the chilled water temperature is also reset) at the cost of possible increased fan energy.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a warmest setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. Currently there is only one choice: Temperature.
-
-#### Field: HVAC Air Loop Name
-
-The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its cooling supply air temperature.
-
-#### Field: Minimum Setpoint Temperature
-
-The minimum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is less than this minimum, the setpoint is set to the minimum.
-
-#### Field: Maximum Setpoint Temperature
-
-The maximum allowed setpoint temperature in degrees C. If the calculated setpoint is greater than this value the setpoint is set to the maximum. This value is also used as the setpoint temperature when none of the zones have a cooling load.
-
-#### Field: Strategy
-
-Currently, the only choice for this field is MaximumTemperature.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
-
-Below is an example input for a Warmest Setpoint Manager.
-
-```idf
-SetpointManager:Warmest,
-       Supply Air Temperature Manager 1,   !- Name
-       Temperature,   !- Control Variable
-       VAV Sys 1,   !- HVAC Air Loop Name
-       11.2,   !- Minimum Setpoint Temperature
-       16.,   !- Maximum Setpoint Temperature
-       MaximumTemperature,   !- Strategy
-       Supply Air Temp Nodes 1;   !- Setpoint Node or NodeList Name
-
-
-SetpointManager:MixedAir,
-       Mixed Air Temp Manager 1,   !- Name
-       Temperature,   !- Control Variable
-       VAV Sys 1 Outlet Node,   !- Reference Setpoint Node Name
-       Main Heating Coil 1 Outlet Node,   !- Fan Inlet Node Name
-       VAV Sys 1 Outlet Node,   !- Fan Outlet Node Name
-       Mixed Air Node 1;             !- Setpoint Node or NodeList Name
-
-
-NodeList, Supply Air Temp Nodes 1,
-       VAV Sys 1 Outlet Node; ! Setpoint Node
-```
-
-
-### SetpointManager:Coldest
-
-The Coldest Setpoint Manager is used in dual duct systems to reset the setpoint temperature of the air in the heating supply duct. Usually it is used in conjunction with a SetpointManager:Warmest resetting the temperature of the air in the cooling supply duct. For each zone in the system at each system timestep, the manager calculates a supply air temperature that will meet the zone heating load at the maximum zone supply air flow rate. The highest of the possible supply air temperatures becomes the new supply air temperature setpoint, subject to minimum and maximum supply air temperature constraints. The resulting temperature setpoint is the lowest supply air temperature that will meet the heating requirements of all the zones. When compared to a fixed heating supply air temperature setpoint, this strategy minimizes central boiler energy consumption (if the hot water temperature is also reset or there are variable speed pumps) at the cost of possible increased fan energy (if there is variable volume control in the air system).
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a coldest setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. Currently there is only one choice: Temperature.
-
-#### Field: HVAC Air Loop Name
-
-The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its heating supply air temperature.
-
-#### Field: Minimum Setpoint Temperature
-
-The minimum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is less than this minimum, the setpoint is set to the minimum. This value is also used as the setpoint temperature when none of the zones have a heating load.
-
-#### Field: Maximum Setpoint Temperature
-
-The maximum allowed setpoint temperature in degrees C. If the calculated setpoint is greater than this value the setpoint is set to the maximum.
-
-#### Field: Strategy
-
-Currently, the only choice for this field is MinimumTemperature.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
-
-Below is an example input for a Coldest Setpoint Manager.
-
-```idf
-   Controller:Simple,
-       Central Cooling Coil Controller 1,   !- Name
-       Temperature,   !- Control Variable
-       Reverse,   !- Action
-       Flow,         !- Actuator Variable
-       VAV Sys 1 Cold Outlet Node,                       !- Sensor Node Name
-       Main Cooling Coil 1 Water Inlet Node,   !- Actuator Node Name
-       0.001,       !- Controller Convergence Tolerance {deltaC}
-       autosize, !- Maximum Actuated Flow {m3/s}
-       0.0;           !- Minimum Actuated Flow {m3/s}
-
-
-   Controller:WaterCoil,
-       Central Heating Coil Controller 1,   !- Name
-       Temperature,   !- Control Variable
-       Normal,   !- Action
-       Flow,       !- Actuator Variable
-       VAV Sys 1 Hot Outlet Node,                         !- Sensor Node Name
-       Main Heating Coil 1 Water Inlet Node,   !- Actuator Node Name
-       0.001,         !- Controller Convergence Tolerance {deltaC}
-       autosize,   !- Maximum Actuated Flow {m3/s}
-       0.0;             !- Minimum Actuated Flow {m3/s}
-
-
-   SetpointManager:Warmest,
-       Supply Air Temperature Manager 1,   !- Name
-       Temperature,             !- Control Variable
-       VAV Sys 1,   !- HVAC Air Loop Name
-       11.2,             !- Minimum Setpoint Temperature {C}
-       16.,               !- Maximum Setpoint Temperature {C}
-       MaximumTemperature,             !- Strategy
-       Supply Air Temp Nodes 1;   !- Setpoint Node or NodeList Name
-
-
-   NodeList,
-       Supply Air Temp Nodes 1,         !- Name
-       VAV Sys 1 Cold Outlet Node;   !- Node 1 Name
-
-
-   SetpointManager:Coldest,
-       Supply Air Temperature Manager 2,   !- Name
-       Temperature,             !- Control Variable
-       VAV Sys 1,   !- HVAC Air Loop Name
-       25.,               !- Minimum Setpoint Temperature {C}
-       50.,               !- Maximum Setpoint Temperature {C}
-       MinimumTemperature,             !- Strategy
-       Supply Air Temp Nodes 2;   !- Setpoint Node or NodeList Name
-
-
-   NodeList,
-       Supply Air Temp Nodes 2,       !- Name
-       VAV Sys 1 Hot Outlet Node;   !- Node 1 Name
-```
-
-
-
-
-### SetpointManager:ReturnAirBypassFlow
-
-This manager is user in conjunction with a return air bypass configuration. This type of air system is basically a standard single duct system with the addition of a bypass duct that bypasses return air around the main system components     in particular, the central cooling coil. This allows the central cooling coil to sufficiently dehumidify the mixed air; the bypassed air is then added to the supply air stream to bring the supply air temperature up to the desired temperature set point. This scheme is very useful in situations where an higher than normal supply air temperature is used     for instance, in underfloor air distribution systems.
-
-This manager relies on the program to figure out the system configuration and to extract the needed data from the system nodes. All the user needs to input is the name of the air system and a schedule giving the desired supply air temperature setpoint. No node names are required. The manager will establish a bypass air flow rate that upon mixing with the non-bypassed air will yield the temperature given in the schedule.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of an Return Air Bypass Flow setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. Currently there is only one choice:   Flow.
-
-#### Field: HVAC Air Loop Name
-
-The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its return air bypass flow rate.
-
-#### Field: Temperature Setpoint Schedule Name
-
-The name of a schedule whose values are temperatures in   <sup>o</sup>C. The schedule value for the time period is the setpoint for this type of setpoint manager. The setpoint is assumed to be at the air handler outlet.
-
-The following shows an example input for SetpointManager:ReturnAirBypassFlow.
-
-```idf
-SetpointManager:ReturnAirBypassFlow,
-       RETURN AIR BYPASS Manager 1,   !- Name
-       Flow,   !- Control Variable
-       VAV Sys 1,   !- HVAC Air Loop Name
-       Seasonal Reset Supply Air Temp Sch;   !- Temperature Setpoint Schedule Name
-```
-
-### SetpointManager:WarmestTemperatureFlow
-
-The Warmest Temperature Flow Setpoint Manager resets the cooling supply air temperature of a central forced air HVAC system according to the cooling demand of the warmest zone. The user can select one of two strategies: *TemperatureFirst* or *FlowFirst*.
-
-For *TemperatureFirst* the manager tries to find the highest setpoint temperature that will satisfy all the zone cooling loads at minimum supply air flow rate. If this setpoint temperature is less than the minimum, the setpoint temperature is set to the minimum, and the supply air flow rate is increased to meet the loads.
-
-For *FlowFirst* the manager tries to find the lowest supply air flow rate that will satisfy all the zone cooling loads at the maximum setpoint temperature. If this flow is greater than the maximum, the flow is set to the maximum and the setpoint temperature is reduced to satisfy the cooling loads.
-
-When compared to a fixed cooling supply air temperature setpoint, the *TemperatureFirst* strategy minimizes fan energy at the cost of possible increased zone reheat coil energy (or overcooling) and central chiller energy consumption, whereas the *FlowFirst* strategy minimizes zone reheat coil energy (or overcooling) and central chiller energy consumption at the cost of possible increased fan energy.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of this setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled. For this setpoint manager, this input should be Temperature.
-
-#### Field: HVAC Air Loop Name
-
-he name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its cooling supply air temperature.
-
-#### Field: Minimum Setpoint Temperature
-
-The minimum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is less than this minimum, the setpoint is set to the minimum.
-
-#### Field: Maximum Setpoint Temperature
-
-The maximum allowed setpoint temperature in degrees C. If the calculated setpoint is greater than this value the setpoint is set to the maximum. This value is also used as the setpoint temperature when none of the zones have a cooling load.
-
-#### Field: Strategy
-
-The choices for this field are *TemperatureFirst* and *FlowFirst*. See discussion above for a description of what each strategy does.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which temperature setpoints will be established by this setpoint manager.
-
-#### Field: Minimum Turndown Ratio
-
-The minimum value of the ratio of the actual air flow rate to the maximum air flow rate, either for the supply fan if there are no VAV terminal boxes, or for the VAV boxes if present.   If there are VAV boxes, it is assumed that the same value of minimum turndown applies to all boxes.
-
-Below is an example input for a SetpointManager:WarmestTemperatureFlow object.
-
-```idf
-SetpointManager:WarmestTemperatureFlow,
-       Supply Air Temperature Manager 1,   !- Name
-       Temperature,   !- Control Variable
-       VAV Sys 1,   !- HVAC Air Loop Name
-       11.2,   !- Minimum Setpoint Temperature
-       16.,     !- Maximum Setpoint Temperature
-       TemperatureFirst,   !- Strategy
-       Supply Air Temp Nodes 1,   !- Setpoint Node or NodeList Name
-       0.3;   !- Minimum Turndown Ratio
-
-
-SetpointManager:MixedAir,
-       Mixed Air Temp Manager 1,   !- Name
-       Temperature,   !- Control Variable
-       VAV Sys 1 Outlet Node,   !- Reference Setpoint Node Name
-       Main Heating Coil 1 Outlet Node,   !- Fan Inlet Node Name
-       VAV Sys 1 Outlet Node,   !- Fan Outlet Node Name
-       Mixed Air Node 1;   !- Setpoint Node or NodeList Name
-
-
-NodeList, Supply Air Temp Nodes 1,
-       VAV Sys 1 Outlet Node; ! Set Point Node
-```
-
-
-### SetpointManager:WarmestTemperatureFlow Outputs
-
-#### Setpoint Manager Warmest Temperature Critical Zone Number []
-
-This is the number of the zone that was the critical zone for the setpoint manager.
-
-#### Setpoint Manager Warmest Temperature Turndown Flow Fraction []
-
-This is the fraction that flow was reduced by the setpoint manager.   This is the actual air flow rate divided by the maximum air flow rate.
-
-### SetpointManager:MultiZone:Cooling:Average
-
-This setpoint manager is used to establish a supply air temperature setpoint for a central forced air HVAC system (air loop) based on the predicted sensible cooling loads and actual supply air mass flow rates for all zones served by the system. For all controlled zones in the air loop (i.e., zones with a thermostat object), the setpoint manager calculates an average supply air temperature that will meet the zone cooling loads based on the actual zone supply air mass flow rates (lagged by one time step). The calculated setpoint temperature is subject to the minimum and maximum setpoint temperature constraints specified by the user. When compared to a fixed cooling supply air temperature setpoint, this strategy may reduce zone reheat coil energy (or overcooling) and central chiller energy consumption (if the chilled water temperature is also reset) at the cost of possible increased fan energy.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of this multizone average cooling setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: HVAC Air Loop Name
-
-The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its cooling supply air temperature.
-
-#### Field: Minimum Setpoint Temperature
-
-The minimum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is less than this minimum, the setpoint is set to the minimum. The default value is 12C.
-
-#### Field: Maximum Setpoint Temperature
-
-The maximum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is greater than this value, the setpoint is set to this maximum value. The default value is 18C.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which temperature setpoints will be established by this setpoint manager.
-
-Below is an example of this object in an input file.
-
-```idf
-   SetpointManager:MultiZone:Cooling:Average,
-       Cooling Coil Air Sys Branch Set Point,   !- Name
-       Main Dual Duct Air Loop, !- HVAC Air Loop Name
-       12.0,                                       !- Minimum Setpoint Temperature {C}
-       22.0,                                       !- Maximum Setpoint Temperature {C}
-       Cooling Coil Supply Air Temp Nodes;   !- Setpoint Node or NodeList Name
-```
-
-
-
-
-### SetpointManager:MultiZone:Heating:Average
-
-This setpoint manager is used to establish a supply air temperature setpoint for a central forced air HVAC system (air loop) based on the predicted sensible heating loads and actual supply air mass flow rates for all zones served by the system. For all controlled zones in the air loop (i.e., zones with a thermostat object), the setpoint manager calculates an average supply air temperature that will meet the zone heating loads based on the actual zone supply air mass flow rates (lagged by one time step). The calculated setpoint temperature is subject to the minimum and maximum setpoint temperature constraints specified by the user. When compared to a fixed heating supply air temperature setpoint, this strategy may reduce central boiler energy consumption (if the hot water temperature is also reset or there are variable speed pumps) at the cost of possible increased fan energy (if there is variable volume control for the air system).
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a multizone average heating setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: HVAC Air Loop Name
-
-The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its heating supply air temperature.
-
-#### Field: Minimum Setpoint Temperature
-
-The minimum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is less than this minimum, the setpoint is set to the minimum. The default value is 20C.
-
-#### Field: Maximum Setpoint Temperature
-
-The maximum allowed setpoint temperature in degrees C. If the calculated setpoint temperature is greater than this value, the setpoint is set to this maximum value. The default value is 50C.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which temperature setpoints will be established by this setpoint manager.
-
-Below is an example of this object in an input file.
-
-```idf
-   SetpointManager:MultiZone:Heating:Average,
-       Heating Coil Air Sys Branch Set Point,   !- Name
-       Main Dual Duct Air Loop, !- HVAC Air Loop Name
-       24.0,                                       !- Minimum Setpoint Temperature {C}
-       41.0,                                       !- Maximum Setpoint Temperature {C}
-       Heating Coil Supply Air Temp Nodes;   !- Setpoint Node or NodeList Name
-```
-
-
-
-### SetpointManager:MultiZone:MinimumHumidity:Average
-
-This setpoint manager allows for controlling the minimum humidity level is multiple zones served by a central forced air HVAC system (air loop). This setpoint manager, used in conjunction with one or more ZoneControl:Humidistat objects, detects the air humidity level in multiple controlled zones served by the HVAC air loop and uses air/moisture mass balances to calculate an average supply air humidity ratio needed to maintain the zone relative humidity levels near their respective humidifying setpoints. The calculated humidity ratio is then used as the minimum humidity ratio setpoint for the designated setpoint node(s). A humidification component (e.g., Humidifier:Steam:Electric) placed upstream of the setpoint node can then use the minimum humidity ratio setpoint to control humidification rate. The use of this object requires that a    ZoneControl:Humidistat    object be specified with a humidifying relative humidity schedule for one or more controlled zones served by the HVAC air loop.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of an average minimum humidity (humidifying) multizone setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: HVAC Air Loop Name
-
-The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its humidification setpoint (minimum air humidity ratio).
-
-#### Field: Minimum Setpoint Humidity Ratio
-
-The minimum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager.   If the calculated setpoint humidity ratio is less than this value, then the setpoint is set to this minimum value. The default value is 0.005 (kgWater/kgDryAir).
-
-#### Field: Maximum Setpoint Humidity Ratio
-
-The maximum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager.   If the calculated setpoint humidity ratio is greater than this value, then the setpoint is set to this maximum value. The default value is 0.012 (kgWater/kgDryAir).
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which humidity ratio setpoints will be established by this setpoint manager.
-
-An example of this object in an input data file (IDF), along with a humidistat object, is shown below.
-
-```idf
-SetpointManager:MultiZone:MinimumHumidity:Average,
-   VAV_1 Humidifier HUMRAT setpoint, !- Name
-   VAV_1,                                                       !- HVAC Air Loop Name
-   0.003,                                                       !- Minimum Setpoint Humidity Ratio (kgWater/kgDryAir)
-   0.012,                                                       !- Maximum Setpoint Humidity Ratio (kgWater/kgDryAir)
-   VAV_1 Humidifier-Outlet Nodes List;           !- Setpoint Node or NodeList Name
-
-
-ZoneControl:Humidistat,
-   ICU_NURSESTN_LOBBY_FLR_2 Humidistat,   !- Name
-   ICU_NURSESTN_LOBBY_FLR_2,   !- Zone Name
-   MinRelHumSetSch,   !- Humidifying Relative Humidity Setpoint Schedule Name
-   MaxRelHumSetSch;   !- Dehumidifying Relative Humidity Setpoint Schedule Name
-```
-
-
-### SetpointManager:MultiZone:MaximumHumidity:Average
-
-This setpoint manager allows for controlling the maximum humidity level is multiple zones served by a central forced air HVAC system (air loop). This setpoint manager, used in conjunction with one or more ZoneControl:Humidistat objects, detects the air humidity level in multiple controlled zones served by the HVAC air loop and uses air/moisture mass balances to calculate an average supply air humidity ratio needed to maintain the zone relative humidity levels near their respective dehumidifying setpoints. The calculated humidity ratio is then used as the maximum humidity ratio setpoint for the designated setpoint node(s). A dehumidification component (e.g., desiccant dehumidifiers) placed upstream of the setpoint node can then use the maximum humidity ratio setpoint to control its moisture removal rate. The use of this object requires that a    ZoneControl:Humidistat    object be specified with a dehumidifying relative humidity schedule for one or more controlled zones served by the HVAC air loop.
-
-In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determine the supply air temperature required to meet both the temperature (sensible) and humidity (latent) load in the control zone. See object Controller:WaterCoil in the EnergyPlus Engineering Reference for a detailed discussion of how this is achieved.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of an average maximum humidity ratio (dehumidifying) multizone setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: HVAC Air Loop Name
-
-The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its dehumidification setpoint (maximum air humidity ratio).
-
-#### Field: Minimum Setpoint Humidity Ratio
-
-The minimum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager.   If the calculated setpoint humidity ratio is less than this value, then the setpoint is set to this minimum value. The default value is 0.008 (kgWater/kgDryAir).
-
-#### Field: Maximum Setpoint Humidity Ratio
-
-The maximum humidity ratio (kgWater/kgDryAir) that is allowed by this set point manager.   If the calculated setpoint humidity ratio is greater than this value, then the setpoint is set to this maximum value. The default value is 0.015 (kgWater/kgDryAir).
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which humidity ratio setpoints will be established by this setpoint manager.
-
-An example of this object in an input data file (IDF), along with a humidistat object, is shown below:
-
-```idf
-SetpointManager:MultiZone:MaximumHumidity:Average,
-   VAV_1_CoolC HUMRAT setpoint,           !- Name
-   VAV_1,                                                       !- HVAC Air Loop Name
-   0.005,                                                       !- Minimum Setpoint Humidity Ratio (kgWater/kgDryAir)
-   0.015,                                                       !- Maximum Setpoint Humidity Ratio (kgWater/kgDryAir)
-   VAV_1 DeHumidifier-Outlet Nodes List;       !- Setpoint Node or NodeList Name
-
-
-ZoneControl:Humidistat,
-   ICU_NURSESTN_LOBBY_FLR_2 Humidistat,   !- Name
-   ICU_NURSESTN_LOBBY_FLR_2,   !- Zone Name
-   MinRelHumSetSch,   !- Humidifying Relative Humidity Setpoint Schedule Name
-   MaxRelHumSetSch;   !- Dehumidifying Relative Humidity Setpoint Schedule Name
-```
-
-
-### SetpointManager:MultiZone:Humidity:Minimum
-
-This setpoint manager allows for controlling the minimum humidity level in multiple zones served by a central forced air HVAC system (air loop). This setpoint manager, used in conjunction with one or more ZoneControl:Humidistat objects, detects the air humidity level in multiple controlled zones served by the HVAC air loop and uses air/moisture mass balances to calculate a supply air minimum humidity ratio based on   a zone with the critical   humidification requirement (i.e., a zone with the highest humidity ratio setpoint) to maintain the zone relative humidity levels near their respective humidifying setpoints. The calculated humidity ratio is then used as the minimum humidity ratio setpoint for the designated setpoint node(s). A humidification component (e.g., Humidifier:Steam:Electric) placed upstream of the setpoint node can then use the minimum humidity ratio setpoint to control humidification rate. The use of this object requires that a    ZoneControl:Humidistat    object be specified with a humidifying relative humidity schedule for one or more controlled zones served by the HVAC air loop.   If    ZoneControl:Humidistat    object is defined for only one of the zones served by the air loop then the SetpointManager:MultiZone:Humidity:Minimum perform as SepointManager:SingleZone:Humidity:Minimum.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a multizone minimum humidity (humidifying) setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: HVAC Air Loop Name
-
-The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its humidification setpoint (minimum air humidity ratio).
-
-#### Field: Minimum Setpoint Humidity Ratio
-
-The minimum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager.   If the calculated setpoint humidity ratio is less than this value, then the setpoint is set to this minimum value. The default value is 0.005 (kgWater/kgDryAir).
-
-#### Field: Maximum Setpoint Humidity Ratio
-
-The maximum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager.   If the calculated setpoint humidity ratio is greater than this value, then the setpoint is set to this maximum value. The default value is 0.012 (kgWater/kgDryAir).
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which humidity ratio setpoints will be established by this setpoint manager.
-
-An example of this object in an input data file (IDF), along with a humidistat object, is shown below.
-
-```idf
-SetpointManager:MultiZone:Humidity:Minimum,
-       Main Humidifier setpoint Mgr,     !- Name
-       VAV Sys 1,                                           !- HVAC Air Loop Name
-       0.003,                                                   !- Minimum Setpoint Humidity Ratio (kgWater/kgDryAir)
-       0.015,                                                   !- Maximum Setpoint Humidity Ratio (kgWater/kgDryAir)
-       Main Humidifier Outlet Node;       !- Setpoint Node or NodeList Name
-
-
-ZoneControl:Humidistat,
-       Space5-1 Humidistat,         !- Name
-       SPACE5-1,                               !- Zone Name
-       HumidifyingHumSetSch,       !- Humidifying Relative Humidity Setpoint Schedule Name
-       DehumidifyingHumSetSch;   !- Dehumidifying Relative Humidity Setpoint Schedule Name
-```
-
-
-### SetpointManager:MultiZone:Humidity:Maximum
-
-This setpoint manager allows for controlling the maximum humidity level in multiple zones served by a central forced air HVAC system (air loop). This setpoint manager, used in conjunction with one or more ZoneControl:Humidistat objects, detects the air humidity level in multiple controlled zones served by the HVAC air loop and uses air/moisture mass balances to calculate the maximum supply air humidity ratio based on   a zone with the critical dehumidification requirement (i.e., a zone with the lowest humidity ratio setpoint) to maintain the zone relative humidity levels near their respective dehumidifying setpoints. The calculated humidity ratio is then used as the maximum humidity ratio setpoint for the designated setpoint node(s). A dehumidification component (e.g., desiccant dehumidifiers) placed upstream of the setpoint node can then use the maximum humidity ratio setpoint to control its moisture removal rate. The use of this object requires that a    ZoneControl:Humidistat    object be specified with a dehumidifying relative humidity schedule for one or more controlled zones served by the HVAC air loop. If    ZoneControl:Humidistat    object is defined for only one of the zones served by the air loop then the SetpointManager:MultiZone:Humidity:Maximum perform as SetpointManager:SingleZone:Humidity:Maximum.
-
-In the case of a chilled water coil which is used for both temperature and high humidity control, this setpoint manager works in conjunction with a Controller:WaterCoil object to determine the supply air temperature required to meet both the temperature (sensible) and dehumidification (latent) load in the control zone. See object Controller:WaterCoil in the EnergyPlus Engineering Reference for a detailed discussion of how this is achieved.
-
-#### Field: Name
-
-A unique, user-assigned name for an instance of a multizone maximum humidity ratio (dehumidifying) setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: HVAC Air Loop Name
-
-The name of the AirLoopHVAC object (the central air system) which will use this setpoint manager to set its dehumidification setpoint (maximum air humidity ratio).
-
-#### Field: Minimum Setpoint Humidity Ratio
-
-The minimum humidity ratio (kgWater/kgDryAir) that is allowed by this setpoint manager.   If the calculated setpoint humidity ratio is less than this value, then the setpoint is set to this minimum value. The default value is 0.008 (kgWater/kgDryAir).
-
-#### Field: Maximum Setpoint Humidity Ratio
-
-The maximum humidity ratio (kgWater/kgDryAir) that is allowed by this set point manager.   If the calculated setpoint humidity ratio is greater than this value, then the setpoint is set to this maximum value. The default value is 0.015 (kgWater/kgDryAir).
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes, or the HVAC System Node Name, for which humidity ratio setpoints will be established by this setpoint manager.
-
-An example of this object in an input data file (IDF), along with a humidistat object, is shown below.
-
-
-
-```idf
-   SetpointManager:MultiZone:Humidity:Maximum,
-       Maximum Mzone HUMRAT setpoint,   !- Name
-       VAV Sys 1,                                           !- HVAC Air Loop Name
-       0.003,                                                   !- Minimum Setpoint Humidity Ratio (kgWater/kgDryAir)
-       0.015,                                                   !- Maximum Setpoint Humidity Ratio (kgWater/kgDryAir)
-       DeHumidifier-Outlet Nodes;           !- Setpoint Node or NodeList Name
-
-
-ZoneControl:Humidistat,
-       Space5-1 Humidistat,         !- Name
-       SPACE5-1,                               !- Zone Name
-       HumidifyingHumSetSch,       !- Humidifying Relative Humidity Setpoint Schedule Name
-```
-
-
-### SetpointManager:FollowOutdoorAirTemperature
-
-This setpoint manager is used to place a temperature setpoint on a system node that is derived from the current outdoor air environmental conditions.   The outdoor air conditions are obtained from the weather information during the simulation.
-
-#### Field: Name
-
-A unique user-defined name for an instance of this setpoint manager.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled.   There are three choices available: Temperature, MaximumTemperature, or MinimumTemperature.
-
-#### Field: Reference Temperature Type
-
-The field specifies the type of temperature value to obtain from the system node referenced in the previous field.   The two available options are OutdoorDryBulb and OutdoorWetBulb.
-
-#### Field: Offset Temperature Difference
-
-This field provides a temperature offset that will be applied to the value of the reference temperature (outdoor air wetbulb/drybulb).   If this value is zero, and the limits are met, then the resulting setpoint will be exactly the same as the outdoor air wetbulb/drybulb temperature.   The sign convention is that a positive value here will increase the resulting setpoint to higher than the outdoor air wetbulb/drybulb.
-
-#### Field: Maximum Setpoint Temperature
-
-This field provides an upper limit to the resulting setpoint value.
-
-#### Field: Minimum Setpoint Temperature
-
-This field provides a lower limit to the resulting setpoint value.
-
-#### Field: Setpoint Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which setpoints will be established by this setpoint manager.
-
-An IDF example of use:
-
-```idf
-SetpointManager:FollowOutdoorAirTemperature,
-   MyCondenserControl,         !- Name
-   Temperature,                       !- Control Variable
-   OutdoorAirDryBulb,           !- Reference Temperature Type
-   0.5,                                       !- Offset Temperature Difference {deltaC}
-   200,                                       !- Maximum Setpoint Temperature {C}
-   21.1,                                     !- Minimum Setpoint Temperature {C}
-   CondSupplyOutletNode;     !- Setpoint Node or NodeList Name
-```
-
-
-### SetpointManager:FollowSystemNodeTemperature
-
-This setpoint manager is used to place a temperature setpoint on a system node that is derived from the current temperatures at a separate system node.   The current value of the temperature at a reference node is obtained and used to generate setpoint on a second system node.   If the reference node is also designated to be an outdoor air (intake) node, then this setpoint manager can be used to follow outdoor air conditions that are adjusted for altitude.
-
-#### Field: Name
-
-A unique user-defined name for an instance of this setpoint manager.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled.   There are three choices available: Temperature, MaximumTemperature, or MinimumTemperature.
-
-#### Field: Reference Node Name
-
-The name of a system node where this setpoint manager will obtain a reference temperature to follow.   Note that the temperature to obtained is the current temperature on the node and not the current value of a temperature *setpoint*.
-
-#### Field: Reference Temperature Type
-
-The field specifies the type of temperature value to obtain from the system node referenced in the previous field.   The two available options are NodeDryBulb and NodeWetBulb.
-
-#### Field: Offset Temperature Difference
-
-This field provides a temperature offset that will be applied to the value obtained from the reference system node.   If this value is zero, and the limits are met, then the resulting setpoint will be exactly the same as the reference system node temperature.   The sign convention is that a positive value here will increase the resulting setpoint to higher than the temperature at the reference node.
-
-#### Field: Maximum Limit Setpoint Temperature
-
-This field provides an upper limit to the resulting setpoint value.
-
-#### Field: Minimum Limit Setpoint Temperature
-
-This field provides a lower limit to the resulting setpoint value.
-
-#### Field: Setpoint System Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which setpoints will be established by this setpoint manager.
-
-An IDF example of use:
-
-```idf
-SetpointManager:FollowSystemNodeTemperature,
-   MyCondenserControl,         !- Name
-   Temperature,                       !- Control Variable
-   MyOAinletNode,                   !- Reference Node Name
-   NodeDryBulb,                       !- Reference Temperature Type
-   0.5,                                       !- Offset Temperature Difference {deltaC}
-   200,                                       !- Maximum Setpoint Temperature {C}
-   24.0,                                     !- Minimum Setpoint Temperature {C}
-   CondSupplyOutletNode;     !- Setpoint Node or NodeList Name
-```
-
-
-### SetpointManager:FollowGroundTemperature
-
-This setpoint manager is used to place a temperature setpoint on a system node that is derived from a current ground temperature.   The ground temperatures are specified in different Site:GroundTemperature:\* objects and used during the simulation.   This setpoint manager is primarily intended for condenser or plant loops using some type of ground heat exchanger.
-
-#### Field: Name
-
-A unique user-defined name for an instance of this setpoint manager.
-
-#### Field: Control Variable
-
-The type of variable that will be controlled.   There are three choices available: Temperature, MaximumTemperature, or MinimumTemperature.
-
-#### Field: Reference Ground Temperature Object Type
-
-This field is used to specify the type of ground temperature to be used by the setpoint manager.   There are four options, Site:GroundTemperature:BuildingSurface, Site:GroundTemperature:Shallow, Site:GroundTemperature:Deep, or Site:GroundTemperature:FCfactorMethod.   Generally the deep ground temperatures are the most useful for a plant loop serving a vertical borehole ground heat exchanger.
-
-#### Field: Offset Temperature Difference
-
-This field provides a temperature offset that will be applied to the value of the ground temperature.   If this value is zero, and the limits are met, then the resulting setpoint will be exactly the same as the ground temperature.   The sign convention is that a positive value here will increase the resulting setpoint to higher than the ground temperature.
-
-#### Field: Maximum Setpoint Temperature
-
-This field provides an upper limit to the resulting setpoint value.
-
-#### Field: Minimum Setpoint Temperature
-
-This field provides a lower limit to the resulting setpoint value.
-
-#### Field: Setpoint System Node or NodeList Name
-
-The name of a NodeList object containing the names of the HVAC system nodes or the HVAC System Node Name for which setpoints will be established by this setpoint manager.
-
-An IDF example of use:
-
-```idf
-SetpointManager:FollowGroundTemperature,
-   MyCondenserControl,                   !- Name
-   Temperature,                                 !- Control Variable
-   Site:GroundTemperature:Deep, !- Reference Ground Temperature Object Type
-   1.5,                                                 !- Offset Temperature Difference {deltaC}
-   50.0,                                               !- Maximum Setpoint Temperature {C}
-   10.0,                                               !- Minimum Setpoint Temperature {C}
-   CondSupplyOutletNode;               !- Setpoint Node or NodeList Name
-```
-
-
-### SetpointManager:CondenserEnteringReset
-
-The object resets the condenser entering water temperature setpoint to the optimal setpoint temperature that will result in minimum net energy consumption for the chiller and cooling tower plant. This chiller-tower optimization scheme uses one curve to determine the optimum condenser entering water temperature for a given time step and two other curves to place limit conditions on the optimized setpoint value. Note that this object will work with only one cooling tower object in a plant loop.
-
-#### Field: Name
-
-A unique, user assigned name for an instance of the optimized condenser entering water setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control variable
-
-The type of variable that will be controlled. The only valid choice for this setpoint manager is **Temperature**.
-
-#### Field: Default Condenser Entering Water Temperature Schedule Name
-
-This schedule should define the default condenser entering water temperature setpoint. This scheduled setpoint value is only used in a given time step if the optimized setpoint value (see the Optimized Condenser Entering Water Temperature Curve Name field) does not fall within its prescribed boundary conditions.
-
-#### Field: Minimum Design Wetbulb Temperature Curve Name
-
-The curve name associated with the coefficients in the equation used to determine the minimum design tower wetbulb referenced by the minimum outside air wetbulb temperature curve below.   The value from this curve is compared to the tower design wet bulb each timestep to establish one of the governing boundaries over the optimized condenser entering water temperature setpoint calculation.   This curve must be quad-linear (Curve:QuadLinear) and is defined as:
-
-<div>\[T = {C_1} + {C_2}\cdot OaWb + {C_3}\cdot WPLR + {C_4}TwrWb + {C_5}NF\]</div>
-
-where,
-
-OaWb = Outside air wet bulb for current timestep, ËšC
-
-WPLR = Weighted Part Load Ratio, dimensionless
-
-TwrWb = Design tower wet bulb boundary condition, ËšC
-
-NF = Normalized condenser water flow per unit of tower capacity, m3/s-W
-
-#### Field: Minimum Outside Air Wetbulb Temperature Curve Name
-
-The curve name associated with the coefficients in the equation used to determine the minimum actual wetbulb referenced by the optimized condenser entering water temperature curve. The value from this curve is compared the actual outside wet bulb each timestep to establish one of the governing boundaries over the optimized condenser entering water temperature setpoint calculation.   This curve must be quad-linear (Curve:QuadLinear) and is defined as:
-
-<div>\[T = {C_1} + {C_2}\cdot MinWb + {C_3}\cdot WPLR + {C_4}\cdot TwrWb + {C_5}NF\]</div>
-
-Where
-
-  MinWb = Minimum design wetbulb for current timestep, ËšC
-
-WPLR = Weighted Part Load Ratio, dimensionless
-
-TwrWb = Design tower wet bulb boundary condition, ËšC
-
-NF = Normalized condenser water flow per unit of tower capacity, m3/s-W
-
-#### Field: Optimized Condenser Entering Temperature Curve Name
-
-The curve name associated with the coefficients in the optimized condenser entering water temperature equation. The value from this curve is used to calculate the optimized condenser entering water temperature for each timestep. If this optimized setpoint does not fall within the bounds established by the two boundary conditions, then the value from the Default Condenser Entering Water Temperature Schedule is used for the Condenser Entering Water Setpoint for that timestep.  This curve must be quad-linear (Curve:QuadLinear) and is defined as:
-
-<div>\[T = {C_1} + {C_2}OaWb + {C_3}WPLR + {C_4}TwrWb + {C_5}NF\]</div>
-
-where,
-
-OaWb = Outside air wet bulb for current timestep, ËšC
-
-WPLR = Weighted Part Load Ratio, dimensionless
-
-TwrWb = Design tower wet bulb boundary condition, ËšC
-
-NF = Normalized condenser water flow per unit of tower capacity, m3/s-W
-
-#### Field: Minimum Lift
-
-This field establishes the minimum Lift allowed.  Lift is generally thought of as the difference between condenser refrigerant pressure and the evaporator refrigerant pressure. Using defined pressure and temperature relationships, lift also can be related to the difference between the leaving chilled water and the leaving condenser water temperature. Further, when the leaving condenser water temperature and condenser water flow are constant, the entering condenser temperature can be used as a proxy for lift. Because most condenser water systems are designed for constant flow, entering condenser temperature is the most common metric for lift, and that is what meant here. If the calculated Condenser Entering Water Setpoint falls below (TEvapLvgWater+ MinimumLift), then the Condenser Entering Water Setpoint is reset to equal TEvapLvgWater+ MinimumLift. The units for this field are deg C TD. Default is 11.1 ËšC (20 F).
-
-#### Field: Maximum Condenser Entering Temperature
-
-This field establishes the maximum condenser entering water setpoint temperature allowed.   If the scheduled or calculated setpoint is above TCondEntMax, then TCondEntSetpoint is reset to equal TCondEntMax. The units for this field are deg C.
-
-#### Field: Cooling Tower Design Inlet Air Wet-Bulb Temperature
-
-This field defines the reference wet bulb temperature used to size the cooling tower. Typically, the design condenser entering water temperature equals TwrRefOaWb + TowerApproachTD. The units for this field are deg C.
-
-#### Field: Setpoint Node or Node List Name
-
-This field defines the condenser node being controlled.
-
-Below is an example input for a CondenserEnteringReset Setpoint Manager.
-
-```idf
-SetpointManager:CondenserEnteringReset,
-       Condenser Optimized Setpoint Manager,   !- Name
-       Temperature,                   !- Control Variable
-       DefaultCondEntSch,       !- Default Condenser Entering Water Temperature Schedule Name
-       MinDsnWBCurveName,       !- Minimum Design Wetbulb Temperature Curve Name
-       MinActWBCurveName,       !- Minimum Outside Air Wetbulb Temperature Curve Name
-       OptCondEntCurveName,   !- Optimized Cond Entering Water Temperature Curve Name
-       12,                                     !- Minimum Lift, C
-       32,                                     !- Maximum Condenser Entering Water Temp, C
-       25.56,                               !- Cooling Tower Design Inlet Air Wetbulb Temperature, C
-       Cond Water Setpoint Node;   !- Setpoint Node or Node List Name
-```
-
-
-### SetpointManager:CondenserEnteringReset:Ideal
-
-The object determines a near-optimal condenser water entering setpoint at each time step that will result in minimum net energy consumption for the chiller and coolingtower plant. The    ideal    chiller-tower optimization scheme uses a search algorithm to find the ideal optimal setpoint at a given timestep. Note that this object will work with only one chiller object and only one cooling tower object in a plant loop.
-
-#### Field: Name
-
-A unique, user assigned name for an instance of the optimized condenser entering water setpoint manager. Anywhere in the input that this setpoint manager is used, it is referred to by this name.
-
-#### Field: Control variable
-
-The type of variable that will be controlled. There is only one choice for this type of setpoint manager: **Temperature**.
-
-#### Field: Minimum Lift
-
-This field establishes the minimum lift allowed.   Lift is generally thought of as the difference between condenser refrigerant pressure and the evaporator refrigerant pressure. Using defined pressure and temperature relationships, lift also can be related to the difference between the leaving chilled water and the leaving condenser water temperature. Further, when the leaving condenser water temperature and condenser water flow are constant, the entering condenser temperature can be used as a proxy for lift. Because most condenser water systems are designed for constant flow, entering condenser temperature is the most common metric for lift, and that is what meant here. If the    optimized    condenser entering water setpoint falls below leaving evaporator water temperature plus minimum lift, then the condenser entering water setpoint is reset to equal this field value plus leaving evaporator water temperature. This determines the minimum boundary of condenser entering water setpoint. The unit for this field is deg C TD. Default is 11.1 deg C (20 deg F).
-
-#### Field: Maximum Condenser Entering Water Temperature
-
-This field establishes the maximum condenser entering water setpoint temperature allowed.   If the    optimized    condenser entering water setpoint is above this field value, then the condenser entering water setpoint is reset to equal this filed value. The units for this field are deg C. Default is 34 deg C
-
-#### Field: Setpoint Node or Node List Name
-
-This field defines the condenser node being controlled.
-
-Below is an example input for a IdealCondenserEnteringReset Setpoint Manager.
-
-```idf
-SetpointManager:CondenserEnteringReset:Ideal,
-       Condenser Optimized Setpoint Manager,   !- Name
-       Temperature,                   !- Control Variable
-       12,                                     !- Minimum Lift, C
-       32,                                     !- Maximum Condenser Entering Water Temp, C
-       Cond Water Setpoint Node;   !- Setpoint Node or Node List Name
-```
-
-
-### SetpointManager:SingleZone:OneStageCooling
-
-The singe-zone, one-stage cooling setpoint manager allows a component to be controlled based on thermostatic control using the object ZoneControl:Thermostat:StagedDualSetpoint.   This setpoint manager differs from other parts of EnergyPlus that control based on predicted loads to setpoint.   This setpoint manager allows modeling on/off cycling of DX coils using CoilSystem:Cooling:DX in continuous fan air handlers.   This setpoint manger detects if the zone is calling for a cooling stage and applies one setpoint value if cooling is called for and another setpoint value if cooling is not called for.
-
-This method of control is much more like real world thermostatic control but it requires short zone timesteps.   Models using this type of control should use 60 timesteps per hour and will run much slower because of that.
-
-#### Field: Name
-
-This alpha field is a unique, user-assigned name for an instance of a single zone one stage cooling setpoint manager.
-
-#### Field: Cooling Stage On Supply Air Setpoint Temperature
-
-This numeric field is the setpoint temperature to apply when the manager intends to turn on cooling, in degrees Celsius.   The default is -99.0 &deg;C.
-
-#### Field: Cooling Stage Off Supply Air Setpoint Temperature
-
-This numeric field is the setpoint temperature to apply when the manager intends to turn off cooling, in degrees Celsius.   The value in this field must be higher than the value in the previous field.   The default is 99.0 &deg;C.
-
-#### Field: Control Zone Name
-
-This alpha field is the name of the control zone for this setpoint manager.   This zone needs to be controlled using ZoneControl:Thermostat:StagedDualSetpoint.
-
-#### Field: Setpoint Node or NodeList Name
-
-This alpha field is the name of a NodeList objet containing the names of the HVAC system nodes, or the name of a system node, for which temperature setpoints will be established by this setpoint manager.
-
-
-
-An example input follows.
-
-```idf
-SetpointManager:SingleZone:OneStageCooling,
-       ZSF2 cooling on_off , !- Name
-       -99.0 , !- Cooling Stage On Supply Air Setpoint Temperature
-       99.0 , !- Cooling Stage Off Supply Air Setpoint Temperature
-       ZSF2 , !- Control Zone Name
-       DX Cooling Coil 3 Outlet Node ; !- Setpoint Node or NodeList Name
-```
-
-### SetpointManager:SingleZoneOneStageHeating
-
-The singe-zone, one-stage heating setpoint manager allows a component to be controlled based on thermostatic control using the object ZoneControl:Thermostat:StagedDualSetpoint.   This setpoint manager differs from other parts of EnergyPlus that control based on predicted loads to setpoint.   This setpoint manager allows modeling on/off cycling of heating coils in continuous fan air handlers.   This setpoint manger detects if the zone is calling for a heating stage and applies one setpoint value if heating is called for and another setpoint value if heating is not called for.
-
-This method of control is much more like real world thermostatic control but it requires short zone timesteps.   Models using this type of control should use 60 timesteps per hour and will run much slower because of that.
-
-#### Field: Name
-
-This alpha field is a unique, user-assigned name for an instance of a single zone one stage heating setpoint manager.
-
-#### Field: Heating Stage On Supply Air Setpoint Temperature
-
-This numeric field is the setpoint temperature to apply when the manager intends to turn on heating, in degrees Celsius.   The default is 99.0 &deg;C.
-
-#### Field: Heating Stage Off Supply Air Setpoint Temperature
-
-This numeric field is the setpoint temperature to apply when the manager intends to turn off heating, in degrees Celsius.   The value in this field must be lower than the value in the previous field.   The default is -99.0 &deg;C.
-
-#### Field: Control Zone Name
-
-This alpha field is the name of the control zone for this setpoint manager.   This zone needs to be controlled using ZoneControl:Thermostat:StagedDualSetpoint.
-
-#### Field: Setpoint Node or NodeList Name
-
-This alpha field is the name of a NodeList objet containing the names of the HVAC system nodes, or the name of a system node, for which temperature setpoints will be established by this setpoint manager.
-
-An example input follows.
-
-```idf
-SetpointManager:SingleZone:OneStageHeating,
-       ZNF1 heating on_off , !- Name
-       99.0 , !- Heating Stage On Supply Air Setpoint Temperature
-       -99.0 , !- Heating Stage Off Supply Air Setpoint Temperature
-       ZNF1 , !- Control Zone Name
-       Main Heating Coil 2 Air Outlet Node ; !- Setpoint Node or NodeList Name
-```
-
-### SetpointManager:ReturnTemperature:ChilledWater
-
-This setpoint manager allows for the central plant simulation in EnergyPlus to target a specific return water temperature entering the plant supply equipment.  This setpoint manager is specifically for "chilled water" (although it could be any fluid) applications.  This setpoint manager senses the current supply and return temperatures, calculates the current demand on the loop, and assuming this load remains constant for this time step, it predicts what set-point temperature would provide the desired target return temperature.
-
-Because this is predictive, and the setpoint is only updated once per system timestep (frequency of the call to ManageSetPoints), the longer the time step, the less accurate the prediction will be.  To make tighter control, the time step can be reduced down even to one minute.  However, as described in the EngineeringReference, for most realistic building profiles the control works quite well under normal timestep size.  If your load profile is highly jagged with step changes in demand, a smaller timestep could help achieve tight control.
-
-#### Field: Name
-
-This alpha field is a unique, user-assigned name for an instance of a chilled water return temperature reset setpoint manager.
-
-#### Plant Loop Supply Outlet Node
-
-This alpha field is the name of the plant loop supply side outlet node for the plant being managed by this setpoint manager.  The current temperature of this node is sensed in order to calculate current loop demand.  This node is typically also where the plant loop setpoint is specified, but not necessarily.  This setpoint manager looks up the actual setpoint node from the PlantLoop internal data structures as it is specified on the PlantLoop object.  If the plant loop setpoint is on a different node than the supply outlet node, the loop may not maintain return temperature control as expected.
-
-#### Plant Loop Supply Inlet Node
-
-This alpha field is the name of the plant loop supply side inlet node whose temperature is controlled using this setpoint manager by resetting the supply setpoint temperature.  The current temperature of this node is also sensed in order to calculate current loop demand.
-
-#### Minimum Supply Temperature Setpoint
-
-This numeric field plays multiple roles.  During initialization, such as before the plant data structures are fully established, this is used as the default plant supply setpoint temperature.  During normal calculation, this is used as the minimum chilled water supply temperature to avoid resetting the setpoint too low.  During times of no-load, or odd conditions such as a negative load, the setpoint is reset to this design setpoint.
-
-#### Maximum Supply Temperature Setpoint
-
-This numeric field is the maximum value to which the supply setpoint can be reset.  This ensures that the chilled water temperature does not go too high during reset operations.
-
-#### Return Temperature Setpoint Input Type
-
-This alpha field must be one of three strings: "Constant", "Scheduled", or "ReturnTemperatureSetpoint".  If the choice is "Constant", the constant value in the next field is used as the target return temperature.  If the choice is "Scheduled", the current value of the schedule named in the following field is used as the target return temperature.  If the choice is "ReturnTemperatureSetpoint", the actual setpoint temperature on the "Plant Loop Supply Inlet Node" specified above is retrieved and used as the target return temperature.  This is convenient as a separate setpoint manager could be established to pre-calculate the desired return temperature, and will assign the Setpoint internally.  Then when this return temperature manager executes, the setpoint will be updated and utilized.
-
-#### Return Temperature Setpoint Constant Value
-
-If the "Return Temperature Setpoint Input Type" field is "constant", the numeric value entered here is used as the target return temperature throughout the simulation.
-
-#### Return Temperature Setpoint Schedule Name
-
-If the "Return Temperature Setpoint Input Type" field is "scheduled", this alpha field defines the name of a user-defined schedule storing values of return target temperature.  The "current" value is looked up throughout the simulation.  This is especially useful as EMS can be employed to do additional sensing and override the schedule value in a given timestep to a new dynamically-calculated return temperature.
-
-An example idf input for a constant return reset setpoint manager is shown here:
-
-```idf
-  SetpointManager:ReturnTemperature:ChilledWater,
-    Main Loop Setpoint Manager, !- Name
-    Supply Outlet Node,      !- Plant Loop Supply Outlet Node
-    Supply Inlet Node,       !- Plant Loop Supply Inlet Node
-    7.0,                     !- Minimum Supply Temperature Setpoint
-    10.0,                    !- Maximum Supply Temperature Setpoint
-    Constant,                !- Return Temperature Setpoint Input Type
-    12.0,                    !- Return Temperature Setpoint Constant Value
-    ;                        !- Return Temperature Setpoint Schedule Name
-```
-
-Another example which uses the "ReturnTemperatureSetpoint" is shown here with the accompanying setpoint being used to set the setpoint on the return node:
-
-```
-  SetpointManager:Scheduled,
-    Return Temperature Setpoint Manager,  !- Name
-    Temperature,             !- Control Variable
-    Return Temperature Sch,  !- Schedule Name
-    Supply Inlet Node;       !- Setpoint Node or NodeList Name
-
-  Schedule:Constant,
-    Return Temperature Sch,  !- Name
-    Any Number,              !- Schedule Limits
-    11.75;                   !- Value
-
-  SetpointManager:ReturnTemperature:ChilledWater,
-    Main Loop Setpoint Manager, !- Name
-    Supply Outlet Node,      !- Plant Loop Supply Outlet Node
-    Supply Inlet Node,       !- Plant Loop Supply Inlet Node
-    7.0,                     !- Minimum Supply Temperature Setpoint
-    10.0,                    !- Maximum Supply Temperature Setpoint
-    ReturnTemperatureSetpoint, !- Return Temperature Setpoint Input Type
-    ,                        !- Return Temperature Setpoint Constant Value
-    ;                        !- Return Temperature Setpoint Schedule Name
-```
-
-### SetpointManager:ReturnTemperature:HotWater
-
-This setpoint manager allows for the central plant simulation in EnergyPlus to target a specific return water temperature entering the plant supply equipment.  This setpoint manager is specifically for "hot water" (although it could be any fluid) applications.  This setpoint manager senses the current supply and return temperatures, calculates the current demand on the loop, and assuming this load remains constant for this time step, it predicts what supply set-point temperature would provide the desired target return temperature.
-
-Because this is predictive, and the setpoint is only updated once per system timestep (frequency of the call to ManageSetPoints), the longer the time step, the less accurate the prediction will be.  To make tighter control, the time step can be reduced down even to one minute.  However, as described in the EngineeringReference, for most realistic building profiles the control works quite well under normal timestep size.  If your load profile is highly jagged with step changes in demand, a smaller timestep could help achieve tight control.
-
-#### Field: Name
-
-This alpha field is a unique, user-assigned name for an instance of a hot water return temperature reset setpoint manager.
-
-#### Plant Loop Supply Outlet Node
-
-This alpha field is the name of the plant loop supply side outlet node for the plant being managed by this setpoint manager.  The current temperature of this node is sensed in order to calculate current loop demand.  This node is typically also where the plant loop setpoint is specified, but not necessarily.  This setpoint manager looks up the actual setpoint node from the PlantLoop internal data structures as it is specified on the PlantLoop object.  If the plant loop setpoint is on a different node than the supply outlet node, the loop may not maintain return temperature control as expected.
-
-#### Plant Loop Supply Inlet Node
-
-This alpha field is the name of the plant loop supply side inlet node whose temperature is controlled using this setpoint manager by resetting the supply setpoint temperature.  The current temperature of this node is also sensed in order to calculate current loop demand.
-
-#### Minimum Supply Temperature Setpoint
-
-This numeric field is the minimum value to which the supply setpoint can be reset.  This ensures that the hot water temperature does not go too low during reset operations.
-
-#### Maximum Supply Temperature Setpoint
-
-This numeric field plays multiple roles.  During initialization, such as before the plant data structures are fully established, this is used as the default plant supply setpoint temperature.  During normal calculation, this is used as the maximum hot water supply temperature to avoid resetting the setpoint too high.  During times of no-load, or odd conditions such as a negative load, the setpoint is reset to this design setpoint.
-
-#### Return Temperature Setpoint Input Type
-
-This alpha field must be one of three strings: "Constant", "Scheduled", or "ReturnTemperatureSetpoint".  If the choice is "Constant", the constant value in the next field is used as the target return temperature.  If the choice is "Scheduled", the current value of the schedule named in the following field is used as the target return temperature.  If the choice is "ReturnTemperatureSetpoint", the actual setpoint temperature on the "Plant Loop Supply Inlet Node" specified above is retrieved and used as the target return temperature.  This is convenient as a separate setpoint manager could be established to pre-calculate the desired return temperature, and will assign the Setpoint internally.  Then when this return temperature manager executes, the setpoint will be updated and utilized.
-
-#### Return Temperature Setpoint Constant Value
-
-If the "Return Temperature Setpoint Input Type" field is "constant", the numeric value entered here is used as the target return temperature throughout the simulation.
-
-#### Return Temperature Setpoint Schedule Name
-
-If the "Return Temperature Setpoint Input Type" field is "scheduled", this alpha field defines the name of a user-defined schedule storing values of return target temperature.  The "current" value is looked up throughout the simulation.  This is especially useful as EMS can be employed to do additional sensing and override the schedule value in a given timestep to a new dynamically-calculated return temperature.
-
-An example idf input for a scheduled return reset setpoint manager is shown here:
-
-```idf
-  SetpointManager:ReturnTemperature:HotWater,
-    Main Loop Setpoint Manager, !- Name
-    Supply Outlet Node,      !- Plant Loop Supply Outlet Node
-    Supply Inlet Node,       !- Plant Loop Supply Inlet Node
-    57.0,                    !- Minimum Supply Temperature Setpoint
-    60.0,                    !- Maximum Supply Temperature Setpoint
-    Scheduled,               !- Return Temperature Setpoint Input Type
-    ,                        !- Return Temperature Setpoint Constant Value
-    ReturnTempSchedule;      !- Return Temperature Setpoint Schedule Name
-
-  Schedule:Compact,
-    ReturnTempSchedule,  !- Name
-    Any Number,              !- Schedule Type Limits Name
-    THROUGH: 12/31,          !- Field 1
-    FOR: AllDays,            !- Field 2
-    UNTIL: 12:00, 55,        !- Field 3
-    UNTIL: 17:00, 53,        !- Field 3
-    UNTIL: 24:00, 55;        !- Field 3
-```
-
-Group     Controllers
--------------------
-
-### Controls (Air Loop and Zone Equipment)
-
-A controller mimics the function of an actual physical controller in a somewhat rudimentary way. It can sense one node variable, compare it with its setpoint, and determine the desired value for another node variable. It should be noted that a controller cannot span a loop manager boundary (but a Setpoint Manager can). Thus, in an air loop (AirLoopHVAC), the sensed node and the controlled device must be in the air loop simulation. This means that a single zone system cannot be modeled with a simple controller sensing zone temperature and controlling coil water flow. Instead this must be modeled as a Setpoint Manager sensing a zone temperature and resetting the supply air temperature setpoint each timestep. This is artificial but should simplify the control modeling task. It should also be noted that there are various types of controllers and that each controller might hook into loops in a slightly different way. As a result, each controller type is described separately below.
-
-### Controller:WaterCoil
-
-This controller is really a solution inverter. For a water coil the simulation cannot be inverted where the mass flow rate of the water through the coil can be solved directly given an air temperature. Thus, this controller will numerically step through all of the water flow possibilities by an interval-halving technique until the mass flow rate is determined to meet the specified outlet air temperature within a specified user tolerance.
-
-As the reader probably noted when reading the descriptions of the coil syntax shown earlier in this section, there were no controls attached directly to a particular component. This is because the input can be simplified somewhat by entering node names to be controlled. This avoids having to search through multiple lists of component types for the sake of simply controlling components. The Controller:WaterCoil shown below is a way of controlling variables at one node based on conditions at another node. After the identifying name for the controller, the user must define which control variable the controller is managing. These options include Temperature, Humidity Ratio, TemperatureAndHumidityRatio, or Flow.
-
-The next parameter in the input syntax is the Action of the control, which determines how the controlled variable (e.g., mass flow rate through a water coil) is changed based on the control signal. The following input parameter is the actuator variable, which is currently limited to mass flow through a water coil.
-
-The next two parameters in the input syntax are node names corresponding to the node that is being sensed and the actuated node which controls the water mass flow through the coil. For example, in the case of a cooling coil the control variable might be the outlet air temperature of the coil while the actuated variable might be the water flow rate through the coil. These two parameters are followed by the controller convergence tolerance. Finally, the last two input parameters represent the maximum and minimum values allowed for the actuated variable at the actuated node.
-
-#### Field: Name
-
-This is the unique name of the controller.
-
-#### Field: Control Variable
-
-This was setup to be generic but to date has only been used for temperature control, or temperature and humidity ratio control, of a water coil in the air loop simulation. The keyword Temperature is used for air temperature control and is normally specified for the coils outlet air node. The keyword TemperatureAndHumidityRatio is used for controlling both air temperature and high humidity levels, and is normally specified for a cooling coils outlet air node. The keyword HumidityRatio is used for humidity control and would normally be specified for a dehumidifier outlet node. These two keywords require a ZoneControl:Humidistat object and a maximum humidity setpoint manager object (SetPointManager:SingleZone:Humidity:Maximum, SetPointManager:MultiZone:MaximumHumidity:Average or  SetPointManager:MultiZone:Humidity:Maximum). If the coil is located in the outdoor air stream, it may also be necessary to use SetpointManager:OutdoorAirPretreat.
-
-#### Field: Action
-
-The next input refers to the action of the control. This can be best described by an example. In a coil where water mass flow rate is to be controlled, a coil will increase the mass flow rate through the coil when more heating or cooling is requested. In a heating coil, this increases the value of heat transfer from the water to the air stream. As a result, this is considered a Normal action controller. In a cooling coil, an increase in water mass flow rate through the coil decreases the value of heat transfer from the water to the air stream (absolute value increases, but since cooling is traditionally described as a negative number, an increase in absolute value results in a decrease in the actual heat transfer value). Thus, the cooling coil controller has Reverse action since an increase in flow rate results in a decrease in heat transfer.
-
-#### Field: Actuator Variable
-
-This was again meant to be more generic but currently has only been used to control the water mass flow rate of a heating or cooling coil. This actuator variable must be set to the keyword Flow to control the water mass flow rate.
-
-#### Field: Sensor Node Name
-
-Name of the node where the temperature, humidity ratio or flow is sensed.
-
-#### Field: Actuator Node Name
-
-Name of the actuated node that controls the water mass flow rate through the coil.
-
-#### Field: Controller Convergence Tolerance
-
-The coil is controlled by knowing the outlet temperature and/or humidity ratio specified by the setpoint managers, and setting the outlet conditions from the coil to meet these setpoints. The hot and chilled water coils use complex models that cannot be inverted directly. Therefore, to determine the correct mass flow rate for the hot or cold water the models are inverted numerically using an iterative procedure. The iterative solution uses an interval-halving routine and needs a termination criteria that is set with the Controller Convergence Tolerance parameter. The convergence tolerance is the maximum difference between the actual temperature at the setpoint node and the setpoint temperature. This control offset is set to a small temperature difference, such as 0.01 to denote 1/100 degree C. The default is 0.1 degree C.
-
-#### Field: Maximum Actuated Flow
-
-This is the maximum water flow (m<sup>3</sup>/sec) through the coil. Set to the maximum design water flow for the coil.
-
-#### Field: Minimum Actuated Flow
-
-Set to the minimum design water flow (m<sup>3</sup>/sec) for the water coil, normally a shut off valve that is set to zero.
-
-An example of this object in an IDF, along with appropriate setpoint managers, is shown below:
-
-
-
-```idf
-   Controller:WaterCoil,
-     Central Cooling Coil Contoller 1,     !- Name
-     TemperatureAndHumidityRatio,          !- Control Variable
-     Reverse,                              !- Action
-     Flow,                                 !- Actuator Variable
-     VAV Sys 1 Outlet Node,                !- Sensor Node Name
-     Main Cooling Coil 1 Water Inlet Node, !- Actuator Node Name
-     0.002,                                !- Controller Convergence Tolerance {deltaC}
-     0.025,                                !- Maximum Actuated Flow {m3/s}
-     0.0;                                  !- Minimum Actuated Flow {m3/s}
-
-
-   SetpointManager:SingleZone:Humidity:Maximum,
-     Zone Max Set Point Manager,           !- Name
-     ,                                     !- Control Variable
-     ,                                     !- Schedule name
-     VAV Sys 1 Outlet Node,                !- Setpoint Node or NodeList Name
-     Zone 2 Node;                          !- Control Zone Air Node Name
-
-
-   SetpointManager:Scheduled,
-     Scheduled Set Point Manager 1,        !- Name
-     Temperature,                          !- Control Variable
-     Seasonal Reset Supply Air Temp Sch,   !- Schedule Name
-     VAV Sys 1 Outlet Node;                !- Setpoint Node or NodeList Name
-```
-
-
-### Controller:OutdoorAir
-
-A mixed air box has its own controller type called Controller:OutdoorAir. The purpose of the outdoor air controller is to provide outdoor air for ventilation and also provide free cooling (through additional outdoor air and/or bypassing an air-to-air heat exchanger) whenever possible. The outdoor air controller includes a number of user-selectable limit controls. If any of the selected limits are exceeded, the outdoor airflow rate is set to the minimum.
-
-If all the limits are satisfied, the outdoor air controller does the following for continuous air flow systems: if the outdoor air temperature is greater than or equal to the mixed air temperature setpoint, the outdoor air flow rate is set to the maximum; if the outdoor air temperature is less than the mixed air temperature setpoint, the outdoor air controller will modulate the outdoor air flow so that the mixed air temperature will match the mixed air setpoint temperature.
-
-A time-of-day schedule may also be used to simulate an increase in outdoor air flow rate for push-button type economizer applications. When the schedule permits (i.e., schedule values are greater than 0), the outdoor air flow rate is increased to the user-specified maximum outdoor air flow rate.
-
-The outdoor air controller can also account for changes in the outdoor air flow rate during times when indoor humidity levels are high. A zone humidistat must be used with this control option. During high indoor humidity, the outdoor air flow rate is modified in response to a high indoor humidity condition. If high humidity control is based on the outdoor air humidity ratio and the outdoor humidity ratio is greater than the indoor humidity ratio, high humidity control is terminated. When the economizer is used in conjunction with the high humidity control option, high humidity control has priority and controls the change in air flow rates. The Night Ventilation Availability Manager has priority over high humidity control and will use the controllers maximum outdoor air flow rate when this Availability Manager cycles the fan on (Ref. System Availability Managers AvailabilityManager:NightVentilation)
-
-The mixed air box connections are defined separately in the **OutdoorAir:Mixer** object.
-
-Although the mixer will commonly be connected directly to the outdoor air, other components may be placed on the outdoor air path upstream of the mixer. When this is the case, any modulation will be determined by the conditions at the inlet node of the mixer rather than the outdoor air. This means that the controller will account for any heat recovery or other preheating/precooling components that may modify the condition of outdoor air before it reaches the mixer.
-
-If all the limits are satisfied, the outdoor air controller does the following for cycling fan systems: the outdoor air flow rate is set to the maximum when the fan cycles on. If the limits are not satisfied, the outdoor air flow rate is at the minimum when the fan cycles on.
-
-#### Field: Name
-
-The unique user-assigned name for an instance of an outdoor air controller. Any other object referencing this outdoor air controller will use this name.
-
-#### Field: Relief Air Outlet Node Name
-
-The name of the relief air node of the outdoor air mixer associated with this outdoor air controller.
-
-#### Field: Return Air Node Name
-
-The name of the return air node of the outdoor air mixer associated with this outdoor air controller.
-
-#### Field: Mixed Air Node Name
-
-Name of the node where the mixed air setpoint is set. The outdoor air controller senses the temperature at this node and attempts to control that temperature to the node setpoint.
-
-#### Field: Actuator Node Name
-
-The name of the node that is associated with the outdoor air damper. This should be the outermost air node on the outdoor air path connected to the outdoor air stream for the mixer associated with this outdoor air controller.
-
-#### Field: Minimum Outdoor Air Flow Rate
-
-Input for this field is the minimum outdoor air flow rate for the system in cubic meters per second.
-
-#### Field: Maximum Outdoor Air Flow Rate
-
-Input for this field is the maximum outdoor air flow rate for the system in cubic meters per second.
-
-#### Field: Economizer Control Type
-
-The options for this field are
-
-- FixedDryBulb
-
-- DifferentialDryBulb
-
-- FixedEnthalpy
-
-- DifferentialEnthalpy
-
-- ElectronicEnthalpy
-
-- FixedDewPointAndDryBulb
-
-- DifferentialDryBulbAndEnthalpy
-
-- NoEconomizer
-
-Choosing **NoEconomizer** means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
-
-Choosing **FixedDryBulb** means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
-
-Choosing **DifferentialDryBulb** will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
-
-**FixedEnthalpy** checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
-
-**DifferentialEnthalpy** does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
-
-Choosing **ElectronicEnthalpy** enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
-
-Choosing **FixedDewPointAndDryBulb** compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
-
-Another option **DifferentialDryBulbAndEnthalpy** enables the control strategy to be based on both the DifferentialDryBulb and DifferentialEnthalpy economizer control strategies.
-
-In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
-
-The default for this field is **NoEconomizer**.
-
-#### Field: Economizer Control Action Type
-
-There are two choices for this Field: **MinimumFlowWithBypass** and **ModulateFlow**, with the default being **ModulateFlow** if this input field is left blank.
-
-**ModulateFlow** means the outdoor air flow rate will be increased to meet the mixed air setpoint temperature, subject to the limits imposed via other inputs for this object (e.g., Economizer Maximum Limit Dry-Bulb Temperature, Maximum Outdoor Air Flow Rate, etc.).
-
-**MinimumFlowWithBypass** is used exclusively in conjunction with air-to-air heat exchanger:objects (Ref. HeatExchanger:\*) for providing free cooling operation in the absence of a conventional air-side economizer (i.e., when outdoor air flow rate is not increased during economizer mode). The MinimumFlowWithBypass choice forces the outdoor air flow rate to always remain at the minimum. However, when high humidity control is used, the outdoor air flow rate is set to the product of the maximum outdoor air flow rate multiplied by the high humidity outdoor air flow ratio. The heat exchanger uses the limit checking in the outdoor air controller to decide whether or not to bypass the outdoor air around the heat exchanger or turn off the wheel motor in the case of a rotary heat exchanger. Heat exchange is also suspended when high humidity control is active.
-
-The **ModulateFlow** option can also be used with the HeatExchanger:AirToAir:FlatPlate or HeatExchanger:AirToAir:SensibleAndLatent objects.
-
-#### Field: Economizer Maximum Limit Dry-Bulb Temperature
-
-Input for this field is the outdoor air temperature high limit ( &deg;C) for economizer operation. If the outdoor air temperature is above this limit, the outdoor airflow rate will be set to the minimum. This field is required if Economizer Control Type    FixedDryBulb or FixedDewPointAndDryBulb has been specified.
-
-No input (blank) in this field means that there is no outdoor air temperature high limit control. This limit applies to the conditions at the Actuator Node regardless of whether or not there are any other components in the outdoor air path upstream of the mixer. If non-blank, this limit is applied regardless of the specified Economizer Control Type.
-
-#### Field: Economizer Maximum Limit Enthalpy
-
-Input for this field is the outdoor air enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor airflow rate will be set to the minimum. This field is required if Economizer Control Type FixedEnthalpy has been specified.
-
-No input (blank) in this field means that there is no outdoor air enthalpy limit control. This limit applies to the conditions at the Actuator Node regardless of whether or not there are any other components in the outdoor air path upstream of the mixer. If non-blank, this limit is applied regardless of the specified Economizer Control Type.
-
-#### Field: Economizer Maximum Limit Dewpoint Temperature
-
-Input for this field is the outdoor air dewpoint limit (&deg;C) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type FixedDewPointAndDryBulb has been specified.
-
-No input (blank) in this field means that there is no outdoor air dewpoint limit control. This limit applies to the conditions at the Actuator Node regardless of whether or not there are any other components in the outdoor air path upstream of the mixer. If non-blank, this limit is applied regardless of the specified Economizer Control Type.
-
-#### Field: Electronic Enthalpy Limit Curve Name
-
-Input for this field is the name of a quadratic or cubic curve which provides the maximum outdoor air humidity ratio (function of outdoor air dry-bulb temperature) for economizer operation. If the outdoor air humidity ratio is greater than the curve's maximum humidity ratio (evaluated at the outdoor air dry-bulb temperature), the outdoor air flow rate will be set to the minimum. This limit applies to the conditions at the Actuator Node regardless of whether or not there are any other components in the outdoor air path upstream of the mixer. No input (blank) in this field means that there is no electronic enthalpy limit control. If non-blank, this limit is applied regardless of the specified Economizer Control Type.
-
-#### Field: Economizer Minimum Limit Dry-Bulb Temperature
-
-Input for this field is the outdoor air temperature low limit ( &deg;C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor airflow rate will be set to the minimum.
-
-No input (blank) in this field means that there is no outdoor air temperature low limit control. This limit applies to the conditions at the Actuator Node regardless of whether or not there are any other components in the outdoor air path upstream of the mixer. If non-blank, this limit is applied regardless of the specified Economizer Control Type.
-
-#### Field: Lockout Type
-
-Choices for this field are NoLockout, LockoutWithHeating, and LockoutWithCompressor. This field is used for packaged systems with DX coils. LockoutWithHeating means that if the packaged unit is in heating mode, the economizer is locked out i.e., the economizer dampers are closed and there is minimum outdoor air flow. LockoutWithCompressor means that in addition to locking out the economizer when the unit is in heating mode the economizer is locked out when the DX unit compressor is operating to provide cooling. In other words, the economizer must meet the entire cooling load; it is not allowed to operate in conjunction with the DX cooling coil. This option (LockoutWithCompressor) is sometimes called a    nonintegrated economizer.
-
-When LockoutWithHeating or LockoutWithCompressor is selected, the lockout may also be applied to non-packaged systems for heating. If any air loop heating coil is operating, the lockout control compares the mixed air temperature at minimum outdoor air flow without heat recovery (if any) to the mixed air temperature set point. If the mixed air temperature at minimum outdoor air flow is less than the mixed air temperature set point, then the economizer is locked out and the outdoor air flow rate is set to the minimum. When the economizer is locked out, the heat recovery bypass control will be set to activate heat recovery (no bypass), if present. This action is meant to minimize heating energy (this action may also disable the heating coil on subsequent iterations, see output variable Air System Outdoor Air Heat Recovery Bypass Heating Coil Activity Status).
-
-The default is NoLockout.
-
-#### Field: Minimum Limit Type
-
-Choices for this field are FixedMinimum or ProportionalMinimum. FixedMinimum means that the minimum outdoor airflow rate is fixed no matter what the actual system flow rate is. ProportionalMinimum means the minimum outdoor airflow rate varies in proportion to the total system air flow rate. The default is ProportionalMinimum.
-
-#### Field: Minimum Outdoor Air Schedule Name
-
-The name of a schedule which uses decimal values (e.g., 0.0 or 1.0).   These values are multiplied by the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours. If this field is not entered, the minimum outdoor air flow rate either remains constant during the simulation period (Minimum Outdoor Air Control Type = FixedMinimum) or varies in proportion to the supply air flow rate (Minimum Outdoor Air Control Type = ProportionalMinimum).
-
-#### Field: Minimum Fraction of Outdoor Air Schedule Name
-
-The name of a schedule which uses decimal values (0.0     1.0) These values are multiplied by the total (design) air flow rate.   This is an alternate method for specifying the minimum outdoor air amount. (The other method is the ***Minimum Outdoor Air Schedule*** *described above.)   Note: This field overrides **Minimum Outdoor Air Schedule** and **Minimum Outdoor Air Flowrate.***
-
-#### Field: Maximum Fraction of Outdoor Air Schedule Name
-
-This is an optional field with the schedule values in decimal fractions (0.0-1.0). This field enables the user to limit the maximum of amount of outdoor air permissible and thus also limits the permissible maximum outdoor air into the system.
-
-If both the above schedules are given values of 1.0, the system works at 100% outdoor air, so in a system if 100% outdoor air is required regardless of any other condition, these fields are helpful.
-
-#### Field: Mechanical Ventilation Controller Name
-
-This optional field is the name of the mechanical ventilation controller object to be used in conjunction with this outdoor air controller. The Controller:MechanicalVentilation object allows the user to define the minimum outdoor air flow rate based on air flow per unit floor area and air flow per person (occupant) for the zones being served by the air loop that utilizes this controller.
-
-This feature allows the user to perform a first-order evaluation of carbon dioxide(CO<sub>2</sub>)-based demand controlled ventilation (outdoor ventilation varied according to occupancy levels).
-
-If a valid name for a Controller:MechanicalVentilation object is entered in this field, the minimum outdoor air flow rate delivered will be the greater of:
-
-- the minimum outdoor air flow rate calculated by the fields Minimum Outdoor Air Flow Rate, Minimum Limit Type, and Minimum Outdoor Air Schedule Name as defined for this outdoor air controller, or
-
-- the outdoor air flow rate calculated using the Controller:MechanicalVentilation object named in this input field.
-
-Leaving this input field blank will bypass the Controller:MechanicalVentilation object calculations and the minimum outdoor air flow rate will be based on the other inputs associated with this outdoor air controller object. Actual outdoor air flow rates may be higher than the minimum if free cooling is available and the object inputs are properly selected. Regardless, the maximum outdoor air flow rate is limited by the field Maximum Outdoor Air Flow Rate.
-
-#### Field: Time of Day Economizer Control Schedule Name
-
-This alpha field is the name of a schedule which controls the outdoor air flow rate based on a time-of-day economizer. Schedule values equal to 0 disable this feature. Schedule values greater than 0 cause the outdoor air flow rate to increase to the maximum. When an economizer is used in conjunction with the high humidity control option, high humidity control has priority.
-
-#### Field: High Humidity Control
-
-This choice field establishes whether or not the outdoor air flow rate is modified in response to high indoor relative humidity. Valid choices are Yes and No. If Yes is selected, the outdoor air flow rate may be modified when the indoor relative humidity is above the humidstat setpoint. If No is selected, this option is disabled and the following three fields are not used.
-
-#### Field: Humidistat Control Zone Name
-
-This input defines the zone name where the humidistat is located. This is the same name used in the ZoneControl:Humidistat object. This field is required when the input field High Humidity Control is specified as Yes.
-
-#### Field: High Humidity Outdoor Air Flow Ratio
-
-This input is the ratio of the modified outdoor air flow rate to the maximum outdoor air flow rate. When the high humidity control algorithm determines that the outdoor air flow rate will be changed (i.e., increased or decreased), the operating outdoor air flow rate is equal to the maximum outdoor air flow rate multiplied by this ratio. The minimum value for this field is 0. If this field is blank, the default value is 1. This field is used only when the input field High Humidity Control is specified as Yes. When an economizer is used in conjunction with the high humidity control option, high humidity control has priority.
-
-#### Field: Control High Indoor Humidity Based on Outdoor Humidity Ratio
-
-This choice field determines if high humidity control is activated based on high indoor relative humidity alone or is activated only when the indoor relative humidity is above the humidstat setpoint *and* the indoor humidity ratio is greater than the outdoor humidity ratio. Valid choices are **Yes** and **No**. If No is selected, high humidity control is active any time the zone humidistat senses a moisture load. If Yes is selected, the model also verifies that the outdoor humidity ratio is less than the humidistat   s zone air humidity ratio. This field is used only when the input field High Humidity Control is specified as Yes. The default value is **Yes**.
-
-#### Field: Heat Recovery Bypass Control Type
-
-This choice field determines if specialized control is used to optimize the use of heat recovery. Valid choices are **BypassWhenWithinEconomizerLimits** and **BypassWhenOAFlowGreaterThanMinimum**. If BypassWhenWithinEconomizerLimits is selected, heat recovery is disabled any time the controller determines that the economizer is active (i.e., all controls are within limits). If BypassWhenOAFlowGreaterThanMinimum is selected, the model first verifies that the economizer is active and then checks to see if the outdoor air flow rate is greater than the minimum. If it is greater than minimum, then heat recovery (if any) is set to bypass. When this option is used with Time of Day Economizer Control or High Humidity Control, this option has priority. The default value is **BypassWhenWithinEconomizerLimits**.
-
-An Example IDF specification:
-
-```idf
-   Controller:OutdoorAir,
-       OA Controller 1,                 !- Name
-       Relief Air Outlet Node,   !- Relief Air Outlet Node Name
-       Outdoor Air Mixer Inlet Node,   !- Return Air Node Name
-       Mixed Air Node,                   !- Mixed Air Node Name
-       Outdoor Air Inlet Node,   !- Actuator Node Name
-       0.25,                                       !- Minimum Outdoor Air Flow Rate {m3/s}
-       1.6,                                         !- Maximum Outdoor Air Flow Rate {m3/s}
-       ElectronicEnthalpy,           !- Economizer Control Type
-       ModulateFlow,                       !- Economizer Control Action Type
-       23.,                                 !- Economizer Maximum Limit Dry-Bulb Temperature {C}
-       ,                                       !- Economizer Maximum Limit Enthalpy {J/kg}
-       13.5,                               !- Economizer Maximum Limit Dewpoint Temperature {C}
-       ElectronicEnthalpyCurveA,!- Electronic Enthalpy Limit Curve Name
-       14.,                                 !- Economizer Minimum Limit Dry-Bulb Temperature {C}
-       NoLockout,                             !- Lockout Type
-       FixedMinimum,                       !- Minimum Limit Type
-       OAFractionSched,                 !- Minimum Outdoor Air Schedule Name
-       ,                                               !- Minimum Fraction of Outdoor Air Schedule Name
-       ,                                               !- Maximum Fraction of Outdoor Air Schedule Name
-       ,                                               !- Mechanical Ventilation Controller Name
-       TimeOfDayEconomizerSch,   !- Time of Day Economizer Control Schedule Name
-       Yes,                                         !- High Humidity Control
-       EAST ZONE,                             !- Humidistat Control Zone Name
-       0.9,                                         !- High Humidity Outdoor Air Flow Ratio
-       Yes;           !- Control High Indoor Humidity Based on Outdoor Humidity Ratio
-
-
-   Curve:Cubic,
-       ElectronicEnthalpyCurveA,!- Name
-       0.01342704,                           !- Coefficient1 Constant
-       -0.00047892,                         !- Coefficient2 x
-       0.000053352,                         !- Coefficient3 x**2
-       -0.0000018103,                     !- Coefficient4 x**3
-      16.6,                                       !- Minimum Value of x
-       29.13;                                     !- Maximum Value of x
-```
-
-
-### Controller:OutdoorAir Outputs
-
-Note that the key value for these outputs is the AirLoopHVAC name, not the name of the Controller:OutdoorAir.
-
-* HVAC,Average,Air System Outdoor Air Economizer Status []
-
-* HVAC,Average,Air System Outdoor Air Heat Recovery Bypass Status []
-
-* HVAC,Average,Air System Outdoor Air Heat Recovery Bypass Heating Coil Activity Status []
-
-* HVAC,Average,Air System Outdoor Air Heat Recovery Bypass Minimum Outdoor Air Mixed Air Temperature [C]
-
-* HVAC,Average,Air System Outdoor Air High Humidity Control Status []
-
-* HVAC,Average,Air System Outdoor Air Flow Fraction []
-
-* HVAC,Average,Air System Outdoor Air Minimum Flow Fraction []
-
-* HVAC,Average,Air System Outdoor Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Air System Mixed Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Air System Outdoor Air Maximum Flow Fraction []
-
-#### Air System Outdoor Air Economizer Status []
-
-Reports the average operating status of an air economizer over the reporting interval. The economizer status is set to 1 when the conditions are favorable for the economizer to operate (i.e., none of the control limits have been exceeded). While conditions may be favorable for economizer operation, it does not guarantee that the air-side economizer has increased outdoor air flow above the minimum level since the actual outdoor air flow rate is also governed by other controls (e.g., mixed air set point tempeature, time of day economizer control, maximum humidity setpoint, etc.). This variable is set to 0 if conditions disable economizer operation or NoEconomizer (Economizer Control Type) is specified.
-
-#### Air System Outdoor Air Heat Recovery Bypass Status []
-
-This indicates if the controls have determined if the bypass mode for heat recovery is in effect or not.
-
-#### Air System Outdoor Air Heat Recovery Bypass Heating Coil Activity Status []
-
-Reports the operating status of any heating coil in the air loop. If the heating coil is active, the heat exchanger will be activated (no air bypassed) and the heating energy will be reduced or eliminated. While conditions may be favorable for economizer operation, it does not guarantee that the air-side economizer has increased outdoor air flow above the minimum level since the actual outdoor air flow rate is also governed by other controls (e.g., mixed air set point temperature, time of day economizer control, maximum humidity setpoint, etc.). This variable is set to 0 if conditions disable economizer operation. This output variable is only available when using Heat Recovery Bypass Control Type = BypassWhenOAFlowGreaterThanMinimum.
-
-#### Air System Outdoor Air Heat Recovery Bypass Minimum Outdoor Air Mixed Air Temperature [C]
-
-Reports the outdoor air mixer   s mixed air node temperature at minimum outdoor air flow rate when the heat exchanger is disabled (off). This temperature is calculated as the return air temperature multiplied by the return air mass flow rate plus the mixer   s inlet node temperature multipled by the minimum outdoor air flow rate. This quantity is then divided by the mixed air mass flow rate. If this temperature is less than the outdoor air mixer   s mixed air node set point temperature, and the Heat Recovery Bypass Control Type = BypassWhenOAFlowGreaterThanMinimum, the outdoor air flow rate is set to the minimum.   This output variable is only available when using Heat Recvoery Bypass Control Type = BypassWhenOAFlowGreaterThanMinimum.
-
-#### Air System Outdoor Air High Humidity Control Status []
-
-Reports the average operating status of the controller   s high humidity control over the reporting interval. The high humidity control status is set to 1 when the controller determines that a zone high humidity condition exists *according to the settings specified in the controller*. This variable is set to 0 if conditions disable high humidity control operation or High Humidity Control is specified as No.
-
-#### Air System Outdoor Air Flow Fraction []
-
-Reports the average actual outdoor air fraction for the outdoor air controller over the reporting interval.
-
-#### Air System Outdoor Air Minimum Flow Fraction []
-
-Reports the average minimum limit of the outdoor air fraction for the outdoor air controller over the reporting interval.
-
-#### Air System Outdoor Air Mass Flow Rate [kg/s]
-
-Reports the average outdoor air mass flow rate introduced by the outdoor air controller over the reporting interval.
-
-#### Air System Mixed Air Mass Flow Rate [kg/s]
-
-Reports the average mixed air mass flow rate of the HVAC air loop associated with this outdoor air controller over the reporting interval.
-
-#### Air System Outdoor Air Maximum Flow Fraction []
-
-Reports the average maximum limit of the outdoor air fraction for the outdoor air controller over the reporting interval. The maximum flow fraction is used to prevent DX cooling coils from freezing, specified by ASHRAE Stadard 90.1. This output variable is available when a corresponding SetpointManager:MixedAir object specifies optional inputs of Cooling Coil Inlet Node Name, Cooling coil Outlet Node Name, and Minimum Temperature at Cooling Coil Outlet Node.     
-
-### Controller:MechanicalVentilation
-
-This object is used in conjunction with an outdoor air controller (Ref. Controller:OutdoorAir, Field: Mechanical Ventilation Controller Name) to establish the minimum outdoor air flow rate provided by a mixed air box.
-
-Ventilation standards provide guidance on appropriate levels of outdoor ventilation air required for acceptable indoor air quality. The Ventilation Rate Procedure (VRP) of ASHRAE Standard 62.1-2007/2010 ([www.ashrae.org](http://www.ashrae.org)) requires outdoor ventilation rates to be determined based on the floor area of each occupied zone plus the number of people in each zone and considers the zone air distribution effectiveness and system ventilation efficiency. The outdoor air ventilation rate can be reset dynamically as operating conditions change (e.g., variations in occupancy). The Controller:MechanicalVentilation object implements the VRP for calculating these outdoor air ventilation requirements and resetting them based on varying occupancy levels and zone diversification. This is particularly useful for large air distribution systems that serve a number of different zone types with varying occupancy levels. This object can also be used to model the Indoor Air Quality Procedure (IAQP) as defined in Standard 62.1
-
-The first five inputs for this object are the name, the availability schedule, the zone outdoor air method, the system outdoor air method, and the zone maximum outdoor air fraction. The next three input fields define the zone name (or zone list name), the design specification outdoor air object name, and the design specification zone air distribution object name to be applied to this zone (or zone list). The last three fields are extensible
-
-#### Field: Name
-
-The unique user assigned name for an instance of mechanical ventilation. Any other object referencing this mechanical ventilation object will use this name.
-
-#### Field: AvailabilitySchedule Name
-
-The name of a schedule whose values are greater than 0 when mechanical ventilation, as calculated by this object, is desired. If the schedule   s value is 0.0, then mechanical ventilation is not available and flow will not be requested. If the schedule   s value is &gt; 0.0 (usually 1 is used), mechanical ventilation is available. If this field is blank, the schedule has values of 1 for all time periods. This schedule is useful for purging the building of contaminants prior to occupancy (i.e., ventilation rate per unit floor area will be provided even if the occupancy is zero).
-
-#### Field: Demand Controlled Ventilation
-
-This field indicates whether the air loop is capable of doing demand controlled ventilation (DCV) to vary the amount of outdoor air based on actual number of occupants in spaces. Two choices: Yes and No. Default is No.
-
-#### Field: System Outdoor Air Method
-
-The method used to calculate the system minimum outdoor air flow. Several choices are allowed: **ZoneSum**, **VentilationRateProcedure,** **IndoorAirQualityProcedure, ProportionalControlBasedonOccupancySchedule,** **ProportionalControlBasedonDesignOccupancy,** and **IndoorAirQualityProcedureGenericContaminant**.   ZoneSum sums the outdoor air flows across all zones served by the system. VentilationRateProcedure (VRP) uses the multi-zone equations defined in 62.1-2007 to calculate the system outdoor air flow. VRP considers zone air distribution effectiveness and zone diversification of outdoor air fractions. IndoorAirQualityProcedure (IAQP) is the other procedure defined in ASHRAE Standard 62.1-2007 for calculate the amount of outdoor air necessary to maintain the levels of indoor air carbon dioxide at or below the setpoint defined in the ZoneControl:ContaminantController object. Appendix A of the ASHRAE 62.1-2010 user's manual discusses another method for implementing CO<sub>2</sub>-based DCV in a single zone system. This method (Proportional Control) calculates the required outdoor air flow rate which varies in proportion to the percentage of the CO<sub>2</sub> signal range and has two choices to calculate occupancy-based outdoor air rate. The ProportionalControlBasedonOccupancySchedule choice uses the real occupancy at the current time step to calculate outdoor air rate, while the ProportionalControlBasedonDesignOccupancy uses the design occupancy level to calculate outdoor air rate. The former choice is a good approach to estimate outdoor air rate.  However, for practical applications, the zone controller usually does not have the real time occupancy information, and  the design occupancy level is assumed. The latter choice is used in the design stage. The IndoorAirQualityProcedure-GenericContaminant method calculates the amount of outdoor air necessary to maintain the levels of indoor air generic contaminant at or below the setpoint defined in the ZoneControl:ContaminantController object.
-
-Note: When System Outdoor Air Method = IndoorAirQualityProcedure or IndoorAirQualityProcedureGenericContaminant is specified, only the Zone &lt;x&gt; Name fields are used. The other field inputs described below are not used.
-
-#### Field: Zone Maximum Outdoor Air Fraction
-
-This positive numeric input is the zone maximum outdoor air fraction. For VAV systems, when a zone requires outdoor air higher than the user specified Zone Maximum Outdoor Air Fraction, the zone supply air flow will be increased (if damper not fully open yet) to cap the outdoor air fraction at the maximum value. This allows the system level outdoor air flow to be reduced while the total supply air flow increases to meet zone outdoor air requirement. Valid values are from 0 to 1.0. Default is 1.0 which indicates zones can have 100% outdoor air maintaining backward compatibility. This inputs work for single and dual duct VAV systems.
-
-#### Field Set (Zone Name, Design Specification Outdoor Air Object Name, and Design Specification Zone Air Distribution Object Name)
-
-The following three fields are needed to define the parameters for the ventilation. This object is extensible by duplicating these three fields.
-
-#### Field:Zone &lt;x&gt; Name
-
-The zone name or zone list to apply the ventilation rates specified in the DesignSpecification:OutdoorAir object.
-
-#### Field: Design Specification Outdoor Air Object Name &lt;x&gt;
-
-The name of the DesignSpecification:OutdoorAir object, defining the amount of outdoor air, that applies to the zone or zone list. If this field is blank, the corresponding DesignSpecification:OutdoorAir object for the zone will come from the DesignSpecification:OutdoorAir object referenced by the Sizing:Zone object for the same zone. If no such zone match is found, default values from the IDD will be used for the DesignSpecification:OutdoorAir object.
-
-#### Field: Design Specification Zone Air Distribution Object Name &lt;x&gt;
-
-The name of the DesignSpecification:ZoneAirDistribution object, defining the air distribution effectiveness and secondary recirculation air fraction, that applies to the zone or zone list. If this field is blank, the corresponding DesignSpecification:ZoneAirDistribution object for the zone will come from the DesignSpecification:ZoneAirDistribution object referenced by the Sizing:Zone object for the same zone. If no such zone match is found, default values from the IDD will be used for the DesignSpecification:ZoneAirDistribution object.
-
-As described previously, the Controller:MechanicalVentilation object works in conjunction with Controller:OutdoorAir. As such, the minimum quantity of outdoor air delivered via the mixed air box will be the greater of:
-
-- the minimum outdoor air flow rate calculated by the fields Minimum Outdoor Air Flow Rate, Minimum Limit and Minimum Outdoor Air Schedule Name in the associated Controller:OutdoorAir object, or
-
-- the outdoor air flow rate calculated by the VRP (details in the Engineering Reference) with inputs specified in this object and the referenced DesignSpecification:OutdoorAir and DesignSpecification:ZoneAirDistribution objects.
-
-The actual outdoor air flow rate may be higher than the minimum if free cooling is available. Regardless, the outdoor air flow rate will not exceed the Maximum Outdoor Air Flow Rate specified in the associated Controller:OutdoorAir object.
-
-An example input for this object is shown below:
-
-```idf
-   Controller:MechanicalVentilation,
-       VentObject,                             !- Name
-       VentSchedule,                         !- Availability Schedule Name
-       VentilationRateProcedure, !- System Outdoor Air Method
-       1.0,                                           !- Zone Maximum Outdoor Air Fraction
-       Resistive Zone,                     !- Zone 1 Name
-       DSOA1,                                       !- Design Specification Outdoor Air Object Name 1
-       DSZADO1,                                   !- Design Specification Zone Air Distribution Object Name 1
-       DCV Zone List,                       !- Zone 2 Name
-       DSO_ZList,                               !- Design Specification Outdoor Air Object Name 2
-       ;                                                !- Design Specification Zone Air Distribution Object Name 2
-
-   ZoneList,
-       DCV Zone List,                       !- Zone List Name
-       East Zone,                               !- Zone Name 1
-       North Zone;                             !- Zone Name 2
-
-   DesignSpecification:OutdoorAir,
-       DSOA1,                                     !- Name
-       SUM,                                         !- Outdoor Air Method
-       0.00236,                                 !- Outdoor Air Flow per Person
-       0.000305,                               !- Outdoor Air Flow per Zone Floor Area
-       0.0,                                         !- Outdoor Air Flow per Zone
-       0.0,                                         !- Outdoor Air Flow Air Changes per Hour
-       ;                                               !- Outdoor Air Flow Rate Fraction Schedule Name
-
-   DesignSpecification:ZoneAirDistribution,
-       DSZADO1,                                 !- Name
-       1.2,                                         !- Zone Air Distribution Effectiveness in Cooling Mode
-       1.0,                                         !- Zone Air Distribution Effectiveness in Heating Mode
-       ,                                               !- Zone Air Distribution Effectiveness Schedule Name
-       0.3;                                         !- Zone Secondary Recirculation Fraction
-```
-
-### ZoneHVAC:EnergyRecoveryVentilator:Controller
-
-This controller object is used exclusively by the stand alone energy recovery ventilator (ZoneHVAC:EnergyRecoveryVentilator, see Figure 143). The purpose of this controller is to simulate economizer operation for the stand alone ERV and provide free cooling whenever possible or modify the outdoor air flow rate during high indoor humidity conditions. During economizer operation, if all of the limits are satisfied, the controller activates economizer mode (fully bypassing the fixed-plate air-to-air heat exchanger or stopping the rotation of a rotary heat exchanger). If any of the selected limits are exceeded, economizer operation is terminated. A time-of-day schedule may also be used to simulate a    push-button    type economizer controller.
-
-In addition, the outdoor air flow rate may be modified and heat exchange suspended in response to high indoor relative humidities. When the indoor relative humidity exceeds the zone humidistat   s relative humidity set point, high humidity control is activated. When activated, if high humidity control is based on the outdoor air humidity ratio and the outdoor humidity ratio is greater than the indoor humidity ratio, high humidity control is terminated.
-
-![Schematic\_StandAloneERV](media/image414.svg)
-
-Figure 143. Schematic of the ZoneHVAC:EnergyRecoveryVentilator compound object
-
-#### Field: Name
-
-A unique user-assigned name for the stand alone ERV controller. Any reference to this controller by another object will use this name.
-
-#### Field: Temperature High Limit
-
-The input for this field is the outdoor air temperature high limit ( &deg;C) for economizer operation. If the outdoor air temperature is above this limit, economizer (free cooling) operation is terminated. No input (blank) in this field means that there is no outdoor air temperature high limit control.
-
-#### Field: Temperature Low Limit
-
-The input for this field is the outdoor air temperature low limit ( &deg;C) for economizer operation. If the outdoor air temperature is below this limit, economizer (free cooling) operation is terminated. No input (blank) in this field means that there is no outdoor air temperature low limit control.
-
-#### Field: Enthalpy High Limit
-
-The input for this field is the outdoor air enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, economizer (free cooling) operation is terminated. No input (blank) in this field means that there is no outdoor air economizer limit control.
-
-#### Field: Dewpoint Temperature Limit
-
-Input for this field is the outdoor air dewpoint limit ( &deg;C) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. No input (blank) in this field means that there is no outdoor air dewpoint limit control. This limit applies to the conditions at the Actuated Node regardless of whether or not there are any other components on the outdoor air path upstream of the mixer.
-
-#### Field: Electronic Enthalpy Limit Curve Name
-
-Input for this field is the name of a quadratic or cubic curve which provides the maximum outdoor air humidity ratio (function of outdoor air dry-bulb temperature) for economizer operation. If the outdoor air humidity ratio is greater than the curve   s maximum humidity ratio (evaluated at the outdoor air dry-bulb temperature), the outdoor air flow rate will be set to the minimum. This limit applies to the conditions at the Actuated Node regardless of whether or not there are any other components on the outdoor air path upstream of the mixer. No input (blank) in this field means that there is no electronic enthalpy limit control.
-
-#### Field: Exhaust Air Temperature Limit
-
-This input establishes whether or not there is a limit control on the exhaust air temperature. The choices are **ExhaustAirTemperatureLimit** or **NoExhaustAirTemperatureLimit**. If **ExhaustAirTemperatureLimit** is chosen, the controller deactivates economizer mode whenever the outdoor air temperature is greater than the exhaust air temperature. If **NoExhaustAirTemperatureLimit** is chosen, no limit check on the exhaust air temperature is performed.
-
-#### Field: Exhaust Air Enthalpy Limit
-
-This input establishes whether or not there is a limit control on the exhaust air enthalpy. The choices are **ExhaustAirEnthalpyLimit** or **NoExhaustAirEnthalpyLimit**. If **ExhaustAirEnthalpyLimit** is chosen, the controller deactivates economizer mode whenever the outdoor air enthalpy is greater than the exhaust air enthalpy. If **NoExhaustAirEnthalpyLimit** is chosen, no limit check on the exhaust air enthalpy is performed.
-
-#### Field: Time of Day Economizer Flow Control Schedule Name
-
-This alpha field is the name of a schedule which controls the change in air flow rate based on time-of-day. Schedule values equal to 0 disable this feature. Schedule values greater than 0 activate the economizer. Note that heat exchange between the air streams is suspended when the economizer is active. This schedule can be used with or without the high humidity control option. When an economizer is used in conjunction with the high humidity control option, high humidity control has priority.
-
-#### Field: High Humidity Control Flag
-
-This optional choice field establishes whether or not the supply and exhaust air flow rates are modified in response to high indoor relative humidity. Valid choices are Yes and No. If Yes is selected, the supply and exhaust air flow rates may be modified when the indoor relative humidity is above the humidstat set point. If No is selected, this option is disabled and the following three fields are not used. Note that heat exchange between the air streams is suspended during times when high humidity control is active. The default value is No.
-
-#### Field: Humidistat Control Zone Name
-
-This optional input defines the zone name where the humidistat is located. This is the same zone name used in the Zone Control:Humidistat object. This field is required when the High Humidity Control Flag is specified as Yes.
-
-#### Field: High Humidity Outdoor Air Flow Ratio
-
-This optional input is the ratio of the modified supply (outdoor) air flow rate to the supply air flow rate specified in the Energy Recovery Ventilator:Stand Alone ERV object. When the high humidity control algorithm determines that the supply air flow rate will be changed (i.e. increased or decreased), the operating supply air flow rate is equal to the supply air flow rate specified in the Energy Recovery Ventilator:Stand Alone ERV object multiplied by this ratio. The minimum value for this field is 0. This field is used to modify both the supply and exhasut air flow rates when high humidity control is active. The supply and exhasut air fan volumetric flow rates must be able to account for the increase in air flow when this input is greater than 1. The default value is 1.
-
-#### Field: Control High Indoor Humidity based on Outdoor Humidity Ratio
-
-This optional choice field determines if high humidity control is activated based on high indoor relative humidity alone or is activated only when the indoor relative humidity is above the humidstat set point *and* the outdoor humidity ratio is less than the indoor humidity ratio. Valid choices are Yes and No. If No is selected, high humidity control is active any time the zone humidistat senses a moisture load. If yes is selected, the model also verifies that the outdoor humidity ratio is less than the humidistat   s zone air humidity ratio. This field is used only when the High Humidity Control Flag is specified as Yes. The default value is Yes.
-
-Following is an example input for this stand alone ERV controller object:
-
-```idf
-ZoneHVAC:EnergyRecoveryVentilator:Controller,
-       ERV OA Controller 1,                       !- ERV controller name
-       19.,                                                       !- Temperature high limit {C}
-       14.,                                                       !- Temperature low limit {C}
-       ,                                                             !- Enthalpy high limit {J/kg}
-       15.55,                                                   !- dew point temperature limit (C)
-       ElectronicEnthalpyCurveA,             !- electronic enthalpy limit curve name
-       NoExhaustAirTemperatureLimit,     !- Exhaust air temperature limit
-       NoExhaustAirEnthalpyLimit,           !- Exhaust air enthalpy limit
-       OutsideAirFlowSchedule,                 !- Time of Day Economizer Flow Control Schedule Name
-       Yes,                                                       !- High Humidity Control Flag
-       East Zone,                                           !- Humidistat Control Zone Name
-       1.2,                                                       !- High Humidity Outdoor air Flow Ratio
-       Yes;                           !- Control High Indoor Humidity based on Outdoor Humidity Ratio
-
-
-Curve:Cubic,
-       ElectronicEnthalpyCurveA, !- Name
-       0.01342704,                             !- Coefficient1 Constant
-     -0.00047892,                             !- Coefficient2 x
-       0.000053352,                           !- Coefficient3 x**2
-     -0.0000018103,                         !- Coefficient4 x**3
-      16.6,                                         !- Minimum Value of x
-       29.13;                                       !- Maximum Value of x
-```
-
-Group     Evaporative Coolers
----------------------------
-
-This group of objects describes the properties and configuration for the evaporative coolers models for the HVAC section.
-
-### EvaporativeCooler:Direct:CelDekPad
-
-The direct stage, shown in the figure below, consists of a rigid media evaporative pad, with water recirculated from a reservoir.   The water is pumped from the reservoir to a water distribution header, for water feed by gravity from above the media.   The evaporative pad provides the area for the adiabatic saturation of the air.   While the process provides a lower dry-bulb temperature, the moisture content of the leaving air is higher than the entering condition.   The direct stage is used for comfort cooling in a building where adding humidity to the air can be tolerated.
-
-![](media/image415.svg)
-
-Figure 144.   Direct Stage Evaporative Cooler
-
-The thermodynamic process is a simultaneous heat and mass transfer, or adiabatic cooling, and follows a constant enthalpy line on the psychrometric chart, it is shown in the figure below as a process from A to B.   Since the deviation of the constant wet-bulb line and the constant enthalpy line is small, it is assumed that the wet-bulb temperature is constant across the direct evaporative stage.
-
-![](media/image416.svg)
-
-Figure 145.   Psychrometric Chart -- Constant Enthalpy
-
-If the direct evaporative process were 100% efficient, the leaving dry-bulb temperature would equal the entering wet-bulb temperature.   The efficiency of the direct evaporative process is less than 100% and by defining saturation efficiency (<span>\(\varepsilon \)</span>se) for the direct stage or evaporative pad, the leaving dry-bulb temperature can be expressed by the following equation.
-
-<div>\[{T_{db\,supout}} = {T_{db\,sup\,in}} - {\varepsilon_{se}}\cdot \left( {{T_{db\,sup\,in}} - {T_{wb\,sup\,in}}} \right)\]</div>
-
-#### Field: Name
-
-A unique identifying name for each evaporative cooler.
-
-#### Field:Availability Schedule Name
-
-The name of a schedule which defines when the evaporative cooler is available. A schedule value of 0 indicates that the evaporative cooler is off for that time period. A schedule value greater than 0 indicates that the evaporative cooler can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Direct Pad Area
-
-The face area of the evaporative pad in m<sup>2</sup>.   With the area and mass flow rate, the air velocity is calculated and is used to determine the saturation efficiency. This field is autosizable.
-
-#### Field: Direct Pad Depth
-
-The depth of the evaporative pad in meters.   The pad depth is used to determine the saturation efficiency. This field is autosizable.
-
-#### Field: Recirculating Water Pump Power Consumption
-
-This field is used to specify the power consumed by the evaporative cooler recirculating pump in Watts.
-
-#### Field: Air Inlet Node Name
-
-The name of the evaporative cooler air inlet node from the Air Loop Simulation.
-
-#### Field: Air Outlet Node Name
-
-The name of the evaporative cooler air outlet node from the Air Loop Simulation.
-
-#### Field: Control Type
-
-This input field is currently unused and can be left blank.
-
-#### Field: Water Supply Storage Tank Name
-
-This field is optional.   It is used to describe where the cooler obtains water used for evaporative cooling.   If blank or omitted, then the cooler will obtain water directly from the mains.   If the name of a WaterUse:Storage object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the cooler will attempt to obtain all the water it uses from the tank.   However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains.
-
-An IDF example showing how this object is:
-
-```idf
-   EvaporativeCooler:Direct:CelDekPad,
-       Evaporative Cooler,           !- Name
-       System Availability Schedule,   !- Availability Schedule Name
-       0.6,                                         !- Direct Pad Area {m2}
-       0.2,                                         !- Direct Pad Depth {m}
-       225,                                         !- Recirculating Water Pump Power Consumption {W}
-       Evap Cooler Inlet Node,   !- Air Inlet Node Name
-       Supply Outlet Node;           !- Air Outlet Node Name
-```
-
-### EvaporativeCooler:Direct:CelDekPad Outputs
-
-The output variables that are available for this direct evaporative cooler are shown below:
-
-* HVAC,Average, Evaporative Cooler Wet Bulb Effectiveness
-
-* HVAC,Average, Evaporative Cooler Electric Power[W]
-
-* HVAC,Sum, Evaporative Cooler Electric Energy [J]
-
-* HVAC,Sum, Evaporative Cooler Water Volume[m3]
-
-* HVAC,Sum,Evaporative Cooler Mains Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Starved Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Starved Mains Water Volume [m3]
-
-#### Evaporative Cooler Wet Bulb Effectiveness
-
-The effectivenss, or saturation efficiency, is the temperature change of the supply air divided by the difference between the inlet air dry-bulb and wet-bulb temperatures. In other words, it is a measure of the approach to the inlet air wet-bulb temperature.
-
-#### Evaporative Cooler Electric Power[W]
-
-#### Evaporative Cooler Electric Energy [J]
-
-These output variables report the electric power and electric energy required to operate the water pump.
-
-#### Evaporative Cooler Water Volume [m3]
-
-The water consumption is the water evaporated from the pad.   This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down.   This output variable appears when mains water is supplied to the cooler.
-
-#### Evaporative Cooler Mains Water Volume [m3]
-
-This is the source of the water consumed.   This output variable appears when mains water is supplied to the cooler.
-
-#### Evaporative Cooler Storage Tank Water Volume [m3]
-
-The water consumption is the water evaporated from the pad.   This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down.   This output variable appears when storage tank water is supplied to the cooler.
-
-#### Evaporative Cooler Starved Water Volume [m3]
-
-This is the water consumed by the evaporative cooler that could not accually be met by the storage tank.   This output variable appears when storage tank water is supplied to the cooler.
-
-#### Evaporative Cooler Starved Mains Water Volume [m3]
-
-This is the source (mains) of water consumed by the evaporative cooler that could not accually be met by the storage tank.   This output variable appears when storage tank water is supplied to the cooler.
-
-### EvaporativeCooler:Direct:ResearchSpecial
-
-This cooler is similar in principal to the EvaporativeCooler:Direct:CelDekPad. The model differs in that it gives the user a simple way of specify the cooler effectiveness. Using the ResearchSpecial input object also allows the cooler to control the amount of cooling based on node setpoints (controlled by SetpointManagers). This avoid problems from over cooling when conditions are such that loads are low and cooling power is high. 
-
-The model allows to vary the effectiveness depending on the primary air flow rates.  The design effectiveness is modified by multiplying with Effectiveness Flow Fraction Modifier Curve value.  The flow fraction is the ratio of the current primary airflow rate to the design flow rate. The recirculating and spray water pump power is assumed to vary with the primary air flow.  The design pump power is modified using user specified pump modifier curve value.  The normalized pump power modifier curve is a function of primary air flow fraction as a independent variable. 
-
-Also the direct evaporative cooler operating range can be controlled depending on the entering air dry bulb and wet bulb temperatures.  The operating range controlled based on minimum and maximum inlet node air temperature limits.  The evaporative cooler can be turned on or off depending user specified minimum and maximum temperature limits.  If the inlet node entering air temperature is lower or higher than the minimum and maximum limits, respectively, then the direct research special evaporative cooler is turned off.  If these two input fields are left blank then, no user specified operating temperature control is applied. Operating range control feature is primarily intended for application in data centers.
-
-#### Field: Name
-
-A unique identifying name for each cooler.
-
-#### Field: Availability Schedule Name
-
-The name of a schedule that defines when the evaporative cooler is available. A schedule value of 0 indicates that the evaporative cooler is off for that time period. A schedule value greater than 0 indicates that the evaporative cooler can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Cooler Design Effectiveness
-
-This field specifies the effectiveness at design flow rate that is applied to the wetbulb depression to determine the conditions leaving the cooler. This model assumes that the effectiveness can vary with supply air flow rate.  For effectiveness variation with supply air flow fraction enter the    Effectiveness Flow Ratio Modifier Curve Name    input field below. The flow fraction is the ratio of the sum of current primary air and secondary air sides flow rates and the sum of the design flow rates. 
-
-#### Field: Effectiveness Flow Ratio Modifier Curve Name
-
-This curve modifies the effectiveness design value specified the previous field by multiplying the value by the result of this curve.  The modifying curve is a function of flow fraction, which is the ratio of the current primary air flow rates divided by the design primary air flow rates. If this input field is left blank, the effectiveness is assumed to be constant. Any curve or table with one independent variable can be used. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
-
-#### Field:Primary Design Air Flow Rate  
-
-This numeric input field is the primary air design air flow rate in m3/s. This input field is autosizable. If the evaporative cooler is on main air loop branch, the design flow rate is the same as branch design flow rate, or else if it is on outdoor air system it will be the maximum of the the outdoor air design flow rate 
-and the half of the primary air flow rate on the main air loop branch. 
-
-#### Field: Recirculationg Water Pump Design Power
-
-This numeric input field is the recirculating and spray pump electric power at Secondary Design Air Flow Rate in W. This is the nominal water recirculating and spray pump power of evaporative cooler at primary air design flow rates and cooler design effectiveness.  This input field is autosizable. Average Pump Power 
-sizing factor was estimated from pump power and primary air design flow rates inputs from energyplus example
-files is about 90.0 [W/(m3/s)] (=90.0 ~ Pump Power / Primary Air Design Flow Rate). The factor ranges from 
-55.0 to 150.0 [W/(m3/s)].
-
-#### Field: Water Pump Power Sizing Factor
-
-This numeric input field value is recirculating water pump sizing factor in W/(m3/s). This field is used when the previous field is set to autosize. The pump design electric power is scaled with Secondary Design Air Flow Rate. This input field is autosizable. Average Pump Power sizing factor was estimated from pump power and primary air design flow rates inputs from energyplus example files is about 90.0 [W/(m3/s)] (=90.0 ~ Pump Power / Primary Air Design Flow Rate). The factor ranges from 55.0 to 150.0 [W/(m3/s)].
-
-#### Field: Water Pump Power Modifier Curve Name
-
-This alpha input field is the name of a dimensionless normalized pump power modifying curve. This curve modifies the pump electric power in the previous field by multiplying the design power by the result of this curve. The normalized curve is a function of the primary air flow fraction as independent variable.  The curve shall yield a value of 1.0 at a flow fraction of 1.0. The flow fraction is the ratio of the primary air during current operation divided by primary air Design Air Flow Rate. If this input field is left blank, the pump power is assumed to lineary vary with the load. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
-
-#### Field: Air Inlet Node Name
-
-The name of the air inlet node for the primary air flow path through the cooler.
-
-#### Field: Air Outlet Node Name
-
-The name of the air outlet node for the primary air flow path through the cooler.
-
-#### Field: Sensor Node Name
-
-This field specifies the name of a node that will provide system air temperature setpoint information.   A separate SetpointManager object should be setup to update this node.
-
-#### Field: Water Supply Storage Tank Name
-
-This field is optional. It is used to describe where the cooler obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the cooler will attempt to obtain all the water it uses from the tank. However, if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains.
-
-#### Field: Drift Loss Fraction
-
-This field is optional and can be used to model additional water consumed by the cooler from drift.   Drift is water that leaves the cooling media as droplets and does not evaporate into the process air stream.   For example, water may get blown off the evaporative media by winds and escape the air system.   The value entered here is a simple fraction of the water consumed by the cooler for normal process evaporation.   The amount of drift is this fraction times the water evaporated for the normal cooling process.   This field can be left blank and then there will be no added water consumption from drift.
-
-#### Field: Blowdown Concentration Ratio
-
-This field is optional and can be used to model additional water consumed by the cooler from blowdown.   Blowdown is water that is intentionally drained from the cooler   s sump to offset the build up of solids in the water that would otherwise occur because of evaporation.   The value entered here is dimensionless.   It can be characterized as the ratio of solids in the blowdown water to solids in the make up water.   Typical values are 3 to 5.   The default is 3.0.
-
-#### Field: Evaporative Cooler Operation Minimum Drybulb Temperature 
-
-This numeric field defines the evaporative cooler inlet node drybulb temperature minimum limit in degrees Celsius. The evaporative cooler will be turned off when evaporator cooler air inlet node dry-bulb temperature falls below this value. The typical minimum value is 16 &deg;C. Users are allowed to specify their own limits. If this field is left blank, then there is no drybulb temperature lower limit for evaporative cooler operation.  
-
-#### Field: Evaporative Operation Maximum Limit Wetbulb Temperature
-
-This numeric field defines the evaporative cooler air inlet node air wetbulb temperature maximum limits in degree Celsius. When the evaporative cooler air inlet node air wetbulb temperature exceeds this limit, then the evaporative cooler is turns off. The typical maximum value is 24 &deg;C. If this input field is left blank, then there is no wetbulb temperature upper limit for evaporative cooler operation.
-
-#### Field: Evaporative Operation Maximum Limit Drybulb Temperature
-
-This numeric field defines the evaporative cooler air inlet node drybulb temperature maximum limits in degree Celsius. The evaporative cooler will be turned off when the evaporative cooler air inlet node drybulb temperature exceeds this value. The typical maximum value is 28 &deg;C. If this input field is left blank, then there is no upper drybulb temperature limit for evaporative cooler operation.
-
-An example IDF entry is
-
-```idf
-EvaporativeCooler:Direct:ResearchSpecial,
-   Direct Evap Cooler, !- Name
-   ALWAYS_ON, !- Availability Schedule Name
-   0.7 , !- Cooler Design Effectiveness
-  ,     !- Effectiveness Flow Ratio Modifier Curve Name
-   30.0 , !- Recirculating Water Pump Design Power
-  ,     !- Water Pump Power Sizing Factor
-  ,     !- Water Pump Power Modifier Curve Name
-   OAIndRDD Evap Cooler- OADirect Evap CoolerNode , !- Air Inlet Node Name
-   OADirect Evap Cooler- OAMixing BoxNode, !- Air Outlet Node Name
-   OADirect Evap Cooler- OAMixing BoxNode, !- Sensor Node Name
-   , !- Water Supply Storage Tank Name
-   0.0, !- Drift Loss Fraction
-   3; !- Blowdown Concentration Ratio
-```
-
-### EvaporativeCooler:Direct:ResearchSpecial Outputs
-
-The output variables that are available for this direct evaporative cooler are shown below:
-
-* HVAC,Average, Evaporative Cooler Electric Power[W]
-
-* HVAC,Average, Evaporative Cooler Stage Effectiveness []
-
-* HVAC,Sum, Evaporative Cooler Electric Energy [J]
-
-* HVAC,Sum, Evaporative Cooler Water Volume[m3]
-
-* HVAC,Sum,Evaporative Cooler Mains Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Starved Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Starved Mains Water Volume [m3]
-
-#### Evaporative Cooler Electric Power[W]
-
-#### Evaporative Cooler Electric Energy [J]
-
-These output variables report the electric power and electric energy required to operate the water pump.
-
-#### Evaporative Cooler Stage Effectiveness []
-
-The cooler stage efficiency is defined as the temperature change of the supply air divided by the difference between the outdoor dry-bulb and wet-bulb temperatures, including the effect of the reduction in the primary air flow rate in other words, it is a measure of the approach to the entering air wet-bulb temperature.
-
-#### Evaporative Cooler Water Volume [m3]
-
-The water consumption is the water evaporated from the pad.   This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down.   This output variable appears when mains water is supplied to the cooler.
-
-#### Evaporative Cooler Mains Water Volume [m3]
-
-This is the source of the water consumed.   This output variable appears when mains water is supplied to the cooler.
-
-#### Evaporative Cooler Storage Tank Water Volume [m3]
-
-The water consumption is the water evaporated from the pad.   This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down.   This output variable appears when storage tank water is supplied to the cooler.
-
-#### Evaporative Cooler Starved Water Volume [m3]
-
-This is the water consumed by the evaporative cooler that could not accually be met by the storage tank.   This output variable appears when storage tank water is supplied to the cooler.
-
-#### Evaporative Cooler Starved Mains Water Volume [m3]
-
-This is the source (mains) of water consumed by the evaporative cooler that could not accually be met by the storage tank.   This output variable appears when storage tank water is supplied to the cooler.
-
-### EvaporativeCooler:Indirect:CelDekPad
-
-The dry coil indirect evaporative cooler, shown in the figure below, has a rigid media pad, similar to the direct evaporative stage, where the adiabatic cooling takes place. The secondary air leaves the rigid media pad and enters an air to air heat exchanger where it cools the supply air flowing through the heat exchanger tubes. The moist secondary air is then exhausted to the environment. The secondary air stream has its own fan and consists of a rigid media evaporative pad, with water recirculated from a reservoir. The water is pumped from the reservoir to a water distribution header, for water feed by gravity from above the media. The evaporative pad provides the area for the adiabatic saturation of the air.
-
-![](media/image419.svg)
-
-Figure 146. Evaporative Cooler -- Indirect Dry Coil
-
-The process that the secondary air goes through, A to C to D, is shown by the dashed lines in   the following figure. Process A to C is adiabatic cooling in the rigid media pad. Then the air enters the shell side of the heat exchanger and is sensibly heated from C to D by the warm supply air passing through the tube side. The secondary air inlet is modeled as a separate stream of outdoor air and the user has the option of defining the name of an outdoor air node.
-
-![](media/image420.svg)
-
-Figure 147. Secondary Air Process -- Indirect Dry Coil Evap Cooler
-
-The advantage of the dry coil heat exchanger is that the heat exchanger does not have the evaporation taking place on the outside of the tubes, thus no mineral deposits are left on the heat exchange surface to reduce the efficiency of the heat exchanger. The rigid media pads are designed to flush the mineral deposits to the sump, so the saturation efficiency of the pad stays relatively constant.
-
-#### Field: Name
-
-A unique identifying name for each evaporative cooler.
-
-#### Field:Availability Schedule Name
-
-The name of a schedule which defines when the evaporative cooler is available. A schedule value of 0 indicates that the evaporative cooler is off for that time period. A schedule value greater than 0 indicates that the evaporative cooler can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Direct Pad Area
-
-The face area of the evaporative pad in m<sup>2</sup>. With the area and mass flow rate, the air velocity is calculated and is used to determine the saturation efficiency on the secondary side of the evaporative cooler. This field is autosizable.
-
-#### Field: Direct Pad Depth
-
-The depth of the evaporative pad in meters. The pad depth is used to determine the saturation efficiency on the secondary side of the evaporative cooler. This field is autosizable.
-
-#### Field: Recirculating Water Pump Power Consumption
-
-This field is used to specify the power consumed by the evaporative cooler recirculating pump in Watts.
-
-#### Field: Secondary Air Fan Flow Rate
-
-This field is used to specify the secondary air fan flow rate and is specified in m<sup>3</sup>/sec.
-
-#### Field: Secondary Fan Total Efficiency
-
-This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1.
-
-#### Field: Secondary Fan Delta Pressure
-
-This field is used to specify the delta pressure across the secondary stage of the evaporative cooler in Pascals.
-
-#### Field: Indirect Heat Exchanger Effectiveness
-
-This field is used to specify the effectiveness of the indirect heat exchanger between the primary and secondary air flow.
-
-#### Field: Primary Air Inlet Node Name
-
-The name of the evaporative cooler   s primary air inlet node from the Air Loop Simulation. This is the air flow being cooled indirectly.
-
-#### Field: Primary Air Outlet Node Name
-
-The name of the evaporative cooler   s primary air outlet node from the Air Loop Simulation.
-
-#### Field: Control Type
-
-This input field is currently unused and can be left blank.
-
-#### Field: Water Supply Storage Tank Name
-
-This field is optional. It is used to describe where the cooler obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the cooler will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains.
-
-#### Field: Secondary Air Inlet Node Name
-
-This field is optional. It is used to explicitly define an outdoor air node for the inlet for secondary air stream. Defining an outdoor air node here allows using the height-dependent model for outdoor air conditions.
-
-And an IDF example showing how this object is specified:
-
-```idf
-  EvaporativeCooler:Indirect:CelDekPad,
-       IndirectEvapCooler1,         !- Name
-       FanAndCoilAvailSched,       !- Availability Schedule Name
-       0.6,                                         !- Direct Pad Area {m2}
-       0.2,                                         !- Direct Pad Depth {m}
-       225.,                                       !- Recirculating Water Pump Power Consumption {W}
-       1.0,                                         !- Secondary Air Fan Flow Rate {m3/s}
-       0.7,                                         !- Secondary Fan Total Efficiency
-       200.0,                                     !- Secondary Fan Delta Pressure {Pa}
-       0.67,                                       !- Indirect Heat Exchanger Effectiveness
-       EvapCoolerIndirectInletAirNode,   !- Primary Air Inlet Node Name
-       EvapCoolerDirectInletAirNode,   !- Primary Air Outlet Node Name
-       ,                                           !- Control Type
-       ,                                               !- Water Supply Storage Tank Name
-       Secondary side OA inlet node;   !- Secondary Air Inlet Node Name
-```
-
-### EvaporativeCooler:Indirect:CelDekPad Outputs
-
-The output variables that are available for the indirect dry evaporative cooler are shown below:
-
-* HVAC,Average, Evaporative Cooler Wetbulb Effectiveness
-
-* HVAC,Average, Evaporative Cooler Total Stage Effectiveness
-
-* HVAC,Average, Evaporative Cooler Electric Power[W]
-
-* HVAC,Sum, Evaporative Cooler Electric Energy [J]
-
-* HVAC,Sum, Evaporative Cooler Water Volume[m3]
-
-* HVAC,Sum,Evaporative Cooler Mains Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Starved Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Starved Mains Water Volume [m3]
-
-#### Evaporative Cooler Wetbulb Effectiveness
-
-The dry evaporation saturation efficiency is the saturation efficiency of the secondary or wet side air stream defined as the temperature change of the supply air divided by the difference between the outdoor dry-bulb and wet-bulb temperatures. In other words, it is a measure of the approach to the outdoor wet-bulb temperature.
-
-#### Evaporative Cooler Total Stage Effectiveness
-
-The total stage efficiency includes the sensible heat exchanger effectiveness of the heat exchanger in the supply air stream. It is the saturation efficiency multiplied by the heat exchanger effectiveness.
-
-#### Evaporative Cooler Electric Power[W]
-
-#### Evaporative Cooler Electric Energy [J]
-
-These output variables report the electric power and energy consumed by the secondary air fan and the sump pump.
-
-#### Evaporative Cooler Water Volume[m3]
-
-The water consumption is the water evaporated from the pad.   This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down.   This output variable appears when mains water is supplied to the cooler.
-
-#### Evaporative Cooler Mains Water Volume [m3]
-
-This is the source of the water consumed.   This output variable appears when mains water is supplied to the cooler.
-
-#### Evaporative Cooler Storage Tank Water Volume [m3]
-
-The water consumption is the water evaporated from the pad.   This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down.   This output variable appears when storage tank water is supplied to the cooler.
-
-#### Evaporative Cooler Starved Water Volume [m3]
-
-This is the water consumed by the evaporative cooler that could not accually be met by the storage tank.   This output variable appears when storage tank water is supplied to the cooler.
-
-#### Evaporative Cooler Starved Mains Water Volume [m3]
-
-This is the source (mains) of water consumed by the evaporative cooler that could not accually be met by the storage tank.   This output variable appears when storage tank water is supplied to the cooler.
-
-### EvaporativeCooler:Indirect:WetCoil
-
-The wetted coil evaporative cooler shown in the figure below, has water sprayed directly on the tubes of the heat exchanger where latent cooling takes place. The vaporization of the water on the outside of the heat exchanger tubes allows the simultaneous heat and mass transfer which removes heat from the supply air on the tube side. Then the moist secondary air is exhausted. The secondary air stream has its own fan.
-
-![](media/image421.svg)
-
-Figure 148. Evaporative Cooler     Indirect Wet Coil
-
-The process that the secondary air goes through, A to C on the following figure, is a path of simultaneous heat and mass transfer, but it does not follow a line of constant enthalpy as in the direct stage. The process is not adiabatic due to the heat gain from the supply air flowing through the tubes of the heat exchanger.
-
-![](media/image422.svg)
-
-Figure 149. Secondary Air Process     Indirect Wet Coil Evap Cooler
-
-The wet coil heat exchanger can have a higher stage efficiency than the dry coil due to a higher heat transfer rate on the outside of the heat exchanger tubes. Over the operating lifetime of the heat exchanger, the vaporization taking place on the heat exchange surface can leave mineral deposits which will decrease the effectiveness of the heat exchanger.
-
-#### Field: Name
-
-A unique identifying name for each evaporative cooler.
-
-#### Field:Availability Schedule Name
-
-The name of a schedule which defines when the evaporative cooler is available. A schedule value of 0 indicates that the evaporative cooler is off for that time period. A schedule value greater than 0 indicates that the evaporative cooler can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Coil Maximum Efficiency
-
-The maximum efficiency of the stage is a combination of the efficiency due to the simultaneous heat and mass transfer on the outside of the tube and the efficiency of the heat exchanger. This value can be higher than the dry coil overall efficiency since the convective coefficients on the outside of the tube are larger.
-
-#### Field: Coil Flow Ratio
-
-The Coil Flow Ratio is determined from performance data. The Coil Flow Ratio tells how quickly the efficiency of the stage would decrease with a mismatch of the supply and secondary flows.
-
-#### Field: Recirculating Water Pump Power Consumption
-
-This field is used to specify the power consumed by the evaporative cooler recirculating pump in Watts.
-
-#### Field: Secondary Air Fan Flow Rate
-
-This field is used to specify the secondary air fan flow rate and is specified in m<sup>3</sup>/sec.
-
-#### Field: Secondary Air Fan Total Efficiency
-
-This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1..
-
-#### Field: Secondary Air Fan Delta Pressure
-
-This field is used to specify the delta pressure across the secondary stage of the evaporative cooler in Pascals.
-
-#### Field: Primary Air Inlet Node Name
-
-The name of the evaporative cooler air inlet from the Air Loop Simulation.
-
-#### Field: Primary Air Outlet Node Name
-
-The name of the evaporative cooler air outlet from the Air Loop Simulation.
-
-#### Field: Control Type
-
-This input field is currently unused and can be left blank.
-
-#### Field: Water Supply Storage Tank Name
-
-This field is optional. It is used to describe where the cooler obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the cooler will attempt to obtain all the water it uses from the tank. However if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains.
-
-#### Field: Secondary Air Inlet Node Name
-
-This field is optional. It is used to explicitly define an outdoor air node for the inlet for secondary air stream. Defining an outdoor air node here allows using the height-dependent model for outdoor air conditions.
-
-#### Field: Drift Loss Fraction
-
-This field is optional and can be used to model additional water consumed by the cooler from drift.   Drift is water that leaves the cooling media as droplets and does not evaporate into the process air stream.   For example, water may get blown off the evaporative media by winds and escape the air system.   The value entered here is a simple fraction of the water consumed by the cooler for normal process evaporation.   The amount of drift is this fraction times the water evaporated for the normal cooling process.   This field can be left blank and then there will be no added water consumption from drift.
-
-#### Field: Blowdown Concentration Ratio
-
-This field is optional and can be used to model additional water consumed by the cooler from blowdown.   Blowdown is water that is intentionally drained from the cooler   s sump to offset the build up of solids in the water that would otherwise occur because of evaporation.   The value entered here is dimensionless.   It can be characterized as the ratio of solids in the blowdown water to solids in the make up water.   Typical values are 3 to 5.   The default is 3.0.
-
-And an IDF example showing how this object is specified:
-
-```idf
-EvaporativeCooler:Indirect:WetCoil,
-       IndirectEvapCooler1,         !- Name
-       FanAndCoilAvailSched,       !- Availability Schedule Name
-       0.8,                                         !- Coil Maximum Efficiency
-       0.16,                                       !- Coil Flow Ratio
-       225.,                                       !- Recirculating Water Pump Power Consumption {W}
-       1.0,                                         !- Secondary Air Fan Flow Rate {m3/s}
-       0.7,                                         !- Secondary Air Fan Total Efficiency
-       200.0,                                     !- Secondary Air Fan Delta Pressure {Pa}
-       EvapCoolerIndirectInletAirNode,   !- Primary Air Inlet Node Name
-       EvapCoolerDirectInletAirNode,   !- Primary Air Outlet Node Name
-       ,                                               !- Control Type
-       ,                                               !- Water Supply Storage Tank Name
-       Secondary side OA inlet node;   !- Secondary Air Inlet Node Name
-```
-
-
-
-### EvaporativeCooler:Indirect:WetCoil Outputs
-
-The output variables that are available for the wet indirect evaporative cooler are shown below:
-
-* HVAC,Average, Evaporative Cooler Total Stage Effectiveness
-
-* HVAC,Average, Evaporative Cooler Electric Power[W]
-
-* HVAC,Sum, Evaporative Cooler Electric Energy [J]
-
-* HVAC,Sum, Evaporative Cooler Water Volume[m3]
-
-* HVAC,Sum,Evaporative Cooler Mains Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Starved Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Starved Mains Water Volume [m3]
-
-#### Evaporative Cooler Total Stage Effectiveness []
-
-The Total Stage Efficiency is defined as the temperature change of the supply air divided by the difference between the outdoor dry-bulb and wet-bulb temperatures, including the effect of the reduction in flow because of the secondary air stream. In other words, it is a measure of the approach to the outdoor wet-bulb temperature.
-
-#### Evaporative Cooler Electric Power [W]
-
-#### Evaporative Cooler Electric Energy [J]
-
-These output variables report the electric power and energy that are consumed by the secondary air fan and the sump pump.
-
-#### Evaporative Cooler Water Volume [m3]
-
-The water consumption is the water evaporated from the pad.   This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down.   This output variable appears when mains water is supplied to the cooler.
-
-#### Evaporative Cooler Mains Water Volume [m3]
-
-This is the source of the water consumed.   This output variable appears when mains water is supplied to the cooler.
-
-#### Evaporative Cooler Storage Tank Water Volume [m3]
-
-The water consumption is the water evaporated from the pad.   This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down.   This output variable appears when storage tank water is supplied to the cooler.
-
-#### Evaporative Cooler Starved Water Volume [m3]
-
-This is the water consumed by the evaporative cooler that could not accually be met by the storage tank.   This output variable appears when storage tank water is supplied to the cooler.
-
-#### Evaporative Cooler Starved Mains Water Volume [m3]
-
-This is the source (mains) of water consumed by the evaporative cooler that could not accually be met by the storage tank.   This output variable appears when storage tank water is supplied to the cooler.
-
-### EvaporativeCooler:Indirect:ResearchSpecial
-
-This cooler is similar in principal to the EvaporativeCooler:Indirect:CelDekPad and EvaporativeCooler:Indirect:WetCoil (see Figure 147, Figure 148, and Figure 149). The model differs in that it gives the user more flexibility to specify the source of secondary air. The cooler effectiveness with respect to wetbulb depression is allowed to go beyond 1.0. Using the ResearchSpecial input object also allows the cooler to control the amount of cooling based on node setpoints (controlled by SetpointManagers). This avoid problems from over cooling when conditions are such that loads are low and cooling power is high. Fan power is assumed to vary linearly when the cooler is operating at less than full capacity.
-
-The indirect evaporative cooler research special calculation procedure allows accounting for dry and wet effectiveness value variation with flow fraction.  Two effectiveness modifier curves are included as optional user inputs for this purpose.  Effectiveness modifier curves operate on the design dry and wet effectiveness values. The flow fraction is calculated as a ratio of the sum of current primary and secondary air flow rates to the sum of the design flow rates. Model also accounts for fan and recirculation water pump power variation with secondary air flow rates using pump power modifying curve. The fan power is calculated by multiplying the design fan power using fan power modify curve value evaluated at current secondary air flow fraction. Similarly, recirculating pump power is is calculated by multiplying the design pump power by pump power modifier curve value evaluated at current secondary air flow fraction. If the secondary air fan and recirculating pump power modifier curves are not specified, then fan and pump power are assumed to vary linearly with part load fraction.
-
-#### Field: Name
-
-A unique identifying name for each cooler.
-
-#### Field: Availability Schedule Name
-
-The name of a schedule that defines when the evaporative cooler is available. A schedule value of 0 indicates that the evaporative cooler is off for that time period. A schedule value greater than 0 indicates that the evaporative cooler can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Cooler Wetbulb Design Effectiveness
-
-This field specifies the design effectiveness that is applied to the wetbulb depression to determine the conditions leaving the cooler. This effectiveness is a complicated function of the efficiency with which heat and mass are transferred on the secondary side and the efficiency of heat exchange between the secondary and primary flows. The model assumes that the effectiveness a function of flow fraction. The flow fraction is the ratio of the sum of primary air and secondary air current flow rates and the sum of the primary air and secondary air design flow rates.
-
-#### Field: Wet Bulb Effectiveness Flow Ratio Modifier Curve Name
-
-This curve modifies the wet bulb effectiveness design value specified the previous field by multiplying the value by the result of this curve.  The modifying curve is a function of flow fraction, which is the ratio of the sum of the primary and secondary flow rates divided by the sum of the design flow rates. If this input field is left blank, the effectiveness is assumed to be constant. Any curve or table with one independent variable can be used. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
-
-#### Field: Cooler Drybulb Design Effectiveness
-
-This input value is dry bulb design effectiveness of the evaporative cooler. This is the nominal design dry blub effectiveness with respect to dry bulb temperature difference, i.e., dry operation and at design air flow rates, and no water evaporation or spraying on the secondary side.
-
-#### Field Drybulb Effectiveness Flow Ratio Modifier Curve Name
-
-This this curve modifies the drybulb effectiveness in the previous field (eff_db_design) by multiplying the design effectiveness value by the result of this curve.  The curve is evaluated flow fraction as independent variable.  The flow fraction is the ratio of sum of the primary and secondary flow rates divided by the sum of the design flow rates. If this input field is left blank, the effectiveness is assumed to be constant. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
-
-#### Field: Recirculating Water Pump Design Power
-
-This numeric input field is the recirculating pump electric power at Secondary Design Air Flow Rate in W. This is the nominal design pump power water recirculation and spray for evaporation at design secondary air flow rates and cooler design effectiveness.  This input field is autosizable.
-
-#### Field: Water Pump Power Sizing Factor
-
-This numeric input field value is recirculating water pump sizing factor in W/(m3/s). This field is used when the previous field is set to autosize. The pump design electric power is scaled with Secondary Design Air Flow Rate. Average Pump Power sizing factor was estimated from pump power and secondary air design flow rates inputs from energyplus example files is about 90.0 [W/(m3/s)] (=90.0 ~ Pump Power / Secondary Air Design Flow Rate). The factor ranges from 55.0 to 150.0 [W/(m3/s)].
-
-#### Field: Water Pump Power Modifier Curve Name
-
-This alpha input field is the name of a dimensionless normalized pump power modifying curve. This curve modifies the pump electric power in the previous field by multiplying the design power by the result of this curve. The normalized curve is a function of the secondary side flow fraction as independent variable.  The curve shall yield a value of 1.0 at a flow fraction of 1.0. The flow fraction is the secondary air flow rate during operation divided by Secondary Design Air Flow Rate. If this input field is left blank, the pump power is assumed to be constant. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
-
-#### Field: Secondary Air Design Flow Rate
-
-This field is used to specify the secondary air fan flow rate and is specified in m<sup>3</sup>/s. This flow rate would typically be similar in magnitude to the flow through the primary side. This field can be autosized. When it is autosized, the program detects if the component is in the main air loop or on an outdoor air path.   If it is on the main air loop, then the flow rate is set to the AirLoopHVAC system   s design supply air flow rate (which is the maximum required for heating and cooling).   If it is on the outdoor air path, then the flow rate is set to the larger of either the design minimum outdoor air flow rate or one-half of the main air loop design flow rate. The flow rate is used to determine parasitic fan energy and cooler effectiveness. The flow rate (and fan power) is effectively reduced by cycling when the amount of cooling needs to be restricted for control purpose.  This field can be autosized. When this input is autosized, the program calculates by scaling the Primary Air Design Flow Rate using secondary air scaling factor specified in the input field below.
-
-#### Field: Secondary Air Flow Scaling Factor
-
-This numeric input field is used to scale the secondary air design flow rate and it is dimensionless. This field is used when the previous field is set to autosize. The Primary Design Air Flow Rate is scaled using this factor to calculate the secondary design air flow rate.
-
-#### Field: Secondary Air Fan Design Power
-
-This numeric input field is the fan electric power at Secondary Design Air Flow Rate.  This is the nominal design electric power at full speed of the secondary air fan.   This input field is autosizable.
-
-#### Field: Secondary Air Fan Sizing Specific Power
-
-This input field value is secondary air fan sizing specific power in W/(m3/s).  This field is used when the previous field is set to autosize. The fan power is scaled with Secondary Design Air Flow Rate.
-
-#### Field: Secondary Air Fan Power Modifier Curve Name
-
-This input field is the name of a dimensionless normalized curve.  The normalized curve modifies the design secondary air fan power in the previous field by multiplying the value by the result of this curve.  The normalized curve is a function of the secondary side flow fraction as independent variable.  The curve shall yield a value of 1.0 at a flow fraction of 1.0. The flow fraction is the secondary air flow rate during operation divided by Secondary Design Air Flow Rate. If this input field is left blank, the fan power is assumed to be constant. Any curve or table with one independent variable can be used: Curve:Linear, Curve:Quadratic, Curve:Cubic, Curve:Quartic, Curve:Exponent, Curve:ExponentialSkewNormal, Curve:Sigmoid, Curve:RectuangularHyperbola1, Curve:RectangularHyperbola2, Curve:ExponentialDecay, Curve:DoubleExponentialDecay, and Table:OneIndependentVariable.
-
-#### Field: Primary Air Inlet Node Name
-
-The name of the air inlet node for the primary air flow path through the cooler.
-
-#### Field: Primary Air Outlet Node Name
-
-The name of the air outlet node for the primary air flow path through the cooler.
-
-#### Field:Primary Design Air Flow Rate  
-
-This numeric input field is the primary air design air flow rate in m3/s. This input field is autosizable. If the evaporative cooler is on main air loop branch, the design flow rate is the same as branch design flow rate, or else if it is on outdoor air system it will be the maximum of the the outdoor air design flow rate 
-and the half of the primary air flow rate on the main air loop branch. 
-
-#### Field: Dewpoint Effectiveness Factor
-
-This field specifies an effectiveness that is applied to the dewpoint depression to determine a bound for the conditions leaving the cooler. The model uses the warmer of the two temperatures determined from wetbulb depression and dewpoint depression.
-
-#### Field: Secondary Air Inlet Node Name
-
-This field specifies the name of the node providing air to the secondary/wet side of the cooler. Typically this node could appear in an outdoor air node list or be part of an air system loop.
-
-#### Field: Secondary Air Outlet Node Name
-
-This alpha input field is the name of the secondary air side outlet node.
-
-#### Field: Sensor Node Name
-
-This field specifies the name of a node that will provide system air temperature setpoint information. A separate SetpointManager object should be setup to update this node.
-
-#### Field: Relief Air Inlet Node Name
-
-This field is optional, but can be used to feed two sources of secondary air into the wet side of the cooler. Typical use is to run the air system relief air into the system. The model first uses all of the air flow available from this node and then adds the air flow from the secondary air inlet node to make up the total defined by Secondary air Fan Flow Rate.
-
-#### Field: Water Supply Storage Tank Name
-
-This field is optional. It is used to describe where the cooler obtains water used for evaporative cooling. If blank or omitted, then the cooler will obtain water directly from the mains. If the name of a WaterUse:Storage object is used here, then the cooler will obtain its water from that tank. If a tank is specified, the cooler will attempt to obtain all the water it uses from the tank. However, if the tank cannot provide all the water the cooler needs, then the cooler will still operate and obtain the rest of the water it needs from the mains.
-
-#### Field: Drift Loss Fraction
-
-This field is optional and can be used to model additional water consumed by the cooler from drift.   Drift is water that leaves the cooling media as droplets and does not evaporate into the process air stream.   For example, water may get blown off the evaporative media by winds and escape the air system.   The value entered here is a simple fraction of the water consumed by the cooler for normal process evaporation.   The amount of drift is this fraction times the water evaporated for the normal cooling process.   This field can be left blank and then there will be no added water consumption from drift.
-
-#### Field: Blowdown Concentration Ratio
-
-This field is optional and can be used to model additional water consumed by the cooler from blowdown.   Blowdown is water that is intentionally drained from the cooler   s sump to offset the build up of solids in the water that would otherwise occur because of evaporation.   The value entered here is dimensionless.   It can be characterized as the ratio of solids in the blowdown water to solids in the make up water.   Typical values are 3 to 5.   The default is 3.0.
-
-#### Field: Evaporative Operation Minimum Limit Drybulb Temperature 
-
-This input field value defines the secondary air inlet node drybulb temperature limits in degree Celsius. When the secondary side entering air dry bulb temperature drops below this limit, then the evaporative cooler operation mode changes to dry heat exchanger. Users specify their own limits. If this field is left blank, then there is no drybulb temperature lower limit for evaporative cooler operation.  If operating range control is desired then this input field and the next two input fields should be specified or all the three should be left blank or left out.  If no minimum drybulb temperature limit is required while there are maximum drybulb and wetbulb temperature limits then specify very low temperature limit value (e.g., -99.0 C).
-
-#### Field: Evaporative Operation Maximum Limit Wetbulb Temperature
-
-This input field value defines the secondary air inlet node wetbulb temperature limits in degree Celsius. When the secondary side entering air wet bulb temperature exceeds this limit, then the evaporative cooler is turns off and does not attempt to do any cooling. If this field is left blank, then there is no wetbulb temperature maximum limit for evaporative cooler wet operation mode. If no upper wetbulb temperature limits is desired while there are minimum drybulb and maximum drybulb upper temperature limits then then specify very high maximum wetbulb temperature limit value (e.g. 99.0 C).
-
-#### Field: Evaporative Operation Maximum Limit Drybulb Temperature
-
-This input field value defines the secondary air inlet node drybulb temperature limits in degree Celsius. When the secondary side entering air drybulb temperature exceeds this limit, the evaporative cooler will not run in dry operation mode or may be turned off depending on its wetbulb temperature. If this field is left blank, then there is no drybulb temperature maximum limit for evaporative cooler dry operation mode.
-
-If no drybulb temperature limit is desired while there are minimum drybulb and maximum wetbulb temperature limits then specify very high maximum drybulb temperature limit value (e.g. 99.0 C).
-
-An IDF example is shown below:
-
-```idf
-EvaporativeCooler:Indirect:ResearchSpecial,
-    DataC_IndirectEvapCooler,     !- Name
-    ALWAYS_ON,                    !- Availability Schedule Name
-    0.75,                         !- Cooler Wetbulb Design Effectiveness
-    ,              !- Wetbulb Effectiveness Flow Ratio Modifier Curve Name
-    ,                          !- Cooler Drybulb Design Effectiveness
-    ,              !- Drybulb Effectiveness Flow Ratio Modifier Curve Name
-    autosize,                     !- Recirculating Water Pump Power
-    autosize,                     !- Secondary Air Design Flow Rate  
-    1.0,                          !- Secondary Air Flow Scaling Factor
-
-    autosize,                     !- Secondary Air Fan Design Power
-    800.0,                        !- Secondary Air Fan Sizing Specific Power W
-    ,               !- Secondary Air Fan Power Modifier Curve Name
-    Return Air Node,              !- Primary Air Inlet Node Name
-    IndEC Outlet Node,            !- Primary Air Outlet Node Name
-    autosize,                     !- Primary Design Air Flow Rate  
-    0.9 ,                         !- Dewpoint Effectiveness Factor
-    IndEC OA Air Inlet Node,      !- Secondary Air Inlet Node Name
-    IndEC OA Air Outlet Node,     !- Secondary Air Outlet Node Name
-    IndEC Outlet Node,            !- Sensor Node Name
-    ,                             !- Relief Air Inlet Node Name
-    ,                             !- Water Supply Storage Tank Name
-    0.0,                          !- Drift Loss Fraction
-    ;                             !- Blowdown Concentration Ratio
-```
-
-### EvaporativeCooler:Indirect:ResearchSpecial Outputs
-
-The output variables that are available for the EvaporativeCooler:Indirect:ResearchSpecial object are shown below:
-
-* HVAC,Average,Evaporative Cooler Total Stage Effectiveness
-
-* HVAC,Average,Evaporative Cooler Part Load Ratio
-
-* HVAC,Average,Evaporative Cooler Dewpoint Bound Status
-
-* HVAC,Average,Evaporative Cooler Operating Mode Satus []
-
-* HVAC,Sum,Evaporative Cooler Electric Energy [J]
-
-* HVAC,Average,Evaporative Cooler Electric Power [W]
-
-* HVAC,Sum,Evaporative Cooler Storage Tank Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Starved Water Volume [m3]
-
-* HVAC,Sum,Evaporative Cooler Starved Mains Water Volume [m3]
-
-
-
-#### Evaporative Cooler Total Stage Effectiveness []
-
-The Total Stage Efficiency is defined as the temperature change of the supply air divided by the difference between the primary air entering dry-bulb temperature and the secondary air enterig wet-bulb temperature for wet operating mode or the the difference between the primary air entering dry-bulb temperature and the secondary air enterig dry-bulb temperature for dry operating mode, including the effect of the reduction in flow because of the secondary air stream. In other words, it is a measure of the approach to the secondary air wet-bulb temperature for wet operating mode, or it is a measure of the approach to the secondary air entering dry-bulb temperature for dry operating mode.
-
-#### Evaporative Cooler Operating Mode Status []
-
-This output variable provides the operating modes or status of the indirect evaporative cooler. This output variable can have status indicator integer value of 0, 1, or 2 representing Off, Dry and Wet operating modes, respectively.
-
-#### Evaporative Cooler Part Load Ratio []
-
-This output variable provides the part load fraction of the indirect cooler.   The ResearchSpecial cooler model is able to modulate to meet a temperature set point to avoid over cooling.   This output variable is the fraction formed by the ratio of the capacity needed over the maximum cooling capacity available.   A value of 1.0 corresponds to full capacity cooling.
-
-#### Evaporative Cooler Dewpoint Bound Status []
-
-This output variable is a flag that indicates if the modeling was based on dewpoint effectivenss rather than wetbulb effectiveness   The ResearchSpecial model is usually based on wet-bulb approach, but since values in excess of 1.0 are allowed, there is a secondary constraint imposed by dewpoint.   If the dewpoint effectiveness was applied, then this flag variable will have the value 1.0, otherwise it is 0.0.
-
-#### Evaporative Cooler Electric Power [W]
-
-#### Evaporative Cooler Electric Energy [J]
-
-These output variables report the electric power and energy that are consumed by the secondary air fan and the sump pump.
-
-#### Evaporative Cooler Water Volume [m3]
-
-The water consumption is the water evaporated from the pad.   This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down.   This output variable appears when mains water is supplied to the cooler.
-
-#### Evaporative Cooler Mains Water Volume [m3]
-
-This is the source of the water consumed.   This output variable appears when mains water is supplied to the cooler.
-
-#### Evaporative Cooler Storage Tank Water Volume [m3]
-
-The water consumption is the water evaporated from the pad.   This water consumption is only from the direct thermodynamics of water evaporation and does not include other sources of consumption such as drift or concentration blow down.   This output variable appears when storage tank water is supplied to the cooler.
-
-#### Evaporative Cooler Starved Water Volume [m3]
-
-This is the water consumed by the evaporative cooler that could not accually be met by the storage tank.   This output variable appears when storage tank water is supplied to the cooler.
-
-#### Evaporative Cooler Starved Mains Water Volume [m3]
-
-This is the source (mains) of water consumed by the evaporative cooler that could not accually be met by the storage tank.   This output variable appears when storage tank water is supplied to the cooler.
-
-Group     Heat Recovery
----------------------
-
-### HeatExchanger:AirToAir:FlatPlate
-
-The air-to-air flat plate heat exchanger is an HVAC component typically used for exhaust or relief air heat recovery. The user can choose the flow arrangement type: counter flow, parallel flow, or cross flow with both streams unmixed. The input requires no geometric data. Performance is defined by specifying primary outlet air temperature at nominal (user specified) inlet conditions. In addition, the ratio (h<sup>.</sup>A)<sub>p</sub> / (h<sup>.</sup>A)<sub>s</sub> at nominal flow needs to be input, where h is the convective heat transfer   coefficient, A is the surface area, p stands for primary side, s for secondary side.
-
-If the heat exchanger is operated in conjunction with an outdoor air economizer (economizer lockout set to *Yes*), the nominal supply air flow rate should be set equal to the minimum outdoor air flow rate specified in the Controller:OutdoorAir. The heat exchanger detects that the economizer is operating by the fact that its inlet air flow rate is greater than its nominal supply air flow rate.
-
-#### Field: Name
-
-A unique user-assigned name for a particular air-to-air flat plate heat exchanger unit. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the unit can run during a given time period. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Flow Arrangement Type
-
-The user specified flow arrangement of the heat exchanger. The possible inputs are *CounterFlow*, *ParallelFlow*, or *CrossFlowBothUnmixed*.
-
-#### Field: Economizer Lockout
-
-This input denotes whether the heat exchanger unit is locked out (bypassed) when the air-side economizer is operating. Both the economizer and high humidity control (Ref. Controller:OutdoorAir) activate the heat exchanger lockout as specified by this input. The input choices are *Yes* (meaning locked out) or *No*. The default input for this field is Yes.
-
-#### Field: Ratio of Supply to Secondary hA Values
-
-The ratio (h<sup>.</sup>A)<sub>p</sub> / (h<sup>.</sup>A)<sub>s</sub> at nominal flow. h is the surface convective heat transfer coefficient, A is the heat transfer area, and p and s stand for primary side and secondary side respectively. A typical value for this ratio is 1.0.
-
-#### Field: Nominal Supply Air Flow Rate
-
-The nominal primary side air flow rate in cubic meters per second. If the unit is operated in conjunction with an outdoor air economizer this should be equal to the minimum outdoor air flow rate. This field is autosizable.
-
-#### Field: Nominal Supply Air Inlet Temperature
-
-The nominal primary side air inlet temperature in Celsius.
-
-#### Field: Nominal Supply Air Outlet Temperature
-
-The nominal primary side air outlet temperature in Celsius.
-
-#### Field: Nominal Secondary Air Flow Rate
-
-The nominal secondary side air flow rate in cubic meters per second. This field is autosizable. It is equal to the primary side air flow rate defined above, if autosized.
-
-#### Field: Nominal Secondary Air Inlet Temperature
-
-The nominal secondary side air inlet temperature in Celsius.
-
-#### Field: Nominal Electric Power
-
-The electric consumption rate of the unit in watts. Electric power is considered constant whenever the unit operates. This input can be used to model electric power consumption by controls (transformers, relays, etc.) and/or a motor for a rotary heat exchanger. None of this electric power contributes thermal load to the supply or exhaust air streams. The default value for this field is 0.
-
-#### Field: Supply Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its primary inlet air.
-
-#### Field: Supply Air Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its primary outlet air.
-
-#### Field: Secondary Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its secondary inlet air.
-
-#### Field: Secondary Air Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its secondary outlet air.
-
-An IDF example:
-
-```idf
-   HeatExchanger:AirToAir:FlatPlate,
-       OA Heat Recovery 1,         !- Name
-       FanAndCoilAvailSched,       !- Availability Schedule Name
-       CounterFlow,                !- Flow Arrangement Type
-       Yes,                        !- Economizer Lockout
-       1.0,                        !- Ratio of Supply to Secondary hA Values
-       0.4333,                     !- Nominal Supply Air Flow Rate {m3/s}
-       5.0,                        !- Nominal Supply Air Inlet Temperature {C}
-       15.0,                       !- Nominal Supply Air Outlet Temperature {C}
-       0.4333,                     !- Nominal Secondary Air Flow Rate {m3/s}
-       20.0,                       !- Nominal Secondary Air Inlet Temperature {C}
-       0.0,                        !- Nominal Electric Power {W}
-       Desiccant Process Outlet Node,   !- Supply Air Inlet Node Name
-       Heat Recovery Outlet Node,   !- Supply Air Outlet Node Name
-       Relief Air Outlet Node,   !- Secondary Air Inlet Node Name
-       Heat Recovery Secondary Outlet Node;   !- Secondary Air Outlet Node Name
-```
-
-### HeatExchanger:AirToAir:FlatPlate Outputs
-
-* HVAC,Average,Heat Exchanger Sensible Heating Rate [W]
-
-* HVAC,Sum,Heat Exchanger Sensible Heating Energy [J]
-
-* HVAC,Average,Heat Exchanger Latent Gain Rate [W]
-
-* HVAC,Sum,Heat Exchanger Latent Gain Energy [J]
-
-* HVAC,Average,Heat Exchanger Total Heating Rate [W]
-
-* HVAC,Sum,Heat Exchanger Total Heating Energy [J]
-
-* HVAC,Average,Heat Exchanger Sensible Cooling Rate [W]
-
-* HVAC,Sum,Heat Exchanger Sensible Cooling Energy [J]
-
-* HVAC,Average,Heat Exchanger Latent Cooling Rate [W]
-
-* HVAC,Sum,Heat Exchanger Latent Cooling Energy [J]
-
-* HVAC,Average,Heat Exchanger Total Cooling Rate [W]
-
-* HVAC,Sum,Heat Exchanger Total Cooling Energy [J]
-
-* HVAC,Average,Heat Exchanger Electric Power[W]
-
-* HVAC,Sum,Heat Exchanger Electric Energy [J]
-
-#### Heat Exchanger Sensible Heating Rate [W]
-
-This output is the sensible heating rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, the supply air inlet and outlet conditions, and the specific heat of the inlet supply air. A positive value is reported if the supply air is heated by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Sensible Heating Energy [J]
-
-This output is the sensible heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Latent Gain Rate [W]
-
-This output is the latent heating rate (humidification) of the supply air by the heat exchanger in Watts. This rate is determined by taking the difference between the Heat Exchanger Total Heating Rate and the Heat Exchanger Sensible Heating Rate. A positive value is reported if the supply air is humidified by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Latent   Heating Energy [J]
-
-This output is the latent heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Total Heating Rate [W]
-
-This output is the total heating rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, and the enthalpy of the supply air entering and leaving the unit. A positive value is reported if the enthalpy of the supply air is increased by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Total Heating Energy [J]
-
-This output is the total heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforHeating, GroupKey = System (ref. Output:Meter objects).
-
-#### Heat Exchanger Sensible Cooling Rate [W]
-
-This output is the sensible cooling rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, the supply air inlet and outlet conditions, and the specific heat of the inlet supply air. A positive value is reported if the supply air is cooled by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Sensible Cooling Energy [J]
-
-This output is the sensible cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Latent Cooling Rate [W]
-
-This output is the latent cooling rate (dehumidification) of the supply air by the heat exchanger in Watts. This rate is determined by taking the difference between the Heat Exchanger Total Cooling Rate and the Heat Exchanger Sensible Cooling Rate. A positive value is reported if the supply air is dehumidified by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Latent Cooling Energy [J]
-
-This output is the latent cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Total Cooling Rate [W]
-
-This output is the total cooling rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, and the enthalpy of the supply air entering and leaving the unit. A positive value is reported if the enthalpy of the supply air is decreased by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Total Cooling Energy [J]
-
-This output is the total cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported. This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforCooling, GroupKey = System (ref. Output:Meter objects).
-
-#### Heat Exchanger Electric Power [W]
-
-This output is the electric consumption rate of the unit in Watts. This rate is applicable whenever the unit operates (i.e., whenever the unit is scheduled to be available and supply and exhaust air flows exist).
-
-#### Heat Exchanger Electric Energy [J]
-
-This output is the electric consumption of the unit in Joules for the timestep being reported. This ouput is also added to a meter with ResourceType = Electricity, EndUseKey = HeatRecovery, GroupKey = System (ref. Output:Meter objects).
-
-### HeatExchanger:AirToAir:SensibleAndLatent
-
-![](media/image423.svg)
-
-The sensible and latent air-to-air heat exchanger is an HVAC component typically used for exhaust or relief air heat recovery (Figure 150). Heat exchanger performance can be specified to transfer sensible energy, latent energy or both between the supply and exhaust air streams. The input requires no geometric data. Performance is defined by specifying sensible and/or latent effectiveness at 75% and 100% of the nominal (rated) supply air flow rate at two operating conditions as shown in Table 30.
-
-Figure 150. Schematic of the Sensible and Latent Air-to-Air Heat Exchanger
-
-Table 30. Operating Conditions for Defining Heat Exchanger Performance
-
-<table class="table table-striped">
-  <tr>
-    <th rowspan="2">Parameter</th>
-    <th colspan="2">Conditions</th>
-  </tr>
-  <tr>
-    <td>Heating</td>
-    <td>Cooling</td>
-  </tr>
-  <tr>
-    <td>Entering supply air temperature:</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>    Dry-bulb:</td>
-    <td>1.7°C (35°F)</td>
-    <td>35°C (95°F)</td>
-  </tr>
-  <tr>
-    <td>    Wet-bulb:</td>
-    <td>0.6°C (33°F)</td>
-    <td>26°C (78°F)</td>
-  </tr>
-  <tr>
-    <td>Entering supply air temperature:</td>
-    <td></td>
-    <td></td>
-  </tr>
-  <tr>
-    <td>    Dry-bulb:</td>
-    <td>21°C (70°F)</td>
-    <td>24°C (75°F)</td>
-  </tr>
-  <tr>
-    <td>    Wet-bulb:<br></td>
-    <td>14°C (58°F)</td>
-    <td>17C (63F)</td>
-  </tr>
-</table>
-
-Note: Conditions consistent with the Air-Conditioning and Refrigeration Institute   s (ARI) Standard 1060-2001.
-
-This object models the basic operation of an air-to-air heat exchanger. Heat exchange between the supply and exhaust air streams occurs whenever the unit is scheduled to be available (Availability schedule) and supply/exhaust air flow is present. This heat exchanger object can be used in conjunction with a conventional air-side economizer (i.e., specify ModulateFlow in the Controller:OutdoorAir object), whereby heat exchange is suspended whenever the air-side economizer (or high humidity control) is active (i.e., air flow is fully bypassed around a fixed-plate heat exchanger or the rotation of a rotary heat exchanger is stopped). This object is also able to suspend heat exchange for the purpose of providing free cooling operation in the absence of a conventional air-side economizer (i.e., specify MinimumFlowWithBypass in the Controller:OutdoorAir object).
-
-During winter weather, humid exhaust air entering the heat exchanger can form frost on the cold heat exchanger surfaces, which can reduce air flow and the amount of energy recovery. Several methods are used to control or eliminate frost formation, and the following types can be modeled for this heat exchanger object: supply air preheat, minimum exhaust air temperature, exhaust air recirculation and exhaust only. For preheat frost control, a separate heating coil object must be placed in the supply inlet air stream to keep the air temperature above the frost threshold temperature. The other frost control types are modeled within this object itself (i.e., do not require a separate object to be defined) based on alpha and numeric inputs to this heat exchanger object.
-
-Air-to-air heat exchangers are sometimes controlled to maintain a fixed supply air outlet temperature to avoid overheating when the heat exchanger is heating the supply (primary) air. To model this control in EnergyPlus, a set point manager object is used to establish a temperature set point at the supply air outlet node of the heat exchanger. Wheel speed modulation or plate supply air bypass is used to control the supply air exiting conditions to this set point. The set point for supply air temperature control should be set at the minimum economizer temperature set point if an air-side economizer is also being used by the air system. If frost control and supply air outlet temperature control are used, frost control takes precedence over supply air temperature control (e.g., frost control defrost time fraction is determined as if wheel speed modulation or plate supply air bypass is not used).
-
-To model a sensible and latent air-to-air heat exchanger located in an air loop, the input data file should include the following objects:
-
-- AirLoopHVAC:OutdoorAirSystem
-
-- Controller:OutdoorAir
-
-- OutdoorAir:Mixer
-
-- HeatExchanger:AirToAir:SensibleAndLatent
-
-- Coil:Heating:Water, Coil:Heating:Electric or Coil:Heating:Gas (if preheat frost control is to be modeled)
-
-- SetpointManager:Scheduled (if supply air outlet temperature control is used)
-
-The sensible and latent air-to-air heat exchanger can also be used in a number of other applications, including conditioning outdoor ventilation air and supplying it directly to a zone without an air loop. See object ZoneHVAC:EnergyRecoveryVentilator for further details on this specific application.
-
-A description of each input field for this object is provided below.
-
-#### Field: Name
-
-A unique user-assigned name for a particular sensible/latent air-to-air heat exchanger. Any reference to this heat exchanger by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the unit can operate during a given time period. A schedule value of less than or equal to 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Nominal Supply Air Flow Rate
-
-The nominal primary side (supply) air flow rate in cubic meters per second. The actual supply and exhaust air flow rates must be between 50% and 130% of this value or a warning will be issued.
-
-#### Field: Sensible Effectiveness at 100% Heating Air Flow
-
-The sensible heat exchange effectiveness at the *heating* condition defined in Table 30 above with both the supply and exhaust air volume flow rates equal to 100% of the nominal supply air flow rate specified in the previous input field. The default value for this field is 0.
-
-#### Field: Latent Effectiveness at 100% Heating Air Flow
-
-The latent heat exchange effectiveness at the *heating* condition defined in Table 30 with both the supply and exhaust air volume flow rates equal to 100% of the nominal supply air flow rate. Specify this value as 0.0 if the heat exchanger does not transfer latent energy. The default value for this field is 0.
-
-#### Field: Sensible Effectiveness at 75% Heating Air Flow
-
-The sensible heat exchange effectiveness at the *heating* condition defined in Table 30 with both the supply and exhaust air volume flow rates equal to 75% of the nominal supply air flow rate. The default value for this field is 0.
-
-#### Field: Latent Effectiveness at 75% Heating Air Flow
-
-The latent heat exchange effectiveness at the *heating* condition defined in Table 30 with both the supply and exhaust air volume flow rates equal to 75% of the nominal supply air flow rate. Specify this value as 0.0 if the heat exchanger does not transfer latent energy. The default value for this field is 0.
-
-#### Field: Sensible Effectiveness at 100% Cooling Air Flow
-
-The sensible heat exchange effectiveness at the *cooling* condition defined in Table 30 with both the supply and exhaust air volume flow rates equal to 100% of the nominal supply air flow rate. The default value for this field is 0.
-
-#### Field: Latent Effectiveness at 100% Cooling Air Flow
-
-The latent heat exchange effectiveness at the *cooling* condition defined in Table 30 with both the supply and exhaust air volume flow rates equal to 100% of the nominal supply air flow rate. Specify this value as 0.0 if the heat exchanger does not transfer latent energy. The default value for this field is 0.
-
-#### Field: Sensible Effectiveness at 75% Cooling Air Flow
-
-The sensible heat exchange effectiveness at the *cooling* condition defined in Table 30 with both the supply and exhaust air volume flow rates equal to 75% of the nominal supply air flow rate. The default value for this field is 0.
-
-#### Field: Latent Effectiveness at 75% Cooling Air Flow
-
-The latent heat exchange effectiveness at the *cooling* condition defined in Table 30 with both the supply and exhaust air volume flow rates equal to 75% of the nominal supply air flow rate. Specify this value as 0.0 if the heat exchanger does not transfer latent energy. The default value for this field is 0.
-
-#### Field: Supply Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its supply (primary) inlet air.
-
-#### Field: Supply Air Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its supply (primary) outlet air.
-
-#### Field: Exhaust Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its exhaust (secondary) inlet air.
-
-#### Field: Exhaust Air Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its exhaust (secondary) outlet air.
-
-#### Field: Nominal Electric Power
-
-The electric consumption rate of the unit in watts. Electric power is considered constant whenever the unit operates. This numeric input can be used to model electric power consumption by controls (transformers, relays, etc.) and/or a motor for a rotary heat exchanger. None of this electric power contributes thermal load to the supply or exhaust air streams. The default value for this field is 0.
-
-#### Field: Supply Air Outlet Temperature Control
-
-This alpha field determines if the heat exchanger's supply air outlet is controlled to a temperature set point when the heat exchanger is actively conditioning the supply (primary) air. The choices for this input field are Yes or No, with the default being No. When supply air outlet temperature control is used, the wheel rotational speed modulates or supply air is bypassed around the plate heat exchanger to maintain the desired setpoint temperature. A setpoint manager object is required to establish the desired set point at the supply air outlet node (reference: SetpointManager:Scheduled). When an air-side economizer is also being modeled for this air system, the heat exchanger is deactivated during economizer operation. Additionally, the set point for the supply air outlet temperature control should be equal to the economizer outdoor air temperature lower limit (reference: Controller:OutdoorAir, field Economizer Minimum Limit Dry-Bulb Temperature), however, any temperature set point may be used.
-
-#### Field: Heat Exchanger Type
-
-This alpha field denotes the type of heat exchanger being modeled: Plate (e.g., fixed plate) or Rotary (e.g., rotating cylinder or wheel). The default choice for this field is    Plate   . The heat exchanger type affects the modeling of frost control options and supply air outlet temperature control. For rotary heat exchangers, rotational speed is varied to control frost formation or the supply air outlet temperature. For plate exchangers, air bypass around the heat exchanger is used to obtain the desired effect.
-
-#### Field: Frost Control Type
-
-This alpha field has four choices: None, ExhaustAirRecirculation, ExhaustOnly and MinimumExhaustTemperature. If this field is left blank, the default frost control type is    None   . For modeling preheat frost control, specify    None    for this input field and insert a separate heating coil object in the supply inlet air stream to keep the air temperature above the desired frost threshold temperature.
-
-*ExhaustAirRecirculation*: dampers are used to direct exhaust air back into the zone through the supply side of the heat exchanger when the supply (outdoor) air inlet temperature falls below a threshold temperature (defined in the next input field). The fraction of time that exhaust air is circulated through the supply side of the heat exchanger is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time fraction (see *Field: Rate of Defrost Time Fraction Increase*). When exhaust air is being recirculated, no supply (outdoor ventilation) air is being provided through the heat exchanger unit (which may or may not be acceptable regarding ventilation for occupants).
-
-*ExhaustOnly (supply air bypass)*: this control cycles off the supply air flow through the heat exchanger for a certain period of time while the exhaust air continues to flow through the exhaust side of the heat exchanger. The fraction of time that the supply flow through the heat exchanger is cycled off is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time fraction (see *Field: Rate of Defrost Time Fraction Increase*). When implemented in real applications, provisions are usually made to avoid building depressurization when this frost control is operating (automatic or pressure-operated dampers, or a bypass air damper around the supply side of the heat exchanger). For this frost control type, it is assumed that the supply air is bypassed around the heat exchanger during frost control operation (i.e., the total supply flow is not reduced during defrost, but merely bypassed around the heat exchanger).
-
-*MinimumExhaustTemperature*: the temperature of the exhaust air leaving the heat exchanger is monitored and the heat exchanger effectiveness is decreased (by slowing heat exchanger rotation or bypassing supply air around the plate exchanger) to keep the exhaust air from falling below the threshold temperature.
-
-#### Field: Threshold Temperature
-
-This numeric field defines the dry-bulb temperature of air which is used to initiate frost control. The default value is 1.7 &deg;C. For ExhaustAirRecirculation and ExhaustOnly frost control, the threshold temperature defines the supply (outdoor) air inlet temperature below which frost control is active. For MinimumExhaustTemperature frost control, heat exchanger effectiveness is controlled to keep the exhaust air outlet temperature from falling below this threshold temperature value.
-
-The appropriate threshold temperature varies with exhaust (inlet) air temperature and humidity, frost control type, heat exchanger type, and whether the heat exchanger transfers sensible energy alone or both sensible and latent energy (enthalpy). Typical threshold temperatures are provided in Table 31 below. However, it is recommended that the user consult manufacturer   s information for the specific air-to-air heat exchanger being modeled.
-
-Table 31. Typical threshold temperatures
-
-Frost control type
-
-Heat exchanger type
-
-Energy exchange
-
-Threshold temperature
-
-Exhaust air recirculation
-
-Plate
-
-Sensible-only
-
--1.1 &deg;C (30 &deg;F)
-
-Sensible + latent
-
--12.2 &deg;C (10 &deg;F)
-
-Rotary
-
-Sensible-only
-
--12.2 &deg;C (10 &deg;F)
-
-Sensible + latent
-
--23.3 &deg;C (-10 &deg;F)
-
-Exhaust only
-
-Plate
-
-Sensible-only
-
--1.1 &deg;C (30 &deg;F)
-
-Sensible + latent
-
--12.2 &deg;C (10 &deg;F)
-
-Rotary
-
-Sensible-only
-
--12.2 &deg;C (10 &deg;F)
-
-Sensible + latent
-
--23.3 &deg;C (-10 &deg;F)
-
-Minimum exhaust temperature
-
-Plate
-
-Sensible-only
-
-1.7 &deg;C (35 &deg;F)
-
-Sensible + latent
-
-1.7 &deg;C (35 &deg;F)
-
-Rotary
-
-Sensible-only
-
-1.7 &deg;C (35 &deg;F)
-
-Sensible + latent
-
-1.7 &deg;C (35 &deg;F)
-
-Preheat\*\*
-
-Plate
-
-Sensible-only
-
--1.1 &deg;C (30 &deg;F)
-
-Sensible + latent
-
--12.2 &deg;C (10 &deg;F)
-
-Rotary
-
-Sensible-only
-
--12.2 &deg;C (10 &deg;F)
-
-Sensible + latent
-
--23.3 &deg;C (-10 &deg;F)
-<table>
-  <tr>
-    <th>Frost Control Type</th>
-    <th>Heat Exchanger Type</th>
-    <th>Energy Exchange</th>
-    <th>Threshold Temperature</th>
-  </tr>
-  <tr>
-    <td rowspan="4">Exhaust Air Recirculation</td>
-    <td rowspan="2">Plate</td>
-    <td>Sensible-only</td>
-    <td>-1.1°C (30°F)</td>
-  </tr>
-  <tr>
-    <td>Sensible + latent</td>
-    <td>-12.2&deg;C (10&deg;F)</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Rotary</td>
-    <td>Sensible-only</td>
-    <td>-12.2&deg;C (10&deg;F)</td>
-  </tr>
-  <tr>
-    <td>Sensible + latent</td>
-    <td>-12.2&deg;C (10&deg;F)</td>
-  </tr>
-  <tr>
-    <td rowspan="4">Exhaust Only</td>
-    <td rowspan="2">Plate</td>
-    <td>Sensible-only</td>
-    <td>-23.3&deg;C (-10&deg;F)</td>
-  </tr>
-  <tr>
-    <td>Sensible + latent</td>
-    <td>-1.1&deg;C (30&deg;F)</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Rotary</td>
-    <td>Sensible-only</td>
-    <td>-12.2&deg;C (10&deg;F)</td>
-  </tr>
-  <tr>
-    <td>Sensible + latent</td>
-    <td>-12.2&deg;C (10&deg;F)</td>
-  </tr>
-  <tr>
-    <td rowspan="4">Minimum Exhaust Temperature</td>
-    <td rowspan="2">Plate</td>
-    <td>Sensible-only</td>
-    <td>-23.3&deg;C (-10&deg;F)</td>
-  </tr>
-  <tr>
-    <td>Sensible + latent</td>
-    <td>1.7&deg;C (35&deg;F)</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Rotary</td>
-    <td>Sensible-only</td>
-    <td>1.7&deg;C (35&deg;F)</td>
-  </tr>
-  <tr>
-    <td>Sensible + latent</td>
-    <td>1.7&deg;C (35&deg;F)</td>
-  </tr>
-  <tr>
-    <td rowspan="4">Preheat **</td>
-    <td rowspan="2">Plate</td>
-    <td>Sensible-only</td>
-    <td>1.7&deg;C (35&deg;F)</td>
-  </tr>
-  <tr>
-    <td>Sensible + latent</td>
-    <td>-1.1&deg;C (30&deg;F)</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Rotary</td>
-    <td>Sensible-only</td>
-    <td>-12.2&deg;C (10&deg;F)</td>
-  </tr>
-  <tr>
-    <td>Sensible + latent</td>
-    <td>-23.3&deg;C (-10&deg;F)</td>
-  </tr>
-</table>
-
-Source: Indoor Humidity Assessment Tool, U.S. Environmental Protection Agency,[http://www.epa.gov/iaq/schooldesign/saves.html](http://www.epa.gov/iaq/schooldesign/saves.html)
-
-\*\* To model preheat frost control, specify frost control type as None and place a heating coil in the supply inlet air stream controlled to the keep the air temperature above the frost threshold temperature.
-
-
-#### Field: Initial Defrost Time Fraction
-
-This numeric field defines the fraction of the simulation timestep when frost control will be invoked when the threshold temperature is reached. This field is only used for the ExhaustAirRecirculation and ExhaustOnly frost control types. The value for this field must be  &ge; 0 and  &le; 1. The default time fraction is 0.083 (e.g., 5 min / 60 min) which is typical for ExhaustAirRecirculation frost control. Higher initial defrost time fractions (e.g., 0.167 = 10 min / 60 min) are typically required for ExhaustOnly frost control. For best results, the user should obtain this information from the manufacturer.
-
-#### Field: Rate of Defrost Time Fraction Increase
-
-This numeric field defines the rate of increase in the defrost time fraction as the supply (outdoor) air inlet temperature falls below the threshold temperature. This field is only used for the ExhaustAirRecirculation and ExhaustOnly frost control types. The value for this field must be  &ge; 0. The default value is 0.012 (e.g., 0.72 min / 60 min per degree C temperature difference) which is typical for ExhaustAirRecirculation frost control. Higher values (e.g., 0.024 = 1.44 min / 60 min per degree C temperature difference) are typically required for ExhaustOnly frost control. For best results, the user should obtain this information from the manufacturer.
-
-This value is used to determine the total defrost time fraction as follows:
-
-Total defrost time fraction = Initial Defrost Time Fraction +
-
-           Rate of Defrost Time Fraction Increase \* (T<sub>threshold</sub>     T<sub>supply\\ air\\ inlet</sub>)
-
-The model does not allow the total defrost time fraction to exceed 1.0 or be less than 0.
-
-#### Field: Economizer Lockout
-
-This input denotes whether the heat exchanger unit is locked out (bypassed for plate type heat exchangers or the rotation is suspended for rotary type heat exchangers) when the air-side economizer is operating. Both the economizer and high humidity control (Ref. Controller:OutdoorAir) activate the heat exchanger lockout as specified by this input. The input choices are *Yes* (meaning locked out) or *No*. The default input for this field is Yes.
-
-Following is an example input for this heat exchanger object:
-
-```idf
-   HeatExchanger:AirToAir:SensibleAndLatent,
-       OA Heat Recovery 1,         !- Name
-       FanAndCoilAvailSched,       !- Availability Schedule Name
-       0.4333,                     !- Nominal Supply Air Flow Rate {m3/s}
-       .76,                        !- Sensible Effectiveness at 100% Heating Air Flow {dimensionless}
-       .68,                        !- Latent Effectiveness at 100% Heating Air Flow {dimensionless}
-       .81,                        !- Sensible Effectiveness at 75% Heating Air Flow {dimensionless}
-       .73,                        !- Latent Effectiveness at 75% Heating Air Flow {dimensionless}
-       .76,                        !- Sensible Effectiveness at 100% Cooling Air Flow {dimensionless}
-       .68,                        !- Latent Effectiveness at 100% Cooling Air Flow {dimensionless}
-       .81,                        !- Sensible Effectiveness at 75% Cooling Air Flow {dimensionless}
-       .73,                        !- Latent Effectiveness at 75% Cooling Air Flow {dimensionless}
-       Outside Air Inlet Node Preheated,   !- Supply Air Inlet Node Name
-       Heat Recovery Outlet Node,  !- Supply Air Outlet Node Name
-       Relief Air Outlet Node,     !- Exhaust Air Inlet Node Name
-       Heat Recovery Secondary Outlet Node,   !- Exhaust Air Outlet Node Name
-       200.0,                      !- Nominal Electric Power {W}
-       No,                         !- Supply Air Outlet Temperature Control
-       Plate,                      !- Heat Exchanger Type
-       None;                       !- Frost Control Type
-```
-
-### HeatExchanger:AirToAir:SensibleAndLatent Outputs
-
-* HVAC,Average,Heat Exchanger Sensible Heating Rate [W]
-
-* HVAC,Sum,Heat Exchanger Sensible Heating Energy [J]
-
-* HVAC,Average,Heat Exchanger Latent Gain Rate [W]
-
-* HVAC,Sum,Heat Exchanger Latent Gain Energy [J]
-
-* HVAC,Average,Heat Exchanger Total Heating Rate [W]
-
-* HVAC,Sum,Heat Exchanger Total Heating Energy [J]
-
-* HVAC,Average,Heat Exchanger Sensible Cooling Rate [W]
-
-* HVAC,Sum,Heat Exchanger Sensible Cooling Energy [J]
-
-* HVAC,Average,Heat Exchanger Latent Cooling Rate [W]
-
-* HVAC,Sum,Heat Exchanger Latent Cooling Energy [J]
-
-* HVAC,Average,Heat Exchanger Total Cooling Rate [W]
-
-* HVAC,Sum,Heat Exchanger Total Cooling Energy [J]
-
-* HVAC,Average,Heat Exchanger Electric Power[W]
-
-* HVAC,Sum,Heat Exchanger Electric Energy [J]
-
-* HVAC,Average,Heat Exchanger Sensible Effectiveness[]
-
-* HVAC,Average,Heat Exchanger Latent Effectiveness[]
-
-* HVAC,Average,Heat Exchanger Supply Air Bypass Mass Flow Rate [kg/s]
-
-* HVAC,Average,Heat Exchanger Exhaust Air Bypass Mass Flow Rate [kg/s] HVAC,Average,Heat Exchanger Defrost Time Fraction[]
-
-#### Heat Exchanger Sensible Heating Rate [W]
-
-This output is the sensible heating rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, the supply air inlet and outlet conditions, and the specific heat of the inlet supply air. A positive value is reported if the supply air is heated by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Sensible Heating Energy [J]
-
-This output is the sensible heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Latent Gain Rate [W]
-
-This output is the latent heating rate (humidification) of the supply air by the heat exchanger in Watts. This rate is determined by taking the difference between the Heat Exchanger Total Heating Rate and the Heat Exchanger Sensible Heating Rate. A positive value is reported if the supply air is humidified by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Latent Gain Energy [J]
-
-This output is the latent heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Total Heating Rate [W]
-
-This output is the total heating rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, and the enthalpy of the supply air entering and leaving the unit. A positive value is reported if the enthalpy of the supply air is increased by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Total Heating Energy [J]
-
-This output is the total heating energy added to the supply air by the heat exchanger in Joules over the timestep being reported.This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforHeating, GroupKey = System (ref. Output:Meter objects).
-
-#### Heat Exchanger Sensible Cooling Rate [W]
-
-This output is the sensible cooling rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, the supply air inlet and outlet conditions, and the specific heat of the inlet supply air. A positive value is reported if the supply air is cooled by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Sensible Cooling Energy [J]
-
-This output is the sensible cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Latent Cooling Rate [W]
-
-This output is the latent cooling rate (dehumidification) of the supply air by the heat exchanger in Watts. This rate is determined by taking the difference between the Heat Exchanger Total Cooling Rate and the Heat Exchanger Sensible Cooling Rate. A positive value is reported if the supply air is dehumidified by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Latent   Cooling Energy [J]
-
-This output is the latent cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Total Cooling Rate [W]
-
-This output is the total cooling rate of the supply air by the heat exchanger in Watts. This rate is determined using the supply air mass flow rate through the heat exchanger unit, and the enthalpy of the supply air entering and leaving the unit. A positive value is reported if the enthalpy of the supply air is decreased by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Total Cooling Energy [J]
-
-This output is the total cooling energy added to the supply air by the heat exchanger in Joules over the timestep being reported. This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforCooling, GroupKey = System (ref. Output:Meter objects).
-
-#### Heat Exchanger Electric Power [W]
-
-This output is the electric consumption rate of the unit in Watts. This rate is applicable whenever the unit operates (i.e., whenever the unit is scheduled to be available and supply and exhaust air flows exist).
-
-#### Heat Exchanger Electric Energy [J]
-
-This output is the electric consumption of the unit in Joules for the timestep being reported. This ouput is also added to a meter with ResourceType = Electricity, EndUseKey = HeatRecovery, GroupKey = System (ref. Output:Meter objects).
-
-#### Heat Exchanger Sensible Effectiveness []
-
-This output is the average sensible effectiveness of the heat exchanger (excluding bypass air, if any) over the timestep being reported.
-
-#### Heat Exchanger Latent Effectiveness []
-
-This output is the average latent effectiveness of the heat exchanger (excluding bypass air, if any) over the timestep being reported.
-
-#### Heat Exchanger Supply Air Bypass Mass Flow Rate [kg/s]
-
-This output is the average mass flow rate in kg/second of the supply (primary) air stream that is bypassing the heat exchanger over the timestep being reported. This flow rate is equal to the total supply mass flow rate through the heat exchanger **unit** minus the amount passing through the supply side of the heat exchanger **core**.
-
-#### Heat Exchanger Exhaust Air Bypass Mass Flow Rate [kg/s]
-
-This output is the average mass flow rate in kg/second of the exhaust (secondary) air stream that is bypassing the heat exchanger over the timestep being reported. This flow rate is equal to the total exhaust mass flow rate through the heat exchanger **unit** minus the amount passing through the exhaust side of the heat exchanger **core**.
-
-#### Heat Exchanger Defrost Time Fraction []
-
-This output is the average fraction of the reporting timestep when frost control is being implemented.
-
-### HeatExchanger:Desiccant:BalancedFlow
-
-This desiccant heat exchanger object is an HVAC component used to model both temperature (sensible) and moisture (latent) heat exchange between two air streams (Figure 151). The model assumes balanced air flow through the regeneration and process sides of the heat exchanger (i.e., regeneration and process air volume flow rates and face velocities are the same). Heat exchanger performance is specified through a performance data type object (e.g., HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1).
-
-![BalancedFlowDesiccantHeatExchanger\_Schematic](media/image424.png)
-
-Figure 151. Schematic of the Balanced Flow Desiccant Heat Exchanger
-
-Currently, this desiccant heat exchanger model can be referenced by two compound objects: CoilSystem:Cooling:DX:HeatExchangerAssisted and Dehumidifier:Desiccant:System, both of which are used to provide enhanced dehumidification over conventional systems. If this heat exchanger is referenced by a compound object, the compound object will control heat exchanger operation (i.e., tell the heat exchanger if heat exchange is needed or not for each simulation timestep).
-
-This desiccant heat exchanger object may also be specified directly in an AirLoopHVAC (air loop BranchList) or in an AirLoopHVAC:OutdoorAirSystem (AirLoopHVAC:OutdoorAirSystem:EquipmentList) without being referenced by a compound object. If specified directly in an AirLoopHVAC or AirLoopHVAC:OutdoorAirSystem, then the heat exchanger can be controlled to provide heat exchange based on a maximum and/or minimum humidity set point placed on the process air outlet node (ref. Setpoint Managers). If no humidity set points are provided on this node, then heat exchange will be provided whenever the heat exchanger is available to operate (via its availability schedule) and there is a temperature and/or humidity ratio difference between the two air streams.
-
-Inputs to this model include an availability schedule name, inlet and outlet air node names, and the type and name of the heat exchanger performance data object. A description of each input field for this object is provided below.
-
-#### Field: Name
-
-A unique, user-assigned name for a particular balanced flow desiccant heat exchanger. Any reference to this heat exchanger by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the heat exchanger can operate during a given time period. A schedule value of less than or equal to 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Regeneration Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its regeneration inlet air.
-
-#### Field: Regeneration Air Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its regeneration outlet air.
-
-#### Field: Process Air Inlet Node Name
-
-The name of the HVAC system node from which the unit draws its process inlet air.
-
-#### Field: Process Air Outlet Node Name
-
-The name of the HVAC system node to which the unit sends its process outlet air.
-
-#### Field: Heat Exchanger Performance Object Type
-
-This alpha field contains the type of model used to simulate the desiccant heat exchanger   s thermal performance and electrical energy use. Currently, the only valid choice is HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1.
-
-#### Field: Heat Exchanger Performance Name
-
-This alpha field contains the identifying name of the specific heat exchanger performance type object (e.g., HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1) that defines the performance for this heat exchanger. A single heat exchanger performance type object may be used to define performance for many HeatExchanger:Desiccant:BalancedFlow objects (i.e., the same name may be used in this input field for more than one balanced flow desiccant heat exchanger).
-
-#### Field: Economizer Lockout
-
-This input denotes whether the heat exchanger unit is locked out (heat exchanger rotation is suspended) when the air-side economizer is operating. Both the economizer and high humidity control (Ref. Controller:OutdoorAir) activate the heat exchanger lockout as specified by this input. The input choices are *Yes* (meaning locked out) or *No*. Economizer lockout is typically *not* used for this type of heat exchanger. For this reason, the default input for this field is No.
-
-Following is an example input for this heat exchanger object:
-
-```idf
-HeatExchanger:Desiccant:BalancedFlow,
-  Desiccant Heat Exchanger 1,                 !- Name
-  OfficeHeatCoolAvail,                               !- Availability Schedule Name
-  DXSystem 1 Mixed Air Node,                   !- Regeneration Air Inlet Node Name
-  DX Cooling Coil Air Inlet Node,         !- Regeneration Air Outlet Node Name
-  DX Cooling Coil Air Outlet Node,       !- Process Air Inlet Node Name
-  DXSystem 1 Fan Air Inlet Node,           !- Process Air Outlet Node Name
-  HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1, !- Heat Exchanger Performance Object Type
-  HXDesPerf1;                                                 !- Heat Exchanger Performance Name
-```
-
-### HeatExchanger:Desiccant:BalancedFlow Outputs
-
-* HVAC,Average,Heat Exchanger Sensible Heating Rate [W]
-
-* HVAC,Sum,Heat Exchanger Sensible Heating Energy [J]
-
-* HVAC,Average,Heat Exchanger Latent Gain Rate [W]
-
-* HVAC,Sum,Heat Exchanger Latent Gain Energy [J]
-
-* HVAC,Average,Heat Exchanger Total Heating Rate [W]
-
-* HVAC,Sum,Heat Exchanger Total Heating Energy [J]
-
-* HVAC,Average,Heat Exchanger Sensible Cooling Rate [W]
-
-* HVAC,Sum,Heat Exchanger Sensible Cooling Energy [J]
-
-* HVAC,Average,Heat Exchanger Latent Cooling Rate [W]
-
-* HVAC,Sum,Heat Exchanger Latent Cooling Energy [J]
-
-* HVAC,Average,Heat Exchanger Total Cooling Rate [W]
-
-* HVAC,Sum,Heat Exchanger Total Cooling Energy [J]
-
-* HVAC,Average,Heat Exchanger Electric Power[W]
-
-* HVAC,Sum,Heat Exchanger Electric Energy [J]
-
-
-
-#### Heat Exchanger Sensible Heating Rate [W]
-
-This output is the sensible heating rate of the process air by the heat exchanger in Watts. This rate is determined using the process air mass flow rate through the heat exchanger unit, the process air inlet and outlet temperatures, and the specific heat of the inlet process air. A positive value is reported if the process air is heated by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Sensible Heating Energy [J]
-
-This output is the sensible heating energy added to the process air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Latent Gain Rate [W]
-
-This output is the latent heating rate (humidification) of the process air by the heat exchanger in Watts. This rate is determined by taking the difference between the heat exchanger   s total heat recovery rate and the sensible heat recovery rate. A positive value is reported if the process air is humidified by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Latent Gain Energy [J]
-
-This output is the latent heating energy added to the process air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Total Heating Rate [W]
-
-This output is the total heating rate of the process air by the heat exchanger in Watts. This rate is determined using the process air mass flow rate through the heat exchanger unit and the enthalpy of the air entering and leaving the process side of the unit. A positive value is reported if the enthalpy of the process air is increased by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Total Heating Energy [J]
-
-This output is the total heating energy added to the process air by the heat exchanger in Joules over the timestep being reported.This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforHeating, GroupKey = System (ref. Output:Meter objects).
-
-#### Heat Exchanger Sensible Cooling Rate [W]
-
-This output is the sensible cooling rate of the process air by the heat exchanger in Watts. This rate is determined using the process air mass flow rate through the heat exchanger unit, the process air inlet and outlet temperatures, and the specific heat of the inlet process air. A positive value is reported if the process air is cooled by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Sensible Cooling Energy [J]
-
-This output is the sensible cooling energy added to the process air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Latent Cooling Rate [W]
-
-This output is the latent cooling rate (dehumidification) of the process air by the heat exchanger in Watts. This rate is determined by taking the difference between the heat exchanger   s total heat recovery rate and the sensible heat recovery rate. A positive value is reported if the process air is dehumidified by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Latent Cooling Energy [J]
-
-This output is the latent cooling energy added to the process air by the heat exchanger in Joules over the timestep being reported.
-
-#### Heat Exchanger Total Cooling Rate [W]
-
-This output is the total cooling rate of the process air by the heat exchanger in Watts. This rate is determined using the process air mass flow rate through the heat exchanger unit and the enthalpy of the air entering and leaving the process side of the unit. A positive value is reported if the enthalpy of the process air is decreased by the heat exchanger, else the rate is set to zero.
-
-#### Heat Exchanger Total Cooling Energy [J]
-
-This output is the total cooling energy added to the process air by the heat exchanger in Joules over the timestep being reported. This output is also added to a meter with ResouceType = EnergyTransfer, EndUseKey = HeatRecoveryforCooling, GroupKey = System (ref. Output:Meter objects).
-
-#### Heat Exchanger Electric Power [W]
-
-This output is the average electric consumption rate of the unit in Watts. This average rate includes portions of the simulation timestep when the heat exchanger may be cycled off (i.e., average of on and off periods, as appropriate).
-
-#### Heat Exchanger Electric Energy [J]
-
-This output is the electric consumption of the unit in Joules for the timestep being reported. This ouput is also added to a meter with ResourceType = Electricity, EndUseKey = HeatRecovery, GroupKey = System (ref. Output:Meter objects).
-
-### HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1
-
-This object specifies a performance model and model coefficients for a balanced flow desiccant heat exchanger. A HeatExchanger:Desiccant:BalancedFlow object will reference a HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 object. This performance data object is used to specify the thermal performance and electric consumption of the heat exchanger. Some representative inputs for this object are provided in the EnergyPlus Reference DataSets (PerfCurves.idf and AllDataSets.idf).
-
-This model predicts the regeneration air stream outlet temperature and humidity ratio values based on the entering regeneration and process air stream temperature, humidity ratio and face velocity. The process air stream outlet humidity ratio and temperatures are calculated based on a simple heat and moisture balance. The model requires that the user enter the nominal volumetric flow rate and a nominal face velocity, electric power consumption, empirical model coefficients for the regeneration outlet air temperature and humidity ratio equations, and the applicable minimum and maximum values for both the independent and dependent variables for the empirical model coefficients provided. This model is based on the following equations:
-
-- The dry-bulb temperature of the regeneration outlet air is defined using the following equation:
-
-<div>\[RTO = B1 + B2*RWI + B3*RTI + B4*\left( {\frac{{RWI}}{{RTI}}} \right) + B5*PWI + B6*PTI + B7*\left( {\frac{{PWI}}{{PTI}}} \right) + B8*RFV\]</div>
-
-where,
-
-<span>\(RTO\)</span>  = Regeneration outlet air dry-bulb temperature (C)
-
-<span>\(RWI\)</span>  = Regeneration inlet air humidity ratio (kgWater/kgDryAir)
-
-<span>\(RTI\)</span>    = Regeneration inlet air dry-bulb temperature (C)
-
-<span>\(PWI\)</span>  = Process inlet air humidity ratio (kgWater/kgDryAir)
-
-<span>\(PTI\)</span>   = Process inlet air dry-bulb temperature (C)
-
-<span>\(RFV\)</span>  = Regeneration (and process) face velocity (m/s)
-
-- The humidity ratio of the regeneration outlet air is defined using the same empirical equation form; however, different coefficients are used as follows:
-
-<div>\[RWO = C1 + C2*RWI + C3*RTI + C4*\left( {\frac{{RWI}}{{RTI}}} \right) + C5*PWI + C6*PTI + C7*\left( {\frac{{PWI}}{{PTI}}} \right) + C8*RFV\]</div>
-
-where,
-
-<span>\(RWO\)</span>  = Regeneration outlet air humidity ratio (kgWater/kgDryAir)
-
-- The process outlet air conditions are then calculated based on the regeneration outlet air conditions (temperature or humidity ratio) calculated above, the actual regeneration inlet air conditions entering the heat exchanger, and assuming the same amount of sensible and total energy transfer across both the process and regeneration sides of the heat exchanger. The difference between the actual inlet air conditions and RTI/RWI/PTI/PWI is made here because user-defined limits for RTI/RWI/PTI/PWI may result in a difference between the actual conditions and those used in the equations shown above (see the EnergyPlus Engineering Reference for further discussion).
-
-
-
-A description of each input field for this object is provided below.
-
-#### Field: Name
-
-This alpha field contains the identifying name for this set of desiccant heat exchanger performance data. Any reference to this performance data set by another object (e.g., HeatExchanger:Desiccant:BalancedFlow) will use this name.
-
-#### Field: Nominal Air Flow Rate
-
-The nominal air volume flow rate in cubic meters per second. This model assumes balanced air flow (i.e., the same air volume flow rate across the process and regeneration sides of the heat exchanger). The minimum value should be greater than 0. This field is autosizable.
-
-#### Field: Nominal Air Face Velocity
-
-This numeric field contains the nominal air velocity across the heat exchanger face area in meters per second. It is assumed that this air velocity is the same for both sides of the heat exchanger. This value, along with the Nominal Air Flow Rate sets the heat exchanger face area. With this fixed face area, the air face velocity is calculated every simulation timestep based on the actual air volume flow rate for the timestep. The minimum value should be greater than 0 and less than or equal to 6. The default value is 3.0.
-
-#### Field: Nominal Electric Power
-
-This numeric field contains the nominal electric consumption rate of the heat exchanger in watts. This electric power is considered constant and is consumed only when the heat exchanger operates (e.g., for all or a portion of the simulation timestep, as appropriate). This numeric input can be used to model electric power consumption by controls (transformers, relays, etc.) and/or a motor for a rotary heat exchanger. None of this electric power contributes thermal load to the process or regeneration air streams. The minimum value should be greater than or equal to 0. The default value for this field is also 0.
-
-The coefficients for the regeneration air outlet temperature equation described above are defined in the following eight fields:
-
-#### Field: Temperature Equation Coefficient 1
-
-The constant coefficient (B<sub>1</sub>) in the temperature equation shown above (RTO).
-
-#### Field: Temperature Equation Coefficient 2
-
-The coefficient (B<sub>2</sub>) in the temperature equation shown above (RTO).
-
-#### Field: Temperature Equation Coefficient 3
-
-The coefficient (B<sub>3</sub>) in the temperature equation shown above (RTO).
-
-#### Field: Temperature Equation Coefficient 4
-
-The coefficient (B<sub>4</sub>) in the temperature equation shown above (RTO).
-
-#### Field: Temperature Equation Coefficient 5
-
-The coefficient (B<sub>5</sub>) in the temperature equation shown above (RTO).
-
-#### Field: Temperature Equation Coefficient 6
-
-The coefficient (B<sub>6</sub>) in the temperature equation shown above (RTO).
-
-#### Field: Temperature Equation Coefficient 7
-
-The coefficient (B<sub>7</sub>) in the temperature equation shown above (RTO).
-
-#### Field: Temperature Equation Coefficient 8
-
-The coefficient (B<sub>8</sub>) in the temperature equation shown above (RTO).
-
-The following 16 fields are used to establish the valid range for the dependent and independent variables associated with the coefficients defined above (B<sub>1</sub> through B<sub>8</sub>) for the regeneration outlet air temperature equation.
-
-#### Field: Minimum Regeneration Inlet Air Humidity Ratio for Temperature Equation
-
-The minimum allowable value of RWI in the temperature equation shown above (kgWater/kgDryAir). Values of RWI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air temperature and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
-
-#### Field: Maximum Regeneration Inlet Air Humidity Ratio for Temperature Equation
-
-The maximum allowable value of RWI in the temperature equation shown above (kgWater/kgDryAir). Values of RWI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air temperature and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
-
-#### Field: Minimum Regeneration Inlet Air Temperature for Temperature Equation
-
-The minimum allowable value of RTI in the temperature equation shown above (C). Values of RTI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air temperature and a warning message will be issued.
-
-#### Field: Maximum Regeneration Inlet Air Temperature for Temperature Equation
-
-The maximum allowable value of RTI in the temperature equation shown above (C). Values of RTI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air temperature and a warning message will be issued.
-
-#### Field: Minimum Process Inlet Air Humidity Ratio for Temperature Equation
-
-The minimum allowable value of PWI in the temperature equation shown above (kg/kg). Values of PWI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air temperature and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
-
-#### Field: Maximum Process Inlet Air Humidity Ratio for Temperature Equation
-
-The maximum allowable value of PWI in the temperature equation shown above (kg/kg). Values of PWI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air temperature and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
-
-#### Field: Minimum Process Inlet Air Temperature for Temperature Equation
-
-The minimum allowable value of PTI in the temperature equation shown above (C). Values of PTI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air temperature and a warning message will be issued.
-
-#### Field: Maximum Process Inlet Air Temperature for Temperature Equation
-
-The maximum allowable value of PTI in the temperature equation shown above (C). Values of PTI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air temperature and a warning message will be issued.
-
-#### Field: Minimum Regeneration Air Velocity for Temperature Equation
-
-The minimum allowable value of RFV in the temperature equation shown above (m/s). Values of RFV less than the minimum will be replaced by this minimum when calculating the regeneration outlet air temperature and a warning message will be issued. The minimum value for this input field should be greater than 0.
-
-#### Field: Maximum Regeneration Air Velocity for Temperature Equation
-
-The maximum allowable value of RFV in the temperature equation shown above (m/s). Values of RFV greater than the maximum will be replaced by this maximum value when calculating the regeneration outlet air temperature and a warning message will be issued. The minimum value for this input field should be greater than 0.
-
-#### Field: Minimum Regeneration Outlet Air Temperature for Temperature Equation
-
-The minimum value of RTO resulting from the temperature equation shown above (C). If RTO is less than this value, RTO will be replaced by this minimum value and a warning message will be issued.
-
-#### Field: Maximum Regeneration Outlet Air Temperature for Temperature Equation
-
-The maximum value of RTO resulting from the temperature equation shown above (C). If RTO is greater than this value, RTO will be replaced by this maximum value and a warning message will be issued.
-
-#### Field: Minimum Regeneration Inlet Air Relative Humidity for Temperature Equation
-
-The minimum relative humidity of the regeneration inlet air for the temperature equation shown above (percent). If the relative humidity of the regeneration inlet air is below this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
-
-#### Field: Maximum Regeneration Inlet Air Relative Humidity for Temperature Equation
-
-The maximum relative humidity of the regeneration inlet air for the temperature equation shown above (percent). If the relative humidity of the regeneration inlet air is above this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
-
-#### Field: Minimum Process Inlet Air Relative Humidity for Temperature Equation
-
-The minimum relative humidity of the process inlet air for the temperature equation shown above (percent). If the relative humidity of the process inlet air is below this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
-
-#### Field: Maximum Process Inlet Air Relative Humidity for Temperature Equation
-
-The maximum relative humidity of the process inlet air for the temperature equation shown above (percent). If the relative humidity of the process inlet air is above this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
-
-The coefficients for the regeneration outlet air humidity ratio equation are defined in the following eight fields:
-
-#### Field: Humidity Ratio Equation Coefficient 1
-
-The constant coefficient (C<sub>1</sub>) in the humidity ratio equation shown above (RWO).
-
-#### Field: Humidity Ratio Equation Coefficient 2
-
-The coefficient (C<sub>2</sub>) in the humidity ratio equation shown above (RWO).
-
-#### Field: Humidity Ratio Equation Coefficient 3
-
-The coefficient (C<sub>3</sub>) in the humidity ratio equation shown above (RWO).
-
-#### Field: Humidity Ratio Equation Coefficient 4
-
-The coefficient (C<sub>4</sub>) in the humidity ratio equation shown above (RWO).
-
-#### Field: Humidity Ratio Equation Coefficient 5
-
-The coefficient (C<sub>5</sub>) in the humidity ratio equation shown above (RWO).
-
-#### Field: Humidity Ratio Equation Coefficient 6
-
-The coefficient (C<sub>6</sub>) in the humidity ratio equation shown above (RWO).
-
-#### Field: Humidity Ratio Equation Coefficient 7
-
-The coefficient (C<sub>7</sub>) in the humidity ratio equation shown above (RWO).
-
-#### Field: Humidity Ratio Equation Coefficient 8
-
-The coefficient (C<sub>8</sub>) in the humidity ratio equation shown above (RWO).
-
-
-
-The following 16 fields are used to establish the valid range for the dependent and independent variables associated with the coefficients defined above (C<sub>1</sub> through C<sub>8</sub>) for the regeneration outlet air humidity ratio equation.
-
-#### Field: Minimum Regeneration Inlet Air Humidity Ratio for Humidity Ratio Equation
-
-The minimum allowable value of RWI in the humidity ratio equation shown above (kgWater/kgDryAir). Values of RWI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
-
-#### Field: Maximum Regeneration Inlet Air Humidity Ratio for Humidity Ratio Equation
-
-The maximum allowable value of RWI in the humidity ratio equation shown above (kgWater/kgDryAir). Values of RWI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
-
-#### Field: Minimum Regeneration Inlet Air Temperature for Humidity Ratio Equation
-
-The minimum allowable value of RTI in the humidity ratio equation shown above (C). Values of RTI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air humidity ratio and a warning message will be issued.
-
-#### Field: Maximum Regeneration Inlet Air Temperature for Humidity Ratio Equation
-
-The maximum allowable value of RTI in the humidity ratio equation shown above (C). Values of RTI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air humidity ratio and a warning message will be issued.
-
-#### Field: Minimum Process Inlet Air Humidity Ratio for Humidity Ratio Equation
-
-The minimum allowable value of PWI in the humidity ratio equation shown above (kgWater/kgDryAir). Values of PWI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
-
-#### Field: Maximum Process Inlet Air Humidity Ratio for Humidity Ratio Equation
-
-The maximum allowable value of PWI in the humidity ratio equation shown above (kgWater/kgDryAir). Values of PWI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
-
-#### Field: Minimum Process Inlet Air Temperature for Humidity Ratio Equation
-
-The minimum allowable value of PTI in the humidity ratio equation shown above (C). Values of PTI less than the minimum will be replaced by this minimum when calculating the regeneration outlet air humidity ratio and a warning message will be issued.
-
-#### Field: Maximum Process Inlet Air Temperature for Humidity Ratio Equation
-
-The maximum allowable value of PTI in the humidity ratio equation shown above (C). Values of PTI greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air humidity ratio and a warning message will be issued.
-
-#### Field: Minimum Regeneration Air Velocity for Humidity Ratio Equation
-
-The minimum allowable value of RFV in the humidity ratio equation shown above (m/s). Values of RFV less than the minimum will be replaced by this minimum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The minimum value for this input field should be greater than 0.
-
-#### Field: Maximum Regeneration Air Velocity for Humidity Ratio Equation
-
-The maximum allowable value of RFV in the humidity ratio equation shown above (m/s). Values of RFV greater than the maximum will be replaced by this maximum when calculating the regeneration outlet air humidity ratio and a warning message will be issued. The minimum value for this input field should be greater than 0.
-
-#### Field: Minimum Regeneration Outlet Air Humidity Ratio for Humidity Ratio Equation
-
-The minimum value of RWO resulting from the humidity ratio equation shown above (kgWater/kgDryAir). If RWO is less than this value, RWO will be replaced by this minimum value and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
-
-#### Field: Maximum Regeneration Outlet Air Humidity Ratio for Humidity Ratio Equation
-
-The maximum value of RWO resulting from the humidity ratio equation shown above (kgWater/kgDryAir). If RWO is greater than this value, RWO will be replaced by this maximum value and a warning message will be issued. The valid range for this input field is 0.0 to 1.0.
-
-#### Field: Minimum Regeneration Inlet Air Relative Humidity for Humidity Ratio Equation
-
-The minimum relative humidity of the regeneration inlet air for the humidity ratio equation shown above (percent). If the relative humidity of the regeneration inlet air is below this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
-
-#### Field: Maximum Regeneration Inlet Air Relative Humidity for Humidity Ratio Equation
-
-The maximum relative humidity of the regeneration inlet air for the humidity ratio equation shown above (percent). If the relative humidity of the regeneration inlet air is above this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
-
-#### Field: Minimum Process Inlet Air Relative Humidity for Humidity Ratio Equation
-
-The minimum relative humidity of the process inlet air for the humidity ratio equation shown above (percent). If the relative humidity of the process inlet air is below this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
-
-#### Field: Maximum Process Inlet Air Relative Humidity for Humidity Ratio Equation
-
-The maximum relative humidity of the process inlet air for the humidity ratio equation shown above (percent). If the relative humidity of the process inlet air is above this value, a warning message will be issued. The valid range for this input field is 0.0 to 100.0.
-
-Following is an example input for this heat exchanger performance data type object:
-
-```idf
-   HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1,
-       HXDesPerf1,         !- Name
-       1.05,                     !- Nominal Air Flow Rate {m3/s}
-       3.25,                     !- Nominal Air Face Velocity {m/s}
-       50.0,                     !- Nominal Electric Power {W}
-       -2.53636E+00,     !- Temperature Equation Coefficient 1
-       2.13247E+01,       !- Temperature Equation Coefficient 2
-       9.23308E-01,       !- Temperature Equation Coefficient 3
-       9.43276E+02,       !- Temperature Equation Coefficient 4
-       -5.92367E+01,     !- Temperature Equation Coefficient 5
-       -4.27465E-02,     !- Temperature Equation Coefficient 6
-       1.12204E+02,       !- Temperature Equation Coefficient 7
-       7.78252E-01,       !- Temperature Equation Coefficient 8
-
-
-       0.007143,             !- Minimum Regeneration Inlet Air Humidity Ratio for Temperature Equation
-       0.024286,             !- Maximum Regeneration Inlet Air Humidity Ratio for Temperature Equation
-       46.111110,           !- Minimum Regeneration Inlet Air Temperature for Temperature Equation {C}
-       46.111112,           !- Maximum Regeneration Inlet Air Temperature for Temperature Equation {C}
-       0.005000,             !- Minimum Process Inlet Air Humidity Ratio for Temperature Equation
-       0.015714,             !- Maximum Process Inlet Air Humidity Ratio for Temperature Equation
-       4.583333,             !- Minimum Process Inlet Air Temperature for Temperature Equation {C}
-       21.83333,             !- Maximum Process Inlet Air Temperature for Temperature Equation {C}
-       2.286,                   !- Minimum Regeneration Air Velocity for Temperature Equation {m/s}
-       4.826,                   !- Maximum Regeneration Air Velocity for Temperature Equation {m/s}
-       35.0,                     !- Minimum Regeneration Outlet Air Temperature for Temperature Equation {C}
-       50.0,                     !- Maximum Regeneration Outlet Air Temperature for Temperature Equation {C}
-       5.0,                       !- Minimum Regeneration Inlet Air Relative Humidity for Temperature Equation {percent}
-       45.0,                     !- Maximum Regeneration Inlet Air Relative Humidity for Temperature Equation {percent}
-       80.0,                     !- Minimum Process Inlet Air Relative Humidity for Temperature Equation {percent}
-       100.0,                   !- Maximum Process Inlet Air Relative Humidity for Temperature Equation {percent}
-       -2.25547E+01,     !- Humidity Ratio Equation Coefficient 1
-       9.76839E-01,       !- Humidity Ratio Equation Coefficient 2
-       4.89176E-01,       !- Humidity Ratio Equation Coefficient 3
-       -6.30019E-02,     !- Humidity Ratio Equation Coefficient 4
-       1.20773E-02,       !- Humidity Ratio Equation Coefficient 5
-       5.17134E-05,       !- Humidity Ratio Equation Coefficient 6
-       4.94917E-02,       !- Humidity Ratio Equation Coefficient 7
-       -2.59417E-04,     !- Humidity Ratio Equation Coefficient 8
-       0.007143,             !- Minimum Regeneration Inlet Air Humidity Ratio for Humidity Ratio Equation
-       0.024286,             !- Maximum Regeneration Inlet Air Humidity Ratio for Humidity Ratio Equation
-       46.111110,           !- Minimum Regeneration Inlet Air Temperature for Humidity Ratio Equation {C}
-       46.111112,           !- Maximum Regeneration Inlet Air Temperature for Humidity Ratio Equation {C}
-       0.005000,             !- Minimum Process Inlet Air Humidity Ratio for Humidity Ratio Equation
-       0.015714,             !- Maximum Process Inlet Air Humidity Ratio for Humidity Ratio Equation
-       4.583333,             !- Minimum Process Inlet Air Temperature for Humidity Ratio Equation {C}
-       21.83333,             !- Maximum Process Inlet Air Temperature for Humidity Ratio Equation {C}
-       2.286,                   !- Minimum Regeneration Air Velocity for Humidity Ratio Equation {m/s}
-       4.826,                   !- Maximum Regeneration Air Velocity for Humidity Ratio Equation {m/s}
-       0.007914,             !- Minimum Regeneration Outlet Air Humidity Ratio for Humidity Ratio Equation
-       0.026279,             !- Maximum Regeneration Outlet Air Humidity Ratio for Humidity Ratio Equation
-       5.0,                 !- Minimum Regeneration Inlet Air Relative Humidity for Humidity Ratio Equation {%}
-       45.0,               !- Maximum Regeneration Inlet Air Relative Humidity for Humidity Ratio Equation {percent}
-       80.0,                   !- Minimum Process Inlet Air Relative Humidity for Humidity Ratio Equation {percent}
-       100.0;                 !- Maximum Process Inlet Air Relative Humidity for Humidity Ratio Equation {percent}
-```
-
-### HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 Outputs
-
-No variables are reported for this object. However, outputs are provided by the HeatExchanger:Desiccant:BalancedFlow object that references this PerformanceDataType1 object.
-
-Group     Demand Limiting Controls
---------------------------------
-
-Demand limiting, or demand management, is a strategy for reducing a building's demand for utilities, e.g., electricity. Utility companies typically charge a monthly fee for "demand charges" that is based on the peak demand during a certain time period. Often the peak demand charge is set by one exceptional day that is much higher than the peak demand for an average day during the month. Therefore, to save utility costs, it is in the interest of building owners to find ways to manage the demand on peak days. While demand management is generally concerned with the demand for electricity, the future will likely see demand management of other utilities, such as natural gas or water.
-
-Demand limiting controls shut off or reduce the power to non-essential loads in order to reduce the overall building demand. Some typical controls:
-
-- shut off or dim electric lights, equipment, or HVAC systems
-
-- reset the thermostatic set points on HVAC systems
-
-- reduce the load of a set of similar components by rotating one or more components "off" for a short time interval
-
-- turn on generators to meet some or all of the building's demand.
-
-The demand limiting controls implemented in EnergyPlus are intended to allow some of the more common demand limiting strategies. Currently, only Exterior:Lights, Lights, ElectricEquipment, ZoneControl:Thermostat, and Controller:OutdoorAir objects can be demand limited. Additional components will be demand limited in future releases.
-
-### DemandManagerAssignmentList
-
-The DemandManagerAssignmentList object is a high level control that makes demand limiting decisions based on a list of possible demand limiting strategies. Each demand limiting strategy is described in a separate DemandManager object. (This is structured like the relationship between the AvailabilityManagerAssignmentList and the AvailabilityManager   objects.)
-
-Each DemandManagerAssignmentList monitors and demand limits one meter. Only electricity meters are currently allowed. In many cases, the meter will be *Electricity:Facility*. A schedule and safety factor are used to set the demand limit above which the DemandManagers become activated. The billing month schedule and demand window are also taken into account when calculating the demand limit.
-
-DemandManagers in the list are activated based on the *Demand Manager Priority*. If the **Sequential** option is used, each manager in the list is activated in sequence from first to last until demand is reduced below the limit or until all managers are activated. If the **All** option is used, all managers are activated simultaneously to achieve the maximum demand reduction.
-
-A DemandManager is skipped if it cannot reduce the demand. Possible reasons that a manager cannot reduce demand include:
-
-- not enough load to limit
-
-- not available because of its *Availability Schedule*
-
-- already activated; load limited during a previous timestep.
-
-#### Field: Name
-
-The name of the DemandManagerAssignmentList object.
-
-#### Field: Meter Name
-
-This field references the meter that is to be monitored and demand limited. Only electricity meters are currently allowed.
-
-#### Field: Demand Limit Schedule Name
-
-The reference to the schedule object specifying the target demand limits [schedule values should be in Watts].
-
-#### Field: Demand Limit Safety Fraction
-
-This field is a multiplier that is applied to the target demand limit (above). When the metered demand exceeds (target demand limit \* safety fraction), the DemandManagers begin to limit the demand. This helps to ensure that the target limit is not exceeded.
-
-#### Field: Billing Period Schedule Name
-
-The reference to the schedule object that defines the monthly billing periods. The peak demand during the peak period of the billing period typically determines the demand charge. This should reference the same schedule that is used in the *Month Schedule Name* field of the UtilityCost:Tariff object. If left blank, it defaults to the regular divisions between months.
-
-#### Field: Peak Period Schedule Name
-
-The reference to the schedule object that defines the peak/off-peak time-of-use periods. The peak demand during the peak period of the billing period typically determines the demand charge. This should reference the same schedule that is used in the *Time of Use Period Schedule Name* field of the UtilityCost:Tariff object. A value of 1 indicates the peak period; any other value is off-peak. If left blank, it defaults to always on the peak period. The DemandManagerAssignmentList only attempts to demand limit during peak periods.
-
-#### Field: Demand Window Length
-
-This field is similar to the field of the same name in the UtilityCost:Tariff object. However, the user may not want to limit using the same demand window as the utility company. This field allows the user to input the number of minutes over which to calculate the current demand. The minutes are rounded to match the nearest multiple of time steps.
-
-#### Field: Demand Manager Priority
-
-This field indicates what logic should be used to activate the individual DemandManagers in the list. **Sequential** treats the list of DemandManagers as a sequential priority list, i.e., the first DemandManager in the list is activated first, then the second, etc., until the demand falls below the limit. **All** activates all demand managers to achieve the maximum demand reduction.
-
-#### Field: Demand Manager Type 1
-
-The key word defining the type of DemandManager.
-
-#### Field: Demand Manager Name 1
-
-The name of a DemandManager object defined elsewhere in the input file.
-
-DemandManagers are listed by pairs of data items:   *Demand Manager Type* and *Demand Manager Name*. Ten managers are accomodated in the list by default. The IDD specification, however, is extensible and additional pairs may be added by directly editing the IDD.
-
-An example IDF showing how this object is used is provided below:
-
-```idf
-   DemandManagerAssignmentList,
-       Demand Manager,                   !- Name
-       Electricity:Facility,       !- Meter Name
-       Limit Schedule,                   !- Demand Limit Schedule Name
-       1.0,                                         !- Demand Limit Safety Fraction
-       ,                                               !- Billing Period Schedule Name
-       ,                                               !- Peak Period Schedule Name
-       15,                                           !- Demand Window Length {minutes}
-       Sequential,                           !- Demand Manager Priority
-       DemandManager:ExteriorLights,   !- DemandManager 1 Object Type
-       Ext Lights Manager,           !- DemandManager 1 Name
-       DemandManager:ElectricEquipment,   !- DemandManager 2 Object Type
-       Eq Mgr Stage 1,                   !- DemandManager 2 Name
-       DemandManager:ElectricEquipment,   !- DemandManager 3 Object Type
-       Eq Mgr Stage 2,                   !- DemandManager 3 Name
-       DemandManager:ElectricEquipment,   !- DemandManager 4 Object Type
-       Eq Mgr Stage 3,                   !- DemandManager 4 Name
-       DemandManager:Lights,       !- DemandManager 5 Object Type
-       Lights Manager,                   !- DemandManager 5 Name
-       DemandManager:Thermostats,   !- DemandManager 6 Object Type
-       Thermostats Manager;         !- DemandManager 6 Name
-```
-
-
-
-### DemandManagerAssignmentList Outputs
-
-The following output variables are reported for the DemandManagerAssignmentList object:
-
-* Zone,Average,Demand Manager Meter Demand Power [W]
-
-* Zone,Average,Demand Manager Average Demand Power [W]
-
-* Zone,Average,Demand Manager Peak Demand Power [W]
-
-* Zone,Average,Demand Manager Scheduled Limit Power [W]
-
-* Zone,Average,Demand Manager Demand Limit Power [W]
-
-* Zone,Average,Demand Manager Avoided Demand [W]
-
-* Zone,Average,Demand Manager Over Limit Power [W]
-
-* Zone,Sum,Demand Manager Over Limit Time [hr]
-
-* Zone,Sum,Demand Manager Exterior Energy Iteration Count []
-
-* Zone,Sum,Demand Manager Heat Balance Iteration Count []
-
-* Zone,Sum,Demand Manager HVAC Iteration Count []
-
-
-
-#### Demand Manager Meter Demand Power [W]
-
-The current demand for the designated meter.
-
-#### Demand Manager Average Demand Power [W]
-
-The current demand for the designated meter averaged over the *Demand Window Length*.
-
-#### Demand Manager Peak Demand Power [W]
-
-The peak demand in the billing month so far.
-
-#### Demand Manager Scheduled Limit Power [W]
-
-The scheduled target demand limit from the *Demand Limit Schedule*.
-
-#### Demand Manager Demand Limit Power [W]
-
-The actual demand limit after multiplication by the *Demand Limit Safety Fraction*.
-
-#### Demand Manager Avoided Demand [W]
-
-The demand that was avoided by the active DemandManagers.
-
-#### Demand Manager Over Limit Power [W]
-
-The difference between the demand limit and the average demand.
-
-#### Demand Manager Over Limit Time [hr]
-
-The number of hours that the demand limit was exceeded.
-
-#### Demand Manager Exterior Energy Iteration Count []
-
-The number times that the exterior energy use was resimulated for demand limiting.
-
-#### Demand Manager Heat Balance Iteration Count []
-
-The number times that the zone heat balance was resimulated for demand limiting.
-
-#### Demand Manager HVAC Iteration Count []
-
-The number times that the HVAC system was resimulated for demand limiting.
-
-### DemandManager:ExteriorLights
-
-The DemandManager:ExteriorLights object is used for demand limiting Exterior:Lights objects.
-
-#### Field: Name
-
-The name of the DemandManager:ExteriorLights object.
-
-#### Field: Availability Schedule Name
-
-The reference to the schedule object specifying the availability of this DemandManager. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Limit Control
-
-This field specifies the type of limiting control. The **Fixed** option reduces the power to the controlled loads by a fixed amount determined by the *Maximum Limit Fraction* field. The **Off** option disables the DemandManager in the simulation.
-
-#### Field: Minimum Limit Duration
-
-The minimum amount of time [minutes] that the DemandManager will continue to demand limit after being activated. This prevents loads from turning on and off every time step.
-
-#### Field: Maximum Limit Fraction
-
-This field specifies a fraction of the *Design Level* power for the load that determines the lowest allowable power level. With *Limit Control* set to **Fixed**, the power is reduced to *Maximum Limit Fraction \* Design Level* whenever the manager is activated. For example, if the *Maximum Limit Fraction* is 0.8, then a 100 W design level load is reduced to 80 W when limiting. A *Maximum Limit Fraction* of zero means that the load can be shut off entirely.
-
-#### Field: Limit Step Change
-
-NOT YET IMPLEMENTED.
-
-#### Field: Selection Control
-
-This field specifies which loads are selected to be limited. The **All** option simultaneously limits all of the loads listed in this DemandManager. The **RotateMany** option limits all loads except for one which rotates sequentially through the loads listed. The **RotateOne** limits only one load which rotates sequentially through the loads listed. The time interval between rotations is set by the *Rotation Duration* field.
-
-#### Field: Rotation Duration
-
-If the **RotateOne** or **RotateMany** option is used for *Selection Control*, this field sets the time interval [minutes] between rotations.
-
-#### Field: Exterior Lights 1-10 Name
-
-The names of Exterior:Lights objects defined elsewhere in the input file. These are the loads to be limited by this DemandManager.
-
-Ten objects are accomodated in the list by default. The IDD specification, however, is extensible and additional fields may be added by directly editing the IDD.
-
-An example IDF showing how this object is used is provided below:
-
-
-
-```idf
-   DemandManager:ExteriorLights,
-       Ext Lights Manager,           !- Name
-       ,                                               !- Availability Schedule Name
-       Fixed,                                     !- Limit Control
-       60,                                           !- Minimum Limit Duration {minutes}
-       0.0,                                         !- Maximum Limit Fraction
-       ,                                               !- Limit Step Change
-       All,                                         !- Selection Control
-       ,                                               !- Rotation Duration {minutes}
-       Exterior Lights;                 !- Exterior Lights 1 Name
-```
-
-
-
-### DemandManager:ExteriorLights Outputs
-
-There are no output variables reported for the DemandManager:ExteriorLights object.
-
-
-
-### DemandManager:Lights
-
-The DemandManager:Lights object is used for demand limiting Lights objects.
-
-#### Field: Name
-
-The name of the DemandManager:Lights object.
-
-#### Field: Availability Schedule Name
-
-The reference to the schedule object specifying the availability of this DemandManager. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Limit Control
-
-This field specifies the type of limiting control. The **Fixed** option reduces the power to the controlled loads by a fixed amount determined by the *Maximum Limit Fraction* field. The **Off** option disables the DemandManager in the simulation.
-
-#### Field: Minimum Limit Duration
-
-The minimum amount of time [minutes] that the DemandManager will continue to demand limit after being activated. This prevents loads from turning on and off every time step.
-
-#### Field: Maximum Limit Fraction
-
-This field specifies a fraction of the *Design Level* power for the load that determines the lowest allowable power level. With *Limit Control* set to **Fixed**, the power is reduced to *Maximum Limit Fraction \* Design Level* whenever the manager is activated. For example, if the *Maximum Limit Fraction* is 0.8, then a 100 W design level load is reduced to 80 W when limiting. A *Maximum Limit Fraction* of zero means that the load can be shut off entirely.
-
-#### Field: Limit Step Change
-
-NOT YET IMPLEMENTED.
-
-#### Field: Selection Control
-
-This field specifies which loads are selected to be limited. The **All** option simultaneously limits all of the loads listed in this DemandManager. The **RotateMany** option limits all loads except for one which rotates sequentially through the loads listed. The **RotateOne** limits only one load which rotates sequentially through the loads listed. The time interval between rotations is set by the *Rotation Duration* field.
-
-#### Field: Rotation Duration
-
-If the **RotateOne** or **RotateMany** option is used for *Selection Control*, this field sets the time interval [minutes] between rotations.
-
-#### Field: Lights 1-10 Name
-
-The names of Lights objects defined elsewhere in the input file. These are the loads to be limited by this DemandManager.
-
-Ten objects are accomodated in the list by default. The IDD specification, however, is extensible and additional fields may be added by directly editing the IDD.
-
-If a global lights statement is used (Ref: Lights), then only that name need be entered and the demand limiting will be applied to all the zones for that lighting. If only one of a set of zones from a global lights statement is desired, then the name to be entered is: &lt;Zone Name&gt; &lt;Name of Lights Global Object&gt;.
-
-An example IDF showing how this object is used is provided below:
-
-
-
-```idf
-   DemandManager:Lights,
-       Lights Manager,                   !- Name
-       ,                                               !- Availability Schedule Name
-       Fixed,                                     !- Limit Control
-       60,                                           !- Minimum Limit Duration {minutes}
-       0.5,                                         !- Maximum Limit Fraction
-       ,                                               !- Limit Step Change
-       All,                                         !- Selection Control
-       ,                                               !- Rotation Duration {minutes}
-       Space1-1 Lights 1,             !- Lights 1 Name
-       Space2-1 Lights 1,             !- Lights 2 Name
-       Space3-1 Lights 1,             !- Lights 3 Name
-       Space4-1 Lights 1,             !- Lights 4 Name
-       Space5-1 Lights 1;             !- Lights 5 Name
-```
-
-
-
-
-### DemandManager:Lights Outputs
-
-There are no output variables reported for the DemandManager:Lights object.
-
-
-
-### DemandManager:ElectricEquipment
-
-The DemandManager:ElectricEquipment object is used for demand limiting ElectricEquipment objects.
-
-#### Field: Name
-
-The name of the DemandManager:ElectricEquipment object.
-
-#### Field: Availability Schedule Name
-
-The reference to the schedule object specifying the availability of this DemandManager. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Limit Control
-
-This field specifies the type of limiting control. The **Fixed** option reduces the power to the controlled loads by a fixed amount determined by the *Maximum Limit Fraction* field. The **Off** option disables the DemandManager in the simulation.
-
-#### Field: Minimum Limit Duration
-
-The minimum amount of time [minutes] that the DemandManager will continue to demand limit after being activated. This prevents loads from turning on and off every time step.
-
-#### Field: Maximum Limit Fraction
-
-This field specifies a fraction of the *Design Level* power for the load that determines the lowest allowable power level. With *Limit Control* set to **Fixed**, the power is reduced to *Maximum Limit Fraction \* Design Level* whenever the manager is activated. For example, if the *Maximum Limit Fraction* is 0.8, then a 100 W design level load is reduced to 80 W when limiting. A *Maximum Limit Fraction* of zero means that the load can be shut off entirely.
-
-#### Field: Limit Step Change
-
-NOT YET IMPLEMENTED.
-
-#### Field: Selection Control
-
-This field specifies which loads are selected to be limited. The **All** option simultaneously limits all of the loads listed in this DemandManager. The **RotateMany** option limits all loads except for one which rotates sequentially through the loads listed. The **RotateOne** limits only one load which rotates sequentially through the loads listed. The time interval between rotations is set by the *Rotation Duration* field.
-
-#### Field: Rotation Duration
-
-If the **RotateOne** or **RotateMany** option is used for *Selection Control*, this field sets the time interval [minutes] between rotations.
-
-#### Field: Electric Equipment 1-10 Name
-
-The names of ElectricEquipment objects defined elsewhere in the input file. These are the loads to be limited by this DemandManager.
-
-Ten objects are accomodated in the list by default. The IDD specification, however, is extensible and additional fields may be added by directly editing the IDD.
-
-If a global Electric Equipment statement is used (Ref: ElectricEquipment), then only that name need be entered and the demand limiting will be applied to all the zones for that equipment. If only one of a set of zones from a global electric equipment statement is desired, then the name to be entered is: &lt;Zone Name&gt; &lt;Name of ElectricEquipment Global Object&gt;.
-
-An example IDF showing how this object is used is provided below:
-
-```idf
-   DemandManager:ElectricEquipment,
-       Eq Mgr Stage 3,                   !- Name
-       ,                                               !- Availability Schedule Name
-       Fixed,                                     !- Limit Control
-       60,                                           !- Minimum Limit Duration {minutes}
-       0.0,                                         !- Maximum Limit Fraction
-       ,                                               !- Limit Step Change
-       All,                                         !- Selection Control
-       ,                                               !- Rotation Duration {minutes}
-       Space5-1 ElecEq 1;             !- Electric Equipment 1 Name
-```
-
-
-
-### DemandManager:ElectricEquipment Outputs
-
-There are no output variables reported for the DemandManager:ElectricEquipment object.
-
-
-
-### DemandManager:Thermostats
-
-The DemandManager:Thermostats object is used for demand limiting ZoneControl:Thermostat objects.
-
-#### Field: Name
-
-The name of the DemandManager:Thermostats object.
-
-#### Field: Availability Schedule Name
-
-The reference to the schedule object specifying the availability of the DemandManager. A schedule value of 0 indicates that the unit is off for that time period. A schedule value greater than 0 indicates that the unit can operate during the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Reset Control
-
-This field specifies the type of limiting control. The **Fixed** option resets the thermostats to a fixed temperature determined by the *Maximum Heating Setpoint Reset* and *Maximum Cooling Setpoint Reset* fields. The **Off** option disables the DemandManager in the simulation.
-
-#### Field: Minimum Reset Duration
-
-The minimum amount of time [minutes] that the DemandManager will continue to demand limit after being activated. This prevents thermostats from resetting on and off every time step.
-
-#### Field: Maximum Heating Setpoint Reset
-
-This field specifies the thermostat heating setpoint temperature [C] that represents the largest allowable temperature reset or setback. With *Reset Control* set to **Fixed**, the setpoint temperature is reset to the *Maximum Heating Setpoint Reset* whenever the manager is activated. For example, if the heating setpoint is normally 22 C and the *Maximum Heating Setpoint Reset* is 20 C, then the setpoint is reset to 20 C when limiting.
-
-#### Field: Maximum Cooling Setpoint Reset
-
-This field specifies the thermostat cooling setpoint temperature [C] that represents the largest allowable temperature reset or setback. With *Reset Control* set to **Fixed**, the setpoint temperature is reset to the *Maximum Cooling Setpoint Reset* whenever the manager is activated. For example, if the cooling setpoint is normally 22 C and the *Maximum Cooling Setpoint Reset* is 24 C, then the setpoint is reset to 24 C when limiting.
-
-#### Field: Reset Step Change
-
-NOT YET IMPLEMENTED.
-
-#### Field: Selection Control
-
-This field specifies which loads are selected to be limited. The **All** option simultaneously limits all of the loads listed in this DemandManager. The **RotateMany** option limits all loads except for one which rotates sequentially through the loads listed. The **RotateOne** limits only one load which rotates sequentially through the loads listed. The time interval between rotations is set by the *Rotation Duration* field.
-
-#### Field: Rotation Duration
-
-If the **RotateOne** or **RotateMany** option is used for *Selection Control*, this field sets the time interval [minutes] between rotations.
-
-#### Field: Thermostat 1-10 Name
-
-The names of ZoneControl:Thermostat objects defined elsewhere in the input file. These are the loads to be limited by this DemandManager.
-
-Ten objects are accomodated in the list by default. The IDD specification, however, is extensible and additional fields may be added by directly editing the IDD.
-
-If a global thermostat statement is used (Ref: ZoneControl:Thermostat), then only that name need be entered and the demand limiting will be applied to all the zones for that thermostatic control. If only one of a set of zones from a global thermostat statement is desired, then the name to be entered is: &lt;Zone Name&gt; &lt;Name of Thermostat Global Object&gt;.
-
-An example IDF showing how this object is used is provided below:
-
-
-
-```idf
-   DemandManager:Thermostats,
-       Thermostats Manager,         !- Name
-       ,                                               !- Availability Schedule Name
-       Fixed,                                     !- Reset Control
-       60,                                           !- Minimum Reset Duration {minutes}
-       19,                                           !- Maximum Heating Setpoint Reset {C}
-       26,                                           !- Maximum Cooling Setpoint Reset {C}
-       ,                                               !- Reset Step Change
-       All,                                         !- Selection Control
-       ,                                               !- Rotation Duration {minutes}
-       SPACE1-1 Control,               !- Thermostat 1 Name
-       SPACE2-1 Control,               !- Thermostat 2 Name
-       SPACE3-1 Control,               !- Thermostat 3 Name
-       SPACE4-1 Control,               !- Thermostat 4 Name
-       SPACE5-1 Control;               !- Thermostat 5 Name
-```
-
-
-### DemandManager:Thermostats Outputs
-
-There are no output variables reported for the DemandManager:Thermostats object.
-
-
-### DemandManager:Ventilation
-
-The DemandManager:Ventilation object is used for limiting the ventilation rate calculated from the Controller:OutdoorAir object.
-
-#### Field: Name
-
-The name of the DemandManager:Ventilation object.
-
-#### Field: Availability Schedule Name
-
-The reference to the schedule object specifying the availability of this demand manager. A schedule value of zero indicates that this demand response (DR) is not applicable for that time period. A schedule greater than zero indicates that the demand response applies during the time period. If this field is blank, the schedule has values of one for all time period.
-
-#### Field: Limit Control
-
-This field specifies the type of limiting control. There are three options. The **FixedRate** option reduces the ventilation to a specified air flow rate. The **ReductionRatio** specifies the multiplier of the ventilation rate. The **Off** option disables the demand manager in the simulation.
-
-#### Field: Minimum Limit Duration
-
-The minimum amount of time [minutes] that the demand manager will continue to demand limit after being activated. This prevent loads from turning on and off every time step.
-
-#### Field: Fixed Rate
-
-This field specifies the amount of fixed ventilation rate when the demand manager is active and *FixedRate* limit control is applied. The unit is m3/s.
-
-#### Field: Reduction Ratio
-
-This field specifies the multiplier of the ventilation rate when the demand manager is active and *ReductionRatio* limit control is applied.
-
-#### Field: Limit Step Change
-
-NOT YET IMPLEMENTED.
-
-#### Field: Selection Control
-
-This field specifies which loads (ventilation rates) are selected to be limited. The **All** option simultaneously limits all of the loads listed in the demand manager. The **RotateMany** option limits all loads except for one which rotates sequentially through the loads listed. The **RotateOne** limits only one load which rotates sequentially through the loads listed. The time interval between rotations is set by the *Rotation Duration* field.
-
-#### Field: Rotation Duration
-
-If the **RotateOne** of **RotateMany** option is used for *Selection Control*, this field sets the time interval [minues] between rotations.
-
-#### Field: Controller Outdoor Air 1-10 Name
-
-The names of Controller:OutdoorAir objects defined elsewhere in the input file. These are the ventilation rates to be limited by this demand manager. Then objects are accommodated in the list by default. The IDD specification, however, is extensible and additional fields may be added by directly editing the IDD.
-
-An example IDF showing how this object is used is provided below:
-
-
-
-```idf
-   DemandManager:Ventilation,
-       Ventilation Manager,         !- Name
-       ,                            !- Availability Schedule Name
-       ReductionRatio,              !- Reset Control
-       60,                          !- Minimum Limit Duration {minutes}
-       ,                            !- Fixed Rate {m3/s}
-       0.5,                         !- Reduction Ratio
-       ,                            !- Limit Step Change
-       All,                         !- Selection Control
-       ,                            !- Rotation Duration {minutes}
-       OA Controller 1;             !- Controller:OutdoorAir Name
-```
-
-
-### DemandManager:Ventilation Outputs
-
-There are no output variables reported for the DemandManager:Ventilation object.
-
-
-Group -- Electric Load Center-Generator Specifications
-------------------------------------------------------
-This group of input objects is related to electric power serving the facility.  EnergyPlus has models for various types of electric generators and power conditioning devices that might be part of the electric power system serving the building being modeled.  Buildings with simple utility electric power service will not necesarily need any of the models in this group.  All EnergyPlus models that have any electric power consumption are assumed to have a straightforward connection to utility grid service and no extra input is needed.  The models in this group of inputs are useful for facilities that more complex electric power service such as:
-
-   - Utility service is at a voltage higher than used in the building and a transformer conditions power coming into to the building as part of the facility.
-   - On site generators produce electricity within the facility.  For example solar photovoltaic panels or natural gas powered electric generators. 
-   - On site electric storage devices. 
-
-For facilities that own their transformer, and the utility services is metered on the high voltage side, the ElectricLoadCenter:Transformer object can be used, and may be the only input object needed.  
-
-All other applications involving on-site generation or storage will require at least one ElectricLoadCenter:Distribution to describe the arrangement and control of a set of electric power devices.  Each of these load centers is like a subpanel connected to the main electrical panel for the facility.  The main panel is assumed to exist whenever the rest of the model includes something that consumes electricity (and does not require any input object).  Each ElectricLoadCenter:Distribution input object describes what devices are on a subpanel connected to the main panel, as well as how they are controlled, dispatched, and arranged to provide some service related to the facility's electric power.  The ElectricLoadCenter:Distribution object manages and calls the individual generator models that are connected to it by being listed in an ElectricLoadCenter:Generators object, such as natural gas powered turbines, photovoltaic panels, wind turbines, etc.  Unlike elsewhere in EnergyPlus where there are loops, branches, or generic equipment lists that allow describing custom arrangements, the electric power service modeling is restricted to a collection of predefined arrangements, called "buss types."  Many on site generation and storage configurations common in buildings can be modeled using just one ElectricLoadCenter:Distribution object.  However, by combining multiple load centers with different equipment and operations schemes, it is possible to model more complex configurations.  (Note that when using multiple ElectricLoadCenter:Distribution objects, the order of the ElectricLoadCenter:Distribution objects within the input file determines the order in which they are called to interact with the main panel.)
-
-The following diagram shows some of the devices and arrangements that can be modeled using the inputs in this group. 
-
-![PowerServiceOverview](media/ElectPowerServiceOverview.png)
-
-
-### ElectricLoadCenter:Transformer
-
-This object is used to model the energy losses of transformers when they are used to transfer electricity from the grid to a building (as distribution transformers) or transfer electricity from onsite generators to the grid. Distribution transformers reduce the voltage on utility distribution lines (34.5 kV or less) to a lower secondary voltage (600 V or less) suitable for customer equipment. According to the medium used for cooling and insulation, distribution transformers can be classified into liquid-immersed and dry type transformers. According to the input voltages, distribution transformers can be classified into medium-voltage (between 600 V and 34.5kV) and low-voltage transformer (less than 600 V). The transformers used to output the surplus electricity from onsite generators to the grid usually match the cogeneration voltage to the grid. This object can be used for all types of distribution transformers and the transformers used to output electricity from onsite generators to the grid, but the model defaults applies to the low-voltage dry type transformers because they are the most common type found in commercial and industrial facilities.
-
-Energy losses in transformers consist of the no load (core) loss and the load (winding) loss. The no load loss comes primarily from the switching of the magnetic fields in the core material. It is roughly constant and exists continuously in the core material as long as the transformer is energized. The load loss comes from the electrical resistance in the windings when there is a load on the transformer. The load loss is proportional to the load squared with a small temperature correction. The energy losses at a given load depend on the transformer   s performance. This object provides the user two alternative ways to indicate the transformer   s performance. First, the user can provide the no load loss and load loss at rated conditions. Second, the user can provide the nameplate efficiency and the corresponding reference conditions. The detailed algorithms to calculate the energy losses are described in the Engineering Reference.
-
-The user needs to specify which loads are connected to the transformer. This is achieved in different manners depending on the transformer usage. For a distribution transformer, the user needs to provide a number of electric meters wired to that transformer. The input object can currently accommodate up to ten meters, but it is extensible by modifying the Energy+.idd entry. For a transformer used to output electricity from onsite generators to the grid, the user needs to indicate the transformer name in the served electric load center.
-
-
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name (ref. Schedule objects) that contains information on the availability of the transformer. A schedule value greater than 0 (usually 1 is used) indicates that the transformer is available to convert AC power from one voltage to another. A value less than or equal to 0 (usually 0 is used) denotes that the transformer is not available. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Transformer Usage
-
-This field indicates one of the three supported transformer application types: PowerInFromGrid, PowerOutToGrid, and LoadCenterPowerConditioning. 
-A PowerInFromGrid type of transformer is used to step down voltage from the electricity grid to the building.  The transformer with this type of use is somewhat free standing and does not need to be referenced in any ElectricLoadCenter:Distribution object.  There should be only one PowerInFromGrid transformer in the model. 
-A PowerOutToGrid type of transformer is used to match voltage from the building to the electricity grid. This conditions power exported out of the facility and feed back into the grid.  This type of transformer will only be needed if the building ever exports power and the building and grid connection have different voltages.  There should be only one PowerOutToGrid transformer in the model and it will serve all the surplus electricity produced by electric load center(s).
-A LoadCenterPowerConditioning type of transformer is used to match voltage between an electic load center (subpanel) and the facility's main panel.  Each electric load center can have its own transformer to condition power fed into the main panel.  For electric load centers that also draw power from the main panel, to charge storage, the transformer is assumed to operate in both directions (at the same performance). This type of transformer should be named in an ElectricLoadCenter:Distribution object.
-
-#### Field: Zone Name
-
-This field contains the name of the thermal zone where the transformer is located. Entering a valid name of zone here will direct EnergyPlus to include the transformer   s losses as heat gains to the named thermal zone. If the transformer is not within a thermal zone, this field can be left blank and the thermal energy associated with transformer losses is removed from the building model.
-
-#### Field: Radiative Fraction
-
-This field contains the fraction of transformer   s losses that enter the zone as long-wave thermal radiation. This numeric filed should have a value between 0.0 and 1.0. The balance of the losses is convective. This field is not used if the previous field for zone name is left blank.
-
-#### Field: Rated Capacity
-
-This field defines the rated capacity of the transformer in VA.
-
-#### Field: Phase
-
-This field indicates whether the transformer is a single phase or three phase type. The two alternative values are 1 or 3. The default is 3. This field is currently not used in the model.
-
-#### Field: Conductor Material
-
-This field specifies the winding material used by the transformer. There are two options: Copper and Aluminum. The choice will determine the thermal coefficient of resistance used to calculate the temperature correction factor for the transformer load losses. The default is Aluminum.
-
-#### Field: Full Load Temperature Rise
-
-This numeric field defines the temperature rise of the windings above the ambient temperature, when the transformer is loaded at its nameplate rating. For liquid-immersed distribution transformers, the full load temperature rise usually takes the value of 65  &deg;C. For dry-type transformers, the temperature rise usually takes three optional values: 80, 115 and 150  &deg;C. This field accepts any value between the minimum (50  &deg;C) and the maximum (180  &deg;C). The default is 150  &deg;C.
-
-#### Field: Fraction of Eddy Current Losses
-
-This field defines the fraction of load losses resulting from the eddy currents. Transformer's load losses comprise two parts: the ohmic loss due to the current flowing in the resistance of the windings and the eddy and stray losses due to the eddy currents. This field indicates the fraction of the load losses due to the eddy currents. This numeric field should have a value between 0.0 and 1.0. The default is 0.1.
-
-#### Field: Performance Input Method
-
-This alpha field contains the method by which the user will specify the transformer performance: RatedLosses or NominalEfficiency. If this field is left blank in the input data file, the default input method is assumed to be RatedLosses. If the method NominalEfficiency is selected, the user must enter the fields for the nameplate efficiency and the corresponding reference coditions as described below. If the method RatedLosses is selected, then the fields for rated no load loss and load loss must be entered as described below.
-
-#### Field: Rated No Load Loss
-
-This field defines the no load loss (W) at rated load and conditions. The no load loss is roughly constant and exists whenever the transformer is energized. The no load loss is also called the core loss. This field is used only if the field of Performance Input Method is specified as RatedLosses.
-
-#### Field: Rated Load Loss
-
-This field defines the load loss (W) at rated load and conditions. The load loss varies with the square of the load being served by the transformer. The load loss is also called the winding loss because the load loss occurs in the primary and secondary windings around the core. This field is used only if the field of Performance Input Method is specified as RatedLosses.
-
-#### Field: Nameplate Efficiency
-
-This field contains the value for transformer efficiency at a given per unit load and specified reference temperature. This field is used only if the field of Performance Input Method is specified as NominalEfficiency. The default is 0.98.
-
-#### Field: Per Unit Load for Nameplate Efficiency
-
-This field defines the percentage of the rated capacity at which the nameplate efficiency is measured. According to the NEMA (National Electrical Manufactures Association) Standard TP-1, the per unit load takes the value of 0.35 for dry-type distribution transformers and it takes the value of 0.50 for liquid-filled distribution transformers. The default is 0.35.
-
-#### Field: Reference Temperature for Nameplate Efficiency
-
-This field defines the conductor temperature at which the nameplate efficiency is measured. This field is used only if the field of Performance Input Method is specified as    NominalEfficiency   . According to the NEMA Standard TP-1, the reference temperature takes the value of 75  &deg;C for dry-type distribution transformers and it takes the value of 55  &deg;C for liquid-filled distribution transformers. The default is 75  &deg;C.
-
-#### Field: Per Unit Load for Maximum Efficiency
-
-This field defines the percentage of the rated capacity at which the maximum efficiency is obtained. This field is used only if the field of Performance Input Method is specified as    NominalEfficiency   . A blank field indicates that it takes the same value as the per unit load for nameplate efficiency.
-
-#### Field: Consider Transformer Loss for Utility Cost
-
-This field indicates whether the transformer losses are considered to calculate utility cost.  This field applies to a PowerInFromGrid type of transformer.  In some cases, the transformer losses are required but they are not part of the energy consumption for utility cost calculation. For example, the transformer is owned by the utility company but it locates in the building. In this case, it might be desired to model transformer energy losses for HVAC operation but the energy losses will not be accounted for utility cost.
-
-#### Field: Electric Meter 1-10 Name
-
-A transformer may serve different loads such as plug loads, some lighting loads, and some HVAC equipment loads. These fields apply to a PowerInFromGrid type of transformer.  The user needs to specify which loads are connected to the transformer.  For example the HVAC and Plant equipment might use a higher voltage than the building and only the building loads need power conditioning.  This is achieved by providing a list of electric meters wired to the transformer. The input object can currently accommodate up to ten meters, but it is extensible by modifying the Energy+.idd entry. Any valid electric meter name can be used here to wire to the transformer loads. Many different meters are automatically generated by the program and will depend on the objects used throughout the input file. The typical process of determining the exact name to enter in this field involves doing an initial run of EnergyPlus and then examining the \*.mdd file which will list the meters and their resulting names. A custom meter is also supported. The meter must have electricity as its resource type.
-
-An example input of the ElectricLoadCenter:Transformer input is:
-
-
-```idf
-   ElectricLoadCenter:Transformer,
-       Transformer 1,                       !-Name
-       Always On,                           !- Availability Schedule Name
-       PowerInFromGrid,                     !- Transformer Usage
-       ,                                    !- Zone Name
-       ,                                    !-Radiative Fraction
-       15000,                               !- Nameplate Rating {VA}
-       3,                                   !- Phase
-       Aluminum,                            !- Conductor Material
-       150,                                 !- Full Load Temperature Rise { &deg;C}
-       0.1,                                 !- Fraction of Eddy Current Losses
-       NominalEfficiency,                   !- Performance Input Method
-       ,                                    !- Rated No Load Loss {W}
-       ,                                    !- Rated Load Loss {W}
-       0.985,                               !- Nameplate Efficiency
-       0.35,                                !- Per Unit Load for Nameplate Efficiency
-       75,                                  !- Reference Temperature for Nameplate Efficiency { &deg;C}
-       ,                                    !- Per Unit Load for Maximum Efficiency
-       Yes,                                 !- Consider Transformer Loss for Utility Cost
-       Electricity:Building;                !- Meter 1 Name
-
-
-   Schedule:Compact,
-       Always On,                             !- Name
-       Fraction,                               !- ScheduleType
-       Through: 12/31,                   !- Field #1
-       For: AllDays,                       !- Field #2
-       Until: 24:00,                       !- Field #3
-       1.0;                                         !- Field #4
-```
-
-
-
-### ElectricLoadCenter:Transformer Outputs
-
-* HVAC,Average,Transformer Efficiency[]
-
-* HVAC,Average,Transformer Output Electric Power[W]
-
-* HVAC,Sum,Transformer Output Elecric Energy [J]
-
-* HVAC,Average,Transformer Input Electric Power[W]
-
-* HVAC,Sum,Transformer Input Electric Energy [J]
-
-* HVAC,Average,Transformer No Load Loss Rate [W]
-
-* HVAC,Sum,Transformer No Load Loss Energy [J]
-
-* HVAC,Average,Transformer Load Loss Rate [W]
-
-* HVAC,Sum,Transformer Load Loss Energy [J]
-
-* HVAC,Average,Transformer Thermal Loss Rate [W]
-
-* HVAC,Sum,Transformer Thermal Loss Energy [J]
-
-* HVAC,Sum,Transformer Distribution Electric Loss Energy [J]
-
-* HVAC,Sum,Transformer Cogeneration Electric Loss Energy [J]
-
-#### Transformer Efficiency
-
-This output field is the efficiency at which the distribution transformer changes alternating current from the higher primary voltage to a lower secondary voltage. The efficiency is calculated for each HVAC system timestep being simulated, and the results are averaged for the timestep being reported.
-
-#### Transformer Output Electric Power [W]
-
-#### Transformer Output Elecric Energy [J]
-
-These outputs are the total electricity power or energy provided by the transformer. They are equal to the metered loads which are wired to the transformer. These values are calculated for each HVAC system timestep being simulated, and the results are averaged (for power) or summed (for energy) for the timestep being reported.
-
-#### Transformer Input Electric Power [W]
-
-#### Transformer Input Electric Energy [J]
-
-These outputs are the total electricity power or energy fed into the transformer. These values are calculated for each HVAC system timestep being simulated, and the results are averaged (for power) or summed (for energy) for the timestep being reported.
-
-#### Transformer No Load Loss Rate [W]
-
-#### Transformer No Load Loss Energy [J]
-
-These outputs are the no load loss occurred in the transformer. These values are calculated for each HVAC system timestep being simulated, and the results are averaged (for rate) or summed (for energy) for the timestep being reported.
-
-#### Transformer Load Loss Rate [W]
-
-#### Transformer Load Loss Energy [J]
-
-These outputs are the load loss occurred in the transformer. These values are calculated for each HVAC system timestep being simulated, and the results are averaged (for rate) or summed (for energy) for the timestep being reported.
-
-#### Transformer Thermal Loss Rate [W]
-
-#### Transformer Thermal Loss Energy [J]
-
-These outputs are the total energy losses occurred in the transformer. They are equal to the sum of the no load loss and the load loss. These values are calculated for each HVAC system timestep being simulated, and the results are averaged (for rate) or summed (for energy) for the timestep being reported.
-
-#### Transformer Distribution Electric Loss Energy [J]
-
-This output is the total energy losses occurred in the transformer when it is used for input power from grid to building. It is set as zero if the transformer is used to transfer energy from onsite power generators to the electricity grid. This output is also added to a meter with ResourceType = Electricity, GroupKey = System.
-
-#### Transformer Cogeneration Electric Loss Energy   [J]
-
-This output is the total energy losses occurred in the transformer when it is used for input onsite cogeneration to the grid. It is set as zero if the transformer is used to transfer the electricity grid to building. This output is also added to a meter with ResourceType = ElectricityProduced, EndUseKey = Cogeneration, GroupKey = System.
-
-### ElectricLoadCenter:Distribution
-
-ElectricLoadCenter:Distribution objects are used to include on-site electricity generators and or storage in a simulation. The electric load center dispatches both generators and storage according to operation schemes and tracks and reports the amount of electricity generated and purchased. When using on-site generators, the program provides various reports for the electricity used, generated on site, stored, exported etc.  There are two separate operation schemes, one for generators and a second for storage, and they can be different.  The generator operation is managed before the storage operation.  Facility electrical demand tracking is done by the internal or custom meters used by EnergyPlus for reporting. The thermal demand tracking uses internal load calculations from the plant simulation. The dispatching of different generators is based on expectations based on their nominal/rated electric power output. If the current conditions are such that the generator model determines that generation was higher or lower, then the results of the dispatch may differ from expectations.
-
-Multiple different ElectricLoadCenter:Distribution objects can be included in an input file.   A great deal of flexibility is available by mixing different load centers and operating schemes. If multiple load centers are used, the supervisory control will dispatch generators sequentially across the load centers.   Therefore, the order of these input objects in the IDF file becomes important with the generators associated with first load center in the file being the first to be managed.   A certain amount of caution is needed to avoid conflicting operating schemes.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the electric load center.
-
-#### Field: Generator List Name
-
-This alpha field contains the identifying name for the list of generators in the set defined in an ElectricLoadCenter:Generators object.  All the generators connected to this load center need to be of the same type in terms of all AC or all DC.  Currently the only DC generators are photovoltaic panels, the others are all AC.  A facility with both AC and DC generators will need to use seperate ElectricLoadCenter:Distribution objects.  The generator list named here can only be associated with one load center.  This field can be left blank if there are no generators. 
-
-#### Field: Generator Operation Scheme Type
-
-This alpha field specifies the type of operating scheme for the generator set. The available operating schemes are Baseload, DemandLimit, TrackElectrical, TrackSchedule, TrackMeter, FollowThermal, and FollowThermalLimitElectrical.  The Baseload scheme operates the generators at their rated (requested) electric power output when the generator is scheduled ON (ref. ElectricLoadCenter:Generators). The Baseload scheme requests all generators scheduled ON (available) to operate, even if the amount of electric power generated exceeds the total facility electric power demand. The DemandLimit scheme limits the amount of purchased electrical from the utility to the amount specified in the input object. The DemandLimit scheme tries to have the generators meet all of the demand above the purchased electric limit set by the user in the next field. The TrackElectrical scheme tries to have the generators meet all of the electrical demand for the building. The TrackSchedule scheme tries to have the generators meet all of the electrical demand determined in a user-defined schedule. The TrackMeter scheme tries to have the generators meet all the electrical demand from a meter, which could also be a user-defined custom meter.
-
-The DemandLimit, TrackElectrical, TrackSchedule, and TrackMeter schemes will sequentially load the available generators. All demand not met by available generator capacity (or storage) will be met by purchased electrical. Therefore, if DemandLimit, TrackElectrical, TrackSchedule, or TrackMeter is utilized and the available generators are not enough to meet demand, then purchased electrical will offset the difference. If a generator is needed in the simulation for a small load and it is less than the minimum part load ratio the generator will operate at the minimum part load ratio and the excess will either reduce demand or the excess energy will be available for returning to the electric grid.
-
-The FollowThermal and FollowThermalLimitElectrical schemes are for heat following cogeneration and run the generators to meet the thermal demand.  The FollowThermal schemes allow excess electrical generation to be exported to the grid, while the FollowThermalLimitElectrical scheme restricts generator output to a maximum of the building's current electrical demand (so that no electricity is exported).  The thermal demand is determined from the plant modeling and depends on the flow requested by other components on the demand side of the plant loop, the loop temperatures, and the loop temperature set point.  The electric load center converts the thermal load to an electrical load using a nominal ratio of the thermal to electrical power production for each generator.  For these schemes, the generator needs to be connected to the supply side of a plant loop and components that request hot water need to be on the demand side of the plant loop.   This is different than the usual configuration for electrical following schemes where the generator is put on the demand side and request flow for the purposes of cooling the generator.  Therefore a switch from one of the electrical-based operating schemes to one of the thermal-based operating schemes requires a substantial change in plant topology.
-
-If the load center includes electrical storage, then the choice of generator operating schemes will also affect how storage is managed.  The generator operation scheme and dispatch is modeled before the storage operation scheme so that the current generator production is available for use with the storage operation scheme. 
-
-#### Field: Demand Limit Scheme Purchased Electric Demand Limit
-
-This numerical field is the user input for the demand limit above which the generators will try and meet the entire electrical load on the building minus the photovoltaic array if available.
-
-#### Field: Track Schedule Name Scheme Schedule Name
-
-This alpha field is the user input for the name of a schedule defined elsewhere in the input file that contains values for the    demand    loads placed on the generator(s). The schedule values should be in Watts.
-
-#### Field: Track Meter Scheme Meter Name
-
-This alpha field is the user input for the name of a meter. Any valid meter name can be used here to control the loads that the generator(s) will try to meet. Many different meters are automatically generated by the program and will depend on the objects used throughout the input file. The typical process of determining the exact name to enter in this field involves doing an initial run of EnergyPlus and then examining the \*.rdd file which will list the meters and their resulting names. The \*.mtd file will also be useful to understand what exactly is included in a meter. The user can also use the Output:CustomMeter objects to redefine meter names and to control what electrical loads are included on them in a flexible manner.
-
-#### Field: Electrical Buss Type
-
-This alpha field is used to describe how the electric load center is configured with respect to any power conditioning and/or storage equipment. There are five configurations available for load centers that are selected using one of these keywords:  AlternatingCurrent, AlternatingCurrentWithStorage, DirectCurrentWithInverter, DirectCurrentWithInverterDCStorage, or DirectCurrentWithInverterACStorage.  This input informs the program which of the five pre-configured arrangements is to be used for this load center.  The following diagrams show the kinds of devices and how they are arranged for each of the buss types.
-
-- AlternatingCurrent.  This type of load center is for adding one or more on-site generators that produce AC power.  If the voltage does not match a transformer can be included but is not needed.  AlternatingCurrent is the default.
-
-![LoadCenterBussType](media/ACBussDiagram.png)
-
-- AlternatingCurrentWithStorage.  This type of load center is for adding one or more on-site generators that produce AC power and one on-site electric storage device that uses AC power.  The connection between the load center and the main building panel is bidirectional so that storage can be charged by drawing from the grid.  Transformer is optional.   
-
-![LoadCenterBussType](media/ACStorageBussDiagram.png)
-
-- DirectCurrentWithInverter.  This type of load center is for adding one or more on-site generators that produce DC power, typically photovoltaic panels.  An inverter is needed to convert generated power from DC to AC.  Transformer is optional. 
-
-![LoadCenterBussType](media/DCInverterBussDiagram.png)
-
-- DirectCurrentWithInverterDCStorage.  This type of load center is for adding one or more on-site generatros the produce DC power and one on-site storage device that uses DC power.  An inverter is needed to convert power from DC to AC and is located between the storage and where the subpanel feeds into the main panel.  The connection between the load center and the main building panel is bidirectional so that storage can be charged by drawing from the grid.  An AC to DC converter is needed if the storage operation scheme is such that the control might draw power from the main facility panel into the load center in order to charge storage. Transformer is optional.
-
-![LoadCenterBussType](media/DCInverterWithDCStorageBussDiagram.png)
-
-- DirectCurrentWithInverterACStorage.  This type of load center is for adding one or more on-site generatros the produce DC power and one on-site storage device that uses AC power.   The connection between the load center and the main building panel is bidirectional so that storage can be charged by drawing from the grid.  The inverter is located between the generators and the storage device. Transformer is optional.
-
-![LoadCenterBussType](media/DCInverterWithACStorageBussDiagram.png)
-
-
-#### Field: Inverter Object Name
-
-This field is used to identify the inverter connected to this load center (if any).  This field is only used if the Electrical Buss Type is set to DirectCurrentWithInverter, DirectCurrentWithInverterDCStorage, or DirectCurrentWithInverterACStorage and should contain the user-defined name of an inverter object.   There are three types of inverter models available  -see ElectricLoadCenter:Inverter:Simple, ElectricLoadCenter:Inverter:LookUpTable,   or ElectricLoadCenter:Inverter:FunctionOfPower.   Enter the name of one of these types of inverter objects defined elsewhere in the input file.
-
-#### Field: Electrical Storage Object Name
-
-This field is used to identify the electrical storage connected to this load center (if any).   This field is only used if the Electrical Buss Type is set to AlternatingCurrentWithStorage, DirectCurrentWithInverterDCStorage or DirectCurrentWithInverterACStorage.   Enter the name of an ElectricLoadCenter:Storage:* object defined elsewhere in the input file.
-
-#### Field: Transformer Object Name
-
-This field is used to identify the transformer connected to this load center (if any). This field can be used for any electrical buss types. Enter the name of an ElectricLoadCenter:Transformer object defined elsewhere in the input file.  The transformer should have use type set to LoadCenterPowerConditioning.
-
-#### Field: Storage Operation Scheme
-
-This field is used to select the operation scheme used to govern how storage charge and discharge is controlled.  There are four options:  TrackFacilityElectricDemandStoreExcessOnSite, TrackMeterDemandStoreExcessOnSite, TrackChargeDischargeSchedules, or FacilityDemandLeveling.  
-
-TrackFacilityElectricDemandStoreExcessOnSite indicates that storage control will follow the facility power demand (meter Facility:Electricity) while accounting for any on-site generation.  Only excess on site generation gets stored.  This is the legacy control behavior before version 8.5 and is the default.
-
-TrackMeterDemandStoreExcessOnSite indicates that storage discharge control will follow an electric meter named in the field called Storage Control Track Meter Name.  This scheme is similar TrackFacilityElectricDemandStoreExcessOnSite except that instead of the main facility electric meter, the control is based off of a user-selected meter.
-
-TrackChargeDischargeSchedules indicates that control will follow the charging and discharging power and schedules defined in the fields called Maximum Storage Charge Grid Supply Power, Storage Charge Grid Supply Power Fraction Schedule Name, Design Storage Discharge Grid Export Power, and Storage Discharge Grid Export Fraction Schedule Name.
-
-FacilityDemandLeveling indicates that storage control will attempt to control the facility's power demand drawn from the utility service to a prescribed level.  The target utility demand is entered in the fields called Storage Control Utility Demand Limit and Storage Control Utility Demand Limit Fraction Schedule Name.  This scheme first accounts for any on-site generation and during times of high use will discharge storage to reduce facility grid demand to meet the target level and during times of low use will charge storage from the grid to increase facility grid demand to meet the target level.  This scheme allows controlling the load factor as long as the storage capacity and rates are not limiting what is possible.  Negative schedule values can be used so that a negative demand target is exporting power out to the grid. 
-
-#### Field: Storage Control Track Meter Name
-
-This field is the name of a meter to use when a custom meter is to be used.  This is required when Storage Operation Scheme is set to TrackMeterDemandStoreExcessOnSite.
-
-#### Field: Storage Converter Object Name
-
-This field is the name of an ElectricLoadCenter:Storage:Converter object defined elsewhere in the input file that describes the performance when converting AC to DC when charging DC storage from grid supply. This field is required when using DC storage (buss type DirectCurrentWithInverterDCStorage) with grid supplied charging power (Storage Operation Scheme is set to TrackChargeDischargeSchedules or FacilityDemandLeveling.)  Although some inverter devices are bidirectional a separate converter object is needed to describe AC to DC performance.
-
-#### Field: Maximum Storage State of Charge Fraction
-
-This numeric field specifies the fraction of storage capacity used as an upper limit for controlling charging.  Charging will be constrained so that charging will stop the once this limit is reached. This fraction is the state of charge of the storage device where 1.0 is completely full and 0.0 is completely empty.  This allows supervisory control over charging to model behavior intended to protect the battery from damage. The legacy behavior prior to version 8.5 was to charge to full capacity and therefore the default is 1.0.  
-
-#### Field: Minimum Storage State of Charge Fraction
-
-This numeric field specifies the fraction of storage capacity used as lower limit for controlling discharging.  Discharging will be constrained so that discharging will stop once this limit is reached.  This fraction is the state of charge of the storage device where 1.0 is completely full and 0.0 is completely empty.  This allows supervisory control over discharging to model behavior intended to protect the battery from damage. The legacy behavior prior to version 8.5 was to discharge to empty and therefore the default is 0.0.  
-
-#### Field: Design Storage Control Charge Power
-
-This field is the design maximum rate that electric power can be charged into storage, in Watts.  This field is used as an upper limit for most storage control operation schemes. However for TrackChargeDischargeSchedules, this is the design value for how much power to use when charging and it is multipled by the power fraction schedule in the next field.  Required field when using Storage Operation Schemes set to FacilityDemandLeveling or TrackChargeDischargeSchedules.
-
-#### Field: Storage Charge Power Fraction Schedule Name
-
-This field contains the name of a schedule that controls the timing and magnitude of charging storage.  This is a required field if Storage Operation Scheme is set to TrackChargeDischargeSchedules.  Schedule values should be fractions from 0.0 to 1.0, inclusive.  This schedule will need to be coordinated with the discharging schedule named below. 
-
-#### Field: Design Storage Control Discharge Power
-
-This field is the design maximum rate that electric power can be discharged from storage.  This field is used as an upper limit for most storage control operation schemes. However for TrackChargeDischargeSchedules, this is the design value for how much power to draw when discharging and it is multiplied by the power fraction schedule in the next field.  Required field when using Storage Operation Schemes set to FacilityDemandLeveling or TrackChargeDischargeSchedules.
-
-#### Field: Storage Discharge Power Fraction Schedule Name
-
-This field contains the name of a schedule that controls the timing and magnitude of discharging storage. Required field if Storage Operation Scheme is set to TrackChargeDischargeSchedules.  Schedule values should be fractions from 0.0 to 1.0, inclusive.  This schedule will need to be coordinated with the charging schedule named above.
-
-#### Field: Storage Control Utility Demand Target
-
-This field contains the design demand target in Watts.  This field is used when the storage operation scheme is set to FacilityDemandLeveling.  This becomes the target utility service demand power for discharge control.  This design value is multiplied by the fraction schedule named in the next field.  This is more than an upper limit, it is also going to call for extra electric power to raise demand up to the target and put the extra power into on-site storage.  This field is required for FacilityDemandLimit storage operation scheme.
-
-#### Field: Storage Control Utility Demand Target Fraction Schedule Name
-
-This field is the name of schedule that modifies the utility demand power target over time. Schedule values should be fractions from -1.0 to 1.0, inclusive. Negative values indicate export to grid.  This field is required if Storage Operation Scheme is set to FacilityDemandLeveling.
-
-
-Examples of this object are:
-
-```idf
-ElectricLoadCenter:Distribution,
-       SOFC Electric Load Center,      !- Name
-       Micro-Generators,               !- Generator List Name
-       Baseload,                       !- Generator Operation Scheme Type
-       0.0,                            !- Demand Limit Scheme Purchased Electric Demand Limit {W}
-       ,                               !- Track Schedule Name Scheme Schedule Name
-       ,                               !- Track Meter Scheme Meter Name
-       AlternatingCurrent,             !- Electrical Buss Type
-       ,                               !- Inverter Object Name
-       ;                               !- Electrical Storage Object Name
-
-
-   ElectricLoadCenter:Distribution,
-       Electric Load Center,       !- Name
-       Backup Generators,             !- Generator List Name
-       DemandLimit,                         !- Generator Operation Scheme Type
-       10000.0,                                 !- Demand Limit Scheme Purchased Electric Demand Limit {W}
-       ,                                               !- Track Schedule Name Scheme Schedule Name
-       ,                                               !- Track Meter Scheme Meter Name
-       AlternatingCurrent,           !- Electrical Buss Type
-       ,                                               !- Inverter Object Name
-       ;                                               !- Electrical Storage Object Name
-```
-
-### ElectricLoadCenter:Distribution Outputs
-
-There are three levels of results reporting related to electric load centers and generators.   The top level of reporting provides results across the whole building and all the different electric load centers and generators.   The second level of reporting provides results for individual load centers.   The third level is for each type of generator (see individual generator descriptions).   This section discusses the first two levels.
-
-Even if no ElectricLoadCenter:Distribution object is included, the following whole-building summary output variables are also available for all simulations that have any electricity consuming equipment.  
-
-* HVAC,Average,Facility Total Purchased Electric Power [W]
-* HVAC,Sum,Facility Total Purchased Electric Energy [J]
-* HVAC,Average,Facility Total Surplus Electric Power [W]
-* HVAC,Sum,Facility Total Surplus Electric Energy [J]
-* HVAC,Average,Facility Net Purchased Electric Power [W]
-* HVAC,Sum,Facility Net Purchased Electric Energy [J]
-* HVAC,Average,Facility Total Building Electric Demand Power [W]
-* HVAC,Average,Facility Total HVAC Electric Demand Power [W]
-* HVAC,Average,Facility Total Electric Demand Power [W]
-* HVAC,Average,Facility Total Produced Electric Power [W]
-* HVAC,Sum,Facility Total Produced Electric Energy [J]
-
-These output variables all use a default keyword    Whole Building.   
-
-#### Facility Total Purchased Electric Power [W]
-#### Facility Total Purchased Electric Energy [J]
- 
-These outputs are the total of electricity purchased for the entire facility in both power and energy units. This value is always positive and indicates the amount of energy that is purchased from the utility.
-
-#### Facility Total Surplus Electric Power [W]
-#### Facility Total Surplus Electric Energy [J]
-
-These outputs are the total excess electricity exported and sent out to the electrical grid in both power and energy units. This value is always positive and indicates the surplus electric power (from generation and/or storage discharge) exceeds the whole-building demand and electricity is being fed from the facility into the grid.
-
-#### Facility Net Purchased Electric Power [W]
-#### Facility Net Purchased Electric Energy [J]
-
-These outputs are the net electricity purchased in both Power and Energy units. This value can be either positive or negative. Positive values are defined as electricity purchased from the utility. Negative values are defined as surplus electricity fed back into the grid.
-
-#### Facility Total Building Electric Demand Power [W]
-
-This output variable includes all of the electric demand from the building (non-HVAC) portion of the simulation, which would contain lights, electrical equipment, exterior lights and equipment, etc.
-
-#### Facility Total HVAC Electric Demand Power [W]
-
-This output variable includes all of the electric demand from the HVAC portion of the simulation, which would contain fans, electric coils, pumps, chillers, cooling towers, etc.
-
-#### Facility Total Electric Demand Power [W]
-
-This is the total of the whole Building and HVAC electric demands.
-
-#### Facility Total Produced Electric Power [W]
-#### Facility Total Produced Electric Energy [J]
-
-These outputs are the total generator and photovoltaic electricity produced on-site for the entire model, and they are in both Power and Energy units.  When the electric power production system includes power conversion devices including DC to AC inverters, AC to DC converters, or transformers, the power conversion losses are included as negative values in these reports. When electrical storage is used with on-site production, the electricity put into storage is decremented from production and the electricity removed storage is added to production.   This means that losses from a round trip through electrical storage decrease on-site electricity production.
-
-
-Each ElectricLoadCenter also collects results from the individual generators that are connected to that load center.  The keywords for these reports are the unique names of ElectricLoadCenter:Distribution objects.  The output variables available at the ElectricLoadCenter level are:
-
-* HVAC,Average,Electric Load Center Produced Electric Power [W]
-* HVAC,Sum,Electric Load Center Produced Electric Energy [J]
-* HVAC,Average,Electric Load Center Supplied Electric Power [W]
-* HVAC,Average,Electric Load Center Drawn Electric Power [W]
-* HVAC,Average,Electric Load Center Produced Thermal Rate [W]
-* HVAC,Sum,Electric Load Center Produced Thermal Energy [J]
-* HVAC,Average,Electric Load Center Requested Electric Power [W]
-
-
-#### Electric Load Center Produced Electric Power [W]
-
-#### Electric Load Center Produced Electric Energy [J]
-
-These outputs are the sum of electrical energy and power produced by the generators attached to a particular load center.  This could be DC or AC depending on the type of buss.  The power actually delivered by the load center may be adjusted by power conversion losses from an inverter or transformer or by interaction with the any electrical storage. 
-
-#### Electric Load Center Supplied Electric Power [W]
-
-This output is the power fed from the electric load center into the main distribution panel, in Watts.  This power is generated or discharged by on site equipment and has been adjusted to account for any power conversion by an inverter and/or transformer on the load center. 
-
-#### Electric Load Center Drawn Electric Power [W]
-
-This output is the power fed from the main distribution panel into the load center, in Watts.  This power draw is typically only for charging storage with power from either the grid or another load center. 
-
-#### Electric Load Center Produced Thermal Rate [W]
-
-#### Electric Load Center Produced Thermal Energy [J]
-
-These outputs are the sum of the thermal energy and power produced by the generators attached to a particular load center.   The keywords for these reports are the unique names of ElectricLoadCenter:Distribution objects.
-
-#### Electric Load Center Requested Electric Power [W]
-
-This output variable is the average electric power supply (in watts) requested of the load center by the facility's main distribution panel, for the time step being reported.  This is used by the load center generator and storage operation control logic when determining how to run the generators and/or storage devices.  For the baseload generator operating scheme, this output variable should equal the sum of the power supply requests for the available generators associated with this load center (ref. ElectricLoadCenter:Generators). In other cases, this output could be different from the sum of the power supply requests for the generators associated with this load center. For example, a generator might be requested to provide a certain amount of power but can only provide a fraction of the requested amount. In this case the load center will detect this shortfall and include it when calculating the power request for the next available generator. Therefore, the sum of the power supply requests for the individual generators associated with this load center (ref. ElectricLoadCenter:Generators) could be greater than the Electric Load Center Requested Electric Power output variable.
-
-
-### ElectricLoadCenter:Generators
-
-The ElectricLoadCenter:Generators object is used to provide a list of the generators to include in the simulation. The list includes the names and types of all the generators along with separate availability schedules, the rated power output, and thermal-to-electrical power ratio for each. Sets of five input fields are repeated for each generator. If more than 30 generators are needed, EnergyPlus will    auto-extend    to suit the needs but other interfaces (such as the IDF Editor may not). The user can always modify the Energy+.idd file to accommodate the extra fields necessary, but it is likely the next release of EnergyPlus will overwrite any user modifications.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the generators in the set.
-
-#### FieldSet: Name, Object Type, Rated Power Output, Availability, Thermal Ratio up to 30
-
-Each generator is specified by a set of 5 input fields that contain an identifying name, a keyword that indicates the type of generator, the rated output of the generator, the availability schedule of the generator, and the thermal to electrical power production ratio.
-
-#### Field: Generator &lt;x&gt; Name
-
-This alpha field contains the identifying name for the first generator in the list.
-
-#### Field: Generator &lt;x&gt; Object Type
-
-This alpha field contains the keyword for the type of generator.   The available types include:
-
-- Generator:InternalCombustionEngine
-
-- Generator:CombustionTurbine
-
-- Generator:Photovoltaic
-
-- Generator:FuelCell
-
-- Generator:MicroCHP
-
-- Generator:MicroTurbine
-
-- Generator:WindTurbine
-
-These keywords are the names of the input objects for the type of generator.
-
-#### Field: Generator &lt;x&gt; Rated Electric Power Output
-
-This numeric field contains the nominal electric power output to be requested from generator 1. It is normally equal to the rated power output of the generator in Watts. This value is used only for supervisory control and generator dispatch; the actual power output for each time step is determined by the generator models. This value affects how much a generator is loaded (i.e., requested electric power output) and can also impact the operation of an electric storage unit (e.g., LoadCenter:Storage:Simple) if one is connected to the associated load distribution center (ref. ElectricLoadCenter:Distribution). Refer to Electrical Storage in the EnergyPlus Engineering Reference for more details regarding this input field and its relationship with electric storage.
-
-#### Field: Generator &lt;x&gt; Availability Schedule Name
-
-This alpha field is used as an identifying field for the generator availability schedule. If not blank, this field must contain the name of a schedule defined elsewhere in the input file.   A schedule value of &lt;=0.0 indicates the generator is not available, while a schedule value &gt; 0.0 indicates that the generator is available to operate. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Generator &lt;x&gt; Rated Thermal to Electrical Power Ratio
-
-This numeric field contains the ratio of the rated thermal output to the rated electric output.   It is required and used if the operation scheme is set to **FollowThermal** or **FollowThermalLimitElectrical**.   This nominal ratio is only used for control and dispatch decisions.   This value should be generally consistent with the more detailed performance input for the individual generator component models but it is not used in those component models.
-
-An example IDF showing how this object is used is provided below:
-
-```idf
-   ElectricLoadCenter:Generators,
-       Backup Generators,             !- Name
-       Cat Diesel,                           !- Generator 1 Name
-       Generator:InternalCombustionEngine,   !- Generator 1 Object Type
-       50000,                                     !- Generator 1 Rated Electric Power Output
-       ON PEAK GENERATOR SCHEDULE,   !- Generator 1 Availability Schedule Name
-       ,                                               !- Generator 1 Rated Thermal to Electrical Power Ratio
-       Solar Turbine,                     !- Generator 2 Name
-       Generator:CombustionTurbine,   !- Generator 2 Object Type
-       30000,                                     !- Generator 2 Rated Electric Power Output
-       OFF PEAK GENERATOR SCHEDULE,   !- Generator 2 Availability Schedule Name
-       ,                                               !- Generator 2 Rated Thermal to Electrical Power Ratio
-       Capstone C65,                       !- Generator 3 Name
-       Generator:Microturbine,   !- Generator 3 Object Type
-       65000,                                     !- Generator 3 Rated Electric Power Output
-       MID PEAK GENERATOR SCHEDULE,   !- Generator 3 Availability Schedule Name
-       ;                                               !- Generator 3 Rated Thermal to Electrical Power Ratio
-```
-
-### ElectricLoadCenter:Generators Outputs
-
-A single output variable is available for each generator specified via this object as described below:
-
-* HVAC,Average,Generator Requested Electric Power [W]
-
-#### Generator Requested Electric Power [W]
-
-This output variable represents the average electric power supply in Watts that is being requested by the generator operation scheme from a specific generator for the time step being reported. In some instances the output value may be the Rated Electric Power Output specified for the generator in the ElectricLoadCenter:Generators object. If the generator is not available for a simulation time step (as indicated by its availability schedule), then the power supply request will be zero. The power supply request may be less than the rated electric power output if the overall electric power reduction target has already been met, partially or completely, by electric power produced by other generators. If an EnergyPlus Energy Management System is used to specify an electric power supply request for this generator, then that EMS request will be reflected in this output variable.
-
-### ElectricLoadCenter:Inverter:Simple
-
-This input object is used to model conversion from Direct Current (DC) to Alternating Current (AC) in an electric load center that contains photovoltaic modules.   Such a load center has an array of photovoltaic modules that feed an inverter DC power and the inverter produces AC power.   This input object is for the simplest inverter model and uses a fixed efficiency.   There are two other types of inverters with more complex models described below.
-
-#### Field: Name
-
-This field contains a unique name for the inverter.   The name entered must also be unique across all other types of inverters that may also be in the input file.
-
-#### Field: Availability Schedule Name
-
-This field contains the name of a schedule that describes when the inverter is available.   If the inverter is scheduled to not be available, by scheduling a value of 0, then it cannot produce AC power and will not consume ancillary power during standby.   Any non-zero schedule value means the inverter is available to produce AC power and consume ancillary power during standby.   If the Inverter is scheduled to be unavailable but it is being supplied with DC power anyway, then the energy is dissipated as heat. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Zone Name
-
-This field contains the name of the thermal zone where the inverter is located.   Entering a valid name of zone here will direct EnergyPlus to include the inverter   s losses as heat gains to the named thermal zone.   If the inverter is not within a thermal zone, then this field can be left blank (and the thermal energy associated with inverter losses is removed from the building model).
-
-#### Field: Radiative Fraction
-
-This field contains the fraction of inverter thermal losses that enter the zone as long-wave thermal radiation.   This should be a factor between 0.0 and 1.0.   The balance of the losses is convective.   This field is not used if the previous field for zone name is left blank.
-
-#### Field: Inverter Efficiency
-
-This field contains the value for inverter efficiency.   In the simple model, efficiency is a constant.   This is the so-called 1-term model.   Input data for different types of inverters is available at http://www.gosolarcalifornia.org/equipment/inverter_tests/summaries where the    CEC Efficiency    would be the value to enter here.
-
-An example IDF showing how this object is used is provided below:
-
-```idf
-   ElectricLoadCenter:Inverter:Simple,
-       Simple Ideal Inverter,     !- Name
-       Always On,                             !- Availability Schedule Name
-       ,                                               !- Zone Name
-       0.0,                                         !- Radiative Fraction
-       1.0;                                         !- Inverter Efficiency
-```
-
-### ElectricLoadCenter:Inverter:FunctionOfPower
-
-This input object is used to model conversion from Direct Current (DC) to Alternating Current (AC) in an electric load center that contains photovoltaic modules.   Such a load center has an array of photovoltaic modules that feed an inverter DC power and the inverter produces AC power.   This input object is for an inverter model where efficiency is a function of normalized power.
-
-#### Field: Name
-
-This field contains a unique name for the inverter.   The name entered must also be unique across all other types of inverters that may also be in the input file.
-
-#### Field: Availability Schedule Name
-
-This field contains the name of a schedule that describes when the inverter is available.   If the inverter is scheduled to not be available, by scheduling a value of 0, then it cannot produce AC power, nor contribute heat gains to the zone, and will not consume ancillary power during standby.   Any non-zero schedule value means the inverter is available to produce AC power, contribute heat gains to the zone and consume ancillary power during standby. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Zone Name
-
-This field contains the name of the thermal zone where the inverter is located.   Entering a valid name of zone here will direct EnergyPlus to include the inverter   s losses as heat gains to the named thermal zone.   If the inverter is not within a thermal zone, then this field can be left blank (and the thermal energy associated with inverter losses is removed from the building model).
-
-#### Field: Radiative Fraction
-
-This field contains the fraction of inverter thermal losses that enter the zone as long-wave thermal radiation.   This should be a factor between 0.0 and 1.0.   The balance of the losses is convective.   This field is not used if the previous field for zone name is left blank.
-
-#### Field: Efficiency Function of Power Curve Name
-
-This field contains the name of curve representing the relationship between DC power input into the inverter and the efficiency with which that power is converted to AC.   The curve can be either a Curve:Linear, Curve:Quadratic, or Curve:Cubic.   The curve   s    x    value is DC power input normalized by the following field.   The result of the curve should be power conversion efficiency expressed as a fraction between 0.0 and 1.0.
-
-#### Field: Rated Maximum Continuous Input Power
-
-This field contains the rated power input in watts.   This is value used to normalize input power for use with the curve named in the previous field.   This is DC power from the PV arrays going into the inverter.
-
-#### Field: Minimum Efficiency
-
-This field contains a minimum bound on the inverter efficiency.   This value will be used as a limit on the curve   s result.
-
-#### Field: Maximum Efficiency
-
-This field contains a maximum bound on the inverter efficiency.   This value will be used as a limit on the curve   s result.
-
-#### Field: Minimum Power Output
-
-This field contains a lower limit on the AC power produced by the inverter.   If the resulting power output would be below this level, then the inverter is assumed to not produce any power and is in stand by mode.   All DC power input is lost (unless it is going into storage).
-
-#### Field: Maximum Power
-
-This field contains an upper limit on the AC power produced by the inverter.   If the resulting power output would be above this level, then the power produced is capped at this level with the rest of input power converted to losses (unless it is going into storage).
-
-#### Field: Ancillary Power Consumed In Standby
-
-This field contains the ancillary power in watts used by the inverter when not producing AC power.   This is AC electricity consumed in standby mode.   Standby mode occurs when the inverter is scheduled to be available but the incoming DC power is too low.
-
-An example IDF showing how this object is used is provided below:
-
-```idf
-   ElectricLoadCenter:Inverter:FunctionOfPower,
-       Curve Inverter,                   !- Name
-       ALWAYS_ON,                             !- Availability Schedule Name
-       ,                                               !- Zone Name
-       0.3,                                         !- Radiative Fraction
-       Inverter Curve,                   !- Efficiency Function of Power Curve Name
-       15000,                                     !- Rated Maximum Continuous Input Power {W}
-       0.0,                                         !- Minimum Efficiency
-       1.0,                                         !- Maximum Efficiency
-       200,                                         !- Minimum Power Output {W}
-       20000,                                     !- Maximum Power Output {W}
-       0.0;                                         !- Ancillary Power Consumed In Standby {W}
-```
-
-### ElectricLoadCenter:Inverter:LookUpTable
-
-This input object is used to model conversion from Direct Current (DC) to Alternating Current (AC) in an electric load center that contains photovoltaic modules.   Such a load center has an array of photovoltaic modules that feed an inverter DC power and the inverter produces AC power.   This input object is for an inverter model where efficiency is interpolated using a look up table.
-
-This object was designed for use with data contained in the Inverter Performance Test Summaries available at http://www.gosolarcalifornia.org/equipment/inverter_tests/summaries.   All of the data needed for this object can be found there by make and model of inverter.   The core of the data set is a 3x6 matrix of efficiency at different voltage and power levels.   These form the look up table used in the model.   Note that EnergyPlus    PV models currently model only power and not the voltage and current situation.   Therefore, only the nominal voltage data are used.   This is the middle row of data in the Go Solar summaries.
-
-#### Field: Name
-
-This field contains a unique name for the inverter.   The name entered must also be unique across all other types of inverters that may also be in the input file.
-
-#### Field: Availability Schedule Name
-
-This field contains the name of a schedule that describes when the inverter is available.   If the inverter is scheduled to not be available, by setting a value of 0, then it cannot produce AC power, nor contribute heat gains to the zone, and will not consume ancillary power during standby.   Any non-zero schedule value means the inverter is available to produce AC power, contribute heat gains to the zone and consume ancillary power during standby. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Zone Name
-
-This field contains the name of the thermal zone where the inverter is located.   Entering a valid name of zone here will direct EnergyPlus to include the inverter   s losses as heat gains to the named thermal zone.   If the inverter is not within a thermal zone, then this field can be left blank (and the thermal energy associated with inverter losses is removed from the building model).
-
-#### Field: Radiative Fraction
-
-This field contains the fraction of inverter thermal losses that enter the zone as long-wave thermal radiation.   This should be a factor between 0.0 and 1.0.   The balance of the losses is convective.   This field is not used if the previous field for zone name is left blank.
-
-#### Field: Rated Maximum Continuous Output Power
-
-This field contains the rated maximum continuous output power in watts.
-
-#### Field: Night Tare Loss Power
-
-This field contains the    night tare loss    in watts.   This is modeled as ancillary power consumed during standby.
-
-#### Field: Nominal Voltage Input
-
-This field contains the nominal DC input voltage in volts.   This is    Vnom    in the Go Solar test summaries.
-
-#### Field: Efficiency at 10% Power and Nominal Voltage
-
-This field contains the fractional efficiency at nominal voltage and 10% power.
-
-#### Field: Efficiency at 20% Power and Nominal Voltage
-
-This field contains the fractional efficiency at nominal voltage and 20% power.
-
-#### Field: Efficiency at 30% Power and Nominal Voltage
-
-This field contains the fractional efficiency at nominal voltage and 30% power.
-
-#### Field: Efficiency at 50% Power and Nominal Voltage
-
-This field contains the fractional efficiency at nominal voltage and 50% power.
-
-#### Field: Efficiency at 75% Power and Nominal Voltage
-
-This field contains the fractional efficiency at nominal voltage and 75% power.
-
-#### Field: Efficiency at 100% Power and Nominal Voltage
-
-This field contains the fractional efficiency at nominal voltage and 100% power.
-
-An example IDF showing how this object is used is provided below:
-
-```idf
-   ElectricLoadCenter:Inverter:LookUpTable,
-       PV Inverter,                         !- Name
-       ALWAYS_ON,                             !- Availability Schedule Name
-       ,                                               !- Zone Name
-       0.25,                                       !- Radiative Fraction
-       14000,                                     !- Rated Maximum Continuous Output Power {W}
-       200.0,                                     !- Night Tare Loss Power {W}
-       368,                                         !- Nominal Voltage Input {V}
-       0.839,                                     !- Efficiency at 10% Power and Nominal Voltage
-       0.897,                                     !- Efficiency at 20% Power and Nominal Voltage
-       0.916,                                     !- Efficiency at 30% Power and Nominal Voltage
-       0.931,                                     !- Efficiency at 50% Power and Nominal Voltage
-       0.934,                                     !- Efficiency at 75% Power and Nominal Voltage
-       0.930;                                     !- Efficiency at 100% Power and Nominal Voltage
-```
-
-### Electric Load Center Inverter Outputs
-
-Each inverter can report the following seven output variables.
-
-* HVAC,Average,Inverter DC to AC Efficiency []
-* HVAC,Average,Inverter DC Input Electric Power [W]
-* HVAC,Sum,Inverter DC Input Electric Energy [J]
-* HVAC,Average,Inverter AC Output Electric Power [W]
-* HVAC,Sum,Inverter AC Output Electric Energy [J]
-* HVAC,Average,Inverter Conversion Loss Power [W]
-* HVAC,Sum,Inverter Conversion Loss Energy [J]
-* HVAC,Sum,Inverter Conversion Loss Decrement Energy [J]
-* HVAC,Average,Inverter Thermal Loss Rate [W]
-* HVAC,Sum,Inverter Thermal Loss Energy [J]
-* HVAC,Average,Inverter Ancillary AC Electric Power [W]
-* HVAC,Sum,Inverter Ancillary AC Electric Energy [J]
-
-#### Inverter DC to AC Efficiency [ ]
-
-This is the efficiency with which DC power is converted to AC power by the inverter.
-
-#### Inverter DC Input Elecric Power [W]
-#### Inverter DC Input Electric Energy [J]
-
-These outputs are total electricity power or energy fed into the inverter.  This is Direct Current from photovoltaics (or DC-based electrical storage) going into the inverter.
-
-#### Inverter AC Output Electric Power [W]
-#### Inverter AC Output Electric Energy [J]
-
-These outputs are the total electricity power or energy produced by the inverter.   This is Alternating Current going out of the inverter.
-
-#### Inverter Conversion Loss Power [W]
-#### Inverter Conversion Loss Energy [J]
-#### Inverter Conversion Loss Decrement Energy [J]
-
-These outputs are the thermal power or energy losses in the inverter that stem from converting from DC to AC.  The decrement energy is negative and is metered as "PowerConversion" on the "ElectricityProduced" resource.
-
-#### Inverter Thermal Loss Rate [W]
-#### Inverter Thermal Loss Energy [J]
-
-These outputs are the thermal power or energy losses in the inverter that stem from converting from DC to AC plus any ancillary electric power. 
-
-#### Inverter Ancillary AC Electric Power [W]
-#### Inverter Ancillary AC Electric Energy [J]
-
-These outputs are the Alternating Current electricity consumed by the inverter.   These are ancillary, or night tare loss, power uses by the inverter and modeled as if powered by the building   s grid connection.   These ancillary power draws generally occur when the inverter is not generating power but waiting in a standby mode ready to begin generating power.
-
-
-###  ElectricLoadCenter:Storage:Converter
-
-This model is for converting AC to DC for grid-supplied charging of DC storage.  The model is only for power conversion and does not consider voltage. There are two methods available for determining the efficiency with which power is converted.  The efficiency is defined as the ratio of DC power output divided by AC power input.  If the name of a zone is entered the power conversion losses will be added to the zone as internal heat gains.  The converter is part of a single electric load center.
-
-#### Field: Name
-
-This field contains a unique name for the AC to DC converter.  This name will be referenced in an ElectricLoadCenter:Distribution object. 
-
-#### Field: Availability Schedule Name
-
-This field contains the name of a schedule that describes when the power converter is available. If power conversion is not available then electric power from the grid cannot be used to charge storage. Any non-zero value means the converter is available. If this field is blank, the schedule has a value of 1 for all time periods and the converter is always available. Standby power consumption is on when converter is available and off when the converter is not available. 
-
-#### Field: Power Conversion Efficiency Method
-
-This choice field is used to select which method is used to define the efficiency with which power is converted from AC to DC.  There are two options: SimpleFixed or FunctionOfPower.
-- SimpleFixed indicates that power conversion efficiency is a constant with the value set in the next field. There is no need to size the converter (with a value in the field called Design Maximum Continuous Input Power) and varying levels of power do not affect the efficiency. SimpleFixed is the default. 
-- FunctionOfPower indicates that the power conversion efficiency is a function of the level of power being converted. This method is intended to model the characteristic that converters tend to operate less efficiently when loaded well below their design size. The converter must be sized with a value in the Design Maximum Continuous Input Power and the functional relationship described in a performance curve or look-up table. 
-
-#### Field: Simple Fixed Efficiency
-
-This numeric field is used to set a constant efficiency for conversion of AC to DC at all power levels. This field is only used, and is required, when the Power Conversion Efficiency Method is set to SimpleFixed. The value must be greater than 0.0 and less than equal to 1.0.  The default is 0.95. 
- 
-#### Field: Design Maximum Continuous Input Power
-
-This numeric field describes the size of the power converter in terms of its design input power level, in Watts.  This is the AC power going into the converter.  This field is only used, and is required, when the the Power Conversion Efficiency Method is set to FunctionOfPower.  This input serves as an upper limit for the AC power input and is used to normalize power for use in the performance curve or table.  The AC power being converted at any given time is divided by the value in this field.  
-
-#### Field: Efficiency Function of Power Curve Name
-
-This field is the name of a performance curve or table object that describes how efficiency varies as a function of normalized power.  The single independent "x" variable input for the curve or table is the ratio of AC input power at a given time divided by design power in the previous field.  The result of the curve should be the power conversion efficiency for that normalized power so that DC power output is the product of efficiency multiplied by the AC power input.  Any of the single-variable performance curves or lookup table objects can be used to describe performance. This field is only used, and is required, when the the Power Conversion Efficiency Method is set to FunctionOfPower. 
-
-#### Field: Ancillary Power Consumed In Standby
-
-This numeric field describes the ancillary power consumed by the converter when it is available but not converting power, in Watts.  This field is optional and can be used with any of the efficiency methods. If this converter is really on mode of a bidirectional inverter, take care not to double count the ancillary consumption by including them in both this component and the inverter component. 
-
-#### Field: Zone Name
-
-This field is the name of thermal zone where the converter is located.  If this field is omitted then the converter is considered outdoors.  The power lost during the conversion process is treated as heat gains and added the thermal zone named in this field.  The split between radiation and convection can be controlled in the next input field. 
-
- #### Field: Radiative Fraction
- 
-This numeric field is the fraction of zone heat gains that are handled as infrared thermal radiation.  This field is only used if a zone is named in the previous field.  The portion of zone gains that are not radiative are added to the zone as convection. If a zone is named and this field left blank or omitted then all the zone heat gains will be convective. 
-
-An example IDF showing how this object is used is provided below:
-
-   ElectricLoadCenter:Storage:Converter,
-       Grid Charge Converter ,   !- Name
-       ALWAYS_ON ,               !- Availability Schedule Name
-       SimpleFixed ,             !- Power Conversion Efficiency Method
-       0.95 ,                    !- Simple Fixed Efficiency
-       ,                         !- Design Maximum Continuous Input Power
-       ,                         !- Efficiency Function of Power Curve Name
-       20 ,                      !- Ancillary Power Consumed In Standby
-        ,                         !- Zone Name
-       0.25;                     !- Radiative Fraction
-
-### Electric Load Center Converter Outputs
-
-Each converter can report the following output variables
-
-* HVAC,Average,Converter AC to DC Efficiency []
-* HVAC,Average,Converter AC Input Electric Power [W]
-* HVAC,Sum,Converter AC Input Electric Energy [J]
-* HVAC,Average,Converter DC Output Electric Power [W]
-* HVAC,Sum,Converter DC Output Electric Energy [J]
-* HVAC,Average,Converter Electric Loss Power [W]
-* HVAC,Sum,Converter Electric Loss Energy [J]
-* HVAC,Sum,Converter Electric Loss Decrement Energy [J]
-* HVAC,Average,Converter Thermal Loss Rate [W]
-* HVAC,Sum,Converter Thermal Loss Energy [J]
-* HVAC,Average,Converter Ancillary AC Electric Power [W]
-* HVAC,Sum,Converter Ancillary AC Electric Energy [J]
-
-#### Converter AC to DC Efficiency []
-
-This is the efficiency with which AC power is converted to DC power by the converter
-
-#### Converter AC Input Electric Power [W]
-#### Converter AC Input Electric Energy [J]
-
-These outputs are the total electric power or energy fed into the converter.  This is Alternating Current, or AC, drawn from the main panel into the load center. 
-
-#### Converter DC Output Electric Power [W]
-#### Converter DC Output Electric Energy [J]
-
-These outputs are the total electric power or energy leaving the converter.  This is Direct Current, or DC, that will go into charging storage. 
-
-#### Converter Electric Loss Power [W]
-#### Converter Electric Loss Energy [J]
-#### Converter Electric Loss Decrement Energy [J]
-
-These outputs are the conversion losses that result from inefficiencies in the conversion from AC to DC.  The power and energy are positive while the decrement energy is negative and is metered on the "PowerConversion" end use for "ElectricityProduced".  
-
-#### Converter Thermal Loss Rate [W]
-#### Converter Thermal Loss Energy [J]
-
-These outputs are the power and energy losses that result from the inefficiencies in the conversion from AC to DC and the ancillary standby power. 
-
-#### Converter Ancillary AC Electric Power [W]
-#### Converter Ancillary AC Electric Energy [J]
-
-These outputs are the power and energy consumed in standby operation when the converter is not being used but is available and ready to be used. The ancillary power consumption is metered on the "Cogeneration" end use for "Electricity."
-
-
-### ElectricLoadCenter:Storage:Simple
-
-This input object is used to model storage of electricity in an electric load center.   This is a simple model that does not attempt to represent any of the characteristics of a real storage device such as a battery.   The type of power, AC or DC, depends on the configuration chosen as the Electrical Buss Type in the ElectricLoadCenter:Distribution object.
-
-#### Field: Name
-
-This field contains a unique name for the electric storage device.
-
-#### Field: Availability Schedule Name
-
-This field contains the name of a schedule that describes when the storage device is available.   If storage is not available, by scheduling a value of 0, then no electrical energy can be stored or drawn from the device.   Any non-zero schedule value means the devices is available. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Zone Name
-
-This field contains the name of the thermal zone where the storage device is located.   Entering a valid name of a zone here will direct EnergyPlus to include the storage losses as heat gains to the name thermal zone.   If the storage is not within a therma zone, then this field can be left blank.
-
-#### Field: Radiative Fraction for Zone Heat Gains
-
-This field contains the fraction of storage losses that enter the zone as long-wave thermal radiation.   This should be a factor between 0.0 and 1.0.   The balance of the losses are convective.   This field is not used if the previous field for zone name is left blank.
-
-#### Field: Nominal Energetic Efficiency for Charging
-
-This field contains the charging efficiency.   This is the energetic efficiency of storing electrical energy in the storage device.   A value of 1.0 means the device does not lose any energy when charging.
-
-#### Field: Nominal Discharging Energetic Efficiency
-
-This field contains the discharging efficiency.     This is the energetic efficiency of drawing electrical energy from the storage device.   A value of 1.0 means the device does not lose any energy when drawing power.
-
-#### Field: Maximum Storage Capacity
-
-This field describes the maximum amount of energy that can be stored in the device in Joules.   Once the storage device is full, no additional energy can be stored in it.
-
-#### Field: Maximum Power for Discharging
-
-This field describes the maximum rate at which electrical power can be discharged from the storage device in watts.
-
-#### Field: Maximum Power for Charging
-
-This field describes the maximum rate at which electrical power can be stored in the device in watts.
-
-#### Field: Initial State of Charge
-
-This field describes the value for the initial state of charge in Joules.   This is used to model the storage device as having some amount of stored energy at the beginning of the simulation period.
-
-An example IDF showing how this object is used is provided below:
-
-```idf
-   ElectricLoadCenter:Storage:Simple,
-       Battery,                                 !- Name
-       ALWAYS_ON,                             !- Availability Schedule Name
-       ,                                               !- Zone Name
-       0.0,                                         !- Radiative Fraction for Zone Heat Gains
-       0.7,                                         !- Nominal Energetic Efficiency for Charging
-       0.7,                                         !- Nominal Discharging Energetic Efficiency
-       1.0E11,                                   !- Maximum Storage Capacity {J}
-       50000,                                     !- Maximum Power for Discharging {W}
-       25000,                                     !- Maximum Power for Charging {W}
-       1.0E10;                                   !- Initial State of Charge {J}
-```
-
-### ElectricLoadCenter:Storage:Simple Outputs
-
-Each electrical storage device can report the following seven output variables.
-
-* HVAC,Average,Electric Storage Simple Charge State [J]
-
-* HVAC,Average,Electric Storage Charge Power [W]
-
-* HVAC,Sum,Electric Storage Charge Energy [J]
-
-* HVAC,Average,Electric Storage Discharge Power [W]
-
-* HVAC,Sum,Electric Storage Discharge Energy [J]
-
-* HVAC,Average,Electric Storage Thermal Loss Rate [W]
-
-* HVAC,Sum,Electric Storage Thermal Loss Energy [J]
-
-* HVAC,Sum,Electric Storage Production Decrement Energy [J]
-
-#### Electric Storage Simple Charge State [J]
-
-This output is the state of charge of the storage device.  State of charge is the amount of electrical energy stored in the device at a point of time.  The amount of energy stored in tracked in Joules.
-
-#### Electric Storage Charge Power [W]
-
-#### Electric Storage Charge Energy [J]
-
-These outputs are total electricity power or energy fed into the storage device.   This is the rate or amount of charging.
-
-#### Electric Storage Production Decrement Energy [J]
-
-This output is the total electricity energy decremented from electricity production because it has fed into the storage device.   This output has the opposite sign of    Electric Storage Charge Energy    but is otherwise similar.   This decrement output variable is also a meter associated with the resource type    ElectricityProduced    that reduces the metered electricity production to account for power that went into storage after production.
-
-#### Electric Storage Discharge Power [W]
-
-#### Electric Storage Discharge Energy [J]
-
-These outputs are total electricity power or energy drawn from the storage device.   This is the rate or amount of discharging.   The energy from storage output variable is also a meter associated with the resource type    ElectricityProduced    that increases the metered electricity production to account for power that has come back out of storage.
-
-#### Electric Storage Thermal Loss Rate [W]
-
-#### Electric Storage Thermal Loss Energy [J]
-
-These outputs are the thermal power or energy losses from both charging and drawing electrical power in or out of the storage device.   These losses are the result of inefficiencies in charging and drawing.
-
-### ElectricLoadCenter:Storage: Battery
-
-This object uses the kinetic battery model (KiBaM) to simulate rechargeable battery banks in an electrical load center. The battery bank is a collection of one or more individual battery modules. Given the surplus or deficit power from the electrical system and the state of charge from the previous time step, this object can model the voltage, current, and energy losses with charging and discharging during each time step. The cumulative battery damage can be also modeled and reported at the end of each simulation run.
-
-This object allows the simulation of both lead-acid and Nickel Cadmium batteries. With input parameters derived from specific battery tests, the object is expected to support other battery types such as Lithium-ion batteries.
-
-The kinetic battery model assumes that part of the battery   s energy storage capacity is immediately available in discharging or charging while the rest is chemically bound. As a function of constant current, the battery capacity is related to three parameters: the maximum capacity at infinitesimal current, the capacity ratio of available charges, and the conversion ratio between available charges and bound charges. These parameters are usually obtained via curve fitting based on battery data sheets or test data.
-
-Each individual battery module is modeled as a voltage source in series with an electrical resistance.   KiBaM assumes that the internal resistance is constant and the open circuit voltage varies with the electric current, the state of charge and the operation mode (charging or discharging). For an individual battery module, the open circuit voltage at any time is correlated to the voltage at fully charged/discharged state and three other regression coefficients.   These regression coefficients are usually obtained via curve fitting based on battery test data.
-
-The object offers user the option to perform battery life calculation. If battery life is modeled, the user needs to provide a group of coefficients for the correlation between the number of cycles for battery failure and the corresponding cycle range. More detailed information can be found from the Engineering Reference.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the battery bank.
-
-#### Field: Availability Schedule Name
-
-This alpha field contains the schedule name (ref. Schedule objects) that describes when the battery is available. A schedule value greater than 0 (usually 1 is used) indicates that electrical energy can be stored or drawn from the battery. A value less than or equal to 0 (usually 0 is used) denotes that the battery is not available. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Zone Name
-
-This field contains the name of the thermal zone where the battery is located. Entering a valid name of zone here will direct EnergyPlus to include the energy storage losses as heat gains to the named thermal zone. If the battery is not within a thermal zone, this field can be left blank and the thermal energy associated with storage losses is removed from the building model.
-
-#### Field: Radiative Fraction
-
-This field contains the fraction of storage losses that enter the zone as long-wave thermal radiation. This numeric filed should have a value between 0.0 and 1.0. The balance of the losses is convective. This field is not used if the previous field for zone name is left blank.
-
-#### Field: Number of Battery Modules in Parallel
-
-This field defines the number of modules connected in parallel in the battery bank.
-
-#### Field: Number of Battery Modules in Series
-
-This field defines the number of modules connected in series in the battery bank. The total number of modules in a battery bank is equal to the number of modules in parallel times the number of modules in series.
-
-#### Field: Maximum Module Capacity
-
-This field indicates the maximum capacity of one battery module. It is evaluated as the total Amp-hours available when a full battery is discharged at infinitesimal current. This capacity is for an individual battery module, not for the whole battery bank. The maximum capacity can be found from manufacture   s data or derived from test data by curve fitting.
-
-#### Field: Initial Fractional State of Charge
-
-This field describes the initial state of charge in terms of the fraction of maximum capacity as defined in the previous field.
-
-#### Field: Fraction of Available Charge Capacity
-
-The kinetic battery model assumes that battery is a two-tank electrical energy storage device: an available tank and a bound tank. The available tank can be immediately charged or discharged, while the bound tank can only be charged or discharged via the available tank. This field specifies the fraction of total charge in the battery that is part of the available tank. The ratio of available charge capacity to total capacity is a parameter usually derived from test data by curve fitting.
-
-#### Field: Change Rate from Bound Charge to Available Charge
-
-This field specifies the rate at which the charge flows between the available tank and the bound tank. It is a parameter used to calculate the conversion between available charge and chemically bound charge when charging and discharging the battery. This parameter is usually derived from test data by curve fitting.
-
-#### Field: Fully Charged Module Open Circuit Voltage
-
-This field indicates the open circuit voltage for a fully charged battery module. It can be found from manufacture   s data or battery tests.
-
-#### Field: Fully Discharged Module Open Circuit Voltage
-
-This field indicates the open circuit voltage for a fully discharged battery module. It can be found from manufacture   s data or battery tests.
-
-#### Field: Voltage Change Curve Name for Charging
-
-This field specifies the name of a rectangular hyperbola type 2 performance curve (ref: Curve:RectangularHyperbola2 in Performance Curves) that determines the change of open circuit voltage (<span>\(\Delta E\)</span>) as a function of the battery state of charge in charging. The change of open circuit voltage is relative to a fully discharged battery.
-
-The curve has the following form:
-
-<div>\[\Delta E = ({C_1}*X)/({C_2} + X) + {C_3}*X\]</div>
-
-where X is the battery charge divided by the maximum capacity at a given current. More details can be found from the Engineering Reference.
-
-#### Field: Voltage Change Curve Name for Discharging
-
-This field specifies the name of a rectangular hyperbola type 2 performance curve (ref: Curve:RectangularHyperbola2 in Performance Curves) that determines the change of open circuit voltage (<span>\(\Delta E\)</span>) as a function of the battery state of charge in discharging. The change of open circuit voltage is relative to a fully charged battery.
-
-The curve has the following form:
-
-<div>\[\Delta E = ({C_1}*X)/({C_2} + X) + {C_3}*X\]</div>
-
-where X is the removed charge divided by the maximum capacity at a given current. More details can be found from the Engineering Reference.
-
-#### Field: Module Internal Electrical Resistance
-
-This field specifies the battery internal resistance in ohms. In theory, the electrical resistance within the battery varies with the state of charge and depends on whether it is in charging or discharging. In the kinetic battery model, the internal resistance is assumed as constant and the terminal voltage varies with current and state of charge. The internal resistance may be obtained from the battery manufacture or battery test data. Note that the field is for an individual module, not for the whole battery bank.
-
-#### Field: Maximum Module Discharging Current
-
-This field indicates the maximum current at which the battery can be discharged continuously. The limit on discharge current is usually defined by the battery manufacture to avoid battery damage. The limit is for an individual battery module.
-
-#### Field: Module Cut-off Voltage
-
-This field specifies the minimum allowable voltage, below which the battery is generally regarded as empty. The cut-off voltage is usually defined by the battery manufacture and it is for an individual battery module.
-
-#### Field: Module Charge Rate Limit
-
-This field specifies the limit on charging current relative to the remaining charge until the battery is full. This limit reflects the common practice that the charge rate is reduced as the battery gets more charged.
-
-#### Field: Battery Life Calculation
-
-This field indicates whether the battery life model is activated in the simulation. If the battery life model is activated, the following five inputs on curve coefficients are required; otherwise, they are not used.
-
-#### Field: Number of Cycle Bins
-
-This field specifies the number of equally ranged cycle bins in battery life simulation. If 10 bins are used, the cycle ranges will include 10%, 20%, ..., 100%.
-
-#### Field: Battery Cycle Life Curve Name
-
-This field specifies the name of a double exponential decay curve (ref: Curve:DoubleExponentialDecay in Performance Curves) that correlates the cycles of battery failure (C<sub>F</sub>) and fractional depth of discharge (R). The curve is:
-
-<div>\[{C_F} = {C_1} + {C_2}{e^{{C_3}R}} + {C_4}{e^{{C_5}R}}\]</div>
-
-
-
-An example input of the ElectricLoadCenter:Storage: Battery input is:
-
-
-
-```idf
-   ElectricLoadCenter:Storage:Battery,
-       Lead Acid Battery A,   !-Name
-       Always On,                       !- Availability Schedule Name
-       ,                                         !- Zone Name
-       ,                                         !-Radiative Fraction
-       1,                                       !- Number of Battery Modules in Parallel
-       1,                                       !- Number of Battery Modules in Series
-       86.1,                                 !- Maximum Module Capacity {Ah}
-       1.0,                                   !- Initial Fractional State of Charge
-       0.3747,                             !- Fraction of Available Charge Capacity
-       0.5874,                             !- Change Rate from Bound Charge to Available Charge {hr<sup>-1</sup>}
-       12.60,                               !- Fully Charged Module Open Circuit Voltage {V}
-       12.37,                               !- Fully Discharged Module Open Circuit Voltage {V}
-       BatteryChargeCurve,     !- Voltage Change Curve Name for Charging
-       BatteryDischargeCurve,!- Voltage Change Curve Name for Discharging
-       0.0538,                             !- Module Internal Electrical Resistance {Ohm}
-       100,                                   !- Maximum Module Discharging Current {A}
-       10.2,                                 !- Module Cut-off Voltage {V}
-       1,                                       !- Module Charge Rate Limit {1/hr}
-       Yes,                                   !- Battery Life Calculation
-         10,                                   !- Number of Cycle Bins
-       BatteryCycleCurve;       !- Battery Cycle Life Curve Name
-
-   Curve:RectangularHyperbola2,
-       BatteryChargeCurve,     !- Name
-       -0.2765,                           !- Coefficient1 C1
-       -93.27,                             !- Coefficient2 C2
-       0.0068,                             !- Coefficient3 C3
-       0,                                       !- Minimum Value of x
-       1.0,                                   !- Maximum Value of x
-       -100,                                 !- Minimum Curve Output
-       100;                                   !- Maximum Curve Output
-
-   Curve:RectangularHyperbola2,
-       BatteryDischargeCurve,     !- Name
-       0.0899,                                   !- Coefficient1 C1
-       -98.24,                                   !- Coefficient2 C2
-       -0.0082,                                 !- Coefficient3 C3
-       0,                                             !- Minimum Value of x
-       1.0,                                         !- Maximum Value of x
-       -100,                                       !- Minimum Curve Output
-       100;                                         !- Maximum Curve Output
-
-   Curve:DoubleExponentialDecay,
-       BatteryCycleCurve,         !- Name
-       1380,                                   !- Coefficient1 C1
-       6834,                                   !- Coefficient2 C2
-       -8.75,                                 !- Coefficient3 C3
-       6747,                                   !- Coefficient4 C4
-       -6.22,                                 !- Coefficient5 C5
-       0,                                         !- Minimum Value of x
-       1.0;                                     !- Maximum Value of x
-```
-
-### ElectricLoadCenter: Storage:Battery Outputs
-
-* HVAC,Average, Electric Storage Operating Mode Index []
-
-* HVAC,Average,Electric Storage Charge State[Ah]
-
-* HVAC,Average, Electric Storage Charge Fraction []
-
-* HVAC,Average,Electric Storage Charge Power[W]
-
-* HVAC,Sum,Electric Storage Charge Energy [J]
-
-* HVAC,Average,Electric Storage Discharge Power[W]
-
-* HVAC,Sum,Electric Storage Discharge Energy [J]
-
-* HVAC,Average,Electric Storage Total Current[A]
-
-* HVAC,Average, Electric Storage Total Voltage [V]
-
-* HVAC,Average,Electric Storage Thermal Loss Rate [W]
-
-* HVAC,Average, Electric Storage Degradation Fraction []
-
-* HVAC,Sum,Electric Storage Production Decrement Energy [J]
-
-* HVAC,Sum,Electric Storage Thermal Loss Energy [J]
-
-
-
-#### Electric Storage Operating Mode Index []
-
-This output reports the battery mode of operation: 0 for idle; 1 for discharging; 2 for charging. It is expected that more operation modes would be added when a smart and active power dispatch controller is used in future.
-
-#### Electric Storage Charge State [Ah]
-
-The state of charge is expressed as the amount of charge stored in the battery at a point of time. It has the same unit as the maximum capacity. This value is given for an individual battery module
-
-#### Electric Storage Charge Fraction []
-
-This output is the ratio between the electrical storage state of charge and the maximum capacity.
-
-#### Electric Storage Charge Power [W]
-
-#### Electric Storage Charge Energy [J]
-
-These outputs are total electricity power or energy fed into the battery. This is the rate of amount of charging.
-
-#### Electric Storage Production Decrement Energy [J]
-
-This output is the total electricity energy decremented from electricity production because it has fed into the battery. This output has the opposite sign of    Electric Storage Charge Energy    but is otherwise similar. This decrement output variable is also a meter associated with the resource type    ElectricityProduced    that reduces the metered electricity production to account for power that went into storage after production.
-
-#### Electric Storage Discharge Power [W]
-
-#### Electric Storage Discharge Energy [J]
-
-These outputs are total electricity power or energy drawn from the battery. This is the rate or amount of discharging. The energy from storage output variable is also a meter associated with the resource type    ElectricityProduced    that increases the metered electricity production to account for power that has come back out of storage.
-
-#### Electric Storage Total Current [A]
-
-This output is the current to or from the battery bank depending on whether the battery is in the state of charging or discharging. The value is positive for discharging and negative for charging.
-
-#### Electric Storage Total Voltage [V]
-
-This output is the total terminal voltage of the battery bank.
-
-#### Electric Storage Thermal Loss Rate [W]
-
-#### Electric Storage Thermal Loss Energy [J]
-
-These outputs are the thermal power or energy losses from both charging and drawing electrical power in or out of the storage device. These losses are due to the battery internal resistance in charging and discharging.
-
-#### Electric Storage Degradation Fraction []
-
-This output reports the fractional battery life used up at a point of time. For example, a value of 0.4 at the end of one year simulation means that the 40% of the battery life is used up, so the battery needs to be replaced every two and a half years.
-
-
-
-### Generator:InternalCombustionEngine
-
-The Internal Combustion (IC) Engine generator uses a modified Otto cycle. This generator model uses the electrical load and rated engine generator size to compute part-load ratios (PLR). Fuel energy input and recoverable jacket and lube oil heat are then computed. Finally, the recoverable exhaust heat is calculated.
-
-Manufacturer's curves or tables must be obtained for IC engine generators to derive the equipment performance parameters that are specified in the quadratic curve fits. Note that simple transformation of the form of the manufacturer's curves may be required. Electric energy output/fuel energy input is related to the part-load ratio (i.e., electric/load generator capacity) with a polynomial. Recoverable jacket heat/fuel energy equipment, recoverable lube oil heat/fuel energy input equipment performance, total exhaust heat/fuel energy input equipment, exhaust gas temperature/fuel energy input equipment performance parameters are all specified with a quadratic curve fit.
-
-When the heat recovery curve fits = 0.0, this means that no heat recovery is done on the IC engine generator exhaust gas; and no heat recovery is specified.
-
-#### Field: Name
-
-This alpha field contains the identifying name for the IC engine generator.
-
-#### Field: Rated Power Output
-
-The design nominal capacity of the generator in Watts [W].
-
-#### Field: Electric Circuit Node Name
-
-This named node contains where the electric power is put in the program simulation for use by the electric equipment in the Load Center.
-
-#### Field: Minimum Part Load Ratio
-
-This field contains the minimum allowed operating fraction of full load. The input value must be &gt;=0.0 and &lt;=1.0.
-
-#### Field: Maximum Part Load Ratio
-
-This field contains the maximum allowed operating fraction of full load. The input value must be &gt;0.0 and &lt;=1.0.
-
-#### Field: Optimum Part Load Ratio
-
-This alpha field contains the optimal operating fraction of full load. This is the part load ratio that gives the optimal production of electric power with the least amount of fuel usage.
-
-#### Field: Shaft Power Curve Name
-
-This alpha field contains the name of the shaft power curve. The curve itself is specified separately using a curve object (ref: Curve:QuadLinear). The Shaft Power Curve is a quadratic equation that determines the electric output versus the fuel used. Used to calculate the electric energy output divided by the fuel energy consumption as a function of part-load ratio. The defining equation is:
-
-<div>\[ShaftPowerToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}\]</div>
-
-where RL is the Ratio of Load to Rated Power Output.
-
-#### Field: Jacket Heat Recovery Curve Name
-
-This alpha field contains the name of the Recovery Jacket Heat curve. The curve itself is specified separately using a curve object (ref: Curve:QuadLinear). The Jacket Heat Recovery Curve is a quadratic equation that determines the ratio of recovery jacket heat to fuel energy. Used to calculate the recoverable jacket heat as a function of part-load ratio.
-
-The defining equation is:
-
-<div>\[RecoveryJacketHeatToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}\]</div>
-
-where RL is the Ratio of Load to Rated Power Output.
-
-#### Field: Lube Heat Recovery Curve Name
-
-This alpha field contains the name of the Recovery Lube Heat curve. The curve itself is specified separately using a curve object (ref Curve:QuadLinear). The Lube Heat Recovery Curve is a quadratic equation that determines the ratio of recovery lube heat to fuel energy. Used to calculate the recoverable lube oil heat as a function of part-load ratio. The defining equation is:
-
-<div>\[RecoveryLubeHeatToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}\]</div>
-
-where RL is the Ratio of Load to Rated Power Output.
-
-#### Field: Total Exhaust Energy Curve Name
-
-This alpha field contains the name of the Total Exhaust Energy curve. The curve itself is specified separately using a curve object (ref Curve:QuadLinear object). The Total Exhaust Energy Curve is a quadratic equation that determines the ratio of total exhaust energy to fuel energy. Used to calculate the total exhaust heat as a function of part-load ratio. The defining equation is:
-
-<div>\[TotalExhaustToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}\]</div>
-
-where RL is the Ratio of Load to Rated Power Output.
-
-#### Field: Exhaust Temperature Curve Name
-
-This alpha field contains the name of the Exhaust Temperature curve. The curve itself is specified separately using a curve object (ref Curve:QuadLinear object). The Exhaust Temperature Curve is a quadratic equation that determines the absolute exhaust temperature. Used to determine the exhaust gas temperature as a function of part-load ratio. The defining equation is:
-
-<div>\[AbsoluteExhaustTemperature = {C_1} + {C_2}RL + {C_3}R{L^2}\]</div>
-
-where RL is the Ratio of Load to Rated Power Output.
-
-#### U-Factor Times Area (UA) Curve
-
-The UA curve applies to the exhaust gas heat exchanger. The curve is an equation that determines the overall heat transfer coefficient for the exhaust gases with the stack. The heat transfer coefficient ultimately helps determine the exhaust stack temperature. The defining equation is:
-
-<div>\[UAToCapacityRatio = {C_1}GeneratorRatedPowerOutpu{t^{{C_2}}}\]</div>
-
-The following two fields contain the coefficients for the equation.
-
-#### Field: Coefficient 1 of U-Factor Times Area Curve
-
-This numeric field contains the first coefficient for the overall heat transfer coefficient curve.
-
-#### Field: Coefficient 2 of U-Factor Times Area Curve
-
-This numeric field contains the second (exponential) coefficient for the overall heat transfer coefficient curve.
-
-#### Field: Maximum Exhaust Flow per Unit of Power Output
-
-Maximum exhaust flow per unit capacity for the generator. The parameter sets an upper limit on exhaust gas flow and exhaust gas heat recovery for the generator. Units: kg/sec per kW capacity
-
-#### Field: Design Minimum Exhaust Temperature
-
-This is the design engine stack saturated steam temperature in degrees C.
-
-#### Field: Fuel Higher Heating Value
-
-This numeric field contains the higher heating value of the fuel used in kJ/kg.
-
-#### Field: Design Heat Recovery Water Flow Rate
-
-Design water volumetric flow rate through heat recovery loop in m<sup>3</sup>/sec.
-
-#### Field: Heat Recovery Inlet Node Name
-
-This alpha field contains the identifying name for the generator   s heat recovery side inlet node.
-
-#### Field: Heat Recovery Outlet Node Name
-
-This alpha field contains the identifying name for the generator   s heat recovery side outlet node.
-
-#### Field: Fuel Type
-
-This alpha field determines the type of fuel that the generator uses.   The default is Diesel. Valid values are: **NaturalGas**, **PropaneGas**, **Diesel**, **Gasoline**, **FuelOil\#1**, **FuelOil\#2, OtherFuel1,** and **OtherFuel2**.
-
-#### Field: Heat Recovery Maximum Temperature
-
-This field sets the maximum temperature that this piece of equipment can produce for heat recovery. The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit. This temperature limit puts an upper bound on the recovered heat and limits the max temperatures leaving the component.
-
-As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting. This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply.
-
-The temperature is specified in degrees C.
-
-An IDF example showing how it is used is provided below:
-
-```idf
-   Generator:InternalCombustionEngine,
-       Cat Diesel,                           !- Name
-       50000,                                     !- Rated Power Output {W}
-       Generator Diesel Electric Node,   !- Electric Circuit Node Name
-       0.15,                                       !- Minimum Part Load Ratio
-       1.0,                                         !- Maximum Part Load Ratio
-       0.65,                                       !- Optimum Part Load Ratio
-       BG Shaft Power Curve,       !- Shaft Power Curve Name
-       BG Recovery Jacket Heat Curve,   !- Jacket Heat Recovery Curve Name
-       BG Recovery Lube Heat Curve,   !- Lube Heat Recovery Curve Name
-       BG Total Exhaust Energy Curve,   !- Total Exhaust Energy Curve Name
-       BG Exhaust Temperature Curve,   !- Exhaust Temperature Curve Name
-       0.00952329,                           !- Coefficient 1 of U-Factor Times Area Curve
-       0.9,                                         !- Coefficient 2 of U-Factor Times Area Curve
-       0.00000063,                           !- Maximum Exhaust Flow per Unit of Power Output {(kg/s)/W}
-       150,                                         !- Design Minimum Exhaust Temperature {C}
-       45500,                                     !- Fuel Higher Heating Value {kJ/kg}
-       0.0,                                         !- Design Heat Recovery Water Flow Rate {m3/s}
-       ,                                               !- Heat Recovery Inlet Node Name
-       ,                                               !- Heat Recovery Outlet Node Name
-       Diesel;                                   !- Fuel Type
-
-   Curve:Quadratic,
-       BG Shaft Power Curve,       !- Name
-       0.09755,                                 !- Coefficient1 Constant
-       0.6318,                                   !- Coefficient2 x
-       -0.4165,                                 !- Coefficient3 x**2
-       0,                                             !- Minimum Value of x
-       1;                                             !- Maximum Value of x
-
-   Curve:Quadratic,
-       BG Recovery Jacket Heat Curve,   !- Name
-       0.25,                                       !- Coefficient1 Constant
-       0,                                             !- Coefficient2 x
-       0,                                             !- Coefficient3 x**2
-       0,                                             !- Minimum Value of x
-       1;                                             !- Maximum Value of x
-
-   Curve:Quadratic,
-       BG Recovery Lube Heat Curve,   !- Name
-       0.15,                                       !- Coefficient1 Constant
-       0,                                             !- Coefficient2 x
-       0,                                             !- Coefficient3 x**2
-       0,                                             !- Minimum Value of x
-       1;                                             !- Maximum Value of x
-
-   Curve:Quadratic,
-       BG Total Exhaust Energy Curve,   !- Name
-       0.1,                                         !- Coefficient1 Constant
-       0,                                             !- Coefficient2 x
-       0,                                             !- Coefficient3 x**2
-       0,                                             !- Minimum Value of x
-       1;                                             !- Maximum Value of x
-
-   Curve:Quadratic,
-       BG Exhaust Temperature Curve,   !- Name
-       425,                                         !- Coefficient1 Constant
-       0,                                             !- Coefficient2 x
-       0,                                             !- Coefficient3 x**2
-       0,                                             !- Minimum Value of x
-       1;                                             !- Maximum Value of x
-```
-
-### Generator:InternalCombustionEngine Outputs
-
-The output variables that are available for the IC engine generator are:
-
-* HVAC,Average,Generator Produced Electric Power [W]
-
-* HVAC,Sum,Generator Produced Electric Energy [J]
-
-
-
-* HVAC,Average,Generator Lube Heat Recovery Rate [W]
-
-* HVAC,Sum,Generator Lube Heat Recovery Energy [J]
-
-
-
-* HVAC,Average,Generator Jacket Heat Recovery Rate [W]
-
-* HVAC,Sum,Generator Jacket Heat Recovery Energy [J]
-
-
-
-* HVAC,Average,Generator Exhaust Heat Recovery Rate [W]
-
-* HVAC,Sum,Generator Exhaust Heat Recovery Energy [J]
-
-
-
-* HVAC,Average,Generator Total Heat Recovery Rate [W]
-
-* HVAC,Sum,Generator Total Heat Recovery [J]
-
-
-
-* HVAC,Average,Generator Exhaust Air Temperature [C]
-
-
-
-* HVAC,Average,Generator Heat Recovery Inlet Temperature [C]
-
-* HVAC,Average,Generator Heat Recovery Outlet Temperature [C]
-
-* HVAC,Average,Generator Heat Recovery Mass Flow Rate [kg/s]
-
-
-
-* HVAC,Average,Generator Fuel HHV Basis Rate [W]
-
-* HVAC,Sum,Generator Fuel HHV Basis Energy [J]
-
-
-
-* HVAC,Average,Generator &lt;Fuel Type&gt; Rate [W]
-
-* HVAC,Sum,Generator&lt;Fuel Type&gt; Energy [J]
-
-* HVAC,Average,Generator &lt;Fuel Type&gt; Mass Flow Rate [kg/s]
-
-#### Generator Produced Electric Power [W]
-
-#### Generator Produced Electric Energy [J]
-
-These outputs are the electric power output from the electric generator. Energy is metered on Cogeneration:ElectricityProduced, ElectricityProduced:Plant, and ElectricityProduced:Facility.
-
-#### Generator Lube Heat Recovery Rate [W]
-
-#### Generator Lube Heat Recovery Energy [J]
-
-#### Generator Jacket Heat Recovery Rate [W]
-
-#### Generator Jacket Heat Recovery Energy [J]
-
-#### Generator Exhaust Heat Recovery Rate [W]
-
-#### Generator Exhaust Heat Recovery Energy [J]
-
-#### Generator Produced Thermal Rate [W]
-
-#### Generator Produced Thermal Energy [J]
-
-For electric generators with heat recovery these outputs are the components of recoverable energy available. For the IC engine generator, the following heat recovery components are reported:   Lube (engine lubricant), Jacket (engine coolant), and Exhaust (engine exhaust).   These components are totaled together for Generator Produced Thermal Rate and Generator Produced Thermal Energy reports. Generator Lube Heat Recovery Energy, Generator Jacket Heat Recovery Energy, and Generator Exhaust Heat Recovery Energy are metered on HeatRecovery:EnergyTransfer, EnergyTransfer:Plant, and EnergyTransfer:Facility.
-
-#### Generator Exhaust Air Temperature [C]
-
-This is the exhaust temperature leaving the engine.
-
-#### Generator Heat Recovery Inlet Temperature [C]
-
-#### Generator Heat Recovery Outlet Temperature [C]
-
-#### Generator Heat Recovery Mass Flow Rate [kg/s]
-
-These outputs are the heat recovery inlet and outlet temperatures and flow rate for generators with heat recovery.
-
-#### Generator Fuel HHV Basis Rate [W]
-
-#### Generator Fuel HHV Basis Energy [J]
-
-These outputs are the generator   s fuel energy and use rate.   The energy content of the fuel is based on the higher heating value (HHV).
-
-#### Generator &lt;Fuel Type&gt; Rate [W]
-
-#### Generator &lt;Fuel Type&gt; Energy [J]
-
-#### Generator &lt;Fuel Type&gt; Mass Flow Rate [kg/s]
-
-If the fuel type is Diesel, then Diesel is shown as the fuel type. They are the diesel fuel input to the electric generator. Consumption is metered on Cogeneration:Diesel, Diesel:Plant, and Diesel:Facility.
-
-If the fuel type is Natural Gas, then Gas is shown as the fuel type. They are the natural gas fuel input to the electric generator. Consumption is metered on Cogeneration:Gas, Gas:Plant, and Gas:Facility.
-
-If the fuel type is Propane, then Propane is shown as the fuel type. They are the propane fuel input to the electric generator. Consumption is metered on Cogeneration:Propane, Propane:Plant, and Propane:Facility.
-
-If the fuel type is Gasoline, then Gasoline is shown as the fuel type. They are the gasoline fuel input to the electric generator. Consumption is metered on Cogeneration:Gasoline, Gasoline:Plant, and Gasoline:Facility.
-
-If the fuel type is FuelOil\#1, then FuelOil\#1 is shown as the fuel type. They are the fuel oil input to the electric generator. Consumption is metered on Cogeneration:FuelOil\#1, FuelOil\#1:Plant, and FuelOil\#1:Facility.
-
-If the fuel type is FuelOil\#2, then FuelOil\#2 is shown as the fuel type. They are the fuel oil input to the electric generator. Consumption is metered on Cogeneration:FuelOil\#2, FuelOil\#2:Plant, and FuelOil\#2:Facility.
-
-If the fuel type is OtherFuel1, then OtherFuel1 is shown as the fuel type. They are the fuel oil input to the electric generator. Consumption is metered on Cogeneration:OtherFuel1, OtherFuel1:Plant, and OtherFuel1:Facility.
-
-If the fuel type is OtherFuel2, then OtherFuel2 is shown as the fuel type. They are the fuel oil input to the electric generator. Consumption is metered on Cogeneration:OtherFuel2, OtherFuel2:Plant, and OtherFuel2:Facility.
-
-### Generator:CombustionTurbine
-
-EnergyPlus has two different models for combustion turbine style generators.   This one stems for a model that was originally in the BLAST computer program.   A newer model with a different formulation is also available  -see the Generator:MicroTurbine input object.   The basic combustion-turbine cycle is the Brayton Cycle or open cycle, which consists of an adiabatic compression, constant pressure heating, and adiabatic expansion. The Combustion turbine model uses the electrical load and engine generator size to compute part-load ratios (PLR). Fuel energy input and recoverable lube oil heat are then computed. Finally, the recoverable exhaust heat is calculated.
-
-Combustion turbine generators use performance parameters to compute fuel energy consumption as a function of part-load and ambient (entering) air temperature. Recoverable fuel energy equipment, recoverable lube oil heat/fuel energy input equipment performance, total exhaust heat/fuel energy input equipment, exhaust gas temperature/fuel energy input equipment performance parameters are all specified with a quadratic curve fit.
-
-When the heat recovery curve fits = 0.0, this means that no heat recovery is done on the diesel generator exhaust gas; and no heat recovery is specified.
-
-#### Field: Name
-
-Unique name to identify this combustion turbine generator.
-
-#### Field: Rated Power Output
-
-The design nominal capacity of the combustion turbine generator in Watts [W].
-
-#### Field: Electric Circuit Node Name
-
-This Named node contains where the electric power is put in the program simulation for use by the electric equipment in the Load Center.
-
-#### Field: Minimum Part Load Ratio
-
-This field contains the minimum allowed operating fraction of full load. The input value must be &gt;=0.0 and &lt;=1.0.
-
-#### Field: Maximum Part Load Ratio
-
-This field contains the maximum allowed operating fraction of full load. The input value must be &gt;0.0 and &lt;=1.0.
-
-#### Field: Optimum Part Load Ratio
-
-This alpha field contains the optimal operating fraction of full load. This is the part load ratio that gives the optimal production of electric power with the least amount of fuel usage.
-
-#### Field: Part Load Based Fuel Input Curve Name
-
-Needs a Curve:Quadratic object   to be specified.
-
-Fuel Input = a + b\*PLR + c\*PLR\*\*2
-
-PLR = Ratio of Generator Load to Rated Power Output. This curve is multiplied to the Temperature Based Fuel Input Curve to determine Fuel Energy In.
-
-#### Field: Temperature Based Fuel Input Curve Name
-
-Needs a Curve:Quadratic object to be specified.
-
-Fuel Input = a + b\*AT + c\*AT\*\*2   where: AT = Ambient Delta T
-
-#### Field: Exhaust Flow Curve Name
-
-The Total Exhaust Energy Curve is a quadratic equation that needs to be specified by a curve object. Used to calculate the total exhaust heat as a function of part-load ratio.
-
-#### Field: Part Load Based Exhaust Temperature Curve Name
-
-The Exhaust Temperature Curve is a quadratic equation that needs to be specified by a curve object. Used to determine the exhaust gas temperature as a function of part-load ratio.
-
-#### Field: Temperature Based Exhaust Temperature Curve Name
-
-The Exhaust Temperature Curve is a quadratic equation that needs to be specified by a curve object. Used to determine the exhaust gas temperature as a function of part-load ratio.
-
-#### Field: Heat Recovery Lube Energy Curve Name
-
-This alpha field contains the name of the Recovery Lube Heat curve. The curve itself is specified separately using a curve object (see Curve:Quadlinear object). The Recovery Lubricant Heat Curve is a quadratic equation that determines the ratio of recovery lube heat to fuel energy. Used to calculate the recoverable lube oil heat as a function of part-load ratio. The defining equation is:
-
-<div>\[RecoveryLubeHeatToFuelRatio = {C_1} + {C_2}RL + {C_3}R{L^2}\]</div>
-
-where RL is the Ratio of Load to Rated Power Output.
-
-#### U-Factor Times Area (UA) Curve
-
-The UA curve applies to the exhaust gas heat exchanger. The curve is an equation that determines the overall heat transfer coefficient for the exhaust gases with the stack. The heat transfer coefficient ultimately helps determine the exhaust stack temperature. The defining equation is:
-
-<div>\[UAToCapacityRatio = {C_1}GeneratorRatedPowerOutpu{t^{{C_2}}}\]</div>
-
-The following two fields contain the coefficients for the equation.
-
-#### Field: Coefficient 1 of U-Factor Times Area Curve
-
-This numeric field contains the first coefficient for the overall heat transfer coefficient curve.
-
-#### Field: Coefficient 2 of U-Factor Times Area Curve
-
-This numeric field contains the second (exponential) coefficient for the overall heat transfer coefficient curve.
-
-#### Field: Maximum Exhaust Flow per Unit of Power Output
-
-Maximum exhaust flow per unit capacity for diesel engines. The parameter sets an upper limit on exhaust gas flow and exhaust gas heat recovery for diesel engines. Units: kg/sec per kW capacity
-
-#### Field: Design Minimum Exhaust Temperature
-
-This is the design engine stack saturated steam temperature in degrees C.
-
-#### Field: Design Air Inlet Temperature
-
-Design air inlet temperature in degrees C.
-
-#### Field: Fuel Higher Heating Value
-
-This numeric field contains the higher heating value of the fuel used in kJ/kg.
-
-#### Field: Design Heat Recovery Water Flow Rate
-
-Design water volumetric flow rate through heat recovery loop in m<sup>3</sup>/sec.
-
-#### Field: Heat Recovery Inlet Node Name
-
-This alpha field contains the identifying name for the combustion turbine generator heat recovery side inlet node.
-
-#### Field: Heat Recovery Outlet Node Name
-
-This alpha field contains the identifying name for the combustion turbine generator heat recovery side outlet node.
-
-#### Field: Fuel Type
-
-This alpha field determines the type of fuel that the generator uses. Valid choices are: **NaturalGas, PropaneGas, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1** and **OtherFuel2**. The default is **NaturalGas**.
-
-#### Field: Heat Recovery Maximum Temperature
-
-This field sets the maximum temperature that this piece of equipment can produce for heat recovery. The idea behind this field is that the current models do not take temperatures into account for availability and they just pass Q's around the loop without a temperature limit. This temperature limit puts an upper bound on the recovered heat and limits the max temperatures leaving the component.
-
-As temperatures in the loop approach the maximum temperature, the temperature difference between the entering water and the surfaces in the piece of equipment becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The reduced amount of heat recovered will diminish if the temperature of the loop approach is the maximum temperature, and this will show up in the reporting. This allows the user to set the availability or the quality of the heat recovered for usage in other parts of the system or to heat domestic hot water supply.
-
-The temperature is specified in degrees C.
-
-#### Field: Outdoor Air Inlet Node Name
-
-This field is optional. It is used to explicitly define an outdoor air node for the inlet for combustion air stream. Defining an outdoor air node here allows using the height-dependent model for outdoor air conditions.
-
-An IDF example showing how it is used is provided below:
-
-```idf
-   Generator:CombustionTurbine,
-       Solar Turbine,                     !- Name
-       30000,                                     !- Rated Power Output {W}
-       GT gen Electric Node,       !- Electric Circuit Node Name
-       0.15,                                       !- Minimum Part Load Ratio
-       1.0,                                         !- Maximum Part Load Ratio
-       0.65,                                       !- Optimum Part Load Ratio
-       BG PL Based Fuel Input Curve,   !- Part Load Based Fuel Input Curve Name
-       BG Temp Based Fuel Input Curve,   !- Temperature Based Fuel Input Curve Name
-       BG Exhaust Flow Curve,     !- Exhaust Flow Curve Name
-       BG PL Based Exhaust Temp Curve,   !- Part Load Based Exhaust Temperature Curve Name
-       BG Temp Based Exhaust Temp Curve,   !- Temperature Based Exhaust Temperature Curve Name
-       BG Tur Recovery Lube Heat Curve,   !- Heat Recovery Lube Energy Curve Name
-       0.01907045,                           !- Coefficient 1 of U-Factor Times Area Curve
-       0.9,                                         !- Coefficient 2 of U-Factor Times Area Curve
-       0.00000504,                           !- Maximum Exhaust Flow per Unit of Power Output {(Kg/s)/W}
-       150,                                         !- Design Minimum Exhaust Temperature {C}
-       25,                                           !- Design Air Inlet Temperature {C}
-       43500,                                     !- Fuel Higher Heating Value {kJ/kg}
-       0.0,                                         !- Design Heat Recovery Water Flow Rate {m3/s}
-       ,                                               !- Heat Recovery Inlet Node Name
-       ,                                               !- Heat Recovery Outlet Node Name
-       NaturalGas,                           !- Fuel Type
-       ,                                               !- Heat Recovery Maximum Temperature {C}
-       CT OA inlet;                         !- Outdoor Air Inlet Node Name
-
-   Curve:Quadratic,
-       BG PL Based Fuel Input Curve,   !- Name
-       9.41,                                       !- Coefficient1 Constant
-       -9.48,                                     !- Coefficient2 x
-       4.32,                                       !- Coefficient3 x**2
-       0,                                             !- Minimum Value of x
-       1;                                             !- Maximum Value of x
-
-   Curve:Quadratic,
-       BG Temp Based Fuel Input Curve,   !- Name
-       1.0044,                                   !- Coefficient1 Constant
-       -0.0008,                                 !- Coefficient2 x
-       0,                                             !- Coefficient3 x**2
-       -30,                                         !- Minimum Value of x
-       +30;                                         !- Maximum Value of x
-
-   Curve:Quadratic,
-       BG Exhaust Flow Curve,     !- Name
-       0.05,                                       !- Coefficient1 Constant
-       0.0,                                         !- Coefficient2 x
-       0.0,                                         !- Coefficient3 x**2
-       0,                                             !- Minimum Value of x
-       1;                                             !- Maximum Value of x
-
-   Curve:Quadratic,
-       BG PL Based Exhaust Temp Curve,   !- Name
-       450,                                         !- Coefficient1 Constant
-       0,                                             !- Coefficient2 x
-       0,                                             !- Coefficient3 x**2
-       0,                                             !- Minimum Value of x
-       1;                                             !- Maximum Value of x
-
-   Curve:Quadratic,
-       BG Temp Based Exhaust Temp Curve,   !- Name
-       1.005,                                     !- Coefficient1 Constant
-       0.0018,                                   !- Coefficient2 x
-       0,                                             !- Coefficient3 x**2
-       -30,                                         !- Minimum Value of x
-       +30;                                         !- Maximum Value of x
-
-   Curve:Quadratic,
-       BG Tur Recovery Lube Heat Curve,   !- Name
-       0.223,                                     !- Coefficient1 Constant
-       -0.4,                                       !- Coefficient2 x
-       0.2286,                                   !- Coefficient3 x**2
-       0,                                             !- Minimum Value of x
-       1;                                             !- Maximum Value of x
-```
-
-### Generator:CombustionTurbine Outputs
-
-The output variables that are available for the combustion turbine generator are:
-
-* HVAC,Average,Generator Produced Electric Power [W]
-
-* HVAC,Sum,Generator Produced Electric Energy [J]
-
-* Zone,Meter,ElectricityProduced:Facility [J]
-
-* Zone,Meter,ElectricityProduced:Plant [J]
-
-* Zone,Meter,Cogeneration:ElectricityProduced [J]
-
-
-
-* HVAC,Average,Generator Lube Heat Recovery Rate [W]
-
-* HVAC,Sum,Generator Lube Heat Recovery Energy [J]
-
-
-
-* HVAC,Average,Generator Exhaust Heat Recovery Rate [W]
-
-* HVAC,Sum,Generator Exhaust Heat Recovery [J]
-
-
-
-* HVAC,Average,Generator Total Heat Recovery Rate [W]
-
-* HVAC,Sum,Generator Total Heat Recovery [J]
-
-
-
-* HVAC,Average,Generator Exhaust Air Temperature [C]
-
-
-
-* HVAC,Average,Generator Heat Recovery Inlet Temperature [C]
-
-* HVAC,Average,Generator Heat Recovery Outlet Temperature [C]
-
-* HVAC,Average,Generator Heat Recovery Mass Flow Rate [kg/s]
-
-
-
-* HVAC,Average,Generator &lt;Fuel Type&gt; Rate [W]
-
-* HVAC,Sum,Generator &lt;Fuel Type&gt; Energy [J]
-
-* HVAC,Average,Generator &lt;Fuel Type&gt; Mass Flow Rate [kg/s]
-
-All of these outputs, except for the Combustion use outputs, are described above under "Generator:InternalCombustionEngine Outputs."
-
-#### Generator &lt;Fuel Type&gt; Rate [W]
-
-#### Generator &lt;Fuel Type&gt; Energy [J]
-
-#### Generator &lt;Fuel Type&gt; Mass Flow Rate [kg/s]
-
-These outputs are the fuel input to the electric generator. Consumption is metered on Cogeneration:&lt;Fuel Type&gt;, &lt;Fuel Type&gt;:Plant, and &lt;Fuel Type&gt;:Facility.
-
-### Generator:MicroTurbine
-
-MicroTurbine generators are small combustion turbines that produce electricity on a relatively small scale (e.g., 25kW to 500kW). This model uses nominal performance at reference conditions along with several modifier curves to determine electrical power output and fuel use at non-reference conditions. Standby and ancillary power can also be taken into account. Furthermore, energy recovery from exhaust air can be used to heat water. Similar to electrical power output, thermal power (heat recovery) output is calculated using nominal performance at reference conditions with modifier curves to account for variations at non-reference conditions.
-
-The following inputs define the MicroTurbine electric generator. The ElectricLoadCenter:Generators   and ElectricLoadCenter:Distribution objects are used to define the availability and control of all electric generators included in the simulation (ref. ElectricLoadCenter:Generators and ElectricLoadCenter:Distribution).
-
-#### Field: Name
-
-This alpha field specifies a unique user-defined name to identify this generator. This is a required input.
-
-#### Field: Reference Electrical Power Output
-
-This numeric field specifies the full-load electrical power output of the microturbine generator in Watts at reference conditions. The reference conditions are defined via additional input fields for this object (see below). This is a required input, and the value entered in this field must be greater than zero.
-
-#### Field: Minimum Full Load Electrical Power Output
-
-This numeric field specifies the minimum electrical power output in Watts at full-load conditions. The electrical power output of the generator is determined by multiplying the Reference Electrical Power Output by the Electrical Power Function of Temperature and Elevation modifier curve. If the result is less than the numeric value specified in this input field, then the generator   s electrical power output is reset to the minimum full-load value specified in this input field. The value entered in this field must be greater than or equal to zero. If this field is left blank, the default value of 0.0 will be used.
-
-#### Field: Maximum Full Load Electrical Power Output
-
-This numeric field specifies the maximum electrical power output in Watts at full-load conditions. The electrical power output of the generator is determined by multiplying the Reference Electrical Power Output by the Electrical Power Function of Temperature and Elevation Modifier curve. If the result is greater than the numeric value specified in this input field, then the generator   s electrical power output is reset to the maximum full-load value specified in this input field. The value entered in this field must be greater than zero. If this field is left blank, then the value entered for the Reference Electrical Power Output field (above) will be used as the Maximum Full Load Electrical Power Output.
-
-#### Field: Reference Electrical Efficiency Using Lower Heating Value
-
-This numeric field contains the electrical efficiency of the generator at reference conditions, based on the lower heating value of the fuel. The electrical efficiency is the electric power output divided by the fuel energy consumption rate (LHV basis). The reference conditions are defined via additional input fields for this object (see below). This is a required input, and the value entered in this field must be greater than zero and less than or equal to 1.0.
-
-#### Field: Reference Combustion Air Inlet Temperature
-
-This numeric field specifies the reference temperature for the combustion inlet air in degrees Celsius. If this field is left blank, the default value of 15 &deg;C will be used.
-
-#### Field: Reference Combustion Air Inlet Humidity Ratio
-
-This numeric field specifies the reference humidity ratio for the combustion inlet air in kgWater/kgDryAir. The value specified for this field must be greater than zero. If this field is left blank, the default value of 0.00638 (kgWater/kgDryAir) will be used.
-
-#### Field: Reference Elevation
-
-This numeric field specifies the reference elevation in meters (relative to sea level). The value specified for this field must be greater than or equal to -300.0 meters. If this field is left blank, the default value of 0.0 meters will be used.
-
-#### Field: Electrical Power Function of Temperature and Elevation Curve Name
-
-This alpha field specifies the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of electrical power output as a function of the combustion air inlet temperature and elevation. The output of this curve is multiplied by the Reference Electrical Power Output to give the full-load power output at a specific combustion air inlet temperature and elevation (i.e., at values different from the reference conditions). This curve should be normalized to have a value of 1.0 at the reference conditions, and the curve should be valid for the range of inlet air temperatures anticipated for the simulation period and for the actual elevation of the generator.
-
-#### Field: Electrical Efficiency Function of Temperature Curve Name
-
-This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of electrical efficiency as a function of the combustion air inlet temperature. The output of this curve is multiplied by the Reference Electrical Efficiency Using Lower Heating Value to give the full-load electrical efficiency at specific combustion air inlet temperatures (i.e., at inlet air temperatures different from the Reference Combustion Air Inlet Temperature). This curve should be normalized to have a value of 1.0 at the Reference Combustion Air Inlet Temperature, and the curve should be valid for the range of inlet air temperatures anticipated for the simulation period.
-
-#### Field: Electrical Efficiency Function of Part Load Ratio Curve Name
-
-This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of electrical efficiency as a function of the generator   s part-load ratio (part-load ratio is the actual electrical power output divided by the full-load electrical power output at the current operating conditions). The output of this curve is multiplied by the Reference Electrical Efficiency Using Lower Heating Value and the output of the Electrical Efficiency Function of Temperature modifier curve to give the electrical efficiency at specific part-load and combustion air inlet (temperature) conditions. This curve should be normalized to have a value of 1.0 when the generator   s part-load ratio is 1.0, and the curve should be valid for the range of part-load ratios anticipated for the simulation period.
-
-#### Field: Fuel Type
-
-This choice field specifies the type of fuel used by the generator. Valid fueld types are PropaneGas and NaturalGas. If the field is left blank, the fuel type will be assumed to be NaturalGas.
-
-#### Field: Fuel Higher Heating Value
-
-This numeric field specifies the higher heating value of the fuel used in kJ/kg. The value specified for this field must be greater than zero and greater than the specified Fuel Lower Heating Value. If this field is left blank, the default value of 50,000 kJ/kg will be used.
-
-#### Field: Fuel Lower Heating Value
-
-This numeric field specifies the lower heating value of the fuel used in kJ/kg. The value specified for this field must be greater than zero but less than the specified Fuel Higher Heating Value. If this field is left blank, the default value of 45,450 kJ/kg will be used.
-
-#### Field: Standby Power
-
-This numeric field specifies the standby electric power consumed by the generator in Watts. The standby power is the electrical power consumed by the generator (e.g., air fans and controls) when the generator is available to operate but the generator electrical power output is zero (power output is not being requested by the electric load center). The value specified for this field must be greater than or equal to zero. If this field is left blank, the default value of 0.0 W will be used.
-
-#### Field: Ancillary Power
-
-This numeric field specifies the ancillary electric power consumed by the generator in Watts. The ancillary power is the electrical power consumed by other associated equipment (e.g., external fuel pressurization pumps) when the generator is operating. Specify this input as 0.0 if the Reference Electrical Power Output and Reference Electrical Efficiency Using Lower Heating Value input fields and associated modifier curves reflect the    net    electrical power output from the generator (i.e., ancillary power already deducted from the generator   s gross electrical power output). A value greater than zero indicates that this electrical power is consumed whenever the generator is operating and will be deducted from the generator   s overall electrical power output (Generator Produced Electric Power). The value specified for this field must be greater than or equal to zero. If this field is left blank, the default value of 0.0 W will be used.
-
-#### Field: Ancillary Power Function of Fuel Input Curve Name
-
-This alpha field specifies the name of a quadratic performance curve (ref: Performance Curves) that parameterizes the variation of ancillary power as a function of the generator   s input fuel mass flow rate (kg/s). The output of this curve is multiplied by the ancillary power to give the ancillary power at a specific fuel mass flow rate. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation (i.e., the ancillary power is constant whenever the generator operates).
-
-#### Field: Heat Recovery Water Inlet Node Name
-
-This alpha field specifies the identifying name for the generator   s heat recovery water inlet node.
-
-#### Field: Heat Recovery Water Outlet Node Name
-
-This alpha field specifies the identifying name for the generator   s heat recovery water outlet node.
-
-#### Field: Reference Thermal Efficiency Using Lower Heat Value
-
-This numeric field specifies the thermal efficiency (heat recovery to water) at reference conditions, based on the lower heating value of the fuel. The thermal efficiency is the thermal power output (to water) divided by the fuel energy consumption rate (LHV basis). The reference conditions are defined via additional input fields for this object. This value must be from 0.0 to 1.0.   If this field is left blank, the default value of 0.0 will be used.
-
-#### Field: Reference Inlet Water Temperature
-
-This numeric field specifies the reference temperature for the inlet water to the heat recovery heat exchanger in degrees Celsius.
-
-#### Field: Heat Recovery Water Flow Operating Mode
-
-This field is used to choose between different modes of controlling the mass flow rate of water being heated by energy recovered from exhaust air. There are two options available for this field:    PlantControl    or    InternalControl.      The    PlantControl    option indicates that the heat recovery water flow rate through the generator is determined externally (by the wider balance of plant). In this case, the generator will request the Reference Heat Recovery Water Flow Rate whenever it operates but the actual flow rate may be limited by other plant components (e.g., pump). The    InternalControl    option indicates the flow of water is controlled inside the generator based on current operating conditions. For InternalControl, the generator should (probably) include a bypass branch when connecting to the plant loop.
-
-#### Field: Reference Heat Recovery Water Flow Rate
-
-This numeric field is the reference heat recovery (volumetric) water flow rate in cubic meters per second. Entered values must be greater than zero.
-
-#### Field: Heat Recovery Water Flow Rate Function of Temperature and Power Curve Name
-
-This alpha field specifies the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of heat recovery water flow rate as a function of the inlet water temperature and net electrical power output. This field is only used if the Heat Recovery Water Flow Operating Mode is    InternalControl   . The output of this curve is multiplied by the Reference Heat Recovery Water Flow Rate to give the water flow rate at the specific inlet water temperature and net power operating conditions. This curve should be normalized to have a value of 1.0 at the reference conditions, and the curve should be valid for the range of inlet water temperatures and net electrical power output anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
-
-#### Field: Thermal Efficiency Function of Temperature and Elevation Curve Name
-
-This alpha field specifies the name of a bi-quadratic performance curve (ref: Performance Curves) that parameterizes the variation of thermal efficiency as a function of the combustion air inlet temperature and elevation. The output of this curve is multiplied by the Reference Thermal Efficiency Using Lower Heating Value to give the full-load thermal efficiency at a specific combustion air inlet temperature and elevation (i.e., at values different from the reference conditions). This curve should be normalized to have a value of 1.0 at the reference conditions, and the curve should be valid for the range of inlet air temperatures anticipated for the simulation period and for the actual elevation of the generator. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
-
-#### Field: Heat Recovery Rate Function of Part Load Ratio Curve Name
-
-This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of heat recovery to water (thermal power output) as a function of the generator   s part-load ratio (part-load ratio is the actual electrical power output divided by the full-load electrical power output at the current operating conditions). The output of this curve is multiplied by the steady-state heat recovery at the current combustion inlet air temperature and elevation to give the heat recovery rate (thermal power output) at specific part-load operating conditions. This curve should be normalized to have a value of 1.0 when the generator   s part-load ratio is 1.0, and the curve should be valid for the range of part-load ratios anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
-
-#### Field: Heat Recovery Rate Function of Inlet Water Temperature Curve Name
-
-This alpha field specifies the name of a quadratic performance curve (ref: Performance Curves) that parameterizes the variation of heat recovery to water (thermal power output) as a function of the inlet water temperature. The output of this curve is multiplied by the steady-state heat recovery at the current combustion inlet air temperature and elevation to give the heat recovery rate (thermal power output) at non-reference inlet water conditions. This curve should be normalized to have a value of 1.0 at the Reference Inlet Water Temperature, and the curve should be valid for the range of inlet water temperatures anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
-
-#### Field: Heat Recovery Rate Function of Water Flow Rate Curve Name
-
-This alpha field specifies the name of a quadratic performance curve (ref: Performance Curves) that parameterizes the variation of heat recovery to water (thermal power output) as a function of the heat recovery water flow rate. The output of this curve is multiplied by the steady-state heat recovery at the current combustion inlet air temperature and elevation to give the heat recovery rate (thermal power output) at non-reference heat recovery water flow rates. This curve should be normalized to have a value of 1.0 at the Reference Heat Recovery Water Flow Rate, and the curve should be valid for the range of water flow rates anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
-
-#### Field: Minimum Heat Recovery Water Flow Rate
-
-This numeric field specifies the minimum (volumetric) water flow rate through the heat recovery heat exchanger in cubic meters per second. The minimum input value is 0.0, and a value of 0.0 is assumed if this field is left blank.
-
-#### Field: Maximum Heat Recovery Water Flow Rate
-
-This numeric field specifies the maximum (volumetric) water flow rate through the heat recovery heat exchanger in cubic meters per second. The minimum input value for this field is 0.0, and a value of 0.0 is assumed if this field is left blank. The maximum heat recovery water flow rate must be greater than or equal to the minimum heat recovery water flow rate.
-
-#### Field: Maximum Heat Recovery Water Temperature
-
-This field sets the maximum water temperature, in degrees Celsius, that this generator can produce via heat recovery. This temperature limit puts an upper bound on the recovered heat and limits the max temperatures leaving the component.
-
-As temperatures in the water loop approach this maximum temperature, the temperature difference between the entering water and the surfaces in generator   s heat recovery heat exchanger becomes smaller. For the given heat recovery flow rate and that temperature difference the amount of heat recovered will be reduced, and eventually there will be no heat recovered when the entering water temperature is equal to the maximum temperature specified by the user in this field. The amount of heat recovered will diminish if the inlet water temperature approaches the maximum temperature, and this will show up in the reporting.
-
-#### Field: Combustion Air Inlet Node Name
-
-This alpha field specifies the name of the combustion air inlet node. If a node name is specified, this node must be an outdoor air node and must also be specified elsewhere in the input (ref: OutdoorAir:Node and OutdoorAir:NodeList). If this field is left blank, the combustion air inlet conditions are assumed to be the outdoor weather conditions used for the simulation.
-
-#### Field: Combustion Air Outlet Node Name
-
-This alpha field specifies the name of the combustion air outlet node.
-
-#### Field: Reference Exhaust Air Mass Flow Rate
-
-This numeric field is the reference exhaust air mass flow rate in kilograms per second. Entered values must be greater than zero.
-
-#### Field: Exhaust Air Flow Rate Function of Temperature Curve Name
-
-This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of exhaust air flow rate as a function of the combustion air inlet temperature. The output of this curve is multiplied by the Reference Exhaust Air Mass Flow Rate to give the exhaust air mass flow rate at non-reference combustion air inlet temperatures. This curve should be normalized to have a value of 1.0 at the Reference Combustion Air Inlet Temperature, and the curve should be valid for the range of inlet air temperatures anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
-
-#### Field: Exhaust Air Flow Rate Function of Part Load Ratio Curve Name
-
-This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of exhaust air flow rate as a function of the generator   s part-load ratio (part-load ratio is the actual electrical power output divided by the full-load electrical power output at the current operating conditions). The output of this curve is multiplied by the Reference Exhaust Air Mass Flow Rate to give the exhaust air mass flow rate at specific part-load operating conditions. This curve should be normalized to have a value of 1.0 when the generator   s part-load ratio is 1.0, and the curve should be valid for the range of part-load ratios anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
-
-#### Field: Nominal Exhaust Air Outlet Temperature
-
-This numeric field is the exhaust air outlet temperature at nominal (reference) conditions in degrees Celsius.
-
-#### Field: Exhaust Air Temperature Function of Temperature Curve Name
-
-This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of exhaust air outlet temperature as a function of the combustion air inlet temperature. The output of this curve is multiplied by the Nominal Exhaust Air Outlet Temperature to give the exhaust air temperature at non-reference combustion air inlet temperatures. This curve should be normalized to have a value of 1.0 at the Reference Combustion Air Inlet Temperature, and the curve should be valid for the range of inlet air temperatures anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
-
-#### Field: Exhaust Air Temperature Function of Part Load Ratio Curve Name
-
-This alpha field specifies the name of a quadratic or cubic performance curve (ref: Performance Curves) that parameterizes the variation of exhaust air outlet temperature as a function of the generator   s part-load ratio (part-load ratio is the actual electrical power output divided by the full-load electrical power output at the current operating conditions). The output of this curve is multiplied by the Nominal Exhaust Air Outlet Temperature to give the exhaust air temperature at specific part-load operating conditions. This curve should be normalized to have a value of 1.0 when the generator   s part-load ratio is 1.0, and the curve should be valid for the range of part-load ratios anticipated for the simulation period. If this field is left blank, the model assumes that the modifier curve is 1.0 for the entire simulation.
-
-An example IDF showing how this object is used is provided below:
-
-
-
-```idf
-Generator:MicroTurbine,
-       Generator 3,                         !- Name
-       65000,                                     !- Reference Electrical Power Output {W}
-       29900,                                     !- Minimum Full Load Electrical Power Output {W}
-       65000,                                     !- Maximum Full Load Electrical Power Output {W}
-       0.29,                                       !- Reference Electrical Efficiency Using Lower Heating Value
-       15.0,                                       !- Reference Combustion Air Inlet Temperature {C}
-       0.00638,                                 !- Reference Combustion Air Inlet Humidity Ratio (kgWater/kgDryAir)
-       0.0,                                         !- Reference Elevation {m}
-       Power_vs_Temp_Elev,           !- Electrical Power Function of Temperature and Elevation Curve Name
-       Efficiency_vs_Temp,           !- Electrical Efficiency Function of Temperature Curve Name
-       Efficiency_vs_PLR,             !- Electrical Efficiency Function of Part Load Ratio Curve Name
-       NaturalGas,                           !- Fuel Type
-       50000,                                     !- Fuel Higher Heating Value {kJ/kg}
-       45450,                                     !- Fuel Lower Heating Value {kJ/kg}
-       300,                                         !- Standby Power {W}
-       4500;                                       !- Ancillary Power {W}
-
-! Electrical Power Modifier Curve (function of temperature and elevation)
-! x = Dry-Bulb Temperature of Combustion Inlet Air (C) and y = Elevation (meters)
-   Curve:Biquadratic,
-       Power_vs_Temp_Elev,           !- Name
-       1.2027697,                             !- Coefficient1 Constant
-       -9.671305E-03,                     !- Coefficient2 x
-       -4.860793E-06,                     !- Coefficient3 x**2
-       -1.542394E-04,                     !- Coefficient4 y
-       9.111418E-09,                       !- Coefficient5 y**2
-       8.797885E-07,                       !- Coefficient6 x*y
-      -17.8,                                     !- Minimum Value of x
-       50.0,                                       !- Maximum Value of x
-       0.0,                                         !- Minimum Value of y
-       3050.;                                     !- Maximum Value of y
-
-! Electrical Efficiency Modifier Curve (function of temperature)
-! x = Dry-Bulb Temperature of Combustion Inlet Air (C)
-   Curve:Cubic,
-       Efficiency_vs_Temp,           !- Name
-       1.0402217,                             !- Coefficient1 Constant
-       -0.0017314,                           !- Coefficient2 x
-       -6.497040E-05,                     !- Coefficient3 x**2
-       5.133175E-07,                       !- Coefficient4 x**3
-       -20.0,                                     !- Minimum Value of x
-       50.0;                                       !- Maximum Value of x
-
-! Electrical Efficiency Modifier Curve (function of part-load ratio)
-! x = Part-Load Ratio (electrical load/steady-state electrical power output)
-   Curve:Cubic,
-       Efficiency_vs_PLR,             !- Name
-       0.215290,                               !- Coefficient1 Constant
-       2.561463,                               !- Coefficient2 x
-       -3.24613,                               !- Coefficient3 x**2
-       1.497306,                               !- Coefficient4 x**3
-       0.03,                                       !- Minimum Value of x
-       1.0;                                         !- Maximum Value of x!
-
-   ElectricLoadCenter:Distribution,
-       Electric Load Center,       !- Name
-       Backup Generators,             !- Generator List Name
-       DemandLimit,                         !- Generator Operation Scheme Type
-       10000.0,                                 !- Demand Limit Scheme Purchased Electric Demand Limit {W}
-       ,                                               !- Track Schedule Name Scheme Schedule Name
-       ,                                               !- Track Meter Scheme Meter Name
-       AlternatingCurrent,           !- Electrical Buss Type
-       ,                                               !- Inverter Object Name
-       ;                                               !- Electrical Storage Object Name
-
-   ElectricLoadCenter:Generators,
-       Backup Generators,             !- Name
-       Generator 1,                         !- Generator 1 Name
-       Generator:InternalCombustionEngine,   !- Generator 1 Object Type
-       50000,                                     !- Generator 1 Rated Electric Power Output
-       ON PEAK GENERATOR SCHEDULE,   !- Generator 1 Availability Schedule Name
-       ,                                               !- Generator 1 Rated Thermal to Electrical Power Ratio
-       Generator 2,                         !- Generator 2 Name
-       Generator:CombustionTurbine,   !- Generator 2 Object Type
-       30000,                                     !- Generator 2 Rated Electric Power Output
-       OFF PEAK GENERATOR SCHEDULE,   !- Generator 2 Availability Schedule Name
-       ,                                               !- Generator 2 Rated Thermal to Electrical Power Ratio
-       Generator 3,                         !- Generator 3 Name
-       Generator:MicroTurbine,   !- Generator 3 Object Type
-       65000,                                     !- Generator 3 Rated Electric Power Output
-       MID PEAK GENERATOR SCHEDULE,   !- Generator 3 Availability Schedule Name
-       ;                                               !- Generator 3 Rated Thermal to Electrical Power Ratio
-```
-
-
-### Generator:MicroTurbine Outputs
-
-The output variables that are available for the microturbine generator are:
-
-* HVAC,Average,Generator Produced Electric Power [W]
-
-* HVAC,Sum,Generator Produced Electric Energy [J]
-
-* HVAC,Average,Generator LHV Basis Electric Efficiency [-]
-
-* HVAC,Average,Generator &lt;Fuel Type&gt; HHV Basis Rate [W]
-
-* HVAC,Average,Generator Fuel HHV Basis Rate [W]
-
-* HVAC,Sum,Generator &lt;Fuel Type&gt; HHV Basis Energy [J]
-
-* HVAC,Sum,Generator Fuel HHV Basis Energy [J]
-
-* HVAC,Average,Generator &lt;Fuel Type&gt; Mass Flow Rate [kg/s]
-
-
-
-If Standby Power input field &gt; 0.0:
-
-* HVAC,Average,Generator Standby Electric Power [W]
-
-* HVAC,Sum,Generator Standby Electric Energy [J]
-
-
-
-If Ancillary Power input field &gt; 0.0:
-
-* HVAC,Average,Generator Ancillary Electric Power [W]
-
-* HVAC,Sum,Generator Ancillary Electric Energy [J]
-
-
-
-If heat recovery water inlet and outlet node names are entered (and valid):
-
-* HVAC,Average,Generator Produced Thermal Rate [W]
-
-* HVAC,Sum,Generator Produced Thermal Energy [J]
-
-* HVAC,Average,Generator Thermal Efficiency LHV Basis [-]
-
-* HVAC,Average,Generator Heat Recovery Inlet Temperature [C]
-
-* HVAC,Average,Generator Heat Recovery Outlet Temperature [C]
-
-* HVAC,Average,Generator Heat Recovery Water Mass Flow Rate [kg/s]
-
-
-
-If exhaust air calculations are performed:
-
-* HVAC,Average,Generator Exhaust Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Generator Exhaust Air Temperature   [C]
-
-
-
-
-
-#### Generator Produced Electric Power [W]
-
-This output variable is the average electric power produced by the generator in Watts for the timestep being reported. This is the    net    electric power produced, accounting for ancillary electric power consumed during generator operation.
-
-#### Generator Produced Electric Energy [J]
-
-This output variable is the electric energy produced by the generator in Joules for the timestep being reported. This output is also added to a meter with Resource Type = ElectricityProduced, End Use Key = Cogeneration, Group Key = Plant (Ref. Output:Meter objects). This is the    net    electric energy produced, accounting for ancillary electric consumption during generator operation.
-
-#### Generator LHV Basis Electric Efficiency []
-
-This output variable is the average electric efficiency of the generator (lower heating value basis) for the timestep being reported. The electric efficiency is the Generator Produced Electric Power in Watts divided by the generator   s fuel energy consumption rate in Watts (lower heating value basis).
-
-#### Generator &lt;Fuel Type&gt; HHV Basis Rate [W]
-
-This output variable is the average fuel-specific energy consumption rate of the electric generator in Watts (higher heating value basis) for the timestep being reported. &lt;Fuel Type&gt; is the name of the fuel used by this electric generator. &lt;Fuel Type&gt; can be one of the following: NaturalGas (=&gt;    Gas   ) or PropaneGas (=&gt;   Propane   ).
-
-#### Generator Fuel HHV Basis Rate [W]
-
-This output variable is the average fuel energy consumption rate of the electric generator in Watts (higher heating value basis) for the timestep being reported. The output variable name is non-fuel specific.
-
-#### Generator &lt;Fuel Type&gt; HHV Basis Energy [J]
-
-This output variable is the fuel-specific energy consumption of the electric generator in Joules (higher heating value basis) for the timestep being reported. This output is also added to a meter with Resource Type = &lt;Fuel Type&gt;, End Use Key = Cogeneration, Group Key = Plant (Ref. Output:Meter objects). &lt;Fuel Type&gt; is the name of the fuel used by this electric generator. &lt;Fuel Type&gt; can be one of the following: NaturalGas (=&gt;    Gas   ) or PropaneGas (=&gt;   Propane   ).
-
-#### Generator Fuel HHV Basis Energy [J]
-
-This output variable is the fuel energy consumption of the electric generator in Joules (higher heating value basis) for the timestep being reported. The output variable name is non-fuel specific.
-
-#### Generator &lt;Fuel Type&gt; Mass Flow Rate [kg/s]
-
-This output variable is the average mass flow rate of fuel being consumed by the electric generator in kg/s for the timestep being reported. &lt;Fuel Type&gt; is the name of the fuel used by this electric generator. &lt;Fuel Type&gt; can be one of the following: Natural Gas (=&gt;    Gas   ) or Propane Gas (=&gt;   Propane   ).
-
-#### Generator Standby Electric Power [W]
-
-This output variable is the average standby electric power consumed by the generator in Watts for the timestep being reported. Standby power is electrical power consumed by the generator (e.g., air fans and controls) when the generator is available to operate but the generator electrical power output is zero (power output is not being requested by the electric load center). This output variable is only produced when the user enters a value greater than 0.0 for the input field Standby Power.
-
-#### Generator Standby Electric Energy [J]
-
-This output variable is the standby electric energy consumption for the generator in Joules for the timestep being reported. This output is also added to a meter with Resource Type = Electricity, End Use Key = Cogeneration, Group Key = Plant (Ref. Output:Meter objects). This output variable is only produced when the user enters a value greater than 0.0 for the input field Standby Power.
-
-#### Generator Ancillary Electric Power [W]
-
-This output variable is the average ancillary electric power consumed by the generator in Watts for the timestep being reported. Ancillary power is the electrical power consumed by other associated equipment (e.g., external fuel pressurization pumps) when the generator is operating. This output variable is only produced when the user enters a value greater than 0.0 for the input field Ancillary Power.
-
-#### Generator Ancillary Electric Energy [J]
-
-This output variable is the ancillary electric energy consumption for the generator in Joules for the timestep being reported. This energy consumption is already deducted from the output variable Generator Produced Electric Energy (   net    electric energy produced by the generator). This output variable is only produced when the user enters a value greater than 0.0 for the input field Ancillary Power.
-
-#### Generator Produced Thermal Rate [W]
-
-This output variable is the average thermal power produced (i.e., exhaust energy recovery to heat water) in Watts for the timestep being reported.
-
-#### Generator Produced Thermal Energy [J]
-
-This output variable is the thermal energy produced (i.e., exhaust energy recovery to heat water) in Joules for the timestep being reported. This output is also added to a meter with Resource Type = EnergyTransfer, End Use Key = HeatRecovery, Group Key = Plant (Ref. Output:Meter objects).
-
-#### Generator Thermal Efficiency LHV Basis [-]
-
-This output variable is the average thermal efficiency of the generator (lower heating value basis) for the timestep being reported. The thermal efficiency is the Generator Produced Thermal Rate in Watts divided by the generator   s fuel energy consumption rate in Watts (lower heating value basis).
-
-#### Generator Heat Recovery Inlet Temperature [C]
-
-This output variable is the average heat recovery inlet water temperature in degrees Celsius for the timestep being reported.
-
-#### Generator Heat Recovery Outlet Temperature [C]
-
-This output variable is the average heat recovery outlet water temperature in degrees Celsius for the timestep being reported.
-
-#### Generator Heat Recovery Water Mass Flow Rate [kg/s]
-
-This output variable is the average heat recovery water mass flow rate in kilograms per second for the timestep being reported.
-
-#### Generator Exhaust Air Mass Flow Rate [kg/s]
-
-This is the mass flow rate of exhaust leaving the generator.   This output is available when the model input is setup for exhaust conditions.
-
-#### Generator Exhaust Air Temperature   [C]
-
-This is the temperature of exhaust leaving the generator.   This output is available when the model input is setup for exhaust conditions.
-
-### Generator:MicroCHP
-
-This object is used to model small-scale combined heat and power (micro CHP) electric generators using the model developed by IEA/ECBCS [Annex 42](http://www.ecbcs.org/annexes/annex42.htm). The model was developed for both internal combustion and Stirling cycle engines, but might be used for other types of residential CHP devices.
-
-Note that unlike other component models in EnergyPlus, this model is not normalized. Therefore, performance coefficients developed for one type and capacity of CHP device cannot be used for a device with a different capacity.
-
-This model is an empirical, curve fit model. This object describes the connections to the rest of the building model and includes a reference to another object called Generator:MicroCHP:NonNormalizedParameters that provides the operating characteristics.
-
-#### Field: Name
-
-This field contains a unique name for the residential CHP device.
-
-#### Field: Performance Parameters Name
-
-This field contains the name of a Generator:MicroCHP:NonNormalizedParameters object defined elsewhere in the input.
-
-#### Field: Zone Name
-
-This field contains the name of the thermal zone where the CHP device is located in the model. If the device is outdoors, or you do not want skin losses to be added to a zone, then leave this field blank.
-
-#### Field: Cooling Water Inlet Node Name
-
-This field provides the name of a node that is the inlet to the CHP device.   The node should be on the plant loop that will receive the heat from the residential CHP unit. This inlet serves as the cooling water for the CHP device.
-
-#### Field: Cooling Water Outlet Node Name
-
-This field provides the name of a node that is the outlet to the CHP device.   The node should be on the plant loop that will receive the heat from the residential CHP unit. This outlet serves as the exit of the cooling water leaving the CHP unit.
-
-#### Field: Air Inlet Node Name
-
-The name of an air node that supplies the CHP unit with air for use inside the generator.
-
-#### Field: Air Outlet Node Name
-
-The name of an air node that receives the exhaust from the CHP unit.
-
-#### Field: Generator Fuel Supply Name
-
-This field contains the name of a Generator:FuelSupply object defined elsewhere in the input file.
-
-#### Field: Availability Schedule Name
-
-This field contains the name of a schedule used to control whether or not the unit is available. It is    available    any time the value is greater than zero. If it is available, it may consume standby power at times when there is no request for power from the Electric Load Center. If it is not available (schedule value = 0.0) then the CHP unit is in a completely off    mode    and will not consume standby power. If this field is blank, the schedule has values of 1 for all time periods.
-
-An example IDF showing how this object is used is provided below:
-
-```idf
-   Generator:MicroCHP,
-       MicroCoGen1,                         !- Name
-       SENERTECH5_5KW,                   !- Performance Parameters Name
-       ZN_1_FLR_1_SEC_1,               !- Zone Name
-       MICROCHP SENERTECH Pump-MicroCoGen1Node,   !- Cooling Water Inlet Node Name
-       MICROCHP SENERTECH Supply Equipment Outlet Node,   !- Cooling Water Outlet Node Name
-       MicroCoGen1 air inlet node,   !- Air Inlet Node Name
-       ,                                               !- Air Outlet Node Name
-       NATURALGAS,                           !- Generator Fuel Supply Name
-       ALWAYS_ON;                             !- Availability Schedule Name
-```
-
-### Generator:MicroCHP:NonNormalizedParameters
-
-This object is referenced by a Generator:MicroCHP object and provides the non-normalized parameters for the MicroCHP generator model.
-
-#### Field: Name
-
-Unique name to identify this set of parameter data.
-
-#### Field: Maximum Electric Power
-
-This is the size of the CHP unit in terms of the maximum electrical power it can produce [W]. If the electric load center requests more power than this maximum, then the unit will restrict its output to this level.
-
-#### Field: Minimum Electric Power
-
-This is the size of the CHP unit in terms of the minimum electrical power it can produce [W]. If the electric load center requests less power than this minimum, then the unit will hold its output to this level.
-
-#### Field: Minimum Cooling Water Flow Rate
-
-This is the minimum flow rate of cooling water that must be available for the unit to operate [kg/s]. If the plant loop is not providing this flow of water, the unit will shut down to protect it from overheating.
-
-#### Field: Maximum Cooling Water Temperature
-
-This is the maximum temperature of cooling water inlet or outlet that can occur without the unit shutting down to protect from overheating [ &deg;C].
-
-#### Field: Electrical Efficiency Curve Name
-
-This is the name of Curve:Triquadratic object that defines the steady-state net electrical efficiency.   The electrical efficiency, <span>$ \eta_e $</span>, is a function of the cooling water mass flow rate <span> $ \dot m_{cw}  $</span>, the temperature of the cooling water at the inlet, <span>$ T_{cw} $</span>, the steady-state net electrical power produced, <span>$ P_{net,ss} $</span>.
-
-<div> \[ \eta_e = f\left( {{P_{net,ss}},{{\dot m}_{cw}},{T_{cw}}} \right) \] </div>
-
-The associated Curve:Triquadratic object should be defined with the independent variables <span> $ {P_{net,ss}},{\dot m_{cw}},{T_{cw}} $ </span>  corresponding to *x*, *y*, and *z*, respectively.
-
-#### Field: Thermal Efficiency Curve Name
-
-This is the name of a Curve:Triquadratic object that defines the steady-state net thermal efficiency.   The thermal efficiency, <span>$ \eta_q $</span>, is a function of the cooling water mass flow rate, <span>$ \dot m_{cw} $</span>, the temperature of the cooling water at the inlet, <span>$ T_{cw} $</span>, the steady-state net electrical power produced, <span> $ P_{net,ss} $ </span>.
-
-<div> \[ {\eta_q} = f\left( {{P_{net,ss}},{{\dot m}_{cw}},{T_{cw}}} \right) \] </div>
-
-The associated Curve:Triquadratic object should be defined with the independent variables <span> $ {P_{net,ss}},{\dot m_{cw}},{T_{cw}} $ </span>  corresponding to *x*, *y*, and *z*, respectively.
-
-#### Field: Cooling Water Flow Rate Mode
-
-This field is used to choose between different modes of controlling the mass flow rate of cooling water. There are two options available for this field:    PlantControl    or    InternalControl.      The    PlantControl    option indicates that the cooling water flow rate through the CHP device is determined externally (by the wider balance of plant). The    InternalControl    option indicates the flow of cooling water is controlled inside the CHP device (e.g., like an automobile   s thermostat).
-
-For internal control, the following field is used to define a Biquadratic curve that will determine the cooling water flow rate. For internal control, the CHP device should (probably) include a bypass branch when connecting to the plant loop.
-
-#### Field: Cooling Water Flow Rate Curve Name
-
-This field contains the name of a Curve:Biquadratic object that defines the mass flow rate of cooling water, <span> $ {\dot m_{cw}} $ </span>.   This field is only used if the prior field is set to InternalControl. The mass flow of cooling water is a function of steady-state power, <span> $ {P_{net,ss}} $ </span>, and the inlet temperature of the cooling water, <span> $ {T_{cw}} $ </span>.   The associated Curve:Biquadratic should be defined with the independent variables <span> $ {P_{net,ss}} $ </span> and <span> $ {T_{cw}} $ </span> corresponding to *x* and *y*, respectively.
-
-#### Field: Air Flow Rate Curve Name
-
-This is the name of a Curve:Quadratic object that defines the steady state air flow into the CHP device as a function of the mass flow rate of fuel.
-
-#### Field: Maximum Net Electrical Power Rate of Change
-
-This field contains input on the limits for how fast the generator can ramp up or down in terms of the net electrical power.
-
-#### Field: Maximum Fuel Flow Rate of Change
-
-This field contains input on the limits for how fast the generator can ramp up or down in terms of the fuel flow rates.
-
-#### Field: Heat Exchanger U-Factor Times Area Value
-
-This field describes the effective UA value for the heat exchanger that transfers heat from the generator to the cooling water.
-
-#### Field: Skin Loss U-Factor Times Area Value
-
-This field describes the effective UA value for the heat transfer from the generator to the surrounding air.
-
-#### Field: Skin Loss Radiative Fraction
-
-This field describes the split between thermal radiation and thermal convection for the heat losses from the skin of the generator.
-
-#### Field: Aggregated Thermal Mass of Energy Conversion Portion of Generator
-
-This field describes the aggregated thermal mass of the energy conversion portion of the generator. This includes the engine block in an internal combustion engine.
-
-#### Field: Aggregated Thermal Mass of Heat Recovery Portion of Generator
-
-This field describes the aggregated thermal mass of the heat recovery portion of the generator. This includes the encapsulated cooling water and heat exchanger shell in immediate thermal contact.
-
-#### Field: Standby Power
-
-This field describes the power used by the CHP unit   s control systems while in standby operation. Standby operation mode occurs whenever the unit is available but not being called upon to produce power.   Power is entered as a positive value but indicates negative generation.
-
-#### Field: Warm Up Mode
-
-This field is used to choose between different modes of controlling the warm up characteristics. Residential CHP units such as Stirling engines have different warm up characteristics than internal combustion engines.   There are two warm up modes available:      NominalEngineTemperature    or    TimeDelay.      If the former mode is input in this field, then the next three fields are used to model warm up. If the later mode is input, then the fourth field below is used to model warm up.
-
-#### Field: Warm Up Fuel Flow Rate Coefficient
-
-This field describes the value for the coefficient used to determine the rate of fuel flow during warm up. The coefficient, *k<sub>f</sub>*, is used in the following relation,
-
-<div>\[{\dot m_{fuel,warm - up}} = {\dot m_{fuel,ss - \max }} + {k_f}{\dot m_{fuel,ss - \max }}\left( {\frac{{{T_{eng,nom}} - {T_{room}}}}{{{T_{eng}} - {T_{room}}}}} \right)\]</div>
-
-#### Field: Nominal Engine Operating Temperature
-
-This field describes the nominal engine temperature during normal, steady-state operation, <span>\({T_{eng,nom}}\)</span>  [ &deg;C].
-
-#### Field: Warm Up Power Coefficient
-
-This field describes the value for the coefficient used to determine the rate of power production during warm up. The coefficient k<sub>p</sub> is used in the following relation,
-
-<div>\[{P_{net,warm - up}} = {P_{\max }}{k_p}\left( {\frac{{{T_{eng}} - {T_{room}}}}{{{T_{eng,nom}} - {T_{room}}}}} \right)\]</div>
-
-#### Field: Warm Up Fuel Flow Rate Limit Ratio
-
-This field is used to describe a limit to the fuel flow rate during warm up. The limit is a ratio multiplied by the maximum fuel flow rate during normal operation (corresponding to the fuel flow for maximum electrical power). If the warm up operating fuel flow rate is twice the steady state fuel flow at maximum power, then a value of 2.0 would be entered in this field. This field is only used with the nominal engine temperature warm up mode and is intended for Stirling engines.
-
-#### Field: Warm Up Delay Time
-
-This field is used to model the warm up operation when the warm up mode is    TimeDelay.   
-
-Enter the time between activation and power generation in seconds.
-
-#### Field: Cool Down Power
-
-This field describes the power used by the CHP unit   s ancillary systems while in cool down operation mode. Cool down operation mode occurs whenever the unit has recently been told to stop producing power.   Power here is consumed and entered as a positive value that indicates negative generation. For example, a component such as a cooling fan might continue to run during cool down.
-
-#### Field: Cool Down Delay Time
-
-This field is used to describe the time it takes for the CHP unit to cool off and complete the cool down operation. Enter the time between deactivation and the end of a cool down period in seconds.
-
-#### Field: Restart Mode
-
-This field is used to choose between two different control situations for the cool down operation. The two options for this field are    MandatoryCoolDown    and    OptionalCoolDown.        The former is used to direct the model to complete the entire cool down period before the generator can subsequently enter warm up mode. The latter directs the model to allow immediately switching to warm up mode, if power is requested before the cool down period is completed.
-
-An example IDF showing how this object is used is provided below:
-
-```idf
-   Generator:MicroCHP:NonNormalizedParameters,
-       SENERTECH5_5KW,         !- Name
-       5500.0000,              !- Maximum Electric Power {W}
-       0.0000,                 !- Minimum Electric Power {W}
-       0.0000,                 !- Minimum Cooling Water Flow Rate {kg/s}
-       80.0000,                !- Maximum Cooling Water Temperature {C}
-       SenerTechElEff,         !- Electrical Efficiency Curve Name
-       SenerTechThermEff,      !- Thermal Efficiency Curve Name
-       InternalControl,        !- Cooling Water Flow Rate Mode
-       SenerTechCoolWaterflow, !- Cooling Water Flow Rate Curve Name
-       SenerTechAirFlow,       !- Air Flow Rate Curve Name
-       1000000000.0000,        !- Maximum Net Electrical Power Rate of Change {W/s}
-       1000000000.0000,        !- Maximum Fuel Flow Rate of Change {kg/s2}
-       741.0000,               !- Heat Exchanger U-Factor Times Area Value {W/K}
-       13.7000,                !- Skin Loss U-Factor Times Area Value {W/K}
-       0.5000,                 !- Skin Loss Radiative Fraction
-       63605.6000,             !- Aggregated Thermal Mass of Energy Conversion Portion of Generator {W/K}
-       1000.7000,              !- Aggregated Thermal Mass of Heat Recovery Portion of Generator {W/K}
-       0.0000,                 !- Standby Power {W}
-       TimeDelay,              !- Warm Up Mode
-       ,                       !- Warm Up Fuel Flow Rate Coefficient
-       ,                       !- Nominal Engine Operating Temperature {C}
-       ,                       !- Warm Up Power Coefficient
-       ,                       !- Warm Up Fuel Flow Rate Limit Ratio
-       60.0000,                !- Warm Up Delay Time {s}
-       0.0000,                 !- Cool Down Power {W}
-       60.0000,                !- Cool Down Delay Time {s}
-       OptionalCoolDown;       !- Restart Mode
-```
-
-### Generator:MicroCHP Outputs
-
-* HVAC,Sum,Generator Off Mode Time [s]
-
-* HVAC,Sum,Generator Standby Mode Time [s]
-
-* HVAC,Sum,Generator Warm Up Mode Time [s]
-
-* HVAC,Sum,Generator Normal Operating Mode Time [s]
-
-* HVAC,Sum,Generator Cool Down Mode Time [s]
-
-* HVAC,Average,Generator Produced Electric Power [W]
-
-* HVAC,Sum,Generator Produced Electric Energy [J]
-
-* HVAC,Average,Generator Electric Efficiency [ ]
-
-* HVAC,Average,Generator Thermal Efficiency [ ]
-
-* HVAC,Average,Generator Gross Input Heat Rate [W]
-
-* HVAC,Average,Generator Steady State Engine Heat Generation Rate [W]
-
-* HVAC,Average, Generator Engine Heat Exchange Rate [W]
-
-* HVAC,Average,Generator Air Mass Flow Rate [kg/s]
-
-* HVAC,Average,Generator Fuel Molar Flow Rate [kmol/s]
-
-* HVAC,Average,Generator Fuel Mass Flow Rate [kg/s]
-
-* HVAC,Average,Generator Engine Temperature [C]
-
-* HVAC,Average,Generator Coolant Inlet Temperature [C]
-
-* HVAC,Average,Generator Coolant Outlet Temperature [C]
-
-* HVAC,Sum,Generator Fuel HHV Basis Energy [J]
-
-* HVAC,Average,Generator Fuel HHV Basis Rate [W]
-
-* HVAC,Sum,Generator Fuel LHV Basis Energy [J]
-
-* HVAC,Average,Generator Fuel LHV Basis Rate [W]
-
-* HVAC,Average,Generator Fuel Compressor Electric Power [W]
-
-* HVAC,Sum,Generator Fuel Compressor Electric Energy [J]
-
-* HVAC,Average,Generator Fuel Compressor Skin Heat Loss Rate [W]
-
-* HVAC,Average,Generator Zone Sensible Heat Transfer Rate [W]
-
-* HVAC,Sum,Generator Zone Sensible Heat Transfer Energy [J]
-
-* HVAC,Average,Generator Zone Convection Heat Transfer Rate [W]
-
-* HVAC,Average,Generator Zone Radiation Heat Transfer Rate [W]
-
-#### Generator Off Mode Time [s]
-
-This report is the amount of time the generator spent in    Off    mode in seconds.
-
-#### Generator Standby Mode Time [s]
-
-This report is the amount of time the generator spent in    Stand By    mode in seconds.
-
-#### Generator Warm Up Mode Time [s]
-
-This report is the amount of time the generator spent in    Warm Up    mode in seconds.
-
-#### Generator Normal Operating Mode Time [s]
-
-This report is the amount of time the generator spent in    Normal Operating    mode in seconds.
-
-#### Generator Cool Down Mode Time [s]
-
-This report is the amount of time the generator spent in    Cool Down    mode in seconds.
-
-#### Generator Produced Electric Power [W]
-
-This report is the net electrical power produced by the generator in watts.
-
-#### Generator Produced Electric Energy [J]
-
-This report is the net electrical energy produced by the generator in joules. This output variable is also put on the meter for on-site production.
-
-#### Generator Electric Efficiency [ ]
-
-This is the result for electrical efficiency.
-
-#### Generator Thermal Efficiency [ ]
-
-This is the result for thermal efficiency.
-
-#### Generator Gross Input Heat Rate [W]
-
-This is the gross rate of heat input (from fuel consumption) into the engine control volume.
-
-#### Generator Steady State Engine Heat Generation Rate [W]
-
-This is an interim value in the dynamic thermal calculation that describes the steady-state heat generation in the engine.
-
-#### Generator Engine Heat Exchange Rate [W]
-
-This is the rate of heat transfer within the generator between the engine section and the heat recovery section, in Watts.
-
-#### Generator Produced Thermal Rate [W]
-
-#### Generator Produced Thermal Energy [J]
-
-These are the rate and energy of thermal heat transferred from the engine to the heat recovery fluid in the coolant control volume.
-
-#### Generator Air Mass Flow Rate [kg/s]
-
-This is the rate of air flow thru the engine on a mass basis.
-
-#### Generator Fuel Molar Flow Rate [kmol/s]
-
-This is the rate of fuel flow thru the engine on a molar basis.
-
-#### Generator Fuel Mass Flow Rate [kg/s]
-
-This is the rate of fuel flow thru the engine on a mass basis.
-
-#### Generator Engine Temperature [C]
-
-This is the model result for engine temperature in C. This is the lumped temperature for the engine control volume.
-
-#### Generator Coolant Inlet Temperature [C]
-
-This is the temperature of the inlet water used for heat recovery. It is determined by the balance of plant connected to the generator.
-
-#### Generator Coolant Outlet Temperature [C]
-
-This report is the model prediction for the leaving temperature of water used for heat recovery. If there is no flow this is the modeled prediction for the mass of cooling water in contact with the engine.
-
-#### Generator Fuel HHV Basis Energy [J]
-
-This is the energy used by the cogeneration device in terms of higher heating value in joules. This is the output variable is also put on the meter for natural gas.
-
-#### Generator Fuel HHV Basis Rate [W]
-
-This is the rate of fuel energy use by the cogeneration device in terms of higher heating value in watts.
-
-#### Generator Fuel LHV Basis Energy [J]
-
-This is the fuel energy used by the cogeneration device in terms of lower heating value in joules.
-
-#### Generator Fuel LHV Basis Rate [W]
-
-This is the rate of fuel energy use by the cogeneration device in terms of lower heating value in watts
-
-#### Generator Zone Sensible Heat Transfer Rate [W]
-
-Rate of heat gain to zone from cogeneration unit.
-
-#### Generator Zone Sensible Heat Transfer Energy [J]
-
-Heat gains to zone from cogeneration unit.
-
-#### Generator Zone Convection Heat Transfer Rate [W]
-
-Portion of rate of heat gain to zone in the form of surface convection heat transfer.
-
-#### Generator Zone Radiation Heat Transfer Rate [W]
-
-Portion of heat gains to zone in the form of surface radiation heat transfer (to other surfaces in zone).
-
-### Generator:FuelCell
-
-This object is used to model small Fuel Cell (FC) generators. IEA/ECBCS Annex 42     see www.cogen-sim.net, developed the FC model implemented in EnergyPlus. The model can be used for two general types of fuel cells, solid oxide fuel cells (SOFC) and proton exchange membrane fuel cells (PEMFC). Warning! This is a complicated model, intended primarily for research. Because fuel cells for cogeneration (producing both heat and electricity) are not yet a mature product for building systems, the input data for this model are extremely difficult to obtain. However, the model is designed to allow investigating the relative implications of a broad array of subsystems and interactions with the building.
-
-There should be one Generator:FuelCell object for each individual FC generator in the model. Multiple fuel cell generators can be included in a given simulation. Because there are a large number of inputs to the FC model and numerous, somewhat separable subsystems within a fuel cell, the EnergyPlus input objects have been organized into a number of separate input objects. This object simply refers to the names of all the other input objects that provide the input details for individual subsystems within the fuel cell cogeneration device. The following figure diagrams these separate subsystems. (not shown is an optional stack cooler with separate connections to heat recovery water loop and surrounding zone air).
-
-![SOFCSchematic](media/image467.png)
-
-Figure 152. Fuel cell subsystems.
-
-Note that the FC model is formulated using the Lower Heating Value (LHV) of the fuel, whereas most other parts of EnergyPlus use the Higher Heating Value (HHV). LHV has important advantages over HHV in the context of the quality of heat recovered. While model coefficients for input performance descriptions are to be based on LHV, energy consumption and tariff calculations are also reported on HHV basis when using this model.
-
-#### Field: Name
-
-This field contains a unique name for the fuel cell.
-
-#### Field: Power Module Name
-
-This field contains the name of a Generator:FuelCell:PowerModule input object.
-
-#### Field: Air Supply   Name
-
-This field contains the name of a Generator:FuelCell:AirSupply input object.
-
-#### Field: Fuel Supply Name
-
-This field contains the name of a Generator:FuelSupply input object.
-
-#### Field: Water Supply Name
-
-This field contains the name of a Generator:FuelCell:WaterSupply input object.
-
-#### Field: Auxiliary Heater Name
-
-This field contains the name of a Generator:FuelCell:AuxiliaryHeater input object.
-
-#### Field: Heat Exchanger Name
-
-This field contains the name of a Generator:FuelCell:ExhaustGasToWaterHeatExchanger input object.
-
-#### Field: Electrical Storage Name
-
-This field contains the name of a Generator:FuelCell:ElectricalStorage input object.
-
-#### Field: Inverter Name
-
-This field contains the name of a Generator:FuelCell:Inverter input object.
-
-#### Field: Stack Cooler Name
-
-This field contains the name of a Generator:FuelCell:StackCooler input object. This is optional. The presence of a stack cooler distinguishes between SOFC and PEMFC with PEMFC operating at lower temperatures and requiring a separate subsystem to maintain stack temperatures.
-
-An example input data file (IDF) entry for this object is provided below:
-
-```idf
-   Generator:FuelCell,
-       FCT SOFC,                               !- Name
-       FCT SOFC Power Module,     !- Power Module Name
-       FCT SOFC Air Supply,         !- Air Supply Name
-       FCT SOFC Fuel Supply,       !- Fuel Supply Name
-       FCT SOFC Water Supply,     !- Water Supply Name
-       FCT SOFC Auxiliary Heater,   !- Auxiliary Heater Name
-       FCT SOFC Exhaust HX,         !- Heat Exchanger Name
-       FCT SOFC Battery,               !- Electrical Storage Name
-       FCT SOFC Inverter;             !- Inverter Name
-```
-
-
-### Generator:FuelCell Outputs
-
-The following output variables are available for the fuel cell model.
-
-* Output:Variable,\*,Generator Produced Electric Power,hourly; !- HVAC Average [W]
-
-* Output:Variable,\*,Generator Produced Electric Energy,hourly; !- HVAC Sum [J]
-
-* Output:Variable,\*,Generator Produced Thermal Rate,hourly; !- HVAC Average [W]
-
-* Output:Variable,\*,Generator Produced Thermal Energy,hourly; !- HVAC Sum [J]
-
-* Output:Variable,\*,Generator Fuel HHV Basis Energy,hourly; !- HVAC Sum [J]
-
-* Output:Variable,\*,Generator Fuel HHV Basis Rate,hourly; !- HVAC Average [W]
-
-* Output:Variable,\*,Generator Fuel LHV Basis Energy,hourly; !- HVAC Sum [J]
-
-* Output:Variable,\*,Generator Fuel Consumption Rate LHV Basis,hourly; !- HVAC Average [W]
-
-* Output:Variable,\*,FuelCell Heat Loss Rate to Zone,hourly; !- HVAC Average [W]
-
-* Output:Variable,\*,FuelCell Heat Loss Energy to Zone,hourly; !- HVAC Sum [J]
-
-* Output:Variable,\*,FuelCell Convection Heat Loss Rate to Zone,hourly; !- HVAC Average [W]
-
-* Output:Variable,\*,FuelCell Radiation Heat Loss Rate to Zone,hourly; !- HVAC Average [W]
-
-#### Generator Produced Electric Power [W]
-
-This report is the net electrical power produced by the generator in watts.
-
-#### Generator Produced Electric Energy [J]
-
-This report is the net electrical energy produced by the generator in joules. This output variable is also put on the meter for on-site production.
-
-#### Generator Produced Thermal Rate [W]
-
-#### Generator Produced Thermal Energy [J]
-
-These are the rate and energy of thermal heat transferred from the engine to the heat recovery fluid in the coolant control volume.
-
-#### Generator Fuel HHV Basis Energy [J]
-
-This is the energy used by the cogeneration device in terms of higher heating value in joules. This is the output variable is also put on the meter for natural gas.
-
-#### Generator Fuel HHV Basis Rate [W]
-
-This is the rate of fuel energy use by the cogeneration device in terms of higher heating value in watts.
-
-#### Generator Fuel LHV Basis Energy [J]
-
-This is the fuel energy used by the cogeneration device in terms of lower heating value in joules.
-
-#### Generator Fuel Consumption Rate LHV Basis [W]
-
-This is the rate of fuel energy use by the cogeneration device in terms of lower heating value in watts.
-
-#### Generator Zone Sensible Heat Transfer Rate [W]
-
-This variable provides the results for the total rate of skin losses from the fuel cell to the surrounding zone.
-
-#### Generator Zone Sensible Heat Transfer Energy [J]
-
-This variable provides the results for the total energy in skin losses from the fuel cell to the surrounding zone.
-
-#### Generator Zone Convection Heat Transfer Rate [W]
-
-This variable provides the results for the rate of skin losses in the form of surface convection heat transfer from the fuel cell to the surrounding zone.
-
-#### Generator Zone Radiation Heat Transfer Rate [W]
-
-This variable provides the results for the rate of skin losses in the form of radiation heat transfer from the fuel cell to the surrounding zone.
-
-Using the FC model with DisplayAdvancedReportVariables (see Diagnostics object or use of operating system   s environment variables) makes the following output variables available as listed in the RDD file. There are a large number of output variables that provide access to the inner workings of the model and individual subsystems that are not likely to be useful for the average user.
-
-* HVAC,Average,Generator Air Inlet Temperature [C]
-
-* HVAC,Average,Generator Power Module Entering Air Temperature [C]
-
-* HVAC,Average,Generator Air Molar Flow Rate [kmol/s]
-
-* HVAC,Average,Generator Power Module Entering Air Enthalpy [W]
-
-* HVAC,Average,Generator Blower Electric Power [W]
-
-* HVAC,Sum,Generator Blower Electric Energy [J]
-
-* HVAC,Average,Generator Blower Skin Heat Loss Rate [W]
-
-* HVAC,Average,Generator Fuel Inlet Temperature [C]
-
-* HVAC,Average,Generator Power Module Entering Fuel Temperature [C]
-
-* HVAC,Average,Generator Fuel Molar Flow Rate [kmol/s]
-
-* HVAC,Average,Generator Power Module Entering Fuel Enthalpy [W]
-
-* HVAC,Average,Generator Fuel Compressor Electric Power [W]
-
-* HVAC,Sum,Generator Fuel Compressor Electric Energy [J]
-
-* HVAC,Average,Generator Fuel Compressor Skin Heat Loss Rate [W]
-
-* HVAC,Average,Generator Fuel Reformer Water Inlet Temperature [C]
-
-* HVAC,Average,Generator Power Module Entering Reforming Water Temperature [C]
-
-* HVAC,Average,Generator Fuel Reformer Water Molar Flow Rate [kmol/s]
-
-* HVAC,Average,Generator Fuel Reformer Water Pump Electric Power [W]
-
-* HVAC,Sum,Generator Fuel Reformer Water Pump Electric Energy [J]
-
-* HVAC,Average,Generator Power Module Entering Reforming Water Enthalpy [W]
-
-* HVAC,Average,Generator Product Gas Temperature [C]
-
-* HVAC,Average,Generator Product Gas Enthalpy [W]
-
-* HVAC,Average,Generator Product Gas Molar Flow Rate [kmol/s]
-
-* HVAC,Average,Generator Product Gas Ar Molar Flow Rate [kmol/s]
-
-* HVAC,Average,Generator Product Gas CO2 Molar Flow Rate [kmol/s]
-
-* HVAC,Average,Generator Product Gas H2O Vapor Molar Flow Rate [kmol/s]
-
-* HVAC,Average,Generator Product Gas N2 Molar Flow Rate [kmol/s]
-
-* HVAC,Average,Generator Product Gas O2 Molar Flow Rate [kmol/s]
-
-* HVAC,Average,Generator Inverter Loss Power [W]
-
-* HVAC,Average,Generator Produced DC Electric Power [W]
-
-* HVAC,Average,Generator DC Power Efficiency [ ]
-
-* HVAC,Average,Generator Electric Storage Charge State [J]
-
-* HVAC,Average,Generator Produced DC Electric Power [W]
-
-* HVAC,Sum,Generator DC Storage Charging Energy [J]
-
-* HVAC,Average,Generator DC Storage Discharging Power [W]
-
-* HVAC,Sum,Generator DC Storage Discharging Energy [J]
-
-* HVAC,Average,Generator Ancillary AC Electric Power [W]
-
-* HVAC,Sum,Generator Ancillary AC Electric Energy [J]
-
-* HVAC,Average,Generator Zone Sensible Heat Transfer Rate [W]
-
-* HVAC,Sum,Generator Zone Sensible Heat Transfer Energy [J]
-
-* HVAC,Average,Generator Zone Convection Heat Transfer Rate [W]
-
-* HVAC,Average,Generator Zone Radiation Heat Transfer Rate [W]
-
-* HVAC,Sum, Generator Fuel Cell Model Iteration Count [ ]
-
-* HVAC,Sum,Generator Regula Falsi Iteration Count [ ]
-
-#### Generator Air Inlet Temperature [C]
-
-This variable provides the temperature of air supplied to the FC.
-
-#### Generator Power Module Entering Air Temperature [C]
-
-This variable provides the temperature of the air supplied to the power module after it has gone through the blower and received any heat recovered from other subsystems.
-
-#### Generator Air Molar Flow Rate [kmol/s]
-
-This variable provides the results for <span>\({\dot N_{air}}\)</span>, the flow rate of air into the FC.
-
-#### Generator Power Module Entering Air Enthalpy [W]
-
-This variable provides the results for <span>\({\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\hat h}_i} - {\Delta_f}\hat h_i^0} \right]} \right)}_{air}}\)</span>, which is the enthalpy flow in the air stream entering the power module relative to 25 &deg;C.
-
-#### Generator Blower Electric Power [W]
-
-This variable provides the results for <span>\({P_{blower - el}}\)</span>, which is the electrical power used by the air supply blower.
-
-#### Generator Blower Electric Energy [J]
-
-This variable provides the results for the energy used by the air supply blower. It is also added to the appropriate meters.
-
-#### Generator Blower Skin Heat Loss Rate [W]
-
-This variable provides the results for <span>\({q_{blower - heat - loss}}\)</span>, which is the rate of energy    lost    to the surroundings.
-
-#### Generator Fuel Inlet Temperature [C]
-
-This variable provides the temperature of the fuel supplied to the FC.
-
-#### Generator Power Module Entering Fuel Temperature [C]
-
-This variable provides the temperature of the fuel supplied to the power module after it has gone through the compressor.
-
-#### Generator Fuel Molar Flow Rate [kmol/s]
-
-This variable provides the results for <span>\({\dot N_{fuel}}\)</span>, which is the flow rate of fuel into the FC.
-
-#### Generator Power Module Entering Fuel Enthalpy [W]
-
-This variable provides the results for <span>\({\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\hat h}_i} - {\Delta_f}\hat h_i^0} \right]} \right)}_{fuel}}\)</span>, which is the enthalpy flow in the fuel stream entering the power module relative to 25 &deg;C.
-
-#### Generator Fuel Compressor Electric Power [W]
-
-This variable provides the results for <span>\({P_{comp - el}}\)</span>, which is the electrical power used by the fuel supply compressor.
-
-#### Generator Fuel Compressor Electric Energy [J]
-
-This variable provides the results for the energy used by the fuel supply compressor. It is also added to the appropriate meters.
-
-#### Generator Fuel Compressor Skin Heat Loss Rate [W]
-
-This variable provides the results for the rate of energy    lost    to the surroundings.
-
-#### Generator Fuel Reformer Water Inlet Temperature [C]
-
-This variable provides the temperature of the water supplied to the FC for reforming.
-
-#### Generator Power Module Entering Reforming Water Temperature [C]
-
-This variable provides the temperature of the water supplied to the power module after it has gone through the pump.
-
-#### Generator Fuel Reformer Water Molar Flow Rate [kmol/s]
-
-This variable provides the results for <span>\({\dot N_{water}}\)</span>, which the flow rate of reforming water into the FC.
-
-#### Generator Fuel Reformer Water Pump Electric Power [W]
-
-This variable provides the results for <span>\({P_{pump - el}}\)</span>, which is the electrical power used by the water pump.
-
-#### Generator Fuel Reformer Water Pump Electric Energy [J]
-
-This variable provides the results for energy used by the water pump. It is also added to the appropriate meters.
-
-#### Generator Power Module Entering Reforming Water Enthalpy [W]
-
-This variable provides the results for <span>\({\dot H_{liq - water}}\)</span>  which is the enthalpy flow of the water stream entering the power module relative to 25 &deg;C.
-
-#### Generator Product Gas Temperature [C]
-
-This variable provides the results for the temperature of the product gas stream leaving the fuel cell power module.
-
-#### Generator Product Gas Enthalpy [W]
-
-This variable provides the results for <span>\({\sum\limits_i {\left( {{{\dot N}_i} \cdot \left[ {{{\hat h}_i} - {\Delta_f}\hat h_i^0} \right]} \right)}_{FCPM - cg}}\)</span>, which is the enthalpy flow in the product gas stream leaving the power module relative to 25 &deg;C.
-
-#### Generator Product Gas Molar Flow Rate [kmol/s]
-
-This variable provides the results for the flow rate of all the product gases leaving the fuel cell power module.
-
-#### Generator Product Gas Ar Molar Flow Rate [kmol/s]
-
-This variable provides the results for the flow rate of the argon gas leaving the fuel cell power module.
-
-#### Generator Product Gas CO2 Molar Flow Rate [kmol/s]
-
-This variable provides the results for the flow rate of the carbon dioxide gas leaving the fuel cell power module.
-
-#### Generator Product Gas H2O Vapor Molar Flow Rate [kmol/s]
-
-This variable provides the results for the flow rate of the water gas leaving the fuel cell power module.
-
-#### Generator Product Gas N2 Molar Flow Rate [kmol/s]
-
-This variable provides the results for the flow rate of the nitrogen gas leaving the fuel cell power module.
-
-#### Generator Product Gas O2 Molar Flow Rate [kmol/s]
-
-This variable provides the results for the flow rate of the oxygen gas leaving the fuel cell power module.
-
-#### Generator Inverter Loss Power [W]
-
-This variable provides the results for the power losses associated with inefficiencies in the inverter.
-
-#### Generator Produced DC Electric Power [W]
-
-This variable provides the results for <span>\({P_{el}}\)</span>, which is the net DC electrical power produced by the fuel cell power module.
-
-#### Generator DC Power Efficiency [ ]
-
-This variable provides the results for <span>\({\varepsilon_{el}}\)</span>, which is the electrical efficiency of the fuel cell power module.
-
-#### Generator Electric Storage Charge State [J]
-
-This variable provides the results for state of charge of the electrical storage device inside the fuel cell. Although the units are Joules, this is a state variable and is reported as an average rather than a sum.
-
-#### Generator Produced DC Electric Power [W]
-
-This variable provides the rate at which power was stored into the fuel cell   s electrical storage subsystem.
-
-#### Generator DC Storage Charging Energy [J]
-
-This variable provides the energy stored into the fuel cell   s electrical storage subsystem.
-
-#### Generator DC Storage Discharging Power [W]
-
-This variable provides the rate at which power was drawn from the fuel cell   s electrical storage subsystem.
-
-#### Generator DC Storage Discharging Energy [J]
-
-This variable provides the energy drawn from the fuel cell   s electrical storage subsystem.
-
-#### Generator Ancillary AC Electric Power [W]
-
-This variable provides the results for <span>\({P_{el,ancillaries - AC}}\)</span>, which is the rate at which ancillary devices within the power module use electricity supplied to the fuel cell by an external source.
-
-#### Generator Ancillary AC Electric Energy [J]
-
-This variable provides the results for the energy used by AC ancillaries. It is also added to the appropriate meters.
-
-#### Generator Fuel Cell Model Iteration Count   [ ]
-
-This variable provides information on the numerical method used to calculate the FC model. EnergyPlus uses a sequential substitution iterative algorithm to solve the main heat balance equation for the FC model. This output variable indicates the number of iterations needed to converge.
-
-#### Generator Regula Falsi Iteration Count [ ]
-
-This variable provides information on the numerical method used to calculate product gas temperature as a function of the product gas   s enthalpy. A Regula Falsi numerical method is used to invert the Shomate equation for enthalpy as a function of temperature. This output variable indicates the number of iterations needed for the Regula Falsi method to converge.
-
-#### Generator Heat Recovery Exit Gas Temperature [C]
-
-This is the temperature of the exiting gas for heat recovery in C.
-
-#### Generator Heat Recovery Exit Gas H2O Vapor Fraction []
-
-This is the water vapor fraction in the exit gas.
-
-#### Generator Heat Recovery Water Condensate Molar Flow Rate [kmol/s]
-
-This is the flow of condensed water in kmol/s.
-
-### Generator:FuelCell:PowerModule
-
-This object is used to describe the core power module subsystem of the FC. This includes the fuel cell stack, fuel reformer, and whatever ancillary devices are included inside. If the model has multiple FC generators that are of the exact same type, then only one of these objects is needed and all the Generator:FuelCell can reference it. The model uses a number of curves to describe operating performance. Input data for specific models of FC are not yet available but will be produced by IEA Annex 42 and should be available in the future.
-
-#### Field: Name
-
-This field contains a unique name for the fuel cell power module subsystem.
-
-#### Field: Efficiency Curve Mode
-
-This field is used to choose between different modes of inputting the electrical efficiency curve. There are two options available for this Field:    Annex42    and    Normalized   . The    Annex42    option indicates that the efficiency curves are not normalized and are used for the single size and type of FC product. The    Normalized    option indicates that the efficiency curves are normalized (as is standard practice in EnergyPlus) relative to a single rating point. In the Annex42 mode, the curves directly represent efficiency as a function of fuel use, but in the Normalized mode, the curves represent an efficiency modification that is applied to the efficiency at the rating point.
-
-#### Field: Efficiency Curve Name
-
-This field contains the name of a Curve:Quadratic input object described elsewhere in the input file. The curve is a function of the net DC electric power, <span>\({P_{el}}\)</span>  (W), produced by the power module and describes either the electrical efficiency or the how the efficiency is modified depending on the mode selected in the previous field. This quadratic curve is just one part of the entire parametric relation used to describe electrical efficiency <span>\({\varepsilon_{el}}\)</span>. For the Annex42 mode the full relation for efficiency is,
-
-<div>\[{\varepsilon_{el}} = \left[ {{\varepsilon_0} + {\varepsilon_1} \cdot {P_{el}} + {\varepsilon_2} \cdot P_{el}^2} \right] \cdot \left[ {1 - {N_{stops}} \cdot D} \right] \cdot \left[ {1 - (MAX(\int\limits_{} {dt - {t_{threshold}},0.0))}  \cdot L} \right]\]</div>
-
-where the Curve:Quadratic input object named in this field serves to define the quadratic portion in the first set of brackets. For the Normalized mode the full relation for efficiency is,
-
-<div>\[{\varepsilon_{el}} = \left[ {{\varepsilon_0} + {\varepsilon_1} \cdot \frac{{{P_{el}}}}{{{P_{nom}}}} + {\varepsilon_2} \cdot {{\left( {\frac{{{P_{el}}}}{{{P_{nom}}}}} \right)}^2}} \right] \cdot {\varepsilon_{nom}} \cdot \left[ {1 - {N_{stops}} \cdot D} \right] \cdot \left[ {1 - (MAX(\int\limits_0 {dt - {t_{threshold}},0.0))}  \cdot L} \right]\]</div>
-
-where <span>\({\varepsilon_{nom}}\)</span>  is the nominal electrical efficiency at the rating point <span>\({P_{nom}}\)</span>  which are described in the next two fields. The Normalized mode may be more useful for a simulation study that needs to vary the capacity of the FC.
-
-#### Field: Nominal Efficiency
-
-This field is used for the    Normalized    efficiency curve mode and provides the nominal efficiency <span>\({\varepsilon_{nom}}\)</span>  (dimensionless) at the rating point. This field can be left blank if using the    Annex42    mode.
-
-#### Field: Nominal Electrical Power
-
-This field is used for the    Normalized    efficiency curve mode and provides the nominal net DC electrical power produced <span>\({P_{nom}}\)</span>  (W) at the rating point. This field can be left blank if using the    Annex42    mode.
-
-#### Field: Number of Stops at Start of Simulation
-
-This field is used to describe the number of times the FC has been cycled on and off prior to the start of the simulation. FC products might degrade as a result of starting and stopping the fuel cell stack, so the model includes terms to model the degradation effects of cycling FC units on and off. This is the initial value of the <span>\({N_{stops}}\)</span>*<sub>  </sub>*term in the efficiency relation above.
-
-#### Field: Cycling Performance Degradation Coefficient
-
-This field is used to describe the fixed value representing the fractional performance degradation associated with each start and stop cycle. This is the value of <span>\(D\)</span>  in the efficiency relations above. If there is no degradation from cycling, then D should be 0.0.
-
-#### Field: Number of Run Hours at Beginning of Simulation
-
-This field is used to describe the amount of time the FC has been operating prior to the start of the simulation. FC products might degrade over time so the model includes terms to model the degradation effects of FC run time. This is the initial value of the integrated run time term <span>\(\int\limits_0 {dt} \)</span>.
-
-#### Field: Accumulated Run Time Degradation Coefficient
-
-This field is used to describe the fixed value representing the fractional performance degradation associated with the total amount of run time. This is the value of <span>\(L\)</span>  in the efficiency relations above. If there is no degradation from run time, the L should be 0.0.
-
-#### Field: Run Time Degradation Initiation Time Threshold
-
-This field is used to describe the time period for which there is no degradation associated with the amount of run time. This provides the ability to model a system that initially operates without degradation for some period time before it starts to degrade. This is the value of <span>\({t_{threshold}}\)</span>  in the efficiency relations above.
-
-#### Field: Power Up Transient Limit
-
-This field is used to describe the maximum allowable rate at which the fuel cell can increase the level of power it produces (W/s). This is a time derivative of the net DC electrical power used to limit how fast the FC can ramp up.
-
-#### Field: Power Down Transient Limit
-
-This field is used to describe the maximum allowable rate at which the fuel cell can decrease the level of power it produces (W/s). This is a time derivative of the net DC electrical power used to limit how fast the FC can ramp down.
-
-#### Field: Start Up Time
-
-This field is used to describe the length of time (seconds) of the start up period when the FC is turned on.
-
-#### Field: Start Up Fuel
-
-This field is used to describe the amount of fuel (kmol) used during the entire start up period. The fuel is the same type as what is described in the Generator:FuelSupply object elsewhere in the input file.
-
-#### Field: Start Up Electricity Consumption
-
-This field is used to describe the amount of electricity (Joules) used by ancillary equipment during the entire start up period.
-
-#### Field: Start Up Electricity Produced
-
-This field is used to describe the amount of electricity (Joules) produced by the power module during the entire start up period.
-
-#### Field: Shut Down Time
-
-This field is used to describe the length of time (seconds) of the shut down period.
-
-#### Field: Shut Down Fuel
-
-This field is used to describe the amount of fuel (kmol) used during the entire shut down period. The fuel is the same type as what is described in the Generator:FuelSupply object elsewhere in the input file.
-
-#### Field: Shut Down Electricity Consumption
-
-This field is used to describe the amount of electricity (J) used by ancillary equipment during the entire shut down period.
-
-#### Field: Ancillary Electricity Constant Term
-
-This field is used to describe the constant term, <span>\(an{c_0}\)</span>, in a relation that describes the AC electrical power used by ancillary equipment located inside the power module, <span>\({P_{el,ancillaries - AC}}\)</span>. The model uses this relation,
-
-<div>\[{P_{el,ancillaries - AC}} = an{c_0} + an{c_1} \cdot {\dot N_{fuel}}\]</div>
-
-where <span>\({\dot N_{fuel}}\)</span>  is the rate of fuel use in the power module (kmol/s).
-
-#### Field: Ancillary Electricity Linear Term
-
-This field is used to describe the linear term, <span>\(an{c_1}\)</span>, in the relation shown in the previous field.
-
-#### Field: Skin Loss Calculation Mode
-
-This field is used to select the mode for how skin losses are modeled. Skin losses are heat energy    lost    from the power module and transferred to the surrounding thermal zone named in the following field.   There are three alpha options to choose from:    ConstantRate   ,    UAForProcessGasTemperature   , or    QuadraticFunctionOfFuelRate.      Enter ConstantRate in this field to model skin losses using a constant rate, e.g. 100 watts. Enter UAForProcessGasTemperature to model skin losses using a    UA-Delta-T    calculation method with the temperature difference determined by the power module   s product gas temperature and the surrounding zone. Enter QuadraticFunctionOfFuelRate to model skin losses as a function of the rate of fuel use.
-
-#### Field: Zone Name
-
-This field is used to describe the thermal zone that will receive skin and other heat losses from the FC. This should be the name of a Zone input object declared elsewhere in the input file.
-
-#### Field: Skin Loss Radiative Fraction
-
-This field is used to describe the portion of skin losses that are in the form of thermal radiation. This controls the radiative/convective split for the energy transferred to the zone by the FC.
-
-#### Field: Constant Skin Loss Rate
-
-This field is used to describe the constant rate of skin losses (W). This field is used with the ConstantRate mode. It can be left blank for other skin loss modes.
-
-#### Field: Skin Loss U-Factor Times Area Term
-
-This field is used to describe the    UA    term (W/K). This field is used with the UAForProcessGasTemperature mode. It can be left blank for other skin loss modes.    UA    is the product of the overall heat transfer coefficient    U    and the area    A.   
-
-#### Field: Skin Loss Quadratic Curve Name
-
-This field is used to refer to the name of a quadratic curve object defined elsewhere in the input file. The quadratic curve should define skin heat loss rate as a function of the fuel use rate (kmol/s) so that,
-
-<div>\[{q_{skin - loss}} = {s_0} + {s_1} \cdot {\dot N_{fuel}} + {s_2} \cdot \dot N_{fuel}^2\]</div>
-
-#### Field: Dilution Air Flow Rate
-
-This field is used to describe the rate of dilution air (kmol/sec) drawn into, or through, the power module. This air stream may not be present in all FC products. It is used for limiting skin and stack heat losses and for strategies that mitigate potential safety issue were fuel gases to escape the stack.
-
-#### Field: Stack Heat loss to Dilution Air
-
-This field is used to describe the rate at which the fuel cell stack adds energy to the dilution air stream. It is entered as a constant heat rate (W).
-
-#### Field: Dilution Inlet Air Node Name
-
-This field is used to describe the air node where the dilution air is drawn from. This would typically be the name of the air node associated with the thermal zone where the FC is located.
-
-#### Field: Dilution Outlet Air Node Name
-
-This field is used to describe the air node where the dilution air is exhausted to. This could be the inlets to a heat recovery ventilator or an exhaust node.
-
-#### Field: Minimum Operating Point
-
-This field is used to describe the minimum operating point for the net DC electric power, <span>\({P_{el}}\)</span>  (W).
-
-#### Field: Maximum Operating Point
-
-This field is used to describe the maximum operating point for the net DC electric power, <span>\({P_{el}}\)</span>  (W).
-
-An example input data file (IDF) entry for this object is provided below:
-
-```idf
-Generator:FuelCell:PowerModule,
-       FCT SOFC Power Module,     !- Name
-       Annex42,                                 !- Efficiency Curve Mode
-       FCT Power Curve,                 !- Efficiency Curve Name
-       0.354,                                     !- Nominal Efficiency
-       3400,                                       !- Nominal Electrical Power {W}
-       0,                                             !- Number of Stops at Start of Simulation
-       0.0,                                         !- Cycling Performance Degradation Coefficient
-       0,                                             !- Number of Run Hours at Beginning of Simulation {hr}
-       0.0,                                         !- Accumulated Run Time Degradation Coefficient
-       10000,                                     !- Run Time Degradation Initiation Time Threshold {hr}
-       1.4,                                         !- Power Up Transient Limit {W/s}
-       0.2,                                         !- Power Down Transient Limit {W/s}
-       0.0,                                         !- Start Up Time {s}
-       0.2,                                         !- Start Up Fuel {kmol}
-       ,                                               !- Start Up Electricity Consumption {J}
-       0.0,                                         !- Start Up Electricity Produced {J}
-       0.0,                                         !- Shut Down Time {s}
-       0.2,                                         !- Shut Down Fuel {kmol}
-       ,                                               !- Shut Down Electricity Consumption {J}
-       0.0,                                         !- Ancillary Electricity Constant Term
-       0.0,                                         !- Ancillary Electricity Linear Term
-       ConstantRate,                       !- Skin Loss Calculation Mode
-       ZN_1_FLR_1_SEC_5,               !- Zone Name
-       0.6392,                                   !- Skin Loss Radiative Fraction
-       729,                                         !- Constant Skin Loss Rate {W}
-       0.0,                                         !- Skin Loss U-Factor Times Area Term {W/K}
-       ,                                               !- Skin Loss Quadratic Curve Name
-       6.156E-3,                               !- Dilution Air Flow Rate {kmol/s}
-       2307,                                       !- Stack Heat loss to Dilution Air {W}
-       SOFC Air HR Inlet,             !- Dilution Inlet Air Node Name
-       SOFC Air HR Outlet,           !- Dilution Outlet Air Node Name
-       3010,                                       !- Minimum Operating Point {W}
-       3728;                                       !- Maximum Operating Point {W}
-```
-
-### Generator:FuelCell:StackCooler
-
-This object is optional and is used to define details needed to model the stack cooler on PEMFC.
-
-#### Field: Name
-
-This field contains a unique name for the PEM fuel cell stack cooler
-
-#### Field: Heat Recovery Water Inlet Node Name
-
-This field contains the node name for the water inlet to the stack cooler.
-
-#### Field: Heat Recovery Water Outlet Node Nane
-
-This field contains the node name for the water outlet from the stack cooler.
-
-#### Field: Nominal Stack Temperature
-
-This field contains the nominal stack operating temperature for the PEMFC, <span>\(T_{stack}^o\)</span>. This field and the next five provide values for use in the empirical equation for the rate of heat extracted from the fuel cell power module by the stack cooler using the following relation
-
-<div>\[{q_{s - cool}} = \left[ {{r_0} + {r_1}\left( {{T_{stack}} - T_{stack}^o} \right)} \right] \cdot \left[ {1 + {r_2}{P_{el}} + {r_3}P_{el}^2} \right]\]</div>
-
-#### Field: Actual Stack Temperature]
-
-This field contains the actual stack operating temperature for the PEMFC, <span>\({T_{stack}}\)</span>.
-
-#### Field: Coefficient r0
-
-This field contains the coefficient r<sub>0</sub> in the equation above.
-
-#### Field: Coefficient r1
-
-This field contains the coefficient r<sub>1</sub> in the equation above.
-
-#### Field: Coefficient r2
-
-This field contains the coefficient r<sub>2</sub> in the equation above.
-
-#### Field: Coefficient r3
-
-This field contains the coefficient r<sub>3</sub> in the equation above.
-
-#### Field: Stack Coolant Flow Rate
-
-The stack cooler is assumed to have a closed water circulation loop that is used to extract heat from the stack and move it to a cogeneration heat exchanger and/or an air cooler. This field is used to enter the flow rate of coolant in this loop.
-
-#### Field: Stack Cooler U-Factor Times Area Value
-
-This is the heat transfer coefficient between the stack and the coolant.
-
-#### Field: Fs-cogen Adjustment Factor
-
-This field provides the value for an adjustment factor, <span>\({F_{s - cogen}}\)</span>, used in the following relation for the cogeneration heat transfer coefficient, <span>\({\left( {UA} \right)_{s - cogen}}\)</span>:
-
-<div>\[{\left( {UA} \right)_{s - cogen}} = {\left[ {\frac{1}{{{{\left( {hA} \right)}_{s - cogen}}}} + {F_{s - cogen}}} \right]^{ - 1}}\]</div>
-
-#### Field: Stack Cogeneration Exchanger Area
-
-This field provides the value for the cogeneration heat exchanger area, <span>\({A_{s - cogen}}\)</span>
-
-#### Field: Stack Cogeneration Exchanger Nominal Flow Rate
-
-This field provides the value for <span>\(\dot N_{s - cogen}^0\)</span>  in the following relation for the cogeneration heat exchanger convection coefficient, <span>\({h_{s - cogen}}\)</span>:
-
-<div>\[{h_{s - cogen}} = h_{s - cogen}^0 \cdot {\left( {\frac{{{{\dot N}_{s - cogen}}}}{{\dot N_{s - cogen}^0}}} \right)^{{n_s}}}\]</div>
-
-#### Field: Stack Cogeneration Exchanger Nominal Heat Transfer Coefficient
-
-This field provides the value for <span>\(h_{s - cogen}^0\)</span>  in the relation above for the cogeneration heat exchanger convection coefficient, <span>\({h_{s - cogen}}\)</span>.
-
-#### Field: Stack Cogeneration Exchanger Nominal Heat Transfer Coefficient Exponent
-
-This field provides the value for <span>\({n_s}\)</span>  is the relation above for the cogeneration heat exchanger convection coefficient, <span>\({h_{s - cogen}}\)</span>.
-
-#### Field: Stack Cooler Pump Power
-
-This field is the power used by the stack cooler   s circulating pump in Watts. It is a constant power draw whenever the stack cooler is active.
-
-#### Field: Stack Cooler Pump Heat loss
-
-This field is the fraction of the pump power consumption that is lost to the surround zone.
-
-#### Field: Stack Air Cooler Fan Coefficient f0
-
-This field and the next two are used to define coefficients for the following relation for the power used by the air-cooler   s fan to dump excess heat into the surrounding zone:
-
-<div>\[{P_{s - air - el}} = {f_0} + {f_1} \cdot {q_{s - air}} + {f_2} \cdot q_{s - air}^2\]</div>
-
-#### Field: Stack Air Cooler Fan Coefficient f1
-
-This field provides a value for the coefficient *f<sub>1</sub>* in the relation above.
-
-#### Field: Stack Air Cooler Fan Coefficient f2
-
-This field provides a value for the coefficient *f<sub>2</sub>* in the relation above.
-
-### Generator:FuelCell:AirSupply
-
-This object is used to define details of the air supply subsystem.
-
-#### Field: Name
-
-This field contains a unique name for the fuel cell air supply subsystem.
-
-#### Field: Air Inlet Node Name
-
-This field is used to define the air node where the inlet air stream is drawn from. If the FC uses outdoor air then the node named here should be designated an outdoor air node. If the FC draws air from its surroundings, then this would be the name of the air node associated with the thermal zone containing the FC.
-
-#### Field: Blower Power Curve Name
-
-This field contains the name of a Curve:Cubic input object described elsewhere in the input file. The curve provides the power used by the air blower (W) as a cubic function of the rate of air supply (kmol/s).
-
-<div>\[{P_{blower - el}} = {b_0} + {b_1} \cdot {\dot N_{air}} + {b_2} \cdot \dot N_{air}^2 + {b_3} \cdot \dot N_{air}^3\]</div>
-
-#### Field: Blower Heat Loss Factor
-
-This field describes the portion of blower electrical power that is    lost    to the surroundings. The rest of the energy is added to the air stream. A heat loss factor of 1.0 indicates that all the heat is lost to the surroundings and no energy is added to the air inlet stream.
-
-#### Field: Air Supply Rate Calculation Mode
-
-This field describes how the model will calculate the air supply rate. There are three options to choose from:      AirRatiobyStoics   ,    QuadraticFunctionofElectricPower   , and    QuadraticFunctionofFuelRate.      The choice will determine how the model calculates the rate of air and will depend on the formulations used to develop model input data. The choices are described in the next four fields.
-
-#### Field: Stoichiometric Ratio
-
-This field describes the excess air ratio beyond stoichiometric air supply. This field is only used if the air supply rate calculation mode is AirRatiobyStoics. The total air supply ratio will be the value entered here plus 1.0. Thus if 1.0 is entered in this field, the total air flow will be 2.0 times what is needed to exactly match stoichiometry with the fuel supply.
-
-#### Field: Air Rate Function of Electric Power Curve Name
-
-This field contains the name of a QuadraticCurve input object described elsewhere in the input file. This field is only used if the air supply rate calculation mode is QuadraticFunctionofElectricPower. The quadratic curve named here describes the first part of the relation below used to calculate the rate of inlet air, <span>\({\dot N_{air}}\)</span>(kmol/s). It is a quadratic function of the net DC electrical power, <span>\({P_{el}}\)</span>  (W).
-
-<div>\[{a_3}\]</div>
-
-#### Field: Air Rate Air Temperature Coefficient
-
-This field is used to describe the air temperature coefficient, <span>\({\dot N_{air}} = \left[ {{a_0} + {a_1} \cdot {{\dot N}_{fuel}} + {a_2} \cdot \dot N_{fuel}^2} \right].\left[ {1 + {a_3} \cdot {T_{air}}} \right]\)</span>, used to adjust inlet air flow rate in the relations for inlet air rate.
-
-#### Field: Air Rate Function of Fuel Rate Curve Name
-
-This field contains the name of a Curve:Quadratic input object described elsewhere in the input file. This field is only used if the air supply rate calculation mode is QuadraticFunctionofFuelRate. The quadratic curve named here describes the first part of the relation used to calculate the rate of inlet air, <span>\({\dot N_{air}}\)</span>(kmol/s). It is a quadratic function of the fuel flow rate, <span>\({\dot N_{fuel}}\)</span>.
-
-<span>\({\dot N_{air}} = \left[ {{a_0} + {a_1} \cdot {P_{el}} + {a_2} \cdot P_{el}^2} \right].\left[ {1 + {a_3} \cdot {T_{air}}} \right]\)</span><span>\({\dot N_{air}} = \left[ {{a_0} + {a_1} \cdot {{\dot N}_{fuel}} + {a_2} \cdot \dot N_{fuel}^2} \right].\left[ {1 + {a_3} \cdot {T_{air}}} \right]\)</span>
-
-#### Field: Air Intake Heat Recovery Mode
-
-This field is used to control how heat losses from three other subsystems within the FC may or may not be recovered by the air inlet. There are six possible choices for what to use in this Field:    NoRecovery       RecoverBurnerInverterStorage       RecoverAuxiliaryBurner       RecoverInverterandStorage       RecoverInverter    and    RecoverElectricalStorage   .   If heat is recovered then that means that energy    losses    from those subsystems are added to the inlet air and fed back into the FC power module. The following table clarifies the meaning of the six possible choices.
-
-Table 32. Air Intake Heat Recovery Mode Choices
-
-<table class="table table-striped">
-<tr>
-<th>Field Choice</th>
-<th>Inverter Heat Losses Recovered?</th>
-<th>Electrical Storage Heat Losses Recovered?</th>
-<th>Auxiliary Heater Losses Recovered?</th>
-</tr>
-<tr>
-<td>NoRecovery   </td>
-<td>No</td>
-<td>No</td>
-<td>No</td>
-</tr>
-<tr>
-<td>RecoverBurnerInverterStorage</td>
-<td>Yes</td>
-<td>Yes</td>
-<td>Yes</td>
-</tr>
-<tr>
-<td>RecoverAuxiliaryBurner</td>
-<td>No</td>
-<td>No</td>
-<td>Yes</td>
-</tr>
-<tr>
-<td>RecoverInverterandStorage</td>
-<td>Yes</td>
-<td>Yes</td>
-<td>No</td>
-</tr>
-<tr>
-<td>RecoverInverter</td>
-<td>Yes</td>
-<td>No</td>
-<td>No</td>
-</tr>
-<tr>
-<td>RecoverElectricalStorage</td>
-<td>No</td>
-<td>Yes</td>
-<td>No</td>
-</tr>
-</table>
-
-#### Field: Air Supply Constituent Mode
-
-This field is used to choose between two different modes for describing the make up of the inlet air stream. There are two possible choices:      AmbientAir    or    UserDefinedConstituents.      Choosing the AmbientAir mode will automatically set the composition of air to be usual at: 77.28% nitrogen, 20.73% oxygen, 1.04% water, 0.92% argon, and 0.03% carbon dioxide. Choosing UserDefinedConstituents allows the user to customize the make up the inlet air in the remaining fields.
-
-#### Field: Number of UserDefined Constituents
-
-This field is used to describe the number of constituents in the inlet air. This field is only used if the air supply constituent mode is set to UserDefinedConstituents. The maximum number is 5.
-
-The remaining fields in this object are repeating pairs of fields with one pair for each constituent and the same number as described in the previous field. The pairs consist of the name of the constituent followed by the molar fraction of that constituent.
-
-#### Field: Constituent 1-5 Name
-
-These fields describe the air stream constituents by name. The name field for each pair must be filled with one of these choices:      CarbonDioxide   ,    Nitrogen,       Oxygen,       Water,    or    Argon.   
-
-#### Field: Molar Fraction 1-5
-
-These fields describe the molar fraction of the air stream constituents. It is very important that the sum of the molar fractions add up to 1.0.
-
-An example input data file (IDF) entry for this object is provided below:
-
-```idf
-   Generator:FuelCell:AirSupply,
-       FCT SOFC Air Supply,         !- Name
-       SOFC Air Inlet Node,         !- Air Inlet Node Name
-       FCT Blower Power Curve,   !- Blower Power Curve Name
-       1.0,                                         !- Blower Heat Loss Factor
-       QuadraticFunctionofElectricPower,   !- Air Supply Rate Calculation Mode
-       ,                                               !- Stoichiometric Ratio
-       FCT Excess Air Ratio Curve,   !- Air Rate Function of Electric Power Curve Name
-       2.83507E-3,                           !- Air Rate Air Temperature Coefficient
-       ,                                               !- Air Rate Function of Fuel Rate Curve Name
-       NoRecovery,                           !- Air Intake Heat Recovery Mode
-       UserDefinedConstituents,   !- Air Supply Constituent Mode
-       5,                                             !- Number of UserDefined Constituents
-       Nitrogen,                               !- Constituent 1 Name
-       0.7728,                                   !- Molar Fraction 1
-       Oxygen,                                   !- Constituent 2 Name
-       0.2073,                                   !- Molar Fraction 2
-       Water,                                     !- Constituent 3 Name
-       0.0104,                                   !- Molar Fraction 3
-       Argon,                                     !- Constituent 4 Name
-       0.0092,                                   !- Molar Fraction 4
-       CarbonDioxide,                     !- Constituent 5 Name
-       0.0003;                                   !- Molar Fraction 5
-```
-
-### Generator:FuelCell:WaterSupply
-
-This object is used to provide details of the water supply subsystem. This water is used for steam reforming of the fuel and is not the same as the water used for thermal heat recovery.
-
-```idd
-Generator:FuelCell:WaterSupply,
-   A1, \field Name
-           \required-field
-           \reference FCWaterSupNames
-   A2, \field Reformer Water Flow Rate Function of Fuel Rate Curve Name
-           \type object-list
-           \object-list QuadraticCurves
-   A3, \field Reformer Water Pump Power Function of Fuel Rate Curve Name
-           \type object-list
-           \object-list QubicCurves
-   N1, \field Pump Heat Loss Factor
-   A4, \field Water Temperature Modeling Mode
-           \type choice
-           \key TemperatureFromAirNode
-           \key TemperatureFromWaterNode
-           \key TemperatureFromSchedule
-           \key MainsWaterTemperature
-   A5, \field Water Temperature Reference Node Name
-   A6; \field Water Temperature Schedule Name
-           \type object-list
-           \object-list ScheduleNames
-```
-
-#### Field: Name
-
-This field contains a unique name for the fuel cell water supply subsystem.
-
-#### Field: Reformer Water Flow Rate Function of Fuel Rate Curve Name
-
-This field contains the name of a Curve:Quadratic input object described elsewhere in the input file. The curve provides the rate of water flow (kmol/sec) as a function of fuel flow rate (kmol/sec).
-
-<div>\[{\dot N_{liq - water}} = {w_0} + {w_1} \cdot {\dot N_{fuel}} + {w_2} \cdot \dot N_{fuel}^2\]</div>
-
-If the unit does not use water for reforming then use a    null    quadratic where all the coefficients are 0.0.
-
-#### Field: Reformer Water Pump Power Function of Fuel Rate Curve Name
-
-This field contains the name of a Curve:Cubic input object described elsewhere in the input file. The curve provides the power used by the water pump (W) as a cubic function of the rate of water supply (kmol/s).
-
-<div>\[{P_{pump - el}} = {p_0} + {p_1} \cdot {\dot N_{water}} + {p_2} \cdot \dot N_{water}^2 + {p_3} \cdot \dot N_{water}^3\]</div>
-
-If the unit does not use water for reforming then use a    null    cubic where all the coefficients are 0.0.
-
-#### Field: Pump Heat Loss Factor
-
-This field describes the portion of pump electrical power that is    lost    to the surroundings. The rest of the energy is added to the water stream. A heat loss factor of 1.0 indicates that all the heat is lost to the surroundings and no energy is added to the water inlet stream.
-
-#### Field: Water Temperature Modeling Mode
-
-This field describes how the model will determine the inlet temperature of the water stream. There are four options to choose from:      TemperatureFromAirNode,       TemperatureFromWaterNode,       TemperatureFromSchedule,    and    MainsWaterTemperature.      For the first two options, the temperature of the water inlet is determined by the temperature at the node named in the next field. For the third option, the temperature is determined by the schedule in the last field. Using the MainsWaterTemperature option requires also defining a separate    Site:WaterMainsTemperature    input object elsewhere in the input file.
-
-#### Field: Water Temperature Reference Node Name
-
-This field is used to define the node where the temperature of the inlet water stream is obtained. This can be either an air node or a water node.
-
-#### Field: Water Temperature Schedule Name
-
-This field is used to define the name of a schedule, defined elsewhere in the input file, that will be used to determine the temperature of the water inlet stream when using the TemperatureFromSchedule mode.
-
-An example input data file (IDF) entry for this object is provided below:
-
-```idf
-   Generator:FuelCell:WaterSupply,
-       FCT SOFC Water Supply,     !- Name
-       Null Quadratic,                   !- Reformer Water Flow Rate Function of Fuel Rate Curve Name
-       Null Cubic,                           !- Reformer Water Pump Power Function of Fuel Rate Curve Name
-       0.0,                                         !- Pump Heat Loss Factor
-       TemperatureFromAirNode,   !- Water Temperature Modeling Mode
-       SOFC Air Inlet Node,         !- Water Temperature Reference Node Name
-       ;                                               !- Water Temperature Schedule Name
-
-   Curve:Quadratic,
-       Null Quadratic,                   !- Name
-       0.0,                                         !- Coefficient1 Constant
-       0.0,                                         !- Coefficient2 x
-       0.0,                                         !- Coefficient3 x**2
-       -1.0E+10,                               !- Minimum Value of x
-       1.0E+10;                                 !- Maximum Value of x
-
-   Curve:Cubic,
-       Null Cubic,                           !- Name
-       0.0,                                         !- Coefficient1 Constant
-       0.0,                                         !- Coefficient2 x
-       0.0,                                         !- Coefficient3 x**2
-       0.0,                                         !- Coefficient4 x**3
-       -1.0E+10,                               !- Minimum Value of x
-       1.0E+10;                                 !- Maximum Value of x
-```
-
-### Generator:FuelCell:AuxiliaryHeater
-
-This object is intended for modeling an auxiliary heater, however this portion of the model is not yet available in EnergyPlus. An auxiliary heater may be present in fuel cell products so that the unit can meet much higher thermal loads than would be possible using only cogeneration. This portion of the model will be added in the future once suitable cogeneration control capabilities are also available. The input fields are described for future reference but may change. The program still requires one of these objects be included even though the data are not yet used (so that internal data structures can be allocated).
-
-#### Field: Name
-
-This field contains a unique name for the fuel cell auxiliary heater subsystem.
-
-#### Field: Excess Air Ratio
-
-This field describes the excess air ratio beyond stoichiometric air supply for the heater. The total air supply ratio will be the value entered here plus 1.0. Thus if 1.0 is entered in this field, the total air flow will be 2.0 times what is needed to exactly match stoichiometry with the fuel supply.
-
-#### Field: Ancillary Power Constant Term
-
-This field describes the constant term, <span>\({x_0}\)</span>, used to model the auxiliary burner   s ancillary devices such as fans and ignition controls. The electrical power for ancillaries is calculated using,
-
-<div>\[{P_{el,aux - ancillaries}} = {x_0} + {x_1} \cdot {\dot N_{aux - fuel}}\]</div>
-
-#### Field: Ancillary Power Linear Term
-
-This field describes the linear term, <span>\({x_1}\)</span>, used to model the auxiliary burner   s ancillary devices.
-
-#### Field: Skin Loss U-Factor Times Area Value
-
-This field describes the    UA    term (W/K) for calculating skin losses in the auxiliary burner.    UA    is the product of the overall heat transfer coefficient    U    and the area    A.      The skin heat losses are calculated using,
-
-<div>\[{q_{aux - skin - losses}} = {(UA)_{aux}} \cdot ({T_{aux - mix}} - {T_{room}})\]</div>
-
-where, <span>\({T_{aux - mix}}\)</span>  is temperature of product gases leaving the auxiliary burner and includes the mixing of the product gases from the fuel cell power module. Thus, the input for UA should reflect this choice of reference temperature rather than an exterior surface temperature of the auxiliary burner.
-
-#### Field: Skin Loss Destination
-
-This field describes the user   s choice for what happens to the skin losses. There are two options:      SurroundingZone    and    AirInletForFuelCell   . Entering SurroundingZone will direct the model to put the    lost    energy into the surrounding thermal Zone named in the next field. Entering AirInletForFuelCell will direct the model to put the    lost    energy into the air inlet stream for the fuel cell to preheat that air.
-
-#### Field: Zone Name to Receive Skin Losses
-
-This field is used to determine the zone that will receive the skin losses. Enter the name of a Zone declared elsewhere in the input file. This field is only used if the    SurroundingZone    mode is used in the previous field.
-
-#### Field: Heating Capacity Units
-
-This field describes the user   s choice for how the capacity of the auxiliary heater will be defined. There are two options:      Watts    or    kmol/s.      Entering Watts will direct the program to use the next two fields to determine the maximum and minimum heating capacity.   Entering kmol/s will direct the program to use the last two fields to determine the maximum and minimum heating capacities.
-
-#### Field: Maximum Heating Capacity in Watts
-
-This field is used to describe the maximum heating capacity of the auxiliary burner (W).
-
-#### Field: Minimum Heating Capacity in Watts
-
-This field is used to describe the minimum heating capacity of the auxiliary burner (W).
-
-#### Field: Maximum Heating Capacity in Kmol per Second
-
-This field is used to describe the maximum fuel use rate for the auxiliary burner (kmol/s).
-
-#### Field: Minimum Heating Capacity in Kmol per Second
-
-This field is used to describe the minimum fuel use rate for the auxiliary burner (kmol/s).
-
-An example input data file (IDF) entry for this object is provided below:
-
-```idf
-   Generator:FuelCell:AuxiliaryHeater,
-       FCT SOFC Auxiliary Heater,   !- Name
-       0.0,                                         !- Excess Air Ratio
-       0.0,                                         !- Ancillary Power Constant Term
-       0.0,                                         !- Ancillary Power Linear Term
-       0.5,                                         !- Skin Loss U-Factor Times Area Value
-       SurroundingZone,                 !- Skin Loss Destination
-       ZN_1_FLR_1_SEC_5,               !- Zone Name to Receive Skin Losses
-       Watts,                                     !- Heating Capacity Units
-       0.0,                                         !- Maximum Heating Capacity in Watts
-       0.0,                                         !- Minimum Heating Capacity in Watts
-       ,                                               !- Maximum Heating Capacity in Kmol per Second
-       ;                                               !- Minimum Heating Capacity in Kmol per Second
-```
-
-
-Generator:FuelCell:ExhaustGasToWaterHeatExchanger
-
-This object is used to describe the exhaust gas heat exchanger subsystem of the FC used to recovery thermal energy.
-
-#### Field: Name
-
-This field contains a unique name for the fuel cell power module subsystem.
-
-#### Field: Heat Recovery Water Inlet Node Name
-
-This field contains the name of the node that connects the heat exchanger   s inlet to the plant loop. This water is used for heat recovery.
-
-#### Field: Heat Recovery Water Outlet Node Name
-
-This field contains the name of the node that connects the heat exchanger   s outlet to the plant loop.
-
-#### Field: Heat Recovery Water Maximum Flow Rate
-
-This field describes the design maximum flow rate of the heat recovery water (m<sup>3</sup>/s). The value should match the design flow rate of the plant loop connected to the FC.
-
-#### Field: Exhaust Outlet Air Node Name
-
-This field is used to determine which node will receive the exhaust air stream leaving the FC. This node will usually be outside and not be referenced elsewhere. However, if the exhaust stream is used in a heat recovery ventilator (as described in section 11 of the Annex 42 specification) then the node would be reference in the heat recovery ventilator object.
-
-#### Field: Heat Exchanger Calculation Method
-
-This field is used to direct how EnergyPlus will calculate heat exchanger performance. The Annex 42 model provides for four different methods of modeling the heat exchanger. The choices available for this field are:      FixedEffectiveness    (method 1 in Annex 42 specification),      EmpiricalUAeff     (method 2),    FundementalUAeff     (method 3), or    Condensing    (method 4). The remaining fields provide input data for the different methods. The heat exchanger correlations are described below.
-
-#### Field: Method 1 Heat Exchanger Effectiveness
-
-This field describes constant heat exchanger effectiveness, <span>\({\varepsilon_{HX}}\)</span>. This field is only used with the    FixedEffectiveness    mode, which corresponds to    method 1    in the Annex 42 specification. For this mode, the heat exchange between the exhaust gases and the heat recovery water are calculated using,
-
-<div>\[{q_{HX}} = {\varepsilon_{HX}} \cdot {\left( {\dot N{{\hat c}_p}} \right)_{\min }} \cdot \left( {{T_{aux - mix}} - {T_{water,in}}} \right)\]</div>
-
-where, <span>\({\left( {\dot N{{\hat c}_p}} \right)_{\min }}\)</span>is the minimum value of <span>\({\left( {\dot N{{\hat c}_p}} \right)_{aux - mix}}\)</span>and <span>\({\left( {\dot N{{\hat c}_p}} \right)_{water}}\)</span>.
-
-#### Field: Method 2 Parameter hxs0
-
-This field describes the value of <span>\(h{x_{s,0}}\)</span>  in the relation below for effective UA. This field is used with the    EmpiricalUAeff    mode, which corresponds to    method 2    in the Annex 42 specification and with the    Condensing    mode, which corresponds to    method 4   . This method uses the log mean temperature difference (LMTD) approach to calculate the heat exchange:
-
-<div>\[{q_{HX}} = {\left( {UA} \right)_{eff}} \cdot \frac{{\left( {{T_{aux - mix}} - {T_{water,out}}} \right) - \left( {{T_{HX - exh}} - {T_{water,in}}} \right)}}{{\ln \left( {\frac{{{T_{aux - mix}} - {T_{water,out}}}}{{{T_{HX - exh}} - {T_{water,in}}}}} \right)}}\]</div>
-
-The user input in this field, and the next four fields, describe coefficients in an empirical relation for <span>\({\left( {UA} \right)_{eff}}\)</span>:
-
-<div>\[{\left( {UA} \right)_{eff}} = h{x_{s,0}} + h{x_{s,1}} \cdot {\dot N_{water}} + h{x_{s,2}} \cdot \dot N_{water}^2 + h{x_{s,3}} \cdot {\dot N_{aux - mix}} + h{x_{s,4}} \cdot \dot N_{aux - mix}^2\]</div>
-
-#### Field: Method 2 Parameter hxs1
-
-This field describes the value of <span>\(h{x_{s,1}}\)</span>  in the relation above for effective UA. This field is used with the    EmpiricalUAeff    mode, which corresponds to    method 2    in the Annex 42 specification and with the    Condensing    mode, which corresponds to    method 4   .
-
-#### Field: Method 2 Parameter hxs2
-
-This field describes the value of <span>\(h{x_{s,2}}\)</span>  in the relation above for effective UA. This field is used with the    EmpiricalUAeff    mode, which corresponds to    method 2    in the Annex 42 specification and with the    Condensing    mode, which corresponds to    method 4   .
-
-#### Field: Method 2 Parameter hxs3
-
-This field describes the value of <span>\(h{x_{s,3}}\)</span>  in the relation above for effective UA. This field is used with the    EmpiricalUAeff    mode, which corresponds to    method 2    in the Annex 42 specification and with the    Condensing    mode, which corresponds to    method 4   .
-
-#### Field: Method 2 Parameter hxs4
-
-This field describes the value of <span>\(h{x_{s,4}}\)</span>  in the relation above for effective UA. This field is used with the    EmpiricalUAeff    mode, which corresponds to    method 2    in the Annex 42 specification and with the    Condensing    mode, which corresponds to    method 4   .
-
-#### Field: Method 3 h0Gas Coefficient
-
-This field describes the value of <span>\(h_{gas}^0\)</span>  in the relation below. This field is only used with the    FundementalUAeff    mode, which corresponds to    method 3    in the Annex 42 specification. For this mode, the heat exchange is calculated using the LMTD method, but the effective UA is determined using:
-
-<div>\[{\left( {UA} \right)_{eff}} = {\left[ {\frac{1}{{{{\left( {hA} \right)}_{gas}}}} + \frac{1}{{{{(hA)}_{water}}}} + {F_{HX}}} \right]^{ - 1}}\]</div>
-
-where,
-
-<span>\({F_{HX}}\)</span>  is an adjustment factor,
-
-<span>\({h_{gas}} = h_{gas}^0 \cdot {\left( {\frac{{{{\dot N}_{gas}}}}{{\dot N_{gas}^0}}} \right)^n}\)</span>,
-
-<div>\[{h_{water}} = h_{water}^0 \cdot {\left( {\frac{{{{\dot N}_{water}}}}{{\dot N_{water}^0}}} \right)^m}\]</div>
-
-#### Field: Method 3 NdotGasRef Coefficient
-
-This field describes the value of <span>\(\dot N_{gas}^0\)</span>  in the relation above. This field is only used with the    FundementalUAeff    mode, which corresponds to    method 3    in the Annex 42 specification.
-
-#### Field: Method 3 n Coefficient
-
-This field describes the value of <span>\(n\)</span>  in the relation above. This field is only used with the    FundementalUAeff    mode, which corresponds to    method 3    in the Annex 42 specification.
-
-
-
-#### Field: Method 3 Gas Area
-
-This field describes the value of <span>\({A_{gas}}\)</span>  in the relation above. This field is only used with the    FundementalUAeff    mode, which corresponds to    method 3    in the Annex 42 specification.
-
-#### Field: Method 3 h0 Water Coefficient
-
-This field describes the value of <span>\(h_{water}^0\)</span>  in the relation above. This field is only used with the    FundementalUAeff    mode, which corresponds to    method 3    in the Annex 42 specification.
-
-#### Field: Method 3 N dot Water ref Coefficient
-
-This field describes the value of <span>\(\dot N_{water}^0\)</span>  in the relation above. This field is only used with the    FundementalUAeff    mode, which corresponds to    method 3    in the Annex 42 specification.
-
-#### Field: Method 3 m Coefficient
-
-This field describes the value of <span>\(m\)</span>  in the relation above. This field is only used with the    FundementalUAeff    mode, which corresponds to    method 3    in the Annex 42 specification.
-
-#### Field: Method 3 Area Water Coefficient
-
-This field describes the value of <span>\({A_{water}}\)</span>  in the relation above. This field is only used with the    FundementalUAeff    mode, which corresponds to    method 3    in the Annex 42 specification.
-
-#### Field: Method 3 F Adjustment Factor
-
-This field describes the value of <span>\({F_{HX}}\)</span>  in the relation above. This field is only used with the    FundementalUAeff    mode, which corresponds to    method 3    in the Annex 42 specification.
-
-#### Field: Method 4 hxl1 Coefficient
-
-This field describes the value of <span>\(h{x_{l,1}}\)</span>  in the relation below for the rate of condensation of water from the gas stream, <span>\({\dot N_{{H_2}O - cond}}\)</span>. This field is only used with the    Condensing    mode, which corresponds to    method 4    in the Annex 42 specification. This method uses a modified version of the LMTD approach to calculate heat exchange:
-
-<div>\[{q_{HX}} = {\left( {UA} \right)_{eff}} \cdot \frac{{\left( {{T_{aux - mix}} - {T_{water,out}}} \right) - \left( {{T_{HX - exh}} - {T_{water,in}}} \right)}}{{\ln \left( {\frac{{{T_{aux - mix}} - {T_{water,out}}}}{{{T_{HX - exh}} - {T_{water,in}}}}} \right)}} + {\dot N_{{H_2}O - cond}} \cdot {\hat h_{fg}}\]</div>
-
-where,
-
-<div>\[{\dot N_{{H_2}O - cond}} = \left( {{T_{cond - threshold}} - {T_{water,in}}} \right) \cdot \left[ {h{x_{l,1}} \cdot \left( {\frac{{{{\dot N}_{{H_2}O}}}}{{{{\dot N}_{aux - mix}}}}} \right) + h{x_{l,2}} \cdot {{\left( {\frac{{{{\dot N}_{{H_2}O}}}}{{{{\dot N}_{aux - mix}}}}} \right)}^2}} \right]\]</div>
-
-#### Field: Method 4 hxl2 Coefficient
-
-This field describes the value of <span>\(h{x_{l,2}}\)</span>  in the relation above for the rate of condensation of water from the gas stream, <span>\({\dot N_{{H_2}O - cond}}\)</span>. This field is only used with the    Condensing    mode, which corresponds to    method 4    in the Annex 42 specification.
-
-
-
-#### Field: Method 4 Condensation Threshold
-
-This field describes the value of <span>\({T_{cond - threshold}}\)</span>  in the relation above for the rate of condensation of water from the gas stream, <span>\({\dot N_{{H_2}O - cond}}\)</span>. This field is only used with the    Condensing    mode, which corresponds to    method 4    in the Annex 42 specification.
-
-
-
-An example input data file (IDF) entry for this object is provided below:
-
-
-
-
-
-```idf
-   Generator:FuelCell:ExhaustGasToWaterHeatExchanger,
-       FCT SOFC Exhaust HX,         !- Name
-       Small SOFC Heat Rec Inlet Node,   !- Heat Recovery Water Inlet Node Name
-       Small SOFC Heat Rec Outlet Node,   !- Heat Recovery Water Outlet Node Name
-       0.0004,                                   !- Heat Recovery Water Maximum Flow Rate {m3/s}
-       SOFC Air Outlet Node,       !- Exhaust Outlet Air Node Name
-       CONDENSING,                           !- Heat Exchanger Calculation Method
-       ,                                               !- Method 1 Heat Exchanger Effectiveness
-       83.1,                                       !- Method 2 Parameter hxs0
-       4798,                                       !- Method 2 Parameter hxs1
-       -138E+3,                                 !- Method 2 Parameter hxs2
-       -353.8E+3,                             !- Method 2 Parameter hxs3
-       5.15E+8,                                 !- Method 2 Parameter hxs4
-       ,                                               !- Method 3 h0Gas Coefficient
-       ,                                               !- Method 3 NdotGasRef Coefficient
-       ,                                               !- Method 3 n Coefficient
-       ,                                               !- Method 3 Gas Area
-       ,                                               !- Method 3 h0 Water Coefficient
-       ,                                               !- Method 3 N dot Water ref Coefficient
-       ,                                               !- Method 3 m Coefficient
-       ,                                               !- Method 3 Area Water Coefficient
-       ,                                               !- Method 3 F Adjustment Factor
-       -1.96E-4,                               !- Method 4 hxl1 Coefficient
-       3.1E-3,                                   !- Method 4 hxl2 Coefficient
-       35.0;                                       !- Method 4 Condensation Threshold {C}
-```
-
-### Generator:FuelCell:ElectricalStorage
-
-This object is used to describe the electrical storage subsystem for the FC. The electrical storage model is a very simple    constrained bucket    model. Future developments made add additional models for battery systems. Note that this electrical storage is embedded within the FC device.
-
-#### Field: Name
-
-This field contains a unique name for the fuel cell electrical storage subsystem.
-
-#### Field: Choice of   Model
-
-This field is used to direct how EnergyPlus will model electrical storage. The only choice currently available is    SimpleEfficiencyWithConstraints,    which should be entered in this field. Future developments may expand the number of models available for electrical storage.
-
-#### Field: Nominal Charging Energetic Efficiency
-
-This field describes the value of <span>\({\varepsilon_{charge}}\)</span>  in the relation for the State of Charge, <span>\(Q_{battery}^{t + \Delta t}\)</span>:
-
-<div>\[Q_{battery}^{t + \Delta t} = Q_{battery}^t + {P_{battery - charge}} \cdot {\varepsilon_{charge}} \cdot \Delta t\]</div>
-
-This is the energetic efficiency of charging the storage device. A value of 1.0 means that the storage device does not lose any energy when charging. Note that the model can recover the    lost    energy into the air supply intake.
-
-#### Field: Nominal Discharging Energetic Efficiency
-
-This field describes the value of <span>\({\varepsilon_{discharge}}\)</span>  in the relation for the State of Charge, <span>\(Q_{battery}^{t + \Delta t}\)</span>:
-
-<div>\[Q_{battery}^{t + \Delta t} = Q_{battery}^t + \frac{{{P_{battery - discharge}} \cdot \Delta t}}{{{\varepsilon_{discharge}}}}\]</div>
-
-This is the energetic efficiency of discharging the storage device. A value of 1.0 means that the storage device does not lose any energy when discharging. Note that the model can recover the    lost    energy into the air supply intake.
-
-#### Field: Simple Maximum Capacity
-
-This field describes the maximum amount of electrical energy that can be stored in the device (J).
-
-#### Field: Simple Maximum Power Draw
-
-This field describes the maximum rate at which electrical power can be discharged from the storage device (W).
-
-#### Field: Simple Maximum Power Store
-
-This field describes the maximum rate at which electrical power can charge the storage device (W).
-
-#### Field: Initial Charge State
-
-This field describes the value for the initial state of charge (J). This allows the storage device to contain some amount of stored electricity at the beginning of the simulation period.
-
-
-
-An example input data file (IDF) entry for this object is provided below:
-
-
-
-```idf
-   Generator:FuelCell:ElectricalStorage,
-       FCT SOFC Battery,               !- Name
-       SimpleEfficiencyWithConstraints,   !- Choice of Model
-       1.0,                                         !- Nominal Charging Energetic Efficiency
-       1.0,                                         !- Nominal Discharging Energetic Efficiency
-       0,                                             !- Simple Maximum Capacity {J}
-       0,                                             !- Simple Maximum Power Draw {W}
-       0,                                             !- Simple Maximum Power Store {W}
-       0;                                             !- Initial Charge State {J}
-```
-
-### Generator:FuelCell:Inverter
-
-This object is used to describe the power condition unit subsystem of the FC. This object models an inverter system contained within a fuel cell system that converts from direct current (DC) to alternating current (AC).
-
-#### Field: Name
-
-This field contains a unique name for the fuel cell inverter subsystem.
-
-#### Field: Inverter Efficiency Calculation Mode
-
-This field is used to direct how EnergyPlus will calculate the inverter efficiency. There are two possible choices:      Constant    or    Quadratic   .
-
-#### Field: Inverter Efficiency
-
-This field describes the value for inverter efficiency when using the **Constant** mode.
-
-#### Field: Efficiency Function of DC Power Curve Name
-
-This field names a Curve:Quadratic object defined elsewhere in the input file. The curve determines inverter efficiency as a function of the DC power entering the inverter as follows:
-
-<div>\[{\eta_{PCU}} = {u_0} + {u_1} \cdot {P_{PCU - in}} + {u_2} \cdot P_{PCU - in}^2\]</div>
-
-An example input data file (IDF) entry for this object is provided below:
-
-
-
-```idf
-   Generator:FuelCell:Inverter,
-       FCT SOFC Inverter,             !- Name
-       Quadratic,                             !- Inverter Efficiency Calculation Mode
-       ,                                               !- Inverter Efficiency
-       FCT Inverter Quadratic;   !- Efficiency Function of DC Power Curve Name
-
-
-   Curve:Quadratic,
-       FCT Inverter Quadratic,   !- Name
-       0.560717,                               !- Coefficient1 Constant
-       1.24019E-4,                           !- Coefficient2 x
-       -2.01648E-8,                         !- Coefficient3 x**2
-       -1.0E+10,                               !- Minimum Value of x
-       1.0E+10;                                 !- Maximum Value of x
-```
-
-### Generator:FuelSupply
-
-This object is used to define details of the fuel supply for certain generators. This object allows the user to describe a wide array of possible fuel mixtures. The program contains data and internal methods to calculate the properties of the various mixtures of gaseous fuels. The program will calculate the Lower Heating Value (LHV), Higher Heating Value (HHV), and molecular weight for the fuel mixture. The fuel properties are then use by both fuel cell and Micro CHP models. Results of the gas phase thermochemistry modeling are also reported in the EIO file.
-
-In addition to gaseous mixtures, the Micro CHP model is able to use generic liquid fuels and this object is used to describe the properties.
-
-Note that the fuel consumption metering is currently handled by the Natural Gas meter. So no matter what fuel mixture is defined in this object, the aggregated reports from EnergyPlus meters for (natural) Gas will include the fuel used for the generator (with the Joule content based on HHV).
-
-#### Field: Name
-
-This field contains a unique name for the fuel cell fuel supply subsystem.
-
-#### Field: Fuel Temperature Modeling Mode
-
-This field describes how the model will determine the temperature of the fuel. There are two options for this field to choose from:      TemperatureFromAirNode    and    Scheduled.      If this field contains TemperatureFromAirNode then the fuel is modeled as having the same temperature as the air node that is named in the next field. If this field contains Scheduled then the fuel is modeled as having the temperature described in a schedule defined elsewhere in the input file.
-
-#### Field: Fuel Temperature Reference Node Name
-
-This field contains the name of the air node used to obtain the inlet temperature of the fuel. This field is only used if the Fuel Temperature Modeling Mode is set to TemperatureFromAirNode.
-
-#### Field: Fuel Temperature Schedule Name
-
-This field contains the name of a temperature schedule defined elsewhere in the input file. This field is only used if the Fuel Temperature Modeling Mode is set to Scheduled. The temperature of the fuel inlet will be obtained from the schedule.
-
-#### Field: Compressor Power Function of Fuel Rate Curve Name
-
-This field contains the name of a Curve:Cubic input object described elsewhere in the input file. The curve provides the electrical power used by the fuel compressor (W) as a cubic function of the rate of fuel supply (kmol/s).
-
-<div>\[{P_{comp - el}} = {c_0} + {c_1} \cdot {\dot N_{fuel}} + {c_2} \cdot \dot N_{fuel}^2 + {c_3} \cdot \dot N_{fuel}^3\]</div>
-
-#### Field: Compressor Heat Loss Factor
-
-This field describes the portion of the compressor electrical power that is    lost    to the surroundings. The rest of the energy is added to the fuel stream. A heat loss factor of 1.0 indicates that all the heat is lost to the surroundings and no energy is added to the fuel inlet stream.
-
-#### Field: Fuel Type
-
-Choose between    GaseousConstituents    or    LiquidGeneric   .
-
-#### Field: Liquid Generic Fuel Lower Heating Value
-
-For fuel type    LiquidGeneric,    this field is used to enter the lower heating value of the fuel in units of kJ/kg.
-
-#### Field: Liquid Generic Fuel Higher Heating Value
-
-For fuel type    LiquidGeneric,    this field is used to enter the higher heating value of the fuel in units of kJ/kg.
-
-#### Field: Liquid Generic Fuel Molecular Weight
-
-For fuel type    LiquidGeneric,    this field is used to enter the molecular weight of the fuel in units of g/mol.
-
-#### Field: Liquid Generic Fuel CO2 Emission Factor
-
-This field is not used. This part of the Annex 42 model was not implemented in EnergyPlus; see the FuelFactors object.
-
-#### Field: Number of Constituents in Gaseous Constituent Fuel Supply
-
-This field is used to describe the number of constituents in the inlet fuel supply. The maximum number of different types of constituents is currently set to 12.
-
-The remaining fields in this object are repeating pairs of fields with one pair for each constituent and the same number as described in the previous field. The field set pairs consist of the name of the constituent followed by the molar fraction of that constituent.
-
-#### Field: Constituent 1-12 Name
-
-These fields describe the fuel stream constituents by name. The name field for each pair must be filled with one of these 14 choices:      CarbonDioxide   ,    Nitrogen   ,    Oxygen   ,    Water   ,    Argon   ,    Hydrogen   ,    Methane   ,    Ethane   ,    Propane   ,    Butane   ,    Pentane   ,    Hexane   ,    Methanol   , and    Ethanol   .   No other fuel constituents can currently be modeled. The properties of the constituents are already contained inside the program as provided in the Annex 42 model specification.
-
-#### Field: Constituent 1-12   Molar Fraction
-
-These fields describe the molar fraction of the fuel stream constituents. It is very important that the sum of the molar fractions add up to 1.0.
-
-### Generator:FuelSupply Outputs
-
-In addition to the following output variables, the resulting fuel heating values are also reported to the eio file.
-
-HVAC,Average,Generator Fuel Compressor Electric Power [W]
-
-HVAC,Sum,Generator Fuel Compressor Electric Energy [J]
-
-HVAC,Average,Generator Fuel Compressor Skin Heat Loss Rate [W]
-
-#### Generator Fuel Compressor Electric Power [W]
-
-This is the rate of energy use by the gas compressor, if any, that provides fuel at a higher pressure.
-
-#### Generator Fuel Compressor Electric Energy [J]
-
-This is the energy used by the gas compressor, if any, that provides fuel at a higher pressure.
-
-#### Generator Fuel Compressor Skin Heat Loss Rate [W]
-
-Convective heat gains to zone from gas compressor, if any, that provides fuel at a higher pressure.
-
-### Photovoltaic Generators
-
-EnergyPlus offers different options for predicting the electricity produced by solar electric photovoltaic (PV) panels. The three different options are    Simple   ,    Equivalent One-Diode    and    Sandia    and the choice will determine the mathematical models used to determine energy production. The first allows the user to input an arbitrary efficiency. The other two models use empirical relationships to predict PV operating performance based on many environmental variables such as cell temperature.   The PV models can be used with either normal PV modules or as part of a hybrid photovoltaic/thermal (PVT) flat plat collector.
-
-The generator is connected to an Electric Load Center.   The   PV models refer to surface input objects defined elsewhere in the input file.   This object describes an array that is    attached    to a surface object in order to describe its orientation and to access results of the solar insolation calculations. These can be either Heat Transfer or Shading objects (see Surfaces). This will define the orientation of the solar panel for the detailed models and also the area for the simple model. The exposure of that surface to incident solar radiation is calculated using the full set of models in EnergyPlus that are used to account for solar thermal loads arising from building windows and walls. Therefore the incident solar radiation is calculated to include the effects of shading and reflections from other surfaces declared in the input file. In addition to the output variables associated with PV models, there are numerous related output variables available for the surfaces including: 'Surface Outside Face Sunlit Area', 'Surface Outside Face Sunlit Fraction', 'Surface Outside Face Incident Solar Radiation Rate per Area', 'Surface Outside Face Incident Beam Solar Radiation Rate per Area', 'Surface Outside Face Incident Sky Diffuse Solar Radiation Rate per Area', 'Surface Outside Face Incident Ground Diffuse Solar Radiation Rate per Area', 'Surface Outside Face Beam Solar Incident Angle Cosine Value', 'Surface Outside Face Incident Sky Diffuse Ground Reflected Solar Radiation Rate per Area', 'Surface Outside Face Incident Sky Diffuse Surface Reflected Solar Radiation Rate per Area', 'Surface Outside Face Incident Beam To Beam Reflected From Surfaces Solar Radiation Rate per Area', 'Surface Outside Face Incident Beam To Diffuse Surface Reflected Solar Radiation Rate per Area', and 'Surface Outside Face Incident Beam To Diffuse Ground Reflected Solar Radiation Rate per Area.      Note that it is possible to define a PV array area that doesn   t conform to the surface area (i.e. model a PV array area that is larger or smaller than what is available on the surface) so it is the users responsibility to not over-specify area when determining how many modules will fit onto a surface. However this type of input is allowed.
-
-EnergyPlus does not include models for ancillary equipment for a PV array including charge controllers or power-point trackers. The operation of the entire electrical system that must go along with a PV array is not currently modeled in EnergyPlus and is therefore assumed to operate in ideal ways.   The PV production models do not resolve voltage and current, only power (and energy).   Electricity production is metered based on the output of the inverter. Output results are available before and after the inverter. One assumption is that the array is assumed to be always operating at the maximum power point. Energy production is based on the assumption that the quasi-steady power prediction is constant and continuous over the simulation timestep.
-
-For a variety of reasons, actual installations of photovoltaics are often observed to exhibit system-level problems that significantly reduce electricity production. Therefore this modeling should be considered a method of bracketing the upper end of electricity production rather than an accurate prediction of what the panels will produce. Also note that the model predictions are closely related to the solar radiation data (typically of of TMY2 origin) in the EnergyPlus weather file, that the solar data in these is usually from a model rather than direct measurements, and that solar resources encountered by a real installation in a given year are likely to differ from the weather data file.
-
-### Generator:Photovoltaic
-
-This object is used to describe an array of PV modules and how they are to be modeled.   A series of different PV arrays can be connected to a single electric load center (and inverter) by listing them all in an ElectricLoadCenter:Generator object.
-
-#### Field: Name
-
-This field is a unique name for the PV array.
-
-#### Field: Surface Name
-
-This field is the name of a surface that defines the location and geometry of the array.
-
-#### Field: Photovoltaic Performance Object Type
-
-This field is the type of PV performance model.   The choices are the class names for the three modeling options:
-
-* PhotovoltaicPerformance:Simple
-
-* PhotovoltaicPerformance:EquivalentOne-Diode
-
-* PhotovoltaicPerformance:Sandia.
-
-#### Field: Module Performance Name
-
-This is the name of the PV performance object define elsewhere (corresponding to the object type listed in the previous field)
-
-#### Field: Heat Transfer Integration Mode
-
-The PV model allows for different ways of integrating with other EnergyPlus heat transfer surfaces and models and calculating cell temperature.   For Building Integrated PV (BIPV), the    Integrated    options allow for the PV modeling to be coupled to the surface heat transfer models elsewhere in EnergyPlus.   The user must select one of these options for this field:
-
-- **Decoupled.  ** The cell temperature of modules in the array is computed based on a energy balance relative to NOCT conditions.   The input fields for Module Heat Capacity and Module Heat Loss Coefficient are ignored.
-
-- **DecoupledUllebergDynamic  ** the cell temperature is calculated based on a dynamic model developed by Ulleberg[[1]](#_ftn1).   The input fields for Module Heat Capacity and Module Heat Loss Coefficient are required.
-
-- **IntegratedSurfaceOutsideFace  ** The cell temperature is obtained from the outside face of the Surface:Heat Transfer named in the previous field.   Energy exported by the module is removed from the heat transfer surface (at the position determined by the associated Construction with Internal Source).   The input fields for Module Heat Capacity and Module Heat Loss Coefficient are ignored.
-
-- **IntegratedTranspiredCollector  ** The cell temperature is obtained from the collector surface temperature in the unglazed transpired collector model.   Energy exported by the module is removed from the collector surface.   The input fields for Module Heat Capacity and Module Heat Loss Coefficient are ignored.
-
-- **IntegratedExteriorVentedCavity  ** The cell temperature is obtained from the exterior baffle temperature in the naturally ventilated exterior cavity model.   Energy exported by the module is removed from the exterior baffle surface.   The input fields for Module Heat Capacity and Module Heat Loss Coefficient are ignored.
-
-- **PhotovoltaicThermalSolarCollector  ** The cell temperature is obtained from the photovoltaic/thermal solar collector model.   If the PV layer is inside the collector, then the incident solar is modified by the photovoltaic/thermal solar collector model.
-
-#### Field: Number of Series Strings in Parallel
-
-This field is the number of series-wired strings of PV modules that are in parallel to form the PV array.   The product of this field and the next field should equal the total number of modules in the array.
-
-#### Field: Number of Modules in Series
-
-This field is the number of modules wired in series (on each string) to form the PV array.   The product of this field and the previous field should equal the total number of modules in the array.
-
-### Generator:Photovoltaic Outputs
-
-Using the Generator:PV:Simple object makes a number of output variables available.\\
-
-* HVAC,Average,Generator Produced DC Electric Power [W]
-
-* HVAC,Sum,Generator Produced DC Electric Energy [J]
-
-* HVAC,Average,Generator PV Cell Temperature [C]
-
-* HVAC,Average,Generator PV Short Circuit Current [A]
-
-* HVAC,Average,Generator PV Open Circuit Voltage [V]
-
-* HVAC,Average,Generator PV Array Efficiency []
-
-#### Generator Produced DC Electric Power [W]
-
-This output variable is the power of DC electricity produced by the PV array in Watts..
-
-#### Generator Produced DC Electric Energy [J]
-
-This output variable is the energy in DC electricity produced by the PV array, in Joules.
-
-#### Generator PV Array Efficiency [ ]
-
-This output variable is the resulting efficiency of the PV array .
-
-
-
-The two more detailed PV models also have the following output variables.
-
-#### Generator PV Cell Temperature [ &deg;C]
-
-This output variable represents the temperature of the solar cell used in the calculation of cell performance.
-
-#### Generator PV Short Circuit Current [A]
-
-This output variable represents the short circuit current of the PV array, in Amps. This is provided to describe the I-V characteristics.
-
-#### Generator PV Open Circuit Voltage [V]
-
-This output variable represents the open circuit voltage of the PV array, in Volts. This is provided to describe the I-V characteristics.
-
-### PhotovoltaicPerformance:Simple
-
-The PhotovoltaicPerformance:Simple object describes a simple model of photovoltaics that may be useful for early phase design analysis. In this model the user has direct access to the efficiency with which surfaces convert incident solar radiation to electricity and need not specify arrays of specific modules. The full geometric model for solar radiation is used, including shading and reflections, to determine the incident solar resource. This model is intended to be useful for design purposes to quickly get an idea of the levels for annual production and peak power. The model can also accept arbitrary conversion efficiencies and does not require actual production units be tested to obtain performance coefficients.
-
-#### Field: Name
-
-This field is the name of the PV array. The name is only used as an identifier. Multiple instances need have unique names.
-
-#### Field: Fraction of Surface Area with Active Solar Cells
-
-This field is the user defined fraction for the area of surface named in the parent PV object that will have active PV cells on it. The area actually covered with solar cells will be the net area of the surface (gross area less any subsurfaces like windows) times the fraction entered here. This fraction includes the difference between PV module area and active cells within it and any losses for how closely packed modules can be arranged on surface.   The value should be between 0.0 and 1.0.
-
-#### Field: Conversion Efficiency Input Mode
-
-This field specifies how the PV array efficiency values are input. There are two choices, **Fixed**   and **Scheduled**.   If this field is set to    Fixed    then the PV array always has the efficiency value specified in the next field. If this field is set to    Scheduled    then the efficiency is determined by a user defined schedule named in the second field to follow.
-
-#### Field: Value for Cell Efficiency if Fixed
-
-This field specifies the efficiency with which solar incident energy is converted to electricity. Efficiency = (electrical power generated [W])/(power of incident solar[W]). These efficiency values are dimensionless and should be between 0.0 and 1.0.
-
-#### Field: Efficiency Schedule Name
-
-This field should be set to the name of schedule defined elsewhere in the input file. This schedule should specify dimensionless efficiency values between 0.0 and 1.0. This could be used for example to vary the efficiency to match results computed with more detailed models.
-
-An example idf instance of this object follows:
-
-```idf
-PhotovoltaicPerformance:Simple,
-     Simple PV Flat, !- Name
-     0.1044 , !- Fraction of Surface area that has active solar cells
-     FIXED ,   !- Conversion efficiency input mode
-     0.12 ,     !- Value for cell efficiency if fixed
-         ;           !- Name of Schedule that Defines Efficiency
-```
-
-### PhotovoltaicPerformance:EquivalentOne-Diode
-
-This object describes the performance characteristics of Photovoltaic (PV) modules to be modeled using an equivalent one-diode circuit.   This model is also known at the 4- or 5-parameter TRNSYS model for photovoltaics.
-
-The following table shows several sample PV array types with their input values.
-
-Table 33. Photovoltaics Array Types with Values
-
-<table class="table table-striped">
-<tr>
-<th>  </th>
-<th>Short Circuit Current</th>
-<th>Open Circuit Voltage</th>
-<th>Voltage at Maximum Power</th>
-<th>Current at Maximum Power</th>
-<th>Temperature Coefficient of Short Circuit Current</th>
-<th>Temperature Coefficient of Open Circuit Voltage</th>
-<th>Number of Cells in Series per Module</th>
-<th>Cell Temperature at NOCT Conditions</th>
-<th>Module Area</th>
-</tr>
-<tr>
-<td>Units:</td>
-<td>[A]</td>
-<td>[V]</td>
-<td>[V]</td>
-<td>[A]</td>
-<td>{A/K]</td>
-<td>[V/K]</td>
-<td>[-]</td>
-<td>[K]</td>
-<td>[m2]</td>
-</tr>
-<tr>
-<td>ASE 300-DFG/50</td>
-<td>6.2</td>
-<td>60</td>
-<td>50.5</td>
-<td>5.6</td>
-<td>0.001</td>
-<td>-0.0038</td>
-<td>216</td>
-<td>318</td>
-<td>2.43</td>
-</tr>
-<tr>
-<td>BPsolar 275</td>
-<td>4.75</td>
-<td>21.4</td>
-<td>17</td>
-<td>4.45</td>
-<td>0.00065</td>
-<td>-0.08</td>
-<td>36</td>
-<td>320</td>
-<td>0.63</td>
-</tr>
-<tr>
-<td>BPsolar 3160</td>
-<td>4.8</td>
-<td>44.2</td>
-<td>35.1</td>
-<td>4.55</td>
-<td>0.00065</td>
-<td>-0.16</td>
-<td>72</td>
-<td>320</td>
-<td>1.26</td>
-</tr>
-<tr>
-<td>BPsolar 380</td>
-<td>4.8</td>
-<td>22.1</td>
-<td>17.6</td>
-<td>4.55</td>
-<td>0.00065</td>
-<td>-0.08</td>
-<td>36</td>
-<td>320</td>
-<td>0.65</td>
-</tr>
-<tr>
-<td>BPsolar 4160</td>
-<td>4.9</td>
-<td>44.2</td>
-<td>35.4</td>
-<td>4.52</td>
-<td>0.00065</td>
-<td>-0.16</td>
-<td>72</td>
-<td>320</td>
-<td>1.26</td>
-</tr>
-<tr>
-<td>BPsolar 5170</td>
-<td>5</td>
-<td>44.2</td>
-<td>36</td>
-<td>4.72</td>
-<td>0.00065</td>
-<td>-0.16</td>
-<td>72</td>
-<td>320</td>
-<td>1.26</td>
-</tr>
-<tr>
-<td>BPsolar 585</td>
-<td>5</td>
-<td>22.1</td>
-<td>18</td>
-<td>4.72</td>
-<td>0.00065</td>
-<td>-0.08</td>
-<td>36</td>
-<td>320</td>
-<td>0.65</td>
-</tr>
-<tr>
-<td>Shell   SM110-12</td>
-<td>6.9</td>
-<td>21.7</td>
-<td>17.5</td>
-<td>6.3</td>
-<td>0.0028</td>
-<td>-0.076</td>
-<td>36</td>
-<td>318</td>
-<td>0.86856</td>
-</tr>
-<tr>
-<td>Shell   SM110-24</td>
-<td>3.45</td>
-<td>43.5</td>
-<td>35</td>
-<td>3.15</td>
-<td>0.0014</td>
-<td>-0.152</td>
-<td>72</td>
-<td>318</td>
-<td>0.86856</td>
-</tr>
-<tr>
-<td>Shell SP70</td>
-<td>4.7</td>
-<td>21.4</td>
-<td>16.5</td>
-<td>4.25</td>
-<td>0.002</td>
-<td>-0.076</td>
-<td>36</td>
-<td>318</td>
-<td>0.6324</td>
-</tr>
-<tr>
-<td>Shell SP75</td>
-<td>4.8</td>
-<td>21.7</td>
-<td>17</td>
-<td>4.4</td>
-<td>0.002</td>
-<td>-0.076</td>
-<td>36</td>
-<td>318</td>
-<td>0.6324</td>
-</tr>
-<tr>
-<td>Shell SP140</td>
-<td>4.7</td>
-<td>42.8</td>
-<td>33</td>
-<td>4.25</td>
-<td>0.002</td>
-<td>-0.152</td>
-<td>72</td>
-<td>318</td>
-<td>1.320308</td>
-</tr>
-<tr>
-<td>Shell SP150</td>
-<td>4.8</td>
-<td>43.4</td>
-<td>34</td>
-<td>4.4</td>
-<td>0.002</td>
-<td>-0.152</td>
-<td>72</td>
-<td>318</td>
-<td>1.320308</td>
-</tr>
-<tr>
-<td>Shell S70</td>
-<td>4.5</td>
-<td>21.2</td>
-<td>17</td>
-<td>4</td>
-<td>0.002</td>
-<td>-0.076</td>
-<td>36</td>
-<td>317</td>
-<td>0.7076</td>
-</tr>
-<tr>
-<td>Shell S75</td>
-<td>4.7</td>
-<td>21.6</td>
-<td>17.6</td>
-<td>4.2</td>
-<td>0.002</td>
-<td>-0.076</td>
-<td>36</td>
-<td>317</td>
-<td>0.7076</td>
-</tr>
-<tr>
-<td>Shell S105</td>
-<td>4.5</td>
-<td>31.8</td>
-<td>25.5</td>
-<td>3.9</td>
-<td>0.002</td>
-<td>-0.115</td>
-<td>54</td>
-<td>317</td>
-<td>1.037</td>
-</tr>
-<tr>
-<td>Shell S115</td>
-<td>4.7</td>
-<td>32.8</td>
-<td>26.8</td>
-<td>4.2</td>
-<td>0.002</td>
-<td>-0.115</td>
-<td>54</td>
-<td>317</td>
-<td>1.037</td>
-</tr>
-<tr>
-<td>Shell ST40</td>
-<td>2.68</td>
-<td>23.3</td>
-<td>16.6</td>
-<td>2.41</td>
-<td>0.00035</td>
-<td>-0.1</td>
-<td>16</td>
-<td>320</td>
-<td>0.424104</td>
-</tr>
-<tr>
-<td>UniSolar   PVL-64</td>
-<td>4.8</td>
-<td>23.8</td>
-<td>16.5</td>
-<td>3.88</td>
-<td>0.00065</td>
-<td>-0.1</td>
-<td>40</td>
-<td>323</td>
-<td>0.65</td>
-</tr>
-<tr>
-<td>UniSolar   PVL-128</td>
-<td>4.8</td>
-<td>47.6</td>
-<td>33</td>
-<td>3.88</td>
-<td>0.00065</td>
-<td>-0.2</td>
-<td>80</td>
-<td>323</td>
-<td>1.25</td>
-</tr>
-</table>
-
-Where:
-
-* Shunt Resistance: the value of shunt resistance is finite only if the PV Module being modeled is a thin film variety. For all crystaline silicon modules the value is essentially infinite
-
-* Shunt Resistance value: 1,000,000 W (ohms)
-
-* Module Heat Loss Coefficient: this value is dependent more on the array configuration than on the module itself.
-
-* Module Heat Loss Coefficient value: 30 W/m2-K
-
-* Module Heat Capacity: this is a typical value for a silicon based sandwich construction framed PV panel.
-
-* Module Heat Capacity Value: 50,000 J/m2-K
-
-* Reference Temperature: 298K (25C)
-
-* Insolation at Reference Conditions: 1000 W/m2
-
-* Ambient Temperature at NOCT conditions: 293K (20C)
-
-* Insolation at NOCT Conditions: 800 W/m2
-
-* Average tau-alpha Product: .9
-
-* Semiconductor Bandgap: 1.12 eV
-
-
-
-#### Field: Name
-
-This field contains the uniqe name for the photovoltaic module performance data.   The name is only used as an identifier.
-
-#### Field: Cell Type
-
-This field is used to describe the type of technology used in the PV module.   There are two options available, **CrystallineSilicon** and **AmorphousSilicon**. The choice affects the modeling.
-
-#### Field: Number of Cells in Series
-
-This field is an integer representing the number of individual cells wired in series to make up a single module. The typical number for a 12V crystalline silicon PV module is 36.
-
-#### Field: Active Area
-
-This field is the active area of the PV module in m<sup>2</sup>.
-
-#### Field: Transmittance Absorptance Product
-
-This field indicates the transmittance-absorptance product at normal incidence angles for the PV modules. If the ta product is positive, that value will be used for all angles of incidence. If the value specified is negative, then the magnitude of the given value will be used for normal incidence and the IAM modifier correlation will be used for all other angles.
-
-#### Field: Semiconductor Bandgap
-
-This field is the semiconductor bandgap for the PV material. The bandgap for silicon is 1.12 eV (electron volts).
-
-#### Field: Shunt Resistance
-
-This field is the shunt (parallel) resistance (in W) in the single diode electrical model of the PV. The shunt resistance is effectively infinite for crystalline silicon based PV modules and is finite for thin film and exotic metal modules.
-
-#### Field: Short Circuit Current
-
-This field is the short circuit current (in Amps) for an individual module in the PV array at reference conditions.
-
-#### Field: Open Circuit Voltage
-
-This field is the open circuit voltage (in Volts) for an individual module in the PV array at reference conditions.
-
-#### Field: Reference Temperature
-
-This field is the ambient temperature (in Kelvin) at reference conditions. The value is usually 298K
-
-#### Field: Reference Insolation
-
-This field is the radiation level (in W/m<sup>2</sup>) at reference conditions. The value is usually 1000 W/m<sup>2</sup>.
-
-#### Field: Module Current at Maximum Power
-
-This field is module current (in Amps) at the maximum power point and reference conditions.
-
-#### Field: Module Voltage at Maximum Power
-
-This field is module voltage (in Volts) at the maximum power point and reference conditions.
-
-#### Field: Temperature Coefficient of Short Circuit Current
-
-This field accounts for the fact that the module short circuit current is temperature dependent. The coefficient is given in Amps/Kelvin.
-
-#### Field: Temperature Coefficient of Open Circuit Voltage
-
-This field accounts for the fact that the module open circuit voltage is temperature dependent. The coefficient is given in Volts/Kelvin.
-
-#### Field: Nominal Operating Cell Temperature Test Ambient Temperature
-
-This field is the ambient temperature (in Kelvin) from the Nominal Operating Cell Temperature (NOCT) test. The value is usually 293 K
-
-#### Field: Nominal Operating Cell Temperature Test Cell Temperature
-
-This field is the cell temperature (in Kelvin) from the Nominal Operating Cell Temperature (NOCT) test.
-
-#### Field: Nominal Operating Cell Temperature Test Insolation
-
-This field is the insolation level (in W/m<sup>2</sup>) from the Nominal Operating Cell Temperature (NOCT) test. The value is usually 800 W/m<sup>2</sup>.
-
-#### Field: Module Heat Loss Coefficient
-
-This field is the heat loss coefficient (in W/m<sup>2</sup>.K) for the array. The heat loss coefficient is dependent upon measures taken to actively or passively promote airflow over the array surface. The heat loss coefficient value is used only if the Integration and Cell Temperature Mode is set to    Decoupled Ulleberg Dynamic.   
-
-#### Field: Total Heat Capacity
-
-This field is the heat capacity (in J/m<sup>2</sup>.K) of the modules in the array. It describes the module   s ability to store incident solar radiation internally. Such energy storage is manifested as a temperature increase in the modules that   is considered to be undesirable. The total heat capacity value is used only if the Integration and Cell Temperature Mode is set to    Decoupled Ulleberg Dynamic.   
-
-
-
-An IDF example:
-
-```idf
-PhotovoltaicPerformance:EquivalentOne-Diode,
-       Siemens, ! Name
-       CrystallineSilicon, !cell Type
-       36,           !cells in series [-]
-       1.0,         !module area [m2]
-       0.9,         !tau alpha product at normal incidence [-]
-       1.12,       !electron bandgap [eV]
-       1000000, !shunt resistance [ohms]
-       6.5,         !short circuit current at reference conditions [A/K]
-       21.6,       !open circuit voltage at reference conditions [V/K]
-       25,           !temperature at reference conditions [C]
-       1000,       !radiation at reference conditions [W/m2]
-       5.9,         !current at max power
-       17,           !voltage at max power
-       0.002,     !temperature coefficient of short circuit current
-       -0.079,   !temperature coefficient of open circuit voltage
-       20,           !ambient temperature at NOCT [C]
-       45,           !cell temperature at NOCT [C]
-       800,         !radiation at NOCT [W/m2]
-       30,           !heat loss coefficient [W/m2.K]
-       50000;     !total heat capacity (only used in TC mode 1)
-```
-
-
-
-### PhotovoltaicPerformance:Sandia
-
-This    PhotovoltaicPerformance:Sandia    object describes the performance of a single type of module.   The model used with this object for predicting the electricity generated by photovoltaics is referred to as the Sandia model. This model is based on work done at Sandia National Lab, Albuquerque, NM by David King -- with the help of many others.
-
-This object describes performance input data needed for specific makes and models of production PV panels using the empirical coefficients assembled by Sandia National Laboratory.   There are a large number of empirical coefficients required to use the Sandia model. These data are obtained after extensive measurements and data reduction. This testing has been performed for some types of production panels and Sandia publishes a database of module and array performance parameters on the web at www.sandia.gov/pv. The entries in the database as of January 15, 2004 were converted to idf segments and are included with the EnergyPlus release in the library file SandiaPVData.imf. There are more than hundred different module types included in the library and identified by the manufacturer   s model names listed at the beginning of the file SandiaPVData.imf. This data library file is arranged for use with EpMacro but the user can also copy .idf segments directly from the macro data set.
-
-The Sandia model itself can aggregate multiple PV modules. Therefore, an instance of a    PhotovoltaicPerformance:Sandia    object could actually represent an array of modules as well as the more usual single module. These can be can be thought of as simple larger modules and used by Generator:PV:Sandia objects in the usual manner.
-
-The many empirical coefficients for the model are listed below and are described in more more detail in the EnergyPlus engineering documentation EngineeringDoc.pdf.
-
-The field descriptions below focus on providing the parameter   s variable name as identified in the Sandia database. See the the EngineeringDoc.pdf for details on how the input fields are used in the correlations. The user generally would not need to worry about the details of the fields since he/she is not likely to generate the data on their own.
-
-#### Field: Name
-
-This field provides a unique name for the PV module. This is often the manufacturer   s identifier for a particular model of a PV module.
-
-#### Field: Active Area
-
-Units m<sup>2</sup> , real number, area of active solar electric cell for the entire module.
-
-#### Field: Number of Cells in Series
-
-   Series\_Cells    in Sandia Database.
-
-#### Field: Number of Cells in Parallel
-
-   Parallel\_Cells    in Sandia Database
-
-#### Field: Short-Circuit Current
-
-   Isco    in Sandia Database. Short-circuit current is a basic parameter Typically supplied by manufacturers at Standard Report Conditions. (Amps)
-
-#### Field: Open-Circuit Voltage
-
-   Voco    in Sandia Database,   Open-circuit voltage is a basic parameter typically provided by manufacturers a t Standard Report Conditions. (Volts)
-
-#### Field: Current at Maximum Power Point
-
-   Impo    in Sandia Database. Current at maximum powerpoint is a basic parameter provided by manufacturers at Standard Report Conditions. (Amps)
-
-#### Field: Voltage at Maximum PowerPoint
-
-   Vmpo    in Sandia Database. Voltage at maximum powerpoint is a a basic parameter typically provided by manufacturers a t Standard Report Conditions. (Volts)
-
-#### Field: Sandia Database Parameter aIsc
-
-   aIsc in Sandia Database        (1/degC)
-
-#### Field: Sandia Database Parameter   aImp
-
-   aImp    in Sandia Database   (1/degC)
-
-#### Field: Sandia Database Parameter c0
-
-   C0    in Sandia Database,       (non-dimensional)
-
-#### Field: Sandia Database Parameter c1
-
-   C1    in Sandia Database         (non-dimensional)
-
-#### Field: Sandia Database Parameter Bvoc0
-
-   Bvoco    in Sandia Database             (Volts/degC)
-
-#### Field: Sandia Database Parameter mBVoc
-
-   mBVoc      in Sandia Database         (Volts/degC)
-
-#### Field: Sandia Database Parameter BVmp0
-
-   Bvmpo    in Sandia Database               (Volts/degC)
-
-#### Field: Sandia Database Parameter mBVmp
-
-   mBVmp    in Sandia Database             (Volts/degC)
-
-#### Field:Diode Factor
-
-   n    in Sandia Database       (non-dimensional)
-
-#### Field: Sandia Database Parameter c2
-
-   C2    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter c3
-
-   C3    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter a0
-
-   A0    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter a1
-
-   A1    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter   a2
-
-   A2    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter a3
-
-   A3    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter a4
-
-   A4    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter b0
-
-   B0    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter b1
-
-   B1    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter b2
-
-   B2    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter b3
-
-   B3    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter b4
-
-   B4    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter b5
-
-   B5    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter Delta(TC)
-
-   d(Tc)    in Sandia Database     (deg C)
-
-#### Field: Sandia Database Parameter fd
-
-   fd    in Sandia Database   (non-dimensional)
-
-#### Field: Sandia Database Parameter a
-
-   a    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter b
-
-   b    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter c4
-
-   C4    in Sandia Database (non-dimensional)
-
-#### Field: Sandia Database Parameter c5
-
-   C5    in Sandia Database (non-dimensional)
-
-#### Field: Sandia Database Parameter Ix0
-
-   Ix0    in Sandia Database (Amps)
-
-#### Field: Sandia Database Parameter Ixx0
-
-   Ixx0    in Sandia Database (Amps)
-
-#### Field: Sandia Database Parameter c6
-
-   C6    in Sandia Database     (non-dimensional)
-
-#### Field: Sandia Database Parameter c7
-
-   C7    in Sandia Database     (non-dimensional)
-
-
-
-An example of the object follows:
-
-```idf
-PhotovoltaicPerformance:Sandia,
-     ASE-50-ATF-17_45, ! Module Name (production Name)
-     0.43, ! field Active Area Acoll {m2}, single module
-     36, ! NcellSer {unitless}
-     1, ! NparSerCells
-     2.90, ! Isc0 {Amps}
-     20.70, ! Voc0 {Volts}
-     2.65, ! Imp0 {Amps}
-     17.00, ! Vmp0 {Volts}
-     7.8e-04, ! aIsc {1/degC}
-     1.0e-04, ! aImp {1/degC}
-     0.99, ! C0 {unitless}
-     3.0e-03, ! C1 {unitless}
-     -0.07, ! BVoc0 {Volts/degC}
-     0.00, ! mBVoc {Volts/degC}
-     -0.07, ! BVmp0 {Volts/degC}
-     0.00, ! mBVmp {Volts/degC}
-     1.29, ! Diode Factor (n) {Unitless}
-
-
-     0.20, ! C2 {Unitless}
-     -8.60, ! C3 {Unitless}
-     0.93, ! A0 {Unitless}
-     0.05, ! A1 {Unitless}
-     -7.9402e-03, ! A2 {Unitless}
-     5.2228e-04, ! A3 {Unitless}
-     -1.3142e-05, ! A4 {Unitless}
-     1.00, ! B0 {Unitless}
-     -2.438e-03, ! B1 {Unitless}
-     3.103e-04, ! B2 {Unitless}
-     -1.246e-05, ! B3 {Unitless}
-     2.112e-07, ! B4 {Unitless}
-     -1.359e-09, ! B5 {Unitless}
-     3.00, ! dT0 {degC}
-     1.00, ! fd {Unitless}
-     -3.47, ! a {Unitless}
-     -0.05, ! b {Unitless}
-     0.98, ! C4 {Unitless}
-     0.01, ! C5 {Unitless}
-     2.86, ! Ix0 {Amps}
-     1.85, ! Ixx0 {Amps}
-     1.13, ! C6 {Unitless}
-     -0.13, ! C7 {Unitless}
-     -1.359e-09, ! B5 {Unitless}
-     3.00, ! dT0 {degC}
-     1.00; ! fd {Unitless}
-```
-
-When using EpMacro with an typical installation of EnergyPlus, the above entry can be included in an input file by adding the following two lines to an input macro file (\*.imf).
-
-\#\#include C:\\EnergyPlus\\MacroDataSets\\SandiaPVdata.imf
- ASE-50-ATF-17\_45[]
-
-### Generator:WindTurbine
-
-A wind turbine is a component that converts the kinetic energy of the surrounding airstream into electricity. This model is intended to calculate the electrical power that a wind turbine system produces. The performance of wind turbine systems is dependent on the local environmental conditions such as wind speed and density of air at the height of the systems. An analysis of these conditions is necessary to accurately estimate power output. The model obtains the weather information from the weather data file in EnergyPlus and then determines the wind speed and air density at the specific height of the system. It also requires the user to input the annual average wind speed measured at the local site and the height of the measurement so that it factors in differences between the weather file wind data and the local wind data.
-
-The model employs the general kinetic energy equation to calculate the performance characteristics of the horizontal axis wind turbine (HAWT) systems. It provides a simple approximation algorithm when the power coefficient, Cp, is available which represents the efficiency of the wind turbine in the wind power extraction from the ambient air stream. It also allows the user to input experimental constants so that the power coefficient can precisely be determined according to the characteristic of the airfoil of the system. As for the vertical axis wind turbine (VAWT) systems, it employs the general mathematical equations for straight-bladed Darrieus-type VAWT systems, which are common to VAWT systems. Various types of VAWT systems such as the Savonius-type and the curved-blade (or Egg-beater) type may be simulated with this same model.
-
-It includes two different types of dynamic power control: FixedSpeedFixedPitch (FSFP) and VariableSpeedFixedPitch (VSFP). Currently, it does not include an algorithm for modeling pitch control such as FixedSpeedVariablePitch (FSVP) and VariableSpeedVariablePitch (VSVP). If the control type of the wind turbine is either FSVP or VSVP, the control type of VSFP will be assumed. In addition, constant power generation is assumed when the ambient wind speed is between the rated wind speed and the cut out wind speed, if the user specifies one of the last three options. The model also has the ability to account for transient losses associate with the power produced during dynamic control by a user-specified fraction.
-
-The model does not include detailed algorithms for generators and inverters due to concerns for computational convergence, time, and usability. Instead, all conversion losses of these subsystems are included by applying a user-supplied total system efficiency to the maximum power extraction of the wind turbine. The field of the total system efficiency must be specified by the user.
-
-#### Field: Name
-
-A unique user assigned name for a particular wind turbine system. Any reference to this unit by another object will use this name.
-
-#### Field: Availability Schedule Name
-
-The name of the schedule (ref: Schedule) that denotes whether the wind turbine system can run during a given time period. A schedule value greater than 0 (usually 1 is used) indicates that the unit can be on during the time period. A value less than or equal to 0 (usually 0 is used) denotes that the unit is off and will not operate for the time period. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Rotor Type
-
-This field is the type of axis of the wind turbine. The user specifies either a horizontal axis wind turbine or a vertical axis wind turbine. Each type of wind turbine employs a different algorithm for the calculation of the electrical power output of the wind turbine. The default value is HorizontalAxisWindTurbine.
-
-#### Field: Power Control
-
-This field is the type of rotor control for the wind turbine. This protects the system against the overloading for a system with no speed or pitch control and also to maximize the energy yield for the system. Four different control types are classified in the literature: FixedSpeedFixedPitch (FSFP), FixedSpeedVariablePitch (FSVP), VariableSpeedFixedPitch (VSFP), and VariableSpeedVariablePitch (VSVP). Currently, FSFP and VSFP types can be modeled in EnergyPlus. The other two types will be modeled as VSFP. If the first FSFP control type is chosen, the model assumes the maximum power at a fixed rotor speed when the power output predicted is greater than the maximum until the rotor speed reaches the maximum wind speed (see next field). If one of the last three control options is chosen, the model assumes that the system produces a constant power at the rated wind speed when the wind speed is between the rated wind speed and cut-out wind speed. The default value is VariableSpeedFixedPitch (VSFP).
-
-#### Field: Rated Rotor Speed
-
-This field is the maximum rotational speed of the rotor at the rated power of the wind turbine in rev/min (revolution per minute). It is used to determine the tip speed ratio of the rotor and relative flow velocity incident on a single blade of the VAWT systems.
-
-#### Field: Rotor Diameter
-
-This field is the diameter of the rotor in meters. Note that this field is not the height of the blade, but the diameter of the perpendicular circle from the vertical pole in the VAWT systems. It determines the swept area of the rotor of the HAWT systems and the chordal velocity of the VAWT systems.
-
-#### Field: Overall Height
-
-This field is the height of the hub of the HAWT system, or of the pole of the VAWT system in meters. It is necessary to estimate local air density and the wind speed at this particular height where the wind turbine system is installed.
-
-#### Field: Number of Blades
-
-This field is the number of blades of the wind turbine. The azimuth angle of the rotor of the VAWT system is determined by dividing 360 degree by this field so that the model determines the chordal velocity component and the normal velocity component of the system. The default value is 3.
-
-#### Field: Rated Power
-
-This field is the nominal power output of the wind turbine system at the rated wind speed in Watts. Note that the user should input the maximum power of the system with no control, i.e., FSFP control type, can physically produce. Manufacturers    data also indicates it as    peak power    or    rated capacity   . If the local wind speed is greater than the rated wind speed, the model assumes constant power output of this field.
-
-#### Field: Rated Wind Speed
-
-This field is the wind speed that the wind turbine system indicates the peak in the power curve in m/s. The system produces the maximum power at this speed and the speed of the rotor is managed based on this wind speed.
-
-#### Field: Cut In Wind Speed
-
-This field is the lowest wind speed where the wind turbine system can be operated in m/s. No power generation is achieved as long as the ambient wind speed is lower than this speed.
-
-#### Field: Cut Out Wind Speed
-
-This field is the greatest wind speed in m/s. When the wind speed exceeds this value, the wind turbine system needs to be stopped because of inefficiencies in the system. All systems that have either pitch or speed control must be stopped when the ambient wind speed exceeds this speed. Note that the user should input a wind speed above which physical damage to the system might be caused in the case of a FSFP system. It appears as    extreme/survival/design wind speed    in the literature. The system will be turned off when the ambient wind speed is over this speed.
-
-#### Field: Fraction System Efficiency
-
-This field is the overall system efficiency of the wind turbine system. It includes all the conversion losses as well as transient losses during the dynamic control when the ambient wind speed is between the rated wind speed and cut-out wind speed (see previous fields). The user also has the ability to specify delivery losses from the system to the local area. If the user does not enter a fraction, the model assumes the default value of 0.835. Note that the fraction must be between zero and one.
-
-#### Field: Maximum Tip Speed Ratio
-
-This field is the maximum tip speed ratio between the rotor velocity and ambient wind velocity. The rotor speed varies with this ratio to maximize the power output when the rotor control types are variable speed ones. This field allows the user to adjust the power output from the particular system or to find the optimal tip speed ratio of the system. Optimal tip speed ratio is dependent on the number of blades. It is typically about 6, 5, and 3 for two-bladed, three-bladed, and four-bladed rotor, respectively.   For the vertical axis wind turbine, it is smaller than horizontal axis wind turbine, and varies with the chord area. The default and maximum values are 5.0 and 12.0.
-
-#### Field: Maximum Power Coefficient
-
-This field is the maximum fraction of power extraction from ambient wind. If the user inputs this field, the simple approximation model is assumed. The model simply employs the value of this field into the general kinetic energy equation, so that the power output is obtained. The user can obtain this field with a simple calculation from the power curve published in almost all manufacturers' specifications by using the kinetic energy equation as:
-
-<div>\[{C_p} = \frac{P}{{0.5\rho A{V^3}}}\]</div>
-
-where
-
-*P* = power production at the rated wind speed [W]
-
-*�* = density of air [kg/m3]
-
-*A* = swept area of rotor [m2]
-
-*V* = rated wind speed [m/s]
-
-*C<sub>p</sub>* = power coefficient
-
-The maximum and default values are 0.59 and 0.35.
-
-#### Field: Annual Local Average Wind Speed
-
-This field is the local annual average wind speed that represents a representative wind profile at the location of the system in m/s. It is used to factor the difference in wind speed between the weather file wind data and the locally measured wind data so that the model minimizes uncertainties caused by improper wind data at the particular location. Considerable differences between the weather file wind data and the local wind data typically appear. The user thus needs to enter this field in order to obtain accurate local wind data. The model internally determines a multiplier and it is multiplied by the weather file wind data adjusted at the height of the system. If this field is not entered, then the model will use the wind speed from the design day or weather file information with only adjustment at the height of the rotor.
-
-#### Field: Height for Local Average Wind Speed
-
-This field is the height that the local wind speed is measured in meters. The annual average wind speed (see previous field) input by the user is internally recalculated by existing EnergyPlus functions at the height of the local station. This modified wind speed is then factored and applied to the weather file wind data. If the annual local average wind speed is not entered, this field is then assumed as zero. The minimum and default values are zero and 50 meters.
-
-#### Field: Blade Chord Area
-
-This field is the blade chord area of a single blade of VAWT system in m2. It is necessary to determine the net tangential and normal forces of a single blade.
-
-#### Field: Blade Drag Coefficient
-
-This field is the blade drag coefficient for a specific blade. It is for determining the tangential and normal force coefficients with the blade lift coefficient (see next field) so that the model can calculate the power output from the system. The user should be able to obtain this parameter for a specific blade from the manufacturers    data. This field is only valid for VAWT systems.
-
-#### Field: Blade Lift Coefficient
-
-This field is the blade lift coefficient for a specific blade. It is for determining the tangential and normal force coefficients with the blade drag coefficient (see previous field) so that the model can calculate the power output from the system. The user should also be able to obtain it for a specific blade from the manufacturers    data. This field is only valid for VAWT systems.
-
-#### Field: Power Coefficient Parameter &lt;x&gt;
-
-These six fields are the parameters for the power coefficient equation shown below. These fields are used to determine the power coefficient of the system. The analytical approximation model of the power coefficient in EnergyPlus is:
-
-<div>\[{C_p} = {C_1}(\frac{{{C_2}}}{{{\lambda_i}}} - {C_3}\theta  - {C_4}{\theta ^x} - {C_5}){e^{ - \frac{{{C_6}(\lambda ,\theta )}}{{{\lambda_i}}}}}\]</div>
-
-with
-
-<div>\[\frac{1}{{{\lambda_i}}} = \frac{1}{{\lambda  + 0.08\theta }} - \frac{{0.035}}{{{\theta ^3} + 1}}\]</div>
-
-where
-
-<span>\(C_p\)</span> = power coefficient
-
-<span>\(C_{1-6}\)</span> = empirical power coefficient parameters
-
-<span>\(\lambda\)</span> = tip speed ratio (often known as TSR)
-
-<span>\(\lambda_i\)</span> = tip speed ratio at ith time step
-
-<span>\(\theta\)</span> = azimuth angle of the pitch, 0 [degree]
-
-
-
-If the user does not input any field of these parameters, the simple approximation model for the power coefficient will be used (see previous maximum power coefficient field). That is, the analytical approximation model of the power coefficient will be chosen only if the user inputs all these six parameters. The user also has the ability to modify each parameter when the specific value of the system is available. The default values are given in the table below.
-
-<table class="table table-striped">
-<tr>
-<th>C<sub>1</sub></th>
-<th>C<sub>2</sub></th>
-<th>C<sub>3</sub></th>
-<th>C<sub>4</sub></th>
-<th>C<sub>5</sub></th>
-<th>C<sub>6</sub></th>
-</tr>
-<tr>
-<td>0.5176</td>
-<td>116</td>
-<td>0.4</td>
-<td>0.0</td>
-<td>5.0</td>
-<td>21</td>
-</tr>
-</table>
-
-These fields are only valid for HAWT systems.
-
-An example input for the wind turbine is shown in below.
-
-```idf
-Generator:WindTurbine,
-WT1,                     ! Name
-WT Schedule,     ! Availability Schedule Name
-HorizontalAxisWindTurbine,     ! Rotor type
-FixedSpeedVariablePitch,         ! Power control type
-41,                       ! Maximum rotational speed of the rotor {rev/min}
-19.2,                   ! Diameter of the rotor {m}
-30.5,                   ! Overall height of the system {m}
-3,                         ! Number of blades
-55000,                 ! Rated power output at the rated wind speed {W}
-11,                       ! Rated wind speed {m/s}
-3.5,                     ! Cut In wind speed {m/s}
-25,                       ! Cut Out wind speed {m/s}
-0.835,                 ! Overall wind turbine system efficiency
-8,                         ! Maximum tip speed ratio
-0.4,                     ! Maximum power coefficient
-6.4,                     ! Annual local wind speed {m/s}
-50,                       ! Height of local meteorological station {m}
-,                           ! Blade chord area {m2}
-,                           ! Blade drag coefficient
-,                           ! Blade lift coefficient
-0.5176,               ! Power Coefficient C1
-116,                     ! Power Coefficient C2
-0.4,                     ! Power Coefficient C3
-0,                         ! Power Coefficient C4
-5,                         ! Power Coefficient C5
-21;                       ! Power Coefficient C6
-```
-
-
-### Generator:WindTurbine Outputs
-
-* HVAC,Average, Generator Produced Electric Power [W]
-
-* HVAC,Sum, Generator Produced Electric Energy [J]
-
-* HVAC,Average, Generator Turbine Local Wind Speed [m/s]
-
-* HVAC,Average, Generator Turbine Local Air Density [kg/m3]
-
-* HVAC,Average, Generator Turbine Power Coefficient []
-
-* HVAC,Average, Generator Turbine Tip Speed Ratio []
-
-* HVAC,Average, Generator Turbine Chordal Component Velocity [m/s]
-
-* HVAC,Average, Generator Turbine Normal Component Velocity [m/s]
-
-* HVAC,Average, Generator Turbine Relative Flow Velocity [m/s]
-
-* HVAC,Average, Generator Turbine Attack Angle [deg]
-
-
-#### Generator Produced Electric Power [W]
-
-This report is the electric power that the wind turbine system produces.
-
-#### Generator Produced Electric Energy [J]
-
-This report is the electric energy that the wind turbine system produces.
-
-#### Generator Turbine Local Wind Speed [m/s]
-
-This report is the local wind speed at the specific height of the wind turbine.
-
-#### Generator Turbine Local Air Density [kg/m3]
-
-This report is the local density of the air at the specific height of the wind turbine.
-
-#### Generator Turbine Tip Speed Ratio []
-
-This report is the ratio between the rotational speed of the tip of the blades and the ambient wind speed at the height of the hub or pole of the wind turbine.
-
-#### Generator Turbine Power Coefficient []
-
-This report represents the efficiency of the power extraction from the ambient wind of the wind turbine. It is function of the tip speed ratio and pitch angle. It is only valid for HAWT systems.
-
-#### Generator Turbine Chordal Component Velocity [m/s]
-
-This report is the axial velocity component along the chord of the wind turbine system. It is only valid for VAWT systems.
-
-#### Generator Turbine Normal Component Velocity [m/s]
-
-This report is the axial velocity component of the rotor of the wind turbine system. It is only valid for VAWT systems.
-
-#### Generator Turbine Relative Flow Velocity [m/s]
-
-This report is the local relative flow velocity that represents actual direction and velocity incident on the blades. It is the square root of the sum of both chordal velocity component and normal velocity component. It is only valid for VAWT systems.
-
-#### Generator Turbine Attack Angle [deg]
-
-This report is the azimuth angle between the relative flow velocity and the plane of chord. It varies as the wind speed increases, so that the lift and drag forces change.
-
-
-------------------------------------------------------------------------
-
-[[1]](#_ftnref1) Ulleberg &#216; . (1997) Simulation of autonomous PV-H2 systems: analysis of the PHOEBUS plant design, operation and energy management. In *Proceedings of ISES 1997 Solar World Congress*, August 24-30, Taejon, Korea.
-
-Ulleberg &#216; . (1998) *Stand-Alone Power Systems for the Future: Optimal Design, Operation & Control of Solar-Hydrogen Energy Systems*. PhD thesis, Norwegian University of Science and Technology, Trondheim.
-
-
-Group     Water Systems
----------------------
-
-This group of objects is used to describe the water systems in the building. EnergyPlus offers water modeling capabilities than include not only hot water systems but also the overall water systems including cold water uses, on-site water collection (e.g., from rain, condensate, or well), and storage. HVAC components may consume or collect a significant portion of the water making it appropriate to include water modeling in EnergyPlus.
-
-All water systems are collected into an end use category called    Water Systems   . This category includes hot and cold water. Water consumed by an HVAC component will be assigned to the end use category for that component. End use subcategories are available to separate hot water from cold water if desired. Simple hot water systems can be configured as stand-alone or use a PlantLoop. The Water Systems can be connected to PlantLoops for modeling heated water end uses. However PlantLoops are not used to model cold water and the WaterUse:Storages portions of the water system. Cold water systems are connected together using WaterUse:Storage objects. WaterUse:Connections are used at the zone level to connect to both cold and hot water.
-
-In addition to the input objects described in this section below, there are a variety of HVAC components that can be configured to interact with the water systems. These component input objects include optional fields that allow describing how the water systems are connected to them by providing the name of a storage tank. The following table lists EnergyPlus input objects that include provisions for connecting to the water systems but are described elsewhere in this document:
-
-Table 34. Water Systems Objects
-
-<table class="table table-striped">
-  <tr>
-    <th>Input Object Name</th>
-    <th>Type of Water Interactions</th>
-  </tr>
-  <tr>
-    <td>Site:Precipitation</td>
-    <td>Describes rainfall for WaterUse:RainCollector</td>
-  </tr>
-  <tr>
-    <td>Coil:Cooling:Water</td>
-    <td>Condensate collection to WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>Coil:Cooling:Water:DetailedGeometry</td>
-    <td>Condensate collection to WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Coil:Cooling:DX:SingleSpeed</td>
-    <td>Optional evaporative condenser can be supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>Condensate collection to WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Coil:Cooling:DX:TwoSpeed</td>
-    <td>Evaporative condenser supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>Condensate collection to WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Coil:Cooling:DX:TwoStageWithHumidityControlMode</td>
-    <td>Evaporative condenser supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>Condensate collection to WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td rowspan="2">Coil:Cooling:DX:MultiSpeed</td>
-    <td>Evaporative condenser supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>Condensate collection to WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>Humidifier:Steam:Electric</td>
-    <td>Water supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>CoolingTower:SingleSpeed</td>
-    <td>Water supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>CoolingTower:TwoSpeed</td>
-    <td>Water supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>CoolingTower:VariableSpeed</td>
-    <td>Water supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>ZoneCoolTower:Shower</td>
-    <td>Water supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>Refrigeration:CompressorRack</td>
-    <td>Water supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>Refrigeration:Condenser:EvaporativeCooled</td>
-    <td>Water supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>EvaporativeCooler:Direct:CelDekPad</td>
-    <td>Evaporation water supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>EvaporativeCooler:Indirect:CelDekPad</td>
-    <td>Evaporation water supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>EvaporativeCooler:Indirect:WetCoil</td>
-    <td>Evaporation water supplied by WaterUse:Storage</td>
-  </tr>
-  <tr>
-    <td>EvaporativeCooler:Indirect:ResearchSpecial</td>
-    <td>Evaporation water supplied by WaterUse:Storage</td>
-  </tr>
-</table>
-
-
-### WaterUse:Equipment
-
-The WaterUse:Equipment object is a generalized object for simulating all water end uses. Hot and cold water uses are included, as well as controlled mixing of hot and cold water at the tap. The WaterUse:Equipment object can be used stand-alone, or coupled into a plant loop using the WaterUse:Connections object (see below). The WaterUse:Connections object allows water uses to be linked to WaterUse:Storage objects to store and draw reclaimed water. The WaterUse:Connections object can also simulate drainwater heat recovery.
-
-The WaterUse:Equipment object serves all of the same purposes as the existing objects:   Exterior:WaterEquipment, and HotWaterEquipment.
-
-The WaterUse:Equipment object does a better job of modeling domestic hot water by allowing mixing at the tap in order to account for both hot **and cold** water used at sinks, showers, etc. It also improves on the stand-alone energy modeling of domestic hot water. Because all of the temperatures and flow rates can be solved, the energy usage can be accounted for as "Purchased Heating".
-
-In either stand-alone mode or used with the WaterUse:Connections object, the WaterUse:Equipment object will attempt to meet a scheduled target temperature at the tap by mixing hot and cold water flows. If the hot water flow is not hot enough, or if the flow is limited by plant loop constraints, the result is a cooler mixed water temperature and the target temperature will not be met. In stand-alone mode the hot and cold water temperatures are specified by schedules. However, if the cold water schedule is omitted, the water temperature will be calculated by the Site:WaterMainsTemperature object. If the hot water schedule or target temperature schedule are omitted, all water is delivered as cold water. If only using cold water, the WaterUse:Equipment object is similar to the Exterior:WaterEquipment object.
-
-The WaterUse:Equipment object improves on the internal gains object HotWaterEquipment by associating actual water usage with a sensible and latent gain to a zone. Equipment, such as showers, that generate a significant heat gain can be modeled using the Sensible Fraction Schedule and Latent Fraction Schedule fields. The schedules are used to set the fraction of the maximum possible heat gain (based on inlet water conditions and ambient zone conditions) that should be added to the zone. The split between sensible and latent will vary depending on the type of equipment that is to be modeled. Typically, both fractions should be small numbers.
-
-#### Field: Name
-
-The unique object name for reference by other objects.
-
-#### Field: End-Use Subcategory
-
-Allows you to specify a user-defined end-use subcategory, e.g., "Laundry", "Dish Washing", etc. A new meter for reporting is created for each unique subcategory (ref: Output:Meter objects). Subcategories are also reported in the ABUPS table under the "Water Systems" end-use category. If this field is omitted or blank, the water use will be assigned to the "General" end-use subcategory.
-
-#### Field: Peak Flow Rate
-
-The peak demanded hot water flow rate [m<sup>3</sup>/s]. This value is multiplied by the Flow Rate Fraction Schedule (below) to determine the actual volumetric flow rate.
-
-#### Field: Flow Rate Fraction Schedule Name
-
-Reference to the schedule object specifying the flow rate fraction relative to the Peak Flow Rate (above). If blank, the schedule defaults to 1.0 at all times.
-
-#### Field: Target Temperature Schedule Name
-
-Reference to the schedule object specifying the target water temperature [C]. Hot and cold water are mixed at the tap to attain the target temperature. If insufficient hot water is available to reach the target temperature, the result is cooler water at the tap. If blank, the target temperature defaults to the hot water supply temperature.
-
-#### Field: Hot Water Supply Temperature Schedule Name
-
-Reference to the schedule object specifying the hot water temperature [C]. The hot water temperature is used to calculate the "Purchased Heating" energy usage in stand-alone mode. If blank in stand-alone mode, the hot water supply temperature defaults to the cold water supply temperature. This field is ignored if the object is used with the WaterUse:Connections object.
-
-#### Field: Cold Water Supply Temperature Schedule Name
-
-Reference to the Schedule object specifying the cold water temperature [C] from the supply mains that provides the cold water to the tap and makes up for all water lost down the drain. If blank, water temperatures are calculated by the Site:WaterMainsTemperature object. This field is ignored if the object is used with the WaterUse:Connections object.
-
-#### Field: Zone Name
-
-Reference to the zone name where the water equipment will be considered as latent load to the zone.
-
-#### Field: Sensible Fraction Schedule Name
-
-Reference to the schedule object specifying the fraction of the maximum possible sensible heat gain (based on inlet water conditions and ambient zone conditions) that is added to the zone. If blank, the schedule defaults to 0 at all times.
-
-#### Field: Latent Fraction Schedule Name
-
-Reference to the schedule object specifying the fraction of the maximum possible latent heat gain (based on inlet water conditions and ambient zone conditions) that is added to the zone. If blank, the schedule defaults to 0 at all times.
-
-IDF examples:
-
-```idf
-WaterUse:Equipment,
-   Landscaping,   !- Name
-   Landscaping,   !- End-Use Subcategory
-   0.003;               !- Peak Flow Rate {m3/s}
-
-WaterUse:Equipment,
-   Dishwashing,   !- Name
-   Domestic Hot Water,   !- End-Use Subcategory
-   0.001,   !- Peak Flow Rate {m3/s}
-   Dishwashing Schedule,   !- Flow Rate Fraction Schedule Name
-   Dishwashing Target Temp,   !- Target Temperature Schedule Name
-   Hot Water Temp,   !- Hot Water Supply Temperature Schedule Name
-   Mains Water;   !- Cold Water Supply Temperature Schedule Name
-
-WaterUse:Equipment,
-   Showers,   !- Name
-   Domestic Hot Water,   !- End-Use Subcategory
-   0.0002,   !- Peak Flow Rate {m3/s}
-   Shower Schedule,   !- Flow Rate Fraction Schedule Name
-   Shower Target Temp,   !- Target Temperature Schedule Name
-   Hot Water Temp,   !- Hot Water Supply Temperature Schedule Name
-   ,   !- Cold Water Supply Temperature Schedule Name
-   Shower Room,   !- Zone Name
-   Sensible Frac Schedule,   !- Sensible Fraction Schedule Name
-   Latent Frac Schedule;   !- Latent Fraction Schedule Name
-```
-
-
-### WaterUse:Equipment Outputs
-
-The following output variables are reported for the WaterUse:Equipment object:
-
-* HVAC,Average,Water Use Equipment Hot Water Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water Use Equipment Cold Water Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water Use Equipment Total Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water Use Equipment Hot Water Volume Flow Rate [m3/s]
-
-* HVAC,Average,Water Use Equipment Cold Water Volume Flow Rate [m3/s]
-
-* HVAC,Average,Water Use Equipment Total Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Water Use Equipment Hot Water Volume [m3]
-
-* HVAC,Sum,Water Use Equipment Cold Water Volume [m3]
-
-* HVAC,Sum,Water Use Equipment Total Volume [m3]
-
-* HVAC,Sum,Water Use Equipment Mains Water Volume [m3]
-
-* HVAC,Average,Water Use Equipment Hot Water Temperature [C]
-
-* HVAC,Average,Water Use Equipment Cold Water Temperature [C]
-
-* HVAC,Average,Water Use Equipment Target Water Temperature [C]
-
-* HVAC,Average,Water Use Equipment Mixed Water Temperature [C]
-
-* HVAC,Average,Water Use Equipment Drain Water Temperature [C]
-
-* HVAC,Average,Water Use Equipment Heating Rate [W]
-
-* HVAC,Sum,Water Use Equipment Heating Energy [J]
-
-* HVAC,Average,Water Use Equipment Zone Sensible Heat Gain Rate [W]
-
-* HVAC,Sum,Water Use Equipment Zone Sensible Heat Gain Energy [J]
-
-* HVAC,Average,Water Use Equipment Zone Latent Gain Rate [W]
-
-* HVAC,Sum,Water Use Equipment Zone Latent Gain Energy [J]
-
-* HVAC,Average,Water Use Equipment Zone Moisture Gain Mass Flow Rate [kg/s]
-
-* HVAC,Sum,Water Use Equipment Zone Moisture Gain Mass [kg]
-
-#### Water Use Equipment Hot Water Mass Flow Rate [kg/s]
-
-The mass flow rate of hot water supplied to the equipment, in units of kilograms per second (kg/s).
-
-#### Water Use Equipment Cold Water Mass Flow Rate [kg/s]
-
-The mass flow rate of cold water supplied to the equipment, in units of kilograms per second (kg/s).
-
-#### Water Use Equipment Total Mass Flow Rate [kg/s]
-
-The total mass flow rate of water (hot + cold) supplied to the equipment, in units of kilograms per second (kg/s).
-
-#### Water Use Equipment Hot Water Volume Flow Rate [m3/s]
-
-The volumetric flow rate of hot water supplied to the equipment and consumed down the drain, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water Use Equipment Cold Water Volume Flow Rate [m3/s]
-
-The volumetric flow rate of cold water supplied to the equipment and consumed down the drain, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water Use Equipment Total Volume Flow Rate [m3/s]
-
-The total volumetric flow rate of water (hot + cold) supplied to the equipment and consumed down the drain, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water Use Equipment Hot Water Volume [m3]
-
-The volume of hot water supplied to the equipment and consumed down the drain, in units of cubic meters (m<sup>3</sup>).
-
-#### Water Use Equipment Cold Water Volume [m3]
-
-The volume of cold water supplied to the equipment and consumed down the drain, in units of cubic meters (m<sup>3</sup>).
-
-#### Water Use Equipment Total Volume [m3]
-
-The total volume of water (hot+cold) supplied to the equipment and consumed down the drain, in units of cubic meters (m<sup>3</sup>). This output is also added to a meter with Resource Type = Water, End Use Key = WaterSystems, and Group Key = Plant. The sub-categories may be entered as any type (e.g., Laundry, Dish Washing, etc. defined in WaterUse:Equipment object input for End-Use Subcategory) with General being the default sub-category (ref. Output Meter)
-
-#### Water Use Equipment Mains Water Volume [m3]
-
-The total volume of water (hot+cold) supplied to the equipment and consumed down the drain, in units of cubic meters (m<sup>3</sup>). This output is also added to a meter with Resource Type = MainsWater, End Use Key = WaterSystems, and Group Key = Plant. The sub-categories may be entered as any type (e.g., Laundry, Dish Washing, etc. defined in WaterUse:Equipment object input for End-Use Subcategory) with General being the default sub-category (ref. Output Meter)
-
-#### Water Use Equipment Hot Water Temperature [C]
-
-The temperature of hot water supplied to the equipment, in units of degrees Celsius (C).
-
-#### Water Use Equipment Cold Water Temperature [C]
-
-The temperature of cold water supplied to the equipment, in units of degrees Celsius (C).
-
-#### Water Use Equipment Target Water Temperature [C]
-
-The user-specified target temperature for the mixing of hot and cold supply flows, in units of degrees Celsius (C).
-
-#### Water Use Equipment Mixed Water Temperature [C]
-
-The actual mixed water temperature possible with the available hot and cold temperatures and flow rates, in units of degrees Celsius (C).
-
-#### Water Use Equipment Drain Water Temperature [C]
-
-The water temperature at the drain equal to the mixed water temperature minus any heat loss to the zone, in units of degrees Celsius (C).
-
-#### Water Use Equipment Heating Rate [W]
-
-The heating rate defined by the hot water flow and the temperature difference between the hot water supply and the cold makeup return water, in units of watts (W).
-
-#### Water Use Equipment Heating Energy [J]
-
-The heating energy accumulated by the heating rate above, in units of Joules (J). This output is also added to a meter with End Use Key = WaterSystems, Group Key = Plant. If both of the node names specified in the WaterUse:Equipment object are blank, then this output is reported with Resource Type = DistrictHeating. If either of the node names are entered, then this output is reported with Resource Type = EnergyTransfer. The sub-categories may be entered as any type (e.g., Laundry, Dish Washing, etc. defined in WaterUse:Equipment object input for End-Use Subcategory) with General being the default sub-category (ref. Output Meter)
-
-#### Water Use Equipment Zone Sensible Heat Gain Rate [W]
-
-The sensible heat rate to the zone due to the water flow being exposed to zone air, in units of watts (W).
-
-#### Water Use Equipment Zone Sensible Heat Gain Energy [J]
-
-The sensible heat energy accumulated by the latent heat rate above, in units of Joules (J).
-
-#### Water Use Equipment Zone Latent Gain Rate [W]
-
-The latent heat rate to the zone due to the water flow being exposed to zone air, in units of watts (W).
-
-#### Water Use Equipment Zone Latent Gain Energy [J]
-
-The latent heat energy accumulated by the latent heat rate above, in units of Joules (J).
-
-#### Water Use Equipment Zone Moisture Gain Mass Flow Rate [kg/s]
-
-The moisture rate of evaporation to the zone due to the water flow being exposed to zone air, in units of kilograms per second (kg/s).
-
-#### Water Use Equipment Zone Moisture Gain Mass [kg]
-
-The moisture mass accumulated by the moisture rate above, in units of kilograms (kg).
-
-### WaterUse:Connections
-
-The WaterUse:Connections object can be thought of as a subsystem that groups together multiple WaterUse:Equipment components. As its name suggests, the object provides connections that are shared by these components, including:
-
-- Inlet node and outlet node connections to a plant loop
-
-- Connections to WaterUse:Storage objects to store and draw reclaimed water
-
-- Internal connections to simulate drainwater heat recovery.
-
-![Water Use Connections IO Diagram](media/image579.png)
-
-Figure 153. Diagram of internal connections for WaterUse:Connections
-
-The WaterUse:Connections object can be used stand-alone or coupled into a plant loop. In stand-alone mode, the Hot and Cold Water Supply Temperature Schedules override the values for the listed WaterUse:Equipment objects. When coupled to the plant, the Hot Water Supply Temperature Schedule is overridden by the actual plant loop inlet water temperature. When coupled to the plant, the WaterUse:Connections object should be on a Branch object whose control type is set to    Active.   
-
-#### Field: Name
-
-The unique object name for reference by other objects.
-
-#### Field: Inlet Node Name
-
-The hot water inlet node when connected to a plant loop. The hot water supplies all of the WaterUse:Equipment objects that demand hot water. Insufficient supply temperature or flow results in cooler water at the tap.
-
-#### Field: Outlet Node Name
-
-The cold water outlet node, i.e. the cold water supply mains, when connected to a plant loop. The return node provides make-up water for the hot water lost down the drain.
-
-#### Field: Supply Water Storage Tank Name
-
-Reference to the WaterUse:Storage object that supplies cold water to the listed WaterUse:Equipment objects. If the field is blank, or the tank is empty, fresh water is supplied from the water mains.
-
-#### Field: Reclamation Water Storage Tank Name
-
-Reference to the WaterUse:Storage object that stores the resulting graywater from the listed WaterUse:Equipment objects. If the field is blank, the graywater is not reclaimed.
-
-#### Field: Hot Water Supply Temperature Schedule Name
-
-Reference to the schedule object specifying the hot water temperature [C]. If blank in stand-alone mode, the hot water supply temperature defaults to the cold water supply temperature. This field (even if blank) overrides the Hot Water Supply Temperature Schedule in all of the listed WaterUse:Equipment objects.
-
-#### Field: Cold Water Supply Temperature Schedule Name
-
-Reference to the schedule object specifying the cold water temperature [C] from the supply mains that provides the cold water to the tap and makes up for all water lost down the drain. If blank, water temperatures are calculated by the Site:WaterMainsTemperature object.
-
-This field (even if blank) overrides the Cold Water Supply Temperature Schedule in all of the listed WaterUse:Equipment objects.
-
-#### Field: Drain Water Heat Exchanger Type
-
-The heat exchanger type to be used for drainwater heat recovery. None indicates no heat recovery is to be simulated. Ideal sets a heat exchanger effectiveness of 1.0. Effectiveness is calculated dynamically for CounterFlow and CrossFlow options.
-
-One popular type of drainwater heat exchanger is the Gravity-Film Heat Exchanger (GFX). The GFX is most closely approximated with the CounterFlow option, but keep in mind that the UA varies more with flow rate for the GFX than for most traditional heat exchangers.
-
-#### Field: Drain Water Heat Exchanger Destination
-
-The heat exchanger configuration to be used for drainwater heat recovery. The configuration determines where the heat will be used after it is recovered.
-
-Plant indicates that the all of the recovered heat will be sent to the return flow at the outlet node of the WaterUse:Connections object to preheat the make-up cold water from the water mains.
-
-Equipment indicates that the all of the recovered heat will be used to preheat the cold water flow side of the WaterUse:Equipment objects listed *in this* WaterUse:Connections object
-
-PlantAndEquipment indicates the recovered heat will be divided between the plant and the WaterUse:Equipment objects, as described above. This is the only option where the flow rates are equal in the drain and the heat exchanger.
-
-#### Field: Drain Water Heat Exchanger U-Factor Times Area
-
-The UA is the heat transfer coefficient [W/K] for the heat exchanger and is the product of U, the overall heat transfer coefficient, and A, the heat exchanger surface area.
-
-#### Field: Water Use Equipment 1-10 Name
-
-References to WaterUse:Equipment objects.
-
-IDF examples:
-
-```idf
-WaterUse:Connections,
-   Domestic Water Uses,   !- Name
-   Water Eq Inlet Node,   !- Inlet Node Name
-   Water Eq Outlet Node, !- Outlet Node Name
-   Rainwater Storage,   !- Supply Water Storage Tank Name
-   Graywater Storage,   !- Reclamation Water Storage Tank Name
-   ,   !- Hot Water Supply Temperature Schedule Name
-   ,   !- Cold Water Supply Temperature Schedule Name
-   CounterFlow,   !- Drain Water Heat Exchanger Type
-   Plant,   !- Drain Water Heat Exchanger Destination
-   1500,   !- Drain Water Heat Exchanger U-Factor Times Area {W/K}
-   Sinks,   !- Water Use Equipment 1 Name
-   Showers,   !- Water Use Equipment 2 Name
-   Dishwasher,   !-   Water Use Equipment 3 Name
-   Clotheswasher;   !- Water Use Equipment 4 Name
-```
-
-### WaterUse:Connections Outputs
-
-The following output variables are reported for the WaterUse:Connections object:
-
-* HVAC,Average,Water Use Connections Hot Water Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water Use Connections Cold Water Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water Use Connections Total Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water Use Connections Drain Water Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water Use Connections Heat Recovery Mass Flow Rate [kg/s]
-
-* HVAC,Average,Water Use Connections Hot Water Volume Flow Rate [m3/s]
-
-* HVAC,Average,Water Use Connections Cold Water Volume Flow Rate [m3/s]
-
-* HVAC,Average,Water Use Connections Total Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Water Use Connections Hot Water Volume [m3]
-
-* HVAC,Sum,Water Use Connections Cold Water Volume [m3]
-
-* HVAC,Sum,Water Use Connections Total Volume [m3]
-
-* HVAC,Average,Water Use Connections Hot Water Temperature [C]
-
-* HVAC,Average,Water Use Connections Cold Water Temperature [C]
-
-* HVAC,Average,Water Use Connections Drain Water Temperature [C]
-
-* HVAC,Average,Water Use Connections Return Water Temperature [C]
-
-* HVAC,Average,Water Use Connections Waste Water Temperature [C]
-
-* HVAC,Average,Water Use Connections Heat Recovery Water Temperature [C]
-
-* HVAC,Average,Water Use Connections Heat Recovery Effectiveness []
-
-* HVAC,Average,Water Use Connections Heat Recovery Rate [W]
-
-* HVAC,Sum,Water Use Connections Heat Recovery Energy [J]
-
-* HVAC,Sum,Water Use Connections Plant Hot Water Energy [J]
-
-
-
-#### Water Use Connections Hot Water Mass Flow Rate [kg/s]
-
-The mass flow rate of hot water supplied to all equipment, in units of kilograms per second (kg/s).
-
-#### Water Use Connections Cold Water Mass Flow Rate [kg/s]
-
-The mass flow rate of cold water supplied to all equipment, in units of kilograms per second (kg/s).
-
-#### Water Use Connections Total Mass Flow Rate [kg/s]
-
-The total mass flow rate of water (hot + cold) supplied to all equipment, in units of kilograms per second (kg/s).
-
-#### Water Use Connections Drain Water Mass Flow Rate [kg/s]
-
-The mass flow rate of drainwater from all equipment, in units of kilograms per second (kg/s).
-
-#### Water Use Connections Heat Recovery Mass Flow Rate [kg/s]
-
-The mass flow rate of make-up water in the heat exchanger, in units of kilograms per second (kg/s).
-
-#### Water Use Connections Hot Water Volume Flow Rate [m3/s]
-
-The volumetric flow rate of hot water supplied to all equipment and consumed down the drain, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water Use Connections Cold Water Volume Flow Rate [m3/s]
-
-The volumetric flow rate of cold water supplied to all equipment and consumed down the drain, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water Use Connections Total Volume Flow Rate [m3/s]
-
-The total volumetric flow rate of water (hot + cold) supplied to all equipment and consumed down the drain, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water Use Connections Hot Water Volume [m3]
-
-The volume of hot water supplied to all equipment and consumed down the drain, in units of cubic meters (m<sup>3</sup>).
-
-#### Water Use Connections Cold Water Volume [m3]
-
-The volume of cold water supplied to all equipment and consumed down the drain, in units of cubic meters (m<sup>3</sup>).
-
-#### Water Use Connections Total Volume [m3]
-
-The total volume of water (hot+cold) supplied to all equipment and consumed down the drain, in units of cubic meters (m<sup>3</sup>).
-
-#### Water Use Connections Hot Water Temperature [C]
-
-The temperature of hot water supplied to all equipment, in units of degrees Celsius (C).
-
-#### Water Use Connections Cold Water Temperature [C]
-
-The temperature of cold water supplied to all equipment, in units of degrees Celsius (C).
-
-#### Water Use Connections Drain Water Temperature [C]
-
-The water temperature at the drain equal to the mixed water temperature minus any heat losses to the zone, in units of degrees Celsius (C).
-
-#### Water Use Connections Return Water Temperature [C]
-
-The temperature of make-up water returned to the plant loop, in units of degrees Celsius (C).
-
-#### Water Use Connections Waste Water Temperature [C]
-
-The temperature of the water leaving the heat exchanger. If no heat exchanger, the waste water temperature equals the drain water temperature, in units of degrees Celsius (C).
-
-#### Water Use Connections Heat Recovery Water Temperature [C]
-
-The temperature of the water leaving the heat exchanger. If no heat exchanger, the waste water temperature equals the drain water temperature, in units of degrees Celsius (C).
-
-#### Water Use Connections Heat Recovery Effectiveness []
-
-The effectiveness value of the heat exchanger. The units are dimensionless.
-
-#### Water Use Connections Heat Recovery Rate [W]
-
-The heat recovered by the heat exchanger and used to preheat the cold make-up water, in units of watts (W).
-
-#### Water Use Connections Heat Recovery Energy [J]
-
-The energy recovered by the heat exchanger and used to preheat the cold make-up water, in units of Joules (J).
-
-#### Water Use Connections Plant Hot Water Energy [J]
-
-The plant loop energy consumed by the hot water used, in units of Joules (J). This output is also added to a meter with Resource Type = PlantLoopHeatingDemand, End Use Key = WaterSystems, and Group Key = Plant (ref. Output Meter).
-
-### WaterUse:Storage
-
-The WaterUse:Storage object is a central component for complex water systems. This object is not needed if the only use of water is directly from the mains, or utility service water. If the building model is to include any on-site collection or wells or storing and reuse of graywater, then a WaterUse:Storage is needed. Each WaterUse:Storage can serve as a central node and make connections to numerous sources of supply or numerous components with demand. If a maximum capacity is not specified, the tank is assumed to have unlimited capacity. This is useful for sizing.
-
-Storage tanks may handle a lot of water but show no use. This is because water usage is metered at the component level were water is    used up.      The only water a storage tank might use up is overflow water if it is discarded.
-
-#### Field: Name
-
-The unique object name for reference by other objects.
-
-#### Field: Water Quality Subcategory
-
-Describes the quality of the water contained in the tank. Used for reporting and to check that the uses and supply match the category of water quality.
-
-#### Field: Maximum Capacity
-
-The maximum volumetric capacity [m3] of the water tank. If blank, this field defaults to unlimited capacity.
-
-#### Field: Initial Volume
-
-The volume of water in the storage tank at the beginning of each simulation environmental period [m3]. This provides a starting point for the amount of water in storage.
-
-#### Field: Design In Flow Rate
-
-The design flow rate [m3/s] of fittings that provide water into the tank from external sources. In a scenario where a heavy rain fall is being harvested, the actual reclamation rate might be limited by pipe size or filtration. If blank, this field defaults to unlimited rate.
-
-#### Field: Design Out Flow Rate
-
-The design flow rate [m3/s] of fitting that withdraw water from the tank to end uses. Heavy demand (landscaping?) might be limited by pipe size or filtration. If Blank, this field defaults to unlimited rate.
-
-#### Field: Overflow Destination
-
-Name of a second WaterUse:Storage that would receive overflow. Overflow could occur if the maximum capacity is reached or if the design in flow rate is exceeded. If left blank, then the overflow is discarded and lost from the water system.
-
-#### Field: Type of Supply Controlled by Float Valve
-
-The storage tank can include the capability of modeling a float valve that will call for water to be added to the tank. This field is used to select the type of system used to respondto fill requests made by a float valve. The available options are    None   ,    Mains   ,    GroundwaterWell   , or    OtherTank.      The float valve settings are described in the next two fields.
-
-#### Field: Float Valve On Capacity
-
-The volumetric capacity [m3] of the water tank when a floating valve would turn on to allow filling the tank.
-
-#### Field: Float Valve Off Capacity
-
-The volumetric capacity [m3] of the water tank when a floating valve would turn off after having been filling the tank.
-
-#### Field: Backup Mains Capacity
-
-The volumetric capacity of the tank that indicates where a secondary float valve will maintain the volume by calling for mains water. Used if the well or other tank cannot keep up with the needs of the main float valve. If left blank or equal 0.0, then there is no mains water backup. If specified, then mains water will be drawn once the storage tank reaches this level and then the mains water will fill all the way to capacity specified in the previous field.
-
-#### Field: Other Tank Name
-
-This field contains the name of another WaterUse:Storage defined elsewhere in the input file. This field is only used if the Type of Controlled Supply field is set to    OtherTank    and the current tank is to be configured to be supplied by a second tank in response to a float valve.
-
-#### Field: Water Thermal Mode
-
-Controls the method of determining the temperature of the water in the storage tank. The only available option at the current time is ScheduledTemperature.
-
-#### Field: Water Temperature Schedule Name
-
-Reference to the schedule object specifying the temperature [C] of the water in the tank. This takes the place of a full thermal model of the tank.
-
-#### Field: Ambient Temperature Indicator
-
-Reserved for future use. The field can be Schedule, Zone, or Outdoors.
-
-#### Field: Ambient Temperature Schedule Name
-
-Reserved for future use. Schedule name for ambient temperature when previous field is Schedule.
-
-#### Field: Zone Name
-
-Reserved for future use. Name of zone where the tank is located.
-
-#### Field: Tank Surface Area
-
-Reserved for future zone thermal model.
-
-#### Field: Tank U Value
-
-Reserved for future zone thermal model.
-
-#### Field: Tank Outside Surface Material Name
-
-Reserved for future zone thermal model.
-
-
-
-IDF examples:
-
-```idf
-  WaterUse:Storage,
-   Tower 2 water tank, !- Name
-   Tower water make up Holding tank, !- Water Quality Subcategory
-   30.0 , !- Maximum Capacity {m3}
-   10.0 , !- Initial Volume   {m3}
-   20.0, !- Design In Flow Rate {m3}
-   20.0, !- Design Out Flow Rate {m3}
-   ,   !- Overflow Destination
-   Mains, !- Type of Supply Controlled by Float Valve
-   8.0 , !- Float Valve On Capacity {m3}
-   10.0,   !- Float Valve Off Capacity {m3}
-   3.0, !- Backup Mains Capacity {m3}
-   ,   !- Other Tank Name
-   ScheduledTemperature , !- Water Thermal Mode
-   Water Tank Temp Sched , !- Water Temperature Schedule Name
-   , !- Ambient Temperature Indicator
-   , !- Ambient Temperature Schedule Name
-   , !- Zone Name
-   , !- Tank Surface Area {m2}
-   , !- Tank U Value {W/m2-K}
-   ; !- Tank Outside Surface Material Name
-```
-
-
-
-### WaterUse:Storage Outputs
-
-The following output variables are available for reporting for each WaterUse:Storage object.
-
-* HVAC,Average,Water System Storage Tank Volume [m3]
-
-* HVAC,Average,Water System Storage Tank Net Volume Flow Rate [m3/s]
-
-* HVAC,Average,Water System Storage Tank Inlet Volume Flow Rate [m3/s]
-
-* HVAC,Average,Water System Storage Tank Outlet Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Water System Storage Tank Mains Water Volume [m3]
-
-* HVAC,Average,Water System Storage Tank Mains Water Volume Flow Rate [m3/s]
-
-* HVAC,Average,Water System Storage Tank Water Temperature [C]
-
-* HVAC,Average,Water System Storage Tank Overflow Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Water System Storage Tank Overflow Water Volume [m3]
-
-* HVAC,Average,Water System Storage Tank Overflow Temperature [C]
-
-#### Water System Storage Tank Volume [m3]
-
-This is the volume of water stored in the storage tank, in units of cubic meters (m<sup>3</sup>).
-
-#### Water System Storage Tank Net Volume Flow Rate [m3]
-
-This is the net rate of flows in and out of the storage tank, in units of cubic meters (m<sup>3</sup>).
-
-#### Water System Storage Tank Inlet Volume Flow Rate [m3/s]
-
-This is the rate of flows into the storage tank, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water System Storage Tank Outlet Volume Flow Rate [m3]
-
-This is the rate of flows out of the storage tank, in units of cubic meters (m<sup>3</sup>).
-
-#### Water System Storage Tank Mains Water Volume [m3]
-
-This is the volume of water drawn from the mains in order to fill the tank, in units of cubic meters per second (m<sup>3</sup>/s). This output is also added to a meter with Resource Type = MainsWater, End Use Key = WaterSystem, and Group Key = System. The water quality sub-category may be entered as any type (defined in WaterUse:Storage object input for Water Quality Subcategory) (ref. Output Meter).
-
-#### Water System Storage Tank Mains Water Volume Flow Rate [m3/s]
-
-This is the rate of water draw from the mains in order to fill the tank, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water System Storage Tank Water Temperature [C]
-
-This is the temperature of the water in the tank, in units of degrees Celsius (C).
-
-#### Water System Storage Tank Overflow Volume Flow Rate [m3/s]
-
-This is the rate of water flows that overflow the tank either because of limits on how fast the tank can fill or because the tank is full and cannot handle the water provided, in units of cubic meters per seconc (m<sup>3</sup>/s).
-
-#### Water System Storage Tank Overflow Water Volume [m3]
-
-This is the volume of water overflowing the tank because of limits on how fast the tank can fill or because the tank is full and cannot handle the water provided, in units of cubic meters (m<sup>3</sup>).
-
-#### Water System Storage Tank Overflow Temperature [C]
-
-This the temperature of overflow water leaving the tank.
-
-### WaterUse:RainCollector
-
-The WaterUse:RainCollector object is used for harvesting rainwater falling on building surfaces. The rainwater is sent to a WaterUse:Storage object. In order to use this object it is necessary to also include a Site:Precipitation object to describe the rates of rainfall.
-
-#### Field: Name
-
-The unique object name for reference by other objects.
-
-#### Field: Storage Tank Name
-
-A reference to a WaterUse:Storage object where the rainwater will be collected and stored for later use.
-
-#### Field: Loss Factor Mode
-
-The WaterUse:RainCollector model includes a loss factor that indicates the portion of incident rain that is not successfully collected. Two modes are available: Constant and Scheduled. Enter Constant in this field for the model to use a simple fixed loss factor defined in the next field. For versatility, the loss factor can follow a schedule by entering Scheduled in this field and then the name of a schedule in the second field below.
-
-#### Field: Collection Loss Factor
-
-Constant loss factor for how much of the incident rainwater is lost and not collected. The factor should be between 0 and 1.
-
-#### Field: Collection Loss Factor Schedule Name
-
-Name of a schedule that defines a variable collection loss factor if the mode is selected as Scheduled.
-
-#### Field: Maximum Collection Rate
-
-The maximum flow rate [m3/s] for rainwater collection. In a scenario where a heavy rain fall is being harvested, the actual reclamation rate might be limited by pipe size or the filtration system.
-
-#### Field: Collection Surface 1-10 Name
-
-A reference to the name of a surface object which will collect the rain. Typically the collection surfaces would correspond to roof surfaces on the building. The effective area for rainwater collection is the horizontal component (area \* cosine of the slope, etc.).   More detailed modeling of rainwater collection can be added later to account for factors such as wind speed and direction, etc.
-
-
-
-IDF examples:
-
-```idf
-WaterUse:RainCollector,
-   My Test Rain Collector ,!- Name
-   My Test Tank ,   !-   Storage Tank Name
-   CONSTANT,   !- Loss Factor Mode
-   0.9 ,   !- Collection Loss Factor
-   ,   !- Collection Loss Factor Schedule Name
-   1.0 ,   !- Maximum Collection Rate
-   SouthRoof ,   !- Collection Surface 1 Name
-   NorthRoof1,   !- Collection Surface 2 Name
-   NorthRoof3 ,   !- Collection Surface 3 Name
-   NorthRoof2 ;   !- Collection Surface 4 Name
-```
-
-
-### WaterUse:RainCollector Outputs
-
-* HVAC,Average,Water System Rainwater Collector Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Water System Rainwater Collector Volume [m3]
-
-#### Water System Rainwater Collector Volume Flow Rate [m3/s]
-
-This output variable provides the rate of water collected by the WaterUse:RainCollector, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water System Rainwater Collector Volume [m3]
-
-This output variable provides the volume of water collected by the WaterUse:RainCollector, in units of cubic meters per second (m<sup>3</sup>/s). This output is also added to a meter with Resource Type = OnSiteWater, End Use Key = RainWater, and Group Key = System (ref. Output Meter).
-
-### WaterUse:Well
-
-The WaterUse:Well object is for simulating on-site water supply from a well. Well water is pumped out of the ground and into a WaterUse:Storage. The operation of the ground water well is controlled by the associated WaterUse:Storage which is assumed to be operated as a vented cistern with no pressure tank. The current implementation is very simple and only requires two numeric inputs: the rated pump flow and power. A more elaborate well model may be added and many input fields are reserved for this future expansion.
-
-#### Field: Name
-
-Unique name of this well.
-
-#### Field: Storage Tank Name
-
-A reference to a WaterUse:Storage object where the rainwater will be collected and stored for later use.
-
-#### Field: Pump Depth
-
-Reserved for future use. Effective depth of well [m]
-
-#### Field: Pump Rated Flow Rate
-
-This is the nominal pump flow rate [m3/s]. This field is required.
-
-#### Field: Pump Rated Head
-
-Reserved for future use [Pa]. Pump head at rated conditions in Pascals.
-
-#### Field: Pump Rated Power Consumption
-
-This is the pump power at the nominal pump flow rate [W]. This field is required.
-
-#### Field: Pump Efficiency
-
-Reserved for future use.
-
-#### Field: Well Recovery Rate
-
-Reserved for future use. Rate at which ground water enters well during a sustained draw, e.g., 2 hour well test   [m3/s].
-
-#### Field: Nominal Well Storage Volume
-
-Reserved for future use. Capacity in well after long period of inactivity and the usual water table depth. [m3]
-
-#### Field: Water Table Depth Mode
-
-Reserved for future use. Two options available: Constant or Scheduled
-
-#### Field: Water Table Depth
-
-Reserved for future use. Depth of water table from WaterUse:Storage
-
-#### Field: Water Table Depth Schedule Name
-
-Reserved for future use.
-
-
-
-An example input object:
-
-```idf
-WaterUse:Well,
-   My Test Well,   !- Name
-   Tower 1 Water Tank,   !- Storage Tank Name
-   ,   !- Pump Depth
-   0.1,   !- Pump Rated Flow Rate {m3/s}
-   ,   !- Pump Rated Head {Pa}
-   120,   !- Pump Rated Power Consumption {W}
-   ,   !- Pump Efficiency
-   ,   !- Well Recovery Rate {m3/s}
-   ,   !- Nominal Well Storage Volume {m3}
-   ,   !- Water Table Depth Mode
-   ,   !- Water Table Depth
-   ;   !- Water Table Depth Schedule Name
-```
-
-
-### WaterUse:Well Outputs
-
-The following output variables are available for reporting for each WaterUse:Well object.
-
-* HVAC,Average,Water System Groundwater Well Requested Volume Flow Rate [m3/s]
-
-* HVAC,Average,Water System Groundwater Well Volume Flow Rate [m3/s]
-
-* HVAC,Sum,Water System Groundwater Well Volume [m3]
-
-* HVAC,Average,Water System Groundwater Well Pump Electric Power [W]
-
-* HVAC,Sum,Water System Groundwater Well Pump Electric Energy [J]
-
-#### Water System Groundwater Well Requested Volume Flow Rate [m3/s]
-
-This is the volume flow rate that the water system requested from the well, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water System Groundwater Well Volume Flow Rate [m3/s]
-
-This is the volume flow water of water actually obtained from the well, in units of cubic meters per second (m<sup>3</sup>/s).
-
-#### Water System Groundwater Well Volume [m3]
-
-This is the volume of water obtained from the well, in units of cubic meters (m<sup>3</sup>). This output is also added to a meter with Resource Type = OnSiteWater, End Use Key = WellWater, and Group Key = System (ref. Output Meter).
-
-#### Water System Groundwater Well Pump Electric Power [W]
-
-This is the electrical power of the pump used to extract water from the well, in units of watts (W).
-
-#### Water System Groundwater Well Pump Electric Energy [J]
-
-This is the electricity energy used by the pump to extract water from the well, in units of Joules (J). This output is also added to a meter with Resource Type = Electricity, End Use Key = WaterSystems, and Group Key = System (ref. Output Meter).
-
-Group - Operational Faults
---------------------------
-
-### Introduction to Operational Faults Modeling
-
-Most of the buildings, either new or old, have operational faults in the sensors, controllers, meters, equipment and systems. Being able to model and simulate these faults and their impact on energy performance of buildings is crucial to improve accuracy of building simulations and to support the retrofit of buildings.
-
-To date, the main practitioner use of EnergyPlus has been for new construction design. With the new high priority attached by USDOE to retrofit and improved operation of existing buildings, there is a need to extend the capabilities of EnergyPlus to model existing buildings, including faulty operation:
-
-- Retrofit analysis: starts with calibrated simulation; the ability to estimate the severity of common faults is expected to improve the accuracy and transparency of the calibrated model and hence the increase accuracy of the analysis of different retrofit measures.
-
-- Commissioning providers can use the fault models to demonstrate the saving to be expected from fixing faults found in retro-commissioning
-
-- Support for building operation by using the calibrated model, including unfixed faults, as a real-time reference model to detect, and verify the diagnosis of, newly occurring faults.
-
-The users in these cases are practitioners, not power users, so it is needed to implement the fault models using conventional EnergyPlus objects rather than the EMS, which, in any case, could only be used to model limited types of faults.
-
-### Operational Fault Objects
-
-EnergyPlus contains a number of objects to model operational faults of sensors, meters, equipment and systems. The current implementation allows the modeling of the following fault types: (1) sensor faults with air economizers, (2) thermostat/humidistat offset faults, and (3) heating and cooling coil fouling faults.
-
-The objects used by EnergyPlus to model the faults are as follows:
-
-- FaultModel:TemperatureSensorOffset:OutdoorAir
-
-- FaultModel:HumiditySensorOffset:OutdoorAir
-
-- FaultModel:EnthalpySensorOffset:OutdoorAir
-
-- FaultModel:TemperatureSensorOffset:ReturnAir
-
-- FaultModel:EnthalpySensorOffset:ReturnAir
-
-- FaultModel:Fouling:Coil
-
-- FaultModel:ThermostatOffset
-
-- FaultModel:HumidistatOffset
-
-### FaultModel:TemperatureSensorOffset:OutdoorAir
-
-This object defines the offset of an outdoor air dry-bulb temperature sensor that is used to determine applicability of an air economizer.
-
-#### Field: Name
-
-This is the user-defined name of the fault.
-
-#### Field: Availability Schedule Name
-
-This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to    1.0    when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Severity Schedule Name
-
-This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined temperature offset. This schedule should be set to a non-zero value when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Controller Object Type
-
-This field defines the controller object type that this fault is associated with. Choices are from a list of applicable controller types. Current implementation supports air economizer     the choice is Controller:OutdoorAir.
-
-#### Field: Controller Object Name
-
-This field defines the name of the controller object associated with the fault. It should be one of the objects with the defined types.
-
-#### Field: Temperature Sensor Offset
-
-This field defines the offset of the temperature sensor. A positive value means the sensor reads a temperature that is higher than the real value. A negative value means the sensor reads a temperature that is lower than the real value. A    0.0    value means no offset. Default is 0.0. The units are in degrees Celsius.
-
-### FaultModel:HumiditySensorOffset:OutdoorAir
-
-This object defines the offset of an outdoor air humidity sensor that is used to determine applicability of an air economizer.
-
-#### Field: Name
-
-This is the user-defined name of the fault.
-
-#### Field: Availability Schedule Name
-
-This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to    1.0    when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Severity Schedule Name
-
-This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined temperature offset. This schedule should be set to a non-zero value when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Controller Object Type
-
-This field defines the controller object type that this fault is associated with. Choices are from a list of applicable controller types. Current implementation supports air economizer     the choice is Controller:OutdoorAir.
-
-#### Field: Controller Object Name
-
-This field defines the name of the controller object associated with the fault. It should be one of the objects with the defined types.
-
-#### Field: Humidity Sensor Offset
-
-This field defines the offset of the humidity ratio sensor. A positive value means the sensor reads a humidity ratio that is higher than the real value. A negative value means the sensor reads a humidity ratio that is lower than the real value. A    0.0    value means no offset. Default is 0.0. The units are in kgWater/kgDryAir.
-
-### FaultModel:EnthalpySensorOffset:OutdoorAir
-
-This object defines the offset of an outdoor enthalpy sensor that is used to determine applicability of an air economizer.
-
-#### Field: Name
-
-This is the user-defined name of the fault.
-
-#### Field: Availability Schedule Name
-
-This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to    1.0    when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Severity Schedule Name
-
-This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined temperature offset. This schedule should be set to a non-zero value when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Controller Object Type
-
-This field defines the controller object type that this fault is associated with. Choices are from a list of applicable controller types. Current implementation supports air economizer     the choice is Controller:OutdoorAir.
-
-#### Field: Controller Object Name
-
-This field defines the name of the controller object associated with the fault. It should be one of the objects with the defined types.
-
-#### Field: Enthalpy Sensor Offset
-
-This field defines the offset of the enthalpy sensor. A positive value means the sensor reads an enthalpy that is higher than the real value. A negative value means the sensor reads an enthalpy that is lower than the real value. A    0.0    value means no offset. Default is 0.0. The units are in J/kg.
-
-### FaultModel:TemperatureSensorOffset:ReturnAir
-
-This object defines the offset of a return air dry-bulb temperature sensor that is used to determine applicability of an air economizer.
-
-#### Field: Name
-
-This is the user-defined name of the fault.
-
-#### Field: Availability Schedule Name
-
-This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to    1.0    when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Severity Schedule Name
-
-This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined temperature offset. This schedule should be set to a non-zero value when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Controller Object Type
-
-This field defines the controller object type that this fault is associated with. Choices are from a list of applicable controller types. Current implementation supports air economizer     the choice is Controller:OutdoorAir.
-
-#### Field: Controller Object Name
-
-This field defines the name of the controller object associated with the fault. It should be one of the objects with the defined types.
-
-#### Field: Temperature Sensor Offset
-
-This field defines the offset of the temperature sensor. A positive value means the sensor reads a temperature that is higher than the real value. A negative value means the sensor reads a temperature that is lower than the real value. A    0.0    value means no offset. Default is 0.0. The units are in degrees Celsius.
-
-### FaultModel:EnthalpySensorOffset:ReturnAir
-
-This object defines the offset of a return air enthalpy sensor that is used to determine applicability of an air economizer.
-
-#### Field: Name
-
-This is the user-defined name of the fault.
-
-#### Field: Availability Schedule Name
-
-This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to    1.0    when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Severity Schedule Name
-
-This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined temperature offset. This schedule should be set to a non-zero value when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Controller Object Type
-
-This field defines the controller object type that this fault is associated with. Choices are from a list of applicable controller types. Current implementation supports air economizer     the choice is Controller:OutdoorAir.
-
-#### Field: Controller Object Name
-
-This field defines the name of the controller object associated with the fault. It should be one of the objects with the defined types.
-
-#### Field: Enthalpy Sensor Offset
-
-This field defines the offset of the enthalpy sensor. A positive value means the sensor reads an enthalpy that is higher than the real value. A negative value means the sensor reads an enthalpy that is lower than the real value. A    0.0    value means no offset. Default is 0.0. The units are in J/kg.
-
-### FaultModel:Fouling:Coil
-
-This object defines the fouling for a simple water cooling coil or simple water heating coil.
-
-#### Field: Name
-
-This is the user-defined name of the fault.
-
-#### Field: Coil Name
-
-This field defines the name of the simple cooling coil or simple heating coil that has the fouling fault.
-
-#### Field: Availability Schedule Name
-
-This field provides the name of a schedule that will determine if this fault is applicable. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then user-defined fouling and a severity schedule will be applied. This schedule should be set to    1.0    when a fault is applicable and    0.0    when it is not. If this field is blank, the schedule has values of 1 for all time periods
-
-#### Field: Severity Schedule Name
-
-This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the user-defined fouling. If this field is blank, the schedule has values of 1 (no changes to fouling) for all time periods.
-
-#### Field: Fouling Input Method
-
-There are two methods to input the fouling, i.e. FouledUARated and FoulingFactor. User chooses the appropriate method to determine the coil fouling.
-
-#### Field: UAFouled
-
-This is the overall coil UA value including the coil fouling when the "FouledUARated" method is used. The unit is W/K.
-
-#### Field: Water Side Fouling Factor
-
-The following four fields specify the required inputs when the "FoulingFactor" method is used. This field defines the fouling factor for the water side. The units are in m<sup>2</sup>-K/W.
-
-#### Field: Air Side Fouling Factor
-
-This field defines the fouling factor for the air side. The units are in m<sup>2</sup>-K/W.
-
-#### Field: Outside Coil Surface Area
-
-This field defines outside surface area of the cooling or heating coil. The units are in m<sup>2</sup>.
-
-#### Field: Inside to Outside Coil Surface Area Ratio
-
-This field specifies the inside to outside surface area ratio of the cooling or heating coil.
-
-
-
-IDF examples:
-
-```idf
-   ! example faults for an air economizer
-
-Schedule:Compact,
-       OATSeveritySch,                   !- Name
-       On/Off,                                   !- Schedule Type Limits Name
-       Through: 6/30,                     !- Field 1
-       For: AllDays,                       !- Field 2
-       Until: 24:00,0,                   !- Field 3
-       Through: 12/31,                   !- Field 4
-       For: AllDays,                       !- Field 5
-       Until: 24:00,1;                   !- Field 6
-
-FaultModel:TemperatureSensorOffset:OutdoorAir,
-     OATFault,                                 !- Name
-     ALWAYS_ON,                               !- Availability Schedule Name
-     OATSeveritySch,                     !- Severity Schedule Name
-     Controller:OutdoorAir,       !- Controller Object Type
-     VAV_1_OA_Controller,           !- Controller Object Name
-     -2.0;                                           !- Temperature Sensor Offset, deg C
-
-FaultModel:TemperatureSensorOffset:ReturnAir,
-     RATFault,                                 !- Name
-     ,                                                 !- Availability Schedule Name
-     ,                                                 !- Severity Schedule Name
-     Controller:OutdoorAir,       !- Controller Object Type
-     VAV_2_OA_Controller,           !- Controller Object Name
-     -2.0;                                         !- Temperature Sensor Offset, deg C
-
-FaultModel:EnthalpySensorOffset:ReturnAir,
-     RAHFault,                                 !- Name
-     ,                                                 !- Availability Schedule Name
-     ,                                                 !- Severity Schedule Name
-     Controller:OutdoorAir,       !- Controller Object Type
-     VAV_2_OA_Controller,           !- Controller Object Name
-     -2000;                                       !- Enthalpy Sensor Offset, J/Kg
-
-! example faults for a fouling coil
-
-FaultModel:Fouling:Coil,
-     CoolingCoilFault,               !- Name
-     VAV_2_CoolC,                         !- Heating or Cooling Coil Name
-     ALWAYS_ON,                             !- Availability Schedule Name
-     ,                                               !- Severity Schedule Name
-     FouledUARated,                     !- Fouling Input Method
-     3000,                                       !- UAFouled, W/K
-     ,                                               !- Water Side Fouling Factor, m2-K/W
-     ,                                               !- Air Side Fouling Factor, m2-K/W
-     ,                                               !- Outside Coil Surface Area, m2
-     ;                                               !- Inside to Outside Coil Surface Area Ratio
-```
-
-### FaultModel:ThermostatOffset
-
-This object defines the offset fault of a thermostat that leads to inappropriate operations of the HVAC system.
-
-#### Field: Name
-
-This is the user-defined name of the fault. 
-
-#### Field: Thermostat Name
-
-This field defines the name of the thermostat object associated with the fault. It should be the name of a ZoneControl:Thermostat object.
-
-#### Field: Availability Schedule Name 
-
-This field provides the name of a schedule that will determine whether this fault is applicable or not. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to "1.0" when a fault is applicable and "0.0" when it is not. If this field is blank, the schedule has values of 1.0 for all time periods.
-
-#### Field: Severity Schedule Name 
-
-This field provides the name of a schedule that represents severity of a fault. This is used as a multiplier to the reference thermostat offset value. This schedule should be set to a non-zero value when a fault is applicable and "0.0" when it is not. If this field is blank, the schedule has values of 1.0 for all time periods.
-
-#### Field: Reference Thermostat Offset
-
-This field defines the reference offset value of the thermostat. A positive value means the zone air temperature reading is higher than the actual value. A negative value means the reading is lower than the actual value. A "0.0" value means no offset. Default is 2.0. The units are in degrees Celsius. 
-
-
-### FaultModel:HumidistatOffset
-
-This object defines the offset fault of a humidistat that leads to inappropriate operations of the HVAC system.
-
-#### Field: Name
-
-This is the user-defined name of the fault. 
-
-#### Field: Humidistat Name
-
-This field defines the name of the humidistat object associated with the fault. It should be the name of a ZoneControl:Humidistat object.
-
-#### Field: Humidistat Offset Type
-
-This choice field determines the humidistat offset fault type. Two fault types are available: (1) Type ThermostatOffsetIndependent: humidistat offset is not related with thermostat offset. For this type, user needs to specify the Reference Humidistat Offset, Availability Schedule, and Severity Schedule (2) Type ThermostatOffsetDependent: humidistat offset is caused by thermostat offset fault. For this type, user only needs to specify the Related Thermostat Offset Fault Name. 
-
-#### Field: Availability Schedule Name
-
-This field provides the name of a schedule that will determine if this fault is applicable. This field is applicable for the Type ThermostatOffsetIndependent. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined sensor offset and a severity schedule will be applied. This schedule should be set to "1.0" when a fault is applicable and "0.0" when it is not. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Severity Schedule Name
-
-This field provides the name of a schedule that represents severity of a fault. This field is applicable for the Type ThermostatOffsetIndependent. This is used as a multiplier to the reference humidistat offset value. This schedule should be set to a non-zero value when a fault is applicable and "0.0" when it is not. If this field is blank, the schedule has values of 1.0 for all time periods. 
-
-#### Field: Reference Humidistat Offset
-
-This field defines the reference offset value of the humidistat. This field is required for the Type ThermostatOffsetIndependent. A positive value means the zone air temperature reading is higher than the actual value. A negative value means the reading is lower than the actual value. A "0.0" value means no offset. Default is 5.0. The units are in percentage. 
-
-#### Field: Related Thermostat Offset Fault Name
-
-This field provides the name of a Thermostat Offset Fault object that causes the humidistat offset fault. It should be the name of a FaultModel:ThermostatOffset object. This field is required for the Type ThermostatOffsetDependent. This is used as a multiplier to the reference humidistat offset value. This schedule should be set to a non-zero value when a fault is applicable and "0.0" when it is not. If this field is blank, the schedule has values of 1.0 for all time periods.
-
-### An example of IDF codes for the thermostat/humidistat offset fault models:
-
-```idf
-FaultModel:ThermostatOffset,
-   Ther_Offset_Zone1,   !- Name
-   Zone 1 Thermostat,   !- Thermostat Name
-   AlwaysOn,            !- Availability Schedule Name
-   AlwaysOne,           !- Severity Schedule Name
-   2.0;                 !- Reference Thermostat Offset
-
-FaultModel:HumidistatOffset, 
-   Humi_Offset_Zone1,   !- Name
-   Zone 1 Humidistat,   !- Humidistat Name
-   ThermostatOffsetDependent, !- Humidistat Offset Type
-   ,                    !- Availability Schedule Name
-   ,                    !- Severity Schedule Name
-   ,                    !- Reference Humidistat Offset
-   Ther_Offset_Zone1;   !- Related Thermostat Offset Fault Name
-
-FaultModel:HumidistatOffset, 
-   Humi_Offset_Zone2,   !- Name
-   Zone 2 Humidistat,   !- Humidistat Name
-   ThermostatOffsetIndependent, !- Humidistat Offset Type
-   AlwaysOn,            !- Availability Schedule Name
-   AlwaysOne,           !- Severity Schedule Name
-   10,                  !- Reference Humidistat Offset
-   ;                    !- Related Thermostat Offset Fault Name
-```
-
-### FaultModel:Fouling:AirFilter
-
-This object defines the fault of fouling air filter that leads to inappropriate operations of the corresponding fan. 
-
-#### Field: Name
-
-This is the user-defined name of the fault. 
-
-#### Field: Fan Name
-
-This field defines the name of a fan object associated with the fault. It should be the name of a fan object (Fan:ConstantVolume, Fan:OnOff, or Fan:VariableVolume). 
-
-#### Field: Fan Object Type
-
-This choice field defines the type of fan. The valid choices are Fan:OnOff, Fan:ConstantVolume, and Fan:VariableVolume. Both cycling and continuous fan operating modes are allowed for Fan:OnOff. Only the continuous fan operating mode is allowed for Fan:ConstantVolume. The variable airflow rate is allowed for Fan:VariableVolume. 
-
-#### Field: Availability Schedule Name
-
-This field provides the name of a schedule that will determine if this fault is applicable. This field is applicable for the Type ThermostatOffsetIndependent. When a fault is not applicable it is not modeled in the simulations. When it is applicable, then a user-defined Pressure Fraction Schedule will be applied. This schedule should be set to "1.0" when a fault is applicable and "0.0" when it is not. If this field is blank, the schedule has values of 1.0 for all time periods.
-
-#### Field: Pressure Fraction Schedule Name 
-
-This field provides the name of a schedule that describes the pressure rise variations of the fan associated with the fouling air filter. This is used as a multiplier to the fan design pressure rise. Because the fan pressure rise in the faulty case is higher than that in the design case, this schedule should be set to a value that is greater than 1.0 when a fault is applicable. If this field is blank, the schedule has values of 1.0 for all time periods.
-
-#### Field: Fan Curve Name
-
-This field provides the name of a fan curve for the fan associated with the fault. The curve describes the relationship between the fan pressure rise and air flow rate. This is used to estimate the variations of the fan air flow rate in the faulty cases, given the Pressure Rise Variation Schedule. For variable speed fans, the curve should be the one corresponding to the maximum fan speed. The fan curve should cover the design operational point specified in the corresponding fan object. It is also required that the faulty fan operatinal state point falls within the fan selection range that is monotonically decreasing.
-
-### An example of IDF codes for the fouling air filter fault models:
-
-```idf
-FaultModel:Fouling:AirFilter,
-   DF_VAV_1_Fan,             !- Name
-   VAV_1_Fan,                !- Fan Name
-   Fan:VariableVolume,       !- Fan Object Type
-   ALWAYS_ON,                !- Availability Schedule Name
-   Pressure_Inc_Sch,         !- Pressure Fraction Schedule Name
-   VAV_1_Fan_Curve;          !- Fan Curve Name
-   
-Schedule:Compact,
-    Pressure_Inc_Sch,        !- Name
-    Any Number,              !- Schedule Type Limits Name
-    Through: 12/31,          !- Field 1
-    For: AllDays,            !- Field 2
-    Until: 24:00,1.1;        !- Field 3
-
-Curve:Cubic,		
-    VAV_1_Fan_Curve,         ! name		
-    1263.1,                  ! Coefficient1 Constant		
-    33.773,                  ! Coefficient2 x		
-   -5.6906,                  ! Coefficient3 x**2		
-   -0.2023,                  ! Coefficient4 x**3		
-    4.0,                     ! Minimum Value of x		
-    15.0;                    ! Maximum Value of x		
-
-Fan:VariableVolume,
-    VAV_1_Fan,               !- Name
-    HVACOperationSchd,       !- Availability Schedule Name
-    0.5915,                  !- Fan Total Efficiency
-    1109.648,                !- Pressure Rise {Pa}
-    7.5202,                  !- Maximum Flow Rate {m3/s}
-    FixedFlowRate,           !- Fan Power Minimum Flow Rate Input Method
-    ,                        !- Fan Power Minimum Flow Fraction
-    0.0000,                  !- Fan Power Minimum Air Flow Rate {m3/s}
-    0.91,                    !- Motor Efficiency
-    1.0,                     !- Motor In Airstream Fraction
-    0.0407598940,            !- Fan Power Coefficient 1
-    0.08804497,              !- Fan Power Coefficient 2
-    -0.072926120,            !- Fan Power Coefficient 3
-    0.9437398230,            !- Fan Power Coefficient 4
-    0,                       !- Fan Power Coefficient 5
-    VAV_1_HeatC-VAV_1_FanNode,  !- Air Inlet Node Name
-    VAV_1 Supply Equipment Outlet Node,  !- Air Outlet Node Name
-    Fan Energy;              !- End-Use Subcategory	
-```
-
-Group - Performance Curves
---------------------------
-
-This group of objects primarily consists of polynomial curves that are used to characterize the performance of HVAC equipment. Several other non-polynomial curves are also included to characterize the performance of pumps and fans. All of the curves are input, stored, and evaluated entirely within the CurveManager module. The curves are usually derived from fits or regressions to data covering a limited range. Results for independent variable values outside this range are likely to be invalid, so curve input always contains a range of validity (maximum and minimum permitted values) for each independent variable and can optionally have limits on the curve ouput. No error or warning message is issued if an independent variable is outside the range. Instead, the curve manager uses the minimum value if an independent variable is less than the minimum, and the maximum if a variable exceeds the maximum. Similarly, no error or warning message is issued if the curve output is outside the range of the optional minimum and maximum curve output limits. Instead, the curve manager uses the minimum and maximum curve limits to cap the output of the performance curve.
-
-Curve names must be unique across all curve types.
-
-### Curve:Linear
-
-Input for the linear curve consists of a curve name, the two coefficients, and the maximum and minimum valid independent variable values. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the linear curve is:
-
-<div>\[y = {C_1} + {C_2}*x\]</div>
-
-#### Field: Name
-
-A user assigned unique name for an instance of a linear curve. When a curve is used, it is referenced by this name.
-
-#### Field: Coefficient1 Constant
-
-The constant coefficient (C<sub>1</sub>) in the equation.
-
-#### Field: Coefficient2 x
-
-The linear coefficient (C<sub>2</sub>) in the equation.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for X
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-Following is an example input:
-
-```idf
-Curve:Linear,
-Curve-Linear, ! name
--1, ! Coefficient1 Constant
-2, ! Coefficient2 x
-0.0, ! min curve output
-1.0; ! max curve output
-```
-
-The following is another example, as might be applied in the Fan:ComponentModel to characterize duct static pressure reset (using a constant duct static pressure set point of 248.84 Pa in this case):
-
-```idf
-Curve:Linear,
-DiagnosticSPR, ! Curve Name f = C1 + C2\*x
-248.84, ! Coefficient1 Constant [Pa]
-0., ! Coefficent 2 Press/Flow [Pa-s/m3]
-0., ! Minimum Value of x (Qfan) [m3/s]
-100., ! Maximum Value of x (Qfan) [m3/s]
-62.5, ! Minimum Curve Output [Pa]
-248.84; ! Maximum Curve Output [Pa]
-```
-
-### Curve:QuadLinear
-
-Input consists of the curve name, the five coefficients, and maximum and minimum values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is represented by this curve:
-
-#### y = C1 + C2 \* w + C3 \* x + C4 \* y + C5 \* z
-
-#### Field: Name
-
-A user assigned unique name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
-
-#### Field: Coefficient1 Constant
-
-The constant coefficient (C1) in the equation.
-
-#### Field: Coefficient2 w
-
-The coefficient (C2) in the equation.
-
-#### Field: Coefficient3 x
-
-The coefficient (C3) in the equation.
-
-#### Field: Coefficient4 y
-
-The coefficient (C4) in the equation.
-
-#### Field: Coefficient5 z
-
-The coefficient (C5) in the equation.
-
-#### Field: Minimum Value of w
-
-The minimum allowable value of w. Values of w less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of w
-
-The maximum allowable value of w. Values of z greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of z greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of y
-
-The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of y
-
-The maximum allowable value of y. Values of z greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of z
-
-The minimum allowable value of z. Values of z less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of z
-
-The maximum allowable value of z. Values of z greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for w
-
-This field is used to indicate the kind of units that may be associated with the w values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of w and Maximum Value of w. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select Dimensionless which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-- VolumetricFlowPerPower
-
-#### Field: Input Unit Type for x
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of x and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select Dimensionless which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-- VolumetricFlowPerPower
-
-#### Field: Input Unit Type for y
-
-This field is used to indicate the kind of units that may be associated with the y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of y and Maximum Value of y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select Dimensionless which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-- VolumetricFlowPerPower
-
-#### Field: Input Unit Type for z
-
-This field is used to indicate the kind of units that may be associated with the z values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of z and Maximum Value of z. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select Dimensionless which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-- VolumetricFlowPerPower
-
-Below are an example inputs for QuadLinear Curves.
-
-```idf
-CURVE:QUADLINEAR,
-MinDsnWBCurveName, ! Curve Name
--3.3333,           ! CoefficientC1
-0.0,               ! CoefficientC2
-38.9,              ! CoefficientC3
-0.,                ! CoefficientC4
-0.,                ! CoefficientC5
--30.,              ! Minimum Value of w
-40.,               ! Maximum Value of w
-0.,                ! Minimum Value of x
-1.,                ! Maximum Value of x
-10.,               ! Minimum Value of y
-8.,                ! Maximum Value of y
-1. E-8,            ! Minimum Value of z
-8. E-8,            ! Maximum Value of z
-0.,                ! Minimum Curve Output
-38.;               ! Maximum Curve Output
-
-Curve:QuadLinear,
-MinActWBCurveName, ! Curve Name
--8.3333,           ! CoefficientC1
-2.0,               ! CoefficientC2
-5.5556.,           ! CoefficientC3
--1.0,              ! CoefficientC4
-0.,                ! CoefficientC5
-0.,                ! Minimum Value of w
-38.,               ! Maximum Value of w
-0.,                ! Minimum Value of x
-1.,                ! Maximum Value of x
-10.,               ! Minimum Value of y
-38.,               ! Maximum Value of y
-1. E-8,            ! Minimum Value of z
-8. E-8,            ! Maximum Value of z
-0.,                ! Minimum Curve Output
-43.;               ! Maximum Curve Output
-
-Curve:QuadLinear,
-OptCondEntCurveName, ! Curve Name
-12.2711,             ! CoefficientC1
-0.80,                ! CoefficientC2
-6.6667,              ! CoefficientC3
--0.266,              ! CoefficientC4
--6193484.,           ! CoefficientC5
-0.,                  ! Minimum Value of w
-38.,                 ! Maximum Value of w
-0.,                  ! Minimum Value of x
-1.,                  ! Maximum Value of x
-10.,                 ! Minimum Value of y
-38.,                 ! Maximum Value of y
-1. E-8,              ! Minimum Value of z
-8. E-8,              ! Maximum Value of z
-0.,                  ! Minimum Curve Output
-32.;                 ! Maximum Curve Output
-```
-
-### Curve:Quadratic
-
-Input for a quadratic curve consists of the curve name, the three coefficients, and the maximum and minimum valid independent variable values. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the quadratic curve is:
-
-<div>\[y = {C_1} + {C_2}*x + {C_3}*{x^2}\]</div>
-
-#### Field: Name
-
-A user assigned unique name for an instance of a quadratic curve. When a curve is used, it is referenced by this name.
-
-#### Field: Coefficient1 Constant
-
-The constant coefficient (C<sub>1</sub>) in the equation.
-
-#### Field: Coefficient2 x
-
-The linear coefficient (C<sub>2</sub>) in the equation.
-
-#### Field: Coefficient3 x\*\*2
-
-The quadratic coefficient (C<sub>3</sub>) in the equation.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for X
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-Following is an example input.
-
-```idf
-Curve:Quadratic,
-WindACCBFFFF, ! name
--2.277,       ! Coefficient1 Constant
-5.2114,       ! Coefficient2 x
--1.9344,      ! Coefficient3 x\*\*2
-0.0,          ! Minimum Value of x
-1.0;          ! Maximum Value of x
-```
-
-### Curve:Cubic
-
-Input for a cubic curve consists of the curve name, the 4 coefficients, and the maximum and minimum valid independent variable values. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the cubic curve is:
-
-<div>\[y = {C_1} + {C_2}*x + {C_3}*{x^2} + {C_4}*{x^3}\]</div>
-
-#### Field: Name
-
-A user assigned unique name for an instance of a cubic curve. When a curve is used, it is referenced by this name.
-
-#### Field: Coefficient1 Constant
-
-The constant coefficient (C<sub>1</sub>) in the equation.
-
-#### Field: Coefficient2 x
-
-The linear coefficient (C<sub>2</sub>) in the equation.
-
-#### Field: Coefficient3 x\*\*2
-
-The quadratic coefficient (C<sub>3</sub>) in the equation.
-
-#### Field: Coefficient4 x\*\*3
-
-The cubic coefficient (C<sub>4</sub>) in the equation.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for X
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-Following is an input example.
-
-```idf
-Curve:Cubic,
-WindACEIRFPLF, ! name
-.00000273404,  ! Coefficient1 Constant
-1.05259,       ! Coefficient2 x
--.0552087,     ! Coefficient3 x**2
-.00262236,     ! Coefficient4
-0.0,           ! min
-1.1;           ! max
-```
-
-### Curve:Quartic
-
-Input for a Quartic (fourth order polynomial) curve consists of the curve name, the five coefficients, and the maximum and minimum valid independent variable values. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the quartic curve is:
-
-<div>\[y = {C_1} + {C_2}x + {C_3}{x^2} + {C_4}{x^3} + {C_5}{x^4}\]</div>
-
-#### Field: Name
-
-A user assigned unique name for an instance of a Quartic curve. When a curve is used, it is referenced by this name.
-
-#### Field: Coefficient1 Constant
-
-The constant coefficient (C<sub>1</sub>) in the equation.
-
-#### Field: Coefficient2 x
-
-The linear coefficient (C<sub>2</sub>) in the equation.
-
-#### Field: Coefficient3 x\*\*2
-
-The quadratic coefficient (C<sub>3</sub>) in the equation.
-
-#### Field: Coefficient4 x\*\*3
-
-The cubic coefficient (C<sub>4</sub>) in the equation.
-
-#### Field: Coefficient5 x\*\*4
-
-The fourth-order coefficient (C<sub>5</sub>) in the equation.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for X
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-Following is an input example.
-
-```idf
-   Curve:Quartic,
-       BGSeries60,                                 !- y = -611.41x4 + 192.68x3 - 88.843x2 + 4.7634x + 5.5656
-       5.5656,                                         !- Constant
-       4.7634,                                         !- 1st coefficient
-       -88.843,                                       !- 2nd coefficient
-       192.68,                                         !- 3rd coefficient
-       -611.41,                                       !- 4th coefficient
-       0.0,                                               !- Min Phi Value
-       0.2412;                                         !- Max Phi Value
-```
-
-The following is another example, as might be applied in the Fan:ComponentModel to characterize belt maximum efficiency (using a medium efficiency belt in this case):
-
-```idf
-   Curve:Quartic,
-       BeltMaxEffMedium,                               ! Curve Name
-       -0.09504,                                               ! CoefficientC1
-       0.03415,                                                 ! CoefficientC2
-       -0.008897,                                             ! CoefficientC3
-       0.001159,                                               ! CoefficientC4
-       -0.00006132,                                         ! CoefficientC5
-       -1.2,                                                       ! Minimum Value of x
-       6.2,                                                         ! Maximum Value of x
-       -4.6,                                                       ! Minimum Curve Output
-       0.;                                                           ! Maximum Curve Output
-```
-
-
-### Curve:Exponent
-
-Input for a exponent curve consists of the curve name, the 3 coefficients, and the maximum and minimum valid independent variable values. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the exponent curve is:
-
-<div>\[y = C1 + C2*{x^{C3}}\]</div>
-
-#### Field: Name
-
-A user assigned unique name for an instance of an exponent curve. When a curve is used, it is referenced by this name.
-
-#### Field: Coefficient1 Constant
-
-The constant coefficient (C<sub>1</sub>) in the equation.
-
-#### Field: Coefficient2 Constant
-
-The linear coefficient (C<sub>2</sub>) in the equation.
-
-#### Field: Coefficient3 Constant
-
-The exponent coefficient (C<sub>3</sub>) in the equation.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for X
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-Following is an input example.
-
-```idf
-   Curve:Exponent,
-!     Curve = C1 + C2\*x\*\*C3, x = fan speed ratio
-       FanPowerExponentCurve, !- Name
-       0.0,                                     !- Coefficient1 Constant
-       1.0,                                     !- Coefficient2 Constant
-       3.0,                                     !- Coefficient3 Constant
-       0.0,                                     !- Minimum Value of x
-       1.5,                                     !- Maximum Value of x
-       0.1,                                     !- Minimum Curve Output
-       1.5;                                     !- Maximum Curve Output
-```
-
-### Curve:Bicubic
-
-This curve type is a function of two independent variables. Input consists of the curve name, the ten coefficients, and the minimum and maximum values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the bicubic curve is:
-
-<div>\[z = {C_1} + {C_2}*x + {C_3}*{x^2} + {C_4}*y + {C_5}*{y^2} + {C_6}*xy + {C_7}*{x^3} + {C_8}*{y^3} + {C_9}*{x^2}y + {C_{10}}*x{y^2}\]</div>
-
-#### Field: Name
-
-A user assigned unique name for an instance of a bicubic curve. When a curve is used by another object, it is referenced by this name.
-
-#### Field: Coefficient1 Constant
-
-The constant coefficient (C<sub>1</sub>) in the equation.
-
-#### Field: Coefficient2 x
-
-The coefficient C<sub>2</sub> in the equation.
-
-#### Field: Coefficient3 x\*\*2
-
-The coefficient C<sub>3</sub> in the equation.
-
-#### Field: Coefficient4 y
-
-The coefficient C<sub>4</sub> in the equation.
-
-#### Field: Coefficient5 y\*\*2
-
-The coefficient C<sub>5</sub> in the equation.
-
-#### Field: Coefficient6 x\*y
-
-The coefficient C<sub>6</sub> in the equation.
-
-#### Field: Coefficient7 x\*\*3
-
-The coefficient C<sub>7</sub> in the equation.
-
-#### Field: Coefficient8 y\*\*3
-
-The coefficient C<sub>8</sub> in the equation.
-
-#### Field: Coefficient9 x\*\*2\*y
-
-The coefficient C<sub>9</sub> in the equation.
-
-#### Field: Coefficient10 x\*y\*\*2
-
-The coefficient C<sub>10</sub> in the equation.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than this minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of x greater than this maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of y
-
-The minimum allowable value of y. Values of y less than this minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of y
-
-The maximum allowable value of y. Values of y greater than this maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for X
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-#### Field: Input Unit Type for Y
-
-This field is used to indicate the kind of units that may be associated with the y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Y and Maximum Value of Y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-Below is an example input.
-
-```idf
-   Curve:Bicubic,
-      Main Chiller EIRFPLR,             !- Name
-       7.086284E-02,                             !- Coefficient1 Constant
-       2.787561E-03,                             !- Coefficient2 x
-     -8.917038E-06,                             !- Coefficient3 x\*\*2
-       2.309734E-01,                             !- Coefficient4 y
-       1.250442E+00,                             !- Coefficient5 y\*\*2
-     -2.161029E-03,                             !- Coefficient6 x\*y
-       0.000000E+00,                             !- Coefficient7 x\*\*3
-     -5.630094E-01,                             !- Coefficient8 y\*\*3
-       0.000000E+00,                             !- Coefficient9 x\*\*2\*y
-       0.000000E+00,                             !- Coefficient10 x\*y\*\*2
-       20.33,                                           !- Minimum Value of x
-       35.00,                                           !- Maximum Value of x
-       0.25,                                             !- Minimum Value of y
-       1.01;                                             !- Maximum Value of y
-```
-
-
-### Curve:Biquadratic
-
-This curve is a function of two independent variables. Input consists of the curve name, the six coefficients, and min and max values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the bicubic curve is:
-
-<div>\[z = {C_1} + {C_2}*x + {C_3}*{x^2} + {C_4}*y + {C_5}*{y^2} + {C_6}*xy\]</div>
-
-#### Field: Name
-
-A user assigned unique name for an instance of a biquadratic curve. When a curve is used, it is referenced by this name.
-
-#### Field: Coefficient1 Constant
-
-The constant coefficient (C<sub>1</sub>) in the equation.
-
-#### Field: Coefficient2 x
-
-The coefficient C<sub>2</sub> in the equation.
-
-#### Field: Coefficient3 x\*\*2
-
-The coefficient C<sub>3</sub> in the equation.
-
-#### Field: Coefficient4 y
-
-The coefficient C<sub>4</sub> in the equation.
-
-#### Field: Coefficient5 y\*\*2
-
-The coefficient C<sub>5</sub> in the equation.
-
-#### Field: Coefficient6 x\*y
-
-The coefficient C<sub>6</sub> in the equation.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of y
-
-The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of y
-
-The maximum allowable value of y. Values of y greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for X
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-#### Field: Input Unit Type for Y
-
-This field is used to indicate the kind of units that may be associated with the y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Y and Maximum Value of Y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-Below is an example input.
-
-```idf
-Curve:Biquadratic,
-WindACCoolCapFT, ! name
-0.942587793,     ! Coefficient1 Constant
-0.009543347,     ! Coefficient2 x
-0.000683770,     ! Coefficient3 x\*\*2
--0.011042676,    ! Coefficient4 y
-0.000005249,     ! Coefficient5 y\*\*2
--0.000009720,    ! Coefficient6 x\*y
-15., 22.,        ! min and max of first independent variable
-29., 47.;        ! min and max of second independent variable
-```
-
-### Curve:CubicLinear
-
-This curve is a function of two independent variables. Input consists of the curve name, the six coefficients, and min and max values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the cubic linear curve:
-
-<div>\[y = \left( {{C_1} + {C_2}*x + {C_3}*{x^2} + {C_4}*{x^3}} \right) + \left( {{C_5} + {C_6}*x} \right)*y\]</div>
-
-#### Field: Name
-A user assigned unique name for an instance of a quadratic-linear curve. When a curve is used, it is referenced by this name.
-
-#### Field: Coefficient1 Constant
-The constant coefficient (<span>\(C_1\)</span>) in the equation.
-
-#### Field: Coefficient2 x
-The coefficient <span>\(C_2</span> in the equation.
-
-#### Field: Coefficient3 x**2
-The coefficient <span>\(C_3</span> in the equation.
-
-#### Field: Coefficient4 x**3
-The coefficient <span>\(C_4</span> in the equation.
-
-#### Field: Coefficient5 y
-The coefficient <span>\(C_5</span> in the equation.
-
-#### Field: Coefficient6 x*y
-The coefficient <span>\(C_6</span> in the equation.
-
-#### Field: Minimum Value of x
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of y
-The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of y
-The maximum allowable value of y. Values of y greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum. 
-
-#### Field: Maximum Curve Output
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for X
-This field is used to indicate the kind of units that may be associated with the x values. The only option at this time is **Dimensionless**.
-
-#### Field: Input Unit Type for Y
-This field is used to indicate the kind of units that may be associated with the x values. The only option at this time is **Dimensionless**.
-
-#### Field: Output Unit Type
-This field is used to indicate the kind of units that may be associated with the output values. The only option at this time is **Dimensionless**.
-
-An example input for the CubicLinear equation form is shown below. 
-
-```idf
-Curve:CubicLinear, 
-InsideMeltIceDischarging, !- Name
-0.108734675,              !- Coefficient1 Constant
--0.989874286,             !- Coefficient2 x
-0.696303562,              !- Coefficient3 x**2
--0.134945307,             !- Coefficient4 x**3
-1.724007415,              !- Coefficient5 y
--1.094020457,             !- Coefficient6 y*x
-0.25,                     !- Minimum Value of x
-1,                        !- Maximum Value of x
-0.69,                     !- Minimum Value of y
-1.26,                     !- Maximum Value of y
-0.0926,                   !- Minimum Curve Output
-0.4938,                   !- Maximum Curve Output
-Dimensionless,            !- Input Unit Type for X
-Dimensionless,            !- Input Unit Type for Y
-Dimensionless,            !- Output Unit Type 
-```
-
-### Curve:ChillerPartLoadCustom
-
-A custom chiller part-load performance curve is a function of three independent variables, i.e., x, y, and z. Input consists of the curve name, the twelve coefficients, and min and max values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve. 
-
-The equation represented by the custom curve is:
-
-<div>\[ C_1 + C_2 \cdot x + C_3 \cdot x^2 + C_4 \cdot y + C_5 \cdot y^2 + C_6 \cdot x \cdot y + C_7 \cdot x^3 + C_8 \cdot y^3 + C_9 \cdot x^2 \cdot y + C_{10} \cdot x \cdot y^2 + C_{11} \cdot x^2 \cdot y^2 + C_{12} \cdot z \cdot y^3 \] </div>
-
-where, 
-
-* x represents the normalized fractional lift (the delta of temperature across the leaving condenser water temperature and leaving evaporator water temperature of a chiller).
-* y represents the normalized deviation of leaving chilled water temperature from the reference condition.
-* z represents the part load ratio.
-
-
-#### Field: Name
-
-A user assigned unique name for an instance of a biquadratic curve. When a curve is used, it is referenced by this name.
-
-#### Field: Coefficient1 
-
-The constant coefficient (C1) in the equation.
-
-#### Field: Coefficient2 
-
-The coefficient C2 in the equation.
-
-#### Field: Coefficient3
-
-The coefficient C3 in the equation.
-
-#### Field: Coefficient4
-
-The coefficient C4 in the equation.
-
-#### Field: Coefficient5
-
-The coefficient C5 in the equation.
-
-#### Field: Coefficient6
-
-The coefficient C6 in the equation.
-
-#### Field: Coefficient7 
-
-The constant coefficient (C7) in the equation.
-
-#### Field: Coefficient8
-
-The coefficient C8 in the equation.
-
-#### Field: Coefficient9
-
-The coefficient C9 in the equation.
-
-#### Field: Coefficient10
-
-The coefficient C10 in the equation.
-
-#### Field: Coefficient11
-
-The coefficient C11 in the equation.
-
-#### Field: Coefficient12
-
-The coefficient C12 in the equation.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of y
-
-The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of y
-
-The maximum allowable value of y. Values of y greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of z
-
-The minimum allowable value of z. Values of y less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of z
-
-The maximum allowable value of z. Values of y greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for x
-
-This field is used to indicate the kind of units that may be associated with the x values. Select Dimensionless.
-
-#### Field: Input Unit Type for y
-
-This field is used to indicate the kind of units that may be associated with the y values. Select Dimensionless.
-
-#### Field: Input Unit Type for z
-
-This field is used to indicate the kind of units that may be associated with the y values. Select Dimensionless.
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. Select Dimensionless.
-
-Below is an example input: 
-
-```idf
-Curve:ChillerPartLoadCustom,
-    EIRFPLR,        !- Name  
-    0.093291598,        !- Coefficient1 Constant
-    -0.234322952,       !- Coefficient2 x
-    0.426950368,        !- Coefficient3 x**2
-    0.188624721,        !- Coefficient4 y
-    -0.608010978,       !- Coefficient5 y**2
-    0.992031248,        !- Coefficient6 x*y
-    0.000000E+00,       !- Coefficient7 x**3
-    0.502338322,        !- Coefficient8 y**3
-    0.000000E+00,       !- Coefficient9 x**2*y
-    0.000000E+00,       !- Coefficient 10 x*y**2
-    -0.360902326,       !- Coefficient 11 x**2*y**2
-    -0.097978985,       !- Coefficient 12 z*y**3 
-    0.2562,             !- Minimum Value of x
-    1.0365,             !- Maximum Value of x
-    0.1,                !- Minimum Value of y
-    1,                  !- Maximum Value of y
-    -0.035,             !- Minimum Value of z
-    0.3144,             !- Maximum Value of z
-    ,                   !- Minimum Curve Output
-    ,                   !- Maximum Curve Output
-    Dimensionless,      !- Input Unit Type for x
-    Dimensionless,      !- Input Unit Type for y
-    Dimensionless,      !- Input Unit Type for z
-    Dimensionless;      !- Output Unit Type
-```
-
-### Curve:QuadraticLinear
-
-This curve is a function of two independent variables. Input consists of the curve name, the six coefficients, and min and max values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the quadratic linear curve:
-
-<div>\[z = \left( {{C_1} + {C_2}*x + {C_3}*{x^2}} \right) + \left( {{C_4} + {C_5}*x + {C_6}*{x^2}} \right)*y\]</div>
-
-#### Field: Name
-
-A user assigned unique name for an instance of a quadratic-linear curve. When a curve is used, it is referenced by this name.
-
-#### Field: Coefficient1 Constant
-
-The constant coefficient (C<sub>1</sub>) in the equation.
-
-#### Field: Coefficient2 x
-
-The coefficient C<sub>2</sub> in the equation.
-
-#### Field: Coefficient3 x\*\*2
-
-The coefficient C<sub>3</sub> in the equation.
-
-#### Field: Coefficient4 y
-
-The coefficient C<sub>4</sub> in the equation.
-
-#### Field: Coefficient5 x\*y
-
-The coefficient C<sub>5</sub> in the equation.
-
-#### Field: Coefficient6 x\*\*2\*y
-
-The coefficient C<sub>6</sub> in the equation.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of y
-
-The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of y
-
-The maximum allowable value of y. Values of y greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for X
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-#### Field: Input Unit Type for Y
-
-This field is used to indicate the kind of units that may be associated with the y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Y and Maximum Value of Y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-Below is an example input.
-
-```idf
-Curve:QuadraticLinear,
-DischargeCurve, !- Curve Name
-0.0,            !- Coefficient1 Constant
-0.09,           !- Coefficient2 x
--0.15,          !- Coefficient3 x\*\*2
-0.612,          !- Coefficient4 y
--0.324,         !- Coefficient5 x\*y
--0.216,         !-Coefficient6 x\*\*2\*y
-0.0,            !- Minimum Value of x
-1.0,            !- Maximum Value of x
-0.0,            !- Minimum Value of y
-9.9;            !- Maximum Value of y
-```
-
-### Curve:Triquadratic
-
-This curve is a 2<sup>nd</sup> order polynomial function of three variable polynomial independent variables. Input consists of the curve name, the twenty seven coefficients, and min and max values for each of the independent variables. Optional inputs for curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation represented by the triquadratic curve:
-
-<div>\[\begin{array}{l}CurveValue = {A_0} + {A_1}*{x^2} + {A_2}*x + {A_3}*{y^2} + {A_4}*y + {A_5}*{z^2} + {A_6}*z + {A_7}*{x^2}{y^2} + {A_8}*xy + \\\quad \quad \quad \quad \quad {A_9}*x{y^2} + {A_{10}}*{x^2}y + {A_{11}}*{x^2}{z^2} + {A_{12}}*xz + {A_{13}}*x{z^2} + {A_{14}}*{x^2}z + {A_{15}}*{y^2}{z^2} + \\\quad \quad \quad \quad \quad {A_{16}}*yz + {A_{17}}*y{z^2} + {A_{18}}*{y^2}z + {A_{19}}*{x^2}{y^2}{z^2} + {A_{20}}*{x^2}{y^2}z + {A_{21}}{x^2}y{z^2} + {A_{22}}x{y^2}{z^2} + \\\quad \quad \quad \quad \quad {A_{23}}{x^2}yz + {A_{24}}x{y^2}z + {A_{25}}xy{z^2} + {A_{26}}xyz\end{array}\]</div>
-
-#### Field: Coefficient1 Constant
-
-The constant coefficient (A<sub>0</sub>) in the equation.
-
-#### Field: Coefficient2 x\*\*2
-
-The coefficient (A<sub>1</sub>) in the equation.
-
-#### Field: Coefficient3 x
-
-The coefficient (A<sub>2</sub>) in the equation.
-
-#### Field: Coefficient4 y\*\*2
-
-The coefficient (A<sub>3</sub>) in the equation.
-
-#### Field: Coefficient5 y
-
-The coefficient (A<sub>4</sub>) in the equation.
-
-#### Field: Coefficient6 z\*\*2
-
-The coefficient (A<sub>5</sub>) in the equation.
-
-#### Field: Coefficient7 z
-
-The coefficient (A<sub>6</sub>) in the equation.
-
-#### Field: Coefficient8 x\*\*2\*y\*\*2
-
-The coefficient (A<sub>7</sub>) in the equation.
-
-#### Field: Coefficient9 x\*y
-
-The coefficient (A<sub>8</sub>) in the equation.
-
-#### Field: Coefficient10 x\*y\*\*2
-
-The coefficient (A<sub>9</sub>) in the equation.
-
-#### Field: Coefficient11 x\*\*2\*y
-
-The coefficient (A<sub>10</sub>) in the equation.
-
-#### Field: Coefficient12 x\*\*2\*z\*\*2
-
-The coefficient (A<sub>11</sub>) in the equation.
-
-#### Field: Coefficient13 x\*z
-
-The coefficient (A<sub>12</sub>) in the equation.
-
-#### Field: Coefficient14 x\*z\*\*2
-
-The coefficient (A<sub>13</sub>) in the equation.
-
-#### Field: Coefficient15 x\*\*2\*z
-
-The coefficient (A<sub>14</sub>) in the equation.
-
-#### Field: Coefficient16 y\*\*2\*z\*\*2
-
-The coefficient (A<sub>15</sub>) in the equation.
-
-#### Field: Coefficient17 y\*z
-
-The coefficient (A<sub>16</sub>) in the equation.
-
-#### Field: Coefficient18 y\*z\*\*2
-
-The coefficient (A<sub>17</sub>) in the equation.
-
-#### Field: Coefficient19 y\*\*2\*z
-
-The coefficient (A<sub>18</sub>) in the equation.
-
-#### Field: Coefficient20 x\*\*2\*y\*\*2\*z\*\*2
-
-The coefficient (A<sub>19</sub>) in the equation.
-
-#### Field: Coefficient21 x\*\*2\*y\*\*2\*z
-
-The coefficient (A<sub>20</sub>) in the equation.
-
-#### Field: Coefficient22 x\*\*2\*y\*z\*\*2
-
-The coefficient (A<sub>21</sub>) in the equation.
-
-#### Field: Coefficient23 x\*y\*\*2\*z\*\*2
-
-The coefficient (A<sub>22</sub>) in the equation.
-
-#### Field: Coefficient24 x\*\*2\*y\*z
-
-The coefficient (A<sub>23</sub>) in the equation.
-
-#### Field: Coefficient25 x\*y\*\*2\*z
-
-The coefficient (A<sub>24</sub>) in the equation.
-
-#### Field: Coefficient26 x\*y\*z\*\*2
-
-The coefficient (A<sub>25</sub>) in the equation.
-
-#### Field: Coefficient27 x\*y\*z
-
-The coefficient (A<sub>26</sub>) in the equation.
-
-#### Field: Minimum Value of x
-
-The minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of y
-
-The minimum allowable value of y. Values of y less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of y
-
-The maximum allowable value of y. Values of y greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Value of z
-
-The minimum allowable value of z. Values of z less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of z
-
-The maximum allowable value of z. Values of z greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for X
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of x. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-#### Field: Input Unit Type for Y
-
-This field is used to indicate the kind of units that may be associated with the y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Y and Maximum Value of Y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-#### Field: Input Unit Type for Z
-
-This field is used to indicate the kind of units that may be associated with the z values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Z and Maximum Value of Z. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Power
-
-- Distance
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-### Curve:Functional:PressureDrop
-
-Input for a pressure drop curve consists of the curve name, a varying number of parameters, and the maximum and minimum valid independent variable values. The equation represented by the pressure drop curve is:
-
-<div>\[\Delta P = \left( {K + f\frac{L}{D}} \right)\frac{{\rho {V^2}}}{2}\]</div>
-
-#### Field: Name
-
-A user assigned unique name for an instance of a pressure drop curve. When a curve is used, it is referenced by this name.
-
-#### Field: Diameter
-
-This diameter represents an equivalent diameter for the given branch. This is parameter (D) in the equation, and has units of {m}. Since varying components may be found on the same branch, this value must be selected along with the other inputs in order to provide a proper value of pressure drop. This is used to calculate the velocity in addition to being used directly in the frictional pressure drop calculation.
-
-#### Field: Minor Loss Coefficient
-
-This is the pressure drop coefficient typically applied to components such as fittings and occasionally heat pumps. This is parameter (K) in the equation and is dimensionless. This coefficient is used to describe the amount of dynamic pressure lost during the process. This value may be left blank if the user only wants to account for frictional losses in this branch.
-
-#### Field: Length
-
-This is the length of a pressure drop process in which friction is applied. This is parameter (L) in the equation and has units of {m}. In a pipe, this would be the length of the pipe, however in many cases, pressure drop in other components are applied as an    equivalent length.      This is only required if the user is wanting to perform frictional pressure drop calculations.
-
-#### Field: Roughness
-
-This field represents the first method to simulate frictional losses. This parameter does not appear directly in the equation above, as it is only used to develop the friction factor (f), but the roughness will have units of {m} if entered. If the user enters this roughness value, the pressure system will use it along with an approximation to the Moody chart to estimate the friction factor given the current flow conditions. This allows the friction calculate to be dynamic throughout the simulation.
-
-#### Field: Fixed Friction Factor
-
-This field represents the second method to simulate frictional losses. This is parameter (f) in the equation and is dimensionless. This parameter is a fixed value of friction factor which would override any calculations performed based on roughness, etc. If the user has a known friction factor for a given component, this is where it should be entered.
-
-In the curve outputs for this object:
-
-- Curve Input 1: MassFlow
-
-- Curve Input 2: Density
-
-- Curve Input 3: Velocity
-
-- Curve Output: the resultant value
-
-Following is an input example.
-
-```idf
-Curve:Functional:PressureDrop,
-   PressureMinorAndFriction,!- Name
-   0.05,                                       !- Diameter
-   53.8,                                       !- Minor Loss Coefficient
-   200,                                         !- Length
-   ,                                               !- Roughness
-   0.008;                                     !- Fixed Friction Factor
-```
-
-### Curve:FanPressureRise
-
-Input for the fan total pressure rise curve consists of the curve name, the four coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
-
-<div>\[\Delta {P_{fan,tot}} = {C_1}*Q_{fan}^2 + {C_2}*Q_{fan}^{} + {C_3}*Q_{fan}^{}*\sqrt {{P_{sm}} - {P_o}}  + {C_4}*\left( {{P_{sm}} - {P_o}} \right)\]</div>
-
-where <span>\(\Delta P_{fan,tot}\)</span> is the fan total pressure rise (Pa) as a function of volumetric flow through the fan (<span>\(Q_{fan}, m^3/s\)</span>), duct static pressure set point (<span>\(P_{sm}\)</span>, Pa), and static pressure surrounding the ducts (<span>\(P_o\)</span>, Pa). <span>\(P_o\)</span> is assumed to be zero.
-
-The first term of the curve looks like the common system curve in which the fan pressure rise is proportional to the square of the fan flow, but here it also depends implicitly on supply and return pressure losses, and in part on the fraction of the fan flow that is outdoor air (essentially "leaks" into and out of the return side of the system). Very often it is the only term considered, but that would only be correct with fixed-position dampers, no distribution system leakage, no linear resistance components, and no duct static pressure control.
-
-The second term accounts for significant flow resistances in the system where the pressure difference is linearly proportional to the flow. Some filters and coils in the return may need this term to be adequately described. This term could be ignored if there are no linear components or if their pressure drops are very small compared to the other terms.
-
-The third term, which depends on the fan flow and square root of the supply duct pressure *P<sub>sm</sub>*, accounts in part for leakage from the supply system when damper positions are fixed or are changed independently of static pressure or fan flow. In this case, reducing or eliminating supply leakage results in a different system curve. This, however, might be only a minor    correction    to the simple system curves generally used. The third term is zero when the VAV box dampers are modulated to control flow. Consequently, with variable-position supply dampers, reducing or eliminating supply leakage does not change the system curve.
-
-The last term also accounts in part for leakage from the supply system when damper positions are fixed or are changed independently of static pressure or fan flow. This term indicates that the same fan pressure rise can be achieved by raising the duct pressure and closing dampers. The only change in the system in such a case is that the leakage flow may increase. The coefficient for this term is one when the VAV box dampers are modulated to control flow. In both cases, this term may be the most important    correction    to the simple system curves generally used, especially at low flows.
-
-#### Field: Name
-
-The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
-
-#### Field: Fan Pressure Rise Coefficient1 C1
-
-The required numeric constant coefficient C*<sub>1</sub>* (Pa s<sup>2</sup>/m<sup>6</sup>) in the curve. Must be greater than zero.
-
-#### Field: Fan Pressure Rise Coefficient2 C2
-
-The required numeric constant coefficient C*<sub>2</sub>* (Pa s/m<sup>3</sup>) in the curve*.*
-
-#### Field: Fan Pressure Rise Coefficient3 C3
-
-The required numeric constant coefficient *C<sub>3</sub>* (Pa<sup>0.5</sup> s/m<sup>3</sup>) in the curve*.*
-
-#### Field: Fan Pressure Rise Coefficient4 C4
-
-The required numeric constant coefficient C*<sub>4</sub>* (dimensionless) in the curve*.*
-
-#### Field: Minimum Value of Qfan
-
-The required numeric minimum allowable value of *Q<sub>fan</sub>* (m<sup>3</sup>/s). Values of *Q<sub>fan</sub>* less than the minimum will be replaced within this curve by the minimum.
-
-#### Field: Maximum Value of Qfan
-
-The required numeric maximum allowable value of *Q<sub>fan</sub>* (m<sup>3</sup>/s). Values of *Q<sub>fan</sub>* greater than the maximum will be replaced within this curve by the maximum.
-
-#### Field: Minimum Value of Psm
-
-The required numeric minimum allowable value of *P<sub>sm</sub>* (Pa). Values of *P<sub>sm</sub>* less than the minimum will be replaced within this curve by the minimum.
-
-#### Field: Maximum Value of Psm
-
-The required numeric maximum allowable value of *P<sub>sm</sub>* (Pa). Values of *P<sub>sm</sub>* greater than the maximum will be replaced within this curve by the maximum.
-
-#### Field: Minimum Curve Output
-
-The optional numeric minimum allowable value of the evaluated curve (Pa). Values less than the minimum will be replaced within this curve by the minimum.
-
-#### Field: Maximum Curve Output
-
-The optional numeric maximum allowable value of the evaluated curve (Pa). Values greater than the maximum will be replaced within this curve by the maximum.
-
-The following is an input example describing the fan total pressure rise for a VAV system with a constant non-zero duct static pressure set point (the set point is described separately; see the Curve:Linear object for a related example):
-
-```idf
-   Curve:FanPressureRise,
-       VSD Example,                   ! Curve Name f = C1*Qfan**2+C2*Qfan+C3*Qfan*(Psm-Po)**0.5+C4*(Psm-Po) with Po=0
-       1446.75833497653,         ! CoefficientC1 Alpha [Pa s2/m6]
-       0.,                                     ! CoefficientC2 Beta [Pa s/m3]
-       0.,                                     ! CoefficientC3 Gamma [Pa0.5 s/m3]
-       1.,                                     ! CoefficientC4 Delta [-]
-       0.,                                     ! Minimum Value of Qfan [m3/s]
-       100.,                                 ! Maximum Value of Qfan [m3/s]
-       62.5,                                 ! Minimum Value of Psm [Pa]
-       300.,                                 ! Maximum Value of Psm [Pa]
-       0.;                                     ! Minimum Curve Output [Pa]
-       5000.;                               ! Maximum Curve Output [Pa]
-```
-
-### Curve:ExponentialSkewNormal
-
-Input for the exponential-modified skew normal curve consists of the curve name, the four coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
-
-<div>\[y = \frac{{{e^{( - 0.5*Z_1^2)}}[1 + \frac{{{Z_2}}}{{\left| {{Z_2}} \right|}}*erf\left( {\frac{{\left| {{Z_2}} \right|}}{{\sqrt 2 }}} \right)}}{{{e^{( - 0.5*Z_3^2)}}[1 + \frac{{{Z_3}}}{{\left| {{Z_3}} \right|}}*erf\left( {\frac{{\left| {{Z_3}} \right|}}{{\sqrt 2 }}} \right)}}\]</div>
-
-where *Z<sub>1</sub> =* (*x     C<sub>1</sub>*) */ C<sub>2</sub>*; *Z<sub>2</sub> =* [(*exp*<sup>(*C*</sup>*3<sup>\*x</sup>*<sup>)</sup> \* *C<sub>4</sub>\*x*) *- C<sub>1</sub>*] */ C<sub>2</sub>*; *Z<sub>3</sub> = -C<sub>1</sub> / C<sub>2</sub>*
-
-#### Field: Name
-
-The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
-
-#### Field: Coefficient1 C1
-
-The required numeric constant coefficient *C<sub>1</sub>* in the curve.
-
-#### Field: Coefficient2 C2
-
-The required numeric constant coefficient *C<sub>2</sub>* in the curve. Must be non-zero.
-
-#### Field: Coefficient3 C3
-
-The required numeric constant coefficient *C<sub>3</sub>* in the curve.
-
-#### Field: Coefficient4 C4
-
-The required numeric constant coefficient *C<sub>4</sub>* in the curve.
-
-#### Field: Minimum Value of x
-
-The required numeric minimum allowable value of *x*. Values of *x* less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The required numeric maximum allowable value of *x*. Values of *x* greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for x
-
-This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Value of *x* and Maximum Value of *x* (currently dimensionless). At this time, only the **Dimensionless** option is provided so that no unit conversion is used for this curve.
-
-#### Field: Output Unit Type
-
-This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Curve Output and Maximum Curve Output (currently dimensionless). At this time, only the **Dimensionless** option is provided so that no unit conversion is used for this curve.
-
-The following are input examples describing the normalized fan efficiency for the normal (non-stall) and stall operating regions of a backward-curved airfoil centrifugal fan:
-
-```idf
-   Curve:ExponentialSkewNormal,
-       FanEff120CPLANormal,                         ! Curve Name
-       0.072613,                                               ! CoefficientC1 Afan
-       0.833213,                                               ! CoefficientC2 Bfan
-       0.,                                                           ! CoefficientC3 Cfan
-       0.013911,                                               ! CoefficientC4 Dfan
-       -4.,                                                         ! Minimum Value of x
-       5.,                                                           ! Maximum Value of x
-       0.1,                                                         ! Minimum Curve Output
-       1.;                                                           ! Maximum Curve Output
-
-
-   Curve:ExponentialSkewNormal,
-       FanEff120CPLAStall,                           ! Curve Name
-       -1.674931,                                             ! CoefficientC1 Afan
-       1.980182,                                               ! CoefficientC2 Bfan
-       0.,                                                           ! CoefficientC3 Cfan
-       1.844950,                                               ! CoefficientC4 Dfan
-       -4.,                                                         ! Minimum Value of x
-       5.,                                                           ! Maximum Value of x
-       0.1,                                                         ! Minimum Curve Output
-       1.;                                                           ! Maximum Curve Output
-```
-
-
-### Curve:Sigmoid
-
-Input for the sigmoid curve consists of the curve name, the five coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
-
-<div>\[y = {C_1} + \frac{{{C_2}}}{{\left( {{{(1 + {e^{\left[ {\frac{{({C_3} - x)}}{{{C_4}}}} \right]}})}^{{C_5}}}} \right)}}\]</div>
-
-#### Field: Name
-
-The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
-
-#### Field: Coefficient1 C1
-
-The required numeric constant coefficient *C<sub>1</sub>* in the equation.
-
-#### Field: Coefficient2 C2
-
-The required numeric constant coefficient *C<sub>2</sub>* in the equation.
-
-#### Field: Coefficient3 C3
-
-The required numeric constant coefficient *C<sub>3</sub>* in the equation.
-
-#### Field: Coefficient4 C4
-
-The required numeric constant coefficient *C<sub>4</sub>* in the equation.
-
-#### Field: Coefficient5 C5
-
-The required numeric constant coefficient *C<sub>5</sub>* in the equation.
-
-#### Field: Minimum Value of x
-
-The required numeric minimum allowable value of *x*. Values of *x* less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The required numeric maximum allowable value of *x*. Values of *x* greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for x
-
-This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Value of *x* and Maximum Value of *x* (currently dimensionless). At this time, only the **Dimensionless** option is provided so that no unit conversion is used for this curve.
-
-#### Field: Output Unit Type
-
-This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Curve Output and Maximum Curve Output (currently dimensionless). At this time, only the **Dimensionless** option is provided so that no unit conversion is used for this curve.
-
-The following are input examples describing the normalized dimensionless flow for normal (non-stall) and stall operating regions of a backward-curved airfoil centrifugal fan:
-
-```idf
-   Curve:Sigmoid,
-       FanDimFlowNormal,                               ! Curve Name
-       0.,                                                           ! CoefficientC1 Aspd
-       1.001423,                                               ! CoefficientC2 Bspd
-       0.123935,                                               ! CoefficientC3 Cspd
-       -0.476026,                                             ! CoefficientC4 Dspd
-       1.,                                                           ! CoefficientC5 Espd
-       -4.,                                                         ! Minimum Value of x
-       5.,                                                           ! Maximum Value of x
-       0.05,                                                       ! Minimum Curve Output
-       1.;                                                           ! Maximum Curve Output
-
-   Curve:Sigmoid,
-       FanDimFlowStall,                                 ! Curve Name
-       0.,                                                           ! CoefficientC1 Aspd
-       5.924993,                                               ! CoefficientC2 Bspd
-       -1.91636,                                               ! CoefficientC3 Cspd
-       -0.851779,                                             ! CoefficientC4 Dspd
-       1.,                                                           ! CoefficientC5 Espd
-       -4.,                                                         ! Minimum Value of x
-       5.,                                                           ! Maximum Value of x
-       0.05,                                                       ! Minimum Curve Output
-       1.;                                                           ! Maximum Curve Output
-```
-
-### Curve:RectangularHyperbola1
-
-Input for the single rectangular hyperbola type 1 curve consists of the curve name, the three coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
-
-*y =*(*C<sub>1</sub> -\* x*) */* (*C<sub>2</sub>+x*) *+ C<sub>3</sub>*
-
-#### Field: Name
-
-The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
-
-#### Field: Coefficient1 C1
-
-The required numeric constant coefficient *C<sub>1</sub>* in the equation.
-
-#### Field: Coefficient2 C2
-
-The required numeric constant coefficient *C<sub>2</sub>* in the equation.
-
-#### Field: Coefficient3 C3
-
-The required numeric constant coefficient *C<sub>3</sub>* in the equation.
-
-#### Field: Minimum Value of x
-
-The required numeric minimum allowable value of *x*. Values of *x* less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The required numeric maximum allowable value of *x*. Values of *x* greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for x
-
-This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Value of *x* and Maximum Value of *x* (currently dimensionless). At this time, only the **Dimensionless** option is provided so that no unit conversion is used for this curve.
-
-#### Field: Output Unit Type
-
-This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Curve Output and Maximum Curve Output (currently dimensionless). At this time, only the **Dimensionless** option is provided so that no unit conversion is used for this curve.
-
-The following is an input example describing the maximum efficiency variation for a    mid- or average-efficiency    type of motor:
-
-```idf
-       Curve:RectangularHyperbola1,
-       MotorMaxEffAvg,                                   ! Curve Name
-       0.29228,                                                 ! CoefficientC1
-       3.368739,                                               ! CoefficientC2
-       0.762471,                                               ! CoefficientC3
-       0.,                                                           ! Minimum Value of x
-       7.6,                                                         ! Maximum Value of x
-       0.01,                                                       ! Minimum Curve Output
-       1.;                                                           ! Maximum Curve Output
-```
-
-### Curve:RectangularHyperbola2
-
-Input for the single rectangular hyperbola type 2 curve consists of the curve name, the three coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
-
-*y =*(*C<sub>1</sub> -\* x*) */* (*C<sub>2</sub>+x*) *+ C<sub>3</sub> -\* x*
-
-#### Field: Name
-
-The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
-
-#### Field: Coefficient1 C1
-
-The required numeric constant coefficient *C<sub>1</sub>* in the equation.
-
-#### Field: Coefficient2 C2
-
-The required numeric constant coefficient *C<sub>2</sub>* in the equation.
-
-#### Field: Coefficient3 C3
-
-The required numeric constant coefficient *C<sub>3</sub>* in the equation.
-
-#### Field: Minimum Value of x
-
-The required numeric minimum allowable value of *x*. Values of *x* less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The required numeric maximum allowable value of *x*. Values of *x* greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for x
-
-This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Value of *x* and Maximum Value of *x* (currently dimensionless). At this time, only the **Dimensionless** option is provided so that no unit conversion is used for this curve.
-
-#### Field: Output Unit Type
-
-This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Curve Output and Maximum Curve Output (currently dimensionless). At this time, only the **Dimensionless** option is provided so that no unit conversion is used for this curve.
-
-The following are input examples describing part-load efficiency variations for a    medium efficiency    type of V-belt (Regions 1 and 3), for a    mid- or average-efficiency    nominal 25 hp 4-pole motor, and a nominal 30 hp VFD:
-
-```idf
-Curve:RectangularHyperbola2,
-       BeltPartLoadRegion1,                         ! Curve Name
-       0.920797,                                               ! CoefficientC1
-       0.0262686,                                             ! CoefficientC2
-       0.151594,                                               ! CoefficientC3
-       0.,                                                           ! Minimum Value of x
-       1.,                                                           ! Maximum Value of x
-       0.01,                                                       ! Minimum Curve Output
-       1.;                                                           ! Maximum Curve Output
-
-   Curve:RectangularHyperbola2,
-       BeltPartLoadRegion3,                         ! Curve Name
-       1.037778,                                               ! CoefficientC1
-       0.0103068,                                             ! CoefficientC2
-       -0.0268146,                                           ! CoefficientC3
-       0.,                                                           ! Minimum Value of x
-       1.,                                                           ! Maximum Value of x
-       0.01,                                                       ! Minimum Curve Output
-       1.;                                                           ! Maximum Curve Output
-
-   Curve:RectangularHyperbola2,
-       MotorPartLoad,                                     ! Curve Name
-       1.137209,                                               ! CoefficientC1
-       0.0502359,                                             ! CoefficientC2
-       -0.0891503,                                           ! CoefficientC3
-       0.,                                                           ! Minimum Value of x
-       1.,                                                           ! Maximum Value of x
-       0.01,                                                       ! Minimum Curve Output
-       1.;                                                           ! Maximum Curve Output
-
-   Curve:RectangularHyperbola2,
-       VFDPartLoad,                                         ! Curve Name
-       0.987405,                                               ! CoefficientC1
-       0.0155361,                                             ! CoefficientC2
-       -0.0059365,                                           ! CoefficientC3
-       0.,                                                           ! Minimum Value of x
-       1.,                                                           ! Maximum Value of x
-       0.01,                                                       ! Minimum Curve Output
-       1.;                                                           ! Maximum Curve Output
-```
-
-### Curve:ExponentialDecay
-
-Input for the exponential decay curve consists of the curve name, the three coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve minimum and maximum may be used to limit the output of the performance curve (e.g., limit extrapolation). The equation is:
-
-*y = C<sub>1</sub> + C<sub>2</sub> \* exp*<sup>(*C*</sup>*3<sup>\\ \*x</sup>*<sup>)</sup>
-
-#### Field: Name
-
-The required user-assigned unique alpha name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
-
-#### Field: Coefficient1 C1
-
-The required numeric constant coefficient *C<sub>1</sub>* in the equation.
-
-#### Field: Coefficient2 C2
-
-The required numeric constant coefficient *C<sub>2</sub>* in the equation.
-
-#### Field: Coefficient3 C3
-
-The required numeric constant coefficient *C<sub>3</sub>* in the equation.
-
-#### Field: Minimum Value of x
-
-The required numeric minimum allowable value of *x*. Values of *x* less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Value of x
-
-The required numeric maximum allowable value of *x*. Values of *x* greater than the maximum will be replaced by the maximum.
-
-#### Field: Minimum Curve Output
-
-The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum.
-
-#### Field: Maximum Curve Output
-
-The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum.
-
-#### Field: Input Unit Type for x
-
-This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Value of *x* and Maximum Value of *x* (currently dimensionless). At this time, only the **Dimensionless** option is provided so that no unit conversion is used for this curve.
-
-#### Field: Output Unit Type
-
-This optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum Curve Output and Maximum Curve Output (currently dimensionless). At this time, only the **Dimensionless** option is provided so that no unit conversion is used for this curve.
-
-The following is an input example describing the part-load efficiency variation for a    medium efficiency    type of V-belt (Region 2):
-
-```idf
-Curve:ExponentialDecay,
-BeltPartLoadRegion2,                         ! Curve Name
-1.011965,                                               ! CoefficientC1
--0.339038,                                             ! CoefficientC2
--3.43626,                                               ! CoefficientC3
-0.,                                                           ! Minimum Value of x
-1.,                                                           ! Maximum Value of x
-0.01,                                                       ! Minimum Curve Output
-1.;                                                           ! Maximum Curve Output
-```
-
-### Curve:DoubleExponentialDecay
-
-Input for the double exponential decay curve consists of the curve name, the five coefficients, and the maximum and minimum valid independent variable values. Optional inputs for the curve include the minimum and maximum output of the performance curve. The equation is:
-
-<div>\[y = {C_1} + {C_2}{\exp ^{({C_3}x)}} + {C_4}{\exp ^{({C_5}x)}}\]</div>
-
-#### Field: Name
-
-This field indicates the required user-assigned name for an instance of this curve. When a curve of this type is used, it is referenced by this name.
-
-#### Field: Coefficient1 C1
-
-The required numeric constant coefficient C<sub>1</sub> in the equation.
-
-#### Field: Coefficient2 C2
-
-The required numeric constant coefficient C<sub>2</sub> in the equation.
-
-#### Field: Coefficient3 C3
-
-The required numeric constant coefficient C<sub>3</sub> in the equation.
-
-#### Field: Coefficient4 C4
-
-The required numeric constant coefficient C<sub>4</sub> in the equation.
-
-#### Field: Coefficient5 C5
-
-The required numeric constant coefficient C<sub>5</sub> in the equation.
-
-#### Field: Minimum Value of x
-
-The required numeric minimum allowable value of x. Values of x less than the minimum will be replaced by the minimum
-
-#### Field: Maximum Value of x
-
-The required numeric maximum allowable value of x. Values of x greater than the maximum will be replaced by the maximum
-
-#### Field: Minimum Curve Output
-
-The optional numeric minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum
-
-#### Field: Maximum Curve Output
-
-The optional numeric maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum
-
-#### Field: Input Unit Type for x
-
-The optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum and Maximum Value of x. Currently, only Dimensionless option is provided so that no unit conversion is used for this curve
-
-#### Field: Output Unit Type
-
-The optional field is provided for future purposes so that the IDF Editor could display the appropriate SI or IP units for the Minimum and Maximum Curve Ouput. Currently, only Dimensionless option is provided so that no unit conversion is used for this curve.
-
-
-
-An example input of the Curve:DoubleExponentialDecay input is:
-
-```idf
-   Curve:DoubleExponentialDecay,
-       BatteryCycleCurve,         !- Name
-       1380,                                   !- Coefficient1 C1
-       6834,                                   !- Coefficient2 C2
-       -8.75,                                 !- Coefficient3 C3
-       6747,                                   !- Coefficient4 C4
-       -6.22,                                 !- Coefficient5 C5
-       0,                                         !- Minimum Value of x
-       1.0;                                     !- Maximum Value of x
-```
-
-### Performance Curve Outputs
-
-#### Performance Curve Output Value
-
-The current value of the performance curve. This value is averaged over the time step being reported. Inactive or unused performance curves will show a value of -999 (e.g., equipment is off, a specific performance curve is not required for this aspect of the equipment model at this time step, etc.). This value means that the performance curve was not called during the simulation and, therefore, not evaluated. This inactive state value is only set at the beginning of each environment. When averaging over long periods of time, this inactive state value may skew results. In this case, use a detaled reporting frequency (ref. Output:Variable object) to view results at each HVAC time step.
-
-#### Performance Curve Input Variable 1(-N) Value []
-
-The current value of the nth independent variable passed to the performance curve. The order of the independent variables is in the same order as the model equation represented by this performance curve object. This value is averaged over the time step being reported.
-
-HVAC,Average,Performance Curve Output Value []
-
-HVAC,Average,Performance Curve Input Variable 1 Value []
-
-HVAC,Average,Performance Curve Input Variable 2 Value []
-
-HVAC,Average,Performance Curve Input Variable 3 Value []
-
-Group     Performance Tables
---------------------------
-
-This group of objects consists of tabular data which are used to characterize the performance of HVAC equipment. The use of performance tables eliminate the need to perform a regression analysis to calculate the performance curve equation coefficients. Two performance tables are available to represent any performance curve having one or two independent variables. The tabular data is entered as data pairs and represent each independent variable followed by the table output at that condition. When using these two performance table objects, a regression analysis may be performed during the simulation to create the associated performance curve. The regression analysis is performed when the user requests to evaluate the curve to the limits specified (see Interpolation Method input field). The performance curve that is created is used throughout the simulation and is also written to the eio file when the user sets the diagnostics output flag DisplayAdvancedVariables (ref. Output:Diagnostics, DisplayAdvancedVariables)   This performance curve object may be directly used in future input files. The following descriptions define the input requirements for the performance table objects.
-
-### Table:OneIndependentVariable
-
-Input for the data table consists of a table name, the curve type, the interpolation method, and the data pairs representing the polynomial equation. Optional inputs for minimum and maximum values for the independent variable and curve minimum and maximum may be used to limit the output of the table when evaluating the regression curve (e.g., limit extrapolation). The existing performance curves represented by this table object are:
-
-<div>\[Linear\,\,Curve:\,\,\,Output = {C_1} + {C_2}x\]</div>
-
-<div>\[Quadratic\,\,Curve:\,\,\,Output = {C_1} + {C_2}x + {C_3}{x^2}\]</div>
-
-<div>\[Cubic\,\,Curve:\,\,\,Output = {C_1} + {C_2}x + {C_3}{x^2} + {C_4}{x^3}\]</div>
-
-<div>\[Quartic\,\,Curve:\,\,\,Output = {C_1} + {C_2}x + {C_3}{x^2} + {C_4}{x^3} + {C_5}{x^4}\]</div>
-
-<div>\[Exponent\,\,Curve:\,\,\,Output = {C_1} + {C_2}{x^{{C_3}}}\]</div>
-
-#### Field: Name
-
-A unique user assigned name for an instance of a performance table. When a table is used, it is referenced by this name. The name of this table object may be used anywhere a valid performance curve object is allowed.
-
-#### Field: Curve Type
-
-The form of the polynomial equation used to represent the tabular data. Choices are *Linear*, *Quadratic*, *Cubic*, *Quartic* and *Exponent*. This field is used to determine if this table object is representative of the type of performance table (curve) allowed for a particular application (i.e., if this type of polynomial is allowed to be used as the curve type for other objects). This input infers the polynomial order (or degree). This input also specifies the number of interpolation points if the next field, Interpolation Method is set to LagrangeInterpolationLinearExtrapolation. The number of interpolation points for Linear, Quadratic, Cubic, Quartic, and Exponent are set at 2, 3, 4, 5, and 4, respectively.
-
-#### Field: Interpolation Method
-
-The method used to evaluate the tabular data. Choices are *LinearInterpolationOfTable, LagrangeInterpolationLinearExtrapolation* and *EvaluateCurveToLimits*. When *LinearInterpolationOfTable* is selected, the tabular data is interpolated within the limits of the data set and the following fields are used only within the boundary of the table limits (i.e., are only used to limit interpolation). Extrapolation of the data set is not allowed. When *LagrangeInterpolationLinearExtrapolation* is selected, a polynomial interpolation routine is used within the table boundaries along with linear extrapolation. Given the valid one independent variable equations above, the polynomial order is up to 5<sup>th</sup> order. When *EvaluateCurveToLimits* is selected, the coefficients (i.e., C in the equations above) of the polynomial equation are calculated and used to determine the table output within the limits specified in the following fields. If these fields are not entered, the limits of the tabular data are used. The minimum number of data pairs required for this choice are 2, 3, 4, 5, and 4 data pairs for linear, quadratic, cubic, quartic, and exponent curves, respectively. If insufficient data is provided, the regression analysis is not performed and the simulation reverts to interpolating the tabular data. The performance curve is written to the eio file when the output diagnotics flag DisplayAdvancedVariables is used (ref. Output:Diagnostics, DisplayAdvancedVariables).
-
-#### Field: Minimum Value of X
-
-The minimum allowable value of X. Values of X less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method*. If this field is left blank, the data set determines the limit.
-
-#### Field: Maximum Value of X
-
-The maximum allowable value of X. Values of X greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method*. If this field is left blank, the data set determines the limit.
-
-#### Field: Minimum Table Output
-
-The minimum allowable value of the table output. Values less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method*. If this field is left blank, the data set determines the limit.
-
-#### Field: Maximum Table Output
-
-The maximum allowable value of the table output. Values greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method*. If this field is left blank, the data set determines the limit.
-
-#### Field: Input Unit Type for X1
-
-This field is used to indicate the kind of units that may be associated with the x values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of X. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-#### Field: Normalization Reference
-
-The normalization point for the data set. This field provides a method for automatically normalizing a set of data. Equipment performance data is typically normalized based on a specific operating condition. Both the output values and minimum/maximum curve limits are normalized. This normalization can be performed simply by entering the data at the reference point. If this field is left blank or a 1 is entered, the data set is assumed to be in the correct format.
-
-#### Data Pairs
-
-The following inputs describe the data set. Data pairs are entered as X and Output pairs where X is the independent variable (i.e., x in the equation above) and Output is the dependent variable (i.e., Output in the equation above). Any number of data pairs may be entered, however, a minimum number of data pairs must be entered and depends on the polynomial equation. Linear (1<sup>st</sup> order), Quadratic (2<sup>nd</sup> order), Cubic (3<sup>rd</sup> order), Quartic (4<sup>th</sup> order), and Exponent (nth order) polynomials require a minimum of 2, 3, 4, 5, and 4 data pairs, respectively. This minimum requirement is for performing a regression analysis, not interpolating the tabular data. If a regression analysis is not performed (i.e., only table interpolation is used), these minimum requirements are not enforced. If a regression analysis is performed and these minimum requirements are not met, the simulation will revert to table interpolation. These fields may be repeated as many times as necessary to define the tabular data.
-
-#### Field: X Value \#n
-
-The value of the independent variable n (i.e., independent variable values for data 1 to number of data pairs).
-
-#### Field: Output Value \#n
-
-The value of the dependent variable n (i.e., dependent variable values for data 1 to number of data pairs).
-
-Following is an example input for a Table:OneIndependentVariable object:
-
-```idf
-Table:OneIndependentVariable,
-WindACCoolCapFFF,             !- Name
-Linear,                                 !- Curve Type
-EvaluateCurveToLimits,   !- Interpolation Type
-0,                                           !- Minimum Value of X1,
-1.5,                                       !- Maximum Value of X1,
-0.8,                                       !- Minimum Table Output
-1.1,                                       !- Maximum Table Output
-Dimensionless,                   !- Input Unit Type for X1
-Dimensionless,                   !- Output Unit Type
-,                                             !- Normalization Point
-0,0.8,                                   !- X Value #1, Output Value #1
-1.5,1.1;                               !- X Value #2, Output Value #2
-```
-
-
-### Performance Table Outputs
-
-#### Performance Curve Output Value []
-
-The current value of the performance table. Performance curves and tables use the same output variable. This value is averaged over the time step being reported. Inactive or unused performance curves will show a value of -999 (e.g., equipment is off, a specific performance curve is not required for this aspect of the equipment model at this time step, etc.). This value means that the performance curve was not called during the simulation and, therefore, not evaluated. This inactive state value is only set at the beginning of each environment. When averaging over long periods of time, this inactive state value may skew results. In this case, use a detaled reporting frequency (ref. Output:Variable object) to view results at each HVAC time step.
-
-#### Performance Curve Input Variable 1 Value []
-
-The current value of the independent variable passed to the performance curve. This value is averaged over the time step being reported.
-
-HVAC,Average,Performance Curve Output Value []
-
-HVAC,Average,Performance Curve Input Variable 1 Value []
-
-### Table:TwoIndependentVariables
-
-Input for the data table consists of a table name, the curve type, the interpolation method, and the data pairs representing the polynomial equation. Optional inputs for minimum and maximum values for the independent variable, and curve minimum and maximum may be used to limit the output of the table (e.g., limit extrapolation) when evaluating the regression curve instead of the tabular data. The polynomial equations currently represented by this table object are:
-
-<div>\[BiQuadratic\,\,Curve:\,\,\,\,Output = {C_1} + {C_2}x + {C_3}{x^2} + {C_4}y + {C_5}{y^2} + {C_6}xy\]</div>
-
-<div>\[QuadraticLinear\,\,Curve:\,\,\,\,Output = {C_1} + {C_2}x + {C_3}{x^2} + {C_4}y + {C_5}xy + {C_6}{x^2}y\]</div>
-
-#### Field: Name
-
-A unique user assigned name for an instance of a performance table. When a table is used, it is referenced by this name. The name of this table object may be used anywhere a valid performance curve object is allowed.
-
-#### Field: Curve Type
-
-The form of the polynomial equation represented by the entered data. The only valid choices are *BiQuadratic* and *QuadraticLinear*. This field is used to determine if this table object is representative of the type of performance table (curve) allowed for a particular equipment model (i.e., if this type of polynomial is allowed to be used as the curve type for specific input fields). A minimum of 6 data pairs are required when selecting *EvaluateCurveToLimits* in the following field. This input also specifies the number of interpolation points if the next field, Interpolation Method is set to LagrangeInterpolationLinearExtrapolation. The number of interpolation points for BiQuadratic and QuadraticLinear are set at 6.
-
-#### Field: Interpolation Method
-
-The method used to evaluate the tabular data. Choices are *LinearInterpolationOfTable, LagrangeInterpolationLinearExtrapolation,* and *EvaluateCurveToLimits*. When *LinearInterpolationOfTable* is selected, the data entered is evaluated within the limits of the data set and the following fields are used only within the boundary of the table limits (i.e., are only used to limit interpolation). A complete data set is required. For each X variable, entries must include all Y variables and associated curve output (i.e., a complete table, no gaps or missing data). Extrapolation of the data set is not allowed. When Lagrange*InterpolationLinearExtrapolation* is selected, a polynomial interpolation routine is used within the table boundaries along with linear extrapolation. Given the valid equations above, the polynomial order is fixed at 2 which infers that 3 data points will be used for interpolation. When *EvaluateCurveToLimits* is selected, the coefficients (i.e., C in the equations above) of the polynomial equation are calculated and used to determine the table output within the limits specified in the following fields (or the tabular data, whichever provide the larger range). If the following fields are not entered, the limits of the data set are used. A complete table is not required when using this method, however, a minimum number of data is required to perform the regression analysis. The minimum number of data pairs required for this choice is 6 data pairs for both bi-quadratic and quadratic-linear curve types. If insufficient data is provided, the simulation reverts to interpolating the tabular data. The performance curve is written to the eio file when the output diagnotics flag DisplayAdvancedVariables is used (ref. Output:Diagnostics, DisplayAdvancedVariables).
-
-#### Field: Minimum Value of X
-
-The minimum allowable value of X. Values of X less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method*. If this field is left blank, the data set determines the limit.
-
-#### Field: Maximum Value of X
-
-The maximum allowable value of X. Values of X greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method*. If this field is left blank, the data set determines the limit.
-
-#### Field: Minimum Value of Y
-
-The minimum allowable value of Y. Values of Y less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method*. If this field is left blank, the data set determines the limit.
-
-#### Field: Maximum Value of Y
-
-The maximum allowable value of Y. Values of Y greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method*. If this field is left blank, the data set determines the limit.
-
-#### Field: Minimum Table Output
-
-The minimum allowable value of the table output. Values less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method*. If this field is left blank, the data set determines the limit.
-
-#### Field: Maximum Table Output
-
-The maximum allowable value of the table output. Values greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method*. If this field is left blank, the data set determines the limit.
-
-#### Field: Input Unit Type for X
-
-This field is used to indicate the kind of units that may be associated with the X values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X and Maximum Value of X. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Input Unit Type for Y
-
-This field is used to indicate the kind of units that may be associated with the Y values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of Y and Maximum Value of Y. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-#### Field: Normalization Reference
-
-The normalization point for the data set. This field provides a method for automatically normalizing a set of data. Equipment performance data is typically normalized based on a specific operating condition. Both the output values and minimum/maximum curve limits are normalized as applicable. This normalization can be performed simply by entering the data at the reference point. If this field is left blank or a 1 is entered, the data set is assumed to be in the correct format.
-
-#### Data Pairs
-
-The following inputs describe the data set. Data pairs are entered as X, Y and Output pairs where X and Y are the independent variables (i.e., x and y in the equations above) and Output is the dependent variable (i.e., Output in the equation above). Any number of data pairs may be entered, however, a minimum number of data pairs must be entered and depends on the polynomial equation. BiQuadratic and QuadraticLinear (2<sup>nd</sup> order with 2 independent variables) require a minimum of 6 data pairs. This minimum requirement is for performing a regression analysis, not interpolating the tabular data. If a regression analysis is not performed (i.e., only table interpolation is used), these minimum requirements are not enforced. If a regression analysis is performed and these minimum requirements are not met, the simulation will revert to table interpolation. These fields may be repeated as many times as necessary to define the tabular data.
-
-#### Field: X Value \#n
-
-The value of the first independent variable n (i.e., first independent variable values for data pair 1 to number of data pairs).
-
-#### Field: Y Value \#n
-
-The value of the second independent variable n (i.e., second independent variable values for data pair 1 to number of data pairs).
-
-#### Field: Output Value \#n
-
-The value of the dependent variable n (i.e., dependent variable values for data pair 1 to number of data pairs).
-
-Following is an example input for a Table:TwoIndependentVariable object:
-
-```idf
-Table:TwoIndependentVariables,
-CCOOLEIRFT,                         !- Name
-BiQuadratic,                       !- Curve Type
-EvaluateCurveToLimits,   !- Interpolation Type
-5.0,                                       !- Minimum Value of x,
-60.0,                                     !- Maximum Value of x,
-5.0,                                       !- Minimum Value of y,
-70.0,                                     !- Maximum Value of y,
-0.01,                                     !- Minimum Table Output
-0.5,                                       !- Maximum Table Output
-Temperature,                       !- Input Unit Type for x
-Temperature,                       !- Input Unit Type for y
-Dimensionless,                   !- Output Unit Type
-0.258266502,                       !- Normalization Point
-17.2222222,18.3333333,0.18275919, !-X Value #1,Y Value #1,Output #1
-17.2222222,23.8888889,0.207383768,!-X Value #2,Y Value #2,Output #2
-17.2222222,29.4444444,0.237525541,!-X Value #3,Y Value #3,Output #3
-17.2222222,35,0.274217751,               !-X Value #4,Y Value #4,Output #4
-17.2222222,40.5555556,0.318548624,!-X Value #5,Y Value #5,Output #5
-17.2222222,46.1111111,0.374560389,!-X Value #6,Y Value #6,Output #6
-19.4444444,18.3333333,0.172982816,!-X Value #7,Y Value #7,Output #7
-19.4444444,23.8888889,0.19637691, !-X Value #8,Y Value #8,Output #8
-19.4444444,29.4444444,0.224789822,!-X Value #9,Y Value #9,Output #9
-19.4444444,35,0.258266502,               !-X Value #10,Y Value #10,Output #10
-19.4444444,40.5555556,0.299896794,!-X Value #11,Y Value #11,Output #11
-19.4444444,46.1111111,0.351242021,!-X Value #12,Y Value #12,Output #12
-21.6666667,18.3333333,0.164081122,!-X Value #13,Y Value #13,Output #13
-21.6666667,23.8888889,0.185603303,!-X Value #14,Y Value #14,Output #14
-21.6666667,29.4444444,0.211709812,!-X Value #15,Y Value #15,Output #15
-21.6666667,35,0.243492052,               !-X Value #16,Y Value #16,Output #16
-21.6666667,40.5555556,0.281757875,!-X Value #17,Y Value #17,Output #17
-21.6666667,46.1111111,0.331185659;!-X Value #18,Y Value #18,Output #18
-```
-
-
-### Two Independent Variable Performance Table Outputs
-
-#### Performance Curve Output Value []
-
-The current value of the performance table. Performance curves and tables use the same output variable. This value is averaged over the time step being reported. Inactive or unused performance curves will show a value of -999 (e.g., equipment is off, a specific performance curve is not required for this aspect of the equipment model at this time step, etc.). This value means that the performance curve was not called during the simulation and, therefore, not evaluated. This inactive state value is only set at the beginning of each environment. When averaging over long periods of time, this inactive state value may skew results. In this case, use a detaled reporting frequency (ref. Output:Variable object) to view results at each HVAC time step.
-
-#### Performance Curve Input Variable 1 Value []
-
-#### Performance Curve Input Variable 2 Value []
-
-The current value of the first and second independent variable passed to the performance curve. The order of the independent variables is in the same order as the model equation represented by this performance curve object. This value is averaged over the time step being reported.
-
-* HVAC,Average,Performance Curve Output Value []
-
-* HVAC,Average,Performance Curve Input Variable 1 Value []
-
-* HVAC,Average,Performance Curve Input Variable 2 Value []
-
-### Lookup Tables
-
-Lookup tables are useful for determining the results of a nth order polynomial without the need to calculate the polynomial coefficients. The Lagrange method for interpolation is currently the only method available for polynomial interpolation. LinearInterpolationOfTable and EvaluateCurveToLimits may also be used. The multi-variable lookup table can represent from 1 to 5 independent variables and can interpolate these independent variables up to a 4<sup>th</sup> order polynomial. The polynomial order is assumed to be the number of interpolation points (n) minus 1. Polynomial interpolation of tabular data takes place when the values of the independent variables are within the upper table boundary and at least n data points are available when approaching the lower table boundary for any independent variable. When any independent variable value is outside the table limits, linear extrapolation is used to predict the table result and is based on the two nearest data points in the table for that particular independent variable.
-
-### Table:MultiVariableLookup
-
-Input for the multi-variable data table consists of a table name, the interpolation method, the number of points to be used for interpolation, an optional external file name, and, if an external file name is not entered, the tabular data. Optional inputs for minimum and maximum values for the independent variable, and curve minimum and maximum may be used to limit the output of the table (e.g., limit extrapolation).
-
-#### Field: Name
-
-A unique user assigned name for an instance of a lookup table. When a table is used, it is referenced by this name. The name of this table object may be used anywhere a valid performance curve object is allowed.
-
-#### Field: Curve Type
-
-The order of the polynomial used to represent the tabular data. Choices are *Linear*, *Quadratic*, *Cubic*, *Quartic, BiQuadratic, QaudraticLinear, BuCibic*. This field is used to determine if this table object is representative of the type of performance table (curve) allowed for a particular application (i.e., if this type of polynomial is allowed to be used as the curve type for other objects). This input also infers the polynomial order (or degree).
-
-#### Field: Interpolation Method
-
-The method used to evaluate the lookup table. The choices are *LinearInterpolationOfTable, LagrangeInterpolationLinearExtrapolation, and EvaluateCurveToLimits*. . When *LinearInterpolationOfTable* is selected, the data entered is evaluated within the limits of the data set and the minimum/maximum value of x and output inputs are used only within the boundary of the table limits (i.e., are only used to limit interpolation). A complete data set is required. For each X variable, entries must include all Y variables and associated curve output (i.e., a complete table, no gaps or missing data). Extrapolation of the data set is not allowed. When *LagrangeInterpolationLinearExtrapolation* is selected, the lookup table is evaluated using Lagrange   s form of the interpolating polynomial. The order of the polynomial is inferred to be one less than the input in the Number of Interpolation Points field below. When *EvaluateCurveToLimits* is selected, the coefficients (i.e., C in the equation above) of the polynomial equation are calculated and used to determine the table output within the limits specified in the following fields (or the tabular data, whichever provide the larger range). If the minimum/maximum fields below are not entered, the limits of the data set are used. A complete table is not required when using this method, however, a minimum number of data is required to perform the regression analysis. The minimum number of data pairs required for this choice is 6 data pairs for both bi-quadratic and quadratic-linear curve types. If insufficient data is provided, the simulation reverts to interpolating the tabular data. The performance curve is written to the eio file when the output diagnotics flag DisplayAdvancedVariables is used (ref. Output:Diagnostics, DisplayAdvancedVariables). A regression analysis may only be performed on lookup tables with one or two independent variables.
-
-#### Field: Table Data Format
-
-The format specifier which determines the method used to read the lookup table. The only valid choice at this time is *SingleLineIndependentVariableWithMatrix*. When *SingleLineIndependentVariableWithMatrix* is selected, a free format is used as shown below. The format shown below assumes the output values are in ascending order for both independent variables 1 and 2. Tabular data are entered in 3 groups of data, the header, the independent variable values, and the tabular data matrix. A summary of the external file format is shown below.
-
-Key:
-
-* IV = independent variable (i.e., the X1, or X2, etc)
-
-* NIV = number of independent variables (i.e., number of values for X1, or X2, etc.)
-
-* IVV = independent variable value (i.e., the value for X1, or X2, etc.)
-
-* NIV1 = number of values for independent variable \#1 (i.e., X1)
-
-* NIV2 = number of values for independent variable \#2 (i.e., X2)
-
-* NIV3 = number of values for independent variable \#3 (i.e., X3)
-
-* NIV4 = number of values for independent variable \#4 (i.e., X4)
-
-* NIV5 = number of values for independent variable \#5 (i.e., X5)
-
-* OV = output value
-
-```
-Header:
-Row 1: <NIV>, <NIV1>, <NIV2> (only used if NIV>1), <NIV3> (only used if NIV>2),
-<NIV4> (only used if NIV>3), <NIV5> (only used if NIV>4)
-
-
-Independent Variable Values:
-Row 2: <IVV1 to IVVn for IV1> where n = NIV1 (max = 10)
-Row 2a (row included only when NIV > 1): IVV1 to IVVn for IV2 where n = NIV2 (max = 10)
-Row 2b (row included only when NIV > 2): IVV1 to IVVn for IV3 where n = NIV3 (max = 10)
-Row 2c (row included only when NIV > 3): IVV1 to IVVn for IV4 where n = NIV4 (max = 10)
-Row 2d (row included only when NIV > 4): IVV1 to IVVn for IV5 where n = NIV5 (max = 10)
-
-
-Tabular Data Matrix Format (repeat rows 3 and 4(1)     4(m) for each occurrence of a unique data pair for independent variable #3, #4, and #5):
-
-
-Row 3 (row included only when NIV > 2): IVVn for IV3, IVVn for IV4 (included only when NIV > 3), IVVn for IV5 (included only when NIV > 4), (where n = a unique value for the independent variable)
-
-
-Row 4(1): OV1/1 to OVn/1 for each value of IV1 where n = NIV1 representing IV2(1)
-Row 4(2): OV1/2 to OVn/2 for each value of IV1 where n = NIV1 representing IV2(2)
-Row 4(3): OV1/3 to OVn/3 for each value of IV1 where n = NIV1 representing IV2(3)
-...
-Row 4(m): OV1/m to OVn/m for each value of IV1 where n = NIV1 representing IV2(m) where m = NIV2
-```
-
-
-
-#### Field: Number of Interpolation Points
-
-This field specifies the number of data points to be used in the lookup table interpolation. The value specified in this field should be 1 greater than the order (or degree) of the polynomial used for interpolation. For example, if 2 is entered here, the polynomial is assumed to be first order where only 2 data points are required to calculate the table solution. If 3 is entered here, the polynomial is assumed to be second order and 3 data points would be required to calculate the table solution. Linear extrapolation is always used when the independent variable values are near the lower edge or outside the range of the table. The interpolation points selected are always the nearest data point greater than the independent variable with 1 or more values less than the independent variable. For example, if 3 interpolation points are used, the data point greater than the independent variable and 2 data points less than the indpenedent variable are used to determine the table solution. If the independent variable exactly equals a table reference point, that value is used as the table solution.
-
-#### Field: External File Name
-
-The name of an external file that represents the tabular data. This file would include all data after the Output Unit Type field below starting with the number of independent variables and continuing until all input and output values have been entered. The tabular data may use either comma, space or tab delimited format. The field should include a full path with file name, for best results. The field must be &lt;= 100 characters. The file name must not include commas or an exclamation point. A relative path or a simple file name should work with version 7.0 or later when using EP-Launch even though EP-Launch uses temporary directories as part of the execution of EnergyPlus. If using RunEPlus.bat to run EnergyPlus from the command line, a relative path or a simple file name may work if RunEPlus.bat is run from the folder that contains EnergyPlus.exe.
-
-#### Field: X1 Sort Order
-
-The choice field specifies the order of the lookup table data for the 1<sup>st</sup> independent variable. Valid choices are *Increasing* or *Decreasing*. If increasing is selected, then the order of the data is from lowest value of the 1<sup>st</sup> independent variable to highest. If decreasing is selected, then the order of the data is from highest value of the 1<sup>st</sup> independent variable to lowest.
-
-#### Field: X2 Sort Order
-
-The choice field specifies the order of the lookup table data for the 2<sup>nd</sup> independent variable. Valid choices are *Increasing* or *Decreasing*. If increasing is selected, then the order of the data is from lowest value of the 2<sup>nd</sup> independent variable to highest. If decreasing is selected, then the order of the data is from highest value of the 2<sup>nd</sup> independent variable to lowest.
-
-#### Field: Minimum Value of X1
-
-The minimum allowable value of X1. Values of X1 less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit.
-
-#### Field: Maximum Value of X1
-
-The maximum allowable value of X1. Values of X1 greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit.
-
-#### Field: Minimum Value of X2
-
-The minimum allowable value of X2. Values of X2 less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 1.
-
-#### Field: Maximum Value of X2
-
-The maximum allowable value of X2. Values of X2 greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 1.
-
-#### Field: Minimum Value of X3
-
-The minimum allowable value of X3. Values of X3 less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 2.
-
-#### Field: Maximum Value of X3
-
-The maximum allowable value of X3. Values of X3 greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 2.
-
-#### Field: Minimum Value of X4
-
-The minimum allowable value of X4. Values of X4 less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 3.
-
-#### Field: Maximum Value of X4
-
-The maximum allowable value of X4. Values of X4 greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 3.
-
-#### Field: Minimum Value of X5
-
-The minimum allowable value of X5. Values of X5 less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 4.
-
-#### Field: Maximum Value of X5
-
-The maximum allowable value of X5. Values of X5 greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit. This field is only used when the number of independent variables is greater than 4.
-
-#### Field: Minimum Curve Output
-
-The minimum allowable value of the evaluated curve. Values less than the minimum will be replaced by the minimum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit.
-
-#### Field: Maximum Curve Output
-
-The maximum allowable value of the evaluated curve. Values greater than the maximum will be replaced by the maximum. This field can only limit extrapolation when the *Interpolation Method* is selected as *EvaluateCurveToLimits or LagrangeInterpolationLinearExtrapolation*. This filed can be used to limit interpolation using any *Interpolation Method.* If this field is left blank, the data set determines the limit.
-
-#### Field: Input Unit Type for X1
-
-This field is used to indicate the kind of units that may be associated with the X1 values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X1 and Maximum Value of X1. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Input Unit Type for X2
-
-This field is used to indicate the kind of units that may be associated with the X2 values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X2 and Maximum Value of X2. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Input Unit Type for X3
-
-This field is used to indicate the kind of units that may be associated with the X3 values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X3 and Maximum Value of X3. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Input Unit Type for X4
-
-This field is used to indicate the kind of units that may be associated with the X4 values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X4 and Maximum Value of X4. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Input Unit Type for X5
-
-This field is used to indicate the kind of units that may be associated with the X5 values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Value of X5 and Maximum Value of X5. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Temperature
-
-- VolumetricFlow
-
-- MassFlow
-
-- Distance
-
-- Power
-
-#### Field: Output Unit Type
-
-This field is used to indicate the kind of units that may be associated with the output values. It is used by IDF Editor to display the appropriate SI and IP units for the Minimum Curve Output and Maximum Curve Output. The unit conversion is not applied to the coefficients. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion.
-
-- Dimensionless
-
-- Capacity
-
-- Power
-
-### Data Input Format
-
-The following inputs describe the data set. These values may also be placed in an external file starting with Field \#1. If an external file name is entered above, the following fields are not used. Data are entered in a specific order according to the number and quantity of independent variables. The data input format is described here in 3 groups as Header, Independent Variable Values, and the Tabular Data. The header is always the first line in the data set and represents the number of independent varibles followed by the number of values for each independent variable. The independent variable values are listed next and represent the values of each independent variable on a separate line. These values are only listed once at the top of the data set and are listed in ascending order. The number of independent variables, the first number in the header, specifies how many lines, or rows, make up this section of tabular data. The remaining lines are repeated as many times as necessary to completely describe the tabular data. The values of independent variables 3     n are listed on a single line followed by a matrix of data that represent the table output corresponding to independent variables 1 and 2.
-
-- **Header:**
-
-Line 1: The first number specified is the number of independent variables followed by the number of variables for each independent variable.
-
-- **Independent Variable Values:**
-
-Line 1: the n values for the first independent variable as specified in the header.
-
-Line 2: the n values for the second independent variable as specified in the header if the number of independent variables is greater than 1. This line is not required if the number of independent variables is less than 2.
-
-Line 3: the n values for the third independent variable as specified in the header if the number of independent variables is greater than 2. This line is not required if the number of independent variables is less than 3.
-
-Line 4: the n values for the fourth independent variable as specified in the header if the number of independent variables is greater than 3. This line is not required if the number of independent variables is less than 4.
-
-Line 5: the n values for the fifth independent variable as specified in the header if the number of independent variables is greater than 4. This line is not required if the number of independent variables is less than 5.
-
-- **Tabular Data:**
-
-Line 1: the values of the 3<sup>rd</sup> through nth independent variables
-
-Line 2     m (where m-1 equals the number of variables for the second independent variable): the tabular data corresponding to the 1<sup>st</sup> independent variable (the number of inputs on this line equals the number of values for 1<sup>st</sup> independent variable), the mth values for the 2<sup>nd</sup> independent variable and corresponding to the values for the 3<sup>rd</sup>     nth independent variables (see Line 1 above for Tabular Data).
-
-Three examples are provided here as this can be difficult to describe in text. This example assumes that the table data are listed in ascending order from lowest to highest.
-
-- **One Independent Variable:**
-
-- **Header:**
-
-1, 5, (1 independent variable with 5 values for the single independent variable)
-
-- **Independent Variable Values:**
-
-70, 72, 74, 76, 78, (the five values for the single independent variable, these values are always listed in ascending order)
-
-- **Tabular Data:**
-
-0.1, 0.3, 0.5, 0.7, 0.9; (the table values associated with the independent variable values listed previously     Note: these values may be read in ascending or descending order based on the input in the X1 Sort Order field above). Example: If X1 Sort Order is ascending, 0.1 corresponds to the value of 70 for the first independent variable. If X1 Sort Order is descending, then 0.1 corresponds to the value of 78 for the first independent variable.   The use of ascending order provides a direct correlation to inputs for the Independent Variable Values group above.
-
-- **Two Independent Variables:**
-
-- **Header:**
-
-2, 5, 6, (2 independent variables with 5 and 6 values for the 1<sup>st</sup> and 2<sup>nd</sup> independent variables, respectively)
-
-- **Independent Variable Values:**
-
-70, 72, 74, 76, 78, (the five values for the 1st independent variable, these values are always listed in ascending order)
-
-32, 45, 68, 81, 94, 107, (the six values for the 2nd independent variable, these values are always listed in ascending order)
-
-- **Tabular Data:**
-
-0.1, 0.3, 0.5, 0.7, 0.9, (the first five table values associated with each value of the 1<sup>st</sup> independent variable and the first value (32) of the second independent variable listed previously     Note: these values may be listed in ascending or descending order based on the input in the X1 Sort Order field above. Each of these rows may also be listed in ascending or descending order based on the input in the X2 Sort Order field above).
-
-0.2, 0.4, 0.6, 0.8, 1.0, (the second five table values associated with each value of the 1<sup>st</sup> independent variable and the second value (45) of the second independent variable listed previously).
-
-0.3, 0.5, 0.7, 0.9, 1.1, (the third five table values associated with each value of the 1<sup>st</sup> independent variable and the third value (68) of the second independent variable listed previously).
-
-0.4, 0.6, 0.8, 1.0, 1.2, (the fourth five table values associated with each value of the 1<sup>st</sup> independent variable and the fourth value (81) of the second independent variable listed previously).
-
-0.5, 0.7, 0.9, 1.1, 1.3, (the fifth five table values associated with each value of the 1<sup>st</sup> independent variable and the fifth value (94) of the second independent variable listed previously).
-
-0.6, 0.8, 1.0, 1.2, 1.4; (the sixth five table values associated with each value of the 1<sup>st</sup> independent variable and the sixth value (107) of the second independent variable listed previously).
-
-- **Three Independent Variables:**
-
-- **Header:**
-
-3, 5, 6, 2, (3 independent variables with 5, 6 and 2 values for the 1<sup>st</sup> , 2<sup>nd</sup>, and 3<sup>rd</sup> independent variables)
-
-- **Independent Variable Values:**
-
-70, 72, 74, 76, 78, (the five values for the 1st independent variable, these values are always listed in ascending order)
-
-32, 45, 68, 81, 94, 107, (the six values for the 2nd independent variable, these values are always listed in ascending order)
-
-15.5, 45.5, (the two values for the 3<sup>rd</sup> independent variable, these values are always listed in ascending order)
-
-- **Tabular Data:**
-
-15.5, (the first value for the 3<sup>rd</sup> independent variable     values for the 4<sup>th</sup> and 5<sup>th</sup> independent variable are also listed on this line if they are used)
-
-0.1, 0.3, 0.5, 0.7, 0.9, (the table values associated with each value of the 1<sup>st</sup> independent variable, the first value (32) of the second independent variable, and the first value (15.5) of the 3<sup>rd</sup> independent variable). Note: these values may be listed in ascending or descending order based on the input in the X1 Sort Order field above).
-
-0.2, 0.4, 0.6, 0.8, 1.0, (the table values associated with each value of the 1<sup>st</sup> independent variable, the second value (45) of the second independent variable, and the first value (15.5) of the 3<sup>rd</sup> independent variable).
-
-0.3, 0.5, 0.7, 0.9, 1.1, (the table values associated with each value of the 1<sup>st</sup> independent variable, the third value (68) of the second independent variable, and the first value (15.5) of the 3<sup>rd</sup> independent variable).
-
-0.4, 0.6, 0.8, 1.0, 1.2, (the table values associated with each value of the 1<sup>st</sup> independent variable, the fourth value (81) of the second independent variable, and the first value (15.5) of the 3<sup>rd</sup> independent variable).
-
-0.5, 0.7, 0.9, 1.1, 1.3, (the table values associated with each value of the 1<sup>st</sup> independent variable, the fifth value (94) of the second independent variable, and the first value (15.5) of the 3<sup>rd</sup> independent variable).
-
-0.6, 0.8, 1.0, 1.2, 1.4. (the table values associated with each value of the 1<sup>st</sup> independent variable, the sixth value (107) of the second independent variable, and the first value (15.5) of the 3<sup>rd</sup> independent variable).
-
-45.5, (the second value for the 3<sup>rd</sup> independent variable     values for the 4<sup>th</sup> and 5<sup>th</sup> independent variable are also listed on this line if they are used)
-
-1.1, 1.3, 1.5, 1.7, 1.9, (the table values associated with each value of the 1<sup>st</sup> independent variable, the first value (32) of the second independent variable, and the second value (45.5) of the 3<sup>rd</sup> independent variable).
-
-1.2, 1.4, 1.6, 1.8, 2.0, (the table values associated with each value of the 1<sup>st</sup> independent variable, the second value (45) of the second independent variable, and the second value (45.5) of the 3<sup>rd</sup> independent variable).
-
-1.3, 1.5, 1.7, 1.9, 2.1, (the table values associated with each value of the 1<sup>st</sup> independent variable, the third value (68) of the second independent variable, and the second value (45.5) of the 3<sup>rd</sup> independent variable).
-
-1.4, 1.6, 1.8, 2.0, 2.2, (the table values associated with each value of the 1<sup>st</sup> independent variable, the fourth value (81) of the second independent variable, and the second value (45.5) of the 3<sup>rd</sup> independent variable).
-
-1.5, 1.7, 1.9, 2.1, 2.3, (the table values associated with each value of the 1<sup>st</sup> independent variable, the fifth value (94) of the second independent variable, and the second value (45.5) of the 3<sup>rd</sup> independent variable).
-
-1.6, 1.8, 2.0, 2.2, 2.4. (the table values associated with each value of the 1<sup>st</sup> independent variable, the sixth value (107) of the second independent variable, and the second value (45.5) of the 3<sup>rd</sup> independent variable).
-
-Note: The following fields define the tabular data as described in the previous examples. These field values depend on the number and quantity of independent variables used in the table. The tabular data can be entered in the following fields or entered using an external file. These fields are echoed to the eio file as a check when the output diganostics flag DisplayAdvancedVariables is used (ref. Output:Diagnostics, DisplayAdvancedVariables). The normalization value is not included in the echoed values.
-
-#### Field: Field \#1 (NumberOfIndependentVariables)
-
-The number of independent variables used in the lookup table. This number (n) can range from 1 to 5. The number entered here will define the following n fields as the number of values for these n independent variables. This is the first number in the external file as shown in the previous examples.
-
-#### Field: Field \#2 (NumberOfValuesForIndependentVariable1)
-
-The number of values for the first independent variable. This is the second number in the tabular data and resides on the same line as Field \#1.
-
-#### Field: Field \#3 (DeterminedByPreviousFields)
-
-The value specified in this field is dependent on the number entered in Field \#1. If a 1 is entered in Field \#1, this field represents the first value of the single independent variable. The number of values entered in Field \#3-\#n will be equal to the number entered in Field \#2. Values entered in fields \#3-\#n are always entered in increasing value (ascending order). If a number greater than 1 is entered in Field \#1, this field represents the number of values for the second independent variable.
-
-#### Field: Field \#4
-
-The value specified in this field is dependent on the number entered in Field \#1. If a 1 is entered in Field \#1, this field represents the second value of the single independent variable. The number of values entered in Field \#3-\#n will be equal to the number entered in Field \#2. Values entered in fields \#3-\#n are always entered in increasing value (ascending order). If a 2 is entered in Field \#1, this field represents the first value of the first independent variable. If a number greater than 2 is entered in Field \#1, this field represents the number of values for the third independent variable.
-
-&lt;reduced for brevity&gt;
-
-
-
-Following is an example input for a Table:MultiVariableLookup object:
-
-```idf
-Table:MultiVariableLookup,
-HPACCoolCapFT,                       !- Name
-LagrangeinterpolationLinearExtrapolation,   !- Interpolation Method
-3,                                               !- Number of Interpolation Points
-BiQuadratic,                           !- Interpolation Type
-SingleLineIndependentVariableWithMatrix, !- Table Data Format
-,                                                 !- External File Name
-ASCENDING,                               !- X1 Sort Order
-ASCENDING,                               !- X2 Sort Order
-24999.9597049817,                 !- Normalization reference
-12.77778,                                 !- Minimum Value of X1,
-23.88889,                                 !- Maximum Value of X1,
-18.0,                                         !- Minimum Value of X2,
-46.11111,                                 !- Maximum Value of X2,
-,                                                 !- Minimum Value of X3
-,                                                 !- Maximum Value of X3
-,                                                 !- Minimum Value of X4
-,                                                 !- Maximum Value of X4
-,                                                 !- Minimum Value of X5
-,                                                 !- Maximum Value of X5
-,                                                 !- Minimum Table Output
-,                                                 !- Maximum Table Output
-Temperature,                           !- Input Unit Type for X1
-Temperature,                           !- Input Unit Type for X2
-,                                                 !- Input Unit Type for X3
-,                                                 !- Input Unit Type for X4
-,                                                 !- Input Unit Type for X5
-Dimensionless,                       !- Output Unit Type
-2, 6, 7,
-12.77778, 15, 18, 19.44448943, 21, 23.88889,
-18, 24, 30, 35, 36, 41, 46.11111,
-24421.69383, 25997.3589, 28392.31868, 29655.22876, 31094.97495, 33988.3473,
-22779.73113, 24352.1562, 26742.74198, 28003.546, 29441.02425, 32330.1846,
-21147.21662, 22716.4017, 25102.61348, 26361.31143, 27796.52175, 30681.4701,
-19794.00525, 21360.49033, 23743.0571, 25000, 26433.32038, 29314.75872,
-19524.15032, 21090.0954, 23471.93318, 24728.52506, 26161.46745, 29042.2038,
-18178.81244, 19742.05753, 22120.2503, 23375.08713, 24806.13958, 27683.36592,
-16810.36004, 18370.84513, 20745.3119, 21998.35468, 23427.47518, 26301.11353;
-```
-
-
-### Lookup Table Outputs
-
-#### Performance Curve Output Value []
-
-The current value of the lookup table. Performance curves and tables use the same output variable. This value is averaged over the time step being reported. Inactive or unused performance curves will show a value of -999 (e.g., equipment is off, a specific performance curve is not required for this aspect of the equipment model at this time step, etc.). This value means that the performance curve was not called during the simulation and, therefore, not evaluated. This inactive state value is only set at the beginning of each environment. When averaging over long periods of time, this inactive state value may skew results. In this case, use a detaled reporting frequency (ref. Output:Variable object) to view results at each HVAC time step.
-
-#### Performance Curve Input Variable 1(-N) Value []
-
-The current value of the nth independent variable passed to the performance curve. The order of the independent variables is in the same order as the model equation represented by this performance curve object. This value is averaged over the time step being reported.
-
-HVAC,Average,Performance Curve Output Value []
-
-HVAC,Average,Performance Curve Input Variable 1 Value []
-
-HVAC,Average,Performance Curve Input Variable 2 Value []
-
-HVAC,Average,Performance Curve Input Variable 3 Value []
-
-HVAC,Average,Performance Curve Input Variable 4 Value []
-
-HVAC,Average,Performance Curve Input Variable 5 Value []
-
-Group     Fluid Properties
-------------------------
-
-The Fluid Property routines in EnergyPlus have been designed for ease of use and to allow users to add refrigerant and glycol data to the input file without having to make any changes to the program code. Fluid properties are calculated by interpolating the tabulated data in the input file. The main input requirement is that in order to add a new fluid, a user must enter a full set of data. The user may determine the interval between data points according to the desired accuracy and range required. Data for a number of common fluids are available in the required format in a reference dataset so that the user may append this data to their input file. In addition, data for Water, Ethylene Glycol (in various concentrations from 0 to 90%), and Propylene Glycol (in various concentrations from 0 to 90%) are available as default values within EnergyPlus.
-
-Each fluid is categorized as either a    Refrigerant    or    Glycol   . Refrigerant data is further categorized as either saturated or superheated. Saturated refrigerant data is indexed, in the input data, according to pressure and temperature i.e. the specific heat, density, enthalpy in the input data are given for a given combination of pressure and temperature. Saturated refrigerant data is indexed according to pressure and quality. In the case of saturated pressure data only a temperature index is used. Glycol data is indexed in the input data according to temperature and concentration. The input data structure for each property is essentially two-dimensional (a matrix). However, since all fluid loops are assumed to be of constant concentration, EnergyPlus internally will interpolate from input data to data for the actual concentration being used in a particular loop. This reduces internally to a one-dimensional array of data for various properties where temperature is the only variable. This saves time since it reduces all interpolations for glycols to a single dimension.
-
-In most cases there will be combinations of index variable (e.g. some combination of pressure and temperature) at which either no data is available, or the property data is invalid/irrelevant. For example, in the superheated refrigerant data, some combinations of temperature and pressure may correspond to a state in the saturated rather than superheated region. Similarly, in the case of glycols there may be some combinations of temperature and concentration that would correspond to the frozen state. In these cases, and where data is just not available, a zero should be present in the data at these points to indicate an invalid condition. EnergyPlus uses the presence of zeros to detect invalid conditions and give warning messages.
-
-### FluidProperties:Name
-
-The names of each fluid for which property data is given in the user input have to be specified in FluidProperties:Name data objects. If data is to be included for a given fluid, either a refrigerant or a glycol, then its name must be included in the FluidProperties:Name objects.
-
-#### Field: Fluid Name
-
-Each fluid name is a unique identifier that will be used in conjunction with the data statements described later in this section. The fluid name is either referred to by a component (in the case of a Refrigerant) or by another input line (in the case of a Glycol). This list is simply a list of user defined fluids present in the input data file.
-
-#### Field: Fluid Type
-
-Each fluid name must be identified by type - either **Refrigerant** or **Glycol**. This designation determines what type of data EnergyPlus expects for the fluid name. If the fluid name is defined as a Refrigerant, the user must supply valid data for pressure, enthalpy, specific heat, and density in the saturated region and enthalpy and density in the superheated region. If the fluid name is defined as a Glycol, the user must supply valid data for specific heat, conductivity, viscosity, and density at various concentrations (percentage of non-water liquid) and temperatures.
-
-An example of these statements in an input data file is:
-
-```idf
-FluidProperties:Name,
-   R11,Refrigerant;
-
-
-FluidProperties:Name,
-   R12,Refrigerant;
-
-
-FluidProperties:Name,
-   R22,Refrigerant;
-
-
-FluidProperties:Name,
-   NH3,Refrigerant;
-
-
-FluidProperties:Name,
-   Steam,Refrigerant;
-
-
-FluidProperties:Name,
-  SaltBrine, Glycol;
-
-
-FluidProperties:Name,
-   NewGlycol, Glycol;
-```
-
-### FluidProperties:GlycolConcentration
-
-This input syntax is used to specify fluids that will be used with HVAC loops such as plant and condenser loops. It allows the user to define a mixture of water and some other substance and the particular concentration being used. The fluid name will be referred to by the loops or components and thus used to identify which value is valid for a particular fluid at a particular temperature. A series of three inputs is requires for each fluid concentration definition.
-
-#### Field: Name
-
-Each glycol concentration name is a unique identifier that will be used to define a particular combination of water and some other substance (usually another fluid). Other input (such as loop definitions) will refer to this name, linking the other input to the proper fluid definition.
-
-#### Field: Glycol Type
-
-This field refers to the substance that is being mixed with water to create the glycol. The user may either select from the two default fluids (**EthyleneGlycol** or **PropyleneGlycol**) or specify **UserDefinedGlycolType** and use a name in the subsequent field for fluids that have been entered elsewhere in the input file. It should be noted that users must enter a complete definition of new glycols  -including values for conductivity, specific heat, density, and viscosity at various concentrations and temperatures  -in order for them to be used in conjunction with a user defined glycol type.
-
-#### Field: User Defined Glycol Name
-
-This field is the name used elsewhere in a FluidProperties:Name object for defining your own glycol properties. This field is left blank unless you enter **UserDefinedGlycolType** in the previous field.
-
-#### Field: Glycol Concentration
-
-This field allows the user to specify the actual concentration of glycol being used for this particular fluid. A concentration of 0.0 refers to pure water. A concentration of 1.0 would denote 100% of the fluid referenced in the Glycol Name input discussed above. Users should enter this value as a decimal fraction since EnergyPlus will limit the range of valid input values to between 0.0 and 1.0.
-
-An example of this statement in an input data file is:
-
-```idf
-FluidProperties:GlycolConcentration,
-   EthGly25Percent, EthyleneGlycol, ,0.25;
-FluidProperties:GlycolConcentration,
-   ProGly40Percent, PropyleneGlycol, ,0.40;
-FluidProperties:GlycolConcentration,
-   HalfAndHalf, UserDefinedGlycolType, NewBrine, 0.5;
-```
-
-
-### FluidProperties:Temperatures
-
-It is assumed that all fluid properties vary with temperature. A common set of temperatures is required for each set of fluid property data. Fluid property data supplied by the user must correspondingly be given at these temperatures. Since in most cases, refrigerant data can be specified at a common set of temperatures, a single set of    FluidProperties:Temperatures    can be referenced by a number of sets of property data. This provides a more compact input structure and avoids listing the temperatures multiple times. In the case of glycol data the same set of temperatures have to be used for each set of data at a given concentration. Units for the temperatures are degrees Celsius.
-
-#### Field: Name
-
-This field is simply an unique identifier name that is used to cross reference the list of temperatures with a specific list of fluid property data. A single temperature list can be used for more than one thermal property or fluid. For example, the same temperature list can be used for the superheated enthalpy of a refrigerant and the specific heat of a glycol if appropriate.
-
-#### Field(s) 1-250: Temperature
-
-These fields (up to 250) are the temperatures at which the data for the thermal properties are to be expected. Temperatures are assumed to be in ascending order in units of Celsius.
-
-An example of this statement in an input data file is:
-
-```idf
-FluidProperties:Temperatures,
-           R11Temperatures,
-           -70,-65,-60,-55,-50,-45,-40,-35,-30,-25,-20,-15,-10,-5,0,2,4,6,8,10,12,
-           14,16,18,20,22,24,26,28,30,32,34,36,38,40,42,44,46,48,50,55,60,65,70,
-           75,80,85,90,95,100,105,110,115,120,125,130,135,140,145,150,155,160,
-           165,170,175,180,185,190,198;
-```
-
-
-### FluidProperties:Saturated
-
-Refrigerant property data for the saturated region is entered with the following syntax. For each set of property data a unique name, the type of property, phase and the corresponding list of temperatures have to be specified along with the property values.
-
-#### Field: Name
-
-This name identifies the fluid for which data follows in the remaining syntax. This fluid name must also be given in the fluid names list (ref: FluidProperties:Names object) as a **Refrigerant**.
-
-#### Field: Fluid Property Type
-
-This field identifies the fluid property for which data is being entered with this statement. The options for the saturated region are **Enthalpy, Density, SpecificHeat**, and **Pressure**. The units for these properties are J/kg, kg/m<sup>3</sup>, J/kg-K and Pa, respectively.
-
-#### Field: Fluid Phase
-
-In the saturated region, each property has two values: one for the saturated liquid state and one for the saturated gaseous state. Accordingly, the phase for which the saturated property data applies is specified as either **Fluid** or **FluidGas**. Data for each phase are required and are interpolated according to quality. However, in the case of saturated pressure data values for only one phase are required (i.e. can be specified with phase specified as either Fluid or FluidGas, as this is irrelevant).
-
-#### Field: Temperatures Values Name
-
-This name refers to the corresponding list of temperatures (ref: FluidProperties:Temperatures object). Each temperature in the temperature list corresponds to a data item found in the remaining fields of this syntax. The first temperature in the temperature list corresponds to the first fluid property value, the second temperature in the temperature list corresponds to the second fluid property value, etc.
-
-#### Field(s) 1-250: Property Value
-
-These fields (up to 250) are the values of the thermal property specified in the fluid property type field for the phase specified in the fluid phase field. The temperature list specified in the temperature list name field links the data with the corresponding temperatures.
-
-An example of this statement in an input data file is:
-
-```idf
-FluidProperties:Saturated,
-           R11,Enthalpy,Fluid,R11Temperatures, ! Enthalpy in J/kg
-           153580,154600,156310,158580,161300,164380,167740,171330,175100,179020,183060,
-           187190,191400,195680,200000,201740,203490,205240,207000,208770,210530,212310,
-           214080,215870,217650,219860,221230,223030,224830,226630,228860,230250,232060,
-           233860,235700,237520,239350,241180,243010,246350,249450,254080,258730,263480,
-           268110,272860,277000,282410,287240,292120,297030,302000,307090,312080,317210,
-           322400,327670,333020,338460,344010,349680,355500,361480,367690,374100,381060,
-           388850,397280,426300;
-```
-
-
-### FluidProperties:Superheated
-
-The format of the data for the superheated region is similar to that of the saturated region but with the addition of the pressure for which each set of property values applies. A single temperature specification is required for each set of property data at a number of pressures.
-
-#### Field: Fluid Name
-
-This name identifies the fluid for which data follows in the remaining syntax. This fluid name must show up in the fluid names list (ref: FluidProperties:Names object) as a **Refrigerant**.
-
-#### Field: Fluid Property Type
-
-This field identifies the fluid property for which data is being entered with this statement. The options for the superheated region are **Enthalpy** and **Density**. The units for these properties are J/kg and kg/m<sup>3</sup>, respectively.
-
-#### Field: Temperatures Values Name
-
-This name refers to the corresponding list of temperatures (ref: FluidProperties:Temperatures object). Each temperature in the temperature list corresponds to a given property data item at each pressure. The first temperature in the temperature list corresponds to the first fluid property value, the second temperature in the temperature list corresponds to the second fluid property value, etc.
-
-#### Field: Pressure
-
-In the superheated region, each fluid property is indexed according to temperature and pressure. Thus, a pressure must be listed for each set of property values. The units for pressure are Pascals (Pa). Lists of properties are various pressures and temperatures form a two-dimensional table from which EnergyPlus interpolates to find the property value at a specified temperature and pressure.
-
-#### Field(s) 1-250: Property Value
-
-These fields (up to 250) are the values of the thermal property specified in the fluid property type field for the phase specified in the fluid phase field. The temperature list specified in the temperature list name field links the data with the corresponding temperatures.
-
-An example of this statement in an input data file is:
-
-```idf
-FluidProperties:Superheated,
-       R11,Density,SuperR11Temperatures, ! Density in kg/m^3
-       62000., !Pressure = 62000Pa
-       0,0,0,0,0,0,0,0.0139,0.0134,0.0129,0.0124,0.012,0.0116,0.0112,0.0109,0.0105,
-       0.0102,0.0099,0.0097,0.0094,0.0092,0.0089,0,0,0,0,0,0,0,0,0,0;
-```
-
-
-### Glycol Fluid Types
-
-A full data set for a glycol fluid type in EnergyPlus includes: a temperature list and lists of values for specific heat at a given concentration. Data have to be given for at least two different concentrations. The syntax lines for the property value lists are described below.
-
-### FluidProperties:Concentration
-
-The format of the data for the glycols is similar to that of superheated refrigerants except that data at a number of concentrations is given, rather than pressures. The concentration is listed before the rest of the data and is normalized (i.e. in the range 0.0 to 1.0, rather than a percentage). Note that glycol solutions are assumed to exist in liquid form only in EnergyPlus.
-
-#### Field: Fluid Name
-
-This name identifies the fluid for which data follows in the remaining syntax. This fluid name must show up in the fluid names list (ref: FluidProperties:Names object) as a **Glycol**.. Note that users should not use Water, EthyleneGlycol, or PropyleneGlycol as names since these are default fluids.
-
-#### Field: Fluid Property Type
-
-This field identifies the fluid property for which data is being entered with this statement. The required data for glycols includes **SpecificHeat** with units of J/kg-K, **Density** with units of kg/m<sup>3</sup>, **Conductivity** with units of W/m-K, and **Viscosity** with units of N-s/m<sup>2</sup>.
-
-#### Field: Temperatures Values Name
-
-This name refers to the corresponding list of temperatures (ref: FluidProperties:Temperatures object). Each temperature in the temperature list corresponds to a data item found in the remaining fields of this syntax. The first temperature in the temperature list corresponds to the first fluid property value, the second temperature in the temperature list corresponds to the second fluid property value, etc.
-
-#### Field: Concentration
-
-A concentration must be listed for the values of specific heat that follow. Lists of properties are various concentrations and temperatures form a two-dimensional table from which EnergyPlus interpolates to find the property value at a specified temperature and concentration. Concentrations are specified in a normalized form (i.e. in the range 0.0 to 1.0, rather than a percentage)
-
-#### Field(s) 1-250: Property Value
-
-These fields (up to 250) are the values of the thermal property specified in the fluid property type field for the phase specified in the fluid phase field. The temperature list specified in the temperature list name field links the data with the corresponding temperatures.
-
-An example of this statement in an input data file is:
-
-```idf
-FluidProperties:Concentration,
-         NewGlycol,SpecificHeat ,GlycolTemperatures, ! Spec. heat in J/kg-K
-         0.8, ! Concentration
-         2572,2600,2627,2655,2683,2710,2738,2766,2793,2821,2849,2876,2904,2931,2959,
-         2987,3014,3042,3070,3097,3125,3153,3180,3208,3236,3263,3291,3319,3346,3374,
-         3402,3429,3457;
-```
-
-
diff --git a/doc/src/docs/InputOutputReference/02-HVACTemplates.md b/doc/src/docs/InputOutputReference/02-HVACTemplates.md
deleted file mode 100644
index aad41edcf94..00000000000
--- a/doc/src/docs/InputOutputReference/02-HVACTemplates.md
+++ /dev/null
@@ -1,7777 +0,0 @@
-HVAC Template Objects
-=====================
-
-HVACTemplate Processing
------------------------
-
-**Unlike other EnergyPlus objects, the HVACTemplate objects are not handled by EnergyPlus directly.** Instead, they are preprocessed by a program called ExpandObjects. If you use EP-Launch or RunEPlus.bat, this preprocessor step is performed automatically using the following sequence:
-
-1)   The preprocessor program, ExpandObjects, reads your IDF file and converts all of the HVACTemplate objects into other EnergyPlus objects.
-
-2)   The ExpandObjects program copies the original idf file with the HVACTemplate objects commented out (i.e., inserts a “!� in front of the object name and its input fields) plus all of the new objects created in Step 1 and writes a new file which is saved with the extension “expidf�. This “expidf� file may be used as a standard EnergyPlus IDF file if the extension is changed to idf; however, for safety’s sake, both filename and extension should be changed.
-
-3)   The EnergyPlus simulation proceeds using the expidf file as the input stream.
-
-4)   If there are error messages from EnergyPlus, they will refer to the contents of the expidf file. Specific objects referred to in error messages may exist in the original idf, but they may be objects created by ExpandObjects and only exist in the expidf. Remember that the expidf will be overwritten everytime the original idf is run using EP-Launch or RunEPlus.bat.
-
-If you are trying to go beyond the capabilities of the HVACTemplate objects, one strategy you can use is to start your specification using the HVACTemplate objects, run EnergyPlus using EP-Launch and producing an expidf file, rename that file and start making modifications. This approach may help with getting all of the objects needed and the node names set consistently.
-
-**Users need to remember that no objects related to HVAC except for HVAC template objects are needed in the IDF file.** The existence of other objects (unless specifically described in the following sections) may cause unexpected errors to occur. Sizing:Zone, Sizing:System, and Sizing:Plant objects will be generated by the corresponding HVACTemplate objects; the user does not need to create these elsewhere in the input file.
-
-There are some exceptions to this rule:
-
-- HVACTemplate:Plant:Chiller:ObjectReference which requires that the corresponding chiller object be present in the idf file along with any required curve or performance objects. In this case, the HVACTemplate object does not create the chiller object, but adds all of the connections. HVACTemplate:Plant:Tower:ObjectReference and HVACTemplate:Plant:Boiler;ObjectReferences are similar.
-
-- For HVACTemplate:Zone:\* objects, if Outdoor Air Method = *DetailedSpecification*, then any referenced DesignSpecification:OutdoorAir and DesignSpecification:ZoneAirDistribution objects must be present in the idf file.
-
-- For HVACTemplate:Zone:VAV and HVACTemplate:Zone:DualDuct, if a Design Specification Outdoor Air Object Name for Control is specified, then the referenced DesignSpecification:OutdoorAir object must be present in the idf file.
-
-
-
-
-
-Group -- HVAC Templates
------------------------
-
-This group of objects allows for the specification of simple zone thermostats and HVAC systems with automatically generated node names. The combinations of HVACTemplate objects are shown below.
-
-For a simple ideal loads system to use for sizing and loads oriented simulations:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:IdealLoadsAirSystem
-
-For baseboard heating systems with optional hot water boiler:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:BaseboardHeat
-
-* HVACTemplate:Plant:HotWaterLoop (optional)
-
-* HVACTemplate:Plant:Boiler (optional)
-
-For fan coil systems with boilers and chillers:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:FanCoil
-
-* HVACTemplate:Plant:ChilledWaterLoop
-
-* HVACTemplate:Plant:HotWaterLoop
-
-* HVACTemplate:Plant:Chiller
-
-* HVACTemplate:Plant:Boiler
-
-* HVACTemplate:Plant:Tower
-
-For packaged terminal air conditioner (PTAC) systems with optional hot water boiler:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:PTAC
-
-* HVACTemplate:Plant:HotWaterLoop (optional)
-
-* HVACTemplate:Plant:Boiler (optional)
-
-For packaged terminal air-to-air heat pump (PTHP) systems:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:PTHP
-
-For water to air heat pumps with boiler and cooling tower:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:WaterToAirHeatPump
-
-* HVACTemplate:Plant:MixedWaterLoop
-
-* HVACTemplate:Plant:Boiler
-
-* HVACTemplate:Plant:Tower
-
-For variable refrigerant flow heat pumps (air-to-air):
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:VRF
-
-* HVACTemplate:System:VRF
-
-For variable refrigerant flow heat pumps (water-to-air)with boiler and cooling tower:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:VRF
-
-* HVACTemplate:System:VRF
-
-* HVACTemplate:Plant:MixedWaterLoop
-
-* HVACTemplate:Plant:Boiler
-
-* HVACTemplate:Plant:Tower
-
-For direct-expansion cooling, packaged and split system simulations:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:Unitary
-
-* HVACTemplate:System:Unitary or
-
-* HVACTemplate:System:UnitarySystem
-
-For direct-expansion heat pump systems:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:Unitary
-
-* HVACTemplate:System:UnitaryHeatPump:AirToAir or
-
-* HVACTemplate:System:UnitarySystem
-
-For packaged variable air volume systems using direct-expansion cooling:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:VAV or
-
-* HVACTemplate:Zone:VAV:FanPowered or
-
-* HVACTemplate:Zone:VAV:HeatAndCool
-
-* HVACTemplate:System:PackagedVAV
-
-For variable air volume systems with boilers and air-cooled chillers:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:VAV or
-
-* HVACTemplate:Zone:VAV:FanPowered or
-
-* HVACTemplate:Zone:VAV:HeatAndCool
-
-* HVACTemplate:System:VAV
-
-* HVACTemplate:Plant:ChilledWaterLoop
-
-* HVACTemplate:Plant:HotWaterLoop
-
-* HVACTemplate:Plant:Chiller
-
-* HVACTemplate:Plant:Boiler
-
-For variable air volume systems with boilers and water-cooled chillers, an object related to towers is added:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:VAV or
-
-* HVACTemplate:Zone:VAV:FanPowered or
-
-* HVACTemplate:Zone:VAV:HeatAndCool
-
-* HVACTemplate:System:VAV
-
-* HVACTemplate:Plant:ChilledWaterLoop
-
-* HVACTemplate:Plant:HotWaterLoop
-
-* HVACTemplate:Plant:Chiller
-
-* HVACTemplate:Plant:Boiler
-
-* HVACTemplate:Plant:Tower
-
-For constant air volume systems with boilers and water-cooled chillers:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:ConstantVolume
-
-* HVACTemplate:System:ConstantVolume
-
-* HVACTemplate:Plant:ChilledWaterLoop
-
-* HVACTemplate:Plant:HotWaterLoop
-
-* HVACTemplate:Plant:Chiller
-
-* HVACTemplate:Plant:Boiler
-
-* HVACTemplate:Plant:Tower
-
-For dual-duct systems (constant or variable air volume) with boilers and water-cooled chillers:
-
-* HVACTemplate:Thermostat
-
-* HVACTemplate:Zone:DualDuct
-
-* HVACTemplate:System:DualDuct
-
-* HVACTemplate:Plant:ChilledWaterLoop
-
-* HVACTemplate:Plant:HotWaterLoop
-
-* HVACTemplate:Plant:Chiller
-
-* HVACTemplate:Plant:Boiler
-
-* HVACTemplate:Plant:Tower
-
-For dedicated outdoor air systems (DOAS) combined with a zonal template system:
-
-* HVACTemplate:System:DedicatedOutdoorAir
-
-* HVACTemplate:Thermostat
-
-One of the following for each zone served by the (DOAS) –
-
-* HVACTemplate:Zone:BaseboardHeat
-
-* HVACTemplate:Zone:PTAC
-
-* HVACTemplate:Zone:PTHP
-
-* HVACTemplate:Zone:FanCoil
-
-* HVACTemplate:Zone:WaterToAirHeatPump
-
-* HVACTemplate:Zone:VRF
-
-* HVACTemplate:Plant:\* objects as needed (depending on the type of zonal system and the type of coils specified in the DOAS system:WaterToAirHeatPump).
-
-The *only* other HVAC related objects besides the HVACTemplate objects that need to be specified related to HVAC systems are:
-
-- Schedule:Year or Schedule:Compact
-
-- SizingPeriod objects (one for heating and one for cooling) Note: all SizingPeriod objects can be used but for simplicity in the following descriptions, we will only reference SizingPeriod:DesignDay
-
-- SimulationControl
-
-- Sizing:Parameters
-
-This makes the input requirements much smaller but sacrifices some of the flexibility normally found in EnergyPlus.
-
-### HVACTemplate:Thermostat
-
-Each type of HVAC template zone object may reference one of these HVAC template thermostat objects. Multiple HVAC template zones can reference the same HVAC template thermostat object. The object allows the setpoints to be specified either as a constant for the entire simulation or as schedules. Referenced schedules must be defined elsewhere in the idf. Thermostat control type is dual setpoint with deadband. This object may be omitted and the user may define zone thermostat controls directly using standard EnergyPlus objects (ZoneControl:Thermostat and related objects).
-
-#### Field: Name
-
-A name used to reference this object. This name is referenced by HVACTemplate:Zone objects: i.e., HVACTemplate:Zone:IdealLoadsAirSystem, HVACTemplate:Zone:FanCoil, HVACTemplate:Zone:Unitary, HVACTemplate:Zone:VAV or HVACTemplate:Zone:VAV:FanPowered objects.
-
-#### Field: Heating Setpoint Schedule Name
-
-Enter the name of a heating setpoint schedule that has values that change at different times of the day or year. If a constant set point is needed simply leave this field blank and use the next field. The values in the schedule are in degrees C.
-
-#### Field: Constant Heating Setpoint
-
-Enter the heating setpoint temperature in degrees C if constant throughout the year. If the previous field is used this field should be left blank and will be ignored.
-
-#### Field: Cooling Setpoint Schedule Name
-
-Enter the name of a cooling setpoint schedule that has values that change at different times of the day or year. If a constant set point is needed simply leave this field blank and use the next field. The values in the schedule are in degrees C.
-
-#### Field: Constant Cooling Setpoint
-
-Enter the cooling setpoint temperature in degrees C if constant throughout the year. If the previous field is used this field should be left blank and will be ignored.
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:Thermostat,
-    Office Thermostat,     !- Thermostat Name
-    Htg-SetP-Sch,          !- Heating Setpoint Schedule
-    ,                      !- Constant Heating Setpoint {C}
-    Clg-SetP-Sch,          !- Cooling Setpoint Schedule
-    ;                      !- Constant Cooling Setpoint {C}
-```
-
-### HVACTemplate:Zone:IdealLoadsAirSystem
-
-This object provides an ideal system to supply conditioned air to the zone that meets all the load requirements and consumes no energy. It is often used for load calculations, an evaluation where the load components of the building are all that is being investigated, or as the first step to a more realistic model of a building.
-
-This component can be operated with infinite or finite heating and cooling capacity. For either mode – infinite or limited capacity – the user can also specify on/off schedules for heating and cooling and outdoor air controls. There are also optional controls for dehumidification, humidification, economizer, and heat recovery. This component may be used in combination with other HVAC equipment serving the same zone.
-
-This component can be thought of as an ideal unit that mixes air at the zone exhaust condition with the specified amount of outdoor air and then adds or removes heat and moisture at 100% efficiency in order to produce a supply air stream at the specified conditions. The energy required to condition the supply air is metered and reported as DistrictHeating and DistrictCooling.
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:IdealLoadsAirSystem objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. There are additional schedules fields for heating and cooling operation.
-
-#### Field: Maximum Heating Supply Air Temperature
-
-The maximum air temperature (degrees C) of the air used for heating the zone. The default is 50C (122F).
-
-#### Field: Minimum Cooling Supply Air Temperature
-
-The minimum air temperature (degrees C) of the air used for cooling the zone. The default is 13C (55.4F).
-
-#### Field: Maximum Heating Supply Air Humidity Ratio
-
-The maximum humidity ratio (kg of water per kg of dry air) of the hot supply air. The default is 0.0156 kgWater/kgDryAir which corresponds to a 20%RH at 50C (122F) dry bulb.
-
-#### Field: Minimum Cooling Supply Air Humidity Ratio
-
-The minimum humidity ratio (kg of water per kg of dry air) of the cool supply air. The default is 0.0077 kgWater/kgDryAir which corresponds to a 10C (50F) dew point.
-
-#### Field: Heating Limit
-
-The input must be either *LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity* or *NoLimit*. *LimitFlowRate* means that the heating supply air flow rate will be limited to the value specified in the next input field. *LimitCapacity* means that the sensible heating capacity will be limited to the value specified in the Maximum Sensible Heating Capacity field. *LimitFlowRateAndCapacity* means that both flow rate and capacity will be limited. *NoLimit* (the default) means that there will not be any limit on the heating supply air flow rate or capacity and the subsequent two fields will be ignored.
-
-#### Field: Maximum Heating Air Flow Rate
-
-The maximum heating supply air flow rate in cubic meters per second if heating limit is set to *LimitFlowRate or LimitFlowRateAndCapacity* *.* This field may be autosized. This field is ignored if heating limit is set to *NoLimit* or *LimitCapacity*.  If blank, there is no limit.
-
-#### Field: Maximum Sensible Heating Capacity
-
-The maximum allowed sensible heating capacity in Watts if Heating Limit is set to *LimitCapacity* or *LimitFlowRateAndCapacity*. This field may be autosized. If blank, there is no limit. If Heating Limit *is set to NoLimit* or *LimitFlowRate*, this field is ignored.
-
-#### Field: Cooling Limit
-
-The input must be either *LimitFlowRate, LimitCapacity, LimitFlowRateAndCapacity* or *NoLimit*. *LimitFlowrate* means that the cooling supply air flow rate will be limited to the value specified in the next input field. *LimitCapacity* means that the total cooling capacity will be limited to the value specified in the Maximum Total Cooling Capacity field. *LimitFlowRateAndCapacity* means that both flow rate and capacity will be limited. *NoLimit* (the default) means that there will not be any limit on the cooling supply air flow rate or capacity and the subsequent two fields will be ignored.
-
-#### Field: Maximum Cooling Air Flow Rate
-
-The maximum cooling supply air flow rate in cubic meters per second if Cooling Limit is set to *LimitFlowRate* or *LimitFlowRateAndCapacity.* This field may be autosized. This field is ignored if cooling limit is set to *NoLimit* or *LimitCapacity*. If blank, there is no limit. If *Cooling Limit is set to NoLimit,* this field is ignored*.* This field is required if Outdoor Air Control Type is *TemperatureEconomizer* in order to establish an upper limit on outdoor air flow when the economizer is active*.*
-
-#### Field: Maximum Total Cooling Capacity
-
-The maximum allowed total (sensible plus latent) cooling capacity in Watts if Cooling Limit is set to *LimitCapacity* or *LimitFlowRateAndCapacity*. This field may be autosized. If blank, there is no limit. If Cooling Limit *is set to NoLimit* or *LimitFlowRate,* this field is ignored*.*
-
-#### Field: Heating Availability Schedule Name
-
-The name of a schedule (ref: Schedule) that denotes whether heating is available. A schedule value greater than 0 (usually 1 is used) indicates that heating and humidification are available. A value less than or equal to 0 (usually 0 is used) denotes that heating and humidification are not available. If blank, heating and humidification are always available.
-
-#### Field: Cooling Availability Schedule Name
-
-The name of a schedule (ref: Schedule) that denotes whether cooling is available. A schedule value greater than 0 (usually 1 is used) indicates that cooling and dehumidification are available. A value less than or equal to 0 (usually 0 is used) denotes that cooling and dehumidification is not available. If blank, cooling and dehumidification are always available.
-
-#### Field: Dehumidification Control Type
-
-Select from *ConstantSensibleHeatRatio*, *Humidistat, None, or ConstantSupplyHumidityRatio*. *ConstantSensibleHeatRatio* (the default) means that the ideal loads system will be controlled to meet the sensible cooling load, and the latent cooling rate will be computed using a constant sensible heat ratio (SHR) (see next field). *Humidistat* means that there is a ZoneControl:Humidistat for this zone and the ideal loads system will attempt to meet the humidistat request (i.e. will dehumidify according to the Dehumidifying Relative Humidity Schedule in the ZoneControl:Humidistat object). *None* means that there is no dehumidification. *ConstantSupplyHumidityRatio* means that during cooling the supply air will always be at the Minimum Cooling Supply Humidity Ratio. For *ConstantSensibleHeatRatio* and *Humidistat*, if the mixed air humidity ratio is less than the target humidity ratio, then the mixed air humidity ratio will be used. For all options, the supply air humidity ratio will never be allowed to exceed saturation at the supply dry bulb temperature.
-
-The selected dehumidification control type is always applied when the unit is in cooling mode. If the unit is in deadband mode (not actively heating the supply air) control type *Humidistat* will be active. If the unit is in heating mode, control type *Humidistat* will be active if the Humidification Control Type field below is set to *Humidistat* or *None*.
-
-This allows the ideal loads system to heat and dehumidify at the same time.
-
-#### Field: Cooling Sensible Heat Ratio
-
-When the Dehumidification Control Type is set to *ConstantSensibleHeatRatio* the ideal loads system will be controlled to meet the sensible cooling load, and the latent cooling rate will be computed using the value of Cooling Sensible Heat Ratio (SHR), where SHR = Sensible Cooling divided by Total Cooling (sensible plus latent). The default is 0.7. If Dehumidification Control Type is set to something other than *ConstantSensibleHeatRatio* then this field will be ignored.
-
-#### Field: Dehumidification Setpoint
-
-This field specifies the zone humidistat relative humidity setpoint for dehumidification in percent (0 to 100).  The default is 60%. This field is used only when the Dehumidification Control Type = *Humidistat.*
-
-#### Field: Humidification Control Type
-
-Select from *None*, *Humidistat, or ConstantSupplyHumidityRatio*. *None* means that there is no humidification. *Humidistat* means that there is a ZoneControl:Humidistat for this zone and the ideal loads system will attempt to meet the humidistat request (i.e., humidify according to the Humidifying Relative Humidity Setpoint Schedule in the ZoneControl:Humidistat object). *ConstantSupplyHumidityRatio* means that during heating the supply air will always be at the Maximum Heating Supply Humidity Ratio. The default is *None*. For *Humidistat*, if the mixed air humidity ratio is greater than the target humidity ratio, then the mixed air humidity ratio will be used. For all options, the supply air humidity ratio will never be allowed to exceed saturation at the supply dry bulb temperature.
-
-The selected humidification control type is always applied when the unit is in heating mode. If the unit is in deadband mode (not actively heating the supply air) control type *Humidistat* will be active. If the unit is in cooling mode, control type *Humidistat* will be active if the Dehumidification Control Type field above is set to *Humidistat* or *None*.
-
-This allows the ideal loads system to cool and humidify at the same time.
-
-#### Field: Humidification Setpoint
-
-This field specifies the zone humidistat relative humidity setpoint for humidification in percent (0 to 100).  The default is 30%. This field is used only when the Humidification Control Type = *Humidistat.*
-
-#### Field: Outdoor Air Method
-
-The input must be either *None, Flow/Zone*, *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *None* means there is no outdoor air provided by this system. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *None.*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object referenced in the Design Specification Outdoor Air Object Name field below.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if Outdoor Air Method is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum.*
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if Outdoor Air Method is *Flow/Area, Sum* or *Maximum*. The default is 0.0.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if Outdoor Air Method is *Flow/Zone, Sum* or *Maximum*. The default is 0.0.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the outdoor air requirements and schedule for this system. The outdoor air flow rate may also be affected by the next two fields, Demand Controlled Ventilation Type and Outdoor Air Economizer Type. If this field is blank, this system will have no outdoor air, and all outdoor air control and heat recovery options will be ignored..
-
-#### Field: Demand Controlled Ventilation Type
-
-This field, along with the Design Specification Outdoor Air Object (if used) specifies how the minimum outdoor air flow rate is calculated. The choices are: *None, OccupancySchedule or CO2Setpoint*. The default is *None*.
-
-- None means that the design occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field).
-
-- OccupancySchedule means that the current occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field).
-
-- CO2Setpoint means that the design occupancy level will be used when computing the minimum outdoor air flow rate based on the inputs in the Design Specification Outdoor Air Object (see previous field). In addition, the minimum outdoor air flow rate may be increased if necessary to maintain the level of indoor air carbon dioxide at or below the setpoint defined in a ZoneControl:ContaminantController object (the user must add this to the idf file along with other related inputs).
-
-#### Field: Outdoor Air Economizer Type
-
-This field specifies if there is an outdoor air economizer. The choices are: *NoEconomizer, DifferentialDryBulb,* or *DifferentialEnthalpy*. The default is *NoEconomizer*. *DifferentialDryBulb* and *DifferentialEnthalpy* mean that the economizer will increase the outdoor air flow rate above the minimum outdoor air flow (see fields Design Specification Outdoor Air Object Name and Demand Controlled Ventilation Type) when there is a cooling load and the outdoor air temperature or enthalpy is below the zone exhaust air temperature or enthalpy. The *DifferentialDryBulb* and *DifferentialEnthalpy* options require that the Maximum Cooling Air Flow Rate be specified which will be used as the limit for maximum outdoor air flow rate.
-
-#### Field: Heat Recovery Type
-
-Select from *None*, *Sensible*, or *Enthalpy*. *None* means that there is no heat recovery. *Sensible* means that there is sensible heat recovery whenever the zone exhaust air temperature is more favorable than the outdoor air temperature. *Enthalpy* means that there is latent and sensible heat recovery whenever the zone exhaust air enthalpy is more favorable than the outdoor air enthalpy. The default is *None*.
-
-#### Field: Sensible Heat Recovery Effectiveness
-
-The sensible heat recovery effectiveness, where effectiveness is defined as the change in supply temperature divided by the difference in entering supply and relief air temperatures. The default is 0.70.
-
-#### Field: Latent Heat Recovery Effectiveness
-
-The latent heat recovery effectiveness, where effectiveness is defined as the change in supply humidity ratio divided by the difference in entering supply and relief air humidity ratios. The default is 0.65.
-
-
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:Zone:IdealLoadsAirSystem,
-    Zone 1,                  !- Zone Name
-    All Zones,               !- Thermostat Name
-    FanAvailSched,           !- System Availability Schedule Name
-    50,                      !- Maximum Heating Supply Air Temperature {C}
-    13,                      !- Minimum Cooling Supply Air Temperature {C}
-    0.0156,         !- Maximum Heating Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.0077,         !- Minimum Cooling Supply Air Humidity Ratio {kgWater/kgDryAir}
-    NoLimit,                 !- Heating Limit
-    ,                        !- Maximum Heating Air Flow Rate {m3/s}
-    ,                        !- Maximum Sensible Heating Capacity {W}
-    NoLimit,                 !- Cooling Limit
-    ,                        !- Maximum Cooling Air Flow Rate {m3/s}
-    ,                        !- Maximum Total Cooling Capacity {W}
-    ,                        !- Heating Availability Schedule Name
-    ,                        !- Cooling Availability Schedule Name
-    ConstantSensibleHeatRatio,  !- Dehumidification Control Type
-    0.7,                     !- Cooling Sensible Heat Ratio
-    60,                      !- Dehumidification Setpoint {percent}
-    None,                    !- Humidification Control Type
-    30,                      !- Humidification Setpoint {percent}
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    0.0,                     !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
-    ,                        !- Design Specification Outdoor Air Object Name
-    None,                    !- Demand Controlled Ventilation Type
-    NoEconomizer,            !- Outdoor Air Economizer Type
-    None,                    !- Heat Recovery Type
-    0.70,                    !- Sensible Heat Recovery Effectiveness
-    0.65;                    !- Latent Heat Recovery Effectiveness
-```
-
-
-### HVACTemplate:Zone:BaseboardHeat
-
-This object simulates a hot water or electric thermostatically controlled baseboard heating system. This object includes optional fields to combine the baseboard heat with a dedicated outdoor air system. If the zone is also served by another HVAC system, such as a PTAC or unitary air handler, then do not use this object. Instead, use the HVACTemplate:Zone:\* object for the forced air system and use the baseboard heating fields in that object.
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:IdealLoadsAirSystem objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that detailed thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating load will be multiplied by the number input in this field when the Baseboard Heating Capacity is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the type of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-The default choice is *HotWater*.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the fan coil system.  The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the fan coil system.
-
-#### Field: Dedicated Outdoor Air System Name
-
-Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the DOAS will provide ventilation air to the zone based on the outdoor air specifications in this object. If this field is blank, then the following outdoor air fields are ignored.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if Outdoor Air Method is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum.*
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if Outdoor Air Method is *Flow/Area, Sum* or *Maximum*. The default is 0.0.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if Outdoor Air Method is *Flow/Zone, Sum* or *Maximum*. The default is 0.0.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when Outdoor Air Method *= DetailedSpecification*.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when Outdoor Air Method *= DetailedSpecification*.
-
-
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:Zone:BaseboardHeat,
-    SPACE1-1,          !- Zone Name
-    All Zones,         !- Template Thermostat Name
-    ,                  !- Zone Heating Sizing Factor
-    HotWater,          !- Baseboard Heating Type
-    ,                  !- Baseboard Heating Availability Schedule Name
-    Autosize;          !- Baseboard Heating Capacity {W}
-    ,                  !- Dedicated Outdoor Air System Name
-    flow/person,       !- Outdoor Air Method
-    0.00944,           !- Outdoor Air Flow Rate per Person {m3/s}
-    0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    0.0,               !- Outdoor Air Flow Rate per Zone {m3/s}
-    ,                  !- Design Specification Outdoor Air Object Name
-    ;                  !- Design Specification Zone Air Distribution Object Name
-```
-
-
-### HVACTemplate:Zone:FanCoil
-
-This object simulates a 4 pipe fan coil unit with hot water heating coil, chilled water cooling coil, and an outdoor air mixer. The coils are served directly by HVACTemplate:Plant:ChilledWaterLoop and HVACTemplate:Plant:HotWaterLoop objects. No HVACTemplate:System object is required. Reference ZoneHVAC:FourPipeFanCoil for more details about the fan coil model.
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Supply Air Maximum Flow Rate
-
-By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. Note that the zone must have a thermostat specified in order to autosize the flow rate. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. Fan coil systems are modeled with continuous fan operation, so this is also the supply fan operating schedule. If this field is blank, the schedule has values of 1 for all time periods.
-
-#### Field: Supply Fan Total Efficiency
-
-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
-
-#### Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa.
-
-#### Field: Supply Fan Motor Efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Supply Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Cooling Coil Type
-
-There are two coil types available:
-
-- ChilledWater
-
-- ChilledWaterDetailedFlatModel
-
-*Chilled Water* uses theCoil:Cooling:Water object with the DetailedAnalysis option.  This is the preferred coil model for most applications.  *ChilledWaterDetailedFlatModel* uses the Coil:Cooling:Water:DetailedGeometry object.  This option is available for special applications.  The default is *ChilledWater*.
-
-#### Field: Cooling Coil Availability Schedule Name
-
-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of one indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
-
-#### Field: Cooling Coil Design Setpoint
-
-This is the design supply air temperature in C used to size the cooling supply air flow and the cooling coil. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 14<sup>o</sup>C.
-
-#### Field: Heating Coil Type
-
-Only one possible value may be entered here:
-
-- HotWater
-
-Future versions may have additional heating coil types.
-
-#### Field: Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period
-
-#### Field: Heating Coil Design Setpoint
-
-This is the design supply air temperature in C used to size the heating supply air flow and the heating coil. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50<sup>o</sup>C.
-
-#### Field: Dedicated Outdoor Air System Name
-
-Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the outdoor air flow rate for this zone equipment object will be set to zero and the DOAS will provide the ventilation air to the zone based on the outdoor air specifications in this object. For this fancoil system (ref. ZoneHVAC:FourPipeFanCoil):, the “Capacity Control Method� will be set to CyclingFan if a DOAS system is specified. If this field is blank, then the zone served by this fancoil system will not be served by a DOAS, and the fancoil Capacity Control Method will be ConstantFanVariableFlow.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Cooling Coil Design Setpoint will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Heating Coil Design Setpoint will be used for sizing the zone heating design air flow rate and the heating coil. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Fan Coil Capacity Control Method
-
-This input denotes how the unit’s output is controlled in order to meet zone heating or cooling requirement. The choices are *ConstantFanVariableFlow*, *CyclingFan*, *VariableFanVariableFlow* or *VariableFanConstantFlow*. For *ConstantFanVariableFlow*, the fan speed is held constant to produce a fixed air flow rate whenever the unit is scheduled on. The hot water or chilled flow rate is varied so that the unit output matches the zone heating or cooling requirement. For *CyclingFan*, the fan speed is chosen so that the unit capacity is greater than or equal to the heating / cooling load and the fan is cycled to match unit output with the load. For *VariableFanVariableFlow*  both air and water flow rates are varied to match the load. For *VariableFanConstantFlow,* the water flow rate is at full flow and the fan speed varies to meet the load. If this field is left blank, it will default to *CyclingFan* if a Dedicated Outdoor Air System is specified (see above), otherwise it will default to *ConstantFanVariableFlow.*
-
-#### Field: Low Speed Supply Air Flow Ratio
-
-This numerical field specifies the ratio of the low speed flow rate to the maximum supply air flow rate. Its value should be less than *Medium Speed Supply Air Flow Ratio.* If left blank, the default value is 0.33. This field is ignored if the capacity control method selected is not *CyclingFan*.
-
-#### Field: Medium Speed Supply Air Flow Ratio
-
-This numerical field specifies the ratio of the medium speed flow rate to the maximum supply air flow rate. Its value should be greater than the *Low Speed Supply Air Flow Ratio* but less than 1.If left blank, the default value is 0.66. This field is ignored if the capacity control method selected is not *CyclingFan*.
-
-#### Field: Outdoor Air Schedule Name
-
-#### The name of a schedule whose values (0.0 to 1.0) are used as multipliers to alter the outdoor air flow rate. If this field is left blank, the values will default to 1.0. This schedule is ignored if the zone is served by an HVACTemplate dedicated outdoor air system.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the fan coil system.  The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the fan coil system.
-
-
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:Zone:FanCoil,
-    SPACE1-1,                !- Zone Name
-    All Zones,               !- Template Thermostat Name
-    autosize,                !- Supply Air Maximum Flow Rate {m3/s}
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
-    FanAvailSched,           !- System Availability Schedule Name
-    0.7,                     !- Supply Fan Total Efficiency
-    75,                      !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    1,                       !- Supply Fan Motor in Air Stream Fraction
-    ChilledWater,            !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule Name
-    12.5,                    !- Cooling Coil Design Setpoint {C}
-    HotWater,                !- Heating Coil Type
-    ,                        !- Heating Coil Availability Schedule Name
-    50,                      !- Heating Coil Design Setpoint {C}
-    ,                        !- Dedicated Outdoor Air System Name
-    SupplyAirTemperature, !- Zone Cooling Design Supply Air Temperature Input Method
-    ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
-    SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
-    ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
-    ,            !- Design Specification Outdoor Air Object Name
-    ,            !- Design Specification Zone Air Distribution Object Name
-    ConstantFanVariableFlow, !- Fan Coil Capacity Control Method
-    ,                        !- Low Speed Supply Air Flow Ratio
-    ,                        !- Medium Speed Supply Air Flow Ratio
-    OUTAIRFANCOILSCHEDULE,   !- Outdoor Air Schedule Name
-    None,        !- Baseboard Heating Type
-    ,            !- Baseboard Heating Availability Schedule Name
-    Autosize;    !- Baseboard Heating Capacity {W}
-```
-
-
-### HVACTemplate:Zone:PTAC
-
-This object simulates a packaged terminal air conditioner (PTAC) with a DX cooling coil, a heating coil (electric, gas, or hot water), and an outdoor air mixer. The optional hot water heating coil is served directly by HVACTemplate:Plant:HotWaterLoop and HVACTemplate:Plant:Boiler objects. No HVACTemplate:System object is required. Reference ZoneHVAC:PackagedTerminalAirConditioner for more details about the PTAC model.
-
-![PTAC\_Drawthrough](media/image603.png)
-
-Figure 154.  Schematic of a packaged terminal air conditioner with draw through fan placement
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Cooling Supply Air Flow Rate
-
-This field specifies the supply air flow rate when the DX cooling coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: Heating Supply Air Flow Rate
-
-This field specifies the supply air flow rate when the heating coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: No Load Supply Air Flow Rate
-
-This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner’s supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).  By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will *not* be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers.The units are in m3/s. The default is autosize.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Heating Supply Air Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Cooling Supply Air Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. When the fan operating mode schedule indicates continuous fan operation, the fan will operate whenever this schedule is 1.0. If the fan operating schedule indicates cycling fan operation, then fan will only cycle on as needed to meet a load.
-
-#### Field: Supply Fan Operating Mode Schedule Name
-
-This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
-
-#### Field: Supply Fan Placement
-
-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *DrawThrough*.
-
-#### Field: Supply Fan Total Efficiency
-
-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
-
-#### Field: Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 75.
-
-#### Field: Supply Fan Motor Efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. The default is 0.9.
-
-#### Field: Cooling Coil Type
-
-Enter the type of cooling coil. There is currently only one choices for this field, SingleSpeedDX.
-
-#### Field: Cooling Coil Availability Schedule Name
-
-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
-
-#### Field: Cooling Coil Gross Rated Total Capacity
-
-Enter autosize to let the automatic sizing algorithm determine the cooling coil gross capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the “gross�, i.e., the effect of supply air fan heat is NOT accounted for. The units are in W. The default is autosize.
-
-#### Field: Cooling Coil Gross Rated Sensible Heat Ratio
-
-Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the rated capacity and air flow rate. Otherwise, enter the value of the ratio of the sensible capacity divided by total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be “gross�, i.e., the effect of supply air fan heat is not accounted for.  The default is autosize.
-
-#### Field: Cooling Coil Gross Rated Cooling COP
-
-Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 3.0.
-
-
-
-#### Field: Heating Coil Type
-
-Enter the type of heating coil. The choices for this field are
-
-- Electric
-
-- HotWater
-
-- Gas
-
-If HotWater is specified, then a HVACTemplate:Plant:HotWaterLoop and a HVACTemplate:Plant:Boiler must be included in the input file to serve this hot water coil. The default is Electric.
-
-#### Field: Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of 1.0 indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period
-
-#### Field: Heating Coil Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the coil can deliver in Watts. The default is autosize.
-
-#### Field: Gas Heating Coil Efficiency
-
-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default. This field applies only if the heating coil type is gas.
-
-#### Field: Gas Heating Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas heating coil operation, such as a combustion fan. The units are in W. This field applies only if the heating coil type is gas.
-
-#### Field: Dedicated Outdoor Air System Name
-
-Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the outdoor air flow rate for this zone equipment object (ref. ZoneHVAC: PackagedTerminalAirConditioner) will be set to zero and the DOAS will provide the ventilation air to the zone based on the outdoor air specifications in this object. If this field is blank, then the zone served by this PTAC system will not be served by a DOAS.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 14<sup>o</sup>C.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Heating Coil Design Setpoint will be used for sizing the zone heating design air flow rate and the heating coil. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50<sup>o</sup>C.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the PTAC system.  The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the PTAC system.
-
-
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:Zone:PTAC,
-    SPACE1-1,                !- Zone Name
-    All Zones,               !- Template Thermostat Name
-    autosize,                !- Cooling Supply Air Flow Rate {m3/s}
-    autosize,                !- Heating Supply Air Flow Rate {m3/s}
-    ,                        !- No Load Supply Air Flow Rate {m3/s}
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    ,                  !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    ,                        !- Outdoor Air Flow Rate per Zone {m3/s}
-    ,                        !- System Availability Schedule Name
-    ,                        !- Supply Fan Operating Mode Schedule Name
-    DrawThrough,             !- Supply Fan Placement
-    0.7,                     !- Supply Fan Total Efficiency
-    75,                      !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    SingleSpeedDX,           !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule Name
-    autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
-    autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
-    3,                       !- Cooling Coil Gross Rated COP
-    Electric,                !- Heating Coil Type
-    ,                        !- Heating Coil Availability Schedule Name
-    autosize,                !- Heating Coil Capacity {W}
-    0.8,                     !- Gas Heating Coil Efficiency
-    ,                        !- Gas Heating Coil Parasitic Electric Load {W}
-    ,                        !- Dedicated Outdoor Air System Name
- SupplyAirTemperature, !- Zone Cooling Design Supply Air Temperature Input Method
-    14.0,        !- Zone Cooling Design Supply Air Temperature {C]
-    ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
- SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
-    50.0,        !- Zone Heating Design Supply Air Temperature {C]
-    ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
-    ,            !- Design Specification Outdoor Air Object Name
-    ,            !- Design Specification Zone Air Distribution Object Name
-    None,        !- Baseboard Heating Type
-    ,            !- Baseboard Heating Availability Schedule Name
-    Autosize;    !- Baseboard Heating Capacity {W}
-```
-
-
-### HVACTemplate:Zone:PTHP
-
-This object simulates a packaged terminal air-to-air heat pump (PTHP) with a DX cooling coil, a DX air-to-air heat pump heating coil, a supplemental heating coil (electric or gas), and an outdoor air mixer. No HVACTemplate:System object is required. Reference ZoneHVAC:PackagedTerminalHeatPump for more details about the PTHP model.
-
-![PTPFigure](media/image604.png)
-
-Figure 155. Schematic of a packaged terminal heat pump (draw through fan placement)
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Cooling Supply Air Flow Rate
-
-This field specifies the supply air flow rate when the DX cooling coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: Heating Supply Air Flow Rate
-
-This field specifies the supply air flow rate when the heating coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: No Load Supply Air Flow Rate
-
-This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner’s supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).  By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will *not* be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Heating Supply Air Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Cooling Supply Air Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. When the fan operating mode schedule indicates continuous fan operation, the fan will operate whenever this schedule is 1.0. If the fan operating schedule indicates cycling fan operation, then fan will only cycle on as needed to meet a load.
-
-#### Field: Supply Fan Operating Mode Schedule Name
-
-This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
-
-#### Field: Supply Fan Placement
-
-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *DrawThrough*.
-
-#### Field: Supply Fan Total Efficiency
-
-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1.  The default is 0.7.
-
-#### Field: Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 75.
-
-#### Field: Supply Fan Motor Efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. The default is 0.9.
-
-#### Field: Cooling Coil Type
-
-Enter the type of cooling coil. There is currently only one choices for this field, SingleSspeedDX.
-
-#### Field: Cooling Coil Availability Schedule Name
-
-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
-
-#### Field: Cooling Coil Gross Rated Total Capacity
-
-Enter autosize to let the automatic sizing algorithm determine the gross cooling coil total capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the “gross�, i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize.
-
-#### Field: Cooling Coil Gross Rated Sensible Heat Ratio
-
-Enter Autosize to allow the sizing algorithm to determine the gross sensible heat ratio based on the gross rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by the gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be “gross�, i.e., the effect of supply air fan heat is not accounted for.  The default is autosize.
-
-#### Field: Cooling Coil Gross Rated COP
-
-Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The default is 3.0. The gross COP should not account for the supply air fan.
-
-#### Field: Heat Pump Heating Coil Type
-
-Enter the type of heat pump heating coil. There is currently only one choices for this field, SingleSpeedDXHeatPump.
-
-#### Field: Heat Pump Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the heat pump heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. A schedule value of 1.0 indicates that the heat pump heating coil can be on during a given time period. A value of zero denotes that the heat pump heating coil cannot be used during that time period.
-
-#### Field: Heat Pump Heating Coil Gross Rated Capacity
-
-Enter autosize to let the automatic sizing algorithm determine the heat pump heating coil gorss rated capacity based on the maximum heating loads during the heating design day. If a value is entered, it represents the full load gross heating capacity, in watts of the DX heat pump unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. Capacity should be the “gross�, i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize.
-
-#### Field: Heat Pump Heating Coil Gross Rated COP
-
-Enter the coefficient of performance defined as the gross heating coil capacity in watts divided by electrical power input in watts of the DX heating coil unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 2.75.
-
-#### Field: Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature
-
-This numeric field defines the minimum outdoor dry-bulb temperature in degrees Celsius for PTHP compressor operation. The compressor will not operate (for DX heating or DX cooling) when outdoor dry-bulb temperatures fall below this value. The minimum value must be greater than or equal to -20 °C. The default value is -8°C.
-
-#### Field: Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature
-
-This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 C and less than or equal to 7.22 C. If this input field is left blank, the default value is 5 C.
-
-#### Field: Heat Pump Defrost Strategy
-
-This alpha field has two choices: *ReverseCycle* or *Resistive*. If the *ReverseCycle* strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a *Resistive* defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is *ReverseCycle*.
-
-#### Field: Heat Pump Defrost Control
-
-This alpha field has two choices: *Timed* or *OnDemand*. If *Timed* control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For *Timed* defrost control, the fractional amount of time the unit is in defrost is entered in the input field “Defrost Time Period Fraction� described below. If *OnDemand* defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field “Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature� described above. If this input field is left blank, the default defrost control is *Timed*.
-
-#### Field: Heat Pump Defrost Time Period Fraction
-
-This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to “timed� defrost (see Heat Pump Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
-
-#### Field: Supplemental Heating Coil Type
-
-Enter the type of supplemental heating coil. The choices for this field are
-
-- Electric
-
-- Gas
-
-- HotWater
-
-The default is Electric.
-
-#### Field: Supplemental Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the supplemental heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when supplemental heating is only available seasonally. The schedule values denote whether the supplemental heating coil can run during a given time period. A schedule value of 1.0 indicates that the supplemental heating coil can be on during a given time period. A value of zero denotes that the supplemental heating coil cannot be used during that time period
-
-#### Field: Supplemental Heating Coil Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the supplemental heating coil can deliver in Watts. The default is autosize.
-
-#### Field: Supplemental Heating Coil Maximum Outdoor Dry-Bulb Temperature
-
-This numeric field defines the outdoor air dry-bulb temperature above which the supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
-
-#### Field: Supplemental Gas Heating Coil Efficiency
-
-Enter supplemental heating coil gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default. This field applies only if the supplemental heating coil type is gas.
-
-#### Field: Supplemental Gas Heating Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas supplemental heating coil operation, such as a combustion fan. The units are in W. The default is 0.0. This field applies only if the supplemental heating coil type is gas.
-
-#### Field: Dedicated Outdoor Air System Name
-
-Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the outdoor air flow rate for this zone equipment object (ref. ZoneHVAC:PackagedTerminalHeatPump) will be set to zero and the DOAS will provide the ventilation air to the zone based on the outdoor air specifications in this object. If this field is blank, then the zone served by this PTHP system will not be served by a DOAS.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 14<sup>o</sup>C.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Heating Coil Design Setpoint will be used for sizing the zone heating design air flow rate and the heating coil. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50<sup>o</sup>C.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the PTHP system.  The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the PTHP system.
-
-
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:Zone:PTHP,
-    SPACE1-1,                !- Zone Name
-    All Zones,               !- Template Thermostat Name
-    autosize,                !- Cooling Supply Air Flow Rate {m3/s}
-    autosize,                !- Heating Supply Air Flow Rate {m3/s}
-    ,                        !- No Load Supply Air Flow Rate {m3/s}
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    ,                  !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    ,                        !- Outdoor Air Flow Rate per Zone {m3/s}
-    ,                        !- System Availability Schedule Name
-    ,                        !- Supply Fan Operating Mode Schedule Name
-    DrawThrough,             !- Supply Fan Placement
-    0.7,                     !- Supply Fan Total Efficiency
-    75,                      !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    SingleSpeedDX,           !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule Name
-    autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
-    autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
-    3,                       !- Cooling Coil Gross Rated COP
-    SingleSpeedDXHeatPump,   !- Heat Pump Heating Coil Type
-    ,                    !- Heat Pump Heating Coil Availability Schedule Name
-    autosize,                !- Heat Pump Heating Coil Gross Rated Capacity {W}
-    2.75,                    !- Heat Pump Heating Coil Gross Rated COP
-    -8,         !- Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature {C}
-    5,          !- Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature {C}
-    ReverseCycle,            !- Heat Pump Defrost Strategy
-    Timed,                   !- Heat Pump Defrost Control
-    0.058333,                !- Heat Pump Defrost Time Period Fraction
-    Electric,                !- Supplemental Heating Coil Type
-    ,           !- Supplemental Heating Coil Availability Schedule Name
-    autosize,                !- Supplemental Heating Coil Capacity {W}
-    21,     !- Supplemental Heating Coil Max Outdoor Dry-Bulb Temperature {C}
-    0.8,                     !- Supplemental Gas Heating Coil Efficiency
-    ,          !- Supplemental Gas Heating Coil Parasitic Electric Load {W}
-    ,                        !- Dedicated Outdoor Air System Name
- SupplyAirTemperature, !- Zone Cooling Design Supply Air Temperature Input Method
-    14.0,        !- Zone Cooling Design Supply Air Temperature {C]
-    ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
- SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
-    50.0,        !- Zone Heating Design Supply Air Temperature {C]
-    ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
-    ,            !- Design Specification Outdoor Air Object Name
-    ,            !- Design Specification Zone Air Distribution Object Name
-    None,        !- Baseboard Heating Type
-    ,            !- Baseboard Heating Availability Schedule Name
-    Autosize;    !- Baseboard Heating Capacity {W}
-```
-
-
-### HVACTemplate:Zone:WaterToAirHeatPump
-
-This object simulates the zone portion of a water source heat pump system. Often many HVACTemplate:Zone:WaterToAirHeatPump objects will be used in a building along with a single HVACTemplate:Plant:MixedWaterLoop that contains a cooling tower and boiler.
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Cooling Supply Air Flow Rate
-
-This field specifies the supply air flow rate when the unit is operating in cooling mode. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: Heating Supply Air Flow Rate
-
-This field specifies the supply air flow rate when the unit is operating in heating mode. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: No Load Supply Air Flow Rate
-
-This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., the coil is off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).  . By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will *not* be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Heating Supply Air Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Cooling Supply Air Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. When the fan operating mode schedule indicates continuous fan operation, the fan will operate whenever this schedule is 1.0. If the fan operating schedule indicates cycling fan operation, then fan will only cycle on as needed to meet a load.
-
-#### Field: Supply Fan Operating Mode Schedule Name
-
-This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
-
-#### Field: Supply Fan Placement
-
-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *DrawThrough*.
-
-#### Field: Supply Fan Total Efficiency
-
-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1.  The default is 0.7.
-
-#### Field: Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 75.
-
-#### Field: Supply Fan Motor Efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. The default is 0.9.
-
-#### Field: Cooling Coil Type
-
-Enter the type of cooling coil. There is currently only one choices for this field, Coil:Cooling:WaterToAirHeatPump:EquationFit.
-
-#### Field: Cooling Coil Gross Rated Total Capacity
-
-Enter autosize to let the automatic sizing algorithm determine the cooling coil gross rated total capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions (26.7C (80F) entering air dry-bulb temperature, 19.4C (67F) entering air wet-bulb temperature, and 29.4C (85F) entering water temperature). Capacity should be the “gross�, i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize. If a value is specified for this field, it is recommended that the Cooling Coil Rated Sensible Heat Ratio also be specified (see below for more details).
-
-#### Field: Cooling Coil Gross Rated Sensible Heat Ratio
-
-Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by gross total cooling capacity of the DX cooling coil at rated conditions (26.7C (80F) entering air dry-bulb temperature, 19.4C (67F) entering air wet-bulb temperature, and 29.4C (85F) entering water temperature). Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be “gross� , i.e., the effect of supply air fan heat is not accounted for.  The default is autosize. If the Cooling Coil Rated Capacity is autosized, this field should also be autosized (any value specified for Cooling Coil Rate Sensibe Heat Ratio will be ignored). If the Cooling Coil Rated Capacity has a specified value, then this field should also have a specified value. This is because the Coil:Cooling:WaterToAirHeatPump:EquationFit object has fields for Rated Total Cooling Capacity and Rated Sensible Cooling Capacity. If this field is autosized, a specified value for Cooling Coil Rated Capacity will not be used when the coil object sensible capacity is autosized.
-
-#### Field: Cooling Coil Gross Rated COP
-
-Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions (26.7C (80F) entering air dry-bulb temperature, 19.4C (67F) entering air wet-bulb temperature, and 29.4C (85F) entering water temperature). The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 3.5.
-
-#### Field: Heat Pump Heating Coil Type
-
-Enter the type of heat pump heating coil. There is currently only one choices for this field, Coil:Heating:WaterToAirHeatPump:EquationFit.
-
-#### Field: Heat Pump Heating Coil Gross Rated Capacity
-
-Enter autosize to let the automatic sizing algorithm determine the heat pump heating coil gross capacity based on the maximum heating loads during the heating design day. If a value is entered, it represents the full load heating capacity, in watts of the DX heat pump unit at rated conditions (21.11C (70F) entering air dry-bulb temperature and 21.11C (70F) entering water temperature). Capacity should be the “gross�, i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize.
-
-#### Field: Heat Pump Heating Coil Gross Rated COP
-
-Enter the coefficient of performance defined as the gross heating coil capacity in watts divided by electrical power input in watts of the DX heating coil unit at rated conditions (21.11C (70F) entering air dry-bulb temperature and 21.11C (70F) entering water temperature). The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 4.2.
-
-#### Field: Supplemental Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when supplemental heating is only available seasonally. The schedule values denote whether the supplemental heating coil can run during a given time period. A schedule value of 1.0 indicates that the supplemental heating coil can be on during a given time period. A value of zero denotes that the supplemental heating coil cannot be used during that time period
-
-#### Field: Supplemental Heating Coil Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the supplemental heating coil can deliver in Watts. The default is autosize.
-
-#### Field: Maximum Cycling Rate
-
-This numeric field contains the maximum on-off cycling rate for the compressor, which occurs at 50% run time fraction. Suggested values are shown below (Henderson et al. 1999):
-
-![](media/image605.svg)
-
-#### Field: Heat Pump Time Constant
-
-This numeric field contains the time constant for the cooling coil's capacity to reach steady state after startup. Suggested values are shown below (Henderson et al. 1999):
-
-![](media/image606.svg)
-
-#### Field: Fraction of On-Cycle Power Use
-
-This numeric field contains the fraction of on-cycle power use to adjust the part load fraction based on the off-cycle power consumption due to crankcase heaters, controls, fans, and etc. Suggested value values are below (Henderson et al. 1999):
-
-![](media/image607.svg)
-
-#### Field: Heat Pump Fan Delay Time
-
-This numeric field contains the time delay in seconds for the heat pump supply air fan to shut off after compressor cycle off. This value can be obtained from the manufacturer or the heat pump catalog. Suggested value is 60 seconds. This value is disregared at times when the WaterToAirHeatPump’s fan operating mode schedule value is greater than 0 (i.e., continuous fan mode).
-
-#### Field: Dedicated Outdoor Air System Name
-
-Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the outdoor air flow rate for this zone equipment object (ref. ZoneHVAC:WaterToAirHeatPump) will be set to zero and the DOAS will provide the ventilation air to the zone based on the outdoor air specifications in this object. If this field is blank, then the zone served by this water-to-air heat pump system will not be served by a DOAS.
-
-#### Field: Supplemental Heating Coil Type
-
-Enter the type of supplemental heating coil. The choices for this field are
-
-- Electric
-
-- HotWater
-
-The default is Electric.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 14<sup>o</sup>C.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Heating Coil Design Setpoint will be used for sizing the zone heating design air flow rate and the heating coil. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50<sup>o</sup>C.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-#### Field: Heat Pump Coil Water Flow Mode
-
-This field specifies the way in which water flow through the heat pump coils will be modeled.  For this template, WatertoAirHeatPump:EquationFit coil objects are generated and, therefore, there are three options:
-
-- Cycling
-
-- Constant
-
-- ConstantOnDemand
-
-**Cycling** varies water flow through the coil based on the heat pump Part Load Ratio.  This control method is appropriate for modeling heat pumps that are outfitted with a soleniod valve which allows water to flow through the coil only when the compressor is active. This is the **default** for EnergyPlus V8 and later.
-
-**Constant** provides a constant water flow regardless of heat pump operation.  Remember that EnergyPlus has two coils (a heating coil and a cooling coil) to approximate the operation of one coil that can operate in either heating mode or cooling mode.  Therefore, when the water flow mode is constant, there will be full flow through either the heating coil or the cooling coil, but not both at the same time.
-
-**ConstantOnDemand** provides full flow through the coil whenever there is a load.  When there is no load, there is zero flow through the coil.  This control strategy represents the way EnergyPlus modeled heat pump water flow prior to Version 8.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the heat pump system.  The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the heat pump system.
-
-
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:Zone:WaterToAirHeatPump,
-    SPACE1-1,                !- Zone Name
-    All Zones,               !- Template Thermostat Name
-    autosize,                !- Cooling Supply Air Flow Rate {m3/s}
-    autosize,                !- Heating Supply Air Flow Rate {m3/s}
-    ,                        !- No Load Supply Air Flow Rate {m3/s}
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-    Flow/Person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    ,                !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    ,                        !- Outdoor Air Flow Rate per Zone {m3/s}
-    ,                        !- System Availability Schedule Name
-    ,                        !- Supply Fan Operating Mode Schedule Name
-    DrawThrough,             !- Supply Fan Placement
-    0.7,                     !- Supply Fan Total Efficiency
-    75,                      !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    Coil:Cooling:WaterToAirHeatPump:EquationFit,  !- Cooling Coil Type
-    autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
-    autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
-    3,                       !- Cooling Coil Gross Rated COP
-    Coil:Heating:WaterToAirHeatPump:EquationFit,  !- HPump Heating Coil Type
-    autosize,                !- Heat Pump Heating Coil Gross Rated Capacity {W}
-    2.75,                    !- Heat Pump Heating Coil Gross Rated COP
-    ,                !- Supplemental Heating Coil Availability Schedule Name
-    autosize,                !- Supplemental Heating Coil Capacity {W}
-    2.5,                     !- Maximum Cycling Rate {cycles/hr}
-    60,                      !- Heat Pump Time Constant {s}
-    0.01,                    !- Fraction of On-Cycle Power Use
-    60,                      !- Heat Pump Fan Delay Time {s}
-    ,                        !- Dedicated Outdoor Air System Name
-    Electric,                !- Supplemental Heating Coil Type
- SupplyAirTemperature, !- Zone Cooling Design Supply Air Temperature Input Method
-    14.0,        !- Zone Cooling Design Supply Air Temperature {C]
-    ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
- SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
-    50.0,        !- Zone Heating Design Supply Air Temperature {C]
-    ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
-    ,            !- Design Specification Outdoor Air Object Name
-                 !- Design Specification Zone Air Distribution Object Name
-```
-
-
-### HVACTemplate:Zone:VRF
-
-This object simulates a variable refrigerant flow (VRF) zone terminal unit which is served by an HVACTemplate:System:VRF condenser unit. Reference ZoneHVAC:TerminalUnit:VariableRefrigerantFlow for more details about the VRF terminal unit model.
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Heating Supply Air Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Cooling Supply Air Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Rated Total Heating Capacity Sizing Ratio
-
-This numeric field defines the ratio of the heating coil to cooling coil size when autosizing is used. The model assumes that when used, this value will be greater than 1. This field supersedes the Rated Total Heating Capacity Sizing Ratio entered in the AirConditioner:VariableRefrigerantFlow object. If this field is left blank, the value entered in the parent object is used for sizing. If neither field is used, the sizing ratio is assumed to be 1.
-
-#### Field: Cooling Supply Air Flow Rate
-
-This field specifies the supply air flow rate when the terminal unit is operating in cooling mode. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: No Cooling Supply Air Flow Rate
-
-This field specifies the supply air flow rate when the terminal unit’s cooling coil is not operating and the previous mode was cooling.. This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner’s supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).  By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will *not* be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: Heating Supply Air Flow Rate
-
-This field specifies the supply air flow rate when the heating coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: No Heating Supply Air Flow Rate
-
-This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner’s supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).  By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will *not* be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is autosize.
-
-#### Field: Cooling Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in cooling mode.        If this field is set to autosize it will be sized based on the outdoor air inputs below, unless a dedicated outdoor air system is specified for this zone and then it will be set to zero.
-
-#### Field: Heating Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is operating in heating mode. If this field is set to autosize it will be sized based on the outdoor air inputs below, unless a dedicated outdoor air system is specified for this zone and then it will be set to zero.
-
-#### Field: No Load Outdoor Air Flow Rate
-
-This numeric field defines the outdoor air volumetric air flow rate in cubic meters per second. This volumetric air flow rate is used when the terminal unit is not operating in cooling or heating mode. If this field is set to autosize it will be sized based on the outdoor air inputs below, unless a dedicated outdoor air system is specified for this zone and then it will be set to zero.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. When the fan operating mode schedule indicates continuous fan operation, the fan will operate whenever this schedule is 1.0. If the fan operating schedule indicates cycling fan operation, then fan will only cycle on as needed to meet a load.
-
-#### Field: Supply Fan Operating Mode Schedule Name
-
-This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load. If this field is left blank, a schedule of always zero (cycling fan) will be used.
-
-#### Field: Supply Fan Placement
-
-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *DrawThrough*.
-
-#### Field: Supply Fan Total Efficiency
-
-Enter the total efficiency of the supply fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1. The default is 0.7.
-
-#### Field: Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 75.
-
-#### Field: Supply Fan Motor Efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. The default is 0.9.
-
-#### Field: Cooling Coil Type
-
-Enter the type of cooling coil. The options are *VariableRefrigerantFlowDX* or None. The default is *VariableRefrigerantFlowDX*.
-
-#### Field: Cooling Coil Availability Schedule Name
-
-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
-
-#### Field: Cooling Coil Gross Rated Total Capacity
-
-Enter autosize to let the automatic sizing algorithm determine the gross cooling coil total capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the “gross�, i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize.
-
-#### Field: Cooling Coil Gross Rated Sensible Heat Ratio
-
-Enter Autosize to allow the sizing algorithm to determine the gross sensible heat ratio based on the gross rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by the gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be “gross�, i.e., the effect of supply air fan heat is not accounted for.  The default is autosize.
-
-#### Field: Heat Pump Heating Coil Type
-
-Enter the type of heat pump heating coil. The options are *VariableRefrigerantFlowDX* or None. The default is *VariableRefrigerantFlowDX*.
-
-#### Field: Heat Pump Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the heat pump heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. A schedule value of 1.0 indicates that the heat pump heating coil can be on during a given time period. A value of zero denotes that the heat pump heating coil cannot be used during that time period.
-
-#### Field: Heat Pump Heating Coil Gross Rated Capacity
-
-Enter autosize to let the automatic sizing algorithm determine the heat pump heating coil gorss rated capacity based on the maximum heating loads during the heating design day. If a value is entered, it represents the full load gross heating capacity, in watts of the DX heat pump unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. Capacity should be the “gross�, i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is autosize.
-
-#### Field: Zone Terminal Unit On Parasitic Electric Energy Use
-
-This numeric field defines the parasitic electrical energy use of the zone terminal unit when either terminal unit coil is operating. When in cooling mode, this electric energy use is reported in a zone terminal unit cooling electric consumption output variable. When in heating mode, this electric energy use is reported in a zone terminal unit heating electric consumption output variable.
-
-#### Field: Zone Terminal Unit Off Parasitic Electric Energy Use
-
-This numeric field defines the parasitic electrical energy use of the zone terminal unit when the terminal unit coil(s) is not operating. When the previous mode was cooling, this electric energy use is reported in a zone terminal unit cooling electric consumption output variable. When the previous mode was heating, this electric energy use is reported in a zone terminal unit heating electric consumption output variable.
-
-#### Field: Dedicated Outdoor Air System Name
-
-Enter the name of an HVACTemplate:System:DedicatedOutdoorAir object if this zone is served by a dedicated outdoor air system (DOAS). When a Dedicated Outdoor Air System Name is entered, the outdoor air flow rate for this zone equipment object (ref. ZoneHVAC: TerminalUnit:VariableRefrigerantFlow) will be set to zero and the DOAS will provide the ventilation air to the zone based on the outdoor air specifications in this object. If this field is blank, then the zone served by this VRF terminal unit will not be served by a DOAS.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 14<sup>o</sup>C.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Heating Coil Design Setpoint will be used for sizing the zone heating design air flow rate and the heating coil. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50<sup>o</sup>C.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the PTHP system.  The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the PTHP system.
-
-
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:Zone:VRF,
-    SPACE1-1,                !- Zone Name
-    All Zones,               !- Template Thermostat Name
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-    ,                        !- Rated Total Heating Capacity Sizing Ratio
-    autosize,                !- Cooling Supply Air Flow Rate{m3/s}
-    autosize,                !- No Cooling Supply Air Flow Rate{m3/s}
-    autosize,                !- Heating Supply Air Flow Rate{m3/s}
-    autosize,                !- No Heating Supply Air Flow Rate{m3/s}
-    autosize,                !- Cooling Outdoor Air Flow Rate{m3/s}
-    autosize,                !- Heating Outdoor Air Flow Rate{m3/s}
-    autosize,                !- No Load Outdoor Air Flow Rate{m3/s}
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    ,            !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    ,                        !- Outdoor Air Flow Rate per Zone {m3/s}
-    ,            !- Design Specification Outdoor Air Object Name
-    ,            !- Design Specification Zone Air Distribution Object Name
-    ,                        !- System Availability Schedule Name
-    ,                        !- Supply Fan Operating Mode Schedule Name
-    DrawThrough,             !- Supply Fan Placement
-    0.7,                     !- Supply Fan Total Efficiency
-    75,                      !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    VariableRefrigerantFlowDX,  !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule Name
-    autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
-    autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
-    VariableRefrigerantFlowDX,  !- Heat Pump Heating Coil Type
-    ,                        !- Heat Pump Heating Coil Availability Schedule Name
-    autosize,                !- Heat Pump Heating Coil Gross Rated Capacity {W}
-    0,           !- Zone Terminal Unit On Parasitic Electric Energy Use {W}
-    0,           !- Zone Terminal Unit Off Parasitic Electric Energy Use {W}
-    ,                        !- Dedicated Outdoor Air System Name
- SupplyAirTemperature, !- Zone Cooling Design Supply Air Temperature Input Method
-    14.0,        !- Zone Cooling Design Supply Air Temperature {C}
-    ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
- SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
-    50.0,        !- Zone Heating Design Supply Air Temperature {C}
-    ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    None,        !- Baseboard Heating Type
-    ,            !- Baseboard Heating Availability Schedule Name
-    Autosize;    !- Baseboard Heating Capacity {W}
-```
-
-### HVACTemplate:Zone:Unitary
-
-This object simulates the zone portion of a constant volume direct-expansion based HVAC configuration with several different heating options. Often a single HVACTemplate:Zone:Unitary object will be used with a single HVACTemplate:System:Unitary (or HVACTemplate:System:UnitaryHeatPump:AirToAir , or HVACTemplate:System:UnitarySystem) object to simulate single zone direct-expansion based air conditioning systems. In addition, multiple HVACTemplate:Zone:Unitary objects may appear that all reference the same HVACTemplate:System object in a multiple zone version. For a multizone system, only one zone is specified as the control zone (see HVACTemplate:System:Unitary, HVACTemplate:System:UnitaryHeatPump:AirToAir , or HVACTemplate:System:UnitarySystem for more information). Direct expansion includes single packaged rooftop systems commonly seen in commercial applications and split systems commonly seen in residential applications.
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template Unitary System Name
-
-Enter the name of the HVACTemplate:System:Unitary, HVACTemplate:System:UnitaryHeatPump:AirToAir , or HVACTemplate:System:UnitarySystem object serving this zone.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Supply Air Maximum Flow Rate
-
-By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. Note that the zone must have a thermostat specified in order to autosize the flow rate, even if it is not the control zone in a multiple zone unitary system. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The template unitary system object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
-
-If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: Supply Plenum Name
-
-This field allows the user to specify a supply plenum which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Return Plenum Name
-
-This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the unitary air handling system.  The baseboard heating will be set to heating priority 2, which means it will meet any remaining heating load not met by the unitary system. Prior to v7.1, the capacity was only applied to electric baseboard. Starting with v7.1, the capacity will be used for both hot water and electric baseboard.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. *SystemSupplyAirTemperature* means that the Cooling Design Supply Air Temperature from the template unitary system serving this zone will be used. The default is *SystemSupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 12.8°C.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Zone Heating Design Supply Air Temperature  will be used for sizing the zone heating design air flow rate. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. *SystemSupplyAirTemperature* means that the Heating Design Supply Air Temperature from the template unitary system serving this zone will be used. The default is *SystemSupplyAirTemperature.*
-
-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50°C.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:Zone:Unitary,
-    SPACE1-1,                !- Zone Name
-    Furnace DX 1-1,          !- Template Unitary System Name
-    All Zones,               !- Template Thermostat Name
-    autosize,                !- Supply Air Maximum Flow Rate {m3/s}
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
-    ,                        !- Supply Plenum Name
-    ,                        !- Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule Name
-    Autosize,                !- Baseboard Heating Capacity {W}
- SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
-    ,            !- Zone Cooling Design Supply Air Temperature {C]
-    ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
- SystemSupplyAirTemperature, !- Zone Heating Design Supply Air . . . Input Method
-    ,            !- Zone Heating Design Supply Air Temperature {C]
-    ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
-    ,            !- Design Specification Outdoor Air Object Name
-    ;            !- Design Specification Zone Air Distribution Object Name
-```
-
-
-### HVACTemplate:Zone:VAV
-
-This object simulates the zone portion of a variable air volume HVAC configuration with several different heating options. When heating is required, this terminal unit will activate the reheat coil first, and then increase airflow if reverse action is specified. Multiple HVACTemplate:Zone:VAV, HVACTemplate:Zone:VAV:FanPowered or HVACTemplate:Zone:VAV:HeatAndCool objects are usually specified for each HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object. Reheat is specified at the zone level. Reference AirTerminal:SingleDuct:VAV:Reheat and AirTerminal:SingleDuct:VAV:NoReheat for more details about VAV terminal units.
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template VAV System Name
-
-Enter the name of the HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object serving this zone.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Supply Air Maximum Flow Rate
-
-By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Minimum Air Flow Method
-
-This field is used to select how the program will determine the minimum flow rate to the zone while the system is operating.  There are three choices for selecting how the minimum flow rate is specified:  Constant, FixedFlowRate, and Scheduled.  If Constant is entered, then the program will use the value for the constant minimum air flow fraction entered in the following field.  If FixedFlowRate is entered, then the program will use the value entered in the field below called Fixed Minimum Air Flow Rate.If Scheduled is entered, then the program will obtain the value for minimum flow fraction from the schedule named in the field below called Minimum Air Flow Fraction Schedule Name.
-
-#### Field: Constant Minimum Air Flow Fraction
-
-The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default).  This field is used if the previous field is set to Constant.  If the previous field is set to Scheduled (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then this field is optional and can be used to separately control the air flow rate used for sizing normal-action reheat coils. If this field and the following field have values, the greater of the two is used for sizing.
-
-#### Field: Fixed Minimum Air Flow Rate
-
-The minimum flow rate to the zone while the system is operating, specified as a fixed minimum air flow rate in meters cubed per second. The minimum air flow rate is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default).  This field is used if the Zone Minimum Air Flow Method field is set to FixedFlowRate. If the Zone Minimum Air Flow Method field is set to Scheduled (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then this field is optional and can be used to separately control the air flow rate used for sizing normal-action reheat coils. Only one of these two minimum air flow fields (i.e., this field and the previous field) should be used at any time. If this field and the previous field have values, the greater of the two is used for sizing.
-
-#### Field: Minimum Air Flow Fraction Schedule Name
-
-The name of a schedule that determines the value of the minimum air flow fraction.  The schedule should contain fractions from 0.0 to 1.0.  These values will define the minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate.  The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default).  This field is used if the previous field is set to Scheduled.  If the previous field is left blank (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then the air flow rate usedfor sizing normal-action reheat coils is the average of the minimum and maximum values in this schedule.  The air flow rate used for reheat coil sizing is reported with other component sizing information as “Reheat Coil Sizing Air Volume Flow Rate.�
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name for Sizing and Design Specification Zone Air Distribution Object Name fields below.
-
-If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: Reheat Coil Type
-
-A reheat coil may be added to the VAV box with this field. The choices are:
-
-- HotWater
-
-- Electric
-
-- Gas
-
-- None
-
-The default choice is None.
-
-#### Field: Reheat Coil Availability Schedule Name
-
-Leave this field blank if you want the reheat coil to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the coil is available should be specified as 1.0. Those times that the coil is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the coil is providing heat but a schedule of when it can provide heat.
-
-#### Field: Damper Heating Action
-
-The VAV box flow rate can be controlled in one of two ways during heating operation:
-
-- Normal
-
-- Reverse
-
-Under “Normal� operation, the supply air flow into the zone is the minimum air flow rate of the VAV system during heating, essentially acting like a constant volume system during heating. Under “Reverse� the air flow rate through the VAV box may increase above the minimum air flow when the heating demand cannot be satisfied unless greater air flow is provided. The default value is Normal. Reverse action only applies when Reheat Coil Type is HotWater. For electric reheat coils, Normal and Reverse behave the same. For more details, please see the section for AirTerminal:SingleDuct:VAV:Reheat.
-
-#### Control Fields for Maximum Flow During Reheat:
-
-The following two fields are used only when Reheat Coil Object Type = Coil:Heating:Water and Damper Heating Action = Reverse. Maximum Flow per Zone Floor Area During Reheat and Maximum Flow Fraction During Reheat are two optional methods to calculate the maximum allowable air flow rate during reheat operation. If both are entered, the greater resulting flow rate is used. If Design Specification Outdoor Air Object Name is also specified, it may increase this limit to meet the outdoor air flow rate requirement. At no time will the maximum flow rate calculated here exceed the value for Maximum Air Flow Rate. This limit is active only when the zone thermostat requests heating and the VAV box damper is reverse acting.
-
-#### Field: Maximum Flow per Zone Floor Area During Reheat
-
-This factor (m<sup>3</sup>/s-m<sup>2</sup>) is multiplied by the zone area, to determine the maximum volume flow rate (m<sup>3</sup>/s) allowed during reheat operation (see detailed explanation above). This field is autocalculatable. If autocalculate is selected, the value is set to 0.002032 m<sup>3</sup>/s-m<sup>2</sup> (0.4 cfm/ft<sup>2</sup>). If this field and the following field are entered, the greater of the two inputs is used. If this field and the following field are left blank, the maximum flow will not be limited.
-
-#### Field: Maximum Flow Fraction During Reheat
-
-This fraction is multiplied by the Maximum Air Flow Rate to determine the maximum volume flow rate (m<sup>3</sup>/s) allowed during reheat operation (see detailed explanation above). This field is autocalculatable. If autocalculate is selected, the value is set to 0.002032 m<sup>3</sup>/s-m<sup>2</sup> (0.4 cfm/ft<sup>2</sup>) multiplied by the zone floor area divided by the Maximum Air Flow Rate. If this field and the previous field are entered, the greater of the two inputs is used. If this field and the previous field are left blank, the maximum flow will not be limited.
-
-#### Field: Maximum Reheat Air Temperature
-
-This field specifies the maximum allowable supply air temperature (°C) leaving the reheat coil in a VAV terminal unit during heating operation. If left blank, there is no limit, and the supply air temperature to the space may become unrealistically high during heating operation. If unknown, a value of 35C (95F) is recommended. There is no default in order to maintain consistency with prior results.
-
-#### Field: Design Specification Outdoor Air Object Name for Control
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object. When this field is used, the terminal unit will increase flow as needed to meet this outdoor air requirement. If Outdoor Air Flow per Person is non-zero (in the specified DesignSpecification:OutdoorAir object), then the outdoor air requirement will be computed based on the current number of occupants in the zone. At no time will the supply air flow rate exceed the value for Maximum Air Flow Rate. If this field is blank, then the terminal unit will not be controlled for outdoor air flow. See documentation for the zone HVAC outdoor air object for further information (Ref DesignSpecification:OutdoorAir object).
-
-Note that this field is used only for specifying the design outdoor air flow rate used for controlling the terminal unit air flow rate. The field *Design Specification Outdoor Air Object Name for Sizing* (see below) is used to specify the design outdoor air flow rate.
-
-#### Field: Supply Plenum Name
-
-This field allows the user to specify a supply plenum which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Return Plenum Name
-
-This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the VAV air handling system. The baseboard heating will be set to heating priority 2, which means it will meet any remaining heating load not met by the VAV system. Prior to v7.1, the capacity was only applied to electric baseboard. Starting with v7.1, the capacity will be used for both hot water and electric baseboard.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. *SystemSupplyAirTemperature* means that the Cooling Design Supply Air Temperature from the template VAV system serving this zone will be used (Ref. HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV). The default is *SystemSupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 12.8°C.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Zone Heating Design Supply Air Temperature will be used for sizing the zone heating design air flow rate and the heating or reheat coil. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50<sup>o</sup>C.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-#### Field: Design Specification Outdoor Air Object Name for Sizing
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*. Note that this field is used only for specifying the design outdoor air flow rate used for sizing. The field *Design Specification Outdoor Air Object Name for Sizing* (see above) is used to actively control the VAV terminal air flow rate.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:Zone:VAV,
-    SPACE1-1,                !- Zone Name
-    VAV Sys 1,               !- Template VAV System Name
-    All Zones,               !- Template Thermostat Name
-    autosize,                !- Supply Air Maximum Flow Rate {m3/s}
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-    Constant,                !- Zone Minimum Air Flow Input Method
-    0.3,                     !- Constant Minimum Air Flow Fraction
-    ,                        !- Fixed Minimum Air Flow Rate {m3/s}
-    ,                        !- Minimum Air Flow Fraction Schedule Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
-    HotWater,                !- Reheat Coil Type
-    ,                        !- Reheat Coil Availability Schedule Name
-    Reverse,                 !- Heating Damper Action
-    ,             !- Maximum Flow per Zone Floor Area During Reheat {m3/s-m2}
-    ,                        !- Maximum Flow Fraction During Reheat
-    ,                        !- Maximum Reheat Air Temperature
-    ,             !- Design Specification Outdoor Air Object Name for Control
-    ,                        !- Supply Plenum Name
-    ,                        !- Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule Name
-    autosize;                !- Baseboard Heating Capacity {W}
- SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
-    ,            !- Zone Cooling Design Supply Air Temperature {C]
-    ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
- SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
-    50.0,        !- Zone Heating Design Supply Air Temperature {C]
-    ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
-    ,            !- Design Specification Outdoor Air Object Name for Sizing
-    ;            !- Design Specification Zone Air Distribution Object Name
-```
-
-
-### HVACTemplate:Zone:VAV:FanPowered
-
-This object simulates the zone portion of a variable air volume HVAC configuration with a series or parallel fan powered terminal unit (also know as a powered induction unit or PIU) and several different heating options. Multiple HVACTemplate:Zone:VAV, HVACTemplate:Zone:VAV:FanPowered or HVACTemplate:Zone:VAV:HeatAndCool objects are usually specified for each HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object. Reheat is specified at the zone level.
-
-The series powered induction unit is an air system terminal unit that mixes varying amounts of secondary (recirculated) air and primary (conditioned supply) air to produce a fixed flow of air to a zone. The unit contains a small fan that acts to induce the secondary air and a heating coil for heating the mixed secondary and primary air. The fan runs at a constant volume flow rate whenever the unit is on (and the fan’s availability schedule is on or it is activated by an availability manager). With HVACTemplate:Zone:VAV:FanPowered, the secondary fan will operate according to the Zone PIU Fan Schedule and any Night Cycle Control specified in the  system it is served by.) The fan is downstream of the primary and secondary air inlets. The variable mixing is accomplished by a damper in the unit’s primary air supply inlet duct. This damper can move from fully open (100% primary air. 0% secondary air) to a minimum stop that is specified in the input description. At full cooling the damper will be fully open. At minimum cooling and for heating the damper will be at the minimum stop and the secondary air flow will be at its maximum. Reference object AirTerminal:SingleDuct:SeriesPIU:Reheat for more details.
-
-![SeriesPIUPicture.png](media/image608.png)
-
-Figure 156. Series PIU Terminal Unit
-
-The parallel powered induction unit is an air system terminal unit that mixes varying amounts of secondary (recirculated) air and primary (conditioned supply) air to produce a variable total flow of air to a zone. The unit contains a small fan that acts to induce the secondary air and a heating coil for heating the mixed secondary and primary air. The secondary and primary air streams enter the unit in parallel. The fan sits in the secondary air stream and runs only when the primary air flow is below the Parallel Fan On Flow Fraction and the fan’s availability schedule is on or it is activated by an availability manager. With HVACTemplate:Zone:VAV:FanPowered, the secondary fan will operate according to the Zone PIU Fan Schedule and any Night Cycle Control specified in the system it is served by.). The primary air inlet contains a damper that can move from fully open (maximum primary air) to a minimum stop (minimum primary air). At full cooling load the primary air damper is fully open and the fan is off. The primary air flow is at maximum and there is little or no secondary air flow. As the cooling load decreases, the primary air damper gradually closes and the secondary air flow remains close to zero. At some point, usually when the primary air flow has reached the minimum, the fan switches on and secondary air is induced. The heating coil will switch on as needed to meet any heating demand. Reference object AirTerminal:SingleDuct:ParallelPIU:Reheat for more details.
-
-![ParallelPIUPicture.png](media/image609.png)
-
-Figure 157. Parallel PIU Terminal Unit
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template VAV System Name
-
-Enter the name of the HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object serving this zone.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Primary Supply Air Maximum Flow Rate
-
-In a fan powered VAV terminal unit, the primary air flow is the air supplied by the central air handler. By entering Autosize, the maximum primary supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified and cooling SizingPeriod:DesignDay. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Primary Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Primary Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Primary Supply Air Minimum Flow Fraction
-
-Enter the fraction that the VAV box can reduce to based on the primary supply air maximum flow rate. This field may be sized automatically by entering Autosize.
-
-#### Field: Secondary Supply Air Maximum Flow Rate
-
-In a fan powered VAV terminal unit, the secondary air flow is the air taken from the zone by the terminal unit fan. By entering Autosize, the maximum secondary supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. If a value is entered, it will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The units are in m3/s.
-
-#### Field: Flow Type
-
-This field specifies the type of fan powered unit (PIU). The choices for this field are:
-
-- Series – Series configuration with recirculation directly from the zone
-
-- Parallel – Parallel configuration with recirculation directly from the zone
-
-- SeriesFromPlenum – Series configuration with recirculation from the return plenum
-
-- ParallelFromPlenum – Parallel configuration with recirculation from the return plenum
-
-See descriptions of these configurations in the general description for this object, above. For all types, the secondary fan will run according to the Zone PIU Fan Schedule (see below) and any Night Cycle Control specified in the system which serves this terminal unit (see Template VAV System Name above). For Parallel PIU, there is an additional secondary fan control based on the primary air flow fraction (see Parallel Fan On Flow Fraction below). For recirculation from plenum, a Return Plenum Name must be specificed in this object or in the system object (HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV) which serves this terminal unit. The default is Parallel.
-
-#### Field: Parallel Fan On Flow Fraction
-
-For parallel PIUs, this field specifies the fraction of the primary air flow at which fan turns on. In the parallel PIU the fan operation is intermittent. If the primary air flow is above this fraction of the maximum, the fan is off. Otherwise the secondary fan will run according to the System Availability Schedule and Night Cycle Control specified in the HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV which serves this terminal unit. This field does not apply to series PIUs.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
-
-If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: Reheat Coil Type
-
-A reheat coil may be added to the VAV box with this field. The choices are:
-
-- HotWater
-
-- Electric
-
-- Gas
-
-The default choice is Electric.
-
-#### Field: Reheat Coil Availability Schedule Name
-
-Leave this field blank if you want the reheat coil to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the coil is available should be specified as 1.0. Those times that the coil is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the coil is providing heat but a schedule of when it can provide heat.
-
-#### Field: Fan Total Efficiency
-
-Enter the total efficiency of the zone induction fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
-
-#### Field: Fan Delta Pressure
-
-Enter the pressure rise of the zone induction fan in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa.
-
-#### Field: Fan Motor Efficiency
-
-Enter the shaft power of the zone induction fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. Note that the zone fan motor is assumed to be 100% in the air stream.
-
-#### Field: Supply Plenum Name
-
-This field allows the user to specify a supply plenum which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Return Plenum Name
-
-This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the VAV air handling system.  The baseboard heating will be set to heating priority 2, which means it will meet any remaining heating load not met by the VAV system. Prior to v7.1, the capacity was only applied to electric baseboard. Starting with v7.1, the capacity will be used for both hot water and electric baseboard.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. *SystemSupplyAirTemperature* means that the Cooling Design Supply Air Temperature from the template VAV system serving this zone will be used (Ref. HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV). The default is *SystemSupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 12.8°C.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Zone Heating Design Supply Air Temperature will be used for sizing the zone heating design air flow rate and the heating or reheat coil. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50<sup>o</sup>C.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-#### Field: Zone PIU Fan Schedule Name
-
-This is the operating schedule for the zone PIU fan. For a parallel PIU, the zone fan operates only when the primary air flow is below the Parallel Fan On Flow Fraction and the Zone PIU Fan Schedule is on, or when it is activated by an availability manager. For a series PIU, the zone fan operates whenever the Zone PIU Fan Schedule is on, or it is activated by an availability manager. If this field is left blank, the System Availability Schedule for the HVACTemplate:System serving this zone will be used.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:Zone:VAV:FanPowered,
-    SPACE1-1,                !- Zone Name
-    VAV Sys 1,               !- Template VAV System Name
-    All Zones,               !- Template Thermostat Name
-    autosize,                !- Primary Supply Air Maximum Flow Rate {m3/s}
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-    autosize,                !- Primary Supply Air Minimum Flow Fraction
-    autosize,                !- Secondary Supply Air Maximum Flow Rate {m3/s}
-    Series,                  !- Flow Type
-    autosize,                !- Parallel Fan On Flow Fraction
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
-    HotWater,                !- Reheat Coil Type
-    ,                        !- Reheat Coil Availability Schedule Name
-    0.7,                     !- Fan Total Efficiency
-    1000,                    !- Fan Delta Pressure {Pa}
-    0.9,                     !- Fan Motor Efficiency
-    ,                        !- Supply Plenum Name
-    ,                        !- Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule Name
-    autosize;                !- Baseboard Heating Capacity {W}
- SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
-    ,            !- Zone Cooling Design Supply Air Temperature {C]
-    ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
- SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
-    50.0,        !- Zone Heating Design Supply Air Temperature {C]
-    ,            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
-    ,            !- Zone PIU Fan Schedule Name
-    ,            !- Design Specification Outdoor Air Object Name
-    ;            !- Design Specification Zone Air Distribution Object Name
-```
-
-
-### HVACTemplate:Zone:VAV:HeatAndCool
-
-This object simulates the zone portion of a variable air volume HVAC configuration with several different heating options. When heating is required, this terminal unit will increase airflow first and then activate the optional reheat coil. Multiple HVACTemplate:Zone:VAV, HVACTemplate:Zone:VAV:FanPowered, or HVACTemplate:Zone:VAV:HeatAndCool objects are usually specified for each HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object. Reheat is specified at the zone level. Reference AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat and AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat for more details about these VAV terminal units.
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template VAV System Name
-
-Enter the name of the HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object serving this zone.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Supply Air Maximum Flow Rate
-
-By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Constant Minimum Air Flow Fraction
-
-The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. The reheat coil operates only when the damper is at this minimum flow rate when Damper Heating Action is set to Normal (the default).  This field is used if the previous field is set to Constant.  If the previous field is set to Scheduled (and the field Maximum Hot Water or Steam Flow Rate is set to autosize), then this field is optional and can be used to separately control the air flow rate used for sizing normal-action reheat coils. If this field and the following field have values, the greater of the two is used for sizing.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name for Sizing and Design Specification Zone Air Distribution Object Name fields below.
-
-If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: Design Specification Outdoor Air Object Name for Sizing
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*. Note that this field is used only for specifying the design outdoor air flow rate used for sizing. The field *Design Specification Outdoor Air Object Name for Sizing* (see above) is used to actively control the VAV terminal air flow rate.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Reheat Coil Type
-
-A reheat coil may be added to the VAV box with this field. The choices are:
-
-- HotWater
-
-- Electric
-
-- Gas
-
-- None
-
-The default choice is None.
-
-#### Field: Reheat Coil Availability Schedule Name
-
-Leave this field blank if you want the reheat coil to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the coil is available should be specified as 1.0. Those times that the coil is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the coil is providing heat but a schedule of when it can provide heat.
-
-#### Field: Maximum Reheat Air Temperature
-
-This field specifies the maximum allowable supply air temperature (°C) leaving the reheat coil in a VAV terminal unit during heating operation. If left blank, there is no limit, and the supply air temperature to the space may become unrealistically high during heating operation. If unknown, a value of 35C (95F) is recommended. There is no default in order to maintain consistency with prior results.
-
-#### Field: Supply Plenum Name
-
-This field allows the user to specify a supply plenum which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Return Plenum Name
-
-This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the VAV air handling system. The baseboard heating will be set to heating priority 2, which means it will meet any remaining heating load not met by the VAV system. Prior to v7.1, the capacity was only applied to electric baseboard. Starting with v7.1, the capacity will be used for both hot water and electric baseboard.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. *SystemSupplyAirTemperature* means that the Cooling Design Supply Air Temperature from the template VAV system serving this zone will be used (Ref. HVACTemplate:System:VAV or HVACTemplate:System:PackagedVAV). The default is *SystemSupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 12.8°C.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Zone Heating Design Supply Air Temperature will be used for sizing the zone heating design air flow rate and the heating or reheat coil. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. The default is *SupplyAirTemperature.*
-
-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50<sup>o</sup>C.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:Zone:VAV:HeatAndCool,
-    SPACE1-1,                !- Zone Name
-    VAV Sys 1,               !- Template VAV System Name
-    All Zones,               !- Template Thermostat Name
-    autosize,                !- Supply Air Maximum Flow Rate {m3/s}
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-    0.3,                     !- Constant Minimum Air Flow Fraction
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    0.0,               !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
-    ,            !- Design Specification Outdoor Air Object Name for Sizing
-    ,            !- Design Specification Zone Air Distribution Object Name
-    HotWater,                !- Reheat Coil Type
-    ,                        !- Reheat Coil Availability Schedule Name
-    ,                        !- Maximum Reheat Air Temperature
-    ,                        !- Supply Plenum Name
-    ,                        !- Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule Name
-    autosize;                !- Baseboard Heating Capacity {W}
- SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
-    ,            !- Zone Cooling Design Supply Air Temperature {C]
-    ,            !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
- SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
-    50.0,        !- Zone Heating Design Supply Air Temperature {C]
-    ;            !- Zone Heating Design Supply Air Temperature Difference {deltaC]
-```
-
-
-### HVACTemplate:Zone:ConstantVolume
-
-This object simulates the zone portion of a constant volume HVAC configuration with or without reheat. One or more HVACTemplate:Zone:ConstantVolume objects will be used with a single HVACTemplate:System:ConstantVolume which has optional chilled water cooling and several types of heating. Reference AirTerminal:SingleDuct:Uncontrolled and AirTerminal:SingleDuct:ConstantVolume:Reheat for more details about the terminal units.
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template Constant Volume System Name
-
-Enter the name of the HVACTemplate:System:ConstantVolume object serving this zone.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Supply Air Maximum Flow Rate
-
-By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. Note that the zone must have a thermostat specified in order to autosize the flow rate, even if it is not the control zone in a multiple zone unitary system. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The HVACTemplate:System:ConstantVolume object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
-
-If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: Design Specification Outdoor Air Object Name
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Reheat Coil Type
-
-A reheat coil may be added to the terminal unit with this field. The choices are:
-
-- HotWater
-
-- Electric
-
-- Gas
-
-- None
-
-The default choice is None.
-
-#### Field: Reheat Coil Availability Schedule Name
-
-Leave this field blank if you want the reheat coil to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the coil is available should be specified as 1.0. Those times that the coil is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the coil is providing heat but a schedule of when it can provide heat.
-
-#### Field: Maximum Reheat Air Temperature
-
-This field specifies the maximum allowable supply air temperature (°C) leaving the reheat coil  during heating operation. If left blank, there is no limit, and the supply air temperature to the space may become unrealistically high during heating operation. If unknown, a value of 35C (95F) is recommended. There is no default in order to maintain consistency with prior results.
-
-#### Field: Supply Plenum Name
-
-This field allows the user to specify a supply plenum which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Return Plenum Name
-
-This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the air handling system. The baseboard heating will be set to heating sequence 2, which means it will meet any remaining heating load not met by the air handling system.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. *SystemSupplyAirTemperature* means that the Cooling Coil Design Setpoint Temperature from the template system serving this zone will be used (Ref. HVACTemplate:System:ConstantVolume). The default is *SystemSupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 12.8°C.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Zone Heating Design Supply Air Temperature  will be used for sizing the zone heating design air flow rate. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. *SystemSupplyAirTemperature* means that the Heating Coil Design Setpoint Temperature from the template system serving this zone will be used (Ref. HVACTemplate:System:ConstantVolume). The default is *SystemSupplyAirTemperature.*
-
-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50<sup>o</sup>C.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:Zone:ConstantVolume,
-    SPACE1-1,                !- Zone Name
-    CAV Sys 1,               !- Template Constant Volume System Name
-    All Zones,               !- Template Thermostat Name
-    autosize,                !- Supply Air Maximum Flow Rate {m3/s}
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    0.0,                     !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
-     ,                        !- Design Specification Outdoor Air Object Name
-     ,                       !- Design Specification Zone Air Distribution Object Name
-    HotWater,                !- Reheat Coil Type
-    ,                        !- Reheat Coil Availability Schedule Name
-    ,                        !- Maximum Reheat Air Temperature {C}
-    ,                        !- Supply Plenum Name
-    ,                        !- Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule Name
-    autosize;                !- Baseboard Heating Capacity {W}
- SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
-    12.8,                    !- Zone Cooling Design Supply Air Temperature {C]
-    11.11,          !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
- SupplyAirTemperature, !- Zone Heating Design Supply Air Temperature Input Method
-    50,                      !- Zone Heating Design Supply Air Temperature {C]
-    30;             !- Zone Heating Design Supply Air Temperature Difference {deltaC]
-```
-
-
-### HVACTemplate:Zone:DualDuct
-
-This object simulates the zone portion of a constant volume or variable volume dual-duct HVAC system. One or more HVACTemplate:Zone:DualDuct objects may be used with a single HVACTemplate:System:DualDuct object which has optional chilled water cooling and several types of heating. A constant air volume dual duct system is simulated by setting the Zone Minimum Air Flow Fraction =1.0.  A variable air volume duct duct system is simulated by setting the Zone Minimum Air Flow Fraction &lt;1.0. . Reference AirTerminal:DualDuct:ConstantVolume and AirTerminal:DualDuct:VAV for more details about the terminal units.
-
-#### Field: Zone Name
-
-Enter the name of the zone. The name must match a building zone name used in the ZONE object.
-
-#### Field: Template Dual Duct System Name
-
-Enter the name of the HVACTemplate:System:DualDuct object serving this zone.
-
-#### Field: Template Thermostat Name
-
-Enter the name of a HVACTemplate:Thermostat object. Multiple HVACTemplate:Zone:\* objects can reference the same HVACTemplate:Thermostat object which makes it easier to revise the thermostat controls for portions of a building.
-
-When this field is blank, it has a special meaning. A blank entry means that traditional thermostat objects referencing the same zone name are used instead of HVACTemplate:Thermostat.
-
-#### Field: Supply Air Maximum Flow Rate
-
-By entering Autosize, the maximum supply air flow rate is automatically determined for the zone based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay and cooling SizingPeriod:DesignDay. Note that the zone must have a thermostat specified in order to autosize the flow rate, even if it is not the control zone in a multiple zone unitary system. If a value is entered it is used as the maximum supply air flow rate into the zone. It will be multiplied by the Supply Air Sizing Factor and by zone multipliers. The HVACTemplate:System:DualDuct object that is referenced also allows the specification of supply air flow. If the value is specified at the system level it will scale the zone values to match. The units are in m3/s.
-
-#### Field: Zone Heating Sizing Factor
-
-This input is the zone level heating sizing ratio. The zone design heating air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Heating Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Cooling Sizing Factor
-
-This input is the zone level cooling sizing ratio. The zone design cooling air flow rate and load will be multiplied by the number input in this field when Supply Air Maximum Flow Rate is autosized.  If this field is left blank, the Cooling Sizing Factor from Sizing:Parameters will be used.
-
-#### Field: Zone Minimum Air Flow Fraction
-
-The minimum flow rate to the zone while the system is operating, specified as a fraction of the maximum air flow rate. The minimum zone fraction is normally specified to meet the minimum ventilation requirement for the occupants. This field is ignored is the system serving this zone is constant volume.
-
-#### Field: Outdoor Air Method
-
-The input must be either *Flow/Zone*, or *Flow/Person*, *Flow/Area*, *Sum*, *Maximum or DetailedSpecification*. *Flow/Zone* means that the program will use the input of the field *Outdoor Air Flow* as the zone design outdoor air flow rate. *Flow/Person* means the program will use the input from the field *Outdoor Air Flow per Person* and the maximum occupancy to calculate a zone design outdoor air flow rate. *Flow/Area* means the program will use the input from the field *Outdoor Air Flow per Zone Floor Area* to calculated a zone design outdoor air flow rate. *Sum* means that the flows calculated from the fields *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be added to obtain the zone design outdoor air flow rate. *Maximum* means that the maximum flow derived from *Outdoor Air Flow per Person,* *Outdoor Air Flow per Area* and *Outdoor Air Flow per Zone* will be used for the zone design outdoor air flow rate. The default is *Flow/Person*.
-
-*DetailedSpecification* means that the outdoor air specifications will be taken from a DesignSpecification:OutdoorAir object and optional DesignSpecification:ZoneAirDistribution object. These objects are referenced in the Design Specification Outdoor Air Object Name and Design Specification Zone Air Distribution Object Name fields below.
-
-If the air handler serving this zone serves more than one zone, the total outdoor air flow for the system is the sum of the zone outdoor air flows if the system outdoor air flow is autosized. Since the zones share a single outdoor air source, the amount of outdoor air actually delivered to the zone is based on the fraction of supply air delivered to the zone to the total supply air from the system.
-
-#### Field: Outdoor Air Flow Rate per Person
-
-The design outdoor air flow rate per person for this zone in cubic meters per second. The default is 0.00944 (20 cfm per person). An outdoor air flow rate is calculated based on the total number of people for all People statements assigned to the zone. Occupancy schedule values are not applied. This input is used if *Outdoor Air Method* is one of  *Outdoor Air Flow per Person*, *Sum*, or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone Floor Area
-
-The design outdoor air volumetric flow rate per square meter of floor area (units are m<sup>3</sup>/s-m<sup>2</sup>). This input is multiplied by the zone area to obtain a flow rate. This input is used if *Outdoor Air Method* is *Flow/Area, Sum* or *Maximum*.
-
-#### Field: Outdoor Air Flow Rate per Zone
-
-The design outdoor air flow rate for this zone in cubic meters per second. This input field is used if *Outdoor Air Method* is *Flow/Zone, Sum* or *Maximum*.
-
-#### Field: Design Specification Outdoor Air Object Name for Sizing
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object which specifies the design outdoor air flow rate for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*. Note that this field is used only for specifying the design outdoor air flow rate used for sizing. The field *Design Specification Outdoor Air Object Name for Control* (see below) is used to actively control the VAV terminal air flow rate.
-
-#### Field: Design Specification Zone Air Distribution Object Name
-
-This alpha field specifies the name of a DesignSpecification:ZoneAirDistribution object which specifies the air distribution effectiveness for the zone.  This field is used only when *Outdoor Air Method = DetailedSpecification*.
-
-#### Field: Design Specification Outdoor Air Object Name for Control
-
-This alpha field specifies the name of a DesignSpecification:OutdoorAir object. When this field is used, the terminal unit will increase flow as needed to meet this outdoor air requirement. If Outdoor Air Flow per Person (in the specified DesignSpecification:OutdoorAir object) is non-zero, then the outdoor air requirement will be computed based on the current number of occupants in the zone. At no time will the supply air flow rate exceed the value for Maximum Air Flow Rate. If this field is blank, then the terminal unit will not be controlled for outdoor air flow. See documentation for the zone HVAC outdoor air object for further information (Ref DesignSpecification:OutdoorAir object).
-
-Note that this field is used only for specifying the design outdoor air flow rate used for controlling the terminal unit air flow rate. The field *Design Specification Outdoor Air Object Name for Sizing* (see above) is used to specify the design outdoor air flow rate.
-
-#### Field: Cold Supply Plenum Name
-
-This field allows the user to specify a cold supply plenum zone which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Hot Supply Plenum Name
-
-This field allows the user to specify a hot supply plenum zone which serves only this zone. The plenum zone is added to the supply air path after the system splitter or system-level supply plenum and before the zone terminal unit. Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Return Plenum Name
-
-This field allows the user to specify a return plenum which serves only this zone. The plenum zone is added to the return air path immediately after the zone and before the system mixer or system-level return plenum. Set to blank if no zone return plenum is to be modeled. If a zone return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here.
-
-#### Field: Baseboard Heating Type
-
-This field specifies the availability of thermostatically controlled baseboard heat in this zone. The choices are:
-
-- HotWater
-
-- Electric
-
-- None
-
-The default choice is None.
-
-#### Field: Baseboard Heating Availability Schedule Name
-
-Leave this field blank if you want the baseboard heating to be available for the entire year to perform heating if called for by the thermostat. If a schedule name is specified, those times that the baseboard heating is available should be specified as 1.0. Those times that the baseboard heating is not available should have a zero value in the schedule. Please note that this is not a schedule of when the baseboard is providing heat but a schedule of when it can provide heat.
-
-#### Field: Baseboard Heating Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the baseboard heating can deliver in Watts.  Note that EnergyPlus autosizing will autosize the baseboard heating to meet the full heating load of the zone, regardless of the heating capability of the VAV air handling system. The baseboard heating will be set to heating priority 2, which means it will meet any remaining heating load not met by the VAV system. Prior to v7.1, the capacity was only applied to electric baseboard. Starting with v7.1, the capacity will be used for both hot water and electric baseboard.
-
-#### Field: Zone Cooling Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the cooling design supply air temperature. *SupplyAirTemperature* means that the field Zone Cooling Design Supply Air Temperature will be used for sizing the zone cooling design air flow rate and the cooling coil. *TemperatureDifference* means that the field Zone Cooling Design Supply Air Temperature Difference will be used. *SystemSupplyAirTemperature* means that the Cooling Design Supply Air Temperature from the template system serving this zone will be used (Ref. HVACTemplate:System:DualDuct). The default is *SystemSupplyAirTemperature.*
-
-#### Field: Zone Cooling Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 12.8°C.
-
-#### Field: Zone Cooling Design Supply Air Temperature Difference
-
-The temperature difference between the cooling design supply air temperature and the zone air temperature in degrees Celsius for the zone cooling design air flow rate calculation and cooling coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Cooling Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 11.11 deltaC.
-
-#### Field: Zone Heating Design Supply Air Temperature Input Method
-
-This field selects the method for specifying the heating design supply air temperature. *SupplyAirTemperature* means that the field Zone Heating Design Supply Air Temperature  will be used for sizing the zone heating design air flow rate. *TemperatureDifference* means that the field Zone Heating Design Supply Air Temperature Difference will be used. *SystemSupplyAirTemperature* means that the Heating Coil Design Setpoint Temperature from the template system serving this zone will be used (Ref. HVACTemplate:System:DualDuct). The default is *SystemSupplyAirTemperature.*
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-#### Field: Zone Heating Design Supply Air Temperature
-
-The supply air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *SupplyAirTemperature.* The default is 50<sup>o</sup>C.
-
-#### Field: Zone Heating Design Supply Air Temperature Difference
-
-The temperature difference between heating design supply air temperature and zone air temperature in degrees Celsius for the zone heating design air flow rate calculation and heating coil sizing. The absolute value is used, so the sign may be positive or negative. This field is used only when Zone Heating Design Supply Air Temperature Input Method is *TemperatureDifference.* The default is 30 deltaC.
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:Zone:DualDuct,
-    SPACE1-1,                !- Zone Name
-    DD Sys 1,                !- Template Dual Duct System Name
-    All Zones,               !- Template Thermostat Name
-    autosize,                !- Supply Air Maximum Flow Rate {m3/s}
-    ,                        !- Zone Heating Sizing Factor
-    ,                        !- Zone Cooling Sizing Factor
-     0.2,                     !- Zone Minimum Air Flow Fraction
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow Rate per Person {m3/s}
-    0.0,                     !- Outdoor Air Flow Rate per Zone Floor Area {m3/s-m2}
-    0.0,                     !- Outdoor Air Flow Rate per Zone {m3/s}
-     ,                    !- Design Specification Outdoor Air Object Name for Sizing
-     ,                      !- Design Specification Zone Air Distribution Object Name
-    ,                    !- Design Specification Outdoor Air Object Name for Control
-     ,                        !- Cold Supply Plenum Name
-     ,                        !- Hot Supply Plenum Name
-    ,                        !- Return Plenum Name
-    None,                    !- Baseboard Heating Type
-    ,                        !- Baseboard Heating Availability Schedule Name
-    autosize;                !- Baseboard Heating Capacity {W}
- SystemSupplyAirTemperature, !- Zone Cooling Design Supply Air . . . Input Method
-    12.8,                    !- Zone Cooling Design Supply Air Temperature {C]
-    11.11,          !- Zone Cooling Design Supply Air Temperature Difference {deltaC]
- SystemSupplyAirTemperature, !- Zone Heating Design Supply Air . . . Input Method
-    50,                      !- Zone Heating Design Supply Air Temperature {C]
-    30;             !- Zone Heating Design Supply Air Temperature Difference {deltaC]
-```
-
-
-### HVACTemplate:System:VRF
-
-This model simulates a variable-refrigerant-flow (or variable-refrigerant-volume) air-conditioning system. This system type models direct-expansion cooling and/or heating coils configured in a zone terminal unit (ref. HVACTemplate:Zone:VRF). For more details about this system type see AirConditioner:VariableRefrigerantFlow.
-
-#### Field: Name
-
-Enter a name for the HVACTemplate:System:VRF object. This name is used in the HVACTemplate:Zone:VRF object to reference this system.
-
-#### Field: System Availability Schedule Name
-
-This alpha field defines the name of the schedule (ref: Schedule) that denotes whether the heat pump operates during a given time period. A schedule value equal to 0 denotes that the heat pump must be off for that time period. A value other than 0 denotes that the heat pump is available to operate during that time period. This schedule may be used to completely disable the heat pump (and all of its terminal units) as required. If this field is blank, the unit is enabled the entire simulation.
-
-#### Field: Gross Rated Total Cooling Capacity
-
-This numeric field defines the gross rated total cooling capacity of the DX cooling coil in watts. The total cooling capacity should be a “gross�, i.e., the effect of supply air fan heat NOT accounted for.
-
-#### Field: Gross Rated Cooling COP
-
-This numeric field defines the cooling coefficient of performance at rated conditions. The cooling coefficient of performance includes compressor power and condenser fan power. This COP value does not account for impacts due to the supply air fan. The nominal heat pump cooling COP must be greater than 0. If this field is left blank, a default coefficient of performance of 3.3 is assumed.
-
-#### Field: Minimum Outdoor Temperature in Cooling Mode
-
-This numeric field defines the minimum outdoor dry-bulb temperature allowed for cooling operation. Below this temperature, cooling is disabled. If this field is left blank, the default value is -6ºC.
-
-#### Field: Maximum Outdoor Temperature in Cooling Mode
-
-This numeric field defines the maximum outdoor dry-bulb temperature allowed for cooling operation. Above this temperature, cooling is disabled. If this field is left blank, the default value is 43ºC.
-
-#### Field: Gross Rated Heating Capacity
-
-This numeric field defines the gross total heat pump heating capacity at rated conditions in watts. The nominal heat pump heating capacity must be greater than 0 or set to autosize.
-
-#### Field: Rated Heating Capacity Sizing Ratio
-
-This numeric field defines the ratio of gross heating to gross cooling capacity. The model assumes that when used, this value will be greater than 1. A similar input is available in the ZoneHVAC:TerminalUnit:VariableRefrigerantFlow object. When the heating capacity is autosized, if this field is non-blank, this ratio is used to scale the heating capacity to the gross rated total cooling capacity regardless of the value entered in the terminal unit objects. When the heating capacity is not autosized, the gross rated heating capacity will be equal to the sum of the terminal unit heating coil size. If this field is blank and the terminal unit sizing ratio input is also blank, then the heating capacity sizing ratio is assumed to be 1. If this field is not blank and the heating capacity sizing ratio in the terminal unit object(s) is blank, then this ratio also applies to each heating coil. If this field is not blank and the heating capacity sizing ratio in the terminal units is also not blank, then the terminal unit heating coil capacity sizing ratio input applies to each heating coil.
-
-#### Field: Gross Rated Heating COP
-
-This numeric field defines the heating coefficient of performance at rated conditions. The heating coefficient of performance includes compressor power and condenser fan power. This gross COP value does NOT account for  the supply air fan. The nominal heat pump heating COP must be greater than 0. If this field is left blank, a coefficient of performance of 3.4 is assumed.
-
-#### Field: Minimum Outdoor Temperature in Heating Mode
-
-This numeric field defines the minimum outdoor temperature allowed for heating operation. Below this temperature, heating is disabled. If this field is left blank, the default value is -20ºC.
-
-#### Field: Maximum Outdoor Temperature in Heating Mode
-
-This numeric field defines the maximum outdoor temperature allowed for heating operation. Above this temperature, heating is disabled. If this field is left blank, the default value is 16ºC.
-
-#### Field: Minimum Heat Pump Part-Load Ratio
-
-This numeric field specifies the minimum operating part-load ratio (PLR) of the heat pump. When the heat pump operates at a PLR below this value, the heat pump’s compressor will cycle to meet the cooling or heating demand. Above this value, the heat pump’s compressor operates the entire time step to meet the cooling or heating demand. The minimum value for this field is 0. If this field is left blank, the default value is 0.15. When the heat pump compressor cycles, the previous field is used to determine cycling losses.
-
-#### Field: Zone Name for Master Thermostat Location
-
-This alpha field defines the name of the zone where the “master� thermostat is located. When the heat pump is connected to multiple zone terminal units, one terminal unit must be selected as the master thermostat. The remaining thermostats are slaves and can operate only in the same mode as the master thermostat.
-
-#### Field: Master Thermostat Priority Control Type
-
-This choice field determines the logic used to simulate the “master� thermostat. Valid choices are LoadPriority, ZonePriority, ThermostatOffsetPriority, MasterThermostatPriority, and Scheduled. The default value is MasterThermostatPriority. When LoadPriority is selected, the total zone load is used to choose the operating mode as either cooling or heating. When ZonePriority is selected, the number of zones requiring cooling or heating determines the operating mode. When ThermostatOffsetPriority is selected, the zone farthest from the thermostat set point determines the operating mode. The MasterThermostatPriority choice operates the system according the zone load where the master thermostat is located. The heat pump can also be scheduled to operate in either cooling or heating mode. For scheduled operation, a schedule name is entered in the following field.
-
-#### Field: Thermostat Priority Schedule Name
-
-This alpha field identifies the schedule used when the previous field is set to Scheduled. Schedule values of 0 denote cooling mode while values of 1 denote heating mode. Any other values will force the system off.
-
-#### Field: Heat Pump Waste Heat Recovery
-
-This choice field defines the configuration of the heat pump refrigeration system. Valid choices are **Yes** and **No**. If Yes is selected, heat recovery is enabled and the heat pump can independently cool and heat different zones. If No is selected, the heat pump is only able to cool or heat for any given time step.
-
-#### Field: Equivalent Piping Length used for Piping Correction Factor in Cooling Mode
-
-This numeric field defines the equivalent pipe length in meters between the farthest terminal unit and the heat pump condenser. This value includes the gas refrigerant line length (for both horizontal and vertical distances), fitting losses, pipe bends, and other connections that contribute to piping losses. This field is used to calculate the piping correction factor in cooling mode. This value defines the head losses due to the pipe length between the farthest terminal unit and the heat pump condenser and impacts the maximum available capacity in cooling mode.
-
-#### Field: Vertical Height used for Piping Correction Factor
-
-This numeric field defines the vertical pipe height in meters between the highest or lowest terminal unit and the heat pump condenser. This value defines the gravitational losses due to a change in height between the highest (positive value), or lowest (negative value) terminal unit and the heat pump condenser. The distance specified here is applied to the piping correction factor calculation for both cooling and heating. If the distance between the highest terminal unit above the heat pump condenser is greater than the distance between the lowest terminal unit below the condenser enter the difference between the highest and lowest terminal units as a positive distance, otherwise enter this difference as a negative distance. Example: if the distance from the heat pump condenser to the highest terminal unit above the condenser is 10 m and the distance from the heat pump condenser to the lowest terminal unit below the condenser is -15 m, then enter a value of -5 m in this field. This head loss impacts the maximum available capacity in cooling mode.
-
-#### Field: Equivalent Piping Length used for Piping Correction Factor in Heating Mode
-
-This numeric field defines the equivalent pipe length in meters between the farthest terminal unit and the heat pump condenser. This value includes the liquid refrigerant line length (for both horizontal and vertical distances), fitting losses, pipe bends, and other connections that contribute to piping losses. This field is used to calculate the piping correction factor in heating mode. This value defines the head losses due to the pipe length between the farthest terminal unit and the heat pump condenser and impacts the maximum available capacity in heating mode.
-
-#### Field: Crankcase Heater Power per Compressor
-
-This numeric field defines the electrical power consumed by the crankcase heater in watts for *each* compressor. This crankcase heater power is consumed when the outdoor temperature is below the maximum outdoor dry-bulb temperature for crankcase heater operation. The minimum value for this field is 0. If this field is left blank, the default value is 33 watts. Crankcase heater electrical consumption is applied only when the compressor is off or is applied during the off cycle when the compressor is cycling below the Minimum Heat Pump Part-Load Ratio. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
-
-#### Field: Number of Compressors
-
-This numeric field defines the number of compressors in the heat pump condensing unit and is used exclusively to determine the operating characteristics of the crankcase heater. For example, if the number of compressors is 3, one crankcase heater will operate when the heat pump condensing unit’s part-load ratio is less than or equal to 0.67 (when the ratio of compressor size to total compressor capacity input is 0.33) and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. Similarly, two crankcase heaters will operate when the heat pump condensing unit’s PLR is less than or equal to 0.33 and the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. If the heat pump condensing unit is off, all 3 crankcase heaters will operate if the outdoor temperature is below the maximum outdoor temperature for crankcase heater operation. The minimum value for this field is 1. If this field is left blank, the default value is 2. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
-
-#### Field: Ratio of Compressor Size to Total Compressor Capacity
-
-This numeric field defines the size of the first stage compressor to the total compressor capacity and is used exclusively for calculating crankcase heater energy. If this field and the previous field are left blank, the default value is 0.5.  If this field is left blank and the previous field is not blank, the compressors are assumed to be equally sized. When the number of compressors is greater than 2, the 2<sup>nd</sup> stage compressor and all additional compressors are assumed to be equally sized. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
-
-#### Field: Maximum Outdoor Dry-bulb Temperature for Crankcase Heater
-
-This numeric field defines the maximum outdoor temperature, in degrees Celsius, below which the crankcase heater will operate. If this field is left blank, the default value is 0°C. This field is only used to calculate crankcase heater power and has no impact on heat pump performance.
-
-#### Field: Defrost Strategy
-
-This alpha field has two choices: reverse-cycle or resistive. If the reverse-cycle strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a resistive defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is reverse-cycle. Defrost can be disabled by entering a resistive defrost strategy using a timed defrost control, a 0 defrost time period fraction and a 0 resistive defrost heater capacity in the following inputs fields. This method is used when the Maximum Outdoor Dry-Bulb Temperature for Defrost Operation field value is greater than the expected minimum outdoor dry-bulb temperature simulated in the weather file.
-
-#### Field: Defrost Control
-
-This alpha field has two choices: timed or on-demand. If timed control is selected, the defrost time period is calculated based on a fixed value of compressor runtime whether or not frost has actually accumulated. For timed defrost control, the fractional amount of time the unit is in defrost is entered in the input field “Defrost Time Period Fraction� described below. If on-demand defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field “Maximum Outdoor Dry-bulb Temperature for Defrost Operation� described above. If this input field is left blank, the default defrost control is timed.
-
-#### Field: Defrost Time Period Fraction
-
-This numeric field defines the fraction of compressor runtime when the defrost cycle is active. For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
-
-#### Field: Resistive Defrost Heater Capacity
-
-This numeric field defines the capacity of the resistive defrost heating element in Watts. This input field is used only when the selected defrost strategy is ‘resistive’ (see input field “Defrost Strategy� above). The value for this input field must be greater than or equal to 0 and it is auotsizable. If this input field is left blank, the default is autosize.
-
-#### Field: Maximum Outdoor Dry-bulb Temperature for Defrost Operation
-
-This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. If this input field is left blank, the default value is 5 C. Defrost can be completely eliminated by selecting a temperature lower than the minimum expected outdoor temperature found in the weather file.
-
-#### Field: Condenser Type
-
-This choice field defines the configuration of the heat pump condenser. Valid choices are **AirCooled**, **EvaporativelyCooled**, and **WaterCooled**. If WaterCooled is specified, then this unit will be served by an HVACTemplate:Plant:MixedWaterLoop.
-
-#### Field: Water Condenser Volume Flow Rate
-
-This numeric field defines the condenser water volume flow rate in cubic meters per second. This field is autosizable and only used for water-cooled systems.
-
-#### Field: Evaporative Condenser Effectiveness
-
-The effectiveness of the evaporative condenser, which is used to determine the temperature of the air entering the outdoor condenser coil as follows:
-
-<div>\[Tcond\,inlet = \,\left( {Twb,o} \right)\,\, + \,\,\left( {1 - EvapCondEffectiveness} \right)\left( {Tdb,o\,\, - Twb,o} \right)\]</div>
-
-where
-
-*T<sub>cond\\ inlet</sub>* = the temperature of the air entering the condenser coil (C)
-
-*T<sub>wb,o</sub>* = the wet-bulb temperature of the outdoor air (C)
-
-*T<sub>db,o</sub>* = the dry-bulb temperature of the outdoor air (C)
-
-The resulting condenser inlet air temperature is used by the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature). The default value for this field is 0.9, although valid entries can range from 0.0 to 1.0. This field is not used when Condenser Type = Air Cooled and the simulation is calculating heating performance.
-
-If the user wants to model an air-cooled condenser, they should simply specify AirCooled in the field Condenser Type. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature.
-
-If the user wishes to model an evaporative-cooled condenser AND they have performance curves that are a function of the wet-bulb temperature of air entering the condenser coil, then the user should specify Condenser Type = EvapCooled and the evaporative condenser effectiveness value should be entered as 1.0. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of the wet-bulb temperature of air entering the condenser coil.
-
-If the user wishes to model an air-cooled condenser that has evaporative media placed in front of it to cool the air entering the condenser coil, then the user should specify Condenser Type = EvapCooled. The user must also enter the appropriate evaporative effectiveness for the media. In this case, the Cooling Capacity Ratio Modifier Curve (function of temperature) and the Cooling Energy Input Ratio Modifier Curve (function of temperature) input fields for this object should reference performance curves that are a function of outdoor dry-bulb temperature. Be aware that the evaporative media will significantly reduce the dry-bulb temperature of the air entering the condenser coil, so the Cooling Capacity and Cooling EIR Modifier Curves must be valid for the expected range of dry-bulb temperatures that will be entering the condenser coil.
-
-#### Field: Evaporative Condenser Air Flow Rate
-
-The air volume flow rate, in m<sup>3</sup> per second, entering the evaporative condenser. This value is used to calculate the amount of water used to evaporatively cool the condenser inlet air. The minimum value for this field must be greater than zero, and this input field is autosizable (equivalent to 0.000144 m<sup>3</sup>/s per watt of rated total cooling capacity [850 cfm/ton]). This field is not used when Condenser Type = AirCooled.
-
-#### Field: Evaporative Condenser Pump Rated Power Consumption
-
-The rated power of the evaporative condenser water pump in Watts. This value is used to calculate the power required to pump the water used to evaporatively cool the condenser inlet air. The default value for this input field is zero, but it is autosizable (equivalent to 0.004266 W per watt [15 W/ton] of rated total cooling capacity). This field is not used when Condenser Type = AirCooled.
-
-#### Field: Basin Heater Capacity
-
-This numeric field contains the capacity of the heat pump’s electric basin heater in watts per degree Kelvin. This field only applies for Condenser Type = EvaporativelyCooled. This field is used in conjunction with the Basin Heater Setpoint Temperature described in the following field. The basin heater electric power is equal to this field multiplied by the difference between the basin heater set point temperature and the outdoor dry-bulb temperature. The basin heater only operates when the heat pump compressor(s) is off, regardless of the basin heater schedule described below. The basin heater capacity must be greater than or equal to zero, with a default value of zero if this field is left blank.
-
-#### Field: Basin Heater Setpoint Temperature
-
-This numeric field contains the set point temperature (ËšC) for the basin heater described in the previous field. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater is active when the outdoor air dry-bulb temperature falls below this setpoint temperature, as long as the heat pump is off. This set point temperature must be greater than or equal to 2ËšC, and the default value is 2ËšC if this field is left blank.
-
-#### Field: Basin Heater Operating Schedule Name
-
-This alpha field contains the name of the basin heater operating schedule. This field only applies for Condenser Type = EvaporativelyCooled. The basin heater operating schedule is assumed to be an on/off schedule and the heater is available to operate any time the schedule value is greater than 0. The basin heater operates when scheduled on and the outdoor air dry-bulb temperature is below the set point temperature described in the previous field. If this field is left blank, the basin heater is available to operate throughout the simulation. Regardless of this schedule, the basin heater may only operate when the heat pump is off.
-
-#### Field: Fuel Type
-
-This alpha field determines the type of fuel that this variable refrigerant flow system uses.  This field has seven choices: Electricity, NaturalGas, PropaneGas, Diesel, Gasoline, FuelOil\#1, FuelOil\#2, OtherFuel1, and OtherFuel2. The default is Electricity. The use of alternate fuel types assumes an engine drives the variable speed compression system and also accounts for condenser air flow (i.e., a fan attached to the engine provides air flow through the outdoor condenser.
-
-#### Field: Minimum Outdoor Temperature in Heat Recovery Mode
-
-This numeric field defines the minimum outdoor dry-bulb temperature allowed for heat recovery operation. Below this temperature, heat recovery is disabled. This input must be greater than the larger of the minimum outdoor temperature in cooling or heating mode. If this field is left blank, the default value is the higher of the Minimum Outdoor Temperature in Cooling Mode or Minimum Outdoor Temperature in Heating Mode inputs. This system may still operate in cooling or heating only mode when outdoor temperatures are below the minimum outdoor temperature in heat recovery mode. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes.
-
-#### Field: Maximum Outdoor Temperature in Heat Recovery Mode
-
-This numeric field defines the maximum outdoor dry-bulb temperature allowed for heat recovery operation. Above this temperature, heat recovery is disabled. This input must be less than the smaller of the maximum outdoor temperature in cooling or heating mode. If this field is left blank, the default value is the lower of the Maximum Outdoor Temperature in Cooling Mode or Maximum Outdoor Temperature in Heating Mode inputs.. This system may still operate in cooling or heating only mode when outdoor temperatures are above the maximum outdoor temperature in heat recovery mode. This input is only used when Heat Pump Waste Heat Recovery is selected as Yes.
-
-
-
-Following is an example input for a AirConditioner:VariableRefrigerantFlow system.
-
-
-
-```idf
-HVACTemplate:System:VRF,
-  VRF Heat Pump,        !- Name
-  VRFCondAvailSched,    !- Availability Schedule Name
-  autosize,             !- Gross Rated Total Cooling Capacity {W}
-  3.16038,              !- Gross Rated Cooling COP {W}
-  -5,                   !- Minimum Outdoor Temperature in Cooling Mode {C}
-  43,                   !- Maximum Outdoor Temperature in Cooling Mode {C}
-  autosize,             !- Gross Rated Heating Capacity {W}
-  ,                     !- Rated Heating Capacity Sizing Ratio (W/W)
-  3.40909,              !- Gross Rated Heating COP
-  -20,                  !- Minimum Outdoor Temperature in Heating Mode {C}
-  15.5,                 !- Maximum Outdoor Temperature in Heating Mode {C}
-  0.25,                 !- Minimum Heat Pump Part-Load Ratio
-  SPACE1-1,             !- Zone Name for Master Thermostat Location
-  LoadPriority,         !- Master Thermostat Priority Control Type
-  ,                     !- Thermostat Priority Schedule Name
-  No,                   !- Heat Pump Waste Heat Recovery
-  30,  !- Equivalent Piping Length . . . Factor in Cooling Mode {m}
-  10,  !- Vertical Height used for Piping Correction Factor {m}
-  30,  !- Equivalent Piping Length . . . Factor in Heating Mode {m}
-  15,  !- Crankcase Heater Power per Compressor {W}
-  3,   !- Number of Compressors
-  0.33,!- Ratio of Compressor Size to Total Compressor Capacity
-  7,   !- Maximum Outdoor Dry-bulb Temperature for Crankcase Heater {C}
-  Resistive,            !- Defrost Strategy
-  Timed,                !- Defrost Control
-  ,                     !- Defrost Time Period Fraction
-  autosize,             !- Resistive Defrost Heater Capacity {W}
-  7,   !- Maximum Outdoor Dry-bulb Temperature for Defrost Operation {C}
-  EvaporativelyCooled,  !- Condenser Type
-  MyVRFOANode,          !- Condenser Inlet Node Name
-  ,                     !- Condenser Outlet Node Name
-  ,                     !- Water Condenser Volume Flow Rate
-  ,             !- Evaporative Condenser Effectiveness {dimensionless}
-  autosize,     !- Evaporative Condenser Air Flow Rate {m3/s}
-  autosize,     !- Evaporative Condenser Pump Rated Power Consumption {W}
-  ,                     !- Supply Water Storage Tank Name
-  200,                  !- Basin Heater Capacity {W/K}
-  ,                     !- Basin Heater Set Point Temperature (C)
-  ,                     !- Basin Heater Operating Schedule Name
-  ,                     !- Fuel Type
-  ,    !- Minimum Outdoor Temperature in Heat Recovery Mode (C)
-  ;    !- Maximum Outdoor Temperature in Heat Recovery Mode (C)
-```
-
-
-
-### HVACTemplate:System:Unitary
-
-This object simulates the system portion of a constant volume air handler with electric, gas, or hot water heating and optional direct-expansion (DX) cooling. This system may serve one or more HVACTemplate:Zone:Unitary objects. If this system serves more than one zone, only one zone is specified as the control zone. Common names for this sytem type include packaged rooftop systems commonly seen in commercial buildings and split systems (furnace with air conditioner)  commonly seen in residential buildings.
-
-#### Field: Name
-
-Enter a name for the HVACTemplate:System:Unitary object. This name is used in the HVACTemplate:Zone:Unitary object to reference this system.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. If the "Supply Fan Operating Mode" (see below) is set to Cycling, then this is the supply fan operating schedule. If the fan mode is Cycling this is not a schedule of when the system is providing heating, cooling or air flow but a schedule of when it can provide either heating, cooling, or air flow.
-
-#### Field: Control Zone or Thermostat Location Name
-
-Enter the name of the HVACTemplate:Zone:Unitary object that contains the thermostat. While multiple HVACTemplate:Zone:Unitary objects can be part of a HVACTemplate:System:Unitary system, only one of the zones contains a thermostat that controls heating and cooling operation. For a single zone system, this field should contain the name of that zone.
-
-#### Field: Supply Fan Maximum Flow Rate
-
-Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m3/s.
-
-#### Field: Supply Fan Operating Mode Schedule Name
-
-This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.  If this field is left blank, a schedule of always zero (cycling fan) will be used.
-
-#### Field: Supply Fan Total Efficiency
-
-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
-
-#### Field: Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa.
-
-#### Field: Supply Fan Motor Efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Supply Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Cooling Coil Type
-
-Enter the type of cooling coil. The choices for this field are:
-
-- None
-
-- SingleSpeedDX
-
-Set this value to “SingleSpeedDX� if you want to simulate a system that provides cooling. You may set this value to “None� if no cooling is desired. The default value is SingleSpeedDX. Future versions may have additional cooling coil types.
-
-#### Field: Cooling Coil Availability Schedule Name
-
-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
-
-#### Field: Cooling Design Supply Air Temperature
-
-Enter the cooling supply air temperature in °C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8°C.
-
-#### Field: Cooling Coil Gross Rated Total Capacity
-
-Enter autosize to let the automatic sizing algorithm determine the cooling coil gross capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the “gross�, i.e.,  the effect of supply air fan heat is not accounted for. The units are in W.
-
-#### Field: Cooling Coil Gross Rated Sensible Heat Ratio
-
-Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the gross rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by the gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be “gross�, i.e., the effect of supply air fan heat is not accounted for.
-
-#### Field: Cooling Coil Gross Rated COP
-
-Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan.
-
-#### Field: Heating Coil Type
-
-Enter the type of heating used in the unitary system. The choices for this field are
-
-- Electric
-
-- Gas
-
-- HotWater
-
-#### Field: Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of 1.0 indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period
-
-#### Field: Heating Design Supply Air Temperature
-
-Enter the heating supply air temperature in °C to be used for sizing the heating coil and zone supply air flow rates. The default is 50°C.
-
-#### Field: Heating Coil Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the coil can deliver in Watts.
-
-#### Field: Gas Heating Coil Efficiency
-
-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default
-
-#### Field: Gas Heating Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas heating coil operation, such as a combustion fan. The units are in W.
-
-#### Field: Maximum Outdoor Air Flow Rate
-
-Enter autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100% of the full supply flow may be taken from outdoor air. If a value is entered, it is used instead of the autosize value. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
-
-#### Field: Minimum Outdoor Air Flow Rate
-
-Enter autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
-
-#### Field: Minimum Outdoor Air Schedule Name
-
-Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 – 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours.
-
-#### Field: Economizer Type
-
-The options for this field are
-
-- 'FixedDryBulb'
-
-- 'DifferentialDryBulb'
-
-- 'FixedEnthalpy'
-
-- 'DifferentialEnthalpy'
-
-- 'ElectronicEnthalpy' (i.e., humidity ratio curve strategy)
-
-- 'FixedDewPointAndDryBulb'
-
-- 'DifferentialDryBulbAndEnthalpy'
-
-- 'NoEconomizer'
-
-Choosing **NoEconomizer** means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
-
-Choosing **FixedDryBulb** means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
-
-Choosing **DifferentialDryBulb** will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
-
-**FixedEnthalpy** checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
-
-**DifferentialEnthalpy** does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
-
-Choosing **ElectronicEnthalpy** enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
-
-Choosing **FixedDewPointAndDryBulb** compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
-
-Another option **DifferentialDryBulbAndEnthalpy** enables the control strategy to be based on both the **DifferentialDryBulb** and **DifferentialEnthalpy** economizer control strategies.
-
-In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
-
-The default for this field is **NoEconomizer**.
-
-#### Field: Economizer Lockout
-
-Enter one of the following choices for this field:
-
-- NoLockout
-
-- LockoutWithHeating
-
-- LockoutWithCompressor
-
-The default value is **NoLockout**. The **LockoutWithHeating** means that if the packaged unit is in heating mode, the economizer is locked out – i.e., the economizer dampers are closed and there is minimum outdoor air flow. **LockoutWithCompressor** means that in addition to locking out the economizer when the unit is in heating mode the economizer is locked out when the DX unit compressor is on. In other words, when the DX coil is off, the economizer must meet the entire cooling load – it isn’t allowed to operate in conjunction with the DX cooling coil. Similarly, when the DX coil is operating, the economizer is not allowed to operate. The **LockoutWithCompressor** option is sometimes called a “nonintegrated� economizer.
-
-#### Field: Economizer Upper Temperature Limit
-
-Enter the outdoor air temperature high limit (<sup>o</sup>C) for economizer operation. If the outdoor air temperature is above this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature high limit control.
-
-#### Field: Economizer Lower Temperature Limit
-
-Enter the outdoor air temperature low limit (<sup>o</sup>C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
-
-#### Field: Economizer Upper Enthalpy Limit
-
-Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
-
-#### Field: Economizer Maximum Limit Dewpoint Temperature
-
-Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type ‘FixedDewPointAndDryBulb’ has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
-
-#### Field: Supply Plenum Name
-
-Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any supply plenums have been specified, the outlet from the system supply plenum will flow through the supply plenum to the zone terminal unit.
-
-#### Field: Return Plenum Name
-
-Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
-
-#### Field: Supply Fan Placement
-
-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *BlowThrough*.
-
-#### Field: Night Cycle Control
-
-Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are *StayOff*, *CycleOnAny*, or *CycleOnControlZone*. *StayOff* means the system will remain off, no matter how hot or cold the zones may be. *CycleOnAny* means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. *CycleOnControlZone* means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. The default is *StayOff*.
-
-#### Field: Night Cycle Control Zone Name
-
-For the Night Cycle Control option *CycleOnControlZone* enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
-
-#### Field: Heat Recovery Type
-
-Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
-
-- None
-
-- Sensible
-
-- Enthalpy
-
-The default is **None***.*
-
-#### Field: Sensible Heat Recovery Effectiveness
-
-Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
-
-#### Field: Latent Heat Recovery Effectiveness
-
-Enter the latent heat recovery effectiveness if Heat Recovery Type is *Enthalpy*. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
-
-#### Field: Dehumidification Control Type
-
-There are three dehumidification control type options available:
-
-- None
-
-- CoolReheatHeatingCoil
-
-- CoolReheatDesuperheater
-
-The *CoolReheatHeatingCoil* option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so.  Reheat is provided as required by the heating coil.  In the simulation, two instances of the heating coil are modeled, one for heating, and one for reheat.  The two coil objects represent the same physical coil and never operate simultaneously.
-
-The *CollReheatDesuperheater* option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so.  Reheat is provided by a desuperheater coil (see object Coil:Heating:Desuperheater).
-
-The default is *None* which meets the sensible cooling load only. The humidistat is located in the same zone that is specified above as the Control Zone or Thermostat Location Name.
-
-#### Field: Dehumidification Control Zone Name
-
-This field is deprecated and will be removed. The humidistat is located in the same zone that is specified above as the Control Zone or Thermostat Location Name.
-
-#### Field: Dehumidification Setpoint
-
-This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100).  The default is 60%.
-
-#### Field: Humidifier Type
-
-There are two humidifier type options available:
-
-- None
-
-- ElectricSteam
-
-The *ElectricSteam* humidifier option uses the Humidifier:Steam:Electric object.  The default is *None.*
-
-#### Field: Humidifier Availability Schedule Name
-
-If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
-
-#### Field: Humidifier Rated Capacity
-
-Enter the rated moisture output rate in m3/s.  The humidifier does not currently autosize, so the default is very large to allow for adequate capacity.  The default is 0.000001 m3/s.
-
-#### Field: Humidifier Rated Electric Power
-
-Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
-
-#### Field: Humidifier Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling humidification.
-
-#### Field: Humidifier Setpoint
-
-This field specifies the zone humidistat setpoint for humidification in percent (0 to 100).  The default is 30%.
-
-#### Field: Return Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 300 Pa.
-
-#### Field: Return Fan Motor efficiency
-
-Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. Default is 0.9.
-
-#### Field: Return Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. Default is 1.0.
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:System:Unitary,
-    AHU 1,                   !- Air Handling System Name
-    FanAndCoilAvailSched,    !- System Availability Schedule
-    EAST ZONE,               !- Control Zone Name or Thermostat Location
-    autosize,                !- Supply Fan Max Flow Rate {m3/s}
-    Fan Mode Schedule,       !- Supply Fan Operating Mode Schedule
-    .7,                      !- Supply Fan Total Efficiency
-    600,                     !- Supply Fan Delta Pressure {Pa}
-    .9,                      !- Supply Fan Motor Efficiency
-    1,                       !- Supply Fan Motor in Air Stream Fraction
-    SingleSspeedDX,          !- Cooling Coil Type
-    FanAndCoilAvailSched,    !- Cooling Coil Availability Schedule
-    14.0,                    !- Cooling Design Supply Air Temperature {C}
-    autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
-    autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
-    3,                       !- Cooling Coil Gross Rated COP
-    Gas,                     !- Heating Coil Type
-    FanAndCoilAvailSched,    !- Heating Coil Availability Schedule
-    50.0,                    !- Heating Design Supply Air Temperature {C}
-    autosize,                !- Heating Coil Capacity {W}
-    .8,                      !- Gas Heating Coil Efficiency
-    0,                       !- Gas Heating Coil Parasitic Electric Load {W}
-    autosize,                !- Maximum Outdoor air Flow Rate {m3/s}
-    autosize,                !- Minimum Outdoor air Flow Rate {m3/s}
-    ,                        !- Minimum Outdoor air Schedule Name
-    NoEconomizer,            !- Economizer Type
-    NoLockout,               !- Economizer Lockout
-    ,                        !- Economizer Upper Temperature Limit {C}
-    ,                        !- Economizer Lower Temperature Limit {C}
-    ,                        !- Economizer Upper Enthalpy Limit {J/kg}
-    ,                        !- Economizer Maximum Limit Dewpoint Temperature {C}
-    ,                        !- Supply Plenum Name
-    ,                        !- Return Plenum Name
-    BlowThrough,             !- Supply Fan Placement
-    CycleOnAny,              !- Night Cycle Control
-    ,                        !- Night Cycle Control Zone Name
-    None,                    !- Heat Recovery Type
-    ,                        !- Sensible Heat Recovery Effectiveness
-    ,                        !- Latent Heat Recovery Effectiveness
-    None,                    !- Dehumidification Control Type
-    ,                        !- Dehumidification Control Zone Name
-    60,                      !- Dehumidification Setpoint {percent}
-    ElectricSteam,           !- Humidifier Type
-    ,                        !- Humidifier Availability Schedule
-    0.000001,                !- Humidifier Rated Capacity {m3/s}
-    2690,                    !- Humidifier Rated Electric Power {W}
-    EAST ZONE,               !- Humidifier Control Zone Name
-    30,                      !- Humidifier Setpoint {percent}
-    No,                      !- Return Fan
-    0.7,                     !- Return Fan Total Efficiency
-    300,                     !- Return Fan Delta Pressure {Pa}
-    0.9,                     !- Return Fan Motor Efficiency
-    1.0;                     !- Return Fan Motor in Air Stream Fraction
-```
-
-
-### HVACTemplate:System:UnitaryHeatPump:AirToAir
-
-This object simulates the system portion of a constant volume air handler with a direct-expansion (DX) air-to-air heat pump and supplemental heating (electric, gas, or hot water). This system may serve one or more HVACTemplate:Zone:Unitary objects. If this system serves more than one zone, only one zone is specified as the control zone. Common names for this sytem type include packaged rooftop heat pumps commonly seen in commercial buildings and split system heat pumps commonly seen in residential buildings.
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-#### Field: Name
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-Enter a name for the HVACTemplate:System:UnitaryHeatPump:AirToAir object. This name is used in the HVACTemplate:Zone:Unitary object to reference this system.
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-#### Field: System Availability Schedule Name
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-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. During times when the system is available,  the supply fan operating mode controls fan operation. (See "Supply Fan Operating Mode Schedule Name" below)
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-#### Field: Control Zone or Thermostat Location Name
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-Enter the name of the HVACTemplate:Zone:Unitary object that contains the thermostat. While multiple HVACTemplate:Zone:Unitary objects can be part of a HVACTemplate:System:UnitaryHeatPump:AirToAir system, only one of the zones contains a thermostat that controls heating and cooling operation. For a single zone system, this field should contain the name of that zone.
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-#### Field: Cooling Supply Air Flow Rate
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-This field specifies the supply air flow rate when the DX cooling coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are in m3/s. The default is Autosize.
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-#### Field: Heating Supply Air Flow Rate
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-This field specifies the supply air flow rate when the heating coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are in m3/s. The default is Autosize.
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-#### Field: No Load Supply Air Flow Rate
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-This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner’s supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).  By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will *not* be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is Autosize.
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-#### Field: Supply Fan Operating Mode Schedule Name
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-This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.  If this field is left blank, a schedule of always zero (cycling fan) will be used.
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-#### Field: Supply Fan Placement
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-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the dx cooling/heating coil and before the supplemental heating coil. *BlowThrough* models a system where the supply air fan is before the dx cooling/heating coil and the  supplemental heating coil. The default is *BlowThrough*.
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-#### Field: Supply Fan Total Efficiency
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-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1.  The default is 0.7.
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-#### Field: Supply Fan Delta Pressure
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-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20 C at sea level, 101325 Pa. The default is 600 Pa.
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-#### Field: Supply Fan Motor Efficiency
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-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater or equal to the Supply Fan Total Efficiency and less than or equal to 1. The default is 0.9.
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-#### Field: Supply Fan Motor in Air Stream Fraction
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-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
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-#### Field: Cooling Coil Type
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-Enter the type of cooling coil. There is currently only one choices for this field,
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-SingleSpeedDX. Future versions may have additional cooling coil types.
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-#### Field: Cooling Coil Availability Schedule Name
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-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
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-#### Field: Cooling Design Supply Air Temperature
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-Enter the cooling supply air temperature in °C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8°C.
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-#### Field: Cooling Coil Gross Rated Total Capacity
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-Enter Autosize to let the automatic sizing algorithm determine the cooling coil capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the “gross� capacity where the effect of supply air fan heat is not accounted for. The units are in W. The default is Autosize.
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-#### Field: Cooling Coil Gross Rated Sensible Heat Ratio
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-Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by the gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be “gross� capacity where the effect of supply air fan heat is not accounted for. The default is Autosize.
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-#### Field: Cooling Coil Gross Rated COP
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-Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 3.0.
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-#### Field: Heat Pump Heating Coil Type
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-Enter the type of heat pump heating coil. There is currently only one choice for this field, SingleSpeedDXHeatPump.
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-#### Field: Heating Design Supply Air Temperature
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-Enter the heating supply air temperature in °C to be used for sizing the heating coil and zone supply air flow rates. The default is 50°C.
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-#### Field: Heat Pump Heating Coil Availability Schedule Name
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-Usually set to blank, which allows the heat pump heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. A schedule value of 1.0 indicates that the heat pump heating coil can be on during a given time period. A value of zero denotes that the heat pump heating coil cannot be used during that time period.
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-#### Field: Heat Pump Heating Coil Gross Rated Capacity
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-Enter Autosize to let the automatic sizing algorithm determine the heat pump heating coil gross capacity based on the maximum heating loads during the heating design day. If a value is entered, it represents the full load gross heating capacity, in watts of the DX heat pump unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. Capacity should be the “gross� capacity where the effect of supply air fan heat is not accounted for. The units are in W. The default is Autosize.
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-#### Field: Heat Pump Heating Coil Gross Rated COP
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-Enter the coefficient of performance defined as the gross heating coil capacity in watts divided by electrical power input in watts of the DX heating coil unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 2.75.
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-#### Field: Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature
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-This numeric field defines the minimum outdoor dry-bulb temperature in degrees Celsius for compressor operation. The compressor will not operate (for DX heating or DX cooling) when outdoor dry-bulb temperatures fall below this value. The minimum value must be greater than or equal to -20 °C. The default value is -8°C.
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-#### Field: Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature
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-This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 C and less than or equal to 7.22 C. If this input field is left blank, the default value is 5 C.
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-#### Field: Heat Pump Defrost Strategy
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-This alpha field has two choices: *ReverseCycle* or *Resistive*. If the *ReverseCycle* strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a *Resistive* defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is *ReverseCycle*.
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-#### Field: Heat Pump Defrost Control
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-This alpha field has two choices: *Timed* or *OnDemand*. If *Timed* control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For *Timed* defrost control, the fractional amount of time the unit is in defrost is entered in the input field “Defrost Time Period Fraction� described below. If *OnDemand* defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field “Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature� described above. If this input field is left blank, the default defrost control is *Timed*.
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-#### Field: Heat Pump Defrost Time Period Fraction
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-This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to “timed� defrost (see Heat Pump Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
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-#### Field: Supplemental Heating Coil Type
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-Enter the type of supplemental heating coil. The choices for this field are
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-- Electric
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-- Gas
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-- HotWater
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-The default is Electric.
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-#### Field: Supplemental Heating Coil Availability Schedule Name
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-Usually set to blank, which allows the supplemental heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when supplemental heating is only available seasonally. The schedule values denote whether the supplemental heating coil can run during a given time period. A schedule value of 1.0 indicates that the supplemental heating coil can be on during a given time period. A value of zero denotes that the supplemental heating coil cannot be used during that time period
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-#### Field: Supplemental Heating Coil Capacity
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-Enter Autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the supplemental heating coil can deliver in Watts. The default is Autosize.
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-#### Field: Supplemental Heating Coil Maximum Outdoor Dry-Bulb Temperature
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-This numeric field defines the outdoor air dry-bulb temperature above which the supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
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-#### Field: Supplemental Gas Heating Coil Efficiency
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-Enter supplemental heating coil gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default. This field applies only if the supplemental heating coil type is gas.
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-#### Field: Supplemental Gas Heating Coil Parasitic Electric Load
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-Enter the parasitic electric load associated with the gas supplemental heating coil operation, such as a combustion fan. The units are in W. The default is 0.0. This field applies only if the supplemental heating coil type is gas.
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-#### Field: Maximum Outdoor Air Flow Rate
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-Enter Autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100% of the full supply flow may be taken from outdoor air. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
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-#### Field: Minimum Outdoor Air Flow Rate
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-Enter Autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
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-#### Field: Minimum Outdoor Air Schedule Name
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-Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 – 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate during unoccupied or start up hours.
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-#### Field: Economizer Type
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-The options for this field are
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-- 'FixedDryBulb'
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-- 'DifferentialDryBulb'
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-- 'FixedEnthalpy'
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-- 'DifferentialEnthalpy'
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-- 'ElectronicEnthalpy' (i.e., humidity ratio curve strategy)
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-- 'FixedDewPointAndDryBulb'
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-- 'DifferentialDryBulbAndEnthalpy'
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-- 'NoEconomizer'
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-Choosing **NoEconomizer** means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
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-Choosing **FixedDryBulb** means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
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-Choosing **DifferentialDryBulb** will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
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-**FixedEnthalpy** checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
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-**DifferentialEnthalpy** does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
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-Choosing **ElectronicEnthalpy** enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
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-Choosing **FixedDewPointAndDryBulb** compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
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-Another option **DifferentialDryBulbAndEnthalpy** enables the control strategy to be based on both the **DifferentialDryBulb** and **DifferentialEnthalpy** economizer control strategies.
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-In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
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-The default for this field is **NoEconomizer**
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-#### Field: Economizer Lockout
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-Enter one of the following choices for this field:
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-- NoLockout
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-- LockoutWithHeating
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-- LockoutWithCompressor
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-The default value is **NoLockout**. The **LockoutWithHeating** means that if the packaged unit is in heating mode, the economizer is locked out – i.e., the economizer dampers are closed and there is minimum outdoor air flow. **LockoutWithCompressor** means that in addition to locking out the economizer when the unit is in heating mode the economizer is locked out when the DX unit compressor is on. In other words, when the DX coil is off, the economizer must meet the entire cooling load – it isn’t allowed to operate in conjunction with the DX cooling coil. Similarly, when the DX coil is operating, the economizer is not allowed to operate. The **LockoutWithCompressor** option is sometimes called a “nonintegrated� economizer.
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-#### Field: Economizer Maximum Limit Dry-Bulb Temperature
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-Input for this field is the outdoor air temperature high limit (ºC) for economizer operation. If the outdoor air temperature is above this limit, the outdoor airflow rate will be set to the minimum. This field is required if Economizer Control Type ‘FixedDryBulb’ or ‘FixedDewPointAndDryBulb’ has been specified. No input (blank) in this field means that there is no outdoor air temperature high limit control.
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-#### Field: Economizer Maximum Limit Enthalpy
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-Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
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-#### Field: Economizer Maximum Limit Dewpoint Temperature
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-Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type ‘FixedDewPointAndDryBulb’ has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
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-#### Field: Economizer Minimum Limit Dry-Bulb Temperature
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-Enter the outdoor air temperature low limit (C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
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-#### Field: Supply Plenum Name
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-Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any zone supply plenums have been specified, the outlet from the system supply plenum will flow through the zone supply plenum to the zone terminal unit.
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-#### Field: Return Plenum Name
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-Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
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-#### Field: Night Cycle Control
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-Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are *StayOff*, *CycleOnAny*, or *CycleOnControlZone*. *StayOff* means the system will remain off, no matter how hot or cold the zones may be. *CycleOnAny* means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. *CycleOnControlZone* means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. The default is *StayOff*.
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-#### Field: Night Cycle Control Zone Name
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-For the Night Cycle Control option *CycleOnControlZone* enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
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-#### Field: Heat Recovery Type
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-Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
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-- None
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-- Sensible
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-- Enthalpy
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-The default is **None***.*
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-#### Field: Sensible Heat Recovery Effectiveness
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-Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
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-#### Field: Latent Heat Recovery Effectiveness
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-Enter the latent heat recovery effectiveness if Heat Recovery Type is *Enthalpy*. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
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-#### Field: Humidifier Type
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-There are two humidifier type options available:
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-- None
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-- ElectricSteam
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-The *ElectricSteam* humidifier option uses the Humidifier:Steam:Electric object.  The default is *None.*
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-#### Field: Humidifier Availability Schedule Name
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-If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
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-#### Field: Humidifier Rated Capacity
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-Enter the rated moisture output rate in m3/s.  The humidifier does not currently autosize, so the default is very large to allow for adequate capacity.  The default is 0.000001 m3/s.
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-#### Field: Humidifier Rated Electric Power
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-Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
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-#### Field: Humidifier Control Zone Name
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-This field specifies the zone name where the humidistat is located for controlling humidification.
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-#### Field: Humidifier Setpoint
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-This field specifies the zone humidistat setpoint for humidification in percent (0 to 100).  The default is 30%.
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-#### Field: Return Fan Delta Pressure
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-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 300 Pa.
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-#### Field: Return Fan Motor efficiency
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-Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. Default is 0.9.
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-#### Field: Return Fan Motor in Air Stream Fraction
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-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. Default is 1.0.
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-As shown in an IDF:
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-```idf
-HVACTemplate:System:UnitaryHeatPump:AirToAir,
-    Heat Pump 1,             !- Name
-    FanAvailSched,           !- System Availability Schedule Name
-    SPACE1-1,                !- Control Zone or Thermostat Location Name
-    autosize,                !- Cooling Supply Air Flow Rate {m3/s}
-    autosize,                !- Heating Supply Air Flow Rate {m3/s}
-    autosize,                !- No Load Supply Air Flow Rate {m3/s}
-    ,                        !- Supply Fan Operating Mode Schedule Name
-    BlowThrough,             !- Supply Fan Placement
-    0.7,                     !- Supply Fan Total Efficiency
-    600,                     !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    1,                       !- Supply Fan Motor in Air Stream Fraction
-    SingleSpeedDX,           !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule Name
-    14,                      !- Cooling Design Supply Air Temperature {C}
-    autosize,                !- Cooling Coil Gross Rated TotalCapacity {W}
-    autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
-    3,                       !- Cooling Coil Gross Rated COP
-    SingleSpeedDXHeatPump,   !- Heat Pump Heating Coil Type
-    ,                    !- Heat Pump Heating Coil Availability Schedule Name
-    50.0,                    !- Heating Design Supply Air Temperature {C}
-    autosize,            !- Heat Pump Heating Coil Gross Rated Capacity {W}
-    2.75,                    !- Heat Pump Heating Coil Gross Rated COP
-    -8,         !- Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature {C}
-    5,          !- Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature {C}
-    ReverseCycle,            !- Heat Pump Defrost Strategy
-    Timed,                   !- Heat Pump Defrost Control
-    0.058333,                !- Heat Pump Defrost Time Period Fraction
-    Electric,                !- Supplemental Heating Coil Type
-    ,           !- Supplemental Heating Coil Availability Schedule Name
-    autosize,                !- Supplemental Heating Coil Capacity {W}
-    21,    !-  Supplemental Heating Coil Max Outdoor Dry-Bulb Temperature {C}
-    0.8,                     !- Supplemental Gas Heating Coil Efficiency
-    ,           !- Supplemental Gas Heating Coil Parasitic Electric Load {W}
-    autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
-    autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}
-    Min OA Sched,            !- Minimum Outdoor Air Schedule Name
-    DifferentialDryBulb,     !- Economizer Type
-    NoLockout,               !- Economizer Lockout
-    19,                 !- Economizer Maximum Limit Dry-Bulb Temperature {C}
-    ,                        !- Economizer Maximum Limit Enthalpy {J/kg}
-    ,                   !- Economizer Maximum Limit Dewpoint Temperature {C}
-    4,                  !- Economizer Minimum Limit Dry-Bulb Temperature {C}
-    ,                        !- Supply Plenum Name
-    ,                        !- Return Plenum Name
-    CycleOnAny,              !- Night Cycle Control
-    ,                        !- Night Cycle Control Zone Name
-    None,                    !- Heat Recovery Type
-    0.7,                     !- Sensible Heat Recovery Effectiveness
-    0.65,                    !- Latent Heat Recovery Effectiveness
-    None,                    !- Humidifier Type
-    ,                        !- Humidifier Availability Schedule Name
-    0.000001,                !- Humidifier Rated Capacity {m3/s}
-    2690,                    !- Humidifier Rated Electric Power {W}
-    ,                        !- Humidifier Control Zone Name
-    30,                      !- Humidifier Setpoint {percent}
-    No,                      !- Return Fan
-    0.7,                     !- Return Fan Total Efficiency
-    300,                     !- Return Fan Delta Pressure {Pa}
-    0.9,                     !- Return Fan Motor Efficiency
-    1.0;                     !- Return Fan Motor in Air Stream Fraction
-```
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-### HVACTemplate:System:UnitarySystem
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-This object simulates a unitary system with option cooling coil (air-cooled DX, water-cooled DX, and chilled water), options heating coil (gas, electric, hot water, air-to-air heat pump, and water-to-air heat pump) with cycling or continous fan controls. Often a single HVACTemplate:Zone:Unitary object will be used with a single HVACTemplate:System:UnitarySystem object to simulate single zone system. In addition, multiple HVACTemplate:Zone:Unitary objects may reference the same HVACTemplate:System:UnitarySystem object in a multiple zone version. For a multiple zone system, only one zone is specified as the control zone. The model can simulate chilled water or heat pump systems seen in commercial buildings and split systems commonly seen in residential buildings. HVACTemplate:System:UnitarySystem is similar to HVACTemplate:System:Unitary and HVACTemplate:System:UnitaryHeatPump:AirToAir, but it offers more flexilbility by using the more general AirLoopHVAC:UnitarySystem object instead of the more specific unitary furnace and heat pump objects.
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-#### Field: Name
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-Enter a name for the HVACTemplate:System:UnitarySystem object. This name is used in the HVACTemplate:Zone:Unitary object to reference this system.
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-#### Field: System Availability Schedule Name
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-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. During times when the system is available,  the supply fan operating mode controls fan operation. (See "Supply Fan Operating Mode Schedule Name" below)
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-#### Field: Control Type
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-This alpha field contains control type i.e. load based or setpoint based for the unitary system. Valid choices are *Load* and *SetPoint*. *Load* control requires a Controlling Zone name and *SetPoint* control is an advanced option which requires set points at each coil outlet node. A single set point at the outlet of the system is allowed but not recommended. The user must add the desired setpoint managers to the idf file. The default is *Load*.
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-#### Field: Control Zone or Thermostat Location Name
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-Enter the name of the HVACTemplate:Zone:Unitary object that contains the thermostat. While multiple HVACTemplate:Zone:Unitary objects can be part of a HVACTemplate:System:UnitarySystem system, only one of the zones contains a thermostat that controls heating and cooling operation. For a single zone system, this field should contain the name of that zone.
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-#### Field: Cooling Supply Air Flow Rate
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-This field specifies the supply air flow rate when the cooling coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified cooling SizingPeriod:DesignDay. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are in m3/s. The default is Autosize.
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-#### Field: Heating Supply Air Flow Rate
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-This field specifies the supply air flow rate when the heating coil is operating. By entering Autosize, the supply air flow rate is automatically determined based on the loads experienced by the zone during the specified heating SizingPeriod:DesignDay. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are in m3/s. The default is Autosize.
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-#### Field: No Load Supply Air Flow Rate
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-This field specifies the supply air flow rate when neither cooling nor heating is required (i.e., DX coil and heater are off but the supply air fan operates). This field is only used when the supply air fan operating mode schedule specifies continuous fan operation. Values must be greater than or equal to zero, or this field is autosizable. If the air conditioner’s supply air fan operating mode schedule specifies continuous fan operation and this value is set to zero or this field is left blank, then the model assumes that the supply air flow rate when no cooling/heating is needed is equal to the supply air flow rate when the cooling or heating coil was last operating (for cooling operation or heating operation).  By entering Autosize, the supply air flow rate will be sized to match the smaller of the Cooling and Heating flow rates. A value entered in this field will *not* be multiplied by the sizing factor or by zone multipliers. It is best to autosize or leave blank when using zone multipliers. The units are in m3/s. The default is Autosize.
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-#### Field: Supply Fan Operating Mode Schedule Name
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-This field specifies the name of the supply air fan operating mode schedule. The supply air fan operating mode may vary during the simulation based on time-of-day or with a change of season. Schedule values of 0 denote that the supply air fan and the heating or cooling coil cycle on and off together to meet the heating or cooling load (a.k.a. AUTO fan). Schedule values other than 0 denote that the supply fan runs continuously while the heating or cooling coil cycles to meet the load.  If this field is left blank, a schedule of always zero (cycling fan) will be used.
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-#### Field: Supply Fan Placement
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-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils and before the supplemental heating (or reheat) coil. *BlowThrough* models a system where the supply air fan is before all of the coils. The default is *BlowThrough*.
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-#### Field: Supply Fan Total Efficiency
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-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
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-#### Field: Supply Fan Delta Pressure
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-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20 C at sea level, 101325 Pa. The default is 600 Pa.
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-#### Field: Supply Fan Motor Efficiency
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-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater or equal to the Supply Fan Total Efficiency and less than or equal to 1. The default is 0.9.
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-#### Field: Supply Fan Motor in Air Stream Fraction
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-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
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-#### Field: Cooling Coil Type
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-There are seven coil types available:
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-- SingleSpeedDX (the default)
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-- TwoSpeedDX
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-- MultiSpeedDX
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-- TwoStageDX
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-- TwoStageHumidityControlDX
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-- HeatExchangerAssistedDX
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-- SingleSpeedDXWaterCooled
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-- ChilledWater
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-- ChilledWaterDetailedFlatModel
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-- HeatExchangerAssistedChilledWater
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-- None
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-*SingleSpeedDX* uses the Coil:Cooling:DX:SingleSpeed object.
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-*TwoSpeedDX* uses the Coil:Cooling:DX:TwoSpeed object.
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-*MultiSpeedDX* uses the Coil:Cooling:DX:MultiSpeed object.
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-*TwoStageDX* and *TwoStageHumidityControlDX*  use the Coil:Cooling:DX:TwoStageWithHumidityControlMode object.
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-*HeatExchangerAssistedDX* uses the CoilSystem:Cooling:DX:HeatExchangerAssisted, HeatExchanger:AirToAir:SensibleAndLatent, and Coil:Cooling:DX:SingleSpeed objects.
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-*SingleSpeedDXWaterCooled* uses the Coil:Cooling:WaterToAirHeatPump:EquationFit object. This option requires an HVACTemplate:Plant:MixedWaterLoop to serve as the water source.
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-The default type is *SingleSpeedDX*
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-*ChilledWater* uses the Coil:Cooling:Water object with the DetailedAnalysis option.  This is the preferred coil model for most chilled water applications.
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-*ChilledWaterDetailedFlatModel* uses the Coil:Cooling:Water:DetailedGeometry object.  This option is available for special applications.
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-*HeatExchangerAssistedChilledWater* uses the CoilSystem:Cooling:DX:HeatExchangerAssisted, HeatExchanger:AirToAir:SensibleAndLatent, and Coil:Cooling:Water objects.
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-#### Field: Number of Speeds for Cooling
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-This field defines the number of cooling speeds is a multi-speed cooling coil is specifiedl. The default is 1, and the maximum allowed is 10. This field only applies if Cooling Coil Type is MultiSpeedDX.
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-#### Field: Cooling Coil Availability Schedule Name
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-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1.0 indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
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-#### Field: Cooling Design Supply Air Temperature
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-Enter the cooling supply air temperature in °C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8°C.
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-#### Field: DX Cooling Coil Gross Rated Total Capacity
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-Enter Autosize to let the automatic sizing algorithm determine the cooling coil gross total cooling capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb. Capacity should be the “gross�, i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is Autosize. This field is only used when the cooling coil type is set to one of the DX options.  For two-speed DX coils, the low-speed capacity is assumed to be 0.33 times this value.  For two-stage DX coils, the stage 1 capacity is assumed to be 0.5 times this value.
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-#### Field: DX Cooling Coil Gross Rated Sensible Heat Ratio
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-Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the gross rated cooling total capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by gross total cooling capacity of the DX cooling coil at rated conditions. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be “gross�, i.e., the effect of supply air fan heat is not accounted for. This field is only used when the cooling coil type is set to one of the DX options. The default is Autosize.
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-For air-cooled DX coils the rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb.
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-For water-cooled DX coilst the rated conditions are 26.7C (80F) entering air dry-bulb temperature, 19.4C (67F) entering air wet-bulb temperature, and 29.4C (85F) entering water temperature.
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-For two-speed DX coils, the low-speed SHR is assumed to be equal to this value. For two-stage DX coils, the stage 1 SHR is assumed to be equal to this value. For two-stage DX coil with humidity control, the humidity control mode SHR is assumed to be 0.9 times this value (for both stage 1 and stage 2).
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-#### Field: DX Cooling Coil Gross Rated COP
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-Enter the coefficient of performance defined as the gross cooling coil total capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The default is 3.0. This field is only used when the cooling coil type is set to one of the DX options.  For two-speed DX coils, the low-speed COP is assumed to be 1.5 times this value.  For two-stage DX coils, the stage 1 COP is assumed to be this this value. For two-stage DX coil with humidity control, the humidity control mode COP is assumed to be 0.9 times this value (for both stage 1 and stage 2). The gross COP should not account for the supply air fan.
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-#### Field: Heating Coil Type
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-The heating coil is located in the supply air stream, downstream of the cooling coil. The choices for this field are
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-- Electric
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-- Gas
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-- HotWater
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-- SingleSpeedDXHeatPumpAirSource (air-to-air heat pump)
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-- MultiSpeedDXHeatPumpAirSource (air-to-air heat pump)
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-- SingleSpeedDXHeatPumpWaterSource (water-to-air heat pump). This option requires an HVACTemplate:Plant:MixedWaterLoop to serve as the water source.
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-- MultiStageElectric (uses coil object type Coil:Heating:Electric:MultiStage)
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-- MultiStageGas (uses coil object type Coil:Heating:Gas:MultiStage)
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-- None
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-The default value is Gas.
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-#### Field: Number of Speeds or Stages for Heating
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-This field defines the number of heating speeds or stages if a multi-speed heatpump or multi-stage heating coil is specifiedl. The default is 1. For heating coil type MultiSpeedDXHeatPumpAirSource, the maximum number of speeds allowed is 10. For heating coil types MultiStageElectric and MultiStageGas, the maximum number of stages allowed is 4. For other heating coil types, this field is ignored.
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-#### Field: Heating Coil Availability Schedule Name
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-Usually left blank, which allows the heating coil to be available as needed anytime the system is operating. If a schedule name is specified, it defines when the heating coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period.
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-#### Field: Heating Design Supply Air Temperature
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-Enter the heating supply air temperature in °C to be used for sizing the heating coil and zone supply air flow rates. The default is 50°C.
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-#### Field: Heating Coil Gross Rated Capacity
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-Enter Autosize to let the automatic sizing algorithm determine the heating coil gross capacity based on the maximum heating loads during the heating design day. The units are in W. The default is Autosize.
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-If the Heating Coil Type is Electric or Gas, this field is the rated output of the heating coil not including any effect of the supply air fan.
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-If the Heating Coil Type is HotWater, this field is the rated output of the heating coil not including any effect of the supply air fan at the following conditions: inlet water temperature is is 82.2 degrees C (180 degrees F), output water temperature is 71.1 degrees C (160 degrees F), inlet air temperature is 16.6 degrees C (60 degrees F), and outlet air temperature is 32.2 degrees C (90 degrees F).
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-If the Heating Coil Type is SingleSpeedDXHeatPumpAir this field represents the full load gross heating capacity, in watts of the DX heat pump unit at rated conditions. Rated conditions are air entering the heat pump heating coil at the heating supply air flow rate at 21.11°C drybulb/15.55°C wetbulb with air entering the outdoor coil at 8.33°C drybulb/6.11C wetbulb. Capacity should be the “gross� capacity where the effect of supply air fan heat is not accounted for.
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-If the Heating Coil Type is SingleSpeedDXHeatPumpWater this field represents the full load heating capacity, in watts of the DX heat pump unit at rated conditions (21.11C (70F) entering air dry-bulb temperature and 21.11C (70F) entering water temperature). Capacity should be the “gross�, i.e., the effect of supply air fan heat is not accounted for.
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-#### Field: Gas Heating Coil Efficiency
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-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default. This field applies only if the heating coil type is gas.
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-#### Field: Gas Heating Coil Parasitic Electric Load
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-Enter the parasitic electric load associated with the gas heating coil operation, such as a combustion fan. The units are in W. This field applies only if the heating coil type is gas.
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-#### Field: Heat Pump Heating Coil Gross Rated COP
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-Enter the coefficient of performance defined as the gross heating coil capacity in watts divided by electrical power input in watts of the DX heat pump heating coil unit at rated conditions. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 2.75 which is appropriate for an air-to-air heat pump. This value should be changed for a water-to-air heat pump. The rated conditions are described above under Heating Coil Gross Rated Capacity.
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-#### Field: Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature
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-This numeric field defines the minimum outdoor dry-bulb temperature in degrees Celsius for compressor operation. The compressor will not operate (for DX heating or DX cooling) when outdoor dry-bulb temperatures fall below this value. The minimum value must be greater than or equal to -20 °C. The default value is -8°C.
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-#### Field: Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature
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-This numeric field defines the outdoor air dry-bulb temperature above which outdoor coil defrosting is disabled. The temperature for this input field must be greater than or equal to 0 C and less than or equal to 7.22 C. If this input field is left blank, the default value is 5 C.
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-#### Field: Heat Pump Defrost Strategy
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-This alpha field has two choices: *ReverseCycle* or *Resistive*. If the *ReverseCycle* strategy is selected, the heating cycle is reversed periodically to provide heat to melt frost accumulated on the outdoor coil. If a *Resistive* defrost strategy is selected, the frost is melted using an electric resistance heater. If this input field is left blank, the default defrost strategy is *ReverseCycle*.
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-#### Field: Heat Pump Defrost Control
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-This alpha field has two choices: *Timed* or *OnDemand*. If *Timed* control is selected, the defrost time period is calculated based on a fixed value or compressor runtime whether or not frost has actually accumulated. For *Timed* defrost control, the fractional amount of time the unit is in defrost is entered in the input field “Defrost Time Period Fraction� described below. If *OnDemand* defrost control is selected, the defrost time period is calculated based on outdoor weather (humidity ratio) conditions. Regardless of which defrost control is selected, defrost does not occur above the user specified outdoor temperature entered in the input field “Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature� described above. If this input field is left blank, the default defrost control is *Timed*.
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-#### Field: Heat Pump Defrost Time Period Fraction
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-This numeric field defines the fraction of compressor runtime when the defrost cycle is active, and only applies to “timed� defrost (see Heat Pump Defrost Control input field above). For example, if the defrost cycle is active for 3.5 minutes for every 60 minutes of compressor runtime, then the user should enter 3.5/60 = 0.058333. The value for this input field must be greater than or equal to 0. If this input field is left blank, the default value is 0.058333.
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-#### Field: Supplemental Heating or Reheat Coil Type
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-Enter the type of supplemental heating coil or reheat coil. The choices for this field are
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-- Electric
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-- Gas
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-- HotWater
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-- DesuperHeater (applicable only if cooling coil type is air-cooled DX)
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-- None
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-The default is None.
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-#### Field: Supplemental Heating or Reheat Coil Availability Schedule Name
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-Usually set to blank, which allows the supplemental heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when supplemental heating is only available seasonally. The schedule values denote whether the supplemental heating coil can run during a given time period. A schedule value of 1.0 indicates that the supplemental heating coil can be on during a given time period. A value of zero denotes that the supplemental heating coil cannot be used during that time period
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-#### Field: Supplemental Heating or Reheat Coil Capacity
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-Enter Autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the supplemental heating coil can deliver in Watts. The default is Autosize.
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-#### Field: Supplemental Heating or Reheat Coil Maximum Outdoor Dry-Bulb Temperature
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-This numeric field defines the outdoor air dry-bulb temperature above which the supplemental heating coil is disabled. The temperature for this input field must be less than or equal to 21 C. If this input field is left blank, the default value is 21 C.
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-#### Field: Supplemental Gas Heating Coil Efficiency
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-Enter supplemental heating coil gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default. This field applies only if the supplemental heating coil type is gas.
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-#### Field: Supplemental Gas Heating Coil Parasitic Electric Load
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-Enter the parasitic electric load associated with the gas supplemental heating coil operation, such as a combustion fan. The units are in W. The default is 0.0. This field applies only if the supplemental heating coil type is gas.
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-#### Field: Maximum Outdoor Air Flow Rate
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-Enter Autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100% of the full supply flow may be taken from outdoor air. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template. The default is Autosize.
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-#### Field: Minimum Outdoor Air Flow Rate
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-Enter Autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
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-#### Field: Minimum Outdoor Air Schedule Name
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-Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 – 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate during unoccupied or start up hours.
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-#### Field: Economizer Type
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-The options for this field are
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-- ‘FixedDryBulb’
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-- ‘DifferentialDryBulb’
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-- ‘FixedEnthalpy’
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-- ‘DifferentialEnthalpy’
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-- ‘ElectronicEnthalpy’ (i.e., humidity ratio curve strategy)
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-- ‘FixedDewPointAndDryBulb’
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-- ‘DifferentialDryBulbAndEnthalpy’
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-- ‘NoEconomizer’
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-Choosing **NoEconomizer** means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
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-Choosing **FixedDryBulb** means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
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-Choosing **DifferentialDryBulb** will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
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-**FixedEnthalpy** checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
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-**DifferentialEnthalpy** does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
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-Choosing **ElectronicEnthalpy** enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
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-Choosing **FixedDewPointAndDryBulb** compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
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-Another option **DifferentialDryBulbAndEnthalpy** enables the control strategy to be based on both the **DifferentialDryBulb** and **DifferentialEnthalpy** economizer control strategies.
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-In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
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-The default for this field is **NoEconomizer**
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-#### Field: Economizer Lockout
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-Enter one of the following choices for this field:
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-- NoLockout
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-- LockoutWithHeating
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-- LockoutWithCompressor
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-The default value is **NoLockout**. The **LockoutWithHeating** means that if the packaged unit is in heating mode, the economizer is locked out – i.e., the economizer dampers are closed and there is minimum outdoor air flow. **LockoutWithCompressor** means that in addition to locking out the economizer when the unit is in heating mode the economizer is locked out when the DX unit compressor is on. In other words, when the DX coil is off, the economizer must meet the entire cooling load – it isn’t allowed to operate in conjunction with the DX cooling coil. Similarly, when the DX coil is operating, the economizer is not allowed to operate. The **LockoutWithCompressor** option is sometimes called a “nonintegrated� economizer.
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-#### Field: Economizer Maximum Limit Dry-Bulb Temperature
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-Input for this field is the outdoor air temperature high limit (ºC) for economizer operation. If the outdoor air temperature is above this limit, the outdoor airflow rate will be set to the minimum. This field is required if Economizer Control Type ‘FixedDryBulb’ or ‘FixedDewPointAndDryBulb’ has been specified. No input (blank) in this field means that there is no outdoor air temperature high limit control.
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-#### Field: Economizer Maximum Limit Enthalpy
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-Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
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-#### Field: Economizer Maximum Limit Dewpoint Temperature
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-Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type ‘FixedDewPointAndDryBulb’ has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
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-#### Field: Economizer Minimum Limit Dry-Bulb Temperature
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-Enter the outdoor air temperature low limit (C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
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-#### Field: Supply Plenum Name
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-Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any zone supply plenums have been specified, the outlet from the system supply plenum will flow through the zone supply plenum to the zone terminal unit.
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-#### Field: Return Plenum Name
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-Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
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-#### Field: Heat Recovery Type
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-Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
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-- None
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-- Sensible
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-- Enthalpy
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-The default is **None***.*
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-#### Field: Sensible Heat Recovery Effectiveness
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-Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
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-#### Field: Latent Heat Recovery Effectiveness
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-Enter the latent heat recovery effectiveness if Heat Recovery Type is *Enthalpy*. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
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-#### Field: Heat Recovery Heat Exchanger Type
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-This alpha field denotes the type of heat exchanger being modeled: Plate (e.g., fixed plate) or Rotary (e.g., rotating cylinder or wheel). The default choice for this field is “Plate�. The heat exchanger type affects the modeling of frost control options and supply air outlet temperature control. For rotary heat exchangers, rotational speed is varied to control frost formation or the supply air outlet temperature. For plate exchangers, air bypass around the heat exchanger is used to obtain the desired effect.
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-#### Field: Heat Recovery Frost Control Type
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-This alpha field has four choices: None, ExhaustAirRecirculation, ExhaustOnly and MinimumExhaustTemperature. If this field is left blank, the default frost control type is “None�. For modeling preheat frost control, specify “None� for this input field and insert a separate heating coil object in the supply inlet air stream to keep the air temperature above the desired frost threshold temperature.
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-*ExhaustAirRecirculation*: dampers are used to direct exhaust air back into the zone through the supply side of the heat exchanger when the supply (outdoor) air inlet temperature falls below a threshold temperature. The fraction of time that exhaust air is circulated through the supply side of the heat exchanger is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When exhaust air is being recirculated, no supply (outdoor ventilation) air is being provided through the heat exchanger unit (which may or may not be acceptable regarding ventilation for occupants).
-
-*ExhaustOnly (supply air bypass)*: this control cycles off the supply air flow through the heat exchanger for a certain period of time while the exhaust air continues to flow through the exhaust side of the heat exchanger. The fraction of time that the supply flow through the heat exchanger is cycled off is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When implemented in real applications, provisions are usually made to avoid building depressurization when this frost control is operating (automatic or pressure-operated dampers, or a bypass air damper around the supply side of the heat exchanger). For this frost control type, it is assumed that the supply air is bypassed around the heat exchanger during frost control operation (i.e., the total supply flow is not reduced during defrost, but merely bypassed around the heat exchanger).
-
-*MinimumExhaustTemperature*: the temperature of the exhaust air leaving the heat exchanger is monitored and the heat exchanger effectiveness is decreased (by slowing heat exchanger rotation or bypassing supply air around the plate exchanger) to keep the exhaust air from falling below the threshold temperature.
-
-#### Field: Dehumidification Control Type
-
-There are three dehumidification control type options available:
-
-- None
-
-- CoolReheat
-
-- Multimode
-
-The *CoolReheat* option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so.  Reheat is provided as required by the reheat coil. In the simulation, two instances of the heating coil are modeled, even if the main heating coil acts as the reheat coil in the actual system.
-
-*Multimode* is only applicable for cooling coil type *TwoStageHumidityControlDX*. In this case, the enhanced dehumidification mode is activated as needed, but the system operates to meet the sensible dry-bulb temperature cooling setpoint.
-
-The default is *None* which meets the sensible cooling load only. The humidistat is located in the same zone that is specified above as the Control Zone or Thermostat Location Name.
-
-#### Field: Dehumidification Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling dehumidification.
-
-#### Field: Dehumidification Relative Humidity Setpoint
-
-This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100).  The default is 60%. This field is ignored if a Dehumidification Relative Humidity Setpoint Schedule Name is specified.
-
-#### Field: Dehumidification Relative Humidity Setpoint Schedule Name
-
-Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint,  The values in the schedule are in percent (0 to 100).
-
-#### Field: Humidifier Type
-
-There are two humidifier type options available:
-
-- None
-
-- ElectricSteam
-
-The *ElectricSteam* humidifier option uses the Humidifier:Steam:Electric object.  The default is *None.*
-
-#### Field: Humidifier Availability Schedule Name
-
-If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
-
-#### Field: Humidifier Rated Capacity
-
-Enter the rated moisture output rate in m3/s.  The humidifier does not currently autosize, so the default is very large to allow for adequate capacity.  The default is 0.000001 m3/s.
-
-#### Field: Humidifier Rated Electric Power
-
-Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
-
-#### Field: Humidifier Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling humidification.
-
-#### Field: Humidifier Relative Humidity Setpoint
-
-This field specifies the zone humidistat setpoint for humidification in percent (0 to 100).  The default is 30%. This field is ignored if a Humidifier Relative Humidity Setpoint Schedule Name is specified.
-
-#### Field: Humidifier Relative Humidity Setpoint Schedule Name
-
-Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint,  The values in the schedule are in percent (0 to 100).
-
-#### Field: Sizing Option
-
-This field specifies the sizing method for the system supply air flow rate. *Coincident* sizes on the sum of the coincident zone supply air flow rates. *NonCoincident* sizes on sum of the noncoincident zone design supply air flow rates. The default is *NonCoincident*.
-
-#### Field: Return Fan
-
-Enter *Yes* if the system has a return fan. The default is *No*.
-
-#### Field: Return Fan Total Efficiency
-
-Enter the total efficiency of the return fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1. Default is 0.7.
-
-#### Field: Return Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 300 Pa.
-
-#### Field: Return Fan Motor efficiency
-
-Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. Default is 0.9.
-
-#### Field: Return Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. Default is 1.0.
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:System:UnitarySystem,
-    AHU 1,                   !- Name
-    FanAvailSched,           !- System Availability Schedule Name
-    Load,                    !- Control Type
-    SPACE1-1,                !- Control Zone or Thermostat Location Name
-    autosize,                !- Cooling Supply Air Flow Rate {m3/s}
-    autosize,                !- Heating Supply Air Flow Rate {m3/s}
-    autosize,                !- No Load Supply Air Flow Rate {m3/s}
-    FanModeSchedule,         !- Supply Fan Operating Mode Schedule Name
-    BlowThrough,             !- Supply Fan Placement
-    0.7,                     !- Supply Fan Total Efficiency
-    600,                     !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    1,                       !- Supply Fan Motor in Air Stream Fraction
-    SingleSpeedDX,           !- Cooling Coil Type
-    1,                       !- Number of Speeds for Cooling
-    ,                        !- Cooling Coil Availability Schedule Name
-    12.8,                    !- Cooling Design Supply Air Temperature {C}
-    autosize,                !- DX Cooling Coil Gross Rated Total Capacity{W}
-    autosize,            !- DX Cooling Coil Gross Rated Sensible Heat Ratio
-    3,                       !- DX Cooling Coil Gross Rated COP
-    Gas,                     !- Heating Coil Type
-    1,                       !- Number of Speeds for Heating
-    ,                        !- Heating Coil Availability Schedule Name
-    50.0,                    !- Heating Design Supply Air Temperature {C}
-    autosize,                !- Heating Coil Gross Rated Capacity{W}
-    .8,                      !- Gas Heating Coil Efficiency
-    0,                       !- Gas Heating Coil Parasitic Electric Load {W}
-    2.75,                    !- Heat Pump Heating Coil Gross Rated COP
-    -8,         !- Heat Pump Heating Minimum Outdoor Dry-Bulb Temperature {C}
-    5,          !- Heat Pump Defrost Maximum Outdoor Dry-Bulb Temperature {C}
-    ReverseCycle,            !- Heat Pump Defrost Strategy
-    Timed,                   !- Heat Pump Defrost Control
-    0.058333,                !- Heat Pump Defrost Time Period Fraction
-    Electric,                !- Supplemental Heating or Reheat Coil Type
-    ,     !- Supplemental Heating  or ReheatCoil Availability Schedule Name
-    autosize,         !- Supplemental Heating or Reheat Coil Capacity {W}
-    21,   !-  Supplemental Heating or Reheat Coil Max . . . Temperature {C}
-    0.8,  !- Supplemental Gas Heating or Reheat Coil Efficiency
-    ,     !- Supplemental Gas Heating or Reheat Coil Parasitic . . . Load {W}
-    autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
-    autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}
-    Min OA Sched,            !- Minimum Outdoor Air Schedule Name
-    DifferentialDryBulb,     !- Economizer Type
-    NoLockout,               !- Economizer Lockout
-    19,                 !- Economizer Maximum Limit Dry-Bulb Temperature {C}
-    ,                   !- Economizer Maximum Limit Enthalpy {J/kg}
-    ,                   !- Economizer Maximum Limit Dewpoint Temperature {C}
-    4,                  !- Economizer Minimum Limit Dry-Bulb Temperature {C}
-    ,                        !- Supply Plenum Name
-    ,                        !- Return Plenum Name
-    None,                    !- Heat Recovery Type
-    0.7,                     !- Sensible Heat Recovery Effectiveness
-    0.65,                    !- Latent Heat Recovery Effectiveness
-    ,                        !- Heat Recovery Heat Exchanger Type
-    ,                        !- Heat Recovery Frost Control Type
-    None,                    !- Dehumidification Control Type
-    ,                        !- Dehumidification Control Zone Name
-    60.0,       !- Dehumidification Relative Humidity Setpoint {percent}
-    ,           !- Dehumidification Relative Humidity Setpoint Schedule Name
-    None,                    !- Humidifier Type
-    ,                        !- Humidifier Availability Schedule Name
-    0.000001,                !- Humidifier Rated Capacity {m3/s}
-    2690.0,                  !- Humidifier Rated Electric Power {W}
-    ,                        !- Humidifier Control Zone Name
-    30.0,       !- Humidifier Relative Humidity Setpoint {percent}
-    ,           !- Humidifier Relative Humidity Setpoint Schedule Name
-    No,                      !- Return Fan
-    0.7,                     !- Return Fan Total Efficiency
-     300,                     !- Return Fan Delta Pressure {Pa}
-     0.9,                     !- Return Fan Motor Efficiency
-     1.0;                     !- Return Fan Motor in Air Stream Fraction
-```
-
-
-### HVACTemplate:System:VAV
-
-This object simulates the system portion of a variable air volume HVAC configuration with chilled water cooling and several different heating options. Multiple HVACTemplate:Zone:VAV objects are usually specified for each HVACTemplate:System:VAV object.
-
-#### Field: Name
-
-Enter a name for the HVACTemplate:System:VAV object. This name is used in the HVACTemplate:Zone:VAV object to reference this system.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. Please note that for this system type, this is a schedule of when the system is providing air flow.
-
-#### Field: Supply Fan Maximum Flow Rate
-
-Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m<sup>3</sup>/s.
-
-#### Field: Supply Fan Minimum Flow Rate
-
-Enter the minimum supply air volume that may be provided. This field may be set to autosize. The units are in m<sup>3</sup>/s.
-
-#### Field: Supply Fan Total Efficiency
-
-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
-
-#### Field: Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 1000 Pa.
-
-#### Field: Supply Fan Motor efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Supply Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Cooling Coil Type
-
-There are two coil types available:
-
-- ChilledWater
-
-- ChilledWaterDetailedFlatModel
-
-*ChilledWater* uses the COIL:Cooling:Water object with the DetailedAnalysis option.  This is the preferred coil model for most applications.  *ChilledWaterDetailedFlatModel* uses the Coil:Cooling:Water:DetailedGeometry object.  This option is available for special applications.  The default is *ChilledWater*.
-
-#### Field: Cooling Coil Availability Schedule Name
-
-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of one indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
-
-#### Field: Cooling Coil Setpoint Schedule Name
-
-If a constant setpoint for the cooling coil is to be specified, leave this field blank, and the Cooling Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the cooling coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the cooling coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Cooling Coil Setpoint Reset Type is something other than None (see below).
-
-#### Field: Cooling Coil Design Setpoint
-
-Enter the cooling supply air temperature in C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8C. If no Cooling Coil Setpoint Schedule or Cooling Coil Setpoint Reset Type is specified, this value is used as a constant cooling supply air setpoint temperature.
-
-#### Field: Heating Coil Type
-
-The heating coil is located in the supply air stream, upstream of the cooling coil and after the outdoor air mixing box. If no central heating coil is used in the VAV system,  then the option “none� should be specified here. Otherwise this indicates the type of heating coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
-
-- HotWater
-
-- Electric
-
-- Gas
-
-- None
-
-The default value is None. Note that the configuration of HVACTemplate:System:VAV assumes that there will be reheat coils or baseboard heating to provide heating control at the zone level. If a heating coil is specified, the heating and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
-
-#### Field: Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period
-
-#### Field: Heating Coil Setpoint Schedule Name
-
-If a constant setpoint for the heating coil is to be specified, leave this field blank, and the Heating Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the heating coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the heating coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Heating Coil Setpoint Reset Type is something other than None (see below).
-
-#### Field: Heating Coil Design Setpoint
-
-Enter the heating supply air temperature in C to be used for sizing the heating coil and zone supply air flow rates. If no Heating Coil Setpoint Schedule or Heating Coil Setpoint Reset Type is specified, this value is used as a constant heating supply air setpoint temperature.  The default is 10.0C.
-
-#### Field: Gas Heating Coil Efficiency
-
-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default
-
-#### Field: Gas Heating Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas heating operation, such as a combustion fan. The units are in W.
-
-#### Field: Preheat Coil Type
-
-The preheat coil is located in the outdoor air stream, upstream of the outdoor air mixing box and tempers the outdoor air. If no preheat coil is used in the VAV system, then the option “none� should be specified here. Otherwise this indicates the type of preheat coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
-
-- HotWater
-
-- Electric
-
-- Gas
-
-- None
-
-The default value is None. If a preheat coil is specified, the preheat and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
-
-#### Field: Preheat Coil Availability Schedule Name
-
-Usually set to blank, which allows the preheat coil to be available anytime the system is operating. If a schedule name is specified, it defines when the preheat coil is available. This is most often used when preheat is only available seasonally. The schedule values denote whether the preheat coil can run during a given time period. A schedule value of 1.0 indicates that the preheat coil can be on during a given time period. A value of zero denotes that the preheat coil cannot be used during that time period
-
-#### Field: Preheat Coil Setpoint Schedule Name
-
-If a constant setpoint for the preheat coil is to be specified, leave this field blank, and the Preheat Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the preheat coil specify the schedule name here. The schedule should control the leaving air temperature from the preheat coil. The values in the schedule are in degrees C.
-
-#### Field: Preheat Coil Design Setpoint
-
-Enter the preheat supply air temperature in C to be used for sizing the preheat coil. If no Preheat Coil Setpoint Schedule is specified, this value is used as a constant preheat supply air setpoint temperature. The default is 7.2C.
-
-#### Field: Gas Preheat Coil Efficiency
-
-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default
-
-#### Field: Gas Preheat Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas heating operation, such as an combustion fan. The units are in W.
-
-#### Field: Maximum Outdoor Air Flow Rate
-
-Enter autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100% of the full supply flow may be taken from outdoor air. If a value is entered, it is used instead of the autosize value. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
-
-#### Field: Minimum Outdoor Air Flow Rate
-
-Enter autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air  specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
-
-#### Field: Minimum Outdoor Air Control Type
-
-Choices for this field are **FixedMinimum** or **ProportionalMinimum**. FixedMinimum means that the minimum outdoor air flow rate is fixed no matter what the actual system flow rate is. ProportionalMinimum means the minimum outdoor air flow rate varies in proportion to the total system air flow rate. The default is ProportionalMinimum.
-
-#### Field: Minimum Outdoor Air Schedule Name Name
-
-Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 – 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours.
-
-#### Field: Economizer Type
-
-The options for this field are
-
-- ‘FixedDryBulb’
-
-- ‘DifferentialDryBulb’
-
-- ‘FixedEnthalpy’
-
-- ‘ DifferentialEnthalpy’
-
-- ‘ElectronicEnthalpy’ (i.e., humidity ratio curve strategy)
-
-- ‘FixedDewPointAndDryBulb’
-
-- ‘DifferentialDryBulbAndEnthalpy’
-
-- ‘NoEconomizer’
-
-Choosing **NoEconomizer** means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
-
-Choosing **FixedDryBulb** means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
-
-Choosing **DifferentialDryBulb** will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
-
-**FixedEnthalpy** checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
-
-**DifferentialEnthalpy** does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
-
-Choosing **ElectronicEnthalpy** enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
-
-Choosing **FixedDewPointAndDryBulb** compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
-
-Another option **DifferentialDryBulbAndEnthalpy** enables the control strategy to be based on both the **DifferentialDryBulb** and **DifferentialEnthalpy** economizer control strategies.
-
-In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
-
-The default for this field is **NoEconomizer**.
-
-#### Field: Economizer Lockout
-
-The only choice for this field is
-
-- NoLockout
-
-The default value is NoLockout. Future versions may have additional options.
-
-#### Field: Economizer Upper Temperature Limit
-
-Enter the outdoor air temperature high limit (<sup>o</sup>C) for economizer operation. If the outdoor air temperature is above this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature high limit control.
-
-#### Field: Economizer Lower Temperature Limit
-
-Enter the outdoor air temperature low limit (<sup>o</sup>C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
-
-#### Field: Economizer Upper Enthalpy Limit
-
-Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
-
-#### Field: Economizer Maximum Limit Dewpoint Temperature
-
-Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type ‘FixedDewPointAndDryBulb’ has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
-
-#### Field: Supply Plenum Name
-
-Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any supply plenums have been specified, the outlet from the system supply plenum will flow through the supply plenum to the zone terminal unit.
-
-#### Field: Return Plenum Name
-
-Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
-
-#### Field: Supply Fan Placement
-
-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *Draw Through*.
-
-#### Field: Supply Fan Part-Load Power Coefficients
-
-Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
-
-- InletVaneDampers
-
-- OutletDampers
-
-- VariableSpeedMotor
-
-- ASHRAE90.1-2004Appendix G
-
-- VariableSpeedMotorPressureReset
-
-The default is *InletVaneDampers*. The resulting power curves are shown in Figure 158. VAV Supply Fan Part-Load Power Coefficient Options below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The *VariableSpeedMotorPressureReset* option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources’: *Design Guidelines: Advanced Variable Air Volume (VAV) Systems* (EDR\_DesignGuidelines\_VAV.pdf).
-
-![](media/image611.svg)
-
-Figure 158. VAV Supply Fan Part-Load Power Coefficient Options
-
-#### Field: Night Cycle Control
-
-Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are *StayOff*, *CycleOnAny*, *CycleOnControl Zone or CycleOnAnyZoneFansOnly*. *StayOff* means the system will remain off, no matter how hot or cold the zones may be. *CycleOnAny* means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. *CycleOnControlZone* means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. *CycleOnAnyZoneFansOnly* is the same as *CycleOnAny* except that only the zone fans are cycled on and the central air handler fan is left off (applicable only if using HVACTemplate:Zone:VAV:FanPowered in one or more zones). The default is *StayOff*.
-
-#### Field: Night Cycle Control Zone Name
-
-For the Night Cycle Control option *Cycle On Control Zone* enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
-
-#### Field: Heat Recovery Type
-
-Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
-
-- None
-
-- Sensible
-
-- Enthalpy
-
-The default is **None***.*
-
-#### Field: Sensible Heat Recovery Effectiveness
-
-Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
-
-#### Field: Latent Heat Recovery Effectiveness
-
-Enter the latent heat recovery effectiveness if Heat Recovery Type is *Enthalpy*. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
-
-#### Field: Cooling Coil Setpoint Reset Type
-
-Select the type of automatic reset control for the cooling supply air temperature. The choices are:
-
-- None – no reset, use the Cooling Coil Setpoint Schedule or Cooling Coil Design Setpoint.
-
-- Warmest – reset the cooling supply air temperature to the highest supply air temperature that will meet the cooling requirements of all the zones at the maximum supply air flow rate. The minimum setpoint allowed is the Cooling Coil Design Setpoint. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:Warmest)
-
-- OutdoorAirTemperatureReset – reset the cooling supply air temperature based on the following default rules. When the outdoor dry-bulb temperature (ODB) is at or below 15.6C the setpoint is the Cooling Coil Design Setpoint plus 5.2C. When the ODB is at or above 26.7C the setpoint is the Cooling Coil Design Setpoint. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset)
-
-- WarmestTemperatureFirst – find the highest setpoint temperature that will satisfy all the zone cooling loads at minimum supply air flow rate. If this setpoint temperature is less than the Cooling Coil Design Setpoint, the setpoint temperature is set to the minimum, and the supply air flow rate is increased to meet the loads. This option is appropriate when modeling a single-zone VAV system. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:WarmestTemperatureFlow)
-
-The default is *None*.
-
-#### Field: Heating Coil Setpoint Reset Type
-
-Select the type of automatic reset control for the central heating supply air temperature. The choices are:
-
-- None – no reset, use the Heating Coil Setpoint Schedule or Heating Coil Design Setpoint.
-
-- OutdoorAirTemperatureReset – reset the heating supply air temperature based on the following default rules. When the outdoor dry-bulb temperature (ODB) is at or below –6.7C the setpoint is the Heating Coil Design Setpoint. When the ODB is at or above 10.0C the setpoint is the Heating Coil Design Setpoint minus 5.2C. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset).
-
-The default is *None*.
-
-#### Field: Dehumidification Control Type
-
-There are two dehumidification control type options available:
-
-- None
-
-- CoolReheat
-
-The *CoolReheat* option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so.  Reheat is provided as required by the terminal unit reheat coils if available.
-
-The default is *None* which meets the sensible cooling setpoint only.
-
-#### Field: Dehumidification Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling dehumidification.
-
-#### Field: Dehumidification Setpoint
-
-This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100).  The default is 60%.
-
-#### Field: Humidifier Type
-
-There are two humidifier type options available:
-
-- None
-
-- ElectricSteam
-
-The *ElectricSteam* humidifier option uses the Humidifier:Steam:Electric object.  The default is *None.*
-
-#### Field: Humidifier Availability Schedule Name
-
-If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
-
-#### Field: Humidifier Rated Capacity
-
-Enter the rated moisture output rate in m3/s.  The humidifier does not currently autosize, so the default is very large to allow for adequate capacity.  The default is 0.000001 m3/s.
-
-#### Field: Humidifier Rated Electric Power
-
-Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
-
-#### Field: Humidifier Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling humidification.
-
-#### Field: Humidifier Setpoint
-
-This field specifies the zone humidistat setpoint for humidification in percent (0 to 100).  The default is 30%.
-
-#### Field: Sizing Option
-
-This field specifies the sizing method for the system supply air flow rate. *Coincident* sizes on the sum of the coincident zone supply air flow rates. *NonCoincident* sizes on sum of the noncoincident zone design supply air flow rates. The default is *NonCoincident*.
-
-#### Field: Return Fan
-
-Enter *Yes* if the system has a return fan. The default is *No*.
-
-#### Field: Return Fan Total Efficiency
-
-Enter the total efficiency of the return fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Return Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 500 Pa.
-
-#### Field: Return Fan Motor efficiency
-
-Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Return Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Return Fan Part-Load Power Coefficients
-
-Select the set of generic pre-defined coefficients to use for the return fan part-load power consumption. This alpha field has the following choices:
-
-- InletVaneDampers
-
-- OutletDampers
-
-- VariableSpeedMotor
-
-- ASHRAE90.1-2004Appendix G
-
-- VariableSpeedMotorPressureReset
-
-The default is *InletVaneDampers*. The resulting power curves are shown in Figure 158. VAV Supply Fan Part-Load Power Coefficient Options (see Supply Fan Part-Load Power Coefficients above). The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The *VariableSpeedMotorPressureReset* option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources’: *Design Guidelines: Advanced Variable Air Volume (VAV) Systems* (EDR\_DesignGuidelines\_VAV.pdf).
-
-
-
-As shown in an IDF:
-
-```idf
-  HVACTemplate:System:VAV,
-    VAV Sys 1,               !-Name
-    FanAvailSched,           !- System Availability Schedule Name
-    autosize,                !- Supply Fan Maximum Flow Rate {m3/s}
-    autosize,                !- Supply Fan Minimum Flow Rate {m3/s}
-    0.7,                     !- Supply Fan Total Efficiency
-    600,                     !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    1,                       !- Supply Fan Motor in Air Stream Fraction
-    ChilledWater,            !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule Name
-    ,                        !- Cooling Coil Setpoint Schedule Name
-    12.8,                    !- Cooling Coil Design Setpoint {C}
-    HotWater,                !- Heating Coil Type
-    ,                        !- Heating Coil Availability Schedule Name
-    ,                        !- Heating Coil Setpoint Schedule Name
-    10.0,                    !- Heating Coil Design Setpoint {C}
-    0.8,                     !- Gas Heating Coil Efficiency
-    0.0,                     !- Gas Heating Coil Parasitic Electric Load {W}
-    None,                    !- Preheat Coil Type
-    ,                        !- Preheat Coil Availability Schedule Name
-    ,                        !- Preheat Coil Setpoint Schedule Name
-    ,                        !- Preheat Coil Design Setpoint {C}
-    0.8,                     !- Gas Preheat Coil Efficiency
-    0.0,                     !- Gas Preheat Coil Parasitic Electric Load {W}
-    autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
-    autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}
-    FixedMinimum,            !- Minimum Outdoor Air Control Type
-    Min OA Sched,            !- Minimum Outdoor Air Schedule Name
-    DifferentialDryBulb,     !- Economizer Type
-    NoLockout,               !- Economizer Lockout
-    19,                      !- Economizer Upper Temperature Limit {C}
-    4,                       !- Economizer Lower Temperature Limit {C}
-    ,                        !- Economizer Upper Enthalpy Limit {J/kg}
-    ,                    !- Economizer Maximum Limit Dewpoint Temperature {C}
-   ,                        !- Supply Plenum Name
-    PLENUM-1,                !- Return Plenum Name
-    DrawThrough,             !- Supply Fan Placement
-    InletVaneDampers,        !- Supply Fan Part-Load Power Coefficients
-    CycleOnAnyZoneFansOnly,  !- Night Cycle Control
-    ,                        !- Night Cycle Control Zone Name
-    None,                    !- Heat Recovery Type
-    0.70,                    !- Sensible Heat Recovery Effectiveness
-    0.65,                    !- Latent Heat Recovery Effectiveness
-    None,                    !- Cooling Coil Setpoint Reset Type
-    None,                    !- Heating Coil Setpoint Reset Type
-    None,                    !- Dehumidification Control Type
-    ,                        !- Dehumidification Control Zone Name
-    60.0,                    !- Dehumidification Setpoint {percent}
-    None,                    !- Humidifier Type
-    ,                        !- Humidifier Availability Schedule Name
-    0.000001,                !- Humidifier Rated Capacity {m3/s}
-    2690.0,                  !- Humidifier Rated Electric Power {W}
-    ,                        !- Humidifier Control Zone Name
-    30.0,                    !- Humidifier Setpoint {percent}
-    NonCoincident,           !- Sizing Option
-    No,                      !- Return Fan
-    0.7,                     !- Return Fan Total Efficiency
-    500,                     !- Return Fan Delta Pressure {Pa}
-    0.9,                     !- Return Fan Motor Efficiency
-    1.0,                     !- Return Fan Motor in Air Stream Fraction
-    InletVaneDampers;        !- Return Fan Part-Load Power Coefficients
-```
-
-
-### HVACTemplate:System:PackagedVAV
-
-This object simulates the system portion of a packaged direct-expansion based variable air volume HVAC configuration with several different heating options. Multiple HVACTemplate:Zone:VAV objects are usually specified for each HVACTemplate:System:PackagedVAV object.
-
-#### Field: Name
-
-Enter a name for the HVACTemplate:System:PackagedVAV object. This name is used in the HVACTemplate:Zone:VAV object to reference this system.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. Please note that for this system type, this is a schedule of when the system is providing air flow.
-
-#### Field: Supply Fan Maximum Flow Rate
-
-Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m<sup>3</sup>/s. The default is Autosize.
-
-#### Field: Supply Fan Minimum Flow Rate
-
-Enter the minimum supply air volume that may be provided. This field may be set to autosize. The units are in m<sup>3</sup>/s.
-
-#### Field: Supply Fan Placement
-
-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *DrawThrough*.
-
-#### Field: Supply Fan Total Efficiency
-
-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1.  The default is 0.7.
-
-#### Field: Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 1000 Pa.
-
-#### Field: Supply Fan Motor Efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater or equal to the Supply Fan Total Efficiency and less than or equal to 1. The default is 0.9.
-
-#### Field: Supply Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. The default is 1.0.
-
-#### Field: Cooling Coil Type
-
-The coil types available:
-
-- TwoSpeedDX
-
-- TwoSpeedHumidControlDX
-
-*TwoSpeedDX*  uses the Coil:Cooling:DX:TwoSpeed object.  This is the preferred coil model for most applications.  The *TwoSpeedHumidControlDX*  option uses the Coil:Cooling:DX:TwoStageWithHumidityControlMode object.
-
-#### Field: Cooling Coil Availability Schedule Name
-
-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of one indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
-
-#### Field: Cooling Coil Setpoint Schedule Name
-
-If a constant setpoint for the cooling coil is to be specified, leave this field blank, and the Cooling Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the cooling coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the cooling coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Cooling Coil Setpoint Reset Type is something other than None (see below). The default is None.
-
-#### Field: Cooling Coil Design Setpoint
-
-Enter the cooling supply air temperature in degrees C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8C. If no Cooling Coil Setpoint Schedule or Cooling Coil Setpoint Reset Type is specified, this value is used as a constant cooling supply air setpoint temperature.
-
-#### Field: Cooling Coil Gross Rated Total Capacity
-
-Enter Autosize to let the automatic sizing algorithm determine the cooling coil gross rated total capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. For Cooling Coil Type = TwoSpeedDX, the low-speed capacity is assumed to be 0.33 times this value. For Cooling Coil Type = TwoSpeedHumidControlDX, the stage 1 capacity is assumed to be 0.5 times this value. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Capacity should be the “gross�, i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is Autosize.
-
-#### Field: Cooling Coil Gross Rated Sensible Heat Ratio
-
-Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the rated capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by the gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be “gross�, i.e., the effect of supply air fan heat is not accounted for.  The default is Autosize.
-
-#### Field: Cooling Coil Gross Rated COP
-
-Enter the coefficient of performance defined as the gross cooling coil capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The gross COP should not account for the supply air fan. The default is 3.0.
-
-#### Field: Heating Coil Type
-
-Enter the type of heating used in the unitary system. The choices for this field are
-
-- Electric
-
-- Gas
-
-- HotWater
-
-#### Field: Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of 1.0 indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period
-
-#### Field: Heating Coil Setpoint Schedule Name
-
-If a constant setpoint for the heating coil is to be specified, leave this field blank, and the Heating Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the heating coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the heating coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Heating Coil Setpoint Reset Type is something other than None (see below).
-
-#### Field: Heating Coil Design Setpoint
-
-Enter the heating supply air temperature in degrees C to be used for sizing the heating coil and zone supply air flow rates. If no Heating Coil Setpoint Schedule or Heating Coil Setpoint Reset Type is specified, this value is used as a constant heating supply air setpoint temperature.  The default is 10.0C.
-
-#### Field: Heating Coil Capacity
-
-Enter Autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the coil can deliver in Watts.
-
-#### Field: Gas Heating Coil Efficiency
-
-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default
-
-#### Field: Gas Heating Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas heating coil operation, such as a combustion fan. The units are in W. The default is 0.0 W.
-
-#### Field: Maximum Outdoor Air Flow Rate
-
-Enter Autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100% of the full supply flow may be taken from outdoor air. If a value is entered, it is used instead of the autosize value. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template. The default is Autosize.
-
-#### Field: Minimum Outdoor Air Flow Rate
-
-Enter Autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air  specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
-
-#### Field: Minimum Outdoor Air Control Type
-
-Choices for this field are **FixedMinimum** or **ProportionalMinimum**. FixedMinimum means that the minimum outdoor air flow rate is fixed no matter what the actual system flow rate is. ProportionalMinimum means the minimum outdoor air flow rate varies in proportion to the total system air flow rate. The default is ProportionalMinimum.
-
-#### Field: Minimum Outdoor Air Schedule Name
-
-Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 – 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours.
-
-#### Field: Economizer Type
-
-The options for this field are
-
-- ‘FixedDryBulb’
-
-- ‘DifferentialDryBulb’
-
-- ‘FixedEnthalpy’
-
-- ‘DifferentialEnthalpy’
-
-- ‘ElectronicEnthalpy’ (i.e., humidity ratio curve strategy)
-
-- ‘FixedDewPointAndDryBulb’
-
-- ‘DifferentialDryBulbAndEnthalpy’
-
-- ‘NoEconomizer’
-
-Choosing **NoEconomizer** means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
-
-Choosing **FixedDryBulb** means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
-
-Choosing **DifferentialDryBulb** will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
-
-**FixedEnthalpy** checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
-
-**DifferentialEnthalpy** does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
-
-Choosing **ElectronicEnthalpy** enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
-
-Choosing **FixedDewPointAndDryBulb** compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
-
-Another option **DifferentialDryBulbAndEnthalpy** enables the control strategy to be based on both the **DifferentialDryBulb** and **DifferentialEnthalpy** economizer control strategies.
-
-In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
-
-The default for this field is **NoEconomizer**.
-
-#### Field: Economizer Lockout
-
-Enter one of the following choices for this field:
-
-- NoLockout
-
-- LockoutWithHeating
-
-- LockoutWithCompressor
-
-The default value is **NoLockout**. The **LockoutWithHeating** means that if the packaged unit is in heating mode, the economizer is locked out – i.e., the economizer dampers are closed and there is minimum outdoor air flow. **LockoutWithCompressor** means that in addition to locking out the economizer when the unit is in heating mode the economizer is locked out when the DX unit compressor is on. In other words, when the DX coil is off, the economizer must meet the entire cooling load – it isn’t allowed to operate in conjunction with the DX cooling coil. Similarly, when the DX coil is operating, the economizer is not allowed to operate. The **LockoutWithCompressor** option is sometimes called a “nonintegrated� economizer.
-
-#### Field: Economizer Maximum Limit Dry-Bulb Temperature
-
-Input for this field is the outdoor air temperature high limit (ºC) for economizer operation. If the outdoor air temperature is above this limit, the outdoor airflow rate will be set to the minimum. This field is required if Economizer Control Type ‘FixedDryBulb’ or ‘FixedDewPointAndDryBulb’ has been specified. No input (blank) in this field means that there is no outdoor air temperature high limit control.
-
-#### Field: Economizer Maximum Limit Enthalpy
-
-Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
-
-#### Field: Economizer Maximum Limit Dewpoint Temperature
-
-Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type ‘FixedDewPointAndDryBulb’ has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
-
-#### Field: Economizer Minimum Limit Dry-Bulb Temperature
-
-Enter the outdoor air temperature low limit (C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
-
-#### Field: Supply Plenum Name
-
-Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any zone supply plenums have been specified, the outlet from the system supply plenum will flow through the zone supply plenum to the zone terminal unit.
-
-#### Field: Return Plenum Name
-
-Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
-
-#### Field: Supply Fan Part-Load Power Coefficients
-
-Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
-
-- InletVaneDampers
-
-- OutletDampers
-
-- VariableSpeedMotor
-
-- ASHRAE90.1-2004Appendix G
-
-- VariableSpeedMotorPressureReset
-
-The default is *InletVaneDampers*. The resulting power curves are shown in Figure 159 below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table.  The *VariableSpeedMotorPressureReset* option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources’: *Design Guidelines: Advanced Variable Air Volume (VAV) Systems* (EDR\_DesignGuidelines\_VAV.pdf).
-
-![](media/image612.svg)
-
-Figure 159. VAV Supply Fan Part-Load Power Coefficient Options
-
-#### Field: Night Cycle Control
-
-Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are *StayOff*, *CycleOnAny*, *CycleOnControl Zone or CycleOnAnyZoneFansOnly*. *StayOff* means the system will remain off, no matter how hot or cold the zones may be. *CycleOnAny* means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. *CycleOnControlZone* means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. *CycleOnAnyZoneFansOnly* is the same as *CycleOnAny* except that only the zone fans are cycled on and the central air handler fan is left off (applicable only if using HVACTemplate:Zone:VAV:FanPowered in one or more zones). The default is *StayOff*.
-
-#### Field: Night Cycle Control Zone Name
-
-For the Night Cycle Control option *Cycle On Control Zone* enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
-
-#### Field: Heat Recovery Type
-
-Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
-
-- None
-
-- Sensible
-
-- Enthalpy
-
-The default is **None***.*
-
-#### Field: Sensible Heat Recovery Effectiveness
-
-Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
-
-#### Field: Latent Heat Recovery Effectiveness
-
-Enter the latent heat recovery effectiveness if Heat Recovery Type is *Enthalpy*. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
-
-#### Field: Cooling Coil Setpoint Reset Type
-
-Select the type of automatic reset control for the cooling supply air temperature. The choices are:
-
-- None – no reset, use the Cooling Coil Setpoint Schedule or Cooling Coil Design Setpoint.
-
-- Warmest – reset the cooling supply air temperature to the highest supply air temperature that will meet the cooling requirements of all the zones at the maximum supply air flow rate. The minimum setpoint allowed is the Cooling Coil Design Setpoint. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:Warmest)
-
-- OutdoorAirTemperatureReset – reset the cooling supply air temperature based on the following default rules. When the outdoor dry-bulb temperature (ODB) is at or below 15.6C the setpoint isthe Cooling Coil Design Setpoint plus 5.2C. When the ODB is at or above 26.7C the setpoint is the Cooling Coil Design Setpoint. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset)
-
-- WarmestTemperatureFirst – find the highest setpoint temperature that will satisfy all the zone cooling loads at minimum supply air flow rate. If this setpoint temperature is less than the Cooling Coil Design Setpoint, the setpoint temperature is set to the minimum, and the supply air flow rate is increased to meet the loads. This option is appropriate when modeling a single-zone VAV system. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:WarmestTemperatureFlow)
-
-The default is *None*.
-
-#### Field: Heating Coil Setpoint Reset Type
-
-Select the type of automatic reset control for the central heating supply air temperature. The choices are:
-
-- None – no reset, use the Heating Coil Setpoint Schedule or Heating Coil Design Setpoint.
-
-- OutdoorAirTemperatureReset – reset the heating supply air temperature based on the following default rules. When the outdoor dry-bulb temperature (ODB) is at or below –6.7C the setpoint is the Heating Coil Design Setpoint. When the ODB is at or above 10.0C the setpoint isthe Heating Coil Design Setpoint minus 5.2C. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset).
-
-The default is *None*.
-
-#### Field: Dehumidification Control Type
-
-There are two dehumidification control type options available:
-
-- None
-
-- CoolReheat
-
-The *CoolReheat* option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so.  Reheat is provided as required by the terminal unit reheat coils if available.
-
-The default is *None* which meets the sensible cooling setpoint only.
-
-#### Field: Dehumidification Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling dehumidification.
-
-#### Field: Dehumidification Setpoint
-
-This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100).  The default is 60%.
-
-#### Field: Humidifier Type
-
-There are two humidifier type options available:
-
-- None
-
-- ElectricSteam
-
-The *ElectricSteam* humidifier option uses the Humidifier:Steam:Electric object.  The default is *None.*
-
-#### Field: Humidifier Availability Schedule Name
-
-If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
-
-#### Field: Humidifier Rated Capacity
-
-Enter the rated moisture output rate in m3/s.  The humidifier does not currently autosize, so the default is very large to allow for adequate capacity.  The default is 0.000001 m3/s.
-
-#### Field: Humidifier Rated Electric Power
-
-Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
-
-#### Field: Humidifier Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling humidification.
-
-#### Field: Humidifier Setpoint
-
-This field specifies the zone humidistat setpoint for humidification in percent (0 to 100).  The default is 30%.
-
-#### Field: Sizing Option
-
-This field specifies the sizing method for the system supply air flow rate. *Coincident* sizes on the sum of the coincident zone supply air flow rates. *NonCoincident* sizes on sum of the noncoincident zone design supply air flow rates. The default is *NonCoincident*.
-
-#### Field: Return Fan
-
-Enter *Yes* if the system has a return fan. The default is *No*.
-
-#### Field: Return Fan Total Efficiency
-
-Enter the total efficiency of the return fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Return Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 500 Pa.
-
-#### Field: Return Fan Motor efficiency
-
-Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Return Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Return Fan Part-Load Power Coefficients
-
-Select the set of generic pre-defined coefficients to use for the return fan part-load power consumption. This alpha field has the following choices:
-
-- InletVaneDampers
-
-- OutletDampers
-
-- VariableSpeedMotor
-
-- ASHRAE90.1-2004Appendix G
-
-- VariableSpeedMotorPressureReset
-
-The default is *InletVaneDampers*. The resulting power curves are shown in Figure 158. VAV Supply Fan Part-Load Power Coefficient Options (see Supply Fan Part-Load Power Coefficients above). The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The *VariableSpeedMotorPressureReset* option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources’: *Design Guidelines: Advanced Variable Air Volume (VAV) Systems* (EDR\_DesignGuidelines\_VAV.pdf).
-
-
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:System:PackagedVAV,
-    DXVAV Sys 1,             !-Name
-    FanAvailSched,           !- System Availability Schedule Name
-    autosize,                !- Supply Fan Maximum Flow Rate {m3/s}
-    autosize,                !- Supply Fan Minimum Flow Rate {m3/s}
-    DrawThrough,             !- Supply Fan Placement
-    0.7,                     !- Supply Fan Total Efficiency
-    1000,                    !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    1,                       !- Supply Fan Motor in Air Stream Fraction
-    TwoSpeedDX,              !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule Name
-    ,                        !- Cooling Coil Setpoint Schedule Name
-    12.8,                    !- Cooling Coil Design Setpoint {C}
-    autosize,                !- Cooling Coil Gross Rated Total Capacity {W}
-    autosize,                !- Cooling Coil Gross Rated Sensible Heat Ratio
-    3,                       !- Cooling Coil Gross Rated COP
-    Gas,                     !- Heating Coil Type
-    ,                        !- Heating Coil Availability Schedule Name
-    ,                        !- Heating Coil Setpoint Schedule Name
-    10,                      !- Heating Coil Design Setpoint {C}
-    autosize,                !- Heating Coil Capacity {W}
-    0.8,                     !- Gas Heating Coil Efficiency
-    ,                        !- Gas Heating Coil Parasitic Electric Load {W}
-    autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
-    autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}
-    ProportionalMinimum,     !- Minimum Outdoor Air Control Type
-    Min OA Sched,            !- Minimum Outdoor Air Schedule Name
-    DifferentialDryBulb,     !- Economizer Type
-    NoLockout,               !- Economizer Lockout
-    19,                  !- Economizer Maximum Limit Dry-Bulb Temperature {C}
-    ,                        !- Economizer Maximum Limit Enthalpy {J/kg}
-    ,                    !- Economizer Maximum Limit Dewpoint Temperature {C}
-    4,                   !- Economizer Minimum Limit Dry-Bulb Temperature {C}
-    ,                        !- Supply Plenum Name
-    PLENUM-1,                !- Return Plenum Name
-    InletVaneDampers,        !- Supply Fan Part-Load Power Coefficients
-    CycleOnAny,              !- Night Cycle Control
-    ,                        !- Night Cycle Control Zone Name
-    None,                    !- Heat Recovery Type
-    0.7,                     !- Sensible Heat Recovery Effectiveness
-    0.65,                    !- Latent Heat Recovery Effectiveness
-    None,                    !- Cooling Coil Setpoint Reset Type
-    None,                    !- Heating Coil Setpoint Reset Type
-    None,                    !- Dehumidification Control Type
-    ,                        !- Dehumidification Control Zone Name
-    60,                      !- Dehumidification Setpoint {percent}
-    None,                    !- Humidifier Type
-   ,                        !- Humidifier Availability Schedule Name
-    0.000001,                !- Humidifier Rated Capacity {m3/s}
-    2690,                    !- Humidifier Rated Electric Power {W}
-    ,                        !- Humidifier Control Zone Name
-    30,                      !- Humidifier Setpoint {percent}
-    NonCoincident,           !- Sizing Option
-    No,                      !- Return Fan
-    0.7,                     !- Return Fan Total Efficiency
-    500,                     !- Return Fan Delta Pressure {Pa}
-    0.9,                     !- Return Fan Motor Efficiency
-    1.0,                     !- Return Fan Motor in Air Stream Fraction
-    InletVaneDampers;        !- Return Fan Part-Load Power Coefficients
-```
-
-### HVACTemplate:System:ConstantVolume
-
-This object simulates the system portion of a constant air volume HVAC configuration with option chilled water cooling and several different heating options. One or more  HVACTemplate:Zone:ConstantVolume objects are specified for each zone served by the HVACTemplate:System:ConstantVolume object.
-
-#### Field: Name
-
-Enter a name for the HVACTemplate:System:ConstantVolume object. This name is used in the HVACTemplate:Zone:ConstantVolume object to reference this system.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. Please note that for this system type, this is a schedule of when the system is providing air flow.
-
-#### Field: Supply Fan Maximum Flow Rate
-
-Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m<sup>3</sup>/s.
-
-#### Field: Supply Fan Total Efficiency
-
-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
-
-#### Field: Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 600 Pa.
-
-#### Field: Supply Fan Motor Efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Supply Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Supply Fan Placement
-
-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *Draw Through*.
-
-#### Field: Cooling Coil Type
-
-There are two coil types available:
-
-- ChilledWater
-
-- ChilledWaterDetailedFlatModel
-
-- HeatExchangerAssistedChilledWater
-
-- None
-
-*ChilledWater* uses the COIL:Cooling:Water object with the DetailedAnalysis option.  This is the preferred coil model for most applications.  *ChilledWaterDetailedFlatModel* uses the Coil:Cooling:Water:DetailedGeometry object.  This option is available for special applications.  *HeatExchangerAssistedChilledWater* uses the CoilSystem:Cooling:Water:HeatExchangerAssisted, HeatExchanger:AirToAir:SensibleAndLatent, and Coil:Cooling:Water objects. The default is *ChilledWater*.
-
-#### Field: Cooling Coil Availability Schedule Name
-
-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1 indicates that the cooling coil can be on during a given time period. A value of 0 denotes that the cooling coil cannot be used during that time period.
-
-#### Field: Cooling Coil Setpoint Control Type
-
-Specifies the cooling coil setpoint control type:
-
-- FixedSetpoint - uses the Cooling Coil Design Setpoint as the supply air setpoint.
-
-- Scheduled - uses the Cooling Coil Design Setpoint as the supply air setpoint.
-
-- OutdoorAirTemperatureReset - varies the supply air setpoint based on the values entered for Cooling Coil Setpoint at Outdoor Dry-Bulb Low, Cooling Coil Reset Outdoor Dry-Bulb Low, Cooling Coil Setpoint at Outdoor Dry-Bulb High, and Cooling Coil Reset Outdoor Dry-Bulb High.
-
-- Warmest – resets the cooling supply air temperature to the highest supply air temperature that will meet the cooling requirements of all the zones. The minimum setpoint allowed is the Cooling Coil Design Setpoint. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:Warmest)
-
-- ControlZone – controls the supply air temperature to meet the current cooling load for the zone specified as the Cooling Coil Control Zone Name (below). The minimum setpoint is the Cooling Coil Design Setpoint. The maximum setpoint allowed is defaulted to the greater of 18C or the Heating Coil Design Setpoint plus 1.0C. (Reference SetpointManager:SingleZone:Cooling)
-
-The default is *FixedSetpoint*.
-
-NOTE: The user must ensure that the cooling coil and heating coil setpoints do not overlap to avoid unwanted simultaneous heating and cooling. The simulation will not check this automatically. It is recommended that the cooling setpoint always be at least 0.1C higher than the heating coil setpoint.
-
-#### Field: Cooling Coil Control Zone Name
-
-If the Cooling Coil Setpoint Control Type is ControlZone, enter the name of the HVACTemplate:Zone:ConstantVolume object that contains the cooling thermostat.
-
-#### Field: Cooling Coil Design Setpoint Temperature
-
-Enter the cooling supply air temperature in C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8C. If no Cooling Coil Setpoint Schedule or Cooling Coil Setpoint Reset Type is specified, this value is used as a constant cooling supply air setpoint temperature.
-
-#### Field: Cooling Coil Setpoint Schedule Name
-
-If a constant setpoint for the cooling coil is to be specified, leave this field blank, and the Cooling Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the cooling coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the cooling coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Cooling Coil Setpoint Reset Type is something other than None (see above).
-
-#### Field: Cooling Coil Setpoint at Outdoor Dry-Bulb Low
-
-The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Cooling Coil Reset Outdoor Dry-Bulb Low). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
-
-#### Field: Cooling Coil Reset Outdoor Dry-Bulb Low
-
-The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
-
-#### Field: Cooling Coil Setpoint at Outdoor Dry-Bulb High
-
-The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Cooling Coil Reset Outdoor Dry-Bulb High). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.8C.
-
-#### Field: Cooling Coil Reset Outdoor Dry-Bulb High
-
-The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb High. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 23.3C.
-
-#### Field: Heating Coil Type
-
-The heating coil is located in the supply air stream, upstream of the cooling coil and after the outdoor air mixing box. If no central heating coil is used in the Constant Volume system,  then the option “none� should be specified here. Otherwise this indicates the type of heating coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
-
-- HotWater
-
-- Electric
-
-- Gas
-
-- None
-
-The default value is *HotWater*. Note that the configuration of HVACTemplate:System:ConstantVolume assumes that there will be reheat coils or baseboard heating to provide heating control at the zone level. If a heating coil is specified, the heating and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
-
-#### Field: Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period.
-
-#### Field: Heating Coil Setpoint Control Type
-
-Specifies the heating coil setpoint control type:
-
-- FixedSetpoint - uses the Heating Coil Design Setpoint as the supply air setpoint.
-
-- Scheduled - uses the Heating Coil Setpoint Schedule to set the supply air setpoint.
-
-- OutdoorAirTemperatureReset - varies the supply air setpoint based on the values entered for Heating Coil Setpoint at Outdoor Dry-Bulb Low, Heating Coil Reset Outdoor Dry-Bulb Low, Heating Coil Setpoint at Outdoor Dry-Bulb High, and Heating Coil Reset Outdoor Dry-Bulb High.
-
-- ControlZone - controls the supply air temperature to meet the current heating load for the zone specified as the Heating Coil Control Zone Name (below). The maximum setpoint is the Heating Coil Design Setpoint. The minimum setpoint allowed is defaulted to the lesser of the Heating Coil Design Setpoint minus 5.2C or the Cooling Coil Design Setpoint minus 1.0C. (Reference SetpointManager:SingleZone:Heating)
-
-The default is FixedSetpoint.
-
-NOTE: The user must ensure that the cooling coil and heating coil setpoints do not overlap to avoid unwanted simultaneous heating and cooling. The simulation will not check this automatically. It is recommended that the cooling setpoint always be at least 0.1C higher than the heating coil setpoint.
-
-#### Field: Heating Coil Control Zone Name
-
-Enter the name of the HVACTemplate:Zone:ConstantVolume object that contains the heating thermostat. While multiple HVACTemplate:Zone:ConstantVolume objects can be part of a HVACTemplate:System:ConstantVolume system, only one of the zones contains a thermostat that controls heating operation. For a single zone system, this field should contain the name of that zone.
-
-#### Field: Heating Coil Design Setpoint
-
-Enter the heating supply air temperature in C to be used for sizing the heating coil and zone supply air flow rates. If no Heating Coil Setpoint Schedule or Heating Coil Setpoint Reset Type is specified, this value is used as a constant heating supply air setpoint temperature.  The default is 10.0C.
-
-#### Field: Heating Coil Setpoint Schedule Name
-
-If a constant setpoint for the heating coil is to be specified, leave this field blank, and the Heating Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the heating coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the heating coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Heating Coil Setpoint Reset Type is something other than None (see above).
-
-#### Field: Heating Coil Setpoint at Outdoor Dry-Bulb Low
-
-The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Heating Coil Reset Outdoor Dry-Bulb Low). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.0C.
-
-#### Field: Heating Coil Reset Outdoor Dry-Bulb Low
-
-The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 7.8C.
-
-#### Field: Heating Coil Setpoint at Outdoor Dry-Bulb High
-
-The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Heating Coil Reset Outdoor Dry-Bulb High). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.2C.
-
-#### Field: Heating Coil Reset Outdoor Dry-Bulb High
-
-The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb High. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.2C.
-
-#### Field: Heating Coil Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the coil can deliver in Watts.
-
-#### Field: Gas Heating Coil Efficiency
-
-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default
-
-#### Field: Gas Heating Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas heating operation, such as a combustion fan. The units are in W.
-
-#### Field: Preheat Coil Type
-
-The preheat coil is located in the outdoor air stream, upstream of the outdoor air mixing box and tempers the outdoor air. If no preheat coil is used in the constant volume system, then the option “none� should be specified here. Otherwise this indicates the type of preheat coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
-
-- HotWater
-
-- Electric
-
-- Gas
-
-- None
-
-The default value is None. If a preheat coil is specified, the preheat and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
-
-#### Field: Preheat Coil Availability Schedule Name
-
-Usually set to blank, which allows the preheat coil to be available anytime the system is operating. If a schedule name is specified, it defines when the preheat coil is available. This is most often used when preheat is only available seasonally. The schedule values denote whether the preheat coil can run during a given time period. A schedule value of 1.0 indicates that the preheat coil can be on during a given time period. A value of zero denotes that the preheat coil cannot be used during that time period
-
-#### Field: Preheat Coil Design Setpoint
-
-Enter the preheat supply air temperature in C to be used for sizing the preheat coil. If no Preheat Coil Setpoint Schedule is specified, this value is used as a constant preheat supply air setpoint temperature. The default is 7.2C.
-
-#### Field: Preheat Coil Setpoint Schedule Name
-
-If a constant setpoint for the preheat coil is to be specified, leave this field blank, and the Preheat Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the preheat coil specify the schedule name here. The schedule should control the leaving air temperature from the preheat coil. The values in the schedule are in degrees C.
-
-#### Field: Gas Preheat Coil Efficiency
-
-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default
-
-#### Field: Gas Preheat Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas heating operation, such as an combustion fan. The units are in W.
-
-#### Field: Maximum Outdoor Air Flow Rate
-
-Enter autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100% of the full supply flow may be taken from outdoor air. If a value is entered, it is used instead of the autosize value. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
-
-#### Field: Minimum Outdoor Air Flow Rate
-
-Enter autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air  specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
-
-#### Field: Minimum Outdoor Air Schedule Name
-
-Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 – 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours.
-
-#### Field: Economizer Type
-
-The options for this field are
-
-- ‘FixedDryBulb’
-
-- ‘DifferentialDryBulb’
-
-- ‘FixedEnthalpy’
-
-- ‘ DifferentialEnthalpy’
-
-- ‘ElectronicEnthalpy’ (i.e., humidity ratio curve strategy)
-
-- ‘FixedDewPointAndDryBulb’
-
-- ‘DifferentialDryBulbAndEnthalpy’
-
-- ‘NoEconomizer’
-
-Choosing **NoEconomizer** means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
-
-Choosing **FixedDryBulb** means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
-
-Choosing **DifferentialDryBulb** will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
-
-**FixedEnthalpy** checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
-
-**DifferentialEnthalpy** does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
-
-Choosing **ElectronicEnthalpy** enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
-
-Choosing **FixedDewPointAndDryBulb** compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
-
-Another option **DifferentialDryBulbAndEnthalpy** enables the control strategy to be based on both the **DifferentialDryBulb** and **DifferentialEnthalpy** economizer control strategies.
-
-In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
-
-The default for this field is **NoEconomizer**.
-
-#### Field: Economizer Upper Temperature Limit
-
-Enter the outdoor air temperature high limit (<sup>o</sup>C) for economizer operation. If the outdoor air temperature is above this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature high limit control.
-
-#### Field: Economizer Lower Temperature Limit
-
-Enter the outdoor air temperature low limit (<sup>o</sup>C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
-
-#### Field: Economizer Upper Enthalpy Limit
-
-Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
-
-#### Field: Economizer Maximum Limit Dewpoint Temperature
-
-Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type ‘FixedDewPointAndDryBulb’ has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
-
-#### Field: Supply Plenum Name
-
-Set to blank if no supply plenum is to be modeled. If a supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves all zones on this system. If any supply plenums have been specified, the outlet from the system supply plenum will flow through the supply plenum to the zone terminal unit.
-
-#### Field: Return Plenum Name
-
-Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
-
-#### Field: Night Cycle Control
-
-Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are *StayOff*, *CycleOnAny*, *CycleOnControlZone or CycleOnAnyZoneFansOnly*. *StayOff* means the system will remain off, no matter how hot or cold the zones may be. *CycleOnAny* means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. *CycleOnControlZone* means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. *CycleOnAnyZoneFansOnly* is the same as *CycleOnAny* except that only the zone fans are cycled on and the central air handler fan is left off (applicable only if using HVACTemplate:Zone:VAV:FanPowered in one or more zones). The default is *StayOff*.
-
-#### Field: Night Cycle Control Zone Name
-
-For the Night Cycle Control option *Cycle On Control Zone* enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
-
-#### Field: Heat Recovery Type
-
-Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
-
-- None
-
-- Sensible
-
-- Enthalpy
-
-The default is **None***.*
-
-#### Field: Sensible Heat Recovery Effectiveness
-
-Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
-
-#### Field: Latent Heat Recovery Effectiveness
-
-Enter the latent heat recovery effectiveness if Heat Recovery Type is *Enthalpy*. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
-
-#### Field: Heat Recovery Heat Exchanger Type
-
-This alpha field denotes the type of heat exchanger being modeled: Plate (e.g., fixed plate) or Rotary (e.g., rotating cylinder or wheel). The default choice for this field is “Plate�. The heat exchanger type affects the modeling of frost control options and supply air outlet temperature control. For rotary heat exchangers, rotational speed is varied to control frost formation or the supply air outlet temperature. For plate exchangers, air bypass around the heat exchanger is used to obtain the desired effect.
-
-#### Field: Heat Recovery Frost Control Type
-
-This alpha field has four choices: None, ExhaustAirRecirculation, ExhaustOnly and MinimumExhaustTemperature. If this field is left blank, the default frost control type is “None�. For modeling preheat frost control, specify “None� for this input field and insert a separate heating coil object in the supply inlet air stream to keep the air temperature above the desired frost threshold temperature.
-
-*ExhaustAirRecirculation*: dampers are used to direct exhaust air back into the zone through the supply side of the heat exchanger when the supply (outdoor) air inlet temperature falls below a threshold temperature. The fraction of time that exhaust air is circulated through the supply side of the heat exchanger is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When exhaust air is being recirculated, no supply (outdoor ventilation) air is being provided through the heat exchanger unit (which may or may not be acceptable regarding ventilation for occupants).
-
-*ExhaustOnly (supply air bypass)*: this control cycles off the supply air flow through the heat exchanger for a certain period of time while the exhaust air continues to flow through the exhaust side of the heat exchanger. The fraction of time that the supply flow through the heat exchanger is cycled off is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When implemented in real applications, provisions are usually made to avoid building depressurization when this frost control is operating (automatic or pressure-operated dampers, or a bypass air damper around the supply side of the heat exchanger). For this frost control type, it is assumed that the supply air is bypassed around the heat exchanger during frost control operation (i.e., the total supply flow is not reduced during defrost, but merely bypassed around the heat exchanger).
-
-*MinimumExhaustTemperature*: the temperature of the exhaust air leaving the heat exchanger is monitored and the heat exchanger effectiveness is decreased (by slowing heat exchanger rotation or bypassing supply air around the plate exchanger) to keep the exhaust air from falling below the threshold temperature.
-
-#### Field: Dehumidification Control Type
-
-There are two dehumidification control type options available:
-
-- None
-
-- CoolReheat
-
-The *CoolReheat* option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so.  Reheat is provided as required by the central heating coil if available or the terminal unit reheat coils if available.
-
-The default is *None* which meets the sensible cooling setpoint only.
-
-#### Field: Dehumidification Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling dehumidification.
-
-#### Field: Dehumidification Relative Humidity Setpoint
-
-This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100).  The default is 60%. This field is ignored if a Dehumidification Relative Humidity Setpoint Schedule Name is specified.
-
-#### Field: Dehumidification Relative Humidity Setpoint Schedule Name
-
-Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint,  The values in the schedule are in percent (0 to 100).
-
-#### Field: Humidifier Type
-
-There are two humidifier type options available:
-
-- None
-
-- ElectricSteam
-
-The *ElectricSteam* humidifier option uses the Humidifier:Steam:Electric object.  The default is *None.*
-
-#### Field: Humidifier Availability Schedule Name
-
-If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
-
-#### Field: Humidifier Rated Capacity
-
-Enter the rated moisture output rate in m3/s.  The humidifier does not currently autosize, so the default is very large to allow for adequate capacity.  The default is 0.000001 m3/s.
-
-#### Field: Humidifier Rated Electric Power
-
-Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
-
-#### Field: Humidifier Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling humidification.
-
-#### Field: Humidifier Relative Humidity Setpoint
-
-This field specifies the zone humidistat setpoint for humidification in percent (0 to 100).  The default is 30%. This field is ignored if a Humidifier Relative Humidity Setpoint Schedule Name is specified.
-
-#### Field: Humidifier Relative Humidity Setpoint Schedule Name
-
-Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint,  The values in the schedule are in percent (0 to 100).
-
-#### Field: Return Fan
-
-Enter *Yes* if the system has a return fan. The default is *No*.
-
-#### Field: Return Fan Total Efficiency
-
-Enter the total efficiency of the return fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1. Default is 0.7.
-
-#### Field: Return Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 300 Pa.
-
-#### Field: Return Fan Motor efficiency
-
-Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1. Default is 0.9.
-
-#### Field: Return Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1. Default is 1.0.
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:System:ConstantVolume,
-    CAV Sys 1,               !-Name
-    FanAvailSched,           !- System Availability Schedule Name
-    autosize,                !- Supply Fan Maximum Flow Rate {m3/s}
-    0.7,                     !- Supply Fan Total Efficiency
-    600,                     !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    1,                       !- Supply Fan Motor in Air Stream Fraction
-     DrawThrough,             !- Supply Fan Placement
-    ChilledWater,            !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule Name
-     ControlZone,             !- Cooling Coil Setpoint Control Type
-     SPACE 1-1,               !- Cooling Coil Conrol Zone
-     12.8,                        !- Cooling Coil Design Setpoint {C}
-    ,                        !- Cooling Coil Setpoint Schedule Name
-     ,                   !- Cooling Coil Setpoint at Outdoor Dry-Bulb Low {C}
-     ,                        !- Cooling Coil Reset Outdoor Dry-Bulb Low {C}
-     ,                   !- Cooling Coil Setpoint at Outdoor Dry-Bulb High {C}
-     ,                        !- Cooling Coil Reset Outdoor Dry-Bulb High {C}
-    HotWater,                !- Heating Coil Type
-    ,                        !- Heating Coil Availability Schedule Name
-     FixedSetpoint,           !- Heating Coil Setpoint Control Type
-     ,                        !- Heating Coil Control Zone
-     50,                        !- Heating Coil Design Setpoint {C}
-    ,                        !- Heating Coil Setpoint Schedule Name
-     ,                   !- Heating Coil Setpoint at Outdoor Dry-Bulb Low {C}
-     ,                        !- Hedating Coil Reset Outdoor Dry-Bulb Low {C}
-     ,                   !- Heating Coil Setpoint at Outdoor Dry-Bulb High {C}
-     ,                        !- Heating Coil Reset Outdoor Dry-Bulb High {C}
-    Autosize,                !- Heating Coil Capacity {W}
-    0.8,                     !- Gas Heating Coil Efficiency
-    0.0,                     !- Gas Heating Coil Parasitic Electric Load {W}
-    None,                    !- Preheat Coil Type
-    ,                        !- Preheat Coil Availability Schedule Name
-    ,                        !- Preheat Coil Design Setpoint {C}
-    ,                        !- Preheat Coil Setpoint Schedule Name
-    0.8,                     !- Gas Preheat Coil Efficiency
-    0.0,                     !- Gas Preheat Coil Parasitic Electric Load {W}
-    autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}
-    autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}
-    Min OA Sched,            !- Minimum Outdoor Air Schedule Name
-    DifferentialDryBulb,     !- Economizer Type
-    19,                      !- Economizer Upper Temperature Limit {C}
-    4,                       !- Economizer Lower Temperature Limit {C}
-    ,                        !- Economizer Upper Enthalpy Limit {J/kg}
-    ,                    !- Economizer Maximum Limit Dewpoint Temperature {C}
-    ,                        !- Supply Plenum Name
-    PLENUM-1,                !- Return Plenum Name
-     CycleOnAnyZoneFansOnly,  !- Night Cycle Control
-    ,                        !- Night Cycle Control Zone Name
-    None,                    !- Heat Recovery Type
-    0.70,                    !- Sensible Heat Recovery Effectiveness
-     0.65,                    !- Latent Heat Recovery Effectiveness
-     ,                        !- Heat Recovery Heat Exchanger Type
-     ,                        !- Heat Recovery Frost Control Type
-     None,                    !- Dehumidification Control Type
-    ,                        !- Dehumidification Control Zone Name
-    60.0,     !- Dehumidification Relative Humidity Setpoint {percent}
-    ,         !- Dehumidification Relative Humidity Setpoint Schedule Name
-    None,                    !- Humidifier Type
-    ,                        !- Humidifier Availability Schedule Name
-    0.000001,                !- Humidifier Rated Capacity {m3/s}
-    2690.0,                  !- Humidifier Rated Electric Power {W}
-    ,                        !- Humidifier Control Zone Name
-    30.0,     !- Humidifier Relative Humidity Setpoint {percent}
-    ,         !- Humidifier Relative Humidity Setpoint Schedule Name
-    No,                      !- Return Fan
-    0.7,                     !- Return Fan Total Efficiency
-     600,                     !- Return Fan Delta Pressure {Pa}
-     0.9,                     !- Return Fan Motor Efficiency
-     1.0;                     !- Return Fan Motor in Air Stream Fraction
-```
-
-
-### HVACTemplate:System:DualDuct
-
-This object simulates the system portion of a constant air volume or variable air volume dual-duct HVAC configuration with optional chilled water cooling and several different heating options. One or more HVACTemplate:Zone:DualDuct objects may be specified for each zone served by the HVACTemplate:System:DualDuct object. The system will be constant volume if all of the HVACTemplate:Zone:DualDuct objects served by this system have Zone Minimum Air Flow Fraction =1.0.
-
-#### Field: Name
-
-Enter a name for the HVACTemplate:System:DualDuct object. This name is used in the HVACTemplate:Zone:DualDuct object to reference this system.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to be available for the entire year to perform heating or cooling if called for by the thermostat. If a schedule name is specified, those times that the system is available should be specified as 1.0. Those times that the system is not available should have a zero value in the schedule specified. Please note that for this system type, this is a schedule of when the system is providing air flow.
-
-#### Field: Supply Fan Configuration Type
-
-This field specifies the supply fan configuration. * SingleConstantVolume* and *SingleVariableVolume* specify one supply fan located in the main supply air duct before the split into a cold supply air duct and a hot supply air duct. This configuration uses the ‘Main Supply Fan’ input fields which follow immediately below.  *DualConstantVolume* and *DualVariableVolume* specify two supply fans, one located in the cold supply air duct and one located in the hot supply air duct. *Dual* uses the ‘Cold Duct Supply Fan’ and Hot Duct Supply Fan’ inputs which follow below. The default is*SingleConstantVolume*.
-
-#### Field: Main Supply Fan Maximum Flow Rate
-
-Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m<sup>3</sup>/s.
-
-#### Field: Main Supply Fan Minimum Flow Fraction
-
-Enter the minimum supply air flow fraction that may be provided. This field is ignored if the system is constant volume.
-
-#### Field: Main Supply Fan Total Efficiency
-
-Enter the total efficiency of the main supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7..
-
-#### Field: Main Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 1000 Pa.
-
-#### Field: Main Supply Fan Motor Efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Main Supply Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Main Supply Fan Part-Load Power Coefficients
-
-Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
-
-- InletVaneDampers
-
-- OutletDampers
-
-- VariableSpeedMotor
-
-- ASHRAE90.1-2004Appendix G
-
-- VariableSpeedMotorPressureReset
-
-The default is *InletVaneDampers*. The resulting power curves are shown in Figure 158. VAV Supply Fan Part-Load Power Coefficient Options below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The *VariableSpeedMotorPressureReset* option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources’: *Design Guidelines: Advanced Variable Air Volume (VAV) Systems* (EDR\_DesignGuidelines\_VAV.pdf).
-
-![](media/image613.svg)
-
-Figure 160. VAV Supply Fan Part-Load Power Coefficient Options
-
-#### Field: Cold Duct Supply Fan Maximum Flow Rate
-
-Enter Autosize to set the system maximum cold duct air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m<sup>3</sup>/s.
-
-#### Field: Cold Duct Supply Fan Minimum Flow Fraction
-
-Enter the minimum cold duct air flow fraction that may be provided. This field is ignored if the system is constant volume.
-
-#### Field: Cold Duct Supply Fan Total Efficiency
-
-Enter the total efficiency of the cold duct supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
-
-#### Field: Cold Duct Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 1000 Pa.
-
-#### Field: Cold Duct Supply Fan Motor efficiency
-
-Enter the shaft power of the cold duct supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Cold Duct Supply Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the cold duct air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Cold Duct Supply Fan Part-Load Power Coefficients
-
-Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
-
-- InletVaneDampers
-
-- OutletDampers
-
-- VariableSpeedMotor
-
-- ASHRAE90.1-2004Appendix G
-
-- VariableSpeedMotorPressureReset
-
-The default is *InletVaneDampers*. The resulting power curves are shown in Figure 158. VAV Supply Fan Part-Load Power Coefficient Options below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The *VariableSpeedMotorPressureReset* option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources’: *Design Guidelines: Advanced Variable Air Volume (VAV) Systems* (EDR\_DesignGuidelines\_VAV.pdf).
-
-#### Field: Cold Duct Supply Fan Placement
-
-Enter the cold duct supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *Draw Through*.
-
-#### Field: Hot Duct Supply Fan Maximum Flow Rate
-
-Enter Autosize to set the system maximum hot duct air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone level air flow inputs sum to a greater value. This flow rate will *not* be multiplied by a sizing factor or by zone multipliers. If using zone multipliers a value entered here must be large enough to serve the multiplied zones. The units are m<sup>3</sup>/s.
-
-#### Field: Hot Duct Supply Fan Minimum Flow Fraction
-
-Enter the minimum hot duct air flow fraction that may be provided. This field is ignored if the system is constant volume.
-
-#### Field: Hot Duct Supply Fan Total Efficiency
-
-Enter the total efficiency of the hot duct supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
-
-#### Field: Hot Duct Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 1000 Pa.
-
-#### Field: Hot Duct Supply Fan Motor efficiency
-
-Enter the shaft power of the hot duct supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Hot Duct Supply Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the hot duct air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Hot Duct Supply Fan Part-Load Power Coefficients
-
-Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
-
-- InletVaneDampers
-
-- OutletDampers
-
-- VariableSpeedMotor
-
-- ASHRAE90.1-2004Appendix G
-
-- VariableSpeedMotorPressureReset
-
-The default is *InletVaneDampers*. The resulting power curves are shown in Figure 158. VAV Supply Fan Part-Load Power Coefficient Options below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The *VariableSpeedMotorPressureReset* option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources’: *Design Guidelines: Advanced Variable Air Volume (VAV) Systems* (EDR\_DesignGuidelines\_VAV.pdf).
-
-#### Field: Hot Duct Supply Fan Placement
-
-Enter the hot duct supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *Draw Through*.
-
-#### Field: Cooling Coil Type
-
-There are two coil types available:
-
-- ChilledWater
-
-- ChilledWaterDetailedFlatModel
-
-- None
-
-*ChilledWater* uses the COIL:Cooling:Water object with the DetailedAnalysis option.  This is the preferred coil model for most applications.  *ChilledWaterDetailedFlatModel* uses the Coil:Cooling:Water:DetailedGeometry object.  This option is available for special applications.  The default is *ChilledWater*.
-
-#### Field: Cooling Coil Availability Schedule Name
-
-Usually set to blank, which allows the cooling coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when cooling is only available seasonally. A schedule value of 1 indicates that the cooling coil can be on during a given time period. A value of 0 denotes that the cooling coil cannot be used during that time period.
-
-#### Field: Cooling Coil Setpoint Control Type
-
-Specifies the cooling coil setpoint control type:
-
-- FixedSetpoint
-
-- Scheduled
-
-- OutdoorAirTemperatureReset
-
-- Warmest – reset the cooling supply air temperature to the highest supply air temperature that will meet the cooling requirements of all the zones. The minimum setpoint allowed is the Cooling Coil Design Setpoint. The maximum setpoint allowed is defaulted to 18C or the Cooling Design Setpoint + 5.2C whichever is greater.. (Reference SetpointManager:Warmest)
-
-FixedSetpoint uses the Cooling Coil Design Setpoint as the supply air setpoint. Scheduled uses the Cooling Coil Setpoint Schedule to set the supply air setpoint. OutdoorAirTemperatureReset varies the supply air setpoint based on the values entered for Cooling Coil Setpoint at Outdoor Dry-Bulb Low, Cooling Coil Reset Outdoor Dry-Bulb Low, Cooling Coil Setpoint at Outdoor Dry-Bulb High, and Cooling Coil Reset Outdoor Dry-Bulb High. The default is FixedSetpoint.
-
-#### Field: Cooling Coil Design Setpoint Temperature
-
-Enter the cooling supply air temperature in C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8C. If no Cooling Coil Setpoint Schedule or Cooling Coil Setpoint Reset Type is specified, this value is used as a constant cooling supply air setpoint temperature.
-
-#### Field: Cooling Coil Setpoint Schedule Name
-
-If a constant setpoint for the cooling coil is to be specified, leave this field blank, and the Cooling Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the cooling coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the cooling coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Cooling Coil Setpoint Reset Type is something other than None (see above).
-
-#### Field: Cooling Coil Setpoint at Outdoor Dry-Bulb Low
-
-The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Cooling Coil Reset Outdoor Dry-Bulb Low). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
-
-#### Field: Cooling Coil Reset Outdoor Dry-Bulb Low
-
-The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
-
-#### Field: Cooling Coil Setpoint at Outdoor Dry-Bulb High
-
-The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Cooling Coil Reset Outdoor Dry-Bulb High). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.8C.
-
-#### Field: Cooling Coil Reset Outdoor Dry-Bulb High
-
-The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb High. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 23.3C.
-
-#### Field: Heating Coil Type
-
-The heating coil is located in the supply air stream, upstream of the cooling coil and after the outdoor air mixing box. If no central heating coil is used in the Constant Volume system,  then the option “none� should be specified here. Otherwise this indicates the type of heating coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
-
-- HotWater
-
-- Electric
-
-- Gas
-
-- None
-
-The default value is HotWater. Note that the configuration of HVACTemplate:System:ConstantVolume assumes that there will be reheat coils or baseboard heating to provide heating control at the zone level. If a heating coil is specified, the heating and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
-
-#### Field: Heating Coil Availability Schedule Name
-
-Usually set to blank, which allows the heating coil to be available anytime the system is operating. If a schedule name is specified, it defines when the coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period.
-
-#### Field: Heating Coil Setpoint Control Type
-
-Specifies the heating coil setpoint control type:
-
-- FixedSetpoint
-
-- Scheduled
-
-- OutdoorAirTemperatureReset
-
-- Warmest – reset the heating supply air temperature to the coldest supply air temperature that will meet the heating requirements of all the zones. The maximum setpoint allowed is the Heating Coil Design Setpoint. The minimum setpoint allowed is defaulted to 20C or the Heating Coil Design Setpoint – 5.2C whichever is lower.. (Reference SetpointManager:Coldest)
-
-FixedSetpoint uses the Heating Coil Design Setpoint as the supply air setpoint. Scheduled uses the Heating Coil Setpoint Schedule to set the supply air setpoint. OutdoorAirTemperatureReset varies the supply air setpoint based on the values entered for Heating Coil Setpoint at Outdoor Dry-Bulb Low, Heating Coil Reset Outdoor Dry-Bulb Low, Heating Coil Setpoint at Outdoor Dry-Bulb High, and Heating Coil Reset Outdoor Dry-Bulb High. The default is FixedSetpoint.
-
-#### Field: Heating Coil Design Setpoint
-
-Enter the heating supply air temperature in C to be used for sizing the heating coil and zone supply air flow rates. If no Heating Coil Setpoint Schedule or Heating Coil Setpoint Reset Type is specified, this value is used as a constant heating supply air setpoint temperature.  The default is 50.0C.
-
-#### Field: Heating Coil Setpoint Schedule Name
-
-If a constant setpoint for the heating coil is to be specified, leave this field blank, and the Heating Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the heating coil specify the schedule name here. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the heating coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Heating Coil Setpoint Reset Type is something other than None (see above).
-
-#### Field: Heating Coil Setpoint at Outdoor Dry-Bulb Low
-
-The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Heating Coil Reset Outdoor Dry-Bulb Low). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 50.0C.
-
-#### Field: Heating Coil Reset Outdoor Dry-Bulb Low
-
-The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 7.8C.
-
-#### Field: Heating Coil Setpoint at Outdoor Dry-Bulb High
-
-The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Heating Coil Reset Outdoor Dry-Bulb High). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 20.0C.
-
-#### Field: Heating Coil Reset Outdoor Dry-Bulb High
-
-The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb High. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.2C.
-
-#### Field: Heating Coil Capacity
-
-Enter autosize to allow the sizing algorithm to determine the proper capacity required based on the loads experienced during the heating design day. If a value is specified, it is the maximum amount of heat that the coil can deliver in Watts.
-
-#### Field: Gas Heating Coil Efficiency
-
-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default
-
-#### Field: Gas Heating Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas heating operation, such as a combustion fan. The units are in W.
-
-#### Field: Preheat Coil Type
-
-The preheat coil is located in the outdoor air stream, upstream of the outdoor air mixing box and tempers the outdoor air. If no preheat coil is used in the constant volume system, then the option “none� should be specified here. Otherwise this indicates the type of preheat coil. It is unlikely that both a heating coil and a preheat coil would be used at the same time. The choices for this field are
-
-- HotWater
-
-- Electric
-
-- Gas
-
-- None
-
-The default value is None. If a preheat coil is specified, the preheat and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other.
-
-#### Field: Preheat Coil Availability Schedule Name
-
-Usually set to blank, which allows the preheat coil to be available anytime the system is operating. If a schedule name is specified, it defines when the preheat coil is available. This is most often used when preheat is only available seasonally. The schedule values denote whether the preheat coil can run during a given time period. A schedule value of 1.0 indicates that the preheat coil can be on during a given time period. A value of zero denotes that the preheat coil cannot be used during that time period
-
-#### Field: Preheat Coil Design Setpoint
-
-Enter the preheat supply air temperature in C to be used for sizing the preheat coil. If no Preheat Coil Setpoint Schedule is specified, this value is used as a constant preheat supply air setpoint temperature. The default is 7.2C.
-
-#### Field: Preheat Coil Setpoint Schedule Name
-
-If a constant setpoint for the preheat coil is to be specified, leave this field blank, and the Preheat Coil Design Setpoint value will be used at all times. If a set point schedule is to be used for the preheat coil specify the schedule name here. The schedule should control the leaving air temperature from the preheat coil. The values in the schedule are in degrees C.
-
-#### Field: Gas Preheat Coil Efficiency
-
-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default
-
-#### Field: Gas Preheat Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas heating operation, such as an combustion fan. The units are in W.
-
-#### Field: Maximum Outdoor Air Flow Rate
-
-Enter autosize or a value for the maximum amount of outdoor air flow into the unit when the economizer is operating. Autosize means that 100% of the full supply flow may be taken from outdoor air. If a value is entered, it is used instead of the autosize value. The units are in m3/s. That is, the entered value is used to define the Maximum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
-
-#### Field: Minimum Outdoor Air Flow Rate
-
-Enter autosize or the value for the minimum amount of outdoor air that can enter the unit and be distributed to the zones. Usually this is set to autosize and the value is calculated by the outdoor air requirements of each zone. If a value is entered it overrides the outdoor air  specification from the zone level. The units are in m3/s. The default is Autosize. The entered value is used to define the Minimum Outdoor Air Flow Rate for the Controller:OutdoorAir object that will be generated by this template.
-
-#### Field: Minimum Outdoor Air Control Type
-
-Choices for this field are **FixedMinimum** or **ProportionalMinimum**. FixedMinimum means that the minimum outdoor air flow rate is fixed no matter what the actual system flow rate is. ProportionalMinimum means the minimum outdoor air flow rate varies in proportion to the total system air flow rate. The default is ProportionalMinimum.
-
-#### Field: Minimum Outdoor Air Schedule Name Name
-
-Leave this field blank if you want the minimum outdoor air to be the same for all hours in the entire year. If a schedule name is specified, values are decimal fractions (0.0 – 1.0) that multiply the minimum outdoor air flow rate. This schedule is useful for reducing the outdoor air flow rate to zero during unoccupied or start up hours.
-
-#### Field: Economizer Type
-
-The options for this field are
-
-- ‘FixedDryBulb’
-
-- ‘DifferentialDryBulb’
-
-- ‘FixedEnthalpy’
-
-- ‘ DifferentialEnthalpy’
-
-- ‘ElectronicEnthalpy’ (i.e., humidity ratio curve strategy)
-
-- ‘FixedDewPointAndDryBulb’
-
-- ‘DifferentialDryBulbAndEnthalpy’
-
-- ‘NoEconomizer’
-
-Choosing **NoEconomizer** means the economizer will not operate and the outdoor airflow rate will be at the minimum for the entire simulation.
-
-Choosing **FixedDryBulb** means the economizer will set the outdoor airflow rate at minimum if the outdoor air temperature is higher than a specified dry-bulb temperature limit.
-
-Choosing **DifferentialDryBulb** will trigger the outdoor airflow to minimum when the dry-bulb temperature of outdoor air is higher than the dry-bulb temperature of the return air.
-
-**FixedEnthalpy** checks the upper limit of the enthalpy given as a field input against the enthalpy content of outdoor air and will set the outdoor airflow rate to minimum if the latter is greater than the former.
-
-**DifferentialEnthalpy** does the same thing but compares the return air enthalpy with the enthalpy of outdoor air. When the enthalpy of outdoor air is greater than the enthalpy of the return air, the outdoor air flow rate is set to minimum.
-
-Choosing **ElectronicEnthalpy** enables the simulation to calculate the humidity ratio limit of outdoor air based on the dry-bulb temperature of outdoor air and a quadratic/cubic curve, and compare it to the actual outdoor air humidity ratio. If the actual outdoor humidity ratio is greater than the calculated humidity ratio limit, then the outdoor airflow rate is set to minimum.
-
-Choosing **FixedDewPointAndDryBulb** compares both the outdoor dewpoint temperature and the outdoor dry-bulb temperature to their specified high limit values. If either outdoor temperature exceeds the high limit value, the outdoor airflow rate is set to minimum.
-
-Another option **DifferentialDryBulbAndEnthalpy** enables the control strategy to be based on both the **DifferentialDryBulb** and **DifferentialEnthalpy** economizer control strategies.
-
-In addition to all economizer control types listed above, each control type checks for user-entered values for the upper limit of dry-bulb temperature, enthalpy limit, humidity ratio limit and dewpoint limit. The outdoor air flow rate is set to minimum if any of these entered limits are exceeded.
-
-The default for this field is **NoEconomizer**.
-
-#### Field: Economizer Lockout
-
-The only choice for this field is
-
-- NoLockout
-
-The default value is NoLockout. Future versions may have additional options.
-
-#### Field: Economizer Upper Temperature Limit
-
-Enter the outdoor air temperature high limit (<sup>o</sup>C) for economizer operation. If the outdoor air temperature is above this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature high limit control.
-
-#### Field: Economizer Lower Temperature Limit
-
-Enter the outdoor air temperature low limit (<sup>o</sup>C) for economizer operation. If the outdoor air temperature is below this limit, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air temperature low limit control.
-
-#### Field: Economizer Upper Enthalpy Limit
-
-Enter the outdoor air upper enthalpy limit (in J/kg) for economizer operation. If the outdoor air enthalpy is above this value, the outdoor air flow rate will be set to the minimum and heat recovery will be enabled if available. No input or zero in this field means that there is no outdoor air enthalpy limit control.
-
-#### Field: Economizer Maximum Limit Dewpoint Temperature
-
-Input for this field is the outdoor air dewpoint limit (ºC) for economizer operation. If the outdoor air dewpoint temperature is above this value, the outdoor airflow rate will be set to the minimum. This field is required if the Economizer Control Type ‘FixedDewPointAndDryBulb’ has been specified. No input (blank) in this field means that there is no outdoor air dewpoint limit control.
-
-#### Field: Cold Supply Plenum Name
-
-Set to blank if no cold supply plenum is to be modeled. If a cold supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves the cold inlets of all zones on this system. If any zone supply plenums have been specified, the outlet from the system supply plenum will flow through the zone supply plenum to the zone terminal unit.
-
-#### Field: Hot Supply Plenum Name
-
-Set to blank if no hot supply plenum is to be modeled. If a hot supply plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This supply plenum serves hot inlets of all zones on this system. If any zone supply plenums have been specified, the outlet from the system supply plenum will flow through the zone supply plenum to the zone terminal unit.
-
-#### Field: Return Plenum Name
-
-Set to blank if no return plenum is to be modeled. If a return plenum is modeled, it must be modeled as a zone with surfaces, and the name of the plenum zone should be entered here. This return plenum serves all zones on this system. If any zone return plenums have been specified, the return air from the zone will flow through the zone return plenum and then into the system return plenum.
-
-#### Field: Night Cycle Control
-
-Enter the system behavior during times when the System Availability Schedule is zero (off). The possible inputs are *StayOff*, *CycleOnAny*, or *CycleOnControlZone*. *StayOff* means the system will remain off, no matter how hot or cold the zones may be. *CycleOnAny* means that if any zone served by this system has an air temperature outside the cooling or heating set points the central fan will turn on even though the System Availability Schedule indicates the fan is off. *CycleOnControlZone* means the same thing except the availability manager looks at the temperature in only the zone specified in Night Cycle Control Zone Name. The default is *StayOff*.
-
-#### Field: Night Cycle Control Zone Name
-
-For the Night Cycle Control option *Cycle On Control Zone* enter the name of the control zone. For other Night Cycle Control options, this field is ignored.
-
-#### Field: Heat Recovery Type
-
-Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
-
-- None
-
-- Sensible
-
-- Enthalpy
-
-The default is **None***.*
-
-#### Field: Sensible Heat Recovery Effectiveness
-
-Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
-
-#### Field: Latent Heat Recovery Effectiveness
-
-Enter the latent heat recovery effectiveness if Heat Recovery Type is *Enthalpy*. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
-
-#### Field: Heat Recovery Heat Exchanger Type
-
-This alpha field denotes the type of heat exchanger being modeled: Plate (e.g., fixed plate) or Rotary (e.g., rotating cylinder or wheel). The default choice for this field is “Plate�. The heat exchanger type affects the modeling of frost control options and supply air outlet temperature control. For rotary heat exchangers, rotational speed is varied to control frost formation or the supply air outlet temperature. For plate exchangers, air bypass around the heat exchanger is used to obtain the desired effect.
-
-#### Field: Heat Recovery Frost Control Type
-
-This alpha field has four choices: None, ExhaustAirRecirculation, ExhaustOnly and MinimumExhaustTemperature. If this field is left blank, the default frost control type is “None�. For modeling preheat frost control, specify “None� for this input field and insert a separate heating coil object in the supply inlet air stream to keep the air temperature above the desired frost threshold temperature.
-
-*ExhaustAirRecirculation*: dampers are used to direct exhaust air back into the zone through the supply side of the heat exchanger when the supply (outdoor) air inlet temperature falls below a threshold temperature. The fraction of time that exhaust air is circulated through the supply side of the heat exchanger is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When exhaust air is being recirculated, no supply (outdoor ventilation) air is being provided through the heat exchanger unit (which may or may not be acceptable regarding ventilation for occupants).
-
-*ExhaustOnly (supply air bypass)*: this control cycles off the supply air flow through the heat exchanger for a certain period of time while the exhaust air continues to flow through the exhaust side of the heat exchanger. The fraction of time that the supply flow through the heat exchanger is cycled off is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When implemented in real applications, provisions are usually made to avoid building depressurization when this frost control is operating (automatic or pressure-operated dampers, or a bypass air damper around the supply side of the heat exchanger). For this frost control type, it is assumed that the supply air is bypassed around the heat exchanger during frost control operation (i.e., the total supply flow is not reduced during defrost, but merely bypassed around the heat exchanger).
-
-*MinimumExhaustTemperature*: the temperature of the exhaust air leaving the heat exchanger is monitored and the heat exchanger effectiveness is decreased (by slowing heat exchanger rotation or bypassing supply air around the plate exchanger) to keep the exhaust air from falling below the threshold temperature.
-
-#### Field: Dehumidification Control Type
-
-There are two dehumidification control type options available:
-
-- None
-
-- CoolReheat
-
-The *CoolReheat* option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so.  Reheat is provided as required by the terminal unit reheat coils if available.
-
-The default is *None* which meets the sensible cooling setpoint only.
-
-#### Field: Dehumidification Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling dehumidification.
-
-#### Field: Dehumidification Relative Humidity Setpoint
-
-This field specifies the zone humidistat setpoint for dehumidification in percent (0 to 100).  The default is 60%. This field is ignored if a Dehumidification Relative Humidity Setpoint Schedule Name is specified.
-
-#### Field: Dehumidification Relative Humidity Setpoint Schedule Name
-
-Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint,  The values in the schedule are in percent (0 to 100).
-
-#### Field: Humidifier Type
-
-There are two humidifier type options available:
-
-- None
-
-- ElectricSteam
-
-The *ElectricSteam* humidifier option uses the Humidifier:Steam:Electric object.  The default is *None.*
-
-#### Field: Humidifier Availability Schedule Name
-
-If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period
-
-#### Field: Humidifier Rated Capacity
-
-Enter the rated moisture output rate in m3/s.  The humidifier does not currently autosize, so the default is very large to allow for adequate capacity.  The default is 0.000001 m3/s.
-
-#### Field: Humidifier Rated Electric Power
-
-Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
-
-#### Field: Humidifier Control Zone Name
-
-This field specifies the zone name where the humidistat is located for controlling humidification.
-
-#### Field: Humidifier Relative Humidity Setpoint
-
-This field specifies the zone humidistat setpoint for humidification in percent (0 to 100).  The default is 30%. This field is ignored if a Humidifier Relative Humidity Setpoint Schedule Name is specified.
-
-#### Field: Humidifier Relative Humidity Setpoint Schedule Name
-
-Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Relative Humidity Setpoint,  The values in the schedule are in percent (0 to 100).
-
-#### Field: Sizing Option
-
-This field specifies the sizing method for the system supply air flow rate when the system type if variable volume. *Coincident* sizes on the sum of the coincident zone supply air flow rates. *NonCoincident* sizes on sum of the noncoincident zone design supply air flow rates. The default is *NonCoincident*.
-
-#### Field: Return Fan
-
-Enter *Yes* if the system has a return fan. The default is *No*.
-
-#### Field: Return Fan Total Efficiency
-
-Enter the total efficiency of the return fan. This is the ratio of the power delivered to the air to the electrical input power at maximum flow. This is also the product of the fan motor efficiency and fan (impeller) efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The fan efficiency is the power delivered to the air divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Return Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered 20<sup>o</sup> C at sea level, 101325 Pa. The default is 500 Pa.
-
-#### Field: Return Fan Motor efficiency
-
-Enter the shaft power of the return fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Return Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Return Fan Part-Load Power Coefficients
-
-Select the set of generic pre-defined coefficients to use for the supply fan part-load power consumption. This alpha field has the following choices:
-
-- InletVaneDampers
-
-- OutletDampers
-
-- VariableSpeedMotor
-
-- ASHRAE90.1-2004Appendix G
-
-- VariableSpeedMotorPressureReset
-
-The default is *InletVaneDampers*. The resulting power curves are shown in Figure 158. VAV Supply Fan Part-Load Power Coefficient Options below. The ASHRAE 90.1-2004 Appendix G coefficients are from TABLE G3.1.3.15, Method 2. The other sets of coefficients are from the EnergyPlus Input Output Reference, Fan Coefficient Values table. The *VariableSpeedMotorPressureReset* option is based on Good Static Pressure Reset VSD Fan from Energy Design Resources’: *Design Guidelines: Advanced Variable Air Volume (VAV) Systems* (EDR\_DesignGuidelines\_VAV.pdf).
-
-
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:System:DualDuct,
-    DD Sys 1,               !-Name
-    FanAvailSched,          !- System Availability Schedule Name
-     Single,                 !- Supply Fan Configuration Type  
-     autosize,               !- Main Supply Fan Maximum Flow Rate {m3/s}
-     0.2,                    !- Main Supply Fan Minimum Flow Fraction
-     0.7,                    !- Main Supply Fan Total Efficiency
-     600,                    !- Main Supply Fan Delta Pressure {Pa}
-     0.9,                    !- Main Supply Fan Motor Efficiency
-     1,                      !- Main Supply Fan Motor in Air Stream Fraction
-     InletVaneDampers,       !- Main Supply Fan Part-Load Power Coefficients
-    autosize,               !- Cold Duct Supply Fan Maximum Flow Rate {m3/s}
-     0.2,                    !- Cold Duct Supply Fan Minimum Flow Fraction
-     0.7,                    !- Cold Duct Supply Fan Total Efficiency
-     600,                    !- Cold Duct Supply Fan Delta Pressure {Pa}
-     0.9,                    !- Cold Duct Supply Fan Motor Efficiency
-     1,                   !- Cold Duct Supply Fan Motor in Air Stream Fraction
-     InletVaneDampers,    !- Cold Duct Supply Fan Part-Load Power Coefficients
-    DrawThrough,            !- Cold Duct Supply Fan Placement
-     autosize,               !- Hot Duct Supply Fan Maximum Flow Rate {m3/s}
-     0.2,                    !- Hot Duct Supply Fan Minimum Flow Fraction
-     0.7,                    !- Hot Duct Supply Fan Total Efficiency
-     600,                    !- Hot Duct Supply Fan Delta Pressure {Pa}
-     0.9,                    !- Hot Duct Supply Fan Motor Efficiency
-     1,                   !- Hot Duct Supply Fan Motor in Air Stream Fraction
-     InletVaneDampers,    !- Hot Duct Supply Fan Part-Load Power Coefficients
-    DrawThrough,            !- Hot Duct Supply Fan Placement
-    ChilledWater,           !- Cooling Coil Type
-    ,                       !- Cooling Coil Availability Schedule Name
-     ControlZone,            !- Cooling Coil Setpoint Control Type
-     12.8,                   !- Cooling Coil Design Setpoint {C}
-    ,                       !- Cooling Coil Setpoint Schedule Name
-     ,                   !- Cooling Coil Setpoint at Outdoor Dry-Bulb Low {C}
-     ,                       !- Cooling Coil Reset Outdoor Dry-Bulb Low {C}
-     ,                   !- Cooling Coil Setpoint at Outdoor Dry-Bulb High {C}
-     ,                       !- Cooling Coil Reset Outdoor Dry-Bulb High {C}
-    HotWater,               !- Heating Coil Type
-    ,                       !- Heating Coil Availability Schedule Name
-     FixedSetpoint,          !- Heating Coil Setpoint Control Type
-     50,                     !- Heating Coil Design Setpoint {C}
-    ,                       !- Heating Coil Setpoint Schedule Name
-     ,                   !- Heating Coil Setpoint at Outdoor Dry-Bulb Low {C}
-     ,                       !- Hedating Coil Reset Outdoor Dry-Bulb Low {C}
-     ,                   !- Heating Coil Setpoint at Outdoor Dry-Bulb High {C}
-     ,                       !- Heating Coil Reset Outdoor Dry-Bulb High {C}
-    Autosize,               !- Heating Coil Capacity {W}
-    0.8,                    !- Gas Heating Coil Efficiency
-    0.0,                    !- Gas Heating Coil Parasitic Electric Load {W}
-    None,                   !- Preheat Coil Type
-    ,                       !- Preheat Coil Availability Schedule Name
-    ,                       !- Preheat Coil Setpoint Schedule Name
-    ,                       !- Preheat Coil Design Setpoint {C}
-    0.8,                    !- Gas Preheat Coil Efficiency
-    0.0,                    !- Gas Preheat Coil Parasitic Electric Load {W}
-    autosize,               !- Maximum Outdoor Air Flow Rate {m3/s}
-    autosize,               !- Minimum Outdoor Air Flow Rate {m3/s}
-    FixedMinimum,           !- Minimum Outdoor Air Control Type
-    Min OA Sched,           !- Minimum Outdoor Air Schedule Name
-    DifferentialDryBulb,    !- Economizer Type
-    NoLockout,              !- Economizer Lockout
-    19,                     !- Economizer Upper Temperature Limit {C}
-    4,                      !- Economizer Lower Temperature Limit {C}
-    ,                       !- Economizer Upper Enthalpy Limit {J/kg}
-    ,                    !- Economizer Maximum Limit Dewpoint Temperature {C}
-    ,                       !- Cold Supply Plenum Name
-    ,                       !- Hot Supply Plenum Name
-    PLENUM-1,               !- Return Plenum Name
-     CycleOnAnyZoneFansOnly, !- Night Cycle Control
-    ,                       !- Night Cycle Control Zone Name
-    None,                   !- Heat Recovery Type
-    0.70,                   !- Sensible Heat Recovery Effectiveness
-     0.65,                   !- Latent Heat Recovery Effectiveness
-     ,                       !- Heat Recovery Heat Exchanger Type
-     ,                       !- Heat Recovery Frost Control Type
-     None,                   !- Dehumidification Control Type
-    ,                       !- Dehumidification Control Zone Name
-    60.0,    !- Dehumidification Relative Humidity Setpoint {percent}
-    ,         !- Dehumidification Relative Humidity Setpoint Schedule Name
-    None,                   !- Humidifier Type
-    ,                       !- Humidifier Availability Schedule Name
-    0.000001,               !- Humidifier Rated Capacity {m3/s}
-    2690.0,                 !- Humidifier Rated Electric Power {W}
-    ,                       !- Humidifier Control Zone Name
-    30.0,    !- Humidifier Relative Humidity Setpoint {percent}
-    ,         !- Humidifier Relative Humidity Setpoint Schedule Name
-    NonCoincident,          !- Sizing Option
-    No,                     !- Return Fan
-    0.7,                    !- Return Fan Total Efficiency
-     600,                    !- Return Fan Delta Pressure {Pa}
-     0.9,                    !- Return Fan Motor Efficiency
-     1.0;                    !- Return Fan Motor in Air Stream Fraction
-    InletVaneDampers;       !- Return Fan Part-Load Power Coefficients
-```
-
-
-### HVACTemplate:System:DedicatedOutdoorAir
-
-The HVACTemplate:System:DedicatedOutdoorAir creates a dedicated outdoor air system which must be used in conjunction with one or more of the following objects:
-
-HVACTemplate:Zone:BaseboardHeat
-
-HVACTemplate:Zone:FanCoil
-
-HVACTemplate:Zone:PTAC
-
-HVACTemplate:Zone:PTHP
-
-HVACTemplate:Zone:WaterToAirHeatPump
-
-HVACTemplate:Zone:VRF
-
-It is a constant volume dedicated outdoor air system which can serve multiple zones. It may have any combination of heating coil, cooling coil, and heat recovery. It may have dehumidification and humidification controls as well as several supply temperature control types. It supplies 100% outdoor air when the system is available, and assumes an equal volume of return air is available for heat recovery. If the system to be modeled does not have actual return ducts, but collects flow from exhaust fans to a central heat recovery point, then this approach should be equivalent. If the system does not have heat recovery and the air is exhausted or leaves by exfiltration, then the return path of this system will simply be a path to dump the flow as relief air with no impact on energy use.
-
-![](media/image614.png)
-
-Figure 161. DOAS serving three zones with PTACs.
-
-There may be more than one HVACTemplate:System:DedicatedOutdoorAir object in an idf file. If a zone is to be served by one of these systems, this is specified in the HVACTemplate:Zone:\* object using the field “Dedicated Outdoor Air System Name�. For zones which are served by one of these DOAS systems, the outdoor air flow rate in the zone equipment (fan coil, PTAC, etc.) will be set to zero.
-
-#### Field: Name
-
-This field is a unique name which the user assigns to this system. This name can then be referred to in an HVACTemplate:Zone:\* object to specify that this system provides outdoor air to that zone.
-
-#### Field: System Availability Schedule Name
-
-Leave this field blank if you want the system to operate at all times.  If a schedule name is specified, those times that the system is operating should be specified as 1.0. Those times that the system is not operating should have a zero value in the schedule specified. Please note that for this system type, this is a schedule of when the system is providing air flow.
-
-#### Field: Air Outlet Type
-
-This field indicates if the air is delivered directly into the zone(s) or into the other system(s) that serve the zone(s) (e.g. fan coil system). For now, only one option is available for this field: DirectIntoZone.
-
-#### Field: Supply Fan Flow Rate
-
-Enter Autosize to set the system maximum air-flow rate to the sum of the zone air flow rates. If a value is entered here for the maximum air-flow rate, it is the upper limit on system flow, even if the zone air flow inputs sum to a greater value. The units are m<sup>3</sup>/s.
-
-#### Field: Supply Fan Total Efficiency
-
-Enter the total efficiency of the supply fan. This value is the overall efficiency of the fan, i.e., the ratio of the power delivered to the fluid to the electrical input power. It is the product of the motor efficiency and the impeller efficiency. The motor efficiency is the power delivered to the shaft divided by the electrical power input to the motor. The impeller efficiency is power delivered to the fluid (air) divided by the shaft power. The power delivered to the fluid is the mass flow rate of the air multiplied by the pressure rise divided by the air density. This input value must be between 0 and 1. The default is 0.7.
-
-#### Field: Supply Fan Delta Pressure
-
-Enter the pressure rise in Pa at full flow and standard conditions. Standard conditions are considered to be 20<sup>o</sup> C at sea level, 101325 Pa.
-
-#### Field: Supply Fan Motor Efficiency
-
-Enter the shaft power of the supply fan divided by the electrical power consumed. Must be greater than 0 and less than or equal to 1.
-
-#### Field: Supply Fan Motor in Air Stream Fraction
-
-Enter the fraction of the motor heat that is added to the air stream. A value of 0 means that the motor is completely outside the air stream. A value of 1 means that all of the motor heat will go into the air stream and act to cause a temperature rise. Must be between 0 and 1.
-
-#### Field: Supply Fan Placement
-
-Enter the supply fan placement type. This alpha field has two choices, *DrawThrough* or *BlowThrough*. *DrawThrough* models a system where the supply air fan is after the cooling and heating coils. *BlowThrough* models a system where the supply air fan is before the cooling and heating coils. The default is *DrawThrough*.
-
-#### Field: Cooling Coil Type
-
-There are seven coil types available:
-
-- ChilledWater
-
-- ChilledWaterDetailedFlatModel
-
-- TwoSpeedDX
-
-- TwoStageDX
-
-- TwoStageHumidityControlDX
-
-- HeatExchangerAssistedChilledWater
-
-- HeatExchangerAssistedDX
-
-- None
-
-*ChilledWater* uses the Coil:Cooling:Water object with the DetailedAnalysis option.  This is the preferred coil model for most chilled water applications.
-
-*ChilledWaterDetailedFlatModel* uses the Coil:Cooling:Water:DetailedGeometry object.  This option is available for special applications.
-
-*TwoSpeedDX* uses the Coil:Cooling:DX:TwoSpeed object.
-
-*TwoStageDX* and *TwoStageHumidityControlDX*  use the Coil:Cooling:DX:TwoStageWithHumidityControlMode object.
-
-*HeatExchangerAssistedChilledWater* uses the CoilSystem:Cooling:Water:HeatExchangerAssisted, HeatExchanger:AirToAir:SensibleAndLatent, and Coil:Cooling:Water objects.
-
-*HeatExchangerAssistedDX* uses the CoilSystem:Cooling:DX:HeatExchangerAssisted, HeatExchanger:AirToAir:SensibleAndLatent, and Coil:Cooling:DX:SingleSpeed objects.
-
-The default type is *ChilledWater*.
-
-#### Field: Cooling Coil Availability Schedule Name
-
-Usually left blank, which allows the cooling coil to be available as needed anytime the system is operating. If a schedule name is specified, it defines when the cooling coil is available. This is most often used when cooling is only available seasonally. A schedule value of one indicates that the cooling coil can be on during a given time period. A value of zero denotes that the cooling coil cannot be used during that time period.
-
-#### Field: Cooling Coil Setpoint Control Type
-
-Specifies the cooling coil setpoint control type:
-
-- FixedSetpoint
-
-- Scheduled
-
-- OutdoorAirTemperatureReset
-
-FixedSetpoint uses the Cooling Coil Design Setpoint as the supply air setpoint. Scheduled uses the Cooling Coil Setpoint Schedule to set the supply air setpoint. OutdoorAirTemperatureReset varies the supply air setpoint based on the values entered for Cooling Coil Setpoint at Outdoor Dry-Bulb Low, Cooling Coil Reset Outdoor Dry-Bulb Low, Cooling Coil Setpoint at Outdoor Dry-Bulb High, and Cooling Coil Reset Outdoor Dry-Bulb High. The default is FixedSetpoint.
-
-NOTE: The user must ensure that the cooling coil and heating coil setpoints do not overlap to avoid unwanted simultaneous heating and cooling. The simulation will not check this automatically. It is recommended that the cooling setpoint always be at least 0.1C higher than the heating coil setpoint.
-
-#### Field: Cooling Coil Design Setpoint
-
-Enter the cooling supply air temperature in C to be used for sizing the cooling coil and zone supply air flow rates. The default is 12.8C. If Cooling Coil Setpoint Control Type  = FixedSetpoint, then this value is also used as the constant cooling supply air setpoint temperature.
-
-#### Field: Cooling Coil Setpoint Schedule Name
-
-This field is used when Cooling Coil Setpoint Control Type  = Scheduled. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the cooling coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C. This field is ignored if the Cooling Coil Setpoint Reset Type is something other than Scheduled (see above).
-
-#### Field: Cooling Coil Setpoint at Outdoor Dry-Bulb Low
-
-The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Cooling Coil Reset Outdoor Dry-Bulb Low). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
-
-#### Field: Cooling Coil Reset Outdoor Dry-Bulb Low
-
-The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.6C.
-
-#### Field: Cooling Coil Setpoint at Outdoor Dry-Bulb High
-
-The cooling coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Cooling Coil Reset Outdoor Dry-Bulb High). Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.8C.
-
-#### Field: Cooling Coil Reset Outdoor Dry-Bulb High
-
-The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Cooling Coil Setpoint at Outdoor Dry-Bulb High. Used only when Cooling Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 23.3C.
-
-#### Field: DX Cooling Coil Gross Rated Total Capacity
-
-Enter Autosize to let the automatic sizing algorithm determine the cooling coil gross total cooling capacity based on the maximum cooling loads during the cooling design day. If a value is entered, it represents the full load gross total cooling capacity, including both sensible and latent capacity, in watts of the DX coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb. Capacity should be the “gross�, i.e., the effect of supply air fan heat is not accounted for. The units are in W. The default is Autosize. This field is only used when the cooling coil type is set to one of the DX options.  For two-speed DX coils, the low-speed capacity is assumed to be 0.33 times this value.  For two-stage DX coils, the stage 1 capacity is assumed to be 0.5 times this value.
-
-#### Field: DX Cooling Coil Gross Rated Sensible Heat Ratio
-
-Enter Autosize to allow the sizing algorithm to determine the sensible heat ratio based on the gross rated cooling total capacity and air flow rate. Otherwise, enter the value of the ratio of the gross sensible capacity divided by gross total cooling capacity of the DX cooling coil at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb. Both the sensible and total cooling capacities used to define the Rated Sensible Heat Ratio (SHR) should be “gross�, i.e., the effect of supply air fan heat is not accounted for.  The default is Autosize. This field is only used when the cooling coil type is set to one of the DX options. For two-speed DX coils, the low-speed SHR is assumed to be equal to this value. For two-stage DX coils, the stage 1 SHR is assumed to be equal to this value. For two-stage DX coil with humidity control, the humidity control mode SHR is assumed to be 0.9 times this value (for both stage 1 and stage 2).
-
-#### Field: DX Cooling Coil Gross Rated COP
-
-Enter the coefficient of performance defined as the gross cooling coil total capacity in watts divided by electrical power input in watts of the DX cooling coil unit at rated conditions. Rated conditions are air entering the cooling coil at the maximum supply air flow rate at 26.7°C drybulb/19.4°C wetbulb with air entering the outdoor air-cooled condenser coil at 35°C drybulb. The input power includes electric power for the compressor and condenser fan but does not include the power consumption of the supply air fan. The default is 3.0. This field is only used when the cooling coil type is set to one of the DX options.  For two-speed DX coils, the low-speed COP is assumed to be 1.5 times this value.  For two-stage DX coils, the stage 1 COP is assumed to be this this value. For two-stage DX coil with humidity control, the humidity control mode COP is assumed to be 0.9 times this value (for both stage 1 and stage 2). The gross COP should not account for the supply air fan.
-
-#### Field: Heating Coil Type
-
-The heating coil is located in the supply air stream, downstream of the cooling coil. If no central heating coil is used in the dedicated outdoor air system, then the option “none� should be specified here. Otherwise this indicates the type of heating coil. The choices for this field are
-
-- HotWater
-
-- Electric
-
-- Gas
-
-- None
-
-The default value is HotWater. If a heating coil is specified, the heating and cooling coil setpoint controls and availability schedules must coordinate to prevent the coils from opposing each other. When the dehumidification control type is set to *CoolReheatHeatingCoil,* the heating coil is used for reheat.
-
-#### Field: Heating Coil Availability Schedule Name
-
-Usually left blank, which allows the heating coil to be available as needed anytime the system is operating. If a schedule name is specified, it defines when the heating coil is available. This is most often used when heating is only available seasonally. The schedule values denote whether the heating coil can run during a given time period. A schedule value of one indicates that the heating coil can be on during a given time period. A value of zero denotes that the heating coil cannot be used during that time period.
-
-#### Field: Heating Coil Setpoint Control Type
-
-Specifies the cooling coil setpoint control type:
-
-- FixedSetpoint
-
-- Scheduled
-
-- OutdoorAirTemperatureReset
-
-FixedSetpoint uses the Heating Coil Design Setpoint as the supply air setpoint. Scheduled uses the Heating Coil Setpoint Schedule to set the supply air setpoint. OutdoorAirTemperatureReset varies the supply air setpoint based on the values entered for Heating Coil Setpoint at Outdoor Dry-Bulb Low, Heating Coil Reset Outdoor Dry-Bulb Low, Heating Coil Setpoint at Outdoor Dry-Bulb High, and Heating Coil Reset Outdoor Dry-Bulb High. The default is FixedSetpoint.
-
-NOTE: The user must ensure that the cooling coil and heating coil setpoints do not overlap to avoid unwanted simultaneous heating and cooling. The simulation will not check this automatically. It is recommended that the cooling setpoint always be at least 0.1C higher than the heating coil setpoint.
-
-#### Field: Heating Coil Design Setpoint
-
-Enter the heating supply air temperature in C to be used for sizing the heating coil and zone supply air flow rates. If Heating Coil Setpoint Control Type = FixedSetpoint, then this value is also used as the constant heating supply air setpoint temperature.  The default is 12.2C.
-
-#### Field: Heating Coil Setpoint Schedule Name
-
-This field is used when Heating Coil Setpoint Control Type = Scheduled. The schedule should control the supply air temperature delivered to the zones. For Blow Through fan placement, this is the leaving air temperature from the heating coil. For Draw Through fan placement, this is the leaving air temperature after the supply fan. The values in the schedule are in degrees C.
-
-#### Field: Heating Coil Setpoint at Outdoor Dry-Bulb Low
-
-The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or below the low limit (Heating Coil Reset Outdoor Dry-Bulb Low). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 15.0C.
-
-#### Field: Heating Coil Reset Outdoor Dry-Bulb Low
-
-The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb Low. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 7.8C.
-
-#### Field: Heating Coil Setpoint at Outdoor Dry-Bulb High
-
-The heating coil supply air setpoint temperature in C when the outdoor dry-bulb temperature is at or above the high limit (Heating Coil Reset Outdoor Dry-Bulb High). Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.2C.
-
-#### Field: Heating Coil Reset Outdoor Dry-Bulb High
-
-The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Heating Coil Setpoint at Outdoor Dry-Bulb High. Used only when Heating Coil Setpoint Control Type = OutdoorAirTemperatureReset. The default is 12.2C.
-
-#### Field: Gas Heating Coil Efficiency
-
-Enter gas burner efficiency as a decimal, not as a percent. A burner that is 80% efficient would have an entry of 0.8 here, which is the default. This field is only used when the heating coil type is set to gas.
-
-#### Field: Gas Heating Coil Parasitic Electric Load
-
-Enter the parasitic electric load associated with the gas heating coil operation, such as a combustion fan. The units are in W. This field is only used when the heating coil type is set to gas.
-
-#### Field: Heat Recovery Type
-
-Enter the type of air-to-air heat recovery which is available between the relief air stream and the outdoor air inlet stream. The choices are:
-
-- None
-
-- Sensible
-
-- Enthalpy
-
-The default is None*.*
-
-#### Field: Heat Recovery Sensible Effectiveness []
-
-Enter the sensible heat recovery effectiveness. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.70.
-
-#### Field: Heat Recovery Latent Effectiveness []
-
-Enter the latent heat recovery effectiveness if Heat Recovery Type is *Enthalpy*. This is applied as a constant effectiveness at all conditions. The valid range is from 0.0 to 1.0, and the default is 0.65.
-
-#### Field: Heat Recovery Heat Exchanger Type
-
-This alpha field denotes the type of heat exchanger being modeled: Plate (e.g., fixed plate) or Rotary (e.g., rotating cylinder or wheel). The default choice for this field is “Plate�. The heat exchanger type affects the modeling of frost control options and supply air outlet temperature control. For rotary heat exchangers, rotational speed is varied to control frost formation or the supply air outlet temperature. For plate exchangers, air bypass around the heat exchanger is used to obtain the desired effect.
-
-#### Field: Heat Recovery Frost Control Type
-
-This alpha field has four choices: None, ExhaustAirRecirculation, ExhaustOnly and MinimumExhaustTemperature. If this field is left blank, the default frost control type is “None�. For modeling preheat frost control, specify “None� for this input field and insert a separate heating coil object in the supply inlet air stream to keep the air temperature above the desired frost threshold temperature.
-
-*ExhaustAirRecirculation*: dampers are used to direct exhaust air back into the zone through the supply side of the heat exchanger when the supply (outdoor) air inlet temperature falls below a threshold temperature. The fraction of time that exhaust air is circulated through the supply side of the heat exchanger is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When exhaust air is being recirculated, no supply (outdoor ventilation) air is being provided through the heat exchanger unit (which may or may not be acceptable regarding ventilation for occupants).
-
-*ExhaustOnly (supply air bypass)*: this control cycles off the supply air flow through the heat exchanger for a certain period of time while the exhaust air continues to flow through the exhaust side of the heat exchanger. The fraction of time that the supply flow through the heat exchanger is cycled off is dependent on the supply (outdoor) air inlet temperature with respect to the threshold temperature, the initial defrost time fraction, and the rate of change of defrost time. When implemented in real applications, provisions are usually made to avoid building depressurization when this frost control is operating (automatic or pressure-operated dampers, or a bypass air damper around the supply side of the heat exchanger). For this frost control type, it is assumed that the supply air is bypassed around the heat exchanger during frost control operation (i.e., the total supply flow is not reduced during defrost, but merely bypassed around the heat exchanger).
-
-*MinimumExhaustTemperature*: the temperature of the exhaust air leaving the heat exchanger is monitored and the heat exchanger effectiveness is decreased (by slowing heat exchanger rotation or bypassing supply air around the plate exchanger) to keep the exhaust air from falling below the threshold temperature.
-
-#### Field: Dehumidification Control Type
-
-There are three dehumidification control type options available:
-
-- None
-
-- CoolReheatHeatingCoil
-
-- CoolReheatDesuperheater
-
-- Multimode
-
-The *CoolReheatHeatingCoil* option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so.  Reheat is provided as required by the heating coil, if available.
-
-The *CollReheatDesuperheater* option cools beyond the dry-bulb setpoint as required to meet the humidity setpoint if the system is capable of doing so. Reheat is provided by a desuperheater coil (Ref. object Coil:Heating:Desuperheater). The desuperheater coil setpoint is set to the cooling setpoint and the desuperheater Heat Reclaim Recovery Efficiency is set to 0.3. *CollReheatDesuperheater* is only applicable for Cooling Coil Type *TwoSpeedDX, TwoStageDX, TwoStageHumidityControlDX, or HeatExchangerAssistedDX.*
-
-*Multimode* is only applicable for cooling coil type *TwoStageHumidityControlDX*. In this case, the enhanced dehumidification mode is activated as needed, but the system operates to meet the sensible dry-bulb temperature cooling setpoint.
-
-The default is *None* which meets the sensible dry-bulb temperature cooling setpoint only.
-
-#### Field: Dehumidification Setpoint
-
-This field specifies the supply air humidity ratio setpoint for dehumidification.  The default is 0.00924 kgWater/kgDryAir (12.8C or 55F dewpoint).  This value is also used as the Central Cooling Design Supply Air Humidity Ratio in the Sizing:System object. If a Dehumidification Setpoint Schedule Name is specified, the schedule will be used for control.
-
-#### Field: Humidifier Type
-
-There are two humidifier type options available:
-
-- None
-
-- ElectricSteam
-
-The *ElectricSteam* humidifier option uses the Humidifier:Steam:Electric object.  The default is *None.*
-
-#### Field: Humidifier Availability Schedule Name
-
-If left blank, the humidifier will be available anytime the system is operating. If a schedule name is specified, it defines when the humidifier is available. The schedule values denote whether the humidifier can run during a given time period. A schedule value of 1.0 indicates that the humidifier can be on during a given time period. A value of zero denotes that the humidifier cannot be used during that time period.
-
-#### Field: Humidifier Rated Capacity
-
-Enter the rated moisture output rate in m3/s.  The humidifier does not currently autosize, so the default is very large to allow for adequate capacity.  The default is 0.000001 m3/s.
-
-#### Field: Humidifier Rated Electric Power
-
-Enter the electric power input at the rated capacity moisture output. This field can be autosized. When it is autosized, it is calculated from the rated capacity in kg/s and the enthalpy rise in J/kg of the feed water from a reference temperature of liquid water at 20°C to saturated steam at 100°C.
-
-#### Field: Humidifier Setpoint
-
-This field specifies the supply air humidity ratio setpoint for humidification. The default is 0.003 kgWater/kgDryAir. This value is also used as the Central Heating Design Supply Air Humidity Ratio in the Sizing:System object. If a Humidifier Setpoint Schedule Name is specified, the schedule will be used for control.
-
-#### Field: Dehumidification Setpoint Schedule Name
-
-Enter the name of the dehumidification setpoint schedule. If this field is left blank, the setpoint will be constant at the Dehumidification Setpoint,  The values in the schedule are in units of humidity ratio (kgWater/kgDryAir or lbWater/lbDryAir).
-
-#### Field: Humidifier Setpoint Schedule Name
-
-Enter the name of the humidifier setpoint schedule. If this field is left blank, the setpoint will be constant at the Humidifier Setpoint,  The values in the schedule are in units of humidity ratio (kgWater/kgDryAir or lbWater/lbDryAir).
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:System:DedicatedOutdoorAir,
-    DOAS,                    !- Name
-    ,                        !- System Availability Schedule Name
-    DirectIntoZone,          !- Air Outlet Type
-    autosize,                !- Supply Fan Flow Rate {m3/s}
-    0.7,                     !- Supply Fan Total Efficiency
-    1000,                    !- Supply Fan Delta Pressure {Pa}
-    0.9,                     !- Supply Fan Motor Efficiency
-    1,                       !- Supply Fan Motor in Air Stream Fraction
-    DrawThrough,             !- Supply Fan Placement
-    ChilledWater,            !- Cooling Coil Type
-    ,                        !- Cooling Coil Availability Schedule Name
-    FixedSetpoint,           !- Cooling Coil Setpoint Control Type
-    ,                        !- Cooling Coil Setpoint Schedule Name
-    12.8,                    !- Cooling Coil Design Setpoint {C}
-    15.6,                !- Cooling Coil Setpoint at Outdoor Dry-Bulb Low {C}
-    15.6,                    !- Cooling Coil Reset Outdoor Dry-Bulb Low {C}
-    12.8,               !- Cooling Coil Setpoint at Outdoor Dry-Bulb High {C}
-    23.3,                    !- Cooling Coil Reset Outdoor Dry-Bulb High {C}
-    autosize,           !- DX Cooling Coil Gross Rated Total Capacity {W}
-    autosize,           !- DX Cooling Coil Gross Rated Sensible Heat Ratio
-    3,                       !- DX Cooling Coil Gross Rated COP
-    HotWater,                !- Heating Coil Type
-    ,                        !- Heating Coil Availability Schedule Name
-    FixedSetpoint,           !- Heating Coil Setpoint Control Type
-    ,                        !- Heating Coil Setpoint Schedule Name
-    12.2,                    !- Heating Coil Design Setpoint {C}
-    15,                  !- Heating Coil Setpoint at Outdoor Dry-Bulb Low {C}
-    7.8,                     !- Heating Coil Reset Outdoor Dry-Bulb Low {C}
-    12.2,               !- Heating Coil Setpoint at Outdoor Dry-Bulb High {C}
-    12.2,                    !- Heating Coil Reset Outdoor Dry-Bulb High {C}
-    0.8,                     !- Gas Heating Coil Efficiency
-    ,                        !- Gas Heating Coil Parasitic Electric Load {W}
-    Enthalpy,                !- Heat Recovery Type
-    0.7,                     !- Sensible Heat Recovery Effectiveness
-    0.65,                    !- Latent Heat Recovery Effectiveness
-    Plate,                   !- Heat Exchanger Type
-    None,                    !- Frost Control Type
-    None,                    !- Dehumidification Control Type
-    0.00924,                 !- Dehumidification Setpoint {kgWater/kgDryAir}
-    None,                    !- Humidifier Type
-    ,                        !- Humidifier Availability Schedule Name
-    0.000001,                !- Humidifier Rated Capacity {m3/s}
-    2690,                    !- Humidifier Rated Electric Power {W}
-    0.003,                   !- Humidifier Setpoint {kgWater/kgDryAir}
-    ,                        !- Dehumidification Setpoint Schedule Name
-    ;                        !- Humidifier Setpoint Schedule Name
-```
-
-
-### HVACTemplate:Plant:ChilledWaterLoop
-
-The piping systems that connect the chilled water coils in the HVAC template objects with the chillers and the cooling towers (if present) are described with this object. The piping systems are called loops and this object describes the controls and pumps on the loops. Only one of these objects may be defined in an input file and all chilled water coils from HVAC template objects are served with this object.
-
-#### Field: Name
-
-The name used to designate the HVACTemplate:Plant:ChilledWaterLoop.
-
-#### Field: Pump Schedule Name
-
-Leave this field blank if the chilled water and condenser water pumps are always available. If a schedule name is specified, those times that the pumps are available should be specified as 1.0. Those times that the pumps are not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the system is providing chilled water to the coils but a schedule of when it can provide chilled water to the coils.
-
-#### Field: Pump Control Type
-
-Applies to both chilled water and condenser loop pumps. The choices for this field are:
-
-- Intermittent
-
-- Continuous
-
-The default value is Intermittent.
-
-If the pump control type is **Continuous**, the pump will run according to the Pump Schedule (see above) regardless of whether or not there is a load. If the pump control type is **Intermittent**, the pump will run if a load is sensed and will shut off if there is no load on the loop.
-
-#### Field: Chiller Plant Operation Scheme Type
-
-The choices for this field are:
-
-- Default
-
-- UserDefined
-
-Default operation type makes all equipment available at all times operating in order of Priority specified in HVACTemplate:Plant:Chiller objects. If a different scheme is to be used to sequence the chillers, then this entry should be set to User Defined. If the User Defined option is chosen, then additional EnergyPlus objects must be included and completely defined in the IDF file such as shown below depending on the type of plant operation control scheme chosen:
-
-- PlantEquipmentOperationSchemes
-
-- PlantEquipmentOperation:CoolingLoad
-
-- PlantEquipmentList (refer to HVACTemplate:Plant:Chiller object description for chiller key name required in this object).
-
-The default value is Default.
-
-#### Field: Chiller Plant Equipment Operation Schemes Name
-
-This field should contain the name of a PlantEquipmentOperationSchemes object only when the previous field is set to UserDefined. It is ignored if Chiller Plant Operation Scheme Type is Default.
-
-#### Field: Chilled Water Setpoint Schedule Name
-
-Enter the name of a chilled water setpoint schedule that has values that change at different times of the year. If a constant set point is needed simply leave this field blank and the value in the next field will be used at all times. The values in the schedule are in degrees C. This field is ignored if the Chilled Water Setpoint Reset Type is something other than None.
-
-#### Field: Chilled Water Design Setpoint
-
-Enter the chilled water setpoint temperature to be used for sizing the chilled water loop and associated equipment in degrees C. If the Chilled Water Setpoint Schedule is blank and the Chilled Water Setpoint Reset Type is *None*, then this value will be used as the setpoint at all times.
-
-#### Field: Chilled Water Pump Configuration
-
-The choices for this field are
-
-- VariablePrimaryNoSecondary – variable flow to chillers and coils
-
-- ConstantPrimaryNoSecondary – constant flow to chillers and coils with bypass
-
-- ConstantPrimaryVariableSecondary – constant flow to chillers with bypass, variable flow to coils
-
-- VariablePrimaryConstantSecondary – variable flow to chillers, constant flow to coils with bypass
-
-The default value is ConstantPrimaryNoSecondary.
-
-The operation of a constant speed pump is fairly straightforward. If the user designates a constant speed pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump is constant speed and operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop.
-
-A variable speed pump is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump is operating intermittently, then the pump can shutdown. For any other condition such as the loop having a load and the pump is operating intermittently or the pump is continuously operating (regardless of the loading condition), the pump will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump is running, it will try to meet the flow request made by demand side components.
-
-#### Field: Primary Chilled Water Pump Rated Head
-
-The rated head of the primary chilled water pump in Pa. The default value is 179352 Pa which is equivalent to 60 feet H2O.
-
-#### Field: Secondary Chilled Water Pump Rated Head
-
-The rated head of the secondary chilled water pump in Pa. The default value is 179352 Pa which is equivalent to 60 feet H<sub>2</sub>O.  This field is applicable only if the “Chilled Water Pump Configuration� is *Constant Primary Variable Secondary* or *Variable Primary Constant Secondary*.
-
-#### Field: Condenser Plant Operation Scheme Type
-
-The choices for this field are:
-
-- Default
-
-- UserDefined
-
-Default operation type makes all equipment available at all times operating in order of Priority specified in HVACTemplate:Plant:Tower objects. If a different scheme is to be used to sequence the towers, then this entry should be set to User Defined. May be left blank if not serving any water cooled chillers.
-
-If User Defined option is chosen, then additional EnergyPlus objects must be included and completely defined in the IDF file such as shown below depending on the type of condenser operation control scheme chosen:
-
-- CondenserEquipmentOperationSchemes
-
-- PlantEquipmentOperation:CoolingLoad
-
-- PlantEquipmentList (refer to the HVACTemplate:Plant:Tower object description for key name required for this object.
-
-The default value is Default.
-
-#### Field: Condenser Equipment Operation Schemes Name
-
-This field should contain the name of a CondenserEquipmentOperationSchemes object only when the previous field is set to UserDefined. It is ignored if Condenser Plant Operation Scheme Type is Default. May be left blank if not serving any water cooled chillers.
-
-#### Field: Condenser Water Temperature Control Type
-
-If water cooled chillers are present the condenser water temperature control can be one of the following options:
-
-- OutdoorWetBulbTemperature
-
-- SpecifiedSetpoint
-
-If a specified set point is used then the towers are operated to deliver that condenser water set point. If outdoor wet-bulb is used then the condenser water temperature decreases with decreasing outdoor wet-bulb temperature. May be left blank if not serving any water cooled chillers.
-
-#### Field: Condenser Water Setpoint Schedule Name
-
-Used when Condenser Water Temperature Control Type is set to Specified Setpoint. Ignored if Condenser Water Temperature Control Type is set to Outdoor Wet-bulb. The field may be left blank if constant setpoint temperature is used for the condenser water temperature. If may also be left blank if not serving any water cooled chillers. If specified, the schedule should contain the set point temperatures in degrees C for the condenser water loop.
-
-#### Field: Condenser Water Design Setpoint
-
-- Enter the condenser water temperature to be used for sizing the condenser loop and associated equipment. If a constant setpoint control is used for the condenser water, this value will be used as the setpoint at all times. May be left blank if not serving any water cooled chillers. Used when Condenser Water Temperature Control Type is set to Specified Setpoint. Ignored if Condenser Water Temperature Control Type is set to OutdoorWetBulbTemperature. The units are in C.
-
-#### Field: Condenser Water Pump Rated Head
-
-The rated head of the condenser water pumps in  Pa. May be left blank if not serving any water cooled chillers. The default value is 179352 Pa which is equivalent to 60 feet H2O.
-
-#### Field: Chilled Water Setpoint Reset Type
-
-Select the type of automatic reset control for the chilled water supply temperature. The choices are:
-
-- None – no reset, use the Chilled Water Setpoint Schedule or Chilled Water Design Setpoint.
-
-- OutdoorAirTemperatureReset – reset the chilled water supply temperature based on the following default rules. The temperature limits and setpoints are specified using the fields below. If the default values are used, when the outdoor dry-bulb temperature (ODB) is at or below 15.6C the setpoint is 12.2C. When the ODB is at or above 26.7C the setpoint is 6.7C. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset)
-
-The default is *None*.
-
-#### Field: Chilled Water Setpoint at Outdoor Dry-Bulb Low
-
-The chilled water setpoint temperature in C when the outdoor dry-bulb is at or below the low limit (Chilled Water Reset Outdoor Dry Bulb Low). The default is 12.2C.
-
-#### Field: Chilled Water Reset Outdoor Dry-Bulb Low
-
-The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Chilled Water Setpoint at Outdoor Dry Bulb Low. The default is 15.6C.
-
-#### Field: Chilled Water Setpoint at Outdoor Dry-Bulb High
-
-The chilled water setpoint temperature in C when the outdoor dry-bulb is at or above the high limit (Chilled Water Reset Outdoor Dry Bulb Low). The default is 6.7C.
-
-#### Field: Chilled Water Reset Outdoor Dry-Bulb High
-
-The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Chilled Water Setpoint at Outdoor Dry Bulb High. The default is 26.7C.
-
-#### Field: Chilled Water Primary Pump Type
-
-Describes the type of pump configuration used for the primary portion of the chilled water loop. The options include:
-
-- SinglePump
-
-- PumpPerChiller
-
-- TwoHeaderedPumps
-
-- ThreeHeaderedPumps
-
-- FourHeaderedPumps
-
-- FiveHeaderedPumps
-
-#### Field: Chilled Water Secondary Pump Type
-
-Describes the type of pump configuration used for the secondary portion of the chilled water loop. The options include:
-
-- SinglePump
-
-- TwoHeaderedPumps
-
-- ThreeHeaderedPumps
-
-- FourHeaderedPumps
-
-- FiveHeaderedPumps
-
-#### Field: Condenser Water Pump Type
-
-Describes the type of pump configuration used for the condenser water loop. The options include:
-
-- SinglePump
-
-- PumpPerTower
-
-- TwoHeaderedPumps
-
-- ThreeHeaderedPumps
-
-- FourHeaderedPumps
-
-- FiveHeaderedPumps
-
-#### Field: Chilled Water Supply Side Bypass Pipe
-
-The field determines if a supply side bypass pipe is present in the chilled water loop. The choices for this field are
-
-- Yes
-
-- No.
-
-#### Field: Chilled Water Demand Side Bypass Pipe
-
-The field determines if a demand side bypass pipe is present in the chilled water loop. The choices for this field are
-
-- Yes
-
-- No.
-
-#### Field: Condenser Water Supply Side Bypass Pipe
-
-The field determines if a supply side bypass pipe is present in the condenser water loop. The choices for this field are
-
-- Yes
-
-- No.
-
-#### Field: Condenser Water Demand Side Bypass Pipe
-
-The field determines if a demand side bypass pipe is present in the condenser water loop. The choices for this field are
-
-- Yes
-
-- No.
-
-#### Field: Fluid Type
-
-This field determines the type of fluid used for the boiler loop. The following options are available:
-
-- Water
-
-- EthyleneGlycol30
-
-- EthyleneGlycol40
-
-- EthyleneGlycol50
-
-- EthyleneGlycol60
-
-- PropyleneGlycol30
-
-- PropyleneGlycol40
-
-- PropyleneGlycol50
-
-- PropyleneGlycol60
-
-#### Field: Loop Design Delta Temperature
-
-The temperature difference used in sizing the loop flow rate. The default is 6.67C.
-
-#### Field: Minimum Outdoor Dry Bulb Temperature
-
-The minimum outdoor dry bulb temperature that the chilled water loops operate.
-
-#### Field: Chilled Water Load Distribution Scheme
-
-The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. **Optimal** operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. **SequentialLoad** loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. **UniformLoad** evenly distributes the loop demand among all available components on the equipment list for a given load range. **SequentialUniformPLR** loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. **UniformPLR** will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
-
-Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
-
-
-#### Field: Condenser Water Load Distribution Scheme
-
-The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. **Optimal** operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. **SequentialLoad** loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. **UniformLoad** evenly distributes the loop demand among all available components on the equipment list for a given load range. **SequentialUniformPLR** loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. **UniformPLR** will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
-
-Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:Plant:ChilledWaterLoop,
-    Chilled Water Loop,      !- Plant Loop Name
-    CoolingPumpAvailSched,   !- Pump Schedule
-    Intermittent,            !- Pump Control Type
-    Default,                 !- Chiller Plant Operation Scheme Type
-    ,                        !- Chiller Plant Operation Scheme Name
-    CW Loop Temp Schedule,   !- Chilled Water Setpoint Schedule
-    7.22,                    !- Chilled Water Design Setpoint {C}
-    VariableFlowNoSecondary, !- Chilled Water Pump Configuration
-    179352,                  !- Primary Chilled Water Pump Rated Head {Pa}
-    179352,                  !- Secondary Chilled Water Pump Rated Head {Pa}
-    Default,                 !- Condenser Plant Operation Scheme Type
-    ,                        !- Condenser Plant Operation Scheme List Name
-    OutdoorWetBulbTemperature,    !- Condenser Water Temperature Control Type
-    ,                        !- Condenser Water Setpoint Schedule
-    29.4,                    !- Condenser Water Design Setpoint {C}
-    179352,                  !- Condenser Water Pump Rated Head {Pa}
-    None,                    !- Chilled Water Setpoint Reset Type
-    12.2,              !- Chilled Water Setpoint at Outdoor Dry Bulb Low {C}
-    15.6,              !- Chilled Water Reset Outdoor Dry Bulb Low {C}
-    6.7,               !- Chilled Water Setpoint at Outdoor Dry Bulb High {C}
-    26.7,              !- Chilled Water Reset Outdoor Dry Bulb High {C}
-    SinglePump,              !- Chilled Water Primary Pump Type
-    SinglePump,              !- Chilled Water Secondary Pump Type
-    SinglePump,              !- Condenser Water Pump Type
-    Yes,                     !- Chilled Water Supply Side Bypass Pipe
-    Yes,                     !- Chilled Water Demand Side Bypass Pipe
-    Yes,                     !- Condenser Water Supply Side Bypass Pipe
-    Yes,                     !- Condenser Water Demand Side Bypass Pipe
-    Water,                   !- Fluid Type
-    6.67,                    !- Loop Design Delta Temperature {deltaC}
-    ,                        !- Minimum Outdoor Dry Bulb Temperature {C}
-    SequentialLoad,          !- Chilled Water Load Distribution Scheme
-    SequentialLoad;          !- Condenser Water Load Distribution Scheme
-```
-
-### HVACTemplate:Plant:Chiller
-
-A chiller or purchased cooling source is described with this object. To define multiple chillers, use multiple HVACTemplate:Plant:Chiller objects and use the Sizing Factor field to apportion the total capacity if autosizing.
-
-#### Field: Name
-
-The name used to reference the HVACTemplate:Plant:Chiller object.
-
-#### Field: Chiller Type
-
-While EnergyPlus has a variety of chiller options, the only choices currently for this field are:
-
-- DistrictChilledWater
-
-- ElectricCentrifugalChiller
-
-- ElectricScrewChiller
-
-- ElectricReciprocatingChiller
-
-The EnergyPlus equipment object types which are used are DistrictCooling or Chiller:Electric:EIR. These equipment type keys must be used if setting up a user-defined chiller plant operation scheme.
-
-#### Field: Capacity
-
-This field may be set to autosize, which means that the capacity is based on the peak loads during the design days. This numeric field contains the design cooling capacity of the chiller. This capacity should be at the design temperatures and water flow rates. The units are in W.
-
-#### Field: Nominal COP
-
-This numeric field contains the chiller’s coefficient of performance. This value should **not** include energy use due to pumps, evap-cooled or air-cooled condenser fans, or cooling tower fans. This Nominal COP should be at the design temperatures and water flow rates. Not applicable if Chiller Type is DistrictChilledWater.
-
-#### Field: Condenser Type
-
-The choices for this field are
-
-- AirCooled
-
-- WaterCooled
-
-- EvaporativelyCooled
-
-The default value is WaterCooled. If WaterCooled, then at least one HVACTemplate:Plant:Tower object should be defined. Not applicable if Chiller Type is Purchased Chilled Water.
-
-#### Field: Priority
-
-Enter the priority number of the chiller where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Chiller Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:ChilledWaterLoop. Equipment is operated in order of the priority number. This allows multiple chillers to be sequenced.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the chiller object inputs that would be altered by the sizing factor are: Reference Capacity, Reference Chilled Water Flow Rate and Reference Condenser Water Flow Rate. Sizing Factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the chiller’s minimum part-load ratio. The expected range is between 0 and 1. Below this part-load ratio, the compressor cycles on and off to meet the cooling load. The Minimum Part Load Ratio must be less than or equal to the Maximum Part Load Ratio. The default value is 0.0.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the chiller’s maximum part-load ratio. This value may exceed 1, but the normal range is between 0.0 and 1.0. The Maximum Part Load Ratio must be greater than or equal to the Minimum Part Load Ratio. The default value is 1.0.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the chiller’s optimum part-load ratio. This is the part-load ratio at which the chiller performs at its maximum COP. The optimum part-load ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 1.0.
-
-#### Field: Minimum Unloading Ratio
-
-This numeric field contains the chiller’s minimum unloading ratio. The expected range is between 0 and 1. The minimum unloading ratio is where the chiller capacity can no longer be reduced by unloading and must be false loaded to meet smaller cooling loads. A typical false loading strategy is hot-gas bypass. The minimum unloading ratio must be greater than or equal to the Minimum Part Load Ratio, and less than or equal to the Maximum Part Load Ratio. The default value is 0.25.
-
-#### Field: Leaving Chilled Water Lower Temperature Limit
-
-This numeric field contains the lower limit for the leaving chilled water temperature in Celsius. This temperature acts as a cut off for heat transfer in the evaporator, so that the fluid doesn’t get too cold. The default value is 5˚C.
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:Plant:Chiller,
-    District Cooling,        !- Chiller Name
-    ElectricCentrifugalChiller,  !- Chiller Type
-    autosize,                !- Capacity {W}
-    3.2,                     !- COP
-    WaterCooled,             !- Condenser Type
-    1,                       !- Priority
-    1,                       !- Sizing Factor
-    0.1,                     !- Minimum Part Load Ratio
-    1.1,                     !- Maximum Part Load Ratio
-    0.9,                     !- Optimum Part Load Ratio
-    0.2,                     !- Minimum Unloading Ratio
-    2;                 !- Leaving Chilled Water Lower Temperature Limit {C}
-```
-
-
-### HVACTemplate:Plant:Chiller:ObjectReference
-
-This object references a detailed chiller object and adds it to an HVACTemplate:Plant:ChilledWaterLoop. The user must create a complete detailed chiller object with all required curve or performance objects. The detailed chiller object is referenced by object type and name and the chiller will be automatically to the chilled water loop branches and equipment list.
-
-#### Field: Name
-
-The name of this object.
-
-#### Field: Chiller Object Type
-
-The object type of the referenced chiller. Select from one of the following supported chiller object types:
-
-- Chiller:Electric:EIR
-
-- Chiller:Electric:ReformulatedEIR
-
-#### Field: Chiller Name
-
-The object name of the referenced chiller.
-
-#### Field: Priority
-
-Enter the priority number of the chiller where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Chiller Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:ChilledWaterLoop. Equipment is operated in order of the priority number. This allows multiple chillers to be sequenced.
-
-An example in an IDF:
-
-```idf
-HVACTemplate:Plant:Chiller:ObjectReference,
-    Main Chiller Connection, !- Name
-    Chiller:Electric:EIR,    !- Chiller Object Type
-    Main Chiller,            !- Chiller Name
-    1;                       !- Priority
-```
-
-
-### HVACTemplate:Plant:Tower
-
-A cooling tower is described with this object. To define multiple cooling towers, use multiple HVACTemplate:Plant:Tower objects and use the Sizing Factor field to apportion the total capacity if autosizing.
-
-#### Field: Name
-
-The name used to reference the HVACTemplate:Plant:Tower object.
-
-#### Field: Tower Type
-
-The choices for this field are
-
-- SingleSpeed
-
-- TwoSpeed
-
-The EnergyPlus equipment object types which are used are CoolingTower:SingleSpeed or CoolingTower:TwoSpeed. These equipment type keys must be used if setting up a user-defined condenser plant operation scheme.
-
-#### Field: High-Speed Nominal Capacity
-
-Applicable for Tower Type Single Speed and Two Speed. This field may be set to autosize. If this field is set to autosize, then the Low-Speed Nominal Capacity and the Free Convection Capacity must also be autosized. The units are W. This numeric input field contains the “nominal� heat rejection capacity of the cooling tower in watts under high-speed fan operation, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of high-speed nominal capacity (3 gpm/ton). 125% of this nominal tower capacity gives the actual tower heat rejection at these operating conditions (based on historical assumption that the tower must dissipate 0.25W of compressor heat for every watt of heat removed by the evaporator).
-
-#### Field: High-Speed Fan Power
-
-The tower fan electric consumption when at high speed. Applicable for Tower Type Single Speed and Two Speed. This field may be set to autosize. The units are W.
-
-#### Field: Low-Speed Nominal Capacity
-
-Applicable only for Tower Type Two Speed. This field may be set to autosize. If this field is set to autosize, then the High-Speed Nominal Capacity and the Free Convection Capacity must also be autosized. The units are W. This numeric input field contains the “nominal� heat rejection capacity of the cooling tower in watts under low-speed fan operation, with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of high-speed nominal tower capacity (input field above). 125% of this nominal tower capacity gives the actual tower heat rejection at these operating conditions (based on historical assumption that the tower must dissipate 0.25W of compressor heat for every watt of heat removed by the evaporator). The value specified for this field must be greater than zero but less than the value specified for the field “Tower High-Speed Nominal Capacity�.
-
-#### Field: Low-Speed Fan Power
-
-The tower fan electric consumption when at low speed. Applicable only for Tower Type Two Speed. This field may be set to autosize. The units are W.
-
-#### Field: Free Convection Capacity
-
-Applicable for Tower Type Single Speed and Two Speed. This field may be set to autosize. If this field is set to autosize, then the High-Speed Nominal Capacity and the Low-Speed Nominal Capacity must also be autosized. The units are W. This numeric input field contains the “nominal� heat rejection capacity of the cooling tower in watts when the tower is in the “free convection� regime (water flow exists but tower fan is turned off), with entering water at 35C (95F), leaving water at 29.4C (85F), entering air at 25.6C (78F) wetbulb and 35C (95F) drybulb temperatures. The design water flow rate is assumed to be 5.382E-8 m<sup>3</sup>/s per watt of high-speed nominal tower capacity (input field above). 125% of this free convection tower capacity gives the actual tower heat rejection at these operating conditions (based on historical assumption that the tower must dissipate 0.25W of compressor heat for every watt of heat removed by the evaporator). If the user does not wish to model “free convection�, then this field should be set to 0.0.
-
-#### Field: Priority
-
-Enter the priority number of the tower where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Condenser Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:ChilledWaterLoop or HVACTemplate:Plant:MixedWaterLoop. Equipment is operated in order of the priority number. This allows multiple towers to be sequenced.
-
-***Field: Sizing Factor***
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.For this component the tower object inputs that would be altered by the sizing factor are:
-
-1.    Design Water Flow Rate;
-
-2.    Air Flow Rate at High Fan Speed;
-
-3.    Fan Power at High Fan Speed;
-
-4.    U-Factor Times Area Value at High Fan Speed;
-
-5.    Air Flow Rate at Low Fan Speed (for two-speed tower);
-
-6.    Fan Power at Low Fan Speed (for two-speed tower);
-
-7.    U-Factor Times Area Value at Low Fan Speed (for two-speed tower);
-
-8.    Air Flow Rate in Free Convection Regime;
-
-9.    U-Factor Times Area Value at Free Convection Air Flow Rate.
-
-Note that the U-Factor Times Area Value at High Fan Speed is not *multiplied* by the Sizing Factor. Instead the design tower load is multiplied by the sizing factor and the design UA then calculated as usual. The U-Factor Times Area Value at Low Fan Speed is set to 60% of the full load design UA. The U-Factor Times Area Value at Free Convection Air Flow Rate is set to 10% of the design Tower UA.
-
-#### Field: Template Plant Loop Type
-
-This field specifies whether this tower will serve a *ChilledWaterLoop* (ref. HVACTemplate:Plant:ChilledWaterLoop) or a *MixedWaterLoop* (ref. HVACTemplate:Plant:MixedWaterLoop). If this field is left blank, this tower will serve a ChilledWaterLoop if present or a MixedWaterLoop (if no ChilledWaterLoop is present).
-
-An example in an IDF:
-
-```idf
-  HVACTemplate:Plant:Tower,
-    Main Tower,              !- Name
-    SingleSpeed,             !- Tower Type
-    autosize,                !- High Speed Nominal Capacity {W}
-    autosize,                !- High Speed Fan Power {W}
-    autosize,                !- Low Speed Nominal Capacity {W}
-    autosize,                !- Low Speed Fan Power {W}
-    autosize,                !- Free Convection Capacity {W}
-    1,                       !- Priority
-    ;                        !- Sizing Factor
-```
-
-
-### HVACTemplate:Plant:Tower:ObjectReference
-
-This object references a detailed cooling tower object and adds it to an HVACTemplate:Plant:ChilledWaterLoop or MixedWaterLoop. The user must create a complete detailed cooling tower object with all required curve or performance objects. The detailed cooling tower object is referenced by object type and name and the tower will be automatically to the chilled water loop or mixed water loop branches and equipment list.
-
-#### Field: Name
-
-The name of this object.
-
-#### Field: Cooling Tower Object Type
-
-The object type of the referenced tower. Select from one of the following supported tower object types:
-
-- CoolingTower:SingleSpeed
-
-- CoolingTower:TwoSpeed
-
-- CoolingTower:VariableSpeed
-
-#### Field: Cooling Tower Name
-
-The object name of the referenced tower.
-
-#### Field: Priority
-
-Enter the priority number of the tower where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Condenser Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:ChilledWaterLoop or MixedWaterLoop. Equipment is operated in order of the priority number. This allows multiple towers to be sequenced.
-
-#### Field: Template Plant Loop Type
-
-This field specifies whether this tower will serve a *ChilledWaterLoop* (ref. HVACTemplate:Plant:ChilledWaterLoop) or a *MixedWaterLoop* (ref. HVACTemplate:Plant:MixedWaterLoop). If this field is left blank, this tower will serve a ChilledWaterLoop if present or a MixedWaterLoop (if no ChilledWaterLoop is present).
-
-
-
-An example in an IDF:
-
-```idf
-HVACTemplate:Plant:Tower:ObjectReference,
-    Main Tower Connection,   !- Name
-    CoolingTower:TwoSpeed,   !- Cooling Tower Object Type
-    Main Tower,              !- Cooling Tower Name
-    1;                       !- Priority
-```
-
-
-### HVACTemplate:Plant:HotWaterLoop
-
-The piping systems that connect the hot water coils in the HVAC template objects with the boilers are described with this object. The piping systems are called loops and this object describes the controls and pumps on the loops. Only one of these objects should be defined in an input file and all hot water coils from HVAC template objects are served with this object.
-
-#### Field: Name
-
-The name used to designate the HVACTemplate:Plant:HotWaterLoop.
-
-#### Field: Pump Schedule Name
-
-Leave this field blank if the hot water pump is always available. If a schedule name is specified, those times that the pump is available should be specified as 1.0. Those times that the pump is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the system is providing hot water to the coils but a schedule of when it can provide hot water to the coils.
-
-#### Field: Pump Control Type
-
-The choices for this field are
-
-- Intermittent
-
-- Continuous
-
-The default value is Intermittent.
-
-If the pump control type is **Continuous**, the pump will run according to the Pump Schedule (see above) regardless of whether or not there is a load. If the pump control type is **Intermittent**, the pump will run if a load is sensed and will shut off if there is no load on the loop.
-
-#### Field: Hot Water Plant Operation Scheme Type
-
-The choices for this field are:
-
-- Default
-
-- UserDefined
-
-Default operation type makes all equipment available at all times operating in order of Priority specified in HVACTemplate:Plant:Boiler objects. If a different scheme is to be used to sequence the boilers, then this entry should be set to User Defined.
-
-If User Defined option is chosen, then additional EnergyPlus objects must be defined in the IDF file such as shown below depending on the type of plant operation control scheme chosen:
-
-- PlantEquipmentOperationSchemes
-
-- PlantEquipmentOperation:HeatingLoad
-
-- PlantEquipmentList (refer to HVACTemplate:Plant:Boiler object description for key name required in this object)
-
-The default value is Default.
-
-#### Field: Hot Water Plant Equipment Operation Schemes Name
-
-This field should contain the name of a PlantEquipmentOperationSchemes object only when the previous field is set to User Defined. It is ignored if Hot Water Plant Operation Scheme Type is Default.
-
-#### Field: Hot Water Setpoint Schedule Name
-
-Enter the name of a hot water setpoint schedule that has values that change at different times of the year. If a constant set point is needed simply leave this field blank and the value in the next field will be used at all times. The values in the schedule are in degrees C. This field is ignored if the Hot Water Setpoint Reset Type is something other than None.
-
-#### Field: Hot Water Design Setpoint
-
-Enter the hot water setpoint temperature to be used for sizing the hot water loop and associated equipment in degrees C. If the Hot Water Setpoint Schedule is blank and the Hot Water Setpoint Reset Type is *None*, then this value will be used as the setpoint at all times.
-
-#### Field: Hot Water Pump Configuration
-
-The choices for this field are
-
-- VariableFlow
-
-- ConstantFlow
-
-The default value is ConstantFlow. The variable flow option simulates a pump with variable flow to boilers and coils, excess bypassed. The constant flow option simulates constant flow to boilers and coils, excess bypassed.
-
-The operation of a constant speed pump is fairly straightforward. If the user designates a constant speed pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump is constant speed and operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop.
-
-A variable speed pump is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump is operating intermittently, then the pump can shutdown. For any other condition such as the loop having a load and the pump is operating intermittently or the pump is continuously operating (regardless of the loading condition), the pump will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump is running, it will try to meet the flow request made by demand side components.
-
-#### Field: Hot Water Pump Rated Head
-
-The rated head of the hot water pump in Pa. The default value is 179352 Pa which is equivalent to 60 feet H2O.
-
-#### Field: Hot Water Setpoint Reset Type
-
-Select the type of automatic reset control for the Hot Water supply temperature. The choices are:
-
-- None – no reset, use the Hot Water Setpoint Schedule or Hot Water Design Setpoint.
-
-- OutdoorAirTemperatureReset – reset the Hot Water supply temperature based on the following default rules. The temperature limits and setpoints are specified using the fields below. If the default values are used, when the outdoor dry-bulb temperature (ODB) is at or below –6.7C the setpoint is 82.2C. When the ODB is at or above 10.0C the setpoint is 65.6C. In between, the setpoint is varied linearly. (Reference SetpointManager:OutdoorAirReset)
-
-The default is *None*.
-
-#### Field: Hot Water Setpoint at Outdoor Dry Bulb Low
-
-The Hot Water setpoint temperature in C when the outdoor dry-bulb is at or below the low limit (Hot Water Reset Outdoor Dry Bulb Low). The default is –6.7C.
-
-#### Field: Hot Water Reset Outdoor Dry Bulb Low
-
-The low limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or below this temperature, the setpoint is the value of Hot Water Setpoint at Outdoor Dry Bulb Low. The default is 82.2C.
-
-#### Field: Hot Water Setpoint at Outdoor Dry Bulb High
-
-The Hot Water setpoint temperature in C when the outdoor dry-bulb is at or above the high limit (Hot Water Reset Outdoor Dry Bulb Low). The default is 10.0C.
-
-#### Field: Hot Water Reset Outdoor Dry Bulb High
-
-The high limit of outdoor dry-bulb temperature in C for outdoor air reset control. When the outdoor dry-bulb is at or above this temperature, the setpoint is the value of Hot Water Setpoint at Outdoor Dry Bulb High. The default is 65.6C.
-
-#### Field: Hot Water Pump Type
-
-Describes the type of pump configuration used for the hot water loop. The options include:
-
-- SinglePump
-
-- PumpPerBoiler
-
-- TwoHeaderedPumps
-
-- ThreeHeaderedPumps
-
-- FourHeaderedPumps
-
-- FiveHeaderedPumps
-
-#### Field: Supply Side Bypass Pipe
-
-The field determines if a supply side bypass pipe is present in the hot water loop. The choices for this field are
-
-- Yes
-
-- No.
-
-#### Field: Demand Side Bypass Pipe
-
-The field determines if a demand side bypass pipe is present in the hot water loop. The choices for this field are
-
-- Yes
-
-- No.
-
-#### Field: Fluid Type
-
-This field determines the type of fluid used for the chilled water loop. The following options are available:
-
-- Water
-
-- EthyleneGlycol30
-
-- EthyleneGlycol40
-
-- EthyleneGlycol50
-
-- EthyleneGlycol60
-
-- PropyleneGlycol30
-
-- PropyleneGlycol40
-
-- PropyleneGlycol50
-
-- PropyleneGlycol60
-
-#### Field: Loop Design Delta Temperature
-
-The temperature difference used in sizing the loop flow rate. The default is 11C.
-
-#### Field: Maximum Outdoor Dry Bulb Temperature
-
-The maximum outdoor dry bulb temperature that the hot water loops operate.
-
-#### Field: Load Distribution Scheme
-
-This alpha field contains the Load Distribution Scheme Keyword. The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. **Optimal** operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. **SequentialLoad** loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. **UniformLoad** evenly distributes the loop demand among all available components on the equipment list for a given load range. **SequentialUniformPLR** loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. **UniformPLR** will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
-
-Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:Plant:HotWaterLoop,
-    Hot Water Loop,          !-Plant Loop Name
-    ,                        !- Pump Schedule
-    Intermittent,            !- Pump Control Type
-    Default,                 !- Hot Water Plant Operation Scheme Type
-    ,                        !- Hot Water Plant Operation Scheme List Name
-    HW Loop Temp Schedule,   !- Hot Water Setpoint Schedule
-    82,                    !- Hot Water Design Setpoint {C}
-    VariableFlow,          !- Hot Water Pump Configuration
-    179352,                !- Hot Water Pump Rated Head {Pa}
-    None,                  !- Hot Water Setpoint Reset Type
-    82.2,                  !- Hot Water Setpoint at Outdoor Dry Bulb Low {C}
-    -6.7,                  !- Hot Water Reset Outdoor Dry Bulb Low {C}
-    65.6,                  !- Hot Water Setpoint at Outdoor Dry Bulb High {C}
-    10,                    !- Hot Water Reset Outdoor Dry Bulb High {C}
-    SinglePump,              !- Hot Water Pump Type
-    Yes,                     !- Supply Side Bypass Pipe
-    Yes,                     !- Demand Side Bypass Pipe
-    Water,                   !- Fluid Type
-    11,                      !- Loop Design Delta Temperature {deltaC}
-    ,                        !- Maximum Outdoor Dry Bulb Temperature {C}
-    SequentialLoad;              !- Load Distribution Scheme
-```
-
-
-### HVACTemplate:Plant:Boiler
-
-A boiler or purchased heating source is described with this object. To define multiple boilers, use multiple HVACTemplate:Plant:Boiler objects and use the Sizing Factor field to apportion the total capacity if autosizing.
-
-#### Field: Name
-
-The name used to reference the HVACTemplate:Plant:Boiler object.
-
-#### Field: Boiler Type
-
-While EnergyPlus has a variety of boiler options, the choices for this field are:
-
-- DistrictHotWater – District heating
-
-- HotWaterBoiler – Hot water boiler (non-condensing)
-
-- CondensingHotWaterBoiler – Hot water boiler (condensing)
-
-The EnergyPlus equipment object types which are used are DistrictHeating or Boiler:HotWater. These equipment type keys must be used if setting up a user-defined boiler plant operation scheme.
-
-#### Field: Capacity
-
-This field may be set to autosize, which means that the capacity is based on the peak loads during the design days. This numeric field contains the design heating capacity of the boiler. This capacity should be at the design water flow rates. The units are in W.
-
-#### Field: Efficiency
-
-This numeric field contains the heating efficiency (as a fraction between 0 and 1) of the boiler’s burner. Not applicable if Boiler Type is DistrictHotWater.
-
-#### Field: Fuel Type
-
-The choices for this field are
-
-- Electricity
-
-- NaturalGas
-
-- PropaneGas
-
-- FuelOil\#1
-
-- FuelOil\#2
-
-- Coal
-
-- Diesel
-
-- Gasoline
-
-- OtherFuel1
-
-- OtherFuel2
-
-Not applicable if Boiler Type is DistrictHotWater
-
-#### Field: Priority
-
-Enter the priority number of the boiler where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Boiler Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:HotWaterLoop. Equipment is operated in order of the priority number. This allows multiple boilers to be sequenced.
-
-#### Field: Sizing Factor
-
-This optional numeric field allows the user to specify a sizing factor for this component. The sizing factor is used when the component design inputs are autosized: the autosizing calculations are performed as usual and the results are multiplied by the sizing factor. For this component the boiler object inputs that would be altered by the sizing factor are: Nominal Capacity and Design Water Flow Rate. Sizing factor allows the user to size a component to meet part of the design load while continuing to use the autosizing feature.
-
-#### Field: Minimum Part Load Ratio
-
-This numeric field contains the minimum part load ratio. If the ratio of demand to boiler nominal capacity is less than the minimum part load ratio, then the Min PLR will determine the operating PLR. The expected range is between 0 and 1. If this field is left blank, the default value is 0.0.
-
-#### Field: Maximum Part Load Ratio
-
-This numeric field contains the maximum part load ratio. If the ratio of demand to boiler nominal capacity is greater than the maximum part load ratio, then the Max PLR will determine the operating PLR. This value may exceed 1, but the normal range is between 0 and 1.1. If this field is left blank, the default value is 1.1.
-
-#### Field: Optimum Part Load Ratio
-
-This numeric field contains the optimum part load ratio. This is the part load ratio at which the boiler performs at its maximum efficiency. If this field is left blank, the default value is 1.0.
-
-#### Field: Water Outlet Upper Temperature Limit
-
-This numeric field contains the outlet temperature upper limit. If this field is left blank, the default value is 100.0ºC.
-
-#### Field: Template Plant Loop Type
-
-This field specifies whether this boiler will serve a *HotWaterLoop* (ref. HVACTemplate:Plant:HotWaterLoop) or a *MixedWaterLoop* (ref. HVACTemplate:Plant:MixedWaterLoop). If this field is left blank, this tower will serve a HotWaterLoop if present or a MixedWaterLoop (if no HotWaterLoop is present).
-
-An example in an IDF:
-
-```idf
-  HVACTemplate:Plant:Boiler,
-    Main Boiler,             !- Name
-    HotWaterBoiler,          !- Boiler Type
-    autosize,                !- Capacity {W}
-    0.8,                     !- Efficiency
-    NaturalGas,              !- Fuel Type
-    1,                       !- Priority
-    1,                       !- Sizing Factor
-    0.1,                     !- Minimum Part Load Ratio
-    1.1,                     !- Maximum Part Load Ratio
-    0.9,                     !- Optimum Part Load Ratio
-    99.9;                    !- Water Outlet Upper Temperature Limit {C}
-```
-
-
-### HVACTemplate:Plant:Boiler:ObjectReference
-
-This object references a detailed boiler object and adds it to an HVACTemplate:Plant:HotWaterLoop or MixedWaterLoop. The user must create a complete detailed boiler object with all required curve or performance objects. The detailed boiler object is referenced by object type and name and the boiler will be automatically to the hot water or mixed water loop branches and equipment list.
-
-#### Field: Name
-
-The name of this object.
-
-#### Field: Boiler Object Type
-
-The object type of the referenced boiler. Select from one of the following supported boiler object types:
-
-- Boiler:HotWater
-
-#### Field: Boiler Name
-
-The object name of the referenced boiler.
-
-#### Field: Priority
-
-Enter the priority number of the boiler where 1 is the highest priority, 2 is just lower, 3 is lower than 2, etc. This is used if Hot Water Plant Operation Scheme Type is set to Default in HVACTemplate:Plant:HotWaterLoop or MixedWaterLoop. Equipment is operated in order of the priority number. This allows multiple boilers to be sequenced.
-
-#### Field: Template Plant Loop Type
-
-This field specifies whether this boiler will serve a *HotWaterLoop* (ref. HVACTemplate:Plant:HotWaterLoop) or a *MixedWaterLoop* (ref. HVACTemplate:Plant:MixedWaterLoop). If this field is left blank, this tower will serve a HotWaterLoop if present or a MixedWaterLoop (if no HotWaterLoop is present).
-
-An example in an IDF:
-
-```idf
-HVACTemplate:Plant:Boiler:ObjectReference,
-    Main Boiler Connection,  !- Name
-    Boiler:HotWater,         !- Boiler Object Type
-    Main Boiler,             !- Boiler Name
-    1;                       !- Priority
-```
-
-
-### HVACTemplate:Plant:MixedWaterLoop
-
-This object simulates the central plant loop portion of a water source heat pump system. Often many HVACTemplate:Zone:WaterToAirHeatPump objects will be used in a building along with a single HVACTemplate:Plant:MixedWaterLoop that contains one or more cooling towers and boilers.  The piping systems are called loops and this object describes the controls and pumps on the loops. Only one of these objects should be defined in an input file.
-
-#### Field: Name
-
-The name used to designate the HVACTemplate:Plant:MixedWaterLoop.
-
-#### Field: Pump Schedule Name
-
-Leave this field blank if the water pump is always available. If a schedule name is specified, those times that the pump is available should be specified as 1.0. Those times that the pump is not available should have a zero value in the schedule specified. Please note that this is not a schedule of when the system is providing water to the water-to-air heat pumps but a schedule of when it can provide water to the water-to-air heat pumps.
-
-#### Field: Pump Control Type
-
-The choices for this field are
-
-- Intermittent
-
-- Continuous
-
-The default value is Intermittent.
-
-If the pump control type is **Continuous**, the pump will run according to the Pump Schedule (see above) regardless of whether or not there is a load. If the pump control type is **Intermittent**, the pump will run if a load is sensed and will shut off if there is no load on the loop.
-
-#### Field: Operation Scheme Type
-
-The choices for this field are:
-
-- Default
-
-- UserDefined
-
-Default operation type makes all equipment available at all times operating in order of Priority specified in HVACTemplate:Plant:Boiler objects. If a different scheme is to be used to sequence the boilers, then this entry should be set to User Defined.
-
-If User Defined option is chosen, then additional EnergyPlus objects must be defined in the IDF file such as shown below depending on the type of plant operation control scheme chosen:
-
-- PlantEquipmentOperationSchemes
-
-- PlantEquipmentOperation:CoolingLoad
-
-- PlantEquipmentOperation:HeatingLoad
-
-- PlantEquipmentList (refer to HVACTemplate:Plant:Boiler object description for key name required in this object)
-
-The default value is Default.
-
-#### Field: Equipment Operation Schemes Name
-
-This field should contain the name of a PlantEquipmentOperationSchemes object only when the previous field is set to User Defined. It is ignored if Hot Water Plant Operation Scheme Type is Default.
-
-#### Field: High Temperature Setpoint Schedule Name
-
-Enter the name of a high temperature setpoint schedule that has values that change at different times of the year. If a constant set point is needed simply leave this field blank and the value in the next field will be used at all times. The values in the schedule are in degrees C.
-
-#### Field: High Temperature Design Setpoint
-
-Enter the high temperature setpoint temperature to be used for sizing the water loop and associated equipment in degrees C. If the High Temperature Setpoint Schedule is blank, then this value will be used as the setpoint at all times.  The default is 33C.
-
-#### Field: Low Temperature Setpoint Schedule Name
-
-Enter the name of a low temperature setpoint schedule that has values that change at different times of the year. If a constant set point is needed simply leave this field blank and the value in the next field will be used at all times. The values in the schedule are in degrees C.
-
-#### Field: Low Temperature Design Setpoint
-
-Enter the low temperature setpoint temperature to be used for sizing the water loop and associated equipment in degrees C. If the Low Temperature Setpoint Schedule is blank, then this value will be used as the setpoint at all times.  The default is 20C.
-
-#### Field: Water Pump Configuration
-
-The choices for this field are
-
-- VariableFlow
-
-- ConstantFlow
-
-The default value is ConstantFlow. The variable flow option simulates a pump with variable flow to boilers, cooling towers, and water to air heat pump, excess bypassed. The constant flow option simulates constant flow to boilers, cooling towers, and water to air heat pumps, excess bypassed.
-
-The operation of a constant speed pump is fairly straightforward. If the user designates a constant speed pump that is operating continuously, the pump will run regardless of whether or not there is a load. This may have the net effect of adding heat to the loop if no equipment is turned on. If the pump is constant speed and operates intermittently, the pump will run at its capacity if a load is sensed and will shut off if there is no load on the loop.
-
-A variable speed pump is defined with maximum and minimum flow rates that are the physical limits of the device. If there is no load on the loop and the pump is operating intermittently, then the pump can shutdown. For any other condition such as the loop having a load and the pump is operating intermittently or the pump is continuously operating (regardless of the loading condition), the pump will operate and select a flow somewhere between the minimum and maximum limits. In these cases where the pump is running, it will try to meet the flow request made by demand side components.
-
-#### Field: Water Pump Rated Head
-
-The rated head of the hot water pump in Pa. The default value is 179352 Pa which is equivalent to 60 feet H2O.
-
-#### Field: Water Pump Type
-
-Describes the type of pump configuration used for mixed water loop. The options include:
-
-- SinglePump
-
-- PumpPerTowerOrBoiler
-
-- TwoHeaderedPumps
-
-- ThreeHeaderedPumps
-
-- FourHeaderedPumps
-
-- FiveHeaderedPumps
-
-#### Field: Supply Side Bypass Pipe
-
-The field determines if a supply side bypass pipe is present in the mixed water loop. The choices for this field are
-
-- Yes
-
-- No
-
-#### Field: Demand Side Bypass Pipe
-
-The field determines if a demand side bypass pipe is present in the mixed water loop. The choices for this field are
-
-- Yes
-
-- No
-
-#### Field: Fluid Type
-
-This field determines the type of fluid used for the mixed water loop.  The following options are available:
-
-- Water
-
-- EthyleneGlycol30
-
-- EthyleneGlycol40
-
-- EthyleneGlycol50
-
-- EthyleneGlycol60
-
-- PropyleneGlycol30
-
-- PropyleneGlycol40
-
-- PropyleneGlycol50
-
-- PropyleneGlycol60
-
-#### Field: Loop Design Delta Temperature
-
-The temperature difference used in sizing the loop flow rate. The default is 5.6C.
-
-#### Field: Load Distribution Scheme
-
-This alpha field contains the Load Distribution Scheme Keyword. The Load Distribution Scheme selects the algorithm used to sequence equipment operation in order to meet the plant loop demand. Currently, five schemes are functional. **Optimal** operates each piece of equipment at its optimal part load ratio and will operate the last component between its minimum and maximum part load ratio in order to meet the loop demand. **SequentialLoad** loads each piece of equipment sequentially in the order specified in the PlantEquipmentList to its maximum part load ratio and will operate the last required piece of equipment between its minimum and maximum part load ratio in order to meet the loop demand. **UniformLoad** evenly distributes the loop demand among all available components on the equipment list for a given load range. **SequentialUniformPLR** loads all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). Components are loaded sequentially based on the order specified in the PlantEquipmentList until each component is fully loaded, at which point the next subsequent component is added and the load is distributed uniformly based on PLR between the components. **UniformPLR** will load all equipment on the PlantEquipmentList to a uniform part load ratio (PLR). No equipment will be loaded below its minimum PLR. If the total load is less than the sum of all equipment on the PlantEquipmentList operating at their respective minimum PLRs, then the last item in the equipment list is dropped and the load is distributed based on a uniform PLR for the remaining plant equipment.
-
-Note: For all schemes, if the load for any individual component is less than the component load at the minimum PLR, the individual component model will false load or reduce duty cycle while operating at the minimum part load ratio until the load is met.
-
-As shown in an IDF:
-
-```idf
-HVACTemplate:Plant:MixedWaterLoop,
-    Only Water Loop,         !- Name
-    ,                        !- Pump Schedule Name
-    Intermittent,            !- Pump Control Type
-    Default,                 !- Operation Scheme Type
-    ,                        !- Equipment Operation Schemes Name
-    ,                        !- High Temperature Setpoint Schedule Name
-    34,                      !- High Temperature Design Setpoint {C}
-    ,                        !- Low Temperature Setpoint Schedule Name
-    20,                      !- Low Temperature Design Setpoint {C}
-    ConstantFlow,            !- Water Pump Configuration
-    179352,                  !- Water Pump Rated Head {Pa}
-    SinglePump,              !- Water Pump Type
-    Yes,                     !- Supply Side Bypass Pipe
-    Yes,                     !- Demand Side Bypass Pipe
-    Water,                   !- Fluid Type
-    6,                       !- Loop Design Delta Temperature {deltaC}
-    SequentialLoad;              !- Load Distribution Scheme
-```
-
-
-
-
diff --git a/doc/src/docs/InputOutputReference/03-Economics.md b/doc/src/docs/InputOutputReference/03-Economics.md
deleted file mode 100644
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--- a/doc/src/docs/InputOutputReference/03-Economics.md
+++ /dev/null
@@ -1,2560 +0,0 @@
-EnergyPlus Economics
-==============================================================================================================
-
-Group – Economics
------------------
-
-EnergyPlus contains a number of objects to model construction cost and utility bill calculations.
-
-The objects used by EnergyPlus for construction cost calculations are as follows:
-
-- ComponentCost:Adjustments
-
-- ComponentCost:Reference
-
-- ComponentCost:LineItem
-
-The objects used by EnergyPlus for utility bill calculations are as follows:
-
-- UtilityCost:Tariff
-
-- UtilityCost:Qualify
-
-- UtilityCost:Charge:Simple
-
-- UtilityCost:Charge:Block
-
-- UtilityCost:Ratchet
-
-- UtilityCost:Variable
-
-- UtilityCost:Computation
-
-The objects used for performing a life-cycle cost analysis are:
-
-- LifeCycleCost:Parameters
-
-- LifeCycleCost:RecurringCosts
-
-- LifeCycleCost:NonrecurringCost
-
-- LifeCycleCost:UsePriceEscalation
-
-- LifeCycleCost:UseAdjustment
-
-The object used for specifying the currency symbol of the monetary unit used is:
-
-- CurrencyType
-
-Introduction to Economics
--------------------------
-
-While it is true that monthly utility bills are often directly related to monthly energy consumption and monthly peak demand, due to the elaborate regulatory environment and the changing value of the energy based on load factor, the calculations involved are often complicated. The EnergyPlus approach is to allow you to model the individual component charges that make up the utility bill and report the results on a monthly basis.
-
-To show you how simple the specification of a rate can be here is a simple example for a flat charge of 8 cents for every kWh sold.
-
-```idf
-UtilityCost:Tariff,
-  TariffExample1,          ! Name
-  Electricity:Facility,    ! Output Meter Name
-  kWh;               ! Conversion Factor Choice
-
-
-UtilityCost:Charge:Simple,
-  ChargeExample1,          ! Charge Variable Name
-  TariffExample1,          ! Tariff Name
-  totalEnergy,             ! Source Variable
-  Annual,                   ! Season
-  EnergyCharges,           ! Category Variable Name
-  0.08;                    ! Cost Per Unit Value or Variable Name
-```
-
-
-
-Overall, the goals of the economics section of EnergyPlus are to make simple tariffs easy to model and complex tariffs possible to model.
-
-The cost implications of alternative, energy-related design options may be important in determining the whether or not a particular design is viable. Although the main purpose of EnergyPlus is to determine the energy performance of a building, component cost modeling is provided to allow estimating initial construction costs associated with the building and HVAC system being modeled. This is provided in order to ensure that cost estimates are consistent with the EnergyPlus model and it allows using results calculated during a simulation such as equipment sizes and surface areas. The cost estimating capabilities are not comprehensive and are not intended to duplicate all the types of analyses included in cost estimating software. Economics modeling is being implemented in stages. Future versions of EnergyPlus will add other investment related analyses such as life-cycle cost. The objects used by EnergyPlus for calculating first costs for construction projects are as follows:
-
-- ComponentCost:Adjustments
-
-- ComponentCost:Reference
-
-- ComponentCost:LineItem
-
-The results of the cost estimate are reported in a Construction Cost Estimate Summary table provided that the user requests the results using the object Output:Table:SummaryReports object with the Component Cost Economics Summary option selected. The style of this predefined report can be controlled using the OutputControl:Table:Style object. If the Annual Building Performance Report Summary is also requested, then cost estimate results will follow that data in the same output file.
-
-The rest of this Economics section is organized to first present reference material on tariff calculations followed by construction cost estimating.
-
-Conceptual Framework – Variables and Hierarchy
-----------------------------------------------
-
-To understand how to use the utility bill calculation portion of EnergyPlus you first need to understand some important concepts of variables and hierarchy. A variable, for the purposes of this section, is simply a named holder of a series of numbers. In most cases, the variable will be a named holder of 12 numbers, one number for each monthly utility bill. Here is a visualization of a variable called Electric Energy Use:
-
-Table 35. Example Electric Energy Use (for Economics Calculation)
-
-<table class="table table-striped">
-<tr>
-<th>Month</th>
-<th>Electric Energy Use</th>
-</tr>
-<tr>
-<td>January</td>
-<td>12143</td>
-</tr>
-<tr>
-<td>February</td>
-<td>13454</td>
-</tr>
-<tr>
-<td>March</td>
-<td>14178</td>
-</tr>
-<tr>
-<td>April</td>
-<td>14876</td>
-</tr>
-<tr>
-<td>May</td>
-<td>15343</td>
-</tr>
-<tr>
-<td>June</td>
-<td>16172</td>
-</tr>
-<tr>
-<td>July</td>
-<td>16105</td>
-</tr>
-<tr>
-<td>August</td>
-<td>15762</td>
-</tr>
-<tr>
-<td>September</td>
-<td>14543</td>
-</tr>
-<tr>
-<td>October</td>
-<td>13987</td>
-</tr>
-<tr>
-<td>November</td>
-<td>13287</td>
-</tr>
-<tr>
-<td>December</td>
-<td>12403</td>
-</tr>
-</table>
-
-If you have ever done any computer programming, you can think of a variable as an array. Many of the names used in the utility bill calculation portion of EnergyPlus are names of variables. In the case of the UtilityCost:Charge objects, the name of the object is also used as a name of a variable.
-
-In many of today’s utility rates, the charges for energy or demand are broken into distribution and supply charges. To allow for this, more than one charge may to be defined for a particular category. The variables assigned to the same category are added together.
-
-The categories are combined in following hierarchy:
-
-![EnergyCharge](media/image615.png)
-
-Figure 162. Hierarchy for Economics Charges
-
-Any charges included in the EnergyCharges category are added together. The EnergyCharges, DemandCharges and ServiceCharges are added together to form the Basis. The Basis, Adjustments and Surcharges are added together to form the Subtotal. The Subtotal and Taxes are added together to be the Total. The total represents the total monthly charges on that tariff for the energy source used. The combining of categories together is performed automatically unless the user specifies the UtilityCost:Computation. In addition, each category, which is also a variable, may be used as a source. For example, a tax that is 5% of the subtotal would be shown as:
-
-```idf
-UtilityCost:Charge:Simple,
-  TaxOfFivePercent,        ! Charge Variable Name
-  TariffExample1,          ! Tariff Name
-  Subtotal,                ! Source Variable
-  Annual,                  ! Season
-  Taxes,                   ! Category Variable Name
-  0.05;                    ! Cost Per Unit Value or Variable Name
-```
-
-
-As you can see, the UtilityCost:Charge:Simple and UtilityCost:Charge:Block objects do most of the “work� of computing the annual energy cost. The benefit of using this categorization is that totals of each category are shown in the output reports and it organizes the charges in the monthly calculations in a logical way that fits almost all tariffs. If no categorization is desired, theoretically, all charges could be assigned to the Total category. The categories themselves are simply variable names. Charges may also be assigned to the “NotIncluded� category if the result of the charge is used as an intermediate calculation and should not be included in the Total.
-
-The rest of this section is divided into a reference of the objects and the fields, a set of examples, discussion of the reporting, and a description of Complex Tariff Modeling. For most tariffs, simply using a variety of UtilityCost:Charge:Simple’s and UtilityCost:Charge:Block’s will result in a good model but for some more complex tariffs, especially ones with complex block sizes, variables may be computed using a very simple programming language that may appear in the UtilityCost:Computation object. This will be described more in the Complex Tariff Modeling section.
-
-UtilityCost:Tariff
-------------------
-
-Defines the name of the tariff, the type of tariff, and other details about the overall tariff. Each other object that is part of the tariff model references the tariff name including the UtilityCost:Charge:Simple, UtilityCost:Charge:Block, UtilityCost:Ratchet, UtilityCost:Qualify, UtilityCost:Variable and UtilityCost:Computation objects.
-
-Multiple UtilityCost:Tariff objects can appear in the same IDF file. It is common that electric and gas utilities have more than one rate that may be used. Only one UtilityCost:Tariff for each Output:Meter object and Group Name is shown in the Economics Summary Report. The one that is shown in that report is chosen by first eliminating UtilityCost:Tariff objects that are not qualified due to their UtilityCost:Qualify objects. If more than one UtilityCost:Tariff object remains, the one that has the lowest cost for a combination of a Meter and Group Name will be selected. If the Group Name field is not used, then the lowest cost UtilityCost:Tariff is chosen for each Meter.
-
-Part of the tariff description is used to transform the annual energy use of any fuel under any meter into a group of named variables containing the values for each of the periods that the bills are calculated (usually monthly). The schedules create a variable for energy use and for demand. If specified it also creates a variable for energy and a variable for demand for the “on-peak�, “off-peak�, and “shoulder� periods for use in time-of-use tariffs. It performs this allocation prior to other calculations for the tariff. The variables that are always created are:
-
-- totalEnergy
-
-- totalDemand
-
-#### Field: Name
-
-The name of the tariff. Tariffs are sometimes called rates. The name is used in identifying the output results and in associating all of the charges and other objects that make up a tariff.
-
-#### Field: Output Meter Name
-
-The name of any meter defined but usually set to either Electricity:Facility or Gas:Facility.
-
-#### Field: Conversion Factor Choice
-
-A choice that allows several different predefined conversion factors to be used; otherwise, user defined conversion factors are used as defined in the next two fields.
-
-- UserDefined
-
-- kWh
-
-- Therm
-
-- MMBtu
-
-- MJ
-
-- KBtu
-
-- MCF
-
-- CCF
-
-The following table shows the conversion factors when specifying one of the predefined choices:
-
-Table 36. Built in UtilityCost:Tariff Conversion Factors
-
-<table class="table table-striped">
-<tr>
-<th>Choice</th>
-<th>Energy Conversion Factor</th>
-<th>Demand Conversion Factor</th>
-</tr>
-<tr>
-<td>kWh</td>
-<td>0.0000002778</td>
-<td>0.001</td>
-</tr>
-<tr>
-<td>Therm</td>
-<td>9.4781712E-09</td>
-<td>0.00003412</td>
-</tr>
-<tr>
-<td>MMBtu</td>
-<td>9.4781712E-10</td>
-<td>0.000003412</td>
-</tr>
-<tr>
-<td>MJ</td>
-<td>0.000001</td>
-<td>0.0036</td>
-</tr>
-<tr>
-<td>KBtu</td>
-<td>9.4781712E-07</td>
-<td>0.003412</td>
-</tr>
-<tr>
-<td>MCF</td>
-<td>9.4781712E-10</td>
-<td>0.000003412</td>
-</tr>
-<tr>
-<td>CCF</td>
-<td>9.4781712E-09</td>
-<td>0.00003412</td>
-</tr>
-</table>
-
-#### Field: Energy Conversion Factor
-
-Is a multiplier used to convert energy into the units specified by the utility in their tariff. If left blank, it defaults to 1 (no conversion). This field will be used only if Conversion Factor Choice is set to UserDefined. Within EnergyPlus energy always has units of J (joules). For conversion from J to kWh use the value of 0.0000002778. This is also used for all objects that reference the UtilityCost:Tariff.
-
-#### Field: Demand Conversion Factor
-
-Is a multiplier used to convert demand into the units specified by the utility in their tariff. If left blank, it defaults to 1 (no conversion). This field will be used only if Conversion Factor Choice is set to UserDefined. Within EnergyPlus demand always has units of J/s (joules/sec) which equivalent to W (watts). For conversion from W to kW use the value of 0.001. This is also used for all objects that reference the UtilityCost:Tariff.
-
-#### Field: Time of Use Period Schedule Name
-
-The name of the schedule that defines the time-of-use periods that occur each day. The period schedule is used to determine which variables are defined. The values for the different variables are:
-
-- 1 is Peak
-
-- 2 is Shoulder
-
-- 3 is OffPeak
-
-- 4 is MidPeak
-
-The following variables are created automatically if these different periods are used in the schedule and include:
-
-- peakEnergy
-
-- peakDemand
-
-- shoulderEnergy
-
-- shoulderDemand
-
-- offPeakEnergy
-
-- offPeakDemand
-
-- midPeakEnergy
-
-- midPeakDemand
-
-Some special variables are created that include only demand from one period that exceeds the demand from another period. For other months that do not exceed, the values are zero. These variables are seldom used but are available for the occasional rate that includes a clause looking at demands during one period that exceed another period.
-
-- PeakExceedsOffPeak
-
-- OffPeakExceedsPeak
-
-- PeakExceedsMidPeak
-
-- MidPeakExceedsPeak
-
-- PeakExceedsShoulder
-
-- ShoulderExceedsPeak
-
-If no Period Schedule is specified then no peak, offPeak, midPeak or shoulder variables are defined.
-
-#### Field: Season Schedule Name
-
-The name of a schedule that defines the seasons. The seasons are
-
-- 1 is Winter
-
-- 2 is Spring
-
-- 3 is Summer
-
-- 4 is Autumn
-
-The change in the season schedule must occur at the same time as the change in the Monthly Schedule. In other words, a season must end at the same time as a billing month. Variables are automatically created if a season schedule is used. These variables are set to 1 within the season and 0 for the months that are not in the season. The variables are:
-
-- isWinter
-
-- isNotWinter
-
-- isSpring
-
-- isNotSpring
-
-- isSummer
-
-- isNotSummer
-
-- isAutumn
-
-- isNotAutumn
-
-#### Field: Month Schedule Name
-
-The name of the schedule that defines the billing periods of the year. Normally this entry is allowed to default and a schedule will be internally used that has the breaks between billing periods occurring at the same time as the breaks between months, i.e., at midnight prior to the first day of the month. If other billing periods are used such as two month cycles or a single bill for an entire season, such as some natural gas companies do in the summer, then the month schedule may be used to redefine it. Make sure that the month schedule and season schedule are consistent, otherwise an error will be issued.
-
-- 1 is the first month, usually January
-
-- 2 is the second month, usually February
-
-- 3 is the third month, usually March
-
-- 4 is the fourth month, usually April
-
-- 5 is the fifth month, usually May
-
-- 6 is the sixth month, usually June
-
-- 7 is the seventh month, usually July
-
-- 8 is the eighth month, usually August
-
-- 9 is the ninth month, usually September
-
-- 10 is the tenth month, usually October
-
-- 11 is the eleventh month, usually November
-
-- 12 is the twelfth month, usually December
-
-Thus, the schedule that represents this would look like the following. If no schedule is specified the following Month Schedule is used which defines the months of the year as the normal calendar months.
-
-```idf
-Schedule:Compact, defaultMonths, number,
-Through: 1/31, For: AllDays, Until: 24:00, 1,
-Through: 2/28, For: AllDays, Until: 24:00, 2,
-Through: 3/31, For: AllDays, Until: 24:00, 3,
-Through: 4/30, For: AllDays, Until: 24:00, 4,
-Through: 5/31, For: AllDays, Until: 24:00, 5,
-Through: 6/30, For: AllDays, Until: 24:00, 6,
-Through: 7/31, For: AllDays, Until: 24:00, 7,
-Through: 8/31, For: AllDays, Until: 24:00, 8,
-Through: 9/30, For: AllDays, Until: 24:00, 9,
-Through: 10/31, For: AllDays, Until: 24:00, 10,
-Through: 11/30, For: AllDays, Until: 24:00, 11,
-Through: 12/31, For: AllDays, Until: 24:00, 12;
-```
-
-
-#### Field: Demand Window Length
-
-The determination of demand can vary by utility. Some utilities use the peak instantaneous demand measured but most use a fifteen minute average demand or a one hour average demand. Some gas utilities measure demand as the use during the peak day or peak week. The choices for demand window are:
-
-- QuarterHour
-
-- HalfHour
-
-- FullHour
-
-- Day
-
-- Week
-
-If no value is entered, QuarterHour is assumed. The choice may be overridden based on the value of Timestep so that they are consistent. If the Timestep is 6, i.e. 10 minute timesteps, then QuarterHour is not used and instead HalfHour is used instead. If Timestep is 3, i.e. 20 minute timesteps, then QuarterHour and HalfHour are not used and instead FullHour is used instead. Day and Week are primarily used by fuel utilities.
-
-#### Field: Monthly Charge or Variable Name
-
-The fixed monthly service charge that many utilities have. The entry may be numeric and gets added to the ServiceCharges variable or if a variable name is entered here, its values for each month are used.
-
-#### Field: Minimum Monthly Charge or Variable Name
-
-The minimum total charge for the tariff or if a variable name is entered here, its values for each month are used.  The sum of the subtotal and taxes usually equals the total unless you have specified the minimum monthly charge. If the minimum monthly charge does not apply to the entire bill, a UtilityCost:Computation object can be specified using a Minimum function for the appropriate variables.
-
-#### Field: Real Time Pricing Charge Schedule Name
-
-Used with real time pricing rates. The name of a schedule that contains the cost of energy for that particular time period of the year. Real time rates can be modeled using a charge schedule with the actual real time prices entered in the schedule. The charges should be consistent with the conversion factor specified in the tariff.
-
-#### Field: Customer Baseline Load Schedule Name
-
-Used with real time pricing rates and often described as the CBL or customer baseline load. The name of a schedule that contains the baseline energy use for the customer. Many real time rates apply the charges as a credit or debit only to the difference between the baseline use and the actual use. The baseline use is established between the customer and the utility using a contract. If this field is used the baseline use schedule will be used for establishing the totalEnergy and totalDemand instead of the metered value and the real time rate charge is added or subtracted to the rate calculation using the real time charge schedule. If this field is not used, the real time charge schedule applies to all energy from the meter and totalEnergy and totalDemand is based on metered value as usual.
-
-#### Field: Group Name
-
-The group name of the tariff such as distribution, transmission, supplier, etc. If more than one tariff with the same group name is present and qualifies, only the lowest cost tariff is used. Usually the group name field is left blank which results in all tariffs using the same meter variable being compared and the lowest cost one being selected.
-
-#### Field: Buy Or Sell
-
-Sets whether the tariff is used for buying, selling or both to the utility. This should be allowed to default to BuyFromUtility unless a power generation system is included in the building that may generate more power than the building needs during the year. The choices are:
-
-- BuyFromUtility – The values from the metered variable are used and are shown as being purchases from the utility.
-
-- SellToUtility – The values from the metered variable are used for a “sell back� rate to the utility. The charges in the rate should be expressed as negative values.
-
-- NetMetering – Negative values are used to reduce any positive values during the specific period on the tariff when negative values occur.
-
-A warning will be issued if the selection of this field does not match the type of meter.
-
-UtilityCost:Qualify
--------------------
-
-Many utilities provide a large number of tariffs and separate their customers by the amount of energy use they have or by the amount of demand. The qualify object allows only certain tariffs that are modeled to be used. If the results of the simulation fall outside of the range of qualifications, that tariff is still calculated but the “Qualified� entry will say “No� and the UtilityCost:Qualify that caused its exclusion is shown. When multiple tariffs from the same utility are modeled and only one of them should be used, make sure that the qualifiers are consistent especially within the same GroupName (see UtilityCost:Tariff). Multiple UtilityCost:Qualify objects can appear for a specific rate and they can be based on any variable.
-
-The energy used and demands for each month vary. Since it is possible that they vary across the minimum and maximum values defined by this object, a choice in how to treat the thresholds is necessary. Say that a utility has two tariffs, a small tariff that has a maximum demand requirement of 50kW and a large tariff that has a minimum demand requirement of 50kW. If the use for a building goes above the 50kW threshold during some summer months and the rest of the time is below 50kW, then how does the utility choose which rate would qualify. The utility probably has very specific requirements about which months or consecutive months can be above or below a threshold to qualify for the rate.
-
-#### Field: Name
-
-The name used for the UtilityCost:Qualify and displayed if the tariff does not qualify. It is also treated as a variable and contains:
-
-- 1 for each month that does qualify,
-
-- 0 for months that do not qualify, and
-
-- -1 for months that are not part of the season selected.
-
-#### Field: Tariff Name
-
-The name of the UtilityCost:Tariff object that is associated with this UtilityCost:Qualify object.
-
-#### Field: Variable Name
-
-The name of the variable used. For energy and demand, the automatically created variables, totalEnergy and totalDemand should be used, respectively.
-
-#### Field: Qualify Type
-
-Enter either “Minimum� or “Maximum�.
-
-#### Field: Threshold Value or Variable Name
-
-The minimum or maximum value for the qualify. If the variable has values that are less than this value when the qualify type is minimum then the tariff may be disqualified. If the variable has values that are greater than this value when the qualify type is maximum then the tariff may be disqualified. For demand, it is still the minimum of the demands set each month even though the demands are, by definition, the peak value for the month. Depending on the threshold test entry (see below) this minimum applies to all months, some of the months, or just a single month.
-
-#### Field: Season
-
-If the UtilityCost:Qualify only applies to a season, enter the season name from the following list:
-
-- Annual
-
-- Winter
-
-- Spring
-
-- Summer
-
-- Fall
-
-If this field is left blank, it defaults to Annual.
-
-#### Field: Threshold Test
-
-Enter either “Count� or “Consecutive�. Uses the number in Number of Months in one of two different ways depending on the Threshold Test. If the Threshold Test is set to “Count� then the qualification is based on the count of the total number of months per year. If the Threshold Test is set to “Consecutive� then the qualification is based on a consecutive number of months. If left blank this field defaults to count and it should be allowed to default for most cases.
-
-#### Field: Number of Months
-
-A number from 1 to 12. If no value entered, 12 is assumed when the qualify type is minimum and 1 when the qualify type is maximum. This is the number of months that the threshold test applies to determine if the rate qualifies or not. If the season is less than 12 months (if it is not annual) then the value is automatically reduced to the number of months of the season.
-
-UtilityCost:Charge:Simple
--------------------------
-
-The UtilityCost:Charge:Simple is one of the most often used objects for tariff calculation. It is used to compute energy and demand charges that are very simple. It may also be used for taxes, surcharges and any other charges that occur on a utility bill. As many UtilityCost:Charge:Simple objects as needed may be defined for a single tariff and they will be added together.
-
-#### Field: Charge Variable Name
-
-This is the name associated with the UtilityCost:Charge:Simple object and will appear in the report. In addition, the results of the UtilityCost:Charge:Simple calculation are stored in a variable with the same name. That way, the results may be used for further calculation. Spaces are not significant in Charge Variable Names. They are removed during the utility bill calculation process.
-
-#### Field: Tariff Name
-
-The name of the tariff that this UtilityCost:Charge:Simple is associated with.
-
-#### Field: Source Variable
-
-The name of the source used by the UtilityCost:Charge:Simple. This is usually the name of the variable holding the energy or demand but may also be the name of any variable including the subtotal or basis if other charges are based on those.
-
-#### Field: Season
-
-This is the name (or number) of a season for which the UtilityCost:Charge:Simple is calculated. If this is set to Annual, the calculations are performed for the UtilityCost:Charge:Simple for the entire year (all months) otherwise it is calculated only for those months in the season defined. The season is defined by the Season Schedule in the UtilityCost:Tariff object. The choices for seasons are the following names or numbers may be used:
-
-- Annual
-
-- Winter
-
-- Spring
-
-- Summer
-
-- Fall
-
-#### Field: Category Variable Name
-
-All charges get added somewhere in the hierarchy described in the introduction to EnergyPlus economics above. This field shows where the charge should be added. The reason to enter this field appropriately is so that the charge gets reported in a reasonable category. The charge automatically gets added to the variable that is the category. The choices for this field are limited to:
-
-- EnergyCharges
-
-- DemandCharges
-
-- ServiceCharges
-
-- Basis
-
-- Adjustment
-
-- Surcharge
-
-- Subtotal
-
-- Taxes
-
-- Total
-
-- NotIncluded
-
-#### Field: Cost per Unit Value or Variable Name
-
-This field contains either a single number or the name of a variable. The number is multiplied with all of the energy or demand or other source that is specified in the source field. If a variable is used, then the monthly values of the variable are multiplied against the variable specified in the source field. This field makes it easy to include a simple charge without specifying block sizes. It is added to any of the block calculations (see later fields) but is most often used by itself. If no value or variable is entered, a zero is assumed. This is a good way to include a tax or cost adjustment. For SellToUtility tariffs, the values in this field are usually expressed as negative numbers.
-
-UtilityCost:Charge:Block
-------------------------
-
-The UtilityCost:Charge:Block objects is also used extensively for tariff calculation. It is used to compute energy and demand charges that are structured in blocks of charges. It may also be used for taxes, surcharges and any other charges that occur on a utility bill but those are more commonly simple flat charges so UtilityCost:Charge:Simple  is more commonly used for those functions. As many UtilityCost:Charge:Block objects as needed may be defined for a single tariff and they will be added together. Blocks are a structure used by almost all utilities for calculating energy and demand charges and they allow the utility to charge more or less per unit of energy or demand if more units are used.
-
-#### Field: Charge Variable Name
-
-This is the name associated with the UtilityCost:Charge:Block object and will appear in the report. In addition, the results of the UtilityCost:Charge:Block are stored in a variable with the same name. That way, the results may be used for further calculation.
-
-#### Field: Tariff Name
-
-The name of the tariff that this UtilityCost:Charge:Block is associated with.
-
-#### Field: Source Variable
-
-The name of the source used by the UtilityCost:Charge:Block. This is usually the name of the variable holding the energy or demand but may also be the name of any variable including the subtotal or basis if other charges are based on those.
-
-#### Field: Season
-
-This is the name (or number) of a season for which the  UtilityCost:Charge:Block is calculated. If this is set to annual, the calculations are performed for the UtilityCost:Charge:Block for the entire year (all months) otherwise it is calculated only for those months in the season defined. The season is defined by the Season Schedule in the UtilityCost:Tariff object. The choices for seasons are the following names or numbers may be used:
-
-- Annual
-
-- Summer
-
-- Winter
-
-- Spring
-
-- Fall
-
-#### Field: Category Variable Name
-
-All charges get added somewhere in the hierarchy described in the introduction to EnergyPlus economics above. This field shows where the charge should be added. The reason to enter this field appropriately is so that the charge gets reported in a reasonable category. The charge automatically gets added to the variable that is the category. The choices for this field are limited to:
-
-- EnergyCharges
-
-- DemandCharges
-
-- ServiceCharges
-
-- Basis
-
-- Adjustment
-
-- Surcharge
-
-- Subtotal
-
-- Taxes
-
-- Total
-
-- NotIncluded
-
-#### Field: Remaining Into Variable
-
-If the blocks do not use all of the energy or demand from the source, some energy and demand remains, then the remaining amount should be assigned to a variable. If no variable is assigned and some amount of energy or demand is not used in the block structure a warning will be issued.
-
-#### Field: Block Size Multiplier Value or Variable Name
-
-The sizes of the blocks are usually used directly but if a value or a variable is entered here, the block sizes entered in the rest of the charge are first multiplied by the entered value prior to being used. This is common for rates that are kWh/kW rates and in that case the variable that holds the monthly total electric demand would be entered. If no value is entered, a default value of one is assumed so that the block sizes remain exactly as entered. This field is unusual for the EnergyPlus syntax because it can be either a number or a name of a variable.
-
-#### Field: Block Size 1 Value or Variable Name
-
-The size of the first block of the charges is entered here. For most rates that use multiple blocks, this will be the value for the first block size. Additional block sizes are entered with every other field. A default variable named “remaining� contains a large value and this may be used when the remaining amount should be included in that block. This field and the next field may be repeated in groups of two for as many blocks as are defined. This field is unusual for the EnergyPlus syntax because it can be either a number or a name of a variable.
-
-#### Field: Block 1 Cost per Unit Value or Variable Name
-
-The cost of the first block. This value is also repeated for every other field in the charge. As many blocks may be entered as are needed. This field and the previous field may be repeated in groups of two for as many blocks as are defined. This field is unusual for the EnergyPlus syntax because it can be either a number or a name of a variable. For SellToUtility tariffs, the values in this field are usually expressed as negative numbers.
-
-These last two fields may be repeated fifteen times. If more blocks are defined by the utility, the computation can be continued using another UtilityCost:Charge:Block and using the variable from Remaining Into Variable as the source variable.
-
-UtilityCost:Ratchet
--------------------
-
-The UtilityCost:Ratchet command allows the modeling of tariffs that include some type of seasonal ratcheting. Ratchets are most common when used with electric demand charges. A ratchet is when a utility requires that the demand charge for a month with a low demand may be increased to be more consistent with a month that set a higher demand charge.
-
-While the details of the UtilityCost:Ratchet command are described further in this section, an example is probably the easiest way to learn the basic functions.
-
-Ratchet Example: A utility has a single ratchet that says that the billing demand for each month of the year is the higher value of the actual demand or 60% of the peak summer demand
-
-```idf
-UtilityCost:Ratchet,
-  BillingDemand1,   ! Ratchet Variable Name
-  ExampleTariff1,   ! Tariff Name
-  TotalDemand,      ! Baseline Source Variable
-  TotalDemand,      ! Adjustment Source Variable
-  Summer,           ! Season From
-  Annual,           ! Season To
-  0.60,             ! Multiplier Value or Variable Name
-  0;                ! Offset Value or Variable Name
-```
-
-
-
-The Ratchet Variable Name (the first field) should be used wherever the ratchet should be applied and is often the source variable for UtilityCost:Charge:Simple or UtilityCost:Charge:Block.
-
-The detailed steps taken for the ratchet are the following:
-
-- AdjSeasonal contains either:
-
-- When SeasonFrom is not set to Monthly, the maximum for all months in Season From in the Adjustment Source Variable. This is a single value.
-
-- When SeasonFrom is set to Monthly, the monthly values of the Adjustment Source Variable.
-
-- AdjPeak = (AdjSeasonal + Offset) \* Multiplier
-
-- MaxAdjBase = maximum value of either AdjPeak or Baseline Source Variable
-
-- The resulting Ratchet Variable contains:
-
-- For months not in SeasonTo, the values of Baseline Source Variable
-
-- For months in SeasonTo, the values of MaxAdjBase
-
-If multiple ratchets occur in the same tariff, multiple UtilityCost:Ratchet commands should be “chained� together with the Baseline Source Variable subsequent ratchets referencing the Ratchet Variable Name of the previous UtilityCost:Ratchet.
-
-Since the ratchet command can add together two variables, mutliply two variables, or take the maximum value between two variables, it may be used for other difficult to model tariffs without needing to use UtilityCost:Computation. Clever use of UtilityCost:Ratchet should be well documented with comments.
-
-#### Field: Ratchet Variable Name
-
-The name of the ratchet and the name of the result of this single ratchet.
-
-#### Field: Tariff Name
-
-The name of the tariff that this UtilityCost:Ratchet is associated with.
-
-#### Field: Baseline Source Variable
-
-The name of the variable used as the baseline value. When the ratcheted value exceeds the baseline value for a month the ratcheted value is used but when the baseline value is greater then the ratcheted value the baseline value is used. Usually the electric demand charge is used. The baseline source variable can be the results of another ratchet object. This allows utility tariffs that have multiple ratchets to be modeled.
-
-#### Field: Adjustment Source Variable
-
-The variable that the ratchet is calculated from. It is often but not always the same as the baseline source variable. The ratcheting calculations using offset and multiplier are using the values from the adjustment source variable. If left blank, the adjustment source variable is the same as the baseline source variable.
-
-#### Field: Season From
-
-The name of the season that is being examined. The maximum value for all of the months in the named season is what is used with the multiplier and offset. This is most commonly Summer or Annual. When Monthly is used, the adjustment source variable is used directly for all months.
-
-- Annual
-
-- Winter
-
-- Spring
-
-- Summer
-
-- Fall
-
-- Monthly
-
-#### Field: Season To
-
-The name of the season when the ratchet would be calculated. This is most commonly Winter. The ratchet only is applied to the months in the named season. The resulting variable for months not in the Season To selection will contain the values as appear in the baseline source variable.
-
-- Annual
-
-- Winter
-
-- Spring
-
-- Summer
-
-- Fall
-
-#### Field: Multiplier Value or Variable Name
-
-Often the ratchet has a clause such as “the current month demand or 90% of the summer month demand�. For this case a value of 0.9 would be entered here as the multiplier. This value may be left blank if no multiplier is needed and a value of one will be used as a default.
-
-#### Field: Offset Value or Variable Name
-
-A less common strategy is to say that the ratchet must be all demand greater than a value, in this case an offset that is added to the demand may be entered here. If entered, it is common for the offset value to be negative representing that the demand be reduced.  If no value is entered it is assumed to be zero and not affect the ratchet.
-
-UtilityCost:Variable
---------------------
-
-The UtilityCost:Variable object allows for the direct entry of monthly values into a variable.
-
-#### Field: Name
-
-The name of the variable.
-
-#### Field: Tariff Name
-
-The name of the tariff that is using the variable.
-
-#### Field: Variable Type
-
-This field is used to indicate the kind of units that may be associated with the variable. It is used by IDF Editor to display the appropriate SI and IP units for the January through December values. The available options are shown below. If none of these options are appropriate, select **Dimensionless** which will have no unit conversion**.**
-
-- Energy
-
-- Demand
-
-- Currency
-
-- Dimensionless
-
-#### Field: January through December Values
-
-An entry (up to 24 are available) of the monthly values of the variable. Normally 12 months are used for most utility rates and so 12 values should be entered. If any values are not entered, the value of the previous entry is used. This allows a variable that is constant for an entire year to be entered using only the first value.
-
-
-
-UtilityCost:Computation
------------------------
-
-The UtilityCost:Computation object lists a series of computations that are used to perform the bill calculation. The object is only used for complex tariffs that cannot be modeled any other way. For 95% of the utility tariffs, using UtilityCost:Computation is unnecessary and should be avoided. If the UtilityCost:Computation object is used, it must contain references to all objects involved in the rate in the order that they should be computed.
-
-#### Field: Name
-
-The name of the UtilityCost:Computation.
-
-#### Field: Tariff Name
-
-The name of the tariff that this UtilityCost:Charge:Simple is associated with.
-
-#### Field: Compute Step N
-
-The Compute Step fields contain a simple language that describes the steps used in the computation process similar to a programming language. If no entry is made to any Compute Step fields (as usually the case) a default method of computing the rates shall be used. Compute Step is described later in this section under Complex Tariff Modeling.
-
-Remember, this object should be omitted for almost all tariffs.
-
-UtilityCost:Tariff Examples
----------------------------
-
-One of the best ways to learn the details of EnergyPlus Economics is to see some example tariffs and how they translate into objects. To do this, several different rates of increasing complexity are shown in the following examples.
-
-Another source of examples is the large set of tariff input objects provided with EnergyPlus in the macro data set file called “UtilityTariffObjects.imf� located in the “MacroDataSets� folder where EnergyPlus is installed. This file contains sets of objects that fully define tariffs for commercial customers from a collection of U.S. utility companies.
-
-
-
-#### Example A – Flat Energy Charge
-
-As an example of the simplest type of tariff.
-
-Customer Charge: $2.51 per month
-
-Energy Charge:    5.5342 cents/kWh
-
-This tariff would use a single UtilityCost:Charge:Simple object. The monthly charge is part of the UtilityCost:Tariff object.
-
-```idf
-UtilityCost:Tariff,
-  ExampleA,                     ! Name
-  Electricity:Facility,         ! Output Meter Name
-  kWh,                          ! Conversion Factor Choice
-  ,                             ! Energy Conversion Factor
-  ,                             ! Demand Conversion Factor
-  ,                             ! Time of Use Period Schedule Name
-  ,                             ! Season Schedule Name
-  ,                             ! Month Schedule Name
-  ,                             ! Demand Window Length
-  2.51;                         ! Monthly Charge or Variable Name
-
-
-UtilityCost:Charge:Simple,
-  FlatEnergyCharge,             ! Charge Variable Name
-  ExampleA,                     ! Tariff Name
-  totalEnergy,                  ! Source Variable
-  Annual,                       ! Season
-  EnergyCharges,                ! Category Variable Name
-  0.055342;                     ! Cost Per Unit Value or Variable Name
-```
-
-
-
-#### Example B – Block Energy Charge
-
-Another simple type of tariff is one where the energy charges vary by the amount of energy consumed each month.
-
-Customer Charge:    $5.75 per month
-
-Energy Charge:        7.231 cents/kWh for first 200 kWh
-
-                                  6.656 cents/kWh for next 1000 kWh
-
-                                  5.876 cents/kWh for over 1200 kWh
-
-This tariff would use a single UtilityCost:Charge:Block object. The monthly charge is part of the UtilityCost:Tariff object. Note that the block sizes are every other field at the bottom of the object and the that final block size references a built in variable called “remaining� that contains a very large number.
-
-```idf
-UtilityCost:Tariff,
-  ExampleB,                     ! Name
-  Electricity:Facility,         ! Output Meter Name
-  kWh,                          ! Conversion Factor Choice
-  ,                             ! Energy Conversion Factor
-  ,                             ! Demand Conversion Factor
-  ,                             ! Time of Use Period Schedule Name
-  ,                             ! Season Schedule Name
-  ,                             ! Month Schedule Name
-  ,                             ! Demand Window Length
-  5.75;                         ! Monthly Charge or Variable Name
-
-
-UtilityCost:Charge:Block,
-  BlockEnergyCharge,            ! Charge Variable Name
-  ExampleB,                     ! Tariff Name
-  totalEnergy,                  ! Source Variable
-  Annual,                       ! Season
-  EnergyCharges,                ! Category Variable Name
-  ,                             ! Remaining Into Variable
-  ,                             ! Block Size Multiplier Value or Variable Name
-  200,                          ! Block Size 1 Value or Variable Name
-  0.07231,                      ! Block 1 Cost per Unit Value or Variable Name
-  1000,                         ! Block Size 2 Value or Variable Name
-  0.06656,                      ! Block 2 Cost per Unit Value or Variable Name
-  remaining,                    ! Block Size 3 Value or Variable Name
-  0.05876;                      ! Block 3 Cost per Unit Value or Variable Name
-```
-
-
-
-#### Example C – Block Energy and Demand Charges
-
-This example contains both a block for energy and a block for demand and is very similar to the previous example except it now includes demand charges as well. The energy and demand charges vary by the amount of energy and demand consumed each month.
-
-Energy Charge:        4.74 cents/kWh for first 20,000 kWh
-
-                                  4.24 cents/kWh for next 180,000 kWh
-
-                                  3.83 cents/kWh for additional kWh
-
-Demand Charge:      5.38 dollars per kW for first 20 kW
-
-                                  4.23 dollars per kW for next 80 kW
-
-                                  3.60 dollars per kW for additional kW
-
-This tariff would use two UtilityCost:Charge:Block objects. No monthly charge is shown so the UtilityCost:Tariff object can include just the first four fields. Note that the block sizes are every other field at the bottom of the object and the that final block size references a built in variable called “remaining� that contains a very large number.
-
-```idf
-UtilityCost:Tariff,
-  ExampleC,                     ! Name
-  Electricity:Facility,         ! Output Meter Name
-  KWh;                          ! Conversion Factor Choice
-
-
-UtilityCost:Charge:Block,
-  BlockEnergyCharge,            ! Charge Variable Name
-  ExampleC,                     ! Tariff Name
-  totalEnergy,                  ! Source Variable
-  Annual,                       ! Season
-  EnergyCharges,                ! Category Variable Name
-  ,                             ! Remaining Into Variable
-  ,                             ! Block Size Multiplier Value or Variable Name
-  20000,                        ! Block Size 1 Value or Variable Name
-  0.0474,                       ! Block 1 Cost per Unit Value or Variable Name
-  180000,                       ! Block Size 2 Value or Variable Name
-  0.0424,                       ! Block 2 Cost per Unit Value or Variable Name
-  remaining,                    ! Block Size 3 Value or Variable Name
-  0.0383;                       ! Block 3 Cost per Unit Value or Variable Name
-
-
-UtilityCost:Charge:Block,
-  BlockDemandCharge,            ! Charge Variable Name
-  ExampleC,                     ! Tariff Name
-  totalDemand,                  ! Source Variable
-  Annual,                       ! Season
-  DemandCharges,                ! Category Variable Name
-  ,                             ! Remaining Into Variable
-  ,                             ! Block Size Multiplier Value or Variable Name
-  20,                           ! Block Size 1 Value or Variable Name
-  5.38,                         ! Block 1 Cost per Unit Value or Variable Name
-  80,                           ! Block Size 2 Value or Variable Name
-  4.23,                         ! Block 2 Cost per Unit Value or Variable Name
-  remaining,                    ! Block Size 3 Value or Variable Name
-  3.60;                         ! Block 3 Cost per Unit Value or Variable Name
-```
-
-
-
-#### Example D - Seasonal Energy Charges with Minimum Charge
-
-Another type of tariff is one where the energy charges vary by the amount of energy consumed each month and are different for the summer and winter. In addition, this example demonstrates the minimum charge field.
-
-Minimum Charge:     $7.00 per month
-
-Winter – October through May
-
-Energy Charge:        4.385 cents/kWh for first 650 kWh
-
-                                  3.763 cents/kWh for next 350 kWh
-
-                                  3.704 cents/kWh for over 1000 kWh
-
-Summer – June through September
-
-Energy Charge:        8.385 cents/kWh for first 650 kWh
-
-                                  7.588 cents/kWh for next 350 kWh
-
-                                  7.103 cents/kWh for over 1000 kWh
-
-This tariff would use two UtilityCost:Charge:Block objects. The monthly charge is part of the UtilityCost:Tariff object. Note that the block sizes are every other field at the bottom of the object and the that final block size references a built in variable called “remaining� that contains a very large number.
-
-```idf
-UtilityCost:Tariff,
-  ExampleD,                     ! Name
-  Electricity:Facility,         ! Output Meter Name
-  KWh,                          ! Conversion Factor Choice
-  ,                             ! Energy Conversion Factor
-  ,                             ! Demand Conversion Factor
-  ,                             ! Time of Use Period Schedule Name
-  TwoSeasonSchedule,            ! Season Schedule Name
-  ,                             ! Month Schedule Name
-  ,                             ! Demand Window Length
-  ,                             ! Monthly Charge or Variable Name
-  7.00;                         ! Minimum Monthly Charge or Variable Name
-
-
-UtilityCost:Charge:Block,
-  WinterEnergyCost,             ! Charge Variable Name
-  ExampleD,                     ! Tariff Name
-  totalEnergy,                  ! Source Variable
-  Winter,                       ! Season
-  EnergyCharges,                ! Category Variable Name
-  ,                             ! Remaining Into Variable
-  ,                             ! Block Size Multiplier Value or Variable Name
-  650,                          ! Block Size 1 Value or Variable Name
-  0.04385,                      ! Block 1 Cost per Unit Value or Variable Name
-  350,                          ! Block Size 2 Value or Variable Name
-  0.03763,                      ! Block 2 Cost per Unit Value or Variable Name
-  remaining,                    ! Block Size 3 Value or Variable Name
-  0.03704;                      ! Block 3 Cost per Unit Value or Variable Name
-
-
-UtilityCost:Charge:Block,
-  SummerEnergyCost,             ! Charge Variable Name
-  ExampleD,                     ! Tariff Name
-  totalEnergy,                  ! Source Variable
-  Summer,                       ! Season
-  EnergyCharges,                ! Category Variable Name
-  ,                             ! Remaining Into Variable
-  ,                             ! Block Size Multiplier Value or Variable Name
-  650,                          ! Block Size 1 Value or Variable Name
-  0.08385,                      ! Block 1 Cost per Unit Value or Variable Name
-  350,                          ! Block Size 2 Value or Variable Name
-  0.07588,                      ! Block 2 Cost per Unit Value or Variable Name
-  remaining,                    ! Block Size 3 Value or Variable Name
-  0.07103;                      ! Block 3 Cost per Unit Value or Variable Name
-
-
-Schedule:Compact, TwoSeasonSchedule, number,
-Through: 5/31, For: AllDays, Until: 24:00, 1,
-Through: 9/30, For: AllDays, Until: 24:00, 3,
-Through: 12/31, For: AllDays, Until: 24:00, 1;
-```
-
-
-#### Example E – kWh/kW Energy Charges
-
-A more advanced rate varies the size of the blocks based on amount of demand for the month. This creates an effective demand charge if the blocks have declining values.
-
-Customer Charge:  $14.00 per month
-
-Energy Charge:   8.756 cents/kWh for all consumption not greater than 200 hours times the demand
-
-                            6.812 cents/kWh for all consumption in excess of 200 hours and not greater than 400 hours times the demand
-
-                            5.029 cents/kWh for all consumption in excess of 400 hours times the demand.
-
-This tariff would use a single  UtilityCost:Charge:Block object. The monthly charge is part of the  UtilityCost:Tariff object. In this case the Block Size Multiplier Value (or Variable) is set to the totalDemand variable.
-
-```idf
-UtilityCost:Tariff,
-  ExampleE,                     ! Name
-  Electricity:Facility,         ! Output Meter Name
-  KWh,                          ! Conversion Factor Choice
-  ,                             ! Energy Conversion Factor
-  ,                             ! Demand Conversion Factor
-  ,                             ! Time of Use Period Schedule Name
-  ,                             ! Season Schedule Name
-  ,                             ! Month Schedule Name
-  ,                             ! Demand Window Length
-  14;                           ! Monthly Charge or Variable Name
-
-
-UtilityCost:Charge:Block,
-  BlockEnergyCharge,            ! Charge Variable Name
-  ExampleE,                     ! Tariff Name
-  totalEnergy,                  ! Source Variable
-  Annual,                       ! Season
-  EnergyCharges,                ! Category Variable Name
-  ,                             ! Remaining Into Variable
-  totalDemand,                  ! Block Size Multiplier Value or Variable Name
-  200,                          ! Block Size 1 Value or Variable Name
-  0.08756,                      ! Block 1 Cost per Unit Value or Variable Name
-  200,                          ! Block Size 2 Value or Variable Name
-  0.06812,                      ! Block 2 Cost per Unit Value or Variable Name
-  remaining,                    ! Block Size 3 Value or Variable Name
-  0.05029;                      ! Block 3 Cost per Unit Value or Variable Name
-```
-
-
-#### Example F – Seasonal Time of Use Energy
-
-Tariffs sometimes have higher costs for energy consumed during the daytime than at night. This example includes energy charges that vary by the time of day and by the season.
-
-Monthly Charge:       $37.75 per month
-
-Winter – October through May
-
-On Peak:                   8.315 cents/kWh
-
-Off-Peak:                   2.420 cents/kWh
-
-Summer – June through September
-
-On Peak:                   14.009 cents/kWh
-
-Off-Peak:                   6.312 cents/kWh
-
-The on-peak period is defined as the hours starting at 10am and ending at 7pm, Monday through Friday for June through September and 3pm to 10pm Monday through Friday for October through May. All other hours are considered off-peak.
-
-The tariff is only applicable for customers that use 50KW for at least one month of the year.
-
-This tariff uses four different UtilityCost:Charge:Simple objects to capture the variation with time of the energy cost. The monthly charge is part of the UtilityCost:Tariff object.
-
-```idf
-UtilityCost:Tariff,
-  ExampleF,                     ! Name
-  Electricity:Facility,         ! Output Meter Name
-  kWh,                          ! Conversion Factor Choice
-  ,                             ! Energy Conversion Factor
-  ,                             ! Demand Conversion Factor
-  TimeOfDaySchedule,            ! Time of Use Period Schedule Name
-  TwoSeasonSchedule,            ! Season Schedule Name
-  ,                             ! Month Schedule Name
-  ,                             ! Demand Window Length
-  37.75;                        ! Monthly Charge or Variable Name
-
-
-UtilityCost:Charge:Simple,
-  SummerOnPeak,                 ! Charge Variable Name
-  ExampleF,                     ! Tariff Name
-  peakEnergy,                   ! Source Variable
-  Summer,                       ! Season
-  EnergyCharges,                ! Category Variable Name
-  0.14009;                      ! Cost per Unit Value or Variable Name
-
-
-UtilityCost:Charge:Simple,
-  SummerOffPeak,                ! Charge Variable Name
-  ExampleF,                     ! Tariff Name
-  offPeakEnergy,                ! Source Variable
-  Summer,                       ! Season
-  EnergyCharges,                ! Category Variable Name
-  0.06312;                      ! Cost per Unit Value or Variable Name
-
-
-UtilityCost:Charge:Simple,
-  WinterOnPeak,                 ! Charge Variable Name
-  ExampleF,                     ! Tariff Name
-  peakEnergy,                   ! Source Variable
-  Winter,                       ! Season
-  EnergyCharges,                ! Category Variable Name
-  0.08315;                      ! Cost per Unit Value or Variable Name
-
-
-UtilityCost:Charge:Simple,
-  WinterOffPeak,                ! Charge Variable Name
-  ExampleF,                     ! Tariff Name
-  offPeakEnergy,                ! Source Variable
-  Winter,                       ! Season
-  EnergyCharges,                ! Category Variable Name
-  0.02420;                      ! Cost per Unit Value or Variable Name
-
-
-UtilityCost:Qualify,
-  MinDemand,                    ! Name
-  ExampleF,                     ! Tariff Name
-  TotalDemand,                  ! Variable Name
-  Minimum,                      ! Qualify Type
-  50,                           ! Threshold Value or Variable Name
-  Annual,                       ! Season
-  Count,                        ! Threshold Test
-  1;                            ! Number of Months
-
-
-Schedule:Compact, TwoSeasonSchedule, number,
-Through: 5/31, For: AllDays,  Until: 24:00, 1,
-Through: 9/30, For: AllDays,  Until: 24:00, 3,
-Through: 12/31, For: AllDays, Until: 24:00, 1;
-
-
-Schedule:Compact, TimeOfDaySchedule, number,
-Through: 5/31, For: AllDays,  Until: 15:00, 3,
-                              Until: 22:00, 1,
-                              Until: 24:00, 3,
-Through: 9/30, For: AllDays,  Until: 10:00, 3,
-                              Until: 19:00, 1,
-                              Until: 24:00, 3,
-Through: 12/31, For: AllDays, Until: 15:00, 3,
-                              Until: 22:00, 1,
-                              Until: 24:00, 3;
-```
-
-
-#### Example G – Blocks within Blocks
-
-Utilities have come up with many different ways to encourage certain load factors and discourage other load factors. One method that has been used is blocks defined within other blocks. In the following example standard kWh blocks exist within the energy allocated for the first of several kWh/kW blocks.
-
-Monthly Charge:   $35 per month
-
-Energy Charge:    For all consumption not greater than 200 hours times the demand use
-
-                              10.32 cents/kWh for the first 1000 kWh
-
-                              7.43 cents/kWh for the next 4000 kWh
-
-                              6.23 cents/kWh for the next 5000 kWh
-
-                              4.27 cents/kWh for the remaining kWh less than 200 hours times the demand
-
-                              6.82 cents/kWh for all consumption in excess of 200 hours and not greater than 400 hours times the demand
-
-                              5.03 cents/kWh for all consumption in excess of 400 hours times the demand.
-
-To set up this “block within a block� a UtilityCost:Charge:Block is first used to separate out the first 200 kWh/kW. The “EnergyFirst200kWhPerkW� charge performs this. It uses demand to multiply the first block size by 200 and the “cost� for the block is simply 1 since it passes through the energy to the variable “EnergyFirst200kWhPerkW�. The remaining energy goes into the “restOfEnergy� variable as specified as the “Remaining Into Variable� field. After this is evaluated we have two new variables that hold energy. Each of these variables are then separately used in UtilityCost:Charge:Block objects to evaluate the different parts of the example tariff. By using the “Remaining Into Variable� along with the concept of variables, many very complex tariffs may be modeled.
-
-
-
-```idf
-  UtilityCost:Tariff,
-    ExampleG,                !- Name
-    ElectricityPurchased:Facility,  !- Output Meter Name
-    KWh,                     !- Conversion Factor Choice
-    ,                        !- Energy Conversion Factor
-    ,                        !- Demand Conversion Factor
-    ,                        !- Time of Use Period Schedule Name
-    ,                        !- Season Schedule Name
-    ,                        !- Month Schedule Name
-    ,                        !- Demand Window Length
-    35;                      !- Monthly Charge or Variable Name
-
-
-  UtilityCost:Charge:Block,
-    EnergyFirst200kWhPerkW,  !- Charge Variable Name
-    ExampleG,                !- Tariff Name
-    totalEnergy,             !- Source Variable
-    Annual,                  !- Season
-    NotIncluded,             !- Category Variable Name
-    restOfEnergy,            !- Remaining Into Variable
-    totalDemand,             !- Block Size Multiplier Value or Variable Name
-    200,                     !- Block Size 1 Value or Variable Name
-    1;                       !- Block 1 Cost Per Unit Value or Variable Name
-
-
-  UtilityCost:Charge:Block,
-    CostOfFirst200kWhPerkW,  !- Charge Variable Name
-    ExampleG,                !- Tariff Name
-    EnergyFirst200kWhPerkW,  !- Source Variable
-    Annual,                  !- Season
-    EnergyCharges,           !- Category Variable Name
-    ,                        !- Remaining Into Variable
-    ,                        !- Block Size Multiplier Value or Variable Name
-    1000,                    !- Block Size 1 Value or Variable Name
-    0.1032,                  !- Block 1 Cost Per Unit Value or Variable Name
-    4000,                    !- Block Size 2 Value or Variable Name
-    0.0743,                  !- Block 2 Cost Per Unit Value or Variable Name
-    5000,                    !- Block Size 3 Value or Variable Name
-    0.0623,                  !- Block 3 Cost Per Unit Value or Variable Name
-    remaining,               !- Block Size 4 Value or Variable Name
-    0.0427;                  !- Block 4 Cost Per Unit Value or Variable Name
-
-
-  UtilityCost:Charge:Block,
-    CostOfRestOfEnergy,      !- Charge Variable Name
-    ExampleG,                !- Tariff Name
-    restOfEnergy,            !- Source Variable
-    Annual,                  !- Season
-    EnergyCharges,           !- Category Variable Name
-    ,                        !- Remaining Into Variable
-    totalDemand,             !- Block Size Multiplier Value or Variable Name
-    200,                     !- Block Size 1 Value or Variable Name
-    0.0682,                  !- Block 1 Cost Per Unit Value or Variable Name
-    remaining,               !- Block Size 2 Value or Variable Name
-    0.0503;                  !- Block 2 Cost Per Unit Value or Variable Name
-```
-
-
-#### Example H – Real Time Pricing
-
-Some utilities have tariffs that can have different prices every hour of the year called Real Time Pricing tariffs. Often the utility will inform the customer of the prices for each hour of the day just one day in advance. To model this type of utility rate a normal schedule is used that contains the prices on an hourly basis.  The “Charge Schedule� field is where the Schedule object containing the prices is referenced.  In addition, the “Baseline Use Schedule� field is used to set the schedule for the customer baseline load. Not all utilities use a customer baseline load so the field can be left blank if none is needed. The Period, Season and Month Schedules are not needed for these tariffs unless UtilityCost:Charge’s are used.  The Schedule:File object can be especially useful to input a complex schedule that changes throughout the year.
-
-Example H, shown below, is an example of how to use the UtilityCost:Tariff object with a schedule to calculate a utility tariff using real time prices.  The example real time pricing schedule results in the same energy cost as Example F – Seasonal Time of Use Energy. This is only an example and usually for real time pricing the schedule values would vary throughout the year.
-
-
-
-!  EXAMPLE H - Real Time Pricing (RTP)
-
-
-```idf
-  UtilityCost:Tariff,
-    ExampleH,                !- Name
-    ElectricityPurchased:Facility,  !- Output Meter Name
-    kWh,                     !- Conversion Factor Choice
-    ,                        !- Energy Conversion Factor
-    ,                        !- Demand Conversion Factor
-    ,                        !- Time of Use Period Schedule Name
-    ,                        !- Season Schedule Name
-    ,                        !- Month Schedule Name
-    ,                        !- Demand Window Length
-    37.75,                   !- Monthly Charge or Variable Name
-    ,                        !- Minimum Monthly Charge or Variable Name
-    RTPpriceSchedule-H,      !- Real Time Pricing Charge Schedule Name
-    ,                        !- Customer Baseline Load Schedule Name
-    ,                        !- Group Name
-    buyFromUtility;          !- Buy Or Sell
-
-
-  Schedule:Compact,
-    RTPpriceSchedule-H,      !- Name
-    Any Number,              !- Schedule Type Limits Name
-    Through: 5/31,           !- Field 1
-    For: AllDays,            !- Field 2
-    Until: 15:00,            !- Field 3
-    0.02420,                 !- Field 4
-    Until: 22:00,            !- Field 5
-    0.08315,                 !- Field 6
-    Until: 24:00,            !- Field 7
-    0.02420,                 !- Field 8
-    Through: 9/30,           !- Field 9
-    For: AllDays,            !- Field 10
-    Until: 10:00,            !- Field 11
-    0.06312,                 !- Field 12
-    Until: 19:00,            !- Field 13
-    0.14009,                 !- Field 14
-    Until: 24:00,            !- Field 15
-    0.06312,                 !- Field 16
-    Through: 12/31,          !- Field 17
-    For: AllDays,            !- Field 18
-    Until: 15:00,            !- Field 19
-    0.02420,                 !- Field 20
-    Until: 22:00,            !- Field 21
-    0.08315,                 !- Field 22
-    Until: 24:00,            !- Field 23
-    0.02420;                 !- Field 24
-```
-
-
-#### Example I – Selling and Net-Metering
-
-When the building contains a generator, photovoltaics, or other sources of electrical power, there is an opportunity for the building generator to produce more power than the building uses. The excess power can either be sold to the utility or offset the energy purchased.
-
-When the excess power is sold, two utility rates need to be defined. The first can be defined just as in any of the previous examples. Since the “Buy or Sell� field of the UtilityCost:Tariff object defaults to “buyFromUtility� it does not even need to be specified. The meter specified in the “Output Meter� is usually set to “ElectricityPurchased:Facility.�
-
-The second tariff needs to be defined with the “Buy or Sell� field set to “sellToUtility.� The “Output Meter� is usually set to “ElectricitySurplusSold:Facility.� It is important to set the appropriate meters that correspond with the “Buy or Sell� field.  The example below shows an tariff that sells the excess electricity back to utility. The UtilityCost:Charge:Simple object contains a “Cost Per Value� with a negative number. A negative number is critical if a credit for selling this electricity is expected.
-
-
-
-!  EXAMPLE I - Selling
-
-
-```idf
-  UtilityCost:Charge:Simple,
-    GeneratedElectricSold,   !- Charge Variable Name
-    ExampleI-Sell,           !- Tariff Name
-    totalEnergy,             !- Source Variable
-    Annual,                  !- Season
-    EnergyCharges,           !- Category Variable Name
-    -0.02;                   !- Cost Per Unit Value (or Variable)
-
-
-  UtilityCost:Tariff,
-    ExampleI-Sell,           !- Name
-    ElectricitySurplusSold:Facility,  !- Output Meter Name
-    kWh,                     !- Conversion Factor Choice
-    ,                        !- Energy Conversion Factor
-    ,                        !- Demand Conversion Factor
-    ,                        !- Time of Use Period Schedule Name
-    ,                        !- Season Schedule Name
-    ,                        !- Month Schedule Name
-    ,                        !- Demand Window Length
-    ,                        !- Monthly Charge or Variable Name
-    ,                        !- Minimum Monthly Charge or Variable Name
-    ,                        !- Real Time Pricing Charge Schedule Name
-    ,                        !- Customer Baseline Load Schedule Name
-    ,                        !- Group Name
-    sellToUtility;           !- Buy Or Sell
-
-
-  UtilityCost:Charge:Simple,
-    GeneratedElectricSold,   !- Charge Variable Name
-    ExampleI-Sell,           !- Tariff Name
-    totalEnergy,             !- Source Variable
-    Annual,                  !- Season
-    EnergyCharges,           !- Category Variable Name
-    -0.02;                   !- Cost Per Unit Value or Variable Name
-
-```
-
-
-
-The next part of this example is a rate that uses net-metering. With net metering the meter conceptually turns backwards when the energy is being sold to the utility directly reducing the energy consumption being charged.  Effectively, the rate charge for purchased electricity is the same as the rate credited for electricity sold to the utility. In this the “Buy or Sell� field should be set to “netMetering.�  It is also important the “Output Meter� is set to a meter that represents net metering such as “ElectricityNet:Facility.� The following example shows a simple example tariff using net metering with a single UtilityCost:Charge:Simple:
-
-
-```idf
-!  EXAMPLE I – Net Metering
-
-
-  UtilityCost:Tariff,
-    ExampleI-NetMeter,       !- Name
-    ElectricityNet:Facility, !- Output Meter Name
-    kWh,                     !- Conversion Factor Choice
-    ,                        !- Energy Conversion Factor
-    ,                        !- Demand Conversion Factor
-    ,                        !- Time of Use Period Schedule Name
-    ,                        !- Season Schedule Name
-    ,                        !- Month Schedule Name
-    ,                        !- Demand Window Length
-    30.00,                   !- Monthly Charge or Variable Name
-    ,                        !- Minimum Monthly Charge or Variable Name
-    ,                        !- Real Time Pricing Charge Schedule Name
-    ,                        !- Customer Baseline Load Schedule Name
-    ,                        !- Group Name
-    netMetering;             !- Buy Or Sell
-
-
-  UtilityCost:Charge:Simple,
-    NetMeteredCharge,        !- Charge Variable Name
-    ExampleI-NetMeter,       !- Tariff Name
-    totalEnergy,             !- Source Variable
-    Annual,                  !- Season
-    EnergyCharges,           !- Category Variable Name
-    0.065;                   !- Cost Per Unit Value or Variable Name
-```
-
-
-UtilityCost:Tariff Reporting
-----------------------------
-
-A standardized tabular output report is created which shows all components of all categories in the calculation sequence on a variable basis (usually 12 numbers, one for each month). The economics report is automatically created if any UtilityCost:Tariff objects are present. The values reported are in the units specified in the UtilityCost:Tariff object. The report includes:
-
-Economic Results Summary Report
--------------------------------
-
-- Annual Cost – Shows the annual cost for qualified and selected electric and gas tariffs and the total cost
-
-- Tariff Summary – For each tariff included shows if that tariff was selected, if it was qualified, what meter it was connected to, what group it was part of, and the annual cost. The qualified tariff with the lowest annual cost for each of the meters is indicated as “selected� and shown in the Annual Cost section of the report. If multiple groups are defined, a tariff is selected from each group.
-
-**Tariff Summary**
-
-- Summary table – Shows the if that tariff was selected, if it was qualified, which qualifier disqualified the tariff, what meter it was connected to, what group it was part of, if the computation was based on a user defined computation or was automatic.
-
-- Categories – Shows the monthly results of all the category variables.
-
-- Charges – Shows the monthly results for all of the simple and block charges.
-
-- Ratchets – Shows the monthly results for all ratchets.
-
-- Qualifies – Shows the monthly results for all qualifies.
-
-- Native Variables – Shows the monthly values for the native variables such as TotalEnergy and TotalDemand.
-
-- Other Variables – Shows the monthly values for any other variables not appearing in the other tables.
-
-- Computation – Shows the computational steps used including those generated automatically.
-
-The report is part of the tabular report and is created using the same style as specified for the tabular reports.
-
-Complex Tariff Modeling
------------------------
-
-Much can be accomplished with the UtilityCost:Charge:Simple and UtilityCost:Charge:Block objects. In almost all cases, these structures are flexible enough to model the tariff. At times the built in approach is not sufficient to model a particular rate. In those cases, the rate may be modeled by using the UtilityCost:Computation object. For most rates this object can be omitted but for difficult to model rates, they may be used to modify the normal way the rate computation is performed.
-
-Each ComputeStep is performed in order and can be either a variable followed by an expression or simply a variable.
-
-- demandMod SUM demand1 demand2
-
-- chargeSummer1
-
-The normal calculations associated with the UtilityCost:Qualify, UtilityCost:Charge:Simple, UtilityCost:Charge:Block, or UtilityCost:Ratchet are performed the first time that object is called. Subsequent times are not recomputed but use the value stored in the appropriate variable. The result of the computation for those objects is available in the expression for further computation. The expressions allow the manipulation of variables directly using simple mathematical functions. Only variable names may be entered along with operators. Numbers may not be entered and should be entered with UtilityCost:Variable. Multiple operators are allowed per step. Variables names do not include spaces. If spaces are found in a variable name then an error is shown. Unused variables are flagged with a warning. All expressions are in the form:
-
-- assignedToVariable OPERATOR variable1 variable2
-
-Each step is performed for each of the months before the next step is taken. The same operation is performed for each step as specified.
-
-The actual evaluation of the expression is performed from the end of the line to the beginning using stack based operations. Some operators pull all values from the stack (SUM, MAXIMUM, MINIMUM) while most use just one or two values from the stack. All operations return a single value to the stack. This stack based approach to expressions is sometimes called Polish Notation. While multiple operators are allowed per line, it reduces confusion if each line has only a single operator.
-
-When the UtilityCost:Computation object is used, it must contain references to all objects involved in the rate in the order that they should be computed. No checking is performed for objects that should or should not be included; instead, the computational process is driven completely by the input of this object.
-
-A typical rate will have a simple series of steps. For example F the following steps would be created automatically by the software:
-
-```idf
-UtilityCost:Computation,
-  SpecialStepsForF,             !- Name
-  ExampleF,                     !- Tariff Name
-  EnergyCharges SUM SummerOnPeak SummerOffPeak WinterOnPeak WinterOffPeak, Compute Step 1
-  Basis SUM EnergyCharges DemandCharges ServiceCharges, Compute Step 2
-  SubTotal SUM Basis Adjustments Surcharges, Compute Step 3
-  Total SUM SubTotal Taxes, Compute Step 4
-  MinDemand; Compute Step 5
-```
-
-
-This example does not have any dependency of different charges that are summed on the same line but if it did the charges could appear by themselves on lines and this would indicate the order that they should be computed. Here is the same example again showing that form.
-
-```idf
-UtilityCost:Computation,
-  SpecialStepsForF,            !- Name
-  ExampleF,                    !- Tariff Name
-  SummerOnPeak,                !- Compute Step 1
-  SummerOffPeak,               !- Compute Step 2
-  WinterOnPeak,                !- Compute Step 3
-  WinterOffPeak,               !- Compute Step 4
-  EnergyCharges SUM SummerOnPeak SummerOffPeak WinterOnPeak WinterOffPeak,  !- Compute Step 5
-  Basis SUM EnergyCharges DemandCharges ServiceCharges,                     !- Compute Step 6
-  SubTotal SUM Basis Adjustments Surcharges,   !- Compute Step 7
-  Total SUM SubTotal Taxes,                    !- Compute Step 8
-  MinDemand;                   !- Compute Step 9
-```
-
-
-This second expanded format is generated automatically when no UtilityCost:Computation object is provided.
-
-The functions built in are (number of arguments in parentheses):
-
-#### Operator:   SUM (unlimited)
-
-Adds together all of the variable values for each month for as many variables that are used.
-
-#### Operator:   ADD (2)
-
-Adds together the first variable value with the second variable value.
-
-#### Operator:   MULTIPLY (2)
-
-Multiplies the first variable value with the second variable value. MULT may also be used.
-
-#### Operator:  SUBTRACT (2)
-
-Subtracts the second variable value from the first variable value. SUBT may also be used.
-
-#### Operator:  DIVIDE (2)
-
-Divides the first variable value by the second variable value. DIV may also be used.
-
-#### Operator:  ABSOLUTE (1)
-
-Takes the absolute value of the variable value. This turns negative values into positive ones. ABS may also be used.
-
-#### Operator:  INTEGER (1)
-
-Removes non-integer portions of the variable values. INT may also be used.
-
-#### Operator:  SIGN (1)
-
-Returns a 1 for positive values, -1 for negative values and 0 for zero values.
-
-#### Operator:  MAXIMUM (unlimited)
-
-Selects the maximum value across variables for each of the months. Two or more variables may be used. MAX may also be used.
-
-#### Operator:  MINIMUM (unlimited)
-
-Selects the minimum value across variables for each of the months. Two or more variables may be used. MIN may also be used.
-
-#### Operator:  EXCEEDS (2)
-
-Returns the difference between the first and second variable if the first variable is greater than the second. If the second variable is greater or equal to the first variable returns a zero.
-
-#### Operator:  ANNUALMINIMUM (1)
-
-Returns the minimum value of the twelve months in the variable. Zero values are ignored (see also ANNUALMINZERO). If all values are zero then zero is returned. ANMIN may also be used.
-
-#### Operator:  ANNUALMAXIMUM (1)
-
-Returns the maximum value of the twelve months in the variable. Zero values are ignored (see also ANNUALMAXZERO). If all values are zero then zero is returned. ANMAX may also be used.
-
-#### Operator:  ANNUALSUM (1)
-
-Returns the sum of the twelve months in the variable. ANSUM may also be used.
-
-#### Operator:  ANNUALAVERAGE (1)
-
-Returns the sum of the twelve monthly values divided by the number of non-zero monthly values. If all values are zero than zero is returned. If an average is desired that includes zero valued elements the SUM() function should be used divided by 12. ANAVG may also be used.
-
-#### Operator:  ANNUALOR (1)
-
-Returns 1 for all monthly values if any of the monthly values are non-zero. ANOR may also be used.
-
-#### Operator:  ANNUALAND (1)
-
-Returns 1 for all monthly values if all of the monthly values are non-zero. ANAND may also be used.
-
-#### Operator:  ANNUALMAXIMUMZERO (1)
-
-Returns the maximum value of the twelve monthly values in x. Zeros are counted so if a zero is the largest value (the rest would be negative) a zero may be returned. ANMAXZ may also be used.
-
-#### Operator:  ANNUALMINIMUMZERO (1)
-
-Returns the minimum value of the twelve monthly values in x. Zeros are counted. ANMINZ may also be used.
-
-#### Operator:  IF (3)
-
-Returns the value of the second variable if the first variable is non-zero otherwise returns the value of the third variable. Usually used with GT, GE, LT, LE, EQ, NE operators.
-
-#### Operator:  GREATERTHAN (2)
-
-1 if the first variable value is greater than the second variable value otherwise 0. GT may also be used.
-
-#### Operator:  GREATEREQUAL (2)
-
-1 if the first variable value is greater than or equal to the second variable value otherwise 0. GE may also be used.
-
-#### Operator:  LESSTHAN (2)
-
-1 if the first variable value is less than the second variable value otherwise 0. LT may also be used.
-
-#### Operator:  LESSEQUAL (2)
-
-1 if the first variable value is less than or equal to the second variable value otherwise 0. LE may also be used.
-
-#### Operator:  EQUAL (2)
-
-1 if the first variable value is equal to the second variable value otherwise 0. EQ may also be used.
-
-#### Operator:  NOTEQUAL (2)
-
-1 if the first variable value is not equal to the second variable value otherwise 0. NE may also be used.
-
-#### Operator:  AND (2)
-
-1 if the first variable value and second variable values are both not zero otherwise 0.
-
-#### Operator:  OR (2)
-
-1 if the first variable value and second variable values are either not zero, otherwise 0 if both the first and second variable value are both zero.
-
-#### Operator:  NOT (2)
-
-1 if the first variable value and only variable value is zero otherwise 0 if the first variable value is not zero.
-
-#### Operator:  FROM (Unlimited)
-
-Indicates what variables a variable is dependant on (or derived from). No computation is performed. The algorithm that creates the automatic sequence of equations uses these to indicate when variables are dependant on other variables so that they can be sorted into the correct order.
-
-
-
-Cost Estimating
----------------
-
-In order to understand how to include cost estimates, it may be helpful to first define some terminology and provide an overview of the process used in EnergyPlus. There are three broad steps involved. The first involves determining *construction* costs by summing individual “line items.�  The second involves determining *project* costs by adjusting construction costs to account for things like profit and design fees. The third involves comparing the current simulation to a reference case so that marginal increases can be calculated. Each of these steps involves using one of the three ‘ComponentCost’ objects described below.
-
-### ComponentCost:LineItem
-
-Each instance of this object creates a cost line item and will contribute to the total for a cost estimate. Each line item is reported in table form in the tabular report file. The user must request that this report be generated by including a Output:Table:SummaryReports object with the Component Cost Economics Summary option selected. The style of a tabular report can be controlled using the OutputControl:Table:Style object.
-
-Cost estimates are not currently general in that they cannot be performed for every type of component that could be included in an EnergyPlus model. Although a “General� option is available where all information needed for the cost line item is input by the user, the usefulness of cost modeling within EnergyPlus is expected to be enhanced when quantities are obtained from elsewhere in the input file or computed during a simulation. The cost computations are programmed in selected ways for selected objects. The objects available and the type of cost modeling that may be performed are discussed in detail in the discussion of Reference Object Type field. A particular instance of this object will always have many blank fields. Entering values in too many fields may cause an error because the program may determine how a particular cost is to be calculated based on the presence of non-zero values in particular fields. The input object includes fields that are reserved for future use in expanded cost estimate and investment analyses planned for future versions of EnergyPlus. If you would like to request additional objects or different methods of modeling component costs, feel free to describe your needs and submit a request via email to energyplus-support@gard.com.
-
-
-
-#### Field: Name
-
-This field is a user-selected name that will appear in the line item description of the cost report. It is not used in the calculation but allows identifying a line item in the subsequent report.
-
-#### Field: Type
-
-This field is not yet used and may be left blank.
-
-#### Field: Line Item Type
-
-The cost estimate line item calculation will be controlled by the name entered in this field. The requirements for the remaining input, and the cost calculations performed, will vary depending on the object referenced here. Only selected objects can be entered here. The objects available for cost estimating are listed in the following table showing the active fields and options available for each.
-
-Table 37. Cost Line Item Types (ref Objects)
-
-<table class="table table-striped">
-<tr>
-<th>Object Types available (choice keys)</th>
-<th>Cost per each</th>
-<th>Cost per m<sup>2</sup></th>
-<th>Cost per kW</th>
-<th>Cost per kW *COP</th>
-<th>Cost per m<sup>3</sup></th>
-<th>Cost per m<sup>3</sup>/s</th>
-<th>Cost per W/K</th>
-<th>Qty</th>
-<th>Wildcard for Name</th>
-</tr>
-<tr>
-<td>General</td>
-<td>X</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>X</td>
-<td> </td>
-</tr>
-<tr>
-<td>Construction</td>
-<td> </td>
-<td>X</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Coil:DX Coil:Cooling:DX: SingleSpeed</td>
-<td>X</td>
-<td> </td>
-<td>X</td>
-<td>X</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>X</td>
-</tr>
-<tr>
-<td>Chiller:Electric</td>
-<td>X</td>
-<td> </td>
-<td>X</td>
-<td>X</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Coil:Heating:Gas</td>
-<td>X</td>
-<td> </td>
-<td>X</td>
-<td>X</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>X</td>
-</tr>
-<tr>
-<td>Daylighting:Controls</td>
-<td>X</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>X</td>
-</tr>
-<tr>
-<td>Shading:Zone:Detailed</td>
-<td> </td>
-<td>X</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Lights</td>
-<td>X</td>
-<td> </td>
-<td>X</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Generator:Photovoltaic</td>
-<td> </td>
-<td> </td>
-<td>X</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
-General
-
-This choice of object is used to calculate costs in a general way. No quantities from internal calculations are used. All information needed for the cost line item is input by the user. The Cost per Each and the Quantity fields that follow need to have values.
-
-#####  Construction
-
-This choice of object type is used to calculate the costs associated with surfaces based on the type of Construction used for the surface. Costs are entered on a per-square-meter basis. The program finds all the surfaces that have the type of Construction named in the Reference Object Name field that follows and determines the total area. If the model includes duplicate surfaces, as for interior partitions or floors, these will be detected and not double-counted. The cost per area should include all the material layers defined in the Construction.
-
-##### Coil:DX or Coil:Cooling:DX:SingleSpeed
-
-This choice of object type is used to calculate the cost of direct expansion cooling equipment. Cost can be entered in three different ways, (1) per each, (2) per kW total cooling capacity, or (3) per kW total cooling capacity per COP (coefficient of performance). The program will determine which method to use by examining which input fields have non-zero values. It is an error to specify costs in more than one way. The per-each approach is most useful for discrete packages. The per-kW approach is useful for autosizing DX coils with the same COP. The per-kW-per-COP approach is convenient for modeling autosized DX coils with differing COPs as long as a linear relationship is sufficient.
-
-The wildcard character “\*� may be used in the object name field that follows to allow a single line item to include all of the DX coils in the model.
-
-Chiller:Electric
-
-This choice of object type is used to calculate the cost of a central chiller. The object name entered in following field must correspond to a Chiller:Electric object name defined elsewhere in the input file. Cost can be entered in three different ways, (1) per each, (2) per kW total cooling capacity or (3) per kW total cooling capacity per COP (coefficient of performance). The program will determine which method to use by examining which input fields have non-zero values. It is an error to specify costs in more than one way. The per-each approach is most useful for discrete chillers. The per-kW approach is useful for autosizing chillers with the same COP. The per-kW-per-COP approach is convenient for modeling autosized chillers with differing COPs as long as a linear relationship is sufficient.
-
-##### Coil:Heating:Gas
-
-This choice of object type is used to calculate the cost of gas-fired heating equipment. Cost can be entered in three different ways, (1) per each, (2) per kW of heating capacity, or (3) per kW total cooling capacity per nominal efficiency (actually uses the per kW per COP field). The program will determine which method to use by examining which input fields have non-zero values. It is an error to specify costs in more than one way. The per-each approach is most useful for discrete packages. The per-kW approach is useful for autosizing heating coils with the same efficiency. The per-kW-per-Eff approach is convenient for modeling autosized heating coils with differing efficiencies as long as a linear relationship is sufficient.
-
-The wildcard character “\*� may be used in the object name field that follows to allow a single line item to include all of the gas heating coils in the model.
-
-##### Daylighting:Controls
-
-These choices of object type are used to include the cost of controllers needed to control electric lighting in response to daylight. The only option for entering costs is “per each�. The wildcard character “\*� may be used in the following object name field to allow a single line item to include all of the simple and detailed daylighting controls in the cost model.
-
-##### Shading:Zone:Detailed
-
-This choice of object type is used to calculate the costs associated with attached shading surfaces. Costs are entered on a per-square-meter basis. The cost calculations are similar to those for heat transfer surfaces but are handled separately because “Construction� is not defined for a shading surface. The object name entered in the following field must correspond to a Shading:Zone:Detailed object name defined elsewhere in the input file.
-
-##### Lights
-
-This choice of object is used to calculate the costs associated with electric lighting. Costs are entered on either a cost-per-each basis or as a cost-per-kilowatt-of-design-level. (This design level is an input in the Lights object.). The object name entered into the following field must match the name of a Zone object defined elsewhere in the input file.
-
-##### Generator:Photovoltaic
-
-This choice of object is used to calculate the costs associated with a photovoltaic system. Costs are entered on a cost-per-kilowatt-of-rated-capacity. The rated capacity of a photovoltaic generator is calculated for cost modeling by exposing the surface to a 1000 W/m2 incident radiation using the area fraction and nominal fixed efficiency input by the user (from the Generator:Photovoltaic object). The object name entered into the following field must match the name of a Generator:Photovoltaic  object defined elsewhere in the input file.
-
-#### Field: Item Name
-
-This field is used to refer to a specific instance of an object. The wildcard character “\*� is acceptable for some objects as described above for the previous field.
-
-#### Field: Object End Use Key
-
-This field is not yet used and may be left blank.
-
-#### Field: Cost per Each
-
-This field is used to enter cost information on a per-each basis. The units are dollars ($).
-
-#### Field: Cost per Area
-
-This field is used to enter cost information on a per-area basis. The units are dollars per square meter ($/m<sup>2</sup>).
-
-#### Field: Cost per Unit of Output Capacity
-
-This field is used to enter cost information on a per-kilowatt basis. The units are dollars per kilowatt ($/kW).
-
-#### Field: Cost per Unit of Output Capacity per COP
-
-This field is used to enter cost information on a per-kilowatt-per-COP basis. The units are dollars per kilowatt per non-dimensional COP ($/kW-COP).  Note that this field can be used for Coil:Heating:Gas cost modeling in which case the better terminology would be per-kilowatt-per-non-dimensional-efficiency.
-
-#### Field: Cost per Volume
-
-This field is not yet used but will be used to enter cost information on a per-cubic-meter basis. The units are dollars per cubic meter ($/m<sup>3</sup>).
-
-#### Field: Cost per Volume Rate
-
-This field is not yet used but will be used to enter cost information on a per-cubic-meter-per-second basis. The units are dollars per cubic meter ($/(m<sup>3</sup>/s)).
-
-#### Field: Cost per Energy per Temperature Difference
-
-This field is not yet used but will be used to enter cost information on a per-watt-per-Kelvin basis. These units will be used to represent a UA description of coils and the like. The units are dollars per watt per delta K ($/(W/K)).
-
-#### Field: Quantity
-
-This field is used to directly enter the line item quantity. The units should correspond to what is used in the Per Each field.
-
-Some examples of this object in an IDF:
-
-```idf
-  ComponentCost:LineItem,
-   PSZ Equipment from scaling , !- Name
-   ,                            !- Type
-   Coil:DX,                     !- Line Item Type
-   ACDXCoil ZN1 ,               !- Item Name
-   ,                            !- Object End Use Key
-   ,                            !- Cost per Each {$}
-   ,                            !- Cost per Area {$/m2}
-   ,                            !- Cost per Unit of Output Capacity {$/kW}
-   82.5;                   !- Cost per Unit of Output Capacity per COP {$/kW}
-
-
-  ComponentCost:LineItem,
-    Lighting Equip: ZN2_E_Space_1, ,
-    Lights,!- Line Item Type
-    ZN2_E_Space_1, ,
-    ,!- Cost per Each {$}
-    ,!- Cost per Area {$/m2}
-    3300.000;!- Cost per Unit of Output Capacity {$/kW}
-
-
-
-
-  ComponentCost:LineItem, DL controls: ZN4_W_Space_1, ,
-    Daylighting:Detailed, !- Line Item Type
-    ZN4_W_Space_1, ,!- Item Name
-    125.000, !- Cost per Each {$}
-    ,!- Cost per Area {$/m2}
-    ;!- Cost per Unit of Output Capacity {$/kW}
-```
-
-
-
-### ComponentCost:Adjustments
-
-This object can be used to perform various modifications to the construction costs to arrive at an estimate for total project costs. This object allows extending the line item model so that the overall costs of the project will reflect various profit and fees. Only one object of this type can be included in the input file. The results are included in the Construction Cost Estimate Summary table by request using the Output:Table:SummaryReports object with the Component Cost Economics Summary option selected.
-
-#### Field: Miscellaneous Cost per Conditioned Area
-
-This optional field can be used to enter a cost model for miscellaneous project costs that are not included in the line item modeling. Miscellaneous costs are entered in dollars per square meter of conditioned floor area. This field allows including the costs of project elements that go beyond what can be modeled using “ComponentCost:LineItem� input objects including such things as structural components, site preparation, finishes, etc. The value input in this field will be multiplied by the conditioned floor area and listed in the Construction Cost Estimate Summary table. The miscellaneous project costs are added to the line item model total to determine the “modeled and miscellaneous Construction costs� that will be multiplied by the fractions in the following five fields.
-
-#### Field: Design and Engineering Fees
-
-This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for design and engineering fees. Note that is not the same as a fraction of the total cost estimate.
-
-#### Field: Contractor Fee
-
-This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for Contractor fees. Note that is not the same as a fraction of the total cost estimate.
-
-#### Field: Contingency
-
-This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added for contingency. Note that is not the same as a fraction of the total cost estimate.
-
-#### Field: Permits, Bonding and Insurance
-
-This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for permitting, bonding, and insurance costs to the project. Note that is not the same as a fraction of the total cost estimate.
-
-#### Field: Commissioning Fee
-
-This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for commissioning services. Note that is not the same as a fraction of the total cost estimate.
-
-#### Field: Regional Adjustment Factor
-
-This optional field can be used to enter an adjustment factor to account for regional differences is construction costs. The factor will be applied to the modeled and miscellaneous construction costs to determine and amount that should be added, or subtracted, to account for local variations in construction costs. The default factor is 1.0. The additive adjustment is calculated by subtracting 1.0 from the value entered in this field. This field is useful for using national average data in the line item and miscellaneous construction cost models and then altering the results based on regional differences.
-
-An example of this object in an IDF is:
-
-```idf
-ComponentCost:Adjustments,
-          467, !- Miscellaneous Cost per Conditioned Area
-         0.07, !- Design and Engineering Fees
-         0.07, !- Contractor Fee
-         0.10, !- Contingency
-         0.04, !- Permits, Bonding and Insurance
-         0.015,!- Commissioning Fee
-        1.136; !- Regional Adjustment Factor
-```
-
-
-
-### ComponentCost:Reference
-
-This object can be used to allow comparing the current cost estimate to the results of a previous estimate for a reference building. This object parallels the ComponentCost:Adjustment object but adds a field for entering the cost line item model result for the reference building. All the various adjustments to the project cost estimate are available here to allow using factors that differ between the current and the reference building models. The factors entered in the field associated with this object are applied to the reference building while the factors listed in the ComponentCost:Adjustment object are applied to the current building model cost estimate. Only one object of this type can be included in the input file. The results are included in the Construction Cost Estimate Summary table by request using the Output:Table:SummaryReports object with the Component Cost Economics Summary option selected.
-
-#### Field: Reference Building Line Item Costs
-
-This field is used to enter a dollar amount representing the total for the reference building that the user would like to compare to the line item cost model for the current building model. A typical source of data for this would be the “Line Item Subtotal� from a previous EnergyPlus simulation.
-
-#### Field: Reference Building Miscellaneous Cost per Conditioned Area
-
-This optional field can be used to enter a cost model for miscellaneous project costs that are not included in the line item modeling. Miscellaneous costs are entered in dollars per square meter of conditioned floor area. This field allows including the costs of project elements that go beyond what can be modeled using “ComponentCost:LineItem� input objects including such things as structural components, site preparation, finishes, etc. The value input in this field will be multiplied by the conditioned floor area and listed in the Construction Cost Estimate Summary table. The miscellaneous project costs are added to the reference building line item subtotal to determine the “modeled and miscellaneous construction costs� that will be multiplied by the fractions in the following five fields.
-
-#### Field: Reference Building Design and Engineering Fees
-
-This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for design and engineering fees. Note that is not the same as a fraction of the total cost estimate.
-
-#### Field: Reference Building Contractor Fee
-
-This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for Contractor fees. Note that is not the same as a fraction of the total cost estimate.
-
-#### Field: Reference Building Contingency
-
-This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added for contingency. Note that is not the same as a fraction of the total cost estimate.
-
-#### Field: Reference Building Permits, Bonding and Insurance
-
-This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for permitting, bonding, and insurance costs to the project. Note that is not the same as a fraction of the total cost estimate.
-
-#### Field: Reference Building Commissioning Fee
-
-This optional field can be used to enter a fraction of modeled and miscellaneous construction costs that should be added to account for commissioning services. Note that is not the same as a fraction of the total cost estimate.
-
-#### Field: Reference Building Regional Adjustment Factor
-
-This optional field can be used to enter an adjustment factor to account for regional differences is construction costs. The factor will be applied to the modeled and miscellaneous construction costs to determine and amount that should be added, or subtracted, to account for local variations in construction costs. The default factor is 1.0. The additive adjustment is calculated by subtracting 1.0 from the value entered in this field. This field is useful for using national average data in the line item and miscellaneous construction cost models and then altering the results based on regional differences.
-
-An example of this object in an IDF is:
-
-```idf
-ComponentCost:Reference,
-  683060.000, !- Reference Building Line Item Costs {$}
-  467.0, !- Reference Building Miscellaneous Cost per Conditioned Area {$/m2}
-  0.060, !- Reference Building Design and Engineering Fees {dimensionless}
-  0.070, !- Reference Building Contractor Fee {dimensionless}
-  0.100, !- Reference Building Contingency
-  0.04,  !- Reference Building Permits, Bonding and Insurance {dimensionless}
-  0.0075,!- Reference Building Commissioning Fee {dimensionless}
-  1.136; !- Reference Building Regional Adjustment Factor {dimensionless}
-```
-
-
-
-### Economics Cost Estimate Reporting
-
-Cost estimate results are only output to tabular reports; they are not available in the standard output file (.eso). The results are included in the Construction Cost Estimate Summary table by request using the object Output:Table:SummaryReports object with the Component Cost Economics Summary option selected. The figure below shows an example of summary output using html style for tabular reporting. A second table is produced that provides the line item details with one line for every line item object. Per-area cost modeling and cost normalization are based on total conditioned floor area which is also provided in the tabular report.
-
-![FigureOutput](media/image616.png)
-
-Figure 163. Economics Cost Modeling
-
-“Line Item Subtotal� is the sum of items explicitly modeled in the cost estimate. For the reference building, this value is input by the user. For the current building, this value is the sum of line items which are detailed in Cost Line Item Details table that follows.
-
-“Misc. Cost� is the product of the user-defined Miscellaneous Cost Model (per Square Meter) and the conditioned floor area.
-
-“Regional Adjustment� is the produce of the user-defined Regional Adjustment Factor and the conditioned floor area.
-
-“Design Fee� is the product of the user-defined Design and Engineering Fee Fraction and the subtotal for construction costs (which includes the Line Item Subtotal, Misc. Cost, and Regional Adjustment).
-
-“Contractor Fee� is the product of the user-defined Contractor Fee Fraction and the subtotal for construction costs (which includes the Line Item Subtotal, Misc. Cost, and Regional Adjustment).
-
-“Contingency� is the product of the user-defined Contingency Fraction and the subtotal for construction costs (which includes the Line Item Subtotal, Misc. Cost, and Regional Adjustment).
-
-“Permits, Bonds, and Insurance� is the product of the Permits, Bonding, Insurance Fraction and the subtotal for construction costs (which includes the Line Item Subtotal, Misc. Cost, and Regional Adjustment).
-
-“Commissioning� is the product of the user-defined Commissioning Fee Fraction and the subtotal for construction costs (which includes the Line Item Subtotal, Misc. Cost, and Regional Adjustment).
-
-“Cost Estimate Total� is the sum of eight items above and represents the total project cost estimate.
-
-“Cost per Conditioned Building Area� is the Cost Estimate Total divided by the total conditioned floor area. This represents a normalized cost intensity.
-
-Life-Cycle Costing
-------------------
-
-Life-cycle costing is used with building energy simulation in order to justify energy efficiency upgrades. Many alterative building technologies that result in energy savings cost more initially, or may cost more to maintain, than traditional solutions. In order to justify selecting these energy savings technologies, it is essential to combine both initial and future costs in the decision process. Using life-cycle costs provides a framework to combine initial costs and future costs into a single combined measure, called the “present value.� Present value is a metric that combines all costs and reduces (or discounts) those costs that occur in the future. Discounting future costs is based on the principal of the time value of money.
-
-The calculations are based on discounting the future values according to normal life-cycle costing techniques as described in NIST Handbook 135 “Life-Cycle Costing Manual for the Federal Energy Management Program.�
-
-The following is a list of life-cycle costing related objects that provide a way to describe the parameters and costs associated with the life-cycle of a building or building system:
-
-- LifeCycleCost:Parameters
-
-- LifeCycleCost:RecurringCosts
-
-- LifeCycleCost:NonrecurringCost
-
-- LifeCycleCost:UsePriceEscalation
-
-- LifeCycleCost:UseAdjustment
-
-The utility costs (see UtilityCost:Tariff) and first costs (see ComponentCost:LineItem) are  calculated by EnergyPlus are used along with other current and future costs input using the LifeCycleCost:RecurringCosts and LifeCycleCost:NonrecurringCost objects and these are combined these into the present value life-cycle cost metric. The LifeCycleCost:Parameters object establishes the set of assumptions for the analysis along with LifeCycleCost:UsePriceEscalation (often from a DataSet) and LifeCycleCost:UseAdjustment.
-
-It is important to understand that the comparison of different simulation results and their present values is not performed by EnergyPlus. Instead, EnergyPlus provides the present value calculations for a specific simulation combining the energy costs, first costs, and future costs and you need to make the comparison between the results of multiple simulations.
-
-The results of using the LifeCycleCost objects are included automatically in the tabular report file whenever the LifeCycleCost:Parameters object is present. The report appearing in the tabular report file is titled “Life Cycle Cost Report.� This report shows the costs and the timing of costs, often called “cash flows,� along with the present value in several different tables. The tabular results would show the present value of all current and future costs.
-
-The datasets file “LCCusePriceEscalationDataSetXXXX.idf� includes the energy escalation factors from the NIST Handbook 135 annual supplement for the year indicated. These are necessary to use because the expected change in price for electricity and various fuels does not change at the same rate as inflation.
-
-Life-cycle costing should not be confused with life-cycle analysis. With life-cycle costing the result is an economic evaluation of current and future expenditures in order to make a decision on alternative investments. In life cycle analysis, the environmental impact such as equivalent CO2 production involved in the materials, delivery, manufacturing, and construction are combined with environmental impacts of the building in operation and the eventual removal of the building and is used to understand the overall environmental impact or embodied energy.
-
-LifeCycleCost:Parameters
-------------------------
-
-Provides inputs related to the overall life-cycle analysis. It establishes many of the assumptions used in computing the present value. It is important that when comparing the results of multiple simulations that the fields in the LifeCycleCost:Parameters objects are the same for all the simulations. To aide in this comparison, the first table in the Life-Cycle Cost Report shows the inputs to this object. Only one LifeCycleCost:Parameters object is permitted for a file. When this object is present the tabular report file will contain the Life-Cycle Cost Report.
-
-#### Field: Name
-
-An identifying name used for the LifeCycleCost:Parameters object.
-
-#### Field: Discounting Convention
-
-The field specifies if the discounting of future costs should be computed as occurring at the end of each year, the middle of each year, or the beginning of each year. The most common discounting convention uses the end of each year. Without a specific reason, the end of each year should be used. Some military projects may specifically require using the middle of each year. The year being used starts with the base year and month and repeats every full year. All costs assumed to occur during that duration are accumulated and shown as an expense either at the beginning, middle or end of the year.  The options are:
-
-- BeginningOfYear
-
-- MidYear
-
-- EndOfYear
-
-#### Field: Inflation Approach
-
-This field is used to determine if the analysis should use constant dollars or current dollars which is related to how inflation is treated. The two options are:
-
-- ConstantDollar
-
-- CurrentDollar
-
-The default option is ConstantDollars
-
-If ConstantDollar is selected, then the Real Discount Rate input is used and it excludes the rate of inflation. If CurrentDollar is selected, then the Nominal Discount Rate input is used and it includes the rate of inflation. From NIST Handbook 135:
-
-“The constant dollar approach has the advantage of avoiding the need to project future rates of inflation or deflation. The price of a good or service stated in constant dollars is not affected by the rate of general inflation. For example, if the price of a piece of equipment is $1,000 today and $1,050 at the end of a year in which prices in general have risen at an annual rate of 5 percent, the price stated in constant dollars is still $1,000; no inflation adjustment is necessary. In contrast, if cash flows are stated in current dollars, future amounts include general inflation, and an adjustment is necessary to convert the current-dollar estimate to its constant-dollar equivalent. This adjustment is important because constant- and current-dollar amounts must not be combined in an LCCA [life cycle cost analysis].�
-
-For most analyses, using the ConstantDollar option will be easier since the effect of inflation may be ignored.
-
-#### Field: Real Discount Rate
-
-Enter the real discount rate as a decimal. For a 3% rate, enter the value 0.03. This input is used when the Inflation Approach is ConstantDollar. The real discount rate reflects the interest rates needed to make current and future expenditures have comparable equivalent values when general inflation is ignored. When Inflation Approach is set to CurrentDollar this input is ignored. If this field is blank and Inflation Approach is ConstantDollar, a warning is issued.
-
-#### Field: Nominal Discount Rate
-
-Enter the nominal discount rate as a decimal. For a 5% rate, enter the value 0.05. This input is used when the Inflation Approach is CurrentDollar. The real discount rate reflects the interest rates needed to make current and future expenditures have comparable equivalent values when general inflation is included. When Inflation Approach is set to ConstantDollar this input is ignored. If this field is blank and Inflation Approach is CurrentDollar, a warning is issued.
-
-#### Field: Inflation Rate
-
-Enter the rate of inflation for general goods and services as a decimal. For a 2% rate, enter the value 0.02. If this field is not blank and Inflation Approach is ConstantDollar, a warning is issued.
-
-#### Field: Base Date Month
-
-Enter the month that is the beginning of study period, also known as the beginning of the base period. According to NIST 135 “the base date is the point in time to which all project-related costs are discounted in an LCCA [life cycle cost analysis]. The base date is usually the first day of the study period for the project, which in turn is usually the date that the LCCA is performed. In a constant dollar analysis, the base date usually defines the time reference for the constant dollars (e.g. 1995 constant dollars). It is essential that you use the same base data and constant-dollar year for all of the project alternatives to be compared. If you set the base date to the date that the LCCA is performed, then the constant dollar basis for the analysis will be the current date, and you can use actual costs as of that date without adjusting for general inflation.�
-
-The choices are:
-
-- January
-
-- February
-
-- March
-
-- April
-
-- May
-
-- June
-
-- July
-
-- August
-
-- September
-
-- October
-
-- November
-
-- December
-
-The default value is January.
-
-This field could also be referred to as part of “the date of study.� It is used as the date for constant dollars.
-
-#### Field: Base Date Year
-
-Enter the four digit year that is the beginning of study period, such as  a year expressed in four digits like “2013�. The study period is also known as the base period. See more details in the previous field.
-
-#### Field: Service Date Month
-
-Enter the month that is the beginning of building occupancy. Energy costs computed by EnergyPlus are assumed to occur during the year following the service date. The service date must be the same or later than the Base Date. The choices are:
-
-- January
-
-- February
-
-- March
-
-- April
-
-- May
-
-- June
-
-- July
-
-- August
-
-- September
-
-- October
-
-- November
-
-- December
-
-The default value is January. According to NIST Handbook 135:
-
-“The service date is the date on which the project is expected to be implemented; operating and maintenance costs (including energy- and water-related costs) are generally incurred after this date, not before.�
-
-This field could also be referred to as part of “beneficial occupancy date.�
-
-#### Field: Service Date Year
-
-Enter the four digit year that is the beginning of occupancy, such as  two years after the previously entered year expressed in four digits like “2013�. See more details in the previous field.
-
-#### Field: Length of Study Period in Years
-
-Enter the number of years of the study period. It is the number of years that the study continues based on the start at the base date. The default value is 25 years. Only integers may be used indicating whole years.  According to NIST Handbook 135, “the study period for an LCCA is the time over which the costs and benefits related to a capital investment decision are of interest to the decision maker. Thus, the study period begins with the base date and includes both the [planning/construction] period (if any) and the relevant service period for the project. The service period begins with the service date and extends to the end of the study period.�
-
-#### Field: Tax rate
-
-Enter the overall marginal tax rate for the project costs. This does not include energy or water taxes. The single tax rate entered here is not intended to be a replacement of the complex calculations necessary to compute personal or corporate taxes; instead it is an approximate that may be used for a simple analysis assuming a constant tax rate is applied on all costs. The tax rate entered should be based on the marginal tax rate for the entity and not the average tax rate. Enter the tax rate results in present value calculations after taxes. Most analyses do not factor in the impact of taxes and assume that all options under consideration have roughly the same tax impact. Due to this, many times the tax rate can be left to default to zero and the present value results before taxes are used to make decisions. The value should be entered as a decimal value. For 15% enter 0.15. For an analysis that does not include tax impacts, enter 0.0. The default is 0.
-
-#### Field: Depreciation Method
-
-For an analysis that includes income tax impacts, this entry describes how capital costs are depreciated. According to IRS Publication 946 – How to Depreciate Property "Depreciation is an annual income tax deduction that allows you to recover the cost or other basis of certain property over the time you use the property. It is an allowance for Fair market value the wear and tear, deterioration, or obsolescence of the Intangible property.� Details on which depreciation method to choose depends on the property being depreciated and IRS Publication 946 and your accountant are the best sources of information in determining which depreciation method to choose. Only one depreciation method may be used for an analysis and is applied to all capital expenditures. Only analyses that include tax impacts need to select a depreciation method.
-
-The options are:
-
-- ModifiedAcceleratedCostRecoverySystem-3year
-
-- ModifiedAcceleratedCostRecoverySystem-5year
-
-- ModifiedAcceleratedCostRecoverySystem-7year
-
-- ModifiedAcceleratedCostRecoverySystem-10year
-
-- ModifiedAcceleratedCostRecoverySystem-15year
-
-- ModifiedAcceleratedCostRecoverySystem-20year
-
-- StraightLine-27year
-
-- StraightLine-31year
-
-- StraightLine-39year
-
-- StraightLine-40year
-
-- None
-
-Depreciation allowances reduce the actual/nominal tax dollars paid by the owner.  Thus, analyses using depreciation should be conducted in nominal dollars. For an analysis that does not include tax effects, None should be selected.
-
-The default value is None.
-
-An example of this object in an IDF:
-
-```idf
-LifeCycleCost:Parameters,
-    TypicalLCC,              !- Name
-    EndOfYear,               !- Discounting Convention
-    ConstantDollar,          !- Inflation Approach
-    0.034314,                !- Real Discount Rate
-    ,                        !- Nominal Discount Rate
-    ,                        !- Inflation
-    January,                 !- Base Date Month
-    2010,                    !- Base Date Year
-    January,                 !- Service Date Month
-    2010,                    !- Service Date Year
-    25,                      !- Length of Study Period in Years
-    0.39,                    !- Tax rate
-    StraightLine-39year;     !- Depreciation Method
-```
-
-
-LifeCycleCost:RecurringCosts
-----------------------------
-
-Recurring costs are costs that repeat over time on a regular schedule during the study period. If costs associated with equipment do repeat but not on a regular schedule, use LifeCycleCost:NonrecurringCost objects instead.  Costs related to energy usage are not included here. The UtilityCost:Tariff and other UtilityCost objects can be used to compute energy costs that are automatically included in the life-cycle cost calculations
-
-#### Field: Name
-
-The identifier used for the object. The name is used in identifying the cash flow equivalent in the output results in the Life-Cycle Cost Report.
-
-#### Field: Category
-
-Enter the category of the recurring costs. Choose the closest category. The options include:
-
-- Maintenance
-
-- Repair
-
-- Operation
-
-- Replacement
-
-- MinorOverhaul
-
-- MajorOverhaul
-
-- OtherOperational
-
-The default value is Maintenance.
-
-For recommendations on estimating other operational costs, see NIST 135 Section 4.6.3.
-
-#### Field: Cost
-
-Enter the cost in dollars (or the appropriate monetary unit) for the recurring costs. Enter the cost for each time it occurs. For example, if the annual maintenance cost is $500, enter 500 here.
-
-#### Field: Start of Costs
-
-Enter when the costs start. The First Year of Cost is based on the number of years past the Start of Costs. For most maintenance costs, the Start of Costs should be Service Period. The options are:
-
-- ServicePeriod
-
-- BasePeriod
-
-The default value is ServicePeriod.
-
-#### Field: Years From Start
-
-This field and the Months From Start field together represent the time from either the start of the Service Period, on the service month and year, or start of the Base Period, on the base month and year (depending on the Start of Costs field) that the costs start to occur. Normally, for most maintenance costs that begin in the first year that the equipment is in service the Start of Costs is the Service Period and the Years from Start will be 0. Only integers should be entered representing whole years. The default value is 0.
-
-#### Field: Months From Start
-
-This field and the Years From Start field together represent the time from either the start of the Service Period, on the service month and year, or start of the Base Period, on the base month and year (depending on the Start of Costs field) that the costs start to occur. Normally, for most maintenance costs the Start of Costs is the Service Period and the Months from Start will be 0. Only integers should be entered representing whole months. The Years From Start (times 12) and Months From Start are added together. The default value is 0.
-
-#### Field: Repeat Period Years
-
-This field and the Repeat Period Months field indicate how much time elapses between reoccurrences of the cost. For costs that occur every year, such as annual maintenance costs, the Repeat Period Years should be 1 and Repeat Period Months should be 0. Only integers should be entered representing whole years. The default value is 1.
-
-#### Field: Repeat Period Months
-
-This field and the Repeat Period Years field indicate how much time elapses between reoccurrences of the cost. For costs that occur every year the Repeat Period Years should be 1 and Repeat Period Months should be 0. For, costs that occur every eighteen months, the Repeat Period Years should be 1 and the Repeat Period Months should be 6. Only integers should be entered representing whole years. The Repeat Period Years (times 12) and Repeat Period Months are added together. The default value is 0.
-
-#### Field: Annual Escalation Rate
-
-Enter the annual escalation rate as a decimal. For a 1% rate, enter the value 0.01. This input is used when the Inflation Approach is CurrentDollar. When Inflation Approach is set to ConstantDollar this input is ignored. The default value is 0.
-
-An example of this object in an IDF:
-
-```idf
-LifeCycleCost:RecurringCosts,
-    AnnualMaint,             !- Name
-    Maintenance,             !- Category
-    2000,                    !- Cost
-    ServicePeriod,           !- Start of Costs
-    0,                       !- Years from Start
-    0,                       !- Months from Start
-    1,                       !- Repeat Period Years
-    0,                       !- Repeat Period Months
-    0;                       !- Annual escalation rate
-```
-
-
-LifeCycleCost:NonrecurringCost
-------------------------------
-
-A non-recurring cost happens only once during the study period. For costs that occur more than once during the study period on a regular schedule, use the LifeCycleCost:RecurringCost object.
-
-#### Field: Name
-
-The identifier used for the object. The name is used in identifying the cash flow equivalent in the output results in the Life-Cycle Cost Report.
-
-#### Field: Category
-
-Enter the category of the non-recurring costs. Choose the closest category. The options include:
-
-- Construction
-
-- Salvage
-
-- OtherCapital
-
-The default is Construction.
-
-For recommendations on estimating capital and salvage (residual) costs, see NIST 135 Section 4.5.
-
-#### Field: Cost
-
-Enter the non-recurring cost value. For construction and other capital costs the value entered is typically a positive value. For salvage costs, the value entered is typically a negative value which represents the money paid to the investor for the equipment at the end of the study period.
-
-#### Field: Start of Costs
-
-Enter when the costs start. The First Year of Cost is based on the number of years past the Start of Costs. For most non-recurring costs the Start of Costs should be Base Period which begins at the base month and year. The options are:
-
-- ServicePeriod
-
-- BasePeriod
-
-The default value is BasePeriod
-
-#### Field: Years From Start
-
-This field and the Months From Start field together represent the time from either the start of the Service Period, on the service month and year, or start of the Base Period, on the base month and year (depending on the Start of Cost field) that the costs start to occur. Normally, for most capital costs the Start of Costs is the Base Period and the Years from Start will be 0. These would be first costs for the building equipment or system. Salvage costs are usually shown as happening in the last year of the analysis. Only integers should be entered representing whole years. The default value is 0.
-
-#### Field: Months From Start
-
-This field and the Years From Start field together represent the time from either the start of the Service Period, on the service month and year, or start of the Base Period, on the base month and year (depending on the Start of Cost field) that the costs start to occur. Normally, for most capital costs the Start of Costs is the Base Period and the Months from Start will be 0. Only integers should be entered representing whole months. The Years From Start (times 12) and Months From Start are added together. The default value is 0.
-
-An example of this object in an IDF:
-
-```idf
-LifeCycleCost:NonrecurringCost,
-    EstimatedSalvage,        !- Name
-    Salvage,                 !- Category
-    -2000,                   !- Cost
-    ServicePeriod,           !- Start of Costs
-    20,                      !- Years from Start
-    0;                       !- Months from Start
-```
-
-
-LifeCycleCost:UsePriceEscalation
---------------------------------
-
-The LifeCycleCost:UsePriceEscalation object will commonly be part of a dataset on life cycle costs. The values for this object may be found in the annual supplement to NIST Handbook 135 in Tables Ca-1 to Ca-5. A dataset file comes with EnergyPlus in the DataSet directory and includes the LCCusePriceEscalationDataSetXXXX.idf file which includes the value for the supplement to NIST 135 from the year indicated. The object provides inputs for the escalations of energy and water costs assuming that they change differently than inflation. According to the NIST 135 supplement the values are “present projected fuel price indices for the four Census regions and for the United States. These indices, when multiplied by annual energy costs computed at base-date prices provide estimates of future-year costs in constant base-date dollars. Constant-dollar cost estimates are needed when discounting is performed with a real discount rate (i.e., a rate that does not include general price inflation).�
-
-The LCCusePriceEscalationDataSetXXXX.idf is periodically updated by the EnergyPlus development team using data available from NIST along with a spreadsheet to convert that data into an IDF dataset file. The NIST 135 annual supplement is available from NIST or through US DOE FEMP program.
-
-http://www1.eere.energy.gov/femp/program/lifecycle.html
-
-If requested, NIST personnel will provide a file called ENCOSTxx.TXT which contains the data used to create Table Ca-1 to Table Ca-5 in the supplement. To convert the data in the ENCOSTxx.TXT file to an IDF file, open the ENCOSTxx.TXT file in a text editor and copy the entire contents into the first tab called “Step 1� of the conversion spreadsheet. The conversion spreadsheet file named ConvertENCOSTtoEnergyPlusLifeCycleCost.xls is available upon request from the EnergyPlus development team. The “Step 2� tab separates the data into columns. The “Step 3� tab computes ratios that are the same as Table Ca-1 to Table C1-6 in the supplement. Checking these values against what appears in the printed supplement is recommended. The “Step 4� and “Step 5� tabs rearrange the data and the “Step 6� tab shows the data in a format that can be easily copied and pasted into a new idf dataset file. The final step requires using your text editor to replace the fuel names with those used by EnergyPlus. The replacement names are listed on the “FuelNameConversion� tab.
-
-#### Field: Name
-
-The identifier used for the object. The name usually identifies the location (such as the state, region, country or census area) that the escalations apply to. In addition the name should identify the building class such as residential, commercial, or industrial and the use type such as electricity, natural gas, or water.
-
-#### Field: Resource
-
-Enter the resource such as:
-
-- Electricity
-
-- FuelOil\#1
-
-- NaturalGas
-
-- PropaneGas
-
-- FuelOil\#2
-
-- Coal
-
-- Steam
-
-- Gasoline
-
-- Diesel
-
-- Water
-
-#### Field: Escalation Start Year
-
-This field and the Escalation Start Month define the time that corresponds to “Year 1 Escalation� such as a year expressed in four digits like “2013�, when the escalation rates are applied. This field and the Escalation Start Month define the time that escalation begins.
-
-#### Field: Escalation Start Month
-
-This field and the Escalation Start Year define the time that corresponds to “Year 1 Escalation� such as  a year expressed in four digits such as “2013�, when the escalation rates are applied. This field and the Escalation Start Year define the time that escalation begins.
-
-The choices are:
-
-- January
-
-- February
-
-- March
-
-- April
-
-- May
-
-- June
-
-- July
-
-- August
-
-- September
-
-- October
-
-- November
-
-- December
-
-The default value is January. According to NIST Handbook 135:
-
-#### Field: Year 1 Escalation
-
-The escalation in price of the energy or water use for the first year expressed as a decimal.
-
-#### Field: Year n Escalation
-
-The escalation in price of the energy or water use for the n-th year expressed as a decimal. This object is extensible and often includes 25 to 50 years of projected values.
-
-If the number of years in LifeCycleCost:UsePriceEscalation is less than the number of years in the analysis period, the remaining years will assume no escalation. Normal inflation will be the only affect for these years.
-
-An example of this object in an IDF:
-
-```idf
-LifeCycleCost:UsePriceEscalation,
-    NorthEast  Residential-Electricity,  !- Name
-    Electricity,                         !- Resource
-    2010,                                !- Escalation Start Year
-    January,                             !- Escalation Start Month
-    0.9374,                              !- Year 1 Escalation
-    0.9790,                              !- Year 2 Escalation
-    1.0138,                              !- Year 3 Escalation
-    1.0127,                              !- Year 4 Escalation
-    1.0096,                              !- Year 5 Escalation
-    1.0177,                              !- Year 6 Escalation
-    1.0279,                              !- Year 7 Escalation
-    1.0334,                              !- Year 8 Escalation
-    1.0327,                              !- Year 9 Escalation
-    1.0382,                              !- Year 10 Escalation
-    1.0454,                              !- Year 11 Escalation
-    1.0494,                              !- Year 12 Escalation
-    1.0564,                              !- Year 13 Escalation
-    1.0587,                              !- Year 14 Escalation
-    1.0549,                              !- Year 15 Escalation
-    1.0566,                              !- Year 16 Escalation
-    1.0630,                              !- Year 17 Escalation
-    1.0707,                              !- Year 18 Escalation
-    1.0857,                              !- Year 19 Escalation
-    1.0953,                              !- Year 20 Escalation
-    1.1063,                              !- Year 21 Escalation
-    1.1165,                              !- Year 22 Escalation
-    1.1227,                              !- Year 23 Escalation
-    1.1292,                              !- Year 24 Escalation
-    1.1349,                              !- Year 25 Escalation
-    1.1414,                              !- Year 26 Escalation
-    1.1480,                              !- Year 27 Escalation
-    1.1550,                              !- Year 28 Escalation
-    1.1617,                              !- Year 29 Escalation
-    1.1686;                              !- Year 30 Escalation
-```
-
-
-LifeCycleCost:UseAdjustment
----------------------------
-
-Used by advanced users to adjust the energy or water use costs for future years. This should not be used for compensating for inflation but should only be used to increase the costs of energy or water based on assumed changes to the actual use of water or energy, such as due to changes in the future function of the building or the impact of future adjacent buildings on energy use. This object is not commonly used and should be used with caution. The adjustments begin at the start of the service period.
-
-#### Field: Name
-
-The identifier used for the object.
-
-#### Field: Resource
-
-Enter the resource such as:
-
-- Electricity
-
-- NaturalGas
-
-- Steam
-
-- Gasoline
-
-- Diesel
-
-- Coal
-
-- FuelOil \#1
-
-- FuelOil \#2
-
-- Propane
-
-- Water
-
-#### Field: Year 1 multiplier
-
-The multiplier to be applied to the end use cost for the first year in the service period. The total utility costs for the selected end use is multiplied by this value. For no change enter 1.0.
-
-#### Field: Year N multiplier
-
-The multiplier to be applied to the end use cost for each following year. The total utility costs for the selected end use is multiplied by this value. For no change enter 1.0.  This object is extensible and often includes 25 to 50 years of values.
-
-An example of this object in an IDF:
-
-```idf
-LifeCycleCost:UseAdjustment,
-    ElecAdjustment,          !- Name
-    Electricity,             !- Resource
-    1.0000,                  !- Year 1 Multiplier
-    1.0022,                  !- Year 2 Multiplier
-    1.0023,                  !- Year 3 Multiplier
-    1.0024,                  !- Year 4 Multiplier
-    1.0025,                  !- Year 5 Multiplier
-    1.0026,                  !- Year 6 Multiplier
-    1.0027;                  !- Year 7 Multiplier
-```
-
-
-### CurrencyType
-
-By default, the predefined reports related to economics use the $ symbol. If a different symbol should be shown in the predefined reports to represent the local currency this object can be used. If the object is not used, the $ sign is used in the reports. Only one CurrencyType object is allowed in the input file.
-
-#### Field: Monetary Unit
-
-The commonly used three letter currency code for the units of money for the country or region. Based on ISO 4217 currency codes.  Common currency codes are USD for the U.S. Dollar represented with ‘$’ and EUR for Euros represented with ‘€’.  The three letter currency codes can be seen at the following web sites (as of 2008):
-
-http://www.iso.org/iso/support/faqs/faqs_widely_used_standards/widely_used_standards_other/currency_codes/currency_codes_list-1.htm
-
-http://www.xe.com/symbols.php
-
-When a three letter currency code is specified, the HTML file will use either an ASCII character if available or one or more UNICODE characters. Since not all browsers and all fonts used by browsers completely support UNICODE, not all currency symbols may be rendered correctly. If a box or a box with four small letters appears, this indicates that the browser and its fonts do not support a specific UNICODE character.
-
-For text reports, an ASCII representation of the currency code will be used. Since ASCII is much more limited than UNICODE, many times the three letter currency code will be shown in the reports.
-
-Since forms of currency change, please contact EnergyPlus support if a new currency code and symbol are needed.
-
diff --git a/doc/src/docs/InputOutputReference/04-Parametrics.md b/doc/src/docs/InputOutputReference/04-Parametrics.md
deleted file mode 100644
index da3f2a2ef68..00000000000
--- a/doc/src/docs/InputOutputReference/04-Parametrics.md
+++ /dev/null
@@ -1,384 +0,0 @@
-Parametric Objects
-==================
-
-Group – Parametrics
--------------------
-
-In order to assess a group of alternatives, the Parametric objects can be used in a single file as an alternative of maintaining a group of files with small differences. Updating portions of the multiple files that do not change between permutations becomes tedious and error prone and may lead to incorrect conclusions concerning the energy savings of specific measures. The ParametricPreprocessor.exe program (described in the AuxiliaryPrograms document) interprets the following objects in a single file and creates the group of files automatically. The objects in the group are:
-
-- Parametric:SetValueForRun
-
-- Parametric:Logic
-
-- Parametric:RunControl
-
-- Parametric:FileNameSuffix
-
-A simple example of part of an IDF file is shown below:
-
-
-
-```idf
-  Parametric:SetValueForRun,
-    $insDepth,                  !- Parameter Name
-    0.0508,                     !- Value 1
-    0.0762,                     !- Value 2
-    0.1016,                     !- Value 3
-    0.1270;                     !- Value 4
-
-
-  Material,
-    IN1,                     !- Name
-    VeryRough,               !- Roughness
-    =$insDepth,              !- Thickness {m}
-    2.3000000E-02,           !- Conductivity {W/m-K}
-    24.00000,                !- Density {kg/m3}
-    1590.000,                !- Specific Heat {J/kg-K}
-    0.9000000,               !- Thermal Absorptance
-    0.5000000,               !- Solar Absorptance
-    0.5000000;               !- Visible Absorptance
-```
-
-
-
-
-In this example, the parameter \$insDepth is used in the Material object to describe the thickness of the material, in this case insulation.  For the first simulation, $insDepth is set to 0.0508 (2 inches) shown as the first value in the Parametric:SetValueForRun object. This value is then substituted in where ever the $insDepth is shown in the file, in this example, in the Material object. The simulation would use this first value and produce a set of results based on this insulation thickness. The second simulation would use the second value of the Parametric:SetValueForRun object of 0.0762 (3 inches) for the thickness of the insulation described in the Material object. This would then be simulated with a second set of results. This would be repeated a third time with 0.1015 (4 inches) and 0.1270 (5 inches) of insulation.
-
-A new IDF file is created for each of these simulations and is named the original name of the file plus either a number or a user defined suffix (if Parametric:FileNameSuffix is used). Looking at how these created IDF files show the substituted values can help understand problems that may occur.
-
-The “=$insDepth� is a simple substation but could also be a more complex expression involving operators and predefined functions such as
-
-  =$insDepth \* 1.1 + 0.0004 \* SQRT(12)
-
-Many sets of simulations can be defined just using different Parametric:SetValueForRun objects but for more advanced sets of parametric runs, the Parametric:Logic object can be used to perform additional calculations, logical operations, and to exclude entire objects in the file. The Parametric:RunControl allows individual runs to be performed or not. The Parametric:FileNameSuffix object controls the naming of the resulting sets of output files.
-
-### Expressions
-
-Expressions can occur anywhere in the IDF file as a field value if the expression begins with an equals sign (=) and can also occur in assignment statements in the Parametric:Logic object. The operators include: +, -, \*, /, ^ (exponent), && (and), || (or), ==, &gt;, &lt;, &lt;=, &gt;=,  &lt;&gt;, and //. These are computed using standard operator precedence rules. The parenthesis are used to execute sub-expressions with higher precedence. Some built in functions, such as ABS, ACOS, ASIN, ATAN, COS, EXP, INT, LEN, LOG, MOD, NOT, SIN, SQRT, TAN are supported in expressions. Theses built in functions all take a single argument.
-
-### Processing Order
-
-The order that the parameters are processed is important to understand their values. Like other objects in EnergyPlus, the order that they occur in the file is not important.  The order of evaluation is:
-
-1)    Parameter values are based on Parametric:SetValueForRun
-
-2)    All lines of the Parametric:Logic object are evaluated
-
-3)    All embedded expressions in the file are evaluated
-
-### Parametric:SetValueForRun
-
-The core parametric object is Parametric:SetValueForRun which sets the parameters value to different values depending on which run is being simulated.
-
-For example
-
-```idf
-Parametric:SetValueForRun
-  $ConstructionToUse,  !- Parameter Name
-  TiltUpConcreteWall,  !- Value for run 1
-  BlockWall,           !- Value for run 2
-  SteelFrameWall,      !- Value for run 3
-  WoodFrameWall;       !- Value for run 4
-
-
-Parametric:SetValueForRun
-  $WallRValue,           !- Parameter Name
-  5,                     !- Value for run 1
-  8,                     !- Value for run 2
-  11,                    !- Value for run 3
-  17;                    !- Value for run 4
-```
-
-
-Using Parametric:SetValueForRun, the value is set based on the which run number is currently being simulated. Multiple objects can be used and a set of parameter values would be defined for a given simulation. For example, the 3rd simulation would assign the "Value 3" value, 11, to the parameter \$WallRValue and the “Value 3� value, “SteelFrameWall� to $ConstructionToUse. Since many Parametric:SetValueForRun objects can be used at once, all of the  3rd values would be assigned to the appropriate parameters. In IDF Editor, this object will appear as a table of values with each row being all the parameter values for a specific simulation and each column belonging to a specific parameter.
-
-#### Field: Parameter Name
-
-The name of the parameter. It must begin with the dollar sign character, and the second character must be a letter. The parameter name, unlike a typical EnergyPlus name, cannot contain spaces or any characters other than letters and numerals.
-
-#### Field: Value for run n
-
-The value that should be substituted for the parameter on the n-th simulation. If multiple Parametric:SetValueForRun objects exist and they have different number of fields, the last field value will be used for the remaining field values. This means that to set all values the same, only the first value needed to be entered.
-
-### Parametric:Logic
-
-The approach of using parameters and expressions, by itself, is very flexible and allows for many possible parametric simulations but it does not allow for objects to be included for some parametric cases and not others. For example, you might want an overhang on a window in some parametric runs and not others. The Parametric:Logic object can help in that scenario.
-
-A single Parametric:Logic object is allowed per file. It has a freeform syntax including IF and SELECT blocks with each field in the object representing a single "line" of code. Essentially, this logic object looks like simple programming code.
-
-```idf
-Parametric:Logic,
-  Main,                            !- name
-  IF $insDepth &lt; 0.1,              !- parametric logic line 1
-     DISABLE “MaterialWallBoard�,  !- parametric logic line 2
-     DISABLE “MaterialExtFinish�,  !- parametric logic line 3
-  ENDIF;                           !- parametric logic line 4
-```
-
-
-In addition, lines could contain assignment statements in the form of
-
-parameter  = expression such as the second control line in the following example.
-
-```idf
-Parametric:Logic,
-  Main,                              !- name
-  PARAMETER $THICKNESS,              !- parametric logic line 1
-  $THICKNESS = 0.01 * $CMDEPTH,      !- parametric logic line 2
-  IF $THICKNESS > 0.5,               !- parametric logic line 3
-     DISABLE “MaterialWallBoard�,    !- parametric logic line 4
-     DISABLE “MaterialExtFinish�,    !- parametric logic line 5
-  ENDIF;                             !- parametric logic line 6
-```
-
-The statements include PARAMETER, IF, ELSE, ELSEIF, ENDIF, SELECT, CASE, DEFAULT, ENDSELECT, ENABLE, DISABLE, and REMARK. Nested IF and SELECT statements are allowed.  All objects are enabled until they are specifically disabled using the DISABLE statement and could be later re-enabled with ENABLE. An object that is named with the DISABLE statement would not appear in that simulation run.
-
-The PARAMETER statement declares the name of the parameter. It is necessary that every parameter used in the Parametric:Logic object be initialized using the PARAMETER statement unless the parametes are created using the Parametric:SetValueForRun object. Requiring explicit parameter declaration reduces errors in software programming. Parameter names would not be case sensitive.
-
-The DISABLE and ENABLE commands can have one or two arguments. If a second argument is present it is the kind of object.
-
-```
-DISABLE “MaterialWallBoard� “Material�,    !- parametric control line 4
-```
-
-The following sections describe each type of statement in more detail.
-
-#### IF ENDIF Block
-
-As previously shown, the simplest IF block is in the form of
-
-```idf
-IF <conditional-expression>
-  <true-block-of-statements>
-ENDIF
-```
-
-The &lt;conditional-expression&gt; usually contains a logical comparison operator such as:
-
-*   == equal
-
-*   &gt; greater than
-
-*   &lt; less than
-
-*   &lt;= less than or equal to
-
-*   &gt;= greater than or equal to
-
-*   &lt;&gt; not equal to
-
-
-The &lt;true-block-of-statements&gt; can contain other statements including other lines of IF and ENDIF. These statement are only executed when the &lt;conditional-expression&gt; evaluates to true. If the &lt;conditional-expression&gt; is false, none of the statements before the ENDIF are executed and instead execution begins again with the statement after the ENDIF statement.
-
-#### IF ELSE  ENDIF Block
-
-Another form of the IF block can contain the ELSE statement:
-
-```idf
-IF <conditional-expression>
-  <true-block-of-statements>
-ELSE
-  <false-block-of-statements>
-ENDIF
-```
-
-Like the simpler IF ENDIF form the &lt;conditional-expression&gt; is computed and the &lt;true-block-of-statements&gt; are executed if it is true. The additional feature of this form is that if the &lt;conditional-expression&gt; is false, the &lt;false-block-of-statements&gt; is executed instead of the &lt;true-block-of-statements&gt;.
-
-#### IF ELSEIF ELSE ENDIF Block
-
-The most complex form of the IF block contains both ELSEIF statement (or statements)  and the ELSE statement:
-
-```idf
-IF <conditional-expression-1>
-  <true-block-of-statements-1>
-ELSEIF <conditional-expression-2>
-  <true-block-of-statements-2>
-ELSEIF <conditional-expression-2>
-  <true-block-of-statements-2>
-ELSE
-  <false-block-of-statements>
-ENDIF
-```
-
-
-This form allows more complex logic to be expressed. If the &lt;conditional-expression-1&gt; is true then &lt;true-block-of-statements-1&gt; executed and when that is complete, execution resumes after the ENDIF statement. If &lt;conditional-expression-1&gt; is false then the ELSEIF &lt;conditional-expression-2&gt; is evaluated and if that is true then &lt;true-block-of-statement-2&gt; is executed. On the other hand, if &lt;conditional-expression-2&gt; is  false, then the next ELSEIF conditional expression is evaluated following the same patter if another ELSEIF is present, otherwise, the &lt;false-block-of-statements&gt; after the ELSE are executed. Another way of thinking of this block is that the conditional expressions are evaluated from the top to the bottom until one is found to be true and then the associated block of statements are executed. If none of the conditional expressions is true, the &lt;false-block-of-statements&gt; are executed.
-
-#### SELECT CASE DEFAULT ENDSELECT Block
-
-The SELECT block is related to the IF block but is for the specific case of trying to match a variable with several specific values. The form of the SELECT block is:
-
-```idf
-SELECT <expression>
-CASE <constant-1>
-  <case-block-of-statements-1>
-CASE <constant-2>
-  <case-block-of-statements-2>
-CASE <constant-3>
-  <case-block-of-statements-3>
-DEFAULT
-  <default-block-of-statements>
-ENDSELECT
-```
-
-
-With any number of CASE statements. The &lt;expression&gt; is evaluated and compared to the constants with each CASE statement. If a match is found the corresponding &lt;case-block-of-statements&gt; are executed otherwise if no match if found the &lt;default-block-of-statements&gt; is excecuted. One one matching CASE statement for each SELECT block is executed. An example of how this works is shown below:
-
-```idf
-Parametric:SetValueForRun,
-  $EndMonth,
-  2;
-
-
-Parametric:Logic,
-  Main2,
-  PARAMETER $EndDay,
-  SELECT $EndMonth,
-   CASE 1,
-    $EndDay = 31,
-   CASE 2,
-    $EndDay = 28,
-   CASE 3,
-    $EndDay = 31,
-   CASE 4,
-    $EndDay = 30,
-   CASE 5,
-    $EndDay = 31,
-   CASE 6,
-    $EndDay = 30,
-   CASE 7,
-    $EndDay = 31,
-   CASE 8,
-    $EndDay = 31,
-   CASE 9,
-    $EndDay = 30,
-   CASE 10,
-    $EndDay = 31,
-   CASE 11,
-    $EndDay = 30,
-   CASE 12,
-    $EndDay = 31,
-   DEFAULT,
-    $EndDay = 30,
-   ENDSELECT;
-```
-
-
-With this example the $EndDay value would be set to 28.
-
-#### ENABLE DISABLE
-
-The ENABLE and DISABLE statements specifically are for removing (and not removing) other objects that appear in the EnergyPlus IDF file. It has two syntaxes:
-
-```idf
-DISABLE <objectname>
-```
-
-and
-
-```idf
-DISABLE <objectname>, <kind-of-object>
-```
-
-The DISABLE statement removes the object identified with either &lt;objectname&gt; or the combination of &lt;objectname&gt; and &lt;kind-of-object&gt; if the &lt;objectname&gt; is not unique in the EnergyPlus input file. By default, all objects are enabled in the input file. Objects need to be specifically disabled using the DISABLE statement. After an object is disabled in can later be re-enabled with the ENABLE statement which has similar syntax.
-
-```idf
-DISABLE <objectname>
-```
-
-and
-
-```idf
-DISABLE <objectname>, <kind-of-object>
-```
-
-
-```idf
-  Parametric:Logic,
-    Main,
-    DISABLE  "SOUTH WALL OVERHANG";
-
-
-  Shading:Zone:Detailed,
-    SOUTH WALL OVERHANG,     !- Name
-    ZONE SURFACE SOUTH,      !- Base Surface Name
-    SCH 2,                   !- Transmittance Schedule Name
-    4,                       !- Number of Vertices
-    0.0,-1.0,3.0,  !- X,Y,Z ==> Vertex 1 {m}
-    0.0,0.0,3.0,  !- X,Y,Z ==> Vertex 2 {m}
-    4.0,0.0,3.0,  !- X,Y,Z ==> Vertex 3 {m}
-    4.0,-1.0,3.0;  !- X,Y,Z ==> Vertex 4 {m}
-```
-
-
-An object that is named with the DISABLE statement would not appear in that simulation run.
-
-#### REMARK
-
-The REMARK statement is simply a way to include a comment in the Parametric:Logic fields. The text that follows the REMARK statement is ignored.
-
-#### OBJECT DEFINITION
-
-The definition of the Parametric:Logic object is shown below:
-
-#### Field: Name
-
-The name of the Parametric:Logic object.
-
-#### Field: Parametric Logic Line n
-
-The line that contains one statement in one of the following forms:
-
-* &lt;parameter&gt; = &lt;expression&gt;
-
-* PARAMETER &lt;parameter&gt;
-
-* IF &lt;expression&gt;
-
-* ELSEIF &lt;expression&gt;
-
-* ELSE
-
-* ENDIF
-
-* SELECT &lt;expression&gt;
-
-* CASE &lt;constant&gt;
-
-* DEFAULT
-
-* ENDSELECT
-
-* ENABLE &lt;constant&gt;
-
-* ENABLE &lt;constant&gt; &lt;constant&gt;
-
-* DISABLE &lt;constant&gt;
-
-* DISABLE &lt;constant&gt; &lt;constant&gt;
-
-* REMARK &lt;text to ignore&gt;
-
-### Parametric:RunControl
-
-The following Parametric:RunControl object controls which runs are simulated. The series of entries indicate if the run should be performed or not. This object is optional and if it is not included all runs are performed.
-
-#### Field: Name
-
-The name of the optional Parametric:RunControl object.
-
-#### Field: Perform run n
-
-The value of the field can be either a yes or no.  It cannot contain a parameter.
-
-### Parametric:FileNameSuffix
-
-The file name of the IDF files that are created for each run and the output files for each run are based on the name of the file plus a “suffix�. The suffixes can be defined using the Parametric:FileNameSuffix object or if the object is missing will default to the run number.
-
-#### Field: Name
-
-The name of the optional Parametric:FileNameSuffix object.
-
-#### Field: Suffix for file name in run n
-
-The value of the field is added to the IDF file name to create the resulting IDF file and output files.  It cannot contain a parameter.
-
diff --git a/doc/src/docs/InputOutputReference/05-InputForOutput.md b/doc/src/docs/InputOutputReference/05-InputForOutput.md
deleted file mode 100644
index 72f884dabce..00000000000
--- a/doc/src/docs/InputOutputReference/05-InputForOutput.md
+++ /dev/null
@@ -1,2333 +0,0 @@
-Input for Output
-================
-
-Several items are used to specify what will appear in the output file(s). The output is described in the next section of this document.
-
-Group – Reports
----------------
-
-### Variable Dictionary Reports
-
-One of the most important outputs for EnergyPlus is the Variable Dictionary reports – these contain the key variable names for each simulation. This single input object is used to produce two important reports that are used to identify the specific output variables and meters available for a specific EnergyPlus model.  Two output files are produced (**eplusout.rdd & eplusout.mdd**) that list the names of the output variables and meters for that simulation.  You may need to run your simulation once and produce these files before you ask for specific output variables (**rdd**) or meters (**mdd**) (see Output:Variable and Output:Meter objects). Variables available, to some extent, depend on the simulation input. Variables are “set up� during the initial “get input� processing done within the modules. Therefore, an item that is specific to a certain type of coil would not be available if that coil were not used during the simulation. This command will produce a list of variables available for reporting.
-
-#### Field: Key Field
-
-For this field there are two choices: **IDF** and **regular**. The regular option is the default and produces a listing that shows the type of variable: Zone or HVAC, Average or Sum. “**Zone**� variables are calculated and can be reported after each Zone/Heat Balance timestep (ref: Timesteps input object). “**HVAC**� variables are calculated and can be reported with each variable HVAC timestep. “**Average**� variables will be averaged over the time interval being reported whereas “**Sum**� variables are summed over that time interval. (Meter variables are always summed.) Units for the variable are shown in “[}�.
-
-#### Field: Sort Option
-
-For this field there are two choices: **Name** and **Unsorted**. By default, the listing of available reporting variables are unsorted – listed in the streaming order that EnergyPlus generates them. Or, you can have them sorted by name.
-
-Examples of the options for this object follow:
-
-```idf
-Output:VariableDictionary,regular;
-```
-
-Results of this are shown in the Output Details document under the **eplusout.rdd** (output variables) and **eplusout.mdd** (meter variables) files.
-
-The eplusout.mdd file has a similar format for meters:
-
-#### Variable Dictionary Report in IDF Format
-
-The common workflow process of examining Variable Dictionary Reports and then adding reporting requests to an IDF file can be facilitated by using the following alternate form (Report Name = IDF) of the input object that requests the reports.
-
-```idf
-Output:VariableDictionary, IDF;
-```
-
-A sorted request would appear similarly:
-
-```idf
-Output:VariableDictionary, IDF, Name;
-```
-
-### Surface Reports
-
-There are two specific objects for surfaces: **Output:Surfaces:List** and **Output:Surfaces:Drawing** – as the names imply, the list reports are simple text reports that are contained in one of the output files whereas the drawing reports will create files that are used in other graphic tools.
-
-These objects and their use is described in the following:
-
-### Output:Surfaces:List
-
-Examples of using the Output:Surfaces:List object follow:
-
-#### Lines Data Report
-
-An example input object for this report follows.
-
-```idf
-Output:Surfaces:List, Lines;
-```
-
-The above IDF line will produce a simple file of line segments that constitute the surfaces in the IDF file. This file is the  “lines� report (**eplusout.sln**) and is decribed in more detail in the Output Details and Examples document.
-
-#### Field: Report Specifications
-
-An extra option of entering “IDF� in this field directs the Lines report to produce coordinates transformed into Surface Geometry (Lower Left Corner, CounterClockwise, WorldCoordinates).  An example of this follows.
-
-```idf
-Output:Surfaces:List, Lines, IDF;
-```
-
-The result is put on the **eplusout.sln** file and is nearly ready for putting into a IDF. Again, it is described in more detail in the Output Details and Examples document.
-
-#### Detailed Surface Data Report
-
-An example input object for this report follows.
-
-```idf
-Output:Surfaces:List, Details;
-```
-
-This report (in **eplusout.eio**) contains details about each surface – including surface name, associated zone, area, approximate height and width, tilt, outward facing angle. Specific details on this report can be found in the Output Details and Examples document.
-
-#### Vertices Data Report
-
-An example input object for this report follows.
-
-```idf
-Output:Surfaces:List, Vertices;
-```
-
-This report (in **eplusout.eio**) contains the vertices of each surface along with surface name and other information. Specific details on this report can be found in the Output Details and Examples document.
-
-#### Detailed Surface Data With Vertices Report
-
-An example input object for this report follows.
-
-```idf
-Output:Surfaces:List, DetailsWithVertices;
-```
-
-This report (in **eplusout.eio**) is the combination of the two preceding reports (Details and Vertices). Specific details on this report can be found in the Output Details and Examples document.
-
-#### View Factor Information Report
-
-An example input object for this report follows.
-
-```idf
-Output:Surfaces:List, ViewFactorInfo;
-```
-
-This report (in **eplusout.eio**) provides details about the thermal radiation exchange view factors and interchange factors.  Specific details on this report can be found in the Output Details and Examples document.
-
-#### DecayCurvesfromZoneComponentLoads
-
-An example input object for this report follows.
-
-```idf
-Output:Surfaces:List, DecayCurvesfromZoneComponentLoads;
-```
-
-This report (in **eplusout.eio**) provides an intermediate calculation used, called a decay curve,  in the Zone Component Loads Summary report for the estimate of the sensible-delayed column values. A decay curve is created for each surface in a zone by introducing a radiant pulse. Each value in each row of the report corresponds to a zone time step from the time the pulse was introduced. See Zone Component Load Summary described in object Output:Table:SummaryReports for more detailed information.
-
-### Output:Surfaces:Drawing
-
-Examples of using the Output:Surfaces:Drawing object follow:
-
-#### DXF Surface Report
-
-Examples input objects follow.
-
-```idf
-Output:Surfaces:Drawing, DXF;
-Output:Surfaces:Drawing, DXF, RegularPolyline;
-Output:Surfaces:Drawing, DXF, Triangulate3DFace, mycolorscheme;
-```
-
-The above IDF specification will produce a DXF file (**eplusout.dxf**) of the surfaces in the IDF file.  Only one DXF report can be produced. More specifics on this report can be found in the Output Details and Examples document.
-
-#### Field: Report Specifications 1
-
-As indicated in the example, you can select among three different ways that surfaces with more than four sides will appear in the DXF file. These are:
-
-- ThickPolyline – surface with &gt;4 sides will be represented as a “thick� line in the appropriate surface color. It will look like a hole in the drawing with a thicker edge.
-
-- RegularPolyline – surface with &gt;4 sides will be represented as a regular line in the appropriate surface color. It will look like a hole in the drawing.
-
-- Triangulate3DFace– surface with &gt;4 sides will be “triangulated� internally within EnergyPlus.  This is only for drawing purposes and does not affect the calculations in any way.  In a line version of the DXF, it will appear that the surface is split into triangles. In a solid view, the surface will appear similar to surfaces with &lt;=4 sides. The triangulation algorithm is not perfect and warnings do result when the software cannot triangulate the surface.
-
-#### Field: Report Specifications 2
-
-This field can be used to control the color scheme in the DXF file by entering the name of an OutputControl:SurfaceColorScheme object.  Using OutputControl:SurfaceColorScheme, you can define color schemes for surface representation. This feature will let you align the colors with the software of your choice (colors don’t seem to be standard across DXF viewers).
-
-Several software programs can render this file into something viewable and are described in more detail in the Output Details and Examples document under the file name (**eplusout.dxf**).
-
-#### DXF Wire Frame Report
-
-An example input object for this report follows.
-
-```idf
-Output:Surfaces:Drawing, DXF:WireFrame;
-```
-
-The above IDF specification will produce a DXF (Drawing Exchange Format) file (**eplusout.dxf**) of the surfaces in the IDF file using the DXF “Lines� command – producing only a wire frame capable file. More specifics on this report can be found in the Output Details and Examples document. Only one DXF report can be produced.
-
-#### VRML Report
-
-Examples input objects for this report follow.
-
-```idf
-Output:Surfaces:Drawing, VRML;
-Output:Surfaces:Drawing, VRML, Triangulate3DFace;
-```
-
-The above IDF specification produces a VRML (Virtual Reality Modeling Language) file (**eplusout.wrl**) of the surfaces in the IDF file.  Only one VRML report can be produced. VRML files can be viewed in many web browsers after adding a “plug-in� and there are some stand-alone viewers as well. More specifics on this report can be found in the Output Details and Examples document.
-
-#### Field: Report Specifications 1
-
-As indicated in the example, you can select several figure types (for &gt;4 sided surfaces) in the DXF report. These are:
-
-- ThickPolyline – surface with &gt;4 sides will be represented as a “thick� line in the appropriate surface color. It will look like a hole in the drawing with a thicker edge.
-
-- RegularPolyline – surface with &gt;4 sides will be represented as a regular line in the appropriate surface color. It will look like a hole in the drawing.
-
-- Triangulate3DFace – surface with &gt;4 sides will be “triangulated� internally within EnergyPlus.  This is only for drawing purposes and does not affect the calculations in any way.  In a line version of the VRML, it will appear that the surface is split into triangles. In a solid view, the surface will appear similar to surfaces with &lt;=4 sides. The triangulation algorithm is not perfect and warnings do result when the software cannot triangulate the surface.
-
-#### Field: Report Specifications 2
-
-Color schemes are not applicable for VRML reports.
-
-### Output:Schedules
-
-This is a condensed reporting that illustrates the full range of schedule values – in the style of input: DaySchedule, WeekSchedule, and Annual Schedule.
-
-#### Field: Key Field
-
-This field should contain the word **Hourly** or **TimeStep** to obtain the respective reports.
-
-```idf
-Output:Schedules, Hourly;  ! values on hourly increments (day schedule resolution)
-Output:Schedules, TimeStep; ! will give them at the timestep of the simulation
-```
-
-This report is placed on the **eplusout.eio** file. Details of this reporting are shown in the Output Details and Examples document.  Schedule values over time can also be obtained in the EnergyPlus Standard Output (in eplusout.eso) using Output:Variable objects.
-
-### Output:Constructions
-
-#### Constructions Report
-
-This report content is added to the “**eplusout.eio**� file. It shows the calculated results related to conduction transfer functions for each construction. It also includes similar details about the windows. Specific details on this report can be found in the Output Details and Examples document.  The following input object is used to obtain the Construction report.
-
-```idf
-Output:Constructions,Constructions;
-```
-
-#### Field: Details Type 1, Details Type 2
-
-Either field can contain the word “**Constructions**� to get the constructions report.
-
-Or either field can contain the word “**Materials**� to obtain the Materials report.
-
-#### Materials Report
-
-This report content is added to the “**eplusout.eio**� file. It provides a summary of the thermal properties and thickness of the construction and window materials in the model.  Specific details on this report can be found in the Output Details and Examples document.  The following input object is used to obtain the Materials report.
-
-```idf
-Output:Constructions,Materials;
-```
-
-### Output:DaylightFactors
-
-Daylight factors are ratios of interior illuminance at a specific location to exterior horizontal illuminance. In EnergyPlus, they are pre-calculated hourly for every shadow calculation day for every exterior window of a daylight zone. The pre-calculated daylight factors are interpolated between hours and for the actual sky conditions in the time-step calculation of the daylighting performance of daylight zones.
-
-EnergyPlus reports the daylight factors for four sky types (clear, turbid clear, intermediate, and overcast) at noon time (12:00pm) for each exterior windows (base window without shading) in the eio file when the daylight factors are first calculated. This new object can report all hourly pre-calculated daylight factors. Details of the report are shown in the Output Details document.
-
-#### Field: Reporting Days
-
-This field is used to select days to report the daylight factors. Two choices are “SizingDays� and “AllShadowCalculationDays�. The SizingDays choice will output the daylight factors for only the sizing calculation days, while the AllShadowCalculationDays choice will output daylight factors for all shadow calculation days.
-
-### Output:EnergyManagementSystem
-
-This report content is added to the “eplusout.edd� file. It shows information useful for the Energy Management System. The user can select the level of detail reported to the file using the fields in this object. However, there must be some other EMS-related input objects in the input file before this report will be generated.
-
-#### Field: Actuator Availability Dictionary Reporting
-
-This field is used to control the level of output reporting related to the EMS actuators that are available for a particular model. When EnergyPlus runs with EMS, it sets up a wide array of possible actuators that the EMS could use. (To actually use them requires an EnergyManagementSystem:Actuator object). Actuator availability dictionary reporting is provided to show the user what actuators are available in a particular building model. Regardless of the level of reporting chosen here, the same set of actuators are actually available. There are three levels to choose from. The “None� choice means that no reporting of available actuators is done. The “NotByUniqueNames� level means that the output includes only the types of actuators and their control options but not the unique, user-defined names that identify a specific actuator in the model. The “Verbose� level means that the output includes all combinations of actuator types, control types, and the unique names of specific actuators. The verbose level provides all the information needed for input in an EnergyManagementSystem:Actuator input object.
-
-#### Field: Internal Variable Availability Dictionary Reporting
-
-This field is used to control the level of output reporting related to the EMS internal variables that are available for a particular model. When EnergyPlus runs with EMS, it sets up a wide array of possible internal data sources that the EMS could use. (To actually use them requires an EnergyManagementSystem:InternalVariable object). Internal variable availability dictionary reporting is provided to show the user what internal data are available. Regardless of the level of reporting chosen here, the same internal data are available. There are three levels to choose from. The “None� choice means that no reporting of available internal data is done. The “NotByUniqueNames� level means that the output includes only the types of internal data but not the unique names that identify a specific instances in the model. The “Verbose� level means that the output includes all combinations of internal variables and the unique names of specific instances. The verbose level provides all the information needed for an EnergyManagementSystem:InternalVariable input object.
-
-#### Field: EnergyPlus Runtime Language Debug Output Level
-
-This field is used to control the level of output reporting related to the execution of EnergyPlus Runtime Language, or Erl. This reporting is valuable for debugging Erl programs. When Erl programs are run inside EnergyPlus they can report error situations (such as divide by zero) or a full trace of each Erl statement. There are three levels of reporting. The “None� choice means that no reporting of Erl debug information is done. The “ErrorsOnly� choice means that Erl debugging traces are only output if the statement produces an error situation. The “Verbose� choice means that Erl debugging traces are done for each line of each Erl program. The verbose setting needs to be used with care because a large model with a long runperiod can easily create an EDD file that is too large for most computer systems (e.g. many GBs of text).
-
-An example of this object follows.
-
-```idf
-Output:EnergyManagementSystem,
-    Verbose,    ! Actuator Availability Dictionary Reporting
-    Verbose,    ! Internal Variable Availability Dictionary Reporting
-    ErrorsOnly; ! EnergyPlus Runtime Language Debug Output Level
-```
-
-### OutputControl:SurfaceColorScheme
-
-This object provides control over the colors that appear in the DXF report, by surface.  In addition, the Datasets folder contains example objects, including the “original� color scheme (prior to the 2.1 release).
-
-#### Field: Name
-
-This assigns a unique name to this colorscheme data set.  This name is used in the DXF output objects.
-
-#### Field Set: Drawing Element Type and Colorr
-
-This set of fields can range from none (accepting the default colors) up to 15 sets with individual types of building elements assigned a color number.  (drawing element types not assigned a color number will use the default color numbers)
-
-#### Field: Drawing Element &lt;\#&gt; Type
-
-This field uses a choice of the drawing types (Text, Walls, Windows, GlassDoors, Doors, Roofs, Floors, DetachedBuildingShades, DetachedFixedShades, AttachedBuildingShades, Photovoltaics, TubularDaylightDomes, TubularDaylightDiffusers, DaylightReferencePoint1, DaylightReferencePoint2) for the color number assignment in the following field.
-
-#### Field: Color for Drawing Element &lt;\#&gt;
-
-This is a color “number� from 0 to 255.  DXF display software is not standardized – you may need to play around with these numbers if you don’t like the supplied default color scheme.
-
-### OutputControl:ReportingTolerances
-
-This input object is created to allow more user control over some aspects of output reporting. Specifically, the reporting of “Time setpoint not met� hours  See thermostat reporting (ZoneControl Thermostat Outputs).
-
-#### Field: Tolerance for Time Heating Setpoint Not Met
-
-This field allows the entry of a value for the tolerance away from the heating setpoint reporting. If the zone temperature is below the heating setpoint by more than this value, the following output variables will increment as appropriate
-
-Zone Heating Setpoint Not Met Time
-
-Zone Heating Setpoint Not Met While Occupied Time
-
-This also impacts table report "Annual Building Utility Performance Summary" subtable "Comfort and Setpoint Not Met Summary".
-
-#### Field: Tolerance for Time Cooling Setpoint Not Met
-
-This field allows the entry of a value for the tolerance away from the cooling setpoint reporting. If the zone temperature is above the cooling setpoint by more than this value, the following output variables will increment as appropriate
-
-Zone Cooling Setpoint Not Met Time
-
-Zone Cooling Setpoint Not Met While Occupied Time
-
-This also impacts table report "Annual Building Utility Performance Summary" subtable "Comfort and Setpoint Not Met Summary".
-
-As seen in an IDF:
-
-```idf
-OutputControl:ReportingTolerances,.21,.21;
-```
-
-### Output:Variable
-
-This input object is used request results reporting.  As shown above in the Variable Dictionary Report section, there are many different output variables available for reporting results from EnergyPlus.  The Output:Variable object is primarily used for reporting time series data at various frequencys.
-
-Each Output:Variable object causes a specific number assignment for outputs. For example, you could request separate reporting for the outside temperature:
-
-```idf
-Output:Variable,*,Site Outdoor Air Drybulb Temperature,timestep;
-Output:Variable,*,Site Outdoor Air Drybulb Temperature,hourly;
-Output:Variable,*,Site Outdoor Air Drybulb Temperature,monthly;
-```
-
-#### Field: Key Value
-
-This alpha field can be used to make a specific reference for reporting. In addition to the generic variable names listed in the Variable Dictionary Report for the input file, variables will also have a key designator (such as Zone name or Surface name). You can reference the standard output file (**eplusout.eso**) to see just how these look.
-
-```
-41,2,ZN001:WALL004,Surface Inside Temperature [C]
-42,2,ZN001:WALL004,Surface Outside Temperature [C]
-43,2,ZN001:WALL004,Surface Int Convection Coeff[W/m2-K]
-44,2,ZN001:WALL004,Surface Ext Convection Coeff[W/m2-K]
-46,2,ZONE ONE,Zone Mean Radiant Temperature [C]
-47,2,ZONE ONE,Zone Total Internal Latent Gain Energy [J]
-51,2,ZONE ONE,Zone Lights Electric Energy [J]
-58,2,ZONE ONE,Zone Air Temperature [C]
-```
-
-For example, in the previous block, the key for the surface variables is **ZN001:WALL004** whereas the key for the zone variables is **ZONE ONE** (note that the space is required and significant for this key).
-
-You can have all keys listed in the standard output file by putting a “\*� in this field or you can have specific items listed by putting in a key value. If this field is left blank, it will use a \* as the default (i.e., you will get all variables of Variable Name).
-
-#### Field: Variable Name
-
-This alpha field is the variable name (you don’t have to put on the units) that is shown in the Variable Dictionary Report file (eplusout.rdd). This field is required.
-
-#### Field: Reporting Frequency
-
-This field specifies how often the variable will be listed in the output file. “**Detailed**� will list the value each calculation step (i.e. Zone or HVAC). “**Timestep**� will be the same as “Detailed� for Zone valued variables and will be aggregated to the Zone timestep (i.e. Timestep in Hour value) for HVAC variables. “**Hourly**� will aggregate the value to the hour. “**Daily**� will aggregate to the day (i.e. one value per day). “**Monthly**� will aggregate to the month (i.e. one value per month). “**RunPeriod**� will aggregate to the runperiod specified (each Design Day is a runperiod as is each runperiod object). Default for this field if left blank or omitted is **Hourly**.
-
-#### Field: Schedule Name
-
-The final field is a schedule name. This can be used to limit the number of lines that appear in your output file. For example, a schedule such as “ON PEAK� or “OFF PEAK� could provide a slice of values. Or, a seasonal schedule could be devised. The output variable will be active during any hour in which the schedule value is &gt;0. For daily, monthly, and environment reporting frequencies, the aggregate value will be only for active schedule hours. Summed variables will report the sum for the active hours only. Averaged variables will report the average during the active hours only. If Schedule\_Name is omitted, the output variable will be active for all hours.
-
-Other IDF examples:
-
-```idf
-Output:Variable, * , Zone Mean Air Temperature, hourly;
-Output:Variable, * , Zone Mean Radiant Temperature, timestep;
-Output:Variable, * , Zone Air System Sensible Heating Energy, hourly;
-Output:Variable, * , Zone Air System Sensible Cooling Energy, hourly;
-Output:Variable, * , Zone Air Temperature, hourly;
-Output:Variable, * , Zone Air Temperature;  ! same as previous line
-```
-
-
-### Output:Meter and Output:Meter:MeterFileOnly
-
-### Output:Meter:Cumulative and Output:Meter:Cumulative:MeterFileOnly
-
-Appropriate variables are grouped onto “meters� for reporting purposes.  (The meters available are listed in the eplusout.mdd file, see Variable Dictionary Report section.) If the “Output:Meter� input object is used, these results written out to both the **eplusout.eso** and **eplusout.mtr** files. This allows easy graphing and comparison with “normal� values (such as Zone Temperature or Outdoor Temperature). If the “Output:Meter:MeterFileOnly� input object is used, then the values results written out to only the **eplusout.mtr** file. The **eplusout.mtr** file has the same structure as the **eplusout.eso** file. A companion file, the **eplusout.mtd** file, contains a detailed list and explanation of all meters for a given run and the component values that are accumulated on each meter.
-
-The cumulative meter outputs (Output:Meter:Cumulative and  Output:Meter:Cumulative:MeterFileOnly) use the same meter names but the output is cumulative for the reporting (for each environment). That is, if the reporting frequency for the cumulative meter output is hourly, then hour 1 value will be that for hour 1, hour 2 value will be hour1 + hour2, etc. In other words, the end value for a cumulative meter reporting should be identical if you reported the value of the meter at the RunPeriod frequency.
-
-#### Field: Name
-
-Meter names applicable for the simulation are shown on the Variable Dictionary Report contained in the **eplusout.mdd** file described in the Output Details and Examples document.
-
-Meter names are of three forms:
-
-- &lt;ResourceType&gt;:&lt;name&gt;
-
-Or
-
-- &lt;EndUseType&gt;:&lt;ResourceType&gt;:&lt;name&gt;
-
-Or
-
-- &lt;EndUseSubcategory&gt;:&lt;EndUseType&gt;:&lt;ResourceType&gt;:&lt;name&gt;.
-
-The user requests reporting by either specifying the full name above (without Units) or a “wildcard� representation of that name (to obtain all meters of a type). For example, entering “Electricity:\*� for the meter name will report on all the Electricity: meters (Electricity:Facility, Electricity:Building, Electricity:Zone:Resistive Zone, Electricity:Zone:East Zone, Electricity:North Zone in the example above). Both the resource types and end-use types are set within the program by the developers. End-use subcategories are user-defined and are an input field for certain objects.
-
-To summarize the previous paragraph, you could use:
-
-```idf
-Output:Meter,Electricity:*;
-```
-
-To get the same outputs as if you had entered:
-
-```idf
-Output:Meter,Electricity:Facility;
-Output:Meter,Electricity:Building;
-Output:Meter,Electricity:Zone:South Zone;
-Output:Meter,Electricity:Zone:East Zone;
-Output:Meter,Electricity:North Zone;
-```
-
-From a three zone file that had no HVAC electricity (i.e., had only electric equipment or lighting equipment in an uncontrolled three zone building).
-
-Current resource types are shown in the table below:
-
-Table 38. Table of Metered Resource  Types
-
-<table class="table table-striped">
-<tr>
-<th>Utility/Fuel Types</th>
-</tr>
-<tr>
-<td>Electricity</td>
-</tr>
-<tr>
-<td>Gas</td>
-</tr>
-<tr>
-<td>Gasoline</td>
-</tr>
-<tr>
-<td>Diesel</td>
-</tr>
-<tr>
-<td>Coal</td>
-</tr>
-<tr>
-<td>FuelOil#1</td>
-</tr>
-<tr>
-<td>FuelOil#2</td>
-</tr>
-<tr>
-<td>Propane</td>
-</tr>
-<tr>
-<td>OtherFuel1</td>
-</tr>
-<tr>
-<td>OtherFuel2</td>
-</tr>
-<tr>
-<td>Water</td>
-</tr>
-<tr>
-<td>Steam</td>
-</tr>
-<tr>
-<td>DistrictCooling</td>
-</tr>
-<tr>
-<td>DistrictHeating</td>
-</tr>
-<tr>
-<td>ElectricityPurchased</td>
-</tr>
-<tr>
-<td>ElectricitySurplusSold</td>
-</tr>
-<tr>
-<td>ElectricityNet</td>
-</tr>
-</table>
-
-
-
-<table class="table table-striped">
-<tr>
-<th>Other Resource Types</th>
-</tr>
-<tr>
-<td>EnergyTransfer</td>
-</tr>
-</table>
-
-
-
-The end use types are shown in the following table (note that certain end use types apply only to the EnergyTransfer resource):
-
-Table 39. End Use Category Types
-
-<table class="table table-striped">
-<tr>
-<th>Utility/Fuel End Use Types</th>
-</tr>
-<tr>
-<td>InteriorLights</td>
-</tr>
-<tr>
-<td>ExteriorLights</td>
-</tr>
-<tr>
-<td>InteriorEquipment</td>
-</tr>
-<tr>
-<td>ExteriorEquipment</td>
-</tr>
-<tr>
-<td>Fans</td>
-</tr>
-<tr>
-<td>Pumps</td>
-</tr>
-<tr>
-<td>Heating</td>
-</tr>
-<tr>
-<td>Cooling</td>
-</tr>
-<tr>
-<td>HeatRejection</td>
-</tr>
-<tr>
-<td>Humidifier</td>
-</tr>
-<tr>
-<td>HeatRecovery</td>
-</tr>
-<tr>
-<td>DHW</td>
-</tr>
-<tr>
-<td>Cogeneration</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-</tr>
-<tr>
-<td>WaterSystems</td>
-</tr>
-</table>
-
-
-
-
-
-<table class="table table-striped">
-<tr>
-<th>Additional End Use Types Only Used for EnergyTransfer</th>
-</tr>
-<tr>
-<td>HeatingCoils</td>
-</tr>
-<tr>
-<td>CoolingCoils</td>
-</tr>
-<tr>
-<td>Chillers</td>
-</tr>
-<tr>
-<td>Boilers</td>
-</tr>
-<tr>
-<td>Baseboard</td>
-</tr>
-<tr>
-<td>HeatRecoveryForCooling</td>
-</tr>
-<tr>
-<td>HeatRecoveryForHeating</td>
-</tr>
-</table>
-
-Specific meter types are then used for grouping the fuel type meters:
-
-Table 40. Overall Meter Types
-
-<table class="table table-striped">
-<tr>
-<th>Meters</th>
-</tr>
-<tr>
-<td>Facility</td>
-</tr>
-<tr>
-<td>Building</td>
-</tr>
-<tr>
-<td>Zone</td>
-</tr>
-<tr>
-<td>HVAC</td>
-</tr>
-<tr>
-<td>Plant</td>
-</tr>
-</table>
-
-Facility meters contain all the energy of a fuel type. Building meters contain the sum of each zone’s energy. HVAC meters contain the energy from the air and zone HVAC system components. Plant meters contain the energy from the plant equipment.
-
-Thus, the following relationships should be observed:
-
-<div>\[Facility = \sum {\left( {Building + HVAC + Plant + Exterior} \right)} \]</div>
-
-<div>\[Building = \sum\limits_1^{NumberOfZones} {Zone} \]</div>
-
-There are also some special purpose meters used to describe electricity resource flows in greater detail.  Electricity metering is tracked in more detail to accommodate the complexities of onsite electricity generation.  There are three variations on the electricity resource type including:  (1) “ElectrictyPurchased� which is the quantity of electricity purchased and is always positive, (2) “ElectricitySold� which is the quantity of electricity exported by the building, that which is typically “sold� back to the power company, and is always positive, and (3) “ElectricityNet� which is the net electricity demand considering all sources of onsite generation and demand and can be either positive or negative.
-
-#### Field: Reporting Frequency
-
-Similar to the output variables, meters can be reported at different frequencies. Their resolution is the Zone Timestep interval (Number of Timesteps input). For this frequency, the elemental value of the meter will be reported. For more inclusive frequencies, the summed value along with the maximum and minimum values for the time interval will be reported. Default for this field if left blank or omitted is **Hourly**.
-
-Examples of specifying the object in the IDF follow.
-
-```idf
-Output:Meter,Electricity:*,RunPeriod;
-Output:Meter,ExteriorEquipment*,RunPeriod;
-Output:Meter:Cumulative,Electricity:*,Monthly;
-```
-
-#### Meter Details File (eplusout.mtd)
-
-The meter details file illustrates what is on each meter and vice versa.  It is described in the Output Details and Examples document under the file name.
-
-### Output:EnvironmentalImpactFactors
-
-The Output:EnvironmentalImpactFactors object triggers the necessary Facility meters to be reported and the Pollutants resulting from these on and off-site energy consumptions. These values are put into the eplusout.mtr file. Facility meters contain all the energy of a fuel type. Thus, the following relationships should be observed:
-
-<div>\[Facility = \sum {\left( {Building + System + Plant + Exterior} \right)} \]</div>
-
-Information regarding how the coefficients are derived and applied can be found in the Engineering Document.
-
-To turn on the reporting and the calculations for the environmental factors the user enters 3 objects:
-
-**Output:EnvironmentalImpactFactors:** (with associated reporting frequency, more than one frequency can be requested)
-
-**EnvironmentalImpactFactors:** (contains additional information necessary for the calculations not included in the Fuel Factors)
-
-**FuelFactors:** (required for every fuel that is simulated and converted in this simulation input file)
-
-Users will enter environmental impact factors for each Fuel Type or FuelFactor. This is the same for each Fuel Type: Natural Gas, Residual Oil, Distillate Oil, Coal, Off-Site Electricity, Gasoline, and Propane. For District Heating, District Cooling, and Steam there are additional fields in the EnvironmentalImpactFactors object that help in the conversion of their energy to Natural Gas and Electricity.
-
-The energy is obtained internally from the following facility meters:
-
-<table class="table table-striped">
-<tr>
-<th>Electricity:Facility</th>
-<th>Diesel:Facility</th>
-</tr>
-<tr>
-<td>DistrictCooling:Facility</td>
-<td>DistrictHeating:Facility</td>
-</tr>
-<tr>
-<td>Gas:Facility</td>
-<td>Gasoline:Facility</td>
-</tr>
-<tr>
-<td>Coal:Facility</td>
-<td>FuelOil#1:Facility</td>
-</tr>
-<tr>
-<td>FuelOil#2:Facility</td>
-<td>Propane:Facility</td>
-</tr>
-<tr>
-<td>ElectricityProduced:Facility</td>
-<td>Steam:Facility</td>
-</tr>
-<tr>
-<td>OtherFuel1:Facility</td>
-<td>OtherFuel2:Facility</td>
-</tr>
-</table>
-
-For the pollutant calculation only the total off-site or purchased electric energy is calculated using Electricity Factors. Off-Site Electricity = Electricity:Facility - ElectricityProduced:Facility, pollutants for the fuel type used by the on-site generator will be calculated, for example Diesel, in these cases.
-
-#### Field: Reporting Frequency
-
-Similar to the output variables and meters the environmental impact calculations can be reported at different frequencies. Their resolution is the Zone Timestep interval (Number of Timesteps input). For this frequency, the elemental value of the Environmental Impact Factors Calculation will be reported. For more inclusive frequencies, the summed value along with the maximum and minimum values for the time interval will be reported.
-
-Valid values are Timestep, Hourly, Daily, Monthly or RunPeriod.
-
-An example of specifying in the IDF:
-
-```idf
-  Output:EnvironmentalImpactFactors,
-    Monthly;  !- Reporting_Frequency
-```
-
-### EnvironmentalImpactFactors
-
-The EnvironmentalImpactFactors object contains additional information that is not individually specified in the FuelFactors object and is the second object needed to complete the calculation.  Source to Site conversion factors for District Heating, District Cooling and Steam are entered in this object.
-
-#### Field: District Heating Efficiency
-
-The District Heating Efficiency value is used to convert the district (purchased) heating energy to Natural Gas for the environmental impact calculation. The efficiency is a number between 0 and 1 and divided into the district heating energy and the default is 0.3.
-
-#### Field: Disctrict Cooling COP
-
-The District Cooling COP value is used to convert the district (purchased) cooling energy to electricity for the environmental impact calculation. The Coefficient of Performance (COP) is a number greater than 0 and divided into the purchased cooling energy with a default of 3.0.
-
-#### Field: Steam Conversion Efficiency
-
-The Steam Conversion Efficiency is used to convert the Steam usage to Natural Gas for the environmental impact calculation. The efficiency is a number between 0 and 1 and divided into the purchased heating energy and the default is 0.25.
-
-#### Field: Total Carbon Equivalent Emission Factor From N2O
-
-The Intergovernmental Panel on Climate Change has studied the effects on the relative radiative forcing effects of various greenhouse gases. This effect, called Global Warming Potential (GWP), is described in terms of the Carbon Equivalent of a particular greenhouse gase. N<sub>2</sub>O (nitrous oxide) can be produced by some Fuel Types and has a default of carbon equivalent emission factor of 80.7272 kg C/kg N<sub>2</sub>O.
-
-#### Field: Total Carbon Equivalent Emission Factor From CH4
-
-The Intergovernmental Panel on Climate Change has studied the effects on the relative radiative forcing effects of various greenhouse gases. This effect, called Global Warming Potential (GWP), is described in terms of the Carbon Equivalent of a particular greenhouse gas. CH<sub>4</sub> (methane) can be produced by all Fuel Types and has a default carbon equivalent emission factor of 6.2727 kg C/kg CH<sub>4</sub>.
-
-#### Field: Total Carbon Equivalent Emission Factor From CO2
-
-The Intergovernmental Panel on Climate Change has studied the effects on the relative radiative forcing effects of various greenhouse gases. This effect, called Global Warming Potential (GWP), is described in terms of the Carbon Equivalent of a particular greenhouse gas. CO<sub>2</sub> (carbon dioxide) can be produced by all Fuel Types and has a default carbon equivalent emission factor of 0.2727 kg C/kg CO<sub>2</sub>.
-
-An example of specifying in the IDF:
-
-```idf
-  EnvironmentalImpactFactors,
-    0.3,         !- Disctrict Heating Efficiency
-    3.0,         !- District Cooling COP
-    0.25,        !- Steam Conversion Efficiency
-    80.7272,     !- Total Carbon Equivalent Emission Factor From N2O
-    6.2727,      !- Total Carbon Equivalent Emission Factor From CH4
-    0.2727;      !- Total Carbon Equivalent Emission Factor From CO2
-```
-
-### FuelFactors
-
-#### Field: Existing Fuel Resource Name
-
-This is the name of the Fuel that is being described with this object. Source to Site conversion factors for each tool are entered with these objects. Allowable Fuel Types are:  Electricity, Natural Gas, FuelOil\#1, FuelOil\#2, Coal, Gasoline, Propane, Diesel, OtherFuel1, OtherFuel2.
-
-#### Field: Units of Measure
-
-Units in mass with kg or by volume in m3.
-
-#### Field: Energy per Unit Factor
-
-The higher heating value of the fuel type.
-
-#### Field: Source Energy Factor
-
-Multiplied by the fuel consumption to compute the source energy contribution for the fuel. If a schedule is also specified in the next field, the value specified here, the schedule value, and the fuel consumption are multiplied together for each timestep to determine the source energy contribution for the fuel. If the multipliers in the schedule specified in the next field fully represent the source energy conversion factor, the value in this field should be set to one. If the TDV files (described in next field) are used the value should be 0.293 for electricity and 0.01 for natural gas to account for the units used in the files. Units of J/J.
-
-#### Field: Source Energy Schedule Name
-
-This field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the source energy. Specifically, each value in the schedule are multiplied by the Source Energy Factor field value and by the fuel consumption to determine the source energy consumption for the fuel. If the values in the schedule fully represent the source energy conversion factor, the value in the previous field, Source Energy Factor should be set to one.
-
-The use of this field is required for evaluations using source energy factors that change throughout the year such as Time Dependent Valuation (TDV), the method used to show compliance with to California’s Title 24 under the ACM (Alternative Compliance Method). Data files containing TDV factors are in the DataSets\\TDV\\ directory. An example file for use with TDV file is in the ExampleFiles directory and is named 5zoneTDV.IDF. When using these TDV files with EnergyPlus it is important that a consistent weather file be used. It is also important that the day of the week for January 1 is set to Tuesday since all the TDV and related weather files use 1991 as the year of reference. Also note that the values in the TDV datasets files are in non SI units of measure. The source energy factor field should contain the value of 0.293 for electricity and 0.01 for natural gas to account for the non-standard units used in the files. A summary report that provides a breakdown of the facility energy use in terms of source energy can be obtained by selecting the '*AllSummary*' or '*SourceEnergyEndUseComponentsSummary*' keywords in the 'Output:Table:SummaryReports' reporting object. To learn more about TDV see:
-
-http://www.energy.ca.gov/title24/2005standards/archive/rulemaking/documents/tdv/index.html
-
-**WARNING**
-
-**THE TDV CALCULATIONS SHOULD ONLY BE PERFORMED ON SIMULATIONS THAT USE THE CALIFORNIA THERMAL ZONE (CTZ REV2) WEATHER FILES. One must match the correct TDV file to its corresponding CTZ weather file. There are 16 TDV files, one for each of the 16 CTZ weather files. The Time Dependent Valuation of TDV files provides a relative cost estimate of the various fuel sources and their relative costs by time of day, month of year and outside temperature. Outside temperature is important as demand for electricity and thus cost of electricity is influenced by temperature. These TDV files are applicable only to the hourly weather data contained in the California Thermal Zone (CTZ rev2) weather files as the time dependent cost information is partially derived from the timing of temperatures in the weather file. Thus using the TDV files with other weather data would provide meaningless results.**
-
-#### Field: CO2 Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the mass of carbon dioxide (CO<sub>2</sub>) released into the atmosphere. The units are grams per MegaJoule. Carbon dioxide gas is naturally produced by animals during respiration and through decay of biomass, and used by plants during photosynthesis. Although it only constitutes 0.04 percent of the atmosphere, it is one of the most important greenhouse gases. The combustion of fossil fuels is increasing carbon dioxide concentrations in the atmosphere, which is believed to be contributing to global warming.
-
-#### Field: CO2 Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: CO Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the mass of carbon monoxide (CO) released into the atmosphere. The units are grams per MegaJoule. Carbon monoxide is a colorless, odorless and poisonous gas produced by incomplete fossil fuel combustion. Carbon monoxide combines with the haemoglobin of human beings, reducing its oxygen carrying capacity, with effects harmful to human beings.
-
-#### Field: CO Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: CH4 Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the mass of methane (CH<sub>4</sub>) released into the atmosphere. The units are grams per MegaJoule. Methane is a colorless, nonpoisonous, flammable gas created by anaerobic decomposition of organic compounds and is one of the more potent greenhouse gases. A major component of natural gas used in the home.
-
-#### Field: CH4 Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: NOx Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the mass of nitrogen oxides (NO<sub>x</sub>) released into the atmosphere. The units are grams per MegaJoule. Nitrogen oxides refers to nitric oxide gas (NO) and nitrogen dioxide gas (NO<sub>2</sub>) and many other gaseous oxides containing nitrogen. The main source of these gases in urban areas are motor vehicle exhaust and indoor gas stoves and kerosene heaters. The brown haze sometimes seen over cities is mainly nitrogen oxides. These gases are also partly responsible for the generation of ozone, which is produced when nitrogen oxides react with other chemicals in the presence of sunlight. Exposure to high levels of nitrogen dioxide can interfere with the ability of blood to carry oxygen, leading to dizziness and shortness of breath. Prolonged exposure can lead to respiratory failure.
-
-#### Field: NOx Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: N2O Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the mass of nitrous oxide (N<sub>2</sub>O) released into the atmosphere. The units are grams per MegaJoule. Relatively inert oxide of nitrogen produced as a result of microbial action in the soil, use of fertilizers containing nitrogen, burning of timber and coil, chemical industry, and so forth. This nitrogen compound may contribute to greenhouse and ozone-depleting effects.
-
-#### Field: N2O Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: SO2 Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the mass of sulfur dioxide (SO<sub>2</sub>) released into the atmosphere. The units are in grams per MegaJoule. Sulfur dioxide gas is formed when fuel containing sulfur, such as coal and oil, is burned, and when gasoline is extracted from oil, or metals are extracted from ore. Sulfur dioxide reacts with other chemicals in the air to form tiny sulfate particles, associated with increased respiratory symptoms and disease, difficulty in breathing, and premature death. Sulfur dioxide and nitrogen oxides react with other substances in the air to form acids, which fall to earth as rain, fog, snow, or dry particles. Acid rain damages forests and crops, changes the makeup of soil, and makes lakes and streams acidic and unsuitable for fish. Sulfur dioxide accelerates the decay of building materials and paints.
-
-#### Field: SO2 Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: PM Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the mass of particulate matter (PM) released into the atmosphere. The units are grams per MegaJoule. PM is the sum of all particular matter emitted, including PM10 and PM2.5. Particulate matter, or PM, are particles found in the air, including dust, dirt, soot, smoke, and liquid droplets, which can be suspended in the air for long periods of time. Some particles are large or dark enough to be seen as soot or smoke. Others are so small that individually they can only be detected with an electron microscope. Breathing particulate matter is linked to significant respiratory health problems.
-
-#### Field: PM Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: PM10 Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the mass of particulate matter 10 (PM<sub>10</sub>) released into the atmosphere. The units are grams per MegaJoule. PM<sub>10</sub>, includes particles with an aerodynamic diameter of less than 10 microns. These smaller particles are most likely responsible for the adverse health effects on humans because particles so small can reach the thoracic or lower regions of the respiratory tract.
-
-#### Field: PM10 Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: PM2.5 Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the mass of particulate matter 2.5 (PM<sub>2.5</sub>) released into the atmosphere. The units are grams per MegaJoule. EPA’s national air quality standards for fine particles, also known as “PM<sub>2.5</sub> standards,� are levels allowed in the outdoor air for particulate matter 2.5 microns in diameter or smaller. EPA issued the PM<sub>2.5</sub> standards in 1997 to protect human health and the environment. Studies have linked increased exposure to PM<sub>2.5</sub> to increases in premature death as well as a range of serious respiratory and cardiovascular effects.
-
-#### Field: PM2.5 Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: NH3 Emission Factor
-
-The Environmental impact coefficient for the Fuel for calculating the mass of ammonia (NH<sub>3</sub>) released into the atmosphere. The units are grams per MegaJoule. Ammonia reacts with nitrogen and sulfur compounds in the atmosphere, mainly nitric and sulfuric acids, to form particulate matter.
-
-#### Field: NH3 Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: NMVOC Emission Factor
-
-The Environmental impact coefficient for the Fuel for calculating the mass of non-methane volatile organic compounds (NMVOC) released into the atmosphere. The units are grams per MegaJoule. Non-methane volatile organic compounds (NMVOC), which include propane, butane, and ethane, are emitted primarily from transportation, industrial processes, and non-industrial consumption of organic solvents. Volatile organic compounds react with nitrogen oxides in the atmosphere to form ozone.
-
-#### Field: NMVOC Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: Hg Emission Factor
-
-The Environmental impact coefficient for the Fuel for calculating the mass lof mercury (Hg) released into the atmosphere. The units are grams per MegaJoule. This heavy metal can accumulate in the environment and is highly toxic if breathed or swallowed. In the U.S., primary sources of mercury air emissions are coal-fired power plants.
-
-#### Field: Hg Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: Pb Emission Factor
-
-The Environmental impact coefficient for the Fuel for calculating the masss of lead (Pb) released into the atmosphere. The units are grams per MegaJoule. A heavy metal that is hazardous to health if breathed or swallowed. Its use in gasoline, paints, and plumbing compounds has been sharply restricted or eliminated by federal laws and regulations.
-
-#### Field: Pb Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: Water Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the volume of water (H<sub>2</sub>O) consumed or evaporated in the generation of electricity. The units are liters per MegaJoule or a volume measurement. This is the water consumed in the production of the energy, ie. electricity off-site evaporated in cooling towers or scrubbers, or in the production or processing of the fuel itself, i.e., refinery for gasoline or diesel.
-
-#### Field: Water Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: Nuclear High Level Emission Factor
-
-The environmental impact coefficient for the Fuel for calculating the mass of high-level nuclear waste, removed as spent nuclear fuel from a nuclear reactor once it no longer is efficient at powering the reactor.. The units are grams per MegaJoule. Once a year, approximately one-third of nuclear fuel is replaced with new fuel. This used fuel is called spent nuclear fuel and is highly radioactive; containing plutonium and other radionuclides. Although there is little information on quantities of high-level nuclear waste, a few utilities are beginning to publish this information.
-
-#### Field: Nuclear High Level Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-#### Field: Nuclear Low Level Emission factor
-
-The environmental impact coefficient for the Fuel for calculating the volume of low-level nuclear waste, removed from a nuclear reactor after radiation contamination. The units are cubic meters per MegaJoule or a volume measurement. Low-level waste can come from nuclear reactors or other users of radioactive material, like hospitals or research institutes. Low-level waste is less hazardous than high-level waste.
-
-#### Field: Nuclear Low Level Emission Factor Schedule Name
-
-Similar to the source energy calculation, this field contains the name of a schedule containing values that are multiplied by the fuel consumption to determine the total emission values. Specifically, each value in the schedule are multiplied by the emission factor field value and by the fuel consumption to determine the overall emission factor for the fuel. If the values in the schedule fully represent the emission factor, the value in the previous field, should be set to one.
-
-An example of specifying in the IDF:
-
-```idf
-FuelFactors,                 !  USA national average based on eGRID, EIA 1605
-    Electricity,             !- Existing Fuel Resource Name
-    kg,                      !- Units of Measure (kg or m3)
-    ,                        !- Energy per Unit Factor
-    2.253,                   !- Source Energy Factor {J/J}
-    ,                        !- Source Energy Schedule Name
-    168.33317,               !- CO2 Emission Factor {g/MJ}
-    ,                        !- CO2 Emission Factor Schedule Name
-    4.20616E-02,             !- CO Emission Factor {g/MJ}
-    ,                        !- CO Emission Factor Schedule Name
-    1.39858E-03,             !- CH4 Emission Factor {g/MJ}
-    ,                        !- CH4 Emission Factor Schedule Name
-    4.10753E-01,             !- NOx Emission Factor {g/MJ}
-    ,                        !- NOx Emission Factor Schedule Name
-    2.41916E-03,             !- N2O Emission Factor {g/MJ}
-    ,                        !- N2O Emission Factor Schedule Name
-    8.65731E-01,             !- SO2 Emission Factor {g/MJ}
-    ,                        !- SO2 Emission Factor Schedule Name
-    2.95827E-02,             !- PM Emission Factor {g/MJ}
-    ,                        !- PM Emission Factor Schedule Name
-    1.80450E-02,             !- PM10 Emission Factor {g/MJ}
-    ,                        !- PM10 Emission Factor Schedule Name
-    1.15377E-02,             !- PM2.5 Emission Factor {g/MJ}
-    ,                        !- PM2.5 Emission Factor Schedule Name
-    1.10837E-03,             !- NH3 Emission Factor {g/MJ}
-    ,                        !- NH3 Emission Factor Schedule Name
-    3.72332E-03,             !- NMVOC Emission Factor {g/MJ}
-    ,                        !- NMVOC Emission Factor Schedule Name
-    3.36414E-06,             !- Hg Emission Factor {g/MJ}
-    ,                        !- Hg Emission Factor Schedule Name
-    0,                       !- Pb Emission Factor {g/MJ}
-    ,                        !- Pb Emission Factor Schedule Name
-    2.10074,                 !- Water Emission Factor {L/MJ}
-    ,                        !- Water Emission Factor Schedule Name
-    0,                       !- Nuclear High Level Emission Factor {g/MJ}
-    ,                        !- Nuclear High Level Emission Factor Schedule Name
-    0;                       !- Nuclear Low Level Emission Factor {m3/MJ}
-```
-
-
-### Environmental Pollution Impact Outputs
-
-Various output variables and meters related to emissions are available when modeling with environmental impact and fuel factor inputs.   Output is available as either output variables or output meters.   The variables and meters available depending on the number of FuelFactor input objects and the type of fuel used in them.  Most of the fuel types have the same set of outputs for emissions that correspond to the types of emission factors in the input objects.  The exception is electricity which has two additional outputs to track possible net metering situations that can occur with on-site generation.
-
-The following pollution-emission-related outputs are available for environmental impacts.
-
-* HVAC,Sum,Environmental Impact Natural Gas Source Energy [J]
-
-* HVAC,Sum,Environmental Impact Natural Gas CO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas CO Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas CH4 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas NOx Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas N2O Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas SO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas PM Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas PM10 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas PM2.5 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas NH3 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas NMVOC Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas Hg Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas Pb Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas Water Consumption Volume [L]
-
-* HVAC,Sum,Nuclear High Level Waste From Natural Gas [kg]
-
-* HVAC,Sum,Environmental Impact Natural Gas Nuclear Low Level Waste Volume [m3]
-
-* HVAC,Sum,Environmental Impact Electricity Source Energy [J]
-
-* HVAC,Sum,Environmental Impact Electricity CO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity CO Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity CH4 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity NOx Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity N2O Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity SO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity PM Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity PM10 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity PM2.5 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity NH3 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity NMVOC Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity Hg Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity Pb Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity Water Consumption Volume [L]
-
-* HVAC,Sum,Environmental Impact Electricity Nuclear High Level Waste Mass [kg]
-
-* HVAC,Sum,Environmental Impact Electricity Nuclear Low Level Waste Volume [m3]
-
-* HVAC,Sum,Environmental Impact Purchased Electricity Source Energy [J]
-
-* HVAC,Sum,Environmental Impact Surplus Sold Electricity Source [J]
-
-* HVAC,Sum,Environmental Impact Coal Source Energy [J]
-
-* HVAC,Sum,Environmental Impact Coal CO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal CO Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal CH4 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal NOx Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal N2O Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal SO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal PM Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal PM10 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal PM2.5 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal NH3 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal NMVOC Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal Hg Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal Pb Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal Water Consumption Volume [L]
-
-* HVAC,Sum,Environmental Impact Coal Nuclear High Level Waste Mass [kg]
-
-* HVAC,Sum,Environmental Impact Coal Nuclear Low Level Waste Volume [m3]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 Source Energy [J]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 CO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 CO Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 CH4 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 NOx Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 N2O Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 SO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 PM Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 PM10 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 PM2.5 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 NH3 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 NMVOC Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 Hg Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 Pb Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 Water Consumption Volume [L]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 Nuclear High Level Waste Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#2 Nuclear Low Level Waste Volume [m3]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 Source Energy [J]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 CO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 CO Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 CH4 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 NOx Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 N2O Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 SO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 PM Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 PM10 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 PM2.5 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 NH3 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 NMVOC Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 Hg Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 Pb Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 Water Consumption Volume [L]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 Nuclear High Level Waste Mass [kg]
-
-* HVAC,Sum,Environmental Impact Fuel Oil \#1 Nuclear Low Level Waste Volume [m3]
-
-* HVAC,Sum,Environmental Impact Propane Source Energy [J]
-
-* HVAC,Sum,Environmental Impact Propane CO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane CO Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane CH4 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane NOx Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane N2O Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane SO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane PM Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane PM10 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane PM2.5 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane NH3 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane NMVOC Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane Hg Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane Pb Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane Water Consumption Volume [L]
-
-* HVAC,Sum,Environmental Impact Propane Nuclear High Level Waste Mass [kg]
-
-* HVAC,Sum,Environmental Impact Propane Nuclear Low Level Waste Volume [m3]
-
-* HVAC,Sum,Environmental Impact Gasoline Source Energy [J]
-
-* HVAC,Sum,Environmental Impact Gasoline CO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline CO Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline CH4 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline NOx Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline N2O Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline SO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline PM Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline PM10 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline PM2.5 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline NH3 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline NMVOC Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline Hg Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline Pb Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline Water Consumption Volume [L]
-
-* HVAC,Sum,Environmental Impact Gasoline Nuclear High Level Waste Mass [kg]
-
-* HVAC,Sum,Environmental Impact Gasoline Nuclear Low Level Waste Volume [m3]
-
-* HVAC,Sum,Environmental Impact Diesel Source Energy [J]
-
-* HVAC,Sum,Environmental Impact Diesel CO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel CO Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel CH4 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel NOx Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel N2O Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel SO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel PM Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel PM10 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel PM2.5 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel NH3 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel NMVOC Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel Hg Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel Pb Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel Water Consumption Volume [L]
-
-* HVAC,Sum,Environmental Impact Diesel Nuclear High Level Waste Mass [kg]
-
-* HVAC,Sum,Environmental Impact Diesel Nuclear Low Level Waste Volume [m3]
-* HVAC,Sum,Environmental Impact OtherFuel1 Source Energy [J]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 CO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 CO Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 CH4 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 NOx Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 N2O Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 SO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 PM Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 PM10 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 PM2.5 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 NH3 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 NMVOC Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 Hg Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 Pb Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 Water Consumption Volume [L]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 Nuclear High Level Waste Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel1 Nuclear Low Level Waste Volume [m3]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 Source Energy [J]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 CO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 CO Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 CH4 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 NOx Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 N2O Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 SO2 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 PM Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 PM10 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 PM2.5 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 NH3 Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 NMVOC Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 Hg Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 Pb Emissions Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 Water Consumption Volume [L]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 Nuclear High Level Waste Mass [kg]
-
-* HVAC,Sum,Environmental Impact OtherFuel2 Nuclear Low Level Waste Volume [m3]
-
-
-* HVAC,Sum,Environmental Impact Total N2O Emissions Carbon Equivalent Mass [kg]
-
-* HVAC,Sum,Environmental Impact Total CH4 Emissions Carbon Equivalent Mass [kg]
-
-* HVAC,Sum,Environmental Impact Total CO2 Emissions Carbon Equivalent Mass [kg]
-
-
-
-#### Environmental Impact Electricity Source Energy [J]
-
-#### Environmental Impact Purchased Electricity Source Energy [J]
-
-#### Environmental Impact Surplus Sold Electricity Source [J]
-
-#### Environmental Impact Natural Gas Source Energy [J]
-
-#### Environmental Impact Fuel Oil \#2 Source Energy [J]
-
-#### Environmental Impact Fuel Oil \#1 Source Energy [J]
-
-#### Environmental Impact Coal Source Energy [J]
-
-#### Environmental Impact Gasoline Source Energy [J]
-
-#### Environmental Impact Propane Source Energy [J]
-
-#### Environmental Impact Diesel Source Energy [J]
-
-#### Environmental Impact OtherFuel1 Source Energy [J]
-
-#### Environmental Impact OtherFuel2 Source Energy [J]
-
-These outputs provide results for the source energy embodied in each type of fuel that might be used at the site.  The units are Joules. The EnergyPlus models energy use at the site and conversion factors are used to determine the added energy used to create, process or deliver a fuel to the building.  There are three types of electricity-related source energy results available.  The first “Environmental Impact Electricity Source Energy� is for the electricity consumed at the site that was not produced at the site.  The second, “Environmental Impact Purchased Electricity Source Energy,� is similar but includes just the electricity purchased form the utility.  The third, “Environmental Impact Surplus Sold Electricity Source,� is the source energy associated with any surplus electricity that is exported to the grid.
-
-#### Environmental Impact Electricity CO2 Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas CO2 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 CO2 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 CO2 Emissions Mass [kg]
-
-#### Environmental Impact Coal CO2 Emissions Mass [kg]
-
-#### Environmental Impact Gasoline CO2 Emissions Mass [kg]
-
-#### Environmental Impact Propane CO2 Emissions Mass [kg]
-
-#### Environmental Impact Diesel CO2 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 CO2 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 CO2 Emissions Mass [kg]
-
-These outputs provide results for the carbon dioxide reelases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity CO Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas CO Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 CO Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 CO Emissions Mass [kg]
-
-#### Environmental Impact Coal CO Emissions Mass [kg]
-
-#### Environmental Impact Gasoline CO Emissions Mass [kg]
-
-#### Environmental Impact Propane CO Emissions Mass [kg]
-
-#### Environmental Impact Diesel CO Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 CO Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 CO Emissions Mass [kg]
-
-These outputs provide results for the carbon monoxide releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity CH4 Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas CH4 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 CH4 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 CH4 Emissions Mass [kg]
-
-#### Environmental Impact Coal CH4 Emissions Mass [kg]
-
-#### Environmental Impact Gasoline CH4 Emissions Mass [kg]
-
-#### Environmental Impact Propane CH4 Emissions Mass [kg]
-
-#### Environmental Impact Diesel CH4 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 CH4 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 CH4 Emissions Mass [kg]
-
-These outputs provide results for the methane releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity NOx Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas NOx Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 NOx Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 NOx Emissions Mass [kg]
-
-#### Environmental Impact Coal NOx Emissions Mass [kg]
-
-#### Environmental Impact Gasoline NOx Emissions Mass [kg]
-
-#### Environmental Impact Propane NOx Emissions Mass [kg]
-
-#### Environmental Impact Diesel NOx Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 NOx Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 NOx Emissions Mass [kg]
-
-These outputs provide results for the various nitrogen oxide releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity N2O Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas N2O Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 N2O Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 N2O Emissions Mass [kg]
-
-#### Environmental Impact Coal N2O Emissions Mass [kg]
-
-#### Environmental Impact Gasoline N2O Emissions Mass [kg]
-
-#### Environmental Impact Propane N2O Emissions Mass [kg]
-
-#### Environmental Impact Diesel N2O Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 N2O Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 N2O Emissions Mass [kg]
-
-These outputs provide results for the nitrous oxide releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity SO2 Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas SO2 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 SO2 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 SO2 Emissions Mass [kg]
-
-#### Environmental Impact Coal SO2 Emissions Mass [kg]
-
-#### Environmental Impact Gasoline SO2 Emissions Mass [kg]
-
-#### Environmental Impact Propane SO2 Emissions Mass [kg]
-
-#### Environmental Impact Diesel SO2 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 SO2 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 SO2 Emissions Mass [kg]
-
-These outputs provide results for the sulphur dioxide releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity PM Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas PM Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 PM Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 PM Emissions Mass [kg]
-
-#### Environmental Impact Coal PM Emissions Mass [kg]
-
-#### Environmental Impact Gasoline PM Emissions Mass [kg]
-
-#### Environmental Impact Propane PM Emissions Mass [kg]
-
-#### Environmental Impact Diesel PM Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 PM Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 PM Emissions Mass [kg]
-
-These outputs provide results for particulate matter releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity PM10 Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas PM10 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 PM10 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 PM10 Emissions Mass [kg]
-
-#### Environmental Impact Coal PM10 Emissions Mass [kg]
-
-#### Environmental Impact Gasoline PM10 Emissions Mass [kg]
-
-#### Environmental Impact Propane PM10 Emissions Mass [kg]
-
-#### Environmental Impact Diesel PM10 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 PM10 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 PM10 Emissions Mass [kg]
-
-These outputs provide results for particulate matter of 10 microns or less releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity PM2.5 Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas PM2.5 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 PM2.5 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 PM2.5 Emissions Mass [kg]
-
-#### Environmental Impact Coal PM2.5 Emissions Mass [kg]
-
-#### Environmental Impact Gasoline PM2.5 Emissions Mass [kg]
-
-#### Environmental Impact Propane PM2.5 Emissions Mass [kg]
-
-#### Environmental Impact Diesel PM2.5 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 PM2.5 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 PM2.5 Emissions Mass [kg]
-
-These outputs provide results for particulate matter of 2.5 microns or less releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity NH3 Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas NH3 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 NH3 Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 NH3 Emissions Mass [kg]
-
-#### Environmental Impact Coal NH3 Emissions Mass [kg]
-
-#### Environmental Impact Gasoline NH3 Emissions Mass [kg]
-
-#### Environmental Impact Propane NH3 Emissions Mass [kg]
-
-#### Environmental Impact Diesel NH3 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 NH3 Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 NH3 Emissions Mass [kg]
-
-These outputs provide results for ammonia releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity NMVOC Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas NMVOC Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 NMVOC Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 NMVOC Emissions Mass [kg]
-
-#### Environmental Impact Coal NMVOC Emissions Mass [kg]
-
-#### Environmental Impact Gasoline NMVOC Emissions Mass [kg]
-
-#### Environmental Impact Propane NMVOC Emissions Mass [kg]
-
-#### Environmental Impact Diesel NMVOC Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 NMVOC Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 NMVOC Emissions Mass [kg]
-
-These outputs provide results for non-methane volatile organic compound releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity Hg Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas Hg Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 Hg Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 Hg Emissions Mass [kg]
-
-#### Environmental Impact Coal Hg Emissions Mass [kg]
-
-#### Environmental Impact Gasoline Hg Emissions Mass [kg]
-
-#### Environmental Impact Propane Hg Emissions Mass [kg]
-
-#### Environmental Impact Diesel Hg Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 Hg Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 Hg Emissions Mass [kg]
-
-These outputs provide results for mercury releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity Pb Emissions Mass [kg]
-
-#### Environmental Impact Natural Gas Pb Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#2 Pb Emissions Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 Pb Emissions Mass [kg]
-
-#### Environmental Impact Coal Pb Emissions Mass [kg]
-
-#### Environmental Impact Gasoline Pb Emissions Mass [kg]
-
-#### Environmental Impact Propane Pb Emissions Mass [kg]
-
-#### Environmental Impact Diesel Pb Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel1 Pb Emissions Mass [kg]
-
-#### Environmental Impact OtherFuel2 Pb Emissions Mass [kg]
-
-These outputs provide results for lead releases associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity Water Consumption Volume [L]
-
-#### Environmental Impact Natural Gas Water Consumption Volume [L]
-
-#### Environmental Impact Fuel Oil \#2 Water Consumption Volume [L]
-
-#### Environmental Impact Fuel Oil \#1 Water Consumption Volume [L]
-
-#### Environmental Impact Coal Water Consumption Volume [L]
-
-#### Environmental Impact Gasoline Water Consumption Volume [L]
-
-#### Environmental Impact Propane Water Consumption Volume [L]
-
-#### Environmental Impact Diesel Water Consumption Volume [L]
-
-#### Environmental Impact OtherFuel1 Water Consumption Volume [L]
-
-#### Environmental Impact OtherFuel2 Water Consumption Volume [L]
-
-These outputs provide results for water consumption or evaporation associated with consumption of each type of fuel that might be used at the site.  The units are liters.
-
-#### Environmental Impact Electricity Nuclear High Level Waste Mass [kg]
-
-#### Nuclear High Level Waste From Natural Gas [kg]
-
-#### Environmental Impact Fuel Oil \#2 Nuclear High Level Waste Mass [kg]
-
-#### Environmental Impact Fuel Oil \#1 Nuclear High Level Waste Mass [kg]
-
-#### Environmental Impact Coal Nuclear High Level Waste Mass [kg]
-
-#### Environmental Impact Gasoline Nuclear High Level Waste Mass [kg]
-
-#### Environmental Impact Propane Nuclear High Level Waste Mass [kg]
-
-#### Environmental Impact Diesel Nuclear High Level Waste Mass [kg]
-
-#### Environmental Impact OtherFuel1 Nuclear High Level Waste Mass [kg]
-
-#### Environmental Impact OtherFuel2 Nuclear High Level Waste Mass [kg]
-
-These outputs provide results for high-level nuclear waste associated with consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Electricity Nuclear Low Level Waste Volume [m3]
-
-#### Environmental Impact Natural Gas Nuclear Low Level Waste Volume [m3]
-
-#### Environmental Impact Fuel Oil \#2 Nuclear Low Level Waste Volume [m3]
-
-#### Environmental Impact Fuel Oil \#1 Nuclear Low Level Waste Volume [m3]
-
-#### Environmental Impact Coal Nuclear Low Level Waste Volume [m3]
-
-#### Environmental Impact Gasoline Nuclear Low Level Waste Volume [m3]
-
-#### Environmental Impact Propane Nuclear Low Level Waste Volume [m3]
-
-#### Environmental Impact Diesel Nuclear Low Level Waste Volume [m3]
-
-#### Environmental Impact OtherFuel1 Nuclear Low Level Waste Volume [m3]
-
-#### Environmental Impact OtherFuel2 Nuclear Low Level Waste Volume [m3]
-
-These outputs provide results for low-level nuclear waste associated with consumption of each type of fuel that might be used at the site.  The units are cubic meters.
-
-#### Environmental Impact Total N2O Emissions Carbon Equivalent Mass [kg]
-
-This output provides the result for equivalent carbon mass associated with the nitrous oxide (N<sub>2</sub>O ) releases that stem from the consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Total CH4 Emissions Carbon Equivalent Mass [kg]
-
-This output provides the result for equivalent carbon mass associated with the methane releases that stem from the consumption of each type of fuel that might be used at the site.  The units are kg.
-
-#### Environmental Impact Total CO2 Emissions Carbon Equivalent Mass [kg]
-
-This output provides the result for equivalent carbon mass associated with the carbon dioxide releases that stem from the consumption of each type of fuel that might be used at the site.  The units are kg.
-
-The following different output meters could appear in the standard meter output (.mdd) file:
-
-* Zone,Meter,Source:Facility [J]
-
-* Zone,Meter,NaturalGasEmissions:Source [J]
-
-* Zone,Meter,CO2:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:CO2 [kg]
-
-* Zone,Meter,CO:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:CO [kg]
-
-* Zone,Meter,CH4:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:CH4 [kg]
-
-* Zone,Meter,NOx:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:NOx [kg]
-
-* Zone,Meter,N2O:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:N2O [kg]
-
-* Zone,Meter,SO2:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:SO2 [kg]
-
-* Zone,Meter,PM:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:PM [kg]
-
-* Zone,Meter,PM10:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:PM10 [kg]
-
-* Zone,Meter,PM2.5:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:PM2.5 [kg]
-
-* Zone,Meter,NH3:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:NH3 [kg]
-
-* Zone,Meter,NMVOC:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:NMVOC [kg]
-
-* Zone,Meter,Hg:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:Hg [kg]
-
-* Zone,Meter,Pb:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:Pb [kg]
-
-* Zone,Meter,WaterEnvironmentalFactors:Facility [L]
-
-* Zone,Meter,NaturalGasEmissions:WaterEnvironmentalFactors [L]
-
-* Zone,Meter,Nuclear High:Facility [kg]
-
-* Zone,Meter,NaturalGasEmissions:Nuclear High [kg]
-
-* Zone,Meter,Nuclear Low:Facility [m3]
-
-* Zone,Meter,NaturalGasEmissions:Nuclear Low [m3]
-
-* Zone,Meter,ElectricEmissions:Source [J]
-
-* Zone,Meter,ElectricEmissions:CO2 [kg]
-
-* Zone,Meter,ElectricEmissions:CO [kg]
-
-* Zone,Meter,ElectricEmissions:CH4 [kg]
-
-* Zone,Meter,ElectricEmissions:NOx [kg]
-
-* Zone,Meter,ElectricEmissions:N2O [kg]
-
-* Zone,Meter,ElectricEmissions:SO2 [kg]
-
-* Zone,Meter,ElectricEmissions:PM [kg]
-
-* Zone,Meter,ElectricEmissions:PM10 [kg]
-
-* Zone,Meter,ElectricEmissions:PM2.5 [kg]
-
-* Zone,Meter,ElectricEmissions:NH3 [kg]
-
-* Zone,Meter,ElectricEmissions:NMVOC [kg]
-
-* Zone,Meter,ElectricEmissions:Hg [kg]
-
-* Zone,Meter,ElectricEmissions:Pb [kg]
-
-* Zone,Meter,ElectricEmissions:WaterEnvironmentalFactors [L]
-
-* Zone,Meter,ElectricEmissions:Nuclear High [kg]
-
-* Zone,Meter,ElectricEmissions:Nuclear Low [m3]
-
-* Zone,Meter,PurchasedElectricEmissions:Source [J]
-
-* Zone,Meter,SoldElectricEmissions:Source [J]
-
-* Zone,Meter,CoalEmissions:Source [J]
-
-* Zone,Meter,CoalEmissions:CO2 [kg]
-
-* Zone,Meter,CoalEmissions:CO [kg]
-
-* Zone,Meter,CoalEmissions:CH4 [kg]
-
-* Zone,Meter,CoalEmissions:NOx [kg]
-
-* Zone,Meter,CoalEmissions:N2O [kg]
-
-* Zone,Meter,CoalEmissions:SO2 [kg]
-
-* Zone,Meter,CoalEmissions:PM [kg]
-
-* Zone,Meter,CoalEmissions:PM10 [kg]
-
-* Zone,Meter,CoalEmissions:PM2.5 [kg]
-
-* Zone,Meter,CoalEmissions:NH3 [kg]
-
-* Zone,Meter,CoalEmissions:NMVOC [kg]
-
-* Zone,Meter,CoalEmissions:Hg [kg]
-
-* Zone,Meter,CoalEmissions:Pb [kg]
-
-* Zone,Meter,CoalEmissions:WaterEnvironmentalFactors [L]
-
-* Zone,Meter,CoalEmissions:Nuclear High [kg]
-
-* Zone,Meter,CoalEmissions:Nuclear Low [m3]
-
-* Zone,Meter,FuelOil\#2Emissions:Source [J]
-
-* Zone,Meter,FuelOil\#2Emissions:CO2 [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:CO [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:CH4 [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:NOx [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:N2O [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:SO2 [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:PM [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:PM10 [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:PM2.5 [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:NH3 [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:NMVOC [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:Hg [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:Pb [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:WaterEnvironmentalFactors [L]
-
-* Zone,Meter,FuelOil\#2Emissions:Nuclear High [kg]
-
-* Zone,Meter,FuelOil\#2Emissions:Nuclear Low [m3]
-
-* Zone,Meter,FuelOil\#1Emissions:Source [J]
-
-* Zone,Meter,FuelOil\#1Emissions:CO2 [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:CO [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:CH4 [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:NOx [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:N2O [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:SO2 [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:PM [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:PM10 [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:PM2.5 [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:NH3 [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:NMVOC [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:Hg [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:Pb [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:WaterEnvironmentalFactors [L]
-
-* Zone,Meter,FuelOil\#1Emissions:Nuclear High [kg]
-
-* Zone,Meter,FuelOil\#1Emissions:Nuclear Low [m3]
-
-* Zone,Meter,PropaneEmissions:Source [J]
-
-* Zone,Meter,PropaneEmissions:CO2 [kg]
-
-* Zone,Meter,PropaneEmissions:CO [kg]
-
-* Zone,Meter,PropaneEmissions:CH4 [kg]
-
-* Zone,Meter,PropaneEmissions:NOx [kg]
-
-* Zone,Meter,PropaneEmissions:N2O [kg]
-
-* Zone,Meter,PropaneEmissions:SO2 [kg]
-
-* Zone,Meter,PropaneEmissions:PM [kg]
-
-* Zone,Meter,PropaneEmissions:PM10 [kg]
-
-* Zone,Meter,PropaneEmissions:PM2.5 [kg]
-
-* Zone,Meter,PropaneEmissions:NH3 [kg]
-
-* Zone,Meter,PropaneEmissions:NMVOC [kg]
-
-* Zone,Meter,PropaneEmissions:Hg [kg]
-
-* Zone,Meter,PropaneEmissions:Pb [kg]
-
-* Zone,Meter,PropaneEmissions:WaterEnvironmentalFactors [L]
-
-* Zone,Meter,PropaneEmissions:Nuclear High [kg]
-
-* Zone,Meter,PropaneEmissions:Nuclear Low [m3]
-
-* Zone,Meter,GasolineEmissions:Source [J]
-
-* Zone,Meter,GasolineEmissions:CO2 [kg]
-
-* Zone,Meter,GasolineEmissions:CO [kg]
-
-* Zone,Meter,GasolineEmissions:CH4 [kg]
-
-* Zone,Meter,GasolineEmissions:NOx [kg]
-
-* Zone,Meter,GasolineEmissions:N2O [kg]
-
-* Zone,Meter,GasolineEmissions:SO2 [kg]
-
-* Zone,Meter,GasolineEmissions:PM [kg]
-
-* Zone,Meter,GasolineEmissions:PM10 [kg]
-
-* Zone,Meter,GasolineEmissions:PM2.5 [kg]
-
-* Zone,Meter,GasolineEmissions:NH3 [kg]
-
-* Zone,Meter,GasolineEmissions:NMVOC [kg]
-
-* Zone,Meter,GasolineEmissions:Hg [kg]
-
-* Zone,Meter,GasolineEmissions:Pb [kg]
-
-* Zone,Meter,GasolineEmissions:WaterEnvironmentalFactors [L]
-
-* Zone,Meter,GasolineEmissions:Nuclear High [kg]
-
-* Zone,Meter,GasolineEmissions:Nuclear Low [m3]
-
-* Zone,Meter,DieselEmissions:Source [J]
-
-* Zone,Meter,DieselEmissions:CO2 [kg]
-
-* Zone,Meter,DieselEmissions:CO [kg]
-
-* Zone,Meter,DieselEmissions:CH4 [kg]
-
-* Zone,Meter,DieselEmissions:NOx [kg]
-
-* Zone,Meter,DieselEmissions:N2O [kg]
-
-* Zone,Meter,DieselEmissions:SO2 [kg]
-
-* Zone,Meter,DieselEmissions:PM [kg]
-
-* Zone,Meter,DieselEmissions:PM10 [kg]
-
-* Zone,Meter,DieselEmissions:PM2.5 [kg]
-
-* Zone,Meter,DieselEmissions:NH3 [kg]
-
-* Zone,Meter,DieselEmissions:NMVOC [kg]
-
-* Zone,Meter,DieselEmissions:Hg [kg]
-
-* Zone,Meter,DieselEmissions:Pb [kg]
-
-* Zone,Meter,DieselEmissions:WaterEnvironmentalFactors [L]
-
-* Zone,Meter,DieselEmissions:Nuclear High [kg]
-
-* Zone,Meter,DieselEmissions:Nuclear Low [m3]
-
-* Zone,Meter,OtherFuel1Emissions:Source [J]
-
-* Zone,Meter,OtherFuel1Emissions:CO2 [kg]
-
-* Zone,Meter,OtherFuel1Emissions:CO [kg]
-
-* Zone,Meter,OtherFuel1Emissions:CH4 [kg]
-
-* Zone,Meter,OtherFuel1Emissions:NOx [kg]
-
-* Zone,Meter,OtherFuel1Emissions:N2O [kg]
-
-* Zone,Meter,OtherFuel1Emissions:SO2 [kg]
-
-* Zone,Meter,OtherFuel1Emissions:PM [kg]
-
-* Zone,Meter,OtherFuel1Emissions:PM10 [kg]
-
-* Zone,Meter,OtherFuel1Emissions:PM2.5 [kg]
-
-* Zone,Meter,OtherFuel1Emissions:NH3 [kg]
-
-* Zone,Meter,OtherFuel1Emissions:NMVOC [kg]
-
-* Zone,Meter,OtherFuel1Emissions:Hg [kg]
-
-* Zone,Meter,OtherFuel1Emissions:Pb [kg]
-
-* Zone,Meter,OtherFuel1Emissions:WaterEnvironmentalFactors [L]
-
-* Zone,Meter,OtherFuel1Emissions:Nuclear High [kg]
-
-* Zone,Meter,OtherFuel1Emissions:Nuclear Low [m3]
-
-* Zone,Meter,OtherFuel2Emissions:Source [J]
-
-* Zone,Meter,OtherFuel2Emissions:CO2 [kg]
-
-* Zone,Meter,OtherFuel2Emissions:CO [kg]
-
-* Zone,Meter,OtherFuel2Emissions:CH4 [kg]
-
-* Zone,Meter,OtherFuel2Emissions:NOx [kg]
-
-* Zone,Meter,OtherFuel2Emissions:N2O [kg]
-
-* Zone,Meter,OtherFuel2Emissions:SO2 [kg]
-
-* Zone,Meter,OtherFuel2Emissions:PM [kg]
-
-* Zone,Meter,OtherFuel2Emissions:PM10 [kg]
-
-* Zone,Meter,OtherFuel2Emissions:PM2.5 [kg]
-
-* Zone,Meter,OtherFuel2Emissions:NH3 [kg]
-
-* Zone,Meter,OtherFuel2Emissions:NMVOC [kg]
-
-* Zone,Meter,OtherFuel2Emissions:Hg [kg]
-
-* Zone,Meter,OtherFuel2Emissions:Pb [kg]
-
-* Zone,Meter,OtherFuel2Emissions:WaterEnvironmentalFactors [L]
-
-* Zone,Meter,OtherFuel2Emissions:Nuclear High [kg]
-
-* Zone,Meter,OtherFuel2Emissions:Nuclear Low [m3]
-
-* Zone,Meter,Carbon Equivalent:Facility [kg]
-
-* Zone,Meter,CarbonEquivalentEmissions:Carbon Equivalent [kg]
-
-What shows up in the output are the Energy Meters that were utilized in this particular input file, the pollutants, and the Total Carbon Equivalent.
-
-### Output:SQLite
-
-Output from EnergyPlus can be written to SQLite files for manipulation outside some of the standard (such as spreadsheet) tools.
-
-#### Field: Option
-
-Currently, there are limited capabilities for specifying SQLite generation.  The Simple option will include all of the predefined database tables as well as time series related data.  Using the SimpleAndTabular choice adds database tables related to the tabular reports that are already output by EnergyPlus in other formats.  The description for SQLite outputs is described fully in the Output Details document.
-
-And one includes it in the IDF using the following.
-
-```idf
-Output:SQLite, Simple;
-```
-
-Output
-======
-
-EnergyPlus produces several output files as shown in the section on “Running EnergyPlus�.  This section will discuss the data contained in the “standard� output files (**eplusout.eso, eplusout.mtr**). They, too, have data dictionaries but unlike the input files, the output data dictionary is contained within the output file. Thus, the basic structure of the standard output file is:
-
-```
-Data Dictionary Information
-End of Data Dictionary
-Data
-...
-Data
-End of Data
-```
-
-
-As with the IDF structure, there are rules associated with the interpretation of the standard output data dictionary. These rules are summarized as follows:
-
-- The first item on each line is an integer which represents the “report code�. This “report code� will be listed in the data section where it will also be the first item on each line, identifying the data. Only 2 lines in the output file will not have an integer as the first item (“End of Data Dictionary� and “End of Data� lines).
-
-- The second item on each line is also an integer. This integer corresponds to the number of items left on the dictionary line. Each string consists of a variable name and units in square brackets. Square brackets are required for all strings. If there are no units associated with a particular variable, then there are no characters between the brackets.
-
-Six standard items appear at the start of every EnergyPlus Standard Output File Data Dictionary:
-
-```
-Program Version,EnergyPlus <version number indicated>
-1,5,Environment Title[],Latitude[degrees],Longitude[degrees],Time Zone[],Elevation[m]
-2,6,Day of Simulation[],Month[],Day of Month[],DST Indicator[1=yes 0=no],Hour[],StartMinute[],EndMinute[],DayType
-3,3,Cumulative Day of Simulation[],Month[],Day of Month[],DST Indicator[1=yes 0=no],DayType  ! When Daily Output variables Requested
-4,2,Cumulative Days of Simulation[],Month[]  ! When Monthly Output variables Requested
-5,1,Cumulative Days of Simulation[] ! When Run Period Output variables Requested
-```
-
-* Item 0 is the program version statement.
-
-* Item 1 is produced at the beginning of each new “environment� (design day, run period).
-
-* Item 2 is produced prior to any variable reported at the timestep or hourly intervals. Hourly intervals will be shown with a start minute of 0.0 and an end minute of 60.0. Timestep intervals will show the appropriate start and end minutes.
-
-* Item 3 is produced prior to any variable reported at the daily interval.
-
-* Item 4 is produced prior to any variable reported at the monthly interval.
-
-* Item 5 is produced prior to any variable reported at the end of the “environment�.
-
-Following these five standard lines will be the variables requested for reporting from the input file (ref. Output:Variable object). For example:
-
-```
-6,1,Environment,Site Outdoor Air Drybulb Temperature [C] !Hourly
-40,1,ZONE ONE,Zone Total Internal Latent Gain Energy [J] !Hourly
-68,1,ZONE ONE,Zone Mean Radiant Temperature [C] !Hourly
-69,1,ZONE ONE,Zone Mean Air Temperature [C] !Hourly
-70,1,ZONE ONE,Zone Air Heat Balance Surface Convection Rate [W] !Hourly
-71,1,ZONE ONE,Zone Air Heat Balance Air Energy Storage Rate [W] !Hourly
-```
-
-This example illustrates the non-consecutive nature of the “report codes�. Internally, EnergyPlus counts each variable that *could* be reported. This is the assigned “report code�. However, the user may not request each possible variable for reporting. Note that, currently, the requested reporting frequency is shown as a comment (!) line in the standard output file.
-
-The data is produced when the actual simulation is performed (after the warmup days unless the Output:Diagnostics requesting ReportDuringWarmup is used). Data output is simpler in format than the data dictionary lines. From the dictionary above:
-
-```
-1,DENVER STAPLETON INTL ARPT ANN HTG 99% CONDNS DB,  39.74,-105.18,  -7.00,1829.00
-2,1,12,21, 0, 1, 0.00,60.00,WinterDesignDay
-6,-16.
-40,0.0
-68,-19.8183039170649
-69,-19.8220899203323
-70,-3.175272922406513E-002
-71,-3.181520440307718E-002
-```
-
-
-This output file can be easily turned into a form that is read into commonly used spreadsheet programs where it can be further analyzed, graphed, etc.
-
-More details including graphs are shown in the Output Details and Examples Document under the file **eplusout.eso**.
-
-Using ReadVarsESO
------------------
-
-### Creating Charts and Spreadsheet files from Output Variables
-
-The ReadVarsESO program is distributed with EnergyPlus as a simple approach to converting the standard output files (**eplusout.eso, eplusout.mtr**) into files that can be put directly into a spreadsheet program and then used to create graphs or do other statistical operations. ReadVarsESO can read the complex output files and sort the data into time-based form, it is a very quick application but does not have a lot of features.  Note that all the **Output:Meter** and **Output:Meter:Cumulative** objects are included on the **eplusout.eso** file as well as the **eplusout.mtr** file.  You can choose the **Output:Meter:MeterFileOnly** or **Output:Meter:Cumulative:MeterFileOnly** objects if you do not want a particular meter to show up on the **eplusout.eso** file. If you wish to see only the metered outputs, the **eplusout.mtr** file will typically be a lot smaller than the **eplusout.eso** file.
-
-The ReadVarsESO program has a very simple set of inputs. By default, you will get all the variables listed in the Output:Variable (**eplusout.eso**) or Output:Meter (**eplusout.mtr**) objects into the appropriate output files. The outputs from ReadVarsESO are limited to 255 variables (Microsoft Excelâ„¢ limit). You can tailor how many variables to list by specifying variables for the ReadVarsESO runs.
-
-You can override the 255 variable limit by specifying an argument on the command line (**EP-Launch** has a special option for this). You use “unlimited� or “nolimit� on the command line to get as many variables into your output file as desired. Again, this will be limited either by the number of variables in the **eplusout.eso** or **eplusout.mtr** files or the contents of the “rvi� file. If you want to use this option, you must include two arguments to the command line of the ReadVars program – 1) the “rvi� file and 2) the “unlimited� argument.
-
-Table 41. ReadVarsESO Command Line Options
-
-<table class="table table-striped">
-<tr>
-<th>Option</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>&lt;filename&gt;</td>
-<td>To use any of these options, you must include a file name (“rvi� file) as the first argument.</td>
-</tr>
-<tr>
-<td>Unlimited (or Nolimit)</td>
-<td>Variables of any number will be produced on the output file.</td>
-</tr>
-<tr>
-<td>Timestep</td>
-<td>Only variables with reported frequency “timestep� (or detailed) will be produced on the output file.</td>
-</tr>
-<tr>
-<td>Hourly</td>
-<td>Only variables with reported frequency “hourly�  will be produced on the output file.</td>
-</tr>
-<tr>
-<td>Daily</td>
-<td>Only variables with reported frequency “daily�  will be produced on the output file.</td>
-</tr>
-<tr>
-<td>Monthly</td>
-<td>Only variables with reported frequency “monthly�  will be produced on the output file.</td>
-</tr>
-<tr>
-<td>Annual (or RunPeriod)</td>
-<td>Only variables with reported frequency “runperiod�  will be produced on the output file.</td>
-</tr>
-</table>
-
-In addition, another argument can be used so that the output file is only one time frequency. (By default, all variables – hourly, monthly, annual, etc. are mixed together in the output file). By using “Timestep� as an argument, you would get only the TimeStep reported variables. Using “Monthly�, only the monthly variables. This is not automated in either **EP-Launch** or the **RunEPlus** batch file but can easily be accomplished.
-
-The program is run automatically from the **EP-Launch** program or the **RunEPlus** batch file (both these methods for executing EnergyPlus are described in the GettingStarted document). These programs use **&lt;filename&gt;.rvi** for input to the ReadVarsESO program executed first after the EnergyPlus execution and **&lt;filename&gt;.mvi** for the second execution. Ostensibly, the .rvi file would apply to the eplusout.eso file and the .mvi would apply to the eplusout.mtr file, BUT the contents of the files actually specify the “**input**� reporting file and the “**output**� reorganized file. Typical contents of an .rvi file are:
-
-Table 42. "RVI" file contents
-
-<table class="table table-striped">
-<tr>
-<th>.rvi line description</th>
-<th>Actual .rvi File Contents</th>
-</tr>
-<tr>
-<td>Input File</td>
-<td>eplusout.eso</td>
-</tr>
-<tr>
-<td>Output File</td>
-<td>eplusout.csv</td>
-</tr>
-<tr>
-<td>Variable Name</td>
-<td>Site Outdoor Drybulb Temperature</td>
-</tr>
-<tr>
-<td>Variable Name</td>
-<td>Zone Air Temperature</td>
-</tr>
-<tr>
-<td>Variable Name</td>
-<td>Zone Air Humidity Ratio</td>
-</tr>
-<tr>
-<td>Variable Name</td>
-<td>Zone Air System Sensible Cooling Rate</td>
-</tr>
-<tr>
-<td>Variable Name</td>
-<td>Zone Air System Sensible Heating Rate</td>
-</tr>
-<tr>
-<td>Variable Name</td>
-<td>Zone Total Internal Latent Gain Rate</td>
-</tr>
-<tr>
-<td>Specific Variable Name</td>
-<td>COOLING COIL AIR OUTLET NODE,System Node Temperature</td>
-</tr>
-<tr>
-<td>Specific Variable Name</td>
-<td>AIR LOOP OUTLET NODE,System Node Temperature</td>
-</tr>
-<tr>
-<td>Specific Variable Name</td>
-<td>AIR LOOP OUTLET NODE,System Node Humidity Ratio</td>
-</tr>
-<tr>
-<td>Specific Variable Name</td>
-<td>Mixed Air Node,System Node Mass Flow Rate</td>
-</tr>
-<tr>
-<td>Specific Variable Name</td>
-<td>Outdoor air Inlet Node,System Node Mass Flow Rate</td>
-</tr>
-<tr>
-<td>Variable Name</td>
-<td>Humidifier Water Consumption Rate</td>
-</tr>
-<tr>
-<td>Variable Name</td>
-<td>Humidifier Electric Power</td>
-</tr>
-<tr>
-<td>Variable Name</td>
-<td>Zone Air Relative Humidity</td>
-</tr>
-<tr>
-<td>Variable Name</td>
-<td>Zone Predicted Moisture Load Moisture Transfer Rate</td>
-</tr>
-<tr>
-<td>Termination Line  (optional)</td>
-<td>0</td>
-</tr>
-</table>
-
-Note that the first two lines of the file are “input file� (where to read the output variable values from) and “output file� (where to put the reorganized data). If you have only those two lines in an “rvi� file, the program will use all the available variables on indicated input file to produce the output.
-
-ReadVarsESO takes the input stream but recognizes the date/time information and appropriately places the required data onto the “output file�. Following these lines are a list of variables to be culled from the “input file� and placed onto the output file. “Variable Name� will take all variables matching that description whereas “Specific Variable Name� will only match the full description of the variable. So, in the above example, “Zone Air Temperature� will report air temperatures for all the zones (but available at the HVAC timestep if you choose the “detailed� reporting frequency in your input file) but “AIR LOOP OUTLET NODE� and “COOLING COIL AIR OUTLET NODE� will be the only values reported for the “System Node Temperature� variable (the node temperature is available for all nodes used in the simulation). The termination line (0) is included to terminate the input to the ReadVarsESO program and begin the scanning.
-
-The output from ReadVarsESO is in the form commonly called “comma de-limited� or “comma separated variable�. This format can be read easily in spreadsheet programs, such as Excel™.
-
-Note as described in the “Input for Output� above, only variables as listed on the **eplusout.rdd** file are available for reporting. If you request others, they will become “Warning� messages in the **eplusout.err** file.
-
-```
-** Warning ** The following Output variables were requested but not generated
-**   ~~~   ** because IDF did not contain these elements or misspelled variable name -- check .rdd file
-************* Key=*, VarName=SYSTEM SENSIBLE COOLING RATE
-```
-
-The above message was generated from an IDF that requested reporting of the “SYSTEM SENSIBLE COOLING RATE� but that variable was not available from the components in the execution.
-
-Table 43. Example ReadVarsESO command lines and results
-
-<table class="table table-striped">
-<tr>
-<th>Command Line</th>
-<th>Description/Result</th>
-</tr>
-<tr>
-<td>ReadVarsESO</td>
-<td>Take eplusout.eso and produce an eplusout.csv file with all variables (up to 255) on it</td>
-</tr>
-<tr>
-<td>ReadVarsESO my.rvi</td>
-<td>Use the contents of “my.rvi� to produce the appropriate output file (limited to 255 variables)</td>
-</tr>
-<tr>
-<td>ReadVarsESO my.rvi unlimited</td>
-<td>Use the contents of “my.rvi� to produce the appropriate output file (no longer limited to 255 variables)</td>
-</tr>
-<tr>
-<td>ReadVarsESO my.rvi Monthly</td>
-<td>Use the contents of “my.rvi� to produce the appropriate output file and only produce those variables reported for “monthly� frequency (up to 255 variables)</td>
-</tr>
-<tr>
-<td>ReadVarsESO my.rvi Daily unlimited</td>
-<td>Use the contents of “my.rvi� to produce the appropriate output file and only produce those variables reported for “daily� frequency (no longer limited to 255 variables)</td>
-</tr>
-</table>
-
diff --git a/doc/src/docs/InputOutputReference/06-StandardOutputReports.md b/doc/src/docs/InputOutputReference/06-StandardOutputReports.md
deleted file mode 100644
index 16dfb55d9bf..00000000000
--- a/doc/src/docs/InputOutputReference/06-StandardOutputReports.md
+++ /dev/null
@@ -1,1579 +0,0 @@
-Standard Output Reports
-=======================
-
-The following objects allow standard reports to be defined and utilized in EnergyPlus:
-
-- Output:Table:TimeBins
-
-- Output:Table:Monthly
-
-- Output:Table:Annual
-
-- Output:Table:SummaryReports
-
-- OutputControl:Table:Style
-
-No **Output:Meter** or **Output:Variable** objects need to be specified to use the standard reports. A good set of example reports are available in the StandardReports.idf file in the DataSets directory of EnergyPlus.
-
-Output:Table:TimeBins
----------------------
-
-The Output:Table:TimeBins report shows the amount of time in hours that occurs in different bins for the single specific variable or meter specified. Two different types of binning occur: by month and by hour of the day.
-
-The IntervalStart, IntervalSize and IntervalCount determine the size of the bins for many of the types of reports that can be generated. The IntervalStart value is the lowest value of the first bin. The first bin is for all values greater or equal to IntervalStart and less than IntervalStart+IntervalSize. This gets repeated IntervalCount times. A bin for below the first interval and above the last interval is automatically created. Each table also has totals for the column and the rows. The report produced by Report:Table:TimeBins also indicates the total time simulated (for an annual simulation this would be 8760 hours).
-
-NOTE:  For summed variables, such as meters, the values are divided by the length of the timestep in seconds before binning. For example, the bins for a variable in Joules are reported in Joules per second (Watts). The interval values must then be entered accordingly.
-
-#### Field: Key Value
-
-The Key Value field indicates which instance of a variable is reported. An asterisk indicates that a table would be produced for every key.
-
-#### Field: Variable Name
-
-The variable name to be reported. Reference the eplusout.rdd file for names that are specific to your simulation input file. You do not need to include the units [ ] field in your names here.
-
-#### Field: Interval Start
-
-The lower value of the first bin. The first bin is for all values greater or equal to the IntervalStart and less than IntervalStart + IntervalSize. See note above regarding summed variables.
-
-#### Field: Interval Size
-
-The amount by which each bin range is to increase, i.e. the difference between the upper and lower limits of each bin. See note above regarding summed variables.
-
-#### Field: Interval Count
-
-The number of bins desired.
-
-#### Field: Schedule Name
-
-Optional schedule name. If left blank, binning is performed for all hours simulated. If a schedule is specified, binning is performed for non-zero hours in the schedule.
-
-#### Field: Variable Type
-
-This field is used to indicate the kind of units that may be associated with the variable. It is used by IDF Editor to display the appropriate SI and IP units for the Interval Start and Interval Size values. The available options are shown below.
-
-- Energy
-
-- Temperature
-
-- Flowrate
-
-- Demand
-
-An example of a time bins input object follows.
-
-```idf
-Output:Table:TimeBins,
-  *,                     ! Key Value
-  Electricity:HVAC,      ! Variable Name
-  4000000,               ! Interval Start
-  500000,                ! Interval Size
-  20;                    ! Interval Count
-```
-
-Output:Table:Monthly
---------------------
-
-The Output:Table:Monthly object provides a generic method of setting up tables of monthly results. These tables are good for creating reports that broadly summarize the building performance. At the bottom of the tables, three rows are added for the sum or average depending on the type of variable, the maximum and the minimum of each column. The report produced has multiple columns that are each defined using a repeated group of fields. The fields for the variable name and the aggregation type can be repeated for any number of columns. A single Output:Table:Monthly object often produces multiple tables in the output. A table is produced for every “key� for a particular output variable. A single table of results shows values only for a specific “key�. The exception to this are environment variables, such as outdoor air temperature, that are included in each table, no matter what the key.
-
-#### Field: Name
-
-The Name field allows the user to give the output table a label that is shown in the output file.
-
-#### Field: Digits After Decimal
-
-The Digits After Decimal field is a numeric value that indicates how many digits after the decimal point should be shown on the table of values.
-
-#### Field Set: Variable or Meter and Aggregation Type
-
-The VariableOrMeterName field and the AggregationType field may be repeated for each column desired in the monthly report. These two fields define each column of the report. The IDD object has been set up to allow up to 25 columns. This object is extensible, so the number of columns may be increased by editing the IDD file and adding the desired number of fields at the end of the object.
-
-#### Field: Variable or Meter &lt;\#&gt; Name
-
-The remainder of this input object consists of pairs of fields that can be repeatedVariable Or Meter Name fields contain the name of a variable (see Output:Variable and eplusout.rdd), meter (see Output:Meter and eplusout.mdd), or schedule. This value is shown on a monthly basis using the aggregation method specified. If the selected name is used for both a variable or a meter and a schedule name, the variable or meter will be used.
-
-#### Field: Aggregation Type for Variable or Meter &lt;\#&gt;
-
-The aggregation type determines how the variable is aggregated in the table. The choices for aggregation type are described below:
-
-Simple Aggregation Types
-
-**SumOrAverage** – For “sum� type variables adds up the values for each timestep and reports the sum of the value monthly. For “average� type variables, the value shown will be the average for the month. SumOrAverage is probably the most common choice for aggregation type.
-
-**Maximum** – Reports the maximum value and the time that the maximum value occurred. When the maximum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the maximum for a variable in Joules is reported in Watts.
-
-**Minimum** – Reports the minimum value and the time that the minimum value occurred. When the minimum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the minimum for a variable in Joules is reported in Watts.
-
-**HoursNonZero** – The HoursNonZero option adds up the elapsed time during the month that this variable is non-zero and would be appropriate to determine the number of hour that a fan operates.
-
-**HoursZero** – The HoursZero option adds up the elapsed time during the month that this variable has a zero value and would be appropriate to determine the number of hour that a fan does not operate.
-
-**HoursPositive** – The HoursPositive option adds up the elapsed time during the month that this variable has a positive value. Hours with a zero value are not included.
-
-**HoursNonPositive** – The HoursNonPositive option adds up the elapsed time during the month that this variable has non-positive value. Hours with a negative value and hours with a zero value are all included.
-
-**HoursNegative** – The HoursNegative option adds up the elapsed time during the month that this variable has a negative value. Hours with a zero value are not included.
-
-**HoursNonNegative** – The HoursNonNegative option adds up the elapsed time during the month that this variable has non-negative value. Hours with a positive value and hours with a zero value are all included.
-
-*Advanced Aggregation Types*
-
-The advanced aggregation types are described below. These aggregation types rely on doing an operation on the current variable but only during the time or times defined by a previously defined field. The ValueWhenMaxOrMin displays the value of one variable at the same time as the maximum or minimum is set on a previous field that is defined as either a maximum or minimum. The “Hours—“ aggregation types display then number of hours that a variable meets a condition. The “—DuringHoursShown� aggregation types perform those aggretations but instead of for all the hours in the month, only for the hours that the previous “Hours—“ entry applies. Multiple “—DuringHoursShown� after an “Hours—“ will all be based on that single “Hours—“ entry, in fact the “—DuringHoursShown� is based on the next column to the left that contains an “Hours—“ entry even if other types of aggregations are used in intermediate columns. Order of the variables in the report is important when using the advanced aggregation types since they often depend on a previous entry.
-
-**ValueWhenMaximumOrMinimum** – The ValueWhenMaximumOrMinimum option looks at the previous variable in the report that sets a maximum or minimum and displays the value of the current variable at that same timestep. Order of the variables in the report is important when using ValueWhenMaxMin. This can be used, for example, when an outdoor temperature should be reported for the time of the maximum cooling load.
-
-**SumOrAverageDuringHoursShown** – Provides the sum or average of the named variable when during the hours that the previous variable displayed with any of the aggregation types starting with “Hours�. For “sum� type variables adds up the values for each timestep and reports the sum of the value monthly during the hours reported on the previous variable. For “average� type variables, the value shown will be the average for the month during the hours reported on the previous variable. Order of the variables in the report is important when using this aggregation type.
-
-**MaximumDuringHoursShown** – Reports the maximum value and the time that the maximum value occurred but only during the hours reported with the previous “hours-“ aggregation type. When the maximum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the maximum for a variable in Joules is reported in Watts. Order of the variables in the report is important when using this aggregation type.
-
-**MinimumDuringHoursShown** - Reports the minimum value and the time that the minimum value occurred but only during the hours reported with the previous “hours-“ aggregation type. When the minimum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the minimum for a variable in Joules is reported in Watts. Order of the variables in the report is important when using this aggregation type.
-
-An example of this object follows.
-
-```idf
-Output:Table:Monthly,
-  Building Monthly Cooling Load Report,               ! Name
-  3,                                                  ! Digits After Decimal
-  Zone Air System Sensible Cooling Energy,                   ! Variable or Meter 1 Name
-  SumOrAverage,                                       ! Aggregation Type for Variable or Meter 1
-  Zone Air System Sensible Cooling Energy,                   ! Variable or Meter 2 Name
-  Maximum,                                            ! Aggregation Type for Variable or Meter 2
-  Site Outdoor Air Drybulb Temperature,                                   ! Variable or Meter 3 Name
-  ValueWhenMaxMin;                                    ! Aggregation Type for Variable or Meter 3
-```
-
-Output:Table:Annual
--------------------
-
-The Output:Table:Annual object provides a generic method of setting up tables of annual results with each row corresponding to an instance of an object. These tables are good for creating reports that broadly summarize the building performance. At the bottom of the tables, three rows are added for the sum or average depending on the type of variable, the maximum and the minimum of each column. The report produced has multiple columns that are each defined using a repeated group of fields. The fields for the variable name and the aggregation type can be repeated for any number of columns. If the variables from different type of objects are specified in a single Output:Table:Annual, all the object names for each type of objects will be shown as rows. Variables that don't apply for certain objects will be left blank for that cell.  
-
-#### Field: Name
-
-The Name field allows the user to give the output table a label that is shown in the output file.
-
-#### Field: Filter
-
-An optional text string that is compared to the names of the objects referenced by the variables and if they match are included in the table. A footnote will appear that indicates that the objects shown may not be all the objects that of that type that occur in the file. 
-
-#### Field: Schedule Name
-
-Optional schedule name. If left blank, aggregation is performed for all hours simulated. If a schedule is specified, aggregation is performed for non-zero hours in the schedule.
-
-#### Field Set: Variable and Aggregation Type
-
-The Variable Name field and the Aggregation Type field may be repeated for each column desired in the report. These two fields define each column of the report. The IDD object has been set up to allow up to 25 columns. This object is extensible, so the number of columns may be increased by editing the IDD file and adding the desired number of fields at the end of the object.
-
-#### Field: Variable or Meter &lt;\#&gt; Name
-
-The remainder of this input object consists of pairs of fields that can be repeatedVariable Or Meter Name fields contain the name of a variable (see Output:Variable and eplusout.rdd), meter (see Output:Meter and eplusout.mdd), or schedule. This value is shown using the aggregation method specified. If the selected name is used for both a variable or a meter and a schedule name, the variable or meter will be used.
-
-#### Field: Aggregation Type for Variable or Meter &lt;\#&gt;
-
-The aggregation type determines how the variable is aggregated in the table. The choices for aggregation type are described below:
-
-*Simple Aggregation Types*
-
-**SumOrAverage** – For “sum� type variables adds up the values for each timestep and reports the sum of the value. For “average� type variables, the value shown will be the average for the month. SumOrAverage is probably the most common choice for aggregation type.
-
-**Maximum** – Reports the maximum value and the time that the maximum value occurred. When the maximum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the maximum for a variable in Joules is reported in Watts.
-
-**Minimum** – Reports the minimum value and the time that the minimum value occurred. When the minimum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the minimum for a variable in Joules is reported in Watts.
-
-**HoursNonZero** – The HoursNonZero option adds up the elapsed time during the month that this variable is non-zero and would be appropriate to determine the number of hour that a fan operates.
-
-**HoursZero** – The HoursZero option adds up the elapsed time during the month that this variable has a zero value and would be appropriate to determine the number of hour that a fan does not operate.
-
-**HoursPositive** – The HoursPositive option adds up the elapsed time during the month that this variable has a positive value. Hours with a zero value are not included.
-
-**HoursNonPositive** – The HoursNonPositive option adds up the elapsed time during the month that this variable has non-positive value. Hours with a negative value and hours with a zero value are all included.
-
-**HoursNegative** – The HoursNegative option adds up the elapsed time during the month that this variable has a negative value. Hours with a zero value are not included.
-
-**HoursNonNegative** – The HoursNonNegative option adds up the elapsed time during the month that this variable has non-negative value. Hours with a positive value and hours with a zero value are all included.
-
-**HourInTenBinsMinToMax** - Creates 10 columns for the specified variable and shows the number of hours in each of 10 bins based on the minimum and maximum value. The bin sizes will be rounded up to the next most signficant digit value (if the min is 0 and the max is 28786.3, the bin size would be 3000 not 2878.63). A table of the bin ranges would be generated below the main table when this option is selected.
-
-**HourInTenBinsZeroToMax** - Creates 11 columns for the specified variable and shows the number of hours in each of 10 bins from zero to the maximum value and a bin for hours below zero. The bin sizes will be rounded up to the next most significant digit value (if the min is 0 and the max is 28786.3, the bin size would be 3000 not 2878.63). A table of the bin ranges would be generated below the main table when this option is selected. 
-
-**HourInTenBinsMinToZero** - Creates 11 columns for the specified variable and shows the number of hours in each of 10 bins from zero to the minimum value and a bin for hours above zero. The bin sizes will be rounded up to the next most significant digit value (if the min is 0 and the min is -28786.3, the bin size would be 3000 not 2878.63). A table of the bin ranges would be generated below the main table when this option is selected.
-
-*Advanced Aggregation Types*
-
-The advanced aggregation types are described below. These aggregation types rely on doing an operation on the current variable but only during the time or times defined by a previously defined field. The ValueWhenMaxOrMin displays the value of one variable at the same time as the maximum or minimum is set on a previous field that is defined as either a maximum or minimum. The “Hours—“ aggregation types (not including binning) display then number of hours that a variable meets a condition. The “—DuringHoursShown� aggregation types perform those aggregations but instead of for all the hours in the month, only for the hours that the previous “Hours—“ entry applies. Multiple “—DuringHoursShown� after an “Hours—“ will all be based on that single “Hours—“ entry, in fact the “—DuringHoursShown� is based on the next column to the left that contains an “Hours—“ entry even if other types of aggregations are used in intermediate columns. Order of the variables in the report is important when using the advanced aggregation types since they often depend on a previous entry.
-
-**ValueWhenMaximumOrMinimum** – The ValueWhenMaximumOrMinimum option looks at the previous variable in the report that sets a maximum or minimum and displays the value of the current variable at that same timestep. Order of the variables in the report is important when using ValueWhenMaxMin. This can be used, for example, when an outdoor temperature should be reported for the time of the maximum cooling load.
-
-**SumOrAverageDuringHoursShown** – Provides the sum or average of the named variable when during the hours that the previous variable displayed with any of the aggregation types starting with “Hours�. For “sum� type variables adds up the values for each timestep and reports the sum of the value during the hours reported on the previous variable. For “average� type variables, the value shown will be the average for the month during the hours reported on the previous variable. Order of the variables in the report is important when using this aggregation type.
-
-**MaximumDuringHoursShown** – Reports the maximum value and the time that the maximum value occurred but only during the hours reported with the previous “hours-“ aggregation type. When the maximum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the maximum for a variable in Joules is reported in Watts. Order of the variables in the report is important when using this aggregation type.
-
-**MinimumDuringHoursShown** - Reports the minimum value and the time that the minimum value occurred but only during the hours reported with the previous “hours-“ aggregation type. When the minimum option is used with a summed variable the value is divided by the length of the timestep in seconds. For example, the minimum for a variable in Joules is reported in Watts. Order of the variables in the report is important when using this aggregation type.
-
-
-#### Field: Digits After Decimal for Variable or Meter &lt;\#&gt;
-
-The Digits After Decimal field is a numeric value that indicates how many digits after the decimal point should be shown for that column.
-
-An example of this object follows.
-
-```idf
-    Output:Table:Annual,
-    Custom Annual Window Report,  !- Name
-    , !- Report Group Name
-    , !- Filter
-    , !- Schedule Name
-    SURFACE WINDOW TRANSMITTED SOLAR RADIATION RATE,  !- Variable, Meter, EMS Int Var, IDF field Name 1
-    SumOrAverage,  !- Aggregation Type for 1
-    2,  !- Digits After Decimal for 1
-    SURFACE WINDOW TRANSMITTED BEAM SOLAR RADIATION RATE,  !- Variable, Meter, EMS Int Var, IDF field Name 2
-    SumOrAverage,  !- Aggregation Type for 2
-    2,  !- Digits After Decimal for 2
-    SURFACE WINDOW TRANSMITTED DIFFUSE SOLAR RADIATION RATE,  !- Variable, Meter, EMS Int Var, IDF field Name 3
-    SumOrAverage,  !- Aggregation Type for 3
-    2,  !- Digits After Decimal for 3
-    SURFACE WINDOW HEAT GAIN RATE,  !- Variable, Meter, EMS Int Var, IDF field Name 4
-    SumOrAverage,  !- Aggregation Type for 4
-    2,  !- Digits After Decimal for 4
-    ACE WINDOW HEAT LOSS RATE,  !- Variable, Meter, EMS Int Var, IDF field Name 5
-    SumOrAverage,  !- Aggregation Type for 5
-    2;  !- Digits After Decimal for 5
-```
-
-
-
-Output:Table:SummaryReports
----------------------------
-
-The Output:Table:SummaryReports object controls which predefined tabular reports are produced.  The easiest option is to specify “AllSummary� which will produce all of the summary reports described in this section and does not include the Zone Component Load report. In addition, “AllMonthly� will produce all of the monthly reports described. If all predefined reports are needed. “AllSummaryAndMonthly� shows all of the summary and monthly predefined reports and does not include the Zone Component Load report. The “AllSummaryAndSizingPeriod� option and “AllSummaryMonthlyAndSizingPeriod� option are similar and add the Zone Component Load report. Including the Zone Component Load Summary report may increase the simulation run time.
-
-#### Field: Report &lt;\#&gt; Name
-
-All of the fields in the Output:Table:SummaryReports are the same. A long list of predefined summary reports is available by entering one of the available key choices described below. Each one indicates the name of the predefined reports that should be output. The input AllSummary will cause all the reports described below to be created.  The Report &lt;\#&gt; Name field can be repeated.
-
-### Predefined Annual Summary Reports
-
-#### Annual Building Utility Performance Summary (sometimes called ABUPS)
-
-The Annual Building Utility Performance Summary report often called ABUPS – (key: AnnualBuildingUtilityPerformanceSummary) produces a report that is an overall summary of the utility consumption of the building. It contains a number of subtables that are each described below.
-
-- Site and Source Energy – Indicates the total site and source energy use. For electricity the net electricity from the utility is used for the electric contribution. The site to source conversion factors are based on those entered by the user. These are entered in the EnvironmentalImpactFactors object and FuelFactors objects.
-
-- Building Area – Shows the total floorspace of the building and the conditioned floorspace.
-
-- End Uses – This shows the total use of electricity, natural gas, other fuels, purchased cooling, purchased heating and water for each major end-use category. The end-use categories are Heating, Cooling, Interior Lighting, Exterior Lighting, Interior Equipment, Exterior Equipment, Fans, Pumps, Heat Rejection, Humidification, Heat Recovery, Hot Water, Refrigeration, and Generators. Not all fuels have corresponding end uses. The values in this sub-table are from output meters. To determine which components are attached to each end-use meter, consult the meter details output file (\*.mtd). The source of the resource does not affect this table – the amount of electricity used for lights does not change if the electricity is from the utility or from an on-site generator. The Other Fuel column includes fuel oil\#1, fuel oil\#2, gasoline, coal, propane, diesel, otherfuel1 and otherfuel2. The district heating column also  includes steam.
-
-- End Uses By Subcategory – Shows a breakdown of the major end uses by user-defined category. If an end-use subcategory was not input for an object, it is automatically added to the General subcategory for that major end-use category.
-
-- Utility Use Per Floor Area – These two sub-tables show the results from the end-uses table divided by the total floor area defined for the building and for the total conditioned floor area. Only three categories for end-uses are used for these sub-tables, lighting, HVAC and other. HVAC includes fans, pumps, heating, cooling, heat rejection, humidification, and domestic hot water heating. The Other Fuel column includes fuel oil\#1, fuel oil\#2, gasoline, coal, propane, diesel, otherfuel1 and otherfuel2. The district heating column also  includes steam.
-
-- Electric Loads Satisfied – Shows the different methods that electric loads are satisfied in the building. The values shown for on site power generation are: Fuel-Fired Power Generation, High Temperature Geothermal, Photovoltaic Power, and Wind Power. The flows to and from the electric utility are shown next and finally the total electricity used at the site is compared to the total generated on site plus the net amount from the electric utility. The percentages shown are based on the total electricity used by the end-uses. Note that High Temperature Geothermal and Wind Power are not yet implemented in EnergyPlus.
-
-- On-Site Thermal Sources – Shows the on-site thermal sources of energy such as Water-Side Heat Recovery, Air to Air Heat Recovery for Cooling, Air to Air Heat Recovery for Heating, High-Temperature Geothermal, Solar Water Thermal, Solar Air Thermal. Note that High-Temperature Geothermal Solar Water Thermal, and Solar Air Thermal are not yet implemented in EnergyPlus.
-
-- Water Loads Summary – Shows the different methods the water loads were satisfied. This table shows all zeros because water use is not yet implemented in EnergyPlus.
-
-#### Input Verification and Results Summary (or IVRS)
-
-The Input Verification and Results Summary report (key: InputVerificationandResultsSummary) produces a report with several tables including:
-
-- General which includes general information like the Program Version and Build, Weather, Latitude, Longitude, Elevation, Time Zone, North Axis Angle, and Hours Simulated.
-
-- Window-Wall Ratio table for envelope which includes the wall area, the window area and the ratio of the two. These are computed for all walls and for walls that are oriented generally north, south, east and west. All walls are categorized into one of these four cardinal directions. This is computed for walls that have a tilt of 60 to 120 degrees.
-
-- Skylight-Roof Ratio table for envelope which includes the roof area and the skylight area and the ratio of the two. This includes all surfaces with a tilt of less than 60 degrees.
-
-- Zone Summary includes internal load summary for each zone including area, if conditioned, volume, multipliers, gross wall area, window area, design lighting, design people, design plug and process.
-
-#### Source Energy End Use Components Summary
-
-The Source Energy End Use Components Summary report produces a report (key: SourceEnergyEndUseComponentsSummary) that includes three tables. These tables display source energy by fuel type that is calculated based on site to source energy factors specified by the user in the EnvironmentalImpactFactors and FuelFactors objects. The last two tables display the source energy in terms of area normalized metrics. Following is a description of each table:
-
-- Source Energy End Use Components – This shows the total use of source electricity, source natural gas, source values of other fuels, source purchased cooling   and purchased heating for each major end-use category. The end-use categories are Heating, Cooling, Interior Lighting, Exterior Lighting, Interior Equipment, Exterior Equipment, Fans, Pumps, Heat Rejection, Humidification, Heat Recovery, Hot Water, Refrigeration, and Generators. Not all fuels have corresponding end uses. The values in this sub-table are from output meters. To determine which components are attached to each end-use meter, consult the meter details output file (\*.mtd). The source of the resource will affect this table – the amount of electricity used for lights will change if the electricity is from the utility or from an on-site generator. The Other Fuel column includes FuelOil\#1, FuelOil\#2, Gasoline, Coal, Propane, Diesel, OtherFuel1 and OtherFuel2. The district heating column also  includes steam.
-
-- Source Energy End Use Components normalized by Conditioned Floor Area – This table shows the total end uses in source energy normalized by conditioned floor area.
-
-- Source Energy End Use Components normalized by Total Floor Area – This table shows the total end uses in source energy normalized by total floor area.
-
-#### Climatic Data Summary
-
-The Climate Summary or Climatic Data Summary report (key: ClimaticDataSummary) produces a report that includes some of the details on each of the design days including: maximum dry-bulb, daily temperature range, humidity value, humidity type, wind speed, and wind direction.
-
-#### Envelope Summary
-
-The Envelope Summary report (key: EnvelopeSummary) produces a report that includes the following tables:
-
-- Opaque which includes all opaque surfaces and includes the name of the construction, reflectance, U-Factor, gross area, azimuth, tilt, cardinal direction.
-
-- Fenestration which includes all non-opaque surfaces and includes the name of the construction, areas (glass, frame, divider, single opening, multiplied openings), U-Factor, SHGC (the solar heat gain coefficient based on summer conditions), visible transmittance, conductance (frame, divider), indication of shade control, the name of the parent surface, azimuth, tilt, cardinal direction.
-
-#### Surface Shadowing Summary
-
-The Surface Shadowing Summary report (key: SurfaceShadowingSummary) produces a report that includes two tables. Note that surfaces starting with “Mir-“ are automatically generated by EnergyPlus and are the mirror images of user entered surfaces.
-
-- Surfaces (Walls, Roofs, etc) that may be Shadowed by Other Surfaces and includes the name of the surface and a list of surfaces that may possibly cast shadows on that named surface. The list of possible shadow casters does not necessarily mean that they do cast shadows during the simulation, only that their relative position makes it possible that shadows from a surface in the list may fall on the named surface.
-
-- Subsurfaces (Windows and Doors) that may be Shadowed by Surfaces, includes the name of the subsurface such as a window or a door and a corresponding list of surfaces that may be casting shadows on the windows and doors.
-
-#### Shading Summary
-
-The Shading Summary report (key: ShadingSummary) produces a report that includes the following tables:
-
-- Sunlit Fraction which shows a list of windows and the fraction of the window that is sunlit for nine specific times of the year. The nine specific times include 9am, noon and 3pm on March 21, June 21, and December 21. These nine times were chosen to represent the range of sun angles. The simulation must include those times for the value to be included in the report.
-
-- Window control includes the names of all windows that have a window shading control (see WindowProperty:ShadingControl) and includes the name of the control, the type of shading, the shaded construction, the kind of control, and if glare control is used.
-
-#### Lighting Summary
-
-The Lighting Summary report (key: LightingSummary) produces a report that includes the following tables:
-
-- Interior Lighting which includes the name of the lights object, the zone that it is used in, the lighting power density, zone area, total power, end use subcategory, schedule name, average hours per week, return air fraction, and whether the zone is conditioned.
-
-- Daylighting which includes the names of the daylighting objects, the zone they are used in, the type of daylighting being used, the control type, the fraction of the lighting controlled, the total power of the lighting installed in the zone and the lighting power that is controlled by the daylighting object.
-
-- Exterior Lighting which includes the name of the ExteriorLights object, the total watts described by the object, if the ExteriorLights uses an astronomical clock or just a schedule, the name of the schedule used, and the average hours per week for the named schedule for the year. The effect of the astronomical clock does not get included in the averaged hours per week shown.
-
-#### Equipment Summary
-
-The Equipment Summary report (key: EquipmentSummary) produces a report that includes some details on the major HVAC equipment present. The report has seven parts.
-
-- Central Plant includes details on chillers, boilers, and cooling towers including the capacity and efficiency. For Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR, IPLV at AHRI standard test conditions is reported.
-
-- Cooling Coils includes the nominal total, sensible and latent capacities, the nominal sensible heat ratio, the nominal efficiency, nominal UA value, and nominal  surface area for each cooling coil. These values are calculated by calling the cooling coil simulation routine with the rated inlet conditions: inlet air dry bulb temperature = 26.67C, inlet air wet bulb temperature = 19.44C, inlet chilled water temperature = 6.67C.
-
-- DX Cooling Coils summarizes the Standard Rating (Net) Cooling Capacity, SEER, EER and IEER values at AHRI standard test. Currently, these values are only reported for coil type = Coil:Cooling:DX:SingleSpeed with condenser type = AirCooled.
-
-- DX Heating Coils summarizes the High Temperature Heating Standard (Net) Rating Capacity, Low Temperature Heating Standard (Net) Rating Capacity and Heating Seasonal Performance Factor (HSPF) values at AHRI standard test. Currently, these values are only reported for coil type = Coil:Heating:DX:SingleSpeed.
-
-- Heating Coils includes the nominal capacity and efficiency for each heating coil. The capacity is calculated by calling the heating coil simulation routine at the rated inlet conditions: inlet air dry bulb temperature = 16.6C, inlet relative humidity = 50%, inlet hot water temperature = 82.2C.
-
-- Fan includes the type of fan, the total efficiency, delta pressure, max flow rate, motor heat in air fraction, and end use.
-
-- Pumps includes the type of pump, control type, head pressure, electric power, and motor efficiency for each pump.
-
-- Service Water Heating includes the type of water heater, the storage volume, input, thermal efficiency, recovery efficiency, and energy factor.
-
-#### HVAC Sizing Summary
-
-The HVAC Sizing Summary report (key: HVACSizingSummary) produces a report that includes the following tables:
-
-- Zone Cooling which includes the following columns for each zone: the calculated design load, the user specified design load, the calculated design air flow, the user specified design air flow, the name of the sizing period, the time of the peak load during the sizing period, the temperature at the time of the peak load during the sizing period, and the humidity ratio at the time of the peak load during the sizing period used.
-
-- Zone Heating which includes the following columns for each zone: the calculated design load, the user specified design load, the calculated design air flow, the user specified design air flow, the name of the sizing period, the time of the peak load during the sizing period, the temperature at the time of the peak load during the sizing period, and the humidity ratio at the time of the peak load during the sizing period used.
-
-- System Design Air Flow Rates which includes the following columns for each air loop: the calculated cooling air flow rate, the user specified air flow rate for cooling, the calculated heating air flow rate, the user specified air flow rate for heating.
-
-- *Note:* values listed as "calculated" are the unaltered result of the zone or system sizing calculations, using the design sizing period weather and schedules specified in the input. Values listed as "user specified" are either the calculated values modified by global or zone sizing factors or values specified with the *flow/zone* or *flow/system* design air flow method.
-
-#### Component Sizing Summary
-
-The Component Sizing Summary report (key: ComponentSizingSummary) produces a report that includes different tables depending on the kinds of HVAC components that exist in the input file. A table is shown for each type of HVAC component that is sized. The table lists the objects of that type of component that appear in the input file and one or more parameters related to that component.  For example, the AirTerminal:SingleDuct:VAV:Reheat component creates a table showing the maximum air flow rate from the sizing calculations and the maximum reheat water flow rate. Another example is the Fan:VariableVolume object which shows a table with both the maximum and minimum flow rates for each fan based on the results from the sizing calculations.
-
-#### Outdoor Air Summary
-
-The Outdoor Air Summary report (key: OutdoorAirSummary) produces a report that includes the following tables:
-
-- Average Outside Air During Occupied Hours table shows for each zone the average and nominal number of occupants, the zone volume, the average air change rate based on mechanical ventilation, infiltration and simple ventilation during occupied hours.
-
-- Minimum Outside Air During Occupied Hours table shows for each zone the average and nominal number of occupants, the zone volume, the minimum air change rate based on mechanical ventilation, infiltration and simple ventilation during occupied hours.
-
-#### System Summary
-
-The System Summary Report (key: SystemSummary) produces a report that includes the following tables:
-
-- Economizer which includes the following columns for each Controller:OutdoorAir object: the high limit shutoff control, the minimum outdoor air flow, the maximum outdoor air flow, if the return air temperature has a control limit, if the return air has an enthalpy limit, the outdoor air temperature limit, and the outdoor air enthalpy limit.
-
-- Demand Controlled Ventilation table is for each Controller:MechanicalVentilation object and shows the name, the nominal outdoor air per person and the nominal outdoor air per zone area.
-
-- Time Not Comfortable Based on Simple ASHRAE 55-2004 table shows how many hours that the space is not comfortable for each zone under the criteria of assuming winter clothes, summer clothes or both summer and winter clothes.  See the People object for more information about this thermal comfort calculation.
-
-- Time Setpoint is Not Met table shows how many hours the space is more than 0.2C from the setpoint during heating and during cooling.  The last two columns indicate those hours that the setpoint is not met while the space is occupied.
-
-#### Adaptive Comfort Summary
-
-The Adaptive Comfort Summary report (key: AdaptiveComfortSummary) produces a report tabulating the sum of occupied hours not meeting adaptive comfort acceptability limits for each relevant People object (People objects for which adaptive comfort calculations are requested). These acceptability limits include ASHRAE Std. 55 80%, ASHRAE Std. 55 90%, CEN-15251 Category I, CEN-15251 Category II, and CEN-15251 Category III.
-
-#### Sensible Heat Gain Summary
-
-The Sensible Heat Gain Summary (key: SensibleHeatGainSummary) provides results for each zone and the overall building for some of the major heat gain components. The first four columns show the loads satisfied by sensible air heating and cooling as well as radiant heating and cooling surfaces in the zone. The heat gains from people, lighting, equipment, windows, interzone air flow, and infiltration are shown when adding heat to the zone and separately when removing heat from the zone (for applicable components). Finally the balance is shown as “Opaque Surface Conduction and Other Heat Addition� and “Opaque Surface Conduction and Other Heat Removal� which is a term indicating the affect of the walls, floors and ceilings/roof to the zone as well as the impact of the delay between heat gains/losses and loads on the HVAC equipment serving the zone.  The following shows each output variable that is used for each column. For each timestep in the simulation, positive values are shown as additions and negative values are shown as removal for most variables.
-
-- HVAC Input Sensible Air Heating
-
-Zone Air Heat Balance System Air Transfer Rate
-
-Zone Air Heat Balance System Convective Heat Gain Rate
-
-- HVAC Input Sensible Air Cooling
-
-Zone Air Heat Balance System Air Transfer Rate
-
-Zone Air Heat Balance System Convective Heat Gain Rate
-
-- HVAC Input Heated Surface Heating
-
-Zone Radiant HVAC Heating Energy
-
-Zone Ventilated Slab Radiant Heating Energy
-
-- HVAC Input Cooled Surface Cooling
-
-Zone Radiant HVAC Cooling Energy
-
-Zone Ventilated Slab Radiant Cooling Energy
-
-- People Sensible Heat Addition
-
-Zone People Sensible Heating Energy
-
-- Lights Sensible Heat Addition
-
-Zone Lights Total Heating Energy
-
-- Equipment Sensible Heat Addition & Equipment Sensible Heat Removal
-
-Zone Electric Equipment Radiant Heating Energy
-
-Zone Gas Equipment Radiant Heating Energy
-
-Zone Steam Equipment Radiant Heating Energy
-
-Zone Hot Water Equipment Radiant Heating Energy
-
-Zone Other Equipment Radiant Heating Energy
-
-Zone Electric Equipment Convective Heating Energy
-
-Zone Gas Equipment Convective Heating Energy
-
-Zone Steam Equipment Convective Heating Energy
-
-Zone Hot Water Equipment Convective Heating Energy
-
-Zone Other Equipment Convective Heating Energy
-
-- Window Heat Addition & Window Heat Removal
-
-Zone Windows Total Heat Gain Energy
-
-- Interzone Air Transfer Heat Addition & Interzone Air Transfer Heat Removal
-
-Zone Air Heat Balance Interzone Air Transfer Rate
-
-- Infiltration Heat Addition & Infiltration Heat Removal
-
-Zone Air Heat Balance Outdoor Air Transfer Rate
-
-The Opaque Surface Conduction and Other Heat Addition and Opaque Surface Conduction and Other Heat Removal columns are also calculated on an timestep basis as the negative value of the other removal and gain columns so that the total for the timestep sums to zero. These columns are derived strictly from the other columns.
-
-#### Zone Component Load Summary
-
-The Zone Component Loads Summary provides an estimate of the heating and cooling peak loads for each zone broken down into various components. This report may help determine which components of the load have the largest impact for the heating and cooling peak design conditions. When specified, the Zone Component Loads Summary report is created for each zone that is conditioned. The difference between the peak design sensible load and the estimated instant + delayed sensible load (as shown in the *Peak Conditions* subtable) is an indication of how consistent the overall total estimate may be to the computed total peak loads for the zone. When the report is called the zone sizing calculations are repeated twice so this may result in longer simulation times.  The key used to obtain this report is ZoneComponentLoadSummary. Since including this report may increase the simulation time, new key options have been added that will display all reports but the Zone Component Load Summary those keys used are AllSummaryButZoneComponentLoad and AllSummaryAndMonthlyButZoneComponentLoad.
-
-The report has four parts:
-
-- Estimated Cooling Peak Load Components
-
-Contains the sensible-instant, sensible-delay, sensible-return air, latent, total and %grand total for people, lights, equipment, refrigeration, water use equipment, HVAC equipment loads, power generation equipment, infiltration, zone ventilation, interzone mixing, roof, interzone ceiling, other roof, exterior wall, interzone wall, ground contact wall, other wall, exterior floor, interzone floor, ground contact floor, other floor, fenestration conduction, fenestration solar, opaque door. The values in the sensible-delay column are estimated using a procedure shown in the Engineering Reference.
-
-- Cooling Peak Conditions
-
-Contains the time of the peak load and the outside dry bulb and wet bulb temperatures as well as the outside humidity ratio for that time. It also shows the zone temperature and relative humidity and humidity ratio for that time.
-
-- Estimated Heating Peak Load Components
-
-Contains the sensible-instant, sensible-delay, sensible-return air, latent, total and %grand total for people, lights, equipment, refrigeration, water use equipment, HVAC equipment loads, power generation equipment, infiltration, zone ventilation, interzone mixing, roof, interzone ceiling, other roof, exterior wall, interzone wall, ground contact wall, other wall, exterior floor, interzone floor, ground contact floor, other floor, fenestration conduction, fenestration solar, opaque door. The values in the sensible-day column are estimated using a procedure shown in the Engineering Reference.
-
-- Heating Peak Conditions
-
-Contains the time of the peak load and the outside dry bulb and wet bulb temperatures as well as the outside humidity ratio for that time. It also shows the zone temperature and the relative humidity and humidity ratio for that time.
-
-#### Standard 62.1 Summary
-
-The Standard 62.1 Summary (key: Standard62.1Summary) produces a report that is consistent with many of the outputs needed when doing calculations consistent with ASHRAE Standard 62.1-2010. The report is generated when sizing calculations are specified. The abbreviations used in the report are consistent with the abbreviations used in Appendix A4 of the Standard. The following tables are part of the report:
-
-- System Ventilation Requirements for Cooling containing: Sum of Zone Primary Air Flow - Vpz-sum, System Population – Ps, Sum of Zone Population - Pz-sum, Occupant Diversity – D, Uncorrected Outdoor Air Intake Airflow – Vou, System Primary Airflow – Vps, Average Outdoor Air Fraction – Xs, System Ventilation Efficiency – Ev, Outdoor Air Intake Flow – Vot, Percent Outdoor Air - %OA.
-
-- System Ventilation Requirements for Heating containing: Sum of Zone Primary Air Flow - Vpz-sum, System Population – Ps, Sum of Zone Population - Pz-sum, Occupant Diversity – D, Uncorrected Outdoor Air Intake Airflow – Vou, System Primary Airflow – Vps, Average Outdoor Air Fraction – Xs, System Ventilation Efficiency – Ev, Outdoor Air Intake Flow – Vot, Percent Outdoor Air - %OA.
-
-- Zone Ventilation Parameters containing: AirLoop Name, People Outdoor Air Rate – Rp,  Zone Population – Pz, Area Outdoor Air Rate – Ra, Zone Floor Area – Az, Breathing Zone Outdoor Airflow – Vbz, Cooling Zone Air Distribution Effectiveness - Ez-clg, Cooling Zone Outdoor Airflow - Voz-clg, Heating Zone Air Distribution Effectiveness - Ez-htg, Heating Zone Outdoor Airflow - Voz-htg.
-
-- System Ventilation Parameters containing: People Outdoor Air Rate – Rp, Sum of Zone Population - Pz-sum, Area Outdoor Air Rate – Ra, Sum of Zone Floor Area - Az-sum, Breathing Zone Outdoor Airflow – Vbz, Cooling Zone Outdoor Airflow - Voz-clg, Heating Zone Outdoor Airflow - Voz-htg.
-
-- Zone Ventilation Calculations for Cooling Design containing: AirLoop Name, Box Type, Zone Primary Airflow – Vpz, Zone Discharge Airflow – Vdz, Minimum Zone Primary Airflow - Vpz-min, Zone Outdoor Airflow Cooling - Voz-clg, Primary Outdoor Air Fraction – Zpz, Primary Air Fraction – Ep, Secondary Recirculation Fraction- Er, Supply Air Fraction- Fa, Mixed Air Fraction – Fb, Outdoor Air Fraction – Fc, Zone Ventilation Efficiency – Evz.
-
-- System Ventilation Calculations for Cooling Design containing: Sum of Zone Primary Airflow - Vpz-sum, System Primary Airflow – Vps, Sum of Zone Discharge Airflow - Vdz-sum, Minimum Zone Primary Airflow - Vpz-min, Zone Outdoor Airflow Cooling - Voz-clg, Zone Ventilation Efficiency - Evz-min.
-
-- Zone Ventilation Calculations for Heating Design containing: AirLoop Name, Box Type, Zone Primary Airflow – Vpz, Zone Discharge Airflow – Vdz, Minimum Zone Primary Airflow - Vpz-min, Zone Outdoor Airflow Cooling - Voz-clg, Primary Outdoor Air Fraction – Zpz, Primary Air Fraction – Ep, Secondary Recirculation Fraction- Er, Supply Air Fraction- Fa, Mixed Air Fraction – Fb, Outdoor Air Fraction – Fc, Zone Ventilation Efficiency – Evz.
-
-- System Ventilation Calculations for Heating Design containing: Sum of Zone Primary Airflow - Vpz-sum, System Primary Airflow – Vps, Sum of Zone Discharge Airflow - Vdz-sum, Minimum Zone Primary Airflow - Vpz-min, Zone Outdoor Airflow Cooling - Voz-clg, Zone Ventilation Efficiency - Evz-min.
-
-#### Energy Meters Summary
-
-The Energy Meters Summary (key: EnergyMeters) (which is a slight misnomer as some meters may not be strictly energy) provides the annual period (runperiod) results for each meter (reference the meter data dictionary file (.mdd) and/or the meter details file (.mtd). The results are broken out by fuel type (resource type) in this report.
-
-#### LEED Summary
-
-The LEED Summary report provides many of the simulation results required for certification of Energy and Atmosphere Credit 1 Optimized Energy Performance according to the LEED Green Building Rating Systemâ„¢. The report can be produced by specifying LEEDSummary in Output:Table:SummaryReports which is also part of the AllSummary option. Directly following is an example of this report.
-
-#### Object Count Summary
-
-The Object Count Summary provides the count on the number of specific objects in the file. The key used to obtain this report is ObjectCountSummary.
-
-#### Component Cost Economics Summary
-
-The Component Cost Economics Summary provides the construction cost estimate summary for the project. The costs are broken into eight catagories and the reference building costs are provided as a comparison. A second table is also produced that provides line item details with one line for every line item object. The key used to obtain this report is ComponentCostEconomicsSummary.
-
-### Predefined Monthly Summary Reports
-
-The predefined monthly report options are shown below. The key name of the predefined monthly report is all that is needed to have that report appear in the tabular output file. After each report name below are the output variables and aggregation types used. These cannot be modified when using the predefined reports but if changes are desired, a Output:Table:Monthly can be used instead. The StandardReports.idf file in the DataSets directory includes a Output:Table:Monthly that exactly corresponds to the predefined monthly reports shown below. They can be copied into an IDF file and extended if additional variables are desired. A listing of each available key for predefined monthly summary reports follows with a discrption of the variables included.
-
-#### ZoneCoolingSummaryMonthly
-
-- Zone Air System Sensible Cooling Energy (SumOrAverage)
-
-- Zone Air System Sensible Cooling Rate (Maximum)
-
-- Site Outdoor Air Drybulb Temperature (ValueWhenMaxMin)
-
-- Site Outdoor Air Wetbulb Temperature (ValueWhenMaxMin)
-
-- Zone Total Internal Latent Gain Energy (SumOrAverage)
-
-- Zone Total Internal Latent Gain Energy (Maximum)
-
-- Site Outdoor Air Drybulb Temperature (ValueWhenMaxMin)
-
-- Site Outdoor Air Wetbulb Temperature (ValueWhenMaxMin)
-
-#### ZoneHeatingSummaryMonthly
-
-- Zone Air System Sensible Heating Energy (SumOrAverage)
-
-- Zone Air System Sensible Heating Rate (Maximum)
-
-- Site Outdoor Air Drybulb Temperature (ValueWhenMaxMin)
-
-#### ZoneElectricSummaryMonthly
-
-- Zone Lights Electric Energy (SumOrAverage)
-
-- Zone Lights Electric Energy (Maximum)
-
-- Zone Electric Equipment Electric Energy (SumOrAverage)
-
-- Zone Electric Equipment Electric Energy (Maximum)
-
-#### SpaceGainsMonthly
-
-- Zone People Total Heating Energy (SumOrAverage)
-
-- Zone Lights Total Heating Energy (SumOrAverage)
-
-- Zone Electric Equipment Total Heating Energy (SumOrAverage)
-
-- Zone Gas Equipment Total Heating Energy (SumOrAverage)
-
-- Zone Hot Water Equipment Total Heating Energy (SumOrAverage)
-
-- Zone Steam Equipment Total Heating Energy (SumOrAverage)
-
-- Zone Other Equipment Total Heating Energy (SumOrAverage)
-
-- Zone Infiltration Sensible Heat Gain Energy (SumOrAverage)
-
-- Zone Infiltration Sensible Heat Loss Energy (SumOrAverage)
-
-#### PeakSpaceGainsMonthly
-
-- Zone People Total Heating Energy (Maximum)
-
-- Zone Lights Total Heating Energy (Maximum)
-
-- Zone Electric Equipment Total Heating Energy (Maximum)
-
-- Zone Gas Equipment Total Heating Energy (Maximum)
-
-- Zone Hot Water Equipment Total Heating Energy (Maximum)
-
-- Zone Steam Equipment Total Heating Energy (Maximum)
-
-- Zone Other Equipment Total Heating Energy (Maximum)
-
-- Zone Infiltration Sensible Heat Gain Energy (Maximum)
-
-- Zone Infiltration Sensible Heat Loss Energy (Maximum)
-
-#### SpaceGainComponentsAtCoolingPeakMonthly
-
-- Zone Air System Sensible Cooling Rate (Maximum)
-
-- Zone People Total Heating Energy (ValueWhenMaxMin)
-
-- Zone Lights Total Heating Energy (ValueWhenMaxMin)
-
-- Zone Electric Equipment Total Heating Energy (ValueWhenMaxMin)
-
-- Zone Gas Equipment Total Heating Energy (ValueWhenMaxMin)
-
-- Zone Hot Water Equipment Total Heating Energy (ValueWhenMaxMin)
-
-- Zone Steam Equipment Total Heating Energy (ValueWhenMaxMin)
-
-- Zone Other Equipment Total Heating Energy (ValueWhenMaxMin)
-
-- Zone Infiltration Sensible Heat Gain Energy (ValueWhenMaxMin)
-
-- Zone Infiltration Sensible Heat Loss Energy (ValueWhenMaxMin)
-
-#### EnergyConsumptionElectricityNaturalGasMonthly
-
-- Electricity:Facility (SumOrAverage)
-
-- Electricity:Facility (Maximum)
-
-- Gas:Facility (SumOrAverage)
-
-- Gas:Facility (Maximum)
-
-#### EnergyConsumptionElectricityGeneratedPropaneMonthly
-
-- ElectricityProduced:Facility (SumOrAverage)
-
-- ElectricityProduced:Facility (Maximum)
-
-- Propane:Facility (SumOrAverage)
-
-- Propane:Facility (Maximum)
-
-#### EnergyConsumptionDieselFuel OilMonthly
-
-- Diesel:Facility (SumOrAverage)
-
-- Diesel:Facility (Maximum)
-
-- FuelOil\#1:Facility (SumOrAverage)
-
-- FuelOil\#1:Facility (Maximum)
-
-- FuelOil\#2:Facility (SumOrAverage)
-
-- FuelOil\#2:Facility (Maximum)
-
-#### EnergyConsumptionDisctrictHeatingCoolingMonthly
-
-- DistrictCooling:Facility (SumOrAverage)
-
-- DistrictCooling:Facility (Maximum)
-
-- DistrictHeating:Facility (SumOrAverage)
-
-- DistrictHeating:Facility (Maximum)
-
-#### EnergyConsumptionCoalGasolineMonthly
-
-- Coal:Facility (SumOrAverage)
-
-- Coal:Facility (Maximum)
-
-- Gasoline:Facility (SumOrAverage)
-
-- Gasoline:Facility (Maximum)
-
-#### EnergyConsumptionOtherFuelsMonthly
-
-- OtherFuel1:Facility (SumOrAverage)
-
-- OtherFuel1:Facility (Maximum)
-
-- OtherFuel2:Facility (SumOrAverage)
-
-- OtherFuel2:Facility (Maximum)
-
-#### EndUseEnergyConsumptionElectricityMonthly
-
-- InteriorLights:Electricity (SumOrAverage)
-
-- ExteriorLights:Electricity (SumOrAverage)
-
-- InteriorEquipment:Electricity (SumOrAverage)
-
-- ExteriorEquipment:Electricity (SumOrAverage)
-
-- Fans:Electricity (SumOrAverage)
-
-- Pumps:Electricity (SumOrAverage)
-
-- Heating:Electricity (SumOrAverage)
-
-- Cooling:Electricity (SumOrAverage)
-
-- HeatRejection:Electricity (SumOrAverage)
-
-- Humidifier:Electricity (SumOrAverage)
-
-- HeatRecovery:Electricity (SumOrAverage)
-
-- WaterSystems:Electricity (SumOrAverage)
-
-- Cogeneration:Electricity (SumOrAverage)
-
-#### EndUseEnergyConsumptionNaturalGasMonthly
-
-- InteriorEquipment:Gas (SumOrAverage)
-
-- ExteriorEquipment:Gas (SumOrAverage)
-
-- Heating:Gas (SumOrAverage)
-
-- Cooling:Gas (SumOrAverage)
-
-- WaterSystems:Gas (SumOrAverage)
-
-- Cogeneration:Gas (SumOrAverage)
-
-#### EndUseEnergyConsumptionDieselMonthly
-
-- ExteriorEquipment:Diesel (SumOrAverage)
-
-- Cooling:Diesel (SumOrAverage)
-
-- Heating:Diesel (SumOrAverage)
-
-- WaterSystems:Diesel (SumOrAverage)
-
-- Cogeneration:Diesel (SumOrAverage)
-
-#### EndUseEnergyConsumptionFuelOilMonthly
-
-- ExteriorEquipment:FuelOil\#1 (SumOrAverage)
-
-- Cooling:FuelOil\#1 (SumOrAverage)
-
-- Heating:FuelOil\#1 (SumOrAverage)
-
-- WaterSystems:FuelOil\#1 (SumOrAverage)
-
-- Cogeneration:FuelOil\#1 (SumOrAverage)
-
-- ExteriorEquipment:FuelOil\#2 (SumOrAverage)
-
-- Cooling:FuelOil\#2 (SumOrAverage)
-
-- Heating:FuelOil\#2 (SumOrAverage)
-
-- WaterSystems:FuelOil\#2 (SumOrAverage)
-
-- Cogeneration:FuelOil\#2 (SumOrAverage)
-
-#### EndUseEnergyConsumptionCoalMonthly
-
-- ExteriorEquipment:Coal (SumOrAverage)
-
-- Heating:Coal (SumOrAverage)
-
-- WaterSystems:Coal (SumOrAverage)
-
-#### EndUseEnergyConsumptionPropaneMonthly
-
-- ExteriorEquipment:Propane (SumOrAverage)
-
-- Cooling:Propane (SumOrAverage)
-
-- Heating:Propane (SumOrAverage)
-
-- WaterSystems:Propane (SumOrAverage)
-
-- Cogeneration:Propane (SumOrAverage)
-
-#### EndUseEnergyConsumptionGasolineMonthly
-
-- ExteriorEquipment:Gasoline (SumOrAverage)
-
-- Cooling:Gasoline (SumOrAverage)
-
-- Heating:Gasoline (SumOrAverage)
-
-- WaterSystems:Gasoline (SumOrAverage)
-
-- Cogeneration:Gasoline (SumOrAverage)
-
-#### EndUseEnergyConsumptionOtherFuelsMonthly
-
-- ExteriorEquipment:OtherFuel1 (SumOrAverage)
-
-- Cooling:OtherFuel1 (SumOrAverage)
-
-- Heating:OtherFuel1 (SumOrAverage)
-
-- WaterSystems:OtherFuel1 (SumOrAverage)
-
-- Cogeneration:OtherFuel1 (SumOrAverage)
-
-- ExteriorEquipment:OtherFuel1 (SumOrAverage)
-
-- Cooling:OtherFuel2 (SumOrAverage)
-
-- Heating:OtherFuel2 (SumOrAverage)
-
-- WaterSystems:OtherFuel2 (SumOrAverage)
-
-- Cogeneration:OtherFuel2 (SumOrAverage)
-
-#### PeakEnergyEndUseElectricityPart1Monthly
-
-- InteriorLights:Electricity (Maximum)
-
-- ExteriorLights:Electricity (Maximum)
-
-- InteriorEquipment:Electricity (Maximum)
-
-- ExteriorEquipment:Electricity (Maximum)
-
-- Fans:Electricity (Maximum)
-
-- Pumps:Electricity (Maximum)
-
-- Heating:Electricity (Maximum)
-
-#### PeakEnergyEndUseElectricityPart2Monthly
-
-- Cooling:Electricity (Maximum)
-
-- HeatRejection:Electricity (Maximum)
-
-- Humidifier:Electricity (Maximum)
-
-- HeatRecovery:Electricity (Maximum)
-
-- WaterSystems:Electricity (Maximum)
-
-- Cogeneration:Electricity (Maximum)
-
-#### ElectricComponentsOfPeakDemandMonthly
-
-- Electricity:Facility (Maximum)
-
-- InteriorLights:Electricity (ValueWhenMaxMin)
-
-- InteriorEquipment:Electricity (ValueWhenMaxMin)
-
-- ExteriorLights:Electricity (ValueWhenMaxMin)
-
-- ExteriorEquipment:Electricity (ValueWhenMaxMin)
-
-- Fans:Electricity (ValueWhenMaxMin)
-
-- Pumps:Electricity (ValueWhenMaxMin)
-
-- Heating:Electricity (ValueWhenMaxMin)
-
-- Cooling:Electricity (ValueWhenMaxMin)
-
-- HeatRejection:Electricity (ValueWhenMaxMin)
-
-#### PeakEnergyEndUseNaturalGasMonthly
-
-- InteriorEquipment:Gas (Maximum)
-
-- ExteriorEquipment:Gas (Maximum)
-
-- Heating:Gas (Maximum)
-
-- Cooling:Gas (Maximum)
-
-- WaterSystems:Gas (Maximum)
-
-- Cogeneration:Gas (Maximum)
-
-#### PeakEnergyEndUseDieselMonthly
-
-- ExteriorEquipment:Diesel (Maximum)
-
-- Cooling:Diesel (Maximum)
-
-- Heating:Diesel (Maximum)
-
-- WaterSystems:Diesel (Maximum)
-
-- Cogeneration:Diesel (Maximum)
-
-#### PeakEnergyEndUseFuelOilMonthly
-
-- ExteriorEquipment:FuelOil\#1 (Maximum)
-
-- Cooling:FuelOil\#1 (Maximum)
-
-- Heating:FuelOil\#1 (Maximum)
-
-- WaterSystems:FuelOil\#1 (Maximum)
-
-- Cogeneration:FuelOil\#1 (Maximum)
-
-- ExteriorEquipment:FuelOil\#2 (Maximum)
-
-- Cooling:FuelOil\#2 (Maximum)
-
-- Heating:FuelOil\#2 (Maximum)
-
-- WaterSystems:FuelOil\#2 (Maximum)
-
-- Cogeneration:FuelOil\#2 (Maximum)
-
-#### PeakEnergyEndUseCoalMonthly
-
-- ExteriorEquipment:Coal (Maximum)
-
-- Heating:Coal (Maximum)
-
-- WaterSystems:Coal (Maximum)
-
-#### PeakEnergyEndUsePropaneMonthly
-
-- ExteriorEquipment:Propane (Maximum)
-
-- Cooling:Propane (Maximum)
-
-- Heating:Propane (Maximum)
-
-- WaterSystems:Propane (Maximum)
-
-- Cogeneration:Propane (Maximum)
-
-#### PeakEnergyEndUseGasolineMonthly
-
-- ExteriorEquipment:Gasoline (Maximum)
-
-- Cooling:Gasoline (Maximum)
-
-- Heating:Gasoline (Maximum)
-
-- WaterSystems:Gasoline (Maximum)
-
-- Cogeneration:Gasoline (Maximum)
-
-#### PeakEnergyEndUseOtherFuelsMonthly
-
-- ExteriorEquipment:OtherFuel1 (Maximum)
-
-- Cooling:OtherFuel1 (Maximum)
-
-- Heating:OtherFuel1 (Maximum)
-
-- WaterSystems:OtherFuel1 (Maximum)
-
-- Cogeneration:OtherFuel1 (Maximum)
-
-- ExteriorEquipment:OtherFuel1 (Maximum)
-
-- Cooling:OtherFuel1 (Maximum)
-
-- Heating:OtherFuel1 (Maximum)
-
-- WaterSystems:OtherFuel1 (Maximum)
-
-- Cogeneration:OtherFuel1 (Maximum)
-
-#### SetpointsNotMetWithTemperaturesMonthly
-
-- Zone Heating Setpoint Not Met Time (HoursNonZero)
-
-- Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
-
-- Zone Heating Setpoint Not Met While Occupied Time (HoursNonZero)
-
-- Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
-
-- Zone Cooling Setpoint Not Met Time (HoursNonZero)
-
-- Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
-
-- Zone Cooling Setpoint Not Met While Occupied Time (HoursNonZero)
-
-- Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
-
-#### ComfortReportSimple55Monthly
-
-- Zone Thermal Comfort ASHRAE 55 Simple Model Summer Clothes Not Comfortable Time (HoursNonZero)
-
-- Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
-
-- Zone Thermal Comfort ASHRAE 55 Simple Model Winter Clothes Not Comfortable Time (HoursNonZero)
-
-- Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
-
-- Zone Thermal Comfort ASHRAE 55 Simple Model Summer or Winter Clothes Not Comfortable Time (HoursNonZero)
-
-- Zone Mean Air Temperature (SumOrAverageDuringHoursShown)
-
-#### UnglazedTranspiredSolarCollectorSummaryMonthly
-
-- Solar Collector System Efficiency (HoursNonZero)
-
-- Solar Collector System Efficiency (SumOrAverageDuringHoursShown)
-
-- Solar Collector Outside Face Suction Velocity (SumOrAverageDuringHoursShown)
-
-- Solar Collector Sensible Heating Rate (SumOrAverageDuringHoursShown)
-
-#### OccupantComfortDataSummaryMonthly
-
-- Zone People Occupant Count (HoursNonZero)
-
-- Zone Air Temperature (SumOrAverageDuringHoursShown)
-
-- Zone Air Relative Humidity (SumOrAverageDuringHoursShown)
-
-- Zone Thermal Comfort Fanger Model PMV (SumOrAverageDuringHoursShown)
-
-- Zone Thermal Comfort Fanger Model PPD (SumOrAverageDuringHoursShown)
-
-#### ChillerReportMonthly
-
-- Chiller Electric Energy (SumOrAverage)
-
-- Chiller Electric Power (Maximum)
-
-- Chiller Electric Energy (HoursNonZero)
-
-- Chiller Evaporator Cooling Energy (SumOrAverage)
-
-- Chiller Condenser Heat Transfer Energy (SumOrAverage)
-
-- Chiller COP (SumOrAverage)
-
-- Chiller COP (Maximum)
-
-#### TowerReportMonthly
-
-- Tower Fan Electric Consumption (SumOrAverage)
-
-- Tower Fan Electric Consumption (HoursNonZero)
-
-- Cooling Tower Fan Electric Power (Maximum)
-
-- Cooling Tower Heat Transfer Rate (Maximum)
-
-- Cooling Tower Inlet Temperature (SumOrAverage)
-
-- Cooling Tower Outlet Temperature (SumOrAverage)
-
-- Cooling Tower Mass Flow Rate (SumOrAverage)
-
-#### BoilerReportMonthly
-
-- Boiler Heating Energy (SumOrAverage)
-
-- Boiler Gas Consumption (SumOrAverage)
-
-- Boiler Heating Energy (HoursNonZero)
-
-- Boiler Heating Rate (Maximum)
-
-- Boiler Gas Consumption Rate (Maximum)
-
-- Boiler Inlet Temperature (SumOrAverage)
-
-- Boiler Outlet Temperature (SumOrAverage)
-
-- Boiler Mass Flow Rate (SumOrAverage)
-
-- Boiler Ancillary Electric Power (SumOrAverage)
-
-#### DXReportMonthly
-
-- Cooling Coil Total Cooling Energy (SumOrAverage)
-
-- Cooling Coil Electric Energy (SumOrAverage)
-
-- Cooling Coil Total Cooling Energy (HoursNonZero)
-
-- Cooling Coil Sensible Cooling Energy (SumOrAverage)
-
-- Cooling Coil Latent Cooling Energy (SumOrAverage)
-
-- Cooling Coil Crankcase Heater Electric Energy (SumOrAverage)
-
-- Cooling Coil Runtime Fraction (Maximum)
-
-- Cooling Coil Runtime Fraction (Minimum)
-
-- DX Coil Total Cooling Rate (Maximum)
-
-- Cooling Coil Sensible Cooling Rate (Maximum)
-
-- Cooling Coil Latent Cooling Rate (Maximum)
-
-- Cooling Coil Electric Power (Maximum)
-
-- Cooling Coil Crankcase Heater Electric Power (Maximum)
-
-#### WindowReportMonthly
-
-- Surface Window Transmitted Solar Radiation Rate (SumOrAverage)
-
-- Surface Window Transmitted Beam Solar Radiation Rate (SumOrAverage)
-
-- Surface Window Transmitted Diffuse Solar Radiation Rate (SumOrAverage)
-
-- Surface Window Heat Gain Rate (SumOrAverage)
-
-- Surface Window Heat Loss Rate (SumOrAverage)
-
-- Surface Window Inside Face Glazing Condensation Status (HoursNonZero)
-
-- Surface Shading Device Is On Time Fraction (HoursNonZero)
-
-- Surface Storm Window On Off Status (HoursNonZero)
-
-#### WindowEnergyReportMonthly
-
-- Surface Window Transmitted Solar Radiation Energy (SumOrAverage)
-
-- Surface Window Transmitted Beam Solar Radiation Rate Energy (SumOrAverage)
-
-- Surface Window Transmitted Diffuse Solar Radiation Energy (SumOrAverage)
-
-- Surface Window Heat Gain Energy (SumOrAverage)
-
-- Surface Window Heat Loss Energy (SumOrAverage)
-
-#### WindowZoneSummaryMonthly
-
-- Zone Windows Total Heat Gain Rate (SumOrAverage)
-
-- Zone Windows Total Heat Loss Rate (SumOrAverage)
-
-- Zone Windows Total Transmitted Solar Radiation Rate (SumOrAverage)
-
-- Zone Exterior Windows Total Transmitted Beam Solar Radiation Rate (SumOrAverage)
-
-- Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Rate (SumOrAverage)
-
-- Zone Interior Windows Total Transmitted Diffuse Solar Radiation Rate (SumOrAverage)
-
-- Zone Interior Windows Total Transmitted Beam Solar Radiation Rate (SumOrAverage)
-
-#### WindowEnergyZoneSummaryMonthly
-
-- Zone Windows Total Heat Gain Energy (SumOrAverage)
-
-- Zone Windows Total Heat Loss Energy (SumOrAverage)
-
-- Zone Windows Total Transmitted Solar Radiation Energy (SumOrAverage)
-
-- Zone Exterior Windows Total Transmitted Beam Solar Radiation Energy (SumOrAverage)
-
-- Zone Exterior Windows Total Transmitted Diffuse Solar Radiation Energy (SumOrAverage)
-
-- Zone Interior Windows Total Transmitted Diffuse Solar Radiation Energy (SumOrAverage)
-
-- Zone Interior Windows Total Transmitted Beam Solar Radiation Energy (SumOrAverage)
-
-#### AverageOutdoorConditionsMonthly
-
-- Site Outdoor Air Drybulb Temperature (SumOrAverage)
-
-- Site Outdoor Air Wetbulb Temperature (SumOrAverage)
-
-- Site Outdoor Air Dewpoint Temperature (SumOrAverage)
-
-- Wind Speed (SumOrAverage)
-
-- Site Sky Temperature (SumOrAverage)
-
-- Site Diffuse Solar Radiation Rate per Area (SumOrAverage)
-
-- Site Direct Solar Radiation Rate per Area (SumOrAverage)
-
-- Raining (SumOrAverage)
-
-#### OutdoorConditionsMaximumDryBulbMonthly
-
-- Site Outdoor Air Drybulb Temperature (Maximum)
-
-- Site Outdoor Air Wetbulb Temperature (ValueWhenMaxMin)
-
-- Site Outdoor Air Dewpoint Temperature (ValueWhenMaxMin)
-
-- Wind Speed (ValueWhenMaxMin)
-
-- Site Sky Temperature (ValueWhenMaxMin)
-
-- Site Diffuse Solar Radiation Rate per Area (ValueWhenMaxMin)
-
-- Site Direct Solar Radiation Rate per Area (ValueWhenMaxMin)
-
-#### OutdoorConditionsMinimumDryBulbMonthly
-
-- Site Outdoor Air Wetbulb Temperature (ValueWhenMaxMin)
-
-- Site Outdoor Air Dewpoint Temperature (ValueWhenMaxMin)
-
-- Wind Speed (ValueWhenMaxMin)
-
-- Site Sky Temperature (ValueWhenMaxMin)
-
-- Site Diffuse Solar Radiation Rate per Area (ValueWhenMaxMin)
-
-- Site Direct Solar Radiation Rate per Area (ValueWhenMaxMin)
-
-#### OutdoorConditionsMaximumWetBulbMonthly
-
-- Site Outdoor Air Wetbulb Temperature (Maximum)
-
-- Site Outdoor Air Drybulb Temperature (ValueWhenMaxMin)
-
-- Site Outdoor Air Dewpoint Temperature (ValueWhenMaxMin)
-
-- Wind Speed (ValueWhenMaxMin)
-
-- Site Sky Temperature (ValueWhenMaxMin)
-
-- Site Diffuse Solar Radiation Rate per Area (ValueWhenMaxMin)
-
-- Site Direct Solar Radiation Rate per Area (ValueWhenMaxMin)
-
-#### OutdoorConditionsMaximumDewPointMonthly
-
-- Site Outdoor Air Dewpoint Temperature (Maximum)
-
-- Site Outdoor Air Drybulb Temperature (ValueWhenMaxMin)
-
-- Site Outdoor Air Wetbulb Temperature (ValueWhenMaxMin)
-
-- Wind Speed (ValueWhenMaxMin)
-
-- Site Sky Temperature (ValueWhenMaxMin)
-
-- Site Diffuse Solar Radiation Rate per Area (ValueWhenMaxMin)
-
-- Site Direct Solar Radiation Rate per Area (ValueWhenMaxMin)
-
-#### OutdoorGroundConditionsMonthly
-
-- Site Ground Temperature (SumOrAverage)
-
-- Site Surface Ground Temperature (SumOrAverage)
-
-- Site Deep Ground Temperature (SumOrAverage)
-
-- Site Mains Water Temperature (SumOrAverage)
-
-- Site Ground Reflected Solar Radiation Rate per Area (SumOrAverage)
-
-- Snow On Ground (SumOrAverage)
-
-#### WindowACReportMonthly
-
-- Zone Window Air Conditioner Total Cooling Energy (SumOrAverage)
-
-- Zone Window Air Conditioner Electric Energy (SumOrAverage)
-
-- Zone Window Air Conditioner Total Cooling Energy (HoursNonZero)
-
-- Zone Window Air Conditioner Sensible Cooling Energy (SumOrAverage)
-
-- Zone Window Air Conditioner Latent Cooling Energy (SumOrAverage)
-
-- Zone Window Air Conditioner Total Cooling Rate (Maximum)
-
-- Zone Window Air Conditioner Sensible Cooling Rate (ValueWhenMaxMin)
-
-- Zone Window Air Conditioner Latent Cooling Rate (ValueWhenMaxMin)
-
-- Zone Window Air Conditioner Electric Power (ValueWhenMaxMin)
-
-#### WaterHeaterReportMonthly
-
-- Water Heater Total Demand Energy (SumOrAverage)
-
-- Water Heater Use Side Heat Transfer Energy (SumOrAverage)
-
-- Water Heater Burner Heating Energy (SumOrAverage)
-
-- Water Heater Gas Consumption (SumOrAverage)
-
-- Water Heater Total Demand Energy (HoursNonZero)
-
-- Water Heater Loss Demand Energy (SumOrAverage)
-
-- Water Heater Heat Loss Energy (SumOrAverage)
-
-- Water Heater Tank Temperature (SumOrAverage)
-
-- Water Heater Heat Recovery Supply Energy (SumOrAverage)
-
-- Water Heater Source Side Heat Transfer Energy (SumOrAverage)
-
-#### GeneratorReportMonthly
-
-- Generator Produced Electric Energy (SumOrAverage)
-
-- Generator Diesel Energy (SumOrAverage)
-
-- Generator Gas Consumption (SumOrAverage)
-
-- Generator Produced Electric Energy (HoursNonZero)
-
-- Generator Total Heat Recovery (SumOrAverage)
-
-- Generator Jacket Heat Recovery Energy (SumOrAverage)
-
-- Generator Lube Heat Recovery Energy (SumOrAverage)
-
-- Generator Exhaust Heat Recovery Energy (SumOrAverage)
-
-- Generator Exhaust Air Temperature (SumOrAverage)
-
-#### DaylightingReportMonthly
-
-- Site Exterior Beam Normal Illuminance (HoursNonZero)
-
-- Daylighting Lighting Power Multiplier (SumOrAverageDuringHoursShown)
-
-- Daylighting Lighting Power Multiplier (MinimumDuringHoursShown)
-
-- Daylighting Reference Point 1 Illuminance (SumOrAverageDuringHoursShown)
-
-- Daylighting Reference Point 1 Glare Index (SumOrAverageDuringHoursShown)
-
-- Daylighting Reference Point 2 Illuminance (SumOrAverageDuringHoursShown)
-
-- Daylighting Reference Point 2 Glare Index (SumOrAverageDuringHoursShown)
-
-- Daylighting Reference Point 1 Glare Index Setpoint Exceeded Time
-
-- Daylighting Reference Point 2 Glare Index Setpoint Exceeded Time
-
-- Daylighting Reference Point 1 Daylight Illuminance Setpoint Exceeded Time
-
-- Daylighting Reference Point 2 Daylight Illuminance Setpoint Exceeded Time
-
-#### CoilReportMonthly
-
-- Heating Coil Heating Energy (SumOrAverage)
-
-- Heating Coil Heating Rate (Maximum)
-
-- Cooling Coil Total Cooling Energy (SumOrAverage)
-
-- Cooling Coil Sensible Cooling Energy (SumOrAverage)
-
-- Cooling Coil Total Cooling Rate (Maximum)
-
-- Cooling Coil Sensible Cooling Rate (ValueWhenMaxMin)
-
-- Cooling Coil Wetted Area Fraction (SumOrAverage)
-
-#### PlantLoopDemandReportMonthly
-
-- Plant Supply Side Cooling Demand Rate (SumOrAverage)
-
-- Plant Supply Side Cooling Demand Rate (Maximum)
-
-- Plant Supply Side Heating Demand Rate (SumOrAverage)
-
-- Plant Supply Side Heating Demand Rate (Maximum)
-
-#### FanReportMonthly
-
-- Fan Electric Consumption (SumOrAverage)
-
-- Fan Rise in Air Temperature (SumOrAverage)
-
-- Fan Electric Power (Maximum)
-
-- Fan Rise in Air Temperature (ValueWhenMaxMin)
-
-#### PumpReportMonthly
-
-- Pump Electric Energy (SumOrAverage)
-
-- Pump Fluid Heat Gain Energy (SumOrAverage)
-
-- Pump Electric Power (Maximum)
-
-- Pump Shaft Power (ValueWhenMaxMin)
-
-- Pump Fluid Heat Gain Rate (ValueWhenMaxMin)
-
-- Pump Outlet Temperature (ValueWhenMaxMin)
-
-- Pump Mass Flow Rate (ValueWhenMaxMin)
-
-#### CondLoopDemandReportMonthly
-
-- Plant Supply Side Cooling Demand Rate (SumOrAverage)
-
-- Plant Supply Side Cooling Demand Rate (Maximum)
-
-- Plant Supply Side Inlet Temperature (ValueWhenMaxMin)
-
-- Plant Supply Side Outlet Temperature (ValueWhenMaxMin)
-
-- Plant Supply Side Heating Demand Rate (SumOrAverage)
-
-- Plant Supply Side Heating Demand Rate (Maximum)
-
-#### ZoneTemperatureOscillationReportMonthly
-
-- Zone Oscillating Temperatures Time (HoursNonZero)
-
-- Zone People Occupant Count (SumOrAverageDuringHoursShown)
-
-#### AirLoopSystemEnergyAndWaterUseMonthly
-
-- Air System Hot Water Energy (SumOrAverage)
-
-- Air System Steam Energy (SumOrAverage)
-
-- Air System Chilled Water Energy (SumOrAverage)
-
-- Air System Electric Energy (SumOrAverage)
-
-- Air System Gas Energy (SumOrAverage)
-
-- Air System Water Volume (SumOrAverage)
-
-#### AirLoopSystemComponentLoadsMonthly
-
-- Air System Fan Air Heating Energy (SumOrAverage)
-
-- Air System Cooling Coil Total Cooling Energy (SumOrAverage)
-
-- Air System Heating Coil Total Heating Energy (SumOrAverage)
-
-- Air System Heat Exchanger Total Heating Energy (SumOrAverage)
-
-- Air System Heat Exchanger Total Cooling Energy (SumOrAverage)
-
-- Air System Humidifier Total Heating Energy (SumOrAverage)
-
-- Air System Evaporative Cooler Total Cooling Energy (SumOrAverage)
-
-- Air System Desiccant Dehumidifier Total Cooling Energy (SumOrAverage)
-
-#### AirLoopSystemComponentEnergyUseMonthly
-
-- Air System Fan Electric Energy (SumOrAverage)
-
-- Air System Heating Coil Hot Water Energy (SumOrAverage)
-
-- Air System Cooling Coil Chilled Water Energy (SumOrAverage)
-
-- Air System DX Heating Coil Electric Energy (SumOrAverage)
-
-- Air System DX Cooling Coil Electric Energy (SumOrAverage)
-
-- Air System Heating Coil Electric Energy (SumOrAverage)
-
-- Air System Heating Coil Gas Energy (SumOrAverage)
-
-- Air System Heating Coil Steam Energy (SumOrAverage)
-
-- Air System Humidifier Electric Energy (SumOrAverage)
-
-- Air System Evaporative Cooler Electric Energy (SumOrAverage)
-
-- Air System Desiccant Dehumidifier Electric Energy (SumOrAverage)
-
-#### MechanicalVentilationLoadsMonthly
-
-- Zone Mechanical Ventilation No Load Heat Removal Energy (SumOrAverage)
-
-- Zone Mechanical Ventilation Cooling Load Increase Energy (SumOrAverage)
-
-- Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy (SumOrAverage)
-
-- Zone Mechanical Ventilation Cooling Load Decrease Energy (SumOrAverage)
-
-- Zone Mechanical Ventilation No Load Heat Addition Energy (SumOrAverage)
-
-- Zone Mechanical Ventilation Heating Load Increase Energy (SumOrAverage)
-
-- Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy (SumOrAverage)
-
-- Zone Mechanical Ventilation Heating Load Decrease Energy (SumOrAverage)
-
-- Zone Mechanical Ventilation Air Changes per Hour (SumOrAverage)
-
-
-
-Sample IDF Input – Output:Table:SummaryReports
-
-```idf
-Output:Table:SummaryReports,
-        AllSummary,  !- Report 1 Name
-        AllMonthly;  !- Report 2 Name
-```
-
-OutputControl:Table:Style
--------------------------
-
-The OutputControl:Table:Style object controls how all standardized reports are produced.
-
-#### Field: Column Separator
-
-You have nine different options:
-
-- Comma
-
-- Tab
-
-- Fixed
-
-- HTML
-
-- XML
-
-- CommaAndHTML
-
-- TabAndHTML
-
-- XMLAndHTML
-
-- All
-
-The Comma style produces a text file (eplustbl.csv) with the values of the table separated by commas. This is a good format for importing the results into a spreadsheet. If you do open the file with a spreadsheet, make sure you close the file prior to rerunning EnergyPlus otherwise the file will not be updated.
-
-The Tab style produces a text file (eplustbl.tab) with the values separated by tabs. It is also a good format for using with a spreadsheet program but has the advantage of being more readable in a text editor.
-
-The Fixed style produces a text file (eplustbl.txt) with the values at specific columns. It is the easiest to view using a text editor.
-
-The HTML style produces a file (eplustbl.htm) that can be opened with an internet browser program. The values are shown in a tabular format that is easy to view. One advantage of the HTML style is that the results can be viewed in an internet browser program and EnergyPlus can be rerun and the “refresh� button pressed in the internet browser program to see the new results. . When the HTML style is specified, a Table of Contents for the file is generated and placed near the top of the file after the Annual Building Utility Performance Summary (aka ABUPS) report. The Table of Contents includes the names of each report and links for each table in the file.
-
-The XML style produces a file (eplustbl.xml) that can be opened by any XML editor and many internet browser programs. The XML output is specifically intended for use by other software programs to make it simple to extract specific results.
-
-The last four options combine the previous styles and allow multiple reports with different styles to be produced during a single simulation.
-
-#### Field: Unit Conversion
-
-This field is optional and if not specified defaults to no unit conversions. Four different input options are available:
-
-- None – no conversions performed
-
-- JtoKWH – Joules converted into kWh (1 / 3,600,000)
-
-- JtoMJ – Joules converted into Megajoules (1 / 1,000,000)
-
-- JtoGJ – Joules converted into Gigajoules (1 / 1,000,000,000)
-
-- InchPound – convert all annual, monthly, economics and timebins tabular values to common Inch-Pound equivalent
-
-The current options are limited to just how the energy is being reported. The default is to report energy in the form of Joules but since the magnitude of those numbers for many buildings is very large, these other conversion factors are available.
-
-The JtoKWH, JtoMJ and JtoGJ unit conversion input option applies only to the Output:Table:Monthly reports and partially to the ABUPS report. For ABUPS, the JtoKWH option changes the report but the JtoMJ and JtoGJ options do not change the report since they it is already in MJ/m2 and GJ.. The InchPound unit conversion input option applies to all annual, monthly, timebins and economic reports that appear in the tabular output file.  In addition, this option does not effect the standard eplusout.eso file. The eplusout.eso file may be converted by using the ConvertESOMTR utility.
-
-An example IDF input object follows.
-
-```idf
-OutputControl:Table:Style,
-  Comma,                     ! Column Separator
-   InchPound;                 ! Unit Conversion
-```
-
-
-
-Examples of the tabular reports and descriptions are contained in the Output Details and Examples document.
-
-
-
diff --git a/doc/src/docs/InputOutputReference/07-WeatherData.md b/doc/src/docs/InputOutputReference/07-WeatherData.md
deleted file mode 100644
index 793fb157f6b..00000000000
--- a/doc/src/docs/InputOutputReference/07-WeatherData.md
+++ /dev/null
@@ -1,227 +0,0 @@
-Weather Data
-============
-
-The description of the weather data format (a simple text-based format) is well described in the Auxiliary Programs document and won’t be repeated here. Descriptions here will be pertinent to running the EnergyPlus program but you may wish to peruse the other descriptions as the statistics reports from the weather files may be useful during design and simulation.
-
-Missing Weather File Data
--------------------------
-
-The weather description of data contains “missing� descriptors, a new concept not introduced previously in our IDD conventions. In this case, it will be processed as though those values are “missing� in the weather conversions and/or EnergyPlus weather processing. This may not always be desirable though EnergyPlus will fill in “missing� value with something “appropriate�. Eventually, these missing values will be available through the IDD and users will be able to supply their own values or EnergyPlus will calculate those values (such as radiation and illuminance) that are not a simple value replacement. Until then, the following are used:
-
-Table 44. Missing weather replacement values
-
-<table class="table table-striped">
-<tr>
-<th>Data item</th>
-<th>Supplied Value</th>
-<th>Units</th>
-</tr>
-<tr>
-<td>Dry-bulb Temperature</td>
-<td>6</td>
-<td>C</td>
-</tr>
-<tr>
-<td>Dewpoint Temperature</td>
-<td>3</td>
-<td>C</td>
-</tr>
-<tr>
-<td>Relative Humidity</td>
-<td>50</td>
-<td>%</td>
-</tr>
-<tr>
-<td>Atmospheric Pressure</td>
-<td>Standard** Barometric Pressure (altitude based)</td>
-<td>Pa</td>
-</tr>
-<tr>
-<td>Wind Speed</td>
-<td>2.5</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>Wind Direction</td>
-<td>180</td>
-<td>Deg</td>
-</tr>
-<tr>
-<td>Total Sky Cover</td>
-<td>5</td>
-<td>(tenths)</td>
-</tr>
-<tr>
-<td>Opaque Sky Cover</td>
-<td>5</td>
-<td>(tenths)</td>
-</tr>
-<tr>
-<td>Visibility</td>
-<td>777.7</td>
-<td>Km</td>
-</tr>
-<tr>
-<td>Ceiling Height</td>
-<td>77777</td>
-<td>m</td>
-</tr>
-<tr>
-<td>Precipitable Water</td>
-<td>0</td>
-<td>Mm</td>
-</tr>
-<tr>
-<td>Aerosol Optical Depth</td>
-<td>0</td>
-<td>Broadband turbidity</td>
-</tr>
-<tr>
-<td>Snow Depth</td>
-<td>0</td>
-<td>Cm</td>
-</tr>
-<tr>
-<td>Days Since Last Snow</td>
-<td>88</td>
-<td>Days</td>
-</tr>
-<tr>
-<td>Radiation Values (Direct/Diffuse)</td>
-<td>0.0</td>
-<td>Wh/m2</td>
-</tr>
-<tr>
-<td>Illuminance Values</td>
-<td>0.0</td>
-<td>lux (or CD/m2)</td>
-</tr>
-</table>
-
-\*\*Standard Barometric pressure based on location elevation is taken from ASHRAE 2001 Handbook of Fundamentals, Page 6.1 & 2.
-
-Weather Data Hourly Interpolation
----------------------------------
-
-Much of the existing weather data is produced in hourly format (refer to the discussion of data formats and weather conversion processing in the Auxiliary Programs Document). In order to match the hourly data in a continuous manner for EnergyPlus (where the timesteps might be less than hourly), simple interpolation between “last hour’s� values and “this hour’s� values is performed; we will refer to this as “Last Hour Interpolation�.
-
-Note that in versions prior to V1.0.3, the interpolation was done between “this hour� and “next hour�. If required, we will refer to this as “Next Hour Interpolation�.
-
-Remember that hour 1 for EnergyPlus is the time interval 00:00:01AM to 1:00:00AM. Hour 2 is 1:00:01AM to 2:00:00AM (hh:mm:ss). With the interpolation scheme (Last Hour Interpolation) and reporting weather data values at timestep resolution, the “hour� values reported should match with the hourly weather data values. (Note that reporting “hourly� resolution will not do this unless your “Number of Timesteps per Hour� is 1).
-
-Note that this interpolation applies to outdoor data only – schedule values are not interpolated in this manner.
-
-The weighting scheme / interpolation is simply:
-
-<div>\[Valu{e_{TimeStep}} = LastHourValue\cdot Weigh{t_{LastHour}} + ThisHourValue\cdot Weigh{t_{ThisHour}}\]</div>
-
-where
-
-<div>\[Weigh{t_{ThisHour}} = \frac{{CurrentTimeStep}}{{Number\,of\,TimeSteps\,in\,Hour}}\]</div>
-
-<div>\[Weigh{t_{LastHour}} = 1.0 - Weigh{t_{ThisHour}}\]</div>
-
-To explain further, the weighting for four (4) timesteps in hour is:
-
-Table 45. Illustration of Data Interpolation for 15 minute timesteps
-
-<table class="table table-striped">
-<tr>
-<th>TimeStep</th>
-<th>Time (mm:ss)</th>
-<th>Weight<sub>LastHour</sub></th>
-<th>Weight<sub>ThisHour</sub></th>
-</tr>
-<tr>
-<td>1</td>
-<td>00:01 to 15:00</td>
-<td>.75</td>
-<td>.25</td>
-</tr>
-<tr>
-<td>2</td>
-<td>15:01 to 30:00</td>
-<td>.5</td>
-<td>.5</td>
-</tr>
-<tr>
-<td>3</td>
-<td>30:01 to 45:00</td>
-<td>.25</td>
-<td>.75</td>
-</tr>
-<tr>
-<td>4</td>
-<td>45:01 to 60:00</td>
-<td>0</td>
-<td>1.0</td>
-</tr>
-</table>
-
-And similarly for six (6) timesteps in hour:
-
-Table 46. Illustration of Data Interpolation for 10 minute timesteps
-
-<table class="table table-striped">
-<tr>
-<th>TimeStep</th>
-<th>Time (mm:ss)</th>
-<th>Weight<sub>LastHour</sub></th>
-<th>Weight<sub>ThisHour</sub></th>
-</tr>
-<tr>
-<td>1</td>
-<td>00:01 to 10:00</td>
-<td>0.833333333333333</td>
-<td>0.166666666666667</td>
-</tr>
-<tr>
-<td>2</td>
-<td>10:01 to 20:00</td>
-<td>0.666666666666667</td>
-<td>0.333333333333333</td>
-</tr>
-<tr>
-<td>3</td>
-<td>20:01 to 30:00</td>
-<td>.5</td>
-<td>.5</td>
-</tr>
-<tr>
-<td>4</td>
-<td>30:01 to 40:00</td>
-<td>0.333333333333333</td>
-<td>0.666666666666667</td>
-</tr>
-<tr>
-<td>5</td>
-<td>40:01 to 50:00</td>
-<td>0.166666666666667</td>
-<td>0.833333333333333</td>
-</tr>
-<tr>
-<td>6</td>
-<td>50:01 to 60:00</td>
-<td>0</td>
-<td>1.0</td>
-</tr>
-</table>
-
-This interpolation gives a smooth, continuous look to the outdoor data. For day boundaries (i.e. from hour 24 to hour 1), the values from the previous day’s last hour (23:00:01 to 24:00:00). For the a design day, this is the values for hour 24. For the first day of a weather simulation, it is likewise values for hour 24 of that day. For subsequent weather days, it will be the last hour of the previous day.
-
-Weather File Data Reporting (errors) during Simulation
-------------------------------------------------------
-
-Missing data on the weather file used will be summarized on the **eplusout.err** file. In EnergyPlus, “missing data� is shown only for fields that EnergyPlus will use. For the “WeatherCodes�, an invalid field count (where the number of items in the field does not = 9) will be shown. The number of items count refers to the number of records on the weather file that are in error or missing – for an hourly weather file, this is the number of hours. Likewise out of range values (see specific fields in the previous definition) will be counted for each occurance and summarized. Note that the out of range values will not be changed by EnergyPlus and could affect your simulation results.
-
-
-
-For example:
-
-```
-   ** Warning ** Missing Data Found on Weather Data File
-   ************* Missing Atmospheric Pressure, Number of items=   48
-   ************* Missing Dry Bulb Temperatures, Number of items=   4
-   ** Warning ** Out of Range Data Found on Weather Data File
-   ************* Out of Range Dry Bulb Temperature [&gt;-70,&lt;70], Number of items=   1
-```
diff --git a/doc/src/docs/InputOutputReference/08-RunningEnergyPlus.md b/doc/src/docs/InputOutputReference/08-RunningEnergyPlus.md
deleted file mode 100644
index 52a69612503..00000000000
--- a/doc/src/docs/InputOutputReference/08-RunningEnergyPlus.md
+++ /dev/null
@@ -1,318 +0,0 @@
-Running EnergyPlus
-==================
-
-EnergyPlus is written in C++, using many C++11 features. It runs as a console application on Windows, Mac, and Linux (tested on latest Ubuntu LTS). Details on running EnergyPlus are available in a separate document (Running EnergyPlus in Auxiliary Programs). The following files are needed to run EnergyPlus:
-
-- EnergyPlus.exe (the executable file)
-- Energy+.ini (described below)
-- Energy+.idd (the input data dictionary file)
-- in.idf (the input file)
-- in.epw – optional (weather data file)
-
-The input data dictionary and input data file have been discussed in the previous sections of this document.
-
-For weather simulations, EnergyPlus accepts EnergyPlus weather files. The actual file name is **in.epw**.
-
-The usual release for Windows platform also includes a dependence on a shared library, EnergyPlusAPI.dll (.so on Linux).
-
-Energy+.ini
------------
-
-The Energy+.ini file is read by the EnergyPlus.exe program and is *very important* to the simulation run. In specific, this file contains a pointer to where the Energy+.idd file will be found. More description of the Energy+.ini contents is contained in the Auxiliary Programs document.
-
-For the advanced user, there is also the “EPMacro� program, described in the Auxiliary programs document. You run it as a separate program before EnergyPlus (the batch file included in the install and shown in the GettingStarted document contains the commands). It is automatically run if you use the EP-Launch program.
-
-EnergyPlus may create several output files. Whether some files are produced depends on the actual simulation (for example, the .rdd file is only produced when you request a Variable Dictionary using the Output:Report object). Similarly, the .dxf file is only produced when a DXF surface report is requested. Common output files are shown in the following table. A complete, up to date list is shown in the “Output Details and Examples Document�.
-
-Table 47. EnergyPlus Output Files
-
-<table class="table table-striped">
-<tr>
-<th>FileName</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>Eplusout.audit</td>
-<td>Echo of input</td>
-</tr>
-<tr>
-<td>Eplusout.err</td>
-<td>Error file</td>
-</tr>
-<tr>
-<td>Eplusout.eso</td>
-<td>Standard Output File (contains results from both Output:Variable and Output:Meter objects).</td>
-</tr>
-<tr>
-<td>Eplusout.eio</td>
-<td>One time output file</td>
-</tr>
-<tr>
-<td>Eplusout.rdd</td>
-<td>Output variable Data Dictionary</td>
-</tr>
-<tr>
-<td>Eplusout.dxf</td>
-<td>DXF (from Output:Report,Surfaces,DXF;)</td>
-</tr>
-<tr>
-<td>Eplusout.mtr</td>
-<td>Similar to .eso but only has Meter outputs.</td>
-</tr>
-<tr>
-<td>Eplusout.mtd</td>
-<td>Meter details report – what variables are on what meters and vice versa.</td>
-</tr>
-<tr>
-<td>Eplusout.end</td>
-<td>A one line summary of success or failure (useful for Interface programs)</td>
-</tr>
-<tr>
-<td>Eplusout.dbg</td>
-<td>From Debug Output object – may be useful to support to help track down problems</td>
-</tr>
-<tr>
-<td>Eplusout.&lt;ext&gt;</td>
-<td>Not directly from EnergyPlus – produced by utility programs that read the .eso file and produce output files for spreadsheet programs</td>
-</tr>
-<tr>
-<td>Eplusout.sln</td>
-<td>Similar to DXF output but less “formatted�. Results of Report Surface, Lines object.</td>
-</tr>
-<tr>
-<td>Epluszsz.&lt;ext&gt;</td>
-<td>Results from the Zone Sizing object with extension noted by the Sizing Style object. This file is “spreadsheet� ready.</td>
-</tr>
-<tr>
-<td>Eplusssz.&lt;ext&gt;</td>
-<td>Results from the System Sizing object with extension noted by the Sizing Style object. This file is “spreadsheet� ready.</td>
-</tr>
-<tr>
-<td>Eplusout.bnd</td>
-<td>This file contains details about the nodes and branches. Useful in determining if all your nodes are connected correctly.</td>
-</tr>
-<tr>
-<td>Eplustbl.&lt;ext&gt;</td>
-<td>Results from various “Report Table� and a few other reporting commands. The extension is from the “style� command and this file is “spreadsheet� ready.</td>
-</tr>
-</table>
-
-Errors
-------
-
-The **eplusout.err** file may contain three levels of errors (Information, Warning, Severe, Fatal) as well as the possibility of just message lines, see Table 48. EnergyPlus Errors and Required Actions. These errors may be duplicated in other files (such as the standard output file). These errors are described more completely in the Output Details and Examples document. An example .err file from the 1ZoneUncontrolled example input file:
-
-```
-Program Version,EnergyPlus 7.0.0.024, 10/9/2011 4:04 PM,IDD\_Version 7.0.0.024
-   ** Warning ** IP: Note -- Some missing fields have been filled with defaults. See the audit output file for details.
-   ** Warning ** Weather file location will be used rather than entered Location object.
-   **   ~~~   ** ..Location object=DENVER STAPLETON INTL ARPT CO USA WMO=724690
-   **   ~~~   ** ..Weather File Location=Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
-   **   ~~~   ** ..due to location differences, Latitude difference=[3.00E-002] degrees, Longitude difference=[0.31] degrees.
-   **   ~~~   ** ..Time Zone difference=[0.0] hour(s), Elevation difference=[13.53] percent, [218.00] meters.
-   ************* Testing Individual Branch Integrity
-   ************* All Branches passed integrity testing
-   ************* Testing Individual Supply Air Path Integrity
-   ************* All Supply Air Paths passed integrity testing
-   ************* Testing Individual Return Air Path Integrity
-   ************* All Return Air Paths passed integrity testing
-   ************* No node connection errors were found.
-   ************* Beginning Simulation
-   ************* Simulation Error Summary *************
-   ************* EnergyPlus Warmup Error Summary. During Warmup: 0 Warning; 0 Severe Errors.
-   ************* EnergyPlus Sizing Error Summary. During Sizing: 0 Warning; 0 Severe Errors.
-   ************* EnergyPlus Completed Successfully-- 2 Warning; 0 Severe Errors; Elapsed Time=00hr 00min  3.91sec
-```
-
-Table 48. EnergyPlus Errors and Required Actions
-
-<table class="table table-striped">
-<tr>
-<th>Error Level</th>
-<th>Action</th>
-</tr>
-<tr>
-<td>Information, shown as *********</td>
-<td>Informative, usually a follow-on to one of the others. No action required.</td>
-</tr>
-<tr>
-<td>**   ~~~   **</td>
-<td>This is a continuation of a previous message.  String all the words/sentences together to form the complete message.</td>
-</tr>
-<tr>
-<td>Warning</td>
-<td>Take note. Fix as applicable.</td>
-</tr>
-<tr>
-<td>Severe</td>
-<td>Should Fix</td>
-</tr>
-<tr>
-<td>Fatal</td>
-<td>Program will abort, Must Fix</td>
-</tr>
-</table>
-
-EnergyPlus produces several messages as it is executing, as a guide to its progress. These message illustrate the sequence of execution as well as provides checkpoints should the simulation fail.
-
-For example, the run of the 1ZoneUncontrolled example input file produces the log:
-```
-Running d:\eppgm\intcheck\energyplus.exe
-ET Start: Sun 10/09/2011 - 16:04:34.71
-Input File  : d:\devtests\inputfiles\checkin\1ZoneUncontrolled.idf
-Output Files: d:\devtests\inputfiles\outputs\
-Weather File: USA\_CO\_Golden-NREL.724666\_TMY3.epw
-ExpandObjects Started.
-No expanded file generated.
-ExpandObjects Finished. Time:     0.016
- EnergyPlus Starting
- EnergyPlus 7.0.0.024, 10/9/2011 4:04 PM
- Processing Data Dictionary
- Processing Input File
- Initializing Simulation
- Reporting Surfaces
- Initializing New Environment Parameters
- Warming up {1}
- Warming up {2}
- Warming up {3}
- Warming up {4}
- Warming up {5}
- Warming up {6}
- Warming up {7}
- Warming up {8}
- Warming up {9}
- Warming up {10}
- Warming up {11}
- Warming up {12}
- Warming up {13}
- Warming up {14}
- Warming up {15}
- Warming up {16}
- Warming up {17}
- Warming up {18}
- Warming up {19}
- Warming up {20}
- Warming up {21}
- Warming up {22}
- Starting Simulation at 12/21 for DENVER STAPLETON INTL ARPT ANN HTG 99% CONDNS DB
- Initializing New Environment Parameters
- Warming up {1}
- Warming up {2}
- Warming up {3}
- Warming up {4}
- Warming up {5}
- Warming up {6}
- Warming up {7}
- Warming up {8}
- Warming up {9}
- Warming up {10}
- Warming up {11}
- Warming up {12}
- Warming up {13}
- Warming up {14}
- Warming up {15}
- Warming up {16}
- Warming up {17}
- Starting Simulation at 07/21 for DENVER STAPLETON INTL ARPT ANN CLG 1% CONDNS DB=&gt;MWB
- Initializing New Environment Parameters
- Warming up {1}
- Warming up {2}
- Warming up {3}
- Warming up {4}
- Warming up {5}
- Warming up {6}
- Warming up {7}
- Warming up {8}
- Warming up {9}
- Warming up {10}
- Warming up {11}
- Warming up {12}
- Warming up {13}
- Warming up {14}
- Warming up {15}
- Warming up {16}
- Warming up {17}
- Warming up {18}
- Warming up {19}
- Warming up {20}
- Starting Simulation at 01/01 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=01/21
- Continuing Simulation at 01/21 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=02/10
- Continuing Simulation at 02/10 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=03/02
- Continuing Simulation at 03/02 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=03/22
- Continuing Simulation at 03/22 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=04/11
- Continuing Simulation at 04/11 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=05/01
- Continuing Simulation at 05/01 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=05/21
- Continuing Simulation at 05/21 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=06/10
- Continuing Simulation at 06/10 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=06/30
- Continuing Simulation at 06/30 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=07/20
- Continuing Simulation at 07/20 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=08/09
- Continuing Simulation at 08/09 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=08/29
- Continuing Simulation at 08/29 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=09/18
- Continuing Simulation at 09/18 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=10/08
- Continuing Simulation at 10/08 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=10/28
- Continuing Simulation at 10/28 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=11/17
- Continuing Simulation at 11/17 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=12/07
- Continuing Simulation at 12/07 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Updating Shadowing Calculations, Start Date=12/27
- Continuing Simulation at 12/27 for Denver Centennial  Golden   Nr CO USA TMY3 WMO\#=724666
- Writing tabular output file results using comma format.
- Writing tabular output file results using tab format.
- Writing tabular output file results using text format.
- Writing tabular output file results using HTML format.
- EnergyPlus Run Time=00hr 00min  3.91sec
- ReadVarsESO program starting.
- ReadVars Run Time=00hr 00min  0.39sec
- ReadVarsESO program completed successfully.
- ReadVarsESO program starting.
- ReadVars Run Time=00hr 00min  0.27sec
- ReadVarsESO program completed successfully.
-  Started HVAC Diagram
-  Complete
-note: Pausing=N
-ET End: Sun 10/09/2011 - 16:04:39.34
-```
-
-In the example, the inclusion of the “ReadVars� program is also shown. It is run twice – once for the **eplusout.eso** file and once for the **eplusout.mtr** file.
-
-EnergyPlus Execution Time
--------------------------
-
-Extensive timing studies and fine-tuning of EnergyPlus are an ongoing process. Remember that hourly simulations cannot be directly compared to EnergyPlus with its less than hourly timesteps.
-
-### Reducing Run Time Tips
-
-Compared with creating energy models either by hand coding the IDF file or by using GUI tools or a combination of both, EnergyPlus run time is normally a small fraction of the total time needed to complete an energy modeling job. Therefore it is very important to build a clean and concise EnergyPlus model up front. Techniques of simplifying large and complex building and systems should be used during the creation of energy models, especially during the early design process when detailed zoning and other information is not available. Producing lots of hourly or sub-hourly reports from EnergyPlus runs can take significant amount of time. Modelers should only request time step reports when necessary. On the other hand, producing summary reports and typical monthly reports take relatively small amount of run time. These reports are valuable references for troubleshooting and model fine tuning.
-
-With powerful personal computers get more and more affordable, EnergyPlus modelers should choose to use current available PCs with 3 or more GHZ and 3 or more GB of RAM. For a large volume of EnergyPlus parametric runs, modelers can launch multiple runs in parallel. For modelers, most time is spent on troubleshooting and fine tuning energy models. During the early modeling process, it is recommended to keep the model as simple as possible and make quick runs to identify problems. Then modify the IDF file to fix problems and re-run the model. This is an iterative process until satisfactory solutions are found. The simulation process can be split into three phases: the diagnostic runs, the preliminary runs, and the final runs. The three phases would use different simulation settings. The diagnostic runs would use a set of simulation settings to speed up the runs with simulation accuracy being set as the second priority. The diagnostic runs will help catch most model problems by
-
-running simulations on summer and winter design days. The preliminary runs use a tighter set of simulation settings in order to catch problems missed in the diagnostic runs, and provide better results for quality assurance purpose. The final runs use the EnergyPlus recommended set of simulation settings in order to achieve better accuracy for simulation results ready for review and reporting.
-
-You might want to read the report on EnergyPlus run time at http://repositories.cdlib.org/lbnl/LBNL-1311E/
-
-Additional run-time tips may be found in the EnergyPlus "Tips and Tricks" document.  Some more tips:
-
-- In the SimulationControl object, Run Simulation for Sizing Periods until everything is working well, then switch to Run Simulation for Weather File Run Periods.
-
-- Turn off (comment them out in the text editor using !) daylighting controls while developing the HVAC simulation.  Then turn back on for final runs.
-
-- HeatBalanceAlgorithm: ConductionTransferFunction is the fastest option.
-
-- In the People object, the thermal comfort reports can be time consuming, especially the KSU model which is more computationally intensive.
-
diff --git a/doc/src/docs/InputOutputReference/09-Appendix.md b/doc/src/docs/InputOutputReference/09-Appendix.md
deleted file mode 100644
index 7f201c9741d..00000000000
--- a/doc/src/docs/InputOutputReference/09-Appendix.md
+++ /dev/null
@@ -1,229 +0,0 @@
-Appendix A. Units and Abbreviations
-===================================
-
-Standard EnergyPlus Conditions
-------------------------------
-
-### Standard Temperature and Pressure
-
-Several objects specify inputs at “standard temperature and pressure�. Standard Temperature  is dry air at 20<sup>o</sup> C drybulb. The program uses local barometric pressure to account for altitude using the equation for "standard atmospheric" pressure on p 6.1 of the ASHRAE 1997 HOF (SI edition) to initialize the air systems being simulated.
-
-<div>\[Stdpressure = 101325\cdot {\left( {1.0 - Z\cdot {{2.25577}^{ - 5}}} \right)^{5.2559}}\]</div>
-
-where
-
-StdPressure = pressure {Pa}
-
-Z = altitude/elevation {m}
-
-
-
-Standard EnergyPlus Units
--------------------------
-
-EnergyPlus expects information in a single unit system (SI). This requires interface developers to convert user inputs from those preferred by architects and engineers into the standard metric units of EnergyPlus. EnergyPlus will not perform any units conversions and will not have any unit conversion routines.
-
-ASCII with no spaces is used for abbreviations. Note that exponents appear without any indication of exponentiation: i.e., kg/m3 not kg/m^3 or kg/m\*\*3. Also note the use of dashes. We have W/m2-K not W/m2\*K or W/(m2\*K).
-
-At the end we note the “problem� variables – the inputs that have non-standard units. Inputs using these units will have to be changed and the code checked to see how the quantities are used internally.
-
-<table class="table table-striped">
-  <caption>Standard EnergyPlus Units</caption>
-  <tr>
-    <th>Quantity</th>
-    <th>unit</th>
-    <th>abbreviation</th>
-  </tr>
-  <tr>
-    <td>angular degrees</td>
-    <td>degree</td>
-    <td>deg</td>
-  </tr>
-  <tr>
-    <td>Length</td>
-    <td>meter</td>
-    <td>m</td>
-  </tr>
-  <tr>
-    <td>Area</td>
-    <td>square meter</td>
-    <td>m2</td>
-  </tr>
-  <tr>
-    <td>Volume</td>
-    <td>cubic meter</td>
-    <td>m3</td>
-  </tr>
-  <tr>
-    <td>Time</td>
-    <td>seconds</td>
-    <td>s</td>
-  </tr>
-  <tr>
-    <td>Frequency</td>
-    <td>Hertz</td>
-    <td>Hz</td>
-  </tr>
-  <tr>
-    <td>Temperature</td>
-    <td>Celsius</td>
-    <td>C</td>
-  </tr>
-  <tr>
-    <td>absolute temperature</td>
-    <td>Kelvin</td>
-    <td>K</td>
-  </tr>
-  <tr>
-    <td>temperature difference</td>
-    <td>Kelvin</td>
-    <td>deltaC</td>
-  </tr>
-  <tr>
-    <td>speed</td>
-    <td>meters per second</td>
-    <td>m/s</td>
-  </tr>
-  <tr>
-    <td>energy (or work)</td>
-    <td>Joules</td>
-    <td>J</td>
-  </tr>
-  <tr>
-    <td>power</td>
-    <td>Watts</td>
-    <td>W</td>
-  </tr>
-  <tr>
-    <td>mass</td>
-    <td>kilograms</td>
-    <td>kg</td>
-  </tr>
-  <tr>
-    <td>force</td>
-    <td>Newton</td>
-    <td>N</td>
-  </tr>
-  <tr>
-    <td>mass flow</td>
-    <td>kilograms per second</td>
-    <td>kg/s</td>
-  </tr>
-  <tr>
-    <td>volume flow</td>
-    <td>cubic meters per second</td>
-    <td>m3/s</td>
-  </tr>
-  <tr>
-    <td>pressure</td>
-    <td>Pascals</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td>pressure difference</td>
-    <td>Pascals</td>
-    <td>Pa</td>
-  </tr>
-  <tr>
-    <td>specific enthalpy</td>
-    <td>Joules per kilogram</td>
-    <td>J/kg</td>
-  </tr>
-  <tr>
-    <td>density</td>
-    <td>kilograms per cubic meter</td>
-    <td>kg/m3</td>
-  </tr>
-  <tr>
-    <td>heat flux</td>
-    <td>watts per square meter</td>
-    <td>W/m2</td>
-  </tr>
-  <tr>
-    <td>specific heat</td>
-    <td>-------</td>
-    <td>J/kg-K</td>
-  </tr>
-  <tr>
-    <td>conductivity</td>
-    <td>-------</td>
-    <td>W/m-K</td>
-  </tr>
-  <tr>
-    <td>diffusivity</td>
-    <td>-------</td>
-    <td>m2/s</td>
-  </tr>
-  <tr>
-    <td>heat transfer coefficient</td>
-    <td>-------</td>
-    <td>W/m2-K</td>
-  </tr>
-  <tr>
-    <td>R-value</td>
-    <td>-------</td>
-    <td>m2-K/W</td>
-  </tr>
-  <tr>
-    <td>heating or cooling capacity</td>
-    <td>Watts</td>
-    <td>W</td>
-  </tr>
-  <tr>
-    <td>electric potential</td>
-    <td>volts</td>
-    <td>V</td>
-  </tr>
-  <tr>
-    <td>electric current</td>
-    <td>Amperes</td>
-    <td>A</td>
-  </tr>
-  <tr>
-    <td>illuminace</td>
-    <td>lux</td>
-    <td>lx</td>
-  </tr>
-  <tr>
-    <td>luminous flux</td>
-    <td>lumen</td>
-    <td>lm</td>
-  </tr>
-  <tr>
-    <td>luminous intensity</td>
-    <td>candelas</td>
-    <td>cd</td>
-  </tr>
-  <tr>
-    <td>luminance</td>
-    <td>candelas per square meter</td>
-    <td>cd/m2</td>
-  </tr>
-  <tr>
-    <td>vapor diffusivity</td>
-    <td>meters squared per second</td>
-    <td>m2/s</td>
-  </tr>
-  <tr>
-    <td>viscosity</td>
-    <td>-------</td>
-    <td>kg/m-s</td>
-  </tr>
-  <tr>
-    <td>dynamic Viscosity</td>
-    <td>-------</td>
-    <td>N-s/m2</td>
-  </tr>
-  <tr>
-    <td>thermal gradient coeff for moisture capacity</td>
-    <td>-------</td>
-    <td>kg/kg-K</td>
-  </tr>
-  <tr>
-    <td>isothermal moisture capacity</td>
-    <td>-------</td>
-    <td>m3/kg</td>
-  </tr>
-</table>
-
-
diff --git a/doc/src/docs/InputOutputReference/media/image001.svg b/doc/src/docs/InputOutputReference/media/image001.svg
deleted file mode 100644
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diff --git a/doc/src/docs/InputOutputReference/media/image080.svg b/doc/src/docs/InputOutputReference/media/image080.svg
deleted file mode 100644
index 80516db1e48..00000000000
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diff --git a/doc/src/docs/InputOutputReference/media/image096.svg b/doc/src/docs/InputOutputReference/media/image096.svg
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diff --git a/doc/src/docs/InputOutputReference/media/image101.svg b/doc/src/docs/InputOutputReference/media/image101.svg
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diff --git a/doc/src/docs/InputOutputReference/media/image222.svg b/doc/src/docs/InputOutputReference/media/image222.svg
deleted file mode 100644
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diff --git a/doc/src/docs/InterfaceDeveloper/InterfaceDeveloper.md b/doc/src/docs/InterfaceDeveloper/InterfaceDeveloper.md
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-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Guide for Interface Developers</h1>
-<h2>Everything You Need to Know about EnergyPlus Input and Output</h2>
-<br/>
-<p><i>(to develop a user-friendly interface)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-Introduction
-============
-
-This document is intended for developers who are creating user interfaces for EnergyPlus.  It provides an overview of the essentials of the input-output structure of EnergyPlus and describes the parts of each in detail.
-
-![](media/image001.png)
-
-Figure 1. EnergyPlus Input/Output Overview
-
-The diagram shown above should give the reader an overall picture of input-output in EnergyPlus.  It can be seen as a linear process that includes the following steps:
-
-1)   The user enters building description (including internal space gains, HVAC arrangements, and Plant equipment properties) using the interface of their choice.  In addition, the user specifies which non-default reports are desired and any optional variables from a predefined list of available simulation quantities.
-
-2)   The interface program writes the Input Data File (IDF) file, which includes the specification of any report items desired by the user.
-
-3)   EnergyPlus processes both the Input Data Dictionary (IDD) and the Input Data File (IDF) files with the “InputProcessor�.  The InputProcessor uses the specifications/rules defined in the IDD and interprets the IDF raw data.  The InputProcessor is really quite “dumb� and only understands a few things about each field (alpha or numeric) qualified by certain key elements in the IDD (\\ comments which are discussed later).
-
-4)   Each module in EnergyPlus has one or several routines (normally called “GetInput� routines) that obtain the information from the IDF file data.  These subroutines decode the portion of the IDF file that is pertinent to the local module.  These GetInput routines are more context sensitive than the InputProcessor and may perform further error detection.  For example, the cooling coil module may read in the coil type and its associated parameters (number of rows, tube diameter, fin spacing, etc.).
-
-5)   EnergyPlus performs the simulation elements specified in the IDF.  Output is generated as a continuous stream (for the most part) and must be interpreted into a more cohesive form by output processing.  The user has control over which outputs are produced and when/how often.
-
-6)   EnergyPlus produces output as required by the user into one of the output files.  These files can be readily processed into spreadsheet formats for graphing and other summarizing.
-
-
-
-Interface Expectations
-----------------------
-
-The input-output interfaces may be combined into a single program or may be available separately.  The following attributes are expected from these interfaces.
-
-### Input Interface Attributes
-
-The input interface agents will be expected to fulfill two main requirements:
-
-- Ability to produce the input file for the simulation.
-
-- Perform the consistency and value checks necessary to assure that the input file conforms to EnergyPlus requirements.
-
-Additionally, the input interface agent might:
-
-- Ability to warn users about potential output file size.  It is expected that the data files generated by the EnergyPlus program will be significantly larger than the output files from its parent programs.  As a result, users may be unaware that selecting too many reports could lead to enormous output files.  It is recommended that some sort of checking be done to alert users when the term of the simulation and the number of reports selected eclipse some reasonable file size limit.
-
-- Ability to perform parametric runs.
-
-The method used by the input interface agent to accomplish these goals is left to the discretion of the interface developer.
-
-### Post-processing Interface Attributes
-
-The post-processing agents will be expected to fulfill the main requirement:
-
-- Ability to read all or selected output formats.
-
-Additionally, a post-processing agent might:
-
-- Ability to combine and summarize data (average, peak, total, etc.) and produce the various text and graphical reports requested by the user.
-
-- Ability to handle multiple output files.
-
-The method used by the post-processing agent to accomplish these goals is left to the discretion of the interface developer.
-
-EnergyPlus Install Contents
-===========================
-
-EnergyPlus Interfaces will naturally need to access the installed EnergyPlus programs, library files, documentation.  It will help to describe how EnergyPlus is installed (on a Windows™ computer).  The EnergyPlus install is written using the WISE™ installation software.
-
-The scheme of installing EnergyPlus includes a “root� directory/folder and all subsequent programs installed as part of the installation are child folders under the parent/root folder.  Several optional components can be selected during install.
-
-The basic (required) installation has crucial files installed in the parent folder – these include **EnergyPlus.exe**, **Energy+.idd** (the input data dictionary), **EPMacro.exe**.  The basic installation also includes a child folder “DataSets� that contains the EnergyPlus “libraries�.  As distributed, EnergyPlus includes several library files, formatted in the standard EnergyPlus IDF format.  These include thermal material properties, moisture material properties, glass and other properties for windows, constructions (material sandwiches which describe walls, windows, roofs), fluid properties, locations, design day definitions, and basic schedule definitions.  There, of course, may be additional data sets added as well as future datasets edited for selectable use from the EPMacro program.  The Templates folder is also included in the basic install.  Currently, the Templates folder contains documentation and the HVAC Template files.  These files can be used somewhat “automatically� to produce HVAC loop structures for running with EnergyPlus.
-
-Optional components of the EnergyPlus install: **Documentation**, **EP-Launch**, **IDFEditor**, **Sample** **Files**, **Weather** **Converter**, and other auxiliary type programs.  All the components are selected by default; to not install them the user must “un-select� them individually.  Highlights of several:
-
-**Documentation:**  The EnergyPlus package includes a comprehensive set of documents intended to help the user and others understand the EnergyPlus program, usage, and other appropriate information.  All documents are created in PDF (Portable Document Format).  There is “index� to all documents to make searching for a subject easier. A shortcut to the Documentation folder and the “main-menu� document is included.  The main-menu document is a navigation aid to the remainder of the documents.  We may want to make the documentation a non-optional component.
-
-**EP-Launch: ** The components of EP-Launch are installed in the parent directory (help files installed in the documentation directory).  Because the basic EnergyPlus program runs as a console application, many beta users did not understand how to make the program execute.  While the developers may be able to tailor the EnergyPlus executable to be more callable under the Windows™ platform, this is still a useful program.  EP-Launch uses the EPL-Run.bat file and prepends several “set� commands that are used in the bat file.  It creates the actual batch file for the run as “RunEP.bat� and then calls the operating system to execute the file.   Having the EPL-Run.bat file as external to the EP-Launch program means that others may tailor the batch file more appropriately to how things are run though this may not be preserved with a future EnergyPlus install. EP-Launch can also execute several utility programs from the “Utilities� tab.
-
-**IDFEditor: ** The IDFEditor is the simple editor that is distributed with EnergyPlus.  As an interface, it is crude.  However, it gets the job done.  It uses the IDD and then reads and/or creates an IDF file.  The objects are shown in the groups (see \\group discussion below) and, when an existing file is used, will display how many of an object is found in the IDF.  This program is installed in the Parent \\ PreProcess \\ IDFEditor folder.
-
-**Sample Files:**  The sample files include several IDF files along with the files the installed version of EnergyPlus created using these files.  There are several possible child folders here, including the Misc child folder that will contain all the development sample files – but without having been run for the install.  These files are installed in the Parent \\ ExampleFiles folder and any appropriate child folders under that.
-
-**Weather Converter:**  The WeatherConverter program can process raw weather data in several formats into the EnergyPlus weather data format (epw).  In addition, the WeatherConverter program can be used to generate a simple report of the weather data as well as produce a .csv file of the format.  The .csv (comma separated variable) format can easily be imported into spread sheet programs or other tables.  This program is installed in the Parent \\ PreProcess \\ WeatherConverter folder.  The WeatherConverter also has a DLL file which could be used directly by an external interface.
-
-**BLAST Translator: ** The BLAST translator program can be used to convert a BLAST input file into a format that can be executed from EnergyPlus.  Extensive system translation is not done with this program – mostly geometry and other space gain elements as well as zone oriented (i.e. People) schedules.  If the BLAST input file contains thermostatic controls in the zones, then the EnergyPlus IDF file will include a purchased-air solution of that BLAST input file.  This program is no longer part of the EnergyPlus install but is available with each new release.
-
-**DOE-2 Translator:**  The DOE-2 translator program is similar to the BLAST Translator program but for DOE-2 files.  DOE-2 translator output must be processed by the EPMacro program prior to running in EnergyPlus (the EP-Launch program/EPL-Run procedure does this automatically for all “.imf� files).  This program is no longer part of the EnergyPlus install but is available with each new release.
-
-Input Overview
-==============
-
-The general structure of the input files for EnergyPlus is plain text.  Fields are comma delimited and each “line� is terminated with a semicolon.  This allows for a very rudimentary input processor that can be instantly flexible to developer’s needs.  However, it puts more burdens on the EnergyPlus developers to process the input information, supply defaults as needed, and perform validity checks.  Guidelines were established for the input:
-
-- Input will be a flat ASCII file with comma-delimited columns and each “line� (where each line can run over several physical file records) terminated with a semicolon.
-
-- Input should be “readable�, “editable�, “simply parsed with few value checks or consistency checks�.
-
-- Input, to the extent possible, should be easily maintainable and extendable.
-
-- Input will be “object based�.
-
-- Definitions in a data dictionary will define the input.  The data dictionary should be self-documenting.
-
-- All input units will be metric (SI).  Conversions from “user units� will be done in the interface agents.
-
-Two input files are necessary for the input processing.  The first is the “data dictionary� which will specify the requirements for each item.  The EnergyPlus Input Processor uses these requirements to process the “input data file� and report any anomalies found.  Both input files have similar structures: 1) Sections – single lines/commands, which may help group the simulation input for readability and 2) Classes/Objects – data attributes for the simulation.  Classes are the term used in the data dictionary – each class will specify the kind of data (alpha or numeric) that will be included in the simulation input.  Objects are instances of these classes and appear in the IDF with appropriate data.
-
-General Input Rules
--------------------
-
-The following rules apply to both the Input Data Dictionary and the Input Data File.
-
-- The initial line of a definition or input MUST have a comma or semicolon.
-
-- Fields do not extend over line boundaries.  Usually, if a comma or (as appropriate) semi-colon is not the last field value on a line, one will be inserted.  Of course, several fields may appear on a single line as long as they are comma separated.
-
-- Commas delimit fields – therefore, no fields can have embedded commas.  No error will occur but you won't get what you want.
-
-- Blank lines are allowed.
-
-- The comment character is a exclamation “!�.  Anything on a line after the exclamation is ignored.
-
-- A special type of comment using the character combination: “!-“ in the input file is a special form of comment that is followed by the field name(s) and units and should not include user provided text. This form is used to indicate automatic comments which may be written by interfaces and other utilities as an endline comment after a field value.
-
-- Input records can be up to 500 characters in length.  If you go over that, no error will occur but you won't get what you want.
-
-- Each Section and Class/Object keyword can be up to 100 characters in length.  Embedded spaces are allowed, but are significant (if you have 2 spaces in the section keyword – you must have 2 when you write the object keyword).
-
-- Each Alpha string (including Section and Class/Object keywords) is mapped to UPPER case during processing, unless the “retaincase� flag marks the field in the IDD.  Get routines from the EnergyPlus code that use the Section and Object keywords automatically map to UPPER case for finding the item.  The primary drawback with this is that error messages coming out of the input processor will be in UPPER case and may not appear exactly as input.
-
-- Special characters, such as tabs, should NOT be included in the file.  However, tabs can be accommodated and are turned into spaces.
-
-Input Data Dictionary
----------------------
-
-The input data dictionary specifies the “definitions� for each line that will be processed in the input data file.
-
-Structure in the input data dictionary allows for descriptions that may be useful for interface developers.  The Input Processor ignores everything but the essentials for getting the “right stuff� into the program.  Developers have been (and will continue to be) encouraged to include comments and other documentation in the IDD.
-
-Internal to the data dictionary (using special “comment� characters) is a structured set of conventions for including information on each object.  This is shown in section on Input Details below.
-
-### Rules specific to the Input Data Dictionary
-
-In addition to the rules for both files (listed above), the IDD also has the limitation:
-
-- Duplicate Section names and Duplicate Class names are not allowed.  That is, the first class of an item named X will be the one used during processing.  Error messages will appear if you try to duplicate definitions.
-
-Input Data File
----------------
-
-This is the only file that EnergyPlus uses to create the building simulation.  The input is order-independent; data can appear in any order and will be retrieved and sorted as necessary by the EnergyPlus simulation modules.  In addition, EnergyPlus allocates everything dynamically, so there are no limitations as to number of zones, surfaces, etc.
-
-All numbers can be flexibly input and are processed into single precision variables (i.e. 1.0, 1.000, 1, .1E+1 are all processed equally).
-
-### Rules specific to Input Data file:
-
-- Each Alpha string in the input data file can be up to 100 characters in length.  Anything beyond that is truncated.
-
-- A special combination of characters “!-“ indicates a comment that contains the name and units of the field after each field value. These, like normal comments, are ignored by EnergyPlus. This type of comment containing the field names are created automatically with IDF Editor, IDF Version Updater (transition) and other user interfaces. Comments added by the user should not use “!-“ because they are deleted and replaced with the field name when the file is saved using IDF Editor. For an example of this syntax, see the example file in Appendix A.
-
-Input Details
-=============
-
-This document does not cover the input “classes� in detail.  For details on each class and examples of both input and output resulting from that class/object, please view the [Input Output Reference](file:///E:\Docs4PDFs\InputOutputReference.pdf) document.  In this document, we will show the “conventions� used in the IDD and provide limited examples for illustration purposes. Even the list of objects is dynamic, so we give you a method to see them from the IDFEditor.
-
-An intelligent editor (IDFEditor) has been written and can be used as an illustration of how the comments in the IDD might be used by Interface Developers to guide their developments.  IDFEditor is described in the [Getting Started](file:///E:\Docs4PDFs\GettingStarted.pdf) document.
-
-A full example of a very simple IDF is included in Appendix A to this document.
-
-IDD Conventions
----------------
-
-The following is a basic description of the structure of the IDD (it’s actually taken directly from the IDD file). As noted within, **!** signifies a comment character as does the **\\**. **\\** has also been adopted as a convention for including more specific comments about each field in an object. These have been used with success in the IDFEditor and it is hoped the flexibility will provide other interface developers with useful information.
-
-```idd
-!IDD_Version VERSION NUMBER
-! **************************************************************************
-! This file is the Input Data Dictionary (IDD) for EnergyPlus.
-! The IDD defines the syntax and data model for each type of input "Object."
-! Lines in EnergyPlus input files (and IDD) are limited to 500 characters.
-!
-! Object Description
-! ------------------
-! To define an object (a record with data), develop a key word that is unique
-! Each data item to the object can be A (Alphanumeric string) or N (numeric)
-! Number each A and N.  This will show how the data items will be put into the
-! arrays that are passed to the Input Processor "Get" (GetObjectItem) routines.
-! All alpha fields are limited to 100 characters.  Numeric fields should be
-! valid numerics (can include such as 1.0E+05) and are placed into double
-! precision variables.
-!
-! NOTE: Even though a field may be optional, a comma representing that field
-!   must be included (unless it is the last field in the object).  Since the
-!   entire input is "field-oriented" and not "keyword-oriented", the EnergyPlus
-!   Input Processor must have some representation (even if blank) for each
-!   field.
-!
-! Object Documentation
-! --------------------
-! In addition, the following special comments appear one per line and
-! most are followed by a value.  Comments may apply to a field or the object
-! or a group of objects.
-!
-! Field-level comments:
-!
-!  \field           Name of field
-!                     (should be succinct and readable, blanks are encouraged)
-!
-!  \note            Note describing the field and its valid values. If multiple lines,
-!                   start each line with \note. Limit line length to 100 characters.
-!
-!  \required-field  To flag fields which may not be left blank
-!                     (this comment has no "value")
-!
-!  \begin-extensible  Marks the first field at which the object accepts an extensible
-!                   field set.  A fixed number of fields from this marker define the
-!                   extensible field set, see the object code \extensible for
-!                   more information.
-!
-!  \units           Units (must be from EnergyPlus standard units list)
-!                   EnergyPlus units are standard SI units
-!
-!  \ip-units        IP-Units (for use by input processors with IP units)
-!                   This is only used if the default conversion is not
-!                   appropriate.
-!
-!  \unitsBasedOnField  For fields that may have multiple possible units, indicates
-!                   the field in the object that can be used to determine
-!                   the units. The field reference is in the A2 form.
-!
-!  \minimum         Minimum that includes the following value
-!
-!  \minimum>        Minimum that must be > than the following value
-!
-!  \maximum         Maximum that includes the following value
-!
-!  \maximum<        Maximum that must be &lt; than the following value
-!
-!  \default         Default for the field (if N/A then omit entire line)
-!
-!  \deprecated      This field is not really used and will be deleted from the object.
-!                   The required information is gotten internally or
-!                   not needed by the program.
-!
-!  \autosizable     Flag to indicate that this field can be used with the Auto
-!                   Sizing routines to produce calculated results for the
-!                   field.  If a value follows this, then that will be used
-!                   when the "Autosize" feature is flagged.  To trigger
-!                   autosizing for a field, enter Autosize as the field's
-!                   value.  Only applicable to numeric fields.
-!
-!  \autocalculatable Flag to indicate that this field can be automatically
-!                   calculated. To trigger auto calculation for a field, enter
-!                   Autocalculate as the field's value.  Only applicable to
-!                   numeric fields.
-!
-!  \type            Type of data for the field -
-!                     integer
-!                     real
-!                     alpha       (arbitrary string),
-!                     choice      (alpha with specific list of choices, see
-!                                 \key)
-!                     object-list (link to a list of objects defined elsewhere,
-!                                  see \object-list and \reference)
-!                     external-list (uses a special list from an external source,
-!                                    see \external-list)
-!                     node        (name used in connecting HVAC components)
-!
-!  \retaincase      Retains the alphabetic case for alpha type fields
-!
-!  \key             Possible value for "\type choice" (blanks are significant)
-!                     use multiple \key lines to indicate all valid choices
-!
-!  \object-list     Name of a list of user-provided object names that are valid
-!                     entries for this field (used with "\reference")
-!                     see Zone and BuildingSurface:Detailed objects below for
-!                     examples.
-!                  ** Note that a field may have multiple \object-list commands.
-!
-!  \external-list   The values for this field should be selected from a special
-!                   list generated outside of the IDD file. The choices for the
-!                   special lists are:
-!                        autoRDDvariable
-!                        autoRDDmeter
-!                        autoRDDvariableMeter
-!                   When one of these are selected the options for the field
-!                   are taken from the RDD or MDD file or both.
-!
-!  \reference       Name of a list of names to which this object belongs
-!                     used with "\type object-list" and with "\object-list"
-!                     see Zone and BuildingSurface:Detailed objects below for
-!                     examples:
-!
-!                        Zone,
-!                          A1 , \field Name
-!                               \type alpha
-!                               \reference ZoneNames
-!
-!                        BuildingSurface:Detailed,
-!                          A4 , \field Zone Name
-!                               \note Zone the surface is a part of
-!                               \type object-list
-!                               \object-list ZoneNames
-!
-!             For each zone, the field "Name" may be referenced
-!             by other objects, such as BuildingSurface:Detailed, so it is
-!             commented with "\reference ZoneNames"
-!             Fields that reference a zone name, such as BuildingSurface:Detailed's
-!             "Zone Name", are commented as
-!             "\type object-list" and "\object-list ZoneNames"
-!             ** Note that a field may have multiple \reference commands.
-!             ** This is useful if the object belongs to a small specific
-!             object-list as well as a larger more general object-list.
-!
-! Object-level comments:
-!
-!  \memo            Memo describing the object. If multiple lines, start each line
-!                   with \memo.
-!                   Limit line length to 100 characters.
-!
-!  \unique-object   To flag objects which should appear only once in an idf
-!                     (this comment has no "value")
-!
-!  \required-object To flag objects which are required in every idf
-!                     (this comment has no "value")
-!
-!  \min-fields      Minimum number of fields that should be included in the
-!                   object.  If appropriate, the Input Processor will fill
-!                   any missing fields with defaults (for numeric fields).
-!                   It will also supply that number of fields to the "get"
-!                   routines using blanks for alpha fields (note -- blanks
-!                   may not be allowable for some alpha fields).
-!
-!  \obsolete        This object has been replaced though is kept (and is read)
-!                   in the current version.  Please refer to documentation as
-!                   to the dispersal of the object.  If this object is
-!                   encountered in an IDF, the InputProcessor will post an
-!                   appropriate message to the error file.
-!                   usage:  \obsolete New=>[New object name]
-!
-!  \extensible:<\#>  This object is dynamically extensible -- meaning, if you
-!           change the IDD appropriately (if the object has a simple list
-!           structure -- just add items to the list arguments (i.e. BRANCH
-!           LIST). These will be automatically redimensioned and used during
-!           the simulation. <\#> should be entered by the developer to signify
-!           how many of the last fields are needed to be extended (and EnergyPlus
-!           will attempt to auto-extend the object).  The first field of the first
-!           instance of the extensible field set is marked with \begin-extensible.
-!
-!  \begin-extensible See previous item, marks beginning of extensible fields in
-!                   an object.
-!
-!  \format          The object should have a special format when saved in
-!                   the IDF Editor with the special format option enabled.
-!                   The options include SingleLine, Vertices, CompactSchedule,
-!                   FluidProperties, ViewFactors, and Spectral.
-!                   The SingleLine option puts all the fields for the object
-!                   on a single line. The Vertices option is used in objects
-!                   that use X, Y and Z fields to format those three fields
-!                   on a single line.
-!                   The CompactSchedule formats that specific object.
-!                   The FluidProperty option formats long lists of fluid
-!                   properties to ten values per line.
-!                   The ViewFactor option formats three fields related to
-!                   view factors per line.
-!                   The Spectral option formats the four fields related to
-!                   window glass spectral data per line.
-!
-!   \reference-class-name Adds the name of the class to the reference list
-!                   similar to \reference.
-!
-! Group-level comments:
-!
-!  \group          Name for a group of related objects
-!
-!
-! Notes on comments
-! -----------------
-!
-! 1.  If a particular comment is not applicable (such as units, or default)
-! then simply omit the comment rather than indicating N/A.
-!
-! 2.  Memos and notes should be brief (recommend 5 lines or less per block).
-! More extensive explanations are expected to be in the user documentation
-```
-
-
-### IDD – IP Units
-
-In addition, the IDD contains indications of IP (inch-pound) units for the EnergyPlus standard SI (Systems International) units. These may be used by input and output interfaces to display values in the IP system. As noted, if the IP units are “standard� (first block below), then no \\ip-units is expected in the field. Note that for some fields – due to their multiple use (for example, schedule values) – there cannot be a ip-unit designation.
-```idf
-! Default IP conversions (no \ip-units necessary)
-!      $/(m3/s)               =>   $/(ft3/min)         0.000472000059660808
-!      $/(W/K)                =>   $/(Btu/h-F)         0.52667614683731
-!      $/kW                   =>   $/(kBtuh/h)         0.293083235638921
-!      $/m2                   =>   $/ft2               0.0928939733269818
-!      $/m3                   =>   $/ft3               0.0283127014102352
-!      (kg/s)/W               =>   (lbm/sec)/(Btu/hr)  0.646078115385742
-!      1/K                    =>   1/F                 0.555555555555556
-!      1/m                    =>   1/ft                0.3048
-!      A/K                    =>   A/F                 0.555555555555556
-!      C                      =>   F                   1.8 (plus 32)
-!      cm                     =>   in                  0.3937
-!      cm2                    =>   inch2               0.15500031000062
-!      deltaC                 =>   deltaF              1.8
-!      deltaJ/kg              =>   deltaBtu/lb         0.0004299
-!      g/GJ                   =>   lb/MWh              0.00793664091373665
-!      g/kg                   =>   grains/lb           7
-!      g/MJ                   =>   lb/MWh              7.93664091373665
-!      g/mol                  =>   lb/mol              0.0022046
-!      g/m-s                  =>   lb/ft-s             0.000671968949659
-!      g/m-s-K                =>   lb/ft-s-F           0.000373574867724868
-!      GJ                     =>   ton-hrs             78.9889415481832
-!      J                      =>   Wh                  0.000277777777777778
-!      J/K                    =>   Btu/F               526.565
-!      J/kg                   =>   Btu/lb              0.00042986
-!      J/kg-K                 =>   Btu/lb-F            0.000239005736137667
-!      J/kg-K2                =>   Btu/lb-F2           0.000132889924714692
-!      J/kg-K3                =>   Btu/lb-F3           7.38277359526066E-05
-!      J/m2-K                 =>   Btu/ft2-F           4.89224766847393E-05
-!      J/m3                   =>   Btu/ft3             2.68096514745308E-05
-!      J/m3-K                 =>   Btu/ft3-F           1.49237004739337E-05
-!      K                      =>   R                   1.8
-!      K/m                    =>   F/ft                0.54861322767449
-!      kg                     =>   lb                  2.2046
-!      kg/J                   =>   lb/Btu              2325.83774250441
-!      kg/kg-K                =>   lb/lb-F             0.555555555555556
-!      kg/m                   =>   lb/ft               0.67196893069637
-!      kg/m2                  =>   lb/ft2              0.204794053596664
-!      kg/m3                  =>   lb/ft3              0.062428
-!      kg/m-s                 =>   lb/ft-s             0.67196893069637
-!      kg/m-s-K               =>   lb/ft-s-F           0.373316072609094
-!      kg/m-s-K2              =>   lb/ft-s-F2          0.207397818116164
-!      kg/Pa-s-m2             =>   lb/psi-s-ft2        1412.00523459398
-!      kg/s                   =>   lb/s                2.20462247603796
-!      kg/s2                  =>   lb/s2               2.2046
-!      kg/s-m                 =>   lb/s-ft             0.67196893069637
-!      kJ/kg                  =>   Btu/lb              0.429925
-!      kPa                    =>   psi                 0.145038
-!      L/day                  =>   pint/day            2.11337629827348
-!      L/GJ                   =>   gal/kWh             0.000951022349025202
-!      L/kWh                  =>   pint/kWh            2.11337629827348
-!      L/MJ                   =>   gal/kWh             0.951022349025202
-!      lux                    =>   foot-candles        0.092902267
-!      m                      =>   ft                  3.28083989501312
-!      m/hr                   =>   ft/hr               3.28083989501312
-!      m/s                    =>   ft/min              196.850393700787
-!      m/s                    =>   miles/hr            2.2369362920544
-!      m/yr                   =>   inch/yr             39.3700787401575
-!      m2                     =>   ft2                 10.7639104167097
-!      m2/m                   =>   ft2/ft              3.28083989501312
-!      m2/person              =>   ft2/person          10.764961
-!      m2/s                   =>   ft2/s               10.7639104167097
-!      m2-K/W                 =>   ft2-F-hr/Btu        5.678263
-!      m3                     =>   ft3                 35.3146667214886
-!      m3                     =>   gal                 264.172037284185
-!      m3/GJ                  =>   ft3/MWh             127.13292
-!      m3/hr                  =>   ft3/hr              35.3146667214886
-!      m3/hr-m2               =>   ft3/hr-ft2          3.28083989501312
-!      m3/hr-person           =>   ft3/hr-person       35.3146667214886
-!      m3/kg                  =>   ft3/lb              16.018
-!      m3/m2                  =>   ft3/ft2             3.28083989501312
-!      m3/MJ                  =>   ft3/kWh             127.13292
-!      m3/person              =>   ft3/person          35.3146667214886
-!      m3/s                   =>   ft3/min             2118.88000328931
-!      m3/s-m                 =>   ft3/min-ft          645.89
-!      m3/s-m2                =>   ft3/min-ft2         196.85
-!      m3/s-person            =>   ft3/min-person      2118.6438
-!      m3/s-W                 =>   (ft3/min)/(Btu/h)   621.099127332943
-!      N-m                    =>   lbf-in              8.85074900525547
-!      N-s/m2                 =>   lbf-s/ft2           0.0208857913669065
-!      Pa                     =>   psi                 0.000145037743897283
-!      percent/K              =>   percent/F           0.555555555555556
-!      person/m2              =>   person/ft2          0.0928939733269818
-!      s/m                    =>   s/ft                0.3048
-!      V/K                    =>   V/F                 0.555555555555556
-!      W                      =>   Btu/h               3.4121412858518
-!      W/(m3/s)               =>   W/(ft3/min)         0.0004719475
-!      W/K                    =>   Btu/h-F             1.89563404769544
-!      W/m                    =>   Btu/h-ft            1.04072
-!      W/m2                   =>   Btu/h-ft2           0.316957210776545
-!      W/m2                   =>   W/ft2               0.09290304
-!      W/m2-K                 =>   Btu/h-ft2-F         0.176110194261872
-!      W/m2-K2                =>   Btu/h-ft2-F2        0.097826
-!      W/m-K                  =>   Btu-in/h-ft2-F      6.93481276005548
-!      W/m-K2                 =>   Btu/h-F2-ft         0.321418310071648
-!      W/m-K3                 =>   Btu/h-F3-ft         0.178565727817582
-!      W/person               =>   Btu/h-person        3.4121412858518
-!
-! Other conversions supported (needs the \ip-units code)
-!
-!      kPa                    =>   inHg                0.29523
-!      m                      =>   in                  39.3700787401575
-!      m3/s                   =>   gal/min             15850.3222370511
-!      Pa                     =>   ftH2O               0.00033455
-!      Pa                     =>   inH2O               0.00401463
-!      Pa                     =>   inHg                0.00029613
-!      Pa                     =>   Pa                  1
-!      W                      =>   W                   1
-!      W/m2                   =>   W/m2                1
-!      W/m-K                  =>   Btu/h-ft-F          0.577796066000163
-!      W/person               =>   W/person            1
-!
-! Units fields that are not translated
-!      $
-!      1/hr
-!      A
-!      Ah
-!      A/V
-!      Availability
-!      Control
-!      cycles/hr
-!      days
-!      deg
-!      dimensionless
-!      eV
-!      hr
-!      J/J
-!      kg/kg
-!      kg-H2O/kg-air
-!      kmol
-!      kmol/s
-!      m3/m3
-!      minutes
-!      Mode
-!      ms
-!      ohms
-!      percent
-!      ppm
-!      rev/min
-!      s
-!      V
-!      VA
-!      W/m2 or deg C
-!      W/m2, W or deg C
-!      W/s
-!      W/W
-!      years
-! **************************************************************************
-```
-
-### Example Object
-
-The Site:Location object will serve as an example.
-
-```idd
-Site:Location,
-       \unique-object
-       \min-fields 5
-  A1 , \field Name
-       \required-field
-       \type  alpha
-  N1 , \field Latitude
-       \units deg
-       \minimum -90.0
-       \maximum +90.0
-       \default 0.0
-       \note + is North, - is South, degree minutes represented in decimal (i.e. 30 minutes is .5)
-       \type real
-  N2 , \field Longitude
-       \units deg
-       \minimum -180.0
-       \maximum +180.0
-       \default 0.0
-       \note - is West, + is East, degree minutes represented in decimal (i.e. 30 minutes is .5)
-       \type real
-  N3 , \field Time Zone
-       \note basic these limits on the WorldTimeZone Map (2003)
-       \units hr
-       \minimum -12.0
-       \maximum +14.0
-       \default 0.0
-       \note  Time relative to GMT. Decimal hours.
-       \type real
-  N4 ; \field Elevation
-       \units m
-       \minimum -300.0
-       \maximum&lt; 6096.0
-       \default 0.0
-       \type real
-```
-
-
-First, the object name is given.  (Site:Location)  This is followed by a comma in both the definition (IDD) and in an input file (IDF).  In fact, all fields except the terminating field of an IDD class object and IDF object are followed by commas.  The final field in an IDD class object or in an IDF object is terminated by a semi-colon.
-
-Next is an alpha field, the location name.  As noted above, for input, spaces are significant in this field.  The main inputs for Location are numeric fields.  These are numbered (as is the alpha field) for convenience.  The \\ designations will show various information about the objects as described above in the IDD conventions discussion.  Of importance for reading this document are the units and possible minimum and maximum values for a  field.  Defaults are produced if applicable and if the field is blank in the IDF.  For this example, that won’t work because there is no default AND the Location name is a required field.
-
-The \\minimum, \\maximum and \\default comments are automatically processed in the Inptu Processor for numeric fields.  Any infractions of the \\minimum, \\maximum fields will be automatically detected and messages will appear in the standard error file.  After all the input is checked, infractions will cause program termination (before the bulk of the simulation is completed).  Defaults are also enforced if you leave the numeric field blank.
-
-\\min-fields deserves some explanation.  This has object level enforcement.  When min-fields is specified for an object, it has meaning to the InputProcessor – telling the IP the number of fields that must be returned to a GetInput routine regardless of how many fields may actually appear in the IDF.  So, min-fields is actually an automatic assistance in most instances.
-
-Some objects need all the parameters listed by the definition; some do not.  In the descriptions that are contained in the Input Output Reference, we try to indicate which parts are optional.  Usually, these will be the last fields in the object input or definition.
-
-### Using the Input-Output Reference Document
-
-To assist you in using the [Input Output Reference](file:///E:\Docs4PDFs\InputOutputReference.pdf) document, it is grouped similarly to the IDD file.
-
-To determine the latest set of groups and objects, it will be useful for you to open the IDFEditor (an intelligent editor that is installed with EnergyPlus) and write out the current object list.  The following figure shows the screen shot of the IDFEditor and the help menu to select the objectlist.  Select “**create objectlist.txt**� to create the object list – it will be put into the IDFEditor program folder.
-
-![](media/image002.jpg)
-
-Figure 2. Using IDFEditor to find the latest groups and objects for the Energy+.idd
-
-The produced list will look something like:
-
-Simulation Parameters
-
----------------------------
-
-[------]  Version
-
-[------]  SimulationControl
-
-[------]  Building
-
-[------]  ShadowCalculation
-
-[------]  SurfaceConvectionAlgorithm:Inside
-
-[------]  SurfaceConvectionAlgorithm:Outside
-
-[------]  HeatBalanceAlgorithm
-
-[------]  ZoneCapacitanceMultiplier
-
-[------]  Timestep
-
-[------]  ConvergenceLimits
-
-
-
-Location - Climate - Weather File Access
-
----------------------------
-
-[------]  Site:Location
-
-[------]  SizingPeriod:DesignDay
-
-[------]  SizingPeriod:WeatherFileDays
-
-[------]  SizingPeriod:WeatherFileConditionType
-
-[------]  RunPeriod
-
-[------]  RunPeriodControl:SpecialDays
-
-[------]  RunPeriodControl:DaylightSavingTime
-
-“Simulation Parameters� and “Location – Climate – Weather File Access� are groups. Version, Building, etc are objects.
-
-Standard EnergyPlus Units
--------------------------
-
-EnergyPlus expects information in a single unit system (SI).  This requires interface developers to convert user inputs from those preferred by architects and engineers into the standard metric units of EnergyPlus.  EnergyPlus will not perform any units conversions and will not have any unit conversion routines.
-
-ASCII with no spaces is used for abbreviations.  Note that exponents appear without any indication of exponentiation: i.e., kg/m3 not kg/m^3 or kg/m\*\*3.  Also note the use of dashes.  We have W/m2-K not W/m2\*K or W/(m2\*K).
-
-At the end we note the “problem� variables – the inputs that have non-standard units. Inputs using these units will have to be changed and the code checked to see how the quantities are used internally.
-
-Table 1. Standard EnergyPlus Units
-
-<table class="table table-striped">
-<tr>
-<th>Quantity</th>
-<th>unit</th>
-<th>abbreviation</th>
-</tr>
-<tr>
-<td>angular degrees</td>
-<td>degree</td>
-<td>deg</td>
-</tr>
-<tr>
-<td>Length</td>
-<td>meter</td>
-<td>m</td>
-</tr>
-<tr>
-<td>Area</td>
-<td>square meter</td>
-<td>m2</td>
-</tr>
-<tr>
-<td>Volume</td>
-<td>cubic meter</td>
-<td>m3</td>
-</tr>
-<tr>
-<td>Time</td>
-<td>seconds</td>
-<td>s</td>
-</tr>
-<tr>
-<td>Frequency</td>
-<td>Hertz</td>
-<td>Hz</td>
-</tr>
-<tr>
-<td>Temperature</td>
-<td>Celsius</td>
-<td>C</td>
-</tr>
-<tr>
-<td>absolute temperature</td>
-<td>Kelvin</td>
-<td>K</td>
-</tr>
-<tr>
-<td>temperature difference</td>
-<td>Kelvin</td>
-<td>delK</td>
-</tr>
-<tr>
-<td>speed</td>
-<td>meters per second</td>
-<td>m/s</td>
-</tr>
-<tr>
-<td>energy (or work)</td>
-<td>Joules</td>
-<td>J</td>
-</tr>
-<tr>
-<td>power</td>
-<td>Watts</td>
-<td>W</td>
-</tr>
-<tr>
-<td>mass</td>
-<td>kilograms</td>
-<td>kg</td>
-</tr>
-<tr>
-<td>force</td>
-<td>Newton</td>
-<td>N</td>
-</tr>
-<tr>
-<td>mass flow</td>
-<td>kilograms per second</td>
-<td>kg/s</td>
-</tr>
-<tr>
-<td>volume flow</td>
-<td>cubic meters per second</td>
-<td>m3/s</td>
-</tr>
-<tr>
-<td>pressure</td>
-<td>Pascals</td>
-<td>Pa</td>
-</tr>
-<tr>
-<td>pressure difference</td>
-<td>Pascals</td>
-<td>delPa</td>
-</tr>
-<tr>
-<td>specific enthalpy</td>
-<td>Joules per kilogram</td>
-<td>J/kg</td>
-</tr>
-<tr>
-<td>density</td>
-<td>kilograms per cubic meter</td>
-<td>kg/m3</td>
-</tr>
-<tr>
-<td>heat flux</td>
-<td>watts per square meter</td>
-<td>W/m2</td>
-</tr>
-<tr>
-<td>specific heat</td>
-<td>-------</td>
-<td>J/kg-K</td>
-</tr>
-<tr>
-<td>conductivity</td>
-<td>-------</td>
-<td>W/m-K</td>
-</tr>
-<tr>
-<td>diffusivity</td>
-<td>-------</td>
-<td>m2/s</td>
-</tr>
-<tr>
-<td>heat transfer coefficient</td>
-<td>-------</td>
-<td>W/m2-K</td>
-</tr>
-<tr>
-<td>R-value</td>
-<td>-------</td>
-<td>m2-K/W</td>
-</tr>
-<tr>
-<td>heating or cooling capacity</td>
-<td>Watts</td>
-<td>W</td>
-</tr>
-<tr>
-<td>electric potential</td>
-<td>volts</td>
-<td>V</td>
-</tr>
-<tr>
-<td>electric current</td>
-<td>Amperes</td>
-<td>A</td>
-</tr>
-<tr>
-<td>illuminace</td>
-<td>lux</td>
-<td>lx</td>
-</tr>
-<tr>
-<td>luminous flux</td>
-<td>lumen</td>
-<td>lm</td>
-</tr>
-<tr>
-<td>luminous intensity</td>
-<td>candelas</td>
-<td>cd</td>
-</tr>
-<tr>
-<td>luminance</td>
-<td>candelas per square meter</td>
-<td>cd/m2</td>
-</tr>
-<tr>
-<td>vapor diffusivity</td>
-<td>m2/s</td>
-<td> </td>
-</tr>
-<tr>
-<td>viscosity</td>
-<td>-------</td>
-<td>kg/m-s</td>
-</tr>
-<tr>
-<td>porosity</td>
-<td>-------</td>
-<td>m3/m3</td>
-</tr>
-<tr>
-<td>thermal gradient coeff for moisture capacity</td>
-<td>-------</td>
-<td>kg/kg-K</td>
-</tr>
-<tr>
-<td>isothermal moisture capacity</td>
-<td>-------</td>
-<td>m3/kg</td>
-</tr>
-</table>
-
-
-
-EnergyPlus Reports
-------------------
-
-Several items are used to specify what will appear in the output file(s).  The output is described in the next section of this document.  What appears here is a sample of outputs – more detailed and complete versions can be found in the “Output Details and Examples� document. In addition to the individual reports, there are sets of predefined reports that can appear.  View the Input for Output section and the Tabular reports section in the Input Output Reference document for more details.
-
-Output
-======
-
-EnergyPlus produces several output files as shown in the section on “Running EnergyPlus�.   This section will discuss the data contained in the “standard� output file (**eplusout.eso**).  It, too, has a data dictionary but unlike the input files, the output data dictionary is contained within the output file.  Thus, the basic structure of the standard output file is:
-
-```
-Data Dictionary Information
-End of Data Dictionary
-Data
-…
-Data
-End of Data
-```
-
-As with the IDF structure, there are rules associated with the interpretation of the standard output data dictionary.  These rules are summarized as follows:
-
-- The first item on each line is an integer which represents the “report code�.  This “report code� will be listed in the data section where it will also be the first item on each line, identifying the data.  Only 2 lines in the output file will not have an integer as the first item (“End of Data Dictionary� and “End of Data� lines).
-
-- The second item on each line is also an integer.  This integer corresponds to the number of items left on the dictionary line.  Each string consists of a variable name and units in square brackets.  Square brackets are required for all strings.  If there are no units associated with a particular variable, then there are no characters between the brackets.
-
-Six standard items appear at the start of every EnergyPlus Standard Output File Data Dictionary:
-
-```
-Program Version,EnergyPlus, 1.0, Beta 2, Build 017
-1,5,Environment Title[],Latitude[degrees],Longitude[degrees],Time Zone[],Elevation[m]
-2,6,Day of Simulation[],Month[],Day of Month[],DST Indicator[1=yes 0=no], Hour[], StartMinute[], EndMinute[], DayType
-3,3,Cumulative Day of Simulation[],Month[],Day of Month[],DST Indicator[1=yes 0=no],DayType
-4,2,Cumulative Days of Simulation[],Month[]
-5,1,Cumulative Days of Simulation[]
-```
-
-* Item 0 is the program version statement.
-
-* Item 1 is produced at the beginning of each new “environment� (design day, run period).
-
-* Item 2 is produced prior to any variable reported at the timestep or hourly intervals.  Hourly intervals will be shown with a start minute of 0.0 and an end minute of 60.0.  Timestep intervals will show the appropriate start and end minutes.
-
-* Item 3 is produced prior to any variable reported at the daily interval.
-
-* Item 4 is produced prior to any variable reported at the monthly interval.
-
-* Item 5 is produced prior to any variable reported at the end of the “environment�.
-
-Following these five standard lines will be the variables requested for reporting from the input file (ref. Report Variable).  For example:
-
-```
-6,2,Environment,Outdoor Dry Bulb [C] !Hourly
-21,2,ZONE ONE,Mean Air Temperature[C] !Hourly
-22,2,ZONE ONE,Zone-Total Latent Gain[J] !Hourly
-26,2,ZONE ONE,Zone-Total Electric Consumption[J] !Hourly
-```
-
-This example illustrates the non-consecutive nature of the “report codes�.  Internally, EnergyPlus counts each variable that *could* be reported.  This is the assigned “report code�.  However, the user may not request each possible variable for reporting.  Note that, currently, the requested reporting frequency is shown as a comment (!) line in the standard output file.
-
-The data is produced when the actual simulation is performed (after the warmup days).  Data output is simpler in format than the data dictionary lines.  From the dictionary above:
-
-```
-1,DENVER COLORADO WINTER,  39.75,-104.87,  -7.00,1610.26
-2,  1, 1,21, 0, 1, 0.00,60.00,Monday
-6,-17.22222
-21,-17.22219
-22,0.0000000E+00
-26,0.0000000E+00
-2,  1, 1,21, 0, 2, 0.00,60.00,Monday
-6,-17.22222
-21,-17.22219
-22,0.0000000E+00
-26,0.0000000E+00
-2,  1, 1,21, 0, 3, 0.00,60.00,Monday
-6,-17.22222
-21,-17.22219
-22,0.0000000E+00
-26,0.0000000E+00
-```
-
-This output file can be easily turned into a form that is read into commonly used spreadsheet programs where it can be further analyzed, graphed, etc.
-
-![](media/image003.png)
-
-Figure 3.  Example Chart from Standard Output File
-
-Weather Data
-============
-
-Weather data in EnergyPlus is a simple text-based format, similar to the input data and output data files. The weather data format includes basic location information in the first eight lines: location (name, state/province/region, country), data source, latitude, longitude, time zone, elevation, peak heating and cooling design conditions, holidays, daylight saving period, typical and extreme periods, two lines for comments, and period covered by the data. The data are also comma-separated and contain much of the same data in the TMY2 weather data set (NREL 1995). EnergyPlus does not require a full year or 8760 (or 8784) hours in its weather files. In fact, EnergyPlus allows and reads subsets of years and even sub-hourly (5 minute, 15 minute) data—the weather format includes a ‘minutes’ field. EnergyPlus comes with a utility that reads standard weather service file types such as TMY2, IWEC and WYEC2 files, as examples, as well as being able to read a user defined custom format.
-
-The “data dictionary� for EnergyPlus Weather Data is shown in the Auxiliary Programs document – please review that document for further information.
-
-Running EnergyPlus
-==================
-
-EnergyPlus is written in C++ and runs as a console application. More explicit details on running EnergyPlus are available in a separate document (Running EnergyPlus in Auxiliary Programs document). Optional command-line arguments are available (energyplus --help, or man energyplus on Linux systems). The following files are used to run EnergyPlus:
-
-* EnergyPlus.exe (the executable file)
-
-* Energy+.ini (described below)
-
-* Energy+.idd (the input data dictionary file)
-
-* In.idf (the input file)
-
-* In.epw – optional (weather data file)
-
-The input data dictionary and input data file have been discussed in the previous sections of this document.
-
-For weather simulations, EnergyPlus accepts EnergyPlus weather files. Previous versions accepted BLAST formatted weather files and now a BLASTWeatherConverter program is provided.  The actual file name is **in.epw**.
-
-The Energy+.ini file is a “standard� Windows™ ini file and can be manipulated using the Windows API calls though EnergyPlus uses standard Fortran to manipulate it.  It is a very simple ini file and is fully described in the [Auxiliary Programs](file:///E:\Docs4PDFs\AuxiliaryPrograms.pdf) document. Energy+.ini and in.idf file should be in the directory from which you are running EnergyPlus.exe.
-
-For the advanced user, there is also the “EPMacro� program, described in the Auxiliary Programs Document.  You run it as a separate program before EnergyPlus (the batch file included in the install and shown in the GettingStarted document contains the commands).
-
-EnergyPlus creates the following files (plus more):
-
-Table 2.  EnergyPlus Output Files
-
-<table class="table table-striped">
-<tr>
-<th>FileName</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>Audit.out</td>
-<td>Echo of input</td>
-</tr>
-<tr>
-<td>Eplusout.err</td>
-<td>Error file</td>
-</tr>
-<tr>
-<td>Eplusout.eso</td>
-<td>Standard Output File</td>
-</tr>
-<tr>
-<td>Eplusout.eio</td>
-<td>One time output file</td>
-</tr>
-<tr>
-<td>Eplusout.rdd</td>
-<td>Report Variable Data Dictionary</td>
-</tr>
-<tr>
-<td>Eplusout.dxf</td>
-<td>DXF (from Report,Surfaces,DXF;)</td>
-</tr>
-<tr>
-<td>Eplusout.end</td>
-<td>A one line summary of success or failure</td>
-</tr>
-</table>
-
-
-
-
-
-The eplusout.err file may contain three levels of errors (Warning, Severe, Fatal) as well as the possibility of just message lines.  These errors may be duplicated in other files (such as the standard output file).
-
-Table 3.  EnergyPlus Errors
-
-<table class="table table-striped">
-<tr>
-<th>Error Level</th>
-<th>Action</th>
-</tr>
-<tr>
-<td>Warning</td>
-<td>Take note</td>
-</tr>
-<tr>
-<td>Severe</td>
-<td>Should Fix</td>
-</tr>
-<tr>
-<td>Fatal</td>
-<td>Program will abort</td>
-</tr>
-</table>
-
-EnergyPlus produces several messages as it is executing, as a guide to its progress.  For example, the run of the 1ZoneUncontrolled input file from Appendix A produces:
-
-```idf
-EnergyPlus Starting
- EnergyPlus 1.3.0.011, 4/5/2006 2:59 PM
- Initializing New Environment Parameters
- Warming up {1}
- Initializing Response Factors
- Initializing Window Optical Properties
- Initializing Solar Calculations
- Initializing HVAC
- Warming up {2}
- Warming up {3}
- Warming up {4}
- Starting Simulation at 12/21 for DENVER_STAPLETON ANN HTG 99% CONDNS DB
- Initializing New Environment Parameters
- Warming up {1}
- Warming up {2}
- Warming up {3}
- Starting Simulation at 07/21 for DENVER_STAPLETON ANN CLG 1% CONDNS DB=&gt;MWB
- EnergyPlus Run Time=00hr 00min  1.00sec
-```
-
-Extensive timing studies and fine-tuning of EnergyPlus is NOT complete.  To give you an idea of comparable run times, we present the following (does not include HVAC) with an early version of EnergyPlus running on a 450MHZ machine.  Remember, BLAST would be 1 calculation per hour, EnergyPlus (in this case) was 4 calculations per hour.  Obviously, these are quite out of date.  However, a recent change in a developer’s test machine illustrates the importance of maximum memory.  A 5 zone full year run on a 1.8GHZ, 1GB machine was running about 8 minutes – with a new 2.1GHZ, 2GB machine the same file takes about 2 minutes.
-
-Table 4.  Timings Comparison (EnergyPlus vs. BLAST)
-
-<table class="table table-striped">
-<tr>
-<th>File</th>
-<th>BLAST Per Zone</th>
-<th>EnergyPlus Per Zone</th>
-</tr>
-<tr>
-<td>GeometryTest (5 Zones, 2 Design Day, Full Weather Year)</td>
-<td>13 sec</td>
-<td>33 sec</td>
-</tr>
-<tr>
-<td>SolarShadingTest (9 Zones, Full Weather Year)</td>
-<td>7 sec</td>
-<td>25 sec</td>
-</tr>
-</table>
-
-Licensing
-=========
-
-In order to make efficient distribution of your interface, you should consider licensing EnergyPlus.  First, you must license/register to use EnergyPlus.  Since we are distributing EnergyPlus via the World Wide Web, at no charge, it will be easy to get your hands on a copy for testing out your interface.  However, you may wish to understand more of the internals and, to make a complete distribution package, will need to at least execute a distribution license.
-
-https://energyplus.net/licensing contains the details on licensing EnergyPlus for commercial or non-commercial use.
-
-Appendix A.  Simple IDF file
-============================
-
-```idf
-!1ZoneUncontrolled.idf
-! Basic file description:  Basic test for EnergyPlus.  Resistive Walls.  Regular (no ground contact) floor.
-!                          Regular roof.  No Windows.
-!
-! Highlights:              Very basic test to see that EnergyPlus "works".
-!
-!
-! Simulation Location/Run: DENVER_STAPLETON_CO_USA_WMO_724690, 2 design days, 1 run period,
-!                          Run Control executes two design days (see RUN PERIOD object)
-!
-! Location:                Denver, CO
-!
-! Design Days:             DENVER_STAPLETON_CO_USA Annual Heating 99%, MaxDB=-16°C
-!                          DENVER_STAPLETON_CO_USA Annual Cooling (DB=&gt;MWB) 1%, MaxDB=32.6°C MWB=15.5°C
-!
-! Run Period (Weather File): Full Annual Simulation, DENVER_STAPLETON_CO_USA_WMO_724690
-!
-! Run Control:             No zone or system sizing, design day run control (no weather file simulation)
-!
-! Building: Fictional 1 zone building with resistive walls.
-!
-!           The building is oriented due north.
-!
-! Floor Area:        232.25 m2
-! Number of Stories: 1
-!
-! Zone Description Details:
-!
-!       (0,15.24,0)                 (15.24,15.24,0)
-!              _____________________________
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |                             |
-!             |_____________________________|
-!
-!          (0,0,0)                      (15.24,0,0)
-!
-! Internal gains description:     NA
-!
-! Interzone Surfaces:             None
-! Internal Mass:                  None
-! People:                         None
-! Lights:                         None
-! Equipment:                      None
-! Windows:                        0
-! Detached Shading:               None
-! Daylight:                       None
-! Natural Ventilation:            None
-! Compact Schedules:              NA (Example of non-Compact Schedules)
-! Solar Distribution:             MinimalShadowing
-!
-! HVAC:                           NA
-!
-! Zonal Equipment:                NA
-! Central Air Handling Equipment: No
-! System Equipment Autosize:      No
-! Purchased Cooling:              No
-! Purchased Heating:              No
-! Purchased Chilled Water:        No
-! Purchased Hot Water:            No
-! Coils:                          None
-! Pumps:                          None
-! Boilers:                        None
-! Chillers:                       None
-! Towers:                         None
-!
-! Results:
-! Standard Reports:               Variable Dictionary, Surfaces (dxf-wireframe), Meter File
-! Timestep or Hourly Variables:   Hourly and Daily
-! Time bins Report:               None
-! HTML Report:                    None
-! Environmental Emissions:        None
-! Utility Tariffs:                None
-
-
-  Output:PreprocessorMessage,
-    No Preprocessor Used,    !- Preprocessor Name
-    Information,             !- Error Severity
-    Illustrative Message,    !- Message Line 1
-    No problems for processing;  !- Message Line 2
-
-
-  Version,
-    3.0;                     !- Version Identifier
-
-
-  Timestep,
-    4;                       !- Number of Timesteps per Hour
-
-
-  Building,
-    Simple One Zone (Wireframe DXF),  !- Name
-    0.0000000E+00,           !- North Axis {deg}
-    Suburbs,                 !- Terrain
-    .04,                     !- Loads Convergence Tolerance Value
-    .004,                    !- Temperature Convergence Tolerance Value {deltaC}
-    MinimalShadowing,        !- Solar Distribution
-    30;                      !- Maximum Number of Warmup Days
-
-
-  HeatBalanceAlgorithm,
-    ConductionTransferFunction;  !- Algorithm
-
-
-  SurfaceConvectionAlgorithm:Inside,
-    Detailed;                !- Algorithm
-
-
-  SurfaceConvectionAlgorithm:Outside,
-    Detailed;                !- Algorithm
-
-
-  SimulationControl,
-    No,                      !- Do Zone Sizing Calculation
-    No,                      !- Do System Sizing Calculation
-    No,                      !- Do Plant Sizing Calculation
-    Yes,                     !- Run Simulation for Sizing Periods
-    Yes;                     !- Run Simulation for Weather File Run Periods
-
-
-  RunPeriod,
-    1,                       !- Begin Month
-    1,                       !- Begin Day of Month
-    12,                      !- End Month
-    31,                      !- End Day of Month
-    Tuesday,                 !- Day of Week for Start Day
-    Yes,                     !- Use Weather File Holidays and Special Days
-    Yes,                     !- Use Weather File Daylight Saving Period
-    No,                      !- Apply Weekend Holiday Rule
-    Yes,                     !- Use Weather File Rain Indicators
-    Yes;                     !- Use Weather File Snow Indicators
-
-
-  Site:Location,
-    DENVER_STAPLETON_CO_USA_WMO_724690,  !- Name
-    39.77,                   !- Latitude {deg}
-    -104.87,                 !- Longitude {deg}
-    -7.00,                   !- Time Zone {hr}
-    1611.00;                 !- Elevation {m}
-
-
- !  WMO=724690 Time Zone=NAM        (GMT-07:00) Mountain Time (US & Canada)
- !  Data Source=ASHRAE 2005 Annual Design Conditions
- ! Using Design Conditions from "Climate Design Data 2005 ASHRAE Handbook"
- ! DENVER_STAPLETON_CO_USA Extreme Annual Wind Speeds, 1%=10.9m/s, 2.5%=8.8m/s, 5%=7.7m/s
- ! DENVER_STAPLETON_CO_USA Extreme Annual Temperatures, Max Drybulb=37.2°C Min Drybulb=-24.6°C
- ! DENVER_STAPLETON_CO_USA Annual Heating Design Conditions Wind Speed=2.3m/s Wind Dir=180
- ! Coldest Month=December
- ! DENVER_STAPLETON_CO_USA Annual Heating 99%, MaxDB=-16°C
-
-
-  SizingPeriod:DesignDay,
-    DENVER_STAPLETON Ann Htg 99% Condns DB,  !- Name
-    -16,                     !- Maximum Dry-Bulb Temperature {C}
-    0.0,                     !- Daily Temperature Range {deltaC}
-    -16,                     !- Humidity Indicating Conditions at Maximum Dry-Bulb
-    83411.,                  !- Barometric Pressure {Pa}
-    2.3,                     !- Wind Speed {m/s}
-    180,                     !- Wind Direction {deg}
-    0.00,                    !- Sky Clearness
-    0,                       !- Rain Indicator
-    0,                       !- Snow Indicator
-    21,                      !- Day of Month
-    12,                      !- Month
-    WinterDesignDay,         !- Day Type
-    0,                       !- Daylight Saving Time Indicator
-    WetBulb;                 !- Humidity Indicating Type
-
-
- ! DENVER_STAPLETON Annual Cooling Design Conditions Wind Speed=4m/s Wind Dir=120
- ! Hottest Month=July
- ! DENVER_STAPLETON_CO_USA Annual Cooling (DB=&gt;MWB) 1%, MaxDB=32.6°C MWB=15.5°C
-
-
-  SizingPeriod:DesignDay,
-    DENVER_STAPLETON Ann Clg 1% Condns DB=&gt;MWB,  !- Name
-    32.6,                    !- Maximum Dry-Bulb Temperature {C}
-    15.2,                    !- Daily Temperature Range {deltaC}
-    15.5,                    !- Humidity Indicating Conditions at Maximum Dry-Bulb
-    83411.,                  !- Barometric Pressure {Pa}
-    4,                       !- Wind Speed {m/s}
-    120,                     !- Wind Direction {deg}
-    1.00,                    !- Sky Clearness
-    0,                       !- Rain Indicator
-    0,                       !- Snow Indicator
-    21,                      !- Day of Month
-    7,                       !- Month
-    SummerDesignDay,         !- Day Type
-    0,                       !- Daylight Saving Time Indicator
-    WetBulb;                 !- Humidity Indicating Type
-
-
-  Material:NoMass,
-    R13LAYER,                !- Name
-    Rough,                   !- Roughness
-    2.290965,                !- Thermal Resistance {m2-K/W}
-    0.9000000,               !- Thermal Absorptance
-    0.7500000,               !- Solar Absorptance
-    0.7500000;               !- Visible Absorptance
-
-
-  Material:NoMass,
-    R31LAYER,                !- Name
-    Rough,                   !- Roughness
-    5.456,                   !- Thermal Resistance {m2-K/W}
-    0.9000000,               !- Thermal Absorptance
-    0.7500000,               !- Solar Absorptance
-    0.7500000;               !- Visible Absorptance
-
-
-  Material,
-    C5 - 4 IN HW CONCRETE,   !- Name
-    MediumRough,             !- Roughness
-    0.1014984,               !- Thickness {m}
-    1.729577,                !- Conductivity {W/m-K}
-    2242.585,                !- Density {kg/m3}
-    836.8000,                !- Specific Heat {J/kg-K}
-    0.9000000,               !- Thermal Absorptance
-    0.6500000,               !- Solar Absorptance
-    0.6500000;               !- Visible Absorptance
-
-
-  Construction,
-    R13WALL,                 !- Name
-    R13LAYER;                !- Outside Layer
-
-
-  Construction,
-    FLOOR,                   !- Name
-    C5 - 4 IN HW CONCRETE;   !- Outside Layer
-
-
-  Construction,
-    ROOF31,                  !- Name
-    R31LAYER;                !- Outside Layer
-
-
-  Site:GroundTemperature:BuildingSurface,
-    18.89,                   !- January Ground Temperature {C}
-    18.92,                   !- February Ground Temperature {C}
-    19.02,                   !- March Ground Temperature {C}
-    19.12,                   !- April Ground Temperature {C}
-    19.21,                   !- May Ground Temperature {C}
-    19.23,                   !- June Ground Temperature {C}
-    19.07,                   !- July Ground Temperature {C}
-    19.32,                   !- August Ground Temperature {C}
-    19.09,                   !- September Ground Temperature {C}
-    19.21,                   !- October Ground Temperature {C}
-    19.13,                   !- November Ground Temperature {C}
-    18.96;                   !- December Ground Temperature {C}
-
-
-  Zone,
-    ZONE ONE,                !- Name
-    0.0000000E+00,           !- Direction of Relative North {deg}
-    0.0000000E+00,           !- X Origin {m}
-    0.0000000E+00,           !- Y Origin {m}
-    0.0000000E+00,           !- Z Origin {m}
-    1,                       !- Type
-    1,                       !- Multiplier
-    autocalculate,           !- Ceiling Height {m}
-    autocalculate;           !- Volume {m3}
-
-
-  ScheduleTypeLimits,
-    Fraction,                !- Name
-    0.0 : 1.0,               !- Range
-    CONTINUOUS;              !- Numeric Type
-
-
-  GlobalGeometryRules,
-    UpperLeftCorner,         !- Starting Vertex Position
-    CounterClockWise,        !- Vertex Entry Direction
-    WorldCoordinateSystem;   !- Coordinate System
-
-
-  BuildingSurface:Detailed,
-    Zn001:Wall001,           !- Name
-    Wall,                    !- Surface Type
-    R13WALL,                 !- Construction Name
-    ZONE ONE,                !- Zone Name
-    Outdoors,                !- Outside Boundary Condition
-    ,                        !- Outside Boundary Condition Object
-    SunExposed,              !- Sun Exposure
-    WindExposed,             !- Wind Exposure
-    0.5000000,               !- View Factor to Ground
-    4,                       !- Number of Vertices
-    0.0000000E+00,0.0000000E+00,4.572000,  !- X,Y,Z ==&gt; Vertex 1
-    0.0000000E+00,0.0000000E+00,0.0000000E+00,  !- X,Y,Z ==&gt; Vertex 2
-    15.24000,0.0000000E+00,0.0000000E+00,  !- X,Y,Z ==&gt; Vertex 3
-    15.24000,0.0000000E+00,4.572000;  !- X,Y,Z ==&gt; Vertex 4
-
-
-  BuildingSurface:Detailed,
-    Zn001:Wall002,           !- Name
-    Wall,                    !- Surface Type
-    R13WALL,                 !- Construction Name
-    ZONE ONE,                !- Zone Name
-    Outdoors,                !- Outside Boundary Condition
-    ,                        !- Outside Boundary Condition Object
-    SunExposed,              !- Sun Exposure
-    WindExposed,             !- Wind Exposure
-    0.5000000,               !- View Factor to Ground
-    4,                       !- Number of Vertices
-    15.24000,0.0000000E+00,4.572000,  !- X,Y,Z ==&gt; Vertex 1
-    15.24000,0.0000000E+00,0.0000000E+00,  !- X,Y,Z ==&gt; Vertex 2
-    15.24000,15.24000,0.0000000E+00,  !- X,Y,Z ==&gt; Vertex 3
-    15.24000,15.24000,4.572000;  !- X,Y,Z ==&gt; Vertex 4
-
-
-  BuildingSurface:Detailed,
-    Zn001:Wall003,           !- Name
-    Wall,                    !- Surface Type
-    R13WALL,                 !- Construction Name
-    ZONE ONE,                !- Zone Name
-    Outdoors,                !- Outside Boundary Condition
-    ,                        !- Outside Boundary Condition Object
-    SunExposed,              !- Sun Exposure
-    WindExposed,             !- Wind Exposure
-    0.5000000,               !- View Factor to Ground
-    4,                       !- Number of Vertices
-    15.24000,15.24000,4.572000,  !- X,Y,Z ==&gt; Vertex 1
-    15.24000,15.24000,0.0000000E+00,  !- X,Y,Z ==&gt; Vertex 2
-    0.0000000E+00,15.24000,0.0000000E+00,  !- X,Y,Z ==&gt; Vertex 3
-    0.0000000E+00,15.24000,4.572000;  !- X,Y,Z ==&gt; Vertex 4
-
-
-  BuildingSurface:Detailed,
-    Zn001:Wall004,           !- Name
-    Wall,                    !- Surface Type
-    R13WALL,                 !- Construction Name
-    ZONE ONE,                !- Zone Name
-    Outdoors,                !- Outside Boundary Condition
-    ,                        !- Outside Boundary Condition Object
-    SunExposed,              !- Sun Exposure
-    WindExposed,             !- Wind Exposure
-    0.5000000,               !- View Factor to Ground
-    4,                       !- Number of Vertices
-    0.0000000E+00,15.24000,4.572000,  !- X,Y,Z ==&gt; Vertex 1
-    0.0000000E+00,15.24000,0.0000000E+00,  !- X,Y,Z ==&gt; Vertex 2
-    0.0000000E+00,0.0000000E+00,0.0000000E+00,  !- X,Y,Z ==&gt; Vertex 3
-    0.0000000E+00,0.0000000E+00,4.572000;  !- X,Y,Z ==&gt; Vertex 4
-
-
-  BuildingSurface:Detailed,
-    Zn001:Flr001,            !- Name
-    Floor,                   !- Surface Type
-    FLOOR,                   !- Construction Name
-    ZONE ONE,                !- Zone Name
-    Surface,                 !- Outside Boundary Condition
-    Zn001:Flr001,            !- Outside Boundary Condition Object
-    NoSun,                   !- Sun Exposure
-    NoWind,                  !- Wind Exposure
-    1.000000,                !- View Factor to Ground
-    4,                       !- Number of Vertices
-    15.24000,0.000000,0.0,  !- X,Y,Z ==&gt; Vertex 1
-    0.000000,0.000000,0.0,  !- X,Y,Z ==&gt; Vertex 2
-    0.000000,15.24000,0.0,  !- X,Y,Z ==&gt; Vertex 3
-    15.24000,15.24000,0.0;  !- X,Y,Z ==&gt; Vertex 4
-
-
-  BuildingSurface:Detailed,
-    Zn001:Roof001,           !- Name
-    Roof,                    !- Surface Type
-    ROOF31,                  !- Construction Name
-    ZONE ONE,                !- Zone Name
-    Outdoors,                !- Outside Boundary Condition
-    ,                        !- Outside Boundary Condition Object
-    SunExposed,              !- Sun Exposure
-    WindExposed,             !- Wind Exposure
-    0.0000000E+00,           !- View Factor to Ground
-    4,                       !- Number of Vertices
-    0.000000,15.24000,4.572,  !- X,Y,Z ==&gt; Vertex 1
-    0.000000,0.000000,4.572,  !- X,Y,Z ==&gt; Vertex 2
-    15.24000,0.000000,4.572,  !- X,Y,Z ==&gt; Vertex 3
-    15.24000,15.24000,4.572;  !- X,Y,Z ==&gt; Vertex 4
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    outdoor dry bulb,        !- Variable Name
-    hourly;                  !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    Daylight Saving Time Indicator,  !- Variable Name
-    daily;                   !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    DayType Index,           !- Variable Name
-    daily;                   !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    Zone Mean Air Temperature,  !- Variable Name
-    hourly;                  !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    Zone Total Internal Latent Gain,  !- Variable Name
-    hourly;                  !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    Zone Mean Radiant Temperature,  !- Variable Name
-    hourly;                  !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    Zone Air Balance Surface Convection Rate,  !- Variable Name
-    hourly;                  !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    Zone Air Balance Air Energy Storage Rate,  !- Variable Name
-    hourly;                  !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    Surface Inside Temperature,  !- Variable Name
-    daily;                   !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    Surface Outside Temperature,  !- Variable Name
-    daily;                   !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    Surface Int Convection Coeff,  !- Variable Name
-    daily;                   !- Reporting Frequency
-
-
-  Output:Variable,
-    *,                       !- Key Value
-    Surface Ext Convection Coeff,  !- Variable Name
-    daily;                   !- Reporting Frequency
-
-
-  Output:Reports,
-    VariableDictionary,      !- Type of Report
-    IDF;                     !- Report Name
-
-
-  Output:Reports,
-    surfaces,                !- Type of Report
-    dxf:wireframe;           !- Report Name
-
-
-  Output:Reports,
-    construction;            !- Type of Report
-
-
-  Output:Meter:MeterFileOnly,
-    ExteriorLights:Electricity,  !- Name
-    hourly;                  !- Reporting Frequency
-
-
-  Output:Meter:MeterFileOnly,
-    Carbon Equivalent:Facility,  !- Name
-    hourly;                  !- Reporting Frequency
-
-
-  Output:Meter:MeterFileOnly,
-    EnergyTransfer:Building, !- Name
-    hourly;                  !- Reporting Frequency
-
-
-  Output:Meter:MeterFileOnly,
-    EnergyTransfer:Facility, !- Name
-    hourly;                  !- Reporting Frequency
-
-
-  OutputControl:Table:Style,
-    HTML;                    !- Column Separator
-
-
-  Output:Table:SummaryReports,
-    AllSummary;              !- Report 1 Name
-
-
-  Exterior:Lights,
-    ExtLights,               !- Name
-    AlwaysOn,                !- Schedule Name
-    5250,                    !- Design Level {W}
-    AstronomicalClock,       !- Control Option
-    Grounds Lights;          !- End-Use Subcategory
-
-
-  ScheduleTypeLimits,
-    On/Off,                  !- Name
-    0:1,                     !- Range
-    DISCRETE;                !- Numeric Type
-
-
-  Schedule:Day:Hourly,
-    On,                      !- Name
-    On/Off,                  !- Schedule Type Limits Name
-    1.,                      !- Hour 1
-    1.,                      !- Hour 2
-    1.,                      !- Hour 3
-    1.,                      !- Hour 4
-    1.,                      !- Hour 5
-    1.,                      !- Hour 6
-    1.,                      !- Hour 7
-    1.,                      !- Hour 8
-    1.,                      !- Hour 9
-    1.,                      !- Hour 10
-    1.,                      !- Hour 11
-    1.,                      !- Hour 12
-    1.,                      !- Hour 13
-    1.,                      !- Hour 14
-    1.,                      !- Hour 15
-    1.,                      !- Hour 16
-    1.,                      !- Hour 17
-    1.,                      !- Hour 18
-    1.,                      !- Hour 19
-    1.,                      !- Hour 20
-    1.,                      !- Hour 21
-    1.,                      !- Hour 22
-    1.,                      !- Hour 23
-    1.;                      !- Hour 24
-
-
-  Schedule:Week:Daily,
-    On Weeks,                !- Name
-    On,                      !- Sunday Schedule:Day Name
-    On,                      !- Monday Schedule:Day Name
-    On,                      !- Tuesday Schedule:Day Name
-    On,                      !- Wednesday Schedule:Day Name
-    On,                      !- Thursday Schedule:Day Name
-    On,                      !- Friday Schedule:Day Name
-    On,                      !- Saturday Schedule:Day Name
-    On,                      !- Holiday Schedule:Day Name
-    On,                      !- SummerDesignDay Schedule:Day Name
-    On,                      !- WinterDesignDay Schedule:Day Name
-    On,                      !- CustomDay1 Schedule:Day Name
-    On;                      !- CustomDay2 Schedule:Day Name
-
-
-  Schedule:Year,
-    AlwaysOn,                !- Name
-    On/Off,                  !- Schedule Type Limits Name
-    On Weeks,                !- Schedule:Week Name 1
-    1,                       !- Start Month 1
-    1,                       !- Start Day 1
-    12,                      !- End Month 1
-    31;                      !- End Day 1
-
-```
-
-
-
-
-
-
diff --git a/doc/src/docs/ModuleDeveloper/ModuleDeveloper.md b/doc/src/docs/ModuleDeveloper/ModuleDeveloper.md
deleted file mode 100644
index 5480686bb0a..00000000000
--- a/doc/src/docs/ModuleDeveloper/ModuleDeveloper.md
+++ /dev/null
@@ -1,11829 +0,0 @@
-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Guide for Module Developers</h1>
-<h2>Everything You Need to Know about Developing Modules and Modifying EnergyPlus</h2>
-<br/>
-<p><i>(but were hesitant to ask)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-Introduction
-============
-
-EnergyPlus is a modular simulation program designed to model the performance, energy consumption and pollutant production of a building. EnergyPlus models energy transport through the building envelope, heat gains within the building, and all the HVAC equipment used to heat and cool the building. The program is designed for ease of development. The concept is that many people will contribute to EnergyPlus and the program structure has been designed to make this possible.
-
-EnergyPlus is written entirely in Fortran 90 with updates to Fortran 95 – all of EnergyPlus code should be at minimum Fortran 90 compliant and can accept the newer features of Fortran 95 as well. Fortran 90/95 is a powerful modern programming language with many features. Using Fortran 90/95 it is possible to program in many different styles. The EnergyPlus team has chosen a particular style that emphasizes code extensibility (ease of development), understandability, maintainability, and robustness. Less emphasis was placed on program speed and size. Fortran 90/95 has all the features that permit the creation of readable, maintainable, and extensible code. In particular, the ability to create data and program modules with various levels of data hiding allows EnergyPlus to be built out of semi-independent modules. This allows a new EnergyPlus developer to concentrate on programming a single component without having to learn the entire program and data structure.
-
-The EnergyPlus programming style is described in the *EnergyPlus Programming Standard.* The *Programming Standard* should be consulted for details such as variable and subroutine naming conventions. In this document, we will describe the steps a developer must follow to create a new EnergyPlus component model. In particular, we will assume the developer wishes to simulate an HVAC component that cannot yet be modeled by EnergyPlus.
-
-Modules in EnergyPlus
-=====================
-
-What is a module anyway?
-------------------------
-
-### Program Modules
-
-A module is a Fortran 90/95 programming construct that can be used in various ways. In EnergyPlus, its primary use is to segment a rather large program into smaller, more manageable pieces. Each module is a separate package of source code stored on a separate file. The entire collection of modules, when compiled and linked, forms the executable code of EnergyPlus.
-
-Each module contains source code for closely related data structures and procedures. For instance, the WeatherManager module contains all the weather handling routines in EnergyPlus. The module is contained in the file WeatherManager.f90.  Another example is PlantPumps. This module contains all the code to simulate pumps in EnergyPlus. It is contained in file PlantPumps.f90.
-
-Of course dividing a program into modules can be done in various ways. We have attempted to create modules that are as self-contained as possible. The philosophy that has been used in creating EnergyPlus is contained in the [Programming Standard](file:///E:\Docs4PDFs\ProgrammingStandards.pdf) reference document.  Logically, the modules in EnergyPlus form an inverted tree structure. At the top is EnergyPlus. Just below that are ProcessInput and ManageSimulation. At the bottom are the modules such as HVACDamperComponent that model the actual HVAC components.
-
-### Data Only Modules
-
-EnergyPlus also uses modules that primary contain data and data structures that may be used by several modules. These modules form one of the primary ways data is structured and shared in EnergyPlus. An example is the DataEnvironment module. Many parts of the program need access to the outdoor conditions. All of that data is encapsulated in DataEnvironment. Modules that need this data obtain access through a Fortran USE statement. Without such access, modules cannot use or change this data.
-
-Sometimes data modules are extended to perform certain utilities or even getting input for the data structures that are the primary focus of the module but this is not a standard approach.
-
-What is a module developer?
----------------------------
-
-A module developer is someone who is going to add to the simulation capabilities of EnergyPlus. Someone, for instance, who is interested in adding code to model a new type of HVAC equipment. The most straightforward way of doing this is to create a new program module – hence the term “module developer�.   Another kind of module developer would be the adaptation of an existing “legacy� code to EnergyPlus.
-
-In EnergyPlus, one of the first steps in creating a new component model is to define the input. So, before we discuss modules in more detail, we must first describe the EnergyPlus input.
-
-Adding new features
--------------------
-
-The process for adding new features or significantly changing some features goes through a development team discussion period where the new feature is outlined, discussed and (hopefully) approved for inclusion.
-
-The team has a New Feature Proposal template document that is available to anyone wishing to add a new feature to EnergyPlus (or to auxiliary programs around EnergyPlus). The full New Feature Proposal format is shown in Appendix F.
-
-The sections of the New Feature Proposal are summarized in the following table:
-
-Table 1. Sections of a New Feature Proposal
-
-<table class="table table-striped">
-<tr>
-<td>Section</td>
-<td>Description</td>
-</tr>
-<tr>
-<td>Justification</td>
-<td>Why is the feature important.  Impact on energy use. What energy aspects the feature is using.</td>
-</tr>
-<tr>
-<td>Conference Call Conclusions</td>
-<td>Conclusions from the discussions (email or conference call)</td>
-</tr>
-<tr>
-<td>Other Conference Call topics</td>
-<td>Items outside the scope of the feature might be brought up but not able to be accomplished.</td>
-</tr>
-<tr>
-<td>Overview</td>
-<td>Description of the feature and references</td>
-</tr>
-<tr>
-<td>Approach</td>
-<td>What approach will be used.</td>
-</tr>
-<tr>
-<td>Testing/Validation data Sources</td>
-<td>Required</td>
-</tr>
-<tr>
-<td>IORef/Draft</td>
-<td>IDD Objects (new or revised) as well as full IOReference text</td>
-</tr>
-<tr>
-<td>Proposed Report Variables</td>
-<td>What outputs will come out of this feature.</td>
-</tr>
-<tr>
-<td>Proposed additions to meters</td>
-<td>How the outputs will affect the meter output</td>
-</tr>
-<tr>
-<td>Engineering Reference Draft</td>
-<td>Draft text for the Engineering Reference document</td>
-</tr>
-<tr>
-<td>Example File</td>
-<td>What/how many example files will be included or used to support this feature</td>
-</tr>
-<tr>
-<td>Transition changes</td>
-<td>What will be the required changes for current input files for this feature</td>
-</tr>
-<tr>
-<td>Other documents</td>
-<td>Other references.</td>
-</tr>
-</table>
-
-
-
-Then, of course, the document in Appendix G must be filled out and given to the proper people as well – to show that rights to the intellectual property of the new feature are owned by the developer.
-
-Input Concepts
-==============
-
-In EnergyPlus, input and output are accomplished by means of ASCII (text) files. On the input side, there are two files:
-
-1)   the Input Data Dictionary (IDD) that describes the types (classes) of input objects and the data associated with each object;
-
-2)   the Input Data File (IDF) that contains all the data for a particular simulation.
-
-Each EnergyPlus module is responsible for getting its own input. Of course, EnergyPlus provides services to the module that make this quite easy. The first task of a module developer is to design and insert a new entry into the Input Data Dictionary.
-
-Input Data Dictionary
----------------------
-
-An entry in the IDD consists of comma-separated text terminated by a semicolon. For instance:
-
-**Coil:Heating:Water,**
-
-       \\min-fields 14
-
-  A1 , \\field Name
-
-       \\required-field
-
-       \\type alpha
-
-       \\reference HeatingCoilName
-
-       \\reference HeatingCoilsWater
-
-  A2 , \\field Availability Schedule Name
-
-       \\type object-list
-
-       \\object-list ScheduleNames
-
-  N1 , \\field U-Factor Times Area Value
-
-       \\units W/K
-
-       \\autosizable
-
-       \\default Autosize
-
-  N2 , \\field Maximum Water Flow Rate
-
-       \\units m3/s
-
-       \\autosizable
-
-       \\ip-units gal/min
-
-       \\default Autosize
-
-  A3 , \\field Water Inlet Node Name
-
-       \\required-field
-
-  A4 , \\field Water Outlet Node Name
-
-       \\required-field
-
-  A5 , \\field Air Inlet Node Name
-
-       \\required-field
-
-  A6 , \\field Air Outlet Node Name
-
-       \\required-field
-
-  A7 , \\field Performance Input Method
-
-       \\type Choice
-
-       \\key UFactorTimesAreaAndDesignWaterFlowRate
-
-       \\key NominalCapacity
-
-       \\default UFactorTimesAreaAndDesignWaterFlowRate
-
-  N3 , \\field Nominal Capacity
-
-       \\type real
-
-       \\units W
-
-       \\autosizable
-
-       \\minimum 0
-
-       \\default Autosize
-
-  N4 , \\field Design Inlet Water Temperature
-
-       \\units C
-
-       \\type real
-
-       \\default 82.2
-
-  N5, \\field Design Inlet Air Temperature
-
-      \\units C
-
-      \\type real
-
-      \\default 16.6
-
-  N6, \\field Design Outlet Water Temperature
-
-      \\units C
-
-      \\type real
-
-      \\default 71.1
-
-  N7; \\field Design Outlet Air Temperature
-
-      \\units C
-
-      \\type real
-
-      \\default 32.2
-
-
-
-This entry defines a simple water-heating coil and specifies all of the input data needed to model it. The following rules apply.
-
-- The first element Coil:Heating:Water is the class name (also called a keyword or key).  This class name must be unique in the IDD.  The maximum length for the class name is 100 characters.  Embedded spaces are allowed and are significant.
-
-- In most cases, one should have fields following the object name.  An object name by itself (terminated with a semicolon) is a “section� – there may be uses for sections in input but the “Getting� of input is not hierarchical – one typically gets all objects of one type and then all objects of the next type.
-
-- In most cases, the second field of an object should be an “alpha� and the field name should contain the word “name�.  (This will allow for certain validations later on.)
-
-- Commas separate fields.  They always act as separators – thus there is no way to include a comma in a class name or as part of a data field.
-
-- Similarly, semicolons are terminators – a semicolon is always interpreted as the end of an EnergyPlus “sentence�. So, avoid embedded semicolons in class names or data fields.
-
-- Blank lines are allowed.
-
-- Each line can be up to 500 characters in length.
-
-- The comment character is an exclamation or a backslash.  Anything on a line after an “!� or a “\\� is ignored during EnergyPlus input.
-
-The only significant syntax elements are the commas, the semicolon, the N’s (denoting numeric data), and the A’s (denoting alphanumeric data) and the exclamation and backslash.  Everything else including blanks, end of lines, or even text that is not a comma, semicolon, N, or A is ignored.  There are several style conventions in use however.
-
-- Sequence numbers are appended to the letters A or N denoting each data element.  Thus, A2 is the second alphanumeric data item and N3 is the third numeric data item.
-
-- The class name contains a naming convention: type:subtype:subsubtype. For further naming conventions, please see the next section of this document.
-
-- Backslashes denote specially formatted comments. These comments provide information about the input, such as a description of the item, units, limits, mins & maxes, etc., in a form that can be processed by an input editor or interface. A complete description of the backslash comment format is given at the start of the IDD file and in the Guide for Interface Developers.  While these are “comments�, they are quite important and allow the InputProcessor module to do some error checking for you.   They are also used by the IDFEditor that many users continue to use and by interface developers in understanding EnergyPlus.
-
-- **\\default** – the number (N fields) or phrase (A fields) after this special field will be filled for any input file that has a blank in that field.
-
-- **\\minimum** or **\\minimum&gt;** -- the number following this special field will be automatically checked during input
-
-- **\\maximum** or **\\maximum&lt;** -- the number following this special field will be automatically checked during input
-
-- **\\extensible:\#** – allows you to structure your GetInput routine so that the object arguments can be expanded (you include the number of fields in the “extension� and the Input Processor can automatically extend IDD definitions) – you will still need to determine how many maximum arguments are in the object. The IDF Editor does not use this field and cannot auto-extend such objects if an IDF is encountered that has a greater number of fields than IDD allows.
-
-- **\\type integer** – (or **real** or **alpha**) – this field has gained increased importance after a user kept hitting an internal maximum detected by the program and kept increasing their input number until it overflowed the system’s integer size. Until all types are shown on numeric fields it will be hard for the InputProcessor to provide proper error detection.
-
-- **There are many more \\ fields** – these are described at the top of the IDD.
-
-Overall, the IDD file has very little structure.  Generally, a new entry should be placed next to entries describing similar components.  *Coil:Heating:Water*, for instance, is grouped with entries describing other water coils.
-
-**Summary**
-
-One of the early tasks for a module developer is to create a new entry in the Input Data Dictionary.  This entry defines the data needed to model the new component.
-
-Data Dictionary Naming Conventions
-----------------------------------
-
-### Class (Object) Names
-
-Class names shall be written in camel case where words are joined together without spaces and each word is capitalized. The colon shall be used to delimit hierarchy moving from general to specific. Natural language terminology shall be used when possible for each member separated by colons.
-
-Example: ZoneHVAC:PackagedTerminalHeatPump
-
-### Field Names
-
-Field names shall be written in title case where every major word is capitalized (exceptions: "a", "the", "for", etc.) with spaces separating words.  Field names shall be written using natural language terminology but should be relatively concise (no unnecessary abbreviations or acronyms).  If the field is for the name of this object, the field name shall simply be "Name" to eliminate redundancy.  The nature of an alpha field shall be explicit, for instance, "Availability Schedule Name" instead of merely "Availability Schedule". Generally, the object is not also included as the field name.
-
-Example: Availability Schedule Name
-
-When object names/types are included as part of the input, then the field name should contain “Object Type�:
-
-Example: Zone Equipment 1 Object Type
-
-### Choice Names
-
-When field choices list object references, the field choices shall list the class/object type name the same as its class definition in the IDD.  When field choices list other key words, the field choice names shall be written in camel case where words are joined together without spaces and each word is capitalized.  Field choice names shall be written using natural language terminology but should be relatively concise (no unnecessary abbreviations or acronyms) and avoid overly lengthy key words.  Field choice names shall only use alphanumeric characters with the addition of the forward slash ("/") character as a concise alternative to the word "per"; colons shall be allowed if the field choices are class names.
-
-  A2 , \\field Period Selection
-
-       \\retaincase
-
-       \\note Following is a list of all possible types of Extreme and Typical periods that
-
-       \\note might be identified in the Weather File. Not all possible types are available
-
-       \\note for all weather files.
-
-       \\type choice
-
-       \\key SummerExtreme
-
-       \\key SummerTypical
-
-       \\key WinterExtreme
-
-       \\key WinterTypical
-
-       \\key AutumnTypical
-
-       \\key SpringTypical
-
-       \\key WetSeason
-
-       \\key DrySeason
-
-       \\key NoDrySeason
-
-       \\key NoWetSeason
-
-       \\key TropicalHot
-
-       \\key TropicalCold
-
-Input Data File
----------------
-
-The Input Data File (IDF) is the file containing the data for an actual simulation.  This file is also a text (ASCII) file with a syntax “filling in the blanks� of the definitions in the IDD.  A portion of an IDF with input data for the hot water coil defined in the IDD example looks like:
-
-
-
-  Coil:Heating:Water,
-
-    SPACE1-1 Zone Coil,      !- Name
-
-    ReheatCoilAvailSched,    !- Availability Schedule Name
-
-    autosize,                !- U-Factor Times Area Value {W/K}
-
-    autosize,                !- Maximum Water Flow Rate {m3/s}
-
-    SPACE1-1 Zone Coil Water In Node,  !- Water Inlet Node Name
-
-    SPACE1-1 Zone Coil Water Out Node,  !- Water Outlet Node Name
-
-    SPACE1-1 Zone Coil Air In Node,  !- Air Inlet Node Name
-
-    SPACE1-1 In Node,        !- Air Outlet Node Name
-
-    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
-
-    autosize,                !- Nominal Capacity {W}
-
-    82.2,                    !- Design Inlet Water Temperature {C}
-
-    16.6,                    !- Design Inlet Air Temperature {C}
-
-    71.1,                    !- Design Outlet Water Temperature {C}
-
-    32.2;                    !- Design Outlet Air Temperature {C}
-
-
-
-  Coil:Heating:Water,
-
-    SPACE2-1 Zone Coil,      !- Name
-
-    ReheatCoilAvailSched,    !- Availability Schedule Name
-
-    autosize,                !- U-Factor Times Area Value {W/K}
-
-    autosize,                !- Maximum Water Flow Rate {m3/s}
-
-    SPACE2-1 Zone Coil Water In Node,  !- Water Inlet Node Name
-
-    SPACE2-1 Zone Coil Water Out Node,  !- Water Outlet Node Name
-
-    SPACE2-1 Zone Coil Air In Node,  !- Air Inlet Node Name
-
-    SPACE2-1 In Node,        !- Air Outlet Node Name
-
-    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
-
-    autosize,                !- Nominal Capacity {W}
-
-    82.2,                    !- Design Inlet Water Temperature {C}
-
-    16.6,                    !- Design Inlet Air Temperature {C}
-
-    71.1,                    !- Design Outlet Water Temperature {C}
-
-    32.2;                    !- Design Outlet Air Temperature {C}
-
-
-
-  Coil:Heating:Water,
-
-    SPACE3-1 Zone Coil,      !- Name
-
-    ReheatCoilAvailSched,    !- Availability Schedule Name
-
-    autosize,                !- U-Factor Times Area Value {W/K}
-
-    autosize,                !- Maximum Water Flow Rate {m3/s}
-
-    SPACE3-1 Zone Coil Water In Node,  !- Water Inlet Node Name
-
-    SPACE3-1 Zone Coil Water Out Node,  !- Water Outlet Node Name
-
-    SPACE3-1 Zone Coil Air In Node,  !- Air Inlet Node Name
-
-    SPACE3-1 In Node,        !- Air Outlet Node Name
-
-    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
-
-    autosize,                !- Nominal Capacity {W}
-
-    82.2,                    !- Design Inlet Water Temperature {C}
-
-    16.6,                    !- Design Inlet Air Temperature {C}
-
-    71.1,                    !- Design Outlet Water Temperature {C}
-
-    32.2;                    !- Design Outlet Air Temperature {C}
-
-
-
-Each coil entry begins with the class name (keyword) specifying the type of coil.  Next is the coil name – a user (or interface) created name that is unique within the given class.  Generally in EnergyPlus, objects within a class are distinguished by unique names.  The object name is usually the first data element following the class name.  Any alphanumeric data item in the IDF can be up to 100 characters long.  Any characters past 100 are truncated (lost). After the object name comes the real data.  If we look at the IDD we see that the first data item after the object name is expected to be an alphanumeric – a schedule name. In the IDF, we see the corresponding field is “ReheatCoilAvailSched�, the object name of a schedule elsewhere in the IDF file. In EnergyPlus, all references to other data entries (objects) are via object names.  The next two data items are numeric: the coil UA and the maximum water mass flow rate. The final four items are again alphanumeric – the names of the coil inlet and outlet nodes. Nodes are used in EnergyPlus to connect HVAC components together into HVAC systems.
-
-The example illustrates the use of comments to create clear input.  The IDF is intended to be human readable, largely for development and debugging purposes.  Of course, most users will never see an IDF – they will interact with EnergyPlus through a Graphical User Interface (GUI), which will write the IDF for them.  However, a module developer is a special kind of user.  The module developer will need to create a portion of an IDF by hand very early in the development process in order to begin testing the module under development.  Thus, it is important to understand the IDF syntax and to use comments to create readable test IDF files.
-
-**Summary**
-
-One of the early tasks of a module developer is to create input (most likely by hand) for the new component and to insert it into an existing IDF file in order to test the new component model.  The IDF syntax resembles the syntax for the IDD.  The data follows the IDD class description.  Comments should be used to make the IDF readable.
-
-Input Considerations
---------------------
-
-The IDD/IDF concept allows the module developer much flexibility.  Along with this flexibility comes a responsibility to the overall development of EnergyPlus. Developers must take care not to obstruct other developers with their additions or changes.  Major changes in the IDD require collaboration among the developers (both module and interface).
-
-In many cases, the developer may be creating a new model – a new HVAC component, for instance. Then the most straightforward approach is to create a new object class in the IDD with its own unique, self-contained input. This will seldom impact other developers.
-
-In some cases, the developer may be adding a calculation within an existing module or for an existing class of objects. This calculation may require new or different input fields. Then the developer has a number of choices. This section will present some ideas for adding to the IDD that will minimize impact to other developers.
-
-For example, consider the implementation of Other Side Coefficients (OSC) in the IDD.  Other side coefficients are a simplification for the surface heat balance and were used mostly in BLAST 2.0 before we had interzone surfaces.  We have carried this forward into EnergyPlus for those users that understand and can use it.  We’ll use it as an example of approaches to adding data items to the IDD.  Moreover, we’ll try to give some hints on which approaches might be used for future additions.
-
-So, you're adding something to EnergyPlus and it is part of an existing module or object class.  What do you do with your required inputs to your model?  There are at least four options:
-
-- Embed your values in a current object class definition.
-
-- Put something in the current definition that will trigger a "GetInput" for your values.
-
-- Put something in the current definition that will signal a "special" case and embed a name (of your item) in the definition (this adds 1 or 2 properties to the object).
-
-- Just get your input and have each of those inputs reference a named object.
-
-For example, using the OSC option in surfaces, in the beta 2 version of EnergyPlus we had
-
-  A8 , \\field Exterior environment
-
-       \\type alpha
-
-       \\note &lt;for Interzone Surface:Adjacent surface name&gt;
-
-       \\note For non-interzone surfaces enter:
-
-       \\note ExteriorEnvironment, Ground, or OtherSideCoeff
-
-       \\note OSC won't use CTFs
-
-
-
-  N24, \\field User selected Constant Temperature
-
-  N25, \\field Coefficient modifying the user selected constant
-
-              temperature
-
-  N26, \\field Coefficient modifying the external dry bulb temperature
-
-  N27, \\field Coefficient modifying the ground temperature
-
-  N28, \\field Combined convective/radiative film coefficient
-
-       \\note if=0, use other coefficients
-
-  N29, \\field Coefficient modifying the wind speed term (s/m)
-
-  N30, \\field Coefficient modifying the zone air temperature part of
-
-              the equation
-
-
-
-**1)  **We have done option 1: embed the values in the input.  (We have also embedded these values in each and every surface derived type (internal data structure) but that can be discussed elsewhere).
-
-When to use:  It makes sense to embed these values when each and every object (SURFACE) needs these values (e.g. we need to specify Vertices for Every Surface -- so these clearly should be embedded).
-
-After beta 2, the definition of Surfaces was changed. Obviously option 1 was not a good choice for the OSC data: the data would be rarely used. Our other options were:
-
-**2)  **Obviously the ExteriorEnvironment field will remain (but its name was changed to Outside Face Environment).
-
-However, we do not want to embed the values for OtherSideCoef in the Surface items.  So, if the ExteriorEnvironment continues to reference OtherSideCoef, we can easily trigger a "GetInput" for them.  An additional object class would be necessary for this case.
-
-OtherSideCoef,  A1, \\field name of OtherSideCoef,
-
-  A2, \\field SurfaceName (reference to surface using OSC)
-
-  ....
-
-
-
-When to use:  This option can be used for many cases.  The same object definition will work for option 4 below.  Obviously, if there is not a convenient trigger in SURFACE but you want to add a feature, this would let you do it without embedding it in the Surface Definition.  If there is a trigger, such as exists with the ExteriorEnvironment, the A2 field might not be needed.  This approach would become a bit cumbersome if you expected there to be a lot of these or if there were a one-to-many relationship (i.e. a single set of OSCs could be used for many surfaces).  Nevertheless, the approach provides a convenient "data check"/cross reference that can be validated inside the code.
-
-**3)  **We could also have the SURFACE definition reference an OSC name (in this instance).
-
-So, we'd add a field to the Surface that would be the name in the OtherSideCoef object above.  Then, the OtherSideCoef objects wouldn’t need a Surface Name. This is the most straightforward approach: including data in one object by referencing another and it was the approach chosen for the redefined Surface class.
-
-When to use:  when there is a set of parameters that would be used extensively, then this would provide a name for those.  If hand editing, then you only would need to change one set of these parameters rather than having to go through many.  Of course, the OtherSideCoef object wouldn’t also have to have the true numbers but could reference yet a third named object...... (starting to get messy).
-
-**4)  **We could have the OtherSideCoef object as above and just "get" it as a matter of course.  (e.g., in the case where we don’t have a convenient trigger such as ExteriorEnvironment).
-
-When to use:  Note that the same structure for 2 works here too.  It's just not triggered (to get the input) by a value in the other object (SURFACE).
-
-**Summary**
-
-There are several approaches to adding items to the IDD.  Developers need to consider impacts to other developers and users early in the implementation planning.
-
-Advanced Input Considerations
------------------------------
-
-Creating a new module/adding a new feature to EnergyPlus is a good accomplishment.  However, it is likely that future additions will be done and will impact any objects created.  In this regard, we ask that module developers take a longer view than “just getting my thing� going.
-
-For example, in the “Fan Coil� object, prior to the V1.2 release, the object definition specified a cooilng coil name.  *But it did not specify a cooling coil type.*  Rather than restrict coil names to be unique over all coils (which becomes difficult as more coil types are added), the developers only have unique names within a type.  Thus, it would become difficult for the Fan Coil module to get the proper link to the correct cooling coil.
-
-In the V1.2 release, a cooling coil type was added to the object.  But the resulting object is less readable now. For upwards compatibility, the coil type was placed at the end of the object whereas the coil name is in the middle.  If this had been thought of earlier, then the coil type and coil name could be in succeeding fields in the object definition.
-
-The “standard� for describing such fields would be to list the “coil type� and then the “coil name� fields, such as in the UNITARYSYSTEM:HEATPUMP:AIRTOAIR object.
-
-The point – try to envision future changes in making up objects, even if you think “that will never happen�.  You do not have to try to address every future case, only the most likely.
-
-**ZoneHVAC:FourPipeFanCoil,**
-
-        \\min-fields 21
-
-   A1 , \\field Name
-
-        \\required-field
-
-   A2 , \\field Availability Schedule Name
-
-        \\required-field
-
-        \\type object-list
-
-        \\object-list ScheduleNames
-
-   N1 , \\field Maximum Supply Air Flow Rate
-
-        \\required-field
-
-        \\autosizable
-
-        \\units m3/s
-
-   N2 , \\field Maximum Outdoor Air Flow Rate
-
-        \\required-field
-
-        \\autosizable
-
-        \\units m3/s
-
-   &lt;snip&gt;
-
-**   A11, \\field Cooling Coil Name**
-
-        \\required-field
-
-        \\type object-list
-
-        \\object-list CoolingCoilsWater
-
-   N3 , \\field Maximum Cold Water Flow Rate
-
-        \\required-field
-
-        \\autosizable
-
-        \\units m3/s
-
-        \\ip-units gal/min
-
-  &lt;snip&gt;
-
-   **A13; \\field Cooling Coil Object Type**
-
-        \\required-field
-
-        \\type choice
-
-        \\key Coil:Cooling:Water
-
-        \\key Coil:Cooling:Water:DetailedGeometry
-
-        \\key CoilSystem:Cooling:Water:HeatExchangerAssisted
-
-DataSets
---------
-
-Akin to the libraries of other programs, EnergyPlus uses data sets.  Data sets are similar to libraries but many items are contained in a single file (usually input file format or sometimes macro format).  Developers are encouraged, as appropriate, to submit data sets along with new features.  Some of the existing data sets include:
-
-- Materials properties
-
-- Construction elements (layers of materials)
-
-- Composite construction definitions (equivalent constructions for complex elements)
-
-- Solar Collector parameters
-
-- Economic Tariffs
-
-- Design Day definitions
-
-- Location definitions
-
-- Standard report definitions
-
-
-
-Module Structure
-================
-
-Let us assume that the novice EnergyPlus developer wishes to model a new HVAC component called *NewHVACComponent*.  Right at the start there is a choice to make: whether to insert the new model into an existing module or to create an entirely new EnergyPlus component simulation model.  Creating a new module is the easier option to explain, implement and test. We will discuss this option in this document.  The discussion should also impart enough information to allow a new developer to insert a model into an existing EnergyPlus module if that option is chosen.
-
-If you intend that the module will become part of the distributed EnergyPlus, follow the guidance in the Programming Standard document.  Even if you don’t intend that your module will become part of EnergyPlus – but you might want some advice from one of the core development team, follow the guidance in the Programming Standard.
-
-Module Outline
---------------
-
-The developer will create a new file NewHVACComponent.f90.  The file shall contain the following elements:
-
-Note – even if your component does not need some of the suggested modules, you should include “stub� routines for these.
-
-**MODULE**NewHVACComponent
-
-*Documentation:* Fortran comments describing and documenting the module. Included are sections showing module author, module creation date, date modified and modification author.  Each routine and/or function should also follow the documentation guidelines as shown in the templates.
-
-*USE Statements:* Fortran statements naming other modules that this module can access, either for data or for routines.
-
-*Module Parameters:* If you will be implementing more than one “type� of component in the module, it is a good idea to assign numeric parameters to each type so as to retain readability yet reduce alpha comparisons which are notoriously slow for most systems.  Assign numeric parameters to alphanumeric fields within a class type (.e.g. object UnitarySystem:HeatPump, field Fan Placement: “blow through� or “draw through�) when this information is required in init, calc, update or report subroutines to further reduce alpha comparisons.  Use string comparison only in GetInput subroutines.
-
-*Module Data structure Definitions:* Using the Fortran TYPE statement define the data structures needed in the module that will not be available from other modules. Define all module level variables that will be needed.
-
-Typically, you define your module’s data structure within the module.  If this data must be used by multiple modules, you should define a separate Data module for the data.
-
-Character strings in structures are not allowed (except for name of object) – any exceptions must be approved. Schedule names, curve object names, and child object types MUST all be referenced by an integer.
-
-For existing code, convert all character string structure variables to integer parameters and delete the character variable from the structure. Also delete unused strings rather than converting to integer. Do not use structure variable to store information used only during GetInput even if you think it could be used in the future, use local variables instead. Usually won't hurt anything until some user puts a large number of objects in their input (memory use impact).
-
-Currently, the furnace structure includes many that should not be there. SuppHeatCoilType is an example of a character string structure variable that is only used in GetInput and is not needed in the structure. Should have been a local instead. And CoolingPLFFPLR and HeatingPLFFPLR structure variables are not even used.
-
-***CONTAINS***
-
-***SUBROUTINE*** *SimNewHVACComponent*
-
-This routine selects the individual component being simulated and calls the other module subroutines that do the real work. This routine is the only routine in the module that is accessible outside the module (*PUBLIC*). All other routines in the module are *PRIVATE* and are only callable within the module. This routine is sometimes called the “driver� routine for the module.
-
-***END SUBROUTINE*** *SimNewHVACComponent*
-
-***SUBROUTINE*** *GetNewHVACComponentInput*
-
-This routine uses the “get� routines from the InputProcessor module to obtain input for NewHVACComponent. The module data arrays are allocated and the data is moved into the arrays.
-
-***END SUBROUTINE*** *GetNewHVACComponentInput*
-
-***SUBROUTINE*** *InitNewHVACComponent*
-
-This routine performs whatever initialization calculations that may be needed at various points in the simulation. For instance, some calculations may only need to be done once; some may need to be done at the start of each simulation weather period; some at the start of each HVAC simulation time step; and some at the start of each loop solution. This routine also transfers data from the component inlet nodes to the component data arrays every time the component is simulated, in preparation for the actual component simulation.
-
-***END SUBROUTINE*** *InitNewHVACComponent*
-
-***SUBROUTINE*** *SizeNewHVACComponent*
-
-This routine can create the sizing options (if applicable) for the component or be left as a placeholder for later manipulation for sizing purposes.
-
-***END SUBROUTINE*** *SizeNewHVACComponent*
-
-***SUBROUTINE*** *CalcNewHVACComponent*
-
-This routine does the actual calculations to simulate the performance of the component. Only calculation is done – there is no moving of data from or to input or output areas. There may be more than one “*CALC*� subroutine if more than one component is being modeled within this module.
-
-***END SUBROUTINE*** *CalcNewHVACComponent*
-
-***SUBROUTINE*** *UpdateNewHVACComponent*
-
-This routine moves the results of the “*Calc*� routine(s) to the component outlet nodes.
-
-***END SUBROUTINE*** *UpdateNewHVACComponent*
-
-***SUBROUTINE*** *ReportNewHVACComponent*
-
-This routine performs any special calculations that are needed purely for reporting purposes.
-
-***END SUBROUTINE*** *ReportNewHVACComponent*
-
-***Utility Routines (as appropriate) – in the Fan module we allow outside modules to access internal fan inlets, outlets, and design volume flow rate.***
-
-***END MODULE*** *NewHVACComponent*
-
-Module Example
---------------
-
-This example can be used as a template for new HVAC component modules. In particular, the commenting structure in the module and within the subroutines should be followed closely. Of course, there is no perfect example module – this one is particularly simple. Some others that might be examined are in files Humidifiers.f90, HVACHeatingCoils.f90 and PlantChillers.f90. Templates are also available as separate files.
-
-In particular, the module template with routines contains structure and information pertinent to module development.
-
-Note that in the following module, the “Data IPShortcuts� is not used – rather those variables are allocated within this module – likely because another module calls this one during input.
-
-**Module Fans**
-
-  ! Module containing the fan simulation routines
-
-
-
-  ! MODULE INFORMATION:
-
-  !       AUTHOR         Richard J. Liesen
-
-  !       DATE WRITTEN   April 1998
-
-  !       MODIFIED       Shirey, May 2001
-
-  !       RE-ENGINEERED  na
-
-
-
-  ! PURPOSE OF THIS MODULE:
-
-  ! To encapsulate the data and algorithms required to
-
-  ! manage the Fan System Component
-
-
-
-  ! REFERENCES: none
-
-
-
-  ! OTHER NOTES: none
-
-
-
-  ! USE STATEMENTS:
-
-  ! Use statements for data only modules
-
-USE DataPrecisionGlobals
-
-USE DataLoopNode
-
-USE DataHVACGlobals, ONLY: TurnFansOn, TurnFansOff, Main, Cooling, Heating, Other, &
-
-          OnOffFanPartLoadFraction, SmallAirVolFlow, UnbalExhMassFlow, NightVentOn, cFanTypes, &
-
-          FanType\_SimpleConstVolume, FanType\_SimpleVAV, FanType\_SimpleOnOff, FanType\_ZoneExhaust
-
-USE DataGlobals,     ONLY: SetupOutputVariable, BeginEnvrnFlag, BeginDayFlag, MaxNameLength, &
-
-       ShowWarningError, ShowFatalError, ShowSevereError, HourofDay, SysSizingCalc, CurrentTime, &
-
-       OutputFileDebug, ShowContinueError, ShowRecurringWarningErrorAtEnd, WarmupFlag, &
-
-                           ShowContinueErrorTimeStamp
-
-Use DataEnvironment, ONLY: StdBaroPress, DayofMonth, Month, StdRhoAir
-
-USE Psychrometrics,  ONLY:PsyRhoAirFnPbTdbW, PsyTdbFnHW, PsyCpAirFnWTdb
-
-
-
-  ! Use statements for access to subroutines in other modules
-
-USE ScheduleManager
-
-
-
-IMPLICIT NONE         ! Enforce explicit typing of all variables
-
-
-
-PRIVATE ! Everything private unless explicitly made public
-
-
-
-
-
-  !MODULE PARAMETER DEFINITIONS
-
-  !na
-
-
-
-  ! DERIVED TYPE DEFINITIONS
-
-TYPE FanEquipConditions
-
-  CHARACTER(len=MaxNameLength) :: FanName  =' '  ! Name of the fan
-
-  CHARACTER(len=MaxNameLength) :: FanType  =' '  ! Type of Fan ie. Simple, Vane axial, Centrifugal, etc.
-
-  CHARACTER(len=MaxNameLength) :: Schedule =' '  ! Fan Operation Schedule
-
-  INTEGER      :: FanType\_Num              =0    ! DataHVACGlobals fan type
-
-  Integer      :: SchedPtr                 =0    ! Pointer to the correct schedule
-
-  REAL(r64)    :: InletAirMassFlowRate     =0.0  !MassFlow through the Fan being Simulated [kg/Sec]
-
-  REAL(r64)    :: OutletAirMassFlowRate    =0.0
-
-  REAL(r64)    :: MaxAirFlowRate           =0.0  !Max Specified Volume Flow Rate of Fan [m3/sec]
-
-  REAL(r64)    :: MinAirFlowRate           =0.0  !Min Specified Volume Flow Rate of Fan [m3/sec]
-
-  REAL(r64)    :: MaxAirMassFlowRate       =0.0  ! Max flow rate of fan in kg/sec
-
-  REAL(r64)    :: MinAirMassFlowRate       =0.0  ! Min flow rate of fan in kg/sec
-
-  REAL(r64)    :: InletAirTemp             =0.0
-
-  REAL(r64)    :: OutletAirTemp            =0.0
-
-  REAL(r64)    :: InletAirHumRat           =0.0
-
-  REAL(r64)    :: OutletAirHumRat          =0.0
-
-  REAL(r64)    :: InletAirEnthalpy         =0.0
-
-  REAL(r64)    :: OutletAirEnthalpy        =0.0
-
-  REAL(r64)    :: FanPower                 =0.0  !Power of the Fan being Simulated [kW]
-
-  REAL(r64)    :: FanEnergy                =0.0  !Fan energy in [kJ]
-
-  REAL(r64)    :: FanRuntimeFraction       =0.0  !Fraction of the timestep that the fan operates
-
-  REAL(r64)    :: DeltaTemp                =0.0  !Temp Rise across the Fan [C]
-
-  REAL(r64)    :: DeltaPress               =0.0  !Delta Pressure Across the Fan [N/m2]
-
-  REAL(r64)    :: FanEff                   =0.0  !Fan total efficiency; motor and mechanical
-
-  REAL(r64)    :: MotEff                   =0.0  !Fan motor efficiency
-
-  REAL(r64)    :: MotInAirFrac             =0.0  !Fraction of motor heat entering air stream
-
-  REAL(r64), Dimension(5):: FanCoeff            =0.0  !Fan Part Load Coefficients to match fan type
-
-  ! Mass Flow Rate Control Variables
-
-  REAL(r64)    :: MassFlowRateMaxAvail     =0.0
-
-  REAL(r64)    :: MassFlowRateMinAvail     =0.0
-
-  REAL(r64)    :: RhoAirStdInit            =0.0
-
-  INTEGER      :: InletNodeNum             =0
-
-  INTEGER      :: OutletNodeNum            =0
-
-  INTEGER      :: NVPerfNum                =0
-
-  INTEGER      :: FanPowerRatAtSpeedRatCurveIndex  =0
-
-  INTEGER      :: FanEffRatioCurveIndex    =0
-
-  CHARACTER(len=MaxNameLength) :: EndUseSubcategoryName=' '
-
-  LOGICAL      :: OneTimePowerRatioCheck = .TRUE. ! one time flag used for error message
-
-  LOGICAL      :: OneTimeEffRatioCheck = .TRUE.   ! one time flag used for error message
-
-END TYPE FanEquipConditions
-
-
-
-TYPE NightVentPerfData
-
-  CHARACTER(len=MaxNameLength) :: FanName  =' ' ! Name of the fan that will use this data
-
-  REAL(r64)    :: FanEff                   =0.0 !Fan total efficiency; motor and mechanical
-
-  REAL(r64)    :: DeltaPress               =0.0 !Delta Pressure Across the Fan [N/m2]
-
-  REAL(r64)    :: MaxAirFlowRate           =0.0 !Max Specified Volume Flow Rate of Fan [m3/s]
-
-  REAL(r64)    :: MaxAirMassFlowRate       =0.0 ! Max flow rate of fan in kg/sec
-
-  REAL(r64)    :: MotEff                   =0.0 !Fan motor efficiency
-
-  REAL(r64)    :: MotInAirFrac             =0.0 !Fraction of motor heat entering air stream
-
-END TYPE NightVentPerfData
-
-
-
-
-
-
-
-  !MODULE VARIABLE DECLARATIONS:
-
-  INTEGER :: NumFans     =0 ! The Number of Fans found in the Input
-
-  INTEGER :: NumNightVentPerf =0 ! number of FAN:NIGHT VENT PERFORMANCE objects found in the input
-
-  TYPE (FanEquipConditions), ALLOCATABLE, DIMENSION(:) :: Fan
-
-  TYPE (NightVentPerfData), ALLOCATABLE, DIMENSION(:)  :: NightVentPerf
-
-  LOGICAL :: GetFanInputFlag = .True.  ! Flag set to make sure you get input once
-
-
-
-! Subroutine Specifications for the Module
-
-          ! Driver/Manager Routines
-
-**Public  SimulateFanComponents**
-
-
-
-          ! Get Input routines for module
-
-PRIVATE GetFanInput
-
-
-
-          ! Initialization routines for module
-
-PRIVATE InitFan
-
-PRIVATE SizeFan
-
-
-
-          ! Algorithms for the module
-
-Private SimSimpleFan
-
-PRIVATE SimVariableVolumeFan
-
-PRIVATE SimZoneExhaustFan
-
-
-
-
-
-          ! Update routine to check convergence and update nodes
-
-Private UpdateFan
-
-
-
-          ! Reporting routines for module
-
-Private ReportFan
-
-
-
-
-
-CONTAINS
-
-
-
-! MODULE SUBROUTINES:
-
-!\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-**SUBROUTINE SimulateFanComponents(CompName,FirstHVACIteration)**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         Richard Liesen
-
-          !       DATE WRITTEN   February 1998
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! This subroutine manages Fan component simulation.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! na
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-  USE InputProcessor, ONLY: FindItemInList
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-  CHARACTER(len=\*), INTENT(IN) :: CompName
-
-  LOGICAL,      INTENT (IN):: FirstHVACIteration
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-  INTEGER             :: FanNum     ! current fan number
-
-  LOGICAL,SAVE        :: GetInputFlag = .True.  ! Flag set to make sure you get input once
-
-
-
-          ! FLOW:
-
-
-
-  ! Obtains and Allocates fan related parameters from input file
-
-  IF (GetInputFlag) THEN  !First time subroutine has been entered
-
-    CALL GetFanInput
-
-    GetInputFlag=.false.
-
-  End If
-
-
-
-  ! Find the correct FanNumber with the AirLoop & CompNum from AirLoop Derived Type
-
-  !FanNum = AirLoopEquip(AirLoopNum)%ComponentOfTypeNum(CompNum)
-
-  ! Determine which Fan given the Fan Name
-
-  FanNum =   FindItemInList(CompName,Fan%FanName,NumFans)
-
-  IF (FanNum == 0) THEN
-
-    CALL ShowFatalError('Fan not found='//TRIM(CompName))
-
-  ENDIF
-
-
-
-  ! With the correct FanNum Initialize
-
-  CALL InitFan(FanNum,FirstHVACIteration)  ! Initialize all fan related parameters
-
-
-
-  ! Calculate the Correct Fan Model with the current FanNum
-
-  IF (Fan(FanNum)%FanType\_Num == FanType\_SimpleConstVolume) THEN
-
-    Call SimSimpleFan(FanNum)
-
-  Else IF (Fan(FanNum)%FanType\_Num == FanType\_SimpleVAV) THEN
-
-    Call SimVariableVolumeFan(FanNum)
-
-  Else If (Fan(FanNum)%FanType\_Num == FanType\_SimpleOnOff) THEN
-
-    Call SimOnOffFan(FanNum)
-
-  Else If (Fan(FanNum)%FanType\_Num == FanType\_ZoneExhaust) THEN
-
-    Call SimZoneExhaustFan(FanNum)
-
-  End If
-
-  ! Update the current fan to the outlet nodes
-
-  Call UpdateFan(FanNum)
-
-
-
-  ! Report the current fan
-
-  Call ReportFan(FanNum)
-
-
-
-  RETURN
-
-
-
-**END SUBROUTINE SimulateFanComponents**
-
-
-
-
-
-! Get Input Section of the Module
-
-!\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-**SUBROUTINE GetFanInput**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         Richard Liesen
-
-          !       DATE WRITTEN   April 1998
-
-          !       MODIFIED       Shirey, May 2001
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! Obtains input data for fans and stores it in fan data structures
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! Uses "Get" routines to read in data.
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-    USE InputProcessor
-
-    USE NodeInputManager,      ONLY: GetOnlySingleNode
-
-    USE CurveManager,          ONLY: GetCurveIndex
-
-    USE BranchNodeConnections, ONLY: TestCompSet
-
-!    USE DataIPShortCuts
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-    INTEGER :: FanNum      ! The fan that you are currently loading input into
-
-    INTEGER :: NumSimpFan  ! The number of Simple Const Vol Fans
-
-    INTEGER :: NumVarVolFan ! The number of Simple Variable Vol Fans
-
-    INTEGER :: NumOnOff     ! The number of Simple on-off Fans
-
-    INTEGER :: NumZoneExhFan
-
-    INTEGER :: SimpFanNum
-
-    INTEGER :: OnOffFanNum
-
-    INTEGER :: VarVolFanNum
-
-    INTEGER :: ExhFanNum
-
-    INTEGER :: NVPerfNum
-
-    LOGICAL :: NVPerfFanFound
-
-    INTEGER :: NumAlphas
-
-    INTEGER :: NumNums
-
-    INTEGER :: IOSTAT
-
-    LOGICAL :: ErrorsFound = .false.   ! If errors detected in input
-
-    LOGICAL :: IsNotOK               ! Flag to verify name
-
-    LOGICAL :: IsBlank               ! Flag for blank name
-
-    CHARACTER(len=\*), PARAMETER    :: RoutineName='GetFanInput: ' ! include trailing blank space
-
-    CHARACTER(len=MaxNameLength+40),ALLOCATABLE, DIMENSION(:) :: cAlphaFieldNames
-
-    CHARACTER(len=MaxNameLength+40),ALLOCATABLE, DIMENSION(:) :: cNumericFieldNames
-
-    LOGICAL, ALLOCATABLE, DIMENSION(:) :: lNumericFieldBlanks
-
-    LOGICAL, ALLOCATABLE, DIMENSION(:) :: lAlphaFieldBlanks
-
-    CHARACTER(len=MaxNameLength),ALLOCATABLE, DIMENSION(:) :: cAlphaArgs
-
-    REAL(r64),ALLOCATABLE, DIMENSION(:) :: rNumericArgs
-
-    CHARACTER(len=MaxNameLength) :: cCurrentModuleObject
-
-    INTEGER :: NumParams
-
-    INTEGER :: MaxAlphas
-
-    INTEGER :: MaxNumbers
-
-
-
-          ! Flow
-
-    MaxAlphas=0
-
-    MaxNumbers=0
-
-    NumSimpFan   = GetNumObjectsFound('Fan:ConstantVolume')
-
-    IF (NumSimpFan &gt; 0) THEN
-
-      CALL GetObjectDefMaxArgs('Fan:ConstantVolume',NumParams,NumAlphas,NumNums)
-
-      MaxAlphas=MAX(MaxAlphas,NumAlphas)
-
-      MaxNumbers=MAX(MaxNumbers,NumNums)
-
-    ENDIF
-
-    NumVarVolFan = GetNumObjectsFound('Fan:VariableVolume')
-
-    IF (NumVarVolFan &gt; 0) THEN
-
-      CALL GetObjectDefMaxArgs('Fan:VariableVolume',NumParams,NumAlphas,NumNums)
-
-      MaxAlphas=MAX(MaxAlphas,NumAlphas)
-
-      MaxNumbers=MAX(MaxNumbers,NumNums)
-
-    ENDIF
-
-    NumOnOff = GetNumObjectsFound('Fan:OnOff')
-
-    IF (NumOnOff &gt; 0) THEN
-
-      CALL GetObjectDefMaxArgs('Fan:OnOff',NumParams,NumAlphas,NumNums)
-
-      MaxAlphas=MAX(MaxAlphas,NumAlphas)
-
-      MaxNumbers=MAX(MaxNumbers,NumNums)
-
-    ENDIF
-
-    NumZoneExhFan = GetNumObjectsFound('Fan:ZoneExhaust')
-
-    IF (NumZoneExhFan &gt; 0) THEN
-
-      CALL GetObjectDefMaxArgs('Fan:ZoneExhaust',NumParams,NumAlphas,NumNums)
-
-      MaxAlphas=MAX(MaxAlphas,NumAlphas)
-
-      MaxNumbers=MAX(MaxNumbers,NumNums)
-
-    ENDIF
-
-    NumNightVentPerf = GetNumObjectsFound('FanPerformance:NightVentilation')
-
-    IF (NumNightVentPerf &gt; 0) THEN
-
-      CALL GetObjectDefMaxArgs('FanPerformance:NightVentilation',NumParams,NumAlphas,NumNums)
-
-      MaxAlphas=MAX(MaxAlphas,NumAlphas)
-
-      MaxNumbers=MAX(MaxNumbers,NumNums)
-
-    ENDIF
-
-    ALLOCATE(cAlphaArgs(MaxAlphas))
-
-    cAlphaArgs=' '
-
-    ALLOCATE(cAlphaFieldNames(MaxAlphas))
-
-    cAlphaFieldNames=' '
-
-    ALLOCATE(lAlphaFieldBlanks(MaxAlphas))
-
-    lAlphaFieldBlanks=.false.
-
-    ALLOCATE(cNumericFieldNames(MaxNumbers))
-
-    cNumericFieldNames=' '
-
-    ALLOCATE(lNumericFieldBlanks(MaxNumbers))
-
-    lNumericFieldBlanks=.false.
-
-    ALLOCATE(rNumericArgs(MaxNumbers))
-
-    rNumericArgs=0.0
-
-
-
-    NumFans = NumSimpFan + NumVarVolFan + NumZoneExhFan+NumOnOff
-
-    IF (NumFans &gt; 0) THEN
-
-      ALLOCATE(Fan(NumFans))
-
-    ENDIF
-
-
-
-      DO SimpFanNum = 1,  NumSimpFan
-
-        FanNum = SimpFanNum
-
-        cCurrentModuleObject= 'Fan:ConstantVolume'
-
-        CALL GetObjectItem(TRIM(cCurrentModuleObject),SimpFanNum,cAlphaArgs,NumAlphas, &
-
-                           rNumericArgs,NumNums,IOSTAT, &
-
-                           NumBlank=lNumericFieldBlanks,AlphaBlank=lAlphaFieldBlanks, &
-
-                           AlphaFieldNames=cAlphaFieldNames,NumericFieldNames=cNumericFieldNames)
-
-        IsNotOK=.false.
-
-        IsBlank=.false.
-
-        CALL VerifyName(cAlphaArgs(1),Fan%FanName,FanNum-1,IsNotOK,IsBlank,TRIM(cCurrentModuleObject)//' Name')
-
-        IF (IsNotOK) THEN
-
-          ErrorsFound=.true.
-
-          IF (IsBlank) cAlphaArgs(1)='xxxxx'
-
-        ENDIF
-
-        Fan(FanNum)%FanName  = cAlphaArgs(1)
-
-        Fan(FanNum)%FanType =  cCurrentModuleObject
-
-        Fan(FanNum)%Schedule = cAlphaArgs(2)
-
-        Fan(FanNum)%SchedPtr = GetScheduleIndex(cAlphaArgs(2))
-
-        IF (Fan(FanNum)%SchedPtr == 0) THEN
-
-          IF (lAlphaFieldBlanks(2)) THEN
-
-            CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//': '//TRIM(cAlphaFieldNames(2))//  &
-
-                 ' is required, missing for '//TRIM(cAlphaFieldNames(1))//'='//TRIM(cAlphaArgs(1)))
-
-          ELSE
-
-            CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//': invalid '//TRIM(cAlphaFieldNames(2))//  &
-
-               ' entered ='//TRIM(cAlphaArgs(2))// &
-
-               ' for '//TRIM(cAlphaFieldNames(1))//'='//TRIM(cAlphaArgs(1)))
-
-          END IF
-
-          ErrorsFound=.true.
-
-        END IF
-
-!        Fan(FanNum)%Control = 'CONSTVOLUME'
-
-        Fan(FanNum)%FanType\_Num=FanType\_SimpleConstVolume
-
-
-
-        Fan(FanNum)%FanEff        = rNumericArgs(1)
-
-        Fan(FanNum)%DeltaPress    = rNumericArgs(2)
-
-        Fan(FanNum)%MaxAirFlowRate= rNumericArgs(3)
-
-        IF (Fan(FanNum)%MaxAirFlowRate == 0.0) THEN
-
-          CALL ShowWarningError(TRIM(cCurrentModuleObject)//'="'//TRIM(Fan(FanNum)%FanName)//  &
-
-             '" has specified 0.0 max air flow rate. It will not be used in the simulation.')
-
-        ENDIF
-
-        Fan(FanNum)%MotEff        = rNumericArgs(4)
-
-        Fan(FanNum)%MotInAirFrac  = rNumericArgs(5)
-
-        Fan(FanNum)%MinAirFlowRate= 0.0
-
-
-
-        Fan(FanNum)%InletNodeNum  = &
-
-               GetOnlySingleNode(cAlphaArgs(3),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),  &
-
-                            NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsNotParent)
-
-        Fan(FanNum)%OutletNodeNum = &
-
-               GetOnlySingleNode(cAlphaArgs(4),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),  &
-
-                            NodeType\_Air,NodeConnectionType\_Outlet,1,ObjectIsNotParent)
-
-
-
-        IF (NumAlphas &gt; 4) THEN
-
-          Fan(FanNum)%EndUseSubcategoryName = cAlphaArgs(5)
-
-        ELSE
-
-          Fan(FanNum)%EndUseSubcategoryName = 'General'
-
-        END IF
-
-
-
-        CALL TestCompSet(TRIM(cCurrentModuleObject),cAlphaArgs(1),cAlphaArgs(3),cAlphaArgs(4),'Air Nodes')
-
-
-
-
-
-      END DO   ! end Number of Simple FAN Loop
-
-
-
-
-
-      DO VarVolFanNum = 1,  NumVarVolFan
-
-        FanNum = NumSimpFan + VarVolFanNum
-
-        cCurrentModuleObject= 'Fan:VariableVolume'
-
-        CALL GetObjectItem(TRIM(cCurrentModuleObject),VarVolFanNum,cAlphaArgs,NumAlphas, &
-
-                           rNumericArgs,NumNums,IOSTAT, &
-
-                           NumBlank=lNumericFieldBlanks,AlphaBlank=lAlphaFieldBlanks, &
-
-                           AlphaFieldNames=cAlphaFieldNames,NumericFieldNames=cNumericFieldNames)
-
-        IsNotOK=.false.
-
-        IsBlank=.false.
-
-        CALL VerifyName(cAlphaArgs(1),Fan%FanName,FanNum-1,IsNotOK,IsBlank,TRIM(cCurrentModuleObject)//' Name')
-
-        IF (IsNotOK) THEN
-
-          ErrorsFound=.true.
-
-          IF (IsBlank) cAlphaArgs(1)='xxxxx'
-
-        ENDIF
-
-        Fan(FanNum)%FanName = cAlphaArgs(1)
-
-        Fan(FanNum)%FanType = cCurrentModuleObject
-
-        Fan(FanNum)%Schedule = cAlphaArgs(2)
-
-        Fan(FanNum)%SchedPtr =GetScheduleIndex(cAlphaArgs(2))
-
-        IF (Fan(FanNum)%SchedPtr == 0) THEN
-
-          IF (lAlphaFieldBlanks(2)) THEN
-
-            CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//': '//TRIM(cAlphaFieldNames(2))//  &
-
-                 ' is required, missing for '//TRIM(cAlphaFieldNames(1))//'='//TRIM(cAlphaArgs(1)))
-
-          ELSE
-
-            CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//': invalid '//TRIM(cAlphaFieldNames(2))//  &
-
-               ' entered ='//TRIM(cAlphaArgs(2))// &
-
-               ' for '//TRIM(cAlphaFieldNames(1))//'='//TRIM(cAlphaArgs(1)))
-
-          END IF
-
-          ErrorsFound=.true.
-
-        ENDIF
-
-!        Fan(FanNum)%Control = 'VARIABLEVOLUME'
-
-        Fan(FanNum)%FanType\_Num=FanType\_SimpleVAV
-
-
-
-        Fan(FanNum)%FanEff        = rNumericArgs(1)
-
-        Fan(FanNum)%DeltaPress    = rNumericArgs(2)
-
-        Fan(FanNum)%MaxAirFlowRate= rNumericArgs(3)
-
-        IF (Fan(FanNum)%MaxAirFlowRate == 0.0) THEN
-
-          CALL ShowWarningError(TRIM(cCurrentModuleObject)//'="'//TRIM(Fan(FanNum)%FanName)//  &
-
-             '" has specified 0.0 max air flow rate. It will not be used in the simulation.')
-
-        ENDIF
-
-        Fan(FanNum)%MinAirFlowRate= rNumericArgs(4)
-
-        Fan(FanNum)%MotEff        = rNumericArgs(5)
-
-        Fan(FanNum)%MotInAirFrac  = rNumericArgs(6)
-
-        Fan(FanNum)%FanCoeff(1)   = rNumericArgs(7)
-
-        Fan(FanNum)%FanCoeff(2)   = rNumericArgs(8)
-
-        Fan(FanNum)%FanCoeff(3)   = rNumericArgs(9)
-
-        Fan(FanNum)%FanCoeff(4)   = rNumericArgs(10)
-
-        Fan(FanNum)%FanCoeff(5)   = rNumericArgs(11)
-
-        IF (Fan(FanNum)%FanCoeff(1) == 0.0 .and. Fan(FanNum)%FanCoeff(2) == 0.0 .and.  &
-
-            Fan(FanNum)%FanCoeff(3) == 0.0 .and. Fan(FanNum)%FanCoeff(4) == 0.0 .and.  &
-
-            Fan(FanNum)%FanCoeff(5) == 0.0)  THEN
-
-            CALL ShowWarningError('Fan Coefficients are all zero.  No Fan power will be reported.')
-
-            CALL ShowContinueError('For '//TRIM(cCurrentModuleObject)//', Fan='//TRIM(cAlphaArgs(1)))
-
-        ENDIF
-
-        Fan(FanNum)%InletNodeNum  = &
-
-               GetOnlySingleNode(cAlphaArgs(3),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),  &
-
-                            NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsNotParent)
-
-        Fan(FanNum)%OutletNodeNum = &
-
-               GetOnlySingleNode(cAlphaArgs(4),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),  &
-
-                            NodeType\_Air,NodeConnectionType\_Outlet,1,ObjectIsNotParent)
-
-
-
-        IF (NumAlphas &gt; 4) THEN
-
-          Fan(FanNum)%EndUseSubcategoryName = cAlphaArgs(5)
-
-        ELSE
-
-          Fan(FanNum)%EndUseSubcategoryName = 'General'
-
-        END IF
-
-
-
-        CALL TestCompSet(TRIM(cCurrentModuleObject),cAlphaArgs(1),cAlphaArgs(3),cAlphaArgs(4),'Air Nodes')
-
-
-
-      END DO   ! end Number of Variable Volume FAN Loop
-
-
-
-      DO ExhFanNum = 1,  NumZoneExhFan
-
-        FanNum = NumSimpFan + NumVarVolFan + ExhFanNum
-
-        cCurrentModuleObject= 'Fan:ZoneExhaust'
-
-        CALL GetObjectItem(TRIM(cCurrentModuleObject),ExhFanNum,cAlphaArgs,NumAlphas, &
-
-                           rNumericArgs,NumNums,IOSTAT, &
-
-                           NumBlank=lNumericFieldBlanks,AlphaBlank=lAlphaFieldBlanks, &
-
-                           AlphaFieldNames=cAlphaFieldNames,NumericFieldNames=cNumericFieldNames)
-
-        IsNotOK=.false.
-
-        IsBlank=.false.
-
-        CALL VerifyName(cAlphaArgs(1),Fan%FanName,FanNum-1,IsNotOK,IsBlank,TRIM(cCurrentModuleObject)//' Name')
-
-        IF (IsNotOK) THEN
-
-          ErrorsFound=.true.
-
-          IF (IsBlank) cAlphaArgs(1)='xxxxx'
-
-        ENDIF
-
-        Fan(FanNum)%FanName = cAlphaArgs(1)
-
-        Fan(FanNum)%FanType = cCurrentModuleObject
-
-        Fan(FanNum)%Schedule = cAlphaArgs(2)
-
-        Fan(FanNum)%SchedPtr =GetScheduleIndex(cAlphaArgs(2))
-
-        IF (Fan(FanNum)%SchedPtr == 0) THEN
-
-          IF (lAlphaFieldBlanks(2)) THEN
-
-            CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//': '//TRIM(cAlphaFieldNames(2))//  &
-
-                 ' is required, missing for '//TRIM(cAlphaFieldNames(1))//'='//TRIM(cAlphaArgs(1)))
-
-          ELSE
-
-            CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//': invalid '//TRIM(cAlphaFieldNames(2))//  &
-
-               ' entered ='//TRIM(cAlphaArgs(2))// &
-
-               ' for '//TRIM(cAlphaFieldNames(1))//'='//TRIM(cAlphaArgs(1)))
-
-          END IF
-
-          ErrorsFound=.true.
-
-        ELSE
-
-          IF (HasFractionalScheduleValue(Fan(FanNum)%SchedPtr)) THEN
-
-            CALL ShowWarningError(TRIM(cCurrentModuleObject)//'="'//TRIM(Fan(FanNum)%FanName)//  &
-
-              '" has fractional values in Schedule='//TRIM(cAlphaArgs(2))//'. Only 0.0 in the schedule value turns the fan off.')
-
-          ENDIF
-
-        ENDIF
-
-!        Fan(FanNum)%Control = 'CONSTVOLUME'
-
-        Fan(FanNum)%FanType\_Num=FanType\_ZoneExhaust
-
-
-
-        Fan(FanNum)%FanEff        = rNumericArgs(1)
-
-        Fan(FanNum)%DeltaPress    = rNumericArgs(2)
-
-        Fan(FanNum)%MaxAirFlowRate= rNumericArgs(3)
-
-        Fan(FanNum)%MotEff        = 1.0
-
-        Fan(FanNum)%MotInAirFrac  = 1.0
-
-        Fan(FanNum)%MinAirFlowRate= 0.0
-
-        Fan(FanNum)%RhoAirStdInit = StdRhoAir
-
-        Fan(FanNum)%MaxAirMassFlowRate = Fan(FanNum)%MaxAirFlowRate \* Fan(FanNum)%RhoAirStdInit
-
-
-
-        IF (Fan(FanNum)%MaxAirFlowRate == 0.0) THEN
-
-          CALL ShowWarningError(TRIM(cCurrentModuleObject)//'="'//TRIM(Fan(FanNum)%FanName)//  &
-
-              '" has specified 0.0 max air flow rate. It will not be used in the simulation.')
-
-        ENDIF
-
-
-
-        Fan(FanNum)%InletNodeNum  = &
-
-               GetOnlySingleNode(cAlphaArgs(3),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),  &
-
-                            NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsNotParent)
-
-        Fan(FanNum)%OutletNodeNum = &
-
-               GetOnlySingleNode(cAlphaArgs(4),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1),  &
-
-                            NodeType\_Air,NodeConnectionType\_Outlet,1,ObjectIsNotParent)
-
-
-
-        IF (NumAlphas &gt; 4) THEN
-
-          Fan(FanNum)%EndUseSubcategoryName = cAlphaArgs(5)
-
-        ELSE
-
-          Fan(FanNum)%EndUseSubcategoryName = 'General'
-
-        END IF
-
-
-
-        ! Component sets not setup yet for zone equipment
-
-        ! CALL TestCompSet(TRIM(cCurrentModuleObject),cAlphaArgs(1),cAlphaArgs(3),cAlphaArgs(4),'Air Nodes')
-
-
-
-      END DO   ! end of Zone Exhaust Fan loop
-
-
-
-      DO OnOffFanNum = 1,  NumOnOff
-
-        FanNum = NumSimpFan + NumVarVolFan + NumZoneExhFan + OnOffFanNum
-
-        cCurrentModuleObject= 'Fan:OnOff'
-
-        CALL GetObjectItem(TRIM(cCurrentModuleObject),OnOffFanNum,cAlphaArgs,NumAlphas, &
-
-                           rNumericArgs,NumNums,IOSTAT, &
-
-                           NumBlank=lNumericFieldBlanks,AlphaBlank=lAlphaFieldBlanks, &
-
-                           AlphaFieldNames=cAlphaFieldNames,NumericFieldNames=cNumericFieldNames)
-
-        IsNotOK=.false.
-
-        IsBlank=.false.
-
-        CALL VerifyName(cAlphaArgs(1),Fan%FanName,FanNum-1,IsNotOK,IsBlank,TRIM(cCurrentModuleObject)//' Name')
-
-        IF (IsNotOK) THEN
-
-          ErrorsFound=.true.
-
-          IF (IsBlank) cAlphaArgs(1)='xxxxx'
-
-        ENDIF
-
-        Fan(FanNum)%FanName  = cAlphaArgs(1)
-
-        Fan(FanNum)%FanType  = cCurrentModuleObject
-
-        Fan(FanNum)%Schedule = cAlphaArgs(2)
-
-        Fan(FanNum)%SchedPtr = GetScheduleIndex(cAlphaArgs(2))
-
-        IF (Fan(FanNum)%SchedPtr == 0) THEN
-
-          IF (lAlphaFieldBlanks(2)) THEN
-
-            CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//': '//TRIM(cAlphaFieldNames(2))//  &
-
-                 ' is required, missing for '//TRIM(cAlphaFieldNames(1))//'='//TRIM(cAlphaArgs(1)))
-
-          ELSE
-
-            CALL ShowSevereError(RoutineName//TRIM(cCurrentModuleObject)//': invalid '//TRIM(cAlphaFieldNames(2))//  &
-
-               ' entered ='//TRIM(cAlphaArgs(2))// &
-
-               ' for '//TRIM(cAlphaFieldNames(1))//'='//TRIM(cAlphaArgs(1)))
-
-          END IF
-
-          ErrorsFound=.true.
-
-        ENDIF
-
-!        Fan(FanNum)%Control = 'ONOFF'
-
-        Fan(FanNum)%FanType\_Num=FanType\_SimpleOnOff
-
-
-
-        Fan(FanNum)%FanEff        = rNumericArgs(1)
-
-        Fan(FanNum)%DeltaPress    = rNumericArgs(2)
-
-        Fan(FanNum)%MaxAirFlowRate= rNumericArgs(3)
-
-        IF (Fan(FanNum)%MaxAirFlowRate == 0.0) THEN
-
-          CALL ShowWarningError(TRIM(cCurrentModuleObject)//'="'//TRIM(Fan(FanNum)%FanName)//  &
-
-              '" has specified 0.0 max air flow rate. It will not be used in the simulation.')
-
-        ENDIF
-
-
-
-!       the following two structure variables are set here, as well as in InitFan, for the Heat Pump:Water Heater object
-
-!       (Standard Rating procedure may be called before BeginEnvirFlag is set to TRUE, if so MaxAirMassFlowRate = 0)
-
-        Fan(FanNum)%RhoAirStdInit = StdRhoAir
-
-        Fan(FanNum)%MaxAirMassFlowRate = Fan(FanNum)%MaxAirFlowRate \* Fan(FanNum)%RhoAirStdInit
-
-
-
-        Fan(FanNum)%MotEff        = rNumericArgs(4)
-
-        Fan(FanNum)%MotInAirFrac  = rNumericArgs(5)
-
-        Fan(FanNum)%MinAirFlowRate= 0.0
-
-
-
-        Fan(FanNum)%InletNodeNum  = &
-
-               GetOnlySingleNode(cAlphaArgs(3),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1), &
-
-                            NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsNotParent)
-
-        Fan(FanNum)%OutletNodeNum = &
-
-               GetOnlySingleNode(cAlphaArgs(4),ErrorsFound,TRIM(cCurrentModuleObject),cAlphaArgs(1), &
-
-                            NodeType\_Air,NodeConnectionType\_Outlet,1,ObjectIsNotParent)
-
-
-
-        IF (NumAlphas &gt; 4 .AND. .NOT. lAlphaFieldBlanks(5)) THEN
-
-          Fan(FanNum)%FanPowerRatAtSpeedRatCurveIndex  = GetCurveIndex(cAlphaArgs(5))
-
-        END IF
-
-
-
-        IF (NumAlphas &gt; 5 .AND. .NOT. lAlphaFieldBlanks(6)) THEN
-
-          Fan(FanNum)%FanEffRatioCurveIndex  = GetCurveIndex(cAlphaArgs(6))
-
-        END IF
-
-
-
-        IF (NumAlphas &gt; 6 .AND. .NOT. lAlphaFieldBlanks(7)) THEN
-
-          Fan(FanNum)%EndUseSubcategoryName = cAlphaArgs(7)
-
-        ELSE
-
-          Fan(FanNum)%EndUseSubcategoryName = 'General'
-
-        END IF
-
-
-
-        CALL TestCompSet(TRIM(cCurrentModuleObject),cAlphaArgs(1),cAlphaArgs(3),cAlphaArgs(4),'Air Nodes')
-
-
-
-
-
-      END DO   ! end Number of Simple  ON-OFF FAN Loop
-
-
-
-
-
-      cCurrentModuleObject= 'FanPerformance:NightVentilation'
-
-      NumNightVentPerf = GetNumObjectsFound(TRIM(cCurrentModuleObject))
-
-
-
-      IF (NumNightVentPerf &gt; 0) THEN
-
-        ALLOCATE(NightVentPerf(NumNightVentPerf))
-
-        NightVentPerf%FanName = ' '
-
-        NightVentPerf%FanEff = 0.0
-
-        NightVentPerf%DeltaPress = 0.0
-
-        NightVentPerf%MaxAirFlowRate = 0.0
-
-        NightVentPerf%MotEff = 0.0
-
-        NightVentPerf%MotInAirFrac = 0.0
-
-        NightVentPerf%MaxAirMassFlowRate = 0.0
-
-      END IF
-
-      ! input the night ventilation performance objects
-
-      DO NVPerfNum=1,NumNightVentPerf
-
-         CALL GetObjectItem(TRIM(cCurrentModuleObject),NVPerfNum,cAlphaArgs,NumAlphas, &
-
-                           rNumericArgs,NumNums,IOSTAT, &
-
-                           NumBlank=lNumericFieldBlanks,AlphaBlank=lAlphaFieldBlanks, &
-
-                           AlphaFieldNames=cAlphaFieldNames,NumericFieldNames=cNumericFieldNames)
-
-        IsNotOK=.false.
-
-        IsBlank=.false.
-
-        CALL VerifyName(cAlphaArgs(1),NightVentPerf%FanName,NVPerfNum-1,IsNotOK,IsBlank,TRIM(cCurrentModuleObject)//' Name')
-
-        IF (IsNotOK) THEN
-
-          ErrorsFound=.true.
-
-          IF (IsBlank) cAlphaArgs(1)='xxxxx'
-
-        ENDIF
-
-        NightVentPerf(NVPerfNum)%FanName        = cAlphaArgs(1)
-
-        NightVentPerf(NVPerfNum)%FanEff         = rNumericArgs(1)
-
-        NightVentPerf(NVPerfNum)%DeltaPress     = rNumericArgs(2)
-
-        NightVentPerf(NVPerfNum)%MaxAirFlowRate = rNumericArgs(3)
-
-        NightVentPerf(NVPerfNum)%MotEff         = rNumericArgs(4)
-
-        NightVentPerf(NVPerfNum)%MotInAirFrac   = rNumericArgs(5)
-
-        ! find the corresponding fan
-
-        NVPerfFanFound = .FALSE.
-
-        DO FanNum=1,NumFans
-
-          IF (NightVentPerf(NVPerfNum)%FanName == Fan(FanNum)%FanName) THEN
-
-            NVPerfFanFound = .TRUE.
-
-            Fan(FanNum)%NVPerfNum = NVPerfNum
-
-            EXIT
-
-          END IF
-
-        END DO
-
-        IF ( .NOT. NVPerfFanFound) THEN
-
-          CALL ShowSevereError(TRIM(cCurrentModuleObject)//', fan name not found='//TRIM(cAlphaArgs(1)))
-
-          ErrorsFound=.true.
-
-        END IF
-
-
-
-      END DO
-
-
-
-      DEALLOCATE(cAlphaArgs)
-
-      DEALLOCATE(cAlphaFieldNames)
-
-      DEALLOCATE(lAlphaFieldBlanks)
-
-      DEALLOCATE(cNumericFieldNames)
-
-      DEALLOCATE(lNumericFieldBlanks)
-
-      DEALLOCATE(rNumericArgs)
-
-
-
-      IF (ErrorsFound) THEN
-
-            CALL ShowFatalError(RoutineName//'Errors found in input.  Program terminates.')
-
-      ENDIF
-
-
-
-      Do FanNum=1,NumFans
-
-             ! Setup Report variables for the Fans
-
-       CALL SetupOutputVariable('Fan Electric Power[W]', Fan(FanNum)%FanPower, 'System','Average',Fan(FanNum)%FanName)
-
-       CALL SetupOutputVariable('Fan Delta Temp[C]', Fan(FanNum)%DeltaTemp, 'System','Average',Fan(FanNum)%FanName)
-
-       CALL SetupOutputVariable('Fan Electric Consumption[J]', Fan(FanNum)%FanEnergy, 'System','Sum',Fan(FanNum)%FanName, &
-
-                                 ResourceTypeKey='Electric',GroupKey='System', &
-
-                                 EndUseKey='Fans',EndUseSubKey=Fan(FanNum)%EndUseSubcategoryName)
-
-      END DO
-
-
-
-      DO OnOffFanNum = 1,  NumOnOff
-
-       FanNum = NumSimpFan + NumVarVolFan + NumZoneExhFan + OnOffFanNum
-
-       CALL SetupOutputVariable('On/Off Fan Runtime Fraction', Fan(FanNum)%FanRuntimeFraction, 'System','Average', &
-
-                                 Fan(FanNum)%FanName)
-
-      END DO
-
-  RETURN
-
-
-
-**END SUBROUTINE GetFanInput**
-
-
-
-! End of Get Input subroutines for the HB Module
-
-!\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-
-
-
-
-
-
-! Beginning Initialization Section of the Module
-
-!\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-
-
-**SUBROUTINE InitFan(FanNum,FirstHVACIteration)**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         Richard J. Liesen
-
-          !       DATE WRITTEN   February 1998
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! This subroutine is for initializations of the Fan Components.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! Uses the status flags to trigger initializations.
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-  USE DataSizing, ONLY: CurSysNum
-
-  USE DataAirLoop, ONLY: AirLoopControlInfo
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-  LOGICAL, INTENT (IN):: FirstHVACIteration
-
-  Integer, Intent(IN) :: FanNum
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-  Integer             :: InletNode
-
-  Integer             :: OutletNode
-
-  Integer             :: InNode
-
-  Integer             :: OutNode
-
-  LOGICAL,SAVE        :: MyOneTimeFlag = .true.
-
-  LOGICAL, ALLOCATABLE,Save, DIMENSION(:) :: MyEnvrnFlag
-
-  LOGICAL, ALLOCATABLE,Save, DIMENSION(:) :: MySizeFlag
-
-
-
-          ! FLOW:
-
-
-
-  IF (MyOneTimeFlag) THEN
-
-
-
-    ALLOCATE(MyEnvrnFlag(NumFans))
-
-    ALLOCATE(MySizeFlag(NumFans))
-
-    MyEnvrnFlag = .TRUE.
-
-    MySizeFlag = .TRUE.
-
-
-
-    MyOneTimeFlag = .false.
-
-
-
-  END IF
-
-
-
-  IF ( .NOT. SysSizingCalc .AND. MySizeFlag(FanNum)) THEN
-
-
-
-    CALL SizeFan(FanNum)
-
-    ! Set the loop cycling flag
-
-    IF (Fan(FanNum)%Control == 'ONOFF') THEN
-
-      IF (CurSysNum &gt; 0) THEN
-
-        AirLoopControlInfo(CurSysNum)%CyclingFan = .TRUE.
-
-      END IF
-
-    END IF
-
-
-
-    MySizeFlag(FanNum) = .FALSE.
-
-  END IF
-
-
-
-
-
-! Do the Begin Environment initializations
-
-  IF (BeginEnvrnFlag .and. MyEnvrnFlag(FanNum)) THEN
-
-
-
-    !For all Fan inlet nodes convert the Volume flow to a mass flow
-
-    InNode = Fan(FanNum)%InletNodeNum
-
-    OutNode = Fan(FanNum)%OutletNodeNum
-
-    Fan(FanNum)%RhoAirStdInit = PsyRhoAirFnPbTdbW(StdBaroPress,20.0,0.0)
-
-
-
-    !Change the Volume Flow Rates to Mass Flow Rates
-
-
-
-    Fan(FanNum)%MaxAirMassFlowRate = Fan(FanNum)%MaxAirFlowRate \*  Fan(FanNum)%RhoAirStdInit
-
-    Fan(FanNum)%MinAirMassFlowRate = Fan(FanNum)%MinAirFlowRate \*  Fan(FanNum)%RhoAirStdInit
-
-
-
-
-
-    !Init the Node Control variables
-
-    Node(OutNode)%MassFlowRateMax      = Fan(FanNum)%MaxAirMassFlowRate
-
-    Node(OutNode)%MassFlowRateMin      = Fan(FanNum)%MinAirMassFlowRate
-
-
-
-
-
-    !Initialize all report variables to a known state at beginning of simulation
-
-    Fan(FanNum)%FanPower = 0.0
-
-    Fan(FanNum)%DeltaTemp = 0.0
-
-    Fan(FanNum)%FanEnergy = 0.0
-
-
-
-    MyEnvrnFlag(FanNum) = .FALSE.
-
-  END IF
-
-
-
-  IF (.not. BeginEnvrnFlag) THEN
-
-    MyEnvrnFlag(FanNum) = .true.
-
-  ENDIF
-
-
-
-  ! Do the Begin Day initializations
-
-    ! none
-
-
-
-  ! Do the begin HVAC time step initializations
-
-    ! none
-
-
-
-  ! Do the following initializations (every time step): This should be the info from
-
-  ! the previous components outlets or the node data in this section.
-
-
-
-  ! Do a check and make sure that the max and min available(control) flow is
-
-  ! between the physical max and min for the Fan while operating.
-
-
-
-  InletNode = Fan(FanNum)%InletNodeNum
-
-  OutletNode = Fan(FanNum)%OutletNodeNum
-
-
-
-  Fan(FanNum)%MassFlowRateMaxAvail = MIN(Node(OutletNode)%MassFlowRateMax, &
-
-                                              Node(InletNode)%MassFlowRateMaxAvail)
-
-  Fan(FanNum)%MassFlowRateMinAvail = MIN(MAX(Node(OutletNode)%MassFlowRateMin, &
-
-                                             Node(InletNode)%MassFlowRateMinAvail), &
-
-                                             Node(InletNode)%MassFlowRateMaxAvail)
-
-
-
-  ! Load the node data in this section for the component simulation
-
-  !
-
-  !First need to make sure that the massflowrate is between the max and min avail.
-
-  IF (Fan(FanNum)%FanType .NE. 'ZONE EXHAUST FAN') THEN
-
-    Fan(FanNum)%InletAirMassFlowRate = Min(Node(InletNode)%MassFlowRate, &
-
-                                           Fan(FanNum)%MassFlowRateMaxAvail)
-
-    Fan(FanNum)%InletAirMassFlowRate = Max(Fan(FanNum)%InletAirMassFlowRate, &
-
-                                           Fan(FanNum)%MassFlowRateMinAvail)
-
-  ELSE  ! zone exhaust fans - always run at the max
-
-    Fan(FanNum)%MassFlowRateMaxAvail = Fan(FanNum)%MaxAirMassFlowRate
-
-    Fan(FanNum)%MassFlowRateMinAvail = 0.0
-
-    Fan(FanNum)%InletAirMassFlowRate = Fan(FanNum)%MassFlowRateMaxAvail
-
-  END IF
-
-
-
-  !Then set the other conditions
-
-  Fan(FanNum)%InletAirTemp         = Node(InletNode)%Temp
-
-  Fan(FanNum)%InletAirHumRat       = Node(InletNode)%HumRat
-
-  Fan(FanNum)%InletAirEnthalpy     = Node(InletNode)%Enthalpy
-
-
-
-  RETURN
-
-
-
-**END SUBROUTINE InitFan**
-
-
-
-**SUBROUTINE SizeFan(FanNum)**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         Fred Buhl
-
-          !       DATE WRITTEN   September 2001
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! This subroutine is for sizing Fan Components for which flow rates have not been
-
-          ! specified in the input.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! Obtains flow rates from the zone or system sizing arrays.
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-  USE DataSizing
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-  Integer, Intent(IN) :: FanNum
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-  REAL :: FanMinAirFlowRate
-
-  EXTERNAL ReportSizingOutput
-
-
-
-  FanMinAirFlowRate = 0.0
-
-  IF (Fan(FanNum)%MaxAirFlowRate == AutoSize) THEN
-
-
-
-    IF (CurSysNum &gt; 0) THEN
-
-
-
-      CALL CheckSysSizing('FAN:'//TRIM(Fan(FanNum)%FanType)// ':' // TRIM(Fan(FanNum)%Control), &
-
-                           Fan(FanNum)%FanName)
-
-
-
-      SELECT CASE(CurDuctType)
-
-        CASE(Main)
-
-          Fan(FanNum)%MaxAirFlowRate = FinalSysSizing(CurSysNum)%DesMainVolFlow
-
-          FanMinAirFlowRate = CalcSysSizing(CurSysNum)%SysAirMinFlowRat \* CalcSysSizing(CurSysNum)%DesMainVolFlow
-
-        CASE(Cooling)
-
-          Fan(FanNum)%MaxAirFlowRate = FinalSysSizing(CurSysNum)%DesCoolVolFlow
-
-          FanMinAirFlowRate = CalcSysSizing(CurSysNum)%SysAirMinFlowRat \* CalcSysSizing(CurSysNum)%DesCoolVolFlow
-
-        CASE(Heating)
-
-          Fan(FanNum)%MaxAirFlowRate = FinalSysSizing(CurSysNum)%DesHeatVolFlow
-
-          FanMinAirFlowRate = CalcSysSizing(CurSysNum)%SysAirMinFlowRat \* CalcSysSizing(CurSysNum)%DesHeatVolFlow
-
-        CASE(Other)
-
-          Fan(FanNum)%MaxAirFlowRate = FinalSysSizing(CurSysNum)%DesMainVolFlow
-
-          FanMinAirFlowRate = CalcSysSizing(CurSysNum)%SysAirMinFlowRat \* CalcSysSizing(CurSysNum)%DesMainVolFlow
-
-        CASE DEFAULT
-
-          Fan(FanNum)%MaxAirFlowRate = FinalSysSizing(CurSysNum)%DesMainVolFlow
-
-          FanMinAirFlowRate = CalcSysSizing(CurSysNum)%SysAirMinFlowRat \* CalcSysSizing(CurSysNum)%DesMainVolFlow
-
-      END SELECT
-
-
-
-    ELSE IF (CurZoneEqNum &gt; 0) THEN
-
-
-
-      CALL CheckZoneSizing('FAN:' // TRIM(Fan(FanNum)%FanType) // ':' // TRIM(Fan(FanNum)%Control), &
-
-                           Fan(FanNum)%FanName)
-
-      IF (.NOT. ZoneHeatingOnlyFan) THEN
-
-        Fan(FanNum)%MaxAirFlowRate = MAX(FinalZoneSizing(CurZoneEqNum)%DesCoolVolFlow, &
-
-                                         FinalZoneSizing(CurZoneEqNum)%DesHeatVolFlow)
-
-      ELSE
-
-        Fan(FanNum)%MaxAirFlowRate = FinalZoneSizing(CurZoneEqNum)%DesHeatVolFlow
-
-      END IF
-
-
-
-    END IF
-
-
-
-    IF (Fan(FanNum)%MaxAirFlowRate &lt; SmallAirVolFlow) THEN
-
-      Fan(FanNum)%MaxAirFlowRate = 0.0
-
-    END IF
-
-
-
-    CALL ReportSizingOutput('FAN:' // TRIM(Fan(FanNum)%FanType) // ':' // TRIM(Fan(FanNum)%Control), &
-
-                            Fan(FanNum)%FanName, 'Max Flow Rate [m3/s]', Fan(FanNum)%MaxAirFlowRate)
-
-
-
-    IF (Fan(FanNum)%Control == 'VARIABLEVOLUME') THEN
-
-      CALL CheckSysSizing('FAN:' // TRIM(Fan(FanNum)%FanType) // ':' // TRIM(Fan(FanNum)%Control), &
-
-                           Fan(FanNum)%FanName)
-
-      Fan(FanNum)%MinAirFlowRate = FanMinAirFlowRate
-
-      CALL ReportSizingOutput('FAN:' // TRIM(Fan(FanNum)%FanType) // ':' // TRIM(Fan(FanNum)%Control), &
-
-                              Fan(FanNum)%FanName, 'Min Flow Rate [m3/s]', Fan(FanNum)%MinAirFlowRate)
-
-    END IF
-
-
-
-  END IF
-
-
-
-  RETURN
-
-
-
-**END SUBROUTINE SizeFan**
-
-
-
-! End Initialization Section of the Module
-
-!\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-
-
-
-
-! Begin Algorithm Section of the Module
-
-!\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-**SUBROUTINE SimSimpleFan(FanNum)**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         Unknown
-
-          !       DATE WRITTEN   Unknown
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! This subroutine simulates the simple constant volume fan.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! Converts design pressure rise and efficiency into fan power and temperature rise
-
-          ! Constant fan pressure rise is assumed.
-
-
-
-          ! REFERENCES:
-
-          ! ASHRAE HVAC 2 Toolkit, page 2-3 (FANSIM)
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-   Integer, Intent(IN) :: FanNum
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-      Real RhoAir
-
-      Real DeltaPress  ! [N/M^2]
-
-      Real FanEff
-
-      Real MassFlow    ! [kg/sec]
-
-      Real Tin         ! [C]
-
-      Real Win
-
-      Real FanShaftPower ! power delivered to fan shaft
-
-      Real PowerLossToAir ! fan and motor loss to air stream (watts)
-
-
-
-   DeltaPress = Fan(FanNum)%DeltaPress
-
-   FanEff     = Fan(FanNum)%FanEff
-
-
-
-   ! For a Constant Volume Simple Fan the Max Flow Rate is the Flow Rate for the fan
-
-   Tin        = Fan(FanNum)%InletAirTemp
-
-   Win        = Fan(FanNum)%InletAirHumRat
-
-   RhoAir     = Fan(FanNum)%RhoAirStdInit
-
-   MassFlow   = MIN(Fan(FanNum)%InletAirMassFlowRate,Fan(FanNum)%MaxAirMassFlowRate)
-
-   MassFlow   = MAX(MassFlow,Fan(FanNum)%MinAirMassFlowRate)
-
-   !
-
-   !Determine the Fan Schedule for the Time step
-
-  If( ( GetCurrentScheduleValue(Fan(FanNum)%SchedPtr)&gt;0.0 .and. Massflow&gt;0.0 .or. TurnFansOn .and. Massflow&gt;0.0) &
-
-        .and. .NOT.TurnFansOff ) Then
-
-   !Fan is operating
-
-   Fan(FanNum)%FanPower = MassFlow\*DeltaPress/(FanEff\*RhoAir) ! total fan power
-
-   FanShaftPower = Fan(FanNum)%MotEff \* Fan(FanNum)%FanPower  ! power delivered to shaft
-
-   PowerLossToAir = FanShaftPower + (Fan(FanNum)%FanPower - FanShaftPower) \* Fan(FanNum)%MotInAirFrac
-
-   Fan(FanNum)%OutletAirEnthalpy = Fan(FanNum)%InletAirEnthalpy + PowerLossToAir/MassFlow
-
-   ! This fan does not change the moisture or Mass Flow across the component
-
-   Fan(FanNum)%OutletAirHumRat       = Fan(FanNum)%InletAirHumRat
-
-   Fan(FanNum)%OutletAirMassFlowRate = MassFlow
-
-   Fan(FanNum)%OutletAirTemp = PsyTdbFnHW(Fan(FanNum)%OutletAirEnthalpy,Fan(FanNum)%OutletAirHumRat)
-
-
-
- Else
-
-   !Fan is off and not operating no power consumed and mass flow rate.
-
-   Fan(FanNum)%FanPower = 0.0
-
-   FanShaftPower = 0.0
-
-   PowerLossToAir = 0.0
-
-   Fan(FanNum)%OutletAirMassFlowRate = 0.0
-
-   Fan(FanNum)%OutletAirHumRat       = Fan(FanNum)%InletAirHumRat
-
-   Fan(FanNum)%OutletAirEnthalpy     = Fan(FanNum)%InletAirEnthalpy
-
-   Fan(FanNum)%OutletAirTemp = Fan(FanNum)%InletAirTemp
-
-   ! Set the Control Flow variables to 0.0 flow when OFF.
-
-   Fan(FanNum)%MassFlowRateMaxAvail = 0.0
-
-   Fan(FanNum)%MassFlowRateMinAvail = 0.0
-
-
-
- End If
-
-
-
- RETURN
-
-**END SUBROUTINE SimSimpleFan**
-
-
-
-
-
-**SUBROUTINE SimVariableVolumeFan(FanNum)**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         Unknown
-
-          !       DATE WRITTEN   Unknown
-
-          !       MODIFIED       Phil Haves
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! This subroutine simulates the simple variable volume fan.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! Converts design pressure rise and efficiency into fan power and temperature rise
-
-          ! Constant fan pressure rise is assumed.
-
-          ! Uses curves of fan power fraction vs. fan part load to determine fan power at
-
-          ! off design conditions.
-
-
-
-          ! REFERENCES:
-
-          ! ASHRAE HVAC 2 Toolkit, page 2-3 (FANSIM)
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-   Integer, Intent(IN) :: FanNum
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-      Real RhoAir
-
-      Real DeltaPress  ! [N/M^2 = Pa]
-
-      Real FanEff      ! Total fan efficiency - combined efficiency of fan, drive train,
-
-                       ! motor and variable speed controller (if any)
-
-      Real MassFlow    ! [kg/sec]
-
-      Real Tin         ! [C]
-
-      Real Win
-
-      Real PartLoadFrac
-
-      REAL MaxFlowFrac   !Variable Volume Fan Max Flow Fraction [-]
-
-      REAL MinFlowFrac   !Variable Volume Fan Min Flow Fraction [-]
-
-      REAL FlowFrac      !Variable Volume Fan Flow Fraction [-]
-
-      Real FanShaftPower ! power delivered to fan shaft
-
-      Real PowerLossToAir ! fan and motor loss to air stream (watts)
-
-
-
-! Simple Variable Volume Fan - default values from DOE-2
-
-! Type of Fan          Coeff1       Coeff2       Coeff3        Coeff4      Coeff5
-
-! INLET VANE DAMPERS   0.35071223   0.30850535   -0.54137364   0.87198823  0.000
-
-! DISCHARGE DAMPERS    0.37073425   0.97250253   -0.34240761   0.000       0.000
-
-! VARIABLE SPEED MOTOR 0.0015302446 0.0052080574  1.1086242   -0.11635563  0.000
-
-
-
-   DeltaPress  = Fan(FanNum)%DeltaPress
-
-   FanEff      = Fan(FanNum)%FanEff
-
-
-
-   Tin         = Fan(FanNum)%InletAirTemp
-
-   Win         = Fan(FanNum)%InletAirHumRat
-
-   RhoAir      = Fan(FanNum)%RhoAirStdInit
-
-   MassFlow    = MIN(Fan(FanNum)%InletAirMassFlowRate,Fan(FanNum)%MaxAirMassFlowRate)
-
-   ! MassFlow    = MAX(MassFlow,Fan(FanNum)%MinAirMassFlowRate)
-
-
-
-  ! Calculate and check limits on fraction of system flow
-
-  MaxFlowFrac = 1.0
-
-  ! MinFlowFrac is calculated from the ration of the volume flows and is non-dimensional
-
-  MinFlowFrac = Fan(FanNum)%MinAirFlowRate/Fan(FanNum)%MaxAirFlowRate
-
-  ! The actual flow fraction is calculated from MassFlow and the MaxVolumeFlow \* AirDensity
-
-  FlowFrac = MassFlow/(Fan(FanNum)%MaxAirMassFlowRate)
-
-
-
-! Calculate the part Load Fraction             (PH 7/13/03)
-
-
-
-  FlowFrac = MAX(MinFlowFrac,MIN(FlowFrac,1.0))  ! limit flow fraction to allowed range
-
-
-
-  PartLoadFrac=Fan(FanNum)%FanCoeff(1) + Fan(FanNum)%FanCoeff(2)\*FlowFrac +  &
-
-                  Fan(FanNum)%FanCoeff(3)\*FlowFrac\*\*2 + Fan(FanNum)%FanCoeff(4)\*FlowFrac\*\*3 + &
-
-                  Fan(FanNum)%FanCoeff(5)\*FlowFrac\*\*4
-
-
-
-
-
-   !Determine the Fan Schedule for the Time step
-
-  If( ( GetCurrentScheduleValue(Fan(FanNum)%SchedPtr)&gt;0.0 .and. Massflow&gt;0.0 .or. TurnFansOn .and. Massflow&gt;0.0) &
-
-        .and. .NOT.TurnFansOff ) Then
-
-   !Fan is operating - calculate power loss and enthalpy rise
-
-!   Fan(FanNum)%FanPower = PartLoadFrac\*FullMassFlow\*DeltaPress/(FanEff\*RhoAir) ! total fan power
-
-   Fan(FanNum)%FanPower = PartLoadFrac\*Fan(FanNum)%MaxAirMassFlowRate\*DeltaPress/(FanEff\*RhoAir) ! total fan power (PH 7/13/03)
-
-   FanShaftPower = Fan(FanNum)%MotEff \* Fan(FanNum)%FanPower  ! power delivered to shaft
-
-   PowerLossToAir = FanShaftPower + (Fan(FanNum)%FanPower - FanShaftPower) \* Fan(FanNum)%MotInAirFrac
-
-   Fan(FanNum)%OutletAirEnthalpy = Fan(FanNum)%InletAirEnthalpy + PowerLossToAir/MassFlow
-
-   ! This fan does not change the moisture or Mass Flow across the component
-
-   Fan(FanNum)%OutletAirHumRat       = Fan(FanNum)%InletAirHumRat
-
-   Fan(FanNum)%OutletAirMassFlowRate = MassFlow
-
-   Fan(FanNum)%OutletAirTemp = PsyTdbFnHW(Fan(FanNum)%OutletAirEnthalpy,Fan(FanNum)%OutletAirHumRat)
-
-  Else
-
-   !Fan is off and not operating no power consumed and mass flow rate.
-
-   Fan(FanNum)%FanPower = 0.0
-
-   FanShaftPower = 0.0
-
-   PowerLossToAir = 0.0
-
-   Fan(FanNum)%OutletAirMassFlowRate = 0.0
-
-   Fan(FanNum)%OutletAirHumRat       = Fan(FanNum)%InletAirHumRat
-
-   Fan(FanNum)%OutletAirEnthalpy     = Fan(FanNum)%InletAirEnthalpy
-
-   Fan(FanNum)%OutletAirTemp = Fan(FanNum)%InletAirTemp
-
-   ! Set the Control Flow variables to 0.0 flow when OFF.
-
-   Fan(FanNum)%MassFlowRateMaxAvail = 0.0
-
-   Fan(FanNum)%MassFlowRateMinAvail = 0.0
-
-  End If
-
-
-
-  RETURN
-
-**END SUBROUTINE SimVariableVolumeFan**
-
-
-
-**SUBROUTINE SimOnOffFan(FanNum)**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         Unknown
-
-          !       DATE WRITTEN   Unknown
-
-          !       MODIFIED       Shirey, May 2001
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! This subroutine simulates the simple on/off fan.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! Converts design pressure rise and efficiency into fan power and temperature rise
-
-          ! Constant fan pressure rise is assumed.
-
-          ! Uses curves of fan power fraction vs. fan part load to determine fan power at
-
-          ! off design conditions.
-
-          ! Same as simple (constant volume) fan, except added part-load curve input
-
-
-
-          ! REFERENCES:
-
-          ! ASHRAE HVAC 2 Toolkit, page 2-3 (FANSIM)
-
-
-
-          ! USE STATEMENTS:
-
-  USE CurveManager, ONLY: CurveValue
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-   Integer, Intent(IN) :: FanNum
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-      Real RhoAir
-
-      Real DeltaPress  ! [N/M^2]
-
-      Real FanEff
-
-      Real MassFlow    ! [kg/sec]
-
-      Real Tin         ! [C]
-
-      Real Win
-
-      Real PartLoadRatio !Ratio of actual mass flow rate to max mass flow rate
-
-      REAL FlowFrac      !Actual Fan Flow Fraction = actual mass flow rate / max air mass flow rate
-
-      Real FanShaftPower ! power delivered to fan shaft
-
-      Real PowerLossToAir ! fan and motor loss to air stream (watts)
-
-
-
-   DeltaPress = Fan(FanNum)%DeltaPress
-
-   FanEff     = Fan(FanNum)%FanEff
-
-
-
-   Tin        = Fan(FanNum)%InletAirTemp
-
-   Win        = Fan(FanNum)%InletAirHumRat
-
-   RhoAir     = Fan(FanNum)%RhoAirStdInit
-
-   MassFlow   = MIN(Fan(FanNum)%InletAirMassFlowRate,Fan(FanNum)%MaxAirMassFlowRate)
-
-   MassFlow   = MAX(MassFlow,Fan(FanNum)%MinAirMassFlowRate)
-
-   Fan(FanNum)%FanRuntimeFraction = 0.0
-
-
-
-  ! The actual flow fraction is calculated from MassFlow and the MaxVolumeFlow \* AirDensity
-
-  FlowFrac = MassFlow/(Fan(FanNum)%MaxAirMassFlowRate)
-
-
-
-  ! Calculate the part load ratio, can't be greater than 1
-
-  PartLoadRatio= MIN(1.0,FlowFrac)
-
-  ! Determine the Fan Schedule for the Time step
-
-  IF( ( GetCurrentScheduleValue(Fan(FanNum)%SchedPtr)&gt;0.0 .and. Massflow&gt;0.0 .or. TurnFansOn .and. Massflow&gt;0.0) &
-
-        .and. .NOT.TurnFansOff ) THEN
-
-   ! Fan is operating
-
-   IF (OnOffFanPartLoadFraction &lt;= 0.0) THEN
-
-     CALL ShowWarningError('FAN:SIMPLE:ONOFF, OnOffFanPartLoadFraction &lt;= 0.0, Reset to 1.0')
-
-     OnOffFanPartLoadFraction = 1.0 ! avoid divide by zero or negative PLF
-
-   END IF
-
-
-
-   IF (OnOffFanPartLoadFraction &lt; 0.7) THEN
-
-        OnOffFanPartLoadFraction = 0.7 ! a warning message is already issued from the DX coils or gas heating coil
-
-   END IF
-
-   ! Keep fan runtime fraction between 0.0 and 1.0
-
-   Fan(FanNum)%FanRuntimeFraction = MAX(0.0,MIN(1.0,PartLoadRatio/OnOffFanPartLoadFraction))
-
-   ! Fan(FanNum)%FanPower = MassFlow\*DeltaPress/(FanEff\*RhoAir\*OnOffFanPartLoadFraction)! total fan power
-
-   Fan(FanNum)%FanPower = Fan(FanNum)%MaxAirMassFlowRate\*Fan(FanNum)%FanRuntimeFraction\*DeltaPress/(FanEff\*RhoAir)!total fan power
-
-   ! OnOffFanPartLoadFraction is passed via DataHVACGlobals from the cooling or heating coil that is
-
-   !   requesting the fan to operate in cycling fan/cycling coil mode
-
-   OnOffFanPartLoadFraction = 1.0 ! reset to 1 in case other on/off fan is called without a part load curve
-
-   FanShaftPower = Fan(FanNum)%MotEff \* Fan(FanNum)%FanPower  ! power delivered to shaft
-
-   PowerLossToAir = FanShaftPower + (Fan(FanNum)%FanPower - FanShaftPower) \* Fan(FanNum)%MotInAirFrac
-
-   Fan(FanNum)%OutletAirEnthalpy = Fan(FanNum)%InletAirEnthalpy + PowerLossToAir/MassFlow
-
-   ! This fan does not change the moisture or Mass Flow across the component
-
-   Fan(FanNum)%OutletAirHumRat       = Fan(FanNum)%InletAirHumRat
-
-   Fan(FanNum)%OutletAirMassFlowRate = MassFlow
-
-!   Fan(FanNum)%OutletAirTemp = Tin + PowerLossToAir/(MassFlow\*PsyCpAirFnWTdb(Win,Tin))
-
-   Fan(FanNum)%OutletAirTemp = PsyTdbFnHW(Fan(FanNum)%OutletAirEnthalpy,Fan(FanNum)%OutletAirHumRat)
-
-  ELSE
-
-   ! Fan is off and not operating no power consumed and mass flow rate.
-
-   Fan(FanNum)%FanPower = 0.0
-
-   FanShaftPower = 0.0
-
-   PowerLossToAir = 0.0
-
-   Fan(FanNum)%OutletAirMassFlowRate = 0.0
-
-   Fan(FanNum)%OutletAirHumRat       = Fan(FanNum)%InletAirHumRat
-
-   Fan(FanNum)%OutletAirEnthalpy     = Fan(FanNum)%InletAirEnthalpy
-
-   Fan(FanNum)%OutletAirTemp = Fan(FanNum)%InletAirTemp
-
-   ! Set the Control Flow variables to 0.0 flow when OFF.
-
-   Fan(FanNum)%MassFlowRateMaxAvail = 0.0
-
-   Fan(FanNum)%MassFlowRateMinAvail = 0.0
-
-  END IF
-
-
-
-  RETURN
-
-**END SUBROUTINE SimOnOffFan**
-
-
-
-
-
-**SUBROUTINE SimZoneExhaustFan(FanNum)**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         Fred Buhl
-
-          !       DATE WRITTEN   Jan 2000
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! This subroutine simulates the Zone Exhaust Fan
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! Converts design pressure rise and efficiency into fan power and temperature rise
-
-          ! Constant fan pressure rise is assumed.
-
-
-
-          ! REFERENCES:
-
-          ! ASHRAE HVAC 2 Toolkit, page 2-3 (FANSIM)
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-   Integer, Intent(IN) :: FanNum
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-      Real RhoAir
-
-      Real DeltaPress  ! [N/M^2]
-
-      Real FanEff
-
-      Real MassFlow    ! [kg/sec]
-
-      Real Tin         ! [C]
-
-      Real Win
-
-      Real PowerLossToAir ! fan and motor loss to air stream (watts)
-
-
-
-   DeltaPress = Fan(FanNum)%DeltaPress
-
-   FanEff     = Fan(FanNum)%FanEff
-
-
-
-   ! For a Constant Volume Simple Fan the Max Flow Rate is the Flow Rate for the fan
-
-   Tin        = Fan(FanNum)%InletAirTemp
-
-   Win        = Fan(FanNum)%InletAirHumRat
-
-   RhoAir     = Fan(FanNum)%RhoAirStdInit
-
-   MassFlow   = Fan(FanNum)%InletAirMassFlowRate
-
-   !
-
-   !Determine the Fan Schedule for the Time step
-
-  If( ( GetCurrentScheduleValue(Fan(FanNum)%SchedPtr)&gt;0.0 .or. TurnFansOn ) &
-
-        .and. .NOT.TurnFansOff ) Then
-
-   !Fan is operating
-
-   Fan(FanNum)%FanPower = MassFlow\*DeltaPress/(FanEff\*RhoAir) ! total fan power
-
-   PowerLossToAir = Fan(FanNum)%FanPower
-
-   Fan(FanNum)%OutletAirEnthalpy = Fan(FanNum)%InletAirEnthalpy + PowerLossToAir/MassFlow
-
-   ! This fan does not change the moisture or Mass Flow across the component
-
-   Fan(FanNum)%OutletAirHumRat       = Fan(FanNum)%InletAirHumRat
-
-   Fan(FanNum)%OutletAirMassFlowRate = MassFlow
-
-   Fan(FanNum)%OutletAirTemp = PsyTdbFnHW(Fan(FanNum)%OutletAirEnthalpy,Fan(FanNum)%OutletAirHumRat)
-
-
-
- Else
-
-   !Fan is off and not operating no power consumed and mass flow rate.
-
-   Fan(FanNum)%FanPower = 0.0
-
-   PowerLossToAir = 0.0
-
-   Fan(FanNum)%OutletAirMassFlowRate = 0.0
-
-   Fan(FanNum)%OutletAirHumRat       = Fan(FanNum)%InletAirHumRat
-
-   Fan(FanNum)%OutletAirEnthalpy     = Fan(FanNum)%InletAirEnthalpy
-
-   Fan(FanNum)%OutletAirTemp = Fan(FanNum)%InletAirTemp
-
-   ! Set the Control Flow variables to 0.0 flow when OFF.
-
-   Fan(FanNum)%MassFlowRateMaxAvail = 0.0
-
-   Fan(FanNum)%MassFlowRateMinAvail = 0.0
-
-   Fan(FanNum)%InletAirMassFlowRate = 0.0
-
-
-
- End If
-
-
-
- RETURN
-
-**END SUBROUTINE SimZoneExhaustFan**
-
-
-
-! End Algorithm Section of the Module
-
-! \*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-
-
-! Beginning of Update subroutines for the Fan Module
-
-! \*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-
-
-**SUBROUTINE UpdateFan(FanNum)**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         Richard Liesen
-
-          !       DATE WRITTEN   April 1998
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! This subroutine updates the fan outlet nodes.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! Data is moved from the fan data structure to the fan outlet nodes.
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-   Integer, Intent(IN) :: FanNum
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-  Integer             :: OutletNode
-
-  Integer             :: InletNode
-
-
-
-
-
-   OutletNode = Fan(FanNum)%OutletNodeNum
-
-   InletNode = Fan(FanNum)%InletNodeNum
-
-
-
-   ! Set the outlet air nodes of the fan
-
-   Node(OutletNode)%MassFlowRate  = Fan(FanNum)%OutletAirMassFlowRate
-
-   Node(OutletNode)%Temp          = Fan(FanNum)%OutletAirTemp
-
-   Node(OutletNode)%HumRat        = Fan(FanNum)%OutletAirHumRat
-
-   Node(OutletNode)%Enthalpy      = Fan(FanNum)%OutletAirEnthalpy
-
-   ! Set the outlet nodes for properties that just pass through & not used
-
-   Node(OutletNode)%Quality         = Node(InletNode)%Quality
-
-   Node(OutletNode)%Press           = Node(InletNode)%Press
-
-
-
-   ! Set the Node Flow Control Variables from the Fan Control Variables
-
-   Node(OutletNode)%MassFlowRateMaxAvail = Fan(FanNum)%MassFlowRateMaxAvail
-
-   Node(OutletNode)%MassFlowRateMinAvail = Fan(FanNum)%MassFlowRateMinAvail
-
-
-
-   IF (Fan(FanNum)%FanType .EQ. 'ZONE EXHAUST FAN') THEN
-
-     Node(InletNode)%MassFlowRate = Fan(FanNum)%InletAirMassFlowRate
-
-   END IF
-
-
-
-  RETURN
-
-**END Subroutine UpdateFan**
-
-
-
-!        End of Update subroutines for the Fan Module
-
-! \*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-
-
-
-
-! Beginning of Reporting subroutines for the Fan Module
-
-! \*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-
-
-**SUBROUTINE ReportFan(FanNum)**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         Richard Liesen
-
-          !       DATE WRITTEN   April 1998
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! This subroutine updates the report variables for the fans.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! na
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-  Use DataHVACGlobals, ONLY: TimeStepSys, FanElecPower
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-   Integer, Intent(IN) :: FanNum
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-          ! na
-
-
-
-    Fan(FanNum)%FanEnergy=Fan(FanNum)%FanPower\*TimeStepSys\*3600
-
-    Fan(FanNum)%DeltaTemp=Fan(FanNum)%OutletAirTemp - Fan(FanNum)%InletAirTemp
-
-    FanElecPower = Fan(FanNum)%FanPower
-
-
-
-  RETURN
-
-**END Subroutine ReportFan**
-
-
-
-!        End of Reporting subroutines for the Fan Module
-
-! \*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-! Beginning of Utility subroutines for the Fan Module
-
-! \*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-**FUNCTION GetFanDesignVolumeFlowRate(FanType,FanName,ErrorsFound) RESULT(DesignVolumeFlowRate)**
-
-
-
-          ! FUNCTION INFORMATION:
-
-          !       AUTHOR         Linda Lawrie
-
-          !       DATE WRITTEN   February 2006
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS FUNCTION:
-
-          ! This function looks up the design volume flow rate for the given fan and returns it.  If
-
-          ! incorrect fan type or name is given, errorsfound is returned as true and value is returned
-
-          ! as negative.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! na
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-  USE InputProcessor,  ONLY: FindItemInList
-
-
-
-  IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! FUNCTION ARGUMENT DEFINITIONS:
-
-  CHARACTER(len=\*), INTENT(IN) :: FanType      ! must match fan types in this module
-
-  CHARACTER(len=\*), INTENT(IN) :: FanName      ! must match fan names for the fan type
-
-  LOGICAL, INTENT(INOUT)       :: ErrorsFound  ! set to true if problem
-
-  REAL                         :: DesignVolumeFlowRate ! returned flow rate of matched fan
-
-
-
-          ! FUNCTION PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS:
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS:
-
-          ! na
-
-
-
-          ! FUNCTION LOCAL VARIABLE DECLARATIONS:
-
-  INTEGER :: WhichFan
-
-
-
-  ! Obtains and Allocates fan related parameters from input file
-
-  IF (GetFanInputFlag) THEN  !First time subroutine has been entered
-
-    CALL GetFanInput
-
-    GetFanInputFlag=.false.
-
-  End If
-
-
-
-  WhichFan=FindItemInList(FanName,Fan%FanName,NumFans)
-
-  IF (WhichFan /= 0) THEN
-
-    DesignVolumeFlowRate=Fan(WhichFan)%MaxAirFlowRate
-
-  ENDIF
-
-
-
-  IF (WhichFan == 0) THEN
-
-    CALL ShowSevereError('Could not find FanType="'//TRIM(FanType)//'" with Name="'//TRIM(FanName)//'"')
-
-    ErrorsFound=.true.
-
-    DesignVolumeFlowRate=-1000.
-
-  ENDIF
-
-
-
-  RETURN
-
-
-
-**END FUNCTION GetFanDesignVolumeFlowRate**
-
-
-
-**FUNCTION GetFanInletNode(FanType,FanName,ErrorsFound) RESULT(NodeNumber)**
-
-
-
-          ! FUNCTION INFORMATION:
-
-          !       AUTHOR         Linda Lawrie
-
-          !       DATE WRITTEN   February 2006
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS FUNCTION:
-
-          ! This function looks up the given fan and returns the inlet node.  If
-
-          ! incorrect fan type or name is given, errorsfound is returned as true and value is returned
-
-          ! as zero.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! na
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-  USE InputProcessor,  ONLY: FindItemInList
-
-
-
-  IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! FUNCTION ARGUMENT DEFINITIONS:
-
-  CHARACTER(len=\*), INTENT(IN) :: FanType      ! must match fan types in this module
-
-  CHARACTER(len=\*), INTENT(IN) :: FanName      ! must match fan names for the fan type
-
-  LOGICAL, INTENT(INOUT)       :: ErrorsFound  ! set to true if problem
-
-  INTEGER                      :: NodeNumber   ! returned outlet node of matched fan
-
-
-
-          ! FUNCTION PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS:
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS:
-
-          ! na
-
-
-
-          ! FUNCTION LOCAL VARIABLE DECLARATIONS:
-
-  INTEGER :: WhichFan
-
-
-
-  ! Obtains and Allocates fan related parameters from input file
-
-  IF (GetFanInputFlag) THEN  !First time subroutine has been entered
-
-    CALL GetFanInput
-
-    GetFanInputFlag=.false.
-
-  End If
-
-
-
-  WhichFan=FindItemInList(FanName,Fan%FanName,NumFans)
-
-  IF (WhichFan /= 0) THEN
-
-    NodeNumber=Fan(WhichFan)%InletNodeNum
-
-  ENDIF
-
-
-
-  IF (WhichFan == 0) THEN
-
-    CALL ShowSevereError('Could not find FanType="'//TRIM(FanType)//'" with Name="'//TRIM(FanName)//'"')
-
-    ErrorsFound=.true.
-
-    NodeNumber=0
-
-  ENDIF
-
-
-
-  RETURN
-
-
-
-**END FUNCTION GetFanInletNode**
-
-
-
-**FUNCTION GetFanOutletNode(FanType,FanName,ErrorsFound) RESULT(NodeNumber)**
-
-
-
-          ! FUNCTION INFORMATION:
-
-          !       AUTHOR         Linda Lawrie
-
-          !       DATE WRITTEN   February 2006
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS FUNCTION:
-
-          ! This function looks up the given fan and returns the outlet node.  If
-
-          ! incorrect fan type or name is given, errorsfound is returned as true and value is returned
-
-          ! as zero.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! na
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-  USE InputProcessor,  ONLY: FindItemInList
-
-
-
-  IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! FUNCTION ARGUMENT DEFINITIONS:
-
-  CHARACTER(len=\*), INTENT(IN) :: FanType      ! must match fan types in this module
-
-  CHARACTER(len=\*), INTENT(IN) :: FanName      ! must match fan names for the fan type
-
-  LOGICAL, INTENT(INOUT)       :: ErrorsFound  ! set to true if problem
-
-  INTEGER                      :: NodeNumber   ! returned outlet node of matched fan
-
-
-
-          ! FUNCTION PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS:
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS:
-
-          ! na
-
-
-
-          ! FUNCTION LOCAL VARIABLE DECLARATIONS:
-
-  INTEGER :: WhichFan
-
-
-
-  ! Obtains and Allocates fan related parameters from input file
-
-  IF (GetFanInputFlag) THEN  !First time subroutine has been entered
-
-    CALL GetFanInput
-
-    GetFanInputFlag=.false.
-
-  End If
-
-
-
-  WhichFan=FindItemInList(FanName,Fan%FanName,NumFans)
-
-  IF (WhichFan /= 0) THEN
-
-    NodeNumber=Fan(WhichFan)%OutletNodeNum
-
-  ENDIF
-
-
-
-  IF (WhichFan == 0) THEN
-
-    CALL ShowSevereError('Could not find FanType="'//TRIM(FanType)//'" with Name="'//TRIM(FanName)//'"')
-
-    ErrorsFound=.true.
-
-    NodeNumber=0
-
-  ENDIF
-
-
-
-  RETURN
-
-
-
-**END FUNCTION GetFanOutletNode**
-
-
-
-! End of Utility subroutines for the Fan Module
-
-! \*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*\*
-
-
-
-!     NOTICE
-
-!
-
-!     Copyright © 1996-xxxx The Board of Trustees of the University of Illinois
-
-!     and The Regents of the University of California through Ernest Orlando Lawrence
-
-!     Berkeley National Laboratory.  All rights reserved.
-
-!
-
-!     Portions of the EnergyPlus software package have been developed and copyrighted
-
-!     by other individuals, companies and institutions.  These portions have been
-
-!     incorporated into the EnergyPlus software package under license.   For a complete
-
-!     list of contributors, see "Notice" located in EnergyPlus.f90.
-
-!
-
-!     NOTICE: The U.S. Government is granted for itself and others acting on its
-
-!     behalf a paid-up, nonexclusive, irrevocable, worldwide license in this data to
-
-!     reproduce, prepare derivative works, and perform publicly and display publicly.
-
-!     Beginning five (5) years after permission to assert copyright is granted,
-
-!     subject to two possible five year renewals, the U.S. Government is granted for
-
-!     itself and others acting on its behalf a paid-up, non-exclusive, irrevocable
-
-!     worldwide license in this data to reproduce, prepare derivative works,
-
-!     distribute copies to the public, perform publicly and display publicly, and to
-
-!     permit others to do so.
-
-!
-
-!     TRADEMARKS: EnergyPlus is a trademark of the US Department of Energy.
-
-!
-
-
-
-**End Module Fans**
-
-
-
-
-
-
-Changing existing code
-----------------------
-
-It may be that your new module or your new feature impacts existing code.  Should that happen, follow the guidance in the Programming Standard about positioning of “global data�.  Likewise, any code written should follow the guidance outlined in the Programming Standard.
-
-Considerations for Legacy Codes
--------------------------------
-
-Those module developers who are adding to EnergyPlus’s capabilities by adapting existing codes into the module structure should take special considerations.
-
-**First and foremost, who owns the legacy code that you are adapting?*  More on this is covered in Appendix C – Submissions and Check-ins.  One must be very careful when developing modules to be implemented in the publicly-available version of EnergyPlus.***
-
-Legacy codes will typically come with their own input and output structures.  In adapting a legacy code to use with EnergyPlus, the module developer will usually want to bypass these routines by embedding the code into EnergyPlus and using input entirely from the IDD/IDF structure.  During original transition, you can consider doing a parallel effort of writing a simple input file for the legacy code while testing results with your developing EnergyPlus transition code.
-
-Code Readability vs. Speed of Execution
----------------------------------------
-
-Programmers throughout time have had to deal with speed of code execution and it’s an ongoing concern.  However, compilers are pretty smart these days and, often, can produce speedier code for the hardware platform than the programmer can when he or she uses “speed up� tips.  The EnergyPlus development team would rather the code be more “readable� to all than to try to outwit the compilers for every platform.  First and foremost, the code is the true document of what EnergyPlus does – other documents will try to explain algorithms and such but must really take a back seat to the code itself.
-
-However, many people may read the code – as developers, we should try to make it as readable at first glance as possible.  For a true example from the code and a general indication of preferred style, take the case of the zone temperature update equation.  In the [Engineering Reference](file:///E:\Docs4PDFs\EngineeringReference.pdf) document, the form is recognizable and usual:
-
-![](media/image001.png)And, this equation appears in the code (ZoneTempPredictorCorrector Module), as:
-
-ZT(ZoneNum)= (CoefSumhat +   CoefAirrat\*(3.0\*ZTM1(ZoneNum) - (3.0/2.0)\*ZTM2(ZoneNum) &
-
-                                              + (1./3.)\* ZTM3(ZoneNum))) &
-
-                             / ((11.0/6.0)\*CoefAirrat+CoefSumha)
-
-Somewhat abbreviated here due to lack of page width but still recognizable from the original.  A better version would actually be:
-
-ZT(ZoneNum)= (CoefSumhat -   CoefAirrat\*(-3.0\*ZTM1(ZoneNum) + (3.0/2.0)\*ZTM2(ZoneNum) &
-
-                                              - (1./3.)\* ZTM3(ZoneNum))) &
-
-                             / ((11.0/6.0)\*CoefAirrat+CoefSumha)
-
-Whereas the natural tendency of programming would lead to the less readable:
-
-ZT(ZoneNum)= (CoefSumhat + CoefAirrat\*(3.0\*ZTM1(ZoneNum) – 1.5\*ZTM2(ZoneNum) + .333333\* ZTM3(ZoneNum))) &
-
-           / (1.83333\*CoefAirrat+CoefSumha)
-
-The final version is a correct translation (more or less) from the Engineering/usual representation but much harder to look at in code and realize what is being represented.
-
-### Speed of Execution
-
-**A critical consideration in speed of execution is character string comparisons.**  These are typically quite slow and should not be used in the core routines (i.e. those that are executed every zone or hvac time step). An alternative to string comparisons is to define module-level integer parameters, equate a string to a parameter during the initial subroutine call (e.g. GetInput), and then do integer comparisons through the remainder of the calls to the module.  Doing this does not deter readability, yet assists in reducing execution time.
-
-For example, in the module shown previously (Module Fans), the parameters for fan types are set as Integers:
-
-  !MODULE PARAMETER DEFINITIONS
-
-INTEGER, PARAMETER :: FanType\_SimpleConstVolume = 1
-
-INTEGER, PARAMETER :: FanType\_SimpleVAV         = 2
-
-INTEGER, PARAMETER :: FanType\_SimpleOnOff       = 3
-
-INTEGER, PARAMETER :: FanType\_ZoneExhaust       = 4
-
-During the GetInput, string types are shown (this is getting these objects):
-
-        CALL GetObjectItem('FAN:SIMPLE:CONSTVOLUME',  &
-
-                           SimpFanNum,AlphArray, &
-
-                           NumAlphas,NumArray,NumNums,IOSTAT)
-
-        . . .
-
-        Fan(FanNum)%FanName = AlphArray(1)
-
-        Fan(FanNum)%FanType = 'SIMPLE'
-
-        . . .
-
-        Fan(FanNum)%Control = 'CONSTVOLUME'
-
-        Fan(FanNum)%FanType\_Num=FanType\_SimpleConstVolume
-
-Then, during the simulation the integer parameters are used:
-
-  ! Calculate the Correct Fan Model with the current FanNum
-
-  IF (Fan(FanNum)%FanType\_Num == FanType\_SimpleConstVolume) THEN
-
-    Call SimSimpleFan(FanNum)
-
-  Else IF (Fan(FanNum)%FanType\_Num == FanType\_SimpleVAV) THEN
-
-    Call SimVariableVolumeFan(FanNum)
-
-  Else If (Fan(FanNum)%FanType\_Num == FanType\_SimpleOnOff) THEN
-
-    Call SimOnOffFan(FanNum)
-
-  Else If (Fan(FanNum)%FanType\_Num == FanType\_ZoneExhaust) THEN
-
-    Call SimZoneExhaustFan(FanNum)
-
-  End If
-
-This does not detract from code readability at all but execution is much speedier with this versus the string comparisons.
-
-How it fits together
---------------------
-
-Although we have designed the EnergyPlus modules to be as independent as possible, obviously they cannot be completely independent.  How does an EnergyPlus HVAC module fit in with the rest of the program?  In the next section we examine and describe the calling structure of the program, with particular emphasis on HVAC/Plant elements.
-
-EnergyPlus Calling Structure
-============================
-
-Top Level Calling Tree
-----------------------
-
-EnergyPlus
-
-
-
-- ProcessInput (in InputProcessor)
-
-- ManageSimulation (in SimulationManager)
-
-- ManageWeather (in WeatherManager)
-
-- ManageHeatBalance (in HeatBalanceManager)
-
-- ManageSurfaceHeatBalance (in HeatBalanceSurfaceManager)
-
-- ManageAirHeatBalance (in HeatBalanceAirManager)
-
-- CalcHeatBalanceAir (in HeatBalanceAirManager)
-
-- ManageHVAC (in HVACManager)
-
-
-
-The HVAC part of EnergyPlus is divided into a number of simulation blocks.  At this point, there are blocks for the air system, the zone equipment, the plant equipment, and the on-site electrical equipment.  There will be simulation blocks for waste heat supply and usage as well as electricity and gas.  Within each HVAC time step, the blocks are simulated repeatedly until the conditions on each side of each block interface match up.  The following calling tree represents the high level HVAC simulation structure.  It is schematic – not all routines are shown.
-
-High Level HVAC Calling Tree (schematic – not all routines are shown)
----------------------------------------------------------------------
-
-ManageHVAC (in HVACManager)
-
-
-
-- ZoneAirUpdate(‘PREDICT’, . . .) (in HVACManager)
-
-*estimate the zone heating or cooling demand*
-
-* *
-
-- SimHVAC (in HVACManager)
-
-- ManageSetPoints (in SetPointManager)
-
-- SimSelectedEquipment (in HVACManager)
-
-- ManageAirLoops (in SimAirServingZones)
-
-- ManageZoneEquipment (in ZoneEquipmentManager)
-
-- ManageElectricLoadCenters (in ElectricPowerManager)
-
-- ManagePlantLoops (in PlantManager)
-
-
-
-- ZoneAirUpdate(‘CORRECT’, . . .) (in HVACManager)
-
-From the amount of heating and cooling actually provided by the HVAC system, calculate the zone temperatures.
-
-
-
-Each of the “Manage� routines has a different structure, since the simulation to be performed is different in each case.  We will show schematic calling trees for several of the “Manage� routines.
-
-Air System Calling Tree (schematic – not all routines are shown)
-----------------------------------------------------------------
-
-ManageAirLoops (in SimAirServingZones)
-
-
-
-- GetAirPathData  (in SimAirServingZones)
-
-- InitAirLoops (in SimAirServingZones)
-
-- SimAirLoops (in SimAirServingZones)
-
-- SimAirLoopComponent (in SimAirServingZones)
-
-- UpdateBranchConnections (in SimAirServingZones)
-
-- ManageOutsideAirSystem (in MixedAir)
-
-- SimOutsideAirSys (in MixedAir)
-
-- SimOAController (in MixedAir)
-
-- SimOAComponent (in Mixed Air)
-
-- SimOAMixer (in MixedAir)
-
-- SimulateFanComponents(in FanSimulation; file HVACFanComponent)
-
-- SimulateWaterCoilComponents (in WaterCoilSimulation; file HVACWaterCoilComponent)
-
-- SimHeatRecovery (in HeatRecovery)
-
-- SimDesiccantDehumidifier (in DesiccantDehumidifiers)
-
-- SimulateFanComponents (in FanSimulation; file HVACFanComponent)
-
-- SimulateWaterCoilComponents (in WaterCoilSimulation; file HVACWaterCoilComponent)
-
-- SimulateHeatingCoilComponents (in HeatingCoils; file HVACHeatingCoils)
-
-- SimDXCoolingSystem (in HVACDXSystem)
-
-- SimFurnace (in Furnaces; file HVACFurnace)
-
-- SimHumidifier (in Humidifiers)
-
-- SimEvapCooler (in EvaporativeCoolers; file HVACEvapComponent)
-
-- SimDesiccantDehumidifier (in DesiccantDehumidifiers)
-
-- SimHeatRecovery (in HeatRecovery)
-
-- ManageControllers (in Controllers)
-
-- GetControllerInput (in Controllers)
-
-- InitController (in Controllers)
-
-- SimpleController (in Controllers)
-
-- LimitController (in Controllers)
-
-- UpdateController (in Controllers)
-
-- Report Controller (in Controllers)
-
-- ResolveSysFlow (in SimAirServingZones)
-
-- UpdateHVACInterface (in HVACInterfaceManager)
-
-- ReportAirLoops (in SimAirServingZones)
-
-
-
-Plant Calling Tree (schematic – not all routines are shown)
------------------------------------------------------------
-
-ManagePlantLoops (in PlantManager)
-
-
-
-- PlantHalfLoopSolver (in PlantLoopSolver)
-
-- InitLoadDistribution (in PlantCondLoopOperation)
-
-- SetupLoopFlowRequest (in PlantLoopSolver)
-
-- SimulateAllLoopSidePumps (in PlantLoopSolver)
-
-- SimulateAllLoopSideBranches (in PlantLoopSolver)
-
-- ManagePlantLoadDistribution (in PlantCondLoopOperation)
-
-- SimPlantEquip (in PlantLoopEquipment)
-
-- Component simulation routines (in various component models)
-
-- UpdateAnyLoopDemandAlterations (in PlantLoopSolver)
-
-- SimPressureDropSystem (in PlantPressureSystem)
-
-- ResolveParallelFlows (in PlantLoopSolver)
-
-- SimulateAllLoopSideBranches (in PlantLoopSolver)
-
-- ManagePlantLoadDistribution (in PlantCondLoopOperation)
-
-- SimPlantEquip (in PlantLoopEquipment)
-
-- Component simulation routines (in various component models)
-
-- UpdateAnyLoopDemandAlterations (in PlantLoopSolver)
-
-- SimPressureDropSystem (in PlantPressureSystem)
-
-- UpdatePlantLoopInterface (in HVACInterfaceManager)
-
-
-
-Zone Equipment Calling Tree (schematic – not all routines are shown)
---------------------------------------------------------------------
-
-ManageZoneEquipment (in ZoneEquipmentManager)
-
-
-
-- GetZoneEquipment (in ZoneEquipmentManager)
-
-- InitZoneEquipment (in ZoneEquipmentManager)
-
-- SimZoneEquioment (in ZoneEquipmentManager)
-
-- SimAirLoopSplitter (in Splitters; file HVACSplitterComponent)
-
-- SimAirZonePlenum (in ZonePlenum; file ZonePlenumComponent)
-
-- SetZoneEquipSimOrder (in ZoneEquipmentManager)
-
-- InitSystemOutputRequired (in ZoneEquipmentManager)
-
-- ManageZoneAirLoopEquipment (in ZoneAirLoopEquipmentManager)
-
-- GetZoneAirLoopEquipment (in ZoneAirLoopEquipmentManager)
-
-- SimZoneAirLoopEquipment (in ZoneAirLoopEquipmentManager)
-
-- SimulateDualDuct (in DualDuct; file HVACDualDuctSystem)
-
-- GetDualDuctInput (in DualDuct; file HVACDualDuctSystem)
-
-- InitDualDuct (in DualDuct; file HVACDualDuctSystem)
-
-- SimDualDuctConstVol (in DualDuct; file HVACDualDuctSystem)
-
-- SimDualDuctVarVol (in DualDuct; file HVACDualDuctSystem)
-
-- UpdateDualDuct (in DualDuct; file HVACDualDuctSystem)
-
-- ReportDualDuct (in DualDuct; file HVACDualDuctSystem)
-
-- SimulateSingleDuct (in SingleDuct; file HVACSingleDuctSystem)
-
-- GetSysInput (in SingleDuct; file HVACSingleDuctSystem)
-
-- InitSys (in SingleDuct; file HVACSingleDuctSystem)
-
-- SimConstVol (in SingleDuct; file HVACSingleDuctSystem)
-
-- SimVAV (in SingleDuct; file HVACSingleDuctSystem)
-
-- ReportSys (in SingleDuct; file HVACSingleDuctSystem)
-
-- SimPIU (in PoweredInductionUnits)
-
-- GetPIUs (in PoweredInductionUnits)
-
-- InitPIUs (in PoweredInductionUnits)
-
-- CalcSeriesPIU (in PoweredInductionUnits)
-
-- CalcParallelPIU (in PoweredInductionUnits)
-
-- ReportPIU (in PoweredInductionUnits)
-
-- SimDirectAir (in DirectAirManager; file DirectAir)
-
-- SimPurchasedAir (in PurchasedAirManager)
-
-- SimWindowAC (in WindowAC)
-
-- SimFanCoilUnit (in FanCoilUnits)
-
-- SimUnitVentilator (in UnitVentilator)
-
-- SimUnitHeater (in UnitHeater)
-
-- SimBaseboard (in BaseboardRadiator)
-
-- SimHighTempRadiantSystem (in HighTempRadiantSystem; file RadiantSystemHighTemp)
-
-- SimLowTempRadiantSystem (in LowTempRadiantSystem; file RadiantSystemLowTemp)
-
-- SimulateFanComponents (in Fans; file HVACFanComponent)
-
-- SimHeatRecovery (in HeatRecovery)
-
-- UpdateSystemOutputRequired (in ZoneEquipmentManager)
-
-- SimAirLoopSplitter (in Splitters; file HVACSplitterComponent)
-
-- SimAirZonePlenum (in ZonePlenum; file ZonePlenumComponent)
-
-- CalcZoneMassBalance (in ZoneEquipmentManager)
-
-- CalcZoneLeavingConditions (in ZoneEquipmentManager)
-
-- SimReturnAirPath (in ReturnAirPathManager; file ReturnAirPath)
-
-- SimAirMixer (in Mixers; HVACMixerComponent)
-
-- SimAirZonePlenum (in ZonePlenum; file ZonePlenumComponent)
-
-- RecordZoneEquipment (in ZoneEquipmentManager)
-
-- ReportZoneEquipment (in ZoneEquipmentManager)
-
-Inserting the New Module into the Program
------------------------------------------
-
-Let us return to our example new module NewHVACComponent.  Since the module gets its own input and output, adding the NewHVACComponent model to the program simply means adding a call to the driver routine SimNewHVACComponent from the correct place in EnergyPlus.  In the simplest case, there is only one location from which the driver routine should be called. In some cases, though, more than one HVAC simulation block will need to use the new component model.  SimulateWaterCoilComponents, for instance, can be used in both zone equipment and air systems for heating, reheating and cooling coils. In the air system simulation it is called from two places: the main air system simulation, and the mixed air simulation – the outside air duct might contain a separate cooling coil.
-
-Let us assume that the NewHVACComponent will be part of the air system – perhaps it is a solid desiccant wheel.  Examining the air system calling tree we see that SimAirLoopComponent is one routine that will invoke the new component, and - if we want the component to possibly be in the outside air stream – then SimOAComponent is the other routine that will need to call the new component simulation. Generally, all that is involved is adding a new CASE statement to a Fortran SELECT construct.  For instance in SimAirLoopComponent this would look like:
-
-SELECT CASE(CompType\_Num)
-
-
-
-  CASE(OAMixer\_Num)  ! 'OUTSIDE AIR SYSTEM'
-
-    CALL ManageOutsideAirSystem( …)
-
-
-
-! Fan Types for the air sys simulation
-
-  CASE(Fan\_Simple\_CV)  ! 'FAN:SIMPLE:CONSTVOLUME'
-
-    CALL SimulateFanComponents(…)
-
-
-
-  CASE(Fan\_Simple\_VAV)  ! 'FAN:SIMPLE:VARIABLEVOLUME'
-
-    CALL SimulateFanComponents(…)
-
-
-
-! Coil Types for the air sys simulation
-
-!                         'COIL:DX:COOLINGHEATEXCHANGERASSISTED'
-
-  CASE(DXCoil\_CoolingHXAsst)
-
-      CALL SimHXAssistedCoolingCoil(…)
-
-!                         'COIL:WATER:COOLINGHEATEXCHANGERASSISTED'  CASE(WaterCoil\_CoolingHXAsst)
-
-    CALL SimHXAssistedCoolingCoil(…)
-
-  CASE(WaterCoil\_SimpleHeat)  ! 'COIL:WATER:SIMPLEHEATING'
-
-    CALL SimulateWaterCoilComponents(…)
-
-  CASE(SteamCoil\_AirHeat)  ! 'COIL:STEAM:AIRHEATING'
-
-    CALL SimulateSteamCoilComponents(…)
-
-  CASE(WaterCoil\_DetailedCool)  ! 'COIL:WATER:DETAILEDFLATCOOLING'
-
-    CALL SimulateWaterCoilComponents(…)
-
-  CASE(WaterCoil\_Cooling)  ! 'COIL:WATER:COOLING'
-
-    CALL SimulateWaterCoilComponents(…)
-
-  CASE(Coil\_ElectricHeat)  ! 'COIL:ELECTRIC:HEATING'
-
-    CALL SimulateHeatingCoilComponents(…)
-
-  CASE(Coil\_GasHeat)  ! 'COIL:GAS:HEATING'
-
-    CALL SimulateHeatingCoilComponents(…)
-
-! Heat reclaim
-
-  CASE(Coil\_DeSuperHeat)  ! 'COIL:DESUPERHEATER:HEATING'
-
-    CALL SimulateHeatingCoilComponents(…)
-
-
-
-  CASE(DXSystem)  ! 'DXSYSTEM:AIRLOOP'
-
-    CALL SimDXCoolingSystem(…)
-
-
-
-
-
-  CASE(Furnace\_UnitarySys)  ! 'FURNACE:BLOWTHRU:HEATONLY',
-
-                            ! 'FURNACE:BLOWTHRU:HEATCOOL',
-
-                            ! 'UNITARYSYSTEM:BLOWTHRU:HEATONLY',
-
-                            ! 'UNITARYSYSTEM:BLOWTHRU:HEATCOOL'
-
-                            ! 'UNITARYSYSTEM:HEATPUMP:AIRTOAIR',
-
-                            ! 'UNITARYSYSTEM:HEATPUMP:WATERTOAIR'
-
-    CALL SimFurnace(…)
-
-
-
-! Humidifier Types for the air system simulation
-
-  CASE(Humidifier)  ! 'HUMIDIFIER:STEAM:ELECTRICAL'
-
-    CALL SimHumidifier(…)
-
-
-
-! Evap Cooler Types for the air system simulation
-
-  CASE(EvapCooler)  ! 'EVAPCOOLER:DIRECT:CELDEKPAD',
-
-                    ! 'EVAPCOOLER:INDIRECT:CELDEKPAD'
-
-                    ! 'EVAPCOOLER:INDIRECT:WETCOIL',
-
-                    ! 'EVAPCOOLER:INDIRECT:RDDSPECIAL'
-
-    CALL SimEvapCooler(…)
-
-
-
-! Desiccant Dehumidifier Types for the air system simulation
-
-  CASE(Desiccant)  ! 'DESICCANT DEHUMIDIFIER:SOLID'
-
-    CALL SimDesiccantDehumidifier(…)
-
-
-
-! Heat recovery
-
-  CASE(HeatXchngr)  ! 'HEAT EXCHANGER:AIR TO AIR:FLAT PLATE'
-
-    CALL SimHeatRecovery(…)
-
-
-
-! Ducts
-
-  CASE(Duct)  ! 'DUCT'
-
-    CALL SimDuct(…)
-
-
-
-*! New HVAC Component*
-
-*  CASE (NewHVACCompNum) ! ‘NEW HVAC COMPONENT’*
-
-*    CALL SimNewHVACComponent(…)*
-
-
-
-  DEFAULT
-
-
-
-END SELECT
-
-
-
-The new code is italicized.  Do the same thing in SimOAComponent and you are done!  Note that “NEW HVAC COMPONENT� is the class name (keyword) for the new component in the IDD file.  The class names are converted to upper case in EnergyPlus, so the CASE statement must have the class name in upper case.  The actual class name on the IDD file would probably be “New HVAC Component�.
-
-If the new HVAC component is a piece of zone equipment – a cooled beam system, for instance – then the zone equipment calling tree indicates that the call to SimNewHVACComponent would be in SimZoneEquipment. If the new component is a gas fired absorption chiller, the call would be in SimPlantEquip.
-
-In every case, since NewHVACComponent is a new module, a USE statement must be added to the calling subroutine. For instance in SimAirLoopComponent this would look like:
-
-SUBROUTINE SimAirLoopComponent(CompType, CompName, FirstHVACIteration, LastSim)
-
-
-
-          ! SUBROUTINE INFORMATION
-
-          !             AUTHOR:  Russ Taylor, Dan Fisher, Fred Buhl
-
-          !       DATE WRITTEN:  Oct 1997
-
-          !           MODIFIED:  Dec 1997 Fred Buhl
-
-          !      RE-ENGINEERED:  This is new code, not reengineered
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! Calls the individual air loop component simulation routines
-
-
-
-          ! METHODOLOGY EMPLOYED: None
-
-
-
-          ! REFERENCES: None
-
-
-
-          ! USE Statements
-
-  USE Fans,       Only:SimulateFanComponents
-
-  USE WaterCoils, Only:SimulateWaterCoilComponents
-
-  USE MixedAir,   Only:ManageOutsideAirSystem
-
-  *USE NewHVACComponent,    Only:SimNewHVACComponent*
-
-HVAC Network
-============
-
-Branches, Connectors, and Nodes
--------------------------------
-
-In EnergyPlus, the HVAC system and plant form a network (technically, a graph). The individual pieces of equipment – the fans, coils, chillers, etc. – are connected together by air ducts and fluid pipes. In EnergyPlus nomenclature, the air and fluid circuits are called loops. Specifying how an individual system and plant are connected is done in the EnergyPlus input (IDF) file. The overall structure of the network is defined with Branch and Connector objects. The detail is filled with components and their inlet and outlet nodes. A Branch consists of one or more components arranged sequentially along a pipe or duct. A Connector specifies how three or more branches are connected through a Splitter or Mixer. Nodes connect components along a branch: the outlet node of one component is the inlet node of the next downstream component. The nodes represent conditions at a point on a loop. Each component has one or more inlet and outlet nodes, depending on how many loops it interacts with. A fan, for instance, has one inlet node and one outlet node, since it interacts with a single air loop. A water coil will have 2 inlet and 2 outlet nodes, since it interacts with an air and a fluid loop. Figure 1 shows a diagram of an EnergyPlus HVAC input.
-
-![](media/image002.png)
-
-Figure 1.  HVAC Input Diagram
-
-As an illustration of how such a network is built up on the IDF, here is the section of the IDF that describes the supply fan, splitter, and heating and cooling coil section of the dual duct air system.
-
-
-
-**BranchList,**
-
-    Dual Duct Air Loop Branches,  !- Name
-
-    Air Loop Main Branch,    !- Branch 1 Name
-
-    Heating Coil Air Sys Branch,  !- Branch 2 Name
-
-    Cooling Coil Air Sys Branch;  !- Branch 3 Name
-
-
-
-**ConnectorList,**
-
-    Dual Duct Connectors,    !- Name
-
-    Connector:Splitter,      !- Connector 1 Object Type
-
-    DualDuctAirSplitter;     !- Connector 1 Name
-
-
-
-**NodeList,**
-
-    Zone Equipment Inlet Node List,  !- Name
-
-    Main Hot Air Inlet,      !- Node 1 Name
-
-    Main Cold Air Inlet;     !- Node 2 Name
-
-
-
-**NodeList,**
-
-    Air Loop Outlet Node List,  !- Name
-
-    Heating Coil Outlet Node,!- Node 1 Name
-
-    Cooling Coil Outlet Node;!- Node 2 Name
-
-
-
-**Branch,**
-
-    Air Loop Main Branch,    !- Name
-
-    autosize,                !- Maximum Flow Rate {m3/s}
-
-    Fan:ConstantVolume,      !- Component 1 Object Type
-
-    Supply Fan 1,            !- Component 1 Name
-
-    Supply Fan Inlet Node,   !- Component 1 Inlet Node Name
-
-    Supply Fan Outlet Node,  !- Component 1 Outlet Node Name
-
-    PASSIVE;                 !- Component 1 Branch Control Type
-
-
-
-**Branch,**
-
-    Heating Coil Air Sys Branch,  !- Name
-
-    autosize,                !- Maximum Flow Rate {m3/s}
-
-    Coil:Heating:Water,      !- Component 1 Object Type
-
-    Main Heating Coil,       !- Component 1 Name
-
-    Heating Coil Inlet Node, !- Component 1 Inlet Node Name
-
-    Heating Coil Outlet Node,!- Component 1 Outlet Node Name
-
-    ACTIVE;                  !- Component 1 Branch Control Type
-
-
-
-**Branch,**
-
-    Cooling Coil Air Sys Branch,  !- Name
-
-    autosize,                !- Maximum Flow Rate {m3/s}
-
-    Coil:Cooling:Water,      !- Component 1 Object Type
-
-    Simple Cooling Coil,     !- Component 1 Name
-
-    Cooling Coil Inlet Node, !- Component 1 Inlet Node Name
-
-    Cooling Coil Outlet Node,!- Component 1 Outlet Node Name
-
-    ACTIVE;                  !- Component 1 Branch Control Type
-
-
-
-**Connector:Splitter,**
-
-    DualDuctAirSplitter,     !- Name
-
-    Air Loop Main Branch,    !- Inlet Branch Name
-
-    Heating Coil Air Sys Branch,  !- Outlet Branch 1 Name
-
-    Cooling Coil Air Sys Branch;  !- Outlet Branch 2 Name
-
-
-
-**Fan:ConstantVolume,**
-
-    Supply Fan 1,            !- Name
-
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-
-    0.7,                     !- Fan Efficiency
-
-    600.0,                   !- Pressure Rise {Pa}
-
-    autosize,                !- Maximum Flow Rate {m3/s}
-
-    0.9,                     !- Motor Efficiency
-
-    1.0,                     !- Motor In Airstream Fraction
-
-    Supply Fan Inlet Node,   !- Fan Inlet Node Name
-
-    Supply Fan Outlet Node;  !- Fan Outlet Node Name
-
-
-
-**Coil:Cooling:Water,**
-
-    Simple Cooling Coil,     !- Name
-
-    CoolingCoilAvailSched,   !- Availability Schedule Name
-
-    autosize,                !- Design Water Flow Rate {m3/s}
-
-    autosize,                !- Design Air Flow Rate {m3/s}
-
-    autosize,         !- Design Inlet Water Temperature {C}
-
-    autosize,         !- Design Inlet Air Temperature {C}
-
-    autosize,         !- Design Outlet Air Temperature {C}
-
-    autosize,     !- Design Inlet Air Humidity Ratio {kg-H2O/kg-air}
-
-    autosize,     !- Design Outlet Air Humidity Ratio {kg-H2O/kg-air}
-
-    Cooling Coil Water Inlet Node,  !- Water Inlet Node Name
-
-    Cooling Coil Water Outlet Node,  !- Water Outlet Node Name
-
-    Cooling Coil Inlet Node, !- Air Inlet Node Name
-
-    Cooling Coil Outlet Node,!- Air Outlet Node Name
-
-    SimpleAnalysis,          !- Type of Analysis
-
-    CrossFlow;               !- Heat Exchanger Configuration
-
-
-
-**AirLoopHVAC:ZoneSplitter,**
-
-    ZoneColdAirSupplySplitter,  !- Name
-
-    Main Cold Air Inlet,     !- Inlet Node Name
-
-    Zone 1 Dual Duct Cold Inlet,  !- Outlet 1 Node Name
-
-    Zone 2 Dual Duct Cold Inlet,  !- Outlet 2 Node Name
-
-    Zone 3 Dual Duct Cold Inlet;  !- Outlet 3 Node Name
-
-
-
-**AirLoopHVAC:ZoneSplitter,**
-
-    ZoneHotAirSupplySplitter,!- Name
-
-    Main Hot Air Inlet,      !- Inlet Node Name
-
-    Zone 1 Dual Duct Hot Inlet,  !- Outlet 1 Node Name
-
-    Zone 2 Dual Duct Hot Inlet,  !- Outlet 2 Node Name
-
-    Zone 3 Dual Duct Hot Inlet;  !- Outlet 3 Node Name
-
-
-
-**AirLoopHVAC:ZoneMixer,**
-
-    ZoneReturnAirMixer,      !- Name
-
-    Return Air Mixer Outlet, !- Outlet Node Name
-
-    Zone 1 Outlet Node,      !- Inlet 1 Node Name
-
-    Zone 2 Outlet Node,      !- Inlet 2 Node Name
-
-    Zone 3 Outlet Node;      !- Inlet 3 Node Name
-
-
-
-**Coil:Heating:Water,**
-
-    Main Heating Coil,       !- Name
-
-    FanAndCoilAvailSched,    !- Availability Schedule Name
-
-    autosize,                !- U-Factor Times Area Value {W/K}
-
-    autosize,                !- Maximum Water Flow Rate {m3/s}
-
-    Heating Coil Water Inlet,!- Water Inlet Node Name
-
-    Heating Coil Water Outlet,  !- Water Outlet Node Name
-
-    Heating Coil Inlet Node, !- Air Inlet Node Name
-
-    Heating Coil Outlet Node,!- Air Outlet Node Name
-
-    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method
-
-    autosize,                !- Nominal Capacity {W}
-
-    82.2,                    !- Design Inlet Water Temperature {C}
-
-    16.6,                    !- Design Inlet Air Temperature {C}
-
-    71.1,                    !- Design Outlet Water Temperature {C}
-
-    32.2;                    !- Design Outlet Air Temperature {C}
-
-
-
-**Controller:WaterCoil,**
-
-    Main Cooling Coil Controller,  !- Name
-
-    Temperature,             !- Control Variable
-
-    Reverse,                 !- Action
-
-    FLOW,                    !- Actuator Variable
-
-    Cooling Coil Outlet Node,!- Sensor Node Name
-
-    Cooling Coil Water Inlet Node,  !- Actuator Node Name
-
-    0.001,             !- Controller Convergence Tolerance {deltaC}
-
-    autosize,                !- Maximum Actuated Flow {m3/s}
-
-    0.0;                     !- Minimum Actuated Flow {m3/s}
-
-
-
-**Controller:WaterCoil,**
-
-    Main Heating Coil Controller,  !- Name
-
-    Temperature,             !- Control Variable
-
-    Normal,                  !- Action
-
-    FLOW,                    !- Actuator Variable
-
-    Heating Coil Outlet Node,!- Sensor Node Name
-
-    Heating Coil Water Inlet,!- Actuator Node Name
-
-    0.01,              !- Controller Convergence Tolerance {deltaC}
-
-    autosize,                !- Maximum Actuated Flow {m3/s}
-
-    0.0;                     !- Minimum Actuated Flow {m3/s}
-
-Obviously, the creation of such a system/plant network description is best handled by a graphical user interface (GUI). However, for testing purposes a developer may have to create the input for a component by hand and insert it into an existing IDF. Then the developer must be careful to choose unique names for the branches and nodes and make sure the entire network makes physical sense.
-
-Nodes in the simulation
------------------------
-
-In the EnergyPlus data structure, the nodes are where each component model gets its input and where it places its output. The module *DataLoopNode* contains all the node related data. In particular, the array *Node* contains the state variables and mass flows for all the nodes in the problem being simulated.
-
-  ! Valid Fluid Types for Nodes
-
-  INTEGER, PARAMETER :: NodeType\_Unknown = 0  ! 'blank'
-
-  INTEGER, PARAMETER :: NodeType\_Air     = 1  ! 'Air'
-
-  INTEGER, PARAMETER :: NodeType\_Water   = 2  ! 'Water'
-
-  INTEGER, PARAMETER :: NodeType\_Steam   = 3  ! 'Steam'
-
-  INTEGER, PARAMETER :: NodeType\_Electric= 4  ! 'Electric'
-
-
-
- **TYPE** NodeData
-
-   **INTEGER**  :: FluidType                 = 0   ! must be one of the valid parameters
-
-   **INTEGER**  :: FluidIndex                = 0   ! For Fluid Properties
-
-   REAL(r64)     :: Temp                      = 0.d0 ! {C}
-
-   REAL(r64)     :: TempMin                   = 0.d0 ! {C}
-
-   REAL(r64)     :: TempMax                   = 0.d0 ! {C}
-
-   REAL(r64)     :: TempSetPoint              = SensedNodeFlagValue ! {C}
-
-   REAL(r64)     :: TempLastTimestep          = 0.d0 ! [C}   DSU
-
-   REAL(r64)     :: MassFlowRateRequest       = 0.d0 ! {kg/s}  DSU
-
-   REAL(r64)     :: MassFlowRate              = 0.d0 ! {kg/s}
-
-   REAL(r64)     :: MassFlowRateMin           = 0.d0 ! {kg/s}
-
-   REAL(r64)     :: MassFlowRateMax           = SensedNodeFlagValue ! {kg/s}
-
-   REAL(r64)     :: MassFlowRateMinAvail      = 0.d0 ! {kg/s}
-
-   REAL(r64)     :: MassFlowRateMaxAvail      = 0.d0 ! {kg/s}
-
-   REAL(r64)     :: MassFlowRateSetPoint      = 0.d0 ! {kg/s}
-
-   REAL(r64)     :: Quality                   = 0.d0 ! {0.0-1.0 vapor fraction/percent}
-
-   REAL(r64)     :: Press                     = 0.d0 ! {Pa}
-
-   REAL(r64)     :: Enthalpy                  = 0.d0 ! {J/kg}
-
-   REAL(r64)     :: EnthalpyLastTimestep      = 0.d0 ! {J/kg}  DSU for steam?
-
-   REAL(r64)     :: HumRat                    = 0.d0 ! {}
-
-   REAL(r64)     :: HumRatMin                 = SensedNodeFlagValue ! {}
-
-   REAL(r64)     :: HumRatMax                 = SensedNodeFlagValue ! {}
-
-   REAL(r64)     :: HumRatSetPoint            = SensedNodeFlagValue ! {}
-
-   REAL(r64)     :: TempSetPointHi            = SensedNodeFlagValue ! {C}
-
-   REAL(r64)     :: TempSetPointLo            = SensedNodeFlagValue ! {C}
-
-   REAL(r64)     :: Height                    = -1.d0 !  {m}
-
-   !  Following are for Outdoor Air Nodes "read only"
-
-   REAL(r64)     :: OutAirDryBulb             = 0.d0 ! {C}
-
-   **LOGICAL**       :: EMSOverrideOutAirDryBulb  = .FALSE. ! if true, the EMS is calling to override outdoor air node drybulb setting
-
-   REAL(r64)     :: EMSValueForOutAirDryBulb  = 0.d0 ! value EMS is directing to use for outdoor air node's drybulb {C}
-
-   REAL(r64)     :: OutAirWetBulb             = 0.d0 ! {C}
-
-   **LOGICAL**       :: EMSOverrideOutAirWetBulb  = .FALSE. ! if true, the EMS is calling to override outdoor air node wetbulb setting
-
-   REAL(r64)     :: EMSValueForOutAirWetBulb  = 0.d0 ! value EMS is directing to use for outdoor air node's wetbulb {C}
-
-   ! Contaminant
-
-   REAL(r64)     :: CO2                       = 0.d0 ! {ppm}
-
-   REAL(r64)     :: CO2SetPoint               = 0.d0 ! {ppm}
-
- **END** **TYPE** NodeData
-
-
-
-**TYPE** MoreNodeData
-
-   REAL(r64)     :: RelHumidity               = 0.d0 ! {%}
-
-   REAL(r64)     :: ReportEnthalpy            = 0.d0 ! specific enthalpy calculated at the HVAC timestep [J/kg]
-
-   REAL(r64)     :: VolFlowRateStdRho         = 0.d0 ! volume flow rate at standard density [m3/s]
-
-   REAL(r64)     :: VolFlowRateCrntRho        = 0.d0 ! volume flow rate at current density, only used for air nodes [m3/s]
-
-   REAL(r64)     :: WetbulbTemp               = 0.d0 ! wetbulb temperature [C]
-
-   REAL(r64)     :: AirDensity                = 0.d0 ! reported air density at standard density [kg/m3]
-
- **END** **TYPE** MoreNodeData
-
-**TYPE** (NodeData), **ALLOCATABLE**, **DIMENSION**(:) :: Node !dim to num nodes in SimHVAC
-
- **TYPE** (NodeData) :: DefaultNodeValues=  &
-
-     NodeData(0,          & ! FluidType
-
-              0,          & ! FluidIndex
-
-              0.0D0,        & ! Temp {C}
-
-              0.0D0,        & ! TempMin {C}
-
-              0.0D0,        & ! TempMax {C}
-
-     SensedNodeFlagValue,   & ! TempSetPoint {C}
-
-              0.0D0,        & ! TempLastTimeStep {C}
-
-              0.0D0,        & ! MassFlowRateRequest {kg/s}
-
-              0.0D0,        & ! MassFlowRate {kg/s}
-
-              0.0D0,        & ! MassFlowRateMin {kg/s}
-
-              0.0D0,        & ! MassFlowRateMax {kg/s}
-
-              0.0D0,        & ! MassFlowRateMinAvail {kg/s}
-
-              0.0D0,        & ! MassFlowRateMaxAvail {kg/s}
-
-              0.0D0,        & ! MassFlowRateSetPoint {kg/s}
-
-              0.0D0,        & ! Quality {0.0-1.0 vapor fraction/percent}
-
-              0.0D0,        & ! Press {Pa}   REAL(r64)     ::
-
-              0.0D0,        & ! Enthalpy {J/kg}
-
-              0.0D0,        & ! EnthalpyLastTimeStep {J/kg}
-
-              0.0D0,        & ! HumRat {}
-
-     SensedNodeFlagValue,   & ! HumRatMin {}
-
-     SensedNodeFlagValue,   & ! HumRatMax {}
-
-     SensedNodeFlagValue,   & ! HumRatSetPoint {}
-
-     SensedNodeFlagValue,   & ! TempSetPointHi {C}
-
-     SensedNodeFlagValue,   & ! TempSetPointLo {C}
-
-             -1.0D0,        & ! Height {m}
-
-              0.0D0,        & ! OutAirDryBulb {C}
-
-              .FALSE.,      & ! EMSOverrideOutAirDryBulb
-
-              0.0D0,        & ! EMSValueForOutAirDryBulb {C}
-
-              0.0D0,          & ! OutAirWetBulb {C}
-
-              .FALSE.,      & ! EMSOverrideOutAirWetBulb
-
-              0.0D0,        & ! EMSValueForOutAirWetBulb {C}
-
-              0.0D0,        & ! CO2 {ppm}
-
-              0.0D0)          ! CO2 setpoint {ppm}
-
- TYPE (MoreNodeData), ALLOCATABLE, DIMENSION(:) :: MoreNodeInfo
-
-In our example module *NewHVACComponent,* the subroutine *InitNewHVACComponent* is responsible for obtaining the input data from the inlet node(s) and putting it into the component data structure for use in C*alcNewHVACComponent*. Then *UpdateNewHVACComponent* takes the calculated data and moves it to the outlet nodes for use by other components. EnergyPlus component models are assumed to be direct models: inlets are input to the calculation and outlets are output from the calculations.
-
-Getting Nodes
--------------
-
-Data Flow in an HVAC Component Module
--------------------------------------
-
-The data in an EnergyPlus HVAC component module resides in three places.
-
-1.   The component inlet nodes – this is where the data input to the model resides.
-
-2.   The component internal data structure(s) – one or more arrays of data structures which contain all the data needed for the component simulation. This includes data from the input file, data from the inlet nodes, and any schedule values. In addition, these data structure(s) store the results of the calculation.
-
-3.   The component outlet nodes – data is moved from the internal data structure(s) to the outlet nodes at the completion of each component simulation.
-
-The data flows from the inlet nodes into the component internal data structure(s) and then into the outlet nodes. Let us see how this works in our example module Fans.
-
-At the start of the module, the component internal data structure is defined.
-
-TYPE FanEquipConditions
-
-  CHARACTER(len=MaxNameLength) :: FanName  ! Name of the fan
-
-  CHARACTER(len=MaxNameLength) :: FanType  ! Type of Fan ie. Simple, Vane axial, Centrifugal, etc.
-
-  CHARACTER(len=MaxNameLength) :: Schedule ! Fan Operation Schedule
-
-  CHARACTER(len=MaxNameLength) :: Control  ! ie. Const Vol, Variable Vol
-
-  Integer      :: SchedPtr ! Pointer to the correct schedule
-
-  REAL(r64)    :: InletAirMassFlowRate  !MassFlow through the Fan being Simulated [kg/Sec]
-
-  REAL(r64)    :: OutletAirMassFlowRate
-
-  REAL(r64)    :: MaxAirFlowRate  !Max Specified Volume Flow Rate of Fan [m^3/sec]
-
-  REAL(r64)    :: MinAirFlowRate  !Min Specified Volume Flow Rate of Fan [m^3/sec]
-
-  REAL(r64)    :: MaxAirMassFlowRate ! Max flow rate of fan in kg/sec
-
-  REAL(r64)    :: MinAirMassFlowRate ! Min flow rate of fan in kg/sec
-
-  REAL(r64)    :: InletAirTemp
-
-  REAL(r64)    :: OutletAirTemp
-
-  REAL(r64)    :: InletAirHumRat
-
-  REAL(r64)    :: OutletAirHumRat
-
-  REAL(r64)    :: InletAirEnthalpy
-
-  REAL(r64)    :: OutletAirEnthalpy
-
-  REAL(r64)    :: FanPower             !Power of the Fan being Simulated [kW]
-
-  REAL(r64)    :: FanEnergy            !Fan energy in [kJ]
-
-  REAL(r64)    :: DeltaTemp            !Temp Rise across the Fan [C]
-
-  REAL(r64)    :: DeltaPress           !Delta Pressure Across the Fan [N/M^2]
-
-  REAL(r64)    :: FanEff               !Fan total efficiency; motor and mechanical
-
-  REAL(r64)    :: MotEff               !Fan motor efficiency
-
-  REAL(r64)    :: MotInAirFrac         !Fraction of motor heat entering air stream
-
-  REAL(r64), Dimension(5):: FanCoeff        !Fan Part Load Coefficients to match fan type
-
-  ! Mass Flow Rate Control Variables
-
-  REAL(r64)    :: MassFlowRateMaxAvail
-
-  REAL(r64)    :: MassFlowRateMinAvail
-
-  INTEGER      :: InletNodeNum
-
-  INTEGER      :: OutletNodeNum
-  END TYPE FanEquipConditions
-
- !MODULE VARIABLE DECLARATIONS:
-
-  INTEGER :: NumFans     ! The Number of Fans found in the Input
-
-  TYPE (FanEquipConditions), ALLOCATABLE, DIMENSION(:) :: Fan
-
-
-
-In this case, there is only one structure that stores all of the fan data. We could have chosen to divide this rather large structure up into separate structures – one for input file data, one for inlet data, and one for outlet data, for instance. Note that in Fortran 90 structures are called defined type.  The TYPE – END TYPE construct defines a new data structure. Then an allocatable array *Fan* of the defined type is created. This one-dimensional array will contain an entry for each fan in the problem.
-
-The internal data array is allocated (sized) in the “GetInput� routine GetFanInput.
-
-NumSimpFan   = GetNumObjectsFound('FAN:SIMPLE:CONSTVOLUME')
-
-    NumVarVolFan = GetNumObjectsFound('FAN:SIMPLE:VARIABLEVOLUME')
-
-    NumOnOff = GetNumObjectsFound('FAN:SIMPLE:ONOFF')
-
-    NumZoneExhFan = GetNumObjectsFound('ZONE EXHAUST FAN')
-
-    NumFans = NumSimpFan + NumVarVolFan + NumZoneExhFan+NumOnOff
-
-    IF (NumFans.GT.0) ALLOCATE(Fan(NumFans))
-
-
-
-The remainder of the “GetInput� routine moves input file data into the Fan array. The “Init� routine transfers data from the inlet nodes into the same array in preparation for performing the calculation.
-
-  ! Load the node data in this section for the component simulation
-
-  !
-
-  !First need to make sure that the massflowrate is between the max and min avail.
-
-  IF (Fan(FanNum)%FanType\_Num /= FanType\_ZoneExhaust ) THEN
-
-    Fan(FanNum)%InletAirMassFlowRate = Min(Node(InletNode)%MassFlowRate, &
-
-                                           Fan(FanNum)%MassFlowRateMaxAvail)
-
-    Fan(FanNum)%InletAirMassFlowRate = Max(Fan(FanNum)%InletAirMassFlowRate, &
-
-                                           Fan(FanNum)%MassFlowRateMinAvail)
-
-  ELSE  ! zone exhaust fans - always run at the max
-
-    Fan(FanNum)%MassFlowRateMaxAvail = Fan(FanNum)%MaxAirMassFlowRate
-
-    Fan(FanNum)%MassFlowRateMinAvail = 0.0
-
-    Fan(FanNum)%InletAirMassFlowRate = Fan(FanNum)%MassFlowRateMaxAvail
-
-    IF (Fan(FanNum)%EMSMaxMassFlowOverrideOn) Fan(FanNum)%InletAirMassFlowRate = &
-
-       MIN(Fan(FanNum)%EMSAirMassFlowValue,Fan(FanNum)%MassFlowRateMaxAvail)
-
-  END IF
-
-
-
-  !Then set the other conditions
-
-  Fan(FanNum)%InletAirTemp         = Node(InletNode)%Temp
-
-  Fan(FanNum)%InletAirHumRat       = Node(InletNode)%HumRat
-
-  Fan(FanNum)%InletAirEnthalpy     = Node(InletNode)%Enthalpy
-
-
-
-The “Calc� routines do the actual component simulation. All the data they need has been stored in the internal data array ready to be used. The results of the calculation are, in this case, stored in the same array. The “Calc� routine always does pure calculation/simulation – it never retrieves or stores data.
-
-DeltaPress = Fan(FanNum)%DeltaPress
-
-   FanEff     = Fan(FanNum)%FanEff
-
-
-
-   ! For a Constant Volume Simple Fan the Max Flow Rate is the Flow Rate for the fan
-
-   Tin        = Fan(FanNum)%InletAirTemp
-
-   Win        = Fan(FanNum)%InletAirHumRat
-
-   RhoAir     = Fan(FanNum)%RhoAirStdInit
-
-   MassFlow   = MIN(Fan(FanNum)%InletAirMassFlowRate,Fan(FanNum)%MaxAirMassFlowRate)
-
-   MassFlow   = MAX(MassFlow,Fan(FanNum)%MinAirMassFlowRate)
-
-   !
-
-   !Determine the Fan Schedule for the Time step
-
-  If( ( GetCurrentScheduleValue(Fan(FanNum)%SchedPtr)&gt;0.0 .and. Massflow&gt;0.0 .or. TurnFansOn .and. Massflow&gt;0.0) &
-
-        .and. .NOT.TurnFansOff ) Then
-
-   !Fan is operating
-
-   Fan(FanNum)%FanPower = MassFlow\*DeltaPress/(FanEff\*RhoAir) ! total fan power
-
-   FanShaftPower = Fan(FanNum)%MotEff \* Fan(FanNum)%FanPower  ! power delivered to shaft
-
-   PowerLossToAir = FanShaftPower + (Fan(FanNum)%FanPower - FanShaftPower) \* &
-
-     Fan(FanNum)%MotInAirFrac
-
-   Fan(FanNum)%OutletAirEnthalpy = Fan(FanNum)%InletAirEnthalpy + PowerLossToAir/MassFlow
-
-   ! This fan does not change the moisture or Mass Flow across the component
-
-   Fan(FanNum)%OutletAirHumRat       = Fan(FanNum)%InletAirHumRat
-
-   Fan(FanNum)%OutletAirMassFlowRate = MassFlow
-
-   Fan(FanNum)%OutletAirTemp = PsyTdbFnHW (Fan(FanNum)%OutletAirEnthalpy,Fan(FanNum)%OutletAirHumRat)
-
-
-
- Else
-
-   !Fan is off and not operating no power consumed and mass flow rate.
-
-   Fan(FanNum)%FanPower = 0.0
-
-   FanShaftPower = 0.0
-
-   PowerLossToAir = 0.0
-
-   Fan(FanNum)%OutletAirMassFlowRate = 0.0
-
-   Fan(FanNum)%OutletAirHumRat       = Fan(FanNum)%InletAirHumRat
-
-   Fan(FanNum)%OutletAirEnthalpy     = Fan(FanNum)%InletAirEnthalpy
-
-   Fan(FanNum)%OutletAirTemp = Fan(FanNum)%InletAirTemp
-
-   ! Set the Control Flow variables to 0.0 flow when OFF.
-
-   Fan(FanNum)%MassFlowRateMaxAvail = 0.0
-
-   Fan(FanNum)%MassFlowRateMinAvail = 0.0
-
-   End If
-
-
-
-Finally, the “Update� routine (UpdateFan) moves the results from the internal data array into the outlet node(s).
-
-   OutletNode = Fan(FanNum)%OutletNodeNum
-
-   InletNode = Fan(FanNum)%InletNodeNum
-
-
-
-   ! Set the outlet air nodes of the fan
-
-   Node(OutletNode)%MassFlowRate  = Fan(FanNum)%OutletAirMassFlowRate
-
-   Node(OutletNode)%Temp          = Fan(FanNum)%OutletAirTemp
-
-   Node(OutletNode)%HumRat        = Fan(FanNum)%OutletAirHumRat
-
-   Node(OutletNode)%Enthalpy      = Fan(FanNum)%OutletAirEnthalpy
-
-   ! Set the outlet nodes for properties that just pass through & not used
-
-   Node(OutletNode)%Quality         = Node(InletNode)%Quality
-
-   Node(OutletNode)%Press           = Node(InletNode)%Press
-
-
-
-   ! Set the Node Flow Control Variables from the Fan Control Variables
-
-   Node(OutletNode)%MassFlowRateMaxAvail = Fan(FanNum)%MassFlowRateMaxAvail
-
-   Node(OutletNode)%MassFlowRateMinAvail = Fan(FanNum)%MassFlowRateMinAvail
-
-
-
-Certain data items must always be transferred from inlet nodes to outlet nodes even if the data item is unaltered by the component model. The data items that must be transferred are:
-
-1.   Temp
-
-2.   HumRat
-
-3.   Enthalpy
-
-4.   Press
-
-5.   MassFlowRate
-
-6.   MassFlowRateMaxAvail
-
-7.   MassFlowRateMinAvail
-
-Interfacing with Plant
-----------------------
-
-Beginning with Version 7.0, EnergyPlus’s plant routines were reengineered and this section discusses protocols for how component models should interact with plant loop modeling.  Component models that reject or obtain heat from a liquid fluid stream, such as hot or chilled water, condenser water, and steam (but not refrigeration), are “plant components� that will need to interface with the central plant solver routines.  This section describes a number of utility routines and concepts for developers of plant component models.
-
-The node structure discussed above is reused for plant.  Each component model related to plant has inlet and outlet nodes that describe how it is connected to the loop.  Many of the routines pass in node indexes as arguments as well as other indexes into the main plant data structure.
-
-### Plant Loop Data Structure
-
-For plant components, in addition to inlet nodes, outlet nodes, and the component’s internal data structure, there is a fourth aspect to data flow that includes central data structures defined in DataPlant.f90.   The main data structure is called PlantLoop.  Both condenser loops and plant loops are treated the same and share the PlantLoop structure.  The PlantLoop structure stores information on the loop topology as well as various control and dispatch input and operational data.   The data structure is nested and component information is stored at this level:
-
-PlantLoop()%LoopSide()%Branch()%Comp()%xxx
-
-Where,
-
-PlantLoop is the top level and will be sized to the total number of plant and condenser loops.
-
-LoopSide is the second level and will be sized to two, one loop side is for the demand side and one loop side is for the supply side.
-
-Branch is the third level and will be sized to the total number of branches on that loop side
-
-Comp is the fourth level and will be sized to the total number of components on the branch.
-
-There are four indices that indentify each component’s location for each of the plant loops it is connected with: : loop number, loop side number, branch number, and component number.  A water cooled chiller will be connected to two loops and so the component itself will appear twice in the data structure and one set of indices will identify its location on the chilled water loop while a second set of indices will locate it on the condenser loop.  
-
-### Initialization
-
-Component models should store indexes that describe their location in the plant data structure.  To obtain these indices, call the routine ScanPlantLoopsForObjectonce for each instance of the component.  The component model’s data structure should store a set of indices for: loop number, loop side number, branch number, and component number.   If the component is connected to more than one plant loop, then there should be set of indices and a call to ScanPlantLoopsForObject for each plant loop it is connected to.  If a component model only has a single node name, the required indices can be similarly obtained using the a call to ScanPlantLoopsForNodeNum.
-
-Component models generally need to do a thorough re-initialization at the start of each new environment.  Component models can call InitComponentNodesto coordinate initializing inlet and outlet nodes. This routine has arguments for the minimum and maximum flow and these should be mass flow rates, in kg/s, that correspond to the “hardware� limits of the device.
-
-Some components are connected to more than one plant loop creating dependencies between loops. For example a water-cooled chiller is connected to both a chilled water loop and a condenser water loop.  The chilled water loop places demands on the condenser water loop so it is beneficial to model the chilled water loop’s supply side before the condenser water loop’s demand side is modeled.  An initialization routine called InterConnectTwoPlantLoopSides is used by the component models to inform the central plant routines of these situations.  One call to this routine describes a connection between two half-loops. The component model developer needs to decide which of the half loops places demands on the other and set the logical argument Loop1DemandsOnLoop2appropriately.  The central plant routines use this information to determine an appropriate calling order for simulating individual half-loops.
-
-### Sizing
-
-Component models need to interact with centralized routines that relate to sizes.  This section provides an overview of how EnergyPlus performs automatic sizing of plant systems and components so that the broader context can be understood when implementing plant components. As of EnergyPlus version 8.3, the plant sizing methods were changed significantly.  We first describe some of the variables involved, then describe the overall process steps, and finally discuss implications for component models.
-
-The following variables are used to help control plant sizing:
-
-- PlantFirstSizesOkayToFinalizePlantSizeNotComplete  This public logical boolean flag is declared in DataPlant.  It starts out FALSE TRUEfalse and is set to TRUE FALSEtrue only after all some intial plant sizing actions iterations have been completed and the first set of sizes can be finalized.   Component models should delay first filling autosized values until this flag is true. The -9999 values that indicate an autosized variable are not filled until this is TRUE.  
-
-- PlantFirstSizesOkayToReportPlantSizesOkayToFinalize  This public logical boolean flag is declared in DataPlant.  It starts out false FALSE and is set to TRUE true after the main iterative phase of sizing is completed but before the final finishing passes are made.  This flag is only used for advanced sizing methods based on HVAC Sizing Simulations, where the program should report both the “Initial� sizes and the final sizes.  Component models should delay final reporting first sizes and filling of autosized values until this is set to TRUEtrue.  The -9999 values that indicate an autosized variable are not filled until this is TRUE.  The first, or intial, cCalls to report the outcome of sizing are not made until this is TRUEtrue.  
-
-- PlantFinalSizesOkayToReport  This public boolean flag is declared in DataPlant.  It starts out false and is set to true when all the sizing is done and it is okay to report the final size values. Component models should delay reporting final sizes until this is set to true.  
-
-- InitLoopEquip  This logical flag is passed as an argument with SimPlantEquip and carries through to the main simulation calls for component models.  This argument is set to TRUE when the plant sizing is being conducted.  The component model needs to handle this argument such that when TRUE the get input, initialization and sizing routines are run, but the calculation routine does not.  When TRUE  most supply side component models need to return values for the minimum, maximum, and optimal capacities (in terms of loop loads that the device can meet).  For plant components with more than one connection to a plant loop, a leading loop connection must be determined and the component sizing routine called with InitLoopEquip is called for only that plant loop. For a example, a chiller only calls its sizing routine when called from a the chilled water loop and does not call it sizing routine when called from the condenser loop. 
-
-- GetSizingFactor  This logical flag is passed as an argument with SimPlantEquip and carries through to the main simulation calls for component models.  This is arguementargument set TRUE during some portions of the plant sizing calls and signals the intent to obtain the value of a component-level sizing factor.  When this argument is TRUE, InitLoopEquip will also be TRUE.  It can be ignored if the component model has no component-level sizing factor as part of its input.  If the component does offer a sizing factor, then the implementation needs to handle this argument such that when TRUE the model returns the value of the SizingFactor as an argument to the simulation routine that is called from SimPlantEquip.
-
-- CurLoopNum  This public integer variable is declared in DataSizing. It is used to communicate to the component models which of the plant loops is actively being sized at the moment. 
-
-- LoopNum and LoopSide These arguments are optional to the main simulation routine     
-
-Plant sizing routines use the approach outlined in the following steps.  These steps occur at a point during the program’s procedural flow when:  zone and system sizing is completed, much of the plant loop input has been read in and processed but the main plant manager is being called for the first time, none of the pure plant component’s simulation routines have yet been called (but components on the air side may have been), and an initial attempt at determining loop calling order has been made in SetupInitialPlantCallingOrder.
-
-1.    Initialize the indices that map between the central plant sizing data structures and the PlantLoop data structure.  This uses the subroutine called InitOneTimePlantSizingInfo. This ensures that the PlantLoop%PlantSizNumvariable is filled before any component models are called.
-
-(steps 2 thru 4 are sequentially repeated for four iterations)
-
-2.    Call each component model in calling order.   InitLoopEquipis TRUE.  The components on each half loop are called in flow order.  Each half loop in the model is called in the order set up for simulation.  These calls are typically the first time certain component models have been called and should trigger input processing and plant loop topology processing including loop interconnections.
-
-3.    Revise the calling order for the sequence with which the various plant loop sides are called for sizing and normal simulation.  Components that connect two loops will have been processed in Step 2 and that information is now available to refine loop side calling order
-
-4.    Call loop sizing routines in calling order.  Component will have registered their design flow rates in step 2 and now the overall loop sizes are determined from the sum of the components on the loop.
-
-5.    A final pass thru each loop side is made in calling order with the flag  PlantFirstSizesOkayToFinalize set to true.  At this point the findings are not expected to change (unless doing HVAC Sizing Simulations).  Component models now finalize their findings and store the results for use during the simulation.  Overall plant loops are finished.  If doing coincident plant sizing using HVAC Sizing Simulations, set the flag PlantFirstSizesOkayToReport and report the “Initial� sizes.  If not doing coincident plant sizing using HVAC Sizing Simulations, the sizes won’t change again and set the flag  PlantFinalSizesOkayToReport and report the final sizes.
-
-6.    Sizing finished and PlantSizeNotCompleteset FALSE
-
-In earlier versions, component sizing routines were only called once and one had to take care not call them repeatedly (or else their flow request would get doubled each time). However, now plant component models should be designed for multiple executions of their component-level sizing routine.  This allows for an iterative approach to plant sizing that is used to solve complex problems raised by inter-connected loops and the interdependence of sizing information.  As of version 8.3, the addition of HVAC Sizing Simulation method makes it very explicit that not only do sizing routines need to be able to rerun, the autosized values need to be set to useable values and then changed.  It is therefore now necessary to store whether or not the original input was set to autosize and so autosizable input now needs to add a boolean “*WasAutoSized� version of the variable to keep track of the user input. 
-
-After the component model has determined a design value for the flow rate, this flow rate needs to be registered with the larger plant routines by calling RegisterPlantCompDesignFlow. This is a volume flow rate in m<sup>3</sup>/s.  The flow rate is associated with the inlet node.  This call can be repeated and the design flow will be updated with the latest request.
-
-Calls to InitComponentNodesshould be done after sizing is complete so that valid sizes are passed for initialing nodes.
-
-### Component Flow Rates
-
-Plant components models need knowledge of the rate of plant fluid flows through the device for each of loops involved. Some components will need to request the flow they desire while others just need to know the mass flow rate.  However, components do not necessarily have complete control over the resulting flow rates because they depend on the state of the entire plant and not just on the individual component model.  Component models need to be implemented to handle situations where they do not get the exact flow rate they requested or expected to get.  For example there could be a shortage of flow and components are starved and get less than they desire. Or a component could be in series with another that is making a larger flow request and therefore a component receives more flow than expected.  Even if a component is usually passive and takes what flow it gets, the user might have placed a component on a branch that is in parallel with other branches making it necessary for even a passive component to make a flow “request� in order for its parallel branch to receive flow when a splitter distributes flow across a set of branches.
-
-SetComponentFlowRate collects code for how to properly deal with plant flow rates.  The idea is to use a central routine that actually changes the various mass flow rate variables on the node and checks against all the constraints.  As of Version 7, component models should no longer assign flows to the Node data structure. (Component models can get data from Node data structure but should not set flow rate data on the Node directly.)  The SetComponentFlowRate subroutine’s argument for fluid mass flow is INOUT; the component model makes a request and if it cannot be satisfied, the mass flow rate variable will be returned with the corrected flow that the plant can actually provide at the moment.
-
-Some models, such as a water coil controller, may only have information about one control node.  If a model does not really represent a single device with inlet and outlet nodes, then there is another useful routine called SetActuatedBranchFlowRate which serves a role similar to SetComponentFlowRate.  This routine handles mass flow issues for all the components on the branch that contains the actuated node but is otherwise similar in concept.
-
-### Controls
-
-Plant component models have different types of control interactions depending on the type of component.   Plant components that are led by the air side of HVAC models will generally be controlled by circumstances on the air side.  A water-based cooling coil will be targeting the achievement of certain air conditions and while the state of the chilled water plant serving the coil will matter in the model calculations, the component itself is not controlled by plant but things outside of plant.
-
-Components that need to be operated to meet the loads placed on plant loops will often be controlled based on some combination of node setpoints and dispatched loads.  The main entry routine (called from PlantLoopEquipment.f90)  for most such primary components should include and use arguments for “MyLoad� and “RunFlag.�  Central routines for operation schemes and availability managers will determine if a component is available (e.g. RunFlag) and what power level the device is being asked to provide (e.g. MyLoad).   MyLoad is now signed as of version 7; a negative value of MyLoad is a cooling load; a positive value of MyLoad is a heating load.
-
-### Updating
-
-Plant component update routines should no longer be setting mass flow rates in the update routine.  The flow setting routines should be called during initialization or calculation routines and should not need to be called again during update.  The state of the outlet node should be updated, such as outlet temperature, but mass flow rate should not be.  Prior to version 7 it was common in EnergyPlus to write
-
-   Node(OutletNode)  = Node(InletNode)
-
-However this is no longer acceptable practice and is not allowed for plant nodes.  Instead this can be replaced with a call to SafeCopyPlantNode.  This avoids problems when two components are in series and the outlet of one is the inlet of another. We cannot allow unsafe node copying because it will wipe out information stored on the inlet node of the second component.
-
-### Reporting
-
-A component model connected to plant via nodes will inherit a great deal of reporting that already occurs for each node.  The output variables that start out “System Node� will already be available to the user.   In general, the focus of reporting should be on data that are internal to the component model.
-
-### Central Routine Modifications
-
-When adding a new plant component, there are several places where the central routines’ code needs to be modified so that the new model can properly interact with them.  The following sections of the code should be expanded when adding a new plant component:
-
-1.    DataPlant.f90.  A new component will need to modify DataPlant.f90 in these places:
-
-a.    Parameter NumSimPlantEquipTypes. Increment up to include new component.
-
-b.   Array SimPlantEquipTypes.  Add array element with new object’s class name in upper case.
-
-c.    Array ccSimPlantEquipTypes.Add array element with new object’s class name in camel case.
-
-d.   Array ValidLoopEquipTypes.  Add array element with classification for what type of loop this component is intended for, primarily with respect to the type of loop it is intended to meet loads.
-
-e.    Parameter TypeOf\_xxxx .  Add an integer parameter to identify “TypeOf� number for subsequent use to identify component type without having to do string comparisions.
-
-2.    PlantManager.f90
-
-a.    GetPlantInput.  There is a large IF-ELSEIF block in this routine that will need to be extended to process the new component.  This is where the “TypeOf� number gets set for subsequent use.  Choose a general equipment type for the component.  Initialize the value for Comp%CurOpSchemeType depending on which loop side is involved and/or the nature of the component
-
-b.   SetupBranchControlTypes.  There is a large Case block in this routine that will need to be extended to process the new component.  Prior to Version 7, the user had to input a branch control type in the IDF.  Now this information is set in code in this routine.  There are three different control classifications that need to be set in this routine:
-
-                                                                  i.   Comp%FlowCtrl.  This is the branch control type input for versions prior to version 7.  Plant components that have some influence over the mass flows should be set to ControlType\_Active.  There are also ControlType\_Passive  and ControlType\_ByPass options that may apply.  The branches are further processed by routines that automatically detect series active situations.
-
-                                                                 ii.   Comp%FlowPriority.  New for version 7 is a plant modeling concept that treats flow requests differently depending on the nature of the component’s priority.  The idea is that when determining the overall flow rate in a loop, some mass flow requests need to be handled differently than others.  The three flow priority options for components are LoopFlowStatus\_NeedyAndTurnsLoopOn, LoopFlowStatus\_NeedyIfLoopOn, and LoopFlowStatus\_TakesWhatGets.  The first is typically a demand side component that when it requests flow will dictate that the loop operate and try to meet its request.  The second is typically a supply side component with a minimum flow requirement that should necessarily turn on the loop, but if it is running already then the overall flow rate needs to satisfy the minimum on the component.  The third is typically a passive device like a water tank.
-
-                                                                iii.   Comp%HowLoadServed.  This variable informs the load dispatch routines about the component. Some components are intended to serve loads in slightly different ways and this information is stored in the plant data structure as different parameters for HowLoadsServed.  HowMet\_NoneDemandis used for demand components or others than never meet a load.  HowMet\_PassiveCap is used for components that can meet a load but are not generally explicitly controllable to meet a certain level of load, such as a ground heat exchanger.  HowMet\_ByNominalCap is used for components that can be controlled to meet a desired load and do not have any additional layers of constraints.  HowMet\_ByNominalCapLowOutLimit is used for components that can be controlled to meet a desired load but have low temperature limit on their outlet node.  HowMet\_ByNominalCapHiOutLimit is used for components that can be controlled to meet a desired load but have a hi temperature limit on their outlet node.
-
-3.    PlantLoopEquipment.f90.  The routine SimPlantEquip includes a large Case statement that will need to expanded to include the new component.  Some demand components, such as a water coil, may not need to actually call a routine from here but a placeholder must be added to the Case statement.  Most plant components will call the main simulation entry point for the component model from SimPlantEquip and new components need to add that call here.  Note that the Case statement are broken up into General equipment and the specific equipment.    Code should support use of InitLoopEquip and GetCompSizFac as appropriate.
-
-Node Mass Flow Variables
-------------------------
-
-The node mass flow variables merit a little more discussion. Six mass flow variables are defined at each node. They are: MassFlowRate, MassFlowRateMin, MassFlowRateMax, MassFlowRateMinAvail, MassFlowRateMaxAvail and MassFlowRateRequest. These variables hold loop mass flow rate information according to the following definitions.
-
-- MassFlowRate – this node variable holds the simulation mass flow rate for the current timestep. The remaining four variables serve as limits to MassFlowRate.
-
-- MassFlowRateMax, MassFlowRateMin – These node variables hold the maximum possible and the minimum allowable flow rates for a particular component. As such, they represent the “hardware limit� on the flow rate for the component.
-
-- MassFlowRateMaxAvail, MassFlowRateMinAvail – these node variables represent the *loop* maximum and minimum flow rate for the current configuration of the loop on which the component resides.
-
-- MassFlowRateRequest  –  this node variable applies only to plant and holds the desired mass flow rate for the current timestep.  This stores a record of what flow was desired.
-
-EnergyPlus Services
-===================
-
-EnergyPlus provides some standard services that make the developer’s task much easier.  The developer can concentrate on the new simulation algorithm rather than have to deal with details of input file structure, writing output, obtaining scheduled data, and accessing weather variables.
-
-Utility Routines/Functions
---------------------------
-
-EnergyPlus supplies an extensive set of routines to help module developers get input, check values, get schedule values, get and check nodes.  These are summarized in the following table and in more detail in the following sections.  The table indicates the routine/function name, times of most likely use, and the module (if applicable) that you must USE in the code in order to make the routine available to you.  Most of the items mentioned in this table are of particular use in “GetInput� processing.  A few later tables will highlight similar functions/routines for simulation purposes.
-
-Table 2.  Table of Utility Functions
-
-Routine/Function Name
-
-Use during
-
-Module
-
-GetNumObjectsFound
-
-“GetInput� Processing
-
-InputProcessor
-
-GetObjectItem
-
-“GetInput� Processing
-
-InputProcessor
-
-GetObjectDefMaxArgs
-
-“GetInput� Processing
-
-InputProcessor
-
-GetObjectItemNum
-
-“GetInput� Processing
-
-InputProcessor
-
-FindItemInList
-
-“GetInput� Processing (best) though some are currently used in Simulation
-
-InputProcessor
-
-FindItem
-
-“GetInput� Processing
-
-InputProcessor
-
-FindItemInSortedList
-
-“Special processing� – list must be sorted.
-
-InputProcessor
-
-SameString
-
-“GetInput� Processing
-
-InputProcessor
-
-VerifyName
-
-“GetInput� Processing
-
-InputProcessor
-
-RangeCheck
-
-“GetInput� Processing
-
-InputProcessor
-
-MakeUPPERCase
-
-“GetInput� Processing
-
-InputProcessor
-
-GetOnlySingleNode
-
-“GetInput� Processing
-
-NodeInputManager
-
-GetNodeNums
-
-“GetInput� Processing
-
-NodeInputManager
-
-InitUniqueNodeCheck, CheckUniqueNodes, EndUniqueNodeCheck
-
-“GetInput� Processing
-
-NodeInputManager
-
-SetupCompSets
-
-“GetInput� Processing
-
-NodeInputManager
-
-TestCompSets
-
-“GetInput� Processing
-
-NodeInputManager
-
-GetNewUnitNumber
-
-(automatically retrieve an available unit number)
-
-EXTERNAL integer function
-
-FindUnitNumber
-
-Find a unit number when you know the name of the file
-
-EXTERNAL integer function
-
-FindNumberinList
-
-“GetInput� Processing/Init processing
-
-EXTERNAL integer function
-
-ValidateComponent
-
-“GetInput� Processing
-
-Subroutine CALL
-
-CheckComponent
-
-“GetInput� Processing – like ValidateComponent but doesn’t generate error message if failure
-
-Subroutine CALL
-
-CreateSysTimeIntervalString
-
-Simulation – Error Messages
-
-General
-
-TrimSigDigits
-
-Simulation – Error Messages
-
-General
-
-RoundSigDigits
-
-Simulation – Error Messages
-
-General
-
-GetScheduleIndex
-
-“GetInput� Processing
-
-ScheduleManager
-
-GetDayScheduleIndex
-
-“GetInput� Processing
-
-ScheduleManager
-
-GetCurrentScheduleValue
-
-Simulation
-
-ScheduleManager
-
-GetScheduleValuesForDay
-
-Simulation
-
-ScheduleManager
-
-GetSingleDayScheduleValues
-
-Simulation/�GetInput�
-
-ScheduleManager
-
-CheckScheduleValueMinMax
-
-“GetInput� Processing
-
-ScheduleManager
-
-CheckScheduleValue
-
-“GetInput� Processing
-
-ScheduleManager
-
-GetScheduleMinValue
-
-“GetInput� Processing
-
-ScheduleManager
-
-GetScheduleMaxValue
-
-“GetInput� Processing
-
-ScheduleManager
-
-LookUpScheduleValue
-
-Simulation
-
-ScheduleManager
-
-CheckOutAirNodeNumber
-
-“GetInput� Processing
-
-OutAirNodeManager
-
-GetCurveIndex
-
-“GetInput� Processing
-
-CurveManager
-
-GetCurveCheck
-
-“GetInput� Processing
-
-CurveManager
-
-GetCurveType
-
-“GetInput� Processing
-
-CurveManager
-
-CurveValue
-
-Simulation
-
-CurveManager
-
-SetupAndSort
-
-Sorting lists of character values
-
-SortAndStringUtilities
-
-SetupZoneInternalGain
-
-“GetInput� Processing
-
-DataInterfaces
-
-Input Services
---------------
-
-The module *InputProcessor* processes the input data files (IDFs).  It also reads and parses the IDD file.  The InputProcessor uses the definition lines in the IDD as directives on how to process each input object in the IDF.  The InputProcessor also turns all alpha strings into all UPPER CASE.  Currently, it does nothing else to those strings – so the number of blanks in a string must match what the calculational modules expect.  The InputProcessor processes all numeric strings into single precision real numbers.  Special characters, such as tabs, should *not* be included in the IDF.
-
-The EnergyPlus module *InputProcessor* provides several routines - generically called the “get� routines – that enable the developer to readily access the data for a new module.  These routines are made available by including a “USE InputProcessor� statement in the module or in the routine that will use the “get� routines.  The GetFanInput subroutine in the example illustrates some of the uses of the “get� routines.
-
-### InputProcessor
-
-The following objects use public routines from the InputProcessor.  To access these, the code has:
-
-Use InputProcessor, ONLY: &lt;routine1&gt;, &lt;routine2&gt;
-
-Where the &lt;routine&gt; is one or more of the following:
-
-### GetNumObjectsFound
-
-This function returns the number of objects in the input belonging to a particular class.  In other terms, it returns the number of instances in the input of a particular component.
-
-Example:
-
-USE InputProcessor, ONLY: GetNumObjectsFound
-
----
-
-NumVAVSys = **GetNumObjectsFound**('SINGLE DUCT:VAV:REHEAT')
-
-
-
-Here NumVAVSys will contain the number of single duct VAV terminal units in the input data file (IDF). SINGLE DUCT:VAV:REHEAT is the class name or keyword defining VAV terminal unit input on the IDD file.
-
-### GetObjectItem
-
-This subroutine is used to obtain the actual alphanumeric and numeric data for a particular object.
-
-Example:
-
-    USE InputProcessor
-
----
-
-    INTEGER :: SysNum = 0     ! The Sys that you are currently loading input into
-
----
-
-    CHARACTER(Len=MaxNameLength)  :: CurrentModuleObject
-
-    CHARACTER(Len=MaxNameLength), ALLOCATABLE, DIMENSION(:) :: Alphas
-
-    CHARACTER(Len=MaxNameLength), ALLOCATABLE, DIMENSION(:) :: cAlphaFields
-
-    CHARACTER(Len=MaxNameLength), ALLOCATABLE, DIMENSION(:) :: cNumericFields
-
-    REAL(r64), ALLOCATABLE, DIMENSION(:) :: Numbers
-
-    LOGICAL, ALLOCATABLE, DIMENSION(:)   :: lAlphaBlanks
-
-    LOGICAL, ALLOCATABLE, DIMENSION(:)   :: lNumericBlanks
-
-    INTEGER                              :: MaxNums=0
-
-    INTEGER                              :: MaxAlphas=0
-
-    INTEGER                              :: TotalArgs=0
-
----
-
-    CALL **GetObjectDefMaxArgs** &
-
-('AirTerminal:SingleDuct:VAV:Reheat', TotalArgs, NumAlphas, NumNums)
-
-    MaxNums=MAX(MaxNums,NumNums)
-
-    MaxAlphas=MAX(MaxAlphas,NumAlphas)
-
----
-
-      !Start Loading the System Input
-
-        CurrentModuleObject='AirTerminal:SingleDuct:VAV:Reheat'
-
-
-
-      DO SysIndex = 1,  NumVAVSys
-
-
-
-        CALL **GetObjectItem** & (TRIM(CurrentModuleObject),SysIndex,Alphas,NumAlphas,Numbers,NumNums, &
-
-    IOSTAT,AlphaBlank=lAlphaBlanks,NumBlank=lNumericBlanks,  &
-
-    AlphaFieldnames=cAlphaFields,NumericFieldNames=cNumericFields)
-
-
-
-        SysNum = SysIndex
-
----     Check to make sure no duplicate names entered
-
-        Sys(SysNum)%SysName     = Alphas(1)
-
-        Sys(SysNum)%SysType     = TRIM(CurrentModuleObject)
-
-        Sys(SysNum)%SysType\_Num = SingleDuctVAVReheat
-
----
-
-      END DO
-
-
-
-Here GetObjectItem is called with inputs ('AirTerminal:SingleDuct:VAV:Reheat')  – passed as CurrentModuleObject the class of object we want to input – and SysIndex – the index of the object on the input file. If SysIndex is 3, the call to GetObjectItem will get the data for the third VAV terminal unit on the input file. Output is returned in the remaining arguments. AlphArray contains in order all the alphanumeric data items for a single VAV terminal unit. NumArray contains all the numeric data items. NumAlphas is the number of alphanumeric items read; NumNums is the number of numeric data items read.  IOSTAT is a status flag: -1 means there was an error; +1 means the input was OK. AlphArray and NumArray should be dimensioned to handle the largest expected input for the item – which in this case is set from a call to **GetObjectDefMaxArgs**. NumBlank is an optional argument to the routine – it can be used to determine if a numeric field was entered as “blank� rather than the filled value of 0.0. Likewise for NumFields and the others.
-
-These are used to make the potential error messages from the GetInput routine correspond more closely to the IDD nomenclature, but look a bit funny in use:
-
-IF (Sys(SysNum)%SchedPtr == 0) THEN
-
-   CALL ShowSevereError(  &
-
-     RoutineName//trim(CurrentModuleObject)//'="'//  &
-
-     TRIM(Sys(SysNum)%SysName)//'", invalid schedule.')
-
-   CALL ShowContinueError(TRIM(cAlphaFields(2))//' = '//  &
-
-     TRIM(Alphas(2))//' not found.')
-
-   ErrorsFound=.true.
-
-ENDIF
-
-More information about standard error message formatting is contained in the [Output Details and Examples](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf) document (for the user) and (for the developer) in this document section: Standard Message Format.
-
-### GetObjectDefMaxArgs
-
-#### Extensible input techniques
-
-While developers do their best to guess how many items are needed in an object, users will often want to extend that object with far more fields than were dreamed of.  Using Allocatable arrays in Fortran usually makes this feasible, the special \\extensible field makes it possible.
-
-Example:
-
-USE InputProcessor, ONLY: GetObjectDefMaxArgs
-
----
-
-CHARACTER(len=MaxNameLength), ALLOCATABLE, DIMENSION(:) :: Alphas
-
-REAL, ALLOCATABLE, DIMENSION(:)                         :: Numbers
-
-
-
-! You supply the object word, routine returns numargs, numalpha, numnumeric
-
-
-
-CALL **GetObjectDefMaxArgs**(‘DAYSCHEDULE:INTERVAL’,NumArgs,NumAlpha,NumNumeric)
-
-
-
-ALLOCATE(Alphas(NumAlpha))
-
-ALLOCATE(Numbers(NumNumeric))
-
-
-
-!  Then, usual get calls…
-
-Thus, you can determine how many arguments that the IDD has defined as “maximum� for a given object.
-
-### GetObjectItemNum
-
-GetObjectItem, described above, requires the input file index of the desired object in order to get the object’s data. Sometimes this index may be unknown, but the name of the object is known. GetObjectItemNum returns the input file index given the class name and object name.
-
-Example:
-
-USE InputProcessor, ONLY: GetObjectItemNum
-
----
-
-ListNum = **GetObjectItemNum**('CONTROLLER LIST',ControllerListName)
-
-
-
-In the example, ListNum will contain the input file index of the ‘CONTROLLER LIST’ whose name is contained in the string variable ControllerListName.
-
-### FindItemInList
-
-This function looks up a string in a similar list of items and returns the index of the item in the list, if found. It is case sensitive.
-
-Example:
-
-USE InputProcessor, ONLY: FindItemInList
-
----
-
-SysNum = **FindItemInList**(CompName,Sys%SysName,NumSys)
-
-
-
-CompName is the input string, Sys%SysName is the list of names to be searched, and NumSys is the size of the list.
-
-### FindItem
-
-Case insensitive version of the FindItemInList.
-
-Example:
-
-USE InputProcessor, ONLY: FindItem
-
----
-
-SysNum = **FindItem**(CompName,Sys%SysName,NumSys)
-
-
-
-CompName is the input string, Sys%SysName is the list of names to be searched, and NumSys is the size of the list.
-
-### FindItemInSortedList
-
-This function looks up a string in a sorted list of items and returns the index of the item in the list, if found. It is case sensitive.
-
-Example:
-
-USE InputProcessor, ONLY: FindItemInSortedList
-
----
-
-SysNum = **FindItemInSortedList**(CompName,Sys%SysName,NumSys)
-
-
-
-CompName is the input string, Sys%SysName is the list of names to be searched, and NumSys is the size of the list. See quick sort utility – most lists are NOT sorted in EnergyPlus.
-
-### SameString
-
-This function returns true if two strings are equal (case insensitively).
-
-Example:
-
-USE InputProcessor, ONLY: SameString
-
----
-
-IF (**SameString**(InputRoughness,'VeryRough')) THEN
-
-    Material(MaterNum)%Roughness=VeryRough
-
-ENDIF
-
-### VerifyName
-
-This subroutine checks that an object name is unique; that is, it hasn’t already been used for the same class of object and the name is not blank.
-
-Example:
-
-USE InputProcessor, ONLY: VerifyName
-
----
-
-CALL **VerifyName**(AlphArray(1),Fan%FanName, &
-
-  FanNum-1,IsNotOK,IsBlank,'FAN:SIMPLE:CONSTVOLUME Name')
-
-The first argument is the name to be checked, the second is the list of names to search, the third argument is the number of entries in the list, the 4<sup>th</sup> argument is set to TRUE if verification fails, the 5<sup>th</sup> argument is set to true if the name is blank, and the last argument is part of the error message written to the error file when verification fails.
-
-### RangeCheck
-
-The routine RangeCheck can be used to produce a reasonable error message to describe the situation in addition to setting the ErrorsFound variable to true.  Errors found can then be checked in the calling routine and the program terminated if desired.
-
-SUBROUTINE RangeCheck(ErrorsFound,WhatFieldString,WhatObjectString,ErrorLevel,  &
-
-                      LowerBoundString,LowerBoundCondition,UpperBoundString,UpperBoundCondition)
-
-It can be used in a variety of places when the \\minimum and \\maximum fields will not work (e.g. different min/max dependent on some other field).
-
-USE InputProcessor, ONLY: RangeCheck
-
----
-
-ErrorsFound=.false.
-
-CALL RangeCheck(ErrorsFound,'DryBulb Temperature','WeatherFile',  &
-
-                'SEVERE','&gt; -70',(Drybulb&gt;-70.),'&lt; 70',(DryBulb &lt;70.))
-
-CALL RangeCheck(ErrorsFound,'DewPoint Temperature','WeatherFile',  &
-
-                'SEVERE','&gt; -70',(Dewpoint&gt;-70.),'&lt; 70',(Dewpoint &lt;70.))
-
-CALL RangeCheck(ErrorsFound,'Relative Humidity','WeatherFile',  &
-
-                'SEVERE','&gt; 0',(RelHum&gt;=0.),'&lt;= 110',(RelHum&lt;=110.))
-
-To examine one call:
-
-The variable **DryBulb** is set to its value.  In this case, it is coming from the **Weather File**.  The **LowerBoundString** is ‘&gt; - 70’ and the **LowerBoundCondition** is (DryBulb&gt;-70.) [this expression will yield true or false depending…]
-
-The LowerBounds (**LowerBoundString**, **LowerBoundCondition**) are optional as are the UpperBounds (**UpperBoundString**, **UpperBoundCondition**).  If we were only testing one set of ranges, the call would look like:
-
-Call **RangeCheck**(ErrorsFound,’DryBulb Temperature’,’WeatherFile’,’SEVERE’,  &
-
-  UpperBoundString=’&lt; 70’, UpperBoundCondition=(DryBulb&lt;70.))
-
-ErrorLevel can be one of the usual Error levels:
-
-WARNING – would be a simple warning message – the calling routine might reset the value to be within bounds
-
-SEVERE – a severe error.  Usually the program would terminate if this is in a “GetInput� routine.  If during execution, the calling program could reset the value but RangeCheck contains too many string comparisons to be called for an execution problem.
-
-FATAL – not likely to be used.  You want to provide a context to the error and if really a fatal type error, you’d like to execute the RangeCheck call and then terminate from the calling program.
-
-And the context for the message may be shown in the calling routine by checking the value of ErrorsFound:
-
-ErrFound=.false.
-
-Call **RangeCheck**(ErrFound,'This field','SEVERE','&lt;= 100',(Value&lt;100.))
-
-IF (ErrFound) THEN
-
-  CALL ShowContinueError('Occurs in routine xyz')
-
-  ErrorsFound=.true.  ! for later termination
-
-ENDIF
-
-### MakeUPPERCase
-
-This function can be used to make sure an upper case string is being used.  (Note this is not needed when using “SameString�).  Parameter 1 to the function is the string to be upper cased:
-
-USE InputProcessor, ONLY: MakeUPPERCase
-
----
-
-UCString=**MakeUPPERCase**(‘lower string’)
-
-Object Services
----------------
-
-It is standard practice in EnergyPlus that only objects associated with a given module be accessed from the input data file using a GetObjectItem function call and that this type of function call only be executed during GetInput. For example, the module HVACDXSystem would only access the object DXSystem:AirLoop in the GetInput subroutine or the module HVACFanComponent would only access the different fan objects as shown in the example below. This programming standard requires that all modules be “responsible� for specific objects and no other module accesses the input data file for this specific object. Using this technique, maintenance of the EnergyPlus modules is limited to specific areas of software as input data for objects evolve for any reason.
-
-*Module HVACDXSystem - SUBROUTINE GetDXCoolingSystemInput:*
-
-    CALL GetObjectItem('DXSYSTEM:AIRLOOP',DXCoolSysNum,AlphArray, &
-
-                           NumAlphas,NumArray,NumNums,IOSTAT)
-
-*Module HVACFanComponent – SUBROUTINE GetFanInput:*
-
-    CALL GetObjectItem('FAN:SIMPLE:CONSTVOLUME',SimpFanNum,AlphArray, &
-
-                           NumAlphas,NumArray,NumNums,IOSTAT)
-
-    CALL GetObjectItem('FAN:SIMPLE:VARIABLEVOLUME',VarVolFanNum, &
-
-                           AlphArray,NumAlphas,NumArray,NumNums,IOSTAT)
-
-    CALL GetObjectItem('ZONE EXHAUST FAN',ExhFanNum,AlphArray, &
-
-                           NumAlphas,NumArray,NumNums,IOSTAT)
-
-    CALL GetObjectItem('FAN:SIMPLE:ONOFF',OnOffFanNum,AlphArray, &
-
-                           NumAlphas,NumArray,NumNums,IOSTAT)
-
-If module developers were allowed to access the input data file for other objects not related to a particular module, both the original module and the alternate module would have to be corrected each time the object changed. This poses a severe hazard for future development of EnergyPlus.
-
-Module developers may at times require information for specific objects from other modules. When this occurs, the Information is “mined� through function or subroutine calls located in the other module. Existing function calls may be used or added to EnergyPlus as needed. In this way, a module developer could confirm that node information provided in a parent object matched the node information specified for its children object. Other error checking may also be performed in this manner. For example, if the module HVACDXSystem needed to know the capacity of the DX cooling coil, a function call to GetCoilCapacity in the DXCoil module would provide this information. The function GetCoilCapacity would the “Get� the input from the input data file if it has not already been accessed and provide the information back to the calling module.
-
-A variety of examples exist to aid the module developer in this area of programming.
-
-
-
--   DXCoil.f90:
-
-FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
-
-FUNCTION GetMinOATCompressor(CoilType,CoilName,ErrorsFound) RESULT(MinOAT)
-
-FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
-
-FUNCTION GetCoilOutletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
-
-FUNCTION GetSupplyAirFanOperatingMode(CoilType,CoilName,ErrorsFound) RESULT(OpMode)
-
-FUNCTION GetCoilCondenserNode(CoilType,CoilName,ErrorsFound) RESULT(CondNode)
-
-FUNCTION GetHPCoolingCoilIndex(HeatingCoilType, HeatingCoilName, HeatingCoilIndex)
-               RESULT(DXCoolingCoilIndex)
-
-
-
--   FanCoilUnits.f90:
-
-INTEGER FUNCTION GetFanCoilZoneInletAirNode(FanCoilNum)
-
-INTEGER FUNCTION GetFanCoilOutAirNode(FanCoilNum)
-
-INTEGER FUNCTION GetFanCoilReturnAirNode(FanCoilNum)
-
-INTEGER FUNCTION GetFanCoilMixedAirNode(FanCoilNum)
-
-
-
--   HeatRecovery.f90:
-
-FUNCTION GetSupplyInletNode(HXName,ErrorsFound)
-
-FUNCTION GetSupplyOutletNode(HXName,ErrorsFound)
-
-FUNCTION GetSecondaryInletNode(HXName,ErrorsFound)
-
-FUNCTION GetSecondaryOutletNode(HXName,ErrorsFound)
-
-
-
--   HVACFanComponent.f90:
-
-FUNCTION GetFanDesignVolumeFlowRate(FanType,FanName,ErrorsFound) RESULT(DesignVolumeFlowRate
-
-FUNCTION GetFanInletNode(FanType,FanName,ErrorsFound) RESULT(NodeNumber)
-
-FUNCTION GetFanOutletNode(FanType,FanName,ErrorsFound) RESULT(NodeNumber)
-
-SUBROUTINE GetFanVolFlow(FanIndex, FanVolFlow)
-
-SUBROUTINE GetFanType(FanName,FanType,ErrorsFound,ThisObjectType)
-
-
-
--   HVACHeatingCoils.f90:
-
-FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
-
-FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
-
-FUNCTION GetCoilOutletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
-
-SUBROUTINE GetHeatingCoilIndex(HeatingCoilName,HeatingCoilIndex,ErrorsFound)
-
-
-
--   HVACHXAssistedCoolingCoil.f90:
-
-FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
-
-FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
-
-FUNCTION GetCoilOutletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
-
-FUNCTION GetHXDXCoilName(CoilType,CoilName,ErrorsFound) RESULT(DXCoilName)
-
-FUNCTION GetCoilMaxWaterFlowRate(CoilType,CoilName,ErrorsFound) RESULT(MaxWaterFlowRate)
-
-
-
--   HVACStandAloneERV.f90
-
-FUNCTION GetSupplyAirFlowRate(ERVType,ERVCtrlName,ErrorsFound) RESULT(AirFlowRate)
-
-FUNCTION GetSupplyAirInletNode(ERVType,ERVCtrlName,ErrorsFound) RESULT(AirInletNode)
-
-FUNCTION GetExhaustAirInletNode(ERVType,ERVCtrlName,ErrorsFound) RESULT(AirInletNode)
-
-INTEGER FUNCTION GetStandAloneERVOutAirNode(StandAloneERVNum)
-
-INTEGER FUNCTION GetStandAloneERVZoneInletAirNode(StandAloneERVNum)
-
-INTEGER FUNCTION GetStandAloneERVReturnAirNode(StandAloneERVNum)
-
-
-
--   HVACSteamCoilComponent.f90:
-
-FUNCTION GetCoilMaxWaterFlowRate(CoilType,CoilName,ErrorsFound) RESULT(MaxWaterFlowRate)
-
-
-
--   HVACWaterCoilComponent.f90:
-
-FUNCTION GetCoilMaxWaterFlowRate(CoilType,CoilName,ErrorsFound) RESULT(MaxWaterFlowRate)
-
-FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
-
-FUNCTION GetCoilOutletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
-
-
-
--   HVACWaterToAir.f90:
-
-FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
-
-FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
-
-FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
-
-FUNCTION GetCoilInletNode(CoilType,CoilName,ErrorsFound) RESULT(NodeNumber)
-
-
-
--   MixedAir.f90:
-
-FUNCTION GetOAMixerNodeNumbers(OAMixerName,ErrorsFound) RESULT(OANodeNumbers)
-
-FUNCTION GetNumOAMixers() RESULT(NumberOfOAMixers)
-
-FUNCTION GetNumOAControllers() RESULT(NumberOfOAControllers)
-
-FUNCTION GetOAMixerReliefNodeNumber(OAMixerNum) RESULT(ReliefNodeNumber)
-
-FUNCTION GetOASystemNumber(OASysName) RESULT(OASysNumber)
-
-FUNCTION GetOAMixerInletNodeNumber(OAMixerNumber) RESULT(OAMixerInletNodeNumber)
-
-FUNCTION GetOAMixerReturnNodeNumber(OAMixerNumber) RESULT(OAMixerReturnNodeNumber)
-
-FUNCTION GetOAMixerMixedNodeNumber(OAMixerNumber) RESULT(OAMixerMixedNodeNumber)
-
-
-
--   PackagedTerminalHeatPump.f90:
-
-INTEGER FUNCTION GetPTHPZoneInletAirNode(PTHPNum)
-
-INTEGER FUNCTION GetPTHPOutAirNode(PTHPNum)
-
-INTEGER FUNCTION GetPTHPReturnAirNode(PTHPNum)
-
-INTEGER FUNCTION GetPTHPMixedAirNode(PTHPNum)
-
-
-
--   PurchasedAirManager.f90:
-
-FUNCTION GetPurchasedAirOutAirMassFlow(PurchAirNum) RESULT(OutAirMassFlow)
-
-
-
--   SetpointManager.f90:
-
-LOGICAL FUNCTION IsNodeOnSetPtManager(NodeNum,SetPtType)
-
-
-
--   UnitVentilator.f90:
-
-INTEGER FUNCTION GetUnitVentilatorOutAirNode(UnitVentNum)
-
-INTEGER FUNCTION GetUnitVentilatorZoneInletAirNode(UnitVentNum)
-
-INTEGER FUNCTION GetUnitVentilatorMixedAirNode(UnitVentNum)
-
-INTEGER FUNCTION GetUnitVentilatorReturnAirNode(UnitVentNum)
-
-
-
--   WindowAC.f90:
-
-INTEGER FUNCTION GetWindowACZoneInletAirNode(WindACNum)
-
-INTEGER FUNCTION GetWindowACOutAirNode(WindACNum)
-
-INTEGER FUNCTION GetWindowACReturnAirNode(WindACNum)
-
-INTEGER FUNCTION GetWindowACMixedAirNode(WindACNum)
-
-These kinds of calls are highly encouraged so that data is mined from the other modules rather than being declared public.
-
-The function call for GetCoilCapacity in module DXCoil.f90 is shown below. Note that the format for these function calls have the same format as other subroutines throughout the EnergyPlus software. The example function shown below is declared as a public routine in module DXCoils for use by other modules through a USE statement.
-
-*Module DXCoils.f90:*
-
-PUBLIC  GetCoilCapacity
-
-FUNCTION GetCoilCapacity(CoilType,CoilName,ErrorsFound) RESULT(CoilCapacity)
-
-
-
-          ! FUNCTION INFORMATION:
-
-          !       AUTHOR         Linda Lawrie
-
-          !       DATE WRITTEN   February 2006
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS FUNCTION:
-
-          ! This function looks up the coil capacity for the given
-
-          ! coil and returns it.  If incorrect coil type or name
-
-          ! is given, errorsfound is returned as true and capacity
-
-          ! is returned as negative.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! na
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-  USE InputProcessor,  ONLY: FindItemInList
-
-
-
-  IMPLICIT NONE ! Enforce explicit typing of all variables in
-
-                ! this routine
-
-
-
-          ! FUNCTION ARGUMENT DEFINITIONS:
-
-  CHARACTER(len=\*), INTENT(IN) :: CoilType   ! must match coil
-
-                                             ! types in this module
-
-  CHARACTER(len=\*), INTENT(IN) :: CoilName   ! must match coil
-
-                                             ! names for the coil type
-
-  LOGICAL, INTENT(INOUT)     :: ErrorsFound  ! set to true if problem
-
-  REAL                       :: CoilCapacity ! returned capacity of
-
-                                             ! matched coil
-
-
-
-          ! FUNCTION PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS:
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS:
-
-          ! na
-
-
-
-          ! FUNCTION LOCAL VARIABLE DECLARATIONS:
-
-  INTEGER :: WhichCoil
-
-
-
-  ! Obtains and Allocates DXCoils
-
-  IF (GetCoilsInputFlag) THEN
-
-    CALL GetDXCoils
-
-    GetCoilsInputFlag = .FALSE.
-
-  END IF
-
-
-
-  IF (CoilType == 'COIL:DX:HEATINGEMPIRICAL' .or.   &
-
-      CoilType == 'COIL:DX:COOLINGBYPASSFACTOREMPIRICAL') THEN
-
-    WhichCoil=FindItemInList(CoilName,DXCoil%Name,NumDXCoils)
-
-    IF (WhichCoil /= 0) THEN
-
-      CoilCapacity=DXCoil(WhichCoil)%RatedTotCap(1)
-
-    ENDIF
-
-  ELSE
-
-    WhichCoil=0
-
-  ENDIF
-
-
-
-  IF (WhichCoil == 0) THEN
-
-    CALL ShowSevereError('Could not find CoilType="' &
-
-             //TRIM(CoilType)//'" with Name="'//TRIM(CoilName)//'"')
-
-    ErrorsFound=.true.
-
-    CoilCapacity=-1000.
-
-  ENDIF
-
-
-
-  RETURN
-
-
-
-END FUNCTION GetCoilCapacity
-
-
-
-Note that the function name in one module can be the same as a function name in a different module. In fact, for EnergyPlus this should be the case – the module should use a generic name that is typical of its function. The calling module should use a “local name� that better specifies the type of item it is accessing. For example, if module HVACFurnace required node or capacity information from identical functions contained in modules HVACHeatingCoils and DXCoils, these function names could easily be assigned more descriptive names in the HVACFurnace module as follows.
-
-*Module HVACFurnace.f90:*
-
-USE HeatingCoils,    ONLY:         GetHeatingCoilCapacity=&gt;GetCoilCapacity,
-
-GetHeatingCoilInletNode=&gt;GetCoilInletNode
-
-USE DXCoils,            ONLY:        GetDXCoilCapacity=&gt;GetCoilCapacity,
-
-GetDXCoilInletNode=&gt;GetCoilInletNode
-
-Branch & Node Checking and Services
------------------------------------
-
-### BranchInputManager
-
-For the most part, new modules do not use the BranchInputManager directly.  Branches are “gotten� at a high management level.  The main routines that might be used from the BranchInputManager are: NumBranchesInBranchList, GetBranchList and GetBranchData.  The BranchInputManager also houses the Splitter and Mixer data: GetLoopSplitter and GetLoopMixer.
-
-### NumBranchesInBranchList
-
-This routine is used to get the number of branches in a branch list name (so that an appropriate array can be allocated).
-
-INTEGER FUNCTION NumBranchesInBranchList(BranchListName)
-
-An example of use:
-
-=== Example ===
-
-USE BranchInputManager, ONLY: NumBranchesInBranchList,. . .
-
-. . .
-
-PrimeAirSys(ASysNum)%NumBranches=  &
-
-              **NumBranchesInBranchList**(BranchListName)
-
-IF (PrimeAirSys(ASysNum)%NumBranches.EQ.0) THEN
-
-  CALL ShowSevereError('There must be at least 1 branch in system ' &
-
-                         //TRIM(PrimeAirSys(ASysNum)%Name))
-
-  ErrorsFound=.true.
-
-END IF
-
-ALLOCATE(BranchNames(PrimeAirSys(ASysNum)%NumBranches))
-
-BranchNames=' '
-
-### GetBranchList
-
-This routine is used to get the names of the branches on a Loop.
-
-SUBROUTINE GetBranchList(LoopName, BranchListName, NumBranchNames, BranchNames, LoopType)
-
-=== Example ===
-
-USE BranchInputManager, ONLY: GetBranchList, . . .
-
-. . .
-
-
-
-(NumBranches from NumBranchesInBranchList)
-
-! get the branch lists
-
-CALL **GetBranchList**(PrimeAirSys(ASysNum)%Name,BranchListName,  &
-
-        PrimeAirSys(ASysNum)%NumBranches,BranchNames,'Air')
-
-ALLOCATE(PrimeAirSys(ASysNum)%Branch(NumBranches))
-
-. . . . . . . .
-
-The first argument is the loop name, the 2<sup>nd</sup> argument is the name of the Branch List, the 3<sup>rd</sup> argument is an output: the number of branch names, the 4<sup>th</sup> argument is an output: the names of the branches in the list, the 5<sup>th</sup> argument is the loop type.
-
-### GetBranchData
-
-This routine is used to get pieces of data about a branch.
-
-SUBROUTINE GetBranchData(LoopName, BranchName, BranchMaxFlow, NumComps, CompType, CompName, CompCtrlType, CompInletNodeNames, CompInletNodeNums, CompOutletNodeNames, CompOutletNodeNums, ErrorsFound)
-
-=== Example ===
-
-! Cycle through all of the branches and set up the branch data
-
-DO BNum = 1,PrimeAirSys(ASysNum)%NumBranches
-
-  PrimeAirSys(ASysNum)%Branch(BNum)%Name = BranchNames(BNum)
-
-  NumBComps=NumCompsInBranch(BranchNames(BNum))
-
-
-
-  ALLOCATE(CompTypes(NumBComps))
-
-  CompTypes=' '
-
-  ALLOCATE(CompNames(NumBComps))
-
-  CompNames=' '
-
-  ALLOCATE(CompCtrls(NumBComps))
-
-  CompCtrls=' '
-
-  ALLOCATE(InletNodeNames(NumBComps))
-
-  InletNodeNames=' '
-
-  ALLOCATE(InletNodeNumbers(NumBComps))
-
-  InletNodeNumbers=0
-
-  ALLOCATE(OutletNodeNames(NumBComps))
-
-  OutletNodeNames=' '
-
-  ALLOCATE(OutletNodeNumbers(NumBComps))
-
-  OutletNodeNumbers=0
-
-
-
-  CALL GetBranchData(PrimeAirSys(ASysNum)%Name,  &
-
-     BranchNames(BNum),             &
-
-     PrimeAirSys(ASysNum)%Branch(BNum)%MaxVolFlowRate, &
-
-     NumBComps,                   &
-
-     CompTypes,CompNames,CompCtrls,      &
-
-     InletNodeNames,InletNodeNumbers,    &
-
-     OutletNodeNames,OutletNodeNumbers,ErrorsFound)
-
-  ALLOCATE &
-
- (PrimeAirSys(ASysNum)%Branch(BNum)%Comp(NumBComps))
-
-  PrimeAirSys(ASysNum)%Branch(BNum)%TotalComponents =  &
-
-                   NumBComps
-
-
-
-  PrimeAirSys(ASysNum)%Branch(BNum)%TotalNodes =   &
-
-                   NumBComps+1
-
-  ALLOCATE (PrimeAirSys(ASysNum)%Branch(BNum)%NodeNum(NumBComps+1))
-
-  PrimeAirSys(ASysNum)%Branch(BNum)%NodeNum(1) =   &
-
-                   InletNodeNumbers(1)
-
-  PrimeAirSys(ASysNum)%Branch(BNum)%DuctType = Main
-
-  DO CNum = 1,PrimeAirSys(ASysNum)%Branch(BNum)%TotalComponents
-
-
-
-    PrimeAirSys(ASysNum)%Branch(BNum)%Comp(CNum)%TypeOf = &
-
-                         CompTypes(CNum)
-
-    PrimeAirSys(ASysNum)%Branch(BNum)%Comp(CNum)%Name  =  &
-
-                       = CompNames(CNum)
-
-    PrimeAirSys(ASysNum)%Branch(BNum)%Comp(CNum)%Index = 0
-
-    PrimeAirSys(ASysNum)%Branch(BNum)%Comp(CNum)%FlowCtrl= &
-
-                         CompCtrls(CNum)
-
-    PrimeAirSys(ASysNum)%Branch(BNum)%Comp(CNum)%NodeNameIn=&
-
-                         InletNodeNames(CNum)
-
-    PrimeAirSys(ASysNum)%Branch(BNum)%Comp(CNum)%NodeNumIn=&
-
-                         InletNodeNumbers(CNum)
-
-    PrimeAirSys(ASysNum)%Branch(BNum)%Comp(CNum)%NodeNameOut=&
-
-                         OutletNodeNames(CNum)
-
-    PrimeAirSys(ASysNum)%Branch(BNum)%Comp(CNum)%NodeNumOut= &
-
-                         OutletNodeNumbers(CNum)
-
-    PrimeAirSys(ASysNum)%Branch(BNum)%NodeNum(CNum+1) = &
-
-                         OutletNodeNumbers(CNum)
-
-### NodeInputManager
-
-The NodeInputManager is responsible for getting all the node names and assigning each a number.  Node names are learned in random order – which can make validation difficult.  Internally nodes are referenced as number and should be integers in any data structure or reference.  Two key routines are used for obtaining node numbers:  GetOnlySingleNode and GetNodeNums.
-
-### Node Information Arguments
-
-Both routines need some extra information about the node as the number is obtained.This information is used to support fluid property calculations, the HVAC Diagram utility, and various diagnostic checks.
-
-#### NodeFluidType
-
-This argument defines the type of fluid at this node such as air or water.  The node fluid type is used for fluid property calculations and is reported in the list of nodes in the bnd output file.   Parameter definitions for this argument can be found in DataLoopNode.  As of version 1.3, the list of valid choices is:
-
-  ! Valid Fluid Types for Nodes
-
-  INTEGER, PARAMETER :: NodeType\_Unknown = 0  ! 'blank'
-
-  INTEGER, PARAMETER :: NodeType\_Air     = 1  ! 'Air'
-
-  INTEGER, PARAMETER :: NodeType\_Water   = 2  ! 'Water'
-
-  INTEGER, PARAMETER :: NodeType\_Steam   = 3  ! 'Steam'
-
-  INTEGER, PARAMETER :: NodeType\_Electric= 4  ! 'Electric'
-
-
-
-  CHARACTER(len=\*), PARAMETER, DIMENSION(0:4) :: ValidNodeFluidTypes=  &
-
-                     (/'blank   ',  &
-
-                       'Air     ',  &
-
-                       'Water   ',  &
-
-                       'Steam   ',  &
-
-                       'Electric'/)
-
-  INTEGER, PARAMETER :: NumValidNodeFluidTypes=4
-
-Note that the argument passed in is an integer value – you can “USE DataLoopNode� and use the above definitions (preferred over either defining your own or passing in a number).  In many cases, a component may not know the fluid type.  For example, most SET POINT MANAGERS are applicable to both air and water nodes.  In this case, NodeType\_Unknown should be used.  It is assumed that for any given node, at least one object referencing it will know the fluid type.  Once a known fluid type is passed for a given node, it cannot be changed.  All references to the same node must specify the same fluid type or unknown.  When all input has been gotten, all node fluid types should be known, but this is not being validated currently.
-
-#### NodeObjectType
-
-This is the type of object which is referencing the node (e.g. Chiller:Electric).  This information is used to generate the list of Parent and Non-Parent Node Connections in the bnd output file.  This list is used by the HVAC Diagram utility.
-
-#### NodeObjectName
-
-This is the name of the object which is referencing the node (e.g. My Chiller).  This information is used to generate the list of Parent and Non-Parent Node Connections in the bnd output file.  This list is used by the HVAC Diagram utility.
-
-#### NodeConnectionType
-
-Parameter definitions for this argument can be found in DataLoopNode. .As of version 1.2.0, the current list of choices is:
-
-  ! Valid Connection Types for Nodes
-
-  CHARACTER(len=\*), PARAMETER, DIMENSION(13) :: ValidConnectionTypes=  &
-
-                     (/'Inlet      ',  &
-
-                       'Outlet     ',  &
-
-                       'Internal   ',  &
-
-                       'ZoneNode   ',  &
-
-                       'Sensor     ',  &
-
-                       'Actuator   ',  &
-
-                       'OutsideAir ',  &
-
-                       'ReliefAir  ',  &
-
-                       'ZoneInlet  ',  &
-
-                       'ZoneReturn ',  &
-
-                       'ZoneExhaust',  &
-
-                       'Setpoint   ',  &
-
-                       'Electric   '/)
-
-  INTEGER, PARAMETER :: NumValidConnectionTypes=13
-
-
-
-  INTEGER, PARAMETER :: NodeConnectionType\_Inlet = 1
-
-  INTEGER, PARAMETER :: NodeConnectionType\_Outlet = 2
-
-  INTEGER, PARAMETER :: NodeConnectionType\_Internal = 3
-
-  INTEGER, PARAMETER :: NodeConnectionType\_ZoneNode = 4
-
-  INTEGER, PARAMETER :: NodeConnectionType\_Sensor = 5
-
-  INTEGER, PARAMETER :: NodeConnectionType\_Actuator = 6
-
-  INTEGER, PARAMETER :: NodeConnectionType\_OutsideAir = 7
-
-  INTEGER, PARAMETER :: NodeConnectionType\_ReliefAir = 8
-
-  INTEGER, PARAMETER :: NodeConnectionType\_ZoneInlet = 9
-
-  INTEGER, PARAMETER :: NodeConnectionType\_ZoneReturn = 10
-
-  INTEGER, PARAMETER :: NodeConnectionType\_ZoneExhaust = 11
-
-  INTEGER, PARAMETER :: NodeConnectionType\_Setpoint = 12
-
-  INTEGER, PARAMETER :: NodeConnectionType\_Electric = 13
-
-This information is used to generate the list of Parent and Non-Parent Node Connections in the bnd output file.  This list is used by the HVAC Diagram utility.
-
-After all input has been gotten, node connection types are also validated in CheckNodeConnections in NodeInputManager according to the following rules. The rules are intended to catch user input errors without placing unnecessary constraints on system configurations. The validation checks are not exhaustive, so it is possible to pass all of the checks yet have a misconnected simulation. The main goal here is to prevent dangling nodes which do not behave as the user expects and can often go undetected without scrutinizing detailed outputs.
-
-- For any node which is used as an actuator, the same node must also be used at least once as a node type which is not sensor or actuator or outsideair.
-
-- For any node which is used as a setpoint, the same node must also be used at least once as a node type which is not a setpoint or outsideair.
-
-- Every ZoneInlet must appear as an outlet from something, otherwise it will do nothing.
-
-- Every ZoneExhaust must appear as an inlet to something, otherwise it will do nothing.
-
-- Every inlet node should match either an Outlet, ZoneReturn, ZoneExhaust, ReliefAir, or OutsideAir node, with the following exceptions:
-
-- If an InletNode's object is AIR PRIMARY LOOP, CONDENSER LOOP, or PLANT LOOP, then skip the test.
-
-- If an InletNode's object is not one of the above types, it is valid if the same node name appears as an INLET to an AIR PRIMARY LOOP, CONDENSER LOOP, or PLANT LOOP.
-
-If a node fails any of the above tests, a severe error message is generated. If a new module generates unexpected errors, check the node connection types used by a similar module. *If a given node is used in more than one way by an object, it may be necessary to register the node more than once by successive calls to GetOnlySingleNode or GetNodeNums with different arguments in each call.*
-
-NodeConnectionType\_OutsideAir is intended to specify nodes which are connected to the outside air.  For example, OUTSIDE AIR MIXER has an Outside\_Air\_Stream\_Node which is registered as NodeConnectionType\_Inlet, because it may have other components such as a preheat coil between it and the outside air. Whichever node ultimately connects to the outside air in this case will be registered as NodeConnectionType\_OutsideAir by an OUTSIDE AIR INLET NODE LIST object.
-
-Some types of equipment take in outside air directly without relying on OUTSIDE AIR INLET NODE LIST to set the conditions on that node.  For example, UNIT VENTILATOR and chillers with air cooled condensers do not require the use of an OUTSIDE AIR INLET NODE LIST. In these cases, the component registers the outside air node directly as NodeConnectionType\_OutsideAir. Given that the use of outside air nodes is not consistent throughout the code, it may be necessary at some point to relax or alter the validation rules associated with outside air nodes to accommodate a new type of module. Please consult with the team before changing these rules.
-
-#### NodeFluidStream
-
-This is an integer indicating which fluid stream this node belongs to (1, 2, 3). For components with a single fluid stream, such as a fan, set this to one for the inlet and outlet nodes.  For components with multiple fluid streams, such as a water coil, matching inlets and outlets should use the same fluid stream number.  For example, the air inlet and air outlet would be stream 1, and the water inlet and water outlet would be stream 2. This information is used to generate the list of Parent and Non-Parent Node Connections in the bnd output file.  This list is used by the HVAC Diagram utility.
-
-#### ObjectIsParent
-
-True If the object is a parent object, false if not. Parameters are defined in DataLoopNode. As of version 1.2.0, the current list of choices is:
-
-  ! Valid IsParent Types for Node Connections
-
-  LOGICAL, PARAMETER :: ObjectIsParent = .TRUE.
-
-  LOGICAL, PARAMETER :: ObjectIsNotParent = .FALSE.
-
-What is a parent object?  A parent object is one which encloses and references other objects.  For example, FAN COIL UNIT:4 PIPE is a parent to a fan, a heating coil, a cooling coil, and an outside air mixer. In most cases, all nodes referenced by a parent object are duplicated in the non-parent objects which are the components which ultimately act on the fluid stream. From the perspective of the HVAC Diagram utility, every fluid loop must be a continuous connection of non-parent objects and zones. In this example, the nodes of the mixer, fan, coils, and zone form a complete loop. Some components, such as UNIT VENTILATOR are part parent and part non-parent. It is a parent to a fan, a heating coil, and a cooling coil, but it does not reference an explicit outside air mixer. The mixer is an implied component within the unit ventilator. In these cases, to facilitate drawing a loop in HVAC Diagram, it is necessary to create a non-parent component to carry the fluid. So, the unit ventilator uses the following approach as illustrated by the comments and source code. Note that Alphas(3), the air inlet node, is registered twice, once as an inlet to parent object UNIT VENTILATOR, and once as an inlet to the implicit non-parent object UNIT VENTILATOR-OA MIXER.
-
-Excerpt from GetUnitVentilatorInput in UnitVentilator
-
-
-
-          ! Main air nodes (except outside air node):
-
-          ! For node connections, this object is both a parent and a non-parent, because the
-
-          ! OA mixing box is not called out as a separate component, its nodes must be connected
-
-          ! as ObjectIsNotParent.  But for the fan and coils, the nodes are connected as ObjectIsParent
-
-          ! To support the diagramming tool, the unit ventilator inlet node must appear both as
-
-          ! an inlet to the unit ventilator parent object and as an inlet to the implied
-
-          ! non-parent OA mixing box within the unit ventilator.
-
-          ! Because there is overlap between the nodes that are parent and non-parent, use a different
-
-          ! object type for the non parent nodes
-
-    UnitVent(UnitVentNum)%AirInNode = &
-
-               GetOnlySingleNode(Alphas(3),ErrorsFound,'UNIT VENTILATOR',Alphas(1), &
-
-                            NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsParent)
-
-    UnitVent(UnitVentNum)%AirInNode = &
-
-               GetOnlySingleNode(Alphas(3),ErrorsFound,'UNIT VENTILATOR-OA MIXER',Alphas(1), &
-
-                            NodeType\_Air,NodeConnectionType\_Inlet,1,ObjectIsNotParent)
-
-
-
-    UnitVent(UnitVentNum)%AirOutNode = &
-
-               GetOnlySingleNode(Alphas(4),ErrorsFound,'UNIT VENTILATOR',Alphas(1), &
-
-                            NodeType\_Air,NodeConnectionType\_Outlet,1,ObjectIsParent)
-
-
-
-    UnitVent(UnitVentNum)%FanOutletNode = &
-
-               GetOnlySingleNode(Alphas(5),ErrorsFound,'UNIT VENTILATOR',Alphas(1), &
-
-                            NodeType\_Air,NodeConnectionType\_Internal,1,ObjectIsParent)
-
-
-
-### GetOnlySingleNode
-
-This is used when only one node is expected as the input point.  If this name points to a NodeList, an appropriate error message will be issued and errFlag (the second argument) will be set .true.
-
-**GetOnlySingleNode**(NodeName,errFlag,NodeObjectType,NodeObjectName,NodeFluidType,NodeConnectionType,NodeFluidStream,ObjectIsParent)
-
-It is used:
-
-Example:
-
-USE NodeInputManager, ONLY: GetOnlySingleNode
-
-. . .
-
-! get inlet node number
-
-Baseboard(BaseboardNum)%WaterInletNode  = &
-
-               **GetOnlySingleNode**(AlphArray(3),ErrorsFound,  &
-
-                    'Baseboard Heater:Water:Convective',AlphArray(1), &
-
-                     NodeType\_Water,NodeConnectionType\_Inlet,  &
-
-                     1,ObjectIsNotParent)
-
-! get outlet node number
-
-Baseboard(BaseboardNum)%WaterOutletNode  = &
-
-               **GetOnlySingleNode**(AlphArray(4),ErrorsFound,  &
-
-                     'Baseboard Heater:Water:Convective',AlphArray(1), &
-
-                      NodeType\_Water,NodeConnectionType\_Outlet,  &
-                       1,ObjectIsNotParent)
-
-The first argument is the node name, the 2<sup>nd</sup> argument is the error flag variable, the 3<sup>rd</sup> argument is the object type, the 4<sup>th</sup> argument is the object name – the remainder arguments are as listed above.
-
-### GetNodeNums
-
-This is used when more than one node is valid for an input. Like the GetOnlySingleNode invocation, GetNodeNums needs the extra information for a node:
-
-SUBROUTINE GetNodeNums(Name,NumNodes,NodeNumbers,ErrorsFound,  &
-
-               NodeFluidType,NodeObjectType,NodeObjectName,  &
-
-               NodeConnectionType,NodeFluidStream,ObjectIsParent)
-
-Example:
-
-USE NodeInputManager, ONLY: GetNodeNums
-
-. . .
-
-CHARACTER(len=MaxNameLength), DIMENSION(4) :: AlphArray
-
-INTEGER :: NumNodes
-
-INTEGER, DIMENSION(25) :: NodeNums
-
-. . . . . . . .
-
-! Get the supply nodes
-
-ErrInList=.false.
-
-CALL **GetNodeNums**(Names(8),NumNodes,NodeNums,ErrInList,NodeType\_Air,  &
-
-                'AIR PRIMARY LOOP',PrimaryAirSystem(AirSysNum)%Name,  &
-
-                NodeConnectionType\_Inlet,1,ObjectIsParent)
-
-IF (ErrInList) THEN
-
- CALL ShowContinueError('Invalid Node Name or Node List in Air System=' &
-
-                        //TRIM(PrimaryAirSystem(AirSysNum)%Name))
-
- ErrorsFound=.true.
-
-ENDIF
-
-! Allow at most 3 supply nodes (for a 3 deck system)
-
-IF (NumNodes &gt; 3) THEN
-
-  CALL ShowSevereError('Air System:Only 1st 3 Nodes will be used from:' &
-
-                        //TRIM(Names(8)))
-
-  CALL ShowContinueError('Occurs in Air System='//  &
-
-                         TRIM(PrimaryAirSystem(AirSysNum)%Name))
-
-  ErrorsFound=.true.
-
-ENDIF
-
-IF (NumNodes.EQ.0) THEN
-
-  CALL ShowSevereError('Air System:there must be at least 1 ‘// &
-
-                       ‘supply node in system '//TRIM(Names(1)))
-
-  CALL ShowContinueError('Occurs in Air System='//  &
-
-                       TRIM(PrimaryAirSystem(AirSysNum)%Name))
-
-  ErrorsFound=.true.
-
-END IF
-
-. . . . . . . .
-
-
-
-The first argument is a node name or the name of a Node List, the 2<sup>nd</sup> argument is the number of nodes in the Node List (1 for a single node), the 3<sup>rd</sup> argument is the output: a list of node numbers – these are followed by the arguments shown above.
-
-### Unique Node Checking
-
-A set of routines will allow you to use the NodeInputManager to check for unique node names across a set of inputs.  This is used currently in the CONTROLLED ZONE EQUIP CONFIGURATION object where each zone node mentioned must be unique.  Three routines comprise the unique node check:  InitUniqueNodeCheck, CheckUniqueNodes, EndUniqueNodeCheck
-
-### InitUniqueNodeCheck
-
-A call to this routine starts the collection and detection of unique/non-unique nodes by the NodeInputManager:
-
-USE NodeInputManager, ONLY: InitUniqueNodeCheck, CheckUniqueNodes, &
-
-                            EndUniqueNodeCheck
-
-. . .
-
-CALL **InitUniqueNodeCheck**(‘CONTROLLED ZONE EQUIP CONFIGURATION’)
-
-The only argument is a simple string that will help with error messages that may come from the NodeInputManager.  Unique node checking can only be done for one context (‘CONTROLLED ZONE EQUIP CONFIGURATION’) at a time.
-
-### CheckUniqueNodes
-
-SUBROUTINE CheckUniqueNodes(NodeTypes,CheckType,ErrorsFound,  &
-
-                            CheckName,CheckNumber)
-
-This is the routine called during the getting of the nodes.  The CheckType argument can be ‘Nodename’ or ‘NodeNumber’ and then pass in the appropriate argument to CheckName or CheckNumber.  CheckName and CheckNumber are optional arguments – only the necessary one need be supplied.
-
-Argument 1, NodeTypes, is the type of node being looked for – this argument is used for error messages within the NodeInput processing.  Argument 2, ErrorsFound, will be set to true of this node is not unique in the current context.
-
-Example:
-
-    UniqueNodeError=.false.
-
-    CALL **CheckUniqueNodes**('Zone Air Node','NodeName',UniqueNodeError,  &
-
-                          CheckName=AlphArray(5))
-
-    IF (UniqueNodeError) THEN
-
-      CALL ShowContinueError('Occurs for Zone='//TRIM(AlphArray(1)))
-
-      ErrorsFound=.true.
-
-    ENDIF
-
-### EndUniqueNodeCheck
-
-This routine terminates the unique node check – allows arrays to be deallocated, etc.
-
-CALL **EndUniqueNodeCheck**(‘CONTROLLED ZONE EQUIP CONFIGURATION’)
-
-The only argument is the Context String – which must match the string given in the InitUniqueNodeCheck routine.
-
-### SetUpCompSets and TestCompSet
-
-SetUpCompSets and TestCompSet are used to develop a list of hierarchical relationships between HVAC objects.  The CompSet routines are housed in the BranchInputManager.  A list of component sets is built which contains the following information:
-
-Parent Object Type (Currently cannot be SPLITTER or MIXER)
-
-Parent Object Name
-
-Child Component Type (Currently cannot be SPLITTER or MIXER)
-
-Child Component Name
-
-Child Component InletNodeName
-
-Child Component OutletNodeName
-
-Node Description
-
-Parent and child refer to a hierarchical relationship of two HVAC objects.  For example, a branch is the parent to a pump, and a fan coil is the parent to a fan.  The component sets do not include peer-to-peer connections such as a splitter connected to a branch, or a zone supply air path connected to an air loop.
-
-The following rules apply to component sets:
-
-- Each parent/child component set is unique.  The same pair of components should never appear in the component sets list more than once.
-
-- Each set of child component plus inlet and outlet nodes is unique.
-
-- Each child component must have a parent component.
-
-- A given component may appear in multiple component sets as a parent component.
-
-- A given component may appear in multiple component sets as a child component only if there is a different set of inlet/outlet nodes.  *(This was originally the intent, but some new components do not fit this rule well and it may need to be relaxed.)*
-
-- If a given node name appears more than once as an inlet node, the two components which use it must share a parent/child relationship.
-
-- If a given node name appears more than once as an outlet node, the two components which use it must share a parent/child relationship.
-
-- After the program has read all the input data, there should be no "UNDEFINED" values in the list of component sets.
-
-When any of these rules are violated, a warning is issued indicating a possible node connection error.
-
-
-
-\*\* Warning \*\* Potential Node Connection Error for object PIPE, name=CW\_BYPASS
-
-   \*\*   ~~~   \*\*   Node Types are still UNDEFINED -- See Branch/Node Details file for further information
-
-   \*\*   ~~~   \*\*   Inlet Node : CW\_BYPASS\_INLET
-
-   \*\*   ~~~   \*\*   Outlet Node: CW\_BYPASS\_OUTLET
-
-
-
-The component sets are reported in the eplusout.bnd file:
-
-
-
-! &lt;Component Set&gt;,&lt;Component Set Count&gt;,&lt;Parent Object Type&gt;,&lt;Parent Object Name&gt;,&lt;Component Type&gt;,&lt;Component Name&gt;,&lt;Inlet Node ID&gt;,&lt;Outlet Node ID&gt;,&lt;Description&gt;
-
-
-
- Component Set,1,BRANCH,COOLING SUPPLY INLET BRANCH,PUMP:VARIABLE SPEED,CHW CIRC PUMP,CHW SUPPLY INLET NODE,CHW PUMP OUTLET NODE,Water Nodes
-
-
-
-Component Set,21,FAN COIL UNIT:4 PIPE,ZONE1FANCOIL,FAN:SIMPLE:CONSTVOLUME,ZONE1FANCOILFAN,ZONE1FANCOILOAMIXEROUTLETNODE,ZONE1FANCOILFANOUTLETNODE,Air Nodes
-
-#### SetUpCompSets
-
-SetUpCompSets should be called any time a parent object such as a branch or a compound object (e.g. furnace) references a child component which is connected to it.  If an object has more than one child component, then SetUpCompSets is called once for each child.
-
-SetUpCompSets first looks for the child component in the existing list of component sets by looking for a matching component type and name.  If it is found, then the parent name and type are filled in.  If the child component is not found is the exisiting list, then a new component set is created.
-
-
-
-SUBROUTINE SetUpCompSets(ParentType,ParentName,CompType,CompName,InletNode,OutletNode,Description)
-
-
-
-The arguments are:
-
-ParentType     Parent Object Type
-
-ParentName   Parent Object Name
-
-CompType      Child Component Type
-
-CompName    Child Component Name
-
-InletNode         Child Component Inlet Node Name
-
-OutletNode      Child Component Outlet Node Name
-
-Description      Description of nodes (optional)
-
-For example, AirLoopHVAC:Unitary:Furnace:HeatOnly references a fan and a heating coil:
-
-**AirLoopHVAC:Unitary:Furnace:HeatOnly**,
-
-        \\memo identical to the AirLoopHVAC:UnitaryHeatOnly object
-
-        \\min-fields 13
-
-   A1,  \\field Name
-
-        \\required-field
-
-        \\type alpha
-
-   A2,  \\field Availability Schedule Name
-
-        \\required-field
-
-        \\type object-list
-
-        \\object-list ScheduleNames
-
-   A3,  \\field Furnace Air Inlet Node Name
-
-        \\required-field
-
-        \\type node
-
-   A4,  \\field Furnace Air Outlet Node Name
-
-        \\required-field
-
-        \\type node
-
-   A5,  \\field Supply Air Fan Operating Mode Schedule Name
-
-        \\type object-list
-
-        \\object-list ScheduleNames
-
-        \\note A fan operating mode schedule value of 0 indicates cycling fan mode (supply air
-
-        \\note fan cycles on and off in tandem with the heating coil).
-
-        \\note Any other schedule value indicates continuous fan mode (supply air fan operates
-
-        \\note continuously regardless of heating coil operation).
-
-        \\note Leaving this schedule name blank will default to cycling fan mode for the
-
-        \\note entire simulation period.
-
-   N1,  \\field Maximum Supply Air Temperature
-
-        \\type real
-
-        \\units C
-
-        \\autosizable
-
-        \\default 80.0
-
-   N2,  \\field Supply Air Flow Rate
-
-        \\required-field
-
-        \\type real
-
-        \\note  This value should be &gt; 0 and &lt;= than the fan air flow rate.
-
-        \\units m3/s
-
-        \\minimum&gt; 0.0
-
-        \\autosizable
-
-
-
-   A6,  \\field Controlling Zone or Thermostat Location
-
-        \\required-field
-
-        \\type object-list
-
-        \\object-list ZoneNames
-
-   A7,  \\field Supply Fan Object Type
-
-        \\required-field
-
-        \\type choice
-
-        \\key Fan:OnOff
-
-        \\key Fan:ConstantVolume
-
-        \\note Fan:ConstantVolume only works with continuous fan operating mode (i.e. fan
-
-        \\note operating mode schedule values are greater than 0).
-
-   A8,  \\field Supply Fan Name
-
-        \\required-field
-
-        \\type object-list
-
-        \\object-list FansCVandOnOff
-
-   A9 , \\field Fan Placement
-
-        \\type choice
-
-        \\key BlowThrough
-
-        \\key DrawThrough
-
-        \\default BlowThrough
-
-   A10, \\field Heating Coil Object Type
-
-        \\required-field
-
-        \\type choice
-
-        \\key Coil:Heating:Gas
-
-        \\key Coil:Heating:Electric
-
-        \\key Coil:Heating:Water
-
-        \\key Coil:Heating:Steam
-
-        \\note works with gas, electric, hot water and steam heating coils
-
-   A11; \\field Heating Coil Name
-
-        \\required-field
-
-        \\type object-list
-
-        \\object-list HeatingCoilName
-
-
-
-In this case, the furnace is the parent object to the fan and the heating coil.  To set up the component set for the furnace and its fan, the furnace type and name, the fan type and name (A7 and A8), and the furnace/fan inlet and fan outlet nodes (A3 and A9) are passed to SetUpCompSets:
-
-
-
-Example:
-
-
-
-USE BranchInputManager, ONLY: SetUpCompSets
-
-. . .
-
-CALL SetUpCompSets(
- Furnace(FurnaceNum)%FurnaceType,Furnace(FurnaceNum)%Name,
- AlphArray(7),AlphArray(8),AlphArray(3),AlphArray(9))
-
-
-
-In some cases, the inlet or outlet node names may not be known by the parent object.  In this case, "UNDEFINED" is passed to SetUpCompSets.
-
-
-
-Examples:
-
-
-
-USE BranchInputManager, ONLY: SetUpCompSets
-
-. . .
-
-CALL SetUpCompSets(
- Furnace(FurnaceNum)%FurnaceType,Furnace(FurnaceNum)%Name,
- AlphArray(8),AlphArray(9),'UNDEFINED','UNDEFINED')
-
-
-
-CALL SetUpCompSets(
- Furnace(FurnaceNum)%FurnaceType,Furnace(FurnaceNum)%Name,
- AlphArray(12),AlphArray(13),'UNDEFINED',AlphArray(4))
-
-
-
-#### TestCompSet
-
-TestCompSet should be called by every HVAC object which has a parent object.  A given object may be both a parent and a child.  For example, **AirLoopHVAC:Unitary:Furnace:HeatOnly** is a child to a branch and a parent to a fan and coils.
-
-TestCompSet first looks for the calling component in the existing list of component sets by looking for a matching component type and name.  If the found compset has inlet and outlet nodes defined, then these must also match.  If  a match is found, then any undefined node names are filled in and the description string for the nodes is added.  If the component is not found, then a new component set is created with undefined parent object type and name.
-
-
-
-SUBROUTINE TestCompSet(CompType,CompName,InletNode,OutletNode,Description)
-
-
-
-The arguments are:
-
-- CompType            Child Component Type
-
-- CompName          Child Component Name
-
-- InletNode               Child Component Inlet Node Name
-
-- OutletNode            Child Component Outlet Node Name
-
-- Description            Description of nodes
-
-For example, **AirLoopHVAC:Unitary:Furnace:HeatOnly** is a child component with inlet and outlet nodes:
-
-**AirLoopHVAC:Unitary:Furnace:HeatOnly,**
-
-        \\memo identical to the AirLoopHVAC:UnitaryHeatOnly object
-
-        \\min-fields 14
-
-   A1,  \\field Name
-
-        \\required-field
-
-        \\type alpha
-
-   A2,  \\field Availability Schedule Name
-
-        \\required-field
-
-        \\type object-list
-
-        \\object-list ScheduleNames
-
-   A3,  \\field Furnace Air Inlet Node Name
-
-        \\required-field
-
-        \\type alpha
-
-   A4,  \\field Furnace Air Outlet Node Name
-
-        \\required-field
-
-        \\type alpha
-
-
-
-To register the component set for the furnace (as a child component), the furnace type and name, and the furnace inlet and outlet nodes (A3 and A4) along with a node descriptor are passed to TestCompSets:
-
-
-
-Example:
-
-
-
-USE BranchInputManager, ONLY: TestCompSet
-
-
-
-CALL TestCompSet (Furnace(FurnaceNum)%FurnaceType,AlphArray(1), &
-
-                  AlphArray(3),AlphArray(4),'Air Nodes')
-
-### CheckOutAirNodeNumber
-
-Outside Air Nodes are special nodes connected to the outside environment.  With the introduction of the Site Atmospheric Variation parameters, it becomes important to know whether the node name (e.g. Condenser Inlet Node on Air Cooled Chillers) is a legitimate outside air node or not.  CheckOutAirNodeNumber allows you to determine if an entered node is, in fact, a proper outside air node.
-
-Declaration:
-
-FUNCTION CheckOutAirNodeNumber(NodeNumber) RESULT(Okay)
-
-Example:
-
-USE OutAirNodeManager, ONLY: CheckOutAirNodeNumber
-
-! outdoor condenser node
-
-  IF (lAlphaBlanks(10)) THEN
-
-    DXCoil(DXCoilNum)%CondenserInletNodeNum(1) = 0
-
-  ELSE
-
-    DXCoil(DXCoilNum)%CondenserInletNodeNum(1) = &
-
-       GetOnlySingleNode(Alphas(10),ErrorsFound,TRIM(CurrentModuleObject),DXCoil(DXCoilNum)%Name, &
-
-                         NodeType\_Air,NodeConnectionType\_OutsideAirReference,1,ObjectIsNotParent)
-
-
-
-    IF (.not. CheckOutAirNodeNumber(DXCoil(DXCoilNum)%CondenserInletNodeNum(1))) THEN
-
-      CALL ShowWarningError(RoutineName//trim(CurrentModuleObject)//'="'//trim(DXCoil(DXCoilNum)%Name)//'", may be invalid')
-
-      CALL ShowContinueError(TRIM(cAlphaFields(10))//'="'//TRIM(Alphas(10))// &
-
-                               '", node does not appear in an OutdoorAir:NodeList or as an OutdoorAir:Node.')
-
-      CALL ShowContinueError('This node needs to be included in an air system or the coil model will not be valid' &
-
-                             //', and the simulation continues')
-
-    END IF
-
-  ENDIF
-
-Note that GetOnlySingleNode is used to get the proper node number, then the node number is used in the outside air node verification.
-
-### CheckAndAddAirNodeNumber
-
-Should you feel really nice about your users (or more likely be updating older code that may have allowed blanks in places that are properly outside air nodes), you can use the CheckAndAddAirNodeNumber routine to not only check to see if it is an outside air node but also add it at the same time.
-
-Declaration:
-
-SUBROUTINE CheckAndAddAirNodeNumber(NodeNumber,Okay)
-
-USE OutAirNodeManager, ONLY: CheckAndAddAirNodeNumber
-
-Example:
-
-ElectricChiller(ChillerNum)%CondInletNodeNum    = &
-
- GetOnlySingleNode(AlphArray(5),ErrorsFound,  &
-
-   'Chiller:Electric',AlphArray(1), NodeType\_Air, &
-
-    NodeConnectionType\_OutsideAirReference, 2, ObjectIsNotParent)
-
-CALL CheckAndAddAirNodeNumber(  &
-
-ElectricChiller(ChillerNum)%CondInletNodeNum, &
-
-Okay)
-
-IF (.not. Okay) THEN
-
-  CALL ShowWarningError('Chiller:Electric, Adding Outside Air Node='//  &
-
-AlphArray(5)))
-
-ENDIF
-
-Note that here “not Okay� is not an error condition but rather the opportunity to notify the user that you are adding an air node.
-
-
-
-Schedule Services
------------------
-
-Schedules are widely used in specifying input for building simulation programs. For instance heat gains from lighting, equipment and occupancy are usually specified using schedules. Schedules are used to indicate when equipment is on or off. Schedules are also used to specify zone and system set points. EnergyPlus uses schedules in all these ways and provides services that make using schedules very easy for the developer.
-
-Schedules are specified in a three level hierarchy in EnergyPlus input.
-
-**Day Schedules** (IDD Objects: Schedule:Day:Hourly, Schedule:Day:Interval, Schedule:Day:List)
-
-**Week Schedules** (IDD Objects: Schedule:Week:Daily, Schedule:Week:Compact)
-
-**Annual Schedules** (IDD Objects: Schedule:Year, Schedule:Compact, Schedule:File)
-
-In addition, a **ScheduleTypeLimits** object can specify certain limits on the schedules.  This is a mostly optional input but can be used effectively.  (That is, if your examples include it, users will probably use it too.)
-
-An example from an input (IDF) file:
-
-  **ScheduleTypeLimits**,
-
-    Fraction,  !- ScheduleType Name
-
-    0.0 : 1.0,  !- range
-
-    CONTINUOUS;  !- Numeric Type
-
-
-
-  **ScheduleTypeLimits**,
-
-    On/Off,  !- ScheduleType Name
-
-    0:1,  !- range
-
-    DISCRETE;  !- Numeric Type
-
-
-
-! Schedule Constant
-
-  **SCHEDULE:COMPACT**,
-
-  Constant,
-
-  on/off,
-
-  Through: 12/31,
-
-  For: AllDays,
-
-  Until: 24:00, 1.0;
-
-
-
-! Schedule Daytime Ventilation
-
-  **SCHEDULE:COMPACT**,
-
-  Daytime Ventilation,
-
-  Fraction,
-
-  Through: 12/31,
-
-  For: Weekdays SummerDesignDay,
-
-  Until: 08:00, 0.0,
-
-  Until: 18:00, 1.0,
-
-  Until: 24:00, 0.0,
-
-  For: Weekends WinterDesignDay,
-
-  Until: 10:00, 0.0,
-
-  Until: 16:00, 1.0,
-
-  Until: 24:00, 0.0,
-
-  For: Holidays AllOtherDays,
-
-  Until: 24:00, 0.0;
-
-
-
-
-
-! Schedule Intermittent
-
-  **SCHEDULE:COMPACT**,
-
-  Intermittent,
-
-  Fraction,
-
-  Through: 12/31,
-
-  For: AllDays,
-
-  Until: 08:00, 0.0,
-
-  Until: 18:00, 1.0,
-
-  Until: 24:00, 0.0;
-
-
-
-The day schedule elements assign numbers that span a full day (24 hours). The week schedule elements indicate which day schedules are applicable to each day of the week plus holiday and some special days. Schedule elements indicate which week schedules are applicable to various periods of the year. Both day schedules and schedules reference a schedule type. A schedule type is characterized by a range (e.g. 0 to 1) and whether it is continuous (can assume any value) or discrete (can assume integer values only). The following routines from the ScheduleManager module enable the developer to use schedules in a simulation.
-
-### GetScheduleIndex
-
-This function takes a schedule name as input and returns an internal pointer to the schedule. Schedule values will always be accessed via the pointer not the name during the simulation for reasons of efficiency. This function should be called once for each schedule during the input phase and the returned value stored in the appropriate data structure.
-
-Example:
-
-USE ScheduleManager, ONLY: GetScheduleIndex
-
-. . .
-
-Baseboard(BaseboardNum)%SchedPtr = **GetScheduleIndex**(AlphArray(2))
-
-
-
-Here the schedule pointer for the schedule name contained in AlphArray(2) is stored in the baseboard data structure for later use.  If a 0 is returned, this is not a valid schedule.  Objects should also typically check for “blank� schedules.
-
-### GetDayScheduleIndex
-
-This function takes a “day schedule� name as input and returns an internal pointer to the schedule. Day schedule values will always be accessed via the pointer not the name during the simulation for reasons of efficiency. This function should be called once for each schedule during the input phase and the returned value stored in the appropriate data structure.
-
-Example:
-
-USE ScheduleManager, ONLY: GetDayScheduleIndex
-
-. . .        DesDayInput(EnvrnNum)%RelHumSchPtr=GetDayScheduleIndex(DDNames(4))
-
-Here the day schedule pointer for the day schedule name contained in DDNames(4) is stored in the design day data structure for later use.  If a 0 is returned, this is not a valid day schedule.  Objects should also typically check for “blank� schedules.
-
-### CheckScheduleValueMinMax
-
-Since you can’t always rely on a user to input the ScheduleType, the ScheduleManager can be used to check the minimum and/or maximum values for a schedule.
-
-LOGICAL FUNCTION **CheckScheduleValueMinMax**(ScheduleIndex,  &
-
-                       MinString,Minimum,MaxString,Maximum)
-
-The pair of specifications (MinString, Minimum) and (MaxString, Maximum) is optional -- only one set need be given.
-
-Examples from the code:
-
-USE ScheduleManager, ONLY: CheckScheduleValueMinMax
-
-. . .
-
-IF (.NOT. **CheckScheduleValueMinMax**(ScheduleIndex,'&gt;=',0.,'&lt;=',1.)) THEN
-
-  CALL ShowSevereError(RoutineName//trim(currentModuleObject)//’,’//  &
-
-    Trim(cAlphaFieldName(3))//’..’)
-
-  CALL ShowContinueError('Error found in schedule ='//TRIM(Alphas(3)))
-
-  CALL ShowContinueError('setpoint values must be (&gt;=0., &lt;=1.)')
-
-  ErrorsFound=.true.
-
-END IF
-
-### CheckScheduleValue
-
-There are times when the “CheckScheduleValueMinMax� will not be sufficient to verify proper values.  A good example is the “control type� schedules – valid values might be 0 through 4, but just checking the min/max will not tell you if it contains a specific value (say, 3).  This function allows you to check the entire schedule for a specific value – this will be more useful for discrete schedules than for schedule types of a continuous nature but can be used for both.
-
-LOGICAL FUNCTION CheckScheduleValue(ScheduleIndex,Value)
-
-Example of use:
-
- IF (**CheckScheduleValue**(CTIndex,REAL(SingleHeatingSetPoint))) THEN
-
-Here, the CTIndex is a schedule index for the Control Type schedules.  SingleHeatingSetPoint is an integer value for that control type.  “CheckScheduleValue� is used to determine if the schedule does, in fact, contain that value.
-
-### GetScheduleMinValue
-
-There are times when you don’t necessarily want to issue an error message but might like to find out what the minimum value of a given schedule is.  For example, if the schedule allowed for &gt;1 multipliers on a given input.
-
-FUNCTION GetScheduleMinValue(ScheduleIndex) RESULT(MinimumValue)
-
-Example of use:
-
-USE ScheduleManager, ONLY: GetScheduleMinValue
-
-. . .
-
-Value=**GetScheduleMinValue**(ScheduleIndex)
-
-The only argument needed is the ScheduleIndex for the schedule.  Note that all schedule values are stored as real numbers – if you have a discrete/integer valued schedule, you may wish to do some special checking of the min value.
-
-### GetScheduleMaxValue
-
-There are times when you don’t necessarily want to issue an error message but might like to find out what the maximum value of a given schedule is.  For example, if the schedule allowed for &gt;1 multipliers on a given input.
-
-FUNCTION GetScheduleMaxValue(ScheduleIndex) RESULT(MaximumValue)
-
-Example of use:
-
-USE ScheduleManager, ONLY: GetScheduleMaxValue
-
-. . .
-
-Value=**GetScheduleMaxValue**(ScheduleIndex)
-
-The only argument needed is the ScheduleIndex for the schedule.  Note that all schedule values are stored as real numbers – if you have a discrete/integer valued schedule, you may wish to do some special checking of the min value.
-
-### GetCurrentScheduleValue
-
-This function returns the current schedule value for the current day and time, given the schedule pointer as input.
-
-REAL FUNCTION GetCurrentScheduleValue(ScheduleIndex)
-
-Example of use:
-
-USE ScheduleManager, ONLY: GetCurrentScheduleValue
-
-. . .
-
-CloUnit = **GetCurrentScheduleValue**(People(PeopleNum)%ClothingPtr)
-
-
-
-Notice that the developer doesn’t have to keep track of hour of the day, day of the month, or month. The program does all of that. The only input needed is the pointer to the schedule.
-
-### GetScheduleValuesForDay
-
-This function returns the schedule values for a specific day, given the schedule index as input.
-
-SUBROUTINE GetScheduleValuesForDay(ScheduleIndex,DayValues,JDay)
-
-Example of use:
-
-    ALLOCATE(SVals1(24,NumOfTimeStepInHour))
-
-    SVals1=0.0
-
-    ...
-
-        DO JDay=1,366
-
-          CALL **GetScheduleValuesForDay**(CrossMixing(Loop)%SchedPtr,  &
-
-                                       SVals1,JDay)
-
-          IF (.not. ANY(SVals1&gt;0.0)) CYCLE
-
-        ...
-
-        END DO
-
-### GetSingleDayScheduleValues
-
-This function returns the schedule values for a specific day schedule (used in Design Day input, for example).
-
-SUBROUTINE GetSingleDayScheduleValues(DayScheduleIndex,DayValues)
-
-Example of use:
-
-   ALLOCATE (DDRelHumValues(TotDesDays,24,NumOfTimeStepInHour))
-
-   DDRelHumValues=0.0
-
-   ...
-
-    CALL **GetSingleDayScheduleValues**(DesDayInput(EnvrnNum)%RelHumSchPtr, &
-
-                                    DDRelHumValues(EnvrnNum,:,:))
-
-### LookUpScheduleValue
-
-This function can be used to look up a schedule value for the current time or optionally for any specific hour, timestep, day of year.
-
-REAL FUNCTION LookUpScheduleValue(ScheduleIndex, ThisHour, ThisTimeStep, ThisDayOfYear)
-
-...
-
-          ! FUNCTION ARGUMENT DEFINITIONS:
-
-  INTEGER ScheduleIndex
-
-  INTEGER, OPTIONAL :: ThisHour
-
-  INTEGER, OPTIONAL :: ThisTimeStep
-
-  INTEGER, OPTIONAL :: ThisDayOfYear
-
-Example of use:
-
-      SchValue=**LookUpScheduleValue**(Surface(SNR)%SchedShadowSurfIndex,IHOUR,TS)
-
-Data Services
--------------
-
-For the most part, modules are independent and only need the data they have within or **USE** from other modules.  Occasionally, this may take on more complicated needs such as accessing “real-time� values for meters and/or custom meters or current report variable names/values..  Meter names are standard; you may have to use user input to get custom meter names.
-
-### Global variable: MetersHaveBeenInitialized
-
-Meters are a bit peculiar and aren’t fully set until the first run through the first time step of the HVAC simulation.  Therefore, there is a global variable “MetersHaveBeenInitialized� which is set to **true** after meters have been set up.  If you have a call to your routine that must use meter values as part of the simulation, you must use this variable before your items can be set.
-
-Example:
-
-…
-
-If (MetersHaveBeenInitialized) CALL ManageDemand
-
-Only the first time step will be missed in your routine and that time step will be part of “warming up� the simulation, so there is minimal impact due to this limitation.
-
-### GetMeterIndex
-
-You use the GetMeterIndex to check if a meter is valid for a particular simulation or if the user has entered a custom meter of that name.  You use the index returned in later calls to get the value of the meter.  Returns 0 if there is no meter of that name.
-
-Example:
-
-INTEGER, EXTERNAL :: GetMeterIndex
-
-…
-
-thismeter=GetMeterIndex(‘Electricity:Facility’)
-
-### GetVariableKeyCountAndType
-
-This subroutine returns the variable type (real, integer, meter, etc.) (varType) whether it is an averaged or summed variable (varAvgSum), whether it is a zone or HVAC time step (varStepType), and the number of keynames for a given report variable or report meter name (varName).  The variable type (varType) and number of keys (numKeys) are used when calling subroutine GetVariableKeys to obtain a list of the keynames for a particular variable and a corresponding list of indexes.  An INTERFACE statement exists in the module OPInterfaces.
-
-Declaration:
-
-SUBROUTINE GetVariableKeyCountandType(varName, numKeys, varType,  &
-
-                                  varAvgSum, varStepType, varUnits)
-
-Example:
-
-USE OPInterfaces, ONLY: GetVariableKeyCountAndType
-
-    ! call the key count function but only need count during this pass
-
-    CALL GetVariableKeyCountandType(AlphArray(fldIndex),  &
-
-                 KeyCount,TypeVar,AvgSumVar,StepTypeVar,UnitsVar)
-
-    ALLOCATE(NamesOfKeys(KeyCount))
-
-    ALLOCATE(IndexesForKeyVar(KeyCount))
-
-### GetVariableKeys
-
-This subroutine returns a list of keynames and indexes associated with a particular report variable or report meter name (varName). This routine assumes that the variable type (real, integer, meter, etc.) may be determined by calling GetVariableKeyCountandType.  The variable type and index can then be used with function GetInternalVariableValue to to retrieve the current value of a particular variable/keyname combination.  An INTERFACE statement exists in the module OPInterfaces.
-
-Declaration:
-
-SUBROUTINE GetVariableKeys(varName,varType,keyNames,keyVarIndexes)
-
-
-
-Example:
-
-USE OPInterfaces, ONLY: GetVariableKeys
-
-CALL GetVariableKeys(AlphArray(fldIndex), TypeVar, NamesOfKeys,  &
-
-                    IndexesForKeyVar)
-
-! See earlier GetVariableKeyCountandType as well.
-
-### GetCurrentMeterValue
-
-You use the GetCurrentMeterValue to obtain the value of a meter at its last “reported value� (timestep).  Note that all meters are reported on the zone time step.  Returns 0.0 if the MeterNumber passed is &lt;=0.
-
-Example:
-
-INTEGER, EXTERNAL :: GetCurrentMeterValue
-
-…
-
-thismetervalue=GetCurrentMeterValue(ElecFacilityMtrIndex)
-
-### GetInstantMeterValue
-
-You use the GetInstantMeterValue to get a component of a meter’s value by index type. The values returned are “raw� (that is, not weighted by time step values).  In these calls, 1 is a zone time step index, 2 is a system time step index.
-
-Example:
-
-INTEGER, EXTERNAL :: GetInstantMeterValue
-
-…
-
-FuelType%ElecFacility = &    GetInstantMeterValue(FuelType%ElecFacilityIndex,1)\*FracTimeStepZone + &
-
-                                GetInstantMeterValue(FuelType%ElecFacilityIndex,2)
-
-### GetInternalVariableValue
-
-This function returns the current value of the Internal Variable assigned to the varType and keyVarIndex.  Values may be accessed for real and integer report variables and meter variables.  The variable type (varType) may be determined by calling subroutine and GetVariableKeyCountandType.  The index (keyVarIndex) may be determined by calling subroutine GetVariableKeys.  To use, there is an INTERFACE statement in DataGlobals.f90
-
-Example:
-
-USE DataGlobals, ONLY: GetInternalVariableValue
-
-
-
-      curValue = GetInternalVariableValue(curTypeOfVar,curVarNum)
-
-Other Useful Utilities
-----------------------
-
-### GetNewUnitNumber
-
-Rather than attempt to keep track of all open files and distribute this list to everyone, we have chosen to use a routine that does this operation.  If you need to have a scratch file (perhaps when porting legacy code into EnergyPlus modules), you can use the GetNewUnitNumber function to determine a logical file number for the OPEN and READ/WRITE commands.  The function works by looking at all open assigned files and returning a number that isn't being used.  This implies that you will OPEN the unit immediately after calling the function (and you should!).
-
-Example:
-
-INTEGER, EXTERNAL :: GetNewUnitNumber
-
-…
-
-myunit=GetNewUnitNumber()
-
-OPEN(Unit=myunit,File=’myscratch’)
-
-### FindUnitNumber
-
-If you want to find out a unit number for a file you think is already open, you can use the FindUnitNumber function.  For example, rather than creating a new unit for debug output, you could latch onto the same unit as currently used for the “eplusout.dbg� file.
-
-Example:
-
-INTEGER, EXTERNAL :: FindUnitNumber
-
-…
-
-myunit=FindUnitNumber(‘eplusout.dbg’)
-
-If that file is already opened, it will get back the unit number it is currently assigned to.  If it is not opened or does not exist, it will go ahead, get a unit number, and OPEN the file.  (Should not be used for Direct Access or Binary files!)
-
-### FindNumberinList
-
-Sometimes you would like to find a number in a list.  This is applicable to integers only (e.g. Index numbers of some item).
-
-Example:
-
-INTEGER, EXTERNAL :: FindNumberInList
-
-…
-
-MatchingCooledZoneNum =  &
-
-   **FindNumberinList**(CtrlZoneNum,  &
-
-     AirToZoneNodeInfo(AirLoopNum)%CoolCtrlZoneNums,NumZonesCooled)
-
-The location/index in the array **AirToZoneNodeInfo%CoolCtrlZoneNums** will be returned if it finds the number in the array.  If 0 is returned, it did not find that number in the list.
-
-### ValidateComponent
-
-Many objects specify a component type as well as a component name.  Or, an object might have only a component name.  The ValidateComponent routine will allow for objects outside the scope of a current “GetInput� routine to verify that the specific component does exist in the input file.
-
-SUBROUTINE ValidateComponent(CompType,CompName,IsNotOK,CallString)
-
-CompType, CompName are the typical nomenclature for “Component Type� (e.g. Fan:Simple:OnOff) and “Component Name� (e.g. “my fan� – user specified).  IsNotOk is a logical from the calling program that is set to true when the component is not on the input file.  CallString should specify the calling object – so that an appropriate error message can be issued.
-
-Example:
-
-  ! No USE needed – straightforward routine in GeneralRoutines
-
-  CALL **ValidateComponent**(Furnace(FurnaceNum)%FanType,  &
-
-                   Furnace(FurnaceNum)%FanName,IsNotOK,  &
-
-                   'Furnace:BlowThru:HeatOnly')
-
-  IF (IsNotOK) THEN
-
-    CALL ShowContinueError('In Furnace='//  &
-
-                         TRIM(Furnace(FurnaceNum)%Name))
-
-    ErrorsFound=.true.
-
-  ENDIF
-
-Note that in the example, the FanType is entered by the user.  This allows for ultimate flexibility though the example could also include appropriate fan types that are inherent to the code (an acceptable, if somewhat inflexible, practice).
-
-### CheckComponent
-
-This routine is exactly like ValidateComponent but doesn’t generate an error message.  It could be used instead of ValidateComponent and you could use the “IsNoOK� to generate your own error message.  However, the intended use is for checking out different components when you don’t have the component type as a field for the object.  Thus, you can easily check if there is an object (component type) with the name entered in your field.
-
-SUBROUTINE CheckComponent(CompType,CompName,IsNotOK)
-
-CompType, CompName are the typical nomenclature for “Component Type� (e.g. Fan:OnOff) and “Component Name� (e.g. “my fan� – user specified).  IsNotOk is a logical from the calling program that is set to true when the component is not on the input file.
-
-Example:
-
-  ! No USE needed – straightforward routine in GeneralRoutines
-
-  CALL **CheckComponent**('Furnace:BlowThru:HeatOnly',  &
-
-                   FurnaceRefName,IsNotOK)
-
-  IF (IsNotOK) THEN
-
-    CALL **CheckComponent**('Furnace:BlowThru:HeatCool',  &
-
-                   FurnaceRefName,IsNotOK)
-
-   . . . more checks on IsNotOK
-
-         ELSE
-
-           FurnaceType='Furnace:BlowThru:HeatOnly'
-
-  ENDIF
-
-. . .
-
-Note that in the example, the FurnaceRefName is entered by the user.  And this module knows what kind of components it might be.
-
-### CreateSysTimeIntervalString
-
-A very important part of EnergyPlus simulation is to be able to alert the user to problems during the simulation.  The CreateSysTimeIntervalString will help do that though a better use is the ShowContinueErrorTimeStamp routine.  The routine has no argument – a string is returned.  The example below also illustrates the preferred method of counting how many times an error is produced and not printing each occurrence.
-
-Example:
-
-USE General, ONLY: CreateSysTimeInterval
-
----
-
-!The warning message will be suppressed during the warm up days.
-
-If (.NOT.WarmUpFlag) Then
-
-  ErrCount = ErrCount + 1
-
-  IF (ErrCount &lt; 15) THEN
-
-    CALL ShowWarningError('SimAirLoops: Max iterations exceeded for '// &
-
-        TRIM(PrimaryAirSystem(AirLoopNum)%Name)//', at '//  &
-
-        TRIM(EnvironmentName)//', '//TRIM(CurMnDy)//' '//   &
-
-        TRIM(**CreateSysTimeIntervalString**()))
-
-  ELSE
-
-    IF (MOD(ErrCount,50) == 0) THEN
-
-      WRITE(CharErrOut,\*) ErrCount
-
-      CharErrOut=ADJUSTL(CharErrOut)
-
-      CALL ShowWarningError ('SimAirLoops: Exceeding max iterations’// &
-
-                            ‘ continues...'//CharErrOut)
-
-    ENDIF
-
-  ENDIF
-
-End If
-
-### TrimSigDigits
-
-Along with error messages to alert the user, oftentimes you’d like to include values that are in error.  You can use what some of the examples have shown – Write(string,\*) value but that will produce many digits in real numbers.  The TrimSigDigits routine will allow for easy modification to a set of digits.  Note that there are two flavors (INTERFACE statement in module General) so that you can easily get the string value of an integer.
-
-FUNCTION TrimSigDigits(RealValue,SigDigits) RESULT(OutputString)
-
-And
-
-FUNCTION TrimSigDigits(IntegerValue) RESULT(OutputString)
-
-As seen in the following example of use in code, a real value is passed in as argument 1 and the number of digits desired is passed in as argument 2.  Note that the routine will preserve any “E+xx� outputs when a value like .000000004 might be passed in.
-
-USE General, ONLY: TrimSigDigits
-
-. . .
-
-CALL ShowWarningError('COIL:Water:DetailedFlatCooling in Coil ='//  &
-
-                     TRIM(WaterCoil(coilNum)%Name))
-
-CALL ShowContinueError('Air Flow Rate Velocity has greatly exceeded ‘// &
-
-                       ‘upper design guildelines of ~2.5 m/s')
-
-CALL ShowContinueError('Air MassFlowRate[kg/s]='//  &
-
-                     TRIM(**TrimSigDigits**(AirMassFlow,6)))
-
-       AirVelocity=AirMassFlow\*AirDensity/WaterCoil(CoilNum)%MinAirFlowArea
-
-CALL ShowContinueError('Air Face Velocity[m/s]='//  &
-
-                     TRIM(**TrimSigDigits**(AirVelocity,6)))
-
-CALL ShowContinueError('Approximate MassFlowRate limit for Face ‘// &
-
-                       Area[kg/s]='//  &                              TRIM(**TrimSigDigits**(2.5\*WaterCoil(CoilNum)%MinAirFlowArea/AirDensity,6)))
-
-CALL ShowContinueError('COIL:Water:DetailedFlatCooling could be ‘// &
-
-                       ‘resized/autosized to handle capacity')
-
-CoilWarningOnceFlag(CoilNum) = .False.
-
-### RoundSigDigits
-
-Similar to TrimSigDigits, the RoundSigDigits function may be used when you want to “round� the output string – perhaps for reporting and/or error messages.  Note that there are two flavors (INTERFACE statement in module General) so that you can easily get the string value of an integer.
-
-FUNCTION RoundSigDigits(RealValue,SigDigits) RESULT(OutputString)
-
-And
-
-FUNCTION RoundSigDigits(IntgerValue) RESULT(OutputString)
-
-As seen in the following example of use in code, a real value is passed in as argument 1 and the number of digits desired is passed in as argument 2.    Note that the routine will preserve any “E+xx� outputs when a value like .000000004 might be passed in.
-
-USE General, ONLY: RoundSigDigits
-
-. . .
-
-    LatOut=**RoundSigDigits**(Latitude,2)
-
-    LongOut=**RoundSigDigits**(Longitude,2)
-
-    TZOut=**RoundSigDigits**(TimeZoneNumber,2)
-
-    NumOut=**RoundSigDigits**(Elevation,2)
-
-    PressOut=**RoundSigDigits**(StdBaroPress,0)
-
-    Write(OutputFileInits,LocFormat) Trim(LocationTitle),TRIM(LatOut),  &
-
-                                     TRIM(LongOut),  &
-
-                                     TRIM(TZOut),  &
-
-                                     TRIM(NumOut),  &
-
-                                     TRIM(PressOut)
-
-### SafeDivide
-
-SafeDivide can be used when you might not be sure that the denominator in a divide will not be zero.
-
-FUNCTION SafeDivide(a, b) RESULT (c)
-
-USE General, ONLY: SafeDivide
-
-. . .
-
-Result=SafeDivide(A,B)
-
-### SetupAndSort
-
-SetupAndSort can be called to order/sort a character array.  A companion index array goes along with it so that one does not have to supply an entire derived type to be sorted.  This companion array is then used to point to the proper element of such structures.
-
-SUBROUTINE SetupAndSort(CharacterList, iCharacterList)
-
-USE SortAndStringUtilities, ONLY: SetupAndSort
-
-. . .
-
-A use:
-
-ALLOCATE(iCharacterList(number of entries))
-
-Do item=1,number of entries
-
-  iCharacterList(item)=item
-
-end do
-
-
-
-! routine sorts this array and its companion
-
-CALL SetUpAndSort(CharacterList,iCharacterList)
-
-
-
-Do item=1,number of entries
-
-  ! iCharacterList now points to actual structure
-
-  Write(output,\*) Structure(iCharacterList(item))%Name
-
-Enddo
-
-
-
-Error Messages
---------------
-
-Several error message routines are provided for the developer, indicating three different levels of error severity: Show**Fatal**Error, Show**Severe**Error, Show**Severe**Message, Show**Warning**Error and Show**Warning**Message. Each takes a string as an argument. The string is printed out as the message body on the file “eplusout.err�. There are two additional optional arguments, which are file unit numbers on which the message will also be printed. In practice, most modules will not use either file unit number argument – but the Input Processor may use these to make sure some files contain a notice.  **ShowFatalError** causes the program to immediately abort.
-
-Two other error messages can be used to help make the error file more readable: ShowContinueError and ShowContinueErrorTimeStamp.  Finally, another similar ShowMessage call can be used to display an informative string to the error file (eplusout.err).
-
-As indicated, all of the “show� error calls look the same:
-
-SUBROUTINE **&lt;ErrorMessageCall&gt;**(ErrorMessage,OutUnit1,OutUnit2)
-
-Or
-
-SUBROUTINE **ShowWarningError**(ErrorMessage,OutUnit1,OutUnit2)
-
-SUBROUTINE **ShowWarningMessage**(ErrorMessage,OutUnit1,OutUnit2)
-
-SUBROUTINE **ShowSevereError**(ErrorMessage,OutUnit1,OutUnit2)
-
-SUBROUTINE **ShowSevereMessage**(ErrorMessage,OutUnit1,OutUnit2)
-
-SUBROUTINE **ShowFatalError**(ErrorMessage,OutUnit1,OutUnit2)
-
-SUBROUTINE **ShowContinueError**(ErrorMessage,OutUnit1,OutUnit2)
-
-SUBROUTINE **ShowContinueErrorTimeStamp**(ErrorMessage,OutUnit1,OutUnit2)
-
-SUBROUTINE **ShowMessage**(Message,OutUnit1,OutUnit2)
-
-As stated previously, you would likely never use either of the optional “OutUnit� arguments.  One use might be if you were, in addition to the normal EnergyPlus output files, writing your own output file that would be processed separately.
-
-Format of the error messages should be such that it makes it easy for the developer or user to realize the context of the error.  Obviously, it is usually easier for the developer as he/she can search the code for the error string, but hard for many users.  Current suggested format is to include the Module Name and/or the Routine name.  (see section Standard Message Format for more details). This is particularly useful when two or more places in the code have the same main error string but may mean different things: where one might be in a Plant Loop context and the other in a Condenser Loop context, for example.
-
-Due to the optional parameters, Interface statements are set in DataGlobals and you must enter USE statements defining which of the error calls you wish to use.
-
-Example:
-
-USE DataGlobals, ONLY: ShowSevereError
-
-. . .
-
-IF (Construct(ConstrNum)%LayerPoint(Layer) == 0) THEN
-
-   CALL ShowSevereError(‘Did not find matching material for construct ‘ &
-
-                        //TRIM(Construct(ConstrNum)%Name)// &
-
-                       ‘, missing material = ‘ &
-
-                       //TRIM(ConstructAlphas(Layer)))
-
-   ErrorsFound=.true.
-
-ENDIF
-
-This code segment will produce (with proper conditions) the message onto the error file:
-
-\*\* Warning \*\* Did not find matching material for construct XYZ, missing material = ABC
-
-The ShowContinueError is used in conjunction with either ShowSevereError or ShowWarningError.  The “~~~� characters represent the continuation:
-
-\*\* Warning \*\* The total number of floors, walls, roofs and internal mass surfaces in Zone ZONE ONE
-
-\*\*   ~~~   \*\* is &lt; 6. This may cause an inaccurate zone heat balance calculation.
-
-\*\* Warning \*\* No floor exists in Zone=ZONE ONE
-
-\*\* Warning \*\* Surfaces in Zone="ZONE ONE" do not define an enclosure.
-
-\*\*   ~~~   \*\* Number of surfaces is &lt;= 4 in this zone. View factor reciprocity forced
-
-The ShowContinueError is particularly useful with some of the previous routines that, in addition to signaling an error, produce their own error message.  For example, see the example code in the ValidateComponent excerpt above.  Note that no ShowContinueError should be used with the ShowFatalError as it immediately terminates the program.  Instead, a Severe-Continue-Fatal sequence should be used.
-
-Each GetInput routine is responsible for verifying its input.  Rather than terminating with the first illegal value, however, it is better to have an “ErrorsFound� logical that gets set to true for error conditions during the main routine processing and terminates at the end of the GetInput routine.  Of course during simulation, conditions should also be checked and terminated if necessary.  Try to give the user as much information as possible with the set of error routine calls.
-
-Quite a complex message can be constructed using concatenation. These routines can also be used to output numeric fields by writing the numeric variables to a string variable, although this isn’t very convenient.
-
-A good use of the ContinueErrorTimeStamp as well as “counting� errors is shown below:
-
-      IF(OutDryBulbTemp .LT. 0.0) THEN
-
-        CINErrCount1=CINErrCount1+1
-
-        IF (CINErrCount1 &lt; 15) THEN
-
-          CALL ShowWarningError('ElectricChillerModel:Air Cooled ‘// &
-
-                ‘Condenser Inlet Temperature below 0C')
-
-          CALL ShowContinueErrorTimeStamp('OutDoor Dry Bulb='//  &
-
-                      TRIM(RoundSigDigits(OutDryBulbTemp,2)//','))
-
-        ELSE
-
-          IF (MOD(CINErrCount1,50) == 0) THEN
-
-            WRITE(CINCharErrOut,\*) CINErrCount1
-
-            CINCharErrOut=ADJUSTL(CINCharErrOut)
-
-              CALL ShowWarningError('ElectricChillerModel:Air Cooled‘// &
-
-                   ‘ Condenser Inlet Temperature below 0C continues...' &
-
-                   //CINCharErrOut)
-
-          ENDIF
-
-        ENDIF
-
-      ENDIF
-
-### ShowWarningError, ShowWarningMessage
-
-Both of these calls produce messages onto the .err file that signal a warning:
-
-   \*\* Warning \*\* Processing Monthly Tabular Reports: PEAK SPACE GAINS
-
-The important difference between the two calls is that the “Error� call will incrase the “number of warnings� counter whereas the “Message� call does not incrase the counter.  The “Message� call can, therefore, be used ro “start� off a recurring sequence without disturbing the total warning count.  To do this, one would place the calls:
-
-CALL ShowWarningMessage(xxx)
-
-&lt;more messages that describe the basic problem&gt;
-
-CALL ShowRecurringWarningErrorAtEnd(xxx,msgindex)
-
-As indicated, this first call can also show significantly more information about the situation than will be captured by using the Recurring error sequence.
-
-### ShowSevereError, ShowSevereMessage
-
-Both of these calls produce messages onto the .err file that signal a warning:
-
-   \*\* Severe  \*\* Node Connection Error, Node="SOFC AIR INLET NODE", ZoneExhaust node did not find a matching inlet node.
-
-The important difference between the two calls is that the “Error� call will incrase the “number of severe errors� counter whereas the “Message� call does not incrase the counter.  The “Message� call can, therefore, be used ro “start� off a recurring sequence without disturbing the total warning count.  To do this, one would place the calls:
-
-CALL ShowSevereMessage(xxx)
-
-&lt;more messages that describe the basic problem&gt;
-
-CALL ShowRecurringSevereErrorAtEnd(xxx,msgindex)
-
-As indicated, this first call can also show significantly more information about the situation than will be captured by using the Recurring error sequence.
-
-### ShowFatalError
-
-This error terminates the program.
-
-   \*\*  Fatal  \*\* EMS user program halted simulation with error code = 9001.30
-
-For clarity, the sequence ending in the fatal error, should start with a Severe error and give the user a good indication of the problem.  During execution, this Severe error may immediately preceed the Fata call. During get input, errors may be found previously in the input, interspersed with Warning errors.  The last Severe error is stored and displayed as the program terminates.
-
-### ShowContinueError, ShowContinueErrorTimeStamp
-
-Continue errors are shown after the initial condition and formatted in a fashion that a post processor could detect and string all the errors about a single condition together.
-
-The basic format is simple:
-
-   \*\*   ~~~   \*\* ..Location object=DENVER STAPLETON INTL ARPT CO USA WMO=724690
-
-The continue error with time stemp adds the time stamp information to the initial message. (It also might show if the error occurred during “warmup�).
-
-   \*\*   ~~~   \*\*  CalcMultiSpeedDXCoil:lowspeedoutlet Occurrence info=Chicago Ohare Intl Ap IL USA TMY3 WMO\#=725300, 04/24 15:45 - 16:00
-
-### ShowMessage
-
-This call is strictly for informative messages that are displayed to the .err file. For example:
-
-   \*\*\*\*\*\*\*\*\*\*\*\*\* Beginning Zone Sizing Calculations
-
-   \*\*\*\*\*\*\*\*\*\*\*\*\* Beginning System Sizing Calculations
-
-   \*\*\*\*\*\*\*\*\*\*\*\*\* Testing Individual Branch Integrity
-
-   \*\*\*\*\*\*\*\*\*\*\*\*\* All Branches passed integrity testing
-
-The indicated messages help establish context for other errors that may be shown.
-
-### Recurring Error Handling
-
-One method of showing recurring errors is shown in the initial error section description with the illustration of counting the number of times the error occurs, printing the first few times and then only printing every x times (e.g. 100) that it occurs after that.
-
-In addition to that method, three routines will help you automate the task.  These routines rely on the error message being displayed and can also keep track of values (min/max/sum) (and units thereof). And an error message index (pointer to the message in the recurring error structure) that is stored in your data structure is used.
-
-
-
-SUBROUTINE ShowRecurringSevereErrorAtEnd(Message,MsgIndex,ReportMaxOf,ReportMinOf,ReportSumOf,  &
-
-                                           ReportMaxUnits,ReportMinUnits,ReportSumUnits)
-
-SUBROUTINE ShowRecurringWarningErrorAtEnd(Message,MsgIndex,ReportMaxOf,ReportMinOf,ReportSumOf, &
-
-                                           ReportMaxUnits,ReportMinUnits,ReportSumUnits)
-
-SUBROUTINE ShowRecurringContinueErrorAtEnd(Message,MsgIndex,ReportMaxOf,ReportMinOf,ReportSumOf, &
-
-                                           ReportMaxUnits,ReportMinUnits,ReportSumUnits)
-
-
-
-The first two parameters (Message, MsgIndex) are required.  The remaining six arguments (ReportMaxOf, ReportMinOf, ReportSumOf, ReportMaxUnits, ReportMinUnits, ReportSumUnits) are optional. To illustrate, we re-write the above call using the recurring error routines.  (Note that we still do the first few counted because we are using the TimeStamp routine – however a message buffer is set up in this instance.).
-
-!   Print warning messages only when valid and only for the first ocurrance. Let summary provide statistics.
-
-!   Wait for next time step to print warnings. If simulation iterates, print out
-
-!   the warning for the last iteration only. Must wait for next time step to accomplish this.
-
-!   If a warning occurs and the simulation down shifts, the warning is not valid.
-
-    IF(CurrentEndTime .GT. CurrentEndTimeLast .AND. TimeStepSys .GE. TimeStepSysLast)THEN
-
-      IF(ElectricChiller(ChillNum)%PrintMessage)THEN
-
-          ElectricChiller(ChillNum)%MsgErrorCount = &
-
-                           ElectricChiller(ChillNum)%MsgErrorCount + 1
-
-!       Show single warning and pass additional info to ShowRecurringWarningErrorAtEnd
-
-        IF (ElectricChiller(ChillNum)%MsgErrorCount &lt; 2) THEN
-
-           CALL ShowWarningError(TRIM(ElectricChiller(ChillNum)%MsgBuffer1)//'.')
-
-           CALL ShowContinueError(TRIM(ElectricChiller(ChillNum)%MsgBuffer2))
-
-        ELSE
-
-          CALL ShowRecurringWarningErrorAtEnd(TRIM(ElectricChiller(ChillNum)%MsgBuffer1)//' error continues.', &
-
-             ElectricChiller(ChillNum)%ErrCount1,ReportMaxOf=ElectricChiller(ChillNum)%MsgDataLast,  &
-
-             ReportMinOf=ElectricChiller(ChillNum)%MsgDataLast,ReportMaxUnits='[C]',ReportMinUnits='[C]')
-
-        END IF
-
-      END IF
-
-    END IF
-
-Illustrations of use of these calls is seen in the Chiller modules, PurchasedAir modules, DXCoil modules and others.
-
-Another example is seen in the Dessicant routines:
-
-  IF (Node(DesicDehum(DesicDehumNum)%RegenAirInNode)%MassFlowRate .NE. &
-
-               RegenAirMassFlowRate) THEN
-
-    ! Initialize standard air density
-
-    IF (MyOneTimeFlag) THEN
-
-      RhoAirStdInit = PsyRhoAirFnPbTdbW(StdBaroPress,20.0,0.0)
-
-    ENDIF
-
-    CALL **ShowRecurringSevereErrorAtEnd**( &
-
-      'Improper flow delivered by desiccant regen fan - RESULTS INVALID!
-
-             Check regen fan capacity and schedule.', &
-
-           DesicDehum(DesicDehumNum)%RegenFanErrorIndex1)
-
-    CALL **ShowRecurringContinueErrorAtEnd**( &
-
-           TRIM(DesicDehum(DesicDehumNum)%DehumType)//'='//  &
-
-             TRIM(DesicDehum(DesicDehumNum)%Name), &
-
-           DesicDehum(DesicDehumNum)%RegenFanErrorIndex2)
-
-    RhoAirStdInit = PsyRhoAirFnPbTdbW(StdBaroPress,20.0,0.0)
-
-    CALL **ShowRecurringContinueErrorAtEnd**( &
-
-           TRIM('Flow requested [m3/s] from '//  &
-
-            DesicDehum(DesicDehumNum)%RegenFanType)//'='// &
-
-           TRIM(DesicDehum(DesicDehumNum)%RegenFanName), &
-
-           DesicDehum(DesicDehumNum)%RegenFanErrorIndex3, &
-
-           **ReportMaxOf**=(RegenAirMassFlowRate / RhoAirStdInit))
-
-    CALL **ShowRecurringContinueErrorAtEnd**( &
-
-           'Flow request varied from delivered by [m3/s]', &
-
-           DesicDehum(DesicDehumNum)%RegenFanErrorIndex4, &
-
-    **ReportMaxOf**=((RegenAirMassFlowRate - Node(DesicDehum(DesicDehumNum)%RegenAirInNode)%MassFlowRate)/ RhoAirStdInit), &
-
-    **ReportMinOf**=((RegenAirMassFlowRate - Node(DesicDehum(DesicDehumNum)%RegenAirInNode)%MassFlowRate)/ RhoAirStdInit))
-
-  ENDIF
-
-### Standard Message Format
-
-With the advent of using the field names as provided from the Input Processor, some of the message formatting has gotten easier for the developer, but harder for the person who might be searching the code to determine a user’s problem.
-
-Suggestion is that the error messages contain the Routine Name. And, for get input routines, the initial portion contain the Object Name and the Name of the object.  For example,
-
-\*\* Warning \*\* GetPlantLoopData/GetPlantAvailabilityManager: AvailabilityManagerAssignmentList=ALWAYS\_ON not found in lists.  No availability will be used.
-
-Similarly, note that this is a summary message after surfaces have been gotten:
-
-\*\* Warning \*\* GetSurfaceData:The total number of floors, walls, roofs and internal mass surfaces in Zone GARAGE ZONE
-
-\*\*   ~~~   \*\* is &lt; 6. This may cause an inaccurate zone heat balance calculation.
-
-Not all of the code is using this style yet.
-
-Display Strings
----------------
-
-Two display routines are useful for displaying to the “run� log the progress of the simulation.  Since EnergyPlus usually runs as a “console� mode application, users may monitor progress of the simulation.  Thus, at times it is useful to have messages displayed there.  These should be minimal in number though can be used effectively during debugging of new modules.
-
-  subroutine DisplayString(String)
-
-  subroutine DisplayNumberandString(Number,String)
-
-The “String� parameters are normal strings.  The “Number� parameter must be an integer.
-
-
-
-Performance Curve Services
---------------------------
-
-Some HVAC equipment models in EnergyPlus use performance curves. These are polynomials in one or two independent variables that are used to modify rated equipment performance for performance at the current, off-rated conditions. Most often the curves are functions of temperature – entering wetbulb and outside drybulb, for instance – or of the part load fraction. EnergyPlus provides services to input, store, and retrieve curve data and to evaluate curves given values of the independent variables. There are 3 curve objects: CURVE:QUADRATIC, CURVE:CUBIC, and CURVE:BIQUADRATIC.
-
-### GetCurveIndex
-
-This function takes a curve name as input and returns an internal pointer to the curve. Curve values will always be accessed via the pointer not the name during the simulation for reasons of efficiency. This function is usually called once for each curve during the input phase.
-
-USE CurveManage, ONLY: GetCurveIndex
-
-. . .
-
-DXCoil(DXCoilNum)%CCapFTemp = **GetCurveIndex**(Alphas(5))
-
-  IF (DXCoil(DXCoilNum)%CCapFTemp .EQ. 0) THEN
-
-    CALL ShowSevereError('COIL:DX:BF-Empirical not found=’ &
-
-                         //TRIM(Alphas(5)))
-
-    ErrorsFound = .TRUE.
-
-  END IF
-
-### GetCurveCheck
-
-This function uses a curve name as well as an error indicator and object name to “get� a curve index and perform error checking in one call.  The calling routine will need to check the value of the error flag and perform appropriate action.
-
-FUNCTION GetCurveCheck(alph, errFlag, ObjName)  &
-
-             RESULT (GetCurveCheckOut)
-
-The curve index (as in GetCurveIndex) is the result. Curve values will always be accessed via the pointer not the name during the simulation for reasons of efficiency. This function would be called during an input phase for an object.
-
-USE CurveManager, ONLY: GetCurveCheck
-
-...
-
-GasAbsorber(AbsorberNum)%CoolCapFTCurve      =   &
-
-      **GetCurveCheck**(AlphArray(8),  ErrorsFound, ChillerName)
-
-GasAbsorber(AbsorberNum)%FuelCoolFTCurve     =   &
-
-      **GetCurveCheck**(AlphArray(9),  ErrorsFound, ChillerName)
-
-### GetCurveType
-
-This function will tell the calling routine what the “curve type� that was input.  This function may be useful if your module does different calculations depending on a curve type (i.e. cubic vs quadratic) or if it should not use a specific curve type.  This function would be called during input phase for an object.
-
-CHARACTER(len=20) FUNCTION GetCurveType (CurveIndex)
-
-Example of use:
-
-USE CurveManager,   ONLY: GetCurveIndex, GetCurveType
-
-…
-
-SELECT CASE(**GetCurveType**(DXCoil(DXCoilNum)%CCapFTemp))
-
-### CurveValue
-
-This function takes the curves index and one or two independent variables as input and returns the curve value.
-
-USE CurveManage, ONLY: CurveValue
-
-. . .
-
-!  Get total capacity modifying factor (function of temperature)
-
-!  for off-rated conditions
-
-50 TotCapTempModFac = **CurveValue**(DXCoil(DXCoilNum)%CCapFTemp,
-                                  InletAirWetbulbC, &
-                                  OutDryBulbTemp)
-
-
-
-Fluid Property Services
------------------------
-
-Fluid property routines have been implemented within EnergyPlus with the goal of making the specification of new fluids relatively easy for the user and not require the user to specify data for the most common loop fluids.  Common refrigerants are listed within an extensive Reference Data Set (RDS) that is provided with the EnergyPlus program.
-
-Fluids in EnergyPlus are broken into two categories: **refrigerants** and **glycols**.  This relates back to the amount of information needed to determine the properties of the various fluid types inside the program.  The decision to define or use one class of fluids or another relates back to whether or not one expects the fluid to change phase (liquid and/or vapor) or remain a liquid.  When a developer feels that a fluid may change phase, all code should access the Refrigerant class of fluid property routines.  When the developer is certain that the fluid will remain a liquid and wishes to abide by that assumption (generally, this is the case for most larger loops), all code from such modules should access the Glycol class of fluid property routines.  Each of these classes will be described in separate sections below since each class has different subroutine access to the main module.
-
-Internally, both the refrigerant and glycol classes of fluids use “table lookup� and interpolation to find the appropriate value of a fluid property.  No curve fits are done internally and the interpolation search routines are currently not optimized (no interval halving or special fast searching techniques are used to find the values).
-
-HOWEVER, if values out of range (too low or too high) are passed to the routines, the value returned is a valid value at the lowest or highest (respectively) input parameter (that was passed in out of range).
-
-You will also note in the succeeding descriptions that IP units can be entered by some editors (IDF Editor) using predefined unit conversions.
-
-### Using Fluid Property Routines in EnergyPlus Modules
-
-The routines are contained within a single module:**FluidProperties.f90**
-
-Developers can use the routines anywhere inside EnergyPlus through the following USE statement:
-
-**USE FluidProperties**
-
-Access to this module may be limited by expanding this line of code with the ONLY designator.
-
-### Fluid Properties Functions for Refrigerant Class Fluids
-
-In EnergyPlus, a refrigerant fluid is capable of being either in the liquid or vapor phase.  Due to this definition, data must be available for both of these regions in order for the program to accurately calculate the various fluid properties.  There are eight possible functions that may be used to obtain refrigerant data using the Fluid Properties module.  They include:
-
-**GetSatPressureRefrig**(Refrigerant,Temperature,RefrigIndex,calledfrom)
-
-**GetSatTemperatureRefrig** (Refrigerant,Pressure,RefrigIndex,calledfrom)
-
-**GetSatEnthalpyRefrig** (Refrigerant,Temperature,Quality,RefrigIndex,calledfrom)
-
-**GetSatDensityRefrig** (Refrigerant,Temperature,Quality,RefrigIndex,calledfrom)
-
-**GetSatSpecificHeatRefrig** (Refrigerant,Temperature,Quality,RefrigIndex,calledfrom)
-
-**GetSupHeatEnthalpyRefrig** (Refrigerant,Temperature,Pressure,RefrigIndex,calledfrom)
-
-**GetSupHeatPressureRefrig** (Refrigerant,Temperature,Enthalpy,RefrigIndex,calledfrom)
-
-**GetSupHeatDensityRefrig** (Refrigerant,Temperature,Pressure,RefrigIndex,calledfrom)
-
-While most of the variables passed into the routine are self-explanatory, the three variables that are common to each of these functions are Refrigerant, RefrigIndex and calledfrom.  **Refrigerant** in this case is the character string name of the refrigerant in question as listed in the input file using the FluidNames object.  This must be passed into the function to identify the fluid being referenced.  **RefrigIndex** is an internal variable.  On the first call to the fluid property routine, it is zero.  All of the fluid property routines are set-up to find a non-zero index in the local fluid property data structure that corresponds to this refrigerant name.  Since finding the proper fluid from the fluid name each and every time is computationally slow, the index allows the code to quickly find the right data without doing an inordinate number of string comparisons.  Thus, module developers should store the RefrigIndex in their own local data structure in addition to the refrigerant name. calledfrom is a string variable passed to the routine so that error messages coming from the above functions can give a better context for errors when they happen.
-
-Units for these other variables in these function calls are: Joules per kilogram for enthalpy, degrees Celsius for temperature, Pascals for pressure, kilograms per cubic meter for density, and Joules per kilogram-degree Celsius for specific heat.  Quality and concentration are dimensionless fractions.  All variables are considered input variables.
-
-Module developers should use the functions listed above to first determine whether they are in the saturated region or the superheated region.  The GetSatPressureRefrig and GetSatTemperatureRefrig functions should assist the users in determining whether they are in or beyond the saturated region.  Once this is determined, the developer can call the appropriate function to obtain the quantity of interest: in the saturated region this includes the enthalpy, density, or specific heat; in the superheated region this includes the enthalpy, pressure, or density.
-
-### Reference Data Set (RDS) Values for Refrigerant Class Fluids
-
-The data for refrigerants that are included in the reference data set that comes with EnergyPlus are as follows (temperatures in Celsius, pressure in MegaPascals):
-
-Table 3.  Regions for Fluid Properties
-
-<table class="table table-striped">
-<tr>
-<td>Refrigerant</td>
-<td>Sat. Temp range {C}</td>
-<td>Super Temp range* {C}</td>
-<td>Super Pressure range* {Pa}</td>
-</tr>
-<tr>
-<td>R11</td>
-<td>-110 to 198</td>
-<td>-110 to 255</td>
-<td>6.8 to 1.6E6</td>
-</tr>
-<tr>
-<td>R11(specheat)</td>
-<td>-110 to 190</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>R12</td>
-<td>-157 to 112</td>
-<td>-156 to 169</td>
-<td>.3 to 1.6E7</td>
-</tr>
-<tr>
-<td>R12(specheat)</td>
-<td>-157 to 104</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>R22</td>
-<td>-157 to 96</td>
-<td>-157 to 153</td>
-<td>0.4 to 1.7E7</td>
-</tr>
-<tr>
-<td>R22(specheat)</td>
-<td>-157 to 88</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>R123</td>
-<td>-107 to 184</td>
-<td>-106 to 240</td>
-<td>4.9 to 1.5E7</td>
-</tr>
-<tr>
-<td>R134a</td>
-<td>-103 to 101</td>
-<td>-103 to 158</td>
-<td>400 to 1.6E7</td>
-</tr>
-<tr>
-<td>R404a</td>
-<td>-72 to 72</td>
-<td>-72 to 72</td>
-<td>2.3E4 to 3.7E6</td>
-</tr>
-<tr>
-<td>R410a</td>
-<td>-72 to 69</td>
-<td>-72 to 69</td>
-<td>3.1E4 to 4.7E6</td>
-</tr>
-<tr>
-<td>R507a</td>
-<td>-72 to 69</td>
-<td>-72 to 69</td>
-<td>2.5E4 to 3.6E6</td>
-</tr>
-<tr>
-<td>NH3</td>
-<td>-77 to 132</td>
-<td>-77 to 189</td>
-<td>6.3E3 to 2.2E7</td>
-</tr>
-<tr>
-<td>NH3(specheat)</td>
-<td>-73 to 124</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Steam</td>
-<td>0 to 370</td>
-<td>0 to 500</td>
-<td>610 to 4.0E8</td>
-</tr>
-<tr>
-<td>Steam(specheat)</td>
-<td>0 to 370</td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-\*Obviously data for all temperatures at all pressures isn't loaded.  The entire range of pressures given above will work, but the temperature range for a given pressure will be some subset of the Super Temp range shown above.
-
-Subcooled region actually only returns h(f) or the saturated liquid value at the temperature you input.
-
-### Fluid Property Data and Expanding the Refrigerants Available to EnergyPlus
-
-The Fluid Property routines have been reengineered to allow other users to add refrigerants to the input file without having to make any changes to the program code.  The only requirement on input is that in order to add a new refrigerant, a user must enter a full set of data.  The exact definition of a full set of data is given below.
-
-As with all EnergyPlus input, the fluid properties data has both an input data description and a reference data set that must show up in the input file.  All of the “standard� refrigerants listed above must show up in the in.idf file for it to be available to the rest of the simulation.  Below is the description of the input data description syntax for the fluid properties entries.
-
-The first syntax item lists all of the fluids present in an input file and categorizes them as either a refrigerant (such as R11, R12, etc.) or a glycol (such as ethylene glycol, propylene glycol, etc.).  A refrigerant or glycol must be in this list in order to be used as a valid fluid in other loops in the input file.
-
-**FluidProperties:Names,**
-
-       \\unique-object
-
-       \\extensible:2 repeat last two fields
-
-       \\memo list of potential fluid names/types in the input file, maximum of ten
-
-  A1,  \\field Fluid 1 Name
-
-       \\type alpha
-
-  A2,  \\field Fluid 1 Type
-
-       \\type choice
-
-       \\key Refrigerant
-
-       \\key Glycol
-
-  A3,  \\field Fluid 2 Name
-
-       \\type alpha
-
-  A4,  \\field Fluid 2 Type
-
-       \\type choice
-
-       \\key Refrigerant
-
-       \\key Glycol
-
-  A5,  \\field Fluid 3 Name
-
-       \\type alpha
-
-  A6,  \\field Fluid 3 Type
-
-       \\type choice
-
-       \\key Refrigerant
-
-       \\key Glycol
-
-An example of this statement in an input data file is:
-
-FluidProperties:Names,
-
-  R11, REFRIGERANT,
-
-  R12, REFRIGERANT,
-
-  R22, REFRIGERANT,
-
-  NH3, REFRIGERANT,
-
-  Steam, REFRIGERANT,
-
-  NewGlycol, GLYCOL,
-
-  SuperGlycol, GLYCOL;
-
-All fluid properties vary with temperature.  As a result, the following syntax allows the user to list the temperatures at which the data points are valid.  Since in many cases, the temperatures will be similar, this provides a more compact input structure and avoids listing the temperatures multiple times.  The name associated with the temperature list is the piece of information that will allow the actual fluid property data statements to refer back to or link to the temperatures.  Up to 250 points may be entered with this syntax and temperatures must be entered in ascending order.  Units for the temperatures are degrees Celsius.  The same temperature list may be used by more than one refrigerant.
-
-**FluidProperties:Temperatures,**
-
-      \\memo property values for fluid properties
-
-      \\memo list of up to 250 temperatures, note that number of property values must match the number of properties
-
-      \\memo in other words, there must be a one-to-one correspondence between the property values in this list and
-
-      \\memo the actual properties list in other syntax
-
-      \\memo degrees C (for all temperature inputs)
-
-      \\format FluidProperty
-
-  A1, \\field Name
-
-      \\type alpha
-
-  N1, \\field Temperature 1
-
-      \\type real
-
-      \\units C
-
-&lt; same thing repeated over and over again&gt;
-
-  N250; \\field Temperature 250
-
-        \\type real
-
-An example of this statement in an input data file is:
-
-FluidProperties:Temperatures,
-
-      R11Temperatures,
-
-      -70,-65,-60,-55,-50,-45,-40,-35,-30,-25,-20,-15,-10,-5,0,2,4,6,8,10,12,14,16,18,
-
-      20,22,24,26,28,30,32,34,36,38,40,42,44,46,48,50,55,60,65,70,75,80,85,90,95,100,
-
-      105,110,115,120,125,130,135,140,145,150,155,160,165,170,175,180,185,190,198;
-
-Property data for the saturated region is entered with the following syntax.  Before the actual data is entered, this line of input must identify the refrigerant the data is to be associated with, what the data represents (choice of one of three keywords), the phase of the data (either fluid or gas), and the temperature list reference that links each data point with a temperature.
-
-**FluidProperties:Saturated,**
-
-      \\memo fluid properties for the saturated region
-
-      \\format FluidProperty
-
-  A1, \\field Name
-
-      \\type object-list
-
-      \\object-list FluidNames
-
-  A2, \\field Fluid Property Type
-
-      \\note Enthalpy Units are J/kg
-
-      \\note Density Units are kg/m3
-
-      \\note SpecificHeat Units are J/kg-K
-
-      \\note Pressure Units are Pa
-
-      \\type choice
-
-      \\key Enthalpy     ! Units are J/kg
-
-      \\key Density      ! Units are kg/m3
-
-      \\key SpecificHeat ! Units are J/kg-K
-
-      \\key Pressure     ! Units are Pa
-
-  A3, \\field Fluid Phase
-
-      \\note Fluid=saturated fluid
-
-      \\note FluidGas=saturated vapor
-
-      \\type choice
-
-      \\key Fluid        ! saturated fluid
-
-      \\key FluidGas     ! saturated vapor
-
-  A4, \\field Temperature Values Name
-
-      \\note Enter the name of a FluidProperties:Temperatures object.
-
-      \\type object-list
-
-      \\object-list FluidPropertyTemperatures
-
-  N1, \\field Property Value 1
-
-      \\type real
-
-      \\unitsBasedOnField A2
-
-  N2, \\field Property Value 2
-
-      \\type real
-
-      \\unitsBasedOnField A2
-
-&lt; same thing repeated over and over again&gt;
-
-  N250; \\field Property Value 250
-
-        \\type real
-
-        \\unitsBasedOnField A2
-
-An example of this statement in an input data file is:
-
-FluidProperties:Saturated,
-
-      R11,ENTHALPY,FLUID,R11Temperatures, ! Enthalpy in J/kg
-
-      153580,154600,156310,158580,161300,164380,167740,171330,175100,179020,183060,
-
-      187190,191400,195680,200000,201740,203490,205240,207000,208770,210530,212310,
-
-      214080,215870,217650,219860,221230,223030,224830,226630,228860,230250,232060,
-
-      233860,235700,237520,239350,241180,243010,246350,249450,254080,258730,263480,
-
-      268110,272860,277000,282410,287240,292120,297030,302000,307090,312080,317210,
-
-      322400,327670,333020,338460,344010,349680,355500,361480,367690,374100,381060,
-
-      388850,397280,426300;
-
-The format of the data for the superheated region is almost identical to that of the saturated region with one addition—a pressure.  The pressure is listed before the rest of the data and has units of Pa.
-
-**FluidProperties:Superheated,**
-
-      \\memo fluid properties for the superheated region
-
-      \\format FluidProperty
-
-  A1, \\field Fluid Name
-
-      \\type object-list
-
-      \\object-list FluidNames
-
-  A2, \\field Fluid Property Type
-
-      \\note Enthalpy Units are J/kg
-
-      \\note Density Units are kg/m3
-
-      \\type choice
-
-      \\key Enthalpy     ! Units are J/kg
-
-      \\key Density      ! Units are kg/m3
-
-  A3, \\field Temperature Values Name
-
-      \\note Enter the name of a FluidProperties:Temperatures object.
-
-      \\type object-list
-
-      \\object-list FluidPropertyTemperatures
-
-  N1, \\field Pressure
-
-      \\note pressure for this list of properties
-
-      \\type real
-
-      \\units Pa
-
-      \\minimum&gt; 0.0
-
-  N2, \\field Property Value 1
-
-      \\type real
-
-      \\unitsBasedOnField A2
-
-  N3, \\field Property Value 2
-
-      \\type real
-
-      \\unitsBasedOnField A2
-
-&lt; same thing repeated over and over again&gt;
-
-  N250; \\field Property Value 250
-
-        \\type real
-
-       \\unitsBasedOnField A2
-
-An example of this statement in an input data file is:
-
-FluidProperties:Superheated,
-
-    R11,DENSITY,SuperR11Temperatures, ! Density in kg/m^3
-
-    62000., !Pressure = 62000Pa
-
-    0,0,0,0,0,0,0,0.0139,0.0134,0.0129,0.0124,0.012,0.0116,0.0112,0.0109,0.0105,
-
-    0.0102,0.0099,0.0097,0.0094,0.0092,0.0089,0,0,0,0,0,0,0,0,0,0;
-
-### Fluid Properties Functions for Glycol Class Fluids
-
-In EnergyPlus, a glycol fluid is assumed to remain in the liquid phase.  As a result, data is only required for fluids in the liquid state.  There are four possible functions that may be used to obtain glycol data using the Fluid Properties module.  These correspond to the fluid property of interest and include:
-
-**GetSpecificHeatGlycol** (Glycol,Temperature,GlycolIndex,calledfrom)
-
-**GetConductivityGlycol** (Glycol,Temperature,GlycolIndex,calledfrom)
-
-**GetDensityGlycol** (Glycol,Temperature,GlycolIndex,calledfrom)
-
-**GetViscosityGlycol** (Glycol,Temperature,GlycolIndex,calledfrom)
-
-All of these functions are used in exactly the same way.  The module developer should send the glycol name (as listed in the GlycolConcentrations object in the input file) to the routine and the GlycolIndex (sent as 0 the first time and then set by the fluid property routine; see RefrigIndex discussion above).  The calledfrom parameter is also used as discussed in the Refrigerant parameter discussion above. In addition, the functions require the temperature of the glycol in degrees Celsius.
-
-### Default Values for Glycol Class Fluids
-
-There are default values for specific heat, density, conductivity, and viscosity for Water, Ethylene Glycol, and Propylene Glycol.  This means that if users accept the values as published in the ASHRAE Handbook of Fundamentals, then the only information the user must include in their input file is a description of the concentration of glycol used (via the GlycolConcentrations object).  If water is used in a loop, the user does not need to enter anything other than WATER as the fluid type in the appropriate input syntax.  Data for various concentrations of these three default fluids encompasses the range over with these fluids and their combinations are in the liquid phase (-35 to 125 degrees Celsius).  When the glycol combination in question is indeed a fluid, the functions will return the appropriate value for the parameter in question.  If the glycol is either a solid or vapor, the routine will return a zero value.  Units for the different properties are: Joules per kilogram-Kelvin for specific heat, Pascal-seconds for viscosity, Watts per meter-Kelvin for conductivity, and kilograms per cubic meter for density.  In contrast to the refrigerant data which is included in the RDS and must be copied into the user input file if it is to be used, the glycol default data has been hardwired into EnergyPlus and does not need to be entered into the input file.
-
-### Fluid Property Data and Expanding the Glycols Available to EnergyPlus
-
-The format of the data for the glycols is almost identical to that of the superheated region for refrigerants with one exception—concentration replaces pressure.  The concentration is listed before the rest of the data and is dimensionless.
-
-**FluidProperties:Concentration,**
-
-      \\memo fluid properties for water/other fluid mixtures
-
-      \\format FluidProperty
-
-  A1, \\field Fluid Name
-
-      \\type object-list
-
-      \\object-list FluidNames
-
-      \\note should not be any of the defaults (Water, EthyleneGlycol, or PropyleneGlycol)
-
-  A2, \\field Fluid Property Type
-
-      \\note Density Units are kg/m3
-
-      \\note SpecificHeat Units are J/kg-K
-
-      \\note Conductivity Units are W/m-K
-
-      \\note Viscosity Units are N-s/m2
-
-      \\type choice
-
-      \\key Density      ! Units are kg/m3
-
-      \\key SpecificHeat ! Units are J/kg-K
-
-      \\key Conductivity ! Units are W/m-K
-
-      \\key Viscosity    ! Units are N-s/m2
-
-  A3, \\field Temperature Values Name
-
-      \\note Enter the name of a FluidProperties:Temperatures object.
-
-      \\type object-list
-
-      \\object-list FluidPropertyTemperatures
-
-  N1, \\field Concentration
-
-      \\note Glycol concentration for this list of properties entered as a fraction
-
-      \\type real
-
-      \\units dimensionless
-
-      \\minimum 0.0
-
-      \\maximum 1.0
-
-  N2, \\field Property Value 1
-
-      \\type real
-
-      \\unitsBasedOnField A2
-
-  N3, \\field Property Value 2
-
-      \\type real
-
-      \\unitsBasedOnField A2
-
-&lt; same thing repeated over and over again&gt;
-
-  N250; \\field Property Value 250
-
-        \\type real
-
-       \\unitsBasedOnField A2
-
-An example of this statement in an input data file is:
-
-FluidProperties:Concentration,
-
-     MyPropyleneGlycol,SPECIFICHEAT ,GlycolTemperatures, ! Specific heat in J/kg-K
-
-     0.8, ! Concentration
-
-     2572,2600,2627,2655,2683,2710,2738,2766,2793,2821,2849,2876,2904,2931,2959,
-
-     2987,3014,3042,3070,3097,3125,3153,3180,3208,3236,3263,3291,3319,3346,3374,
-
-     3402,3429,3457;
-
-The above input syntax is used to define data for a particular new fluid beyond the default glycol fluids.  It would be repeated at other appropriate concentration values, if necessary, to define the fluid.  It should be noted that in order to enter a fluid, the user must specify all four of the properties: conductivity, specific heat, viscosity, and density.
-
-In addition to specifying the raw data for a new glycol, the user must list the fluid in the FluidNames object and then specify the concentration in the GlycolConcentrations object as shown below:
-
-FluidProperties:Names,
-
-  MyPropyleneGlycol, GLYCOL;
-
-GlycolConcentrations,
-
-  MyPropyleneGlycol, GLYCOL;
-
-The IDD description for the FluidProperties:GlycolConcentrations object is given below:
-
-**FluidProperties:GlycolConcentrations,**
-
-       \\unique-object
-
-       \\memo list of glycols and what concentration they are, maximum of ten
-
-  A1,  \\field Fluid 1 Name
-
-       \\type alpha
-
-       \\reference GlycolConcentrations
-
-  A2,  \\field Glycol 1 Name
-
-       \\type choice
-
-       \\key EthyleneGlycol
-
-       \\key PropyleneGlycol
-
-       \\memo or UserDefined Fluid (must show up as a glycol in FluidProperties:Names list)
-
-  N1,  \\field Glycol 1 Concentration
-
-       \\type real
-
-       \\minimum 0.0
-
-       \\maximum 1.0
-
-  A3,  \\field Fluid 2 Name
-
-       \\type alpha
-
-       \\reference GlycolConcentrations
-
-&lt; . . . repeated up to 10 times . . .&gt;
-
-  A19, \\field Fluid 10 Name
-
-       \\type alpha
-
-  A20, \\field Glycol 10 Name
-
-       \\type choice
-
-       \\key EthyleneGlycol
-
-       \\key PropyleneGlycol
-
-       \\memo or UserDefined Fluid (must show up as a glycol in FluidProperties:Names list)
-
-  N10; \\field Glycol 10 Concentration
-
-       \\type real
-
-       \\minimum 0.0
-
-       \\maximum 1.0
-
-An example of how this would be used in an actual IDF is:
-
-FluidProperties:GlycolConcentrations,
-
-  MyProGly80Percent,  !- fluid name 1
-
-  MyPropyleneGlycol,  !- glycol name 1
-
-  0.8,
-
-  EthGly30Percent,  !- fluid name 2
-
-  EthyleneGlycol,  !- glycol name 2
-
-  0.3;  !- concentration 2
-
-The key relationship in this syntax is how FluidNames relates to GlycolConcentrations and how to have modules access through the proper name.  FluidNames are used to define raw data, whether for refrigerants or glycols.  With a glycol, it is not enough to define raw data since this does not necessarily define the actual concentration of glycol being used.  Thus, the GlycolConcentrations object is needed.  It defines a name for the actual glycol and then refers back to the FluidNames (first fluid listed in the above example) or to one of the default glycol fluids (second fluid listed in the above example).  It is critical that module developers refer to the “fluid name� listed in the GlycolConcentrations object.  This is the name used inside the fluid property module to access the proper data.  Note that when the GlycolConcentrations object is read in during execution that the module will interpolate down from a two-dimensional array of data (variation on temperature and concentration) to a one-dimensional array of data (with temperature as the only independent variable, concentration of a glycol fluid on any loop is assumed to be constant).  This means that only the temperature (along with the glycol fluid name and index) must be passed into the fluid property module and also saves execution time since only a one-dimensional interpolation is needed.
-
-Weather Services
-----------------
-
-All weather data (including SizingPeriod:DesignDay and Site:Location validation) are processed by the WeatherManager module.  The SimulationManager invokes the WeatherManager at the proper times to retrieve data.  The WeatherManager will retrieve the proper data for the current timestep/hour/day/month from the proper data source (design day definition, weather data file).  The WeatherManager puts weather-type data (outside dry bulb, outside wet bulb, humidity, barometric pressure) into the DataEnvironment global data area.  There is no need for other modules to call the WeatherManager directly.  However, if there is some weather-type data that is needed and not provided in the DataEnvironment global area, contact us.
-
-Global Data: Flags and Parameters
----------------------------------
-
-Global data is used sparsely in EnergyPlus, according to our goals and programming standards.  Data-only modules should be used to share data, usually across a limited number of other modules.  Two critical data-only modules have been used:
-
-**DataGlobals** – contains truly global data (such as number of zones, current hour, simulation status flags, interface statements to error and output routines)
-
-**DataEnvironment** – contains weather data that is global (such as current outdoor dry-bulb temperature, barometric pressure, etc.)
-
-As an example of a limited data-only module, **DataSurfaces** contains data that is used in the modules that reference surfaces e.g., shadowing calculations, heat balance calculations.
-
-Module excerpts in this document show uses of these data-only modules.
-
-### Parameters
-
-Constants that might be useful throughout the program are defined as Fortran parameters in the DataGlobals data module. Examples include *PI*, *PiOvr2*, *DegToRadians*, and *MaxNameLength*. DataHVACGlobals contains parameters that might be useful anywhere in the HVAC simulation. Some examples are *SmallTempDiff* and *SmallMassFlow* that can be used for preventing divide by zero errors. The full set of global parameters can be obtained by examining the modules DataGlobals and DataHVACGlobals.
-
-### Simulation Flags
-
-A number of logical flags (variables that are either *true* or *false*) are used throughout EnergyPlus. These flags are normally used to indicate the start or end of a time or simulation period. The following shows a complete list.
-
-
-
-**In DataGlobals:**
-
-
-
-BeginSimFlag
-
-Set to true until the actual simulation has begun, set to false after first heat balance time step.
-
-BeginFullSimFlag
-
-Set to true until a full simulation begins (as opposed to a sizing simulation); set to false after the first heat balance time step of the full simulation.
-
-EndSimFlag
-
-Normally false, but set to true at the end of the simulation (last heat balance time step of last hour of last day of last environment).
-
-
-
-WarmupFlag
-
-Set to true during the warmup portion of a simulation; otherwise false.
-
-BeginEnvrnFlag
-
-Set to true at the start of each environment (design day or run period), set to false after first heat balance time step in environment. This flag should be used for beginning of environment initializations in most HVAC components. See the example module for correct usage.
-
-EndEnvrnFlag
-
-Normally false, but set to true at the end of each environment (last heat balance time step of last hour of last day of environment).
-
-BeginDayFlag
-
-Set to true at the start of each day, set to false after first heat balance time step in day.
-
-EndDayFlag
-
-Normally false, but set to true at the end of each day (last heat balance time step of last hour of day).
-
-BeginHourFlag
-
-Set to true at the start of each hour, set to false after first heat balance time step in hour.
-
-EndHourFlag
-
-Normally false, but set to true at the end of each hour (last heat balance time step of hour)
-
-BeginTimeStepFlag
-
-Set to true at the start of each heat balance time step, set to false after first HVAC step in the heat balance time step.
-
-**In DataHVACGlobals:**
-
-FirstTimeStepSysFlag
-
-Set to true at the start of the first HVAC time step within each heat balance time step, false at the end of the HVAC time step.  In other words, this flag is true during the first HVAC time step in a heat balance time step, and is false otherwise.
-
-**In Subroutine SimHVAC:**
-
-FirstHVACIteration
-
-True when HVAC solution technique on first iteration, false otherwise. Passed as a subroutine argument into the HVAC equipment simulation driver routines.
-
-The most commonly used logical flag in the HVAC simulation is FirstHVACIteration that is passed around as an argument among the HVAC simulation subroutines. The HVAC simulation is solved iteratively each HVAC time step. FirstHVACIteration is true for the first iteration in each time step and false for the remaining iterations.
-
-Finally, each developer must define and set a “GetInput� flag to make sure input data is read in only once. In the example module Fans the GetInput flag is GetInputFlag; the new developer can follow this example in using such a flag.
-
-Psychrometric services
-----------------------
-
-EnergyPlus has a full complement of psychrometric functions. All the routines are Fortran functions returning a single precision real value.  All arguments and results are in SI units.
-
-Note that each of the psychrometric routines has a “calledfrom� optional parameter – this has been implemented in some of the calling routines and is useful when errors are detected during simulation for support personnel to figure out where the psych routine is called from.
-
-The Names for the different Psychrometric Routines are based on the following self-explanatory format; the different variables used in the Psych Routine taxonomy are as follows.
-
--   H = Enthalpy
--   W= Humidity Ratio
--   Rh= Relative Humidity
--   V= Specific Volume
--   Rhov= Vapor Density of Air
--   Hfg = Latent energy (heat of vaporization for moist air)
--   Hg= Enthalpy of gaseous moisture
--   Pb= Barometric Pressure
--   Twb=Temperature Wet Bulb
--   Twd= Temperature Dry Bulb
--   Tdp= Temperature Dew Point
--   Tsat and Psat= Saturation Temperature and Saturation Pressure
--   Psy\#\# Fn \#\#     = Psy {\#\# is a Function of  \#\#}
--   Note: Each of the two capital alphabets together have different meaning
-
-       Eg:     **{Psy \#\# Fn HW}= {Psy \#\# Function of  *Enthalpy and Humidity Ratio*}**
-
-
-
-### PsyRhoAirFnPbTdbW (Pb,Tdb,W,calledfrom)
-
-Returns the density of air in kilograms per cubic meter as a function of barometric pressure [Pb] (in Pascals), dry bulb temperature [Tdb] (in Celsius), and humidity ratio [W] (kilograms of water per kilogram of dry air).
-
-### PsyCpAirFnWTdb (W,Tdb,calledfrom)
-
-Returns the specific heat of air in Joules per kilogram degree Celsius as a function of humidity ratio [W] (kilograms of water per kilogram of dry air) and dry bulb temperature [Tdb] (Celsius).
-
-### PsyHfgAirFnWTdb (W,Tdb,calledfrom)
-
-Returns the Latent energy of air [Hfg](Joules per kilogram) as a function of humidity ratio [W] (kilograms of water per kilogram of dry air) and dry bulb temperature [Tdb] (Celsius).  It calculates hg and then hf and the difference is Hfg.
-
-### PsyHgAirFnWTdb (W,Tdb,calledfrom)
-
-Returns the specific enthalpy of the moisture as a gas in the air in Joules per kilogram as a function of humidity ratio [W] (kilograms of water per kilogram of dry air) and dry bulb temperature [Tdb] (Celsius).
-
-### PsyTdpFnTdbTwbPb (Tdb,Twb,Pb,calledfrom)
-
-Returns the dew point temperature in Celsius as a function of dry bulb temperature [Tdb] (Celsius), wet bulb temperature [Twb] (Celsius), and barometric pressure [Pb] (Pascals).
-
-### PsyTdpFnWPb (W,Pb,calledfrom)
-
-Returns the dew point temperature in Celsius as a function of humidity ratio [W] (kilograms of water per kilogram of dry air) and barometric pressure [Pb] (Pascals).
-
-### PsyHFnTdbW (Tdb,W,calledfrom)
-
-Returns the specific enthalpy of air in Joules per kilogram as a function of dry bulb temperature [Tdb] (Celsius) and humidity ratio [W] (kilograms of water per kilogram of dry air).
-
-### PsyHFnTdbRhPb (Tdb,Rh,Pb,calledfrom)
-
-Returns the specific enthalpy of air in Joules per kilogram as a function of dry bulb temperature [Tdb] (Celsius), relative humidity [Rh] (fraction), and barometric pressure [Pb] (Pascals).
-
-### PsyTdbFnHW  (H,W,calledfrom)
-
-Returns the air temperature in Celsius as a function of air specific enthalpy [H] (Joules per kilogram) and humidity ratio [W] (kilograms of water per kilogram of dry air).
-
-### PsyRhovFnTdbRh (Tdb,Rh,calledfrom)
-
-Returns the Vapor Density in air [RhoVapor](kilograms of water per cubic meter of air) as a function of dry bulb temperature [Tdb](Celcius), Relative Humidity [Rh] (fraction).
-
-### PsyRhovFnTdbWP (Tdb,W,Pb,calledfrom)
-
-Returns the Vapor Density in air [RhoVapor](kilograms of water per cubic meter of air) as a function of dry bulb temperature [Tdb](Celcius), humidity ratio [W] (kilograms of water per kilogram of dry air) and barometric pressure [Pb] (Pascals).
-
-### PsyRhFnTdbRhov (Tdb,Rhov,calledfrom)
-
-Returns the Relative Humidity [Rh] (fraction) in air as a function of dry bulb temperature [Tdb] (Celcius) and Vapor Density in air [RhoVapor](kilograms of water per cubic meter of air).
-
-### PsyRhFnTdbWPb (Tdb,W,Pb,calledfrom)
-
-Returns the relative humifity (fraction) as a function of of dry bulb temperature [Tdb] (Celsius), humidity ratio [W] (kilograms of water per kilogram of dry air) and barometric pressure [Pb] (Pascals).
-
-### PsyTwbFnTdbWPb (Tdb,W,Pb,calledfrom)
-
-Returns the air wet bulb temperatute in Celsius as a function of dry bulb temperature [Tdb] (Celsius), humidity ratio [W] (kilograms of water per kilogram of dry air) and barometric pressure [Pb] (Pascals).
-
-### PsyVFnTdbWPb (Tdb,W,Pb,calledfrom)
-
-Returns the specific volume in cubic meters per kilogram as a function of dry bulb temperature [Tdb] (Celsius), humidity ratio [W] (kilograms of water per kilogram of dry air) and barometric pressure [Pb] (Pascals).
-
-### PsyWFnTdpPb (Tdp,Pb,calledfrom)
-
-Returns the humidity ratio in kilograms of water per kilogram of dry air as a function of the dew point temperature [Tdp] (Celsius) and barometric pressure [Pb] (Pascals).
-
-### PsyWFnTdbH (Tdb,H,calledfrom)
-
-Returns the humidity ratio in kilograms of water per kilogram of dry air as a function of dry bulb temperature [Tdb] (Celsius) and air specific enthalpy [H] (Joules per kilogram).
-
-### PsyWFnTdbTwbPb (Tdb,Twb,Pb,calledfrom)
-
-Returns the humidity ratio in kilograms of water per kilogram of dry air as a function of dry bulb temperature [Tdb] (Celsius), wet bulb temperature [Twb] (Celsius), and barometric pressure [Pb] (Pascals).
-
-### PsyWFnTdbRhPb (Tdb,Rh,Pb,calledfrom)
-
-Returns the humidity ratio in kilograms of water per kilogram of dry air as a function of dry bulb temperature [Tdb] (Celsius), relative humidity [RH] (fraction), and barometric pressure [Pb] (Pascals).
-
-### PsyPsatFnTemp (T,calledfrom)
-
-Returns the saturation pressure in Pascals as a function of the air saturation temperature [T] (Celsius).
-
-### PsyTsatFnHPb  (H,Pb,calledfrom)
-
-Returns the air saturation temperature in Celsius as a function of air specific enthalpy [H] (Joules per kilogram) and barometric pressure [Pb] (Pascals).
-
-### PsyTsatFnPb (P,calledfrom)
-
-Returns the air saturation temperature in Celsius as a function of saturation pressure [P] (Pascals).
-
-### CPCW (Temp,calledfrom)
-
-Returns Specific heat capacity   (Joule/kilogram/kelvin) for chilled water as function of temperature [T] (Celsius).
-
-### CPHW (Temp,calledfrom)
-
-Returns Specific heat capacity (Joule/kilogram/kelvin) for hot water as function of temperature [T] (Celsius).
-
-### CVHW (Temp,calledfrom)
-
-Returns Specific heat capacity (Joule/kilogram/kelvin) for hot water at constant volume as function of temperature [T] (Celsius).
-
-### RhoH2O (Temp,calledfrom)
-
-Returns density of water (kg/m3) as function of Temperature [T] (Celsius).
-
-Tabular Output Utilities
-------------------------
-
-Several utility routines are available to help generate tabular reports. To create tabular reports, the developer needs to create a routine called something like WriteTabularX.  The WriteTabularX routine should appear in SimulationManger between the OpenOutputTabularFile and CloseOutputTabularFile calls.  The WriteTabularX routine should make use of several utilities described below.  The “USE� statement reference OutputReportTabular module.  Good example of how to use this facility are in the OutputReportTabular file and the EconomicTariff file.
-
-### WriteReportHeaders(reportName,objectName,averageOrSum)
-
-Where reportName is the name that you want the report to be called and the objectName is the name of the object that appears after the “For: “ for each instance of the report. The averageOrSum flag when set to SUM adds the phrase “per second� after the reportName.
-
-### WriteSubtitle(subtitle)
-
-Where the subtitle is a string that usually appears before a specific table. This is useful if the report includes multiple tables.
-
-### WriteTable(body,rowLabels,columnLabels,widthColumn)
-
-The WriteTable routine actually generates the tables that appear in the tabular output file (CSV, HTML, or TXT).  The rowLabels and columnLables are both one dimensional string arrays that contain the appropriate labels. If the column labels strings include the vertical bar symbol “|� then when creating a text report, the labels will be split between lines at the vertical bar.  For HTML and CSV output, the vertical bar symbols are removed prior to display.
-
-The body array is a two dimensional array (row,column order) containing the cells in the body of the table.  It must be strings so conversion utilities such as RealToStr should be used to convert from numeric values.
-
-WidthColumn is a one dimensional integer array containing the column widths for use only with the fixed width text output option.
-
-Internal Zone Gains Services
-----------------------------
-
-Services are available to help with modeling internal gains.  Internal gains include the usual sources such as people, lights, plug loads, etc., but in EnergyPlus there can also be zone gains from the skin losses from certain equipment such as thermal tanks, electric load center equipment and refrigeration case credits.  Developers adding new device models, or adding skin loss modeling to exisiting device models, need to use a call to SetupZoneInternalGains.  This call is defined in DataInterfaces.f90 and contains a number of optional arguments depending on the type of internal gains involved.  The types of gains that can be added with this call include convection, radiation, and latent gains to the zone, convection and latent gains to the return air, carbon dioxide gains to the zone and generic air contaminant gains to the zone.  For example, the call to register gains for the People object includes convection(sensible), thermal radiation, latent, and CO2 and is:
-
-**CALL** SetupZoneInternalGain(People(Loop)%ZonePtr, &
-
-     **'People'**, &
-
-     People(Loop)%Name, &
-
-     IntGainTypeOf\_People, &
-
-     ConvectionGainRate       = People(Loop)%ConGainRate,&
-
-     ThermalRadiationGainRate = People(Loop)%RadGainRate, &
-
-     LatentGainRate           = People(Loop)%LatGainRate, &
-
-     CarbonDioxideGainRate    = People(Loop)%CO2GainRate)
-
-The refrigerated case model includes terms for sensible and latent gains to both the zone and the return air.  These are really negative gains, or sinks, and the call to register them is:
-
-**CALL** SetupZoneInternalGain(RefrigCase(CaseNum)%ActualZoneNum, &
-
-     **'Refrigeration:Case'**,  &
-
-     RefrigCase(CaseNum)%Name , &
-
-     IntGainTypeOf\_RefrigerationCase,         &
-
-     ConvectionGainRate          = RefrigCase(CaseNum)%SensZoneCreditRate , &
-
-     ReturnAirConvectionGainRate = RefrigCase(CaseNum)%SensHVACCreditRate , &
-
-     LatentGainRate              = RefrigCase(CaseNum)%LatZoneCreditRate  , &
-
-     ReturnAirLatentGainRate     = RefrigCase(CaseNum)%LatHVACCreditRate )
-
-The module developer needs to program the model to update the variable in their module, the one being registered by the call, and central routines use pointers to include the term in the appropriate energy balances elsewhere in the model.  When adding a new type of internal gain, the new device needs to be added to arrays in **DataHeatBalance.f90** called **ZoneIntGainDeviceTypes** and **ccZoneIntGainDeviceTypes** and a new unique **“IntGainTypeOf\_�** parameter.
-
-Output
-======
-
-There are several output files available in EnergyPlus.  As you can see in Appendix A, DataGlobals contains OutputFileStandard, OutputFileInits, and OutputFileDebug.
-
-OutputFileDebug is initialized very early in the EnergyPlus execution and is available for any debugging output the developer might need.
-
-OutputFileInits is intended for “one-time� outputs.  If the value is calculated or entered and should be echoed to output, this file is the place for it.  The structure is similar to the IDD/IDF structure in that there is a “definition� line followed by the data being reported. Since the data may be produced in several places during the simulation, the actual file looks a bit hodge-podge but can be easily imported into a spreadsheet program and grouped.
-
-OutputFileStandard is the reporting variable output file from EnergyPlus.  You can read more details from the [*Guide for Interface Developers*](file:///E:\Docs4PDFs\InterfaceDeveloper.pdf) document and in the [Input Output Reference](file:///E:\Docs4PDFs\InputOutputReference.pdf) document.  OutputFileMeters is a similar file to contain meter (only) output.  Meter values also may appear in the OutputFileStandard file. Only values that change during the simulation should be output to these files.  They are automaticallly included by the SetupOutputVariable calls.
-
-How Do I Output My Variables?
------------------------------
-
-Module developers are responsible for “setting� up the variables that will appear in the OutputFileStandard.
-
-To do this is very simple.  All you need to do is place a simple call to *SetupOutputVariable* into your module for each variable to be available for reporting.  This call should be done only once for each Variable/KeyedValue pair (see below).  For HVAC and Plant components, this call is usually at the end of the “GetInput� subroutine. See the example module for an illustration of this. Other calls in the simulation routines will invoke the EnergyPlus *OutputProcessor* automatically at the proper time to have the data appear in the OutputFileStandard.
-
-For you the call is:
-
-Call SetupOutputVariable(VariableName,ActualVariable,  &
-
-                         IndexTypeKey, VariableTypeKey,KeyedValue,ReportFreq &
-
-                         ResourceTypeKey,EndUseKey,GroupKey)
-
-Interface statements allow for the same call to be used for either real or integer “ActualVariable� variables.  A few examples from EnergyPlus and then we will define the arguments:
-
-CALL SetupOutputVariable('Site Outdoor Drybulb Temperature [C]', &
-
-        OutDryBulbTemp,'Zone','Average','Environment')
-
-
-
-CALL SetupOutputVariable('Zone Mean Air Temperature [C]', &
-
-        ZnRpt(Loop)%MeanAirTemp,'Zone', 'State',Zone(Loop)%Name)
-
-
-
-CALL SetupOutputVariable('Fan Coil Heating Energy [J]', &
-
-        FanCoil(FanCoilNum)%HeatEnergy,'System',   &
-
-       'Sum',FanCoil(FanCoilNum)%Name)
-
-
-
-CALL SetupOutputVariable('Humidifier Electric Energy [J]',
-
-        Humidifier(HumNum)%ElecUseEnergy,'System','Sum', &
-
-        Humidifier(HumNum)%Name, ResourceTypeKey='ELECTRICITY',&
-
-        EndUseKey = 'HUMIDIFIER', GroupKey = 'System')
-
-
-
-Table 4.  SetupOutputVariable Arguments
-
-<table class="table table-striped">
-<tr>
-<td>SetupOutput Variable Arguments</td>
-<td>Description</td>
-</tr>
-<tr>
-<td>VariableName</td>
-<td>String name of variable, units should be included in [].  If no units, use []</td>
-</tr>
-<tr>
-<td>ActualVariable</td>
-<td>This should be the actual variable that will store the value.  The OutputProcessor sets up a pointer to this variable, so it will need to be a SAVEd variable if in a local routine.  As noted in examples, can be a simple variable or part of an array/derived type.</td>
-</tr>
-<tr>
-<td>IndexTypeKey</td>
-<td>When this variable has its proper value.  ‘Zone’ is used for variables that will have value on the global timestep (alias “HeatBalance�).  ‘HVAC’ is used for variables that will have values calculated on the variable system timesteps (alias “System�, “Plant�)</td>
-</tr>
-<tr>
-<td>VariableTypeKey</td>
-<td>Two kinds of variables are produced.  ‘State’ or ‘Average’ are values that are instantaneous at the timestep (zone air temperature, outdoor weather conditions).  ‘NonState’ or ‘Sum’ are values which need to be summed for a period (energy).</td>
-</tr>
-<tr>
-<td>KeyedValue</td>
-<td>Every variable to be reported needs to have an associated keyed value.  Zone Air Temperature is available for each Zone, thus the keyed value is the Zone Name.</td>
-</tr>
-<tr>
-<td>ReportFreq</td>
-<td>This optional argument should only be used during debugging of your module but it is provided for the developers so that these variables would always show up in the OutputFile.  (All other variables must be requested by the user).</td>
-</tr>
-<tr>
-<td>ResourceTypeKey</td>
-<td>Meter Resource Type; an optional argument used for including the variable in a meter. The meter resource type can be 'Electricity', ‘Gas’, ‘Coal’, ‘FuelOil#1’, ‘FuelOil#2’, ‘Propane’, ‘Water’, or ‘EnergyTransfer’.</td>
-</tr>
-<tr>
-<td>EndUseKey</td>
-<td>Meter End Use Key; an optional argument used when the variable is included in a meter. The end use keys can be: 'InteriorLights’, 'ExteriorLights', 'Heating', ‘Cooling’, 'DHW', 'Cogeneration', 'ExteriorEquipment', 'ZoneSource', 'PurchasedHotWater', 'PurchasedChilledWater', 'Fans', 'HeatingCoils', 'CoolingCoils', 'Pumps', 'Chillers', 'Boilers', 'Baseboard', 'HeatRejection', 'Humidifier', 'HeatRecovery' or ‘Refrigeration’.</td>
-</tr>
-<tr>
-<td>EndUseSubKey</td>
-<td>Meter End Use Subcategory Key; an optional argument to further divide a particular End Use.  This key is user-defined in the input object and can be any string, e.g., 'Task Lights', 'Exit Lights', 'Landscape Lights', 'Computers', or 'Fax Machines'.</td>
-</tr>
-<tr>
-<td>GroupKey</td>
-<td>Meter Super Group Key; an optional argument used when the variable is included in a meter. The group key denotes whether the variable belongs to the building, system, or plant.The choices are: 'Building', 'HVAC' or 'Plant'.</td>
-</tr>
-</table>
-
-As described in the *Input Output Reference*, not all variables may be available in any particular simulation.  Only those variables that will have values generated will be available for reporting.  In the IDF, you can include a “Output:VariableDictionary,regular;� command that will produce the eplusout.rdd file containing all the variables with their IndexTypeKeys.  This list can be used to tailor the requests for values in the OutputFileStandard.
-
-This variable dictionary is separated into two pieces: regular reporting variables and meter variables.  It can also be sorted by name (ascending).
-
-Output Variable Dos and Don’ts
-------------------------------
-
-For general output variables there aren’t many rules. For meter output variables there are quite a few. Here are some tips to keep you out of trouble.
-
-### What Variables Should I Output?
-
-The choice of variables to output is really up to the developer. Since variables don’t appear on the output file unless requested by the user in the IDF input file, it is better to “SetUp� too many rather than too few. For an HVAC component one should generally output the heating and cooling outputs of the component both in terms of energy and power. Energy is always output in Joules, power in Watts. If there is humidification or dehumidification both total and sensible cooling should be reported. Any electricity or fuel consumed by a component should be reported out, again both in terms of energy (Joules) and power (Watts). For HVAC components in most cases reporting inlet and outlet temperatures and humidities is unnecessary since these quantities can be obtained from the system node outputs.
-
-### Output Variable Naming Conventions
-
-The names for output variables need to be selected carefully to maintain a high level of consistency and clarity. Well-chosen names help users quickly understand the meaning of a specific output.
-
-The following general guidelines are to be followed when choosing names for new output variables:
-
-- Output variable names shall be written in title case where every major word is capitalized (exceptions: "a", "the", "for", etc.) with spaces separating words.
-
-- Output variable names shall be written using natural language terminology but should be relatively concise. The language is American English.
-
-- Although they should be avoided where practical, acronyms (and symbols) are acceptable where their use is commonplace and contributes to conciseness in identifying a complex engineering concept. Examples of acceptable acronyms for output variable names are listed in the table below.
-
-- Abbreviations should not be used and the words spelled out completely (except for Units).
-
-- Where practical, reuse existing names for output variables across different models for similar components.  For example, a new model for a zone baseboard heater should reuse the existing names for output variables already in use for other baseboard models rather than use new names that distinguish the kind of baseboard model that the output is associated with.  The user-defined name of the component should allow the user to know the association without the basic name of the output variable reflecting that association.  This has the advantage of reducing the total number of output variable names and making it simpler for users.
-
-- Engineering terminology should generally be consistent with that used in ASHRAE handbooks and literature (American Society of Heating, Refrigeration and  Air-Conditioning Engineers, Inc., Atlanta, CA, USA)
-
-- Output variable names shall have no punctuation or special characters. The names are expected to contain many adjectives adjacent to each other and no hyphens or commas are needed to clarify.
-
-- Output variable names shall always be less than 100 characters long.
-
-An output variable name should be constructed from up to six separate name elements.  The following diagram shows the elements and the order that they are to be used in the name.  The first three are each somewhat optional and are used as needed to identify the type of engineering model, object, or device being reported on.  The last three are nearly always needed. Units are always needed (as described below.
-
-![OutputNameScheme.png](media/image003.jpg)
-
-Figure 2. Output Variable Classification Elements
-
-**Model Classification**. This name element is used to identify the specific type of modeling being conducted.  When used, it will form the first part of the name. This name element is often not needed, such as when the output is for a more or less usual aspect of buildings and HVAC system models.  This is typically used to identify outputs that are associated with an alternative, usually more advanced, model, such as AirflowNetwork (AFN) or Conduction Finite Difference (CondFD).  Although modeling domains such as Building, HVAC, or Internal Loads are usually obvious and not needed here, this classification can be useful for non-obvious sub-domains such as Environmental Impact, Refrigeration, or Daylighting.
-
-**Spatial Classification**. This name element is used to identify spatial or topological location of the thing being reported on.  It is generally used to identify which part of the building or system is being referred to by the output.  For parts of the building, classifications such as “Zone� and “Surface� are the most common.  For a model such as Refrigeration this classification may identify specific parts of the system, such as “Secondary Loop.�  There is often no spatial or topological aspect needed and in that case this name element can be omitted.
-
-**Type of Component**. This name element is used to identify the type of device or phenomena being modeled and reported on.  For most component models this should be a simple generic term for the type of device and attempt to reuse established names for similar devices or models.  In cases where the Model and Spatial Classifications are sufficient, this element can be omitted.
-
-**Specific Nature.** This name element is used to identify the nature of what is being reported for the device or phenomena being modeled. This is where the most low-level and specific detail is applied to describe the output variable.  This name element is nearly always needed.
-
-**Dimensional Nature.** This name element is used to identify the nature of the physical dimensions of the quantity being reported in words.  This name element is nearly always needed. This name element is the final part of the name so that names end with terms that reflect the nature of the value being reported. However, the name element should not be the actual units.  For example, an output that has units of degrees Celsius, the final word in the name should be “Temperature.�  Or an output for air flow that has units of kg/s, the final words in the name should be “Mass Flow Rate.�  When reporting on electricity use in Watts, the term “Power� is used; however most other uses of Watts use the term “Rate.�
-
-**Units**. This name element is used to identify the units of the value being reported.   Units of output variables are strictly SI, as used in EnergyPlus.  Units are concatenated on the end of the name with square brackets and separated by a space and.  Dimensionless quantities shall use empty brackets “[ ].�  The preferred set of units is listed at the top of the Energy+.idd file. Units are always abbreviated.
-
-In some situations, a model may lend itself to generating a series of related output variables that depend on input.  For example a surface heat transfer model may have results for numerous individual nodes or cells across the thickness of the surfaces.  The number of nodes in the model will vary at runtime depending on the Construction.  When this is the case, the standard approach used in EnergyPlus is to produce a series of output variables by enumerating the output variable name (rather than the key value) to generate a specific name for each instance.  The generated name element for each instance in the series is appended to the end of the name (but before the Units element) and should end in a number. For example, the third node in a stratified tank model is called “Chilled Water Thermal Storage Temperature Node 3 [C].�  This is done to facilitate wildcarding when postprocessing output.
-
-For Version 8.0, a comprehensive effort was made to rename output variables to follow the guidelines and scheme described above.  As of Version 8.0 the existing output variables demonstrate the pattern and should serve as good examples to follow for future output variables. The following table lists a few examples of terms, but these are not meant to be comprehensive or restrictive.  It is expected that new models may have valid reasons to introduce new terms and units. Developers should examine RDD output files for comprehensive lists of example output variable names.
-
-Table 5. Output Variable Classifications
-
-<table class="table table-striped">
-<tr>
-<td>Model Classification</td>
-<td>Spatial Classification</td>
-<td>Type of Component</td>
-<td>Dimensional Nature</td>
-</tr>
-<tr>
-<td>AFN</td>
-<td>Zone</td>
-<td>Inside Face</td>
-<td>Rate</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>Surface</td>
-<td>Outside Face</td>
-<td>Rate per Area</td>
-</tr>
-<tr>
-<td>Room Air</td>
-<td>Linkage</td>
-<td>Air Terminal</td>
-<td>Energy</td>
-</tr>
-<tr>
-<td>HAMT</td>
-<td>Interior</td>
-<td>Boiler</td>
-<td>Temperature</td>
-</tr>
-<tr>
-<td>CondFD</td>
-<td>Exterior</td>
-<td>Chiller</td>
-<td>Mass Flow Rate</td>
-</tr>
-<tr>
-<td>EMPD</td>
-<td>Site</td>
-<td>Cooling Coil</td>
-<td>COP</td>
-</tr>
-<tr>
-<td>Plant</td>
-<td>Supply Side</td>
-<td>Infiltration</td>
-<td>Power (electric)</td>
-</tr>
-<tr>
-<td>Environmental Impact</td>
-<td>Air System</td>
-<td>Unit Heater</td>
-<td>Level</td>
-</tr>
-<tr>
-<td>HVAC</td>
-<td>Facility</td>
-<td>Generator</td>
-<td>Fraction</td>
-</tr>
-<tr>
-<td>Setpoint Manager</td>
-<td>Node</td>
-<td>Baseboard</td>
-<td>Status</td>
-</tr>
-</table>
-
-
-
- The following table lists acronyms and symbols used in output variable names.
-
-Table 6. Output Variable Example Abbreviations
-
-Acronym
-
-Definition
-
-AC
-
-Alternating Current
-
-AFN
-
-AirflowNetwork
-
-Ar
-
-Argon
-
-ASHRAE
-
-American Society of Heating, Refrigeration, and Air-Conditioning Engineers, Inc.
-
-BSDF
-
-Bidirectional Scattering Distribution Function
-
-CEN
-
-European Committee for Standardization (Comite Europeen de Normalisation)
-
-CH4
-
-Methane
-
-CO
-
-Carbon Monoxide
-
-CO2
-
-Carbon Dioxide
-
-CondFD
-
-Conduction Finite Difference
-
-COP
-
-Coefficient of Performance
-
-DC
-
-Direct Current
-
-DX
-
-Direct Expansion
-
-EIR
-
-Energy Input Ratio
-
-EMPD
-
-Effective Moisture Penetration Depth
-
-H20
-
-Water
-
-HAMT
-
-Heat and Moisture Transfer
-
-Hg
-
-Mercury
-
-HHV
-
-Higher Heating Value
-
-HVAC
-
-Heating Ventilation and Air Conditioning
-
-KSU
-
-Kansas State University
-
-LHV
-
-Lower Heating Value
-
-N2
-
-Nitrogen
-
-N2O
-
-Nitrous Oxide
-
-NH3
-
-Ammonia
-
-NMVOC
-
-Non-Methane Volatile Organic Compounds
-
-NOx
-
-Nitrogen Oxides
-
-O2
-
-Oxygen
-
-Pb
-
-Lead
-
-PM
-
-Particulate Matter
-
-PM10
-
-Particulate Matter of 10 microns or less in size
-
-PM2.5
-
-Particulate Matter of 2.5 microns or less in size
-
-PMV
-
-Predicted Mean Vote
-
-PPD
-
-Percent People Dissatisfied
-
-PV
-
-Photovoltaic
-
-PVT
-
-Photovoltaic-Thermal
-
-SO2
-
-Sulfur Dioxide
-
-VAV
-
-Variable Air Volume
-
-VRF
-
-Variable Refrigerant Flow
-
-WAHP
-
-Water to Air Heat Pump
-
-### What are Meters?
-
-In EnergyPlus meters are an additional output reporting capability. A meter is a way of grouping similar output variables. Meters are output variables just like ordinary output variables except that they sum or average a collection of ordinary output variables. In EnergyPlus the meter variables serve two purposes.
-
-- Providing output of fuel and electricity consumption by end use categories and at the system plant, building and facility level.
-
-- Providing a way of summing heating or cooling outputs for a category of components. The resource type EnergyTransfer is used for this purpose. An example would be reporting out the sum of the heating energy from all the heating coils in a system.
-
-### How Do I Create A Meter?
-
-Meter output variables are created at the same time and in the same manner as ordinary output variables. SetupOutputVariable is called but the optional arguments ResourceTypeKey, EndUseKey, and GroupKey must be used in addition to the usual arguments. For example, in the electric steam humidifier module
-
-CALL SetupOutputVariable('Humidifier Electric Energy [J]', &
-
-  Humidifier(HumNum)%ElecUseEnergy, 'System','Sum', &
-
-  Humidifier(HumNum)%Name)
-
-creates an output variable labeled 'Humidifier Electric Energy [J]' with the value of Humidifier(HumNum)%ElecUseEnergy.
-
-
-
-CALL SetupOutputVariable('Humidifier Electric Energy [J]', &
-
-  Humidifier(HumNum)%ElecUseEnergy, 'System','Sum', &
-
-  Humidifier(HumNum)%Name, &
-   ResourceTypeKey='ELECTRICITY',EndUseKey = 'HUMIDIFIER', &
-
-  GroupKey = 'System')
-
-Creates the same output variable but in addition creates a meter output variable Humidifier:Electricity [J]. This variable will contain the sum of all the electricity consumption of the humidifiers in the system. In addition, this electrical consumption will be added into the meter variables Electricity:HVAC [J] and Electricity:Facility [J].
-
-### Rules for Meter Variables
-
-There are a number of rules developers must follow in order to account for all electricity and fuel consumption as well as to prevent consumables from being double counted.
-
-t Electricity and fuel meters must always be defined at the simple component level. Some EnergyPlus components are compound components: they are built up from simple components. Examples are fan coils (composed of heating coils, cooling coils, and fans), terminal units etc. Some example simple components are heating and cooling coils, fans, humidifiers etc. Electricity and fuel consumption should always be metered at the simple component level and never at the compound component level. This prevents double counting of the fuel or energy consumption.
-
-t A variable should be metered once only. This means a variable can be assigned to only one resource type and to only one end use category.
-
-t Energy Transfer should be metered in the same way as fuel or electricity use. Energy Transfer meters should only be defined for simple components and should be assigned the same end use category as the fuel or electricity consumption.
-
-t All fuel and electricity consumption must be put in some (one) meter.
-
-t Use Energy Transfer judiciously; if in doubt, leave it out.
-
-Energy Management System
-========================
-
-The Energy Management System (EMS) feature in EnergyPlus is an advanced user feature that many users will not need (but may try anyway). Custom programming features are written in the EMS runtime language (Erl). Most of the features have been added to the modules as appropriate. Further “actuators� may need to be added (or desired to be added) and new component developers should review the following information and determine if actuators are useful for the component.
-
-EMS Actuator Interface
-----------------------
-
-New component models may need to register certain control variables with the Energy Management System. In many cases, a component model will be controlled by setpoints placed on a system node, such as the component outlet, and the setpoints placed on the nodes can already be actuated by the EMS. But a given new component may have internal controls that should be made to work with EMS. When this is the case, the developer needs to register the control point as an actuator that EMS users can reference. The content of registered actuators is reported to the EDD file when EMS is used in a model and the Output:EnergyManagementSystem object is configured to do so.
-
-The EMS actuator interface is similar to SetupOutputVariable. Here is the syntax:
-
-CALL SetupEMSActuator(&lt;component type&gt;, &lt;component unique name&gt;,
-
-       &lt;control type name&gt;, &lt;units&gt;, &lt;logical variable on flag&gt;,
-
-       &lt; variable to be controlled&gt;  )
-
-**&lt;component type&gt;**is a string representing the type of component or entity being registered. This is usually the class name of the IDF object. Or it could be another identifying string, if not directly associated with an object. For example the call to setup actuator for nodes uses “System Node Setpoint.’
-
-**&lt;component unique name&gt;**is the local user-specified object name that identifies a unique instance among a set of the same or similar components.
-
-**&lt;control type name&gt;** is the string identifying the type of actuator. A model may have more than one type of control and this argument clarifys which one is being registered. A thermostat object could, for instance, have several actuators for that object type: "On/Off", "Heating Set Point Temperature", and "Cooling Set Point Temperature".
-
- **&lt;units&gt;** is the string for the units of the control variable, used for reporting.
-
- **&lt;logical variable ON flag&gt;** is a local variable attached to the object data structure that says whether or not the actuator value should be used (see below). This becomes a pointer in the EMS data structure so that the EMS can set the value of this variable remotely. The variable type needs to be LOGICAL.
-
- **&lt;variable to be controlled&gt;**  is another variable attached to the object data structure that specifies the value or state of the actuator, used in conjunction with the flag above. Similar to above, this also becomes a pointer in the EMS data structure so that the EMS can set the value of this variable remotely. A Fortran INTERFACE is used to overload the call the SetupEMSActuator so that this can be either a real, integer, or logical value.
-
-However, it is not desirable to register EMS actuators in every simulation because if there is no use of the EMS then this just adds to memory and computation. Therefore, we wrap calls to SetupEMSActuator inside logical checks using a global variable called “AnyEnergyManagementSystemInModel.�
-
-Here is an example to create an actuator that can set the power on EXTERIORLIGHTS:
-
-if (AnyEnergyManagementSystemInModel) Then
-
- CALL SetupEMSActuator('ExteriorLights', ExteriorLights(Item)%Name, &
-
-    'Electric Power', 'W',  ExteriorLights(Item)%PowerActuatorOn, &
-
-     ExteriorLights(Item)%PowerActuatorValue)
-
-ENDIF
-
-
-
-Variables analogous to “PowerActuatorOn� and “PowerActuatorValue� are added to data structure for the component model.
-
-Code must then be written at the object or component level to react to the variables that are being actuated by the EMS Manager. Often it only requires one or two lines of code per actuator. ExteriorLights is particularly simple:
-
-  IF (ExteriorLights(Item)%PowerActuatorOn) THEN
-
-    ExteriorLights(Item)%Power = &
-
-           ExteriorLights(Item)%PowerActuatorValue
-
-  END IF
-
-Finally, once SetupEMSActuator is called, several things happen:
-
-  1. Two pointers are created in the EMS Manager
-
-  2. The actuator is made available for use Erl programs.
-
-  3. The actuator name and associated information are logged in the EDD output file
-
-All of the available actuators that can be accessed are shown in the EDD output file. Like the RDD, the list changes depending on what objects you have in your input file.
-
-In addition to setting up actuators, component model developers can also register design data for components and systems to be made available for possible use in Erl programs. These are generally static data that do not vary across an environment period but might vary from one run to the next. These are registered using calls to SetupEMSInternalVariable such as:
-
-      **CALL** SetupEMSInternalVariable('Zone Floor Area', Zone(ZoneNum)%Name, '[m2]', &
-
-                                    Zone(ZoneNum)%FloorArea )
-
-      **CALL** SetupEMSInternalVariable('Zone Air Volume', Zone(ZoneNum)%Name, '[m3]', &
-
-                                    Zone(ZoneNum)%Volume )
-
-The calls to SetupEMSInternalVariable should also be protected by logic that uses the AnyEnergyManagementSystemInModel logic flag. The internal data available can also be listed in the EDD output file.
-
-Running/Testing EnergyPlus – for Developers
-===========================================
-
-Any item mentioned in this section is available at no charge to collaborative or other developers – the documentation, however, may be rudimentary and use of the procedures require some knowledge of command line (Windows) or Linux scripts.
-
-EnergyPlus is rigorously tested during each release cycle and prior to each release.  Details on some of the test suites that have been used can be seen at:
-
-http://www.eere.energy.gov/buildings/energyplus/testing.html
-
-Equally important is the testing done by each developer during feature development or changes.  For example, on the core development team, developers are charged with executing the entire test suite (≥230 files) for their checkins.  In addition, one of the core development team does run the entire test suite with each checkin and compares those results to previous results.  Unexpected changes, and certainly crashes, should NOT occur.
-
-Since most modules being developed are aimed at the HVAC or plant features, there is a standard 5-zone template geometry that can be used.  This should form the basis of any new additions.  The old 3-zone model should not be used.  Of course, you may develop your own model.
-
-Developers are also charged with making sure their input file runs an entire weather year, has minimal errors (including max simulation errors) and results compare *exactly* when design days (preferably winter-summer vs summer-winter) are reversed in consecutive runs (also known as ReverseDD).  To assist in ReverseDD testing, each input file *should* have a “Run Control� object as well as (at least) two design days (winter-summer / summer-winter as the first two).
-
-Input files should report Zone Air temperatures (Zone Mean Air Temperature or Zone/Sys Air Temperature) as well as meters such as electricity and gas (if applicable).  Of course, reporting features being implemented should be done as well.  These variables will help identify files that have proper “ReverseDD� requirements (failures usually indicate some initialization problems).  Developers should try to minimize output file size – if you are running a full annual simulation (as required by your feature), you should *NOT* report variables at the timestep level.
-
-To compare results, we have a python script (Mathdiff) that is run on the .csv files.  It will report (by default) differences &lt;=.001 or &lt;=.5% as “within range� and outside those limits as “differences�.  If they are exactly the same (from the .csv precision limits), they will be reported as such.
-
-Developers in the core development team use several methods for running the entire test suite.
-
-- One method uses a list of input file names along with an indication of the proper weather file.  A program reads this file and produces several batch files which help with not only running the file but comparing them to previous results, building the “composite error� (the .err files from each file run), and other utility features.  (The same file can be used in Linux testing)
-
-- Another method uses a batch file with options that will allow running old vs. new exes as well as somewhat automating the reverse dd testing.
-
-- Still another method uses a simple batch procedure to “run� all files in a folder.
-
-- Finally, EP-Launch and “groups� can be used.
-
-To facilitate testing, Environment Variables “values� have been implemented in EnergyPlus and/or script files.  To use, one uses the “Set� command and the value as indicated.  Environment variable value testing is inherent in F2003 compliant compilers; for others we have written a set of routines that can either be modified or used directly.
-
-Environment Variables to Assist Running
----------------------------------------
-
-Some environment variables can be used with single or several idf file(s) to keep IDF files pristine while allowing developers or others trying to determine a problem or run a group of files. Many of these have counterparts in Output:Diagnostics objects (some may not be documented). Likewise there may be some “sections� that will produce certain outputs not generally documented.
-
-#### DDOnly: Design Days Only
-
-Setting to “yes� will cause EnergyPlus to set Run Control option (regardless of whether there is a Run Control object in the input file) for Do the Design Day Simulation to “yes� and Do the Weather File Simulation to “no�.  (Uses logical variable **DDOnly** in module DataSystemVariables). There is no Output:Diagnostics equivalent.
-
-    Set DDOnly=yes
-
-#### FullAnnualRun: Full Annual simulation
-
-Setting to “yes� will cause EnergyPlus to set Run Control option (regardless of whether there is a Run Control object in the input file) for Do the Weather File Simulation to “yes�. Scripts should use a weather file when this environment variable is set.  (Uses logical variable **FullAnnualRun** in module DataSystemVariables). There is no Output:Diagnostics equivalent.
-
-    Set FullAnnualRun=yes
-
-And appropriate changes to script files
-
-#### NoWeatherFile: Do not use weatherfile even if indicated
-
-Setting to “yes� doesn’t cause EnergyPlus to do anything but can be used in the scripts to not copy a weather file even when indicated. There is no Output:Diagnostics equivalent.
-
-    Set NoWeatherFile=yes
-
-And appropriate changes to script files
-
-#### ReverseDD: Reverse Design Days during run
-
-Setting to “yes� causes the first two design days requested in the input file to be reversed during EnergyPlus execution.  (Uses logical variable **ReverseDD** in module DataSystemVariables).  For proper comparisons to original order, a program such as **ReverseDDInCSV** or **ReverseDDInESO** must be run or hand edited. There is no Output:Diagnostics equivalent.
-
-    Set ReverseDD=yes
-
-And appropriate changes to script files
-
-#### MinReportFrequency: Set minimum reporting frequency for outputs
-
-Some developers persist in reporting at the timestep or detailed level even if their runs are full annual runs. This is really burdensome on developers that try to run the full test suite for checking changes. The MinReportFrequency environment variable allows EnergyPlus to report at a higher/less frequent level that still allows for changes to be checked (though differences may require more frequent reporting to track down). EnergyPlus reads this environment variable and sets reporting frequency appropriately. There is no Output:Diagnostics equivalent.
-
-    Set MinReportFrequency=daily
-
-The standard frequencies accepted by EnergyPlus must be used: detail, timestep, hourly, daily, monthly, runperiod, environment, annual. In addition, if this environment variable is used, the following will show in the .eio file:
-
-! &lt;Minimum Reporting Frequency (overriding input value)&gt;, Value, Input Value
-
- Minimum Reporting Frequency,  !Daily [Value,Min,Hour,Minute,Max,Hour,Minute],DAILY
-
-#### ReportDuringWarmup: Cause reporting during warmup
-
-Setting to “yes� causes reporting (Output:Variable, Output:Meter) to be reporting during the warmup days at the start of each environment. (Uses logical variable **ReportDuringWarmup** in module DataSystemVariables).  The Output:Diagnostics, ReportDuringWarmup; is equivalent.
-
-    Set ReportDuringWarmup=yes
-
-#### REPORTDURINGHVACSIZINGSIMULATION: Cause SQLite reporting during HVAC Sizing Simulations
-
-Setting to “yes� causes output to be sent to SQLite database file during HVAC Sizing Simulations.  (Uses Boolean variable ReportDuringHVACSizingSimulation in DataSystemVariables).  The Output:Diagnostics, ReportDuringHVAVSizingSimulation; is equivalent.
-
-    Set REPORTDURINGHVACSIZINGSIMULATIN=YES
-
-#### DisplayAllWarnings: turn on all extra warnings
-
-Setting to “yes� causes turning on the warnings: DisplayAllWarnings, DisplayExtraWarnings, DisplayUnusedSchedules, DisplayUnusedObjects. DisplayUnusedObjects also displays unused fluids (that is, fluids that are not directly retrieved by the simulation). The Output:Diagnostics, DisplayAllWarnings; is equivalent.
-
-    Set DisplayAllWarnings=yes
-
-#### DisplayExtraWarnings: turn on  extra warnings
-
-Setting to “yes� causes turning on DispalyExtraWarnings. The Output:Diagnostics, DisplayExtraWarnings; is equivalent.
-
-    Set DisplayExtraWarnings=yes
-
-#### DisplayUnusedObjects: turn on display of unused objects and fluids
-
-Setting to “yes� causes the orphan objects and fluids that are in the input file but not used to be displayed at the end of the simulation. The Output:Diagnostics, DisplayUnusedObjects; is equivalent.
-
-    Set DisplayUnusedObjects=yes
-
-#### DisplayUnusedSchedules: turn on display of unused schedules
-
-Setting to “yes� causes the schedules that are in the input file but not used to be displayed at the end of the simulation. The Output:Diagnostics, DisplayUnusedSchedules; is equivalent.
-
-    Set DisplayUnusedSchedules=yes
-
-#### DisplayZoneAirHeatBalanceOffBalance: turn on this development output
-
-Setting to “yes� causes the program to calculate and display the Zone Air Heat Balance “out of balance� warnings. The Output:Diagnostics, DisplayZoneAirHeatBalanceOffBalance; is equivalent.
-
-    Set DisplayZoneAirHeatBalanceOffBalance=yes
-
-#### IgnoreSolarRadiation: turn off using Solar in simulation
-
-Setting to “yes� causes the program to ignore all solar values during simulation.  One might use this when a new set of weather files are produced but you are unsure of their impacts. It also speeds the program as no shading calculations are done. The Output:Diagnostics, IgnoreSolarRadiation; is equivalent.
-
-    Set IgnoreSolarRadiation=yes
-
-#### DisplayAdvancedReportVariables: turn on access to advance report variables
-
-Setting to “yes� causes the program to be able to access the “advanced report variable� set in the program.The Output:Diagnostics, DisplayAdvancedReportVariables; is equivalent.
-
-    Set DisplayAdvancedReportVariables=yes
-
-#### SortIDD: turn on (or off) the sorting of IDD objects
-
-Setting to “yes� (internal default) causes the program to use sorted lists (a speed up mechanism) in searching for existant objects during IDF processing. There is really no reason to turn it off. There is no Output:Diagnostics equivalent.
-
-    Set SortIDD=yes
-
-#### DeveloperFlag: turn on (or off) some different outputs for the developer
-
-Setting to “yes� (internal default is “no�) causes the program to display some different information that could be useful to developers. In particular, this will cause the Warmup Convergence output to show the last day for each zone, each timestep. There is no Output:Diagnostics equivalent.
-
-    Set DeveloperFlag=yes
-
-#### IgnoreBeamRadiation: turn on (or off) the beam radiation
-
-Setting to “yes� causes the program to ignore beam radiation in solar calculations. Of limited use, but may be useful for some simulation developments or isolating problems. There is no Output:Diagnostics equivalent.
-
-    Set IgnoreBeamRadiation=yes
-
-#### IgnoreDiffuseRadiation: turn on (or off) the diffuse radiation
-
-Setting to “yes� causes the program to ignore diffuse radiation in solar calculations. Of limited use, but may be useful for some simulation developments or isolating problems. There is no Output:Diagnostics equivalent.
-
-    Set IgnoreDiffuseRadiation=yes
-
-#### SutherlandHodgman: turn on (or off) the polygon clipping algorithm
-
-Setting to “yes� (internal default) causes the program to use the SutherlandHodgman polygon clipping algorithm. You might use this if you wanted to run a bunch of files with the legacy clipping algorithm (convex Weiler Atherton). There is no Output:Diagnostics equivalent.
-
-    Set SutherlandHodgman=yes
-
-#### MinimalShadowing: turn on (or off) the use of Minimal Shadowing
-
-Setting to “yes� causes the program to use Minimal Shadowing (a speed up mechanism) in calculations. This could be useful when large files are being run to search for non-shadowing related problems. There is no Output:Diagnostics equivalent.
-
-    Set MinimalShadowing=yes
-
-#### DisplayInputInAudit: turn on (or off) to show the input file in the audit file
-
-Setting to “yes� causes the audit file to include a line-by-line echoing of the input file which may be useful for debugging purposes. For versions 8.2 and earlier, the default behavior was to include the line-by-line echoing of the input file into the audit file but it was changed to not do this by default as a way to speed up the input processing portion of executing EnergyPlus. When not set to “yes�, the audit file contains a reference on using the DisplayInputInAudit environment variable to see the line-by-line echoing of the input file.
-
-#### Caution: Environment Variables
-
-Some combinations will cause fatal errors from EnergyPlus – **DDOnly** and **FullAnnualRun**, for example.  **FullAnnualRun** and **NoWeatherFile** won’t cause fatal errors from EnergyPlus but probably should from the script files.  We welcome any suggestions for future environment variables.
-
-Air Loop Simulation Environment Variables
------------------------------------------
-
-To facilitate comparing the runtime performance of various solution techniques for the air loop simulation a mechanism to track runtime statistics has been implemented in EnergyPlus. To facilitate debugging the air loop simulation a tracing mechanism operating either at the air loop-level or at the controller-level has been implemented in EnergyPlus.  To use, one uses the “Set� command and the value as indicated.
-
-#### TRACK\_AIRLOOP: Runtime performance tracker for air loop simulation
-
-Setting to “yes� will cause EnergyPlus to track the performance of the air loop simulation at runtime and dump the results in a file named “statistics.HVACControllers.csv� upon ending the simulation.  (Uses logical variable **TrackAirLoopEnvFlag** in module DataSystemVariables).
-
-Set TRACK\_AIRLOOP=yes
-
-#### TRACE\_AIRLOOP: Air loop simulation tracer
-
-Setting to “yes� will cause EnergyPlus to write to a trace file named “controller.&lt;Air Loop Name&gt;.csv� the converged solutions of all controllers defined on each air loop, at each HVAC iteration.  (Uses logical variable **TraceAirLoopEnvFlag** in module DataSystemVariables).
-
-Set TRACE\_AIRLOOP=yes
-
-#### TRACE\_HVACCONTROLLER: Individual HVAC controller tracer
-
-Setting to “yes� will cause EnergyPlus to write to a trace file named “controller.&lt;Controller Name&gt;.csv� a detailed description of each controller iteration at each HVAC iteration.  (Uses logical variable **TraceControllerEnvFlag** in module DataSystemVariables).
-
-Set TRACE\_HVACCONTROLLER=yes
-
-
-
-Quick Procedure Outline For Making Code Changes to EnergyPlus
-=============================================================
-
-Some of the steps in this section are primarily applicable to developers who are part of the “EnergyPlus Team�.  However, these steps should also be followed as you develop a module or other piece to submit to the EnergyPlus Team for inclusion in an EnergyPlus release.
-
-1.   Write a New Feature Proposal (often called NFP) for discussion at a bi-weekly conference call.  Based on that discussion, update the NFP. Out of team developers: use the NFP format to help formulate your submission documentation to the EnergyPlus Team. ***The NFP format is shown in Appendix F. The sections of the NFP format are shown in*** ***Table 1. Sections of a New Feature Proposal.***
-
-2.   Get the relevant files for your development. Team developers can check out files from StarTeam.
-
-a.   Energy+.idd and Featurechanges.csv are in the ‘Release’ Folder. This folder also contains the “Rules� spreadsheet and “Report Variables� files.
-
-b.   ExampleFiles.xls, ExampleFilesDoc.txt, and baseline or relevant IDF files from ‘Test Files - Utilities\\InternalTests\\InputFiles‘
-
-c.   F90 files from the ‘SourceCode’ folder.
-
-d.   Documents (InputOutputReference.doc, EngineeringReference.doc, OutputDetailsAndExamples.doc, etc.) from the ‘External Documentation\\Documentation Sources’ folder.
-
-3.   Following proper procedures (*e.g., Object naming conventions are specified earlier in this document*) make your object changes to the Energy+.idd and relevant IDF files.  If your IDD modifications make changes for existing objects, you must determine if you need to add to the “Rules� spreadsheet so that the transition program can be made for existing IDF files.  Likewise, if you change existing report variable names, you must update the “Report Variables� file. Note that the ExampleFiles.xls has some guidance on the contents of new test suite files. Create or change existing IDF files for your feature.
-
-4.   Make code changes to F90 files for subroutines, GetInput, Sim, Report or create your own module following the Programming Standards and Programming Templates.  Programming Templates are available in Appendix D.  Programming Standards is a separate document.
-
-5.   Compile and run in debug mode to track errors.
-
-6.   Test making sample runs; review summary and time step reports to identify issues. Test many features of your module even if you are not including all in the Test Suite IDF file. Go back to Step 4 as necessary. Note some of the issues in the “Important Rules for Developers�.
-
-7.   When complete, run full test suite to make sure there are no crashes or unexpected changes in other files.
-
-8.   Run Reverse DD for your featured files – making sure the results *exactly* match.
-
-9.   Update relevant portions of documents: InputOutputReference.doc, EngineeringReference.doc, OutputDetailsAndExamples.doc, etc.  Only excerpted portions of the document should be sent forward for review and final inclusion in the whole document. Depending on the changes, it may be better to “track changes� in the document or give instructions for inclusion in the whole document. Send these documents up the review chain as appropriate.  ***Appendix C also has some information about formatting documents.***
-
-10. Procedure on checking in files changes from time to time.  Currently, all source code files are kept locked and your code may go through another reivew before you are allowed to check in.  ***Follow procedures in Appendix B as well about submitting your feature – many parts are repeated in this section.***
-
-11. Check in modified or new files. If changes have been made to the original checked out file, you must carefully merge your changes into the file – this also may necessitate you repeating your test runs. Usually, your featurechanges modification will be very simple and be the last line in that file.
-
-12. Send email to the team notifying them of the new feature/changed feature/defect fix and what files were changed/added/etc.
-
-13. Incorporate any feedback after checkin.
-
-14. Use ***Appendix G*** to submit information, if applicable, about your feature.
-
-Important Rules for Module Developers
-=====================================
-
-1.   INITIALIZE!!!!!  INITIALIZE either fully or "invalidly" when you ALLOCATE the array/derived type.  Two items have been set up to help you: BigNumber and DBigNumber are in DataGlobals.  They get initialized before anything happens in the main routine (EnergyPlus). An invalid initialization can use one of these, appropriately (i.e. set and test for “BigNumber�).  Another example of “invalid� initialization is a value that shouldn’t be legal for the item (-999).
-
-2.   Warning errors during "get input" should only be used when program termination is not required (this is rare). Each GetInput routine should be structured so that errors detected (such as an invalid schedule name which currently is just a warning) cause a fatal error after all the input for that item/module/etc is gotten.  (See HBManager, BaseboardRadiator, others)  In addition, don't make GetInputFlag a module variable.  Make it as "local" as possible.  Look at BaseboardRadiator for an example.
-
-3.   Error messages during simulation should be semi-intelligent.  No one wants to see 5,000 messages saying "this flow invalid".  If the error condition might happen a lot (especially during debugging), count each occurrence and only put out a message every 50 or so.   It is better to use the “Recurring Error Handling� routines. (See examples of both above in the Error Messages section).  Also, if you are putting the same message in two modules, identify the error message with some designation.  For Example,
-
- CALL ShowWarningError (**'SimRoutinename**: this condition happened again')
-
-will help everyone track it down.   Use the ShowContinueErrorTimeStamp so the time/date/environment of occurrence is known, as appropriate for the condition.
-
-4.   Use the templates for documentation!  Modules, subroutines, functions templates all have been checked into StarTeam.  Use them.  Put INTENTs on your Subroutine Arguments.  Document variables.
-
-**5.   Add “meter� variables as appropriate!  If your module uses fuel or electricity and that energy is not accounted for by other components (i.e. pumps, coils, chillers, etc), then you need to report it onto a “meter�.**
-
-**6.   Avoid the use of string comparisons in subroutines other than GetInput.  Check string comparisons in the GetInput subroutines and assign an integer parameter for comparisons elsewhere in the module. Character strings in structures are not allowed (except for name of object) – any exceptions must be approved. Schedule names, curve object names, and child object types MUST all be referenced by an integer. Existing code must be changed as you change any of the code within a module. **
-
-**7.   If you are submitting code for insertion in the public version of EnergyPlus, make sure that the proper “Grant-Back� procedure has been followed so that the correct attributions of code authorship are given as well as permission to use this code in publicly available software is assured. (see Appendix G, Code/Module Contribution Questionnaire – also available separately)**
-
-
-
-
-
-
-
-Appendix A.  DataGlobals and DataEnvironments Modules
-=====================================================
-
-Rather than include the code of the DataGlobals and DataEnvironments modules, they will be described here.
-
-DataGlobals
------------
-
-DataGlobals contains parameters, variables, Interface descriptors that could be used by every part of the program.  For example, this is where the “MaxNameLength� (maximum name length (characters) of objects.  All other pieces of the code that need this will need to
-
-USE DataGlobals
-
-and, if that’s the only piece it needs, can say
-
-USE DataGlobals, ONLY: MaxNameLength
-
-Interface specifications for the ShowError routines are here because there are optional parameters in these routines.  Then,
-
-USE DataGlobals, ONLY: ShowWarningError, ShowFatalError
-
-can be used safely from any routine.  Constants such as Pi (p), Degrees To Radians, and Number of Seconds in Hour are also stored there.  Remember that we suggest compiling EnergyPlus in double precision and these constants (as should all constants) are representative of double precision (even if someone were to compile in single precision).
-
-Finally, the interface specifications for the Setup Report Variables is contained in this module.  The interface allows for a single call for accomplishing that while actually forking to call several different routines based on the type of data being used.
-
-DataEnvironment
----------------
-
-DataEnvironment is intended to address global environmental variables (such as current outdoor temperature, barometric pressure, and so forth).  It is also extends the concept of a “data only� module a bit to encompass a few functions that calculate values for the site atmospheric variation concept.
-
-
-
-Appendix B.  Submissions and Check-ins
-======================================
-
-There are two methods by which new modules are entered into the EnergyPlus (publicly available) program.
-
-- **Checkin:** Part of the core development team may create or modify an existing module.  As we use a configuration management system – this is called a check in.
-
-*Note --- to save people grief and rework effort and to work toward consistency in approach, new features or changes to existing features must be proposed in a documented way for discussion during one of the bi-weekly conference calls.*
-
-- **Submission:** When someone outside the core development team submits a module or modification of an existing module for inclusion, this is termed a submission.
-
-*Submissions are subjected to the same kind of scrutiny as team checkins and usually will require rework by the submitter.  We welcome outside developers to send their ideas as early documents for comment with the understanding that revising does not guarantee automatic inclusion.  See the proposed feature outline document in Appendix F and/or the “doc� file in the Documents for Developers Zip file.*
-
-Both kinds of inclusions need to follow the checklist procedure for new inclusions:
-
-ü **Source Code Rules**
-
-Shall follow programming standard
-
-Shall follow F90/95 or later standards  (use “allocatable� for allocatable structures within Derived Types)
-
-Shall follow the Template standards (documentation, naming conventions)
-
-Shall follow the guidelines shown in this document
-
-All items shall be directly initialized (exception: derived type elements may be staticly initialized)
-
-There shall be no “unused� variables.  If you put in a variable that you “might use later� – comment it out and comment it to be used later.
-
-No Tabs in source code!!!
-
-Lines shall be less than 133 characters in length.  (Some compilers allow longer lines without warning).
-
-Suggest using F95 standards checking during compiles -- you may use the compiler option to generate warnings for non-standard code.
-
-**Permission to use the code shall be supplied -- written, even email, is required.  LBNL is monitoring this aspect – so a grant-back letter can also be obtained from them.**
-
-ü **Energy+.IDD rules**
-
-Standard Units shall be used (SI only on Input)
-
-Show units with the **\\units** field.  Supply **\\ip-units** only if your input would require it (see comments at top of the Energy+.idd).
-
-Use **\\minimum** and **\\maximum**
-
-The first field following the object name should contain “**name**� as part of the field name
-
-Use **\\default, \\min-fields** and **\\required-field** appropriately
-
-Object changes during minor releases (x.x.xxx) should not change fields in the middle – only at the end
-
-Surface objects may not add further fields to the end (the end is reserved for vertices and extension to the current limits)
-
-Note that changes in the Energy+.idd will require a “transition� rule change in the Rules Spreadsheet file (Rules…xls).  Likewise, changes in report variable names must be documented in the “report variables� change file that is a companion to the Rules spreadsheet.
-
-ü **Testing**
-
-Shall run the full test suite for all new features and unless you are absolutely, positively sure that your change will not impact other parts of the code.  We have a python script that can compare between two run versions (using the .csv files output from ReadVarsESO).
-
-If you need a script, look under StarTeam…Test Files&gt;ScriptMaker.  Other scripts are mentioned in the section on “Running EnergyPlus for Developers� (Module Developer’s Guide).
-
-If you modify objects, you must change all test suite files that are impacted by your object modifications.
-
-ü **New Features need a new example file**
-
-You must create a new input file for your changes—input files shall include appropriate internal documentation!  (Test files have a document template as well seeAppendix E.  Test File Documentation).  Some features may be appropriately added to an existing file but documentation must be updated.
-
-You must fill out a line in the “ExampleFiles.xls� spreadsheet for your new input file.
-
-You must run a full annual run with your test file even if that is not the configuration that ends up in the internal test suite.  Annual runs have been known to fail – obviously, your input file should not.
-
-You must try to minimize the number of errors shown in the eplusout.err file for your files.
-
-Reverse DD Compliance Test: You must run a test that reverses a run of two environments (design days) and make sure that the results (when you also reverse the results files) are identical.  (Identical means *exactly* the same.)  Several scripts and automated programs to accomplish this feat are available.
-
-ü **Documentation (must be included at the same time as code!!!)**
-
-A document template is available for use – only the styles in that document should be used.  (Microsoft™ Word is our standard word processing software).
-
-Equations – limited in IORef, necessary in Engineering Doc – limit the number of “references� though.  You can use standard Equation formatting from Microsoft™ Word or Mathtype™ is an acceptable alternate.
-
-Figures – Though AutoShapes may draw nice pictures, they are not often “captionable� without undue editing.  Please make figures into Jpegs or GIFs.  Use “insert caption� (below the figure) so that auto-numbering of figures is used (these will transfer automatically to EnergyPlus documents).
-
-Tables – use “insert caption� (above the table) so that auto-numbering of figures is used (these will transfer automatically to EnergyPlus documents).
-
-Cross-References – limit your “insert cross references�.  You should highlight these so that “editing� from your inclusion is more obvious – use a different color to help them stand out.
-
-IORef – See the InputOutputReference document for indications of what is included.
-
-Eng Ref – New modules shall include an engineering document reference.  See the Engineering Reference for indications of typical writeups.
-
-Output Details and Examples – this can help illustrate your changes.  Any new files *must* be detailed in here.  Likewise, changes to the .eio file must be described.
-
-ü **FeatureChanges.csv**
-
-Every change to source code, example files, datsets, utilities (any change other than documentation) must include a line in the “featurechanges.csv� file.
-
-ü **Checked in?**
-
-A courtesy message to the EnergyPlus team should be done for each check in, with details of files checked in, etc.  Save one of the emails you have received if you don’t know how many to send it to.
-
-ü **Defect fixing?**
-
-If you fix a defect or “fix� a suggested change (CR), you should mark it “fixed� in StarTeam and the responsibility should automatically change back to the author of the CR.  If you fix your own CR, assign it to someone else for verification.
-
-If you fix a defect or “fix� a suggested change, you should provide a “synopsis for users� (on the “Custom� tab in the CR edit dialog) so that when we release the version with your fix, we can provide something descriptive for the users.
-
-  If a defect has a workaround, you should enter this in the “Workaround� field (on the “Solution� tab) to inform users until the fix is released in a public version.
-
-ü **Rules…xls**
-
-If a transition rule will be needed (or a deleted / obsolete / renamed object is needed) – a line (or more) in this spreadsheet must be used.  See example rules files from previous releases.  If in doubt, put something in.
-
-ü **ReportVariables…csv**
-
-If you change the name of a report variable, the transition program for release can automatically transition older input files **IF** you put the old and new names into this file.
-
-If you delete a report variable, that detail should go in this file.  Note that you must consult others on the core development team before deleting a reported variable.
-
-Appendix C.  Documentation Specifics
-====================================
-
-Documents that module developers will typically be updating or changing are the: Input Output Reference, Engineering Documentation, and Output Details and Examples.  You may, of course, note revisions to other documents.
-
-All of the EnergyPlus documentation follows a Word™ template – report.dot.
-
-This template takes care of many of the nuances of formatting so that the documents all retain the same “look and feel�.  The template itself will contain examples for the IORef and Engineering Documentation.
-
-General guidelines:
-
-- Don’t get fancy with formatting.  No extra “enters� are needed to space the paragraphs.
-
-- Submit your pictures as pictures (jpeg, tif, gif).  This will allow you to “insert captions� below them and have them automatically numbered.  (This also allows them to be re-numbered once inside the EnergyPlus documents).  Don’t use Text boxes.
-
-- Likewise, use an “insert caption� on tables.
-
-- Table captions go above the table.  Figure captions go below.
-
-- If you want to reference a table or figure in your text, use “insert cross reference� and select table or figure as appropriate.  Usually, just use the “label and number� option.
-
-- Body Text is the expected style for most text.  DO NOT put object names in a different font (such as Courier) or as a different size though you may bold them for emphasis.
-
-- Headings are used judiciously to help separate text.
-
-- Object names (IOReference) are Heading 3.
-
-- Each field must be described and shown as Heading 4 followed by the description.  Form should be “Field: &lt;field Name&gt;�. (Exception: if your object has a repeating set of fields – you may describe the initial field set in detail such as is done for the branch specifications fields in the Branch object).
-
-- Each object’s IDD must be shown and use the format “IDD Definition�.
-
-- An excerpt IDF using the object must be shown.
-
-- Output variables for the object must be shown (heading 4) with a heading 3 &lt;object name&gt; Output variables preceding.
-
-- Equations may be inserted using the Microsoft™ Equation Editor.  Internally we use software called “MathType� – that also may be used for Equations.  It is not desirable to number every equation.  If you want to reference the equations, of course, you will need to number them – it is best to number them in plain text and then we can edit them into the rest of the documents.
-
-- Each Engineering Reference section should contain a “References� section and should be formatted in author style (not numbered).
-
-Example References:
-
-ASHRAE. 1993. 1993 ASHRAE Handbook – Fundamentals. Atlanta: American Society of Heating, Refrigerating, and Air-Conditioning Engineers, Inc.
-
-Chapman, A. J. 1984. Heat Transfer, 4<sup>th</sup> Edition, New York: Macmillan Publishing Company.
-
-Lienhard, J. H. 1981. A Heat Transfer Textbook, Englewood Cliffs, N.J.: Prentice-Hall, Inc.
-
-McClellan, T. M., and C. O. Pedersen. 1997. Investigation of Outside Heat Balance Models for Use in a Heat Balance Cooling Load Calculation. ASHRAE Transactions, Vol. 103, Part 2, pp. 469-484.
-
-Walton, G. N. 1983. Thermal Analysis Research Program Reference Manual. NBSSIR 83-2655. National Bureau of Standards.
-
-
-
-
-
-Appendix D.  Module, Subroutine, Function Templates
-===================================================
-
-The following module template can and should be used to create new modules.  Following the module template are subroutine and function templates.  You should be able to copy the template for your own use (or you can get a plain text version).
-
-**MODULE &lt;module\_name&gt;**
-
-
-
-          ! Module containing the routines dealing with the &lt;module\_name&gt;
-
-
-
-          ! MODULE INFORMATION:
-
-          !       AUTHOR         &lt;author&gt;
-
-          !       DATE WRITTEN   &lt;date\_written&gt;
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS MODULE:
-
-          ! &lt;description&gt;
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! &lt;description&gt;
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! OTHER NOTES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-          ! &lt;use statements for data only modules&gt;
-
-USE DataGlobals, ONLY: ShowWarningError, ShowSevereError, ShowFatalError, &
-
-                       MaxNameLength, ...
-
-
-
-          ! &lt;use statements for access to subroutines in other modules&gt;
-
-
-
-IMPLICIT NONE ! Enforce explicit typing of all variables
-
-
-
-PRIVATE ! Everything private unless explicitly made public
-
-
-
-          ! MODULE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS:
-
-          ! na
-
-
-
-          ! MODULE VARIABLE DECLARATIONS:
-
-          ! na
-
-
-
-
-
-
-
-          ! SUBROUTINE SPECIFICATIONS FOR MODULE:
-
-     ! Driver/Manager Routines
-
-PUBLIC  Sim&lt;module\_name&gt;
-
-
-
-     ! Get Input routines for module
-
-PRIVATE Get&lt;module\_name&gt;
-
-
-
-     ! Initialization routines for module
-
-PRIVATE Init&lt;module\_name&gt;
-
-PRIVATE Size&lt;module\_name&gt;
-
-
-
-     ! Algorithms/Calculation routines for the module
-
-PRIVATE Calc&lt;module\_name&gt;
-
-
-
-     ! Update routines to check convergence and update nodes
-
-PRIVATE Update&lt;module\_name&gt;
-
-
-
-     ! Reporting routines for module
-
-PRIVATE Report&lt;module\_name&gt;
-
-
-
-     ! Utility routines for module
-
-! these would be public such as:
-
-! PUBLIC  Get&lt;module&gt;InletNode
-
-! PUBLIC  Get&lt;module&gt;OutletNode
-
-
-
-**CONTAINS**
-
-
-
-**SUBROUTINE Sim&lt;module\_name&gt;**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         &lt;author&gt;
-
-          !       DATE WRITTEN   &lt;date\_written&gt;
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! &lt;description&gt;
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! &lt;description&gt;
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS:
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-  LOGICAL,SAVE      :: GetInputFlag = .true.  ! First time, input is "gotten"
-
-
-
-  IF (GetInputFlag) THEN
-
-    CALL Get&lt;module\_name&gt;Input
-
-    GetInputFlag=.false.
-
-  ENDIF
-
-
-
-  &lt;... insert any necessary code here&gt;
-
-
-
-  CALL Init&lt;module\_name&gt;(Args)
-
-
-
-  CALL Calc&lt;module\_name&gt;(Args)
-
-
-
-  CALL Update&lt;module\_name&gt;(Args)
-
-
-
-  CALL Report&lt;module\_name&gt;(Args)
-
-
-
-  RETURN
-
-
-
-**END SUBROUTINE Sim&lt;module\_name&gt;**
-
-
-
-**SUBROUTINE Get&lt;module\_name&gt;Input**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         &lt;author&gt;
-
-          !       DATE WRITTEN   &lt;date\_written&gt;
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! &lt;description&gt;
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! &lt;description&gt;
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-  USE InputProcessor, ONLY: GetNumObjectsFound, GetObjectItem ! might also use FindItemInList
-
-  USE DataIPShortCuts
-
-
-
-  IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-  CHARACTER(len=\*), PARAMETER :: RoutineName='PutRoutineNameHere'
-
-  CHARACTER(len=\*), PARAMETER :: CurrentModuleObject='GetModuleObject'
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS:
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-  INTEGER                        :: Item    ! Item to be "gotten"
-
-  !  Instead of below, use Variables in IPShortCuts
-
-!  CHARACTER(len=MaxNameLength), &
-
-!                    DIMENSION(x) :: Alphas  ! Alpha items for object
-
-!  REAL, DIMENSION(y)             :: Numbers ! Numeric items for object
-
-  INTEGER                        :: NumAlphas  ! Number of Alphas for each GetObjectItem call
-
-  INTEGER                        :: NumNumbers ! Number of Numbers for each GetObjectItem call
-
-  INTEGER                        :: IOStatus   ! Used in GetObjectItem
-
-  LOGICAL                        :: ErrorsFound=.false.  ! Set to true if errors in input, fatal at end of routine
-
-
-
-  &lt;NumItems&gt;=GetNumObjectsFound(CurrentModuleObject)
-
-  DO Item=1,&lt;NumItems&gt;
-
-    CALL GetObjectItem(CurrentModuleObject,Item,cAlphaArgs,NumAlphas, &
-
-                         rNumericArgs,NumNumbers,IOStatus,  &
-
-                         AlphaBlank=lAlphaFieldBlanks,NumBlank=lNumericFieldBlanks,  &
-
-                         AlphaFieldnames=cAlphaFieldNames,NumericFieldNames=cNumericFieldNames)
-
-    &lt;process, noting errors&gt;
-
-    ! Errors should be formatted as (alpha 1 should hold the name of the object)
-
-    CALL ShowSevereError(RoutineName//':'//CurrentModuleObject//'="'//trim(cAlphaArgs(1)))//  &
-
-      '", invalid '//trim(cAlphaFieldNames(x))//'="'//trim(cAlphaArgs(x))//'" &lt;condition&gt;.')
-
-    ! likewise for numeric fields
-
-
-
-  ENDDO
-
-
-
-  &lt;SetupOutputVariables here...&gt;
-
-
-
-  IF (ErrorsFound) THEN
-
-    CALL ShowFatalError(RoutineName//':'//CurrentModuleObject//': Errors found in input.')
-
-  ENDIF
-
-
-
-  RETURN
-
-
-
-**END SUBROUTINE Get&lt;module\_name&gt;Input**
-
-
-
-**SUBROUTINE Init&lt;module\_name&gt;**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         &lt;author&gt;
-
-          !       DATE WRITTEN   &lt;date\_written&gt;
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! &lt;description&gt;
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! &lt;description&gt;
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-          ! na
-
-
-
-  RETURN
-
-
-
-**END SUBROUTINE Init&lt;module\_name&gt;**
-
-
-
-**SUBROUTINE Size&lt;module\_name&gt;**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         &lt;author&gt;
-
-          !       DATE WRITTEN   &lt;date\_written&gt;
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! &lt;description&gt;
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! &lt;description&gt;
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-          ! na
-
-
-
-  RETURN
-
-
-
-**END SUBROUTINE Size&lt;module\_name&gt;**
-
-
-
-**SUBROUTINE Calc&lt;module\_name&gt;**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         &lt;author&gt;
-
-          !       DATE WRITTEN   &lt;date\_written&gt;
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! &lt;description&gt;
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! &lt;description&gt;
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS:
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-          ! na
-
-
-
-  RETURN
-
-
-
-**END SUBROUTINE Calc&lt;module\_name&gt;**
-
-
-
-**SUBROUTINE Update&lt;module\_name&gt;**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         &lt;author&gt;
-
-          !       DATE WRITTEN   &lt;date\_written&gt;
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! &lt;description&gt;
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! &lt;description&gt;
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS:
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-          ! na
-
-
-
-  RETURN
-
-
-
-**END SUBROUTINE Update&lt;module\_name&gt;**
-
-
-
-**SUBROUTINE Report&lt;module\_name&gt;**
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         &lt;author&gt;
-
-          !       DATE WRITTEN   &lt;date\_written&gt;
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! &lt;description&gt;
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! &lt;description&gt;
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS:
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-          ! na
-
-
-
- ! &lt;this routine is typically needed only for those cases where you must transform the internal data to a reportable form&gt;
-
-
-
-  RETURN
-
-
-
-**END SUBROUTINE Report&lt;module\_name&gt;**
-
-
-
-**!=====================  Utility/Other routines for module.**
-
-! Insert as appropriate
-
-
-
-! Insert Standard Copyright Notice here.
-
-
-
-**END MODULE &lt;module\_name&gt;**
-
-
-
-The Subroutine Template:
-
-SUBROUTINE &lt;name&gt;
-
-
-
-          ! SUBROUTINE INFORMATION:
-
-          !       AUTHOR         &lt;author&gt;
-
-          !       DATE WRITTEN   &lt;date\_written&gt;
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS SUBROUTINE:
-
-          ! This subroutine needs a description.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! Needs description, as appropriate.
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! SUBROUTINE ARGUMENT DEFINITIONS:
-
-          ! na
-
-
-
-          ! SUBROUTINE PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-
-          ! na
-
-
-
-  RETURN
-
-
-
-END SUBROUTINE &lt;name&gt;
-
-
-
-And the Function Template:
-
-&lt;type&gt; FUNCTION &lt;name&gt;
-
-
-
-          ! FUNCTION INFORMATION:
-
-          !       AUTHOR         &lt;author&gt;
-
-          !       DATE WRITTEN   &lt;date\_written&gt;
-
-          !       MODIFIED       na
-
-          !       RE-ENGINEERED  na
-
-
-
-          ! PURPOSE OF THIS FUNCTION:
-
-          ! This function needs a description.
-
-
-
-          ! METHODOLOGY EMPLOYED:
-
-          ! Needs description, as appropriate.
-
-
-
-          ! REFERENCES:
-
-          ! na
-
-
-
-          ! USE STATEMENTS:
-
-          ! na
-
-
-
-  IMPLICIT NONE    ! Enforce explicit typing of all variables in this routine
-
-
-
-          ! FUNCTION ARGUMENT DEFINITIONS:
-
-          ! na
-
-
-
-          ! FUNCTION PARAMETER DEFINITIONS:
-
-          ! na
-
-
-
-          ! INTERFACE BLOCK SPECIFICATIONS
-
-          ! na
-
-
-
-          ! DERIVED TYPE DEFINITIONS
-
-          ! na
-
-
-
-          ! FUNCTION LOCAL VARIABLE DECLARATIONS:
-
-          ! na
-
-
-
-  RETURN
-
-
-
-END FUNCTION &lt;name&gt;
-
-Appendix E.  Test File Documentation
-====================================
-
-Each test file, whether released to the public or not, should be a best practice model and documented (comments at the top of the file) following the guidelines below.  The document template file is also included with each installation in the “ExampleFiles� folder – ExampleFilesDoc.txt
-
-! &lt;name of file&gt;
-
-! Basic file description: &lt;specify number of zones, stories in building, etc&gt;
-
-! Highlights: &lt;Purpose of this example file&gt;
-
-! Simulation Location/Run: &lt;location information, design days, run periods&gt;
-
-! Location:
-
-! Design Days (should have SummerDesignDay,WinterDesignDay designations):
-
-! Run Period (Weather File):
-
-! Run Control (should include this):
-
-!
-
-! Building: &lt;more details about building.  metric units, if also english enclose in []{} or ()&gt;
-
-! Floor Area:
-
-! Number of Stories:
-
-!
-
-! Zone Description Details:
-
-! Internal gains description: &lt;lighting level, equipment, number of occupants, infiltration, daylighting, etc&gt;
-
-! Interzone Surfaces:
-
-! Internal Mass:
-
-! People:
-
-! Lights:
-
-! Windows:
-
-! Detached Shading:
-
-! Daylight:
-
-! Natural Ventilation          :
-
-! Compact Schedules (preferred):
-
-! Solar Distribution:
-
-
-
-!
-
-! HVAC: &lt;HVAC description and plant supply, as appropriate&gt;
-
-! Purchased Air:
-
-! Zonal Equipment:
-
-! Central Air Handling Equipment:
-
-! System Equipment Autosize:
-
-! Purchased Cooling:
-
-! Purchased Heating:
-
-! Coils:
-
-! Pumps:
-
-! Boilers:
-
-! Chillers:
-
-! Towers:
-
-!
-
-! Results: &lt;how are results reported&gt;
-
-! Standard Reports:
-
-! Timestep or Hourly Variables:
-
-! Time bins Report:
-
-! HTML Report:
-
-! Environmental Emissions:
-
-! Utility Tariffs:
-
-Most of the example files have completed their documentation requirements and include plan views of the building.  Our naming convention uses an underscore (\_) as the first character of an input file “not for publication�.
-
-Appendix F. New or Changed Proposal Feature Template
-====================================================
-
-&lt;TITLE&gt;
-
-&lt;organization&gt;
-
-&lt;Date(s), Original, Revision, etc&gt;
-
-**Justification for Feature Update:**
-
-&lt;Required&gt;
-
-**Conference Call Conclusions:**
-
-&lt;Optional – note date of conference call where talked about&gt;
-
-**Other Conference Call Topics (not in scope of current proposal):**
-
-&lt;Optional&gt;
-
-**Overview:**
-
-&lt;Include Description of Feature and references&gt;
-
-**Approach:**
-
-**Testing/Validation/Data Source(s):**
-
-&lt;required&gt;
-
-**IO Ref (draft):**
-
-&lt;required&gt;
-
-**IDD Object (New):**
-
-&lt;include as appropriate&gt;
-
-**IDD Object(s) (Revised):**
-
-&lt;include as appropriate&gt;
-
-**Proposed Report Variables:**
-
-**Proposed additions to Meters:**
-
-**EngRef (draft):**
-
-&lt;required&gt;
-
-**Example File and Transition changes:**
-
-As needed.
-
-**Other documents:**
-
-As needed.
-
-Appendix G.
-===========
-
-
-
-
diff --git a/doc/src/docs/OutputDetailsAndExamples/OutputDetailsAndExamples.md b/doc/src/docs/OutputDetailsAndExamples/OutputDetailsAndExamples.md
deleted file mode 100644
index 5b428e68265..00000000000
--- a/doc/src/docs/OutputDetailsAndExamples/OutputDetailsAndExamples.md
+++ /dev/null
@@ -1,20372 +0,0 @@
-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Output Details and Examples</h1>
-<h2>EnergyPlus Outputs, Example Inputs and Data Set Files</h2>
-<br/>
-<p><i>( &#42;&#42;&#42;&#42;&#42;&#42;&#42;&#42; Message: This is a snazzy output tagline)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-Introduction
-============
-
-This document is intended to give an in-depth look at the various output files produced by EnergyPlus. Some of these may be referenced in various other parts of the documentation but are presented here with more details.
-
-The scripts that assist in running EnergyPlus will usually rename the standard names used in the program. The two scripts that are distributed with EnergyPlus are: **EPL-Run.bat** (which is used by the EP-Launch program) and **RunEPlus.bat**  (which can be used from the command line). The RunEPlus batch file can also be used to string together several runs such as usually termed “batch processing�. In renaming the files created by the program or its post-processing program(s), usually the file extension will be retained. The following table will illustrate the native EnergyPlus file name, a description of its contents and the EP-Launch “version� of the file. In this table, &lt;filename&gt; refers to the source/original file name (without extension) selected. Files are presented in alphabetic order. For output purposes, the most important files to understand are the eplusout.eso, eplusout.mtr and eplusout.err files. The first two are manipulated with the ReadVarsESO post processing program. The latter will contain any critical errors that were encountered during the run.
-
-Output Files
-============
-
-Output File List
-----------------
-
-Following are the native file names that are output from EnergyPlus; native – directly out of EnergyPlus. Usually you will not see these file names as batch files and interfaces will change them to be &lt;file name&gt;.&lt;ext&gt; or in some instances &lt;file name&gt;&lt;qualifier&gt;.&lt;ext&gt;. Usually the extension is the important piece and is described in the following table.
-
-Table 1. EnergyPlus Basic Output  Files
-
-<table class="table table-striped">
-<tr> 
- <th>Output File Name</th>
- <th>Description</th>
- <th>EP-Launch File Name</th>
-</tr>
-<tr>
- <td>eplusout.audit</td>
- <td>Echo of input, includes both IDD echo and IDF echo – may have errors shown in context with IDD or IDF statements</td>
- <td>&lt;filename&gt;.audit (without echoing IDD unless errors in IDD).</td>
-</tr>
-<tr>
- <td>eplusout.bnd</td>
- <td>This file contains details about the nodes and branches. Useful in determining if all your nodes are connected correctly. May be used to diagram the network/ nodes of the HVAC system.</td>
- <td>&lt;filename&gt;.bnd</td>
-</tr>
-<tr>
- <td>eplusout.dbg</td>
- <td>From Debug Output object – may be useful to support to help track down problems</td>
- <td>&lt;filename&gt;.dbg</td>
-</tr>
-<tr>
- <td>eplusout.dxf</td>
- <td>DXF (from Output:Surfaces:Drawing,DXF;)</td>
- <td>&lt;filename&gt;.dxf</td>
-</tr>
-<tr>
- <td>eplusout.edd</td>
- <td>Descriptive output from the EMS portion</td>
- <td>&lt;filename&gt;.edd</td>
-</tr>
-<tr>
- <td>eplusout.eio</td>
- <td>Contains several standard and optional “report� elements. CSV format – may be read directly into spreadsheet program for better formatting.</td>
- <td>&lt;filename&gt;.eio</td>
-</tr>
-<tr>
- <td>eplusout.end</td>
- <td>A one line summary of success or failure (useful for Interface programs)</td>
- <td>Not saved in the standard EPL-Run script file.</td>
-</tr>
-<tr>
- <td>eplusout.epmidf</td>
- <td>Output from EPMacro program – contains the idf created from the input imf file</td>
- <td>&lt;filename&gt;.epmidf</td>
-</tr>
-<tr>
- <td>eplusout.epmdet</td>
- <td>Output from EPMacro program – the audit/details of the EPMacro processing</td>
- <td>&lt;filename&gt;.epmdet</td>
-</tr>
-<tr>
- <td>eplusout.err</td>
- <td>Error file – contains very important information from running the program.</td>
- <td>&lt;filename&gt;.err</td>
-</tr>
-<tr>
- <td>eplusout.eso</td>
- <td>Standard Output File (contains results from both Output:Variable and Output:Meter objects).</td>
- <td>&lt;filename&gt;.eso</td>
-</tr>
-<tr>
- <td>eplusout.log</td>
- <td>Log of items that appear in the command file output from the run.</td>
- <td>&lt;filename&gt;.log</td>
-</tr>
-<tr>
- <td>eplusout.mdd</td>
- <td>Meter names that are applicable for reporting in the current simulation.</td>
- <td>&lt;filename&gt;.mdd</td>
-</tr>
-<tr>
- <td>eplusout.mtd</td>
- <td>Meter details report – what variables are on what meters and vice versa. This shows the meters on which the Zone: Lights Electric Energy appear as well as the contents of the Electricity:Facility meter.</td>
- <td>&lt;filename&gt;.mtd</td>
-</tr>
-<tr>
- <td>eplusout.mtr</td>
- <td>Similar to .eso but only has Output:Meter outputs.</td>
- <td>&lt;filename&gt;.mtr</td>
-</tr>
-<tr>
- <td>eplusout.rdd</td>
- <td>Variable names that are applicable for reporting in the current simulation.</td>
- <td>&lt;filename&gt;.rdd</td>
-</tr>
-<tr>
- <td>eplusout.shd</td>
- <td>Surface shadowing combinations report</td>
- <td>&lt;filename&gt;.shd</td>
-</tr>
-<tr>
- <td>eplusout.sln</td>
- <td>Similar to DXF output but less structured. Results of Output:Reports,Surface, Lines object.</td>
- <td>&lt;filename&gt;.sln</td>
-</tr>
-<tr>
- <td>eplusout.sql</td>
- <td>Mirrors the data in the .eso and .mtr files but is in SQLite format (for viewing with SQLite tools).</td>
- <td>&lt;filename&gt;.sql</td>
-</tr>
-<tr>
- <td>eplusssz.&lt;ext&gt;</td>
- <td>Results from the Sizing:System object. This file is “spreadsheet� ready. Different extensions (csv, tab, and txt) denote different “separators� in the file.</td>
- <td>&lt;filename&gt;Ssz.&lt;ext&gt;</td>
-</tr>
-<tr>
- <td>epluszsz.&lt;ext&gt;</td>
- <td>Results from the Sizing:Zone object. This file is “spreadsheet� ready. Different extensions (csv, tab, and txt) denote different “separators� in the file.</td>
- <td>&lt;filename&gt;Zsz.&lt;ext&gt;</td>
-</tr>
-<tr>
- <td>eplusmap.&lt;ext&gt;</td>
- <td>Daylighting intensity “map� output. Different extensions (csv, tab, and txt) denote different “separators� in the file.</td>
- <td>&lt;filename&gt;Map.&lt;ext&gt;</td>
-</tr>
-<tr>
- <td>eplusout.dfs</td>
- <td>This file contains the hourly pre-calculated daylight factors for exterior windows of a daylight zone.</td>
- <td>&lt;filename&gt;DFS.csv</td>
-</tr>
-<tr>
- <td>eplusscreen.csv</td>
- <td>Window screen transmittance (direct and reflected) “map� output.</td>
- <td>&lt;filename&gt;Screen.csv</td>
-</tr>
-<tr>
- <td>eplustbl.&lt;ext&gt;</td>
- <td>Results of tabular and economics requests. Different extensions (csv, tab, and txt) denote different “separators� in the file.</td>
- <td>&lt;filename&gt;Table.&lt;ext&gt;</td>
-</tr>
-<tr>
- <td>eplusout.svg</td>
- <td>Results from the HVAC-Diagram application. SVG is a Scalable Vector Graphics file for which several viewers can be found.</td>
- <td>&lt;filename&gt;.svg</td>
-</tr>
-<tr>
- <td>eplusout.sci</td>
- <td>File of cost information</td>
- <td>&lt;filename&gt;.sci</td>
-</tr>
-<tr>
- <td>eplusout.delightin</td>
- <td>File produced during DElight simulations – descriptive of EnergyPlus inputs into DElight inputs.</td>
- <td>&lt;filename&gt;delight.in</td>
-</tr>
-<tr>
- <td>eplusout.delightout</td>
- <td>File produced during DElight simulations – basic results from DElight simulation.</td>
- <td>&lt;filename&gt;delight.out</td>
-</tr>
-<tr>
- <td>eplusout.wrl</td>
- <td>VRML output from (Output:Reports, Surfaces, VRML)</td>
- <td>&lt;filename&gt;.wrl</td>
-</tr>
-</table>
-
-
-
-
-In addition to the basic output files from EnergyPlus there are three standard “hybrid� output files. These are called “hybrid� because they are a result of post-processing after EnergyPlus has completed. Note that if there is an error during processing, these will not normally be “complete�.
-
-Table 2. "Hybrid" EnergyPlus Output Files
-
-<table class="table table-striped">
-<tr>
-<th>Output File Name</th>
-<th>Description</th>
-<th>EP-Launch File Name</th>
-</tr>
-<tr>
-<td>eplusout.&lt;ext&gt;
- </td>
-<td>“spreadsheet� ready file that contains either all the report variables requested (default: up to limit of 255) from the input file or specific ones specified by the user. Different extensions (csv, tab, and txt denote different “separators� in the file.</td>
-<td>&lt;filename&gt;.csv
-or
-&lt;filename&gt;.tab
-or
-&lt;filename&gt;.txt</td>
-</tr>
-<tr>
-<td>eplusmtr.&lt;ext&gt;
- </td>
-<td>“spreadsheet� ready file that contains either all the report meter requests (default: up to 255) from the input file or specific ones specified by the user. Different extensions (csv, tab, and txt denote different “separators� in the file.</td>
-<td>&lt;filename&gt;Meter.csv
-or
-&lt;filename&gt;Meter.tab
-or
-&lt;filename&gt;Meter.txt</td>
-</tr>
-<tr>
-<td>readvars.rvaudit</td>
-<td>Results of any “ReadVarsESO� execution in the current batch run.</td>
-<td>&lt;filename&gt;.rvaudit</td>
-</tr>
-</table>
-
-Now, each file will be described in more detail with some examples of use.
-
-eplusout.audit
---------------
-
-This file is simply the echo of the inputs to the EnergyPlus program – the Energy+.idd (data dictionary) and in.idf (&lt;filename&gt;.idf – the input data file). Every attempt has been made to not require this file to be saved – errors are interpreted as much as possible and encapsulated onto the eplusout.err file. Any errors in the data dictionary processing should be accomplished during development – users should never see errors there. Thus, this file is not “saved� after processing by the standard script file. Occasionally, you may wish to view this file because of something obscure.
-
-An excerpt of the file follows. Lines in green are notes produced from EnergyPlus (some of these are more useful to developers than users). Lines in red are lines with error messages shown to illustrate context. The other lines are echoes from inputs (with line numbers).
-
-In all the examples, the actual version of the EnergyPlus exe would appear. In the examples these will be shown as: &lt;version&gt;.
-
-```
-  Processing Data Dictionary (Energy+.idd) File -- Start
-     1 !IDD_Version <version>
-     2 ! **************************************************************************
-     3 !
-<reduced for brevity>
- 13000        \key DETAILS
- 13001        \key Vertices
- 13002        \key DetailsWithVertices
-  Processing Data Dictionary (Energy+.idd) File -- Complete
-  Maximum number of Alpha Args=        4500
-  Maximum number of Numeric Args=        1800
-  Number of Object Definitions=         473
-  Number of Section Definitions=           2
-  Processing Input Data File (in.idf) -- Start
-     1 ! Basic file description: Basic illustration of using Purchased Air as a system
-     2 ! Run:      2 design days.
-     3 !           2 annual run periods, 2 summer days and 3 winter days.
-<reduced for brevity>
-    63     RunPeriod,          ! 3 day winter simuluation
-    64               1,                1,  ! Start Month ,Day
-    65               1,                3;  ! End Month ,Day
-   ** Warning ** Object=RUNPERIOD, entered with less than minimum number of fields.
-   **   ~~~   ** Attempting fill to minimum.
-    66  MATERIAL:Regular,A1 - 1 IN STUCCO,  !- Material Name
-<reduced for brevity>
-   784 End Simulation Data;
-  Processing Input Data File (in.idf) -- Complete
-  Number of IDF "Lines"=         359
-  Maximum number of Alpha IDF Args=          29
-  Maximum number of Numeric IDF Args=          20
- Getting object=VERSION
- Getting object=TIMESTEP
- Getting object=SIMULATIONCONTROL
- Getting object=SIZING:PARAMETERS
- Getting object=SIZING:ZONE
- Getting object=SIZING:SYSTEM
- Getting object=SIZING:PLANT
-<etc>
-MaxRVariable=        5000
-MaxIVariable=         100
-NumEnergyMeters=         108
-NumVarMeterArrays=         106
-```
-
-eplusout.bnd
-------------
-
-The “branch node details� (bnd) file is intended to give enough information that one could (with a chosen software) diagram the nodes and components of the HVAC system. It may or may not achieve that objective. Of more use may be its illustration of node connection/branch errors that aren’t detected by the software. This file has the details to support any “node connection� errors that will be noted in the eplusout.err file. Branch validation is shown in this file. Branches are checked to assure that each output node of the branch element is an input node to the next branch element. Cross-branch checking is not done directly within the program though the details will illustrate some problems of that nature.
-
-Supply and Return Air Paths are also checked and feedback about each item are shown.
-
-As is standard with many EnergyPlus output files, this file is CSV (comma-delimited) such that it can be read by spreadsheet programs for further manipulation by the user.
-
-An example will illustrate. Notes about the reporting are highlighted in green.
-
-Program Version,EnergyPlus, &lt;version&gt;
-
-! This file shows details about the branches, nodes, and other
-
-! elements of the flow connections.
-
-! This file is intended for use in "debugging" potential problems
-
-! that may also be detected by the program, but may be more easily
-
-! identified by "eye".
-
-! This file is also intended to support software which draws a
-
-! schematic diagram of the HVAC system.
-
-! ===============================================================
-
-! \#Nodes,&lt;Number of Unique Nodes&gt;
-
- \#Nodes,11
-
-**List of all nodes follows. \# references may be an indication of faulty node spec (or not)**
-
-! &lt;Node&gt;,&lt;NodeNumber&gt;,&lt;Node Name&gt;,&lt;Node Fluid Type&gt;,&lt;\# Times Node Referenced After Definition&gt;
-
- Node,1,SUPPLY INLET NODE,Air,3
-
- Node,2,FAN INLET NODE,Air,4
-
-&lt;reduced for brevity&gt;
-
-Node,10,ZONE EQUIPMENT OUTLET NODE,Air,2
-
- Node,11,RELIEF AIR OUTLET NODE,Air,1
-
-! ===============================================================
-
-! Suspicious nodes have 0 references. It is normal for some nodes, however.
-
-! Suspicious nodes have 0 references.  It is normal for some nodes, however.
-
-! Listing nodes with 0 references (culled from previous list):
-
-! &lt;Suspicious Node&gt;,&lt;NodeNumber&gt;,&lt;Node Name&gt;,&lt;Node Fluid Type&gt;,&lt;\# Times Node Referenced After Definition&gt;
-
- Suspicious Node,7,MAIN ZONE NODE,Air,0
-
-**List of branches follow.**
-
-! &lt;\#Branch Lists&gt;,&lt;Number of Branch Lists&gt;
-
- \#Branch Lists,1
-
-! &lt;Branch List&gt;,&lt;Branch List Count&gt;,&lt;Branch List Name&gt;,&lt;Loop Name&gt;,&lt;Loop Type&gt;,&lt;Number of Branches&gt;
-
-! &lt;Branch&gt;,&lt;Branch Count&gt;,&lt;Branch Name&gt;,&lt;Loop Name&gt;,&lt;Loop Type&gt;,&lt;Branch Inlet Node Name&gt;,&lt;Branch Outlet Node Name&gt;
-
- Branch List,1,AIR LOOP BRANCHES,EVAP COOLER SYSTEM,Air,1
-
-   Branch,1,AIR LOOP MAIN BRANCH,EVAP COOLER SYSTEM,Air,SUPPLY INLET NODE,SUPPLY OUTLET NODE
-
-! ===============================================================
-
-! &lt;\#Supply Air Paths&gt;,&lt;Number of Supply Air Paths&gt;
-
-! &lt;\#Supply Air Paths&gt;,&lt;Number of Supply Air Paths&gt;
-
- \#Supply Air Paths,1
-
-! &lt;Supply Air Path&gt;,&lt;Supply Air Path Count&gt;,&lt;Supply Air Path Name&gt;,&lt;AirLoopHVAC Name&gt;
-
-! &lt;\#Components on Supply Air Path&gt;,&lt;Number of Components&gt;
-
-! &lt;Supply Air Path Component&gt;,&lt;Component Count&gt;,&lt;Component Type&gt;,&lt;Component Name&gt;,&lt;AirLoopHVAC Name&gt;
-
-! &lt;\#Outlet Nodes on Supply Air Path Component&gt;,&lt;Number of Nodes&gt;
-
-! &lt;Supply Air Path Component Nodes&gt;,&lt;Node Count&gt;,&lt;Component Type&gt;,&lt;Component Name&gt;,&lt;Inlet Node Name&gt;,&lt;Outlet Node Name&gt;,&lt;AirLoopHVAC Name&gt;
-
- Supply Air Path,1,ZONE SUPPLY AIR PATH,EVAP COOLER SYSTEM
-
-   \#Components on Supply Air Path,1
-
-   Supply Air Path Component,1,AIRLOOPHVAC:ZONESPLITTER,ZONE SUPPLY AIR SPLITTER,EVAP COOLER SYSTEM
-
-     \#Outlet Nodes on Supply Air Path Component,1
-
-     Supply Air Path Component Nodes,1,AIRLOOPHVAC:ZONESPLITTER,ZONE SUPPLY AIR SPLITTER,ZONE EQUIPMENT INLET NODE,MAIN ZONE INLET NODE,EVAP COOLER SYSTEM
-
-! &lt;\#Nodes on Supply Air Path&gt;,&lt;Number of Nodes&gt;
-
-! &lt;Supply Air Path Node&gt;,&lt;Node Type&gt;,&lt;Node Count&gt;,&lt;Node Name&gt;,&lt;AirLoopHVAC Name&gt;
-
-\#Nodes on Supply Air Path,2
-
-   Supply Air Path Node,Inlet Node,1,ZONE EQUIPMENT INLET NODE,EVAP COOLER SYSTEM
-
-   Supply Air Path Node,Outlet Node,2,MAIN ZONE INLET NODE,EVAP COOLER SYSTEM
-
-! ===============================================================
-
-! &lt;\#Return Air Paths&gt;,&lt;Number of Return Air Paths&gt;
-
-! &lt;\#Return Air Paths&gt;,&lt;Number of Return Air Paths&gt;
-
- \#Return Air Paths,1
-
-! &lt;Return Air Path&gt;,&lt;Return Air Path Count&gt;,&lt;Return Air Path Name&gt;,&lt;AirLoopHVAC Name&gt;
-
-! &lt;\#Components on Return Air Path&gt;,&lt;Number of Components&gt;
-
-! &lt;Return Air Path Component&gt;,&lt;Component Count&gt;,&lt;Component Type&gt;,&lt;Component Name&gt;,&lt;AirLoopHVAC Name&gt;
-
-! &lt;\#Inlet Nodes on Return Air Path Component&gt;,&lt;Number of Nodes&gt;
-
-! &lt;Return Air Path Component Nodes&gt;,&lt;Node Count&gt;,&lt;Component Type&gt;,&lt;Component Name&gt;,&lt;Inlet Node Name&gt;,&lt;Outlet Node Name&gt;,&lt;AirLoopHVAC Name&gt;
-
- Return Air Path,1,ZONE RETURN AIR PATH,EVAP COOLER SYSTEM
-
-   \#Components on Return Air Path,1
-
-   Return Air Path Component,1,AIRLOOPHVAC:ZONEMIXER,ZONE RETURN AIR MIXER,EVAP COOLER SYSTEM
-
-     \#Inlet Nodes on Return Air Path Component,1
-
-     Return Air Path Component Nodes,1,AIRLOOPHVAC:ZONEMIXER,ZONE RETURN AIR MIXER,MAIN ZONE OUTLET NODE,ZONE EQUIPMENT OUTLET NODE,EVAP COOLER SYSTEM
-
-! &lt;\#Nodes on Return Air Path&gt;,&lt;Number of Nodes&gt;
-
-! &lt;Return Air Path Node&gt;,&lt;Node Type&gt;,&lt;Node Count&gt;,&lt;Node Name&gt;,&lt;AirLoopHVAC Name&gt;
-
-   \#Nodes on Return Air Path,2
-
-   Return Air Path Node,Outlet Node,1,ZONE EQUIPMENT OUTLET NODE,EVAP COOLER SYSTEM
-
-   Return Air Path Node,Inlet Node,2,MAIN ZONE OUTLET NODE,EVAP COOLER SYSTEM
-
-! ===============================================================
-
-! \#Outside Air Nodes,&lt;Number of Outside Air Nodes&gt;
-
-! \#Outdoor Air Nodes,&lt;Number of Outdoor Air Nodes&gt;
-
- \#Outdoor Air Nodes,1
-
-! &lt;Outdoor Air Node&gt;,&lt;NodeNumber&gt;,&lt;Node Name&gt;
-
- Outdoor Air Node,5,OUTSIDE AIR INLET NODE
-
-! ===============================================================
-
-**Component sets. Very important for node connection error detection.**
-
-! &lt;\#Component Sets&gt;,&lt;Number of Component Sets&gt;
-
- \#Component Sets,4
-
-! &lt;Component Set&gt;,&lt;Component Set Count&gt;,&lt;Parent Object Type&gt;,&lt;Parent Object Name&gt;,&lt;Component Type&gt;,&lt;Component Name&gt;,&lt;Inlet Node ID&gt;,&lt;Outlet Node ID&gt;,&lt;Description&gt;
-
- Component Set,1,BRANCH,AIR LOOP MAIN BRANCH,AIRLOOPHVAC:OUTDOORAIRSYSTEM,OUTSIDE AIR SYSTEM,SUPPLY INLET NODE,FAN INLET NODE,Air Nodes
-
- Component Set,2,BRANCH,AIR LOOP MAIN BRANCH,FAN:CONSTANTVOLUME,SUPPLY FAN,FAN INLET NODE,EVAP COOLER INLET NODE,Air Nodes
-
- Component Set,3,BRANCH,AIR LOOP MAIN BRANCH,EVAPORATIVECOOLER:DIRECT:CELDEKPAD,EVAPORATIVE COOLER,EVAP COOLER INLET NODE,SUPPLY OUTLET NODE,Evap Air Nodes
-
- Component Set,4,AIRLOOPHVAC:OUTDOORAIRSYSTEM,OUTSIDE AIR SYSTEM,OUTDOORAIR:MIXER,OUTSIDE AIR MIXING BOX,OUTSIDE AIR INLET NODE,FAN INLET NODE,Air Nodes
-
-**Similar details for Plant Loops, Condenser Loops, Controlled Zones, etc.**
-
-
-
-eplusout.dbg
-------------
-
-Developers use this file during debugging and can be “turned on� by the DEBUG OUTPUT object in the input file. The only reason a user might specify this flag would be to send a file to the support group.
-
-**Output:DebuggingData, 1, 0;    ! standard debug output, during simulation days**
-
-The standard debug output appears like this:
-
-Day of Sim     Hour of Day    Time
-
-           1           1  0.166666666666667
-
-node \#   Temp      MassMinAv  MassMaxAv TempSP   MassFlow   MassMin    MassMax    MassSP      Press        Enthal     HumRat    Fluid Type
-
-   1    -12.500     0.000     0.000     0.000     0.0000     0.0000     0.0000     0.0000   100344.00     -9363.63    0.00129  Air
-
-   2    -12.500     0.000     0.000     0.000     0.0000     0.0000     0.0000     0.0000   100344.00     -9363.63    0.00129  Air
-
-   3    -12.500     0.000     0.000     0.000     0.0000     0.0000     0.0000     0.0000   100344.00     -9363.63    0.00129  Air
-
-   4    -12.500     0.000     0.000     0.000     0.0000     0.0000     0.0000     0.0000   100344.00     -9363.63    0.00129  Air
-
-   5     50.000     0.000     0.000     0.000     0.0320     0.0000     0.0000     0.0000   100344.00     60617.55    0.00400  Air
-
-   6     50.000     0.000     0.000     0.000     0.0326     0.0000     0.0000     0.0000   100344.00     60617.55    0.00400  Air
-
-   7     50.000     0.000     0.000     0.000     0.1636     0.0000     0.0000     0.0000   100344.00     60617.55    0.00400  Air
-
-   8     50.000     0.000     0.000     0.000     0.1648     0.0000     0.0000     0.0000   100344.00     60617.55    0.00400  Air
-
-   9      0.000     0.000     0.000     0.000     0.0000     0.0000     0.0000     0.0000        0.00         0.00    0.00000  blank
-
-  10      0.000     0.000     0.000     0.000     0.0000     0.0000     0.0000     0.0000        0.00         0.00    0.00000  blank
-
-  11      0.000     0.000     0.000     0.000     0.0000     0.0000     0.0000     0.0000        0.00         0.00    0.00000  blank
-
-  12      0.000     0.000     0.000     0.000     0.0000     0.0000     0.0000     0.0000        0.00         0.00    0.00000  blank
-
-eplusout.dxf
-------------
-
-The DXF output report file is formatted according to the “Data Exchange Format� standard rules for representing CADD type coordinates. The file can be used in several inexpensive, shareware or freeware viewers. Quickview Plus ™ can display DXF files as shown in Figure 1 below. A free program originally from Autocad™, Voloview Express™, can display solid model rendering as shown in Figure 2. Other viewers are available from Microstation™, Visio™ and other shareware or freeware vendors.
-
-This file is generated when the following line is included in the IDF.
-
-**Output:Surfaces:Drawing, DXF;**
-
-You can ask it to triangulate surfaces with &gt;4 sides:
-
-**Output:Surfaces:Drawing, DXF, Triangulate3dface;**
-
-In addition to the building shape (including detached shading elements), the DXF view includes a “true north� arrow (at ground level) and the name from the BUILDING object.
-
-![SCCPAPER](media/image001.jpg)
-
-Figure 1. Quick View Plus version of DXF file
-
-Even in the Quick View version, you can see that the different building elements have different colors. These are the “original� colors used in EnergyPlus. The current default color scheme is shown in the following figure of the solid model.
-
-![DXFSolid](media/image002.jpg)
-
-Figure 2. Voloview 3D Solid view
-
-The DXF file of itself is an ASCII file, with a specific structure as specified in the standard. An excerpt of the file is shown below:
-
-```
-SECTION
-  2
-ENTITIES
-  0
-TEXT
-  8
-1
-  6
-CONTINUOUS
- 62
-  3
- 10
-      -11.00000
- 20
-        3.00000
- 30
-        0.10000
- 40
- .25
-  1
-True North
- 41
- 0.0
-  7
-MONOTXT
-210
-0.0
-220
-0.0
-230
-1.0
-  0
-<reduced for brevity>
-
-3DFACE
-  8
-1
- 62
-  3
- 10
-      -10.00000
- 20
-        3.00000
- 30
-        0.10000
- 11
-      -10.00000
- 21
-        3.00000
- 31
-        0.00000
- 12
-      -10.00000
- 22
-        0.00000
- 32
-        0.00000
- 13
-      -10.00000
- 23
-        0.00000
- 33
-        0.10000
-  0
-ENDSEC
-  0
-EOF
-999
-DXF created from EnergyPlus
-999
-```
-Program Version,EnergyPlus, &lt;version&gt;
-
-eplusout.edd
------------
-
-This file is invoked by including an Output:EnergyManagementSystem input object. The EDD file contains three different types of information related to the Energy Management System (EMS) including: (1) listing of available actuators, (2) listing of available internal variables, and (3) a record of the execution of user’s programs for the EnergyPlus Runtime Language (Erl).
-
-The EMS feature in EnergyPlus uses “Actuators� to do control operations. The actuators available in a given model depend on the non-EMS-related content of the input file. Similar to how EnergyPlus reports the available output variables to the RDD file, a list of available actuators can be written to the EDD file. There are three settings in the Output:EnergyManagementSystem input object that control how actuators are listed. Selecting “None� directs the program to not list the available actuators. Selecting “NotByUniqueKeyNames� directs the program to provide a concise listing of the available actuators that does not include their enumeration by unique name. Selecting “Verbose� directs the program to provide a complete listing of the available actuators including the unique identifying names. An example listing of actuators using the  “NotByUniqueKeyNames�  option follows.
-
-! &lt;EnergyManagementSystem:Actuator Available&gt;, \*, Component Type, 'Control Type, Units
-
-EnergyManagementSystem:Actuator Available, \*,Schedule:Compact,Schedule Value,[ ]
-
-EnergyManagementSystem:Actuator Available, \*,People,Number of People,[each]
-
-EnergyManagementSystem:Actuator Available, \*,Lights,Electric Power Level,[W]
-
-EnergyManagementSystem:Actuator Available, \*,ElectricEquipment,Electric Power Level,[W]
-
-EnergyManagementSystem:Actuator Available, \*,Window Shading Control,Control Status,[ShadeStatus]
-
-EnergyManagementSystem:Actuator Available, \*,Zone Temperature Control,Heating Setpoint,[C]
-
-EnergyManagementSystem:Actuator Available, \*,Zone Temperature Control,Cooling Setpoint,[C]
-
-EnergyManagementSystem:Actuator Available, \*,Surface,Interior Surface Convection Heat Transfer Coefficient,[W/m2-K]
-
-EnergyManagementSystem:Actuator Available, \*,Surface,Exterior Surface Convection Heat Transfer Coefficient,[W/m2-K]
-
-EnergyManagementSystem:Actuator Available, \*,Ideal Loads Air System,Air Mass Flow Rate,[kg/s]
-
-
-
-The EMS feature in EnergyPlus uses “Internal Variables� to obtain input data for use in scaling the results of control calculations. The internal variables available in a give model depend on the non-EMS-related content of the input file. Similar to how EnergyPlus reports the available output variables to the RDD file, a list of available internal variables can be written to the EDD file. There are three settings in the Output:EnergyManagementSystem input object that control how internal variables are listed. Selecting “None� directs the program to not list the available internal variables. Selecting “NotByUniqueKeyNames� directs the program to provide a concise listing of the available internal variables that does not include their enumeration by unique name. Selecting “Verbose� directs the program to provide a complete listing of the available internal variables including the unique identifying names. An example listing of actuators using the  “NotByUniqueKeyNames�  option follows.
-
-! &lt;EnergyManagementSystem:InternalVariable Available&gt;, \*, Internal Data Type
-
-EnergyManagementSystem:InternalVariable Available, \*,People Count Design Level,[each]
-
-EnergyManagementSystem:InternalVariable Available, \*,Lighting Power Design Level,[W]
-
-EnergyManagementSystem:InternalVariable Available, \*,Plug and Process Power Design Level,[W]
-
-EnergyManagementSystem:InternalVariable Available, \*,Zone List Multiplier,[ ]
-
-EnergyManagementSystem:InternalVariable Available, \*,Zone Floor Area,[m2]
-
-EnergyManagementSystem:InternalVariable Available, \*,Zone Air Volume,[m3]
-
-EnergyManagementSystem:InternalVariable Available, \*,Zone Multiplier,[ ]
-
-EnergyManagementSystem:InternalVariable Available, \*,Zone List Multiplier,[ ]
-
-
-
-The EMS uses the EnergyPlus Runtime Language, or Erl, to do custom controlling. When Erl programs are being developed, the EDD becomes a primary source of information for debugging. When a line of Erl code is executed, the program can output records called “line traces� that are useful for debugging because they show the outcome of each line of code. There are three settings in the Output:EnergyManagementSystem input object that control how line traces are reported. Selecting “None� directs the program to not write out any line traces. Selecting “ErrorsOnly� directs the program to only write line traces when computation errors are encountered (such as divide by zero). Selecting “Verbose� directs the program to write out line traces for each and every line of Erl program code that is executed.
-
-It is very important to be careful with the EDD file. The Verbose option should be used with care because a full line-by-line trace of Erl program execution for an annual run can easily create an enormous computer file that is too large for most computer systems.  It is possible for EnergyPlus to generate an EDD file that cannot be opened in traditional text editors.
-
-eplusout.eio
-------------
-
-This file contains some standard and some optional “reports�. It is intended to be a somewhat intelligent report of input conditions when they don’t fit well in other places or when they aren’t substantial enough for their own “file�. (e.g. **eplusout.bnd**)  Contents of the file are somewhat documented in various places in the [Input Output Reference document](file:///E:\Docs4PDFs\InputOutputReference.pdf) – as results of objects. This file or portions of it can be easily imported into spreadsheet programs and more analysis done there. Contents of this file include construction details, location information, “environment� information, number of “warmup� days required in each environment.
-
-The form of the file is a data dictionary line followed by the data. In this case, the data dictionary line precedes the first “data� line though there may be several defining “dictionary lines�. Each dictionary line will show the field as &lt;field name&gt; followed by other fields that will be in the data lines. Data will be displayed similarly. Each field of dictionary or data will be separated from the next by a comma “,� – and produce a comma delimited file. However, the lines for data will not be contiguous – some follow a stream of consciousness of the EnergyPlus execution.
-
-This section is subdivided into grouped sections by type.
-
-Note that the lines in the eplusout.eio file can be extremely long (current limit is 500 characters).
-
-### Simulation Parameters
-
-! &lt;Version&gt;, Version ID
-
- Version, &lt;version&gt;
-
-! &lt;Timesteps per Hour&gt;, \#TimeSteps, Minutes per TimeStep
-
- Timesteps Per Hour,  4, 15
-
-! &lt;Run Control&gt;, Do Zone Sizing, Do System Sizing, Do Plant Sizing, Do Design Days, Do Weather Simulation
-
- Run Control, Yes, Yes, No, No, Yes
-
-! &lt;GroundTemperatures&gt;, Months From Jan to Dec {Deg C}
-
- GroundTemperatures,  20.03,  20.03,  20.13,  20.30,  20.43,  20.52,  20.62,  20.77,  20.78,  20.55,  20.44,  20.20
-
-! &lt;GroundTemperatures:Surface&gt;, Months From Jan to Dec {Deg C}
-
- GroundTemperatures:Surface,  18.00,  18.00,  18.00,  18.00,  18.00,  18.00,  18.00,  18.00,  18.00,  18.00,  18.00,  18.00
-
-! &lt;GroundTemperatures:Deep&gt;, Months From Jan to Dec {Deg C}
-
- GroundTemperatures:Deep,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00
-
-! &lt;GroundReflectances&gt;, Months From Jan to Dec {dimensionless}
-
- GroundReflectances,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20
-
-! &lt;Snow Ground Reflectance Modifiers&gt;, Normal, Daylighting {dimensionless}
-
- Snow Ground Reflectance Modifiers,   1.000,   1.000
-
-! &lt;Snow GroundReflectances&gt;, Months From Jan to Dec {dimensionless}
-
- Snow GroundReflectances,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20
-
-! &lt;Snow GroundReflectances For Daylighting&gt;, Months From Jan to Dec {dimensionless}
-
- Snow GroundReflectances For Daylighting,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20
-
-! &lt;Location&gt;, Location Name, Latitude {N+/S- Deg}, Longitude {E+/W- Deg},  Time Zone Number {GMT+/-}, Elevation {m},  Standard Pressure at Elevation {Pa}
-
-Location,CHICAGO IL USA TMY2-94846 WMO\#=725300,41.78,-87.75,-6.00,190.00,99063.
-
-! &lt;Building Information&gt;, Building Name,North Axis {deg},Terrain,  Loads Convergence Tolerance Value,Temperature Convergence Tolerance Value,  Solar Distribution,Maximum Number of Warmup Days,Minimum Number of Warmup Days
-
- Building, BUILDING,  30.000,City,   0.04000,   0.40000,FullExterior,25,6
-
-! Inside Convection Algorithm, Value {Simple | Detailed | CeilingDiffuser}
-
-Inside Convection Algorithm,Simple
-
-! Outside Convection Algorithm, Value {Simple | Detailed}
-
-Outside Convection Algorithm,Simple
-
-! Solution Algorithm, Value {CTF | EMPD | CONDFD | HAMT}
-
-Solution Algorithm, CTF
-
-! Sky Radiance Distribution, Value {Anisotropic}
-
-Sky Radiance Distribution,Anisotropic
-
-! &lt;Environment:Site Atmospheric Variation&gt;,Wind Speed Profile Exponent {},Wind Speed Profile Boundary Layer Thickness {m},Air Temperature Gradient Coefficient {K/m}
-
-Environment:Site Atmospheric Variation,0.330,460.000,6.500000E-003
-
-! &lt; Input Surface Geometry Information&gt;,Starting Corner,Vertex Input Direction,Coordinate System
-
- SurfaceGeometry,UpperLeftCorner,CounterClockwise,RelativeCoordinateSystem
-
-! &lt;Program Control Information:Threads/Parallel Sims&gt;, Threading Supported,Maximum Number of Threads, Env Set Threads (OMP\_NUM\_THREADS), EP Env Set Threads (EP\_OMP\_NUM\_THREADS). IDF Set Threads, Number of Threads Used (Interior Radiant Exchange), Number NominalSurface, Number Parallel Sims
-
-Program Control:Threads/Parallel Sims, Yes,2, Not Set, Not Set, Not Set, 2, 60, N/A
-
-The simulation parameters output is the simplest form of reporting in the **eplusout.eio** file. Each of the “header� records (lines starting with an “!�) are followed immediately by the one and only data line. By and large, these data lines are all merely echoes of the entries in the IDF (or defaulted for blank fields). For most of these descriptions, you can look at the object fields (of same name) in the [Input Output Reference](file:///E:\Docs4PDFs\InputOutputReference.pdf) document.
-
-### Version
-
-! &lt;Version&gt;, Version ID
-
- Version, &lt;version&gt;
-
-This is the version of the IDF as entered in the IDF file. If it does not match the current EnergyPlus Version, a warning will be issued and show in the **eplusout.err** file.
-
-### Timestep
-
-! &lt;Timesteps per Hour&gt;, \#TimeSteps, Minutes per TimeStep
-
- Timesteps Per Hour,  4, 15
-
-This is the number of timesteps in hour as entered in the IDF file as well as showing how many minutes will encompass each timestep (i.e. 4 timesteps in hour = 15 minutes per timestep).
-
-### SimulationControl
-
-! &lt;Run Control&gt;, Do Zone Sizing, Do System Sizing, Do Plant Sizing, Do Design Days, Do Weather Simulation, Do HVAC Sizing Simulation
-
- Run Control, Yes, Yes, Yes, No, Yes, No
-
-This shows how the sizing and running (design days vs. weather file) will be accomplished. Design days are required for sizing but do not necessarily need to be “run� after sizing has completed. Thus, the user can choose to do sizing, not do a “normal� calculation with the design day definitions but then go ahead and run the full simulation year.  Some advanced sizing methods require also running HVAC Sizing Simulations.
-
-### Building
-
-! &lt;Building Information&gt;, Building Name,North Axis {deg},Terrain,  Loads Convergence Tolerance Value,Temperature Convergence Tolerance Value,  Solar Distribution,Maximum Number of Warmup Days
-
- Building Information, BUILDING,  30.000,City,   0.04000,   0.40000,FullExterior,25
-
-This shows the values put in for the Building Object in the IDF.
-
-### Inside Convection Algorithm
-
-! &lt;Inside Convection Algorithm&gt;, Value {Simple | Detailed | CeilingDiffuser}
-
-Inside Convection Algorithm,Simple
-
-This shows the global inside (interior) convection algorithm selected by the IDF value. This may be overridden by zone entries or even surface entries.
-
-### Outside Convection Algorithm
-
-! &lt;Outside Convection Algorithm&gt;, Value {Simple | Detailed ! TARP ! MoWitt ! DOE-2 ! BLAST}
-
-Outside Convection Algorithm,Simple
-
-This shows the global outside (exterior) convection algorithm selected by the IDF value. This may be overridden by zone entries or even surface entries.
-
-### Solution Algorithm
-
-! &lt;Solution Algorithm&gt;, Value {CTF | EMPD | CONDFD | HAMT},Inside Surface Max Temperature Limit{C}
-
-Solution Algorithm, CTF,200
-
-This shows the solution algorithm approach selected by the IDF value and Inside Surface Max Temperature override or default value.
-
-### Sky Radiance Distribution
-
-! &lt;Sky Radiance Distribution&gt;, Value {Anisotropic}
-
-Sky Radiance Distribution,Anisotropic
-
-This shows the solution algorithm approach used in the simulation. As this value cannot be changed by the user, it is shown for information only.
-
-### Site Atmospheric Variation
-
-! &lt;Environment:Site Atmospheric Variation&gt;,Wind Speed Profile Exponent {},Wind Speed Profile Boundary Layer Thickness {m},Air Temperature Gradient Coefficient {K/m}
-
-Environment:Site Atmospheric Variation,0.330,460.000,6.500000E-003
-
-This shows actual values used for Site Atmospheric Variations.
-
-### Shadowing/Sun Position Calculations
-
-! &lt;Shadowing/Sun Position Calculations&gt; [Annual Simulations], Calculation Method, Value {days}, Allowable Number Figures in Shadow Overlap {}, Polygon Clipping Algorithm, Sky Diffuse Modeling Algorithm
-
-Shadowing/Sun Position Calculations, AverageOverDaysInFrequency, 20, 15000, SutherlandHodgman, SimpleSkyDiffuseModeling
-
-This shows how many days between the re-calculation of solar position during a weather file simulation. While a smaller number of days will lead to a more accurate solar position estimation (solar position is important in shadowing as well as determining how much solar enters the space), it also increases the calculation time necessarily to complete the simulation. The default, re-calculating every 20 days, gives a good compromise. The allowable number of figures in a shadow overlap can be increased if necessary for the model. There are two calculation methods available: AverageOverDaysInFrequency (default) and DetailedTimestepIntegration.
-
-### AirflowNetwork Model:Control
-
-! &lt;AirflowNetwork Model:Control&gt;, No Multizone or Distribution/Multizone with Distribution/Multizone without Distribution/Multizone with Distribution only during Fan Operation
-
-AirflowNetwork Model:Control,MultizoneWithoutDistribution
-
-This shows the AirflowNetwork Model:Control selected by the IDF value in the object AirflowNetwork:SimulationControl.
-
-### AirflowNetwork Model:Wind Direction
-
-! &lt;AirflowNetwork Model:Wind Direction&gt;, Wind Direction \#1 to n (degree)
-
-AirflowNetwork Model:Wind Direction, 0.0,30.0,60.0,90.0,120.0,150.0,180.0,210.0,240.0,270.0,300.0,330.0
-
-#### Field: &lt;AirflowNetwork Model:Wind Direction&gt;
-
-This field contains the field name “AirflowNetwork Model:Wind Direction�.
-
-#### Field: Wind Direction \#1 to n
-
-These values are the wind directions corresponding to the first through the Nth wind pressure coefficient value. If Wind Pressure Coefficient Type = Input in the AirflowNetwork:SimulationControl object, the wind directions described here are the inputs specified in the AirflowNetwork:MultiZone:WindPressureCoefficientArray object,. If Wind Pressure Coefficient Type = SurfaceAverageCalculation in the AirflowNetwork:SimulationControl object, the wind directions are also described here and are fixed at 30 degree increments.
-
-### AirflowNetwork Model:Wind Pressure Coefficients
-
-! &lt;AirflowNetwork Model:Wind Pressure Coefficients&gt;, Name, Wind Pressure Coefficients \#1 to n (dimensionless)
-
-AirflowNetwork Model:Wind Pressure Coefficients, NFACADE\_WPCVALUE, 0.60,0.48,4.00E-002,-0.56,-0.56,-0.42,-0.37,-0.42,-0.56,-0.56,4.00E-002,0.48
-
-AirflowNetwork Model:Wind Pressure Coefficients, EFACADE\_WPCVALUE, -0.56,4.00E-002,0.48,0.60,0.48,4.00E-002,-0.56,-0.56,-0.42,-0.37,-0.42,-0.56
-
-AirflowNetwork Model:Wind Pressure Coefficients, SFACADE\_WPCVALUE, -0.37,-0.42,-0.56,-0.56,4.00E-002,0.48,0.60,0.48,4.00E-002,-0.56,-0.56,-0.42
-
-AirflowNetwork Model:Wind Pressure Coefficients, WFACADE\_WPCVALUE, -0.56,-0.56,-0.42,-0.37,-0.42,-0.56,-0.56,4.00E-002,0.48,0.60,0.48,4.00E-002
-
-#### Field:  &lt; AirflowNetwork Model: Wind Pressure Coefficients&gt;
-
-This field contains the constant “AirflowNetwork Model: Wind Pressure Coefficients� for each line.
-
-#### Field: Name
-
-This is the WindPressureCoefficientValues object name entered from the IDF.
-
-#### Field: Wind Pressure Coefficients \#1 to n
-
-These values are the wind pressure coefficient for the building façade. These wind pressure coefficient values correspond to the first through Nth wind directions reported above for &lt;AirflowNetwork Model:Wind Direction&gt;. If Wind Pressure Coefficient Type = INPUT in the AirflowNetwork:SimulationControl object, the wind pressure coefficients described here are the inputs specified in the AirflowNetwork:MultiZone:Wind Pressure Coefficient Values object,. If Wind Pressure Coefficient Type = SurfaceAverageCalculation in the AirflowNetwork:SimulationControl object, the wind pressure coefficients are calculated internally and also described here.
-
-### Zone Volume Capacitance Multiplier
-
-! &lt;Zone Volume Capacitance Multiplier&gt;, Sensible Heat Capacity Multiplier, Moisture Capacity Multiplier, Carbon Dioxide Capacity Multiplier, Generic Contaminant Capacity Multiplier
-
-Zone Volume Capacitance Multiplier,   1.000, 1.000, 1.000, 1.000
-
-This shows the zone volume capacitance multipliers selected by the IDF value or defaulted. The object for this item is ZoneCapacitanceMultiplier:ResearchSpecial.
-
-#### Field: Sensible Heat Capacity Multiplier
-
-Value used to alter the effective heat capacitance of the zone air volume.
-
-#### Field: Moisture Capacity Multiplier
-
-Value used to alter the effective moisture capacitance of the zone air volume.
-
-#### Field: Carbon Dioxide Capacity Multiplier
-
-Value used to alter the effective carbon dioxide capacitance of the zone air volume.
-
-#### Field: Generic Contaminant Capacity Multiplier
-
-Value used to alter the effective generic contaminant capacitance of the zone air volume.
-
-#### Surface Geometry
-
-! &lt;SurfaceGeometry&gt;,Starting Corner,Vertex Input Direction,Coordinate System,Daylight Reference Point Coordinate System,Rectangular (Simple) Surface Coordinate System
-
-Surface Geometry, UpperLeftCorner, Counterclockwise, RelativeCoordinateSystem, RelativeCoordinateSystem, RelativeToZoneOrigin
-
-This shows the expected order of the vertices for each surface. The object for this item is GlobalGeometryRules.
-
-#### Field: Starting Corner
-
-Value used to designate which corner the surface(s) start with.
-
-#### Field: Vertex Input Direction
-
-Value whether the coordinates for the surface are entered clockwise or counter-clockwise.
-
-#### Field: Coordinate System
-
-Value whether the coordinate system is World/Absolute or Relative.
-
-#### Field: Daylight Reference Point Coordinate System
-
-If daylighting is used, this describes the coordinate system for entering daylight reference points.
-
-#### Field: Rectangular (Simple) Surface Coordinate System
-
-For simple surfaces (Wall, Window, Door, and so forth) the coordinate system that is used to describe their starting point.
-
-### Program Control
-
-! &lt;Program Control Information:Threads/Parallel Sims&gt;, Threading Supported,Maximum Number of Threads, Env Set Threads (OMP\_NUM\_THREADS), EP Env Set Threads (EP\_OMP\_NUM\_THREADS). IDF Set Threads, Number of Threads Used (Interior Radiant Exchange), Number Nominal Surfaces, Number Parallel Sims
-
-Program Control:Threads/Parallel Sims, Yes,2, Not Set, Not Set, Not Set, 2, 60, N/A
-
-
-
-More examples:
-
-Program Control:Threads/Parallel Sims, Yes,2, Not Set, Not Set, Not Set, 1, 6, N/A
-
-Program Control:Threads/Parallel Sims, Yes,2, Not Set, Not Set, 1, 1, 46, N/A
-
-This describes the threading that may be active for the simulation. The ProgramControl object is used for this output. As described in that object, only the Interior Radiant Exchange calculation has been exposed to use threading, goal being to speed up calculations but may not always be the most beneficial.
-
-#### Field: Threading Supported
-
-The compile of the program has to support threading (OpenMP for now). If it is compiled thus, this field will be **Yes**.  Otherwise it will be **No**.
-
-#### Field: Maximum Number of Threads
-
-Regardless of whether the compile has supported threading, the system is queried for the number of threads possible – that number is entered in this field.
-
-#### Field: Env Set Threads (OMP\_NUM\_THREADS)
-
-The Environment Variable OMP\_NUM\_THREADS can be manually inserted to set the number of system threads to be used. This would be reported here if set.  If not set, **Not Set** will be shown. This is a system variable, but suggest that you use the following environment variable if you want to manually control the number of threads.
-
-#### Field: EP Env Set Threads (EP\_OMP\_NUM\_THREADS)
-
-The Environment Variable EP\_OMP\_NUM\_THREADS can be manually inserted to set the number of system threads to be used. This would be reported here if set.  If not set, **Not Set** will be shown.
-
-#### Field: IDF Set Threads
-
-If you use the ProgramControl object in your IDF, you can again manually control the number of threads to be used. This would be reported here if set.  If not set, **Not Set** will be shown.
-
-#### Field: Number of Threads Used (Interior Radiant Exchange)
-
-This is the number of threads that was actually used in the Interior Radiant Exchange routines (which calculates the interior surface temperatures).
-
-#### Field: Number Nominal Surfaces
-
-This is the number of “nominal� surfaces (based on surface objects) that a quick calculation from the program has found. If the number of surfaces is not greater than 30, then the number of threads to be used will be set by the program to 1.
-
-#### Field: Number Parallel Sims
-
-This is the number of windowed/parallel simulations being run simultaneously as set by EP-Launch or other scripts distributed with the EnergyPlus program. Third party distributions may also set this item.
-
-
-
-### Climate Group Outputs
-
-Climate related variables appear in two places for EnergyPlus outputs. Certain objects that are invariant throughout a simulation period have lines appear in the eplusout.eio file:
-
-! &lt;Environment:Weather Station&gt;,Wind Sensor Height Above Ground {m},Wind Speed Profile Exponent {},Wind Speed Profile Boundary Layer Thickness {m},Air Temperature Sensor Height Above Ground {m},Wind Speed Modifier Coefficient [Internal],Temperature Modifier Coefficient [Internal]
-
-Environment:Weather Station,10.000,0.140,270.000,1.500,1.586,9.750E-003
-
-! &lt;Environment:Site Atmospheric Variation&gt;,Wind Speed Profile Exponent {},Wind Speed Profile Boundary Layer Thickness {m},Air Temperature Gradient Coefficient {K/m}
-
-Environment:Site Atmospheric Variation,   0.220, 370.000, 0.006500
-
-! &lt;Location&gt;, Location Name, Latitude, Longitude, Time Zone Number, Elevation {m}
-
- Location, DENVER COLORADO,   39.75, -104.87,   -7.00,      1610.26
-
-
-
-In addition for each “environment� simulated, information about the environment is shown:
-
-! &lt;Environment&gt;,Environment Name,Environment Type, Start Date, End Date, Start DayOfWeek, Duration {\#days}, Source:Start DayOfWeek,  Use Daylight Savings, Use Holidays, Apply Weekend Holiday Rule
-
-! &lt;Environment:Special Days&gt;, Special Day Name, Special Day Type, Source, Start Date, Duration {\#days}
-
-! &lt;Environment:Daylight Saving&gt;, Daylight Saving Indicator, Source, Start Date, End Date
-
-! &lt;Environment:Design\_Day\_Misc&gt;,DayOfYear,ASHRAE A Coeff,ASHRAE B Coeff,ASHRAE C Coeff,Solar Constant-Annual Variation,Eq of Time {minutes}, Solar Declination Angle {deg}, Solar Model
-
-! &lt;Environment:WarmupDays&gt;, NumberofWarmupDays
-
-For example, a DesignDay:
-
-Environment,PHOENIX ARIZONA WINTER,DesignDay, 1/21, 1/21,MONDAY,  1,N/A,N/A,N/A,N/A
-
-Environment:Daylight Saving,No,DesignDay
-
-Environment:Design\_Day\_Misc, 21,1228.9,0.1414,5.7310E-002,1.0,-11.14,-20.0
-
-A Design RunPeriod:
-
-Environment,EXTREME SUMMER WEATHER PERIOD FOR DESIGN,User Selected WeatherFile Typical/Extreme Period (Design)=Summer Extreme,07/13,07/19,SummerDesignDay,  7,Use RunPeriod Specified Day,No ,No ,No ,No ,No
-
-Environment:Daylight Saving,No,RunPeriod Object
-
-Environment:WarmupDays,  3
-
-Or a RunPeriod (Name listed in the RunPeriod output is dependent on user input for the RunPeriod object – when a blank is input, the name of the weather file location is used):
-
-Environment,CHICAGO IL TMY2-94846 WMO\#=725300,WeatherRunPeriod, 1/ 1,12/31,SUNDAY,365,UseWeatherFile,Yes,Yes,No
-
-Environment:Daylight Saving,No,
-
-Environment:Special Days,NEW YEARS DAY,Holiday,WeatherFile, 1/ 1,  1
-
-Environment:Special Days,MEMORIAL DAY,Holiday,WeatherFile, 5/31,  1
-
-Environment:Special Days,INDEPENDENCE DAY,Holiday,WeatherFile, 7/ 5,  1
-
-Environment:Special Days,LABOR DAY,Holiday,WeatherFile, 9/ 6,  1
-
-Environment:Special Days,THANKSGIVING,Holiday,WeatherFile,11/25,  1
-
-Environment:Special Days,CHRISTMAS,Holiday,WeatherFile,12/25,  1
-
-Environment:WarmupDays,  4
-
-Note that in this display, using “weekend rule� and specific date holidays, the actual observed dates are shown in the output display – in the example above, Independence Day (July 4) is actually observed on July 5.
-
-### Climate Group – Simple Outputs
-
-Some of the climate outputs are a “simple� group. The “header� line is followed immediately by the data line.
-
-### Location
-
-This output represents the location data used for the simulation. Note that if a runperiod is used, the IDF “Location� is ignored and the location from the weather file is used instead.
-
-#### Field: &lt;Location&gt;
-
-This data field will contain the constant “Location�.
-
-#### Field: Location Name
-
-This is the name given to the location whether from the IDF or the weather file.
-
-#### Field: Latitude
-
-This is the latitude of the site, expressed decimally. Convention uses positive (+) values for North of the Equator and negative (-) values for South of the Equator. For example, S 30° 15’ is expressed as –30.25.
-
-#### Field: Longitude
-
-This is the longitude of the site, expressed decimally. Convention uses positive (+) values for East of the Greenwich meridian and negative (-) values for West of the Greenwich meridian. For example, E 130° 45’ is expressed as +130.75.
-
-#### Field: Time Zone Number
-
-This is the time zone of the site, expressed decimally. Convention uses positive (+) values for GMT+ (Longitude East of the Greenwich meridian) and negative (-) values for GMT- (Longitude West of the Greenwich meridian). For example, the time zone for Central US time is –6. The time zone for parts of Newfoundland is –3.5 (-3 hours, 30 minutes from GMT).
-
-#### Field: Elevation {m}
-
-This is the elevation of the site. Units are m.
-
-### Weather Station
-
-#### Field: Wind Sensor Height Above Ground {m}
-
-This is the wind sensor height above ground for weather data measurements.
-
-#### Field: Wind Speed Profile Exponent {}
-
-The wind speed profile exponent for the terrain surrounding the weather station.
-
-#### Field: Wind Speed Profile Boundary Layer Thickness {m}
-
-The wind speed profile boundary layer thickness [m] for the terrain surrounding the weather station.
-
-#### Field: Air Temperature Sensor Height Above Ground {m}
-
-The height [m] above ground for the air temperature sensor.
-
-#### Field: Wind Speed Modifier Coefficient [Internal]
-
-This field is intended to provide a slight help for the user to determine the calculations that will be used to calculate the Wind Speed at a specific height at the site.
-
-The full calculation for Local Wind Speed is:
-
-<div>\[ \text{LocalWindSpeed} = \text{WindSpeed}_{met} \left( \frac{\text{WindBoundaryLayerThickness}_{met}}{\text{AirSensorHeight}_{met}} \right)^{\text{WindExponent}_{met}} \left(\frac{\text{HeightAboveGround}_{site/component}}{\text{WindBoundaryLayerThickness}_{site}}\right)^{\text{SiteWindExponent}}  \]</div>
-
-The Wind Speed Modifier Coefficient [Internal] simplifies the equation to:
-
-<div>\[ \text{LocalWindSpeed} = \text{WindSpeed}_{met} \left( \text{WindSpeedModifier} \right) \left(\frac{\text{HeightAboveGround}_{site/component}}{\text{WindBoundaryLayerThickness}_{site}}\right)^{\text{SiteWindExponent}}  \]</div>
-
-Where the Wind Speed Modifier encapsulates:
-
-<div>\[ \text{WindSpeedModifier} = \left( \frac{\text{WindBoundaryLayerThickness}_{met}}{\text{AirSensorHeight}_{met}} \right)^{\text{WindExponent}_{met}} \]</div>
-
-Where
-
-* met = meteorological station
-* site = location of the building
-
-#### Field:Temperature Modifier Coefficient [Internal]
-
-This field is intended to provide a slight help for the user to determine the calculations that will be used to calculate the air (dry-bulb) or wet-bulb temperature at a specific height at the site.
-
-The site temperature modifier coefficient (TMC) is defined as:
-
-<div>\[ TMC = frac{ \text{AtmosphericTemperatureGradient} \cdot \text{EarthRadius} \cdot \text{TemperatureSensorHeight}_{met} }
-                  { \text{EarthRadius} + \text{TemperatureSensorHeight}_{met} } \]</div>
-
-Then, the temperature at a height above ground is calculated as:
-
-<div>\[ \text{ActualTemperature} = \text{Temperature}_{met} + TMC - 
-    frac{ \text{TemperatureGradient}_{site} * \text{EarthRadius} * \text{Height}_{site/component} }
-        { \text{EarthRadius} + \text{Height}_{site/component} } \]</div>
-
-Where
-
-* met = meteorological station
-* site = location of the building
-
-### Site Atmospheric Variation
-
-#### Field: Wind Speed Profile Exponent {}
-
-The wind speed profile exponent for the terrain surrounding the site.
-
-#### Field: Wind Speed Profile Boundary Layer Thickness {m}
-
-The wind speed profile boundary layer thickness [m] for the terrain surrounding the site.
-
-#### Field: Air Temperature Gradient Coefficient {K/m}
-
-The air temperature gradient coefficient [K/m] is a research option that allows the user to control the variation in outdoor air temperature as a function of height above ground. The real physical value is 0.0065 K/m.
-
-### Ground Temperatures and Ground Reflectances
-
-! &lt;Site:GroundTemperature:BuildingSurface&gt;, Months From Jan to Dec {Deg C}
-
- Site:GroundTemperature:BuildingSurface,  20.03,  20.03,  20.13,  20.30,  20.43,  20.52,  20.62,  20.77,  20.78,  20.55,  20.44,  20.20
-
-! &lt;Site:GroundTemperature:FCfactorMethod&gt;, Months From Jan to Dec {Deg C}
-
- Site:GroundTemperature:FCfactorMethod,  -1.89,  -3.06,  -0.99,   2.23,  10.68,  17.20,  21.60,  22.94,  20.66,  15.60,   8.83,   2.56
-
-! &lt;Site:GroundTemperature:Shallow&gt;, Months From Jan to Dec {Deg C}
-
- Site:GroundTemperature:Shallow,  13.00,  13.00,  13.00,  13.00,  13.00,  13.00,  13.00,  13.00,  13.00,  13.00,  13.00,  13.00
-
-! &lt;Site:GroundTemperature:Deep&gt;, Months From Jan to Dec {Deg C}
-
- Site:GroundTemperature:Deep,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00,  16.00
-
-! &lt;Site:GroundReflectance&gt;, Months From Jan to Dec {dimensionless}
-
- Site:GroundReflectance,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20
-
-! &lt;Site:GroundReflectance:SnowModifier&gt;, Normal, Daylighting {dimensionless}
-
- Site:GroundReflectance:SnowModifier,   1.000,   1.000
-
-! &lt;Site:GroundReflectance:Snow&gt;, Months From Jan to Dec {dimensionless}
-
- Site:GroundReflectance:Snow,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20
-
-! &lt;Site:GroundReflectance:Snow:Daylighting&gt;, Months From Jan to Dec {dimensionless}
-
- Site:GroundReflectance:Snow:Daylighting,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20,  0.20
-
-### Ground Temperatures
-
-#### Field: &lt;GroundTemperatures&gt;
-
-This data field will contain the constant “GroundTemperatures�.
-
-#### Field Set (1-12) – Monthly Ground Temperatures
-
-There will be a set of 12 numbers – the ground temperatures by month: January, February, March, April, May, June, July, August, September, October, November, December. Units are C.
-
-### Ground Reflectance
-
-#### Field: &lt;GroundReflectances&gt;
-
-This data field will contain the constant “GroundReflectances�.
-
-#### Field Set (1-12) – Monthly Ground Reflectances
-
-There will be a set of 12 numbers – the ground reflectances by month: January, February, March, April, May, June, July, August, September, October, November, December.
-
-### Snow Ground Reflectance Modifiers
-
-It is generally accepted that snow resident on the ground increases the basic ground reflectance. EnergyPlus allows the user control over the snow ground reflectance for both “normal ground reflected solar� calculations (see above) and snow ground reflected solar modified for daylighting. This is the display of the user entered or defaulted values.
-
-#### Field: &lt;Snow Ground Reflectance  Modifiers&gt;
-
-This data field will contain the constant “Snow Ground Reflectance Modifiers�.
-
-#### Field: Normal
-
-This field is the value between 0.0 and 1.0 which is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values).
-
-<div>\[ \text{GroundReflectance}_{used} = \text{GroundReflectance} \cdot \text{Modifier}_{snow} \]</div>
-
-#### Field: Daylighting
-
-This field is the value between 0.0 and 1.0 which is used to modified the basic monthly ground reflectance when snow is on the ground (from design day input or weather data values).
-
-<div>\[ \text{DaylightingGroundReflectance}_{used} = \text{GroundReflectance} \cdot \text{Modifier}_{snow} \]</div>
-
-### Snow Ground Reflectance
-
-This data is the result of using the Snow Ground Reflectance modifier and the basic Ground Reflectance value.
-
-#### Field: &lt;GroundReflectances&gt;
-
-This data field will contain the constant “Snow GroundReflectances�.
-
-#### Field Set (1-12) – Monthly Snow Ground Reflectances
-
-There will be a set of 12 numbers – the snow ground reflectances by month: January, February, March, April, May, June, July, August, September, October, November, December.
-
-### Snow Ground Reflectance for Daylighting
-
-This data is the result of using the Snow Ground Reflectance for Daylighting modifier and the basic Ground Reflectance value.
-
-#### Field: &lt; Snow GroundReflectances For Daylighting&gt;
-
-This data field will contain the constant “Snow GroundReflectances For Daylighting�.
-
-#### Field Set (1-12) – Monthly Snow Ground Reflectances for Daylighting
-
-There will be a set of 12 numbers – the ground reflectances by month: January, February, March, April, May, June, July, August, September, October, November, December.
-
-### Climate Group – Not so Simple Outputs
-
-For each “environment� simulated, a set of outputs is produced. The header group is only produced once. (The Design Day Misc header is produced only when there is a design day.)
-
-! &lt;Environment&gt;,Environment Name,Environment Type, Start Date, End Date, Start DayOfWeek, Duration {\#days}, Source:Start DayOfWeek,  Use Daylight Saving, Use Holidays, Apply Weekend Holiday Rule
-
-! &lt;Environment:Special Days&gt;, Special Day Name, Special Day Type, Source, Start Date, Duration {\#days}
-
-! &lt;Environment:Daylight Saving&gt;, Daylight Saving Indicator, Source, Start Date, End Date
-
-! &lt;Environment:Design\_Day\_Misc&gt;,DayOfYear,ASHRAE A Coeff,ASHRAE B Coeff,ASHRAE C Coeff,Solar Constant-Annual Variation,Eq of Time {minutes}, Solar Declination Angle {deg}
-
-! &lt;Environment:WarmupDays&gt;, NumberofWarmupDays
-
-### Environment Line
-
-Each “environment� (i.e. each design day, each run period) will have this line shown.
-
-#### Field: &lt;Environment&gt;
-
-This field will have the constant “Environment� in each data line.
-
-#### Field:Environment Name
-
-This field will have the “name� of the environment. For example, the design day name (“DENVER COLORADO SUMMER�) or the weather file location name (“BOULDER CO TMY2-94018 WMO\#=724699�).
-
-#### Field:Environment Type
-
-This will be “DesignDay� for design day simulations and “WeatherRunPeriod� for weather file run periods.
-
-#### Field: Start Date
-
-This will have the month/day that is the starting date for the simulation period. (7/21, for example).
-
-#### Field: End Date
-
-This will have the month/day that is the ending date for the simulation period. Note that Design Days are only one day and the end date will be the same as the start date.
-
-#### Field: Start DayOfWeek
-
-For weather periods, this will be the designated starting day of week. For design days, it will be the day type listed for the design day object (e.g. SummerDesignDay or Monday).
-
-#### Field: Duration {\#days}
-
-Number of days in the simulation period will be displayed in this field. Design days are only 1 day.
-
-#### Field: Source:Start DayOfWeek
-
-This field will list the “source� of the Start Day of Week listed earlier. This could be the RunPeriod command from the input file or the Weather File if the UseWeatherFile option was chosen in the RunPeriod command. For design days, this will be “N/A�.
-
-#### Field: Use Daylight Saving
-
-This field reflects the value of the Use Daylight Saving field of the RunPeriod object. For design days, this will be “N/A�.
-
-#### Field: Use Holidays
-
-This field reflects the value of the Use Holidays field of the RunPeriod object. For design days, this will be “N/A�.
-
-#### Field: Apply Weekend Holiday Rule
-
-For design days, this will show “N/A�. For weather periods, this will show “Yes� if the Apply Weekend Holiday Rule is in effect or “No� if it isn’t.
-
-### Design Day Misc Line
-
-This line is shown for each design day simulated. It is not shown for sizing runs that do not subsequently use the design day as a simulation period.
-
-#### Field: &lt;Design Day Misc&gt;
-
-This is a constant that will display “Environment:Design\_Day\_Misc�.
-
-#### Field:DayOfYear
-
-This is the Julian day of year for the design day (i.e. Jan 1 is 1, Jan 31 is 31).
-
-#### Field:ASHRAE A Coeff
-
-Reference ASHRAE HOF 30 – this is the A Coefficient in Wh/m<sup>2</sup> calculated from EnergyPlus.
-
-#### Field:ASHRAE B Coeff
-
-Likewise, this is the ASHRAE B Coefficient (dimensionless).
-
-#### Field:ASHRAE C Coeff
-
-This is the ASHRAE C Coefficient (dimensionless).
-
-#### Field:Solar Constant-Annual Variation
-
-This is the calculated solar constant using the given location and day of year.
-
-#### Field:Eq of Time {minutes}
-
-This is the calculated equation of time (minutes) using the given location and day of year.
-
-#### Field: Solar Declination Angle {deg}
-
-This is the solar declination angle for the day of year, degrees.
-
-### Special Day Line
-
-#### Field: &lt;Environment:Special Days&gt;
-
-This is a constant that will display “Environment:SpecialDays�.
-
-#### Field: Special Day Name
-
-This is the user designated name for the special day.
-
-#### Field: Special Day Type
-
-This shows the type for the special day (e.g. Holiday).
-
-#### Field: Source
-
-This will display “InputFile� if it was specified in the IDF or “WeatherFile� if it came from the weather file designation.
-
-#### Field: Start Date
-
-This shows the starting date as month/day (e.g. 7/4).
-
-#### Field: Duration {\#days}
-
-This shows how many days the special day period continues. Usually, holidays are only 1 day duration.
-
-### Daylight Saving Line
-
-#### Field: &lt;Environment:Daylight Saving&gt;
-
-This is a constant that will display “Environment:DaylightSaving�.
-
-#### Field: Daylight Saving Indicator
-
-This will be Yes if daylight saving is to be observed for this simulation period and No if it is not observed.
-
-#### Field: Source
-
-This will show the source of this invocation (or non-invocation). Inputfile if DaylightSavingPeriod was entered (weather files only), WeatherFile if used in the Weather file and selected in the Run Period object and designday if that was the source.
-
-#### Field: Start Date
-
-If the indicator field is Yes, then this field will be displayed and the month/day (e.g. 4/1) that starts the daylight saving period observance will be shown.
-
-#### Field: End Date
-
-If the indicator field is Yes, then this field will be displayed and the month/day (e.g. 10/29) that ends the daylight saving period observance will be shown.
-
-### Zone Outputs
-
-### Zone Summary
-
-An overall zone summary is shown:
-
-! &lt;Zone Summary&gt;, Number of Zones, Number of Surfaces, Number of SubSurfaces
-
- Zone Summary,19,158,12
-
-As indicated:
-
-#### Field: &lt;Zone Summary&gt;
-
-This field contains the constant “Zone Summary�.
-
-#### Field: Number of Zones
-
-This field will contain the number of zones in the simulation.
-
-#### Field: Number of Surfaces
-
-This field will contain the total number of surfaces in the simulation.
-
-#### Field: Number of SubSurfaces
-
-This field will contain the total number of subsurfaces in the simulation.
-
-### Zone Information
-
-Each zone is summarized in a simple set of statements as shown below:
-
-! &lt;Zone Information&gt;,Zone Name,North Axis {deg},Origin X-Coordinate {m},Origin Y-Coordinate {m},Origin Z-Coordinate {m},Centroid X-Coordinate {m},Centroid Y-Coordinate {m},Centroid Z-Coordinate {m},Type,Zone Multiplier,Zone List Multiplier,Minimum X {m},Maximum X {m},Minimum Y {m},Maximum Y {m},Minimum Z {m},Maximum Z {m},Ceiling Height {m},Volume {m3},Zone Inside Convection Algorithm {Simple-Detailed-CeilingDiffuser-TrombeWall},Zone Outside Convection Algorithm {Simple-Detailed-Tarp-MoWitt-DOE-2-BLAST}, Floor Area {m2},Exterior Gross Wall Area {m2},Exterior Net Wall Area {m2},Exterior Window Area {m2}, Number of Surfaces, Number of SubSurfaces, Number of Shading SubSurfaces,  Part of Total Building Area
-
- Zone Information, PSI FOYER,0.0,0.00,0.00,0.00,8.56,-1.80,2.27,1,1,1,0.00,16.34,-9.51,4.88,0.00,6.10,3.81,368.12,Detailed,DOE-2,96.62,70.61,70.61,106.84,6,1,0,Yes
-
- Zone Information, DORM ROOMS AND COMMON AREAS,0.0,0.00,6.10,0.00,18.35,11.26,3.05,1,1,1,3.57,31.70,-4.75,25.36,0.00,6.10,6.10,2723.33,Detailed,DOE-2,445.93,312.15,267.56,52.59,10,22,0,Yes
-
- Zone Information, LEFT FORK,-36.9,0.00,31.70,0.00,22.07,31.46,3.05,1,1,1,19.02,25.12,25.36,37.55,0.00,6.10,6.10,453.07,Detailed,DOE-2,74.32,185.81,135.64,50.17,6,10,0,Yes
-
- Zone Information, MIDDLE FORK,0.0,4.88,35.36,0.00,31.21,28.41,3.05,1,1,1,25.12,37.31,21.70,35.11,0.00,6.10,6.10,453.07,Detailed,DOE-2,74.32,185.81,155.71,30.10,6,1,0,Yes
-
- Zone Information, RIGHT FORK,36.9,10.97,35.36,0.00,36.70,20.48,3.05,1,1,1,29.99,43.40,15.85,25.12,0.00,6.10,6.10,453.07,Detailed,DOE-2,74.32,185.81,135.64,50.17,6,10,0,Yes
-
-#### Field:  &lt;Zone Information&gt;
-
-This field contains the constant “Zone Information� for each line.
-
-#### Field: Zone Name
-
-This is the Zone Name entered from the IDF.
-
-#### Field: North Axis {deg}
-
-This is the North Axis entered from the IDF. Note that this is used primarily in the positioning of the building when “relative� coordinates are used – however, the Daylighting:Detailed object also uses this. Units are degrees, clockwise from North.
-
-#### Fields: X Origin {m}, Y Origin {m}, Z Origin {m}
-
-This is the origin vertex {X,Y,Z} entered from the IDF. Note that this is used primarily in the positioning of the building when “relative� coordinates are used – however, the Daylighting:Detailed object also uses this. Units are m.
-
-#### Field: TypeField: Multiplier
-
-This is the multiplier (must be integral) entered from the IDF.
-
-#### Field: Ceiling Height {m}
-
-This is the ceiling height entered, if any, in the IDF. Ceiling height is also heuristically calculated from the surfaces in the zone – however, not all surfaces need to be entered and sometimes the user would rather enter the ceiling height for the zone. If no ceiling height was entered (i.e. the default of 0), this field will be the calculated value. A minor warning message will be issued if the calculated value is significantly different than the entered value. Units are m.
-
-#### Field: Volume {m3}
-
-Like the ceiling height, this user can also enter this value in the IDF. Volume is also heuristically calculated using the ceiling height (entered or calculated) as well as the calculated floor area (see later field). If entered here, this value will be used rather than the calculated value. A minor warning message will be issued if the calculated value is significantly different than the entered value. Units are m<sup>3</sup>.
-
-#### Field: Zone Inside Convection Algorithm {Simple-Detailed-CeilingDiffuser-TrombeWall}
-
-The interior convection algorithm shown earlier (entire building) can be overridden for each zone by an entry in the individual Zone object. This field will show which method is operational for the zone.
-
-#### Field:  Floor Area {m2}
-
-This field is calculated from the floor surfaces entered for the zone. Units are m<sup>2</sup>.
-
-#### Field: Exterior Gross Wall Area {m2}
-
-This field is calculated from the exterior wall surfaces entered for the zone. Units are m<sup>2</sup>.
-
-#### Field: Exterior Net Wall Area {m2}
-
-This field is calculated from the exterior wall surfaces entered for the zone. Any sub-surface area is subtracted from the gross area to determine the net area. Units are m<sup>2</sup>.
-
-#### Field: Exterior Window Area {m2}
-
-This field is calculated from the exterior window surfaces entered for the zone. Units are m<sup>2</sup>.
-
-#### Field: Number of Surfaces
-
-This field is a count of the number of base surfaces in the zone.
-
-#### Field: Number of SubSurfaces
-
-This field is a count of the number of subsurfaces (windows, doors, glass doors and the list) in the zone.
-
-#### Field: Number of Shading SubSurfaces
-
-This field is a count of the number of shading surfaces (overhangs, fins) for the zone.
-
-#### Field: Part of Total Building Area
-
-This field displays “Yes� when the zone is to be considered part of the total building floor area or “No� when it’s not to be considered. This consideration has no impact on simulation but on reporting. Namely, when the value is “no�, the zone is not part of the Total Floor Area as shown in the Annual Building Utility Performance Summary tables. In addition, when “No� is specified, the area is excluded from both the conditioned floor area and the total floor area in the Building Area sub table and the Normalized Metrics sub tables.
-
-### Internal Gains Outputs
-
-### Zone Internal Gains
-
-Nominal Zone Internal Gains (people, lights, electric equipment, etc.) are summarized:
-
-! &lt;Zone Internal Gains/Equipment Information - Nominal&gt;,Zone Name, Floor Area {m2},\# Occupants,Area per Occupant {m2/person},Occupant per Area {person/m2},Interior Lighting {W/m2},Electric Load {W/m2},Gas Load {W/m2},Other Load {W/m2},Hot Water Eq {W/m2},Steam Equipment {W/m2},Sum Loads per Area {W/m2},Outdoor Controlled Baseboard Heat
-
- Zone Internal Gains, PLENUM-1,463.60,0.0,N/A,0.000,0.000,0.000,0.000,0.000,0.000,0.000,0.000,No
-
- Zone Internal Gains, SPACE1-1,99.16,11.0,9.015,0.111,15.974,10.649,0.000,0.000,0.000,0.000,26.624,No
-
- Zone Internal Gains, SPACE2-1,42.74,5.0,8.547,0.117,16.006,10.670,0.000,0.000,0.000,0.000,26.676,No
-
- Zone Internal Gains, SPACE3-1,96.48,11.0,8.771,0.114,16.418,10.945,0.000,0.000,0.000,0.000,27.363,No
-
- Zone Internal Gains, SPACE4-1,42.74,5.0,8.547,0.117,16.006,10.670,0.000,0.000,0.000,0.000,26.676,No
-
- Zone Internal Gains, SPACE5-1,182.49,20.0,9.125,0.110,16.242,10.828,0.000,0.000,0.000,0.000,27.070,No
-
-#### Field:  &lt;Zone Internal Gains/Equipment Information - Nominal&gt;
-
-This field contains the constant “Zone Internal Gains� for each line.
-
-#### Field: Zone Name
-
-This is the Zone Name entered from the IDF.
-
-#### Field: Floor Area {m2}
-
-This is the floor area for the zone.
-
-#### Field: \# Occupants
-
-This is the nominal number of occupants (from the PEOPLE statements).
-
-#### Field: Area per Occupant {m2/person}
-
-This is the Zone Floor Area per occupant (person).
-
-#### Field: Occupant per Area {person/m2}
-
-This is the number of occupants per area.
-
-#### Field: Interior Lighting {W/m2}
-
-This is the lighting (Lights) per floor area.
-
-#### Field: Electric Load {W/m2}
-
-This is the electric equipment load (**Electric Equipment**) per floor area.
-
-#### Field: Gas Load {W/m2}
-
-This is the gas equipment load (**Gas Equipment**) per floor area.
-
-#### Field: Other Load {W/m2
-
-This is the other equipment load (**Other Equipment**) per floor area.
-
-#### Field: Hot Water Eq {W/m2}
-
-This is the hot water equipment load (**Hot Water Equipment**) per floor area.
-
-#### Field: Steam Equipment {W/m2}
-
-This is the steam equipment load (**Steam Equipment**) per floor area.
-
-#### Field: Sum Loads per Area {W/m2}
-
-This is the nominal sum of loads per area (equipment). This metric can be useful for incorrect (too much) loads in a zone.
-
-#### Field: Outdoor Controlled Baseboard Heat
-
-This field is “yes� if there is outdoor controlled baseboard heat in a Zone.
-
-### People Gains
-
-! &lt;People Internal Gains - Nominal&gt;,Name,Schedule Name,Zone Name,Zone Floor Area {m2},\# Zone Occupants,Number of People {},People/Floor Area {person/m2},Floor Area per person {m2/person},Fraction Radiant,Fraction Convected,Sensible Fraction Calculation,Activity level,ASHRAE 55 Warnings,Carbon Dioxide Generation Rate,Nominal Minimum Number of People,Nominal Maximum Number of People
-
-People Internal Gains,  SPACE1-1 PEOPLE 1, OCCUPY-1, SPACE1-1, 99.16, 11.0, 11.0, 0.111, 9.015, 0.300, 0.700, AutoCalculate, ACTSCHD, No, 3.8200E-008, 0, 11
-
- People Internal Gains,  SPACE2-1 PEOPLE 1, OCCUPY-1, SPACE2-1, 42.74, 5.0, 5.0, 0.117, 8.547, 0.300, 0.700, AutoCalculate, ACTSCHD, No, 3.8200E-008, 0, 5
-
- People Internal Gains,  SPACE3-1 PEOPLE 1, OCCUPY-1, SPACE3-1, 96.48, 11.0, 11.0, 0.114, 8.771, 0.300, 0.700, AutoCalculate, ACTSCHD, No, 3.8200E-008, 0, 11
-
- People Internal Gains,  SPACE4-1 PEOPLE 1, OCCUPY-1, SPACE4-1, 42.74, 5.0, 5.0, 0.117, 8.547, 0.300, 0.700, AutoCalculate, ACTSCHD, No, 3.8200E-008, 0, 5
-
- People Internal Gains,  SPACE5-1 PEOPLE 1, OCCUPY-1, SPACE5-1, 182.49, 20.0, 20.0, 0.110, 9.125, 0.300, 0.700, AutoCalculate, ACTSCHD, No, 3.8200E-008, 0, 20
-
-#### Field: &lt;People Internal Gains - Nominal&gt;
-
-This field contains the constant “People Internal Gains� for each line.
-
-#### Field: Name
-
-This field contains the name of the People statement from the IDF file.
-
-#### Field: Schedule Name
-
-This is the schedule of occupancy fraction – the fraction is applied to the number of occupants for the statement. Limits are [0,1].
-
-#### Field: Zone Name
-
-This is the name of the Zone for the people/occupants.
-
-#### Field: Zone Floor Area {m2}
-
-This is the floor area (m2) of the zone.
-
-#### Field: \# Zone Occupants
-
-This is the total number of occupants for the zone.
-
-#### Field: Number of People {}
-
-This is the specific number of people for this statement (nominal).
-
-#### Field: People/Floor Area {person/m2}
-
-This value represents the number of people density (this statement) per area (zone floor area).
-
-#### Field: Floor Area per person {m2/person}
-
-This is the floor area per person (this statement)
-
-#### Field: Fraction Radiant
-
-This is the fraction radiant for each person (this statement).
-
-#### Field: Fraction Convected
-
-This is the fraction convected for each person (this statement).
-
-#### Field: Sensible Fraction Calculation
-
-This field will show “Autocalculate� if the default calculation for sensible fraction of load is to be used. Or a specific value can be entered. If so, that value will be displayed.
-
-#### Field: Activity level
-
-This field will show the activity level schedule name.
-
-#### Field: ASHRAE 55 Warnings
-
-If this field shows “yes�, then ASHRAE 55 comfort warnings are enabled. If “no�, then no ASHRAE 55 comfort warnings are calculated or issued.
-
-**The following fields are shown only when one of the Comfort calculations (Fanger, KSU, Pierce) is used.**
-
-#### Field: MRT Calculation Type
-
-This field’s value will be one of the valid MRT calculation types (Zone Averaged, Surface Weighted, Angle Factor).
-
-#### Field: Work Efficiency
-
-This field will be the work efficiency schedule name for this people statement.
-
-#### Field: Clothing
-
-This field will be the clothing schedule name for this people statement.
-
-#### Field: Air Velocity
-
-This field will be the air velocity schedule name for this people statement.
-
-#### Field: Fanger Calculation
-
-This field will be “yes� if Fanger calculations are enabled for this people statement; otherwise it will be “no�.
-
-#### Field: Pierce Calculation
-
-This field will be “yes� if Pierce calculations are enabled for this people statement; otherwise it will be “no�.
-
-#### Field: KSU Calculation
-
-This field will be “yes� if KSU calculations are enabled for this people statement; otherwise it will be “no�.
-
-#### Field: Carbon Dioxide Generation Rate
-
-This numeric input field specifies carbon dioxide generation rate per person with units of m3/s-W. The total carbon dioxide generation rate from this object is:
-
-Number of People \* People Schedule \* People Activity \* Carbon Dioxide Generation Rate. The default value is 3.82E-8 m3/s-W (obtained from ASHRAE Standard 62.1-2007 value at 0.0084 cfm/met/person over the general adult population). The maximum value can be 10 times the default value.
-
-#### Field: Nominal Minimum Number of People
-
-This numeric field is the calculated minimum number of people based on the number of people field \* the minimum value (annual) for the people schedule. It may be useful in diagnosing errors that occur during simulation.
-
-#### Field: Nominal Maximum Number of People
-
-This numeric field is the calculated maximum number of people based on the number of people field \* the maxnimum value (annual) for the people schedule. It may be useful in diagnosing errors that occur during simulation.
-
-
-
-### Lights Gains
-
-! &lt;Lights Internal Gains - Nominal&gt;, Name, Schedule Name, Zone Name, Zone Floor Area {m2}, \# Zone Occupants, Lighting Level {W}, Lights/Floor Area {W/m2}, Lights per person {W/person}, Fraction Return Air, Fraction Radiant, Fraction Short Wave, Fraction Convected, Fraction Replaceable, End-Use Category, Nominal Minimum Lighting Level {W}, Nominal Maximum Lighting Level {W}
-
-Lights Internal Gains,  SPACE1-1 LIGHTS 1, LIGHTS-1, SPACE1-1, 99.16, 11.0, 1584.000, 15.974, 144.000, 0.200, 0.590, 0.200, 1.000E-002, 0.000, GeneralLights, 79.200, 1584.000
-
- Lights Internal Gains,  SPACE2-1 LIGHTS 1, LIGHTS-1, SPACE2-1, 42.74, 5.0, 684.000, 16.006, 136.800, 0.200, 0.590, 0.200, 1.000E-002, 0.000, GeneralLights, 34.200, 684.000
-
- Lights Internal Gains,  SPACE3-1 LIGHTS 1, LIGHTS-1, SPACE3-1, 96.48, 11.0, 1584.000, 16.418, 144.000, 0.200, 0.590, 0.200, 1.000E-002, 0.000, GeneralLights, 79.200, 1584.000
-
- Lights Internal Gains,  SPACE4-1 LIGHTS 1, LIGHTS-1, SPACE4-1, 42.74, 5.0, 684.000, 16.006, 136.800, 0.200, 0.590, 0.200, 1.000E-002, 0.000, GeneralLights, 34.200, 684.000
-
- Lights Internal Gains,  SPACE5-1 LIGHTS 1, LIGHTS-1, SPACE5-1, 182.49, 20.0, 2964.000, 16.242, 148.200, 0.200, 0.590, 0.200, 1.000E-002, 0.000, GeneralLights, 148.200, 2964.000
-
-#### Field: &lt;Lights Internal Gains - Nominal&gt;
-
-This field contains the constant “Lights Internal Gains� for each line.
-
-#### Field: Name
-
-This field contains the name of the Lights statement from the IDF file.
-
-#### Field: Schedule Name
-
-This is the schedule of lights fraction – the fraction is applied to the nominal lighting level for the statement. Limits are [0,1].
-
-#### Field: Zone Name
-
-This is the name of the Zone for the lights.
-
-#### Field: Zone Floor Area {m2}
-
-This is the floor area (m2) of the zone.
-
-#### Field: \# Zone Occupants
-
-This is the total number of occupants for the zone.
-
-#### Field: Lighting Level {W}
-
-This is the nominal lighting level (this statement) in Watts.
-
-#### Field: Lights/Floor Area {W/m2}
-
-This is the watts per floor area (this statement)
-
-#### Field: Lights per person {W/person}
-
-This is the watts per person that this statement represents.
-
-#### Field: Fraction Return Air
-
-This is the fraction return air for this statement.
-
-#### Field: Fraction Radiant
-
-This is the fraction radiant for this lighting level.
-
-#### Field: Fraction Short Wave
-
-This is the fraction short wave for this lighting level.
-
-#### Field: Fraction Convected
-
-This is the fraction convected for this lighting level.
-
-#### Field: Fraction Replaceable
-
-This is the fraction replaceable for this lighting level. For daylighting calculations, this value should either be 0 (no dimming control) or 1 (full dimming control).
-
-#### Field: End-Use Category
-
-This field shows the end-use category for this lights statement. Usage can be reported by end-use category.
-
-#### Field: Nominal Minimum Lighting Level {W}
-
-This numeric field is the calculated minimum amount of lighting in Watts based on the calculated lighting level (above) \* the minimum value (annual) for the lights schedule. It may be useful in diagnosing errors that occur during simulation.
-
-#### Field: Nominal Maximum Lighting Level {W}
-
-This numeric field is the calculated maximum amount of lighting in Watts based on the calculated lighting level (above) \* the maximum value (annual) for the lights schedule. It may be useful in diagnosing errors that occur during simulation.
-
-### Equipment (Electric, Gas, Steam, Hot Water) Gains
-
-These equipments are all reported similarly. Electric Equipment is used in the example below:
-
-! &lt;ElectricEquipment Internal Gains - Nominal&gt;, Name, Schedule Name, Zone Name, Zone Floor Area {m2}, \# Zone Occupants, Equipment Level {W}, Equipment/Floor Area {W/m2}, Equipment per person {W/person}, Fraction Latent, Fraction Radiant, Fraction Lost, Fraction Convected, End-Use SubCategory, Nominal Minimum Equipment Level {W}, Nominal Maximum Equipment Level {W}
-
-ElectricEquipment Internal Gains,  SPACE1-1 ELECEQ 1, EQUIP-1, SPACE1-1, 99.16, 11.0, 1056.000, 10.649, 96.000, 0.000, 0.300, 0.000, 0.700, General, 21.120, 950.400
-
- ElectricEquipment Internal Gains,  SPACE2-1 ELECEQ 1, EQUIP-1, SPACE2-1, 42.74, 5.0, 456.000, 10.670, 91.200, 0.000, 0.300, 0.000, 0.700, General, 9.120, 410.400
-
- ElectricEquipment Internal Gains,  SPACE3-1 ELECEQ 1, EQUIP-1, SPACE3-1, 96.48, 11.0, 1056.000, 10.945, 96.000, 0.000, 0.300, 0.000, 0.700, General, 21.120, 950.400
-
- ElectricEquipment Internal Gains,  SPACE4-1 ELECEQ 1, EQUIP-1, SPACE4-1, 42.74, 5.0, 456.000, 10.670, 91.200, 0.000, 0.300, 0.000, 0.700, General, 9.120, 410.400
-
- ElectricEquipment Internal Gains,  SPACE5-1 ELECEQ 1, EQUIP-1, SPACE5-1, 182.49, 20.0, 1976.000, 10.828, 98.800, 0.000, 0.300, 0.000, 0.700, General, 39.520, 1778.400
-
-#### Field: &lt;[Specific] Equipment Internal Gains - Nominal&gt;
-
-This field will contain the type of equipment internal gain in each line (i.e. Electric Equipment Internal Gains, Gas Equipment Internal Gains, …).
-
-#### Field: Name
-
-This field contains the name of the equipment statement from the IDF file.
-
-#### Field: Schedule Name
-
-This is the schedule of equipment fraction – the fraction is applied to the nominal equipment level for the statement. Limits are [0,1].
-
-#### Field: Zone Name
-
-This is the name of the Zone for the equipment.
-
-#### Field: Zone Floor Area {m2}
-
-This is the floor area (m2) of the zone.
-
-#### Field: \# Zone Occupants
-
-This is the total number of occupants for the zone.
-
-#### Field: Equipment Level {W}
-
-This is the nominal equipment level (in Watts) for the statement.
-
-#### Field: Equipment/Floor Area {W/m2}
-
-This is the watts per floor area (this statement)
-
-#### Field: Equipment per person {W/person}
-
-This is the watts per person that this statement represents.
-
-#### Field: Fraction Latent
-
-This is the fraction latent for this equipment.
-
-#### Field: Fraction Radiant
-
-This is the fraction radiant for this equipment.
-
-#### Field: Fraction Lost
-
-This is the fraction lost (not attributed to the zone) for this equipment.
-
-#### Field: Fraction Convected
-
-This is the fraction convected for this equipment.
-
-#### Field: End-Use SubCategory
-
-This field shows the end-use category for this statement. Usage can be reported by end-use category.
-
-#### Field: Nominal Minimum Equipment Level {W}
-
-This numeric field is the calculated minimum amount of the equipment in Watts based on the calculated design level (above) \* the minimum value (annual) for the equipment schedule. It may be useful in diagnosing errors that occur during simulation.
-
-#### Field: Nominal Maximum Equipment Level {W}
-
-This numeric field is the calculated maximum amount of the equipment in Watts based on the calculated design level (above) \* the maximum value (annual) for the equipment schedule. It may be useful in diagnosing errors that occur during simulation.
-
-### Other Equipment Gains
-
-Other equipment report is shown below (does not have an end-use category – is not attached to any normal meter):
-
-! &lt;OtherEquipment Internal Gains - Nominal&gt;, Name, Schedule Name, Zone Name, Zone Floor Area {m2}, \# Zone Occupants, Equipment Level {W}, Equipment/Floor Area {W/m2}, Equipment per person {W/person}, Fraction Latent, Fraction Radiant, Fraction Lost, Fraction Convected, Nominal Minimum Equipment Level {W}, Nominal Maximum Equipment Level {W}
-
-OtherEquipment Internal Gains,  TEST 352A, ALWAYSON, ZONE ONE, 232.26, 0.0, 352.000, 1.516, N/A, 0.000, 0.000, 0.000, 1.000, 352.000, 352.000
-
- OtherEquipment Internal Gains,  TEST 352 MINUS, ALWAYSON, ZONE ONE, 232.26, 0.0, -352.000, -1.516, N/A, 0.000, 0.000, 0.000, 1.000, -352.000, -352.000
-
-#### Field: &lt;Other Equipment Internal Gains - Nominal&gt;
-
-This field contains the constant “OtherEquipment Internal Gains� for each line.
-
-#### Field: Name
-
-This field contains the name of the equipment statement from the IDF file.
-
-#### Field: Schedule Name
-
-This is the schedule of equipment fraction – the fraction is applied to the nominal equipment level for the statement. Limits are [0,1].
-
-#### Field: Zone Name
-
-This is the name of the Zone for the equipment.
-
-#### Field: Zone Floor Area {m2}
-
-This is the floor area (m2) of the zone.
-
-#### Field: \# Zone Occupants
-
-This is the total number of occupants for the zone.
-
-#### Field: Equipment Level {W}
-
-This is the nominal equipment level (in Watts) for the statement.
-
-#### Field: Equipment/Floor Area {W/m2}
-
-This is the watts per floor area (this statement)
-
-#### Field: Equipment per person {W/person}
-
-This is the watts per person that this statement represents.
-
-#### Field: Fraction Latent
-
-This is the fraction latent for this equipment.
-
-#### Field: Fraction Radiant
-
-This is the fraction radiant for this equipment.
-
-#### Field: Fraction Lost
-
-This is the fraction lost (not attributed to the zone) for this equipment.
-
-#### Field: Fraction Convected
-
-This is the fraction convected for this equipment.
-
-#### Field: Nominal Minimum Equipment Level {W}
-
-This numeric field is the calculated minimum amount of the equipment in Watts based on the calculated design level (above) \* the minimum value (annual) for the equipment schedule. It may be useful in diagnosing errors that occur during simulation.
-
-#### Field: Nominal Maximum Equipment Level {W}
-
-This numeric field is the calculated maximum amount of the equipment in Watts based on the calculated design level (above) \* the maximum value (annual) for the equipment schedule. It may be useful in diagnosing errors that occur during simulation.
-
-### Outdoor Controlled Baseboard Heat
-
-! &lt;Outdoor Controlled Baseboard Heat Internal Gains - Nominal&gt;,Name,Schedule Name,Zone Name,Zone Floor Area {m2},\# Zone Occupants,Capacity at Low Temperature {W},Low Temperature {C},Capacity at High Temperature {W},High Temperature {C},Fraction Radiant,Fraction Convected,End-Use Subcategory
-
- Outdoor Controlled Baseboard Heat Internal Gains, SPACE4-1 BBHEAT 1,EQUIP-1,SPACE4-1,42.74,5.0,1500.000,0.000,500.000,10.000,0.500,0.500,Baseboard Heat
-
-#### Field: &lt;Outdoor Controlled Baseboard Heat Internal Gains - Nominal&gt;
-
-This field contains the constant “Outdoor Controlled Baseboard Heat Internal Gains� for each line.
-
-#### Field: Name
-
-This field contains the name of the baseboard heat statement from the IDF file.
-
-#### Field: Schedule Name
-
-This is the schedule of equipment fraction – the fraction is applied to the nominal equipment level for the statement. Limits are [0,1].
-
-#### Field: Zone Name
-
-This is the name of the Zone for the equipment.
-
-#### Field: Zone Floor Area {m2}
-
-This is the floor area (m2) of the zone.
-
-#### Field: \# Zone Occupants
-
-This is the total number of occupants for the zone.
-
-#### Field: Capacity at Low Temperature {W}
-
-This is the capacity (in Watts) of the equipment at low outdoor temperature.
-
-#### Field: Low Temperature {C}
-
-This is the low outdoor temperature (dry-bulb) for the capacity in the previous field. If the outdoor dry-bulb temperature (degrees Celsius) is at or below the low temperature, thebaseboard heater operates at the low temperature capacity.
-
-#### Field: Capacity at High Temperature {W}
-
-This is the capacity (in Watts) of the equipment at high outdoor temperature.
-
-#### Field: High Temperature {C}
-
-This is the high outdoor temperature (dry-bulb) for the capacity in the previous field. If the outdoor dry-bulb temperature (degrees Celsius) is exceeds the high temperature, thebaseboard heater turns off.
-
-#### Field: Fraction Radiant
-
-This is the fraction radiant for this equipment.
-
-#### Field: Fraction Convected
-
-This is the fraction convected for this equipment.
-
-#### Field: EndUse Subcategory
-
-This field shows the enduse category for this statement. Usage can be reported by enduse category.
-
-### Simple Airflow Outputs
-
-### Infiltration, Ventilation, Mixing, Cross Mixing Statistics
-
-Infiltration, Ventilation, Mixing, Cross Mixing are only specified when the Airflow Model is “Simple� (no Airflow Network).
-
-### Infiltration
-
-! &lt;Infiltration Airflow Stats - Nominal&gt;,Name,Schedule Name,Zone Name, Zone Floor Area {m2}, \# Zone Occupants,Design Volume Flow Rate {m3/s},Volume Flow Rate/Floor Area {m3/s/m2},Volume Flow Rate/Exterior Surface Area {m3/s/m2},ACH - Air Changes per Hour,Equation A - Constant Term Coefficient {},Equation B - Temperature Term Coefficient {1/C},Equation C - Velocity Term Coefficient {s/m}, Equation D - Velocity Squared Term Coefficient {s2/m2}
-
-ZoneInfiltration Airflow Stats, SPACE1-1 INFIL 1,INFIL-SCH,SPACE1-1,99.16,11.0,3.200E-002,3.227E-004,4.372E-004,0.482,0.000,0.000,0.224,0.000
-
- ZoneInfiltration Airflow Stats, SPACE2-1 INFIL 1,INFIL-SCH,SPACE2-1,42.74,5.0,1.400E-002,3.276E-004,3.838E-004,0.488,0.000,0.000,0.224,0.000
-
- ZoneInfiltration Airflow Stats, SPACE3-1 INFIL 1,INFIL-SCH,SPACE3-1,96.48,11.0,3.200E-002,3.317E-004,4.372E-004,0.482,0.000,0.000,0.224,0.000
-
- ZoneInfiltration Airflow Stats, SPACE4-1 INFIL 1,INFIL-SCH,SPACE4-1,42.74,5.0,1.400E-002,3.276E-004,3.838E-004,0.488,0.000,0.000,0.224,0.000
-
- ZoneInfiltration Airflow Stats, SPACE5-1 INFIL 1,INFIL-SCH,SPACE5-1,182.49,20.0,6.200E-002,3.397E-004,N/A,0.499,0.000,0.000,0.224,0.000
-
-#### Field: &lt;Infiltration Airflow Stats - Nominal&gt;
-
-This field contains the constant “Infiltration Airflow Stats� for each line.
-
-#### Field: Name
-
-This field contains the name of the infiltration statement from the IDF file.
-
-#### Field: Schedule Name
-
-This is the schedule of use fraction – the fraction is applied to the nominal volume flow rate for the statement. Limits are [0,1].
-
-#### Field: Zone Name
-
-This is the name of the Zone for the infiltration.
-
-#### Field: Zone Floor Area {m2}
-
-This is the floor area (m2) of the zone.
-
-#### Field: \# Zone Occupants
-
-This is the total number of occupants for the zone.
-
-#### Field: Design Volume Flow Rate {m3/s}
-
-This is the nominal flow rate for the infiltration in m3/s.
-
-#### Field: Volume Flow Rate/Floor Area {m3/s/m2}
-
-This field is the volume flow rate density per floor area (flow rate per floor area) for infiltration.
-
-#### Field: Volume Flow Rate/Exterior Surface Area {m3/s/m2}
-
-This field is the volume flow rate density per exterior surface area (flow rate per exterior area) for infiltration.
-
-#### Field: ACH - Air Changes per Hour
-
-This field is the air changes per hour for the given infiltration rate.
-
-#### Field: Equation A - Constant Term Coefficient {}
-
-Actual infiltration amount is an equation based value:
-
-<div>\[ \text{Infiltration} = I_{design} F_{schedule} \left[ A + B \left| T_{zone}-T_{odb} \right| + C\left(\text{WindSpeed}\right) + D\left(\text{WindSpeed}^2\right)  \right] \]</div>
-
-This field value is the A coefficient in the above equation.
-
-#### Field: Equation B - Temperature Term Coefficient {1/C}
-
-This field value is the B coefficient in the above equation.
-
-#### Field: Equation C - Velocity Term Coefficient {s/m}
-
-This field value is the C coefficient in the above equation.
-
-#### Field:  Equation D - Velocity Squared Term Coefficient {s2/m2}
-
-This field value is the D coefficient in the above equation.
-
-### Ventilation
-
-! &lt;Ventilation Airflow Stats - Nominal&gt;,Name,Schedule Name,Zone Name, Zone Floor Area {m2}, \# Zone Occupants,Design Volume Flow Rate {m3/s},Volume Flow Rate/Floor Area {m3/s/m2},Volume Flow Rate/person Area {m3/s/person},ACH - Air Changes per Hour,Fan Type {Exhaust;Intake;Natural/None},Fan Pressure Rise {?},Fan Efficiency {},Equation A - Constant Term Coefficient {},Equation B - Temperature Term Coefficient {1/C},Equation C - Velocity Term Coefficient {s/m}, Equation D - Velocity Squared Term Coefficient {s2/m2},Minimum Indoor Temperature/Schedule,Maximum Indoor Temperature/Schedule,Delta Temperature/Schedule,Minimum Outdoor Temperature/Schedule,Maximum Outdoor Temperature/Schedule,Maximum WindSpeed
-
- Ventilation Airflow Stats, SPACE1-1 VENTL 1,NIGHTVENTSCHED,SPACE1-1,99.16,11.0,5.295E-002,5.340E-004,4.814E-003,0.797,Intake,67.000,0.7,1.000,0.000,0.000,0.000,MININDOORTEMP,MAXINDOORTEMP,DELTATEMP,MINOUTDOORTEMP,MAXOUTDOORTEMP,40.00
-
- Ventilation Airflow Stats, SPACE1-1 VENTL 2,NIGHTVENTSCHED,SPACE1-1,99.16,11.0,5.295E-002,5.340E-004,4.814E-003,0.797,Intake,67.000,0.7,1.000,0.000,0.000,0.000,MININDOORTEMP,MAXINDOORTEMP,DELTATEMP,MINOUTDOORTEMP,MAXOUTDOORTEMP,40.00
-
- Ventilation Airflow Stats, SPACE2-1 VENTL 1,NIGHTVENTSCHED,SPACE2-1,42.74,5.0,7.030E-002,1.645E-003,1.406E-002,2.450,Intake,67.000,0.7,1.000,0.000,0.000,0.000,18.00,100.00,2.00,-100.00,100.00,40.00
-
-Ventilation Airflow Stats, RESISTIVE ZONE VENTL 1,INF-SCHED,RESISTIVE ZONE,37.16,3.0,2.000E-002,5.382E-004,6.667E-003,0.636,Natural,0.000,1.0,0.606,2.020E-002,5.980E-004,0.000,18.00,100.00,1.00,-100.00,100.00,40.00
-
- Ventilation Airflow Stats, EAST ZONE VENTL 1,INF-SCHED,EAST ZONE,37.16,3.0,2.000E-002,5.382E-004,6.667E-003,0.636,Natural,0.000,1.0,0.606,2.020E-002,5.980E-004,0.000,18.00,100.00,1.00,-100.00,100.00,40.00
-
- Ventilation Airflow Stats, NORTH ZONE VENTL 1,INF-SCHED,NORTH ZONE,55.74,4.0,2.000E-002,3.588E-004,5.000E-003,0.424,Natural,0.000,1.0,0.606,2.020E-002,5.980E-004,0.000,18.00,100.00,1.00,-100.00,100.00,40.00
-
-#### Field: &lt;Ventilation Airflow Stats - Nominal&gt;
-
-This field contains the constant “Ventilation Airflow Stats� for each line.
-
-#### Field: Name
-
-This field contains the name of the ventilation statement from the IDF file.
-
-#### Field: Schedule Name
-
-This is the schedule of use fraction – the fraction is applied to the nominal volume flow rate for the statement. Limits are [0,1].
-
-#### Field: Zone Name
-
-This is the name of the Zone for the ventilation.
-
-#### Field: Zone Floor Area {m2}
-
-This is the floor area (m2) of the zone.
-
-#### Field: \# Zone Occupants
-
-This is the total number of occupants for the zone.
-
-#### Field: Design Volume Flow Rate {m3/s}
-
-This is the nominal flow rate for the ventilation in m3/s.
-
-#### Field: Volume Flow Rate/Floor Area {m3/s/m2}
-
-This field is the volume flow rate density per floor area (flow rate per floor area) for ventilation.
-
-#### Field: Volume Flow Rate/person Area {m3/s/person}
-
-This field is the volume flow rate density per person (flow rate per person) for ventilation.
-
-#### Field: ACH - Air Changes per Hour
-
-This field is the air changes per hour for the given ventilation rate.
-
-#### Field: Fan Type {Exhaust;Intake;Natural}
-
-This field shows the entered value for the type of ventilation [NATURAL, EXHAUST, or INTAKE]. Natural ventilation is the air movement/exchange a result of openings in the building façade and does not consume any fan energy. For either EXHAUST or INTAKE, values for fan pressure and efficiency define the fan electric consumption. For NATURAL and EXHAUST ventilation, the conditions of the air entering the space are assumed to be equivalent to outdoor air conditions. For INTAKE ventilation, an appropriate amount of fan heat is added to the air stream.
-
-#### Field: Fan Pressure Rise {Pa}
-
-Operational when Fan Type is INTAKE or EXHAUST, this is the pressure rise experienced across the fan in Pascals (N/m<sup>2</sup>). This is a function of the fan and plays a role in determining the amount of energy consumed by the fan.
-
-#### Field: Fan Efficiency {}
-
-Operational when Fan Type is INTAKE or EXHAUST, this is the total fan efficiency (a decimal number between 0.0 and 1.0). This is a function of the fan and plays a role in determining the amount of energy consumed by the fan.
-
-#### Field: Equation A - Constant Term Coefficient {}
-
-Actual ventilation amount is an equation based value:
-
-<div>\[ \text{Ventilation} = V_{design} F_{schedule} \left[ A + B \left| T_{zone}-T_{odb} \right| + C\left(\text{WindSpeed}\right) + D\left(\text{WindSpeed}^2\right)  \right] \]</div>
-
-This field value is the A coefficient in the above equation.
-
-#### Field: Equation B - Temperature Term Coefficient {1/C}
-
-This field value is the B coefficient in the above equation.
-
-#### Field: Equation C - Velocity Term Coefficient {s/m}
-
-This field value is the C coefficient in the above equation.
-
-#### Field:  Equation D - Velocity Squared Term Coefficient {s2/m2}
-
-This field value is the D coefficient in the above equation.
-
-#### Field: Minimum Indoor Temperature{C}/Schedule
-
-This is the indoor temperature (in Celsius) below which ventilation is shutoff. As the values can also be entered as a schedule, the schedule name may be listed here rather than a temperature.
-
-#### Field: Maximum Indoor Temperature{C}/Schedule
-
-This is the indoor temperature (in Celsius) above which ventilation is shutoff. As the values can also be entered as a schedule, the schedule name may be listed here rather than a temperature.
-
-#### Field: Delta Temperature{C}/Schedule
-
-This is the temperature difference (in Celsius) between the indoor and outdoor air dry-bulb temperatures below which ventilation is shutoff. As the values can also be entered as a schedule, the schedule name may be listed here rather than a temperature.
-
-#### Field: Minimum Outdoor Temperature{C}/Schedule
-
-This is the outdoor temperature (in Celsius) below which ventilation is shut off. As the values can also be entered as a schedule, the schedule name may be listed here rather than a temperature.
-
-#### Field: Maximum Outdoor Temperature{C}/Schedule
-
-This is the outdoor temperature (in Celsius) above which ventilation is shut off. As the values can also be entered as a schedule, the schedule name may be listed here rather than a temperature.
-
-#### Field: Maximum WindSpeed{m/s}
-
-This is the wind speed (m/s) above which ventilation is shut off.
-
-### Mixing
-
-! &lt;Mixing Airflow Stats - Nominal&gt;,Name,Schedule Name,Zone Name, Zone Floor Area {m2}, \# Zone Occupants,Design Volume Flow Rate {m3/s},Volume Flow Rate/Floor Area {m3/s/m2},Volume Flow Rate/person Area {m3/s/person},ACH - Air Changes per Hour,From/Source Zone,Delta Temperature {C}
-
- Mixing Airflow Stats, RESISTIVE ZONE MIXNG 1,ZONE MIXING,RESISTIVE ZONE,37.16,3.0,5.000E-002,1.345E-003,1.667E-002,1.589,EAST ZONE,0.00
-
-#### Field: &lt;Mixing Airflow Stats - Nominal&gt;
-
-This field contains the constant “Mixing Airflow Stats� for each line.
-
-#### Field: Name
-
-This field contains the name of the mixing statement from the IDF file.
-
-#### Field: Schedule Name
-
-This is the schedule of use fraction – the fraction is applied to the nominal volume flow rate for the statement. Limits are [0,1].
-
-#### Field: Zone Name
-
-This is the name of the Zone for the mixing.
-
-#### Field: Zone Floor Area {m2}
-
-This is the floor area (m2) of the zone.
-
-#### Field: \# Zone Occupants
-
-This is the total number of occupants for the zone.
-
-#### Field: Design Volume Flow Rate {m3/s}
-
-This is the nominal flow rate for the mixing in m3/s.
-
-#### Field: Volume Flow Rate/Floor Area {m3/s/m2}
-
-This field is the volume flow rate density per floor area (flow rate per floor area) for mixing.
-
-#### Field: Volume Flow Rate/person Area {m3/s/person}
-
-This field is the volume flow rate density per person (flow rate per person) for mixing.
-
-#### Field: ACH - Air Changes per Hour
-
-This field is the air changes per hour for the given mixing rate.
-
-#### Field: From/Source Zone
-
-This is the source zone for the mixing rate.
-
-#### Field: Delta Temperature {C}
-
-This number controls when mixing air from the source zone is sent to the receiving zone. This parameter is a temperature {units Celsius}. If this field is positive, the temperature of the zone from which the air is being drawn (source zone) must be “Delta Temperature� warmer than the receiving zone air or else no mixing occurs. If this field is negative, the temperature of the source zone must be “Delta Temperature� cooler than the receiving zone air or else no mixing occurs. If this parameter is zero, mixing occurs regardless of the relative zone temperatures.
-
-### Cross Mixing
-
-! &lt;CrossMixing Airflow Stats - Nominal&gt;,Name,Schedule Name,Zone Name, Zone Floor Area {m2}, \# Zone Occupants,Design Volume Flow Rate {m3/s},Volume Flow Rate/Floor Area {m3/s/m2},Volume Flow Rate/person Area {m3/s/person},ACH - Air Changes per Hour,From/Source Zone,Delta Temperature {C}
-
- CrossMixing Airflow Stats, EAST ZONE XMIXNG 1,ZONE MIXING,EAST ZONE,37.16,3.0,0.100,2.691E-003,3.333E-002,3.178,NORTH ZONE,1.00
-
- CrossMixing Airflow Stats, NORTH ZONE XMIXNG 1,ZONE MIXING,NORTH ZONE,55.74,4.0,0.100,1.794E-003,2.500E-002,2.119,EAST ZONE,1.00
-
-#### Field: &lt;CrossMixing Airflow Stats - Nominal&gt;
-
-This field contains the constant “CrossMixing Airflow Stats� for each line.
-
-#### Field: Name
-
-This field contains the name of the mixing statement from the IDF file.
-
-#### Field: Schedule Name
-
-This is the schedule of use fraction – the fraction is applied to the nominal volume flow rate for the statement. Limits are [0,1].
-
-#### Field: Zone Name
-
-This is the name of the Zone for the mixing.
-
-#### Field: Zone Floor Area {m2}
-
-This is the floor area (m2) of the zone.
-
-#### Field: \# Zone Occupants
-
-This is the total number of occupants for the zone.
-
-#### Field: Design Volume Flow Rate {m3/s}
-
-This is the nominal flow rate for the mixing in m3/s.
-
-#### Field: Volume Flow Rate/Floor Area {m3/s/m2}
-
-This field is the volume flow rate density per floor area (flow rate per floor area) for mixing.
-
-#### Field: Volume Flow Rate/person Area {m3/s/person}
-
-This field is the volume flow rate density per person (flow rate per person) for mixing.
-
-#### Field: ACH - Air Changes per Hour
-
-This field is the air changes per hour for the given mixing rate.
-
-#### Field: From/Source Zone
-
-This is the source zone for the mixing – air is exchanged equally between the two zones.
-
-#### Field: Delta Temperature {C}
-
-This number controls when mixing air from the source zone is sent to the receiving zone. This parameter is a temperature {units Celsius}. If this field is positive, the temperature of the zone from which air is being drawn (“source zone�) must be “Delta Temperature� warmer than the zone air or no mixing occurs. If this field is zero, mixing occurs regardless of the relative air temperatures. Negative values for “Delta Temperature� are not permitted.
-
-### RefrigerationDoor Mixing
-
-! &lt;RefrigerationDoorMixing  Airflow Stats - Nominal&gt;, Name, Zone 1 Name, Zone 2 Name, Door Opening Schedule Name, Door Height {m},Door Area {m2},Door Protection Type
-
- RefrigerationDoorMixing Airflow Stats, FREEZER1\_SUBFREEZER1, FREEZER\_1, SUBFREEZER, FREEZER1DOORSCHEDA, 1.800, 2.300, StripCurtain
-
- RefrigerationDoorMixing Airflow Stats, FREEZER5\_COOLER2, COOLER\_2, FREEZER\_5, FREEZER5DOORSCHEDA, 1.800, 2.300, AirCurtain
-
-#### Field: &lt;RefrigerationDoorMixing Airflow Stats - Nominal&gt;
-
-This field contains the constant “RefrigerationDoor Airflow Stats� for each line.
-
-#### Field: Name
-
-This field contains the name of the mixing statement from the IDF file.
-
-#### Field: Zone 1 Name
-
-This is the name of one of the two Zones for the mixing.
-
-#### Field: Zone 2 Name
-
-This is the name of the other Zone for the mixing.
-
-#### Field: Door Opening Schedule Name
-
-This is the schedule of use fraction – the fraction is applied to the nominal volume flow rate for the statement. Limits are [0,1].
-
-#### Field: Door Height {m}
-
-This is the nominal flow rate for the mixing in m3/s.
-
-#### Field: Door Area {m2}
-
-This is the floor area (m2) of the zone.
-
-#### Field: Door Protection Type
-
-This is one of three keywords, None, StripCurtain, or AirCurtain.
-
-### Shading Summary
-
-Similar to the Zone Summary, the Shading Summary:
-
-! &lt;Shading Summary&gt;, Number of Fixed Detached Shades, Number of Building Detached Shades, Number of Attached Shades
-
- Shading Summary,0,6,14
-
-#### Field: &lt;Shading Summary&gt;
-
-This field contains the constant “Shading Summary�.
-
-#### Field: Number of Fixed Detached Shades
-
-This field contains the number of fixed detached shades (e.g. Shading:Site or Shading:Site:Detailed) in the simulation.
-
-#### Field: Number of Building Detached Shades
-
-This field contains the number of building relative detached shades (e.g. Shading:Building or Shading:Building:Detailed) in the simulation.
-
-#### Field: Number of Attached Shades
-
-This field contains the number of building attached shading surfaces (e.g. Overhang, Shading:Zone:Detailed, etc.) in the simulation.
-
-### Surface Details Report
-
-A good example of this is the surface details report(s) (**Output:Surfaces:List, Details;** **Output:Surfaces:List, Vertices; Output:Surfaces:List, DetailsWithVertices;**). Excerpt from the file:
-
-**Line 1:**! &lt;Zone/Shading Surfaces&gt;**,**&lt;Zone Name&gt;/\#Shading Surfaces,\# Surfaces, Vertices are shown starting at Upper-Left-Corner =&gt; Counter-Clockwise =&gt; World Coordinates
-
-**Line 2:**! &lt;HeatTransfer/Shading/Frame/Divider\_Surface&gt;,Surface Name,Surface Class, Base Surface,Construction,Nominal U (w/o film coefs),Nominal U (with film coefs),Area (Net), Area (Gross), Area (Sunlit Calc), Aimuth, Tilt, ~Width, ~Height, Reveal, &lt;ExtBoundCondition&gt;, &lt;ExtConvCoeffCalc&gt;, &lt;IntConvCoeffCalc&gt;,&lt;SunExposure&gt;,&lt;WindExposure&gt;,ViewFactorToGround,ViewFactorToSky,ViewFactorToGround-IR,ViewFactorToSky-IR,\#Sides, {Vertex 1},,, {Vertex 2},,, {Vertex 3},,, {Vertex 4}, ,,{etc}
-
-**Line 3:** ! &lt;Units&gt;,,,,,{W/m2-K},{W/m2-K},{m2},{m2},{m2},{deg},{deg},{m},{m},{m},,,,,,,,,,X {m},Y {m},Z {m},X {m},Y {m},Z {m},X {m},Y {m},Z {m},X {m},Y {m},Z {m}
-
-**Ex Line 1:** Shading\_Surfaces,Number of Shading Surfaces,   10
-
-**Ex Line 2:** Shading\_Surface,WEST SIDE BUSHES,Detached Shading:Building,,,,, 180.0, 180.0, 180.0, 90.0, 90.0, 60.00, 3.00,,,,,,,,,,, 4, -5.00, 0.00, 3.00, -5.00, 0.00, 0.00, -5.00, 60.00, 0.00, -5.00, 60.00, 3.00
-
-**Ex Line 2:** Shading\_Surface,EAST SIDE TREE1,Detached Shading:Building,,,,, 500.0, 500.0, 500.0, 270.0, 90.0, 20.00, 50.99,,,,,,,,,,, 3, 70.00, 30.00, 50.00, 70.00, 40.00, 0.00, 70.00, 20.00, 0.00
-
-**Ex Line 2:** Shading\_Surface,EAST SIDE TREE2,Detached Shading:Building,,,,, 500.0, 500.0, 500.0, 0.0, 90.0, 20.00, 50.99,,,,,,,,,,, 3, 70.00, 30.00, 50.00, 80.00, 30.00, 0.00, 60.00, 30.00, 0.00
-
-**Ex Line 1:** Zone\_Surfaces,HEARTLAND AREA,   35
-
-**Ex Line 2:** HeatTransfer\_Surface,ZN001:WALL001,Wall,,EXTERIOR,0.644, 0.588, 136.0, 200.0, 136.0, 180.0, 90.0, 20.0, 10.0, 0.00,ExternalEnvironment,ASHRAEDetailed,ASHRAEDetailed,SunExposed,WindExposed, 0.50, 0.50, 0.67,  0.33, 4, 20.00, 10.00, 10.00, 20.00, 10.00, 0.00, 40.00, 10.00, 0.00, 40.00, 10.00, 10.00
-
-**Ex Line 2:** HeatTransfer\_Surface,ZN001:WALL001:WIN001,Window,ZN001:WALL001,SINGLE PANE HW WINDOW,N/A,6.121, 64.00000, 64.00000, 64.00000,180.0, 90.0, 8.00, 8.00, 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed,  0.50,  0.50,  0.71,  0.29, 4, 26.00, 10.00, 8.10, 26.00, 10.00, 0.10, 34.00, 10.00, 0.10, 34.00, 10.00, 8.10
-
-**Ex Line 2:** HeatTransfer\_Surface,ZN001:WALL002,Wall,,EXTERIOR,0.644,0.588, 155.0, 200.0, 155.0, 90.0, 90.0, 20.00, 10.00, 0.00,ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed, 0.50,  0.50,  0.73,  0.27, 4, 50.00, 20.00, 10.00, 50.00, 20.00, 0.00, 50.00, 40.00, 0.00, 50.00, 40.00, 10.00
-
-**Ex Line 2:** HeatTransfer\_Surface,ZN001:WALL002:WIN001,Window,ZN001:WALL002,SINGLE PANE HW WINDOW,N/A,6.121, 15.0, 15.0, 15.0, 90.0, 90.0, 3.00, 5.00,  0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed,  0.50,  0.50,  0.76,  0.24, 4, 50.00, 22.20, 7.30, 50.00, 22.20, 2.30, 50.00, 25.20, 2.30, 50.00, 25.20, 7.30
-
-
-
-**Ex Line 2:** HeatTransfer\_Surface,ZN001:WALL002:WIN002,Window,ZN001:WALL002,SINGLE PANE HW WINDOW, N/A, 6.121, 15.00, 15.00, 15.00, 90.00, 90.00, 3.00, 5.00, 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed, 0.50, 0.50, 0.71, 0.29, 4, 50.00, 28.50, 7.30, 50.00, 28.50, 2.30, 50.00, 31.50, 2.30, 50.00, 31.50, 7.30
-
-**Ex Line 2:** HeatTransfer\_Surface, ZN001:WALL002:WIN003, Window, ZN001:WALL002, SINGLE PANE HW WINDOW, N/A, 6.121, 15.00, 15.00, 15.00, 90.00, 90.00, 3.00, 5.00, 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed, 0.50, 0.50, 0.77, 0.23, 4, 50.00, 35.30, 7.30, 50.00, 35.30, 2.30, 50.00, 38.30, 2.30, 50.00, 38.30, 7.30
-
-&lt;reduced for brevity&gt;
-
-
-
-**Ex Line 1:** Zone\_Surfaces,MAINE WING,   12
-
-**Ex Line 2:** HeatTransfer\_Surface, ZN005:WALL001, Wall, , EXTERIOR, 0.644, 0.588, 100.00, 100.00, 100.00, 180.00, 90.00, 10.00, 10.00, 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed, 0.50, 0.50, 0.74, 0.26, 4, 50.00, 40.00, 10.00, 50.00, 40.00, 0.00, 60.00, 40.00, 0.00, 60.00, 40.00, 10.00
-
-**Ex Line 2:** HeatTransfer\_Surface, ZN005:FLR001, Floor, , SLAB FLOOR, 17.040, 3.314, 400.00, 400.00, 400.00, 90.00, 180.00, 20.00, 20.00, 0.00, Ground, N/A-Ground, ASHRAEDetailed, NoSun, NoWind, 1.00, 0.00, 1.00, 0.00, 4, 60.00, 40.00, 0.00, 40.00, 40.00, 0.00, 40.00, 60.00, 0.00, 60.00, 60.00, 0.00
-
-**Ex Line 2:** HeatTransfer\_Surface, ZN005:ROOF001, Roof, , ROOF31, 0.790, 0.688, 400.00, 400.00, 400.00, 180.00, 0.00, 20.00, 20.00, 0.00, ExternalEnvironment, ASHRAEDetailed, ASHRAEDetailed, SunExposed, WindExposed, 0.00, 1.00, 2.41E-002, 0.98, 4, 40.00, 60.00, 10.00, 40.00, 40.00, 10.00, 60.00, 40.00, 10.00, 60.00, 60.00, 10.00
-
-#### Description of the Detailed Surfaces Report(s)
-
-The preceding excerpt includes the surface details *and* vertices. You can also obtain the report with *just* the details or *just* the vertices.
-
-**Line 1:**! &lt;Zone/Shading Surfaces&gt;**,**&lt;Zone Name&gt;/\#Shading Surfaces,\# Surfaces, Vertices are shown starting at Upper-Left-Corner =&gt; Counter-Clockwise =&gt; World Coordinates
-
-When a line is shown with the comment character (!) in the first position, it signifies a informational “header� record for the report. In addition, “Line 1� is also a header for the subsequent “real� surface lines.
-
-#### Field: &lt;Zone/Shading Surfaces&gt;
-
-This field is a dual purpose field. For beginning of the Shading Surfaces, it will show “Shading\_Surfaces�. At each Zone, it will show “Zone\_Surfaces�.
-
-#### Field: &lt;Zone Name&gt;/\#Shading Surfaces
-
-This field is a dual purpose field. It will either show the Zone Name of the subsequent surfaces or the “Number of Shading Surfaces� for the entire building.
-
-#### Field: \# Surfaces
-
-This field, then, specifies the number of surfaces of the type (zone or shading) that will follow.
-
-The example lines illustrate:
-
-Shading\_Surfaces,Number of Shading Surfaces,   10
-
-Zone\_Surfaces,HEARTLAND AREA,   35
-
-Zone\_Surfaces,MAINE WING,   12
-
-
-
-**Line 2:**! &lt;HeatTransfer/Shading/Frame/Divider\_Surface&gt;, Surface Name, Surface Class, Base Surface, Construction, Nominal U (w/o film coefs), Nominal U (with film coefs), Area (Net), Area (Gross), Area (Sunlit Calc), Azimuth, Tilt, ~Width, ~Height, Reveal, &lt;ExtBoundCondition&gt;, &lt;ExtConvCoeffCalc&gt;, &lt;IntConvCoeffCalc&gt;, &lt;SunExposure&gt;, &lt;WindExposure&gt;, ViewFactorToGround, ViewFactorToSky, ViewFactorToGround-IR, ViewFactorToSky-IR, \#Sides, {Vertex 1},,, {Vertex 2},,, {Vertex 3},,, {Vertex 4}, ,,{etc}
-
-**Line 3:** ! &lt;Units&gt;,,,,,{W/m2-K},{W/m2-K},{m2},{m2},{m2},{deg},{deg},{m},{m},{m},,,,,,,,,,X {m},Y {m},Z {m},X {m},Y {m},Z {m},X {m},Y {m},Z {m},X {m},Y {m},Z {m}
-
-Line 2 shows the full detail of each surface record with Line 3 used for illustrating the units of individual fields (as appropriate).
-
-The first four fields (&lt;HeatTransfer/ShadingSurface&gt;,Surface Name, Surface Class, Base Surface) are included in all the Surface reports (Details, Vertices, Details with Vertices).
-
-#### Field: &lt;HeatTransfer/Shading/Frame/Divider\_Surface&gt;
-
-For shading surfaces, this will be a constant “Shading\_Surface�. For heat transfer surfaces, this will be a constant “HeatTransfer\_Surface�. For Frame and Divider Surfaces, it will be a constant “Frame/Divider\_Surface� with the proper type showing in the Surface Class.
-
-#### Field: Surface Name
-
-This field will contain the actual surface name as entered in the IDF.
-
-#### Field: Surface Class
-
-This field contains the surface class (e.g. Window, Door, Wall, Roof) as entered in the IDF.
-
-#### Field: Base Surface
-
-This field contains the base surface name if this surface is a sub-surface (i.e. Window, Door).
-
-#### Fields in Details and Details with Vertices report.
-
-#### Field: Construction
-
-This field will contain the name of the construction used for the surface. (Will be empty for shading surfaces).
-
-#### Field: Nominal U (w/o film coefs)
-
-A nominal thermal conductance for the surface is calculated for the surface. It does not include interior or exterior film coefficients as this is calculated during the simulation and is dependent on several factors that may change during the simulation time period. Units for this field are W/m<sup>2</sup>-K.
-
-For windows, no value is reported because the film coefficients cannot be removed from the U-value.
-
-#### Field: Nominal U (with film coefs)
-
-A nominal thermal conductance for the surface is calculated for the surface, including film coefficients. Units for this field are W/m<sup>2</sup>-K.
-
-For opaque surfaces, interior and exterior film coefficients are added to the surface construction based on the prescribed R-values for interior and exterior film coefficients as found in ASHRAE 90.1-2004, Appendix A, and shown below:  The SI values are the exact values used inside EnergyPlus.
-
-<table class="table table-striped">
-  <tr>
-    <th>Surface Class</th>
-    <th colspan="2">Interior Film Coefficient</th>
-    <th colspan="2">Exterior Film Coefficient</th>
-  </tr>
-  <tr>
-    <td></td>
-    <td>(ft2-F-hr/BTU)</td>
-    <td>(m2-K/W)</td>
-    <td>(ft2-F-hr/BTU)</td>
-    <td>(m2-K/W)</td>
-  </tr>
-  <tr>
-    <td>WALL</td>
-    <td>0.68</td>
-    <td>0.1197548</td>
-    <td>0.17</td>
-    <td>0.0299387</td>
-  </tr>
-  <tr>
-    <td>FLOOR</td>
-    <td>0.92</td>
-    <td>0.1620212</td>
-    <td>0.46</td>
-    <td>0.0810106</td>
-  </tr>
-  <tr>
-    <td>CEILING/ROOF</td>
-    <td>0.61</td>
-    <td>0.1074271</td>
-    <td>0.46</td>
-    <td>0.0810106</td>
-  </tr>
-</table>
-
-
-NOTE:  The resulting "Nominal U with film coefs" is only for comparison purposes with the ASHRAE 90.1 requirements. Actual film coefficients are calculated during the simulation and are dependent on several factors that may change during the simulation time period.
-
-For windows, the "Nominal U with film coefs" is calculated using the following assumptions from the WINDOW 5 program (also NFRC winter conditions):
-
-- Indoor air temperature = 21 C (69.8 F)
-
-- Outdoor air temperature = -18 C (-.4 F)
-
-- Exterior film coefficient =  26 W/m<sup>2</sup> (4.58 ft<sup>2</sup>-F-hr/BTU)
-
-- Interior film coefficient = Calculated by EnergyPlus convection algorithm
-
-- No incident solar beam radiation
-
-#### Field: Area (Net)
-
-When surfaces are entered, the gross area of the surface is calculated from the vertices (except for Internal Mass where it is entered directly). As net area is needed in the calculations, any sub-surfaces to the primary surface are subtracted from the original gross area. This field will show the final “net� area for the surface. For example, walls with windows will have the multiplier (of the window) \* window area subtracted from the gross amount. Likewise, any divider area (including multipliers) for the window will be subtracted. Units for this field are m<sup>2</sup>.
-
-#### Field: Area (Gross)
-
-This field shows the gross area of the surface. Units for this field are m<sup>2</sup>.
-
-#### Field: Area (Sunlit Calc)
-
-This field shows the net area for the purposes of sunlit/shading calculations. For these, only 1 unit of a multiplied window/door is subtracted from the gross area of a wall that the window/door is on. This net area includes the *frame area* (if any) for the windows on the wall. For windows, this value includes the divider area of the window. Thus for both frames and dividers, there will be a \* in this field – since the areas are included in the wall/window areas. Units for this field are m<sup>2</sup>.
-
-#### Field: Azimuth
-
-Using the specified vertices for the surface (and order of entry), EnergyPlus can determine the outward facing normal angle for the surface. That angle is displayed in this field. Units for this field are degrees.
-
-#### Field: Tilt
-
-Using the specified vertices for the surface (and order of entry), EnergyPlus can determine the tilt of the surface with respect to “horizontal�. That angle is displayed in this field. Units for this field are degrees.
-
-#### Field: ~Width
-
-This field (approximate width of the surface) is calculated and filled by EnergyPlus from the entered vertices. Some parts of EnergyPlus use a width and height rather than the more detailed vertex/area calculations. Units for this field are m.
-
-#### Field: ~Height
-
-This field (approximate height of the surface) is calculated and filled by EnergyPlus from the entered vertices. Some parts of EnergyPlus use a width and height rather than the more detailed vertex/area calculations. Units for this field are m.
-
-#### Field: Reveal
-
-This field is calculated for sub-surfaces with respect to their base surfaces using the entered vertices, plane of the two surfaces, and distance between the planes. Reveal may be important in shading of windows, in particular. Units for this field are m.
-
-#### Field: &lt;ExtBoundCondition&gt;
-
-This field shows the exterior boundary condition for the surface. If this is a surface that is “external� the values will be **ExternalEnvironment** or **Ground**. If this surface is an interzone surface, this value will be the surface name in the “other� zone. If this surface is an internal surface, this value will be the same as the surface name. If this is a special surface with “Other Side Coefficients�, the value will be the OtherSideCoefficient name (see description of OtherSideCoefficient reporting later in this document). If this is a special surface with “Other Side Condition Model�, the value will be the OtherSideConditionModel name.
-
-#### Field: &lt;ExtConvCoeffCalc&gt;
-
-The value for this field will be a descriptor of the External Convection Coefficient calculation. If this surface uses Other Side Coefficients, this field will display **N/A-OSC**. If this surface uses Other Side Condition Model, this field will display **N/A-OSCM**. Ground surfaces will display **N/A-Ground**. If this is an interior or inter-zone surface, it will display **Other/Same Surface Int Conv**. If a schedule is used, it will display **User Supplied Schedule.** If a constant value is supplied by the user, it will display **User Supplied Value**. The standard values may also be displayed here (e.g. **ASHRAEDetailed**).
-
-#### Field: &lt;IntConvCoeffCalc&gt;
-
-The value for this field will be a descriptor of the Internal Convection Coefficient calculation. If a schedule is used, it will display **User Supplied Schedule.** If a constant value is supplied by the user, it will display **User Supplied Value**. The standard values may also be displayed here (e.g. **ASHRAEDetailed**).
-
-#### Field: &lt;SunExposure&gt;
-
-The value for this field will be **SunExposed** or **NoSun**. Internal surfaces should have NoSun exposure.
-
-#### Field: &lt;WindExposure&gt;
-
-The value for this field will be **WindExposed** or **NoWind**. Internal surfaces should have NoWind exposure.
-
-#### Field: ViewFactorToGround
-
-This value has been entered as part of the surface description. View factor to ground is described in the Input Output Reference document during the Surface:HeatTransfer description.
-
-#### Field: ViewFactorToSky
-
-This value is calculated by EnergyPlus based on surface tilt and shadowing surfaces.
-
-#### Field: ViewFactorToGround-IR
-
-This value is calculated by EnergyPlus based on surface tilt and shadowing surfaces. Shadowing surfaces are considered to have the same emissivity and temperature as the ground, so they are lumped together with the ground in calculating the ground IR view factor.
-
-#### Field: ViewFactorToSky-IR
-
-This value is calculated by EnergyPlus based on surface tilt and shadowing surfaces.
-
-#### Field: \#Sides
-
-This value is the number of sides / vertices the surface has.
-
-#### Fields in Vertices Reports
-
-#### Field Set: Vertex x [X {m}, Y {m}, Z {m}]
-
-For each side of the surface, the vertices are shown in three separate fields (comma separated) in the EnergyPlus “standard� coordinate order (Upper Left Corner first, Counter-Clockwise, World Coordinates). Units for each vertex is m.
-
-### Calculating with Surface Details Report
-
-It is reasonably easy to import this data into a spreadsheet and then calculate glazing area percentage based on wall facing direction:
-
-![](media/image012.png)
-
-Figure 3. Surface Details with Window/Wall % calculated
-
-### Surface Convection Parameters
-
-When detailed surface reports are requested, extra information on the surfaces related to how convection coefficients are calculated are also output to the EIO file.  The first block of data relates to overall geometry parameters assigned to each surface and has the following header
-
-! &lt;Surface Convection Parameters&gt;, Surface Name, Outside Model Assignment , Outside Area [m2], Outside Perimeter [m], Outside Height [m], Inside Model Assignment, Inside Height [cm], Inside Perimeter Envelope [m], Inside Hydraulic Diameter [m], Window Wall Ratio [ ],Window Location [ ], Near Radiant [T/F], Has Active HVAC [T/F]
-
-With example data record.
-
-Surface Convection Parameters,PERIMETER\_ZN\_1\_WALL\_SOUTH,0,84.45,61.48,3.05,0,3.05,27.69,6.94,0.24,0, F, F
-
-
-
-#### Field: Outside Model Assignment
-
-This is an integer code for the type of model assigned to the outside face, if a specific model has been assigned. Surface(SurfLoop)%ExtConvCoeff
-
-
-
-<table class="table table-striped">
-<tr>
-<th>Code value</th>
-<th>meaning</th>
-</tr>
-<tr>
-<td>0</td>
-<td>Not set special for this surface</td>
-</tr>
-<tr>
-<td>+/-1</td>
-<td>Simplest ASHRAE model</td>
-</tr>
-<tr>
-<td>+/-2</td>
-<td>TARP, ASHRAE-Walton model</td>
-</tr>
-<tr>
-<td>+/-5</td>
-<td>TARP, ASHRAE-Walton model</td>
-</tr>
-<tr>
-<td>+/- 6</td>
-<td>MoWITT model</td>
-</tr>
-<tr>
-<td>+/- 7</td>
-<td>DOE-2 model</td>
-</tr>
-<tr>
-<td>+/- 9</td>
-<td>Adaptive Convection Algorithm</td>
-</tr>
-<tr>
-<td>&gt;9</td>
-<td>Key values are indexes that are associated with the input order of SurfaceProperty:ConvectionCoefficients ( and MultipleSurface)</td>
-</tr>
-</table>
-
-
-
-#### Field: Outside Area
-
-This is the area used for convection calculations for the outside face.  It is intended to be a model of the area of the larger group of surfaces that this surfaces is a part of. [m<sup>2</sup>]
-
-#### Field Outside Perimeter
-
-This is the length of edge used for convection calculations for the outside face.  It is intended to be a model of the perimeter for a larger group of surfaces that surface is a part of.  [m]
-
-#### Field: Outside Height
-
-This is the height scale used for convection calculations for the outside face.  It is intended to be a model of the overall height of a larger group of surfaces that this surface is a part of. [m]
-
-#### Field: Inside Model Assignment
-
- This is an integer code for the type of model assigned to the inside face, if a specific model has been assigned. Surface(SurfLoop)%IntConvCoeff
-
-#### Field: Inside Height
-
-This is the height scale used for convection calculations for the inside face.  It is intended to be for the entire zone. [m]
-
-#### Field: Inside Perimeter Envelope
-
-This is the length scale for the zone for the amount of exterior envelope with glazing.  It is the length of wall that has glazed exterior.[m]
-
-#### Field: Inside Hydraulic Diameter
-
-This is the length scale for horizontal surfaces in the zone.   It is calculated using 4 \* area/ perimeter and is used for natural convection on the floor or ceiling. [m]
-
-#### Field: Window to Wall Ratio
-
-This is the ratio of exterior window area to exterior wall area.  It is for the zone. [non dimensional]
-
-#### Field: Window Location
-
-This is an integer code for relative window positioning.  It is used for some inside face correlations.
-
-#### Field: Near Radiant
-
-This is a true or false flag indicating if this surfaces is near a radiant HVAC unit. If “T� then surface is is modeled as near a radiant HVAC device.  If  “F� then surface is normal.
-
-#### Field: Has Active HVAC
-
-This is a true or false flag indicating if this surface has active HVAC elements inside it.  If “T� then surface is modeled has having HVAC pipes or element inside it making it active for heating or cooling.  If  “F� then surface is normal.
-
-### OtherSideCoefficient Outputs
-
-For the most part, the output for the Other Side Coefficients represents the input as entered. The header record for the Other Side Coefficients output is shown below:
-
-**Line 1:** ! Other Side Coefficients,Name,Combined convective/radiative film coefficient,User selected Constant Temperature,Coefficient modifying the constant temperature term,Coefficient modifying the external dry bulb temperature term,Coefficient modifying the ground temperature term,Coefficient modifying the wind speed term {s/m},Coefficient modifying the zone air temperature term,Constant Temperature Schedule Name
-
-#### Field: Other Side Coefficients
-
-This field will be filled with the text **OtherSideCoefficients**.
-
-The report describes the actions for the following equation:
-
-The coefficients listed above are used in the following equation:
-
-<div>\[ T = C_2 T_{zone} + C_3 T_{oadb} + C_4 C_5 + C_6 T_{grnd} + C_7 W_{spd} T_{oadb}\]</div>
-
-where:
-
-* T = Outdoor air Temperature when Combined convective/radiative film Coeff &gt; 0
-* T = Exterior Surface Temperatre when Combined convective/radiative film Coeff &lt;= 0
-* Tzone  = Temperature of the zone being simulated (°C)
-* Toadb  = Dry-bulb temperature of the outdoor air (°C)
-* Tgrnd  = Temperature of the ground (°C)
-* Wspd  = Outdoor wind speed (m/sec)
-
-#### Field: Name
-
-This is the unique name entered for the OtherSideCoefficient. Note that the surface it applies to will have this name in the &lt;ExtBoundCondition&gt; field.
-
-#### Field: Combined convective/radiative film coefficient
-
-This field is a trigger value. When entered as &gt;0, it is used as the combined convective/radiative film coefficient. The other fields in the OtherSideCoefficient object are used then as well: the remaining fields are used first to calculate the outdoor air temperature for the surface and then to calculate the outside surface temperature based on the outdoor air temperature and the film coefficient. If this field contains **N/A**, then the remaining fields are used to calculate the surface temperature (not the outdoor air temperature).
-
-#### Field: User selected Constant Temperature
-
-This field is a temperature that remains a constant part of the calculation either of the surface or outdoor air temperature. When the schedule option is used, this field will show **N/A**. The parameter in the equation for this or the schedule value is ***C5***.
-
-#### Field: Coefficient modifying the constant temperature term
-
-This field is multiplied to the previous field when a simple number is entered. This parameter is shown as ***C4*** in the equation. This parameter is dimensionless. The value of this parameter should be 1.0 if a schedule is used to set ***C5***.
-
-#### Field: Coefficient modifying the external dry bulb temperature term
-
-This field defines a constant coefficient that is applied to the outdoor air dry-bulb temperature. This parameter is shown as ***C3*** in the equation. This parameter is dimensionless.
-
-#### Field: Coefficient modifying the ground temperature term
-
-This field defines a constant coefficient that is applied to the ground temperature. This parameter is shown as ***C6*** in the equation. This parameter is dimensionless.
-
-#### Field: Coefficient modifying the wind speed term {s/m}
-
-This field defines a constant coefficient that is applied to the product of the outdoor air dry-bulb temperature and the wind speed. This parameter is shown as ***C7*** in the equation. This parameter has dimensions of inverse velocity or s/m.
-
-#### Field: Coefficient modifying the zone air temperature term
-
-This field defines a constant coefficient that is applied to the temperature of the zone to which this surface belongs. This parameter is shown as ***C2*** in the equation. This parameter is dimensionless.
-
-#### Field: Constant Temperature Schedule Name
-
-This field is used to supply a schedule name. That schedule supplies the “constant� temperature value ***C5***. Note that the value of the ***C4*** field should normally be 1.0 if a schedule is used for ***C5***. If this field contains a value, then constant temperature field will be **N/A** in this report.
-
-### Construction Element Outputs
-
-An optional report (contained in **eplusout.eio**) gives calculated elements for the materials and constructions used in the input. One report is specific to opaque constructions (note that nominal thermal conductance is calculated).
-
-The report is invoked by including the following in the IDF:
-
-**Output:Constructions,Constructions;**
-
-
-
-**Line 1:**! &lt;Construction&gt;,Construction Name,\#Layers,\#CTFs,Time Step {hours},ThermalConductance {w/m2-K},OuterThermalAbsorptance,InnerThermalAbsorptance,OuterSolarAbsorptance,InnerSolarAbsorptance,Roughness
-
-**Line 2:**! &lt;Material&gt;,Material Name,Thickness {m},Conductivity {w/m-K},Density {kg/m3},Specific Heat {J/kg-K},ThermalResistance {m2-K/w}
-
-**Line 3:**! &lt;Material:Air&gt;,Material Name,ThermalResistance {m2-K/w}
-
-**Line 4:**! &lt;CTF&gt;,Time,Outside,Cross,Inside,Flux (except final one)
-
-**Ex Line 1:** Construction,EXTWALL09, 4,10, 0.250,2.545    ,   0.900,   0.900,   0.930,   0.920,Rough
-
-**Ex Line 2:** Material,A2 - 4 IN DENSE FACE BRICK,  0.1015, 1.245, 2082.400, 920.480,  0.8151E-01
-
-**Ex Line 2:** Material:Air,B1 - AIRSPACE RESISTANCE,  0.1604
-
-**Ex Line 2:** Material,C3 - 4 IN HW CONCRETE BLOCK,  0.1015, 0.813,  977.126,  836.800,  0.1249
-
-**Ex Line 2:** Material,E1 - 3 / 4 IN PLASTER OR GYP BOARD,0.0191,0.726, 1601.846,  836.800,  0.2622E-01
-
-**Ex Line 3:** CTF,  10,      0.13890138E-11,      0.95367648E-14,      0.62566281E-10,     -0.39500133E-14
-
-**Ex Line 3:** CTF,   9,     -0.32803336E-08,      0.29933755E-10,     -0.60855613E-07,      0.10196216E-10
-
-**Ex Line 3:** CTF,   8,      0.23798948E-05,      0.21201413E-07,      0.21649376E-04,     -0.88463084E-08
-
-**Ex Line 3:** CTF,   7,     -0.58681847E-03,      0.38118098E-05,     -0.26539198E-02,      0.25879187E-05
-
-**Ex Line 3:** CTF,   6,      0.46201324E-01,      0.18871269E-03,      0.12095720    ,     -0.26290432E-03
-
-**Ex Line 3:** CTF,   5,      -1.2828328    ,      0.27337395E-02,      -2.1646103    ,      0.91268499E-02
-
-**Ex Line 3:** CTF,   4,       13.603723    ,      0.11920108E-01,       17.065325    ,     -0.12663354
-
-**Ex Line 3:** CTF,   3,      -62.546625    ,      0.15112689E-01,      -64.276824    ,      0.73877389
-
-**Ex Line 3:** CTF,   2,       133.27916    ,      0.47414487E-02,       120.00640    ,      -1.9706501
-
-**Ex Line 3:** CTF,   1,      -130.02410    ,      0.22383019E-03,      -106.88260    ,       2.3359193
-
-**Ex Line 3:** CTF,   0,       46.959981    ,      0.53137072E-06,       36.168919   
-
-### Opaque Constructions
-
-#### Description of the Opaque Construction Report
-
-The Opaque Construction report has 3 parts for each construction.
-
-Part 1 is the construction name along with some derived values for the entire construction (i.e. Thermal Conductance) as well as noting other details about the surface (\# CTFs, \#  Layers).
-
-Part 2 shows the material layers for the construction. This is essentially just an echo of the entered properties of the materials from the IDF.
-
-Part 3 shows the CTFs as calculated for the Construction. CTFs are described more completely in the Engineering Reference document.
-
-#### Fields in Part 1 – Opaque Construction Report
-
-#### Field: &lt;Construction&gt;
-
-This will be filled with the constant “Construction� for each Construction line.
-
-#### Field: Construction Name
-
-This is the name of the construction as entered in the IDF.
-
-#### Field: \#Layers
-
-This is the number of material layers inferred from the construction entry in the IDF. Material layers are listed “outside� to “inside� of the construction. This, of course, depends on the placement of the surface in the building – the “outside� of an internal surface is the layer that is closest to whatever the surface touches whereas the “inside� of an internal surface is the layer that shows in the surface’s “zone�. The outside of an external surface is the layer that faces the outside environment and, again, the inside is the layer that shows in the zone.
-
-#### Field: \#CTFs
-
-This is the calculated number of CTFs (Conduction Transfer Functions). The conduction transfer functions are temperature and flux coefficients that characterize the thermal properties of the wall.
-
-#### Field: Time Step
-
-The "timestep" in the construction line is the timestep at which the CTFs are valid. Because CTFs for certain constructions might not be stable at the user specified timestep (might be too "heavy" from a thermal mass standpoint), this may be different from the zone timestep (specified in “TimeStep in Hour�). In all cases though, this will be greater than or equal to the zone timestep. If the timestep for the construction is greater than the zone timestep, E+ will use interpolated histories to solve for the surface heat balances for this surface (see discussion on interpolated histories in the [Engineering Reference](file:///E:\Docs4PDFs\EngineeringDoc.pdf) document).
-
-#### Field: Thermal Conductance
-
-This is the nominal thermal conductance of the construction calculated without film coefficients. Units are w/m<sup>2</sup>-K.
-
-#### Field: Outer Thermal Absorptance
-
-This will be the thermal absorptance of the outer material layer.
-
-#### Field: Inner Thermal Absorptance
-
-This will be the thermal absorptance of the inner material layer.
-
-#### Field: Outer Solar Absorptance
-
-This will be the solar absorptance of the outer material layer.
-
-#### Field: Inner Solar Absorptance
-
-This will be the solar absorptance of the inner material layer.
-
-#### Field: Roughness
-
-The construction takes on the roughness from the outer material layer. Roughness is used in several parts of external environment calculations.
-
-#### Fields in Part 2 – Opaque Construction Report
-
-**Line 2:** ! &lt;Material&gt;,Material Name,Thickness {m},Conductivity {w/m-K},Density {kg/m3},Specific Heat {J/kg-K},ThermalResistance {m2-K/w}
-
-In this version of part 2, the full material properties are entered by the user and displayed in the report.
-
-#### Field: &lt;Material&gt;
-
-This will be filled with the constant “Material� for each material layer line.
-
-#### Field: Material Name
-
-This is the name of the material as entered in the IDF.
-
-#### Field: Thickness
-
-This is the entered thickness of the material. Units are m.
-
-#### Field: Conductivity
-
-For Material:Regular materials, this will be the entered conductivity in w/m-K. For Material:Regular-R materials, this will be shown as 0.0.
-
-#### Field: Density
-
-For Material:Regular materials, this will be the entered density in kg/m<sup>3</sup>. For Material:Regular-R materials, this will be shown as 0.0.
-
-#### Field: Specific Heat
-
-For Material:Regular materials, this will be the entered specific heat in J/kg-K. For Material:Regular-R materials, this will be shown as 0.0.
-
-#### Field: Thermal Resistance
-
-For Material:Regular-R materials, this is the entered thermal resistance in m<sup>2</sup>-K/w. For Material:Regular materials, this is the calculated thermal resistance based on the other properties.
-
-**Line 3:** ! &lt;Material:Air&gt;,Material Name,ThermalResistance {m2-K/w}
-
-In this version of part 2, only the thermal resistance of the air layer is entered by the user and displayed in the report.
-
-#### Field: &lt;Material:Air&gt;
-
-This will be filled with the constant “Material:Air� for each material layer line.
-
-#### Field: Material Name
-
-This is the name of the material as entered in the IDF.
-
-#### Field: Thermal Resistance
-
-This is the entered thermal resistance in m<sup>2</sup>-K/w.
-
-#### Fields in Part 3 – Opaque Construction Report
-
-**Line 4:** ! &lt;CTF&gt;,Time,Outside,Cross,Inside,Flux (except final one)
-
-In part 3, the CTF calculations are shown. It is necessary to use the conduction transfer functions labeled "Inside" and "Cross" to calculate the heat flux at the inside surface and the conduction transfer functions labeled "Outside" and "Cross" to calculate the heat flux at the outside surface. Inside and outside coefficients will be identical for symmetric walls.
-
-Conduction through constructions such as walls, roofs, floors, etc. is generally characterized as one-dimensional and transient within EnergyPlus. The solution to this partial differential equation results in "conduction transfer functions" or CTFs. In a CTF equation, the current heat transfer flux due to conduction through a construction is a function of the current temperature at either face of the surface as well as the history of temperatures at either face and the history of conductive fluxes at this face. CTFs are a simplification of response factors which are based solely on temperature histories and require an "infinite" history. The inclusion of heat flux history terms reduces the overall number of terms in the equation for conductive flux significantly, resulting in a more efficient solution.
-
-For each unique combination of materials, there are a unique set of CTFs. While there are other procedures to determine the CTFs for a particular construction, EnergyPlus uses a state-space method (see conduction transfer function documentation) to obtain the CTF coefficients. These coefficients are calculated once at the beginning of the simulation and are constant for a particular construction. The CTF equation itself is a linear equation with these constant coefficients.
-
-Conduction heat transfer flux at the outside face of a particular surface is a function of the construction of the surface (which leads to the CTF coefficients), the current and previous temperatures at both the inside and outside face of the surface, and the previous conduction heat transfer fluxes at the outside surface. The CTF coefficients that would be used in this equation would be the "Outside" (multiplied by the temperature history at the outside face) terms, the "Cross" (multiplied by the temperature history at the inside face) terms, and the "Flux" (multiplied by the flux history at the outside face) terms. Solving for the conductive flux at the inside surface would require the use of the "Inside" (multiplied by the temperature history at the inside face) terms, the "Cross" (multiplied by the temperature history at the outside face) terms, and the "Flux" (multiplied by the flux history at the inside face) terms. A textual example is given below for illustration purposes:
-
-Current Outside Conductive Flux = (Outside Term 0) \* (Current Outside Face Temperature)
-
-                                 +(Outside Term 1) \* (Previous Outside Face Temperature)
-
-                                 +(Outside Term 2) \* (Outside Face Temperature 2 Time Steps Ago)
-
-                                 +(Outside Term 3) \* (Outside Face Temperature 3 Time Steps Ago)
-
-                                 + ...
-
-                                 +(Cross Term 0) \* (Current Inside Face Temperature)
-
-                                 +(Cross Term 1) \* (Previous Inside Face Temperature)
-
-                                 +(Cross Term 2) \* (Inside Face Temperature 2 Time Steps Ago)
-
-                                 +(Cross Term 3) \* (Inside Face Temperature 3 Time Steps Ago)
-
-                                 + ...
-
-                                 +(Flux Term 1) \* (Previous Outside Face Flux)
-
-                                 +(Flux Term 2) \* (Outside Face Flux 2 Time Steps Ago)
-
-                                 +(Flux Term 3) \* (Outside Face Flux 3 Time Steps Ago)
-
-                                 + ...
-
-
-
-The number of terms is based on the CTF coefficient calculation routine and is related to the amount of thermal mass contained within a particular construction. Actual signs (positive or negative) of various terms in the preceding equation will vary based on their definition and use within the equation. Those interested in more details on the use and calculation of CTFs are encouraged to read the Engineering Documentation.
-
-#### Field: &lt;CTF&gt;
-
-This will be filled with the constant “CTF� for each CTF coefficient line.
-
-#### Field: Time
-
-This field "time" refers to the history term to which the coefficients are applied. The last line is the "zero" term that gets applied to the current values of temperatures. The line with a "1" refers to the temperatures and fluxes from the previous timestep--previous as in time minus one timestep. Timestep, in this case, is defined by the construction timestep (see description on “Fields in Part 1 – Opaque Construction Report�) *not* the zone timestep. Lines with other values are for previous timesteps at t-n(timestep). These are the terms that are used to model conduction through a construction.
-
-#### Field: Outside
-
-#### Field: Cross
-
-#### Field: Inside
-
-#### Field: Flux (except final one)
-
-### Window Constructions
-
-#### Description of the Windows Construction Report
-
-A separate report is available for windows (note that both nominal conductance and Solar Heat Gain Coefficient are calculated for windows). Like the opaque construction, the window construction report has multiple parts – in this case, 2.
-
-
-
-**Line 1:** ! &lt;WindowConstruction&gt;,Construction Name,\#Layers,Roughness,Conductance {W/m2-K},SHGC,SolarTransmittanceNormalIncid,VisibleTransmittanceNormalIncid
-
-**Line 2:** ! &lt;WindowMaterial:Glazing&gt;, Material Name, Optical Data Type, Spectral Data Set Name, Thickness {m}, Solar Transmittance,Front Solar Reflectance, Back Solar Reflectance, Visible Transmittance, Front Visible Reflectance,Back Visible Reflectance,Infrared Transmittance, Front Thermal Emissivity, Back Thermal Emissivity,Conductivity {W/m-K},Dirt Factor,Solar Diffusing
-
-**Line 3:** ! &lt;WindowMaterial:Gas&gt;,Material Name,GasType,Thickness {m}
-
-**Line 4:** ! &lt;WindowMaterial:Shade&gt;,Material Name,Thickness {m},Conductivity {W/m-K},ThermalAbsorptance,Transmittance,VisibleTransmittance,ShadeReflectance
-
-**Line 5:** ! &lt;WindowMaterial:Screen&gt;,Material Name,Thickness {m},Conductivity {W/m-K},ThermalAbsorptance,Transmittance,Reflectance,VisibleReflectance,DiffuseReflectance,DiffuseVisibleReflectance,ScreenMaterialDiameterToSpacingRatio,ScreenToGlassDistance {m}
-
-**Line 6:** ! &lt;WindowMaterial:Blind&gt;,Material Name,SlatWidth {m},SlatSeparation {m},SlatThickness {m},SlatAngle {deg},SlatBeamSolarTransmittance,SlatBeamSolarFrontReflectance,BlindToGlassDistance {m}
-
-WindowConstruction,DOUBLE PANE WITH SCREEN,   4,MediumRough,   2.514,   0.555,   0.511,   0.589
-
- WindowMaterial:Screen,BRIGHT ALUMINUM SCREEN 1, 0.00025,  2.210E+02,  0.272,  0.697,  0.166,  0.166,  0.195,  0.195,  0.165,  0.025
-
- WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,SpectralAverage,,  0.00300,  0.83700,  0.07500,  0.07500,  0.89800,  0.08100,  0.08100,  0.00000,  0.84000,  0.84000,  0.90000,  1.00000,No
-
- WindowMaterial:Gas,WINAIRB1 - AIRSPACE RESISTANCE,Air,  1.300E-02,
-
- WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,SpectralAverage,,  0.00300,  0.83700,  0.07500,  0.07500,  0.89800,  0.08100,  0.08100,  0.00000,  0.84000,  0.84000,  0.90000,  1.00000,No
-
-WindowConstruction,DOUBLE PANE WITH SHADE,   4,VerySmooth,   2.716,   0.482,   0.039,   0.050
-
- WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,SpectralAverage,,  0.00300,  0.83700,  0.07500,  0.07500,  0.89800,  0.08100,  0.08100,  0.00000,  0.84000,  0.84000,  0.90000,  1.00000,No
-
- WindowMaterial:Gas,WINAIRB1 - AIRSPACE RESISTANCE,Air,  1.300E-02,
-
- WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,SpectralAverage,,  0.00300,  0.83700,  0.07500,  0.07500,  0.89800,  0.08100,  0.08100,  0.00000,  0.84000,  0.84000,  0.90000,  1.00000,No
-
- WindowMaterial:Shade,SHADE ROLL - LIGHT OPAQUE,  0.003,  1.000E-01,  0.900,  0.050,  0.050,  0.500
-
-WindowConstruction,DOUBLE PANE WITH BLIND,   4,VerySmooth,   2.761,   0.714,   0.395,   0.456
-
- WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,  0.003,  0.900,  0.837,  0.898,  0.840,  0.840,  0.075,  0.075,  0.081,  0.081,  1.000,NO
-
- WindowMaterial:Gas,WINAIRB1 - AIRSPACE RESISTANCE,Air,  1.300E-02,
-
- WindowMaterial:Glazing,GLASS - CLEAR SHEET 1 / 8 IN,  0.003,  0.900,  0.837,  0.898,  0.840,  0.840,  0.075,  0.075,  0.081,  0.081,  1.000,NO
-
- WindowMaterial:Blind,INTERIOR BLIND, 0.0010, 0.0022, 0.0010,  0.000,  0.000,  0.200,  0.025
-
-#### Fields in Part 1 – Window Construction Report
-
-**Line 1:** ! &lt;WindowConstruction&gt;,Construction Name,\#Layers,Roughness,Conductance {W/m2-K},SHGC,SolarTransmittanceNormalIncid,VisibleTransmittanceNormalIncid
-
-#### Field: &lt;WindowConstruction&gt;
-
-This will be filled with the constant “Construction� for each Window Construction line.
-
-#### Field: Construction Name
-
-This is the name of the window as entered in the IDF.
-
-#### Field: \#Layers
-
-This is the number of material layers inferred from the windows construction entry in the IDF. Material layers are listed “outside� to “inside� of the construction. This, of course, depends on the placement of the surface in the building – the “outside� of an internal surface is the layer that is closest to whatever the surface touches whereas the “inside� of an internal surface is the layer that shows in the surface’s “zone�. The outside of an external surface is the layer that faces the outside environment and, again, the inside is the layer that shows in the zone.
-
-#### Field: Roughness
-
-The window construction takes on the roughness from the outer material layer. Roughness is used in several parts of external environment calculations.
-
-#### Field: Conductance
-
-This is the center-of-glass conductance of the construction calculated with film coefficients, for winter conditions (indoor air temperature = 21C (69.8F), outdoor air temperature = -18C (-.4F), windspeed = 5.5 m/s (12.3 mph), no solar radiation). Units are W/m<sup>2</sup>-K.
-
-#### Field: SHGC
-
-This is the center-of-glass Solar Heat Gain Coefficient for summer conditions (indoor air temperature = 24C (75.2F), outdoor air temperature = 32C (89.6F), windspeed = 2.8 m/s (6.2 mph), 783 W/m2 (248 Btu/h-ft2) incident beam solar radiation normal to glazing.
-
-The following transmittance and reflectance values are for the window glazing (plus shade, screen or blind, if present in the construction). For exterior windows, “front� means the side of the window facing the exterior environment and “back� means the side facing the zone. For interior windows, “front� means the side to window facing the zone and “back� means the side facing the adjacent zone.
-
-#### Field: Solar Transmittance at Normal Incidence (SolarTransmittanceNormalIncid)
-
-Transmittance at normal incidence averaged over the solar spectrum.
-
-#### Field: Visible Transmittance at Normal Incidence (VisibleTransmittanceNormalIncid)
-
-Transmittance normal incidence averaged over the solar spectrum and weighted by the response of the human eye.
-
-#### Fields in Part 2 – Window Construction Report
-
-Part 2 of the Window Construction Report encompasses several “lines�.
-
-**Line 2:** ! &lt;WindowMaterial:Glazing&gt;, Material Name, Optical Data Type, Spectral Data Set Name, Thickness {m}, Solar Transmittance,Front Solar Reflectance, Back Solar Reflectance, Visible Transmittance, Front Visible Reflectance,Back Visible Reflectance,Infrared Transmittance, Front Thermal Emissivity, Back Thermal Emissivity,Conductivity {W/m-K},Dirt Factor,Solar Diffusing
-
-**Line 3:** ! &lt;WindowMaterial:Gas&gt;,Material Name,GasType,Thickness {m}
-
-**Line 4:** ! &lt;WindowMaterial:Shade&gt;,Material Name,Thickness {m},Conductivity {W/m-K},ThermalAbsorptance,Transmittance,VisibleTransmittance,ShadeReflectance
-
-**Line 5:** ! &lt;WindowMaterial:Screen&gt;,Material Name,Thickness {m},Conductivity {W/m-K},ThermalAbsorptance,Transmittance,Reflectance,VisibleReflectance,DiffuseReflectance,DiffuseVisibleReflectance,ScreenMaterialDiameterToSpacingRatio,ScreenToGlassDistance {m}
-
-**Line 6:** ! &lt;WindowMaterial:Blind&gt;,Material Name,SlatWidth {m},SlatSeparation {m},SlatThickness {m},SlatAngle {deg},SlatBeamSolarTransmittance,SlatBeamSolarFrontReflectance,BlindToGlassDistance {m}
-
-### Material**:**WindowGlass
-
-#### Field:  &lt;Material:WindowGlass&gt;
-
-This will be filled with the constant “Material:WindowGlass� for each material of this type in the construction.
-
-#### Field: Material Name
-
-Name of the glass layer.
-
-#### Field: Thickness {m}
-
-Thickness of the glass layer.
-
-#### Field: Conductivity {w/m-K}
-
-Conductivity of the glass layer.
-
-#### Field: SolarTransmittance
-
-Transmittance of the glass layer at normal incidence averaged over the solar spectrum.
-
-#### Field: VisibleTransmittance
-
-Transmittance normal incidence of the glass layer averaged over the solar spectrum and weighted by the response of the human eye.
-
-#### Field: ThermalFrontAbsorptance
-
-Thermal emissivity of the front face of the glass layer.
-
-#### Field: ThermalBackAbsorptance
-
-Thermal emissivity of the back face of the glass layer.
-
-#### Field: SolarFrontReflectance
-
-Reflectance of the front face of the glass layer at normal incidence averaged over the solar spectrum.
-
-#### Field: SolarBackReflectance
-
-Reflectance of the back face of the glass layer at normal incidence averaged over the solar spectrum.
-
-#### Field: VisibleFrontReflectance
-
-Reflectance of the front face of the glass layer at normal incidence averaged over the solar spectrum.
-
-#### Field: VisibleBackReflectance
-
-Reflectance of the back face of the glass layer at normal incidence averaged over the solar spectrum.
-
-#### Field: GlassTransDirtFactor
-
-Glass transmittance dirt factor (1.0 is clear, no dirt factor).
-
-#### Field: SolarDiffusing
-
-Solar Diffusing value – Yes if solar diffusing glass, No if not.
-
-#### Material:WindowGas
-
-#### Field:  &lt;Material:WindowGas&gt;
-
-This will be filled with the constant “Material:WindowGas� for each material of this type in the construction.
-
-#### Field: Material Name
-
-Name of the gas layer.
-
-#### Field: GasType
-
-Type of the gas layer. Possibilities are Air, Argon, Krypton,  Xenon, and Custom.
-
-#### Field: Thickness {m}
-
-Thickness of the gas layer.
-
-#### Material:WindowShade
-
-#### Field:  &lt;Material:WindowShade&gt;
-
-This will be filled with the constant “Material:WindowShade� for each material of this type in the construction.
-
-#### Field: Material Name
-
-Name of the window shade layer.
-
-#### Field: Thickness {m}
-
-Thickness of the window shade layer.
-
-#### Field: Conductivity {w/m-K}
-
-Thermal conductivity of the window shade layer.
-
-#### Field: ThermalAbsorptance
-
-Emissivity of the window shade layer (assumed same for front and back faces).
-
-#### Field: SolarTransmittance
-
-Transmittance of the window shade layer averaged over the solar spectrum. Assumed same for beam solar radiation and diffuse solar radiation. Transmittance of beam solar radiation is assumed to be independent of angle of incidence.
-
-#### Field: VisibleTransmittance
-
-Transmittance of the window shade layer averaged over the solar spectrum and weighted by the response of the human eye. Assumed same for beam visible radiation and diffuse visible radiation. Transmittance of beam visible radiation is assumed to be independent of angle of incidence.
-
-#### Field: ShadeReflectance
-
-Reflectance of the window shade layer averaged over the solar spectrum. Assumed same for beam solar radiation and diffuse solar radiation. Reflectance of beam solar radiation is assumed to be independent of angle of incidence. Reflectance is assumed to be the same for the front and back faces of the shade layer.
-
-### Material:WindowBlind
-
-This will be filled with the constant “Material:WindowBlind� for each material of this type in the construction.
-
-#### Field: &lt;Material:WindowBlind&gt;
-
-#### Field: Material Name
-
-Name of the blind layer.
-
-#### Field: SlatWidth {m}
-
-Width of the slats in the blind.
-
-#### Field: SlatSeparation {m}
-
-Distance between the centerline of adjacent slats.
-
-#### Field: SlatThickness {m}
-
-Distance between front and back faces of a slat.
-
-#### Field: SlatAngle {deg}
-
-This is the angle between the glazing outward normal and the slat outward normal, where the outward normal points away from the front face of the slat.
-
-#### Field: SlatBeamSolarTransmittance
-
-The beam solar transmittance of the slat at normal incidence. Any transmitted beam radiation is assumed to be 100% diffuse (i.e., slats are translucent). Transmittance is assumed to have the same value at other angles of incidence.
-
-#### Field: SlatBeamSolarFrontReflectance
-
-The beam solar reflectance at normal incidence on the front side of the slat. Assumed to have the same value at other angles of incidence (matte finish).
-
-#### Field: BlindToGlassDistance {m}
-
-Distance from the mid-plane of the blind to the adjacent glass (m).
-
-#### Material:WindowScreen
-
-#### Field:  &lt;Material:WindowScreen&gt;
-
-This will be filled with the constant “Material:WindowScreen� for each material of this type in the construction.
-
-#### Field: Material Name
-
-Name of the window screen layer.
-
-#### Field: Thickness {m}
-
-Thickness of the window screen layer (screen material diameter).
-
-#### Field: Conductivity {w/m-K}
-
-Thermal conductivity of the window screen layer. This is the effective value for the overall screen “assembly� including open spaces between the screen material.
-
-#### Field: ThermalAbsorptance
-
-Emissivity of the window screen layer (assumed same for front and back faces). This is the effective value for the overall screen “assembly� including open spaces between the screen material.
-
-#### Field: Transmittance
-
-Beam transmittance of the window screen layer including any inward reflections from the material surface if specified (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method). This is the effective value for the overall screen “assembly� including open spaces between the screen material. The value reported here is for direct normal incidence.
-
-#### Field: Reflectance
-
-Solar reflectance (beam-to-diffuse) of the window screen layer accounting for inward-reflected beam solar radiation as specified (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method). This is the effective value for the overall screen “assembly� including open spaces between the screen material averaged over the solar spectrum. The value reported here is for direct normal incidence.
-
-#### Field: VisibleReflectance
-
-Visible reflectance (beam-to-diffuse) of the window screen layer accounting for inward-reflected beam solar radiation as specified (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method). This is the effective value for the overall screen “assembly� including open spaces between the screen material averaged over the solar spectrum and weighted by the response of the human eye. The value reported here is for direct normal incidence.
-
-#### Field: DiffuseReflectance
-
-Solar reflectance (diffuse-to-diffuse) of the window screen layer accounting for inward-reflected beam solar radiation as specified (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method). Reflectance of diffuse solar radiation is considered constant and applies to both the front and back surfaces of the screen. Diffuse reflectance is calculated by the model as an average value by integrating the screen’s solar reflectance (beam-to-diffuse) over a quarter hemisphere of incident radiation.
-
-#### Field: DiffuseVisibleReflectance
-
-Visible reflectance (diffuse-to-diffuse) of the window screen layer accounting for inward-reflected beam solar radiation as specified (i.e., Material: WindowScreen, field Reflected Beam Transmittance Accounting Method). Visible reflectance of diffuse solar radiation is considered constant and applies to both the front and back surfaces of the screen. Diffuse visible reflectance is calculated by the model as an average value by integrating the screen’s visible beam reflectance (beam-to-diffuse) over a quarter hemisphere of incident radiation.
-
-#### Field: ScreenMaterialDiameterToSpacingRatio
-
-The aspect ratio of the screen material. The aspect ratio is calculated as the ratio of the screen material diameter to screen material spacing.
-
-#### Field: ScreenToGlassDistance {m}
-
-Distance from the mid-plane of the screen to the adjacent glass (m).
-
-### ThermoChromic Windows
-
-Windows with Thermochromic constructions are reported similarly to other window constructions. First, you see the window as entered in the IDF:
-
-WindowConstruction,TCWINDOW,   5,VerySmooth,   1.666,   0.429,   0.242,   0.520
-
- WindowMaterial:Glazing,CLEAR3PPG,Spectral,CLEAR3PPGSP,  0.00328,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.84000,  0.84000,  1.00000,  1.00000,No
-
- WindowMaterial:Gas,AIR 3MM,Air,  3.000E-03,
-
- WindowMaterial:Glazing,WO18RT25,Spectral,WO18RT25SP,  0.00750,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.84000,  0.84000,  0.60000,  1.00000,No
-
- WindowMaterial:Gas,AIR 8MM,Air,  8.000E-03,
-
- WindowMaterial:Glazing,SB60CLEAR3PPG,Spectral,SB60CLEAR3PPGSP,  0.00328,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.03500,  0.84000,  1.00000,  1.00000,No
-
-Then, there will be a list of window constructions reported with each one corresponding to a particular temperature of the thermochromic glazing layer. For example, the following excerpt shows a list of window constructions for the thermochromic window TCWINDOW at different temperature of the thermochromic layer - TCWINDOW\_TC\_25 at 25°C, TCWINDOW\_TC\_27 at 27°C, and TCWINDOW\_TC\_29 at 29°C. Detailed properties of the thermochromic glazing layer are also listed for each temperature - WO18RT25 **at** 25°C, WO18RT27 **at** 27°C, and WO18RT29 **at** 29°C.
-
-WindowConstruction,TCWINDOW\_TC\_25,   5,VerySmooth,   1.666,   0.429,   0.242,   0.520
-
- WindowMaterial:Glazing,CLEAR3PPG,Spectral,CLEAR3PPGSP,  0.00328,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.84000,  0.84000,  1.00000,  1.00000,No
-
- WindowMaterial:Gas,AIR 3MM,Air,  3.000E-03,
-
- WindowMaterial:Glazing,WO18RT25,Spectral,WO18RT25SP,  0.00750,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.84000,  0.84000,  0.60000,  1.00000,No
-
- WindowMaterial:Gas,AIR 8MM,Air,  8.000E-03,
-
- WindowMaterial:Glazing,SB60CLEAR3PPG,Spectral,SB60CLEAR3PPGSP,  0.00328,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.03500,  0.84000,  1.00000,  1.00000,No
-
-
-
- WindowConstruction,TCWINDOW\_TC\_27,   5,VerySmooth,   1.666,   0.424,   0.236,   0.504
-
- WindowMaterial:Glazing,CLEAR3PPG,Spectral,CLEAR3PPGSP,  0.00328,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.84000,  0.84000,  1.00000,  1.00000,No
-
- WindowMaterial:Gas,AIR 3MM,Air,  3.000E-03,
-
- WindowMaterial:Glazing,WO18RT27,Spectral,WO18RT27SP,  0.00750,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.84000,  0.84000,  0.60000,  1.00000,No
-
- WindowMaterial:Gas,AIR 8MM,Air,  8.000E-03,
-
- WindowMaterial:Glazing,SB60CLEAR3PPG,Spectral,SB60CLEAR3PPGSP,  0.00328,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.03500,  0.84000,  1.00000,  1.00000,No
-
-
-
- WindowConstruction,TCWINDOW\_TC\_29,   5,VerySmooth,   1.666,   0.419,   0.230,   0.490
-
- WindowMaterial:Glazing,CLEAR3PPG,Spectral,CLEAR3PPGSP,  0.00328,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.84000,  0.84000,  1.00000,  1.00000,No
-
- WindowMaterial:Gas,AIR 3MM,Air,  3.000E-03,
-
- WindowMaterial:Glazing,WO18RT29,Spectral,WO18RT29SP,  0.00750,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.84000,  0.84000,  0.60000,  1.00000,No
-
- WindowMaterial:Gas,AIR 8MM,Air,  8.000E-03,
-
- WindowMaterial:Glazing,SB60CLEAR3PPG,Spectral,SB60CLEAR3PPGSP,  0.00328,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.00000,  0.03500,  0.84000,  1.00000,  1.00000,No
-
-### Complex Fenestration
-
-Complex fenestration is reported in a similar manner as other windows.  The first line is the header, followed by details about each fenestration object (window).
-
- ! &lt;WindowConstruction:Complex&gt;,Construction Name,Index,\#Layers,U-factor {W/m2-K},SHGC
-
- WindowConstruction:Complex,CFS\_GLZ\_813,6,4,0.544,9.104E-002
-
- WindowConstruction:Complex,CFS\_GLZ\_2015,7,3,1.777,9.205E-002
-
- WindowConstruction:Complex,CFS\_GLZ\_2046,8,3,2.418,9.273E-002
-
- WindowConstruction:Complex,CFS\_GLZ\_2001,9,3,1.989,9.253E-002
-
-#### Field: Construction Name
-
-Name of the complex fenestration construction.
-
-#### Field: Index
-
-Index number in construction data.
-
-#### Field: \#Layers
-
-Number of solid layers in the complex fenestration construction.  This number accounts for glass and shading layers.
-
-#### Field: U-factor
-
-Complex fenestration U-factor according to ASHRAE winter conditions.
-
-#### Field: SHGC
-
-Complex fenestration solar heat gain coefficient according to ASHRAE summer conditions.
-
-### HAMT Cell Data
-
-This gives the surface name,the construction name, the origins and cell numbers of the cells used within the HAMT solutions algorithm. The cell numbering starts from the external surface to the internal surface.
-
-! &lt;HAMT origins&gt;, Surface Name, Construction Name, Cell origins (m)
-
-! &lt;HAMT cells&gt;, Surface Name, Construction Name, Cell Numbers
-
-HAMT origins,SOUTH WALL,EXTERIOR WALL, 0.0000000, 0.0005729,
-
-0.0026459, 0.0060000, 0.0093541, 0.0114271, 0.0128076, 0.0159588,
-
-0.0219528, 0.0302028, 0.0399012, 0.0500988, 0.0597972, 0.0680472,
-
-0.0740412, 0.0771924, 0.0785729, 0.0806459, 0.0840000, 0.0873541,
-
-0.0894271, 0.0900000
-
-HAMT cells, SOUTH WALL,EXTERIOR
-
-WALL,   1,   2,   3,   4,   5,   6,   7,   8,   9,  10,  11,  12,
-
-13,  14,  15,  16,  17,  18,  19,  20,  21,  22
-
-#### Field: Surface Name
-
-Name of the Surface.
-
-#### Field: Construction Name
-
-Name of the construction.
-
-#### Field: Cell origins
-
-Origins of the Cells.
-
-#### Field: Cell Numbers
-
-Numbers for the Cells.
-
-### Sizing Information
-
-The sizing information in the .eio file reflects the inputs and results for the zone, system and plant (component). Actual fields/details included depend on the “autosize� inputs.
-
-#### Timesteps in Zone Design Calculation
-
-**! &lt;Load Timesteps in Zone Design Calculation Averaging Window&gt;, Value**
-
- Load Timesteps in Zone Design Calculation Averaging Window,    1
-
-#### Field: Load Timesteps in Zone Design Calculation Averaging Window
-
-The number of load timesteps in the zone design flow sequence averaging window. The default is 1, in which case the calculated zone design flow rates are averaged over the load timestep.
-
-The zone design air flow rate calculation is performed assuming a potentially infinite supply of heating or cooling air at a fixed temperature. Thus, the calculated design air flow rate will always be able to meet any load or change in load no matter how large or abrupt. In reality air flow rates are limited by duct sizes and fan capacities. The idealized zone design flow calculation may result in unrealistically large flow rates, especially if the user is performing the sizing calculations using thermostat schedules with night setup or setback. The calculated zone design flow rates are always averaged over the load timestep. The user may want to perform a broader average to mitigate the effect of thermostat setup and setback and prevent the warm up or cool down flow rates from dominating the design flow rate calculation. Specifying the width of the averaging window allows the user to do this.
-
-For example, if the load calculation timestep is 15 minutes and the user specifies the *timesteps in averaging window*to be 4, the zone design air flows will be averaged over a time period of 1 hour. Specifying 8 would result in averaging over a 2 hour period.
-
-#### Sizing Factor Information
-
-**! &lt;Sizing Factor Information&gt;, Sizing Factor ID, Value**
-
-Sizing Factor Information, Global,   1.3000
-
- Sizing Factor Information, Zone SPACE1-1,   1.3000
-
- Sizing Factor Information, Zone SPACE2-1,   1.3000
-
- Sizing Factor Information, Zone SPACE3-1,   1.3000
-
- Sizing Factor Information, Zone SPACE4-1,   1.3000
-
- Sizing Factor Information, Zone SPACE5-1,   1.3000
-
-#### Field: Sizing Factor ID
-
-Sizing factors can be entered in two places: Sizing Parameters, Zone Sizing. If entered in the Sizing Parameters statement, the Sizing Factor ID is “Global� (applied to all if not specified). If entered in the Zone Sizing statement, the Zone and Zone Name designation are shown.
-
-This sizing factor ratio is applied at the zone level to all of the zone heating and cooling loads and air flow rates. These new loads and air flow rates are then used to calculate the system level flow rates and capacities and are used in all of the component sizing calculations.
-
-#### Field: Value
-
-This is the sizing factor ratio to be applied as described previously.
-
-### Zone Sizing Information
-
-! &lt;Zone Sizing Information&gt;, Zone Name, Load Type, Calc Des Load {W}, User Des Load {W}, Calc Des Air Flow Rate {m3/s}, User Des Air Flow Rate {m3/s}, Design Day Name, Date/Time of Peak, Temperature at Peak {C}, Humidity Ratio at Peak {kgWater/kgAir}, Floor Area {m2}, \# Occupants, Calc Outdoor Air Flow Rate {m3/s}
-
- Zone Sizing Information, SPACE1-1, Cooling, 2502.43786, 3253.16922, 0.21023, 0.27329, CHICAGO ANN CLG 1% CONDNS DB=&gt;MWB, 7/21 16:00:00, 30.85800, 1.45947E-002, 99.16000, 11.00000, 0.10384
-
- Zone Sizing Information, SPACE1-1, Heating, 2606.90880, 3388.98144, 7.56806E-002, 0.10384, CHICAGO ANN HTG 99% CONDNS DB, 1/21 23:45:00, -17.30000, 8.38927E-004, 99.16000, 11.00000, 0.10384
-
- Zone Sizing Information, SPACE2-1, Cooling, 2038.79983, 2650.43978, 0.17125, 0.22263, CHICAGO ANN CLG 1% CONDNS DB=&gt;MWB, 7/21 10:15:00, 27.83525, 1.45947E-002, 42.73500, 5.00000, 4.72000E-002
-
- Zone Sizing Information, SPACE2-1, Heating, 1149.09174, 1493.81926, 3.33591E-002, 4.72000E-002, CHICAGO ANN HTG 99% CONDNS DB, 1/21 24:00:00, -17.30000, 8.38927E-004, 42.73500, 5.00000, 4.72000E-002
-
- Zone Sizing Information, SPACE3-1, Cooling, 2318.10750, 3013.53976, 0.19473, 0.25315, CHICAGO ANN CLG 1% CONDNS DB=&gt;MWB, 7/21 15:00:00, 31.50000, 1.45947E-002, 96.48000, 11.00000, 0.10384
-
- Zone Sizing Information, SPACE3-1, Heating, 2589.95436, 3366.94067, 7.51884E-002, 0.10384, CHICAGO ANN HTG 99% CONDNS DB, 1/21 23:30:00, -17.30000, 8.38927E-004, 96.48000, 11.00000, 0.10384
-
- Zone Sizing Information, SPACE4-1, Cooling, 2325.33534, 3022.93594, 0.19534, 0.25394, CHICAGO ANN CLG 1% CONDNS DB=&gt;MWB, 7/21 17:30:00, 29.46700, 1.45947E-002, 42.73500, 5.00000, 4.72000E-002
-
- Zone Sizing Information, SPACE4-1, Heating, 1143.87745, 1487.04068, 3.32077E-002, 4.72000E-002, CHICAGO ANN HTG 99% CONDNS DB, 1/21 23:30:00, -17.30000, 8.38927E-004, 42.73500, 5.00000, 4.72000E-002
-
- Zone Sizing Information, SPACE5-1, Cooling, 2589.39474, 3366.21317, 0.21753, 0.28279, CHICAGO ANN CLG 1% CONDNS DB=&gt;MWB, 7/21 15:00:00, 31.50000, 1.45947E-002, 182.49000, 20.00000, 0.18880
-
- Zone Sizing Information, SPACE5-1, Heating, 1706.17191, 2218.02348, 4.95314E-002, 0.18880, CHICAGO ANN HTG 99% CONDNS DB, 1/21 23:45:00, -17.30000, 8.38927E-004, 182.49000, 20.00000, 0.18880
-
-#### Field: &lt;Zone Sizing Information&gt;
-
-This field just contains “Zone Sizing Information�.
-
-#### Field: Zone Name
-
-This field contains the Zone Name.
-
-#### Field: Load Type
-
-This field specifies which kind of load is being sized – Heating or Cooling.
-
-#### Field: Calc Des Load {W}
-
-The unaltered zone load resulting from the zone sizing calculations, using the design weather and schedules specified in the input.
-
-#### Field: User Des Load {W}
-
-User Des Load is the load after user specified adjustments and is the load actually used for sizing components. Following the calculations (as in the previous field) various adjustments can be made based on user input - the most obvious is a sizing factor; but it could also be something like cooling min air flow per zone area or just a user input design flow rate.
-
-#### Field: Calc Des Air Flow Rate {m3/s}
-
-This is the calculated design air flow rate in m3/s. The calculated design air flow rate is the "non-adjusted" air flow rate. It is the air flow rate sufficient to meet the zone loads from the design day simulation.
-
-#### Field: User Des Air Flow Rate {m3/s}
-
-User Des Air Flow Rate is the flow rate after user specified adjustments and is the flow rate actually used for sizing components. Following the calculations (as in the previous field) various adjustments can be made based on user input - the most obvious is a sizing factor; but it could also be something like cooling min air flow per zone area or just a user input design flow rate.
-
-#### Field: Design Day Name
-
-This is the name of the design day or design run period that triggered the sizing calculations.
-
-#### Field: Date/Time of Peak
-
-This is the date and time of the peak load (used for the sizing calculations).
-
-#### Field: Temperature at Peak {C}
-
-This is the temperature (outdoor dry-bulb) at the time of the peak load.
-
-#### Field: Humidity Ratio at Peak {kgWater/kgAir}
-
-This is the humidity ratio (outdoor) at the time of the peak load.
-
-#### Field: Floor Area {m2}
-
-This is the floor area of the zone.
-
-#### Field: \# Occupants
-
-This is the number of occupants in the zone.
-
-#### Field: Calc Outdoor air Flow Rate {m3/s}
-
-This is the calculated outdoor air flow rate.
-
-### System Sizing Information
-
-**! &lt;System Sizing Information&gt;, System Name, Field Description, Value**
-
- System Sizing Information, VAV SYS 1, Calculated Cooling Design Air Flow Rate [m3/s], 1.05725
-
- System Sizing Information, VAV SYS 1, User Cooling Design Air Flow Rate [m3/s], 1.05725
-
- System Sizing Information, VAV SYS 1, Calculated Heating Design Air Flow Rate [m3/s], 0.43343
-
- System Sizing Information, VAV SYS 1, User Heating Design Air Flow Rate [m3/s], 0.43343
-
-#### Field: &lt;System Sizing Information&gt;
-
-This field just contains “System Sizing Information�.
-
-#### Field: System Name
-
-This field contains the system (Air Loop) name.
-
-#### Field: Field Description
-
-This contains the field description and units.
-
-#### Field: Value
-
-This contains the value of the field.
-
-***Note:*** "Calculated" values are the unaltered result of the system sizing calculations, using the design day weather and schedules given in the input. "User" values are the calculated values altered by various user inputs in Sizing:Zone and Sizing:System. For instance, sizing factors will alter the calculated values. Another example would be using the *flow/system* method to specify a system design flow rate.
-
-### Plant Coincident Sizing Algorithm
-
-A special report is issued to the eio file that provides details for the Coincident sizing option.  Coincident plant sizing adjustments using HVAC Sizing Simulations run a sizing algorithm at the end of each Sizing Pass.  The following report provides details on the calculations and observations from monitoring the previous Sizing Pass. 
-
-    ! <Plant Coincident Sizing Algorithm>,Plant Loop Name,Sizing Pass {#},Measured Mass Flow{kg/s},Measured Demand {W},Demand Calculated Mass Flow{kg/s},Sizes Changed {Yes/No},Previous Volume Flow Rate {m3/s},New Volume Flow Rate {m3/s},Demand Check Applied {Yes/No},Sizing Factor {},Normalized Change {},Specific Heat{J/kg-K},Density {kg/m3}
-    Plant Coincident Sizing Algorithm,HOT WATER LOOP,1,0.1062471,11942.67,0.2586269,Yes,7.324432E-004,2.586533E-004,Yes,1.0000,0.646862,4197.9300,999.8980
-    Plant Coincident Sizing Algorithm,CHILLED WATER LOOP,1,1.1222815,17614.26,0.6290764,Yes,1.197307E-003,1.122396E-003,No,1.0000,6.256652E-002,4197.9300,999.8980
-
-#### Field: <Plant Coincident Sizing Algorithm>
-
-This field simply contains the words “Plant Sizing Coincident Flow Algorithm.� 
-
-#### Field: Plant Loop Name
-
-This field shows the name of the plant loop being analyzed.
-
-#### Field: Sizing Pass #
-
-This field shows which sizing pass has just completed prior to running the sizing algorithm.  Each Sizing Pass is an iteration of a set of HVAC Sizing Simulations. 
-
-#### Field: Measured Mass Flow {kg/s}
-
-This is the maximum coincident mass flow rate, in kg/s, found at the supply side inlet system node. This was recorded by a data logging system tracking node mass flow rate over all the sizing periods.  It will include any zone timestep averaging. 
-
-#### Field: Measured Demand {W}
-
-This is the maximum loop coincident demand, in W, on the supply side.  This was recorded by a data logging system tracking the report value for loop demand over all the sizing periods.  It will include and zone timestep averaging. 
-
-#### Field: Demand Calculated Mass Flow {kg/s}
-
-This is the flow rate, in kg/s, that was calculated from measured demand, the temperature difference in the plant sizing object, and the fluid specific heat.   
-
-#### Field: Sizes Changed {Yes/No}
-
-This field indicates if the sizing algorithm resulted in a change of size.  If the flows did not change significantly, the sizes might not change. 
-
-#### Field: Previous Volume Flow Rate {m3/s}
-
-This field is the prior size of the plant loop, in m3/s.  This is the size before the adjustment if the size changes. 
-
-#### Field: New Volume Flow Rate {m3/s}
-
-This field is the result of the sizing algorithm, in m3/s.  If the size changes, this is the new value used for the plant loop maximum volume flow rate. 
-
-#### Field: Demand Check Applied {Yes/No}
-
-This field indicates if the algorithm produced a new mass flow rate from the measured demand or not.  If this field is “No,� then the algorithm used coincident mass flow.  If this field is “Yes,� then the mass flow derived from demand was larger than the measured mass flow and the demand drove the result. 
-
-#### Field: Sizing Factor { }
-
-This field is the value of the sizing factor applied to the measured or calculated coincident flows.  
-
-#### Field: Normalized Change { }
-
-This field is the normalized change used to determine if the new flow size is significantly different from the previous. 
-
-#### Field: Specific Heat {J/kg-K }
-
-This is the fluid specific heat, in J/kg-K, used in the calculation of mass flow from the maximum coincident demand.
-
-#### Field: Density {kg/m3}
-
-This is the fluid density , in kg/m3, used in the calculation of volume flow rate from the mass flow rate.
-
-
-### Component Sizing Information
-
-Component sizing is applicable to all manners of autosized components and equipments (coils, boilers, chillers, towers, humidifiers, namely – whatever can be autosized)
-
-**! &lt;Component Sizing Information&gt;, Component Type, Component Name, Input Field Description, Value**
-
- Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE1-1 VAV REHEAT, Maximum Air Flow Rate [m3/s], 0.22672
-
- Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE1-1 VAV REHEAT, Maximum Reheat Water Flow Rate [m3/s], 5.87104E-005
-
- Component Sizing Information, Coil:Heating:Water, SPACE1-1 ZONE COIL, Maximum Water Flow Rate [m3/s], 5.87104E-005
-
- Component Sizing Information, Coil:Heating:Water, SPACE1-1 ZONE COIL, Design Coil Load [W], 2699.50304
-
- Component Sizing Information, Coil:Heating:Water, SPACE1-1 ZONE COIL, U-Factor Times Area Value [W/K], 66.15122
-
- Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE2-1 VAV REHEAT, Maximum Air Flow Rate [m3/s], 0.17666
-
- Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE2-1 VAV REHEAT, Maximum Reheat Water Flow Rate [m3/s], 4.57480E-005
-
- Component Sizing Information, Coil:Heating:Water, SPACE2-1 ZONE COIL, Maximum Water Flow Rate [m3/s], 4.57480E-005
-
- Component Sizing Information, Coil:Heating:Water, SPACE2-1 ZONE COIL, Design Coil Load [W], 2103.49527
-
- Component Sizing Information, Coil:Heating:Water, SPACE2-1 ZONE COIL, U-Factor Times Area Value [W/K], 51.54607
-
- Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE3-1 VAV REHEAT, Maximum Air Flow Rate [m3/s], 0.20944
-
- Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE3-1 VAV REHEAT, Maximum Reheat Water Flow Rate [m3/s], 5.42362E-005
-
- Component Sizing Information, Coil:Heating:Water, SPACE3-1 ZONE COIL, Maximum Water Flow Rate [m3/s], 5.42362E-005
-
- Component Sizing Information, Coil:Heating:Water, SPACE3-1 ZONE COIL, Design Coil Load [W], 2493.78307
-
- Component Sizing Information, Coil:Heating:Water, SPACE3-1 ZONE COIL, U-Factor Times Area Value [W/K], 61.11006
-
- Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE4-1 VAV REHEAT, Maximum Air Flow Rate [m3/s], 0.22257
-
- Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE4-1 VAV REHEAT, Maximum Reheat Water Flow Rate [m3/s], 5.76351E-005
-
- Component Sizing Information, Coil:Heating:Water, SPACE4-1 ZONE COIL, Maximum Water Flow Rate [m3/s], 5.76351E-005
-
- Component Sizing Information, Coil:Heating:Water, SPACE4-1 ZONE COIL, Design Coil Load [W], 2650.06093
-
- Component Sizing Information, Coil:Heating:Water, SPACE4-1 ZONE COIL, U-Factor Times Area Value [W/K], 64.93964
-
- Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE5-1 VAV REHEAT, Maximum Air Flow Rate [m3/s], 0.22187
-
- Component Sizing Information, AirTerminal:SingleDuct:VAV:Reheat, SPACE5-1 VAV REHEAT, Maximum Reheat Water Flow Rate [m3/s], 5.74541E-005
-
- Component Sizing Information, Coil:Heating:Water, SPACE5-1 ZONE COIL, Maximum Water Flow Rate [m3/s], 5.74541E-005
-
- Component Sizing Information, Coil:Heating:Water, SPACE5-1 ZONE COIL, Design Coil Load [W], 2641.74210
-
- Component Sizing Information, Coil:Heating:Water, SPACE5-1 ZONE COIL, U-Factor Times Area Value [W/K], 64.73579
-
- Component Sizing Information, Branch, VAV SYS 1 MAIN BRANCH, Maximum Flow Rate [m3/s], 1.05725
-
- Component Sizing Information, AirLoopHVAC, VAV SYS 1, Design Supply Air Flow Rate [m3/s], 1.05725
-
- Component Sizing Information, Controller:OutdoorAir, OA CONTROLLER 1, Maximum Outdoor Air Flow Rate [m3/s], 1.05725
-
- Component Sizing Information, Controller:OutdoorAir, OA CONTROLLER 1, Minimum Outdoor Air Flow Rate [m3/s], 0.26412
-
- Component Sizing Information, Coil:Heating:Water, OA HEATING COIL 1, Maximum Water Flow Rate [m3/s], 1.48158E-004
-
- Component Sizing Information, Coil:Heating:Water, OA HEATING COIL 1, Design Coil Load [W], 6812.28921
-
- Component Sizing Information, Coil:Heating:Water, OA HEATING COIL 1, U-Factor Times Area Value [W/K], 84.72044
-
- Component Sizing Information, Coil:Cooling:Water, OA COOLING COIL 1, Design Water Flow Rate [m3/s], 1.14523E-003
-
- Component Sizing Information, Coil:Cooling:Water, OA COOLING COIL 1, Design Air Flow Rate [m3/s], 0.26412
-
- Component Sizing Information, Coil:Cooling:Water, OA COOLING COIL 1, Design Inlet Air Temperature [C], 30.01375
-
- Component Sizing Information, Coil:Cooling:Water, OA COOLING COIL 1, Design Outlet Air Humidity Ratio, 8.00000E-003
-
- Component Sizing Information, Coil:Cooling:Water, MAIN COOLING COIL 1, Design Inlet Air Humidity Ratio, 9.33031E-003
-
- Component Sizing Information, Coil:Cooling:Water, MAIN COOLING COIL 1, Design Outlet Air Humidity Ratio, 8.00000E-003
-
- Component Sizing Information, Coil:Cooling:DX:TwoStageWithHumidityControlMode, ACDXCOIL 2:ACDXCOIL 2 STANDARD MODE-STAGE 1, Rated Air Flow Rate [m3/s], 2.04925
-
- Component Sizing Information, Coil:Heating:Water, MAIN HEATING COIL 1, Maximum Water Flow Rate [m3/s], 7.51969E-005
-
- Component Sizing Information, Coil:Heating:Water, MAIN HEATING COIL 1, Design Coil Load [W], 3457.55329
-
- Component Sizing Information, Coil:Heating:Water, MAIN HEATING COIL 1, U-Factor Times Area Value [W/K], 55.78870
-
- Component Sizing Information, Fan:VariableVolume, SUPPLY FAN 1, Maximum Flow Rate [m3/s], 1.05725
-
- Component Sizing Information, Fan:VariableVolume, SUPPLY FAN 1, Minimum Flow Rate [m3/s], 0.35326
-
- Component Sizing Information, Controller:WaterCoil, OA CC CONTROLLER 1, Maximum Actuated Flow [m3/s], 1.14523E-003
-
- Component Sizing Information, Controller:WaterCoil, OA HC CONTROLLER 1, Maximum Actuated Flow [m3/s], 1.48158E-004
-
- Component Sizing Information, Controller:WaterCoil, CENTRAL COOLING COIL CONTROLLER 1, Maximum Actuated Flow [m3/s], 9.16309E-004
-
- Component Sizing Information, Controller:WaterCoil, CENTRAL HEATING COIL CONTROLLER 1, Maximum Actuated Flow [m3/s], 7.51969E-005
-
- Component Sizing Information, PlantLoop, HOT WATER LOOP, Maximum Loop Flow Rate [m3/s], 4.97138E-004
-
- Component Sizing Information, PlantLoop, HOT WATER LOOP, Plant Loop Volume [m3], 0.55928
-
- Component Sizing Information, PlantLoop, CHILLED WATER LOOP, Maximum Loop Flow Rate [m3/s], 2.06154E-003
-
- Component Sizing Information, PlantLoop, CHILLED WATER LOOP, Plant Loop Volume [m3], 2.31923
-
- Component Sizing Information, Chiller:Electric, CENTRAL CHILLER, Nominal Capacity [W], 34468.93699
-
- Component Sizing Information, Chiller:Electric, CENTRAL CHILLER, Design Chilled Water Flow Rate [m3/s], 2.06154E-003
-
- Component Sizing Information, Boiler:HotWater, CENTRAL BOILER, Nominal Capacity [W], 22858.42690
-
- Component Sizing Information, Boiler:HotWater, CENTRAL BOILER, Design Water Flow Rate [m3/s], 4.97138E-004
-
- Component Sizing Information, Pump:VariableSpeed, HW CIRC PUMP, Rated Flow Rate [m3/s], 4.97138E-004
-
- Component Sizing Information, Pump:VariableSpeed, HW CIRC PUMP, Rated Power Consumption [W], 127.01247
-
- Component Sizing Information, Pump:VariableSpeed, CW CIRC PUMP, Rated Flow Rate [m3/s], 2.06154E-003
-
- Component Sizing Information, Pump:VariableSpeed, CW CIRC PUMP, Rated Power Consumption [W], 526.69672
-
- Component Sizing Information, Humidifier:Steam:Electric, HUMIDIFIER 1, Rated Power [W], 9826.56303
-
- Component Sizing Information, Humidifier:Steam:Gas, MAIN GAS HUMIDIFIER, Design Size Nominal Capacity Volume [m3/s], 1.05405E-002
- 
- Component Sizing Information, Humidifier:Steam:Gas, MAIN GAS HUMIDIFIER, Design Size Rated Power [W], 103710.42776
-
-#### Field: &lt;Component Sizing Information&gt;
-
-This field simply contains the words “Component Sizing�.
-
-#### Field:  Component Type
-
-This field shows the component type (e.g. Pump:Variable Speed, Plant Loop, Fan:Simple:VariableVolume) being sized.
-
-#### Field:  Component Name
-
-This field shows the name of the component.
-
-#### Field:  Input Field Description
-
-This field shows the field description/variable with units.  When using HVAC Sizing Simulation for advanced sizing methods, there are two versions of the report for each component that might be affected.  With HVAC Sizing Simulation, there is a first size value reported, which is the result of the Ideal Loads Sizing Simulation, and there is the final value after all the Sizing Passes have completed.  This input field description will have “Initial� prepended to the description to indicate that this is the first size, the same report without “Initial� is the final size. Note that with HVAC Sizing Simulation, these reports will occur much later in the simulation and hence appear further down in the .eio file.
-
-#### Field:  Value
-
-This field shows the value of the sized component.
-
-### Heating/Cooling Coil Capacity Information
-
-Water heating coils appear:
-
-! &lt;Water Heating Coil Capacity Information&gt;,Component Type,Name,Nominal Total Capacity {W}
-
-Water Heating Coil Capacity Information,Coil:Heating:Water,BASEMENT VAV BOX REHEAT COIL,66543.21
-
-#### Field: &lt;Water Heating Coil Capacity Information&gt;
-
-This field simply contains the words “Water Heating Coil Capacity Information�.
-
-#### Field: Component Type
-
-This field contains the component type (e.g. Coil:Heating:Water).
-
-#### Field: Component Name
-
-This field contains the user supplied name for the coil.
-
-#### Field: Nominal Total Capacity {W}
-
-This field contains the nominal heating capacity of the coil in Watts. The capacity is calculated using the rated inlet conditions: inlet air dry bulb temperature = 16.6C, inlet relative humidity = 50%, inlet hot water temperature = 82.2C.
-
-! &lt;Water Cooling Coil Capacity Information&gt;,Component Type, Name, Nominal Total Capacity {W},Nominal Sensible Capacity {W},Nominal Latent Capacity {W},Nominal Sensible Heat Ratio, Nominal Coil UA Value {W/C}, Nominal Coil Surface Area {m2}
-
-Water Cooling Coil Capacity Information, Coil:Cooling:Water, MAIN COOLING COIL 1,37219.64,24969.42,12250.22,0.67,4202.30,42.62
-
-#### Field: &lt;Water Cooling Coil Capacity Information&gt;
-
-This field simply contains the words “Water Cooling Coil Capacity Information�.
-
-#### Field: Component Type
-
-This field contains the component type (e.g. Coil:Cooling:Water).
-
-#### Field: Component Name
-
-This field contains the user supplied name for the coil.
-
-#### Field: Nominal Total Capacity {W}
-
-This field contains the nominal cooling capacity of the coil in Watts.
-
-#### Field: Nominal Sensible Capacity {W}
-
-This field contains the nominal sensible cooling capacity of the coil in Watts.
-
-#### Field: Nominal Latent Capacity {W}
-
-This field contains the nominal latent cooling capacity of the coil in Watts.
-
-#### Field: Nominal Sensible Heat Ratio Capacity {W}
-
-This field contains the nominal sensible heat ratio (SHR) capacity of the coil in Watts.
-
-#### Field: Nominal UA Value {W/C}
-
-This field contains the nominal cooling coil UA value in Watts per deg C.
-
-#### Field: Nominal Surface Area {m<sup>2</sup>}
-
-This field contains the nominal cooling coil surface area in square meter.
-
-***Note:*** values labeled "Nominal" are calculated using the rated inlet conditions: inlet air dry bulb temperature = 26.67C, inlet air wet bulb temperature = 19.44C, inlet chilled water temperature = 6.67C.
-
-### Refrigerated Case and WalkIn Output
-
-Refrigeration related variables appear in the eio file according to the refrigeration models selected. The total possible header records would show:
-
-! &lt;\#Refrigeration Compressor Racks&gt;,Number of Refrigeration Compressor Racks
-
-! &lt;Refrigeration Compressor Rack&gt;,Compressor Rack Name, \# Refrigerated Cases Connected,\# WalkIn Coolers Connected, Heat Rejection Location, Condenser Type, COP
-
-! &lt;\#Detailed Refrigeration Systems&gt;,Number of Detailed Refrigeration Systems
-
-! &lt;Detailed Refrigeration System&gt;,Refrigeration System Name,Refrigerant Used, \# Refrigerated Cases Connected, \# WalkInCoolers Connected, \#Air Chillers Connected, \# Secondary Loops Served, \# Cascade Condensers Served, \# Mechanical Subcoolers Served, \# Compressors Connected, \# Compression Stages, Intercooler Type, Intercooler Effectiveness, \# Subcoolers Connected, Minimum Condensing Temperature (C)
-
-!  &lt;\#Detailed Transcritical Refrigeration Systems&gt;,Number of Detailed Transcritical Refrigeration Systems
-
-!  &lt;Detailed Transcritical Refrigeration System&gt;,Transcritical Refrigeration System Name, Refrigerant Used, \# Medium Temperature Refrigerated Cases Connected, \# Low Temperature Refrigerated Cases Connected, \# Medium Temperature WalkInCoolers Connected, \# Low Temperature WalkInCoolers Connected, \# High Pressure Compressors Connected, \# Low Pressure Compressors Connected, Minimum Condensing Temperature (C)
-
-! &lt;\#Secondary Refrigeration Systems&gt;,Number of Secondary Refrigeration Systems
-
-! &lt;Secondary Refrigeration System: Fluid Always Liquid&gt;, Secondary Number, Secondary Name, \# Refrigerated Cases Connected, \# WalkIn Coolers Connected, Fluid Name, Capacity (W),Evap Temperature in Secondary Evaporator (C), Approach Temperature Difference (DeltaC), Temperature Range (DeltaC), TotalPumpPower (W)
-
-! &lt;Secondary Refrigeration System: Liquid Overfeed&gt;, Secondary Number, Secondary Name, \# Refrigerated Cases Connected, \# WalkIn Coolers Connected, Fluid Name, Capacity (W),Evap Temperature in Secondary Evaporator (C), Approach Temperature Difference (DeltaC), Circulating Rate, TotalPumpPower (W)
-
-!  &lt;Refrigeration Case&gt;,Refrigeration Case Number, Refrigeration Case Name,Zone Name,Zone Node \#,Zone Node Name,Capacity (W/m),LHR,Temperature (C),Length (m),Fan (W/m),Installed Lighting (W/m),Anti-Sweat (W/m),Defrost (W/m)
-
-!  &lt;Refrigeration Walk In Cooler&gt;, Walk In Number, Walk In Name,Capacity (W),Temperature (C),Coil Fan (W), Circulating Fan (W), Lighting (W),Heaters (W),Defrost (W), \# Zones
-
-!      &lt;Walk-In Surfaces Facing Zone&gt;, ZoneName, Wall/Ceiling Area (m2), UValue (W/m2-C), AreaStockDoors (m2), HeightStockDoors, UValueStockDoors (W/m2-C), AreaGlassDoors (m2), HeightGlassDoors (m),  UValueGlassDoors (W/m2-C)
-
-!  &lt;Refrigeration Compressor&gt;,Compressor Number,Compressor Name,Nominal Capacity (W)
-
-!  &lt;Refrigeration Condenser:Air-Cooled&gt;,Condenser Number,Condenser Name,Rated Condensing Temperature (C),Rated Capacity (W), Rated Fan Power (W)
-
-!  &lt;Refrigeration Condenser:Evaporative-Cooled&gt;,Condenser Number,Condenser Name,Rated Capacity (W), Rated Fan Power (W)
-
-!  &lt;Refrigeration Condenser:Water-Cooled&gt;,Condenser Number,Condenser Name,Rated Condensing Temperature (C),Rated Capacity (W), Rated Water Inlet Temperature (C), Rated Water Flow Rate (m3/s)
-
-!  &lt;Refrigeration Condenser:Cascade&gt;, Condenser Number, Condenser Name, Condensing Temperature Control Type, Rated Condensing Temperature (C), Capacity (W), Approach Temperature Difference (DeltaC)
-
-!  &lt;Refrigeration GasCooler:Air-Cooled&gt;,Gas Cooler Number, Gas Cooler Name, Rated Outlet Pressure (Pa), Rated Outlet Temperature (C), Rated Approach Temperature (C), Rated Capacity (W), Rated Fan Power (W)
-
-!  &lt;Secondary Load&gt;, Secondary System Served Name, Secondary Number
-
-!  &lt;Cascade Load&gt;, System Name Connected, Condenser Number, Condenser Name
-
-!  &lt;Mechanical Subcooler Load&gt;, Subcooler Number, Subcooler Name
-
-!  &lt;Refrigeration Mechanical Subcooler&gt;, Subcooler Number, Subcooler Name, Name of System Providing Cooling, Design Outlet Temperature (C)
-
-!  &lt;Refrigeration Liquid Suction Subcooler&gt;, Subcooler Number, Subcooler Name, Design Subcooling (DeltaC),Design liquid inlet temperature (C), Design vapor inlet temperature (C)
-
-
-
-For example, a supermarket refrigeration system including models for a compressor rack and four detailed systems that include refrigerated cases, walk-ins, subcoolers, air-, water-, and evaporative-cooled condensers, and a secondary loop would show the following data lines following the header lines :
-
-\#Refrigeration Compressor Racks: 1
-
- Refrigeration Compressor Rack,RACKA,4,0,Outdoors,Air-Cooled,  2.500
-
-   Refrigeration Case,1,DELI\_CASE:1\_ MULTIDECKDAIRYANDDELICASE,DELI,76,DELI AIR NODE,  1442.2,   0.30,    2.2,    3.0,   87.6,   38.7,   65.6,    0.0
-
-   Refrigeration Case,3,SALES\_CASE:1\_MEATDISPLAYCASE,SALES,78,SALES AIR NODE,  1442.2,   0.10,    2.2,   33.6,   87.6,   38.7,   65.6,  443.0
-
-   Refrigeration Case,4,SALES\_CASE:2\_ MULTIDECKDIARYANDDELICASE,SALES,78,SALES AIR NODE,  1442.2,   0.30,    2.2,   49.2,   41.0,   60.0,    0.0,    0.0
-
-   Refrigeration Case,10,PRODUCE\_CASE:1\_ MULTIDECKDIARYANDDELICASE,PRODUCE,80,PRODUCE AIR NODE,  1442.2,   0.30,    2.2,   30.0,   41.0,   60.0,    0.0,    0.0
-
-\#Detailed Refrigeration Systems,4
-
- Detailed Refrigeration System,MEDIUMTEMPSYSTEM,R22,3,0,0,0,1,3,0,    25.0
-
-   Refrigeration Case,2,FISHDISPLAYCASE,SALESFLOOR,9,SALESFLOOR NODE,   288.4,   0.10,    1.1,   15.0,    0.0,   41.6,    0.0,    0.0
-
-   Refrigeration Case,5,MEATDISPLAYCASE,SALESFLOOR,9,SALESFLOOR NODE,   456.6,   0.10,   -4.4,   26.0,   47.2,   86.8,   13.2,  585.8
-
-   Refrigeration Case,6,MULTIDECKDAIRYANDDELICASE,SALESFLOOR,9,SALESFLOOR NODE,  1890.0,   0.30,   -1.1,   12.0,   78.7,  307.3,    0.0,    0.0
-
-   Mechanical Subcooler Load, 2,SampleMSC
-
-   Refrigeration Compressor,1,MEDTEMP001CARLYLE\_R-22\_MED\_06DR820,           15535.
-
-   Refrigeration Compressor,2,MEDTEMP002CARLYLE\_R-22\_MED\_06DR820,           15535.
-
-   Refrigeration Compressor,3,MEDTEMP003CARLYLE\_R-22\_MED\_06DR820,           15535.
-
-   Refrigeration Condenser:Air-Cooled,1,MEDIUMTEMPCONDENSER  ,         51.7,      52563.5,       4000.0
-
-Detailed Refrigeration System,LOWTEMPSYSTEM,R22,3,0,0,0,0,3,1,0,0.80,2,    25.0
-
-   Refrigeration Case,7,OPENWELLICECREAMDISPLAYCASE,SALESFLOOR,9,SALESFLOOR NODE,   441.6,   0.08,  -34.4,   14.6,   28.7,   42.7,   70.0,   76.5
-
-   Refrigeration Case,8,GLASSDOORFROZENFOOD,SALESFLOOR,9,SALESFLOOR NODE,   615.8,   0.13,  -23.3,   11.7,   57.9,   99.8,  218.7, 1106.5
-
-   Refrigeration Case,9,WALKINFREEZER,BACKROOM,11,BACKROOM NODE,  1098.0,   0.10,   -2.2,    4.3,  172.2,   28.1,    0.0, 1291.7
-
-   Refrigeration Compressor,4,LOWTEMP001CARLYLE\_R-22\_LOW\_06CC665,           15952.
-
-   Refrigeration Compressor,5,LOWTEMP002CARLYLE\_R-22\_LOW\_06DR718,            2940.
-
-   Refrigeration Compressor,6,LOWTEMP003CARLYLE\_R-22\_LOW\_06DR718,            2940.
-
-   Refrigeration Condenser:Air-Cooled,2,LOWTEMPCONDENSER  ,         51.7,      34875.5,       2600.0
-
-   Refrigeration Mechanical Subcooler,2,SAMPLEMSC,MEDIUMTEMPSYSTEM,    10.0
-
-   Refrigeration Liquid Suction Subcooler,1,SAMPLELSHX,     6.0,    16.0,     0.0
-
- Detailed Refrigeration System,MEDIUMTEMPSYSTEM2,R22,0,0,1,0,0,3,1,0,0.80,0,    25.0
-
-  Secondary Load,SECONDARY,1
-
-   Refrigeration Compressor,7,MEDTEMP004CARLYLE\_R-22\_MED\_06DR820,           15535.
-
-   Refrigeration Compressor,8,MEDTEMP005CARLYLE\_R-22\_MED\_06DR820,           15535.
-
-   Refrigeration Compressor,9,MEDTEMP006CARLYLE\_R-22\_MED\_06DR820,           15535.
-
-   Refrigeration Condenser:Evaporative-Cooled,1,MEDIUMTEMPEVAPCOOLEDCONDENSER1  ,      64800.0,        746.0
-
-
-
- Detailed Refrigeration System,LOWTEMPSYSTEM2,R22,4,1,0,0,0,3,1,0,0.80,0,    25.0
-
-   Refrigeration Case,11,OPENWELLICECREAMDISPLAYCASE2,SALESFLOOR,9,SALESFLOOR NODE,   441.6,   0.08,  -34.4,   14.6,   28.7,   42.7,   70.0,   76.5
-
-   Refrigeration Case,12,GLASSDOORFROZENFOODA,SALESFLOOR,9,SALESFLOOR NODE,   615.8,   0.13,  -23.3,    4.0,   57.9,   99.8,  218.7, 1106.5
-
-   Refrigeration Case,13,GLASSDOORFROZENFOODB,SALESFLOOR,9,SALESFLOOR NODE,   615.8,   0.13,  -23.3,    4.0,   57.9,   99.8,  218.7, 1106.5
-
-   Refrigeration Case,14,GLASSDOORFROZENFOODC,SALESFLOOR,9,SALESFLOOR NODE,   615.8,   0.13,  -23.3,    4.0,   57.9,   99.8,  218.7, 1106.5
-
-   Refrigeration Walk In Cooler,  1,  WALKINFREEZER2,   4690.0,     -2.2,    735.0,      0.0,    120.0,      0.0,   5512.0,      0.0,   1
-
-       Walk-In Surfaces Facing Zone,BACKROOM,     43.4,   0.2350 ,    2.00,     2.00,   0.3785 ,    1.00,     2.00,   1.2050
-
-   Refrigeration Compressor,10,LOWTEMP004CARLYLE\_R-22\_LOW\_06CC665,           15952.
-
-   Refrigeration Compressor,11,LOWTEMP005CARLYLE\_R-22\_LOW\_06DR718,            2940.
-
-   Refrigeration Compressor,12,LOWTEMP006CARLYLE\_R-22\_LOW\_06DR718,            2940.
-
-   Refrigeration Condenser:Water-Cooled,2,LOWTEMPCONDENSERWATER  ,         29.4,      58000.0,          0.0,          0.0
-
-\#Secondary Refrigeration Systems,1
-
- Secondary Refrigeration System: Fluid Always Liquid,1,SECONDARY,3,0,PROGLY30PERCENT, 35000.0, -12.60,    2.7,    4.0,  725.0,
-
-  Refrigeration Case,15,FISHDISPLAYCASE2,SALESFLOOR,9,SALESFLOOR NODE,   288.4,   0.10,    1.1,   15.0,    0.0,   41.6,    0.0,    0.0
-
-  Refrigeration Case,16,MEATDISPLAYCASE2,SALESFLOOR,9,SALESFLOOR NODE,   456.6,   0.10,   -4.4,   26.0,   47.2,   86.8,   13.2,  585.8
-
-  Refrigeration Case,17,MULTIDECKDAIRYANDDELICASE2,SALESFLOOR,9,SALESFLOOR NODE,  1890.0,   0.30,   -1.1,   12.0,   78.7,  307.3,    0.0,    0.0
-
-For a supermarket system including a model for a cascade condenser arrangement, the eio would show:
-
-Detailed Refrigeration System,CASCADELOWTEMPSYSTEM,R22,4,1,0,0,0,3,1,0,0.80,0,    -4.0
-
-   Refrigeration Case,5,OPENWELLICECREAMDISPLAYCASE,SALESFLOOR,10,SALESFLOOR NODE,   441.6,   0.08,  -34.4,   14.6,   28.7,   42.7,   70.0,   76.5
-
-   Refrigeration Case,6,GLASSDOORFROZENFOODA,SALESFLOOR,10,SALESFLOOR NODE,   615.8,   0.13,  -23.3,    4.0,   57.9,   99.8,  218.7, 1106.5
-
-   Refrigeration Case,7,GLASSDOORFROZENFOODB,SALESFLOOR,10,SALESFLOOR NODE,   615.8,   0.13,  -23.3,    4.0,   57.9,   99.8,  218.7, 1106.5
-
-   Refrigeration Case,8,GLASSDOORFROZENFOODC,SALESFLOOR,10,SALESFLOOR NODE,   615.8,   0.13,  -23.3,    4.0,   57.9,   99.8,  218.7, 1106.5
-
-   Refrigeration Walk In Cooler,  1,  WALKINFREEZER,   4690.0,     -2.2,    735.0,      0.0,    120.0,      0.0,   5512.0,      0.0,   1
-
-       Walk-In Surfaces Facing Zone,BACKROOM,     43.4,   0.2350 ,    2.00,     2.00,   0.3785 ,    2.00,     2.00,   1.2050
-
-   Refrigeration Compressor,4,LOWTEMP001CARLYLE\_R-22\_LOW\_06CC665,           16680.
-
-   Refrigeration Compressor,5,LOWTEMP002CARLYLE\_R-22\_LOW\_06DR718,            5523.
-
-   Refrigeration Compressor,6,LOWTEMP003CARLYLE\_R-22\_LOW\_06DR718,            5523.
-
-   Refrigeration Condenser:Cascade,4,CASCADECONDENSER1,Fixed  ,         -4.0,      20000.0,          3.0
-
- Detailed Refrigeration System,CASCADEHIGHTEMPSYSTEM,R22,0,0,0,1,0,4,1,0,0.80,0,    25.0
-
-   Cascade Load,CASCADELOWTEMPSYSTEM,4,CASCADECONDENSER1
-
-   Refrigeration Compressor,7,MEDTEMP005CARLYLE\_R-22\_MED\_06DR820,           17190.
-
-   Refrigeration Compressor,8,MEDTEMP006CARLYLE\_R-22\_MED\_06DR820,           17190.
-
-   Refrigeration Compressor,9,MEDTEMP007CARLYLE\_R-22\_MED\_06DR820,           17190.
-
-   Refrigeration Compressor,10,MEDTEMP008CARLYLE\_R-22\_MED\_06DR820,           17190.
-
-   Refrigeration Condenser:Air-Cooled,3,CASCADETOPSYSTEMCONDENSER  ,         51.7,      52563.5,       4000.0
-
-The refrigeration output in the **eplusout.eio** file shows the number of refrigeration compressor racks, detailed refrigeration systems, detailed transcritical refrigeration systems, and secondary refrigeration systems found in the input data file (IDF). Additional information is shown for each compressor rack and the refrigerated case(s) and walk-in(s) connected to each compressor rack. For the detailed systems, additional information is shown for each refrigerated case(s), walk-in(s), cascade loads, secondary loads, mechanical subcooler loads, compressors, condenser, and mechanical and liquid suction heat exchanger subcoolers connected to the system. For the detailed transcritical refrigeration systems, additional information is shown for each refrigerated case(s), walk-in(s), compressor and gas cooler connected to the system. For secondary refrigeration systems, additional information is shown for each refrigerated case(s) and walk-in(s) connected to the system. For walk-ins, additional information is shown for each zone exchanging energy with that walk-in.
-
-The refrigeration “header� records (lines starting with an “!�) precede all the data lines. The data lines are grouped, showing the number of refrigeration compressor racks specified in the input data file followed by lines that reflect the information for each refrigeration compressor rack followed by the information for each refrigerated case and walk-in connected to this rack. The number of detailed systems is followed by a group of data lines describing the input values for the detailed refrigeration systems and similarly for the secondary refrigeration systems.
-
-This output reflects information for the specified refrigeration equipment along with entries from the IDF (or default data for blank fields). The data are preceded by a description (i.e. \#Refrigeration Compressor Racks, Refrigeration Compressor Rack, Refrigerated Case, \#Orphaned Refrigerated Cases, and Orphaned Refrigerated Case) followed by the information associated with each description.
-
-A final set of “header� records and descriptions are output only when a refrigeration object is found in the IDF but is not connected to a refrigeration compressor rack or refrigeration system object (i.e., orphaned).
-
-The following fields define each description and associated information.
-
-#### Header Record: \#Refrigeration Compressor Racks
-
-This field simply says “\#Refrigeration Compressor Racks� .
-
-#### Field: Number ofRefrigeration Compressor Racks
-
-The total number of refrigeration compressor racks simulated. This is the number of Refrigeration:CompressorRack objects found in the IDF.
-
-#### Header Record: Refrigeration Compressor Rack
-
-#### Field: Compressor Rack Name
-
-The name of the compressor rack simulated. Echoes the field Name in object Refrigeration:CompressorRack from the IDF.
-
-#### Field: \# Refrigerated Cases Connected
-
-The total number of refrigerated cases connected to the compressor rack.
-
-#### Field: \# WalkInCoolers Connected
-
-The total number of refrigeration walk-ins connected to the compressor rack.
-
-#### Field: Heat Rejection Location
-
-The location of the compressor rack’s air-cooled condenser. Echoes the field Heat Rejection Location in object Refrigeration:CompressorRack from the IDF.
-
-#### Field: COP
-
-The Coefficient of Performance (W/W) of the compressor rack. Echoes the field Design Compressor Rack COP in object Refrigeration:CompressorRack from the IDF.
-
-#### Header Record: Refrigeration Case
-
-#### Field: Refrigeration Case Number
-
-The number of the refrigerated case, assigned sequentially according to the order in which these objects are defined in the IDF.
-
-#### Field: Refrigeration  Case Name
-
-The name of the refrigerated case simulated. Echoes the field Name in object Refrigeration:Case from the IDF.
-
-#### Field: Zone Name
-
-The name of the zone where the refrigerated case is located. Echoes the field Zone Name in object Refrigeration:Case from the IDF.
-
-#### Field: Zone Node \#
-
-The number of the zone node (connection to the air loop) where the refrigerated case is located. This is the number of the zone node as found in the **eplusout.bnd** file.
-
-#### Field: Zone Node Name
-
-The name of the zone node where the refrigerated case is located. The refrigerated case will impact the air heat balance in this zone.
-
-#### Field: Capacity
-
-The total cooling capacity (W/m) of the refrigerated case. Echoes the field Rated Total Cooling Capacity per Unit Length in object Refrigeration:Case from the IDF.
-
-#### Field: LHR
-
-The design latent heat ratio (latent capacity divided by total cooling capacity) of the refrigerated case. Echoes the field Rated LHR in object Refrigeration:Case from the IDF.
-
-#### Field: Temperature {C}
-
-The average temperature (C) of the air and products within the refrigerated case. Echoes the field Case Operating Temperature in object Refrigeration:Case from the IDF.
-
-#### Field: Length {m}
-
-The length (m) of the refrigerated case. Echoes the field Case Length in object Refrigeration:Case from the IDF.
-
-#### Field: Fan {W/m}
-
-The total operating fan power (W/m) in the refrigerated case. Echoes the field Operating Case Fan Power per Unit Length in object Refrigeration:Case from the IDF.
-
-#### Field:Installed Lighting {W/m}
-
-The total installed lighting power (W/m) in the refrigerated case. Echoes the field Installed Case Lighting Power per Unit Length in object Refrigeration:Case from the IDF.
-
-#### Field: Anti-Sweat {W/m}
-
-The electric anti-sweat heater power (W/m) in the refrigerated case. Echoes the field Case Anti-Sweat Heater Power per Unit Length in object Refrigeration:Case from the IDF.
-
-#### Field: Defrost {W/m}
-
-The defrost power (W/m) in the refrigerated case. Echoes the field Case Defrost Power per Unit Length in object Refrigeration:Case from the IDF.
-
-#### Header Record: Refrigeration Walk In Cooler
-
-#### Field: Walk In Number
-
-The number of the refrigerated walk-in, assigned sequentially according to the order in which these objects are defined in the IDF.
-
-#### Field: Walk In Name
-
-The name of the refrigerated walk-in simulated. Echoes the field Name in object Refrigeration:WalkIn from the IDF.
-
-#### Field: Capacity
-
-The total cooling capacity (W) of the walk-in. Echoes the field Rated Coil Cooling Capacity in object Refrigeration:WalkIn from the IDF.
-
-#### Field: Temperature {C}
-
-The average temperature (C) of the air and products within the refrigerated case. Echoes the field Operating Temperature in object Refrigeration:WalkIn from the IDF.
-
-#### Field: Coil Fan {W}
-
-The coil fan power (W) in the walk-in . Echoes the field Cooling Coil Fan Power in object Refrigeration:WalkIn from the IDF.
-
-#### Field: Circulation Fan {W}
-
-The circulation fan power (W) in the walk-in. Echoes the field Circulation Fan Power in object Refrigeration:WalkIn from the IDF.
-
-#### Field: Lighting {W}
-
-The total lighting power (W) in the walk-in. Echoes the field Total Lighting Power in object Refrigeration:WalkIn from the IDF.
-
-#### Field: Heaters {W}
-
-The total electric heater power (W) in the walk-in. Echoes the field Total Heating Power in object Refrigeration:WalkIn from the IDF.
-
-#### Field: Defrost {W}
-
-The defrost power (W) in the walk-in. Echoes the field Defrost Power in object Refrigeration:WalkIn from the IDF.
-
-#### Field: \# Zones
-
-The number of zones that exchange energy with the walk-in. Counted according to the number of records in the Refrigeration:WalkIn object in the IDF..
-
-#### Header Record: Walk-In Surfaces Facing Zone
-
-#### Field: Zone Name
-
-The name of a zone adjacent to the walk-in. Echoes the field Zone Name in object Refrigeration:WalkIn from the IDF.
-
-#### Field: Wall/Ceiling Area {m2}
-
-The insulated surface area facing this zone adjacent to the walk-in. Echoes the field Total Insulated Surface Area Facing this Zone in object Refrigeration:WalkIn from the IDF.
-
-#### Field: UValue {W/m2-C]}
-
-The thermal conductance of the insulated surface area facing this zone adjacent to the walk-in. Echoes the field Insulated Surface UValue Facing this Zone in object Refrigeration:WalkIn from the IDF.
-
-#### Field: AreaStockDoors {m2}
-
-The total surface area of stock doors facing this zone adjacent to the walk-in. Echoes the field Area of Stocking Doors Facing this Zone in object Refrigeration:WalkIn from the IDF.
-
-#### Field: HeightStockDoors {m}
-
-The height of stock doors facing this zone adjacent to the walk-in. Echoes the field Height of Stocking Doors Facing this Zone in object Refrigeration:WalkIn from the IDF.
-
-#### Field: UValueStockDoors {W/m2-C]}
-
-The thermal conductance of the stock doors facing this zone adjacent to the walk-in. Echoes the field Stocking Door U Value Facing this Zone in object Refrigeration:WalkIn from the IDF.
-
-#### Field: AreaGlassDoors {m2}
-
-The total surface area of glass doors facing this zone adjacent to the walk-in. Echoes the field Area of Glass Reach In Doors Facing this Zone in object Refrigeration:WalkIn from the IDF.
-
-#### Field: HeightGlassDoors {m}
-
-The height of glass doors facing this zone adjacent to the walk-in. Echoes the field Height of Glass Doors Facing this Zone in object Refrigeration:WalkIn from the IDF.
-
-#### Field: UValueGlassDoors {W/m2-C]}
-
-The thermal conductance of the glass doors facing this zone adjacent to the walk-in. Echoes the field Glass Reach In Door U Value Facing this Zone in object Refrigeration:WalkIn from the IDF.
-
-#### Header Record: \#Detailed Refrigeration Systems
-
-#### Field: Number of Detailed Refrigeration Systems
-
-The total number of detailed refrigeration systems found in the IDF.
-
-#### Header Record:  Detailed Refrigeration System
-
-#### Field: Refrigeration System Name
-
-The name of the Refrigeration System simulated. Echoes the field Name in object Refrigeration:System from the IDF.
-
-#### Field: Refrigerant Used
-
-The name of the refrigerant used in the system. Echoes the field Working Fluid ID in object Refrigeration:System from the IDF.
-
-#### Field: \# Refrigerated Cases Connected
-
-The total number of refrigerated cases connected to the refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:System from the IDF.
-
-#### Field: \# WalkInCoolers  Connected
-
-The total number of walk-ins connected to the refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:System from the IDF.
-
-#### Field: \# Secondary Loops Served
-
-The total number of secondary loops connected to the refrigeration system. These are assigned to the refrigeration system through the field Refrigeration Transfer Load or TransferLoad List Name in object Refrigeration:System from the IDF.
-
-#### Field: \# Cascade Condensers Served
-
-The total number of cascade condensers cooled by the refrigeration system. These are assigned to the refrigeration system through the field Refrigeration Transfer Load or TransferLoad List Name in object Refrigeration:System from the IDF.
-
-#### Field: \# Mechanical Subcoolers Served
-
-The total number of mechanical subcoolers cooled by the refrigeration system. These are assigned to the refrigeration system through the field Capacity-Providing System in object Refrigeration:Subcooler from the IDF.
-
-#### Field: \# Compressors Connected
-
-The total number of compressors connected to the refrigeration system. These are assigned to the refrigeration system through the field Compressor Name or CompressorList Name in object Refrigeration:System from the IDF.
-
-#### Field: \# Compression Stages
-
-The number of compressor stages for the refrigeration system. The value is either “1� for single-stage compression systems or “2� for two-stage compression systems.
-
-#### Field: Intercooler Type
-
-The intercooler type (either “1� for Flash Intercooler or “2� for Shell-and-Coil Intercooler) for two-stage compression systems.  A value of “0� indicates no intercooler (single-stage compression systems only).
-
-#### Field: Intercooler Effectiveness
-
-The intercooler effectiveness for the shell-and-coil intercooler.
-
-#### Field: \# Subcoolers Connected
-
-The total number of subcoolers, both liquid suction and mechanical, that provide cooling to the refrigeration system. These are assigned to the refrigeration system through the fields Mechanical Subcooler Name and Liquid Suction Heat Exchanger Subcooler Name in object Refrigeration:System from the IDF.
-
-#### Field: Minimum Condensing Temperature (C)
-
-The minimum condensing temperature allowed for the refrigeration system. Echoes the field Minimum Condensing Temperature in object Refrigeration:WalkIn from the IDF.
-
-#### Header Record: \#Detailed Transcritical Refrigeration Systems
-
-#### Field: Number of Detailed Transcritical Refrigeration Systems
-
-The total number of detailed transcritical CO<sub>2</sub> refrigeration systems found in the IDF.
-
-#### Header Record:  Detailed Transcritical Refrigeration System
-
-#### Field: Transcritical Refrigeration System Name
-
-The name of the Transcritical Refrigeration System simulated. Echoes the field Name in object Refrigeration:TranscriticalSystem from the IDF.
-
-#### Field: Refrigerant Used
-
-The name of the refrigerant used in the transcritical refrigeration system. Echoes the field Working Fluid ID in object Refrigeration:TranscriticalSystem from the IDF.
-
-#### Field: \# Medium Temperature Refrigerated Cases Connected
-
-The total number of medium temperature refrigerated cases connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:TranscriticalSystem from the IDF.
-
-#### Field: \# Low Temperature Refrigerated Cases Connected
-
-The total number of low temperature refrigerated cases connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:TranscriticalSystem from the IDF.
-
-#### Field: \# Medium Temperature WalkInCoolers  Connected
-
-The total number of medium temperature walk-ins connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:TranscriticalSystem from the IDF.
-
-#### Field: \# Low Temperature WalkInCoolers  Connected
-
-The total number of low temperature walk-ins connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:TranscriticalSystem from the IDF.
-
-#### Field: \# High Pressure Compressors Connected
-
-The total number of high pressure compressors connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Compressor Name or CompressorList Name in object Refrigeration:TranscriticalSystem from the IDF.
-
-#### Field: \# Low Pressure Compressors Connected
-
-The total number of low pressure compressors connected to the transcritical refrigeration system. These are assigned to the refrigeration system through the field Compressor Name or CompressorList Name in object Refrigeration:TranscriticalSystem from the IDF.
-
-#### Field: Minimum Condensing Temperature (C)
-
-The minimum condensing temperature allowed during subcritical operation for the transcritical refrigeration system. Echoes the field Minimum Condensing Temperature in object Refrigeration:GasCooler:AirCooled from the IDF.
-
-#### Header Record: Cascade Load
-
-#### Field: System Name Connected
-
-The name of another detailed system that rejects heat to a cascade condenser cooled by this detailed system. These are assigned to the refrigeration system, via the name of the cascade condenser, through the field Refrigeration Transfer Load or TransferLoad List Name in object Refrigeration:System from the IDF.
-
-#### Field: Condenser Number
-
-The number of the cascade condenser cooled by this detailed system, assigned sequentially according to the order in which these objects are defined in the IDF.
-
-#### Field: Condenser Name
-
-The name of a cascade condenser cooled by this detailed system. These are assigned to the refrigeration system, via the name of the cascade condenser, through the field Refrigeration Transfer Load or TransferLoad List Name in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Condenser:Cascade
-
-#### Header Record: Secondary Load
-
-#### Field: Secondary System Served Name
-
-The name of the secondary system cooled by this detailed system. These are assigned to the refrigeration system through the field Refrigeration Transfer Load or TransferLoad List Name in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:SecondarySystem.
-
-#### Field: Secondary Number
-
-The number of the secondary system cooled by this detailed system, assigned sequentially according to the order in which these objects are defined in the IDF.
-
-#### Header Record: Mechanical Subcooler Load
-
-#### Field: Subcooler Number
-
-The number of the mechanical subcooler cooled by this detailed system, assigned sequentially according to the order in which these objects are defined in the IDF.
-
-#### Field: Subcooler Name
-
-The name of the secondary system cooled by this detailed system. These are assigned to the refrigeration system through the field Capacity-Providing System in object Refrigeration:Subcooler from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Subcooler.
-
-#### Header Record:  Refrigeration Compressor
-
-#### Field: Compressor Number
-
-The number of the refrigeration compressor, assigned sequentially according to the order in which these objects are defined in the IDF.
-
-#### Field: Compressor Name
-
-The name of the compressor simulated. Echoes the field Name of Compressor in object List:Refrigeration:Compressors from the IDF.
-
-#### Field: Nominal Capacity, W
-
-The nominal capacity of the compressor based on the capacity curve (identified by the field Unique Name of Capacity Curve in the object Refrigeration:Compressor in the IDF) evaluated at the lowest design evaporating temperature of all the cases attached to the system and at the design condensing temperature of the condenser attached to the system.
-
-#### Header Record:  Refrigeration Condenser, Air-Cooled
-
-#### Field: Condenser  Number
-
-The number of the refrigeration condenser, assigned sequentially according to the order in which all the Refrigeration:Condenser:\*  objects are defined in the IDF.
-
-#### Field: Condenser Name
-
-The name of the condenser simulated. Echoes the field Name of Condenser for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Condenser:Aircooled.
-
-#### Field: Rated Condensing Temperature, C
-
-The rated condensing temperature of the condenser, set by standard ARI 460 for air-cooled condensers.
-
-#### Field: Rated Capacity, W
-
-The rated capacity of the condenser. This value is taken from the capacity curve (identified by the field Name of Condenser Heat of Rejection Curve, Linear, in the object Refrigeration:Condenser:AirCooled in the IDF) evaluated at the temperature difference specified in standard ARI 460.
-
-#### Field: Rated Fan Power, W
-
-The rated fan power of the condenser. Echoes the field Rated Fan Power in object Refrigeration:Condenser:AirCooled from the IDF.
-
-#### Header Record:  Refrigeration Condenser, Water-Cooled
-
-#### Field: Condenser  Number
-
-The number of the refrigeration condenser, assigned sequentially according to the order in which all the Refrigeration: Condenser:\* objects are defined in the IDF.
-
-#### Field: Condenser Name
-
-The name of the condenser simulated. Echoes the field Name of Condenser for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Condenser:WaterCooled.
-
-#### Field: Rated Condensing Temperature, C
-
-The rated condensing temperature of the condenser, echos the field Rated Condensing Temperature in the object Refrigeration:Condenser:WaterCooled.
-
-#### Field: Rated Capacity, W
-
-The rated capacity of the condenser. Echos the field Rated Total Heat Rejection Effect in the object Refrigeration:Condenser:WaterCooled in the IDF.
-
-#### Field: Rated Water Inlet Temperature, C
-
-The rated water inlet temperature of the condenser. Echos the field Rated Water Inlet Temperature in the object Refrigeration:Condenser:WaterCooled in the IDF.
-
-#### Field: Rated Water Flow Rate, m3/s
-
-The rated water flow rate of the condenser. Echos the field Water Design Flow Rate in the object Refrigeration:Condenser:WaterCooled in the IDF.
-
-#### Header Record:  Refrigeration Condenser, Evaporative-Cooled
-
-#### Field: Condenser  Number
-
-The number of the refrigeration condenser, assigned sequentially according to the order in which all the Refrigeration: Condenser:\* objects are defined in the IDF.
-
-#### Field: Condenser Name
-
-The name of the condenser simulated. Echoes the field Name of Condenser for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Condenser: EvaporativeCooled.
-
-#### Field: Rated Capacity, W
-
-The rated capacity of the condenser. Echos the field Rated Total Heat Rejection Effect in the object Refrigeration:Condenser:EvaporativeCooled in the IDF.
-
-#### Field: Rated Fan Power, W
-
-The rated fan power of the condenser. Echoes the field Rated Fan Power in object  Refrigeration:Condenser: EvaporativeCooled in the IDF.
-
-#### Header Record:  Refrigeration Condenser, Cascade
-
-#### Field: Condenser  Number
-
-The number of the refrigeration condenser, assigned sequentially according to the order in which all the Refrigeration: Condenser \*  objects are defined in the IDF.
-
-#### Field: Condenser Name
-
-The name of the condenser simulated. Echoes the field Name of Condenser for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Condenser:Cascade.
-
-#### Field: Condensing Temperature Control Type,
-
-Echoes the field Condensing Temperature Control Type in object Refrigeration:Condenser:Cascade.
-
-#### Field: Rated Condensing Temperature, C
-
-The rated condensing temperature of the condenser, echoes the field Rated Condensing Temperature in object Refrigeration:Condenser:Cascade.
-
-#### Field: Rated Capacity, W
-
-The rated capacity of the condenser, echoes the field Rated Effective Total Heat Rejection Rate in object Refrigeration:Condenser:Cascade.
-
-#### Field: Approach Temperature Difference, DeltaC
-
-The approach temperature difference of the condenser, echoes the field Rated Approach Temperature Difference in object Refrigeration:Condenser:Cascade from the IDF.
-
-#### Header Record:  Refrigeration GasCooler:Air-Cooled
-
-#### Field: Gas Cooler Number
-
-The number of the refrigeration gas cooler, assigned sequentially according to the order in which all the Refrigeration:GasCooler objects are defined in the IDF.
-
-#### Field: Gas Cooler Name
-
-The name of the gas cooler simulated. Echoes the field Refrigeration Gas Cooler Name in object Refrigeration:TranscriticalSystem from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:GasCooler:Aircooled.
-
-#### Field: Rated Outlet Pressure, Pa
-
-The rated gas cooler pressure corresponding to the rated capacity.
-
-#### Field: Rated Outlet Temperature, C
-
-The rated gas cooler outlet temperature corresponding to the rated capacity.
-
-#### Field: Rated Approach Temperature, C
-
-The rated gas cooler approach temperature corresponding to the rated capacity.
-
-#### Field: Rated Capacity, W
-
-The rated capacity of the gas cooler. This value is taken from the capacity curve (identified by the field Rated Total Heat Rejection Rate Curve Name, in the object Refrigeration:GasCoooler:AirCooled in the IDF) evaluated at the rated approach temperature.
-
-#### Field: Rated Fan Power, W
-
-The rated fan power of the gas cooler. Echoes the field Rated Fan Power in object Refrigeration:GasCooler:AirCooled from the IDF.
-
-#### Header Record: Refrigeration  Mechanical Subcooler
-
-#### Field: Subcooler Number
-
-The number of the mechanical subcooler, assigned sequentially according to the order in which all the Refrigeration:Subcooler  objects are defined in the IDF.
-
-#### Field: Subcooler Name
-
-The name of the subcooler simulated. Echoes the field Mechanical Subcooler Name for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Subcooler.
-
-#### Field: Name of System Providing Cooling
-
-The name of the detailed system that absorbs heat from the subcooler. These are assigned to the subcooer through the field Capacity-Providing System in object Refrigeration:Subcooler from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:System.
-
-#### Field: Design Outlet Temperature, C
-
-The controlled outlet temperature of the subcooler, echoes the field Outlet Control Temperature in object Refrigeration: Subcooler.
-
-#### Header Record:  Refrigeration Liquid Suction Subcooler
-
-#### Field: Subcooler Number
-
-The number of the liquid suction subcooler, assigned sequentially according to the order in which all the Refrigeration:Subcooler  objects are defined in the IDF.
-
-#### Field: Subcooler Name
-
-The name of the subcooler simulated. Echoes the field Liquid Suction Heat Exchanger Subcooler Name for the System in object Refrigeration:System from the IDF. The name corresponds to an entry in the field Name in the object Refrigeration:Subcooler.
-
-#### Field: Design Subcooling, deltaC
-
-The design change in temperature of the warm fluid within the liquid suction subcooler, echoes the field Liquid Suction Design Subcooling Temperature in object Refrigeration: Subcooler.
-
-#### Field: Design liquid inlet temperature, C
-
-The design warm liquid inlet temperature of the liquid suction subcooler, echoes the field Design Liquid Inlet Temperature in object Refrigeration: Subcooler.
-
-#### Field: Design vapor inlet temperature, C
-
-The design cold vapor inlet temperature of the liquid suction subcooler, echoes the field Design Vapor Inlet Temperature in object Refrigeration: Subcooler.
-
-#### Header Record: \# Secondary Refrigeration Systems
-
-#### Field: Number of Secondary Refrigeration Systems
-
-The total number of secondary refrigeration systems found in the IDF.
-
-#### Header Record:  Secondary Refrigeration System: Fluid Always Liquid
-
-#### Field: Secondary Number
-
-The number of the secondary refrigeration system, assigned sequentially according to the order in which all the Refrigeration:SecondarySystem  objects are defined in the IDF.
-
-#### Field: Secondary Name
-
-The name of the secondary refrigeration system simulated. Echoes the field Name in object Refrigeration:SecondarySystem from the IDF.
-
-#### Field: \# Refrigerated Cases Connected
-
-The total number of refrigerated cases connected to the secondary refrigeration system. These are assigned to the secondary refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:SecondarySystem from the IDF.
-
-#### Field: \# WalkInCoolers  Connected
-
-The total number of walk-ins connected to the secondary refrigeration system. These are assigned to the secondary refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:System from the IDF.
-
-#### Field: Fluid Name
-
-The name of the circulating fluid used in the system. Echoes the field Circulating Fluid Name in object Refrigeration:SecondarySystem from the IDF.
-
-#### Field: Capacity, W
-
-The rated capacity of the evaporator, echoes the field Evaporator Design Capacity In Watts in object Refrigeration:SecondarySystem.
-
-#### Field: Evap Temperature in Secondary Evaporator, C
-
-The rated evaporating temperature of the heat exchanger, echoes the field Design Evaporating Temperature in object Refrigeration:SecondarySystem.
-
-#### Field: Approach Temperature Difference, DeltaC
-
-The approach temperature difference of the heat exchanger, echoes the field Design Approach Temperature Difference in object Refrigeration:SecondarySystem from the IDF.
-
-#### Field: Temperature Range, DeltaC
-
-The temperature range of the heat exchanger, echoes the field Design Range Temperature Difference in object Refrigeration:SecondarySystem from the IDF.
-
-#### Field: TotalPumpPower, W
-
-The rated total pump power of the secondary loop, echoes the field Design Total Pump Power in object Refrigeration:SecondarySystem.
-
-#### Header Record:  Secondary Refrigeration System: Liquid Overfeed
-
-#### Field: Secondary Number
-
-The number of the secondary refrigeration system, assigned sequentially according to the order in which all the Refrigeration:SecondarySystem  objects are defined in the IDF.
-
-#### Field: Secondary Name
-
-The name of the secondary refrigeration system simulated. Echoes the field Name in object Refrigeration:SecondarySystem from the IDF.
-
-#### Field: \# Refrigerated Cases Connected
-
-The total number of refrigerated cases connected to the secondary refrigeration system. These are assigned to the secondary refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:SecondarySystem from the IDF.
-
-#### Field: \# WalkInCoolers  Connected
-
-The total number of walk-ins connected to the secondary refrigeration system. These are assigned to the secondary refrigeration system through the field Refrigerated Case or Walkin or CaseAndWalkInList Name in object Refrigeration:System from the IDF.
-
-#### Field: Fluid Name
-
-The name of the circulating fluid used in the system. Echoes the field Circulating Fluid Name in object Refrigeration:SecondarySystem from the IDF.
-
-#### Field: Capacity, W
-
-The rated capacity of the evaporator, echoes the field Evaporator Design Capacity In Watts in object Refrigeration:SecondarySystem.
-
-#### Field: Evap Temperature in Secondary Evaporator, C
-
-The rated evaporating temperature of the heat exchanger, echoes the field Design Evaporating Temperature in object Refrigeration:SecondarySystem.
-
-#### Field: Approach Temperature Difference, DeltaC
-
-The approach temperature difference of the heat exchanger, echoes the field Design Approach Temperature Difference in object Refrigeration:SecondarySystem from the IDF.
-
-#### Field: Circulating Rate
-
-The ratio of the mass flow rate of refrigerant at the pump to the mass flow rate of refrigerant vapor leaving the refrigeration load(s), echoes the field PhaseChange Circulating Rate in object Refrigeration:SecondarySystem from the IDF.
-
-#### Field: TotalPumpPower, W
-
-The rated total pump power of the secondary loop, echoes the field Design Total Pump Power in object Refrigeration:SecondarySystem.
-
-#### Header Record: \#Orphaned Refrigerated Cases
-
-#### Field: Number of Orphaned Refrigerated Cases
-
-The total number of orphaned refrigerated cases found in the IDF.
-
-#### Field: Message
-
-A message stating “NOTE: These cases were not simulated...�.
-
-#### Header Record: Orphaned Refrigerated Case
-
-#### Field: Refrigerated Case Number
-
-The number of the orphaned refrigerated case found in the IDF. The refrigerated case numbers are assigned sequentially according to the order in which these objects are defined in the IDF.
-
-#### Field: Refrigerated Case Name
-
-The name of the orphaned refrigerated case which is **not** connected to a compressor rack or detailed refrigeration system. Echoes the field Name in object Refrigeration:Case from the IDF.
-
-#### Field: Zone Name
-
-The name of the zone where the refrigerated case is located. Echoes the field Zone Name in object Refrigeration:Case from the IDF.
-
-#### Field: Zone Node \#
-
-The number of the zone node (connection to the air loop) where the refrigerated case is located. This is the number of the zone node as found in the **eplusout.bnd** file.
-
-#### Field: Zone Node Name
-
-The name of the zone node where the orphaned refrigerated case is located. This orphaned refrigerated case will **not** impact the air heat balance in this zone.
-
-#### Header Record: \#Orphaned Walk Ins
-
-#### Field: Number of OrphanedWalk Ins
-
-The total number of orphaned Walk Ins found in the IDF.
-
-#### Field: Message
-
-A message stating “NOTE: These Walk Ins were not simulated...�.
-
-#### Header Record: Orphaned Walk In
-
-#### Field:Walk In Number
-
-The number of the orphaned Walk In found in the IDF. The Walk In numbers are assigned sequentially according to the order in which these objects are defined in the IDF.
-
-#### Field: Walk In Name
-
-The name of the orphaned Walk In which is **not** connected to a compressor rack or refrigeration system. Echoes the field Name in object Refrigeration:WalkIn from the IDF.
-
-#### Header Record: \#Orphaned Refrigeration Compressors
-
-#### Field: Number of Orphaned Refrigeration Compressors
-
-The total number of orphaned Refrigeration Compressors found in the IDF.
-
-#### Field: Message
-
-A message stating “NOTE: These Compressors were not simulated...�.
-
-#### Header Record: Orphaned Refrigeration Compressor
-
-#### Field:Compressor  Number
-
-The number of the orphaned Compressor found in the IDF. The Compressor numbers are assigned sequentially according to the order in which these objects are defined in the IDF.
-
-#### Field: Compressor Name
-
-The name of the orphaned Compressor which is **not** connected to a detailed refrigeration system. Echoes the field Name in object Refrigeration:Compressor from the IDF.
-
-#### Header Record: \#Orphaned Refrigeration Secondary Loops
-
-#### Field: Number of Orphaned Secondary Loops
-
-The total number of orphaned Secondary Loops found in the IDF.
-
-#### Field: Message
-
-A message stating “NOTE: These Secondary Loops were not simulated...�.
-
-#### Header Record: Orphaned Refrigeration Secondary Loop
-
-#### Field:Secondary  Number
-
-The number of the orphaned Secondary System found in the IDF. The Secondary System numbers are assigned sequentially according to the order in which these objects are defined in the IDF.
-
-#### Field: Secondary Name
-
-The name of the orphaned Secondary which is not connected to a detailed refrigeration system. Echoes the field Name in object Refrigeration:SecondarySystem from the IDF.
-
-### View Factor Info
-
-A semi-debugging, informational report on View Factors for each zone/surface is available when you add **Output:Diagnostics,DisplayAdvancedVariables;** to your input file.
-
-After EnergyPlus receives the geometry information for the building, it calculates the view factors and grey interchange information for each zone and surface. These are used to calculate the interior radiant exchange between surfaces. The first set is called the approximate view factors; then, a deeper evaluation of the zone’s geometry and surfaces is performed to see if corrections need to be applied. Three sets of values are provided for the user’s information.
-
-! &lt;Surface View Factor Check Values&gt;,ZoneName,Original Check Value,Calculated Fixed Check Value,Final Check Value
-
-Surface View Factor Check Values,ZONE ONE,8.881784E-016,8.637788E-004,8.881784E-016
-
-#### Field: Zone Name
-
-This is the zone name for the values.
-
-#### Field: Original Check Value
-
-Original check value as submitted to the “Test and Check� routine. This value represents the Sum of the N (number of surfaces) by N matrix – the Number of Surfaces. Ideally, it should be very close to zero. The original check value could come from either the User inputting the view factors for the zone or the approximate view factor calculation in EnergyPlus.
-
-#### Field: Calculated Fixed Check Value
-
-This is the value of the view factor matrix (i.e. SUM(NXNmatrix – N) after the fix routine has applied them.
-
-#### Field: Final Check Value
-
-This value should match one of the previous values and indicate whether the original matrix or the modfied/fixed matrix will be used in the calculations.
-
-### View Factor Details
-
-View factors for zones (surfaces) can be entered into the input file (object: ZoneProperty:UserViewFactors) if desired. Or they can be reported from the input file. The following describes the reporting of these view factors. You can report the surface view factor information by using:
-
-Output:Surfaces:List,ViewFactorInfo;
-
-This triggers EnergyPlus to produce a special output section in the file eplusout.eio. This file, which is csv format, can be opened in Excel, and will show detailed information about the surfaces in all the zones.
-
-In order to get user view factors ready for inclusion in an input file, several steps much be taken. *First, because EnergyPlus has a data structure for zones that only is defined at initialization, it is necessary to use EnergyPlus to determine the surface numbers (i,j) before a UserViewFactors object can be constructed.* (This is a known defect – a new object is being defined that will make this unnecessary). THIS STILL NEEDS TO BE REVISED BASE ON IF WE GO FOR NEW INPUT OR NOT.
-
-
-
-! &lt;Surface View Factor and Grey Interchange Information&gt;
-
-! &lt;View Factor - Zone Information&gt;,Zone Name,Number of Surfaces
-
-! &lt;View Factor - Surface Information&gt;,Surface Name,Surface Class,Area {m2},Azimuth,Tilt,Thermal Emissivity,\#Sides,Vertices
-
-! &lt;View Factor / Grey Interchange Type&gt;,Surface Name(s)
-
-! &lt;View Factor&gt;,Surface Name,Surface Class,Row Sum,View Factors for each Surface
-
-Surface View Factor - Zone Information,ZONE ONE,6
-
-Surface View Factor - Surface Information, ZN001:WALL001,Wall,69.6773,180.0000,90.0000,0.9000,4, 0.0000,0.0000,4.5720,0.0000,0.0000,0.0000,15.2400,0.0000,0.0000,15.2400,0.0000,4.5720,
-
-Surface View Factor - Surface Information,ZN001:WALL002,Wall,69.6773,90.0000,90.0000,0.9000,4, 15.2400,0.0000,4.5720,15.2400,0.0000,0.0000,15.2400,15.2400,0.0000,15.2400,15.2400,4.5720,
-
-Surface View Factor - Surface Information,ZN001:WALL003,Wall,69.6773,0.0000,90.0000,0.9000,4, 15.2400,15.2400,4.5720,15.2400,15.2400,0.0000,0.0000,15.2400,0.0000,0.0000,15.2400,4.5720,
-
-Surface View Factor - Surface Information,ZN001:WALL004,Wall,69.6773,270.0000,90.0000,0.9000,4, 0.0000,15.2400,4.5720,0.0000,15.2400,0.0000,0.0000,0.0000,0.0000,0.0000,0.0000,4.5720,
-
-Surface View Factor - Surface Information,ZN001:FLR001,Floor,232.2576,90.0000,180.0000,0.9000,4, 15.2400,0.0000,0.0000,0.0000,0.0000,0.0000,0.0000,15.2400,0.0000,15.2400,15.2400,0.0000,
-
-Surface View Factor - Surface Information,ZN001:ROOF001,Roof,232.2576,180.0000,0.0000,0.9000,4, 0.0000,15.2400,4.5720,0.0000,0.0000,4.5720,15.2400,0.0000,4.5720,15.2400,15.2400,4.5720,
-
-Approximate or User Input ViewFactors,To Surface,Surface Class,RowSum,ZN001:WALL001,ZN001:WALL002,ZN001:WALL003,ZN001:WALL004,ZN001:FLR001,ZN001:ROOF001,
-
-View Factor,ZN001:WALL001,Wall,1.0000,0.0000,0.1034,0.1034,0.1034,0.3448,0.3448,
-
-View Factor,ZN001:WALL002,Wall,1.0000,0.1034,0.0000,0.1034,0.1034,0.3448,0.3448,
-
-View Factor,ZN001:WALL003,Wall,1.0000,0.1034,0.1034,0.0000,0.1034,0.3448,0.3448,
-
-View Factor,ZN001:WALL004,Wall,1.0000,0.1034,0.1034,0.1034,0.0000,0.3448,0.3448,
-
-View Factor,ZN001:FLR001,Floor,1.0000,0.1364,0.1364,0.1364,0.1364,0.0000,0.4545,
-
-View Factor,ZN001:ROOF001,Roof,1.0000,0.1364,0.1364,0.1364,0.1364,0.4545,0.0000,
-
-Final ViewFactors,To Surface,Surface Class,RowSum,ZN001:WALL001,ZN001:WALL002,ZN001:WALL003,ZN001:WALL004,ZN001:FLR001,ZN001:ROOF001,
-
-View Factor,ZN001:WALL001,Wall,1.0000,0.0000,0.1034,0.1034,0.1034,0.3448,0.3448,
-
-View Factor,ZN001:WALL002,Wall,1.0000,0.1034,0.0000,0.1034,0.1034,0.3448,0.3448,
-
-View Factor,ZN001:WALL003,Wall,1.0000,0.1034,0.1034,0.0000,0.1034,0.3448,0.3448,
-
-View Factor,ZN001:WALL004,Wall,1.0000,0.1034,0.1034,0.1034,0.0000,0.3448,0.3448,
-
-View Factor,ZN001:FLR001,Floor,1.0000,0.1364,0.1364,0.1364,0.1364,0.0000,0.4545,
-
-View Factor,ZN001:ROOF001,Roof,1.0000,0.1364,0.1364,0.1364,0.1364,0.4545,0.0000,
-
-Script F Factors,X Surface,ZN001:WALL001,ZN001:WALL002,ZN001:WALL003,ZN001:WALL004,ZN001:FLR001,ZN001:ROOF001,
-
-Script F Factor,ZN001:WALL001,1.1191E-002,9.4126E-002,9.4126E-002,9.4126E-002,0.3032,0.3032,
-
-Script F Factor,ZN001:WALL002,9.4126E-002,1.1191E-002,9.4126E-002,9.4126E-002,0.3032,0.3032,
-
-Script F Factor,ZN001:WALL003,9.4126E-002,9.4126E-002,1.1191E-002,9.4126E-002,0.3032,0.3032,
-
-Script F Factor,ZN001:WALL004,9.4126E-002,9.4126E-002,9.4126E-002,1.1191E-002,0.3032,0.3032,
-
-Script F Factor,ZN001:FLR001,0.1199,0.1199,0.1199,0.1199,3.4097E-002,0.3863,
-
-Script F Factor,ZN001:ROOF001,0.1199,0.1199,0.1199,0.1199,0.3863,3.4097E-002,
-
-#### Surface View Factor – Zone Information
-
-This line provides the zone name and the number of surfaces (heat transfer) in the zone. This information may be redundant with other reports in the eio file. It is included here to assist users who wish to use the auxiliary view factor program to generate view factors.
-
-#### Surface View Factor – Surface Information
-
-These lines provide the surface information for each surface in the zone. This includes the name, class, area, azimuth (outward facing normal angle), the tilt angle, the thermal emissivity, the number of sides to the surface and the vertices.  Again, this information may be redundant with other reports in the eio file. It is included here to assist users who wish to use the auxiliary view factor program to generate view factors.
-
-#### Approximate or User Input View Factors
-
-This section/lines provide the original view factors after either user input or approximate calculation. Surface name and class information are given again as well as each row sum (these should sum to 1, ideally) and then the view factors to other surfaces shown in columnar order.
-
-#### Final View Factors
-
-This section/lines shows view factors after they have been corrected for reciprocity and completeness. Correction may be necessary to make sure any two surfaces exchange radiation reciprocally, that is, the radiation leaving one surface directed at another surface is the same as the amount of radiation arriving at the other surface, and that the sum of all the radiant energy exchanges in the zone is zero. If the user input view factors are perfect in these characteristics, the correction will not change them. The displayed lines show what view factors will be used during the simulation.
-
-#### Script F Factors
-
-Finally, grey interchange coefficients are presented. These are the coefficients that are used to calculate the radiant energy exchange between the surfaces in the zone. They are calculated to include reflection from intervening surfaces in the zone.
-
-### DX Coil Outputs
-
-### DX Cooling Coil Outputs
-
-Outputs are provided for air-cooled, single-speed direct expansion (DX) cooling coils as follows:
-
-    ! &lt;DX Cooling Coil Standard Rating Information&gt;, Component Type, Component Name, Standard Rating (Net) Cooling Capacity {W}, Standard Rated Net COP {W/W}, EER {Btu/W-h}, SEER {Btu/W-h}, IEER {Btu/W-h}
-
-    DX Cooling Coil Standard Rating Information, Coil:Cooling:DX:SingleSpeed, PSZ-AC\_1:1\_COOLC DXCOIL, 29299.3, 3.04, 10.38, 10.47, 10.67
-
-    DX Cooling Coil Standard Rating Information, Coil:Cooling:DX:SingleSpeed, PSZ-AC\_2:2\_COOLC DXCOIL, 17427.1, 3.21, 10.95, 11.04, 11.20
-
-#### Field: Component Type
-
-This is the component type, currently Coil:Cooling:DX:SingleSpeed is the only valid type.
-
-#### Field: Component Name
-
-The name of the DX cooling coil from the input data file (IDF).
-
-#### Field: Standard Rating (Net) Cooling Capacity {W}
-
-The standard rating (net) cooling capacity for this DX cooling coil. Units are Watts. See the EnergyPlus Engineering Reference (Single Speed DX Cooling Coil, Standard Ratings) for details on how this value is calculated.
-
-#### Field: Standard Rated Net COP {W/W}
-
-The standard rated net COP or energy efficiency ratio (*EER*) at standard rating conditions for the DX cooling coil in SI units of W/W. See the EnergyPlus Engineering Reference (Single Speed DX Cooling Coil, Standard Ratings) for details on how this value is calculated.
-
-#### Field: EER {Btu/W-h}
-
-The energy efficiency ratio (*EER*) at standard rating conditions for the DX cooling coil in IP units of Btu/W-hr. See the EnergyPlus Engineering Reference (Single Speed DX Cooling Coil, Standard Ratings) for details on how this value is calculated.
-
-#### Field: SEER {Btu/W-h}
-
-The seasonal energy efficiency ratio (SEER) for the DX cooling coil in IP units of Btu/W-hr. See the EnergyPlus Engineering Reference (Single Speed DX Cooling Coil, Standard Ratings) for details on how this value is calculated.
-
-#### Field: IEER {Btu/W-h}
-
-The integrated energy efficiency ratio (*IEER*) for the DX cooling coil in IP units of Btu/W-hr. See the EnergyPlus Engineering Reference (Single Speed DX Cooling Coil, Standard Ratings) for details on how this value is calculated.
-
-### DX Cooling Coil Outputs for ASHRAE 127 Standard Ratings
-
-#### Field: Component Type
-
-This is the component type, currently Coil:Cooling:DX:SingleSpeed is the only valid type.
-
-#### Field: Component Name
-
-The name of the DX cooling coil from the input data file (IDF).
-
-#### Field: Class
-
-The application classification classes of the DX cooling coil. There are four application classification classes per ASHRAE standard 127: Class I, Class II, Class III, and Class IV.  The standard ratings are reported for each the four classification classes and test conditions.
-
-#### Field: Rated Net Cooling Capacity at Test A {W}
-
-Rated net cooling capacity for this DX cooling coil at Test condition A per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The net cooling capacity is reported for class I, II, II and IV test conditions.
-
-#### Field: Rated Total Electric Power Test A {W}
-
-Rated total electric power input of the unit at Test condition A per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The total electric power includes the supply fan power as well. The total electric power input is reported for class I, II, III and IV test conditions.
-
-#### Field: Rated Net Cooling Capacity at Test B {W}
-
-Rated net cooling capacity of this unit at Test condition B per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The net cooling capacity is reported for class I, II, II and IV test conditions.
-
-#### Field: Rated Total Electric Power Test B {W}
-
-Rated total electric power input of the unit at Test condition B per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The total electric power includes the supply fan power as well. The total electric power input is reported for class I, II, III and IV test conditions.
-
-#### Field: Rated Net Cooling Capacity at Test C {W}
-
-Rated net cooling capacity of this unit at Test condition C per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The net cooling capacity is reported for class I, II, II and IV test conditions.
-
-#### Field: Rated Total Electric Power Test C {W}
-
-Rated total electric power input of the unit at Test condition C per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The total electric power includes the supply fan power as well. The total electric power input is reported for class I, II, III and IV test conditions.
-
-#### Field: Rated Net Cooling Capacity at Test D {W}
-
-Rated net cooling capacity of unit at Test condition D per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The net cooling capacity is reported for class I, II, II and IV test conditions.
-
-#### Field: Rated Total Electric Power Test D {W}
-
-Rated total electric power input of the unit at Test condition D per Standard ASHRAE 127. Units are Watts. See the EnergyPlus Engineering Reference (ANSI/ASHRAE 127 - Standard Ratings of Single-Speed DX Cooling Coils) for details on how this value is calculated. The total electric power includes the supply fan power as well. The total electric power input is reported for class I, II, III and IV test conditions.
-
-```
-! <DX Cooling Coil ASHRAE 127 Standard Ratings Information>, Component Type, Component Name, Standard 127 Classification, Rated Net Cooling Capacity Test A {W}, Rated Total Electric Power Test A {W}, Rated Net Cooling Capacity Test B {W}, Rated Total Electric Power Test B {W}, Rated Net Cooling Capacity Test C {W}, Rated Total Electric Power Test C {W}, Rated Net Cooling Capacity Test D {W}, Rated Total Electric Power Test D {W} 
- DX Cooling Coil ASHRAE 127 Standard Ratings Information, Coil:Cooling:DX:SingleSpeed, MAIN COOLING COIL 1, Class 1, 126953.8, 35918.5, 135678.7, 30852.7, 141523.1, 24400.1, 141727.0, 13951.0
- DX Cooling Coil ASHRAE 127 Standard Ratings Information, Coil:Cooling:DX:SingleSpeed, MAIN COOLING COIL 1, Class 2, 133377.6, 37330.3, 140336.0, 31647.7, 141727.0, 24424.7, 141727.0, 13951.0
- DX Cooling Coil ASHRAE 127 Standard Ratings Information, Coil:Cooling:DX:SingleSpeed, MAIN COOLING COIL 1, Class 3, 139488.4, 38673.3, 141354.0, 31821.4, 141727.0, 24424.7, 141727.0, 13951.0
- DX Cooling Coil ASHRAE 127 Standard Ratings Information, Coil:Cooling:DX:SingleSpeed, MAIN COOLING COIL 1, Class 4, 145024.0, 39889.8, 141727.0, 31885.1, 141727.0, 24424.7, 141727.0, 13951.0
-```
-
-### DX Heating Coil Outputs
-
-Outputs are provided for single-speed direct expansion (DX) heating coils as follows:
-
-```
-! &lt;DX Heating Coil Standard Rating Information&gt;, Component Type, Component Name, High Temperature Heating Standard (Net) Rating Capacity {W}, Low Temperature Heating Standard (Net) Rating Capacity {W}, HSPF {Btu/W-h, Region Number
-DX Heating Coil Standard Rating Information, Coil:Heating:DX:SingleSpeed, PSZ-AC\_1:1\_HEATC DXCOIL, 10476.1, 5833.2, 6.10, 4
-```
-
-#### Field: Component Type
-
-This is the component type, currently Coil:Heating:DX:SingleSpeed is the only valid type.
-
-#### Field: Component Name
-
-The name of the DX heating coil from the input data file (IDF).
-
-#### Field: High Temperature Heating Standard (Net) Rating Capacity {W}
-
-The standard rating (net) heating capacity for this DX heating coil at high temperature. Units are Watts. See the EnergyPlus Engineering Reference (Single Speed DX Heating Coil, Standard Ratings) for details on how this value is calculated.
-
-#### Field: Low Temperature Heating Standard (Net) Rating Capacity {W}
-
-The standard rating (net) heating capacity for this DX heating coil at low temperature. Units are Watts. See the EnergyPlus Engineering Reference (Single Speed DX Heating Coil, Standard Ratings) for details on how this value is calculated.
-
-#### Field: HSPF {Btu/W-h}
-
-The heating seasonal performance factor (*HSPF*) for the DX heating coil in IP units of Btu/W-h. See the EnergyPlus Engineering Reference (Single Speed DX Heating Coil, Standard Ratings) for details on how this value is calculated.
-
-#### Field: Region Number
-
-The standard region number for which above ratings are calculated (from the input data file).
-
-### Chiller Outputs
-
-Outputs are provided for Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR objects as follows:
-
-```
-! &lt;Chiller Standard Rating Information&gt;, Component Type, Component Name, IPLV in SI Units {W/W}, IPLV in IP Units {Btu/W-h}
-Chiller Standard Rating Information, Chiller:Electric:EIR, Big Chiller 1, 4.5, 15.4
-Chiller Standard Rating Information, Chiller:Electric:ReformulatedEIR, Big Chiller 2, 4.8, 16.4
-```
-
-#### Field: Component Type
-
-This is the component type, Chiller:Electric:EIR and/or Chiller:Electric:ReformulatedEIR.
-
-#### Field: Component Name
-
-The name of the Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR objects from the input data file (IDF).
-
-#### Field: IPLV in SI Units {W/W}
-
-The integrated part load value (*IPLV*) for the Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR in SI units of W/W. See the EnergyPlus Engineering Reference (Electric Chiller Model Based on Condenser Entering Temperature, Standard Ratings) for details on how this value is calculated.
-
-#### Field: IPLV in IP Units {Btu/W-h}
-
-The integrated part load value (*IPLV*) for the Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR in IP units of Btu/W-hr. See the EnergyPlus Engineering Reference (Electric Chiller Model Based on Condenser Entering Temperature, Standard Ratings) for details on how this value is calculated.
-
-### Lookup Table Outputs
-
-**The following fields are shown only when the diagnostics flag is set to DisplayExtraWarnings (ref. Output:Diagnotstics, DisplayAdvancedReportVariables).**
-
-Outputs are provided for lookup tables in two forms. The first being the outputs related to the creation of a performance curve. When the Interpolation Method for table objects is set to EvaluateCurveToLimits, a performance curve object is created. The coefficients of the performance curve are calculated and a curve object is written for review. The regression statistics are also included. This performance curve may be used in subsequent simulations or saved in a library file for future use.
-
-```
-! <CREATING NEW CURVE OBJECT>
-CREATING NEW CURVE OBJECT
-! Input as Table:OneIndependentVariable "HPACCOOLCAPFFF"
-! RSquared       = 1.0000000000
-! Standard Error = 0.0000000000
-! Sample Size    = 3
-Curve:Quadratic,
-FromTable_HPACCOOLCAPFFF,  !- Name
-  0.8000000000,  !- Coefficient1 Constant
-  0.2000000000,  !- Coefficient2 x
-  -3.1086244690E-015,  !- Coefficient3 x**2
-  0.0000000000,  !- Minimum Value of x
-  1.5000000000,  !- Maximum Value of x
-  0.8000000000,  !- Minimum Curve Output
-  1.5000000000;  !- Maximum Curve Output
-END CREATING NEW CURVE OBJECT
-``
-
-A second output form is provided to echo the reading of tabular data. The tabular data is echoed for each multi-variable lookup table object (ref. Table:MultiVariableLookup). The data is echoed using an increasing order sort format regardless of the format specified by the user. In addition, the tabular data is echoed when the data is included in the table object, or when read from an external file. This output form is provided as a verification step when reading tabular data. The normalization point is not included in the raw data varification.
-
-```
-! <READING LOOKUP TABLE DATA&>
-READING LOOKUP TABLE DATA
-! Reading tabular data for Table:MultiVariableLookup "HPACCOOLCAPFFF2"
-  1   3
-  0.000000000000000E+000   1.00000000000000        1.50000000000000
-  0.800000000000000        1.00000000000000        1.10000000000000
-END READING LOOKUP TABLE DATA
-```
-
-### Warmup Days Line
-
-As described elsewhere, EnergyPlus simulates the first day of each simulation period until it reaches “convergence�. This data line will show how many warm up days were required to reach that state.
-
-! &lt;Environment:WarmupDays&gt;, NumberofWarmupDays
-
-Environment:WarmupDays,  6
-
-#### Field: &lt;Environment:WarmupDays&gt;
-
-This is a constant that will display “Environment:WarmupDays�.
-
-#### Field: NumberofWarmupDays
-
-This field will show the number of days required to reach the convergence state for the simulation.
-
-### Warmup Convergence Outputs
-
-Warmup is performed for each environment being simulated. When a file passes convergence, no warnings are shown.  However, when it doesn’t a warning appears in the eplusout.err file, for example:
-
-CheckWarmupConvergence: Loads Initialization, Zone="BACKROOM" did not converge after 25 warmup days.
-
-See Warmup Convergence Information in .eio file for details
-
-...Environment(RunPeriod)="Phoenix Sky Harbor Intl Ap AZ USA TMY3 WMO\#=722780"
-
-..Max Temp Comparison = 8.46E-005 vs Temperature Convergence Tolerance=0.40 - Pass Convergence
-
-..Min Temp Comparison = 7.05E-002 vs Temperature Convergence Tolerance=0.40 - Pass Convergence
-
-..Max Heat Load Comparison = 9.8513E-002 vs Loads Convergence Tolerance=4.00E-002 - Fail Convergence
-
-..Max Cool Load Comparison = 8.2481E-003 vs Loads Convergence Tolerance=4.00E-002 - Pass Convergence
-
-### Warmup Convergence Information
-
-Warmup convergence information reflects the warmup days calculations and whether or not the zone has reached “convergence�. Warmup calculations are done for each environment (e.g. each sizing period simulated, each run period simulated). Reference the building parameters on Minimum and Maximum Number of Warmup Days as well as Loads and Temperature convergence Tolerance. The file contains two possible flavors of warmup information: summary and detailed.
-
-### Summary Warmup Convergence Information
-
-Summary (warmup convergance information is not reported during sizing and only at the end of the calculations). The below information is included after each warmup period.
-
-! &lt;Warmup Convergence Information&gt;,Zone Name,Environment Type/Name,Average Warmup Temperature Difference {deltaC},Std Dev Warmup Temperature Difference {deltaC},Max Temperature Pass/Fail Convergence,Min Temperature Pass/Fail Convergence,Average Warmup Load Difference {W},Std Dev Warmup Load Difference {W},Heating Load Pass/Fail Convergence,Cooling Load Pass/Fail Convergence
-
-Warmup Convergence Information,PLENUM-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\#=725300,0.1459548118,7.6866834879E-002,Pass,Pass,6.4148162842E-002,0.1344412193,Pass,Pass
-
- Warmup Convergence Information,SPACE1-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\#=725300,0.1205887641,0.2962564087,Pass,Pass,0.6840608138,3.7598304674,Pass,Pass
-
- Warmup Convergence Information,SPACE2-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\#=725300,0.1494584750,0.4540146507,Pass,Pass,0.7552649309,3.0925096445,Pass,Pass
-
- Warmup Convergence Information,SPACE3-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\#=725300,0.1150550710,0.2873890950,Pass,Pass,7.0443709912,61.6558566585,Pass,Pass
-
- Warmup Convergence Information,SPACE4-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\#=725300,0.1153798692,0.4838241280,Pass,Pass,2.4744275587,18.1154149427,Pass,Pass
-
- Warmup Convergence Information,SPACE5-1,RunPeriod: Chicago Ohare Intl Ap IL USA TMY3 WMO\#=725300,0.1208173250,0.2114200039,Pass,Pass,0.4984428726,2.8997025264,Pass,Pass
-
-#### Field: Zone Name
-
-This field will show the name of individual zone.
-
-#### Field: Environment Type/Name
-
-Type of environment being run (SizingPeriod, RunPeriod) as well as it’s “name�.
-
-#### Field: Average Warmup Temperature Difference {deltaC}
-
-This field displays the average mean air temperature difference of the zone over the warmup days.
-
-#### Field: Std Dev Warmup Temperature Difference {deltaC}
-
-This field displays the standard deviation of mean air temperature difference of the zone over the warmup days.
-
-#### Field: Max Temperature Pass/Fail Convergence
-
-This field indicates **Pass** or **Fail** for the maximum temperature difference criteria.
-
-#### Field: Min Temperature Pass/Fail Convergence
-
-This field indicates **Pass** or **Fail** for the minimum temperature difference criteria.
-
-#### Field: Average Warmup Load Difference {W}
-
-This field displays the average load difference of the zone over the warmup days.
-
-#### Field: Std Dev Warmup Load Difference {W}
-
-This field displays the standard deviation load difference of the zone over the warmup days.
-
-#### Field: Heating Load Pass/Fail Convergence
-
-This field indicates **Pass** or **Fail** for the heating load criteria.
-
-#### Field: Cooling Load Pass/Fail Convergence
-
-This field indicates **Pass** or **Fail** for the cooling load criteria.
-
-### Detailed Warmup Convergence Information
-
-Detailed warmup convergence information is reported if you add an Output:Diagnostics, ReportDetailedWarmupConvergence; object statement to the input file. It does not include the current environment name or type as it is displayed immediately after the environment details.
-
-! &lt;Warmup Convergence Information&gt;, Zone Name,Time Step,Hour of Day, Warmup Temperature Difference {deltaC}, Warmup Load Difference {W}
-
- Warmup Convergence Information, PLENUM-1,1,1,7.2649997289E-005,0.3830511891
-
- Warmup Convergence Information, SPACE1-1,1,1,1.9871863274E-004,1.6099213169E-002
-
- Warmup Convergence Information, SPACE2-1,1,1,4.2767539998E-003,3.1481614518
-
- Warmup Convergence Information, SPACE3-1,1,1,1.2388614949E-003,5.9934952313
-
- Warmup Convergence Information, SPACE4-1,1,1,2.7512443391E-003,3.9192729035
-
- Warmup Convergence Information, SPACE5-1,1,1,1.7415692658E-003,5.3879887714
-
-#### Field: Zone Name
-
-This field will show the name of individual zone.
-
-#### Field: Time Step
-
-This field will show the value of time step.
-
-#### Field: Hour of Day
-
-This field will show the value of hour of the day.
-
-#### Field: Warmup Temperature Difference
-
-This field will provide a mean air temperature comparison between the second to last and the last warmup day for the simulation.  In other words, it will provide a DT between, for example, 9:10AM on the second to last warmup day and 9:10AM on the last warmup day. The value will be on a zone-by-zone basis for each time step in the simulation.
-
-#### Field: Warmup Load Difference
-
-This field is similar to the previous field except that it displays the heating or cooling load of the zone in question.
-
-eplusout.end
-------------
-
-This is a simple one line synopsis of the simulation. Successful or Not Successful, including number of errors/warnings:
-
-EnergyPlus Completed Successfully-- 8 Warning; 0 Severe Errors
-
-If no file is produced, it is really *not* successful and EnergyPlus has probably crashed during the run. This file and its contents are intended for interfaces that will put friendly front-ends onto EnergyPlus. This file is also used by the EP-Launch program so that it can determine if the run was successful or not – if not, the user should review the eplusout.err file. (Actually, the eplusout.err file should always be reviewed but often is ignored in haste to view the results.)
-
-eplusout.epmidf
----------------
-
-If you use an EPMacro file (usual extension is .imf) as your basis for input, then this file is the “idf� that the EPMacro program produces.
-
-eplusout.epmdet
----------------
-
-If you use an EPMacro file (usual extension is .imf) as your basis for input, then this file is the details of the EPMacro run (including any error messages).
-
-eplusout.err
-------------
-
-This file is *very important* to every simulation run. All of the warnings, errors, etc that occur during the run will show up in this file. They may show up in other files as well. The first line of the error file is also significant:
-
-Program Version,EnergyPlus, &lt;version&gt;,IDD\_Version &lt;version&gt;
-
-This shows not only the current version of the program but the “version� of the Energy+.idd file that was used.
-
-Table 3. EnergyPlus Errors
-
-<table class="table table-striped">
-<tr>
-<th>Error Level</th>
-<th>Action</th>
-</tr>
-<tr>
-<td>Warning</td>
-<td>Take note</td>
-</tr>
-<tr>
-<td>Severe</td>
-<td>Should Fix</td>
-</tr>
-<tr>
-<td>Fatal</td>
-<td>Program will abort</td>
-</tr>
-</table>
-
-The previous table illustrates the three levels of errors that occur in the eplusout.err file. Several other message lines may be shown as well. For example:
-
-\*\* Warning \*\* World Coordinate System selected.  Any non-zero Building/Zone North Axes or non-zero Zone Origins are ignored.
-
-\*\*   ~~~   \*\* These may be used in daylighting reference point coordinate calculations  but not in normal geometry inputs.
-
-The line that includes the “~~~� is a “continue� error line. It continues from the previous line to help describe the context of the error.
-
-Some common errors, their consequences, and what to do about them follows:
-
-\*\* Severe  \*\* IP: Possible incorrect IDD File
-
-\*\* Severe  \*\* IP: Possible Invalid Numerics
-
-\*\*  Fatal  \*\* IP: Errors occurred on processing IDF file. Preceding condition(s) cause termination.
-
-The previous errors cause program termination. The most likely cause is that you have an “old� IDF and have not converted it to work with the current version of the program. In this case, you will likely has some other hints such as alphas in numeric fields or too many fields in an object. Energyplus also has built in range checking:
-
-\*\* Severe  \*\* Out of range value Numeric Field\#7 (Sky Clearness), value=100.00000, range={&gt;=0.0 and &lt;=1.2}, in SIZINGPERIOD:DESIGNDAY=CHICAGO ANN CLG .4% CONDNS WB=&gt;MDB
-
-If these occur during the initial processing of the IDF, you will see a termination clause:
-
-\*\* Severe  \*\* IP: Out of "range" values found in input
-
-\*\* Severe  \*\* IP: Out of "range" values and/or blank required fields found in input
-
-\*\*  Fatal  \*\* IP: Errors occurred on processing IDF file. Preceding condition(s) cause termination.
-
-The error message should supply you with enough information to find the line with the error. More details on error message formatting and some standard error messages are described in the Tips & Tricks document.
-
-eplusout.eso
-------------
-
-The standard output file from EnergyPlus. It includes all the applicable variables selected with the “Output:Variable� commands as well as those with the “Output:Meter� commands. All levels of frequency of reporting are included intermingled as occurs in the running of the program. The form of the file is a data dictionary, followed by the data.
-
-In this case, the dictionary portion of the file comes first followed by an “end of data dictionary line� and then the data makes up the rest of the file.
-
-Thus, the basic structure of the standard output file is:
-
-Data Dictionary Information
-
-End of Data Dictionary
-
-Data
-
-…
-
-Data
-
-End of Data
-
-As with the IDF structure, there are rules associated with the interpretation of the standard output data dictionary. These rules are summarized as follows:
-
-- The first item on each line is an integer which represents the “report code�. This “report code� will be listed in the data section where it will also be the first item on each line, identifying the data. Only 2 lines in the output file will not have an integer as the first item (“End of Data Dictionary� and “End of Data� lines).
-
-- The second item on each line is also an integer. This integer corresponds to the number of items left on the dictionary line. Each string consists of a variable name and units in square brackets. Square brackets are required for all strings. If there are no units associated with a particular variable, then there are no characters between the brackets.
-
-Six standard items appear at the start of every EnergyPlus Standard Output File Data Dictionary:
-
-Program Version,EnergyPlus &lt;version number indicated&gt;
-
-  1,5,Environment Title[],Latitude[deg],Longitude[deg],Time Zone[],Elevation[m]
-
-  2,6,Day of Simulation[],Month[],Day of Month[],DST Indicator[1=yes 0=no],Hour[],StartMinute[],EndMinute[],DayType
-
-  3,3,Cumulative Day of Simulation[],Month[],Day of Month[],DST Indicator[1=yes 0=no],DayType  ! When Daily Report Variables Requested
-
-  4,2,Cumulative Days of Simulation[],Month[]  ! When Monthly Report Variables Requested
-
-  5,1,Cumulative Days of Simulation[] ! When Run Period Report Variables Requested
-
-Item 0 is the program version statement.
-
-Item 1 is produced at the beginning of each new “environment� (design day, run period).
-
-Item 2 is produced prior to any variable reported at the timestep or hourly intervals. Hourly intervals will be shown with a start minute of 0.0 and an end minute of 60.0. Timestep intervals will show the appropriate start and end minutes.
-
-Item 3 is produced prior to any variable reported at the daily interval.
-
-Item 4 is produced prior to any variable reported at the monthly interval.
-
-Item 5 is produced prior to any variable reported at the end of the “environment�.
-
-Following these five standard lines will be the variables requested for reporting from the input file (ref. Report Variable). For example:
-
-6,2,Environment,Site Outdoor Air Drybulb Temperature [C] !Hourly
-
-21,2,ZONE ONE,Zone Mean Air Temperature [C] !Hourly
-
-22,2,ZONE ONE,Zone Total Latent Gain [J] !Hourly
-
-26,2,ZONE ONE,Zone Lights Electric Energy [J] !Hourly
-
-This example illustrates the non-consecutive nature of the “report codes�. Internally, EnergyPlus counts each variable that *could* be reported. This is the assigned “report code�. However, the user may not request each possible variable for reporting. Note that, currently, the requested reporting frequency is shown as a comment (!) line in the standard output file.
-
-The data is produced when the actual simulation is performed (after the warmup days unless the Output:Diagnostics requesting ReportDuringWarmup is used). Data output is simpler in format than the data dictionary lines. From the dictionary above:
-
-     1,DENVER COLORADO WINTER,  39.75,-104.87,  -7.00,1610.26
-
-     2,  1, 1,21, 0, 1, 0.00,60.00,Monday
-
-6,-17.22222
-
-21,-17.22219
-
-22,0.0000000E+00
-
-26,0.0000000E+00
-
-     2,  1, 1,21, 0, 2, 0.00,60.00,Monday
-
-6,-17.22222
-
-21,-17.22219
-
-22,0.0000000E+00
-
-26,0.0000000E+00
-
-     2,  1, 1,21, 0, 3, 0.00,60.00,Monday
-
-6,-17.22222
-
-21,-17.22219
-
-22,0.0000000E+00
-
-26,0.0000000E+00
-
-…
-
-This output file can be easily turned into a form that is read into commonly used spreadsheet programs where it can be further analyzed, graphed, etc.
-
-![](media/image014.png)
-
-Figure 4. Example Chart from Standard Output File
-
-
-
-Program Version,EnergyPlus, &lt;version&gt;
-
-     1,5,Environment Title[],Latitude[deg],Longitude[deg],Time Zone[],Elevation[m]
-
-     2,6,Day of Simulation[],Month[],Day of Month[],DST Indicator[1=yes 0=no],Hour[],StartMinute[],EndMinute[],DayType
-
-     3,3,Cumulative Day of Simulation[],Month[],Day of Month[],DST Indicator[1=yes 0=no],DayType  ! When Daily Report Variables Requested
-
-     4,2,Cumulative Days of Simulation[],Month[]  ! When Monthly Report Variables Requested
-
-     5,1,Cumulative Days of Simulation[] ! When Run Period Report Variables Requested
-
-6,2,Environment, Site Outdoor Air Drybulb Temperature [C] !Hourly
-
-429,2,RESISTIVE ZONE, Zone Air System Sensible Heating Energy [J] !Hourly
-
-450,2,RESISTIVE ZONE, Zone Air System Sensible Cooling Energy [J] !Hourly
-
-458,2,RESISTIVE ZONE, Zone Air Temperature [C] !Hourly
-
-463,2,EAST ZONE, Zone Air System Sensible Heating Energy [J] !Hourly
-
-469,2,EAST ZONE, Zone Air System Sensible Cooling Energy [J] !Hourly
-
-472,2,EAST ZONE, Zone Air Temperature [C] !Hourly
-
-477,2,NORTH ZONE, Zone Air System Sensible Heating Energy [J] !Hourly
-
-483,2,NORTH ZONE, Zone Air System Sensible Cooling Energy [J] !Hourly
-
-486,2,NORTH ZONE, Zone Air Temperature [C] !Hourly
-
-491,2,SimHVAC, HVAC System Solver Iteration Count !Hourly
-
-521,2,SimAir, Air System Simulation Maximum Iteration Count !Hourly
-
-&lt;reduced for brevity&gt;
-
-
-
-End of Data Dictionary
-
-  1,CHANUTE AFB ILLINOIS SUMMER,  40.30, -88.13,  -6.00, 229.51
-
-  2,   1, 7,21, 0, 1, 0.00,60.00,Monday
-
-6,21.2884261500000
-
-429,0.000000000000000E+000
-
-450,0.000000000000000E+000
-
-458,31.1054947436037
-
-463,0.000000000000000E+000
-
-469,0.000000000000000E+000
-
-472,31.2222148107451
-
-477,0.000000000000000E+000
-
-483,0.000000000000000E+000
-
-486,31.5855358697037
-
-Each report variable (ref: eplusout.rdd) is assigned an identification number, as in the line:
-
-486,2,NORTH ZONE,Zone Air Temperature [C] !Hourly
-
-**\#486** is the id number of the Zone/Sys Air Temperature value for the North Zone.
-
-**2** – is the number of parameters on the line
-
-**North Zone** – the identifying “key name� for the line
-
-**Zone Air Temperature [C]** – the actual report variable name along with units [C]
-
-**! Hourly** – the ! is the standard comment character, information following this character reminds the user how frequently this data will appear in the following.
-
-As another example:
-
-Each **Output:Variable** object causes a specific number assignment for outputs. For example, you could request separate reporting for the outside temperature:
-
-Output:Variable,\*, Site Outdoor Air Drybulb Temperature,timestep;
-
-Output:Variable,\*, Site Outdoor Air Drybulb Temperature,hourly;
-
-Output:Variable,\*, Site Outdoor Air Drybulb Temperature,monthly;
-
-And the following would appear in the standard output file:
-
-6,2,Environment,Site Outdoor Air Drybulb Temperature [C] !TimeStep
-
-7,2,Environment,Site Outdoor Air Drybulb Temperature [C] !Hourly
-
-8,2,Environment,Site Outdoor Air Drybulb Temperature [C] !Monthly [Value,Min,Day,Hour,Minute,Max,Day,Hour,Minute]
-
-Item \# 6 will be listed following the TimeStep timestamp for each timestep. Item \#7 will be listed following an hourly timestamp. And item \#8 will be listed following a monthly timestamp and has additional fields (because it is an “average� variable) that show the minimum and maximum values with identifying times for those minimum and maximum. An excerpt will illustrate:
-
-     2,  1, 7,21, 0, 1, 0.00,15.00,Monday** – timestep timestamp**
-
-6,17.08889
-
-48,21.39851
-
-49,0.0000000E+00
-
-53,0.0000000E+00
-
-60,21.87214
-
-     2,  1, 7,21, 0, 1, 0.00,60.00,Monday** – hourly timestamp**
-
-7,16.75555
-
-     4,  1, 7** – monthly timestamp**
-
-8,22.77037,15.00000,21, 4,60,32.77778,21,14,60
-
-To interpret, the first value (\#6) is 17.09 C, \#7 is 16.76 C (average for the hour), and \#8 is 22.77 C, the average for the month with the low (minimum) of 15 C occurring on 7/21 4:60 (or 5:00) and the high (maximum) occurring on 7/21 14:60 (or 15:00).
-
-eplusout.log
-------------
-
-When EnergyPlus is running, it is usually running from a “command� window (unless inside another interface program) and some items may appear in the command window. These messages are preserved in the “log� output file. For example:
-
-```
- EnergyPlus Starting
- EnergyPlus, Version <version>
- Processing Data Dictionary
- Processing Input File
- Warming up
- Initializing Response Factors
- Calculating CTFs for "ROOF-1", Construction #1
- Calculating CTFs for "WALL-1", Construction #2
- Calculating CTFs for "FLOOR-SLAB-1", Construction #6
- Calculating CTFs for "INT-WALL-1", Construction #7
- Initializing Window Optical Properties
- Initializing Solar Calculations
- Initializing HVAC
- Warming up
- Warming up
- Performing Zone Sizing Simulation
- Warming up
- Warming up
- Performing Zone Sizing Simulation
- Calculating System sizing
- Calculating System sizing
- Initializing New Environment Parameters
- Warming up {1}
- Warming up {2}
- Warming up {3}
- Starting Simulation at 01/01 for CHICAGO IL USA TMY2-94846 WMO#=725300
- Updating Shadowing Calculations, Start Date=01/21
- Continuing Simulation at 01/21 for CHICAGO IL USA TMY2-94846 WMO#=725300
- Updating Shadowing Calculations, Start Date=02/10
- Continuing Simulation at 02/10 for CHICAGO IL USA TMY2-94846 WMO#=725300
- Updating Shadowing Calculations, Start Date=03/02
- Continuing Simulation at 03/02 for CHICAGO IL USA TMY2-94846 WMO#=725300
- Updating Shadowing Calculations, Start Date=03/22
- Continuing Simulation at 03/22 for CHICAGO IL USA TMY2-94846 WMO#=725300
-<reduced>
-Updating Shadowing Calculations, Start Date=12/07
- Continuing Simulation at 12/07 for CHICAGO IL USA TMY2-94846 WMO#=725300
- Updating Shadowing Calculations, Start Date=12/27
- Continuing Simulation at 12/27 for CHICAGO IL USA TMY2-94846 WMO#=725300
- EnergyPlus Run Time=00hr 00min 46.00sec
-ReadVarsESO program starting.
-ReadVars Run Time=00hr 00min  1.11sec
-ReadVarsESO program completed successfully.
-ReadVarsESO program starting.
-ReadVars Run Time=00hr 00min  0.00sec
-ReadVarsESO program completed successfully.
-  Started HVAC Diagram
-  Complete
-```
-
-eplusout.mtd
-------------
-
-This file contains the “meter details� for the run. This shows what report variables are on which meters and vice versa – which meters contain what report variables.
-
-The meter details file consists of two parts:
-
-- For report variables that are on meters, it shows all the meters that the report variable is on.  In the following example, “Meters for “ &lt;report variable \#&gt;, &lt;report variable name&gt; is shown and then the meters that accumulate the value of that variable as a “meter�.
-
- Meters for 1240,SPACE1-1:Lights-Electric Energy [J]
-
-  OnMeter=Electricity:Facility [J]
-
-  OnMeter=Electricity:Building [J]
-
-  OnMeter=Electricity:Zone:SPACE1-1 [J]
-
-  OnMeter=InteriorLights:Electricity [J]
-
-  OnMeter=InteriorLights:Electricity:Zone:SPACE1-1 [J]
-
-
-
- Meters for 1460,SPACE1-1:Zone Air System Sensible Heating Energy [J]
-
-  OnMeter=EnergyTransfer:Facility [J]
-
-  OnMeter=EnergyTransfer:Building [J]
-
-  OnMeter=EnergyTransfer:Zone:SPACE1-1 [J]
-
-  OnMeter=Heating:EnergyTransfer [J]
-
-
-
-
-
- Meters for 1557,SPACE1-1 ZONE COIL:Heating Coil Heating Energy [J]
-
-  OnMeter=EnergyTransfer:Facility [J]
-
-  OnMeter=EnergyTransfer:HVAC [J]
-
-  OnMeter=HeatingCoils:EnergyTransfer [J]
-
-
-
-- For each meter, the report variables that make up that meter are shown. In the following example, “For Meter=� &lt;name of meter&gt;, “contents are:� and then each variable that occurs on that “meter� are shown.
-
-For Meter=Electricity:Facility [J], contents are:
-
-  SPACE1-1 LIGHTS 1:Lights Electric Energy
-
-  SPACE2-1 LIGHTS 1:Lights Electric Energy
-
-  SPACE3-1 LIGHTS 1:Lights Electric Energy
-
-  SPACE4-1 LIGHTS 1:Lights Electric Energy
-
-  SPACE5-1 LIGHTS 1:Lights Electric Energy
-
-  SPACE1-1 ELECEQ 1:Electric Equipment Electric Energy
-
-  SPACE2-1 ELECEQ 1:Electric Equipment Electric Energy
-
-  SPACE3-1 ELECEQ 1:Electric Equipment Electric Energy
-
-  SPACE4-1 ELECEQ 1:Electric Equipment Electric Energy
-
-  SPACE5-1 ELECEQ 1:Electric Equipment Electric Energy
-
-  SUPPLY FAN 1:Fan Electric Energy
-
-  CENTRAL CHILLER:Chiller Electric Energy
-
-  HW CIRC PUMP:Pump Electric Energy
-
-  CW CIRC PUMP:Pump Electric Energy
-
-
-
- For Meter=Electricity:Building [J], contents are:
-
-  SPACE1-1 LIGHTS 1:Lights Electric Energy
-
-  SPACE2-1 LIGHTS 1:Lights Electric Energy
-
-  SPACE3-1 LIGHTS 1:Lights Electric Energy
-
-  SPACE4-1 LIGHTS 1:Lights Electric Energy
-
-  SPACE5-1 LIGHTS 1:Lights Electric Energy
-
-  SPACE1-1 ELECEQ 1:Electric Equipment Electric Energy
-
-  SPACE2-1 ELECEQ 1:Electric Equipment Electric Energy
-
-  SPACE3-1 ELECEQ 1:Electric Equipment Electric Energy
-
-  SPACE4-1 ELECEQ 1:Electric Equipment Electric Energy
-
-  SPACE5-1 ELECEQ 1:Electric Equipment Electric Energy
-
-
-
- For Meter=Electricity:Zone:SPACE1-1 [J], contents are:
-
-  SPACE1-1 LIGHTS:Lights Electric Energy
-
-  SPACE1-1 ELECEQ:Electric Equipment Electric Energy
-
-
-
- For Meter=InteriorLights:Electricity [J], contents are:
-
-  SPACE1-1 LIGHTS:Lights Electric Energy
-
-  SPACE2-1 LIGHTS:Lights Electric Energy
-
-  SPACE3-1 LIGHTS:Lights Electric Energy
-
-  SPACE4-1 LIGHTS:Lights Electric Energy
-
-  SPACE5-1 LIGHTS:Lights Electric Energy
-
-
-
-
-
-For Meter=Gas:Facility [J], contents are:
-
-  CENTRAL BOILER:Boiler Gas Energy
-
-
-
- For Meter=Gas:Plant [J], contents are:
-
-  CENTRAL BOILER:Boiler Gas Energy
-
-
-
- For Meter=Heating:Gas [J], contents are:
-
-  CENTRAL BOILER:Boiler Gas Energy
-
-
-
- For Meter=Electricity:Plant [J], contents are:
-
-  CENTRAL CHILLER:Chiller Electric Energy
-
-  HW CIRC PUMP:Pump Electric Energy
-
-  CW CIRC PUMP:Pump Electric Energy
-
-
-
- For Meter=Cooling:Electricity [J], contents are:
-
-  CENTRAL CHILLER:Chiller Electric Energy
-
-
-
- For Meter=Cooling:EnergyTransfer [J], contents are:
-
-  PLENUM-1:Zone Air System Sensible Cooling Energy
-
-  SPACE1-1:Zone Air System Sensible Cooling Energy
-
-  SPACE2-1:Zone Air System Sensible Cooling Energy
-
-  SPACE3-1:Zone Air System Sensible Cooling Energy
-
-  SPACE4-1:Zone Air System Sensible Cooling Energy
-
-  SPACE5-1:Zone Air System Sensible Cooling Energy
-
-
-
-
-
-
-
-As further illustration, an abbreviated example shows:
-
-Meters for 6,EAST ZONE LIGHTS 1:Lights Electric Energy [J]
-
-  OnMeter=Electricity:Facility [J]
-
-  OnMeter=Electricity:Building [J]
-
-  OnMeter=Electricity:Zone:EAST ZONE [J]
-
-  OnMeter=InteriorLights:Electricity [J]
-
-  OnMeter=InteriorLights:Electricity:Zone:EAST ZONE [J]
-
-  OnMeter=GeneralLights:InteriorLights:Electricity [J]
-
-
-
-For Meter=Electricity:Facility [J], ResourceType=Electricity, contents are:
-
-  EAST ZONE LIGHTS 1:Lights Electric Energy
-
-  NORTH ZONE LIGHTS 1:Lights Electric Energy
-
-  WEST ZONE ELECEQ 1:Electric Equipment Electric Energy
-
-  EAST ZONE ELECEQ 1:Electric Equipment Electric Energy
-
-  NORTH ZONE ELECEQ 1:Electric Equipment Electric Energy
-
-  SUPPLY FAN 1:Fan Electric Energy
-
-  LITTLE CHILLER:Chiller Electric Energy
-
-  BIG CHILLER:Chiller Electric Energy
-
-  BIG TOWER:Cooling Tower Fan Electric Energy
-
-  CIRC PUMP:Pump Electric Energy
-
-  COND CIRC PUMP:Pump Electric Energy
-
-  HW CIRC PUMP:Pump Electric Energy
-
-This shows the meters on which the Zone: Lights Electric Energy appear as well as the contents of the Electricity:Facility meter.
-
-eplusout.mtr
-------------
-
-This is the equivalent file to the eplusout.eso file but contains only the Report Meter requests. The format and style of the file is identical to the eplusout.eso file.
-
-eplusout.rdd
-------------
-
-This file (from the **Output:VariableDictionary,regular;** and **Output:VariableDictionary,IDF;** commands) shows all the report variables along with their “availability� for the current input file. Each simulation *may have* different output variables though some are constant (for example the environmental/outdoor variables! A user must first run the simulation (at least semi-successfully) before the available output variables are known. This output file is available in two flavors: regular (listed as they are in the Input Output Reference) and IDF (ready to be copied and pasted into your Input File). Once this file is generated, the IDF editor can use them for Output:Variable keys. You can also ask for the outputs to be sorted by name.
-
-Output:VariableDictionary,regular,Name;
-
-“**Zone**� variables are calculated and can be reported after each Zone/Heat Balance timestep (ref: TimeSteps in Hour command). “**HVAC**� variables are calculated and can be reported with each variable HVAC timestep. “Average� variables will be averaged over the time interval being reported whereas “sum� variables are summed over that time interval.
-
-There are two mitigating factors for this output variable list. One is the “Advanced Report Variables� and the other is the “Create Minimal Surface Variables�.
-
-### Normal Output Variables – regular format
-
-A typical rdd file might be:
-
-Program Version,EnergyPlus, &lt;version&gt;, &lt;date/time of run&gt;,IDD\_Version &lt;IDD Version&gt;
-
-Var Type (reported timestep),Var Report Type,Variable Name [Units]
-
-Zone,Average,Site Outdoor Air Drybulb Temperature [C]
-
-Zone,Average,Site Outdoor Air Dewpoint Temperature [C]
-
-Zone,Average,Site Outdoor Air Wetbulb Temperature [C]
-
-Zone,Average,Site Outdoor Air Humidity Ratio [kgWater/kgAir]
-
-Zone,Average,Site Outdoor Air Relative Humidity [%]
-
-Zone,Average,Site Outdoor Air Barometric Pressure [Pa]
-
-Zone,Average,Site Wind Speed [m/s]
-
-Zone,Average,Site Wind Direction [deg]
-
-Zone,Average,Site Sky Temperature [C]
-
-Zone,Average,Site Diffuse Solar Radiation Rate per Area [W/m2]
-
-Zone,Average,Site Direct Solar Radiation Rate per Area [W/m2]
-
-Zone,Average,Site Ground Reflected Solar Radiation Rate per Area [W/m2]
-
-Zone,Average,Site Ground Temperature [C]
-
-&lt;reduced&gt;
-
-
-
-Zone,Average,Surface Window Transmitted Solar Radiation Rate[W]
-
-Zone,Average,Surface Window Transmitted Beam Solar Radiation Rate[W]
-
-Zone,Average,Surface Window Transmitted Diffuse Solar Radiation Rate[W]
-
-Zone,Average,Zone Windows Total Heat Gain Rate[W]
-
-Zone,Average,Zone Windows Total Heat Loss Rate[W]
-
-Zone,Average,Surface Window Gap Convective Heat Transfer Rate[W]
-
-Zone,Average,Surface Window Shading Device Absorbed Solar Radiation Rate[W]
-
-&lt;reduced&gt;
-
-
-
-HVAC,Average,System Node Temperature [C]
-
-HVAC,Average,System Node Mass Flow Rate[kg/s]
-
-HVAC,Average,System Node Humidity Ratio[]
-
-HVAC,Average,System Node Setpoint Temperature[C]
-
-HVAC,Average,System Node Setpoint Temperature Hi[C]
-
-HVAC,Average,System Node Setpoint Temperature Lo[C]
-
-HVAC,Average,System Node Setpoint Humidity Ratio[kgWater/kgDryAir]
-
-HVAC,Average,System Node Setpoint Minimum Humidity Ratio[kgWater/kgDryAir]
-
-HVAC,Average,System Node Setpoint Maximum Humidity Ratio[kgWater/kgDryAir]
-
-HVAC,Average,System Node Current Density Volume Flow Rate[m3/s]HVAC,Average,System Node Enthalpy[J/kg]
-
-HVAC,Average,System Node Wetbulb Temperature[C]
-
-&lt;reduced&gt;
-
-
-
-HVAC,Sum, Zone Mechanical Ventilation No Load Heat Removal Energy [J]
-
-HVAC,Sum,Zone Mechanical Ventilation Cooling Load Increase Energy [J]
-
-HVAC,Sum, Zone Mechanical Ventilation Cooling Load Increase Due to Overheating Energy [J]
-
-HVAC,Sum,Zone Mechanical Ventilation Cooling Load Decrease Energy [J]
-
-HVAC,Sum,Zone Mechanical Ventilation No Load Heat Addition [J]
-
-HVAC,Sum,Zone Mechanical Ventilation Heating Load Increase Energy [J]
-
-HVAC,Sum, Zone Mechanical Ventilation Heating Load Increase Due to Overcooling Energy[J]
-
-HVAC,Sum,Zone Mechanical Ventilation Heating Load Decrease Energy [J]
-
-HVAC,Average,Zone Mechanical Ventilation Mass Flow Rate [kg/s]
-
-HVAC,Average, Zone Mechanical Ventilation Standard Density Volume Flow Rate [m3/s]
-
-HVAC,Sum,Zone Mechanical Ventilation Standard Density Volume [m3]
-
-HVAC,Sum,Zone Mechanical Ventilation Mass [kg]
-
-HVAC,Average,Zone Mechanical Ventilation Air Changes per Hour [ach]
-
-
-
-### Normal Output Variables – regular format – sorted by name
-
-The same variables but now sorted alphabetically by name.
-
-Program Version,EnergyPlus, &lt;version&gt;, &lt;date/time of run&gt;,IDD\_Version &lt;IDD Version&gt;
-
-Var Type (reported time step),Var Report Type,Variable Name [Units]
-
-HVAC,Sum,Air System Solver Iteration Count []
-
-HVAC,Sum,Environmental Impact Total CH4 Emissions Carbon Equivalent Mass [kg]
-
-HVAC,Sum,Environmental Impact Total CO2 Emissions Carbon Equivalent Mass [kg]
-
-HVAC,Sum, Environmental Impact Total N2O Emissions Carbon Equivalent Mass [kg]
-
-Zone,Sum,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Energy [J]
-
-Zone,Sum,Surface Inside Face Interior Windows Incident Beam Solar Radiation Energy [J]
-
-Zone,Average,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate [W]
-
-Zone,Average,Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate [W]
-
-Zone,Average,Surface Inside Face Exterior Windows Incident Beam Solar Radiation Rate per Area [W/m2]
-
-Zone,Average, Surface Inside Face Interior Windows Incident Beam Solar Radiation Rate per Area [W/m2]
-
-### Normal Output Variables – IDF format
-
-A brief excerpt of the IDF format is shown below. These can be copied and pasted directly into an IDF or used from the IDF Editor.
-
-! Program Version, &lt;version&gt;, &lt;date/time of run&gt;,IDD\_Version &lt;IDD version&gt;
-
-! Output:Variable Objects (applicable to this run)
-
-Output:Variable,\*,Site Outdoor Air Drybulb Temperature,hourly; !- Zone Average [C]
-
-Output:Variable,\*,Site Outdoor Air Dewpoint Temperature,hourly; !- Zone Average [C]
-
-Output:Variable,\*,Site Outdoor Air Wetbulb Temperature,hourly; !- Zone Average [C]
-
-Output:Variable,\*,Site Outdoor Air Humidity Ratio,hourly; !- Zone Average [kgWater/kgDryAir]
-
-Output:Variable,\*,Site Outdoor Air Relative Humidity,hourly; !- Zone Average [%]
-
-Output:Variable,\*,Site Outdoor Air Barometric Pressure,hourly; !- Zone Average [Pa]
-
-Output:Variable,\*,Site Wind Speed,hourly; !- Zone Average [m/s]
-
-Output:Variable,\*,Site Wind Direction,hourly; !- Zone Average [deg]
-
-### Advanced Output Variables
-
-The DisplayAdvancedReportVariables key to the Output:Diagnostics object adds a number of variables that may need special handling or understanding of the users. Search on the Input Output Reference document for DisplayAdvancedReportVariables for more details.
-
-eplusout.mdd
-------------
-
-This file (from the **Output:VariableDictionary,regular;** and **Output:VariableDictionary,IDF;** commands) shows all the report meters along with their “availability� for the current input file. A user must first run the simulation (at least semi-successfully) before the available output meters are known. This output file is available in two flavors: **regular** (listed as they are in the Input Output Reference) and **IDF** (ready to be copied and pasted into your Input File). Once this file is generated, the IDF editor can use them for Output:Meter and Output:CumulativeMeter keys.
-
-Note that meters are always accumulated to the Zone timestep. They are always “summed� variables.
-
-### Meter Variables – regular format
-
-Program Version,EnergyPlus &lt;version&gt;, &lt;date time of run&gt;,IDD\_Version &lt;IDD Version&gt;
-
-Var Type (reported timestep),Var Report Type,Variable Name [Units]
-
-Zone,Meter,Electricity:Facility [J]
-
-Zone,Meter,Electricity:Building [J]
-
-Zone,Meter,Electricity:Zone:SOUTHZONE\_1STFLOOR [J]
-
-Zone,Meter,InteriorLights:Electricity [J]
-
-Zone,Meter,InteriorLights:Electricity:Zone:SOUTHZONE\_1STFLOOR [J]
-
-Zone,Meter,GeneralLights:InteriorLights:Electricity [J]
-
-&lt;reduced&gt;
-
-
-
-Note that custom meters also appear on this file:
-
-Zone,Meter,MYGENERALLIGHTS [J]
-
-Zone,Meter,MYBUILDINGELECTRIC [J]
-
-Zone,Meter,MYBUILDINGOTHER [J]
-
-### Meter Variables – regular format – sorted by name
-
-The meter variable file can also be sorted by name. If the rdd is sorted by name, then the meter mdd file will be as well.
-
-Program Version,EnergyPlus &lt;version&gt;, &lt;date time of run&gt;,IDD\_Version &lt;IDD Version&gt;
-
-Var Type (reported time step),Var Report Type,Variable Name [Units]
-
-Zone,Meter,Carbon Equivalent:Facility [kg]
-
-Zone,Meter,CarbonEquivalentEmissions:Carbon Equivalent [kg]
-
-Zone,Meter,Cogeneration:ElectricityNet [J]
-
-Zone,Meter,Cogeneration:ElectricityPurchased [J]
-
-Zone,Meter,Cogeneration:ElectricitySurplusSold [J]
-
-&lt;snip&gt;
-
-### Meter Variables – IDF format
-
-This report produces the variable names in a form that are ready to be merged into an input file. By design, hourly reporting is selected – replace this with your desired frequency. An example of the results:
-
-! Program Version, &lt;version&gt;, &lt;date/time of run&gt;, IDD\_Version &lt;IDD version&gt;
-
-! Output:Meter Objects (applicable to this run)
-
-Output:Meter,DistrictHeating:Facility,hourly; !- [J]
-
-Output:Meter:Cumulative,DistrictHeating:Facility,hourly; !- [J]
-
-Output:Meter,DistrictHeating:HVAC,hourly; !- [J]
-
-Output:Meter:Cumulative,DistrictHeating:HVAC,hourly; !- [J]
-
-Output:Meter,Heating:DistrictHeating,hourly; !- [J]
-
-Output:Meter:Cumulative,Heating:DistrictHeating,hourly; !- [J]
-
-Output:Meter,DistrictCooling:Facility,hourly; !- [J]
-
-Output:Meter:Cumulative,DistrictCooling:Facility,hourly; !- [J]
-
-Output:Meter,DistrictCooling:HVAC,hourly; !- [J]
-
-Output:Meter:Cumulative,DistrictCooling:HVAC,hourly; !- [J]
-
-### Meter Naming Convention
-
-To repeat some of the detail described in the Input Output Reference document:
-
-Meter names are of three forms:
-
-- &lt;ResourceType&gt;:&lt;name&gt;
-
-Or
-
-- &lt;EndUseType&gt;:&lt;ResourceType&gt;:&lt;name&gt;
-
-Or
-
-- &lt;EndUseSubcategory&gt;:&lt;EndUseType&gt;:&lt;ResourceType&gt;:&lt;name&gt;.
-
-The user requests reporting by either specifying the full name above (without Units) or a “wildcard� representation of that name (to obtain all meters of a type). For example, entering “Electricity:\*� for the meter name will report on all the Electricity: meters (Electricity:Facility, Electricity:Building, Electricity:Zone:Resistive Zone, Electricity:Zone:East Zone, Electricity:North Zone in the example above). Both the resource types and end-use types are set within the program by the developers. End-use subcategories are user-defined and are an input field for certain objects.
-
-To summarize the previous paragraph, you could use:
-
-Output:Meter,Electricity:\*;
-
-To get the same outputs as if you had entered:
-
-Output:Meter,Electricity:Facility;
-
-Output:Meter,Electricity:Building;
-
-Output:Meter,Electricity:Zone:South Zone;
-
-Output:Meter,Electricity:Zone:East Zone;
-
-Output:Meter,Electricity:North Zone;
-
-From a three zone file that had no HVAC electricity (i.e., had only electric equipment or lighting equipment in an uncontrolled three zone building).
-
-Current resource types are shown in the table below:
-
-Table 4. Table of Metered Resource  Types
-
-<table class="table table-striped">
-<tr>
- <th>Utility/Fuel Types</th>
-</tr>
-<tr>
- <td>Electricity</td>
- <td>Gas</td>
- <td>Gasoline</td>
- <td>Diesel</td>
- <td>Coal</td>
- <td>FuelOil\#1</td>
- <td>FuelOil\#2</td>
- <td>Propane</td>
- <td>Water</td>
- <td>Steam</td>
- <td>DistrictCooling</td>
- <td>DistrictHeating</td>
-</tr>
-</table>
-
-<table class="table table-striped">
-<tr>
-<th>Other Resource Types</th>
-</tr>
-<tr>
-<td>EnergyTransfer</td>
-</tr>
-</table>
-
-The end use types are shown in the following table (note that certain end use types apply only to the EnergyTransfer resource):
-
-The end use types are shown in the following table:
-
-Table 5. End Use Category Types
-
-<table class="table table-striped">
- <tr>
-  <th>End Use Types</th>
- </tr>
- <tr>
-  <td>InteriorLights</td>
-  <td>ExteriorLights</td>
-  <td>InteriorEquipment</td>
-  <td>ExteriorEquipment</td>
-  <td>Fans</td>
-  <td>Pumps</td>
-  <td>Heating</td>
-  <td>Cooling</td>
-  <td>HeatRejection</td>
-  <td>Humidifier</td>
-  <td>HeatRecovery</td>
-  <td>DHW</td>
-  <td>Cogeneration</td>
-  <td>Refrigeration</td>
-  <td>Miscellaneous</td>
- </tr>
-</table>
-
-<table class="table table-striped">
- <tr>
-  <th>Additional End Use Types Only Used for EnergyTransfer</th>
- </tr>
- <tr>
-  <td>HeatingCoils</td>
-  <td>CoolingCoils</td>
-  <td>Chillers</td>
-  <td>Boilers</td>
-  <td>Baseboard</td>
-  <td>HeatRecoveryForCooling</td>
-  <td>HeatReoveryFor Heating</td>
- </tr>
-</table>
-
-Specific meter types are then used for grouping the fuel type meters:
-
-Table 6. Overall Meter Types
-
-<table class="table table-striped">
-<tr>
-<th>Meters</th>
-</tr>
-<tr>
-<td>Facility</td>
-</tr>
-<tr>
-<td>Building</td>
-</tr>
-<tr>
-<td>Zone</td>
-</tr>
-<tr>
-<td>System</td>
-</tr>
-<tr>
-<td>Plant</td>
-</tr>
-</table>
-
-Facility meters contain all the energy of a fuel type. Building meters contain the sum of each zone’s energy. System meters contain the energy from the system components. Plant meters contain the energy from the plant equipments.
-
-Thus, the following relationships should be observed:
-
-<div>\[ \text{Facility} = \sum\left(\text{Building} + \text{System} + \text{Plant} + \text{Exterior}\right) \]</div>
-
-<div>\[ \text{Building} = \sum_{i}^{\#Zones} \text{Zone} \]</div>
-
-Custom Meters, (review Input Output Reference, objects: **Meter:Custom** and **Meter:CustomDecrement**) for further requirements, are reported in the same way as pre-defined meters.
-
-For example, one might put the Building Infiltration Heat Loss & Heat Gain on a set of custom meters:
-
-```
-  Meter:Custom,
-    Building Infiltration Heat Loss,  !- Name
-    Generic,             !- Fuel Type
-    *,                       !- Key Name 1
-    Zone Infiltration Total Heat Loss Energy;  !- Output Variable Name 1
-
-  Meter:Custom,
-    Building Infiltration Heat Gain,  !- Name
-    Generic,             !- Fuel Type
-    *,                       !- Key Name 1
-    Zone Infiltration Total Heat Gain Energy;  !- Output Variable Name 1
-```
-
-One can then report these values the same way one reports other standard meters.
-
-
-
-eplusout.shd
-------------
-
-This file contains details of the shadow casting, back and receiving surfaces for the building. The [Engineering Reference](file:///E:\Docs4PDFs\EngineeringReference.pdf) explains the shadowing calculations in more detail; this report file merely shows the level of interactions that the calculations will use. The report shows the Solar Distribution algorithm (in the example Full Interior and Exterior) and then proceeds to illustrate which surfaces shade (possibly) which other surfaces.
-
-Note, a casting surface -- a shadow casting surface or general casting surface (so called in the file) -- is one that casts a shadow on other surfaces. A receiving surface - a shadow receiving surface -- is one that receives shadows from other surfaces (i.e. casting surfaces). A back surface -- an inside surface -- is one that may be partially sunlit/receive solar transmission for interior solar distribution.
-
-An example follows:
-
-Shadowing Combinations
-
-..Solar Distribution=FullInteriorAndExterior
-
- ==================================
-
- Surface=ZN001:WALL001 is used as Receiving Surface in calculations.
-
- Number of general casting surfaces=           0
-
- Number of back surfaces=           5
-
- ...Surface=ZN001:WALL002
-
- ...Surface=ZN001:WALL003
-
- ...Surface=ZN001:WALL004
-
- ...Surface=ZN001:FLR001
-
- ...Surface=ZN001:ROOF001
-
- Number of receiving sub surfaces=           1
-
- ....Surface=ZN001:WALL001:WIN001
-
- ==================================
-
- Surface=ZN001:WALL001:WIN001 is not used as Receiving Surface in calculations.
-
- Number of general casting surfaces=           0
-
- Number of back surfaces=           0
-
- Number of receiving sub surfaces=           0
-
-
-
- ==================================
-
- Surface=ZN001:WALL002 is used as Receiving Surface in calculations.
-
- Number of general casting surfaces=           0
-
- Number of back surfaces=           0
-
- Number of receiving sub surfaces=           0
-
- ==================================
-
- Surface=ZN001:WALL003 is not used as Receiving Surface in calculations.
-
- Number of general casting surfaces=           0
-
- Number of back surfaces=           0
-
- Number of receiving sub surfaces=           0
-
- ==================================
-
- Surface=ZN001:WALL004 is not used as Receiving Surface in calculations.
-
- Number of general casting surfaces=           0
-
- Number of back surfaces=           0
-
- Number of receiving sub surfaces=           0
-
- ==================================
-
- Surface=ZN001:FLR001 is not used as Receiving Surface in calculations.
-
- Number of general casting surfaces=           0
-
- Number of back surfaces=           0
-
- Number of receiving sub surfaces=           0
-
- ==================================
-
- Surface=ZN001:ROOF001 is used as Receiving Surface in calculations.
-
- Number of general casting surfaces=           0
-
- Number of back surfaces=           0
-
- Number of receiving sub surfaces=           0
-
-eplusout.sln
-------------
-
-The following shows an excerpt of “lines� report (**eplusout.sln**) for a single surface. It gives the surface name and then the coordinates in the “standard� EnergyPlus fashion (that is, UpperLeftCorner first and proceeding around, in this case, the four vertices in the surface.
-
-SPACE1-1:MAIN SOUTH OVERHANG
-
-     -0.65,     -1.13,      2.20,      0.00,      0.00,      2.20
-
-      0.00,      0.00,      2.20,     17.15,     -9.90,      2.20
-
-     17.15,     -9.90,      2.20,     16.50,    -11.03,      2.20
-
-     16.50,    -11.03,      2.20,     -0.65,     -1.13,      2.20
-
-The following shows an excerpt of “lines, IDF� report (**eplusout.sln**) for a single surface. It gives the coordinates in the “standard� EnergyPlus fashion (that is, UpperLeftCorner first and proceeding around, in this case, the four vertices in the surface. Note that this is NOT a complete description of the surface but enough to change your IDF file, if you want to.
-
-Building North Axis = 0
-
-GlobalGeometryRules,UpperLeftCorner,CounterClockwise,WorldCoordinates;
-
- Surface=SHADING, Name=ROOMSOUTH SURF6-VFIN1-6
-
-  4,  !- Number of (X,Y,Z) groups in this surface
-
-      -23.34,    -14.85,      2.41,  !- X,Y,Z ==&gt; Vertex 1
-
-      -23.34,    -14.76,      2.49,  !- X,Y,Z ==&gt; Vertex 2
-
-      -18.13,    -14.76,      2.49,  !- X,Y,Z ==&gt; Vertex 3
-
-      -18.13,    -14.85,      2.41;  !- X,Y,Z ==&gt; Vertex 4
-
- Surface=WALL, Name=ROOMNORTH SURF3-1
-
-  4,  !- Number of (X,Y,Z) groups in this surface
-
-      -15.94,     -5.34,      3.00,  !- X,Y,Z ==&gt; Vertex 1
-
-      -15.94,     -5.34,      0.00,  !- X,Y,Z ==&gt; Vertex 2
-
-      -18.91,     -5.34,      0.00,  !- X,Y,Z ==&gt; Vertex 3
-
-      -18.91,     -5.34,      3.00;  !- X,Y,Z ==&gt; Vertex 4
-
- Surface=WALL, Name=ROOMNORTH SURF4-1
-
-  4,  !- Number of (X,Y,Z) groups in this surface
-
-      -18.91,     -5.34,      3.00,  !- X,Y,Z ==&gt; Vertex 1
-
-      -18.91,     -5.34,      0.00,  !- X,Y,Z ==&gt; Vertex 2
-
-      -22.65,     -5.34,      0.00,  !- X,Y,Z ==&gt; Vertex 3
-
-      -22.65,     -5.34,      3.00;  !- X,Y,Z ==&gt; Vertex 4
-
- Surface=WINDOW, Name=ROOMNORTH SURF5-1-NOSHADE
-
-  4,  !- Number of (X,Y,Z) groups in this surface
-
-      -19.02,     -5.34,      2.59,  !- X,Y,Z ==&gt; Vertex 1
-
-      -19.02,     -5.34,      0.41,  !- X,Y,Z ==&gt; Vertex 2
-
-      -22.54,     -5.34,      0.41,  !- X,Y,Z ==&gt; Vertex 3
-
-      -22.54,     -5.34,      2.59;  !- X,Y,Z ==&gt; Vertex 4
-
-
-
-eplusout.sql
-------------
-
-eplusout.sql is an optional output format for EnergyPlus. The eplusout.sql output file is a sqlite3 database file (see http://www.sqlite.org) and includes all of the data found in EnergyPlus’ eplustbl.\* files, eplusout.eso and eplusout.mtr output files (i.e., EnergyPlus’ standard variable and meter output files) plus a number of reports that are found in the eplusout.eio output file.
-
-A discussion of the individual data tables is presented below followed by a discussion about how to access data within the SQL file.
-
-### List of Available SQLite Tables
-
-This initial release of the SQL database output option includes a variety of data in the following tables:
-
-- ComponentSizes Table
-
-- ConstructionLayers Table
-
-- Constructions Table
-
-- Materials Table
-
-- NominalBaseboardHeaters Table
-
-- NominalElectricEquipment Table
-
-- NominalGasEquipment Table
-
-- NominalHotWaterEquipment Table
-
-- NominalInfiltration Table
-
-- NominalLighting Table
-
-- NominalOtherEquipment Table
-
-- NominalPeople Table
-
-- NominalSteamEquipment Table
-
-- NominalVentilation Table
-
-- ReportData Table
-
-- ReportDataDictionary Table
-
-- ReportExtendedData Table
-
-- RoomAirModels Table
-
-- Schedules Table
-
-- Surfaces Table
-
-- SystemSizes Table
-
-- Time Table
-
-- ZoneGroups Table
-
-- Zones Table
-
-- ZoneLists Table
-
-- ZoneSizes Table
-
-- ZoneInfoLists Table
-
-- [Simulations](#_Simulations_Table_1)Table
-
-- [EnvironmentPeriods](#_EnvironmentPeriods_Table)Table
-
-- TabularData Table
-
-- [Strings](#_Strings_Table)Table
-
-- [StringTypes](#_StringTypes_Table)Table
-
-- [TabularDataWithStrings](#_TabularDataWithStrings_Table)Table
-
-- Errors Table
-
-A short discussion of contents of each of the above SQL tables is given in the sections that follow.
-
-### Report Data
-
-Data in the following four tables are also found in EnergyPlus’ standard output file (i.e., eplusout.eso – see that section for more information) or in EnergyPlus' eplusout.mtr (i.e. meter) output file. As with the standard output file, the “Report Variable� and “Report Meter� commands control the data in these tables.
-
-#### ReportDataDictionary Table
-
-The ReportDataDictionary table provides the equivalent of the dictionary portion of the ESO file (i.e., the first section of the .eso file) or eplusout.mtr. Please see the Report Variable section of the Input-Output Reference for more information.  Like in the eplusout.mtr file (see the eplusout.mtr section), only data requested by "Report Meter" commands will set isMeter to 1 or True.
-
-
-
-<table class="table table-striped">
-<caption>Table 7. SQL ReportDataDictionary Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-<th>Enumeration</th>
-</tr>
-<tr>
-<td>ReportDataDictionaryIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>The ReportDataDictionaryIndex links the dictionary data to the variable data (see ReportData table)</td>
-<td> </td>
-</tr>
-<tr>
-<td>IsMeter</td>
-<td>INTEGER</td>
-<td>Boolean flag whether dictionary data is report of meter data</td>
-<td>0, 1</td>
-</tr>
-<tr>
-<td>Type</td>
-<td>TEXT</td>
-<td>Nature of data type with respect to state, (e.g. average or sum type of data).</td>
-<td>“Sum� “Avg�</td>
-</tr>
-<tr>
-<td>IndexGroup</td>
-<td>TEXT</td>
-<td>The reporting group (e.g., Zone, Plant, etc.)</td>
-<td> </td>
-</tr>
-<tr>
-<td>TimestepType</td>
-<td>TEXT</td>
-<td>Type of timestep for data</td>
-<td>“Zone�
-“HVAC System�</td>
-</tr>
-<tr>
-<td>KeyValue</td>
-<td>TEXT</td>
-<td>The identifying “key name� for the data</td>
-<td> </td>
-</tr>
-<tr>
-<td>Name</td>
-<td>TEXT</td>
-<td>The actual report data name</td>
-<td> </td>
-</tr>
-<tr>
-<td>ReportingFrequency</td>
-<td>TEXT</td>
-<td>The reporting frequency of the variable, e.g.</td>
-<td>“HVAC System Timestep�,  “Zone Timestep�,  “Hourly�, “Daily�, “Monthly�, “Run Period�.</td>
-</tr>
-<tr>
-<td>ScheduleName</td>
-<td>TEXT</td>
-<td>The name of the schedule that controls reporting frequency</td>
-<td> </td>
-</tr>
-<tr>
-<td>Units</td>
-<td>TEXT</td>
-<td>The data units</td>
-<td> </td>
-</tr>
-</table>
-
-#### ReportData Table
-
-The ReportData table contains the report or meter variable data (e.g., the hourly, daily, and monthly report variable data). Please see the Report Variable section of the Input-Output Reference for more information.
-
-
-
-<table class="table table-striped">
-<caption>Table 8. SQL ReportData Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ReportDataIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td></td>
-</tr>
-<tr>
-<td>TimeIndex</td>
-<td>INTEGER</td>
-<td>This index links the record to its time record (see the Time table below)</td>
-</tr>
-<tr>
-<td>ReportDataDictionaryIndex</td>
-<td>INTEGER</td>
-<td>The ReportDataDictionaryIndex links the data to the respective data dictionary record (see ReportDataDictionary table above)</td>
-</tr>
-<tr>
-<td>Value</td>
-<td>REAL</td>
-<td>The data value</td>
-</tr>
-</table>
-
-#### ReportExtendedData Table
-
-The ReportExtendedData table contains additional data (e.g., monthly maximums and minimums) that is available for certain report or meter variables.
-
-
-
-<table class="table table-striped">
-<caption>Table 9. SQL ReportExtendedData Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ReportExtendedDataIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td></td>
-</tr>
-<tr>
-<td>ReportDataIndex</td>
-<td>INTEGER</td>
-<td>Associates ReportData record with ReportExtendedData record</td>
-</tr>
-<tr>
-<td>MaxValue</td>
-<td>REAL</td>
-<td>The maximum value during the reporting interval</td>
-</tr>
-<tr>
-<td>MaxMonth</td>
-<td>INTEGER</td>
-<td>The month in which the maximum value occurred</td>
-</tr>
-<tr>
-<td>MaxDay</td>
-<td>INTEGER</td>
-<td>The day on which the maximum value occurred</td>
-</tr>
-<tr>
-<td>MaxHour</td>
-<td>INTEGER</td>
-<td>The hour in which the maximum value occurred</td>
-</tr>
-<tr>
-<td>MaxStartMinute</td>
-<td>INTEGER</td>
-<td>The starting minute of the interval in which the maximum value occurred</td>
-</tr>
-<tr>
-<td>MaxMinute</td>
-<td>INTEGER</td>
-<td>The minute that the maximum value occurred</td>
-</tr>
-<tr>
-<td>MinValue</td>
-<td>REAL</td>
-<td>The minimum value</td>
-</tr>
-<tr>
-<td>MinMonth</td>
-<td>INTEGER</td>
-<td>The month in which the minimum value occurred</td>
-</tr>
-<tr>
-<td>MinDay</td>
-<td>INTEGER</td>
-<td>The day on which the minimum value occurred</td>
-</tr>
-<tr>
-<td>MinHour</td>
-<td>INTEGER</td>
-<td>The hour in which the minimum value occurred</td>
-</tr>
-<tr>
-<td>MinStartMinute</td>
-<td>INTEGER</td>
-<td>The starting minute of the interval in which the minimum value occurred</td>
-</tr>
-<tr>
-<td>MinMinute</td>
-<td>INTEGER</td>
-<td>The minute that the minimum value occurred</td>
-</tr>
-</table>
-
-#### Time Table
-
-The Time table provides the time information for both the “report variable� and “report meter� variables (the ReportData table).
-
-
-
-<table class="table table-striped">
-<caption>Table 10. Time Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>TimeIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Connects the time information with the report variables and meter variables (see the ReportData table)</td>
-</tr>
-<tr>
-<td>Month</td>
-<td>INTEGER</td>
-<td>Month</td>
-</tr>
-<tr>
-<td>Day</td>
-<td>INTEGER</td>
-<td>Day</td>
-</tr>
-<tr>
-<td>Hour</td>
-<td>INTEGER</td>
-<td>Hour</td>
-</tr>
-<tr>
-<td>Minute</td>
-<td>INTEGER</td>
-<td>Minute</td>
-</tr>
-<tr>
-<td>DST</td>
-<td>INTEGER</td>
-<td>Daylight saving time indicator</td>
-</tr>
-<tr>
-<td>Interval</td>
-<td>INTEGER</td>
-<td>Length of the reporting interval</td>
-</tr>
-<tr>
-<td>IntervalType</td>
-<td>INTEGER</td>
-<td>The index for the type of reporting interval. (enum: -1=detailed HVAC system timestep; 0=zone timestep, 1=hourly, 2=daily, 3=monthly, 4=runperiod)</td>
-</tr>
-<tr>
-<td>SimulationDays</td>
-<td>INTEGER</td>
-<td>Day of simulation.  This number resets after warmup and at the beginning of an environment period</td>
-</tr>
-<tr>
-<td>DayType</td>
-<td>TEXT</td>
-<td>The type of day. (enum: “Sunday�, “Monday�, “Tuesday�, Wednesday�, “Thursday�, “Friday�, “Saturday�, “Holiday�, “SummerDesignDay�, “WinterDesignDay�, “CustomDay1�, “CustomDay2�)</td>
-</tr>
-<tr>
-<td>EnvironmentPeriodIndex</td>
-<td>INTEGER</td>
-<td>Foreign Key to the EnvironmentPeriods table</td>
-</tr>
-<tr>
-<td>WarmupFlag</td>
-<td>INTEGER</td>
-<td>1 during warmup, 0 otherwise</td>
-</tr>
-</table>
-
-### One time (EIO) File Data
-
-Data in the tables below can also be found in EnergyPlus input output file (i.e., in the eplusout.eio output file).
-
-#### Zones Table
-
-The Zones table provides a variety of information about the zones specified within EnergyPlus. One of its most common uses is to provide zone name and area information for the other tables within the SQL database (e.g., use the ZoneIndex to look up the ZoneName).
-
-
-
-<table class="table table-striped">
-<caption>Table 14. SQL Zones Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>The ZoneIndex is used to link this table to related tables</td>
-</tr>
-<tr>
-<td>ZoneName</td>
-<td>TEXT</td>
-<td>Zone Name</td>
-</tr>
-<tr>
-<td>RelNorth</td>
-<td>REAL</td>
-<td>Relative North, in degrees</td>
-</tr>
-<tr>
-<td>OriginX</td>
-<td>REAL</td>
-<td>X origin, in meters</td>
-</tr>
-<tr>
-<td>OriginY</td>
-<td>REAL</td>
-<td>Y origin, in meters</td>
-</tr>
-<tr>
-<td>OriginZ</td>
-<td>REAL</td>
-<td>Z origin, in meters</td>
-</tr>
-<tr>
-<td>CentroidX</td>
-<td>REAL</td>
-<td>X position of zone Centroid, in meters</td>
-</tr>
-<tr>
-<td>CentroidY</td>
-<td>REAL</td>
-<td>Y position of zone Centroid, in meters</td>
-</tr>
-<tr>
-<td>CentroidZ</td>
-<td>REAL</td>
-<td>Z position of zone Centroid, in meters</td>
-</tr>
-<tr>
-<td>OfType</td>
-<td>INTEGER</td>
-<td>(not used yet)</td>
-</tr>
-<tr>
-<td>Multiplier</td>
-<td>REAL</td>
-<td>Zone multiplier</td>
-</tr>
-<tr>
-<td>ListMultiplier</td>
-<td>REAL</td>
-<td>Zone Group multiplier</td>
-</tr>
-<tr>
-<td>MinimumX</td>
-<td>REAL</td>
-<td>Minimum X value, in meters</td>
-</tr>
-<tr>
-<td>MaximumX</td>
-<td>REAL</td>
-<td>Maximum X value, in meters</td>
-</tr>
-<tr>
-<td>MinimumY</td>
-<td>REAL</td>
-<td>Minimum Y value, in meters</td>
-</tr>
-<tr>
-<td>MaximumY</td>
-<td>REAL</td>
-<td>Maximum Y value, in meters</td>
-</tr>
-<tr>
-<td>MinimumZ</td>
-<td>REAL</td>
-<td>Minimum Z value, in meters</td>
-</tr>
-<tr>
-<td>MaximumZ</td>
-<td>REAL</td>
-<td>Maximum Z value, in meters</td>
-</tr>
-<tr>
-<td>CeilingHeight</td>
-<td>REAL</td>
-<td>Ceiling height, in meters</td>
-</tr>
-<tr>
-<td>Volume</td>
-<td>REAL</td>
-<td>Zone volume, in cubic meters</td>
-</tr>
-<tr>
-<td>InsideConvectionAlgo</td>
-<td>INTEGER</td>
-<td>Inside convection algorithm (enum: 1=simple, 2=detailed, 3=Ceiling diffuser, 4=TrombeWall)</td>
-</tr>
-<tr>
-<td>OutsideConvectionAlgo</td>
-<td>INTEGER</td>
-<td>Outside convection algorithm (enum: 1=simple, 2=detailed, 6=MoWitt, 7=DOE-2)</td>
-</tr>
-<tr>
-<td>FloorArea</td>
-<td>REAL</td>
-<td>Zone floor area, in square meters</td>
-</tr>
-<tr>
-<td>ExtGrossWallArea</td>
-<td>REAL</td>
-<td>Zone external gross wall area (includes windows and doors), in square meters</td>
-</tr>
-<tr>
-<td>ExtNetWallArea</td>
-<td>REAL</td>
-<td>Zone net wall area (excludes windows and doors), and square meters</td>
-</tr>
-<tr>
-<td>ExtWindowArea</td>
-<td>REAL</td>
-<td>Zone window area (includes glass doors), and square meters</td>
-</tr>
-<tr>
-<td>IsPartOfTotalArea</td>
-<td>INTEGER</td>
-<td>See Zone input object documentation</td>
-</tr>
-</table>
-
-Please see the Zone object in the Group-Thermal Zone Description/Geometry section of the Input-Output Reference for more information.
-
-#### NominalPeople Table
-
-An overview of the NominalPeople SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 15. SQL NominalPeople Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>NominalPeopleIndex</td>
-<td>INTEGER</td>
-<td>The internal statement number</td>
-</tr>
-<tr>
-<td>ObjectName</td>
-<td>TEXT</td>
-<td>The name of the People object</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Connects the NominalPeople table to the Zones table</td>
-</tr>
-<tr>
-<td>NumberOfPeople</td>
-<td>INTEGER</td>
-<td>Nominal number of people in the zone</td>
-</tr>
-<tr>
-<td>NumberOfPeopleScheduleIndex</td>
-<td>INTEGER</td>
-<td>Number of people schedule number (see Schedule table)</td>
-</tr>
-<tr>
-<td>ActivityScheduleIndex</td>
-<td>INTEGER</td>
-<td>Activity level schedule (see People object documentation)</td>
-</tr>
-<tr>
-<td>FractionRadiant</td>
-<td>REAL</td>
-<td>see People object documentation</td>
-</tr>
-<tr>
-<td>FractionConvected</td>
-<td>REAL</td>
-<td>see People object documentation</td>
-</tr>
-<tr>
-<td>WorkEfficiencyScheduleIndex</td>
-<td>INTEGER</td>
-<td>Work efficiency schedule number (see schedule table and people object documentation)</td>
-</tr>
-<tr>
-<td>ClothingEfficiencyScheduleIndex</td>
-<td>INTEGER</td>
-<td>Clothing efficiency schedule number (see schedule table and people object documentation)</td>
-</tr>
-<tr>
-<td>AirVelocityScheduleIndex</td>
-<td>INTEGER</td>
-<td>Air velocity schedule number (see schedule table and people object documentation)</td>
-</tr>
-<tr>
-<td>Fanger</td>
-<td>INTEGER</td>
-<td>Flag indicating whether Fanger calculations are active</td>
-</tr>
-<tr>
-<td>Pierce</td>
-<td>INTEGER</td>
-<td>Flag indicating whether Pierce calculations are active</td>
-</tr>
-<tr>
-<td>KSU</td>
-<td>INTEGER</td>
-<td>Flag indicating whether KSU calculations are active</td>
-</tr>
-<tr>
-<td>MRTCalcType</td>
-<td>INTEGER</td>
-<td>see People object documentation</td>
-</tr>
-<tr>
-<td>SurfaceIndex</td>
-<td>INTEGER</td>
-<td>see Surfaces table and People object documentation</td>
-</tr>
-<tr>
-<td>UserSpecifeidSensibleFraction</td>
-<td>REAL</td>
-<td>see People object documentation</td>
-</tr>
-<tr>
-<td>Show55Warning</td>
-<td>INTEGER</td>
-<td>see People object documentation</td>
-</tr>
-</table>
-
-Please see the People object in the Group-Internal Gains section of the Input-Output Reference for more information.
-
-#### NominalLighting Table
-
-An overview of the NominalLighting SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 16. SQL NominalLighting Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>NominalLightingIndex</td>
-<td>INTEGER</td>
-<td>The internal statement number</td>
-</tr>
-<tr>
-<td>ObjectName</td>
-<td>TEXT</td>
-<td>The LIGHTS object name</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Connects the NominalLighting table to the Zones table</td>
-</tr>
-<tr>
-<td>ScheduleIndex</td>
-<td>INTEGER</td>
-<td>Lighting schedule number (see Schedule table)</td>
-</tr>
-<tr>
-<td>DesignLevel</td>
-<td>REAL</td>
-<td>Nominal design level, in Watts</td>
-</tr>
-<tr>
-<td>FractionReturnAir</td>
-<td>REAL</td>
-<td>User-specified return air fraction</td>
-</tr>
-<tr>
-<td>FractionRadiant</td>
-<td>REAL</td>
-<td>User-specified radiant fraction</td>
-</tr>
-<tr>
-<td>FractionReplaceable</td>
-<td>REAL</td>
-<td>Defines the daylighting control for the LIGHTS object</td>
-</tr>
-<tr>
-<td>EndUseSubcategory</td>
-<td>TEXT</td>
-<td>User-specified end-use subcategory</td>
-</tr>
-</table>
-
-Please see the LIGHTS object in the Group-Internal Gains section of the Input-Output Reference for more information.
-
-#### NominalElectricEquipment Table
-
-An overview of the NominalElectricEquipment SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 17. SQL NominalElectricEquipment Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>NominalElectricEquipmentIndex</td>
-<td>INTEGER</td>
-<td>The internal statement number</td>
-</tr>
-<tr>
-<td>ObjectName</td>
-<td>TEXT</td>
-<td>The Electric Equipment object name</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Connects the NominalElectricEquipment table to the Zones table</td>
-</tr>
-<tr>
-<td>ScheduleIndex</td>
-<td>INTEGER</td>
-<td>Electric equipment schedule number (see Schedule table)</td>
-</tr>
-<tr>
-<td>DesignLevel</td>
-<td>REAL</td>
-<td>Nominal design level, in Watts</td>
-</tr>
-<tr>
-<td>FractionLatent</td>
-<td>REAL</td>
-<td>User-specified latent heat fraction</td>
-</tr>
-<tr>
-<td>FractionRadiant</td>
-<td>REAL</td>
-<td>User-specified radiant heat fraction</td>
-</tr>
-<tr>
-<td>FractionLost</td>
-<td>REAL</td>
-<td>User-specified lost heat fraction</td>
-</tr>
-<tr>
-<td>FractionConvected</td>
-<td>REAL</td>
-<td>User-specified convicted heat fraction</td>
-</tr>
-<tr>
-<td>EndUseSubcategory</td>
-<td>TEXT</td>
-<td>User-specified end-use subcategory</td>
-</tr>
-</table>
-
-Please see the Electric Equipment object in the Group-Internal Gains section of the Input-Output Reference for more information.
-
-#### NominalGasEquipment Table
-
-An overview of the NominalGasEquipment SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 18. SQL NominalGasEquipment Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>NominalGasEquipmentIndex</td>
-<td>INTEGER</td>
-<td>The internal statement number</td>
-</tr>
-<tr>
-<td>ObjectName</td>
-<td>TEXT</td>
-<td>The Gas Equipment object name</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Connects the NominalGasEquipment table to the Zones table</td>
-</tr>
-<tr>
-<td>ScheduleIndex</td>
-<td>INTEGER</td>
-<td>Gas equipment schedule number (see Schedule table)</td>
-</tr>
-<tr>
-<td>DesignLevel</td>
-<td>REAL</td>
-<td>Nominal design level, in Watts</td>
-</tr>
-<tr>
-<td>FractionLatent</td>
-<td>REAL</td>
-<td>User-specified latent heat fraction</td>
-</tr>
-<tr>
-<td>FractionRadiant</td>
-<td>REAL</td>
-<td>User-specified radiant heat fraction</td>
-</tr>
-<tr>
-<td>FractionLost</td>
-<td>REAL</td>
-<td>User-specified lost heat fraction</td>
-</tr>
-<tr>
-<td>FractionConvected</td>
-<td>REAL</td>
-<td>User-specified convicted heat fraction</td>
-</tr>
-<tr>
-<td>EndUseSubcategory</td>
-<td>TEXT</td>
-<td>User-specified end-use subcategory</td>
-</tr>
-</table>
-
-Please see the Gas Equipment object in the Group-Internal Gains section of the Input-Output Reference for more information.
-
-#### NominalSteamEquipment Table
-
-An overview of the NominalSteamEquipment SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 19. SQL NominalSteamEquipment Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>NominalSteamEquipmentIndex</td>
-<td>INTEGER</td>
-<td>The internal statement number</td>
-</tr>
-<tr>
-<td>ObjectName</td>
-<td>TEXT</td>
-<td>The Steam Equipment object name</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Connects the NominalSteamEquipment table to the Zones table</td>
-</tr>
-<tr>
-<td>ScheduleIndex</td>
-<td>INTEGER</td>
-<td>Steam equipment schedule number (see Schedule table)</td>
-</tr>
-<tr>
-<td>DesignLevel</td>
-<td>REAL</td>
-<td>Nominal design level, in Watts</td>
-</tr>
-<tr>
-<td>FractionLatent</td>
-<td>REAL</td>
-<td>User-specified latent heat fraction</td>
-</tr>
-<tr>
-<td>FractionRadiant</td>
-<td>REAL</td>
-<td>User-specified radiant heat fraction</td>
-</tr>
-<tr>
-<td>FractionLost</td>
-<td>REAL</td>
-<td>User-specified lost heat fraction</td>
-</tr>
-<tr>
-<td>FractionConvected</td>
-<td>REAL</td>
-<td>User-specified convicted heat fraction</td>
-</tr>
-<tr>
-<td>EndUseSubcategory</td>
-<td>TEXT</td>
-<td>User-specified end-use subcategory</td>
-</tr>
-</table>
-
-Please see the Steam Equipment object in the Group-Internal Gains section of the Input-Output Reference for more information.
-
-#### NominalHotWaterEquipment Table
-
-An overview of the NominalHotWaterEquipment SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 20. SQL NominalHotWaterEquipment Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>NominalHotWaterEquipmentIndex</td>
-<td>INTEGER</td>
-<td>The internal statement number</td>
-</tr>
-<tr>
-<td>ObjectName</td>
-<td>TEXT</td>
-<td>The Hot Water Equipment object name</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Connects the NominalHotWaterEquipment table to the Zones table</td>
-</tr>
-<tr>
-<td>ScheduleIndex</td>
-<td>INTEGER</td>
-<td>Hot water equipment schedule number (see Schedule table)</td>
-</tr>
-<tr>
-<td>DesignLevel</td>
-<td>REAL</td>
-<td>Nominal design level, in Watts</td>
-</tr>
-<tr>
-<td>FractionLatent</td>
-<td>REAL</td>
-<td>User-specified latent heat fraction</td>
-</tr>
-<tr>
-<td>FractionRadiant</td>
-<td>REAL</td>
-<td>User-specified radiant heat fraction</td>
-</tr>
-<tr>
-<td>FractionLost</td>
-<td>REAL</td>
-<td>User-specified lost heat fraction</td>
-</tr>
-<tr>
-<td>FractionConvected</td>
-<td>REAL</td>
-<td>User-specified convicted heat fraction</td>
-</tr>
-<tr>
-<td>EndUseSubcategory</td>
-<td>TEXT</td>
-<td>User-specified end-use subcategory</td>
-</tr>
-</table>
-
-Please see the Hot Water Equipment object in the Group-Internal Gains section of the Input-Output Reference for more information.
-
-#### NominalOtherEquipment Table
-
-An overview of the NominalOtherEquipment SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 21. SQL NominalOtherEquipment Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>NominalOtherEquipmentIndex</td>
-<td>INTEGER</td>
-<td>The internal statement number</td>
-</tr>
-<tr>
-<td>ObjectName</td>
-<td>TEXT</td>
-<td>The Other Equipment object name</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Connects the NominalOtherEquipment table to the Zones table</td>
-</tr>
-<tr>
-<td>ScheduleIndex</td>
-<td>INTEGER</td>
-<td>Other equipment schedule number (see Schedule table)</td>
-</tr>
-<tr>
-<td>DesignLevel</td>
-<td>REAL</td>
-<td>Nominal design level, in Watts</td>
-</tr>
-<tr>
-<td>FractionLatent</td>
-<td>REAL</td>
-<td>User-specified latent heat fraction</td>
-</tr>
-<tr>
-<td>FractionRadiant</td>
-<td>REAL</td>
-<td>User-specified radiant heat fraction</td>
-</tr>
-<tr>
-<td>FractionLost</td>
-<td>REAL</td>
-<td>User-specified lost heat fraction</td>
-</tr>
-<tr>
-<td>FractionConvected</td>
-<td>REAL</td>
-<td>User-specified convicted heat fraction</td>
-</tr>
-<tr>
-<td>EndUseSubcategory</td>
-<td>TEXT</td>
-<td>User-specified end-use subcategory</td>
-</tr>
-</table>
-
-Please see the Other Equipment object in the Group-Internal Gains section of the Input-Output Reference for more information.
-
-#### NominalBaseboardHeaters Table
-
-An overview of the NominalBaseboardHeaters SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 22. SQL NominalBaseboardHeaters Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>NominalBaseboardHeaterIndex</td>
-<td>INTEGER</td>
-<td>The internal statement number</td>
-</tr>
-<tr>
-<td>ObjectName</td>
-<td>TEXT</td>
-<td>The Baseboard Heat object name</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Connects the NominalBaseboardHeat table to the Zones table</td>
-</tr>
-<tr>
-<td>ScheduleIndex</td>
-<td>INTEGER</td>
-<td>Baseboard heat schedule number (see Schedules table)</td>
-</tr>
-<tr>
-<td>CapatLowTemperature</td>
-<td>REAL</td>
-<td>Capacity at low temperature, in Watts</td>
-</tr>
-<tr>
-<td>LowTemperature</td>
-<td>REAL</td>
-<td>Low temperature capacity setpoint</td>
-</tr>
-<tr>
-<td>CapatHighTemperature</td>
-<td>REAL</td>
-<td>Capacity at high temperature, in Watts</td>
-</tr>
-<tr>
-<td>HighTemperature</td>
-<td>REAL</td>
-<td>High temperature capacity setpoint</td>
-</tr>
-<tr>
-<td>FractionRadiant</td>
-<td>REAL</td>
-<td>User-specified radiant heat fraction</td>
-</tr>
-<tr>
-<td>FractionConvected</td>
-<td>REAL</td>
-<td>User-specified convicted heat fraction</td>
-</tr>
-<tr>
-<td>EndUseSubcategory</td>
-<td>TEXT</td>
-<td>User-specified end-use subcategory</td>
-</tr>
-</table>
-
-Please see the Baseboard Heat object in the Group-Internal Gains section of the Input-Output Reference for more information.
-
-#### NominalInfiltration Table
-
-An overview of the NominalInfiltration SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 23. SQL NominalInfiltration Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>NominalInfiltrationIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>The internal statement number</td>
-</tr>
-<tr>
-<td>ObjectName</td>
-<td>TEXT</td>
-<td>The Infiltration object name</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Connects the NominalInfiltration table to the Zones table</td>
-</tr>
-<tr>
-<td>ScheduleIndex</td>
-<td>INTEGER</td>
-<td>Infiltration schedule number (see Schedule table)</td>
-</tr>
-<tr>
-<td>DesignLevel</td>
-<td>REAL</td>
-<td>Nominal design level, in m3/s</td>
-</tr>
-</table>
-
-Please see the Infiltration object in the Group-Airflow section of the Input-Output Reference for more information.
-
-#### NominalVentilation Table
-
-An overview of the NominalVentilation SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 24. SQL NominalVentilation Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>NominalVentilationIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>The internal statement number</td>
-</tr>
-<tr>
-<td>ObjectName</td>
-<td>TEXT</td>
-<td>The Ventilation object name</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Connects the NominalVentilation table to the Zones table</td>
-</tr>
-<tr>
-<td>ScheduleIndex</td>
-<td>INTEGER</td>
-<td>Ventilation schedule number (see Schedule table)</td>
-</tr>
-<tr>
-<td>DesignLevel</td>
-<td>REAL</td>
-<td>Nominal design level, in m3/s</td>
-</tr>
-</table>
-
-Please see the Ventilation object in the Group-Airflow section of the Input-Output Reference for more information.
-
-#### Surfaces Table
-
-An overview of the Surfaces SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 25. SQL Surfaces Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>SurfaceIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Surface number (used for cross-referencing)</td>
-</tr>
-<tr>
-<td>SurfaceName</td>
-<td>TEXT</td>
-<td>Surface name</td>
-</tr>
-<tr>
-<td>ConstructionIndex</td>
-<td>INTEGER</td>
-<td>Construction Index</td>
-</tr>
-<tr>
-<td>ClassName</td>
-<td>TEXT</td>
-<td>Surface class name (e.g., shading, wall)</td>
-</tr>
-<tr>
-<td>Area</td>
-<td>REAL</td>
-<td>Surface area (excluding cutouts)</td>
-</tr>
-<tr>
-<td>GrossArea</td>
-<td>REAL</td>
-<td>Surface area (including cutouts)</td>
-</tr>
-<tr>
-<td>Perimeter</td>
-<td>REAL</td>
-<td>Surface perimeter, in meters</td>
-</tr>
-<tr>
-<td>Azimuth</td>
-<td>REAL</td>
-<td>As news angle, in degrees</td>
-</tr>
-<tr>
-<td>Height</td>
-<td>REAL</td>
-<td>Surface height, in meters</td>
-</tr>
-<tr>
-<td>Reveal</td>
-<td>REAL</td>
-<td>Reveal depth, in meters</td>
-</tr>
-<tr>
-<td>Shape</td>
-<td>INTEGER</td>
-<td>Shape index</td>
-</tr>
-<tr>
-<td>Sides</td>
-<td>INTEGER</td>
-<td>Number of sides</td>
-</tr>
-<tr>
-<td>Tilt</td>
-<td>REAL</td>
-<td>Tilt angle, in degrees</td>
-</tr>
-<tr>
-<td>Width</td>
-<td>REAL</td>
-<td>Surface width, in meters</td>
-</tr>
-<tr>
-<td>HeatTransferSurf</td>
-<td>INTEGER</td>
-<td>Flag indicating whether the surface is a heat transfer surface</td>
-</tr>
-<tr>
-<td>BaseSurfaceIndex</td>
-<td>INTEGER</td>
-<td>Based surface index</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Zone index</td>
-</tr>
-<tr>
-<td>ExtBoundCond</td>
-<td>INTEGER</td>
-<td>External boundary condition index. For interzone surface, this is the adjacent surface number. For an internal/adiabatic surface this is the current surface number. 0=external environment, -1=ground, -2=other side coefficients, -3=other side conditions model.</td>
-</tr>
-<tr>
-<td>ExtSolar</td>
-<td>INTEGER</td>
-<td>Flag indicating whether the surface is exposed to solar</td>
-</tr>
-<tr>
-<td>ExtWind</td>
-<td>INTEGER</td>
-<td>Flag indicating whether the surface is exposed to wind</td>
-</tr>
-</table>
-
-Please see the Surface(s) object in the Group-Thermal Zone Description/Geometry section of the Input-Output Reference for more information.
-
-#### Constructions Table
-
-An overview of the Constructions SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 26. SQL Constructions Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ConstructionIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Construction Index</td>
-</tr>
-<tr>
-<td>Name</td>
-<td>TEXT</td>
-<td>Construction name</td>
-</tr>
-<tr>
-<td>TotalLayers</td>
-<td>INTEGER</td>
-<td>Total number of layers</td>
-</tr>
-<tr>
-<td>TotalSolidLayers</td>
-<td>INTEGER</td>
-<td>Total number of solid layers</td>
-</tr>
-<tr>
-<td>TotalGlassLayers</td>
-<td>INTEGER</td>
-<td>Total number of glass layers</td>
-</tr>
-<tr>
-<td>InsideAbsorpVis</td>
-<td>REAL</td>
-<td>The visible absorptance of the inside layer (see Materials table)</td>
-</tr>
-<tr>
-<td>OutsideAbsorpVis</td>
-<td>REAL</td>
-<td>The visible absorptance of the outside layer (see Materials table)</td>
-</tr>
-<tr>
-<td>InsideAbsorpSolar</td>
-<td>REAL</td>
-<td>The solar absorptance of the inside layer (see Materials table)</td>
-</tr>
-<tr>
-<td>OutsideAbsorpSolar</td>
-<td>REAL</td>
-<td>The solar absorptance of the outside layer (see Materials table)</td>
-</tr>
-<tr>
-<td>InsideAbsorpThermal</td>
-<td>REAL</td>
-<td>The thermal absorptance of the inside layer (see Materials table)</td>
-</tr>
-<tr>
-<td>OutsideAbsorpThermal</td>
-<td>REAL</td>
-<td>The thermal absorptance of the outside layer (see Materials table)</td>
-</tr>
-<tr>
-<td>OutsideRoughness</td>
-<td>INTEGER</td>
-<td>The roughness of the outside layer</td>
-</tr>
-<tr>
-<td>TypeIsWindow</td>
-<td>INTEGER</td>
-<td>Flag indicating whether the construction is a window or glass door</td>
-</tr>
-<tr>
-<td>Uvalue</td>
-<td>REAL</td>
-<td>Nominal U-value for the construction</td>
-</tr>
-</table>
-
-Please see the Construction object in the Group-Surface Construction Elements section of the Input-Output Reference for more information.
-
-#### ConstructionLayers Table
-
-An overview of the ConstructionLayers SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 27. SQL ConstructionLayers Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ConstructionLayersIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Construction Layers Index</td>
-</tr>
-<tr>
-<td>ConstructionIndex</td>
-<td>INTEGER</td>
-<td>Construction Index (see Constructions table)</td>
-</tr>
-<tr>
-<td>LayerIndex</td>
-<td>INTEGER</td>
-<td>Layer number (layer 1 is the outside layer)</td>
-</tr>
-<tr>
-<td>MaterialIndex</td>
-<td>INTEGER</td>
-<td>Material index (see Materials table)</td>
-</tr>
-</table>
-
-Please see the Construction object in the Group-Surface Construction Elements section of the Input-Output Reference for more information.
-
-#### Materials Table
-
-An overview of the Materials SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 28. SQL Materials Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>MaterialIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Material Index (links the Materials table with the ConstructionLayers and Constructions tables)</td>
-</tr>
-<tr>
-<td>Name</td>
-<td>TEXT</td>
-<td>Material name</td>
-</tr>
-<tr>
-<td>MaterialType</td>
-<td>INTEGER</td>
-<td>Material type</td>
-</tr>
-<tr>
-<td>Roughness</td>
-<td>INTEGER</td>
-<td>Roughness index</td>
-</tr>
-<tr>
-<td>Conductivity</td>
-<td>REAL</td>
-<td>Conductivity, in W/(m-K)</td>
-</tr>
-<tr>
-<td>Density</td>
-<td>REAL</td>
-<td>Density, in kg/m3</td>
-</tr>
-<tr>
-<td>Porosity</td>
-<td>REAL</td>
-<td>Porosity</td>
-</tr>
-<tr>
-<td>Resistance</td>
-<td>REAL</td>
-<td>Resistance</td>
-</tr>
-<tr>
-<td>Ronly</td>
-<td>INTEGER</td>
-<td>Flag that indicates the material definition is of type Material:Regular-R</td>
-</tr>
-<tr>
-<td>SpecHeat</td>
-<td>REAL</td>
-<td>Specific heat</td>
-</tr>
-<tr>
-<td>ThermGradCoef</td>
-<td>REAL</td>
-<td>Thermal gradient coefficient</td>
-</tr>
-<tr>
-<td>Thickness</td>
-<td>REAL</td>
-<td>Thickness, in meters</td>
-</tr>
-<tr>
-<td>VaporDiffus</td>
-<td>REAL</td>
-<td>Vapor diffusivity</td>
-</tr>
-</table>
-
-Please see the Materials object in the Group-Surface Construction Elements section of the Input-Output Reference for more information.
-
-#### RoomAirModels Table
-
-An overview of the RoomAirModels SQL table is shown below. Please see the Group-RoomAir Models section of the Input-Output Reference for more information.
-
-
-
-<table class="table table-striped">
-<caption>Table 29. SQL RoomAirModels Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Zone index</td>
-</tr>
-<tr>
-<td>AirModelName</td>
-<td>TEXT</td>
-<td>Air model name</td>
-</tr>
-<tr>
-<td>AirModelType</td>
-<td>INTEGER</td>
-<td>Air model index</td>
-</tr>
-<tr>
-<td>TempCoupleScheme</td>
-<td>INTEGER</td>
-<td>Temperature coupling index</td>
-</tr>
-<tr>
-<td>SimAirModel</td>
-<td>INTEGER</td>
-<td>Simulation air model index</td>
-</tr>
-</table>
-
-#### ComponentSizes Table
-
-An overview of the ComponentSizes SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 30. SQL ComponentSizes Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ComponentSizesIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Component Sizes Index</td>
-</tr>
-<tr>
-<td>CompType</td>
-<td>TEXT</td>
-<td>Component type</td>
-</tr>
-<tr>
-<td>CompName</td>
-<td>TEXT</td>
-<td>Component name</td>
-</tr>
-<tr>
-<td>Description</td>
-<td>TEXT</td>
-<td>Component description</td>
-</tr>
-<tr>
-<td>Value</td>
-<td>REAL</td>
-<td>Sizing value</td>
-</tr>
-<tr>
-<td>Units</td>
-<td>TEXT</td>
-<td>Sizing units</td>
-</tr>
-</table>
-
-Please see the Sizing object in the Group-Design Objects section of the Input-Output Reference for more information.
-
-#### SystemSizes Table
-
-An overview of the SystemSizes SQL table is shown below. Please see the System Sizing object in the Group-Design Objects section of the Input-Output Reference for more information.
-
-
-
-<table class="table table-striped">
-<caption>Table 31. SQL SystemSizes Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>SystemSizesIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>System Sizes Index</td>
-</tr>
-<tr>
-<td>SystemName</td>
-<td>TEXT</td>
-<td>System name</td>
-</tr>
-<tr>
-<td>Description</td>
-<td>TEXT</td>
-<td>System description</td>
-</tr>
-<tr>
-<td>Value</td>
-<td>REAL</td>
-<td>Sizing value</td>
-</tr>
-<tr>
-<td>Units</td>
-<td>TEXT</td>
-<td>Sizing units</td>
-</tr>
-</table>
-
-#### ZoneSizes Table
-
-An overview of the ZoneSizes SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 32. SQL ZoneSizes Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ZoneSizesIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Zone Sizes Index</td>
-</tr>
-<tr>
-<td>ZoneName</td>
-<td>TEXT</td>
-<td>Zone name</td>
-</tr>
-<tr>
-<td>LoadType</td>
-<td>TEXT</td>
-<td>Load type</td>
-</tr>
-<tr>
-<td>DesLoad</td>
-<td>REAL</td>
-<td>Design load</td>
-</tr>
-<tr>
-<td>CalcDesFlow</td>
-<td>REAL</td>
-<td>Calculated design flow</td>
-</tr>
-<tr>
-<td>UserDesFlow</td>
-<td>REAL</td>
-<td>User-specified design flow</td>
-</tr>
-<tr>
-<td>DesDayName</td>
-<td>TEXT</td>
-<td>Design day name</td>
-</tr>
-<tr>
-<td>PeakHrMin</td>
-<td>TEXT</td>
-<td>Time of the peak temperature</td>
-</tr>
-<tr>
-<td>PeakTemp</td>
-<td>REAL</td>
-<td>Peak temperature</td>
-</tr>
-<tr>
-<td>PeakHumRat</td>
-<td>REAL</td>
-<td>Peak humidity ratio</td>
-</tr>
-<tr>
-<td>CalcOutsideAirFlow</td>
-<td>REAL</td>
-<td>Calculated outside air flow rate, in m3/s</td>
-</tr>
-</table>
-
-Please see the Zone Sizing object in the Group-Design Objects section of the Input-Output Reference for more information.
-
-#### ZoneGroups Table
-
-An overview of the ZoneGroups SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 33. SQL ZoneGroups Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ZoneGroupIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Zone group index</td>
-</tr>
-<tr>
-<td>ZoneGroupName</td>
-<td>TEXT</td>
-<td>Zone list name</td>
-</tr>
-<tr>
-<td>ZoneListIndex</td>
-<td>INTEGER</td>
-<td>The ZoneListIndex links this record to the respective zone list record (see ZoneLists table below)</td>
-</tr>
-<tr>
-<td>ZoneListMultiplier</td>
-<td>INTEGER</td>
-<td>Zone list multiplier</td>
-</tr>
-</table>
-
-Please see the Zone Group object in the Group-Thermal Zone Description/Geometry section of the Input-Output Reference for more information.
-
-#### ZoneLists Table
-
-An overview of the ZoneLists SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 34. SQL ZoneLists Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ZoneListIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Zone list index</td>
-</tr>
-<tr>
-<td>Name</td>
-<td>TEXT</td>
-<td>Zone list name</td>
-</tr>
-</table>
-
-Please see the Zone List object in the Group-Thermal Zone Description/Geometry section of the Input-Output Reference for more information.
-
-#### ZoneInfoZoneLists Table
-
-An overview of the ZoneInfoZoneLists SQL table is shown below.
-
-<table class="table table-striped">
-<caption>SQL ZoneLists Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ZoneListIndex</td>
-<td>INTEGER</td>
-<td>Zone list index</td>
-</tr>
-<tr>
-<td>ZoneIndex</td>
-<td>INTEGER</td>
-<td>Zone index</td>
-</tr>
-</table>
-
-This is a join table to represent the many-to-many relationship of zones and zone lists.  ZoneListIndex and ZoneIndex together are the Primary Key for this table.
-
-### Miscellaneous Tables
-
-#### Schedules Table
-
-An overview of the Schedules SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 35. SQL Schedules Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ScheduleIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Schedule index</td>
-</tr>
-<tr>
-<td>ScheduleName</td>
-<td>TEXT</td>
-<td>Schedule name</td>
-</tr>
-<tr>
-<td>ScheduleType</td>
-<td>TEXT</td>
-<td>Schedule Type</td>
-</tr>
-<tr>
-<td>ScheduleMinimum</td>
-<td>REAL</td>
-<td>ScheduleMinimum</td>
-</tr>
-<tr>
-<td>ScheduleMaximum</td>
-<td>REAL</td>
-<td>ScheduleMaximum</td>
-</tr>
-</table>
-
-Please see the Group-Schedules section of the Input-Output Reference for more information.
-
-#### Simulations Table
-
-An overview of the Simulations SQL table is shown below.  Currently there will only be one record in the table, because the SQLite database is relevant to only one simulation.  In the future this might change if multiple simulations are aggregated into a larger database.
-
-
-
-<table class="table table-striped">
-<caption>Table 36. SQL Simulations Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>SimulationIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Simulation index, currently there will be only one record in this table.</td>
-</tr>
-<tr>
-<td>EnergyPlusVersion</td>
-<td>TEXT</td>
-<td>The version of EnergyPlus that was used to run the simulation.</td>
-</tr>
-<tr>
-<td>TimeStamp</td>
-<td>TEXT</td>
-<td>A text string containing the timestamp when the simulation was run.</td>
-</tr>
-<tr>
-<td>NumTimestepsPerHour</td>
-<td>INTEGER</td>
-<td>The number of timesteps per hour used for the simulation.  See the Timestep object for more information.</td>
-</tr>
-<tr>
-<td>Completed</td>
-<td>BOOL</td>
-<td>True if the simulation completed without crashing.</td>
-</tr>
-<tr>
-<td>CompletedSuccessfully</td>
-<td>BOOL</td>
-<td>True if the simulation completed without any severe or fatal errors.</td>
-</tr>
-</table>
-
-#### EnvironmentPeriods Table
-
-An overview of the EnvironmentPeriods SQL table is shown below.
-
-
-
-<table class="table table-striped">
-<caption>Table 37. SQL EnvironmentPeriods Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>EnvironmentPeriodIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Environment period index</td>
-</tr>
-<tr>
-<td>SimulationIndex</td>
-<td>INTEGER</td>
-<td>A foreign key to a record in the Simulations table.</td>
-</tr>
-<tr>
-<td>EnvironmentName</td>
-<td>TEXT</td>
-<td>A text string identifying the environment.</td>
-</tr>
-<tr>
-<td>EnvironmentType</td>
-<td>INTEGER</td>
-<td>An enumeration of the environment type.  (1 = Design Day, 2 =  Design Run Period, 3 = Weather Run Period)  See the various SizingPeriod objects and the RunPeriod object for details.</td>
-</tr>
-</table>
-
-#### TabularData Table
-
-An overview of the TabularData SQL table is shown below.   The TabularData table is only output when the “SimpleAndTabular� choice is made in the Output:SQLite object.  The TabularData table contains all of the tabular report information that is typically output to one of the formats controlled by the OutputControl:Table:Style object.  This is a generic way of dumping all of the existing tabular reports to the SQLite database.  This table has many references to the companion Strings table.  The Strings table simply associates strings to an integer value for space efficiency of the database.  Tabular data is easier to query from the TabularDataWithStrings table, which is implemented as a database view that joins this table with the Strings table.
-
-
-
-<table class="table table-striped">
-<caption>Table 38. SQL TabularData Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>TabularDataIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>Tabular Data Index</td>
-</tr>
-<tr>
-<td>ReportNameIndex</td>
-<td>INTEGER</td>
-<td>A foreign key to an entry in the Strings table, which indicates the name of the report the record belongs to.</td>
-</tr>
-<tr>
-<td>ReportForStringIndex</td>
-<td>INTEGER</td>
-<td>A foreign key to an entry in the Strings table, which indicates the “For� text that is associated with the record.  An example is the Space Loads report where the “For� text identifies which zone the record pertains to.</td>
-</tr>
-<tr>
-<td>TableNameIndex</td>
-<td>INTEGER</td>
-<td>A foreign key to an entry in the Strings table, which indicates the name of the table the record belongs to.  This is typically the text that immediately precedes the tables in html format.</td>
-</tr>
-<tr>
-<td>SimulationIndex</td>
-<td>INTEGER</td>
-<td>A foreign key to the Simulations table.</td>
-</tr>
-<tr>
-<td>RowNameIndex</td>
-<td>INTEGER</td>
-<td>A foreign key to an entry in the Strings table, which indicates the name of the row the record belongs to.</td>
-</tr>
-<tr>
-<td>ColumnNameIndex</td>
-<td>INTEGER</td>
-<td>A foreign key to an entry in the Strings table, which indicates the name of the column the record belongs to.</td>
-</tr>
-<tr>
-<td>UnitsIndex</td>
-<td>INTEGER</td>
-<td>A foreign key to an entry in the Strings table, which indicates the units associated with the record.</td>
-</tr>
-<tr>
-<td>SimulationIndex</td>
-<td>INTEGER</td>
-<td>A foreign key to the Simulations table.</td>
-</tr>
-<tr>
-<td>RowId</td>
-<td>INTEGER</td>
-<td>The index of the row associated with the record.  Data in the first row of a tabular report would have the Id 1.</td>
-</tr>
-<tr>
-<td>ColumnId</td>
-<td>INTEGER</td>
-<td>The index of the column associated with the record.  Data in the first column of a tabular report would have the Id 1.</td>
-</tr>
-<tr>
-<td>Value</td>
-<td>REAL</td>
-<td>The value of the record.  Most data is numeric, thus the type for this column is REAL.  The SQLite engine will first try to store the value as a REAL, however if this fails the value will be stored as text.</td>
-</tr>
-</table>
-
-#### Strings Table
-
-An overview of the Strings SQL table is shown below. The Strings table is only output when the “SimpleAndTabular� choice is made in the Output:SQLite object.  The Strings table simply associates strings with integers to save space in the database.
-
-
-
-<table class="table table-striped">
-<caption>Table 39. SQL Strings Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>StringIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>The integer primary key that uniquely identifies the string record.</td>
-</tr>
-<tr>
-<td>StringTypeIndex</td>
-<td>INTEGER</td>
-<td>A foreign key to the StringTypes table.</td>
-</tr>
-<tr>
-<td>Value</td>
-<td>TEXT</td>
-<td>The record’s string value.</td>
-</tr>
-</table>
-
-#### StringTypes Table
-
-An overview of the StringTypes SQL table is shown below. The StringTypes table is only output when the “SimpleAndTabular� choice is made in the Output:SQLite object.
-
-
-
-<table class="table table-striped">
-<caption>Table 40. SQL StringTypes Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>StringTypeIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>The integer primary key.</td>
-</tr>
-<tr>
-<td>Value</td>
-<td>TEXT</td>
-<td>The record’s string value.  Currently there are 6 possible values; ReportName, ReportForString, TableName, RowName, ColumnName, and Units.  That is, entries in the Strings table are one of these types.</td>
-</tr>
-</table>
-
-#### TabularDataWithStrings Table
-
-An overview of the TabularDataWithStrings SQL table is shown below.  This table is implemented as a view of other tables and is not actually a table in the database.  This view is similar to the TabularData table except text strings are directly available in place of foreign keys to the Strings table.   The TabularDataWithStrings view is only created when the “SimpleAndTabular� choice is made in the Output:SQLite object.
-
-An example of a SQL query to get a table out of the AnnualBuildingUtilityPerformanceSummary report is the following.
-
-````
-select \* FROM TabularDataWithStrings WHERE 
-ReportName='AnnualBuildingUtilityPerformanceSummary' 
-and TableName='Site and Source Energy';
-````
-
-
-
-<table class="table table-striped">
-<caption>Table 41. SQL TabularDataWithStrings Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>TabularDataIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>The index of the record</td>
-</tr>
-<tr>
-<td>Value</td>
-<td>REAL</td>
-<td>The value of the record</td>
-</tr>
-<tr>
-<td>ReportName</td>
-<td>TEXT</td>
-<td>The name of the report the record belongs to.</td>
-</tr>
-<tr>
-<td>ReportForString</td>
-<td>TEXT</td>
-<td>The “For� string.</td>
-</tr>
-<tr>
-<td>TableName</td>
-<td>TEXT</td>
-<td>The name of the table the record belongs to.</td>
-</tr>
-<tr>
-<td>RowName</td>
-<td>TEXT</td>
-<td>The name of the row associated with the record.</td>
-</tr>
-<tr>
-<td>ColumnName</td>
-<td>TEXT</td>
-<td>The name of the column associated with the record.</td>
-</tr>
-<tr>
-<td>Units</td>
-<td>TEXT</td>
-<td>The units associated with the record.</td>
-</tr>
-</table>
-
-#### Errors Table
-
-The Errors SQL table reports errors and warnings for the simulation.  The content of this table includes most of the content of the error file.  However, it does not contain purely informational messages (e.g. not warnings or errors) and some of the error summary statistics which may be readily computed. Users should be aware that errors experienced while processing input cause EnergyPlus to exit before the SQLite output database has been initialized.  This is because the Output:SQLite object must be parsed from the input to request the database.  Therefore, failures in input processing are indicated by the absence of a SQLite output file.  The regular error or audit files must be used to identify the erroneous input objects in this case.  Because each error or warning message is expected to be unique these messages are stored directly in the Errors table and not in the Strings table.
-
-
-
-<table class="table table-striped">
-<caption>Table 42. SQL Errors Table Contents</caption>
-<tr>
-<th>Field Name</th>
-<th>Field Type</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>ErrorIndex</td>
-<td>INTEGER PRIMARY KEY</td>
-<td>The index of the error or warning message.</td>
-</tr>
-<tr>
-<td>SimulationIndex</td>
-<td>INTEGER FOREIGN KEY</td>
-<td>The simulation the error or warning pertains to.</td>
-</tr>
-<tr>
-<td>ErrorType</td>
-<td>INTEGER</td>
-<td>Type of error or warning 0=Warning, 1=Severe, 2=Fatal.</td>
-</tr>
-<tr>
-<td>ErrorMessage</td>
-<td>TEXT</td>
-<td>The text of the error message.</td>
-</tr>
-<tr>
-<td>Count</td>
-<td>INTEGER</td>
-<td>Number of times that the error was repeated.  This will be 1 for normal warnings or errors, 0 for warning and error messages, and the number of times the error or warning is repeated.</td>
-</tr>
-</table>
-
-
-
-### How to Access the SQLite Data
-
-The SQL database can be accessed in a number of ways, including via the command line, through ODBC, or through as SQLite’s API interface. SQLite uses the industry standard SQL 92 language.
-
-#### Command Line
-
-One of the simplest ways to access the data in the SQL database is by way of the SQL command line tool (i.e., sqlite3). A brief description of how to use sqlite3 for each computing platform is given below.
-
-#### Windows XP and Windows Vista
-
-While Windows does not ship with sqlite3 installed, the sqlite3 binary can be downloaded from the SQLite webpage (www.sqlite.org/download.html). After downloading the precompiled binary, install it in the EnergyPlus directory.
-
-Once the sqlite3 executable is installed, access the program from the command line by typing “sqlite3� at the DOS prompt.
-
-#### Linux
-
-The sqlite3 command line tool comes preinstalled on a number of more recent Linux releases. To see if sqlite3 is available (and which version is installed), type “sqlite3 --version� from the command line. If sqlite3 is not installed, the sqlite3 binary, as well as source code, can be downloaded from the SQLite webpage (http://www.sqlite.org/download.html) and installed in the directory of your choice.
-
-#### Macintosh OS X
-
-The sqlite3 program comes standard on MacOS X 10.5. From the command line, type “sqlite3 --version� to see which version of sqlite3 is installed.  In order to access the database created by EnergyPlus, version 3 or later is required.
-
-#### Accessing the Data from the Command Line
-
-Once it has been confirmed that SQLite3 is installed on your machine, the SQL database can be accessed by typing:
-
-```
-sqlite3 <database name>
-```
-
-at the command line, where &lt;database name &gt; is the name of the SQL database (e.g., sqlite3 eplusout.sql).
-
-The sqlite.org [website](http://www.sqlite.org/sqlite.html) gives examples of how sqlite3 can be used to access and output data in various formats.
-
-#### ODBC
-
-ODBC allows access to the SQL database from a variety of programs, including Microsoft Excel, Microsoft Access, and FileMaker. How to install and use ODBC drivers is outside the scope of this document, and more information can be found at the following websites:
-
-Macintosh ODBC drivers:
-
-http://www.actualtechnologies.com/
-
-Windows and Linux ODBC information and drivers:
-
-http://www.sqlite.org/cvstrac/wiki?p=SqliteOdbc
-
-http://www.ch-werner.de/sqliteodbc/
-
-#### API
-
-Sqlite3 includes a rich C++ API (detailed on the SQLite website [www.sqlite.org/cintro.html](http://www.sqlite.org/cintro.html)), and wrappers for the API interface are available in a variety of programming languages, including Fortran, TCL, and Ruby (see [www.sqlite.org/cvstrac/wiki?p=SqliteWrappers](http://www.sqlite.org/cvstrac/wiki?p=SqliteWrappers) for more information).
-
-eplusssz.&lt;ext&gt;
-----------------
-
-This file is the result of the system sizing calculation. As usual, the file can be read into a spreadsheet for easy viewing. System Sizing (see Sizing:System object) performs a special calculation that, to oversimplify, sums up the results of the zone sizing calculation and saves the results in the system sizing arrays for reporting on component size requirements.
-
-An excerpt of the file:
-
-Time,:Des Heat Mass Flow [kg/s],:Des Cool Mass Flow [kg/s],:Des Heat Cap [W],:Des Sens Cool Cap [W],
-
-00:15:00,1.063942E+00,0.000000E+00,5.944201E+03,0.000000E+00,
-
-00:30:00,1.063942E+00,0.000000E+00,5.944201E+03,0.000000E+00,
-
-00:45:00,1.063942E+00,0.000000E+00,5.944201E+03,0.000000E+00,
-
-01:00:00,1.063942E+00,0.000000E+00,5.944201E+03,0.000000E+00,
-
-01:15:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-01:30:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-01:45:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-02:00:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-02:15:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-02:30:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-02:45:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-03:00:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-03:15:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-03:30:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-03:45:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-04:00:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-04:15:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-04:30:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-04:45:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-05:00:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-05:15:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
-
-05:30:00,1.063942E+00,0.000000E+00,5.944200E+03,0.000000E+00,
- === reduced for brevity ===
-
-
-
-
-
-Coinc Peak   ,1.063943E+00,1.378986E+00,5.944199E+03,2.165922E+04,
-
-NonCoinc Peak,1.063943E+00,1.553319E+00,5.944199E+03,2.165922E+04,
-
-#### Field: Time
-
-Calculation time – this will show the time steps used by the simulation and by the sizing calculation.
-
-#### Field: Des Heat Mass Flow [kg/s]
-
-Calculated design heating mass flow rate.
-
-#### Field: Des Cool Mass Flow [kg/s]
-
-Calculated design cooling mass flow rate.
-
-#### Field: Des Heat Cap [W]
-
-Calculated design heating capacity.
-
-#### Field: Des Sens Cool Cap [W]
-
-Calculated design sensible cooling capacity.
-
-#### Line: Coinc Peak
-
-The values in this line only apply to the Mass Flow Rates. The coincident peak cooling mass flow rate is the maximum of the sum of the zone peak cooling mass flow rates occurring at each time step. The coincident peak heating mass flow rate is the maximum of the sum of the zone peak heating mass flow rates occurring at each time step.
-
-#### Line: NonCoinc Peak
-
-The values in this line only apply to the Mass Flow Rates. The noncoincident peak cooling mass flow rate is the sum of the zone peak cooling mass flow rates, no matter what time of day the individual zone peaks occurred. The noncoincident peak heating mass flow rate is the sum of the zone peak heating mass flow rates, no matter what time of day the individual zone peaks occurred.
-
-Or as depicted graphically:
-
-![](media/image017.png)
-
-Figure 5. System Size depiction from eplusout.ssz
-
-
-
-epluszsz.&lt;ext&gt;
-----------------
-
-This file is a result of the zone sizing calculation. Zone Sizing (see Sizing:Zone object) performs a special calculation, using a theoretical ideal zonal system, and determines the zone design heating and cooling flow rates and loads, saving the results in the zone sizing arrays. The file has a similar format to the eplusssz.&lt;ext&gt; file.
-
-An excerpt (this is a direct copy of the CSV data, so you can copy it to a spreadsheet to view it easier):
-
-Time,SPACE1-1:CHICAGO\_IL\_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB:Des Heat Load [W],SPACE1-1:CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB:Des Sens Cool Load [W],SPACE1-1:CHICAGO\_IL\_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB:Des Heat Mass Flow [kg/s],SPACE1-1:CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB:Des Cool Mass Flow [kg/s],SPACE2-1:CHICAGO\_IL\_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB:Des Heat Load [W],SPACE2-1:CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB:Des Sens Cool Load [W],SPACE2-1:CHICAGO\_IL\_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB:Des Heat Mass Flow [kg/s],SPACE2-1:CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB:Des Cool Mass Flow [kg/s],SPACE3-1:CHICAGO\_IL\_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB:Des Heat Load [W],SPACE3-1:CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB:Des Sens Cool Load [W],SPACE3-1:CHICAGO\_IL\_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB:Des Heat Mass Flow [kg/s],SPACE3-1:CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB:Des Cool Mass Flow [kg/s],SPACE4-1:CHICAGO\_IL\_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB:Des Heat Load [W],SPACE4-1:CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB:Des Sens Cool Load [W],SPACE4-1:CHICAGO\_IL\_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB:Des Heat Mass Flow [kg/s],SPACE4-1:CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB:Des Cool Mass Flow [kg/s],SPACE5-1:CHICAGO\_IL\_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB:Des Heat Load [W],SPACE5-1:CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB:Des Sens Cool Load [W],SPACE5-1:CHICAGO\_IL\_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB:Des Heat Mass Flow [kg/s],SPACE5-1:CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB:Des Cool Mass Flow [kg/s]
-
-00:15:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
-00:30:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
-00:45:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
-01:00:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
-01:15:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
-01:30:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
-01:45:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
-02:00:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
-02:15:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
-02:30:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
-02:45:00,3.860764E+03,0.000000E+00,1.371872E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,3.753069E+03,0.000000E+00,1.333603E-01,0.000000E+00,1.625149E+03,0.000000E+00,5.774764E-02,0.000000E+00,2.981568E+03,0.000000E+00,1.059457E-01,0.000000E+00
-
- === reduced for brevity ===
-
-
-
-
-
-Peak,3.860764E+03,2.647331E+03,1.371872E-01,2.618408E-01,1.625149E+03,2.234379E+03,5.774764E-02,2.209833E-01,3.753069E+03,2.506339E+03,1.333603E-01,2.478849E-01,1.625149E+03,2.464720E+03,5.774764E-02,2.437670E-01,2.981568E+03,2.628694E+03,1.059457E-01,2.599981E-01
-
-
-
-Peak Vol Flow (m3/s),,,1.166672E-01,2.226756E-01,,,4.910995E-02,1.879294E-01,,,1.134128E-01,2.108072E-01,,,4.910995E-02,2.073052E-01,,,9.009871E-02,2.211085E-01
-
-The columns are:
-
-#### Field: Time
-
-Calculation time – this will show the time steps used by the simulation and by the sizing calculation.
-
-#### Sizing Calculation Fields
-
-Each of the Zone Sizing output fields has the Zone Name, the Environment Name for the peak prepended to the item that has been calculated.  The four fields calculated are:
-
-- Des Heat Load
-
-- Des Sens Cool Load
-
-- Des Heat Mass Flow
-
-- Des Cool Mass Flow
-
-These are repeated for the number of zones in the sizing calculation.
-
-#### Field:  Des Heat Load [W]
-
-This is the calculated design/required heating load at the time step.
-
-#### Field:  Des Sens Cool Load [W]
-
-This is the calculated design/required cooling load at the time step.
-
-#### Field:  Des Heat Mass Flow [kg/s]
-
-This is the calculated design/required heating mass flow rate at the time step.
-
-#### Field: Des Cool Mass Flow [kg/s]
-
-This is the calculated design/required cooling mass flow rate at the time step.
-
-#### Line: Peak
-
-This indicates the peak calculation (load or mass flow) over the 24 hour condensed sizing period.
-
-#### Line: Peak Vol Flow [m3/s]
-
-For the mass flow rates, this indicates the peak volume flow calculation (m3/s) over the 24 hour condensed sizing period.
-
-Or as depicted in a chart:
-
-![](media/image018.jpg)
-
-Figure 6. Zone Sizing from epluszsz.csv
-
-
-
-eplusout.&lt;ext&gt;
-----------------
-
-The eplusout.csv (or txt or tab extension) is a file that can be produced by post-processing on the eplusout.eso file. EnergyPlus distributes a post-processing program (ReadVarsESO – see next section) with the installation.
-
-eplusmtr.&lt;ext&gt;
-----------------
-
-The eplusmtr.csv (or txt or tab extension) is a file that can be produced by post-processing on the eplusout.mtr file. EnergyPlus distributes a post-processing program (ReadVarsESO – see next section) with the installation.
-
-eplusmap.&lt;ext&gt;
-----------------
-
-The eplusmap.csv (or txt or tab extension) is a file that is generated by the Output:IlluminanceMap object. These are calculated for the Daylighting:Controls daylighting option. By default, this is a comma delimited text file (csv) that can be imported into a spreadsheet program. For example, the input for the Output:IlluminanceMap object shown below:
-
-```
-Output:IlluminanceMap,
-    Daylit Map,              !- Map Name
-    Daylit Zone,             !- Zone Name
-    0.8,                     !- Z height {m}
-    0.1,                     !- X minimum coordinate {m}
-    4.9,                     !- X maximum coordinate {m}
-    10,                      !- Number of X grid points
-    0.1,                     !- Y minimum coordinate {m}
-    9.9,                     !- Y maximum coordinate {m}
-    10;                      !- Number of Y grid points
-```
-
-generates the following output in csv format when viewed with Microsoft Excel.  **Note that if the point is outside the zone a “\*� will be shown.**
-
-![](media/image019.png)
-
-Figure 7. Spreadsheet view of Daylight Map output
-
-Each cell reports the illuminance (in lux) at the location specified by the (X;Y) coordinates in the column and row headers. These are XY pairs separated by a semi-colon for ease in importing into the spreadsheet. The Z coordinate of the map is shown in the title (the illuminance map is set in a plane). The date and time are indicated in the upper left cell of the map. One map is reported for every hour of the simulation.
-
-The illuminance values are organized to allow the user to rapidly plot a visualization of the data using Microsoft Excel’s standard “3-D Column� graph. A 3-D graph is shown below for the data in a single day similar to the earlier example.
-
-![](media/image020.png)
-
-Figure 8. 3D Graph of Illuminance Map
-
-The following figure illustrates a similar map for the tubular daylighting device example file that is included with the installation.
-
-![](media/image021.png)
-
-Figure 9. A 3D illuminance map for the tubular daylighting device file
-
-Individual 3-D graphs can be generated for each hour of a given day and collected to generate a sequence of graphs representing the progression of daylighting conditions over the course of the day. Using additional software tools (not provided with EnergyPlus) the user can do further post-processing to link screenshots of the graphs into an animated sequence.
-
-eplusout.dfs
-------------
-
-The daylight factors report contains the pre-calculated hourly daylight factors for the four CIE sky types (clear, clear turbid, intermediate, and overcast sky) and two daylight reference points for each exterior window of a daylight zone. The file is CSV formatted – ready for spreadsheet viewing. The input for requesting the report is simple:
-
-The following shows an excerpt the daylight factors for a window without shade:
-
-This file contains daylight factors for all exterior windows of daylight zones.
-
-If only one reference point the last 4 columns in the data will be zero.
-
-MonthAndDay,Zone Name,Window Name,Window State
-
-Hour,Daylight Factor for Clear Sky at Reference point 1,Daylight Factor for Clear Turbid Sky at Reference point 1,Daylight Factor for Intermediate Sky at Reference point 1,Daylight Factor for Overcast Sky at Reference point 1,Daylight Factor for Clear Sky at Reference point 2,Daylight Factor for Clear Turbid Sky at Reference point 2,Daylight Factor for Intermediate Sky at Reference point 2,Daylight Factor for Overcast Sky at Reference point 2
-
-01/21,PERIMETER\_BOT\_ZN\_1,PERIMETER\_BOT\_ZN\_1\_WALL\_SOUTH\_WINDOW,Base Window
-
-1,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-2,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-3,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-4,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-5,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-6,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-7,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-8,5.08810E-002,5.78633E-002,2.59271E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
-
-9,5.85018E-002,6.68126E-002,3.02054E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
-
-10,6.26710E-002,7.12830E-002,3.37475E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
-
-11,6.35876E-002,7.17181E-002,3.59982E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
-
-12,6.23746E-002,6.98139E-002,3.66365E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
-
-13,6.39669E-002,7.21972E-002,3.61684E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
-
-14,6.25455E-002,7.10272E-002,3.39911E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
-
-15,5.85994E-002,6.67866E-002,3.05581E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
-
-16,5.17581E-002,5.89493E-002,2.63461E-002,1.42712E-002,0.00000,0.00000,0.00000,0.00000
-
-17,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-18,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-19,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-20,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-21,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-22,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-23,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-24,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000,0.00000
-
-
-
-The first line describes the data in the eplusout.dfs file. The second line describes the header of the daily row:
-
-<table class="table table-striped">
-<tr>
-<th>Month and Day</th>
-<th>Zone Name</th>
-<th>Window Name</th>
-<th>Window State</th>
-</tr>
-<tr>
-<td>01/21</td>
-<td>PERIMETER_BOT_ZN_1</td>
-<td>PERIMETER_BOT_ZN_1_WALL_SOUTH_WINDOW</td>
-<td>Base Window</td>
-</tr>
-</table>
-
-
-
-The Window State column has three possible outputs – Base Window indicating windows without shades; a numeric value, from 0.0 to 180.0 for every 10.0 step, indicating the slat angle (in degrees) of the blind shading the window; blink indicating windows in shaded state by shades, screens, and blinds with fixed slat angle.
-
-The third line describes the hourly daylight factors. Note that the last 4 columns are 0.0 because there is only one daylight reference point.:
-
-<table class="table table-striped">
-<tr>
-<th>Hour</th>
-<th>Daylight factor for clear sky at reference point 1</th>
-<th>Daylight factor for clear turbid sky at reference point 1</th>
-<th>Daylight factor for intermediate sky at reference point 1</th>
-<th>Daylight factor for overcast sky at reference point 1</th>
-<th>Daylight factor for clear sky at reference point 2</th>
-<th>Daylight factor for clear turbid sky at reference point 2</th>
-<th>Daylight factor for intermediate sky at reference point 2</th>
-<th>Daylight factor for overcast sky at reference point 2</th>
-</tr>
-<tr>
-<td>10</td>
-<td>0.06239</td>
-<td>0.07088</td>
-<td>0.03377</td>
-<td>0.01427</td>
-<td>0.0</td>
-<td>0.0</td>
-<td>0.0</td>
-<td>0.0</td>
-</tr>
-</table>
-
-
-
-eplusscreen.csv
----------------
-
-Results of the window screen transmittance map. This file can be used to create a 3-D Column chart for graphically viewing the direct beam and reflected beam transmittance at various relative azimuth and relative altitude angles. The “relative� angles in this file are the incident solar angles with respect to the outward surface normal. The figures below are example 3-D charts generated using the data provided in this output file.
-
-![TransmittancePlotExample](media/image022.jpg)
-
-
-
-eplustbl.&lt;ext&gt;
-----------------
-
-The eplustbl file contains the tabular output results that are created when using the following objects:
-
-- Output:Table:SummaryReports
-
-- Output:Table:TimeBins
-
-- Output:Table:Monthly
-
-- UtilityCost:Tariff
-
-- ComponentCost:Line Item
-
-The format and the extension for the file depends on the setting of the ColumnSeparator field of the Output:Table:Style object. The choices of HTML, tab, fixed, comma, and XML result in eplustbl.htm, eplustbl.tab, eplustbl.txt, eplustbl.csv, eplustbl.xml respectively. The HTML version of the report also includes a table of contents that allows easier navigation through the file.
-
-By default the energy units reported in all of the eplustbl files are in Joules (J) but the UnitConversion field of the Output:Table:Style object allows for the values to be reported in MJ, GJ or in kWh. In addition, the Output:Table:Style object can specify for the tables to be in IP units for all fields.
-
-### Output:Table:SummaryReports
-
-Several predefined reports are available from the Output:Table:SummaryReports object including the following. (spaces are inserted in names for readability; keys are included in the Input Data Dictionary or by just removing the spaces):
-
-- All Summary
-
-Lists all following applicable tables with “Summary� in the name.
-
-- All Monthly
-
-Lists all following applicable tables with “Monthly� in the name.
-
-- All Summary And Monthly
-
-Lists all following applicable tables with both “Summary� and “Monthly� in the name. This does not include the Zone Component Load Summary report.
-
-- All Summary and Sizing Period
-
-Lists the All Summary tables as well as the Zone Component Load report (currently the only Sizing Period report). Please note that the Zone Component Load report does increase the run time because it repeats sizing periods.
-
-- All Summary Monthly and Sizing Period
-
-Lists the All Summary tables, the Monthly tables as well as the Zone Component Load report (currently the only Sizing Period report). Please note that the Zone Component Load report does increase the run time because it repeats sizing periods.
-
-- Annual Building Utility Performance Summary
-
-- Input Verification and Results Summary
-
-- Demand End Use Components Summary
-
-- Source Energy End Use Components Summary
-
-- Climatic Data Summary
-
-- Equipment Summary
-
-- Envelope Summary
-
-- Surface Shadowing Summary
-
-- Shading Summary
-
-- Lighting Summary
-
-- HVAC Sizing Summary
-
-- System Summary
-
-- Component Sizing Summary
-
-- Outdoor Air Summary
-
-- Object Count Summary
-
-- Component Cost Economics Summary
-
-- Energy Meters
-
-- Sensible Heat Gain Summary
-
-- Standard 62.1 Summary
-
-- Zone Component Load Summary
-
-- Zone Cooling Summary Monthly
-
-- Zone Heating Summary Monthly
-
-- Zone Electric Summary Monthly
-
-- Space Gains Monthly
-
-- Peak Space Gains Monthly
-
-- Space Gain Components At Cooling Peak Monthly
-
-- Energy Consumption Electricity Natural Gas Monthly
-
-- Energy Consumption Electricity Generated Propane Monthly
-
-- Energy Consumption Diesel FuelOil Monthly
-
-- Energy Consumption District Heating Cooling Monthly
-
-- Energy Consumption Coal Gasoline Monthly
-
-- End Use Energy Consumption Electricity Monthly
-
-- End Use Energy Consumption NaturalGas Monthly
-
-- End Use Energy Consumption Diesel Monthly
-
-- End Use Energy Consumption FuelOil Monthly
-
-- End Use Energy Consumption Coal Monthly
-
-- End Use Energy Consumption Propane Monthly
-
-- End Use Energy Consumption Gasoline Monthly
-
-- Peak Energy End Use Electricity Part1 Monthly
-
-- Peak Energy End Use Electricity Part2 Monthly
-
-- Electric Components Of Peak Demand Monthly
-
-- Peak Energy End Use NaturalGas Monthly
-
-- Peak Energy End Use Diesel Monthly
-
-- Peak Energy End Use FuelOil Monthly
-
-- Peak Energy End Use Coal Monthly
-
-- Peak Energy End Use Propane Monthly
-
-- Peak Energy End Use Gasoline Monthly
-
-- Setpoints Not Met With Temperatures Monthly
-
-- Comfort Report Simple55 Monthly
-
-- Unglazed Transpired Solar Collector Summary Monthly
-
-- Occupant Comfort Data Summary Monthly
-
-- Chiller Report Monthly
-
-- Tower Report Monthly
-
-- Boiler Report Monthly
-
-- DX Report Monthly
-
-- Window Report Monthly
-
-- Window Energy Report Monthly
-
-- Window Zone Summary Monthly
-
-- Window Energy Zone Summary Monthly
-
-- Average Outdoor Conditions Monthly
-
-- Outdoor Conditions Maximum DryBulb Monthly
-
-- Outdoor Conditions Minimum DryBulb Monthly
-
-- Outdoor Conditions Maximum WetBulb Monthly
-
-- Outdoor Conditions Maximum DewPoint Monthly
-
-- Outdoor Ground Conditions Monthly
-
-- WindowAC Report Monthly
-
-- Water Heater Report Monthly
-
-- Generator Report Monthly
-
-- Daylighting Report Monthly
-
-- Coil Report Monthly
-
-- PlantLoop Demand Report Monthly
-
-- Fan Report Monthly
-
-- Pump Report Monthly
-
-- CondLoop Demand Report Monthly
-
-- Zone Temperature Oscillation Report Monthly
-
-- AirLoop System Energy And Water Use Monthly
-
-- AirLoop System Component Loads Monthly
-
-- AirLoop System Component Energy Use Monthly
-
-- Mechanical Ventilation Loads Monthly
-
-Each of these reports is made up of several sub-tables of information. Examples of some of the tables are shown below. To enable all of the reports the single All Summary may be specified.
-
-### Annual Building Utility Performance Summary
-
-The Annual Building Utility Performance Summary report provides an overview of energy consumption in the building for different end uses. The following is an example this report (some columns may be truncated due to page size). The key used to obtain this report is AnnualBuildingUtilityPerformanceSummary.
-
-In the *Comfort and Setpoint Not Met Summary* sub-table, facility hours represents the total number of hours that any single zone did not meet the comfort or setpoint criteria. It is not weighted by number of zones or number of occupants.
-
-The values in the *End Uses* sub-table are from report meters. To determine which components are attached to each end-use meter, consult the meter details output file (\*.mtd).
-
-
-
-Report: Annual Building Utility Performance Summary
-
-For: Entire Facility
-
-Timestamp: 2009-02-10 12:39:35
-
-Values gathered over 8760.00 hours
-
-
-
-
-
-
-Site and Source Energy
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Total Energy (GJ)</th>
-<th>Energy Per Total Building Area (MJ/m2)</th>
-<th>Energy Per Conditioned Building Area (MJ/m2)</th>
-</tr>
-<tr>
-<td>Total Site Energy</td>
-<td>194.80</td>
-<td>210.09</td>
-<td>210.09</td>
-</tr>
-<tr>
-<td>Net Site Energy</td>
-<td>194.80</td>
-<td>210.09</td>
-<td>210.09</td>
-</tr>
-<tr>
-<td>Total Source Energy</td>
-<td>532.25</td>
-<td>574.04</td>
-<td>574.04</td>
-</tr>
-<tr>
-<td>Net Source Energy</td>
-<td>532.25</td>
-<td>574.04</td>
-<td>574.04</td>
-</tr>
-</table>
-
-
-
-
-
-Source to Site Energy Converstion Factors
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Source=&gt;Site Conversion Factor</th>
-</tr>
-<tr>
-<td>Electricity</td>
-<td>3.167</td>
-</tr>
-<tr>
-<td>Natural Gas</td>
-<td>1.084</td>
-</tr>
-<tr>
-<td>District Cooling</td>
-<td>1.056</td>
-</tr>
-<tr>
-<td>District Heating</td>
-<td>3.613</td>
-</tr>
-<tr>
-<td>Steam</td>
-<td>0.300</td>
-</tr>
-<tr>
-<td>Gasoline</td>
-<td>1.050</td>
-</tr>
-<tr>
-<td>Diesel</td>
-<td>1.050</td>
-</tr>
-<tr>
-<td>Coal</td>
-<td>1.050</td>
-</tr>
-<tr>
-<td>Fuel Oil #1</td>
-<td>1.050</td>
-</tr>
-<tr>
-<td>Fuel Oil #2</td>
-<td>1.050</td>
-</tr>
-<tr>
-<td>Propane</td>
-<td>1.050</td>
-</tr>
-</table>
-
-
-
-
-
-Building Area
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Area (m2)</th>
-</tr>
-<tr>
-<td>Total Building Area</td>
-<td>927.20</td>
-</tr>
-<tr>
-<td>Net Conditioned Building Area</td>
-<td>927.20</td>
-</tr>
-<tr>
-<td>Unconditioned Building Area</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
-
-
-End Uses
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Electricity (GJ)</th>
-<th>Natural Gas (GJ)</th>
-<th>Other Fuel (GJ)</th>
-<th>District Cooling (GJ)</th>
-<th>District Heating (GJ)</th>
-<th>Water (m3)</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>0.00</td>
-<td>40.65</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>18.18</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>81.24</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>47.70</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>7.03</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Total End Uses</td>
-<td>154.15</td>
-<td>40.65</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-*Note: Natural gas appears to be the principal heating source based on energy usage.*
-
-
-
-End Uses By Subcategory
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Subcategory</th>
-<th>Electricity (GJ)</th>
-<th>Natural Gas (GJ)</th>
-<th>Other Fuel (GJ)</th>
-<th>District Cooling (GJ)</th>
-<th>District Heating (GJ)</th>
-<th>Water (m3)</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>General</td>
-<td>0.00</td>
-<td>40.65</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>General</td>
-<td>18.18</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>GeneralLights</td>
-<td>81.24</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>General</td>
-<td>47.70</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>General</td>
-<td>7.03</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
-
-
-Normalized Metrics
-
-
-
-Utility Use Per Conditioned Floor Area
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Electricity Intensity (MJ/m2)</th>
-<th>Natural Gas Intensity (MJ/m2)</th>
-<th>Other Fuel Intensity (MJ/m2)</th>
-<th>District Cooling Intensity (MJ/m2)</th>
-<th>District Heating Intensity (MJ/m2)</th>
-<th>Water Intensity (m3/m2)</th>
-</tr>
-<tr>
-<td>Lighting</td>
-<td>87.62</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>HVAC</td>
-<td>27.19</td>
-<td>43.84</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Other</td>
-<td>51.44</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>166.25</td>
-<td>43.84</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
-
-
-Utility Use Per Total Floor Area
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Electricity Intensity (MJ/m2)</th>
-<th>Natural Gas Intensity (MJ/m2)</th>
-<th>Other Fuel Intensity (MJ/m2)</th>
-<th>District Cooling Intensity (MJ/m2)</th>
-<th>District Heating Intensity (MJ/m2)</th>
-<th>Water Intensity (m3/m2)</th>
-</tr>
-<tr>
-<td>Lighting</td>
-<td>87.62</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>HVAC</td>
-<td>27.19</td>
-<td>43.84</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Other</td>
-<td>51.44</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>166.25</td>
-<td>43.84</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
-
-
-Electric Loads Satisfied
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Electricity (GJ)</th>
-<th>Percent Electricity (%)</th>
-</tr>
-<tr>
-<td>Fuel-Fired Power Generation</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>High Temperature Geothermal*</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Photovoltaic Power</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Wind Power*</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Net Decrease in On-Site Storage</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total On-Site Electric Sources</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Electricity Coming From Utility</td>
-<td>154.15</td>
-<td>100.00</td>
-</tr>
-<tr>
-<td>Surplus Electricity Going To Utility</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Net Electricity From Utility</td>
-<td>154.15</td>
-<td>100.00</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Total On-Site and Utility Electric Sources</td>
-<td>154.15</td>
-<td>100.00</td>
-</tr>
-<tr>
-<td>Total Electricity End Uses</td>
-<td>154.15</td>
-<td>100.00</td>
-</tr>
-</table>
-
-
-
- On-Site Thermal Sources
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Heat (GJ)</th>
-<th>Percent Heat (%)</th>
-</tr>
-<tr>
-<td>Water-Side Heat Recovery</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>Air to Air Heat Recovery for Cooling</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>Air to Air Heat Recovery for Heating</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>High-Temperature Geothermal*</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>Solar Water Thermal</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>Solar Air Thermal</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>Total On-Site Thermal Sources</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-</table>
-
-
-
-
-
-Water Source Summary
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Water (m3)</th>
-<th>Percent Water (%)</th>
-</tr>
-<tr>
-<td>Rainwater Collection</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Condensate Collection</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Groundwater Well</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Total On Site Water Sources</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>-</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Initial Storage</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Final Storage</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Change in Storage</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>-</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Water Supplied by Utility</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>-</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Total On Site, Change in Storage, and Utility Water Sources</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Total Water End Uses</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-</table>
-
-
-
-
-
-Comfort and Setpoint Not Met Summary
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Facility (Hours)</th>
-</tr>
-<tr>
-<td>Time Set Point Not Met During Occupied Heating</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Time Set Point Not Met During Occupied Cooling</td>
-<td>406.00</td>
-</tr>
-<tr>
-<td>Time Not Comfortable Based on Simple ASHRAE 55-2004</td>
-<td>1033.00</td>
-</tr>
-</table>
-
-
-
-
-
-Note 1: An asterisk (\*) indicates that the feature is not yet implemented.
-
-### Input Verification and Results Summary
-
-The Input Verification and Results Summary report provides a summary of some of the most common input assumptions that are not included in any of the other predefined reports. Directly following is an example of the report. The key used to obtain this report is InputVerificationandResultsSummary.
-
-Report: Input Verification and Results Summary
-
-For: Entire Facility
-
-Timestamp: 2009-02-10 12:39:35
-
-General
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Value</th>
-</tr>
-<tr>
-<td>Program Version and Build</td>
-<td>EnergyPlus, Version 3.1</td>
-</tr>
-<tr>
-<td>Weather</td>
-<td>Chicago IL United States TMY2 94846 WMO#=725340</td>
-</tr>
-<tr>
-<td>Latitude (deg)</td>
-<td>41.78</td>
-</tr>
-<tr>
-<td>Longitude (deg)</td>
-<td>-87.8</td>
-</tr>
-<tr>
-<td>Elevation (m)</td>
-<td>190.00</td>
-</tr>
-<tr>
-<td>Time Zone</td>
-<td>-6.0</td>
-</tr>
-<tr>
-<td>North Axis Angle (deg)</td>
-<td>30.00</td>
-</tr>
-<tr>
-<td>Hours Simulated (hrs)</td>
-<td>8760.00</td>
-</tr>
-</table>
-
-
-
-
-
-ENVELOPE
-
-
-
-Window-Wall Ratio
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Total</th>
-<th>North (315 to 45 deg)</th>
-<th>East (45 to 135 deg)</th>
-<th>South (135 to 225 deg)</th>
-<th>West (225 to 315 deg)</th>
-</tr>
-<tr>
-<td>Gross Wall Area (m2)</td>
-<td>274.20</td>
-<td>91.50</td>
-<td>45.60</td>
-<td>91.50</td>
-<td>45.60</td>
-</tr>
-<tr>
-<td>Window Opening Area (m2)</td>
-<td>61.65</td>
-<td>20.85</td>
-<td>9.12</td>
-<td>22.56</td>
-<td>9.12</td>
-</tr>
-<tr>
-<td>Window-Wall Ratio (%)</td>
-<td>22.48</td>
-<td>22.79</td>
-<td>20.00</td>
-<td>24.66</td>
-<td>20.00</td>
-</tr>
-</table>
-
-
-
-
-
-Skylight-Roof Ratio
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Total</th>
-</tr>
-<tr>
-<td>Gross Roof Area (m2)</td>
-<td>463.60</td>
-</tr>
-<tr>
-<td>Skylight Area (m2)</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Skylight-Roof Ratio (%)</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
-
-
-PERFORMANCE
-
-
-
-Zone Summary
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Area (m2)</th>
-<th>Conditioned (Y/N)</th>
-<th>Volume (m3)</th>
-<th>Multipliers</th>
-<th>Gross Wall Area (m2)</th>
-<th>Window Glass Area (m2)</th>
-<th>Lighting (W/m2)</th>
-<th>People (m2/person)</th>
-<th>Plug and Process(W/m2)</th>
-</tr>
-<tr>
-<td>PLENUM-1</td>
-<td>463.60</td>
-<td>Yes</td>
-<td>283.20</td>
-<td>1.00</td>
-<td>54.84</td>
-<td>0.00</td>
-<td>0.0000</td>
-<td> </td>
-<td>0.0000</td>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>99.16</td>
-<td>Yes</td>
-<td>239.25</td>
-<td>1.00</td>
-<td>73.20</td>
-<td>22.56</td>
-<td>15.9742</td>
-<td>9.01</td>
-<td>10.6495</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>42.73</td>
-<td>Yes</td>
-<td>103.31</td>
-<td>1.00</td>
-<td>36.48</td>
-<td>9.12</td>
-<td>16.0056</td>
-<td>8.55</td>
-<td>10.6704</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>96.48</td>
-<td>Yes</td>
-<td>239.25</td>
-<td>1.00</td>
-<td>73.20</td>
-<td>20.85</td>
-<td>16.4179</td>
-<td>8.77</td>
-<td>10.9453</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>42.73</td>
-<td>Yes</td>
-<td>103.31</td>
-<td>1.00</td>
-<td>36.48</td>
-<td>9.12</td>
-<td>16.0056</td>
-<td>8.55</td>
-<td>10.6704</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>182.49</td>
-<td>Yes</td>
-<td>447.68</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>16.2420</td>
-<td>9.12</td>
-<td>10.8280</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>927.20</td>
-<td> </td>
-<td>1416.00</td>
-<td> </td>
-<td>274.20</td>
-<td>61.65</td>
-<td>8.0889</td>
-<td>17.83</td>
-<td>5.3926</td>
-</tr>
-<tr>
-<td>Conditioned Total</td>
-<td>927.20</td>
-<td> </td>
-<td>1416.00</td>
-<td> </td>
-<td>274.20</td>
-<td>61.65</td>
-<td>8.0889</td>
-<td>17.83</td>
-<td>5.3926</td>
-</tr>
-<tr>
-<td>Unconditioned Total</td>
-<td>0.00</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-### Demand End Use Components Summary
-
-The Demand End Use Components Summary report shows the demand breakdown by component end use at the time that the peak demand for each source of energy is set. The time of the peak demand is shown in the first row. The contributions of each end use at the time of the peak demand of the energy source is shown in this report. The key used to obtain this report is DemandEndUseComponentsSummary.
-
-
-
-Report: Demand End Use Components Summary
-
-For: Entire Facility
-
-Timestamp: 2009-02-10 12:39:35
-
-End Uses
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Electricity (W)</th>
-<th>Natural Gas (W)</th>
-<th>Propane (W)</th>
-<th>District Cooling (W)</th>
-<th>Steam (W)</th>
-<th>Water (m3/s)</th>
-</tr>
-<tr>
-<td>Time of Peak</td>
-<td>02-JUL-14:00</td>
-<td>31-DEC-07:15</td>
-<td>-</td>
-<td>-</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Heating</td>
-<td>0.00</td>
-<td>81764.44</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>12342.62</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>7500.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>4000.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>1498.36</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Total End Uses</td>
-<td>25340.97</td>
-<td>81764.44</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
-
-
-End Uses By Subcategory
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Subcategory</th>
-<th>Electricity (W)</th>
-<th>Natural Gas (W)</th>
-<th>Propane (W)</th>
-<th>District Cooling (W)</th>
-<th>Steam (W)</th>
-<th>Water (m3/s)</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>General</td>
-<td>0.00</td>
-<td>81764.44</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>General</td>
-<td>12342.62</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>GeneralLights</td>
-<td>7500.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>General</td>
-<td>4000.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>General</td>
-<td>1498.36</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-### Source Energy End Use Components Summary
-
-The Source Energy End Use Components Summary report produces a report that includes three tables. These tables display source energy by fuel type that is calculated based on site to source energy factors specified by the user in the EnvironmentalImpactFactors and FuelFactors objects. The last two tables display the source energy in terms of area normalized metrics. Directly following is an example of the three tables. The key used to obtain this report is SourceEnergyEndUseComponentsSummary.
-
-
-
-Report: **Source Energy End Use Components Summary**
-
-For: **Entire Facility**
-
-Timestamp: **2011-10-07 20:53:43**
-
-**Values gathered over 8760.00 hours**
-
- **Source Energy End Use Components Summary**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Source Electricity [GJ]</th>
-<th>Source Natural Gas [GJ]</th>
-<th>Source Other Fuel [GJ]</th>
-<th>Source District Cooling [GJ]</th>
-<th>Source District Heating [GJ]</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>0.00</td>
-<td>140.03</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>167.65</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>569.39</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>325.49</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>55.72</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>7.57</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-</tr>
-<tr>
-<td>Total Source Energy End Use Components</td>
-<td>1125.82</td>
-<td>140.03</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
- **Normalized Metrics**
-
- **Source Energy End Use Components Per Conditioned Floor Area**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Source Electricity [MJ/m2]</th>
-<th>Source Natural Gas [MJ/m2]</th>
-<th>Source Other Fuel [MJ/m2]</th>
-<th>Source District Cooling [MJ/m2]</th>
-<th>Source District Heating [MJ/m2]</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>0.00</td>
-<td>151.02</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>180.82</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>614.09</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>351.05</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>60.10</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>8.16</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-</tr>
-<tr>
-<td>Total Source Energy End Use Components</td>
-<td>1214.22</td>
-<td>151.02</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
- **Source Energy End Use Components Per Total Floor Area**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Source Electricity [MJ/m2]</th>
-<th>Source Natural Gas [MJ/m2]</th>
-<th>Source Other Fuel [MJ/m2]</th>
-<th>Source District Cooling [MJ/m2]</th>
-<th>Source District Heating [MJ/m2]</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>0.00</td>
-<td>151.02</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>180.82</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>614.09</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>351.05</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>60.10</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>8.16</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-</tr>
-<tr>
-<td>Total Source Energy End Use Components</td>
-<td>1214.22</td>
-<td>151.02</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
-### Equipment Summary
-
-The Equipment Summary report provides a summary of the HVAC related equipment in the building. The central chiller example shows the most common type of chillers, boilers and towers used in EnergyPlus. The remaining subtables cover DX coils, fans and water heating equipment. Not every type of HVAC equipment is represented in this report. Directly following is an example of the report. The key used to obtain this report is EquipmentSummary.
-
-
-
-Report: Equipment Summary
-
-For: Entire Facility
-
-Timestamp: 2009-02-10 12:39:35
-
-Central Plant
-
-<table class="table table-striped">
-<tr>
-<td> </td>
-<th>Type</th>
-<th>Nominal Capacity (W)</th>
-<th>Nominal Efficiency (W/W)</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Cooling Coils
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Nominal Total Capacity (W)</th>
-<th>Nominal Sensible Capacity (W)</th>
-<th>Nominal Latent Capacity (W)</th>
-<th>Nominal Sensible Heat Ratio</th>
-<th>Nominal Efficiency (W/W)</th>
-</tr>
-<tr>
-<td>MAIN COOLING COIL 1</td>
-<td>Coil:Cooling:DX:TwoSpeed</td>
-<td>37506.82</td>
-<td>25504.64</td>
-<td>12002.18</td>
-<td>0.68</td>
-<td>3.00</td>
-</tr>
-</table>
-
-
-
- Heating Coils
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Nominal Total Capacity (W)</th>
-<th>Nominal Efficiency (W/W)</th>
-</tr>
-<tr>
-<td>SPACE1-1 ZONE COIL</td>
-<td>Coil:Heating:Gas</td>
-<td>17614.83</td>
-<td>0.80</td>
-</tr>
-<tr>
-<td>SPACE2-1 ZONE COIL</td>
-<td>Coil:Heating:Gas</td>
-<td>14619.82</td>
-<td>0.80</td>
-</tr>
-<tr>
-<td>SPACE3-1 ZONE COIL</td>
-<td>Coil:Heating:Gas</td>
-<td>16093.74</td>
-<td>0.80</td>
-</tr>
-<tr>
-<td>SPACE4-1 ZONE COIL</td>
-<td>Coil:Heating:Gas</td>
-<td>18942.35</td>
-<td>0.80</td>
-</tr>
-<tr>
-<td>SPACE5-1 ZONE COIL</td>
-<td>Coil:Heating:Gas</td>
-<td>19146.73</td>
-<td>0.80</td>
-</tr>
-<tr>
-<td>MAIN HEATING COIL 1</td>
-<td>Coil:Heating:Gas</td>
-<td>19754.61</td>
-<td>0.80</td>
-</tr>
-</table>
-
-
-
- Fans
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Total Efficiency (W/W)</th>
-<th>Delta Pressure (pa)</th>
-<th>Max Flow Rate (m3/s)</th>
-<th>Rated Power (W)</th>
-<th>Motor Heat In Air Fraction</th>
-<th>End Use</th>
-</tr>
-<tr>
-<td>SUPPLY FAN 1</td>
-<td>Fan:VariableVolume</td>
-<td>0.70</td>
-<td>600.00</td>
-<td>2.27</td>
-<td>1942.10</td>
-<td>1.00</td>
-<td>General</td>
-</tr>
-</table>
-
-
-
- Pumps
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Control</th>
-<th>Head (pa)</th>
-<th>Power (W)</th>
-<th>Motor Efficiency (W/W)</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Service Water Heating
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Storage Volume (m3)</th>
-<th>Input(W)</th>
-<th>Thermal Efficiency (W/W)</th>
-<th>Recovery Efficiency (W/W)</th>
-<th>Energy Factor</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-### Envelope Summary
-
-The Envelope Summary report provides a summary of the elements of the envelope of the building. The first table describes the exterior opaque elements and the second table describes the fenestration elements. Reflectance is defined as one minus the thermal absorptance. Directly following is an example of the report. The key used to obtain this report is EnvelopeSummary.
-
-
-
-Report: Envelope Summary
-
-For: Entire Facility
-
-Timestamp: 2009-02-10 12:39:35
-
-Opaque Exterior
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Construction</th>
-<th>Reflectance</th>
-<th>U-Factor with Film (W/m2-K)</th>
-<th>U-Factor no Film (W/m2-K)</th>
-<th>Gross Area (m2)</th>
-<th>Azimuth (deg)</th>
-<th>Tilt (deg)</th>
-<th>Cardinal Direction</th>
-</tr>
-<tr>
-<td>WALL-1PF</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.41</td>
-<td>18.30</td>
-<td>210.00</td>
-<td>90.00</td>
-<td>S</td>
-</tr>
-<tr>
-<td>WALL-1PR</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.41</td>
-<td>9.12</td>
-<td>120.00</td>
-<td>90.00</td>
-<td>E</td>
-</tr>
-<tr>
-<td>WALL-1PB</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.41</td>
-<td>18.30</td>
-<td>30.00</td>
-<td>90.00</td>
-<td>N</td>
-</tr>
-<tr>
-<td>WALL-1PL</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.41</td>
-<td>9.12</td>
-<td>300.00</td>
-<td>90.00</td>
-<td>W</td>
-</tr>
-<tr>
-<td>TOP-1</td>
-<td>ROOF-1</td>
-<td>0.35</td>
-<td>0.268</td>
-<td>0.28</td>
-<td>463.60</td>
-<td>210.00</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>FRONT-1</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.41</td>
-<td>73.20</td>
-<td>210.00</td>
-<td>90.00</td>
-<td>S</td>
-</tr>
-<tr>
-<td>F1-1</td>
-<td>FLOOR-SLAB-1</td>
-<td>0.35</td>
-<td>1.454</td>
-<td>2.25</td>
-<td>99.16</td>
-<td>30.00</td>
-<td>180.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>RIGHT-1</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.41</td>
-<td>36.48</td>
-<td>120.00</td>
-<td>90.00</td>
-<td>E</td>
-</tr>
-<tr>
-<td>F2-1</td>
-<td>FLOOR-SLAB-1</td>
-<td>0.35</td>
-<td>1.454</td>
-<td>2.25</td>
-<td>42.73</td>
-<td>300.00</td>
-<td>180.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>BACK-1</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.41</td>
-<td>73.20</td>
-<td>30.00</td>
-<td>90.00</td>
-<td>N</td>
-</tr>
-<tr>
-<td>F3-1</td>
-<td>FLOOR-SLAB-1</td>
-<td>0.35</td>
-<td>1.454</td>
-<td>2.25</td>
-<td>96.48</td>
-<td>74.22</td>
-<td>180.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>LEFT-1</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.41</td>
-<td>36.48</td>
-<td>300.00</td>
-<td>90.00</td>
-<td>W</td>
-</tr>
-<tr>
-<td>F4-1</td>
-<td>FLOOR-SLAB-1</td>
-<td>0.35</td>
-<td>1.454</td>
-<td>2.25</td>
-<td>42.73</td>
-<td>120.00</td>
-<td>180.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>F5-1</td>
-<td>FLOOR-SLAB-1</td>
-<td>0.35</td>
-<td>1.454</td>
-<td>2.25</td>
-<td>182.49</td>
-<td>30.00</td>
-<td>180.00</td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Fenestration
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Construction</th>
-<th>Area of One Opening (m2)</th>
-<th>Area of Openings (m2)</th>
-<th>U-Factor</th>
-<th>SHGC</th>
-<th>Visible Transmittance</th>
-<th>Shade Control</th>
-<th>Parent Surface</th>
-<th>Azimuth (deg)</th>
-<th>Cardinal Direction</th>
-</tr>
-<tr>
-<td>WF-1</td>
-<td>DBL CLR 3MM/13MM AIR</td>
-<td>16.56</td>
-<td>16.56</td>
-<td>2.72</td>
-<td>0.763</td>
-<td>0.812</td>
-<td>No</td>
-<td>FRONT-1</td>
-<td>210.00</td>
-<td>S</td>
-</tr>
-<tr>
-<td>DF-1</td>
-<td>SGL GREY 3MM</td>
-<td>6.00</td>
-<td>6.00</td>
-<td>5.89</td>
-<td>0.708</td>
-<td>0.611</td>
-<td>No</td>
-<td>FRONT-1</td>
-<td>210.00</td>
-<td>S</td>
-</tr>
-<tr>
-<td>WR-1</td>
-<td>DBL CLR 3MM/13MM AIR</td>
-<td>9.12</td>
-<td>9.12</td>
-<td>2.72</td>
-<td>0.763</td>
-<td>0.812</td>
-<td>No</td>
-<td>RIGHT-1</td>
-<td>120.00</td>
-<td>E</td>
-</tr>
-<tr>
-<td>WB-1</td>
-<td>DBL CLR 3MM/13MM AIR</td>
-<td>16.44</td>
-<td>16.44</td>
-<td>2.72</td>
-<td>0.763</td>
-<td>0.812</td>
-<td>No</td>
-<td>BACK-1</td>
-<td>30.00</td>
-<td>N</td>
-</tr>
-<tr>
-<td>DB-1</td>
-<td>SGL GREY 3MM</td>
-<td>4.41</td>
-<td>4.41</td>
-<td>5.89</td>
-<td>0.708</td>
-<td>0.611</td>
-<td>No</td>
-<td>BACK-1</td>
-<td>30.00</td>
-<td>N</td>
-</tr>
-<tr>
-<td>WL-1</td>
-<td>DBL CLR 3MM/13MM AIR</td>
-<td>9.12</td>
-<td>9.12</td>
-<td>2.72</td>
-<td>0.763</td>
-<td>0.812</td>
-<td>No</td>
-<td>LEFT-1</td>
-<td>300.00</td>
-<td>W</td>
-</tr>
-<tr>
-<td>Total or Average</td>
-<td> </td>
-<td> </td>
-<td>61.65</td>
-<td>3.26</td>
-<td>0.753</td>
-<td>0.778</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>North Total or Average</td>
-<td> </td>
-<td> </td>
-<td>20.85</td>
-<td>3.39</td>
-<td>0.751</td>
-<td>0.769</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Non-North Total or Average</td>
-<td> </td>
-<td> </td>
-<td>40.80</td>
-<td>3.19</td>
-<td>0.755</td>
-<td>0.782</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-### Surface Shadowing Summary
-
-The Surface Shadowing Summary report summarizes how the surfaces may cast shadows on other surfaces. Directly following is an example of the report. The key used to obtain this report is SurfaceShadowingSummary.
-
-Report: Surface Shadowing Summary
-
-For: Entire Facility
-
-Timestamp: 2007-10-17 08:54:27
-
-Surfaces (Walls, Roofs, etc) that may be Shadowed by Other Surfaces
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Possible Shadow Casters</th>
-</tr>
-<tr>
-<td>FRONT-1</td>
-<td>MAIN SOUTH OVERHANG |Mir-MAIN SOUTH OVERHANG |</td>
-</tr>
-<tr>
-<td>SOUTH DOOR OVERHANG</td>
-<td>Mir-MAIN SOUTH OVERHANG |WALL-1PF |FRONT-1 |</td>
-</tr>
-<tr>
-<td>WALL-1PF</td>
-<td>Mir-MAIN SOUTH OVERHANG |SOUTH DOOR OVERHANG |Mir-SOUTH DOOR OVERHANG |</td>
-</tr>
-<tr>
-<td>MAIN SOUTH OVERHANG</td>
-<td>FRONT-1 |</td>
-</tr>
-</table>
-
-
-
- Subsurfaces (Windows and Doors) that may be Shadowed by Surfaces
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Possible Shadow Casters</th>
-</tr>
-<tr>
-<td>WF-1</td>
-<td>FRONT-1 |</td>
-</tr>
-<tr>
-<td>DF-1</td>
-<td>FRONT-1 |</td>
-</tr>
-<tr>
-<td>WR-1</td>
-<td>RIGHT-1 |</td>
-</tr>
-<tr>
-<td>WB-1</td>
-<td>BACK-1 |</td>
-</tr>
-<tr>
-<td>DB-1</td>
-<td>BACK-1 |</td>
-</tr>
-<tr>
-<td>WL-1</td>
-<td>LEFT-1 |</td>
-</tr>
-</table>
-
-### Shading Summary
-
-The Shading Summary report shows how much of each window is sunlit at different times of the year and also includes a summary of the window controls. Directly following is an example of the report. The key used to obtain this report is ShadingSummary.
-
-Report: Shading Summary
-
-For: Entire Facility
-
-Timestamp: 2007-10-17 08:54:27
-
-Sunlit Fraction
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>March 21 9am</th>
-<th>March 21 noon</th>
-<th>March 21 3pm</th>
-<th>June 21 9am</th>
-<th>June 21 noon</th>
-<th>June 21 3pm</th>
-<th>December 21 9am</th>
-<th>December 21 noon</th>
-<th>December 21 3pm</th>
-</tr>
-<tr>
-<td>WF-1</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.43</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.30</td>
-<td>0.52</td>
-<td>0.86</td>
-</tr>
-<tr>
-<td>DF-1</td>
-<td>0.73</td>
-<td>0.26</td>
-<td>0.62</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.28</td>
-<td>0.90</td>
-<td>0.69</td>
-<td>0.92</td>
-</tr>
-<tr>
-<td>WR-1</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>WB-1</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>DB-1</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>WL-1</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-</tr>
-</table>
-
-
-
- Window Control
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Name</th>
-<th>Type</th>
-<th>Shaded Construction</th>
-<th>Control</th>
-<th>Glare Control</th>
-</tr>
-<tr>
-<td>none</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-### Lighting Summary
-
-The Lighting Summary report provides a description of the interior and exterior lighting systems being simulated. It also provides a summary of daylighting controls. The Interior Lighting table has three columns that are explained below:
-
-Scheduled Hours/Week [hr] - In the schedule shown, this represents the average weekly sum of hourly values. It is based on a full year even if the simulation is only performed for part of the year. It is not affected by daylighting.
-
-Hours/Week &gt; 1% [hr] – This represents the average hours per week that are above 1% of the design value.
-
-Full Load Hours/Week [hr] – This is based on consumption and hours that the consumption occurred. It is dependent on the run period used. When simulating only a portion of the year, the value depends on which days of the year (the number of weekdays versus weekend days, for example) are simulated. It also indicates the impact of daylighting control. Directly following is an example of the report. The key used to obtain this report is LightingSummary.
-
-Report: Lighting Summary
-
-For: Entire Facility
-
-Timestamp: 2012-09-05 12:10:52
-
-Interior Lighting
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Zone</th>
-<th>Lighting Power Density [W/m2]</th>
-<th>Zone Area [m2]</th>
-<th>Total Power [W]</th>
-<th>End Use Subcategory</th>
-<th>Schedule Name</th>
-<th>Scheduled Hours/Week [hr]</th>
-<th>Hours/Week &gt; 1% [hr]</th>
-<th>Full Load Hours/Week [hr]</th>
-<th>Return Air Fraction</th>
-<th>Conditioned (Y/N)</th>
-<th>Consumption [GJ]</th>
-</tr>
-<tr>
-<td>SPACE1-1 LIGHTS 1</td>
-<td>SPACE1-1</td>
-<td>15.9742</td>
-<td>99.16</td>
-<td>1584.00</td>
-<td>GeneralLights</td>
-<td>LIGHTS-1</td>
-<td>57.70</td>
-<td>168.00</td>
-<td>57.70</td>
-<td>0.2000</td>
-<td>Y</td>
-<td>17.16</td>
-</tr>
-<tr>
-<td>SPACE2-1 LIGHTS 1</td>
-<td>SPACE2-1</td>
-<td>16.0056</td>
-<td>42.73</td>
-<td>684.00</td>
-<td>GeneralLights</td>
-<td>HALFPERCENT</td>
-<td>0.60</td>
-<td>0.00</td>
-<td>0.59</td>
-<td>0.2000</td>
-<td>Y</td>
-<td>0.08</td>
-</tr>
-<tr>
-<td>SPACE3-1 LIGHTS 1</td>
-<td>SPACE3-1</td>
-<td>16.4179</td>
-<td>96.48</td>
-<td>1584.00</td>
-<td>GeneralLights</td>
-<td>ALWAYSON</td>
-<td>168.00</td>
-<td>168.00</td>
-<td>168.00</td>
-<td>0.2000</td>
-<td>Y</td>
-<td>49.95</td>
-</tr>
-<tr>
-<td>SPACE4-1 LIGHTS 1</td>
-<td>SPACE4-1</td>
-<td>16.0056</td>
-<td>42.73</td>
-<td>684.00</td>
-<td>GeneralLights</td>
-<td>LIGHTS-1</td>
-<td>57.70</td>
-<td>168.00</td>
-<td>57.70</td>
-<td>0.2000</td>
-<td>Y</td>
-<td>7.41</td>
-</tr>
-<tr>
-<td>SPACE5-1 LIGHTS 1</td>
-<td>SPACE5-1</td>
-<td>16.2420</td>
-<td>182.49</td>
-<td>2964.00</td>
-<td>GeneralLights</td>
-<td>LIGHTS-1</td>
-<td>57.70</td>
-<td>168.00</td>
-<td>57.70</td>
-<td>0.2000</td>
-<td>Y</td>
-<td>32.11</td>
-</tr>
-<tr>
-<td>Interior Lighting Total</td>
-<td> </td>
-<td>16.1777</td>
-<td>463.60</td>
-<td>7500.00</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>106.70</td>
-</tr>
-</table>
-
-
-
- Daylighting
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Zone</th>
-<th>Daylighting Type</th>
-<th>Control Type</th>
-<th>Fraction Controlled</th>
-<th>Lighting Installed in Zone [W]</th>
-<th>Lighting Controlled [W]</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Exterior Lighting
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Total Watts</th>
-<th>Astronomical Clock/Schedule</th>
-<th>Schedule Name</th>
-<th>Scheduled Hours/Week [hr]</th>
-<th>Hours/Week &gt; 1% [hr]</th>
-<th>Full Load Hours/Week [hr]</th>
-<th>Consumption [GJ]</th>
-</tr>
-<tr>
-<td>Exterior Lighting Total</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
-### HVAC Sizing Summary
-
-The HVAC Sizing Summary report provides information on the zone cooling and heating sizing and the peak load conditions as well as information about the system air flow sizing. The Design Load is the zone sensible load only and it does not include any system effects or ventilation loads. The user specified design load and airflow and the values calculated by the program are shown in the report along with the time of the peak load and the temperature and humidity ratio at the time of the peak during the sizing periods. This information is generated for both the Zone Sensible Cooling and Zone Sensible Heating tables. 
-
-Also included is the System Design Air Flow Rates which includes the calculated cooling air flow rate, the user specified air flow rate for cooling, the calculated heating air flow rate, and the user specified air flow rate for heating.
-
-*Note:* values listed as "calculated" are the unaltered result of the zone or system sizing calculations, using the design sizing period weather and schedules specified in the input. Values listed as "user specified" are either the calculated values modified by global or zone sizing factors or values specified with the *flow/zone* or *flow/system* design air flow method.
-
-Directly following is an example of the report.
-
-The key used to obtain this report is HVACSizingSummary. 
-
-Report: **HVAC Sizing Summary**
-
-For: **Entire Facility**
-
-** Timestamp: **2011-09-23 15:09:34
-
-**Zone Sensible Cooling**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Calculated Design Load [W]</th>
-<th>User Design Load [W]</th>
-<th>Calculated Design Air Flow [m3/s]</th>
-<th>User Design Air Flow [m3/s]</th>
-<th>Design Day Name</th>
-<th>Date/Time Of Peak</th>
-<th>Temperature at Peak [C]</th>
-<th>Humidity Ratio at Peak [kgWater/kgAir]</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>2647.33</td>
-<td>2647.33</td>
-<td>0.223</td>
-<td>0.223</td>
-<td>CHICAGO_IL_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB</td>
-<td>7/21 15:45:00</td>
-<td>31.02</td>
-<td>0.01459</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>2234.38</td>
-<td>2234.38</td>
-<td>0.188</td>
-<td>0.188</td>
-<td>CHICAGO_IL_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB</td>
-<td>7/21 10:00:00</td>
-<td>27.43</td>
-<td>0.01459</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>2506.34</td>
-<td>2506.34</td>
-<td>0.211</td>
-<td>0.211</td>
-<td>CHICAGO_IL_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB</td>
-<td>7/21 15:00:00</td>
-<td>31.50</td>
-<td>0.01459</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>2464.72</td>
-<td>2464.72</td>
-<td>0.207</td>
-<td>0.207</td>
-<td>CHICAGO_IL_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB</td>
-<td>7/21 17:30:00</td>
-<td>29.47</td>
-<td>0.01459</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>2628.69</td>
-<td>2628.69</td>
-<td>0.221</td>
-<td>0.221</td>
-<td>CHICAGO_IL_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB</td>
-<td>7/21 15:00:00</td>
-<td>31.50</td>
-<td>0.01459</td>
-</tr>
-</table>
-
-
-
- **Zone Sensible Heating**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Calculated Design Load [W]</th>
-<th>User Design Load [W]</th>
-<th>Calculated Design Air Flow [m3/s]</th>
-<th>User Design Air Flow [m3/s]</th>
-<th>Design Day Name</th>
-<th>Date/Time Of Peak</th>
-<th>Temperature at Peak [C]</th>
-<th>Humidity Ratio at Peak [kgWater/kgAir]</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>3860.76</td>
-<td>3860.76</td>
-<td>0.117</td>
-<td>0.117</td>
-<td>CHICAGO_IL_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB</td>
-<td>1/21 24:00:00</td>
-<td>-17.30</td>
-<td>0.00084</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>1625.15</td>
-<td>1625.15</td>
-<td>0.049</td>
-<td>0.049</td>
-<td>CHICAGO_IL_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB</td>
-<td>1/21 24:00:00</td>
-<td>-17.30</td>
-<td>0.00084</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>3753.07</td>
-<td>3753.07</td>
-<td>0.113</td>
-<td>0.113</td>
-<td>CHICAGO_IL_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB</td>
-<td>1/21 24:00:00</td>
-<td>-17.30</td>
-<td>0.00084</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>1625.15</td>
-<td>1625.15</td>
-<td>0.049</td>
-<td>0.049</td>
-<td>CHICAGO_IL_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB</td>
-<td>1/21 24:00:00</td>
-<td>-17.30</td>
-<td>0.00084</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>2981.57</td>
-<td>2981.57</td>
-<td>0.090</td>
-<td>0.103</td>
-<td>CHICAGO_IL_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB</td>
-<td>1/21 24:00:00</td>
-<td>-17.30</td>
-<td>0.00084</td>
-</tr>
-</table>
-
-
-
- **System Design Air Flow Rates**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Calculated cooling [m3/s]</th>
-<th>User cooling [m3/s]</th>
-<th>Calculated heating [m3/s]</th>
-<th>User heating [m3/s]</th>
-</tr>
-<tr>
-<td>VAV SYS 1</td>
-<td>1.05</td>
-<td>1.05</td>
-<td>0.43</td>
-<td>0.43</td>
-</tr>
-</table>
-
-**Plant Loop Coincident Design Fluid Flow Rate Adjustments**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Previous Design Volume Flow Rate [m3/s]</th>
-<th>Algorithm Volume Flow Rate [m3/s]</th>
-<th>Coincident Design Volume Flow Rate [m3/s]</th>
-<th>Coincident Size Adjusted</th>
-<th>Peak Sizing Period Name</th>
-<th>Peak Day into Period</th>
-<th>Peak Hour Of Day</th>
-<th>Peak Step Start Minute</th>
-</tr>
-<tr>
-<td>COOLSYS1 Sizing Pass 1</td>
-<td>0.120672</td>
-<td>0.141525</td>
-<td>0.141525</td>
-<td>Yes</td>
-<td>CHICAGO ANN CLG .4% CONDNS WB=>MDB HVAC Sizing Pass 1</td>
-<td>1</td>
-<td>2</td>
-<td>30></td>
-</tr>
-<tr>
-<td>HEATSYS1 Sizing Pass 1</td>
-<td>0.060598</td>
-<td>0.049054</td>
-<td>0.049054</td>
-<td>Yes</td>
-<td>CHICAGO ANN HTG 99.6% CONDNS DB HVAC Sizing Pass 1</td>
-<td>1</td>
-<td>7</td>
-<td>20></td>
-</tr>
-</table>
-
-### System Summary
-
-The System Summary report provides information about some of the primary components in the system including the economizer and demand controlled ventilation. In addition, this report describes when the zone conditions are not comfortable or when set points are not met.
-
-In the *Time Not Comfortable Based on Simple ASHRAE 55-2004* and Time Setpoint Not Met sub-tables, The reported time represents the total number of hours that a given zone did not meet the comfort or setpoint criteria. For the Facility row, this is the total numbers of hours that one or more zones were out of range. The values are not weighted by number of zones or number of occupants.
-
-Directly following is an example of the report. The key used to obtain this report is SystemSummary.
-
-
-
-Report: System Summary
-
-For: Entire Facility
-
-Timestamp: 2007-10-17 08:54:27
-
-Economizer
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>High Limit Shutoff Control</th>
-<th>Minimum Outside Air (m3/s)</th>
-<th>Maximum Outside Air (m3/s)</th>
-<th>Return Air Temp Limit</th>
-<th>Return Air Enthalpy Limit</th>
-<th>Outside Air Temperature Limit (C)</th>
-<th>Outside Air Enthalpy Limit (C)</th>
-</tr>
-<tr>
-<td>none</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Demand Controlled Ventilation using VENTILATION:MECHANICAL
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Ventilation:Mechanical Name</th>
-<th>Outside Air Per Person(m3/s-person)</th>
-<th>Outside Air Per Area (m3/s-m2)</th>
-</tr>
-<tr>
-<td>none</td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Time Not Comfortable Based on Simple ASHRAE 55-2004
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Winter Clothes (hr)</th>
-<th>Summer Clothes (hr)</th>
-<th>Summer or Winter Clothes (hr)</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>429.00</td>
-<td>1913.75</td>
-<td>79.25</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>739.25</td>
-<td>1719.75</td>
-<td>22.50</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>482.00</td>
-<td>1885.50</td>
-<td>85.50</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>588.25</td>
-<td>2039.75</td>
-<td>59.50</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>14.75</td>
-<td>2535.75</td>
-<td>14.75</td>
-</tr>
-<tr>
-<td>PLENUM-1</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Facility</td>
-<td>1041.75</td>
-<td>2564.75</td>
-<td>97.00</td>
-</tr>
-</table>
-
-
-
- Time Setpoint Not Met
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>During Heating (hr)</th>
-<th>During Cooling (hr)</th>
-<th>During Occupied Heating (hr)</th>
-<th>During Occupied Cooling (hr)</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>321.00</td>
-<td>45.25</td>
-<td>35.00</td>
-<td>45.25</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>104.25</td>
-<td>44.00</td>
-<td>0.25</td>
-<td>10.75</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>297.50</td>
-<td>0.75</td>
-<td>36.25</td>
-<td>0.75</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>77.75</td>
-<td>27.00</td>
-<td>0.25</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>292.25</td>
-<td>1.00</td>
-<td>13.75</td>
-<td>1.00</td>
-</tr>
-<tr>
-<td>PLENUM-1</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Facility</td>
-<td>333.50</td>
-<td>117.00</td>
-<td>37.25</td>
-<td>56.75</td>
-</tr>
-</table>
-
-### Component Sizing Summary
-
-The Component Sizing Summary report includes details on many of the HVAC components in the simulation. For each of the components, one or more parameters are shown. Directly following is an example of the report. The key used to obtain this report is ComponentSizingSummary.
-
-Report: Component Sizing Summary
-
-For: Entire Facility
-
-Timestamp: 2007-10-17 08:54:27
-
-SINGLE DUCT:VAV:REHEAT
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Maximum air flow rate [m3/s]</th>
-<th>Max Reheat Water Flow [m3/s]</th>
-</tr>
-<tr>
-<td>SPACE1-1 VAV REHEAT</td>
-<td>0.226630</td>
-<td>0.000059</td>
-</tr>
-<tr>
-<td>SPACE2-1 VAV REHEAT</td>
-<td>0.176548</td>
-<td>0.000046</td>
-</tr>
-<tr>
-<td>SPACE3-1 VAV REHEAT</td>
-<td>0.209331</td>
-<td>0.000054</td>
-</tr>
-<tr>
-<td>SPACE4-1 VAV REHEAT</td>
-<td>0.222526</td>
-<td>0.000058</td>
-</tr>
-<tr>
-<td>SPACE5-1 VAV REHEAT</td>
-<td>0.221695</td>
-<td>0.000057</td>
-</tr>
-</table>
-
-
-
- COIL:Water:SimpleHeating
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Max Water Flow Rate of Coil [m3/s]</th>
-<th>Design Coil Load [W]</th>
-<th>UA of the Coil [W/delK]</th>
-</tr>
-<tr>
-<td>SPACE1-1 ZONE COIL</td>
-<td>0.000059</td>
-<td>2698.50</td>
-<td>66.13</td>
-</tr>
-<tr>
-<td>SPACE2-1 ZONE COIL</td>
-<td>0.000046</td>
-<td>2102.17</td>
-<td>51.51</td>
-</tr>
-<tr>
-<td>SPACE3-1 ZONE COIL</td>
-<td>0.000054</td>
-<td>2492.52</td>
-<td>61.08</td>
-</tr>
-<tr>
-<td>SPACE4-1 ZONE COIL</td>
-<td>0.000058</td>
-<td>2649.63</td>
-<td>64.93</td>
-</tr>
-<tr>
-<td>SPACE5-1 ZONE COIL</td>
-<td>0.000057</td>
-<td>2639.74</td>
-<td>64.69</td>
-</tr>
-<tr>
-<td>OA HEATING COIL 1</td>
-<td>0.000148</td>
-<td>6812.27</td>
-<td>84.72</td>
-</tr>
-<tr>
-<td>MAIN HEATING COIL 1</td>
-<td>0.000075</td>
-<td>3458.59</td>
-<td>55.80</td>
-</tr>
-</table>
-
-
-
- BRANCH
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Maximum Branch Flow Rate [m3/s]</th>
-</tr>
-<tr>
-<td>VAV SYS 1 MAIN BRANCH</td>
-<td>1.06</td>
-</tr>
-</table>
-
-
-
- AIR PRIMARY LOOP
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Primary air design volumetric flow rate [m3/s]</th>
-</tr>
-<tr>
-<td>VAV SYS 1</td>
-<td>1.06</td>
-</tr>
-</table>
-
-
-
- CONTROLLER:OUTSIDE AIR
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>maximum outside air flow rate [m3/s]</th>
-<th>minimum outside air flow rate [m3/s]</th>
-</tr>
-<tr>
-<td>OA CONTROLLER 1</td>
-<td>1.06</td>
-<td>0.264118</td>
-</tr>
-</table>
-
-
-
- COIL:Water:Cooling
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Max Water Flow Rate of Coil [m3/s]</th>
-<th>Max Air Flow Rate of Coil [m3/s]</th>
-<th>Design Air Inlet Temperature [C]</th>
-<th>Design Air Outlet Temperature [C]</th>
-<th>Design Water Inlet Temperature [C]</th>
-<th>Design Air Inlet Humidity Ratio</th>
-<th>Design Air Outlet Humidity Ratio</th>
-</tr>
-<tr>
-<td>OA COOLING COIL 1</td>
-<td>0.001145</td>
-<td>0.264118</td>
-<td>30.01</td>
-<td>11.00</td>
-<td>7.00</td>
-<td>0.014595</td>
-<td>0.008000</td>
-</tr>
-<tr>
-<td>MAIN COOLING COIL 1</td>
-<td>0.000916</td>
-<td>1.06</td>
-<td>21.55</td>
-<td>12.80</td>
-<td>7.00</td>
-<td>0.009333</td>
-<td>0.008000</td>
-</tr>
-</table>
-
-
-
- FAN:SIMPLE:VARIABLEVOLUME
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Max Flow Rate [m3/s]</th>
-<th>Min Flow Rate [m3/s]</th>
-</tr>
-<tr>
-<td>SUPPLY FAN 1</td>
-<td>1.06</td>
-<td>0.353263</td>
-</tr>
-</table>
-
-
-
- CONTROLLER:SIMPLE
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Max Actuated Flow [m3/s]</th>
-</tr>
-<tr>
-<td>OA CC CONTROLLER 1</td>
-<td>0.001145</td>
-</tr>
-<tr>
-<td>OA HC CONTROLLER 1</td>
-<td>0.000148</td>
-</tr>
-<tr>
-<td>CENTRAL COOLING COIL CONTROLLER 1</td>
-<td>0.000916</td>
-</tr>
-<tr>
-<td>CENTRAL HEATING COIL CONTROLLER 1</td>
-<td>0.000075</td>
-</tr>
-</table>
-
-
-
- PLANT LOOP
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Maximum Loop Volumetric Flow Rate [m3/s]</th>
-<th>Volume of the plant loop [m3]</th>
-</tr>
-<tr>
-<td>HOT WATER LOOP</td>
-<td>0.000497</td>
-<td>0.559158</td>
-</tr>
-<tr>
-<td>CHILLED WATER LOOP</td>
-<td>0.002061</td>
-<td>2.32</td>
-</tr>
-</table>
-
-
-
- BOILER:SIMPLE
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Nominal Capacity [W]</th>
-<th>Design Boiler Water Flow Rate [m3/s]</th>
-</tr>
-<tr>
-<td>CENTRAL BOILER</td>
-<td>22853.43</td>
-<td>0.000497</td>
-</tr>
-</table>
-
-
-
- CHILLER:ELECTRIC
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Nominal Capacity [W]</th>
-<th>Design Evaporator Volumetric Water Flow Rate [m3/s]</th>
-</tr>
-<tr>
-<td>CENTRAL CHILLER</td>
-<td>34468.25</td>
-<td>0.002061</td>
-</tr>
-</table>
-
-
-
- PUMP:VARIABLE SPEED
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Rated Volumetric Flow Rate [m3/s]</th>
-<th>Rated Power Consumption [W]</th>
-</tr>
-<tr>
-<td>HW CIRC PUMP</td>
-<td>0.000497</td>
-<td>126.98</td>
-</tr>
-<tr>
-<td>CW CIRC PUMP</td>
-<td>0.002061</td>
-<td>526.69</td>
-</tr>
-</table>
-
-### Outdoor Air Summary
-
-The Outdoor Air Summary provides information for each zone on the average and minimum ventilation provided.
-
-The reports described so far in this section are displayed when specified in the Output:Table:Predefined object. They are either on or off and are not customizable. The next few types of tabular reports are customizable. You can specify the report variables being used in each one.
-
-Directly following is an example of the report. The key used to obtain this report is OutdoorAirSummary.
-
-Report: Outdoor Air Summary
-
-For: Entire Facility
-
-Timestamp: 2007-10-17 08:54:27
-
-Average Outside Air During Occupied Hours
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Average Number of Occupants</th>
-<th>Nominal Number of Occupants</th>
-<th>Zone Volume (m3)</th>
-<th>Mechanical Ventilation (ach)</th>
-<th>Infiltration (ach)</th>
-<th>Simple Ventilation (ach)</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>9.50</td>
-<td>11.00</td>
-<td>239.25</td>
-<td>0.365</td>
-<td>0.050</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>4.32</td>
-<td>5.00</td>
-<td>103.31</td>
-<td>0.630</td>
-<td>0.051</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>9.50</td>
-<td>11.00</td>
-<td>239.25</td>
-<td>0.338</td>
-<td>0.050</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>4.32</td>
-<td>5.00</td>
-<td>103.31</td>
-<td>0.708</td>
-<td>0.051</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>17.27</td>
-<td>20.00</td>
-<td>447.68</td>
-<td>0.214</td>
-<td>0.052</td>
-<td>0.000</td>
-</tr>
-</table>
-
-
-
- Minimum Outside Air During Occupied Hours
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Average Number of Occupants</th>
-<th>Nominal Number of Occupants</th>
-<th>Zone Volume (m3)</th>
-<th>Mechanical Ventilation (ach)</th>
-<th>Infiltration (ach)</th>
-<th>Simple Ventilation (ach)</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>9.50</td>
-<td>11.00</td>
-<td>239.25</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>4.32</td>
-<td>5.00</td>
-<td>103.31</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>9.50</td>
-<td>11.00</td>
-<td>239.25</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>4.32</td>
-<td>5.00</td>
-<td>103.31</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>17.27</td>
-<td>20.00</td>
-<td>447.68</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-</tr>
-</table>
-
-### Climatic Data Summary
-
-The Climatic Data Summary provides some statistics from the .STAT file concerning the selected weather. The Stat file must be available (it is included with all the weather files on the EnergyPlus website) for the report to be fully produced. Directly following is an example of the report. The key used to obtain this report is ClimaticDataSummary.
-
-
-
-Report: Climatic Data Summary
-
-For: Entire Facility
-
-Timestamp: 2009-02-10 13:27:45
-
-SizingPeriod:DesignDay
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Maximum Dry Bulb (C)</th>
-<th>Daily Temperature Range (C)</th>
-<th>Humidity Value</th>
-<th>Humidity Type</th>
-<th>Wind Speed (m/s)</th>
-<th>Wind Direction</th>
-</tr>
-<tr>
-<td>CHICAGO_IL_USA ANNUAL HEATING 99% DESIGN CONDITIONS DB</td>
-<td>-17.30</td>
-<td>0.00</td>
-<td>-17.30</td>
-<td>WETBULB</td>
-<td>4.90</td>
-<td>270.00</td>
-</tr>
-<tr>
-<td>CHICAGO_IL_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB</td>
-<td>31.50</td>
-<td>10.70</td>
-<td>23.00</td>
-<td>WETBULB</td>
-<td>5.30</td>
-<td>230.00</td>
-</tr>
-</table>
-
-
-
- Weather Statistics File
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Value</th>
-</tr>
-<tr>
-<td>Reference</td>
-<td>USA_Chicago-OHare_TMY2</td>
-</tr>
-<tr>
-<td>Site:Location</td>
-<td>Chicago IL USA</td>
-</tr>
-<tr>
-<td>Latitude</td>
-<td>N 41° 58'</td>
-</tr>
-<tr>
-<td>Longitude</td>
-<td>W 87° 54'</td>
-</tr>
-<tr>
-<td>Time Zone</td>
-<td>GMT -6.0 Hours</td>
-</tr>
-<tr>
-<td>Elevation</td>
-<td>190m above sea level</td>
-</tr>
-<tr>
-<td>Standard Pressure at Elevation</td>
-<td>99063Pa</td>
-</tr>
-<tr>
-<td>Data Source</td>
-<td>Release Test</td>
-</tr>
-<tr>
-<td>WMO Station</td>
-<td>725300</td>
-</tr>
-<tr>
-<td>Design Conditions</td>
-<td>Climate Design Data 2005 ASHRAE Handbook</td>
-</tr>
-<tr>
-<td>Heating Design Temperature 99.6% (C)</td>
-<td>-20.6</td>
-</tr>
-<tr>
-<td>Heating Design Temperature 99% (C)</td>
-<td>-17.3</td>
-</tr>
-<tr>
-<td>Cooling Design Temperature 0.4% (C)</td>
-<td>33.2</td>
-</tr>
-<tr>
-<td>Cooling Design Temperature 1% (C)</td>
-<td>31.5</td>
-</tr>
-<tr>
-<td>Cooling Design Temperature 2% (C)</td>
-<td>29.9</td>
-</tr>
-<tr>
-<td>Maximum Dry Bulb Temperature (C)</td>
-<td>35.6°</td>
-</tr>
-<tr>
-<td>Maximum Dry Bulb Occurs on</td>
-<td>Jul 9</td>
-</tr>
-<tr>
-<td>Minimum Dry Bulb Temperature (C)</td>
-<td>-22.8°</td>
-</tr>
-<tr>
-<td>Minimum Dry Bulb Occurs on</td>
-<td>Jan 7</td>
-</tr>
-<tr>
-<td>Maximum Dew Point Temperature (C)</td>
-<td>25.6</td>
-</tr>
-<tr>
-<td>Maximum Dew Point Occurs on</td>
-<td>Aug 4</td>
-</tr>
-<tr>
-<td>Minimum Dew Point Temperature (C)</td>
-<td>-28.9</td>
-</tr>
-<tr>
-<td>Minimum Dew Point Occurs on</td>
-<td>Dec 31</td>
-</tr>
-<tr>
-<td>Heating Degree-Days (base 10°C)</td>
-<td>1745</td>
-</tr>
-<tr>
-<td>Cooling Degree-Days (base 18°C)</td>
-<td>464</td>
-</tr>
-<tr>
-<td>Köppen Classification</td>
-<td>Dfa</td>
-</tr>
-<tr>
-<td>Köppen Description</td>
-<td>Humid continental (hot summer, cold winter, no dry season, lat. 30-60°N)</td>
-</tr>
-<tr>
-<td>Köppen Recommendation</td>
-<td>Unbearably humid periods in summer, but passive cooling is possible</td>
-</tr>
-<tr>
-<td>ASHRAE Climate Zone</td>
-<td>5A</td>
-</tr>
-<tr>
-<td>ASHRAE Description</td>
-<td>Cool-Humid</td>
-</tr>
-</table>
-
-
-
-### Object Count Summary
-
-The object count summary report provides the count on the number of specific objects in the file. Directly following is an example of the report. The key used to obtain this report is ObjectCountSummary.
-
-Report: Object Count Summary
-
-For: Entire Facility
-
-Timestamp: 2009-02-10 12:39:35
-
-Surfaces by Class
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Total</th>
-<th>Outdoors</th>
-</tr>
-<tr>
-<td>Wall</td>
-<td>24</td>
-<td>8</td>
-</tr>
-<tr>
-<td>Floor</td>
-<td>10</td>
-<td>5</td>
-</tr>
-<tr>
-<td>Roof</td>
-<td>6</td>
-<td>1</td>
-</tr>
-<tr>
-<td>Internal Mass</td>
-<td>0</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Building Detached Shading</td>
-<td>0</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Fixed Detached Shading</td>
-<td>0</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Window</td>
-<td>6</td>
-<td>6</td>
-</tr>
-<tr>
-<td>Door</td>
-<td>0</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Glass Door</td>
-<td>0</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Shading</td>
-<td>4</td>
-<td>4</td>
-</tr>
-<tr>
-<td>Overhang</td>
-<td>0</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Fin</td>
-<td>0</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Tubular Daylighting Device Dome</td>
-<td>0</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Tubular Daylighting Device Diffuser</td>
-<td>0</td>
-<td>0</td>
-</tr>
-</table>
-
-
-
-
-
-
-
-
-
-
-
-
-
-HVAC
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Count</th>
-</tr>
-<tr>
-<td>HVAC Air Loops</td>
-<td>1</td>
-</tr>
-<tr>
-<td>Conditioned Zones</td>
-<td>6</td>
-</tr>
-<tr>
-<td>Unconditioned Zones</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Supply Plenums</td>
-<td>0</td>
-</tr>
-<tr>
-<td>Return Plenums</td>
-<td>1</td>
-</tr>
-</table>
-
-
-
-### Component Cost Economics Summary
-
-The Component Cost Economics Summary provides the construction cost estimate summary for the project. The costs are broken into eight catagories and the reference building costs are provided as a comparison. A second table is also produced that provides line item details with one line for every line item object. Directly following is an example of this report.
-
-Report: Component Cost Economics Summary
-
-For: Entire Facility
-
-Timestamp: 2016-01-12 15:47:39
-
-Construction Cost Estimate Summary
-
-<table class="table table-striped">
-  <tr>
-    <th></th>
-    <th>Reference Bldg.</th>
-    <th>Current Bldg. Model</th>
-    <th>Difference</th>
-  </tr>
-  <tr>
-    <td>Line Item SubTotal ($)</td>
-    <td>665082.04</td>
-    <td>719946.72</td>
-    <td>54864.68</td>
-  </tr>
-  <tr>
-    <td>Misc. Costs ($)</td>
-    <td>928979.09</td>
-    <td>928979.09</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>Regional Adjustment ($)</td>
-    <td>216792.31</td>
-    <td>224253.91</td>
-    <td>7461.6</td>
-  </tr>
-  <tr>
-    <td>Design Fee ($)</td>
-    <td>108651.21</td>
-    <td>149854.38</td>
-    <td>41203.17</td>
-  </tr>
-  <tr>
-    <td>Contractor Fee ($)</td>
-    <td>126759.74</td>
-    <td>131122.58</td>
-    <td>4362.84</td>
-  </tr>
-  <tr>
-    <td>Contingency ($)</td>
-    <td>181085.34</td>
-    <td>187317.97</td>
-    <td>6232.63</td>
-  </tr>
-  <tr>
-    <td>Permits, Bonds, Insurance ($)</td>
-    <td>0</td>
-    <td>0</td>
-    <td>0</td>
-  </tr>
-  <tr>
-    <td>Commissioning ($)</td>
-    <td>9054.27</td>
-    <td>18731.8</td>
-    <td>9677.53</td>
-  </tr>
-  <tr>
-    <td>Cost Estimate Total ($)</td>
-    <td>2236404</td>
-    <td>2360206.45</td>
-    <td>123802.44</td>
-  </tr>
-  <tr>
-    <td>Cost Per Conditioned Building Area ($/m2)</td>
-    <td>1203.69</td>
-    <td>1270.32</td>
-    <td>66.63</td>
-  </tr>
-</table>
-
-
-
-Cost Line Item Details
-
-<table class="table table-striped">
-  <tr>
-    <th></th>
-    <th>Line No.</th>
-    <th>Item Name</th>
-    <th>Quantity.</th>
-    <th>Units</th>
-    <th>$ per Qty.</th>
-    <th>SubTotal $</th>
-  </tr>
-  <tr>
-    <td>--</td>
-    <td>1</td>
-    <td>EXTERIOR WALLS</td>
-    <td>627.57</td>
-    <td>m2</td>
-    <td>168.64</td>
-    <td>105832.65</td>
-  </tr>
-  <tr>
-    <td>--</td>
-    <td>2</td>
-    <td>INTERIOR WALLS</td>
-    <td>854.18</td>
-    <td>m2</td>
-    <td>31.16</td>
-    <td>26616.23</td>
-  </tr>
-  <tr>
-    <td>--</td>
-    <td>3</td>
-    <td>ROOF</td>
-    <td>1857.96</td>
-    <td>m2</td>
-    <td>104.69</td>
-    <td>194509.64</td>
-  </tr>
-  <tr>
-    <td>--</td>
-    <td>4</td>
-    <td>GROUND FLR SLAB</td>
-    <td>1857.96</td>
-    <td>m2</td>
-    <td>56.06</td>
-    <td>104157.14</td>
-  </tr>
-  <tr>
-    <td>--</td>
-    <td>5</td>
-    <td>ACOUSTICAL DROP CEILINGS</td>
-    <td>1857.96</td>
-    <td>m2</td>
-    <td>23.79</td>
-    <td>44200.83</td>
-  </tr>
-  <tr>
-    <td>--</td>
-    <td>6</td>
-    <td>QUAD HIGH SHGC SUPERWINDOWS</td>
-    <td>226.22</td>
-    <td>m2</td>
-    <td>687.84</td>
-    <td>155604.96</td>
-  </tr>
-  <tr>
-    <td>--</td>
-    <td>7</td>
-    <td>QUAD LOW SHGC SUPERWINDOWS</td>
-    <td>42.68</td>
-    <td>m2</td>
-    <td>687.84</td>
-    <td>29359.55</td>
-  </tr>
-  <tr>
-    <td>--</td>
-    <td>8</td>
-    <td>CENTRAL CHILLER</td>
-    <td>150.49</td>
-    <td>kW (tot cool cap.)</td>
-    <td>340</td>
-    <td>51165.73</td>
-  </tr>
-  <tr>
-    <td>--</td>
-    <td>9</td>
-    <td>CONTINUOUS AIR BARRIER</td>
-    <td>1</td>
-    <td>Ea.</td>
-    <td>8500</td>
-    <td>8500</td>
-  </tr>
-  <tr>
-    <td>Line Item SubTotal</td>
-    <td>--</td>
-    <td>--</td>
-    <td>--</td>
-    <td>--</td>
-    <td>--</td>
-    <td>719946.72</td>
-  </tr>
-</table>
-
-
-
-###LEED Summary
-
-The LEED Summary report provides many of the simulation results required for certification of Energy and Atmosphere Credit 1 Optimized Energy Performance according to the LEED Green Building Rating Systemâ„¢. The report can be produced by specifying LEEDSummary in Output:Table:SummaryReports which is also part of the AllSummary option. Directly following is an example of this report.
-
-Report: LEED Summary
-
-For: Entire Facility
-
-Timestamp: 2013-03-01 15:24:37
-
-Sec1.1A-General Information
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Data</th>
-</tr>
-<tr>
-<td>Heating Degree Days</td>
-<td>1748</td>
-</tr>
-<tr>
-<td>Cooling Degree Days</td>
-<td>506</td>
-</tr>
-<tr>
-<td>Climate Zone</td>
-<td>5A</td>
-</tr>
-<tr>
-<td>Weather File</td>
-<td>Chicago Ohare Intl Ap IL USA TMY3 WMO#=725300</td>
-</tr>
-<tr>
-<td>HDD and CDD data source</td>
-<td>Weather File Stat</td>
-</tr>
-<tr>
-<td>Total gross floor area [m2]</td>
-<td>927.20</td>
-</tr>
-<tr>
-<td>Principal Heating Source</td>
-<td>Natural Gas</td>
-</tr>
-</table>
-
-
-
- EAp2-1. Space Usage Type
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Space Area [m2]</th>
-<th>Regularly Occupied Area [m2]</th>
-<th>Unconditioned Area [m2]</th>
-<th>Typical Hours/Week in Operation [hr/wk]</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>99.16</td>
-<td>99.16</td>
-<td>0.00</td>
-<td>55.06</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>42.73</td>
-<td>42.73</td>
-<td>0.00</td>
-<td>55.06</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>96.48</td>
-<td>96.48</td>
-<td>0.00</td>
-<td>55.06</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>42.73</td>
-<td>42.73</td>
-<td>0.00</td>
-<td>55.06</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>182.49</td>
-<td>182.49</td>
-<td>0.00</td>
-<td>55.06</td>
-</tr>
-<tr>
-<td>PLENUM-1</td>
-<td>463.60</td>
-<td>463.60</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Totals</td>
-<td>927.20</td>
-<td>927.20</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-</table>
-
-
-
- EAp2-2. Advisory Messages
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Data</th>
-</tr>
-<tr>
-<td>Number of hours heating loads not met</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Number of hours cooling loads not met</td>
-<td>10.75</td>
-</tr>
-<tr>
-<td>Number of hours not met</td>
-<td>10.75</td>
-</tr>
-</table>
-
-
-
- EAp2-3. Energy Type Summary
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Utility Rate</th>
-<th>Virtual Rate [$/unit energy]</th>
-<th>Units of Energy</th>
-<th>Units of Demand</th>
-</tr>
-<tr>
-<td>Electricity</td>
-<td>EXAMPLEA EXAMPLEI-SELL</td>
-<td>0.055</td>
-<td>kWh</td>
-<td>kW</td>
-</tr>
-<tr>
-<td>Natural Gas</td>
-<td>EXAMPLEA-GAS</td>
-<td>0.569</td>
-<td>Therm</td>
-<td>Therm/Hr</td>
-</tr>
-<tr>
-<td>Other</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- EAp2-4/5. Performance Rating Method Compliance
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Electric Energy Use [GJ]</th>
-<th>Electric Demand [W]</th>
-<th>Natural Gas Energy Use [GJ]</th>
-<th>Natural Gas Demand [W]</th>
-<th>Other Energy Use [GJ]</th>
-<th>Other Demand [W]</th>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>81.24</td>
-<td>7125.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Space Heating</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>103.92</td>
-<td>62499.99</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Space Cooling</td>
-<td>17.63</td>
-<td>9523.66</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>1.54</td>
-<td>319.57</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans-Interior</td>
-<td>7.01</td>
-<td>609.44</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans-Parking Garage</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Service Water Heating</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Receptacle Equipment</td>
-<td>47.70</td>
-<td>4500.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting (process)</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooking</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Industrial Process</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Elevators and Escalators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total Line</td>
-<td>155.12</td>
-<td> </td>
-<td>274.01</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-</tr>
-</table>
-
-
-
- EAp2-6. Energy Use Summary
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Process Subtotal [GJ]</th>
-<th>Total Energy Use [GJ]</th>
-</tr>
-<tr>
-<td>Electricity</td>
-<td>47.70</td>
-<td>155.12</td>
-</tr>
-<tr>
-<td>Natural Gas</td>
-<td>0.00</td>
-<td>274.01</td>
-</tr>
-<tr>
-<td>Other</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>47.70</td>
-<td>429.13</td>
-</tr>
-</table>
-
-
-
- EAp2-7. Energy Cost Summary
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Process Subtotal [$]</th>
-<th>Total Energy Cost [$]</th>
-</tr>
-<tr>
-<td>Electricity</td>
-<td>552.55</td>
-<td>1796.99</td>
-</tr>
-<tr>
-<td>Natural Gas</td>
-<td>0.00</td>
-<td>1478.58</td>
-</tr>
-<tr>
-<td>Other</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>552.55</td>
-<td>3275.57</td>
-</tr>
-</table>
-
-Process energy cost based on ratio of process to total energy.
-
- L-1. Renewable Energy Source Summary
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Rated Capacity [kW]</th>
-<th>Annual Energy Generated [GJ]</th>
-</tr>
-<tr>
-<td>Photovoltaic</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Wind</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
- EAp2-17a. Energy Use Intensity - Electricity
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Electricty [MJ/m2]</th>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>87.62</td>
-</tr>
-<tr>
-<td>Space Heating</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Space Cooling</td>
-<td>19.02</td>
-</tr>
-<tr>
-<td>Fans-Interior</td>
-<td>7.56</td>
-</tr>
-<tr>
-<td>Service Water Heating</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Receptacle Equipment</td>
-<td>51.44</td>
-</tr>
-<tr>
-<td>Miscellaneous</td>
-<td>1.66</td>
-</tr>
-<tr>
-<td>Subtotal</td>
-<td>167.30</td>
-</tr>
-</table>
-
-
-
- EAp2-17b. Energy Use Intensity - Natural Gas
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Natural Gas [MJ/m2]</th>
-</tr>
-<tr>
-<td>Space Heating</td>
-<td>112.08</td>
-</tr>
-<tr>
-<td>Service Water Heating</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Miscellaneous</td>
-<td>183.45</td>
-</tr>
-<tr>
-<td>Subtotal</td>
-<td>295.53</td>
-</tr>
-</table>
-
-
-
- EAp2-17c. Energy Use Intensity - Other
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Other [MJ/m2]</th>
-</tr>
-<tr>
-<td>Miscellaneous</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Subtotal</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
- EAp2-18. End Use Percentage
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Percent [%]</th>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>18.93</td>
-</tr>
-<tr>
-<td>Space Heating</td>
-<td>24.22</td>
-</tr>
-<tr>
-<td>Space Cooling</td>
-<td>4.11</td>
-</tr>
-<tr>
-<td>Fans-Interior</td>
-<td>1.63</td>
-</tr>
-<tr>
-<td>Service Water Heating</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Receptacle Equipment</td>
-<td>11.11</td>
-</tr>
-<tr>
-<td>Miscellaneous</td>
-<td>39.99</td>
-</tr>
-</table>
-
-
-
-### Energy Meters
-
-This report provides the details on all the energy meters generated by the simulation. Directly following is an example of the report. The key used to obtain this report is EnergyMeters.
-
-Report: Energy Meters
-
-For: Entire Facility
-
-Timestamp: 2012-05-01 17:07:24
-
-Annual and Peak Values - Electricity
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Electricity Annual Value [GJ]</th>
-<th>Electricity Minimum Value [W]</th>
-<th>Timestamp of Minimum</th>
-<th>Electricity Maximum Value [W]</th>
-<th>Timestamp of Maximum</th>
-</tr>
-<tr>
-<td>Electricity:Facility</td>
-<td>156.68</td>
-<td>475.00</td>
-<td>01-APR-00:15</td>
-<td>20165.58</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>Electricity:Building</td>
-<td>128.94</td>
-<td>475.00</td>
-<td>01-JAN-00:15</td>
-<td>12000.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>Electricity:Zone:SPACE1-1</td>
-<td>27.23</td>
-<td>100.32</td>
-<td>01-JAN-00:15</td>
-<td>2534.40</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>InteriorLights:Electricity</td>
-<td>81.24</td>
-<td>375.00</td>
-<td>01-JAN-00:15</td>
-<td>7500.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>InteriorLights:Electricity:Zone:SPACE1-1</td>
-<td>17.16</td>
-<td>79.20</td>
-<td>01-JAN-00:15</td>
-<td>1584.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>GeneralLights:InteriorLights:Electricity</td>
-<td>81.24</td>
-<td>375.00</td>
-<td>01-JAN-00:15</td>
-<td>7500.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>Electricity:Zone:SPACE2-1</td>
-<td>11.76</td>
-<td>43.32</td>
-<td>01-JAN-00:15</td>
-<td>1094.40</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>InteriorLights:Electricity:Zone:SPACE2-1</td>
-<td>7.41</td>
-<td>34.20</td>
-<td>01-JAN-00:15</td>
-<td>684.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>Electricity:Zone:SPACE3-1</td>
-<td>27.23</td>
-<td>100.32</td>
-<td>01-JAN-00:15</td>
-<td>2534.40</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>InteriorLights:Electricity:Zone:SPACE3-1</td>
-<td>17.16</td>
-<td>79.20</td>
-<td>01-JAN-00:15</td>
-<td>1584.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>Electricity:Zone:SPACE4-1</td>
-<td>11.76</td>
-<td>43.32</td>
-<td>01-JAN-00:15</td>
-<td>1094.40</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>InteriorLights:Electricity:Zone:SPACE4-1</td>
-<td>7.41</td>
-<td>34.20</td>
-<td>01-JAN-00:15</td>
-<td>684.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>Electricity:Zone:SPACE5-1</td>
-<td>50.96</td>
-<td>187.72</td>
-<td>01-JAN-00:15</td>
-<td>4742.40</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>InteriorLights:Electricity:Zone:SPACE5-1</td>
-<td>32.11</td>
-<td>148.20</td>
-<td>01-JAN-00:15</td>
-<td>2964.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>InteriorEquipment:Electricity</td>
-<td>47.70</td>
-<td>100.00</td>
-<td>01-JAN-00:15</td>
-<td>4500.00</td>
-<td>01-JAN-09:15</td>
-</tr>
-<tr>
-<td>InteriorEquipment:Electricity:Zone:SPACE1-1</td>
-<td>10.07</td>
-<td>21.12</td>
-<td>01-JAN-00:15</td>
-<td>950.40</td>
-<td>01-JAN-09:15</td>
-</tr>
-<tr>
-<td>General:InteriorEquipment:Electricity</td>
-<td>47.70</td>
-<td>100.00</td>
-<td>01-JAN-00:15</td>
-<td>4500.00</td>
-<td>01-JAN-09:15</td>
-</tr>
-<tr>
-<td>InteriorEquipment:Electricity:Zone:SPACE2-1</td>
-<td>4.35</td>
-<td>9.12</td>
-<td>01-JAN-00:15</td>
-<td>410.40</td>
-<td>01-JAN-09:15</td>
-</tr>
-<tr>
-<td>InteriorEquipment:Electricity:Zone:SPACE3-1</td>
-<td>10.07</td>
-<td>21.12</td>
-<td>01-JAN-00:15</td>
-<td>950.40</td>
-<td>01-JAN-09:15</td>
-</tr>
-<tr>
-<td>InteriorEquipment:Electricity:Zone:SPACE4-1</td>
-<td>4.35</td>
-<td>9.12</td>
-<td>01-JAN-00:15</td>
-<td>410.40</td>
-<td>01-JAN-09:15</td>
-</tr>
-<tr>
-<td>InteriorEquipment:Electricity:Zone:SPACE5-1</td>
-<td>18.85</td>
-<td>39.52</td>
-<td>01-JAN-00:15</td>
-<td>1778.40</td>
-<td>01-JAN-09:15</td>
-</tr>
-<tr>
-<td>ElectricityPurchased:Facility</td>
-<td>156.68</td>
-<td>475.00</td>
-<td>28-JUN-05:15</td>
-<td>20165.58</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>ElectricityPurchased:Plant</td>
-<td>156.68</td>
-<td>475.00</td>
-<td>28-JUN-05:15</td>
-<td>20165.58</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>Cogeneration:ElectricityPurchased</td>
-<td>156.68</td>
-<td>475.00</td>
-<td>28-JUN-05:15</td>
-<td>20165.58</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>ElectricitySurplusSold:Facility</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-</tr>
-<tr>
-<td>ElectricitySurplusSold:Plant</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-</tr>
-<tr>
-<td>Cogeneration:ElectricitySurplusSold</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-</tr>
-<tr>
-<td>ElectricityNet:Facility</td>
-<td>156.68</td>
-<td>475.00</td>
-<td>28-JUN-05:15</td>
-<td>20165.58</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>ElectricityNet:Plant</td>
-<td>156.68</td>
-<td>475.00</td>
-<td>28-JUN-05:15</td>
-<td>20165.58</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>Cogeneration:ElectricityNet</td>
-<td>156.68</td>
-<td>475.00</td>
-<td>28-JUN-05:15</td>
-<td>20165.58</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>Electricity:HVAC</td>
-<td>8.87</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>655.43</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>Fans:Electricity</td>
-<td>8.87</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>655.43</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>General:Fans:Electricity</td>
-<td>8.87</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>655.43</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>Electricity:Plant</td>
-<td>18.88</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>8053.88</td>
-<td>19-JUL-16:00</td>
-</tr>
-<tr>
-<td>Heating:Electricity</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-</tr>
-<tr>
-<td>Boiler Parasitic:Heating:Electricity</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-</tr>
-<tr>
-<td>Cooling:Electricity</td>
-<td>16.44</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>7478.31</td>
-<td>19-JUL-16:00</td>
-</tr>
-<tr>
-<td>Pumps:Electricity</td>
-<td>2.44</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>575.73</td>
-<td>24-JUL-20:00</td>
-</tr>
-<tr>
-<td>MYGENERALLIGHTS</td>
-<td>81.24</td>
-<td>375.00</td>
-<td>01-JAN-00:15</td>
-<td>7500.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>MYBUILDINGELECTRIC</td>
-<td>128.94</td>
-<td>475.00</td>
-<td>01-JAN-00:15</td>
-<td>12000.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-<tr>
-<td>MYBUILDINGOTHER</td>
-<td>47.70</td>
-<td>375.00</td>
-<td>01-JAN-00:15</td>
-<td>7500.00</td>
-<td>01-JAN-10:15</td>
-</tr>
-</table>
-
-
-
- Annual and Peak Values - Gas
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Gas Annual Value [GJ]</th>
-<th>Gas Minimum Value [W]</th>
-<th>Timestamp of Minimum</th>
-<th>Gas Maximum Value [W]</th>
-<th>Timestamp of Maximum</th>
-</tr>
-<tr>
-<td>Gas:Facility</td>
-<td>68.82</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>42092.68</td>
-<td>01-FEB-06:15</td>
-</tr>
-<tr>
-<td>Gas:Plant</td>
-<td>68.82</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>42092.68</td>
-<td>01-FEB-06:15</td>
-</tr>
-<tr>
-<td>Heating:Gas</td>
-<td>68.82</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>42092.68</td>
-<td>01-FEB-06:15</td>
-</tr>
-<tr>
-<td>Boiler:Heating:Gas</td>
-<td>68.82</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>42092.68</td>
-<td>01-FEB-06:15</td>
-</tr>
-</table>
-
-
-
- Annual and Peak Values - Cooling
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Cooling Annual Value [GJ]</th>
-<th>Cooling Minimum Value [W]</th>
-<th>Timestamp of Minimum</th>
-<th>Cooling Maximum Value [W]</th>
-<th>Timestamp of Maximum</th>
-</tr>
-<tr>
-<td>PlantLoopCoolingDemand:Facility</td>
-<td>62.41</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>27050.46</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>PlantLoopCoolingDemand:HVAC</td>
-<td>62.41</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>27050.46</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>CoolingCoils:PlantLoopCoolingDemand</td>
-<td>62.41</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>27050.46</td>
-<td>17-JUL-15:00</td>
-</tr>
-</table>
-
-
-
- Annual and Peak Values - Water
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Annual Value [m3]</th>
-<th>Minimum Value [m3/s]</th>
-<th>Timestamp of Minimum</th>
-<th>Maximum Value [m3/s]</th>
-<th>Timestamp of Maximum</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Annual and Peak Values - Other by Weight/Mass
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Annual Value [kg]</th>
-<th>Minimum Value [kg/s]</th>
-<th>Timestamp of Minimum</th>
-<th>Maximum Value [kg/s]</th>
-<th>Timestamp of Maximum</th>
-</tr>
-<tr>
-<td>Carbon Equivalent:Facility</td>
-<td>0.00</td>
-<td>0.000</td>
-<td>01-JAN-00:15</td>
-<td>0.000</td>
-<td>01-JAN-00:15</td>
-</tr>
-<tr>
-<td>CarbonEquivalentEmissions:Carbon Equivalent</td>
-<td>0.00</td>
-<td>0.000</td>
-<td>01-JAN-00:15</td>
-<td>0.000</td>
-<td>01-JAN-00:15</td>
-</tr>
-</table>
-
-
-
- Annual and Peak Values - Other Volumetric
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Annual Value [m3]</th>
-<th>Minimum Value [m3/s]</th>
-<th>Timestamp of Minimum</th>
-<th>Maximum Value [m3/s]</th>
-<th>Timestamp of Maximum</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Annual and Peak Values - Other Liquid/Gas
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Annual Value [L]</th>
-<th>Minimum Value [L]</th>
-<th>Timestamp of Minimum</th>
-<th>Maximum Value [L]</th>
-<th>Timestamp of Maximum</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Annual and Peak Values - Other
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Annual Value [GJ]</th>
-<th>Minimum Value [W]</th>
-<th>Timestamp of Minimum</th>
-<th>Maximum Value [W]</th>
-<th>Timestamp of Maximum</th>
-</tr>
-<tr>
-<td>EnergyTransfer:Facility</td>
-<td>415.65</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>102784.74</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>EnergyTransfer:Building</td>
-<td>97.60</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>21488.05</td>
-<td>28-JAN-06:15</td>
-</tr>
-<tr>
-<td>EnergyTransfer:Zone:PLENUM-1</td>
-<td>22.50</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>4218.21</td>
-<td>07-JAN-08:15</td>
-</tr>
-<tr>
-<td>Heating:EnergyTransfer</td>
-<td>42.23</td>
-<td>0.00</td>
-<td>19-MAR-15:30</td>
-<td>21488.05</td>
-<td>28-JAN-06:15</td>
-</tr>
-<tr>
-<td>Heating:EnergyTransfer:Zone:PLENUM-1</td>
-<td>19.63</td>
-<td>0.00</td>
-<td>16-JAN-21:15</td>
-<td>4218.21</td>
-<td>07-JAN-08:15</td>
-</tr>
-<tr>
-<td>Cooling:EnergyTransfer</td>
-<td>55.38</td>
-<td>0.00</td>
-<td>01-JAN-06:15</td>
-<td>13937.19</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>Cooling:EnergyTransfer:Zone:PLENUM-1</td>
-<td>2.87</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>2539.33</td>
-<td>18-JUL-15:00</td>
-</tr>
-<tr>
-<td>EnergyTransfer:Zone:SPACE1-1</td>
-<td>17.91</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>4012.66</td>
-<td>30-DEC-06:15</td>
-</tr>
-<tr>
-<td>Heating:EnergyTransfer:Zone:SPACE1-1</td>
-<td>6.51</td>
-<td>0.00</td>
-<td>01-JAN-10:15</td>
-<td>4012.66</td>
-<td>30-DEC-06:15</td>
-</tr>
-<tr>
-<td>Cooling:EnergyTransfer:Zone:SPACE1-1</td>
-<td>11.40</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>3138.67</td>
-<td>27-SEP-16:00</td>
-</tr>
-<tr>
-<td>EnergyTransfer:Zone:SPACE2-1</td>
-<td>10.67</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>3432.93</td>
-<td>30-DEC-06:15</td>
-</tr>
-<tr>
-<td>Heating:EnergyTransfer:Zone:SPACE2-1</td>
-<td>2.42</td>
-<td>0.00</td>
-<td>01-JAN-01:30</td>
-<td>3432.93</td>
-<td>30-DEC-06:15</td>
-</tr>
-<tr>
-<td>Cooling:EnergyTransfer:Zone:SPACE2-1</td>
-<td>8.25</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>2460.04</td>
-<td>06-SEP-10:15</td>
-</tr>
-<tr>
-<td>EnergyTransfer:Zone:SPACE3-1</td>
-<td>16.79</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>3788.83</td>
-<td>30-DEC-06:15</td>
-</tr>
-<tr>
-<td>Heating:EnergyTransfer:Zone:SPACE3-1</td>
-<td>6.09</td>
-<td>0.00</td>
-<td>01-JAN-12:00</td>
-<td>3788.83</td>
-<td>30-DEC-06:15</td>
-</tr>
-<tr>
-<td>Cooling:EnergyTransfer:Zone:SPACE3-1</td>
-<td>10.70</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>2807.57</td>
-<td>19-JUL-11:00</td>
-</tr>
-<tr>
-<td>EnergyTransfer:Zone:SPACE4-1</td>
-<td>9.82</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>3746.68</td>
-<td>28-JAN-06:15</td>
-</tr>
-<tr>
-<td>Heating:EnergyTransfer:Zone:SPACE4-1</td>
-<td>2.98</td>
-<td>0.00</td>
-<td>01-JAN-01:30</td>
-<td>3746.68</td>
-<td>28-JAN-06:15</td>
-</tr>
-<tr>
-<td>Cooling:EnergyTransfer:Zone:SPACE4-1</td>
-<td>6.85</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>2281.99</td>
-<td>25-JUN-17:15</td>
-</tr>
-<tr>
-<td>EnergyTransfer:Zone:SPACE5-1</td>
-<td>19.91</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>4037.31</td>
-<td>30-DEC-06:15</td>
-</tr>
-<tr>
-<td>Heating:EnergyTransfer:Zone:SPACE5-1</td>
-<td>4.60</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>4037.31</td>
-<td>30-DEC-06:15</td>
-</tr>
-<tr>
-<td>Cooling:EnergyTransfer:Zone:SPACE5-1</td>
-<td>15.31</td>
-<td>0.00</td>
-<td>01-JAN-06:15</td>
-<td>2611.53</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>EnergyTransfer:HVAC</td>
-<td>117.82</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>31769.77</td>
-<td>07-JAN-06:15</td>
-</tr>
-<tr>
-<td>HeatingCoils:EnergyTransfer</td>
-<td>55.41</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>31769.77</td>
-<td>07-JAN-06:15</td>
-</tr>
-<tr>
-<td>PlantLoopHeatingDemand:Facility</td>
-<td>55.41</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>31769.77</td>
-<td>07-JAN-06:15</td>
-</tr>
-<tr>
-<td>PlantLoopHeatingDemand:HVAC</td>
-<td>55.41</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>31769.77</td>
-<td>07-JAN-06:15</td>
-</tr>
-<tr>
-<td>HeatingCoils:PlantLoopHeatingDemand</td>
-<td>55.41</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>31769.77</td>
-<td>07-JAN-06:15</td>
-</tr>
-<tr>
-<td>CoolingCoils:EnergyTransfer</td>
-<td>62.41</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>27050.46</td>
-<td>17-JUL-15:00</td>
-</tr>
-<tr>
-<td>EnergyTransfer:Plant</td>
-<td>200.23</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>62116.41</td>
-<td>19-JUL-16:00</td>
-</tr>
-<tr>
-<td>Boilers:EnergyTransfer</td>
-<td>55.06</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>33674.15</td>
-<td>28-MAR-06:15</td>
-</tr>
-<tr>
-<td>Chillers:EnergyTransfer</td>
-<td>64.37</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>27319.05</td>
-<td>19-JUL-16:00</td>
-</tr>
-<tr>
-<td>HeatRejection:EnergyTransfer</td>
-<td>80.81</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>34797.36</td>
-<td>19-JUL-16:00</td>
-</tr>
-</table>
-
-### Sensible Heat Gain Summary
-
-This report is more fully described in the Input Output Reference but represents the major heat gain components for each zone as well as the HVAC loads satisfied. Directly following is an example of the report. The key used to obtain this report is SensibleHeatGainSummary.
-
-
-
-Report: Sensible Heat Gain Summary
-
-For: Entire Facility
-
-Timestamp: 2011-09-09 08:02:03
-
-Annual Building Sensible Heat Gain Components
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>HVAC Input Sensible Air Heating [GJ]</th>
-<th>HVAC Input Sensible Air Cooling [GJ]</th>
-<th>HVAC Input Heated Surface Heating [GJ]</th>
-<th>HVAC Input Cooled Surface Cooling [GJ]</th>
-<th>People Sensible Heat Addition [GJ]</th>
-<th>Lights Sensible Heat Addition [GJ]</th>
-<th>Equipment Sensible Heat Addition [GJ]</th>
-<th>Window Heat Addition [GJ]</th>
-<th>Interzone Air Transfer Heat Addition [GJ]</th>
-<th>Infiltration Heat Addition [GJ]</th>
-<th>Opaque Surface Conduction and Other Heat Addition [GJ]</th>
-<th>Equipment Sensible Heat Removal [GJ]</th>
-<th>Window Heat Removal [GJ]</th>
-<th>Interzone Air Transfer Heat Removal [GJ]</th>
-<th>Infiltration Heat Removal [GJ]</th>
-<th>Opaque Surface Conduction and Other Heat Removal [GJ]</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>0.096</td>
-<td>-0.070</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.035</td>
-<td>0.131</td>
-<td>0.065</td>
-<td>0.220</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.001</td>
-<td>0.000</td>
-<td>-0.078</td>
-<td>0.000</td>
-<td>-0.004</td>
-<td>-0.395</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>0.051</td>
-<td>-0.038</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.014</td>
-<td>0.056</td>
-<td>0.028</td>
-<td>0.173</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.001</td>
-<td>0.000</td>
-<td>-0.029</td>
-<td>0.000</td>
-<td>-0.002</td>
-<td>-0.253</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>0.093</td>
-<td>-0.030</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.034</td>
-<td>0.131</td>
-<td>0.065</td>
-<td>0.157</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>-0.082</td>
-<td>0.000</td>
-<td>-0.004</td>
-<td>-0.363</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>0.055</td>
-<td>-0.015</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.015</td>
-<td>0.056</td>
-<td>0.028</td>
-<td>0.105</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>-0.032</td>
-<td>0.000</td>
-<td>-0.002</td>
-<td>-0.211</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>0.032</td>
-<td>-0.072</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.073</td>
-<td>0.244</td>
-<td>0.121</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>-0.007</td>
-<td>-0.392</td>
-</tr>
-<tr>
-<td>PLENUM-1</td>
-<td>0.118</td>
-<td>-0.024</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>-0.094</td>
-</tr>
-<tr>
-<td>Total Facility</td>
-<td>0.445</td>
-<td>-0.248</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.170</td>
-<td>0.618</td>
-<td>0.307</td>
-<td>0.655</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.002</td>
-<td>0.000</td>
-<td>-0.221</td>
-<td>0.000</td>
-<td>-0.017</td>
-<td>-1.709</td>
-</tr>
-</table>
-
-
-
- Peak Cooling Sensible Heat Gain Components
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Time of Peak</th>
-<th>HVAC Input Sensible Air Heating [W]</th>
-<th>HVAC Input Sensible Air Cooling [W]</th>
-<th>HVAC Input Heated Surface Heating [W]</th>
-<th>HVAC Input Cooled Surface Cooling [W]</th>
-<th>People Sensible Heat Addition [W]</th>
-<th>Lights Sensible Heat Addition [W]</th>
-<th>Equipment Sensible Heat Addition [W]</th>
-<th>Window Heat Addition [W]</th>
-<th>Interzone Air Transfer Heat Addition [W]</th>
-<th>Infiltration Heat Addition [W]</th>
-<th>Opaque Surface Conduction and Other Heat Addition [W]</th>
-<th>Equipment Sensible Heat Removal [W]</th>
-<th>Window Heat Removal [W]</th>
-<th>Interzone Air Transfer Heat Removal [W]</th>
-<th>Infiltration Heat Removal [W]</th>
-<th>Opaque Surface Conduction and Other Heat Removal [W]</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>14-JAN-15:00</td>
-<td>0.00</td>
-<td>-3502.16</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>724.60</td>
-<td>1584.00</td>
-<td>739.20</td>
-<td>9347.85</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-8893.49</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>14-JAN-10:07</td>
-<td>0.00</td>
-<td>-1738.94</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>345.99</td>
-<td>684.00</td>
-<td>410.40</td>
-<td>4684.27</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-4385.71</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>14-JAN-14:45</td>
-<td>0.00</td>
-<td>-1095.49</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>761.13</td>
-<td>1584.00</td>
-<td>844.80</td>
-<td>356.87</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-2451.31</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>14-JAN-16:00</td>
-<td>0.00</td>
-<td>-736.19</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>345.95</td>
-<td>684.00</td>
-<td>228.00</td>
-<td>1157.98</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-1679.74</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>14-JAN-13:35</td>
-<td>0.00</td>
-<td>-2315.43</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1135.19</td>
-<td>2667.60</td>
-<td>1778.40</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-3265.77</td>
-</tr>
-<tr>
-<td>PLENUM-1</td>
-<td>07-JUL-19:46</td>
-<td>0.00</td>
-<td>-1579.40</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1579.40</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total Facility</td>
-<td>14-JAN-15:00</td>
-<td>0.00</td>
-<td>-7822.86</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>3561.18</td>
-<td>7500.00</td>
-<td>3500.00</td>
-<td>10470.76</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-17209.08</td>
-</tr>
-</table>
-
-
-
- Peak Heating Sensible Heat Gain Components
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Time of Peak</th>
-<th>HVAC Input Sensible Air Heating [W]</th>
-<th>HVAC Input Sensible Air Cooling [W]</th>
-<th>HVAC Input Heated Surface Heating [W]</th>
-<th>HVAC Input Cooled Surface Cooling [W]</th>
-<th>People Sensible Heat Addition [W]</th>
-<th>Lights Sensible Heat Addition [W]</th>
-<th>Equipment Sensible Heat Addition [W]</th>
-<th>Window Heat Addition [W]</th>
-<th>Interzone Air Transfer Heat Addition [W]</th>
-<th>Infiltration Heat Addition [W]</th>
-<th>Opaque Surface Conduction and Other Heat Addition [W]</th>
-<th>Equipment Sensible Heat Removal [W]</th>
-<th>Window Heat Removal [W]</th>
-<th>Interzone Air Transfer Heat Removal [W]</th>
-<th>Infiltration Heat Removal [W]</th>
-<th>Opaque Surface Conduction and Other Heat Removal [W]</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>14-JAN-07:00</td>
-<td>10652.50</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>79.20</td>
-<td>21.12</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-1551.57</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-9201.25</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>14-JAN-07:00</td>
-<td>7816.55</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>34.20</td>
-<td>9.12</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-594.65</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-7265.22</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>14-JAN-07:00</td>
-<td>11495.41</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>79.20</td>
-<td>21.12</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-1539.09</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-10056.64</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>14-JAN-07:00</td>
-<td>8837.62</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>34.20</td>
-<td>9.12</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-604.20</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-8276.74</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>14-JAN-07:00</td>
-<td>12359.25</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>148.20</td>
-<td>39.52</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-12546.97</td>
-</tr>
-<tr>
-<td>PLENUM-1</td>
-<td>14-JAN-07:18</td>
-<td>5275.99</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-5275.99</td>
-</tr>
-<tr>
-<td>Total Facility</td>
-<td>14-JAN-07:15</td>
-<td>55720.39</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>375.00</td>
-<td>100.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-4289.51</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>-51905.88</td>
-</tr>
-</table>
-
-
-
-
-
-### Standard 62.1 Summary
-
-This report is more fully described in the Input Output Reference. The Standard 62.1 Summary produces a report that is consistent with many of the outputs needed when doing calculations consistent with ASHRAE Standard 62.1-2010. The report is generated when sizing calculations are specified. The abbreviations used in the report are consistent with the abbreviations used in Appendix A4 of the Standard. Directly following is an example of the report. The key used to obtain this report is Standard62.1Summary.
-
-Report: Standard 62.1 Summary
-
-For: Entire Facility
-
-Timestamp: 2012-04-20 12:00:57
-
-System Ventilation Requirements for Cooling
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Sum of Zone Primary Air Flow - Vpz-sum [m3/s]</th>
-<th>System Population - Ps</th>
-<th>Sum of Zone Population - Pz-sum</th>
-<th>Occupant Diversity - D</th>
-<th>Uncorrected Outdoor Air Intake Airflow - Vou [m3/s]</th>
-<th>System Primary Airflow - Vps [m3/s]</th>
-<th>Average Outdoor Air Fraction - Xs</th>
-<th>System Ventilation Efficiency - Ev</th>
-<th>Outdoor Air Intake Flow - Vot [m3/s]</th>
-<th>Percent Outdoor Air - %OA</th>
-</tr>
-<tr>
-<td>VAV SYS 1</td>
-<td>1.05</td>
-<td>52.00</td>
-<td>52.00</td>
-<td>1.00</td>
-<td>0.26</td>
-<td>1.05</td>
-<td>0.252</td>
-<td>1.000</td>
-<td>0.27</td>
-<td>0.26</td>
-</tr>
-</table>
-
-
-
- System Ventilation Requirements for Heating
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Sum of Zone Primary Air Flow - Vpz-sum [m3/s]</th>
-<th>System Population - Ps</th>
-<th>Sum of Zone Population - Pz-sum</th>
-<th>Occupant Diversity - D</th>
-<th>Uncorrected Outdoor Air Intake Airflow - Vou [m3/s]</th>
-<th>System Primary Airflow - Vps [m3/s]</th>
-<th>Average Outdoor Air Fraction - Xs</th>
-<th>System Ventilation Efficiency - Ev</th>
-<th>Outdoor Air Intake Flow Vot [m3/s]</th>
-<th>Percent Outdoor Air - %OA</th>
-</tr>
-<tr>
-<td>VAV SYS 1</td>
-<td>1.05</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>0.26</td>
-<td>0.43</td>
-<td>0.967</td>
-<td>1.000</td>
-<td>0.27</td>
-<td>0.26</td>
-</tr>
-</table>
-
-
-
- Zone Ventilation Parameters
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>AirLoop Name</th>
-<th>People Outdoor Air Rate - Rp [m3/s-person]</th>
-<th>Zone Population - Pz</th>
-<th>Area Outdoor Air Rate - Ra [m3/s-m2]</th>
-<th>Zone Floor Area - Az [m2]</th>
-<th>Breathing Zone Outdoor Airflow - Vbz [m3/s]</th>
-<th>Cooling Zone Air Distribution Effectiveness - Ez-clg</th>
-<th>Cooling Zone Outdoor Airflow - Voz-clg [m3/s]</th>
-<th>Heating Zone Air Distribution Effectiveness - Ez-htg</th>
-<th>Heating Zone Outdoor Airflow - Voz-htg [m3/s]</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>VAV SYS 1</td>
-<td>0.002360</td>
-<td>11.00</td>
-<td>0.000305</td>
-<td>99.16</td>
-<td>0.0562</td>
-<td>0.900</td>
-<td>0.0624</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>VAV SYS 1</td>
-<td>0.002360</td>
-<td>5.00</td>
-<td>0.000305</td>
-<td>42.73</td>
-<td>0.0248</td>
-<td>0.900</td>
-<td>0.0276</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>VAV SYS 1</td>
-<td>0.002360</td>
-<td>11.00</td>
-<td>0.000305</td>
-<td>96.48</td>
-<td>0.0554</td>
-<td>1.000</td>
-<td>0.0554</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>VAV SYS 1</td>
-<td>0.002360</td>
-<td>5.00</td>
-<td>0.000305</td>
-<td>42.73</td>
-<td>0.0248</td>
-<td>1.000</td>
-<td>0.0248</td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>VAV SYS 1</td>
-<td>0.002360</td>
-<td>20.00</td>
-<td>0.000305</td>
-<td>182.49</td>
-<td>0.1029</td>
-<td>1.000</td>
-<td>0.1029</td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- System Ventilation Parameters
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>People Outdoor Air Rate - Rp [m3/s-person]</th>
-<th>Sum of Zone Population - Pz-sum</th>
-<th>Area Outdoor Air Rate - Ra [m3/s-m2]</th>
-<th>Sum of Zone Floor Area - Az-sum [m2]</th>
-<th>Breathing Zone Outdoor Airflow - Vbz [m3/s]</th>
-<th>Cooling Zone Outdoor Airflow - Voz-clg [m3/s]</th>
-<th>Heating Zone Outdoor Airflow - Voz-htg [m3/s]</th>
-</tr>
-<tr>
-<td>VAV SYS 1</td>
-<td>0.002360</td>
-<td>52.00</td>
-<td>0.000305</td>
-<td>463.60</td>
-<td>0.2641</td>
-<td>0.2731</td>
-<td>0.0000</td>
-</tr>
-</table>
-
-
-
- Zone Ventilation Calculations for Cooling Design
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>AirLoop Name</th>
-<th>Box Type</th>
-<th>Zone Primary Airflow - Vpz [m3/s]</th>
-<th>Zone Discharge Airflow - Vdz [m3/s]</th>
-<th>Minimum Zone Primary Airflow - Vpz-min [m3/s]</th>
-<th>Zone Outdoor Airflow Cooling - Voz-clg [m3/s]</th>
-<th>Primary Outdoor Air Fraction - Zpz</th>
-<th>Primary Air Fraction - Ep</th>
-<th>Secondary Recirculation Fraction- Er</th>
-<th>Supply Air Fraction- Fa</th>
-<th>Mixed Air Fraction - Fb</th>
-<th>Outdoor Air Fraction - Fc</th>
-<th>Zone Ventilation Efficiency - Evz</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>VAV SYS 1</td>
-<td>AIRTERMINAL:SINGLEDUCT:VAV:REHEAT</td>
-<td>0.22</td>
-<td>0.22</td>
-<td>0.08</td>
-<td>0.0624</td>
-<td>0.280</td>
-<td>1.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.900</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>VAV SYS 1</td>
-<td>AIRTERMINAL:SINGLEDUCT:VAV:REHEAT</td>
-<td>0.19</td>
-<td>0.19</td>
-<td>0.03</td>
-<td>0.0276</td>
-<td>0.147</td>
-<td>1.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.900</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>VAV SYS 1</td>
-<td>AIRTERMINAL:SINGLEDUCT:VAV:REHEAT</td>
-<td>0.21</td>
-<td>0.21</td>
-<td>0.07</td>
-<td>0.0554</td>
-<td>0.263</td>
-<td>1.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>1.000</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>VAV SYS 1</td>
-<td>AIRTERMINAL:SINGLEDUCT:VAV:REHEAT</td>
-<td>0.21</td>
-<td>0.21</td>
-<td>0.03</td>
-<td>0.0248</td>
-<td>0.120</td>
-<td>1.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>1.000</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>VAV SYS 1</td>
-<td>AIRTERMINAL:SINGLEDUCT:VAV:REHEAT</td>
-<td>0.22</td>
-<td>0.22</td>
-<td>0.14</td>
-<td>0.1029</td>
-<td>0.465</td>
-<td>1.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>0.000</td>
-<td>1.000</td>
-</tr>
-</table>
-
-
-
- System Ventilation Calculations for Cooling Design
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Sum of Zone Primary Airflow - Vpz-sum [m3/s]</th>
-<th>System Primary Airflow - Vps [m3/s]</th>
-<th>Sum of Zone Discharge Airflow - Vdz-sum [m3/s]</th>
-<th>Minimum Zone Primary Airflow - Vpz-min [m3/s]</th>
-<th>Zone Outdoor Airflow Cooling - Voz-clg [m3/s]</th>
-<th>Zone Ventilation Efficiency - Evz-min</th>
-</tr>
-<tr>
-<td>VAV SYS 1</td>
-<td>1.05</td>
-<td>1.05</td>
-<td>1.05</td>
-<td>0.19</td>
-<td>0.2731</td>
-<td>1.000</td>
-</tr>
-</table>
-
-
-
- Zone Ventilation Calculations for Heating Design
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>AirLoop Name</th>
-<th>Box Type</th>
-<th>Zone Primary Airflow - Vpz [m3/s]</th>
-<th>Zone Discharge Airflow - Vdz [m3/s]</th>
-<th>Minimum Zone Primary Airflow - Vpz-min [m3/s]</th>
-<th>Zone Outdoor Airflow Heating - Voz-htg [m3/s]</th>
-<th>Primary Outdoor Air Fraction - Zpz</th>
-<th>Primary Air Fraction - Ep</th>
-<th>Secondary Recirculation Fraction- Er</th>
-<th>Supply Air Fraction- Fa</th>
-<th>Mixed Air Fraction - Fb</th>
-<th>Outdoor Air Fraction - Fc</th>
-<th>Zone Ventilation Efficiency - Evz</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- System Ventilation Calculations for Heating Design
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Sum of Zone Primary Airflow - Vpz-sum [m3/s]</th>
-<th>System Primary Airflow - Vps [m3/s]</th>
-<th>Sum of Zone Discharge Airflow - Vdz-sum [m3/s]</th>
-<th>Minimum Zone Primary Airflow - Vpz-min [m3/s]</th>
-<th>Zone Outdoor Airflow Heating - Voz-htg [m3/s]</th>
-<th>Zone Ventilation Efficiency - Evz-min</th>
-</tr>
-<tr>
-<td>VAV SYS 1</td>
-<td>1.05</td>
-<td>1.05</td>
-<td>1.05</td>
-<td>0.18+309</td>
-<td>0.0000</td>
-<td>1.000</td>
-</tr>
-</table>
-
-
-
-### Zone Component Loads Summary
-
-The Zone Component Loads Summary provides an estimate of the heating and cooling peak loads for each zone broken down into various components. This report may help determine which components of the load have the largest impact for the heating and cooling peak design conditions. When specified, the Zone Component Loads Summary report is created for each zone that is conditioned. The Sensible-Delayed column of the summary is only an estimate based on a procedure described in the Engineering Reference documentation. An intermediate calculation in this procedure is the decay curves that are shown in the the EIO file when Output:Surfaces:List is set to show DecayCurvesFromZoneComponentLoads. The difference between the peak design sensible load and the estimated instant + delayed sensible load (as shown in the *Peak Conditions* subtable) is an indication of how consistent the overall total estimate may be to the computed total peak loads for the zone. When the report is called the zone sizing calculations are repeated twice so this may result in longer simulation times.  The key used to obtain this report is ZoneComponentLoadSummary.
-
-
-
-Report: ZoneComponentLoadSummary
-
-For: SPACE1-1
-
-Timestamp: 2012-09-21 15:48:46
-
-Estimated Cooling Peak Load Components
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Sensible - Instant [W]</th>
-<th>Sensible - Delayed [W]</th>
-<th>Sensible - Return Air [W]</th>
-<th>Latent [W]</th>
-<th>Total [W]</th>
-<th>%Grand Total</th>
-</tr>
-<tr>
-<td>People</td>
-<td>533.03</td>
-<td>272.38</td>
-<td> </td>
-<td>528.17</td>
-<td>1333.58</td>
-<td>30.78</td>
-</tr>
-<tr>
-<td>Lights</td>
-<td>15.84</td>
-<td>1424.81</td>
-<td>316.80</td>
-<td> </td>
-<td>1757.45</td>
-<td>40.57</td>
-</tr>
-<tr>
-<td>Equipment</td>
-<td>517.44</td>
-<td>318.36</td>
-<td> </td>
-<td>0.00</td>
-<td>835.80</td>
-<td>19.29</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Use Equipment</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>HVAC Equipment Losses</td>
-<td>0.00</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Power Generation Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Infiltration</td>
-<td>34.65</td>
-<td> </td>
-<td> </td>
-<td>69.37</td>
-<td>104.03</td>
-<td>2.40</td>
-</tr>
-<tr>
-<td>Zone Ventilation</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interzone Mixing</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Roof</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interzone Ceiling</td>
-<td> </td>
-<td>132.59</td>
-<td> </td>
-<td> </td>
-<td>132.59</td>
-<td>3.06</td>
-</tr>
-<tr>
-<td>Other Roof</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Wall</td>
-<td> </td>
-<td>451.39</td>
-<td> </td>
-<td> </td>
-<td>451.39</td>
-<td>10.42</td>
-</tr>
-<tr>
-<td>Interzone Wall</td>
-<td> </td>
-<td>-511.9</td>
-<td> </td>
-<td> </td>
-<td>-511.9</td>
-<td>-11.8</td>
-</tr>
-<tr>
-<td>Ground Contact Wall</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Other Wall</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Floor</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interzone Floor</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Ground Contact Floor</td>
-<td> </td>
-<td>-1745.4</td>
-<td> </td>
-<td> </td>
-<td>-1745.4</td>
-<td>-40.3</td>
-</tr>
-<tr>
-<td>Other Floor</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fenestration Conduction</td>
-<td>655.17</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>655.17</td>
-<td>15.12</td>
-</tr>
-<tr>
-<td>Fenestration Solar</td>
-<td>-</td>
-<td>1319.55</td>
-<td> </td>
-<td> </td>
-<td>1319.55</td>
-<td>30.46</td>
-</tr>
-<tr>
-<td>Opaque Door</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Grand Total</td>
-<td>1756.13</td>
-<td>1661.76</td>
-<td>316.80</td>
-<td>597.54</td>
-<td>4332.24</td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Cooling Peak Conditions
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Value</th>
-</tr>
-<tr>
-<td>Time of Peak Load</td>
-<td>7/21 16:00:00</td>
-</tr>
-<tr>
-<td>Outside Dry Bulb Temperature [C]</td>
-<td>30.86</td>
-</tr>
-<tr>
-<td>Outside Wet Bulb Temperature [C]</td>
-<td>23.10</td>
-</tr>
-<tr>
-<td>Outside Humidity Ratio at Peak [kgWater/kgAir]</td>
-<td>0.01459</td>
-</tr>
-<tr>
-<td>Zone Dry Bulb Temperature [C]</td>
-<td>24.00</td>
-</tr>
-<tr>
-<td>Zone Relative Humdity [%]</td>
-<td>47.16</td>
-</tr>
-<tr>
-<td>Zone Humidity Ratio at Peak [kgWater/kgAir]</td>
-<td>0.00876</td>
-</tr>
-<tr>
-<td>Peak Design Sensible Load [W]</td>
-<td>3187.17</td>
-</tr>
-<tr>
-<td>Estimated Instant + Delayed Sensible Load [W]</td>
-<td>3417.89</td>
-</tr>
-<tr>
-<td>Difference [W]</td>
-<td>-230.7</td>
-</tr>
-</table>
-
-
-
-
- Estimated Heating Peak Load Components
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Sensible - Instant [W]</th>
-<th>Sensible - Delayed [W]</th>
-<th>Sensible - Return Air [W]</th>
-<th>Latent [W]</th>
-<th>Total [W]</th>
-<th>%Grand Total</th>
-</tr>
-<tr>
-<td>People</td>
-<td>0.00</td>
-<td>0.00</td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Lights</td>
-<td>0.79</td>
-<td>85.74</td>
-<td>15.84</td>
-<td> </td>
-<td>102.37</td>
-<td>-3.3</td>
-</tr>
-<tr>
-<td>Equipment</td>
-<td>14.78</td>
-<td>9.37</td>
-<td> </td>
-<td>0.00</td>
-<td>24.15</td>
-<td>-0.8</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Use Equipment</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>HVAC Equipment Losses</td>
-<td>0.00</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Power Generation Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Infiltration</td>
-<td>-222.8</td>
-<td> </td>
-<td> </td>
-<td>-93.8</td>
-<td>-316.6</td>
-<td>10.07</td>
-</tr>
-<tr>
-<td>Zone Ventilation</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interzone Mixing</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Roof</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interzone Ceiling</td>
-<td> </td>
-<td>-1027.9</td>
-<td> </td>
-<td> </td>
-<td>-1027.9</td>
-<td>32.70</td>
-</tr>
-<tr>
-<td>Other Roof</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Wall</td>
-<td> </td>
-<td>-762.5</td>
-<td> </td>
-<td> </td>
-<td>-762.5</td>
-<td>24.26</td>
-</tr>
-<tr>
-<td>Interzone Wall</td>
-<td> </td>
-<td>102.80</td>
-<td> </td>
-<td> </td>
-<td>102.80</td>
-<td>-3.3</td>
-</tr>
-<tr>
-<td>Ground Contact Wall</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Other Wall</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Floor</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interzone Floor</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Ground Contact Floor</td>
-<td> </td>
-<td>889.07</td>
-<td> </td>
-<td> </td>
-<td>889.07</td>
-<td>-28.3</td>
-</tr>
-<tr>
-<td>Other Floor</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fenestration Conduction</td>
-<td>-2155.0</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>-2155.0</td>
-<td>68.55</td>
-</tr>
-<tr>
-<td>Fenestration Solar</td>
-<td>-</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Opaque Door</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Grand Total</td>
-<td>-2362.2</td>
-<td>-703.3</td>
-<td>15.84</td>
-<td>-93.8</td>
-<td>-3143.5</td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Heating Peak Conditions
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Value</th>
-</tr>
-<tr>
-<td>Time of Peak Load</td>
-<td>1/21 20:15:00</td>
-</tr>
-<tr>
-<td>Outside Dry Bulb Temperature [C]</td>
-<td>-17.3</td>
-</tr>
-<tr>
-<td>Outside Wet Bulb Temperature [C]</td>
-<td>-19.0</td>
-</tr>
-<tr>
-<td>Outside Humidity Ratio at Peak [kgWater/kgAir]</td>
-<td>0.00084</td>
-</tr>
-<tr>
-<td>Zone Dry Bulb Temperature [C]</td>
-<td>23.00</td>
-</tr>
-<tr>
-<td>Zone Relative Humdity [%]</td>
-<td>43.89</td>
-</tr>
-<tr>
-<td>Zone Humidity Ratio at Peak [kgWater/kgAir]</td>
-<td>0.00766</td>
-</tr>
-<tr>
-<td>Peak Design Sensible Load [W]</td>
-<td>-3077.1</td>
-</tr>
-<tr>
-<td>Estimated Instant + Delayed Sensible Load [W]</td>
-<td>-3065.5</td>
-</tr>
-<tr>
-<td>Difference [W]</td>
-<td>-11.6</td>
-</tr>
-</table>
-
-### Output:Table:TimeBins
-
-A TimeBins report shows a grid of the number of hours that specific report variable spend in a range of values. The first table is broken into two parts. The first part is monthly and the second part is for each hour of the day. The columns show the range of values. A second table is provided to show some statistics on the report variable for the entire year including the maximum and minimum. These statistics are helpful in setting the field values for the interval in the Output Table:TimeBins object. Due to this, it is often necessary to run two simulations to fully utilize the TimeBins report with the first run used to find the minimum and maximum of the variable, these values are then used in the TimeBins object and the second run a better table of binned results are displayed.
-
-Report: PURCHASEDCOOLING:FACILITY J per second
-
-For: Meter
-
-Timestamp: 2006-08-30 07:48:55
-
-Values in table are in hours.
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th> </th>
-<th>1</th>
-<th>2</th>
-<th>3</th>
-<th>4</th>
-<th>5</th>
-<th>6</th>
-<th>7</th>
-<th>8</th>
-<th>9</th>
-<th>10</th>
-<th> </th>
-<th> </th>
-</tr>
-<tr>
-<td>Interval Start</td>
-<td>less than</td>
-<td>0.&lt;=</td>
-<td>2000.&lt;=</td>
-<td>4000.&lt;=</td>
-<td>6000.&lt;=</td>
-<td>8000.&lt;=</td>
-<td>10000.&lt;=</td>
-<td>12000.&lt;=</td>
-<td>14000.&lt;=</td>
-<td>16000.&lt;=</td>
-<td>18000.&lt;=</td>
-<td>equal to or more than</td>
-<td>Row</td>
-</tr>
-<tr>
-<td>Interval End</td>
-<td>0.</td>
-<td>2000.&gt;</td>
-<td>4000.&gt;</td>
-<td>6000.&gt;</td>
-<td>8000.&gt;</td>
-<td>10000.&gt;</td>
-<td>12000.&gt;</td>
-<td>14000.&gt;</td>
-<td>16000.&gt;</td>
-<td>18000.&gt;</td>
-<td>20000.&gt;</td>
-<td>20000.</td>
-<td>Total</td>
-</tr>
-<tr>
-<td>January</td>
-<td>0.00</td>
-<td>744.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>744.00</td>
-</tr>
-<tr>
-<td>February</td>
-<td>0.00</td>
-<td>672.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>672.00</td>
-</tr>
-<tr>
-<td>March</td>
-<td>0.00</td>
-<td>744.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>744.00</td>
-</tr>
-<tr>
-<td>April</td>
-<td>0.00</td>
-<td>524.17</td>
-<td>40.67</td>
-<td>40.33</td>
-<td>45.67</td>
-<td>45.50</td>
-<td>19.67</td>
-<td>4.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>720.00</td>
-</tr>
-<tr>
-<td>May</td>
-<td>0.00</td>
-<td>480.33</td>
-<td>44.50</td>
-<td>55.50</td>
-<td>41.00</td>
-<td>53.50</td>
-<td>38.17</td>
-<td>20.67</td>
-<td>10.33</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>744.00</td>
-</tr>
-<tr>
-<td>June</td>
-<td>0.00</td>
-<td>393.50</td>
-<td>31.83</td>
-<td>55.33</td>
-<td>19.83</td>
-<td>53.00</td>
-<td>65.83</td>
-<td>62.83</td>
-<td>24.00</td>
-<td>13.83</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>720.00</td>
-</tr>
-<tr>
-<td>July</td>
-<td>0.00</td>
-<td>372.67</td>
-<td>30.83</td>
-<td>40.83</td>
-<td>45.67</td>
-<td>53.83</td>
-<td>42.83</td>
-<td>48.33</td>
-<td>45.33</td>
-<td>47.83</td>
-<td>15.83</td>
-<td>0.00</td>
-<td>744.00</td>
-</tr>
-<tr>
-<td>August</td>
-<td>0.00</td>
-<td>373.50</td>
-<td>24.50</td>
-<td>37.17</td>
-<td>44.50</td>
-<td>64.50</td>
-<td>56.67</td>
-<td>50.67</td>
-<td>52.33</td>
-<td>35.00</td>
-<td>5.17</td>
-<td>0.00</td>
-<td>744.00</td>
-</tr>
-<tr>
-<td>September</td>
-<td>0.00</td>
-<td>406.33</td>
-<td>52.00</td>
-<td>42.50</td>
-<td>14.83</td>
-<td>54.50</td>
-<td>64.67</td>
-<td>54.50</td>
-<td>27.17</td>
-<td>3.50</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>720.00</td>
-</tr>
-<tr>
-<td>October</td>
-<td>0.00</td>
-<td>744.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>744.00</td>
-</tr>
-<tr>
-<td>November</td>
-<td>0.00</td>
-<td>720.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>720.00</td>
-</tr>
-<tr>
-<td>December</td>
-<td>0.00</td>
-<td>744.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>744.00</td>
-</tr>
-<tr>
-<td>12:01 to 1:00 am</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>1:01 to 2:00 am</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>2:01 to 3:00 am</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>3:01 to 4:00 am</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>4:01 to 5:00 am</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>5:01 to 6:00 am</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>6:01 to 7:00 am</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>7:01 to 8:00 am</td>
-<td>0.00</td>
-<td>294.33</td>
-<td>33.83</td>
-<td>25.00</td>
-<td>5.17</td>
-<td>2.17</td>
-<td>1.67</td>
-<td>1.17</td>
-<td>1.00</td>
-<td>0.67</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>8:01 to 9:00 am</td>
-<td>0.00</td>
-<td>238.00</td>
-<td>14.17</td>
-<td>16.50</td>
-<td>17.00</td>
-<td>40.33</td>
-<td>29.67</td>
-<td>9.33</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>9:01 to 10:00 am</td>
-<td>0.00</td>
-<td>231.83</td>
-<td>14.50</td>
-<td>13.00</td>
-<td>21.83</td>
-<td>38.83</td>
-<td>31.83</td>
-<td>12.00</td>
-<td>1.17</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>10:01 to 11:00 am</td>
-<td>0.00</td>
-<td>226.33</td>
-<td>14.00</td>
-<td>12.50</td>
-<td>17.50</td>
-<td>36.50</td>
-<td>31.33</td>
-<td>22.17</td>
-<td>4.67</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>11:01 to 12:00 pm</td>
-<td>0.00</td>
-<td>221.33</td>
-<td>12.17</td>
-<td>13.00</td>
-<td>14.50</td>
-<td>30.67</td>
-<td>33.50</td>
-<td>27.83</td>
-<td>11.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>12:01 to 1:00 pm</td>
-<td>0.00</td>
-<td>211.00</td>
-<td>18.00</td>
-<td>14.00</td>
-<td>14.00</td>
-<td>29.17</td>
-<td>32.33</td>
-<td>25.67</td>
-<td>17.67</td>
-<td>3.17</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>1:01 to 2:00 pm</td>
-<td>0.00</td>
-<td>208.00</td>
-<td>15.00</td>
-<td>15.33</td>
-<td>11.00</td>
-<td>22.17</td>
-<td>27.83</td>
-<td>27.50</td>
-<td>26.83</td>
-<td>10.83</td>
-<td>0.50</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>2:01 to 3:00 pm</td>
-<td>0.00</td>
-<td>205.33</td>
-<td>11.83</td>
-<td>18.17</td>
-<td>11.00</td>
-<td>17.50</td>
-<td>23.17</td>
-<td>29.50</td>
-<td>26.17</td>
-<td>18.17</td>
-<td>4.17</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>3:01 to 4:00 pm</td>
-<td>0.00</td>
-<td>203.00</td>
-<td>9.50</td>
-<td>17.67</td>
-<td>14.00</td>
-<td>16.17</td>
-<td>20.67</td>
-<td>30.17</td>
-<td>22.00</td>
-<td>24.83</td>
-<td>7.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>4:01 to 5:00 pm</td>
-<td>0.00</td>
-<td>201.17</td>
-<td>10.83</td>
-<td>18.83</td>
-<td>13.67</td>
-<td>16.33</td>
-<td>19.50</td>
-<td>29.67</td>
-<td>22.83</td>
-<td>25.17</td>
-<td>7.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>5:01 to 6:00 pm</td>
-<td>0.00</td>
-<td>200.00</td>
-<td>13.50</td>
-<td>21.33</td>
-<td>14.83</td>
-<td>22.17</td>
-<td>22.67</td>
-<td>26.00</td>
-<td>25.83</td>
-<td>16.33</td>
-<td>2.33</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>6:01 to 7:00 pm</td>
-<td>0.00</td>
-<td>227.33</td>
-<td>29.17</td>
-<td>43.17</td>
-<td>28.33</td>
-<td>27.50</td>
-<td>9.50</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>7:01 to 8:00 pm</td>
-<td>0.00</td>
-<td>235.83</td>
-<td>27.83</td>
-<td>43.17</td>
-<td>28.67</td>
-<td>25.33</td>
-<td>4.17</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>8:01 to 9:00 pm</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>9:01 to 10:00 pm</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>10:01 to 11:00 pm</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>11:01 to 12:00 am</td>
-<td>0.00</td>
-<td>365.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>365.00</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>0.00</td>
-<td>6918.50</td>
-<td>224.33</td>
-<td>271.67</td>
-<td>211.50</td>
-<td>324.83</td>
-<td>287.83</td>
-<td>241.00</td>
-<td>159.17</td>
-<td>100.17</td>
-<td>21.00</td>
-<td>0.00</td>
-<td>8760.00</td>
-</tr>
-</table>
-
-
- Statistics
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Statistic</th>
-</tr>
-<tr>
-<td>Minimum</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Mean minus two standard deviations</td>
-<td>-6496.35</td>
-</tr>
-<tr>
-<td>Mean</td>
-<td>1995.71</td>
-</tr>
-<tr>
-<td>Mean plus two standard deviations</td>
-<td>10487.78</td>
-</tr>
-<tr>
-<td>Maximum</td>
-<td>19476.00</td>
-</tr>
-<tr>
-<td>Standard deviation</td>
-<td>4246.03</td>
-</tr>
-</table>
-
-### Output:Table:Monthly
-
-Monthly reports are not predefined. Instead each column is defined when using the Output:Table:Monthly object. In that object each column is defined by a variable and how it should be aggregated. The StandardReports.idf file is located in DataSets directory where EnergyPlus is installed and contains a large number of examples of how to use Output:Table:Monthly to get summaries of the performance of different components in the building model. These examples include:
-
-- Zone Cooling Summary
-
-- Zone Heating Summary
-
-- Zone Electric Summary
-
-- Space Gains
-
-- Peak Space Gains
-
-- Space Gain Components at Cooling Peak
-
-- Energy Consumption - Electricity & Natural Gas
-
-- Energy Consumption - Electricity Generated & Propane
-
-- Energy Consumption - Diesel & Fuel Oil
-
-- Energy Consumption  - Purchased Heating & Cooling
-
-- Energy Consumption - Coal & Gasoline
-
-- End-Use Energy Consumption - Electricity
-
-- End-Use Energy Consumption - Natural Gas
-
-- End-Use Energy Consumption - Diesel
-
-- End-Use Energy Consumption - Fuel Oil
-
-- End-Use Energy Consumption - Coal
-
-- End-Use Energy Consumption - Propane
-
-- End-Use Energy Consumption - Gasoline
-
-- Peak Energy End-Use - Electricity Part 1
-
-- Peak Energy End-Use - Electricity Part 2
-
-- Electric Components of Peak Demand
-
-- Peak Energy End-Use - Natural Gas
-
-- Peak Energy End-Use - Diesel
-
-- Peak Energy End-Use - Fuel Oil
-
-- Peak Energy End-Use - Coal
-
-- Peak Energy End-Use - Propane
-
-- Peak Energy End-Use - Gasoline
-
-- Setpoints Not Met With Temperatures
-
-- Comfort Report - Simple 55
-
-- Unglazed Transpired Solar Collector Summary
-
-- Occupant Comfort Data Summary
-
-- Chiller Report
-
-- Tower Report
-
-- Boiler Report
-
-- DX Report
-
-- Window Report
-
-- Window Energy Report
-
-- Window Zone Summary
-
-- Average Outdoor Conditions
-
-- Outdoor Conditions Maximum Drybulb
-
-- Outdoor Conditions Minimum Drybulb
-
-- Outdoor Conditions Maximum Wetbulb
-
-- Outdoor Conditions Maximum Dewpoint
-
-- Outdoor Ground Conditions
-
-- Window AC Report
-
-- Water Heater Report
-
-- Generator Report
-
-- Daylighting Report
-
-- Coil Report
-
-- Plant Loop Demand Report
-
-- Fan Report
-
-- Pump Report
-
-- Cond Loop Demand Report
-
-- Zone Temperature Oscillation Report
-
-- Air Loop System Energy and Water Use
-
-- Air Loop System Component Loads
-
-- Air Loop System Component Energy Use
-
-- Mechanical Ventilation Loads
-
-An example of the Zone Cooling Summary monthly report is shown below.
-
-Report: ZONE COOLING SUMMARY
-
-For: SPACE2-1
-
-Timestamp: 2006-08-29 07:21:57
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>ZONE/SYS SENSIBLE COOLING ENERGY [J]</th>
-<th>ZONE/SYS SENSIBLE COOLING RATE {MAXIMUM}[W]</th>
-<th>ZONE/SYS SENSIBLE COOLING RATE {TIMESTAMP}</th>
-<th>OUTDOOR DRY BULB {AT MAX/MIN} [C]</th>
-<th>OUTDOOR WET BULB {AT MAX/MIN} [C]</th>
-<th>ZONE TOTAL INTERNAL LATENT GAIN [J]</th>
-<th>ZONE TOTAL INTERNAL LATENT GAIN {MAXIMUM}[W]</th>
-<th>ZONE TOTAL INTERNAL LATENT GAIN {TIMESTAMP}</th>
-<th>OUTDOOR DRY BULB {AT MAX/MIN} [C]</th>
-<th>OUTDOOR WET BULB {AT MAX/MIN} [C]</th>
-</tr>
-<tr>
-<td>January</td>
-<td>281755456.00</td>
-<td>1427.84</td>
-<td>17-JAN-10:07</td>
-<td>8.30</td>
-<td>5.48</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-JAN-00:15</td>
-<td>-4.32</td>
-<td>-5.53</td>
-</tr>
-<tr>
-<td>February</td>
-<td>306879872.00</td>
-<td>1440.59</td>
-<td>28-FEB-10:46</td>
-<td>11.27</td>
-<td>6.67</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-FEB-00:15</td>
-<td>-3.17</td>
-<td>-4.91</td>
-</tr>
-<tr>
-<td>March</td>
-<td>419829728.00</td>
-<td>1822.13</td>
-<td>26-MAR-09:14</td>
-<td>3.90</td>
-<td>-0.20</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-MAR-00:15</td>
-<td>-1.40</td>
-<td>-2.84</td>
-</tr>
-<tr>
-<td>April</td>
-<td>752874688.00</td>
-<td>1986.25</td>
-<td>29-APR-10:22</td>
-<td>21.10</td>
-<td>11.44</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-APR-00:15</td>
-<td>17.12</td>
-<td>10.64</td>
-</tr>
-<tr>
-<td>May</td>
-<td>0.100670E+10</td>
-<td>2163.18</td>
-<td>22-MAY-09:45</td>
-<td>25.17</td>
-<td>15.42</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-MAY-00:15</td>
-<td>3.75</td>
-<td>1.60</td>
-</tr>
-<tr>
-<td>June</td>
-<td>0.100822E+10</td>
-<td>2129.73</td>
-<td>28-JUN-09:45</td>
-<td>28.02</td>
-<td>22.39</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-JUN-00:15</td>
-<td>17.30</td>
-<td>14.95</td>
-</tr>
-<tr>
-<td>July</td>
-<td>0.120671E+10</td>
-<td>2312.36</td>
-<td>08-JUL-09:00</td>
-<td>31.70</td>
-<td>23.35</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-JUL-00:15</td>
-<td>15.60</td>
-<td>12.95</td>
-</tr>
-<tr>
-<td>August</td>
-<td>0.109213E+10</td>
-<td>2352.64</td>
-<td>02-AUG-09:45</td>
-<td>27.08</td>
-<td>20.48</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-AUG-00:15</td>
-<td>17.20</td>
-<td>15.70</td>
-</tr>
-<tr>
-<td>September</td>
-<td>0.100619E+10</td>
-<td>2453.23</td>
-<td>06-SEP-10:15</td>
-<td>28.35</td>
-<td>20.53</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-SEP-00:15</td>
-<td>16.75</td>
-<td>15.45</td>
-</tr>
-<tr>
-<td>October</td>
-<td>771385600.00</td>
-<td>2181.25</td>
-<td>10-OCT-10:16</td>
-<td>15.25</td>
-<td>10.12</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-OCT-00:15</td>
-<td>4.88</td>
-<td>3.31</td>
-</tr>
-<tr>
-<td>November</td>
-<td>384831744.00</td>
-<td>1566.35</td>
-<td>11-NOV-10:45</td>
-<td>14.00</td>
-<td>8.89</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-NOV-00:15</td>
-<td>14.65</td>
-<td>11.75</td>
-</tr>
-<tr>
-<td>December</td>
-<td>246930448.00</td>
-<td>1306.75</td>
-<td>11-DEC-10:07</td>
-<td>5.00</td>
-<td>1.69</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>01-DEC-00:15</td>
-<td>1.80</td>
-<td>-0.11</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Annual Sum or Average</td>
-<td>0.848444E+10</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Minimum of Months</td>
-<td>246930448.00</td>
-<td>1306.75</td>
-<td> </td>
-<td>3.90</td>
-<td>-0.20</td>
-<td>0.00</td>
-<td>0.00</td>
-<td> </td>
-<td>-4.32</td>
-<td>-5.53</td>
-</tr>
-<tr>
-<td>Maximum of Months</td>
-<td>0.120671E+10</td>
-<td>2453.23</td>
-<td> </td>
-<td>31.70</td>
-<td>23.35</td>
-<td>0.00</td>
-<td>0.00</td>
-<td> </td>
-<td>17.30</td>
-<td>15.70</td>
-</tr>
-</table>
-
-
-
-### UtilityCost:Tariff
-
-The use of UtilityCost:Tariff objects automatically generates two reports related to the calculation of annual utility costs. The first report is a summary across multiple tariffs and is called the Economics Results Summary report and is shown directly below. After that example is an example of the Tariff report which is created for each of the UtilityCost:Tariff Objects defined in the IDF file  (some columns may be truncated due to page size).
-
-Report: Economics Results Summary Report
-
-For: Entire Facility
-
-Timestamp: 2006-08-29 07:21:57
-
-Annual Cost
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Facility:Electric</th>
-<th>Facility:Gas</th>
-<th>Other</th>
-<th>Total</th>
-</tr>
-<tr>
-<td>Cost ($)</td>
-<td>2269.11</td>
-<td>612.08</td>
-<td>0.00</td>
-<td>2881.19</td>
-</tr>
-<tr>
-<td>Cost per Total Building Area ($/m2)</td>
-<td>2.45</td>
-<td>0.66</td>
-<td>0.00</td>
-<td>3.11</td>
-</tr>
-<tr>
-<td>Cost per Net Conditioned Building Area ($/m2)</td>
-<td>2.45</td>
-<td>0.66</td>
-<td>0.00</td>
-<td>3.11</td>
-</tr>
-</table>
-
-
- Tariff Summary
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Selected</th>
-<th>Qualified</th>
-<th>Meter</th>
-<th>Group</th>
-<th>Annual Cost</th>
-</tr>
-<tr>
-<td>EXAMPLEA</td>
-<td>No</td>
-<td>Yes</td>
-<td>ELECTRICITY:FACILITY</td>
-<td>(none)</td>
-<td>2359.48</td>
-</tr>
-<tr>
-<td>EXAMPLEA-GAS</td>
-<td>Yes</td>
-<td>Yes</td>
-<td>GAS:FACILITY</td>
-<td>(none)</td>
-<td>612.08</td>
-</tr>
-<tr>
-<td>EXAMPLEAWITHVARIABLEMONTHLYCHARGE</td>
-<td>No</td>
-<td>Yes</td>
-<td>ELECTRICITY:FACILITY</td>
-<td>(none)</td>
-<td>2407.36</td>
-</tr>
-<tr>
-<td>EXAMPLEB</td>
-<td>No</td>
-<td>Yes</td>
-<td>ELECTRICITY:FACILITY</td>
-<td>(none)</td>
-<td>2668.34</td>
-</tr>
-<tr>
-<td>EXAMPLEC</td>
-<td>No</td>
-<td>Yes</td>
-<td>ELECTRICITY:FACILITY</td>
-<td>(none)</td>
-<td>3017.45</td>
-</tr>
-<tr>
-<td>EXAMPLED</td>
-<td>Yes</td>
-<td>Yes</td>
-<td>ELECTRICITY:FACILITY</td>
-<td>(none)</td>
-<td>2269.11</td>
-</tr>
-<tr>
-<td>EXAMPLEDWITHRATCHET</td>
-<td>No</td>
-<td>Yes</td>
-<td>ELECTRICITY:FACILITY</td>
-<td>(none)</td>
-<td>3745.90</td>
-</tr>
-<tr>
-<td>EXAMPLEE</td>
-<td>No</td>
-<td>Yes</td>
-<td>ELECTRICITY:FACILITY</td>
-<td>(none)</td>
-<td>3766.76</td>
-</tr>
-<tr>
-<td>EXAMPLEF</td>
-<td>No</td>
-<td>Yes</td>
-<td>ELECTRICITY:FACILITY</td>
-<td>(none)</td>
-<td>3512.12</td>
-</tr>
-<tr>
-<td>EXAMPLEFMC</td>
-<td>No</td>
-<td>Yes</td>
-<td>ELECTRICITY:FACILITY</td>
-<td>(none)</td>
-<td>3512.12</td>
-</tr>
-<tr>
-<td>EXAMPLEG</td>
-<td>No</td>
-<td>Yes</td>
-<td>ELECTRICITY:FACILITY</td>
-<td>(none)</td>
-<td>3866.91</td>
-</tr>
-</table>
-
-
-
-The following is an example of the Tariff report which is created for each of the UtilityCost:Tariff objects defined in the file.
-
-Report: Tariff Report
-
-For: EXAMPLEA
-
-Timestamp: 2006-08-29 07:21:57
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Parameter</th>
-</tr>
-<tr>
-<td>Meter</td>
-<td>ELECTRICITY:FACILITY</td>
-</tr>
-<tr>
-<td>Selected</td>
-<td>No</td>
-</tr>
-<tr>
-<td>Group</td>
-<td>(none)</td>
-</tr>
-<tr>
-<td>Qualified</td>
-<td>Yes</td>
-</tr>
-<tr>
-<td>Disqualifier</td>
-<td>n/a</td>
-</tr>
-<tr>
-<td>Computation</td>
-<td>automatic</td>
-</tr>
-<tr>
-<td>Units</td>
-<td>kWh</td>
-</tr>
-</table>
-
-
- Categories
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Jan</th>
-<th>Feb</th>
-<th>Mar</th>
-<th>Apr</th>
-<th>May</th>
-<th>Jun</th>
-<th>Jul</th>
-<th>Aug</th>
-<th>Sep</th>
-<th>Oct</th>
-<th>Nov</th>
-<th>Dec</th>
-<th>Sum</th>
-<th>Max</th>
-</tr>
-<tr>
-<td>EnergyCharges</td>
-<td>181.84</td>
-<td>159.97</td>
-<td>170.98</td>
-<td>178.85</td>
-<td>207.28</td>
-<td>207.97</td>
-<td>249.10</td>
-<td>234.09</td>
-<td>202.57</td>
-<td>191.20</td>
-<td>169.19</td>
-<td>176.34</td>
-<td>2329.36</td>
-<td>249.10</td>
-</tr>
-<tr>
-<td>DemandCharges</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>ServiceCharges</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>2.51</td>
-<td>30.12</td>
-<td>2.51</td>
-</tr>
-<tr>
-<td>Basis</td>
-<td>184.35</td>
-<td>162.48</td>
-<td>173.49</td>
-<td>181.36</td>
-<td>209.79</td>
-<td>210.48</td>
-<td>251.61</td>
-<td>236.60</td>
-<td>205.08</td>
-<td>193.71</td>
-<td>171.70</td>
-<td>178.85</td>
-<td>2359.48</td>
-<td>251.61</td>
-</tr>
-<tr>
-<td>Adjustment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Surcharge</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Subtotal</td>
-<td>184.35</td>
-<td>162.48</td>
-<td>173.49</td>
-<td>181.36</td>
-<td>209.79</td>
-<td>210.48</td>
-<td>251.61</td>
-<td>236.60</td>
-<td>205.08</td>
-<td>193.71</td>
-<td>171.70</td>
-<td>178.85</td>
-<td>2359.48</td>
-<td>251.61</td>
-</tr>
-<tr>
-<td>Taxes</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>184.35</td>
-<td>162.48</td>
-<td>173.49</td>
-<td>181.36</td>
-<td>209.79</td>
-<td>210.48</td>
-<td>251.61</td>
-<td>236.60</td>
-<td>205.08</td>
-<td>193.71</td>
-<td>171.70</td>
-<td>178.85</td>
-<td>2359.48</td>
-<td>251.61</td>
-</tr>
-</table>
-
-
- Charges
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Jan</th>
-<th>Feb</th>
-<th>Mar</th>
-<th>Apr</th>
-<th>May</th>
-<th>Jun</th>
-<th>Jul</th>
-<th>Aug</th>
-<th>Sep</th>
-<th>Oct</th>
-<th>Nov</th>
-<th>Dec</th>
-<th>Sum</th>
-<th>Max</th>
-<th>Category</th>
-</tr>
-<tr>
-<td>FLATENERGYCHARGE</td>
-<td>181.84</td>
-<td>159.97</td>
-<td>170.98</td>
-<td>178.85</td>
-<td>207.28</td>
-<td>207.97</td>
-<td>249.10</td>
-<td>234.09</td>
-<td>202.57</td>
-<td>191.20</td>
-<td>169.19</td>
-<td>176.34</td>
-<td>2329.36</td>
-<td>249.10</td>
-<td>none</td>
-</tr>
-</table>
-
-
- Ratchets
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Jan</th>
-<th>Feb</th>
-<th>Mar</th>
-<th>Apr</th>
-<th>May</th>
-<th>Jun</th>
-<th>Jul</th>
-<th>Aug</th>
-<th>Sep</th>
-<th>Oct</th>
-<th>Nov</th>
-<th>Dec</th>
-<th>Sum</th>
-<th>Max</th>
-</tr>
-</table>
-
-
- Qualifies
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Jan</th>
-<th>Feb</th>
-<th>Mar</th>
-<th>Apr</th>
-<th>May</th>
-<th>Jun</th>
-<th>Jul</th>
-<th>Aug</th>
-<th>Sep</th>
-<th>Oct</th>
-<th>Nov</th>
-<th>Dec</th>
-<th>Sum</th>
-<th>Max</th>
-</tr>
-</table>
-
-
- Native Variables
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Jan</th>
-<th>Feb</th>
-<th>Mar</th>
-<th>Apr</th>
-<th>May</th>
-<th>Jun</th>
-<th>Jul</th>
-<th>Aug</th>
-<th>Sep</th>
-<th>Oct</th>
-<th>Nov</th>
-<th>Dec</th>
-<th>Sum</th>
-<th>Max</th>
-</tr>
-<tr>
-<td>TotalEnergy</td>
-<td>3285.70</td>
-<td>2890.52</td>
-<td>3089.52</td>
-<td>3231.79</td>
-<td>3745.42</td>
-<td>3757.86</td>
-<td>4501.09</td>
-<td>4229.79</td>
-<td>3660.28</td>
-<td>3454.82</td>
-<td>3057.13</td>
-<td>3186.33</td>
-<td>42090.24</td>
-<td>4501.09</td>
-</tr>
-<tr>
-<td>TotalDemand</td>
-<td>12.52</td>
-<td>12.53</td>
-<td>12.53</td>
-<td>14.53</td>
-<td>17.40</td>
-<td>20.71</td>
-<td>21.08</td>
-<td>19.50</td>
-<td>18.63</td>
-<td>15.53</td>
-<td>12.90</td>
-<td>12.55</td>
-<td>190.42</td>
-<td>21.08</td>
-</tr>
-<tr>
-<td>PeakEnergy</td>
-<td>3285.70</td>
-<td>2890.52</td>
-<td>3089.52</td>
-<td>3231.79</td>
-<td>3745.42</td>
-<td>3757.86</td>
-<td>4501.09</td>
-<td>4229.79</td>
-<td>3660.28</td>
-<td>3454.82</td>
-<td>3057.13</td>
-<td>3186.33</td>
-<td>42090.24</td>
-<td>4501.09</td>
-</tr>
-<tr>
-<td>PeakDemand</td>
-<td>12.52</td>
-<td>12.53</td>
-<td>12.53</td>
-<td>14.53</td>
-<td>17.40</td>
-<td>20.71</td>
-<td>21.08</td>
-<td>19.50</td>
-<td>18.63</td>
-<td>15.53</td>
-<td>12.90</td>
-<td>12.55</td>
-<td>190.42</td>
-<td>21.08</td>
-</tr>
-<tr>
-<td>ShoulderEnergy</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>ShoulderDemand</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>OffPeakEnergy</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>OffPeakDemand</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>MidPeakEnergy</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>MidPeakDemand</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>PeakExceedsOffPeak</td>
-<td>12.52</td>
-<td>12.53</td>
-<td>12.53</td>
-<td>14.53</td>
-<td>17.40</td>
-<td>20.71</td>
-<td>21.08</td>
-<td>19.50</td>
-<td>18.63</td>
-<td>15.53</td>
-<td>12.90</td>
-<td>12.55</td>
-<td>190.42</td>
-<td>21.08</td>
-</tr>
-<tr>
-<td>OffPeakExceedsPeak</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>PeakExceedsMidPeak</td>
-<td>12.52</td>
-<td>12.53</td>
-<td>12.53</td>
-<td>14.53</td>
-<td>17.40</td>
-<td>20.71</td>
-<td>21.08</td>
-<td>19.50</td>
-<td>18.63</td>
-<td>15.53</td>
-<td>12.90</td>
-<td>12.55</td>
-<td>190.42</td>
-<td>21.08</td>
-</tr>
-<tr>
-<td>MidPeakExceedsPeak</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>PeakExceedsShoulder</td>
-<td>12.52</td>
-<td>12.53</td>
-<td>12.53</td>
-<td>14.53</td>
-<td>17.40</td>
-<td>20.71</td>
-<td>21.08</td>
-<td>19.50</td>
-<td>18.63</td>
-<td>15.53</td>
-<td>12.90</td>
-<td>12.55</td>
-<td>190.42</td>
-<td>21.08</td>
-</tr>
-<tr>
-<td>ShoulderExceedsPeak</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>IsWinter</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>12.00</td>
-<td>1.00</td>
-</tr>
-<tr>
-<td>IsNotWinter</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>IsSpring</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>IsNotSpring</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>12.00</td>
-<td>1.00</td>
-</tr>
-<tr>
-<td>IsSummer</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>IsNotSummer</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>12.00</td>
-<td>1.00</td>
-</tr>
-<tr>
-<td>IsAutumn</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>IsNotAutumn</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>12.00</td>
-<td>1.00</td>
-</tr>
-<tr>
-<td>PeakAndShoulderEnergy</td>
-<td>3285.70</td>
-<td>2890.52</td>
-<td>3089.52</td>
-<td>3231.79</td>
-<td>3745.42</td>
-<td>3757.86</td>
-<td>4501.09</td>
-<td>4229.79</td>
-<td>3660.28</td>
-<td>3454.82</td>
-<td>3057.13</td>
-<td>3186.33</td>
-<td>42090.24</td>
-<td>4501.09</td>
-</tr>
-<tr>
-<td>PeakAndShoulderDemand</td>
-<td>12.52</td>
-<td>12.53</td>
-<td>12.53</td>
-<td>14.53</td>
-<td>17.40</td>
-<td>20.71</td>
-<td>21.08</td>
-<td>19.50</td>
-<td>18.63</td>
-<td>15.53</td>
-<td>12.90</td>
-<td>12.55</td>
-<td>190.42</td>
-<td>21.08</td>
-</tr>
-<tr>
-<td>PeakAndMidPeakEnergy</td>
-<td>3285.70</td>
-<td>2890.52</td>
-<td>3089.52</td>
-<td>3231.79</td>
-<td>3745.42</td>
-<td>3757.86</td>
-<td>4501.09</td>
-<td>4229.79</td>
-<td>3660.28</td>
-<td>3454.82</td>
-<td>3057.13</td>
-<td>3186.33</td>
-<td>42090.24</td>
-<td>4501.09</td>
-</tr>
-<tr>
-<td>PeakAndMidPeakDemand</td>
-<td>12.52</td>
-<td>12.53</td>
-<td>12.53</td>
-<td>14.53</td>
-<td>17.40</td>
-<td>20.71</td>
-<td>21.08</td>
-<td>19.50</td>
-<td>18.63</td>
-<td>15.53</td>
-<td>12.90</td>
-<td>12.55</td>
-<td>190.42</td>
-<td>21.08</td>
-</tr>
-<tr>
-<td>ShoulderAndOffPeakEnergy</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>ShoulderAndOffPeakDemand</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>PeakAndOffPeakEnergy</td>
-<td>3285.70</td>
-<td>2890.52</td>
-<td>3089.52</td>
-<td>3231.79</td>
-<td>3745.42</td>
-<td>3757.86</td>
-<td>4501.09</td>
-<td>4229.79</td>
-<td>3660.28</td>
-<td>3454.82</td>
-<td>3057.13</td>
-<td>3186.33</td>
-<td>42090.24</td>
-<td>4501.09</td>
-</tr>
-<tr>
-<td>PeakAndOffPeakDemand</td>
-<td>12.52</td>
-<td>12.53</td>
-<td>12.53</td>
-<td>14.53</td>
-<td>17.40</td>
-<td>20.71</td>
-<td>21.08</td>
-<td>19.50</td>
-<td>18.63</td>
-<td>15.53</td>
-<td>12.90</td>
-<td>12.55</td>
-<td>190.42</td>
-<td>21.08</td>
-</tr>
-</table>
-
-
- Other Variables
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Jan</th>
-<th>Feb</th>
-<th>Mar</th>
-<th>Apr</th>
-<th>May</th>
-<th>Jun</th>
-<th>Jul</th>
-<th>Aug</th>
-<th>Sep</th>
-<th>Oct</th>
-<th>Nov</th>
-<th>Dec</th>
-<th>Sum</th>
-<th>Max</th>
-</tr>
-<tr>
-<td>NotIncluded</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
- Computation - Automatic
- FLATENERGYCHARGE FROM TotalEnergy
- EnergyCharges SUM FLATENERGYCHARGE
- Basis SUM EnergyCharges DemandCharges ServiceCharges
- Subtotal SUM Basis Adjustment Surcharge
- Total SUM Subtotal Taxes
-
-### Construction Cost Estimate Summary
-
-The Construction Cost Estimate Summary report shows the details of a simplified cost estimate of the building along with a comparison with reference building costs entered by the user. An example of the Construction Cost Estimate Summary report is shown below.
-
-Construction Cost Estimate Summary
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Reference Bldg.</th>
-<th>Current Bldg. Model</th>
-<th>Difference</th>
-</tr>
-<tr>
-<td>Line Item SubTotal ($)</td>
-<td>665082.04</td>
-<td>720964.07</td>
-<td>55882.03</td>
-</tr>
-<tr>
-<td>Misc. Costs ($)</td>
-<td>928979.09</td>
-<td>928979.09</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Regional Adjustment ($)</td>
-<td>216792.31</td>
-<td>224392.27</td>
-<td>7599.96</td>
-</tr>
-<tr>
-<td>Design Fee ($)</td>
-<td>108651.21</td>
-<td>149946.83</td>
-<td>41295.63</td>
-</tr>
-<tr>
-<td>Contractor Fee ($)</td>
-<td>126759.74</td>
-<td>131203.48</td>
-<td>4443.74</td>
-</tr>
-<tr>
-<td>Contigency ($)</td>
-<td>181085.34</td>
-<td>187433.54</td>
-<td>6348.20</td>
-</tr>
-<tr>
-<td>Permits, Bonds, Insurance ($)</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Commissioning ($)</td>
-<td>9054.27</td>
-<td>18743.35</td>
-<td>9689.09</td>
-</tr>
-<tr>
-<td>Cost Estimate Total ($)</td>
-<td>2236404.00</td>
-<td>2361662.65</td>
-<td>125258.65</td>
-</tr>
-<tr>
-<td>Cost Per Conditioned Building Area ($/m2)</td>
-<td>1203.69</td>
-<td>1271.11</td>
-<td>67.42</td>
-</tr>
-</table>
-
-
-
- Cost Line Item Details
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Line No.</th>
-<th>Item Name</th>
-<th>Quantity.</th>
-<th>Units</th>
-<th>$ per Qty.</th>
-<th>SubTotal $</th>
-</tr>
-<tr>
-<td>--</td>
-<td>1</td>
-<td>EXTERIOR WALLS</td>
-<td>627.57</td>
-<td>m2</td>
-<td>168.64</td>
-<td>105832.65</td>
-</tr>
-<tr>
-<td>--</td>
-<td>2</td>
-<td>INTERIOR WALLS</td>
-<td>854.18</td>
-<td>m2</td>
-<td>31.16</td>
-<td>26616.23</td>
-</tr>
-<tr>
-<td>--</td>
-<td>3</td>
-<td>ROOF</td>
-<td>1857.96</td>
-<td>m2</td>
-<td>104.69</td>
-<td>194509.64</td>
-</tr>
-<tr>
-<td>--</td>
-<td>4</td>
-<td>GROUND FLR SLAB</td>
-<td>1857.96</td>
-<td>m2</td>
-<td>56.06</td>
-<td>104157.14</td>
-</tr>
-<tr>
-<td>--</td>
-<td>5</td>
-<td>ACOUSTICAL DROP CEILINGS</td>
-<td>1857.96</td>
-<td>m2</td>
-<td>23.79</td>
-<td>44200.83</td>
-</tr>
-<tr>
-<td>--</td>
-<td>6</td>
-<td>QUAD HIGH SHGC SUPERWINDOWS</td>
-<td>226.22</td>
-<td>m2</td>
-<td>687.84</td>
-<td>155604.96</td>
-</tr>
-<tr>
-<td>--</td>
-<td>7</td>
-<td>QUAD LOW SHGC SUPERWINDOWS</td>
-<td>42.68</td>
-<td>m2</td>
-<td>687.84</td>
-<td>29359.55</td>
-</tr>
-<tr>
-<td>--</td>
-<td>8</td>
-<td>CENTRAL CHILLER</td>
-<td>153.48</td>
-<td>kW (tot cool cap.)</td>
-<td>340.00</td>
-<td>52183.09</td>
-</tr>
-<tr>
-<td>--</td>
-<td>9</td>
-<td>CONTINUOUS AIR BARRIER</td>
-<td>1.00</td>
-<td>Ea.</td>
-<td>8500.00</td>
-<td>8500.00</td>
-</tr>
-<tr>
-<td>Line Item SubTotal</td>
-<td>--</td>
-<td>--</td>
-<td>--</td>
-<td>--</td>
-<td>--</td>
-<td>720964.07</td>
-</tr>
-</table>
-
-### XML Tabular Output
-
-The tables discussed in this section can also be output in an XML format that may be easier for some other programs to extract specific results. An excerpt of the XML file format is shown below. This report presents the same output results as the other tabular report formats but using XML tags.
-
-
-
-&lt;?xml version="1.0"?&gt;
-
-&lt;EnergyPlusTabularReports&gt;
-
-  &lt;BuildingName&gt;NONE&lt;/BuildingName&gt;
-
-  &lt;EnvironmentName&gt;Chicago Ohare Intl Ap IL USA TMY3 WMO\#=725300&lt;/EnvironmentName&gt;
-
-  &lt;WeatherFileLocationTitle&gt;Chicago Ohare Intl Ap IL USA TMY3 WMO\#=725300&lt;/WeatherFileLocationTitle&gt;
-
-  &lt;ProgramVersion&gt;EnergyPlus, Version 8.0, YMD=2013.02.18 15:50&lt;/ProgramVersion&gt;
-
-  &lt;SimulationTimestamp&gt;
-
-    &lt;Date&gt;
-
-      2013-02-18
-
-    &lt;/Date&gt;
-
-    &lt;Time&gt;
-
-      15:50:33
-
-    &lt;/Time&gt;
-
-  &lt;/SimulationTimestamp&gt;
-
-
-
-
-
-&lt;AnnualBuildingUtilityPerformanceSummary&gt;
-
-  &lt;for&gt;Entire Facility&lt;/for&gt;
-
-  &lt;SiteAndSourceEnergy&gt;
-
-    &lt;name&gt;TotalSiteEnergy&lt;/name&gt;
-
-    &lt;TotalEnergy units="kBtu"&gt;200671.97&lt;/TotalEnergy&gt;
-
-    &lt;EnergyPerTotalBuildingArea units="kBtu/ft2"&gt;143.32&lt;/EnergyPerTotalBuildingArea&gt;
-
-    &lt;EnergyPerConditionedBuildingArea units="kBtu/ft2"&gt;143.32&lt;/EnergyPerConditionedBuildingArea&gt;
-
-  &lt;/SiteAndSourceEnergy&gt;
-
-  &lt;SiteAndSourceEnergy&gt;
-
-    &lt;name&gt;NetSiteEnergy&lt;/name&gt;
-
-    &lt;TotalEnergy units="kBtu"&gt;200671.97&lt;/TotalEnergy&gt;
-
-    &lt;EnergyPerTotalBuildingArea units="kBtu/ft2"&gt;143.32&lt;/EnergyPerTotalBuildingArea&gt;
-
-    &lt;EnergyPerConditionedBuildingArea units="kBtu/ft2"&gt;143.32&lt;/EnergyPerConditionedBuildingArea&gt;
-
-  &lt;/SiteAndSourceEnergy&gt;
-
-  &lt;SiteAndSourceEnergy&gt;
-
-    &lt;name&gt;TotalSourceEnergy&lt;/name&gt;
-
-    &lt;TotalEnergy units="kBtu"&gt;442504.19&lt;/TotalEnergy&gt;
-
-    &lt;EnergyPerTotalBuildingArea units="kBtu/ft2"&gt;316.04&lt;/EnergyPerTotalBuildingArea&gt;
-
-    &lt;EnergyPerConditionedBuildingArea units="kBtu/ft2"&gt;316.04&lt;/EnergyPerConditionedBuildingArea&gt;
-
-  &lt;/SiteAndSourceEnergy&gt;
-
-  &lt;SiteAndSourceEnergy&gt;
-
-    &lt;name&gt;NetSourceEnergy&lt;/name&gt;
-
-    &lt;TotalEnergy units="kBtu"&gt;397810.98&lt;/TotalEnergy&gt;
-
-    &lt;EnergyPerTotalBuildingArea units="kBtu/ft2"&gt;284.12&lt;/EnergyPerTotalBuildingArea&gt;
-
-    &lt;EnergyPerConditionedBuildingArea units="kBtu/ft2"&gt;284.12&lt;/EnergyPerConditionedBuildingArea&gt;
-
-  &lt;/SiteAndSourceEnergy&gt;
-
-
-
-*An actual file will be much longer than this example but follows this format.*
-
-readvars.rvaudit
-----------------
-
-This file is available from standard EnergyPlus runs (batch file, EP-Launch, etc) where the included utility “ReadVarsESO� is used to create .csv or other delimited files. It shows what steps were taken during the read vars run(s) – in standard EnergyPlus runs there are two: one for the .eso file and one for the .mtr file. Contents might be:
-
-Mon 04/02/2007 19:34:17.09 ReadVars
-
- ReadVarsESO
-
- processing:eplusout.inp
-
- input file:eplusout.eso
-
- output file:eplusout.csv
-
- found/finding:
-
-     1 Outdoor Dry Bulb
-
-     6 Zone/Sys Air Temperature
-
-     6 Zone/Sys Sensible Cooling Rate
-
-     6 Zone/Sys Sensible Heating Rate
-
-     6 Total Water Heating Coil Rate
-
-     1 Total Water Cooling Coil Rate
-
-     1 Sensible Water Cooling Coil Rate
-
-     2 Plant Loop Cooling Demand
-
-     2 Plant Loop Heating Demand
-
-     1 Boiler Gas Consumption Rate
-
-     1 Boiler Heating Output Rate
-
-     1 Chiller Electric Power
-
-     1 Chiller Evap Heat Trans Rate
-
-     1 Chiller Evap Water Inlet Temp
-
-     1 Chiller Evap Water Outlet Temp
-
-     1 Chiller Evap Water Mass Flow Rate
-
-     1 Chiller Cond Heat Trans Rate
-
-     0 Chiller Cond Water Inlet Temp
-
-     0 Chiller Cond Water Outlet Temp
-
-     0 Chiller Cond Water Mass Flow Rate
-
-     2 Pump Mass Flow Rate
-
-     2 Pump Outlet Temp
-
- ReadVars Run Time=00hr 00min  1.78sec
-
- ReadVarsESO program completed successfully.
-
- ReadVarsESO
-
- processing:test.mvi
-
- input file:eplusout.mtr
-
- output file:eplusmtr.csv
-
- getting all vars from:eplusout.mtr
-
- ReadVars Run Time=00hr 00min  0.00sec
-
- ReadVarsESO program completed successfully.
-
-eplusout.svg
-------------
-
-This is a Scalable Vector Graphics (SVG) file that shows a diagram of the HVAC system from the inputs of the simulation. The diagram is generated for most HVAC systems but a few valid HVAC configurations cannot be displayed correctly. The SVG file is generated by the HVAC Diagram utility that is included with EnergyPlus and is run automatically when using EP-Launch.
-
-The SVG format is a graphics format that includes a descriptions of lines, boxes, text, etc. set in a two dimensional perspective. To learn more about the SVG format see:
-
-http://www.w3.org/Graphics/SVG/
-
-Several viewers are available so that you can view these files including plug-ins for Internet Explorer by Adobe and Corel. The Adobe SVG plug in can be found at:
-
-http://www.adobe.com/svg/viewer/install/
-
-But many different viewers are available and links are shown at:
-
-http://www.svgi.org/
-
-An example of a diagram generated by HVAC Diagram is shown
-
-
-
-![](media/image023.jpg)
-
-A close up of one part of this diagram is shown below
-
-![](media/image024.jpg)
-
-The SVG file format is an XML based format so it is text based. The diagram shown above is shown below in text (reduced).
-
-&lt;?xml version="1.0" standalone="no"?&gt;
-
-&lt;!DOCTYPE svg&gt;
-
-&lt;svg width="250mm" height="200mm" viewBox="0 0   3200    1500" xmlns:ev="http://www.w3.org/2001/xml-events" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" preserveAspectRatio="xMidYMid meet" zoomAndPan="magnify"&gt;
-
-&lt;g font-family="Verdana" font-size="8"&gt;
-
-  &lt;line x1="  2400" y1="   470" x2="  2100" y2="    30" style="stroke:linen ;"/&gt;
-
-  &lt;line x1="  2400" y1="   510" x2="  2100" y2="    70" style="stroke:linen ;"/&gt;
-
-  &lt;line x1="  2400" y1="   550" x2="  2100" y2="   110" style="stroke:linen ;"/&gt;
-
-  &lt;line x1="  2400" y1="   590" x2="  2100" y2="   150" style="stroke:linen ;"/&gt;
-
-  &lt;line x1="  2400" y1="   630" x2="  2100" y2="   190" style="stroke:linen ;"/&gt;
-
-  &lt;line x1="  2400" y1="   670" x2="   900" y2="    30" style="stroke:linen ;"/&gt;
-
-  &lt;line x1="  2050" y1="   830" x2="   600" y2="    30" style="stroke:linen ;"/&gt;
-
-  &lt;line x1="   300" y1="    30" x2="   550" y2="   950" style="stroke:linen ;"/&gt;
-
-  &lt;line x1="   800" y1="   790" x2="  2050" y2="   310" style="stroke:linen ;"/&gt;
-
-  &lt;rect x="   200" y="   940" width="   200" height="    20" style="fill:snow; stroke: Black;"/&gt;     1
-
-  &lt;text x="   202" y="   953" startOffset="0"&gt;OUTSIDE AIR INLET NODE LIST&lt;/text&gt;
-
-  &lt;rect x="  2300" y="    20" width="   200" height="    20" style="fill:chartreuse; stroke: Black;"/&gt;     2
-
-  &lt;text x="  2302" y="    33" startOffset="0"&gt;ZN1\_S\_SPACE\_1&lt;/text&gt;
-
-  &lt;rect x="  1400" y="    20" width="   200" height="    20" style="fill:wheat; stroke: Black;"/&gt;     7
-
-  &lt;text x="  1402" y="    33" startOffset="0"&gt;VAV SYS 1 ZONE SPLITTER&lt;/text&gt;
-
-  &lt;rect x="  1700" y="    20" width="   200" height="    20" style="fill:wheat; stroke: Black;"/&gt;     8
-
-  &lt;text x="  1702" y="    33" startOffset="0"&gt;ZN1\_S\_SPACE\_1 VAV REHEAT&lt;/text&gt;
-
-&lt;reduced&gt;
-
-  &lt;line x1="  1600" y1="    30" x2="  1700" y2="    30" style="stroke: Black;"/&gt;
-
-  &lt;line x1="  1600" y1="    30" x2="  1700" y2="    70" style="stroke: Black;"/&gt;
-
-  &lt;line x1="  1600" y1="    30" x2="  1700" y2="   110" style="stroke: Black;"/&gt;
-
-  &lt;line x1="  1600" y1="    30" x2="  1700" y2="   150" style="stroke: Black;"/&gt;
-
-  &lt;line x1="  1600" y1="    30" x2="  1700" y2="   190" style="stroke: Black;"/&gt;
-
-  &lt;line x1="  1900" y1="    30" x2="  2000" y2="    30" style="stroke: Black;"/&gt;
-
-  &lt;line x1="  1900" y1="    70" x2="  2000" y2="    70" style="stroke: Black;"/&gt;
-
-  &lt;line x1="  1900" y1="   110" x2="  2000" y2="   110" style="stroke: Black;"/&gt;
-
-&lt;reduced&gt;
-
-  &lt;text x="   200" y="  1000" startOffset="0"&gt;Unused Non-Parent Objects:&lt;/text&gt;
-
-  &lt;text x="   220" y="  1020" startOffset="0"&gt;VAV SYS 1 SUPPLY AIR TEMP MANAGER&lt;/text&gt;
-
-  &lt;text x="   220" y="  1040" startOffset="0"&gt;VAV SYS 1 HEATING COIL AIR TEMP MANAGER&lt;/text&gt;
-
-  &lt;text x="   220" y="  1060" startOffset="0"&gt;CHILLER PLANT CHW TEMP MANAGER&lt;/text&gt;
-
-  &lt;text x="   220" y="  1080" startOffset="0"&gt;BOILER PLANT HW TEMP MANAGER&lt;/text&gt;
-
-  &lt;text x="   220" y="  1100" startOffset="0"&gt;VAV SYS 1 COOLING COIL AIR TEMP MANAGER&lt;/text&gt;
-
-  &lt;text x="   220" y="  1120" startOffset="0"&gt;VAV SYS 1 MIXED AIR TEMP MANAGER&lt;/text&gt;
-
-  &lt;text x="   220" y="  1140" startOffset="0"&gt;VAV SYS 1 COOLING COIL CONTROLLER&lt;/text&gt;
-
-  &lt;text x="   220" y="  1160" startOffset="0"&gt;VAV SYS 1 HEATING COIL CONTROLLER&lt;/text&gt;
-
-  &lt;text x="   220" y="  1180" startOffset="0"&gt;VAV SYS 1 OA CONTROLLER&lt;/text&gt;
-
-  &lt;text x="   200" y="  1220" startOffset="0"&gt;
-
-The following are not supported:  objects related to controls, DIRECT AIR, or  PURCHASED AIR&lt;/text&gt;
-
-&lt;/g&gt;
-
-&lt;/svg&gt;
-
-
-
-eplusout.sci
-------------
-
-This is the surface cost information report. This report file is obtained by including the following in the input file:
-
-**Output:Surfaces:List, CostInfo;**
-
-The intent is to make available a separate file that lists the unique surfaces and their construction types for potential use in external calculations that need to estimate the cost of construction. Note that such cost estimating can now also be performed internal to EnergyPlus using Cost Estimate objects. The listing can also be used to check that the input for surfaces is producing the expected areas (although the DXF is probably more useful for such checking).
-
-The output file contains a list of the unique surfaces and their net and gross areas. The area information is calculated by EnergyPlus from the vertices entered for individual surfaces. The net area is the area remaining after the areas of subsurfaces are subtracted. The file contains six columns of comma-separate-data as shown in the following table:
-
-
-
-<table class="table table-striped">
-<tr>
-<th>Column</th>
-<th>Description</th>
-</tr>
-<tr>
-<td>1</td>
-<td>Integer counter for surfaces. The surfaces are listed in the order that they are stored internally in EnergyPlus. Note that in this report, the algorithms sort out and exclude duplicate surfaces that are entered for the interior partitions between adjacent thermal zones. Therefore the list is usually not consecutive.</td>
-</tr>
-<tr>
-<td>2</td>
-<td>The name of the surface entered by the user</td>
-</tr>
-<tr>
-<td>3</td>
-<td>The name of the construction for the surface entered by the user</td>
-</tr>
-<tr>
-<td>4</td>
-<td>The type of the surface (e.g. wall, roof, floor, window …)</td>
-</tr>
-<tr>
-<td>5</td>
-<td>The net area of the surface in m<sup>2</sup></td>
-</tr>
-<tr>
-<td>6</td>
-<td>The gross area of the surface in m<sup>2</sup></td>
-</tr>
-</table>
-
-eplusout.wrl
-------------
-
-The VRML output report file is formatted according to the “Virtual Reality Modeling Language� standard rules for representing building type surfaces. The file can be used in several inexpensive, shareware or freeware viewers. There are a variety of stand alone and viewers integrated within browsers. A good list of viewers can be found at:
-
-http://cic.nist.gov/vrml/vbdetect.html
-
-This site detects what, if any, VRML plugin is installed in your browser as well as gives a list of active ones with links to their sites.
-
-This file is generated when the following line is included in the IDF.
-
-**Output:Surfaces:Drawing, VRML;**
-
-In addition, like the DXF output, you can ask it to triangulate (algorithm within EnergyPlus) surfaces with &gt;4 sides:
-
-**Output:Surfaces:Drawing, VRML, Triangulate 3dface;**
-
-Most viewers will illustrate a solid model by default:
-
-![5zone](media/image025.jpg)
-
-Figure 10. VRML output - solid model
-
-With some/many viewers, you can also see a wireframe model; some will even fill this model. Also, viewers can triangulate any surface that isn’t labeled as “convex� by the software writing the file (i.e. EnergyPlus). However, this triangulation may not be correct so you may wish to do it from within EnergyPlus as illustrated above.
-
-A wireframe model of the same building as above is:
-
-![5zonewire](media/image026.jpg)
-
-Figure 11. VRML output - wireframe model
-
-The actual file produced is a text file. EnergyPlus adds some comments, such as the list of zone names and surface names before each coordinate specification. The line/solid colors are set as Floor, Wall, etc. so the file is somewhat readable.
-
-```
-#VRML V2.0 utf8
-WorldInfo {
-   title "Building - Building"
-   info ["EnergyPlus Program Version EnergyPlus <version>, 9/14/2006 1:31 PM"]
-}
-# Zone Names
-# Zone=1:PLENUM-1
-# Zone=2:SPACE1-1
-# Zone=3:SPACE2-1
-# Zone=4:SPACE3-1
-# Zone=5:SPACE4-1
-# Zone=6:SPACE5-1
-Shape {
-appearance DEF FLOOR Appearance {
-material Material { diffuseColor 0.502 0.502 0.502 }
-}
-}
-```
-
-```
-# PLENUM-1:WALL-1PF
-Shape {
-appearance USE WALL
-geometry IndexedFaceSet {
-solid TRUE
-coord DEF Surf5 Coordinate {
-point [
-        0.00000         0.00000         3.00000,
-        0.00000         0.00000         2.40000,
-       26.41377       -15.25000         2.40000,
-       26.41377       -15.25000         3.00000,
-]
-}
-coordIndex [
- 0 1 2 3 -1
-]
-ccw TRUE
-solid TRUE
-}
-}
-```
-
-```
-# PLENUM-1:WALL-1PR
-Shape {
-appearance USE WALL
-geometry IndexedFaceSet {
-solid TRUE
-coord DEF Surf6 Coordinate {
-point [
-       26.41377       -15.25000         3.00000,
-       26.41377       -15.25000         2.40000,
-       34.01377        -2.08641         2.40000,
-       34.01377        -2.08641         3.00000,
-]
-}
-coordIndex [
- 0 1 2 3 -1
-]
-ccw TRUE
-solid TRUE
-}
-}
-```
-
-Delight output files
---------------------
-
-### eplusout.delightin
-
-Following completion of an EnergyPlus run that includes Daylighting:DElight objects, an ASCII text file created during the run is given a file name that consists of the project name appended with DElight.in (e.g., MyProjectDElight.in).
-
-This text file is a formatted DElight input file that was created from the EnergyPlus input data relevant to a DElight simulation. This file can be manually reviewed to determine the exact data that were transformed from EnergyPlus into DElight input.
-
-### eplusout.delightout
-
-Following completion of an EnergyPlus run that includes Daylighting:DElight objects, an ASCII text file created during the run is given a file name that consists of the project name appended with DElight.out (e.g., MyProjectDElight.out).
-
-This text file is a formatted DElight output file that was generated by the DElight simulation engine following the pre-processing daylight factors calculation. This file can be manually reviewed to see the results of these calculations. The file contains an echo of DElight input data, as well as the results of intermediate calculations such as geometrical transformations, surface gridding, and daylight factors, including the following.
-
-**Surface Data**
-
-- Vertex coordinates in the Building coordinate system. Search for the string “BldgSystem\_Surface\_Vertices� within the output file.
-
-- Exterior face luminance values under overcast skies, and for each sun position under clear skies. Search for the string “Surface Exterior Luminance� within the output file.
-
-- Common data for radiosity nodal patches for each surface including Area and Number of Nodes. Search for the string “Surface\_Node\_Area� within the output file.
-
-- Individual data for radiosity nodal patches for each node on each surface including: building coordinate system coordinates; direct and total luminance values under overcast skies, and for each sun position under clear skies. Search for the string “BldgSystem\_Node\_Coordinates� within the output file.
-
-**Reference Point Data**
-
-- Illuminance values from the daylighting factors preprocessor for overcast skies, and for each sun position under clear skies.
-
-- Daylight Factor values from the daylighting factors preprocessor for overcast skies, and for each sun position under clear skies.
-
-- NOTE: The Monthly Average data for Daylight Illuminances and Electric Lighting Reduction will all be zero since these data are not calculated as part of the pre-processing done by the point at which this output file is generated for EnergyPlus.
-
-Example Input Files
-===================
-
-The EnergyPlus install includes a sample of example input files. For the most part, the developers create these files to illustrate and test a specific feature in EnergyPlus. Then, we pass them along to you for illustrative purposes. The install contains two spreadsheet files related to the example files:
-
-- **ExampleFiles.xls** - lists all the files available – whether through the install or through an external site.
-
-- **ExampleFiles-ObjectLink.xls** - illustrates the first 3 occurances in the example files of an object.
-
-Following convention, each example file should have at the top a set of comments that tell what the purpose of the file is and the key features.
-
-For example, the file titled “5ZoneAirCooled.idf� has:
-
-```idf
-! 5ZoneAirCooled.idf
-! Basic file description:  1 story building divided into 4 exterior and one interior conditioned zones and return plenum.
-!
-! Highlights:              Electric chiller with air cooled condenser; autosized preheating and precooling water coils in the
-!                          outside air stream controlled to preheat and precool setpoints.
-!
-! Simulation Location/Run: CHICAGO_IL_USA TMY2-94846, 2 design days, 2 run periods,
-!                          Run Control executes the run periods using the weather file
-!
-! Location:                Chicago, IL
-!
-! Design Days:             CHICAGO_IL_USA Annual Heating 99% Design Conditions DB, MaxDB= -17.3°C
-!                          CHICAGO_IL_USA Annual Cooling 1% Design Conditions, MaxDB=  31.5°C MCWB=  23.0°C
-!
-! Run Period (Weather File): Winter 1/14, Summer 7/7, CHICAGO_IL_USA TMY2-94846
-!
-! Run Control:             Zone and System sizing with weather file run control (no design days run)
-!
-! Building: Single floor rectangular building 100 ft x 50 ft. 5 zones - 4 exterior, 1 interior, zone height 8 feet.
-!           Exterior zone depth is 12 feet. There is a 2 foot high return plenum: the overall building height is
-!           10 feet. There are windows on all 4 facades; the south and north facades have glass doors.
-!           The south facing glass is shaded by overhangs. The walls are woodshingle over plywood, R11 insulation,
-!           and gypboard. The roof is a gravel built up roof with R-3 mineral board insulation and plywood sheathing.
-!           The windows are of various single and double pane construction with 3mm and 6mm glass and either 6mm or
-!           13mm argon or air gap. The window to wall ratio is approxomately 0.29.
-!           The south wall and door have overhangs.
-!
-!           The building is oriented 30 degrees east of north.
-!
-
-
-! Floor Area:        463.6 m2 (5000 ft2)
-! Number of Stories: 1
-!
-! Zone Description Details:
-!
-!      (0,15.2,0)                      (30.5,15.2,0)
-!           _____   ________                ____
-!         |\     ***        ****************   /|
-!         | \                                 / |
-!         |  \                 (26.8,11.6,0) /  |
-!         *   \_____________________________/   *
-!         *    |(3.7,11.6,0)               |    *
-!         *    |                           |    *
-!         *    |                           |    *
-!         *    |               (26.8,3.7,0)|    *
-!         *    |___________________________|    *
-!         *   / (3.7,3.7,0)                 \   *
-!         |  /                               \  |
-!         | /                                 \ |
-!         |/___******************___***________\|
-!          |       Overhang        |   |
-!          |_______________________|   |   window/door = *
-!                                  |___|
-!
-!      (0,0,0)                            (30.5,0,0)
-!
-! Internal gains description:     lighting is 1.5 watts/ft2, office equip is 1.0 watts/ft2. There is 1 occupant
-!                                 per 100 ft2 of floor area. The infiltration is 0.25 air changes per hour.
-!
-! Interzone Surfaces:             6 interzone surfaces (see diagram)
-! Internal Mass:                  None
-! People:                         50
-! Lights:                         7500 W
-! Windows:                        4 ea.: 1) Double pane clear, 3mm glass, 13mm air gap
-!                                        2) Double pane clear, 3mm glass, 13mm argon gap
-!                                        3) Double pane clear, 6mm glass, 6mm air gap
-!                                        4) Double pane lowE,  6mm lowE glass outside, 6mm air gap, 6mm clear glass
-!
-! Doors:                          2 ea.:    Single pane grey,  3mm glass
-!
-! Detached Shading:               None
-! Daylight:                       None
-! Natural Ventilation:            None
-! Compact Schedules:              Yes
-!
-! HVAC:                           Standard VAV system with outside air, hot water reheat coils,
-!                                 central chilled water cooling coil. Central Plant is single hot water
-!                                 boiler, electric compression chiller with air cooled condenser.
-!                                 All equipment is autosized. HW and ChW coils are used in the outside air
-!                                 stream to precondition the outside air.
-!
-! Zonal Equipment:                AirTerminal:SingleDuct:VAV:Reheat
-! Central Air Handling Equipment: Yes
-! System Equipment Autosize:      Yes
-! Purchased Cooling:              None
-! Purchased Heating:              None
-! Coils:                          Coil:Cooling:Water, Coil:Heating:Water
-! Pumps:                          Pump:VariableSpeed
-! Boilers:                        Boiler:HotWater
-! Chillers:                       Chiller:Electric
-!
-! Results:
-! Standard Reports:               None
-! Timestep or Hourly Variables:   Hourly
-! Time bins Report:               None
-! HTML Report:                    None
-! Environmental Emissions:        None
-! Utility Tariffs:                None
-```
-
-
-In addition to the idf files, usually an .rvi and perhaps a .mvi of the same file set is included. As discussed previously, the .rvi is used with the ReadVarsESO post-processing program and the .eso file to create a .csv file which can be read easily into Excel™. Like the .rvi, the .mvi file can be used with the .mtr file to create a similar version for “metered� outputs.
-
-Data Sets
-=========
-
-Data sets are the EnergyPlus answer to “libraries�. Data sets come in two flavors – a simple list and a “macroized� list. Macroized lists are files that could have the elements extracted using a simple macro name.
-
-Simple List Data Sets
----------------------
-
-### AirCooledChillers.idf
-
-This dataset includes performance curves for air cooled electric EIR chiller (object type: Chiller:Electric:EIR). Knowing the type of chiller that you want to simulate, you can find it and the associated performance curves in the dataset file. A brief synopsis of AirCooledChiller.idf is shown below:
-
-```idf
-! AirCooledChillers.idf
-!
-! This dataset includes performance curves for object type Chiller:Electric:EIR
-!
-! Summary Table for Electric EIR Chiller reference data sets.
-! Chillers are listed in order of reference capacity. Reference capacity and COP do not necessarily
-! indicate rated capacity and COP at standard rating conditions (e.g. ARI Standard 550/590).
-!
-! Performance curves developed from information collected from manufacturer's catalog data
-! The nomenclature used for the chiller is as follows:
-! ElectricEIRChiller - Manufacturer's Name - Model - Reference Capacity in kW - Reference COP
-!
-!                                                      Compressor   Reference    Reference
-! Chiller Name                                            Type       Capacity      COP
-!                                                                    kW (tons)
-! ElectricEIRChiller McQuay AGZ010BS 34.5kW/2.67COP      Scroll     34.5 (9.8)      2.67
-! ElectricEIRChiller McQuay AGZ013BS 47.1kW/2.67COP      Scroll     47.1 (13.4)     2.67
-! ElectricEIRChiller York YCAL0019EE 54.2kW/2.9COP       Scroll     54.2 (15.4)     2.9
-! ElectricEIRChiller McQuay AGZ017BS 54.5kW/2.67COP      Scroll     54.5 (15.5)     2.67
-
-```
-
-
-
-### ASHRAE\_2005\_HOF\_Materials.idf
-
-This reference data set contains content from two chapters in the ASHRAE 2005 Handbook of Fundamentals, Chapter 30 - the Cooling and Heating Loads calculations chapter has both materials with thermal properties and constructions for Light, Medium, and Heavy buildings. Chapter 25 contains details thermal properties of many materials -- no constructions are created from that data.
-
-The following materials and constructions are created from ASHRAE Handbook of Fundamentals, 2005, Chapter 30, Table 19 and Table 22. These are representative of materials and constructions used in Cooling and Heating Load Calculations.
-
-### Boilers.idf
-
-This dataset includes performance curves for non-electric boilers. Reference: Condensing Technology, Technical Series, Viessmann, 9446 803 - 1 GB Nov. 2004.
-
-### California\_Title\_24-2008.idf
-
-This dataset includes occupancy data and non-residential schedules for California Title 24-2008 compliance calculations when lighting plans are submitted for the Entire Building or when lighting compliance is not performed. Data is based on Table N2-5 of the 2008 Non-residential ACM Manual.
-
-### Chillers.idf
-
-This dataset includes object types for specific (by manufacturer and type) Chiller:Electric:EIR and Chiller: Electric:ReformulatedEIR and associated performance curves.
-
-Knowing the type of chiller that you want to simulate, you can find it and the associated performance curves in the dataset file. By example, here is part of the comments in the Chiller.idf file:
-
-```idf
-! Summary Table for Electric EIR Chiller reference data sets (Ref. CoolTools project).
-! Chillers are listed in order of compressor type and reference capacity (model calibration
-! point). Reference capacity and COP do not necessarily indicate rated capacity and COP at
-! standard rating conditions (e.g. ARI Standard 550/590).
-!
-! Performance curves developed from information collected over a 10-year period from 1991 to 2001.
-!
-!                                                      Compressor   Reference  Reference Unloading
-! Chiller Name                                            Type       Capacity    COP     Mechanism
-!                                                                    kW (tons)
-!-------------------------------------------------------------------------------------------------
-! ElectricEIRChiller McQuay WSC 471kW/5.89COP/Vanes    Centrifugal   471 (134)   5.89   Inlet Vanes
-! ElectricEIRChiller York YT 563kW/10.61COP/Vanes      Centrifugal   563 (160)   10.61  Inlet Vanes
-! ElectricEIRChiller McQuay PEH 703kW/7.03COP/Vanes    Centrifugal   703 (200)   7.03   Inlet Vanes
-! ElectricEIRChiller Carrier 23XL 724kW/6.04COP/Vanes  Centrifugal   724 (206)   6.04   Inlet Vanes
-```
-
-
-### CompositeWallConstructions.idf
-
-The Reference Data Set CompositeWallConstructions.idf contains constructions and associated materials for a set of **composite** walls. These are walls—such as stud walls—that have complicated heat-flow paths so that the conduction is two- or three-dimensional.
-
-An example entry in this data set--for an insulated 2�x4� steel-stud wall--looks like:
-
-```idf
-CONSTRUCTION,Composite 2x4 Steel Stud R11,
-! ASHRAE 1145-RP Wall Assembly 10
-! 2"x4" steel studs at 24" on center with between-stud R11 fibreglass insulation.
-! Studs are 3.5", 16 gauge, 15 flange.
-! Layers are 1/2" wood siding, 1/2" plywood, 2x4 steel studs and R11 insulation, 1/2" gypsum board.
-! Area-average R-Value = 8.796 ft2-F-h/Btu (1.548 m2-K/W).
-! Total wall thickness = 5.00in (0.127m)
-! Material layer names follow:
-  Composite 2x4 Steel Stud R11 \#3,
-  Composite 2x4 Steel Stud R11 \#2,
-  Composite 2x4 Steel Stud R11 \#1;
-MATERIAL,Composite 2x4 Steel Stud R11 \#1,
-  Smooth,  !- Roughness
-  0.013,   !- Thickness (m)
-  0.720,   !- Conductivity (W/m-K)
-  640.0,   !- Density (kg/m3)
-  1048,    !- Specific Heat (J/kg-K)
-  0.9,     !- Absorptance:Thermal
-  0.7,     !- Absorptance:Solar
-  0.7;     !- Absorptance:Visible
-MATERIAL,Composite 2x4 Steel Stud R11 \#2,
-  Smooth,  !- Roughness
-  0.089,   !- Thickness (m)
-  0.060,   !- Conductivity (W/m-K)
-  118.223, !- Density (kg/m3)
-  1048,    !- Specific Heat (J/kg-K)
-  0.9,     !- Absorptance:Thermal
-  0.7,     !- Absorptance:Solar
-  0.7;     !- Absorptance:Visible
-MATERIAL,Composite 2x4 Steel Stud R11 \#3,
-  Smooth,  !- Roughness
-  0.025,   !- Thickness (m)
-  0.452,   !- Conductivity (W/m-K)
-  413.782, !- Density (kg/m3)
-  1048,    !- Specific Heat (J/kg-K)
-  0.9,     !- Absorptance:Thermal
-  0.7,     !- Absorptance:Solar
-  0.7;     !- Absorptance:Visible
-```
-
-
-The materials here are **not** real materials but are “equivalent� materials obtained from finite-difference modeling. The thickness, conductivity, density and specific heat values of the material layers for the different constructions have been taken from the ASHRAE report “Modeling Two- and Three-Dimensional Heat Transfer through Composite Wall and Roof Assemblies in Hourly Energy Simulation Programs (1145-TRP),� by Enermodal Engineering Limited, Oak Ridge National Laboratory, and the Polish Academy of Sciences, January 2001. EnergyPlus will calculate conduction transfer functions using these materials. The heat transfer based on these conduction transfer functions will then be very close to what would be calculated with a two- or three-dimensional heat transfer calculation.
-
-For stud walls, using these composite constructions will give more accurate heat flow than you would get by manually dividing the wall into a stud section and a non-stud section.
-
-If your wall’s exterior or interior roughness or thermal, solar or visible absorptances are different from those in the data set, you can make the appropriate changes to the first material (the outside layer) or the third material (the inside layer). **None of the other values should be changed.**
-
-Following is a summary of the constructions in the composite wall data set:
-
-```idf
-CONSTRUCTION,Composite 2x4 Wood Stud R11,
-! ASHRAE 1145-RP Wall Assembly 1
-! 2"x4" wood studs at 24" on center with between-stud R11 fibreglass insulation.
-! Layers are 1/2" wood siding, 1/2" plywood, 2x4 wood studs and R11 insulation, 1/2" gypsum board.
-! Area-average R-Value = 11.391 ft2-F-h/Btu (2.005 m2-K/W).
-
-CONSTRUCTION,Composite 2x6 Wood Stud R19,
-! ASHRAE 1145-RP Wall Assembly 2
-! 2"x6" wood studs at 24" on center with between-stud R19 fibreglass insulation.
-! Layers are 1/2" wood siding, 1/2" plywood, 2x6 wood studs and R19 insulation, 1/2" gypsum board.
-! Area-average R-Value = 17.487 ft2-F-h/Btu (3.078 m2-K/W).
-
-CONSTRUCTION,Composite Insulated Concrete Form Wall With Steel Ties,
-! ASHRAE 1145-RP Wall Assembly 7
-! Wall system is made of two rigid insulation sides held together with wire mesh.
-! The two sides come together to create the formwork for the concrete.
-! Layers are 3/4" concrete stucco, outer polystyrene shell, concrete core, inner polystyrene shell.
-! Area-average R-Value = 11.230 ft2-F-h/Btu (1.977 m2-K/W).
-
-CONSTRUCTION,Composite Concrete/Foam/Concrete With Steel Connectors,
-! ASHRAE 1145-RP Wall Assembly 8
-! Wall system is made of two 3" concrete slabs separated by 2" rigid insulation.
-! The slab connectors are steel ties with a 0.15"x0.15" cross section.
-! Layers are 3" concrete, 2" polystyrene, 3" concrete.
-! Area-average R-Value = 7.659 ft2-F-h/Btu (1.348 m2-K/W).
-
-CONSTRUCTION,Composite Concrete/Foam/Concrete With Plastic Connectors,
-! ASHRAE 1145-RP Wall Assembly 9
-! Wall system is made of two 3" concrete slabs separated by 2" rigid insulation.
-! The slab connectors are plasic ties with a 0.25"x0.25" cross section.
-! Layers are 3" concrete, 2" polystyrene, 3" concrete.
-! Area-average R-Value = 10.582 ft2-F-h/Btu (1.862 m2-K/W).
-
-CONSTRUCTION,Composite 2x4 Steel Stud R11,
-! ASHRAE 1145-RP Wall Assembly 10
-! 2"x4" steel studs at 24" on center with between-stud R11 fibreglass insulation.
-! Studs are 3.5", 16 gauge, 15 flange.
-! Layers are 1/2" wood siding, 1/2" plywood, 2x4 steel studs and R11 insulation, 1/2" gypsum board.
-! Area-average R-Value = 8.796 ft2-F-h/Btu (1.548 m2-K/W).
-
-CONSTRUCTION,Composite Brick Foam 2x4 Steel Stud R11,
-! ASHRAE 1145-RP Wall Assembly 15
-! Brick veneer, polystyrene, 2"x4" steel studs at 24" on center with
-!  between-stud R11 fibreglass insulation.
-! Studs are 3.5", 16 gauge, 15 flange.
-! Layers are 3.25" brick,1" polystyrene insulation, 1/2" plywood, 2x4 steel studs and R11 insulation,
-!  1/2" gypsum board.
-! Area-average R-Value = 12.792 ft2-F-h/Btu (2.251 m2-K/W).
-
-CONSTRUCTION,Composite 2x6 Steel Stud R19,
-! ASHRAE 1145-RP Wall Assembly 16
-! 2"x6" steel studs at 24" on center with between-stud R19 fibreglass insulation.
-! Studs are 5.5", 16 gauge, 15 flange.
-! Layers are 1/2" wood siding, 1/2" plywood, 2x6 steel studs and R19 insulation, 1/2" gypsum board.
-! Area-average R-Value = 12.792 ft2-F-h/Btu (1.991 m2-K/W).
-
-CONSTRUCTION,Composite Foam 2x6 Steel Stud R19,
-! ASHRAE 1145-RP Wall Assembly 17
-! Polystyrene, 2"x6" steel studs at 24" on center with between-stud R19 fibreglass insulation.
-! Studs are 5.5", 16 gauge, 15 flange.
-! Layers are 3/4" concrete stucco,1" polystyrene insulation, 1/2" plywood, 2x6 steel studs and R19 insulation,
-!  1/2" gypsum board.
-! Area-average R-Value = 15.157 ft2-F-h/Btu (2.668 m2-K/W).
-
-CONSTRUCTION,Composite Brick Foam 2x6 Steel Stud R19,
-! ASHRAE 1145-RP Wall Assembly 18
-! Brick veneer, polystyrene, 2"x6" steel studs at 24" on center with
-!  between-stud R19 fibreglass insulation.
-! Studs are 5.5", 16 gauge, 15 flange.
-! Layers are 3.25" brick,1" polystyrene insulation, 1/2" plywood, 2x6 steel studs and R19 insulation,
-!  1/2" gypsum board.
-! Area-average R-Value = 15.465 ft2-F-h/Btu (2.722 m2-K/W).
-
-CONSTRUCTION,Composite 2-Core Filled Concrete Block Uninsulated,
-! ASHRAE 1145-RP Wall Assembly 19
-! Wall system is made of 12" 2-core concrete blocks without insulation.
-! The core area is filled with rebar and poured concrete.
-! Area-average R-Value = 1.326 ft2-F-h/Btu (0.239 m2-K/W).
-
-CONSTRUCTION,Composite 2-Core Filled Concrete Block Insulated,
-! ASHRAE 1145-RP Wall Assembly 20
-! Wall system is made of 12" 2-core concrete blocks with 1.875"-thick
-!  foam inserts in the block cores.
-! The remaining core area is filled with poured concrete.
-! Area-average R-Value = 2.291 ft2-F-h/Btu (0.403 m2-K/W).
-```
-
-
-### DXCoolingCoil.idf
-
-This dataset includes performance curves for the object types Coil:Cooling:DX:SingleSpeed and Coil:Cooling:DX:TwoStageWithHumidityControlMode. This data set is developed by using catalog data published by different manufacturers which are listed in the file.
-
-Here is a synopsis of the DXCoolingCoil.idf:
-
-```idf
-! DXCoolingCoil.idf
-!
-! This dataset includes performance curves for the object types Coil:Cooling:DX:SingleSpeed and
-! Coil:Cooling:DX:TwoStageWithHumidityControlMode
-!
-! Reference capacity at standard rating conditions (ARI 95F OAT, 67F EWBT and air flow rate
-! around 400 cfm/Ton).
-!
-! In the objects Coil:Cooling:DX:SingleSpeed and Coil:Cooling:DX:TwoStageWithHumidityControlMode
-! below, input fields 'Availability Schedule Name', 'Air Inlet Node Name' and 'Air Outlet Node
-! Name' need to be defined by the user.
-!
-!------------------------------------------------------------------------------------------------!                             Compressor  Nominal    Reference      Reference   Refrig  Expansion
-!                                                                                         Valve
-! Name                           Type     Capacity   Capacity          COP       Type      Type
-!                                         (tons)     kW (tons)
-!------------------------------------------------------------------------------------------------! Carrier Centurion 50PG06      Scroll      5        18.28(5.2)        4.15     R-410A    TXV
-! Carrier Centurion 50PG12      Scroll      10       36.79(10.47)      4.05     R-410A    TXV
-! Carrier Centurion 50PG24      Scroll      20       73.81(21)         3.95     R-410A    TXV
-
-  Coil:Cooling:DX:SingleSpeed,
-    Carrier Centurion 50PG06,     !- Name
-    CoolingCoilAvailSched,        !- Availability Schedule Name
-    18276.96,                     !- Rated Total Cooling Capacity {W}
-    0.74,                         !- Rated Sensible Heat Ratio
-    4.15,                         !- Rated COP
-    0.944,                        !- Rated Air Flow Rate {m3/s}
-    ,                             !- Rated Evaporator Fan Power Per Volume Flow Rate {W/(m3/s)}
-    DXCoilAirInletNode,           !- Air Inlet Node Name
-    DXCoilAirOutletNode,          !- Air Outlet Node Name
-    CarrierCenturion50PG06CapFT,  !- Total Cooling Capacity Function of Temperature Curve Name
-    CarrierCenturion50PG06CapFFF, !- Total Cooling Capacity Function of Flow Fraction Curve Name
-    CarrierCenturion50PG06EIRFT,       !- Energy Input Ratio Function of Temperature Curve Name
-    CarrierCenturion50PG06EIRFFF,      !- Energy Input Ratio Function of Flow Fraction Curve Name
-    Carrier Centurion 50PG06 PLFFPLR;  !- Part Load Fraction Correlation Curve Name
-
-! Curve set (5 Curves):
-
-! Cooling Capacity Function of Temperature Curve
-! x = Entering Wet-bulb Temp and y = Outdoor Dry-bulb Temp
-
-  Curve:Biquadratic,
-    CarrierCenturion50PG06CapFT,  !- Name
-    0.9953455,               !- Coefficient1 Constant
-    -0.0118418,              !- Coefficient2 x
-    0.0012277,               !- Coefficient3 x**2
-    0.0030246,               !- Coefficient4 y
-    -0.0000702,              !- Coefficient5 y**2
-    -0.0003685,              !- Coefficient6 x*y
-    12.22,                   !- Minimum Value of x
-    26.67,                   !- Maximum Value of x
-    15.56,                   !- Minimum Value of y
-    51.67,                   !- Maximum Value of y
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature,             !- Input Unit Type for Y
-    Dimensionless;           !- Output Unit Type
-
-! EIR Function of Temperature Curve
-! x = Entering Wet-bulb Temp and y = Outdoor Dry-bulb Temp
-
-  Curve:Biquadratic,
-    CarrierCenturion50PG06EIRFT,  !- Name
-    0.3802131,               !- Coefficient1 Constant
-    0.0199468,               !- Coefficient2 x
-    -0.0006682,              !- Coefficient3 x**2
-    0.0058933,               !- Coefficient4 y
-    0.0004646,               !- Coefficient5 y**2
-    -0.0004072,              !- Coefficient6 x*y
-    12.22,                   !- Minimum Value of x
-    26.67,                   !- Maximum Value of x
-    15.56,                   !- Minimum Value of y
-    51.67,                   !- Maximum Value of y
-    ,                        !- Minimum Curve Output
-    ,                        !- Maximum Curve Output
-    Temperature,             !- Input Unit Type for X
-    Temperature,             !- Input Unit Type for Y
-    Dimensionless;           !- Output Unit Type
-
-! Cooling Capacity Function of Flow Fraction Curve
-! x = Flow Fraction
-
-  Curve:Quadratic,
-    CarrierCenturion50PG06CapFFF,  !- Name
-    0.7705358,               !- Coefficient1 Constant
-    0.2848007,               !- Coefficient2 x
-    -0.0580891,              !- Coefficient3 x**2
-    0.75,                    !- Minimum Value of x
-    1.25;                    !- Maximum Value of x
-
-! EIR Function of Flow Fraction Curve
-! x = Flow Fraction
-
-  Curve:Quadratic,
-    CarrierCenturion50PG06EIRFFF,   !- Name
-    1.3439758,               !- Coefficient1 Constant
-    -0.5111244,              !- Coefficient2 x
-    0.1732549,               !- Coefficient3 x**2
-    0.75,                    !- Minimum Value of x
-    1.25;                    !- Maximum Value of x
-
-! Part Load Fraction Function of Part Load Ratio Curve
-! x = Part Load Ratio
-
-  Curve:Quadratic,
-    CarrierCenturion50PG06PLFFPLR,   !- Name
-    0.85,                    !- Coefficient1 Constant
-    0.15,                    !- Coefficient2 x
-    0.0,                     !- Coefficient3 x**2
-    0.0,                     !- Minimum Value of x
-    1.0;                     !- Maximum Value of x
-```
-
-
-### ElectricGenerators.idf
-
-This dataset includes inputs for the GENERATOR:MICROTURBINE object and associated performance curves. The performance curves were developed from manufacturer data collected in Summer 2007.
-
-Includes data for generators: Capstone C65, Elliott TA100,  Ingersoll Rand MT70, Ingersoll Rand MT250.
-
-Further documentation is contained in the dataset file.
-
-### Electricity USA Environmental Impact Factors.idf
-
-United States 1999 national average electricity emissions factors based on eGRID, 1605, AirData. United States Water Emission Fuel Factors are the combined thermoelectric and hydroelectric weighted averages from:
-
-Torcellini, Paul; Long, Nicholas; Judkoff, Ron; "Consumptive Water Use for U.S. Power Production";NREL Report No. TP-550-33905. Golden, CO; 2003; http://www.nrel.gov/docs/fy04osti/33905.pdf;
-
-or
-
-Torcellini, Paul; Long, Nicholas; Judkoff, Ron; "Consumptive Water Use for U.S. Power Production"; ASHRAE Transactions 2003, Vol 110, Part 1. Atlanta, GA; January 2004;
-
-### ElectronicEnthalpyEconomizerCurves.idf
-
-These curves approximate the electronic (variable) enthalpy curves used to simulate humidity biased economizer control. This control scheme adjusts the upper outdoor air humidity ratio based on outdoor air dry-bulb temperature as shown in the figure below. California Title 24 ACM 2005 lists the optional economizer control strategies. One of these control strategies is referred to as variable enthalpy control curve A. This control strategy is also cited in ASHRAE Standard 90.1-2004, using the term “electronic enthalpy�. Electronic enthalpy curves A-D are included in this dataset.
-
-![Schematic\_ElectronicEnthalpyEconomizerControl](media/image027.jpg)
-
-Figure 12. Psychrometric Chart Illustration of the Electronic (Variable) Enthalpy Economizer Limit Example Curve Objects
-
-For the curves provided, curve A has the highest limit and curve D has the lowest limit. These curve objects represent a single-point electronic enthalpy control curve with the curve object’s minimum value of x (temperature) crossing the psychrometric chart's saturation line and the curve object’s maximum value of x crossing the psychrometric chart's dry-bulb temperature axis. The curve object’s minimum (maximum) value of x should be just low (high) enough to ensure that the curve crosses the psychrometric chart’s saturation line (temperature axis). The curves are evaluated at an outdoor dry-bulb temperature to provide a maximum operating outdoor humidity ratio for economizer operation. If the outdoor humidity ratio is greater than this maximum value, economizer operation is terminated. These curves may be used with other economizer limits to create multi-point economizer control (Temperature Limit, Temperature Low Limit, Enthalpy Limit, and Dewpoint Temperature Limit).
-
-#### Form of the Electronic Enthalpy Curve Equation:
-
-The electronic enthalpy curve equation represents a unique curve and is a function of both temperature and relative humidity. The equation is set equal to a constant which provides a unique temperature for each relative humidity entered into the equation. Each control curve has a unique constant as shown in the table below. Other constants may be used to develop specialized electronic enthalpy curves.
-
-<div>\[ K = 45.672192 - 1.1559942 \cdot T - 0.144599 \cdot RH \]</div>
-
-where:
-
-* K  = Constant value to represent specific curve
-* T  = Outdoor Dry-Bulb Temperature (C)
-* RH = Outdoor Relative Humidity (%)
-
-
-NOTE:  modifying the RH multiplier (-0.144599) tends to "wag" the curvature at the upper relative humidities. Decreasing the multiplier "wags" the upper portion of the curve downward, increasing "wags" it upwards. Modifying the constant (K) moves the intersection of the curve with the Dry-Bulb Temperature  axis. Increasing the constant moves the intersection to the left as shown in the figure, decreasing moves to the right. The minimum and/or maximum x boundaries in the curve objects may have to be adjusted when modifying the equation.
-
-Table 43. Electronic Enthalpy Curve Constants and approximate control point at 50% RH
-
-<table class="table table-striped">
-<tr>
-<th>Control Curve</th>
-<th>Curve Constant K</th>
-<th>Approximate Control Point at 50% RH (ºC)</th>
-</tr>
-<tr>
-<td>A</td>
-<td>12</td>
-<td>22.9</td>
-</tr>
-<tr>
-<td>B</td>
-<td>14</td>
-<td>21.1</td>
-</tr>
-<tr>
-<td>C</td>
-<td>16</td>
-<td>19.4</td>
-</tr>
-<tr>
-<td>D</td>
-<td>18</td>
-<td>17.7</td>
-</tr>
-</table>
-
-
-
-#### Example Curve A:
-
-The method described here was used to create each of the four "cubic" curve objects provided in the electronic enthalpy economizer control data set.
-
-**Step 1:** Substitute the curve constant K for curve A (12) into the electronic enthalpy curve equation and solve for temperature. Then identify the outdoor air dry-bulb temperatures at known values of relative humidity (e.g., columns 1 and 2 in the table below). Psychrometric routines are helpful for this step.
-
-<div>\[ \text{Temperature} = \frac{12 - 45.672192 + 0.144599 \cdot \text{RelativeHumidity}}{-1.1559942} \]</div>
-
-**Step 2:** Identify humidity ratio at each point (e.g. column 3 in the following table). Psychrometric routines are helpful for this step.
-
-<table class="table table-striped">
-<tr>
-<th>Relative Humidity (%)</th>
-<th>Temperature (ºC)</th>
-<th>Calculated Humidity Ratio (kg/kg)</th>
-</tr>
-<tr>
-<td>0</td>
-<td>29.128</td>
-<td>0.00000</td>
-</tr>
-<tr>
-<td>10</td>
-<td>27.877</td>
-<td>0.00232</td>
-</tr>
-<tr>
-<td>20</td>
-<td>26.627</td>
-<td>0.00433</td>
-</tr>
-<tr>
-<td>30</td>
-<td>25.376</td>
-<td>0.00605</td>
-</tr>
-<tr>
-<td>40</td>
-<td>24.125</td>
-<td>0.00750</td>
-</tr>
-<tr>
-<td>50</td>
-<td>22.874</td>
-<td>0.00872</td>
-</tr>
-<tr>
-<td>60</td>
-<td>21.623</td>
-<td>0.00971</td>
-</tr>
-<tr>
-<td>70</td>
-<td>20.372</td>
-<td>0.01051</td>
-</tr>
-<tr>
-<td>80</td>
-<td>19.121</td>
-<td>0.01112</td>
-</tr>
-<tr>
-<td>90</td>
-<td>17.871</td>
-<td>0.01158</td>
-</tr>
-<tr>
-<td>100</td>
-<td>16.620</td>
-<td>0.01189</td>
-</tr>
-</table>
-
-** **
-
-**Step 3:** Use multiple linear regression to solve one of the following equations:
-
-*Quadratic  Curve*: Humidity Ratio = A0 + A1\*Temperature + A2\*Temperature<sup>2</sup>
-
-*Cubic  Curve*: Humidity Ratio = A0 + A1\*Temperature + A2\*Temperature<sup>2</sup> + A3\*Temperature<sup>3</sup>
-
-**Step 4:** Use the coefficients calculated in the multiple linear regression to create a cubic (or quadratic) curve object.
-
-### Exhaust Fired Chiller.idf
-
-This dataset includes the curves for exhaust fired absorption chiller.
-
-1)   Cooling Capacity Function of Temperature Curve
-
-2)   Thermal Energy Input to Cooling Output Ratio Function of Temperature Curve
-
-3)   Thermal Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve
-
-### Fossil Fuel Environmental Impact Factors.idf
-
-Impact factors for environmental reporting. References for each fuel are given in the dataset.
-
-### FluidPropertiesRefData.idf
-
-This data set includes fluid properties reference data. Fluid properties for R404a, R407a, R410a, R505a, R744, were developed using the NIST Standard Reference Database 23, NIST Reference Thermodynamic and Transport Properties – REFPROP, April 2007 Version 8.0, National Institute of Standards and Technology, 2007. The other refrigerants were developed using older versions of the NIST Standard Reference Database. The entire data set includes:
-
-<table class="table table-striped">
-<tr>
-<th>Refrigerants</th>
-</tr>
-<tr>
-<td>R11</td>
-</tr>
-<tr>
-<td>R12</td>
-</tr>
-<tr>
-<td>R22</td>
-</tr>
-<tr>
-<td>R123</td>
-</tr>
-<tr>
-<td>R134a</td>
-</tr>
-<tr>
-<td>R404a</td>
-</tr>
-<tr>
-<td>R410a</td>
-</tr>
-<tr>
-<td>R507a</td>
-</tr>
-<tr>
-<td>NH3</td>
-</tr>
-<tr>
-<td>Steam</td>
-</tr>
-<tr>
-<td>R744</td>
-</tr>
-</table>
-
-To use the data, copy the appropriate data for the refrigerant you desire into your input file.
-
-### GlycolPropertiesRefData.idf
-
-This data set includes fluid properties (glycol) reference data. Reference for the data is the ASHRAE Handbook of Fundamentals. Included are:
-
-<table class="table table-striped">
-<tr>
-<th>Glycols</th>
-</tr>
-<tr>
-<td>EthyleneGlycol</td>
-</tr>
-<tr>
-<td>PropyleneGlycol</td>
-</tr>
-<tr>
-<td>Water</td>
-</tr>
-</table>
-
-To use the data, copy the appropriate data for the glycol you desire into your input file.
-
-### GHLERefData.idf
-
-This file contains sample input for the ground loop heat exchanger model. The response of the borehole/ground is found from the 'G-function' that is  defined in the input as series of 'n' pairs of values (LNTTSn, GNFCn). It is important to note that the G-functions have to be calculated for specific GHE configurations and borehole resitance, length and borehole/ length ratio. That is, the parameters for the units vary with each design. The data in this file are intended as examples/samples and may not represent actual designs.
-
-The sample data has been calculated for a number of configurations:
-
-* 1 x 2 boreholes
-* 4 x 4 boreholes
-* 8 x 8 boreholes
-
-Data is given for both 'standard' grout (k=0.744 W/m.K) and 'thermally enhanced' grout (k= 1.471 W/m.K). The flow rate per borehole is .1514 kg/s. The pipe given is 0.75in. Dia. SDR11 HDPE. The fluid is water. The borehole/length ratio is 0.06  (76.2m/4.572m [300ft/15ft])
-
-### MoistureMaterials.idf
-
-This data set includes the special moisture materials that can be used with the Moisture Penetration Depth Conduction Transfer Function (EMPD) and Combined Heat and Moisture Finite Element (HAMT) calculation procedures.
-
-### PerfCurves.idf
-
-This file contains performance curves for various EnergyPlus equipment objects.
-
-- Variable speed DX cooling:  These curves are appropriate for small DX cooling units with variable speed compressors. These curves would be referenced by the EnergyPlus object Coil:Cooling:DX:TwoSpeed. See the example input file 5ZoneAutoDXVAV for an example of their use.
-
-- Variable Speed Cooling Tower: These model coefficient objects are appropriate for use with the variable speed cooling tower object and represent the coefficients used in the YorkCalc and CoolTools empirical models. These model coefficient objects would be referenced by the EnergyPlus object Cooling Tower:Variable Speed. See the example input file CoolingTower\_VariableSpeed.idf for an example of where these curves could be used (these model coefficient objects are not specifically used in this idf but could be used by the Cooling Tower:Variable Speed object). Additional information on variable speed cooling tower model coefficients can be found in the Input Output Reference and Engineering Reference documents.
-
-- Note that performance curves for the Electric EIR chiller and the Electric Reformulated EIR chiller are contained in the Chillers.idf dataset.
-
-### PrecipitationSchedulesUSA.idf
-
-This file contains schedules (for an entire year) of precipitation for use with the SitePrecipitation object. Use these schedules for adding rain water to the simulation. The values are in meters per hour and are scaled to match the average monthly precipitation. They also coincide with the EPW rain/snow flags from the original source files.
-
-### RefrigerationCasesDataSet.idf
-
-All the refrigerated cases included in this database are listed in the following list. Comments before each refrigeration:case object include the manufacturer's model number and assumptions about the fan, lights, defrost etc. The user must ensure that the case names used in the idf file are UNIQUE and must supply the correct zone name.  The user must also supply any required correction curves or schedules. The defrost and drip-down schedule names included here indicate the frequency and duration required. The user must ensure that schedules are provided that meet these needs and that are diversified so that all the cases don't start their defrost cycles at the same time. Please see the example cases for supermarkets to see how these case objects are included with the rest of a supermarket refrigeration system.
-
-* Multi-Deck Dairy/Deli Merchandiser with Synergy-E
-
-* Multi-Deck Rear Dairy/Deli Merchandiser with Synergy-E
-
-* Multi-Deck Deli back
-
-* Single Deck Club Case Merchandiser
-
-* Single Deck Club Case Merchandiser
-
-* Single Deck Club Merchandiser
-
-* Single Deck Club Case Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
-
-* Multi-Deck Dairy/Deli Merchandiser with Synergy-E
-
-* Multi Deck Frozen Food Merchandiser
-
-* Multi Deck Frozen Food Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* International Style Service Deli/Meat/Seafood Merchandiser
-
-* International Style Flat Glass Service Deli/Meat/Seafood Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
-
-* Multi-Deck Deli/Meat End Cap Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
-
-* Multi-Deck Dairy/Deli/Produce/Meat Merchandiser with Synergy-E
-
-* Multi-Deck Dairy/Deli/Produce/Meat Merchandiser with Synergy-E
-
-* Multi-Deck Produce/Dairy/Deli/Meat Merchandiser
-
-* Multi-Deck Deli/Meat End Cap Merchandiser
-
-* Multi-Deck Bulk Produce End Cap Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Produce Merchandiser
-
-* Wide Island Multi-Deck Produce Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Multi-Deck Dairy/Deli/Produce Merchandiser
-
-* Multi-Deck Dairy/Deli/Produce Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Wide Island Multi-Deck Deli/Meat Merchandiser
-
-* Multi-Deck Dairy/Deli/Produce Merchandiser
-
-* Multi-Deck Dairy/Deli/Produce Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Multi-Deck Merchandiser with Synergy-E
-
-* Multi-Deck Merchandiser with Synergy-E
-
-* Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* High Multi-Deck Merchandiser with Synergy-E
-
-* High Multi-Deck Merchandiser with Synergy-E
-
-* High Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* High Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* High Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Multi-Deck Read Load Merchandiser with Synergy-E
-
-* Multi-Deck Rear Load Dairy Merchandiser
-
-* Multi-Deck Rear Load Dairy Merchandiser
-
-* High Multi-Deck Rear Load Dairy Merchandiser
-
-* High Multi-Deck Rear Load Dairy Merchandiser
-
-* Multi Deck Merchandiser with Synergy-E
-
-* Multi-Deck Deli/Meat Merchandiser
-
-* High Multi-Deck  Merchandiser with Synergy-E
-
-* Multi-Deck Rear Load Deli/Meat Merchandiser
-
-* Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Multi-Deck Frozen Food Merchandiser
-
-* Multi-Deck Frozen Food Merchandiser
-
-* Multi-Deck Dairy/Deli/Produce Merchandiser with Synergy E
-
-* Multi-Deck Dairy/Deli/Produce Merchandiser with Synergy E
-
-* Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Full Service Bakery Merchandiser
-
-* Full Service Flat Glass Bakery Merchandiser
-
-* Self Service Bakery/Deli Merchandiser
-
-* Self Service Bakery/Deli Merchandiser
-
-* Self Service Bakery/Deli Merchandiser
-
-* Self Service Deli/Cheese Merchandiser
-
-* Self Service Deli/Cheese Merchandiser
-
-* Single Deck Deli/Meat End Cap Merchandiser
-
-* Single Deck Buck Produce End Cap Merchandiser
-
-* American Style Vertical Glass Service Deli/Meat/Seafood Gravity Coil Merchandiser
-
-* Multi-Deck Deli/Meat Merchandiser
-
-* Multi-Deck Deli/Meat Merchandiser
-
-* Multi-Deck Merchandiser with Synergy-E
-
-* Multi-Deck Merchandiser with Synergy-E
-
-* High Multi-Deck Deli/Meat Merchandiser
-
-* High Multi-Deck Deli/Meat Merchandiser
-
-* Multi-Deck Produce Merchandiser
-
-* Multi-Deck Produce Merchandiser
-
-* High Multi-Deck Merchandiser with Synergy-E
-
-* High Multi-Deck Merchandiser with Synergy-E
-
-* High Multi-Deck Merchandiser with Synergy-E
-
-* High Multi-Deck Merchandiser with Synergy-E
-
-* Wide Island Deli/Meat Merchandiser
-
-* Wide Island Deli/Meat Merchandiser
-
-* Wide Island Deli/Meat Merchandiser
-
-* Wide Island Deli/Meat Merchandiser
-
-* Wide Island Deli/Meat Merchandiser
-
-* Wide Island Deli/Meat Merchandiser
-
-* Wide Island Bulk Produce Merchandiser
-
-* Wide Island Bulk Produce Merchandiser
-
-* Wide Island Bulk Produce Merchandiser
-
-* Island Frozen Food Merchandiser
-
-* Island Frozen Food Merchandiser
-
-* Flat Glass Service Deli Merchandiser
-
-* Flat Glass Service Deli Gravity Coil Merchandiser
-
-* Single-Deck Deli/Meat/Seafood Merchandiser with Synergy -E
-
-* Single-Deck Deli/Meat/Seafood Merchandiser
-
-* Single-Deck Deli/Meat/Seafood Merchandiser
-
-* Single Deck Frozen Meat Merchandiser
-
-* Single Deck Frozen Food/Ice Cream Merchandiser
-
-* Single Deck Frozen Food/Ice Cream Merchandiser
-
-* Narrow Mulit Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
-
-* Narrow Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
-
-* Narrow Multi Deck Deli Meat End Cap Merchandiser
-
-* Narrow Multi Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
-
-* Narrow Multi-Deck Deli/Meat End Cap Merchandiser
-
-* Narrow Multi Deck Bulk Produce End Cap Merchandiser
-
-* Narrow Island Multi Deck Deli/Meat Merchandiser
-
-* Narrow Island Multi Deck Deli/Meat Merchandiser
-
-* Narrow Multi Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
-
-* Multi-Deck Self Service Hot Foods Merchandiser
-
-* Narrow Multi Deck Produce/Dairy/Deli Merchandiser
-
-* Narrow Multi Deck Produce/Dairy/Deli Merchandiser
-
-* Narrow Multi Deck Produce/Dairy/Deli Merchandiser
-
-* High Narrow Multi-Deck Merchandiser with Synergy-E
-
-* High Narrow Multi-Deck Merchandiser with Synergy-E
-
-* High Narrow Multi-Deck Produce/Dairy Merchandiser
-
-* High Narrow Multi-Deck Produce/Dairy Merchandiser
-
-* Narrow Multi-Deck Deli End Cap Merchandiser
-
-* Narrow Multi-Deck Produce Merchandiser
-
-* Narrow Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Narrow Single Deck Frozen Meat End Cap Merchandiser
-
-* Narrow Multi-Deck Deli/Meat Merchandiser
-
-* Narrow Multi-Deck Deli/Meat Merchandiser
-
-* High Narrow Multi-Deck Deli/Meat Merchandiser
-
-* High Narrow Multi-Deck Deli/Meat Merchandiser
-
-* Narrow Multi-Deck Produce Merchandiser
-
-* Narrow Multi-Deck Produce Merchandiser
-
-* High Narrow Multi-Deck Produce Merchandiser
-
-* High Narrow Multi-Deck Produce Merchandiser
-
-* Narrow Island Deli/Meat Merchandiser double Wraparound end
-
-* Narrow Island Deli/Meat Merchandiser double Wraparound end
-
-* Narrow Island Bulk Produce Merchandiser
-
-* Narrow Island Bulk Produce Merchandiser
-
-* Narrow Island Bulk Produce Merchandiser
-
-* Narrow Island Frozen Food/Ice Cream Merchandiser
-
-* Narrow Island Frozen Food/Ice Cream Merchandiser
-
-* Narrow Island Frozen Food/Ice Cream Merchandiser
-
-* Narrow Island Frozen Food Merchandiser
-
-* Narrow Single Deck Frozen Meat Merchandiser
-
-* Multi Deck Dairy Merchandiser
-
-* Narrow Multi Deck Deli Merchandiser
-
-* Multi Deck Utility Merchandiser
-
-* Narrow Single Deck Produce Merchandiser
-
-* Narrow Glass Door Reach In Beverage Merchandiser
-
-* Narrow Glass Door Reach In Beverage Merchandiser
-
-* High Narrow Glass Door Reach-in Beverage Merchandiser
-
-* High Narrow Glass Door Reach-in Beverage Merchandiser
-
-* Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser: Frozen food
-
-* Narrow Glass Door Reach in  Back-toBack Frozen Food/Ice Cream Merchandiser: Ice Cream
-
-* High Narrow Glass Door Reach-in Back-to-Back Frozen Food/Ice Cream: Frozen food
-
-* High Narrow Glass Door Reach-in Back-to-Back Frozen Food/Ice Cream: Ice cream
-
-* Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser: Frozen food
-
-* Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser: Ice Cream
-
-* High Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser
-
-* High Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser
-
-* High Narrow Glass Door Reach in Back to back Frozen Food/Ice Cream Merchandiser
-
-* Narrow Multi-Deck Produce/Dairy/Deli/Meat Merchandiser
-
-* Narrow Multi-Deck Produce/Dairy/Deli/Meat/Seafood Merchandiser
-
-* Narrow Multi-Deck Dome Deli Merchandiser
-
-* Narrow Single-Deck Frozen Food/Ice Cream Merchandiser
-
-* Narrow Single-Deck Frozen Food/Ice Cream Merchandiser
-
-* Narrow Single-Deck Frozen Food/Ice Cream Merchandiser
-
-* Single Deck Produce Merchandiser
-
-* Single Deck Produce Merchandiser
-
-* Single Deck Produce Merchandiser
-
-* Single Deck Produce Merchandiser
-
-* Glass Door Reach-in Beverage Merchandiser
-
-* Glass Door Reach-in Beverage Merchandiser
-
-* High Glass Door Reach-in Beverage Merchandiser
-
-* High Glass Door Reach-in Beverage Merchandiser
-
-* Glass Door Reach-in Rear Load Beverage Merchandiser
-
-* Roll in Rear Load Merchandiser with Synergy-E
-
-* Roll in Rear Load Dairy Merchandiser
-
-* Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
-
-* Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
-
-* Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
-
-* Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
-
-* Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
-
-* Glass Door Reach-in Back too Back Frozen Food/Ice Cream Merchandiser
-
-* High Glass Door Reach-in Frozen Food/Ice Cream Merchandiser
-
-* High Glass Door Reach-in Frozen Food/Ice Cream Merchandiser
-
-* American Style Curved Glass Service Deli Merchandiser
-
-* American Style Curved Glass Service Deli/Meat/Seafood Gravity Merchandiser
-
-* American Style Curved Glass Service Deli/Meat/Seafood Gravity Merchandiser
-
-* American Style Glass Service Deli Merchandiser
-
-* American Style Glass Service Deli Merchandiser
-
-* American Style Flat Glass Service Deli/Meat/Seafood Gravity Coil Merchandiser
-
-* International Style Service Deli/Seafood Merchandiser
-
-* International Style Flat Glass Service Deli/Meat/Seafood Merchandiser
-
-* International Style Single Deck Deli Seafood Merchandiser
-
-* American Style Vertical Glass Service Deli Merchandiser
-
-* American Style Flat Glass Service Frozen Food Merchandiser
-
-* Multi-Deck Produce/Dairy/Meat/Seafood Merchandiser
-
-* Wide Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Wide Multi-Deck Produce/Dairy/Deli Merchandiser
-
-* Wide Island End Cap Frozen Food/Ice Cream Merchandiser
-
-* Wide Island End Cap Frozen Food/Ice Cream Merchandiser
-
-* Wide Island End Cap Frozen Food/Ice Cream Merchandiser
-
-* Wide High Multi-Deck Produce Merchandiser
-
-* Wide High Multi-Deck Produce Merchandiser
-
-* Wide Island Frozen Food/Ice Cream Merchandiser
-
-* Wide Island Frozen Food/Ice Cream Merchandiser
-
-* Wide Island Frozen Food/Ice Cream Merchandiser
-
-* Wide Single Deck Produce Merchandiser
-
-* Wide Single Deck Produce Merchandiser
-
-* Wide Single Deck Produce Merchandiser
-
-* Wide Single Deck Produce Merchandiser
-
-* Wide International Style Service Deli/Seafood Merchandiser
-
-* Wide International Style Single Deck Deli/Seafood Merchandiser
-
-* Single Deck Frozen Food Merchandiser
-
-* Single Deck Frozen Food Merchandiser
-
-* Wide Single Deck Frozen Food Merchandiser
-
-* Full Service Flat Glass Deli Merchandiser
-
-* Multi-Deck Curved Glass Dome Deli/Meat/Seafood Merchandiser
-
-* Multi-Deck Curved Glass Dome Deli/Meat/Seafood Merchandiser
-
-* Glass Door Reach-in Beverage Merchandiser
-
-* Narrow Glass Door Reach in Frozen Food/Ice Cream Merchandiser: Frozen food
-
-* Narrow Glass Door Reach in  Back-toBack Frozen Food/Ice Cream Merchandiser: Ice Cream
-
-* High Glass Door Reach-in Frozen Food/Ice Cream Merchandiser
-
-* High Glass Door Reach-in Frozen Food/Ice Cream Merchandiser
-
-* Single Deck Wood Clad Merchandiser for Medium Temp Application
-
-* Single Deck Wood Clad Merchandiser for Medium Temp Application
-
-* 55'' Tall Convertible With Extended Canopy. Medium Temperature Merchandiser
-
-* C2LGE MultiDeck 3 display levels
-
-* Convertible Island End. Low Profile Multi-Deck
-
-* Unitized Convertible Island. Low Profile Multi-Deck
-
-* Convertible Island. Low Profile Multi-Deck
-
-* Unitized Convertible Island. Low Profile Multi-Deck
-
-* Unitized Convertible Island. Low Profile Multi-Deck
-
-* Unitized Convertible Island. Low Profile Multi-Deck
-
-* Unitized Convertible Island. Low Profile Multi-Deck
-
-* Convertible Island. Low Profile Multi-Deck
-
-* Self-Serve Three-Level Display With Extended Canopy
-
-* Self-Serve Four-Level Display With Extended Canopy
-
-* Self-Serve Four-Level Display With Extended Canopy
-
-* ED1 Impact Service Merchandiser with curved hinged glass 1 display level
-
-* ED1 Impact Service Merchandiser with curved hinged glass 1 display level
-
-* EDS1 Impact self service glass 1 display level
-
-* E1 Self Service Single Deck Display for Deli Cheese and Salads
-
-* E1S Self Service Single Deck Display for Deli Cheese and Salads
-
-* E2 Self-Serve Multi-Deck Display For Deli Cheese Pizza Floral Fresh Juice
-
-* E2 Self-Serve Multi-Deck Display For Deli Cheese Pizza Floral Fresh Juice
-
-* E2S Self-Serve Three Level Display For Deli Cheese Pizza
-
-* E2S Self-Serve Three Level Display For Deli Cheese Pizza
-
-* E2S Self-Serve Three Level Display For Deli Cheese Pizza
-
-* E2S Self-Serve Three Level Display For Deli Cheese Pizza
-
-* E3 Self-Serve Multi-Deck Display For Deli Cheese Pizza Floral Fresh Juice
-
-* Self Serve Multi-Deck Display Merchandiser
-
-* Self Serve Multi-Deck Display Merchandiser
-
-* ES1 Single-Deck Curved Glass Service Case with 1 display level
-
-* ES1S Single-Deck Straight glass Service Case with one display level
-
-* ESBD Curved glass case for deli with blower coil and one display level with optional shelves
-
-* ESBDHV High Volume Curved Glass Blower Coil Service Case for Deli with 3 display levels
-
-* ESBDS Straight glass service case for deli with blower coil and one display level with optional 2 shelves
-
-* ESGM Curved Glass Gravity Coil Service Case for Meat and Seafood
-
-* ESGMS Straight Glass Gravity Coil Service Case for Meat and Seafood
-
-* ESGMVS Vertical hinged glass service case for Deli with Gravity Coil\_single display level
-
-* ESGS Curved Glass Gravity Coil Service Case for Meat and Seafood
-
-* ESGSS Straight Glass Gravity Coil Service Case for Meat and Seafood
-
-* ESBDVS Straight hinged glass service case for Deli with Blower Coil\_1 display level with optional shelves
-
-* B1X BulkSinlge Decked Extended Depth Glass Front
-
-* B3XC Bulk Multi-Deck Convertible Merchandiser
-
-* B3XC Bulk Multi-Deck Convertible Merchandiser
-
-* B4-XE Four-Deck High Volume Bulk Convertible Merchandiser
-
-* C2X Low-Profile Multi-Deck Convertible Merchandiser
-
-* C2X Low-Profile Multi-Deck Convertible Merchandiser
-
-* C2X Low-Profile Multi-Deck Convertible Merchandiser
-
-* C2X Low-Profile Multi-Deck Convertible Merchandiser
-
-* C2X Low-Profile Multi-Deck Convertible Merchandiser
-
-* C2X Low-Profile Multi-Deck Convertible Merchandiser
-
-* C2X Low-Profile Multi-Deck Convertible Merchandiser
-
-* C2X Low-Profile Multi-Deck Convertible Merchandiser
-
-* C2X Low-Profile Multi-Deck Convertible Merchandiser
-
-* C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
-
-* C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
-
-* C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
-
-* C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
-
-* C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
-
-* C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
-
-* C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
-
-* C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
-
-* C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
-
-* C2XX Extra-Height C2XX Multi-Deck Convertible Merchandiser
-
-* C3X Multi-Deck Convertible Merchandiser with four display levels
-
-* C3X Multi-Deck Convertible Merchandiser with four display levels
-
-* C4X Multi-Deck Convertible Merchandiser
-
-* C4X Multi-Deck Convertible Merchandiser
-
-* C4X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C5X Multi-Deck Convertible Merchandiser
-
-* C6X High Capacity Multi-Deck Convertible Merchandiser
-
-* C6X High Capacity Multi-Deck Convertible Merchandiser
-
-* C6X High Capacity Multi-Deck Convertible Merchandiser
-
-* C6X High Capacity Multi-Deck Convertible Merchandiser
-
-* C6X High Capacity Multi-Deck Convertible Merchandiser
-
-* C6X High Capacity Multi-Deck Convertible Merchandiser
-
-* C6X High Capacity Multi-Deck Convertible Merchandiser
-
-* C6X High Capacity Multi-Deck Convertible Merchandiser
-
-* C6XLRE High Capacity Multi-Deck Convertible Merchandiser with Rear Load-In for Dairy and Deli
-
-* D5X-ULEP Ultra Low Front Multi-Deck Dairy/Deli Merchandiser
-
-* D5X-E Multi-Deck Dairy/Deli Merchandiser
-
-* D5X-EP Multi-Deck Dairy/Deli Merchandiser
-
-* D5X-EP Multi-Deck Dairy/Deli Merchandiser
-
-* D5X-HE Multi-Deck Dairy/Deli Merchandiser
-
-* D5X Multi-Deck Dairy/Deli Merchandiser
-
-* D5X-LE Multi-Deck Dairy/Deli Merchandiser
-
-* D5X-LEP Multi-Deck Dairy/Deli Merchandiser
-
-* D5X-LEP Multi-Deck Dairy/Deli Merchandiser
-
-* D5XLRE Multi-Deck Dairy/Deli Merchandiser With Rear Sliding Doors and low front
-
-* D5XRRI Rear Roll-IN Dairy Merchandiser
-
-* D5XRRIS Rear Roll-IN Dairy Merchandiser
-
-* D6NX Narrow Footprint Extra Tall Multi-Deck Dairy/Deli Merchandiser
-
-* D6NX Narrow Footprint Extra Tall Multi-Deck Dairy/Deli Merchandiser
-
-* D6NX Narrow Footprint Extra Tall Multi-Deck Dairy/Deli Merchandiser
-
-* D6NX Narrow Footprint Extra Tall Multi-Deck Dairy/Deli Merchandiser
-
-* D6X-ULEP Ultra Low Front Dairy Merchandiser
-
-* F Single Deck Wall Model Merchandiser  with solid front for Frozen Food
-
-* F Single Deck Wall Model Merchandiser  with solid front for Ice Cream
-
-* F Single Deck Wall Model Merchandiser  with solid front for Medium Temp Products
-
-* FI Intermediate Island Merchandiser with solid walls for Frozen Food
-
-* F2XLG Low Temperature Multi-Deck Merchandiser for Frozen Seafood and Meat
-
-* F6 Low Temperature Multi-Deck Open Merchandiser
-
-* F6L Low Temperature Multi-Deck Open Merchandiser
-
-* FG Single Deck Wall Model Merchandiser with glass front for Frozen Food
-
-* FG Single Deck Wall Model Merchandiser r with glass front for Ice Cream
-
-* FG Single Deck Wall Model Merchandiser r with glass front for Medium Temp Products
-
-* FIG Intermediate Island Merchandiser with glass walls for Frozen Food
-
-* FL5NX Excel Multi-Deck Narrow Footprint Floral Merchandiser
-
-* FN Narrow Island display with solid walls for Frozen Food
-
-* FN Narrow Island display with solid walls for Ice Cream
-
-* FN Narrow Island display with solid walls for medium temperature
-
-* FNG Narrow Glass Sided Island Merchandiser for Frozen
-
-* FNG Narrow Glass Sided Island Merchandiser for Ice Cream
-
-* FNG Narrow Glass Sided Island Merchandiser for Medium Temperature
-
-* FW Wide Island Display with Solid Walls for Frozen Food
-
-* FW Wide Island Display with Solid Walls for Ice Cream
-
-* FW Wide Island Display with Solid Walls for Medium Temperature;
-
-
-### RefrigerationCompressorCurves.idf
-
-This dataset includes object types for specific (by manufacturer and type) Refrigeration:Compressor and associated performance curves. Knowing the nominal refrigerating capacity, power, and refrigerant for the compressor(s) that you want to simulate, you can find it and the associated performance curves in the dataset file. By example, here is part of the RefrigerationCompressorCurves.idf file:
-
-! Capacity Curve for Carlyle\_R-22\_Low\_06CC016,   !nominal MBtu/h = 18561.0
-
-! Results in Watts, Inputs:  Sat Suction Temp (C), Sat Discharge Temp (C)
-
-```idf
-Curve:Bicubic,
-    06CC016_R-22_Low_qcurv,  !- Name
-    2.350e+004,              !- Coefficient1 Constant
-    816.7,                   !- Coefficient2 x
-    10.70,                   !- Coefficient3 x**2
-    -28.24,                  !- Coefficient4 y
-    0.1131,                  !- Coefficient5 y**2
-    -0.4553,                 !- Coefficient6 x*y
-    0.05604,                 !- Coefficient7 x**3
-    -0.004120,               !- Coefficient8 y**3
-    -0.006728,               !- Coefficient9 x**2*y
-    0.006782,                !- Coefficient10 x*y**2
-    -40.0,                   !- Minimum Value of x
-    -17.8,                   !- Maximum Value of x
-    10.0,                    !- Minimum Value of y
-    48.9;                    !- Maximum Value of y
-
-! Power Curve for Carlyle_R-22_Low_06CC016,   !nominal kW = 3.1
-! Results in Watts, Inputs:  Sat Suction Temp (C), Sat Discharge Temp (C)
-Curve:Bicubic,
-    06CC016_R-22_Low_pwrcurv,!- Name
-    4018.,                   !- Coefficient1 Constant
-    95.00,                   !- Coefficient2 x
-    1.507,                   !- Coefficient3 x**2
-    5.705,                   !- Coefficient4 y
-    1.247,                   !- Coefficient5 y**2
-    -1.381,                  !- Coefficient6 x*y
-    0.01277,                 !- Coefficient7 x**3
-    -0.007518,               !- Coefficient8 y**3
-    -0.02424,                !- Coefficient9 x**2*y
-    0.02917,                 !- Coefficient10 x*y**2
-    -40.0,                   !- Minimum Value of x
-    -17.8,                   !- Maximum Value of x
-    10.0,                    !- Minimum Value of y
-    48.9;                    !- Maximum Value of y
-
-!Detailed Compressor: Carlyle_R-22_Low_06CC016,   !nominal MBtu/h = 18561.0, !nominal kW = 3.1
-Refrigeration:Compressor,
-    Carlyle_R-22_Low_06CC016,!- Name
-    06CC016_R-22_Low_pwrcurv,!- Refrigeration Compressor Power Curve Name
-    06CC016_R-22_Low_qcurv,  !- Refrigeration Compressor Capacity Curve Name
-    ,                        !- Rated Superheat {deltaC}
-    18.3,                    !- Compressor Rated Suction Temperature {C}
-    4.4,                     !- Rated Liquid Temperature {C}
-    ;                        !- Compressor Rated Subcooling {C}
-```
-
-
-### RooftopPackagedHeatPump.idf
-
-This dataset includes performance curves for the object types Coil:Cooling:DX:SingleSpeed, Coil:Cooling:DX:TwoStageWithHumidityControlMode and Coil:Heating:DX:SingleSpeed required to model rooftop packaged heat pumps in EnergyPlus. Manufacturer’s data used to develop the data set is also listed in the file. The part of RooftopPackagedHeatPump.idf is shown below.
-
-### SandiaPVData.idf
-
-Use these PV statements for implementing PV modules in an EnergyPlus input file when using the Sandia model.
-
-### Schedules.idf
-
-This data set contains the schedule information for various common (e.g. Office Occupancy) scheduling instances. Derived from the Schedules Library issued with the BLAST program. Includes the building types schedules from ASHRAE 90.1-1989, Section 13. Schedules are listed alphabetically, with general schedules first, followed by the ten 90.1 building type schedules.
-
-### SolarCollectors.idf
-
-Use these SOLAR COLLECTOR PARAMETERS objects for implementing solar collector modules in an EnergyPlus input file.
-
-Data has been reproduced with permission from: "Directory of SRCC Certified Solar Collector Ratings"  Copyright (c) 2004 by the Solar Rating and Certification Corporation. For more information, contact: Solar Rating and Certification Corporation, c/o FSEC, 1679 Clearlake Road, Cocoa, FL 32922-5703 USA  Tel: (321) 638-1537  Fax: (321) 638-1010  ,   www.solar-rating.org
-
-### StandardReports.idf
-
-This file contains the Report Table:Monthly command for some commonly used/desired monthly reports.
-
-### SurfaceColorSchemes.idf
-
-This file offers examples for using custom color schemes for DXF output.
-
-### USHolidays-DST.idf
-
-This is the set of US national holidays as well as daylight saving period defaults.
-
-### Window5DataFile.dat
-
-This is an example data file from the Window5 program that can be used with EnergyPlus windows.
-
-### WindowBlindMaterials.idf
-
-This is a data set of Window Blind materials.
-
-### WindowConstructs.idf
-
-This is a data set of Window constructions. It does not include the required pieces of the Window construction (glass materials, gas materials).
-
-### WindowGasMaterials.idf
-
-This is a data set of Window Gas materials.
-
-### WindowGlassMaterials.idf
-
-This is a data set of Window Glass materials.
-
-### WindowShadeMaterials.idf
-
-This is a data set of Window Shade materials.
-
-### WindowScreenMaterials.idf
-
-This is a data set of Window Screen materials.
-
-Macro Data Sets
----------------
-
-### Locations-DesignDays.xls
-
-Strictly speaking, the locations-designdays.xls file is not a macro enabled input file. Rather, it is the “pointer� to other files and can be searched by city name, country, etc. All the Design Conditions from the ASHRAE Handbook of Fundamentals (2005) have been encoded into Design Day definitions and are stored on the EnergyPlus web site by WMO Region (similarly to how the weather data is stored). The spreadsheet contains a “readme� page as well as cities, countries, and links to the proper web pages.
-
-### SandiaPVData.idf
-
-Use these PV statements for implementing PV modules in an EnergyPlus input file when using the Sandia model.
-
-### SolarCollectors.idf
-
-Use these SOLAR COLLECTOR PARAMETERS objects for implementing solar collector modules in an EnergyPlus input file.
-
-Data has been reproduced with permission from: "Directory of SRCC Certified Solar Collector Ratings" Copyright (c) 2004 by the Solar Rating and Certification Corporation. For more information, contact: Solar Rating and Certification Corporation, c/o FSEC, 1679 Clearlake Road, Cocoa, FL 32922-5703 USA  Tel: (321) 638-1537  Fax: (321) 638-1010  ,   www.solar-rating.org
-
-### UtilityTariffObjects.imf
-
-Use the large collections of input objects to model the costs of energy supplied by utility companies. This file is ready for use in macro processing but the input objects can readily be copied out of the macro file and used in a regular input file. The data were assembled by NREL researcher Brent Griffith and represent a best effort at putting together a comprehensive set of utility tariffs for commercial buildings for the USA as of Spring 2005. Use the data at your own risk and note that utility tariffs need to be continually updated to reflect current conditions.
-
-
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-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Application Guide for Plant Loops</h1>
-<h2>User Guide for Modeling Plant Systems</h2>
-<br/>
-<p><i>(a central location for central plant knowledge)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-Introduction
-============
-
-This document provides an in-depth look at plant modeling in EnergyPlus. Plant refers to the subset of HVAC that involves hydronic equipment for heating, cooling, and service water heating (or domestic hot water).
-
-This guide serves as an aid to help model plant systems in EnergyPlus simulations.  It is intended to augment the Input Output Reference, which describes the syntax and the details of individual input objects. This guide will discuss how the different objects can be used to construct a plant loop that can service a building load.
-
-Organization
-------------
-
-This document begins with some general information to introduce users to the syntax used in EnergyPlus as well as this guide. Then some basic conversion methods needed to take a real system and format it to simplify the input process are provided.  The bulk of this Application Guide is devoted to modeling example systems. The example systems are intended to demonstrate the input process for various types of plant systems, such as systems that use thermal energy storage tanks and those that have a primary/secondary pumping configurations.
-
-The example systems are defined by breaking the system into its constituent loops. The loops are then separated into supply and demand sides.  These half-loops are then defined by branches, connectors, and components.  The controls for each loop are set after the loop has been completed.  Figures and flowcharts are used to display the definition process.  The flow charts should be read from top to bottom and each branched level should be read from left to right.
-
-The Object Class Names and Object Names used in the flow charts match those used in the input file provided for the example.  One thing that is not specified in the flow charts or figures is the node names used.  The various object class names and object names used in the examples refer to the entries in the example input files.
-
-Scope
-=====
-
-The scope of modeling plant loops in EnergyPlus is limited depending on the application. For example, there is no provision to model nested loops, and multiple splitter-mixer pairs in a single loop which are often used in large scale systems. Thus, it has to be realized that modeling large scale district loops may be challenging in EnergyPlus. One way to model such systems is to make some assumptions to condense some arrangements of components that cannot be modeled in EnergyPlus. This approach may not work because the arrangements could be very important to the system. Figure 1 shows a central plant chilled water system for the University of California, Riverside (Hyman and Little, 2004). This system contains a total of eight splitter-mixer pairs, four on the supply side, and four on the demand side. We could make some assumptions to simplify the system. For example we can use a single chiller instead of the array of five chillers, this could work if we size and control the chiller properly, but the concept of scheduling the different chillers to operate at different times of the day to improve efficiency will be lost. Hence, it should be noted that while simplifications can provide a general overview of how the system will operate, they may defeat the original purpose of the complex design. Therefore, this guide will only discuss building plant systems which are less complicated.
-
-
-
-![](media/image001.png)
-
-Figure 1 - Central plant chilled water schematic for the University of California, Riverside (recreated from Hyman and Little, 2004)
-
-EnergyPlus Nomenclature
-=======================
-
-The following is a list of terms that are used in this guide. A simple description of each of the terms is provided. More detailed descriptions can be obtained from the EnergyPlus Input Output Reference. Some keywords are provided to assist with the search for these terms in the Input Output Reference guide.
-
-- **Loops** – Loops are high-level construction objects in EnergyPlus. Loops are paths through which the working fluid is circulated in order to satisfy a cooling or heating load. An HVAC system may consist of a zone, plant loop, and a condenser loop. Loops are constructed by using branches. (Keywords: *PlantLoop*)*.* Note: Although EnergyPlus has separate object classes for *CondenserLoops* and *PlantLoops,* the difference between them is very trivial; therefore all the condenser loops in this guide will be modeled by a *PlantLoop* object.
-
-- **Supply side half-loop** – This is the half loop that contains components (such as Boilers and chillers) which treat the working fluid to supply a working fluid state to the demand components.
-
-- **Demand side half-loop** – This is the half loop that contains components (such as cooling coils and heating coils which use the working fluid to satisfy a load.
-
-- **Branches** – Branches are mid-level construction objects in EnergyPlus. Branches are the segments used to construct the loops. They are constructed by using nodes and a series of components. Every branch must have at least one component. Branches will be denoted by using blue colored lines in the EnergyPlus schematics. (Keyword: *Branch*)*.*
-
-- **Branchlists** – Branchlists list all the branches on one side of a loop. (Keyword: *Branchlist*)*.*
-
-- **Bypass Branch** – A bypass branch is used to bypass the core operating components, it ensures that when the operating components are not required, the working fluid can be circulated through the bypass pipe instead of component. Note: Only one bypass per half loop is required.
-
-- **Connectors** – Connectors are mid-level loop construction objects that are used to connect the various branches in the loops. There are two kinds of connectors: splitter which split the flow into two or more branches, and mixers which mix the flow from two or more branches. A connector pair consists of a splitter and a mixer. A maximum of one connector pair is allowed on each half loop. Connectors will be denoted by using green colored lines in the EnergyPlus schematics used in this guide. (Keywords: *Connector:Mixer, Connector:Splitter*)*.*
-
-- **Connectorlists** – Connectorlists list all the connectors on one side of a loop. (Keyword: *Connectorlist*)*.*
-
-- **Components** – Components are the low-level construction objects in EnergyPlus. Physical objects that are present in the loop are generally called components. Components such as a chiller, cooling tower, and a circulation pump can be considered as the operating/active components. Pipes and ducts can be considered as passive or supporting components. (Keywords: *Chiller:Electric, Pipe:Adiabatic, and many others*)*.*
-
-- **Nodes** – Nodes define the starting and ending points of components and branches.
-
-- **Nodelists** – Nodelists can be used to list a set of nodes in the loop. These nodelists can then be used for a variety of purposes. For example, a setpoint can be assigned to multiple nodes by referring to a particular nodelist. (Keyword: *Nodelist*)*.*
-
-- **Set-point** – Setpoints are control conditions imposed on node(s) that are monitored by the *SetpointManager* to control the system. (Keyword: *SetpointManager:Scheduled, and others*).
-
-- **Plant equipment operation scheme** – This object details the mechanism required to control the operation of the plant loop, as well as the availability of the plant equipment under various conditions. (Keyword: *PlantEquipmentOperation:CoolingLoad, and others*).
-
-- **Schedule** – Schedules allow the user to influence the scheduling of many operational parameters in the loop. For example, a schedule can determine the time period of a simulation, or instruct the load profile object of a plant to import data from a certain external file, among other actions. (Keywords: *Schedule:Compact, Schedule:file*)*.*
-
-- **Load Profile** – A load profile object is used to simulate a demand profile. This object can be used when the load profile of a building is already known. (Keyword: *LoadProfile:Plant*). Note: This object does not allow feedback from the plant conditions to the air system or the zones. However, this object is a great tool for plant-only development and debugging.
-
-Generating an EnergyPlus Line Diagram
-=====================================
-
-The following list of steps will outline the process for converting an engineering line diagram into an EnergyPlus line diagram. Throughout the process, the components in the systems should be identified and named properly. It is easier to input the system if a list of components and their names is available.
-
-1.    **Obtain an engineering line diagram for the system.**
-
-2.    **Identify all the loops in the system.** Some systems may be very complex, but an effort should be made to separate the system into its constituent plant loops. A system may have multiple plant loops. Therefore, proper documentation of the loops and their components should be a priority.
-
-3.    **Identify the demand side and supply side of the individual loops.** EnergyPlus expects the demand side loop and supply side loop to be entered separately. Some examples of simple plant loops are: a hot water heater (supply component) connected to a heating coil (demand component), a chiller (supply component) connected to a cooling coil (demand component) or a cooling tower (supply component) connected to a water cooled chiller (demand component). These loops may have multiple supply components and multiple demand components. A chiller may also be a supply or demand component depending on the loop.
-
-4.    **Identify the components in the system.** All the operating/active components, such as chillers, pumps, cooling towers, thermal energy storage tanks, heating and cooling coils, and other components should be identified and named properly. It should be noted that even though EnergyPlus has objects for modeling valves, they are not often used. Instead the flow through a component is regulated by using schedules, plant equipment operation schemes and set points. Passive components such as inlet and outlet pipes for each side of the loop should also be identified, as they will help in modeling the loop connectors.
-
-5.    **Identify all the nodes in the system.** Nodes are necessary to connect the different components in the system. Nodes define the starting and ending points of branches as well as intermediate nodes on multi-component branches. A good method to pin-point nodes on the line diagram would be to put a node on either side of an active or passive component. Note: If the outlet of one component does not feed into a splitter or a mixer, then the outlet node will be the same as the inlet node of the downstream component.
-
-6.    **Identify all the branches in the loops.** A good way to define a branch would be to include at least one of the components in the branch. Branches can accommodate multiple components in series, but parallel components should be modeled on separate branches. Operating/active components (except pumps) should be bypassed by adding a bypass branch parallel to the branch containing the active component. Multiple bypass branches in parallel can be replaced by a single bypass branch.
-
-7.    **Identify the position of the connectors in the system.** Connectors are an integral part of the system and are important in constructing the loop. There are two types of connectors, splitters and mixers. Splitters can distribute the flow from a single branch into multiple parallel branches. Mixers can combine the flow from multiple branches into a single branch. As mentioned above, most systems have multiple supply and demand side components, so splitters and mixers play a crucial role in distributing and recombining the flow of the working fluid through all the components.
-
-8.    **Generate an EnergyPlus diagram** of the whole system as well as the individual loops by using the information gathered from the preceding steps.
-
-A flowchart for this process is provided in Figure 2 .
-
-![](media/image002.png)
-
-Figure 2 - Flowchart for EnergyPlus line diagram generation
-
-Example for EnergyPlus Line Diagram Generation
-----------------------------------------------
-
-A series of figures are provided below to detail the process for generating an EnergyPlus line diagram.
-
-1.    **Obtain a simple engineering line diagram for the system.** This system is a simple cooling system that employs a primary/secondary pumping setup with a one-way common pipe to circulate chilled water through a building. Figure 3 shows the simple line diagram for the system.
-
-![](media/image003.png)
-
-Figure 3 - Simple line diagram for the example system, (recreated from Reed and Davis 2007)
-
-2.    **Identify all the loops in the system.** This system contains only one plant loop. Loop name: Cooling Loop.
-
-**3.    Identify the demand side and supply side of the loop.**  The half loops are depicted in Figure 4.
-
-![](media/image004.png)
-
-Figure 4 - Breakdown of a loop into its constituent half-loops
-
-
-
-4.    **Identify the components in the system.** While identifying the main components in the loop, it should be noted that this loop has a primary/secondary pumping setup, and that there is a common pipe that allows for flow imbalance. (Note: The *PlantLoop* object in EnergyPlus has a provision for the input of a common pipe. The user only has to specify the existence of a common pipe in the loop, and the program calculates its position in the loop). The primary pump is shown below is shown in Figure 5.
-
-![](media/image005.png)
-
-Figure 5 - A component in the loop
-
-5.    **Identify all the nodes in the system.** As mentioned above, placing a node on each side of a component is a good way to pinpoint all the nodes in the system. This process should be repeated for every component in the loop. Figure 6 shows the placement of all the nodes on Individual components, while Figure 7 shows all the nodes in the system.
-
-![](media/image006.png)
-
-Figure 6 - Node placement on components
-
-
-
-![](media/image007.png)
-
-Figure 7 - Nodes in the system
-
-Note: No nodes were placed on the common pipe, but its existence should be specified in the *PlantLoop* object.
-
-6.    **Identify all the branches in the system.** Remember to add the bypass branches to the operating components (except the pumps). Branches have to start and end with nodes, and should contain at least one component. The branches are denoted by the blue lines in Figure 8.
-
-
-
-![](media/image008.png)
-
-Figure 8 - Branch definition
-
-
-
-7.    **Identify the position of the connectors in the system.** The *PlantLoop* accepts only one splitter-mixer pair per half loop. The connectors are defined by using branches; a splitter can have one inlet branch and any number of outlet branches whereas a mixer can have any number of inlet branches and one outlet branch. All the connectors in the loop are denoted by the green lines in Figure 9.
-
-
-
-![](media/image009.png)
-
-Figure 9 - Splitters and mixers in the loop
-
-
-
-8.    An EnergyPlus diagram can be generated by using all the identified components. The complete schematic is shown in Figure 10.
-
-
-
-![](media/image010.png)
-
-Figure 10 - Complete EnergyPlus line diagram
-
-Inputting the system into the IDF file
-======================================
-
-Since, it is not possible to input schematics into the input file, it is important to add descriptive comments to all of the entries to ensure that all the components in the system have been accounted for. Such documentation will also make debugging easier. It should be noted that all of the syntax for the inputs is documented in the Input-Output reference guide. A flowchart for the basic input process is provided in Figure 11.
-
-![](media/image011.png)
-
-Figure 11 - Flowchart for input process
-
-Example System 1: Chiller and Condenser Loops
-=============================================
-
-A simple cooling system will be used as an example to demonstrate the process of inputting a system into the input file. The input file for this example can be found under the name: PlantApplicationsGuide\_Example1.idf.
-
-This particular system consists of two unique sub-systems/loops. It contains the *PlantLoop* with the chiller and the load profile, and another *PlantLoop* with the cooling tower. A schedule containing previously obtained simulation loads is used to simulate the demand load profile for this loop (Note: In a more general scenario a cooling coil placed in a building zone would provide the load profile). Flow diagrams along with some keywords from the input file will be used to record to steps that are required to properly input the system into EnergyPlus. The simple line diagram for this system is provided in Figure 12. The complete EnergyPlus schematic for the system is provided in Figure 13.
-
-
-
-![](media/image012.png)
-
-Figure 12 - Simple cooling system line diagram
-
-
-
-**![](media/image013.png)**
-
-Figure 13 – EnergyPlus line diagram for the simple cooling system
-
-
-
-
-
-The cooling system consists of a chilled water loop which is defined by the *PlantLoop* object, and a condenser loop which is also defined by the *PlantLoop* object. Identification of these loops in the system is critical for the process of modeling the system in the input file the flowchart for loop identification is provided in Figure 14.
-
-
-
-![](media/image014.png)
-
-Figure 14 - Flowchart for loop identification
-
-Chilled water (CW) loop
------------------------
-
-The chilled water loop is constructed by using a *PlantLoop* object*.* This loop uses a water-cooled electric chiller to supply chilled water to the demand side of this loop. As mentioned above, the cooling coil is replaced by a load profile object that contains the demand load profile. The chiller is operated by using set points, plant equipment operation schemes and schedules. Refer to Figure 15 for a simple diagram of the Chilled Water Loop.
-
-
-
-![](media/image015.png)
-
-Figure 15 - Simple line diagram for the chilled water loop
-
-
-
-### Flowcharts for the CW Loop Input Process
-
-This series of flow charts serve as a process guide for identifying and inputting the chilled water loop and its components into the input file. Refer to Figure 16 for an EnergyPlus schematic of the Chilled Water Loop.
-
-![](media/image016.png)
-
-Figure 16 - EnergyPlus line diagram for the chilled water loop
-
-The “PlantLoop� object is entered into the input file, with water as the working fluid. The supply side of the chilled water loop is then input into the system followed by the demand side. A flow chart for separating the half loops in the loop is provided in Figure 17.
-
-
-
-![](media/image017.png)
-
-Figure 17 - Simple flowchart for separation of half loops in the chilled water loop
-
-
-
-
-
-#### CW Loop Supply Side Loop Construction
-
-The main components in the supply side of the chilled water loop are the circulation pump for the chilled water and the electric chiller that supplies the chilled water. The set-point is set to the outlet node of this half of the loop; the temperature at this node is controlled to regulate the operation of the chiller. This side of the loop has eight nodes, four components and four branches, while it is not required to define individual node positions in the loop, the components and branches have to be defined with an inlet and an outlet node. Connectors are the objects that connect the branches together and complete the loop. Therefore, the branches and the connectors will set the positions of the nodes in the loop. The EnergyPlus line diagram for the Chilled Water Loop supply side is provided in Figure 18. The flowchart for supply side branches and components is provided in Figure 19. The flowchart for the supply side connectors is provided in Figure 20.
-
-
-
-![](media/image018.png)
-
-Figure 18 - EnergyPlus line diagram for the supply side of the chilled water loop
-
-![](media/image019.png)
-
-Figure 19 – Flowchart for chilled water loop supply side branches and components
-
-
-
-
-
-![](media/image020.png)
-
-Figure 20 – Flowchart for chilled water loop supply side connectors
-
-
-
-
-
-#### CW Loop Demand Side Loop Construction
-
-The demand side of the loop is entered next. The main component in this side of the loop is the cooling load profile(instead of the cooling coil). This load profile is input by using a Schedule:Compact object which indicates the hourly cooling loads for the annual run period. In a more general scenario a cooling coil would take the place of the load profile and the cooling load will be simulated from the data obtained in the building system energy simulation. Apart from the load profile, the structure of the loop is very similar to the structure of the supply side. This side of the loop also has eight nodes, four components, and four branches. An EnergyPlus schematic for the demand side is provided in Figure 21. The flowchart for demand side branch definition is provided in Figure 22. The flowchart for the demand side connectors is provided in Figure 23.
-
-**![](media/image021.png)**
-
-Figure 21 - EnergyPlus line diagram for the demand side of the chilled water loop
-
-![](media/image022.png)
-
-Figure 22 – Flowchart for chilled water loop demand side branches and components
-
-
-
-**![](media/image023.png)**
-
-Figure 23 – Flowchart for chilled water loop demand side connectors
-
-
-
-As shown in the flowchart above, the load profile is attached to the chilled water loop at its designated position (the LoadProfile:Plant object can be used just like any other component) on the demand side of the loop.
-
-
-
-
-
-### Flowcharts for CW Loop Controls
-
-The chilled water loop is operated by using set-points, plant equipment operation schemes and schedules.
-
-#### Chilled Water Loop Schedules
-
-The chilled water loop uses two different schedules to operate properly. The *Chiller AlwaysOnSchedule* is a compact schedule that keeps the chiller ON at all times of the day for a whole year. This compact schedule uses a discrete *ScheduleTypeLimit* (*CW Loop On/Off)* which defines that the value of On is 1 and that of Off is 0. This plant loop also uses another compact schedule named *CW Loop Temp Schedule* to set the temperature at the chilled water loop outlet node. This schedule uses a schedule type limit named *CW Loop Any Number*. The flowchart for chilled water loop schedule definition is provided in Figure 24.
-
-
-
-* *
-
-![](media/image024.png)
-
-Figure 24 – Flowchart for chilled water loop schedules
-
-
-
-
-
-#### Chilled Water Loop Plant Equipment Operation Schemes
-
-The *PlantEquipmentOperationschemes* object uses the *Chiller AlwaysOnSchedule* and the *CW Loop Cooling Load* objects to set the range of the demand load for which the chiller can be operated during the simulation period. Operation schemes are especially useful and crucial when using multiple active components. For example, the performance of multiple chillers can be optimized by carefully managing the load ranges on each of the chillers. A flowchart detailing the chilled water loop plant equipment operation schemes is provided in Figure 25.
-
-
-
-![](media/image025.png)
-
-Figure 25 – Flowchart for chilled water loop plant equipment operation schemes
-
-
-
-#### Chilled Water Loop Setpoints
-
-The *Chilled Water Loop Setpoint Manager* uses the *CW Loop Temp Schedule* to set a temperature control point at the *CW Supply Outlet Node*. This setpoint allows the program to control the temperature at the node by operating the components in the chilled water loop.  Since, setpoint managers are high-level control objects, their usefulness is realized in much more complex systems, where multiple nodes have to be monitored in order to operate the system properly. A flowchart for chilled water loop setpoints is provided in Figure 26.
-
-
-
-![](media/image026.png)
-
-Figure 26 – Flowchart for chilled water Loop setpoints
-
-
-
-#### Chilled Water Loop Sizing
-
-The chilled water loop is sized such a way that the design loop exit temperature is 7 degrees Celsius, and the loop design temperature difference is 5 degrees Celsius. A flowchart for the chilled water loop sizing is provided in Figure 27. Note: Since the Load Profile object does not demand any feedback from the *PlantLoop* object, the chilled water loop does not necessarily need to be sized (This object is commented out in the example file). The sizing shown here is just an example of how the object class can be used in EnergyPlus.
-
-
-
-![](media/image027.png)
-
-Figure 27 – Flowchart for chilled water loop sizing
-
-
-
-
-
-Condenser Loop
---------------
-
-The condenser loop uses a cooling tower to supply cooling water to the water-cooled electric chiller in the chilled water loop. Hence, the supply side of this loop consists of the cooling tower and the demand side consists of the electric chiller. The schedules for this loop are almost identical to the ones applied on the CW loop. They dictate that the cooling tower also works around the year. The plant equipment schemes specify the cooling capacity/load of the cooling tower. The operation of the cooling tower is managed by monitoring the outdoor air wet bulb (air cooled condenser) temperature at the location of the simulation. The structure of this loop is very similar to that of the chilled water loop, the only difference being the main components in the loop. A simple line diagram of the condenser loop is provided in Figure 28.
-
-
-
-![](media/image028.png)
-
-Figure 28 - Simple line diagram for the condenser loop
-
-### Flowcharts for the Condenser Loop Input Process
-
-As discussed in Section 1 the supply side and the demand side of the loop are modeled separately by following the process provided in the flow chart. The flow charts for this loop are provided below.
-
-A *PlantLoop* object is used to model the condenser loop with the chiller and the cooling tower as its main components. The working fluid is water. This loop is also sized such that the loop exit temperature is set to 20 degrees Celsius and the loop design temperature difference is 5 degrees Celsius. The chiller serves as the bridge between the chilled water loop and the condenser loop. This is achieved by managing the nodal connections on the chiller, hence the chiller appears on two branches in the system (supply branch of the CW loop, and the demand branch of the condenser loop). The EnergyPlus line diagram for the condenser loop is provided in Figure 29. A simple flow chart for the separation of the half loops is provided in Figure 30.
-
-![](media/image029.png)
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-Figure 29 - EnergyPlus line diagram for the condenser loop
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-
-![](media/image030.png)
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-Figure 30 - Simple flowchart for separation of half loops in the condenser loop
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-
-#### Condenser Loop Supply Side Construction
-
-The main components in the supply side of the condenser loop are the condenser circulation pump and the cooling tower. The temperature set-point is set at the outlet node, where the outdoor air wet bulb temperature is monitored to regulate the operation of the cooling tower. The outdoor air conditions are obtained from the weather information file during the simulation. This side of the loop has eight nodes and four branches. An EnergyPlus diagram for the condenser loop supply side is provided in Figure 31. The flowchart for supply side branch definition is provided in Figure 32. The flowchart for the supply side connectors is provided in Figure 33.
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-![](media/image031.png)
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-Figure 31 - EnergyPlus line diagram for the supply side of the condenser loop
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-![](media/image032.png)
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-Figure 32 - Flowchart for condenser supply side branches and components
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-![](media/image033.png)
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-Figure 33 - Condenser loop supply side connectors
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-***
-***
-#### Condenser Loop Demand Side Construction
-
-The central component of the demand side is the chiller. The flowchart for the construction of the demand side is also provided below. The schedules for this side do not need to be specified, because the schedules that apply to the chiller also apply to this side of the condenser loop. This side of the loop also contains eight nodes and four branches. An EnergyPlus schematic for the demand side is provided in Figure 34. The flowchart for demand side branch definition is provided in Figure 35. The flowchart for the demand side connectors is provided in Figure 23.
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-![](media/image034.png)
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-Figure 34 - EnergyPlus line diagram for the demand side of the condenser loop
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-![](media/image035.png)
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-Figure 35 - Condenser loop demand side construction
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-![](media/image036.png)
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-Figure 36 - Condenser loop demand side schedules, equipment schemes and setpoints
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-
-
-### Flowcharts for Condenser Loop Controls
-
-The cooling tower is also scheduled similar to the chiller because both of these units have to work together in order to satisfy the cooling load. The operation of the cooling tower is determined by using a set point at the condenser supply exit node. This set point monitors the temperature at this node as well as the outdoor air wet bulb temperature to operate the cooling tower. The flowchart for the schedules, plant equipment schemes, and the set points are also provided below.
-
-#### Condenser Loop Schedules
-
-The *Tower AlwaysOnSchedule* is a compact schedule that keeps the tower ON at all times of the day for a whole year, this compact schedule uses a discrete *scheduletypelimit* (*Tower On/Off)* which defines that the value of On is 1 and that of Off is 0. A flowchart for condenser loop schedules is provided in Figure 37.
-
-* *
-
-![](media/image037.png)
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-Figure 37 - Condenser loop schedules
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-#### Condenser Loop Plant Equipment Operation Schemes
-
-The plant equipment operation schemes for the condenser loop are very similar to those of the chilled water loop. The *PlantEquipmentOperationschemes* object uses the *Tower AlwaysOnSchedule* and the *Tower Load* objects to set the range of the demand loads for which the cooling tower is operated during the simulation period. A flowchart for the condenser loop plant equipment operation schemes is provided in Figure 38.
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-![](media/image038.png)
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-Figure 38 - Condenser loop plant equipment operation schemes
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-
-#### Condenser Loop Setpoints
-
-The *Condensercontrol setpointmanager* places a temperature setpoint at the *Condenser Supply Outlet Node.* The temperature at this point is controlled with respect to the outdoor air wet bulb temperature at that point in the simulation. The outdoor air wet bulb temperature is obtained from the weather data at the location of the simulation. A flowchart for the condenser loop setpoint is provided in Figure 39.
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-![](media/image039.png)
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-Figure 39 - Condenser loop setpoints
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-#### Condenser Loop Sizing
-
-The condenser loop is sized such that the loop exit temperature is 20 degrees Celsius and the loop temperature difference is 5 degrees Celsius. A flowchart for condenser loop sizing is provided in Figure 40.
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-![](media/image040.png)
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-Figure 40 - Condenser loop sizing
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-
-Example System 2: Thermal Energy Storage
-========================================
-
-This system will detail the process required to model a Plant Loop coupled with Thermal Energy Storage (TES) in EnergyPlus. The input file for this example can be found under the name: PlantApplicationsGuide\_Example2.idf.
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-The TES tank will be charged by using a chiller loop, which will in turn be cooled by a condenser loop. The schedules for this system are setup such that the TES tank will be charged by the chiller during the night and then the stored chilled water is used to satisfy the building cooling load during the day. The TES tank used in this system is a stratified tank. This system also includes one heating loop which satisfies the heating load. The cooling and heating system operate in conjunction with an air loop that is spread across a total of five zones. The air loop modeling will not be discussed in this guide. This system consists of a total of three separate plant loops, the cooling side is comprised of two loops and the heating side contains one loop. A simple line diagram for the cooling system is provided in Figure 41. The EnergyPlus line diagram for the cooling loop is provided in Figure 43. A simple line diagram for the heating loop is provided in Figure 42, whereas its EnergyPlus line diagram is provided in Figure 44.
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-![](media/image041.png)
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-Figure 41 – Simple line diagram for cooling system
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-      ![](media/image042.png)
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-Figure 42 - Simple line diagram for heating loop
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-![](media/image043.png)
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-Figure 43 - EnergyPlus line diagram for cooling system
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-![](media/image044.png)
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-Figure 44 - EnergyPlus line diagram for heating loop
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-SHWSys1
-
-The cooling side of the system will be modeled first. The primary cooling loop (named “CoolSysPrimary� in the input file) uses the chiller as the supply side component to charge the TES tank. The chilled water that is stored in the TES tank is then supplied to the cooling coil. A cooling tower that operates on the supply side of the condenser loop (named “Condenser Loop�) supplies the cooling water to the chiller that is used in the primary cooling loop. These two loops serve as the cooling system for this building. This system will be modeled first with emphasis placed on the primary cooling loop. In particular the schedules used for the charging and discharging the TES tank play a crucial role in the efficient operation of the system.
-
-The building also has one heating loop. The heating loop (named “HeatSys 1�) uses a boiler to provide hot water to five heating coils that are located in the five zones. This heating loop also supplies hot water to the reheat coil. A flow chart for loop identification is provided in Figure 45.
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-![](media/image045.png)
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-Figure 45 - Flowchart for loop identification
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-
-
-Primary Cooling Loop (*CoolSysPrimary*) - Chiller
--------------------------------------------------
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-The primary cooling system is constructed by using a *PlantLoop* object. It uses an electric chiller that generates chilled water which is used to charge the TES tank at night. The chilled water stored in the TES tank is later used during the peak hours to satisfy the demand loads. Therefore, the supply side of the loop contains the electric chiller and the charge side of the TES tank. The demand side loop contains the cooling coil. The loop is operated by using plant equipment operation schemes, and schedules. Refer to Figure 46 for a simple diagram of the Primary Cooling Loop.
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-![](media/image046.png)
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-Figure 46 - Simple line diagram for the primary cooling system
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-
-
-### Flowcharts for the Primary Cooling Loop Input Process
-
-This series of flowcharts serve as a guide for identifying and inputting the CoolSysPrimary loop and its components into the input file. The working fluid in this loop is water. The important area for this loop is its controls. The EnergyPlus line diagram for this loop is provided in Figure 47. A simple flowchart for the separation of the half loops is provided in Figure 48.
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-![](media/image047.png)
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-Figure 47 - EnergyPlus line diagram for the primary cooling system
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-![](media/image048.png)
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-Figure 48 - Simple flowchart for the separation of half-loops in the primary cooling system
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-#### CoolSysPrimary Supply Side Loop Construction
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-The main components on the supply side half loop for the primary cooling system are the electric chiller that supplies the chilled water, the variable speed pump that circulates the chilled water through the loop, and the TES tank that stores the supplied chilled water. This half loop supplies chilled water to the cooling coil which is placed on the demand side half loop. The supply side half loop contains five components, four branches, nine nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the primary cooling loop supply side is provided in Figure 49. The flowchart for supply side branches and components is provided in Figure 50. The flowchart for supply side connectors is provided in Figure 51.
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-![](media/image049.png)
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-Figure 49 - EnergyPlus line diagram for the supply side of the primary cooling loop
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-![](media/image050.png)
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-Figure 50 – Flowchart for primary cooling loop supply side branches and components
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-![](media/image051.png)
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-Figure 51 – Flowchart for primary cooling loop supply side connectors
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-
-#### CoolSysPrimary Demand Side Loop Construction
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-The main component on the demand side half loop is the cooling coil which cools the air in the building by using the chilled water that is supplied by the supply side half loop. This side of the loop has eight nodes, four components, four branches, and one splitter mixer pair. An EnergyPlus line diagram for the demand side is provided in Figure 52. The flowchart for demand side branch definition is provided in Figure 53. The flowchart for the demand side connectors is provided in Figure 54.
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-**![](media/image052.png)**
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-Figure 52 - EnergyPlus line diagram for the demand side of the primary cooling loop
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-![](media/image053.png)
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-Figure 53 – Flowchart for primary cooling loop demand side branches and components
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-![](media/image054.png)
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-Figure 54 – Flowchart for primary cooling loop demand side connectors
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-
-### Flowcharts for Primary Cooling Loop Controls
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-The Primary Cooling loop is operated by using set-points, plant equipment operation schemes and schedules. The TES tank charging schedule is one of the most important schedules in this system.
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-#### CoolSysPrimary Schedules
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-The flowchart for Primary Cooling loop schedule definition is provided in Figure 56. The Primary Cooling loop uses five different schedules to operate properly.  The *PlantOnSchedule* is a compact schedule that keeps the chiller and the TES tank ON at all times of the day, this compact schedule uses a discrete *ScheduleTypeLimit* (*On/Off)* which defines that the value of On is 1 and that of Off is 0. This plant loop also uses another compact schedule named *CW Primary Loop Temp Schedule* declare that the temperature of the chilled water loop outlet flow is 6.7 degrees Celsius at all times. This schedule is used by the setpoint manager (*CoolSysPrimary Loop Setpoint Manager)*. This schedule uses a schedule type limit named *Temperature,* which defines the upper and lower loop temperature limits
-
-The compact schedule *ALWAYS\_ON* dictates that the use/discharge side of the TES tank is On at all times of the day. This schedule uses the *ScheduleTypeLimit (Fraction)* to set the fractional flow rate of the use side. This schedule is used to define the use side availability of the TES tank. The compact schedule *CW Tank Temp Schedule* is input in the TES tank object class to define the limits of the temperature for the chilled water storage tank outlet. This schedule uses the *ScheduleTypeLimit (Temperature)* to define that the temperature at that outlet should be 7.5 degrees Celsius at all times of the day.
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-The *TES Charge Schedule* is a very important schedule for the functioning of the CoolSysPrimary Loop the schedule from the input file is provided in Figure 55. The schedule shows that, the on/off *ScheduleTypeLimit* is used to determine if the TES schedule is On or off for a certain period of time. A value of 1.0 means On and a value of 0 means Off. For example, it can be observed from the figure that, for the weekdays the TES tank is charged until 10:00AM, then it is operated during the day from 10:00 AM to 5:00 PM and then it is charged until midnight. The schedule for the other days is also shown in the figure.
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-![](media/image055.png)
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-Figure 55 - TES Charge Schedule
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-![](media/image056.png)
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-Figure 56 – Flowchart for primary cooling loop schedules
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-
-#### CoolSysPrimary Plant Equipment Operation Schemes
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-This loop has two plant equipment operation schemes, one for the chiller and one for the TES tank. The *PlantEquipmentOperationschemes* object uses the *PlantOnSchedule* and the *CoolSysPrimary Operation Scheme* objects to set the range of demand loads for which the chiller is operated during the simulation period. Operation schemes are especially useful and crucial when using multiple active components. For example, the performance of multiple chillers can be optimized by carefully managing the load ranges on each of the chillers. It should be noted that it is required to enter a plant equipment operation scheme for every plant loop in the system. A flowchart detailing the chilled water loop plant equipment operation schemes is provided in Figure 57.
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-
-![](media/image057.png)
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-Figure 57 – Flowchart for Chiller plant equipment operation schemes
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-The TES tank operation is modeled here. The *PlantEquipmentOperationschemes* object uses the *PlantOnSchedule* and the *TES Operation Scheme* objects to set the range of the demand loads for which the TES tank is operated during the simulation period. A flowchart detailing the Secondary Cooling Loop plant equipment operation schemes is provided in Figure 58.
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-
-![](media/image058.png)
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-Figure 58 – Flowchart for Thermal Energy Storage plant equipment operation schemes
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-
-
-#### CoolSysPrimary Setpoints
-
-The *CoolSysPrimary Loop Setpoint Manager* uses the *CoolSysPrimary Loop Temp Schedule* to set a temperature control point at the *CoolSysPrimary Supply Outlet Node*. This setpoint allows the program to control the temperature at the node by operating the components in the Primary Cooling loop.  A flowchart for Secondary Cooling loop setpoints is provided in Figure 59.
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-![](media/image059.png)
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-Figure 59 – Flowchart for primary cooling loop setpoints
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-
-
-#### CoolSysPrimary Sizing
-
-The chilled water loop is sized such a way that the design loop exit temperature is 6.7 degrees Celsius, and the loop design temperature difference is 5 degrees Celsius. A flowchart for the Secondary Cooling loop sizing is provided in Figure 60.
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-![](media/image060.png)
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-Figure 60 – Flowchart for primary cooling loop sizing
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-
-
-Condenser Loop (*Condenser Loop*) - Cooling Tower
--------------------------------------------------
-
-The Condenser Loop is constructed by using a *PlantLoop* object. It uses a cooling tower (modeled by using a *CoolingTower:SingleSpeed* object class) and a constant speed pump (modeled by using a *Pump:ConstantSpeed)* to supply cooling water to the electric chiller (modeled by using a *Chiller:Electric* object). Therefore, the supply side of the loop contains the Cooling Tower and the demand side contains the electric chiller. The loop is operated by using plant equipment operation schemes, and schedules.  Refer to Figure 61 for a simple diagram of the Condenser Loop.
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-
-![](media/image061.png)
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-Figure 61 - Simple line diagram for the condenser loop
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-
-
-### Flowcharts for the Condenser Loop Input Process
-
-This series of flowcharts serve as a guide for identifying and inputting the Condenser Loop and its components into the input file. The EnergyPlus line diagram for this loop is provided in Figure 62. A simple flowchart for the separation of the half loops is provided in Figure 63.
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-![](media/image062.png)
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-Figure 62 - EnergyPlus line diagram for the condenser loop
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-
-![](media/image063.png)
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-Figure 63 - Simple flow chart for separation on half loops in the condenser loop
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-
-
-
-
-#### Condenser Loop Supply Side Construction
-
-The main components on the supply side half loop for the Condenser Loop are the Cooling Tower that supplies the cooling water and the constant speed pump that circulates the cooling water through the loop. This half loop supplies cooling water to the electric chiller on the demand side half loop. The supply side half loop contains four components, four branches, eight nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the Condenser loop supply side is provided in Figure 64. The flowchart for supply side branches and components is provided in Figure 65. The flowchart for supply side connectors is provided in Figure 66.
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-
-![](media/image064.png)
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-Figure 64 - EnergyPlus line diagram for the supply side of the condenser loop
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-
-![](media/image065.png)
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-Figure 65 – Flowchart for condenser loop supply side branches and components
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-![](media/image066.png)
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-Figure 66 – Flowchart for condenser loop supply side connectors
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-
-
-
-
-#### Condenser Loop Demand Side Construction
-
-The main component on the demand side half loop is the Chiller that uses the cooling water supplied by the cooling tower. The chiller in turn is used to supply chilled water in the Primary Cooling loop.  This side of the loop also has eight nodes, four components, four branches and one splitter-mixer pair. An EnergyPlus schematic for the demand side is provided in Figure 67. The flowchart for demand side branch definition is provided in Figure 68. The flowchart for the demand side connectors is provided in Figure 69.
-
-**![](media/image067.png)**
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-Figure 67 - EnergyPlus line diagram for the demand side of the condenser loop
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-
-![](media/image068.png)
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-Figure 68 – Flowchart for condenser loop demand side branches and components
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-![](media/image069.png)
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-Figure 69 – Flowchart for condenser loop demand side connectors
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-
-
-
-
-
-
-### Flowcharts for Condenser Loop Controls
-
-The Condenser Loop is operated by using set-points, plant equipment operation schemes and schedules.
-
-#### Condenser Loop Schedules
-
-The flowchart for condenser loop schedule definition is provided in Figure 70. The Condenser loop uses one schedule to operate properly. *PlantOnSchedule* is a compact schedule that keeps the Cooling Tower On at all times of the day, this compact schedule uses a discrete *ScheduleTypeLimit* (*On/Off)* which defines that the value of On is 1 and that of Off is 0.
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-
-
-![](media/image070.png)
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-Figure 70 – Flowchart for condenser loop schedules
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-
-
-#### Condenser Loop Plant Equipment Operation Schemes
-
-The *PlantEquipmentOperationschemes* object uses the *PlantOnSchedule* and the *Condenser Loop Operation Scheme* objects to set the range of demand loads for which the cooling tower is operated during the simulation period. A flowchart detailing the Condenser Loop plant equipment operation schemes is provided in Figure 71.
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-
-
-![](media/image071.png)
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-Figure 71 – Flowchart for condenser loop plant equipment operation schemes
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-#### Condenser Loop Setpoints
-
-The *MyCondenserControl* setpointmanager places a temperature setpoint at the *Condenser Supply Outlet Node.* The temperature at this point is controlled with respect to the outdoor air wet bulb temperature at that point in the simulation. The outdoor air wet bulb temperature is obtained from the weather data at the location of the simulation. The minimum setpoint temperature is 5 degrees Celsius and the maximum setpoint temperature is 80 degrees Celsius. A flowchart for Secondary Cooling loop setpoints is provided in Figure 72.
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-
-
-![](media/image072.png)
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-Figure 72 – Flowchart for condenser loop setpoints
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-
-
-#### Condenser Loop Sizing
-
-The Condenser loop is sized such a way that the design loop exit temperature is 29.4 degrees Celsius, and the loop design temperature difference is 5.6 degrees Celsius. A flowchart for the chilled water loop sizing is provided in Figure 73.
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-
-![](media/image073.png)
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-Figure 73 – Flowchart for condenser loop sizing
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-
-
-Heating Loop (*HeatSys1*) - Boiler
-----------------------------------
-
-The Heating loop is constructed by using a *PlantLoop* object. It uses an electric boiler to (modeled by using a *Boiler:HotWater* object class) to supply hot water to the five heating coils placed in the five zones of the building (modeled by using a *Coil:Heating:Water* object class). Therefore, the supply side of the loop contains the hot water boiler and the demand side contains a total of six heating coils. The loop is operated by using plant equipment operation schemes, and schedules.  Refer to Figure 74 for a simple diagram of the Condenser Loop.
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-
-
-![](media/image074.png)
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-Figure 74 - Simple line diagram for the heating loop
-
-### Flowcharts for the Heating Loop Input Process
-
-This series of flowcharts serve as a guide for identifying and inputting the Heating loop and its components into the input file. The EnergyPlus line diagram for this loop is provided in Figure 75. A simple flowchart for the separation of the half loops is provided in Figure 76.
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-
-![](media/image075.png)
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-Figure 75 - EnergyPlus line diagram for the heating loop
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-
-![](media/image076.png)
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-Figure 76 - Simple flow chart for separation on half loops in the heating loop
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-
-
-
-
-#### Heating Loop Supply Side Construction
-
-The main components on the supply side half loop for the Heating Loop are the hot water boiler that generates hot water and the variable speed pump that circulates the hot water through the loop. This half loop supplies hot water to five heating coils on the demand side half loop. The supply side half loop contains four components, four branches, eight nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the Primary Cooling loop supply side is provided in Figure 77. The flowchart for supply side branches and components is provided in Figure 78. The flowchart for supply side connectors is provided in Figure 79.
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-
-![](media/image077.png)
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-Figure 77 - EnergyPlus line diagram for the supply side of the heating loop
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-
-![](media/image078.png)
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-Figure 78 – Flowchart for heating loop supply side branches and components
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-
-![](media/image079.png)
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-Figure 79 – Flowchart for heating loop supply side connectors
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-
-
-
-
-#### Heating Loop Demand Side Construction
-
-The demand side half loop contains five heating coils that heat the air in the different zones of the building by using the hot water that is supplied by the hot water boiler. This side of the loop also has sixteen nodes, eight components, eight branches, and one splitter-mixer pair. An EnergyPlus schematic for the demand side is provided in Figure 80. The flowchart for demand side branch definition is provided in Figure 81. The flowchart for the demand side connectors is provided in Figure 82.
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-
-
-**![](media/image080.png)**
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-Figure 80 - EnergyPlus line diagram for the demand side of the heating loop
-
-![](media/image081.png)
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-Figure 81 – Flowchart for heating loop demand side branches and components
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-
-![](media/image082.png)
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-Figure 82 – Flowchart for heating loop demand side connectors
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-
-
-### Flowcharts for Heating Loop Controls
-
-The Heating Loop is operated by using set-points, plant equipment operation schemes and schedules.
-
-#### Heating Loop Schedules
-
-The flowchart for Primary Cooling loop schedule definition is provided in Figure 83. The Heating Loop uses three different schedules to operate properly. *PlantOnSchedule* is a compact schedule that uses a discrete *ScheduleTypeLimit* (*On/Off)* which defines that the value of ON is 1 and that of Off is 0. This plant loop also uses another compact schedule named *HW Loop Temp Schedule* to declare that the temperature at the heating loop outlet and the boiler outlet to be 82 degrees Celsius. This schedule uses a schedule type limit named *Temperature,* which defines the loop upper and lower temperature limits. The compact schedule *ALWAYS\_ON* dictates that the boiler and the cooling coils are On at all times of the day. This schedule uses the *ScheduleTypeLimit (Fraction)* to set the fractional flow rate of the components to 1.
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-
-![](media/image083.png)
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-Figure 83 – Flowchart for heating loop schedules
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-
-
-#### Heating Loop Plant Equipment Operation Schemes
-
-The *PlantEquipmentOperationschemes* object uses the *PlantOnSchedule* and the *HeatSys1 Operation Scheme* objects to set the range of the demand loads for which the boiler is operated during the simulation period. Operation schemes are especially useful and crucial when using multiple active components but it is required to enter set up a plant equipment operation scheme for every *PlantLoop* that is used in a system. A flowchart detailing the heating loop plant equipment operation scheme is provided in Figure 84.
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-
-
-![](media/image084.png)
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-Figure 84 – Flowchart for heating loop plant equipment operation schemes
-
-#### Heating Loop Setpoints
-
-The *HeatSys1 Loop Setpoint Manager* uses the *HW Loop Temp Schedule* to set a temperature control point at the *HeatSys1 Supply Outlet Node*. This setpoint allows the program to control the temperature (set to 82 degrees Celsius) at the node by operating the components in the Heating loop. The Heating Loop also uses another schedule (*HeatSys1 Boiler Setpoint Manager)* to set the temperature of the boiler outlet to 82 degrees Celsius. If the *HeatSys1 Boiler Setpoint Manager* is not entered the program assumes the overall loop setpoint for the boiler outlet node. Since, setpoint managers are high-level control objects, their usefulness is realized in much more complex systems, where multiple nodes have to be monitored in order to operate the system properly. A flowchart for heating loop setpoints is provided in Figure 85.
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-
-![](media/image085.png)
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-Figure 85 – Flowchart for heating loop setpoints
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-
-
-#### Heating Loop Sizing
-
-The Heating Loop is sized such a way that the design loop exit temperature is 82.0 degrees Celsius, and the loop design temperature difference is 11.0 degrees Celsius. A flowchart for the chilled water loop sizing is provided in Figure 86.
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-
-![](media/image086.png)
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-Figure 86 - Flowchart for heating loop sizing
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-
-
-Example System 3: Primary/Secondary Pumping
-===========================================
-
-This example will discuss the basics of primary/secondary pumping systems and some of the controls that are used in managing such systems. The input file for this example can be found under the name: PlantApplicationsGuide\_Example3.idf.
-
-Although it is common for these systems to have a common pipe setup to allow for flow imbalance as shown in Figure 87 and even though there is a provision in EnergyPlus to model common pipes, this example will not discuss them. In the future, the common pipe is expected to be obsolesced, and therefore using a heat exchanger and two separate loops is recommended for future primary/secondary pumping arrangements.
-
-![](media/image087.png)
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-Figure 87 – Example of a common pipe setup
-
-This system services a three zone building by using, two chillers and purchased cooling on the primary chilled water loop to satisfy the demand loads. The chilled water from the supply side of the primary chilled water loop is passes through a plate heat exchanger which serves as the supply side for the secondary chilled water loop. The cooling coil is placed on the demand side of the secondary loop. The primary loop uses a constant speed pump to circulate the working fluid (water). The secondary loop uses a variable speed pump to manipulate the flow of the fluid such that the cooling coil demand is satisfied. The above mentioned pumps are considered as a primary/secondary pumping pair.
-
-Therefore there are four different loops in the system. The cooling loops in the system will be modeled first. The primary cooling loop (‘Primary Chilled Water Loop’) which contains a small chiller, a big chiller and a purchased cooling object on the supply side half loop for supplying chilled water to a fluid to fluid plate heat exchanger on the demand side. The secondary cooling loop (‘Secondary Chilled Water Loop’) contains the fluid to fluid plate heat exchanger on the supply side half loop and a cooling coil on the demand side. The condenser loop (‘Condenser Loop’) which uses a cooling tower to supply cold water to the chillers on the demand side is modeled next. The heating loop (‘Heating Loop’) uses purchased heating to serve the demand loads of three reheat coils places in each of the zones of the buildings, this loop will not be discussed in this application guide because it does not relate to the primary/secondary pumping setup in any way.
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-The plant equipment operation scheme for the primary chilled water loop and the primary/secondary pumping setup are the most important features of this system.
-
-The simple line diagram for the system is shown in Figure 89. The EnergyPlus line diagram is shown in Figure 89.
-
-![](media/image088.png)
-
-Figure 88 - Simple line diagram for the cooling system
-
-
-
-![](media/image089.png)
-
-Figure 89 - EnergyPlus line diagram for the cooling system
-
-Primary Chilled Water Loop – Chiller(s) and purchased cooling
--------------------------------------------------------------
-
-The Secondary Cooling system is constructed by using a *PlantLoop* object. It uses two chillers (a small constant COP chiller and a bigger electric chiller) and purchased district cooling. Therefore, the supply side of the loop contains the chillers and the purchased cooling, and the demand side contains one side of the plate heat exchanger. The loop is operated by using plant equipment operation schemes and schedules. Refer to Figure 90 for a simple diagram of the Primary Cooling Loop.
-
-
-
-![](media/image090.png)
-
-Figure 90 - Simple line diagram for the primary chilled water loop
-
-
-
-### Flowcharts for the Primary Chilled Water Loop Input Process
-
-This series of flowcharts serve as a guide for identifying and inputting the Primary Chilled Water loop and its components into the input file. The working fluid in this loop is water. The EnergyPlus line diagram for this loop is provided in Figure 91. A simple flowchart for the separation of the half loops is provided in Figure 92.
-
-
-
-![](media/image091.png)
-
-Figure 91 - EnergyPlus line diagram for the primary chilled water loop
-
-
-
-![](media/image092.png)
-
-Figure 92 - Simple flowchart for the separation of half-loops in the primary chilled water loop
-
-
-
-
-
-#### Primary Cooling System Supply Side Loop Construction
-
-The main components on the supply side half loop for the primary chilled water loop are two chillers and district cooling object that supply chilled water and the constant speed pump that circulates the chilled water through the loop. This pump (‘CW Primary Circ Pump’) is the primary pump in the primary/secondary pumping setup. This half loop supplies chilled water to the plate heat exchanger which is placed on the demand side half loop. The supply side half loop contains six components, six branches, twelve nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the Primary Cooling loop supply side is provided in Figure 93. The flowchart for supply side branches and components is provided in Figure 94. The flowchart for supply side connectors is provided in Figure 95.
-
-
-
-![](media/image093.png)
-
-Figure 93 - EnergyPlus line diagram for the supply side of the primary chilled water loop
-
-
-
-![](media/image094.png)
-
-Figure 94 – Flowchart for Primary Cooling Loop supply side branches and components
-
-
-
-![](media/image095.png)
-
-Figure 95 – Flowchart for Primary Cooling Loop supply side connectors
-
-
-
-
-
-#### Primary Cooling Loop Demand Side Loop Construction
-
-The main component on the demand side half loop is the plate heat exchanger that facilitates the exchange of heat between the fluids of the primary and secondary chilled water loop. The plate heat exchanger will not be discussed in this loop. Instead the object will be discussed in the supply side half loop of the secondary chilled water loop. This side of the loop also has eight nodes, four components, four branches, and one splitter mixer pair. An EnergyPlus schematic for the demand side is provided in Figure 96. The flowchart for demand side branch definition is provided in Figure 97. The flowchart for the demand side connectors is provided in Figure 98.
-
-**![](media/image096.png)**
-
-Figure 96 - EnergyPlus line diagram for the demand side of the primary chilled water loop
-
-![](media/image097.png)
-
-Figure 97 – Flowchart for primary chilled water loop demand side branches and components
-
-
-
-![](media/image098.png)
-
-Figure 98 – Flowchart for primary chilled water loop demand side connectors
-
-
-
-
-
-
-
-### Flowcharts for Primary Chilled Water Loop Controls
-
-The Primary Cooling loop is operated by using set-points, plant equipment operation schemes and schedules. The plant equipment scheme for the on peak and off peak operation of the chillers is very important
-
-#### Primary Chilled Water Loop Schedules
-
-The Primary Cooling loop uses three different schedules to operate properly. *On Peak* is a compact schedule that defines the on peak hours (9 AM to 6 PM). The *Off Peak* is a compact schedule that defines the off peak hours (6 PM to 9 AM). This plant loop also uses another compact schedule named *CW Loop Temp Schedule* declare that the temperature of the chilled water loop outlet flow is 6.7 degrees Celsius at all times. This schedule is used by the setpoint manager (*Primary CW Loop Setpoint Manager)*. This schedule uses a schedule type limit named *Temperature,* which defines the loop upper and lower temperature limits. The flowchart for Primary Cooling loop schedule definition is provided in Figure 99.
-
-
-
-![](media/image099.png)
-
-Figure 99 – Flowchart for primary chilled water loop schedules
-
-
-
-
-
-#### Primary Chilled Water Loop Plant Equipment Operation Schemes
-
-There are two important operation schemes in the primary chilled water loop. The *CW Loop Operation* plant equipment operation scheme used two schedules (*On Peak* and *off Peak*) to control the supply components in the primary cooling loop. *Peak Operation* is set up such that different components or combinations of components are operated for different values of cooling load during the peak hours (9AM to 6PM everyday) of the simulation period. Up to 25,000 W of cooling load, the small constant COP chiller is operated, for 25,000-245,000 W the big electric chiller and purchased cooling are used and for 245,000-500,000 W purchased cooling is used. This setup serves to increase the efficiency of the system. *Off Peak Operation* is set up such that both the chillers are operated during the off peak hours (6 PM to 9 AM). Flowcharts detailing the chilled water loop plant equipment operation schemes are provided in Figure 100 and Figure 101.
-
-![](media/image100.png)
-
-Figure 100 – Flowchart for on peak operation of the primary chilled water loop
-
-
-
-![](media/image101.png)
-
-Figure 101 - Flowchart for off peak plant operation of the primary chilled water loop
-
-#### Primary Chilled Water Loop Setpoints
-
-The *Primary CW Loop Setpoint Manager* uses the *CW Loop Temp Schedule* to set a temperature control point at the *CW Primary Supply Outlet Node*. This setpoint allows the program to control the temperature at the node by operating the components in the Primary Cooling loop.  Since, setpoint managers are high-level control objects, their usefulness is realized in much more complex systems, where multiple nodes have to be monitored in order to operate the system properly. A flowchart for Secondary Cooling loop setpoints is provided in Figure 102.
-
-
-
-![](media/image102.png)
-
-Figure 102 – Flowchart for Primary Cooling Loop setpoints
-
-
-
-
-
-
-
-
-
-Secondary Chilled Water Loop – Plate Heat Exchanger
----------------------------------------------------
-
-The Secondary Cooling system is constructed by using a *PlantLoop* object, the working fluid in this loop is water. It uses one side of a plate heat exchanger (modeled using a *HeatExchanger:FluidToFluid* object) to supply chilled water to a cooling coil (modeled by using a *Coil:Cooling:DetailedGeometry* object). Therefore, the supply side of the loop contains the heat exchanger and the demand side contains the cooling coil. The loop is operated by using plant equipment operation schemes, and schedules.  Refer to Figure 103 for a simple diagram of the secondary chilled water loop.
-
-
-
-![](media/image103.png)
-
-Figure 103 - Simple line diagram for the secondary chilled water loop
-
-
-
-
-
-### Flowcharts for the Secondary Chilled Water Loop Input Process
-
-This series of flowcharts serve as a guide for identifying and inputting the secondary chilled water loop and its components into the input file. The EnergyPlus line diagram for this loop is provided in Figure 104. A simple flowchart for the separation of the half loops is provided in Figure 105.
-
-
-
-![](media/image104.png)
-
-Figure 104 - EnergyPlus line diagram for the secondary chilled water loop
-
-
-
-![](media/image105.png)
-
-Figure 105 - Simple flow chart for separation on half loops in the secondary chilled water loop
-
-
-
-
-
-#### Secondary Chilled Water Loop Supply Side Loop Construction
-
-The main components on the supply side half loop for the Secondary Cooling System are the plate heat exchanger that supplies the chilled water and the variable speed pump that circulates the chilled water through the loop. The variable speed pump (named ‘CW Sec Circ Pump’) is the secondary pump in the primary/secondary pumping setup. This half loop supplies chilled water to a cooling coil on the demand side half loop. The supply side half loop contains four components, four branches, eight nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the secondary chilled water loop supply side is provided in Figure 106. The flowchart for supply side branches and components is provided in Figure 107. The flowchart for supply side connectors is provided in Figure 108.
-
-
-
-![](media/image106.png)
-
-Figure 106 - EnergyPlus line diagram for the supply side of the secondary chilled water loop
-
-
-
-![](media/image107.png)
-
-Figure 107 – Flowchart for secondary chilled water loop supply side branches and components
-
-
-
-![](media/image108.png)
-
-Figure 108 – Flowchart for secondary chilled water loop supply side connectors
-
-
-
-
-
-#### Secondary Chilled Water Loop Demand Side Loop Construction
-
-The main component on the demand side half loop is the Cooling Coil that cools the air in the building by using the chilled water that is supplied by the plate heat exchanger. This side of the loop also has eight nodes, four components, four branches, and one splitter-mixer pair. An EnergyPlus schematic for the demand side is provided in Figure 109. The flowchart for demand side branch definition is provided in Figure 110. The flowchart for the demand side connectors is provided in Figure 111.
-
-**![](media/image109.png)**
-
-Figure 109 - EnergyPlus line diagram for the demand side of the secondary chilled water loop
-
-
-
-
-
-![](media/image110.png)
-
-Figure 110 – Flowchart for secondary chilled water loop demand side branches and components
-
-
-
-![](media/image111.png)
-
-Figure 111 – Flowchart for secondary chilled water loop demand side connectors
-
-
-
-
-
-
-
-### Flowcharts for secondary chilled water loop Controls
-
-The secondary chilled water loop is operated by using set-points, plant equipment operation schemes and schedules.
-
-#### Secondary Chilled Water Loop Schedules
-
-The flowchart for Primary Cooling loop schedule definition is provided in Figure 112. The Secondary Cooling loop uses two different schedules to operate properly. *ON* is a compact schedule that keeps the plate heat exchanger running at all times of the day, this compact schedule uses a continuous *ScheduleTypeLimit* (*Fraction)* which defines that the value of On is 1 and that of Off is 0. This plant loop also uses another compact schedule named *CW Sec Loop Temp Schedule* declares that the outlet temperature of the Secondary Cooling loop should be 6.67 degrees Celsius at any time; this schedule is used by the setpoint manager (*CW Sec Loop Setpoint Manager)*. This schedule uses a schedule type limit named *Temperature,* which defines the loop upper and lower temperature limits.
-
-
-
-![](media/image112.png)
-
-Figure 112 – Flowchart for secondary chilled water loop schedules
-
-
-
-
-
-#### Secondary Chilled Water Loop Plant Equipment Operation Schemes
-
-The *PlantEquipmentOperationschemes* object uses the *ON* schedule and the *CW Sec Operation Scheme* objects to set the range of the demand loads for which the heat exchanger is operated during the simulation period. A flowchart detailing the secondary chilled water loop plant equipment operation schemes is provided in Figure 113.
-
-
-
-![](media/image113.png)
-
-Figure 113 – Flowchart for secondary chilled water loop plant equipment operation schemes
-
-#### Secondary Chilled Water Loop Setpoints
-
-The *CW Sec Loop Setpoint Manager* uses the *CW Sec Loop Temp Schedule* to set a temperature control point at the *CW Sec Supply Outlet Node*. This setpoint allows the program to control the temperature at the node by operating the components in the Secondary Cooling loop. A flowchart for Secondary Cooling loop setpoints is provided in Figure 114.
-
-
-
-![](media/image114.png)
-
-Figure 114 – Flowchart for secondary chilled water loop setpoints
-
-
-
-#### Secondary Chilled Water Loop Sizing
-
-The secondary chilled water loop is sized such a way that the design loop exit temperature is 6.67 degrees Celsius, and the loop design temperature difference is 5 degrees Celsius. A flowchart for the chilled water loop sizing is provided in Figure 115.
-
-
-
-![](media/image115.png)
-
-Figure 115 – Flowchart for secondary chilled water loop sizing
-
-Primary/Secondary Pumping
--------------------------
-
-As mentioned in sections *Primary Cooling System Supply Side Loop Construction* and *Secondary Chilled Water Loop Supply Side Loop Construction*, the CW primary Circ Pump and the CW Sec Circ Pump function as the primary/secondary (respectively) pumping system. The primary pump is a constant speed pump that circulates chilled water at a constant flow rate through one side the plate heat exchanger in the primary chilled water loop. The secondary pump is a variable speed pump that circulates chilled water at a variable flow rate through the other side of the plate heat exchanger depending on the demand load.
-
-Condenser Loop - Cooling Tower
-------------------------------
-
-The Condenser Loop is constructed by using a *PlantLoop* object. It uses a cooling tower (modeled by using a *CoolingTower:SingleSpeed* object class) and a variable speed pump (modeled by using a *Pump:VariableSpeed)* to supply cooling water to the chillers in the primary cooling loop. Therefore, the supply side of the loop contains the Cooling Tower and the demand side contains the chillers. The loop is operated by using plant equipment operation schemes, and schedules.  Refer to Figure 116 for a simple diagram of the Condenser Loop.
-
-
-
-![](media/image116.png)
-
-Figure 116 - Simple line diagram for the condenser loop
-
-
-
-### Flowcharts for the Condenser Loop Input Process
-
-This series of flowcharts serve as a guide for identifying and inputting the Condenser Loop and its components into the input file. The EnergyPlus line diagram for this loop is provided in Figure 117. A simple flowchart for the separation of the half loops is provided in Figure 118.
-
-![](media/image117.png)
-
-Figure 117 - EnergyPlus line diagram for the condenser loop
-
-
-
-
-
-![](media/image118.png)
-
-Figure 118 - Simple flow chart for separation on half loops in the condenser loop
-
-
-
-
-
-#### Condenser Loop Supply Side Construction
-
-The main components on the supply side half loop for the Condenser Loop are the Cooling Tower that supplies the cooling water and the variable speed pump that circulates the cooling water through the loop. This half loop supplies cooling water to the chillers on the demand side half loop. The supply side half loop contains four components, four branches, eight nodes, and one splitter-mixer pair. The EnergyPlus line diagram for the Condenser loop supply side is provided in Figure 119. The flowchart for supply side branches and components is provided in Figure 120. The flowchart for supply side connectors is provided in Figure 121.
-
-
-
-![](media/image119.png)
-
-Figure 119 - EnergyPlus line diagram for the supply side of the Condenser Loop
-
-
-
-![](media/image120.png)
-
-Figure 120 – Flowchart for Condenser Loop supply side branches and components
-
-
-
-![](media/image121.png)
-
-Figure 121 – Flowchart for Condenser Loop supply side connectors
-
-
-
-
-
-#### Condenser Loop Demand Side Construction
-
-The main components on the demand side half loop are the small constant COP chiller and the bigger electric chiller that use the cooling water supplied by the cooling tower. The chillers are in turn used to supply chilled water in the Primary Cooling loop.  This side of the loop also has ten nodes, five components, five branches and one splitter-mixer pair. An EnergyPlus schematic for the demand side is provided in Figure 122. The flowchart for demand side branch definition is provided in Figure 123. The flowchart for the demand side connectors is provided in Figure 123.
-
-**![](media/image122.png)**
-
-Figure 122 - EnergyPlus line diagram for the demand side of the Condenser Loop
-
-![](media/image123.png)
-
-Figure 123 – Flowchart for Condenser Loop demand side branches and components
-
-
-
-![](media/image124.png)
-
-Figure 124 – Flowchart for Condenser Loop demand side connectors
-
-
-
-
-
-
-
-### Flowcharts for Condenser Loop Controls
-
-The Condenser loop is operated by using set-points, plant equipment operation schemes and schedules.
-
-#### Condenser Loop Schedules
-
-The flowchart for condenser loop schedule definition is provided in Figure 125. The Condenser loop uses one schedule to operate properly. *ON* is a compact schedule that keeps the Cooling Tower On at all times of the day, this compact schedule uses a continuous *ScheduleTypeLimit* (*Fraction)* which defines that the value of On is 1 and that of Off is 0.
-
-
-
-![](media/image125.png)
-
-Figure 125 – Flowchart for condenser loop schedules
-
-
-
-#### Condenser Loop Plant Equipment Operation Schemes
-
-The *PlantEquipmentOperationschemes* object uses the *ON* schedule and the *Tower Operation* objects to set the range of demand loads for which the cooling tower is operated during the simulation period. A flowchart detailing the Condenser Loop plant equipment operation schemes is provided in Figure 126.
-
-
-
-![](media/image126.png)
-
-Figure 126 – Flowchart for Condenser Loop plant equipment operation schemes
-
-#### Condenser Loop Setpoints
-
-The *MyCondenserControl* setpoint manager places a temperature setpoint at the *Condenser Supply Outlet Node.* The temperature at this point is controlled with respect to the outdoor air wet bulb temperature at that point in the simulation. The outdoor air wet bulb temperature is obtained from the weather data at the location of the simulation. A flowchart for Secondary Cooling loop setpoints is provided in Figure 127.
-
-
-
-![](media/image127.png)
-
-Figure 127 – Flowchart for Condenser Loop setpoints
-
-
-
-
-
-
-
-References
-==========
-
-Reed, M. A., Davis, C. 2007, “Chilled Water Plant Savings at No Cost.� *ASHRAE Journal* 49(7), 38-44.
-
-Hyman, L. B., Little, D. 2004, “Overcoming Low Delta T, Negative Delta P At Large University Campus.� *ASHRAE Journal* 46(2), 28-34.
-
-
diff --git a/doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/Tips_and_Tricks_Using_EnergyPlus.md b/doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/Tips_and_Tricks_Using_EnergyPlus.md
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-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Tips &amp; Tricks for Using EnergyPlus</h1>
-<h2>Insider secrets to Using EnergyPlus</h2>
-<br/>
-<p><i>(just don’t tell anyone...)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-Introduction & Support
-======================
-
-This is a quick guide for using and troubleshooting EnergyPlus simulation software. The information here is taken from the knowledge base and from EnergyPlus users looking for answers.
-
-**Note that these articles are taken from actual user questions and may not be applicable to your model.**
-
-For more detailed information about using EnergyPlus, refer to the user guides and manuals that are installed in the Documentation folder and are also available from [www.energyplus.gov](http://www.energyplus.gov).
-
-This is a short guide
-
-… meant to save time and energy!
-
-Organization
-------------
-
-The organization of this document roughly uses the categories of the new features documents that have been included with EnergyPlus since April 2001 (the initial offering).
-
-Under the subject categories, there may be a mix of short articles and Q&A format.
-
-EnergyPlus Support
-------------------
-
-The primary EnergyPlus support site is supplied at: http://energyplus.helpserve.com
-
-The site is monitored by EnergyPlus developers and questions are attempted to be answered in a timely manner. Standard EnergyPlus support is provided free of charge by the U.S. Deparment of Energy, as part of a continuing effort to improve the EnergyPlus building simulation tool. Expedited, priority support may be available from other sources. The helpdesk has a files area where important (after release) files may be put as well as the storage for the Transition file set that are prior to the current release.
-
-http://simulationresearch.lbl.gov/EP/ep_consult.html is a list of EnergyPlus consultants.
-
-Yahooâ„¢ Groups is also used as a peer to peer discussion group. To join the group (which now has about 2,600 participants), visit [http://groups.yahoo.com/group/EnergyPlus\_Support](http://groups.yahoo.com/EnergyPlus_Support) The Yahoo group has some file storage capabilities and that is also where the Meteonormâ„¢ files that supplement the primary EnergyPlus weather data are housed. The Yahoo group may not be monitored by EnergyPlus developers.
-
-A similar Yahoo group has been set up for collaborative developers.
-
-General
-=======
-
-What EnergyPlus Is
-------------------
-
-The primary website for EnergyPlus is http://www.energyplus.gov
-
-EnergyPlus is an energy analysis and thermal load simulation program. Based on a user’s description of a building from the perspective of the building’s physical make-up, associated mechanical systems, etc., EnergyPlus will calculate the heating and cooling loads necessary to maintain thermal control set points, conditions throughout a secondary HVAC system and coil loads, and the energy consumption of primary plant equipment as well as many other simulation details that are necessary to verify that the simulation is performing as the actual building would. More details on what EnergyPlus is can be found in the [GettingStarted Document](file:///E:\Docs4PDFs\GettingStarted.pdf).
-
-No program is able to handle every simulation situation. However, it is the intent of EnergyPlus to handle as many building and HVAC design options either directly or indirectly through links to other programs in order to calculate thermal loads and/or energy consumption on for a design day or an extended period of time (up to, including, and beyond a year).
-
-What EnergyPlus Isn’t
----------------------
-
-- a user interface. It is intended to be the simulation engine around which a third-party interface can be wrapped. Inputs and outputs are simple ASCII text that is decipherable but may be best left to a GUI (graphical user interface). The current known third-party interfaces/tools can be found at
-
-http://apps1.eere.energy.gov/buildings/energyplus/interfaces_tools.cfm
-
-- a life cycle cost analysis tool. It produces results that can then be fed into an LCC program.
-
-- an architect or design engineer replacement. It does not check input, verify the acceptability or range of various parameters (expect for a limited number of very basic checks), or attempt to interpret the results. However, it does have several reporting features to help you do exactly that.
-
-Getting Started
----------------
-
-If you’re familiar with building simulation, use the 300+ example files that come with the program and the Input/Output Reference to help you.
-
-If you’re new to building simulation, read and work through the tutorials in the “Getting Started� document or visit the online tutorial, http://www.vibyor.com (tutorial was created by Prof. Vishal Garg from IIIT Hyberabad, India).
-
-Another avenue you might use is the EnergyPlus Example File Generator (EEFG) program, which will not only produce an input file for your later use, but also run your specifications on EnergyPlus and send you the results. EEFG is available through the interface page referenced above or http://apps1.eere.energy.gov/buildings/energyplus/cfm/inputs/
-
-Comparing EnergyPlus to Other Programs
---------------------------------------
-
-A paper comparing and contrasting Energy Simulation Programs can be found here:
-
-http://www.eere.energy.gov/buildings/tools_directory/pdfs/contrasting_the_capabilities_of_building_energy_performance_simulation_programs_v1.0.pdf
-
-As this paper was published in 2005, it is out of date (at least with current EnergyPlus capabilities).
-
-The feature highlights from EnergyPlus releases can be seen here:
-
-http://apps1.eere.energy.gov/buildings/energyplus/pdfs/featurehighlights.pdf
-
-In addition you can see how EnergyPlus compares to other programs (which have submitted their models) in our testing reports:
-
-http://apps1.eere.energy.gov/buildings/energyplus/testing.cfm
-
-DataSets
-========
-
-Datasets aka Libraries
-----------------------
-
-EnergyPlus uses the term DataSets for what many would call libraries. These files are included, for the most part, in the instalation package but may be available from other sites (such as the helpdesk or Yahoo Groups).
-
-There are two flavors of DataSets: **simple** and **Macro**. Some sets have files in both camps (for example, Solar Collectors). Both flavors contain IDF objects ready to be put into EnergyPlus input files. With the simple datasets, you may need to use a text editor or the IDF Editor to search the file for the one you want to use.  With the macro datsets and a simply structured imf (input macro file), you can name the item you want to include. (The macro program is described in the [Auxiliary Programs document](file:///E:\Docs4PDFs\AuxiliaryPrograms.pdf)).
-
-Primary documentation for each dataset is found in the [Output Details and Examples document](file:///E:\Docs4PDFs\OutputDetailsAndExamples.pdf). Highlights of some datasets are given here.
-
-Locations-DesignDays
---------------------
-
-This file (Locations-DesignDays.xls) can be found in the MacroDataSets folder. While not strictly a macro file, it leads one to be able to download the ASHRAE design day definitions from the EnergyPlus website. The spreadsheet format contains a sheet for each of the WMO regions as well as the California Climate Zones, specifically sheets included are:
-
-- Readme – an upfront readme page
-
-- WMO1 Africa
-
-- WMO2 Asia
-
-- WMO3 South America
-
-- WMO4 North & Central America
-
-- CZ Files – California Climate Zones
-
-- WMO5 Southwest Pacific
-
-- WMO6 Europe
-
-- WMO7 Antarctica
-
-Each WMO (World Meteorological Organization) page contains the countries represented, specific cities that have design conditions data from ASHRAE, a link to the full imf file with location, daylighting saving and design day definitions as well as a link to that region’s weather page on the EnergyPlus website. Pressing the links here will allow you to download the files.
-
-
-
-Design Day / Weather Data
-=========================
-
-Design Day Creation
--------------------
-
-*How do I create the profile used in the SizingPeriod:DesignDay object?*
-
-Typically, the EnergyPlus Development Team uses the data from the most recent ASHRAE Handbook of Fundamentals to create a set of design day profiles that can be used. Description of ASHRAE’s data is contained in Chapter 14 of the 2009 Handbook of Fundamentals. Table 1 shows the kind of data that is embodied in the design day definitions shown earlier (ref. Locations-DesignDays).
-
-Design Days (aka Design Conditions) are very important for use in HVAC Sizing calculations – refer to the ASHRAE Handbook of Fundamentals for further information.
-
-From this, you can determine if you should use one of these profiles and modify it or determine how to create your own profile.
-
-The Weather Converter program accesses this file when it processes (even for statistics) a weather file. Design Day definitions are also included with the zips on the EnergyPlus weather data site. For locations that don’t have ASHRAE design conditions, the Weather Converter uses the data within the weather file to generate pseudo conditions in the statistics file.
-
-EPW Weather Files
------------------
-
-The WeatherConverter converts from other source formats to EPW and EnergyPlus CSV formats. The WeatherConverter also produces a statistics file that provides a quick synopsis of the converted data and is used by the tabular reports (ref: Climatic Data Summary report). For Ecotect users, the Weather Converter can also save as .wea format. We do not support conversion of EPWs to other formats, including to TMY2. The Weather Converter is described in detail in the [Auxiliary Programs document](file:///E:\Docs4PDFs\AuxiliaryPrograms.pdf).
-
-Meteonorm Weather Files
------------------------
-
-For locations that aren’t on the regular EnergyPlus weather site (http://apps1.eere.energy.gov/buildings/energyplus/cfm/weather_data.cfm ), the team has created weather data using the Meteonorm™ software. Meteonorm extrapolates hourly data from statistical data for a location. Where statistical data aren't available, Meteonorm interpolates from other nearby sites. Generally, a statistical approach is a last resort—weather files generated from statistics will not demonstrate the normal hour-to-hour and day-to-day variability seen in measured data. Each .ZIP includes a .STAT (EnergyPlus weather data statistics), .EPW (EnergyPlus weather file), and .INFO (Information about the source data and limitations from Meteonorm).
-
-In all cases, review the .STAT file for the location before using any of these files to ensure that it represents the climate of the locations as you understand it. In many cases, a nearby location with measured data may be more appropriate than one derived from statistics. These files, once created, are published on the EnergyPlus Yahoo Group site.
-
-As always, if you know of sources of weather data that we might be able to share with the EnergyPlus community, please contact us.
-
-Weather Data for Simulations
-----------------------------
-
-Weather data can be used for various purposes by simulation program such as EnergyPlus. For some purposes, such as validating a model to actual energy use, you may wish to match the weather data to the simulation period. However, for most purposes, you will wish to have a more typical weather data profile. Information on selecting weather data is described in this paper:
-
-Drury B. Crawley. 1998. "Which Weather Data Should You Use for Energy Simulations of Commercial Buildings?" in ASHRAE Transactions, pp. 498-515, Vol. 104, Pt. 2. Atlanta: ASHRAE. (PDF 197 KB)
-
-PDF: http://energyplus.gov/pdfs/bibliography/whichweatherdatashouldyouuseforenergysimulations.pdf
-
-Weather File Sources
---------------------
-
-The description of sources for the EnergyPlus weather data that is on the website are available here: http://apps1.eere.energy.gov/buildings/energyplus/weatherdata_sources.cfm
-
-Measuring Solar Data
---------------------
-
-*Can the following weather file metrics be directly measured by some inexpensive devices?*
-
-Extraterrestrial Horizontal Radiation {Wh/m2}
- Extraterrestrial Direct Normal Radiation {Wh/m2}
- Horizontal Infrared Radiation Intensity from Sky {Wh/m2}
- Global Horizontal Radiation {Wh/m2}
- Direct Normal Radiation {Wh/m2}
- Diffuse Horizontal Radiation {Wh/m2}
- Global Horizontal Illuminance {lux}
- Direct Normal Illuminance {lux}
- Diffuse Horizontal Illuminance {lux}\*
-
-You can't measure extraterrestrial unless you're in outer space, but then it's assumed to be constant anyway. For the various radiation and illuminance values, they can measured by various instrumentation ranging from the very cheap to the very expensive. Properly, radiation needs to be measured with a pyranometer (Eppley), which is pricy, but I'm also seen people use simpler apparatus (Lycors) that are really photometers. Direct beam is generally not measured, but derived by subtracting the diffuse from the global. Diffuse is measured by adding a shadow band over a pyranometer to block out the direct beam. Pyranometers measure heat, photometers measure light. All the illuminance on the weather files are derived from the radiation and sky conditions.
-
-Do not forget that the quantities you list are the inputs to the models that are used to derive the variables you really need in practice: irradiance and illuminance on the facets of the building (windows especially). These facets are usually NOT horizontal. Measuring all the components for all tilts and azimuths can be a costly proposition, and that's why it is rarely done (hence the need for models), but that's what should be done in serious experiments to remove the (large) uncertainties in modeled radiation.
-
-Illuminance is measured with photometers (from, e.g., Licor), which resemble silicon-based pyranometers. Both are less costly than thermopile radiometers, which are normally the best in terms of accuracy. Measurements obtained with silicon-based pyranometers need various corrections to account for their limited spectral range. No correction is needed for photometers, though. So you have this issue of accuracy vs cost to consider.
-
-Direct irradiance is measured with a pyrheliometer, which tracks the sun and is therefore costly, but also the most accurate of all radiometers. Obtaining direct irradiance by subtracting diffuse from global is convenient, but not accurate, as shown in recent publications.
-
-Input
-=====
-
-Creating Files for EnergyPlus
------------------------------
-
-The install package includes the IDF Editor (Windows platform) for creating EnergyPlus Input Files (aka IDFs). Likewise, text editors such as NotePad or WordPad can be used to create flat ASCII files for use with EnergyPlus.
-
-### dxf or dwg CAD Files
-
-*How can I convert dxf or dwg CAD files to EnergyPlus?*
-
-Several EnergyPlus interfaces, including DesignBuilder and OpenStudio (plug in for Google SketchUp), allow you to import the dxf drawings and trace over them to create EnergyPlus geometry. If you have the full AutoCAD 3-D dwg model (more than just dxf), then you might be able to export to EnergyPlus using one of the available utilities that work with AutoCAD, but only if the model was created in the correct way to support these tools. As of February 2009, Green Building Studio and EnergyPlugged (a plug in to AutoCAD) support export to EnergyPlus.
-
-For more information about current tools which support EnergyPlus, see http://www.energyplus.gov/interfaces_tools.cfm.
-
-### OpenStudio for Google Sketchup
-
-[OpenStudio](http://apps1.eere.energy.gov/buildings/energyplus/openstudio.cfm) is a free plugin for the Google SketchUp 3D drawing program. The plugin makes it easy to create and edit the building geometry in your EnergyPlus input files. The plugin also allows you to launch EnergyPlus simulations and view the results without leaving SketchUp.
-
-### EnergyPlus Example File Generator
-
-A Web-based service is available that creates and runs EnergyPlus input files for simple models of commercial buildings. The input files (and annual results summary files) are sent to your e-mail address as attachments. You can access the service and customize the characteristics of the building you want to model on the [EnergyPlus Example File Generator Application](http://apps1.eere.energy.gov/buildings/energyplus/cfm/inputs/) (pop-ups must be enabled). Learn more by viewing the [EnergyPlus Building Data Input Forms Help](http://apps1.eere.energy.gov/buildings/energyplus/cfm/inputs/help.cfm) File.
-
-Converting Older Version EnergyPlus Files
------------------------------------------
-
-*Can I convert an older file to a newer version of EnergyPlus?*
-
-If the older version is from the previous release, then yes. Use the pull-down File menu and select Transition. This will update the older file to the newer version.
-
-If the older version is older than the previous release, then you must use the multiple transition program. You can download the transition programs from this site.
-
-(That is http://energyplus.helpserve.com and go to the “downloads� area).
-
-The Multiple Transition folder is set up on the EnergyPlus install.
-
-Unzip the file into the MultipleTransition folder and use the IDF Converter GUI program to transition your older files. The IDF converter can also save the transitioned file for each intermediate version, if desired.
-
-Using Macros and Editing Inputs in IDF Editor
----------------------------------------------
-
-*How can I use macros, and continue to edit my input in IDF editor?*
-
-*(Using or ignoring macros in the IDF editor is a potential Enhancement List item.)*
-
-1)   Separate files into "IDF editable" and "macro" (actually, the AbsorptionChiller\_Macro.imf example file shows a little of this but it doesn't really use macros). For the pieces you think you'd like to manipulate in the IDF editor, call them with extension IDF. For the others, they would be IMF and the master file would be IMF with "includes" of your IDF pieces.
-
-2)   Use the expanded IDF (extension epmidf) file for your IDF editor changes and then run it from there.
-
-Getting data from WINDOW program
---------------------------------
-
-The WINDOW program is published from LBNL at http://windows.lbl.gov/software. More specifics on the program and its details are shown in the Input Output Reference under “Importing Windows from WINDOW program� topic.
-
-### EnergyPlus IDF Excerpt Data
-
-The preferred method of using WINDOW data in EnergyPlus is to excerpt or “report� a specific Window from the Window library screen (see below):
-
-![](media/image001.jpg)
-
-Figure 1. WINDOW screen for exporting IDF Window specifications
-
-The file can then be saved at a location of your choice and added into your overall simulation IDF file.
-
-### WINDOW Data File
-
-The other “older� option for creating data for EnergyPlus is to use the “EnergyPlus� option above and create a WindowDataFile. The general format of this data is described in the following paragraphs and must use the Construction:WindowDataFile object and an external file to be used in EnergyPlus. While this is a convenient small file (that can contain multiple windows), there is no way to import this file back into WINDOW and obtain the above, more preferred method.
-
-Please note that there is a bug in WINDOW 5 that causes two of the lines in the EnergyPlus data file to be joined. This bug is fixed in versions of Window 5.02 (and above). To be sure, you can check the data file for a line that looks like:
-
-GLAZING SYSTEM OPTICAL DATAAngle     0    10    20    30    40    50    60    70    80    90 Hemis
-
-The fixed version of the program will not show the above line; rather, there will be two lines such as shown below. If you have the above condition, with an editor you would break this into two lines:
-
-GLAZING SYSTEM OPTICAL DATA
-
-Angle     0    10    20    30    40    50    60    70    80    90 Hemis
-
-In EnergyPlus, the Window data file is searched for each “Construction:WindowDataFile� object in the EnergyPlus input. This object has a very simple form:
-
-Construction:WindowDataFile,
-
-ConstructionName,
-
-FileName; ! Default is Window5DataFile.dat in the “run� folder.
-
-If there is a window called ConstructionName on the Window data file, the data for that window is read from the file and the following EnergyPlus objects and their names are created. The “W5� prefixed to these names indicates that the object originated in the Window5 data file.
-
-- **WindowMaterial:Glazing** for each of the glass layers. They will be named **W5:ConstructionName:GLASS1**, **W5:ConstructionName:GLASS2** , etc.
-
-- **WindowMaterial:Gas** or **WindowMaterial:GasMixture** for each of the gap layers. They will be named **W5:ConstructionName:GAP1**, **W5:ConstructionName:GAP2** , etc.
-
-- **WindowProperty:FrameAndDivider** (if the window on the Window5 data file has a frame and/or divider). It will be named **W5:ConstructionName**. This WindowProperty:FrameAndDivider will be assigned to any window on the input file that has a construction called “ConstructionName� *even if that window has  referenced another WindowProperty:FrameAndDivider (i.e., if WindowProperty:FrameAndDivider Name for that window is specified).* In this case a warning will result.
-
-Note that:
-
-An entry on the WINDOW data file usually has just one glazing system. It is also possible to have an entry with two glazing systems separated by a horizontal or vertical mullion. In this case, the two glazing systems can have different dimensions and different properties. For example, one of the two glazing systems could be single glazed and the other could be double glazed. An example  of the two glazing system case is given in the sample WINDOW data file shown below (although in this case the properties of the two glazing systems are the same).
-
-EnergyPlus handles the “one glazing system� and “two glazing systems� cases differently. If there is one glazing system, the glazing system height and width from the Window5 data file are not used. Instead, the window dimensions are obtained from the window vertices that have been specified on the IDF file. However, a warning message will result if the height or width calculated from the window’s vertex inputs differs from the corresponding Window5 data file values by more than 10%. This warning is given since the effective frame and edge-of-glass conductances on the WINDOW data file can depend on the window dimensions if the frame is non-uniform, i.e., consists of sections with different values of width, projection, or thermal properties.
-
-If the WINDOW data file entry has two glazing systems, System1 and System2, the following happens, as shown in the figure below. Assume that the original window is called WinOriginal. System1 is assigned to WinOriginal. Then EnergyPlus automatically creates a second window, called WinOriginal:2, and assigns System2 to it. The dimensions of WinOriginal are ignored; the dimensions of System1 on the data file are assigned to it, but the position of the lower left-hand vertex of WinOriginal is retained. The dimensions of System2 on the data file are assigned to WinOriginal:2. The lower left-hand vertex of WinOriginal:2 is determined from the mullion orientation and width.
-
-**Note: WinOriginal would have been the IDF window definition – it’s dimensions will be overridden by the systems dimensions from the Window data file. Two windows will be made and called WinOriginal and WinOriginal:2.**
-
-
-
-![](media/image002.png)
-
-Figure 2. Window Glazing system with dual glazing constructions
-
-The Window Data File contains no information on shading devices. See “Specify the Material Name of the Shading Device� under WindowProperty:ShadingControl for a method to attach a shading layer to windows read in from this file.
-
-Following is an example WINDOW data file for a slider window with two identical double low-E glazing systems separated by a horizontal mullion. Each system has a frame and divider. Note that all dimensions, such as glazing height and width, are in millimeters; when EnergyPlus reads the file these are converted to meters. Following the data file example is a description of the contents of the file. That data used by EnergyPlus is shown in bold.
-
-
-
-Window5 Data File for EnergyPlus
-
-&lt;WINDOW program version&gt;
-
-Date             : Tue Nov 13 17:07:40 2001
-
-Window name      : **DoubleLowE**
-
-Description      : Horizontal Slider, AA
-
-\# Glazing Systems: **2**
-
-GLAZING SYSTEM DATA: Height Width nPanes Uval-center SC-center SHGC-center Tvis-center
-
- System1         :   1032   669      2      1.660      0.538      0.467       0.696
-
- System2         :   1033   669      2      1.660      0.538      0.467       0.696
-
-FRAME/MULLION DATA: Width OutsideProj InsideProj Cond EdgeCondRatio SolAbs VisAbs Emiss  Orient'n (mull)
-
-    L Sill       :   97.3     25.4       25.4   500.000    1.467     0.500  0.500  0.90
-
-    R Sill       :   97.3     25.4       25.4   500.000    1.467     0.500  0.500  0.90
-
-    L Head       :   70.2     25.4       25.4   18.822     1.490     0.500  0.500  0.90
-
-    R Head       :   70.2     25.4       25.4   18.822     1.490     0.500  0.500  0.90
-
-    Top L Jamb   :   54.3     25.4       25.4   31.141     1.503     0.500  0.500  0.90
-
-    Bot L Jamb   :   54.3     25.4       25.4   500.000    1.494     0.500  0.500  0.90
-
-    Top R Jamb   :   70.2     25.4       25.4   500.000    1.518     0.500  0.500  0.90
-
-    Bot R Jamb   :   97.6     25.4       25.4   264.673    1.547     0.500  0.500  0.90
-
-    Mullion      :   53.5     25.4       25.4   500.000    1.361     0.500  0.500  0.90 **Horizontal**
-
-    Average frame:   **75.5     25.4       25.4   326.149    1.464     0.500  0.500  0.90**
-
-DIVIDER DATA     : Width OutsideProj InsideProj Cond EdgeCondRatio SolAbs VisAbs Emiss Type            \#Hor \#Vert
-
- System1         :  **25.4    25.4       25.4    3.068      1.191     0.500  0.500 0.900 DividedLite       2    3**
-
- System2         :  **25.4    25.4       25.4    3.068      1.191     0.500  0.500 0.900 DividedLite       2    3**
-
-GLASS DATA       : Layer\#  Thickness  Cond Tsol Rfsol Rbsol Tvis Rfvis Rbvis  Tir  EmissF  EmissB  SpectralDataFile
-
- System1         :   1      **3.00     0.900** 0.50  0.33  0.39 0.78  0.16  0.13 **0.00   0.16    0.13**   CMFTIR\_3.AFG
-
-                     2      **6.00     0.900** 0.77  0.07  0.07 0.88  0.08  0.08 **0.00   0.84    0.84**   CLEAR\_6.DAT
-
- System2         :   1      **3.00     0.900** 0.50  0.33  0.39 0.78  0.16  0.13 **0.00   0.16    0.13**   CMFTIR\_3.AFG
-
-                     2      **6.00     0.900** 0.77  0.07  0.07 0.88  0.08  0.08 **0.00   0.84    0.84**   CLEAR\_6.DAT
-
-GAP DATA         : Gap\# Thick nGasses
-
- System1         :   1  **12.70    1**
-
- System2         :   1  **12.70    1**
-
-GAS DATA         : GasName Fraction MolWeight ACond   BCond  CCond AVisc   BVisc   CVisc ASpHeat  BSpHeat CSpHeat
-
- System1 Gap1    : Air     **1.0000   28.97    0.002873 7.76e-5 0.0 3.723e-6 4.94e-8 0.0   1002.737 0.012324 0.0**
-
- System2 Gap1    : Air     **1.0000   28.97    0.002873 7.76e-5 0.0 3.723e-6 4.94e-8 0.0   1002.737 0.012324 0.0**
-
-GLAZING SYSTEM OPTICAL DATA
-
-Angle     0    10    20    30    40    50    60    70    80    90 Hemis
-
-System1
-
-Tsol  **0.408 0.410 0.404 0.395 0.383 0.362 0.316 0.230 0.106 0.000 0.338**
-
-Abs1  **0.177 0.180 0.188 0.193 0.195 0.201 0.218 0.239 0.210 0.001 0.201**
-
-Abs2  **0.060 0.060 0.061 0.061 0.063 0.063 0.061 0.053 0.038 0.000 0.059**
-
-Rfsol **0.355 0.350 0.348 0.350 0.359 0.374 0.405 0.478 0.646 0.999 0.392**
-
-Rbsol **0.289 0.285 0.283 0.282 0.285 0.296 0.328 0.411 0.594 1.000 0.322**
-
-Tvis  **0.696 0.700 0.690 0.677 0.660 0.625 0.548 0.399 0.187 0.000 0.581**
-
-Rfvis **0.207 0.201 0.198 0.201 0.212 0.234 0.278 0.374 0.582 0.999 0.260**
-
-Rbvis **0.180 0.174 0.173 0.176 0.189 0.215 0.271 0.401 0.648 1.000 0.251**
-
-System2
-
-Tsol  **0.408 0.410 0.404 0.395 0.383 0.362 0.316 0.230 0.106 0.000 0.338**
-
-Abs1  **0.177 0.180 0.188 0.193 0.195 0.201 0.218 0.239 0.210 0.001 0.201**
-
-Abs2  **0.060 0.060 0.061 0.061 0.063 0.063 0.061 0.053 0.038 0.000 0.059**
-
-Rfsol **0.355 0.350 0.348 0.350 0.359 0.374 0.405 0.478 0.646 0.999 0.392**
-
-Rbsol **0.289 0.285 0.283 0.282 0.285 0.296 0.328 0.411 0.594 1.000 0.322**
-
-Tvis  **0.696 0.700 0.690 0.677 0.660 0.625 0.548 0.399 0.187 0.000 0.581**
-
-Rfvis **0.207 0.201 0.198 0.201 0.212 0.234 0.278 0.374 0.582 0.999 0.260**
-
-Rbvis **0.180 0.174 0.173 0.176 0.189 0.215 0.271 0.401 0.648 1.000 0.251**
-
-
-
-**Description of Contents of WINDOW Data File**
-
-
-
-(Quantities used in EnergyPlus are in bold; others are informative only)
-
-
-
-Second line = version of WINDOW used to create the data file
-
-*Date* = date the data file was created
-
-***Window name*** = name of this window; chosen by WINDOW5 user; EnergyPlus user enters the same name in EnergyPlus as name of a “Construction from Window5 Data File� object. EnergyPlus will search the Window5 data file for an entry of this name.
-
-*Description* = One-line description of the window; this is treated as a comment.
-
-***\# Glazing Systems***: 1 or 2; value is usually 1 but can be 2 if window has a horizontal or vertical mullion that separates the window into two glazing systems that may or may not be different.
-
-
-
-GLAZING SYSTEM DATA
-
-*System1, System2*: separate characteristics given if window has a mullion.
-
-***Height***, \****width*** = height and width of glazed portion (i.e., excluding frame; and, if mullion present, excluding mullion).
-
-***nPanes***     = number of glass layers
-
-*Uval-center* = center-of-glass U-value (including air films) under standard winter conditions\*  (W/m2)
-
-*SC-center*  = center-of-glass shading coefficient under standard summer conditions\*.
-
-*SHCG-center* = center-of-glass solar heat gain coefficient under standard summer conditions\*.
-
-*Tvis-center* = center-of-glass visible transmittance at normal incidence
-
-
-
-FRAME/MULLION DATA
-
-*L,R Sill*   = left, right sill of frame
-
-*L,R Head*   = left, right header of frame
-
-*Top L, Bot L jamb* = top-left, bottom-left jamb of frame
-
-*Bot L, Bot R jamb* = bottom-left, bottom-right jamb of frame
-
-***Average frame*** = average characteristics of frame for use in EnergyPlus calculation. If mullion is present, original window is divided into two separate windows with the same average frame (with the mullion being split lengthwise and included in the average frame).
-
-***Width***     = width (m)
-
-***OutsideProj*** = amount of projection from outside glass (m)
-
-***InsideProj*** = amount of projection from inside glass (m)
-
-***Cond*** = effective surface-to-surface conductance (from THERM calculation) (W/m2)
-
-***EdgeCondRatio*** = ratio of surface-to-surface edge-of-glass conductance to surface-to-surface center-of-glass conductance (from THERM calculation)
-
-***SolAbs***    = solar absorptance
-
-***VisAbs***    = visible absorptance
-
-***Emiss***     = hemispherical thermal emissivity
-
-***Orientation*** = Horizontal or Vertical (mullion only); = None if no mullion.
-
-
-
-DIVIDER DATA
-
-***Width*** through ***Emiss*** are the same as for FRAME/MULLION DATA
-
-***\#Hor***     = number of horizontal dividers
-
-***\#Vert***     = number of vertical dividers
-
-***Type***      = DividedLite or Suspended
-
-
-
-GLASS DATA
-
-*System1, System2*: separate characteristics are given if window has a mullion.
-
-***Cond***       = conductivity (W/m-K)
-
-*Tsol*       = spectral-average solar transmittance at normal incidence
-
-*Rfsol*      = spectral-average front solar reflectance at normal incidence
-
-*Rbsol*      = spectral-average back solar reflectance at normal incidence
-
-*Tvis*       = spectral-average visible transmittance at normal incidence
-
-*Rfvis*      = spectral-average front visible reflectance at normal incidence
-
-*Rbvis*      = spectral-average back visible reflectance at normal incidence
-
-***Tir***       = hemispherical IR transmittance
-
-***EmissF***    = hemispherical front emissivity
-
-***EmissB***    = hemispherical back emissivity
-
-SpectralDataFile = name of spectral data file with wavelength-dependent transmission and reflection data used by WINDOW 5 to calculate the glazing system optical data. “None� will appear here if spectral-average data for this glass layer were used by WINDOW 5.
-
-
-
-GAP DATA
-
-System1, System2: separate characteristics are given if the window has a mullion.
-
-***Thick***    = thickness (m)
-
-***nGasses***  = number of gasses (1, 2 or 3)
-
-GasName   = name of the gas
-
-***Fraction***  = fraction of the gas
-
-***MolecWeight*** = molecular weight of the Nth gas
-
-(In the following, conductivity, viscosity and specific heat as a function
-
-of temperature, T (deg K), are expressed as A + B\*T + C\*T^2)
-
-***ACond***     = A coeff of conductivity (W/m-K)
-
-***BCond***     = B coeff of conductivity (W/m-K^2)
-
-***CCond***     = C coeff of conductivity (W/m-K^3)
-
-***AVisc***     = A coeff of viscosity (g/m-s)
-
-***BVisc***     = B coeff of viscosity (g/m-s-K)
-
-***CVisc***     = C coeff of viscosity (g/m-s-K^2)
-
-***ASpHeat***   = A coeff of specific heat (J/kg-K)
-
-***BSpHeat***   = B coeff of specific heat (J/kg-K^2)
-
-***CSpHeat***   = C coeff of specific heat (J/kg-K^3)
-
-
-
-GLAZING SYSTEM OPTICAL DATA
-
-System1, System2: separate characteristics are given if the window has a mullion.
-
-***Hemisph***   = hemispherical (i.e., diffuse)
-
-***Tsol***      = solar transmittance vs. angle of incidence
-
-***AbsN***      = solar absorptance of Nth layer vs. angle of incidence
-
-***Rfsol***     = front solar reflectance vs. angle of incidence
-
-***Rbsol***     = back solar reflectance vs. angle of incidence
-
-***Tvis***      = visible transmittance vs. angle of incidence
-
-***Rfvis***     = front visible reflectance vs. angle of incidence
-
-***Rbvis***     = back visible reflectance vs. angle of incidence
-
----------------------------------------------------------
-
-\*Standard conditions are
-
-  Winter:
-
-  Indoor air temperature = 21.1C (70F)
-
-  Outdoor air temperature = -17.8C (0F)
-
-  Wind speed = 6.71 m/s (15 mph)
-
-  No solar radiation
-
-
-
-  Summer:
-
-  Indoor air temperature = 23.9C (75F)
-
-  Outdoor air temperature = 31.7C (89F)
-
-  Wind speed = 3.35 m/s (7.5 mph)
-
-  783 W/m2 (248 Btu/h-ft2) incident beam solar radiation normal to glazing
-
-
-
-Building Geometry, Shading & Zone Model
-=======================================
-
-Building Surface Dimensions – Inside, Outside or Centerline
--------------------------------------------------------------------------------------------
-
-When describing the geometry of building surfaces in EnergyPlus, all surfaces are a thin plane without any thickness. The thickness property of the materials which are assigned to the building surface are only used for heat conduction and thermal mass calculations. Because EnegyPlus geometry is represented with a thin plane, which actual dimension is the proper one to use: inside, outside, or centerline dimensions. For most buildings, the difference is small, and the user may use whatever dimensions are most convenient. A suggested approach is to use outside dimensions for exterior surfaces, and centerline dimensions for interior surfaces. This produces fully connected geometry with an appropriate amount of floor area, zone volume, and thermal mass. If desired, zone volume and floor area may be overridden by entering values in the Zone object. For buildings with very thick walls, such as centuries-old masonry buildings, it is recommended that centerline dimensions be used for all surfaces (exterior and interior) so that the model will have the correct amount of thermal mass.
-
-Describing Roof Overhangs
-----------------------------------------------------------------------------------------
-
-Building heat transfer surfaces, such as roofs and walls, only cast shadows in a hemisphere in the direction of the outward facing normal (see Figure 3). Because roof surfaces generally face upward, a roof surface which extends beyond the walls of the building will not cast shadows on the walls below it (see Figure 4).
-
-
-
-![](media/image003.png)
-
-Figure 3. Building heat transfer surfaces cast shadows in the direction of outward facing normal.
-
-
-
-![](media/image004.png)
-
-Figure 4. Extended roof surface will not shade the walls below.
-
-Figure 5 shows the proper surface configurations for two types of attic construction. In all cases, the roof surface should only include the area of the roof which contacts the zone below it. In these drawings, this is an unconditioned attic space, but it could also be a conditioned zone. Any extensions of the roof which are exposed to the outdoors on both sides should be described as a shading surface.
-
-For the configuration on the left, the overhang should be a shading surface which will cast shadows in both directions (if the default mirroring is disabled the shading surface must face downward). This ensures that the correct shading will be modeled, and it also avoids overstating the heat transfer through the roof into the attic.
-
-For the configuration on the right, the attic is fully enclosed with building heat transfer surfaces for the roof and soffits. The soffits would be described as floor surfaces in the attic and would face downward. The central portion of the attic floor would be described as an interzone floor surface where the outside boundary condition is the ceiling surface in the zone below.
-
-![](media/image005.png)
-
-Figure 5. Proper surface configurations for roof overhangs for two types of attic construction.
-
-Solar Reflection from Shading Surfaces
---------------------------------------
-
-Exterior shading surfaces modeled using "FullInteriorAndExteriorWithReflections" can show some sky diffuse solar getting through the shades. When "\*WithReflections" is active a partially sunlit shading surface reflects uniformly from the entire surface.
- If using WithReflections, shading surfaces should be broken into multiple surfaces at lines of intersection with other shading surfaces. This also includes places where another surface may tee into a shading surface.
-
-For example, a building is shaded by surfaces A, B, and C. Shading Surface A intercepts with Shading Surfaces B and C, and are broken into three areas A1, A2, and A3. Surface A should be entered as the shown three shading areas in order to correctly model sky diffuse solar reflection from Shading Surface A.
-
-![Reflections](media/image006.jpg)
-
-Figure 6. Limitations in modeling reflections from surfaces
-
-Air wall, Open air connection between zones
--------------------------------------------
-
-It is extremely difficult to model the interactions between thermal zones which are connected by a large opening. If the zones are controlled to the same conditions, then there is little to be gained by making them interact, so you could neglect any connections between the zones. In fact, if this is the case, you might consider combining the spaces into a single thermal zone. If you expect the zones to have significantly different temperatures and/or humidities, then use one of the following options. If they are modeled as separate zones, EnergyPlus models only what is explicitly described in the input file, so simply leaving a void (no surfaces) between two zones will accomplish nothing - the two zones will not be connected. The main interactions which occur across the dividing line between two zones which are fully open to each other are:
-
-1)   Convection or airflow, which will transfer both sensible heat and moisture. Some modelers use MIXING (one-way flow) or CROSS MIXING (two-way flow) to move air between the zones, but the user must specify airflow rates and schedules for this flow, and it cannot be automatically linked to HVAC system operation. Other modelers use AirFlowNetwork with large vertical openings between the zones as well as other openings and cracks in the exterior envelope to provide the driving forces. It can also be connected with the HVAC system (for limited system types). This requires a much higher level of detailed input and should be used only if the detailed specification data is available. If the two zones are controlled to similar conditions, this effect could be safely neglected.
-
-2)   Solar gains and daylighting. The only way to pass solar and daylight from one zone to the next is through a window or glass door described as a subsurface on an interzone wall surface. Note that all solar is diffuse after passing through an interior window.
-
-3)   Radiant (long-wave thermal) transfer. There is currently no direct radiant exchange between surfaces in different thermal zones. Windows in EnergyPlus are opaque to direct radiant exchange, so an interzone window will not behave any differently than an opaque interzone surface for this aspect. However, a large interzone surface (opaque or window) would result in some indirect radiant exchange since the interzone surface will exchange directly with surfaces in zone A and in zone B. The surface thermal resistance should be low in order to most closely approximate this effect.
-
-4)   Conduction. If an interzone surface is placed between the two zones, it will conduct sensible heat between the two zones. Using a low thermal resistance helps to move radiant exchange between the zones.
-
-5)    Visible and thermal radiant output from internal gains. These gains will not cross zone boundaries. But again, they will impact any interzone surfaces, so some of the energy may move across to the next zone."
-
-Daylight Modeling
------------------
-
-*Why isn’t my lighting energy being reduced with a daylighting system?*
-
-In order to see changes in the lighting electric power consumption due to daylighting, the Fraction Replaceable in the **Lights** input object must be set to 1.0. This is documented in the I/O reference, and also a warning is generated in the ERR file.
-
-Rain Flag
----------
-
-*Why is my exterior convection coefficient value 1000?*
-
-When the outside environment indicates that it is raining, the exterior surfaces (exposed to wind) are assumed to be wet. The convection coefficient is set to a very high number (1000) and the outside temperature used for the surface will be the wet-bulb temperature. (If you choose to report this variable, you will see 1000 as its value.)
-
-Interzone Exterior Convection
------------------------------
-
-*Why is my exterior convection coefficient value 0?*
-
-When two surfaces are linked as interzone surfaces, the "exterior" side of these surfaces does not really exist. EnergyPlus links the two surfaces by using the inside temperature of surface A as the outside temperature of surface B, and the reverse. For example:
-
-Zone1WestWall has an outside boundary of Surface = Zone2EastWall
-
-Zone2EastWall has an outside boundary of Surface = Zone1WestWall
-
-Let's say that at hour 2, the inside surface temperature of Zone1WestWall is 19C, and the inside temperature of Zone2EastWall is 22C. When the heat balance is calculated for Zone1WestWall, its outside surface temperature will be set to 22C. Likewise, when the heat balance is calculated for Zone2EastWall, its outside surface temperature will be set to 19C. So, for interzone surfaces, h ext does not apply. That is why it is reported as zero.
-
-Modeling Reflective Radiant Barriers
-------------------------------------
-
-*Can EnergyPlus model reflective radiant barriers?*
-
-1. For radiant barriers which are exposed to a thermal zone, such as an attic space, specify a reduced thermal absorptance for the innermost material layer.
-
-For example, an attic roof construction might be (outer to inner)
-
-```idf
-Asphalt shingles,
-R-30 insulation,
-Radiant barrier;
-```
-
-
-The radiant barrier material would be a thin layer with some small resistance with a low thermal absorptance value. This will reduce the radiant heat transfer from the roof surface to other surfaces in the attic zone.
-
-2. If the radiant barrier is within a cavity which is not modeled as a separate thermal zone, then there is not an easy way to model its impact. For example, a wall construction:
-
-```idf
-Brick,
-R-12 insulation,
-Radiant barrier,
-Air gap,
-Gypsum board;
-```
-
-
-Here, the radiant barrier would reduce the radiant transfer across the air gap. But EnergyPlus air gaps are a fixed thermal resistance, specified in the Material:Airgap object. The user would need to compute an average effective resistance which represents the reduced radiant heat transfer across the air gap due to the radiant barrier. This resistance could then be assigned to the radiant barrier material layer.
-
-Cavity Algorithm Model
-----------------------
-
-*Reading the documentation, I'm wondering if the Cavity algorithm is usable for other double facade types or only Trombe wall?  In other words, does Cavity implicitly presume that the inner wall is highly solar absorbent and so generate specific convection?*
-
-The Trombe wall convection algorithm is applicable to just about any vertical cavity with a high aspect ratio and relatively narrow width. I'm not sure if a double facade cavity would meet the aspect ratio requirement. But I do know the Trombe wall algorithm is not picky about whether the inner wall is highly absorbant, or about any particular properties of the walls. Actually the same basic algorithm is used by the window model to calculate the convection between the two panes of a window. The full reference is ISO 15099.
-
-Using Multipliers (Zone and/or Window)
---------------------------------------
-
-### Background and Study using Multipliers
-
-Multipliers are used in EnergyPlus for convenience in modeling. Though window multipliers are useful for any size building when you have multiple windows on a façade, zone multipliers are more useful in large buildings with several to many stories.
-
-Zone multipliers are designed as a “multiplier� for floor area, zone loads, and energy consumed by internal gains. It takes the calculated load for the zone and multiplies it, sending the multiplied load to the attached HVAC system. The HVAC system size is specified to meet the entire multiplied zone load and will report the amount of the load met in the Zone/Sys Sensible Heating or Cooling Energy/Rate report variable. Autosizing automatically accounts for multipliers. Metered energy consumption by internal gains objects such as Lights or Electric Equipment will be multiplied.
-
-To illustrate the benefits (and comparison of results), the MultiStory.idf example file was used. The MultiStory file is a 9 zone, 10 story/floored building with heating (ZoneHVAC:Baseboard:Convective:Electric object) and cooling (ZoneHVAC:WindowAirConditioner object). The middle zone of each floor in the original represents 4 zones (multiplier=4) and the middle floor (ZoneGroup) represents 8 floors (ZoneGroup multiplier=8). Clone representations were made for comparisons:
-
-![Multistory](media/image007.png)
-
-Figure 7. Original Multistory IDF
-
-In the figure above, each “middle� zone represents 4 zones.  The middle “floor� represents 8 floors. Additionally, each of the windows has a multiplier of 4 – so each window represents 4 windows of the same size. For the Multistory file, the Zone object for the center zones has the multiplier of 4. And for the center floors, the ZoneList and ZoneGroup objects to collect the zones and apply multipliers. The top floor then uses the Zone object multiplier for the center zones. Specifically:
-
-
-```idf
-<snip>
-  Zone,
-    Gnd Center Zone,         !- Name
-    0.0,                     !- Direction of Relative North {deg}
-    8.0, 0.0, 0.0,           !- Origin [X,Y,Z] {m}
-    1,                       !- Type
-    4,                       !- Multiplier
-    autocalculate,           !- Ceiling Height {m}
-    autocalculate;           !- Volume {m3}
-
-<snip>
-
-  ZoneGroup,
-    Mid Floor,               !- Zone Group Name
-    Mid Floor List,          !- Zone List Name
-    8;                       !- Zone List Multiplier
-
-
-  ZoneList,
-    Mid Floor List,          !- Zone List Name
-    Mid West Zone,           !- Zone 1 Name
-    Mid Center Zone,         !- Zone 2 Name
-    Mid East Zone;           !- Zone 3 Name
-
-<snip>
-
-  Zone,
-    Top Center Zone,         !- Name
-    0.0,                     !- Direction of Relative North {deg}
-    8.0,                     !- X Origin {m}
-    0.0,                     !- Y Origin {m}
-    22.5,                    !- Z Origin {m}
-    1,                       !- Type
-    4,                       !- Multiplier
-    autocalculate,           !- Ceiling Height {m}
-    autocalculate;           !- Volume {m3}
-```
-
-
-For comparison purposes, clones of the middle zones were done.
-
-![Multistory-clones1](media/image008.png)
-
-Figure 8. Multistory with cloned middle zones.
-
-And, finally, the entire building was created:
-
-![Multistory-clones2](media/image009.png)
-
-Figure 9. Multistory building -- fully cloned.
-
-The building is autosized. For convenience in comparison, the extreme summer and winter days were used for autosizing and the simulation was run for the 5 United States weather files that are included in the EnergyPlus release: Chicago IL; San Francisco CA; Golden CO; Tampa FL; and Washington DC.
-
-Comparisons were done with the Zone Group Loads values (Zone Group Sensible Heating Energy and Zone Group Sensible Cooling Energy) as well as meter values for Electricity. Using the regression testing limits that are used during EnergyPlus development testing (i.e. small differences are within .001 or .5%; big differences are greater than those limits).
-
-For the purposes of dicussion, the buildings will be called: Multistory 1 – the original 9 zone building (with multipliers and groups) ref: Figure 7; Multistory 2 – the building shown in Figure 8. Multistory with cloned middle zones.; Multistory 3 – the fully configured building – ref Figure 9.
-
-The following table illustrates the regression testing for Multistory 2 and Multistory 3, group loads and meters versus Multistory 1 results.
-
-Table 1. Multistory vs Multistory 2 and Multistory 3
-
-<table class="table table-striped">
-  <tr>
-    <th>LOCATION</th>
-    <th>MULTI-STORY 2 LOADS</th>
-    <th>MULTI-STORY 2 METER</th>
-    <th>MULTI-STORY 3 LOADS</th>
-    <th>MULTI-STORY 3 METER</th>
-  </tr>
-  <tr>
-    <td>USA_IL_Chicago-OHare.Intl.AP.725300_TMY3</td>
-    <td>Small Diffs</td>
-    <td>Equal</td>
-    <td>Big Diffs* (76%)</td>
-    <td>Big Diffs* (62%)</td>
-  </tr>
-  <tr>
-    <td>USA_CA_San.Francisco.Intl.AP.724940_TMY3</td>
-    <td>Big Diffs* (2.43%)</td>
-    <td>Big Diffs* (0.6%)</td>
-    <td>Big Diffs* (49%)</td>
-    <td>Big Diffs* (41%)</td>
-  </tr>
-  <tr>
-    <td>USA_CO_GOLDEN-NREL.724666_TMY3</td>
-    <td>Small Diffs</td>
-    <td>Small Diffs</td>
-    <td>Big Diffs* (26%)</td>
-    <td>Big Diffs* (24%)</td>
-  </tr>
-  <tr>
-    <td>USA_FL_Tampa.Intl.AP.722110_TMY3</td>
-    <td>Small Diffs</td>
-    <td>Small Diffs</td>
-    <td>Big Diffs* (6%)</td>
-    <td>Big Diffs* (2%)</td>
-  </tr>
-  <tr>
-    <td>USA_VA_Sterling-Washington.Dulles.Intl.AP.724030_TMY3</td>
-    <td>Equal</td>
-    <td>Equal</td>
-    <td>Big Diffs* (91%)</td>
-    <td>Big Diffs* (72%)</td>
-  </tr>
-</table>
-
-\* Big Diffs maximum occur in monthly values whereas the runperiod values are much smaller.
-
-To try to pare down the discrepancies shown here, the effects of height that are used in the calculations were removed (i.e., the Site:WeatherStation and Site:HeightVariation objects were entered as below to negate the effects of height on the environmental variables such as wind and temperature).  In addition the height effect was removed from the OutdoorAir:Node object.
-
-```idf
-  Site:WeatherStation,
-    ,          !- Wind Sensor Height Above Ground {m}
-    ,          !- Wind Speed Profile Exponent
-    ,          !- Wind Speed Profile Boundary Layer Thickness {m}
-    0;         !- Air Temperature Sensor Height Above Ground {m}
-
-
-  Site:HeightVariation,
-    0,         !- Wind Speed Profile Exponent
-    ,          !- Wind Speed Profile Boundary Layer Thickness {m}
-    0;         !- Air Temperature Gradient Coefficient {K/m}
-```
-
-
-Figure 10. Objects removing height from building impacts.
-
-With these included, the files were rerun with the following results:
-
-Table 2. Multiplier Results with negated height variation.
-
-<table class="table table-striped">
-<tr>
-<th>Location</th>
-<th>Multi-story 2 Loahs</th>
-<th>Multi-story 2 Meter</th>
-<th>Multi-story 3 Loahs</th>
-<th>Multi-story 3 Meter</th>
-</tr>
-<tr>
-<td>USA_IL_Chicago-OHare.Intl.AP.725300_TMY3</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-</tr>
-<tr>
-<td>USA_CA_San.Francisco.Intl.AP.724940_TMY3</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-</tr>
-<tr>
-<td>USA_CO_GOLDEN-NREL.724666_TMY3</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-</tr>
-<tr>
-<td>USA_FL_Tampa.Intl.AP.722110_TMY3</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-</tr>
-<tr>
-<td>USA_VA_Sterling-Washington.Dulles.Intl.AP.724030_TMY3</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-<td>Small diffs</td>
-</tr>
-</table>
-
-To investigate if other systems might have different results, the Ideal Loads System was used as the system.  Similar results were found for the multipliers vs cloned results. However, it may also be noted that the results between the original systems (baseboard and window ac) vs the ideal loads were very similar.
-
-The biggest difference really comes in calculation time. As shown in the following table,
-
-Table 3. Runtimes for Multistory files (baseboard/window ac)
-
-<table class="table table-striped">
-<tr>
-<th>Location</th>
-<th>Multi-story 1 (9 zones) (mm:ss)</th>
-<th>Multi-story 2  (18 zones) (MM:SS)</th>
-<th>Multi-story 3 (60 zones) (MM:SS)</th>
-</tr>
-<tr>
-<td>USA_IL_Chicago-OHare.Intl.AP.725300_TMY3</td>
-<td>1:05</td>
-<td>2:14</td>
-<td>13:15</td>
-</tr>
-<tr>
-<td>USA_CA_San.Francisco.Intl.AP.724940_TMY3</td>
-<td>1:04</td>
-<td>2:05</td>
-<td>13:20</td>
-</tr>
-<tr>
-<td>USA_CO_GOLDEN-NREL.724666_TMY3</td>
-<td>1:17</td>
-<td>2:28</td>
-<td>14:43</td>
-</tr>
-<tr>
-<td>USA_FL_Tampa.Intl.AP.722110_TMY3</td>
-<td>1:11</td>
-<td>2:21</td>
-<td>13:43</td>
-</tr>
-<tr>
-<td>USA_VA_Sterling-Washington.Dulles.Intl.AP.724030_TMY3</td>
-<td>1:05</td>
-<td>2:15</td>
-<td>13:18</td>
-</tr>
-</table>
-
-Because the overall results were so similar, the run times for the Ideal Loads runs are included:
-
-Table 4. Runtime for Multistory files (ideal loads)
-
-<table class="table table-striped">
-<tr>
-<td>Location</td>
-<th>Multi-story 1 (9 zones) (mm:ss)</th>
-<th>Multi-story 2 (18 zones) (MM:SS)</th>
-<th>Multi-story 3 (60 zones) (MM:SS)</th>
-</tr>
-<tr>
-<td>USA_IL_Chicago-OHare.Intl.AP.725300_TMY3</td>
-<td>0:51</td>
-<td>1:34</td>
-<td>9:37</td>
-</tr>
-<tr>
-<td>USA_CA_San.Francisco.Intl.AP.724940_TMY3</td>
-<td>0:50</td>
-<td>1:34</td>
-<td>9:59</td>
-</tr>
-<tr>
-<td>USA_CO_GOLDEN-NREL.724666_TMY3</td>
-<td>0:51</td>
-<td>1:40</td>
-<td>10:31</td>
-</tr>
-<tr>
-<td>USA_FL_Tampa.Intl.AP.722110_TMY3</td>
-<td>0:51</td>
-<td>1:36</td>
-<td>10:05</td>
-</tr>
-<tr>
-<td>USA_VA_Sterling-Washington.Dulles.Intl.AP.724030_TMY3</td>
-<td>0:51</td>
-<td>1:36</td>
-<td>9:48</td>
-</tr>
-</table>
-
-More zones (and, particularly more surfaces) make for longer run times.
-
-### Guidelines for Using Multipliers and Groups
-
-- If the basic zone geometry is identical, make one zone, copy & paste it as necessary, then change the Zone Origin field to locate each zone correctly.
-
-- Do not use interzone surfaces between zones that are multiplied. Set the adjoining surfaces to be adiabatic, i.e. use the OtherZoneSurface exterior boundary condition with the other surface pointing back to itself.
-
-- Locate the middle floor zones roughly halfway between top and ground because exterior convection coefficients change with height. Halfway should cause the differences to average out. If you have many stories (the example only has 10 stories), consider using more middle floor zones.
-
-- Consider removing the effects of height variation for the simulation.
-
-- Follow guidelines in HVACTemplate and other objects about sizing if you are mixing autosize fields with hard sized fields (recommended to “autosize� all fields rather than mix).
-
-- All HVAC system sizes must be specified to meet the entire multiplied zone load.
-
-- Autosizing automatically accounts for multipliers.
-
-Using OSC (Other Side Coefficients) to create controlled panels
----------------------------------------------------------------
-
-The Other Side Coefficient (OSC) equation permits setting either the outside surface temperature or the outside air temperature to a constant value or a scheduled value based on the size of the first input parameter, N1. The original temperature equation was:
-
-<div>\[ T = N_2 T_{zone} + N_3 T_{oadb} + N_4 N_5 + N_6 T_{grnd} + N_7 W_{spd} T_{oadb} \]</div>
-
-where: 
-
-* <span>\(T\)</span> = Outside Air Temperature when N1 (Combined convective/radiative film Coeff) &gt; 0
-
-* <span>\(T\)</span> = Exterior Surface Temperature when N1 (Combined convective/radiative film Coeff) &lt;= 0
-
-* <span>\(T_{zone}\)</span> =MAT =Temperature of the zone being simulated (°C)
-
-* <span>\(T_{oadb}\)</span> = Dry-bulb temperature of the outdoor air (°C)
-
-* <span>\(T_{grnd}\)</span> = Temperature of the ground (°C) Wspd = Outdoor wind speed (m/sec)
-
-The coefficients N<sub>2</sub>, N<sub>3</sub>, N<sub>4</sub>, N<sub>6</sub>, and N<sub>7</sub> scale the contribution of the various terms that follow them.  In the case of N<sub>4</sub>, it is followed by another term N<sub>5</sub>.  This is a constant temperature that can also be overridden by a scheduled value. Note that in some EnergyPlus documentation, the N’s are given as C’s.
-
-This object has been changed to permit the outside temperature, T, to be controlled to a set point temperature that is specified as N<sub>5</sub> or comes from the schedule A2.
-
-Note that since the surface that contains the panel subsurfaces (that must be called doors in EnergyPlus) receives that same outside temperature as the panels, it should have a construction with a very high thermal resistance to essentially take it out of the room heat balance calculation.
-
-An Example input file object is shown below.
-
-```idf
-SurfaceProperty:OtherSideCoefficients,
-   Zn001:Roof001:OSC, !- Name
-   0,   ! (N1) Combined Convective/Radiative Film Coefficient {W/m2-K}
-   0,   ! (N5) Constant Temperature {C}
-   0.95,!(N4) Constant Temperature Coefficient
-   ,    ! (N3)External Dry-Bulb Temperature Coefficient
-   ,    ! (N6)Ground Temperature Coefficient
-   ,    ! (N7)Wind Speed Coefficient
-   -.95,! (N2) Zone Air Temperature Coefficient
-   ConstantCooling,     ! (A2) Constant Temperature Schedule Name
-   No,  ! (A3)Sinusoidal Variation of Constant Temperature Coefficient
-   24,  ! (N8)Period of Sinusoidal Variation {hr}
-   1.,  ! (N9)Previous Other Side Temperature Coefficient
-   5.,  !(N10) Minimum Other Side Temperature Limit
-   25.; ! (N11) Maximum Other Side Temperature Limit
-```
-
-
-This object results in the following equation for T:
-
-T = 1.0\*Tlast +0.95\*(Tsetpoint – TzoneAir)   (with limits)
-
-The result of this is that the surface temperature, T, will be changed to the temperature that will force the zone air temperature to the setpoint providing the temperature limits are not reached. When the zone air temperature is at the setpoint, T remains at the value it had in the prior time step.
-
-A complete example with all pertinent objects:
-
-```idf
-  Construction,
-    PanelConst,              !- Name
-    Std Steel_Brown_Regular; !- Outside Layer
-
-
-  Material,
-    Std Steel_Brown_Regular, !- Name
-    Smooth,                  !- Roughness
-    1.5000000E-03,           !- Thickness {m}
-    44.96960,                !- Conductivity {W/m-K}
-    7689.000,                !- Density {kg/m3}
-    418.0000,                !- Specific Heat {J/kg-K}
-    0.9000000,               !- Thermal Absorptance
-    0.9200000,               !- Solar Absorptance
-    0.92000000;              !- Visible Absorptance
-
-
-  BuildingSurface:Detailed,
-    Zn001:Roof001,           !- Name
-    Roof,                    !- Surface Type
-    ROOF31,                  !- Construction Name
-    ZONE ONE,                !- Zone Name
-    OtherSideCoefficients,   !- Outside Boundary Condition
-    Zn001:Roof001:OSC,       !- Outside Boundary Condition Object
-    NoSun,                   !- Sun Exposure
-    NoWind,                  !- Wind Exposure
-    0,                       !- View Factor to Ground
-    4,                       !- Number of Vertices
-    0.000000,15.24000,4.572,  !- X,Y,Z ==&gt; Vertex 1 {m}
-    0.000000,0.000000,4.572,  !- X,Y,Z ==&gt; Vertex 2 {m}
-    15.24000,0.000000,4.572,  !- X,Y,Z ==&gt; Vertex 3 {m}
-    15.24000,15.24000,4.572;  !- X,Y,Z ==&gt; Vertex 4 {m}
-
-
-  FenestrationSurface:Detailed,
-    panel002,                !- Name
-    Door,                    !- Surface Type
-    PanelConst,              !- Construction Name
-    Zn001:Roof001,           !- Building Surface Name
-    ,                        !- Outside Boundary Condition Object
-    autocalculate,           !- View Factor to Ground
-    ,                        !- Shading Control Name
-    ,                        !- Frame and Divider Name
-    1,                       !- Multiplier
-    4,                       !- Number of Vertices
-    3,2,4.572,  !- X,Y,Z ==&gt; Vertex 1 {m}
-    3,3,4.572,  !- X,Y,Z ==&gt; Vertex 2 {m}
-    4,3,4.572,  !- X,Y,Z ==&gt; Vertex 3 {m}
-    4,2,4.572;  !- X,Y,Z ==&gt; Vertex 4 {m}
-
-
-  SurfaceProperty:OtherSideCoefficients,
-    Zn001:Roof001:OSC,       !- Name
-    0,            !- Combined Convective/Radiative Film Coefficient {W/m2-K}
-    0,                       !- Constant Temperature {C}
-    0.95,                    !- Constant Temperature Coefficient
-    ,                        !- External Dry-Bulb Temperature Coefficient
-    ,                        !- Ground Temperature Coefficient
-    ,                        !- Wind Speed Coefficient
-    -.95,                    !- Zone Air Temperature Coefficient
-    ConstantTwentyTwo,       !- Constant Temperature Schedule Name
-    No,           !- Sinusoidal Variation of Constant Temperature Coefficient
-    24,                      !- Period of Sinusoidal Variation {hr}
-    1.,                      !- Previous Other Side Temperature Coefficient
-    5.,                      !- Minimum Other Side Temperature Limit {C}
-    25.;                     !- Maximum Other Side Temperature Limit {C}
-
-
-Schedule:Constant,ConstantTwentyTwo,PanelControl,22;
-```
-
-
-Natural and Mechanical Ventilation
-==================================
-
-AirflowNetwork and EarthTube
-----------------------------
-
-*When I use an Earthtube with an AirFlowNetwork, I get a "Orphan Object" warning.*
-
-Currently, Earthtube and AirFlowNetworks do not work together.  If both objects co-exist, the AirflowNetwork mode supersedes the Earthtube mode at two control choices. Since this causes the Earthtube objects to not be used, the "orphan" warning appears.
-
-There are four control choices in the second field of the AirflowNetwork Simulation object (spaces included for readability)
-
-- MULTIZONE WITH DISTRIBUTION
-
-- MULTIZONE WITHOUT DISTRIBUTION
-
-- MULTIZONE WITH DISTRIBUTION ONLY DURING FAN OPERATION
-
-- NO MULTIZONE OR DISTRIBUTION
-
-When the first two choices are selected, the AirflowNetwork model takes over airflow calculation. The earthtube objects are not used in the airflow calculation, causing the "orphan" warning. The example file, AirflowNetwork\_Multizone\_SmallOffice.idf, uses the first choice.  When the second choice is used, the AirflowNetwork model is only used during HVAC operation time. During system off time, the earthtube model is used to calculate airflows.  Thus, no "orphan" warning will be given, but the earthtube may be being used less than expected.  The example file, AirflowNetwork\_Simple\_House.idf, uses the third choice.
-
-HVAC, Sizing, Equipment Simulation and Controls
-===============================================
-
-HVAC Sizing Tips
-----------------
-
-To help achieve successful autosizing of HVAC equipment, note the following general guidelines.
-
-- Begin with everything fully autosized (no user-specified values) and get a working system before trying to control any specific sized.
-
-- The user must coordinate system controls with sizing inputs. For example, if the Sizing:System “Central Cooling Design Supply Air Temperature� is set to 13C, the user must make sure that the setpoint manager for the central cooling coil controls to 13C as design conditions. EnergyPlus does not cross-check these inputs. The sizing calculations use the information in the Sizing:\* objects. The simulation uses the information in controllers and setpoint managers.
-
-- User-specified flow rates will only impact the sizing calculations if entered in the Sizing:Zone or Sizing:System objects. Sizing information flows only from the sizing objects to the components. The sizing calculations have no knowledge of user-specified values in a component. The only exception to this rule is that plant loop sizing will collect all component design water flow rates whether autosized or user-specified.
-
-- The zone thermostat schedules determine the times at which design loads will be calculated. All zone-level schedules (such as lights, electric equipment, infiltration) are active during the sizing calculations (using the day type specified for the sizing period). System and plant schedules (such as availability managers and component schedules) are unknown to the sizing calculations. To exclude certain times of day from the sizing load calculations, use the thermostat setpoint schedules for SummerDesignDay and/or WinterDesignDay. For example, setting the cooling setpoint schedule to 99C during nighttime hours for the SummerDesignDay day type will turn off cooling during those hours.
-
-For more information, read the Input Output Reference section on “Input for Design Calculations and Component Autosizing.�
-
-Variable Refrigerant Flow Air Conditioner
------------------------------------------
-
-***The EnergyPlus v7.0 release (October 2011) includes an initial model for VRF systems.  See AirConditioner:VariableRefrigerantFlow and related objects.***
-
-*Can I model a VRV or VRF system in EnergyPlus?*
-
-Variable Refrigerant Flow (VRF, or Variable Refrigerant Volume - VRV) air conditioners are available in EnergyPlus V7 and later.
-
-Otherwise, the closest model available would be the multi-speed cooling and heating AC (AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed used with Coil:Cooling:DX:Multispeed and Coil:Heating:DX:Multispeed coils). This model will provide information for cooling-only or heating-only operation (VRF heat pump mode).
-
-Others have attempted to simulate a VRF system with the existing VAV model. This model will only provide valid information when cooling is required. The results will only be as good as the DX cooling coil performance curves allow. The heating side of a VAV system does not use a DX compression system (i.e., uses gas or electric heat) so this part of the VRV system cannot be modeled with a VAV system.
-
-Note that using either of these models will not provide accurate results since each of these system types provides conditioned air to all zones served by the HVAC system. The VAV system terminal unit may be set to use a minimum flow of 0 where the resulting air flow to that zone is 0 when cooling is not required. Energy use in this case may be slightly more accurate.
-
-Modeling Desiccant DeHumidifiers
---------------------------------
-
-*How do I enter performance data for a desiccant dehumidifier?*
-
-It depends on which specific EnergyPlus object you are trying to use.
-
-The Dehumidifier:Desiccant:NoFans object has default performance curves within the model itself that you can use.  Set field A12, "Performance Model," to DEFAULT.  Alternatively, you could also obtain manufacturer's data and develop your own curve fits, then set "Performance Model" to User Curves.   See the Input Output Reference for more details.
-
-If you want to use the Dehumidifier:Desiccant:System object, then some data set inputs for the required HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 object are contained in the file "PerfCurves.idf" in the DataSets folder.  You could also obtain manufacturer's data and develop your own inputs for the HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 object.
-
-Boiler Control Schedule
------------------------
-
-*How can I get my boiler to only work when the outdoor temperature is less than 5°C?*
-
-To schedule the boiler to work only when the outdoor dry bulb temperature is below 5°C, create two schedules based on the temperatures in the weather file. You can do this by reporting Outdoor Dry Bulb hourly, then make a spreadsheet with two columns, one which =1 whenever ODB≥5, and the other which =1 whenever ODB &lt; 5. Save this spreadsheet as a csv format file, and then you can use Schedule:File to read these as EnergyPlus schedules. Use these schedules in the PlantEquipmentOperationSchemes object to make "boiler heating" active in cold weather and "heatpump Heating" active in warmer weather.
-
-Note that you will need to have two PlantEquipmentList objects, one which lists only the boiler, and the other which lists only the heat pump. And the two different PlantEquipmentOperation:HeatingLoad objects should reference different PlantEquipmentList objects.
-
-Report temperatures and flow rates at selected points on the hot water loop to see if things are working properly.
-
-Difference between EIR and Reformulated EIR Chillers
-----------------------------------------------------
-
-*What is the difference between the EIR and ReformulatedEIR models of Electric Chillers?  I am getting strange results.*
-
-The COP of a chiller is a function of part load ratio. It is mainly determined by the Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve.  When the EIR model is used for an electric chiller, the curve has an independent variable: part load ratio.  For the ReformulatedEIR model, the curve requires two independent variables: leaving condenser water temperature and part load ratio.  Each independent variable has its min and max values. If a variable is outside the allowed range, the nearest allowed value is used, possibly resulting in an unexpected result.
-
-If you would like to compare COP values for two types of chillers, you may need to ensure that the same conditions are applied. For simplicity, you may want to use a spreadsheet to calculate the curve values.
-
-Using Well Water
-----------------
-
-The water-to-water heat pumps have not been programmed to allow well water. However, cooling towers have (see 5ZoneWaterSystems.idf) and you should be able to connect the WSHP to a condenser loop with a cooling tower.
-
-Currently, there is no method to directly simulate well water as the condensing fluid for water source heat pumps. So to get as close as possible, program the cooling towers to allow well water via the water use object. If the cooling tower inlet node water temperature represents the well water temperature, and if you can set up the cooling tower to provide an outlet water temperature very close to the inlet water temperature, then this would be the same as connecting the well water directly to the WSHP. Minimize the cooling tower fan energy or disregard it completely when performing your simulation. Use report variables at the inlet/outlet node of the cooling tower to investigate how close you can get to your equipment configuration.
-
-Plant Load Profile
-------------------
-
-The Plant Load Profile object is used to "pass" a load to the plant where the plant meets this load. The load profile places an inlet and outlet water temperature and a mass flow rate at the inlet to the plant loop. This is where you will need to focus when you try to alter the boiler performance.
-
-HVAC System Turn Off
---------------------
-
-*My HVAC system won’t turn off even when my availability schedule is 0 (off).*
-
-The night cycle option is set to Cycle On Any in the HVACTemplate:System:Unitary object. This will turn on the AC system. Change the night cycle option to Stay Off and the system shuts down correctly. For future reference, an indicator of night cycle operation is the on one time step, off the next type of operation.
-
-Fan Types
----------
-
-*I am confused about the differences between the different fan types.  Can you explain?*
-
-In short:
-
-Fan:ConstantVolume is a constant volume, continuous operation fan which can be turned on and off via a schedule.
-
-Fan:OnOff is similar to the one above, but it cycles itself on and off as required by its thermostat ... all during the scheduled operation period. This is a typical mode of operation for a home furnace.
-
-Fan:VariableVolume runs continuously during the Schedule period, but varies its volume to meet the heating or cooling demand.
-
-Consult the [Input Output Reference document](file:///E:\Docs4PDFs\InputOutputReference.pdf) (group Fans) for additional information.
-
-Use of Set Point Managers
--------------------------
-
-A coil will check its inlet air temperature compared to the set point temperature. For cooling, if the inlet air temperature is above the set point temp, the coil turns on. It's opposite that for heating. In the 5ZoneAutoDXVAV example file, a schedule temperature set point is placed at the system outlet node. This is the temperture the designer wants at the outlet. The mixed air SP manager is used to account for fan heat and places the required SP at the outlet of the cooling coil so the coil slightly overcools the air to overcome fan heat and meet the system outlet node set point.
-
-You don't blindly place the SP's at the coil outlet node, but this is a likely starting point in most cases. If there is a fan after the coil's, the "actual" SP will need to be placed on a different node (other than the coils). Then a mixed air manager will be used to reference that SP and the fan's inlet/outlet node to calculate the correct SP to place wherever you want (at the coil outlet, the mixed air node, etc.). Place it at the mixed air node if you want the outside air system to try and meet that setpoint through mixing. Place it at the cooling coil outlet if you want the coil control to account for fan heat. Place it at both locations if you want the outside air system to try and meet the load with the coil picking up the remainder of the load.
-
-See if the coils are fully on when the SP is not met. If they are the coils are too small. If they are at part-load, the control SP is calculated incorrectly.
-
-### Relationship of Set Point Managers and Controllers
-
-*Could you elaborate further on the relation between SetPoint managers and Controllers?*
-
-SetpointManager objects place a setpoint on a node, for example, one might place a setpoint of 12C on the node named "Main Cooling Coil Air Outlet Node".
-
-In the case of Controler:WaterCoil which controls a hot water or chilled water coil, the controller reads the setpoint and tries to adjust the water flow so that the air temperature at the controlled node matches the current setpoint.  Continuing the example above:
-
-```idf
-  Controller:WaterCoil,
-    Main Cooling Coil Controller,  !- Name
-    Temperature,                   !- Control variable
-    Reverse,                       !- Action
-    Flow,                          !- Actuator variable
-    Main Cooling Coil Air Outlet Node,   !- Control_Node
-    Main Cooling Coil Water Inlet Node,  !- Actuator_Node
-    0.002,                         !- Controller Convergence Tolerance:
-                                   !- delta temp from setpoint temp {deltaC}
-    autosize,                      !- Max Actuated Flow {m3/s}
-    0.0;                           !- Min Actuated Flow {m3/s}
-```
-
-
-It is possible to place the control node downstream of the actual object being controlled, for example after other coils and the supply fan, but I recommend using the coil leaving air node as the control node for tighter control.
-
-HVAC Availability Schedules
----------------------------
-
-*How do availability schedules work?*
-
-Apply the availability schedule to the HVAC System (i.e., Furnace or DXSystem), the coils and the fan objects. If compact HVAC objects are used, apply the availability schedule to the compact HVAC object. You will get different results depending on the selection for the night cycle option.
-
-HVAC System Types
------------------
-
-*What kind of systems are available in EnergyPlus?*
-
-EnergyPlus HVAC systems input is flexible, so many different types of systems can be built using the basic available components. There are also compound components which represent common equipment types, and HVACTemplate systems which simplify the input for specific systems. This list gives an overview of HVAC objects in EnergyPlus:
-
-HVAC Templates
-
-* HVACTemplate:Thermostat
-* HVACTemplate:Zone:IdealLoadsAirSystem
-* HVACTemplate:Zone:FanCoil
-* HVACTemplate:Zone:PTAC
-* HVACTemplate:Zone:PTHP
-* HVACTemplate:Zone:Unitary
-* HVACTemplate:Zone:VAV
-* HVACTemplate:Zone:VAV:FanPowered
-* HVACTemplate:Zone:WaterToAirHeatPump
-* HVACTemplate:System:Unitary
-* HVACTemplate:System:Unitary:AirToAir
-* HVACTemplate:System:VAV
-* HVACTemplate:System:PackagedVAV
-* HVACTemplate:System:DedicatedOutdoorAir
-* HVACTemplate:Plant:ChilledWaterLoop
-* HVACTemplate:Plant:Chiller
-* HVACTemplate:Plant:Tower
-* HVACTemplate:Plant:HotWaterLoop
-* HVACTemplate:Plant:Boiler
-* HVACTemplate:Plant:MixedWaterLoop
-
-Zone HVAC Forced Air Units
-
-* ZoneHVAC:IdealLoadsAirSystem
-* ZoneHVAC:FourPipeFanCoil
-* ZoneHVAC:WindowAirConditioner
-* ZoneHVAC:PackagedTerminalAirConditioner
-* ZoneHVAC:PackagedTerminalHeatPump
-* ZoneHVAC:WaterToAirHeatPump
-* ZoneHVAC:Dehumidified:DX
-* ZoneHVAC:EnergyRecoveryVentilator
-* ZoneHVAC:EnergyRecoveryVentilator:Controller
-* ZoneHVAC:UnitVentilator
-* ZoneHVAC:UnitHeater
-* ZoneHVAC:OutdoorAirUnit
-* ZoneHVAC:TerminalUnit:VariableRefrigerantFlow
-
-Zone HVAC Radiative/Convective Units
-
-* ZoneHVAC:Baseboard:RadiantConvective:Water
-* ZoneHVAC:Baseboard:RadiantConvective:Steam
-* ZoneHVAC:Baseboard:RadiantConvective:Electric
-* ZoneHVAC:Baseboard:Convective:Water
-* ZoneHVAC:Baseboard:Convective:Electric
-* ZoneHVAC:LowTemperatureRadiant:VariableFlow
-* ZoneHVAC:LowTemperatureRadiant:ConstantFlow
-* ZoneHVAC:LowTemperatureRadiant:Electric
-* ZoneHVAC:HighTemperatureRadiant
-* ZoneHVAC:VentilatedSlab
-
-Zone HVAC Air Loop Terminal Units
-
-* AirTerminal:SingleDuct:Uncontrolled
-* AirTerminal:SingleDuct:ConstantVolume:Reheat
-* AirTerminal:SingleDuct:VAV:NoReheat
-* AirTerminal:SingleDuct:VAV:Reheat
-* AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan
-* AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat
-* AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat
-* AirTerminal:SingleDuct:SeriesPIU:Reheat
-* AirTerminal:SingleDuct:ParallelPIU:Reheat
-* AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction
-* AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam
-* AirTerminal:SingleDuct:ConstantVolume:CooledBeam
-* AirTerminal:DualDuct:ConstantVolume
-* AirTerminal:DualDuct:VAV
-* AirTerminal:DualDuct:VAV:OutdoorAir
-* ZoneHVAC:AirDistributionUnit
-
-Fans
-
-* Fan:ConstantVolume
-* Fan:VariableVolume
-* Fan:OnOff
-* Fan:ZoneExhaust
-* FanPerformance:NightVentilation
-* Fan:ComponentModel
-
-Coils
-
-* Coil:Cooling:Water
-* Coil:Cooling:Water:DetailedGeometry
-* Coil:Cooling:DX:SingleSpeed
-* Coil:Cooling:DX:TwoSpeed
-* Coil:Cooling:DX:MultiSpeed
-* Coil:Cooling:DX:TwoStageWithHumidityControlMode
-* CoilPerformance:DX:Cooling
-* Coil:Cooling:DX:VariableRefrigerantFlow
-* Coil:Heating:DX:VariableRefrigerantFlow
-* Coil:Heating:Water
-* Coil:Heating:Steam
-* Coil:Heating:Electric
-* Coil:Heating:Gas
-* Coil:Heating:Desuperheater
-* Coil:Heating:DX:SingleSpeed
-* Coil:Heating:DX:MultiSpeed
-* Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
-* Coil:Heating:WaterToAirHeatPump:ParameterEstimation
-* Coil:Cooling:WaterToAirHeatPump:EquationFit
-* Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit
-* Coil:Heating:WaterToAirHeatPump:EquationFit
-* Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit
-* Coil:WaterHeating:AirToWaterHeatPump
-* Coil:WaterHeating:Desuperheater
-* CoilSystem:Cooling:DX
-* CoilSystem:Heating:DX
-* CoilSystem:Cooling:Water:HeatExchangerAssisted
-* CoilSystem:Cooling:DX:HeatExchangerAssisted
-
-Evaporative Coolers
-
-* EvaporativeCooler:Direct:CelDekPad
-* EvaporativeCooler:Indirect:CelDekPad
-* EvaporativeCooler:Indirect:WetCoil
-* EvaporativeCooler:Indirect:ResearchSpecial
-
-Humidifiers and Dehumidifiers
-
-* Humidifier:Steam:Electric
-* Dehumidifier:Desiccant:NoFans
-* Dehumidifier:Desiccant:System
-
-Heat Recovery
-
-* HeatExchanger:AirToAir:FlatPlate
-* HeatExchanger:AirToAir:SensibleAndLatent
-* HeatExchanger:Desiccant:BalancedFlow
-* HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1
-
-Unitary Equipment
-
-* AirLoopHVAC:Unitary:Furnace:HeatOnly
-* AirLoopHVAC:Unitary:Furnace:HeatCool
-* AirLoopHVAC:UnitaryHeatOnly
-* AirLoopHVAC:UnitaryHeatCool
-* AirLoopHVAC:UnitaryHeatPump:AirToAir
-* AirLoopHVAC:UnitaryHeatPump:WaterToAir
-* AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass
-* AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed
-
-Variable Refrigerant Flow Equipment
-
-* AirConditioner:VariableRefrigerantFlow
-
-Air Distribution
-
-* AirLoopHVAC
-* AirLoopHVAC:OutdoorAirSystem:EquipmentList
-* AirLoopHVAC:OutdoorAirSystem
-* OutdoorAir:Mixer
-* AirLoopHVAC:ZoneSplitter
-* AirLoopHVAC:SupplyPlenum
-* AirLoopHVAC:SupplyPath
-* AirLoopHVAC:ZoneMixer
-* AirLoopHVAC:ReturnPlenum
-* AirLoopHVAC:ReturnPath
-
-Pumps
-
-* Pump:VariableSpeed
-* Pump:ConstantSpeed
-* Pump:VariableSpeed:Condensate
-* HeaderedPumps:VariableSpeed
-* HeaderedPumps:ConstantSpeed
-
-Solar Collectors
-
-* SolarCollectorPerformance:FlatPlate
-* SolarCollector:FlatPlate:Water
-* SolarCollector:FlatPlate:PhotovoltaicThermal
-* SolarCollectorPerformance:PhotovoltaicThermal:Simple
-* SolarCollector:IntegralCollectorStorage
-* SolarCollectorPerformance:IntegralCollectorStorage
-* SolarCollector:UnglazedTranspired
-* SolarCollector:UnglazedTranspired:Multisystem
-
-Plant Heating and Cooling Equipment
-
-* Boiler:HotWater
-* Boiler:Steam
-* Chiller:Electric:EIR
-* Chiller:Electric:ReformulatedEIR
-* Chiller:Electric
-* Chiller:Absorption:Indirect
-* Chiller:Absorption
-* Chiller:ConstantCOP
-* Chiller:EngineDriven
-* Chiller:CombustionTurbine
-* ChillerHeater:Absorption:DirectFired
-* ChillerHeater:Absorption:DoubleEffect
-* HeatPump:WaterToWater:EquationFit:Heating
-* HeatPump:WaterToWater:EquationFit:Cooling
-* HeatPump:WaterToWater:ParameterEstimation:Cooling
-* HeatPump:WaterToWater:ParameterEstimation:Heating
-* DistrictCooling
-* DistrictHeating
-
-Condenser Equipment and Heat Exchangers
-
-* CoolingTower:SingleSpeed
-* CoolingTower:TwoSpeed
-* CoolingTower:VariableSpeed
-* CoolingTowerPerformance:CoolTools
-* CoolingTowerPerformance:YorkCalc
-* EvaporativeFluidCooler:SingleSpeed
-* EvaporativeFluidCooler:TwoSpeed
-* FluidCooler:SingleSpeed
-* FluidCooler:TwoSpeed
-* GroundHeatExchanger:Vertical
-* GroundHeatExchanger:Pond
-* GroundHeatExchanger:Surface
-* HeatExchanger:FluidToFluid
-
-Water Heaters and Thermal Storage
-
-* WaterHeater:Mixed
-* WaterHeater:Stratified
-* WaterHeater:Sizing
-* WaterHeater:HeatPump:PumpedCondenser
-* WaterHeater:HeatPump:WrappedCondenser
-* ThermalStorage:Ice:Simple
-* ThermalStorage:Ice:Detailed
-* ThermalStorage:ChilledWater:Mixed
-* ThermalStorage:ChilledWater:Stratified
-
-Plant-Condenser Loops
-
-* PlantLoop
-* CondenserLoop
-* Pipe:Adiabatic
-* Pipe:Adiabatic:Steam
-* Pipe:Indoor
-* Pipe:Outdoor
-* Pipe:Underground
-
-Separating Ventilation Loads v. Zone Loads
-------------------------------------------
-
-*Can I determine the ventilation load for PAU in PAU  + FCUs system? If can, how to split the total cooling load into room load and ventilation load for PAU sizing in energyplus?*
-
-*In the HTML report, "Nominal total capacity [W]" (EquipmentSummary) and "Design Load [W]" (HVACSizingSummary) can be found. Are they equal to "Total cooling load" and "Room load"? (i.e. Ventilation load = "nominal total capacity" - "Design Load")*
-
-PAU – Primary Fresh Air Handling Unit or DOAS – Dedicated Outdoor Air Unit
-
-FCU – Fan Coil Unit
-
-There are several ways to split the total cooling load into room load and ventilation load for PAU sizing in EnergyPlus:
-
-1)   In the eio output, section, the heating and cooling loads reported there are the peak \*sensible\* loads for each zone, without any ventilation load. These are the same values reported as "Design Load" in the HVACSizingSummary table report.
-
-2)   In the EquipmentSummary table report, the component capacities reported there are the total (cooling, sensible for heating) output capacities include any ventilation load if it impacts that component.
-
-3)   If you have a central air loop that serves only the ventilation load, and zone equipment that serves only the zone load, there is an autosizing option in Sizing:System that should autosize the central system appropriately.
-
-From example file 5ZoneCoolBeam.idf:
-
-```idf
-Sizing:System,
- VAV Sys 1, !- AirLoop Name
- VentilationRequirement, !- Type of Load to Size On
- autosize, !- Design Outdoor Air Flow Rate {m3/s}
- 1.0, !- Minimum System Air Flow Ratio
-```
-
-When you run a simulation, if you want to report ventilation loads, the following Output:Variable names are available:
-
-* HVAC,Sum,Zone Mechanical Ventilation No Load Heat Removal [J]
-* HVAC,Sum,Zone Mechanical Ventilation Cooling Load Increase [J]
-* HVAC,Sum,Zone Mech Ventilation Cooling Load Increase: OverHeating [J]
-* HVAC,Sum,Zone Mechanical Ventilation Cooling Load Decrease [J]
-* HVAC,Sum,Zone Mechanical Ventilation No Load Heat Addition [J]
-* HVAC,Sum,Zone Mechanical Ventilation Heating Load Increase [J]
-* HVAC,Sum,Zone Mech Ventilation Heating Load Increase: OverCooling [J]
-* HVAC,Sum,Zone Mechanical Ventilation Heating Load Decrease [J]
-
-System not Cooling
-------------------
-
-*I built a very simple system 5 zones VAV no reheat to understand how a E+ system is put together. The results show that the cooling coil is not seeing a load. I then build the same HVACTemplate system and made sure all the details are exactly the same. The template works but not my system.*
-
-It is much easier to use HVACTemplate objects to set up your system. All required supporting objects are set up for you. Notice in your 5Zone input file, you have specified AHU1CCController for BOTH cooling coil controller lists. The second controller list should use controller name AHU2CCController. The 5Zone file worked when I used the correct controller name.
-
-```idf
-AirLoopHVAC:ControllerList,
-    AHU1SystemController,    !- Name
-    Controller:WaterCoil,       !- Controller Type 1
-    AHU1CCController;        !- Controller Name 1
-
-
-AirLoopHVAC:ControllerList,
-    AHU2SystemController,    !- Name
-    Controller:WaterCoil,       !- Controller Type 1
-    AHU1CCController;        !- Controller Name 1
-```
-
-
-Output
-======
-
-Output does not match EPW values
---------------------------------
-
-*Why do values in the EPW differ from the output reports of EnergyPlus?*
-
-This is expected. The difference comes from interpolating hourly weather data for subhourly timesteps in EnergyPlus. In an hourly weather file, the temperatures and other state-point readings are the value at the time the reading was taken. For example, in the USA\_IL\_Chicago-OHare\_TMY2.epw file, the outdoor dry bulb value for July 2, hour 1, is 19.4C. This is the temperature at 1:00 am.
-
-If you set Timestep = 1, then EnergyPlus will report 19.4C for 07/02 01:00 and will use that value for the entire one hour timestep.
-
-If Timestep = 4, then 19.4C is used only for the time step which ends at 01:00. The other timesteps use linearly interpolated values between the hourly weather file values. When you report at the "hourly" frequency in EnergyPlus, you see the average temperature over the hour. If you report at the "timestep" frequency, you will see the values from the weather data file appear at the last timestep of each hour.
-
-Schedules off by 1 hour
------------------------
-
-When active, DaylightSavingTime will shift all scheduled items by one hour. Reporting is always in standard time and uses the same day (scheduled values wrap). In short, the Daylight Saving Time flag uses the schedule value from the *next hour* in the simulation. This can be confusing if your schedules are not symmetric around the midnight hours. Because… the new schedule value will show up on the *same day*, not the next day as it might in real life. EnergyPlus does not currently to look ahead/back for next hour schedules (particularly at day boundaries).
-
-More information on Daylight Saving Periods can be seen on the web at: http://www.webexhibits.org/daylightsaving/
-
-Reporting Options
------------------
-
-There are many report variables in EnergyPlus. The ones available for a specific simulation are listed in the report data dictionary (rdd) file. These report variables may be generated automatically if the following is included in the input file.
-
-```idf
-Output:VariableDictionary,
-  Regular; !- Key Field
-```
-
-When the object above is included in an input file, the rdd file is available for review AFTER the simulation has completed. If this object is not included in the input file, the user may still use report variables, but must select them based on the objects included in the simulation. The Input Output Reference document describes all report variables available for each EnergyPlus object.
-
-There are two flavors to output variables: ZONE or HVAC.  ZONE does not mean that it is a zone variable – rather, it is produced at the Zone Time Step (the same timestep that you specify in the Timestep object. HVAC type variables, likewise, are produced at the HVAC timestep (which can differ from the zone timestep frequency based on the ConvergenceLimits object).
-
-There are several choices on format with this object. You can specify "Regular" as the key field and the rdd will show all report variables along with the variable description as shown below.
-
-* HVAC,Average,Boiler Heating Output Rate [W]
-* HVAC,Sum,Boiler Heating Output Energy [J]
-* HVAC,Average,Boiler Gas Consumption Rate [W]
-* HVAC,Sum,Boiler Gas Consumption [J]
-* HVAC,Average,Boiler Water Inlet Temp [C]
-* HVAC,Average,Boiler Water Outlet Temp [C]
-* HVAC,Average,Boiler Water Mass Flow Rate [kg/s]
-* HVAC,Average,Boiler Parasitic Electric Consumption Rate [W]
-* HVAC,Sum,Boiler Parasitic Electric Consumption [J]
-* HVAC,Average,Boiler Part-Load Ratio []
-
-As an alternative, the key field "IDF" may also be used.
-
-```idf
-Output:VariableDictionary,
-  IDF; !- Key Field
-```
-
-With this option the rdd will format the report variable so that they may be copied directly into the input file using a text editor.
-
-* Output:Variable,\*,Boiler Heating Output Rate,hourly; !- HVAC Average [W]
-* Output:Variable,\*,Boiler Heating Output Energy,hourly; !- HVAC Sum [J]
-* Output:Variable,\*,Boiler Gas Consumption Rate,hourly; !- HVAC Average [W]
-* Output:Variable,\*,Boiler Gas Consumption,hourly; !- HVAC Sum [J]
-* Output:Variable,\*,Boiler Water Inlet Temp,hourly; !- HVAC Average [C]
-* Output:Variable,\*,Boiler Water Outlet Temp,hourly; !- HVAC Average [C]
-* Output:Variable,\*,Boiler Water Mass Flow Rate,hourly; !- HVAC Average [kg/s]
-* Output:Variable,\*,Boiler Parasitic Electric Consumption Rate,hourly; !- HVAC Average [W]
-* Output:Variable,\*,Boiler Parasitic Electric Consumption,hourly; !- HVAC Sum [J]
-* Output:Variable,\*,Boiler Part-Load Ratio,hourly; !- HVAC Average ]
-
-A different version of the output variable object is shown below.
-
-```idf
-Output:Variable,
- *, !- Key Value
- Boiler Heating Output Rate, !- Variable Name
- hourly, !- Reporting Frequency
- MyReportVarSchedule; !- Schedule Name
-
-Schedule:Compact,
- MyReportVarSchedule, !- Name
- On/Off, !- Schedule Type Limits Name
- Through: 1/20, !- Field 1
- For: AllDays, !- Field 2
- Until: 24:00, 0.0, !- Field 4
- Through: 12/31, !- Field 5
- For: AllDays, !- Field 6
- Until: 24:00, 1.0; !- Field 8
-
-ScheduleTypeLimits,
- On/Off, !- Name
- 0:1, !- Range
- DISCRETE; !- Numeric Type
-```
-
-
-This allows several options for reporting. First the key value may be an asterisk (\*) where all report variables of this type are reported (for all boilers). Or the key value could be specified such that only a single output will be generated. For example if the key value was specified as "My Boiler" and a boiler object with the name My Boiler was included in the input, only the Boiler Heating Output Rate for this specific boiler will be in the output file (.csv). The reporting output for all other boilers in the simulation will not be included in the csv file.
-
-The reporting frequency is also another option and may be one of several choices (e.g., Timestep, Hourly, Daily, Monthly, RunPeriod, Environment, Annual or Detailed).
-
-The detailed reporting frequency reports the data for every simulation time step (HVAC variable time steps). This choice is useful for detailed troubleshooting and reporting. The other choices average or sum the data over the selected interval. Timestep refers to the zone Timestep/Number of Timesteps in hour value and reports the data at regular intervals. Using RunPeriod, Environment, or Annual will have the same affect on the reporting frequency and refer to the length of the simulaiton as specified in the RunPeriod object.
-
-```idf
-Timestep,
- 4; !- Number of Timesteps per Hour
-
-
-RunPeriod,
- 1, !- Begin Month
- 1, !- Begin Day of Month
- 12, !- End Month
- 31, !- End Day of Month
- Tuesday, !- Day of Week for Start Day
- Yes, !- Use Weather File Holidays and Special Days
- Yes, !- Use Weather File Daylight Saving Period
- No, !- Apply Weekend Holiday Rule
- Yes, !- Use Weather File Rain Indicators
- Yes; !- Use Weather File Snow Indicator
-```
-
-A schedule may also be used to turn on or off report variable at selected intervals.
-
-Table reports and meters are also available as reporting options. See the Input Output and Engineering Reference manuals for further details.
-
-Output Variables in IDF Editor
-------------------------------
-
-You must run the simulation before anything will show in the dropdown menu (rdd/mdd files must be present).
-
-Output Variable Definition
---------------------------
-
-In order to define output variables in your simulation, you must place the following statement in your input file:
-
-```idf
-Output:VariableDictionary,IDF;
-```
-
-Then you can cut and paste from the rdd file directly into your idf file. You must first run your simulation to create the rdd file. Output variables found in the rdd file are specific to the simulation and are based on the objects used in your input file.
-
-```idf
-Output:Variable,*,System Node Temp,hourly; !- HVAC Average [C]
-```
-
-To get only information for a single node, change to: Output:Variable,"The Name of the Node",System Node Temp,hourly; !- HVAC Average [C].
-
-Where "The Name of the Node" is the specific node name for one or more nodes.
-
-Advanced Output Variable Reporting
-----------------------------------
-
-Files for the following exercise can be found in the ExampleFiles\\AdvancedOutput folder in your installation. A four page instruction sheet is included.
-
-A shortened, bulleted list of steps is shown:
-
-- run the existing input file to generate a list of the report variables available for your simulations.
-
-- add report variables at various time aggregations to the file and run the simulation again.
-
-- create a .RVI file to extract specific data at various time aggregations.
-
-Read more about obtaining custom output files (.CSV) using .RVI (Report Variable Input) files from the output in the InputOutputReference.pdf, subject: Using ReadVarsESO.
-
-Simply said, an .RVI is a text file with a list of report variables that you want reported in a .CSV. You can easily develop multiple .RVI files which create different types of .CSV files. For example, separate .CSVs for only the exterior environment data or for only equipment energy consumption. MVI files are the equivalent kind of files for meter only output files (the .mtr files). Both .RVI and .MVI files follow this structure:
-
-```
-eplusout.eso   ! name of input eso file
-eplusout.csv   ! name of target csv file (or .tab)
-<variable name 1>
-<variable name 2>
-...
-<variable name n>
-0
-```
-
-The first two lines are the default output file .ESO and the default .CSV filename. This is followed by a list of report variables, with the last line containing a 0.
-
-1    Run the ExerciseOutput1.IDF file.
-
-2    Open ExerciseOutput1.RDD and select at least 10 loads-related variables. *Note in ExerciseOutput1.IDF, the object “Output:VariableDictionary, idf;� writes the RDD output file as complete objects which can be pasted directly into the IDF file and then edit the reporting frequency.*
-
-Edit ExerciseOutput1.IDF using the text editor, and save as ExerciseOutput1A.IDF. Paste output:variable objects for each of your loads-related variables requesting hourly data. Then copy each object and paste in 4 copies for a total of 5. Then edit the frequency parameter on each, changing “hourly� to timestep, daily, monthly, and annual, retaining hourly for one of them. There are already system related output variables with multiple reporting frequencies in the .idf file that you can use as a model. For example, Zone Window Heat Gain and Zone Window Heat Loss, insert these objects in your IDF to get data at each of these time steps:
-
-* Output:Variable, \*, Zone Window Heat Gain, timestep;
-
-* Output:Variable, \*, Zone Window Heat Gain, hourly;
-
-* Output:Variable, \*, Zone Window Heat Gain, daily;
-
-* Output:Variable, \*, Zone Window Heat Gain, monthly;
-
-* Output:Variable, \*, Zone Window Heat Gain, annual;
-
-* Output:Variable, \*, Zone Window Heat Loss, timestep;
-
-* Output:Variable, \*, Zone Window Heat Loss, hourly;
-
-* Output:Variable, \*, Zone Window Heat Loss, daily;
-
-* Output:Variable, \*, Zone Window Heat Loss, monthly;
-
-* Output:Variable, \*, Zone Window Heat Loss, annual;
-
-*Note that this step may also be done using IDF Editor. When an RDD file is present, the Output:Variable object will have an active drop-down list showing all of the report variable names present in the RDD output file.*
-
-- Run the ExerciseOutput1A.IDF file.
-
-- Using your text editor, open ExerciseOutput1A.idf. Open a new file, and save it as ExerciseOutput1A-LOADS.RVI. Type in the following:
-
-```
-eplusout.eso
-eplusout.csv
-```
-
-In the .idf file, locate the Output:Variable commands you just added. Copy them, and paste them into the new .RVI file. Delete the duplicates with different reporting frequencies, saving one instance of each variable. Delete everything but the variable name. Add a final line containing only a 0 (zero). For Window Heat Loss and Heat Gain, the .RVI file would look like this:
-
-```
-eplusout.eso
-eplusout.csv
-Zone Window Heat Gain
-Zone Window Heat Loss
-0
-```
-
-- Rename file “ExerciseOutput1-CustomCSV.b~t� to “ExerciseOutput1¬CustomCSV.bat� and edit this file in a text editor to make sure the path at the top of the file matches where your version of EnergyPlus is installed. The current path in the file is:
-
-- set post\_proc=C:\\EnergyPlusV6-0-0\\PostProcess\\
-
-- Open a Command Window (Start, Run, Command)
-
-- Change to the directory containing your ExerciseOutput1A.IDF, results files, and your new ExerciseOutput1A-LOADS.RVI. For example:
-
-- CD D:\\EnergyPlus Training\\EnergyPlusExercises ßsubstitute your path here
-
-Note: This assumes that the ExerciseOutput1-CustomCSV.bat file is located in the same directory as your IDF and RVI. This is what EP-Launch does for single simulations.
-
-- Type: ExerciseOutput1-CustomCSV ExerciseOutput1A ExerciseOutput1A-LOADS and press Enter. That is,
-
-ExerciseOutput1-CustomCSV ExerciseOutput1A ExerciseOutput1A-LOADS
-
-- ExerciseOutput1-CustomCSV reads the ESO output and creates a .CSV for the .RVI for only the variables listed in the .RVI. A .CSV is created for each of the time steps in the output file--timestep, hourly, daily, monthly, or runperiod: inputfilename\_timestep.csv, or for this exercise, ExerciseOutput1A.idf:
-
-ExerciseOutput1A\_timestep.csv
-
-ExerciseOutput1A\_hourly.csv
-
-ExerciseOutput1A\_daily.csv
-
-ExerciseOutput1A\_monthly.csv
-
-ExerciseOutput1A\_annual.csv
-
-*If there is no data at the requested time step, that .CSV file will be empty, although that should not occur here.*
-
-- Add report variables to the IDF for energy end-uses. Review .RDD, .MDD and .MTR file for variables to include. Open and save ExerciseOutput1A.idf as ExerciseOutput1B.idf. Create an energy end-use .MVI using the same structure as above but replace eplusout.eso with eplusout.mtr in the first line. Rerun the new IDF and run ExerciseOutput1-CustomCSV again:
-
-ExerciseOutput1-CustomCSV ExerciseOutput1B ExerciseOutput1B-ENERGYENDUSE
-
-- Experiment with creating other .RVIs and variables. Example .RVIs for ExerciseOutput1-EquipmentConsumption and ExerciseOutput1-ExternalEnvironment are included.
-
-Use of Comma and Point in Numeric Output
--------------------------------------------------------
-
-All EnergyPlus numeric output is written using the U.S. convention of a period or point “.� as the decimal separator. No thousands separator is used. For example, the numeric output for “one thousand two hundred and one half� would be 1200.5 in output files. The same conventions apply for EnergyPlus input files (idf), Exponent format (1.2005E+03) is also valid on input but is not used in output files.
-
-Commas are used to separate values or fields in EnergyPlus input and output. They should not be used as part of any numeric value, not as a decimal separator and not as a thousands separator. This can cause problems for users in regions of the world which normally use comma as the decimal separator. This is especially important when viewing EnergyPlusvariables (\*.csv) and meters (\*Meter.csv) output files. Typically csv output files are viewed in a spreadsheet program, such as Excel. “csv� stands for “comma separated values�, so the spreadsheet software needs to recognize comma as a list separator, not a decimal or thousands separator. If the values from a csv file appear to be nonsense when displayed in a spreadsheet program, this may be the source of the problem. Change the decimal separator to be “.�  in your system settings or in the spreadsheet program settings.
-
-Utilities
-=========
-
-Documentation and Guides
-========================
-
-Note that the PDF documents are fully indexed and searchable. Will save you time and waiting for support to answer on some questions.
-
-Errors and Warnings
-===================
-
-Max iterations exceeded
------------------------
-
-*I get the "Max Iteration" warning often, in varying quantities. I'd like to understand better what they mean. *
-
-*1) If these are a concern, at what frequency? (e.g., "whenever it occurs more than 100? 500? 1000? times in a full year run.")*
-
-*2) Roughly how much does it affect accuracy of the simulation? (A lot or a little? proportional to the number of occurrences?)*
-
-*3) Any tips about how to avoid it?*
-
-This is a good question, but it is difficult to answer.  It is something to be concerned about, but in many cases there does not seem to be a way to completely eliminate them and they aren't necessarily a cause for alarm.
-
-1) The total count is a difficult measure to use because it varies with number of zones, number and type of air systems, and length of run period.  A 1,000 might not be a problem for a big model with an annual run, but it could be way too many for a single zone design day run.  The errors are more common with VAV than CV. The frequency is key though.  I look at the timing of the errors. If they happen every time step during some period, then it usually means there is something wrong with HVAC.  If they happen only sometimes, and those times are when things are changing quickly (like recovery from setback), then I don't worry much.
-
-2) It depends if the system is succeeding at controlling the zone conditions.  If the systems are controlling well, and the errors are intermittent, then the results are probably not affected significantly.  If the systems are not controlling zone conditions, then the errors are probably very significant.  Check the comfort conditions and zone air temperatures to see.
-
-3) When the errors are significant, they usually indicate something is wrong with HVAC input that EnergyPlus isn't able to trap in some other way.  Possibilities include all sorts of things that can go wrong such as:  systems connected wrong (node connections usually), sized wrong (mixing hard and auto sizes), controlled wrong (check operation of set point managers by reporting node set point values).
-
-Error Messages (Details)
-========================
-
-Error messages are produced from several parts of EnergyPlus and at several times prior to and during Input Processing (comparing IDF fields/values to IDD requirements); during GetInput for each module (further checking for correct values from the IDF); during Sizing operations; during Warmup operations; and finally during simulation of the environments.
-
-It is easy to separate the Sizing and Warmup errors from the rest. A summary is provided at the end of the simulation:
-
-```
-************* EnergyPlus Warmup Error Summary. During Warmup: 0 Warning; 0 Severe Errors.
-************* EnergyPlus Sizing Error Summary. During Sizing: 0 Warning; 0 Severe Errors.
-************* EnergyPlus Completed Successfully-- 1 Warning; 0 Severe Errors; Elapsed Time=00hr 00min  6.58sec
-```
-
-Standard Error Message Format
------------------------------
-
-Standard error message format changes depending on where the error message is coming from. The standard error message format for GetInput goes something like this:
-
-&lt;modulename&gt;&lt;routine name&gt;: &lt;object name&gt; = &lt;name field&gt; “condition�
-
-&lt;several lines with more information may follow&gt;
-
-The &lt;modulename&gt;(optional) &lt;routinename&gt; part is so that people answering support questions can more easily find the code, if necessary and without running the input file through the debugger.
-
-As noted elsewhere, errors come in several flavors with typical user responses required.
-
-In the examples for this section, the severity (Warning/Severe/Fatal) will be left off the message unless necessary for the rest of the example. For example:
-
-**GetPlantLoopData/GetPlantAvailabilityManager:** AvailabilityManagerAssignmentList=ALWAYS\_ON not found in lists.  No availability will be used.
-
-Here the routine GetPlantLoopData/GetPlantAvailabilityManager for object AvailabilityManagerAssignmentList with name Always\_On is not found. And then the result is shown.  (This is a warning level error, by the way).
-
-The development team is working to standardize the error format, as time allows. So, sometimes you will likely see something like:
-
-Check input. Pump nominal power or motor efficiency is set to 0, for pump=HEAT RECOVERY CIRC PUMP
-
-Here, at least you know which pump (Heat Recovery Circ Pump) has the power or motor efficiency of 0.
-
-Example Error Messages for Preprocessors
-----------------------------------------
-
-All of the preprocessing programs (e.g., EP-Macro, ExpandObjects) produce Output:PreprocessorMessage objects for the errors they detect. Any preprocessor can produce these objects.  You may need to consult with actual preprocessor program documentation to understand these errors. The output preprocessor messages appear first in the .err file. The format for the messages are: &lt;objectname&gt; (i.e. Output:Preprocessormessage) followed by the program name (e.g. EPMacro) in quotes and then the strings for the message, whether Warning, Severe or Fatal.  If Fatal, EnergyPlus will fatal out after producing all the error messages.
-
-Here are some examples:
-
-### Warning
-
-```
-Output:PreprocessorMessage="EPXMLPreProc2" has the following Warning conditions:
-   **   ~~~   ** Problem with the width for requested floor area and
-   **   ~~~   ** perimeter depth.  Reduced perimeter depth from 4.57
-   **   ~~~   ** to 3.656 to accommodate perimeter and core layout
-```
-
-### Severe
-
-```
-Output:PreprocessorMessage="EPMacro" has the following Severe conditions:
-   **   ~~~   ** at approximately input line number=200: column=11
-   **   ~~~   ** cannot find/read include file
-   **   ~~~   ** symbol=HVAC3ZoneMat-Const.imf
-   **   ~~~   ** refer to <file>.epmdet for details.
-```
-
-Some preprocessor utility programs will give more details than others.  Here, you see at input file line number 200, about column 11, that the program cannot find (or read) the include file and that there will be more details after the end of EnergyPlus processing in the file with epmdet for extension.
-
-```
-Output:PreprocessorMessage="GroundTempCalc - Slab" has the following Fatal condition:
-   **   ~~~   ** No in.epw file found
-```
-
-This message is coming from the Slab preprocessor program after the ExpandObjects program has processed the input file and triggered the Slab program to be executed. There is no weather file and the Slab program cannot run.
-
-### Fatal
-
-Preprocessor condition(s) cause termination.
-
-As you can see from the above Slab message, preprocessor programs may signal a fatal condition but the actual message you see in the .err file is a Severe. You will see the above message if any of the preprocessor conditions signaled a fatal error.
-
-
-
-Example Error Messages for the Input Processor
-----------------------------------------------
-
-The InputProcessor is a part of the EnergyPlus program and scans each input file, matching it against requirements from the Energy+.idd file (Input Data Dictionary). InputProcessor errors all start with IP as their first characters.
-
-### Warning
-
-```
-IP: Note -- Some missing fields have been filled with defaults. See the audit output file for details.
-```
-
-This message notes that you have some objects where the “min-fields� for the object have not been fulfilled and, therefore, the object will be filled with defaults. If you are curious, open the .audit file and search for Warnings.
-
-### Severe
-
-```
-IP: IDF line~345 Did not find "UNTIL: 22:00" in list of Objects
-```
-
-You may have entered a semi-colon character (;) at the end of one of the lines in a [Schedule:Compact](http://www.designbuilder.co.uk/programhelp/schedules_-_energyplus_compact_schedules.htm) when you meant to enter a comma (,). Note that the approximate line number in your file (345) is given to help you locate it in a text editor. Look in the prior line – it probably needs to end in a comma.
-
-```
-IP: IDF line~xxx Did not find "xxxxxx" in list of Objects
-```
-
-Same basic description as the previous error message.  The line number in your file is given to help you locate it.  Look in the prior line (ignoring any comment lines) – it probably needs to end with a comma.
-
-```
-IP: No items found for Required Object=BUILDING
-IP: Required Object="BUILDING" not found in IDF.
-```
-
-The Building object is required for all inputs.  It was not found in this input file.
-
-```
-IP: No items found for Required Object=GLOBALGEOMETRYRULES
-IP: Required Object="GLOBALGEOMETRYRULES" not found in IDF.
-```
-
-The GlobalGeometryRules object is required for all inputs. It was not found in this input file.
-
-```
-IP: Possible incorrect IDD File
-IDD Version:"IDD\_Version xxx"
-Possible Invalid Numerics or other problems
-```
-
-This message means the program is about to terminate. You look at previous error messages in the .err file to determine the most likely cause(s). The IDD version number is given in case you have an “x� version file and you are running it with a “y� version IDD (which may or may not work, in general).
-
-### Fatal
-
-```
-IP: Errors occurred on processing IDF file. Preceding condition(s) cause termination.
-```
-
-Just the final note before the program terminates. Look at previous error messages in the .err file.
-
-Example Error Messages from Module GetInput routines
-----------------------------------------------------
-
-As the simulation starts, each module gets called and gets the values from the input file. These are usually referred to as GetInput routines. They add another error check on the inputs that cannot be fully described by the IDD limits plus they are privy to interactions that their object may have to another object.
-
-### Warning
-
-```
-Site:GroundTemperature:BuildingSurface: Some values fall outside the range of 15-25C.
-These values may be inappropriate.  Please consult the Input Output Reference for more details.
-```
-
-Ground temperatures can have a significant influence on buildings. Values outside the range indicated may give you inaccurate simulation temperatures. Consult the Input Output Reference for more details.
-
-```
-GetSurfaceData: CAUTION -- Interzone surfaces are usually in different zones
-Surface=WALLMASS, Zone=ZONE1
-Surface=iz-WALLMASS, Zone=ZONE1
-```
-
-Conventionally, interzone surfaces separate two zones. However, some advanced users may create them in the same zone for certain heat transfer efficiencies. This warning message alerts you in case that was not your intention.
-
-```
-Weather file location will be used rather than entered Location object.
-..Location object=ATLANTA
-..Weather File Location=Tampa International Ap FL USA TMY3 WMO#=722110
-..due to location differences, Latitude difference=[5.68] degrees, Longitude difference=[1.89] degrees.
-..Time Zone difference=[0.0] hour(s), Elevation difference=[98.10] percent, [309.00] meters.
-```
-
-You have “attached� a weather file that contains different location information than your Site:Location object. The program is warning you of this condition.
-
-```
-GetPollutionFactorInput: Requested reporting for Carbon Equivalent Pollution, but insufficient information is entered.
-```
-
-Both "FuelFactors" and "EnvironmentalImpactFactors" must be entered or the displayed carbon pollution will all be zero.
-
-You have requested reporting for Carbon Equivalent Pollution (output variables) but you have not entered the required FuelFactor and EnvironmentalImpactFactor objects that are necessary to trigger these outputs properly.
-
-```
-BuildingSurface:Detailed="SURF:xyz", Sun Exposure="SUNEXPOSED".
- ..This surface is not exposed to External Environment.  Sun exposure has no effect.
-```
-
-The surface has been entered with SunExposed but it is not an exterior/outdoor surface.
-
-```
-GetSurfaceData: InterZone Surface Areas do not match as expected and might not satisfy conservation of energy:
-   Area=1.4E-002 in Surface=319767, Zone=2PAV_CONDIC_LOJA_D
-   Area=67.0 in Surface=6C0708, Zone=3PAV_CONDIC_TEATRO_G
-```
-
-Interzone surface areas usually should be matching between the two zones.
-
-```
-GetSurfaceData: InterZone Surface Azimuths do not match as expected.
-   Azimuth=270.0, Tilt=90.0, in Surface=319767, Zone=2PAV_CONDIC_LOJA_D
-   Azimuth=180.0, Tilt=90.0, in Surface=6C0708, Zone=3PAV_CONDIC_TEATRO_G
-..surface class of base surface=Wall
-```
-
-Interzone surfaces should be opposite each other – therefore when Azimuth/Facing do not differ by 180 degrees, a warning is shown. Likewise, Tilt angles should be checked here.
-
-```
-GetVertices: Floor is upside down! Tilt angle=[0.0], should be near 180, Surface="ROOM302-FLOOR", in Zone="ROOM302".
-Automatic fix is attempted.
-```
-
-```
-GetVertices: Roof is upside down! Tilt angle=[180.0], should be near 0, Surface="ROOM302-CEILING", in Zone="ROOM302".
-Automatic fix is attempted.
-```
-
-In both of these messages, it has been detected that the outward surface normal for the surfaces is not as expected. With not as expected angles, the sun will not be received on these surfaces (typically), so it is something to correct. The program attempts to fix these – usually caused by entering the vertices backwards (i.e. clockwise when should have been counter-clockwise or vice versa).
-
-```
-GetInternalHeatGains: Zone="02AO_FCU04_AN" occupant density is extremely high.
-Occupant Density=[14] person/m2.
-Occupant Density=[7.000E-002] m2/person. Problems in Temperature Out of Bounds may result.
-```
-
-The Get Internal Heat Gains routine does some checks as far as Design Level (and maximum schedule \* Design Level) and compares to density values. Extremely high gains, especially when no exit for the air (i.e. infiltration, ventilation) can often result in Temperature Out of Bounds errors (see below in Simulation messages) and these can be fatal.
-
-```
-GetVertices: Distance between two vertices < .01, possibly coincident. for Surface=1%PIANOINTERRATO:UFFICI_WALL_3_0_1, in Zone=1%PIANOINTERRATO:UFFICI
-Vertex [2]=(-53.99,5.86,0.50)
-Vertex [1]=(-53.99,5.86,0.51)
-Dropping Vertex [2].
-```
-
-The distance between two vertices is very small (.01 meter ~ .4 inches). This distance is too small for shading calculations and the vertex is dropped.
-
-```
-CheckConvexity: Surface="ZN001:ROOF001" is non-convex.
-```
-
-Shown when DisplayExtraWarnings is on and a surface is not a convex shape. By itself, this is only a warning but see the severe in the next section when it has impact on the calculations.
-
-### Severe
-
-```
-GetSurfaceData: Some Outward Facing angles of subsurfaces differ significantly from base surface.
-...use Output:Diagnostics,DisplayExtraWarnings; to show more details on individual surfaces.
-```
-
-```
-GetSurfaceData: Outward facing angle [95.5] of subsurface="WL2-1" significantly different than
-..facing angle [275.5] of base surface=WEST WALL 2 Tilt=90.0
-..surface class of base surface=Wall
-```
-
-These are two versions of the same message.  The first is shown when DisplayExtraWarnings is not activated. The second is shown for details on each subsurface that has the error.  The error is usually that the subsurface vertices have been entered in opposite order (i.e. clockwise vs counter-clockwise) from the base surface.
-
-```
-This building has no thermal mass which can cause an unstable solution.
-Use Material object for all opaque material definitions except very light insulation layers.
-```
-
-You have probably defined all the surfaces in this building with resistive only constructions (i.e. object Material:NoMass). An unstable solution can result (including crashes).
-
-```
-GetVertices: Distance between two vertices < .01, possibly coincident. for Surface=1%PIANOINTERRATO:UFFICI_WALL_3_0_1, in Zone=1%PIANOINTERRATO:UFFICI
-Vertex [3]=(-44.82,-12.14,0.51)
-Vertex [2]=(-44.82,-12.14,0.50)
-Cannot Drop Vertex [3].
-Number of Surface Sides at minimum.
-```
-
-The distance between two vertices is very small (.01 meter ~ .4 inches). This distance is too small for shading calculations but the vertex cannot be dropped as that would bring the surface to less than 3 sides. This surface is degenerate and should be removed from your input file.
-
-```
-DetermineShadowingCombinations: Surface="0%VESPAIO:ZONA1\_ROOF\_1\_6\_0" is a receiving surface and is non-convex.
-...Shadowing values may be inaccurate. Check .shd report file for more surface shading details
-```
-
-Receiving surfaces which are not convex shapes will not be calculated correctly with the shadowing routines. You should view the results carefully.
-
-### Fatal
-
-Severes in this realm usually lead to Fatals.
-
-```
-<RoutineName> Preceding conditions lead to termination.
-```
-
-Example Error Messages during Sizing and Simulation
----------------------------------------------------
-
-### Warning
-
-```
-Calculated design cooling load for zone=B1AE_FCU02_AN is zero.
-Check Sizing:Zone and ZoneControl:Thermostat inputs.
-```
-
-```
-Calculated design heating load for zone=B1AE\_FCU02\_AN is zero.
-Check Sizing:Zone and ZoneControl:Thermostat inputs.
-```
-
-Two flavors of the same message showing up during Sizing. Read about Day Types in the Sizing:\* objects.  Schedules may affect how the program looks at loads during sizing. Another suggestion is:
-
-Plot the zone temperature and check against the zone thermostat set point temperature.
-
-```
-Output:Variable,*,Zone/Sys Air Temperature at Thermostat,timestep;
-Output:Variable,*,Zone/Sys Thermostat Heating Setpoint,timestep;
-```
-
-If the zone temperature never falls below the thermostat set point temperature then there really is no load and lighting, equipment, occupancy, etc inputs/schedules need to be checked. Usually these types of load will be turned off for the design days in winter to correctly size the heating system. If the zone temperature does fall below the zone thermostat temperature, then the zone sizing objects probably have bad inputs.
-
-### Severe
-
-```
-Temperature (high) out of bounds (206.82] for zone="ZONE 1", for surface="SOUTH WALL"
-During Warmup & Sizing, Environment=ALEXANDRIA ESLER REGIONAL AP ANN HTG 99.6% CONDNS DB, at Simulation time=12/21 01:00 - 01:04
-Zone="ZONE 1", Diagnostic Details:
-...Internal Heat Gain [155.557] W/m2
-...Infiltration/Ventilation [3.500E-002] m3/s
-...Mixing/Cross Mixing [0.000] m3/s
-...Zone is part of HVAC controlled system.
-```
-
-This error may be related to one of the warnings during get input routines on the Design Level of some heat gains at the zone level. Also to be noted here is the amount of Infiltration/Ventilation being introduced at the zone level. This diagnostics detail is produced once for each zone where the error occurs.
-
-### Fatal
-
-```
-EnergyPlus has exited due to the reason stated above
-...Summary of Errors that led to program termination:
-..... Reference severe error count=11
-..... Last severe error=Temperature (high) out of bounds (210.11] for zone="ZONE 1", for surface="ROOF1"
-```
-
-Typical fatal condition. A small summary of the number of severe errors that were produced along with the last severe error.
-
-Recurring Errors
-----------------
-
-The recurring error category is employed during the actual simulation periods. Usually, a heading message will appear:
-
-```
-   ** Warning ** Coil:Cooling:DX:SingleSpeed "DXCOOLINGCOIL_SOUTHZONE_2NDFLOOR" - Full load outlet air dry-bulb temperature < 2C. This indicates the possibility of coil frost/freeze. Outlet temperature = -4.60 C.
-   **   ~~~   **  ...Occurrence info = Washington Dc Dulles IntL Ar VA USA TMY3 WMO#=724030, 01/02 06:01 - 06:02
-   **   ~~~   ** ... Possible reasons for low outlet air dry-bulb temperatures are: This DX coil
-   **   ~~~   **    1) may have a low inlet air dry-bulb temperature. Inlet air temperature = 9.778 C.
-   **   ~~~   **    2) may have a low air flow rate per watt of cooling capacity. Check inputs.
-   **   ~~~   **    3) is used as part of a HX assisted cooling coil which uses a high sensible effectiveness. Check inputs.
-```
-
-This message contains quite a bit of information: the basic object and name of the object, the context of the error, the time of the error as well as some reasons why this might have occurred.
-
-At the end of the simulation, the summary appears:
-
-```
-   *************  ** Warning ** Coil:Cooling:DX:SingleSpeed "DXCOOLINGCOIL_SOUTHZONE_2NDFLOOR" - Full load outlet temperature indicates a possibility of frost/freeze error continues. Outlet air temperature statistics follow:
-   *************  **   ~~~   **   This error occurred 1240 total times;
-   *************  **   ~~~   **   during Warmup 0 times;
-   *************  **   ~~~   **   during Sizing 0 times.
-   *************  **   ~~~   **   Max=1.995912  Min=-4.60024
-```
-
-Here you see a summary of how many times the error occurred (1240) as well as how many times during Warmup (0) and how many times during Sizing (0). Plus a minimum (-4.6) and maximum (1.99) for the terms of the message.
-
-Summaries at End of Simulation
-------------------------------
-
-Some classes of warnings produce more information at the end of the simulation. For example,
-
-```
-Loads Initialization did not Converge (CheckWarmupConvergence) after 25 warmup days.
-Environment=SAN_FRANCISCO ANN CLG 1% CONDNS DB=&gt;MWB
-Max Temp Comparison=9.15E-002 vs Temperature Convergence Tolerance=4.00E-003 - Fail Convergence
-Min Temp Comparison=1.75E-003 vs Temperature Convergence Tolerance=4.00E-003 - Pass Convergence
-Max Cool Load Comparison=2.9010E-002 vs Loads Convergence Tolerance=4.00E-002 - Pass Convergence
-Then, at the end of the simulation, you will see:
-******** The following error categories occurred.  Consider correcting or noting.
-******** Loads Initialization did not Converge
-******** ..1) very high thermal mass such as very thick concrete (solution: increase max number of warmup
-******** ..   days in the BUILDING object);
-******** ..2) moderate mass and inadequate space conditioning such that the building keeps getting warmer
-******** ..   and warmer on successive days (solution: add HVAC, check building thermal properties,
-******** ..   check if infiltration is included, make sure HVAC properly controlled);
-******** ..3) a soil layer modeled below the concrete slab - (solution remove this layer and read about
-******** ..   ground temperatures in the Auxiliary Programs document).
-******** ..4) unreasonable (too small) limits in the BUILDING object for temperature (.4 default) or
-******** ..   loads tolerances (.04 default)
-```
-
-Psychrometric Errors
---------------------
-
-EnergyPlus has built-in psychrometric routines that perform various calculations for the simulation modules. They typically fall into the recurring error category but may warrant some view:
-
-```
-   ** Warning ** Calculated Relative Humidity out of range (PsyRhFnTdbWPb)
-
-   **   ~~~   **  Routine=NodeReportingCalc:NODE_1, Environment=CHICAGO_IL_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB, at Simulation time=07/21 00:00 - 00:10
-
-   **   ~~~   **  Dry-Bulb= 13.00 Humidity Ratio= 1.000E-002 Calculated Relative Humidity [%]= 104.65
-
-   **   ~~~   ** Relative Humidity being reset to 100.0%
-```
-
-This warning notes that the calculated relative humidity is out of rage (routine name: PsyRhFnTdbWPb). It happened during routine NodeReportingCalc for NODE\_1 at the environment “CHICAGO\_IL\_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB� during the time interval 00:00 – 00:10 on July 21. The dry bulb temperature was 13 C, the humidity ratio was .001 for a calculated relative humidity of 104.65%. It is reset to 100%.
-
-Then, at the end of the run, you will see a summary of how many times that occur and the min/max extent:
-
-```
-   *************  ** Warning ** Calculated Relative Humidity out of range (PsyRhFnTdbWPb)
-
-   *************  **   ~~~   **   This error occurred 645 total times;
-
-   *************  **   ~~~   **   during Warmup 0 times;
-
-   *************  **   ~~~   **   during Sizing 0 times.
-
-   *************  **   ~~~   **   Max=104.652877 %  Min=104.652877 %
-```
-
-Error Summary
--------------
-
-This section has provided a flavor of the breadth of messages coming out of EnergyPlus for various conditions. They are consolidated into one file (eplusout.err) for the most part though some may have more contexts given in other files. (eplusout.audit may illustrate exact places in the IDF where warnings or errors occur – as noted during Input Processing.)
-
-The error section in this document will continue to grow as time allows. Suggestions are always welcome.
-
-Validation and Testing
-======================
-
-An important ongoing part of EnergyPlus development is testing using industry standard methods as major builds are completed. The goal is to make EnergyPlus as bug-free as possible. Three major types of tests are currently conducted:
-
-- Analytical tests:
-
-- HVAC tests, based on ASHRAE Research Project 865
-
-- Building fabric tests, based on ASHRAE Research Project 1052
-
-- Comparative tests:
-
-- ANSI/ASHRAE Standard 140-2007
-
-- International Energy Agency Solar Heating and Cooling Programme (IEA SHC) BESTest (Building Energy Simulation Test) methods not yet in Standard 140
-
-- EnergyPlus HVAC Component Comparative tests
-
-- EnergyPlus Global Heat Balance tests
-
-- Release and executable tests
-
-For detailed reports, please use the following link:
-
-http://apps1.eere.energy.gov/buildings/energyplus/energyplus\_testing.cfm
-
-Platforms and Run-Time
-======================
-
-EnergyPlus is available for the Windows, Macintosh, and Linux Platforms. It may not be available for all flavors of those platforms. Usually, the newer versions of those platforms will be the ones most supported with some older versions as well.
-
-Reduce EnergyPlus Run Time
---------------------------
-
-*What affects EnergyPlus Run-Time?*
-
-Compared with creating energy models either by hand coding the IDF file or by using GUI tools or a combination of both, EnergyPlus run time is normally a small fraction of the total time needed to complete an energy modeling job. Therefore it is very important to build a clean and concise EnergyPlus model up front. Techniques of simplifying large and complex building and systems should be used during the creation of energy models, especially during the early design process when detailed zoning and other information is not available. Producing lots of hourly or sub-hourly reports from EnergyPlus runs can take significant amount of time. Modelers should only request time step reports when necessary. On the other hand, producing summary reports and typical monthly reports take relatively small amount of run time. These reports are valuable references for troubleshooting and model fine tuning.
-
-With powerful personal computers get more and more affordable, EnergyPlus modelers should choose to use current available PCs with 3 or more GHZ clock speed and 3 or more GB of RAM and multiple core processors. EP-Launch will now automatically launch multiple runs on multiple processors (group runs).
-
-For modelers, most time is spent on troubleshooting and fine tuning energy models. During the early modeling process, it is recommended to keep the model as simple as possible and make quick runs to identify problems. Then modify the IDF file to fix problems and re-run the model. This is an iterative process until satisfactory solutions are found. The simulation process can be split into three phases: the diagnostic runs, the preliminary runs, and the final runs. The three phases would use different simulation settings. The diagnostic runs would use a set of simulation settings to speed up the runs with simulation accuracy being set as the second priority. The diagnostic runs will help catch most model problems by running simulations on summer and winter design days. The preliminary runs use a tighter set of simulation settings in order to catch problems missed in the diagnostic runs, and provide better results for quality assurance purpose. The final runs use the EnergyPlus recommended set of simulation settings in order to achieve better accuracy for simulation results ready for review and reporting.
-
-Specifically, recommendations (and particularly recommended for large buildings with large numbers of surfaces and shading surfaces):
-
-Table 5. Recommended Reduce Time Settings for Early Diagnostic runs
-
-<table class="table table-striped">
-<tr>
-<th>Object</th>
-<th>Recommenheh Early Diagnostic Setting</th>
-</tr>
-<tr>
-<td>Building</td>
-<td>MinimalShadowing (Solar Distribution field)</td>
-</tr>
-<tr>
-<td>ShadowCalculation</td>
-<td>200 (Maximum Figures in Shadow Overlap Calculations field)</td>
-</tr>
-<tr>
-<td>SizingPeriod:DesignDays</td>
-<td>Only perform design day or limited run period runs until you have the model set.</td>
-</tr>
-</table>
-
-
-
-You might want to read the report on EnergyPlus run time at http://repositories.cdlib.org/lbnl/LBNL-1311E/
-
-Remember, too, that EnergyPlus is, by design, a multiple timestep per hour simulation. Comparing its run-time to programs that are only hourly has potential for comparing apples and grapes. In addition, EnergyPlus is a simultaneous solution of the building loads, HVAC system and plant equipment simulation with possible multiple iterations to reach balance.
-
-Run EnergyPlus in Parallel
---------------------------
-
-EnergyPlus is a multi-thread application but is not optimized for parallel runs on multi-core machines. However, multiple parametric runs can be launched in parallel if these runs are independent. One way to do it is to create multiple folders and copy files EnergyPlus.exe, Energy+.idd, DElight2.dll, libexpat.dll, bcvtb.dll, EPMacro.exe (if macros are used), ExpandObjects.exe (if HVACTemplate or Compact HVAC objects are used) from the original EnergyPlus installed folder. Inside each folder, copy IDF file as in.idf and EPW file as in.epw, then run EnergyPlus.exe from each folder. This is better handled with a batch file. If the Energy+.ini file exists in one of the created folders, make sure it is empty or points to the current EnergyPlus folder.
-
-EP-Launch now does this automatically for Group or Parametric-Preprocessor runs.
-
-The benefit of run time savings depends on computer configurations including number of CPUs, CPU clock speed, amount of RAM and cache, and hard drive speed. To be time efficient, the number of parallel EnergyPlus runs should not be more than the number of CPUs on a computer. The EnergyPlus utility program EP-Launch is being modified to add the parallel capability for group simulations. The long term goal is to run EnergyPlus in parallel on multi-core computers even for a single EnergyPlus run without degradation to accuracy.
-
-Running EnergyPlus on Windows Vista and/or Windows 7
-----------------------------------------------------
-
-For all operating systems, make sure that you have read and write access to files in the main EnergyPlus folder (by default EnergyPlus is installed in C:\\EnergyPlus&lt;version&gt;). If you do not have this kind of access some very peculiar messages may appear when you try to run simulations.
-
-EnergyPlus has no problems running on Vista or Windows 7 computers if it is run directly by executing the EnergyPlus.exe file assuming you have prepared the in.idf and in.epw files at the same folder. There were some issues running earlier versions of EP-Launch, but most have been fixed for the latest version of EP-Launch. If EnergyPlus was installed at a user folder like C:\\ EnergyPlusV3-0-0, there should be no problems running EP-Launch. If EnergyPlus was installed at a windows system folder like ‘C:\\Program files\\ EnergyPlusV3-0-0’, you have to run EP-Launch every time with administrator rights by right clicking the EP-Launch.exe file and choose ‘Run as Administrator’. Another way is to create a shortcut to EPLaunch and change settings appropriately.
-
-
diff --git a/doc/src/docs/Using_EnergyPlus_for_Compliance/Using_EnergyPlus_for_Compliance.md b/doc/src/docs/Using_EnergyPlus_for_Compliance/Using_EnergyPlus_for_Compliance.md
deleted file mode 100644
index 73d0b5cc75f..00000000000
--- a/doc/src/docs/Using_EnergyPlus_for_Compliance/Using_EnergyPlus_for_Compliance.md
+++ /dev/null
@@ -1,3153 +0,0 @@
-![](media/ep.gif)
-
-<br/>
-<p><h1>EnergyPlus<sup>TM</sup> Documentation, v8.4.0</h1></p>
-<hr>
-<h1>Using EnergyPlus for Compliance</h1>
-<h2>Hints on using EnergyPlus for Compliance with Standards and Rating Systems</h2>
-<br/>
-<p><i>(stay inside the lines...)</i></p>
-<br/>
-<p><small>COPYRIGHT (c) 1996-2015 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.</small></p>
-<p style="page-break-after:always;"></p>
-<div id="generated-toc"></div>
-<p style="page-break-after:always;"></p>
-
-Introduction
-============
-
-Background
-----------
-
-Energy Standards abound throughout the world. This document provides guidance on using EnergyPlus and its reports for compliance with energy standards.
-
-The tabular reports from EnergyPlus were designed to help collate information into a form usually required for reporting on designs for energy use. The tabular reports are fully described in the Output Details document and will be judiciously reproduced here for clarity and reference. In addition, by using the Output:Table:Style object, one can obtain the reports in a variety of formats – ready for incorporating into your own style for submission or presentation.
-
-First, we describe the features available in the tabular report that might be used for energy compliance reporting or presentation of energy designs to clients.
-
-Compliance Objects
-------------------
-
-To facilitate using EnergyPlus for compliance reporting, a group of Compliance Objects is described in the Input Output Reference document. Currently, there is only one object in this group: **Compliance:Building** which, when fully populated, will describe various aspects that are needed specific to buildings. Other compliance objects will be added to this group when appropriate.
-
-Tabular Summary Reports
------------------------
-
-Several predefined reports are available from the Output Table:Predefined object including the following.
-
-- Annual Building Utility Performance Summary
-
-- Input Verification and Results Summary
-
-- Demand End Use Components Summary
-
-- Source Energy End Use Components Summary
-
-- Climatic Data Summary
-
-- Equipment Summary
-
-- Envelope Summary
-
-- Surface Shadowing Summary
-
-- Shading Summary
-
-- Lighting Summary
-
-- HVAC Sizing Summary
-
-- System Summary
-
-- Component Sizing Summary
-
-- Outside Air Summary
-
-- Object Count Summary
-
-In addition, specifying “All Summary� will enable all the reports in this category (more than are shown here).
-
-### Annual Building Utility Performance Summary
-
-First and foremost, the Annual Building Utility Performance Summary gives a good overview of the energy use by category:
-
-
-
-Report: **AnnualBuildingUtilityPerformanceSummary**
-
-For: **Entire Facility**
-
-Timestamp: **2009-09-17 17:30:22**
-
-Values gathered over 8760.00 hours
-
-
-
-
-Site and Source Energy
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Total Energy [GJ]</th>
-<th>Energy Per Total Building Area [MJ/m2]</th>
-<th>Energy Per Conditioned Building Area [MJ/m2]</th>
-</tr>
-<tr>
-<td>Total Site Energy</td>
-<td>180.73</td>
-<td>194.92</td>
-<td>194.92</td>
-</tr>
-<tr>
-<td>Net Site Energy</td>
-<td>180.73</td>
-<td>194.92</td>
-<td>194.92</td>
-</tr>
-<tr>
-<td>Total Source Energy</td>
-<td>1141.64</td>
-<td>1231.28</td>
-<td>1231.28</td>
-</tr>
-<tr>
-<td>Net Source Energy</td>
-<td>1141.64</td>
-<td>1231.28</td>
-<td>1231.28</td>
-</tr>
-</table>
-
-
-
- Source to Site Energy Conversion Factors
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Source=&gt;Site Conversion Factor</th>
-</tr>
-<tr>
-<td>Electricity</td>
-<td>0.293</td>
-</tr>
-<tr>
-<td>Natural Gas</td>
-<td>0.010</td>
-</tr>
-<tr>
-<td>District Cooling</td>
-<td>0.098</td>
-</tr>
-<tr>
-<td>District Heating</td>
-<td>0.033</td>
-</tr>
-<tr>
-<td>Steam</td>
-<td>0.250</td>
-</tr>
-<tr>
-<td>Gasoline</td>
-<td>1.050</td>
-</tr>
-<tr>
-<td>Diesel</td>
-<td>1.050</td>
-</tr>
-<tr>
-<td>Coal</td>
-<td>1.050</td>
-</tr>
-<tr>
-<td>Fuel Oil #1</td>
-<td>1.050</td>
-</tr>
-<tr>
-<td>Fuel Oil #2</td>
-<td>1.050</td>
-</tr>
-<tr>
-<td>Propane</td>
-<td>1.050</td>
-</tr>
-</table>
-
-
-
- Building Area
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Area [m2]</th>
-</tr>
-<tr>
-<td>Total Building Area</td>
-<td>927.20</td>
-</tr>
-<tr>
-<td>Net Conditioned Building Area</td>
-<td>927.20</td>
-</tr>
-<tr>
-<td>Unconditioned Building Area</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
- End Uses
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Electricity [GJ]</th>
-<th>Natural Gas [GJ]</th>
-<th>Other Fuel [GJ]</th>
-<th>District Cooling [GJ]</th>
-<th>District Heating [GJ]</th>
-<th>Water [m3]</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>0.00</td>
-<td>28.16</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>16.56</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>81.24</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>47.70</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>6.59</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>0.48</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Total End Uses</td>
-<td>152.57</td>
-<td>28.16</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-*Note: Natural gas appears to be the principal heating source based on energy usage.*
-
- End Uses By Subcategory
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Subcategory</th>
-<th>Electricity [GJ]</th>
-<th>Natural Gas [GJ]</th>
-<th>Other Fuel [GJ]</th>
-<th>District Cooling [GJ]</th>
-<th>District Heating [GJ]</th>
-<th>Water [m3]</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>Boiler</td>
-<td>0.00</td>
-<td>28.16</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td> </td>
-<td>Boiler Parasitic</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>General</td>
-<td>16.56</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>GeneralLights</td>
-<td>81.24</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>General</td>
-<td>47.70</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>General</td>
-<td>6.59</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>General</td>
-<td>0.48</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>General</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
- Normalized Metrics
-
- Utility Use Per Conditioned Floor Area
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Electricity Intensity [MJ/m2]</th>
-<th>Natural Gas Intensity [MJ/m2]</th>
-<th>Other Fuel Intensity [MJ/m2]</th>
-<th>District Cooling Intensity [MJ/m2]</th>
-<th>District Heating Intensity [MJ/m2]</th>
-<th>Water Intensity [m3/m2]</th>
-</tr>
-<tr>
-<td>Lighting</td>
-<td>87.62</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>HVAC</td>
-<td>25.49</td>
-<td>30.37</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Other</td>
-<td>51.44</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>164.55</td>
-<td>30.37</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
- Utility Use Per Total Floor Area
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Electricity Intensity [MJ/m2]</th>
-<th>Natural Gas Intensity [MJ/m2]</th>
-<th>Other Fuel Intensity [MJ/m2]</th>
-<th>District Cooling Intensity [MJ/m2]</th>
-<th>District Heating Intensity [MJ/m2]</th>
-<th>Water Intensity [m3/m2]</th>
-</tr>
-<tr>
-<td>Lighting</td>
-<td>87.62</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>HVAC</td>
-<td>25.49</td>
-<td>30.37</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Other</td>
-<td>51.44</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>164.55</td>
-<td>30.37</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
- Electric Loads Satisfied
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Electricity [GJ]</th>
-<th>Percent Electricity [%]</th>
-</tr>
-<tr>
-<td>Fuel-Fired Power Generation</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>High Temperature Geothermal*</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Photovoltaic Power</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Wind Power*</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Net Decrease in On-Site Storage</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total On-Site Electric Sources</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Electricity Coming From Utility</td>
-<td>152.57</td>
-<td>100.00</td>
-</tr>
-<tr>
-<td>Surplus Electricity Going To Utility</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Net Electricity From Utility</td>
-<td>152.57</td>
-<td>100.00</td>
-</tr>
-<tr>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Total On-Site and Utility Electric Sources</td>
-<td>152.57</td>
-<td>100.00</td>
-</tr>
-<tr>
-<td>Total Electricity End Uses</td>
-<td>152.57</td>
-<td>100.00</td>
-</tr>
-</table>
-
-
-
- On-Site Thermal Sources
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Heat [GJ]</th>
-<th>Percent Heat [%]</th>
-</tr>
-<tr>
-<td>Water-Side Heat Recovery</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>Air to Air Heat Recovery for Cooling</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>Air to Air Heat Recovery for Heating</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>High-Temperature Geothermal*</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>Solar Water Thermal</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>Solar Air Thermal</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>Total On-Site Thermal Sources</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Water Source Summary
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Water [m3]</th>
-<th>Percent Water [%]</th>
-</tr>
-<tr>
-<td>Rainwater Collection</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Condensate Collection</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Groundwater Well</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Total On Site Water Sources</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>-</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Initial Storage</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Final Storage</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Change in Storage</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>-</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Water Supplied by Utility</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>-</td>
-<td>-</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Total On Site, Change in Storage, and Utility Water Sources</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-<tr>
-<td>Total Water End Uses</td>
-<td>0.00</td>
-<td>-</td>
-</tr>
-</table>
-
-
-
- Comfort and Setpoint Not Met Summary
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Facility [Hours]</th>
-</tr>
-<tr>
-<td>Time Set Point Not Met During Occupied Heating</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Time Set Point Not Met During Occupied Cooling</td>
-<td>213.25</td>
-</tr>
-<tr>
-<td>Time Not Comfortable Based on Simple ASHRAE 55-2004</td>
-<td>72.50</td>
-</tr>
-</table>
-
-
-
- Note 1: An asterisk (\*) indicates that the feature is not yet implemented.
-
-### Input Verification Summary
-
-The input verification summary gives a good overview of the facility being simulated:
-
-
-
-Report: **InputVerificationandResultsSummary**
-
-For: **Entire Facility**
-
-**Timestamp: 2009-09-17 17:30:22**
-
-General
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Value</th>
-</tr>
-<tr>
-<td>Program Version and Build</td>
-<td>EnergyPlus 4.0.0.017, 9/17/2009 5:30 PM</td>
-</tr>
-<tr>
-<td>Weather</td>
-<td>Climate Zone 6 CA USA WYEC2-C-00006 WMO#=722970</td>
-</tr>
-<tr>
-<td>Latitude [deg]</td>
-<td>33.90</td>
-</tr>
-<tr>
-<td>Longitude [deg]</td>
-<td>-118.5</td>
-</tr>
-<tr>
-<td>Elevation [m]</td>
-<td>30.00</td>
-</tr>
-<tr>
-<td>Time Zone</td>
-<td>-8.0</td>
-</tr>
-<tr>
-<td>North Axis Angle [deg]</td>
-<td>30.00</td>
-</tr>
-<tr>
-<td>Rotation for Appendix G [deg]</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Hours Simulated [hrs]</td>
-<td>8760.00</td>
-</tr>
-</table>
-
-
-
- ENVELOPE
-
- Window-Wall Ratio
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Total</th>
-<th>North (315 to 45 deg)</th>
-<th>East (45 to 135 deg)</th>
-<th>South (135 to 225 deg)</th>
-<th>West (225 to 315 deg)</th>
-</tr>
-<tr>
-<td>Gross Wall Area [m2]</td>
-<td>274.20</td>
-<td>91.50</td>
-<td>45.60</td>
-<td>91.50</td>
-<td>45.60</td>
-</tr>
-<tr>
-<td>Window Opening Area [m2]</td>
-<td>60.90</td>
-<td>20.85</td>
-<td>9.12</td>
-<td>21.81</td>
-<td>9.12</td>
-</tr>
-<tr>
-<td>Window-Wall Ratio [%]</td>
-<td>22.21</td>
-<td>22.79</td>
-<td>20.00</td>
-<td>23.84</td>
-<td>20.00</td>
-</tr>
-</table>
-
-
-
- Skylight-Roof Ratio
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Total</th>
-</tr>
-<tr>
-<td>Gross Roof Area [m2]</td>
-<td>463.60</td>
-</tr>
-<tr>
-<td>Skylight Area [m2]</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Skylight-Roof Ratio [%]</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
- PERFORMANCE
-
- Zone Summary
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Area [m2]</th>
-<th>Conditioned (Y/N)</th>
-<th>Volume [m3]</th>
-<th>Multipliers</th>
-<th>Gross Wall Area [m2]</th>
-<th>Window Glass Area [m2]</th>
-<th>Lighting [W/m2]</th>
-<th>People [m2] per person</th>
-<th>Plug and Process [W/m2]</th>
-</tr>
-<tr>
-<td>PLENUM-1</td>
-<td>463.60</td>
-<td>Yes</td>
-<td>283.20</td>
-<td>1.00</td>
-<td>54.84</td>
-<td>0.00</td>
-<td>0.0000</td>
-<td> </td>
-<td>0.0000</td>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>99.16</td>
-<td>Yes</td>
-<td>239.25</td>
-<td>1.00</td>
-<td>73.20</td>
-<td>21.81</td>
-<td>15.9742</td>
-<td>9.01</td>
-<td>10.6495</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>42.73</td>
-<td>Yes</td>
-<td>103.31</td>
-<td>1.00</td>
-<td>36.48</td>
-<td>9.12</td>
-<td>16.0056</td>
-<td>8.55</td>
-<td>10.6704</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>96.48</td>
-<td>Yes</td>
-<td>239.25</td>
-<td>1.00</td>
-<td>73.20</td>
-<td>20.85</td>
-<td>16.4179</td>
-<td>8.77</td>
-<td>10.9453</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>42.73</td>
-<td>Yes</td>
-<td>103.31</td>
-<td>1.00</td>
-<td>36.48</td>
-<td>9.12</td>
-<td>16.0056</td>
-<td>8.55</td>
-<td>10.6704</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>182.49</td>
-<td>Yes</td>
-<td>447.68</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>16.2420</td>
-<td>9.12</td>
-<td>10.8280</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>927.20</td>
-<td> </td>
-<td>1416.00</td>
-<td> </td>
-<td>274.20</td>
-<td>60.90</td>
-<td>8.0889</td>
-<td>17.83</td>
-<td>5.3926</td>
-</tr>
-<tr>
-<td>Conditioned Total</td>
-<td>927.20</td>
-<td> </td>
-<td>1416.00</td>
-<td> </td>
-<td>274.20</td>
-<td>60.90</td>
-<td>8.0889</td>
-<td>17.83</td>
-<td>5.3926</td>
-</tr>
-<tr>
-<td>Unconditioned Total</td>
-<td>0.00</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-<td>0.00</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
-### Source Energy End Use Components Summary
-
-The source energy end use components summary gives a good overview of the source energy consumption broken down by end uses for the facility being simulated:
-
-
-
-Report: **SourceEnergyEndUseComponentsSummary**
-
-For: **Entire Facility**
-
-Timestamp: **2011-10-07 20:53:43**
-
-**Values gathered over 8760.00 hours**
-
- **Source Energy End Use Components Summary**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Source Electricity [GJ]</th>
-<th>Source Natural Gas [GJ]</th>
-<th>Source Other Fuel [GJ]</th>
-<th>Source District Cooling [GJ]</th>
-<th>Source District Heating [GJ]</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>0.00</td>
-<td>140.03</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>167.65</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>569.39</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>325.49</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>55.72</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>7.57</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-</tr>
-<tr>
-<td>Total Source Energy End Use Components</td>
-<td>1125.82</td>
-<td>140.03</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
- **Normalized Metrics**
-
- **Source Energy End Use Components Per Conditioned Floor Area**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Source Electricity [MJ/m2]</th>
-<th>Source Natural Gas [MJ/m2]</th>
-<th>Source Other Fuel [MJ/m2]</th>
-<th>Source District Cooling [MJ/m2]</th>
-<th>Source District Heating [MJ/m2]</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>0.00</td>
-<td>151.02</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>180.82</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>614.09</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>351.05</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>60.10</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>8.16</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-</tr>
-<tr>
-<td>Total Source Energy End Use Components</td>
-<td>1214.22</td>
-<td>151.02</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
- **Source Energy End Use Components Per Total Floor Area**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Source Electricity [MJ/m2]</th>
-<th>Source Natural Gas [MJ/m2]</th>
-<th>Source Other Fuel [MJ/m2]</th>
-<th>Source District Cooling [MJ/m2]</th>
-<th>Source District Heating [MJ/m2]</th>
-</tr>
-<tr>
-<td>Heating</td>
-<td>0.00</td>
-<td>151.02</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooling</td>
-<td>180.82</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>614.09</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Equipment</td>
-<td>351.05</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans</td>
-<td>60.10</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>8.16</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Humidification</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Recovery</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Water Systems</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Generators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-<td></td>
-</tr>
-<tr>
-<td>Total Source Energy End Use Components</td>
-<td>1214.22</td>
-<td>151.02</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-### Other Summary Reports
-
-The Climatic Data Summary, Envelope Summary and Equipment Summary reports might be quite important to some reporting or presentation.
-
-
-
-Report: **ClimaticDataSummary**
-
-For: **Entire Facility**
-
-**Timestamp: 2009-09-17 17:30:22**
-
-SizingPeriod:DesignDay
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Maximum Dry Bulb [C]</th>
-<th>Daily Temperature Range [C]</th>
-<th>Humidity Value</th>
-<th>Humidity Type</th>
-<th>Wind Speed [m/s]</th>
-<th>Wind Direction</th>
-</tr>
-<tr>
-<td>LOS_ANGELES_CA_USA HEATING 99% CONDITIONS</td>
-<td>7.40</td>
-<td>0.00</td>
-<td>7.40</td>
-<td>0</td>
-<td>2.80</td>
-<td>70.00</td>
-</tr>
-<tr>
-<td>LOS_ANGELES_CA_USA COOLING 1% CONDITIONS DB=&gt;MWB</td>
-<td>27.00</td>
-<td>6.10</td>
-<td>17.60</td>
-<td>0</td>
-<td>4.40</td>
-<td>250.00</td>
-</tr>
-</table>
-
-
-
-Weather Statistics File
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Value</th>
-</tr>
-<tr>
-<td>Reference</td>
-<td>CZ06RV2</td>
-</tr>
-<tr>
-<td>Site:Location</td>
-<td>Climate Zone 6 CA USA</td>
-</tr>
-<tr>
-<td>Latitude</td>
-<td>N 33° 54'</td>
-</tr>
-<tr>
-<td>Longitude</td>
-<td>W 118° 30'</td>
-</tr>
-<tr>
-<td>Time Zone</td>
-<td>GMT -8.0 Hours</td>
-</tr>
-<tr>
-<td>Elevation</td>
-<td>30m above sea level</td>
-</tr>
-<tr>
-<td>Standard Pressure at Elevation</td>
-<td>100965Pa</td>
-</tr>
-<tr>
-<td>Data Source</td>
-<td>WYEC2-C-00006</td>
-</tr>
-<tr>
-<td>WMO Station</td>
-<td>722970</td>
-</tr>
-<tr>
-<td>Design Conditions</td>
-<td>Climate Design Data 2005 ASHRAE Handbook</td>
-</tr>
-<tr>
-<td>Heating Design Temperature 99.6% (C)</td>
-<td>4.9</td>
-</tr>
-<tr>
-<td>Heating Design Temperature 99% (C)</td>
-<td>6.2</td>
-</tr>
-<tr>
-<td>Cooling Design Temperature 0.4% (C)</td>
-<td>33.1</td>
-</tr>
-<tr>
-<td>Cooling Design Temperature 1% (C)</td>
-<td>30.9</td>
-</tr>
-<tr>
-<td>Cooling Design Temperature 2% (C)</td>
-<td>29.2</td>
-</tr>
-<tr>
-<td>Maximum Dry Bulb Temperature (C)</td>
-<td>31.7°</td>
-</tr>
-<tr>
-<td>Maximum Dry Bulb Occurs on</td>
-<td>Sep 24</td>
-</tr>
-<tr>
-<td>Minimum Dry Bulb Temperature (C)</td>
-<td>3.5°</td>
-</tr>
-<tr>
-<td>Minimum Dry Bulb Occurs on</td>
-<td>Jan 8</td>
-</tr>
-<tr>
-<td>Maximum Dew Point Temperature (C)</td>
-<td>20.9</td>
-</tr>
-<tr>
-<td>Maximum Dew Point Occurs on</td>
-<td>Jun 20</td>
-</tr>
-<tr>
-<td>Minimum Dew Point Temperature (C)</td>
-<td>-21.7</td>
-</tr>
-<tr>
-<td>Minimum Dew Point Occurs on</td>
-<td>Dec 27</td>
-</tr>
-<tr>
-<td>Heating Degree-Days (base 10°C)</td>
-<td>2</td>
-</tr>
-<tr>
-<td>Cooling Degree-Days (base 18°C)</td>
-<td>216</td>
-</tr>
-<tr>
-<td>Köppen Classification</td>
-<td>Csb</td>
-</tr>
-<tr>
-<td>Köppen Description</td>
-<td>Mediterranean climate (dry warm summer, mild winter, lat. 30-45°N)</td>
-</tr>
-<tr>
-<td>Köppen Recommendation</td>
-<td> </td>
-</tr>
-<tr>
-<td>ASHRAE Climate Zone</td>
-<td>3C</td>
-</tr>
-<tr>
-<td>ASHRAE Description</td>
-<td>Warm-Marine</td>
-</tr>
-</table>
-
-
-
-
-
-Report: **EnvelopeSummary**
-
-For: **Entire Facility**
-
-**Timestamp: 2009-09-17 17:30:22**
-
-Opaque Exterior
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Construction</th>
-<th>Reflectance</th>
-<th>U-Factor with Film [W/m2-K]</th>
-<th>U-Factor no Film [W/m2-K]</th>
-<th>Gross Area [m2]</th>
-<th>Azimuth [deg]</th>
-<th>Tilt [deg]</th>
-<th>Cardinal Direction</th>
-</tr>
-<tr>
-<td>WALL-1PF</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.408</td>
-<td>18.30</td>
-<td>210.00</td>
-<td>90.00</td>
-<td>S</td>
-</tr>
-<tr>
-<td>WALL-1PR</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.408</td>
-<td>9.12</td>
-<td>120.00</td>
-<td>90.00</td>
-<td>E</td>
-</tr>
-<tr>
-<td>WALL-1PB</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.408</td>
-<td>18.30</td>
-<td>30.00</td>
-<td>90.00</td>
-<td>N</td>
-</tr>
-<tr>
-<td>WALL-1PL</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.408</td>
-<td>9.12</td>
-<td>300.00</td>
-<td>90.00</td>
-<td>W</td>
-</tr>
-<tr>
-<td>TOP-1</td>
-<td>ROOF-1</td>
-<td>0.35</td>
-<td>0.268</td>
-<td>0.282</td>
-<td>463.60</td>
-<td>210.00</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>FRONT-1</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.408</td>
-<td>73.20</td>
-<td>210.00</td>
-<td>90.00</td>
-<td>S</td>
-</tr>
-<tr>
-<td>F1-1</td>
-<td>FLOOR-SLAB-1</td>
-<td>0.35</td>
-<td>3.119</td>
-<td>12.894</td>
-<td>99.16</td>
-<td>30.00</td>
-<td>180.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>RIGHT-1</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.408</td>
-<td>36.48</td>
-<td>120.00</td>
-<td>90.00</td>
-<td>E</td>
-</tr>
-<tr>
-<td>F2-1</td>
-<td>FLOOR-SLAB-1</td>
-<td>0.35</td>
-<td>3.119</td>
-<td>12.894</td>
-<td>42.73</td>
-<td>300.00</td>
-<td>180.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>BACK-1</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.408</td>
-<td>73.20</td>
-<td>30.00</td>
-<td>90.00</td>
-<td>N</td>
-</tr>
-<tr>
-<td>F3-1</td>
-<td>FLOOR-SLAB-1</td>
-<td>0.35</td>
-<td>3.119</td>
-<td>12.894</td>
-<td>96.48</td>
-<td>74.22</td>
-<td>180.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>LEFT-1</td>
-<td>WALL-1</td>
-<td>0.22</td>
-<td>0.384</td>
-<td>0.408</td>
-<td>36.48</td>
-<td>300.00</td>
-<td>90.00</td>
-<td>W</td>
-</tr>
-<tr>
-<td>F4-1</td>
-<td>FLOOR-SLAB-1</td>
-<td>0.35</td>
-<td>3.119</td>
-<td>12.894</td>
-<td>42.73</td>
-<td>120.00</td>
-<td>180.00</td>
-<td> </td>
-</tr>
-<tr>
-<td>F5-1</td>
-<td>FLOOR-SLAB-1</td>
-<td>0.35</td>
-<td>3.119</td>
-<td>12.894</td>
-<td>182.49</td>
-<td>30.00</td>
-<td>180.00</td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Fenestration
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Construction</th>
-<th>Area of One Opening [m2]</th>
-<th>Area of Openings [m2]</th>
-<th>U-Factor [W/m2-K]</th>
-<th>SHGC</th>
-<th>Visible Transmittance</th>
-<th>Shade Control</th>
-<th>Parent Surface</th>
-<th>Azimuth [deg]</th>
-<th>Cardinal Direction</th>
-</tr>
-<tr>
-<td>WF-1</td>
-<td>DBL CLR 3MM/13MM AIR</td>
-<td>16.56</td>
-<td>16.56</td>
-<td>2.720</td>
-<td>0.764</td>
-<td>0.812</td>
-<td>No</td>
-<td>FRONT-1</td>
-<td>210.00</td>
-<td>S</td>
-</tr>
-<tr>
-<td>DF-1</td>
-<td>SGL GREY 3MM</td>
-<td>5.25</td>
-<td>5.25</td>
-<td>5.894</td>
-<td>0.716</td>
-<td>0.611</td>
-<td>No</td>
-<td>FRONT-1</td>
-<td>210.00</td>
-<td>S</td>
-</tr>
-<tr>
-<td>WR-1</td>
-<td>DBL CLR 3MM/13MM AIR</td>
-<td>9.12</td>
-<td>9.12</td>
-<td>2.720</td>
-<td>0.764</td>
-<td>0.812</td>
-<td>No</td>
-<td>RIGHT-1</td>
-<td>120.00</td>
-<td>E</td>
-</tr>
-<tr>
-<td>WB-1</td>
-<td>DBL CLR 3MM/13MM AIR</td>
-<td>16.44</td>
-<td>16.44</td>
-<td>2.720</td>
-<td>0.764</td>
-<td>0.812</td>
-<td>No</td>
-<td>BACK-1</td>
-<td>30.00</td>
-<td>N</td>
-</tr>
-<tr>
-<td>DB-1</td>
-<td>SGL GREY 3MM</td>
-<td>4.41</td>
-<td>4.41</td>
-<td>5.894</td>
-<td>0.716</td>
-<td>0.611</td>
-<td>No</td>
-<td>BACK-1</td>
-<td>30.00</td>
-<td>N</td>
-</tr>
-<tr>
-<td>WL-1</td>
-<td>DBL CLR 3MM/13MM AIR</td>
-<td>9.12</td>
-<td>9.12</td>
-<td>2.720</td>
-<td>0.764</td>
-<td>0.812</td>
-<td>No</td>
-<td>LEFT-1</td>
-<td>300.00</td>
-<td>W</td>
-</tr>
-<tr>
-<td>Total or Average</td>
-<td> </td>
-<td> </td>
-<td>60.90</td>
-<td>3.22</td>
-<td>0.756</td>
-<td>0.780</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>North Total or Average</td>
-<td> </td>
-<td> </td>
-<td>20.85</td>
-<td>3.39</td>
-<td>0.754</td>
-<td>0.769</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-<tr>
-<td>Non-North Total or Average</td>
-<td> </td>
-<td> </td>
-<td>40.05</td>
-<td>3.14</td>
-<td>0.757</td>
-<td>0.785</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
-
-
-------------------------------------------------------------------------
-
-Report: **ShadingSummary**
-
-For: **Entire Facility**
-
-**Timestamp: 2009-09-17 17:30:22**
-
-Sunlit Fraction
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>March 21 9am</th>
-<th>March 21 noon</th>
-<th>March 21 3pm</th>
-<th>June 21 9am</th>
-<th>June 21 noon</th>
-<th>June 21 3pm</th>
-<th>December 21 9am</th>
-<th>December 21 noon</th>
-<th>December 21 3pm</th>
-</tr>
-<tr>
-<td>WF-1</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.26</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.30</td>
-<td>0.74</td>
-</tr>
-<tr>
-<td>DF-1</td>
-<td>0.75</td>
-<td>0.13</td>
-<td>0.59</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.35</td>
-<td>0.92</td>
-<td>0.62</td>
-<td>0.94</td>
-</tr>
-<tr>
-<td>WR-1</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>1.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>WB-1</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>DB-1</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>WL-1</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>1.00</td>
-</tr>
-</table>
-
-
-
- Window Control
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Name</th>
-<th>Type</th>
-<th>Shaded Construction</th>
-<th>Control</th>
-<th>Glare Control</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
-
-
-Report: **LightingSummary**
-
-For: **Entire Facility**
-
-**Timestamp: 2009-09-17 17:30:22**
-
-Interior Lighting
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Zone</th>
-<th>Lighting Power Density [W/m2]</th>
-<th>Zone Area [m2]</th>
-<th>Total Power [W]</th>
-<th>End Use Subcategory</th>
-<th>Schedule Name</th>
-<th>Average Hours/Week [hr]</th>
-<th>Return Air Fraction</th>
-<th>Conditioned (Y/N)</th>
-</tr>
-<tr>
-<td>SPACE1-1 LIGHTS 1</td>
-<td>SPACE1-1</td>
-<td>15.9742</td>
-<td>99.16</td>
-<td>1584.00</td>
-<td>GeneralLights</td>
-<td>LIGHTS-1</td>
-<td>0.00</td>
-<td>0.2000</td>
-<td>Y</td>
-</tr>
-<tr>
-<td>SPACE2-1 LIGHTS 1</td>
-<td>SPACE2-1</td>
-<td>16.0056</td>
-<td>42.73</td>
-<td>684.00</td>
-<td>GeneralLights</td>
-<td>LIGHTS-1</td>
-<td>0.00</td>
-<td>0.2000</td>
-<td>Y</td>
-</tr>
-<tr>
-<td>SPACE3-1 LIGHTS 1</td>
-<td>SPACE3-1</td>
-<td>16.4179</td>
-<td>96.48</td>
-<td>1584.00</td>
-<td>GeneralLights</td>
-<td>LIGHTS-1</td>
-<td>0.00</td>
-<td>0.2000</td>
-<td>Y</td>
-</tr>
-<tr>
-<td>SPACE4-1 LIGHTS 1</td>
-<td>SPACE4-1</td>
-<td>16.0056</td>
-<td>42.73</td>
-<td>684.00</td>
-<td>GeneralLights</td>
-<td>LIGHTS-1</td>
-<td>0.00</td>
-<td>0.2000</td>
-<td>Y</td>
-</tr>
-<tr>
-<td>SPACE5-1 LIGHTS 1</td>
-<td>SPACE5-1</td>
-<td>16.2420</td>
-<td>182.49</td>
-<td>2964.00</td>
-<td>GeneralLights</td>
-<td>LIGHTS-1</td>
-<td>0.00</td>
-<td>0.2000</td>
-<td>Y</td>
-</tr>
-<tr>
-<td>Interior Lighting Total</td>
-<td> </td>
-<td>16.1777</td>
-<td>463.60</td>
-<td>7500.00</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Daylighting
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Zone</th>
-<th>Daylighting Type</th>
-<th>Control Type</th>
-<th>Fraction Controlled</th>
-<th>Lighting Installed in Zone [W]</th>
-<th>Lighting Controlled [W]</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- Exterior Lighting
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Total Watts</th>
-<th>Astronomical Clock/Schedule</th>
-<th>Schedule Name</th>
-<th>Average Annual Hours/Week</th>
-</tr>
-<tr>
-<td>Exterior Lighting Total</td>
-<td>0.00</td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
-
-
-Report: **EquipmentSummary**
-
-For: **Entire Facility**
-
-**Timestamp: 2009-09-17 17:30:22**
-
-Central Plant
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Nominal Capacity [W]</th>
-<th>Nominal Efficiency [W/W]</th>
-</tr>
-<tr>
-<td>CENTRAL CHILLER</td>
-<td>Chiller:Electric</td>
-<td>25311.64</td>
-<td>3.20</td>
-</tr>
-<tr>
-<td>CENTRAL BOILER</td>
-<td>Boiler:HotWater</td>
-<td>56191.29</td>
-<td>0.80</td>
-</tr>
-</table>
-
-
-
- Cooling Coils
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Nominal Total Capacity [W]</th>
-<th>Nominal Sensible Capacity [W]</th>
-<th>Nominal Latent Capacity [W]</th>
-<th>Nominal Sensible Heat Ratio</th>
-<th>Nominal Efficiency [W/W]</th>
-</tr>
-<tr>
-<td>MAIN COOLING COIL 1</td>
-<td>Coil:Cooling:Water</td>
-<td>28159.12</td>
-<td>19476.53</td>
-<td>8682.60</td>
-<td>0.69</td>
-<td>-</td>
-</tr>
-</table>
-
-
-
- Heating Coils
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Nominal Total Capacity [W]</th>
-<th>Nominal Efficiency [W/W]</th>
-</tr>
-<tr>
-<td>SPACE1-1 ZONE COIL</td>
-<td>Coil:Heating:Water</td>
-<td>10384.85</td>
-<td>-</td>
-</tr>
-<tr>
-<td>SPACE2-1 ZONE COIL</td>
-<td>Coil:Heating:Water</td>
-<td>8470.48</td>
-<td>-</td>
-</tr>
-<tr>
-<td>SPACE3-1 ZONE COIL</td>
-<td>Coil:Heating:Water</td>
-<td>10477.88</td>
-<td>-</td>
-</tr>
-<tr>
-<td>SPACE4-1 ZONE COIL</td>
-<td>Coil:Heating:Water</td>
-<td>11334.29</td>
-<td>-</td>
-</tr>
-<tr>
-<td>SPACE5-1 ZONE COIL</td>
-<td>Coil:Heating:Water</td>
-<td>11391.33</td>
-<td>-</td>
-</tr>
-<tr>
-<td>MAIN HEATING COIL 1</td>
-<td>Coil:Heating:Water</td>
-<td>4061.83</td>
-<td>-</td>
-</tr>
-</table>
-
-
-
- Fans
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Total Efficiency [W/W]</th>
-<th>Delta Pressure [pa]</th>
-<th>Max Flow Rate [m3/s]</th>
-<th>Rated Power [W]</th>
-<th>Motor Heat In Air Fraction</th>
-<th>End Use</th>
-</tr>
-<tr>
-<td>SUPPLY FAN 1</td>
-<td>Fan:VariableVolume</td>
-<td>0.70</td>
-<td>600.00</td>
-<td>1.28</td>
-<td>1099.23</td>
-<td>1.00</td>
-<td>General</td>
-</tr>
-</table>
-
-
-
- Pumps
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Control</th>
-<th>Head [pa]</th>
-<th>Power [W]</th>
-<th>Motor Efficiency [W/W]</th>
-</tr>
-<tr>
-<td>HW CIRC PUMP</td>
-<td>Pump:VariableSpeed</td>
-<td>INTERMITTENT</td>
-<td>179352.00</td>
-<td>312.23</td>
-<td>0.90</td>
-</tr>
-<tr>
-<td>CW CIRC PUMP</td>
-<td>Pump:VariableSpeed</td>
-<td>INTERMITTENT</td>
-<td>179352.00</td>
-<td>231.95</td>
-<td>0.90</td>
-</tr>
-</table>
-
-
-
- Service Water Heating
-
-<table class="table table-striped">
-<tr>
-<th> </th>
-<th>Type</th>
-<th>Storage Volume [m3]</th>
-<th>Input [W]</th>
-<th>Thermal Efficiency [W/W]</th>
-<th>Recovery Efficiency [W/W]</th>
-<th>Energy Factor</th>
-</tr>
-<tr>
-<td>None</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-Features Related to Appendix G and LEED
----------------------------------------
-
-EnergyPlus has several built-in features to make demonstrating compliance with ASHRAE Standard 90.1 Appendix G easier. Appendix G is used in Energy and Atmosphere Credit 1 Optimize Energy Performance of the U.S. Green Building Council (USGBC) building certification system called Leadership in Energy and Environmental Design (LEED) Green Building Rating Systemâ„¢. The following sections describe the features.
-
-### Baseline Building Rotations
-
-Table G3.1 Section 5 Building Envelope of ASHRAE Standard 90.1 Appendix G requires that the baseline building be simulated facing four directions:
-
-Orientation. The baseline building performance shall be generated by simulating the building with its actual orientation and again after rotating the entire building 90, 180, and 270 degrees, then averaging the results.
-
-This provision intends to provide a baseline that is neutral to building orientation so that buildings purposely oriented to minimize energy use can realize a percent savings.
-
-**Step 1.** The first step of performing the building rotations is to include a Compliance:Building object which contains the Building Rotation for Appendix G field. The value of the field should be different for four simulations, 0, 90, 180 and 270 (see Step 2 below). This is further documented in the Input Output Reference.
-
-```idf
-Compliance:Building,
-    90;                 Building Rotation for Appendix G
-```
-
-Also make sure that the HTML summary reports will be generated by including the following:
-
-```idf
-OutputControl:Table:Style,
-  HTML;                      !- type
-
-Output:Table:SummaryReports,
-  AllSummary;                !- type
-```
-
-**Step 2.** The ParametricPreprocessor automates the creation of the four simulation input files so that only a single simulation file is needs to be created by the user. By setting the file name suffixes (which are appended to the existing file name for each simulation), setting a variable that varies for the four simulations, and setting the Building Rotation for Appendix G to this variable, the user can automatically create the four files when using EnergyPlus. The following example shows what should be included in the EnergyPlus file. The Parametric objects are described further in the Input Output Reference and the ParametricPreprocessor is described in the Auxiliary Programs documentation.
-
-```
-Parametric:FileNameSuffix,
-  Names,
-  G000,
-  G090,
-  G180,
-  G270;
-
-Parametric:SetValueForRun,
-  $appGAngle,            !- Parameter Name
-  0.0,                   !- Value 1
-  90.0,                  !- Value 2
-  180.0,                 !- Value 3
-  270.0;                 !- Value 4
-
-Compliance:Building,
-    =$appGAngle;        !- Building Rotation for Appendix G {deg}
-
-OutputControl:Table:Style,
-  HTML;                      !- type
-
-Output:Table:SummaryReports,
-  AllSummary;                !- type
-```
-
-**Step 3.** Run the simulation using EP-Launch. Using the “Single Input File� tab of EP-Launch select the input that contains the Compliance:Building, Parametric:FileNameSuffix, Parametric:SetValueForRun objects as shown above in Step 2 as well as the weather file. In EP-Launch, make sure under VIEW .. OPTIONS .. MISCELLANEOUS that the RUN PARAMETRICPREPROCESSOR option is checked.
-
-**Step 4**. Review the results and revise the model inputs as needed. You can view the results of the simulation by using the EP-Launch and the History tab. At the bottom of the history list, four simulations that use the G000, G090, G180 and G270 file name suffixes should appear and the result files associated with each can be selected and opened.
-
-**Step 5.** Use the AppGPostProcess to average results across the simulations. In EP-Launch under the UTILITIES tab, select AppGPostProcess utility and select one of the HTML files resulting from the multiple simulation runs (e.g., &lt;filename&gt;-G000.html). This will open all four files and generate a new output file with the file suffix GAVG for the HTML and other results files that can be opened on that tab.
-
-### Completing LEED Forms from Tabular Reports
-
-The U.S. Green Building Council building certification system called Leadership in Energy and Environmental Design (LEED) Green Building Rating System™ includes Energy and Atmosphere Credit 1 Optimize Energy Performance. Credit 1 includes an option that requires a series of building energy simulations that follow the procedures of ASHRAE Standard 90.1 Appendix G Performance Rating Method. The  LEED Summary report provides many of the simulation results required for the forms. The report can be produced by specifying LEEDSummary in Output:Table:SummaryReports which is also part of the AllSummary option.
-
-
-
-Report: **LEED Summary**
-
-For: **Entire Facility**
-
-Timestamp: **2013-03-01 15:24:37**
-
-**Sec1.1A-General Information**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Data</th>
-</tr>
-<tr>
-<td>Heating Degree Days</td>
-<td>1748</td>
-</tr>
-<tr>
-<td>Cooling Degree Days</td>
-<td>506</td>
-</tr>
-<tr>
-<td>Climate Zone</td>
-<td>5A</td>
-</tr>
-<tr>
-<td>Weather File</td>
-<td>Chicago Ohare Intl Ap IL USA TMY3 WMO#=725300</td>
-</tr>
-<tr>
-<td>HDD and CDD data source</td>
-<td>Weather File Stat</td>
-</tr>
-<tr>
-<td>Total gross floor area [m2]</td>
-<td>927.20</td>
-</tr>
-<tr>
-<td>Principal Heating Source</td>
-<td>Natural Gas</td>
-</tr>
-</table>
-
-
-
- **EAp2-1. Space Usage Type**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Space Area [m2]</th>
-<th>Regularly Occupied Area [m2]</th>
-<th>Unconditioned Area [m2]</th>
-<th>Typical Hours/Week in Operation [hr/wk]</th>
-</tr>
-<tr>
-<td>SPACE1-1</td>
-<td>99.16</td>
-<td>99.16</td>
-<td>0.00</td>
-<td>55.06</td>
-</tr>
-<tr>
-<td>SPACE2-1</td>
-<td>42.73</td>
-<td>42.73</td>
-<td>0.00</td>
-<td>55.06</td>
-</tr>
-<tr>
-<td>SPACE3-1</td>
-<td>96.48</td>
-<td>96.48</td>
-<td>0.00</td>
-<td>55.06</td>
-</tr>
-<tr>
-<td>SPACE4-1</td>
-<td>42.73</td>
-<td>42.73</td>
-<td>0.00</td>
-<td>55.06</td>
-</tr>
-<tr>
-<td>SPACE5-1</td>
-<td>182.49</td>
-<td>182.49</td>
-<td>0.00</td>
-<td>55.06</td>
-</tr>
-<tr>
-<td>PLENUM-1</td>
-<td>463.60</td>
-<td>463.60</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Totals</td>
-<td>927.20</td>
-<td>927.20</td>
-<td>0.00</td>
-<td> </td>
-</tr>
-</table>
-
-
-
- **EAp2-2. Advisory Messages**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Data</th>
-</tr>
-<tr>
-<td>Number of hours heating loads not met</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Number of hours cooling loads not met</td>
-<td>10.75</td>
-</tr>
-<tr>
-<td>Number of hours not met</td>
-<td>10.75</td>
-</tr>
-</table>
-
-
-
- **EAp2-3. Energy Type Summary**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Utility Rate</th>
-<th>Virtual Rate [$/unit energy]</th>
-<th>Units of Energy</th>
-<th>Units of Demand</th>
-</tr>
-<tr>
-<td>Electricity</td>
-<td>EXAMPLEA EXAMPLEI-SELL</td>
-<td>0.055</td>
-<td>kWh</td>
-<td>kW</td>
-</tr>
-<tr>
-<td>Natural Gas</td>
-<td>EXAMPLEA-GAS</td>
-<td>0.569</td>
-<td>Therm</td>
-<td>Therm/Hr</td>
-</tr>
-<tr>
-<td>Other</td>
-<td> </td>
-<td> </td>
-<td> </td>
-<td> </td>
-</tr>
-</table>
-
-
-
- **EAp2-4/5. Performance Rating Method Compliance**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Electric Energy Use [GJ]</th>
-<th>Electric Demand [W]</th>
-<th>Natural Gas Energy Use [GJ]</th>
-<th>Natural Gas Demand [W]</th>
-<th>Other Energy Use [GJ]</th>
-<th>Other Demand [W]</th>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>81.24</td>
-<td>7125.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Exterior Lighting</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Space Heating</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>103.92</td>
-<td>62499.99</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Space Cooling</td>
-<td>17.63</td>
-<td>9523.66</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Pumps</td>
-<td>1.54</td>
-<td>319.57</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Heat Rejection</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans-Interior</td>
-<td>7.01</td>
-<td>609.44</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Fans-Parking Garage</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Service Water Heating</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Receptacle Equipment</td>
-<td>47.70</td>
-<td>4500.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Interior Lighting (process)</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Refrigeration Equipment</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Cooking</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Industrial Process</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Elevators and Escalators</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total Line</td>
-<td>155.12</td>
-<td> </td>
-<td>274.01</td>
-<td> </td>
-<td>0.00</td>
-<td> </td>
-</tr>
-</table>
-
-
-
- **EAp2-6. Energy Use Summary**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Process Subtotal [GJ]</th>
-<th>Total Energy Use [GJ]</th>
-</tr>
-<tr>
-<td>Electricity</td>
-<td>47.70</td>
-<td>155.12</td>
-</tr>
-<tr>
-<td>Natural Gas</td>
-<td>0.00</td>
-<td>274.01</td>
-</tr>
-<tr>
-<td>Other</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>47.70</td>
-<td>429.13</td>
-</tr>
-</table>
-
-
-
- **EAp2-7. Energy Cost Summary**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Process Subtotal [$]</th>
-<th>Total Energy Cost [$]</th>
-</tr>
-<tr>
-<td>Electricity</td>
-<td>552.55</td>
-<td>1796.99</td>
-</tr>
-<tr>
-<td>Natural Gas</td>
-<td>0.00</td>
-<td>1478.58</td>
-</tr>
-<tr>
-<td>Other</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Total</td>
-<td>552.55</td>
-<td>3275.57</td>
-</tr>
-</table>
-
-*Process energy cost based on ratio of process to total energy.*
-
- **L-1. Renewable Energy Source Summary**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Rated Capacity [kW]</th>
-<th>Annual Energy Generated [GJ]</th>
-</tr>
-<tr>
-<td>Photovoltaic</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Wind</td>
-<td>0.00</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
- **EAp2-17a. Energy Use Intensity - Electricity**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Electricty [MJ/m2]</th>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>87.62</td>
-</tr>
-<tr>
-<td>Space Heating</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Space Cooling</td>
-<td>19.02</td>
-</tr>
-<tr>
-<td>Fans-Interior</td>
-<td>7.56</td>
-</tr>
-<tr>
-<td>Service Water Heating</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Receptacle Equipment</td>
-<td>51.44</td>
-</tr>
-<tr>
-<td>Miscellaneous</td>
-<td>1.66</td>
-</tr>
-<tr>
-<td>Subtotal</td>
-<td>167.30</td>
-</tr>
-</table>
-
-
-
- **EAp2-17b. Energy Use Intensity - Natural Gas**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Natural Gas [MJ/m2]</th>
-</tr>
-<tr>
-<td>Space Heating</td>
-<td>112.08</td>
-</tr>
-<tr>
-<td>Service Water Heating</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Miscellaneous</td>
-<td>183.45</td>
-</tr>
-<tr>
-<td>Subtotal</td>
-<td>295.53</td>
-</tr>
-</table>
-
-
-
- **EAp2-17c. Energy Use Intensity - Other**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Other [MJ/m2]</th>
-</tr>
-<tr>
-<td>Miscellaneous</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Subtotal</td>
-<td>0.00</td>
-</tr>
-</table>
-
-
-
- **EAp2-18. End Use Percentage**
-
-<table class="table table-striped">
-<tr>
-<th></th>
-<th>Percent [%]</th>
-</tr>
-<tr>
-<td>Interior Lighting</td>
-<td>18.93</td>
-</tr>
-<tr>
-<td>Space Heating</td>
-<td>24.22</td>
-</tr>
-<tr>
-<td>Space Cooling</td>
-<td>4.11</td>
-</tr>
-<tr>
-<td>Fans-Interior</td>
-<td>1.63</td>
-</tr>
-<tr>
-<td>Service Water Heating</td>
-<td>0.00</td>
-</tr>
-<tr>
-<td>Receptacle Equipment</td>
-<td>11.11</td>
-</tr>
-<tr>
-<td>Miscellaneous</td>
-<td>39.99</td>
-</tr>
-</table>
-
-
-
-#### LEED Form Section 1.4 – Comparison of Proposed Design Versus Baseline Design
-
-Unlike other portions of the LEED forms, Section 1.4 Comparison of Proposed Design Versus Baseline Design is less structured with many possible “Model Input Parameters� to match with the “Proposed Design Input� and “Baseline Design Input�.
-
-*1. Exterior wall, underground wall, roof, floor, and slab assemblies including framing type, assembly R-values, assembly U-factors, and roof reflectivity when modeling cool roofs. (Refer to ASHRAE 90.1 Appendix A)*
-
-Use the values from the Envelope Summary table, Opaque Exterior subtable for Construction, Reflectance, U-Factor with Film, and U-Factor no Film.
-
-*2. Fenestration types, assembly U-factors (including the impact of the frame on the assembly, SHGCs, and visual light transmittances, overall window-to-gross wall ratio, fixed shading devices, and automated movable shading devices*
-
-Use the values from Input Verification and Results Summary table, Window-Wall Ratio table Window-Wall Ratio percentage as well as Skylight-Roof Ratio table. Also use the values from the Envelope Summary table, Fenestration subtable for Construction, Area of Openings, U-Factor, SHGC, Visible Transmittance, and Shade Control. For shading use the Shading Summary report including Sunlit Fraction and Window Control.
-
-*3. Interior lighting power densities, exterior lighting power, process lighting power, and lighting controls modeled for credit.*
-
-Use the values from the Lighting Summary report for Interior Lighting, Daylighting and Exterior Lighting including Lighting Power Density, Schedule Name, Average Hours/Week, Daylighting Type, Control Type, Fraction Controlled, Lighting Installed in Zone, Lighting Controlled.
-
-*4. Receptacle equipment, elevators or escalators, refrigeration equipment and other process loads.*
-
-Use the values from Input Verification and Results Summary table, Zone Summary subtable for Plug and Process.
-
-*5. HVAC system information including types and efficiencies, exhaust heat recovery, pump power and controls, and other pertinent system information. (Include the ASRHAE 90.1-2004 Table G3.1.1B Baseline System Number)*
-
-Use the Equipment Summary report, Central Plant subtable for Type, Nominal Capacity and Nominal Efficiency; Cooling Coils subtable for Nominal Total Capacity and Nominal Efficiency; Heating Coils subtable for Type, Nominal Total Capacity and Nominal Efficiency; Fans subtable for Type, Total Efficiency, Delta Pressure, Max Flow Rate, Rated Power, Motor Heat in Air Fraction; Pumps subtable for Type, Control, Head, Power and Motor Efficiency. Use the System Summary report, Economizer subtable for High Limit Shutoff Control and Minimum Outdoor Air; the Demand Controlled Ventilation using Controller:MechanicalVentilation subtable.
-
-*6. Domestic hot water system type, efficiency and storage tank volume.*
-
-Use the Equipment Summary report, Service Water Heating subtable for Type, Storage Volume, Input, Thermal Efficiency, Recovery Efficiency, and Energy Factor.
-
-*7. General schedule information.*
-
-Use the Lighting Summary report, Interior Lighting subtable Schedule Name and Average Hours/Week; Exterior Lighting subtable Schedule Name and Average Hours/Week. Use the System Summary report, Demand Controlled Ventilation using Controller:MechanicalVentilation subtable for the Air Distribution Effectiveness Schedule.
-
-Features Related to California Title 24 Compliance
---------------------------------------------------
-
-EnergyPlus has a reporting feature that is useful for obtaining Time Dependant Valuation (TDV) of source energy use for the entire facility being simulated. Hourly variations of fuel factors can be specified through the 'FuelFactors' input object and will be used to calculate TDV based source energy consumption broken down by end uses. The Source Energy End Use Components Summary report above provides these TDV based values. The source energy consumption is also reported based on area normalized metrics. Refer to 'Fuel Factors' and 'Output:Table:SummaryReports' in the Input-Output Reference manual for more details.
-
-Also included is the California\_Title\_24-2008.idf dataset (described briefly in the Output Details document).
-
-
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-# EnergyPlus Documentation
-
-This site provides an interactive view of the EnergyPlus documentation.  The headers at the top provide quick access to each documentation, plus sections are broken out for the larger docs.  A search feature is being implemented and should be available soon.
-
-For convenience, here are links to the core documentation:
-
-* Intro & Application
-    * [Getting Started](GettingStarted/GettingStarted.md)
-    * [Tips and Tricks for EnergyPlus](Tips_and_Tricks_Using_EnergyPlus/Tips_and_Tricks_Using_EnergyPlus.md)
-    * [EMS Application Guide](EMS_Application_Guide/EMS_Application_Guide.md)
-    * [External Interface Application Guide](ExternalInterfaces_Application_Guide/ExternalInterfaces_Application_Guide.md)
-    * [Plant Application Guide](PlantApplicationGuide/PlantApplicationGuide.md)
-* [Input Output Reference](InputOutputReference/01a-InputOutputReference.md)
-* [Engineering Reference](EngineeringReference/01-Overview.md)
-* [Engineering Reference: Encyclopedic Guide to Simulation Models](EngineeringReference/13-EncyclopaedicRefs.md)
-* Developer Guides
-    * [Interface Developer](InterfaceDeveloper/InterfaceDeveloper.md)
-    * [Module Developer](ModuleDeveloper/ModuleDeveloper.md)
-* Other
-    * [Acknowledgements](Acknowledgements/Acknowledgements.md)
-    * [Auxiliary Programs](AuxiliaryPrograms/AuxiliaryPrograms.md)
-    * [Output Details and Examples](OutputDetailsAndExamples/OutputDetailsAndExamples.md)
-    * [Using E+ for Compliance](Using_EnergyPlus_for_Compliance/Using_EnergyPlus_for_Compliance.md)
diff --git a/doc/src/docs/index_htmlpdf.md b/doc/src/docs/index_htmlpdf.md
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-# EnergyPlus Documentation
-
-This site provides an interactive view of the EnergyPlus documentation.  The headers at the top provide quick access to each documentation, plus sections are broken out for the larger docs.  A search feature is being implemented and should be available soon.
-
-For convenience, here are links to the core documentation:
-
-* Intro & Application
-    * [Getting Started](GettingStarted/GettingStarted.md)
-    * [Tips and Tricks for EnergyPlus](Tips_and_Tricks_Using_EnergyPlus/Tips_and_Tricks_Using_EnergyPlus.md)
-    * [EMS Application Guide](EMS_Application_Guide/EMS_Application_Guide.md)
-    * [External Interface Application Guide](ExternalInterfaces_Application_Guide/ExternalInterfaces_Application_Guide.md)
-    * [Plant Application Guide](PlantApplicationGuide/PlantApplicationGuide.md)
-* User Guides
-    * [Input Output Reference](InputOutputReference/IORef.md)
-    * [Engineering Reference](EngineeringReference/EngRef.md)
-* Developer Guides
-    * [Interface Developer](InterfaceDeveloper/InterfaceDeveloper.md)
-    * [Module Developer](ModuleDeveloper/ModuleDeveloper.md)
-* Other
-    * [Acknowledgements](Acknowledgements/Acknowledgements.md)
-    * [Auxiliary Programs](AuxiliaryPrograms/AuxiliaryPrograms.md)
-    * [Output Details and Examples](OutputDetailsAndExamples/OutputDetailsAndExamples.md)
-    * [Using E+ for Compliance](Using_EnergyPlus_for_Compliance/Using_EnergyPlus_for_Compliance.md)
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-          li {list-style: none;}
-          ul {
-            font-size: 20px;
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-          ul {padding-left: 0em;}
-          ul ul {padding-left: 1em;}
-          a {text-decoration:none; color: black;}
-        </style>
-      </head>
-      <body>
-        <h1>Table of Contents</h1>
-        <ul><xsl:apply-templates select="outline:item/outline:item"/></ul>
-      </body>
-    </html>
-  </xsl:template>
-  <xsl:template match="outline:outline/outline:item/outline:item|outline:outline/outline:item/outline:item/outline:item|outline:outline/outline:item/outline:item/outline:item/outline:item">
-    <li>
-      <xsl:if test="@title!=''">
-        <div>
-          <a>
-            <xsl:if test="@link">
-              <xsl:attribute name="href"><xsl:value-of select="@link"/></xsl:attribute>
-            </xsl:if>
-            <xsl:if test="@backLink">
-              <xsl:attribute name="name"><xsl:value-of select="@backLink"/></xsl:attribute>
-            </xsl:if>
-            <xsl:value-of select="@title" /> 
-          </a>
-          <span> <xsl:value-of select="@page" /> </span>
-        </div>
-      </xsl:if>
-      <ul>
-        <xsl:comment>added to prevent self-closing tags in QtXmlPatterns</xsl:comment>
-        <xsl:apply-templates select="outline:item"/>
-      </ul>
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diff --git a/doc/src/mkdocs_html.yml b/doc/src/mkdocs_html.yml
deleted file mode 100644
index 1b952cd553a..00000000000
--- a/doc/src/mkdocs_html.yml
+++ /dev/null
@@ -1,61 +0,0 @@
-site_name: EnergyPlus Documentation
-site_favicon: favicon.ico
-site_logo: 'EP_32x32.png'
-site_dir: site_html
-repo_url: https://github.com/NREL/EnergyPlus
-
-pages:
-- [index.md, "Home"]
-- [GettingStarted/GettingStarted.md, "Intro & Application", "Getting Started"]
-- [Tips_and_Tricks_Using_EnergyPlus/Tips_and_Tricks_Using_EnergyPlus.md, "Intro & Application", "Tips and Tricks for EnergyPlus"]
-- [EMS_Application_Guide/EMS_Application_Guide.md, "Intro & Application", "EMS Applications"]
-- [ExternalInterfaces_Application_Guide/ExternalInterfaces_Application_Guide.md, "Intro & Application", "External Interface Applications"]
-- [PlantApplicationGuide/PlantApplicationGuide.md, "Intro & Application", "Plant Applications"]
-- [InputOutputReference/01a-InputOutputReference.md, "Input/Output Reference", "Input Output Reference - Vol 1"]
-- [InputOutputReference/01b-InputOutputReference.md, "Input/Output Reference", "Input Output Reference - Vol 2"]
-- [InputOutputReference/01c-InputOutputReference.md, "Input/Output Reference", "Input Output Reference - Vol 3"]
-- [InputOutputReference/01d-InputOutputReference.md, "Input/Output Reference", "Input Output Reference - Vol 4"]
-- [InputOutputReference/02-HVACTemplates.md, "Input/Output Reference", "HVACTemplates"]
-- [InputOutputReference/03-Economics.md, "Input/Output Reference", "Economics"]
-- [InputOutputReference/04-Parametrics.md, "Input/Output Reference", "Parametrics"]
-- [InputOutputReference/05-InputForOutput.md, "Input/Output Reference", "Input for Output"]
-- [InputOutputReference/06-StandardOutputReports.md, "Input/Output Reference", "Standard Output Reports"]
-- [InputOutputReference/07-WeatherData.md, "Input/Output Reference", "Weather Data"]
-- [InputOutputReference/08-RunningEnergyPlus.md, "Input/Output Reference", "Running EnergyPlus"]
-- [InputOutputReference/09-Appendix.md, "Input/Output Reference", "Appendices"]
-- [EngineeringReference/01-Overview.md, "Engineering Reference", "Overview"]
-- [EngineeringReference/02-IntegratedSolution.md, "Engineering Reference", "Integrated Solution Manager"]
-- [EngineeringReference/03-SurfaceHeatBalance.md, "Engineering Reference", "Surface Heat Balance Manager"]
-- [EngineeringReference/04-AdvancedSurface.md, "Engineering Reference", "Advanced Surface Concepts"]
-- [EngineeringReference/05-Climate.md, "Engineering Reference", "Climate, Sky and Solar Calculation"]
-- [EngineeringReference/06-SolarRadiation.md, "Engineering Reference", "Solar Reflection"]
-- [EngineeringReference/07-Daylighting.md, "Engineering Reference", "Daylighting and Window Calcs"]
-- [EngineeringReference/08-AirHeatBalance.md, "Engineering Reference", "Air Heat Balance Manager"]
-- [EngineeringReference/09-BuildingSystemSimulation.md, "Engineering Reference", "Building System Simulation Manager"]
-- [EngineeringReference/10-Sizing.md, "Engineering Reference", "Sizing and Design Data"]
-- [EngineeringReference/OperationalFaults.md, "Engineering Reference", "Operational Faults"]
-- [EngineeringReference/11-DemandLimiting.md, "Engineering Reference", "Demand Limiting"]
-- [EngineeringReference/12-AlternativeModeling.md, "Engineering Reference", "Alternative Modeling Processes"]
-- [EngineeringReference/13-EncyclopaedicRefs.md, "Engineering Reference", "Encyclopedic Reference of Simulation Models"]
-- [EngineeringReference/13a-EncyclopaedicRefs.md, "Engineering Reference", " - - - - Encyclopedia Volume 1"]
-- [EngineeringReference/13b-EncyclopaedicRefs.md, "Engineering Reference", " - - - - Encyclopedia Volume 2"]
-- [EngineeringReference/13c-EncyclopaedicRefs.md, "Engineering Reference", " - - - - Encyclopedia Volume 3"]
-- [EngineeringReference/13d-EncyclopaedicRefs.md, "Engineering Reference", " - - - - Encyclopedia Volume 4"]
-- [EngineeringReference/13e-EncyclopaedicRefs.md, "Engineering Reference", " - - - - Encyclopedia Volume 5"]
-- [EngineeringReference/13f-EncyclopaedicRefs.md, "Engineering Reference", " - - - - Encyclopedia Volume 6"]
-- [EngineeringReference/14-OnSiteGeneration.md, "Engineering Reference", "On-SIte Generation"]
-- [EngineeringReference/15-PerformanceCurves.md, "Engineering Reference", "Performance Curves and Lookup Tables"]
-- [EngineeringReference/16-Economics.md, "Engineering Reference", "Economic Calculations"]
-- [EngineeringReference/17-SpecialModulesReporting.md, "Engineering Reference", "Special Modules and Reporting"]
-- [InterfaceDeveloper/InterfaceDeveloper.md, "Developer Guides", "Interface Developer"]
-- [ModuleDeveloper/ModuleDeveloper.md, "Developer Guides", "Module Developer"]
-- [Acknowledgements/Acknowledgements.md, "Other", "Acknowledgements"]
-- [AuxiliaryPrograms/AuxiliaryPrograms.md, "Other", "Auxiliary Programs"]
-- [OutputDetailsAndExamples/OutputDetailsAndExamples.md, "Other", "Output Details and Examples"]
-- [Using_EnergyPlus_for_Compliance/Using_EnergyPlus_for_Compliance.md, "Other", "Using E+ for Compliance"]
-
-theme: simplex
-theme_dir: 'bootstrap_nrel_html'
-
-
-
diff --git a/doc/src/mkdocs_htmlpdf.yml b/doc/src/mkdocs_htmlpdf.yml
deleted file mode 100644
index 0271a93d5ec..00000000000
--- a/doc/src/mkdocs_htmlpdf.yml
+++ /dev/null
@@ -1,26 +0,0 @@
-site_name: EnergyPlus Documentation
-site_favicon: favicon.ico
-site_logo: 'EP_32x32.png'
-site_dir: site_htmlpdf
-repo_url: https://github.com/NREL/EnergyPlus
-
-pages:
-- [GettingStarted/GettingStarted.md, "Intro & Application", "Getting Started"]
-- [Tips_and_Tricks_Using_EnergyPlus/Tips_and_Tricks_Using_EnergyPlus.md, "Intro & Application", "Tips and Tricks for EnergyPlus"]
-- [EMS_Application_Guide/EMS_Application_Guide.md, "Intro & Application", "EMS Applications"]
-- [ExternalInterfaces_Application_Guide/ExternalInterfaces_Application_Guide.md, "Intro & Application", "External Interface Applications"]
-- [PlantApplicationGuide/PlantApplicationGuide.md, "Intro & Application", "Plant Applications"]
-- [InputOutputReference/IORef.md, "Input/Output Reference", "Input Output Reference"]
-- [EngineeringReference/EngRef.md, "Engineering Reference", "Engineering Reference"]
-- [InterfaceDeveloper/InterfaceDeveloper.md, "Developer Guides", "Interface Developer"]
-- [ModuleDeveloper/ModuleDeveloper.md, "Developer Guides", "Module Developer"]
-- [Acknowledgements/Acknowledgements.md, "Other", "Acknowledgements"]
-- [AuxiliaryPrograms/AuxiliaryPrograms.md, "Other", "Auxiliary Programs"]
-- [OutputDetailsAndExamples/OutputDetailsAndExamples.md, "Other", "Output Details and Examples"]
-- [Using_EnergyPlus_for_Compliance/Using_EnergyPlus_for_Compliance.md, "Other", "Using E+ for Compliance"]
-
-theme: simplex
-theme_dir: 'bootstrap_nrel_htmlpdf'
-
-
-
diff --git a/doc/tips-and-tricks-using-energyplus/CMakeLists.txt b/doc/tips-and-tricks-using-energyplus/CMakeLists.txt
new file mode 100644
index 00000000000..a00749a89eb
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/CMakeLists.txt
@@ -0,0 +1,116 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/title.tex
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/tips-and-tricks-using-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/tips-tricks-for-using-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/introduction-support.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/introduction-support/organization.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/introduction-support/energyplus-support.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/general.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/general/what-energyplus-is.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/general/what-energyplus-isn-t.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/general/getting-started.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/general/comparing-energyplus-to-other-programs.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/datasets.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/datasets/datasets-aka-libraries.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/datasets/locations-designdays.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/design-day-creation.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/epw-weather-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/meteonorm-weather-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/weather-data-for-simulations.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/weather-file-sources.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/measuring-solar-data.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/input.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/input/creating-files-for-energyplus.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/input/converting-older-version-energyplus-files.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/input/using-macros-and-editing-inputs-in-idf-editor.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/input/getting-data-from-window-program.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/building-surface-dimensions-inside-outside.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/describing-roof-overhangs.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/solar-reflection-from-shading-surfaces.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/air-wall-open-air-connection-between-zones.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/daylight-modeling.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/rain-flag.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/interzone-exterior-convection.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/modeling-reflective-radiant-barriers.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/cavity-algorithm-model.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/using-multipliers-zone-and-or-window.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/using-osc-other-side-coefficients-to-create.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/natural-and-mechanical-ventilation.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/natural-and-mechanical-ventilation/airflownetwork-and-earthtube.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-sizing-tips.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/variable-refrigerant-flow-air-conditioner.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/modeling-desiccant-dehumidifiers.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/boiler-control-schedule.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/difference-between-eir-and-reformulated-eir.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/using-well-water.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/plant-load-profile.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-system-turn-off.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/fan-types.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/use-of-set-point-managers.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-availability-schedules.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-system-types.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/separating-ventilation-loads-v-zone-loads.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/system-not-cooling.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/output.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/output/output-does-not-match-epw-values.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/output/schedules-off-by-1-hour.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/output/reporting-options.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/output/output-variables-in-idf-editor.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/output/output-variable-definition.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/output/advanced-output-variable-reporting.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/output/use-of-comma-and-point-in-numeric-output.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/utilities.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/documentation-and-guides.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/errors-and-warnings.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/errors-and-warnings/max-iterations-exceeded.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/error-messages-details.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/error-messages-details/standard-error-message-format.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-for-preprocessors.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-for-the-input.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-from-module-getinput.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-during-sizing.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/error-messages-details/recurring-errors.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/error-messages-details/summaries-at-end-of-simulation.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/error-messages-details/psychrometric-errors.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/error-messages-details/error-summary.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/validation-and-testing.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/reduce-energyplus-run-time.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/run-energyplus-in-parallel.tex
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/running-energyplus-on-windows-vista-and.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/media/image001.jpg
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/media/image002.png
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/media/image003.png
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/media/image004.png
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/media/image005.png
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/media/image006.jpg
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/media/image007.png
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/media/image008.png
+  ${CMAKE_SOURCE_DIR}/doc/tips-and-tricks-using-energyplus/media/image009.png
+) 
+
+SET( SOURCE_FILENAME "tips-and-tricks-using-energyplus" )
+SET( OUTPUT_FILENAME "TipsAndTricksUsingEnergyPlus" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/ep.gif b/doc/tips-and-tricks-using-energyplus/media/ep.gif
similarity index 100%
rename from doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/ep.gif
rename to doc/tips-and-tricks-using-energyplus/media/ep.gif
diff --git a/doc/tips-and-tricks-using-energyplus/media/ep.png b/doc/tips-and-tricks-using-energyplus/media/ep.png
new file mode 100644
index 00000000000..a808760c870
Binary files /dev/null and b/doc/tips-and-tricks-using-energyplus/media/ep.png differ
diff --git a/doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/image001.jpg b/doc/tips-and-tricks-using-energyplus/media/image001.jpg
similarity index 100%
rename from doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/image001.jpg
rename to doc/tips-and-tricks-using-energyplus/media/image001.jpg
diff --git a/doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/image002.png b/doc/tips-and-tricks-using-energyplus/media/image002.png
similarity index 100%
rename from doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/image002.png
rename to doc/tips-and-tricks-using-energyplus/media/image002.png
diff --git a/doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/image003.png b/doc/tips-and-tricks-using-energyplus/media/image003.png
similarity index 100%
rename from doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/image003.png
rename to doc/tips-and-tricks-using-energyplus/media/image003.png
diff --git a/doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/image004.png b/doc/tips-and-tricks-using-energyplus/media/image004.png
similarity index 100%
rename from doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/image004.png
rename to doc/tips-and-tricks-using-energyplus/media/image004.png
diff --git a/doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/image005.png b/doc/tips-and-tricks-using-energyplus/media/image005.png
similarity index 100%
rename from doc/src/docs/Tips_and_Tricks_Using_EnergyPlus/media/image005.png
rename to doc/tips-and-tricks-using-energyplus/media/image005.png
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diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model.tex
new file mode 100644
index 00000000000..da4fc56be95
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model.tex
@@ -0,0 +1 @@
+\chapter{Building Geometry, Shading \& Zone Model}\label{building-geometry-shading-zone-model}
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/air-wall-open-air-connection-between-zones.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/air-wall-open-air-connection-between-zones.tex
new file mode 100644
index 00000000000..a4e5205f134
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/air-wall-open-air-connection-between-zones.tex
@@ -0,0 +1,13 @@
+\section{Air wall, Open air connection between zones}\label{air-wall-open-air-connection-between-zones}
+
+It is extremely difficult to model the interactions between thermal zones which are connected by a large opening. If the zones are controlled to the same conditions, then there is little to be gained by making them interact, so you could neglect any connections between the zones. In fact, if this is the case, you might consider combining the spaces into a single thermal zone. If you expect the zones to have significantly different temperatures and/or humidities, then use one of the following options. If they are modeled as separate zones, EnergyPlus models only what is explicitly described in the input file, so simply leaving a void (no surfaces) between two zones will accomplish nothing - the two zones will not be connected. The main interactions which occur across the dividing line between two zones which are fully open to each other are:
+
+1)~~~Convection or airflow, which will transfer both sensible heat and moisture. Some modelers use MIXING (one-way flow) or CROSS MIXING (two-way flow) to move air between the zones, but the user must specify airflow rates and schedules for this flow, and it cannot be automatically linked to HVAC system operation. Other modelers use AirFlowNetwork with large vertical openings between the zones as well as other openings and cracks in the exterior envelope to provide the driving forces. It can also be connected with the HVAC system (for limited system types). This requires a much higher level of detailed input and should be used only if the detailed specification data is available. If the two zones are controlled to similar conditions, this effect could be safely neglected.
+
+2)~~~Solar gains and daylighting. The only way to pass solar and daylight from one zone to the next is through a window or glass door described as a subsurface on an interzone wall surface. Note that all solar is diffuse after passing through an interior window.
+
+3)~~~Radiant (long-wave thermal) transfer. There is currently no direct radiant exchange between surfaces in different thermal zones. Windows in EnergyPlus are opaque to direct radiant exchange, so an interzone window will not behave any differently than an opaque interzone surface for this aspect. However, a large interzone surface (opaque or window) would result in some indirect radiant exchange since the interzone surface will exchange directly with surfaces in zone A and in zone B. The surface thermal resistance should be low in order to most closely approximate this effect.
+
+4)~~~Conduction. If an interzone surface is placed between the two zones, it will conduct sensible heat between the two zones. Using a low thermal resistance helps to move radiant exchange between the zones.
+
+5)~~~~Visible and thermal radiant output from internal gains. These gains will not cross zone boundaries. But again, they will impact any interzone surfaces, so some of the energy may move across to the next zone."
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/building-surface-dimensions-inside-outside.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/building-surface-dimensions-inside-outside.tex
new file mode 100644
index 00000000000..3f8012148fb
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/building-surface-dimensions-inside-outside.tex
@@ -0,0 +1,3 @@
+\section{Building Surface Dimensions -- Inside, Outside or Centerline}\label{building-surface-dimensions-inside-outside-or-centerline}
+
+When describing the geometry of building surfaces in EnergyPlus, all surfaces are a thin plane without any thickness. The thickness property of the materials which are assigned to the building surface are only used for heat conduction and thermal mass calculations. Because EnegyPlus geometry is represented with a thin plane, which actual dimension is the proper one to use: inside, outside, or centerline dimensions. For most buildings, the difference is small, and the user may use whatever dimensions are most convenient. A suggested approach is to use outside dimensions for exterior surfaces, and centerline dimensions for interior surfaces. This produces fully connected geometry with an appropriate amount of floor area, zone volume, and thermal mass. If desired, zone volume and floor area may be overridden by entering values in the Zone object. For buildings with very thick walls, such as centuries-old masonry buildings, it is recommended that centerline dimensions be used for all surfaces (exterior and interior) so that the model will have the correct amount of thermal mass.
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/cavity-algorithm-model.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/cavity-algorithm-model.tex
new file mode 100644
index 00000000000..721f59ecc8e
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/cavity-algorithm-model.tex
@@ -0,0 +1,5 @@
+\section{Cavity Algorithm Model}\label{cavity-algorithm-model}
+
+\emph{Reading the documentation, I'm wondering if the Cavity algorithm is usable for other double facade types or only Trombe wall?~ In other words, does Cavity implicitly presume that the inner wall is highly solar absorbent and so generate specific convection?}
+
+The Trombe wall convection algorithm is applicable to just about any vertical cavity with a high aspect ratio and relatively narrow width. I'm not sure if a double facade cavity would meet the aspect ratio requirement. But I do know the Trombe wall algorithm is not picky about whether the inner wall is highly absorbant, or about any particular properties of the walls. Actually the same basic algorithm is used by the window model to calculate the convection between the two panes of a window. The full reference is ISO 15099.
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/daylight-modeling.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/daylight-modeling.tex
new file mode 100644
index 00000000000..7699c1ce2a4
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/daylight-modeling.tex
@@ -0,0 +1,5 @@
+\section{Daylight Modeling}\label{daylight-modeling}
+
+\emph{Why isn't my lighting energy being reduced with a daylighting system?}
+
+In order to see changes in the lighting electric power consumption due to daylighting, the Fraction Replaceable in the \textbf{Lights} input object must be set to 1.0. This is documented in the I/O reference, and also a warning is generated in the ERR file.
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/describing-roof-overhangs.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/describing-roof-overhangs.tex
new file mode 100644
index 00000000000..21dfca708bb
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/describing-roof-overhangs.tex
@@ -0,0 +1,27 @@
+\section{Describing Roof Overhangs}\label{describing-roof-overhangs}
+
+Building heat transfer surfaces, such as roofs and walls, only cast shadows in a hemisphere in the direction of the outward facing normal (see Figure~\ref{fig:building-heat-transfer-surfaces-cast-shadows}). Because roof surfaces generally face upward, a roof surface which extends beyond the walls of the building will not cast shadows on the walls below it (see Figure~\ref{fig:extended-roof-surface-will-not-shade}).
+
+\begin{figure}[hbtp] % fig 3
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image003.png}
+\caption{Building heat transfer surfaces cast shadows in the direction of outward facing normal. \protect \label{fig:building-heat-transfer-surfaces-cast-shadows}}
+\end{figure}
+
+\begin{figure}[hbtp] % fig 4
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image004.png}
+\caption{Extended roof surface will not shade the walls below. \protect \label{fig:extended-roof-surface-will-not-shade}}
+\end{figure}
+
+Figure~\ref{fig:proper-surface-configurations-for-roof} shows the proper surface configurations for two types of attic construction. In all cases, the roof surface should only include the area of the roof which contacts the zone below it. In these drawings, this is an unconditioned attic space, but it could also be a conditioned zone. Any extensions of the roof which are exposed to the outdoors on both sides should be described as a shading surface.
+
+For the configuration on the left, the overhang should be a shading surface which will cast shadows in both directions (if the default mirroring is disabled the shading surface must face downward). This ensures that the correct shading will be modeled, and it also avoids overstating the heat transfer through the roof into the attic.
+
+For the configuration on the right, the attic is fully enclosed with building heat transfer surfaces for the roof and soffits. The soffits would be described as floor surfaces in the attic and would face downward. The central portion of the attic floor would be described as an interzone floor surface where the outside boundary condition is the ceiling surface in the zone below.
+
+\begin{figure}[hbtp] % fig 5
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image005.png}
+\caption{Proper surface configurations for roof overhangs for two types of attic construction. \protect \label{fig:proper-surface-configurations-for-roof}}
+\end{figure}
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/interzone-exterior-convection.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/interzone-exterior-convection.tex
new file mode 100644
index 00000000000..f978292cf19
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/interzone-exterior-convection.tex
@@ -0,0 +1,11 @@
+\section{Interzone Exterior Convection}\label{interzone-exterior-convection}
+
+\emph{Why is my exterior convection coefficient value 0?}
+
+When two surfaces are linked as interzone surfaces, the ``exterior'' side of these surfaces does not really exist. EnergyPlus links the two surfaces by using the inside temperature of surface A as the outside temperature of surface B, and the reverse. For example:
+
+Zone1WestWall has an outside boundary of Surface = Zone2EastWall
+
+Zone2EastWall has an outside boundary of Surface = Zone1WestWall
+
+Let's say that at hour 2, the inside surface temperature of Zone1WestWall is 19C, and the inside temperature of Zone2EastWall is 22C. When the heat balance is calculated for Zone1WestWall, its outside surface temperature will be set to 22C. Likewise, when the heat balance is calculated for Zone2EastWall, its outside surface temperature will be set to 19C. So, for interzone surfaces, h ext does not apply. That is why it is reported as zero.
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/modeling-reflective-radiant-barriers.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/modeling-reflective-radiant-barriers.tex
new file mode 100644
index 00000000000..f0fa57b5020
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/modeling-reflective-radiant-barriers.tex
@@ -0,0 +1,40 @@
+\section{Modeling Reflective Radiant Barriers}\label{modeling-reflective-radiant-barriers}
+
+\emph{Can EnergyPlus model reflective radiant barriers?}
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\tightlist
+\item
+  For radiant barriers which are exposed to a thermal zone, such as an attic space, specify a reduced thermal absorptance for the innermost material layer.
+\end{enumerate}
+
+For example, an attic roof construction might be (outer to inner)
+
+\begin{lstlisting}
+
+Asphalt shingles,
+  R-30 insulation,
+  Radiant barrier;
+\end{lstlisting}
+
+The radiant barrier material would be a thin layer with some small resistance with a low thermal absorptance value. This will reduce the radiant heat transfer from the roof surface to other surfaces in the attic zone.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi}.}
+\setcounter{enumi}{1}
+\tightlist
+\item
+  If the radiant barrier is within a cavity which is not modeled as a separate thermal zone, then there is not an easy way to model its impact. For example, a wall construction:
+\end{enumerate}
+
+\begin{lstlisting}
+
+Brick,
+  R-12 insulation,
+  Radiant barrier,
+  Air gap,
+  Gypsum board;
+\end{lstlisting}
+
+Here, the radiant barrier would reduce the radiant transfer across the air gap. But EnergyPlus air gaps are a fixed thermal resistance, specified in the Material:Airgap object. The user would need to compute an average effective resistance which represents the reduced radiant heat transfer across the air gap due to the radiant barrier. This resistance could then be assigned to the radiant barrier material layer.
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/rain-flag.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/rain-flag.tex
new file mode 100644
index 00000000000..24b28d9d93e
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/rain-flag.tex
@@ -0,0 +1,5 @@
+\section{Rain Flag}\label{rain-flag}
+
+\emph{Why is my exterior convection coefficient value 1000?}
+
+When the outside environment indicates that it is raining, the exterior surfaces (exposed to wind) are assumed to be wet. The convection coefficient is set to a very high number (1000) and the outside temperature used for the surface will be the wet-bulb temperature. (If you choose to report this variable, you will see 1000 as its value.)
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/solar-reflection-from-shading-surfaces.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/solar-reflection-from-shading-surfaces.tex
new file mode 100644
index 00000000000..baee3524675
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/solar-reflection-from-shading-surfaces.tex
@@ -0,0 +1,11 @@
+\section{Solar Reflection from Shading Surfaces}\label{solar-reflection-from-shading-surfaces}
+
+Exterior shading surfaces modeled using ``FullInteriorAndExteriorWithReflections'' can show some sky diffuse solar getting through the shades. When ``*WithReflections'' is active a partially sunlit shading surface reflects uniformly from the entire surface. If using WithReflections, shading surfaces should be broken into multiple surfaces at lines of intersection with other shading surfaces. This also includes places where another surface may tee into a shading surface.
+
+For example, a building is shaded by surfaces A, B, and C. Shading Surface A intercepts with Shading Surfaces B and C, and are broken into three areas A1, A2, and A3. Surface A should be entered as the shown three shading areas in order to correctly model sky diffuse solar reflection from Shading Surface A.
+
+\begin{figure}[hbtp] % fig 6
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image006.jpg}
+\caption{Limitations in modeling reflections from surfaces \protect \label{fig:limitations-in-modeling-reflections-from}}
+\end{figure}
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/using-multipliers-zone-and-or-window.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/using-multipliers-zone-and-or-window.tex
new file mode 100644
index 00000000000..23b3eda9902
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/using-multipliers-zone-and-or-window.tex
@@ -0,0 +1,217 @@
+\section{Using Multipliers (Zone and/or Window)}\label{using-multipliers-zone-andor-window}
+
+\subsection{Background and Study using Multipliers}\label{background-and-study-using-multipliers}
+
+Multipliers are used in EnergyPlus for convenience in modeling. Though window multipliers are useful for any size building when you have multiple windows on a façade, zone multipliers are more useful in large buildings with several to many stories.
+
+Zone multipliers are designed as a ``multiplier'' for floor area, zone loads, and energy consumed by internal gains. It takes the calculated load for the zone and multiplies it, sending the multiplied load to the attached HVAC system. The HVAC system size is specified to meet the entire multiplied zone load and will report the amount of the load met in the Zone/Sys Sensible Heating or Cooling Energy/Rate report variable. Autosizing automatically accounts for multipliers. Metered energy consumption by internal gains objects such as Lights or Electric Equipment will be multiplied.
+
+To illustrate the benefits (and comparison of results), the MultiStory.idf example file was used. The MultiStory file is a 9 zone, 10 story/floored building with heating (ZoneHVAC:Baseboard:Convective:Electric object) and cooling (ZoneHVAC:WindowAirConditioner object). The middle zone of each floor in the original represents 4 zones (multiplier = 4) and the middle floor (ZoneGroup) represents 8 floors (ZoneGroup multiplier = 8). Clone representations were made for comparisons:
+
+\begin{figure}[hbtp] % fig 7
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image007.png}
+\caption{Original Multistory IDF \protect \label{fig:original-multistory-idf}}
+\end{figure}
+
+In the figure above, each ``middle'' zone represents 4 zones.~ The middle ``floor'' represents 8 floors. Additionally, each of the windows has a multiplier of 4 -- so each window represents 4 windows of the same size. For the Multistory file, the Zone object for the center zones has the multiplier of 4. And for the center floors, the ZoneList and ZoneGroup objects to collect the zones and apply multipliers. The top floor then uses the Zone object multiplier for the center zones. Specifically:
+
+\begin{lstlisting}
+
+<snip>
+    Zone,
+      Gnd Center Zone,         !- Name
+      0.0,                     !- Direction of Relative North {deg}
+      8.0, 0.0, 0.0,           !- Origin [X,Y,Z] {m}
+      1,                       !- Type
+      4,                       !- Multiplier
+      autocalculate,           !- Ceiling Height {m}
+      autocalculate;           !- Volume {m3}
+  <snip>
+
+    ZoneGroup,
+      Mid Floor,               !- Zone Group Name
+      Mid Floor List,          !- Zone List Name
+      8;                       !- Zone List Multiplier
+
+
+    ZoneList,
+      Mid Floor List,          !- Zone List Name
+      Mid West Zone,           !- Zone 1 Name
+      Mid Center Zone,         !- Zone 2 Name
+      Mid East Zone;           !- Zone 3 Name
+  <snip>
+
+    Zone,
+      Top Center Zone,         !- Name
+      0.0,                     !- Direction of Relative North {deg}
+      8.0,                     !- X Origin {m}
+      0.0,                     !- Y Origin {m}
+      22.5,                    !- Z Origin {m}
+      1,                       !- Type
+      4,                       !- Multiplier
+      autocalculate,           !- Ceiling Height {m}
+      autocalculate;           !- Volume {m3}
+\end{lstlisting}
+
+For comparison purposes, clones of the middle zones were done.
+
+\begin{figure}[hbtp] % fig 8
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image008.png}
+\caption{Multistory with cloned middle zones. \protect \label{fig:multistory-with-cloned-middle-zones.}}
+\end{figure}
+
+And, finally, the entire building was created:
+
+\begin{figure}[hbtp] % fig 9
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image009.png}
+\caption{Multistory building -- fully cloned. \protect \label{fig:multistory-building-fully-cloned.}}
+\end{figure}
+
+The building is autosized. For convenience in comparison, the extreme summer and winter days were used for autosizing and the simulation was run for the 5 United States weather files that are included in the EnergyPlus release: Chicago IL; San Francisco CA; Golden CO; Tampa FL; and Washington DC.
+
+Comparisons were done with the Zone Group Loads values (Zone Group Sensible Heating Energy and Zone Group Sensible Cooling Energy) as well as meter values for Electricity. Using the regression testing limits that are used during EnergyPlus development testing (i.e.~small differences are within .001 or .5\%; big differences are greater than those limits).
+
+For the purposes of dicussion, the buildings will be called: Multistory 1 -- the original 9 zone building (with multipliers and groups) ref: Figure~\ref{fig:original-multistory-idf}; Multistory 2 -- the building shown in Figure~\ref{fig:multistory-with-cloned-middle-zones.}. Multistory with cloned middle zones.; Multistory 3 -- the fully configured building -- ref Figure~\ref{fig:multistory-building-fully-cloned.}.
+
+The following table illustrates the regression testing for Multistory 2 and Multistory 3, group loads and meters versus Multistory 1 results.
+
+% table 1
+\begin{longtable}[c]{p{1.2in}p{1.2in}p{1.2in}p{1.2in}p{1.2in}}
+\caption{Multistory vs Multistory 2 and Multistory 3 \label{table:multistory-vs-multistory-2-and-multistory-3}} \tabularnewline
+\toprule 
+LOCATION & MULTI-STORY 2 LOADS & MULTI-STORY 2 METER & MULTI-STORY 3 LOADS & MULTI-STORY 3 METER \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Multistory vs Multistory 2 and Multistory 3} \tabularnewline
+\toprule 
+LOCATION & MULTI-STORY 2 LOADS & MULTI-STORY 2 METER & MULTI-STORY 3 LOADS & MULTI-STORY 3 METER \tabularnewline
+\midrule
+\endhead
+
+USA\_IL\_Chicago-OHare.Intl.AP.725300\_TMY3 & Small Diffs & Equal & Big Diffs* (76\%) & Big Diffs* (62\%) \tabularnewline
+USA\_CA\_San.Francisco.Intl.AP.724940\_TMY3 & Big Diffs* (2.43\%) & Big Diffs* (0.6\%) & Big Diffs* (49\%) & Big Diffs* (41\%) \tabularnewline
+USA\_CO\_GOLDEN-NREL.724666\_TMY3 & Small Diffs & Small Diffs & Big Diffs* (26\%) & Big Diffs* (24\%) \tabularnewline
+USA\_FL\_Tampa.Intl.AP.722110\_TMY3 & Small Diffs & Small Diffs & Big Diffs* (6\%) & Big Diffs* (2\%) \tabularnewline
+USA\_VA\_Sterling-Washington.Dulles.Intl.AP.724030\_TMY3 & Equal & Equal & Big Diffs* (91\%) & Big Diffs* (72\%) \tabularnewline
+\bottomrule
+\end{longtable}
+
+* Big Diffs maximum occur in monthly values whereas the runperiod values are much smaller.
+
+To try to pare down the discrepancies shown here, the effects of height that are used in the calculations were removed (i.e., the Site:WeatherStation and Site:HeightVariation objects were entered as below to negate the effects of height on the environmental variables such as wind and temperature).~ In addition the height effect was removed from the OutdoorAir:Node object.
+
+\begin{lstlisting}
+
+  Site:WeatherStation,
+      ,          !- Wind Sensor Height Above Ground {m}
+      ,          !- Wind Speed Profile Exponent
+      ,          !- Wind Speed Profile Boundary Layer Thickness {m}
+      0;         !- Air Temperature Sensor Height Above Ground {m}
+
+
+    Site:HeightVariation,
+      0,         !- Wind Speed Profile Exponent
+      ,          !- Wind Speed Profile Boundary Layer Thickness {m}
+      0;         !- Air Temperature Gradient Coefficient {K/m}
+\end{lstlisting}
+
+Figure 10. Objects removing height from building impacts.
+
+With these included, the files were rerun with the following results:
+
+% table 2
+\begin{longtable}[c]{p{1.2in}p{1.2in}p{1.2in}p{1.2in}p{1.2in}}
+\caption{Multiplier Results with negated height variation. \label{table:multiplier-results-with-negated-height}} \tabularnewline
+\toprule 
+Location & Multi-story 2 Loahs & Multi-story 2 Meter & Multi-story 3 Loahs & Multi-story 3 Meter \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Multiplier Results with negated height variation.} \tabularnewline
+\toprule 
+Location & Multi-story 2 Loahs & Multi-story 2 Meter & Multi-story 3 Loahs & Multi-story 3 Meter \tabularnewline
+\midrule
+\endhead
+
+USA\_IL\_Chicago-OHare.Intl.AP.725300\_TMY3 & Small diffs & Small diffs & Small diffs & Small diffs \tabularnewline
+USA\_CA\_San.Francisco.Intl.AP.724940\_TMY3 & Small diffs & Small diffs & Small diffs & Small diffs \tabularnewline
+USA\_CO\_GOLDEN-NREL.724666\_TMY3 & Small diffs & Small diffs & Small diffs & Small diffs \tabularnewline
+USA\_FL\_Tampa.Intl.AP.722110\_TMY3 & Small diffs & Small diffs & Small diffs & Small diffs \tabularnewline
+USA\_VA\_Sterling-Washington.Dulles.Intl.AP.724030\_TMY3 & Small diffs & Small diffs & Small diffs & Small diffs \tabularnewline
+\bottomrule
+\end{longtable}
+
+To investigate if other systems might have different results, the Ideal Loads System was used as the system.~ Similar results were found for the multipliers vs cloned results. However, it may also be noted that the results between the original systems (baseboard and window ac) vs the ideal loads were very similar.
+
+The biggest difference really comes in calculation time. As shown in the following table,
+
+% table 3
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Runtimes for Multistory files (baseboard/window ac) \label{table:runtimes-for-multistory-files-baseboardwindow}} \tabularnewline
+\toprule 
+Location & Multi-story 1 (9 zones) (mm:ss) & Multi-story 2~ (18 zones) (MM:SS) & Multi-story 3 (60 zones) (MM:SS) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Runtimes for Multistory files (baseboard/window ac)} \tabularnewline
+\toprule 
+Location & Multi-story 1 (9 zones) (mm:ss) & Multi-story 2~ (18 zones) (MM:SS) & Multi-story 3 (60 zones) (MM:SS) \tabularnewline
+\midrule
+\endhead
+
+USA\_IL\_Chicago-OHare.Intl.AP.725300\_TMY3 & 1:05 & 2:14 & 13:15 \tabularnewline
+USA\_CA\_San.Francisco.Intl.AP.724940\_TMY3 & 1:04 & 2:05 & 13:20 \tabularnewline
+USA\_CO\_GOLDEN-NREL.724666\_TMY3 & 1:17 & 2:28 & 14:43 \tabularnewline
+USA\_FL\_Tampa.Intl.AP.722110\_TMY3 & 1:11 & 2:21 & 13:43 \tabularnewline
+USA\_VA\_Sterling-Washington.Dulles.Intl.AP.724030\_TMY3 & 1:05 & 2:15 & 13:18 \tabularnewline
+\bottomrule
+\end{longtable}
+
+Because the overall results were so similar, the run times for the Ideal Loads runs are included:
+
+% table 4
+\begin{longtable}[c]{p{1.5in}p{1.5in}p{1.5in}p{1.5in}}
+\caption{Runtime for Multistory files (ideal loads) \label{table:runtime-for-multistory-files-ideal-loads}} \tabularnewline
+\toprule 
+Location & Multi-story 1 (9 zones) (mm:ss) & Multi-story 2 (18 zones) (MM:SS) & Multi-story 3 (60 zones) (MM:SS) \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Runtime for Multistory files (ideal loads)} \tabularnewline
+\toprule 
+Location & Multi-story 1 (9 zones) (mm:ss) & Multi-story 2 (18 zones) (MM:SS) & Multi-story 3 (60 zones) (MM:SS) \tabularnewline
+\midrule
+\endhead
+
+USA\_IL\_Chicago-OHare.Intl.AP.725300\_TMY3 & 0:51 & 1:34 & 9:37 \tabularnewline
+USA\_CA\_San.Francisco.Intl.AP.724940\_TMY3 & 0:50 & 1:34 & 9:59 \tabularnewline
+USA\_CO\_GOLDEN-NREL.724666\_TMY3 & 0:51 & 1:40 & 10:31 \tabularnewline
+USA\_FL\_Tampa.Intl.AP.722110\_TMY3 & 0:51 & 1:36 & 10:05 \tabularnewline
+USA\_VA\_Sterling-Washington.Dulles.Intl.AP.724030\_TMY3 & 0:51 & 1:36 & 9:48 \tabularnewline
+\bottomrule
+\end{longtable}
+
+More zones (and, particularly more surfaces) make for longer run times.
+
+\subsection{Guidelines for Using Multipliers and Groups}\label{guidelines-for-using-multipliers-and-groups}
+
+\begin{itemize}
+\item
+  If the basic zone geometry is identical, make one zone, copy \& paste it as necessary, then change the Zone Origin field to locate each zone correctly.
+\item
+  Do not use interzone surfaces between zones that are multiplied. Set the adjoining surfaces to be adiabatic, i.e.~use the OtherZoneSurface exterior boundary condition with the other surface pointing back to itself.
+\item
+  Locate the middle floor zones roughly halfway between top and ground because exterior convection coefficients change with height. Halfway should cause the differences to average out. If you have many stories (the example only has 10 stories), consider using more middle floor zones.
+\item
+  Consider removing the effects of height variation for the simulation.
+\item
+  Follow guidelines in HVACTemplate and other objects about sizing if you are mixing autosize fields with hard sized fields (recommended to ``autosize'' all fields rather than mix).
+\item
+  All HVAC system sizes must be specified to meet the entire multiplied zone load.
+\item
+  Autosizing automatically accounts for multipliers.
+\end{itemize}
diff --git a/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/using-osc-other-side-coefficients-to-create.tex b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/using-osc-other-side-coefficients-to-create.tex
new file mode 100644
index 00000000000..c3e5de96136
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/building-geometry-shading-zone-model/using-osc-other-side-coefficients-to-create.tex
@@ -0,0 +1,130 @@
+\section{Using OSC (Other Side Coefficients) to create controlled panels}\label{using-osc-other-side-coefficients-to-create-controlled-panels}
+
+The Other Side Coefficient (OSC) equation permits setting either the outside surface temperature or the outside air temperature to a constant value or a scheduled value based on the size of the first input parameter, N1. The original temperature equation was:
+
+\begin{equation}
+T = N_2 T_{zone} + N_3 T_{oadb} + N_4 N_5 + N_6 T_{grnd} + N_7 W_{spd} T_{oadb}
+\end{equation}
+
+where:
+
+\begin{itemize}
+\item
+  \(T\) = Outside Air Temperature when N1 (Combined convective/radiative film Coeff) \textgreater{} 0
+\item
+  \(T\) = Exterior Surface Temperature when N1 (Combined convective/radiative film Coeff) \textless{} = 0
+\item
+  \(T_{zone}\) = MAT = Temperature of the zone being simulated (°C)
+\item
+  \(T_{oadb}\) = Dry-bulb temperature of the outdoor air (°C)
+\item
+  \(T_{grnd}\) = Temperature of the ground (°C) Wspd = Outdoor wind speed (m/sec)
+\end{itemize}
+
+The coefficients N\(_{2}\), N\(_{3}\), N\(_{4}\), N\(_{6}\), and N\(_{7}\) scale the contribution of the various terms that follow them.~ In the case of N\(_{4}\), it is followed by another term N\(_{5}\).~ This is a constant temperature that can also be overridden by a scheduled value. Note that in some EnergyPlus documentation, the N's are given as C's.
+
+This object has been changed to permit the outside temperature, T, to be controlled to a set point temperature that is specified as N\(_{5}\) or comes from the schedule A2.
+
+Note that since the surface that contains the panel subsurfaces (that must be called doors in EnergyPlus) receives that same outside temperature as the panels, it should have a construction with a very high thermal resistance to essentially take it out of the room heat balance calculation.
+
+An Example input file object is shown below.
+
+\begin{lstlisting}
+
+SurfaceProperty:OtherSideCoefficients,
+     Zn001:Roof001:OSC, !- Name
+     0,   ! (N1) Combined Convective/Radiative Film Coefficient {W/m2-K}
+     0,   ! (N5) Constant Temperature {C}
+     0.95,!(N4) Constant Temperature Coefficient
+     ,    ! (N3)External Dry-Bulb Temperature Coefficient
+     ,    ! (N6)Ground Temperature Coefficient
+     ,    ! (N7)Wind Speed Coefficient
+     -.95,! (N2) Zone Air Temperature Coefficient
+     ConstantCooling,     ! (A2) Constant Temperature Schedule Name
+     No,  ! (A3)Sinusoidal Variation of Constant Temperature Coefficient
+     24,  ! (N8)Period of Sinusoidal Variation {hr}
+     1.,  ! (N9)Previous Other Side Temperature Coefficient
+     5.,  !(N10) Minimum Other Side Temperature Limit
+     25.; ! (N11) Maximum Other Side Temperature Limit
+\end{lstlisting}
+
+This object results in the following equation for T:
+
+T = 1.0*Tlast +0.95*(Tsetpoint -- TzoneAir)~~ (with limits)
+
+The result of this is that the surface temperature, T, will be changed to the temperature that will force the zone air temperature to the setpoint providing the temperature limits are not reached. When the zone air temperature is at the setpoint, T remains at the value it had in the prior time step.
+
+A complete example with all pertinent objects:
+
+\begin{lstlisting}
+
+  Construction,
+      PanelConst,              !- Name
+      Std Steel_Brown_Regular; !- Outside Layer
+
+
+    Material,
+      Std Steel_Brown_Regular, !- Name
+      Smooth,                  !- Roughness
+      1.5000000E-03,           !- Thickness {m}
+      44.96960,                !- Conductivity {W/m-K}
+      7689.000,                !- Density {kg/m3}
+      418.0000,                !- Specific Heat {J/kg-K}
+      0.9000000,               !- Thermal Absorptance
+      0.9200000,               !- Solar Absorptance
+      0.92000000;              !- Visible Absorptance
+
+
+    BuildingSurface:Detailed,
+      Zn001:Roof001,           !- Name
+      Roof,                    !- Surface Type
+      ROOF31,                  !- Construction Name
+      ZONE ONE,                !- Zone Name
+      OtherSideCoefficients,   !- Outside Boundary Condition
+      Zn001:Roof001:OSC,       !- Outside Boundary Condition Object
+      NoSun,                   !- Sun Exposure
+      NoWind,                  !- Wind Exposure
+      0,                       !- View Factor to Ground
+      4,                       !- Number of Vertices
+      0.000000,15.24000,4.572,  !- X,Y,Z = = > Vertex 1 {m}
+      0.000000,0.000000,4.572,  !- X,Y,Z = = > Vertex 2 {m}
+      15.24000,0.000000,4.572,  !- X,Y,Z = = > Vertex 3 {m}
+      15.24000,15.24000,4.572;  !- X,Y,Z = = > Vertex 4 {m}
+
+
+    FenestrationSurface:Detailed,
+      panel002,                !- Name
+      Door,                    !- Surface Type
+      PanelConst,              !- Construction Name
+      Zn001:Roof001,           !- Building Surface Name
+      ,                        !- Outside Boundary Condition Object
+      autocalculate,           !- View Factor to Ground
+      ,                        !- Shading Control Name
+      ,                        !- Frame and Divider Name
+      1,                       !- Multiplier
+      4,                       !- Number of Vertices
+      3,2,4.572,  !- X,Y,Z = = > Vertex 1 {m}
+      3,3,4.572,  !- X,Y,Z = = > Vertex 2 {m}
+      4,3,4.572,  !- X,Y,Z = = > Vertex 3 {m}
+      4,2,4.572;  !- X,Y,Z = = > Vertex 4 {m}
+
+
+    SurfaceProperty:OtherSideCoefficients,
+      Zn001:Roof001:OSC,       !- Name
+      0,            !- Combined Convective/Radiative Film Coefficient {W/m2-K}
+      0,                       !- Constant Temperature {C}
+      0.95,                    !- Constant Temperature Coefficient
+      ,                        !- External Dry-Bulb Temperature Coefficient
+      ,                        !- Ground Temperature Coefficient
+      ,                        !- Wind Speed Coefficient
+      -.95,                    !- Zone Air Temperature Coefficient
+      ConstantTwentyTwo,       !- Constant Temperature Schedule Name
+      No,           !- Sinusoidal Variation of Constant Temperature Coefficient
+      24,                      !- Period of Sinusoidal Variation {hr}
+      1.,                      !- Previous Other Side Temperature Coefficient
+      5.,                      !- Minimum Other Side Temperature Limit {C}
+      25.;                     !- Maximum Other Side Temperature Limit {C}
+
+
+  Schedule:Constant,ConstantTwentyTwo,PanelControl,22;
+\end{lstlisting}
diff --git a/doc/tips-and-tricks-using-energyplus/src/datasets.tex b/doc/tips-and-tricks-using-energyplus/src/datasets.tex
new file mode 100644
index 00000000000..1396d202832
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/datasets.tex
@@ -0,0 +1 @@
+\chapter{DataSets}\label{datasets}
diff --git a/doc/tips-and-tricks-using-energyplus/src/datasets/datasets-aka-libraries.tex b/doc/tips-and-tricks-using-energyplus/src/datasets/datasets-aka-libraries.tex
new file mode 100644
index 00000000000..8f2f7ad8632
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/datasets/datasets-aka-libraries.tex
@@ -0,0 +1,7 @@
+\section{Datasets aka Libraries}\label{datasets-aka-libraries}
+
+EnergyPlus uses the term DataSets for what many would call libraries. These files are included, for the most part, in the instalation package but may be available from other sites (such as the helpdesk or Yahoo Groups).
+
+There are two flavors of DataSets: \textbf{simple} and \textbf{Macro}. Some sets have files in both camps (for example, Solar Collectors). Both flavors contain IDF objects ready to be put into EnergyPlus input files. With the simple datasets, you may need to use a text editor or the IDF Editor to search the file for the one you want to use.~ With the macro datsets and a simply structured imf (input macro file), you can name the item you want to include. (The macro program is described in the \href{file:///E:/Docs4PDFs/AuxiliaryPrograms.pdf}{Auxiliary Programs document}).
+
+Primary documentation for each dataset is found in the \href{file:///E:/Docs4PDFs/OutputDetailsAndExamples.pdf}{Output Details and Examples document}. Highlights of some datasets are given here.
diff --git a/doc/tips-and-tricks-using-energyplus/src/datasets/locations-designdays.tex b/doc/tips-and-tricks-using-energyplus/src/datasets/locations-designdays.tex
new file mode 100644
index 00000000000..8129e7c275d
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/datasets/locations-designdays.tex
@@ -0,0 +1,26 @@
+\section{Locations-DesignDays}\label{locations-designdays}
+
+This file (Locations-DesignDays.xls) can be found in the MacroDataSets folder. While not strictly a macro file, it leads one to be able to download the ASHRAE design day definitions from the EnergyPlus website. The spreadsheet format contains a sheet for each of the WMO regions as well as the California Climate Zones, specifically sheets included are:
+
+\begin{itemize}
+\item
+  Readme -- an upfront readme page
+\item
+  WMO1 Africa
+\item
+  WMO2 Asia
+\item
+  WMO3 South America
+\item
+  WMO4 North \& Central America
+\item
+  CZ Files -- California Climate Zones
+\item
+  WMO5 Southwest Pacific
+\item
+  WMO6 Europe
+\item
+  WMO7 Antarctica
+\end{itemize}
+
+Each WMO (World Meteorological Organization) page contains the countries represented, specific cities that have design conditions data from ASHRAE, a link to the full imf file with location, daylighting saving and design day definitions as well as a link to that region's weather page on the EnergyPlus website. Pressing the links here will allow you to download the files.
diff --git a/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data.tex b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data.tex
new file mode 100644
index 00000000000..106585c69ed
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data.tex
@@ -0,0 +1 @@
+\chapter{Design Day / Weather Data}\label{design-day-weather-data}
diff --git a/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/design-day-creation.tex b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/design-day-creation.tex
new file mode 100644
index 00000000000..e75da1444d2
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/design-day-creation.tex
@@ -0,0 +1,11 @@
+\section{Design Day Creation}\label{design-day-creation}
+
+\emph{How do I create the profile used in the SizingPeriod:DesignDay object?}
+
+Typically, the EnergyPlus Development Team uses the data from the most recent ASHRAE Handbook of Fundamentals to create a set of design day profiles that can be used. Description of ASHRAE's data is contained in Chapter 14 of the 2009 Handbook of Fundamentals. Table~\ref{table:multistory-vs-multistory-2-and-multistory-3} shows the kind of data that is embodied in the design day definitions shown earlier (ref. Locations-DesignDays).
+
+Design Days (aka Design Conditions) are very important for use in HVAC Sizing calculations -- refer to the ASHRAE Handbook of Fundamentals for further information.
+
+From this, you can determine if you should use one of these profiles and modify it or determine how to create your own profile.
+
+The Weather Converter program accesses this file when it processes (even for statistics) a weather file. Design Day definitions are also included with the zips on the EnergyPlus weather data site. For locations that don't have ASHRAE design conditions, the Weather Converter uses the data within the weather file to generate pseudo conditions in the statistics file.
diff --git a/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/epw-weather-files.tex b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/epw-weather-files.tex
new file mode 100644
index 00000000000..583d8ea5def
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/epw-weather-files.tex
@@ -0,0 +1,3 @@
+\section{EPW Weather Files}\label{epw-weather-files}
+
+The WeatherConverter converts from other source formats to EPW and EnergyPlus CSV formats. The WeatherConverter also produces a statistics file that provides a quick synopsis of the converted data and is used by the tabular reports (ref: Climatic Data Summary report). For Ecotect users, the Weather Converter can also save as .wea format. We do not support conversion of EPWs to other formats, including to TMY2. The Weather Converter is described in detail in the \href{file:///E:/Docs4PDFs/AuxiliaryPrograms.pdf}{Auxiliary Programs document}.
diff --git a/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/measuring-solar-data.tex b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/measuring-solar-data.tex
new file mode 100644
index 00000000000..416a1a16c82
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/measuring-solar-data.tex
@@ -0,0 +1,13 @@
+\section{Measuring Solar Data}\label{measuring-solar-data}
+
+\emph{Can the following weather file metrics be directly measured by some inexpensive devices?}
+
+Extraterrestrial Horizontal Radiation \{Wh/m2\} Extraterrestrial Direct Normal Radiation \{Wh/m2\} Horizontal Infrared Radiation Intensity from Sky \{Wh/m2\} Global Horizontal Radiation \{Wh/m2\} Direct Normal Radiation \{Wh/m2\} Diffuse Horizontal Radiation \{Wh/m2\} Global Horizontal Illuminance \{lux\} Direct Normal Illuminance \{lux\} Diffuse Horizontal Illuminance \{lux\}*
+
+You can't measure extraterrestrial unless you're in outer space, but then it's assumed to be constant anyway. For the various radiation and illuminance values, they can measured by various instrumentation ranging from the very cheap to the very expensive. Properly, radiation needs to be measured with a pyranometer (Eppley), which is pricy, but I'm also seen people use simpler apparatus (Lycors) that are really photometers. Direct beam is generally not measured, but derived by subtracting the diffuse from the global. Diffuse is measured by adding a shadow band over a pyranometer to block out the direct beam. Pyranometers measure heat, photometers measure light. All the illuminance on the weather files are derived from the radiation and sky conditions.
+
+Do not forget that the quantities you list are the inputs to the models that are used to derive the variables you really need in practice: irradiance and illuminance on the facets of the building (windows especially). These facets are usually NOT horizontal. Measuring all the components for all tilts and azimuths can be a costly proposition, and that's why it is rarely done (hence the need for models), but that's what should be done in serious experiments to remove the (large) uncertainties in modeled radiation.
+
+Illuminance is measured with photometers (from, e.g., Licor), which resemble silicon-based pyranometers. Both are less costly than thermopile radiometers, which are normally the best in terms of accuracy. Measurements obtained with silicon-based pyranometers need various corrections to account for their limited spectral range. No correction is needed for photometers, though. So you have this issue of accuracy vs cost to consider.
+
+Direct irradiance is measured with a pyrheliometer, which tracks the sun and is therefore costly, but also the most accurate of all radiometers. Obtaining direct irradiance by subtracting diffuse from global is convenient, but not accurate, as shown in recent publications.
diff --git a/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/meteonorm-weather-files.tex b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/meteonorm-weather-files.tex
new file mode 100644
index 00000000000..2398d5d4c59
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/meteonorm-weather-files.tex
@@ -0,0 +1,7 @@
+\section{Meteonorm Weather Files}\label{meteonorm-weather-files}
+
+For locations that aren't on the regular EnergyPlus weather site (http://apps1.eere.energy.gov/buildings/energyplus/cfm/weather\_data.cfm ), the team has created weather data using the Meteonormâ„¢ software. Meteonorm extrapolates hourly data from statistical data for a location. Where statistical data aren't available, Meteonorm interpolates from other nearby sites. Generally, a statistical approach is a last resort---weather files generated from statistics will not demonstrate the normal hour-to-hour and day-to-day variability seen in measured data. Each .ZIP includes a .STAT (EnergyPlus weather data statistics), .EPW (EnergyPlus weather file), and .INFO (Information about the source data and limitations from Meteonorm).
+
+In all cases, review the .STAT file for the location before using any of these files to ensure that it represents the climate of the locations as you understand it. In many cases, a nearby location with measured data may be more appropriate than one derived from statistics. These files, once created, are published on the EnergyPlus Yahoo Group site.
+
+As always, if you know of sources of weather data that we might be able to share with the EnergyPlus community, please contact us.
diff --git a/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/weather-data-for-simulations.tex b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/weather-data-for-simulations.tex
new file mode 100644
index 00000000000..3eb3f80b084
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/weather-data-for-simulations.tex
@@ -0,0 +1,7 @@
+\section{Weather Data for Simulations}\label{weather-data-for-simulations}
+
+Weather data can be used for various purposes by simulation program such as EnergyPlus. For some purposes, such as validating a model to actual energy use, you may wish to match the weather data to the simulation period. However, for most purposes, you will wish to have a more typical weather data profile. Information on selecting weather data is described in this paper:
+
+Drury B. Crawley. 1998. ``Which Weather Data Should You Use for Energy Simulations of Commercial Buildings?'' in ASHRAE Transactions, pp.~498-515, Vol. 104, Pt. 2. Atlanta: ASHRAE. (PDF 197 KB)
+
+PDF: http://energyplus.gov/pdfs/bibliography/whichweatherdatashouldyouuseforenergysimulations.pdf
diff --git a/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/weather-file-sources.tex b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/weather-file-sources.tex
new file mode 100644
index 00000000000..147f2817367
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/design-day-weather-data/weather-file-sources.tex
@@ -0,0 +1,3 @@
+\section{Weather File Sources}\label{weather-file-sources}
+
+The description of sources for the EnergyPlus weather data that is on the website are available here: http://apps1.eere.energy.gov/buildings/energyplus/weatherdata\_sources.cfm
diff --git a/doc/tips-and-tricks-using-energyplus/src/documentation-and-guides.tex b/doc/tips-and-tricks-using-energyplus/src/documentation-and-guides.tex
new file mode 100644
index 00000000000..08e70851814
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/documentation-and-guides.tex
@@ -0,0 +1,3 @@
+\chapter{Documentation and Guides}\label{documentation-and-guides}
+
+Note that the PDF documents are fully indexed and searchable. Will save you time and waiting for support to answer on some questions.
diff --git a/doc/tips-and-tricks-using-energyplus/src/error-messages-details.tex b/doc/tips-and-tricks-using-energyplus/src/error-messages-details.tex
new file mode 100644
index 00000000000..8879bc36259
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/error-messages-details.tex
@@ -0,0 +1,11 @@
+\chapter{Error Messages (Details)}\label{error-messages-details}
+
+Error messages are produced from several parts of EnergyPlus and at several times prior to and during Input Processing (comparing IDF fields/values to IDD requirements); during GetInput for each module (further checking for correct values from the IDF); during Sizing operations; during Warmup operations; and finally during simulation of the environments.
+
+It is easy to separate the Sizing and Warmup errors from the rest. A summary is provided at the end of the simulation:
+
+\begin{lstlisting}
+************* EnergyPlus Warmup Error Summary. During Warmup: 0 Warning; 0 Severe Errors.
+************* EnergyPlus Sizing Error Summary. During Sizing: 0 Warning; 0 Severe Errors.
+************* EnergyPlus Completed Successfully-- 1 Warning; 0 Severe Errors; Elapsed Time = 00hr 00min  6.58sec
+\end{lstlisting}
diff --git a/doc/tips-and-tricks-using-energyplus/src/error-messages-details/error-summary.tex b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/error-summary.tex
new file mode 100644
index 00000000000..abf8d443af8
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/error-summary.tex
@@ -0,0 +1,5 @@
+\section{Error Summary}\label{error-summary}
+
+This section has provided a flavor of the breadth of messages coming out of EnergyPlus for various conditions. They are consolidated into one file (eplusout.err) for the most part though some may have more contexts given in other files. (eplusout.audit may illustrate exact places in the IDF where warnings or errors occur -- as noted during Input Processing.)
+
+The error section in this document will continue to grow as time allows. Suggestions are always welcome.
diff --git a/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-during-sizing.tex b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-during-sizing.tex
new file mode 100644
index 00000000000..791b9d0383d
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-during-sizing.tex
@@ -0,0 +1,49 @@
+\section{Example Error Messages during Sizing and Simulation}\label{example-error-messages-during-sizing-and-simulation}
+
+\subsection{Warning}\label{warning}
+
+\begin{lstlisting}
+Calculated design cooling load for zone = B1AE_FCU02_AN is zero.
+Check Sizing:Zone and ZoneControl:Thermostat inputs.
+\end{lstlisting}
+
+\begin{lstlisting}
+Calculated design heating load for zone = B1AE\_FCU02\_AN is zero.
+Check Sizing:Zone and ZoneControl:Thermostat inputs.
+\end{lstlisting}
+
+Two flavors of the same message showing up during Sizing. Read about Day Types in the Sizing:* objects.~ Schedules may affect how the program looks at loads during sizing. Another suggestion is:
+
+Plot the zone temperature and check against the zone thermostat set point temperature.
+
+\begin{lstlisting}
+Output:Variable,*,Zone/Sys Air Temperature at Thermostat,timestep;
+Output:Variable,*,Zone/Sys Thermostat Heating Setpoint,timestep;
+\end{lstlisting}
+
+If the zone temperature never falls below the thermostat set point temperature then there really is no load and lighting, equipment, occupancy, etc inputs/schedules need to be checked. Usually these types of load will be turned off for the design days in winter to correctly size the heating system. If the zone temperature does fall below the zone thermostat temperature, then the zone sizing objects probably have bad inputs.
+
+\subsection{Severe}\label{severe}
+
+\begin{lstlisting}
+Temperature (high) out of bounds (206.82] for zone = "ZONE 1", for surface = "SOUTH WALL"
+During Warmup & Sizing, Environment = ALEXANDRIA ESLER REGIONAL AP ANN HTG 99.6% CONDNS DB, at Simulation time = 12/21 01:00 - 01:04
+Zone = "ZONE 1", Diagnostic Details:
+...Internal Heat Gain [155.557] W/m2
+...Infiltration/Ventilation [3.500E-002] m3/s
+...Mixing/Cross Mixing [0.000] m3/s
+...Zone is part of HVAC controlled system.
+\end{lstlisting}
+
+This error may be related to one of the warnings during get input routines on the Design Level of some heat gains at the zone level. Also to be noted here is the amount of Infiltration/Ventilation being introduced at the zone level. This diagnostics detail is produced once for each zone where the error occurs.
+
+\subsection{Fatal}\label{fatal}
+
+\begin{lstlisting}
+EnergyPlus has exited due to the reason stated above
+...Summary of Errors that led to program termination:
+..... Reference severe error count = 11
+..... Last severe error = Temperature (high) out of bounds (210.11] for zone = "ZONE 1", for surface = "ROOF1"
+\end{lstlisting}
+
+Typical fatal condition. A small summary of the number of severe errors that were produced along with the last severe error.
diff --git a/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-for-preprocessors.tex b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-for-preprocessors.tex
new file mode 100644
index 00000000000..e2fdde0b777
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-for-preprocessors.tex
@@ -0,0 +1,39 @@
+\section{Example Error Messages for Preprocessors}\label{example-error-messages-for-preprocessors}
+
+All of the preprocessing programs (e.g., EP-Macro, ExpandObjects) produce Output:PreprocessorMessage objects for the errors they detect. Any preprocessor can produce these objects.~ You may need to consult with actual preprocessor program documentation to understand these errors. The output preprocessor messages appear first in the .err file. The format for the messages are: \textless{}objectname\textgreater{} (i.e.~Output:Preprocessormessage) followed by the program name (e.g.~EPMacro) in quotes and then the strings for the message, whether Warning, Severe or Fatal.~ If Fatal, EnergyPlus will fatal out after producing all the error messages.
+
+Here are some examples:
+
+\subsection{Warning}\label{warning-000}
+
+\begin{lstlisting}
+Output:PreprocessorMessage = "EPXMLPreProc2" has the following Warning conditions:
+   **   ~~~   ** Problem with the width for requested floor area and
+   **   ~~~   ** perimeter depth.  Reduced perimeter depth from 4.57
+   **   ~~~   ** to 3.656 to accommodate perimeter and core layout
+\end{lstlisting}
+
+\subsection{Severe}\label{severe-000}
+
+\begin{lstlisting}
+Output:PreprocessorMessage = "EPMacro" has the following Severe conditions:
+   **   ~~~   ** at approximately input line number = 200: column = 11
+   **   ~~~   ** cannot find/read include file
+   **   ~~~   ** symbol = HVAC3ZoneMat-Const.imf
+   **   ~~~   ** refer to <file>.epmdet for details.
+\end{lstlisting}
+
+Some preprocessor utility programs will give more details than others.~ Here, you see at input file line number 200, about column 11, that the program cannot find (or read) the include file and that there will be more details after the end of EnergyPlus processing in the file with epmdet for extension.
+
+\begin{lstlisting}
+Output:PreprocessorMessage = "GroundTempCalc - Slab" has the following Fatal condition:
+   **   ~~~   ** No in.epw file found
+\end{lstlisting}
+
+This message is coming from the Slab preprocessor program after the ExpandObjects program has processed the input file and triggered the Slab program to be executed. There is no weather file and the Slab program cannot run.
+
+\subsection{Fatal}\label{fatal-000}
+
+Preprocessor condition(s) cause termination.
+
+As you can see from the above Slab message, preprocessor programs may signal a fatal condition but the actual message you see in the .err file is a Severe. You will see the above message if any of the preprocessor conditions signaled a fatal error.
diff --git a/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-for-the-input.tex b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-for-the-input.tex
new file mode 100644
index 00000000000..c5590ef1f7b
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-for-the-input.tex
@@ -0,0 +1,55 @@
+\section{Example Error Messages for the Input Processor}\label{example-error-messages-for-the-input-processor}
+
+The InputProcessor is a part of the EnergyPlus program and scans each input file, matching it against requirements from the Energy+.idd file (Input Data Dictionary). InputProcessor errors all start with IP as their first characters.
+
+\subsection{Warning}\label{warning-001}
+
+\begin{lstlisting}
+IP: Note -- Some missing fields have been filled with defaults. See the audit output file for details.
+\end{lstlisting}
+
+This message notes that you have some objects where the ``min-fields'' for the object have not been fulfilled and, therefore, the object will be filled with defaults. If you are curious, open the .audit file and search for Warnings.
+
+\subsection{Severe}\label{severe-001}
+
+\begin{lstlisting}
+IP: IDF line~345 Did not find "UNTIL: 22:00" in list of Objects
+\end{lstlisting}
+
+You may have entered a semi-colon character (;) at the end of one of the lines in a~\href{http://www.designbuilder.co.uk/programhelp/schedules_-_energyplus_compact_schedules.htm}{Schedule:Compact} when you meant to enter a comma (,). Note that the approximate line number in your file (345) is given to help you locate it in a text editor. Look in the prior line -- it probably needs to end in a comma.
+
+\begin{lstlisting}
+IP: IDF line~xxx Did not find "xxxxxx" in list of Objects
+\end{lstlisting}
+
+Same basic description as the previous error message.~ The line number in your file is given to help you locate it.~ Look in the prior line (ignoring any comment lines) -- it probably needs to end with a comma.
+
+\begin{lstlisting}
+IP: No items found for Required Object = BUILDING
+IP: Required Object = "BUILDING" not found in IDF.
+\end{lstlisting}
+
+The Building object is required for all inputs.~ It was not found in this input file.
+
+\begin{lstlisting}
+IP: No items found for Required Object = GLOBALGEOMETRYRULES
+IP: Required Object = "GLOBALGEOMETRYRULES" not found in IDF.
+\end{lstlisting}
+
+The GlobalGeometryRules object is required for all inputs. It was not found in this input file.
+
+\begin{lstlisting}
+IP: Possible incorrect IDD File
+IDD Version:"IDD\_Version xxx"
+Possible Invalid Numerics or other problems
+\end{lstlisting}
+
+This message means the program is about to terminate. You look at previous error messages in the .err file to determine the most likely cause(s). The IDD version number is given in case you have an ``x'' version file and you are running it with a ``y'' version IDD (which may or may not work, in general).
+
+\subsection{Fatal}\label{fatal-001}
+
+\begin{lstlisting}
+IP: Errors occurred on processing IDF file. Preceding condition(s) cause termination.
+\end{lstlisting}
+
+Just the final note before the program terminates. Look at previous error messages in the .err file.
diff --git a/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-from-module-getinput.tex b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-from-module-getinput.tex
new file mode 100644
index 00000000000..d318dc543b8
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/example-error-messages-from-module-getinput.tex
@@ -0,0 +1,140 @@
+\section{Example Error Messages from Module GetInput routines}\label{example-error-messages-from-module-getinput-routines}
+
+As the simulation starts, each module gets called and gets the values from the input file. These are usually referred to as GetInput routines. They add another error check on the inputs that cannot be fully described by the IDD limits plus they are privy to interactions that their object may have to another object.
+
+\subsection{Warning}\label{warning-002}
+
+\begin{lstlisting}
+Site:GroundTemperature:BuildingSurface: Some values fall outside the range of 15-25C.
+These values may be inappropriate.  Please consult the Input Output Reference for more details.
+\end{lstlisting}
+
+Ground temperatures can have a significant influence on buildings. Values outside the range indicated may give you inaccurate simulation temperatures. Consult the Input Output Reference for more details.
+
+\begin{lstlisting}
+GetSurfaceData: CAUTION -- Interzone surfaces are usually in different zones
+Surface = WALLMASS, Zone = ZONE1
+Surface = iz-WALLMASS, Zone = ZONE1
+\end{lstlisting}
+
+Conventionally, interzone surfaces separate two zones. However, some advanced users may create them in the same zone for certain heat transfer efficiencies. This warning message alerts you in case that was not your intention.
+
+\begin{lstlisting}
+Weather file location will be used rather than entered Location object.
+..Location object = ATLANTA
+..Weather File Location = Tampa International Ap FL USA TMY3 WMO# = 722110
+..due to location differences, Latitude difference = [5.68] degrees, Longitude difference = [1.89] degrees.
+..Time Zone difference = [0.0] hour(s), Elevation difference = [98.10] percent, [309.00] meters.
+\end{lstlisting}
+
+You have ``attached'' a weather file that contains different location information than your Site:Location object. The program is warning you of this condition.
+
+\begin{lstlisting}
+GetPollutionFactorInput: Requested reporting for Carbon Equivalent Pollution, but insufficient information is entered.
+\end{lstlisting}
+
+Both ``FuelFactors'' and ``EnvironmentalImpactFactors'' must be entered or the displayed carbon pollution will all be zero.
+
+You have requested reporting for Carbon Equivalent Pollution (output variables) but you have not entered the required FuelFactor and EnvironmentalImpactFactor objects that are necessary to trigger these outputs properly.
+
+\begin{lstlisting}
+BuildingSurface:Detailed = "SURF:xyz", Sun Exposure = "SUNEXPOSED".
+ ..This surface is not exposed to External Environment.  Sun exposure has no effect.
+\end{lstlisting}
+
+The surface has been entered with SunExposed but it is not an exterior/outdoor surface.
+
+\begin{lstlisting}
+GetSurfaceData: InterZone Surface Areas do not match as expected and might not satisfy conservation of energy:
+   Area = 1.4E-002 in Surface = 319767, Zone = 2PAV_CONDIC_LOJA_D
+   Area = 67.0 in Surface = 6C0708, Zone = 3PAV_CONDIC_TEATRO_G
+\end{lstlisting}
+
+Interzone surface areas usually should be matching between the two zones.
+
+\begin{lstlisting}
+GetSurfaceData: InterZone Surface Azimuths do not match as expected.
+   Azimuth = 270.0, Tilt = 90.0, in Surface = 319767, Zone = 2PAV_CONDIC_LOJA_D
+   Azimuth = 180.0, Tilt = 90.0, in Surface = 6C0708, Zone = 3PAV_CONDIC_TEATRO_G
+..surface class of base surface = Wall
+\end{lstlisting}
+
+Interzone surfaces should be opposite each other -- therefore when Azimuth/Facing do not differ by 180 degrees, a warning is shown. Likewise, Tilt angles should be checked here.
+
+\begin{lstlisting}
+GetVertices: Floor is upside down! Tilt angle = [0.0], should be near 180, Surface = "ROOM302-FLOOR", in Zone = "ROOM302".
+Automatic fix is attempted.
+\end{lstlisting}
+
+\begin{lstlisting}
+GetVertices: Roof is upside down! Tilt angle = [180.0], should be near 0, Surface = "ROOM302-CEILING", in Zone = "ROOM302".
+Automatic fix is attempted.
+\end{lstlisting}
+
+In both of these messages, it has been detected that the outward surface normal for the surfaces is not as expected. With not as expected angles, the sun will not be received on these surfaces (typically), so it is something to correct. The program attempts to fix these -- usually caused by entering the vertices backwards (i.e.~clockwise when should have been counter-clockwise or vice versa).
+
+\begin{lstlisting}
+GetInternalHeatGains: Zone = "02AO_FCU04_AN" occupant density is extremely high.
+Occupant Density = [14] person/m2.
+Occupant Density = [7.000E-002] m2/person. Problems in Temperature Out of Bounds may result.
+\end{lstlisting}
+
+The Get Internal Heat Gains routine does some checks as far as Design Level (and maximum schedule * Design Level) and compares to density values. Extremely high gains, especially when no exit for the air (i.e.~infiltration, ventilation) can often result in Temperature Out of Bounds errors (see below in Simulation messages) and these can be fatal.
+
+\begin{lstlisting}
+GetVertices: Distance between two vertices < .01, possibly coincident. for Surface = 1%PIANOINTERRATO:UFFICI_WALL_3_0_1, in Zone = 1%PIANOINTERRATO:UFFICI
+Vertex [2] = (-53.99,5.86,0.50)
+Vertex [1] = (-53.99,5.86,0.51)
+Dropping Vertex [2].
+\end{lstlisting}
+
+The distance between two vertices is very small (.01 meter \textasciitilde{} .4 inches). This distance is too small for shading calculations and the vertex is dropped.
+
+\begin{lstlisting}
+CheckConvexity: Surface = "ZN001:ROOF001" is non-convex.
+\end{lstlisting}
+
+Shown when DisplayExtraWarnings is on and a surface is not a convex shape. By itself, this is only a warning but see the severe in the next section when it has impact on the calculations.
+
+\subsection{Severe}\label{severe-002}
+
+\begin{lstlisting}
+GetSurfaceData: Some Outward Facing angles of subsurfaces differ significantly from base surface.
+...use Output:Diagnostics,DisplayExtraWarnings; to show more details on individual surfaces.
+\end{lstlisting}
+
+\begin{lstlisting}
+GetSurfaceData: Outward facing angle [95.5] of subsurface = "WL2-1" significantly different than
+..facing angle [275.5] of base surface = WEST WALL 2 Tilt = 90.0
+..surface class of base surface = Wall
+\end{lstlisting}
+
+These are two versions of the same message.~ The first is shown when DisplayExtraWarnings is not activated. The second is shown for details on each subsurface that has the error.~ The error is usually that the subsurface vertices have been entered in opposite order (i.e.~clockwise vs counter-clockwise) from the base surface.
+
+\begin{lstlisting}
+This building has no thermal mass which can cause an unstable solution.
+Use Material object for all opaque material definitions except very light insulation layers.
+\end{lstlisting}
+
+You have probably defined all the surfaces in this building with resistive only constructions (i.e.~object Material:NoMass). An unstable solution can result (including crashes).
+
+\begin{lstlisting}
+GetVertices: Distance between two vertices < .01, possibly coincident. for Surface = 1%PIANOINTERRATO:UFFICI_WALL_3_0_1, in Zone = 1%PIANOINTERRATO:UFFICI
+Vertex [3] = (-44.82,-12.14,0.51)
+Vertex [2] = (-44.82,-12.14,0.50)
+Cannot Drop Vertex [3].
+Number of Surface Sides at minimum.
+\end{lstlisting}
+
+The distance between two vertices is very small (.01 meter \textasciitilde{} .4 inches). This distance is too small for shading calculations but the vertex cannot be dropped as that would bring the surface to less than 3 sides. This surface is degenerate and should be removed from your input file.
+
+\begin{lstlisting}
+DetermineShadowingCombinations: Surface = "0%VESPAIO:ZONA1\_ROOF\_1\_6\_0" is a receiving surface and is non-convex.
+...Shadowing values may be inaccurate. Check .shd report file for more surface shading details
+\end{lstlisting}
+
+Receiving surfaces which are not convex shapes will not be calculated correctly with the shadowing routines. You should view the results carefully.
+
+\subsection{Fatal}\label{fatal-002}
+
+Severes in this realm usually lead to Fatals. Preceding conditions lead to termination.
diff --git a/doc/tips-and-tricks-using-energyplus/src/error-messages-details/psychrometric-errors.tex b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/psychrometric-errors.tex
new file mode 100644
index 00000000000..804d7d30ae2
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/psychrometric-errors.tex
@@ -0,0 +1,43 @@
+\section{Psychrometric Errors}\label{psychrometric-errors}
+
+EnergyPlus has built-in psychrometric routines that perform various calculations for the simulation modules. They typically fall into the recurring error category but may warrant some view:
+
+\begin{lstlisting}
+   ** Warning ** Calculated Relative Humidity out of range (PsyRhFnTdbWPb)
+\end{lstlisting}
+
+\begin{lstlisting}
+   **   ~~~   **  Routine = NodeReportingCalc:NODE_1, Environment = CHICAGO_IL_USA ANNUAL COOLING 1% DESIGN CONDITIONS DB/MCWB, at Simulation time = 07/21 00:00 - 00:10
+\end{lstlisting}
+
+\begin{lstlisting}
+   **   ~~~   **  Dry-Bulb = 13.00 Humidity Ratio = 1.000E-002 Calculated Relative Humidity [%] = 104.65
+\end{lstlisting}
+
+\begin{lstlisting}
+   **   ~~~   ** Relative Humidity being reset to 100.0%
+\end{lstlisting}
+
+This warning notes that the calculated relative humidity is out of rage (routine name: PsyRhFnTdbWPb). It happened during routine NodeReportingCalc for NODE\_1 at the environment ``CHICAGO\_IL\_USA ANNUAL COOLING 1\% DESIGN CONDITIONS DB/MCWB'' during the time interval 00:00 -- 00:10 on July 21. The dry bulb temperature was 13 C, the humidity ratio was .001 for a calculated relative humidity of 104.65\%. It is reset to 100\%.
+
+Then, at the end of the run, you will see a summary of how many times that occur and the min/max extent:
+
+\begin{lstlisting}
+   *************  ** Warning ** Calculated Relative Humidity out of range (PsyRhFnTdbWPb)
+\end{lstlisting}
+
+\begin{lstlisting}
+   *************  **   ~~~   **   This error occurred 645 total times;
+\end{lstlisting}
+
+\begin{lstlisting}
+   *************  **   ~~~   **   during Warmup 0 times;
+\end{lstlisting}
+
+\begin{lstlisting}
+   *************  **   ~~~   **   during Sizing 0 times.
+\end{lstlisting}
+
+\begin{lstlisting}
+   *************  **   ~~~   **   Max = 104.652877 %  Min = 104.652877 %
+\end{lstlisting}
diff --git a/doc/tips-and-tricks-using-energyplus/src/error-messages-details/recurring-errors.tex b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/recurring-errors.tex
new file mode 100644
index 00000000000..737af6ab2e0
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/recurring-errors.tex
@@ -0,0 +1,26 @@
+\section{Recurring Errors}\label{recurring-errors}
+
+The recurring error category is employed during the actual simulation periods. Usually, a heading message will appear:
+
+\begin{lstlisting}
+   ** Warning ** Coil:Cooling:DX:SingleSpeed "DXCOOLINGCOIL_SOUTHZONE_2NDFLOOR" - Full load outlet air dry-bulb temperature < 2C. This indicates the possibility of coil frost/freeze. Outlet temperature = -4.60 C.
+   **   ~~~   **  ...Occurrence info = Washington Dc Dulles IntL Ar VA USA TMY3 WMO# = 724030, 01/02 06:01 - 06:02
+   **   ~~~   ** ... Possible reasons for low outlet air dry-bulb temperatures are: This DX coil
+   **   ~~~   **    1) may have a low inlet air dry-bulb temperature. Inlet air temperature = 9.778 C.
+   **   ~~~   **    2) may have a low air flow rate per watt of cooling capacity. Check inputs.
+   **   ~~~   **    3) is used as part of a HX assisted cooling coil which uses a high sensible effectiveness. Check inputs.
+\end{lstlisting}
+
+This message contains quite a bit of information: the basic object and name of the object, the context of the error, the time of the error as well as some reasons why this might have occurred.
+
+At the end of the simulation, the summary appears:
+
+\begin{lstlisting}
+   *************  ** Warning ** Coil:Cooling:DX:SingleSpeed "DXCOOLINGCOIL_SOUTHZONE_2NDFLOOR" - Full load outlet temperature indicates a possibility of frost/freeze error continues. Outlet air temperature statistics follow:
+   *************  **   ~~~   **   This error occurred 1240 total times;
+   *************  **   ~~~   **   during Warmup 0 times;
+   *************  **   ~~~   **   during Sizing 0 times.
+   *************  **   ~~~   **   Max = 1.995912  Min = -4.60024
+\end{lstlisting}
+
+Here you see a summary of how many times the error occurred (1240) as well as how many times during Warmup (0) and how many times during Sizing (0). Plus a minimum (-4.6) and maximum (1.99) for the terms of the message.
diff --git a/doc/tips-and-tricks-using-energyplus/src/error-messages-details/standard-error-message-format.tex b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/standard-error-message-format.tex
new file mode 100644
index 00000000000..b53aa396437
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/standard-error-message-format.tex
@@ -0,0 +1,23 @@
+\section{Standard Error Message Format}\label{standard-error-message-format}
+
+Standard error message format changes depending on where the error message is coming from. The standard error message format for GetInput goes something like this:
+
+\textless{}modulename\textgreater{}\textless{}routine name\textgreater{}: \textless{}object name\textgreater{} = \textless{}name field\textgreater{} ``condition''
+
+\textless{}several lines with more information may follow\textgreater{}
+
+The \textless{}modulename\textgreater{}(optional) \textless{}routinename\textgreater{} part is so that people answering support questions can more easily find the code, if necessary and without running the input file through the debugger.
+
+As noted elsewhere, errors come in several flavors with typical user responses required.
+
+In the examples for this section, the severity (Warning/Severe/Fatal) will be left off the message unless necessary for the rest of the example. For example:
+
+\textbf{GetPlantLoopData/GetPlantAvailabilityManager:} AvailabilityManagerAssignmentList = ALWAYS\_ON not found in lists.~ No availability will be used.
+
+Here the routine GetPlantLoopData/GetPlantAvailabilityManager for object AvailabilityManagerAssignmentList with name Always\_On is not found. And then the result is shown.~ (This is a warning level error, by the way).
+
+The development team is working to standardize the error format, as time allows. So, sometimes you will likely see something like:
+
+Check input. Pump nominal power or motor efficiency is set to 0, for pump = HEAT RECOVERY CIRC PUMP
+
+Here, at least you know which pump (Heat Recovery Circ Pump) has the power or motor efficiency of 0.
diff --git a/doc/tips-and-tricks-using-energyplus/src/error-messages-details/summaries-at-end-of-simulation.tex b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/summaries-at-end-of-simulation.tex
new file mode 100644
index 00000000000..45ff725037e
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/error-messages-details/summaries-at-end-of-simulation.tex
@@ -0,0 +1,23 @@
+\section{Summaries at End of Simulation}\label{summaries-at-end-of-simulation}
+
+Some classes of warnings produce more information at the end of the simulation. For example,
+
+\begin{lstlisting}
+Loads Initialization did not Converge (CheckWarmupConvergence) after 25 warmup days.
+Environment = SAN_FRANCISCO ANN CLG 1% CONDNS DB = >MWB
+Max Temp Comparison = 9.15E-002 vs Temperature Convergence Tolerance = 4.00E-003 - Fail Convergence
+Min Temp Comparison = 1.75E-003 vs Temperature Convergence Tolerance = 4.00E-003 - Pass Convergence
+Max Cool Load Comparison = 2.9010E-002 vs Loads Convergence Tolerance = 4.00E-002 - Pass Convergence
+Then, at the end of the simulation, you will see:
+******** The following error categories occurred.  Consider correcting or noting.
+******** Loads Initialization did not Converge
+******** ..1) very high thermal mass such as very thick concrete (solution: increase max number of warmup
+******** ..   days in the BUILDING object);
+******** ..2) moderate mass and inadequate space conditioning such that the building keeps getting warmer
+******** ..   and warmer on successive days (solution: add HVAC, check building thermal properties,
+******** ..   check if infiltration is included, make sure HVAC properly controlled);
+******** ..3) a soil layer modeled below the concrete slab - (solution remove this layer and read about
+******** ..   ground temperatures in the Auxiliary Programs document).
+******** ..4) unreasonable (too small) limits in the BUILDING object for temperature (.4 default) or
+******** ..   loads tolerances (.04 default)
+\end{lstlisting}
diff --git a/doc/tips-and-tricks-using-energyplus/src/errors-and-warnings.tex b/doc/tips-and-tricks-using-energyplus/src/errors-and-warnings.tex
new file mode 100644
index 00000000000..bd78e791b76
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/errors-and-warnings.tex
@@ -0,0 +1 @@
+\chapter{Errors and Warnings}\label{errors-and-warnings}
diff --git a/doc/tips-and-tricks-using-energyplus/src/errors-and-warnings/max-iterations-exceeded.tex b/doc/tips-and-tricks-using-energyplus/src/errors-and-warnings/max-iterations-exceeded.tex
new file mode 100644
index 00000000000..efb28d6e0a7
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/errors-and-warnings/max-iterations-exceeded.tex
@@ -0,0 +1,21 @@
+\section{Max iterations exceeded}\label{max-iterations-exceeded}
+
+\emph{I get the ``Max Iteration'' warning often, in varying quantities. I'd like to understand better what they mean.~}
+
+\emph{1) If these are a concern, at what frequency? (e.g., ``whenever it occurs more than 100? 500? 1000? times in a full year run.'')}
+
+\emph{2) Roughly how much does it affect accuracy of the simulation? (A lot or a little? proportional to the number of occurrences?)}
+
+\emph{3) Any tips about how to avoid it?}
+
+This is a good question, but it is difficult to answer.~ It is something to be concerned about, but in many cases there does not seem to be a way to completely eliminate them and they aren't necessarily a cause for alarm.
+
+\begin{enumerate}
+\def\labelenumi{\arabic{enumi})}
+\item
+  The total count is a difficult measure to use because it varies with number of zones, number and type of air systems, and length of run period.~ A 1,000 might not be a problem for a big model with an annual run, but it could be way too many for a single zone design day run.~ The errors are more common with VAV than CV. The frequency is key though.~ I look at the timing of the errors. If they happen every time step during some period, then it usually means there is something wrong with HVAC.~ If they happen only sometimes, and those times are when things are changing quickly (like recovery from setback), then I don't worry much.
+\item
+  It depends if the system is succeeding at controlling the zone conditions.~ If the systems are controlling well, and the errors are intermittent, then the results are probably not affected significantly.~ If the systems are not controlling zone conditions, then the errors are probably very significant.~ Check the comfort conditions and zone air temperatures to see.
+\item
+  When the errors are significant, they usually indicate something is wrong with HVAC input that EnergyPlus isn't able to trap in some other way.~ Possibilities include all sorts of things that can go wrong such as:~ systems connected wrong (node connections usually), sized wrong (mixing hard and auto sizes), controlled wrong (check operation of set point managers by reporting node set point values).
+\end{enumerate}
diff --git a/doc/tips-and-tricks-using-energyplus/src/general.tex b/doc/tips-and-tricks-using-energyplus/src/general.tex
new file mode 100644
index 00000000000..1bb12fa4e87
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/general.tex
@@ -0,0 +1 @@
+\chapter{General}\label{general}
diff --git a/doc/tips-and-tricks-using-energyplus/src/general/comparing-energyplus-to-other-programs.tex b/doc/tips-and-tricks-using-energyplus/src/general/comparing-energyplus-to-other-programs.tex
new file mode 100644
index 00000000000..b781fbc6cb8
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/general/comparing-energyplus-to-other-programs.tex
@@ -0,0 +1,15 @@
+\section{Comparing EnergyPlus to Other Programs}\label{comparing-energyplus-to-other-programs}
+
+A paper comparing and contrasting Energy Simulation Programs can be found here:
+
+http://www.eere.energy.gov/buildings/tools\_directory/pdfs/contrasting\_the\_capabilities\_of\_building\_energy\_performance\_simulation\_programs\_v1.0.pdf
+
+As this paper was published in 2005, it is out of date (at least with current EnergyPlus capabilities).
+
+The feature highlights from EnergyPlus releases can be seen here:
+
+http://apps1.eere.energy.gov/buildings/energyplus/pdfs/featurehighlights.pdf
+
+In addition you can see how EnergyPlus compares to other programs (which have submitted their models) in our testing reports:
+
+http://apps1.eere.energy.gov/buildings/energyplus/testing.cfm
diff --git a/doc/tips-and-tricks-using-energyplus/src/general/getting-started.tex b/doc/tips-and-tricks-using-energyplus/src/general/getting-started.tex
new file mode 100644
index 00000000000..a8d4ccf33d1
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/general/getting-started.tex
@@ -0,0 +1,7 @@
+\section{Getting Started}\label{getting-started}
+
+If you're familiar with building simulation, use the 300+ example files that come with the program and the Input/Output Reference to help you.
+
+If you're new to building simulation, read and work through the tutorials in the ``Getting Started'' document or visit the online tutorial, http://www.vibyor.com (tutorial was created by Prof.~Vishal Garg from IIIT Hyberabad, India).
+
+Another avenue you might use is the EnergyPlus Example File Generator (EEFG) program, which will not only produce an input file for your later use, but also run your specifications on EnergyPlus and send you the results. EEFG is available through the interface page referenced above or http://apps1.eere.energy.gov/buildings/energyplus/cfm/inputs/
diff --git a/doc/tips-and-tricks-using-energyplus/src/general/what-energyplus-is.tex b/doc/tips-and-tricks-using-energyplus/src/general/what-energyplus-is.tex
new file mode 100644
index 00000000000..333dacddf41
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/general/what-energyplus-is.tex
@@ -0,0 +1,7 @@
+\section{What EnergyPlus Is}\label{what-energyplus-is}
+
+The primary website for EnergyPlus is http://www.energyplus.gov
+
+EnergyPlus is an energy analysis and thermal load simulation program. Based on a user's description of a building from the perspective of the building's physical make-up, associated mechanical systems, etc., EnergyPlus will calculate the heating and cooling loads necessary to maintain thermal control set points, conditions throughout a secondary HVAC system and coil loads, and the energy consumption of primary plant equipment as well as many other simulation details that are necessary to verify that the simulation is performing as the actual building would. More details on what EnergyPlus is can be found in the \href{file:///E:/Docs4PDFs/GettingStarted.pdf}{GettingStarted Document}.
+
+No program is able to handle every simulation situation. However, it is the intent of EnergyPlus to handle as many building and HVAC design options either directly or indirectly through links to other programs in order to calculate thermal loads and/or energy consumption on for a design day or an extended period of time (up to, including, and beyond a year).
diff --git a/doc/tips-and-tricks-using-energyplus/src/general/what-energyplus-isn-t.tex b/doc/tips-and-tricks-using-energyplus/src/general/what-energyplus-isn-t.tex
new file mode 100644
index 00000000000..8777b5eca11
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/general/what-energyplus-isn-t.tex
@@ -0,0 +1,16 @@
+\section{What EnergyPlus Isn't}\label{what-energyplus-isnt}
+
+\begin{itemize}
+\tightlist
+\item
+  a user interface. It is intended to be the simulation engine around which a third-party interface can be wrapped. Inputs and outputs are simple ASCII text that is decipherable but may be best left to a GUI (graphical user interface). The current known third-party interfaces/tools can be found at
+\end{itemize}
+
+http://apps1.eere.energy.gov/buildings/energyplus/interfaces\_tools.cfm
+
+\begin{itemize}
+\item
+  a life cycle cost analysis tool. It produces results that can then be fed into an LCC program.
+\item
+  an architect or design engineer replacement. It does not check input, verify the acceptability or range of various parameters (expect for a limited number of very basic checks), or attempt to interpret the results. However, it does have several reporting features to help you do exactly that.
+\end{itemize}
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls.tex
new file mode 100644
index 00000000000..f4bd8fbd00e
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls.tex
@@ -0,0 +1 @@
+\chapter{HVAC, Sizing, Equipment Simulation and Controls}\label{hvac-sizing-equipment-simulation-and-controls}
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/boiler-control-schedule.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/boiler-control-schedule.tex
new file mode 100644
index 00000000000..2db4e923f8b
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/boiler-control-schedule.tex
@@ -0,0 +1,9 @@
+\section{Boiler Control Schedule}\label{boiler-control-schedule}
+
+\emph{How can I get my boiler to only work when the outdoor temperature is less than 5°C?}
+
+To schedule the boiler to work only when the outdoor dry bulb temperature is below 5°C, create two schedules based on the temperatures in the weather file. You can do this by reporting Outdoor Dry Bulb hourly, then make a spreadsheet with two columns, one which = 1 whenever ODB≥5, and the other which = 1 whenever ODB \textless{} 5. Save this spreadsheet as a csv format file, and then you can use Schedule:File to read these as EnergyPlus schedules. Use these schedules in the PlantEquipmentOperationSchemes object to make ``boiler heating'' active in cold weather and ``heatpump Heating'' active in warmer weather.
+
+Note that you will need to have two PlantEquipmentList objects, one which lists only the boiler, and the other which lists only the heat pump. And the two different PlantEquipmentOperation:HeatingLoad objects should reference different PlantEquipmentList objects.
+
+Report temperatures and flow rates at selected points on the hot water loop to see if things are working properly.
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/difference-between-eir-and-reformulated-eir.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/difference-between-eir-and-reformulated-eir.tex
new file mode 100644
index 00000000000..faf4ec3927e
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/difference-between-eir-and-reformulated-eir.tex
@@ -0,0 +1,7 @@
+\section{Difference between EIR and Reformulated EIR Chillers}\label{difference-between-eir-and-reformulated-eir-chillers}
+
+\emph{What is the difference between the EIR and ReformulatedEIR models of Electric Chillers?~ I am getting strange results.}
+
+The COP of a chiller is a function of part load ratio. It is mainly determined by the Energy Input to Cooling Output Ratio Function of Part Load Ratio Curve.~ When the EIR model is used for an electric chiller, the curve has an independent variable: part load ratio.~ For the ReformulatedEIR model, the curve requires two independent variables: leaving condenser water temperature and part load ratio.~ Each independent variable has its min and max values. If a variable is outside the allowed range, the nearest allowed value is used, possibly resulting in an unexpected result.
+
+If you would like to compare COP values for two types of chillers, you may need to ensure that the same conditions are applied. For simplicity, you may want to use a spreadsheet to calculate the curve values.
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/fan-types.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/fan-types.tex
new file mode 100644
index 00000000000..ba9ea8b60f9
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/fan-types.tex
@@ -0,0 +1,13 @@
+\section{Fan Types}\label{fan-types}
+
+\emph{I am confused about the differences between the different fan types.~ Can you explain?}
+
+In short:
+
+Fan:ConstantVolume is a constant volume, continuous operation fan which can be turned on and off via a schedule.
+
+Fan:OnOff is similar to the one above, but it cycles itself on and off as required by its thermostat \ldots{} all during the scheduled operation period. This is a typical mode of operation for a home furnace.
+
+Fan:VariableVolume runs continuously during the Schedule period, but varies its volume to meet the heating or cooling demand.
+
+Consult the \href{file:///E:/Docs4PDFs/InputOutputReference.pdf}{Input Output Reference document} (group Fans) for additional information.
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-availability-schedules.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-availability-schedules.tex
new file mode 100644
index 00000000000..6b5dd27037a
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-availability-schedules.tex
@@ -0,0 +1,5 @@
+\section{HVAC Availability Schedules}\label{hvac-availability-schedules}
+
+\emph{How do availability schedules work?}
+
+Apply the availability schedule to the HVAC System (i.e., Furnace or DXSystem), the coils and the fan objects. If compact HVAC objects are used, apply the availability schedule to the compact HVAC object. You will get different results depending on the selection for the night cycle option.
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-sizing-tips.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-sizing-tips.tex
new file mode 100644
index 00000000000..20896f13251
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-sizing-tips.tex
@@ -0,0 +1,16 @@
+\section{HVAC Sizing Tips}\label{hvac-sizing-tips}
+
+To help achieve successful autosizing of HVAC equipment, note the following general guidelines.
+
+\begin{itemize}
+\item
+  Begin with everything fully autosized (no user-specified values) and get a working system before trying to control any specific sized.
+\item
+  The user must coordinate system controls with sizing inputs. For example, if the Sizing:System ``Central Cooling Design Supply Air Temperature'' is set to 13C, the user must make sure that the setpoint manager for the central cooling coil controls to 13C as design conditions. EnergyPlus does not cross-check these inputs. The sizing calculations use the information in the Sizing:* objects. The simulation uses the information in controllers and setpoint managers.
+\item
+  User-specified flow rates will only impact the sizing calculations if entered in the Sizing:Zone or Sizing:System objects. Sizing information flows only from the sizing objects to the components. The sizing calculations have no knowledge of user-specified values in a component. The only exception to this rule is that plant loop sizing will collect all component design water flow rates whether autosized or user-specified.
+\item
+  The zone thermostat schedules determine the times at which design loads will be calculated. All zone-level schedules (such as lights, electric equipment, infiltration) are active during the sizing calculations (using the day type specified for the sizing period). System and plant schedules (such as availability managers and component schedules) are unknown to the sizing calculations. To exclude certain times of day from the sizing load calculations, use the thermostat setpoint schedules for SummerDesignDay and/or WinterDesignDay. For example, setting the cooling setpoint schedule to 99C during nighttime hours for the SummerDesignDay day type will turn off cooling during those hours.
+\end{itemize}
+
+For more information, read the Input Output Reference section on ``Input for Design Calculations and Component Autosizing.''
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-system-turn-off.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-system-turn-off.tex
new file mode 100644
index 00000000000..0936b3e7ec2
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-system-turn-off.tex
@@ -0,0 +1,5 @@
+\section{HVAC System Turn Off}\label{hvac-system-turn-off}
+
+\emph{My HVAC system won't turn off even when my availability schedule is 0 (off).}
+
+The night cycle option is set to Cycle On Any in the HVACTemplate:System:Unitary object. This will turn on the AC system. Change the night cycle option to Stay Off and the system shuts down correctly. For future reference, an indicator of night cycle operation is the on one time step, off the next type of operation.
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-system-types.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-system-types.tex
new file mode 100644
index 00000000000..a1e7632fc81
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/hvac-system-types.tex
@@ -0,0 +1,479 @@
+\section{HVAC System Types}\label{hvac-system-types}
+
+\emph{What kind of systems are available in EnergyPlus?}
+
+EnergyPlus HVAC systems input is flexible, so many different types of systems can be built using the basic available components. There are also compound components which represent common equipment types, and HVACTemplate systems which simplify the input for specific systems. This list gives an overview of HVAC objects in EnergyPlus:
+
+HVAC Templates
+
+\begin{itemize}
+\tightlist
+\item
+  HVACTemplate:Thermostat
+\item
+  HVACTemplate:Zone:IdealLoadsAirSystem
+\item
+  HVACTemplate:Zone:FanCoil
+\item
+  HVACTemplate:Zone:PTAC
+\item
+  HVACTemplate:Zone:PTHP
+\item
+  HVACTemplate:Zone:Unitary
+\item
+  HVACTemplate:Zone:VAV
+\item
+  HVACTemplate:Zone:VAV:FanPowered
+\item
+  HVACTemplate:Zone:WaterToAirHeatPump
+\item
+  HVACTemplate:System:Unitary
+\item
+  HVACTemplate:System:Unitary:AirToAir
+\item
+  HVACTemplate:System:VAV
+\item
+  HVACTemplate:System:PackagedVAV
+\item
+  HVACTemplate:System:DedicatedOutdoorAir
+\item
+  HVACTemplate:Plant:ChilledWaterLoop
+\item
+  HVACTemplate:Plant:Chiller
+\item
+  HVACTemplate:Plant:Tower
+\item
+  HVACTemplate:Plant:HotWaterLoop
+\item
+  HVACTemplate:Plant:Boiler
+\item
+  HVACTemplate:Plant:MixedWaterLoop
+\end{itemize}
+
+Zone HVAC Forced Air Units
+
+\begin{itemize}
+\tightlist
+\item
+  ZoneHVAC:IdealLoadsAirSystem
+\item
+  ZoneHVAC:FourPipeFanCoil
+\item
+  ZoneHVAC:WindowAirConditioner
+\item
+  ZoneHVAC:PackagedTerminalAirConditioner
+\item
+  ZoneHVAC:PackagedTerminalHeatPump
+\item
+  ZoneHVAC:WaterToAirHeatPump
+\item
+  ZoneHVAC:Dehumidified:DX
+\item
+  ZoneHVAC:EnergyRecoveryVentilator
+\item
+  ZoneHVAC:EnergyRecoveryVentilator:Controller
+\item
+  ZoneHVAC:UnitVentilator
+\item
+  ZoneHVAC:UnitHeater
+\item
+  ZoneHVAC:OutdoorAirUnit
+\item
+  ZoneHVAC:TerminalUnit:VariableRefrigerantFlow
+\end{itemize}
+
+Zone HVAC Radiative/Convective Units
+
+\begin{itemize}
+\tightlist
+\item
+  ZoneHVAC:Baseboard:RadiantConvective:Water
+\item
+  ZoneHVAC:Baseboard:RadiantConvective:Steam
+\item
+  ZoneHVAC:Baseboard:RadiantConvective:Electric
+\item
+  ZoneHVAC:Baseboard:Convective:Water
+\item
+  ZoneHVAC:Baseboard:Convective:Electric
+\item
+  ZoneHVAC:LowTemperatureRadiant:VariableFlow
+\item
+  ZoneHVAC:LowTemperatureRadiant:ConstantFlow
+\item
+  ZoneHVAC:LowTemperatureRadiant:Electric
+\item
+  ZoneHVAC:HighTemperatureRadiant
+\item
+  ZoneHVAC:VentilatedSlab
+\end{itemize}
+
+Zone HVAC Air Loop Terminal Units
+
+\begin{itemize}
+\tightlist
+\item
+  AirTerminal:SingleDuct:Uncontrolled
+\item
+  AirTerminal:SingleDuct:ConstantVolume:Reheat
+\item
+  AirTerminal:SingleDuct:VAV:NoReheat
+\item
+  AirTerminal:SingleDuct:VAV:Reheat
+\item
+  AirTerminal:SingleDuct:VAV:Reheat:VariableSpeedFan
+\item
+  AirTerminal:SingleDuct:VAV:HeatAndCool:NoReheat
+\item
+  AirTerminal:SingleDuct:VAV:HeatAndCool:Reheat
+\item
+  AirTerminal:SingleDuct:SeriesPIU:Reheat
+\item
+  AirTerminal:SingleDuct:ParallelPIU:Reheat
+\item
+  AirTerminal:SingleDuct:ConstantVolume:FourPipeInduction
+\item
+  AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam
+\item
+  AirTerminal:SingleDuct:ConstantVolume:CooledBeam
+\item
+  AirTerminal:DualDuct:ConstantVolume
+\item
+  AirTerminal:DualDuct:VAV
+\item
+  AirTerminal:DualDuct:VAV:OutdoorAir
+\item
+  ZoneHVAC:AirDistributionUnit
+\end{itemize}
+
+Fans
+
+\begin{itemize}
+\tightlist
+\item
+  Fan:ConstantVolume
+\item
+  Fan:VariableVolume
+\item
+  Fan:OnOff
+\item
+  Fan:ZoneExhaust
+\item
+  FanPerformance:NightVentilation
+\item
+  Fan:ComponentModel
+\end{itemize}
+
+Coils
+
+\begin{itemize}
+\tightlist
+\item
+  Coil:Cooling:Water
+\item
+  Coil:Cooling:Water:DetailedGeometry
+\item
+  Coil:Cooling:DX:SingleSpeed
+\item
+  Coil:Cooling:DX:TwoSpeed
+\item
+  Coil:Cooling:DX:MultiSpeed
+\item
+  Coil:Cooling:DX:TwoStageWithHumidityControlMode
+\item
+  CoilPerformance:DX:Cooling
+\item
+  Coil:Cooling:DX:VariableRefrigerantFlow
+\item
+  Coil:Heating:DX:VariableRefrigerantFlow
+\item
+  Coil:Heating:Water
+\item
+  Coil:Heating:Steam
+\item
+  Coil:Heating:Electric
+\item
+  Coil:Heating:Gas
+\item
+  Coil:Heating:Desuperheater
+\item
+  Coil:Heating:DX:SingleSpeed
+\item
+  Coil:Heating:DX:MultiSpeed
+\item
+  Coil:Cooling:WaterToAirHeatPump:ParameterEstimation
+\item
+  Coil:Heating:WaterToAirHeatPump:ParameterEstimation
+\item
+  Coil:Cooling:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Cooling:WaterToAirHeatPump:VariableSpeedEquationFit
+\item
+  Coil:Heating:WaterToAirHeatPump:EquationFit
+\item
+  Coil:Heating:WaterToAirHeatPump:VariableSpeedEquationFit
+\item
+  Coil:WaterHeating:AirToWaterHeatPump
+\item
+  Coil:WaterHeating:Desuperheater
+\item
+  CoilSystem:Cooling:DX
+\item
+  CoilSystem:Heating:DX
+\item
+  CoilSystem:Cooling:Water:HeatExchangerAssisted
+\item
+  CoilSystem:Cooling:DX:HeatExchangerAssisted
+\end{itemize}
+
+Evaporative Coolers
+
+\begin{itemize}
+\tightlist
+\item
+  EvaporativeCooler:Direct:CelDekPad
+\item
+  EvaporativeCooler:Indirect:CelDekPad
+\item
+  EvaporativeCooler:Indirect:WetCoil
+\item
+  EvaporativeCooler:Indirect:ResearchSpecial
+\end{itemize}
+
+Humidifiers and Dehumidifiers
+
+\begin{itemize}
+\tightlist
+\item
+  Humidifier:Steam:Electric
+\item
+  Dehumidifier:Desiccant:NoFans
+\item
+  Dehumidifier:Desiccant:System
+\end{itemize}
+
+Heat Recovery
+
+\begin{itemize}
+\tightlist
+\item
+  HeatExchanger:AirToAir:FlatPlate
+\item
+  HeatExchanger:AirToAir:SensibleAndLatent
+\item
+  HeatExchanger:Desiccant:BalancedFlow
+\item
+  HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1
+\end{itemize}
+
+Unitary Equipment
+
+\begin{itemize}
+\tightlist
+\item
+  AirLoopHVAC:Unitary:Furnace:HeatOnly
+\item
+  AirLoopHVAC:Unitary:Furnace:HeatCool
+\item
+  AirLoopHVAC:UnitaryHeatOnly
+\item
+  AirLoopHVAC:UnitaryHeatCool
+\item
+  AirLoopHVAC:UnitaryHeatPump:AirToAir
+\item
+  AirLoopHVAC:UnitaryHeatPump:WaterToAir
+\item
+  AirLoopHVAC:UnitaryHeatCool:VAVChangeoverBypass
+\item
+  AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed
+\end{itemize}
+
+Variable Refrigerant Flow Equipment
+
+\begin{itemize}
+\tightlist
+\item
+  AirConditioner:VariableRefrigerantFlow
+\end{itemize}
+
+Air Distribution
+
+\begin{itemize}
+\tightlist
+\item
+  AirLoopHVAC
+\item
+  AirLoopHVAC:OutdoorAirSystem:EquipmentList
+\item
+  AirLoopHVAC:OutdoorAirSystem
+\item
+  OutdoorAir:Mixer
+\item
+  AirLoopHVAC:ZoneSplitter
+\item
+  AirLoopHVAC:SupplyPlenum
+\item
+  AirLoopHVAC:SupplyPath
+\item
+  AirLoopHVAC:ZoneMixer
+\item
+  AirLoopHVAC:ReturnPlenum
+\item
+  AirLoopHVAC:ReturnPath
+\end{itemize}
+
+Pumps
+
+\begin{itemize}
+\tightlist
+\item
+  Pump:VariableSpeed
+\item
+  Pump:ConstantSpeed
+\item
+  Pump:VariableSpeed:Condensate
+\item
+  HeaderedPumps:VariableSpeed
+\item
+  HeaderedPumps:ConstantSpeed
+\end{itemize}
+
+Solar Collectors
+
+\begin{itemize}
+\tightlist
+\item
+  SolarCollectorPerformance:FlatPlate
+\item
+  SolarCollector:FlatPlate:Water
+\item
+  SolarCollector:FlatPlate:PhotovoltaicThermal
+\item
+  SolarCollectorPerformance:PhotovoltaicThermal:Simple
+\item
+  SolarCollector:IntegralCollectorStorage
+\item
+  SolarCollectorPerformance:IntegralCollectorStorage
+\item
+  SolarCollector:UnglazedTranspired
+\item
+  SolarCollector:UnglazedTranspired:Multisystem
+\end{itemize}
+
+Plant Heating and Cooling Equipment
+
+\begin{itemize}
+\tightlist
+\item
+  Boiler:HotWater
+\item
+  Boiler:Steam
+\item
+  Chiller:Electric:EIR
+\item
+  Chiller:Electric:ReformulatedEIR
+\item
+  Chiller:Electric
+\item
+  Chiller:Absorption:Indirect
+\item
+  Chiller:Absorption
+\item
+  Chiller:ConstantCOP
+\item
+  Chiller:EngineDriven
+\item
+  Chiller:CombustionTurbine
+\item
+  ChillerHeater:Absorption:DirectFired
+\item
+  ChillerHeater:Absorption:DoubleEffect
+\item
+  HeatPump:WaterToWater:EquationFit:Heating
+\item
+  HeatPump:WaterToWater:EquationFit:Cooling
+\item
+  HeatPump:WaterToWater:ParameterEstimation:Cooling
+\item
+  HeatPump:WaterToWater:ParameterEstimation:Heating
+\item
+  DistrictCooling
+\item
+  DistrictHeating
+\end{itemize}
+
+Condenser Equipment and Heat Exchangers
+
+\begin{itemize}
+\tightlist
+\item
+  CoolingTower:SingleSpeed
+\item
+  CoolingTower:TwoSpeed
+\item
+  CoolingTower:VariableSpeed
+\item
+  CoolingTowerPerformance:CoolTools
+\item
+  CoolingTowerPerformance:YorkCalc
+\item
+  EvaporativeFluidCooler:SingleSpeed
+\item
+  EvaporativeFluidCooler:TwoSpeed
+\item
+  FluidCooler:SingleSpeed
+\item
+  FluidCooler:TwoSpeed
+\item
+  GroundHeatExchanger:Vertical
+\item
+  GroundHeatExchanger:Pond
+\item
+  GroundHeatExchanger:Surface
+\item
+  HeatExchanger:FluidToFluid
+\end{itemize}
+
+Water Heaters and Thermal Storage
+
+\begin{itemize}
+\tightlist
+\item
+  WaterHeater:Mixed
+\item
+  WaterHeater:Stratified
+\item
+  WaterHeater:Sizing
+\item
+  WaterHeater:HeatPump:PumpedCondenser
+\item
+  WaterHeater:HeatPump:WrappedCondenser
+\item
+  ThermalStorage:Ice:Simple
+\item
+  ThermalStorage:Ice:Detailed
+\item
+  ThermalStorage:ChilledWater:Mixed
+\item
+  ThermalStorage:ChilledWater:Stratified
+\end{itemize}
+
+Plant-Condenser Loops
+
+\begin{itemize}
+\tightlist
+\item
+  PlantLoop
+\item
+  CondenserLoop
+\item
+  Pipe:Adiabatic
+\item
+  Pipe:Adiabatic:Steam
+\item
+  Pipe:Indoor
+\item
+  Pipe:Outdoor
+\item
+  Pipe:Underground
+\end{itemize}
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/modeling-desiccant-dehumidifiers.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/modeling-desiccant-dehumidifiers.tex
new file mode 100644
index 00000000000..ac8d32d0828
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/modeling-desiccant-dehumidifiers.tex
@@ -0,0 +1,9 @@
+\section{Modeling Desiccant DeHumidifiers}\label{modeling-desiccant-dehumidifiers}
+
+\emph{How do I enter performance data for a desiccant dehumidifier?}
+
+It depends on which specific EnergyPlus object you are trying to use.
+
+The Dehumidifier:Desiccant:NoFans object has default performance curves within the model itself that you can use.~ Set field A12, ``Performance Model,'' to DEFAULT.~ Alternatively, you could also obtain manufacturer's data and develop your own curve fits, then set ``Performance Model'' to User Curves.~~ See the Input Output Reference for more details.
+
+If you want to use the Dehumidifier:Desiccant:System object, then some data set inputs for the required HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 object are contained in the file ``PerfCurves.idf'' in the DataSets folder.~ You could also obtain manufacturer's data and develop your own inputs for the HeatExchanger:Desiccant:BalancedFlow:PerformanceDataType1 object.
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/plant-load-profile.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/plant-load-profile.tex
new file mode 100644
index 00000000000..a28996b3228
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/plant-load-profile.tex
@@ -0,0 +1,3 @@
+\section{Plant Load Profile}\label{plant-load-profile}
+
+The Plant Load Profile object is used to ``pass'' a load to the plant where the plant meets this load. The load profile places an inlet and outlet water temperature and a mass flow rate at the inlet to the plant loop. This is where you will need to focus when you try to alter the boiler performance.
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/separating-ventilation-loads-v-zone-loads.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/separating-ventilation-loads-v-zone-loads.tex
new file mode 100644
index 00000000000..c36dbbd60dd
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/separating-ventilation-loads-v-zone-loads.tex
@@ -0,0 +1,50 @@
+\section{Separating Ventilation Loads v. Zone Loads}\label{separating-ventilation-loads-v.-zone-loads}
+
+\emph{Can I determine the ventilation load for PAU in PAU~ + FCUs system? If can, how to split the total cooling load into room load and ventilation load for PAU sizing in energyplus?}
+
+\emph{In the HTML report, ``Nominal total capacity {[}W{]}'' (EquipmentSummary) and ``Design Load {[}W{]}'' (HVACSizingSummary) can be found. Are they equal to ``Total cooling load'' and ``Room load''? (i.e.~Ventilation load = ``nominal total capacity'' - ``Design Load'')}
+
+PAU -- Primary Fresh Air Handling Unit or DOAS -- Dedicated Outdoor Air Unit
+
+FCU -- Fan Coil Unit
+
+There are several ways to split the total cooling load into room load and ventilation load for PAU sizing in EnergyPlus:
+
+1)~~~In the eio output, section, the heating and cooling loads reported there are the peak *sensible* loads for each zone, without any ventilation load. These are the same values reported as ``Design Load'' in the HVACSizingSummary table report.
+
+2)~~~In the EquipmentSummary table report, the component capacities reported there are the total (cooling, sensible for heating) output capacities include any ventilation load if it impacts that component.
+
+3)~~~If you have a central air loop that serves only the ventilation load, and zone equipment that serves only the zone load, there is an autosizing option in Sizing:System that should autosize the central system appropriately.
+
+From example file 5ZoneCoolBeam.idf:
+
+\begin{lstlisting}
+
+Sizing:System,
+  VAV Sys 1, !- AirLoop Name
+  VentilationRequirement, !- Type of Load to Size On
+  autosize, !- Design Outdoor Air Flow Rate {m3/s}
+  1.0, !- Minimum System Air Flow Ratio
+\end{lstlisting}
+
+When you run a simulation, if you want to report ventilation loads, the following Output:Variable names are available:
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Sum,Zone Mechanical Ventilation No Load Heat Removal {[}J{]}
+\item
+  HVAC,Sum,Zone Mechanical Ventilation Cooling Load Increase {[}J{]}
+\item
+  HVAC,Sum,Zone Mech Ventilation Cooling Load Increase: OverHeating {[}J{]}
+\item
+  HVAC,Sum,Zone Mechanical Ventilation Cooling Load Decrease {[}J{]}
+\item
+  HVAC,Sum,Zone Mechanical Ventilation No Load Heat Addition {[}J{]}
+\item
+  HVAC,Sum,Zone Mechanical Ventilation Heating Load Increase {[}J{]}
+\item
+  HVAC,Sum,Zone Mech Ventilation Heating Load Increase: OverCooling {[}J{]}
+\item
+  HVAC,Sum,Zone Mechanical Ventilation Heating Load Decrease {[}J{]}
+\end{itemize}
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/system-not-cooling.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/system-not-cooling.tex
new file mode 100644
index 00000000000..fa20aebe901
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/system-not-cooling.tex
@@ -0,0 +1,19 @@
+\section{System not Cooling}\label{system-not-cooling}
+
+\emph{I built a very simple system 5 zones VAV no reheat to understand how a E+ system is put together. The results show that the cooling coil is not seeing a load. I then build the same HVACTemplate system and made sure all the details are exactly the same. The template works but not my system.}
+
+It is much easier to use HVACTemplate objects to set up your system. All required supporting objects are set up for you. Notice in your 5Zone input file, you have specified AHU1CCController for BOTH cooling coil controller lists. The second controller list should use controller name AHU2CCController. The 5Zone file worked when I used the correct controller name.
+
+\begin{lstlisting}
+
+AirLoopHVAC:ControllerList,
+      AHU1SystemController,    !- Name
+      Controller:WaterCoil,       !- Controller Type 1
+      AHU1CCController;        !- Controller Name 1
+
+
+  AirLoopHVAC:ControllerList,
+      AHU2SystemController,    !- Name
+      Controller:WaterCoil,       !- Controller Type 1
+      AHU1CCController;        !- Controller Name 1
+\end{lstlisting}
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/use-of-set-point-managers.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/use-of-set-point-managers.tex
new file mode 100644
index 00000000000..e37f6cec541
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/use-of-set-point-managers.tex
@@ -0,0 +1,32 @@
+\section{Use of Set Point Managers}\label{use-of-set-point-managers}
+
+A coil will check its inlet air temperature compared to the set point temperature. For cooling, if the inlet air temperature is above the set point temp, the coil turns on. It's opposite that for heating. In the 5ZoneAutoDXVAV example file, a schedule temperature set point is placed at the system outlet node. This is the temperture the designer wants at the outlet. The mixed air SP manager is used to account for fan heat and places the required SP at the outlet of the cooling coil so the coil slightly overcools the air to overcome fan heat and meet the system outlet node set point.
+
+You don't blindly place the SP's at the coil outlet node, but this is a likely starting point in most cases. If there is a fan after the coil's, the ``actual'' SP will need to be placed on a different node (other than the coils). Then a mixed air manager will be used to reference that SP and the fan's inlet/outlet node to calculate the correct SP to place wherever you want (at the coil outlet, the mixed air node, etc.). Place it at the mixed air node if you want the outside air system to try and meet that setpoint through mixing. Place it at the cooling coil outlet if you want the coil control to account for fan heat. Place it at both locations if you want the outside air system to try and meet the load with the coil picking up the remainder of the load.
+
+See if the coils are fully on when the SP is not met. If they are the coils are too small. If they are at part-load, the control SP is calculated incorrectly.
+
+\subsection{Relationship of Set Point Managers and Controllers}\label{relationship-of-set-point-managers-and-controllers}
+
+\emph{Could you elaborate further on the relation between SetPoint managers and Controllers?}
+
+SetpointManager objects place a setpoint on a node, for example, one might place a setpoint of 12C on the node named ``Main Cooling Coil Air Outlet Node''.
+
+In the case of Controler:WaterCoil which controls a hot water or chilled water coil, the controller reads the setpoint and tries to adjust the water flow so that the air temperature at the controlled node matches the current setpoint.~ Continuing the example above:
+
+\begin{lstlisting}
+
+  Controller:WaterCoil,
+      Main Cooling Coil Controller,  !- Name
+      Temperature,                   !- Control variable
+      Reverse,                       !- Action
+      Flow,                          !- Actuator variable
+      Main Cooling Coil Air Outlet Node,   !- Control_Node
+      Main Cooling Coil Water Inlet Node,  !- Actuator_Node
+      0.002,                         !- Controller Convergence Tolerance:
+                                     !- delta temp from setpoint temp {deltaC}
+      autosize,                      !- Max Actuated Flow {m3/s}
+      0.0;                           !- Min Actuated Flow {m3/s}
+\end{lstlisting}
+
+It is possible to place the control node downstream of the actual object being controlled, for example after other coils and the supply fan, but I recommend using the coil leaving air node as the control node for tighter control.
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/using-well-water.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/using-well-water.tex
new file mode 100644
index 00000000000..651940130b1
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/using-well-water.tex
@@ -0,0 +1,5 @@
+\section{Using Well Water}\label{using-well-water}
+
+The water-to-water heat pumps have not been programmed to allow well water. However, cooling towers have (see 5ZoneWaterSystems.idf) and you should be able to connect the WSHP to a condenser loop with a cooling tower.
+
+Currently, there is no method to directly simulate well water as the condensing fluid for water source heat pumps. So to get as close as possible, program the cooling towers to allow well water via the water use object. If the cooling tower inlet node water temperature represents the well water temperature, and if you can set up the cooling tower to provide an outlet water temperature very close to the inlet water temperature, then this would be the same as connecting the well water directly to the WSHP. Minimize the cooling tower fan energy or disregard it completely when performing your simulation. Use report variables at the inlet/outlet node of the cooling tower to investigate how close you can get to your equipment configuration.
diff --git a/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/variable-refrigerant-flow-air-conditioner.tex b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/variable-refrigerant-flow-air-conditioner.tex
new file mode 100644
index 00000000000..3bdc610e20c
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/hvac-sizing-equipment-simulation-and-controls/variable-refrigerant-flow-air-conditioner.tex
@@ -0,0 +1,13 @@
+\section{Variable Refrigerant Flow Air Conditioner}\label{variable-refrigerant-flow-air-conditioner}
+
+\textbf{\emph{The EnergyPlus v7.0 release (October 2011) includes an initial model for VRF systems.~ See AirConditioner:VariableRefrigerantFlow and related objects.}}
+
+\emph{Can I model a VRV or VRF system in EnergyPlus?}
+
+Variable Refrigerant Flow (VRF, or Variable Refrigerant Volume - VRV) air conditioners are available in EnergyPlus V7 and later.
+
+Otherwise, the closest model available would be the multi-speed cooling and heating AC (AirLoopHVAC:UnitaryHeatPump:AirToAir:MultiSpeed used with Coil:Cooling:DX:Multispeed and Coil:Heating:DX:Multispeed coils). This model will provide information for cooling-only or heating-only operation (VRF heat pump mode).
+
+Others have attempted to simulate a VRF system with the existing VAV model. This model will only provide valid information when cooling is required. The results will only be as good as the DX cooling coil performance curves allow. The heating side of a VAV system does not use a DX compression system (i.e., uses gas or electric heat) so this part of the VRV system cannot be modeled with a VAV system.
+
+Note that using either of these models will not provide accurate results since each of these system types provides conditioned air to all zones served by the HVAC system. The VAV system terminal unit may be set to use a minimum flow of 0 where the resulting air flow to that zone is 0 when cooling is not required. Energy use in this case may be slightly more accurate.
diff --git a/doc/tips-and-tricks-using-energyplus/src/input.tex b/doc/tips-and-tricks-using-energyplus/src/input.tex
new file mode 100644
index 00000000000..afceeba6c68
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/input.tex
@@ -0,0 +1 @@
+\chapter{Input}\label{input}
diff --git a/doc/tips-and-tricks-using-energyplus/src/input/converting-older-version-energyplus-files.tex b/doc/tips-and-tricks-using-energyplus/src/input/converting-older-version-energyplus-files.tex
new file mode 100644
index 00000000000..70b2b9f6a55
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/input/converting-older-version-energyplus-files.tex
@@ -0,0 +1,13 @@
+\section{Converting Older Version EnergyPlus Files}\label{converting-older-version-energyplus-files}
+
+\emph{Can I convert an older file to a newer version of EnergyPlus?}
+
+If the older version is from the previous release, then yes. Use the pull-down File menu and select Transition. This will update the older file to the newer version.
+
+If the older version is older than the previous release, then you must use the multiple transition program. You can download the transition programs from this site.
+
+(That is http://energyplus.helpserve.com and go to the ``downloads'' area).
+
+The Multiple Transition folder is set up on the EnergyPlus install.
+
+Unzip the file into the MultipleTransition folder and use the IDF Converter GUI program to transition your older files. The IDF converter can also save the transitioned file for each intermediate version, if desired.
diff --git a/doc/tips-and-tricks-using-energyplus/src/input/creating-files-for-energyplus.tex b/doc/tips-and-tricks-using-energyplus/src/input/creating-files-for-energyplus.tex
new file mode 100644
index 00000000000..ba33af92439
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/input/creating-files-for-energyplus.tex
@@ -0,0 +1,19 @@
+\section{Creating Files for EnergyPlus}\label{creating-files-for-energyplus}
+
+The install package includes the IDF Editor (Windows platform) for creating EnergyPlus Input Files (aka IDFs). Likewise, text editors such as NotePad or WordPad can be used to create flat ASCII files for use with EnergyPlus.
+
+\subsection{dxf or dwg CAD Files}\label{dxf-or-dwg-cad-files}
+
+\emph{How can I convert dxf or dwg CAD files to EnergyPlus?}
+
+Several EnergyPlus interfaces, including DesignBuilder and OpenStudio (plug in for Google SketchUp), allow you to import the dxf drawings and trace over them to create EnergyPlus geometry. If you have the full AutoCAD 3-D dwg model (more than just dxf), then you might be able to export to EnergyPlus using one of the available utilities that work with AutoCAD, but only if the model was created in the correct way to support these tools. As of February 2009, Green Building Studio and EnergyPlugged (a plug in to AutoCAD) support export to EnergyPlus.
+
+For more information about current tools which support EnergyPlus, see http://www.energyplus.gov/interfaces\_tools.cfm.
+
+\subsection{OpenStudio for Google Sketchup}\label{openstudio-for-google-sketchup}
+
+\href{http://apps1.eere.energy.gov/buildings/energyplus/openstudio.cfm}{OpenStudio} is a free plugin for the Google SketchUp 3D drawing program. The plugin makes it easy to create and edit the building geometry in your EnergyPlus input files. The plugin also allows you to launch EnergyPlus simulations and view the results without leaving SketchUp.
+
+\subsection{EnergyPlus Example File Generator}\label{energyplus-example-file-generator}
+
+A Web-based service is available that creates and runs EnergyPlus input files for simple models of commercial buildings. The input files (and annual results summary files) are sent to your e-mail address as attachments. You can access the service and customize the characteristics of the building you want to model on the \href{http://apps1.eere.energy.gov/buildings/energyplus/cfm/inputs/}{EnergyPlus Example File Generator Application} (pop-ups must be enabled). Learn more by viewing the \href{http://apps1.eere.energy.gov/buildings/energyplus/cfm/inputs/help.cfm}{EnergyPlus Building Data Input Forms Help} File.
diff --git a/doc/tips-and-tricks-using-energyplus/src/input/getting-data-from-window-program.tex b/doc/tips-and-tricks-using-energyplus/src/input/getting-data-from-window-program.tex
new file mode 100644
index 00000000000..bac0a1fc1a3
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/input/getting-data-from-window-program.tex
@@ -0,0 +1,352 @@
+\section{Getting data from WINDOW program}\label{getting-data-from-window-program}
+
+The WINDOW program is published from LBNL at http://windows.lbl.gov/software. More specifics on the program and its details are shown in the Input Output Reference under ``Importing Windows from WINDOW program'' topic.
+
+\subsection{EnergyPlus IDF Excerpt Data}\label{energyplus-idf-excerpt-data}
+
+The preferred method of using WINDOW data in EnergyPlus is to excerpt or ``report'' a specific Window from the Window library screen (see below):
+
+\begin{figure}[hbtp] % fig 1
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image001.jpg}
+\caption{WINDOW screen for exporting IDF Window specifications \protect \label{fig:window-screen-for-exporting-idf-window}}
+\end{figure}
+
+The file can then be saved at a location of your choice and added into your overall simulation IDF file.
+
+\subsection{WINDOW Data File}\label{window-data-file}
+
+The other ``older'' option for creating data for EnergyPlus is to use the ``EnergyPlus'' option above and create a WindowDataFile. The general format of this data is described in the following paragraphs and must use the Construction:WindowDataFile object and an external file to be used in EnergyPlus. While this is a convenient small file (that can contain multiple windows), there is no way to import this file back into WINDOW and obtain the above, more preferred method.
+
+Please note that there is a bug in WINDOW 5 that causes two of the lines in the EnergyPlus data file to be joined. This bug is fixed in versions of Window 5.02 (and above). To be sure, you can check the data file for a line that looks like:
+
+GLAZING SYSTEM OPTICAL DATAAngle~~~~ 0~~~ 10~~~ 20~~~ 30~~~ 40~~~ 50~~~ 60~~~ 70~~~ 80~~~ 90 Hemis
+
+The fixed version of the program will not show the above line; rather, there will be two lines such as shown below. If you have the above condition, with an editor you would break this into two lines:
+
+GLAZING SYSTEM OPTICAL DATA
+
+Angle~~~~ 0~~~ 10~~~ 20~~~ 30~~~ 40~~~ 50~~~ 60~~~ 70~~~ 80~~~ 90 Hemis
+
+In EnergyPlus, the Window data file is searched for each ``Construction:WindowDataFile'' object in the EnergyPlus input. This object has a very simple form:
+
+Construction:WindowDataFile,
+
+ConstructionName,
+
+FileName; ! Default is Window5DataFile.dat in the ``run'' folder.
+
+If there is a window called ConstructionName on the Window data file, the data for that window is read from the file and the following EnergyPlus objects and their names are created. The ``W5'' prefixed to these names indicates that the object originated in the Window5 data file.
+
+\begin{itemize}
+\item
+  \textbf{WindowMaterial:Glazing} for each of the glass layers. They will be named \textbf{W5:ConstructionName:GLASS1}, \textbf{W5:ConstructionName:GLASS2} , etc.
+\item
+  \textbf{WindowMaterial:Gas} or \textbf{WindowMaterial:GasMixture} for each of the gap layers. They will be named \textbf{W5:ConstructionName:GAP1}, \textbf{W5:ConstructionName:GAP2} , etc.
+\item
+  \textbf{WindowProperty:FrameAndDivider} (if the window on the Window5 data file has a frame and/or divider). It will be named \textbf{W5:ConstructionName}. This WindowProperty:FrameAndDivider will be assigned to any window on the input file that has a construction called ``ConstructionName'' \emph{even if that window has~ referenced another WindowProperty:FrameAndDivider (i.e., if WindowProperty:FrameAndDivider Name for that window is specified).} In this case a warning will result.
+\end{itemize}
+
+Note that:
+
+An entry on the WINDOW data file usually has just one glazing system. It is also possible to have an entry with two glazing systems separated by a horizontal or vertical mullion. In this case, the two glazing systems can have different dimensions and different properties. For example, one of the two glazing systems could be single glazed and the other could be double glazed. An example~ of the two glazing system case is given in the sample WINDOW data file shown below (although in this case the properties of the two glazing systems are the same).
+
+EnergyPlus handles the ``one glazing system'' and ``two glazing systems'' cases differently. If there is one glazing system, the glazing system height and width from the Window5 data file are not used. Instead, the window dimensions are obtained from the window vertices that have been specified on the IDF file. However, a warning message will result if the height or width calculated from the window's vertex inputs differs from the corresponding Window5 data file values by more than 10\%. This warning is given since the effective frame and edge-of-glass conductances on the WINDOW data file can depend on the window dimensions if the frame is non-uniform, i.e., consists of sections with different values of width, projection, or thermal properties.
+
+If the WINDOW data file entry has two glazing systems, System1 and System2, the following happens, as shown in the figure below. Assume that the original window is called WinOriginal. System1 is assigned to WinOriginal. Then EnergyPlus automatically creates a second window, called WinOriginal:2, and assigns System2 to it. The dimensions of WinOriginal are ignored; the dimensions of System1 on the data file are assigned to it, but the position of the lower left-hand vertex of WinOriginal is retained. The dimensions of System2 on the data file are assigned to WinOriginal:2. The lower left-hand vertex of WinOriginal:2 is determined from the mullion orientation and width.
+
+\textbf{Note: WinOriginal would have been the IDF window definition -- it's dimensions will be overridden by the systems dimensions from the Window data file. Two windows will be made and called WinOriginal and WinOriginal:2.}
+
+\begin{figure}[hbtp] % fig 2
+\centering
+\includegraphics[width=0.9\textwidth, height=0.9\textheight, keepaspectratio=true]{media/image002.png}
+\caption{Window Glazing system with dual glazing constructions \protect \label{fig:window-glazing-system-with-dual-glazing}}
+\end{figure}
+
+The Window Data File contains no information on shading devices. See ``Specify the Material Name of the Shading Device'' under WindowProperty:ShadingControl for a method to attach a shading layer to windows read in from this file.
+
+Following is an example WINDOW data file for a slider window with two identical double low-E glazing systems separated by a horizontal mullion. Each system has a frame and divider. Note that all dimensions, such as glazing height and width, are in millimeters; when EnergyPlus reads the file these are converted to meters. Following the data file example is a description of the contents of the file. That data used by EnergyPlus is shown in bold.
+
+Window5 Data File for EnergyPlus
+
+\textless{}WINDOW program version\textgreater{}
+
+Date~~~~~~~~~~~~ : Tue Nov 13 17:07:40 2001
+
+Window name~~~~~ : \textbf{DoubleLowE}
+
+Description~~~~~ : Horizontal Slider, AA
+
+\# Glazing Systems: \textbf{2}
+
+GLAZING SYSTEM DATA: Height Width nPanes Uval-center SC-center SHGC-center Tvis-center
+
+~System1~~~~~~~~ :~~ 1032~~ 669~~~~~ 2~~~~~ 1.660~~~~~ 0.538~~~~~ 0.467~~~~~~ 0.696
+
+~System2~~~~~~~~ :~~ 1033~~ 669~~~~~ 2~~~~~ 1.660~~~~~ 0.538~~ ~~~0.467~~~~~~ 0.696
+
+FRAME/MULLION DATA: Width OutsideProj InsideProj Cond EdgeCondRatio SolAbs VisAbs Emiss~ Orient'n (mull)
+
+~~~ L Sill~~~~~~ :~~ 97.3~~~~ 25.4~~~~~~ 25.4~~ 500.000~~~ 1.467~~~~ 0.500~ 0.500~ 0.90
+
+~~~ R Sill~~~~~~ :~~ 97.3~~~~ 25.4~~~~~~ 25.4~~ 500.000~~~ 1.467~~~~ 0.500~ 0.500~ 0.90
+
+~~~ L Head~~~~~~ :~~ 70.2~~~~ 25.4~~~~~~ 25.4~~ 18.822~~~~ 1.490~~~~ 0.500~ 0.500~ 0.90
+
+~~~ R Head~~~~~~ :~~ 70.2~~~~ 25.4~~~~~~ 25.4~~ 18.822~~~~ 1.490~~~~ 0.500~ 0.500~ 0.90
+
+~~~ Top L Jamb~~ :~~ 54.3~~~~ 25.4~~~~~~ 25.4~~ 31.141~~~~ 1.503~~~~ 0.500~ 0.500~ 0.90
+
+~~~ Bot L Jamb~~ :~~ 54.3~~~~ 25.4~~~~~~ 25.4~~ 500.000~~~ 1.494~~~~ 0.500~ 0.500~ 0.90
+
+~~~ Top R Jamb~~ :~~ 70.2~~~~ 25.4~~~~~~ 25.4~~ 500.000~~~ 1.518~~~~ 0.500~ 0.500~ 0.90
+
+~~~ Bot R Jamb~~ :~~ 97.6 ~~~~25.4~~~~~~ 25.4~~ 264.673~~~ 1.547~~~~ 0.500~ 0.500~ 0.90
+
+~~~ Mullion~~~~~ :~~ 53.5~~~~ 25.4~~~~~~ 25.4~~ 500.000~~~ 1.361~~~~ 0.500~ 0.500~ 0.90 \textbf{Horizontal}
+
+~~~ Average frame:~~ \textbf{75.5~~~~ 25.4~~~~~~ 25.4~~ 326.149~~~ 1.464~~~~ 0.500~ 0.500~ 0.90}
+
+DIVIDER DATA~~~~ : Width OutsideProj InsideProj Cond EdgeCondRatio SolAbs VisAbs Emiss Type~~~~~~~~~~~ \#Hor \#Vert
+
+~System1~~~~~~~~ :~ \textbf{25.4~~~ 25.4~~~~~~ 25.4~~~ 3.068~~~~~ 1.191~~~~ 0.500~ 0.500 0.900 DividedLite~~~~~~ 2~~~ 3}
+
+~System2~~~~~~~~ :~ \textbf{25.4~~~ 25.4~~~~ ~~25.4~~~ 3.068~~~~~ 1.191~~~~ 0.500~ 0.500 0.900 DividedLite~~~~~~ 2~~~ 3}
+
+GLASS DATA~~~~~~ : Layer\#~ Thickness~ Cond Tsol Rfsol Rbsol Tvis Rfvis Rbvis~ Tir~ EmissF~ EmissB~ SpectralDataFile
+
+~System1~~~~~~~~ :~~ 1~~~~~ \textbf{3.00~~~~ 0.900} 0.50~ 0.33~ 0.39 0.78~ 0.16~ 0.13 \textbf{0.00~~ 0.16~~~ 0.13}~~ CMFTIR\_3.AFG
+
+~~~~~~~~~~~~~~~~~~~~ 2~~~~~ \textbf{6.00~~~~ 0.900} 0.77~ 0.07~ 0.07 0.88~ 0.08~ 0.08 \textbf{0.00~~ 0.84~~~ 0.84}~~ CLEAR\_6.DAT
+
+~System2~~~~~~~~ :~~ 1~~~~~ \textbf{3.00~~~~ 0.900} 0.50~ 0.33~ 0.39 0.78~ 0.16~ 0.13 \textbf{0.00~~ 0.16~~~ 0.13}~~ CMFTIR\_3.AFG
+
+~~~~~~~~~~~~~~~~~~~~ 2~~~~~ \textbf{6.00~~~~ 0.900} 0.77~ 0.07~ 0.07 0.88~ 0.08~ 0.08 \textbf{0.00~~ 0.84~~~ 0.84}~~ CLEAR\_6.DAT
+
+GAP DATA~~~~~~~~ : Gap\# Thick nGasses
+
+~System1~~~~~~~~ :~~ 1~ \textbf{12.70~~~ 1}
+
+~System2~~~~~~~~ :~~ 1~ \textbf{12.70~~~ 1}
+
+GAS DATA~~~~~~~~ : GasName Fraction MolWeight ACond~~ BCond~ CCond AVisc~~ BVisc~~ CVisc ASpHeat~ BSpHeat CSpHeat
+
+~System1 Gap1~~~ : Air~~~~ \textbf{1.0000~~ 28.97~~~ 0.002873 7.76e-5 0.0 3.723e-6 4.94e-8 0.0~~ 1002.737 0.012324 0.0}
+
+~System2 Gap1~~~ : Air~~~~ \textbf{1.0000~~ 28.97~~~ 0.002873 7.76e-5 0.0 3.723e-6 4.94e-8 0.0~~ 1002.737 0.012324 0.0}
+
+GLAZING SYSTEM OPTICAL DATA
+
+Angle~~~~ 0~~~ 10~~~ 20~~~ 30~~~ 40~~~ 50~~~ 60~~~ 70~~~ 80~~~ 90 Hemis
+
+System1
+
+Tsol~ \textbf{0.408 0.410 0.404 0.395 0.383 0.362 0.316 0.230 0.106 0.000 0.338}
+
+Abs1~ \textbf{0.177 0.180 0.188 0.193 0.195 0.201 0.218 0.239 0.210 0.001 0.201}
+
+Abs2~ \textbf{0.060 0.060 0.061 0.061 0.063 0.063 0.061 0.053 0.038 0.000 0.059}
+
+Rfsol \textbf{0.355 0.350 0.348 0.350 0.359 0.374 0.405 0.478 0.646 0.999 0.392}
+
+Rbsol \textbf{0.289 0.285 0.283 0.282 0.285 0.296 0.328 0.411 0.594 1.000 0.322}
+
+Tvis~ \textbf{0.696 0.700 0.690 0.677 0.660 0.625 0.548 0.399 0.187 0.000 0.581}
+
+Rfvis \textbf{0.207 0.201 0.198 0.201 0.212 0.234 0.278 0.374 0.582 0.999 0.260}
+
+Rbvis \textbf{0.180 0.174 0.173 0.176 0.189 0.215 0.271 0.401 0.648 1.000 0.251}
+
+System2
+
+Tsol~ \textbf{0.408 0.410 0.404 0.395 0.383 0.362 0.316 0.230 0.106 0.000 0.338}
+
+Abs1~ \textbf{0.177 0.180 0.188 0.193 0.195 0.201 0.218 0.239 0.210 0.001 0.201}
+
+Abs2~ \textbf{0.060 0.060 0.061 0.061 0.063 0.063 0.061 0.053 0.038 0.000 0.059}
+
+Rfsol \textbf{0.355 0.350 0.348 0.350 0.359 0.374 0.405 0.478 0.646 0.999 0.392}
+
+Rbsol \textbf{0.289 0.285 0.283 0.282 0.285 0.296 0.328 0.411 0.594 1.000 0.322}
+
+Tvis~ \textbf{0.696 0.700 0.690 0.677 0.660 0.625 0.548 0.399 0.187 0.000 0.581}
+
+Rfvis \textbf{0.207 0.201 0.198 0.201 0.212 0.234 0.278 0.374 0.582 0.999 0.260}
+
+Rbvis \textbf{0.180 0.174 0.173 0.176 0.189 0.215 0.271 0.401 0.648 1.000 0.251}
+
+\textbf{Description of Contents of WINDOW Data File}
+
+(Quantities used in EnergyPlus are in bold; others are informative only)
+
+Second line = version of WINDOW used to create the data file
+
+\emph{Date} = date the data file was created
+
+\textbf{\emph{Window name}} = name of this window; chosen by WINDOW5 user; EnergyPlus user enters the same name in EnergyPlus as name of a ``Construction from Window5 Data File'' object. EnergyPlus will search the Window5 data file for an entry of this name.
+
+\emph{Description} = One-line description of the window; this is treated as a comment.
+
+\textbf{\emph{\# Glazing Systems}}: 1 or 2; value is usually 1 but can be 2 if window has a horizontal or vertical mullion that separates the window into two glazing systems that may or may not be different.
+
+GLAZING SYSTEM DATA
+
+\emph{System1, System2}: separate characteristics given if window has a mullion.
+
+\textbf{\emph{Height}}, *\textbf{\emph{width}} = height and width of glazed portion (i.e., excluding frame; and, if mullion present, excluding mullion).
+
+\textbf{\emph{nPanes}}~~~~ = number of glass layers
+
+\emph{Uval-center} = center-of-glass U-value (including air films) under standard winter conditions*~ (W/m2)
+
+\emph{SC-center}~~ = center-of-glass shading coefficient under standard summer conditions*.
+
+\emph{SHCG-center} = center-of-glass solar heat gain coefficient under standard summer conditions*.
+
+\emph{Tvis-center} = center-of-glass visible transmittance at normal incidence
+
+FRAME/MULLION DATA
+
+\emph{L,R Sill}~~ = left, right sill of frame
+
+\emph{L,R Head}~~ = left, right header of frame
+
+\emph{Top L, Bot L jamb} = top-left, bottom-left jamb of frame
+
+\emph{Bot L, Bot R jamb} = bottom-left, bottom-right jamb of frame
+
+\textbf{\emph{Average frame}} = average characteristics of frame for use in EnergyPlus calculation. If mullion is present, original window is divided into two separate windows with the same average frame (with the mullion being split lengthwise and included in the average frame).
+
+\textbf{\emph{Width}}~~~~ = width (m)
+
+\textbf{\emph{OutsideProj}} = amount of projection from outside glass (m)
+
+\textbf{\emph{InsideProj}} = amount of projection from inside glass (m)
+
+\textbf{\emph{Cond}} = effective surface-to-surface conductance (from THERM calculation) (W/m2)
+
+\textbf{\emph{EdgeCondRatio}} = ratio of surface-to-surface edge-of-glass conductance to surface-to-surface center-of-glass conductance (from THERM calculation)
+
+\textbf{\emph{SolAbs}}~~~ = solar absorptance
+
+\textbf{\emph{VisAbs}}~~~ = visible absorptance
+
+\textbf{\emph{Emiss}}~~~~ = hemispherical thermal emissivity
+
+\textbf{\emph{Orientation}} = Horizontal or Vertical (mullion only); = None if no mullion.
+
+DIVIDER DATA
+
+\textbf{\emph{Width}} through \textbf{\emph{Emiss}} are the same as for FRAME/MULLION DATA
+
+\textbf{\emph{\#Hor}}~~~~~ = number of horizontal dividers
+
+\textbf{\emph{\#Vert}}~~~~ = number of vertical dividers
+
+\textbf{\emph{Type}}~~~~~ = DividedLite or Suspended
+
+GLASS DATA
+
+\emph{System1, System2}: separate characteristics are given if window has a mullion.
+
+\textbf{\emph{Cond}}~~~~~~ = conductivity (W/m-K)
+
+\emph{Tsol}~~~~~~ = spectral-average solar transmittance at normal incidence
+
+\emph{Rfsol}~~~~~ = spectral-average front solar reflectance at normal incidence
+
+\emph{Rbsol}~~~~~ = spectral-average back solar reflectance at normal incidence
+
+\emph{Tvis}~~~~~~ = spectral-average visible transmittance at normal incidence
+
+\emph{Rfvis}~~~~~ = spectral-average front visible reflectance at normal incidence
+
+\emph{Rbvis}~~~~~ = spectral-average back visible reflectance at normal incidence
+
+\textbf{\emph{Tir}}~~~~~~ = hemispherical IR transmittance
+
+\textbf{\emph{EmissF}}~~~ = hemispherical front emissivity
+
+\textbf{\emph{EmissB}}~~~ = hemispherical back emissivity
+
+SpectralDataFile = name of spectral data file with wavelength-dependent transmission and reflection data used by WINDOW 5 to calculate the glazing system optical data. ``None'' will appear here if spectral-average data for this glass layer were used by WINDOW 5.
+
+GAP DATA
+
+System1, System2: separate characteristics are given if the window has a mullion.
+
+\textbf{\emph{Thick}}~~~~ = thickness (m)
+
+\textbf{\emph{nGasses}}~ = number of gasses (1, 2 or 3)
+
+GasName~~ = name of the gas
+
+\textbf{\emph{Fraction}}~ = fraction of the gas
+
+\textbf{\emph{MolecWeight}} = molecular weight of the Nth gas
+
+(In the following, conductivity, viscosity and specific heat as a function
+
+of temperature, T (deg K), are expressed as A + B*T + C*T\^{}2)
+
+\textbf{\emph{ACond}}~~~~ = A coeff of conductivity (W/m-K)
+
+\textbf{\emph{BCond}}~~~~ = B coeff of conductivity (W/m-K\^{}2)
+
+\textbf{\emph{CCond}}~~~~ = C coeff of conductivity (W/m-K\^{}3)
+
+\textbf{\emph{AVisc}}~~~~ = A coeff of viscosity (g/m-s)
+
+\textbf{\emph{BVisc}}~~~~ = B coeff of viscosity (g/m-s-K)
+
+\textbf{\emph{CVisc}}~~~~ = C coeff of viscosity (g/m-s-K\^{}2)
+
+\textbf{\emph{ASpHeat}}~~ = A coeff of specific heat (J/kg-K)
+
+\textbf{\emph{BSpHeat}}~~ = B coeff of specific heat (J/kg-K\^{}2)
+
+\textbf{\emph{CSpHeat}}~~ = C coeff of specific heat (J/kg-K\^{}3)
+
+GLAZING SYSTEM OPTICAL DATA
+
+System1, System2: separate characteristics are given if the window has a mullion.
+
+\textbf{\emph{Hemisph}}~~ = hemispherical (i.e., diffuse)
+
+\textbf{\emph{Tsol}}~~~~~ = solar transmittance vs.~angle of incidence
+
+\textbf{\emph{AbsN}}~~~~~ = solar absorptance of Nth layer vs.~angle of incidence
+
+\textbf{\emph{Rfsol}}~~~~ = front solar reflectance vs.~angle of incidence
+
+\textbf{\emph{Rbsol}}~~~~ = back solar reflectance vs.~angle of incidence
+
+\textbf{\emph{Tvis}}~~~~~ = visible transmittance vs.~angle of incidence
+
+\textbf{\emph{Rfvis}}~~~~ = front visible reflectance vs.~angle of incidence
+
+\textbf{\emph{Rbvis}}~~~~ = back visible reflectance vs.~angle of incidence
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+*Standard conditions are
+
+~ Winter:
+
+~ Indoor air temperature = 21.1C (70F)
+
+~ Outdoor air temperature = -17.8C (0F)
+
+~ Wind speed = 6.71 m/s (15 mph)
+
+~ No solar radiation
+
+~ Summer:
+
+~ Indoor air temperature = 23.9C (75F)
+
+~ Outdoor air temperature = 31.7C (89F)
+
+~ Wind speed = 3.35 m/s (7.5 mph)
+
+~ 783 W/m2 (248 Btu/h-ft2) incident beam solar radiation normal to glazing
diff --git a/doc/tips-and-tricks-using-energyplus/src/input/using-macros-and-editing-inputs-in-idf-editor.tex b/doc/tips-and-tricks-using-energyplus/src/input/using-macros-and-editing-inputs-in-idf-editor.tex
new file mode 100644
index 00000000000..5f6b67afd30
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/input/using-macros-and-editing-inputs-in-idf-editor.tex
@@ -0,0 +1,9 @@
+\section{Using Macros and Editing Inputs in IDF Editor}\label{using-macros-and-editing-inputs-in-idf-editor}
+
+\emph{How can I use macros, and continue to edit my input in IDF editor?}
+
+\emph{(Using or ignoring macros in the IDF editor is a potential Enhancement List item.)}
+
+1)~~~Separate files into ``IDF editable'' and ``macro'' (actually, the AbsorptionChiller\_Macro.imf example file shows a little of this but it doesn't really use macros). For the pieces you think you'd like to manipulate in the IDF editor, call them with extension IDF. For the others, they would be IMF and the master file would be IMF with ``includes'' of your IDF pieces.
+
+2)~~~Use the expanded IDF (extension epmidf) file for your IDF editor changes and then run it from there.
diff --git a/doc/tips-and-tricks-using-energyplus/src/introduction-support.tex b/doc/tips-and-tricks-using-energyplus/src/introduction-support.tex
new file mode 100644
index 00000000000..8c9f57eb423
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/introduction-support.tex
@@ -0,0 +1,11 @@
+\chapter{Introduction \& Support}\label{introduction-support}
+
+This is a quick guide for using and troubleshooting EnergyPlus simulation software. The information here is taken from the knowledge base and from EnergyPlus users looking for answers.
+
+\textbf{Note that these articles are taken from actual user questions and may not be applicable to your model.}
+
+For more detailed information about using EnergyPlus, refer to the user guides and manuals that are installed in the Documentation folder and are also available from \href{http://www.energyplus.gov}{www.energyplus.gov}.
+
+This is a short guide
+
+\ldots{} meant to save time and energy!
diff --git a/doc/tips-and-tricks-using-energyplus/src/introduction-support/energyplus-support.tex b/doc/tips-and-tricks-using-energyplus/src/introduction-support/energyplus-support.tex
new file mode 100644
index 00000000000..4cffe82f620
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/introduction-support/energyplus-support.tex
@@ -0,0 +1,11 @@
+\section{EnergyPlus Support}\label{energyplus-support}
+
+The primary EnergyPlus support site is supplied at: http://energyplus.helpserve.com
+
+The site is monitored by EnergyPlus developers and questions are attempted to be answered in a timely manner. Standard EnergyPlus support is provided free of charge by the U.S. Deparment of Energy, as part of a continuing effort to improve the EnergyPlus building simulation tool. Expedited, priority support may be available from other sources. The helpdesk has a files area where important (after release) files may be put as well as the storage for the Transition file set that are prior to the current release.
+
+http://simulationresearch.lbl.gov/EP/ep\_consult.html is a list of EnergyPlus consultants.
+
+Yahooâ„¢ Groups is also used as a peer to peer discussion group. To join the group (which now has about 2,600 participants), visit \href{http://groups.yahoo.com/EnergyPlus_Support}{http://groups.yahoo.com/group/EnergyPlus\_Support} The Yahoo group has some file storage capabilities and that is also where the Meteonormâ„¢ files that supplement the primary EnergyPlus weather data are housed. The Yahoo group may not be monitored by EnergyPlus developers.
+
+A similar Yahoo group has been set up for collaborative developers.
diff --git a/doc/tips-and-tricks-using-energyplus/src/introduction-support/organization.tex b/doc/tips-and-tricks-using-energyplus/src/introduction-support/organization.tex
new file mode 100644
index 00000000000..b3e7313d2b5
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/introduction-support/organization.tex
@@ -0,0 +1,5 @@
+\section{Organization}\label{organization}
+
+The organization of this document roughly uses the categories of the new features documents that have been included with EnergyPlus since April 2001 (the initial offering).
+
+Under the subject categories, there may be a mix of short articles and Q\&A format.
diff --git a/doc/tips-and-tricks-using-energyplus/src/natural-and-mechanical-ventilation.tex b/doc/tips-and-tricks-using-energyplus/src/natural-and-mechanical-ventilation.tex
new file mode 100644
index 00000000000..810ed959010
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/natural-and-mechanical-ventilation.tex
@@ -0,0 +1 @@
+\chapter{Natural and Mechanical Ventilation}\label{natural-and-mechanical-ventilation}
diff --git a/doc/tips-and-tricks-using-energyplus/src/natural-and-mechanical-ventilation/airflownetwork-and-earthtube.tex b/doc/tips-and-tricks-using-energyplus/src/natural-and-mechanical-ventilation/airflownetwork-and-earthtube.tex
new file mode 100644
index 00000000000..d23c500d658
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/natural-and-mechanical-ventilation/airflownetwork-and-earthtube.tex
@@ -0,0 +1,20 @@
+\section{AirflowNetwork and EarthTube}\label{airflownetwork-and-earthtube}
+
+\emph{When I use an Earthtube with an AirFlowNetwork, I get a ``Orphan Object'' warning.}
+
+Currently, Earthtube and AirFlowNetworks do not work together.~ If both objects co-exist, the AirflowNetwork mode supersedes the Earthtube mode at two control choices. Since this causes the Earthtube objects to not be used, the ``orphan'' warning appears.
+
+There are four control choices in the second field of the AirflowNetwork Simulation object (spaces included for readability)
+
+\begin{itemize}
+\item
+  MULTIZONE WITH DISTRIBUTION
+\item
+  MULTIZONE WITHOUT DISTRIBUTION
+\item
+  MULTIZONE WITH DISTRIBUTION ONLY DURING FAN OPERATION
+\item
+  NO MULTIZONE OR DISTRIBUTION
+\end{itemize}
+
+When the first two choices are selected, the AirflowNetwork model takes over airflow calculation. The earthtube objects are not used in the airflow calculation, causing the ``orphan'' warning. The example file, AirflowNetwork\_Multizone\_SmallOffice.idf, uses the first choice.~ When the second choice is used, the AirflowNetwork model is only used during HVAC operation time. During system off time, the earthtube model is used to calculate airflows.~ Thus, no ``orphan'' warning will be given, but the earthtube may be being used less than expected.~ The example file, AirflowNetwork\_Simple\_House.idf, uses the third choice.
diff --git a/doc/tips-and-tricks-using-energyplus/src/output.tex b/doc/tips-and-tricks-using-energyplus/src/output.tex
new file mode 100644
index 00000000000..342c02e6231
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/output.tex
@@ -0,0 +1 @@
+\chapter{Output}\label{output}
diff --git a/doc/tips-and-tricks-using-energyplus/src/output/advanced-output-variable-reporting.tex b/doc/tips-and-tricks-using-energyplus/src/output/advanced-output-variable-reporting.tex
new file mode 100644
index 00000000000..3ebe89d5cc1
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/output/advanced-output-variable-reporting.tex
@@ -0,0 +1,134 @@
+\section{Advanced Output Variable Reporting}\label{advanced-output-variable-reporting}
+
+Files for the following exercise can be found in the ExampleFiles\textbackslash{}AdvancedOutput folder in your installation. A four page instruction sheet is included.
+
+A shortened, bulleted list of steps is shown:
+
+\begin{itemize}
+\item
+  run the existing input file to generate a list of the report variables available for your simulations.
+\item
+  add report variables at various time aggregations to the file and run the simulation again.
+\item
+  create a .RVI file to extract specific data at various time aggregations.
+\end{itemize}
+
+Read more about obtaining custom output files (.CSV) using .RVI (Report Variable Input) files from the output in the InputOutputReference.pdf, subject: Using ReadVarsESO.
+
+Simply said, an .RVI is a text file with a list of report variables that you want reported in a .CSV. You can easily develop multiple .RVI files which create different types of .CSV files. For example, separate .CSVs for only the exterior environment data or for only equipment energy consumption. MVI files are the equivalent kind of files for meter only output files (the .mtr files). Both .RVI and .MVI files follow this structure:
+
+\begin{lstlisting}
+eplusout.eso   ! name of input eso file
+eplusout.csv   ! name of target csv file (or .tab)
+\end{lstlisting}
+
+ \ldots{} 0
+
+The first two lines are the default output file .ESO and the default .CSV filename. This is followed by a list of report variables, with the last line containing a 0.
+
+1~~~ Run the ExerciseOutput1.IDF file.
+
+2~~~ Open ExerciseOutput1.RDD and select at least 10 loads-related variables. \emph{Note in ExerciseOutput1.IDF, the object ``Output:VariableDictionary, idf;'' writes the RDD output file as complete objects which can be pasted directly into the IDF file and then edit the reporting frequency.}
+
+Edit ExerciseOutput1.IDF using the text editor, and save as ExerciseOutput1A.IDF. Paste output:variable objects for each of your loads-related variables requesting hourly data. Then copy each object and paste in 4 copies for a total of 5. Then edit the frequency parameter on each, changing ``hourly'' to timestep, daily, monthly, and annual, retaining hourly for one of them. There are already system related output variables with multiple reporting frequencies in the .idf file that you can use as a model. For example, Zone Window Heat Gain and Zone Window Heat Loss, insert these objects in your IDF to get data at each of these time steps:
+
+\begin{itemize}
+\item
+  Output:Variable, *, Zone Window Heat Gain, timestep;
+\item
+  Output:Variable, *, Zone Window Heat Gain, hourly;
+\item
+  Output:Variable, *, Zone Window Heat Gain, daily;
+\item
+  Output:Variable, *, Zone Window Heat Gain, monthly;
+\item
+  Output:Variable, *, Zone Window Heat Gain, annual;
+\item
+  Output:Variable, *, Zone Window Heat Loss, timestep;
+\item
+  Output:Variable, *, Zone Window Heat Loss, hourly;
+\item
+  Output:Variable, *, Zone Window Heat Loss, daily;
+\item
+  Output:Variable, *, Zone Window Heat Loss, monthly;
+\item
+  Output:Variable, *, Zone Window Heat Loss, annual;
+\end{itemize}
+
+\emph{Note that this step may also be done using IDF Editor. When an RDD file is present, the Output:Variable object will have an active drop-down list showing all of the report variable names present in the RDD output file.}
+
+\begin{itemize}
+\item
+  Run the ExerciseOutput1A.IDF file.
+\item
+  Using your text editor, open ExerciseOutput1A.idf. Open a new file, and save it as ExerciseOutput1A-LOADS.RVI. Type in the following: 
+\end{itemize}
+
+\begin{lstlisting}
+eplusout.eso eplusout.csv
+\end{lstlisting}
+
+In the .idf file, locate the Output:Variable commands you just added. Copy them, and paste them into the new .RVI file. Delete the duplicates with different reporting frequencies, saving one instance of each variable. Delete everything but the variable name. Add a final line containing only a 0 (zero). For Window Heat Loss and Heat Gain, the .RVI file would look like this:
+
+\begin{lstlisting}
+eplusout.eso
+eplusout.csv
+Zone Window Heat Gain
+Zone Window Heat Loss
+0
+\end{lstlisting}
+
+\begin{itemize}
+\item
+  Rename file ``ExerciseOutput1-CustomCSV.b\textasciitilde{}t'' to ``ExerciseOutput1¬CustomCSV.bat'' and edit this file in a text editor to make sure the path at the top of the file matches where your version of EnergyPlus is installed. The current path in the file is:
+\item
+  set post\_proc = C:\textbackslash{}EnergyPlusV6-0-0\textbackslash{}PostProcess\textbackslash{}
+\item
+  Open a Command Window (Start, Run, Command)
+\item
+  Change to the directory containing your ExerciseOutput1A.IDF, results files, and your new ExerciseOutput1A-LOADS.RVI. For example:
+\item
+  CD D:\textbackslash{}EnergyPlus Training\textbackslash{}EnergyPlusExercises ßsubstitute your path here
+\end{itemize}
+
+Note: This assumes that the ExerciseOutput1-CustomCSV.bat file is located in the same directory as your IDF and RVI. This is what EP-Launch does for single simulations.
+
+\begin{itemize}
+\tightlist
+\item
+  Type: ExerciseOutput1-CustomCSV ExerciseOutput1A ExerciseOutput1A-LOADS and press Enter. That is,
+\end{itemize}
+
+ExerciseOutput1-CustomCSV ExerciseOutput1A ExerciseOutput1A-LOADS
+
+\begin{itemize}
+\tightlist
+\item
+  ExerciseOutput1-CustomCSV reads the ESO output and creates a .CSV for the .RVI for only the variables listed in the .RVI. A .CSV is created for each of the time steps in the output file--timestep, hourly, daily, monthly, or runperiod: inputfilename\_timestep.csv, or for this exercise, ExerciseOutput1A.idf:
+\end{itemize}
+
+ExerciseOutput1A\_timestep.csv
+
+ExerciseOutput1A\_hourly.csv
+
+ExerciseOutput1A\_daily.csv
+
+ExerciseOutput1A\_monthly.csv
+
+ExerciseOutput1A\_annual.csv
+
+\emph{If there is no data at the requested time step, that .CSV file will be empty, although that should not occur here.}
+
+\begin{itemize}
+\tightlist
+\item
+  Add report variables to the IDF for energy end-uses. Review .RDD, .MDD and .MTR file for variables to include. Open and save ExerciseOutput1A.idf as ExerciseOutput1B.idf. Create an energy end-use .MVI using the same structure as above but replace eplusout.eso with eplusout.mtr in the first line. Rerun the new IDF and run ExerciseOutput1-CustomCSV again:
+\end{itemize}
+
+ExerciseOutput1-CustomCSV ExerciseOutput1B ExerciseOutput1B-ENERGYENDUSE
+
+\begin{itemize}
+\tightlist
+\item
+  Experiment with creating other .RVIs and variables. Example .RVIs for ExerciseOutput1-EquipmentConsumption and ExerciseOutput1-ExternalEnvironment are included.
+\end{itemize}
diff --git a/doc/tips-and-tricks-using-energyplus/src/output/output-does-not-match-epw-values.tex b/doc/tips-and-tricks-using-energyplus/src/output/output-does-not-match-epw-values.tex
new file mode 100644
index 00000000000..dac92109146
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/output/output-does-not-match-epw-values.tex
@@ -0,0 +1,9 @@
+\section{Output does not match EPW values}\label{output-does-not-match-epw-values}
+
+\emph{Why do values in the EPW differ from the output reports of EnergyPlus?}
+
+This is expected. The difference comes from interpolating hourly weather data for subhourly timesteps in EnergyPlus. In an hourly weather file, the temperatures and other state-point readings are the value at the time the reading was taken. For example, in the USA\_IL\_Chicago-OHare\_TMY2.epw file, the outdoor dry bulb value for July 2, hour 1, is 19.4C. This is the temperature at 1:00 am.
+
+If you set Timestep = 1, then EnergyPlus will report 19.4C for 07/02 01:00 and will use that value for the entire one hour timestep.
+
+If Timestep = 4, then 19.4C is used only for the time step which ends at 01:00. The other timesteps use linearly interpolated values between the hourly weather file values. When you report at the ``hourly'' frequency in EnergyPlus, you see the average temperature over the hour. If you report at the ``timestep'' frequency, you will see the values from the weather data file appear at the last timestep of each hour.
diff --git a/doc/tips-and-tricks-using-energyplus/src/output/output-variable-definition.tex b/doc/tips-and-tricks-using-energyplus/src/output/output-variable-definition.tex
new file mode 100644
index 00000000000..1a5c805b2c9
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/output/output-variable-definition.tex
@@ -0,0 +1,19 @@
+\section{Output Variable Definition}\label{output-variable-definition}
+
+In order to define output variables in your simulation, you must place the following statement in your input file:
+
+\begin{lstlisting}
+
+Output:VariableDictionary,IDF;
+\end{lstlisting}
+
+Then you can cut and paste from the rdd file directly into your idf file. You must first run your simulation to create the rdd file. Output variables found in the rdd file are specific to the simulation and are based on the objects used in your input file.
+
+\begin{lstlisting}
+
+Output:Variable,*,System Node Temp,hourly; !- HVAC Average [C]
+\end{lstlisting}
+
+To get only information for a single node, change to: Output:Variable,``The Name of the Node'',System Node Temp,hourly; !- HVAC Average {[}C{]}.
+
+Where ``The Name of the Node'' is the specific node name for one or more nodes.
diff --git a/doc/tips-and-tricks-using-energyplus/src/output/output-variables-in-idf-editor.tex b/doc/tips-and-tricks-using-energyplus/src/output/output-variables-in-idf-editor.tex
new file mode 100644
index 00000000000..7cd6a4fd9b3
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/output/output-variables-in-idf-editor.tex
@@ -0,0 +1,3 @@
+\section{Output Variables in IDF Editor}\label{output-variables-in-idf-editor}
+
+You must run the simulation before anything will show in the dropdown menu (rdd/mdd files must be present).
diff --git a/doc/tips-and-tricks-using-energyplus/src/output/reporting-options.tex b/doc/tips-and-tricks-using-energyplus/src/output/reporting-options.tex
new file mode 100644
index 00000000000..4b349019dcb
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/output/reporting-options.tex
@@ -0,0 +1,128 @@
+\section{Reporting Options}\label{reporting-options}
+
+There are many report variables in EnergyPlus. The ones available for a specific simulation are listed in the report data dictionary (rdd) file. These report variables may be generated automatically if the following is included in the input file.
+
+\begin{lstlisting}
+
+Output:VariableDictionary,
+  Regular; !- Key Field
+\end{lstlisting}
+
+When the object above is included in an input file, the rdd file is available for review AFTER the simulation has completed. If this object is not included in the input file, the user may still use report variables, but must select them based on the objects included in the simulation. The Input Output Reference document describes all report variables available for each EnergyPlus object.
+
+There are two flavors to output variables: ZONE or HVAC.~ ZONE does not mean that it is a zone variable -- rather, it is produced at the Zone Time Step (the same timestep that you specify in the Timestep object. HVAC type variables, likewise, are produced at the HVAC timestep (which can differ from the zone timestep frequency based on the ConvergenceLimits object).
+
+There are several choices on format with this object. You can specify ``Regular'' as the key field and the rdd will show all report variables along with the variable description as shown below.
+
+\begin{itemize}
+\tightlist
+\item
+  HVAC,Average,Boiler Heating Output Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Heating Output Energy {[}J{]}
+\item
+  HVAC,Average,Boiler Gas Consumption Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Gas Consumption {[}J{]}
+\item
+  HVAC,Average,Boiler Water Inlet Temp {[}C{]}
+\item
+  HVAC,Average,Boiler Water Outlet Temp {[}C{]}
+\item
+  HVAC,Average,Boiler Water Mass Flow Rate {[}kg/s{]}
+\item
+  HVAC,Average,Boiler Parasitic Electric Consumption Rate {[}W{]}
+\item
+  HVAC,Sum,Boiler Parasitic Electric Consumption {[}J{]}
+\item
+  HVAC,Average,Boiler Part-Load Ratio {[}{]}
+\end{itemize}
+
+As an alternative, the key field ``IDF'' may also be used.
+
+\begin{lstlisting}
+
+Output:VariableDictionary,
+  IDF; !- Key Field
+\end{lstlisting}
+
+With this option the rdd will format the report variable so that they may be copied directly into the input file using a text editor.
+
+\begin{itemize}
+\tightlist
+\item
+  Output:Variable,*,Boiler Heating Output Rate,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,Boiler Heating Output Energy,hourly; !- HVAC Sum {[}J{]}
+\item
+  Output:Variable,*,Boiler Gas Consumption Rate,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,Boiler Gas Consumption,hourly; !- HVAC Sum {[}J{]}
+\item
+  Output:Variable,*,Boiler Water Inlet Temp,hourly; !- HVAC Average {[}C{]}
+\item
+  Output:Variable,*,Boiler Water Outlet Temp,hourly; !- HVAC Average {[}C{]}
+\item
+  Output:Variable,*,Boiler Water Mass Flow Rate,hourly; !- HVAC Average {[}kg/s{]}
+\item
+  Output:Variable,*,Boiler Parasitic Electric Consumption Rate,hourly; !- HVAC Average {[}W{]}
+\item
+  Output:Variable,*,Boiler Parasitic Electric Consumption,hourly; !- HVAC Sum {[}J{]}
+\item
+  Output:Variable,*,Boiler Part-Load Ratio,hourly; !- HVAC Average {]}
+\end{itemize}
+
+A different version of the output variable object is shown below.
+
+\begin{lstlisting}
+
+Output:Variable,
+  *, !- Key Value
+  Boiler Heating Output Rate, !- Variable Name
+  hourly, !- Reporting Frequency
+  MyReportVarSchedule; !- Schedule Name
+
+  Schedule:Compact,
+  MyReportVarSchedule, !- Name
+  On/Off, !- Schedule Type Limits Name
+  Through: 1/20, !- Field 1
+  For: AllDays, !- Field 2
+  Until: 24:00, 0.0, !- Field 4
+  Through: 12/31, !- Field 5
+  For: AllDays, !- Field 6
+  Until: 24:00, 1.0; !- Field 8
+
+  ScheduleTypeLimits,
+  On/Off, !- Name
+  0:1, !- Range
+  DISCRETE; !- Numeric Type
+\end{lstlisting}
+
+This allows several options for reporting. First the key value may be an asterisk (*) where all report variables of this type are reported (for all boilers). Or the key value could be specified such that only a single output will be generated. For example if the key value was specified as ``My Boiler'' and a boiler object with the name My Boiler was included in the input, only the Boiler Heating Output Rate for this specific boiler will be in the output file (.csv). The reporting output for all other boilers in the simulation will not be included in the csv file.
+
+The reporting frequency is also another option and may be one of several choices (e.g., Timestep, Hourly, Daily, Monthly, RunPeriod, Environment, Annual or Detailed).
+
+The detailed reporting frequency reports the data for every simulation time step (HVAC variable time steps). This choice is useful for detailed troubleshooting and reporting. The other choices average or sum the data over the selected interval. Timestep refers to the zone Timestep/Number of Timesteps in hour value and reports the data at regular intervals. Using RunPeriod, Environment, or Annual will have the same affect on the reporting frequency and refer to the length of the simulaiton as specified in the RunPeriod object.
+
+\begin{lstlisting}
+
+Timestep,
+  4; !- Number of Timesteps per Hour
+
+
+  RunPeriod,
+  1, !- Begin Month
+  1, !- Begin Day of Month
+  12, !- End Month
+  31, !- End Day of Month
+  Tuesday, !- Day of Week for Start Day
+  Yes, !- Use Weather File Holidays and Special Days
+  Yes, !- Use Weather File Daylight Saving Period
+  No, !- Apply Weekend Holiday Rule
+  Yes, !- Use Weather File Rain Indicators
+  Yes; !- Use Weather File Snow Indicator
+\end{lstlisting}
+
+A schedule may also be used to turn on or off report variable at selected intervals.
+
+Table reports and meters are also available as reporting options. See the Input Output and Engineering Reference manuals for further details.
diff --git a/doc/tips-and-tricks-using-energyplus/src/output/schedules-off-by-1-hour.tex b/doc/tips-and-tricks-using-energyplus/src/output/schedules-off-by-1-hour.tex
new file mode 100644
index 00000000000..3bdff0fe8e6
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/output/schedules-off-by-1-hour.tex
@@ -0,0 +1,5 @@
+\section{Schedules off by 1 hour}\label{schedules-off-by-1-hour}
+
+When active, DaylightSavingTime will shift all scheduled items by one hour. Reporting is always in standard time and uses the same day (scheduled values wrap). In short, the Daylight Saving Time flag uses the schedule value from the \emph{next hour} in the simulation. This can be confusing if your schedules are not symmetric around the midnight hours. Because\ldots{} the new schedule value will show up on the \emph{same day}, not the next day as it might in real life. EnergyPlus does not currently to look ahead/back for next hour schedules (particularly at day boundaries).
+
+More information on Daylight Saving Periods can be seen on the web at: http://www.webexhibits.org/daylightsaving/
diff --git a/doc/tips-and-tricks-using-energyplus/src/output/use-of-comma-and-point-in-numeric-output.tex b/doc/tips-and-tricks-using-energyplus/src/output/use-of-comma-and-point-in-numeric-output.tex
new file mode 100644
index 00000000000..707f2ff7781
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/output/use-of-comma-and-point-in-numeric-output.tex
@@ -0,0 +1,5 @@
+\section{Use of Comma and Point in Numeric Output}\label{use-of-comma-and-point-in-numeric-output}
+
+All EnergyPlus numeric output is written using the U.S. convention of a period or point ``.'' as the decimal separator. No thousands separator is used. For example, the numeric output for ``one thousand two hundred and one half'' would be 1200.5 in output files. The same conventions apply for EnergyPlus input files (idf), Exponent format (1.2005E+03) is also valid on input but is not used in output files.
+
+Commas are used to separate values or fields in EnergyPlus input and output. They should not be used as part of any numeric value, not as a decimal separator and not as a thousands separator. This can cause problems for users in regions of the world which normally use comma as the decimal separator. This is especially important when viewing EnergyPlusvariables (*.csv) and meters (*Meter.csv) output files. Typically csv output files are viewed in a spreadsheet program, such as Excel. ``csv'' stands for ``comma separated values'', so the spreadsheet software needs to recognize comma as a list separator, not a decimal or thousands separator. If the values from a csv file appear to be nonsense when displayed in a spreadsheet program, this may be the source of the problem. Change the decimal separator to be ``.''~ in your system settings or in the spreadsheet program settings.
diff --git a/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time.tex b/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time.tex
new file mode 100644
index 00000000000..02d6c3b13d3
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time.tex
@@ -0,0 +1,3 @@
+\chapter{Platforms and Run-Time}\label{platforms-and-run-time}
+
+EnergyPlus is available for the Windows, Macintosh, and Linux Platforms. It may not be available for all flavors of those platforms. Usually, the newer versions of those platforms will be the ones most supported with some older versions as well.
diff --git a/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/reduce-energyplus-run-time.tex b/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/reduce-energyplus-run-time.tex
new file mode 100644
index 00000000000..5e2892f3e6c
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/reduce-energyplus-run-time.tex
@@ -0,0 +1,35 @@
+\section{Reduce EnergyPlus Run Time}\label{reduce-energyplus-run-time}
+
+\emph{What affects EnergyPlus Run-Time?}
+
+Compared with creating energy models either by hand coding the IDF file or by using GUI tools or a combination of both, EnergyPlus run time is normally a small fraction of the total time needed to complete an energy modeling job. Therefore it is very important to build a clean and concise EnergyPlus model up front. Techniques of simplifying large and complex building and systems should be used during the creation of energy models, especially during the early design process when detailed zoning and other information is not available. Producing lots of hourly or sub-hourly reports from EnergyPlus runs can take significant amount of time. Modelers should only request time step reports when necessary. On the other hand, producing summary reports and typical monthly reports take relatively small amount of run time. These reports are valuable references for troubleshooting and model fine tuning.
+
+With powerful personal computers get more and more affordable, EnergyPlus modelers should choose to use current available PCs with 3 or more GHZ clock speed and 3 or more GB of RAM and multiple core processors. EP-Launch will now automatically launch multiple runs on multiple processors (group runs).
+
+For modelers, most time is spent on troubleshooting and fine tuning energy models. During the early modeling process, it is recommended to keep the model as simple as possible and make quick runs to identify problems. Then modify the IDF file to fix problems and re-run the model. This is an iterative process until satisfactory solutions are found. The simulation process can be split into three phases: the diagnostic runs, the preliminary runs, and the final runs. The three phases would use different simulation settings. The diagnostic runs would use a set of simulation settings to speed up the runs with simulation accuracy being set as the second priority. The diagnostic runs will help catch most model problems by running simulations on summer and winter design days. The preliminary runs use a tighter set of simulation settings in order to catch problems missed in the diagnostic runs, and provide better results for quality assurance purpose. The final runs use the EnergyPlus recommended set of simulation settings in order to achieve better accuracy for simulation results ready for review and reporting.
+
+Specifically, recommendations (and particularly recommended for large buildings with large numbers of surfaces and shading surfaces):
+
+% table 5
+\begin{longtable}[c]{p{1.5in}p{4.5in}}
+\caption{Recommended Reduce Time Settings for Early Diagnostic runs \label{table:recommended-reduce-time-settings-for-early}} \tabularnewline
+\toprule 
+Object & Recommenheh Early Diagnostic Setting \tabularnewline
+\midrule
+\endfirsthead
+
+\caption[]{Recommended Reduce Time Settings for Early Diagnostic runs} \tabularnewline
+\toprule 
+Object & Recommenheh Early Diagnostic Setting \tabularnewline
+\midrule
+\endhead
+
+Building & MinimalShadowing (Solar Distribution field) \tabularnewline
+ShadowCalculation & 200 (Maximum Figures in Shadow Overlap Calculations field) \tabularnewline
+SizingPeriod:DesignDays & Only perform design day or limited run period runs until you have the model set. \tabularnewline
+\bottomrule
+\end{longtable}
+
+You might want to read the report on EnergyPlus run time at http://repositories.cdlib.org/lbnl/LBNL-1311E/
+
+Remember, too, that EnergyPlus is, by design, a multiple timestep per hour simulation. Comparing its run-time to programs that are only hourly has potential for comparing apples and grapes. In addition, EnergyPlus is a simultaneous solution of the building loads, HVAC system and plant equipment simulation with possible multiple iterations to reach balance.
diff --git a/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/run-energyplus-in-parallel.tex b/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/run-energyplus-in-parallel.tex
new file mode 100644
index 00000000000..c9fca3b25c7
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/run-energyplus-in-parallel.tex
@@ -0,0 +1,7 @@
+\section{Run EnergyPlus in Parallel}\label{run-energyplus-in-parallel}
+
+EnergyPlus is a multi-thread application but is not optimized for parallel runs on multi-core machines. However, multiple parametric runs can be launched in parallel if these runs are independent. One way to do it is to create multiple folders and copy files EnergyPlus.exe, Energy+.idd, DElight2.dll, libexpat.dll, bcvtb.dll, EPMacro.exe (if macros are used), ExpandObjects.exe (if HVACTemplate or Compact HVAC objects are used) from the original EnergyPlus installed folder. Inside each folder, copy IDF file as in.idf and EPW file as in.epw, then run EnergyPlus.exe from each folder. This is better handled with a batch file. If the Energy+.ini file exists in one of the created folders, make sure it is empty or points to the current EnergyPlus folder.
+
+EP-Launch now does this automatically for Group or Parametric-Preprocessor runs.
+
+The benefit of run time savings depends on computer configurations including number of CPUs, CPU clock speed, amount of RAM and cache, and hard drive speed. To be time efficient, the number of parallel EnergyPlus runs should not be more than the number of CPUs on a computer. The EnergyPlus utility program EP-Launch is being modified to add the parallel capability for group simulations. The long term goal is to run EnergyPlus in parallel on multi-core computers even for a single EnergyPlus run without degradation to accuracy.
diff --git a/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/running-energyplus-on-windows-vista-and.tex b/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/running-energyplus-on-windows-vista-and.tex
new file mode 100644
index 00000000000..d47133cc084
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/platforms-and-run-time/running-energyplus-on-windows-vista-and.tex
@@ -0,0 +1,5 @@
+\section{Running EnergyPlus on Windows Vista and/or Windows 7}\label{running-energyplus-on-windows-vista-andor-windows-7}
+
+For all operating systems, make sure that you have read and write access to files in the main EnergyPlus folder (by default EnergyPlus is installed in C:\textbackslash{}EnergyPlus\textless{}version\textgreater{}). If you do not have this kind of access some very peculiar messages may appear when you try to run simulations.
+
+EnergyPlus has no problems running on Vista or Windows 7 computers if it is run directly by executing the EnergyPlus.exe file assuming you have prepared the in.idf and in.epw files at the same folder. There were some issues running earlier versions of EP-Launch, but most have been fixed for the latest version of EP-Launch. If EnergyPlus was installed at a user folder like C:\textbackslash{} EnergyPlusV3-0-0, there should be no problems running EP-Launch. If EnergyPlus was installed at a windows system folder like `C:\textbackslash{}Program files\textbackslash{} EnergyPlusV3-0-0', you have to run EP-Launch every time with administrator rights by right clicking the EP-Launch.exe file and choose `Run as Administrator'. Another way is to create a shortcut to EPLaunch and change settings appropriately.
diff --git a/doc/tips-and-tricks-using-energyplus/src/tips-tricks-for-using-energyplus.tex b/doc/tips-and-tricks-using-energyplus/src/tips-tricks-for-using-energyplus.tex
new file mode 100644
index 00000000000..63f37402bb8
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/tips-tricks-for-using-energyplus.tex
@@ -0,0 +1 @@
+\input{../title}
diff --git a/doc/tips-and-tricks-using-energyplus/src/utilities.tex b/doc/tips-and-tricks-using-energyplus/src/utilities.tex
new file mode 100644
index 00000000000..fcc3075e385
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/utilities.tex
@@ -0,0 +1 @@
+\chapter{Utilities}\label{utilities}
diff --git a/doc/tips-and-tricks-using-energyplus/src/validation-and-testing.tex b/doc/tips-and-tricks-using-energyplus/src/validation-and-testing.tex
new file mode 100644
index 00000000000..7cb31ac1313
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/src/validation-and-testing.tex
@@ -0,0 +1,28 @@
+\chapter{Validation and Testing}\label{validation-and-testing}
+
+An important ongoing part of EnergyPlus development is testing using industry standard methods as major builds are completed. The goal is to make EnergyPlus as bug-free as possible. Three major types of tests are currently conducted:
+
+\begin{itemize}
+\item
+  Analytical tests:
+\item
+  HVAC tests, based on ASHRAE Research Project 865
+\item
+  Building fabric tests, based on ASHRAE Research Project 1052
+\item
+  Comparative tests:
+\item
+  ANSI/ASHRAE Standard 140-2007
+\item
+  International Energy Agency Solar Heating and Cooling Programme (IEA SHC) BESTest (Building Energy Simulation Test) methods not yet in Standard 140
+\item
+  EnergyPlus HVAC Component Comparative tests
+\item
+  EnergyPlus Global Heat Balance tests
+\item
+  Release and executable tests
+\end{itemize}
+
+For detailed reports, please use the following link:
+
+http://apps1.eere.energy.gov/buildings/energyplus/energyplus\_testing.cfm
diff --git a/doc/tips-and-tricks-using-energyplus/tips-and-tricks-using-energyplus.tex b/doc/tips-and-tricks-using-energyplus/tips-and-tricks-using-energyplus.tex
new file mode 100644
index 00000000000..474113907ae
--- /dev/null
+++ b/doc/tips-and-tricks-using-energyplus/tips-and-tricks-using-energyplus.tex
@@ -0,0 +1,178 @@
+\input{../header}
+
+\title{Tips and Tricks for Using EnergyPlus}
+
+\hypersetup{unicode=true,
+            pdftitle={Tips and Tricks for Using EnergyPlus},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/tips-tricks-for-using-energyplus}
+
+\input{src/introduction-support}
+
+\input{src/introduction-support/organization}
+
+\input{src/introduction-support/energyplus-support}
+
+\input{src/general}
+
+\input{src/general/what-energyplus-is}
+
+\input{src/general/what-energyplus-isn-t}
+
+\input{src/general/getting-started}
+
+\input{src/general/comparing-energyplus-to-other-programs}
+
+\input{src/datasets}
+
+\input{src/datasets/datasets-aka-libraries}
+
+\input{src/datasets/locations-designdays}
+
+\input{src/design-day-weather-data}
+
+\input{src/design-day-weather-data/design-day-creation}
+
+\input{src/design-day-weather-data/epw-weather-files}
+
+\input{src/design-day-weather-data/meteonorm-weather-files}
+
+\input{src/design-day-weather-data/weather-data-for-simulations}
+
+\input{src/design-day-weather-data/weather-file-sources}
+
+\input{src/design-day-weather-data/measuring-solar-data}
+
+\input{src/input}
+
+\input{src/input/creating-files-for-energyplus}
+
+\input{src/input/converting-older-version-energyplus-files}
+
+\input{src/input/using-macros-and-editing-inputs-in-idf-editor}
+
+\input{src/input/getting-data-from-window-program}
+
+\input{src/building-geometry-shading-zone-model}
+
+\input{src/building-geometry-shading-zone-model/building-surface-dimensions-inside-outside}
+
+\input{src/building-geometry-shading-zone-model/describing-roof-overhangs}
+
+\input{src/building-geometry-shading-zone-model/solar-reflection-from-shading-surfaces}
+
+\input{src/building-geometry-shading-zone-model/air-wall-open-air-connection-between-zones}
+
+\input{src/building-geometry-shading-zone-model/daylight-modeling}
+
+\input{src/building-geometry-shading-zone-model/rain-flag}
+
+\input{src/building-geometry-shading-zone-model/interzone-exterior-convection}
+
+\input{src/building-geometry-shading-zone-model/modeling-reflective-radiant-barriers}
+
+\input{src/building-geometry-shading-zone-model/cavity-algorithm-model}
+
+\input{src/building-geometry-shading-zone-model/using-multipliers-zone-and-or-window}
+
+\input{src/building-geometry-shading-zone-model/using-osc-other-side-coefficients-to-create}
+
+\input{src/natural-and-mechanical-ventilation}
+
+\input{src/natural-and-mechanical-ventilation/airflownetwork-and-earthtube}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/hvac-sizing-tips}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/variable-refrigerant-flow-air-conditioner}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/modeling-desiccant-dehumidifiers}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/boiler-control-schedule}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/difference-between-eir-and-reformulated-eir}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/using-well-water}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/plant-load-profile}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/hvac-system-turn-off}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/fan-types}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/use-of-set-point-managers}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/hvac-availability-schedules}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/hvac-system-types}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/separating-ventilation-loads-v-zone-loads}
+
+\input{src/hvac-sizing-equipment-simulation-and-controls/system-not-cooling}
+
+\input{src/output}
+
+\input{src/output/output-does-not-match-epw-values}
+
+\input{src/output/schedules-off-by-1-hour}
+
+\input{src/output/reporting-options}
+
+\input{src/output/output-variables-in-idf-editor}
+
+\input{src/output/output-variable-definition}
+
+\input{src/output/advanced-output-variable-reporting}
+
+\input{src/output/use-of-comma-and-point-in-numeric-output}
+
+\input{src/utilities}
+
+\input{src/documentation-and-guides}
+
+\input{src/errors-and-warnings}
+
+\input{src/errors-and-warnings/max-iterations-exceeded}
+
+\input{src/error-messages-details}
+
+\input{src/error-messages-details/standard-error-message-format}
+
+\input{src/error-messages-details/example-error-messages-for-preprocessors}
+
+\input{src/error-messages-details/example-error-messages-for-the-input}
+
+\input{src/error-messages-details/example-error-messages-from-module-getinput}
+
+\input{src/error-messages-details/example-error-messages-during-sizing}
+
+\input{src/error-messages-details/recurring-errors}
+
+\input{src/error-messages-details/summaries-at-end-of-simulation}
+
+\input{src/error-messages-details/psychrometric-errors}
+
+\input{src/error-messages-details/error-summary}
+
+\input{src/validation-and-testing}
+
+\input{src/platforms-and-run-time}
+
+\input{src/platforms-and-run-time/reduce-energyplus-run-time}
+
+\input{src/platforms-and-run-time/run-energyplus-in-parallel}
+
+\input{src/platforms-and-run-time/running-energyplus-on-windows-vista-and}
+
+\end{document}
diff --git a/doc/title.tex b/doc/title.tex
new file mode 100644
index 00000000000..9ed4bf71d79
--- /dev/null
+++ b/doc/title.tex
@@ -0,0 +1,30 @@
+% Reference for making your own Title Page: 
+% http://tex.stackexchange.com/questions/10130/use-the-values-of-title-author-and-date-on-a-custom-title-page
+\makeatletter
+\begin{titlepage}
+  \begin{center}
+    {\scshape\LARGE EnergyPlus\texttrademark{} Version 8.5 Documentation \par}
+    \vspace{1.5cm}
+    {\bfseries\huge \@title \par}
+    \vspace{1.5cm}
+    {\Large\itshape \@author \par}
+    \vspace{2.5cm}
+    \includegraphics[width=0.2\textwidth]{media/ep.png}\par\vspace{1cm}
+    \vfill
+
+    % Bottom of the page
+    {\large \@date \par}
+    \vspace{1.5cm}
+  \end{center}
+  {\small
+COPYRIGHT (c) 1996-2016 THE BOARD OF TRUSTEES OF THE UNIVERSITY OF ILLINOIS AND THE REGENTS OF THE UNIVERSITY OF CALIFORNIA THROUGH THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ALL RIGHTS RESERVED. NO PART OF THIS MATERIAL MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS WITHOUT THE PRIOR WRITTEN PERMISSION OF THE UNIVERSITY OF ILLINOIS OR THE ERNEST ORLANDO LAWRENCE BERKELEY NATIONAL LABORATORY. ENERGYPLUS IS A TRADEMARK OF THE US DEPARTMENT OF ENERGY.
+  }
+\end{titlepage}
+\makeatother
+
+{
+\setcounter{tocdepth}{2}
+\tableofcontents
+}
+
+\hypertarget{generated-toc}{}
diff --git a/doc/tools/create_changelog.py b/doc/tools/create_changelog.py
index 13041ef0ecc..a2a56f48bb2 100755
--- a/doc/tools/create_changelog.py
+++ b/doc/tools/create_changelog.py
@@ -21,13 +21,14 @@
 debug = False
 
 def usage():
-    print("""Script should be called with 4 positional arguments:
+    print("""Script should be called with 8 positional arguments:
  - the path to a repository
  - the path to a markdown output file
  - the path to a html output file
  - the path to a local git executable
  - a github token for performing authentication API requests
- - the commit SHA for the last major release""")
+ - the commit SHA for the last major release
+ - a program version identifier""")
 
 # command line arguments: repo base path, output markdown and html file paths, a git exe path, and a github token
 if len(sys.argv) == 7:
@@ -37,6 +38,7 @@ def usage():
     git_exe = sys.argv[4]
     github_token = sys.argv[5]
     last_commit = sys.argv[6]
+    program_version = sys.argv[7]
 elif len(sys.argv) == 8:
     repo = sys.argv[1]
     md_file = sys.argv[2]
@@ -44,6 +46,7 @@ def usage():
     git_exe = sys.argv[4]
     github_token = sys.argv[5]
     last_commit = sys.argv[6]
+    program_version = sys.argv[7]
 else:
     usage()
     sys.exit(1)
@@ -100,14 +103,6 @@ def usage():
 		label_name = label['name']
 		if label_name in ValidPRTypes:
 			PRS[label_name].append([pr_num, title])
-    #if len(labels) != 1:
-        #print(" +++ AutoDocs: %s,%s,Pull request has wrong number of labels (%i)...expected 1" % (pr_num, title, len(labels)))
-    #else:
-        #key = 'Unknown'
-        #first_label_name = labels[0]['name']
-        #if first_label_name in ValidPRTypes:
-            #key = first_label_name
-        #PRS[key].append([pr_num, title])
 
 # Now write the nice markdown output file
 with io.open(md_file, 'w') as f:
@@ -120,8 +115,8 @@ def out_pr_class(pr_type, descriptor):
         for pr in PRS[pr_type]:
             out(' - [#' + pr[0] + '](' + EPlusRepoPath + '/pull/' + pr[0] + ') : ' + pr[1])
 
-    out('# ChangeLog')
-    out('Consists of pull requests merged in since the last release.')
+    out('# Changelog for EnergyPlus ' + program_version)
+    out('Consists of pull requests merged in since the last release - starting with SHA [' + last_commit + '](https://github.com/' + RepoName + '/commit/' + last_commit + ')')
     out_pr_class('NewFeature', 'New Features')
     out_pr_class('Performance', 'Performance Enhancements')
     out_pr_class('Defect', 'Defects Repaired')
@@ -159,8 +154,8 @@ def out_pr_class(pr_type, descriptor):
     out(' padding: 6px;')
     out('}')
     out('</style>')
-    out('<h1>EnergyPlus ChangeLog</h1>')
-    out('This file is auto-generated from merged pull requests in the repository.')
+    out('<h1>ChangeLog for EnergyPlus ' + program_version + '</h1>')
+    out('<h1>Consists of pull requests merged in since the last release - starting with SHA <a href = "https://github.com/' + RepoName + '/commit/' + last_commit + '">' + last_commit + '</a>' + '</h1>')
     out_pr_class('NewFeature', 'New Features')
     out_pr_class('Performance', 'Performance Enhancements')
     out_pr_class('Defect', 'Defects Repaired')
diff --git a/doc/using-energyplus-for-compliance/CMakeLists.txt b/doc/using-energyplus-for-compliance/CMakeLists.txt
new file mode 100644
index 00000000000..803bfa83109
--- /dev/null
+++ b/doc/using-energyplus-for-compliance/CMakeLists.txt
@@ -0,0 +1,34 @@
+
+# to get the list of input files, go to the root of the document folder, and:
+# grep -r '\\input{' * | cut -d ':' -f 2 | cut -c 8- | rev | cut -c 2- | rev | sed 's|^|  ${CMAKE_SOURCE_DIR}/doc/acknowledgements/|g' | sed 's/$/.tex/g' 
+SET( INCLUDED_TEX
+  ${CMAKE_SOURCE_DIR}/doc/title.tex
+  ${CMAKE_SOURCE_DIR}/doc/using-energyplus-for-compliance/using-energyplus-for-compliance.tex
+  ${CMAKE_SOURCE_DIR}/doc/header.tex
+  ${CMAKE_SOURCE_DIR}/doc/using-energyplus-for-compliance/src/using-energyplus-for-compliance.tex
+  ${CMAKE_SOURCE_DIR}/doc/using-energyplus-for-compliance/src/introduction.tex
+  ${CMAKE_SOURCE_DIR}/doc/using-energyplus-for-compliance/src/introduction/background.tex
+  ${CMAKE_SOURCE_DIR}/doc/using-energyplus-for-compliance/src/introduction/compliance-objects.tex
+  ${CMAKE_SOURCE_DIR}/doc/using-energyplus-for-compliance/src/introduction/tabular-summary-reports.tex
+  ${CMAKE_SOURCE_DIR}/doc/using-energyplus-for-compliance/src/introduction/features-related-to-appendix-g-and-leed.tex
+  ${CMAKE_SOURCE_DIR}/doc/using-energyplus-for-compliance/src/introduction/features-related-to-california-title-24.tex
+)
+
+# to get the list of inluded images, go to the root of the document folder and:
+# grep -r '\\includegraphics' * | cut -d ':' -f 2 | rev | cut -d '{' -f 1 | rev | cut -d '}' -f 1 | sed 's/^/  /g' | sort -n -t'.' -k 1.14
+SET( INCLUDED_IMAGES 
+) 
+
+SET( SOURCE_FILENAME "using-energyplus-for-compliance" )
+SET( OUTPUT_FILENAME "UsingEnergyPlusForCompliance" )
+
+FILE(MAKE_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME})
+
+add_custom_command( OUTPUT ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+	COMMAND ${CMAKE_COMMAND} -DXELATEX=${XELATEX} -DINNAME=${SOURCE_FILENAME} -DOUTNAME=${OUTPUT_FILENAME} -DORIGINAL_CMAKE_SOURCE_DIR=${CMAKE_SOURCE_DIR} -DORIGINAL_CMAKE_BINARY_DIR=${CMAKE_BINARY_DIR} -P ${CMAKE_SOURCE_DIR}/cmake/BuildDocumentation.cmake
+		    WORKING_DIRECTORY ${CMAKE_BINARY_DIR}/doc-build/${SOURCE_FILENAME}
+		    DEPENDS ${INCLUDED_TEX} ${INCLUDED_IMAGES}
+                 ) 
+add_custom_target( zPDF_${OUTPUT_FILENAME} ALL
+                   DEPENDS ${CMAKE_BINARY_DIR}/doc-build/${OUTPUT_FILENAME}.pdf
+                 )
diff --git a/doc/src/docs/Using_EnergyPlus_for_Compliance/media/ep.gif b/doc/using-energyplus-for-compliance/media/ep.gif
similarity index 100%
rename from doc/src/docs/Using_EnergyPlus_for_Compliance/media/ep.gif
rename to doc/using-energyplus-for-compliance/media/ep.gif
diff --git a/doc/using-energyplus-for-compliance/media/ep.png b/doc/using-energyplus-for-compliance/media/ep.png
new file mode 100644
index 00000000000..a808760c870
Binary files /dev/null and b/doc/using-energyplus-for-compliance/media/ep.png differ
diff --git a/doc/using-energyplus-for-compliance/src/introduction.tex b/doc/using-energyplus-for-compliance/src/introduction.tex
new file mode 100644
index 00000000000..580eb9302ed
--- /dev/null
+++ b/doc/using-energyplus-for-compliance/src/introduction.tex
@@ -0,0 +1 @@
+\chapter{Introduction}\label{introduction}
diff --git a/doc/using-energyplus-for-compliance/src/introduction/background.tex b/doc/using-energyplus-for-compliance/src/introduction/background.tex
new file mode 100644
index 00000000000..933cc8a5bb7
--- /dev/null
+++ b/doc/using-energyplus-for-compliance/src/introduction/background.tex
@@ -0,0 +1,7 @@
+\section{Background}\label{background}
+
+Energy Standards abound throughout the world. This document provides guidance on using EnergyPlus and its reports for compliance with energy standards.
+
+The tabular reports from EnergyPlus were designed to help collate information into a form usually required for reporting on designs for energy use. The tabular reports are fully described in the Output Details document and will be judiciously reproduced here for clarity and reference. In addition, by using the Output:Table:Style object, one can obtain the reports in a variety of formats -- ready for incorporating into your own style for submission or presentation.
+
+First, we describe the features available in the tabular report that might be used for energy compliance reporting or presentation of energy designs to clients.
diff --git a/doc/using-energyplus-for-compliance/src/introduction/compliance-objects.tex b/doc/using-energyplus-for-compliance/src/introduction/compliance-objects.tex
new file mode 100644
index 00000000000..58b4395e80a
--- /dev/null
+++ b/doc/using-energyplus-for-compliance/src/introduction/compliance-objects.tex
@@ -0,0 +1,3 @@
+\section{Compliance Objects}\label{compliance-objects}
+
+To facilitate using EnergyPlus for compliance reporting, a group of Compliance Objects is described in the Input Output Reference document. Currently, there is only one object in this group: \textbf{Compliance:Building} which, when fully populated, will describe various aspects that are needed specific to buildings. Other compliance objects will be added to this group when appropriate.
diff --git a/doc/using-energyplus-for-compliance/src/introduction/features-related-to-appendix-g-and-leed.tex b/doc/using-energyplus-for-compliance/src/introduction/features-related-to-appendix-g-and-leed.tex
new file mode 100644
index 00000000000..16929638331
--- /dev/null
+++ b/doc/using-energyplus-for-compliance/src/introduction/features-related-to-appendix-g-and-leed.tex
@@ -0,0 +1,391 @@
+\section{Features Related to Appendix G and LEED}\label{features-related-to-appendix-g-and-leed}
+
+EnergyPlus has several built-in features to make demonstrating compliance with ASHRAE Standard 90.1 Appendix G easier. Appendix G is used in Energy and Atmosphere Credit 1 Optimize Energy Performance of the U.S. Green Building Council (USGBC) building certification system called Leadership in Energy and Environmental Design (LEED) Green Building Rating Systemâ„¢. The following sections describe the features.
+
+\subsection{Baseline Building Rotations}\label{baseline-building-rotations}
+
+Table G3.1 Section 5 Building Envelope of ASHRAE Standard 90.1 Appendix G requires that the baseline building be simulated facing four directions:
+
+Orientation. The baseline building performance shall be generated by simulating the building with its actual orientation and again after rotating the entire building 90, 180, and 270 degrees, then averaging the results.
+
+This provision intends to provide a baseline that is neutral to building orientation so that buildings purposely oriented to minimize energy use can realize a percent savings.
+
+\textbf{Step 1.} The first step of performing the building rotations is to include a Compliance:Building object which contains the Building Rotation for Appendix G field. The value of the field should be different for four simulations, 0, 90, 180 and 270 (see Step 2 below). This is further documented in the Input Output Reference.
+
+\begin{lstlisting}
+
+Compliance:Building,
+      90;                 Building Rotation for Appendix G
+\end{lstlisting}
+
+Also make sure that the HTML summary reports will be generated by including the following:
+
+\begin{lstlisting}
+
+OutputControl:Table:Style,
+    HTML;                      !- type
+
+  Output:Table:SummaryReports,
+    AllSummary;                !- type
+\end{lstlisting}
+
+\textbf{Step 2.} The ParametricPreprocessor automates the creation of the four simulation input files so that only a single simulation file is needs to be created by the user. By setting the file name suffixes (which are appended to the existing file name for each simulation), setting a variable that varies for the four simulations, and setting the Building Rotation for Appendix G to this variable, the user can automatically create the four files when using EnergyPlus. The following example shows what should be included in the EnergyPlus file. The Parametric objects are described further in the Input Output Reference and the ParametricPreprocessor is described in the Auxiliary Programs documentation.
+
+\begin{lstlisting}
+Parametric:FileNameSuffix,
+  Names,
+  G000,
+  G090,
+  G180,
+  G270;
+\end{lstlisting}
+
+\begin{lstlisting}
+Parametric:SetValueForRun,
+  $appGAngle,            !- Parameter Name
+  0.0,                   !- Value 1
+  90.0,                  !- Value 2
+  180.0,                 !- Value 3
+  270.0;                 !- Value 4
+\end{lstlisting}
+
+\begin{lstlisting}
+Compliance:Building,
+    = $appGAngle;        !- Building Rotation for Appendix G {deg}
+\end{lstlisting}
+
+\begin{lstlisting}
+OutputControl:Table:Style,
+  HTML;                      !- type
+\end{lstlisting}
+
+\begin{lstlisting}
+Output:Table:SummaryReports,
+  AllSummary;                !- type
+\end{lstlisting}
+
+\textbf{Step 3.} Run the simulation using EP-Launch. Using the ``Single Input File'' tab of EP-Launch select the input that contains the Compliance:Building, Parametric:FileNameSuffix, Parametric:SetValueForRun objects as shown above in Step 2 as well as the weather file. In EP-Launch, make sure under VIEW .. OPTIONS .. MISCELLANEOUS that the RUN PARAMETRICPREPROCESSOR option is checked.
+
+\textbf{Step 4}. Review the results and revise the model inputs as needed. You can view the results of the simulation by using the EP-Launch and the History tab. At the bottom of the history list, four simulations that use the G000, G090, G180 and G270 file name suffixes should appear and the result files associated with each can be selected and opened.
+
+\textbf{Step 5.} Use the AppGPostProcess to average results across the simulations. In EP-Launch under the UTILITIES tab, select AppGPostProcess utility and select one of the HTML files resulting from the multiple simulation runs (e.g., \textless{}filename\textgreater{}-G000.html). This will open all four files and generate a new output file with the file suffix GAVG for the HTML and other results files that can be opened on that tab.
+
+\subsection{Completing LEED Forms from Tabular Reports}\label{completing-leed-forms-from-tabular-reports}
+
+The U.S. Green Building Council building certification system called Leadership in Energy and Environmental Design (LEED) Green Building Rating Systemâ„¢ includes Energy and Atmosphere Credit 1 Optimize Energy Performance. Credit 1 includes an option that requires a series of building energy simulations that follow the procedures of ASHRAE Standard 90.1 Appendix G Performance Rating Method. The~ LEED Summary report provides many of the simulation results required for the forms. The report can be produced by specifying LEEDSummary in Output:Table:SummaryReports which is also part of the AllSummary option.
+
+Report: \textbf{LEED Summary}
+
+For: \textbf{Entire Facility}
+
+Timestamp: \textbf{2013-03-01 15:24:37}
+
+\textbf{Sec1.1A-General Information}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{EAp2-1. Space Usage Type}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{EAp2-2. Advisory Messages}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{EAp2-3. Energy Type Summary}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{EAp2-4/5. Performance Rating Method Compliance}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{EAp2-6. Energy Use Summary}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{EAp2-7. Energy Cost Summary}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\emph{Process energy cost based on ratio of process to total energy.}
+
+\textbf{L-1. Renewable Energy Source Summary}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{EAp2-17a. Energy Use Intensity - Electricity}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{EAp2-17b. Energy Use Intensity - Natural Gas}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{EAp2-17c. Energy Use Intensity - Other}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{EAp2-18. End Use Percentage}
+
+\begin{longtable}[c]{@{}ll@{}}
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+ & Percent [\%] \tabularnewline
+\midrule
+\endhead
+
+Interior Lighting & 18.93 \tabularnewline
+Space Heating & 24.22 \tabularnewline
+Space Cooling & 4.11 \tabularnewline
+Fans-Interior & 1.63 \tabularnewline
+Service Water Heating & 0.00 \tabularnewline
+Receptacle Equipment & 11.11 \tabularnewline
+Miscellaneous & 39.99 \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsubsection{LEED Form Section 1.4 -- Comparison of Proposed Design Versus Baseline Design}\label{leed-form-section-1.4-comparison-of-proposed-design-versus-baseline-design}
+
+Unlike other portions of the LEED forms, Section 1.4 Comparison of Proposed Design Versus Baseline Design is less structured with many possible ``Model Input Parameters'' to match with the ``Proposed Design Input'' and ``Baseline Design Input''.
+
+\emph{1. Exterior wall, underground wall, roof, floor, and slab assemblies including framing type, assembly R-values, assembly U-factors, and roof reflectivity when modeling cool roofs. (Refer to ASHRAE 90.1 Appendix A)}
+
+Use the values from the Envelope Summary table, Opaque Exterior subtable for Construction, Reflectance, U-Factor with Film, and U-Factor no Film.
+
+\emph{2. Fenestration types, assembly U-factors (including the impact of the frame on the assembly, SHGCs, and visual light transmittances, overall window-to-gross wall ratio, fixed shading devices, and automated movable shading devices}
+
+Use the values from Input Verification and Results Summary table, Window-Wall Ratio table Window-Wall Ratio percentage as well as Skylight-Roof Ratio table. Also use the values from the Envelope Summary table, Fenestration subtable for Construction, Area of Openings, U-Factor, SHGC, Visible Transmittance, and Shade Control. For shading use the Shading Summary report including Sunlit Fraction and Window Control.
+
+\emph{3. Interior lighting power densities, exterior lighting power, process lighting power, and lighting controls modeled for credit.}
+
+Use the values from the Lighting Summary report for Interior Lighting, Daylighting and Exterior Lighting including Lighting Power Density, Schedule Name, Average Hours/Week, Daylighting Type, Control Type, Fraction Controlled, Lighting Installed in Zone, Lighting Controlled.
+
+\emph{4. Receptacle equipment, elevators or escalators, refrigeration equipment and other process loads.}
+
+Use the values from Input Verification and Results Summary table, Zone Summary subtable for Plug and Process.
+
+\emph{5. HVAC system information including types and efficiencies, exhaust heat recovery, pump power and controls, and other pertinent system information. (Include the ASRHAE 90.1-2004 Table G3.1.1B Baseline System Number)}
+
+Use the Equipment Summary report, Central Plant subtable for Type, Nominal Capacity and Nominal Efficiency; Cooling Coils subtable for Nominal Total Capacity and Nominal Efficiency; Heating Coils subtable for Type, Nominal Total Capacity and Nominal Efficiency; Fans subtable for Type, Total Efficiency, Delta Pressure, Max Flow Rate, Rated Power, Motor Heat in Air Fraction; Pumps subtable for Type, Control, Head, Power and Motor Efficiency. Use the System Summary report, Economizer subtable for High Limit Shutoff Control and Minimum Outdoor Air; the Demand Controlled Ventilation using Controller:MechanicalVentilation subtable.
+
+\emph{6. Domestic hot water system type, efficiency and storage tank volume.}
+
+Use the Equipment Summary report, Service Water Heating subtable for Type, Storage Volume, Input, Thermal Efficiency, Recovery Efficiency, and Energy Factor.
+
+\emph{7. General schedule information.}
+
+Use the Lighting Summary report, Interior Lighting subtable Schedule Name and Average Hours/Week; Exterior Lighting subtable Schedule Name and Average Hours/Week. Use the System Summary report, Demand Controlled Ventilation using Controller:MechanicalVentilation subtable for the Air Distribution Effectiveness Schedule.
diff --git a/doc/using-energyplus-for-compliance/src/introduction/features-related-to-california-title-24.tex b/doc/using-energyplus-for-compliance/src/introduction/features-related-to-california-title-24.tex
new file mode 100644
index 00000000000..9c3d60031eb
--- /dev/null
+++ b/doc/using-energyplus-for-compliance/src/introduction/features-related-to-california-title-24.tex
@@ -0,0 +1,5 @@
+\section{Features Related to California Title 24 Compliance}\label{features-related-to-california-title-24-compliance}
+
+EnergyPlus has a reporting feature that is useful for obtaining Time Dependant Valuation (TDV) of source energy use for the entire facility being simulated. Hourly variations of fuel factors can be specified through the `FuelFactors' input object and will be used to calculate TDV based source energy consumption broken down by end uses. The Source Energy End Use Components Summary report above provides these TDV based values. The source energy consumption is also reported based on area normalized metrics. Refer to `Fuel Factors' and `Output:Table:SummaryReports' in the Input-Output Reference manual for more details.
+
+Also included is the California\_Title\_24-2008.idf dataset (described briefly in the Output Details document).
diff --git a/doc/using-energyplus-for-compliance/src/introduction/tabular-summary-reports.tex b/doc/using-energyplus-for-compliance/src/introduction/tabular-summary-reports.tex
new file mode 100644
index 00000000000..b612f92cb8d
--- /dev/null
+++ b/doc/using-energyplus-for-compliance/src/introduction/tabular-summary-reports.tex
@@ -0,0 +1,681 @@
+\section{Tabular Summary Reports}\label{tabular-summary-reports}
+
+Several predefined reports are available from the Output Table:Predefined object including the following.
+
+\begin{itemize}
+\item
+  Annual Building Utility Performance Summary
+\item
+  Input Verification and Results Summary
+\item
+  Demand End Use Components Summary
+\item
+  Source Energy End Use Components Summary
+\item
+  Climatic Data Summary
+\item
+  Equipment Summary
+\item
+  Envelope Summary
+\item
+  Surface Shadowing Summary
+\item
+  Shading Summary
+\item
+  Lighting Summary
+\item
+  HVAC Sizing Summary
+\item
+  System Summary
+\item
+  Component Sizing Summary
+\item
+  Outside Air Summary
+\item
+  Object Count Summary
+\end{itemize}
+
+In addition, specifying ``All Summary'' will enable all the reports in this category (more than are shown here).
+
+\subsection{Annual Building Utility Performance Summary}\label{annual-building-utility-performance-summary}
+
+First and foremost, the Annual Building Utility Performance Summary gives a good overview of the energy use by category:
+
+Report: \textbf{AnnualBuildingUtilityPerformanceSummary}
+
+For: \textbf{Entire Facility}
+
+Timestamp: \textbf{2009-09-17 17:30:22}
+
+Values gathered over 8760.00 hours
+
+Site and Source Energy
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Source to Site Energy Conversion Factors
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Building Area
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+End Uses
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\emph{Note: Natural gas appears to be the principal heating source based on energy usage.}
+
+End Uses By Subcategory
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Normalized Metrics
+
+Utility Use Per Conditioned Floor Area
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Utility Use Per Total Floor Area
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Electric Loads Satisfied
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+On-Site Thermal Sources
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Water Source Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Comfort and Setpoint Not Met Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Note 1: An asterisk (*) indicates that the feature is not yet implemented.
+
+\subsection{Input Verification Summary}\label{input-verification-summary}
+
+The input verification summary gives a good overview of the facility being simulated:
+
+Report: \textbf{InputVerificationandResultsSummary}
+
+For: \textbf{Entire Facility}
+
+\textbf{Timestamp: 2009-09-17 17:30:22}
+
+General
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+ENVELOPE
+
+Window-Wall Ratio
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Skylight-Roof Ratio
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+PERFORMANCE
+
+Zone Summary
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Source Energy End Use Components Summary}\label{source-energy-end-use-components-summary}
+
+The source energy end use components summary gives a good overview of the source energy consumption broken down by end uses for the facility being simulated:
+
+Report: \textbf{SourceEnergyEndUseComponentsSummary}
+
+For: \textbf{Entire Facility}
+
+Timestamp: \textbf{2011-10-07 20:53:43}
+
+\textbf{Values gathered over 8760.00 hours}
+
+\textbf{Source Energy End Use Components Summary}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{Normalized Metrics}
+
+\textbf{Source Energy End Use Components Per Conditioned Floor Area}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\textbf{Source Energy End Use Components Per Total Floor Area}
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\subsection{Other Summary Reports}\label{other-summary-reports}
+
+The Climatic Data Summary, Envelope Summary and Equipment Summary reports might be quite important to some reporting or presentation.
+
+Report: \textbf{ClimaticDataSummary}
+
+For: \textbf{Entire Facility}
+
+\textbf{Timestamp: 2009-09-17 17:30:22}
+
+SizingPeriod:DesignDay
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Weather Statistics File
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Report: \textbf{EnvelopeSummary}
+
+For: \textbf{Entire Facility}
+
+\textbf{Timestamp: 2009-09-17 17:30:22}
+
+Opaque Exterior
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Fenestration
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+\begin{center}\rule{0.5\linewidth}{\linethickness}\end{center}
+
+Report: \textbf{ShadingSummary}
+
+For: \textbf{Entire Facility}
+
+\textbf{Timestamp: 2009-09-17 17:30:22}
+
+Sunlit Fraction
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Window Control
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Report: \textbf{LightingSummary}
+
+For: \textbf{Entire Facility}
+
+\textbf{Timestamp: 2009-09-17 17:30:22}
+
+Interior Lighting
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Daylighting
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Exterior Lighting
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Report: \textbf{EquipmentSummary}
+
+For: \textbf{Entire Facility}
+
+\textbf{Timestamp: 2009-09-17 17:30:22}
+
+Central Plant
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Cooling Coils
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Heating Coils
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Fans
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Pumps
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
+
+Service Water Heating
+
+\begin{longtable}[c]{p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}p{0.85in}}
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endfirsthead
+
+\toprule 
+~ & Type & Storage Volume [m3] & Input [W] & Thermal Efficiency [W/W] & Recovery Efficiency [W/W] & Energy Factor \tabularnewline
+\midrule
+\endhead
+
+None & ~ & ~ & ~ & ~ & ~ & ~ \tabularnewline
+\bottomrule
+\end{longtable}
diff --git a/doc/using-energyplus-for-compliance/src/using-energyplus-for-compliance.tex b/doc/using-energyplus-for-compliance/src/using-energyplus-for-compliance.tex
new file mode 100644
index 00000000000..63f37402bb8
--- /dev/null
+++ b/doc/using-energyplus-for-compliance/src/using-energyplus-for-compliance.tex
@@ -0,0 +1 @@
+\input{../title}
diff --git a/doc/using-energyplus-for-compliance/using-energyplus-for-compliance.tex b/doc/using-energyplus-for-compliance/using-energyplus-for-compliance.tex
new file mode 100644
index 00000000000..de61beab3f3
--- /dev/null
+++ b/doc/using-energyplus-for-compliance/using-energyplus-for-compliance.tex
@@ -0,0 +1,32 @@
+\input{../header}
+
+\title{Using EnergyPlus for Compliance}
+
+\hypersetup{unicode=true,
+            pdftitle={Using EnergyPlus for Compliance},
+            pdfauthor={U.S. Department of Energy},
+            colorlinks=true,
+            linkcolor=Maroon,
+            citecolor=Blue,
+            urlcolor=Blue,
+            breaklinks=true}
+\urlstyle{same}  % don't use monospace font for urls
+
+\begin{document}
+
+
+\input{src/using-energyplus-for-compliance}
+
+\input{src/introduction}
+
+\input{src/introduction/background}
+
+\input{src/introduction/compliance-objects}
+
+\input{src/introduction/tabular-summary-reports}
+
+\input{src/introduction/features-related-to-appendix-g-and-leed}
+
+\input{src/introduction/features-related-to-california-title-24}
+
+\end{document}
diff --git a/idd/Energy+.idd.in b/idd/Energy+.idd.in
index 7928f21b407..724d235c91f 100644
--- a/idd/Energy+.idd.in
+++ b/idd/Energy+.idd.in
@@ -296,6 +296,7 @@
 !      s/m                    =>   s/ft                0.3048
 !      V/K                    =>   V/F                 0.555555555555556
 !      W                      =>   Btu/h               3.4121412858518
+!      W/((m3/s)-Pa)          =>   W/((gal/min)-ftH20) 0.188582274697355
 !      W/(m3/s)               =>   W/(ft3/min)         0.0004719475
 !      W/K                    =>   Btu/h-F             1.89563404769544
 !      W/m                    =>   Btu/h-ft            1.04072
@@ -312,24 +313,30 @@
 !
 !      kPa                    =>   inHg                0.29523
 !      m                      =>   in                  39.3700787401575
+!      m3/hr                  =>   gal/hr              264.172037284185
+!      m3/hr-m2               =>   gal/hr-ft2          24.5423853466941
+!      m3/hr-person           =>   gal/hr-person       264.172037284185
+!      m3/m2                  =>   gal/ft2             24.5423853466941
+!      m3/person              =>   gal/person          264.172037284185
 !      m3/s                   =>   gal/min             15850.3222370511
+!      m3/s-m                 =>   gal/min-ft          4831.17821785317
+!      m3/s-W                 =>   (gal/min)/(Btu/h)   4645.27137336702
 !      Pa                     =>   ftH2O               0.00033455
 !      Pa                     =>   inH2O               0.00401463
 !      Pa                     =>   inHg                0.00029613
 !      Pa                     =>   Pa                  1
 !      W                      =>   W                   1
+!      W/(m3/s)               =>   W/(gal/min)         0.0000630902
 !      W/m2                   =>   W/m2                1
 !      W/m-K                  =>   Btu/h-ft-F          0.577796066000163
 !      W/person               =>   W/person            1
-!      W/(m3/s)               =>   W/(gal/min)         0.0000630902
-!      W/((m3/s)-Pa)          =>   W/((gal/min)-ftH20) 0.188554
 !
 ! Units fields that are not translated
 !      $
 !      1/hr
 !      A
+!      A/V                 
 !      Ah
-!      A/V
 !      Availability
 !      Control
 !      cycles/hr
@@ -63513,7 +63520,7 @@ CoolingTower:VariableSpeed:Merkel,
   N6 , \field Design Water Flow Rate per Unit of Nominal Capacity
        \note This field is only used if the previous is set to autocalculate and performance input method is NominalCapacity
        \units m3/s-W
-       \ip-units gal/min-W
+       \ip-units (gal/min)/(Btu/h)
        \default 5.382E-8
        \type real
   N7 , \field Design Air Flow Rate
@@ -66446,8 +66453,8 @@ WaterHeater:Sizing,
        \minimum 1
   N6 , \field Storage Capacity per Person
        \type real
-       \units m3/Person
-       \ip-units gal/Person
+       \units m3/person
+       \ip-units gal/person
        \note Only used for Design Mode = PerPerson
        \minimum 0.0
   N7 , \field Recovery Capacity per Person
diff --git a/src/EnergyPlus/DXCoils.cc b/src/EnergyPlus/DXCoils.cc
index 1bf975d1ae9..4df62a0cc0e 100644
--- a/src/EnergyPlus/DXCoils.cc
+++ b/src/EnergyPlus/DXCoils.cc
@@ -5404,7 +5404,8 @@ namespace DXCoils {
 		Numbers2.deallocate();
 		lAlphaBlanks2.deallocate();
 		lNumericBlanks2.deallocate();
-		ManageEMS( emsCallFromComponentGetInput );
+		bool anyEMSRan;
+		ManageEMS( emsCallFromComponentGetInput, anyEMSRan );
 
 	}
 
@@ -10661,12 +10662,19 @@ Label50: ;
 		AirMassFlow = DXCoil( DXCoilNum ).InletAirMassFlowRate;
 		AirMassFlowRatioLS = MSHPMassFlowRateLow / DXCoil( DXCoilNum ).MSRatedAirMassFlowRate( SpeedNumLS );
 		AirMassFlowRatioHS = MSHPMassFlowRateHigh / DXCoil( DXCoilNum ).MSRatedAirMassFlowRate( SpeedNumHS );
-		if ( ( AirMassFlow > 0.0 ) && ( CycRatio > 0.0 ) && ( ( MSHPMassFlowRateLow == 0.0 ) || ( MSHPMassFlowRateHigh == 0.0 ) ) ) {
+		if ( ( AirMassFlow > 0.0 ) && ( CycRatio > 0.0 ) && ( MSHPMassFlowRateHigh == 0.0 ) ) {
 			ShowSevereError( "CalcMultiSpeedDXCoilCooling: " + DXCoil( DXCoilNum ).DXCoilType + " \"" + DXCoil( DXCoilNum ).Name + " Developer error - inconsistent airflow rates." );
-			ShowContinueError( "When AirMassFlow > 0.0 and CycRatio > 0.0, then MSHPMassFlowRateLow and MSHPMassFlowRateHigh must also be > 0.0" );
-			ShowContinueErrorTimeStamp( "" );
-			ShowContinueError( "AirMassFlow = " + RoundSigDigits( AirMassFlow, 3 ) + ",CycRatio = " + RoundSigDigits( CycRatio, 3 ) + ", MSHPMassFlowRateLow = " + RoundSigDigits( MSHPMassFlowRateLow, 3 ) + ", MSHPMassFlowRateHigh = " + RoundSigDigits( MSHPMassFlowRateHigh, 3 ) );
-			ShowFatalError( "Preceding condition(s) causes termination." );
+			if ( MSHPMassFlowRateLow == 0.0 && SpeedNum > 1 ) {
+				ShowContinueError( "When AirMassFlow > 0.0 and CycRatio > 0.0 and SpeedNum > 1, then MSHPMassFlowRateLow and MSHPMassFlowRateHigh must also be > 0.0" );
+				ShowContinueErrorTimeStamp( "" );
+				ShowContinueError( "AirMassFlow=" + RoundSigDigits( AirMassFlow, 3 ) + ",CycRatio=" + RoundSigDigits( CycRatio, 3 ) + ",SpeedNum=" + RoundSigDigits( double( SpeedNum ), 0 ) + ", MSHPMassFlowRateLow=" + RoundSigDigits( MSHPMassFlowRateLow, 3 ) + ", MSHPMassFlowRateHigh=" + RoundSigDigits( MSHPMassFlowRateHigh, 3 ) );
+				ShowFatalError( "Preceding condition(s) causes termination." );
+			} else {
+				ShowContinueError( "When AirMassFlow > 0.0 and CycRatio > 0.0, then MSHPMassFlowRateHigh must also be > 0.0" );
+				ShowContinueErrorTimeStamp( "" );
+				ShowContinueError( "AirMassFlow=" + RoundSigDigits( AirMassFlow, 3 ) + ",CycRatio=" + RoundSigDigits( CycRatio, 3 ) + ", MSHPMassFlowRateHigh=" + RoundSigDigits( MSHPMassFlowRateHigh, 3 ) );
+				ShowFatalError( "Preceding condition(s) causes termination." );
+			}
 		} else if ( CycRatio > 1.0 || SpeedRatio > 1.0 ) {
 			ShowSevereError( "CalcMultiSpeedDXCoilCooling: " + DXCoil( DXCoilNum ).DXCoilType + " \"" + DXCoil( DXCoilNum ).Name + " Developer error - inconsistent speed ratios." );
 			ShowContinueError( "CycRatio and SpeedRatio must be between 0.0 and 1.0" );
@@ -10880,9 +10888,13 @@ Label50: ;
 					OutletAirHumRat = HSOutletAirHumRat;
 					OutletAirDryBulbTemp = HSOutletAirDryBulbTemp;
 				} else {
-					Hfg = PsyHfgAirFnWTdb( MinAirHumRat, HSOutletAirDryBulbTemp * SpeedRatio + ( 1.0 - SpeedRatio ) * LSOutletAirDryBulbTemp );
-					// Average outlet HR
-					OutletAirHumRat = InletAirHumRat - DXCoil( DXCoilNum ).LatCoolingEnergyRate / Hfg / DXCoil( DXCoilNum ).InletAirMassFlowRate;
+					if ( FanOpMode == ContFanCycCoil ) {
+						Hfg = PsyHfgAirFnWTdb( MinAirHumRat, HSOutletAirDryBulbTemp * SpeedRatio + ( 1.0 - SpeedRatio ) * LSOutletAirDryBulbTemp );
+						// Average outlet HR
+						OutletAirHumRat = InletAirHumRat - DXCoil( DXCoilNum ).LatCoolingEnergyRate / Hfg / DXCoil( DXCoilNum ).InletAirMassFlowRate;
+					} else {
+						OutletAirHumRat = ( HSOutletAirHumRat * SpeedRatio ) + ( LSOutletAirHumRat * ( 1.0 - SpeedRatio ) );
+					}
 					OutletAirDryBulbTemp = PsyTdbFnHW( OutletAirEnthalpy, OutletAirHumRat );
 					if ( OutletAirDryBulbTemp < OutletAirDryBulbTempSat ) { // Limit to saturated conditions at OutletAirEnthalpy
 						OutletAirDryBulbTemp = OutletAirDryBulbTempSat;
@@ -10934,7 +10946,7 @@ Label50: ;
 				DXCoil( DXCoilNum ).OutletAirTemp = OutletAirDryBulbTemp;
 				DXCoil( DXCoilNum ).CrankcaseHeaterPower = 0.0;
 
-			} else if ( CycRatio > 0.0 || ( CycRatio > 0.0 && SingleMode == 1 ) ) {
+			} else if ( CycRatio > 0.0 ) {
 
 				if ( FanOpMode == CycFanCycCoil ) AirMassFlow /= CycRatio;
 				if ( FanOpMode == ContFanCycCoil ) AirMassFlow = MSHPMassFlowRateHigh;
@@ -11309,12 +11321,19 @@ Label50: ;
 		AirMassFlow = DXCoil( DXCoilNum ).InletAirMassFlowRate;
 		AirMassFlowRatioLS = MSHPMassFlowRateLow / DXCoil( DXCoilNum ).MSRatedAirMassFlowRate( SpeedNumLS );
 		AirMassFlowRatioHS = MSHPMassFlowRateHigh / DXCoil( DXCoilNum ).MSRatedAirMassFlowRate( SpeedNumHS );
-		if ( ( AirMassFlow > 0.0 ) && ( CycRatio > 0.0 ) && ( ( MSHPMassFlowRateLow == 0.0 ) || ( MSHPMassFlowRateHigh == 0.0 ) ) ) {
+		if ( ( AirMassFlow > 0.0 ) && ( CycRatio > 0.0 ) && ( MSHPMassFlowRateHigh == 0.0 ) ) {
 			ShowSevereError( "CalcMultiSpeedDXCoilHeating: " + DXCoil( DXCoilNum ).DXCoilType + " \"" + DXCoil( DXCoilNum ).Name + " Developer error - inconsistent airflow rates." );
-			ShowContinueError( "When AirMassFlow > 0.0 and CycRatio > 0.0, then MSHPMassFlowRateLow and MSHPMassFlowRateHigh must also be > 0.0" );
-			ShowContinueErrorTimeStamp( "" );
-			ShowContinueError( "AirMassFlow=" + RoundSigDigits( AirMassFlow, 3 ) + ",CycRatio=" + RoundSigDigits( CycRatio, 3 ) + ", MSHPMassFlowRateLow=" + RoundSigDigits( MSHPMassFlowRateLow, 3 ) + ", MSHPMassFlowRateHigh=" + RoundSigDigits( MSHPMassFlowRateHigh, 3 ) );
-			ShowFatalError( "Preceding condition(s) causes termination." );
+			if ( MSHPMassFlowRateLow == 0.0 && SpeedNum > 1 ) {
+				ShowContinueError( "When AirMassFlow > 0.0 and CycRatio > 0.0 and SpeedNum > 1, then MSHPMassFlowRateLow and MSHPMassFlowRateHigh must also be > 0.0" );
+				ShowContinueErrorTimeStamp( "" );
+				ShowContinueError( "AirMassFlow=" + RoundSigDigits( AirMassFlow, 3 ) + ",CycRatio=" + RoundSigDigits( CycRatio, 3 ) + ",SpeedNum=" + RoundSigDigits( double( SpeedNum ), 0 ) + ", MSHPMassFlowRateLow=" + RoundSigDigits( MSHPMassFlowRateLow, 3 ) + ", MSHPMassFlowRateHigh=" + RoundSigDigits( MSHPMassFlowRateHigh, 3 ) );
+				ShowFatalError( "Preceding condition(s) causes termination." );
+			} else {
+				ShowContinueError( "When AirMassFlow > 0.0 and CycRatio > 0.0, then MSHPMassFlowRateHigh must also be > 0.0" );
+				ShowContinueErrorTimeStamp( "" );
+				ShowContinueError( "AirMassFlow=" + RoundSigDigits( AirMassFlow, 3 ) + ",CycRatio=" + RoundSigDigits( CycRatio, 3 ) + ", MSHPMassFlowRateHigh=" + RoundSigDigits( MSHPMassFlowRateHigh, 3 ) );
+				ShowFatalError( "Preceding condition(s) causes termination." );
+			}
 		} else if ( CycRatio > 1.0 || SpeedRatio > 1.0 ) {
 			ShowSevereError( "CalcMultiSpeedDXCoilHeating: " + DXCoil( DXCoilNum ).DXCoilType + " \"" + DXCoil( DXCoilNum ).Name + " Developer error - inconsistent speed ratios." );
 			ShowContinueError( "CycRatio and SpeedRatio must be between 0.0 and 1.0" );
diff --git a/src/EnergyPlus/DataPlantPipingSystems.hh b/src/EnergyPlus/DataPlantPipingSystems.hh
index 9c6a5e1f515..98d6213f8fc 100644
--- a/src/EnergyPlus/DataPlantPipingSystems.hh
+++ b/src/EnergyPlus/DataPlantPipingSystems.hh
@@ -919,8 +919,8 @@ namespace DataPlantPipingSystems {
 		bool DomainNeedsToBeMeshed;
 		bool IsActuallyPartOfAHorizontalTrench;
 		bool HasAPipeCircuit;
-		bool IsZoneCoupledSlab;
-		bool HasCoupledBasement;
+		bool HasZoneCoupledSlab;
+		bool HasZoneCoupledBasement;
 		// "Input" data structure variables
 		MeshExtents Extents;
 		MeshProperties Mesh;
@@ -996,8 +996,8 @@ namespace DataPlantPipingSystems {
 			DomainNeedsToBeMeshed( true ),
 			IsActuallyPartOfAHorizontalTrench( false ),
 			HasAPipeCircuit( true ),
-			IsZoneCoupledSlab( false ),
-			HasCoupledBasement( false ),
+			HasZoneCoupledSlab( false ),
+			HasZoneCoupledBasement( false ),
 			HasBasement( false ),
 			ZoneCoupledOSCMIndex( 0 ),
 			PerimeterOffset( 0.0 ),
diff --git a/src/EnergyPlus/DataSurfaces.cc b/src/EnergyPlus/DataSurfaces.cc
index 29249c08587..37ad5e394e8 100644
--- a/src/EnergyPlus/DataSurfaces.cc
+++ b/src/EnergyPlus/DataSurfaces.cc
@@ -106,20 +106,6 @@ namespace DataSurfaces {
 	// MODULE PARAMETER DEFINITIONS:
 	int const MaxSlatAngs( 19 );
 
-	// Parameters to indicate surface shape for use with the Surface
-	// derived type (see below):
-
-	int const Triangle( 1 );
-	int const Quadrilateral( 2 );
-	int const Rectangle( 3 );
-	int const Polygonal( 9 );
-	int const RectangularDoorWindow( 4 );
-	int const RectangularOverhang( 5 );
-	int const RectangularLeftFin( 6 );
-	int const RectangularRightFin( 7 );
-	int const TriangularWindow( 8 );
-	int const TriangularDoor( 9 );
-
 	// Parameters to indicate exterior boundary conditions for use with
 	// the Surface derived type (see below):
 	// Note:  Positive values correspond to an interzone adjacent surface
@@ -691,21 +677,21 @@ namespace DataSurfaces {
 		SurfaceData::
 		computed_shapeCat() const
 		{
-			if ( Shape == Triangle ) {
+			if ( Shape == SurfaceShape::Triangle ) {
 				return ShapeCat::Triangular;
-			} else if ( Shape == TriangularWindow ) {
+			} else if ( Shape == SurfaceShape::TriangularWindow ) {
 				return ShapeCat::Triangular;
-			} else if ( Shape == TriangularDoor ) {
+			} else if ( Shape == SurfaceShape::TriangularDoor ) {
 				return ShapeCat::Triangular;
-			} else if ( Shape == Rectangle ) {
+			} else if ( Shape == SurfaceShape::Rectangle ) {
 				return ShapeCat::Rectangular;
-			} else if ( Shape == RectangularDoorWindow ) {
+			} else if ( Shape == SurfaceShape::RectangularDoorWindow ) {
 				return ShapeCat::Rectangular;
-			} else if ( Shape == RectangularOverhang ) {
+			} else if ( Shape == SurfaceShape::RectangularOverhang ) {
 				return ShapeCat::Rectangular;
-			} else if ( Shape == RectangularLeftFin ) {
+			} else if ( Shape == SurfaceShape::RectangularLeftFin ) {
 				return ShapeCat::Rectangular;
-			} else if ( Shape == RectangularRightFin ) {
+			} else if ( Shape == SurfaceShape::RectangularRightFin ) {
 				return ShapeCat::Rectangular;
 			} else if ( IsConvex ) {
 				return ShapeCat::Convex;
diff --git a/src/EnergyPlus/DataSurfaces.hh b/src/EnergyPlus/DataSurfaces.hh
index 5421efa40b9..2671273c1d0 100644
--- a/src/EnergyPlus/DataSurfaces.hh
+++ b/src/EnergyPlus/DataSurfaces.hh
@@ -93,16 +93,19 @@ namespace DataSurfaces {
 	// Parameters to indicate surface shape for use with the Surface
 	// derived type (see below):
 
-	extern int const Triangle;
-	extern int const Quadrilateral;
-	extern int const Rectangle;
-	extern int const Polygonal;
-	extern int const RectangularDoorWindow;
-	extern int const RectangularOverhang;
-	extern int const RectangularLeftFin;
-	extern int const RectangularRightFin;
-	extern int const TriangularWindow;
-	extern int const TriangularDoor;
+	enum class SurfaceShape : int {
+		None = 0,
+		Triangle,
+		Quadrilateral,
+		Rectangle,
+		RectangularDoorWindow,
+		RectangularOverhang,
+		RectangularLeftFin,
+		RectangularRightFin,
+		TriangularWindow,
+		TriangularDoor,
+		Polygonal
+	};
 
 	// Parameters to indicate exterior boundary conditions for use with
 	// the Surface derived type (see below):
@@ -585,7 +588,7 @@ namespace DataSurfaces {
 		int ConstructionStoredInputValue; // holds the original value for Construction per surface input
 		int Class;
 		// Geometry related parameters
-		int Shape; // Surface shape (Triangle=1,Quadrilateral=2,Rectangle=3,
+		SurfaceShape Shape; // Surface shape (Triangle=1,Quadrilateral=2,Rectangle=3,
 		//                Rectangular Window/Door=4,Rectangular Overhang=5,
 		//                Rectangular Left Fin=6,Rectangular Right Fin=7,
 		//                Triangular Window=8)
@@ -756,7 +759,7 @@ namespace DataSurfaces {
 			EMSConstructionOverrideValue( 0 ),
 			ConstructionStoredInputValue( 0 ),
 			Class( 0 ),
-			Shape( 0 ),
+			Shape( SurfaceShape::None ),
 			Sides( 0 ),
 			Area( 0.0 ),
 			GrossArea( 0.0 ),
diff --git a/src/EnergyPlus/DirectAirManager.cc b/src/EnergyPlus/DirectAirManager.cc
index a3070d8f0d0..4b098e5af1c 100644
--- a/src/EnergyPlus/DirectAirManager.cc
+++ b/src/EnergyPlus/DirectAirManager.cc
@@ -511,6 +511,7 @@ namespace DirectAirManager {
 				} else {
 					Node( ZoneNode ).MassFlowRate = 0.0;
 					Node( ZoneNode ).MassFlowRateMaxAvail = 0.0;
+					Node( ZoneNode ).MassFlowRateMinAvail = 0.0;
 				}
 			} else { // EMS override on
 				Node( ZoneNode ).MassFlowRate = DirectAir( DirectAirNum ).EMSMassFlowRateValue;
diff --git a/src/EnergyPlus/EMSManager.cc b/src/EnergyPlus/EMSManager.cc
index 267a5bb396e..07c8a1ed47b 100644
--- a/src/EnergyPlus/EMSManager.cc
+++ b/src/EnergyPlus/EMSManager.cc
@@ -276,6 +276,7 @@ namespace EMSManager {
 	void
 	ManageEMS(
 		int const iCalledFrom, // indicates where subroutine was called from, parameters in DataGlobals.
+		bool & anyProgramRan, // true if any Erl programs ran for this call 
 		Optional_int_const ProgramManagerToRun // specific program manager to run
 	)
 	{
@@ -327,11 +328,12 @@ namespace EMSManager {
 		int ErlProgramNum; // local index
 		int ActuatorUsedLoop; // local loop
 		int EMSActuatorVariableNum;
-		bool AnyProgramRan; // local logical
+
 		int tmpInteger;
 		//  INTEGER  :: ProgramNum
 
 		// FLOW:
+		anyProgramRan = false;
 		if ( ! AnyEnergyManagementSystemInModel ) return; // quick return if nothing to do
 
 		if ( iCalledFrom == emsCallFromBeginNewEvironment ) BeginEnvrnInitializeRuntimeLanguage();
@@ -344,14 +346,14 @@ namespace EMSManager {
 		}
 
 		// Run the Erl programs depending on calling point.
-		AnyProgramRan = false;
+
 		if ( iCalledFrom != emsCallFromUserDefinedComponentModel ) {
 			for ( ProgramManagerNum = 1; ProgramManagerNum <= NumProgramCallManagers; ++ProgramManagerNum ) {
 
 				if ( EMSProgramCallManager( ProgramManagerNum ).CallingPoint == iCalledFrom ) {
 					for ( ErlProgramNum = 1; ErlProgramNum <= EMSProgramCallManager( ProgramManagerNum ).NumErlPrograms; ++ErlProgramNum ) {
 						EvaluateStack( EMSProgramCallManager( ProgramManagerNum ).ErlProgramARR( ErlProgramNum ) );
-						AnyProgramRan = true;
+						anyProgramRan = true;
 					}
 				}
 			}
@@ -359,16 +361,16 @@ namespace EMSManager {
 			if ( present( ProgramManagerToRun ) ) {
 				for ( ErlProgramNum = 1; ErlProgramNum <= EMSProgramCallManager( ProgramManagerToRun ).NumErlPrograms; ++ErlProgramNum ) {
 					EvaluateStack( EMSProgramCallManager( ProgramManagerToRun ).ErlProgramARR( ErlProgramNum ) );
-					AnyProgramRan = true;
+					anyProgramRan = true;
 				}
 			}
 		}
 
 		if ( iCalledFrom == emsCallFromExternalInterface ) {
-			AnyProgramRan = true;
+			anyProgramRan = true;
 		}
 
-		if ( ! AnyProgramRan ) return;
+		if ( ! anyProgramRan ) return;
 
 		// Set actuated variables with new values
 		for ( ActuatorUsedLoop = 1; ActuatorUsedLoop <= numActuatorsUsed + NumExternalInterfaceActuatorsUsed + NumExternalInterfaceFunctionalMockupUnitImportActuatorsUsed + NumExternalInterfaceFunctionalMockupUnitExportActuatorsUsed; ++ActuatorUsedLoop ) {
diff --git a/src/EnergyPlus/EMSManager.hh b/src/EnergyPlus/EMSManager.hh
index d6269903c09..d1ba698caab 100644
--- a/src/EnergyPlus/EMSManager.hh
+++ b/src/EnergyPlus/EMSManager.hh
@@ -106,6 +106,7 @@ namespace EMSManager {
 	void
 	ManageEMS(
 		int const iCalledFrom, // indicates where subroutine was called from, parameters in DataGlobals.
+		bool & anyProgramRan, // true if any Erl programs ran for this call 
 		Optional_int_const ProgramManagerToRun = _ // specific program manager to run
 	);
 
diff --git a/src/EnergyPlus/ExternalInterface.cc b/src/EnergyPlus/ExternalInterface.cc
index 01960cb12c9..c3a73d3ff37 100644
--- a/src/EnergyPlus/ExternalInterface.cc
+++ b/src/EnergyPlus/ExternalInterface.cc
@@ -885,7 +885,8 @@ namespace ExternalInterface {
 
 		// If we have Erl variables, we need to call ManageEMS so that they get updated in the Erl data structure
 		if ( useEMS ) {
-			ManageEMS( emsCallFromExternalInterface );
+			bool anyRan;
+			ManageEMS( emsCallFromExternalInterface, anyRan );
 		}
 
 		FirstCallGetSetDoStep = false;
@@ -2154,7 +2155,8 @@ namespace ExternalInterface {
 
 		// If we have Erl variables, we need to call ManageEMS so that they get updated in the Erl data structure
 		if ( useEMS ) {
-			ManageEMS( emsCallFromExternalInterface );
+			bool anyRan;
+			ManageEMS( emsCallFromExternalInterface, anyRan );
 		}
 
 		firstCall = false; // bug fix causing external interface to send zero at the beginning of sim, Thierry Nouidui
diff --git a/src/EnergyPlus/FanCoilUnits.cc b/src/EnergyPlus/FanCoilUnits.cc
index e5f47c87670..610061c7437 100644
--- a/src/EnergyPlus/FanCoilUnits.cc
+++ b/src/EnergyPlus/FanCoilUnits.cc
@@ -1770,7 +1770,7 @@ namespace FanCoilUnits {
 					FanCoil( FanCoilNum ).DesZoneCoolingLoad = -1.0 * FanCoil( FanCoilNum ).DesCoolingLoad;
 					FanCoil( FanCoilNum ).DesZoneHeatingLoad = FanCoil( FanCoilNum ).DesHeatingLoad;
 
-				}
+		}
 			}
 
 		} // if ( CurZoneEqNum > 0 )
@@ -1846,13 +1846,12 @@ namespace FanCoilUnits {
 		using PlantUtilities::SetComponentFlowRate;
 		using General::SolveRegulaFalsi;
 		using DataZoneEquipment::CalcDesignSpecificationOutdoorAir;
-
+		using namespace DataPlant;
+		using namespace DataLoopNode;
 		// Locals
 		// SUBROUTINE ARGUMENT DEFINITIONS:
 
 		// SUBROUTINE PARAMETER DEFINITIONS:
-		int const iReverseAction( 1 );
-		int const iNormalAction( 2 );
 		int const MaxIterCycl( 100 );
 
 		// INTERFACE BLOCK SPECIFICATIONS
@@ -1875,7 +1874,8 @@ namespace FanCoilUnits {
 		Real64 QTotUnitOut; // total unit output [watts]
 		Real64 AirMassFlow; // air mass flow rate [kg/sec]
 		Real64 QUnitOutNoHC; // unit output with no active heating or cooling [W]
-		Real64 QUnitOutMaxHC; // unit output with full active heating or cooling [W]
+		Real64 QUnitOutMaxC; // unit output with full active cooling [W]
+		Real64 QUnitOutMaxH; // unit output with full active heating [W]
 		Real64 QCoilHeatSP; // coil load to the heating setpoint [W]
 		Real64 QCoilCoolSP; // coil load to the cooling setpoint [W]
 		Real64 LatentOutput; // Latent (moisture) add/removal rate, negative is dehumidification [kg/s]
@@ -1898,7 +1898,14 @@ namespace FanCoilUnits {
 		Real64 MinSAMassFlowRate; // minimum supply air mass flow rate [kg/s]
 		Real64 MaxSAMassFlowRate; // maximum supply air mass flow rate [kg/s]
 		Real64 FCOutletTempOn; // ASHRAE outlet air temperature when coil is on [C]
-
+		Real64 HWFlow; // hot water mass flow rate solution [kg/s]		Real64 HWFlowBypass; // hot water bypassed mass flow rate [kg/s]
+		Real64 MdotLockH; // saved value of locked chilled water mass flow rate [kg/s]
+		Real64 MdotLockC; // saved value of locked hot water mass flow rate [kg/s]
+		Real64 CWFlow; // cold water mass flow rate solution [kg/s]
+		Real64 CWFlowBypass; // cold water bypassed mass flow rate [kg/s]
+		Real64 HWFlowBypass; // hot water bypassed mass flow rate [kg/s]
+		bool ColdFlowLocked; // if true cold water flow is locked
+		bool HotFlowLocked; // if true Hot water flow is locked
 		// FLOW
 		FanElecPower = 0.0;
 		// initialize local variables
@@ -1923,6 +1930,12 @@ namespace FanCoilUnits {
 		Iter = 0;
 		Relax = 1.0;
 		ElectricHeaterControl = 0.0;
+		HWFlow = 0.0;
+		HWFlowBypass = 0.0;
+		MdotLockH = 0.0;
+		MdotLockC = 0.0;
+		ColdFlowLocked = false;
+		HotFlowLocked = false;
 
 		// select capacity control method
 		{ auto const SELECT_CASE_var( FanCoil( FanCoilNum ).CapCtrlMeth_Num );
@@ -1936,61 +1949,174 @@ namespace FanCoilUnits {
 			//    Node(FanCoil(FanCoilNum)%HotControlNode)%MassFlowRate = 0.0
 			mdot = 0.0;
 			SetComponentFlowRate( mdot, FanCoil( FanCoilNum ).ColdControlNode, FanCoil( FanCoilNum ).ColdPlantOutletNode, FanCoil( FanCoilNum ).CWLoopNum, FanCoil( FanCoilNum ).CWLoopSide, FanCoil( FanCoilNum ).CWBranchNum, FanCoil( FanCoilNum ).CWCompNum );
-
+			if ( PlantLoop( FanCoil( FanCoilNum ).CWLoopNum ).LoopSide( FanCoil( FanCoilNum ).CWLoopSide ).FlowLock == FlowLocked ) {
+				ColdFlowLocked = true; // check for flow lock
+			}
 			if ( FanCoil( FanCoilNum ).HCoilType_Num == HCoil_Water ) {
 				mdot = 0.0;
 				SetComponentFlowRate( mdot, FanCoil( FanCoilNum ).HotControlNode, FanCoil( FanCoilNum ).HotPlantOutletNode, FanCoil( FanCoilNum ).HWLoopNum, FanCoil( FanCoilNum ).HWLoopSide, FanCoil( FanCoilNum ).HWBranchNum, FanCoil( FanCoilNum ).HWCompNum );
-				// obtain unit output with no active heating/cooling
+				if ( PlantLoop( FanCoil( FanCoilNum ).HWLoopNum ).LoopSide( FanCoil( FanCoilNum ).HWLoopSide ).FlowLock == FlowLocked ) {
+					HotFlowLocked = true; // save locked flow
+				}
 			}
+			// obtain unit output with no active heating/cooling
 			Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOutNoHC, 0.0 );
-
+			if ( FirstHVACIteration ) {
+				FanCoil( FanCoilNum ).QUnitOutNoHC = QUnitOutNoHC;
+			}
+			else {
+				QUnitOutNoHC = FanCoil( FanCoilNum ).QUnitOutNoHC;
+			}
 			// get the loads at the coils
 			QCoilHeatSP = ZoneSysEnergyDemand( ZoneNum ).RemainingOutputReqToHeatSP - QUnitOutNoHC;
 			QCoilCoolSP = ZoneSysEnergyDemand( ZoneNum ).RemainingOutputReqToCoolSP - QUnitOutNoHC;
+			// if cooling
 			if ( UnitOn && QCoilCoolSP < ( -1.0 * SmallLoad ) && TempControlType( ZoneNum ) != SingleHeatingSetPoint ) {
+				ControlNode = FanCoil( FanCoilNum ).ColdControlNode;
+				ControlOffset = FanCoil( FanCoilNum ).ColdControlOffset;
+				MaxWaterFlow = FanCoil( FanCoilNum ).MaxColdWaterFlow;
+				MinWaterFlow = FanCoil( FanCoilNum ).MinColdWaterFlow;
+				//On the first HVAC iteration the system values are given to the controller, but after that
+				// the demand limits are in place and there needs to be feedback to the Zone Equipment
+				if ( ! FirstHVACIteration ) {
+					MaxWaterFlow = Node( ControlNode ).MassFlowRateMaxAvail;
+					MinWaterFlow = Node( ControlNode ).MassFlowRateMinAvail;
+				}
 				// get full load result
-				mdot = FanCoil( FanCoilNum ).MaxColdWaterFlow;
+				mdot = MaxWaterFlow;
 				SetComponentFlowRate( mdot, FanCoil( FanCoilNum ).ColdControlNode, FanCoil( FanCoilNum ).ColdPlantOutletNode, FanCoil( FanCoilNum ).CWLoopNum, FanCoil( FanCoilNum ).CWLoopSide, FanCoil( FanCoilNum ).CWBranchNum, FanCoil( FanCoilNum ).CWCompNum );
-				Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOutMaxHC );
-				if ( QUnitOutMaxHC < QCoilCoolSP ) {
+				Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOutMaxC );
+				if ( ! ColdFlowLocked ) {
+					FanCoil( FanCoilNum ).QUnitOutMaxC = QUnitOutMaxC;
+				} else {
+					QUnitOutMaxC = FanCoil( FanCoilNum ).QUnitOutMaxC;
+					MdotLockC = mdot; // save locked flow
+				}
+				QZnReq = ZoneSysEnergyDemand( ZoneNum ).RemainingOutputReqToCoolSP;
+				if ( QUnitOutMaxC < QZnReq ) {
 					// more cooling than required, find reduced water flow rate to meet the load
-					ControlNode = FanCoil( FanCoilNum ).ColdControlNode;
-					ControlOffset = FanCoil( FanCoilNum ).ColdControlOffset;
-					MaxWaterFlow = FanCoil( FanCoilNum ).MaxColdWaterFlow;
-					MinWaterFlow = FanCoil( FanCoilNum ).MinColdWaterFlow;
-					//On the first HVAC iteration the system values are given to the controller, but after that
-					// the demand limits are in place and there needs to be feedback to the Zone Equipment
-					if ( ! FirstHVACIteration ) {
-						MaxWaterFlow = Node( ControlNode ).MassFlowRateMaxAvail;
-						MinWaterFlow = Node( ControlNode ).MassFlowRateMinAvail;
+					//solve for the cold water flow rate with no limit set by flow rate lockdown
+					Par( 1 ) = double( FanCoilNum );
+					Par( 2 ) = 0.0; // FLAG, IF 1.0 then FirstHVACIteration equals TRUE, if 0.0 then FirstHVACIteration equals false
+					if ( FirstHVACIteration ) Par( 2 ) = 1.0;
+					Par( 3 ) = ControlledZoneNum;
+					Par( 4 ) = QZnReq;
+					SolveRegulaFalsi( 0.001, MaxIterCycl, SolFlag, CWFlow, CalcFanCoilCWLoadResidual, 0.0, MaxWaterFlow, Par );
+					if ( SolFlag == -1 ) {
+						++FanCoil( FanCoilNum ).ConvgErrCountC;
+						if ( FanCoil( FanCoilNum ).ConvgErrCountC < 2 ) {
+							ShowWarningError( "Cold Water control failed in fan coil unit " + FanCoil( FanCoilNum ).Name );
+							ShowContinueError( "  Iteration limit exceeded in calculating water flow rate " );
+							ShowContinueErrorTimeStamp( "..Water flow rate set to last iteration value " );
+						} else {
+							ShowRecurringWarningErrorAtEnd( "Cold water flow Iteration limit exceeded in fan coil unit " + FanCoil( FanCoilNum ).Name,
+								FanCoil( FanCoilNum ).MaxIterIndexC );
+						}
+					} else if ( SolFlag == -2 ) {
+						++FanCoil( FanCoilNum ).LimitErrCountC;
+						if ( FanCoil( FanCoilNum ).LimitErrCountC < 2 ) {
+							ShowWarningError( "Cold Water control failed in fan coil unit " + FanCoil( FanCoilNum ).Name );
+							ShowContinueError( "  Bad cold water mass flow limits" );
+							ShowContinueErrorTimeStamp( "..Water flow rate set to lower limit " );
+						} else{
+							ShowRecurringWarningErrorAtEnd( "Cold Water control failed in fan coil unit " + FanCoil( FanCoilNum ).Name,
+								FanCoil( FanCoilNum ).BadMassFlowLimIndexC );
+						}
+					}
+				} else {
+					// demand greater than capacity
+					CWFlow = MaxWaterFlow;
+				}
+				if ( ! ColdFlowLocked ) {
+					mdot = CWFlow; // not flowlocked - set flow to CWFlow
+					SetComponentFlowRate( mdot, FanCoil( FanCoilNum ).ColdControlNode, FanCoil( FanCoilNum ).ColdPlantOutletNode, FanCoil( FanCoilNum ).CWLoopNum,
+						FanCoil( FanCoilNum ).CWLoopSide, FanCoil( FanCoilNum ).CWBranchNum, FanCoil( FanCoilNum ).CWCompNum );
+					Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOut ); // get QUnitOut
+				}
+				else {
+					// flow lock on 
+					if ( MdotLockC > CWFlow ) { // if mdot > CWFlow, bypass extra flow
+						Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOut ); // get QUnitOut with CWFlow; rest will be bypassed 
+						Node( FanCoil( FanCoilNum ).ColdControlNode ).MassFlowRate = MdotLockC; // reset flow to locked value. Since lock is on, must do this by hand
+						Node( FanCoil( FanCoilNum ).ColdPlantOutletNode ).MassFlowRate = MdotLockC;
+						// Keep soln flow rate but reset outlet water temperature - i.e. bypass extra water
+						CWFlowBypass = MdotLockC - CWFlow;
+						// change water outlet temperature and enthalpy
+						Node( FanCoil( FanCoilNum ).ColdPlantOutletNode ).Temp = ( CWFlowBypass * Node( FanCoil( FanCoilNum ).ColdControlNode ).Temp +
+							CWFlow * Node( FanCoil( FanCoilNum ).ColdPlantOutletNode ).Temp ) / MdotLockC;
+						Node( FanCoil( FanCoilNum ).ColdPlantOutletNode ).Enthalpy = ( CWFlowBypass * Node( FanCoil( FanCoilNum ).ColdControlNode ).Enthalpy +
+							CWFlow * Node( FanCoil( FanCoilNum ).ColdPlantOutletNode ).Enthalpy ) / MdotLockC;
+					}
+					else {
+						// if MdotLockC <= HWFlow use MdotLockC as is
+						Node( FanCoil( FanCoilNum ).ColdControlNode ).MassFlowRate = MdotLockC; // reset flow to locked value. Since lock is on, must do this by hand
+						Node( FanCoil( FanCoilNum ).ColdPlantOutletNode ).MassFlowRate = MdotLockC;
+						Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOut );
 					}
-					QZnReq = ZoneSysEnergyDemand( ZoneNum ).RemainingOutputReqToCoolSP;
-					ControlCompOutput( FanCoil( FanCoilNum ).Name, cMO_FanCoil, FanCoilNum, FirstHVACIteration, QZnReq, ControlNode, MaxWaterFlow, MinWaterFlow, ControlOffset, FanCoil( FanCoilNum ).ControlCompTypeNum, FanCoil( FanCoilNum ).CompErrIndex, _, _, _, iReverseAction, _, FanCoil( FanCoilNum ).CWLoopNum, FanCoil( FanCoilNum ).CWLoopSide, FanCoil( FanCoilNum ).CWBranchNum, ControlledZoneNum );
 				}
 				QUnitOut = AirMassFlow * ( PsyHFnTdbW( Node( OutletNode ).Temp, Node( InletNode ).HumRat ) - PsyHFnTdbW( Node( InletNode ).Temp, Node( InletNode ).HumRat ) );
+			// if heating
 			} else if ( UnitOn && QCoilHeatSP > SmallLoad && TempControlType( ZoneNum ) != SingleCoolingSetPoint ) {
 				// get full load result
-				if ( FanCoil( FanCoilNum ).HCoilType_Num == HCoil_Water ) {
-					mdot = FanCoil( FanCoilNum ).MaxHotWaterFlow;
+				if ( FanCoil( FanCoilNum ).HCoilType_Num == HCoil_Water ) { // if HW Coil
+					ControlNode = FanCoil( FanCoilNum ).HotControlNode;
+					ControlOffset = FanCoil( FanCoilNum ).HotControlOffset;
+					MaxWaterFlow = FanCoil( FanCoilNum ).MaxHotWaterFlow;
+					MinWaterFlow = FanCoil( FanCoilNum ).MinHotWaterFlow;
+					//On the first HVAC iteration the system values are given to the controller, but after that
+					// the demand limits are in place and there needs to be feedback to the Zone Equipment
+					if ( !FirstHVACIteration ) {
+						MaxWaterFlow = Node( ControlNode ).MassFlowRateMaxAvail;
+						MinWaterFlow = Node( ControlNode ).MassFlowRateMinAvail;
+					}
+					mdot = MaxWaterFlow;
 					SetComponentFlowRate( mdot, FanCoil( FanCoilNum ).HotControlNode, FanCoil( FanCoilNum ).HotPlantOutletNode, FanCoil( FanCoilNum ).HWLoopNum, FanCoil( FanCoilNum ).HWLoopSide, FanCoil( FanCoilNum ).HWBranchNum, FanCoil( FanCoilNum ).HWCompNum );
+					Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOutMaxH );
+					if ( ! HotFlowLocked ) {
+						FanCoil( FanCoilNum ).QUnitOutMaxH = QUnitOutMaxH;
+					}
+					else {
+						QUnitOutMaxH = FanCoil( FanCoilNum ).QUnitOutMaxH;
+						MdotLockH = mdot; // save locked flow
+					}
+				} else {
+					// not HW coil
+					Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOutMaxH, 1.0 );
 				}
-				Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOutMaxHC );
-				if ( QUnitOutMaxHC > QCoilHeatSP ) {
+				QZnReq = ZoneSysEnergyDemand( ZoneNum ).RemainingOutputReqToHeatSP;
+				if ( QUnitOutMaxH > QZnReq ) {
 					// more heating than required, find reduced water flow rate to meet the load
-					QZnReq = ZoneSysEnergyDemand( ZoneNum ).RemainingOutputReqToHeatSP;
 					if ( FanCoil( FanCoilNum ).HCoilType_Num == HCoil_Water ) {
-						ControlNode = FanCoil( FanCoilNum ).HotControlNode;
-						ControlOffset = FanCoil( FanCoilNum ).HotControlOffset;
-						MaxWaterFlow = FanCoil( FanCoilNum ).MaxHotWaterFlow;
-						MinWaterFlow = FanCoil( FanCoilNum ).MinHotWaterFlow;
-						//On the first HVAC iteration the system values are given to the controller, but after that
-						// the demand limits are in place and there needs to be feedback to the Zone Equipment
-						if ( ! FirstHVACIteration ) {
-							MaxWaterFlow = Node( ControlNode ).MassFlowRateMaxAvail;
-							MinWaterFlow = Node( ControlNode ).MassFlowRateMinAvail;
+						//solve for the hot water flow rate with no limit set by flow rate lockdown
+						Par( 1 ) = double( FanCoilNum );
+						Par( 2 ) = 0.0; // FLAG, IF 1.0 then FirstHVACIteration equals TRUE, if 0.0 then FirstHVACIteration equals false
+						if ( FirstHVACIteration ) Par( 2 ) = 1.0;
+						Par( 3 ) = ControlledZoneNum;
+						Par( 4 ) = QZnReq;
+						SolveRegulaFalsi( 0.001, MaxIterCycl, SolFlag, HWFlow, CalcFanCoilHWLoadResidual, 0.0, MaxWaterFlow, Par );
+						if ( SolFlag == -1 ) {
+							++FanCoil( FanCoilNum ).ConvgErrCountH;
+							if ( FanCoil( FanCoilNum ).ConvgErrCountH < 2 ) {
+								ShowWarningError( "Hot Water control failed in fan coil unit " + FanCoil( FanCoilNum ).Name );
+								ShowContinueError( "  Iteration limit exceeded in calculating water flow rate " );
+								ShowContinueErrorTimeStamp( "..Water flow rate set to last iteration value " );
+							} else {
+								ShowRecurringWarningErrorAtEnd( "Hot water flow Iteration limit exceeded in fan coil unit " + FanCoil( FanCoilNum ).Name,
+									FanCoil( FanCoilNum ).MaxIterIndexH );
+							}
+						} else if ( SolFlag == -2 ) {
+							++FanCoil( FanCoilNum ).LimitErrCountH;
+							if ( FanCoil( FanCoilNum ).LimitErrCountH < 2 ) {
+								ShowWarningError( "Hot Water control failed in fan coil unit " + FanCoil( FanCoilNum ).Name );
+								ShowContinueError( "  Bad hot water mass flow limits" );
+								ShowContinueErrorTimeStamp( "..Water flow rate set to lower limit " );
+							} else {
+								ShowRecurringWarningErrorAtEnd( "Hot Water control failed in fan coil unit " + FanCoil( FanCoilNum ).Name,
+									FanCoil( FanCoilNum ).BadMassFlowLimIndexH );
+							}
 						}
-						ControlCompOutput( FanCoil( FanCoilNum ).Name, cMO_FanCoil, FanCoilNum, FirstHVACIteration, QZnReq, ControlNode, MaxWaterFlow, MinWaterFlow, ControlOffset, FanCoil( FanCoilNum ).ControlCompTypeNum, FanCoil( FanCoilNum ).CompErrIndex, _, _, _, iNormalAction, _, FanCoil( FanCoilNum ).HWLoopNum, FanCoil( FanCoilNum ).HWLoopSide, FanCoil( FanCoilNum ).HWBranchNum, ControlledZoneNum );
-					} else {
+					}
+					else {
 						Par( 1 ) = double( FanCoilNum );
 						Par( 2 ) = 0.0; // FLAG, IF 1.0 then FirstHVACIteration equals TRUE, if 0.0 then FirstHVACIteration equals false
 						if ( FirstHVACIteration ) Par( 2 ) = 1.0;
@@ -1998,6 +2124,42 @@ namespace FanCoilUnits {
 						Par( 4 ) = QZnReq;
 						SolveRegulaFalsi( 0.001, MaxIterCycl, SolFlag, PLR, CalcFanCoilLoadResidual, 0.0, 1.0, Par );
 					}
+				} else {
+					// demand greater than capacity
+					if ( FanCoil( FanCoilNum ).HCoilType_Num == HCoil_Water ) {
+						HWFlow = MaxWaterFlow;
+					} else{
+						Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, 1.0 );
+					}
+				}
+				if ( FanCoil( FanCoilNum ).HCoilType_Num == HCoil_Water ) {
+					if ( !HotFlowLocked ) {
+						mdot = HWFlow; // not flowlocked - set flow to HWFlow
+						SetComponentFlowRate( mdot, FanCoil( FanCoilNum ).HotControlNode, FanCoil( FanCoilNum ).HotPlantOutletNode, FanCoil( FanCoilNum ).HWLoopNum,
+							FanCoil( FanCoilNum ).HWLoopSide, FanCoil( FanCoilNum ).HWBranchNum, FanCoil( FanCoilNum ).HWCompNum );
+						Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOut ); // get QUnitOut
+					}
+					else {
+						// flow lock on 
+						if ( MdotLockH > HWFlow ) { // if mdot > HWFlow, bypass extra flow
+							Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOut ); // get QUnitOut with HWFlow; rest will be bypassed 
+							Node( FanCoil( FanCoilNum ).HotControlNode ).MassFlowRate = MdotLockH; // reset flow to locked value. Since lock is on, must do this by hand
+							Node( FanCoil( FanCoilNum ).HotPlantOutletNode ).MassFlowRate = MdotLockH;
+							// Keep soln flow rate but reset outlet water temperature - i.e. bypass extra water
+							HWFlowBypass = MdotLockH - HWFlow;
+							// change outlet water temperature and enthalpy
+							Node( FanCoil( FanCoilNum ).HotPlantOutletNode ).Temp = ( HWFlowBypass * Node( FanCoil( FanCoilNum ).HotControlNode ).Temp +
+								HWFlow * Node( FanCoil( FanCoilNum ).HotPlantOutletNode ).Temp ) / MdotLockH;
+							Node( FanCoil( FanCoilNum ).HotPlantOutletNode ).Enthalpy = ( HWFlowBypass * Node( FanCoil( FanCoilNum ).HotControlNode ).Enthalpy +
+								HWFlow * Node( FanCoil( FanCoilNum ).HotPlantOutletNode ).Enthalpy ) / MdotLockH;
+						}
+						else {
+							// if MdotLockH <= HWFlow use MdotLockH as is
+							Node( FanCoil( FanCoilNum ).HotControlNode ).MassFlowRate = MdotLockH; // reset flow to locked value. Since lock is on, must do this by hand
+							Node( FanCoil( FanCoilNum ).HotPlantOutletNode ).MassFlowRate = MdotLockH;
+							Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOut );
+						}
+					}
 				}
 				QUnitOut = AirMassFlow * ( PsyHFnTdbW( Node( OutletNode ).Temp, Node( InletNode ).HumRat ) - PsyHFnTdbW( Node( InletNode ).Temp, Node( InletNode ).HumRat ) );
 			} else {
@@ -4143,6 +4305,165 @@ namespace FanCoilUnits {
 		return Residuum;
 	}
 
+	Real64
+		CalcFanCoilHWLoadResidual(
+		Real64 const HWFlow, // water mass flow rate [kg/s]
+		Array1< Real64 > const & Par // Function parameters
+		)
+	{
+
+		// FUNCTION INFORMATION:
+		//       AUTHOR         Fred Buhl, FSEC
+		//       DATE WRITTEN   Jan 2016
+		//       MODIFIED       na
+		//       RE-ENGINEERED  na
+
+		// PURPOSE OF THIS SUBROUTINE:
+		// To calculate the part-load ratio for the FCU with electric heating coil
+
+		// METHODOLOGY EMPLOYED:
+		// Use SolveRegulaFalsi to CALL this Function to converge on a solution
+
+		// REFERENCES:
+		// na
+		
+		// USE STATEMENTS:
+		// na
+
+		// Return value
+		Real64 Residuum; // Result (force to 0)
+
+		// Argument array dimensioning
+
+		// Locals
+		// SUBROUTINE ARGUMENT DEFINITIONS:
+
+		//   Parameter description example:
+		//       Par(1)  = REAL(FanCoilNum,r64) ! Index to fan coil unit
+		//       Par(2)  = 0.0                  ! FirstHVACIteration FLAG, IF 1.0 then TRUE, if 0.0 then FALSE
+		//       Par(3)  = REAL(ControlledZoneNum,r64)     ! zone index
+		//       Par(4)  = QZnReq               ! zone load [W]
+
+		// SUBROUTINE PARAMETER DEFINITIONS:
+		// na
+
+		// INTERFACE BLOCK SPECIFICATIONS
+		// na
+
+		// DERIVED TYPE DEFINITIONS
+		// na
+
+		// SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+		int FanCoilNum; // Index to this fan coil unit
+		bool FirstHVACIteration; // FirstHVACIteration flag
+		int ControlledZoneNum; // zone index
+		Real64 QZnReq; // Sensible load to be met [W]
+		Real64 QUnitOut; // delivered capacity [W]
+
+		// Convert parameters to usable variables
+		FanCoilNum = int( Par( 1 ) );
+		if ( Par( 2 ) == 1.0 ) {
+			FirstHVACIteration = true;
+		}
+		else {
+			FirstHVACIteration = false;
+		}
+		ControlledZoneNum = int( Par( 3 ) );
+		QZnReq = Par( 4 );
+
+		Node( FanCoil( FanCoilNum ).HotControlNode ).MassFlowRate = HWFlow;
+		Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, 1.0 ); 
+
+		// Calculate residual based on output magnitude
+		if ( std::abs( QZnReq ) <= 100.0 ) {
+			Residuum = ( QUnitOut - QZnReq ) / 100.0;
+		}
+		else {
+			Residuum = ( QUnitOut - QZnReq ) / QZnReq;
+		}
+
+		return Residuum;
+	}
+
+	Real64
+		CalcFanCoilCWLoadResidual(
+		Real64 const CWFlow, // water mass flow rate [kg/s]
+		Array1< Real64 > const & Par // Function parameters
+		)
+	{
+
+		// FUNCTION INFORMATION:
+		//       AUTHOR         Fred Buhl Jan 2016
+		//       DATE WRITTEN   July 2015
+		//       MODIFIED       na
+		//       RE-ENGINEERED  na
+
+		// PURPOSE OF THIS SUBROUTINE:
+		// To calculate the part-load ratio for the FCU with electric heating coil
+
+		// METHODOLOGY EMPLOYED:
+		// Use SolveRegulaFalsi to CALL this Function to converge on a solution
+
+		// REFERENCES:
+		// na
+
+		// USE STATEMENTS:
+		// na
+
+		// Return value
+		Real64 Residuum; // Result (force to 0)
+
+		// Argument array dimensioning
+
+		// Locals
+		// SUBROUTINE ARGUMENT DEFINITIONS:
+
+		//   Parameter description example:
+		//       Par(1)  = REAL(FanCoilNum,r64) ! Index to fan coil unit
+		//       Par(2)  = 0.0                  ! FirstHVACIteration FLAG, IF 1.0 then TRUE, if 0.0 then FALSE
+		//       Par(3)  = REAL(ControlledZoneNum,r64)     ! zone index
+		//       Par(4)  = QZnReq               ! zone load [W]
+
+		// SUBROUTINE PARAMETER DEFINITIONS:
+		// na
+
+		// INTERFACE BLOCK SPECIFICATIONS
+		// na
+
+		// DERIVED TYPE DEFINITIONS
+		// na
+
+		// SUBROUTINE LOCAL VARIABLE DECLARATIONS:
+		int FanCoilNum; // Index to this fan coil unit
+		bool FirstHVACIteration; // FirstHVACIteration flag
+		int ControlledZoneNum; // zone index
+		Real64 QZnReq; // Sensible load to be met [W]
+		Real64 QUnitOut; // delivered capacity [W]
+
+		// Convert parameters to usable variables
+		FanCoilNum = int( Par( 1 ) );
+		if ( Par( 2 ) == 1.0 ) {
+			FirstHVACIteration = true;
+		}
+		else {
+			FirstHVACIteration = false;
+		}
+		ControlledZoneNum = int( Par( 3 ) );
+		QZnReq = Par( 4 );
+
+		Node( FanCoil( FanCoilNum ).ColdControlNode ).MassFlowRate = CWFlow;
+		Calc4PipeFanCoil( FanCoilNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, 1.0 ); 
+
+		// Calculate residual based on output magnitude
+		if ( std::abs( QZnReq ) <= 100.0 ) {
+			Residuum = ( QUnitOut - QZnReq ) / 100.0;
+		}
+		else {
+			Residuum = ( QUnitOut - QZnReq ) / QZnReq;
+		}
+
+		return Residuum;
+	}
 	Real64
 	CalcFanCoilWaterFlowTempResidual(
 		Real64 const WaterFlow, // water mass flow rate [kg/s]
@@ -4843,29 +5164,6 @@ namespace FanCoilUnits {
 		return Residuum;
 	}
 
-	//     NOTICE
-
-	//     Copyright (c) 1996-2015 The Board of Trustees of the University of Illinois
-	//     and The Regents of the University of California through Ernest Orlando Lawrence
-	//     Berkeley National Laboratory.  All rights reserved.
-
-	//     Portions of the EnergyPlus software package have been developed and copyrighted
-	//     by other individuals, companies and institutions.  These portions have been
-	//     incorporated into the EnergyPlus software package under license.   For a complete
-	//     list of contributors, see "Notice" located in main.cc.
-
-	//     NOTICE: The U.S. Government is granted for itself and others acting on its
-	//     behalf a paid-up, nonexclusive, irrevocable, worldwide license in this data to
-	//     reproduce, prepare derivative works, and perform publicly and display publicly.
-	//     Beginning five (5) years after permission to assert copyright is granted,
-	//     subject to two possible five year renewals, the U.S. Government is granted for
-	//     itself and others acting on its behalf a paid-up, non-exclusive, irrevocable
-	//     worldwide license in this data to reproduce, prepare derivative works,
-	//     distribute copies to the public, perform publicly and display publicly, and to
-	//     permit others to do so.
-
-	//     TRADEMARKS: EnergyPlus is a trademark of the US Department of Energy.
-
 } // FanCoilUnits
 
 } // EnergyPlus
diff --git a/src/EnergyPlus/FanCoilUnits.hh b/src/EnergyPlus/FanCoilUnits.hh
index f5035859bf8..22e5d424b7a 100644
--- a/src/EnergyPlus/FanCoilUnits.hh
+++ b/src/EnergyPlus/FanCoilUnits.hh
@@ -140,7 +140,9 @@ namespace FanCoilUnits {
 		int CapCtrlMeth_Num;
 		Real64 PLR; // Part Load Ratio, fraction of time step fancoil is on
 		int MaxIterIndexH; // Maximum iterations exceeded for heating
+		int BadMassFlowLimIndexH; // Bad mass flow limit error index for heating
 		int MaxIterIndexC; // Maximum iterations exceeded for cooling
+		int BadMassFlowLimIndexC; // Bad mass flow limit error index for cooling
 		Real64 FanAirVolFlow; // m3/s
 		Real64 MaxAirVolFlow; // m3/s
 		Real64 MaxAirMassFlow; // kg/s
@@ -219,7 +221,13 @@ namespace FanCoilUnits {
 		Real64 MinSATempCooling; // ASHRAE90.1 maximum supply air temperature in Cooling mode
 		Real64 MaxSATempHeating; // ASHRAE90.1 maximum supply air temperature in Heating mode
 		bool ASHRAETempControl; // ASHRAE90.1 control to temperature set point when true
-
+		Real64 QUnitOutNoHC; // unit output when no active heating or cooling [W]
+		Real64 QUnitOutMaxH; // unit output at maximum heating [W]
+		Real64 QUnitOutMaxC; // unit output at maximum cooling [W]
+		int LimitErrCountH; // count of SolveRegulaFalsi limit errors
+		int LimitErrCountC; // count of SolveRegulaFalsi limit errors
+		int ConvgErrCountH; // count of SolveRegulaFalsi iteration limit errors
+		int ConvgErrCountC; // count of SolveRegulaFalsi iteration limit errors
 		// Report data
 		Real64 HeatPower; // unit heating output in watts
 		Real64 HeatEnergy; // unit heating output in J
@@ -245,7 +253,9 @@ namespace FanCoilUnits {
 			CapCtrlMeth_Num( 0 ),
 			PLR( 0.0 ),
 			MaxIterIndexH( 0 ),
+			BadMassFlowLimIndexH( 0 ),
 			MaxIterIndexC( 0 ),
+			BadMassFlowLimIndexC( 0 ),
 			FanAirVolFlow( 0.0 ),
 			MaxAirVolFlow( 0.0 ),
 			MaxAirMassFlow( 0.0 ),
@@ -307,6 +317,13 @@ namespace FanCoilUnits {
 			MinSATempCooling( 0.0 ),
 			MaxSATempHeating( 0.0 ),
 			ASHRAETempControl( false ),
+			QUnitOutNoHC( 0.0 ),
+			QUnitOutMaxH( 0.0 ),
+			QUnitOutMaxC( 0.0 ),
+			LimitErrCountH( 0 ),
+			LimitErrCountC( 0 ),
+			ConvgErrCountH( 0 ),
+			ConvgErrCountC( 0 ),
 			HeatPower( 0.0 ),
 			HeatEnergy( 0.0 ),
 			TotCoolPower( 0.0 ),
@@ -447,6 +464,16 @@ namespace FanCoilUnits {
 	);
 
 	Real64
+	CalcFanCoilHWLoadResidual(
+		Real64 const HWFlow, // water mass flow rate [kg/s]
+		Array1< Real64 > const & Par // Function parameters
+	);
+
+	Real64
+		CalcFanCoilCWLoadResidual(
+		Real64 const CWFlow, // water mass flow rate [kg/s]
+		Array1< Real64 > const & Par // Function parameters
+		);	Real64
 	CalcFanCoilWaterFlowTempResidual(
 		Real64 const WaterFlow, // water mass flow rate [kg/s]
 		Array1< Real64 > const & Par // Function parameters
@@ -492,32 +519,7 @@ namespace FanCoilUnits {
 	CalcFanCoilElecHeatTempResidual(
 		Real64 const PLR, // electric heating coil part load ratio
 		Array1< Real64 > const & Par // Function parameters
-	);
-
-	//     NOTICE
-
-	//     Copyright (c) 1996-2015 The Board of Trustees of the University of Illinois
-	//     and The Regents of the University of California through Ernest Orlando Lawrence
-	//     Berkeley National Laboratory.  All rights reserved.
-
-	//     Portions of the EnergyPlus software package have been developed and copyrighted
-	//     by other individuals, companies and institutions.  These portions have been
-	//     incorporated into the EnergyPlus software package under license.   For a complete
-	//     list of contributors, see "Notice" located in main.cc.
-
-	//     NOTICE: The U.S. Government is granted for itself and others acting on its
-	//     behalf a paid-up, nonexclusive, irrevocable, worldwide license in this data to
-	//     reproduce, prepare derivative works, and perform publicly and display publicly.
-	//     Beginning five (5) years after permission to assert copyright is granted,
-	//     subject to two possible five year renewals, the U.S. Government is granted for
-	//     itself and others acting on its behalf a paid-up, non-exclusive, irrevocable
-	//     worldwide license in this data to reproduce, prepare derivative works,
-	//     distribute copies to the public, perform publicly and display publicly, and to
-	//     permit others to do so.
-
-	//     TRADEMARKS: EnergyPlus is a trademark of the US Department of Energy.
-
-} // FanCoilUnits
+	);} // FanCoilUnits
 
 } // EnergyPlus
 
diff --git a/src/EnergyPlus/Fans.cc b/src/EnergyPlus/Fans.cc
index 1bf31570e28..f04364c8751 100644
--- a/src/EnergyPlus/Fans.cc
+++ b/src/EnergyPlus/Fans.cc
@@ -956,7 +956,8 @@ namespace Fans {
 			SetupOutputVariable( "Fan Runtime Fraction []", Fan( FanNum ).FanRuntimeFraction, "System", "Average", Fan( FanNum ).FanName );
 		}
 
-		ManageEMS( emsCallFromComponentGetInput );
+		bool anyRan;
+		ManageEMS( emsCallFromComponentGetInput, anyRan );
 		MySizeFlag.dimension( NumFans, true );
 
 	}
diff --git a/src/EnergyPlus/Furnaces.cc b/src/EnergyPlus/Furnaces.cc
index fc4bfabb9e4..50151c4cae4 100644
--- a/src/EnergyPlus/Furnaces.cc
+++ b/src/EnergyPlus/Furnaces.cc
@@ -4184,8 +4184,8 @@ namespace Furnaces {
 
 			}
 		}
-
-		ManageEMS( emsCallFromComponentGetInput );
+		bool anyRan;
+		ManageEMS( emsCallFromComponentGetInput, anyRan );
 
 	}
 
@@ -5273,7 +5273,8 @@ namespace Furnaces {
 		Real64 MulSpeedFlowScale; // variable speed air flow scaling factor
 		bool ErrFound; // flag returned from mining functions
 		Real64 BranchFlow; // branch volumetric flow rate [m3/s]
-		ManageEMS( emsCallFromUnitarySystemSizing ); // calling point
+		bool anyRan;
+		ManageEMS( emsCallFromUnitarySystemSizing, anyRan ); // calling point
 		ThisCtrlZoneNum = 0;
 		DXCoolCap = 0.0;
 		UnitaryHeatCap = 0.0;
diff --git a/src/EnergyPlus/GroundTemperatureModeling/KusudaAchenbachGroundTemperatureModel.cc b/src/EnergyPlus/GroundTemperatureModeling/KusudaAchenbachGroundTemperatureModel.cc
index 9d7918e113f..52c8a8620dd 100644
--- a/src/EnergyPlus/GroundTemperatureModeling/KusudaAchenbachGroundTemperatureModel.cc
+++ b/src/EnergyPlus/GroundTemperatureModeling/KusudaAchenbachGroundTemperatureModel.cc
@@ -73,9 +73,9 @@ namespace EnergyPlus {
 	//******************************************************************************
 
 	// Kusuda model factory
-	std::shared_ptr< KusudaGroundTempsModel > 
-	KusudaGroundTempsModel::KusudaGTMFactory( 
-		int objectType, 
+	std::shared_ptr< KusudaGroundTempsModel >
+	KusudaGroundTempsModel::KusudaGTMFactory(
+		int objectType,
 		std::string objectName
 	)
 	{
@@ -94,7 +94,7 @@ namespace EnergyPlus {
 		using namespace GroundTemperatureManager;
 
 		// Locals
-		// SUBROUTINE LOCAL VARIABLE DECLARATIONS:	
+		// SUBROUTINE LOCAL VARIABLE DECLARATIONS:
 		bool found = false;
 		int NumNums;
 		int NumAlphas;
@@ -141,10 +141,10 @@ namespace EnergyPlus {
 
 					for ( int monthIndex = 1; monthIndex <= 12; ++monthIndex ) {
 						Real64 currMonthTemp = shallowObj->getGroundTempAtTimeInMonths( 0.0, monthIndex );
-						
+
 						// Calculate Average Ground Temperature for all 12 months of the year:
 						averageGroundTemp += currMonthTemp;
-						
+
 						// Need max temp, min temp, and month of min surf temp to set amplitude and month of min surf temp
 						if ( currMonthTemp <= minSurfTemp ) {
 							monthOfMinSurfTemp = monthIndex;
@@ -226,7 +226,7 @@ namespace EnergyPlus {
 		Real64 const _depth,
 		Real64 const _seconds
 	)
-	{	
+	{
 		// SUBROUTINE INFORMATION:
 		//       AUTHOR         Matt Mitchell
 		//       DATE WRITTEN   Summer 2015
@@ -287,7 +287,7 @@ namespace EnergyPlus {
 		if ( simTimeInSeconds > secondsPerYear ) {
 			simTimeInSeconds = remainder( simTimeInSeconds, secondsPerYear );
 		}
-		
+
 		// Get and return ground temperature
 		return getGroundTemp();
 	}
diff --git a/src/EnergyPlus/HVACManager.cc b/src/EnergyPlus/HVACManager.cc
index 5452d5bc787..43cd55022d9 100644
--- a/src/EnergyPlus/HVACManager.cc
+++ b/src/EnergyPlus/HVACManager.cc
@@ -389,7 +389,8 @@ namespace HVACManager {
 		NumOfSysTimeSteps = 1;
 		FracTimeStepZone = TimeStepSys / TimeStepZone;
 
-		ManageEMS( emsCallFromBeginTimestepBeforePredictor ); //calling point
+		bool anyEMSRan;
+		ManageEMS( emsCallFromBeginTimestepBeforePredictor, anyEMSRan ); //calling point
 
 		SetOutAirNodes();
 
@@ -512,7 +513,7 @@ namespace HVACManager {
 			// Update the plant and condenser loop capacitance model temperature history.
 			UpdateNodeThermalHistory();
 
-			ManageEMS( emsCallFromEndSystemTimestepBeforeHVACReporting ); // EMS calling point
+			ManageEMS( emsCallFromEndSystemTimestepBeforeHVACReporting, anyEMSRan ); // EMS calling point
 
 			// This is where output processor data is updated for System Timestep reporting
 			if ( ! WarmupFlag ) {
@@ -582,7 +583,7 @@ namespace HVACManager {
 				}
 				UpdateDataandReport( HVACTSReporting );
 			}
-			ManageEMS( emsCallFromEndSystemTimestepAfterHVACReporting ); // EMS calling point
+			ManageEMS( emsCallFromEndSystemTimestepAfterHVACReporting, anyEMSRan ); // EMS calling point
 			//UPDATE SYSTEM CLOCKS
 			SysTimeElapsed += TimeStepSys;
 
@@ -807,8 +808,8 @@ namespace HVACManager {
 
 		// Before the HVAC simulation, call ManageSetPoints to set all the HVAC
 		// node setpoints
-
-		ManageEMS( emsCallFromBeforeHVACManagers ); // calling point
+		bool anyEMSRan = false;
+		ManageEMS( emsCallFromBeforeHVACManagers, anyEMSRan ); // calling point
 
 		ManageSetPoints();
 
@@ -819,7 +820,8 @@ namespace HVACManager {
 		// the system on/off flags
 		ManageSystemAvailability();
 
-		ManageEMS( emsCallFromAfterHVACManagers ); // calling point
+		ManageEMS( emsCallFromAfterHVACManagers, anyEMSRan ); // calling point
+		ManageEMS( emsCallFromHVACIterationLoop, anyEMSRan ); // calling point id
 
 		// first explicitly call each system type with FirstHVACIteration,
 
@@ -840,7 +842,7 @@ namespace HVACManager {
 		// true, then specific components must be resimulated.
 		while ( ( SimAirLoopsFlag || SimZoneEquipmentFlag || SimNonZoneEquipmentFlag || SimPlantLoopsFlag || SimElecCircuitsFlag ) && ( HVACManageIteration <= MaxIter ) ) {
 
-			ManageEMS( emsCallFromHVACIterationLoop ); // calling point id
+			ManageEMS( emsCallFromHVACIterationLoop, anyEMSRan ); // calling point id
 
 			// Manages the various component simulations
 			SimSelectedEquipment( SimAirLoopsFlag, SimZoneEquipmentFlag, SimNonZoneEquipmentFlag, SimPlantLoopsFlag, SimElecCircuitsFlag, FirstHVACIteration, SimWithPlantFlowUnlocked );
@@ -852,6 +854,11 @@ namespace HVACManager {
 
 			++HVACManageIteration; // Increment the iteration counter
 
+			if ( anyEMSRan && HVACManageIteration <= 2 ) {
+				// the calling point emsCallFromHVACIterationLoop is only effective for air loops if this while loop runs at least twice 
+				SimAirLoopsFlag = true;
+			}
+
 		}
 		if ( AnyPlantInModel ) {
 			if ( AnyPlantSplitterMixerLacksContinuity() ) {
@@ -1619,7 +1626,7 @@ namespace HVACManager {
 				}
 				if ( SimZoneEquipment ) {
 					if ( ( IterAir == 1 ) && ( ! FlowMaxAvailAlreadyReset ) ) { // don't do reset if already done in FirstHVACIteration
-						ResetTerminalUnitFlowLimits();
+						// ResetTerminalUnitFlowLimits(); // don't do reset at all - interferes with convergence and terminal unit flow controls
 						FlowResolutionNeeded = true;
 					} else {
 						ResolveAirLoopFlowLimits();
@@ -1812,6 +1819,7 @@ namespace HVACManager {
 								for ( ZonesCooledIndex = 1; ZonesCooledIndex <= AirToZoneNodeInfo( AirLoopIndex ).NumZonesCooled; ++ZonesCooledIndex ) {
 									TermInletNode = AirToZoneNodeInfo( AirLoopIndex ).TermUnitCoolInletNodes( ZonesCooledIndex );
 									Node( TermInletNode ).MassFlowRateMinAvail = Node( TermInletNode ).MassFlowRate * FlowRatio;
+									Node( TermInletNode ).MassFlowRateMaxAvail = max(Node(TermInletNode).MassFlowRateMaxAvail, Node(TermInletNode).MassFlowRateMinAvail);
 								}
 							}
 						}
diff --git a/src/EnergyPlus/HVACSizingSimulationManager.cc b/src/EnergyPlus/HVACSizingSimulationManager.cc
index 6a3660a9f5f..742fdd4b6b6 100644
--- a/src/EnergyPlus/HVACSizingSimulationManager.cc
+++ b/src/EnergyPlus/HVACSizingSimulationManager.cc
@@ -320,7 +320,8 @@ namespace EnergyPlus {
 				DayOfSimChr = "0";
 				NumOfWarmupDays = 0;
 
-				ManageEMS(emsCallFromBeginNewEvironment); // calling point
+				bool anyEMSRan;
+				ManageEMS( emsCallFromBeginNewEvironment, anyEMSRan ); // calling point
 
 				while ( (DayOfSim < NumOfDayInEnvrn) || (WarmupFlag) ) { // Begin day loop ...
 
diff --git a/src/EnergyPlus/HVACStandAloneERV.cc b/src/EnergyPlus/HVACStandAloneERV.cc
index 36e04f7f58b..b71e590a5d0 100644
--- a/src/EnergyPlus/HVACStandAloneERV.cc
+++ b/src/EnergyPlus/HVACStandAloneERV.cc
@@ -355,7 +355,6 @@ namespace HVACStandAloneERV {
 		static bool ErrorsFound( false ); // Set to true if errors in input, fatal at end of routine
 		bool IsNotOK; // Flag to verify name
 		bool IsBlank; // Flag for blank name
-		int OutAirNum; // total number of CONTROLLER:OUTSIDE AIR objects
 		int NumERVCtrlrs; // total number of CONTROLLER:STAND ALONE ERV objects
 		int ERVControllerNum; // index to ERV controller
 		int WhichERV; // used in controller GetInput
@@ -728,7 +727,7 @@ namespace HVACStandAloneERV {
 
 		}
 
-		OutAirNum = GetNumObjectsFound( "Controller:OutdoorAir" );
+		int OutAirNum = 0;
 		CurrentModuleObject = "ZoneHVAC:EnergyRecoveryVentilator:Controller";
 		NumERVCtrlrs = GetNumObjectsFound( CurrentModuleObject );
 
@@ -737,7 +736,7 @@ namespace HVACStandAloneERV {
 
 			IsNotOK = false;
 			IsBlank = false;
-			CheckOAControllerName( Alphas( 1 ), OutAirNum, IsNotOK, IsBlank, CurrentModuleObject + " Name" );
+			CheckOAControllerName( Alphas( 1 ), ERVControllerNum, IsNotOK, IsBlank, CurrentModuleObject + " Name" );
 			if ( IsNotOK ) {
 				ErrorsFound = true;
 				if ( IsBlank ) Alphas( 1 ) = "xxxxx";
diff --git a/src/EnergyPlus/HVACUnitarySystem.cc b/src/EnergyPlus/HVACUnitarySystem.cc
index 2606acaa2fd..cc248f8c410 100644
--- a/src/EnergyPlus/HVACUnitarySystem.cc
+++ b/src/EnergyPlus/HVACUnitarySystem.cc
@@ -1911,8 +1911,8 @@ namespace HVACUnitarySystem {
 		EqSizing.DesCoolingLoad = 0.0;
 		EqSizing.DesHeatingLoad = 0.0;
 
-
-		ManageEMS( emsCallFromUnitarySystemSizing ); // calling point
+		bool anyEMSRan;
+		ManageEMS( emsCallFromUnitarySystemSizing, anyEMSRan ); // calling point
 
 		CompName = UnitarySystem( UnitarySysNum ).Name;
 		CompType = UnitarySystem( UnitarySysNum ).UnitarySystemType;
@@ -5923,20 +5923,23 @@ namespace HVACUnitarySystem {
 				}
 			}
 
-			if ( UnitarySystem( UnitarySysNum ).HeatingCoilType_Num == CoilDX_MultiSpeedHeating && UnitarySystem( UnitarySysNum ).CoolingCoilType_Num == CoilDX_MultiSpeedCooling ) {
+			if ( ( UnitarySystem( UnitarySysNum ).HeatingCoilType_Num == CoilDX_MultiSpeedHeating && UnitarySystem( UnitarySysNum ).CoolingCoilType_Num == CoilDX_MultiSpeedCooling ) ||
+				( UnitarySystem( UnitarySysNum ).HeatingCoilType_Num == Coil_HeatingGas && UnitarySystem( UnitarySysNum ).CoolingCoilType_Num == CoilDX_MultiSpeedCooling ) ) {
 				Index = UnitarySystem( UnitarySysNum ).DesignSpecMSHPIndex;
-				if ( DesignSpecMSHP( Index ).SingleModeFlag ) {
-					UnitarySystem( UnitarySysNum ).SingleMode = 1;
+				if ( Index > 0 ) {
+					if ( DesignSpecMSHP( Index ).SingleModeFlag ) {
+						UnitarySystem( UnitarySysNum ).SingleMode = 1;
+					}
 				}
-			}
-			// Check fan operation mode to ensure cycling fan mode
-			if ( UnitarySystem( UnitarySysNum ).SingleMode == 1 ) {
-				if ( !CheckScheduleValueMinMax( UnitarySystem( UnitarySysNum ).FanOpModeSchedPtr, ">=", 0.0, "<=", 0.0 ) ) {
-					ShowSevereError( CurrentModuleObject + ": " + UnitarySystem( UnitarySysNum ).Name );
-					ShowContinueError( "The schedule values in " + cAlphaFields( iFanSchedAlphaNum ) + " must be 0 when Single Mode Operation is applied." );
-					ShowContinueError( "A value of 0 represents cycling fan mode, any other value up to 1 represents constant fan mode." );
-					ErrorsFound = true;
+			} else {
+				if ( UnitarySystem( UnitarySysNum ).DesignSpecMSHPIndex > 0 ) {
+					if ( DesignSpecMSHP( UnitarySystem( UnitarySysNum ).DesignSpecMSHPIndex ).SingleModeFlag ) {
+						ShowSevereError( CurrentModuleObject + ": " + UnitarySystem( UnitarySysNum ).Name );
+						ShowContinueError( "In order to perform Single Mode Operation, the valid cooling coil type is Coil:Cooling:DX:MultiSpeed and the valid heating is Coil:Heating:DX:MultiSpeed or Coil:Heating:Gas." );
+						ShowContinueError( "The input cooliing coil type = " + Alphas( iCoolingCoilTypeAlphaNum ) + " and the input heating coil type = " + Alphas( iHeatingCoilTypeAlphaNum ) );
+					}
 				}
+
 			}
 
 			// set global logicals that denote coil type
@@ -6065,8 +6068,8 @@ namespace HVACUnitarySystem {
 
 			}
 		}
-
-		ManageEMS( emsCallFromComponentGetInput );
+		bool anyEMSRan;
+		ManageEMS( emsCallFromComponentGetInput,anyEMSRan );
 
 	}
 
@@ -6830,20 +6833,23 @@ namespace HVACUnitarySystem {
 						CalcUnitarySystemToLoad( UnitarySysNum, AirLoopNum, FirstHVACIteration, CoolPLR, HeatPLR, OnOffAirFlowRatio, TempSensOutput, TempLatOutput, HXUnitOn, _, _, CompressorONFlag );
 					} else if ( CoolingLoad ) {
 						// RegulaFalsi may not find cooling PLR when the latent degradation model is used.
-						// IF iteration limit is exceeded, find tighter boundary of solution and repeat RegulaFalsi
+						// IF iteration limit is exceeded (SolFlag = -1), find tighter boundary of solution and repeat RegulaFalsi
 						TempMaxPLR = -0.1;
 						TempSysOutput = SensOutputOff;
 						TempLoad = ZoneLoad;
-						while ( ( TempSysOutput - TempLoad ) > 0.0 && TempMaxPLR < 1.0 ) {
+						while ( ( TempSysOutput - TempLoad ) > 0.0 && TempMaxPLR < 0.95 ) { // avoid PLR > 1 by limiting TempMaxPLR to 1 (i.e., TempMaxPLR += 0.1)
 							// find upper limit of HeatingPLR
 							TempMaxPLR += 0.1;
+							if ( TempMaxPLR > 0.95 && TempMaxPLR < 1.05 ) {
+								TempMaxPLR = 1.0; // enforce a perfect 1.0 at the top end
+							}
 							SetSpeedVariables( UnitarySysNum, true, TempMaxPLR );
 							CalcUnitarySystemToLoad( UnitarySysNum, AirLoopNum, FirstHVACIteration, TempMaxPLR, HeatPLR, OnOffAirFlowRatio, TempSensOutput, TempLatOutput, HXUnitOn, _, _, CompressorONFlag );
 							TempSysOutput = TempSensOutput;
 						}
 						TempMinPLR = TempMaxPLR;
-						while ( ( TempSysOutput - TempLoad ) < 0.0 && TempMinPLR > 0.0 ) {
-							// pull upper limit of HeatingPLR DOwn to last valid limit (i.e. heat output still exceeds SystemSensibleLoad)
+						while ( ( TempSysOutput - TempLoad ) < 0.0 && TempMinPLR > 0.05 ) {
+							// pull upper limit of HeatingPLR down to last valid limit (i.e. heat output still exceeds SystemSensibleLoad)
 							TempMaxPLR = TempMinPLR;
 							// find minimum limit of HeatingPLR
 							TempMinPLR -= 0.01;
@@ -7142,9 +7148,10 @@ namespace HVACUnitarySystem {
 			UnitarySystem( UnitarySysNum ).CoolingSpeedRatio = 0.0;
 			UnitarySystem( UnitarySysNum ).CoolingCycRatio = 0.0;
 			if ( UnitarySystem( UnitarySysNum ).MultiSpeedHeatingCoil || UnitarySystem( UnitarySysNum ).VarSpeedHeatingCoil ) {
-				if ( UnitarySystem( UnitarySysNum ).HeatingSpeedNum == 1 ) {
+				if ( UnitarySystem( UnitarySysNum ).HeatingSpeedNum <= 1 ) {
 					UnitarySystem( UnitarySysNum ).HeatingSpeedRatio = 0.0;
 					UnitarySystem( UnitarySysNum ).HeatingCycRatio = PartLoadRatio;
+					MSHPMassFlowRateLow = CompOnMassFlow * PartLoadRatio; // #5518
 				} else {
 					if ( UnitarySystem( UnitarySysNum ).SingleMode == 0 ) {
 						UnitarySystem( UnitarySysNum ).HeatingSpeedRatio = PartLoadRatio;
@@ -7169,9 +7176,10 @@ namespace HVACUnitarySystem {
 			UnitarySystem( UnitarySysNum ).HeatingSpeedRatio = 0.0;
 			UnitarySystem( UnitarySysNum ).HeatingCycRatio = 0.0;
 			if ( UnitarySystem( UnitarySysNum ).MultiSpeedCoolingCoil || UnitarySystem( UnitarySysNum ).VarSpeedCoolingCoil ) {
-				if ( UnitarySystem( UnitarySysNum ).CoolingSpeedNum == 1 ) {
+				if ( UnitarySystem( UnitarySysNum ).CoolingSpeedNum <= 1 ) {
 					UnitarySystem( UnitarySysNum ).CoolingSpeedRatio = 0.0;
 					UnitarySystem( UnitarySysNum ).CoolingCycRatio = PartLoadRatio;
+					MSHPMassFlowRateLow = CompOnMassFlow * PartLoadRatio; // #5518
 				} else {
 					if ( UnitarySystem( UnitarySysNum ).SingleMode == 0 ) {
 						UnitarySystem( UnitarySysNum ).CoolingSpeedRatio = PartLoadRatio;
@@ -7204,10 +7212,8 @@ namespace HVACUnitarySystem {
 				UnitarySystem( UnitarySysNum ).CoolingSpeedNum = 0;
 			}
 		}
-		if ( UnitarySystem( UnitarySysNum ).CoolingSpeedNum > 1 || UnitarySystem( UnitarySysNum ).HeatingSpeedNum > 1 ) {
-			OnOffAirFlowRatio = 1.0;
-			SetAverageAirFlow( UnitarySysNum, PartLoadRatio, OnOffAirFlowRatio );
-		}
+		OnOffAirFlowRatio = 1.0;
+		SetAverageAirFlow( UnitarySysNum, PartLoadRatio, OnOffAirFlowRatio );
 	}
 
 	Real64
@@ -10382,9 +10388,17 @@ namespace HVACUnitarySystem {
 						}
 					}
 				} else {
-					if ( HeatSpeedNum <= 1 ) {
+					if ( HeatSpeedNum < 1 ) {
 						CompOffMassFlow = UnitarySystem( UnitarySysNum ).IdleMassFlowRate;
 						CompOffFlowRatio = UnitarySystem( UnitarySysNum ).IdleSpeedRatio;
+					} else if ( HeatSpeedNum == 1 ) {
+						if ( UnitarySystem( UnitarySysNum ).MultiSpeedHeatingCoil ) {
+							CompOffMassFlow = 0.0; // #5518
+							CompOffFlowRatio = 0.0;
+						} else {
+							CompOffMassFlow = UnitarySystem( UnitarySysNum ).HeatMassFlowRate( HeatSpeedNum );
+							CompOffFlowRatio = UnitarySystem( UnitarySysNum ).HeatMassFlowRate( HeatSpeedNum );
+						}
 					} else {
 						CompOffMassFlow = UnitarySystem( UnitarySysNum ).HeatMassFlowRate( HeatSpeedNum - 1 );
 						CompOffFlowRatio = UnitarySystem( UnitarySysNum ).MSHeatingSpeedRatio( HeatSpeedNum - 1 );
@@ -10463,9 +10477,17 @@ namespace HVACUnitarySystem {
 						CompOffFlowRatio = UnitarySystem( UnitarySysNum ).MSCoolingSpeedRatio( CoolSpeedNum - 1 );
 					}
 				} else {
-					if ( CoolSpeedNum <= 1 ) {
+					if ( CoolSpeedNum < 1 ) {
 						CompOffMassFlow = UnitarySystem( UnitarySysNum ).IdleMassFlowRate;
 						CompOffFlowRatio = UnitarySystem( UnitarySysNum ).IdleSpeedRatio;
+					} else if ( CoolSpeedNum == 1 ) {
+						if ( UnitarySystem( UnitarySysNum ).MultiSpeedCoolingCoil ) {
+							CompOffMassFlow = 0.0; // #5518
+							CompOffFlowRatio = 0.0;
+						} else {
+							CompOffMassFlow = UnitarySystem( UnitarySysNum ).IdleMassFlowRate;
+							CompOffFlowRatio = UnitarySystem( UnitarySysNum ).IdleSpeedRatio;
+						}
 					} else {
 						CompOffMassFlow = UnitarySystem( UnitarySysNum ).CoolMassFlowRate( CoolSpeedNum - 1 );
 						CompOffFlowRatio = UnitarySystem( UnitarySysNum ).MSCoolingSpeedRatio( CoolSpeedNum - 1 );
@@ -10650,7 +10672,13 @@ namespace HVACUnitarySystem {
 			} // ELSE ! No Moisture Load
 		} // No Heating/Cooling Load
 
-		MSHPMassFlowRateLow = CompOffMassFlow; // these need to be set for multi-speed coils
+		if ( UnitarySystem( UnitarySysNum ).MultiSpeedHeatingCoil && ( HeatingLoad && HeatSpeedNum == 1 ) ) {
+			MSHPMassFlowRateLow = CompOnMassFlow * PartLoadRatio; // proportional to PLR when speed = 1,  #5518
+		} else if ( UnitarySystem( UnitarySysNum ).MultiSpeedCoolingCoil && ( CoolingLoad && CoolSpeedNum == 1 ) ) {
+			MSHPMassFlowRateLow = CompOnMassFlow * PartLoadRatio; // proportional to PLR when speed = 1,  #5518
+		} else {
+			MSHPMassFlowRateLow = CompOffMassFlow; // these need to be set for multi-speed coils
+		}
 		MSHPMassFlowRateHigh = CompOnMassFlow; // doesn't hurt to set these if multi-speed coils are not used
 
 		// Set the system mass flow rates
@@ -10731,11 +10759,15 @@ namespace HVACUnitarySystem {
 			FanSpeedRatio = CompOnFlowRatio;
 		}
 
-		if ( UnitarySystem( UnitarySysNum ).SingleMode == 1 ) {
-			AverageUnitMassFlow = PartLoadRatio * CompOnMassFlow;
-			FanSpeedRatio = PartLoadRatio * CompOnFlowRatio;
-			if ( !HeatingLoad && !CoolingLoad ) {
-				AverageUnitMassFlow = UnitarySystem( UnitarySysNum ).MaxNoCoolHeatAirMassFlow;
+		if ( !( HeatingLoad && UnitarySystem( UnitarySysNum ).NumOfSpeedHeating == 0 ) ) {
+			if ( UnitarySystem( UnitarySysNum ).SingleMode == 1 ) {
+				if ( UnitarySystem( UnitarySysNum ).FanOpMode == ContFanCycCoil ) {
+					AverageUnitMassFlow = CompOnMassFlow;
+					FanSpeedRatio = CompOnFlowRatio;
+				} else {
+					AverageUnitMassFlow = PartLoadRatio * CompOnMassFlow;
+					FanSpeedRatio = PartLoadRatio * CompOnFlowRatio;
+				}
 			}
 		}
 
diff --git a/src/EnergyPlus/HVACVariableRefrigerantFlow.cc b/src/EnergyPlus/HVACVariableRefrigerantFlow.cc
index c038df00c02..7a5c132b117 100644
--- a/src/EnergyPlus/HVACVariableRefrigerantFlow.cc
+++ b/src/EnergyPlus/HVACVariableRefrigerantFlow.cc
@@ -6271,7 +6271,6 @@ namespace HVACVariableRefrigerantFlow {
 		Real64 LoadToCoolingSP; // thermostat load to cooling setpoint (W)
 		Real64 LoadToHeatingSP; // thermostat load to heating setpoint (W)
 		Real64 TempOutput; // terminal unit output [W]
-		int FanOpMode; // TU fan operating mode
 
 		MaxDeltaT = 0.0;
 		MinDeltaT = 0.0;
@@ -6325,12 +6324,15 @@ namespace HVACVariableRefrigerantFlow {
 					SPTempLo = ZoneThermostatSetPointLo( ThisZoneNum );
 					{ auto const SELECT_CASE_var( TempControlType( ThisZoneNum ) );
 					if ( SELECT_CASE_var == 0 ) { // Uncontrolled
+					// MaxDeltaT denotes cooling, MinDeltaT denotes heating
 					} else if ( SELECT_CASE_var == SingleHeatingSetPoint ) {
-						ZoneDeltaT = max( 0.0, SPTempLo - ZT( ThisZoneNum ) );
-						MaxDeltaT( VRFCond ) = max( MaxDeltaT( VRFCond ), ZoneDeltaT );
-					} else if ( SELECT_CASE_var == SingleCoolingSetPoint ) {
-						ZoneDeltaT = min( 0.0, SPTempHi - ZT( ThisZoneNum ) );
+						// if heating load, ZoneDeltaT will be negative
+						ZoneDeltaT = min( 0.0, ZT( ThisZoneNum ) - SPTempLo );
 						MinDeltaT( VRFCond ) = min( MinDeltaT( VRFCond ), ZoneDeltaT );
+					} else if ( SELECT_CASE_var == SingleCoolingSetPoint ) {
+						// if cooling load, ZoneDeltaT will be positive
+						ZoneDeltaT = max( 0.0, ZT( ThisZoneNum ) - SPTempHi );
+						MaxDeltaT( VRFCond ) = max( MaxDeltaT( VRFCond ), ZoneDeltaT );
 					} else if ( SELECT_CASE_var == SingleHeatCoolSetPoint ) {
 						ZoneDeltaT = ZT( ThisZoneNum ) - SPTempHi; //- SPTempHi and SPTempLo are same value
 						if ( ZoneDeltaT > 0.0 ) {
@@ -6472,28 +6474,12 @@ namespace HVACVariableRefrigerantFlow {
 		// Determine operating mode based on VRF type and thermostat control selection
 		{ auto const SELECT_CASE_var( VRF( VRFCond ).ThermostatPriority );
 		if ( SELECT_CASE_var == ThermostatOffsetPriority ) {
-			TUIndex = VRF( VRFCond ).MasterZoneTUIndex;
-			if ( VRFTU( TUIndex ).FanOpModeSchedPtr > 0 ) {
-				if ( GetCurrentScheduleValue( VRFTU( TUIndex ).FanOpModeSchedPtr ) == 0.0 ) {
-					FanOpMode = CycFanCycCoil;
-				} else {
-					FanOpMode = ContFanCycCoil;
-				}
-			}
 			if ( MaxDeltaT( VRFCond ) > std::abs( MinDeltaT( VRFCond ) ) && MaxDeltaT( VRFCond ) > 0.0 ) {
 				HeatingLoad( VRFCond ) = false;
 				CoolingLoad( VRFCond ) = true;
 			} else if ( MaxDeltaT( VRFCond ) < std::abs( MinDeltaT( VRFCond ) ) && MinDeltaT( VRFCond ) < 0.0 ) {
 				HeatingLoad( VRFCond ) = true;
 				CoolingLoad( VRFCond ) = false;
-				// assuming if constant fan mode then previous operating mode will be needed
-				// could actually run the master zone TU to see if overshoot occurs, but seems overkill
-			} else if ( FanOpMode == ContFanCycCoil && LastModeCooling( VRFCond ) ) {
-				HeatingLoad( VRFCond ) = false;
-				CoolingLoad( VRFCond ) = true;
-			} else if ( FanOpMode == ContFanCycCoil && LastModeHeating( VRFCond ) ) {
-				HeatingLoad( VRFCond ) = true;
-				CoolingLoad( VRFCond ) = false;
 			} else {
 				HeatingLoad( VRFCond ) = false;
 				CoolingLoad( VRFCond ) = false;
diff --git a/src/EnergyPlus/HeatBalanceManager.cc b/src/EnergyPlus/HeatBalanceManager.cc
index 2a531540a4a..4ef76a47d71 100644
--- a/src/EnergyPlus/HeatBalanceManager.cc
+++ b/src/EnergyPlus/HeatBalanceManager.cc
@@ -367,7 +367,8 @@ namespace HeatBalanceManager {
 		// the HVAC system (called from the Air Heat Balance) and the zone (simulated
 		// in the Surface Heat Balance Manager).  In the future, this may be improved.
 		ManageSurfaceHeatBalance();
-		ManageEMS( emsCallFromEndZoneTimestepBeforeZoneReporting ); // EMS calling point
+		bool anyRan;
+		ManageEMS( emsCallFromEndZoneTimestepBeforeZoneReporting, anyRan ); // EMS calling point
 		RecKeepHeatBalance(); // Do any heat balance related record keeping
 
 		// This call has been moved to the FanSystemModule and does effect the output file
@@ -376,7 +377,7 @@ namespace HeatBalanceManager {
 
 		ReportHeatBalance(); // Manage heat balance reporting until the new reporting is in place
 
-		ManageEMS( emsCallFromEndZoneTimestepAfterZoneReporting ); // EMS calling point
+		ManageEMS( emsCallFromEndZoneTimestepAfterZoneReporting, anyRan ); // EMS calling point
 
 		UpdateEMSTrendVariables();
 
@@ -387,7 +388,7 @@ namespace HeatBalanceManager {
 				DayOfSim = 0; // Reset DayOfSim if Warmup converged
 				DayOfSimChr = "0";
 
-				ManageEMS( emsCallFromBeginNewEvironmentAfterWarmUp ); // calling point
+				ManageEMS( emsCallFromBeginNewEvironmentAfterWarmUp, anyRan ); // calling point
 			}
 
 		}
diff --git a/src/EnergyPlus/HeatBalanceSurfaceManager.cc b/src/EnergyPlus/HeatBalanceSurfaceManager.cc
index 19ed09d4fd3..e202b5d252b 100644
--- a/src/EnergyPlus/HeatBalanceSurfaceManager.cc
+++ b/src/EnergyPlus/HeatBalanceSurfaceManager.cc
@@ -1130,8 +1130,23 @@ namespace HeatBalanceSurfaceManager {
 				if ( isExterior ) {
 					++numExtSurfaces( Surface( iSurf ).Class );
 				}
+				if ( Surface( iSurf ).Class == SurfaceClass_Window ){
+					if ( SurfaceWindow( iSurf ).OriginalClass == SurfaceClass_GlassDoor || SurfaceWindow( iSurf ).OriginalClass == SurfaceClass_TDD_Diffuser ){
+						++numSurfaces( SurfaceWindow( iSurf ).OriginalClass );
+						if ( isExterior ) {
+							++numExtSurfaces( SurfaceWindow( iSurf ).OriginalClass );
+						}
+					}
+				}
 			}
 		}
+		// for fins and overhangs just add them explicitly since not otherwise classified
+		int totOverhangs = GetNumObjectsFound( "Shading:Overhang" ) + GetNumObjectsFound( "Shading:Overhang:Projection" );
+		numSurfaces( SurfaceClass_Overhang ) = totOverhangs;
+		numExtSurfaces( SurfaceClass_Overhang ) = totOverhangs;
+		int totFins = GetNumObjectsFound( "Shading:Fin" ) + GetNumObjectsFound( "Shading:Fin:Projection" );
+		numSurfaces( SurfaceClass_Fin ) = totFins;
+		numExtSurfaces( SurfaceClass_Fin ) = totFins;
 		// go through all the surfaces again and this time insert the net area results
 		for ( iSurf = 1; iSurf <= TotSurfaces; ++iSurf ) {
 			zonePt = Surface( iSurf ).Zone;
diff --git a/src/EnergyPlus/MixedAir.cc b/src/EnergyPlus/MixedAir.cc
index 8aecad2cec5..1c8c14ca445 100644
--- a/src/EnergyPlus/MixedAir.cc
+++ b/src/EnergyPlus/MixedAir.cc
@@ -213,7 +213,6 @@ namespace MixedAir {
 	int const UnitarySystem( 21 );
 	int const Humidifier( 22 );
 
-	int const ControllerSimple( 1 );
 	int const ControllerOutsideAir( 2 );
 	int const ControllerStandAloneERV( 3 );
 
@@ -276,8 +275,9 @@ namespace MixedAir {
 	// use these. They are cleared by clear_state() for use by unit tests, but normal simulations should be unaffected.
 	// This is purposefully in an anonymous namespace so nothing outside this implementation file can use it.
 		bool InitOAControllerOneTimeFlag( true );
-		bool InitOAControllerSetPointCheckFlag( true );
+		Array1D_bool InitOAControllerSetPointCheckFlag( true );
 		bool InitOAControllerSetUpAirLoopHVACVariables( true );
+		bool AllocateOAControllersFlag( true );
 		Array1D_string DesignSpecOAObjName; // name of the design specification outdoor air object
 		Array1D_int DesignSpecOAObjIndex; // index of the design specification outdoor air object
 		Array1D_string VentMechZoneName; // Zone or Zone List to apply mechanical ventilation rate
@@ -384,8 +384,9 @@ namespace MixedAir {
 		GetOAMixerInputFlag = true;
 		GetOAControllerInputFlag = true;
 		InitOAControllerOneTimeFlag = true;
-		InitOAControllerSetPointCheckFlag = true;
+		InitOAControllerSetPointCheckFlag.deallocate();
 		InitOAControllerSetUpAirLoopHVACVariables = true;
+		AllocateOAControllersFlag = true;
 		ControllerLists.deallocate();
 		OAController.deallocate();
 		OAMixer.deallocate();
@@ -910,7 +911,7 @@ namespace MixedAir {
 		// SUBROUTINE LOCAL VARIABLE DECLARATIONS:
 		int OAControllerNum;
 
-		if ( GetOAControllerInputFlag ) { // Gets input for object  first time Sim routine is called
+		if ( ( GetOAControllerInputFlag ) && ( AirLoopNum > 0 ) ) { // Gets input for object  first time Sim routine is called from an airloop
 			GetOAControllerInputs();
 			GetOAControllerInputFlag = false;
 		}
@@ -1426,22 +1427,18 @@ namespace MixedAir {
 		cAlphaFields.allocate( MaxAlphas );
 		cNumericFields.allocate( MaxNums );
 
-		NumOAControllers = GetNumObjectsFound( CurrentModuleObjects( CMO_OAController ) );
-		NumERVControllers = GetNumObjectsFound( CurrentModuleObjects( CMO_ERVController ) );
-		NumOAControllers += NumERVControllers;
 
-		//     Mangesh code to fix CR 8225 - 09/14/2010
-		//NumControllerList = GetNumObjectsFound("AirLoopHVAC:ControllerList")
-		//NumOASys = GetNumObjectsFound("AirLoopHVAC:OutdoorAirSystem")
+		// Count OAcontrollers and ERVcontrollers and allocate arrays
+		AllocateOAControllers();
 
-		if ( NumOAControllers > 0 ) {
 
-			OAController.allocate( NumOAControllers );
-			OAControllerInfo.allocate( NumOAControllers );
+		// If there are ERV controllers, they have been filled before now NumOAControllers includes the count of NumERVControllers
+		if ( NumOAControllers > NumERVControllers ) {
 			CurrentModuleObject = CurrentModuleObjects( CMO_OAController );
-			for ( OutAirNum = 1; OutAirNum <= NumOAControllers - NumERVControllers; ++OutAirNum ) {
-				GetObjectItem( CurrentModuleObject, OutAirNum, AlphArray, NumAlphas, NumArray, NumNums, IOStat, lNumericBlanks, lAlphaBlanks, cAlphaFields, cNumericFields );
-
+			int currentOAControllerNum = 0;
+			for ( OutAirNum = NumERVControllers+1; OutAirNum <= NumOAControllers; ++OutAirNum ) {
+				++currentOAControllerNum;
+				GetObjectItem( CurrentModuleObject, currentOAControllerNum, AlphArray, NumAlphas, NumArray, NumNums, IOStat, lNumericBlanks, lAlphaBlanks, cAlphaFields, cNumericFields );
 				IsNotOK = false;
 				IsBlank = false;
 				VerifyName( AlphArray( 1 ), OAController, OutAirNum - 1, IsNotOK, IsBlank, CurrentModuleObject + " Name" );
@@ -1685,14 +1682,6 @@ namespace MixedAir {
 				for ( groupNum = 1; groupNum <= NumGroups; ++groupNum ) {
 					VentMechZoneName( groupNum ) = AlphArray( ( groupNum - 1 ) * 3 + 5 );
 
-					for ( OutAirNum = 1; OutAirNum <= NumOAControllers; ++OutAirNum ) {
-						if ( OAController( OutAirNum ).VentilationMechanicalName == VentilationMechanical( VentMechNum ).Name && VentilationMechanical( VentMechNum ).DCVFlag ) {
-							AirLoopControlInfo( OutAirNum ).AirLoopDCVFlag = true;
-						} else {
-							AirLoopControlInfo( OutAirNum ).AirLoopDCVFlag = false;
-						}
-					}
-
 					//     Getting OA details from design specification OA object
 					if ( ! lAlphaBlanks( ( groupNum - 1 ) * 3 + 6 ) ) {
 						DesignSpecOAObjName( groupNum ) = AlphArray( ( groupNum - 1 ) * 3 + 6 );
@@ -2216,6 +2205,26 @@ namespace MixedAir {
 
 	}
 
+	void
+	AllocateOAControllers()
+	{
+
+		// PURPOSE OF THIS SUBROUTINE:
+		// Allocate the OA controller arrays which are shared by Controller:OutdoorAir and ZoneHVAC:EnergyRecoveryVentilator:Controller
+
+		using namespace InputProcessor;
+
+		if ( AllocateOAControllersFlag ) {
+			NumOAControllers = GetNumObjectsFound( CurrentModuleObjects( CMO_OAController ) );
+			NumERVControllers = GetNumObjectsFound( CurrentModuleObjects( CMO_ERVController ) );
+			NumOAControllers += NumERVControllers;
+			OAController.allocate( NumOAControllers );
+			OAControllerInfo.allocate( NumOAControllers );
+			AllocateOAControllersFlag = false;
+		}
+
+	}
+
 	void
 	GetOAMixerInputs()
 	{
@@ -2655,14 +2664,24 @@ namespace MixedAir {
 				}
 			}
 
-			if ( SameString( AlphArray( 18 ), "Yes" ) ) {
-				OAController( OutAirNum ).ModifyDuringHighOAMoisture = false;
-			} else if ( SameString( AlphArray( 18 ), "No" ) ) {
-				OAController( OutAirNum ).ModifyDuringHighOAMoisture = true;
+			if ( NumAlphas >= 18 ) {
+				if ( SameString( AlphArray( 18 ), "Yes" ) ) {
+					OAController( OutAirNum ).ModifyDuringHighOAMoisture = false;
+				} else if ( SameString( AlphArray( 18 ), "No" ) ) {
+					OAController( OutAirNum ).ModifyDuringHighOAMoisture = true;
+				} else {
+					ShowSevereError( CurrentModuleObject + " \"" + OAController( OutAirNum ).Name + "\", invalid field value" );
+					ShowContinueError( "..." + cAlphaFields( 18 ) + "=\"" + AlphArray( 18 ) + "\" - valid values are \"Yes\" or \"No\"." );
+					ErrorsFound = true;
+				}
 			} else {
-				ShowSevereError( CurrentModuleObject + " \"" + OAController( OutAirNum ).Name + "\", invalid field value" );
-				ShowContinueError( "..." + cAlphaFields( 18 ) + "=\"" + AlphArray( 18 ) + "\" - valid values are \"Yes\" or \"No\"." );
-				ErrorsFound = true;
+				if( OAController( OutAirNum ).Econo == NoEconomizer ) {
+					OAController( OutAirNum ).ModifyDuringHighOAMoisture = true;
+				} else {
+					OAController( OutAirNum ).ModifyDuringHighOAMoisture = false;
+					ShowWarningError( CurrentModuleObject + " \"" + OAController( OutAirNum ).Name + "\", missing field value" );
+					ShowContinueError( "..." + cAlphaFields( 18 ) + " will default to Yes when " + cAlphaFields( 16 ) + "= \"Yes\"" );
+				}
 			}
 
 		} else if ( SameString( AlphArray( 16 ), "No" ) || lAlphaBlanks( 16 ) ) {
@@ -2823,8 +2842,9 @@ namespace MixedAir {
 		//static bool MySetPointCheckFlag( true ); // One-time initialization flag
 		//static bool SetUpAirLoopHVACVariables( true ); // One-time initialization flag
 		//////////////////////////////////
-		static Array1D_bool MyEnvrnFlag; // One-time initialization flag
-		static Array1D_bool MySizeFlag; // One-time initialization flag
+		static Array1D_bool OAControllerMyOneTimeFlag; // One-time initialization flag
+		static Array1D_bool OAControllerMyEnvrnFlag; // One-time initialization flag
+		static Array1D_bool OAControllerMySizeFlag; // One-time initialization flag
 		static Array1D_bool MechVentCheckFlag; // One-time initialization flag
 		bool FoundZone; // Logical determines if ZONE object is accounted for in VENTILATION:MECHANICAL object
 		bool FoundAreaZone; // Logical determines if ZONE object is accounted for in VENTILATION:MECHANICAL object
@@ -2835,7 +2855,6 @@ namespace MixedAir {
 		Real64 RhoAirStdInit; // Standard air density
 		Real64 TotalPeopleOAFlow; // Total outside air required for PEOPLE objects served by this OA controller
 		int MixedAirNode; // Controller:OutdoorAir mixed air node
-		int OAControllerIndex; // Index to Controller:OutdoorAir
 		int ZoneNum; // DO loop index (zone number)
 		int ZoneIndex; // Index to zone in mechanical ventilation zone list
 		int AirLoopZoneInfoZoneNum; // Index to AirLoopZoneInfo structure
@@ -2847,7 +2866,6 @@ namespace MixedAir {
 		int thisNumForMixer; // Temporary array counter
 		int thisMixerIndex; // Temporary array counter
 		int OASysNum; // Temporary array counter
-		int thisOAController; // Temporary array counter
 		int found; // Temporary index to equipment
 		int OANode; // OA node index
 		int VentMechObjectNum; // Temporary variable
@@ -2869,104 +2887,100 @@ namespace MixedAir {
 		ErrorsFound = false;
 		OANode = 0;
 
-		if ( InitOAControllerOneTimeFlag ) {
-
-			MyEnvrnFlag.dimension( NumOAControllers, true );
-			MySizeFlag.dimension( NumOAControllers, true );
+		if (InitOAControllerOneTimeFlag) {
+			OAControllerMyOneTimeFlag.dimension(NumOAControllers, true);
+			OAControllerMyEnvrnFlag.dimension( NumOAControllers, true );
+			OAControllerMySizeFlag.dimension( NumOAControllers, true );
 			MechVentCheckFlag.dimension( NumOAControllers, true );
-
+			InitOAControllerSetPointCheckFlag.dimension ( NumOAControllers, true );
+			InitOAControllerOneTimeFlag = false;
+		}
+		if ( OAControllerMyOneTimeFlag( OAControllerNum ) ) {
 			// Determine Inlet node index for OAController, not a user input for controller, but is obtained from OutsideAirSys and OAMixer
-			// This input setup needs to happen for all controllers, not just the one first passed into this init routine
-			for ( thisOAController = 1; thisOAController <= NumOAControllers; ++thisOAController ) {
-
-				{ auto const SELECT_CASE_var( OAController( thisOAController ).ControllerType_Num );
-
-				if ( SELECT_CASE_var == ControllerOutsideAir ) {
-					thisOASys = 0;
-					for ( OASysNum = 1; OASysNum <= NumOASystems; ++OASysNum ) {
-						// find which OAsys has this controller
-						found = FindItemInList( OAController( thisOAController ).Name, OutsideAirSys( OASysNum ).ControllerName, isize( OutsideAirSys( OASysNum ).ControllerName ) );
-						if ( found != 0 ) {
-							thisOASys = OASysNum;
-							break; // we found it
-						}
+			{ auto const SELECT_CASE_var( OAController( OAControllerNum ).ControllerType_Num );
+
+			if ( SELECT_CASE_var == ControllerOutsideAir ) {
+				thisOASys = 0;
+				for ( OASysNum = 1; OASysNum <= NumOASystems; ++OASysNum ) {
+					// find which OAsys has this controller
+					found = FindItemInList( OAController( OAControllerNum ).Name, OutsideAirSys( OASysNum ).ControllerName, isize( OutsideAirSys( OASysNum ).ControllerName ) );
+					if ( found != 0 ) {
+						thisOASys = OASysNum;
+						break; // we found it
 					}
-					if ( thisOASys == 0 ) {
-						ShowSevereError( "InitOAController: Did not find OAController=\"" + OAController( thisOAController ).Name + "\"." );
-						ShowContinueError( "in list of valid OA Controllers." );
-						ErrorsFound = true;
-						continue;
-					}
-					thisNumForMixer = FindItem( CurrentModuleObjects( CMO_OAMixer ), OutsideAirSys( thisOASys ).ComponentType, isize( OutsideAirSys( thisOASys ).ComponentType ) );
-					if ( thisNumForMixer != 0 ) {
-						equipName = OutsideAirSys( thisOASys ).ComponentName( thisNumForMixer );
-						thisMixerIndex = FindItemInList( equipName, OAMixer );
-						if ( thisMixerIndex != 0 ) {
-							OAController( thisOAController ).InletNode = OAMixer( thisMixerIndex ).InletNode;
-						} else {
-							ShowSevereError( "InitOAController: Did not find OAMixer=\"" + equipName + "\"." );
-							ShowContinueError( "in list of valid OA Mixers." );
-							ErrorsFound = true;
-						}
+				}
+				if ( thisOASys == 0 ) {
+					ShowSevereError( "InitOAController: Did not find OAController=\"" + OAController( OAControllerNum ).Name + "\"." );
+					ShowContinueError( "in list of valid OA Controllers." );
+					ErrorsFound = true;
+				}
+				thisNumForMixer = FindItem( CurrentModuleObjects( CMO_OAMixer ), OutsideAirSys( thisOASys ).ComponentType, isize( OutsideAirSys( thisOASys ).ComponentType ) );
+				if ( thisNumForMixer != 0 ) {
+					equipName = OutsideAirSys( thisOASys ).ComponentName( thisNumForMixer );
+					thisMixerIndex = FindItemInList( equipName, OAMixer );
+					if ( thisMixerIndex != 0 ) {
+						OAController( OAControllerNum ).InletNode = OAMixer( thisMixerIndex ).InletNode;
 					} else {
-						ShowSevereError( "InitOAController: Did not find OutdoorAir:Mixer Component=\"OutdoorAir:Mixer\"." );
-						ShowContinueError( "in list of valid OA Components." );
+						ShowSevereError( "InitOAController: Did not find OAMixer=\"" + equipName + "\"." );
+						ShowContinueError( "in list of valid OA Mixers." );
 						ErrorsFound = true;
 					}
+				} else {
+					ShowSevereError( "InitOAController: Did not find OutdoorAir:Mixer Component=\"OutdoorAir:Mixer\"." );
+					ShowContinueError( "in list of valid OA Components." );
+					ErrorsFound = true;
+				}
 
-					if ( OAController( thisOAController ).InletNode == 0 ) { //throw an error
-						ShowSevereError( "InitOAController: Failed to find proper inlet node for OutdoorAir:Mixer and Controller = " + OAController( thisOAController ).Name );
-						ErrorsFound = true;
-					}
+				if ( OAController( OAControllerNum ).InletNode == 0 ) { //throw an error
+					ShowSevereError( "InitOAController: Failed to find proper inlet node for OutdoorAir:Mixer and Controller = " + OAController( OAControllerNum ).Name );
+					ErrorsFound = true;
+				}
 
-				} else if ( SELECT_CASE_var == ControllerStandAloneERV ) {
-					// set the inlet node to also equal the OA node because this is a special controller for economizing stand alone ERV
-					// with the assumption that equipment is bypassed....
+			} else if ( SELECT_CASE_var == ControllerStandAloneERV ) {
+				// set the inlet node to also equal the OA node because this is a special controller for economizing stand alone ERV
+				// with the assumption that equipment is bypassed....
 
-					OAController( thisOAController ).InletNode = OAController( thisOAController ).OANode;
+				OAController( OAControllerNum ).InletNode = OAController( OAControllerNum ).OANode;
 
-				} else {
-					ShowSevereError( "InitOAController: Failed to find ControllerType: " + OAController( thisOAController ).ControllerType );
-					ErrorsFound = true;
+			} else {
+				ShowSevereError( "InitOAController: Failed to find ControllerType: " + OAController( OAControllerNum ).ControllerType );
+				ErrorsFound = true;
 
-				}}
+			}}
 
-			}
-			InitOAControllerOneTimeFlag = false;
+			OAControllerMyOneTimeFlag( OAControllerNum ) = false;
 
 		}
 
-		if ( ! SysSizingCalc && InitOAControllerSetPointCheckFlag && DoSetPointTest && ! FirstHVACIteration ) {
-			for ( OAControllerIndex = 1; OAControllerIndex <= NumOAControllers; ++OAControllerIndex ) {
-				MixedAirNode = OAController( OAControllerIndex ).MixNode;
-				if ( MixedAirNode > 0 ) {
-					//      IF (OAController(OAControllerIndex)%Econo == 1 .AND. .NOT. AirLoopControlInfo(AirLoopNum)%CyclingFan) THEN
-					if ( OAController( OAControllerIndex ).Econo > NoEconomizer && AirLoopControlInfo( AirLoopNum ).AnyContFan ) {
-						if ( Node( MixedAirNode ).TempSetPoint == SensedNodeFlagValue ) {
-							if ( ! AnyEnergyManagementSystemInModel ) {
-								ShowSevereError( "MixedAir: Missing temperature setpoint for economizer controller " + OAController( OAControllerIndex ).Name );
+		if ( ! SysSizingCalc && InitOAControllerSetPointCheckFlag( OAControllerNum ) && DoSetPointTest && ! FirstHVACIteration ) {
+			MixedAirNode = OAController( OAControllerNum ).MixNode;
+			if ( MixedAirNode > 0 ) {
+				//      IF (OAController(OAControllerNum)%Econo == 1 .AND. .NOT. AirLoopControlInfo(AirLoopNum)%CyclingFan) THEN
+				if ( OAController( OAControllerNum ).Econo > NoEconomizer && AirLoopControlInfo( AirLoopNum ).AnyContFan ) {
+					if ( Node( MixedAirNode ).TempSetPoint == SensedNodeFlagValue ) {
+						if ( ! AnyEnergyManagementSystemInModel ) {
+							ShowSevereError( "MixedAir: Missing temperature setpoint for economizer controller " + OAController( OAControllerNum ).Name );
+							ShowSevereError( "Node Referenced (by Controller)=" + NodeID( MixedAirNode ) );
+							ShowContinueError( "  use a Setpoint Manager with Control Variable = \"Temperature\" to establish a setpoint at the mixed air node." );
+							SetPointErrorFlag = true;
+						} else {
+							// add call to check node in EMS
+							CheckIfNodeSetPointManagedByEMS( MixedAirNode, iTemperatureSetPoint, SetPointErrorFlag );
+							if ( SetPointErrorFlag ) {
+								ShowSevereError( "MixedAir: Missing temperature setpoint for economizer controller " + OAController( OAControllerNum ).Name );
 								ShowSevereError( "Node Referenced (by Controller)=" + NodeID( MixedAirNode ) );
 								ShowContinueError( "  use a Setpoint Manager with Control Variable = \"Temperature\" to establish a setpoint at the mixed air node." );
-								SetPointErrorFlag = true;
-							} else {
-								// add call to check node in EMS
-								CheckIfNodeSetPointManagedByEMS( MixedAirNode, iTemperatureSetPoint, SetPointErrorFlag );
-								if ( SetPointErrorFlag ) {
-									ShowSevereError( "MixedAir: Missing temperature setpoint for economizer controller " + OAController( OAControllerIndex ).Name );
-									ShowSevereError( "Node Referenced (by Controller)=" + NodeID( MixedAirNode ) );
-									ShowContinueError( "  use a Setpoint Manager with Control Variable = \"Temperature\" to establish a setpoint at the mixed air node." );
-									ShowContinueError( "Or add EMS Actuator to provide temperature setpoint at this node" );
-								}
+								ShowContinueError( "Or add EMS Actuator to provide temperature setpoint at this node" );
 							}
 						}
 					}
 				}
 			}
 
-			InitOAControllerSetPointCheckFlag = false;
+			InitOAControllerSetPointCheckFlag( OAControllerNum ) = false;
 		}
 
-		if ( ! SysSizingCalc && MySizeFlag( OAControllerNum ) ) {
+		if ( ! SysSizingCalc && OAControllerMySizeFlag( OAControllerNum ) ) {
 			SizeOAController( OAControllerNum );
 			if ( AirLoopNum > 0 ) {
 				AirLoopControlInfo( AirLoopNum ).OACtrlNum = OAControllerNum;
@@ -2991,15 +3005,15 @@ namespace MixedAir {
 				ShowContinueError( "  To set the minimum outside air flow rate use the \"Design (minimum) outdoor air flow rate\" field in the Sizing:System object" );
 				ErrorsFound = true;
 			}
-			MySizeFlag( OAControllerNum ) = false;
+			OAControllerMySizeFlag( OAControllerNum ) = false;
 		}
 
-		if ( BeginEnvrnFlag && MyEnvrnFlag( OAControllerNum ) ) {
+		if ( BeginEnvrnFlag && OAControllerMyEnvrnFlag( OAControllerNum ) ) {
 			OANode = OAController( OAControllerNum ).OANode;
 			RhoAirStdInit = StdRhoAir;
 			OAController( OAControllerNum ).MinOAMassFlowRate = OAController( OAControllerNum ).MinOA * RhoAirStdInit;
 			OAController( OAControllerNum ).MaxOAMassFlowRate = OAController( OAControllerNum ).MaxOA * RhoAirStdInit;
-			MyEnvrnFlag( OAControllerNum ) = false;
+			OAControllerMyEnvrnFlag( OAControllerNum ) = false;
 			Node( OANode ).MassFlowRateMax = OAController( OAControllerNum ).MaxOAMassFlowRate;
 
 			//predefined reporting
@@ -3047,7 +3061,7 @@ namespace MixedAir {
 		}
 
 		if ( ! BeginEnvrnFlag ) {
-			MyEnvrnFlag( OAControllerNum ) = true;
+			OAControllerMyEnvrnFlag( OAControllerNum ) = true;
 		}
 
 		VentMechObjectNum = OAController( OAControllerNum ).VentMechObjectNum;
@@ -3203,7 +3217,7 @@ namespace MixedAir {
 		// two IF statements are checked each time through Init (e.g., if StandAloneERV controllers are used
 		// without AirloopHVAC objects).
 		if ( InitOAControllerSetUpAirLoopHVACVariables ) {
-			if ( NumPrimaryAirSys > 0 ) {
+			if ( AirLoopNum > 0 ) {
 				// Added code to report (TH, 10/20/2008):
 				//   air economizer status (1 = on, 0 = off or does not exist), and
 				//   actual and minimum outside air fraction (0 to 1)
@@ -3279,6 +3293,12 @@ namespace MixedAir {
 						SetupEMSActuator( "Outdoor Air Controller", OAController( OAControllerLoop ).Name, "Air Mass Flow Rate", "[kg/s]", OAController( OAControllerLoop ).EMSOverrideOARate, OAController( OAControllerLoop ).EMSOARateValue );
 					}
 
+					VentMechObjectNum = OAController( OAControllerLoop ).VentMechObjectNum;
+					if ( VentMechObjectNum > 0 && thisAirLoop > 0){
+						if (!VentilationMechanical( VentMechObjectNum ).DCVFlag){
+							AirLoopControlInfo( thisAirLoop ).AirLoopDCVFlag = false;
+						}
+					}
 				}
 
 				InitOAControllerSetUpAirLoopHVACVariables = false;
@@ -3657,7 +3677,7 @@ namespace MixedAir {
 		Real64 ZoneMinCO2; // Minimum CO2 concentration in zone
 		Real64 ZoneContamControllerSched; // Schedule value for ZoneControl:ContaminantController
 		Real64 CO2PeopleGeneration; // CO2 generation from people at design level
-		Real64 MaximumOAFracBySetPoint; // The maximum OA fraction due to freezing cooling coil check 
+		Real64 MaximumOAFracBySetPoint; // The maximum OA fraction due to freezing cooling coil check
 
 		static Real64 Ep( 1.0 ); // zone primary air fraction
 		static Real64 Er( 0.0 ); // zone secondary recirculation fraction
@@ -3677,6 +3697,9 @@ namespace MixedAir {
 		ZoneOAMax = 0.0;
 		ZoneContamControllerSched = 0.0;
 
+		// Assign references
+		auto & thisController( OAController( OAControllerNum ) );
+		auto & thisControllerInfo( OAControllerInfo( OAControllerNum ) );
 		if ( AirLoopNum > 0 ) {
 			AirLoopEconoLockout = AirLoopControlInfo( AirLoopNum ).EconoLockout;
 			AirLoopNightVent = AirLoopControlInfo( AirLoopNum ).NightVent;
@@ -3688,22 +3711,22 @@ namespace MixedAir {
 		}
 
 		// Check for no flow
-		if ( OAController( OAControllerNum ).MixMassFlow <= SmallMassFlow ) {
+		if ( thisController.MixMassFlow <= SmallMassFlow ) {
 
-			OAController( OAControllerNum ).OAMassFlow = 0.0; // outside air mass flow rate
-			OAController( OAControllerNum ).RelMassFlow = 0.0; // relief air mass flow rate
-			OAController( OAControllerNum ).MixMassFlow = 0.0; // mixed air mass flow rate
-			OAController( OAControllerNum ).MinOAFracLimit = 0.0; // minimum OA fraction limit
+			thisController.OAMassFlow = 0.0; // outside air mass flow rate
+			thisController.RelMassFlow = 0.0; // relief air mass flow rate
+			thisController.MixMassFlow = 0.0; // mixed air mass flow rate
+			thisController.MinOAFracLimit = 0.0; // minimum OA fraction limit
 
-			OAController( OAControllerNum ).EconomizerStatus = 0; // economizer status for reporting
-			OAController( OAControllerNum ).HeatRecoveryBypassStatus = 0; // HR bypass status for reporting
-			OAController( OAControllerNum ).HRHeatingCoilActive = 0; // resets report variable
-			OAController( OAControllerNum ).MixedAirTempAtMinOAFlow = Node( OAController( OAControllerNum ).RetNode ).Temp; // track return T
-			OAController( OAControllerNum ).HighHumCtrlStatus = 0; // high humdity control status for reporting
-			OAController( OAControllerNum ).OAFractionRpt = 0.0; // actual OA fraction for reporting
+			thisController.EconomizerStatus = 0; // economizer status for reporting
+			thisController.HeatRecoveryBypassStatus = 0; // HR bypass status for reporting
+			thisController.HRHeatingCoilActive = 0; // resets report variable
+			thisController.MixedAirTempAtMinOAFlow = Node( thisController.RetNode ).Temp; // track return T
+			thisController.HighHumCtrlStatus = 0; // high humdity control status for reporting
+			thisController.OAFractionRpt = 0.0; // actual OA fraction for reporting
 
-			OAControllerInfo( OAControllerNum ).EconoActive = false; // DataAirLoop variable (OA Controllers)
-			OAControllerInfo( OAControllerNum ).HighHumCtrlActive = false; // DataAirLoop variable (OA Controllers)
+			thisControllerInfo.EconoActive = false; // DataAirLoop variable (OA Controllers)
+			thisControllerInfo.HighHumCtrlActive = false; // DataAirLoop variable (OA Controllers)
 
 			// also reset air loop data for use by other routines
 			if ( AirLoopNum > 0 ) {
@@ -3722,25 +3745,25 @@ namespace MixedAir {
 		// set OutAirMinFrac
 		if ( AirLoopNum > 0 ) {
 			if ( AirLoopFlow( AirLoopNum ).DesSupply >= SmallAirVolFlow ) {
-				OutAirMinFrac = OAController( OAControllerNum ).MinOAMassFlowRate / AirLoopFlow( AirLoopNum ).DesSupply;
+				OutAirMinFrac = thisController.MinOAMassFlowRate / AirLoopFlow( AirLoopNum ).DesSupply;
 			} else {
 				OutAirMinFrac = 0.0;
 			}
 		} else {
-			if ( OAController( OAControllerNum ).MaxOA >= SmallAirVolFlow ) {
-				OutAirMinFrac = OAController( OAControllerNum ).MinOA / OAController( OAControllerNum ).MaxOA;
+			if ( thisController.MaxOA >= SmallAirVolFlow ) {
+				OutAirMinFrac = thisController.MinOA / thisController.MaxOA;
 			} else {
 				OutAirMinFrac = 0.0;
 			}
 		}
-		if ( OAController( OAControllerNum ).MinOASchPtr > 0 ) {
-			MinOASchedVal = GetCurrentScheduleValue( OAController( OAControllerNum ).MinOASchPtr );
+		if ( thisController.MinOASchPtr > 0 ) {
+			MinOASchedVal = GetCurrentScheduleValue( thisController.MinOASchPtr );
 			MinOASchedVal = min( max( MinOASchedVal, 0.0 ), 1.0 );
 			OutAirMinFrac *= MinOASchedVal;
 		}
 
 		// Get mechanical ventilation
-		VentMechObjectNum = OAController( OAControllerNum ).VentMechObjectNum;
+		VentMechObjectNum = thisController.VentMechObjectNum;
 		if ( AirLoopNum > 0 && VentMechObjectNum != 0 ) {
 			// Apply mechanical ventilation only when it is available/allowed
 			if ( GetCurrentScheduleValue( VentilationMechanical( VentMechObjectNum ).SchPtr ) > 0 ) {
@@ -4171,26 +4194,26 @@ namespace MixedAir {
 		}
 
 		// Define an outside air signal
-		if ( OAController( OAControllerNum ).MixedAirSPMNum > 0 ) {
-			OAController( OAControllerNum ).CoolCoilFreezeCheck = GetCoilFreezingCheckFlag( OAController( OAControllerNum ).MixedAirSPMNum );
+		if ( thisController.MixedAirSPMNum > 0 ) {
+			thisController.CoolCoilFreezeCheck = GetCoilFreezingCheckFlag( thisController.MixedAirSPMNum );
 		} else {
-			OAController( OAControllerNum ).CoolCoilFreezeCheck = false;
+			thisController.CoolCoilFreezeCheck = false;
 		}
-		if ( std::abs( OAController( OAControllerNum ).RetTemp - OAController( OAControllerNum ).InletTemp ) > SmallTempDiff ) {
-			OutAirSignal = ( OAController( OAControllerNum ).RetTemp - OAController( OAControllerNum ).MixSetTemp ) / ( OAController( OAControllerNum ).RetTemp - OAController( OAControllerNum ).InletTemp );
-			if ( OAController( OAControllerNum ).CoolCoilFreezeCheck ) {
-				OAController( OAControllerNum ).MaxOAFracBySetPoint = 0.0;
+		if ( std::abs( thisController.RetTemp - thisController.InletTemp ) > SmallTempDiff ) {
+			OutAirSignal = ( thisController.RetTemp - thisController.MixSetTemp ) / ( thisController.RetTemp - thisController.InletTemp );
+			if ( thisController.CoolCoilFreezeCheck ) {
+				thisController.MaxOAFracBySetPoint = 0.0;
 				MaximumOAFracBySetPoint = OutAirSignal;
 			}
 		} else {
-			if ( OAController( OAControllerNum ).RetTemp - OAController( OAControllerNum ).MixSetTemp < 0.0 ) {
-				if ( OAController( OAControllerNum ).RetTemp - OAController( OAControllerNum ).InletTemp >= 0.0 ) {
+			if ( thisController.RetTemp - thisController.MixSetTemp < 0.0 ) {
+				if ( thisController.RetTemp - thisController.InletTemp >= 0.0 ) {
 					OutAirSignal = -1.0;
 				} else {
 					OutAirSignal = 1.0;
 				}
 			} else {
-				if ( OAController( OAControllerNum ).RetTemp - OAController( OAControllerNum ).InletTemp >= 0.0 ) {
+				if ( thisController.RetTemp - thisController.InletTemp >= 0.0 ) {
 					OutAirSignal = 1.0;
 				} else {
 					OutAirSignal = -1.0;
@@ -4200,12 +4223,12 @@ namespace MixedAir {
 		OutAirSignal = min( max( OutAirSignal, OutAirMinFrac ), 1.0 );
 
 		// If no economizer, set to minimum and disable economizer and high humidity control
-		if ( OAController( OAControllerNum ).Econo == NoEconomizer ) {
+		if ( thisController.Econo == NoEconomizer ) {
 			OutAirSignal = OutAirMinFrac;
 			EconomizerOperationFlag = false;
 			EconomizerAirFlowScheduleValue = 0.0;
 			HighHumidityOperationFlag = false;
-		} else if ( OAController( OAControllerNum ).MaxOA < SmallAirVolFlow ) {
+		} else if ( thisController.MaxOA < SmallAirVolFlow ) {
 			OutAirSignal = OutAirMinFrac;
 			EconomizerOperationFlag = false;
 			EconomizerAirFlowScheduleValue = 0.0;
@@ -4220,66 +4243,66 @@ namespace MixedAir {
 			// Otherwise do the limit checks
 			EconomizerOperationFlag = true;
 			// Outside air temp greater than mix air setpoint
-			if ( OAController( OAControllerNum ).InletTemp > OAController( OAControllerNum ).MixSetTemp ) {
+			if ( thisController.InletTemp > thisController.MixSetTemp ) {
 				OutAirSignal = 1.0;
 			}
 			// Return air temp limit
-			if ( OAController( OAControllerNum ).Econo == DifferentialDryBulb ) {
-				if ( OAController( OAControllerNum ).InletTemp > OAController( OAControllerNum ).RetTemp ) {
+			if ( thisController.Econo == DifferentialDryBulb ) {
+				if ( thisController.InletTemp > thisController.RetTemp ) {
 					OutAirSignal = OutAirMinFrac;
 					EconomizerOperationFlag = false;
 				}
 				Checksetpoints( OAControllerNum, OutAirMinFrac, OutAirSignal, EconomizerOperationFlag );
 			}
 			// Return air enthalpy limit
-			if ( OAController( OAControllerNum ).Econo == DifferentialEnthalpy ) {
-				if ( OAController( OAControllerNum ).InletEnth > OAController( OAControllerNum ).RetEnth ) {
+			if ( thisController.Econo == DifferentialEnthalpy ) {
+				if ( thisController.InletEnth > thisController.RetEnth ) {
 					OutAirSignal = OutAirMinFrac;
 					EconomizerOperationFlag = false;
 				}
 				Checksetpoints( OAControllerNum, OutAirMinFrac, OutAirSignal, EconomizerOperationFlag );
 			}
 			// Outside air temperature limit
-			if ( OAController( OAControllerNum ).Econo == FixedDryBulb ) {
+			if ( thisController.Econo == FixedDryBulb ) {
 				Checksetpoints( OAControllerNum, OutAirMinFrac, OutAirSignal, EconomizerOperationFlag );
 			}
 			//Fixed Enthalpy limit
-			if ( OAController( OAControllerNum ).Econo == FixedEnthalpy ) {
+			if ( thisController.Econo == FixedEnthalpy ) {
 				Checksetpoints( OAControllerNum, OutAirMinFrac, OutAirSignal, EconomizerOperationFlag );
 			}
 			//FIXED DEW POINT AND DRY BULB TEMPERATURE STRATEGY
-			if ( OAController( OAControllerNum ).Econo == FixedDewPointAndDryBulb ) {
+			if ( thisController.Econo == FixedDewPointAndDryBulb ) {
 				Checksetpoints( OAControllerNum, OutAirMinFrac, OutAirSignal, EconomizerOperationFlag );
 			}
 			// ELECRONIC ENTHALPY, HUMIDITY RATIO CURVE
-			if ( OAController( OAControllerNum ).Econo == ElectronicEnthalpy ) {
+			if ( thisController.Econo == ElectronicEnthalpy ) {
 				Checksetpoints( OAControllerNum, OutAirMinFrac, OutAirSignal, EconomizerOperationFlag );
 			}
 			// Differential dry bulb and enthalpy strategy
-			if ( OAController( OAControllerNum ).Econo == DifferentialDryBulbAndEnthalpy ) {
-				if ( OAController( OAControllerNum ).InletTemp > OAController( OAControllerNum ).RetTemp ) {
+			if ( thisController.Econo == DifferentialDryBulbAndEnthalpy ) {
+				if ( thisController.InletTemp > thisController.RetTemp ) {
 					OutAirSignal = OutAirMinFrac;
 					EconomizerOperationFlag = false;
 				}
-				if ( OAController( OAControllerNum ).InletEnth > OAController( OAControllerNum ).RetEnth ) {
+				if ( thisController.InletEnth > thisController.RetEnth ) {
 					OutAirSignal = OutAirMinFrac;
 					EconomizerOperationFlag = false;
 				}
 				Checksetpoints( OAControllerNum, OutAirMinFrac, OutAirSignal, EconomizerOperationFlag );
 			}
 
-			if ( OAController( OAControllerNum ).TempLowLim != BlankNumeric && OAController( OAControllerNum ).OATemp < OAController( OAControllerNum ).TempLowLim ) {
+			if ( thisController.TempLowLim != BlankNumeric && thisController.OATemp < thisController.TempLowLim ) {
 				OutAirSignal = OutAirMinFrac;
 				EconomizerOperationFlag = false;
 			}
 			// Increase air flow for humidity control
 			// (HumidistatZoneNum is greater than 0 IF High Humidity Control Flag = YES, checked in GetInput)
-			if ( OAController( OAControllerNum ).HumidistatZoneNum > 0 ) {
+			if ( thisController.HumidistatZoneNum > 0 ) {
 				//   IF humidistat senses a moisture load check to see if modifying air flow is appropriate, otherwise disable modified air flow
-				if ( ZoneSysMoistureDemand( OAController( OAControllerNum ).HumidistatZoneNum ).TotalOutputRequired < 0.0 ) {
+				if ( ZoneSysMoistureDemand( thisController.HumidistatZoneNum ).TotalOutputRequired < 0.0 ) {
 					//     IF OAController is not allowed to modify air flow during high outdoor humrat condition, then disable modified air flow
 					//     if indoor humrat is less than or equal to outdoor humrat
-					if ( ! OAController( OAControllerNum ).ModifyDuringHighOAMoisture && Node( OAController( OAControllerNum ).NodeNumofHumidistatZone ).HumRat <= OAController( OAControllerNum ).OAHumRat ) {
+					if ( ! thisController.ModifyDuringHighOAMoisture && Node( thisController.NodeNumofHumidistatZone ).HumRat <= thisController.OAHumRat ) {
 						HighHumidityOperationFlag = false;
 					} else {
 						HighHumidityOperationFlag = true;
@@ -4293,8 +4316,8 @@ namespace MixedAir {
 
 			// Check time of day economizer schedule, enable economizer if schedule value > 0
 			EconomizerAirFlowScheduleValue = 0.0;
-			if ( OAController( OAControllerNum ).EconomizerOASchedPtr > 0 ) {
-				EconomizerAirFlowScheduleValue = GetCurrentScheduleValue( OAController( OAControllerNum ).EconomizerOASchedPtr );
+			if ( thisController.EconomizerOASchedPtr > 0 ) {
+				EconomizerAirFlowScheduleValue = GetCurrentScheduleValue( thisController.EconomizerOASchedPtr );
 				if ( EconomizerAirFlowScheduleValue > 0.0 ) {
 					EconomizerOperationFlag = true;
 					OutAirSignal = 1.0;
@@ -4306,11 +4329,11 @@ namespace MixedAir {
 		// OutAirSignal will not give exactly the correct mixed air temperature (equal to the setpoint) since
 		// it was calculated using the approximate method of sensible energy balance. Now we have to get the
 		// accurate result using a full mass, enthalpy and moisture balance and iteration.
-		if ( OutAirSignal > OutAirMinFrac && OutAirSignal < 1.0 && OAController( OAControllerNum ).MixMassFlow > VerySmallMassFlow && OAController( OAControllerNum ).ControllerType_Num == ControllerOutsideAir && ! AirLoopNightVent ) {
-			Par( 1 ) = OAController( OAControllerNum ).MixNode;
-			Par( 2 ) = OAController( OAControllerNum ).RetNode;
-			Par( 3 ) = OAController( OAControllerNum ).InletNode;
-			Par( 4 ) = OAController( OAControllerNum ).MixMassFlow;
+		if ( OutAirSignal > OutAirMinFrac && OutAirSignal < 1.0 && thisController.MixMassFlow > VerySmallMassFlow && thisController.ControllerType_Num == ControllerOutsideAir && ! AirLoopNightVent ) {
+			Par( 1 ) = thisController.MixNode;
+			Par( 2 ) = thisController.RetNode;
+			Par( 3 ) = thisController.InletNode;
+			Par( 4 ) = thisController.MixMassFlow;
 			SolveRegulaFalsi( Acc, MaxIte, SolFla, OASignal, MixedAirControlTempResidual, OutAirMinFrac, 1.0, Par );
 			if ( SolFla < 0 ) {
 				OASignal = OutAirSignal;
@@ -4320,15 +4343,15 @@ namespace MixedAir {
 		}
 
 		// Economizer choice "Bypass" forces minimum OA except when high humidity air flow is active based on indoor RH
-		if ( OAController( OAControllerNum ).EconBypass && EconomizerAirFlowScheduleValue == 0.0 ) {
+		if ( thisController.EconBypass && EconomizerAirFlowScheduleValue == 0.0 ) {
 			OASignal = OutAirMinFrac;
 		}
 
 		// Set outdoor air signal based on OA flow ratio if high humidity air flow is enabled
 		if ( HighHumidityOperationFlag ) {
-			if ( OAController( OAControllerNum ).MixMassFlow > 0.0 ) {
+			if ( thisController.MixMassFlow > 0.0 ) {
 				//   calculate the actual ratio of outside air to mixed air so the magnitude of OA during high humidity control is correct
-				OASignal = max( OutAirMinFrac, ( OAController( OAControllerNum ).HighRHOAFlowRatio * OAController( OAControllerNum ).MaxOAMassFlowRate / OAController( OAControllerNum ).MixMassFlow ) );
+				OASignal = max( OutAirMinFrac, ( thisController.HighRHOAFlowRatio * thisController.MaxOAMassFlowRate / thisController.MixMassFlow ) );
 			}
 		}
 
@@ -4336,8 +4359,8 @@ namespace MixedAir {
 		if ( AirLoopNightVent ) OASignal = 1.0;
 
 		// Changed by Amit for new feature
-		if ( OAController( OAControllerNum ).MinOAflowSchPtr > 0 ) {
-			MinOAflowfracVal = GetCurrentScheduleValue( OAController( OAControllerNum ).MinOAflowSchPtr );
+		if ( thisController.MinOAflowSchPtr > 0 ) {
+			MinOAflowfracVal = GetCurrentScheduleValue( thisController.MinOAflowSchPtr );
 			MinOAflowfracVal = min( max( MinOAflowfracVal, 0.0 ), 1.0 );
 			if ( MinOAflowfracVal > OutAirMinFrac ) {
 				OutAirMinFrac = MinOAflowfracVal;
@@ -4345,114 +4368,114 @@ namespace MixedAir {
 			OASignal = max( MinOAflowfracVal, OASignal );
 		}
 
-		if ( OAController( OAControllerNum ).MaxOAflowSchPtr > 0 ) {
-			MaxOAflowfracVal = GetCurrentScheduleValue( OAController( OAControllerNum ).MaxOAflowSchPtr );
+		if ( thisController.MaxOAflowSchPtr > 0 ) {
+			MaxOAflowfracVal = GetCurrentScheduleValue( thisController.MaxOAflowSchPtr );
 			MaxOAflowfracVal = min( max( MaxOAflowfracVal, 0.0 ), 1.0 );
 			if ( MaxOAflowfracVal < OutAirMinFrac ) {
 				OutAirMinFrac = MaxOAflowfracVal;
 			}
 			OASignal = min( MaxOAflowfracVal, OASignal );
 
-			if ( OAController( OAControllerNum ).MinOAflowSchPtr > 0 ) {
+			if ( thisController.MinOAflowSchPtr > 0 ) {
 				if ( MaxOAflowfracVal < MinOAflowfracVal ) {
-					ShowWarningError( "Min OA flow frac Greater than Max OA flow frac - check the Schedules in \"Controller:OutdoorAir \" " + OAController( OAControllerNum ).MinOAflowSch + OAController( OAControllerNum ).MaxOAflowSch );
+					ShowWarningError( "Min OA flow frac Greater than Max OA flow frac - check the Schedules in \"Controller:OutdoorAir \" " + thisController.MinOAflowSch + thisController.MaxOAflowSch );
 				}
 			}
 
 		}
 
-		if ( OAController( OAControllerNum ).CoolCoilFreezeCheck ) {
+		if ( thisController.CoolCoilFreezeCheck ) {
 			MaximumOAFracBySetPoint = min( max( MaximumOAFracBySetPoint, 0.0 ), 1.0 );
-			OAController( OAControllerNum ).MaxOAFracBySetPoint = MaximumOAFracBySetPoint;
+			thisController.MaxOAFracBySetPoint = MaximumOAFracBySetPoint;
 			if ( MaximumOAFracBySetPoint < OutAirMinFrac ) {
 				OutAirMinFrac = MaximumOAFracBySetPoint;
-				if ( AirLoopNum > 0 ) AirLoopFlow( AirLoopNum ).MinOutAir = OutAirMinFrac * OAController( OAControllerNum ).MixMassFlow;
+				if ( AirLoopNum > 0 ) AirLoopFlow( AirLoopNum ).MinOutAir = OutAirMinFrac * thisController.MixMassFlow;
 			}
 			OASignal = min( MaximumOAFracBySetPoint, OASignal );
 		}
 
-		OAController( OAControllerNum ).OAMassFlow = OASignal * OAController( OAControllerNum ).MixMassFlow;
+		thisController.OAMassFlow = OASignal * thisController.MixMassFlow;
 
 		// Do not allow OA to be below Ventilation:Mechanical flow rate or above mixed mass flow rate
 		if ( AirLoopNum > 0 && VentMechObjectNum != 0 ) {
-			if ( MechVentOutsideAirFlow > OAController( OAControllerNum ).OAMassFlow ) {
-				OAController( OAControllerNum ).OAMassFlow = min( MechVentOutsideAirFlow, OAController( OAControllerNum ).MixMassFlow );
+			if ( MechVentOutsideAirFlow > thisController.OAMassFlow ) {
+				thisController.OAMassFlow = min( MechVentOutsideAirFlow, thisController.MixMassFlow );
 			}
 		}
 
 		// Do not allow OA to be below Exh for controller:outside air
-		if ( OAController( OAControllerNum ).ControllerType_Num == ControllerOutsideAir ) {
-			OAController( OAControllerNum ).OAMassFlow = max( OAController( OAControllerNum ).ExhMassFlow, OAController( OAControllerNum ).OAMassFlow );
+		if ( thisController.ControllerType_Num == ControllerOutsideAir ) {
+			thisController.OAMassFlow = max( thisController.ExhMassFlow, thisController.OAMassFlow );
 		}
 
 		// if fixed minimum, don't let go below min OA
-		if ( OAController( OAControllerNum ).FixedMin ) {
+		if ( thisController.FixedMin ) {
 			// cycling fans allow "average" min OA to be below minimum
 			if ( ! AirLoopCyclingFan ) {
-				OAController( OAControllerNum ).OAMassFlow = max( OAController( OAControllerNum ).OAMassFlow, OAController( OAControllerNum ).MinOAMassFlowRate * MinOASchedVal );
+				thisController.OAMassFlow = max( thisController.OAMassFlow, thisController.MinOAMassFlowRate * MinOASchedVal );
 			}
 		}
 
 		// Don't let OA flow be > mixed air flow.
 		// Seems if RAB (return air bypass) that this should be don't let OA flow be > design supply flow but that causes other issues
-		OAController( OAControllerNum ).OAMassFlow = min( OAController( OAControllerNum ).OAMassFlow, OAController( OAControllerNum ).MixMassFlow );
+		thisController.OAMassFlow = min( thisController.OAMassFlow, thisController.MixMassFlow );
 
 		// Don't let the OA flow be > than the max OA limit. OA for high humidity control is allowed to be greater than max OA.
 		// Night Ventilation has priority and may override an OASignal > 1 high humidity condition with OASignal = 1
 		if ( HighHumidityOperationFlag ) {
-			OAController( OAControllerNum ).OAMassFlow = min( OAController( OAControllerNum ).OAMassFlow, OAController( OAControllerNum ).MaxOAMassFlowRate * max( 1.0, OASignal ) );
+			thisController.OAMassFlow = min( thisController.OAMassFlow, thisController.MaxOAMassFlowRate * max( 1.0, OASignal ) );
 		} else {
-			OAController( OAControllerNum ).OAMassFlow = min( OAController( OAControllerNum ).OAMassFlow, OAController( OAControllerNum ).MaxOAMassFlowRate );
+			thisController.OAMassFlow = min( thisController.OAMassFlow, thisController.MaxOAMassFlowRate );
 		}
 
-		if ( !WarmupFlag && !DoingSizing && ( OAController( OAControllerNum ).ManageDemand ) && ( OAController( OAControllerNum ).OAMassFlow > OAController( OAControllerNum ).DemandLimitFlowRate ) )
-			OAController( OAControllerNum ).OAMassFlow = OAController( OAControllerNum ).DemandLimitFlowRate;
-		if ( OAController( OAControllerNum ).EMSOverrideOARate ) {
-			OAController( OAControllerNum ).OAMassFlow = OAController( OAControllerNum ).EMSOARateValue;
+		if ( !WarmupFlag && !DoingSizing && ( thisController.ManageDemand ) && ( thisController.OAMassFlow > thisController.DemandLimitFlowRate ) )
+			thisController.OAMassFlow = thisController.DemandLimitFlowRate;
+		if ( thisController.EMSOverrideOARate ) {
+			thisController.OAMassFlow = thisController.EMSOARateValue;
 		}
 
 		// save the min outside air flow fraction and max outside air mass flow rate
 		if ( AirLoopNum > 0 ) {
 			AirLoopFlow( AirLoopNum ).OAMinFrac = OutAirMinFrac;
-			AirLoopFlow( AirLoopNum ).MinOutAir = OutAirMinFrac * OAController( OAControllerNum ).MixMassFlow;
-			if ( OAController( OAControllerNum ).MixMassFlow > 0.0 ) {
-				AirLoopFlow( AirLoopNum ).OAFrac = OAController( OAControllerNum ).OAMassFlow / OAController( OAControllerNum ).MixMassFlow;
+			AirLoopFlow( AirLoopNum ).MinOutAir = OutAirMinFrac * thisController.MixMassFlow;
+			if ( thisController.MixMassFlow > 0.0 ) {
+				AirLoopFlow( AirLoopNum ).OAFrac = thisController.OAMassFlow / thisController.MixMassFlow;
 			} else {
 				AirLoopFlow( AirLoopNum ).OAFrac = 0.0;
 			}
-			OAController( OAControllerNum ).MinOAFracLimit = OutAirMinFrac;
+			thisController.MinOAFracLimit = OutAirMinFrac;
 			if ( HighHumidityOperationFlag && OASignal > 1.0 ) {
-				AirLoopFlow( AirLoopNum ).MaxOutAir = OAController( OAControllerNum ).MaxOAMassFlowRate * OASignal;
+				AirLoopFlow( AirLoopNum ).MaxOutAir = thisController.MaxOAMassFlowRate * OASignal;
 			} else {
-				AirLoopFlow( AirLoopNum ).MaxOutAir = OAController( OAControllerNum ).MaxOAMassFlowRate;
+				AirLoopFlow( AirLoopNum ).MaxOutAir = thisController.MaxOAMassFlowRate;
 			}
 
 			// calculate mixed air temp at min OA flow rate
-			ReliefMassFlowAtMinOA = max( AirLoopFlow( AirLoopNum ).MinOutAir - OAController( OAControllerNum ).ExhMassFlow, 0.0 );
-			RecircMassFlowRateAtMinOAFlow = max( Node( OAController( OAControllerNum ).RetNode ).MassFlowRate - ReliefMassFlowAtMinOA, 0.0 );
+			ReliefMassFlowAtMinOA = max( AirLoopFlow( AirLoopNum ).MinOutAir - thisController.ExhMassFlow, 0.0 );
+			RecircMassFlowRateAtMinOAFlow = max( Node( thisController.RetNode ).MassFlowRate - ReliefMassFlowAtMinOA, 0.0 );
 			if ( ( RecircMassFlowRateAtMinOAFlow + AirLoopFlow( AirLoopNum ).MinOutAir ) > 0.0 ) {
-				RecircTemp = Node( OAController( OAControllerNum ).RetNode ).Temp;
-				MixedAirTempAtMinOAFlow = ( RecircMassFlowRateAtMinOAFlow * RecircTemp + AirLoopFlow( AirLoopNum ).MinOutAir * Node( OAController( OAControllerNum ).OANode ).Temp ) / ( RecircMassFlowRateAtMinOAFlow + AirLoopFlow( AirLoopNum ).MinOutAir );
+				RecircTemp = Node( thisController.RetNode ).Temp;
+				MixedAirTempAtMinOAFlow = ( RecircMassFlowRateAtMinOAFlow * RecircTemp + AirLoopFlow( AirLoopNum ).MinOutAir * Node( thisController.OANode ).Temp ) / ( RecircMassFlowRateAtMinOAFlow + AirLoopFlow( AirLoopNum ).MinOutAir );
 			} else {
-				MixedAirTempAtMinOAFlow = Node( OAController( OAControllerNum ).RetNode ).Temp;
+				MixedAirTempAtMinOAFlow = Node( thisController.RetNode ).Temp;
 			}
-			OAController( OAControllerNum ).MixedAirTempAtMinOAFlow = MixedAirTempAtMinOAFlow;
+			thisController.MixedAirTempAtMinOAFlow = MixedAirTempAtMinOAFlow;
 
 			// Check lockout with heating for any airloop - will lockout economizer even on airloops without a unitary system
 			if ( EconomizerOperationFlag ) {
-				if ( OAController( OAControllerNum ).Lockout == LockoutWithHeatingPossible ) {
+				if ( thisController.Lockout == LockoutWithHeatingPossible ) {
 					// For all system types (even ones that don't set AirLoopEconoLockout) lock out economizer if unfavorable for heating
 					if ( AirLoopControlInfo( AirLoopNum ).CheckHeatRecoveryBypassStatus && AirLoopControlInfo( AirLoopNum ).OASysComponentsSimulated ) {
 
-						if ( MixedAirTempAtMinOAFlow <= Node( OAController( OAControllerNum ).MixNode ).TempSetPoint ) {
+						if ( MixedAirTempAtMinOAFlow <= Node( thisController.MixNode ).TempSetPoint ) {
 							AirLoopControlInfo( AirLoopNum ).EconomizerFlowLocked = true;
-							OAController( OAControllerNum ).OAMassFlow = AirLoopFlow( AirLoopNum ).MinOutAir;
-							AirLoopFlow( AirLoopNum ).OAFrac = OAController( OAControllerNum ).OAMassFlow / OAController( OAControllerNum ).MixMassFlow;
+							thisController.OAMassFlow = AirLoopFlow( AirLoopNum ).MinOutAir;
+							AirLoopFlow( AirLoopNum ).OAFrac = thisController.OAMassFlow / thisController.MixMassFlow;
 							AirLoopControlInfo( AirLoopNum ).EconoLockout = true;
 							EconomizerOperationFlag = false ;
 						} else { // IF (MixedAirTempAtMinOAFlow .LE. Node(OAController(OAControllerNum)%MixNode)%TempSetPoint) THEN
 							AirLoopControlInfo( AirLoopNum ).EconomizerFlowLocked = false;
-							OAController( OAControllerNum ).HRHeatingCoilActive = 0;
+							thisController.HRHeatingCoilActive = 0;
 						} // IF (MixedAirTempAtMinOAFlow .LE. Node(OAController(OAControllerNum)%MixNode)%TempSetPoint) THEN
 						AirLoopControlInfo( AirLoopNum ).CheckHeatRecoveryBypassStatus = false;
 					}
@@ -4461,15 +4484,15 @@ namespace MixedAir {
 
 			// Check heat exchanger bypass control
 			AirLoopControlInfo( AirLoopNum ).HeatRecoveryBypass = false;
-			OAController( OAControllerNum ).HeatRecoveryBypassStatus = 0;
+			thisController.HeatRecoveryBypassStatus = 0;
 			if ( EconomizerOperationFlag ) {
-				if ( OAController( OAControllerNum ).HeatRecoveryBypassControlType == BypassWhenWithinEconomizerLimits ) {
+				if ( thisController.HeatRecoveryBypassControlType == BypassWhenWithinEconomizerLimits ) {
 					AirLoopControlInfo( AirLoopNum ).HeatRecoveryBypass = true;
-					OAController( OAControllerNum ).HeatRecoveryBypassStatus = 1;
-				} else if ( OAController( OAControllerNum ).HeatRecoveryBypassControlType == BypassWhenOAFlowGreaterThanMinimum ) {
-					if ( OAController( OAControllerNum ).OAMassFlow > AirLoopFlow( AirLoopNum ).MinOutAir ) {
+					thisController.HeatRecoveryBypassStatus = 1;
+				} else if ( thisController.HeatRecoveryBypassControlType == BypassWhenOAFlowGreaterThanMinimum ) {
+					if ( thisController.OAMassFlow > AirLoopFlow( AirLoopNum ).MinOutAir ) {
 						AirLoopControlInfo( AirLoopNum ).HeatRecoveryBypass = true;
-						OAController( OAControllerNum ).HeatRecoveryBypassStatus = 1;
+						thisController.HeatRecoveryBypassStatus = 1;
 					}
 				}
 			}
@@ -4478,8 +4501,8 @@ namespace MixedAir {
 			AirLoopControlInfo( AirLoopNum ).EconoActive = EconomizerOperationFlag;
 			AirLoopControlInfo( AirLoopNum ).HighHumCtrlActive = HighHumidityOperationFlag;
 			if ( AirLoopControlInfo( AirLoopNum ).EconomizerFlowLocked ) {
-				OAController( OAControllerNum ).OAMassFlow = AirLoopFlow( AirLoopNum ).MinOutAir;
-				AirLoopFlow( AirLoopNum ).OAFrac = OAController( OAControllerNum ).OAMassFlow / OAController( OAControllerNum ).MixMassFlow;
+				thisController.OAMassFlow = AirLoopFlow( AirLoopNum ).MinOutAir;
+				AirLoopFlow( AirLoopNum ).OAFrac = thisController.OAMassFlow / thisController.MixMassFlow;
 			}
 
 
@@ -4495,9 +4518,9 @@ namespace MixedAir {
 					// reset heating coil active status and HX since logic tests may turn off heating coil
 					// the ResimAirLoopFlag will force another iteration and things should line up on subsequent iterations
 					AirLoopControlInfo( AirLoopNum ).HeatingActiveFlag = false;
-					OAController( OAControllerNum ).HRHeatingCoilActive = 0;
+					thisController.HRHeatingCoilActive = 0;
 					AirLoopControlInfo( AirLoopNum ).HeatRecoveryBypass = true;
-					OAController( OAControllerNum ).HeatRecoveryBypassStatus = 1;
+					thisController.HeatRecoveryBypassStatus = 1;
 				} else if ( AirLoopControlInfo( AirLoopNum ).HeatRecoveryResimFlag2 ) {
 					AirLoopControlInfo( AirLoopNum ).ResimAirLoopFlag = true;
 					AirLoopControlInfo( AirLoopNum ).HeatRecoveryResimFlag2 = false;
@@ -4505,49 +4528,49 @@ namespace MixedAir {
 					AirLoopControlInfo( AirLoopNum ).ResimAirLoopFlag = false;
 				}
 			} else {
-				OAController( OAControllerNum ).HRHeatingCoilActive = 0;
+				thisController.HRHeatingCoilActive = 0;
 			}
 
 		} // if (AirLoopNum > 0)
 
 		// Set the relief air flow rate (must be done last to account for changes in OAMassFlow
-		OAController( OAControllerNum ).RelMassFlow = max( OAController( OAControllerNum ).OAMassFlow - OAController( OAControllerNum ).ExhMassFlow, 0.0 );
+		thisController.RelMassFlow = max( thisController.OAMassFlow - thisController.ExhMassFlow, 0.0 );
 
 		// Set economizer report variable and status flag
-		if ( OAController( OAControllerNum ).Econo == NoEconomizer ) {
+		if ( thisController.Econo == NoEconomizer ) {
 			// No economizer
-			OAController( OAControllerNum ).EconomizerStatus = 0;
-			OAControllerInfo( OAControllerNum ).EconoActive = false;
+			thisController.EconomizerStatus = 0;
+			thisControllerInfo.EconoActive = false;
 		} else {
 			// With economizer.
 			if ( EconomizerOperationFlag ) {
 				// Economizer is enabled
-				OAController( OAControllerNum ).EconomizerStatus = 1;
-				OAControllerInfo( OAControllerNum ).EconoActive = true;
+				thisController.EconomizerStatus = 1;
+				thisControllerInfo.EconoActive = true;
 			} else {
 				// Economizer is disabled
-				OAController( OAControllerNum ).EconomizerStatus = 0;
-				OAControllerInfo( OAControllerNum ).EconoActive = false;
+				thisController.EconomizerStatus = 0;
+				thisControllerInfo.EconoActive = false;
 			}
 		}
 
 		// Set high humidity control report variable and status flag
 		if ( HighHumidityOperationFlag ) {
-			OAController( OAControllerNum ).HighHumCtrlStatus = 1;
-			OAControllerInfo( OAControllerNum ).HighHumCtrlActive = true;
+			thisController.HighHumCtrlStatus = 1;
+			thisControllerInfo.HighHumCtrlActive = true;
 		} else {
-			OAController( OAControllerNum ).HighHumCtrlStatus = 0;
-			OAControllerInfo( OAControllerNum ).HighHumCtrlActive = false;
+			thisController.HighHumCtrlStatus = 0;
+			thisControllerInfo.HighHumCtrlActive = false;
 		}
 
 		// Save OA fraction for reporting
-		if ( OAController( OAControllerNum ).MixMassFlow > 0 ) {
-			OAController( OAControllerNum ).OAFractionRpt = OAController( OAControllerNum ).OAMassFlow / OAController( OAControllerNum ).MixMassFlow;
+		if ( thisController.MixMassFlow > 0 ) {
+			thisController.OAFractionRpt = thisController.OAMassFlow / thisController.MixMassFlow;
 		} else {
-			if ( OAController( OAControllerNum ).OAMassFlow > 0 ) {
-				OAController( OAControllerNum ).OAFractionRpt = OASignal;
+			if ( thisController.OAMassFlow > 0 ) {
+				thisController.OAFractionRpt = OASignal;
 			} else {
-				OAController( OAControllerNum ).OAFractionRpt = 0.0;
+				thisController.OAFractionRpt = 0.0;
 			}
 		}
 
@@ -4710,8 +4733,6 @@ namespace MixedAir {
 						OAController( OAControllerNum ).MaxOA = FinalSysSizing( CurSysNum ).DesMainVolFlow;
 					}}
 
-				} else if ( SELECT_CASE_var == ControllerSimple ) {
-
 				} else if ( SELECT_CASE_var == ControllerStandAloneERV ) {
 
 				} else {
@@ -4727,8 +4748,6 @@ namespace MixedAir {
 					CheckZoneSizing( CurrentModuleObject, OAController( OAControllerNum ).Name );
 					OAController( OAControllerNum ).MaxOA = max( FinalZoneSizing( CurZoneEqNum ).DesCoolVolFlow, FinalZoneSizing( CurZoneEqNum ).DesHeatVolFlow );
 
-				} else if ( SELECT_CASE_var == ControllerSimple ) {
-
 				} else if ( SELECT_CASE_var == ControllerStandAloneERV ) {
 
 				} else {
@@ -4860,8 +4879,8 @@ namespace MixedAir {
 			}
 			else
 			{
-			Node( OutAirNodeNum ).MassFlowRate = OAController( OAControllerNum ).OAMassFlow;
-			Node( InletAirNodeNum ).MassFlowRate = OAController( OAControllerNum ).OAMassFlow;
+				Node( OutAirNodeNum ).MassFlowRate = OAController( OAControllerNum ).OAMassFlow;
+				Node( InletAirNodeNum ).MassFlowRate = OAController( OAControllerNum ).OAMassFlow;
 				Node( OutAirNodeNum ).MassFlowRateMaxAvail = OAController( OAControllerNum ).OAMassFlow;
 			}
 			Node( RelAirNodeNum ).MassFlowRate = OAController( OAControllerNum ).RelMassFlow;
@@ -4877,31 +4896,13 @@ namespace MixedAir {
 			}
 			else
 			{
-			Node( OutAirNodeNum ).MassFlowRate = OAController( OAControllerNum ).OAMassFlow;
-			Node( OutAirNodeNum ).MassFlowRateMaxAvail = OAController( OAControllerNum ).OAMassFlow;
+				Node( OutAirNodeNum ).MassFlowRate = OAController( OAControllerNum ).OAMassFlow;
+				Node( OutAirNodeNum ).MassFlowRateMaxAvail = OAController( OAControllerNum ).OAMassFlow;
 			}
 			Node( RetAirNodeNum ).MassFlowRate = Node( OAController( OAControllerNum ).RetNode ).MassFlowRate;
 			Node( RetAirNodeNum ).MassFlowRateMaxAvail = Node( OAController( OAControllerNum ).RetNode ).MassFlowRate;
 		}
 
-		if ( Contaminant.CO2Simulation && OAController( OAControllerNum ).ControllerType_Num == ControllerSimple ) {
-			Node( RelAirNodeNum ).CO2 = Node( InletAirNodeNum ).CO2;
-			if ( Node( RetAirNodeNum ).MassFlowRate > 0.0 ) {
-				Node( RetAirNodeNum ).CO2 = ( ( Node( InletAirNodeNum ).MassFlowRate - Node( RelAirNodeNum ).MassFlowRate ) * Node( InletAirNodeNum ).CO2 + Node( OutAirNodeNum ).MassFlowRate * OutdoorCO2 ) / Node( RetAirNodeNum ).MassFlowRate;
-			} else {
-				Node( RetAirNodeNum ).CO2 = Node( InletAirNodeNum ).CO2;
-			}
-		}
-
-		if ( Contaminant.GenericContamSimulation && OAController( OAControllerNum ).ControllerType_Num == ControllerSimple ) {
-			Node( RelAirNodeNum ).GenContam = Node( InletAirNodeNum ).GenContam;
-			if ( Node( RetAirNodeNum ).MassFlowRate > 0.0 ) {
-				Node( RetAirNodeNum ).GenContam = ( ( Node( InletAirNodeNum ).MassFlowRate - Node( RelAirNodeNum ).MassFlowRate ) * Node( InletAirNodeNum ).GenContam + Node( OutAirNodeNum ).MassFlowRate * OutdoorGC ) / Node( RetAirNodeNum ).MassFlowRate;
-			} else {
-				Node( RetAirNodeNum ).GenContam = Node( InletAirNodeNum ).GenContam;
-			}
-		}
-
 	}
 
 	void
@@ -5235,10 +5236,9 @@ namespace MixedAir {
 		// FUNCTION LOCAL VARIABLE DECLARATIONS:
 		// na
 
-		if ( GetOAControllerInputFlag ) {
-			// Make sure OAControllers are "gotten"
-			GetOAControllerInputs();
-			GetOAControllerInputFlag = false;
+		if ( AllocateOAControllersFlag ) {
+			// Make sure OAControllers are allocated
+			AllocateOAControllers();
 		}
 
 		NumberOfOAControllers = NumOAControllers;
@@ -5473,7 +5473,7 @@ namespace MixedAir {
 	}
 
 	int
-	GetOASysNumHXs( int const OASysNumber ) 
+	GetOASysNumHXs( int const OASysNumber )
 	{
 
 		// FUNCTION INFORMATION:
@@ -6168,10 +6168,9 @@ namespace MixedAir {
 		// SUBROUTINE LOCAL VARIABLE DECLARATIONS:
 		// na
 
-		if ( GetOAControllerInputFlag ) {
-			// Make sure OAControllers are "gotten"
-			GetOAControllerInputs();
-			GetOAControllerInputFlag = false;
+		if ( AllocateOAControllersFlag ) {
+			// Make sure OAControllers are allocated
+			AllocateOAControllers();
 		}
 
 		if ( OACtrlNum <= 0 || OACtrlNum > NumOAControllers ) {
@@ -6326,6 +6325,7 @@ namespace MixedAir {
 		// PURPOSE OF THIS SUBROUTINE:
 		// When OA Controller data is gotten from other routines, must check to make sure
 		// new name doesn't duplicate.  (Essentially a pass through to call Verify Name)
+		// Currently, this is only called from HVACStandAlongERV::GetStandaloneERV()
 
 		// METHODOLOGY EMPLOYED:
 		// na
@@ -6351,10 +6351,9 @@ namespace MixedAir {
 		// SUBROUTINE LOCAL VARIABLE DECLARATIONS:
 		// na
 
-		if ( GetOAControllerInputFlag ) {
-			// Make sure OAControllers are "gotten"
-			GetOAControllerInputs();
-			GetOAControllerInputFlag = false;
+		if ( AllocateOAControllersFlag ) {
+			// Make sure OAControllers are allocated
+			AllocateOAControllers();
 		}
 
 		VerifyName( OAControllerName, OAController, NumCurrentOAControllers, IsNotOK, IsBlank, SourceID );
diff --git a/src/EnergyPlus/MixedAir.hh b/src/EnergyPlus/MixedAir.hh
index 704dc3b4b0d..a80595d3e30 100644
--- a/src/EnergyPlus/MixedAir.hh
+++ b/src/EnergyPlus/MixedAir.hh
@@ -117,7 +117,6 @@ namespace MixedAir {
 	extern int const UnitarySystem;
 	extern int const Humidifier;
 
-	extern int const ControllerSimple;
 	extern int const ControllerOutsideAir;
 	extern int const ControllerStandAloneERV;
 
@@ -551,6 +550,9 @@ namespace MixedAir {
 	void
 	GetOAControllerInputs();
 
+	void
+	AllocateOAControllers();
+
 	void
 	GetOAMixerInputs();
 
diff --git a/src/EnergyPlus/OutputReportPredefined.cc b/src/EnergyPlus/OutputReportPredefined.cc
index 0eb27bf40ff..bf4857b8326 100644
--- a/src/EnergyPlus/OutputReportPredefined.cc
+++ b/src/EnergyPlus/OutputReportPredefined.cc
@@ -2242,6 +2242,22 @@ namespace OutputReportPredefined {
 		tableEntry( numTableEntry ).indexColumn = columnIndex;
 	}
 
+	std::string
+	RetrievePreDefTableEntry(
+		int const columnIndex,
+		std::string const & objName
+		)
+	{
+		for ( int iTableEntry = 1; iTableEntry <= numTableEntry; ++iTableEntry ) {
+			if ( tableEntry( iTableEntry ).indexColumn == columnIndex && tableEntry( iTableEntry ).objectName == objName ){
+				return trimmed( left_justified(tableEntry( iTableEntry ).charEntry) );
+				break;
+			}
+		}
+		return "NOT FOUND";
+	}
+
+
 	void
 	incrementTableEntry()
 	{
diff --git a/src/EnergyPlus/OutputReportPredefined.hh b/src/EnergyPlus/OutputReportPredefined.hh
index 183343357a4..f1be0b8e006 100644
--- a/src/EnergyPlus/OutputReportPredefined.hh
+++ b/src/EnergyPlus/OutputReportPredefined.hh
@@ -853,6 +853,13 @@ namespace OutputReportPredefined {
 		int const tableEntryInt
 	);
 
+	std::string
+		RetrievePreDefTableEntry(
+		int const columnIndex,
+		std::string const & objName
+	);
+
+
 	void
 	incrementTableEntry();
 
diff --git a/src/EnergyPlus/OutputReports.cc b/src/EnergyPlus/OutputReports.cc
index ae778c30eb9..5f72863e0e8 100644
--- a/src/EnergyPlus/OutputReports.cc
+++ b/src/EnergyPlus/OutputReports.cc
@@ -770,7 +770,7 @@ DXFOut(
 					}
 					gio::write( unit, Format_717 ) << TempZoneName;
 				} else {
-					if ( Surface( surf ).Shape == RectangularOverhang ) {
+					if ( Surface( surf ).Shape == SurfaceShape::RectangularOverhang ) {
 						ntri = Triangulate( Surface( surf ).Sides, Surface( surf ).Vertex, mytriangles, Surface( surf ).Azimuth, Surface( surf ).Tilt, Surface( surf ).Name, SurfaceClass_Overhang );
 					} else {
 						ntri = Triangulate( Surface( surf ).Sides, Surface( surf ).Vertex, mytriangles, Surface( surf ).Azimuth, Surface( surf ).Tilt, Surface( surf ).Name, SurfaceClass_Fin );
diff --git a/src/EnergyPlus/PlantCondLoopOperation.cc b/src/EnergyPlus/PlantCondLoopOperation.cc
index e11b0f8d90d..aa26787fa83 100644
--- a/src/EnergyPlus/PlantCondLoopOperation.cc
+++ b/src/EnergyPlus/PlantCondLoopOperation.cc
@@ -2025,7 +2025,8 @@ namespace PlantCondLoopOperation {
 					if ( this_op_scheme.OpSchemeType == EMSOpSchemeType ) {
 						if ( BeginEnvrnFlag && this_op_scheme.MyEnvrnFlag ) {
 							if ( this_op_scheme.ErlInitProgramMngr > 0 ) {
-								ManageEMS( emsCallFromUserDefinedComponentModel, this_op_scheme.ErlInitProgramMngr );
+								bool anyEMSRan;
+								ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, this_op_scheme.ErlInitProgramMngr );
 							}
 							this_op_scheme.MyEnvrnFlag = false;
 						}
@@ -3016,7 +3017,8 @@ namespace PlantCondLoopOperation {
 
 		// Call EMS program(s)
 		if ( PlantLoop( LoopNum ).OpScheme( CurSchemePtr ).ErlSimProgramMngr > 0 ) {
-			ManageEMS( emsCallFromUserDefinedComponentModel, PlantLoop( LoopNum ).OpScheme( CurSchemePtr ).ErlSimProgramMngr );
+			bool anyEMSRan;
+			ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, PlantLoop( LoopNum ).OpScheme( CurSchemePtr ).ErlSimProgramMngr );
 		}
 
 		// move actuated value to MyLoad
diff --git a/src/EnergyPlus/PlantPipingSystemsManager.cc b/src/EnergyPlus/PlantPipingSystemsManager.cc
index c9d124055e0..69405789d92 100644
--- a/src/EnergyPlus/PlantPipingSystemsManager.cc
+++ b/src/EnergyPlus/PlantPipingSystemsManager.cc
@@ -304,7 +304,7 @@ namespace PlantPipingSystemsManager {
 
 		// Read input if necessary
 		if ( GetInputFlag ) {
-			GetPipingSystemsInput();
+			GetPipingSystemsAndGroundDomainsInput();
 			GetInputFlag = false;
 		}
 
@@ -401,7 +401,7 @@ namespace PlantPipingSystemsManager {
 
 		// Read input if necessary
 		if ( GetInputFlag ) {
-			GetPipingSystemsInput();
+			GetPipingSystemsAndGroundDomainsInput();
 			GetInputFlag = false;
 		}
 
@@ -442,7 +442,7 @@ namespace PlantPipingSystemsManager {
 
 			// Aggregate the heat flux
 			// Zone-coupled slab
-			if ( PipingSystemDomains( DomainNum ).IsZoneCoupledSlab ) {
+			if ( PipingSystemDomains( DomainNum ).HasZoneCoupledSlab ) {
 				PipingSystemDomains( DomainNum ).AggregateHeatFlux += GetZoneInterfaceHeatFlux( DomainNum );
 				PipingSystemDomains( DomainNum ).NumHeatFlux += 1;
 				PipingSystemDomains( DomainNum ).HeatFlux = PipingSystemDomains( DomainNum ).AggregateHeatFlux / PipingSystemDomains( DomainNum ).NumHeatFlux;
@@ -495,7 +495,7 @@ namespace PlantPipingSystemsManager {
 	//*********************************************************************************************!
 
 	void
-	GetPipingSystemsInput()
+	GetPipingSystemsAndGroundDomainsInput()
 	{
 
 		// SUBROUTINE INFORMATION:
@@ -524,7 +524,7 @@ namespace PlantPipingSystemsManager {
 		// na
 
 		// SUBROUTINE PARAMETER DEFINITIONS:
-		static std::string const RoutineName( "GetPipingSystemsInput" );
+		static std::string const RoutineName( "GetPipingSystemsAndGroundDomainsInput" );
 
 		// INTERFACE BLOCK SPECIFICATIONS:
 		// na
@@ -926,7 +926,7 @@ namespace PlantPipingSystemsManager {
 					IssueSevereInputFieldError( RoutineName, ObjName_ug_GeneralDomain, cAlphaArgs( 1 ), cAlphaFieldNames( CurIndex ), cAlphaArgs( CurIndex ), "Must enter either yes or no.", ErrorsFound );
 				}
 
-				// get boundary condition model names and indeces --error check
+				// get boundary condition model names and indices --error check
 				CurIndex = 9;
 				PipingSystemDomains( DomainNum ).BasementZone.WallBoundaryOSCMName = cAlphaArgs( CurIndex );
 				PipingSystemDomains( DomainNum ).BasementZone.WallBoundaryOSCMIndex = FindItemInList( PipingSystemDomains( DomainNum ).BasementZone.WallBoundaryOSCMName, OSCM );
@@ -998,7 +998,7 @@ namespace PlantPipingSystemsManager {
 			// SUBROUTINE INFORMATION:
 			//       AUTHOR         Edwin Lee
 			//       DATE WRITTEN   Summer 2011
-			//       MODIFIED       Spring 2014 by Matt Mitchell and Sushobhit Acharya to accomodate ground coupled calculations
+			//       MODIFIED       Spring 2014 by Matt Mitchell and Sushobhit Acharya to accommodate ground coupled calculations
 			//       RE-ENGINEERED  na
 
 			// PURPOSE OF THIS SUBROUTINE:
@@ -1088,7 +1088,7 @@ namespace PlantPipingSystemsManager {
 			// initialize these counters properly so they can be incremented within the DO loop
 			DomainCtr = StartingDomainNumForZone - 1;
 
-			// For each domain, we need to process the inputs into a local array of derived type, then resolve each one, creating definitions for a zonecoupled domain.
+			// For each domain, we need to process the inputs into a local array of derived type, then resolve each one, creating definitions for a zone coupled domain.
 			// This way, the outer get input routines can handle it as though they were generalized routines
 
 			for ( ZoneCoupledDomainCtr = 1; ZoneCoupledDomainCtr <= NumZoneCoupledDomains; ++ZoneCoupledDomainCtr ) {
@@ -1133,8 +1133,9 @@ namespace PlantPipingSystemsManager {
 				} else if ( SameString( cAlphaArgs( 5 ), "ONGRADE" ) ) {
 					PipingSystemDomains( DomainCtr ).SlabInGradeFlag = false;
 				} else {
-					ShowContinueError( "Slab location not determined." );
-					ShowContinueError( "Preceding error causes program termination." );
+					ShowSevereError( "Invalid " + cAlphaFieldNames( 5 ) + "=" + cAlphaArgs( 5 ) );
+					ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
+					ErrorsFound = true;
 				}
 
 				// Get slab material properties
@@ -1143,10 +1144,9 @@ namespace PlantPipingSystemsManager {
 					PipingSystemDomains( DomainCtr ).SlabMaterialNum = FindItemInList( cAlphaArgs( 6 ), Material, TotMaterials );
 					if ( PipingSystemDomains( DomainCtr ).SlabMaterialNum == 0 ) {
 						ShowSevereError( "Invalid " + cAlphaFieldNames( 6 ) + "=" + cAlphaArgs( 6 ) );
-						ShowContinueError( "Found in " + PipingSystemDomains( DomainCtr ).Name );
+						ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
 						ErrorsFound = true;
 					} else {
-						// check this
 						PipingSystemDomains( DomainCtr ).SlabThickness = Material( PipingSystemDomains( DomainCtr ).SlabMaterialNum ).Thickness;
 						PipingSystemDomains( DomainCtr ).SlabProperties.Density = Material( PipingSystemDomains( DomainCtr ).SlabMaterialNum ).Density;
 						PipingSystemDomains( DomainCtr ).SlabProperties.SpecificHeat = Material( PipingSystemDomains( DomainCtr ).SlabMaterialNum ).SpecHeat;
@@ -1161,8 +1161,9 @@ namespace PlantPipingSystemsManager {
 					} else if ( SameString( cAlphaArgs( 7 ), "YES" ) ) {
 						PipingSystemDomains( DomainCtr ).HorizInsPresentFlag = true;
 					} else {
-						ShowContinueError( "Must enter either yes or no for horizontal insulation." );
-						ShowFatalError( "Preceding error causes program termination." );
+						ShowSevereError( "Invalid " + cAlphaFieldNames( 7 ) + "=" + cAlphaArgs( 7 ) );
+						ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
+						ErrorsFound = true;
 					}
 				}
 
@@ -1172,7 +1173,7 @@ namespace PlantPipingSystemsManager {
 					PipingSystemDomains( DomainCtr ).HorizInsMaterialNum = FindItemInList( cAlphaArgs( 8 ), Material, TotMaterials );
 					if ( PipingSystemDomains( DomainCtr ).HorizInsMaterialNum == 0 ) {
 						ShowSevereError( "Invalid " + cAlphaFieldNames( 8 ) + "=" + cAlphaArgs( 8 ) );
-						ShowContinueError( "Found in " + Domain( ZoneCoupledDomainCtr ).HorizInsMaterial );
+						ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
 						ErrorsFound = true;
 					} else {
 						PipingSystemDomains( DomainCtr ).HorizInsThickness = Material( PipingSystemDomains( DomainCtr ).HorizInsMaterialNum ).Thickness;
@@ -1184,15 +1185,21 @@ namespace PlantPipingSystemsManager {
 					// Set flag for horizontal insulation extents
 					if ( SameString( cAlphaArgs( 9 ), "PERIMETER" ) ) {
 						PipingSystemDomains( DomainCtr ).FullHorizInsPresent = false;
+						// Horizontal insulation perimeter width
+						if ( Domain( ZoneCoupledDomainCtr ).HorizInsWidth > 0.0 ) {
+							PipingSystemDomains( DomainCtr ).HorizInsWidth = Domain( ZoneCoupledDomainCtr ).HorizInsWidth;
+						} else {
+							ShowSevereError( "Invalid " + cNumericFieldNames( 10 ) );
+							ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
+							ErrorsFound = true;
+						}
 					} else if ( SameString( cAlphaArgs( 9 ), "FULL" ) ) {
 						PipingSystemDomains( DomainCtr ).FullHorizInsPresent = true;
 					} else {
-						ShowContinueError( "Must enter either PERIMETER or FULL for horizontal insulation extents." );
-						ShowFatalError( "Preceding error causes program termination." );
+						ShowSevereError( "Invalid " + cAlphaFieldNames( 9 ) + "=" + cAlphaArgs( 9 ) );
+						ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
+						ErrorsFound = true;
 					}
-
-					// Horizontal insualtion perimeter width
-					PipingSystemDomains( DomainCtr ).HorizInsWidth = Domain( ZoneCoupledDomainCtr ).HorizInsWidth;
 				}
 
 				// set flag for vertical insulation
@@ -1201,8 +1208,9 @@ namespace PlantPipingSystemsManager {
 				} else if ( SameString( cAlphaArgs( 10 ), "YES" ) ) {
 					PipingSystemDomains( DomainCtr ).VertInsPresentFlag = true;
 				} else {
-					ShowContinueError( "Must enter either yes or no for vertical insulation." );
-					ShowFatalError( "Preceding error causes program termination." );
+					ShowSevereError( "Invalid " + cAlphaFieldNames( 10 ) + "=" + cAlphaArgs( 10 ) );
+					ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
+					ErrorsFound = true;
 				}
 
 				// Get vertical insulation material properties
@@ -1211,7 +1219,7 @@ namespace PlantPipingSystemsManager {
 					PipingSystemDomains( DomainCtr ).VertInsMaterialNum = FindItemInList( cAlphaArgs( 11 ), Material, TotMaterials );
 					if ( PipingSystemDomains( DomainCtr ).VertInsMaterialNum == 0 ) {
 						ShowSevereError( "Invalid " + cAlphaFieldNames( 11 ) + "=" + cAlphaArgs( 11 ) );
-						ShowContinueError( "Found in " + Domain( ZoneCoupledDomainCtr ).VertInsMaterial );
+						ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
 						ErrorsFound = true;
 					} else {
 						PipingSystemDomains( DomainCtr ).VertInsThickness = Material( PipingSystemDomains( DomainCtr ).VertInsMaterialNum ).Thickness;
@@ -1221,13 +1229,13 @@ namespace PlantPipingSystemsManager {
 					}
 
 					// vertical insulation depth
-					if ( Domain( ZoneCoupledDomainCtr ).VertInsDepth < Domain( ZoneCoupledDomainCtr ).Depth ) {
-						PipingSystemDomains( DomainCtr ).VertInsDepth = Domain( ZoneCoupledDomainCtr ).VertInsDepth;
+					if ( Domain( ZoneCoupledDomainCtr ).VertInsDepth > Domain( ZoneCoupledDomainCtr ).Depth || Domain( ZoneCoupledDomainCtr ).VertInsDepth <= 0.0 ) {
+						ShowSevereError( "Invalid " + cNumericFieldNames( 11 ) );
+						ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
+						ErrorsFound = true;
 					} else {
-						ShowContinueError( "Vertical insulation depth must be less than the domain depth. Check input." );
-						ShowFatalError( "Preceding error causes program termination." );
+						PipingSystemDomains( DomainCtr ).VertInsDepth = Domain( ZoneCoupledDomainCtr ).VertInsDepth;
 					}
-
 				}
 
 				// Domain perimeter offset
@@ -1239,15 +1247,16 @@ namespace PlantPipingSystemsManager {
 				} else if ( SameString( cAlphaArgs( 12 ), "HOURLY" ) ) {
 					PipingSystemDomains( DomainCtr ).SimHourlyFlag = true;
 				} else {
-					ShowContinueError( "Could not determine slab simulation interval. Check input." );
-					ShowFatalError( "Preceding error causes program termination." );
+					ShowSevereError( "Invalid " + cAlphaFieldNames( 12 ) + "=" + cAlphaArgs( 12 ) );
+					ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
+					ErrorsFound = true;
 				}
 
 
 				//******* We'll first set up the domain ********
 				PipingSystemDomains( DomainCtr ).IsActuallyPartOfAHorizontalTrench = false;
 				PipingSystemDomains( DomainCtr ).HasAPipeCircuit = false;
-				PipingSystemDomains( DomainCtr ).IsZoneCoupledSlab = true;
+				PipingSystemDomains( DomainCtr ).HasZoneCoupledSlab = true;
 
 				// Domain name
 				PipingSystemDomains( DomainCtr ).Name = Domain( ZoneCoupledDomainCtr ).ObjName;
@@ -1255,11 +1264,13 @@ namespace PlantPipingSystemsManager {
 				// get boundary condition model names and indices -- error check
 				PipingSystemDomains( DomainCtr ).ZoneCoupledOSCMIndex = FindItemInList( Domain( ZoneCoupledDomainCtr ).OSCMName, OSCM );
 				if ( PipingSystemDomains( DomainCtr ).ZoneCoupledOSCMIndex <= 0 ) {
-					IssueSevereInputFieldError( RoutineName, ObjName_ZoneCoupled_Slab, cAlphaArgs( 1 ), cAlphaFieldNames( 2 ), cAlphaArgs( 2 ), "Could not match with an Other Side Conditions Model input object.", ErrorsFound );
+					IssueSevereInputFieldError( RoutineName, ObjName_ZoneCoupled_Slab, cAlphaArgs( 1 ), cAlphaFieldNames( 4 ), cAlphaArgs( 4 ), "Could not match with an Other Side Conditions Model input object.", ErrorsFound );
+					ErrorsFound = true;
 				} else {
 					NumSurfacesWithThisOSCM = GetSurfaceCountForOSCM( PipingSystemDomains( DomainCtr ).ZoneCoupledOSCMIndex );
 					if ( NumSurfacesWithThisOSCM <= 0 ) {
-						IssueSevereInputFieldError( RoutineName, ObjName_ZoneCoupled_Slab, cAlphaArgs( 1 ), cAlphaFieldNames( 2 ), cAlphaArgs( 2 ), "Entry matched an Other Side Conditions Model, but no surfaces were found to be using this Other Side Conditions Model.", ErrorsFound );
+						IssueSevereInputFieldError( RoutineName, ObjName_ZoneCoupled_Slab, cAlphaArgs( 1 ), cAlphaFieldNames( 4 ), cAlphaArgs( 4 ), "Entry matched an Other Side Conditions Model, but no surfaces were found to be using this Other Side Conditions Model.", ErrorsFound );
+						ErrorsFound = true;
 					} else {
 						PipingSystemDomains( DomainCtr ).ZoneCoupledSurfaces.allocate( NumSurfacesWithThisOSCM );
 						// Create GetSurfaceDataForOSCM function
@@ -1279,9 +1290,15 @@ namespace PlantPipingSystemsManager {
 				PipingSystemDomains( DomainCtr ).SlabLength = PipingSystemDomains( DomainCtr ).SlabWidth * Domain( ZoneCoupledDomainCtr ).AspectRatio;
 
 				// Check horizontal insulation width so as to prevent overlapping insulation. VertInsThickness is used here since it is used for vertical partition thickness.
-				if ( 2 * PipingSystemDomains( DomainCtr ).HorizInsWidth + PipingSystemDomains( DomainCtr ).VertInsThickness > PipingSystemDomains( DomainCtr ).SlabWidth || 2 * PipingSystemDomains( DomainCtr ).HorizInsWidth + PipingSystemDomains( DomainCtr ).VertInsThickness > PipingSystemDomains( DomainCtr ).SlabLength ) {
-					ShowSevereError( "PipingSystems:" + RoutineName + ": Perimeter Insulation Width is too high" );
-					ShowFatalError( "Preceding error(s) cause program termination." );
+				if ( !PipingSystemDomains( DomainCtr ).FullHorizInsPresent && ThisArea > 0.0 ) {
+					if ( 2 * ( PipingSystemDomains( DomainCtr ).HorizInsWidth + PipingSystemDomains( DomainCtr ).VertInsThickness ) > PipingSystemDomains( DomainCtr ).SlabWidth ||
+						2 * ( PipingSystemDomains( DomainCtr ).HorizInsWidth + PipingSystemDomains( DomainCtr ).VertInsThickness ) > PipingSystemDomains( DomainCtr ).SlabLength ) {
+						ShowContinueError( RoutineName + ": Perimeter insulation width is too large." );
+						ShowContinueError( "This would cause overlapping insulation. Check inputs." );
+						ShowContinueError( "Defaulting to full horizontal insulation." );
+						ShowContinueError( "Found in: " + Domain( ZoneCoupledDomainCtr ).ObjName );
+						PipingSystemDomains( DomainCtr ).FullHorizInsPresent = true;
+					}
 				}
 
 				// Set ground domain dimensions
@@ -1339,7 +1356,7 @@ namespace PlantPipingSystemsManager {
 		// SUBROUTINE INFORMATION:
 		//       AUTHOR         Edwin Lee
 		//       DATE WRITTEN   Summer 2011
-		//       MODIFIED       Summer 2014  Sushobhit Acharya to accomodate basement calculations
+		//       MODIFIED       Summer 2014  Sushobhit Acharya to accommodate basement calculations
 		//       RE-ENGINEERED  na
 
 		// PURPOSE OF THIS SUBROUTINE:
@@ -1415,7 +1432,7 @@ namespace PlantPipingSystemsManager {
 		// initialize these counters properly so they can be incremented within the DO loop
 		DomainNum = StartingDomainNumForBasement - 1;
 
-		// For each domain, we need to process the inputs into a local array of derived type, then resolve each one, creating definitions for a zonecoupled domain.
+		// For each domain, we need to process the inputs into a local array of derived type, then resolve each one, creating definitions for a zone coupled domain.
 		// This way, the outer get input routines can handle it as though they were generalized routines
 
 		for ( BasementCtr = 1; BasementCtr <= NumBasements; ++BasementCtr ) {
@@ -1447,6 +1464,9 @@ namespace PlantPipingSystemsManager {
 			Domain( BasementCtr ).HorizInsWidth = rNumericArgs( 10 );
 			Domain( BasementCtr ).VertInsDepth = rNumericArgs( 12 );
 
+			// Other inputs
+			PipingSystemDomains( DomainNum ).Name = cAlphaArgs( 1 );
+
 			// Soil properties, validated min/max by IP
 			PipingSystemDomains( DomainNum ).GroundProperties.Conductivity = rNumericArgs( 4 );
 			PipingSystemDomains( DomainNum ).GroundProperties.Density = rNumericArgs( 5 );
@@ -1466,11 +1486,13 @@ namespace PlantPipingSystemsManager {
 			// Basement zone depth
 			CurIndex = 11;
 			PipingSystemDomains( DomainNum ).BasementZone.Depth = rNumericArgs( CurIndex );
-			if ( PipingSystemDomains( DomainNum ).BasementZone.Depth <= 0.0 ) {
-				IssueSevereInputFieldError( RoutineName, ObjName_ZoneCoupled_Basement, cAlphaArgs( 1 ), cNumericFieldNames( CurIndex ), rNumericArgs( CurIndex ), "Basement depth must be a positive nonzero value.", ErrorsFound );
+			if ( PipingSystemDomains( DomainNum ).BasementZone.Depth >= Domain( BasementCtr ).Depth || PipingSystemDomains( DomainNum ).BasementZone.Depth <= 0.0 ) {
+				ShowSevereError( "Invalid " + cNumericFieldNames( CurIndex ) );
+				ShowContinueError( "Found in: " + PipingSystemDomains( DomainNum ).Name );
+				ErrorsFound = true;
 			}
 
-			// get boundary condition model names and indeces --error check
+			// get boundary condition model names and indices --error check
 			CurIndex = 4;
 			PipingSystemDomains( DomainNum ).BasementZone.FloorBoundaryOSCMName = cAlphaArgs( CurIndex );
 			PipingSystemDomains( DomainNum ).BasementZone.FloorBoundaryOSCMIndex = FindItemInList( PipingSystemDomains( DomainNum ).BasementZone.FloorBoundaryOSCMName, OSCM );
@@ -1494,10 +1516,12 @@ namespace PlantPipingSystemsManager {
 			PipingSystemDomains( DomainNum ).BasementZone.WallBoundaryOSCMIndex = FindItemInList( PipingSystemDomains( DomainNum ).BasementZone.WallBoundaryOSCMName, OSCM );
 			if ( PipingSystemDomains( DomainNum ).BasementZone.WallBoundaryOSCMIndex <= 0 ) {
 				IssueSevereInputFieldError( RoutineName, ObjName_ZoneCoupled_Basement, cAlphaArgs( 1 ), cAlphaFieldNames( CurIndex ), cAlphaArgs( CurIndex ), "Could not match with an Other Side Conditions Model input object.", ErrorsFound );
+				ErrorsFound = true;
 			} else {
 				NumSurfacesWithThisOSCM = GetSurfaceCountForOSCM( PipingSystemDomains( DomainNum ).BasementZone.WallBoundaryOSCMIndex );
 				if ( NumSurfacesWithThisOSCM <= 0 ) {
 					IssueSevereInputFieldError( RoutineName, ObjName_ZoneCoupled_Basement, cAlphaArgs( 1 ), cAlphaFieldNames( CurIndex ), cAlphaArgs( CurIndex ), "Entry matched an Other Side Conditions Model, but no surfaces were found to be using this Other Side Conditions Model.", ErrorsFound );
+					ErrorsFound = true;
 				} else {
 					PipingSystemDomains( DomainNum ).BasementZone.WallSurfacePointers.allocate( NumSurfacesWithThisOSCM );
 					PipingSystemDomains( DomainNum ).BasementZone.WallSurfacePointers = GetSurfaceIndecesForOSCM( PipingSystemDomains( DomainNum ).BasementZone.WallBoundaryOSCMIndex, NumSurfacesWithThisOSCM );
@@ -1539,8 +1563,9 @@ namespace PlantPipingSystemsManager {
 			} else if ( SameString( cAlphaArgs( 5 ), "YES" ) ) {
 				PipingSystemDomains( DomainNum ).HorizInsPresentFlag = true;
 			} else {
-				ShowContinueError( "Must enter either yes or no for horizontal insulation." );
-				ShowFatalError( "Preceding error causes program termination." );
+				ShowSevereError( "Invalid " + cAlphaFieldNames( 5 ) + "=" + cAlphaArgs( 5 ) );
+				ShowContinueError( "Found in: " + PipingSystemDomains( DomainNum ).Name );
+				ErrorsFound = true;
 			}
 
 			// Get horizontal insulation material properties
@@ -1549,7 +1574,7 @@ namespace PlantPipingSystemsManager {
 				PipingSystemDomains( DomainNum ).HorizInsMaterialNum = FindItemInList( cAlphaArgs( 6 ), Material, TotMaterials );
 				if ( PipingSystemDomains( DomainNum ).HorizInsMaterialNum == 0 ) {
 					ShowSevereError( "Invalid " + cAlphaFieldNames( 6 ) + "=" + cAlphaArgs( 6 ) );
-					ShowContinueError( "Found in " + Domain( BasementCtr ).HorizInsMaterial );
+					ShowContinueError( "Found in: " + PipingSystemDomains( DomainNum ).Name );
 					ErrorsFound = true;
 				} else {
 					PipingSystemDomains( DomainNum ).HorizInsThickness = Material( PipingSystemDomains( DomainNum ).HorizInsMaterialNum ).Thickness;
@@ -1561,15 +1586,21 @@ namespace PlantPipingSystemsManager {
 				// Set flag for horizontal insulation extents
 				if ( SameString( cAlphaArgs( 7 ), "PERIMETER" ) ) {
 					PipingSystemDomains( DomainNum ).FullHorizInsPresent = false;
+					// Horizontal insulation perimeter width
+					if ( Domain( BasementCtr ).HorizInsWidth > 0.0 ) {
+						PipingSystemDomains( DomainNum ).HorizInsWidth = Domain( BasementCtr ).HorizInsWidth;
+					} else {
+						ShowSevereError( "Invalid " + cNumericFieldNames( 10 ) );
+						ShowContinueError( "Found in: " + PipingSystemDomains( DomainNum ).Name );
+						ErrorsFound = true;
+					}
 				} else if ( SameString( cAlphaArgs( 7 ), "FULL" ) ) {
 					PipingSystemDomains( DomainNum ).FullHorizInsPresent = true;
 				} else {
-					ShowContinueError( "Must enter either PERIMETER or FULL for horizontal insulation extents." );
-					ShowFatalError( "Preceding error causes program termination." );
+					ShowSevereError( "Invalid " + cAlphaFieldNames( 7 ) + "=" + cAlphaArgs( 7 ) );
+					ShowContinueError( "Found in: " + PipingSystemDomains( DomainNum ).Name );
+					ErrorsFound = true;
 				}
-
-				// Horizontal insualtion perimeter width
-				PipingSystemDomains( DomainNum ).HorizInsWidth = Domain( BasementCtr ).HorizInsWidth;
 			}
 
 			// set flag for vertical insulation
@@ -1578,17 +1609,28 @@ namespace PlantPipingSystemsManager {
 			} else if ( SameString( cAlphaArgs( 9 ), "YES" ) ) {
 				PipingSystemDomains( DomainNum ).VertInsPresentFlag = true;
 			} else {
-				ShowContinueError( "Must enter either yes or no for vertical insulation." );
-				ShowFatalError( "Preceding error causes program termination." );
+				ShowSevereError( "Invalid " + cAlphaFieldNames( 9 ) + "=" + cAlphaArgs( 9 ) );
+				ShowContinueError( "Found in: " + PipingSystemDomains( DomainNum ).Name );
+				ErrorsFound = true;
 			}
 
 			// Get vertical insulation material properties
 			if ( PipingSystemDomains( DomainNum ).VertInsPresentFlag ) {
+				// Check if vertical insulation is in domain
+				if ( Domain( BasementCtr ).VertInsDepth >= Domain( BasementCtr ).Depth || Domain( BasementCtr ).VertInsDepth <= 0.0 ) {
+					ShowSevereError( "Invalid " + cNumericFieldNames( 12 ) );
+					ShowContinueError( "Found in: " + PipingSystemDomains( DomainNum ).Name );
+					ErrorsFound = true;
+				} else {
+					// Set insulation depth
+					PipingSystemDomains( DomainNum ).VertInsDepth = Domain( BasementCtr ).VertInsDepth;
+				}
+
 				Domain( BasementCtr ).VertInsMaterial = cAlphaArgs( 10 );
 				PipingSystemDomains( DomainNum ).VertInsMaterialNum = FindItemInList( cAlphaArgs( 10 ), Material, TotMaterials );
 				if ( PipingSystemDomains( DomainNum ).VertInsMaterialNum == 0 ) {
 					ShowSevereError( "Invalid " + cAlphaFieldNames( 10 ) + "=" + cAlphaArgs( 10 ) );
-					ShowContinueError( "Found in " + Domain( BasementCtr ).VertInsMaterial );
+					ShowContinueError( "Found in: " + PipingSystemDomains( DomainNum ).Name );
 					ErrorsFound = true;
 				} else {
 					PipingSystemDomains( DomainNum ).VertInsThickness = Material( PipingSystemDomains( DomainNum ).VertInsMaterialNum ).Thickness;
@@ -1596,9 +1638,6 @@ namespace PlantPipingSystemsManager {
 					PipingSystemDomains( DomainNum ).VertInsProperties.SpecificHeat = Material( PipingSystemDomains( DomainNum ).VertInsMaterialNum ).SpecHeat;
 					PipingSystemDomains( DomainNum ).VertInsProperties.Conductivity = Material( PipingSystemDomains( DomainNum ).VertInsMaterialNum ).Conductivity;
 				}
-
-				// vertical insulation depth
-				PipingSystemDomains( DomainNum ).VertInsDepth = Domain( BasementCtr ).VertInsDepth;
 			}
 
 			// Set simulation interval flag
@@ -1607,8 +1646,9 @@ namespace PlantPipingSystemsManager {
 			} else if ( SameString( cAlphaArgs( 11 ), "HOURLY" ) ) {
 				PipingSystemDomains( DomainNum ).SimHourlyFlag = true;
 			} else {
-				ShowContinueError( "Could not determine basement simulation interval. Check input." );
-				ShowFatalError( "Preceding error causes program termination." );
+				ShowSevereError( "Invalid " + cAlphaFieldNames( 11 ) + "=" + cAlphaArgs( 11 ) );
+				ShowContinueError( "Found in: " + PipingSystemDomains( DomainNum ).Name );
+				ErrorsFound = true;
 			}
 
 			// Farfield ground temperature model
@@ -1632,21 +1672,26 @@ namespace PlantPipingSystemsManager {
 			// get width and length from aspect ratio later
 			PipingSystemDomains( DomainNum ).Extents.Xmax = Domain( BasementCtr ).PerimeterOffset + PipingSystemDomains( DomainNum ).BasementZone.Width / 2;
 			PipingSystemDomains( DomainNum ).Extents.Ymax = Domain( BasementCtr ).Depth;
-			PipingSystemDomains( DomainNum ).Extents.Zmax = Domain( BasementCtr ).PerimeterOffset + PipingSystemDomains( DomainNum ).BasementZone.Width / 2;
+			PipingSystemDomains( DomainNum ).Extents.Zmax = Domain( BasementCtr ).PerimeterOffset + PipingSystemDomains( DomainNum ).BasementZone.Length / 2;
 
 			// Check horizontal insulation width so as to prevent overlapping insulation. VertInsThickness is used here since it is used for vertical partition thickness.
-			if ( PipingSystemDomains( DomainNum ).HorizInsWidth + PipingSystemDomains( DomainNum ).VertInsThickness > PipingSystemDomains( DomainNum ).BasementZone.Width / 2.0
-				|| PipingSystemDomains( DomainNum ).HorizInsWidth + PipingSystemDomains( DomainNum ).VertInsThickness > PipingSystemDomains( DomainNum ).BasementZone.Width /2.0 ) {
-				ShowSevereError( "PipingSystems:" + RoutineName + ": Perimeter Horizontal Insulation Width is too high compared to basement floor dimensions" );
-				ShowFatalError( "Preceding error(s) cause program termination." );
+			if ( !PipingSystemDomains( DomainNum ).FullHorizInsPresent && ThisArea > 0.0 ) {
+				if ( ( PipingSystemDomains( DomainNum ).HorizInsWidth + PipingSystemDomains( DomainNum ).VertInsThickness ) > PipingSystemDomains( DomainNum ).BasementZone.Width / 2.0 ||
+					( PipingSystemDomains( DomainNum ).HorizInsWidth + PipingSystemDomains( DomainNum ).VertInsThickness ) > PipingSystemDomains( DomainNum ).BasementZone.Length / 2.0 ) {
+					ShowContinueError( RoutineName + ": Perimeter insulation width is too large." );
+					ShowContinueError( "This would cause overlapping insulation. Check inputs." );
+					ShowContinueError( "Defaulting to full horizontal insulation." );
+					ShowContinueError( "Found in: " + PipingSystemDomains( DomainNum ).Name );
+					PipingSystemDomains( DomainNum ).FullHorizInsPresent = true;
+				}
 			}
 
 			//******* We'll first set up the domain ********
 			PipingSystemDomains( DomainNum ).IsActuallyPartOfAHorizontalTrench = false;
 			PipingSystemDomains( DomainNum ).HasAPipeCircuit = false;
-			PipingSystemDomains( DomainNum ).IsZoneCoupledSlab = false;
+			PipingSystemDomains( DomainNum ).HasZoneCoupledSlab = false;
 			PipingSystemDomains( DomainNum ).HasBasement = false;
-			PipingSystemDomains( DomainNum ).HasCoupledBasement = true;
+			PipingSystemDomains( DomainNum ).HasZoneCoupledBasement = true;
 
 			// Domain name
 			PipingSystemDomains( DomainNum ).Name = Domain( BasementCtr ).ObjName;
@@ -1654,8 +1699,6 @@ namespace PlantPipingSystemsManager {
 			// setup output variables
 			SetupZoneCoupledOutputVariables( BasementCtr );
 
-			// Add error-handling for vertical insulation depth
-
 		}
 
 	}
@@ -2275,11 +2318,11 @@ namespace PlantPipingSystemsManager {
 
 		// SUBROUTINE LOCAL VARIABLE DECLARATIONS:
 
-		if ( PipingSystemDomains( DomainNum ).IsZoneCoupledSlab ) {
+		if ( PipingSystemDomains( DomainNum ).HasZoneCoupledSlab ) {
 			// Zone-coupled slab outputs
 			SetupOutputVariable( "GroundDomain Slab Zone Coupled Surface Heat Flux [W/m2]", PipingSystemDomains( DomainNum ).HeatFlux, "Zone", "Average", PipingSystemDomains( DomainNum ).Name );
 			SetupOutputVariable( "GroundDomain Slab Zone Coupled Surface Temperature [C]", PipingSystemDomains( DomainNum ).ZoneCoupledSurfaceTemp, "Zone", "Average", PipingSystemDomains( DomainNum ).Name );
-		} else if ( PipingSystemDomains( DomainNum ).HasCoupledBasement ) {
+		} else if ( PipingSystemDomains( DomainNum ).HasZoneCoupledBasement ) {
 			// Zone-coupled basement wall outputs
 			SetupOutputVariable( "GroundDomain Basement Wall Interface Heat Flux [W/m2]", PipingSystemDomains( DomainNum ).WallHeatFlux, "Zone", "Average", PipingSystemDomains( DomainNum ).Name );
 			SetupOutputVariable( "GroundDomain Basement Wall Interface Temperature [C]", PipingSystemDomains( DomainNum ).BasementWallTemp, "Zone", "Average", PipingSystemDomains( DomainNum ).Name );
@@ -4151,7 +4194,7 @@ namespace PlantPipingSystemsManager {
 
 		//'***** LAYOUT MESH REGIONS *****'
 		// Zone-coupled slab  models
-		if ( PipingSystemDomains( DomainNum ).HasCoupledBasement ) {
+		if ( PipingSystemDomains( DomainNum ).HasZoneCoupledBasement ) {
 			RegionListCount = CreateRegionListCount( XPartitionRegions, PipingSystemDomains( DomainNum ).Extents.Xmax, XPartitionsExist );
 			XRegions.allocate( { 0, RegionListCount - 1 } );
 			XRegions = CreateRegionList( DomainNum, XPartitionRegions, PipingSystemDomains( DomainNum ).Extents.Xmax, RegionType_XDirection, RegionListCount - 1, XPartitionsExist, _, _, PipingSystemDomains( DomainNum ).XIndex, PipingSystemDomains( DomainNum ).XWallIndex, PipingSystemDomains( DomainNum ).InsulationXIndex );
@@ -4163,7 +4206,7 @@ namespace PlantPipingSystemsManager {
 			RegionListCount = CreateRegionListCount( ZPartitionRegions, PipingSystemDomains( DomainNum ).Extents.Zmax, ZPartitionsExist );
 			ZRegions.allocate( { 0, RegionListCount - 1 } );
 			ZRegions = CreateRegionList( DomainNum, ZPartitionRegions, PipingSystemDomains( DomainNum ).Extents.Zmax, RegionType_ZDirection, RegionListCount - 1, ZPartitionsExist, _, _, _, _, _, _, _, _, PipingSystemDomains( DomainNum ).ZIndex, PipingSystemDomains( DomainNum ).ZWallIndex, PipingSystemDomains( DomainNum ).InsulationZIndex );
-		} else if ( PipingSystemDomains( DomainNum ).IsZoneCoupledSlab ) {
+		} else if ( PipingSystemDomains( DomainNum ).HasZoneCoupledSlab ) {
 			RegionListCount = CreateRegionListCount( XPartitionRegions, PipingSystemDomains( DomainNum ).Extents.Xmax, XPartitionsExist );
 			XRegions.allocate( { 0, RegionListCount - 1 } );
 			XRegions = CreateRegionList( DomainNum, XPartitionRegions, PipingSystemDomains( DomainNum ).Extents.Xmax, RegionType_XDirection, RegionListCount - 1, XPartitionsExist, _, _, PipingSystemDomains( DomainNum ).XIndex, _, PipingSystemDomains( DomainNum ).InsulationXIndex );
@@ -4334,7 +4377,7 @@ namespace PlantPipingSystemsManager {
 		}
 
 		// Underground Piping Systems Ground domain with basement interaction
-		if ( !PipingSystemDomains( DomainNum ).HasCoupledBasement ) {
+		if ( !PipingSystemDomains( DomainNum ).HasZoneCoupledBasement ) {
 			if ( PipingSystemDomains( DomainNum ).HasBasement ) { // FHX model
 				//'NOTE: the basement depth is still a depth from the ground surface, need to correct for this here
 				if ( PipingSystemDomains( DomainNum ).BasementZone.Width > 0 ) {
@@ -4568,7 +4611,7 @@ namespace PlantPipingSystemsManager {
 		}
 
 		// Zone-coupled slab
-		if ( PipingSystemDomains( DomainNum ).IsZoneCoupledSlab ) {
+		if ( PipingSystemDomains( DomainNum ).HasZoneCoupledSlab ) {
 			// NOTE: the slab depth is still a depth from the ground surface, need to correct for this here.
 			// Create partition at slab edges in the X direction
 			if ( PipingSystemDomains( DomainNum ).SlabWidth > 0 ) {
@@ -4824,7 +4867,7 @@ namespace PlantPipingSystemsManager {
 			// Scan all grid regions to make sure this range doesn't fall within an already entered range
 			for ( SubIndex = 0; SubIndex <= Index - 1; ++SubIndex ) {
 				// Coupled-basement model has adjacent partitions: ThesePartitionRegions( 0 ) and ThesePartitionRegions( 1 ) - SA
-				if ( PipingSystemDomains( DomainNum ).HasCoupledBasement && Index ==1 ) {
+				if ( PipingSystemDomains( DomainNum ).HasZoneCoupledBasement && Index ==1 ) {
 					if ( IsInRange_BasementModel( CellLeft, ThesePartitionRegions( SubIndex ).Min, ThesePartitionRegions( SubIndex ).Max ) || IsInRange( CellRight, ThesePartitionRegions( SubIndex ).Min, ThesePartitionRegions( SubIndex ).Max ) ) {
 
 						ShowSevereError( "PlantPipingSystems::" + RoutineName + ": Invalid partition location in domain." );
@@ -5034,7 +5077,7 @@ namespace PlantPipingSystemsManager {
 					LeftRegionExtent = ThesePartitionRegions( Index - 1 ).Max;
 				}
 				// Coupled-basement model has adjacent partitions: ThesePartitionRegions( 0 ) and ThesePartitionRegions( 1 ). Do not add a mesh region to the left of ThesePartitionRegions( 1 ).-SA
-				if ( ! PipingSystemDomains( DomainNum ).HasCoupledBasement || ( Index == 0 || Index == 2 ) ) {
+				if ( ! PipingSystemDomains( DomainNum ).HasZoneCoupledBasement || ( Index == 0 || Index == 2 ) ) {
 					//'add a mesh region to the "left" of the partition
 					++PreviousUbound;
 					TempRegions( PreviousUbound ) = TempGridRegionData( LeftRegionExtent, ThisRegion.Min, DirDirection );
@@ -5455,7 +5498,7 @@ namespace PlantPipingSystemsManager {
 					//'apply boundary conditions
 
 					// For zone-coupled ground domain
-					if ( PipingSystemDomains( DomainNum ).IsZoneCoupledSlab ) {
+					if ( PipingSystemDomains( DomainNum ).HasZoneCoupledSlab ) {
 						if ( PipingSystemDomains( DomainNum ).SlabInGradeFlag ) { // Slab in-grade
 							if ( CellYIndex == cells.l2() ) { // Farfield cells
 								CellType = CellType_FarfieldBoundary;
@@ -5548,7 +5591,7 @@ namespace PlantPipingSystemsManager {
 								++TotNumCells;
 							}
 						}
-					} else if ( PipingSystemDomains( DomainNum ).HasCoupledBasement ) { // basement model, zone-coupled
+					} else if ( PipingSystemDomains( DomainNum ).HasZoneCoupledBasement ) { // basement model, zone-coupled
 						// Set the appropriate cell type
 						if ( CellYIndex == cells.l2() ) { // Farfield cells
 							CellType = CellType_FarfieldBoundary;
@@ -6222,12 +6265,12 @@ namespace PlantPipingSystemsManager {
 			}
 
 			// Update the basement surface temperatures, if any
-			if ( PipingSystemDomains( DomainNum ).HasBasement || PipingSystemDomains( DomainNum ).HasCoupledBasement ) {
+			if ( PipingSystemDomains( DomainNum ).HasBasement || PipingSystemDomains( DomainNum ).HasZoneCoupledBasement ) {
 				UpdateBasementSurfaceTemperatures( DomainNum );
 			}
 
 			// Update the slab surface temperatures, if any
-			if ( PipingSystemDomains( DomainNum ).IsZoneCoupledSlab ) {
+			if ( PipingSystemDomains( DomainNum ).HasZoneCoupledSlab ) {
 				UpdateZoneSurfaceTemperatures( DomainNum );
 			}
 		}
@@ -6282,7 +6325,7 @@ namespace PlantPipingSystemsManager {
 						cell.MyBase.Temperature = EvaluateFarfieldBoundaryTemperature( DomainNum, cell );
 					} else if ( ( SELECT_CASE_var == CellType_BasementWall ) || ( SELECT_CASE_var == CellType_BasementCorner ) || ( SELECT_CASE_var == CellType_BasementFloor ) ) {
 						// basement model, zone-coupled. Call EvaluateZoneInterfaceTemperature routine to handle timestep/hourly simulation.
-						if ( PipingSystemDomains( DomainNum ).HasCoupledBasement ) {
+						if ( PipingSystemDomains( DomainNum ).HasZoneCoupledBasement ) {
 							cell.MyBase.Temperature = EvaluateZoneInterfaceTemperature( DomainNum, cell );
 						} else { // FHX model
 							cell.MyBase.Temperature = EvaluateBasementCellTemperature( DomainNum, cell );
@@ -6533,7 +6576,7 @@ namespace PlantPipingSystemsManager {
 			CurDirection = NeighborBoundaryCells( DirectionCounter );
 
 			// For Zone-coupled slab or basement configuration
-			if ( PipingSystemDomains( DomainNum ).IsZoneCoupledSlab || PipingSystemDomains( DomainNum ).HasCoupledBasement ) {
+			if ( PipingSystemDomains( DomainNum ).HasZoneCoupledSlab || PipingSystemDomains( DomainNum ).HasZoneCoupledBasement ) {
 				//-x-direction will always be a farfield boundary
 				//-z will also be a farfield boundary
 				//+x and +z will be handled above
@@ -8622,7 +8665,7 @@ namespace PlantPipingSystemsManager {
 					} else if ( ( SELECT_CASE_var == CellType_GeneralField ) || ( SELECT_CASE_var == CellType_GroundSurface ) || ( SELECT_CASE_var == CellType_AdiabaticWall ) || ( SELECT_CASE_var == CellType_FarfieldBoundary ) ) {
 						cell.MyBase.Properties = PipingSystemDomains( DomainNum ).GroundProperties;
 					} else if ( ( SELECT_CASE_var == CellType_BasementWall ) || ( SELECT_CASE_var == CellType_BasementFloor ) || ( SELECT_CASE_var == CellType_BasementCorner ) ) {
-						if ( PipingSystemDomains( DomainNum ).HasCoupledBasement ) { // Basement interface layer
+						if ( PipingSystemDomains( DomainNum ).HasZoneCoupledBasement ) { // Basement interface layer
 							cell.MyBase.Properties = PipingSystemDomains( DomainNum ).BasementInterfaceProperties;
 						} else { // Basement cells are partially ground, give them some props
 							cell.MyBase.Properties = PipingSystemDomains( DomainNum ).GroundProperties;
@@ -8799,8 +8842,8 @@ namespace PlantPipingSystemsManager {
 
 		// If pipe circuit present
 		if ( present( CircuitNum ) ) {
-			// retreive fluid properties based on the circuit inlet temperature -- which varies during the simulation
-			// but need to verify the value of inlet temperature during warmup, etc.
+			// retrieve fluid properties based on the circuit inlet temperature -- which varies during the simulation
+			// but need to verify the value of inlet temperature during warm up, etc.
 			FluidCp = GetSpecificHeatGlycol( PlantLoop( PipingSystemCircuits( CircuitNum ).LoopNum ).FluidName, PipingSystemCircuits( CircuitNum ).InletTemperature, PlantLoop( PipingSystemCircuits( CircuitNum ).LoopNum ).FluidIndex, RoutineName );
 			FluidDensity = GetDensityGlycol( PlantLoop( PipingSystemCircuits( CircuitNum ).LoopNum ).FluidName, PipingSystemCircuits( CircuitNum ).InletTemperature, PlantLoop( PipingSystemCircuits( CircuitNum ).LoopNum ).FluidIndex, RoutineName );
 			FluidConductivity = GetConductivityGlycol( PlantLoop( PipingSystemCircuits( CircuitNum ).LoopNum ).FluidName, PipingSystemCircuits( CircuitNum ).InletTemperature, PlantLoop( PipingSystemCircuits( CircuitNum ).LoopNum ).FluidIndex, RoutineName );
@@ -8964,10 +9007,22 @@ namespace PlantPipingSystemsManager {
 		//'this routine should be *much* more restrictive than the exceptions, so we should be safe with this location
 		OutOfRange = CheckForOutOfRangeTemps( DomainNum );
 		if ( OutOfRange ) {
-			ShowSevereError( "PipingSystems:" + RoutineName + ": Out of range temperatures detected in piping system simulation." );
-			ShowContinueError( "This could be due to the size of the pipe circuit in relation to the loads being imposed." );
-			ShowContinueError( "Try increasing the size of the pipe circuit and investigate sizing effects." );
-			ShowFatalError( "Preceding error(s) cause program termination" );
+			if ( PipingSystemDomains( DomainNum ).HasZoneCoupledSlab ) {
+				ShowSevereError( "Site:GroundDomain:Slab" + RoutineName + ": Out of range temperatures detected in the ground domain." );
+				ShowContinueError( "This could be due to the size of the loads on the domain." );
+				ShowContinueError( "Verify inputs are correct. If problem persists, notify EnergyPlus support." );
+				ShowFatalError( "Preceding error(s) cause program termination" );
+			} else if ( PipingSystemDomains( DomainNum ).HasZoneCoupledBasement ) {
+				ShowSevereError( "Site:GroundDomain:Basement" + RoutineName + ": Out of range temperatures detected in the ground domain." );
+				ShowContinueError( "This could be due to the size of the loads on the domain." );
+				ShowContinueError( "Verify inputs are correct. If problem persists, notify EnergyPlus support." );
+				ShowFatalError( "Preceding error(s) cause program termination" );
+			} else {
+				ShowSevereError( "PipingSystems:" + RoutineName + ": Out of range temperatures detected in piping system simulation." );
+				ShowContinueError( "This could be due to the size of the pipe circuit in relation to the loads being imposed." );
+				ShowContinueError( "Try increasing the size of the pipe circuit and investigate sizing effects." );
+				ShowFatalError( "Preceding error(s) cause program termination" );
+			}
 		}
 
 	}
diff --git a/src/EnergyPlus/PlantPipingSystemsManager.hh b/src/EnergyPlus/PlantPipingSystemsManager.hh
index 7bb137843f1..6736a524c12 100644
--- a/src/EnergyPlus/PlantPipingSystemsManager.hh
+++ b/src/EnergyPlus/PlantPipingSystemsManager.hh
@@ -180,7 +180,7 @@ namespace PlantPipingSystemsManager {
 
 	//*********************************************************************************************!
 	void
-	GetPipingSystemsInput();
+	GetPipingSystemsAndGroundDomainsInput();
 
 	//*********************************************************************************************!
 
diff --git a/src/EnergyPlus/PurchasedAirManager.cc b/src/EnergyPlus/PurchasedAirManager.cc
index 54d8ae35872..46d03b6e055 100644
--- a/src/EnergyPlus/PurchasedAirManager.cc
+++ b/src/EnergyPlus/PurchasedAirManager.cc
@@ -198,6 +198,21 @@ namespace PurchasedAirManager {
 
 	// Functions
 
+	namespace {
+		// These were static variables within different functions. They were pulled out into the namespace
+		// to facilitate easier unit testing of those functions.
+		// These are purposefully not in the header file as an extern variable. No one outside of this should
+		// use these. They are cleared by clear_state() for use by unit tests, but normal simulations should be unaffected.
+		// This is purposefully in an anonymous namespace so nothing outside this implementation file can use it.
+		bool InitPurchasedAirMyOneTimeFlag( true );
+		bool InitPurchasedAirZoneEquipmentListChecked( false ); // True after the Zone Equipment List has been checked for items
+		Array1D_bool InitPurchasedAirMyEnvrnFlag;
+		Array1D_bool InitPurchasedAirMySizeFlag;
+		Array1D_bool InitPurchasedAirOneTimeUnitInitsDone; // True if one-time inits for PurchAirNum are completed
+
+	}
+
+
 	void
 	SimPurchasedAir(
 		std::string const & PurchAirName,
@@ -831,12 +846,7 @@ namespace PurchasedAirManager {
 		// na
 
 		// SUBROUTINE LOCAL VARIABLE DECLARATIONS:
-		static bool MyOneTimeFlag( true );
-		static bool ZoneEquipmentListChecked( false ); // True after the Zone Equipment List has been checked for items
 		int Loop;
-		static Array1D_bool MyEnvrnFlag;
-		static Array1D_bool MySizeFlag;
-		static Array1D_bool OneTimeUnitInitsDone; // True if one-time inits for PurchAirNum are completed
 		//      LOGICAL :: ErrorsFound = .FALSE.   ! If errors detected in input
 		bool UnitOn; // simple checks for error
 		bool CoolOn; // simple checks for error
@@ -847,21 +857,21 @@ namespace PurchasedAirManager {
 		bool UseReturnNode; // simple checks for error
 
 		// Do the Begin Simulation initializations
-		if ( MyOneTimeFlag ) {
+		if ( InitPurchasedAirMyOneTimeFlag ) {
 
-			MyEnvrnFlag.allocate( NumPurchAir );
-			MySizeFlag.allocate( NumPurchAir );
-			OneTimeUnitInitsDone.allocate( NumPurchAir );
-			MyEnvrnFlag = true;
-			MySizeFlag = true;
-			OneTimeUnitInitsDone = false;
-			MyOneTimeFlag = false;
+			InitPurchasedAirMyEnvrnFlag.allocate( NumPurchAir );
+			InitPurchasedAirMySizeFlag.allocate( NumPurchAir );
+			InitPurchasedAirOneTimeUnitInitsDone.allocate( NumPurchAir );
+			InitPurchasedAirMyEnvrnFlag = true;
+			InitPurchasedAirMySizeFlag = true;
+			InitPurchasedAirOneTimeUnitInitsDone = false;
+			InitPurchasedAirMyOneTimeFlag = false;
 
 		}
 
 		// need to check all units to see if they are on Zone Equipment List or issue warning
-		if ( ! ZoneEquipmentListChecked && ZoneEquipInputsFilled ) {
-			ZoneEquipmentListChecked = true;
+		if ( !InitPurchasedAirZoneEquipmentListChecked && ZoneEquipInputsFilled ) {
+			InitPurchasedAirZoneEquipmentListChecked = true;
 			for ( Loop = 1; Loop <= NumPurchAir; ++Loop ) {
 				if ( CheckZoneEquipmentList( PurchAir( Loop ).cObjectName, PurchAir( Loop ).Name ) ) continue;
 				ShowSevereError( "InitPurchasedAir: " + PurchAir( Loop ).cObjectName + " = " + PurchAir( Loop ).Name + " is not on any ZoneHVAC:EquipmentList.  It will not be simulated." );
@@ -869,8 +879,8 @@ namespace PurchasedAirManager {
 		}
 
 		// one time inits for each unit - links PurchAirNum with static input data from ControlledZoneNum and ActualZoneNum
-		if ( ! OneTimeUnitInitsDone( PurchAirNum ) ) {
-			OneTimeUnitInitsDone( PurchAirNum ) = true;
+		if ( !InitPurchasedAirOneTimeUnitInitsDone( PurchAirNum ) ) {
+			InitPurchasedAirOneTimeUnitInitsDone( PurchAirNum ) = true;
 
 			// Is the supply node really a zone inlet node?
 			// this check has to be done here because of SimPurchasedAir passing in ControlledZoneNum
@@ -924,15 +934,15 @@ namespace PurchasedAirManager {
 			}
 		}
 
-		if ( ! SysSizingCalc && MySizeFlag( PurchAirNum ) ) {
+		if ( !SysSizingCalc && InitPurchasedAirMySizeFlag( PurchAirNum ) ) {
 
 			SizePurchasedAir( PurchAirNum );
 
-			MySizeFlag( PurchAirNum ) = false;
+			InitPurchasedAirMySizeFlag( PurchAirNum ) = false;
 		}
 
 		// Do the Begin Environment initializations
-		if ( BeginEnvrnFlag && MyEnvrnFlag( PurchAirNum ) ) {
+		if ( BeginEnvrnFlag && InitPurchasedAirMyEnvrnFlag( PurchAirNum ) ) {
 
 			if ( ( PurchAir( PurchAirNum ).HeatingLimit == LimitFlowRate ) || ( PurchAir( PurchAirNum ).HeatingLimit == LimitFlowRateAndCapacity ) ) {
 				PurchAir( PurchAirNum ).MaxHeatMassFlowRate = StdRhoAir * PurchAir( PurchAirNum ).MaxHeatVolFlowRate;
@@ -944,11 +954,11 @@ namespace PurchasedAirManager {
 			} else {
 				PurchAir( PurchAirNum ).MaxCoolMassFlowRate = 0.0;
 			}
-			MyEnvrnFlag( PurchAirNum ) = false;
+			InitPurchasedAirMyEnvrnFlag( PurchAirNum ) = false;
 		}
 
 		if ( ! BeginEnvrnFlag ) {
-			MyEnvrnFlag( PurchAirNum ) = true;
+			InitPurchasedAirMyEnvrnFlag( PurchAirNum ) = true;
 		}
 
 		// These initializations are done every iteration
@@ -2905,8 +2915,16 @@ namespace PurchasedAirManager {
 	clear_state()
 	{
 		NumPurchAir = 0;
+		GetPurchAirInputFlag = true;
+		CheckEquipName.deallocate();
 		PurchAir.deallocate();
 		PurchAirNumericFields.deallocate();
+		// from anonymous namespace
+		InitPurchasedAirMyOneTimeFlag = true ;
+		InitPurchasedAirZoneEquipmentListChecked =  false ; // True after the Zone Equipment List has been checked for items
+		InitPurchasedAirMyEnvrnFlag.deallocate();
+		InitPurchasedAirMySizeFlag.deallocate();
+		InitPurchasedAirOneTimeUnitInitsDone.deallocate(); // True if one-time inits for PurchAirNum are completed
 	}
 
 } // PurchasedAirManager
diff --git a/src/EnergyPlus/SQLiteProcedures.cc b/src/EnergyPlus/SQLiteProcedures.cc
index 5d9fb2703ba..dfa10d078ac 100644
--- a/src/EnergyPlus/SQLiteProcedures.cc
+++ b/src/EnergyPlus/SQLiteProcedures.cc
@@ -2526,7 +2526,7 @@ bool SQLite::Surface::insertIntoSQLite( sqlite3_stmt * insertStmt )
 	sqliteBindDouble(insertStmt, 8, azimuth);
 	sqliteBindDouble(insertStmt, 9, height);
 	sqliteBindDouble(insertStmt, 10, reveal);
-	sqliteBindInteger(insertStmt, 11, shape);
+	sqliteBindInteger(insertStmt, 11, static_cast<int>( shape ) );
 	sqliteBindInteger(insertStmt, 12, sides);
 	sqliteBindDouble(insertStmt, 13, tilt);
 	sqliteBindDouble(insertStmt, 14, width);
diff --git a/src/EnergyPlus/SQLiteProcedures.hh b/src/EnergyPlus/SQLiteProcedures.hh
index 24c87762137..e51300ce379 100644
--- a/src/EnergyPlus/SQLiteProcedures.hh
+++ b/src/EnergyPlus/SQLiteProcedures.hh
@@ -459,7 +459,7 @@ private:
 			double const & azimuth;
 			double const & height;
 			double const & reveal;
-			int const & shape;
+			DataSurfaces::SurfaceShape const & shape;
 			int const & sides;
 			double const & tilt;
 			double const & width;
diff --git a/src/EnergyPlus/SimAirServingZones.cc b/src/EnergyPlus/SimAirServingZones.cc
index be03f8f696c..94a0b68b667 100644
--- a/src/EnergyPlus/SimAirServingZones.cc
+++ b/src/EnergyPlus/SimAirServingZones.cc
@@ -6081,7 +6081,8 @@ namespace SimAirServingZones {
 			}
 
 			// EMS calling point to customize zone sizing results
-			ManageEMS( emsCallFromSystemSizing );
+			bool anyEMSRan;
+			ManageEMS( emsCallFromSystemSizing, anyEMSRan );
 
 			//EMS override point
 			if ( AnyEnergyManagementSystemInModel ) {
diff --git a/src/EnergyPlus/SimulationManager.cc b/src/EnergyPlus/SimulationManager.cc
index 75105a787bf..222af01ced5 100644
--- a/src/EnergyPlus/SimulationManager.cc
+++ b/src/EnergyPlus/SimulationManager.cc
@@ -452,8 +452,8 @@ namespace SimulationManager {
 			}
 
 			CreateEnergyReportStructure();
-
-			ManageEMS( emsCallFromSetupSimulation ); // point to finish setup processing EMS, sensor ready now
+			bool anyEMSRan;
+			ManageEMS( emsCallFromSetupSimulation, anyEMSRan ); // point to finish setup processing EMS, sensor ready now
 
 			ProduceRDDMDD();
 
@@ -518,7 +518,8 @@ namespace SimulationManager {
 				isFinalYear = true;
 			}
 
-			ManageEMS( emsCallFromBeginNewEvironment ); // calling point
+			bool anyEMSRan;
+			ManageEMS( emsCallFromBeginNewEvironment, anyEMSRan ); // calling point
 
 			while ( ( DayOfSim < NumOfDayInEnvrn ) || ( WarmupFlag ) ) { // Begin day loop ...
 
diff --git a/src/EnergyPlus/SingleDuct.cc b/src/EnergyPlus/SingleDuct.cc
index 77b2ae06ff8..c2e628c6e2c 100644
--- a/src/EnergyPlus/SingleDuct.cc
+++ b/src/EnergyPlus/SingleDuct.cc
@@ -700,7 +700,7 @@ namespace SingleDuct {
 
 			//Setup the Average damper Position output variable
 			SetupOutputVariable( "Zone Air Terminal VAV Damper Position []", Sys( SysNum ).DamperPosition, "System", "Average", Sys( SysNum ).SysName );
-			SetupOutputVariable( "Zone Air Terminal Minimum Air Flow Fraction []", Sys( SysNum ).ZoneMinAirFrac, "System", "Average", Sys( SysNum ).SysName );
+			SetupOutputVariable( "Zone Air Terminal Minimum Air Flow Fraction []", Sys( SysNum ).ZoneMinAirFracReport, "System", "Average", Sys( SysNum ).SysName );
 			SetupOutputVariable( "Zone Air Terminal Outdoor Air Volume Flow Rate [m3/s]", Sys( SysNum ).OutdoorAirFlowRate, "System", "Average", Sys( SysNum ).SysName );
 
 		} // end Number of Sys Loop
@@ -1140,6 +1140,7 @@ namespace SingleDuct {
 
 			//Setup the Average damper Position output variable
 			SetupOutputVariable( "Zone Air Terminal VAV Damper Position []", Sys( SysNum ).DamperPosition, "System", "Average", Sys( SysNum ).SysName );
+			SetupOutputVariable( "Zone Air Terminal Minimum Air Flow Fraction []", Sys( SysNum ).ZoneMinAirFracReport, "System", "Average", Sys( SysNum ).SysName );
 			SetupOutputVariable( "Zone Air Terminal Outdoor Air Volume Flow Rate [m3/s]", Sys( SysNum ).OutdoorAirFlowRate, "System", "Average", Sys( SysNum ).SysName );
 
 		} // end Number of Sys Loop
@@ -2398,7 +2399,7 @@ namespace SingleDuct {
 		// the massflow rate for cooling is determined to meet the entire load.  Then
 		// if the massflow is below the minimum or greater than the Max it is set to either the Min
 		// or the Max as specified for the VAV model.
-		if ( ( QTotLoad < 0.0 ) && ( SysInlet( SysNum ).AirMassFlowRateMaxAvail > 0.0 ) && ( TempControlType( ZoneNum ) != SingleHeatingSetPoint ) ) {
+		if ( ( QTotLoad < 0.0 ) && ( SysInlet( SysNum ).AirMassFlowRateMaxAvail > 0.0 ) && ( TempControlType( ZoneNum ) != SingleHeatingSetPoint ) && ( GetCurrentScheduleValue( Sys( SysNum ).SchedPtr ) > 0.0 ) ) {
 			// Calculate the flow required for cooling
 			CpAirSysIn = PsyCpAirFnWTdb( SysInlet( SysNum ).AirHumRat, SysInlet( SysNum ).AirTemp );
 			DeltaTemp = CpAirSysIn * SysInlet( SysNum ).AirTemp - CpAirZn * ZoneTemp;
@@ -2436,7 +2437,7 @@ namespace SingleDuct {
 				}
 			}
 
-		} else if ( ( SysInlet( SysNum ).AirMassFlowRateMaxAvail > 0.0 ) && ( QTotLoad >= 0.0 || TempControlType( ZoneNum ) == SingleHeatingSetPoint ) ) {
+		} else if ( ( SysInlet( SysNum ).AirMassFlowRateMaxAvail > 0.0 ) && ( QTotLoad >= 0.0 || TempControlType( ZoneNum ) == SingleHeatingSetPoint ) && ( GetCurrentScheduleValue( Sys( SysNum ).SchedPtr ) > 0.0 ) ) {
 			//     IF (Sys(SysNum)%DamperHeatingAction .EQ. ReverseAction .AND. SysInlet(SysNum)%AirMassFlowRateMinAvail <= SmallMassFlow) THEN
 			// special case for heating: reverse action and damper allowed to close - set the minimum flow rate to a small but nonzero value
 			//       MassFlow = 0.01d0*SysInlet(SysNum)%AirMassFlowRateMaxAvail
@@ -2502,10 +2503,13 @@ namespace SingleDuct {
 
 		if ( MassFlow == 0.0 ) {
 			Sys( SysNum ).DamperPosition = 0.0;
+			Sys( SysNum ).ZoneMinAirFracReport = 0.0;
 		} else if ( ( MassFlow > 0.0 ) && ( MassFlow < Sys( SysNum ).AirMassFlowRateMax ) ) {
 			Sys( SysNum ).DamperPosition = MassFlow / Sys( SysNum ).AirMassFlowRateMax;
+			Sys( SysNum ).ZoneMinAirFracReport = Sys( SysNum ).ZoneMinAirFrac;
 		} else if ( MassFlow == Sys( SysNum ).AirMassFlowRateMax ) {
 			Sys( SysNum ).DamperPosition = 1.0;
+			Sys( SysNum ).ZoneMinAirFracReport = Sys( SysNum ).ZoneMinAirFrac;
 		}
 
 		//Need to make sure that the damper outlets are passed to the coil inlet
@@ -2648,10 +2652,13 @@ namespace SingleDuct {
 				// Recalculate the Damper Position.
 				if ( MassFlow == 0.0 ) {
 					Sys( SysNum ).DamperPosition = 0.0;
+					Sys( SysNum ).ZoneMinAirFracReport = 0.0;
 				} else if ( ( MassFlow > 0.0 ) && ( MassFlow < Sys( SysNum ).AirMassFlowRateMax ) ) {
 					Sys( SysNum ).DamperPosition = MassFlow / Sys( SysNum ).AirMassFlowRateMax;
+					Sys( SysNum ).ZoneMinAirFracReport = Sys( SysNum ).ZoneMinAirFrac;
 				} else if ( MassFlow == Sys( SysNum ).AirMassFlowRateMax ) {
 					Sys( SysNum ).DamperPosition = 1.0;
+					Sys( SysNum ).ZoneMinAirFracReport = Sys( SysNum ).ZoneMinAirFrac;
 				}
 
 			} else if ( SELECT_CASE_var == HCoilType_SteamAirHeating ) { // ! COIL:STEAM:AIRHEATING
diff --git a/src/EnergyPlus/SingleDuct.hh b/src/EnergyPlus/SingleDuct.hh
index d5b5f5cd110..0f006af093c 100644
--- a/src/EnergyPlus/SingleDuct.hh
+++ b/src/EnergyPlus/SingleDuct.hh
@@ -155,6 +155,7 @@ namespace SingleDuct {
 		Real64 HeatAirMassFlowRateMax; // Max Specified Mass Flow Rate of unit at max heating [kg/sec]
 		int ZoneMinAirFracMethod; // parameter for what method is used for min flow fraction
 		Real64 ZoneMinAirFrac; // Fraction of supply air used as minimum flow
+		Real64 ZoneMinAirFracReport; // Fraction of supply air used as minimum flow for reporting (zero if terminal unit flow is zero)
 		Real64 ZoneFixedMinAir; // Absolute minimum supply air flow
 		int ZoneMinAirFracSchPtr; // pointer to the schedule for min flow fraction
 		bool ConstantMinAirFracSetByUser; // record if user left field blank for constant min fraction.
@@ -225,6 +226,7 @@ namespace SingleDuct {
 			HeatAirMassFlowRateMax( 0.0 ),
 			ZoneMinAirFracMethod( ConstantMinFrac ),
 			ZoneMinAirFrac( 0.0 ),
+			ZoneMinAirFracReport( 0.0 ),
 			ZoneFixedMinAir( 0.0 ),
 			ZoneMinAirFracSchPtr( 0 ),
 			ConstantMinAirFracSetByUser( false ),
diff --git a/src/EnergyPlus/SolarShading.cc b/src/EnergyPlus/SolarShading.cc
index ee8fb74195c..d25bc5e054a 100644
--- a/src/EnergyPlus/SolarShading.cc
+++ b/src/EnergyPlus/SolarShading.cc
@@ -7194,6 +7194,10 @@ namespace SolarShading {
 			} else {
 				SUN3( DayOfYear, AvgSinSolarDeclin, AvgEqOfTime );
 				AvgCosSolarDeclin = std::sqrt( 1.0 - pow_2( AvgSinSolarDeclin ) );
+				// trigger display of progress in the simulation every two weeks
+				if ( !WarmupFlag && BeginDayFlag && ( DayOfSim % 14 == 0 ) ) {
+					DisplayPerfSimulationFlag = true;
+				}
 			}
 
 			CalcPerSolarBeam( AvgEqOfTime, AvgSinSolarDeclin, AvgCosSolarDeclin );
diff --git a/src/EnergyPlus/SurfaceGeometry.cc b/src/EnergyPlus/SurfaceGeometry.cc
index a60227edcca..931d0cd9c02 100644
--- a/src/EnergyPlus/SurfaceGeometry.cc
+++ b/src/EnergyPlus/SurfaceGeometry.cc
@@ -8309,7 +8309,7 @@ namespace SurfaceGeometry {
 		//  REAL(r64) testval
 		//  INTEGER ploop
 		//  INTEGER vloop
-		int ThisShape( 0 );
+		SurfaceShape ThisShape( SurfaceShape::None );
 		bool BaseSurface; // True if a base surface or a detached shading surface
 		Real64 ThisSurfAz;
 		Real64 ThisSurfTilt;
@@ -8398,16 +8398,16 @@ namespace SurfaceGeometry {
 			Surface( ThisSurf ).Width = ThisWidth;
 			Surface( ThisSurf ).Height = ThisHeight; // For a horizontal surface this is actually length!
 			if ( Surface( ThisSurf ).Sides == 3 ) {
-				Surface( ThisSurf ).Shape = Triangle;
+				Surface( ThisSurf ).Shape = SurfaceShape::Triangle;
 			} else if ( Surface( ThisSurf ).Sides == 4 ) {
 				// Test for rectangularity
 				if ( isRectangle( ThisSurf ) ) {
-					Surface( ThisSurf ).Shape = Rectangle;
+					Surface( ThisSurf ).Shape = SurfaceShape::Rectangle;
 				} else {
-					Surface( ThisSurf ).Shape = Quadrilateral;
+					Surface( ThisSurf ).Shape = SurfaceShape::Quadrilateral;
 				}
 			} else { // Surface( ThisSurf ).Sides > 4
-				Surface( ThisSurf ).Shape = Polygonal;
+				Surface( ThisSurf ).Shape = SurfaceShape::Polygonal;
 				if ( std::abs( ThisHeight * ThisWidth - Surface( ThisSurf ).GrossArea ) > 0.001 ) {
 					Surface( ThisSurf ).Width = std::sqrt( Surface( ThisSurf ).GrossArea );
 					Surface( ThisSurf ).Height = Surface( ThisSurf ).Width;
@@ -8424,11 +8424,11 @@ namespace SurfaceGeometry {
 			if ( HeatTransSurf ) {
 
 				if ( Surface( ThisSurf ).Sides == 4 ) {
-					ThisShape = RectangularDoorWindow;
+					ThisShape = SurfaceShape::RectangularDoorWindow;
 				} else if ( Surface( ThisSurf ).Sides == 3 && Surface( ThisSurf ).Class == SurfaceClass_Window ) {
-					ThisShape = TriangularWindow;
+					ThisShape = SurfaceShape::TriangularWindow;
 				} else if ( Surface( ThisSurf ).Sides == 3 && Surface( ThisSurf ).Class == SurfaceClass_Door ) {
-					ThisShape = TriangularDoor;
+					ThisShape = SurfaceShape::TriangularDoor;
 				} else {
 					assert( false );
 				}
@@ -8439,12 +8439,12 @@ namespace SurfaceGeometry {
 					// left or right fin
 					if ( ThisSurfAz < 0.0 ) ThisSurfAz += 360.0;
 					if ( ThisSurfAz > Surface( Surface( ThisSurf ).BaseSurf ).Azimuth ) {
-						ThisShape = RectangularLeftFin;
+						ThisShape = SurfaceShape::RectangularLeftFin;
 					} else {
-						ThisShape = RectangularRightFin;
+						ThisShape = SurfaceShape::RectangularRightFin;
 					}
 				} else {
-					ThisShape = RectangularOverhang;
+					ThisShape = SurfaceShape::RectangularOverhang;
 				}
 
 			}
@@ -8452,7 +8452,7 @@ namespace SurfaceGeometry {
 			// Setting relative coordinates for shadowing calculations for subsurfaces
 			{ auto const SELECT_CASE_var( ThisShape );
 
-			if ( SELECT_CASE_var == RectangularDoorWindow ) { // Rectangular heat transfer subsurface
+			if ( SELECT_CASE_var == SurfaceShape::RectangularDoorWindow ) { // Rectangular heat transfer subsurface
 
 				PlaneEquation( Surface( Surface( ThisSurf ).BaseSurf ).Vertex, Surface( Surface( ThisSurf ).BaseSurf ).Sides, BasePlane, SError );
 				if ( SError ) {
@@ -8550,7 +8550,7 @@ namespace SurfaceGeometry {
 					}
 				}
 
-			} else if ( ( SELECT_CASE_var == TriangularWindow ) || ( SELECT_CASE_var == TriangularDoor ) ) {
+			} else if ( ( SELECT_CASE_var == SurfaceShape::TriangularWindow ) || ( SELECT_CASE_var == SurfaceShape::TriangularDoor ) ) {
 
 				PlaneEquation( Surface( Surface( ThisSurf ).BaseSurf ).Vertex, Surface( Surface( ThisSurf ).BaseSurf ).Sides, BasePlane, SError );
 				if ( SError ) {
@@ -8591,7 +8591,7 @@ namespace SurfaceGeometry {
 				Ypsv( 3 ) = -Xp * BaseSinAzimuth * BaseCosTilt - Yp * BaseCosAzimuth * BaseCosTilt + Zp * BaseSinTilt;
 				Zpsv( 3 ) = Xp * BaseSinAzimuth * BaseSinTilt + Yp * BaseCosAzimuth * BaseSinTilt + Zp * BaseCosTilt;
 
-			} else if ( SELECT_CASE_var == RectangularOverhang ) {
+			} else if ( SELECT_CASE_var == SurfaceShape::RectangularOverhang ) {
 
 				Xp = Surface( ThisSurf ).Vertex( 2 ).x - BaseXLLC;
 				Yp = Surface( ThisSurf ).Vertex( 2 ).y - BaseYLLC;
@@ -8618,7 +8618,7 @@ namespace SurfaceGeometry {
 				Zpsv( 2 ) = 0.0;
 				Zpsv( 3 ) = 0.0;
 
-			} else if ( SELECT_CASE_var == RectangularLeftFin ) {
+			} else if ( SELECT_CASE_var == SurfaceShape::RectangularLeftFin ) {
 
 				Xp = Surface( ThisSurf ).Vertex( 2 ).x - BaseXLLC;
 				Yp = Surface( ThisSurf ).Vertex( 2 ).y - BaseYLLC;
@@ -8645,7 +8645,7 @@ namespace SurfaceGeometry {
 				Zpsv( 2 ) = 0.0;
 				Zpsv( 3 ) = 0.0;
 
-			} else if ( SELECT_CASE_var == RectangularRightFin ) {
+			} else if ( SELECT_CASE_var == SurfaceShape::RectangularRightFin ) {
 
 				Xp = Surface( ThisSurf ).Vertex( 2 ).x - BaseXLLC;
 				Yp = Surface( ThisSurf ).Vertex( 2 ).y - BaseYLLC;
diff --git a/src/EnergyPlus/ThermalComfort.cc b/src/EnergyPlus/ThermalComfort.cc
index c5e5014bebd..8ffb3e041bf 100644
--- a/src/EnergyPlus/ThermalComfort.cc
+++ b/src/EnergyPlus/ThermalComfort.cc
@@ -665,7 +665,7 @@ namespace ThermalComfort {
 					if ( present( PNum ) ) {
 						AirTemp = Tset;
 					} else {
-						AirTemp = ZTAV( ZoneNum );
+						AirTemp = ZTAVComf( ZoneNum );
 					}
 				}
 			} else {
@@ -678,9 +678,9 @@ namespace ThermalComfort {
 			RadTemp = CalcRadTemp( PeopleNum );
 			// Use mean air temp for calculating RH when thermal comfort control is used
 			if ( present( PNum ) ) {
-				RelHum = PsyRhFnTdbWPb( MAT( ZoneNum ), ZoneAirHumRat( ZoneNum ), OutBaroPress );
+				RelHum = PsyRhFnTdbWPb( MAT( ZoneNum ), ZoneAirHumRatAvgComf( ZoneNum ), OutBaroPress );
 			} else {
-				RelHum = PsyRhFnTdbWPb( ZTAVComf( ZoneNum ), ZoneAirHumRatAvgComf( ZoneNum ), OutBaroPress );
+				RelHum = PsyRhFnTdbWPb( AirTemp, ZoneAirHumRatAvgComf( ZoneNum ), OutBaroPress );
 			}
 			People( PeopleNum ).TemperatureInZone = AirTemp;
 			People( PeopleNum ).RelativeHumidityInZone = RelHum * 100.0;
@@ -960,10 +960,10 @@ namespace ThermalComfort {
 			if ( IsZoneDV( ZoneNum ) || IsZoneUI( ZoneNum ) ) {
 				AirTemp = TCMF( ZoneNum ); //PH 3/7/04
 			} else {
-				AirTemp = ZTAV( ZoneNum );
+				AirTemp = ZTAVComf( ZoneNum );
 			}
 			RadTemp = CalcRadTemp( PeopleNum );
-			RelHum = PsyRhFnTdbWPb( ZTAV( ZoneNum ), ZoneAirHumRat( ZoneNum ), OutBaroPress );
+			RelHum = PsyRhFnTdbWPb( AirTemp, ZoneAirHumRatAvgComf( ZoneNum ), OutBaroPress );
 			// Metabolic rate of body (W/m2)
 			ActLevel = GetCurrentScheduleValue( People( PeopleNum ).ActivityLevelPtr ) / BodySurfArea;
 			// Energy consumption by external work (W/m2)
@@ -1392,10 +1392,10 @@ namespace ThermalComfort {
 			if ( IsZoneDV( ZoneNum ) || IsZoneUI( ZoneNum ) ) {
 				AirTemp = TCMF( ZoneNum ); //PH 3/7/04
 			} else {
-				AirTemp = ZTAV( ZoneNum );
+				AirTemp = ZTAVComf( ZoneNum );
 			}
 			RadTemp = CalcRadTemp( PeopleNum );
-			RelHum = PsyRhFnTdbWPb( ZTAV( ZoneNum ), ZoneAirHumRat( ZoneNum ), OutBaroPress );
+			RelHum = PsyRhFnTdbWPb( AirTemp, ZoneAirHumRatAvgComf( ZoneNum ), OutBaroPress );
 			ActLevel = GetCurrentScheduleValue( People( PeopleNum ).ActivityLevelPtr ) / BodySurfArea;
 			WorkEff = GetCurrentScheduleValue( People( PeopleNum ).WorkEffPtr ) * ActLevel;
 			{ auto const SELECT_CASE_var( People( PeopleNum ).ClothingType );
@@ -2228,11 +2228,11 @@ namespace ThermalComfort {
 				if ( IsZoneDV( iZone ) || IsZoneUI( iZone ) ) {
 					CurAirTemp = TCMF( iZone );
 				} else {
-					CurAirTemp = ZTAV( iZone );
+					CurAirTemp = ZTAVComf( iZone );
 				}
 				CurMeanRadiantTemp = MRT( iZone );
 				OperTemp = CurAirTemp * 0.5 + CurMeanRadiantTemp * 0.5;
-				HumidRatio = ZoneAirHumRat( iZone );
+				HumidRatio = ZoneAirHumRatAvgComf( iZone );
 				//for debugging
 				//ThermalComfortInASH55(iZone)%dCurAirTemp = CurAirTemp
 				//ThermalComfortInASH55(iZone)%dCurMeanRadiantTemp = CurMeanRadiantTemp
@@ -2781,7 +2781,7 @@ namespace ThermalComfort {
 			if ( IsZoneDV( ZoneNum ) || IsZoneUI( ZoneNum ) ) {
 				AirTemp = TCMF( ZoneNum );
 			} else {
-				AirTemp = ZTAV( ZoneNum );
+				AirTemp = ZTAVComf( ZoneNum );
 			}
 			RadTemp = CalcRadTemp( PeopleNum );
 			OpTemp = ( AirTemp + RadTemp ) / 2.0;
@@ -3007,7 +3007,7 @@ namespace ThermalComfort {
 			if ( IsZoneDV( ZoneNum ) || IsZoneUI( ZoneNum ) ) {
 				AirTemp = TCMF( ZoneNum );
 			} else {
-				AirTemp = ZTAV( ZoneNum );
+				AirTemp = ZTAVComf( ZoneNum );
 			}
 			RadTemp = CalcRadTemp( PeopleNum );
 			OpTemp = ( AirTemp + RadTemp ) / 2.0;
diff --git a/src/EnergyPlus/UserDefinedComponents.cc b/src/EnergyPlus/UserDefinedComponents.cc
index eb3be5b631b..1f714834263 100644
--- a/src/EnergyPlus/UserDefinedComponents.cc
+++ b/src/EnergyPlus/UserDefinedComponents.cc
@@ -232,7 +232,7 @@ namespace UserDefinedComponents {
 				CheckUserPlantCompName( CompNum ) = false;
 			}
 		}
-
+		bool anyEMSRan;
 		if ( InitLoopEquip || BeginEnvrnFlag ) {
 			InitPlantUserComponent( CompNum, LoopNum, MyLoad );
 			// find loop connection number from LoopNum and LoopSide
@@ -244,7 +244,7 @@ namespace UserDefinedComponents {
 			}
 			if ( ThisLoop > 0 ) {
 				if ( UserPlantComp( CompNum ).Loop( ThisLoop ).ErlInitProgramMngr > 0 ) {
-					ManageEMS( emsCallFromUserDefinedComponentModel, UserPlantComp( CompNum ).Loop( ThisLoop ).ErlInitProgramMngr );
+					ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, UserPlantComp( CompNum ).Loop( ThisLoop ).ErlInitProgramMngr );
 				}
 				// now interface sizing related values with rest of E+
 				MinCap = UserPlantComp( CompNum ).Loop( ThisLoop ).MinLoad;
@@ -273,12 +273,12 @@ namespace UserDefinedComponents {
 
 		if ( ThisLoop > 0 ) {
 			if ( UserPlantComp( CompNum ).Loop( ThisLoop ).ErlSimProgramMngr > 0 ) {
-				ManageEMS( emsCallFromUserDefinedComponentModel, UserPlantComp( CompNum ).Loop( ThisLoop ).ErlSimProgramMngr );
+				ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, UserPlantComp( CompNum ).Loop( ThisLoop ).ErlSimProgramMngr );
 			}
 		}
 
 		if ( UserPlantComp( CompNum ).ErlSimProgramMngr > 0 ) {
-			ManageEMS( emsCallFromUserDefinedComponentModel, UserPlantComp( CompNum ).ErlSimProgramMngr );
+			ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, UserPlantComp( CompNum ).ErlSimProgramMngr );
 		}
 
 		ReportPlantUserComponent( CompNum, ThisLoop );
@@ -360,10 +360,10 @@ namespace UserDefinedComponents {
 				CheckUserCoilName( CompNum ) = false;
 			}
 		}
-
+		bool anyEMSRan;
 		if ( BeginEnvrnFlag ) {
 			if ( UserCoil( CompNum ).ErlInitProgramMngr > 0 ) {
-				ManageEMS( emsCallFromUserDefinedComponentModel, UserCoil( CompNum ).ErlInitProgramMngr );
+				ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, UserCoil( CompNum ).ErlInitProgramMngr );
 			}
 
 			if ( UserCoil( CompNum ).PlantIsConnected ) {
@@ -378,7 +378,7 @@ namespace UserDefinedComponents {
 		InitCoilUserDefined( CompNum );
 
 		if ( UserCoil( CompNum ).ErlSimProgramMngr > 0 ) {
-			ManageEMS( emsCallFromUserDefinedComponentModel, UserCoil( CompNum ).ErlSimProgramMngr );
+			ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, UserCoil( CompNum ).ErlSimProgramMngr );
 		}
 
 		ReportCoilUserDefined( CompNum );
@@ -479,12 +479,12 @@ namespace UserDefinedComponents {
 				CheckUserZoneAirName( CompNum ) = false;
 			}
 		}
-
+		bool anyEMSRan;
 		if ( BeginEnvrnFlag ) {
 			InitZoneAirUserDefined( CompNum, ZoneNum );
 
 			if ( UserZoneAirHVAC( CompNum ).ErlInitProgramMngr > 0 ) {
-				ManageEMS( emsCallFromUserDefinedComponentModel, UserZoneAirHVAC( CompNum ).ErlInitProgramMngr );
+				ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, UserZoneAirHVAC( CompNum ).ErlInitProgramMngr );
 			}
 			if ( UserZoneAirHVAC( CompNum ).NumPlantConnections > 0 ) {
 				for ( Loop = 1; Loop <= UserZoneAirHVAC( CompNum ).NumPlantConnections; ++Loop ) {
@@ -500,7 +500,7 @@ namespace UserDefinedComponents {
 		InitZoneAirUserDefined( CompNum, ZoneNum );
 
 		if ( UserZoneAirHVAC( CompNum ).ErlSimProgramMngr > 0 ) {
-			ManageEMS( emsCallFromUserDefinedComponentModel, UserZoneAirHVAC( CompNum ).ErlSimProgramMngr );
+			ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, UserZoneAirHVAC( CompNum ).ErlSimProgramMngr );
 		}
 
 		ReportZoneAirUserDefined( CompNum );
@@ -591,12 +591,12 @@ namespace UserDefinedComponents {
 				CheckUserAirTerminal( CompNum ) = false;
 			}
 		}
-
+		bool anyEMSRan;
 		if ( BeginEnvrnFlag ) {
 			InitAirTerminalUserDefined( CompNum, ZoneNum );
 
 			if ( UserAirTerminal( CompNum ).ErlInitProgramMngr > 0 ) {
-				ManageEMS( emsCallFromUserDefinedComponentModel, UserAirTerminal( CompNum ).ErlInitProgramMngr );
+				ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, UserAirTerminal( CompNum ).ErlInitProgramMngr );
 			}
 			if ( UserAirTerminal( CompNum ).NumPlantConnections > 0 ) {
 				for ( Loop = 1; Loop <= UserAirTerminal( CompNum ).NumPlantConnections; ++Loop ) {
@@ -613,7 +613,7 @@ namespace UserDefinedComponents {
 		InitAirTerminalUserDefined( CompNum, ZoneNum );
 
 		if ( UserAirTerminal( CompNum ).ErlSimProgramMngr > 0 ) {
-			ManageEMS( emsCallFromUserDefinedComponentModel, UserAirTerminal( CompNum ).ErlSimProgramMngr );
+			ManageEMS( emsCallFromUserDefinedComponentModel, anyEMSRan, UserAirTerminal( CompNum ).ErlSimProgramMngr );
 		}
 
 		ReportAirTerminalUserDefined( CompNum );
diff --git a/src/EnergyPlus/ZoneEquipmentManager.cc b/src/EnergyPlus/ZoneEquipmentManager.cc
index 099487ad5b3..df42907c464 100644
--- a/src/EnergyPlus/ZoneEquipmentManager.cc
+++ b/src/EnergyPlus/ZoneEquipmentManager.cc
@@ -84,6 +84,7 @@
 #include <DataPrecisionGlobals.hh>
 #include <DataRoomAirModel.hh>
 #include <DataSizing.hh>
+#include <DataStringGlobals.hh>
 #include <DataSurfaces.hh>
 #include <DataZoneEnergyDemands.hh>
 #include <DataZoneEquipment.hh>
@@ -193,6 +194,7 @@ namespace ZoneEquipmentManager {
 	// These are purposefully not in the header file as an extern variable. No one outside of this should
 	// use these. They are cleared by clear_state() for use by unit tests, but normal simulations should be unaffected.
 	// This is purposefully in an anonymous namespace so nothing outside this implementation file can use it.
+		bool reportDOASZoneSizingHeader( true );
 		bool InitZoneEquipmentOneTimeFlag( true );
 		bool InitZoneEquipmentEnvrnFlag( true );
 		bool FirstPassZoneEquipFlag( true ); // indicates first pass through zone equipment, used to reset selected ZoneEqSizing variables
@@ -222,6 +224,7 @@ namespace ZoneEquipmentManager {
 		GetZoneEquipmentInputFlag = true;
 		PrioritySimOrder.deallocate();
 		FirstPassZoneEquipFlag = true;
+		reportDOASZoneSizingHeader = true;
 	}
 
 	void
@@ -1035,6 +1038,9 @@ namespace ZoneEquipmentManager {
 			ShowFatalError( "SetUpZoneSizingArrays: Errors found in Sizing:Zone input" );
 		}
 
+		// Put Auto Sizing of Sizing:Zone inputs here!
+		AutoCalcDOASControlStrategy();
+
 		ZoneSizing.allocate( TotDesDays + TotRunDesPersDays, NumOfZones );
 		FinalZoneSizing.allocate( NumOfZones );
 		CalcZoneSizing.allocate( TotDesDays + TotRunDesPersDays, NumOfZones );
@@ -2381,7 +2387,8 @@ namespace ZoneEquipmentManager {
 		} else if ( SELECT_CASE_var == EndZoneSizingCalc ) {
 
 			// candidate EMS calling point to customize CalcFinalZoneSizing
-			ManageEMS( emsCallFromZoneSizing );
+			bool anyEMSRan;
+			ManageEMS( emsCallFromZoneSizing, anyEMSRan );
 
 			// now apply EMS overrides (if any)
 
@@ -5455,6 +5462,150 @@ namespace ZoneEquipmentManager {
 		MassConservation(ZoneNum).MixingSourceMassFlowRate = ZoneSourceMassFlowRate;
 	}
 
+	void
+	AutoCalcDOASControlStrategy()
+	{
+		// SUBROUTINE INFORMATION:
+		//       AUTHOR         Fred Buhl
+		//       DATE WRITTEN   March 2016
+		//       MODIFIED       na
+		//       RE-ENGINEERED  na
+
+		// PURPOSE OF THIS Function:
+		// This subroutine does the autosizing calculations for the Sizing:Zone
+		// DOAS input.
+
+		// METHODOLOGY EMPLOYED:
+		// na
+
+		// REFERENCES:
+		// See IO Ref for suggested values
+		
+		// Using/Aliasing
+
+		// FUNCTION ARGUMENT DEFINITIONS:
+		// na
+
+		// FUNCTION PARAMETER DEFINITIONS:
+		// na
+
+		// FUNCTION LOCAL VARIABLE DECLARATIONS:
+		int ZoneSizIndex;
+		bool ErrorsFound;
+
+		ErrorsFound = false;
+		for ( ZoneSizIndex = 1; ZoneSizIndex <= NumZoneSizingInput; ++ZoneSizIndex ) {
+			if ( ZoneSizingInput( ZoneSizIndex ).AccountForDOAS ) {
+				if ( ZoneSizingInput( ZoneSizIndex ).DOASControlStrategy == DOANeutralSup ) {
+					if ( ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint == AutoSize &&
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint == AutoSize ) {
+						ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint = 21.1;
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint = 23.9;
+					} else if ( ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint == AutoSize &&
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint > 0.0 ) {
+						ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint = ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint
+							- 2.8;
+					} else if ( ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint > 0.0 &&
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint == AutoSize ) {
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint = ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint
+							+ 2.8;
+					}
+					ReportZoneSizingDOASInputs( ZoneSizingInput( ZoneSizIndex ).ZoneName, "NeutralSupplyAir",
+						ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint, ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint  );
+				} else if ( ZoneSizingInput( ZoneSizIndex ).DOASControlStrategy == DOANeutralDehumSup ) {
+					if ( ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint == AutoSize &&
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint == AutoSize ) {
+						ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint = 14.4;
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint = 22.2;
+					} else if ( ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint == AutoSize &&
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint > 0.0 ) {
+						ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint = 14.4;
+					} else if ( ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint > 0.0 &&
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint == AutoSize ) {
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint = 22.2;
+					}
+					ReportZoneSizingDOASInputs( ZoneSizingInput( ZoneSizIndex ).ZoneName, "NeutralDehumidifiedSupplyAir",
+						ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint, ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint );
+				} else if ( ZoneSizingInput( ZoneSizIndex ).DOASControlStrategy == DOACoolSup ) {
+					if ( ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint == AutoSize &&
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint == AutoSize ) {
+						ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint = 12.2;
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint = 14.4;
+					} else if ( ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint == AutoSize &&
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint > 0.0 ) {
+						ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint = ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint
+							- 2.2;
+					} else if ( ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint > 0.0 &&
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint == AutoSize ) {
+						ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint = ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint
+							+ 2.2;
+					}
+					ReportZoneSizingDOASInputs( ZoneSizingInput( ZoneSizIndex ).ZoneName, "ColdSupplyAir",
+						ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint, ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint );
+				}
+				if ( ZoneSizingInput( ZoneSizIndex ).DOASLowSetpoint > ZoneSizingInput( ZoneSizIndex ).DOASHighSetpoint ) {
+					ShowSevereError( "For Sizing:Zone = " + ZoneSizingInput( ZoneSizIndex ).ZoneName );
+					ShowContinueError( "... Dedicated Outside Air Low Setpoint for Design must be less than the High Setpoint" );
+					ErrorsFound = true;
+				}
+
+			}
+		}
+		if ( ErrorsFound ) {
+			ShowFatalError( "Errors found in DOAS sizing input. Program terminates." );
+		}
+	}
+
+	void
+	ReportZoneSizingDOASInputs(
+		std::string const & ZoneName, // the name of the zone
+		std::string const & DOASCtrlStrategy, // DOAS control strategy
+		Real64 const DOASLowTemp, // DOAS design low setpoint temperature [C]
+		Real64 const DOASHighTemp // DOAS design high setpoint temperature [C]
+		)
+	{
+
+		// SUBROUTINE INFORMATION:
+		//       AUTHOR         Fred Buhl
+		//       DATE WRITTEN   March 2016
+		//       MODIFIED       na
+		//       RE-ENGINEERED  na
+
+		// PURPOSE OF THIS SUBROUTINE:
+		// This subroutine writes the DOAS Sizing:Zone input for 1 zone to the eio file
+
+		// METHODOLOGY EMPLOYED:
+		// na
+
+		// REFERENCES:
+		// na
+
+		// Using/Aliasing
+		using namespace DataPrecisionGlobals;
+		using DataGlobals::OutputFileInits;
+		using DataStringGlobals::VerString;
+		using General::RoundSigDigits;
+
+		// Formats
+		static gio::Fmt Format_990( "('! <Zone Sizing DOAS Inputs>, Zone Name, DOAS Design Control Strategy, DOAS Design Low Setpoint Temperature {C}, DOAS Design High Setpoint Temperature {C} ')" );
+		static gio::Fmt Format_991( "(' Zone Sizing DOAS Inputs',4(', ',A))" );
+
+		if ( reportDOASZoneSizingHeader ) {
+			gio::write( OutputFileInits, Format_990 );
+			reportDOASZoneSizingHeader = false;
+		}
+
+		gio::write( OutputFileInits, Format_991 ) << ZoneName << DOASCtrlStrategy << RoundSigDigits( DOASLowTemp, 3 ) << RoundSigDigits( DOASHighTemp, 3 );
+
+		// BSLLC Start
+		// if ( sqlite ) {
+		// 	sqlite->addSQLiteZoneSizingRecord( ZoneName, LoadType, CalcDesLoad, UserDesLoad, CalcDesFlow, UserDesFlow, DesDayName, PeakHrMin, 
+		// 		PeakTemp, PeakHumRat, MinOAVolFlow, DOASHeatAddRate );
+		// }
+		// BSLLC Finish
+
+	}
+
 } // ZoneEquipmentManager
 
 } // EnergyPlus
diff --git a/src/EnergyPlus/ZoneEquipmentManager.hh b/src/EnergyPlus/ZoneEquipmentManager.hh
index beceb8af34c..a7024665487 100644
--- a/src/EnergyPlus/ZoneEquipmentManager.hh
+++ b/src/EnergyPlus/ZoneEquipmentManager.hh
@@ -213,6 +213,17 @@ namespace ZoneEquipmentManager {
 		Real64 & DOASSupHR // DOAS Supply Humidity ratio [kg Water / kg Dry Air]
 	);
 
+	void
+	AutoCalcDOASControlStrategy();
+
+	void
+	ReportZoneSizingDOASInputs(
+		std::string const & ZoneName, // the name of the zone
+		std::string const & DOASCtrlStrategy, // DOAS control strategy
+		Real64 const DOASLowTemp, // DOAS design low setpoint temperature [C]
+		Real64 const DOASHighTemp // DOAS design high setpoint temperature [C]
+	);
+
 } // ZoneEquipmentManager
 
 } // EnergyPlus
diff --git a/src/Transition/CreateNewIDFUsingRulesV8_3_0.f90 b/src/Transition/CreateNewIDFUsingRulesV8_3_0.f90
index 5a874b989ec..01437a568cb 100644
--- a/src/Transition/CreateNewIDFUsingRulesV8_3_0.f90
+++ b/src/Transition/CreateNewIDFUsingRulesV8_3_0.f90
@@ -378,7 +378,9 @@ SUBROUTINE CreateNewIDFUsingRules(EndOfFile,DiffOnly,InLfn,AskForInput,InputFile
                 ! Remove Max flow rate field
                 nodiff=.false.
                 CALL GetNewObjectDefInIDD(ObjectName,NwNUmArgs,NwAorN,NwReqFld,NwObjMinFlds,NwFldNames,NwFldDefaults,NwFldUnits)
-                OutArgs(1:10) = InArgs(1:10)
+                OutArgs(1:3) = InArgs(1:3)
+                OutArgs(4) = InArgs(11) 
+                OutArgs(5:10) = InArgs(5:10)
                 OutArgs(11:CurArgs-1) = InArgs(12:CurArgs)
                 CurArgs = CurArgs - 1
 
diff --git a/src/Transition/CreateNewIDFUsingRulesV8_5_0.f90 b/src/Transition/CreateNewIDFUsingRulesV8_5_0.f90
index 7fc62766250..fc0d2a03724 100644
--- a/src/Transition/CreateNewIDFUsingRulesV8_5_0.f90
+++ b/src/Transition/CreateNewIDFUsingRulesV8_5_0.f90
@@ -369,6 +369,8 @@ SUBROUTINE CreateNewIDFUsingRules(EndOfFile,DiffOnly,InLfn,AskForInput,InputFile
               ! So for now I'll just change them on a version by version basis.
               CASE ('ENERGYMANAGEMENTSYSTEM:ACTUATOR')
                 CALL GetNewObjectDefInIDD(ObjectName,NwNumArgs,NwAorN,NwReqFld,NwObjMinFlds,NwFldNames,NwFldDefaults,NwFldUnits)
+                OutArgs(1:CurArgs)=InArgs(1:CurArgs)
+                nodiff=.true.
                 SELECT CASE ( MakeUPPERCase ( InArgs(4) ) )
                 CASE ('OUTDOOR AIR DRYBLUB TEMPERATURE')
 				  nodiff = .true.
diff --git a/src/Transition/InputRulesFiles/Rules8-4-0-to-8-5-0.xls b/src/Transition/InputRulesFiles/Rules8-4-0-to-8-5-0.xls
index fdba2ee292f..bdd699c4af3 100644
Binary files a/src/Transition/InputRulesFiles/Rules8-4-0-to-8-5-0.xls and b/src/Transition/InputRulesFiles/Rules8-4-0-to-8-5-0.xls differ
diff --git a/testfiles/5ZoneWLHPPlantLoopTower.idf b/testfiles/5ZoneWLHPPlantLoopTower.idf
index 65daadbf67b..72f7f3d0cc3 100644
--- a/testfiles/5ZoneWLHPPlantLoopTower.idf
+++ b/testfiles/5ZoneWLHPPlantLoopTower.idf
@@ -21,7 +21,7 @@
 !
 ! Run Period (Weather File): Winter 1/14, Summer 7/7, CHICAGO_IL_USA TMY2-94846
 !
-! Run Control:             Zone and System sizing with design day simulations (design days run)
+! Run Control:             Design day simulations (design days run)
 !
 ! Building: Single floor rectangular building 100 ft x 50 ft. 5 zones - 4 exterior, 1 interior, zone height 8 feet.
 !           Exterior zone depth is 12 feet. There is a 2 foot high return plenum: the overall building height is
@@ -87,7 +87,7 @@
 !
 ! Zonal Equipment:                Water Loop Heat PUmp
 ! Central Air Handling Equipment: Yes
-! System Equipment Autosize:      Yes
+! System Equipment Autosize:      No
 ! Purchased Cooling:              None
 ! Purchased Heating:              None
 ! Coils:                          COIL:WATERTOAIRHP:PARAMETERESTIMATION:COOLING, COIL:WATERTOAIRHP:PARAMETERESTIMATION:HEATING
@@ -204,9 +204,9 @@
     190.00;                  !- Elevation {m}
 
   SimulationControl,
-    Yes,                     !- Do Zone Sizing Calculation
-    Yes,                     !- Do System Sizing Calculation
-    Yes,                     !- Do Plant Sizing Calculation
+    No,                      !- Do Zone Sizing Calculation
+    No,                      !- Do System Sizing Calculation
+    No,                      !- Do Plant Sizing Calculation
     Yes,                     !- Run Simulation for Sizing Periods
     No;                      !- Run Simulation for Weather File Run Periods
 
@@ -1067,7 +1067,7 @@
     1584,                    !- Lighting Level {W}
     ,                        !- Watts per Zone Floor Area {W/m2}
     ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
+    ,                        !- Return Air Fraction
     0.59,                    !- Fraction Radiant
     0.2,                     !- Fraction Visible
     0,                       !- Fraction Replaceable
@@ -1278,7 +1278,7 @@
     684,                     !- Lighting Level {W}
     ,                        !- Watts per Zone Floor Area {W/m2}
     ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
+    ,                        !- Return Air Fraction
     0.59,                    !- Fraction Radiant
     0.2,                     !- Fraction Visible
     0,                       !- Fraction Replaceable
@@ -1453,7 +1453,7 @@
     1584,                    !- Lighting Level {W}
     ,                        !- Watts per Zone Floor Area {W/m2}
     ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
+    ,                        !- Return Air Fraction
     0.59,                    !- Fraction Radiant
     0.2,                     !- Fraction Visible
     0,                       !- Fraction Replaceable
@@ -1644,7 +1644,7 @@
     684,                     !- Lighting Level {W}
     ,                        !- Watts per Zone Floor Area {W/m2}
     ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
+    ,                        !- Return Air Fraction
     0.59,                    !- Fraction Radiant
     0.2,                     !- Fraction Visible
     0,                       !- Fraction Replaceable
@@ -1819,7 +1819,7 @@
     2964,                    !- Lighting Level {W}
     ,                        !- Watts per Zone Floor Area {W/m2}
     ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
+    ,                        !- Return Air Fraction
     0.59,                    !- Fraction Radiant
     0.2,                     !- Fraction Visible
     0,                       !- Fraction Replaceable
@@ -1933,23 +1933,6 @@
     3.7,3.7,0.0,  !- X,Y,Z ==> Vertex 3 {m}
     3.7,3.7,2.4;  !- X,Y,Z ==> Vertex 4 {m}
 
-  Sizing:Parameters,
-    1.3,                     !- Heating Sizing Factor
-    1.3,                     !- Cooling Sizing Factor
-    ;                        !- Timesteps in Averaging Window
-
-  Sizing:Plant,
-    Hot Water Loop,          !- Plant or Condenser Loop Name
-    heating,                 !- Loop Type
-    82.,                     !- Design Loop Exit Temperature {C}
-    11;                      !- Loop Design Temperature Difference {deltaC}
-
-  Sizing:Plant,
-    Chilled Water Loop,      !- Plant or Condenser Loop Name
-    cooling,                 !- Loop Type
-    7.22,                    !- Design Loop Exit Temperature {C}
-    6.67;                    !- Loop Design Temperature Difference {deltaC}
-
   ZoneControl:Thermostat,
     SPACE1-1 Control,        !- Name
     SPACE1-1,                !- Zone or ZoneList Name
@@ -2029,37 +2012,6 @@
 !*********************************************************************************************************************************************************
 ! HP Air Loop #1
 
-  Sizing:Zone,
-    SPACE1-1,                !- Zone or ZoneList Name
-    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method
-    14.,                     !- Zone Cooling Design Supply Air Temperature {C}
-    ,                        !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
-    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method
-    50.,                     !- Zone Heating Design Supply Air Temperature {C}
-    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    SZ DSOA SPACE1-1,        !- Design Specification Outdoor Air Object Name
-    0.0,                     !- Zone Heating Sizing Factor
-    0.0,                     !- Zone Cooling Sizing Factor
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- Cooling Minimum Air Flow Fraction
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Heating Maximum Air Flow {m3/s}
-    ;                        !- Heating Maximum Air Flow Fraction
-
-  DesignSpecification:OutdoorAir,
-    SZ DSOA SPACE1-1,        !- Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}
-    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0;                     !- Outdoor Air Flow per Zone {m3/s}
-
   ZoneHVAC:EquipmentConnections,
     SPACE1-1,                !- Zone Name
     SPACE1-1 Equipment,      !- Zone Conditioning Equipment List Name
@@ -2083,52 +2035,13 @@
     SPACE1-1 Direct Air,     !- Name
     FanAvailSched,           !- Availability Schedule Name
     SPACE1-1 Supply Inlet,   !- Zone Supply Air Node Name
-    autosize;                !- Maximum Air Flow Rate {m3/s}
-
-  Sizing:System,
-    AHU 1,                   !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    0.0,                     !- Design Outdoor Air Flow Rate {m3/s}
-    1.0,                     !- Central Heating Maximum System Air Flow Ratio
-    7.0,                     !- Preheat Design Temperature {C}
-    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.,                     !- Central Cooling Design Supply Air Temperature {C}
-    50.,                     !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Type of Zone Sum to Use
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Cooling Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Heating Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Heating Supply Air Flow Rate
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ,                        !- System Outdoor Air Method
-    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Heating Design Capacity
-    VAV;                     !- Central Cooling Capacity Control Method
+    2.0;                     !- Maximum Air Flow Rate {m3/s}
 
   AirLoopHVAC,
     AHU 1,                   !- Name
     ,                        !- Controller List Name
     AHU 1 Availability Managers,  !- Availability Manager List Name
-    autosize,                !- Design Supply Air Flow Rate {m3/s}
+    2.0,                     !- Design Supply Air Flow Rate {m3/s}
     AHU 1 Branches,          !- Branch List Name
     ,                        !- Connector List Name
     AHU 1 Air Loop Inlet,    !- Supply Side Inlet Node Name
@@ -2257,7 +2170,7 @@
     R22,                     !- Refrigerant Type
     0.0015,                  !- Design Source Side Flow Rate {m3/s}
     38000,                   !- Gross Rated Heating Capacity {W}
-    4000000,                 !- High Pressure Cutoff
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU1 Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
     AHU1 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
@@ -2287,37 +2200,6 @@
 
 ! HP Air Loop #2
 
-  Sizing:Zone,
-    SPACE2-1,                !- Zone or ZoneList Name
-    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method
-    14.,                     !- Zone Cooling Design Supply Air Temperature {C}
-    ,                        !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
-    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method
-    50.,                     !- Zone Heating Design Supply Air Temperature {C}
-    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    SZ DSOA SPACE2-1,        !- Design Specification Outdoor Air Object Name
-    0.0,                     !- Zone Heating Sizing Factor
-    0.0,                     !- Zone Cooling Sizing Factor
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- Cooling Minimum Air Flow Fraction
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Heating Maximum Air Flow {m3/s}
-    ;                        !- Heating Maximum Air Flow Fraction
-
-  DesignSpecification:OutdoorAir,
-    SZ DSOA SPACE2-1,        !- Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}
-    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0;                     !- Outdoor Air Flow per Zone {m3/s}
-
   ZoneHVAC:EquipmentConnections,
     SPACE2-1,                !- Zone Name
     SPACE2-1 Equipment,      !- Zone Conditioning Equipment List Name
@@ -2341,52 +2223,13 @@
     SPACE2-1 Direct Air,     !- Name
     FanAvailSched,           !- Availability Schedule Name
     SPACE2-1 Supply Inlet,   !- Zone Supply Air Node Name
-    autosize;                !- Maximum Air Flow Rate {m3/s}
-
-  Sizing:System,
-    AHU 2,                   !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    0.0,                     !- Design Outdoor Air Flow Rate {m3/s}
-    1.0,                     !- Central Heating Maximum System Air Flow Ratio
-    7.0,                     !- Preheat Design Temperature {C}
-    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.,                     !- Central Cooling Design Supply Air Temperature {C}
-    50.,                     !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Type of Zone Sum to Use
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Cooling Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Heating Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Heating Supply Air Flow Rate
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ,                        !- System Outdoor Air Method
-    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Heating Design Capacity
-    VAV;                     !- Central Cooling Capacity Control Method
+    2.0;                     !- Maximum Air Flow Rate {m3/s}
 
   AirLoopHVAC,
     AHU 2,                   !- Name
     ,                        !- Controller List Name
     AHU 2 Availability Managers,  !- Availability Manager List Name
-    autosize,                !- Design Supply Air Flow Rate {m3/s}
+    2.0,                     !- Design Supply Air Flow Rate {m3/s}
     AHU 2 Branches,          !- Branch List Name
     ,                        !- Connector List Name
     AHU 2 Air Loop Inlet,    !- Supply Side Inlet Node Name
@@ -2512,7 +2355,7 @@
     R22,                     !- Refrigerant Type
     0.0015,                  !- Design Source Side Flow Rate {m3/s}
     38000,                   !- Gross Rated Heating Capacity {W}
-    4000000,                 !- High Pressure Cutoff
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU2 Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
     AHU2 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
@@ -2542,37 +2385,6 @@
 
 ! HP Air Loop #3
 
-  Sizing:Zone,
-    SPACE3-1,                !- Zone or ZoneList Name
-    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method
-    14.,                     !- Zone Cooling Design Supply Air Temperature {C}
-    ,                        !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
-    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method
-    50.,                     !- Zone Heating Design Supply Air Temperature {C}
-    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    SZ DSOA SPACE3-1,        !- Design Specification Outdoor Air Object Name
-    0.0,                     !- Zone Heating Sizing Factor
-    0.0,                     !- Zone Cooling Sizing Factor
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- Cooling Minimum Air Flow Fraction
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Heating Maximum Air Flow {m3/s}
-    ;                        !- Heating Maximum Air Flow Fraction
-
-  DesignSpecification:OutdoorAir,
-    SZ DSOA SPACE3-1,        !- Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}
-    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0;                     !- Outdoor Air Flow per Zone {m3/s}
-
   ZoneHVAC:EquipmentConnections,
     SPACE3-1,                !- Zone Name
     SPACE3-1 Equipment,      !- Zone Conditioning Equipment List Name
@@ -2596,52 +2408,13 @@
     SPACE3-1 Direct Air,     !- Name
     FanAvailSched,           !- Availability Schedule Name
     SPACE3-1 Supply Inlet,   !- Zone Supply Air Node Name
-    autosize;                !- Maximum Air Flow Rate {m3/s}
-
-  Sizing:System,
-    AHU 3,                   !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    0.0,                     !- Design Outdoor Air Flow Rate {m3/s}
-    1.0,                     !- Central Heating Maximum System Air Flow Ratio
-    7.0,                     !- Preheat Design Temperature {C}
-    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.,                     !- Central Cooling Design Supply Air Temperature {C}
-    50.,                     !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Type of Zone Sum to Use
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Cooling Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Heating Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Heating Supply Air Flow Rate
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ,                        !- System Outdoor Air Method
-    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Heating Design Capacity
-    VAV;                     !- Central Cooling Capacity Control Method
+    2.0;                     !- Maximum Air Flow Rate {m3/s}
 
   AirLoopHVAC,
     AHU 3,                   !- Name
     ,                        !- Controller List Name
     AHU 3 Availability Managers,  !- Availability Manager List Name
-    autosize,                !- Design Supply Air Flow Rate {m3/s}
+    2.0,                     !- Design Supply Air Flow Rate {m3/s}
     AHU 3 Branches,          !- Branch List Name
     ,                        !- Connector List Name
     AHU 3 Air Loop Inlet,    !- Supply Side Inlet Node Name
@@ -2767,7 +2540,7 @@
     R22,                     !- Refrigerant Type
     0.0015,                  !- Design Source Side Flow Rate {m3/s}
     38000,                   !- Gross Rated Heating Capacity {W}
-    4000000,                 !- High Pressure Cutoff
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU3 Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
     AHU3 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
@@ -2797,37 +2570,6 @@
 
 ! HP Air Loop #4
 
-  Sizing:Zone,
-    SPACE4-1,                !- Zone or ZoneList Name
-    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method
-    14.,                     !- Zone Cooling Design Supply Air Temperature {C}
-    ,                        !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
-    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method
-    50.,                     !- Zone Heating Design Supply Air Temperature {C}
-    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    SZ DSOA SPACE4-1,        !- Design Specification Outdoor Air Object Name
-    0.0,                     !- Zone Heating Sizing Factor
-    0.0,                     !- Zone Cooling Sizing Factor
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- Cooling Minimum Air Flow Fraction
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Heating Maximum Air Flow {m3/s}
-    ;                        !- Heating Maximum Air Flow Fraction
-
-  DesignSpecification:OutdoorAir,
-    SZ DSOA SPACE4-1,        !- Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}
-    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0;                     !- Outdoor Air Flow per Zone {m3/s}
-
   ZoneHVAC:EquipmentConnections,
     SPACE4-1,                !- Zone Name
     SPACE4-1 Equipment,      !- Zone Conditioning Equipment List Name
@@ -2851,52 +2593,13 @@
     SPACE4-1 Direct Air,     !- Name
     FanAvailSched,           !- Availability Schedule Name
     SPACE4-1 Supply Inlet,   !- Zone Supply Air Node Name
-    autosize;                !- Maximum Air Flow Rate {m3/s}
-
-  Sizing:System,
-    AHU 4,                   !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    0.0,                     !- Design Outdoor Air Flow Rate {m3/s}
-    1.0,                     !- Central Heating Maximum System Air Flow Ratio
-    7.0,                     !- Preheat Design Temperature {C}
-    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.,                     !- Central Cooling Design Supply Air Temperature {C}
-    50.,                     !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Type of Zone Sum to Use
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Cooling Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Heating Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Heating Supply Air Flow Rate
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ,                        !- System Outdoor Air Method
-    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Heating Design Capacity
-    VAV;                     !- Central Cooling Capacity Control Method
+    2.0;                     !- Maximum Air Flow Rate {m3/s}
 
   AirLoopHVAC,
     AHU 4,                   !- Name
     ,                        !- Controller List Name
     AHU 4 Availability Managers,  !- Availability Manager List Name
-    autosize,                !- Design Supply Air Flow Rate {m3/s}
+    2.0,                     !- Design Supply Air Flow Rate {m3/s}
     AHU 4 Branches,          !- Branch List Name
     ,                        !- Connector List Name
     AHU 4 Air Loop Inlet,    !- Supply Side Inlet Node Name
@@ -3022,7 +2725,7 @@
     R22,                     !- Refrigerant Type
     0.0015,                  !- Design Source Side Flow Rate {m3/s}
     38000,                   !- Gross Rated Heating Capacity {W}
-    4000000,                 !- High Pressure Cutoff
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU4 Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
     AHU4 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
@@ -3052,37 +2755,6 @@
 
 ! HP Air Loop #5
 
-  Sizing:Zone,
-    SPACE5-1,                !- Zone or ZoneList Name
-    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method
-    14.,                     !- Zone Cooling Design Supply Air Temperature {C}
-    ,                        !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
-    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method
-    50.,                     !- Zone Heating Design Supply Air Temperature {C}
-    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    SZ DSOA SPACE5-1,        !- Design Specification Outdoor Air Object Name
-    0.0,                     !- Zone Heating Sizing Factor
-    0.0,                     !- Zone Cooling Sizing Factor
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- Cooling Minimum Air Flow Fraction
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Heating Maximum Air Flow {m3/s}
-    ;                        !- Heating Maximum Air Flow Fraction
-
-  DesignSpecification:OutdoorAir,
-    SZ DSOA SPACE5-1,        !- Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}
-    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0;                     !- Outdoor Air Flow per Zone {m3/s}
-
   ZoneHVAC:EquipmentConnections,
     SPACE5-1,                !- Zone Name
     SPACE5-1 Equipment,      !- Zone Conditioning Equipment List Name
@@ -3106,52 +2778,13 @@
     SPACE5-1 Direct Air,     !- Name
     FanAvailSched,           !- Availability Schedule Name
     SPACE5-1 Supply Inlet,   !- Zone Supply Air Node Name
-    autosize;                !- Maximum Air Flow Rate {m3/s}
-
-  Sizing:System,
-    AHU 5,                   !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    0.0,                     !- Design Outdoor Air Flow Rate {m3/s}
-    1.0,                     !- Central Heating Maximum System Air Flow Ratio
-    7.0,                     !- Preheat Design Temperature {C}
-    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.,                     !- Central Cooling Design Supply Air Temperature {C}
-    50.,                     !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Type of Zone Sum to Use
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Cooling Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Heating Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Heating Supply Air Flow Rate
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ,                        !- System Outdoor Air Method
-    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Heating Design Capacity
-    VAV;                     !- Central Cooling Capacity Control Method
+    2.0;                     !- Maximum Air Flow Rate {m3/s}
 
   AirLoopHVAC,
     AHU 5,                   !- Name
     ,                        !- Controller List Name
     AHU 5 Availability Managers,  !- Availability Manager List Name
-    autosize,                !- Design Supply Air Flow Rate {m3/s}
+    2.0,                     !- Design Supply Air Flow Rate {m3/s}
     AHU 5 Branches,          !- Branch List Name
     ,                        !- Connector List Name
     AHU 5 Air Loop Inlet,    !- Supply Side Inlet Node Name
@@ -3277,7 +2910,7 @@
     R22,                     !- Refrigerant Type
     0.0015,                  !- Design Source Side Flow Rate {m3/s}
     38000,                   !- Gross Rated Heating Capacity {W}
-    4000000,                 !- High Pressure Cutoff
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU5 Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
     AHU5 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
diff --git a/testfiles/5ZoneWaterLoopHeatPump.idf b/testfiles/5ZoneWaterLoopHeatPump.idf
index 2886f8f159d..94ef97b3594 100644
--- a/testfiles/5ZoneWaterLoopHeatPump.idf
+++ b/testfiles/5ZoneWaterLoopHeatPump.idf
@@ -21,7 +21,7 @@
 !
 ! Run Period (Weather File): Winter 1/14, Summer 7/7, CHICAGO_IL_USA TMY2-94846
 !
-! Run Control:             Zone and System sizing with design day simulations (design days run)
+! Run Control:             Design day simulations (design days run)
 !
 ! Building: Single floor rectangular building 100 ft x 50 ft. 5 zones - 4 exterior, 1 interior, zone height 8 feet.
 !           Exterior zone depth is 12 feet. There is a 2 foot high return plenum: the overall building height is
@@ -87,7 +87,7 @@
 !
 ! Zonal Equipment:                Water Loop Heat PUmp
 ! Central Air Handling Equipment: Yes
-! System Equipment Autosize:      Yes
+! System Equipment Autosize:      No
 ! Purchased Cooling:              None
 ! Purchased Heating:              None
 ! Coils:                          COIL:WATERTOAIRHP:COOLING, COIL:WATERTOAIRHP:HEATING
@@ -198,9 +198,9 @@
     190.00;                  !- Elevation {m}
 
   SimulationControl,
-    Yes,                     !- Do Zone Sizing Calculation
-    Yes,                     !- Do System Sizing Calculation
-    Yes,                     !- Do Plant Sizing Calculation
+    No,                      !- Do Zone Sizing Calculation
+    No,                      !- Do System Sizing Calculation
+    No,                      !- Do Plant Sizing Calculation
     Yes,                     !- Run Simulation for Sizing Periods
     No;                      !- Run Simulation for Weather File Run Periods
 
@@ -775,7 +775,7 @@
     1584,                    !- Lighting Level {W}
     ,                        !- Watts per Zone Floor Area {W/m2}
     ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
+    ,                        !- Return Air Fraction
     0.59,                    !- Fraction Radiant
     0.2,                     !- Fraction Visible
     0,                       !- Fraction Replaceable
@@ -986,7 +986,7 @@
     684,                     !- Lighting Level {W}
     ,                        !- Watts per Zone Floor Area {W/m2}
     ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
+    ,                        !- Return Air Fraction
     0.59,                    !- Fraction Radiant
     0.2,                     !- Fraction Visible
     0,                       !- Fraction Replaceable
@@ -1161,7 +1161,7 @@
     1584,                    !- Lighting Level {W}
     ,                        !- Watts per Zone Floor Area {W/m2}
     ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
+    ,                        !- Return Air Fraction
     0.59,                    !- Fraction Radiant
     0.2,                     !- Fraction Visible
     0,                       !- Fraction Replaceable
@@ -1352,7 +1352,7 @@
     684,                     !- Lighting Level {W}
     ,                        !- Watts per Zone Floor Area {W/m2}
     ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
+    ,                        !- Return Air Fraction
     0.59,                    !- Fraction Radiant
     0.2,                     !- Fraction Visible
     0,                       !- Fraction Replaceable
@@ -1527,7 +1527,7 @@
     2964,                    !- Lighting Level {W}
     ,                        !- Watts per Zone Floor Area {W/m2}
     ,                        !- Watts per Person {W/person}
-    0.2,                     !- Return Air Fraction
+    ,                        !- Return Air Fraction
     0.59,                    !- Fraction Radiant
     0.2,                     !- Fraction Visible
     0,                       !- Fraction Replaceable
@@ -1641,23 +1641,6 @@
     3.7,3.7,0.0,  !- X,Y,Z ==> Vertex 3 {m}
     3.7,3.7,2.4;  !- X,Y,Z ==> Vertex 4 {m}
 
-  Sizing:Parameters,
-    1.3,                     !- Heating Sizing Factor
-    1.3,                     !- Cooling Sizing Factor
-    ;                        !- Timesteps in Averaging Window
-
-  Sizing:Plant,
-    Hot Water Loop,          !- Plant or Condenser Loop Name
-    heating,                 !- Loop Type
-    82.,                     !- Design Loop Exit Temperature {C}
-    11;                      !- Loop Design Temperature Difference {deltaC}
-
-  Sizing:Plant,
-    Chilled Water Loop,      !- Plant or Condenser Loop Name
-    cooling,                 !- Loop Type
-    7.22,                    !- Design Loop Exit Temperature {C}
-    6.67;                    !- Loop Design Temperature Difference {deltaC}
-
   Schedule:Compact,
     OCCUPY-1,                !- Name
     FRACTION,                !- Schedule Type Limits Name
@@ -1943,37 +1926,6 @@
 !*********************************************************************************************************************************************************
 ! HP Air Loop #1
 
-  Sizing:Zone,
-    SPACE1-1,                !- Zone or ZoneList Name
-    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method
-    14.,                     !- Zone Cooling Design Supply Air Temperature {C}
-    ,                        !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
-    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method
-    50.,                     !- Zone Heating Design Supply Air Temperature {C}
-    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    SZ DSOA SPACE1-1,        !- Design Specification Outdoor Air Object Name
-    0.0,                     !- Zone Heating Sizing Factor
-    0.0,                     !- Zone Cooling Sizing Factor
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- Cooling Minimum Air Flow Fraction
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Heating Maximum Air Flow {m3/s}
-    ;                        !- Heating Maximum Air Flow Fraction
-
-  DesignSpecification:OutdoorAir,
-    SZ DSOA SPACE1-1,        !- Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}
-    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0;                     !- Outdoor Air Flow per Zone {m3/s}
-
   ZoneHVAC:EquipmentConnections,
     SPACE1-1,                !- Zone Name
     SPACE1-1 Equipment,      !- Zone Conditioning Equipment List Name
@@ -1997,52 +1949,13 @@
     SPACE1-1 Direct Air,     !- Name
     FanAvailSched,           !- Availability Schedule Name
     SPACE1-1 Supply Inlet,   !- Zone Supply Air Node Name
-    autosize;                !- Maximum Air Flow Rate {m3/s}
-
-  Sizing:System,
-    AHU 1,                   !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    0.0,                     !- Design Outdoor Air Flow Rate {m3/s}
-    1.0,                     !- Central Heating Maximum System Air Flow Ratio
-    7.0,                     !- Preheat Design Temperature {C}
-    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.,                     !- Central Cooling Design Supply Air Temperature {C}
-    50.,                     !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Type of Zone Sum to Use
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Cooling Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Heating Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Heating Supply Air Flow Rate
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ,                        !- System Outdoor Air Method
-    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Heating Design Capacity
-    VAV;                     !- Central Cooling Capacity Control Method
+    2.0;                     !- Maximum Air Flow Rate {m3/s}
 
   AirLoopHVAC,
     AHU 1,                   !- Name
     ,                        !- Controller List Name
     AHU 1 Availability Managers,  !- Availability Manager List Name
-    autosize,                !- Design Supply Air Flow Rate {m3/s}
+    2.0,                     !- Design Supply Air Flow Rate {m3/s}
     AHU 1 Branches,          !- Branch List Name
     ,                        !- Connector List Name
     AHU 1 Air Loop Inlet,    !- Supply Side Inlet Node Name
@@ -2144,7 +2057,7 @@
     38000,                   !- Nominal Cooling Coil Capacity {W}
     0,                       !- Nominal Time for Condensate Removal to Begin {s}
     0,                       !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
-    3000000,                 !- High Pressure Cutoff {Pa}
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU1 Water to Air Heat Pump Source Side1 Inlet Node,  !- Water Inlet Node Name
     AHU1 Water to Air Heat Pump Source Side1 Outlet Node,  !- Water Outlet Node Name
@@ -2171,7 +2084,7 @@
     R22,                     !- Refrigerant Type
     0.0015,                  !- Design Source Side Flow Rate {m3/s}
     38000,                   !- Gross Rated Heating Capacity {W}
-    3000000,                 !- High Pressure Cutoff
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU1 Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
     AHU1 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
@@ -2201,37 +2114,6 @@
 
 ! HP Air Loop #2
 
-  Sizing:Zone,
-    SPACE2-1,                !- Zone or ZoneList Name
-    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method
-    14.,                     !- Zone Cooling Design Supply Air Temperature {C}
-    ,                        !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
-    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method
-    50.,                     !- Zone Heating Design Supply Air Temperature {C}
-    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    SZ DSOA SPACE2-1,        !- Design Specification Outdoor Air Object Name
-    0.0,                     !- Zone Heating Sizing Factor
-    0.0,                     !- Zone Cooling Sizing Factor
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- Cooling Minimum Air Flow Fraction
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Heating Maximum Air Flow {m3/s}
-    ;                        !- Heating Maximum Air Flow Fraction
-
-  DesignSpecification:OutdoorAir,
-    SZ DSOA SPACE2-1,        !- Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}
-    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0;                     !- Outdoor Air Flow per Zone {m3/s}
-
   ZoneHVAC:EquipmentConnections,
     SPACE2-1,                !- Zone Name
     SPACE2-1 Equipment,      !- Zone Conditioning Equipment List Name
@@ -2255,52 +2137,13 @@
     SPACE2-1 Direct Air,     !- Name
     FanAvailSched,           !- Availability Schedule Name
     SPACE2-1 Supply Inlet,   !- Zone Supply Air Node Name
-    autosize;                !- Maximum Air Flow Rate {m3/s}
-
-  Sizing:System,
-    AHU 2,                   !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    0.0,                     !- Design Outdoor Air Flow Rate {m3/s}
-    1.0,                     !- Central Heating Maximum System Air Flow Ratio
-    7.0,                     !- Preheat Design Temperature {C}
-    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.,                     !- Central Cooling Design Supply Air Temperature {C}
-    50.,                     !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Type of Zone Sum to Use
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Cooling Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Heating Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Heating Supply Air Flow Rate
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ,                        !- System Outdoor Air Method
-    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Heating Design Capacity
-    VAV;                     !- Central Cooling Capacity Control Method
+    2.0;                     !- Maximum Air Flow Rate {m3/s}
 
   AirLoopHVAC,
     AHU 2,                   !- Name
     ,                        !- Controller List Name
     AHU 2 Availability Managers,  !- Availability Manager List Name
-    autosize,                !- Design Supply Air Flow Rate {m3/s}
+    2.0,                     !- Design Supply Air Flow Rate {m3/s}
     AHU 2 Branches,          !- Branch List Name
     ,                        !- Connector List Name
     AHU 2 Air Loop Inlet,    !- Supply Side Inlet Node Name
@@ -2399,7 +2242,7 @@
     38000,                   !- Nominal Cooling Coil Capacity {W}
     0,                       !- Nominal Time for Condensate Removal to Begin {s}
     0,                       !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
-    3000000,                 !- High Pressure Cutoff {Pa}
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU2 Water to Air Heat Pump Source Side1 Inlet Node,  !- Water Inlet Node Name
     AHU2 Water to Air Heat Pump Source Side1 Outlet Node,  !- Water Outlet Node Name
@@ -2426,7 +2269,7 @@
     R22,                     !- Refrigerant Type
     0.0015,                  !- Design Source Side Flow Rate {m3/s}
     38000,                   !- Gross Rated Heating Capacity {W}
-    3000000,                 !- High Pressure Cutoff
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU2 Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
     AHU2 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
@@ -2456,37 +2299,6 @@
 
 ! HP Air Loop #3
 
-  Sizing:Zone,
-    SPACE3-1,                !- Zone or ZoneList Name
-    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method
-    14.,                     !- Zone Cooling Design Supply Air Temperature {C}
-    ,                        !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
-    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method
-    50.,                     !- Zone Heating Design Supply Air Temperature {C}
-    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    SZ DSOA SPACE3-1,        !- Design Specification Outdoor Air Object Name
-    0.0,                     !- Zone Heating Sizing Factor
-    0.0,                     !- Zone Cooling Sizing Factor
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- Cooling Minimum Air Flow Fraction
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Heating Maximum Air Flow {m3/s}
-    ;                        !- Heating Maximum Air Flow Fraction
-
-  DesignSpecification:OutdoorAir,
-    SZ DSOA SPACE3-1,        !- Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}
-    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0;                     !- Outdoor Air Flow per Zone {m3/s}
-
   ZoneHVAC:EquipmentConnections,
     SPACE3-1,                !- Zone Name
     SPACE3-1 Equipment,      !- Zone Conditioning Equipment List Name
@@ -2510,52 +2322,13 @@
     SPACE3-1 Direct Air,     !- Name
     FanAvailSched,           !- Availability Schedule Name
     SPACE3-1 Supply Inlet,   !- Zone Supply Air Node Name
-    autosize;                !- Maximum Air Flow Rate {m3/s}
-
-  Sizing:System,
-    AHU 3,                   !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    0.0,                     !- Design Outdoor Air Flow Rate {m3/s}
-    1.0,                     !- Central Heating Maximum System Air Flow Ratio
-    7.0,                     !- Preheat Design Temperature {C}
-    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.,                     !- Central Cooling Design Supply Air Temperature {C}
-    50.,                     !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Type of Zone Sum to Use
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Cooling Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Heating Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Heating Supply Air Flow Rate
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ,                        !- System Outdoor Air Method
-    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Heating Design Capacity
-    VAV;                     !- Central Cooling Capacity Control Method
+    2.0;                     !- Maximum Air Flow Rate {m3/s}
 
   AirLoopHVAC,
     AHU 3,                   !- Name
     ,                        !- Controller List Name
     AHU 3 Availability Managers,  !- Availability Manager List Name
-    autosize,                !- Design Supply Air Flow Rate {m3/s}
+    2.0,                     !- Design Supply Air Flow Rate {m3/s}
     AHU 3 Branches,          !- Branch List Name
     ,                        !- Connector List Name
     AHU 3 Air Loop Inlet,    !- Supply Side Inlet Node Name
@@ -2654,7 +2427,7 @@
     38000,                   !- Nominal Cooling Coil Capacity {W}
     0,                       !- Nominal Time for Condensate Removal to Begin {s}
     0,                       !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
-    3000000,                 !- High Pressure Cutoff {Pa}
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU3 Water to Air Heat Pump Source Side1 Inlet Node,  !- Water Inlet Node Name
     AHU3 Water to Air Heat Pump Source Side1 Outlet Node,  !- Water Outlet Node Name
@@ -2681,7 +2454,7 @@
     R22,                     !- Refrigerant Type
     0.0015,                  !- Design Source Side Flow Rate {m3/s}
     38000,                   !- Gross Rated Heating Capacity {W}
-    3000000,                 !- High Pressure Cutoff
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU3 Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
     AHU3 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
@@ -2711,37 +2484,6 @@
 
 ! HP Air Loop #4
 
-  Sizing:Zone,
-    SPACE4-1,                !- Zone or ZoneList Name
-    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method
-    14.,                     !- Zone Cooling Design Supply Air Temperature {C}
-    ,                        !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
-    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method
-    50.,                     !- Zone Heating Design Supply Air Temperature {C}
-    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    SZ DSOA SPACE4-1,        !- Design Specification Outdoor Air Object Name
-    0.0,                     !- Zone Heating Sizing Factor
-    0.0,                     !- Zone Cooling Sizing Factor
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- Cooling Minimum Air Flow Fraction
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Heating Maximum Air Flow {m3/s}
-    ;                        !- Heating Maximum Air Flow Fraction
-
-  DesignSpecification:OutdoorAir,
-    SZ DSOA SPACE4-1,        !- Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}
-    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0;                     !- Outdoor Air Flow per Zone {m3/s}
-
   ZoneHVAC:EquipmentConnections,
     SPACE4-1,                !- Zone Name
     SPACE4-1 Equipment,      !- Zone Conditioning Equipment List Name
@@ -2765,52 +2507,13 @@
     SPACE4-1 Direct Air,     !- Name
     FanAvailSched,           !- Availability Schedule Name
     SPACE4-1 Supply Inlet,   !- Zone Supply Air Node Name
-    autosize;                !- Maximum Air Flow Rate {m3/s}
-
-  Sizing:System,
-    AHU 4,                   !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    0.0,                     !- Design Outdoor Air Flow Rate {m3/s}
-    1.0,                     !- Central Heating Maximum System Air Flow Ratio
-    7.0,                     !- Preheat Design Temperature {C}
-    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.,                     !- Central Cooling Design Supply Air Temperature {C}
-    50.,                     !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Type of Zone Sum to Use
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Cooling Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Heating Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Heating Supply Air Flow Rate
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ,                        !- System Outdoor Air Method
-    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Heating Design Capacity
-    VAV;                     !- Central Cooling Capacity Control Method
+    2.0;                     !- Maximum Air Flow Rate {m3/s}
 
   AirLoopHVAC,
     AHU 4,                   !- Name
     ,                        !- Controller List Name
     AHU 4 Availability Managers,  !- Availability Manager List Name
-    autosize,                !- Design Supply Air Flow Rate {m3/s}
+    2.0,                     !- Design Supply Air Flow Rate {m3/s}
     AHU 4 Branches,          !- Branch List Name
     ,                        !- Connector List Name
     AHU 4 Air Loop Inlet,    !- Supply Side Inlet Node Name
@@ -2909,7 +2612,7 @@
     38000,                   !- Nominal Cooling Coil Capacity {W}
     0,                       !- Nominal Time for Condensate Removal to Begin {s}
     0,                       !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
-    3000000,                 !- High Pressure Cutoff {Pa}
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU4 Water to Air Heat Pump Source Side1 Inlet Node,  !- Water Inlet Node Name
     AHU4 Water to Air Heat Pump Source Side1 Outlet Node,  !- Water Outlet Node Name
@@ -2936,7 +2639,7 @@
     R22,                     !- Refrigerant Type
     0.0015,                  !- Design Source Side Flow Rate {m3/s}
     38000,                   !- Gross Rated Heating Capacity {W}
-    3000000,                 !- High Pressure Cutoff
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU4 Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
     AHU4 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
@@ -2966,37 +2669,6 @@
 
 ! HP Air Loop #5
 
-  Sizing:Zone,
-    SPACE5-1,                !- Zone or ZoneList Name
-    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method
-    14.,                     !- Zone Cooling Design Supply Air Temperature {C}
-    ,                        !- Zone Cooling Design Supply Air Temperature Difference {deltaC}
-    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method
-    50.,                     !- Zone Heating Design Supply Air Temperature {C}
-    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}
-    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    SZ DSOA SPACE5-1,        !- Design Specification Outdoor Air Object Name
-    0.0,                     !- Zone Heating Sizing Factor
-    0.0,                     !- Zone Cooling Sizing Factor
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Cooling Minimum Air Flow {m3/s}
-    ,                        !- Cooling Minimum Air Flow Fraction
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}
-    ,                        !- Heating Maximum Air Flow {m3/s}
-    ;                        !- Heating Maximum Air Flow Fraction
-
-  DesignSpecification:OutdoorAir,
-    SZ DSOA SPACE5-1,        !- Name
-    flow/person,             !- Outdoor Air Method
-    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}
-    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}
-    0.0;                     !- Outdoor Air Flow per Zone {m3/s}
-
   ZoneHVAC:EquipmentConnections,
     SPACE5-1,                !- Zone Name
     SPACE5-1 Equipment,      !- Zone Conditioning Equipment List Name
@@ -3020,52 +2692,13 @@
     SPACE5-1 Direct Air,     !- Name
     FanAvailSched,           !- Availability Schedule Name
     SPACE5-1 Supply Inlet,   !- Zone Supply Air Node Name
-    autosize;                !- Maximum Air Flow Rate {m3/s}
-
-  Sizing:System,
-    AHU 5,                   !- AirLoop Name
-    sensible,                !- Type of Load to Size On
-    0.0,                     !- Design Outdoor Air Flow Rate {m3/s}
-    1.0,                     !- Central Heating Maximum System Air Flow Ratio
-    7.0,                     !- Preheat Design Temperature {C}
-    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}
-    11.0,                    !- Precool Design Temperature {C}
-    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}
-    12.,                     !- Central Cooling Design Supply Air Temperature {C}
-    50.,                     !- Central Heating Design Supply Air Temperature {C}
-    noncoincident,           !- Type of Zone Sum to Use
-    no,                      !- 100% Outdoor Air in Cooling
-    no,                      !- 100% Outdoor Air in Heating
-    0.008,                   !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    0.008,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}
-    DesignDay,               !- Cooling Design Air Flow Method
-    0,                       !- Cooling Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Cooling Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}
-    DesignDay,               !- Heating Design Air Flow Method
-    0,                       !- Heating Design Air Flow Rate {m3/s}
-    ,                        !- Supply Air Flow Rate Per Floor Area During Heating Operation {m3/s-m2}
-    ,                        !- Fraction of Autosized Design Heating Supply Air Flow Rate
-    ,                        !- Fraction of Autosized Design Cooling Supply Air Flow Rate
-    ,                        !- Design Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}
-    ,                        !- System Outdoor Air Method
-    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}
-    CoolingDesignCapacity,   !- Cooling Design Capacity Method
-    autosize,                !- Cooling Design Capacity {W}
-    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Cooling Design Capacity
-    HeatingDesignCapacity,   !- Heating Design Capacity Method
-    autosize,                !- Heating Design Capacity {W}
-    ,                        !- Heating Design Capacity Per Floor Area {W/m2}
-    ,                        !- Fraction of Autosized Heating Design Capacity
-    VAV;                     !- Central Cooling Capacity Control Method
+    2.0;                     !- Maximum Air Flow Rate {m3/s}
 
   AirLoopHVAC,
     AHU 5,                   !- Name
     ,                        !- Controller List Name
     AHU 5 Availability Managers,  !- Availability Manager List Name
-    autosize,                !- Design Supply Air Flow Rate {m3/s}
+    2.0,                     !- Design Supply Air Flow Rate {m3/s}
     AHU 5 Branches,          !- Branch List Name
     ,                        !- Connector List Name
     AHU 5 Air Loop Inlet,    !- Supply Side Inlet Node Name
@@ -3164,7 +2797,7 @@
     38000,                   !- Nominal Cooling Coil Capacity {W}
     0,                       !- Nominal Time for Condensate Removal to Begin {s}
     0,                       !- Ratio of Initial Moisture Evaporation Rate and Steady State Latent Capacity {dimensionless}
-    3000000,                 !- High Pressure Cutoff {Pa}
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU5 Water to Air Heat Pump Source Side1 Inlet Node,  !- Water Inlet Node Name
     AHU5 Water to Air Heat Pump Source Side1 Outlet Node,  !- Water Outlet Node Name
@@ -3191,7 +2824,7 @@
     R22,                     !- Refrigerant Type
     0.0015,                  !- Design Source Side Flow Rate {m3/s}
     38000,                   !- Gross Rated Heating Capacity {W}
-    3000000,                 !- High Pressure Cutoff
+    4000000,                 !- High Pressure Cutoff {Pa}
     0,                       !- Low Pressure Cutoff {Pa}
     AHU5 Water to Air Heat Pump Source Side2 Inlet Node,  !- Water Inlet Node Name
     AHU5 Water to Air Heat Pump Source Side2 Outlet Node,  !- Water Outlet Node Name
diff --git a/testfiles/UnitarySystem_MultiSpeedCoils_SingleMode.idf b/testfiles/UnitarySystem_MultiSpeedCoils_SingleMode.idf
index 0e8c42acf75..03832b26d59 100644
--- a/testfiles/UnitarySystem_MultiSpeedCoils_SingleMode.idf
+++ b/testfiles/UnitarySystem_MultiSpeedCoils_SingleMode.idf
@@ -1656,7 +1656,7 @@
     0.058333,                !- Defrost Time Period Fraction
     2000.0,                  !- Resistive Defrost Heater Capacity {W}
     No,                      !- Apply Part Load Fraction to Speeds Greater than 1
-    NaturalGas,              !- Fuel Type
+    Electricity,             !- Fuel Type
     4,                       !- Region number for Calculating HSPF
     4,                       !- Number of Speeds
     7500,                    !- Speed 1 Gross Rated Heating Capacity {W}
@@ -2032,7 +2032,7 @@
     ,                        !- Basin Heater Capacity {W/K}
     ,                        !- Basin Heater Setpoint Temperature {C}
     ,                        !- Basin Heater Operating Schedule Name
-    NaturalGas,              !- Fuel Type
+    Electricity,             !- Fuel Type
     4,                       !- Number of Speeds
     7500,                    !- Speed 1 Gross Rated Total Cooling Capacity {W}
     0.75,                    !- Speed 1 Gross Rated Sensible Heat Ratio
diff --git a/tst/EnergyPlus/unit/CMakeLists.txt b/tst/EnergyPlus/unit/CMakeLists.txt
index b46b4816018..ab616d389b3 100644
--- a/tst/EnergyPlus/unit/CMakeLists.txt
+++ b/tst/EnergyPlus/unit/CMakeLists.txt
@@ -64,6 +64,7 @@ set( test_src
   MixerComponent.unit.cc
   NodeInputManager.unit.cc
   PlantHeatExchangerFluidToFluid.unit.cc
+  PlantPipingSystemsManager.unit.cc
   PlantUtilities.unit.cc
   Pumps.unit.cc
   PurchasedAirManager.unit.cc
@@ -81,6 +82,7 @@ set( test_src
   SecondaryDXCoils.unit.cc
   SetPointManager.unit.cc
   SimAirServingZones.unit.cc
+  SingleDuct.unit.cc
   SiteBuildingSurfaceGroundTemperatures.unit.cc
   SiteDeepGroundTemperatures.unit.cc
   SiteFCFactorMethodGroundTemperatures.unit.cc
diff --git a/tst/EnergyPlus/unit/DOASEffectOnZoneSizing.unit.cc b/tst/EnergyPlus/unit/DOASEffectOnZoneSizing.unit.cc
index 5c55dabbf51..3bdb7353628 100644
--- a/tst/EnergyPlus/unit/DOASEffectOnZoneSizing.unit.cc
+++ b/tst/EnergyPlus/unit/DOASEffectOnZoneSizing.unit.cc
@@ -352,3 +352,81 @@ TEST_F( EnergyPlusFixture, DOASEffectOnZoneSizing_SizeZoneEquipment )
 	MassConservation.deallocate();
 
 }
+
+TEST_F( EnergyPlusFixture, TestAutoCalcDOASControlStrategy )
+{
+
+	NumZoneSizingInput = 2;
+	ZoneSizingInput.allocate( NumZoneSizingInput );
+	ZoneSizingInput( 1 ).AccountForDOAS = false;
+	ZoneSizingInput( 2 ).AccountForDOAS = true;
+
+	ZoneSizingInput( 2 ).DOASControlStrategy = DOANeutralSup;
+	ZoneSizingInput( 2 ).DOASLowSetpoint = AutoSize;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = AutoSize;
+	AutoCalcDOASControlStrategy();
+	EXPECT_DOUBLE_EQ( 21.1, ZoneSizingInput( 2 ).DOASLowSetpoint );
+	EXPECT_DOUBLE_EQ( 23.9, ZoneSizingInput( 2 ).DOASHighSetpoint );
+	ZoneSizingInput( 2 ).DOASLowSetpoint = AutoSize;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = 23.7;
+	AutoCalcDOASControlStrategy();
+	EXPECT_NEAR( 20.9, ZoneSizingInput( 2 ).DOASLowSetpoint, .000001 );
+	EXPECT_DOUBLE_EQ( 23.7, ZoneSizingInput( 2 ).DOASHighSetpoint );
+	ZoneSizingInput( 2 ).DOASLowSetpoint = 21.2;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = AutoSize;
+	AutoCalcDOASControlStrategy();
+	EXPECT_NEAR( 24.0, ZoneSizingInput( 2 ).DOASHighSetpoint, .000001 );
+	EXPECT_DOUBLE_EQ( 21.2, ZoneSizingInput( 2 ).DOASLowSetpoint );
+	ZoneSizingInput( 2 ).DOASLowSetpoint = 21.5;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = 22.6;
+	AutoCalcDOASControlStrategy();
+	EXPECT_DOUBLE_EQ( 22.6, ZoneSizingInput( 2 ).DOASHighSetpoint );
+	EXPECT_DOUBLE_EQ( 21.5, ZoneSizingInput( 2 ).DOASLowSetpoint );
+
+	ZoneSizingInput( 2 ).DOASControlStrategy = DOANeutralDehumSup;
+	ZoneSizingInput( 2 ).DOASLowSetpoint = AutoSize;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = AutoSize;
+	AutoCalcDOASControlStrategy();
+	EXPECT_DOUBLE_EQ( 14.4, ZoneSizingInput( 2 ).DOASLowSetpoint );
+	EXPECT_DOUBLE_EQ( 22.2, ZoneSizingInput( 2 ).DOASHighSetpoint );
+	ZoneSizingInput( 2 ).DOASLowSetpoint = AutoSize;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = 22.4;
+	AutoCalcDOASControlStrategy();
+	EXPECT_DOUBLE_EQ( 14.4, ZoneSizingInput( 2 ).DOASLowSetpoint );
+	EXPECT_DOUBLE_EQ( 22.4, ZoneSizingInput( 2 ).DOASHighSetpoint );
+	ZoneSizingInput( 2 ).DOASLowSetpoint = 13.8;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = AutoSize;
+	AutoCalcDOASControlStrategy();
+	EXPECT_DOUBLE_EQ( 22.2, ZoneSizingInput( 2 ).DOASHighSetpoint );
+	EXPECT_DOUBLE_EQ( 13.8, ZoneSizingInput( 2 ).DOASLowSetpoint );
+	ZoneSizingInput( 2 ).DOASLowSetpoint = 13.9;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = 22.6;
+	AutoCalcDOASControlStrategy();
+	EXPECT_DOUBLE_EQ( 22.6, ZoneSizingInput( 2 ).DOASHighSetpoint );
+	EXPECT_DOUBLE_EQ( 13.9, ZoneSizingInput( 2 ).DOASLowSetpoint );
+
+	ZoneSizingInput( 2 ).DOASControlStrategy = DOACoolSup;
+	ZoneSizingInput( 2 ).DOASLowSetpoint = AutoSize;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = AutoSize;
+	AutoCalcDOASControlStrategy();
+	EXPECT_DOUBLE_EQ( 12.2, ZoneSizingInput( 2 ).DOASLowSetpoint );
+	EXPECT_DOUBLE_EQ( 14.4, ZoneSizingInput( 2 ).DOASHighSetpoint );
+	ZoneSizingInput( 2 ).DOASLowSetpoint = AutoSize;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = 14.6;
+	AutoCalcDOASControlStrategy();
+	EXPECT_NEAR( 12.4, ZoneSizingInput( 2 ).DOASLowSetpoint, .000001 );
+	EXPECT_DOUBLE_EQ( 14.6, ZoneSizingInput( 2 ).DOASHighSetpoint );
+	ZoneSizingInput( 2 ).DOASLowSetpoint = 12.3;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = AutoSize;
+	AutoCalcDOASControlStrategy();
+	EXPECT_NEAR( 14.5, ZoneSizingInput( 2 ).DOASHighSetpoint, .000001 );
+	EXPECT_DOUBLE_EQ( 12.3, ZoneSizingInput( 2 ).DOASLowSetpoint );
+	ZoneSizingInput( 2 ).DOASLowSetpoint = 12.6;
+	ZoneSizingInput( 2 ).DOASHighSetpoint = 13.8;
+	AutoCalcDOASControlStrategy();
+	EXPECT_DOUBLE_EQ( 13.8, ZoneSizingInput( 2 ).DOASHighSetpoint );
+	EXPECT_DOUBLE_EQ( 12.6, ZoneSizingInput( 2 ).DOASLowSetpoint );
+
+	ZoneSizingInput.deallocate();
+
+}
diff --git a/tst/EnergyPlus/unit/DXCoils.unit.cc b/tst/EnergyPlus/unit/DXCoils.unit.cc
index 1d1e7c9b0d1..7e5e44ef6ee 100644
--- a/tst/EnergyPlus/unit/DXCoils.unit.cc
+++ b/tst/EnergyPlus/unit/DXCoils.unit.cc
@@ -668,6 +668,58 @@ namespace EnergyPlus {
 		COPwDefrost = Coil.TotalHeatingEnergyRate / Coil.ElecHeatingPower;
 		EXPECT_DOUBLE_EQ( COPwoDefrost, COPwDefrost );
 
+		// Now test that coil output at Speed = 1, CyclingRatio = 1 is the same as Speed = 2 and SpeedRatio = 0
+		Real64 DXCoilOutletNodeTemp = Coil.OutletAirTemp;
+		Real64 DXCoilOutletNodeHumRat = Coil.OutletAirHumRat;
+		Real64 DXCoilOutletNodeEnthalpy = Coil.OutletAirEnthalpy;
+		Real64 DXCoilHeatingCapacity = Coil.TotalHeatingEnergyRate;
+
+		SpeedRatio = 0.0;
+		CycRatio = 1.0;
+		SpeedNum = 2;
+
+		CalcMultiSpeedDXCoilHeating( DXCoilNum, SpeedRatio, CycRatio, SpeedNum, FanOpMode, 0 );
+
+		Real64 DXCoilOutletNodeTemp2 = Coil.OutletAirTemp;
+		Real64 DXCoilOutletNodeHumRat2 = Coil.OutletAirHumRat;
+		Real64 DXCoilOutletNodeEnthalpy2 = Coil.OutletAirEnthalpy;
+		Real64 DXCoilHeatingCapacity2 = Coil.TotalHeatingEnergyRate;
+
+		EXPECT_DOUBLE_EQ( DXCoilOutletNodeTemp, DXCoilOutletNodeTemp2 );
+		EXPECT_DOUBLE_EQ( DXCoilOutletNodeHumRat, DXCoilOutletNodeHumRat2 );
+		EXPECT_DOUBLE_EQ( DXCoilOutletNodeEnthalpy, DXCoilOutletNodeEnthalpy2 );
+		EXPECT_DOUBLE_EQ( DXCoilHeatingCapacity, DXCoilHeatingCapacity2 );
+
+		// Defroster on
+		OutDryBulbTemp = -5.0; // cold
+
+		SpeedRatio = 0.0;
+		CycRatio = 1.0;
+		SpeedNum = 1;
+
+		CalcMultiSpeedDXCoilHeating( DXCoilNum, SpeedRatio, CycRatio, SpeedNum, FanOpMode, 0 );
+
+		DXCoilOutletNodeTemp = Coil.OutletAirTemp;
+		DXCoilOutletNodeHumRat = Coil.OutletAirHumRat;
+		DXCoilOutletNodeEnthalpy = Coil.OutletAirEnthalpy;
+		DXCoilHeatingCapacity = Coil.TotalHeatingEnergyRate;
+
+		SpeedRatio = 0.0;
+		CycRatio = 1.0;
+		SpeedNum = 2;
+
+		CalcMultiSpeedDXCoilHeating( DXCoilNum, SpeedRatio, CycRatio, SpeedNum, FanOpMode, 0 );
+
+		DXCoilOutletNodeTemp2 = Coil.OutletAirTemp;
+		DXCoilOutletNodeHumRat2 = Coil.OutletAirHumRat;
+		DXCoilOutletNodeEnthalpy2 = Coil.OutletAirEnthalpy;
+		DXCoilHeatingCapacity2 = Coil.TotalHeatingEnergyRate;
+
+		EXPECT_DOUBLE_EQ( DXCoilOutletNodeTemp, DXCoilOutletNodeTemp2 );
+		EXPECT_DOUBLE_EQ( DXCoilOutletNodeHumRat, DXCoilOutletNodeHumRat2 );
+		EXPECT_DOUBLE_EQ( DXCoilOutletNodeEnthalpy, DXCoilOutletNodeEnthalpy2 );
+		EXPECT_DOUBLE_EQ( DXCoilHeatingCapacity, DXCoilHeatingCapacity2 );
+
 	}
 
 	TEST_F( EnergyPlusFixture, TestSingleSpeedDefrostCOP ) {
diff --git a/tst/EnergyPlus/unit/DataSurfaces.unit.cc b/tst/EnergyPlus/unit/DataSurfaces.unit.cc
index 322f83efc1a..29fd7598f62 100644
--- a/tst/EnergyPlus/unit/DataSurfaces.unit.cc
+++ b/tst/EnergyPlus/unit/DataSurfaces.unit.cc
@@ -210,7 +210,7 @@ TEST( SurfaceTest, Plane )
 		SurfaceData s;
 		s.Vertex.dimension( 3 );
 		s.Vertex = { Vector(1,1,1), Vector(-1,1,0), Vector(2,0,3) };
-		s.Shape = Triangle;
+		s.Shape = SurfaceShape::Triangle;
 		s.set_computed_geometry();
 
 		EXPECT_DOUBLE_EQ( -1.0, s.plane.x );
@@ -222,7 +222,7 @@ TEST( SurfaceTest, Plane )
 		SurfaceData s;
 		s.Vertex.dimension( 3 );
 		s.Vertex = { Vector(2,1,-1), Vector(0,-2,0), Vector(1,-1,2) };
-		s.Shape = Triangle;
+		s.Shape = SurfaceShape::Triangle;
 		s.set_computed_geometry();
 
 		EXPECT_DOUBLE_EQ( -7.0, s.plane.x );
@@ -239,7 +239,7 @@ TEST( SurfaceTest, Surface2D )
 		SurfaceData s;
 		s.Vertex.dimension( 4 );
 		s.Vertex = { Vector(0,0,0), Vector(1,0,0), Vector(1,1,0), Vector(0,1,0) };
-		s.Shape = Rectangle;
+		s.Shape = SurfaceShape::Rectangle;
 		s.set_computed_geometry();
 
 		Surface2D const & s2d( s.surface2d );
diff --git a/tst/EnergyPlus/unit/Datasets.unit.cc b/tst/EnergyPlus/unit/Datasets.unit.cc
index 72b815679ca..c676b5a0fd1 100644
--- a/tst/EnergyPlus/unit/Datasets.unit.cc
+++ b/tst/EnergyPlus/unit/Datasets.unit.cc
@@ -129,9 +129,6 @@ namespace EnergyPlus {
 	TEST_F( DataSetFixture, GlycolPropertiesRefData ) {
 		ASSERT_FALSE( process_idf( delimited_string( getAllLinesInFile( configured_source_directory() + "/datasets/GlycolPropertiesRefData.idf" ) ) ) );
 	}
-	TEST_F( DataSetFixture, LCCusePriceEscalationDataSet2010 ) {
-		ASSERT_FALSE( process_idf( delimited_string( getAllLinesInFile( configured_source_directory() + "/datasets/LCCusePriceEscalationDataSet2010.idf" ) ) ) );
-	}
 	TEST_F( DataSetFixture, LCCusePriceEscalationDataSet2011 ) {
 		ASSERT_FALSE( process_idf( delimited_string( getAllLinesInFile( configured_source_directory() + "/datasets/LCCusePriceEscalationDataSet2011.idf" ) ) ) );
 	}
@@ -144,6 +141,9 @@ namespace EnergyPlus {
 	TEST_F( DataSetFixture, LCCusePriceEscalationDataSet2014 ) {
 		ASSERT_FALSE( process_idf( delimited_string( getAllLinesInFile( configured_source_directory() + "/datasets/LCCusePriceEscalationDataSet2014.idf" ) ) ) );
 	}
+	TEST_F( DataSetFixture, LCCusePriceEscalationDataSet2015 ) {
+		ASSERT_FALSE( process_idf( delimited_string( getAllLinesInFile( configured_source_directory() + "/datasets/LCCusePriceEscalationDataSet2015.idf" ) ) ) );
+	}
 	TEST_F( DataSetFixture, MoistureMaterials ) {
 		ASSERT_FALSE( process_idf( delimited_string( getAllLinesInFile( configured_source_directory() + "/datasets/MoistureMaterials.idf" ) ) ) );
 	}
diff --git a/tst/EnergyPlus/unit/EMSManager.unit.cc b/tst/EnergyPlus/unit/EMSManager.unit.cc
index f4b9c383cd3..52d128eb805 100644
--- a/tst/EnergyPlus/unit/EMSManager.unit.cc
+++ b/tst/EnergyPlus/unit/EMSManager.unit.cc
@@ -68,6 +68,9 @@
 #include <EnergyPlus/UtilityRoutines.hh>
 #include <EnergyPlus/OutAirNodeManager.hh>
 #include <EnergyPlus/DataLoopNode.hh>
+#include <EnergyPlus/NodeInputManager.hh>
+#include <EnergyPlus/OutputProcessor.hh>
+#include <EnergyPlus/SimulationManager.hh>
 
 using namespace EnergyPlus;
 using namespace EnergyPlus::EMSManager;
@@ -159,9 +162,10 @@ TEST_F( EnergyPlusFixture, Dual_NodeTempSetpoints ) {
 
 		EMSManager::FinishProcessingUserInput = true;
 
-		EMSManager::ManageEMS( DataGlobals::emsCallFromSetupSimulation );
+		bool anyRan;
+		EMSManager::ManageEMS( DataGlobals::emsCallFromSetupSimulation, anyRan );
 
-		EMSManager::ManageEMS( DataGlobals::emsCallFromBeginNewEvironment );
+		EMSManager::ManageEMS( DataGlobals::emsCallFromBeginNewEvironment, anyRan );
 
 
 		EXPECT_NEAR(DataLoopNode::Node(1).TempSetPointHi, 20.0, 0.000001 );
@@ -339,8 +343,9 @@ TEST_F( EnergyPlusFixture, Test_EMSLogic ) {
 
 	EMSManager::CheckIfAnyEMS();
 	EMSManager::FinishProcessingUserInput = true;
-	EMSManager::ManageEMS( DataGlobals::emsCallFromSetupSimulation );
-	EMSManager::ManageEMS( DataGlobals::emsCallFromBeginNewEvironment );
+	bool anyRan;
+	EMSManager::ManageEMS( DataGlobals::emsCallFromSetupSimulation, anyRan );
+	EMSManager::ManageEMS( DataGlobals::emsCallFromBeginNewEvironment, anyRan );
 
 
 	EXPECT_NEAR( DataLoopNode::Node( 1 ).TempSetPoint, 11.0, 0.0000001 );
@@ -351,7 +356,7 @@ TEST_F( EnergyPlusFixture, Test_EMSLogic ) {
 	EXPECT_NEAR( DataLoopNode::Node( 6 ).TempSetPoint, 16.0, 0.0000001 );
 	EXPECT_NEAR( DataLoopNode::Node( 7 ).TempSetPoint, 17.0, 0.0000001 );
 
-	EMSManager::ManageEMS( DataGlobals::emsCallFromBeginTimestepBeforePredictor );
+	EMSManager::ManageEMS( DataGlobals::emsCallFromBeginTimestepBeforePredictor, anyRan );
 
 
 	EXPECT_NEAR( DataLoopNode::Node( 1 ).TempSetPoint, 21.0, 0.0000001 );
@@ -409,10 +414,59 @@ TEST_F( EnergyPlusFixture, Debug_EMSLogic ) {
 
 	EMSManager::CheckIfAnyEMS();
 	EMSManager::FinishProcessingUserInput = true;
-	EMSManager::ManageEMS( DataGlobals::emsCallFromSetupSimulation );
-	EMSManager::ManageEMS( DataGlobals::emsCallFromBeginNewEvironment );
+	bool anyRan;
+	EMSManager::ManageEMS( DataGlobals::emsCallFromSetupSimulation, anyRan );
+	EMSManager::ManageEMS( DataGlobals::emsCallFromBeginNewEvironment, anyRan );
 
 
 	EXPECT_NEAR( DataLoopNode::Node( 1 ).TempSetPoint, 1.0, 0.0000001 );
 
 }
+
+
+TEST_F( EnergyPlusFixture, TestAnyRanArgument ) {
+		// small test to demonstrate new boolean argument. 
+		// shows a simple way to setup sensor on a node, need to call SetupNodeVarsForReporting()
+
+		std::string const idf_objects = delimited_string( { 
+		"Version,8.5;",
+
+		"OutdoorAir:Node, Test node;",
+
+		"EnergyManagementSystem:Sensor,",
+		"Node_mdot,",
+		"Test node,",
+		"System Node Mass Flow Rate;",
+
+		"EnergyManagementSystem:ProgramCallingManager,",
+		"Test inside HVAC system iteration Loop,",
+		"InsideHVACSystemIterationLoop,",
+		"Test_InsideHVACSystemIterationLoop;",
+	
+		"EnergyManagementSystem:Program,",
+		"Test_InsideHVACSystemIterationLoop,",
+		"set dumm1 = Node_mdot;",
+
+		} );
+
+		ASSERT_FALSE( process_idf( idf_objects ) );
+
+		OutAirNodeManager::SetOutAirNodes();
+		NodeInputManager::SetupNodeVarsForReporting();
+		EMSManager::CheckIfAnyEMS();
+
+		EMSManager::FinishProcessingUserInput = true;
+
+		bool anyRan;
+		EMSManager::ManageEMS( DataGlobals::emsCallFromSetupSimulation, anyRan );
+		EXPECT_FALSE( anyRan );
+
+		EMSManager::ManageEMS( DataGlobals::emsCallFromBeginNewEvironment, anyRan );
+		EXPECT_FALSE( anyRan );
+
+		EMSManager::ManageEMS( DataGlobals::emsCallFromHVACIterationLoop, anyRan );
+		EXPECT_TRUE( anyRan );
+
+}
+
+
diff --git a/tst/EnergyPlus/unit/FanCoilUnits.unit.cc b/tst/EnergyPlus/unit/FanCoilUnits.unit.cc
index 50ea5865168..6cd4e662103 100644
--- a/tst/EnergyPlus/unit/FanCoilUnits.unit.cc
+++ b/tst/EnergyPlus/unit/FanCoilUnits.unit.cc
@@ -95,6 +95,7 @@ using namespace EnergyPlus::DataGlobals;
 using namespace EnergyPlus::DataZoneEquipment;
 using namespace EnergyPlus::DataZoneEquipment;
 using namespace EnergyPlus::DataHeatBalance;
+using namespace EnergyPlus::DataHeatBalFanSys;
 using namespace EnergyPlus::DataPlant;
 using namespace EnergyPlus::DataEnvironment;
 using namespace EnergyPlus::DataSizing;
@@ -733,9 +734,1013 @@ namespace EnergyPlus {
 		CoilNames.deallocate();
 
 	}
+	TEST_F( EnergyPlusFixture, ConstantFanVariableFlowFanCoilHeatingTest ) {
 
-	TEST_F( EnergyPlusFixture, FanCoil_ASHRAE90VariableFan ) {
+		int FanCoilNum( 1 );
+		int ZoneNum( 1 );
+		int ControlledZoneNum( 1 );
+		bool FirstHVACIteration( true );
+		bool ErrorsFound( false );
+		Real64 QZnReq( 0.0 );
+		Real64 HotWaterMassFlowRate( 0.0 );
+		Real64 ColdWaterMassFlowRate( 0.0 );
+		Real64 QUnitOut( 0.0 );
+		Real64 AirMassFlow( 0.0 );
+		Real64 MaxAirMassFlow( 0.0 );
+		Real64 LatOutputProvided( 0.0 );
+
+		DataEnvironment::OutBaroPress = 101325.0;
+		DataEnvironment::StdRhoAir = 1.20;
+		WaterCoils::GetWaterCoilsInputFlag = true;
+		NumCoils = 0;
+		DataGlobals::NumOfTimeStepInHour = 1;
+		DataGlobals::TimeStep = 1;
+		DataGlobals::MinutesPerTimeStep = 60;
+
+		InitializePsychRoutines();
+
+		std::string const idf_objects = delimited_string( {
+			"	Version,8.3;",
+			"	Zone,",
+			"	EAST ZONE, !- Name",
+			"	0, !- Direction of Relative North { deg }",
+			"	0, !- X Origin { m }",
+			"	0, !- Y Origin { m }",
+			"	0, !- Z Origin { m }",
+			"	1, !- Type",
+			"	1, !- Multiplier",
+			"	autocalculate, !- Ceiling Height { m }",
+			"	autocalculate; !- Volume { m3 }",
+			"	ZoneHVAC:EquipmentConnections,",
+			"	EAST ZONE, !- Zone Name",
+			"	Zone1Equipment, !- Zone Conditioning Equipment List Name",
+			"	Zone1Inlets, !- Zone Air Inlet Node or NodeList Name",
+			"	Zone1Exhausts, !- Zone Air Exhaust Node or NodeList Name",
+			"	Zone 1 Node, !- Zone Air Node Name",
+			"	Zone 1 Outlet Node;      !- Zone Return Air Node Name",
+			"	ZoneHVAC:EquipmentList,",
+			"	Zone1Equipment, !- Name",
+			"	ZoneHVAC:FourPipeFanCoil, !- Zone Equipment 1 Object Type",
+			"	Zone1FanCoil, !- Zone Equipment 1 Name",
+			"	1, !- Zone Equipment 1 Cooling Sequence",
+			"	1;                       !- Zone Equipment 1 Heating or No - Load Sequence",
+			"   NodeList,",
+			"	Zone1Inlets, !- Name",
+			"	Zone1FanCoilAirOutletNode;  !- Node 1 Name",
+			"	NodeList,",
+			"	Zone1Exhausts, !- Name",
+			"	Zone1FanCoilAirInletNode; !- Node 1 Name",
+			"	OutdoorAir:NodeList,",
+			"	Zone1FanCoilOAInNode;    !- Node or NodeList Name 1",
+			"	OutdoorAir:Mixer,",
+			"	Zone1FanCoilOAMixer, !- Name",
+			"	Zone1FanCoilOAMixerOutletNode, !- Mixed Air Node Name",
+			"	Zone1FanCoilOAInNode, !- Outdoor Air Stream Node Name",
+			"	Zone1FanCoilExhNode, !- Relief Air Stream Node Name",
+			"	Zone1FanCoilAirInletNode; !- Return Air Stream Node Name",
+			"	Schedule:Constant,",
+			"	FanAndCoilAvailSched, !- Name",
+			"	FRACTION, !- Schedule Type",
+			"	1;        !- TimeStep Value",
+			"	ScheduleTypeLimits,",
+			"	Fraction, !- Name",
+			"	0.0, !- Lower Limit Value",
+			"	1.0, !- Upper Limit Value",
+			"	CONTINUOUS;              !- Numeric Type",
+			"   Fan:OnOff,",
+			"	Zone1FanCoilFan, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Name",
+			"	0.5, !- Fan Total Efficiency",
+			"	75.0, !- Pressure Rise { Pa }",
+			"	0.6, !- Maximum Flow Rate { m3 / s }",
+			"	0.9, !- Motor Efficiency",
+			"	1.0, !- Motor In Airstream Fraction",
+			"	Zone1FanCoilOAMixerOutletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilFanOutletNode, !- Air Outlet Node Name",
+			"	, !- Fan Power Ratio Function of Speed Ratio Curve Name",
+			"	;                        !- Fan Efficiency Ratio Function of Speed Ratio Curve Name	",
+			"	Coil:Cooling:Water,",
+			"	Zone1FanCoilCoolingCoil, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Namev",
+			"	0.0002, !- Design Water Flow Rate { m3 / s }",
+			"	0.5000, !- Design Air Flow Rate { m3 / s }",
+			"	7.22,   !- Design Inlet Water Temperature { Cv }",
+			"	24.340, !- Design Inlet Air Temperature { C }",
+			"	14.000, !- Design Outlet Air Temperature { C }",
+			"	0.0095, !- Design Inlet Air Humidity Ratio { kgWater / kgDryAir }",
+			"	0.0090, !- Design Outlet Air Humidity Ratio { kgWater / kgDryAir }",
+			"	Zone1FanCoilChWInletNode, !- Water Inlet Node Name",
+			"	Zone1FanCoilChWOutletNode, !- Water Outlet Node Name",
+			"	Zone1FanCoilFanOutletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilCCOutletNode, !- Air Outlet Node Name",
+			"	SimpleAnalysis, !- Type of Analysis",
+			"	CrossFlow;               !- Heat Exchanger Configuration",
+			"	Coil:Heating:Water,",
+			"   Zone1FanCoilHeatingCoil, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Name",
+			"	150.0,   !- U - Factor Times Area Value { W / K }",
+			"	0.00014, !- Maximum Water Flow Rate { m3 / s }",
+			"	Zone1FanCoilHWInletNode, !- Water Inlet Node Name",
+			"	Zone1FanCoilHWOutletNode, !- Water Outlet Node Name",
+			"	Zone1FanCoilCCOutletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilAirOutletNode, !- Air Outlet Node Name",
+			"	UFactorTimesAreaAndDesignWaterFlowRate, !- Performance Input Method",
+			"	autosize, !- Rated Capacity { W }",
+			"	82.2, !- Rated Inlet Water Temperature { C }",
+			"	16.6, !- Rated Inlet Air Temperature { C }",
+			"	71.1, !- Rated Outlet Water Temperature { C }",
+			"	32.2, !- Rated Outlet Air Temperature { C }",
+			"	;     !- Rated Ratio for Air and Water Convection",
+			"	ZoneHVAC:FourPipeFanCoil,",
+			"	Zone1FanCoil, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Name",
+			"	ConstantFanVariableFlow, !- Capacity Control Method",
+			"	0.5, !- Maximum Supply Air Flow Rate { m3 / s }",
+			"	0.3, !- Low Speed Supply Air Flow Ratio",
+			"	0.6, !- Medium Speed Supply Air Flow Ratio",
+			"	0.0, !- Maximum Outdoor Air Flow Rate { m3 / s }",
+			"	FanAndCoilAvailSched, !- Outdoor Air Schedule Name",
+			"	Zone1FanCoilAirInletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilAirOutletNode, !- Air Outlet Node Name",
+			"	OutdoorAir:Mixer, !- Outdoor Air Mixer Object Type",
+			"	Zone1FanCoilOAMixer, !- Outdoor Air Mixer Name",
+			"	Fan:OnOff, !- Supply Air Fan Object Type",
+			"	Zone1FanCoilFan, !- Supply Air Fan Name",
+			"	Coil:Cooling:Water, !- Cooling Coil Object Type",
+			"	Zone1FanCoilCoolingCoil, !- Cooling Coil Name",
+			"	0.00014, !- Maximum Cold Water Flow Rate { m3 / s }",
+			"	0.0, !- Minimum Cold Water Flow Rate { m3 / s }",
+			"	0.001, !- Cooling Convergence Tolerance",
+			"	Coil:Heating:Water, !- Heating Coil Object Type",
+			"	Zone1FanCoilHeatingCoil, !- Heating Coil Name",
+			"	0.00014, !- Maximum Hot Water Flow Rate { m3 / s }",
+			"	0.0, !- Minimum Hot Water Flow Rate { m3 / s }",
+			"	0.001; !- Heating Convergence Tolerance",
+
+		} );
+
+		ASSERT_FALSE( process_idf( idf_objects ) );
+
+		GetZoneData( ErrorsFound );
+		EXPECT_EQ( "EAST ZONE", Zone( 1 ).Name );
+
+		GetZoneEquipmentData1();
+		ProcessScheduleInput();
+		ScheduleInputProcessed = true;
+		GetFanInput();
+		EXPECT_EQ( DataHVACGlobals::FanType_SimpleOnOff, Fan( 1 ).FanType_Num );
+
+		GetFanCoilUnits();
+		EXPECT_EQ( "CONSTANTFANVARIABLEFLOW", FanCoil( 1 ).CapCtrlMeth );
+		EXPECT_EQ( "OUTDOORAIR:MIXER", FanCoil( 1 ).OAMixType );
+		EXPECT_EQ( "FAN:ONOFF", FanCoil( 1 ).FanType );
+		EXPECT_EQ( "COIL:COOLING:WATER", FanCoil( 1 ).CCoilType );
+		EXPECT_EQ( "COIL:HEATING:WATER", FanCoil( 1 ).HCoilType );
+
+		TotNumLoops = 2;
+		PlantLoop.allocate( TotNumLoops );
+
+		AirMassFlow = 0.60;
+		MaxAirMassFlow = 0.60;
+		// heating load only
+		ColdWaterMassFlowRate = 0.0;
+		HotWaterMassFlowRate = 0.14;
+
+		Node( OAMixer( 1 ).RetNode ).MassFlowRate = AirMassFlow;
+		Node( OAMixer( 1 ).RetNode ).MassFlowRateMax = MaxAirMassFlow;
+
+		Node( OAMixer( 1 ).RetNode ).Temp = 22.0;
+		Node( OAMixer( 1 ).RetNode ).Enthalpy = 36000;
+		Node( OAMixer( 1 ).RetNode ).HumRat = PsyWFnTdbH( Node( OAMixer( 1 ).RetNode ).Temp, Node( OAMixer( 1 ).RetNode ).Enthalpy );
+
+		Node( OAMixer( 1 ).InletNode ).Temp = 10.0;
+		Node( OAMixer( 1 ).InletNode ).Enthalpy = 18000;
+		Node( OAMixer( 1 ).InletNode ).HumRat = PsyWFnTdbH( Node( OAMixer( 1 ).InletNode ).Temp, Node( OAMixer( 1 ).InletNode ).Enthalpy );
+
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRate = AirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMin = AirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMinAvail = AirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMax = MaxAirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMaxAvail = MaxAirMassFlow;
+
+		FanCoil( 1 ).OutAirMassFlow = 0.0;
+		FanCoil( 1 ).MaxAirMassFlow = MaxAirMassFlow;
+		FanCoil( 1 ).MaxColdWaterFlow = 0.14;
+		FanCoil( 1 ).MaxHotWaterFlow = 0.14;
+
+		Node( FanCoil( 1 ).OutsideAirNode ).MassFlowRateMax = 0.0;
+		Node( FanCoil( 1 ).ColdControlNode ).MassFlowRateMax = 0.14;
+		Node( FanCoil( 1 ).HotControlNode ).MassFlowRateMax = 0.14;
+		Node( FanCoil( 1 ).ColdControlNode ).MassFlowRateMaxAvail = 0.14;
+		Node( FanCoil( 1 ).HotControlNode ).MassFlowRateMaxAvail = 0.14;
+
+
+		Fan( 1 ).InletAirMassFlowRate = AirMassFlow;
+		Fan( 1 ).MaxAirMassFlowRate = MaxAirMassFlow;
+
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRate = AirMassFlow;
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRateMin = AirMassFlow;
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRateMax = AirMassFlow;
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRateMaxAvail = AirMassFlow;
+
+		WaterCoil( 2 ).UACoilTotal = 470.0;
+		WaterCoil( 2 ).UACoilExternal = 611.0;
+		WaterCoil( 2 ).UACoilInternal = 2010.0;
+		WaterCoil( 2 ).TotCoilOutsideSurfArea = 50.0;
+
+		Node( WaterCoil( 2 ).AirInletNodeNum ).MassFlowRate = AirMassFlow;
+		Node( WaterCoil( 2 ).AirInletNodeNum ).MassFlowRateMin = AirMassFlow;
+		Node( WaterCoil( 2 ).AirInletNodeNum ).MassFlowRateMax = AirMassFlow;
+		Node( WaterCoil( 2 ).AirInletNodeNum ).MassFlowRateMaxAvail = AirMassFlow;
+
+		WaterCoil( 2 ).InletWaterMassFlowRate = ColdWaterMassFlowRate;
+		WaterCoil( 2 ).MaxWaterMassFlowRate = ColdWaterMassFlowRate;
+		Node( WaterCoil( 2 ).WaterInletNodeNum ).MassFlowRate = ColdWaterMassFlowRate;
+		Node( WaterCoil( 2 ).WaterInletNodeNum ).MassFlowRateMaxAvail = ColdWaterMassFlowRate;
+		Node( WaterCoil( 2 ).WaterInletNodeNum ).Temp = 6.0;
+		Node( WaterCoil( 2 ).WaterOutletNodeNum ).MassFlowRate = ColdWaterMassFlowRate;
+		Node( WaterCoil( 2 ).WaterOutletNodeNum ).MassFlowRateMaxAvail = ColdWaterMassFlowRate;
+
+		Node( WaterCoil( 1 ).AirInletNodeNum ).MassFlowRate = AirMassFlow;
+		Node( WaterCoil( 1 ).AirInletNodeNum ).MassFlowRateMaxAvail = AirMassFlow;
+
+		Node( WaterCoil( 1 ).WaterInletNodeNum ).Temp = 60.0;
+		Node( WaterCoil( 1 ).WaterInletNodeNum ).MassFlowRate = HotWaterMassFlowRate;
+		Node( WaterCoil( 1 ).WaterInletNodeNum ).MassFlowRateMaxAvail = HotWaterMassFlowRate;
+		Node( WaterCoil( 1 ).WaterOutletNodeNum ).MassFlowRate = HotWaterMassFlowRate;
+		Node( WaterCoil( 1 ).WaterOutletNodeNum ).MassFlowRateMaxAvail = HotWaterMassFlowRate;
+		WaterCoil( 1 ).InletWaterMassFlowRate = HotWaterMassFlowRate;
+		WaterCoil( 1 ).MaxWaterMassFlowRate = HotWaterMassFlowRate;
+
+		for ( int l = 1; l <= TotNumLoops; ++l ) {
+			auto & loop( PlantLoop( l ) );
+			loop.LoopSide.allocate( 2 );
+			auto & loopside( PlantLoop( l ).LoopSide( 1 ) );
+			loopside.TotalBranches = 1;
+			loopside.Branch.allocate( 1 );
+			auto & loopsidebranch( PlantLoop( l ).LoopSide( 1 ).Branch( 1 ) );
+			loopsidebranch.TotalComponents = 1;
+			loopsidebranch.Comp.allocate( 1 );
+		}
+
+		TempControlType.allocate( 1 );
+		TempControlType( 1 ) = 4;
+
+		WaterCoil( 2 ).WaterLoopNum = 1;
+		WaterCoil( 2 ).WaterLoopSide = 1;
+		WaterCoil( 2 ).WaterLoopBranchNum = 1;
+		WaterCoil( 2 ).WaterLoopCompNum = 1;
+
+		WaterCoil( 1 ).WaterLoopNum = 2;
+		WaterCoil( 1 ).WaterLoopSide = 1;
+		WaterCoil( 1 ).WaterLoopBranchNum = 1;
+		WaterCoil( 1 ).WaterLoopCompNum = 1;
+
+		PlantLoop( 2 ).Name = "ChilledWaterLoop";
+		PlantLoop( 2 ).FluidName = "ChilledWater";
+		PlantLoop( 2 ).FluidIndex = 1;
+		PlantLoop( 2 ).FluidName = "WATER";
+		PlantLoop( 2 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).Name = WaterCoil( 2 ).Name;
+		PlantLoop( 2 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).TypeOf_Num = WaterCoil_Cooling;
+		PlantLoop( 2 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).NodeNumIn = WaterCoil( 2 ).WaterInletNodeNum;
+		PlantLoop( 2 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).NodeNumOut = WaterCoil( 2 ).WaterOutletNodeNum;
+		PlantLoop( 2 ).LoopSide( 1 ).FlowLock = 0;
+
+		PlantLoop( 1 ).Name = "HotWaterLoop";
+		PlantLoop( 1 ).FluidName = "HotWater";
+		PlantLoop( 1 ).FluidIndex = 1;
+		PlantLoop( 1 ).FluidName = "WATER";
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).Name = WaterCoil( 1 ).Name;
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).TypeOf_Num = WaterCoil_SimpleHeating;
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).NodeNumIn = WaterCoil( 1 ).WaterInletNodeNum;
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).NodeNumOut = WaterCoil( 1 ).WaterOutletNodeNum;
+		PlantLoop( 1 ).LoopSide( 1 ).FlowLock = 0;
+
+		FanCoil( 1 ).CWLoopNum = 2;
+		FanCoil( 1 ).HWLoopNum = 1;
+		FanCoil( 1 ).CWLoopSide = 1;
+		FanCoil( 1 ).HWLoopSide = 1;
+		FanCoil( 1 ).HotPlantOutletNode = WaterCoil( 1 ).WaterOutletNodeNum;
+		FanCoil( 1 ).ColdPlantOutletNode = WaterCoil( 2 ).WaterOutletNodeNum;
+		FanCoil( 1 ).CWBranchNum = 1;
+		FanCoil( 1 ).CWCompNum = 1;
+		FanCoil( 1 ).HWBranchNum = 1;
+		FanCoil( 1 ).HWCompNum = 1;
+
+		CoolingLoad = false;
+		HeatingLoad = true;
+		ZoneSysEnergyDemand.allocate( 1 );
+		ZoneSysEnergyDemand( 1 ).RemainingOutputReqToCoolSP = 8000.0;
+		ZoneSysEnergyDemand( 1 ).RemainingOutputReqToHeatSP = 4000.0;
+		FanCoil( 1 ).SpeedFanSel = 2;
+		QUnitOut = 0.0;
+		QZnReq = 4000.0;
+
+		MyUAAndFlowCalcFlag.allocate( 2 );
+		MyUAAndFlowCalcFlag( 1 ) = true;
+		MyUAAndFlowCalcFlag( 2 ) = true;
+		DataGlobals::DoingSizing = true;
+
+		LocalTurnFansOff = false;
+		LocalTurnFansOn = true;
+
+		DataEnvironment::Month = 1;
+		DataEnvironment::DayOfMonth = 21;
+		DataGlobals::HourOfDay = 1;
+		DataEnvironment::DSTIndicator = 0;
+		DataEnvironment::DayOfWeek = 2;
+		DataEnvironment::HolidayIndex = 0;
+		DataEnvironment::DayOfYear_Schedule = JulianDay( Month, DayOfMonth, 1 );
+		UpdateScheduleValues();
+
+		// Normal heating simulation for fan coil with constant fan, variable water flow
+		Sim4PipeFanCoil( FanCoilNum, ZoneNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, LatOutputProvided );
+		EXPECT_NEAR( QZnReq, QUnitOut, 5.0 );
+		FirstHVACIteration = false;
+		PlantLoop( 1 ).LoopSide( 1 ).FlowLock = 1;
+		Node( FanCoil( 1 ).HotControlNode ).MassFlowRate = 0.2;
+		// Simulate with flow lock on and locked flow > demand flow; bypass extra flow
+		Sim4PipeFanCoil( FanCoilNum, ZoneNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, LatOutputProvided );
+		EXPECT_NEAR( QZnReq, QUnitOut, 5.0 );
+		EXPECT_NEAR( 55.31, Node( 10 ).Temp, 0.1 );
+		// heating simulation with flow lock on and locked flow < flow required for load; use locked flow
+		Node( FanCoil( 1 ).HotControlNode ).MassFlowRate = 0.05;
+		Sim4PipeFanCoil( FanCoilNum, ZoneNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, LatOutputProvided );
+		EXPECT_NEAR( 3780.0, QUnitOut, 5.0 );
+		// normal heating, no flow lock, heating capacity exceeded
+		QZnReq = 5000.0;
+		ZoneSysEnergyDemand( 1 ).RemainingOutputReqToHeatSP = 5000.00;
+		PlantLoop( 1 ).LoopSide( 1 ).FlowLock = 0;
+		Sim4PipeFanCoil( FanCoilNum, ZoneNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, LatOutputProvided );
+		EXPECT_NEAR( 4420.0, QUnitOut, 5.0 );
+
+		DataGlobals::DoingSizing = false;
+		PlantLoop.deallocate();
+		ZoneSysEnergyDemand.deallocate();
+		FanCoil.deallocate();
+		Node.deallocate();
+		WaterCoil.deallocate();
+		ZoneEquipConfig.deallocate();
+		Zone.deallocate();
+		CoilNames.deallocate();
+	}
+	TEST_F( EnergyPlusFixture, ElectricCoilFanCoilHeatingTest ) {
+
+		int FanCoilNum( 1 );
+		int ZoneNum( 1 );
+		int ControlledZoneNum( 1 );
+		bool FirstHVACIteration( true );
+		bool ErrorsFound( false );
+		Real64 QZnReq( 0.0 );
+		Real64 HotWaterMassFlowRate( 0.0 );
+		Real64 ColdWaterMassFlowRate( 0.0 );
+		Real64 QUnitOut( 0.0 );
+		Real64 AirMassFlow( 0.0 );
+		Real64 MaxAirMassFlow( 0.0 );
+		Real64 LatOutputProvided( 0.0 );
+
+		DataEnvironment::OutBaroPress = 101325.0;
+		DataEnvironment::StdRhoAir = 1.20;
+		WaterCoils::GetWaterCoilsInputFlag = true;
+		NumCoils = 0;
+		DataGlobals::NumOfTimeStepInHour = 1;
+		DataGlobals::TimeStep = 1;
+		DataGlobals::MinutesPerTimeStep = 60;
+
+		InitializePsychRoutines();
+
+		std::string const idf_objects = delimited_string( {
+			"	Version,8.3;",
+			"	Zone,",
+			"	EAST ZONE, !- Name",
+			"	0, !- Direction of Relative North { deg }",
+			"	0, !- X Origin { m }",
+			"	0, !- Y Origin { m }",
+			"	0, !- Z Origin { m }",
+			"	1, !- Type",
+			"	1, !- Multiplier",
+			"	autocalculate, !- Ceiling Height { m }",
+			"	autocalculate; !- Volume { m3 }",
+			"	ZoneHVAC:EquipmentConnections,",
+			"	EAST ZONE, !- Zone Name",
+			"	Zone1Equipment, !- Zone Conditioning Equipment List Name",
+			"	Zone1Inlets, !- Zone Air Inlet Node or NodeList Name",
+			"	Zone1Exhausts, !- Zone Air Exhaust Node or NodeList Name",
+			"	Zone 1 Node, !- Zone Air Node Name",
+			"	Zone 1 Outlet Node;      !- Zone Return Air Node Name",
+			"	ZoneHVAC:EquipmentList,",
+			"	Zone1Equipment, !- Name",
+			"	ZoneHVAC:FourPipeFanCoil, !- Zone Equipment 1 Object Type",
+			"	Zone1FanCoil, !- Zone Equipment 1 Name",
+			"	1, !- Zone Equipment 1 Cooling Sequence",
+			"	1;                       !- Zone Equipment 1 Heating or No - Load Sequence",
+			"   NodeList,",
+			"	Zone1Inlets, !- Name",
+			"	Zone1FanCoilAirOutletNode;  !- Node 1 Name",
+			"	NodeList,",
+			"	Zone1Exhausts, !- Name",
+			"	Zone1FanCoilAirInletNode; !- Node 1 Name",
+			"	OutdoorAir:NodeList,",
+			"	Zone1FanCoilOAInNode;    !- Node or NodeList Name 1",
+			"	OutdoorAir:Mixer,",
+			"	Zone1FanCoilOAMixer, !- Name",
+			"	Zone1FanCoilOAMixerOutletNode, !- Mixed Air Node Name",
+			"	Zone1FanCoilOAInNode, !- Outdoor Air Stream Node Name",
+			"	Zone1FanCoilExhNode, !- Relief Air Stream Node Name",
+			"	Zone1FanCoilAirInletNode; !- Return Air Stream Node Name",
+			"	Schedule:Constant,",
+			"	FanAndCoilAvailSched, !- Name",
+			"	FRACTION, !- Schedule Type",
+			"	1;        !- TimeStep Value",
+			"	ScheduleTypeLimits,",
+			"	Fraction, !- Name",
+			"	0.0, !- Lower Limit Value",
+			"	1.0, !- Upper Limit Value",
+			"	CONTINUOUS;              !- Numeric Type",
+			"	Fan:OnOff,",
+			"	Zone1FanCoilFan, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Name",
+			"	0.5, !- Fan Total Efficiency",
+			"	75.0, !- Pressure Rise { Pa }",
+			"	0.6, !- Maximum Flow Rate { m3 / s }",
+			"	0.9, !- Motor Efficiency",
+			"	1.0, !- Motor In Airstream Fraction",
+			"	Zone1FanCoilOAMixerOutletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilFanOutletNode, !- Air Outlet Node Name",
+			"	, !- Fan Power Ratio Function of Speed Ratio Curve Name",
+			"	;                        !- Fan Efficiency Ratio Function of Speed Ratio Curve Name	",
+			"	Coil:Cooling:Water,",
+			"	Zone1FanCoilCoolingCoil, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Namev",
+			"	0.0002, !- Design Water Flow Rate { m3 / s }",
+			"	0.5000, !- Design Air Flow Rate { m3 / s }",
+			"	7.22,   !- Design Inlet Water Temperature { Cv }",
+			"	24.340, !- Design Inlet Air Temperature { C }",
+			"	14.000, !- Design Outlet Air Temperature { C }",
+			"	0.0095, !- Design Inlet Air Humidity Ratio { kgWater / kgDryAir }",
+			"	0.0090, !- Design Outlet Air Humidity Ratio { kgWater / kgDryAir }",
+			"	Zone1FanCoilChWInletNode, !- Water Inlet Node Name",
+			"	Zone1FanCoilChWOutletNode, !- Water Outlet Node Name",
+			"	Zone1FanCoilFanOutletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilCCOutletNode, !- Air Outlet Node Name",
+			"	SimpleAnalysis, !- Type of Analysis",
+			"	CrossFlow;               !- Heat Exchanger Configuration",
+			"	Coil:Heating:Electric,",
+			"   Zone1FanCoilHeatingCoil, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Name",
+			"	0.9,   !- Efficiency",
+			"	4500., !- Nominal Capacity",
+			"	Zone1FanCoilCCOutletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilAirOutletNode; !- Air Outlet Node Name",
+			"	ZoneHVAC:FourPipeFanCoil,",
+			"	Zone1FanCoil, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Name",
+			"	ConstantFanVariableFlow, !- Capacity Control Method",
+			"	0.5, !- Maximum Supply Air Flow Rate { m3 / s }",
+			"	0.3, !- Low Speed Supply Air Flow Ratio",
+			"	0.6, !- Medium Speed Supply Air Flow Ratio",
+			"	0.0, !- Maximum Outdoor Air Flow Rate { m3 / s }",
+			"	FanAndCoilAvailSched, !- Outdoor Air Schedule Name",
+			"	Zone1FanCoilAirInletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilAirOutletNode, !- Air Outlet Node Name",
+			"	OutdoorAir:Mixer, !- Outdoor Air Mixer Object Type",
+			"	Zone1FanCoilOAMixer, !- Outdoor Air Mixer Name",
+			"	Fan:OnOff, !- Supply Air Fan Object Type",
+			"	Zone1FanCoilFan, !- Supply Air Fan Name",
+			"	Coil:Cooling:Water, !- Cooling Coil Object Type",
+			"	Zone1FanCoilCoolingCoil, !- Cooling Coil Name",
+			"	0.00014, !- Maximum Cold Water Flow Rate { m3 / s }",
+			"	0.0, !- Minimum Cold Water Flow Rate { m3 / s }",
+			"	0.001, !- Cooling Convergence Tolerance",
+			"	Coil:Heating:Electric, !- Heating Coil Object Type",
+			"	Zone1FanCoilHeatingCoil, !- Heating Coil Name",
+			"	0.00014, !- Maximum Hot Water Flow Rate { m3 / s }",
+			"	0.0, !- Minimum Hot Water Flow Rate { m3 / s }",
+			"	0.001; !- Heating Convergence Tolerance",
+
+		} );
+
+		ASSERT_FALSE( process_idf( idf_objects ) );
+
+		GetZoneData( ErrorsFound );
+		EXPECT_EQ( "EAST ZONE", Zone( 1 ).Name );
+
+		GetZoneEquipmentData1();
+		ProcessScheduleInput();
+		ScheduleInputProcessed = true;
+		GetFanInput();
+		EXPECT_EQ( DataHVACGlobals::FanType_SimpleOnOff, Fan( 1 ).FanType_Num );
+
+		GetFanCoilUnits();
+		EXPECT_EQ( "CONSTANTFANVARIABLEFLOW", FanCoil( 1 ).CapCtrlMeth );
+		EXPECT_EQ( "OUTDOORAIR:MIXER", FanCoil( 1 ).OAMixType );
+		EXPECT_EQ( "FAN:ONOFF", FanCoil( 1 ).FanType );
+		EXPECT_EQ( "COIL:COOLING:WATER", FanCoil( 1 ).CCoilType );
+		EXPECT_EQ( "COIL:HEATING:ELECTRIC", FanCoil( 1 ).HCoilType );
+
+		TotNumLoops = 1;
+		PlantLoop.allocate( TotNumLoops );
+
+		AirMassFlow = 0.60;
+		MaxAirMassFlow = 0.60;
+		// heating load only
+		ColdWaterMassFlowRate = 0.0;
+		HotWaterMassFlowRate = 0.14;
+
+		Node( OAMixer( 1 ).RetNode ).MassFlowRate = AirMassFlow;
+		Node( OAMixer( 1 ).RetNode ).MassFlowRateMax = MaxAirMassFlow;
+
+		Node( OAMixer( 1 ).RetNode ).Temp = 22.0;
+		Node( OAMixer( 1 ).RetNode ).Enthalpy = 36000;
+		Node( OAMixer( 1 ).RetNode ).HumRat = PsyWFnTdbH( Node( OAMixer( 1 ).RetNode ).Temp, Node( OAMixer( 1 ).RetNode ).Enthalpy );
+
+		Node( OAMixer( 1 ).InletNode ).Temp = 10.0;
+		Node( OAMixer( 1 ).InletNode ).Enthalpy = 18000;
+		Node( OAMixer( 1 ).InletNode ).HumRat = PsyWFnTdbH( Node( OAMixer( 1 ).InletNode ).Temp, Node( OAMixer( 1 ).InletNode ).Enthalpy );
+
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRate = AirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMin = AirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMinAvail = AirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMax = MaxAirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMaxAvail = MaxAirMassFlow;
+
+		FanCoil( 1 ).OutAirMassFlow = 0.0;
+		FanCoil( 1 ).MaxAirMassFlow = MaxAirMassFlow;
+		FanCoil( 1 ).MaxColdWaterFlow = 0.14;
+		FanCoil( 1 ).MaxHotWaterFlow = 0.14;
+
+		Node( FanCoil( 1 ).OutsideAirNode ).MassFlowRateMax = 0.0;
+		Node( FanCoil( 1 ).ColdControlNode ).MassFlowRateMax = 0.14;
+		Node( FanCoil( 1 ).ColdControlNode ).MassFlowRateMaxAvail = 0.14;
+
+
+		Fan( 1 ).InletAirMassFlowRate = AirMassFlow;
+		Fan( 1 ).MaxAirMassFlowRate = MaxAirMassFlow;
+
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRate = AirMassFlow;
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRateMin = AirMassFlow;
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRateMax = AirMassFlow;
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRateMaxAvail = AirMassFlow;
+
+		WaterCoil( 1 ).UACoilTotal = 470.0;
+		WaterCoil( 1 ).UACoilExternal = 611.0;
+		WaterCoil( 1 ).UACoilInternal = 2010.0;
+		WaterCoil( 1 ).TotCoilOutsideSurfArea = 50.0;
+
+		Node( WaterCoil( 1 ).AirInletNodeNum ).MassFlowRate = AirMassFlow;
+		Node( WaterCoil( 1 ).AirInletNodeNum ).MassFlowRateMin = AirMassFlow;
+		Node( WaterCoil( 1 ).AirInletNodeNum ).MassFlowRateMax = AirMassFlow;
+		Node( WaterCoil( 1 ).AirInletNodeNum ).MassFlowRateMaxAvail = AirMassFlow;
+
+		WaterCoil( 1 ).InletWaterMassFlowRate = ColdWaterMassFlowRate;
+		WaterCoil( 1 ).MaxWaterMassFlowRate = ColdWaterMassFlowRate;
+		Node( WaterCoil( 1 ).WaterInletNodeNum ).MassFlowRate = ColdWaterMassFlowRate;
+		Node( WaterCoil( 1 ).WaterInletNodeNum ).MassFlowRateMaxAvail = ColdWaterMassFlowRate;
+		Node( WaterCoil( 1 ).WaterInletNodeNum ).Temp = 6.0;
+		Node( WaterCoil( 1 ).WaterOutletNodeNum ).MassFlowRate = ColdWaterMassFlowRate;
+		Node( WaterCoil( 1 ).WaterOutletNodeNum ).MassFlowRateMaxAvail = ColdWaterMassFlowRate;
+
+		Node( WaterCoil( 1 ).AirInletNodeNum ).MassFlowRate = AirMassFlow;
+		Node( WaterCoil( 1 ).AirInletNodeNum ).MassFlowRateMaxAvail = AirMassFlow;
+
+		for ( int l = 1; l <= TotNumLoops; ++l ) {
+			auto & loop( PlantLoop( l ) );
+			loop.LoopSide.allocate( 2 );
+			auto & loopside( PlantLoop( l ).LoopSide( 1 ) );
+			loopside.TotalBranches = 1;
+			loopside.Branch.allocate( 1 );
+			auto & loopsidebranch( PlantLoop( l ).LoopSide( 1 ).Branch( 1 ) );
+			loopsidebranch.TotalComponents = 1;
+			loopsidebranch.Comp.allocate( 1 );
+		}
+
+		TempControlType.allocate( 1 );
+		TempControlType( 1 ) = 4;
+
+		WaterCoil( 1 ).WaterLoopNum = 1;
+		WaterCoil( 1 ).WaterLoopSide = 1;
+		WaterCoil( 1 ).WaterLoopBranchNum = 1;
+		WaterCoil( 1 ).WaterLoopCompNum = 1;
+
+
+		PlantLoop( 1 ).Name = "ChilledWaterLoop";
+		PlantLoop( 1 ).FluidName = "ChilledWater";
+		PlantLoop( 1 ).FluidIndex = 1;
+		PlantLoop( 1 ).FluidName = "WATER";
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).Name = WaterCoil( 1 ).Name;
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).TypeOf_Num = WaterCoil_Cooling;
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).NodeNumIn = WaterCoil( 1 ).WaterInletNodeNum;
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).NodeNumOut = WaterCoil( 1 ).WaterOutletNodeNum;
+		PlantLoop( 1 ).LoopSide( 1 ).FlowLock = 0;
+
+		FanCoil( 1 ).CWLoopNum = 1;
+		FanCoil( 1 ).HWLoopNum = 0;
+		FanCoil( 1 ).CWLoopSide = 1;
+		FanCoil( 1 ).HWLoopSide = 0;
+		FanCoil( 1 ).HotPlantOutletNode = 0;
+		FanCoil( 1 ).ColdPlantOutletNode = WaterCoil( 1 ).WaterOutletNodeNum;
+		FanCoil( 1 ).CWBranchNum = 1;
+		FanCoil( 1 ).CWCompNum = 1;
+		FanCoil( 1 ).HWBranchNum = 0;
+		FanCoil( 1 ).HWCompNum = 0;
+
+		CoolingLoad = false;
+		HeatingLoad = true;
+		ZoneSysEnergyDemand.allocate( 1 );
+		ZoneSysEnergyDemand( 1 ).RemainingOutputReqToCoolSP = 8000.0;
+		ZoneSysEnergyDemand( 1 ).RemainingOutputReqToHeatSP = 4000.0;
+		FanCoil( 1 ).SpeedFanSel = 2;
+		QUnitOut = 0.0;
+		QZnReq = 4000.0;
+
+		MyUAAndFlowCalcFlag.allocate( 2 );
+		MyUAAndFlowCalcFlag( 1 ) = true;
+		MyUAAndFlowCalcFlag( 2 ) = true;
+		DataGlobals::DoingSizing = true;
+
+		LocalTurnFansOff = false;
+		LocalTurnFansOn = true;
+
+		DataEnvironment::Month = 1;
+		DataEnvironment::DayOfMonth = 21;
+		DataGlobals::HourOfDay = 1;
+		DataEnvironment::DSTIndicator = 0;
+		DataEnvironment::DayOfWeek = 2;
+		DataEnvironment::HolidayIndex = 0;
+		DataEnvironment::DayOfYear_Schedule = JulianDay( Month, DayOfMonth, 1 );
+		UpdateScheduleValues();
+
+		// Normal heating simulation for fan coil with constant fan, electric heating
+		Sim4PipeFanCoil( FanCoilNum, ZoneNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, LatOutputProvided );
+		EXPECT_NEAR( QZnReq, QUnitOut, 5.0 );
+		// normal heating, heating capacity exceeded
+		QZnReq = 5000.0;
+		ZoneSysEnergyDemand( 1 ).RemainingOutputReqToHeatSP = 5000.00;
+		Sim4PipeFanCoil( FanCoilNum, ZoneNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, LatOutputProvided );
+		EXPECT_NEAR( 4575.0, QUnitOut, 5.0 );
+
+		DataGlobals::DoingSizing = false;
+		PlantLoop.deallocate();
+		ZoneSysEnergyDemand.deallocate();
+		FanCoil.deallocate();
+		Node.deallocate();
+		WaterCoil.deallocate();
+		ZoneEquipConfig.deallocate();
+		Zone.deallocate();
+		CoilNames.deallocate();
+	}
+	TEST_F( EnergyPlusFixture, ConstantFanVariableFlowFanCoilCoolingTest ) {
+
+		int FanCoilNum( 1 );
+		int ZoneNum( 1 );
+		int ControlledZoneNum( 1 );
+		bool FirstHVACIteration( true );
+		bool ErrorsFound( false );
+		Real64 QZnReq( 0.0 );
+		Real64 HotWaterMassFlowRate( 0.0 );
+		Real64 ColdWaterMassFlowRate( 0.0 );
+		Real64 QUnitOut( 0.0 );
+		Real64 AirMassFlow( 0.0 );
+		Real64 MaxAirMassFlow( 0.0 );
+		Real64 LatOutputProvided( 0.0 );
+
+		DataEnvironment::OutBaroPress = 101325.0;
+		DataEnvironment::StdRhoAir = 1.20;
+		WaterCoils::GetWaterCoilsInputFlag = true;
+		NumCoils = 0;
+		DataGlobals::NumOfTimeStepInHour = 1;
+		DataGlobals::TimeStep = 1;
+		DataGlobals::MinutesPerTimeStep = 60;
+
+		InitializePsychRoutines();
+
+		std::string const idf_objects = delimited_string( {
+			"	Version,8.3;",
+			"	Zone,",
+			"	EAST ZONE, !- Name",
+			"	0, !- Direction of Relative North { deg }",
+			"	0, !- X Origin { m }",
+			"	0, !- Y Origin { m }",
+			"	0, !- Z Origin { m }",
+			"	1, !- Type",
+			"	1, !- Multiplier",
+			"	autocalculate, !- Ceiling Height { m }",
+			"	autocalculate; !- Volume { m3 }",
+			"	ZoneHVAC:EquipmentConnections,",
+			"	EAST ZONE, !- Zone Name",
+			"	Zone1Equipment, !- Zone Conditioning Equipment List Name",
+			"	Zone1Inlets, !- Zone Air Inlet Node or NodeList Name",
+			"	Zone1Exhausts, !- Zone Air Exhaust Node or NodeList Name",
+			"	Zone 1 Node, !- Zone Air Node Name",
+			"	Zone 1 Outlet Node;      !- Zone Return Air Node Name",
+			"	ZoneHVAC:EquipmentList,",
+			"	Zone1Equipment, !- Name",
+			"	ZoneHVAC:FourPipeFanCoil, !- Zone Equipment 1 Object Type",
+			"	Zone1FanCoil, !- Zone Equipment 1 Name",
+			"	1, !- Zone Equipment 1 Cooling Sequence",
+			"	1;                       !- Zone Equipment 1 Heating or No - Load Sequence",
+			"   NodeList,",
+			"	Zone1Inlets, !- Name",
+			"	Zone1FanCoilAirOutletNode;  !- Node 1 Name",
+			"	NodeList,",
+			"	Zone1Exhausts, !- Name",
+			"	Zone1FanCoilAirInletNode; !- Node 1 Name",
+			"	OutdoorAir:NodeList,",
+			"	Zone1FanCoilOAInNode;    !- Node or NodeList Name 1",
+			"	OutdoorAir:Mixer,",
+			"	Zone1FanCoilOAMixer, !- Name",
+			"	Zone1FanCoilOAMixerOutletNode, !- Mixed Air Node Name",
+			"	Zone1FanCoilOAInNode, !- Outdoor Air Stream Node Name",
+			"	Zone1FanCoilExhNode, !- Relief Air Stream Node Name",
+			"	Zone1FanCoilAirInletNode; !- Return Air Stream Node Name",
+			"	Schedule:Compact,",
+			"	FanAndCoilAvailSched, !- Name",
+			"	Fraction, !- Schedule Type Limits Name",
+			"	Through: 12/31, !- Field 1",
+			"	For: AllDays, !- Field 2",
+			"	Until: 24:00, 1.0;        !- Field 3",
+			"	ScheduleTypeLimits,",
+			"	Fraction, !- Name",
+			"	0.0, !- Lower Limit Value",
+			"	1.0, !- Upper Limit Value",
+			"	CONTINUOUS;              !- Numeric Type",
+			"   Fan:OnOff,",
+			"	Zone1FanCoilFan, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Name",
+			"	0.5, !- Fan Total Efficiency",
+			"	75.0, !- Pressure Rise { Pa }",
+			"	0.6, !- Maximum Flow Rate { m3 / s }",
+			"	0.9, !- Motor Efficiency",
+			"	1.0, !- Motor In Airstream Fraction",
+			"	Zone1FanCoilOAMixerOutletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilFanOutletNode, !- Air Outlet Node Name",
+			"	, !- Fan Power Ratio Function of Speed Ratio Curve Name",
+			"	;                        !- Fan Efficiency Ratio Function of Speed Ratio Curve Name	",
+			"	Coil:Cooling:Water,",
+			"	Zone1FanCoilCoolingCoil, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Namev",
+			"	0.0002, !- Design Water Flow Rate { m3 / s }",
+			"	0.5000, !- Design Air Flow Rate { m3 / s }",
+			"	7.22,   !- Design Inlet Water Temperature { Cv }",
+			"	24.340, !- Design Inlet Air Temperature { C }",
+			"	14.000, !- Design Outlet Air Temperature { C }",
+			"	0.0095, !- Design Inlet Air Humidity Ratio { kgWater / kgDryAir }",
+			"	0.0090, !- Design Outlet Air Humidity Ratio { kgWater / kgDryAir }",
+			"	Zone1FanCoilChWInletNode, !- Water Inlet Node Name",
+			"	Zone1FanCoilChWOutletNode, !- Water Outlet Node Name",
+			"	Zone1FanCoilFanOutletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilCCOutletNode, !- Air Outlet Node Name",
+			"	SimpleAnalysis, !- Type of Analysis",
+			"	CrossFlow;               !- Heat Exchanger Configuration",
+			"	Coil:Heating:Water,",
+			"   Zone1FanCoilHeatingCoil, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Name",
+			"	150.0,   !- U - Factor Times Area Value { W / K }",
+			"	0.00014, !- Maximum Water Flow Rate { m3 / s }",
+			"	Zone1FanCoilHWInletNode, !- Water Inlet Node Name",
+			"	Zone1FanCoilHWOutletNode, !- Water Outlet Node Name",
+			"	Zone1FanCoilCCOutletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilAirOutletNode, !- Air Outlet Node Name",
+			"	UFactorTimesAreaAndDesignWaterFlowRate, !- Performance Input Method",
+			"	autosize, !- Rated Capacity { W }",
+			"	82.2, !- Rated Inlet Water Temperature { C }",
+			"	16.6, !- Rated Inlet Air Temperature { C }",
+			"	71.1, !- Rated Outlet Water Temperature { C }",
+			"	32.2, !- Rated Outlet Air Temperature { C }",
+			"	;     !- Rated Ratio for Air and Water Convection",
+			"	ZoneHVAC:FourPipeFanCoil,",
+			"	Zone1FanCoil, !- Name",
+			"	FanAndCoilAvailSched, !- Availability Schedule Name",
+			"	ConstantFanVariableFlow, !- Capacity Control Method",
+			"	0.5, !- Maximum Supply Air Flow Rate { m3 / s }",
+			"	0.3, !- Low Speed Supply Air Flow Ratio",
+			"	0.6, !- Medium Speed Supply Air Flow Ratio",
+			"	0.1, !- Maximum Outdoor Air Flow Rate { m3 / s }",
+			"	FanAndCoilAvailSched, !- Outdoor Air Schedule Name",
+			"	Zone1FanCoilAirInletNode, !- Air Inlet Node Name",
+			"	Zone1FanCoilAirOutletNode, !- Air Outlet Node Name",
+			"	OutdoorAir:Mixer, !- Outdoor Air Mixer Object Type",
+			"	Zone1FanCoilOAMixer, !- Outdoor Air Mixer Name",
+			"	Fan:OnOff, !- Supply Air Fan Object Type",
+			"	Zone1FanCoilFan, !- Supply Air Fan Name",
+			"	Coil:Cooling:Water, !- Cooling Coil Object Type",
+			"	Zone1FanCoilCoolingCoil, !- Cooling Coil Name",
+			"	0.00014, !- Maximum Cold Water Flow Rate { m3 / s }",
+			"	0.0, !- Minimum Cold Water Flow Rate { m3 / s }",
+			"	0.001, !- Cooling Convergence Tolerance",
+			"	Coil:Heating:Water, !- Heating Coil Object Type",
+			"	Zone1FanCoilHeatingCoil, !- Heating Coil Name",
+			"	0.00014, !- Maximum Hot Water Flow Rate { m3 / s }",
+			"	0.0, !- Minimum Hot Water Flow Rate { m3 / s }",
+			"	0.001; !- Heating Convergence Tolerance",
+
+		} );
+
+		ASSERT_FALSE( process_idf( idf_objects ) );
+
+		GetZoneData( ErrorsFound );
+		EXPECT_EQ( "EAST ZONE", Zone( 1 ).Name );
+
+		GetZoneEquipmentData1();
+		ProcessScheduleInput();
+		ScheduleInputProcessed = true;
+		GetFanInput();
+		EXPECT_EQ( DataHVACGlobals::FanType_SimpleOnOff, Fan( 1 ).FanType_Num );
+
+		GetFanCoilUnits();
+		EXPECT_EQ( "CONSTANTFANVARIABLEFLOW", FanCoil( 1 ).CapCtrlMeth );
+		EXPECT_EQ( "OUTDOORAIR:MIXER", FanCoil( 1 ).OAMixType );
+		EXPECT_EQ( "FAN:ONOFF", FanCoil( 1 ).FanType );
+		EXPECT_EQ( "COIL:COOLING:WATER", FanCoil( 1 ).CCoilType );
+		EXPECT_EQ( "COIL:HEATING:WATER", FanCoil( 1 ).HCoilType );
+
+		TotNumLoops = 2;
+		PlantLoop.allocate( TotNumLoops );
+
+		AirMassFlow = 0.60;
+		MaxAirMassFlow = 0.60;
+
+		// cooling load only
+		HotWaterMassFlowRate = 0.0;
+		ColdWaterMassFlowRate = 0.14;
+
+		Node( OAMixer( 1 ).RetNode ).MassFlowRate = AirMassFlow;
+		Node( OAMixer( 1 ).RetNode ).MassFlowRateMax = MaxAirMassFlow;
+
+		Node( OAMixer( 1 ).RetNode ).Temp = 24.0;
+		Node( OAMixer( 1 ).RetNode ).Enthalpy = 36000;
+		Node( OAMixer( 1 ).RetNode ).HumRat = PsyWFnTdbH( Node( OAMixer( 1 ).RetNode ).Temp, Node( OAMixer( 1 ).RetNode ).Enthalpy );
+
+		Node( OAMixer( 1 ).InletNode ).Temp = 30.0;
+		Node( OAMixer( 1 ).InletNode ).Enthalpy = 53000;
+		Node( OAMixer( 1 ).InletNode ).HumRat = PsyWFnTdbH( Node( OAMixer( 1 ).InletNode ).Temp, Node( OAMixer( 1 ).InletNode ).Enthalpy );
+
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRate = AirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMin = AirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMinAvail = AirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMax = MaxAirMassFlow;
+		Node( FanCoil( 1 ).AirInNode ).MassFlowRateMaxAvail = MaxAirMassFlow;
+
+		FanCoil( 1 ).OutAirMassFlow = 0.0;
+		FanCoil( 1 ).MaxAirMassFlow = MaxAirMassFlow;
+		FanCoil( 1 ).MaxColdWaterFlow = 0.14;
+		FanCoil( 1 ).MaxHotWaterFlow = 0.14;
+
+		Node( FanCoil( 1 ).OutsideAirNode ).MassFlowRateMax = 0.0;
+		Node( FanCoil( 1 ).ColdControlNode ).MassFlowRateMax = 0.14;
+		Node( FanCoil( 1 ).HotControlNode ).MassFlowRateMax = 0.14;
+		Node( FanCoil( 1 ).ColdControlNode ).MassFlowRateMaxAvail = 0.14;
+		Node( FanCoil( 1 ).HotControlNode ).MassFlowRateMaxAvail = 0.14;
+
+		Fan( 1 ).InletAirMassFlowRate = AirMassFlow;
+		Fan( 1 ).MaxAirMassFlowRate = MaxAirMassFlow;
+
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRate = AirMassFlow;
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRateMin = AirMassFlow;
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRateMax = AirMassFlow;
+		Node( Fan( 1 ).InletNodeNum ).MassFlowRateMaxAvail = AirMassFlow;
+
+		WaterCoil( 2 ).UACoilTotal = 470.0;
+		WaterCoil( 2 ).UACoilExternal = 611.0;
+		WaterCoil( 2 ).UACoilInternal = 2010.0;
+		WaterCoil( 2 ).TotCoilOutsideSurfArea = 50.0;
+
+		Node( WaterCoil( 2 ).AirInletNodeNum ).MassFlowRate = AirMassFlow;
+		Node( WaterCoil( 2 ).AirInletNodeNum ).MassFlowRateMin = AirMassFlow;
+		Node( WaterCoil( 2 ).AirInletNodeNum ).MassFlowRateMax = AirMassFlow;
+		Node( WaterCoil( 2 ).AirInletNodeNum ).MassFlowRateMaxAvail = AirMassFlow;
+
+		WaterCoil( 2 ).InletWaterMassFlowRate = ColdWaterMassFlowRate;
+		WaterCoil( 2 ).MaxWaterMassFlowRate = ColdWaterMassFlowRate;
+		Node( WaterCoil( 2 ).WaterInletNodeNum ).MassFlowRate = ColdWaterMassFlowRate;
+		Node( WaterCoil( 2 ).WaterInletNodeNum ).MassFlowRateMaxAvail = ColdWaterMassFlowRate;
+		Node( WaterCoil( 2 ).WaterInletNodeNum ).Temp = 6.0;
+		Node( WaterCoil( 2 ).WaterOutletNodeNum ).MassFlowRate = ColdWaterMassFlowRate;
+		Node( WaterCoil( 2 ).WaterOutletNodeNum ).MassFlowRateMaxAvail = ColdWaterMassFlowRate;
+
+		Node( WaterCoil( 1 ).AirInletNodeNum ).MassFlowRate = AirMassFlow;
+		Node( WaterCoil( 1 ).AirInletNodeNum ).MassFlowRateMaxAvail = AirMassFlow;
+
+		Node( WaterCoil( 1 ).WaterInletNodeNum ).Temp = 60.0;
+		Node( WaterCoil( 1 ).WaterInletNodeNum ).MassFlowRate = HotWaterMassFlowRate;
+		Node( WaterCoil( 1 ).WaterInletNodeNum ).MassFlowRateMaxAvail = HotWaterMassFlowRate;
+		Node( WaterCoil( 1 ).WaterOutletNodeNum ).MassFlowRate = HotWaterMassFlowRate;
+		Node( WaterCoil( 1 ).WaterOutletNodeNum ).MassFlowRateMaxAvail = HotWaterMassFlowRate;
+		WaterCoil( 1 ).InletWaterMassFlowRate = HotWaterMassFlowRate;
+		WaterCoil( 1 ).MaxWaterMassFlowRate = HotWaterMassFlowRate;
+
+		for ( int l = 1; l <= TotNumLoops; ++l ) {
+			auto & loop( PlantLoop( l ) );
+			loop.LoopSide.allocate( 2 );
+			auto & loopside( PlantLoop( l ).LoopSide( 1 ) );
+			loopside.TotalBranches = 1;
+			loopside.Branch.allocate( 1 );
+			auto & loopsidebranch( PlantLoop( l ).LoopSide( 1 ).Branch( 1 ) );
+			loopsidebranch.TotalComponents = 1;
+			loopsidebranch.Comp.allocate( 1 );
+		}
+
+		TempControlType.allocate( 1 );
+		TempControlType( 1 ) = 4;
+
+		WaterCoil( 2 ).WaterLoopNum = 1;
+		WaterCoil( 2 ).WaterLoopSide = 1;
+		WaterCoil( 2 ).WaterLoopBranchNum = 1;
+		WaterCoil( 2 ).WaterLoopCompNum = 1;
+
+		WaterCoil( 1 ).WaterLoopNum = 2;
+		WaterCoil( 1 ).WaterLoopSide = 1;
+		WaterCoil( 1 ).WaterLoopBranchNum = 1;
+		WaterCoil( 1 ).WaterLoopCompNum = 1;
+
+		PlantLoop( 2 ).Name = "ChilledWaterLoop";
+		PlantLoop( 2 ).FluidName = "ChilledWater";
+		PlantLoop( 2 ).FluidIndex = 1;
+		PlantLoop( 2 ).FluidName = "WATER";
+		PlantLoop( 2 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).Name = WaterCoil( 2 ).Name;
+		PlantLoop( 2 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).TypeOf_Num = WaterCoil_Cooling;
+		PlantLoop( 2 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).NodeNumIn = WaterCoil( 2 ).WaterInletNodeNum;
+		PlantLoop( 2 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).NodeNumOut = WaterCoil( 2 ).WaterOutletNodeNum;
+		PlantLoop( 2 ).LoopSide( 1 ).FlowLock = 0;
+
+		PlantLoop( 1 ).Name = "HotWaterLoop";
+		PlantLoop( 1 ).FluidName = "HotWater";
+		PlantLoop( 1 ).FluidIndex = 1;
+		PlantLoop( 1 ).FluidName = "WATER";
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).Name = WaterCoil( 1 ).Name;
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).TypeOf_Num = WaterCoil_SimpleHeating;
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).NodeNumIn = WaterCoil( 1 ).WaterInletNodeNum;
+		PlantLoop( 1 ).LoopSide( 1 ).Branch( 1 ).Comp( 1 ).NodeNumOut = WaterCoil( 1 ).WaterOutletNodeNum;
+		PlantLoop( 1 ).LoopSide( 1 ).FlowLock = 0;
+
+		FanCoil( 1 ).CWLoopNum = 2;
+		FanCoil( 1 ).HWLoopNum = 1;
+		FanCoil( 1 ).CWLoopSide = 1;
+		FanCoil( 1 ).HWLoopSide = 1;
+		FanCoil( 1 ).HotPlantOutletNode = WaterCoil( 1 ).WaterOutletNodeNum;
+		FanCoil( 1 ).ColdPlantOutletNode = WaterCoil( 2 ).WaterOutletNodeNum;
+		FanCoil( 1 ).CWBranchNum = 1;
+		FanCoil( 1 ).CWCompNum = 1;
+		FanCoil( 1 ).HWBranchNum = 1;
+		FanCoil( 1 ).HWCompNum = 1;
+
+		HeatingLoad = false;
+		CoolingLoad = true;
+		ZoneSysEnergyDemand.allocate( 1 );
+		ZoneSysEnergyDemand( 1 ).RemainingOutputReqToCoolSP = -4000.00;
+		ZoneSysEnergyDemand( 1 ).RemainingOutputReqToHeatSP = -8000.0;
+		FanCoil( 1 ).SpeedFanSel = 2;
+		QUnitOut = 0.0;
+		QZnReq = -4000.0;
+
+		MyUAAndFlowCalcFlag.allocate( 2 );
+		MyUAAndFlowCalcFlag( 1 ) = true;
+		MyUAAndFlowCalcFlag( 2 ) = true;
+		DataGlobals::DoingSizing = true;
+
+		LocalTurnFansOff = false;
+		LocalTurnFansOn = true;
+
+		DataEnvironment::Month = 1;
+		DataEnvironment::DayOfMonth = 21;
+		DataGlobals::HourOfDay = 1;
+		DataEnvironment::DSTIndicator = 0;
+		DataEnvironment::DayOfWeek = 2;
+		DataEnvironment::HolidayIndex = 0;
+		DataEnvironment::DayOfYear_Schedule = JulianDay( Month, DayOfMonth, 1 );
+		UpdateScheduleValues();
+		// normal cooling simulation for constant fan variable flow fan coil
+		Sim4PipeFanCoil( FanCoilNum, ZoneNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, LatOutputProvided );
+		EXPECT_NEAR( QZnReq, QUnitOut, 5.0 );
+		FirstHVACIteration = false;
+		PlantLoop( 2 ).LoopSide( 1 ).FlowLock = 1;
+		Node( FanCoil( 1 ).ColdControlNode ).MassFlowRate = 0.2;
+		// cooling simulation with flow lock on and locked flow > flow that meets load; bypass extra flow
+		Sim4PipeFanCoil( FanCoilNum, ZoneNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, LatOutputProvided );
+		EXPECT_NEAR( QZnReq, QUnitOut, 5.0 );
+		EXPECT_NEAR( 10.86, Node(13).Temp, 0.1 );
+		// cooling simulation with flow lock on and locked flow < flow required for load; use locked flow
+		Node( FanCoil( 1 ).ColdControlNode ).MassFlowRate = 0.05;
+		Sim4PipeFanCoil( FanCoilNum, ZoneNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, LatOutputProvided );
+		EXPECT_NEAR( -3000.0, QUnitOut, 5.0 );
+		// normal cooling, no flow lock, cooling capacity exceeded
+		QZnReq = -5000.0;
+		ZoneSysEnergyDemand( 1 ).RemainingOutputReqToCoolSP = -5000.00;
+		PlantLoop( 2 ).LoopSide( 1 ).FlowLock = 0;
+		Sim4PipeFanCoil( FanCoilNum, ZoneNum, ControlledZoneNum, FirstHVACIteration, QUnitOut, LatOutputProvided );
+		EXPECT_NEAR( -4420.0, QUnitOut, 5.0 );
+		DataGlobals::DoingSizing = false;
+		PlantLoop.deallocate();
+		ZoneSysEnergyDemand.deallocate();
+		FanCoil.deallocate();
+		Node.deallocate();
+		WaterCoil.deallocate();
+		ZoneEquipConfig.deallocate();
+		Zone.deallocate();
+		CoilNames.deallocate();
 
+	}
+	TEST_F( EnergyPlusFixture, FanCoil_ASHRAE90VariableFan ) {
 
 		int FanCoilNum( 1 );
 		int ZoneNum( 1 );
@@ -1114,5 +2119,4 @@ namespace EnergyPlus {
 		CoilNames.deallocate();
 
 	}
-
-}
+}
\ No newline at end of file
diff --git a/tst/EnergyPlus/unit/HVACUnitarySystem.unit.cc b/tst/EnergyPlus/unit/HVACUnitarySystem.unit.cc
index d46a460cdad..6460954f1c3 100644
--- a/tst/EnergyPlus/unit/HVACUnitarySystem.unit.cc
+++ b/tst/EnergyPlus/unit/HVACUnitarySystem.unit.cc
@@ -234,13 +234,24 @@ TEST_F( EnergyPlusFixture, SetOnOffMassFlowRateTest )
 	HeatingLoad = true;
 	CoolingLoad = false;
 	SetOnOffMassFlowRate( UnitarySysNum, OnOffAirFlowRatio, PartLoadRatio );
+	EXPECT_EQ( 0.6, CompOffMassFlow );
+	EXPECT_EQ( 1.2, CompOnMassFlow );
 	EXPECT_EQ( 0.6, MSHPMassFlowRateLow );
 	EXPECT_EQ( 1.2, MSHPMassFlowRateHigh );
+
+	PartLoadRatio = 0.5;
+	SetOnOffMassFlowRate( UnitarySysNum, OnOffAirFlowRatio, PartLoadRatio );
+	EXPECT_EQ( 0.6, CompOffMassFlow );
+	EXPECT_EQ( 1.2, CompOnMassFlow );
+	EXPECT_EQ( 0.6, MSHPMassFlowRateLow );
+	EXPECT_EQ( 1.2, MSHPMassFlowRateHigh );
+
+	PartLoadRatio = 1.0;
 	MoistureLoad = 0.0;
 	UnitarySystem( UnitarySysNum ).Humidistat = false;
 	UnitarySystem( UnitarySysNum ).DehumidControlType_Num = DataSizing::None;
 
-	// cycling fan mode should drop to idle flow rate as speed = 1
+	// cycling fan mode should drop to idle flow rate only below speed = 1
 	UnitarySystem( UnitarySysNum ).FanOpMode = CycFanCycCoil;
 
 	UnitarySystem( UnitarySysNum ).HeatingSpeedNum = 1;
@@ -248,7 +259,9 @@ TEST_F( EnergyPlusFixture, SetOnOffMassFlowRateTest )
 	HeatingLoad = true;
 	CoolingLoad = false;
 	SetOnOffMassFlowRate( UnitarySysNum, OnOffAirFlowRatio, PartLoadRatio );
-	EXPECT_EQ( 0.20, MSHPMassFlowRateLow );
+	EXPECT_EQ( 0.25, CompOffMassFlow );
+	EXPECT_EQ( 0.25, CompOnMassFlow );
+	EXPECT_EQ( 0.25, MSHPMassFlowRateLow );
 	EXPECT_EQ( 0.25, MSHPMassFlowRateHigh );
 
 	// cooling load at various speeds
@@ -274,10 +287,12 @@ TEST_F( EnergyPlusFixture, SetOnOffMassFlowRateTest )
 	HeatingLoad = false;
 	CoolingLoad = true;
 	SetOnOffMassFlowRate( UnitarySysNum, OnOffAirFlowRatio, PartLoadRatio );
+	EXPECT_EQ( 0.2, CompOffMassFlow ); // CompOffMassFlow equal to idle mass flow rate
+	EXPECT_EQ( 0.3, CompOnMassFlow );
 	EXPECT_EQ( 0.2, MSHPMassFlowRateLow );
 	EXPECT_EQ( 0.3, MSHPMassFlowRateHigh );
 
-	// constant fan mode should not drop to idle flow rate as speed = 1
+	// constant fan mode should not drop to idle flow rate at speed = 1
 	UnitarySystem( UnitarySysNum ).FanOpMode = ContFanCycCoil;
 
 	UnitarySystem( UnitarySysNum ).HeatingSpeedNum = 0;
@@ -285,6 +300,8 @@ TEST_F( EnergyPlusFixture, SetOnOffMassFlowRateTest )
 	HeatingLoad = false;
 	CoolingLoad = true;
 	SetOnOffMassFlowRate( UnitarySysNum, OnOffAirFlowRatio, PartLoadRatio );
+	EXPECT_EQ( 0.3, CompOffMassFlow ); // CompOffMassFlow equal to speed 1 mass flow rate
+	EXPECT_EQ( 0.3, CompOnMassFlow );
 	EXPECT_EQ( 0.3, MSHPMassFlowRateLow );
 	EXPECT_EQ( 0.3, MSHPMassFlowRateHigh );
 
@@ -294,6 +311,8 @@ TEST_F( EnergyPlusFixture, SetOnOffMassFlowRateTest )
 	HeatingLoad = false;
 	CoolingLoad = false;
 	SetOnOffMassFlowRate( UnitarySysNum, OnOffAirFlowRatio, PartLoadRatio );
+	EXPECT_EQ( 0.2, CompOffMassFlow ); // CompOffMassFlow equal to spped 1 mass flow rate
+	EXPECT_EQ( 0.2, CompOnMassFlow );
 	EXPECT_EQ( 0.2, MSHPMassFlowRateLow );
 	EXPECT_EQ( 0.2, MSHPMassFlowRateHigh );
 
@@ -4076,7 +4095,7 @@ TEST_F( EnergyPlusFixture, UnitarySystem_MultiSpeedCoils_SingleMode ) {
 	DataEnvironment::OutBaroPress = 101325.0;
 
 	SimUnitarySystem( UnitarySystem( 1 ).Name, FirstHVACIteration, UnitarySystem( 1 ).ControlZoneNum, ZoneEquipList( 1 ).EquipIndex( 1 ), true, _, _, _, _ );
-	EXPECT_NEAR( 0.153581, UnitarySystem( UnitarySysNum ).CycRatio, 0.0001 ); // cycling ratio
+	EXPECT_NEAR( 0.16177, UnitarySystem( UnitarySysNum ).CycRatio, 0.0001 ); // cycling ratio
 	EXPECT_EQ( 1, UnitarySystem( UnitarySysNum ).HeatingSpeedNum );
 	EXPECT_EQ( 0.0, UnitarySystem( UnitarySysNum ).HeatingSpeedRatio );
 
diff --git a/tst/EnergyPlus/unit/HVACVariableRefrigerantFlow.unit.cc b/tst/EnergyPlus/unit/HVACVariableRefrigerantFlow.unit.cc
index 0ed3063b694..15591a104c3 100644
--- a/tst/EnergyPlus/unit/HVACVariableRefrigerantFlow.unit.cc
+++ b/tst/EnergyPlus/unit/HVACVariableRefrigerantFlow.unit.cc
@@ -79,6 +79,7 @@
 #include <DataEnvironment.hh>
 #include <DataGlobals.hh>
 #include <DataHeatBalance.hh>
+#include <DataHeatBalFanSys.hh>
 #include <DataHVACGlobals.hh>
 #include <DataLoopNode.hh>
 #include <DataPlant.hh>
@@ -106,6 +107,7 @@ using namespace EnergyPlus::DataAirSystems;
 using namespace EnergyPlus::DataEnvironment;
 using namespace EnergyPlus::DataGlobals;
 using namespace EnergyPlus::DataHeatBalance;
+using namespace EnergyPlus::DataHeatBalFanSys;
 using namespace EnergyPlus::DataHVACGlobals;
 using namespace EnergyPlus::DataLoopNode;
 using namespace EnergyPlus::DataPlant;
@@ -1094,8 +1096,30 @@ namespace EnergyPlus {
 		DefrostWatts = VRF( VRFCond ).VRFCondRTF * ( VRF( VRFCond ).HeatingCapacity / 1.01667 ) * VRF( VRFCond ).DefrostFraction;
 		ASSERT_EQ( DefrostWatts, VRF( VRFCond ).DefrostPower ); // defrost power calculation check
 
-		// clean up
-		ZoneSysEnergyDemand.deallocate();
+		// test other ThermostatPriority control types
+		ZoneThermostatSetPointHi.allocate( 1 );
+		ZoneThermostatSetPointHi = 24.0;
+		ZoneThermostatSetPointLo.allocate( 1 );
+		ZoneThermostatSetPointLo = 21.0;
+		TempControlType.allocate( 1 );
+		TempControlType = 4;
+		ZT.allocate( 1 );
+		ZT = 25.0;
+
+		ZoneSysEnergyDemand( CurZoneNum ).RemainingOutputRequired = -VRF( VRFCond ).CoolingCapacity; // set load equal to the VRF cooling capacity
+		ZoneSysEnergyDemand( CurZoneNum ).RemainingOutputReqToCoolSP = -VRF( VRFCond ).CoolingCapacity;
+		ZoneSysEnergyDemand( CurZoneNum ).RemainingOutputReqToHeatSP = -VRF( VRFCond ).CoolingCapacity - 1000.0;
+
+		Node( VRF( VRFCond ).CondenserNodeNum ).Temp = 35.0; // AHRI condition at 95 F db
+		Node( VRFTU( VRFTUNum ).VRFTUInletNodeNum ).Temp = 25.0;
+		Node( VRFTU( VRFTUNum ).VRFTUOAMixerOANodeNum ).Temp = 35.0; // AHRI condition at 95 F db
+		Node( VRFTU( VRFTUNum ).VRFTUOAMixerOANodeNum ).HumRat = 0.01; // don't care
+
+		VRF( VRFCond ).MasterZonePtr = 0;
+		VRF( VRFCond ).MasterZoneTUIndex = 0;
+		VRF( VRFCond ).ThermostatPriority = ThermostatOffsetPriority;
+		SimulateVRF( VRFTU( VRFTUNum ).Name, CurZoneNum, FirstHVACIteration, SysOutputProvided, LatOutputProvided, ZoneEquipList( CurZoneEqNum ).EquipIndex( EquipPtr ) );
+		EXPECT_NEAR( SysOutputProvided, ZoneSysEnergyDemand( CurZoneNum ).RemainingOutputRequired, 5.0 ); // system output should be less than 0
 
 	}
 
diff --git a/tst/EnergyPlus/unit/MixedAir.unit.cc b/tst/EnergyPlus/unit/MixedAir.unit.cc
index 443ae05d697..30ba81cc894 100644
--- a/tst/EnergyPlus/unit/MixedAir.unit.cc
+++ b/tst/EnergyPlus/unit/MixedAir.unit.cc
@@ -65,6 +65,7 @@
 #include <EnergyPlus/MixedAir.hh>
 #include <EnergyPlus/DataContaminantBalance.hh>
 #include <EnergyPlus/DataAirLoop.hh>
+#include <EnergyPlus/DataAirSystems.hh>
 #include <EnergyPlus/DataGlobals.hh>
 #include <EnergyPlus/DataSizing.hh>
 #include <EnergyPlus/DataHeatBalance.hh>
@@ -76,6 +77,7 @@
 #include <EnergyPlus/DataZoneEquipment.hh>
 #include <EnergyPlus/DataLoopNode.hh>
 #include <EnergyPlus/DataZoneEnergyDemands.hh>
+#include <EnergyPlus/DataZoneControls.hh>
 #include <EnergyPlus/Psychrometrics.hh>
 
 #include "Fixtures/EnergyPlusFixture.hh"
@@ -84,6 +86,7 @@
 using namespace EnergyPlus::MixedAir;
 using namespace EnergyPlus::DataContaminantBalance;
 using namespace EnergyPlus::DataAirLoop;
+using namespace EnergyPlus::DataAirSystems;
 using namespace EnergyPlus::DataSizing;
 using namespace EnergyPlus::DataHeatBalance;
 using namespace EnergyPlus::ScheduleManager;
@@ -91,6 +94,7 @@ using namespace EnergyPlus::DataEnvironment;
 using namespace EnergyPlus::DataZoneEquipment;
 using namespace EnergyPlus::DataLoopNode;
 using namespace EnergyPlus::DataZoneEnergyDemands;
+using namespace EnergyPlus::DataZoneControls;
 using namespace EnergyPlus::HeatBalanceManager;
 using namespace EnergyPlus::Humidifiers;
 using namespace EnergyPlus::SizingManager;
@@ -859,7 +863,7 @@ namespace EnergyPlus {
 			"    Through: 12/31,          !- Field 1",
 			"    For: Alldays,            !- Field 2",
 			"    Until: 24:00, 1.0;       !- Field 3",
-			
+
 			"ScheduleTypeLimits,",
 			"    Fraction,                !- Name",
 			"    0.0,                     !- Lower Limit Value",
@@ -948,8 +952,8 @@ namespace EnergyPlus {
 		Real64 WaterConsumptionRate( 0.0 ); // water use rate of the humidifier
 		Real64 ElecPowerInput( 0.0 ); // electric use rate of the humidifier
 
-		AirLoopControlInfo.allocate( AirloopNum ); 
-		AirLoopFlow.allocate( AirloopNum ); 
+		AirLoopControlInfo.allocate( AirloopNum );
+		AirLoopFlow.allocate( AirloopNum );
 		AirLoopFlow( AirloopNum ).DesSupply = 1.0;
 		DataEnvironment::StdRhoAir = 1.2;
 		DataEnvironment::OutBaroPress = 101250.0;
@@ -990,7 +994,7 @@ namespace EnergyPlus {
 		ElecPowerInput = ( WaterConsumptionRate / Humidifiers::Humidifier( HumNum ).NomCap ) * Humidifiers::Humidifier( HumNum ).NomPower;
 		// Confirm humidifier water consumption calculation
 		EXPECT_EQ( WaterConsumptionRate, Humidifiers::Humidifier( HumNum ).WaterAdd );
-		// confirm that electric energy is used by the humidifier		
+		// confirm that electric energy is used by the humidifier
 		EXPECT_EQ( ElecPowerInput, Humidifiers::Humidifier( HumNum ).ElecUseRate );
 	}
 
@@ -1075,4 +1079,3633 @@ namespace EnergyPlus {
 		EXPECT_NEAR( 0.2408617, OAController( 1 ).OAFractionRpt, 0.00001 );
 
 	}
+
+	TEST_F( EnergyPlusFixture, MixedAir_ControllerTypeTest ) {
+
+		int OAControllerNum = 1;
+
+		OAController.allocate( OAControllerNum );
+		Node.allocate( 4 );
+
+		OAController( OAControllerNum ).ControllerType_Num = ControllerOutsideAir;
+		OAController( OAControllerNum ).OANode = 1;
+		OAController( OAControllerNum ).InletNode = 2;
+		OAController( OAControllerNum ).RelNode = 3;
+		OAController( OAControllerNum ).RetNode = 4;
+		OAController( OAControllerNum ).OAMassFlow = 0.1;
+		OAController( OAControllerNum ).ExhMassFlow = 0.0;
+		OAController( OAControllerNum ).RelMassFlow = max( OAController( OAControllerNum ).OAMassFlow - OAController( OAControllerNum ).ExhMassFlow, 0.0 );
+		Node( OAController( OAControllerNum ).RetNode ).MassFlowRate = 0.2;
+		Node( OAController( OAControllerNum ).RelNode ).MassFlowRate = OAController( OAControllerNum ).RelMassFlow;
+		Node( OAController( OAControllerNum ).InletNode ).CO2 = 600.0;
+		Node( OAController( OAControllerNum ).RelNode ).CO2 = 500.0;
+		OutdoorCO2 = 400.0;
+
+		Node( OAController( OAControllerNum ).InletNode ).GenContam = 0.5;
+		Node( OAController( OAControllerNum ).RelNode ).GenContam = 0.3;
+		OutdoorGC = 0.1;
+
+		Contaminant.CO2Simulation = true;
+		Contaminant.GenericContamSimulation = true;
+
+		UpdateOAController( OAControllerNum );
+		// Expect no value changes of relief node due to no actions.
+		EXPECT_NEAR( 500.0, Node( OAController( OAControllerNum ).RelNode ).CO2, 0.00001 );
+		EXPECT_NEAR( 0.3, Node( OAController( OAControllerNum ).RelNode ).GenContam, 0.00001 );
+
+		Contaminant.CO2Simulation = false;
+		Contaminant.GenericContamSimulation = false;
+		OAController.deallocate( );
+		Node.deallocate( );
+
+	}
+
+
+	TEST_F( EnergyPlusFixture, MixedAir_MissingHIghRHControlInputTest )
+	{
+		std::string const idf_objects = delimited_string({
+			"Version,8.3;",
+
+			"  OutdoorAir:Node,",
+			"    Outside Air Inlet Node 1; !- Name",
+
+			"  Schedule:Constant,",
+			"    Min OA Sched,             !- Name",
+			"     Any Number,              !- Schedule Type Limits Name",
+			"     0.5;                     !- Value",
+
+			"  ScheduleTypeLimits,",
+			"    Any Number;              !- Name",
+
+			"  Controller:OutdoorAir,",
+			"    OA Controller 1,          !- Name",
+			"    Relief Air Outlet Node 1, !- Relief Air Outlet Node Name",
+			"    VAV Sys 1 Inlet Node,     !- Return Air Node Name",
+			"    Mixed Air Node 1,         !- Mixed Air Node Name",
+			"    Outside Air Inlet Node 1, !- Actuator Node Name",
+			"    autosize,                 !- Minimum Outdoor Air Flow Rate {m3/s}",
+			"    autosize,                 !- Maximum Outdoor Air Flow Rate {m3/s}",
+			"    FixedDryBulb,             !- Economizer Control Type",
+			"    ModulateFlow,             !- Economizer Control Action Type",
+			"    ,                         !- Economizer Maximum Limit Dry-Bulb Temperature {C}",
+			"    ,                         !- Economizer Maximum Limit Enthalpy {J/kg}",
+			"    ,                         !- Economizer Maximum Limit Dewpoint Temperature {C}",
+			"    ,                         !- Electronic Enthalpy Limit Curve Name",
+			"    ,                         !- Economizer Minimum Limit Dry-Bulb Temperature {C}",
+			"    NoLockout,                !- Lockout Type",
+			"    ProportionalMinimum,      !- Minimum Limit Type",
+			"    Min OA Sched,             !- Minimum Outdoor Air Schedule Name",
+			"    ,                         !- Minimum Fraction of Outdoor Air Schedule Name",
+			"    ,                         !- Maximum Fraction of Outdoor Air Schedule Name",
+			"    ,                         !- Mechanical Ventilation Controller Name",
+			"    ,                         !- Time of Day Economizer Control Schedule Name",
+			"    Yes,                      !- High Humidity Control",
+			"    Zone1,                    !- Humidistat Control Zone Name",
+			"    1;                        !- High Humidity Outdoor Air Flow Ratio",
+		});
+
+		ASSERT_FALSE( process_idf( idf_objects ) );
+
+		compare_err_stream( "" ); // just for debugging
+
+		bool ErrorsFound( false ); // If errors detected in input
+		int ControllerNum( 0 ); // Controller number
+		int NumArg( 0 );
+		int NumNums( 0 );
+		int NumAlphas( 0 );
+		int IOStat( 0 );
+		std::string const CurrentModuleObject = CurrentModuleObjects( CMO_OAController );
+
+		InputProcessor::GetObjectDefMaxArgs( CurrentModuleObjects( CMO_OAController ), NumArg, NumAlphas, NumNums );
+
+		Array1D< Real64 > NumArray( NumNums, 0.0 );
+		Array1D_string AlphArray( NumAlphas );
+		Array1D_string cAlphaFields( NumAlphas );
+		Array1D_string cNumericFields( NumNums );
+		Array1D_bool lAlphaBlanks( NumAlphas, true );
+		Array1D_bool lNumericBlanks( NumNums, true );
+
+		NumOAControllers = InputProcessor::GetNumObjectsFound( CurrentModuleObject );
+		OAController.allocate( NumOAControllers );
+
+		ControllerNum = 1;
+		Zone.allocate( 1 );
+		Zone( 1 ).Name = "ZONE1";
+		NumOfZones = 1;
+		ZoneEquipConfig.allocate( 1 );
+		ZoneEquipConfig( 1 ).ActualZoneNum = 1;
+		ZoneEquipConfig( 1 ).ZoneNode = 2;
+		ZoneEquipConfig( 1 ).AirLoopNum = 1;
+		PrimaryAirSystem.allocate( 1 );
+		PrimaryAirSystem( 1 ).NumBranches = 1;
+		PrimaryAirSystem( 1 ).Branch.allocate( 1 );
+		PrimaryAirSystem( 1 ).Branch( 1 ).Comp.allocate( 1 );
+		PrimaryAirSystem( 1 ).Branch( 1 ).TotalComponents = 1;
+		PrimaryAirSystem( 1 ).Branch( 1 ).Comp( 1 ).Name = "OASysName";
+		PrimaryAirSystem( 1 ).Branch( 1 ).Comp( 1 ).TypeOf = "AirLoopHVAC:OutdoorAirSystem";
+		OutsideAirSys.allocate( 1 );
+		OutsideAirSys( 1 ).Name = "OASysName";
+		OutsideAirSys( 1 ).NumControllers = 1;
+		OutsideAirSys( 1 ).ControllerType.allocate( 1 );
+		OutsideAirSys( 1 ).ControllerType( 1 ) = "Controller:OutdoorAir";
+		OutsideAirSys( 1 ).ControllerName.allocate( 1 );
+		OutsideAirSys( 1 ).ControllerName( 1 ) = "OA Controller 1";
+		DataAirLoop::NumOASystems = 1;
+		HumidityControlZone.allocate( 1 );
+		HumidityControlZone( 1 ).ActualZoneNum = 1;
+		NumHumidityControlZones = 1;
+
+		InputProcessor::GetObjectItem( CurrentModuleObject, ControllerNum, AlphArray, NumAlphas, NumArray, NumNums, IOStat, lNumericBlanks, lAlphaBlanks, cAlphaFields, cNumericFields );
+
+		ProcessOAControllerInputs( CurrentModuleObject, ControllerNum, AlphArray, NumAlphas, NumArray, NumNums, lNumericBlanks, lAlphaBlanks, cAlphaFields, cNumericFields, ErrorsFound );
+		//compare_err_stream( "" ); // just for debugging
+
+		EXPECT_FALSE( ErrorsFound );
+		EXPECT_FALSE( OAController( ControllerNum ).ModifyDuringHighOAMoisture ); // missing input defaults "Control High Indoor Humidity Based on Outdoor Humidity Ratio" to false
+
+		std::string const error_string = delimited_string( {
+			"   ** Warning ** Controller:OutdoorAir \"OA CONTROLLER 1\", missing field value",
+			"   **   ~~~   ** ...Control High Indoor Humidity Based on Outdoor Humidity Ratio will default to Yes when High Humidity Control= \"Yes\"",
+		} );
+		EXPECT_TRUE( compare_err_stream( error_string, true ) );
+
+	}
+
+	TEST_F( EnergyPlusFixture, MixedAir_MiscGetsPart1 )
+	{
+		std::string const idf_objects = delimited_string( {
+			"Version,8.3;",
+
+			"  OutdoorAir:Node,",
+			"    Outside Air Inlet Node;  !- Name",
+
+			"  Controller:OutdoorAir,",
+			"    OA Controller 1,         !- Name",
+			"    Relief Air Outlet Node,  !- Relief Air Outlet Node Name",
+			"    Air Loop Inlet Node,     !- Return Air Node Name",
+			"    Mixed Air Node,          !- Mixed Air Node Name",
+			"    Outside Air Inlet Node,  !- Actuator Node Name",
+			"    1.0,                     !- Minimum Outdoor Air Flow Rate {m3/s}",
+			"    1.0,                     !- Maximum Outdoor Air Flow Rate {m3/s}",
+			"    NoEconomizer,            !- Economizer Control Type", // Economizer should open for this one, so OA flow should be > min OA
+			"    ModulateFlow,            !- Economizer Control Action Type",
+			"    ,                        !- Economizer Maximum Limit Dry-Bulb Temperature {C}",
+			"    ,                        !- Economizer Maximum Limit Enthalpy {J/kg}",
+			"    ,                        !- Economizer Maximum Limit Dewpoint Temperature {C}",
+			"    ,                        !- Electronic Enthalpy Limit Curve Name",
+			"    ,                        !- Economizer Minimum Limit Dry-Bulb Temperature {C}",
+			"    NoLockout,               !- Lockout Type", // No lockout
+			"    ProportionalMinimum,     !- Minimum Limit Type",
+			"    ,                        !- Minimum Outdoor Air Schedule Name",
+			"    ,                        !- Minimum Fraction of Outdoor Air Schedule Name",
+			"    ,                        !- Maximum Fraction of Outdoor Air Schedule Name",
+			"    ,                        !- Mechanical Ventilation Controller Name",
+			"    ,                        !- Time of Day Economizer Control Schedule Name",
+			"    No,                      !- High Humidity Control",
+			"    ,                        !- Humidistat Control Zone Name",
+			"    ,                        !- High Humidity Outdoor Air Flow Ratio",
+			"    No;                      !- Control High Indoor Humidity Based on Outdoor Humidity Ratio",
+
+			"  HeatExchanger:AirToAir:FlatPlate,",
+			"    OA Heat Exchanger 1,     !- Name",
+			"    ,                        !- Availability Schedule Name",
+			"    ParallelFlow,            !- Flow Arrangement Type",
+			"    No,                      !- Economizer Lockout",
+			"    1,                       !- Ratio of Supply to Secondary hA Values",
+			"    1.0,                     !- Nominal Supply Air Flow Rate{ m3 / s }",
+			"    5,                       !- Nominal Supply Air Inlet Temperature{ C }",
+			"    10,                      !- Nominal Supply Air Outlet Temperature{ C }",
+			"    1.0,                     !- Nominal Secondary Air Flow Rate{ m3 / s }",
+			"    20,                      !- Nominal Secondary Air Inlet Temperature{ C }",
+			"    0,                       !- Nominal Electric Power{ W }",
+			"    Heat Exchanger Outlet Node2, !- Supply Air Inlet Node Name",
+			"    Heat Exchanger Outlet Node,  !- Supply Air Outlet Node Name",
+			"    Relief Air Outlet Node,      !- Secondary Air Inlet Node Name",
+			"    Heat Exchanger Secondary Outlet Node;  !- Secondary Air Outlet Node Name",
+
+			"  HeatExchanger:AirToAir:FlatPlate,",
+			"    OA Heat Exchanger 2,     !- Name",
+			"    ,                        !- Availability Schedule Name",
+			"    ParallelFlow,            !- Flow Arrangement Type",
+			"    No,                      !- Economizer Lockout",
+			"    1,                       !- Ratio of Supply to Secondary hA Values",
+			"    1.0,                     !- Nominal Supply Air Flow Rate{ m3 / s }",
+			"    5,                       !- Nominal Supply Air Inlet Temperature{ C }",
+			"    10,                      !- Nominal Supply Air Outlet Temperature{ C }",
+			"    1.0,                     !- Nominal Secondary Air Flow Rate{ m3 / s }",
+			"    20,                      !- Nominal Secondary Air Inlet Temperature{ C }",
+			"    0,                       !- Nominal Electric Power{ W }",
+			"    Outside Air Inlet Node,  !- Supply Air Inlet Node Name",
+			"    Heat Exchanger Outlet Node2,           !- Supply Air Outlet Node Name",
+			"    Heat Exchanger Secondary Outlet Node,  !- Secondary Air Inlet Node Name",
+			"    Heat Exchanger Secondary Outlet Node2; !- Secondary Air Outlet Node Name",
+
+			"  OutdoorAir:Mixer,",
+			"    OA Mixer,                !- Name",
+			"    Mixed Air Node,          !- Mixed Air Node Name",
+			"    Heat Exchanger Outlet Node, !- Outdoor Air Stream Node Name",
+			"    Relief Air Outlet Node,  !- Relief Air Stream Node Name",
+			"    Air Loop Inlet Node;     !- Return Air Stream Node Name",
+
+			" AirLoopHVAC:ControllerList,",
+			"    OA Sys 1 controller,     !- Name",
+			"    Controller:OutdoorAir,   !- Controller 1 Object Type",
+			"    OA Controller 1;         !- Controller 1 Name",
+
+			" AirLoopHVAC:OutdoorAirSystem:EquipmentList,",
+			"    OA Sys 1 Equipment list, !- Name",
+			"    HeatExchanger:AirToAir:FlatPlate, !- Component 1 Object Type",
+			"    OA Heat Exchanger 2,     !- Component 1 Name",
+			"    HeatExchanger:AirToAir:FlatPlate, !- Component 1 Object Type",
+			"    OA Heat Exchanger 1,     !- Component 1 Name",
+			"    OutdoorAir:Mixer,        !- Component 2 Object Type",
+			"    OA Mixer;                !- Component 2 Name",
+
+			" AirLoopHVAC:OutdoorAirSystem,",
+			"    OA Sys 1, !- Name",
+			"    OA Sys 1 controller,     !- Controller List Name",
+			"    OA Sys 1 Equipment list; !- Outdoor Air Equipment List Name",
+		} );
+
+		ASSERT_FALSE( process_idf( idf_objects ) );
+		GetOAControllerInputs();
+
+		EXPECT_EQ( 1, GetNumOAMixers() );
+		EXPECT_EQ( 1, GetNumOAControllers() );
+		EXPECT_EQ( 3, GetOAMixerReliefNodeNumber( 1 ) );
+		EXPECT_EQ( 1, GetOAMixerIndex( "OA Mixer" ) );
+	}
+
+	TEST_F( EnergyPlusFixture, MixedAir_MiscGetsPart2 )
+	{
+		std::string const idf_objects = delimited_string( {
+
+			"Version,8.4;",
+
+			"SimulationControl,",
+			"    Yes,                     !- Do Zone Sizing Calculation",
+			"    Yes,                     !- Do System Sizing Calculation",
+			"    Yes,                     !- Do Plant Sizing Calculation",
+			"    Yes,                     !- Run Simulation for Sizing Periods",
+			"    No;                      !- Run Simulation for Weather File Run Periods",
+
+			"Building,",
+			"    Fan Coil with DOAS,      !- Name",
+			"    30.,                     !- North Axis {deg}",
+			"    City,                    !- Terrain",
+			"    0.04,                    !- Loads Convergence Tolerance Value",
+			"    0.4,                     !- Temperature Convergence Tolerance Value {deltaC}",
+			"    FullExterior,            !- Solar Distribution",
+			"    25,                      !- Maximum Number of Warmup Days",
+			"    6;                       !- Minimum Number of Warmup Days",
+
+			"Timestep,4;",
+
+			"Site:Location,",
+			"    CHICAGO_IL_USA TMY2-94846,  !- Name",
+			"    41.78,                   !- Latitude {deg}",
+			"    -87.75,                  !- Longitude {deg}",
+			"    -6.00,                   !- Time Zone {hr}",
+			"    190.00;                  !- Elevation {m}",
+
+			"! CHICAGO_IL_USA Annual Cooling 1% Design Conditions, MaxDB=  31.5°C MCWB=  23.0°C",
+			"SizingPeriod:DesignDay,",
+			"    CHICAGO_IL_USA Annual Cooling 1% Design Conditions DB/MCWB,  !- Name",
+			"    7,                       !- Month",
+			"    21,                      !- Day of Month",
+			"    SummerDesignDay,         !- Day Type",
+			"    31.5,                    !- Maximum Dry-Bulb Temperature {C}",
+			"    10.7,                    !- Daily Dry-Bulb Temperature Range {deltaC}",
+			"    ,                        !- Dry-Bulb Temperature Range Modifier Type",
+			"    ,                        !- Dry-Bulb Temperature Range Modifier Day Schedule Name",
+			"    Wetbulb,                 !- Humidity Condition Type",
+			"    23.0,                    !- Wetbulb or DewPoint at Maximum Dry-Bulb {C}",
+			"    ,                        !- Humidity Condition Day Schedule Name",
+			"    ,                        !- Humidity Ratio at Maximum Dry-Bulb {kgWater/kgDryAir}",
+			"    ,                        !- Enthalpy at Maximum Dry-Bulb {J/kg}",
+			"    ,                        !- Daily Wet-Bulb Temperature Range {deltaC}",
+			"    99063.,                  !- Barometric Pressure {Pa}",
+			"    5.3,                     !- Wind Speed {m/s}",
+			"    230,                     !- Wind Direction {deg}",
+			"    No,                      !- Rain Indicator",
+			"    No,                      !- Snow Indicator",
+			"    No,                      !- Daylight Saving Time Indicator",
+			"    ASHRAEClearSky,          !- Solar Model Indicator",
+			"    ,                        !- Beam Solar Day Schedule Name",
+			"    ,                        !- Diffuse Solar Day Schedule Name",
+			"    ,                        !- ASHRAE Clear Sky Optical Depth for Beam Irradiance (taub) {dimensionless}",
+			"    ,                        !- ASHRAE Clear Sky Optical Depth for Diffuse Irradiance (taud) {dimensionless}",
+			"    1.0;                     !- Sky Clearness",
+
+
+			"! CHICAGO_IL_USA Annual Heating 99% Design Conditions DB, MaxDB= -17.3°C",
+			"SizingPeriod:DesignDay,",
+			"    CHICAGO_IL_USA Annual Heating 99% Design Conditions DB,  !- Name",
+			"    1,                       !- Month",
+			"    21,                      !- Day of Month",
+			"    WinterDesignDay,         !- Day Type",
+			"    -17.3,                   !- Maximum Dry-Bulb Temperature {C}",
+			"    0.0,                     !- Daily Dry-Bulb Temperature Range {deltaC}",
+			"    ,                        !- Dry-Bulb Temperature Range Modifier Type",
+			"    ,                        !- Dry-Bulb Temperature Range Modifier Day Schedule Name",
+			"    Wetbulb,                 !- Humidity Condition Type",
+			"    -17.3,                   !- Wetbulb or DewPoint at Maximum Dry-Bulb {C}",
+			"    ,                        !- Humidity Condition Day Schedule Name",
+			"    ,                        !- Humidity Ratio at Maximum Dry-Bulb {kgWater/kgDryAir}",
+			"    ,                        !- Enthalpy at Maximum Dry-Bulb {J/kg}",
+			"    ,                        !- Daily Wet-Bulb Temperature Range {deltaC}",
+			"    99063.,                  !- Barometric Pressure {Pa}",
+			"    4.9,                     !- Wind Speed {m/s}",
+			"    270,                     !- Wind Direction {deg}",
+			"    No,                      !- Rain Indicator",
+			"    No,                      !- Snow Indicator",
+			"    No,                      !- Daylight Saving Time Indicator",
+			"    ASHRAEClearSky,          !- Solar Model Indicator",
+			"    ,                        !- Beam Solar Day Schedule Name",
+			"    ,                        !- Diffuse Solar Day Schedule Name",
+			"    ,                        !- ASHRAE Clear Sky Optical Depth for Beam Irradiance (taub) {dimensionless}",
+			"    ,                        !- ASHRAE Clear Sky Optical Depth for Diffuse Irradiance (taud) {dimensionless}",
+			"    0.0;                     !- Sky Clearness",
+
+			"Site:GroundTemperature:BuildingSurface,21.5,21.4,21.5,21.5,22.0,22.9,23.0,23.1,23.1,22.2,21.7,21.6;",
+
+			"ScheduleTypeLimits,",
+			"    Any Number;              !- Name",
+
+			"ScheduleTypeLimits,",
+			"    Fraction,                !- Name",
+			"    0.0,                     !- Lower Limit Value",
+			"    1.0,                     !- Upper Limit Value",
+			"    CONTINUOUS;              !- Numeric Type",
+
+			"ScheduleTypeLimits,",
+			"    Temperature,             !- Name",
+			"    -60,                     !- Lower Limit Value",
+			"    200,                     !- Upper Limit Value",
+			"    CONTINUOUS,              !- Numeric Type",
+			"    Temperature;             !- Unit Type",
+
+			"ScheduleTypeLimits,",
+			"    Control Type,            !- Name",
+			"    0,                       !- Lower Limit Value",
+			"    4,                       !- Upper Limit Value",
+			"    DISCRETE;                !- Numeric Type",
+
+			"ScheduleTypeLimits,",
+			"    On/Off,                  !- Name",
+			"    0,                       !- Lower Limit Value",
+			"    1,                       !- Upper Limit Value",
+			"    DISCRETE;                !- Numeric Type",
+
+			"ScheduleTypeLimits,",
+			"    FlowRate,                !- Name",
+			"    0.0,                     !- Lower Limit Value",
+			"    10,                      !- Upper Limit Value",
+			"    CONTINUOUS;              !- Numeric Type",
+
+			"ScheduleTypeLimits,",
+			"    HVACTemplate Any Number; !- Name",
+
+			"!-   ===========  ALL OBJECTS IN CLASS: SCHEDULE:COMPACT ===========",
+
+			"Schedule:Compact,",
+			"    OCCUPY-1,                !- Name",
+			"    Fraction,                !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: WeekDays SummerDesignDay CustomDay1 CustomDay2,  !- Field 2",
+			"    Until: 8:00, 0.0,        !- Field 4",
+			"    Until: 11:00, 1.00,      !- Field 6",
+			"    Until: 12:00, 0.80,      !- Field 8",
+			"    Until: 13:00, 0.40,      !- Field 10",
+			"    Until: 14:00, 0.80,      !- Field 12",
+			"    Until: 18:00, 1.00,      !- Field 14",
+			"    Until: 19:00, 0.50,      !- Field 16",
+			"    Until: 21:00, 0.10,      !- Field 18",
+			"    Until: 24:00, 0.0,       !- Field 20",
+			"    For: Weekends WinterDesignDay Holiday,  !- Field 21",
+			"    Until: 24:00, 0.0;       !- Field 23",
+
+			"Schedule:Compact,",
+			"    LIGHTS-1,                !- Name",
+			"    Fraction,                !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: WeekDays SummerDesignDay CustomDay1 CustomDay2,  !- Field 2",
+			"    Until: 8:00, 0.05,       !- Field 4",
+			"    Until: 9:00, 0.9,        !- Field 6",
+			"    Until: 10:00, 0.95,      !- Field 8",
+			"    Until: 11:00, 1.00,      !- Field 10",
+			"    Until: 12:00, 0.95,      !- Field 12",
+			"    Until: 13:00, 0.8,       !- Field 14",
+			"    Until: 14:00, 0.9,       !- Field 16",
+			"    Until: 18:00, 1.00,      !- Field 18",
+			"    Until: 19:00, 0.60,      !- Field 20",
+			"    Until: 21:00, 0.40,      !- Field 22",
+			"    Until: 24:00, 0.05,      !- Field 24",
+			"    For: Weekends WinterDesignDay Holiday,  !- Field 25",
+			"    Until: 24:00, 0.05;      !- Field 27",
+
+			"Schedule:Compact,",
+			"    EQUIP-1,                 !- Name",
+			"    Fraction,                !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: WeekDays SummerDesignDay CustomDay1 CustomDay2,  !- Field 2",
+			"    Until: 8:00, 0.02,       !- Field 4",
+			"    Until: 9:00, 0.4,        !- Field 6",
+			"    Until: 14:00, 0.9,       !- Field 8",
+			"    Until: 15:00, 0.8,       !- Field 10",
+			"    Until: 16:00, 0.7,       !- Field 12",
+			"    Until: 18:00, 0.5,       !- Field 14",
+			"    Until: 21:00, 0.3,       !- Field 16",
+			"    Until: 24:00, 0.02,      !- Field 18",
+			"    For: Weekends WinterDesignDay Holiday,  !- Field 19",
+			"    Until: 24:00, 0.02;      !- Field 21",
+
+			"Schedule:Compact,",
+			"    INFIL-SCH,               !- Name",
+			"    Fraction,                !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: WeekDays CustomDay1 CustomDay2,  !- Field 2",
+			"    Until: 7:00, 1.0,        !- Field 4",
+			"    Until: 21:00, 0.0,       !- Field 6",
+			"    Until: 24:00, 1.0,       !- Field 8",
+			"    For: Weekends Holiday,   !- Field 9",
+			"    Until: 24:00, 1.0,       !- Field 11",
+			"    For: SummerDesignDay,    !- Field 12",
+			"    Until: 24:00, 1.0,       !- Field 14",
+			"    For: WinterDesignDay,    !- Field 15",
+			"    Until: 24:00, 1.0;       !- Field 17",
+
+			"Schedule:Compact,",
+			"    ActSchd,                 !- Name",
+			"    Any Number,              !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: AllDays,            !- Field 2",
+			"    Until: 24:00, 117.239997864;",
+			"                             !- Field 4",
+
+			"Schedule:Compact,",
+			"    ShadeTransSch,           !- Name",
+			"    Fraction,                !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: AllDays,            !- Field 2",
+			"    Until: 24:00, 0.0;       !- Field 4",
+
+			"! For heating, recover 2 hrs early",
+			"Schedule:Compact,",
+			"    Htg-SetP-Sch,            !- Name",
+			"    Temperature,             !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: WeekDays CustomDay1 CustomDay2,  !- Field 2",
+			"    Until: 6:00, 13.0,       !- Field 4",
+			"    Until: 7:00, 18.0,       !- Field 6",
+			"    Until: 21:00, 23.0,      !- Field 8",
+			"    Until: 24:00, 13.0,      !- Field 10",
+			"    For: WeekEnds Holiday,   !- Field 11",
+			"    Until: 24:00, 13.0,      !- Field 13",
+			"    For: SummerDesignDay,    !- Field 14",
+			"    Until: 24:00, 13.0,      !- Field 16",
+			"    For: WinterDesignDay,    !- Field 17",
+			"    Until: 24:00, 23.0;      !- Field 19",
+
+			"! For cooling, recover 1 hr early",
+			"Schedule:Compact,",
+			"    Clg-SetP-Sch,            !- Name",
+			"    Temperature,             !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: WeekDays CustomDay1 CustomDay2,  !- Field 2",
+			"    Until: 7:00, 32.0,       !- Field 4",
+			"    Until: 21:00, 24.0,      !- Field 6",
+			"    Until: 24:00, 32.0,      !- Field 8",
+			"    For: WeekEnds Holiday,   !- Field 9",
+			"    Until: 24:00, 32.0,      !- Field 11",
+			"    For: SummerDesignDay,    !- Field 12",
+			"    Until: 24:00, 24.0,      !- Field 14",
+			"    For: WinterDesignDay,    !- Field 15",
+			"    Until: 24:00, 32.0;      !- Field 17",
+
+			"Schedule:Compact,",
+			"    FanAvailSched,           !- Name",
+			"    Fraction,                !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: WeekDays CustomDay1 CustomDay2,  !- Field 2",
+			"    Until: 7:00, 0.0,        !- Field 4",
+			"    Until: 21:00, 1.0,       !- Field 6",
+			"    Until: 24:00, 0.0,       !- Field 8",
+			"    For: Weekends Holiday,   !- Field 9",
+			"    Until: 24:00, 0.0,       !- Field 11",
+			"    For: SummerDesignDay,    !- Field 12",
+			"    Until: 24:00, 1.0,       !- Field 14",
+			"    For: WinterDesignDay,    !- Field 15",
+			"    Until: 24:00, 1.0;       !- Field 17",
+
+			"Schedule:Compact,",
+			"    HVACTemplate-Always 1,   !- Name",
+			"    HVACTemplate Any Number, !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: AllDays,            !- Field 2",
+			"    Until: 24:00, 1;         !- Field 4",
+
+			"Schedule:Compact,",
+			"    HVACTemplate-Always 4,   !- Name",
+			"    HVACTemplate Any Number, !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: AllDays,            !- Field 2",
+			"    Until: 24:00, 4;         !- Field 4",
+
+			"Schedule:Compact,",
+			"    HVACTemplate-Always 12.2,!- Name",
+			"    HVACTemplate Any Number, !- Schedule Type Limits Name",
+			"    Through: 12/31,          !- Field 1",
+			"    For: AllDays,            !- Field 2",
+			"    Until: 24:00, 12.2;      !- Field 4",
+
+			"Material,",
+			"    WD10,                    !- Name",
+			"    MediumSmooth,            !- Roughness",
+			"    0.667,                   !- Thickness {m}",
+			"    0.115,                   !- Conductivity {W/m-K}",
+			"    513,                     !- Density {kg/m3}",
+			"    1381,                    !- Specific Heat {J/kg-K}",
+			"    0.9,                     !- Thermal Absorptance",
+			"    0.78,                    !- Solar Absorptance",
+			"    0.78;                    !- Visible Absorptance",
+
+			"Material,",
+			"    RG01,                    !- Name",
+			"    Rough,                   !- Roughness",
+			"    1.2700000E-02,           !- Thickness {m}",
+			"    1.442000,                !- Conductivity {W/m-K}",
+			"    881.0000,                !- Density {kg/m3}",
+			"    1674.000,                !- Specific Heat {J/kg-K}",
+			"    0.9000000,               !- Thermal Absorptance",
+			"    0.6500000,               !- Solar Absorptance",
+			"    0.6500000;               !- Visible Absorptance",
+
+			"Material,",
+			"    BR01,                    !- Name",
+			"    VeryRough,               !- Roughness",
+			"    9.4999997E-03,           !- Thickness {m}",
+			"    0.1620000,               !- Conductivity {W/m-K}",
+			"    1121.000,                !- Density {kg/m3}",
+			"    1464.000,                !- Specific Heat {J/kg-K}",
+			"    0.9000000,               !- Thermal Absorptance",
+			"    0.7000000,               !- Solar Absorptance",
+			"    0.7000000;               !- Visible Absorptance",
+
+			"Material,",
+			"    IN46,                    !- Name",
+			"    VeryRough,               !- Roughness",
+			"    7.6200001E-02,           !- Thickness {m}",
+			"    2.3000000E-02,           !- Conductivity {W/m-K}",
+			"    24.00000,                !- Density {kg/m3}",
+			"    1590.000,                !- Specific Heat {J/kg-K}",
+			"    0.9000000,               !- Thermal Absorptance",
+			"    0.5000000,               !- Solar Absorptance",
+			"    0.5000000;               !- Visible Absorptance",
+
+			"Material,",
+			"    WD01,                    !- Name",
+			"    MediumSmooth,            !- Roughness",
+			"    1.9099999E-02,           !- Thickness {m}",
+			"    0.1150000,               !- Conductivity {W/m-K}",
+			"    513.0000,                !- Density {kg/m3}",
+			"    1381.000,                !- Specific Heat {J/kg-K}",
+			"    0.9000000,               !- Thermal Absorptance",
+			"    0.7800000,               !- Solar Absorptance",
+			"    0.7800000;               !- Visible Absorptance",
+
+			"Material,",
+			"    PW03,                    !- Name",
+			"    MediumSmooth,            !- Roughness",
+			"    1.2700000E-02,           !- Thickness {m}",
+			"    0.1150000,               !- Conductivity {W/m-K}",
+			"    545.0000,                !- Density {kg/m3}",
+			"    1213.000,                !- Specific Heat {J/kg-K}",
+			"    0.9000000,               !- Thermal Absorptance",
+			"    0.7800000,               !- Solar Absorptance",
+			"    0.7800000;               !- Visible Absorptance",
+
+			"Material,",
+			"    IN02,                    !- Name",
+			"    Rough,                   !- Roughness",
+			"    9.0099998E-02,           !- Thickness {m}",
+			"    4.3000001E-02,           !- Conductivity {W/m-K}",
+			"    10.00000,                !- Density {kg/m3}",
+			"    837.0000,                !- Specific Heat {J/kg-K}",
+			"    0.9000000,               !- Thermal Absorptance",
+			"    0.7500000,               !- Solar Absorptance",
+			"    0.7500000;               !- Visible Absorptance",
+
+			"Material,",
+			"    GP01,                    !- Name",
+			"    MediumSmooth,            !- Roughness",
+			"    1.2700000E-02,           !- Thickness {m}",
+			"    0.1600000,               !- Conductivity {W/m-K}",
+			"    801.0000,                !- Density {kg/m3}",
+			"    837.0000,                !- Specific Heat {J/kg-K}",
+			"    0.9000000,               !- Thermal Absorptance",
+			"    0.7500000,               !- Solar Absorptance",
+			"    0.7500000;               !- Visible Absorptance",
+
+			"Material,",
+			"    GP02,                    !- Name",
+			"    MediumSmooth,            !- Roughness",
+			"    1.5900001E-02,           !- Thickness {m}",
+			"    0.1600000,               !- Conductivity {W/m-K}",
+			"    801.0000,                !- Density {kg/m3}",
+			"    837.0000,                !- Specific Heat {J/kg-K}",
+			"    0.9000000,               !- Thermal Absorptance",
+			"    0.7500000,               !- Solar Absorptance",
+			"    0.7500000;               !- Visible Absorptance",
+
+			"Material,",
+			"    CC03,                    !- Name",
+			"    MediumRough,             !- Roughness",
+			"    0.1016000,               !- Thickness {m}",
+			"    1.310000,                !- Conductivity {W/m-K}",
+			"    2243.000,                !- Density {kg/m3}",
+			"    837.0000,                !- Specific Heat {J/kg-K}",
+			"    0.9000000,               !- Thermal Absorptance",
+			"    0.6500000,               !- Solar Absorptance",
+			"    0.6500000;               !- Visible Absorptance",
+
+			"Material:NoMass,",
+			"    CP01,                    !- Name",
+			"    Rough,                   !- Roughness",
+			"    0.3670000,               !- Thermal Resistance {m2-K/W}",
+			"    0.9000000,               !- Thermal Absorptance",
+			"    0.7500000,               !- Solar Absorptance",
+			"    0.7500000;               !- Visible Absorptance",
+
+			"Material:NoMass,",
+			"    MAT-CLNG-1,              !- Name",
+			"    Rough,                   !- Roughness",
+			"    0.652259290,             !- Thermal Resistance {m2-K/W}",
+			"    0.65,                    !- Thermal Absorptance",
+			"    0.65,                    !- Solar Absorptance",
+			"    0.65;                    !- Visible Absorptance",
+
+			"Material:AirGap,",
+			"    AL21,                    !- Name",
+			"    0.1570000;               !- Thermal Resistance {m2-K/W}",
+
+			"Material:AirGap,",
+			"    AL23,                    !- Name",
+			"    0.1530000;               !- Thermal Resistance {m2-K/W}",
+
+			"WindowMaterial:Glazing,",
+			"    CLEAR 3MM,               !- Name",
+			"    SpectralAverage,         !- Optical Data Type",
+			"    ,                        !- Window Glass Spectral Data Set Name",
+			"    0.003,                   !- Thickness {m}",
+			"    0.837,                   !- Solar Transmittance at Normal Incidence",
+			"    0.075,                   !- Front Side Solar Reflectance at Normal Incidence",
+			"    0.075,                   !- Back Side Solar Reflectance at Normal Incidence",
+			"    0.898,                   !- Visible Transmittance at Normal Incidence",
+			"    0.081,                   !- Front Side Visible Reflectance at Normal Incidence",
+			"    0.081,                   !- Back Side Visible Reflectance at Normal Incidence",
+			"    0.0,                     !- Infrared Transmittance at Normal Incidence",
+			"    0.84,                    !- Front Side Infrared Hemispherical Emissivity",
+			"    0.84,                    !- Back Side Infrared Hemispherical Emissivity",
+			"    0.9;                     !- Conductivity {W/m-K}",
+
+			"WindowMaterial:Glazing,",
+			"    GREY 3MM,                !- Name",
+			"    SpectralAverage,         !- Optical Data Type",
+			"    ,                        !- Window Glass Spectral Data Set Name",
+			"    0.003,                   !- Thickness {m}",
+			"    0.626,                   !- Solar Transmittance at Normal Incidence",
+			"    0.061,                   !- Front Side Solar Reflectance at Normal Incidence",
+			"    0.061,                   !- Back Side Solar Reflectance at Normal Incidence",
+			"    0.611,                   !- Visible Transmittance at Normal Incidence",
+			"    0.061,                   !- Front Side Visible Reflectance at Normal Incidence",
+			"    0.061,                   !- Back Side Visible Reflectance at Normal Incidence",
+			"    0.0,                     !- Infrared Transmittance at Normal Incidence",
+			"    0.84,                    !- Front Side Infrared Hemispherical Emissivity",
+			"    0.84,                    !- Back Side Infrared Hemispherical Emissivity",
+			"    0.9;                     !- Conductivity {W/m-K}",
+
+			"WindowMaterial:Glazing,",
+			"    CLEAR 6MM,               !- Name",
+			"    SpectralAverage,         !- Optical Data Type",
+			"    ,                        !- Window Glass Spectral Data Set Name",
+			"    0.006,                   !- Thickness {m}",
+			"    0.775,                   !- Solar Transmittance at Normal Incidence",
+			"    0.071,                   !- Front Side Solar Reflectance at Normal Incidence",
+			"    0.071,                   !- Back Side Solar Reflectance at Normal Incidence",
+			"    0.881,                   !- Visible Transmittance at Normal Incidence",
+			"    0.080,                   !- Front Side Visible Reflectance at Normal Incidence",
+			"    0.080,                   !- Back Side Visible Reflectance at Normal Incidence",
+			"    0.0,                     !- Infrared Transmittance at Normal Incidence",
+			"    0.84,                    !- Front Side Infrared Hemispherical Emissivity",
+			"    0.84,                    !- Back Side Infrared Hemispherical Emissivity",
+			"    0.9;                     !- Conductivity {W/m-K}",
+
+			"WindowMaterial:Glazing,",
+			"    LoE CLEAR 6MM,           !- Name",
+			"    SpectralAverage,         !- Optical Data Type",
+			"    ,                        !- Window Glass Spectral Data Set Name",
+			"    0.006,                   !- Thickness {m}",
+			"    0.600,                   !- Solar Transmittance at Normal Incidence",
+			"    0.170,                   !- Front Side Solar Reflectance at Normal Incidence",
+			"    0.220,                   !- Back Side Solar Reflectance at Normal Incidence",
+			"    0.840,                   !- Visible Transmittance at Normal Incidence",
+			"    0.055,                   !- Front Side Visible Reflectance at Normal Incidence",
+			"    0.078,                   !- Back Side Visible Reflectance at Normal Incidence",
+			"    0.0,                     !- Infrared Transmittance at Normal Incidence",
+			"    0.84,                    !- Front Side Infrared Hemispherical Emissivity",
+			"    0.10,                    !- Back Side Infrared Hemispherical Emissivity",
+			"    0.9;                     !- Conductivity {W/m-K}",
+
+			"WindowMaterial:Gas,",
+			"    AIR 6MM,                 !- Name",
+			"    Air,                     !- Gas Type",
+			"    0.0063;                  !- Thickness {m}",
+
+			"WindowMaterial:Gas,",
+			"    AIR 13MM,                !- Name",
+			"    Air,                     !- Gas Type",
+			"    0.0127;                  !- Thickness {m}",
+
+			"WindowMaterial:Gas,",
+			"    ARGON 13MM,              !- Name",
+			"    Argon,                   !- Gas Type",
+			"    0.0127;                  !- Thickness {m}",
+
+			"Construction,",
+			"    ROOF-1,                  !- Name",
+			"    RG01,                    !- Outside Layer",
+			"    BR01,                    !- Layer 2",
+			"    IN46,                    !- Layer 3",
+			"    WD01;                    !- Layer 4",
+
+			"Construction,",
+			"    WALL-1,                  !- Name",
+			"    WD01,                    !- Outside Layer",
+			"    PW03,                    !- Layer 2",
+			"    IN02,                    !- Layer 3",
+			"    GP01;                    !- Layer 4",
+
+			"Construction,",
+			"    CLNG-1,                  !- Name",
+			"    MAT-CLNG-1;              !- Outside Layer",
+
+			"Construction,",
+			"    FLOOR-SLAB-1,            !- Name",
+			"    CC03;                    !- Outside Layer",
+
+			"Construction,",
+			"    INT-WALL-1,              !- Name",
+			"    GP02,                    !- Outside Layer",
+			"    AL21,                    !- Layer 2",
+			"    GP02;                    !- Layer 3",
+
+			"Construction,",
+			"    Dbl Clr 3mm/13mm Air,    !- Name",
+			"    CLEAR 3MM,               !- Outside Layer",
+			"    AIR 13MM,                !- Layer 2",
+			"    CLEAR 3MM;               !- Layer 3",
+
+			"Construction,",
+			"    Sgl Grey 3mm,            !- Name",
+			"    GREY 3MM;                !- Outside Layer",
+
+			"GlobalGeometryRules,",
+			"    UpperLeftCorner,         !- Starting Vertex Position",
+			"    CounterClockWise,        !- Vertex Entry Direction",
+			"    relative;                !- Coordinate System",
+
+			"Zone,",
+			"    PLENUM-1,                !- Name",
+			"    0,                       !- Direction of Relative North {deg}",
+			"    0, 0, 0,                            !- X,Y,Z  {m}",
+			"    1,                       !- Type",
+			"    1,                       !- Multiplier",
+			"    0.609600067,             !- Ceiling Height {m}",
+			"    283.2;                   !- Volume {m3}",
+
+			"Zone,",
+			"    SPACE1-1,                !- Name",
+			"    0,                       !- Direction of Relative North {deg}",
+			"    0, 0, 0,                            !- X,Y,Z  {m}",
+			"    1,                       !- Type",
+			"    1,                       !- Multiplier",
+			"    2.438400269,             !- Ceiling Height {m}",
+			"    239.247360229;           !- Volume {m3}",
+
+			"Zone,",
+			"    SPACE2-1,                !- Name",
+			"    0,                       !- Direction of Relative North {deg}",
+			"    0, 0, 0,                            !- X,Y,Z  {m}",
+			"    1,                       !- Type",
+			"    1,                       !- Multiplier",
+			"    2.438400269,             !- Ceiling Height {m}",
+			"    103.311355591;           !- Volume {m3}",
+
+			"Zone,",
+			"    SPACE3-1,                !- Name",
+			"    0,                       !- Direction of Relative North {deg}",
+			"    0, 0, 0,                            !- X,Y,Z  {m}",
+			"    1,                       !- Type",
+			"    1,                       !- Multiplier",
+			"    2.438400269,             !- Ceiling Height {m}",
+			"    239.247360229;           !- Volume {m3}",
+
+			"Zone,",
+			"    SPACE4-1,                !- Name",
+			"    0,                       !- Direction of Relative North {deg}",
+			"    0, 0, 0,                            !- X,Y,Z  {m}",
+			"    1,                       !- Type",
+			"    1,                       !- Multiplier",
+			"    2.438400269,             !- Ceiling Height {m}",
+			"    103.311355591;           !- Volume {m3}",
+
+			"Zone,",
+			"    SPACE5-1,                !- Name",
+			"    0,                       !- Direction of Relative North {deg}",
+			"    0, 0, 0,                            !- X,Y,Z  {m}",
+			"    1,                       !- Type",
+			"    1,                       !- Multiplier",
+			"    2.438400269,             !- Ceiling Height {m}",
+			"    447.682556152;           !- Volume {m3}",
+
+			"BuildingSurface:Detailed,",
+			"    WALL-1PF,                !- Name",
+			"    WALL,                    !- Surface Type",
+			"    WALL-1,                  !- Construction Name",
+			"    PLENUM-1,                !- Zone Name",
+			"    Outdoors,                !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    SunExposed,              !- Sun Exposure",
+			"    WindExposed,             !- Wind Exposure",
+			"    0.50000,                 !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    0.0, 0.0, 3.0,                      !- X,Y,Z  1 {m}",
+			"    0.0, 0.0, 2.4,                      !- X,Y,Z  2 {m}",
+			"    30.5, 0.0, 2.4,                     !- X,Y,Z  3 {m}",
+			"    30.5, 0.0, 3.0;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    WALL-1PR,                !- Name",
+			"    WALL,                    !- Surface Type",
+			"    WALL-1,                  !- Construction Name",
+			"    PLENUM-1,                !- Zone Name",
+			"    Outdoors,                !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    SunExposed,              !- Sun Exposure",
+			"    WindExposed,             !- Wind Exposure",
+			"    0.50000,                 !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    30.5, 0.0, 3.0,                     !- X,Y,Z  1 {m}",
+			"    30.5, 0.0, 2.4,                     !- X,Y,Z  2 {m}",
+			"    30.5, 15.2, 2.4,                    !- X,Y,Z  3 {m}",
+			"    30.5, 15.2, 3.0;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    WALL-1PB,                !- Name",
+			"    WALL,                    !- Surface Type",
+			"    WALL-1,                  !- Construction Name",
+			"    PLENUM-1,                !- Zone Name",
+			"    Outdoors,                !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    SunExposed,              !- Sun Exposure",
+			"    WindExposed,             !- Wind Exposure",
+			"    0.50000,                 !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    30.5, 15.2, 3.0,                    !- X,Y,Z  1 {m}",
+			"    30.5, 15.2, 2.4,                    !- X,Y,Z  2 {m}",
+			"    0.0, 15.2, 2.4,                     !- X,Y,Z  3 {m}",
+			"    0.0, 15.2, 3.0;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    WALL-1PL,                !- Name",
+			"    WALL,                    !- Surface Type",
+			"    WALL-1,                  !- Construction Name",
+			"    PLENUM-1,                !- Zone Name",
+			"    Outdoors,                !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    SunExposed,              !- Sun Exposure",
+			"    WindExposed,             !- Wind Exposure",
+			"    0.50000,                 !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    0.0, 15.2, 3.0,                     !- X,Y,Z  1 {m}",
+			"    0.0, 15.2, 2.4,                     !- X,Y,Z  2 {m}",
+			"    0.0, 0.0, 2.4,                      !- X,Y,Z  3 {m}",
+			"    0.0, 0.0, 3.0;                      !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    TOP-1,                   !- Name",
+			"    ROOF,                    !- Surface Type",
+			"    ROOF-1,                  !- Construction Name",
+			"    PLENUM-1,                !- Zone Name",
+			"    Outdoors,                !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    SunExposed,              !- Sun Exposure",
+			"    WindExposed,             !- Wind Exposure",
+			"    0.00000,                 !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    0.0, 15.2, 3.0,                     !- X,Y,Z  1 {m}",
+			"    0.0, 0.0, 3.0,                      !- X,Y,Z  2 {m}",
+			"    30.5, 0.0, 3.0,                     !- X,Y,Z  3 {m}",
+			"    30.5, 15.2, 3.0;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    C1-1P,                   !- Name",
+			"    FLOOR,                   !- Surface Type",
+			"    CLNG-1,                  !- Construction Name",
+			"    PLENUM-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    C1-1,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 3.7, 2.4,                     !- X,Y,Z  1 {m}",
+			"    30.5, 0.0, 2.4,                     !- X,Y,Z  2 {m}",
+			"    0.0, 0.0, 2.4,                      !- X,Y,Z  3 {m}",
+			"    3.7, 3.7, 2.4;                      !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    C2-1P,                   !- Name",
+			"    FLOOR,                   !- Surface Type",
+			"    CLNG-1,                  !- Construction Name",
+			"    PLENUM-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    C2-1,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 11.6, 2.4,                    !- X,Y,Z  1 {m}",
+			"    30.5, 15.2, 2.4,                    !- X,Y,Z  2 {m}",
+			"    30.5, 0.0, 2.4,                     !- X,Y,Z  3 {m}",
+			"    26.8, 3.7, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    C3-1P,                   !- Name",
+			"    FLOOR,                   !- Surface Type",
+			"    CLNG-1,                  !- Construction Name",
+			"    PLENUM-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    C3-1,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 11.6, 2.4,                    !- X,Y,Z  1 {m}",
+			"    3.7, 11.6, 2.4,                     !- X,Y,Z  2 {m}",
+			"    0.0, 15.2, 2.4,                     !- X,Y,Z  3 {m}",
+			"    30.5, 15.2, 2.4;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    C4-1P,                   !- Name",
+			"    FLOOR,                   !- Surface Type",
+			"    CLNG-1,                  !- Construction Name",
+			"    PLENUM-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    C4-1,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 3.7, 2.4,                      !- X,Y,Z  1 {m}",
+			"    0.0, 0.0, 2.4,                      !- X,Y,Z  2 {m}",
+			"    0.0, 15.2, 2.4,                     !- X,Y,Z  3 {m}",
+			"    3.7, 11.6, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    C5-1P,                   !- Name",
+			"    FLOOR,                   !- Surface Type",
+			"    CLNG-1,                  !- Construction Name",
+			"    PLENUM-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    C5-1,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 11.6, 2.4,                    !- X,Y,Z  1 {m}",
+			"    26.8, 3.7, 2.4,                     !- X,Y,Z  2 {m}",
+			"    3.7, 3.7, 2.4,                      !- X,Y,Z  3 {m}",
+			"    3.7, 11.6, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    FRONT-1,                 !- Name",
+			"    WALL,                    !- Surface Type",
+			"    WALL-1,                  !- Construction Name",
+			"    SPACE1-1,                !- Zone Name",
+			"    Outdoors,                !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    SunExposed,              !- Sun Exposure",
+			"    WindExposed,             !- Wind Exposure",
+			"    0.50000,                 !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    0.0, 0.0, 2.4,                      !- X,Y,Z  1 {m}",
+			"    0.0, 0.0, 0.0,                      !- X,Y,Z  2 {m}",
+			"    30.5, 0.0, 0.0,                     !- X,Y,Z  3 {m}",
+			"    30.5, 0.0, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    C1-1,                    !- Name",
+			"    CEILING,                 !- Surface Type",
+			"    CLNG-1,                  !- Construction Name",
+			"    SPACE1-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    C1-1P,                   !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 3.7, 2.4,                      !- X,Y,Z  1 {m}",
+			"    0.0, 0.0, 2.4,                      !- X,Y,Z  2 {m}",
+			"    30.5, 0.0, 2.4,                     !- X,Y,Z  3 {m}",
+			"    26.8, 3.7, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    F1-1,                    !- Name",
+			"    FLOOR,                   !- Surface Type",
+			"    FLOOR-SLAB-1,            !- Construction Name",
+			"    SPACE1-1,                !- Zone Name",
+			"    Ground,                  !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 3.7, 0.0,                     !- X,Y,Z  1 {m}",
+			"    30.5, 0.0, 0.0,                     !- X,Y,Z  2 {m}",
+			"    0.0, 0.0, 0.0,                      !- X,Y,Z  3 {m}",
+			"    3.7, 3.7, 0.0;                      !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB12,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE1-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB21,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    30.5, 0.0, 2.4,                     !- X,Y,Z  1 {m}",
+			"    30.5, 0.0, 0.0,                     !- X,Y,Z  2 {m}",
+			"    26.8, 3.7, 0.0,                     !- X,Y,Z  3 {m}",
+			"    26.8, 3.7, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB14,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE1-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB41,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 3.7, 2.4,                      !- X,Y,Z  1 {m}",
+			"    3.7, 3.7, 0.0,                      !- X,Y,Z  2 {m}",
+			"    0.0, 0.0, 0.0,                      !- X,Y,Z  3 {m}",
+			"    0.0, 0.0, 2.4;                      !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB15,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE1-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB51,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 3.7, 2.4,                     !- X,Y,Z  1 {m}",
+			"    26.8, 3.7, 0.0,                     !- X,Y,Z  2 {m}",
+			"    3.7, 3.7, 0.0,                      !- X,Y,Z  3 {m}",
+			"    3.7, 3.7, 2.4;                      !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    RIGHT-1,                 !- Name",
+			"    WALL,                    !- Surface Type",
+			"    WALL-1,                  !- Construction Name",
+			"    SPACE2-1,                !- Zone Name",
+			"    Outdoors,                !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    SunExposed,              !- Sun Exposure",
+			"    WindExposed,             !- Wind Exposure",
+			"    0.50000,                 !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    30.5, 0.0, 2.4,                     !- X,Y,Z  1 {m}",
+			"    30.5, 0.0, 0.0,                     !- X,Y,Z  2 {m}",
+			"    30.5, 15.2, 0.0,                    !- X,Y,Z  3 {m}",
+			"    30.5, 15.2, 2.4;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    C2-1,                    !- Name",
+			"    CEILING,                 !- Surface Type",
+			"    CLNG-1,                  !- Construction Name",
+			"    SPACE2-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    C2-1P,                   !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 3.7, 2.4,                     !- X,Y,Z  1 {m}",
+			"    30.5, 0.0, 2.4,                     !- X,Y,Z  2 {m}",
+			"    30.5, 15.2, 2.4,                    !- X,Y,Z  3 {m}",
+			"    26.8, 11.6, 2.4;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    F2-1,                    !- Name",
+			"    FLOOR,                   !- Surface Type",
+			"    FLOOR-SLAB-1,            !- Construction Name",
+			"    SPACE2-1,                !- Zone Name",
+			"    Ground,                  !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 11.6, 0.0,                    !- X,Y,Z  1 {m}",
+			"    30.5, 15.2, 0.0,                    !- X,Y,Z  2 {m}",
+			"    30.5, 0.0, 0.0,                     !- X,Y,Z  3 {m}",
+			"    26.8, 3.7, 0.0;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB21,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE2-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB12,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 3.7, 2.4,                     !- X,Y,Z  1 {m}",
+			"    26.8, 3.7, 0.0,                     !- X,Y,Z  2 {m}",
+			"    30.5, 0.0, 0.0,                     !- X,Y,Z  3 {m}",
+			"    30.5, 0.0, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB23,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE2-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB32,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    30.5, 15.2, 2.4,                    !- X,Y,Z  1 {m}",
+			"    30.5, 15.2, 0.0,                    !- X,Y,Z  2 {m}",
+			"    26.8, 11.6, 0.0,                    !- X,Y,Z  3 {m}",
+			"    26.8, 11.6, 2.4;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB25,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE2-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB52,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 11.6, 2.4,                    !- X,Y,Z  1 {m}",
+			"    26.8, 11.6, 0.0,                    !- X,Y,Z  2 {m}",
+			"    26.8, 3.7, 0.0,                     !- X,Y,Z  3 {m}",
+			"    26.8, 3.7, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    BACK-1,                  !- Name",
+			"    WALL,                    !- Surface Type",
+			"    WALL-1,                  !- Construction Name",
+			"    SPACE3-1,                !- Zone Name",
+			"    Outdoors,                !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    SunExposed,              !- Sun Exposure",
+			"    WindExposed,             !- Wind Exposure",
+			"    0.50000,                 !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    30.5, 15.2, 2.4,                    !- X,Y,Z  1 {m}",
+			"    30.5, 15.2, 0.0,                    !- X,Y,Z  2 {m}",
+			"    0.0, 15.2, 0.0,                     !- X,Y,Z  3 {m}",
+			"    0.0, 15.2, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    C3-1,                    !- Name",
+			"    CEILING,                 !- Surface Type",
+			"    CLNG-1,                  !- Construction Name",
+			"    SPACE3-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    C3-1P,                   !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    30.5, 15.2, 2.4,                    !- X,Y,Z  1 {m}",
+			"    0.0, 15.2, 2.4,                     !- X,Y,Z  2 {m}",
+			"    3.7, 11.6, 2.4,                     !- X,Y,Z  3 {m}",
+			"    26.8, 11.6, 2.4;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    F3-1,                    !- Name",
+			"    FLOOR,                   !- Surface Type",
+			"    FLOOR-SLAB-1,            !- Construction Name",
+			"    SPACE3-1,                !- Zone Name",
+			"    Ground,                  !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 11.6, 0.0,                    !- X,Y,Z  1 {m}",
+			"    3.7, 11.6, 0.0,                     !- X,Y,Z  2 {m}",
+			"    0.0, 15.2, 0.0,                     !- X,Y,Z  3 {m}",
+			"    30.5, 15.2, 0.0;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB32,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE3-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB23,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 11.6, 2.4,                    !- X,Y,Z  1 {m}",
+			"    26.8, 11.6, 0.0,                    !- X,Y,Z  2 {m}",
+			"    30.5, 15.2, 0.0,                    !- X,Y,Z  3 {m}",
+			"    30.5, 15.2, 2.4;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB34,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE3-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB43,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    0.0, 15.2, 2.4,                     !- X,Y,Z  1 {m}",
+			"    0.0, 15.2, 0.0,                     !- X,Y,Z  2 {m}",
+			"    3.7, 11.6, 0.0,                     !- X,Y,Z  3 {m}",
+			"    3.7, 11.6, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB35,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE3-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB53,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 11.6, 2.4,                     !- X,Y,Z  1 {m}",
+			"    3.7, 11.6, 0.0,                     !- X,Y,Z  2 {m}",
+			"    26.8, 11.6, 0.0,                    !- X,Y,Z  3 {m}",
+			"    26.8, 11.6, 2.4;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    LEFT-1,                  !- Name",
+			"    WALL,                    !- Surface Type",
+			"    WALL-1,                  !- Construction Name",
+			"    SPACE4-1,                !- Zone Name",
+			"    Outdoors,                !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    SunExposed,              !- Sun Exposure",
+			"    WindExposed,             !- Wind Exposure",
+			"    0.50000,                 !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    0.0, 15.2, 2.4,                     !- X,Y,Z  1 {m}",
+			"    0.0, 15.2, 0.0,                     !- X,Y,Z  2 {m}",
+			"    0.0, 0.0, 0.0,                      !- X,Y,Z  3 {m}",
+			"    0.0, 0.0, 2.4;                      !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    C4-1,                    !- Name",
+			"    CEILING,                 !- Surface Type",
+			"    CLNG-1,                  !- Construction Name",
+			"    SPACE4-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    C4-1P,                   !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 11.6, 2.4,                     !- X,Y,Z  1 {m}",
+			"    0.0, 15.2, 2.4,                     !- X,Y,Z  2 {m}",
+			"    0.0, 0.0, 2.4,                      !- X,Y,Z  3 {m}",
+			"    3.7, 3.7, 2.4;                      !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    F4-1,                    !- Name",
+			"    FLOOR,                   !- Surface Type",
+			"    FLOOR-SLAB-1,            !- Construction Name",
+			"    SPACE4-1,                !- Zone Name",
+			"    Ground,                  !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 3.7, 0.0,                      !- X,Y,Z  1 {m}",
+			"    0.0, 0.0, 0.0,                      !- X,Y,Z  2 {m}",
+			"    0.0, 15.2, 0.0,                     !- X,Y,Z  3 {m}",
+			"    3.7, 11.6, 0.0;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB41,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE4-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB14,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    0.0, 0.0, 2.4,                      !- X,Y,Z  1 {m}",
+			"    0.0, 0.0, 0.0,                      !- X,Y,Z  2 {m}",
+			"    3.7, 3.7, 0.0,                      !- X,Y,Z  3 {m}",
+			"    3.7, 3.7, 2.4;                      !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB43,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE4-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB34,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 11.6, 2.4,                     !- X,Y,Z  1 {m}",
+			"    3.7, 11.6, 0.0,                     !- X,Y,Z  2 {m}",
+			"    0.0, 15.2, 0.0,                     !- X,Y,Z  3 {m}",
+			"    0.0, 15.2, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB45,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE4-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB54,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 3.7, 2.4,                      !- X,Y,Z  1 {m}",
+			"    3.7, 3.7, 0.0,                      !- X,Y,Z  2 {m}",
+			"    3.7, 11.6, 0.0,                     !- X,Y,Z  3 {m}",
+			"    3.7, 11.6, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    C5-1,                    !- Name",
+			"    CEILING,                 !- Surface Type",
+			"    CLNG-1,                  !- Construction Name",
+			"    SPACE5-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    C5-1P,                   !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 11.6, 2.4,                     !- X,Y,Z  1 {m}",
+			"    3.7, 3.7, 2.4,                      !- X,Y,Z  2 {m}",
+			"    26.8, 3.7, 2.4,                     !- X,Y,Z  3 {m}",
+			"    26.8, 11.6, 2.4;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    F5-1,                    !- Name",
+			"    FLOOR,                   !- Surface Type",
+			"    FLOOR-SLAB-1,            !- Construction Name",
+			"    SPACE5-1,                !- Zone Name",
+			"    Ground,                  !- Outside Boundary Condition",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 11.6, 0.0,                    !- X,Y,Z  1 {m}",
+			"    26.8, 3.7, 0.0,                     !- X,Y,Z  2 {m}",
+			"    3.7, 3.7, 0.0,                      !- X,Y,Z  3 {m}",
+			"    3.7, 11.6, 0.0;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB51,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE5-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB15,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 3.7, 2.4,                      !- X,Y,Z  1 {m}",
+			"    3.7, 3.7, 0.0,                      !- X,Y,Z  2 {m}",
+			"    26.8, 3.7, 0.0,                     !- X,Y,Z  3 {m}",
+			"    26.8, 3.7, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB52,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE5-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB25,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 3.7, 2.4,                     !- X,Y,Z  1 {m}",
+			"    26.8, 3.7, 0.0,                     !- X,Y,Z  2 {m}",
+			"    26.8, 11.6, 0.0,                    !- X,Y,Z  3 {m}",
+			"    26.8, 11.6, 2.4;                    !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB53,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE5-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB35,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    26.8, 11.6, 2.4,                    !- X,Y,Z  1 {m}",
+			"    26.8, 11.6, 0.0,                    !- X,Y,Z  2 {m}",
+			"    3.7, 11.6, 0.0,                     !- X,Y,Z  3 {m}",
+			"    3.7, 11.6, 2.4;                     !- X,Y,Z  4 {m}",
+
+			"BuildingSurface:Detailed,",
+			"    SB54,                    !- Name",
+			"    WALL,                    !- Surface Type",
+			"    INT-WALL-1,              !- Construction Name",
+			"    SPACE5-1,                !- Zone Name",
+			"    Surface,                 !- Outside Boundary Condition",
+			"    SB45,                    !- Outside Boundary Condition Object",
+			"    NoSun,                   !- Sun Exposure",
+			"    NoWind,                  !- Wind Exposure",
+			"    0.0,                     !- View Factor to Ground",
+			"    4,                       !- Number of Vertices",
+			"    3.7, 11.6, 2.4,                     !- X,Y,Z  1 {m}",
+			"    3.7, 11.6, 0.0,                     !- X,Y,Z  2 {m}",
+			"    3.7, 3.7, 0.0,                      !- X,Y,Z  3 {m}",
+			"    3.7, 3.7, 2.4;                      !- X,Y,Z  4 {m}",
+
+			"FenestrationSurface:Detailed,",
+			"    WF-1,                    !- Name",
+			"    WINDOW,                  !- Surface Type",
+			"    Dbl Clr 3mm/13mm Air,    !- Construction Name",
+			"    FRONT-1,                 !- Building Surface Name",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    0.50000,                 !- View Factor to Ground",
+			"    ,                        !- Shading Control Name",
+			"    ,                        !- Frame and Divider Name",
+			"    1,                       !- Multiplier",
+			"    4,                       !- Number of Vertices",
+			"    3.0, 0.0, 2.1,                      !- X,Y,Z  1 {m}",
+			"    3.0, 0.0, 0.9,                      !- X,Y,Z  2 {m}",
+			"    16.8, 0.0, 0.9,                     !- X,Y,Z  3 {m}",
+			"    16.8, 0.0, 2.1;                     !- X,Y,Z  4 {m}",
+
+			"FenestrationSurface:Detailed,",
+			"    DF-1,                    !- Name",
+			"    GLASSDOOR,               !- Surface Type",
+			"    Sgl Grey 3mm,            !- Construction Name",
+			"    FRONT-1,                 !- Building Surface Name",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    0.50000,                 !- View Factor to Ground",
+			"    ,                        !- Shading Control Name",
+			"    ,                        !- Frame and Divider Name",
+			"    1,                       !- Multiplier",
+			"    4,                       !- Number of Vertices",
+			"    21.3, 0.0, 2.1,                     !- X,Y,Z  1 {m}",
+			"    21.3, 0.0, 0.0,                     !- X,Y,Z  2 {m}",
+			"    23.8, 0.0, 0.0,                     !- X,Y,Z  3 {m}",
+			"    23.8, 0.0, 2.1;                     !- X,Y,Z  4 {m}",
+
+			"FenestrationSurface:Detailed,",
+			"    WR-1,                    !- Name",
+			"    WINDOW,                  !- Surface Type",
+			"    Dbl Clr 3mm/13mm Air,    !- Construction Name",
+			"    RIGHT-1,                 !- Building Surface Name",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    0.50000,                 !- View Factor to Ground",
+			"    ,                        !- Shading Control Name",
+			"    ,                        !- Frame and Divider Name",
+			"    1,                       !- Multiplier",
+			"    4,                       !- Number of Vertices",
+			"    30.5, 3.8, 2.1,                     !- X,Y,Z  1 {m}",
+			"    30.5, 3.8, 0.9,                     !- X,Y,Z  2 {m}",
+			"    30.5, 11.4, 0.9,                    !- X,Y,Z  3 {m}",
+			"    30.5, 11.4, 2.1;                    !- X,Y,Z  4 {m}",
+
+			"FenestrationSurface:Detailed,",
+			"    WB-1,                    !- Name",
+			"    WINDOW,                  !- Surface Type",
+			"    Dbl Clr 3mm/13mm Air,    !- Construction Name",
+			"    BACK-1,                  !- Building Surface Name",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    0.50000,                 !- View Factor to Ground",
+			"    ,                        !- Shading Control Name",
+			"    ,                        !- Frame and Divider Name",
+			"    1,                       !- Multiplier",
+			"    4,                       !- Number of Vertices",
+			"    27.4, 15.2, 2.1,                    !- X,Y,Z  1 {m}",
+			"    27.4, 15.2, 0.9,                    !- X,Y,Z  2 {m}",
+			"    13.7, 15.2, 0.9,                    !- X,Y,Z  3 {m}",
+			"    13.7, 15.2, 2.1;                    !- X,Y,Z  4 {m}",
+
+			"FenestrationSurface:Detailed,",
+			"    DB-1,                    !- Name",
+			"    GLASSDOOR,               !- Surface Type",
+			"    Sgl Grey 3mm,            !- Construction Name",
+			"    BACK-1,                  !- Building Surface Name",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    0.50000,                 !- View Factor to Ground",
+			"    ,                        !- Shading Control Name",
+			"    ,                        !- Frame and Divider Name",
+			"    1,                       !- Multiplier",
+			"    4,                       !- Number of Vertices",
+			"    9.1, 15.2, 2.1,                     !- X,Y,Z  1 {m}",
+			"    9.1, 15.2, 0.0,                     !- X,Y,Z  2 {m}",
+			"    7.0, 15.2, 0.0,                     !- X,Y,Z  3 {m}",
+			"    7.0, 15.2, 2.1;                     !- X,Y,Z  4 {m}",
+
+			"FenestrationSurface:Detailed,",
+			"    WL-1,                    !- Name",
+			"    WINDOW,                  !- Surface Type",
+			"    Dbl Clr 3mm/13mm Air,    !- Construction Name",
+			"    LEFT-1,                  !- Building Surface Name",
+			"    ,                        !- Outside Boundary Condition Object",
+			"    0.50000,                 !- View Factor to Ground",
+			"    ,                        !- Shading Control Name",
+			"    ,                        !- Frame and Divider Name",
+			"    1,                       !- Multiplier",
+			"    4,                       !- Number of Vertices",
+			"    0.0, 11.4, 2.1,                     !- X,Y,Z  1 {m}",
+			"    0.0, 11.4, 0.9,                     !- X,Y,Z  2 {m}",
+			"    0.0, 3.8, 0.9,                      !- X,Y,Z  3 {m}",
+			"    0.0, 3.8, 2.1;                      !- X,Y,Z  4 {m}",
+
+			"Shading:Zone:Detailed,",
+			"    Main South Overhang,     !- Name",
+			"    FRONT-1,                 !- Base Surface Name",
+			"    ShadeTransSch,           !- Transmittance Schedule Name",
+			"    4,                       !- Number of Vertices",
+			"    0.0, -1.3, 2.2,                     !- X,Y,Z  1 {m}",
+			"    0.0, 0.0, 2.2,                      !- X,Y,Z  2 {m}",
+			"    19.8, 0.0, 2.2,                     !- X,Y,Z  3 {m}",
+			"    19.8, -1.3, 2.2;                    !- X,Y,Z  4 {m}",
+
+			"Shading:Zone:Detailed,",
+			"    South Door Overhang,     !- Name",
+			"    FRONT-1,                 !- Base Surface Name",
+			"    ShadeTransSch,           !- Transmittance Schedule Name",
+			"    4,                       !- Number of Vertices",
+			"    21.0, -2.0, 2.6,                    !- X,Y,Z  1 {m}",
+			"    21.0, 0.0, 2.6,                     !- X,Y,Z  2 {m}",
+			"    24.1, 0.0, 2.6,                     !- X,Y,Z  3 {m}",
+			"    24.1, -2.0, 2.6;                    !- X,Y,Z  4 {m}",
+
+			"People,",
+			"    SPACE1-1 People 1,       !- Name",
+			"    SPACE1-1,                !- Zone or ZoneList Name",
+			"    OCCUPY-1,                !- Number of People Schedule Name",
+			"    people,                  !- Number of People Calculation Method",
+			"    11,                      !- Number of People",
+			"    ,                        !- People per Zone Floor Area {person/m2}",
+			"    ,                        !- Zone Floor Area per Person {m2/person}",
+			"    0.3,                     !- Fraction Radiant",
+			"    ,                        !- Sensible Heat Fraction",
+			"    ActSchd;                 !- Activity Level Schedule Name",
+
+			"People,",
+			"    SPACE2-1 People 1,       !- Name",
+			"    SPACE2-1,                !- Zone or ZoneList Name",
+			"    OCCUPY-1,                !- Number of People Schedule Name",
+			"    people,                  !- Number of People Calculation Method",
+			"    5,                       !- Number of People",
+			"    ,                        !- People per Zone Floor Area {person/m2}",
+			"    ,                        !- Zone Floor Area per Person {m2/person}",
+			"    0.3,                     !- Fraction Radiant",
+			"    ,                        !- Sensible Heat Fraction",
+			"    ActSchd;                 !- Activity Level Schedule Name",
+
+			"People,",
+			"    SPACE3-1 People 1,       !- Name",
+			"    SPACE3-1,                !- Zone or ZoneList Name",
+			"    OCCUPY-1,                !- Number of People Schedule Name",
+			"    people,                  !- Number of People Calculation Method",
+			"    11,                      !- Number of People",
+			"    ,                        !- People per Zone Floor Area {person/m2}",
+			"    ,                        !- Zone Floor Area per Person {m2/person}",
+			"    0.3,                     !- Fraction Radiant",
+			"    ,                        !- Sensible Heat Fraction",
+			"    ActSchd;                 !- Activity Level Schedule Name",
+
+			"People,",
+			"    SPACE4-1 People 1,       !- Name",
+			"    SPACE4-1,                !- Zone or ZoneList Name",
+			"    OCCUPY-1,                !- Number of People Schedule Name",
+			"    people,                  !- Number of People Calculation Method",
+			"    5,                       !- Number of People",
+			"    ,                        !- People per Zone Floor Area {person/m2}",
+			"    ,                        !- Zone Floor Area per Person {m2/person}",
+			"    0.3,                     !- Fraction Radiant",
+			"    ,                        !- Sensible Heat Fraction",
+			"    ActSchd;                 !- Activity Level Schedule Name",
+
+			"People,",
+			"    SPACE5-1 People 1,       !- Name",
+			"    SPACE5-1,                !- Zone or ZoneList Name",
+			"    OCCUPY-1,                !- Number of People Schedule Name",
+			"    people,                  !- Number of People Calculation Method",
+			"    20,                      !- Number of People",
+			"    ,                        !- People per Zone Floor Area {person/m2}",
+			"    ,                        !- Zone Floor Area per Person {m2/person}",
+			"    0.3,                     !- Fraction Radiant",
+			"    ,                        !- Sensible Heat Fraction",
+			"    ActSchd;                 !- Activity Level Schedule Name",
+
+			"Lights,",
+			"    SPACE1-1 Lights 1,       !- Name",
+			"    SPACE1-1,                !- Zone or ZoneList Name",
+			"    LIGHTS-1,                !- Schedule Name",
+			"    LightingLevel,           !- Design Level Calculation Method",
+			"    1584,                    !- Lighting Level {W}",
+			"    ,                        !- Watts per Zone Floor Area {W/m2}",
+			"    ,                        !- Watts per Person {W/person}",
+			"    0,                       !- Return Air Fraction",
+			"    0.59,                    !- Fraction Radiant",
+			"    0.2,                     !- Fraction Visible",
+			"    0,                       !- Fraction Replaceable",
+			"    GeneralLights;           !- End-Use Subcategory",
+
+			"Lights,",
+			"    SPACE2-1 Lights 1,       !- Name",
+			"    SPACE2-1,                !- Zone or ZoneList Name",
+			"    LIGHTS-1,                !- Schedule Name",
+			"    LightingLevel,           !- Design Level Calculation Method",
+			"    684,                     !- Lighting Level {W}",
+			"    ,                        !- Watts per Zone Floor Area {W/m2}",
+			"    ,                        !- Watts per Person {W/person}",
+			"    0,                       !- Return Air Fraction",
+			"    0.59,                    !- Fraction Radiant",
+			"    0.2,                     !- Fraction Visible",
+			"    0,                       !- Fraction Replaceable",
+			"    GeneralLights;           !- End-Use Subcategory",
+
+			"Lights,",
+			"    SPACE3-1 Lights 1,       !- Name",
+			"    SPACE3-1,                !- Zone or ZoneList Name",
+			"    LIGHTS-1,                !- Schedule Name",
+			"    LightingLevel,           !- Design Level Calculation Method",
+			"    1584,                    !- Lighting Level {W}",
+			"    ,                        !- Watts per Zone Floor Area {W/m2}",
+			"    ,                        !- Watts per Person {W/person}",
+			"    0,                       !- Return Air Fraction",
+			"    0.59,                    !- Fraction Radiant",
+			"    0.2,                     !- Fraction Visible",
+			"    0,                       !- Fraction Replaceable",
+			"    GeneralLights;           !- End-Use Subcategory",
+
+			"Lights,",
+			"    SPACE4-1 Lights 1,       !- Name",
+			"    SPACE4-1,                !- Zone or ZoneList Name",
+			"    LIGHTS-1,                !- Schedule Name",
+			"    LightingLevel,           !- Design Level Calculation Method",
+			"    684,                     !- Lighting Level {W}",
+			"    ,                        !- Watts per Zone Floor Area {W/m2}",
+			"    ,                        !- Watts per Person {W/person}",
+			"    0,                       !- Return Air Fraction",
+			"    0.59,                    !- Fraction Radiant",
+			"    0.2,                     !- Fraction Visible",
+			"    0,                       !- Fraction Replaceable",
+			"    GeneralLights;           !- End-Use Subcategory",
+
+			"Lights,",
+			"    SPACE5-1 Lights 1,       !- Name",
+			"    SPACE5-1,                !- Zone or ZoneList Name",
+			"    LIGHTS-1,                !- Schedule Name",
+			"    LightingLevel,           !- Design Level Calculation Method",
+			"    2964,                    !- Lighting Level {W}",
+			"    ,                        !- Watts per Zone Floor Area {W/m2}",
+			"    ,                        !- Watts per Person {W/person}",
+			"    0,                       !- Return Air Fraction",
+			"    0.59,                    !- Fraction Radiant",
+			"    0.2,                     !- Fraction Visible",
+			"    0,                       !- Fraction Replaceable",
+			"    GeneralLights;           !- End-Use Subcategory",
+
+			"ElectricEquipment,",
+			"    SPACE1-1 ElecEq 1,       !- Name",
+			"    SPACE1-1,                !- Zone or ZoneList Name",
+			"    EQUIP-1,                 !- Schedule Name",
+			"    EquipmentLevel,          !- Design Level Calculation Method",
+			"    1056,                    !- Design Level {W}",
+			"    ,                        !- Watts per Zone Floor Area {W/m2}",
+			"    ,                        !- Watts per Person {W/person}",
+			"    0,                       !- Fraction Latent",
+			"    0.3,                     !- Fraction Radiant",
+			"    0;                       !- Fraction Lost",
+
+			"ElectricEquipment,",
+			"    SPACE2-1 ElecEq 1,       !- Name",
+			"    SPACE2-1,                !- Zone or ZoneList Name",
+			"    EQUIP-1,                 !- Schedule Name",
+			"    EquipmentLevel,          !- Design Level Calculation Method",
+			"    456,                     !- Design Level {W}",
+			"    ,                        !- Watts per Zone Floor Area {W/m2}",
+			"    ,                        !- Watts per Person {W/person}",
+			"    0,                       !- Fraction Latent",
+			"    0.3,                     !- Fraction Radiant",
+			"    0;                       !- Fraction Lost",
+
+			"ElectricEquipment,",
+			"    SPACE3-1 ElecEq 1,       !- Name",
+			"    SPACE3-1,                !- Zone or ZoneList Name",
+			"    EQUIP-1,                 !- Schedule Name",
+			"    EquipmentLevel,          !- Design Level Calculation Method",
+			"    1056,                    !- Design Level {W}",
+			"    ,                        !- Watts per Zone Floor Area {W/m2}",
+			"    ,                        !- Watts per Person {W/person}",
+			"    0,                       !- Fraction Latent",
+			"    0.3,                     !- Fraction Radiant",
+			"    0;                       !- Fraction Lost",
+
+			"ElectricEquipment,",
+			"    SPACE4-1 ElecEq 1,       !- Name",
+			"    SPACE4-1,                !- Zone or ZoneList Name",
+			"    EQUIP-1,                 !- Schedule Name",
+			"    EquipmentLevel,          !- Design Level Calculation Method",
+			"    456,                     !- Design Level {W}",
+			"    ,                        !- Watts per Zone Floor Area {W/m2}",
+			"    ,                        !- Watts per Person {W/person}",
+			"    0,                       !- Fraction Latent",
+			"    0.3,                     !- Fraction Radiant",
+			"    0;                       !- Fraction Lost",
+
+			"ElectricEquipment,",
+			"    SPACE5-1 ElecEq 1,       !- Name",
+			"    SPACE5-1,                !- Zone or ZoneList Name",
+			"    EQUIP-1,                 !- Schedule Name",
+			"    EquipmentLevel,          !- Design Level Calculation Method",
+			"    1976,                    !- Design Level {W}",
+			"    ,                        !- Watts per Zone Floor Area {W/m2}",
+			"    ,                        !- Watts per Person {W/person}",
+			"    0,                       !- Fraction Latent",
+			"    0.3,                     !- Fraction Radiant",
+			"    0;                       !- Fraction Lost",
+
+			"ZoneInfiltration:DesignFlowRate,",
+			"    SPACE1-1 Infil 1,        !- Name",
+			"    SPACE1-1,                !- Zone or ZoneList Name",
+			"    INFIL-SCH,               !- Schedule Name",
+			"    flow/zone,               !- Design Flow Rate Calculation Method",
+			"    0.0167,                  !- Design Flow Rate {m3/s}",
+			"    ,                        !- Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Flow per Exterior Surface Area {m3/s-m2}",
+			"    ,                        !- Air Changes per Hour {1/hr}",
+			"    0,                       !- Constant Term Coefficient",
+			"    0,                       !- Temperature Term Coefficient",
+			"    0.2237,                  !- Velocity Term Coefficient",
+			"    0;                       !- Velocity Squared Term Coefficient",
+
+			"ZoneInfiltration:DesignFlowRate,",
+			"    SPACE2-1 Infil 1,        !- Name",
+			"    SPACE2-1,                !- Zone or ZoneList Name",
+			"    INFIL-SCH,               !- Schedule Name",
+			"    flow/zone,               !- Design Flow Rate Calculation Method",
+			"    0.00717,                 !- Design Flow Rate {m3/s}",
+			"    ,                        !- Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Flow per Exterior Surface Area {m3/s-m2}",
+			"    ,                        !- Air Changes per Hour {1/hr}",
+			"    0,                       !- Constant Term Coefficient",
+			"    0,                       !- Temperature Term Coefficient",
+			"    0.2237,                  !- Velocity Term Coefficient",
+			"    0;                       !- Velocity Squared Term Coefficient",
+
+			"ZoneInfiltration:DesignFlowRate,",
+			"    SPACE3-1 Infil 1,        !- Name",
+			"    SPACE3-1,                !- Zone or ZoneList Name",
+			"    INFIL-SCH,               !- Schedule Name",
+			"    flow/zone,               !- Design Flow Rate Calculation Method",
+			"    0.0167,                  !- Design Flow Rate {m3/s}",
+			"    ,                        !- Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Flow per Exterior Surface Area {m3/s-m2}",
+			"    ,                        !- Air Changes per Hour {1/hr}",
+			"    0,                       !- Constant Term Coefficient",
+			"    0,                       !- Temperature Term Coefficient",
+			"    0.2237,                  !- Velocity Term Coefficient",
+			"    0;                       !- Velocity Squared Term Coefficient",
+
+			"ZoneInfiltration:DesignFlowRate,",
+			"    SPACE4-1 Infil 1,        !- Name",
+			"    SPACE4-1,                !- Zone or ZoneList Name",
+			"    INFIL-SCH,               !- Schedule Name",
+			"    flow/zone,               !- Design Flow Rate Calculation Method",
+			"    0.00717,                 !- Design Flow Rate {m3/s}",
+			"    ,                        !- Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Flow per Exterior Surface Area {m3/s-m2}",
+			"    ,                        !- Air Changes per Hour {1/hr}",
+			"    0,                       !- Constant Term Coefficient",
+			"    0,                       !- Temperature Term Coefficient",
+			"    0.2237,                  !- Velocity Term Coefficient",
+			"    0;                       !- Velocity Squared Term Coefficient",
+
+			"ZoneInfiltration:DesignFlowRate,",
+			"    SPACE5-1 Infil 1,        !- Name",
+			"    SPACE5-1,                !- Zone or ZoneList Name",
+			"    INFIL-SCH,               !- Schedule Name",
+			"    flow/zone,               !- Design Flow Rate Calculation Method",
+			"    0.031089,                !- Design Flow Rate {m3/s}",
+			"    ,                        !- Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Flow per Exterior Surface Area {m3/s-m2}",
+			"    ,                        !- Air Changes per Hour {1/hr}",
+			"    0,                       !- Constant Term Coefficient",
+			"    0,                       !- Temperature Term Coefficient",
+			"    0.2237,                  !- Velocity Term Coefficient",
+			"    0;                       !- Velocity Squared Term Coefficient",
+
+			"DesignSpecification:OutdoorAir,",
+			"    SZ DSOA SPACE1-1,        !- Name",
+			"    flow/person,             !- Outdoor Air Method",
+			"    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}",
+			"    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}",
+			"    0.0;                     !- Outdoor Air Flow per Zone {m3/s}",
+
+			"DesignSpecification:OutdoorAir,",
+			"    SZ DSOA SPACE2-1,        !- Name",
+			"    flow/person,             !- Outdoor Air Method",
+			"    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}",
+			"    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}",
+			"    0.0;                     !- Outdoor Air Flow per Zone {m3/s}",
+
+			"DesignSpecification:OutdoorAir,",
+			"    SZ DSOA SPACE3-1,        !- Name",
+			"    flow/person,             !- Outdoor Air Method",
+			"    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}",
+			"    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}",
+			"    0.0;                     !- Outdoor Air Flow per Zone {m3/s}",
+
+			"DesignSpecification:OutdoorAir,",
+			"    SZ DSOA SPACE4-1,        !- Name",
+			"    flow/person,             !- Outdoor Air Method",
+			"    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}",
+			"    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}",
+			"    0.0;                     !- Outdoor Air Flow per Zone {m3/s}",
+
+			"DesignSpecification:OutdoorAir,",
+			"    SZ DSOA SPACE5-1,        !- Name",
+			"    flow/person,             !- Outdoor Air Method",
+			"    0.00944,                 !- Outdoor Air Flow per Person {m3/s-person}",
+			"    0.0,                     !- Outdoor Air Flow per Zone Floor Area {m3/s-m2}",
+			"    0.0;                     !- Outdoor Air Flow per Zone {m3/s}",
+
+			"Sizing:Zone,",
+			"    SPACE1-1,                !- Zone or ZoneList Name",
+			"    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method",
+			"    12.5,                    !- Zone Cooling Design Supply Air Temperature {C}",
+			"    11.11,                   !- Zone Cooling Design Supply Air Temperature Difference {deltaC}",
+			"    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method",
+			"    50,                      !- Zone Heating Design Supply Air Temperature {C}",
+			"    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}",
+			"    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    SZ DSOA SPACE1-1,        !- Design Specification Outdoor Air Object Name",
+			"    ,                        !- Zone Heating Sizing Factor",
+			"    ,                        !- Zone Cooling Sizing Factor",
+			"    DesignDay,               !- Cooling Design Air Flow Method",
+			"    0,                       !- Cooling Design Air Flow Rate {m3/s}",
+			"    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Cooling Minimum Air Flow {m3/s}",
+			"    0,                       !- Cooling Minimum Air Flow Fraction",
+			"    DesignDay,               !- Heating Design Air Flow Method",
+			"    0,                       !- Heating Design Air Flow Rate {m3/s}",
+			"    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Heating Maximum Air Flow {m3/s}",
+			"    0,                       !- Heating Maximum Air Flow Fraction",
+			"    ,                        !- Design Specification Zone Air Distribution Object Name",
+			"    Yes,                     !- Account for Dedicated Outside Air System",
+			"    ColdSupplyAir,           !- Dedicated Outside Air System Control Strategy",
+			"    12.8,                    !- Dedicated Outside Air Low Setpoint for Design",
+			"    15.6;                    !- Dedicated Outside Air High Setpoint for Design",
+
+			"Sizing:Zone,",
+			"    SPACE2-1,                !- Zone or ZoneList Name",
+			"    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method",
+			"    12.5,                    !- Zone Cooling Design Supply Air Temperature {C}",
+			"    11.11,                   !- Zone Cooling Design Supply Air Temperature Difference {deltaC}",
+			"    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method",
+			"    50,                      !- Zone Heating Design Supply Air Temperature {C}",
+			"    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}",
+			"    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    SZ DSOA SPACE2-1,        !- Design Specification Outdoor Air Object Name",
+			"    ,                        !- Zone Heating Sizing Factor",
+			"    ,                        !- Zone Cooling Sizing Factor",
+			"    DesignDay,               !- Cooling Design Air Flow Method",
+			"    0,                       !- Cooling Design Air Flow Rate {m3/s}",
+			"    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Cooling Minimum Air Flow {m3/s}",
+			"    0,                       !- Cooling Minimum Air Flow Fraction",
+			"    DesignDay,               !- Heating Design Air Flow Method",
+			"    0,                       !- Heating Design Air Flow Rate {m3/s}",
+			"    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Heating Maximum Air Flow {m3/s}",
+			"    0,                       !- Heating Maximum Air Flow Fraction",
+			"    ,                        !- Design Specification Zone Air Distribution Object Name",
+			"    Yes,                     !- Account for Dedicated Outside Air System",
+			"    ColdSupplyAir,           !- Dedicated Outside Air System Control Strategy",
+			"    12.8,                    !- Dedicated Outside Air Low Setpoint for Design",
+			"    15.6;                    !- Dedicated Outside Air High Setpoint for Design",
+
+			"Sizing:Zone,",
+			"    SPACE3-1,                !- Zone or ZoneList Name",
+			"    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method",
+			"    12.5,                    !- Zone Cooling Design Supply Air Temperature {C}",
+			"    11.11,                   !- Zone Cooling Design Supply Air Temperature Difference {deltaC}",
+			"    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method",
+			"    50,                      !- Zone Heating Design Supply Air Temperature {C}",
+			"    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}",
+			"    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    SZ DSOA SPACE3-1,        !- Design Specification Outdoor Air Object Name",
+			"    ,                        !- Zone Heating Sizing Factor",
+			"    ,                        !- Zone Cooling Sizing Factor",
+			"    DesignDay,               !- Cooling Design Air Flow Method",
+			"    0,                       !- Cooling Design Air Flow Rate {m3/s}",
+			"    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Cooling Minimum Air Flow {m3/s}",
+			"    0,                       !- Cooling Minimum Air Flow Fraction",
+			"    DesignDay,               !- Heating Design Air Flow Method",
+			"    0,                       !- Heating Design Air Flow Rate {m3/s}",
+			"    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Heating Maximum Air Flow {m3/s}",
+			"    0,                       !- Heating Maximum Air Flow Fraction",
+			"    ,                        !- Design Specification Zone Air Distribution Object Name",
+			"    Yes,                     !- Account for Dedicated Outside Air System",
+			"    ColdSupplyAir,           !- Dedicated Outside Air System Control Strategy",
+			"    12.8,                    !- Dedicated Outside Air Low Setpoint for Design",
+			"    15.6;                    !- Dedicated Outside Air High Setpoint for Design",
+
+			"Sizing:Zone,",
+			"    SPACE4-1,                !- Zone or ZoneList Name",
+			"    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method",
+			"    12.5,                    !- Zone Cooling Design Supply Air Temperature {C}",
+			"    11.11,                   !- Zone Cooling Design Supply Air Temperature Difference {deltaC}",
+			"    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method",
+			"    50,                      !- Zone Heating Design Supply Air Temperature {C}",
+			"    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}",
+			"    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    SZ DSOA SPACE4-1,        !- Design Specification Outdoor Air Object Name",
+			"    ,                        !- Zone Heating Sizing Factor",
+			"    ,                        !- Zone Cooling Sizing Factor",
+			"    DesignDay,               !- Cooling Design Air Flow Method",
+			"    0,                       !- Cooling Design Air Flow Rate {m3/s}",
+			"    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Cooling Minimum Air Flow {m3/s}",
+			"    0,                       !- Cooling Minimum Air Flow Fraction",
+			"    DesignDay,               !- Heating Design Air Flow Method",
+			"    0,                       !- Heating Design Air Flow Rate {m3/s}",
+			"    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Heating Maximum Air Flow {m3/s}",
+			"    0,                       !- Heating Maximum Air Flow Fraction",
+			"    ,                        !- Design Specification Zone Air Distribution Object Name",
+			"    Yes,                     !- Account for Dedicated Outside Air System",
+			"    ColdSupplyAir,           !- Dedicated Outside Air System Control Strategy",
+			"    12.8,                    !- Dedicated Outside Air Low Setpoint for Design",
+			"    15.6;                    !- Dedicated Outside Air High Setpoint for Design",
+
+			"Sizing:Zone,",
+			"    SPACE5-1,                !- Zone or ZoneList Name",
+			"    SupplyAirTemperature,    !- Zone Cooling Design Supply Air Temperature Input Method",
+			"    12.5,                    !- Zone Cooling Design Supply Air Temperature {C}",
+			"    11.11,                   !- Zone Cooling Design Supply Air Temperature Difference {deltaC}",
+			"    SupplyAirTemperature,    !- Zone Heating Design Supply Air Temperature Input Method",
+			"    50,                      !- Zone Heating Design Supply Air Temperature {C}",
+			"    ,                        !- Zone Heating Design Supply Air Temperature Difference {deltaC}",
+			"    0.008,                   !- Zone Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    0.008,                   !- Zone Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    SZ DSOA SPACE5-1,        !- Design Specification Outdoor Air Object Name",
+			"    ,                        !- Zone Heating Sizing Factor",
+			"    ,                        !- Zone Cooling Sizing Factor",
+			"    DesignDay,               !- Cooling Design Air Flow Method",
+			"    0,                       !- Cooling Design Air Flow Rate {m3/s}",
+			"    ,                        !- Cooling Minimum Air Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Cooling Minimum Air Flow {m3/s}",
+			"    0,                       !- Cooling Minimum Air Flow Fraction",
+			"    DesignDay,               !- Heating Design Air Flow Method",
+			"    0,                       !- Heating Design Air Flow Rate {m3/s}",
+			"    ,                        !- Heating Maximum Air Flow per Zone Floor Area {m3/s-m2}",
+			"    ,                        !- Heating Maximum Air Flow {m3/s}",
+			"    0,                       !- Heating Maximum Air Flow Fraction",
+			"    ,                        !- Design Specification Zone Air Distribution Object Name",
+			"    Yes,                     !- Account for Dedicated Outside Air System",
+			"    ColdSupplyAir,           !- Dedicated Outside Air System Control Strategy",
+			"    12.8,                    !- Dedicated Outside Air Low Setpoint for Design",
+			"    15.6;                    !- Dedicated Outside Air High Setpoint for Design",
+
+			"Sizing:System,",
+			"    DOAS,                    !- AirLoop Name",
+			"    VentilationRequirement,  !- Type of Load to Size On",
+			"    autosize,                !- Design Outdoor Air Flow Rate {m3/s}",
+			"    1.0,                     !- Central Heating Maximum System Air Flow Ratio",
+			"    2,                       !- Preheat Design Temperature {C}",
+			"    0.008,                   !- Preheat Design Humidity Ratio {kgWater/kgDryAir}",
+			"    11,                      !- Precool Design Temperature {C}",
+			"    0.008,                   !- Precool Design Humidity Ratio {kgWater/kgDryAir}",
+			"    12.8,                    !- Central Cooling Design Supply Air Temperature {C}",
+			"    12.2,                    !- Central Heating Design Supply Air Temperature {C}",
+			"    NonCoincident,           !- Type of Zone Sum to Use",
+			"    Yes,                     !- 100% Outdoor Air in Cooling",
+			"    Yes,                     !- 100% Outdoor Air in Heating",
+			"    0.00924,                 !- Central Cooling Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    0.003,                   !- Central Heating Design Supply Air Humidity Ratio {kgWater/kgDryAir}",
+			"    DesignDay,               !- Cooling Supply Air Flow Rate Method",
+			"    0,                       !- Cooling Supply Air Flow Rate {m3/s}",
+			"    ,                        !- Cooling Supply Air Flow Rate Per Floor Area {m3/s-m2}",
+			"    ,                        !- Cooling Fraction of Autosized Cooling Supply Air Flow Rate",
+			"    ,                        !- Cooling Supply Air Flow Rate Per Unit Cooling Capacity {m3/s-W}",
+			"    DesignDay,               !- Heating Supply Air Flow Rate Method",
+			"    0,                       !- Heating Supply Air Flow Rate {m3/s}",
+			"    ,                        !- Heating Supply Air Flow Rate Per Floor Area {m3/s-m2}",
+			"    ,                        !- Heating Fraction of Autosized Heating Supply Air Flow Rate",
+			"    ,                        !- Heating Fraction of Autosized Cooling Supply Air Flow Rate",
+			"    ,                        !- Heating Supply Air Flow Rate Per Unit Heating Capacity {m3/s-W}",
+			"    ZoneSum,                 !- System Outdoor Air Method",
+			"    1.0,                     !- Zone Maximum Outdoor Air Fraction {dimensionless}",
+			"    CoolingDesignCapacity,   !- Cooling Design Capacity Method",
+			"    autosize,                !- Cooling Design Capacity {W}",
+			"    ,                        !- Cooling Design Capacity Per Floor Area {W/m2}",
+			"    ,                        !- Fraction of Autosized Cooling Design Capacity",
+			"    HeatingDesignCapacity,   !- Heating Design Capacity Method",
+			"    autosize,                !- Heating Design Capacity {W}",
+			"    ,                        !- Heating Design Capacity Per Floor Area {W/m2}",
+			"    ,                        !- Fraction of Autosized Heating Design Capacity",
+			"    OnOff;                   !- Central Cooling Capacity Control Method",
+
+			"Sizing:Plant,",
+			"    Hot Water Loop Hot Water Loop,  !- Plant or Condenser Loop Name",
+			"    Heating,                 !- Loop Type",
+			"    82,                      !- Design Loop Exit Temperature {C}",
+			"    11.0;                    !- Loop Design Temperature Difference {deltaC}",
+
+			"Sizing:Plant,",
+			"    Chilled Water Loop Chilled Water Loop,  !- Plant or Condenser Loop Name",
+			"    Cooling,                 !- Loop Type",
+			"    7.22,                    !- Design Loop Exit Temperature {C}",
+			"    6.67;                    !- Loop Design Temperature Difference {deltaC}",
+
+			"ZoneControl:Thermostat,",
+			"    SPACE1-1 Thermostat,     !- Name",
+			"    SPACE1-1,                !- Zone or ZoneList Name",
+			"    HVACTemplate-Always 4,   !- Control Type Schedule Name",
+			"    ThermostatSetpoint:DualSetpoint,  !- Control 1 Object Type",
+			"    All Zones Dual SP Control;  !- Control 1 Name",
+
+			"ZoneControl:Thermostat,",
+			"    SPACE2-1 Thermostat,     !- Name",
+			"    SPACE2-1,                !- Zone or ZoneList Name",
+			"    HVACTemplate-Always 4,   !- Control Type Schedule Name",
+			"    ThermostatSetpoint:DualSetpoint,  !- Control 1 Object Type",
+			"    All Zones Dual SP Control;  !- Control 1 Name",
+
+			"ZoneControl:Thermostat,",
+			"    SPACE3-1 Thermostat,     !- Name",
+			"    SPACE3-1,                !- Zone or ZoneList Name",
+			"    HVACTemplate-Always 4,   !- Control Type Schedule Name",
+			"    ThermostatSetpoint:DualSetpoint,  !- Control 1 Object Type",
+			"    All Zones Dual SP Control;  !- Control 1 Name",
+
+			"ZoneControl:Thermostat,",
+			"    SPACE4-1 Thermostat,     !- Name",
+			"    SPACE4-1,                !- Zone or ZoneList Name",
+			"    HVACTemplate-Always 4,   !- Control Type Schedule Name",
+			"    ThermostatSetpoint:DualSetpoint,  !- Control 1 Object Type",
+			"    All Zones Dual SP Control;  !- Control 1 Name",
+
+			"ZoneControl:Thermostat,",
+			"    SPACE5-1 Thermostat,     !- Name",
+			"    SPACE5-1,                !- Zone or ZoneList Name",
+			"    HVACTemplate-Always 4,   !- Control Type Schedule Name",
+			"    ThermostatSetpoint:DualSetpoint,  !- Control 1 Object Type",
+			"    All Zones Dual SP Control;  !- Control 1 Name",
+
+			"ThermostatSetpoint:DualSetpoint,",
+			"    All Zones Dual SP Control,  !- Name",
+			"    Htg-SetP-Sch,            !- Heating Setpoint Temperature Schedule Name",
+			"    Clg-SetP-Sch;            !- Cooling Setpoint Temperature Schedule Name",
+
+			"ZoneHVAC:FourPipeFanCoil,",
+			"    SPACE1-1 Fan Coil,       !- Name",
+			"    FanAvailSched,           !- Availability Schedule Name",
+			"    CyclingFan,              !- Capacity Control Method",
+			"    autosize,                !- Maximum Supply Air Flow Rate {m3/s}",
+			"    0.33,                    !- Low Speed Supply Air Flow Ratio",
+			"    0.66,                    !- Medium Speed Supply Air Flow Ratio",
+			"    0.0,                     !- Maximum Outdoor Air Flow Rate {m3/s}",
+			"    ,                        !- Outdoor Air Schedule Name",
+			"    SPACE1-1 Fan Coil Return,!- Air Inlet Node Name",
+			"    SPACE1-1 Supply Inlet,   !- Air Outlet Node Name",
+			"    OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type",
+			"    SPACE1-1 OA Mixing Box,  !- Outdoor Air Mixer Name",
+			"    Fan:OnOff,               !- Supply Air Fan Object Type",
+			"    SPACE1-1 Supply Fan,     !- Supply Air Fan Name",
+			"    Coil:Cooling:Water,      !- Cooling Coil Object Type",
+			"    SPACE1-1 Cooling Coil,   !- Cooling Coil Name",
+			"    autosize,                !- Maximum Cold Water Flow Rate {m3/s}",
+			"    0,                       !- Minimum Cold Water Flow Rate {m3/s}",
+			"    0.001,                   !- Cooling Convergence Tolerance",
+			"    Coil:Heating:Water,      !- Heating Coil Object Type",
+			"    SPACE1-1 Heating Coil,   !- Heating Coil Name",
+			"    autosize,                !- Maximum Hot Water Flow Rate {m3/s}",
+			"    0,                       !- Minimum Hot Water Flow Rate {m3/s}",
+			"    0.001;                   !- Heating Convergence Tolerance",
+
+			"ZoneHVAC:FourPipeFanCoil,",
+			"    SPACE2-1 Fan Coil,       !- Name",
+			"    FanAvailSched,           !- Availability Schedule Name",
+			"    CyclingFan,              !- Capacity Control Method",
+			"    autosize,                !- Maximum Supply Air Flow Rate {m3/s}",
+			"    0.33,                    !- Low Speed Supply Air Flow Ratio",
+			"    0.66,                    !- Medium Speed Supply Air Flow Ratio",
+			"    0.0,                     !- Maximum Outdoor Air Flow Rate {m3/s}",
+			"    ,                        !- Outdoor Air Schedule Name",
+			"    SPACE2-1 Fan Coil Return,!- Air Inlet Node Name",
+			"    SPACE2-1 Supply Inlet,   !- Air Outlet Node Name",
+			"    OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type",
+			"    SPACE2-1 OA Mixing Box,  !- Outdoor Air Mixer Name",
+			"    Fan:OnOff,               !- Supply Air Fan Object Type",
+			"    SPACE2-1 Supply Fan,     !- Supply Air Fan Name",
+			"    Coil:Cooling:Water,      !- Cooling Coil Object Type",
+			"    SPACE2-1 Cooling Coil,   !- Cooling Coil Name",
+			"    autosize,                !- Maximum Cold Water Flow Rate {m3/s}",
+			"    0,                       !- Minimum Cold Water Flow Rate {m3/s}",
+			"    0.001,                   !- Cooling Convergence Tolerance",
+			"    Coil:Heating:Water,      !- Heating Coil Object Type",
+			"    SPACE2-1 Heating Coil,   !- Heating Coil Name",
+			"    autosize,                !- Maximum Hot Water Flow Rate {m3/s}",
+			"    0,                       !- Minimum Hot Water Flow Rate {m3/s}",
+			"    0.001;                   !- Heating Convergence Tolerance",
+
+			"ZoneHVAC:FourPipeFanCoil,",
+			"    SPACE3-1 Fan Coil,       !- Name",
+			"    FanAvailSched,           !- Availability Schedule Name",
+			"    CyclingFan,              !- Capacity Control Method",
+			"    autosize,                !- Maximum Supply Air Flow Rate {m3/s}",
+			"    0.33,                    !- Low Speed Supply Air Flow Ratio",
+			"    0.66,                    !- Medium Speed Supply Air Flow Ratio",
+			"    0.0,                     !- Maximum Outdoor Air Flow Rate {m3/s}",
+			"    ,                        !- Outdoor Air Schedule Name",
+			"    SPACE3-1 Fan Coil Return,!- Air Inlet Node Name",
+			"    SPACE3-1 Supply Inlet,   !- Air Outlet Node Name",
+			"    OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type",
+			"    SPACE3-1 OA Mixing Box,  !- Outdoor Air Mixer Name",
+			"    Fan:OnOff,               !- Supply Air Fan Object Type",
+			"    SPACE3-1 Supply Fan,     !- Supply Air Fan Name",
+			"    Coil:Cooling:Water,      !- Cooling Coil Object Type",
+			"    SPACE3-1 Cooling Coil,   !- Cooling Coil Name",
+			"    autosize,                !- Maximum Cold Water Flow Rate {m3/s}",
+			"    0,                       !- Minimum Cold Water Flow Rate {m3/s}",
+			"    0.001,                   !- Cooling Convergence Tolerance",
+			"    Coil:Heating:Water,      !- Heating Coil Object Type",
+			"    SPACE3-1 Heating Coil,   !- Heating Coil Name",
+			"    autosize,                !- Maximum Hot Water Flow Rate {m3/s}",
+			"    0,                       !- Minimum Hot Water Flow Rate {m3/s}",
+			"    0.001;                   !- Heating Convergence Tolerance",
+
+			"ZoneHVAC:FourPipeFanCoil,",
+			"    SPACE4-1 Fan Coil,       !- Name",
+			"    FanAvailSched,           !- Availability Schedule Name",
+			"    CyclingFan,              !- Capacity Control Method",
+			"    autosize,                !- Maximum Supply Air Flow Rate {m3/s}",
+			"    0.33,                    !- Low Speed Supply Air Flow Ratio",
+			"    0.66,                    !- Medium Speed Supply Air Flow Ratio",
+			"    0.0,                     !- Maximum Outdoor Air Flow Rate {m3/s}",
+			"    ,                        !- Outdoor Air Schedule Name",
+			"    SPACE4-1 Fan Coil Return,!- Air Inlet Node Name",
+			"    SPACE4-1 Supply Inlet,   !- Air Outlet Node Name",
+			"    OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type",
+			"    SPACE4-1 OA Mixing Box,  !- Outdoor Air Mixer Name",
+			"    Fan:OnOff,               !- Supply Air Fan Object Type",
+			"    SPACE4-1 Supply Fan,     !- Supply Air Fan Name",
+			"    Coil:Cooling:Water,      !- Cooling Coil Object Type",
+			"    SPACE4-1 Cooling Coil,   !- Cooling Coil Name",
+			"    autosize,                !- Maximum Cold Water Flow Rate {m3/s}",
+			"    0,                       !- Minimum Cold Water Flow Rate {m3/s}",
+			"    0.001,                   !- Cooling Convergence Tolerance",
+			"    Coil:Heating:Water,      !- Heating Coil Object Type",
+			"    SPACE4-1 Heating Coil,   !- Heating Coil Name",
+			"    autosize,                !- Maximum Hot Water Flow Rate {m3/s}",
+			"    0,                       !- Minimum Hot Water Flow Rate {m3/s}",
+			"    0.001;                   !- Heating Convergence Tolerance",
+
+			"ZoneHVAC:FourPipeFanCoil,",
+			"    SPACE5-1 Fan Coil,       !- Name",
+			"    FanAvailSched,           !- Availability Schedule Name",
+			"    CyclingFan,              !- Capacity Control Method",
+			"    autosize,                !- Maximum Supply Air Flow Rate {m3/s}",
+			"    0.33,                    !- Low Speed Supply Air Flow Ratio",
+			"    0.66,                    !- Medium Speed Supply Air Flow Ratio",
+			"    0.0,                     !- Maximum Outdoor Air Flow Rate {m3/s}",
+			"    ,                        !- Outdoor Air Schedule Name",
+			"    SPACE5-1 Fan Coil Return,!- Air Inlet Node Name",
+			"    SPACE5-1 Supply Inlet,   !- Air Outlet Node Name",
+			"    OutdoorAir:Mixer,        !- Outdoor Air Mixer Object Type",
+			"    SPACE5-1 OA Mixing Box,  !- Outdoor Air Mixer Name",
+			"    Fan:OnOff,               !- Supply Air Fan Object Type",
+			"    SPACE5-1 Supply Fan,     !- Supply Air Fan Name",
+			"    Coil:Cooling:Water,      !- Cooling Coil Object Type",
+			"    SPACE5-1 Cooling Coil,   !- Cooling Coil Name",
+			"    autosize,                !- Maximum Cold Water Flow Rate {m3/s}",
+			"    0,                       !- Minimum Cold Water Flow Rate {m3/s}",
+			"    0.001,                   !- Cooling Convergence Tolerance",
+			"    Coil:Heating:Water,      !- Heating Coil Object Type",
+			"    SPACE5-1 Heating Coil,   !- Heating Coil Name",
+			"    autosize,                !- Maximum Hot Water Flow Rate {m3/s}",
+			"    0,                       !- Minimum Hot Water Flow Rate {m3/s}",
+			"    0.001;                   !- Heating Convergence Tolerance",
+
+			"AirTerminal:SingleDuct:VAV:NoReheat,",
+			"    SPACE1-1 DOAS Air Terminal,  !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    SPACE1-1 DOAS Supply Inlet,  !- Air Outlet Node Name",
+			"    SPACE1-1 Zone Equip Inlet,  !- Air Inlet Node Name",
+			"    autosize,                !- Maximum Air Flow Rate {m3/s}",
+			"    Constant,                !- Zone Minimum Air Flow Input Method",
+			"    1.0;                     !- Constant Minimum Air Flow Fraction",
+
+			"AirTerminal:SingleDuct:VAV:NoReheat,",
+			"    SPACE2-1 DOAS Air Terminal,  !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    SPACE2-1 DOAS Supply Inlet,  !- Air Outlet Node Name",
+			"    SPACE2-1 Zone Equip Inlet,  !- Air Inlet Node Name",
+			"    autosize,                !- Maximum Air Flow Rate {m3/s}",
+			"    Constant,                !- Zone Minimum Air Flow Input Method",
+			"    1.0;                     !- Constant Minimum Air Flow Fraction",
+
+			"AirTerminal:SingleDuct:VAV:NoReheat,",
+			"    SPACE3-1 DOAS Air Terminal,  !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    SPACE3-1 DOAS Supply Inlet,  !- Air Outlet Node Name",
+			"    SPACE3-1 Zone Equip Inlet,  !- Air Inlet Node Name",
+			"    autosize,                !- Maximum Air Flow Rate {m3/s}",
+			"    Constant,                !- Zone Minimum Air Flow Input Method",
+			"    1.0;                     !- Constant Minimum Air Flow Fraction",
+
+			"AirTerminal:SingleDuct:VAV:NoReheat,",
+			"    SPACE4-1 DOAS Air Terminal,  !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    SPACE4-1 DOAS Supply Inlet,  !- Air Outlet Node Name",
+			"    SPACE4-1 Zone Equip Inlet,  !- Air Inlet Node Name",
+			"    autosize,                !- Maximum Air Flow Rate {m3/s}",
+			"    Constant,                !- Zone Minimum Air Flow Input Method",
+			"    1.0;                     !- Constant Minimum Air Flow Fraction",
+
+			"AirTerminal:SingleDuct:VAV:NoReheat,",
+			"    SPACE5-1 DOAS Air Terminal,  !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    SPACE5-1 DOAS Supply Inlet,  !- Air Outlet Node Name",
+			"    SPACE5-1 Zone Equip Inlet,  !- Air Inlet Node Name",
+			"    autosize,                !- Maximum Air Flow Rate {m3/s}",
+			"    Constant,                !- Zone Minimum Air Flow Input Method",
+			"    1.0;                     !- Constant Minimum Air Flow Fraction",
+
+			"ZoneHVAC:AirDistributionUnit,",
+			"    SPACE1-1 DOAS ATU,       !- Name",
+			"    SPACE1-1 DOAS Supply Inlet,  !- Air Distribution Unit Outlet Node Name",
+			"    AirTerminal:SingleDuct:VAV:NoReheat,  !- Air Terminal Object Type",
+			"    SPACE1-1 DOAS Air Terminal;  !- Air Terminal Name",
+
+			"ZoneHVAC:AirDistributionUnit,",
+			"    SPACE2-1 DOAS ATU,       !- Name",
+			"    SPACE2-1 DOAS Supply Inlet,  !- Air Distribution Unit Outlet Node Name",
+			"    AirTerminal:SingleDuct:VAV:NoReheat,  !- Air Terminal Object Type",
+			"    SPACE2-1 DOAS Air Terminal;  !- Air Terminal Name",
+
+			"ZoneHVAC:AirDistributionUnit,",
+			"    SPACE3-1 DOAS ATU,       !- Name",
+			"    SPACE3-1 DOAS Supply Inlet,  !- Air Distribution Unit Outlet Node Name",
+			"    AirTerminal:SingleDuct:VAV:NoReheat,  !- Air Terminal Object Type",
+			"    SPACE3-1 DOAS Air Terminal;  !- Air Terminal Name",
+
+			"ZoneHVAC:AirDistributionUnit,",
+			"    SPACE4-1 DOAS ATU,       !- Name",
+			"    SPACE4-1 DOAS Supply Inlet,  !- Air Distribution Unit Outlet Node Name",
+			"    AirTerminal:SingleDuct:VAV:NoReheat,  !- Air Terminal Object Type",
+			"    SPACE4-1 DOAS Air Terminal;  !- Air Terminal Name",
+
+			"ZoneHVAC:AirDistributionUnit,",
+			"    SPACE5-1 DOAS ATU,       !- Name",
+			"    SPACE5-1 DOAS Supply Inlet,  !- Air Distribution Unit Outlet Node Name",
+			"    AirTerminal:SingleDuct:VAV:NoReheat,  !- Air Terminal Object Type",
+			"    SPACE5-1 DOAS Air Terminal;  !- Air Terminal Name",
+
+			"ZoneHVAC:EquipmentList,",
+			"    SPACE1-1 Equipment,      !- Name",
+			"    ZoneHVAC:AirDistributionUnit,  !- Zone Equipment 1 Object Type",
+			"    SPACE1-1 DOAS ATU,       !- Zone Equipment 1 Name",
+			"    1,                       !- Zone Equipment 1 Cooling Sequence",
+			"    1,                       !- Zone Equipment 1 Heating or No-Load Sequence",
+			"    ZoneHVAC:FourPipeFanCoil,!- Zone Equipment 2 Object Type",
+			"    SPACE1-1 Fan Coil,       !- Zone Equipment 2 Name",
+			"    2,                       !- Zone Equipment 2 Cooling Sequence",
+			"    2;                       !- Zone Equipment 2 Heating or No-Load Sequence",
+
+			"ZoneHVAC:EquipmentList,",
+			"    SPACE2-1 Equipment,      !- Name",
+			"    ZoneHVAC:AirDistributionUnit,  !- Zone Equipment 1 Object Type",
+			"    SPACE2-1 DOAS ATU,       !- Zone Equipment 1 Name",
+			"    1,                       !- Zone Equipment 1 Cooling Sequence",
+			"    1,                       !- Zone Equipment 1 Heating or No-Load Sequence",
+			"    ZoneHVAC:FourPipeFanCoil,!- Zone Equipment 2 Object Type",
+			"    SPACE2-1 Fan Coil,       !- Zone Equipment 2 Name",
+			"    2,                       !- Zone Equipment 2 Cooling Sequence",
+			"    2;                       !- Zone Equipment 2 Heating or No-Load Sequence",
+
+			"ZoneHVAC:EquipmentList,",
+			"    SPACE3-1 Equipment,      !- Name",
+			"    ZoneHVAC:AirDistributionUnit,  !- Zone Equipment 1 Object Type",
+			"    SPACE3-1 DOAS ATU,       !- Zone Equipment 1 Name",
+			"    1,                       !- Zone Equipment 1 Cooling Sequence",
+			"    1,                       !- Zone Equipment 1 Heating or No-Load Sequence",
+			"    ZoneHVAC:FourPipeFanCoil,!- Zone Equipment 2 Object Type",
+			"    SPACE3-1 Fan Coil,       !- Zone Equipment 2 Name",
+			"    2,                       !- Zone Equipment 2 Cooling Sequence",
+			"    2;                       !- Zone Equipment 2 Heating or No-Load Sequence",
+
+			"ZoneHVAC:EquipmentList,",
+			"    SPACE4-1 Equipment,      !- Name",
+			"    ZoneHVAC:AirDistributionUnit,  !- Zone Equipment 1 Object Type",
+			"    SPACE4-1 DOAS ATU,       !- Zone Equipment 1 Name",
+			"    1,                       !- Zone Equipment 1 Cooling Sequence",
+			"    1,                       !- Zone Equipment 1 Heating or No-Load Sequence",
+			"    ZoneHVAC:FourPipeFanCoil,!- Zone Equipment 2 Object Type",
+			"    SPACE4-1 Fan Coil,       !- Zone Equipment 2 Name",
+			"    2,                       !- Zone Equipment 2 Cooling Sequence",
+			"    2;                       !- Zone Equipment 2 Heating or No-Load Sequence",
+
+			"ZoneHVAC:EquipmentList,",
+			"    SPACE5-1 Equipment,      !- Name",
+			"    ZoneHVAC:AirDistributionUnit,  !- Zone Equipment 1 Object Type",
+			"    SPACE5-1 DOAS ATU,       !- Zone Equipment 1 Name",
+			"    1,                       !- Zone Equipment 1 Cooling Sequence",
+			"    1,                       !- Zone Equipment 1 Heating or No-Load Sequence",
+			"    ZoneHVAC:FourPipeFanCoil,!- Zone Equipment 2 Object Type",
+			"    SPACE5-1 Fan Coil,       !- Zone Equipment 2 Name",
+			"    2,                       !- Zone Equipment 2 Cooling Sequence",
+			"    2;                       !- Zone Equipment 2 Heating or No-Load Sequence",
+
+			"ZoneHVAC:EquipmentConnections,",
+			"    SPACE1-1,                !- Zone Name",
+			"    SPACE1-1 Equipment,      !- Zone Conditioning Equipment List Name",
+			"    SPACE1-1 Inlets,         !- Zone Air Inlet Node or NodeList Name",
+			"    SPACE1-1 Fan Coil Return,!- Zone Air Exhaust Node or NodeList Name",
+			"    SPACE1-1 Zone Air Node,  !- Zone Air Node Name",
+			"    SPACE1-1 Return Outlet;  !- Zone Return Air Node Name",
+
+			"ZoneHVAC:EquipmentConnections,",
+			"    SPACE2-1,                !- Zone Name",
+			"    SPACE2-1 Equipment,      !- Zone Conditioning Equipment List Name",
+			"    SPACE2-1 Inlets,         !- Zone Air Inlet Node or NodeList Name",
+			"    SPACE2-1 Fan Coil Return,!- Zone Air Exhaust Node or NodeList Name",
+			"    SPACE2-1 Zone Air Node,  !- Zone Air Node Name",
+			"    SPACE2-1 Return Outlet;  !- Zone Return Air Node Name",
+
+			"ZoneHVAC:EquipmentConnections,",
+			"    SPACE3-1,                !- Zone Name",
+			"    SPACE3-1 Equipment,      !- Zone Conditioning Equipment List Name",
+			"    SPACE3-1 Inlets,         !- Zone Air Inlet Node or NodeList Name",
+			"    SPACE3-1 Fan Coil Return,!- Zone Air Exhaust Node or NodeList Name",
+			"    SPACE3-1 Zone Air Node,  !- Zone Air Node Name",
+			"    SPACE3-1 Return Outlet;  !- Zone Return Air Node Name",
+
+			"ZoneHVAC:EquipmentConnections,",
+			"    SPACE4-1,                !- Zone Name",
+			"    SPACE4-1 Equipment,      !- Zone Conditioning Equipment List Name",
+			"    SPACE4-1 Inlets,         !- Zone Air Inlet Node or NodeList Name",
+			"    SPACE4-1 Fan Coil Return,!- Zone Air Exhaust Node or NodeList Name",
+			"    SPACE4-1 Zone Air Node,  !- Zone Air Node Name",
+			"    SPACE4-1 Return Outlet;  !- Zone Return Air Node Name",
+
+			"ZoneHVAC:EquipmentConnections,",
+			"    SPACE5-1,                !- Zone Name",
+			"    SPACE5-1 Equipment,      !- Zone Conditioning Equipment List Name",
+			"    SPACE5-1 Inlets,         !- Zone Air Inlet Node or NodeList Name",
+			"    SPACE5-1 Fan Coil Return,!- Zone Air Exhaust Node or NodeList Name",
+			"    SPACE5-1 Zone Air Node,  !- Zone Air Node Name",
+			"    SPACE5-1 Return Outlet;  !- Zone Return Air Node Name",
+
+			"Fan:VariableVolume,",
+			"    DOAS Supply Fan,         !- Name",
+			"    FanAvailSched,                !- Availability Schedule Name",
+			"    0.7,                     !- Fan Total Efficiency",
+			"    1000,                    !- Pressure Rise {Pa}",
+			"    autosize,                !- Maximum Flow Rate {m3/s}",
+			"    Fraction,                !- Fan Power Minimum Flow Rate Input Method",
+			"    0.0,                     !- Fan Power Minimum Flow Fraction",
+			"    ,                        !- Fan Power Minimum Air Flow Rate {m3/s}",
+			"    0.9,                     !- Motor Efficiency",
+			"    1,                       !- Motor In Airstream Fraction",
+			"    0.0015302446,            !- Fan Power Coefficient 1",
+			"    0.0052080574,            !- Fan Power Coefficient 2",
+			"    1.1086242,               !- Fan Power Coefficient 3",
+			"    -0.11635563,             !- Fan Power Coefficient 4",
+			"    0,                       !- Fan Power Coefficient 5",
+			"    DOAS Heating Coil Outlet,!- Air Inlet Node Name",
+			"    DOAS Supply Fan Outlet;  !- Air Outlet Node Name",
+
+			"Fan:OnOff,",
+			"    SPACE1-1 Supply Fan,     !- Name",
+			"    FanAvailSched,           !- Availability Schedule Name",
+			"    0.7,                     !- Fan Total Efficiency",
+			"    75,                      !- Pressure Rise {Pa}",
+			"    autosize,                !- Maximum Flow Rate {m3/s}",
+			"    0.9,                     !- Motor Efficiency",
+			"    1,                       !- Motor In Airstream Fraction",
+			"    SPACE1-1 Mixed Air Outlet,  !- Air Inlet Node Name",
+			"    SPACE1-1 Supply Fan Outlet;  !- Air Outlet Node Name",
+
+			"Fan:OnOff,",
+			"    SPACE2-1 Supply Fan,     !- Name",
+			"    FanAvailSched,           !- Availability Schedule Name",
+			"    0.7,                     !- Fan Total Efficiency",
+			"    75,                      !- Pressure Rise {Pa}",
+			"    autosize,                !- Maximum Flow Rate {m3/s}",
+			"    0.9,                     !- Motor Efficiency",
+			"    1,                       !- Motor In Airstream Fraction",
+			"    SPACE2-1 Mixed Air Outlet,  !- Air Inlet Node Name",
+			"    SPACE2-1 Supply Fan Outlet;  !- Air Outlet Node Name",
+
+			"Fan:OnOff,",
+			"    SPACE3-1 Supply Fan,     !- Name",
+			"    FanAvailSched,           !- Availability Schedule Name",
+			"    0.7,                     !- Fan Total Efficiency",
+			"    75,                      !- Pressure Rise {Pa}",
+			"    autosize,                !- Maximum Flow Rate {m3/s}",
+			"    0.9,                     !- Motor Efficiency",
+			"    1,                       !- Motor In Airstream Fraction",
+			"    SPACE3-1 Mixed Air Outlet,  !- Air Inlet Node Name",
+			"    SPACE3-1 Supply Fan Outlet;  !- Air Outlet Node Name",
+
+			"Fan:OnOff,",
+			"    SPACE4-1 Supply Fan,     !- Name",
+			"    FanAvailSched,           !- Availability Schedule Name",
+			"    0.7,                     !- Fan Total Efficiency",
+			"    75,                      !- Pressure Rise {Pa}",
+			"    autosize,                !- Maximum Flow Rate {m3/s}",
+			"    0.9,                     !- Motor Efficiency",
+			"    1,                       !- Motor In Airstream Fraction",
+			"    SPACE4-1 Mixed Air Outlet,  !- Air Inlet Node Name",
+			"    SPACE4-1 Supply Fan Outlet;  !- Air Outlet Node Name",
+
+			"Fan:OnOff,",
+			"    SPACE5-1 Supply Fan,     !- Name",
+			"    FanAvailSched,           !- Availability Schedule Name",
+			"    0.7,                     !- Fan Total Efficiency",
+			"    75,                      !- Pressure Rise {Pa}",
+			"    autosize,                !- Maximum Flow Rate {m3/s}",
+			"    0.9,                     !- Motor Efficiency",
+			"    1,                       !- Motor In Airstream Fraction",
+			"    SPACE5-1 Mixed Air Outlet,  !- Air Inlet Node Name",
+			"    SPACE5-1 Supply Fan Outlet;  !- Air Outlet Node Name",
+
+			"Coil:Cooling:Water,",
+			"    SPACE1-1 Cooling Coil,   !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- Design Water Flow Rate {m3/s}",
+			"    autosize,                !- Design Air Flow Rate {m3/s}",
+			"    autosize,                !- Design Inlet Water Temperature {C}",
+			"    autosize,                !- Design Inlet Air Temperature {C}",
+			"    autosize,                !- Design Outlet Air Temperature {C}",
+			"    autosize,                !- Design Inlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    autosize,                !- Design Outlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    SPACE1-1 Cooling Coil ChW Inlet,  !- Water Inlet Node Name",
+			"    SPACE1-1 Cooling Coil ChW Outlet,  !- Water Outlet Node Name",
+			"    SPACE1-1 Supply Fan Outlet,  !- Air Inlet Node Name",
+			"    SPACE1-1 Cooling Coil Outlet,  !- Air Outlet Node Name",
+			"    DetailedAnalysis,        !- Type of Analysis",
+			"    CrossFlow;               !- Heat Exchanger Configuration",
+
+			"Coil:Cooling:Water,",
+			"    SPACE2-1 Cooling Coil,   !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- Design Water Flow Rate {m3/s}",
+			"    autosize,                !- Design Air Flow Rate {m3/s}",
+			"    autosize,                !- Design Inlet Water Temperature {C}",
+			"    autosize,                !- Design Inlet Air Temperature {C}",
+			"    autosize,                !- Design Outlet Air Temperature {C}",
+			"    autosize,                !- Design Inlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    autosize,                !- Design Outlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    SPACE2-1 Cooling Coil ChW Inlet,  !- Water Inlet Node Name",
+			"    SPACE2-1 Cooling Coil ChW Outlet,  !- Water Outlet Node Name",
+			"    SPACE2-1 Supply Fan Outlet,  !- Air Inlet Node Name",
+			"    SPACE2-1 Cooling Coil Outlet,  !- Air Outlet Node Name",
+			"    DetailedAnalysis,        !- Type of Analysis",
+			"    CrossFlow;               !- Heat Exchanger Configuration",
+
+			"Coil:Cooling:Water,",
+			"    SPACE3-1 Cooling Coil,   !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- Design Water Flow Rate {m3/s}",
+			"    autosize,                !- Design Air Flow Rate {m3/s}",
+			"    autosize,                !- Design Inlet Water Temperature {C}",
+			"    autosize,                !- Design Inlet Air Temperature {C}",
+			"    autosize,                !- Design Outlet Air Temperature {C}",
+			"    autosize,                !- Design Inlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    autosize,                !- Design Outlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    SPACE3-1 Cooling Coil ChW Inlet,  !- Water Inlet Node Name",
+			"    SPACE3-1 Cooling Coil ChW Outlet,  !- Water Outlet Node Name",
+			"    SPACE3-1 Supply Fan Outlet,  !- Air Inlet Node Name",
+			"    SPACE3-1 Cooling Coil Outlet,  !- Air Outlet Node Name",
+			"    DetailedAnalysis,        !- Type of Analysis",
+			"    CrossFlow;               !- Heat Exchanger Configuration",
+
+			"Coil:Cooling:Water,",
+			"    SPACE4-1 Cooling Coil,   !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- Design Water Flow Rate {m3/s}",
+			"    autosize,                !- Design Air Flow Rate {m3/s}",
+			"    autosize,                !- Design Inlet Water Temperature {C}",
+			"    autosize,                !- Design Inlet Air Temperature {C}",
+			"    autosize,                !- Design Outlet Air Temperature {C}",
+			"    autosize,                !- Design Inlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    autosize,                !- Design Outlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    SPACE4-1 Cooling Coil ChW Inlet,  !- Water Inlet Node Name",
+			"    SPACE4-1 Cooling Coil ChW Outlet,  !- Water Outlet Node Name",
+			"    SPACE4-1 Supply Fan Outlet,  !- Air Inlet Node Name",
+			"    SPACE4-1 Cooling Coil Outlet,  !- Air Outlet Node Name",
+			"    DetailedAnalysis,        !- Type of Analysis",
+			"    CrossFlow;               !- Heat Exchanger Configuration",
+
+			"Coil:Cooling:Water,",
+			"    SPACE5-1 Cooling Coil,   !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- Design Water Flow Rate {m3/s}",
+			"    autosize,                !- Design Air Flow Rate {m3/s}",
+			"    autosize,                !- Design Inlet Water Temperature {C}",
+			"    autosize,                !- Design Inlet Air Temperature {C}",
+			"    autosize,                !- Design Outlet Air Temperature {C}",
+			"    autosize,                !- Design Inlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    autosize,                !- Design Outlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    SPACE5-1 Cooling Coil ChW Inlet,  !- Water Inlet Node Name",
+			"    SPACE5-1 Cooling Coil ChW Outlet,  !- Water Outlet Node Name",
+			"    SPACE5-1 Supply Fan Outlet,  !- Air Inlet Node Name",
+			"    SPACE5-1 Cooling Coil Outlet,  !- Air Outlet Node Name",
+			"    DetailedAnalysis,        !- Type of Analysis",
+			"    CrossFlow;               !- Heat Exchanger Configuration",
+
+			"Coil:Cooling:Water,",
+			"    DOAS Cooling Coil,       !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- Design Water Flow Rate {m3/s}",
+			"    autosize,                !- Design Air Flow Rate {m3/s}",
+			"    autosize,                !- Design Inlet Water Temperature {C}",
+			"    autosize,                !- Design Inlet Air Temperature {C}",
+			"    autosize,                !- Design Outlet Air Temperature {C}",
+			"    autosize,                !- Design Inlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    autosize,                !- Design Outlet Air Humidity Ratio {kgWater/kgDryAir}",
+			"    DOAS Cooling Coil ChW Inlet,  !- Water Inlet Node Name",
+			"    DOAS Cooling Coil ChW Outlet,  !- Water Outlet Node Name",
+			"    DOAS Heat Recovery Supply Outlet,   !- Air Inlet Node Name",
+			"    DOAS Cooling Coil Outlet,!- Air Outlet Node Name",
+			"    DetailedAnalysis,        !- Type of Analysis",
+			"    CrossFlow;               !- Heat Exchanger Configuration",
+
+			"Coil:Heating:Water,",
+			"    SPACE1-1 Heating Coil,   !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- U-Factor Times Area Value {W/K}",
+			"    autosize,                !- Maximum Water Flow Rate {m3/s}",
+			"    SPACE1-1 Heating Coil HW Inlet,  !- Water Inlet Node Name",
+			"    SPACE1-1 Heating Coil HW Outlet,  !- Water Outlet Node Name",
+			"    SPACE1-1 Cooling Coil Outlet,  !- Air Inlet Node Name",
+			"    SPACE1-1 Supply Inlet,   !- Air Outlet Node Name",
+			"    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method",
+			"    autosize,                !- Rated Capacity {W}",
+			"    82.2,                    !- Rated Inlet Water Temperature {C}",
+			"    16.6,                    !- Rated Inlet Air Temperature {C}",
+			"    71.1,                    !- Rated Outlet Water Temperature {C}",
+			"    32.2,                    !- Rated Outlet Air Temperature {C}",
+			"    0.5;                     !- Rated Ratio for Air and Water Convection",
+
+			"Coil:Heating:Water,",
+			"    SPACE2-1 Heating Coil,   !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- U-Factor Times Area Value {W/K}",
+			"    autosize,                !- Maximum Water Flow Rate {m3/s}",
+			"    SPACE2-1 Heating Coil HW Inlet,  !- Water Inlet Node Name",
+			"    SPACE2-1 Heating Coil HW Outlet,  !- Water Outlet Node Name",
+			"    SPACE2-1 Cooling Coil Outlet,  !- Air Inlet Node Name",
+			"    SPACE2-1 Supply Inlet,   !- Air Outlet Node Name",
+			"    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method",
+			"    autosize,                !- Rated Capacity {W}",
+			"    82.2,                    !- Rated Inlet Water Temperature {C}",
+			"    16.6,                    !- Rated Inlet Air Temperature {C}",
+			"    71.1,                    !- Rated Outlet Water Temperature {C}",
+			"    32.2,                    !- Rated Outlet Air Temperature {C}",
+			"    0.5;                     !- Rated Ratio for Air and Water Convection",
+
+			"Coil:Heating:Water,",
+			"    SPACE3-1 Heating Coil,   !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- U-Factor Times Area Value {W/K}",
+			"    autosize,                !- Maximum Water Flow Rate {m3/s}",
+			"    SPACE3-1 Heating Coil HW Inlet,  !- Water Inlet Node Name",
+			"    SPACE3-1 Heating Coil HW Outlet,  !- Water Outlet Node Name",
+			"    SPACE3-1 Cooling Coil Outlet,  !- Air Inlet Node Name",
+			"    SPACE3-1 Supply Inlet,   !- Air Outlet Node Name",
+			"    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method",
+			"    autosize,                !- Rated Capacity {W}",
+			"    82.2,                    !- Rated Inlet Water Temperature {C}",
+			"    16.6,                    !- Rated Inlet Air Temperature {C}",
+			"    71.1,                    !- Rated Outlet Water Temperature {C}",
+			"    32.2,                    !- Rated Outlet Air Temperature {C}",
+			"    0.5;                     !- Rated Ratio for Air and Water Convection",
+
+			"Coil:Heating:Water,",
+			"    SPACE4-1 Heating Coil,   !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- U-Factor Times Area Value {W/K}",
+			"    autosize,                !- Maximum Water Flow Rate {m3/s}",
+			"    SPACE4-1 Heating Coil HW Inlet,  !- Water Inlet Node Name",
+			"    SPACE4-1 Heating Coil HW Outlet,  !- Water Outlet Node Name",
+			"    SPACE4-1 Cooling Coil Outlet,  !- Air Inlet Node Name",
+			"    SPACE4-1 Supply Inlet,   !- Air Outlet Node Name",
+			"    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method",
+			"    autosize,                !- Rated Capacity {W}",
+			"    82.2,                    !- Rated Inlet Water Temperature {C}",
+			"    16.6,                    !- Rated Inlet Air Temperature {C}",
+			"    71.1,                    !- Rated Outlet Water Temperature {C}",
+			"    32.2,                    !- Rated Outlet Air Temperature {C}",
+			"    0.5;                     !- Rated Ratio for Air and Water Convection",
+
+			"Coil:Heating:Water,",
+			"    SPACE5-1 Heating Coil,   !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- U-Factor Times Area Value {W/K}",
+			"    autosize,                !- Maximum Water Flow Rate {m3/s}",
+			"    SPACE5-1 Heating Coil HW Inlet,  !- Water Inlet Node Name",
+			"    SPACE5-1 Heating Coil HW Outlet,  !- Water Outlet Node Name",
+			"    SPACE5-1 Cooling Coil Outlet,  !- Air Inlet Node Name",
+			"    SPACE5-1 Supply Inlet,   !- Air Outlet Node Name",
+			"    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method",
+			"    autosize,                !- Rated Capacity {W}",
+			"    82.2,                    !- Rated Inlet Water Temperature {C}",
+			"    16.6,                    !- Rated Inlet Air Temperature {C}",
+			"    71.1,                    !- Rated Outlet Water Temperature {C}",
+			"    32.2,                    !- Rated Outlet Air Temperature {C}",
+			"    0.5;                     !- Rated Ratio for Air and Water Convection",
+
+			"Coil:Heating:Water,",
+			"    DOAS Heating Coil,       !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- U-Factor Times Area Value {W/K}",
+			"    autosize,                !- Maximum Water Flow Rate {m3/s}",
+			"    DOAS Heating Coil HW Inlet,  !- Water Inlet Node Name",
+			"    DOAS Heating Coil HW Outlet,  !- Water Outlet Node Name",
+			"    DOAS Cooling Coil Outlet,!- Air Inlet Node Name",
+			"    DOAS Heating Coil Outlet,!- Air Outlet Node Name",
+			"    UFactorTimesAreaAndDesignWaterFlowRate,  !- Performance Input Method",
+			"    autosize,                !- Rated Capacity {W}",
+			"    82.2,                    !- Rated Inlet Water Temperature {C}",
+			"    16.6,                    !- Rated Inlet Air Temperature {C}",
+			"    71.1,                    !- Rated Outlet Water Temperature {C}",
+			"    32.2,                    !- Rated Outlet Air Temperature {C}",
+			"    0.5;                     !- Rated Ratio for Air and Water Convection",
+
+			"HeatExchanger:AirToAir:SensibleAndLatent,",
+			"    DOAS Heat Recovery,      !- Name",
+			"    HVACTemplate-Always 1,   !- Availability Schedule Name",
+			"    autosize,                !- Nominal Supply Air Flow Rate {m3/s}",
+			"    0.7,                     !- Sensible Effectiveness at 100% Heating Air Flow {dimensionless}",
+			"    0.65,                    !- Latent Effectiveness at 100% Heating Air Flow {dimensionless}",
+			"    0.750000,                !- Sensible Effectiveness at 75% Heating Air Flow {dimensionless}",
+			"    0.700000,                !- Latent Effectiveness at 75% Heating Air Flow {dimensionless}",
+			"    0.7,                     !- Sensible Effectiveness at 100% Cooling Air Flow {dimensionless}",
+			"    0.65,                    !- Latent Effectiveness at 100% Cooling Air Flow {dimensionless}",
+			"    0.750000,                !- Sensible Effectiveness at 75% Cooling Air Flow {dimensionless}",
+			"    0.700000,                !- Latent Effectiveness at 75% Cooling Air Flow {dimensionless}",
+			"    DOAS Mixed Air Outlet,   !- Supply Air Inlet Node Name",
+			"    DOAS Heat Recovery Supply Outlet,  !- Supply Air Outlet Node Name",
+			"    DOAS Relief Air Outlet,  !- Exhaust Air Inlet Node Name",
+			"    DOAS Heat Recovery Relief Outlet,  !- Exhaust Air Outlet Node Name",
+			"    0,                       !- Nominal Electric Power {W}",
+			"    Yes,                     !- Supply Air Outlet Temperature Control",
+			"    Plate,                   !- Heat Exchanger Type",
+			"    MinimumExhaustTemperature,  !- Frost Control Type",
+			"    1.7,                     !- Threshold Temperature {C}",
+			"    0.083,                   !- Initial Defrost Time Fraction {dimensionless}",
+			"    0.012,                   !- Rate of Defrost Time Fraction Increase {1/K}",
+			"    Yes;                     !- Economizer Lockout",
+
+			"Controller:WaterCoil,",
+			"    DOAS Cooling Coil Controller,  !- Name",
+			"    Temperature,             !- Control Variable",
+			"    Reverse,                 !- Action",
+			"    Flow,                    !- Actuator Variable",
+			"    DOAS Cooling Coil Outlet,!- Sensor Node Name",
+			"    DOAS Cooling Coil ChW Inlet,  !- Actuator Node Name",
+			"    autosize,                !- Controller Convergence Tolerance {deltaC}",
+			"    autosize,                !- Maximum Actuated Flow {m3/s}",
+			"    0;                       !- Minimum Actuated Flow {m3/s}",
+
+			"Controller:WaterCoil,",
+			"    DOAS Heating Coil Controller,  !- Name",
+			"    Temperature,             !- Control Variable",
+			"    Normal,                  !- Action",
+			"    Flow,                    !- Actuator Variable",
+			"    DOAS Heating Coil Outlet,!- Sensor Node Name",
+			"    DOAS Heating Coil HW Inlet,  !- Actuator Node Name",
+			"    autosize,                !- Controller Convergence Tolerance {deltaC}",
+			"    autosize,                !- Maximum Actuated Flow {m3/s}",
+			"    0;                       !- Minimum Actuated Flow {m3/s}",
+
+			"Controller:OutdoorAir,",
+			"    DOAS OA Controller,      !- Name",
+			"    DOAS Relief Air Outlet,  !- Relief Air Outlet Node Name",
+			"    DOAS Air Loop Inlet,     !- Return Air Node Name",
+			"    DOAS Mixed Air Outlet,   !- Mixed Air Node Name",
+			"    DOAS Outdoor Air Inlet,  !- Actuator Node Name",
+			"    autosize,                !- Minimum Outdoor Air Flow Rate {m3/s}",
+			"    autosize,                !- Maximum Outdoor Air Flow Rate {m3/s}",
+			"    DifferentialEnthalpy,    !- Economizer Control Type",
+			"    MinimumFlowWithBypass,   !- Economizer Control Action Type",
+			"    ,                        !- Economizer Maximum Limit Dry-Bulb Temperature {C}",
+			"    ,                        !- Economizer Maximum Limit Enthalpy {J/kg}",
+			"    ,                        !- Economizer Maximum Limit Dewpoint Temperature {C}",
+			"    ,                        !- Electronic Enthalpy Limit Curve Name",
+			"    12.2,                    !- Economizer Minimum Limit Dry-Bulb Temperature {C}",
+			"    NoLockout,               !- Lockout Type",
+			"    ProportionalMinimum;     !- Minimum Limit Type",
+
+			"AirLoopHVAC:ControllerList,",
+			"    DOAS Controllers,        !- Name",
+			"    Controller:WaterCoil,    !- Controller 1 Object Type",
+			"    DOAS Cooling Coil Controller,  !- Controller 1 Name",
+			"    Controller:WaterCoil,    !- Controller 2 Object Type",
+			"    DOAS Heating Coil Controller;  !- Controller 2 Name",
+
+			"AirLoopHVAC:ControllerList,",
+			"    DOAS OA System Controllers,  !- Name",
+			"    Controller:OutdoorAir,   !- Controller 1 Object Type",
+			"    DOAS OA Controller;      !- Controller 1 Name",
+
+			"AirLoopHVAC,",
+			"    DOAS,                    !- Name",
+			"    DOAS Controllers,        !- Controller List Name",
+			"    DOAS Availability Managers,  !- Availability Manager List Name",
+			"    autosize,                !- Design Supply Air Flow Rate {m3/s}",
+			"    DOAS Branches,           !- Branch List Name",
+			"    ,                        !- Connector List Name",
+			"    DOAS Air Loop Inlet,     !- Supply Side Inlet Node Name",
+			"    DOAS Return Air Outlet,  !- Demand Side Outlet Node Name",
+			"    DOAS Supply Path Inlet,  !- Demand Side Inlet Node Names",
+			"    DOAS Supply Fan Outlet;  !- Supply Side Outlet Node Names",
+
+			"AirLoopHVAC:OutdoorAirSystem:EquipmentList,",
+			"    DOAS OA System Equipment,!- Name",
+			"    OutdoorAir:Mixer,        !- Component 2 Object Type",
+			"    DOAS OA Mixing Box;      !- Component 2 Name",
+
+			"AirLoopHVAC:OutdoorAirSystem,",
+			"    DOAS OA System,          !- Name",
+			"    DOAS OA System Controllers,  !- Controller List Name",
+			"    DOAS OA System Equipment,!- Outdoor Air Equipment List Name",
+			"    DOAS Availability Managers;  !- Availability Manager List Name",
+
+			"OutdoorAir:Mixer,",
+			"    SPACE1-1 OA Mixing Box,  !- Name",
+			"    SPACE1-1 Mixed Air Outlet,  !- Mixed Air Node Name",
+			"    SPACE1-1 Outside Air Inlet,  !- Outdoor Air Stream Node Name",
+			"    SPACE1-1 Relief Air Outlet,  !- Relief Air Stream Node Name",
+			"    SPACE1-1 Fan Coil Return;!- Return Air Stream Node Name",
+
+			"OutdoorAir:Mixer,",
+			"    SPACE2-1 OA Mixing Box,  !- Name",
+			"    SPACE2-1 Mixed Air Outlet,  !- Mixed Air Node Name",
+			"    SPACE2-1 Outside Air Inlet,  !- Outdoor Air Stream Node Name",
+			"    SPACE2-1 Relief Air Outlet,  !- Relief Air Stream Node Name",
+			"    SPACE2-1 Fan Coil Return;!- Return Air Stream Node Name",
+
+			"OutdoorAir:Mixer,",
+			"    SPACE3-1 OA Mixing Box,  !- Name",
+			"    SPACE3-1 Mixed Air Outlet,  !- Mixed Air Node Name",
+			"    SPACE3-1 Outside Air Inlet,  !- Outdoor Air Stream Node Name",
+			"    SPACE3-1 Relief Air Outlet,  !- Relief Air Stream Node Name",
+			"    SPACE3-1 Fan Coil Return;!- Return Air Stream Node Name",
+
+			"OutdoorAir:Mixer,",
+			"    SPACE4-1 OA Mixing Box,  !- Name",
+			"    SPACE4-1 Mixed Air Outlet,  !- Mixed Air Node Name",
+			"    SPACE4-1 Outside Air Inlet,  !- Outdoor Air Stream Node Name",
+			"    SPACE4-1 Relief Air Outlet,  !- Relief Air Stream Node Name",
+			"    SPACE4-1 Fan Coil Return;!- Return Air Stream Node Name",
+
+			"OutdoorAir:Mixer,",
+			"    SPACE5-1 OA Mixing Box,  !- Name",
+			"    SPACE5-1 Mixed Air Outlet,  !- Mixed Air Node Name",
+			"    SPACE5-1 Outside Air Inlet,  !- Outdoor Air Stream Node Name",
+			"    SPACE5-1 Relief Air Outlet,  !- Relief Air Stream Node Name",
+			"    SPACE5-1 Fan Coil Return;!- Return Air Stream Node Name",
+
+			"OutdoorAir:Mixer,",
+			"    DOAS OA Mixing Box,      !- Name",
+			"    DOAS Mixed Air Outlet,   !- Mixed Air Node Name",
+			"    DOAS Outdoor Air Inlet,  !- Outdoor Air Stream Node Name",
+			"    DOAS Relief Air Outlet,  !- Relief Air Stream Node Name",
+			"    DOAS Air Loop Inlet;     !- Return Air Stream Node Name",
+
+			"AirLoopHVAC:ZoneSplitter,",
+			"    DOAS Zone Splitter,      !- Name",
+			"    DOAS Supply Path Inlet,  !- Inlet Node Name",
+			"    SPACE1-1 Zone Equip Inlet,  !- Outlet 1 Node Name",
+			"    SPACE2-1 Zone Equip Inlet,  !- Outlet 2 Node Name",
+			"    SPACE3-1 Zone Equip Inlet,  !- Outlet 3 Node Name",
+			"    SPACE4-1 Zone Equip Inlet,  !- Outlet 4 Node Name",
+			"    SPACE5-1 Zone Equip Inlet;  !- Outlet 5 Node Name",
+
+			"AirLoopHVAC:SupplyPath,",
+			"    DOAS Supply Path,        !- Name",
+			"    DOAS Supply Path Inlet,  !- Supply Air Path Inlet Node Name",
+			"    AirLoopHVAC:ZoneSplitter,!- Component 1 Object Type",
+			"    DOAS Zone Splitter;      !- Component 1 Name",
+
+			"AirLoopHVAC:ZoneMixer,",
+			"    DOAS Zone Mixer,         !- Name",
+			"    DOAS Return Air Outlet,  !- Outlet Node Name",
+			"    SPACE1-1 Return Outlet,  !- Inlet 1 Node Name",
+			"    SPACE2-1 Return Outlet,  !- Inlet 2 Node Name",
+			"    SPACE3-1 Return Outlet,  !- Inlet 3 Node Name",
+			"    SPACE4-1 Return Outlet,  !- Inlet 4 Node Name",
+			"    SPACE5-1 Return Outlet;  !- Inlet 5 Node Name",
+
+			"AirLoopHVAC:ReturnPath,",
+			"    DOAS Return Path,        !- Name",
+			"    DOAS Return Air Outlet,  !- Return Air Path Outlet Node Name",
+			"    AirLoopHVAC:ZoneMixer,   !- Component 1 Object Type",
+			"    DOAS Zone Mixer;         !- Component 1 Name",
+
+			"Branch,",
+			"    SPACE1-1 Cooling Coil ChW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Cooling:Water,      !- Component 1 Object Type",
+			"    SPACE1-1 Cooling Coil,   !- Component 1 Name",
+			"    SPACE1-1 Cooling Coil ChW Inlet,  !- Component 1 Inlet Node Name",
+			"    SPACE1-1 Cooling Coil ChW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    SPACE1-1 Heating Coil HW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Heating:Water,      !- Component 1 Object Type",
+			"    SPACE1-1 Heating Coil,   !- Component 1 Name",
+			"    SPACE1-1 Heating Coil HW Inlet,  !- Component 1 Inlet Node Name",
+			"    SPACE1-1 Heating Coil HW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    SPACE2-1 Cooling Coil ChW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Cooling:Water,      !- Component 1 Object Type",
+			"    SPACE2-1 Cooling Coil,   !- Component 1 Name",
+			"    SPACE2-1 Cooling Coil ChW Inlet,  !- Component 1 Inlet Node Name",
+			"    SPACE2-1 Cooling Coil ChW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    SPACE2-1 Heating Coil HW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Heating:Water,      !- Component 1 Object Type",
+			"    SPACE2-1 Heating Coil,   !- Component 1 Name",
+			"    SPACE2-1 Heating Coil HW Inlet,  !- Component 1 Inlet Node Name",
+			"    SPACE2-1 Heating Coil HW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    SPACE3-1 Cooling Coil ChW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Cooling:Water,      !- Component 1 Object Type",
+			"    SPACE3-1 Cooling Coil,   !- Component 1 Name",
+			"    SPACE3-1 Cooling Coil ChW Inlet,  !- Component 1 Inlet Node Name",
+			"    SPACE3-1 Cooling Coil ChW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    SPACE3-1 Heating Coil HW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Heating:Water,      !- Component 1 Object Type",
+			"    SPACE3-1 Heating Coil,   !- Component 1 Name",
+			"    SPACE3-1 Heating Coil HW Inlet,  !- Component 1 Inlet Node Name",
+			"    SPACE3-1 Heating Coil HW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    SPACE4-1 Cooling Coil ChW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Cooling:Water,      !- Component 1 Object Type",
+			"    SPACE4-1 Cooling Coil,   !- Component 1 Name",
+			"    SPACE4-1 Cooling Coil ChW Inlet,  !- Component 1 Inlet Node Name",
+			"    SPACE4-1 Cooling Coil ChW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    SPACE4-1 Heating Coil HW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Heating:Water,      !- Component 1 Object Type",
+			"    SPACE4-1 Heating Coil,   !- Component 1 Name",
+			"    SPACE4-1 Heating Coil HW Inlet,  !- Component 1 Inlet Node Name",
+			"    SPACE4-1 Heating Coil HW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    SPACE5-1 Cooling Coil ChW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Cooling:Water,      !- Component 1 Object Type",
+			"    SPACE5-1 Cooling Coil,   !- Component 1 Name",
+			"    SPACE5-1 Cooling Coil ChW Inlet,  !- Component 1 Inlet Node Name",
+			"    SPACE5-1 Cooling Coil ChW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    SPACE5-1 Heating Coil HW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Heating:Water,      !- Component 1 Object Type",
+			"    SPACE5-1 Heating Coil,   !- Component 1 Name",
+			"    SPACE5-1 Heating Coil HW Inlet,  !- Component 1 Inlet Node Name",
+			"    SPACE5-1 Heating Coil HW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    DOAS Main Branch,        !- Name",
+			"    autosize,                !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    AirLoopHVAC:OutdoorAirSystem,  !- Component 1 Object Type",
+			"    DOAS OA System,          !- Component 1 Name",
+			"    DOAS Air Loop Inlet,     !- Component 1 Inlet Node Name",
+			"    DOAS Mixed Air Outlet,   !- Component 1 Outlet Node Name",
+			"    Passive,                 !- Component 1 Branch Control Type",
+			"    HeatExchanger:AirToAir:SensibleAndLatent,  !- Component 1 Object Type",
+			"    DOAS Heat Recovery,      !- Component 2 Name",
+			"    DOAS Mixed Air Outlet,   !- Component 2 Inlet Node Name",
+			"    DOAS Heat Recovery Supply Outlet,  !- Component 2 Outlet Node Name",
+			"    Passive,                 !- Component 2 Branch Control Type",
+			"    Coil:Cooling:Water,      !- Component 3 Object Type",
+			"    DOAS Cooling Coil,       !- Component 3 Name",
+			"    DOAS Heat Recovery Supply Outlet,   !- Component 3 Inlet Node Name",
+			"    DOAS Cooling Coil Outlet,!- Component 3 Outlet Node Name",
+			"    Passive,                 !- Component 3 Branch Control Type",
+			"    Coil:Heating:Water,      !- Component 4 Object Type",
+			"    DOAS Heating Coil,       !- Component 4 Name",
+			"    DOAS Cooling Coil Outlet,!- Component 4 Inlet Node Name",
+			"    DOAS Heating Coil Outlet,!- Component 4 Outlet Node Name",
+			"    Passive,                 !- Component 4 Branch Control Type",
+			"    Fan:VariableVolume,      !- Component 5 Object Type",
+			"    DOAS Supply Fan,         !- Component 5 Name",
+			"    DOAS Heating Coil Outlet,!- Component 5 Inlet Node Name",
+			"    DOAS Supply Fan Outlet,  !- Component 5 Outlet Node Name",
+			"    Active;                  !- Component 5 Branch Control Type",
+
+			"Branch,",
+			"    DOAS Cooling Coil ChW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Cooling:Water,      !- Component 1 Object Type",
+			"    DOAS Cooling Coil,       !- Component 1 Name",
+			"    DOAS Cooling Coil ChW Inlet,  !- Component 1 Inlet Node Name",
+			"    DOAS Cooling Coil ChW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    DOAS Heating Coil HW Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Coil:Heating:Water,      !- Component 1 Object Type",
+			"    DOAS Heating Coil,       !- Component 1 Name",
+			"    DOAS Heating Coil HW Inlet,  !- Component 1 Inlet Node Name",
+			"    DOAS Heating Coil HW Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Main Boiler HW Branch,   !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    DistrictHeating,         !- Component 1 Object Type",
+			"    Purchased Heating,         !- Component 1 Name",
+			"    Purchased Heat Inlet Node, !- Component 1 Inlet Node Name",
+			"    Purchased Heat Outlet Node,   !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Main Chiller ChW Branch, !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    DistrictCooling,         !- Component 1 Object Type",
+			"    Purchased Cooling,            !- Component 1 Name",
+			"    Purchased Cooling Inlet Node,  !- Component 1 Inlet Node Name",
+			"    Purchased Cooling Outlet Node, !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Hot Water Loop HW Supply Bypass Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pipe:Adiabatic,          !- Component 1 Object Type",
+			"    Hot Water Loop HW Supply Side Bypass Pipe,  !- Component 1 Name",
+			"    Hot Water Loop HW Supply Bypass Inlet,  !- Component 1 Inlet Node Name",
+			"    Hot Water Loop HW Supply Bypass Outlet,  !- Component 1 Outlet Node Name",
+			"    Bypass;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Hot Water Loop HW Supply Inlet Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pump:ConstantSpeed,      !- Component 1 Object Type",
+			"    Hot Water Loop HW Supply Pump,  !- Component 1 Name",
+			"    Hot Water Loop HW Supply Inlet,  !- Component 1 Inlet Node Name",
+			"    Hot Water Loop HW Pump Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Hot Water Loop HW Supply Outlet Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pipe:Adiabatic,          !- Component 1 Object Type",
+			"    Hot Water Loop HW Supply Outlet Pipe,  !- Component 1 Name",
+			"    Hot Water Loop HW Supply Outlet Pipe Inlet,  !- Component 1 Inlet Node Name",
+			"    Hot Water Loop HW Supply Outlet,  !- Component 1 Outlet Node Name",
+			"    Passive;                 !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Hot Water Loop HW Demand Inlet Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pipe:Adiabatic,          !- Component 1 Object Type",
+			"    Hot Water Loop HW Demand Inlet Pipe,  !- Component 1 Name",
+			"    Hot Water Loop HW Demand Inlet,  !- Component 1 Inlet Node Name",
+			"    Hot Water Loop HW Demand Inlet Pipe Outlet,  !- Component 1 Outlet Node Name",
+			"    Passive;                 !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Hot Water Loop HW Demand Bypass Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pipe:Adiabatic,          !- Component 1 Object Type",
+			"    Hot Water Loop HW Demand Side Bypass Pipe,  !- Component 1 Name",
+			"    Hot Water Loop HW Demand Bypass Inlet,  !- Component 1 Inlet Node Name",
+			"    Hot Water Loop HW Demand Bypass Outlet,  !- Component 1 Outlet Node Name",
+			"    Bypass;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Hot Water Loop HW Demand Outlet Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pipe:Adiabatic,          !- Component 1 Object Type",
+			"    Hot Water Loop HW Demand Outlet Pipe,  !- Component 1 Name",
+			"    Hot Water Loop HW Demand Outlet Pipe Inlet,  !- Component 1 Inlet Node Name",
+			"    Hot Water Loop HW Demand Outlet,  !- Component 1 Outlet Node Name",
+			"    Passive;                 !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Chilled Water Loop ChW Supply Bypass Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pipe:Adiabatic,          !- Component 1 Object Type",
+			"    Chilled Water Loop ChW Supply Side Bypass Pipe,  !- Component 1 Name",
+			"    Chilled Water Loop ChW Supply Bypass Inlet,  !- Component 1 Inlet Node Name",
+			"    Chilled Water Loop ChW Supply Bypass Outlet,  !- Component 1 Outlet Node Name",
+			"    Bypass;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Chilled Water Loop ChW Supply Inlet Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pump:ConstantSpeed,      !- Component 1 Object Type",
+			"    Chilled Water Loop ChW Supply Pump,  !- Component 1 Name",
+			"    Chilled Water Loop ChW Supply Inlet,  !- Component 1 Inlet Node Name",
+			"    Chilled Water Loop ChW Pump Outlet,  !- Component 1 Outlet Node Name",
+			"    Active;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Chilled Water Loop ChW Supply Outlet Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pipe:Adiabatic,          !- Component 1 Object Type",
+			"    Chilled Water Loop ChW Supply Outlet Pipe,  !- Component 1 Name",
+			"    Chilled Water Loop ChW Supply Outlet Pipe Inlet,  !- Component 1 Inlet Node Name",
+			"    Chilled Water Loop ChW Supply Outlet,  !- Component 1 Outlet Node Name",
+			"    Passive;                 !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Chilled Water Loop ChW Demand Inlet Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pipe:Adiabatic,          !- Component 1 Object Type",
+			"    Chilled Water Loop ChW Demand Inlet Pipe,  !- Component 1 Name",
+			"    Chilled Water Loop ChW Demand Inlet,  !- Component 1 Inlet Node Name",
+			"    Chilled Water Loop ChW Demand Inlet Pipe Outlet,  !- Component 1 Outlet Node Name",
+			"    Passive;                 !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Chilled Water Loop ChW Demand Bypass Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pipe:Adiabatic,          !- Component 1 Object Type",
+			"    Chilled Water Loop ChW Demand Side Bypass Pipe,  !- Component 1 Name",
+			"    Chilled Water Loop ChW Demand Bypass Inlet,  !- Component 1 Inlet Node Name",
+			"    Chilled Water Loop ChW Demand Bypass Outlet,  !- Component 1 Outlet Node Name",
+			"    Bypass;                  !- Component 1 Branch Control Type",
+
+			"Branch,",
+			"    Chilled Water Loop ChW Demand Outlet Branch,  !- Name",
+			"    ,                        !- Maximum Flow Rate {m3/s}",
+			"    ,                        !- Pressure Drop Curve Name",
+			"    Pipe:Adiabatic,          !- Component 1 Object Type",
+			"    Chilled Water Loop ChW Demand Outlet Pipe,  !- Component 1 Name",
+			"    Chilled Water Loop ChW Demand Outlet Pipe Inlet,  !- Component 1 Inlet Node Name",
+			"    Chilled Water Loop ChW Demand Outlet,  !- Component 1 Outlet Node Name",
+			"    Passive;                 !- Component 1 Branch Control Type",
+
+			"BranchList,",
+			"    DOAS Branches,           !- Name",
+			"    DOAS Main Branch;        !- Branch 1 Name",
+
+			"BranchList,",
+			"    Hot Water Loop HW Supply Side Branches,  !- Name",
+			"    Hot Water Loop HW Supply Inlet Branch,  !- Branch 1 Name",
+			"    Main Boiler HW Branch,   !- Branch 2 Name",
+			"    Hot Water Loop HW Supply Bypass Branch,  !- Branch 3 Name",
+			"    Hot Water Loop HW Supply Outlet Branch;  !- Branch 4 Name",
+
+			"BranchList,",
+			"    Hot Water Loop HW Demand Side Branches,  !- Name",
+			"    Hot Water Loop HW Demand Inlet Branch,  !- Branch 1 Name",
+			"    SPACE1-1 Heating Coil HW Branch,  !- Branch 2 Name",
+			"    SPACE2-1 Heating Coil HW Branch,  !- Branch 3 Name",
+			"    SPACE3-1 Heating Coil HW Branch,  !- Branch 4 Name",
+			"    SPACE4-1 Heating Coil HW Branch,  !- Branch 5 Name",
+			"    SPACE5-1 Heating Coil HW Branch,  !- Branch 6 Name",
+			"    DOAS Heating Coil HW Branch,  !- Branch 7 Name",
+			"    Hot Water Loop HW Demand Bypass Branch,  !- Branch 8 Name",
+			"    Hot Water Loop HW Demand Outlet Branch;  !- Branch 9 Name",
+
+			"BranchList,",
+			"    Chilled Water Loop ChW Supply Side Branches,  !- Name",
+			"    Chilled Water Loop ChW Supply Inlet Branch,  !- Branch 1 Name",
+			"    Main Chiller ChW Branch, !- Branch 2 Name",
+			"    Chilled Water Loop ChW Supply Bypass Branch,  !- Branch 3 Name",
+			"    Chilled Water Loop ChW Supply Outlet Branch;  !- Branch 4 Name",
+
+			"BranchList,",
+			"    Chilled Water Loop ChW Demand Side Branches,  !- Name",
+			"    Chilled Water Loop ChW Demand Inlet Branch,  !- Branch 1 Name",
+			"    SPACE1-1 Cooling Coil ChW Branch,  !- Branch 2 Name",
+			"    SPACE2-1 Cooling Coil ChW Branch,  !- Branch 3 Name",
+			"    SPACE3-1 Cooling Coil ChW Branch,  !- Branch 4 Name",
+			"    SPACE4-1 Cooling Coil ChW Branch,  !- Branch 5 Name",
+			"    SPACE5-1 Cooling Coil ChW Branch,  !- Branch 6 Name",
+			"    DOAS Cooling Coil ChW Branch,  !- Branch 7 Name",
+			"    Chilled Water Loop ChW Demand Bypass Branch,  !- Branch 8 Name",
+			"    Chilled Water Loop ChW Demand Outlet Branch;  !- Branch 9 Name",
+
+			"Connector:Splitter,",
+			"    Hot Water Loop HW Supply Splitter,  !- Name",
+			"    Hot Water Loop HW Supply Inlet Branch,  !- Inlet Branch Name",
+			"    Main Boiler HW Branch,   !- Outlet Branch 1 Name",
+			"    Hot Water Loop HW Supply Bypass Branch;  !- Outlet Branch 2 Name",
+
+			"Connector:Splitter,",
+			"    Hot Water Loop HW Demand Splitter,  !- Name",
+			"    Hot Water Loop HW Demand Inlet Branch,  !- Inlet Branch Name",
+			"    Hot Water Loop HW Demand Bypass Branch,  !- Outlet Branch 1 Name",
+			"    SPACE1-1 Heating Coil HW Branch,  !- Outlet Branch 2 Name",
+			"    SPACE2-1 Heating Coil HW Branch,  !- Outlet Branch 3 Name",
+			"    SPACE3-1 Heating Coil HW Branch,  !- Outlet Branch 4 Name",
+			"    SPACE4-1 Heating Coil HW Branch,  !- Outlet Branch 5 Name",
+			"    SPACE5-1 Heating Coil HW Branch,  !- Outlet Branch 6 Name",
+			"    DOAS Heating Coil HW Branch;  !- Outlet Branch 7 Name",
+
+			"Connector:Splitter,",
+			"    Chilled Water Loop ChW Supply Splitter,  !- Name",
+			"    Chilled Water Loop ChW Supply Inlet Branch,  !- Inlet Branch Name",
+			"    Chilled Water Loop ChW Supply Bypass Branch,  !- Outlet Branch 1 Name",
+			"    Main Chiller ChW Branch; !- Outlet Branch 2 Name",
+
+			"Connector:Splitter,",
+			"    Chilled Water Loop ChW Demand Splitter,  !- Name",
+			"    Chilled Water Loop ChW Demand Inlet Branch,  !- Inlet Branch Name",
+			"    Chilled Water Loop ChW Demand Bypass Branch,  !- Outlet Branch 1 Name",
+			"    SPACE1-1 Cooling Coil ChW Branch,  !- Outlet Branch 2 Name",
+			"    SPACE2-1 Cooling Coil ChW Branch,  !- Outlet Branch 3 Name",
+			"    SPACE3-1 Cooling Coil ChW Branch,  !- Outlet Branch 4 Name",
+			"    SPACE4-1 Cooling Coil ChW Branch,  !- Outlet Branch 5 Name",
+			"    SPACE5-1 Cooling Coil ChW Branch,  !- Outlet Branch 6 Name",
+			"    DOAS Cooling Coil ChW Branch;  !- Outlet Branch 7 Name",
+
+			"Connector:Mixer,",
+			"    Hot Water Loop HW Supply Mixer,  !- Name",
+			"    Hot Water Loop HW Supply Outlet Branch,  !- Outlet Branch Name",
+			"    Main Boiler HW Branch,   !- Inlet Branch 1 Name",
+			"    Hot Water Loop HW Supply Bypass Branch;  !- Inlet Branch 2 Name",
+
+			"Connector:Mixer,",
+			"    Hot Water Loop HW Demand Mixer,  !- Name",
+			"    Hot Water Loop HW Demand Outlet Branch,  !- Outlet Branch Name",
+			"    Hot Water Loop HW Demand Bypass Branch,  !- Inlet Branch 1 Name",
+			"    SPACE1-1 Heating Coil HW Branch,  !- Inlet Branch 2 Name",
+			"    SPACE2-1 Heating Coil HW Branch,  !- Inlet Branch 3 Name",
+			"    SPACE3-1 Heating Coil HW Branch,  !- Inlet Branch 4 Name",
+			"    SPACE4-1 Heating Coil HW Branch,  !- Inlet Branch 5 Name",
+			"    SPACE5-1 Heating Coil HW Branch,  !- Inlet Branch 6 Name",
+			"    DOAS Heating Coil HW Branch;  !- Inlet Branch 7 Name",
+
+			"Connector:Mixer,",
+			"    Chilled Water Loop ChW Supply Mixer,  !- Name",
+			"    Chilled Water Loop ChW Supply Outlet Branch,  !- Outlet Branch Name",
+			"    Chilled Water Loop ChW Supply Bypass Branch,  !- Inlet Branch 1 Name",
+			"    Main Chiller ChW Branch; !- Inlet Branch 2 Name",
+
+			"Connector:Mixer,",
+			"    Chilled Water Loop ChW Demand Mixer,  !- Name",
+			"    Chilled Water Loop ChW Demand Outlet Branch,  !- Outlet Branch Name",
+			"    Chilled Water Loop ChW Demand Bypass Branch,  !- Inlet Branch 1 Name",
+			"    SPACE1-1 Cooling Coil ChW Branch,  !- Inlet Branch 2 Name",
+			"    SPACE2-1 Cooling Coil ChW Branch,  !- Inlet Branch 3 Name",
+			"    SPACE3-1 Cooling Coil ChW Branch,  !- Inlet Branch 4 Name",
+			"    SPACE4-1 Cooling Coil ChW Branch,  !- Inlet Branch 5 Name",
+			"    SPACE5-1 Cooling Coil ChW Branch,  !- Inlet Branch 6 Name",
+			"    DOAS Cooling Coil ChW Branch;  !- Inlet Branch 7 Name",
+
+			"ConnectorList,",
+			"    Hot Water Loop HW Supply Side Connectors,  !- Name",
+			"    Connector:Splitter,      !- Connector 1 Object Type",
+			"    Hot Water Loop HW Supply Splitter,  !- Connector 1 Name",
+			"    Connector:Mixer,         !- Connector 2 Object Type",
+			"    Hot Water Loop HW Supply Mixer;  !- Connector 2 Name",
+
+			"ConnectorList,",
+			"    Hot Water Loop HW Demand Side Connectors,  !- Name",
+			"    Connector:Splitter,      !- Connector 1 Object Type",
+			"    Hot Water Loop HW Demand Splitter,  !- Connector 1 Name",
+			"    Connector:Mixer,         !- Connector 2 Object Type",
+			"    Hot Water Loop HW Demand Mixer;  !- Connector 2 Name",
+
+			"ConnectorList,",
+			"    Chilled Water Loop ChW Supply Side Connectors,  !- Name",
+			"    Connector:Splitter,      !- Connector 1 Object Type",
+			"    Chilled Water Loop ChW Supply Splitter,  !- Connector 1 Name",
+			"    Connector:Mixer,         !- Connector 2 Object Type",
+			"    Chilled Water Loop ChW Supply Mixer;  !- Connector 2 Name",
+
+			"ConnectorList,",
+			"    Chilled Water Loop ChW Demand Side Connectors,  !- Name",
+			"    Connector:Splitter,      !- Connector 1 Object Type",
+			"    Chilled Water Loop ChW Demand Splitter,  !- Connector 1 Name",
+			"    Connector:Mixer,         !- Connector 2 Object Type",
+			"    Chilled Water Loop ChW Demand Mixer;  !- Connector 2 Name",
+
+			"NodeList,",
+			"    SPACE1-1 Inlets,         !- Name",
+			"    SPACE1-1 Supply Inlet,   !- Node 1 Name",
+			"    SPACE1-1 DOAS Supply Inlet;  !- Node 2 Name",
+
+			"NodeList,",
+			"    SPACE2-1 Inlets,         !- Name",
+			"    SPACE2-1 Supply Inlet,   !- Node 1 Name",
+			"    SPACE2-1 DOAS Supply Inlet;  !- Node 2 Name",
+
+			"NodeList,",
+			"    SPACE3-1 Inlets,         !- Name",
+			"    SPACE3-1 Supply Inlet,   !- Node 1 Name",
+			"    SPACE3-1 DOAS Supply Inlet;  !- Node 2 Name",
+
+			"NodeList,",
+			"    SPACE4-1 Inlets,         !- Name",
+			"    SPACE4-1 Supply Inlet,   !- Node 1 Name",
+			"    SPACE4-1 DOAS Supply Inlet;  !- Node 2 Name",
+
+			"NodeList,",
+			"    SPACE5-1 Inlets,         !- Name",
+			"    SPACE5-1 Supply Inlet,   !- Node 1 Name",
+			"    SPACE5-1 DOAS Supply Inlet;  !- Node 2 Name",
+
+			"NodeList,",
+			"    DOAS Cooling Setpoint Nodes,  !- Name",
+			"    DOAS Cooling Coil Outlet;!- Node 1 Name",
+
+			"NodeList,",
+			"    Hot Water Loop HW Supply Setpoint Nodes,  !- Name",
+			"    Purchased Heat Outlet Node,   !- Node 1 Name",
+			"    Hot Water Loop HW Supply Outlet;  !- Node 2 Name",
+
+			"NodeList,",
+			"    Chilled Water Loop ChW Supply Setpoint Nodes,  !- Name",
+			"    Purchased Cooling Outlet Node, !- Node 1 Name",
+			"    Chilled Water Loop ChW Supply Outlet;  !- Node 2 Name",
+
+			"OutdoorAir:NodeList,",
+			"    SPACE1-1 Outside Air Inlet;  !- Node or NodeList Name 1",
+
+			"OutdoorAir:NodeList,",
+			"    SPACE2-1 Outside Air Inlet;  !- Node or NodeList Name 1",
+
+			"OutdoorAir:NodeList,",
+			"    SPACE3-1 Outside Air Inlet;  !- Node or NodeList Name 1",
+
+			"OutdoorAir:NodeList,",
+			"    SPACE4-1 Outside Air Inlet;  !- Node or NodeList Name 1",
+
+			"OutdoorAir:NodeList,",
+			"    SPACE5-1 Outside Air Inlet;  !- Node or NodeList Name 1",
+
+			"OutdoorAir:NodeList,",
+			"    DOAS Outdoor Air Inlet;  !- Node or NodeList Name 1",
+
+			"Pipe:Adiabatic,",
+			"    Hot Water Loop HW Supply Side Bypass Pipe,  !- Name",
+			"    Hot Water Loop HW Supply Bypass Inlet,  !- Inlet Node Name",
+			"    Hot Water Loop HW Supply Bypass Outlet;  !- Outlet Node Name",
+
+			"Pipe:Adiabatic,",
+			"    Hot Water Loop HW Supply Outlet Pipe,  !- Name",
+			"    Hot Water Loop HW Supply Outlet Pipe Inlet,  !- Inlet Node Name",
+			"    Hot Water Loop HW Supply Outlet;  !- Outlet Node Name",
+
+			"Pipe:Adiabatic,",
+			"    Hot Water Loop HW Demand Inlet Pipe,  !- Name",
+			"    Hot Water Loop HW Demand Inlet,  !- Inlet Node Name",
+			"    Hot Water Loop HW Demand Inlet Pipe Outlet;  !- Outlet Node Name",
+
+			"Pipe:Adiabatic,",
+			"    Hot Water Loop HW Demand Side Bypass Pipe,  !- Name",
+			"    Hot Water Loop HW Demand Bypass Inlet,  !- Inlet Node Name",
+			"    Hot Water Loop HW Demand Bypass Outlet;  !- Outlet Node Name",
+
+			"Pipe:Adiabatic,",
+			"    Hot Water Loop HW Demand Outlet Pipe,  !- Name",
+			"    Hot Water Loop HW Demand Outlet Pipe Inlet,  !- Inlet Node Name",
+			"    Hot Water Loop HW Demand Outlet;  !- Outlet Node Name",
+
+			"Pipe:Adiabatic,",
+			"    Chilled Water Loop ChW Supply Side Bypass Pipe,  !- Name",
+			"    Chilled Water Loop ChW Supply Bypass Inlet,  !- Inlet Node Name",
+			"    Chilled Water Loop ChW Supply Bypass Outlet;  !- Outlet Node Name",
+
+			"Pipe:Adiabatic,",
+			"    Chilled Water Loop ChW Supply Outlet Pipe,  !- Name",
+			"    Chilled Water Loop ChW Supply Outlet Pipe Inlet,  !- Inlet Node Name",
+			"    Chilled Water Loop ChW Supply Outlet;  !- Outlet Node Name",
+
+			"Pipe:Adiabatic,",
+			"    Chilled Water Loop ChW Demand Inlet Pipe,  !- Name",
+			"    Chilled Water Loop ChW Demand Inlet,  !- Inlet Node Name",
+			"    Chilled Water Loop ChW Demand Inlet Pipe Outlet;  !- Outlet Node Name",
+
+			"Pipe:Adiabatic,",
+			"    Chilled Water Loop ChW Demand Side Bypass Pipe,  !- Name",
+			"    Chilled Water Loop ChW Demand Bypass Inlet,  !- Inlet Node Name",
+			"    Chilled Water Loop ChW Demand Bypass Outlet;  !- Outlet Node Name",
+
+			"Pipe:Adiabatic,",
+			"    Chilled Water Loop ChW Demand Outlet Pipe,  !- Name",
+			"    Chilled Water Loop ChW Demand Outlet Pipe Inlet,  !- Inlet Node Name",
+			"    Chilled Water Loop ChW Demand Outlet;  !- Outlet Node Name",
+
+			"Pump:ConstantSpeed,",
+			"    Hot Water Loop HW Supply Pump,  !- Name",
+			"    Hot Water Loop HW Supply Inlet,  !- Inlet Node Name",
+			"    Hot Water Loop HW Pump Outlet,  !- Outlet Node Name",
+			"    autosize,                !- Rated Flow Rate {m3/s}",
+			"    179352,                  !- Rated Pump Head {Pa}",
+			"    autosize,                !- Rated Power Consumption {W}",
+			"    0.9,                     !- Motor Efficiency",
+			"    0,                       !- Fraction of Motor Inefficiencies to Fluid Stream",
+			"    INTERMITTENT;            !- Pump Control Type",
+
+			"Pump:ConstantSpeed,",
+			"    Chilled Water Loop ChW Supply Pump,  !- Name",
+			"    Chilled Water Loop ChW Supply Inlet,  !- Inlet Node Name",
+			"    Chilled Water Loop ChW Pump Outlet,  !- Outlet Node Name",
+			"    autosize,                !- Rated Flow Rate {m3/s}",
+			"    179352,                  !- Rated Pump Head {Pa}",
+			"    autosize,                !- Rated Power Consumption {W}",
+			"    0.9,                     !- Motor Efficiency",
+			"    0,                       !- Fraction of Motor Inefficiencies to Fluid Stream",
+			"    INTERMITTENT;            !- Pump Control Type",
+
+			"  DistrictHeating,",
+			"    Purchased Heating,          !- Name",
+			"    Purchased Heat Inlet Node,  !- Hot Water Inlet Node Name",
+			"    Purchased Heat Outlet Node, !- Hot Water Outlet Node Name",
+			"    35000;                      !- Nominal Capacity {W}",
+
+			"  DistrictCooling,",
+			"    Purchased Cooling,       !- Name",
+			"    Purchased Cooling Inlet Node,  !- Chilled Water Inlet Node Name",
+			"    Purchased Cooling Outlet Node,  !- Chilled Water Outlet Node Name",
+			"    35000;                   !- Nominal Capacity {W}",
+
+			"PlantLoop,",
+			"    Hot Water Loop Hot Water Loop,  !- Name",
+			"    Water,                   !- Fluid Type",
+			"    ,                        !- User Defined Fluid Type",
+			"    Hot Water Loop Operation,!- Plant Equipment Operation Scheme Name",
+			"    Hot Water Loop HW Supply Outlet,  !- Loop Temperature Setpoint Node Name",
+			"    100,                     !- Maximum Loop Temperature {C}",
+			"    10,                      !- Minimum Loop Temperature {C}",
+			"    autosize,                !- Maximum Loop Flow Rate {m3/s}",
+			"    0,                       !- Minimum Loop Flow Rate {m3/s}",
+			"    autosize,                !- Plant Loop Volume {m3}",
+			"    Hot Water Loop HW Supply Inlet,  !- Plant Side Inlet Node Name",
+			"    Hot Water Loop HW Supply Outlet,  !- Plant Side Outlet Node Name",
+			"    Hot Water Loop HW Supply Side Branches,  !- Plant Side Branch List Name",
+			"    Hot Water Loop HW Supply Side Connectors,  !- Plant Side Connector List Name",
+			"    Hot Water Loop HW Demand Inlet,  !- Demand Side Inlet Node Name",
+			"    Hot Water Loop HW Demand Outlet,  !- Demand Side Outlet Node Name",
+			"    Hot Water Loop HW Demand Side Branches,  !- Demand Side Branch List Name",
+			"    Hot Water Loop HW Demand Side Connectors,  !- Demand Side Connector List Name",
+			"    SequentialLoad,          !- Load Distribution Scheme",
+			"    ,                        !- Availability Manager List Name",
+			"    SingleSetpoint;          !- Plant Loop Demand Calculation Scheme",
+
+			"PlantLoop,",
+			"    Chilled Water Loop Chilled Water Loop,  !- Name",
+			"    Water,                   !- Fluid Type",
+			"    ,                        !- User Defined Fluid Type",
+			"    Chilled Water Loop Chiller Operation,  !- Plant Equipment Operation Scheme Name",
+			"    Chilled Water Loop ChW Supply Outlet,  !- Loop Temperature Setpoint Node Name",
+			"    98,                      !- Maximum Loop Temperature {C}",
+			"    1,                       !- Minimum Loop Temperature {C}",
+			"    autosize,                !- Maximum Loop Flow Rate {m3/s}",
+			"    0,                       !- Minimum Loop Flow Rate {m3/s}",
+			"    autosize,                !- Plant Loop Volume {m3}",
+			"    Chilled Water Loop ChW Supply Inlet,  !- Plant Side Inlet Node Name",
+			"    Chilled Water Loop ChW Supply Outlet,  !- Plant Side Outlet Node Name",
+			"    Chilled Water Loop ChW Supply Side Branches,  !- Plant Side Branch List Name",
+			"    Chilled Water Loop ChW Supply Side Connectors,  !- Plant Side Connector List Name",
+			"    Chilled Water Loop ChW Demand Inlet,  !- Demand Side Inlet Node Name",
+			"    Chilled Water Loop ChW Demand Outlet,  !- Demand Side Outlet Node Name",
+			"    Chilled Water Loop ChW Demand Side Branches,  !- Demand Side Branch List Name",
+			"    Chilled Water Loop ChW Demand Side Connectors,  !- Demand Side Connector List Name",
+			"    SequentialLoad,          !- Load Distribution Scheme",
+			"    ,                        !- Availability Manager List Name",
+			"    SingleSetpoint,          !- Plant Loop Demand Calculation Scheme",
+			"    None;                    !- Common Pipe Simulation",
+
+			"PlantEquipmentList,",
+			"    Hot Water Loop All Equipment,           !- Name",
+			"    DistrictHeating,          !- Equipment 1 Object Type",
+			"    Purchased Heating;        !- Equipment 1 Name",
+
+			"PlantEquipmentList,",
+			"    Chilled Water Loop All Chillers,  !- Name",
+			"    DistrictCooling,    !- Equipment 1 Object Type",
+			"    Purchased Cooling;            !- Equipment 1 Name",
+
+			"PlantEquipmentOperation:CoolingLoad,",
+			"    Chilled Water Loop Chiller Operation All Hours,  !- Name",
+			"    0,                       !- Load Range 1 Lower Limit {W}",
+			"    1000000000000000,        !- Load Range 1 Upper Limit {W}",
+			"    Chilled Water Loop All Chillers;  !- Range 1 Equipment List Name",
+
+			"PlantEquipmentOperation:HeatingLoad,",
+			"    Hot Water Loop Operation All Hours,  !- Name",
+			"    0,                       !- Load Range 1 Lower Limit {W}",
+			"    1000000000000000,        !- Load Range 1 Upper Limit {W}",
+			"    Hot Water Loop All Equipment;  !- Range 1 Equipment List Name",
+
+			"PlantEquipmentOperationSchemes,",
+			"    Hot Water Loop Operation,!- Name",
+			"    PlantEquipmentOperation:HeatingLoad,  !- Control Scheme 1 Object Type",
+			"    Hot Water Loop Operation All Hours,  !- Control Scheme 1 Name",
+			"    HVACTemplate-Always 1;   !- Control Scheme 1 Schedule Name",
+
+			"PlantEquipmentOperationSchemes,",
+			"    Chilled Water Loop Chiller Operation,  !- Name",
+			"    PlantEquipmentOperation:CoolingLoad,  !- Control Scheme 1 Object Type",
+			"    Chilled Water Loop Chiller Operation All Hours,  !- Control Scheme 1 Name",
+			"    HVACTemplate-Always 1;   !- Control Scheme 1 Schedule Name",
+
+			"AvailabilityManager:Scheduled,",
+			"    DOAS Availability,       !- Name",
+			"    FanAvailSched;                !- Schedule Name",
+
+			"AvailabilityManagerAssignmentList,",
+			"    DOAS Availability Managers,  !- Name",
+			"    AvailabilityManager:Scheduled,  !- Availability Manager 1 Object Type",
+			"    DOAS Availability;       !- Availability Manager 1 Name",
+
+			"SetpointManager:Scheduled,",
+			"    DOAS Heating Supply Air Temp Manager,",
+			"    Temperature,",
+			"    HVACTemplate-Always 12.2,",
+			"    DOAS Supply Path Inlet;",
+
+			"SetpointManager:OutdoorAirReset,",
+			"    DOAS Cooling Supply Air Temp Manager, !- Name",
+			"    Temperature,  !- Control Variable",
+			"    18.3,                    !- Setpoint at Outdoor Low Temperature {C}",
+			"    4.4,                    !- Outdoor Low Temperature (C)",
+			"    12.8,                    !- Setpoint at Outdoor High Temperature (C)",
+			"    26.7,                    !- Outdoor High Temperature (C)",
+			"    DOAS Supply Fan Outlet;  !- Setpoint Node or NodeList Name",
+
+			"SetpointManager:OutdoorAirReset,",
+			"    Hot Water Loop HW Temp Manager,  !- Name",
+			"    Temperature,             !- Control Variable",
+			"    82.2,                    !- Setpoint at Outdoor Low Temperature {C}",
+			"    -6.7,                    !- Outdoor Low Temperature {C}",
+			"    65.6,                    !- Setpoint at Outdoor High Temperature {C}",
+			"    10,                      !- Outdoor High Temperature {C}",
+			"    Hot Water Loop HW Supply Setpoint Nodes;  !- Setpoint Node or NodeList Name",
+
+			"SetpointManager:OutdoorAirReset,",
+			"    Chilled Water Loop ChW Temp Manager,  !- Name",
+			"    Temperature,             !- Control Variable",
+			"    12.2,                    !- Setpoint at Outdoor Low Temperature {C}",
+			"    15.6,                    !- Outdoor Low Temperature {C}",
+			"    6.7,                     !- Setpoint at Outdoor High Temperature {C}",
+			"    26.7,                    !- Outdoor High Temperature {C}",
+			"    Chilled Water Loop ChW Supply Setpoint Nodes;  !- Setpoint Node or NodeList Name",
+
+			"SetpointManager:MixedAir,",
+			"    DOAS Cooling Coil Air Temp Manager,  !- Name",
+			"    Temperature,             !- Control Variable",
+			"    DOAS Supply Fan Outlet,  !- Reference Setpoint Node Name",
+			"    DOAS Heating Coil Outlet,!- Fan Inlet Node Name",
+			"    DOAS Supply Fan Outlet,  !- Fan Outlet Node Name",
+			"    DOAS Cooling Setpoint Nodes;  !- Setpoint Node or NodeList Name",
+
+			"SetpointManager:MixedAir,",
+			"    DOAS Heating Coil Air Temp Manager,  !- Name",
+			"    Temperature,             !- Control Variable",
+			"    DOAS Supply Path Inlet,  !- Reference Setpoint Node Name",
+			"    DOAS Heating Coil Outlet,!- Fan Inlet Node Name",
+			"    DOAS Supply Fan Outlet,  !- Fan Outlet Node Name",
+			"    DOAS Heating Coil Outlet;!- Setpoint Node or NodeList Name",
+
+			"SetpointManager:MixedAir,",
+			"    DOAS Heat Recovery Air Temp Manager,  !- Name",
+			"    Temperature,             !- Control Variable",
+			"    DOAS Supply Path Inlet,  !- Reference Setpoint Node Name",
+			"    DOAS Heating Coil Outlet,!- Fan Inlet Node Name",
+			"    DOAS Supply Fan Outlet,  !- Fan Outlet Node Name",
+			"    DOAS Heat Recovery Supply Outlet;  !- Setpoint Node or NodeList Name",
+
+			"SetpointManager:MixedAir,",
+			"    DOAS Heat Recovery Economizer Temp Manager,  !- Name",
+			"    Temperature,             !- Control Variable",
+			"    DOAS Supply Fan Outlet,  !- Reference Setpoint Node Name",
+			"    DOAS Heating Coil Outlet,!- Fan Inlet Node Name",
+			"    DOAS Supply Fan Outlet,  !- Fan Outlet Node Name",
+			"    DOAS Mixed Air Outlet;   !- Setpoint Node or NodeList Name",
+
+		} );
+
+
+			ASSERT_FALSE( process_idf( idf_objects ) );
+			GetOAControllerInputs();
+
+			EXPECT_EQ( 6, GetNumOAMixers() );
+			EXPECT_EQ( 1, GetNumOAControllers() );
+			EXPECT_EQ( 18, GetOAMixerReliefNodeNumber( 1 ) );
+			EXPECT_EQ( 1, GetOAMixerIndex( "SPACE1-1 OA Mixing Box" ) );
+			EXPECT_EQ( 2, GetOAMixerIndex( "SPACE2-1 OA Mixing Box" ) );
+			EXPECT_EQ( 3, GetOAMixerIndex( "SPACE3-1 OA Mixing Box" ) );
+			EXPECT_EQ( 4, GetOAMixerIndex( "SPACE4-1 OA Mixing Box" ) );
+			EXPECT_EQ( 5, GetOAMixerIndex( "SPACE5-1 OA Mixing Box" ) );
+			EXPECT_EQ( 6, GetOAMixerIndex( "DOAS OA Mixing Box" ) );
+
+	}
+
 }
diff --git a/tst/EnergyPlus/unit/NodeInputManager.unit.cc b/tst/EnergyPlus/unit/NodeInputManager.unit.cc
index 392514e744f..c7c9eefe7ba 100644
--- a/tst/EnergyPlus/unit/NodeInputManager.unit.cc
+++ b/tst/EnergyPlus/unit/NodeInputManager.unit.cc
@@ -115,7 +115,8 @@ namespace EnergyPlus {
 
 		EMSManager::FinishProcessingUserInput = true;
 
-		EMSManager::ManageEMS( DataGlobals::emsCallFromSetupSimulation );
+		bool anyEMSRan;
+		EMSManager::ManageEMS( DataGlobals::emsCallFromSetupSimulation,anyEMSRan );
 
 		DataLoopNode::Node( 1 ).Temp = 20.0;
 		DataLoopNode::Node( 1 ).HumRat = 0.01;
diff --git a/tst/EnergyPlus/unit/OutputReportTabular.unit.cc b/tst/EnergyPlus/unit/OutputReportTabular.unit.cc
index 5fe245fa239..67bcf8fb0e1 100644
--- a/tst/EnergyPlus/unit/OutputReportTabular.unit.cc
+++ b/tst/EnergyPlus/unit/OutputReportTabular.unit.cc
@@ -91,6 +91,7 @@ using namespace EnergyPlus::DataSizing;
 using namespace EnergyPlus::DataSurfaces;
 using namespace EnergyPlus::HeatBalanceManager;
 using namespace EnergyPlus::OutputProcessor;
+using namespace EnergyPlus::OutputReportPredefined;
 using namespace EnergyPlus::OutputReportTabular;
 using namespace EnergyPlus::OutputProcessor;
 using namespace SimulationManager;
@@ -1256,7 +1257,7 @@ TEST_F( EnergyPlusFixture, OutputReportTabular_ZoneMultiplierTest )
 	ASSERT_FALSE( process_idf( idf_objects ) );
 
 	OutputProcessor::TimeValue.allocate( 2 );
- 
+
 	ManageSimulation(); // run the design day over the warmup period (24 hrs, 25 days)
 
 	EXPECT_EQ( 10.0, ( Zone( 2 ).Volume * Zone( 2 ).Multiplier * Zone( 2 ).ListMultiplier ) / ( Zone( 1 ).Volume * Zone( 1 ).Multiplier * Zone( 1 ).ListMultiplier ) );
@@ -1333,6 +1334,7 @@ TEST_F( EnergyPlusFixture, AirloopHVAC_ZoneSumTest )
 	// DATE WRITTEN: Sep 2015
 
 	std::string const idf_objects = delimited_string( {
+
 		" Version,8.3;",
 		" Output:Diagnostics, DisplayExtraWarnings;",
 		" Timestep, 4;",
@@ -2294,7 +2296,7 @@ TEST_F( EnergyPlusFixture, AirloopHVAC_ZoneSumTest )
 
 	OutputProcessor::TimeValue.allocate( 2 );
 	DataGlobals::DDOnlySimulation = true;
- 
+
 	ManageSimulation(); // run the design day over the warmup period (24 hrs, 25 days)
 
 	EXPECT_EQ( 10.0, ( Zone( 2 ).Volume * Zone( 2 ).Multiplier * Zone( 2 ).ListMultiplier ) / ( Zone( 1 ).Volume * Zone( 1 ).Multiplier * Zone( 1 ).ListMultiplier ) );
@@ -3274,7 +3276,7 @@ TEST_F( EnergyPlusFixture, AirloopHVAC_VentilationRateProcedure )
 
 	OutputProcessor::TimeValue.allocate( 2 );
 	DataGlobals::DDOnlySimulation = true;
- 
+
 	ManageSimulation(); // run the design day over the warmup period (24 hrs, 25 days)
 
 	EXPECT_EQ( 10.0, ( Zone( 2 ).Volume * Zone( 2 ).Multiplier * Zone( 2 ).ListMultiplier ) / ( Zone( 1 ).Volume * Zone( 1 ).Multiplier * Zone( 1 ).ListMultiplier ) );
@@ -3421,3 +3423,2240 @@ TEST_F( EnergyPlusFixture, OutputTableTimeBins_GetInput )
 	EXPECT_EQ( OutputTableBinned( 1 ).intervalCount, 5 );
 	EXPECT_EQ( OutputTableBinned( 1 ).ScheduleName, "ALWAYS1" );
 }
+
+
+TEST_F( EnergyPlusFixture, FinAndOverhangCount )
+{
+	// based on 4ZoneWithShading_Simple_2.idf
+	std::string const idf_objects = delimited_string( {
+
+		"  Version,8.5;                                                                                     ",
+		"                                                                                                   ",
+		" Output:Diagnostics, DisplayExtraWarnings;",
+		"  Timestep,4;                                                                                      ",
+		"                                                                                                   ",
+		"  Building,                                                                                        ",
+		"    BUILDING #1,             !- Name                                                               ",
+		"    0.0000000E+00,           !- North Axis {deg}                                                   ",
+		"    Suburbs,                 !- Terrain                                                            ",
+		"    3.9999999E-02,           !- Loads Convergence Tolerance Value                                  ",
+		"    0.4000000,               !- Temperature Convergence Tolerance Value {deltaC}                   ",
+		"    FullExterior,            !- Solar Distribution                                                 ",
+		"    25,                      !- Maximum Number of Warmup Days                                      ",
+		"    6;                       !- Minimum Number of Warmup Days                                      ",
+		"                                                                                                   ",
+		"  SurfaceConvectionAlgorithm:Inside,Simple;                                                        ",
+		"                                                                                                   ",
+		"  SurfaceConvectionAlgorithm:Outside,SimpleCombined;                                               ",
+		"                                                                                                   ",
+		"  HeatBalanceAlgorithm,ConductionTransferFunction;                                                 ",
+		"                                                                                                   ",
+		"  SimulationControl,                                                                               ",
+		"    No,                     !- Do Zone Sizing Calculation                                         ",
+		"    No,                      !- Do System Sizing Calculation                                       ",
+		"    No,                      !- Do Plant Sizing Calculation                                        ",
+		"    Yes,                     !- Run Simulation for Sizing Periods                                  ",
+		"    No;                      !- Run Simulation for Weather File Run Periods                        ",
+		"                                                                                                   ",
+		"  Site:Location,                                                                                   ",
+		"    Chicago Ohare Intl Ap IL USA WMO=725300,  !- Name                                              ",
+		"    41.99,                   !- Latitude {deg}                                                     ",
+		"    -87.91,                  !- Longitude {deg}                                                    ",
+		"    -6.00,                   !- Time Zone {hr}                                                     ",
+		"    205.00;                  !- Elevation {m}                                                      ",
+		"                                                                                                   ",
+		"  SizingPeriod:DesignDay,                                                                          ",
+		"    Chicago Ohare Intl Ap Ann Htg 99% Condns DB,  !- Name                                          ",
+		"    1,                       !- Month                                                              ",
+		"    21,                      !- Day of Month                                                       ",
+		"    WinterDesignDay,         !- Day Type                                                           ",
+		"    -16.6,                   !- Maximum Dry-Bulb Temperature {C}                                   ",
+		"    0.0,                     !- Daily Dry-Bulb Temperature Range {deltaC}                          ",
+		"    ,                        !- Dry-Bulb Temperature Range Modifier Type                           ",
+		"    ,                        !- Dry-Bulb Temperature Range Modifier Day Schedule Name              ",
+		"    Wetbulb,                 !- Humidity Condition Type                                            ",
+		"    -16.6,                   !- Wetbulb or DewPoint at Maximum Dry-Bulb {C}                        ",
+		"    ,                        !- Humidity Condition Day Schedule Name                               ",
+		"    ,                        !- Humidity Ratio at Maximum Dry-Bulb {kgWater/kgDryAir}              ",
+		"    ,                        !- Enthalpy at Maximum Dry-Bulb {J/kg}                                ",
+		"    ,                        !- Daily Wet-Bulb Temperature Range {deltaC}                          ",
+		"    98886.,                  !- Barometric Pressure {Pa}                                           ",
+		"    4.9,                     !- Wind Speed {m/s}                                                   ",
+		"    270,                     !- Wind Direction {deg}                                               ",
+		"    No,                      !- Rain Indicator                                                     ",
+		"    No,                      !- Snow Indicator                                                     ",
+		"    No,                      !- Daylight Saving Time Indicator                                     ",
+		"    ASHRAEClearSky,          !- Solar Model Indicator                                              ",
+		"    ,                        !- Beam Solar Day Schedule Name                                       ",
+		"    ,                        !- Diffuse Solar Day Schedule Name                                    ",
+		"    ,                        !- ASHRAE Clear Sky Optical Depth for Beam Irradiance (taub) {dimensio",
+		"    ,                        !- ASHRAE Clear Sky Optical Depth for Diffuse Irradiance (taud) {dimen",
+		"    0.00;                    !- Sky Clearness                                                      ",
+		"                                                                                                   ",
+		"  SizingPeriod:DesignDay,                                                                          ",
+		"    Chicago Ohare Intl Ap Ann Clg 1% Condns DB=>MWB,  !- Name                                      ",
+		"    7,                       !- Month                                                              ",
+		"    21,                      !- Day of Month                                                       ",
+		"    SummerDesignDay,         !- Day Type                                                           ",
+		"    31.6,                    !- Maximum Dry-Bulb Temperature {C}                                   ",
+		"    10.5,                    !- Daily Dry-Bulb Temperature Range {deltaC}                          ",
+		"    ,                        !- Dry-Bulb Temperature Range Modifier Type                           ",
+		"    ,                        !- Dry-Bulb Temperature Range Modifier Day Schedule Name              ",
+		"    Wetbulb,                 !- Humidity Condition Type                                            ",
+		"    23,                      !- Wetbulb or DewPoint at Maximum Dry-Bulb {C}                        ",
+		"    ,                        !- Humidity Condition Day Schedule Name                               ",
+		"    ,                        !- Humidity Ratio at Maximum Dry-Bulb {kgWater/kgDryAir}              ",
+		"    ,                        !- Enthalpy at Maximum Dry-Bulb {J/kg}                                ",
+		"    ,                        !- Daily Wet-Bulb Temperature Range {deltaC}                          ",
+		"    98886.,                  !- Barometric Pressure {Pa}                                           ",
+		"    5.2,                     !- Wind Speed {m/s}                                                   ",
+		"    230,                     !- Wind Direction {deg}                                               ",
+		"    No,                      !- Rain Indicator                                                     ",
+		"    No,                      !- Snow Indicator                                                     ",
+		"    No,                      !- Daylight Saving Time Indicator                                     ",
+		"    ASHRAEClearSky,          !- Solar Model Indicator                                              ",
+		"    ,                        !- Beam Solar Day Schedule Name                                       ",
+		"    ,                        !- Diffuse Solar Day Schedule Name                                    ",
+		"    ,                        !- ASHRAE Clear Sky Optical Depth for Beam Irradiance (taub) {dimensio",
+		"    ,                        !- ASHRAE Clear Sky Optical Depth for Diffuse Irradiance (taud) {dimen",
+		"    1.00;                    !- Sky Clearness                                                      ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    A2 - 4 IN DENSE FACE BRICK,  !- Name                                                           ",
+		"    Rough,                   !- Roughness                                                          ",
+		"    0.1014984,               !- Thickness {m}                                                      ",
+		"    1.245296,                !- Conductivity {W/m-K}                                               ",
+		"    2082.400,                !- Density {kg/m3}                                                    ",
+		"    920.4800,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.9300000,               !- Solar Absorptance                                                  ",
+		"    0.9300000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    B3 - 2 IN INSULATION,    !- Name                                                               ",
+		"    VeryRough,               !- Roughness                                                          ",
+		"    5.0901599E-02,           !- Thickness {m}                                                      ",
+		"    4.3239430E-02,           !- Conductivity {W/m-K}                                               ",
+		"    32.03693,                !- Density {kg/m3}                                                    ",
+		"    836.8000,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.5000000,               !- Solar Absorptance                                                  ",
+		"    0.5000000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    C2 - 4 IN LW CONCRETE BLOCK,  !- Name                                                          ",
+		"    MediumRough,             !- Roughness                                                          ",
+		"    0.1014984,               !- Thickness {m}                                                      ",
+		"    0.3805070,               !- Conductivity {W/m-K}                                               ",
+		"    608.7016,                !- Density {kg/m3}                                                    ",
+		"    836.8000,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.6500000,               !- Solar Absorptance                                                  ",
+		"    0.6500000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Name                                                   ",
+		"    Smooth,                  !- Roughness                                                          ",
+		"    1.9050000E-02,           !- Thickness {m}                                                      ",
+		"    0.7264224,               !- Conductivity {W/m-K}                                               ",
+		"    1601.846,                !- Density {kg/m3}                                                    ",
+		"    836.8000,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.9200000,               !- Solar Absorptance                                                  ",
+		"    0.9200000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"   ! (R=.0472,TRANS=.80,VERY SMOOTH,GLASS), from 6mm clear                                         ",
+		"                                                                                                   ",
+		"  WindowMaterial:Glazing,                                                                          ",
+		"    GLASS - CLEAR PLATE 1 / 4 IN,  !- Name                                                         ",
+		"    SpectralAverage,         !- Optical Data Type                                                  ",
+		"    ,                        !- Window Glass Spectral Data Set Name                                ",
+		"    6.0000001E-03,           !- Thickness {m}                                                      ",
+		"    0.7750000,               !- Solar Transmittance at Normal Incidence                            ",
+		"    7.1000002E-02,           !- Front Side Solar Reflectance at Normal Incidence                   ",
+		"    7.1000002E-02,           !- Back Side Solar Reflectance at Normal Incidence                    ",
+		"    0.8810000,               !- Visible Transmittance at Normal Incidence                          ",
+		"    7.9999998E-02,           !- Front Side Visible Reflectance at Normal Incidence                 ",
+		"    7.9999998E-02,           !- Back Side Visible Reflectance at Normal Incidence                  ",
+		"    0.0000000E+00,           !- Infrared Transmittance at Normal Incidence                         ",
+		"    0.8400000,               !- Front Side Infrared Hemispherical Emissivity                       ",
+		"    0.8400000,               !- Back Side Infrared Hemispherical Emissivity                        ",
+		"    0.9000000;               !- Conductivity {W/m-K}                                               ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    WOOD - HARDWOOD 1 / 8 IN,!- Name                                                               ",
+		"    MediumSmooth,            !- Roughness                                                          ",
+		"    3.1699201E-03,           !- Thickness {m}                                                      ",
+		"    0.1591211,               !- Conductivity {W/m-K}                                               ",
+		"    720.8308,                !- Density {kg/m3}                                                    ",
+		"    1255.200,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.7800000,               !- Solar Absorptance                                                  ",
+		"    0.7800000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material:AirGap,                                                                                 ",
+		"    B1 - AIRSPACE RESISTANCE,!- Name                                                               ",
+		"    0.1603675;               !- Thermal Resistance {m2-K/W}                                        ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    C7 - 8 IN LW CONCRETE BLOCK,  !- Name                                                          ",
+		"    Rough,                   !- Roughness                                                          ",
+		"    0.2033016,               !- Thickness {m}                                                      ",
+		"    0.5707605,               !- Conductivity {W/m-K}                                               ",
+		"    608.7016,                !- Density {kg/m3}                                                    ",
+		"    836.8000,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.6500000,               !- Solar Absorptance                                                  ",
+		"    0.6500000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    E5 - ACOUSTIC TILE,      !- Name                                                               ",
+		"    MediumSmooth,            !- Roughness                                                          ",
+		"    1.9050000E-02,           !- Thickness {m}                                                      ",
+		"    6.0535200E-02,           !- Conductivity {W/m-K}                                               ",
+		"    480.5539,                !- Density {kg/m3}                                                    ",
+		"    836.8000,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.3200000,               !- Solar Absorptance                                                  ",
+		"    0.3200000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material:AirGap,                                                                                 ",
+		"    E4 - CEILING AIRSPACE,   !- Name                                                               ",
+		"    0.1762280;               !- Thermal Resistance {m2-K/W}                                        ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    C5 - 4 IN HW CONCRETE,   !- Name                                                               ",
+		"    MediumRough,             !- Roughness                                                          ",
+		"    0.1014984,               !- Thickness {m}                                                      ",
+		"    1.729577,                !- Conductivity {W/m-K}                                               ",
+		"    2242.585,                !- Density {kg/m3}                                                    ",
+		"    836.8000,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.6500000,               !- Solar Absorptance                                                  ",
+		"    0.6500000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    C10 - 8 IN HW CONCRETE,  !- Name                                                               ",
+		"    MediumRough,             !- Roughness                                                          ",
+		"    0.2033016,               !- Thickness {m}                                                      ",
+		"    1.729577,                !- Conductivity {W/m-K}                                               ",
+		"    2242.585,                !- Density {kg/m3}                                                    ",
+		"    836.8000,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.6500000,               !- Solar Absorptance                                                  ",
+		"    0.6500000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    E2 - 1 / 2 IN SLAG OR STONE,  !- Name                                                          ",
+		"    Rough,                   !- Roughness                                                          ",
+		"    1.2710161E-02,           !- Thickness {m}                                                      ",
+		"    1.435549,                !- Conductivity {W/m-K}                                               ",
+		"    881.0155,                !- Density {kg/m3}                                                    ",
+		"    1673.600,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.5500000,               !- Solar Absorptance                                                  ",
+		"    0.5500000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    E3 - 3 / 8 IN FELT AND MEMBRANE,  !- Name                                                      ",
+		"    Rough,                   !- Roughness                                                          ",
+		"    9.5402403E-03,           !- Thickness {m}                                                      ",
+		"    0.1902535,               !- Conductivity {W/m-K}                                               ",
+		"    1121.292,                !- Density {kg/m3}                                                    ",
+		"    1673.600,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.7500000,               !- Solar Absorptance                                                  ",
+		"    0.7500000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    B6 - 2 IN DENSE INSULATION,  !- Name                                                           ",
+		"    VeryRough,               !- Roughness                                                          ",
+		"    5.0901599E-02,           !- Thickness {m}                                                      ",
+		"    4.3239430E-02,           !- Conductivity {W/m-K}                                               ",
+		"    91.30524,                !- Density {kg/m3}                                                    ",
+		"    836.8000,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.5000000,               !- Solar Absorptance                                                  ",
+		"    0.5000000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Material,                                                                                        ",
+		"    C12 - 2 IN HW CONCRETE,  !- Name                                                               ",
+		"    MediumRough,             !- Roughness                                                          ",
+		"    5.0901599E-02,           !- Thickness {m}                                                      ",
+		"    1.729577,                !- Conductivity {W/m-K}                                               ",
+		"    2242.585,                !- Density {kg/m3}                                                    ",
+		"    836.8000,                !- Specific Heat {J/kg-K}                                             ",
+		"    0.9000000,               !- Thermal Absorptance                                                ",
+		"    0.6500000,               !- Solar Absorptance                                                  ",
+		"    0.6500000;               !- Visible Absorptance                                                ",
+		"                                                                                                   ",
+		"  Construction,                                                                                    ",
+		"    EXTERIOR,                !- Name                                                               ",
+		"    A2 - 4 IN DENSE FACE BRICK,  !- Outside Layer                                                  ",
+		"    B3 - 2 IN INSULATION,    !- Layer 2                                                            ",
+		"    C2 - 4 IN LW CONCRETE BLOCK,  !- Layer 3                                                       ",
+		"    E1 - 3 / 4 IN PLASTER OR GYP BOARD;  !- Layer 4                                                ",
+		"                                                                                                   ",
+		"  Construction,                                                                                    ",
+		"    SINGLE PANE HW WINDOW,   !- Name                                                               ",
+		"    GLASS - CLEAR PLATE 1 / 4 IN;  !- Outside Layer                                                ",
+		"                                                                                                   ",
+		"  Construction,                                                                                    ",
+		"    HOLLOW WOOD DOOR,        !- Name                                                               ",
+		"    WOOD - HARDWOOD 1 / 8 IN,!- Outside Layer                                                      ",
+		"    B1 - AIRSPACE RESISTANCE,!- Layer 2                                                            ",
+		"    WOOD - HARDWOOD 1 / 8 IN;!- Layer 3                                                            ",
+		"                                                                                                   ",
+		"  Construction,                                                                                    ",
+		"    INTERIOR,                !- Name                                                               ",
+		"    C7 - 8 IN LW CONCRETE BLOCK;  !- Outside Layer                                                 ",
+		"                                                                                                   ",
+		"  Construction,                                                                                    ",
+		"    FLOOR,                   !- Name                                                               ",
+		"    E5 - ACOUSTIC TILE,      !- Outside Layer                                                      ",
+		"    E4 - CEILING AIRSPACE,   !- Layer 2                                                            ",
+		"    C5 - 4 IN HW CONCRETE;   !- Layer 3                                                            ",
+		"                                                                                                   ",
+		"  Construction,                                                                                    ",
+		"    CEILING34,               !- Name                                                               ",
+		"    C10 - 8 IN HW CONCRETE;  !- Outside Layer                                                      ",
+		"                                                                                                   ",
+		"  Construction,                                                                                    ",
+		"    FLOOR34,                 !- Name                                                               ",
+		"    C10 - 8 IN HW CONCRETE;  !- Outside Layer                                                      ",
+		"                                                                                                   ",
+		"  Construction,                                                                                    ",
+		"    ROOF31,                  !- Name                                                               ",
+		"    E2 - 1 / 2 IN SLAG OR STONE,  !- Outside Layer                                                 ",
+		"    E3 - 3 / 8 IN FELT AND MEMBRANE,  !- Layer 2                                                   ",
+		"    B6 - 2 IN DENSE INSULATION,  !- Layer 3                                                        ",
+		"    C12 - 2 IN HW CONCRETE;  !- Layer 4                                                            ",
+		"                                                                                                   ",
+		"  ScheduleTypeLimits,                                                                              ",
+		"    Any Number;              !- Name                                                               ",
+		"                                                                                                   ",
+		"  ScheduleTypeLimits,                                                                              ",
+		"    Fraction,                !- Name                                                               ",
+		"    0.0,                     !- Lower Limit Value                                                  ",
+		"    1.0,                     !- Upper Limit Value                                                  ",
+		"    CONTINUOUS;              !- Numeric Type                                                       ",
+		"                                                                                                   ",
+		"  Site:GroundTemperature:BuildingSurface,20,20,20,20,20,20,20,20,20,20,20,20;                      ",
+		"                                                                                                   ",
+		"  Zone,                                                                                            ",
+		"    ZONE 1,                  !- Name                                                               ",
+		"    0,                       !- Direction of Relative North {deg}                                  ",
+		"    0,                       !- X Origin {m}                                                       ",
+		"    0,                       !- Y Origin {m}                                                       ",
+		"    -10,                     !- Z Origin {m}                                                       ",
+		"    1,                       !- Type                                                               ",
+		"    1,                       !- Multiplier                                                         ",
+		"    AutoCalculate,           !- Ceiling Height {m}                                                 ",
+		"    AutoCalculate;           !- Volume {m3}                                                        ",
+		"                                                                                                   ",
+		"  Zone,                                                                                            ",
+		"    ZONE 2,                  !- Name                                                               ",
+		"    0,                       !- Direction of Relative North {deg}                                  ",
+		"    20,                      !- X Origin {m}                                                       ",
+		"    0,                       !- Y Origin {m}                                                       ",
+		"    -10,                     !- Z Origin {m}                                                       ",
+		"    1,                       !- Type                                                               ",
+		"    1,                       !- Multiplier                                                         ",
+		"    AutoCalculate,           !- Ceiling Height {m}                                                 ",
+		"    AutoCalculate;           !- Volume {m3}                                                        ",
+		"                                                                                                   ",
+		"  Zone,                                                                                            ",
+		"    ZONE 3,                  !- Name                                                               ",
+		"    0,                       !- Direction of Relative North {deg}                                  ",
+		"    0,                       !- X Origin {m}                                                       ",
+		"    0,                       !- Y Origin {m}                                                       ",
+		"    0,                       !- Z Origin {m}                                                       ",
+		"    1,                       !- Type                                                               ",
+		"    1,                       !- Multiplier                                                         ",
+		"    AutoCalculate,           !- Ceiling Height {m}                                                 ",
+		"    AutoCalculate;           !- Volume {m3}                                                        ",
+		"                                                                                                   ",
+		"  Zone,                                                                                            ",
+		"    ZONE 4,                  !- Name                                                               ",
+		"    0,                       !- Direction of Relative North {deg}                                  ",
+		"    20,                      !- X Origin {m}                                                       ",
+		"    0,                       !- Y Origin {m}                                                       ",
+		"    0,                       !- Z Origin {m}                                                       ",
+		"    1,                       !- Type                                                               ",
+		"    1,                       !- Multiplier                                                         ",
+		"    AutoCalculate,           !- Ceiling Height {m}                                                 ",
+		"    AutoCalculate;           !- Volume {m3}                                                        ",
+		"                                                                                                   ",
+		"  GlobalGeometryRules,                                                                             ",
+		"    UpperLeftCorner,         !- Starting Vertex Position                                           ",
+		"    CounterClockWise,        !- Vertex Entry Direction                                             ",
+		"    Relative,                !- Coordinate System                                                  ",
+		"    ,                        !- Daylighting Reference Point Coordinate System                      ",
+		"    Relative;                !- Rectangular Surface Coordinate System                              ",
+		"                                                                                                   ",
+		"  Shading:Building,                                                                                ",
+		"    Bushes-East,             !- Name                                                               ",
+		"    90,                      !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    45,                      !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    50,                      !- Length {m}                                                         ",
+		"    1;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Shading:Site,                                                                                    ",
+		"    Bushes-North,            !- Name                                                               ",
+		"    0,                       !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    45,                      !- Starting X Coordinate {m}                                          ",
+		"    50,                      !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    50,                      !- Length {m}                                                         ",
+		"    1;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Shading:Site,                                                                                    ",
+		"    Bushes-West,             !- Name                                                               ",
+		"    270,                     !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    -5,                      !- Starting X Coordinate {m}                                          ",
+		"    50,                      !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    50,                      !- Length {m}                                                         ",
+		"    1;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Exterior,                                                                                   ",
+		"    Zn001:Wall001,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 1,                  !- Zone Name                                                          ",
+		"    180,                     !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Window,                                                                                          ",
+		"    Zn001:Wall001:Win001,    !- Name                                                               ",
+		"    SINGLE PANE HW WINDOW,   !- Construction Name                                                  ",
+		"    Zn001:Wall001,           !- Building Surface Name                                              ",
+		"    ,                        !- Shading Control Name                                               ",
+		"    ,                        !- Frame and Divider Name                                             ",
+		"    1,                       !- Multiplier                                                         ",
+		"    4,                       !- Starting X Coordinate {m}                                          ",
+		"    3,                       !- Starting Z Coordinate {m}                                          ",
+		"    3,                       !- Length {m}                                                         ",
+		"    5;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  GlazedDoor,                                                                                      ",
+		"    Zn001:Wall001:Door001,   !- Name                                                               ",
+		"    SINGLE PANE HW WINDOW,   !- Construction Name                                                  ",
+		"    Zn001:Wall001,           !- Building Surface Name                                              ",
+		"    ,                        !- Shading Control Name                                               ",
+		"    ,                        !- Frame and Divider Name                                             ",
+		"    1,                       !- Multiplier                                                         ",
+		"    14,                      !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    3,                       !- Length {m}                                                         ",
+		"    5;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Shading:Overhang:Projection,                                                                     ",
+		"    Zn001:Wall001:Win001:Shade001,  !- Name                                                        ",
+		"    Zn001:Wall001:Win001,    !- Window or Door Name                                                ",
+		"    .7,                      !- Height above Window or Door {m}                                    ",
+		"    90,                      !- Tilt Angle from Window/Door {deg}                                  ",
+		"    .2,                      !- Left extension from Window/Door Width {m}                          ",
+		"    .2,                      !- Right extension from Window/Door Width {m}                         ",
+		"    .6;                      !- Depth as Fraction of Window/Door Height {dimensionless}            ",
+		"                                                                                                   ",
+		"  Shading:Overhang,                                                                                ",
+		"    Zn001:Wall001:Door001:Shade001,  !- Name                                                       ",
+		"    Zn001:Wall001:Door001,   !- Window or Door Name                                                ",
+		"    .6,                      !- Height above Window or Door {m}                                    ",
+		"    90,                      !- Tilt Angle from Window/Door {deg}                                  ",
+		"    0,                       !- Left extension from Window/Door Width {m}                          ",
+		"    0,                       !- Right extension from Window/Door Width {m}                         ",
+		"    3;                       !- Depth {m}                                                          ",
+		"                                                                                                   ",
+		"  Shading:Fin:Projection,                                                                          ",
+		"    Zn001:Wall001:Shade003,  !- Name                                                               ",
+		"    Zn001:Wall001:Win001,    !- Window or Door Name                                                ",
+		"    .1,                      !- Left Extension from Window/Door {m}                                ",
+		"    .1,                      !- Left Distance Above Top of Window {m}                              ",
+		"    .1,                      !- Left Distance Below Bottom of Window {m}                           ",
+		"    90,                      !- Left Tilt Angle from Window/Door {deg}                             ",
+		"    .6,                      !- Left Depth as Fraction of Window/Door Width {dimensionless}        ",
+		"    .1,                      !- Right Extension from Window/Door {m}                               ",
+		"    .1,                      !- Right Distance Above Top of Window {m}                             ",
+		"    .1,                      !- Right Distance Below Bottom of Window {m}                          ",
+		"    90,                      !- Right Tilt Angle from Window/Door {deg}                            ",
+		"    .6;                      !- Right Depth as Fraction of Window/Door Width {dimensionless}       ",
+		"                                                                                                   ",
+		"  Wall:Underground,                                                                                ",
+		"    Zn001:Wall002,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 1,                  !- Zone Name                                                          ",
+		"    0,                       !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    20,                      !- Starting X Coordinate {m}                                          ",
+		"    20,                      !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Underground,                                                                                ",
+		"    Zn001:Wall003,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 1,                  !- Zone Name                                                          ",
+		"    270,                     !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    20,                      !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Door,                                                                                            ",
+		"    Zn001:Wall001:Door002,   !- Name                                                               ",
+		"    HOLLOW WOOD DOOR,        !- Construction Name                                                  ",
+		"    Zn001:Wall003,           !- Building Surface Name                                              ",
+		"    1,                       !- Multiplier                                                         ",
+		"    14,                      !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    3,                       !- Length {m}                                                         ",
+		"    5;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Adiabatic,                                                                                  ",
+		"    Zn001:Wall004,           !- Name                                                               ",
+		"    INTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 1,                  !- Zone Name                                                          ",
+		"    90,                      !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    20,                      !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Floor:GroundContact,                                                                             ",
+		"    Zn001:Flr001,            !- Name                                                               ",
+		"    FLOOR,                   !- Construction Name                                                  ",
+		"    ZONE 1,                  !- Zone Name                                                          ",
+		"    90,                      !- Azimuth Angle {deg}                                                ",
+		"    180,                     !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    20;                      !- Width {m}                                                          ",
+		"                                                                                                   ",
+		"  Ceiling:Adiabatic,                                                                               ",
+		"    Zn001:Roof001,           !- Name                                                               ",
+		"    CEILING34,               !- Construction Name                                                  ",
+		"    ZONE 1,                  !- Zone Name                                                          ",
+		"    180,                     !- Azimuth Angle {deg}                                                ",
+		"    0,                       !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    10,                      !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    20;                      !- Width {m}                                                          ",
+		"                                                                                                   ",
+		"  Wall:Exterior,                                                                                   ",
+		"    Zn002:Wall001,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 2,                  !- Zone Name                                                          ",
+		"    180,                     !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Window,                                                                                          ",
+		"    Zn002:Wall001:Win001,    !- Name                                                               ",
+		"    SINGLE PANE HW WINDOW,   !- Construction Name                                                  ",
+		"    Zn002:Wall001,           !- Building Surface Name                                              ",
+		"    ,                        !- Shading Control Name                                               ",
+		"    ,                        !- Frame and Divider Name                                             ",
+		"    1,                       !- Multiplier                                                         ",
+		"    4,                       !- Starting X Coordinate {m}                                          ",
+		"    3,                       !- Starting Z Coordinate {m}                                          ",
+		"    3,                       !- Length {m}                                                         ",
+		"    5;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Shading:Overhang,                                                                                ",
+		"    Zn002:Wall001:Win001:Shade001,  !- Name                                                        ",
+		"    Zn002:Wall001:Win001,    !- Window or Door Name                                                ",
+		"    .7,                      !- Height above Window or Door {m}                                    ",
+		"    90,                      !- Tilt Angle from Window/Door {deg}                                  ",
+		"    0,                       !- Left extension from Window/Door Width {m}                          ",
+		"    0,                       !- Right extension from Window/Door Width {m}                         ",
+		"    3;                       !- Depth {m}                                                          ",
+		"                                                                                                   ",
+		"  Window,                                                                                          ",
+		"    Zn002:Wall001:Win002,    !- Name                                                               ",
+		"    SINGLE PANE HW WINDOW,   !- Construction Name                                                  ",
+		"    Zn002:Wall001,           !- Building Surface Name                                              ",
+		"    ,                        !- Shading Control Name                                               ",
+		"    ,                        !- Frame and Divider Name                                             ",
+		"    1,                       !- Multiplier                                                         ",
+		"    10,                      !- Starting X Coordinate {m}                                          ",
+		"    3,                       !- Starting Z Coordinate {m}                                          ",
+		"    3,                       !- Length {m}                                                         ",
+		"    5;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Underground,                                                                                ",
+		"    Zn002:Wall002,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 2,                  !- Zone Name                                                          ",
+		"    90,                      !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    20,                      !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Underground,                                                                                ",
+		"    Zn002:Wall003,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 2,                  !- Zone Name                                                          ",
+		"    0,                       !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    20,                      !- Starting X Coordinate {m}                                          ",
+		"    20,                      !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Adiabatic,                                                                                  ",
+		"    Zn002:Wall004,           !- Name                                                               ",
+		"    INTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 2,                  !- Zone Name                                                          ",
+		"    270,                     !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    20,                      !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Floor:GroundContact,                                                                             ",
+		"    Zn002:Flr001,            !- Name                                                               ",
+		"    FLOOR,                   !- Construction Name                                                  ",
+		"    ZONE 2,                  !- Zone Name                                                          ",
+		"    90,                      !- Azimuth Angle {deg}                                                ",
+		"    180,                     !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    20;                      !- Width {m}                                                          ",
+		"                                                                                                   ",
+		"  Ceiling:Adiabatic,                                                                               ",
+		"    Zn002:Roof001,           !- Name                                                               ",
+		"    CEILING34,               !- Construction Name                                                  ",
+		"    ZONE 2,                  !- Zone Name                                                          ",
+		"    180,                     !- Azimuth Angle {deg}                                                ",
+		"    0,                       !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    10,                      !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    20;                      !- Width {m}                                                          ",
+		"                                                                                                   ",
+		"  Wall:Exterior,                                                                                   ",
+		"    Zn003:Wall001,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 3,                  !- Zone Name                                                          ",
+		"    180,                     !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Window,                                                                                          ",
+		"    Zn003:Wall001:Win001,    !- Name                                                               ",
+		"    SINGLE PANE HW WINDOW,   !- Construction Name                                                  ",
+		"    Zn003:Wall001,           !- Building Surface Name                                              ",
+		"    ,                        !- Shading Control Name                                               ",
+		"    ,                        !- Frame and Divider Name                                             ",
+		"    1,                       !- Multiplier                                                         ",
+		"    8,                       !- Starting X Coordinate {m}                                          ",
+		"    3,                       !- Starting Z Coordinate {m}                                          ",
+		"    3,                       !- Length {m}                                                         ",
+		"    5;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Exterior,                                                                                   ",
+		"    Zn003:Wall002,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 3,                  !- Zone Name                                                          ",
+		"    0,                       !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    20,                      !- Starting X Coordinate {m}                                          ",
+		"    20,                      !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Exterior,                                                                                   ",
+		"    Zn003:Wall003,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 3,                  !- Zone Name                                                          ",
+		"    270,                     !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    20,                      !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Interzone,                                                                                  ",
+		"    Zn003:Wall004,           !- Name                                                               ",
+		"    INTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 3,                  !- Zone Name                                                          ",
+		"    ZONE 4,                  !- Outside Boundary Condition Object                                  ",
+		"    90,                      !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    20,                      !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  GlazedDoor:Interzone,                                                                            ",
+		"    Zn003:Wall004:Door002,   !- Name                                                               ",
+		"    SINGLE PANE HW WINDOW,   !- Construction Name                                                  ",
+		"    Zn003:Wall004,           !- Building Surface Name                                              ",
+		"    ZONE 4,                  !- Outside Boundary Condition Object                                  ",
+		"    1,                       !- Multiplier                                                         ",
+		"    10,                      !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    3,                       !- Length {m}                                                         ",
+		"    5;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Window:Interzone,                                                                                ",
+		"    Zn003:Wall004:Win001,    !- Name                                                               ",
+		"    SINGLE PANE HW WINDOW,   !- Construction Name                                                  ",
+		"    Zn003:Wall004,           !- Building Surface Name                                              ",
+		"    ZONE 4,                  !- Outside Boundary Condition Object                                  ",
+		"    1,                       !- Multiplier                                                         ",
+		"    4,                       !- Starting X Coordinate {m}                                          ",
+		"    3,                       !- Starting Z Coordinate {m}                                          ",
+		"    3,                       !- Length {m}                                                         ",
+		"    5;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Door:Interzone,                                                                                  ",
+		"    Zn003:Wall004:Door001,   !- Name                                                               ",
+		"    HOLLOW WOOD DOOR,        !- Construction Name                                                  ",
+		"    Zn003:Wall004,           !- Building Surface Name                                              ",
+		"    ZONE 4,                  !- Outside Boundary Condition Object                                  ",
+		"    1,                       !- Multiplier                                                         ",
+		"    10,                      !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    3,                       !- Length {m}                                                         ",
+		"    5;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Floor:Interzone,                                                                                 ",
+		"    Zn003:Flr001,            !- Name                                                               ",
+		"    FLOOR34,                 !- Construction Name                                                  ",
+		"    ZONE 3,                  !- Zone Name                                                          ",
+		"    Zn001:Roof001,           !- Outside Boundary Condition Object                                  ",
+		"    90,                      !- Azimuth Angle {deg}                                                ",
+		"    180,                     !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    20;                      !- Width {m}                                                          ",
+		"                                                                                                   ",
+		"  Roof,                                                                                            ",
+		"    Zn003:Roof001,           !- Name                                                               ",
+		"    ROOF31,                  !- Construction Name                                                  ",
+		"    ZONE 3,                  !- Zone Name                                                          ",
+		"    180,                     !- Azimuth Angle {deg}                                                ",
+		"    0,                       !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    10,                      !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    20;                      !- Width {m}                                                          ",
+		"                                                                                                   ",
+		"  Wall:Exterior,                                                                                   ",
+		"    Zn004:Wall001,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 4,                  !- Zone Name                                                          ",
+		"    180,                     !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Window,                                                                                          ",
+		"    Zn004:Wall001:Win001,    !- Name                                                               ",
+		"    SINGLE PANE HW WINDOW,   !- Construction Name                                                  ",
+		"    Zn004:Wall001,           !- Building Surface Name                                              ",
+		"    ,                        !- Shading Control Name                                               ",
+		"    ,                        !- Frame and Divider Name                                             ",
+		"    1,                       !- Multiplier                                                         ",
+		"    8,                       !- Starting X Coordinate {m}                                          ",
+		"    3,                       !- Starting Z Coordinate {m}                                          ",
+		"    3,                       !- Length {m}                                                         ",
+		"    5;                       !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Exterior,                                                                                   ",
+		"    Zn004:Wall002,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 4,                  !- Zone Name                                                          ",
+		"    90,                      !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    20,                      !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Wall:Exterior,                                                                                   ",
+		"    Zn004:Wall003,           !- Name                                                               ",
+		"    EXTERIOR,                !- Construction Name                                                  ",
+		"    ZONE 4,                  !- Zone Name                                                          ",
+		"    0,                       !- Azimuth Angle {deg}                                                ",
+		"    90,                      !- Tilt Angle {deg}                                                   ",
+		"    20,                      !- Starting X Coordinate {m}                                          ",
+		"    20,                      !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    10;                      !- Height {m}                                                         ",
+		"                                                                                                   ",
+		"  Floor:Interzone,                                                                                 ",
+		"    Zn004:Flr001,            !- Name                                                               ",
+		"    FLOOR34,                 !- Construction Name                                                  ",
+		"    ZONE 4,                  !- Zone Name                                                          ",
+		"    Zn002:Roof001,           !- Outside Boundary Condition Object                                  ",
+		"    90,                      !- Azimuth Angle {deg}                                                ",
+		"    180,                     !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    0,                       !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    20;                      !- Width {m}                                                          ",
+		"                                                                                                   ",
+		"  Roof,                                                                                            ",
+		"    Zn004:Roof001,           !- Name                                                               ",
+		"    ROOF31,                  !- Construction Name                                                  ",
+		"    ZONE 4,                  !- Zone Name                                                          ",
+		"    180,                     !- Azimuth Angle {deg}                                                ",
+		"    0,                       !- Tilt Angle {deg}                                                   ",
+		"    0,                       !- Starting X Coordinate {m}                                          ",
+		"    0,                       !- Starting Y Coordinate {m}                                          ",
+		"    10,                      !- Starting Z Coordinate {m}                                          ",
+		"    20,                      !- Length {m}                                                         ",
+		"    20;                      !- Width {m}                                                          ",
+		"                                                                                                   ",
+		"  ScheduleTypeLimits,                                                                              ",
+		"    Temperature,             !- Name                                                               ",
+		"    -100,                    !- Lower Limit Value                                                  ",
+		"    200,                     !- Upper Limit Value                                                  ",
+		"    CONTINUOUS;              !- Numeric Type                                                       ",
+		"                                                                                                   ",
+		"  ScheduleTypeLimits,                                                                              ",
+		"    ControlType,             !- Name                                                               ",
+		"    0,                       !- Lower Limit Value                                                  ",
+		"    4,                       !- Upper Limit Value                                                  ",
+		"    DISCRETE;                !- Numeric Type                                                       ",
+		"                                                                                                   ",
+		"  SCHEDULE:COMPACT,                                                                                ",
+		"    ZONE CONTROL TYPE SCHEDULE,  !- Name                                                           ",
+		"    CONTROLTYPE,             !- Schedule Type Limits Name                                          ",
+		"    Through: 12/31,          !- Field 1                                                            ",
+		"    For: AllDays,            !- Field 2                                                            ",
+		"    Until: 24:00,4;          !- Field 3                                                            ",
+		"                                                                                                   ",
+		"  SCHEDULE:COMPACT,                                                                                ",
+		"    ZONE HEATING SETPOINTS,  !- Name                                                               ",
+		"    TEMPERATURE,             !- Schedule Type Limits Name                                          ",
+		"    Through: 12/31,          !- Field 1                                                            ",
+		"    For: Weekdays WinterDesignDay, !- Field 2                                                      ",
+		"    Until: 7:00,15.60,       !- Field 3                                                            ",
+		"    Until: 17:00,19.40,      !- Field 5                                                            ",
+		"    Until: 24:00,15.60,      !- Field 7                                                            ",
+		"    For: AllOtherDays,       !- Field 9                                                            ",
+		"    Until: 24:00,15.60;      !- Field 10                                                           ",
+		"                                                                                                   ",
+		"  SCHEDULE:COMPACT,                                                                                ",
+		"    ZONE COOLING SETPOINTS,  !- Name                                                               ",
+		"    TEMPERATURE,             !- Schedule Type Limits Name                                          ",
+		"    Through: 12/31,          !- Field 1                                                            ",
+		"    For: Weekdays SummerDesignDay, !- Field 2                                                      ",
+		"    Until: 7:00,100.00,      !- Field 3                                                            ",
+		"    Until: 17:00,26.10,      !- Field 5                                                            ",
+		"    Until: 24:00,100.00,     !- Field 7                                                            ",
+		"    For: AllOtherDays,       !- Field 9                                                            ",
+		"    Until: 24:00,100.00;     !- Field 10                                                           ",
+		"                                                                                                   ",
+		"  ZoneControl:Thermostat,                                                                          ",
+		"    ZONE 1 CONTROLS,         !- Name                                                               ",
+		"    ZONE 1,                  !- Zone or ZoneList Name                                              ",
+		"    Zone Control Type Schedule,  !- Control Type Schedule Name                                     ",
+		"    ThermostatSetpoint:DualSetpoint,  !- Control 1 Object Type                                     ",
+		"    ZONE 1 SETPOINTS;        !- Control 1 Name                                                     ",
+		"                                                                                                   ",
+		"  ThermostatSetpoint:DualSetpoint,                                                                 ",
+		"    ZONE 1 SETPOINTS,        !- Name                                                               ",
+		"    ZONE Heating Setpoints,  !- Heating Setpoint Temperature Schedule Name                         ",
+		"    ZONE Cooling Setpoints;  !- Cooling Setpoint Temperature Schedule Name                         ",
+		"                                                                                                   ",
+		"  ZoneHVAC:EquipmentConnections,                                                                   ",
+		"    ZONE 1,                  !- Zone Name                                                          ",
+		"    ZONE 1 EQUIPMENT,        !- Zone Conditioning Equipment List Name                              ",
+		"    ZONE 1 INLETS,           !- Zone Air Inlet Node or NodeList Name                               ",
+		"    ,                        !- Zone Air Exhaust Node or NodeList Name                             ",
+		"    ZONE 1 NODE,             !- Zone Air Node Name                                                 ",
+		"    ZONE 1 OUTLET;           !- Zone Return Air Node Name                                          ",
+		"                                                                                                   ",
+		"  ZoneHVAC:EquipmentList,                                                                          ",
+		"    ZONE 1 EQUIPMENT,        !- Name                                                               ",
+		"    ZoneHVAC:IdealLoadsAirSystem,  !- Zone Equipment 1 Object Type                                 ",
+		"    ZONE 1 Ideal Loads,      !- Zone Equipment 1 Name                                              ",
+		"    1,                       !- Zone Equipment 1 Cooling Sequence                                  ",
+		"    1;                       !- Zone Equipment 1 Heating or No-Load Sequence                       ",
+		"                                                                                                   ",
+		"  ZoneHVAC:IdealLoadsAirSystem,                                                                    ",
+		"    ZONE 1 Ideal Loads,      !- Name                                                               ",
+		"    ,                        !- Availability Schedule Name                                         ",
+		"    ZONE 1 INLETS,           !- Zone Supply Air Node Name                                          ",
+		"    ,                        !- Zone Exhaust Air Node Name                                         ",
+		"    50,                      !- Maximum Heating Supply Air Temperature {C}                         ",
+		"    13,                      !- Minimum Cooling Supply Air Temperature {C}                         ",
+		"    0.015,                   !- Maximum Heating Supply Air Humidity Ratio {kgWater/kgDryAir}       ",
+		"    0.009,                   !- Minimum Cooling Supply Air Humidity Ratio {kgWater/kgDryAir}       ",
+		"    NoLimit,                 !- Heating Limit                                                      ",
+		"    autosize,                !- Maximum Heating Air Flow Rate {m3/s}                               ",
+		"    ,                        !- Maximum Sensible Heating Capacity {W}                              ",
+		"    NoLimit,                 !- Cooling Limit                                                      ",
+		"    autosize,                !- Maximum Cooling Air Flow Rate {m3/s}                               ",
+		"    ,                        !- Maximum Total Cooling Capacity {W}                                 ",
+		"    ,                        !- Heating Availability Schedule Name                                 ",
+		"    ,                        !- Cooling Availability Schedule Name                                 ",
+		"    ConstantSupplyHumidityRatio,  !- Dehumidification Control Type                                 ",
+		"    ,                        !- Cooling Sensible Heat Ratio {dimensionless}                        ",
+		"    ConstantSupplyHumidityRatio,  !- Humidification Control Type                                   ",
+		"    ,                        !- Design Specification Outdoor Air Object Name                       ",
+		"    ,                        !- Outdoor Air Inlet Node Name                                        ",
+		"    ,                        !- Demand Controlled Ventilation Type                                 ",
+		"    ,                        !- Outdoor Air Economizer Type                                        ",
+		"    ,                        !- Heat Recovery Type                                                 ",
+		"    ,                        !- Sensible Heat Recovery Effectiveness {dimensionless}               ",
+		"    ;                        !- Latent Heat Recovery Effectiveness {dimensionless}                 ",
+		"                                                                                                   ",
+		"  NodeList,                                                                                        ",
+		"    ZONE 1 INLETS,           !- Name                                                               ",
+		"    ZONE 1 INLET;            !- Node 1 Name                                                        ",
+		"                                                                                                   ",
+		"  ZoneControl:Thermostat,                                                                          ",
+		"    ZONE 2 CONTROLS,         !- Name                                                               ",
+		"    ZONE 2,                  !- Zone or ZoneList Name                                              ",
+		"    Zone Control Type Schedule,  !- Control Type Schedule Name                                     ",
+		"    ThermostatSetpoint:DualSetpoint,  !- Control 1 Object Type                                     ",
+		"    ZONE 2 SETPOINTS;        !- Control 1 Name                                                     ",
+		"                                                                                                   ",
+		"  ThermostatSetpoint:DualSetpoint,                                                                 ",
+		"    ZONE 2 SETPOINTS,        !- Name                                                               ",
+		"    ZONE Heating Setpoints,  !- Heating Setpoint Temperature Schedule Name                         ",
+		"    ZONE Cooling Setpoints;  !- Cooling Setpoint Temperature Schedule Name                         ",
+		"                                                                                                   ",
+		"  ZoneHVAC:EquipmentConnections,                                                                   ",
+		"    ZONE 2,                  !- Zone Name                                                          ",
+		"    ZONE 2 EQUIPMENT,        !- Zone Conditioning Equipment List Name                              ",
+		"    ZONE 2 INLETS,           !- Zone Air Inlet Node or NodeList Name                               ",
+		"    ,                        !- Zone Air Exhaust Node or NodeList Name                             ",
+		"    ZONE 2 NODE,             !- Zone Air Node Name                                                 ",
+		"    ZONE 2 OUTLET;           !- Zone Return Air Node Name                                          ",
+		"                                                                                                   ",
+		"  ZoneHVAC:EquipmentList,                                                                          ",
+		"    ZONE 2 EQUIPMENT,        !- Name                                                               ",
+		"    ZoneHVAC:IdealLoadsAirSystem,  !- Zone Equipment 1 Object Type                                 ",
+		"    ZONE 2 Ideal Loads,      !- Zone Equipment 1 Name                                              ",
+		"    1,                       !- Zone Equipment 1 Cooling Sequence                                  ",
+		"    1;                       !- Zone Equipment 1 Heating or No-Load Sequence                       ",
+		"                                                                                                   ",
+		"  ZoneHVAC:IdealLoadsAirSystem,                                                                    ",
+		"    ZONE 2 Ideal Loads,      !- Name                                                               ",
+		"    ,                        !- Availability Schedule Name                                         ",
+		"    ZONE 2 INLETS,           !- Zone Supply Air Node Name                                          ",
+		"    ,                        !- Zone Exhaust Air Node Name                                         ",
+		"    50,                      !- Maximum Heating Supply Air Temperature {C}                         ",
+		"    13,                      !- Minimum Cooling Supply Air Temperature {C}                         ",
+		"    0.015,                   !- Maximum Heating Supply Air Humidity Ratio {kgWater/kgDryAir}       ",
+		"    0.009,                   !- Minimum Cooling Supply Air Humidity Ratio {kgWater/kgDryAir}       ",
+		"    NoLimit,                 !- Heating Limit                                                      ",
+		"    autosize,                !- Maximum Heating Air Flow Rate {m3/s}                               ",
+		"    ,                        !- Maximum Sensible Heating Capacity {W}                              ",
+		"    NoLimit,                 !- Cooling Limit                                                      ",
+		"    autosize,                !- Maximum Cooling Air Flow Rate {m3/s}                               ",
+		"    ,                        !- Maximum Total Cooling Capacity {W}                                 ",
+		"    ,                        !- Heating Availability Schedule Name                                 ",
+		"    ,                        !- Cooling Availability Schedule Name                                 ",
+		"    ConstantSupplyHumidityRatio,  !- Dehumidification Control Type                                 ",
+		"    ,                        !- Cooling Sensible Heat Ratio {dimensionless}                        ",
+		"    ConstantSupplyHumidityRatio,  !- Humidification Control Type                                   ",
+		"    ,                        !- Design Specification Outdoor Air Object Name                       ",
+		"    ,                        !- Outdoor Air Inlet Node Name                                        ",
+		"    ,                        !- Demand Controlled Ventilation Type                                 ",
+		"    ,                        !- Outdoor Air Economizer Type                                        ",
+		"    ,                        !- Heat Recovery Type                                                 ",
+		"    ,                        !- Sensible Heat Recovery Effectiveness {dimensionless}               ",
+		"    ;                        !- Latent Heat Recovery Effectiveness {dimensionless}                 ",
+		"                                                                                                   ",
+		"  NodeList,                                                                                        ",
+		"    ZONE 2 INLETS,           !- Name                                                               ",
+		"    ZONE 2 INLET;            !- Node 1 Name                                                        ",
+		"                                                                                                   ",
+		"  ZoneControl:Thermostat,                                                                          ",
+		"    ZONE 3 CONTROLS,         !- Name                                                               ",
+		"    ZONE 3,                  !- Zone or ZoneList Name                                              ",
+		"    Zone Control Type Schedule,  !- Control Type Schedule Name                                     ",
+		"    ThermostatSetpoint:DualSetpoint,  !- Control 1 Object Type                                     ",
+		"    ZONE 3 SETPOINTS;        !- Control 1 Name                                                     ",
+		"                                                                                                   ",
+		"  ThermostatSetpoint:DualSetpoint,                                                                 ",
+		"    ZONE 3 SETPOINTS,        !- Name                                                               ",
+		"    ZONE Heating Setpoints,  !- Heating Setpoint Temperature Schedule Name                         ",
+		"    ZONE Cooling Setpoints;  !- Cooling Setpoint Temperature Schedule Name                         ",
+		"                                                                                                   ",
+		"  ZoneHVAC:EquipmentConnections,                                                                   ",
+		"    ZONE 3,                  !- Zone Name                                                          ",
+		"    ZONE 3 EQUIPMENT,        !- Zone Conditioning Equipment List Name                              ",
+		"    ZONE 3 INLETS,           !- Zone Air Inlet Node or NodeList Name                               ",
+		"    ,                        !- Zone Air Exhaust Node or NodeList Name                             ",
+		"    ZONE 3 NODE,             !- Zone Air Node Name                                                 ",
+		"    ZONE 3 OUTLET;           !- Zone Return Air Node Name                                          ",
+		"                                                                                                   ",
+		"  ZoneHVAC:EquipmentList,                                                                          ",
+		"    ZONE 3 EQUIPMENT,        !- Name                                                               ",
+		"    ZoneHVAC:IdealLoadsAirSystem,  !- Zone Equipment 1 Object Type                                 ",
+		"    ZONE 3 Ideal Loads,      !- Zone Equipment 1 Name                                              ",
+		"    1,                       !- Zone Equipment 1 Cooling Sequence                                  ",
+		"    1;                       !- Zone Equipment 1 Heating or No-Load Sequence                       ",
+		"                                                                                                   ",
+		"  ZoneHVAC:IdealLoadsAirSystem,                                                                    ",
+		"    ZONE 3 Ideal Loads,      !- Name                                                               ",
+		"    ,                        !- Availability Schedule Name                                         ",
+		"    ZONE 3 INLETS,           !- Zone Supply Air Node Name                                          ",
+		"    ,                        !- Zone Exhaust Air Node Name                                         ",
+		"    50,                      !- Maximum Heating Supply Air Temperature {C}                         ",
+		"    13,                      !- Minimum Cooling Supply Air Temperature {C}                         ",
+		"    0.015,                   !- Maximum Heating Supply Air Humidity Ratio {kgWater/kgDryAir}       ",
+		"    0.009,                   !- Minimum Cooling Supply Air Humidity Ratio {kgWater/kgDryAir}       ",
+		"    NoLimit,                 !- Heating Limit                                                      ",
+		"    autosize,                !- Maximum Heating Air Flow Rate {m3/s}                               ",
+		"    ,                        !- Maximum Sensible Heating Capacity {W}                              ",
+		"    NoLimit,                 !- Cooling Limit                                                      ",
+		"    autosize,                !- Maximum Cooling Air Flow Rate {m3/s}                               ",
+		"    ,                        !- Maximum Total Cooling Capacity {W}                                 ",
+		"    ,                        !- Heating Availability Schedule Name                                 ",
+		"    ,                        !- Cooling Availability Schedule Name                                 ",
+		"    ConstantSupplyHumidityRatio,  !- Dehumidification Control Type                                 ",
+		"    ,                        !- Cooling Sensible Heat Ratio {dimensionless}                        ",
+		"    ConstantSupplyHumidityRatio,  !- Humidification Control Type                                   ",
+		"    ,                        !- Design Specification Outdoor Air Object Name                       ",
+		"    ,                        !- Outdoor Air Inlet Node Name                                        ",
+		"    ,                        !- Demand Controlled Ventilation Type                                 ",
+		"    ,                        !- Outdoor Air Economizer Type                                        ",
+		"    ,                        !- Heat Recovery Type                                                 ",
+		"    ,                        !- Sensible Heat Recovery Effectiveness {dimensionless}               ",
+		"    ;                        !- Latent Heat Recovery Effectiveness {dimensionless}                 ",
+		"                                                                                                   ",
+		"  NodeList,                                                                                        ",
+		"    ZONE 3 INLETS,           !- Name                                                               ",
+		"    ZONE 3 INLET;            !- Node 1 Name                                                        ",
+		"                                                                                                   ",
+		"  ZoneControl:Thermostat,                                                                          ",
+		"    ZONE 4 CONTROLS,         !- Name                                                               ",
+		"    ZONE 4,                  !- Zone or ZoneList Name                                              ",
+		"    Zone Control Type Schedule,  !- Control Type Schedule Name                                     ",
+		"    ThermostatSetpoint:DualSetpoint,  !- Control 1 Object Type                                     ",
+		"    ZONE 4 SETPOINTS;        !- Control 1 Name                                                     ",
+		"                                                                                                   ",
+		"  ThermostatSetpoint:DualSetpoint,                                                                 ",
+		"    ZONE 4 SETPOINTS,        !- Name                                                               ",
+		"    ZONE Heating Setpoints,  !- Heating Setpoint Temperature Schedule Name                         ",
+		"    ZONE Cooling Setpoints;  !- Cooling Setpoint Temperature Schedule Name                         ",
+		"                                                                                                   ",
+		"  ZoneHVAC:EquipmentConnections,                                                                   ",
+		"    ZONE 4,                  !- Zone Name                                                          ",
+		"    ZONE 4 EQUIPMENT,        !- Zone Conditioning Equipment List Name                              ",
+		"    ZONE 4 INLETS,           !- Zone Air Inlet Node or NodeList Name                               ",
+		"    ,                        !- Zone Air Exhaust Node or NodeList Name                             ",
+		"    ZONE 4 NODE,             !- Zone Air Node Name                                                 ",
+		"    ZONE 4 OUTLET;           !- Zone Return Air Node Name                                          ",
+		"                                                                                                   ",
+		"  ZoneHVAC:EquipmentList,                                                                          ",
+		"    ZONE 4 EQUIPMENT,        !- Name                                                               ",
+		"    ZoneHVAC:IdealLoadsAirSystem,  !- Zone Equipment 1 Object Type                                 ",
+		"    ZONE 4 Ideal Loads,      !- Zone Equipment 1 Name                                              ",
+		"    1,                       !- Zone Equipment 1 Cooling Sequence                                  ",
+		"    1;                       !- Zone Equipment 1 Heating or No-Load Sequence                       ",
+		"                                                                                                   ",
+		"  ZoneHVAC:IdealLoadsAirSystem,                                                                    ",
+		"    ZONE 4 Ideal Loads,      !- Name                                                               ",
+		"    ,                        !- Availability Schedule Name                                         ",
+		"    ZONE 4 INLETS,           !- Zone Supply Air Node Name                                          ",
+		"    ,                        !- Zone Exhaust Air Node Name                                         ",
+		"    50,                      !- Maximum Heating Supply Air Temperature {C}                         ",
+		"    13,                      !- Minimum Cooling Supply Air Temperature {C}                         ",
+		"    0.015,                   !- Maximum Heating Supply Air Humidity Ratio {kgWater/kgDryAir}       ",
+		"    0.009,                   !- Minimum Cooling Supply Air Humidity Ratio {kgWater/kgDryAir}       ",
+		"    NoLimit,                 !- Heating Limit                                                      ",
+		"    autosize,                !- Maximum Heating Air Flow Rate {m3/s}                               ",
+		"    ,                        !- Maximum Sensible Heating Capacity {W}                              ",
+		"    NoLimit,                 !- Cooling Limit                                                      ",
+		"    autosize,                !- Maximum Cooling Air Flow Rate {m3/s}                               ",
+		"    ,                        !- Maximum Total Cooling Capacity {W}                                 ",
+		"    ,                        !- Heating Availability Schedule Name                                 ",
+		"    ,                        !- Cooling Availability Schedule Name                                 ",
+		"    ConstantSupplyHumidityRatio,  !- Dehumidification Control Type                                 ",
+		"    ,                        !- Cooling Sensible Heat Ratio {dimensionless}                        ",
+		"    ConstantSupplyHumidityRatio,  !- Humidification Control Type                                   ",
+		"    ,                        !- Design Specification Outdoor Air Object Name                       ",
+		"    ,                        !- Outdoor Air Inlet Node Name                                        ",
+		"    ,                        !- Demand Controlled Ventilation Type                                 ",
+		"    ,                        !- Outdoor Air Economizer Type                                        ",
+		"    ,                        !- Heat Recovery Type                                                 ",
+		"    ,                        !- Sensible Heat Recovery Effectiveness {dimensionless}               ",
+		"    ;                        !- Latent Heat Recovery Effectiveness {dimensionless}                 ",
+		"                                                                                                   ",
+		"  NodeList,                                                                                        ",
+		"    ZONE 4 INLETS,           !- Name                                                               ",
+		"    ZONE 4 INLET;            !- Node 1 Name                                                        ",
+		"                                                                                                   ",
+		"OutputControl:Table:Style,                                                                         ",
+		"    HTML,                    !- Column Separator                                                   ",
+		"    JtoKWH;                  !- Unit Conversion                                                    ",
+		"                                                                                                   ",
+		"Output:Table:SummaryReports,                                                                       ",
+		"    AllSummary;              !- Report 1 Name                                                      ",
+		"                                                                                                   "
+	} );
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	OutputProcessor::TimeValue.allocate( 2 );
+	DataGlobals::DDOnlySimulation = true;
+
+	ManageSimulation();
+//	compare_err_stream( "" );
+
+	EXPECT_EQ( "3", RetrievePreDefTableEntry( pdchSurfCntTot, "Overhang" ) );
+	EXPECT_EQ( "3", RetrievePreDefTableEntry( pdchSurfCntExt, "Overhang" ) );
+
+	EXPECT_EQ( "1", RetrievePreDefTableEntry( pdchSurfCntTot, "Fin" ) );
+	EXPECT_EQ( "1", RetrievePreDefTableEntry( pdchSurfCntExt, "Fin" ) );
+
+
+}
+
+TEST_F( EnergyPlusFixture, TubularDaylightDiffuserCount )
+{
+	// based on DaylightingDeviceTubular.idf
+	std::string const idf_objects = delimited_string( {
+		"  Version,8.5;                                                                            ",
+		"                                                                                          ",
+		"  Building,                                                                               ",
+		"    Tubular Daylighting Device Example,  !- Name                                          ",
+		"    0.0,                     !- North Axis {deg}                                          ",
+		"    Suburbs,                 !- Terrain                                                   ",
+		"    0.04,                    !- Loads Convergence Tolerance Value                         ",
+		"    0.04,                    !- Temperature Convergence Tolerance Value {deltaC}          ",
+		"    FullInteriorAndExterior, !- Solar Distribution                                        ",
+		"    25,                      !- Maximum Number of Warmup Days                             ",
+		"    6;                       !- Minimum Number of Warmup Days                             ",
+		"                                                                                          ",
+		"  Timestep,6;                                                                             ",
+		"                                                                                          ",
+		"  ShadowCalculation,                                                                      ",
+		"    AverageOverDaysInFrequency,  !- Calculation Method                                    ",
+		"    20;                      !- Calculation Frequency                                     ",
+		"                                                                                          ",
+		"  HeatBalanceAlgorithm,ConductionTransferFunction;                                        ",
+		"                                                                                          ",
+		"  SurfaceConvectionAlgorithm:Inside,TARP;                                                 ",
+		"                                                                                          ",
+		"  SurfaceConvectionAlgorithm:Outside,DOE-2;                                               ",
+		"                                                                                          ",
+		"  GlobalGeometryRules,                                                                    ",
+		"    UpperLeftCorner,         !- Starting Vertex Position                                  ",
+		"    CounterClockWise,        !- Vertex Entry Direction                                    ",
+		"    Relative;                !- Coordinate System                                         ",
+		"                                                                                          ",
+		"  Site:Location,                                                                          ",
+		"    CHICAGO_IL_USA_WMO_725300,  !- Name                                                   ",
+		"    42.00,                   !- Latitude {deg}                                            ",
+		"    -87.88,                  !- Longitude {deg}                                           ",
+		"    -6.00,                   !- Time Zone {hr}                                            ",
+		"    190.00;                  !- Elevation {m}                                             ",
+		"                                                                                          ",
+		"  SizingPeriod:DesignDay,                                                                 ",
+		"    CHICAGO Ann Htg 99% Condns DB,  !- Name                                               ",
+		"    1,                       !- Month                                                     ",
+		"    21,                      !- Day of Month                                              ",
+		"    WinterDesignDay,         !- Day Type                                                  ",
+		"    -17.3,                   !- Maximum Dry-Bulb Temperature {C}                          ",
+		"    0.0,                     !- Daily Dry-Bulb Temperature Range {deltaC}                 ",
+		"    ,                        !- Dry-Bulb Temperature Range Modifier Type                  ",
+		"    ,                        !- Dry-Bulb Temperature Range Modifier Day Schedule Name     ",
+		"    Wetbulb,                 !- Humidity Condition Type                                   ",
+		"    -17.3,                   !- Wetbulb or DewPoint at Maximum Dry-Bulb {C}               ",
+		"    ,                        !- Humidity Condition Day Schedule Name                      ",
+		"    ,                        !- Humidity Ratio at Maximum Dry-Bulb {kgWater/kgDryAir}     ",
+		"    ,                        !- Enthalpy at Maximum Dry-Bulb {J/kg}                       ",
+		"    ,                        !- Daily Wet-Bulb Temperature Range {deltaC}                 ",
+		"    99063.,                  !- Barometric Pressure {Pa}                                  ",
+		"    4.9,                     !- Wind Speed {m/s}                                          ",
+		"    270,                     !- Wind Direction {deg}                                      ",
+		"    No,                      !- Rain Indicator                                            ",
+		"    No,                      !- Snow Indicator                                            ",
+		"    No,                      !- Daylight Saving Time Indicator                            ",
+		"    ASHRAEClearSky,          !- Solar Model Indicator                                     ",
+		"    ,                        !- Beam Solar Day Schedule Name                              ",
+		"    ,                        !- Diffuse Solar Day Schedule Name                           ",
+		"    ,                        !- ASHRAE Clear Sky Optical Depth for Beam Irradiance (taub) ",
+		"    ,                        !- ASHRAE Clear Sky Optical Depth for Diffuse Irradiance (tau",
+		"    0.00;                    !- Sky Clearness                                             ",
+		"                                                                                          ",
+		"  SizingPeriod:DesignDay,                                                                 ",
+		"    CHICAGO Ann Clg 1% Condns DB=>MWB,  !- Name                                           ",
+		"    7,                       !- Month                                                     ",
+		"    21,                      !- Day of Month                                              ",
+		"    SummerDesignDay,         !- Day Type                                                  ",
+		"    31.5,                    !- Maximum Dry-Bulb Temperature {C}                          ",
+		"    10.7,                    !- Daily Dry-Bulb Temperature Range {deltaC}                 ",
+		"    ,                        !- Dry-Bulb Temperature Range Modifier Type                  ",
+		"    ,                        !- Dry-Bulb Temperature Range Modifier Day Schedule Name     ",
+		"    Wetbulb,                 !- Humidity Condition Type                                   ",
+		"    23,                      !- Wetbulb or DewPoint at Maximum Dry-Bulb {C}               ",
+		"    ,                        !- Humidity Condition Day Schedule Name                      ",
+		"    ,                        !- Humidity Ratio at Maximum Dry-Bulb {kgWater/kgDryAir}     ",
+		"    ,                        !- Enthalpy at Maximum Dry-Bulb {J/kg}                       ",
+		"    ,                        !- Daily Wet-Bulb Temperature Range {deltaC}                 ",
+		"    99063.,                  !- Barometric Pressure {Pa}                                  ",
+		"    5.3,                     !- Wind Speed {m/s}                                          ",
+		"    230,                     !- Wind Direction {deg}                                      ",
+		"    No,                      !- Rain Indicator                                            ",
+		"    No,                      !- Snow Indicator                                            ",
+		"    No,                      !- Daylight Saving Time Indicator                            ",
+		"    ASHRAEClearSky,          !- Solar Model Indicator                                     ",
+		"    ,                        !- Beam Solar Day Schedule Name                              ",
+		"    ,                        !- Diffuse Solar Day Schedule Name                           ",
+		"    ,                        !- ASHRAE Clear Sky Optical Depth for Beam Irradiance (taub) ",
+		"    ,                        !- ASHRAE Clear Sky Optical Depth for Diffuse Irradiance (tau",
+		"    1.00;                    !- Sky Clearness                                             ",
+		"                                                                                          ",
+		"  RunPeriod,                                                                              ",
+		"    ,                        !- Name                                                      ",
+		"    1,                       !- Begin Month                                               ",
+		"    1,                       !- Begin Day of Month                                        ",
+		"    12,                      !- End Month                                                 ",
+		"    31,                      !- End Day of Month                                          ",
+		"    Tuesday,                 !- Day of Week for Start Day                                 ",
+		"    Yes,                     !- Use Weather File Holidays and Special Days                ",
+		"    Yes,                     !- Use Weather File Daylight Saving Period                   ",
+		"    No,                      !- Apply Weekend Holiday Rule                                ",
+		"    Yes,                     !- Use Weather File Rain Indicators                          ",
+		"    Yes;                     !- Use Weather File Snow Indicators                          ",
+		"                                                                                          ",
+		"  SimulationControl,                                                                      ",
+		"    NO,                      !- Do Zone Sizing Calculation                                ",
+		"    NO,                      !- Do System Sizing Calculation                              ",
+		"    NO,                      !- Do Plant Sizing Calculation                               ",
+		"    YES,                     !- Run Simulation for Sizing Periods                         ",
+		"    NO;                      !- Run Simulation for Weather File Run Periods               ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    A1 - 1 IN STUCCO,        !- Name                                                      ",
+		"    Smooth,                  !- Roughness                                                 ",
+		"    2.5389841E-02,           !- Thickness {m}                                             ",
+		"    0.6918309,               !- Conductivity {W/m-K}                                      ",
+		"    1858.142,                !- Density {kg/m3}                                           ",
+		"    836.8,                   !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.92,                    !- Solar Absorptance                                         ",
+		"    0.92;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    C4 - 4 IN COMMON BRICK,  !- Name                                                      ",
+		"    Rough,                   !- Roughness                                                 ",
+		"    0.1014984,               !- Thickness {m}                                             ",
+		"    0.7264224,               !- Conductivity {W/m-K}                                      ",
+		"    1922.216,                !- Density {kg/m3}                                           ",
+		"    836.8,                   !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.76,                    !- Solar Absorptance                                         ",
+		"    0.76;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Name                                          ",
+		"    Smooth,                  !- Roughness                                                 ",
+		"    1.9050000E-02,           !- Thickness {m}                                             ",
+		"    0.7264224,               !- Conductivity {W/m-K}                                      ",
+		"    1601.846,                !- Density {kg/m3}                                           ",
+		"    836.8,                   !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.92,                    !- Solar Absorptance                                         ",
+		"    0.92;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    C6 - 8 IN CLAY TILE,     !- Name                                                      ",
+		"    Smooth,                  !- Roughness                                                 ",
+		"    0.2033016,               !- Thickness {m}                                             ",
+		"    0.5707605,               !- Conductivity {W/m-K}                                      ",
+		"    1121.292,                !- Density {kg/m3}                                           ",
+		"    836.8,                   !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.82,                    !- Solar Absorptance                                         ",
+		"    0.82;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    C10 - 8 IN HW CONCRETE,  !- Name                                                      ",
+		"    MediumRough,             !- Roughness                                                 ",
+		"    0.2033016,               !- Thickness {m}                                             ",
+		"    1.729577,                !- Conductivity {W/m-K}                                      ",
+		"    2242.585,                !- Density {kg/m3}                                           ",
+		"    836.8,                   !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.65,                    !- Solar Absorptance                                         ",
+		"    0.65;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    E2 - 1 / 2 IN SLAG OR STONE,  !- Name                                                 ",
+		"    Rough,                   !- Roughness                                                 ",
+		"    1.2710161E-02,           !- Thickness {m}                                             ",
+		"    1.435549,                !- Conductivity {W/m-K}                                      ",
+		"    881.0155,                !- Density {kg/m3}                                           ",
+		"    1673.6,                  !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.55,                    !- Solar Absorptance                                         ",
+		"    0.55;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    E3 - 3 / 8 IN FELT AND MEMBRANE,  !- Name                                             ",
+		"    Rough,                   !- Roughness                                                 ",
+		"    9.5402403E-03,           !- Thickness {m}                                             ",
+		"    0.1902535,               !- Conductivity {W/m-K}                                      ",
+		"    1121.292,                !- Density {kg/m3}                                           ",
+		"    1673.6,                  !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.75,                    !- Solar Absorptance                                         ",
+		"    0.75;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    B5 - 1 IN DENSE INSULATION,  !- Name                                                  ",
+		"    VeryRough,               !- Roughness                                                 ",
+		"    2.5389841E-02,           !- Thickness {m}                                             ",
+		"    4.3239430E-02,           !- Conductivity {W/m-K}                                      ",
+		"    91.30524,                !- Density {kg/m3}                                           ",
+		"    836.8,                   !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.50,                    !- Solar Absorptance                                         ",
+		"    0.50;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    C12 - 2 IN HW CONCRETE,  !- Name                                                      ",
+		"    MediumRough,             !- Roughness                                                 ",
+		"    5.0901599E-02,           !- Thickness {m}                                             ",
+		"    1.729577,                !- Conductivity {W/m-K}                                      ",
+		"    2242.585,                !- Density {kg/m3}                                           ",
+		"    836.8,                   !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.65,                    !- Solar Absorptance                                         ",
+		"    0.65;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    ROOFING - ASPHALT SHINGLES,  !- Name                                                  ",
+		"    VeryRough,               !- Roughness                                                 ",
+		"    3.1999999E-03,           !- Thickness {m}                                             ",
+		"    2.9999999E-02,           !- Conductivity {W/m-K}                                      ",
+		"    1121.29,                 !- Density {kg/m3}                                           ",
+		"    830.0,                   !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.70,                    !- Solar Absorptance                                         ",
+		"    0.70;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    BB46 - 5 / 8 IN PLYWOOD, !- Name                                                      ",
+		"    Smooth,                  !- Roughness                                                 ",
+		"    9.9999998E-03,           !- Thickness {m}                                             ",
+		"    0.110,                   !- Conductivity {W/m-K}                                      ",
+		"    544.62,                  !- Density {kg/m3}                                           ",
+		"    1210.0,                  !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.70,                    !- Solar Absorptance                                         ",
+		"    0.70;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    INS - GLASS FIBER BONDED 3 IN,  !- Name                                               ",
+		"    VeryRough,               !- Roughness                                                 ",
+		"    7.000E-02,               !- Thickness {m}                                             ",
+		"    2.9999999E-02,           !- Conductivity {W/m-K}                                      ",
+		"    96.11,                   !- Density {kg/m3}                                           ",
+		"    790.0,                   !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.50,                    !- Solar Absorptance                                         ",
+		"    0.50;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  WindowMaterial:Glazing,                                                                 ",
+		"    Clear Acrylic Plastic,   !- Name                                                      ",
+		"    SpectralAverage,         !- Optical Data Type                                         ",
+		"    ,                        !- Window Glass Spectral Data Set Name                       ",
+		"    0.003,                   !- Thickness {m}                                             ",
+		"    0.92,                    !- Solar Transmittance at Normal Incidence                   ",
+		"    0.05,                    !- Front Side Solar Reflectance at Normal Incidence          ",
+		"    0.05,                    !- Back Side Solar Reflectance at Normal Incidence           ",
+		"    0.92,                    !- Visible Transmittance at Normal Incidence                 ",
+		"    0.05,                    !- Front Side Visible Reflectance at Normal Incidence        ",
+		"    0.05,                    !- Back Side Visible Reflectance at Normal Incidence         ",
+		"    0.00,                    !- Infrared Transmittance at Normal Incidence                ",
+		"    0.90,                    !- Front Side Infrared Hemispherical Emissivity              ",
+		"    0.90,                    !- Back Side Infrared Hemispherical Emissivity               ",
+		"    0.90;                    !- Conductivity {W/m-K}                                      ",
+		"                                                                                          ",
+		"  WindowMaterial:Glazing,                                                                 ",
+		"    Diffusing Acrylic Plastic,  !- Name                                                   ",
+		"    SpectralAverage,         !- Optical Data Type                                         ",
+		"    ,                        !- Window Glass Spectral Data Set Name                       ",
+		"    0.0022,                  !- Thickness {m}                                             ",
+		"    0.90,                    !- Solar Transmittance at Normal Incidence                   ",
+		"    0.08,                    !- Front Side Solar Reflectance at Normal Incidence          ",
+		"    0.08,                    !- Back Side Solar Reflectance at Normal Incidence           ",
+		"    0.90,                    !- Visible Transmittance at Normal Incidence                 ",
+		"    0.08,                    !- Front Side Visible Reflectance at Normal Incidence        ",
+		"    0.08,                    !- Back Side Visible Reflectance at Normal Incidence         ",
+		"    0.00,                    !- Infrared Transmittance at Normal Incidence                ",
+		"    0.90,                    !- Front Side Infrared Hemispherical Emissivity              ",
+		"    0.90,                    !- Back Side Infrared Hemispherical Emissivity               ",
+		"    0.90;                    !- Conductivity {W/m-K}                                      ",
+		"                                                                                          ",
+		"  Material,                                                                               ",
+		"    Very High Reflectivity Surface,  !- Name                                              ",
+		"    Smooth,                  !- Roughness                                                 ",
+		"    0.0005,                  !- Thickness {m}                                             ",
+		"    237,                     !- Conductivity {W/m-K}                                      ",
+		"    2702,                    !- Density {kg/m3}                                           ",
+		"    903,                     !- Specific Heat {J/kg-K}                                    ",
+		"    0.90,                    !- Thermal Absorptance                                       ",
+		"    0.05,                    !- Solar Absorptance                                         ",
+		"    0.05;                    !- Visible Absorptance                                       ",
+		"                                                                                          ",
+		"  Construction,                                                                           ",
+		"    EXTWALL80,               !- Name                                                      ",
+		"    A1 - 1 IN STUCCO,        !- Outside Layer                                             ",
+		"    C4 - 4 IN COMMON BRICK,  !- Layer 2                                                   ",
+		"    E1 - 3 / 4 IN PLASTER OR GYP BOARD;  !- Layer 3                                       ",
+		"                                                                                          ",
+		"  Construction,                                                                           ",
+		"    FLOOR SLAB 8 IN,         !- Name                                                      ",
+		"    C10 - 8 IN HW CONCRETE;  !- Outside Layer                                             ",
+		"                                                                                          ",
+		"  Construction,                                                                           ",
+		"    ROOF,                    !- Name                                                      ",
+		"    ROOFING - ASPHALT SHINGLES,  !- Outside Layer                                         ",
+		"    E3 - 3 / 8 IN FELT AND MEMBRANE,  !- Layer 2                                          ",
+		"    BB46 - 5 / 8 IN PLYWOOD; !- Layer 3                                                   ",
+		"                                                                                          ",
+		"  Construction,                                                                           ",
+		"    CEILING IN ZONE,         !- Name                                                      ",
+		"    INS - GLASS FIBER BONDED 3 IN,  !- Outside Layer                                      ",
+		"    E1 - 3 / 4 IN PLASTER OR GYP BOARD;  !- Layer 2                                       ",
+		"                                                                                          ",
+		"  Construction,                                                                           ",
+		"    CEILING IN ATTIC,        !- Name                                                      ",
+		"    E1 - 3 / 4 IN PLASTER OR GYP BOARD,  !- Outside Layer                                 ",
+		"    INS - GLASS FIBER BONDED 3 IN;  !- Layer 2                                            ",
+		"                                                                                          ",
+		"  Construction,                                                                           ",
+		"    TDD Pipe,                !- Name                                                      ",
+		"    Very High Reflectivity Surface;  !- Outside Layer                                     ",
+		"                                                                                          ",
+		"  Construction,                                                                           ",
+		"    TDD Dome,                !- Name                                                      ",
+		"    Clear Acrylic Plastic;   !- Outside Layer                                             ",
+		"                                                                                          ",
+		"  Construction,                                                                           ",
+		"    TDD Diffuser,            !- Name                                                      ",
+		"    Diffusing Acrylic Plastic;  !- Outside Layer                                          ",
+		"                                                                                          ",
+		"  Zone,                                                                                   ",
+		"    Daylit Zone,             !- Name                                                      ",
+		"    0.0,                     !- Direction of Relative North {deg}                         ",
+		"    0.0,                     !- X Origin {m}                                              ",
+		"    0.0,                     !- Y Origin {m}                                              ",
+		"    0.0,                     !- Z Origin {m}                                              ",
+		"    1,                       !- Type                                                      ",
+		"    1,                       !- Multiplier                                                ",
+		"    autocalculate,           !- Ceiling Height {m}                                        ",
+		"    autocalculate;           !- Volume {m3}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit South Wall,       !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Daylit Zone,             !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,0.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    0.0,0.0,0.0,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,0.0,0.0,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    5.0,0.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit West Wall,        !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Daylit Zone,             !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,10.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    0.0,10.0,0.0,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    0.0,0.0,0.0,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    0.0,0.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit North Wall,       !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Daylit Zone,             !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    5.0,10.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    5.0,10.0,0.0,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    0.0,10.0,0.0,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    0.0,10.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit East Wall,        !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Daylit Zone,             !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    5.0,0.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    5.0,0.0,0.0,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,10.0,0.0,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    5.0,10.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit Floor,            !- Name                                                      ",
+		"    Floor,                   !- Surface Type                                              ",
+		"    FLOOR SLAB 8 IN,         !- Construction Name                                         ",
+		"    Daylit Zone,             !- Zone Name                                                 ",
+		"    Surface,                 !- Outside Boundary Condition                                ",
+		"    Daylit Floor,            !- Outside Boundary Condition Object                         ",
+		"    NoSun,                   !- Sun Exposure                                              ",
+		"    NoWind,                  !- Wind Exposure                                             ",
+		"    1.0,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,0.0,0.0,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    0.0,10.0,0.0,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    5.0,10.0,0.0,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    5.0,0.0,0.0;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit Ceiling,          !- Name                                                      ",
+		"    Roof,                    !- Surface Type                                              ",
+		"    CEILING IN ZONE,         !- Construction Name                                         ",
+		"    Daylit Zone,             !- Zone Name                                                 ",
+		"    Surface,                 !- Outside Boundary Condition                                ",
+		"    Daylit Attic Floor,      !- Outside Boundary Condition Object                         ",
+		"    NoSun,                   !- Sun Exposure                                              ",
+		"    NoWind,                  !- Wind Exposure                                             ",
+		"    0.0,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,10.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    0.0,0.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,0.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    5.0,10.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  Zone,                                                                                   ",
+		"    Daylit Attic Zone,       !- Name                                                      ",
+		"    0.0,                     !- Direction of Relative North {deg}                         ",
+		"    0.0,                     !- X Origin {m}                                              ",
+		"    0.0,                     !- Y Origin {m}                                              ",
+		"    0.0,                     !- Z Origin {m}                                              ",
+		"    1,                       !- Type                                                      ",
+		"    1,                       !- Multiplier                                                ",
+		"    autocalculate,           !- Ceiling Height {m}                                        ",
+		"    autocalculate;           !- Volume {m3}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit Attic South Wall, !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Daylit Attic Zone,       !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,0.0,3.0,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    0.0,0.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,0.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    5.0,0.0,3.0;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit Attic West Wall,  !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Daylit Attic Zone,       !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,10.0,5.0,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    0.0,10.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    0.0,0.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    0.0,0.0,3.0;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit Attic North Wall, !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Daylit Attic Zone,       !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    5.0,10.0,5.0,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    5.0,10.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    0.0,10.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    0.0,10.0,5.0;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit Attic East Wall,  !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Daylit Attic Zone,       !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    5.0,0.0,3.0,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    5.0,0.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,10.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    5.0,10.0,5.0;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit Attic Floor,      !- Name                                                      ",
+		"    Floor,                   !- Surface Type                                              ",
+		"    CEILING IN ATTIC,        !- Construction Name                                         ",
+		"    Daylit Attic Zone,       !- Zone Name                                                 ",
+		"    Surface,                 !- Outside Boundary Condition                                ",
+		"    Daylit Ceiling,          !- Outside Boundary Condition Object                         ",
+		"    NoSun,                   !- Sun Exposure                                              ",
+		"    NoWind,                  !- Wind Exposure                                             ",
+		"    0.0,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,0.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    0.0,10.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    5.0,10.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    5.0,0.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Daylit Attic Roof,       !- Name                                                      ",
+		"    Roof,                    !- Surface Type                                              ",
+		"    ROOF,                    !- Construction Name                                         ",
+		"    Daylit Attic Zone,       !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.0,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,10.0,5.0,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    0.0,0.0,3.0,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,0.0,3.0,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    5.0,10.0,5.0;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  Zone,                                                                                   ",
+		"    Standard Zone,           !- Name                                                      ",
+		"    0.0,                     !- Direction of Relative North {deg}                         ",
+		"    50.0,                    !- X Origin {m}                                              ",
+		"    50.0,                    !- Y Origin {m}                                              ",
+		"    0.0,                     !- Z Origin {m}                                              ",
+		"    1,                       !- Type                                                      ",
+		"    1,                       !- Multiplier                                                ",
+		"    autocalculate,           !- Ceiling Height {m}                                        ",
+		"    autocalculate;           !- Volume {m3}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard South Wall,     !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Standard Zone,           !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,0.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    0.0,0.0,0.0,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,0.0,0.0,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    5.0,0.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard West Wall,      !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Standard Zone,           !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,10.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    0.0,10.0,0.0,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    0.0,0.0,0.0,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    0.0,0.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard North Wall,     !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Standard Zone,           !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    5.0,10.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    5.0,10.0,0.0,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    0.0,10.0,0.0,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    0.0,10.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard East Wall,      !- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Standard Zone,           !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    5.0,0.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    5.0,0.0,0.0,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,10.0,0.0,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    5.0,10.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard Floor,          !- Name                                                      ",
+		"    Floor,                   !- Surface Type                                              ",
+		"    FLOOR SLAB 8 IN,         !- Construction Name                                         ",
+		"    Standard Zone,           !- Zone Name                                                 ",
+		"    Surface,                 !- Outside Boundary Condition                                ",
+		"    Standard Floor,          !- Outside Boundary Condition Object                         ",
+		"    NoSun,                   !- Sun Exposure                                              ",
+		"    NoWind,                  !- Wind Exposure                                             ",
+		"    1.0,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,0.0,0.0,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    0.0,10.0,0.0,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    5.0,10.0,0.0,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    5.0,0.0,0.0;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard Ceiling,        !- Name                                                      ",
+		"    Roof,                    !- Surface Type                                              ",
+		"    CEILING IN ZONE,         !- Construction Name                                         ",
+		"    Standard Zone,           !- Zone Name                                                 ",
+		"    Surface,                 !- Outside Boundary Condition                                ",
+		"    Standard Attic Floor,    !- Outside Boundary Condition Object                         ",
+		"    NoSun,                   !- Sun Exposure                                              ",
+		"    NoWind,                  !- Wind Exposure                                             ",
+		"    0.0,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,10.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    0.0,0.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,0.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    5.0,10.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  Zone,                                                                                   ",
+		"    Standard Attic Zone,     !- Name                                                      ",
+		"    0.0,                     !- Direction of Relative North {deg}                         ",
+		"    50.0,                    !- X Origin {m}                                              ",
+		"    50.0,                    !- Y Origin {m}                                              ",
+		"    0.0,                     !- Z Origin {m}                                              ",
+		"    1,                       !- Type                                                      ",
+		"    1,                       !- Multiplier                                                ",
+		"    autocalculate,           !- Ceiling Height {m}                                        ",
+		"    autocalculate;           !- Volume {m3}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard Attic South Wall,  !- Name                                                   ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Standard Attic Zone,     !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,0.0,3.0,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    0.0,0.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,0.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    5.0,0.0,3.0;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard Attic West Wall,!- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Standard Attic Zone,     !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,10.0,5.0,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    0.0,10.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    0.0,0.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    0.0,0.0,3.0;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard Attic North Wall,  !- Name                                                   ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Standard Attic Zone,     !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    5.0,10.0,5.0,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    5.0,10.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    0.0,10.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    0.0,10.0,5.0;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard Attic East Wall,!- Name                                                      ",
+		"    Wall,                    !- Surface Type                                              ",
+		"    EXTWALL80,               !- Construction Name                                         ",
+		"    Standard Attic Zone,     !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.5,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    5.0,0.0,3.0,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    5.0,0.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,10.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    5.0,10.0,5.0;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard Attic Floor,    !- Name                                                      ",
+		"    Floor,                   !- Surface Type                                              ",
+		"    CEILING IN ATTIC,        !- Construction Name                                         ",
+		"    Standard Attic Zone,     !- Zone Name                                                 ",
+		"    Surface,                 !- Outside Boundary Condition                                ",
+		"    Standard Ceiling,        !- Outside Boundary Condition Object                         ",
+		"    NoSun,                   !- Sun Exposure                                              ",
+		"    NoWind,                  !- Wind Exposure                                             ",
+		"    0.0,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,0.0,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                               ",
+		"    0.0,10.0,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                              ",
+		"    5.0,10.0,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                              ",
+		"    5.0,0.0,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                               ",
+		"                                                                                          ",
+		"  BuildingSurface:Detailed,                                                               ",
+		"    Standard Attic Roof,     !- Name                                                      ",
+		"    Roof,                    !- Surface Type                                              ",
+		"    ROOF,                    !- Construction Name                                         ",
+		"    Standard Attic Zone,     !- Zone Name                                                 ",
+		"    Outdoors,                !- Outside Boundary Condition                                ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    SunExposed,              !- Sun Exposure                                              ",
+		"    WindExposed,             !- Wind Exposure                                             ",
+		"    0.0,                     !- View Factor to Ground                                     ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    0.0,10.0,5.0,  !- X,Y,Z ==> Vertex 1 {m}                                              ",
+		"    0.0,0.0,3.0,  !- X,Y,Z ==> Vertex 2 {m}                                               ",
+		"    5.0,0.0,3.0,  !- X,Y,Z ==> Vertex 3 {m}                                               ",
+		"    5.0,10.0,5.0;  !- X,Y,Z ==> Vertex 4 {m}                                              ",
+		"                                                                                          ",
+		"  Lights,                                                                                 ",
+		"    Daylit Zone Lights 1,    !- Name                                                      ",
+		"    Daylit Zone,             !- Zone or ZoneList Name                                     ",
+		"    AlwaysOnSchedule,        !- Schedule Name                                             ",
+		"    LightingLevel,           !- Design Level Calculation Method                           ",
+		"    800,                     !- Lighting Level {W}                                        ",
+		"    ,                        !- Watts per Zone Floor Area {W/m2}                          ",
+		"    ,                        !- Watts per Person {W/person}                               ",
+		"    0,                       !- Return Air Fraction                                       ",
+		"    0.40,                    !- Fraction Radiant                                          ",
+		"    0.20,                    !- Fraction Visible                                          ",
+		"    1.0,                     !- Fraction Replaceable                                      ",
+		"    GeneralLights;           !- End-Use Subcategory                                       ",
+		"                                                                                          ",
+		"  Lights,                                                                                 ",
+		"    Standard Zone Lights 1,  !- Name                                                      ",
+		"    Standard Zone,           !- Zone or ZoneList Name                                     ",
+		"    AlwaysOnSchedule,        !- Schedule Name                                             ",
+		"    LightingLevel,           !- Design Level Calculation Method                           ",
+		"    800,                     !- Lighting Level {W}                                        ",
+		"    ,                        !- Watts per Zone Floor Area {W/m2}                          ",
+		"    ,                        !- Watts per Person {W/person}                               ",
+		"    0,                       !- Return Air Fraction                                       ",
+		"    0.40,                    !- Fraction Radiant                                          ",
+		"    0.20,                    !- Fraction Visible                                          ",
+		"    1.0,                     !- Fraction Replaceable                                      ",
+		"    GeneralLights;           !- End-Use Subcategory                                       ",
+		"                                                                                          ",
+		"  DaylightingDevice:Tubular,                                                              ",
+		"    Pipe1,                   !- Name                                                      ",
+		"    Dome1,                   !- Dome Name                                                 ",
+		"    Diffuser1,               !- Diffuser Name                                             ",
+		"    TDD Pipe,                !- Construction Name                                         ",
+		"    0.3556,                  !- Diameter {m}                                              ",
+		"    1.4,                     !- Total Length {m}                                          ",
+		"    0.28,                    !- Effective Thermal Resistance {m2-K/W}                     ",
+		"    Daylit Attic Zone,       !- Transition Zone 1 Name                                    ",
+		"    1.1;                     !- Transition Zone 1 Length {m}                              ",
+		"                                                                                          ",
+		"  FenestrationSurface:Detailed,                                                           ",
+		"    Dome1,                   !- Name                                                      ",
+		"    TubularDaylightDome,     !- Surface Type                                              ",
+		"    TDD Dome,                !- Construction Name                                         ",
+		"    Daylit Attic Roof,       !- Building Surface Name                                     ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    0.0,                     !- View Factor to Ground                                     ",
+		"    ,                        !- Shading Control Name                                      ",
+		"    ,                        !- Frame and Divider Name                                    ",
+		"    1.0,                     !- Multiplier                                                ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    2.3425,3.209,3.64,  !- X,Y,Z ==> Vertex 1 {m}                                         ",
+		"    2.3425,2.906,3.58,  !- X,Y,Z ==> Vertex 2 {m}                                         ",
+		"    2.6575,2.906,3.58,  !- X,Y,Z ==> Vertex 3 {m}                                         ",
+		"    2.6575,3.209,3.64;  !- X,Y,Z ==> Vertex 4 {m}                                         ",
+		"                                                                                          ",
+		"  FenestrationSurface:Detailed,                                                           ",
+		"    Diffuser1,               !- Name                                                      ",
+		"    TubularDaylightDiffuser, !- Surface Type                                              ",
+		"    TDD Diffuser,            !- Construction Name                                         ",
+		"    Daylit Ceiling,          !- Building Surface Name                                     ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    0.0,                     !- View Factor to Ground                                     ",
+		"    ,                        !- Shading Control Name                                      ",
+		"    ,                        !- Frame and Divider Name                                    ",
+		"    1.0,                     !- Multiplier                                                ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    2.3425,3.1575,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                         ",
+		"    2.3425,2.8425,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                         ",
+		"    2.6575,2.8425,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                         ",
+		"    2.6575,3.1575,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                         ",
+		"                                                                                          ",
+		"  DaylightingDevice:Tubular,                                                              ",
+		"    Pipe2,                   !- Name                                                      ",
+		"    Dome2,                   !- Dome Name                                                 ",
+		"    Diffuser2,               !- Diffuser Name                                             ",
+		"    TDD Pipe,                !- Construction Name                                         ",
+		"    0.3556,                  !- Diameter {m}                                              ",
+		"    2.2,                     !- Total Length {m}                                          ",
+		"    0.28,                    !- Effective Thermal Resistance {m2-K/W}                     ",
+		"    Daylit Attic Zone,       !- Transition Zone 1 Name                                    ",
+		"    1.9;                     !- Transition Zone 1 Length {m}                              ",
+		"                                                                                          ",
+		"  FenestrationSurface:Detailed,                                                           ",
+		"    Dome2,                   !- Name                                                      ",
+		"    TubularDaylightDome,     !- Surface Type                                              ",
+		"    TDD Dome,                !- Construction Name                                         ",
+		"    Daylit Attic Roof,       !- Building Surface Name                                     ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    0.0,                     !- View Factor to Ground                                     ",
+		"    ,                        !- Shading Control Name                                      ",
+		"    ,                        !- Frame and Divider Name                                    ",
+		"    1.0,                     !- Multiplier                                                ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    2.3425,7.209134615385,4.441826923077,  !- X,Y,Z ==> Vertex 1 {m}                      ",
+		"    2.3425,6.90625,4.38125,  !- X,Y,Z ==> Vertex 2 {m}                                    ",
+		"    2.6575,6.90625,4.38125,  !- X,Y,Z ==> Vertex 3 {m}                                    ",
+		"    2.6575,7.209134615385,4.441826923077;  !- X,Y,Z ==> Vertex 4 {m}                      ",
+		"                                                                                          ",
+		"  FenestrationSurface:Detailed,                                                           ",
+		"    Diffuser2,               !- Name                                                      ",
+		"    TubularDaylightDiffuser, !- Surface Type                                              ",
+		"    TDD Diffuser,            !- Construction Name                                         ",
+		"    Daylit Ceiling,          !- Building Surface Name                                     ",
+		"    ,                        !- Outside Boundary Condition Object                         ",
+		"    0.0,                     !- View Factor to Ground                                     ",
+		"    ,                        !- Shading Control Name                                      ",
+		"    ,                        !- Frame and Divider Name                                    ",
+		"    1.0,                     !- Multiplier                                                ",
+		"    4,                       !- Number of Vertices                                        ",
+		"    2.3425,7.1575,2.5,  !- X,Y,Z ==> Vertex 1 {m}                                         ",
+		"    2.3425,6.8425,2.5,  !- X,Y,Z ==> Vertex 2 {m}                                         ",
+		"    2.6575,6.8425,2.5,  !- X,Y,Z ==> Vertex 3 {m}                                         ",
+		"    2.6575,7.1575,2.5;  !- X,Y,Z ==> Vertex 4 {m}                                         ",
+		"                                                                                          ",
+		"  Daylighting:Controls,                                                                   ",
+		"    Daylit Zone,             !- Zone Name                                                 ",
+		"    2,                       !- Total Daylighting Reference Points                        ",
+		"    2.5,                     !- X-Coordinate of First Reference Point {m}                 ",
+		"    5.0,                     !- Y-Coordinate of First Reference Point {m}                 ",
+		"    0.8,                     !- Z-Coordinate of First Reference Point {m}                 ",
+		"    2.5,                     !- X-Coordinate of Second Reference Point {m}                ",
+		"    3.0,                     !- Y-Coordinate of Second Reference Point {m}                ",
+		"    0.8,                     !- Z-Coordinate of Second Reference Point {m}                ",
+		"    1.0,                     !- Fraction of Zone Controlled by First Reference Point      ",
+		"    0.0,                     !- Fraction of Zone Controlled by Second Reference Point     ",
+		"    550,                     !- Illuminance Setpoint at First Reference Point {lux}       ",
+		"    0,                       !- Illuminance Setpoint at Second Reference Point {lux}      ",
+		"    1,                       !- Lighting Control Type                                     ",
+		"    0.0,                     !- Glare Calculation Azimuth Angle of View Direction Clockwis",
+		"    20.0,                    !- Maximum Allowable Discomfort Glare Index                  ",
+		"    0.3,                     !- Minimum Input Power Fraction for Continuous Dimming Contro",
+		"    0.2,                     !- Minimum Light Output Fraction for Continuous Dimming Contr",
+		"    0,                       !- Number of Stepped Control Steps                           ",
+		"    1.0;                     !- Probability Lighting will be Reset When Needed in Manual S",
+		"                                                                                          ",
+		"  OutputControl:IlluminanceMap:Style,                                                     ",
+		"    Comma;                   !- Column Separator                                          ",
+		"                                                                                          ",
+		"  Output:IlluminanceMap,                                                                  ",
+		"    Daylit Map,              !- Name                                                      ",
+		"    Daylit Zone,             !- Zone Name                                                 ",
+		"    0.8,                     !- Z height {m}                                              ",
+		"    0.1,                     !- X Minimum Coordinate {m}                                  ",
+		"    4.9,                     !- X Maximum Coordinate {m}                                  ",
+		"    10,                      !- Number of X Grid Points                                   ",
+		"    0.1,                     !- Y Minimum Coordinate {m}                                  ",
+		"    9.9,                     !- Y Maximum Coordinate {m}                                  ",
+		"    10;                      !- Number of Y Grid Points                                   ",
+		"                                                                                          ",
+		"  ScheduleTypeLimits,                                                                     ",
+		"    On/Off,                  !- Name                                                      ",
+		"    0,                       !- Lower Limit Value                                         ",
+		"    1,                       !- Upper Limit Value                                         ",
+		"    DISCRETE;                !- Numeric Type                                              ",
+		"                                                                                          ",
+		"  Schedule:Compact,                                                                       ",
+		"    AlwaysOnSchedule,        !- Name                                                      ",
+		"    On/Off,                  !- Schedule Type Limits Name                                 ",
+		"    THROUGH: 12/31,          !- Field 1                                                   ",
+		"    FOR: AllDays,            !- Field 2                                                   ",
+		"    UNTIL: 24:00,1;          !- Field 3                                                   ",
+		"                                                                                          ",
+		"  ScheduleTypeLimits,                                                                     ",
+		"    Control Type,            !- Name                                                      ",
+		"    0,                       !- Lower Limit Value                                         ",
+		"    4,                       !- Upper Limit Value                                         ",
+		"    DISCRETE;                !- Numeric Type                                              ",
+		"                                                                                          ",
+		"  Schedule:Compact,                                                                       ",
+		"    Zone Control Type Sch,   !- Name                                                      ",
+		"    Control Type,            !- Schedule Type Limits Name                                 ",
+		"    THROUGH: 12/31,          !- Field 1                                                   ",
+		"    FOR: AllDays,            !- Field 2                                                   ",
+		"    UNTIL: 24:00,3;          !- Field 3                                                   ",
+		"                                                                                          ",
+		"  ScheduleTypeLimits,                                                                     ",
+		"    Temperature,             !- Name                                                      ",
+		"    -60,                     !- Lower Limit Value                                         ",
+		"    200,                     !- Upper Limit Value                                         ",
+		"    CONTINUOUS,              !- Numeric Type                                              ",
+		"    Temperature;             !- Unit Type                                                 ",
+		"                                                                                          ",
+		"  Schedule:Compact,                                                                       ",
+		"    Zone Temp Sch,           !- Name                                                      ",
+		"    Temperature,             !- Schedule Type Limits Name                                 ",
+		"    THROUGH: 12/31,          !- Field 1                                                   ",
+		"    FOR: AllDays,            !- Field 2                                                   ",
+		"    UNTIL: 24:00,21;         !- Field 3                                                   ",
+		"                                                                                          ",
+		"  NodeList,                                                                               ",
+		"    Daylit Zone Inlets,      !- Name                                                      ",
+		"    Daylit Zone Supply Node; !- Node 1 Name                                               ",
+		"                                                                                          ",
+		"  ZoneHVAC:EquipmentConnections,                                                          ",
+		"    Daylit Zone,             !- Zone Name                                                 ",
+		"    Daylit Zone Equipment,   !- Zone Conditioning Equipment List Name                     ",
+		"    Daylit Zone Inlets,      !- Zone Air Inlet Node or NodeList Name                      ",
+		"    ,                        !- Zone Air Exhaust Node or NodeList Name                    ",
+		"    Daylit Zone Air Node,    !- Zone Air Node Name                                        ",
+		"    Daylit Zone Return Node; !- Zone Return Air Node Name                                 ",
+		"                                                                                          ",
+		"  ThermostatSetpoint:SingleHeatingOrCooling,                                              ",
+		"    Heating Cooling Setpoint,!- Name                                                      ",
+		"    Zone Temp Sch;           !- Setpoint Temperature Schedule Name                        ",
+		"                                                                                          ",
+		"  ZoneControl:Thermostat,                                                                 ",
+		"    Daylit Zone Thermostat,  !- Name                                                      ",
+		"    Daylit Zone,             !- Zone or ZoneList Name                                     ",
+		"    Zone Control Type Sch,   !- Control Type Schedule Name                                ",
+		"    ThermostatSetpoint:SingleHeatingOrCooling,  !- Control 1 Object Type                  ",
+		"    Heating Cooling Setpoint;!- Control 1 Name                                            ",
+		"                                                                                          ",
+		"  ZoneHVAC:EquipmentList,                                                                 ",
+		"    Daylit Zone Equipment,   !- Name                                                      ",
+		"    ZoneHVAC:IdealLoadsAirSystem,  !- Zone Equipment 1 Object Type                        ",
+		"    Daylit Zone Air,         !- Zone Equipment 1 Name                                     ",
+		"    1,                       !- Zone Equipment 1 Cooling Sequence                         ",
+		"    1;                       !- Zone Equipment 1 Heating or No-Load Sequence              ",
+		"                                                                                          ",
+		"  ZoneHVAC:IdealLoadsAirSystem,                                                           ",
+		"    Daylit Zone Air,         !- Name                                                      ",
+		"    ,                        !- Availability Schedule Name                                ",
+		"    Daylit Zone Supply Node, !- Zone Supply Air Node Name                                 ",
+		"    ,                        !- Zone Exhaust Air Node Name                                ",
+		"    50,                      !- Maximum Heating Supply Air Temperature {C}                ",
+		"    13,                      !- Minimum Cooling Supply Air Temperature {C}                ",
+		"    0.015,                   !- Maximum Heating Supply Air Humidity Ratio {kgWater/kgDryAi",
+		"    0.009,                   !- Minimum Cooling Supply Air Humidity Ratio {kgWater/kgDryAi",
+		"    NoLimit,                 !- Heating Limit                                             ",
+		"    AUTOSIZE,                !- Maximum Heating Air Flow Rate {m3/s}                      ",
+		"    ,                        !- Maximum Sensible Heating Capacity {W}                     ",
+		"    NoLimit,                 !- Cooling Limit                                             ",
+		"    AUTOSIZE,                !- Maximum Cooling Air Flow Rate {m3/s}                      ",
+		"    ,                        !- Maximum Total Cooling Capacity {W}                        ",
+		"    ,                        !- Heating Availability Schedule Name                        ",
+		"    ,                        !- Cooling Availability Schedule Name                        ",
+		"    ConstantSupplyHumidityRatio,  !- Dehumidification Control Type                        ",
+		"    ,                        !- Cooling Sensible Heat Ratio {dimensionless}               ",
+		"    ConstantSupplyHumidityRatio,  !- Humidification Control Type                          ",
+		"    ,                        !- Design Specification Outdoor Air Object Name              ",
+		"    ,                        !- Outdoor Air Inlet Node Name                               ",
+		"    ,                        !- Demand Controlled Ventilation Type                        ",
+		"    ,                        !- Outdoor Air Economizer Type                               ",
+		"    ,                        !- Heat Recovery Type                                        ",
+		"    ,                        !- Sensible Heat Recovery Effectiveness {dimensionless}      ",
+		"    ;                        !- Latent Heat Recovery Effectiveness {dimensionless}        ",
+		"                                                                                          ",
+		"  NodeList,                                                                               ",
+		"    Standard Zone Inlets,    !- Name                                                      ",
+		"    Standard Zone Supply Node;  !- Node 1 Name                                            ",
+		"                                                                                          ",
+		"  ZoneHVAC:EquipmentConnections,                                                          ",
+		"    Standard Zone,           !- Zone Name                                                 ",
+		"    Standard Zone Equipment, !- Zone Conditioning Equipment List Name                     ",
+		"    Standard Zone Inlets,    !- Zone Air Inlet Node or NodeList Name                      ",
+		"    ,                        !- Zone Air Exhaust Node or NodeList Name                    ",
+		"    Standard Zone Air Node,  !- Zone Air Node Name                                        ",
+		"    Standard Zone Return Node;  !- Zone Return Air Node Name                              ",
+		"                                                                                          ",
+		"  ThermostatSetpoint:SingleHeatingOrCooling,                                              ",
+		"    Heating Cooling Setpoint,!- Name                                                      ",
+		"    Zone Temp Sch;           !- Setpoint Temperature Schedule Name                        ",
+		"                                                                                          ",
+		"  ZoneControl:Thermostat,                                                                 ",
+		"    Standard Zone Thermostat,!- Name                                                      ",
+		"    Standard Zone,           !- Zone or ZoneList Name                                     ",
+		"    Zone Control Type Sch,   !- Control Type Schedule Name                                ",
+		"    ThermostatSetpoint:SingleHeatingOrCooling,  !- Control 1 Object Type                  ",
+		"    Heating Cooling Setpoint;!- Control 1 Name                                            ",
+		"                                                                                          ",
+		"  ZoneHVAC:EquipmentList,                                                                 ",
+		"    Standard Zone Equipment, !- Name                                                      ",
+		"    ZoneHVAC:IdealLoadsAirSystem,  !- Zone Equipment 1 Object Type                        ",
+		"    Standard Zone Air,       !- Zone Equipment 1 Name                                     ",
+		"    1,                       !- Zone Equipment 1 Cooling Sequence                         ",
+		"    1;                       !- Zone Equipment 1 Heating or No-Load Sequence              ",
+		"                                                                                          ",
+		"  ZoneHVAC:IdealLoadsAirSystem,                                                           ",
+		"    Standard Zone Air,       !- Name                                                      ",
+		"    ,                        !- Availability Schedule Name                                ",
+		"    Standard Zone Supply Node,  !- Zone Supply Air Node Name                              ",
+		"    ,                        !- Zone Exhaust Air Node Name                                ",
+		"    50,                      !- Maximum Heating Supply Air Temperature {C}                ",
+		"    13,                      !- Minimum Cooling Supply Air Temperature {C}                ",
+		"    0.015,                   !- Maximum Heating Supply Air Humidity Ratio {kgWater/kgDryAi",
+		"    0.009,                   !- Minimum Cooling Supply Air Humidity Ratio {kgWater/kgDryAi",
+		"    NoLimit,                 !- Heating Limit                                             ",
+		"    AUTOSIZE,                !- Maximum Heating Air Flow Rate {m3/s}                      ",
+		"    ,                        !- Maximum Sensible Heating Capacity {W}                     ",
+		"    NoLimit,                 !- Cooling Limit                                             ",
+		"    AUTOSIZE,                !- Maximum Cooling Air Flow Rate {m3/s}                      ",
+		"    ,                        !- Maximum Total Cooling Capacity {W}                        ",
+		"    ,                        !- Heating Availability Schedule Name                        ",
+		"    ,                        !- Cooling Availability Schedule Name                        ",
+		"    ConstantSupplyHumidityRatio,  !- Dehumidification Control Type                        ",
+		"    ,                        !- Cooling Sensible Heat Ratio {dimensionless}               ",
+		"    ConstantSupplyHumidityRatio,  !- Humidification Control Type                          ",
+		"    ,                        !- Design Specification Outdoor Air Object Name              ",
+		"    ,                        !- Outdoor Air Inlet Node Name                               ",
+		"    ,                        !- Demand Controlled Ventilation Type                        ",
+		"    ,                        !- Outdoor Air Economizer Type                               ",
+		"    ,                        !- Heat Recovery Type                                        ",
+		"    ,                        !- Sensible Heat Recovery Effectiveness {dimensionless}      ",
+		"    ;                        !- Latent Heat Recovery Effectiveness {dimensionless}        ",
+		"                                                                                          ",
+		"  Output:VariableDictionary,Regular;                                                      ",
+		"                                                                                          ",
+		"  Output:Surfaces:Drawing,DXF;                                                            ",
+		"                                                                                          ",
+		"  Output:Constructions,Constructions;                                                     ",
+		"                                                                                          ",
+		"  Output:Surfaces:List,Detailswithvertices;                                               ",
+		"                                                                                          ",
+		"  OutputControl:Table:Style,                                                              ",
+		"    HTML;                    !- Column Separator                                          ",
+		"                                                                                          ",
+		"  Output:Table:SummaryReports,                                                            ",
+		"    AllSummary;              !- Report 1 Name                                             ",
+		"                                                                                          ",
+		"  Output:SQLite,                                                                          ",
+		"    SimpleAndTabular;        !- Option Type                                               ",
+	} );
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	OutputProcessor::TimeValue.allocate( 2 );
+	DataGlobals::DDOnlySimulation = true;
+
+	ManageSimulation();
+	//compare_err_stream( "" );
+
+	EXPECT_EQ( "2", RetrievePreDefTableEntry( pdchSurfCntTot, "Tubular Daylighting Device Diffuser" ) );
+	EXPECT_EQ( "2", RetrievePreDefTableEntry( pdchSurfCntExt, "Tubular Daylighting Device Diffuser" ) );
+
+}
+
+
+
+
+
+
diff --git a/tst/EnergyPlus/unit/PierceSurface.unit.cc b/tst/EnergyPlus/unit/PierceSurface.unit.cc
index 56160ab5b0b..ea24c451e79 100644
--- a/tst/EnergyPlus/unit/PierceSurface.unit.cc
+++ b/tst/EnergyPlus/unit/PierceSurface.unit.cc
@@ -83,7 +83,7 @@ TEST( PierceSurfaceTest, Rectangular )
 	DataSurfaces::SurfaceData floor;
 	floor.Vertex.dimension( 4 );
 	floor.Vertex = { Vector(0,0,0), Vector(1,0,0), Vector(1,1,0), Vector(0,1,0) };
-	floor.Shape = Rectangle;
+	floor.Shape = SurfaceShape::Rectangle;
 	floor.set_computed_geometry();
 	DataSurfaces::Surface2D const & floor2d( floor.surface2d );
 	EXPECT_EQ( ShapeCat::Rectangular, floor.shapeCat );
@@ -155,7 +155,7 @@ TEST( PierceSurfaceTest, Triangular )
 	DataSurfaces::SurfaceData floor;
 	floor.Vertex.dimension( 3 );
 	floor.Vertex = { Vector(0,0,0), Vector(1,0,0), Vector(1,1,0) };
-	floor.Shape = Triangle;
+	floor.Shape = SurfaceShape::Triangle;
 	floor.set_computed_geometry();
 	DataSurfaces::Surface2D const & floor2d( floor.surface2d );
 	EXPECT_EQ( ShapeCat::Triangular, floor.shapeCat );
diff --git a/tst/EnergyPlus/unit/PlantPipingSystemsManager.unit.cc b/tst/EnergyPlus/unit/PlantPipingSystemsManager.unit.cc
new file mode 100644
index 00000000000..0ae0aab2596
--- /dev/null
+++ b/tst/EnergyPlus/unit/PlantPipingSystemsManager.unit.cc
@@ -0,0 +1,1638 @@
+// EnergyPlus, Copyright (c) 1996-2016, The Board of Trustees of the University of Illinois and
+// The Regents of the University of California, through Lawrence Berkeley National Laboratory
+// (subject to receipt of any required approvals from the U.S. Dept. of Energy). All rights
+// reserved.
+//
+// If you have questions about your rights to use or distribute this software, please contact
+// Berkeley Lab's Innovation & Partnerships Office at IPO@lbl.gov.
+//
+// NOTICE: This Software was developed under funding from the U.S. Department of Energy and the
+// U.S. Government consequently retains certain rights. As such, the U.S. Government has been
+// granted for itself and others acting on its behalf a paid-up, nonexclusive, irrevocable,
+// worldwide license in the Software to reproduce, distribute copies to the public, prepare
+// derivative works, and perform publicly and display publicly, and to permit others to do so.
+//
+// Redistribution and use in source and binary forms, with or without modification, are permitted
+// provided that the following conditions are met:
+//
+// (1) Redistributions of source code must retain the above copyright notice, this list of
+//     conditions and the following disclaimer.
+//
+// (2) Redistributions in binary form must reproduce the above copyright notice, this list of
+//     conditions and the following disclaimer in the documentation and/or other materials
+//     provided with the distribution.
+//
+// (3) Neither the name of the University of California, Lawrence Berkeley National Laboratory,
+//     the University of Illinois, U.S. Dept. of Energy nor the names of its contributors may be
+//     used to endorse or promote products derived from this software without specific prior
+//     written permission.
+//
+// (4) Use of EnergyPlus(TM) Name. If Licensee (i) distributes the software in stand-alone form
+//     without changes from the version obtained under this License, or (ii) Licensee makes a
+//     reference solely to the software portion of its product, Licensee must refer to the
+//     software as "EnergyPlus version X" software, where "X" is the version number Licensee
+//     obtained under this License and may not use a different name for the software. Except as
+//     specifically required in this Section (4), Licensee shall not use in a company name, a
+//     product name, in advertising, publicity, or other promotional activities any name, trade
+//     name, trademark, logo, or other designation of "EnergyPlus", "E+", "e+" or confusingly
+//     similar designation, without Lawrence Berkeley National Laboratory's prior written consent.
+//
+// THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS" AND ANY EXPRESS OR
+// IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY
+// AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT OWNER OR
+// CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR
+// CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR
+// SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY
+// THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR
+// OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
+// POSSIBILITY OF SUCH DAMAGE.
+//
+// You are under no obligation whatsoever to provide any bug fixes, patches, or upgrades to the
+// features, functionality or performance of the source code ("Enhancements") to anyone; however,
+// if you choose to make your Enhancements available either publicly, or directly to Lawrence
+// Berkeley National Laboratory, without imposing a separate written license agreement for such
+// Enhancements, then you hereby grant the following license: a non-exclusive, royalty-free
+// perpetual license to install, use, modify, prepare derivative works, incorporate into other
+// computer software, distribute, and sublicense such enhancements or derivative works thereof,
+// in binary and source code form.
+
+// EnergyPlus::PlantPipingSystemsManager Unit Tests
+
+// Google Test Headers
+#include <gtest/gtest.h>
+
+#include "Fixtures/EnergyPlusFixture.hh"
+#include "EnergyPlus/DataPlantPipingSystems.hh"
+#include "EnergyPlus/DataSurfaces.hh"
+#include "EnergyPlus/HeatBalanceManager.hh"
+#include "EnergyPlus/PlantPipingSystemsManager.hh"
+#include "EnergyPlus/SurfaceGeometry.hh"
+
+using namespace EnergyPlus;
+using namespace PlantPipingSystemsManager;
+using DataPlantPipingSystems::PipingSystemDomains;
+using DataSurfaces::Surface;
+using HeatBalanceManager::GetMaterialData;
+using SurfaceGeometry::GetOSCMData;
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_CorrectInputs ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Full,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_FALSE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_BadOSCMName ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSC,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Full,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_BadSlabLocation ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Full,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_BadSlabMaterialName ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Materia,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Full,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_BadHorizInsSelection ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Ye,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Full,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_BadHorizInsMaterialName ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Materal,	!- Horizontal Insulation Material Name",
+			"Full,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_BadHorizInsExtentsSelection ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Ful,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_PerimeterInsulationWidth ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Perimeter,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_BadVertInsSelection ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Full,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Ye,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_BadVertInsMaterialName ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Full,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Materia,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_BadVertInsDepth ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Full,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			",			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourly;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainSlab_CheckInputs_BadTimeStepSelection ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Slab,",
+			"CoupledSlab,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,	!- Name of Floor Boundary Condition Model",
+			"InGrade,		!- Slab Location (InGrade/OnGrade)",
+			"Dummy Material,	!- Slab Material Name",
+			"Yes,			!- Horizontal Insulation (Yes/No)",
+			"Dummy Material,	!- Horizontal Insulation Material Name",
+			"Full,			!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			",				!- Perimeter insulation width (m)",
+			"Yes,			!- Vertical Insulation (Yes/No)",
+			"Dummy Material,	!- Vertical Insulation Name",
+			"1.5,			!- Vertical perimeter insulation depth from surface (m)",
+			"Hourl;		!- Domain Simulation Interval. (Timestep/Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadZoneCoupledDomainInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainBasement_CheckInputs_CorrectInputs ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Basement,",
+			"CoupledBasement,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Horizontal Underfloor Insulation Present (Yes/No)",
+			"Dummy Material,		!- Basement Horizontal Insulation Underfloor Material Name",
+			"Perimeter,				!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			"1,						!- Perimeter width (m)",
+			"2.5,					!- Depth of Basement Wall In Ground Domain {m}",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Wall Vertical Insulation Present(Yes/No)",
+			"Dummy Material,		!- Basement Wall Vertical Insulation Material Name",
+			"2.3,					!- Vertical insulation depth from surface (m)",
+			"timestep;				!- Domain Update interval. (Timestep, Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadBasementInputs( 1, 1, errorsFound );
+
+	EXPECT_FALSE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainBasement_CheckInputs_BadOSCMName ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Basement,",
+			"CoupledBasement,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSC,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Horizontal Underfloor Insulation Present (Yes/No)",
+			"Dummy Material,		!- Basement Horizontal Insulation Underfloor Material Name",
+			"Perimeter,				!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			"1,						!- Perimeter width (m)",
+			"2.5,					!- Depth of Basement Wall In Ground Domain {m}",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Wall Vertical Insulation Present(Yes/No)",
+			"Dummy Material,		!- Basement Wall Vertical Insulation Material Name",
+			"2.3,					!- Vertical insulation depth from surface (m)",
+			"timestep;				!- Domain Update interval. (Timestep, Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadBasementInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainBasement_CheckInputs_BadHorizInsSelection ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Basement,",
+			"CoupledBasement,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Ye,					!- Basement Horizontal Underfloor Insulation Present (Yes/No)",
+			"Dummy Material,		!- Basement Horizontal Insulation Underfloor Material Name",
+			"Perimeter,				!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			"1,						!- Perimeter width (m)",
+			"2.5,					!- Depth of Basement Wall In Ground Domain {m}",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Wall Vertical Insulation Present(Yes/No)",
+			"Dummy Material,		!- Basement Wall Vertical Insulation Material Name",
+			"2.3,					!- Vertical insulation depth from surface (m)",
+			"timestep;				!- Domain Update interval. (Timestep, Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadBasementInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainBasement_CheckInputs_BadHorizInsMaterial ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Basement,",
+			"CoupledBasement,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Horizontal Underfloor Insulation Present (Yes/No)",
+			"Dummy Materia,			!- Basement Horizontal Insulation Underfloor Material Name",
+			"Perimeter,				!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			"1,						!- Perimeter width (m)",
+			"2.5,					!- Depth of Basement Wall In Ground Domain {m}",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Wall Vertical Insulation Present(Yes/No)",
+			"Dummy Material,		!- Basement Wall Vertical Insulation Material Name",
+			"2.3,					!- Vertical insulation depth from surface (m)",
+			"timestep;				!- Domain Update interval. (Timestep, Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadBasementInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainBasement_CheckInputs_BadHorizInsExtents ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Basement,",
+			"CoupledBasement,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Horizontal Underfloor Insulation Present (Yes/No)",
+			"Dummy Material,			!- Basement Horizontal Insulation Underfloor Material Name",
+			"Perimete,				!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			"1,						!- Perimeter width (m)",
+			"2.5,					!- Depth of Basement Wall In Ground Domain {m}",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Wall Vertical Insulation Present(Yes/No)",
+			"Dummy Material,		!- Basement Wall Vertical Insulation Material Name",
+			"2.3,					!- Vertical insulation depth from surface (m)",
+			"timestep;				!- Domain Update interval. (Timestep, Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadBasementInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainBasement_CheckInputs_BadBasementDepth ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Basement,",
+			"CoupledBasement,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Horizontal Underfloor Insulation Present (Yes/No)",
+			"Dummy Material,		!- Basement Horizontal Insulation Underfloor Material Name",
+			"Perimeter,				!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			"1,						!- Perimeter width (m)",
+			"25,					!- Depth of Basement Wall In Ground Domain {m}",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Wall Vertical Insulation Present(Yes/No)",
+			"Dummy Material,		!- Basement Wall Vertical Insulation Material Name",
+			"2.3,					!- Vertical insulation depth from surface (m)",
+			"timestep;				!- Domain Update interval. (Timestep, Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadBasementInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainBasement_CheckInputs_BadFloorOSCMName ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Basement,",
+			"CoupledBasement,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Horizontal Underfloor Insulation Present (Yes/No)",
+			"Dummy Material,		!- Basement Horizontal Insulation Underfloor Material Name",
+			"Perimeter,				!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			"1,						!- Perimeter width (m)",
+			"2.5,					!- Depth of Basement Wall In Ground Domain {m}",
+			"GroundCoupledOSC,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Wall Vertical Insulation Present(Yes/No)",
+			"Dummy Material,		!- Basement Wall Vertical Insulation Material Name",
+			"2.3,					!- Vertical insulation depth from surface (m)",
+			"timestep;				!- Domain Update interval. (Timestep, Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadBasementInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainBasement_CheckInputs_BadVertInsSelection ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Basement,",
+			"CoupledBasement,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Horizontal Underfloor Insulation Present (Yes/No)",
+			"Dummy Material,		!- Basement Horizontal Insulation Underfloor Material Name",
+			"Perimeter,				!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			"1,						!- Perimeter width (m)",
+			"2.5,					!- Depth of Basement Wall In Ground Domain {m}",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Ye,					!- Basement Wall Vertical Insulation Present(Yes/No)",
+			"Dummy Material,		!- Basement Wall Vertical Insulation Material Name",
+			"2.3,					!- Vertical insulation depth from surface (m)",
+			"timestep;				!- Domain Update interval. (Timestep, Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadBasementInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainBasement_CheckInputs_BadVertInsName ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Basement,",
+			"CoupledBasement,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Horizontal Underfloor Insulation Present (Yes/No)",
+			"Dummy Material,		!- Basement Horizontal Insulation Underfloor Material Name",
+			"Perimeter,				!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			"1,						!- Perimeter width (m)",
+			"2.5,					!- Depth of Basement Wall In Ground Domain {m}",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Wall Vertical Insulation Present(Yes/No)",
+			"Dummy Materia,			!- Basement Wall Vertical Insulation Material Name",
+			"2.3,					!- Vertical insulation depth from surface (m)",
+			"timestep;				!- Domain Update interval. (Timestep, Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadBasementInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
+
+TEST_F( EnergyPlusFixture, SiteGroundDomainBasement_CheckInputs_BadTimestepSelection ) {
+
+	std::string const idf_objects = delimited_string({
+		"Version,8.5;",
+		"Site:GroundDomain:Basement,",
+			"CoupledBasement,	!- Name",
+			"5,				!- Ground Domain Depth {m}",
+			"1,				!- Aspect Ratio",
+			"5,				!- Domain Perimeter Offset {m}",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"30,			!- Soil Moisture Content Volume Fraction {percent}",
+			"50,			!- Soil Moisture Content Volume Fraction at Saturation {percent}",
+			"Site:GroundTemperature:Undisturbed:KusudaAchenbach,	!- Type of Undisturbed Ground Temperature Model",
+			"KATemps,		!- Name of Undisturbed Ground Temperature Model",
+			"1,				!- Evapotranspiration Ground Cover Parameter",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Horizontal Underfloor Insulation Present (Yes/No)",
+			"Dummy Material,		!- Basement Horizontal Insulation Underfloor Material Name",
+			"Perimeter,				!- Full Horizontal or Perimeter Only (Full/Perimeter)",
+			"1,						!- Perimeter width (m)",
+			"2.5,					!- Depth of Basement Wall In Ground Domain {m}",
+			"GroundCoupledOSCM,		!- Name of Basement Floor Boundary Condition Model",
+			"Yes,					!- Basement Wall Vertical Insulation Present(Yes/No)",
+			"Dummy Material,		!- Basement Wall Vertical Insulation Material Name",
+			"2.3,					!- Vertical insulation depth from surface (m)",
+			"timeste;				!- Domain Update interval. (Timestep, Hourly)",
+		"Site:GroundTemperature:Undisturbed:KusudaAchenbach,",
+			"KATemps,		!- Name of object",
+			"1.8,			!- Soil Thermal Conductivity {W/m-K}",
+			"3200,			!- Soil Density {kg/m3}",
+			"836,			!- Soil Specific Heat {J/kg-K}",
+			"15.5,			!- Annual average surface temperature {C}",
+			"12.8,			!- Annual amplitude of surface temperature {delta C}",
+			"17.3;			!- Phase shift of minimum surface temperature {days}",
+		"SurfaceProperty:OtherSideConditionsModel,",
+			"GroundCoupledOSCM,		!- Name",
+			"GroundCoupledSurface;	!- Type of Modeling",
+		"Material,",
+			"Dummy Material, !- Name",
+			"MediumRough,	!- Roughness",
+			"0.1397,		!- Thickness {m}",
+			"1.8,			!- Conductivity {W/m-K}",
+			"2400,			!- Density {kg/m3}",
+			"750,			!- Specific Heat {J/kg-K}",
+			"0.9,			!- Thermal Absorptance",
+			"0.65,			!- Solar Absorptance",
+			"0.65;			!- Visible Absorptance",
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	// Dummy surface
+	Surface.allocate( 1 );
+	Surface( 1 ).OSCMPtr = 1;
+	Surface( 1 ).Area = 100;
+
+	PipingSystemDomains.allocate( 1 );
+
+	bool errorsFound = false;
+
+	// Other necessary inputs
+	GetOSCMData( errorsFound );
+	GetMaterialData( errorsFound );
+
+	ReadBasementInputs( 1, 1, errorsFound );
+
+	EXPECT_TRUE( errorsFound );
+}
diff --git a/tst/EnergyPlus/unit/SQLite.unit.cc b/tst/EnergyPlus/unit/SQLite.unit.cc
index d477a8ab577..7d7c71f408c 100644
--- a/tst/EnergyPlus/unit/SQLite.unit.cc
+++ b/tst/EnergyPlus/unit/SQLite.unit.cc
@@ -585,7 +585,7 @@ namespace EnergyPlus {
 		surfaceData1->Azimuth = 2;
 		surfaceData1->Height = 2;
 		surfaceData1->Reveal = 2;
-		surfaceData1->Shape = 2;
+		surfaceData1->Shape = DataSurfaces::SurfaceShape::Quadrilateral;
 		surfaceData1->Sides = 2;
 		surfaceData1->Tilt = 2;
 		surfaceData1->Width = 2;
diff --git a/tst/EnergyPlus/unit/SingleDuct.unit.cc b/tst/EnergyPlus/unit/SingleDuct.unit.cc
new file mode 100644
index 00000000000..6a201bd9d72
--- /dev/null
+++ b/tst/EnergyPlus/unit/SingleDuct.unit.cc
@@ -0,0 +1,402 @@
+// EnergyPlus, Copyright (c) 1996-2016, The Board of Trustees of the University of Illinois and
+// The Regents of the University of California, through Lawrence Berkeley National Laboratory
+// (subject to receipt of any required approvals from the U.S. Dept. of Energy). All rights
+// reserved.
+//
+// If you have questions about your rights to use or distribute this software, please contact
+// Berkeley Lab's Innovation & Partnerships Office at IPO@lbl.gov.
+//
+// NOTICE: This Software was developed under funding from the U.S. Department of Energy and the
+// U.S. Government consequently retains certain rights. As such, the U.S. Government has been
+// granted for itself and others acting on its behalf a paid-up, nonexclusive, irrevocable,
+// worldwide license in the Software to reproduce, distribute copies to the public, prepare
+// derivative works, and perform publicly and display publicly, and to permit others to do so.
+//
+// Redistribution and use in source and binary forms, with or without modification, are permitted
+// provided that the following conditions are met:
+//
+// (1) Redistributions of source code must retain the above copyright notice, this list of
+//     conditions and the following disclaimer.
+//
+// (2) Redistributions in binary form must reproduce the above copyright notice, this list of
+//     conditions and the following disclaimer in the documentation and/or other materials
+//     provided with the distribution.
+//
+// (3) Neither the name of the University of California, Lawrence Berkeley National Laboratory,
+//     the University of Illinois, U.S. Dept. of Energy nor the names of its contributors may be
+//     used to endorse or promote products derived from this software without specific prior
+//     written permission.
+//
+// (4) Use of EnergyPlus(TM) Name. If Licensee (i) distributes the software in stand-alone form
+//     without changes from the version obtained under this License, or (ii) Licensee makes a
+//     reference solely to the software portion of its product, Licensee must refer to the
+//     software as "EnergyPlus version X" software, where "X" is the version number Licensee
+//     obtained under this License and may not use a different name for the software. Except as
+//     specifically required in this Section (4), Licensee shall not use in a company name, a
+//     product name, in advertising, publicity, or other promotional activities any name, trade
+//     name, trademark, logo, or other designation of "EnergyPlus", "E+", "e+" or confusingly
+//     similar designation, without Lawrence Berkeley National Laboratory's prior written consent.
+//
+// THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS" AND ANY EXPRESS OR
+// IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY
+// AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT OWNER OR
+// CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR
+// CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR
+// SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY
+// THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR
+// OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
+// POSSIBILITY OF SUCH DAMAGE.
+//
+// You are under no obligation whatsoever to provide any bug fixes, patches, or upgrades to the
+// features, functionality or performance of the source code ("Enhancements") to anyone; however,
+// if you choose to make your Enhancements available either publicly, or directly to Lawrence
+// Berkeley National Laboratory, without imposing a separate written license agreement for such
+// Enhancements, then you hereby grant the following license: a non-exclusive, royalty-free
+// perpetual license to install, use, modify, prepare derivative works, incorporate into other
+// computer software, distribute, and sublicense such enhancements or derivative works thereof,
+// in binary and source code form.
+
+// EnergyPlus::Standalone ERV Unit Tests
+
+#include <fstream>
+
+// Google Test Headers
+#include <gtest/gtest.h>
+
+// EnergyPlus Headers
+#include "Fixtures/EnergyPlusFixture.hh"
+#include <General.hh>
+#include <DataEnvironment.hh>
+#include <DataHeatBalFanSys.hh>
+#include <DataHVACGlobals.hh>
+#include <DataLoopNode.hh>
+#include <DataZoneEnergyDemands.hh>
+#include <DataZoneEquipment.hh>
+#include <HeatBalanceManager.hh>
+#include <Psychrometrics.hh>
+#include <ScheduleManager.hh>
+#include <SingleDuct.hh>
+#include <ZoneAirLoopEquipmentManager.hh>
+
+using namespace EnergyPlus;
+
+
+TEST_F( EnergyPlusFixture, VAVNoReheatTerminalUnitSchedule ) {
+	std::string const idf_objects = delimited_string( {
+		"Version,8.4;",
+		"  Zone,",
+		"    Zone 1;                !- Name",
+		"ZoneHVAC:EquipmentConnections,",
+		"    Zone 1,                !- Zone Name",
+		"    Zone 1 Equipment,             !- Zone Conditioning Equipment List Name",
+		"    Zone 1 Supply Inlet,       !- Zone Air Inlet Node or NodeList Name",
+		"    ,      !- Zone Air Exhaust Node or NodeList Name",
+		"    Zone 1 Air Node,           !- Zone Air Node Name",
+		"    Zone 1 Return Node;       !- Zone Return Air Node Name",
+		"ZoneHVAC:EquipmentList,",
+		"    Zone 1 Equipment,             !- Name",
+		"    ZoneHVAC:AirDistributionUnit,  !- Zone Equipment 1 Object Type",
+		"    Zone 1 ADU,            !- Zone Equipment 1 Name",
+		"    1,                       !- Zone Equipment 1 Cooling Sequence",
+		"    1;                       !- Zone Equipment 1 Heating or No-Load Sequence",
+		"ZoneHVAC:AirDistributionUnit,",
+		"    Zone 1 ADU,    !- Name",
+		"    Zone 1 Supply Inlet,     !- Air Distribution Unit Outlet Node Name",
+		"    AirTerminal:SingleDuct:VAV:NoReheat,  !- Air Terminal Object Type",
+		"    Zone 1 VAV No Reheat;           !- Air Terminal Name",
+		"AirTerminal:SingleDuct:VAV:NoReheat,",
+		"    Zone 1 VAV No Reheat,    !- Name",
+		"    AlwaysOff,               !- Availability Schedule Name",
+		"    Zone 1 Supply Inlet,     !- Air Outlet Node Name",
+		"    Zone 1 Zone Equip Inlet, !- Air Inlet Node Name",
+		"    2.0,                     !- Maximum Air Flow Rate {m3/s}",
+		"    Constant,                !- Zone Minimum Air Flow Input Method",
+		"    0.5;                     !- Constant Minimum Air Flow Fraction",
+		"Schedule:Constant,",
+		"    AlwaysOff,               !- Name",
+		"    ,                        !- Schedule Type Limits Name",
+		"    0;                       !- Hourly Value",
+		"Schedule:Constant,",
+		"    AlwaysOn,               !- Name",
+		"    ,                        !- Schedule Type Limits Name",
+		"    1;                       !- Hourly Value",
+
+	} ) ;
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	DataGlobals::NumOfTimeStepInHour = 1; // must initialize this to get schedules initialized
+	DataGlobals::MinutesPerTimeStep = 60; // must initialize this to get schedules initialized
+	ScheduleManager::ProcessScheduleInput(); // read schedules
+	ScheduleManager::ScheduleInputProcessed = true;
+	DataEnvironment::Month = 1;
+	DataEnvironment::DayOfMonth = 21;
+	DataGlobals::HourOfDay = 1;
+	DataGlobals::TimeStep = 1;
+	DataEnvironment::DSTIndicator = 0;
+	DataEnvironment::DayOfWeek = 2;
+	DataEnvironment::HolidayIndex = 0;
+	DataEnvironment::DayOfYear_Schedule = General::JulianDay(DataEnvironment::Month, DataEnvironment::DayOfMonth, 1);
+	DataEnvironment::StdRhoAir = Psychrometrics::PsyRhoAirFnPbTdbW( 101325.0, 20.0, 0.0 ); 
+	ScheduleManager::UpdateScheduleValues();
+
+	bool ErrorsFound = false;
+	HeatBalanceManager::GetZoneData(ErrorsFound);
+	ASSERT_FALSE(ErrorsFound);
+	DataZoneEquipment::GetZoneEquipmentData1();
+	ZoneAirLoopEquipmentManager::GetZoneAirLoopEquipment();
+	SingleDuct::GetSysInput();
+	EXPECT_TRUE( compare_err_stream( "" ) );
+	DataHeatBalFanSys::TempControlType.allocate( 1 );
+	DataHeatBalFanSys::TempControlType( 1 ) = DataHVACGlobals::DualSetPointWithDeadBand;
+
+	// node number table
+	//  1   Zone 1 Air Node
+	//  2   Zone 1 Return Node
+	//  3   Zone 1 Supply Inlet
+	//  4   Zone 1 Zone Equip Inlet
+
+	DataZoneEnergyDemands::ZoneSysEnergyDemand.allocate(1);
+
+	// Setup for Zone 1 VAV No Reheat
+	int SysNum = 1;
+	int ZoneNum = 1;
+	int ZoneNodeNum = 1;
+	int InletNodeNum = 4;
+	bool FirstHVACIteration = true;
+	Real64 SysMinMassFlow = 1.0 * DataEnvironment::StdRhoAir; // From inputs for Zone 1 VAV
+	Real64 SysMaxMassFlow = 2.0 * DataEnvironment::StdRhoAir; // From inputs for Zone 1 VAV
+
+	// Test with heating load
+	DataZoneEnergyDemands::ZoneSysEnergyDemand( 1 ).RemainingOutputRequired = 2000.0; // Heating load - expect min flow rate
+
+	// First test - AlwaysOff Schedule - expecting no flow
+	SingleDuct::Sys( SysNum ).SchedPtr = 1;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRate = SysMinMassFlow;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRateMaxAvail = SysMaxMassFlow;
+	DataGlobals::BeginEnvrnFlag = true; // Must be true for initial pass thru SingleDuct::InitSys for this terminal unit
+	FirstHVACIteration = true;
+	SingleDuct::InitSys( SysNum, FirstHVACIteration ); // Run thru init once with FirstHVACIteration set to true
+	DataGlobals::BeginEnvrnFlag = false;
+	FirstHVACIteration = false;
+	SingleDuct::InitSys(SysNum, FirstHVACIteration); // Run thru init a second time with FirstHVACIteration set to false
+	SingleDuct::SimVAV( SysNum, FirstHVACIteration, ZoneNum, ZoneNodeNum );
+	EXPECT_EQ( 0.0, SingleDuct::SysOutlet( SysNum ).AirMassFlowRateMaxAvail );
+	EXPECT_EQ( 0.0, SingleDuct::SysOutlet( SysNum ).AirMassFlowRate );
+
+	// Second test - AlwaysOn Schedule - expecting flow
+	// Reset flows and switch to AlwaysOn Schedule
+	DataLoopNode::Node( InletNodeNum ).MassFlowRate = SysMinMassFlow;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRateMaxAvail = SysMaxMassFlow;
+	SingleDuct::Sys( SysNum ).SchedPtr = 2;
+	FirstHVACIteration = true;
+	SingleDuct::InitSys( SysNum, FirstHVACIteration ); // Run thru init once with FirstHVACIteration set to true
+	FirstHVACIteration = false;
+	SingleDuct::InitSys(SysNum, FirstHVACIteration); // Run thru init a second time with FirstHVACIteration set to false
+	SingleDuct::SimVAV( SysNum, FirstHVACIteration, ZoneNum, ZoneNodeNum );
+	EXPECT_EQ( SysMaxMassFlow, SingleDuct::SysOutlet( SysNum ).AirMassFlowRateMaxAvail );
+	EXPECT_EQ( SysMinMassFlow, SingleDuct::SysOutlet( SysNum ).AirMassFlowRate );
+
+	// Test with cooling load
+	DataZoneEnergyDemands::ZoneSysEnergyDemand( 1 ).RemainingOutputRequired = -2000.0; // Cooling load - expect max flow rate
+
+	// First test - AlwaysOff Schedule - expecting no flow
+	SingleDuct::Sys( SysNum ).SchedPtr = 1;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRate = SysMinMassFlow;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRateMaxAvail = SysMaxMassFlow;
+	DataGlobals::BeginEnvrnFlag = true; // Must be true for initial pass thru SingleDuct::InitSys for this terminal unit
+	FirstHVACIteration = true;
+	SingleDuct::InitSys( SysNum, FirstHVACIteration ); // Run thru init once with FirstHVACIteration set to true
+	DataGlobals::BeginEnvrnFlag = false;
+	FirstHVACIteration = false;
+	SingleDuct::InitSys(SysNum, FirstHVACIteration); // Run thru init a second time with FirstHVACIteration set to false
+	SingleDuct::SimVAV( SysNum, FirstHVACIteration, ZoneNum, ZoneNodeNum );
+	EXPECT_EQ( 0.0, SingleDuct::SysOutlet( SysNum ).AirMassFlowRateMaxAvail );
+	EXPECT_EQ( 0.0, SingleDuct::SysOutlet( SysNum ).AirMassFlowRate );
+
+	// Second test - AlwaysOn Schedule - expecting flow
+	// Reset flows and switch to AlwaysOn Schedule
+	DataLoopNode::Node( InletNodeNum ).MassFlowRate = SysMinMassFlow;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRateMaxAvail = SysMaxMassFlow;
+	SingleDuct::Sys( SysNum ).SchedPtr = 2;
+	FirstHVACIteration = true;
+	SingleDuct::InitSys( SysNum, FirstHVACIteration ); // Run thru init once with FirstHVACIteration set to true
+	FirstHVACIteration = false;
+	SingleDuct::InitSys(SysNum, FirstHVACIteration); // Run thru init a second time with FirstHVACIteration set to false
+	SingleDuct::SimVAV( SysNum, FirstHVACIteration, ZoneNum, ZoneNodeNum );
+	EXPECT_EQ( SysMaxMassFlow, SingleDuct::SysOutlet( SysNum ).AirMassFlowRateMaxAvail );
+	EXPECT_EQ( SysMaxMassFlow, SingleDuct::SysOutlet( SysNum ).AirMassFlowRate );
+
+	// Cleanup
+	DataHeatBalFanSys::TempControlType.deallocate();
+	DataZoneEnergyDemands::ZoneSysEnergyDemand.deallocate();
+
+}
+
+TEST_F( EnergyPlusFixture, VAVReheatTerminalUnitSchedule ) {
+	std::string const idf_objects = delimited_string( {
+		"Version,8.4;",
+		"  Zone,",
+		"    Zone 1;                !- Name",
+		"ZoneHVAC:EquipmentConnections,",
+		"    Zone 1,                !- Zone Name",
+		"    Zone 1 Equipment,             !- Zone Conditioning Equipment List Name",
+		"    Zone 1 Supply Inlet,       !- Zone Air Inlet Node or NodeList Name",
+		"    ,      !- Zone Air Exhaust Node or NodeList Name",
+		"    Zone 1 Air Node,           !- Zone Air Node Name",
+		"    Zone 1 Return Node;       !- Zone Return Air Node Name",
+		"ZoneHVAC:EquipmentList,",
+		"    Zone 1 Equipment,             !- Name",
+		"    ZoneHVAC:AirDistributionUnit,  !- Zone Equipment 1 Object Type",
+		"    Zone 1 ADU,            !- Zone Equipment 1 Name",
+		"    1,                       !- Zone Equipment 1 Cooling Sequence",
+		"    1;                       !- Zone Equipment 1 Heating or No-Load Sequence",
+		"ZoneHVAC:AirDistributionUnit,",
+		"    Zone 1 ADU,    !- Name",
+		"    Zone 1 Supply Inlet,     !- Air Distribution Unit Outlet Node Name",
+		"    AirTerminal:SingleDuct:VAV:Reheat,  !- Air Terminal Object Type",
+		"    Zone 1 VAV Reheat;           !- Air Terminal Name",
+		"AirTerminal:SingleDuct:VAV:Reheat,",
+		"    Zone 1 VAV Reheat,       !- Name",
+		"    AlwaysOff,               !- Availability Schedule Name",
+		"    Zone 1 VAV Reheat Coil Air Inlet,  !- Damper Air Outlet Node Name",
+		"    Zone 1 Zone Equip Inlet, !- Air Inlet Node Name",
+		"    1.0,                     !- Maximum Air Flow Rate {m3/s}",
+		"    Constant,                !- Zone Minimum Air Flow Input Method",
+		"    0.25,                     !- Constant Minimum Air Flow Fraction",
+		"    ,                        !- Fixed Minimum Air Flow Rate{m3/s}",
+		"    ,                        !- Minimum Air Flow Fraction Schedule Name",
+		"    Coil:Heating:Electric,   !- Reheat Coil Object Type",
+		"    Zone 1 Reheat Coil,      !- Reheat Coil Name",
+		"    ,                        !- Maximum Hot Water or Steam Flow Rate{m3/s}",
+		"    ,                        !- Minimum Hot Water or Steam Flow Rate{m3/s}",
+		"    Zone 1 Supply Inlet;     !- Air Outlet Node Name",
+		"Coil:Heating:Electric,",
+		"    Zone 1 Reheat Coil,      !- Name",
+		"    ,                        !- Availability Schedule Name",
+		"    1,                       !- Efficiency",
+		"    100,                     !- Nominal Capacity of the Coil {W}",
+		"    Zone 1 VAV Reheat Coil Air Inlet,  !- Air Inlet Node Name",
+		"    Zone 1 Supply Inlet,     !- Air Outlet Node Name",
+		"    ;                        !- Temperature Setpoint Node Name",
+		"Schedule:Constant,",
+		"    AlwaysOff,               !- Name",
+		"    ,                        !- Schedule Type Limits Name",
+		"    0;                       !- Hourly Value",
+		"Schedule:Constant,",
+		"    AlwaysOn,               !- Name",
+		"    ,                        !- Schedule Type Limits Name",
+		"    1;                       !- Hourly Value",
+
+	} ) ;
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	DataGlobals::NumOfTimeStepInHour = 1; // must initialize this to get schedules initialized
+	DataGlobals::MinutesPerTimeStep = 60; // must initialize this to get schedules initialized
+	ScheduleManager::ProcessScheduleInput(); // read schedules
+	ScheduleManager::ScheduleInputProcessed = true;
+	DataEnvironment::Month = 1;
+	DataEnvironment::DayOfMonth = 21;
+	DataGlobals::HourOfDay = 1;
+	DataGlobals::TimeStep = 1;
+	DataEnvironment::DSTIndicator = 0;
+	DataEnvironment::DayOfWeek = 2;
+	DataEnvironment::HolidayIndex = 0;
+	DataEnvironment::DayOfYear_Schedule = General::JulianDay(DataEnvironment::Month, DataEnvironment::DayOfMonth, 1);
+	DataEnvironment::StdRhoAir = Psychrometrics::PsyRhoAirFnPbTdbW( 101325.0, 20.0, 0.0 ); 
+	ScheduleManager::UpdateScheduleValues();
+
+	bool ErrorsFound = false;
+	HeatBalanceManager::GetZoneData(ErrorsFound);
+	ASSERT_FALSE(ErrorsFound);
+	DataZoneEquipment::GetZoneEquipmentData1();
+	ZoneAirLoopEquipmentManager::GetZoneAirLoopEquipment();
+	SingleDuct::GetSysInput();
+	EXPECT_TRUE( compare_err_stream( "" ) );
+	DataHeatBalFanSys::TempControlType.allocate( 1 );
+	DataHeatBalFanSys::TempControlType( 1 ) = DataHVACGlobals::DualSetPointWithDeadBand;
+
+	// node number table
+	//  1   Zone 1 Air Node
+	//  2   Zone 1 Return Node
+	//  3   Zone 1 Supply Inlet
+	//  4   Zone 1 VAV Reheat Coil Air Inlet
+	//  5   Zone 1 Zone Equip Inlet
+
+	DataZoneEnergyDemands::ZoneSysEnergyDemand.allocate(1);
+
+	// Setup for Zone 1 VAV No Reheat
+	int SysNum = 1;
+	int ZoneNum = 1;
+	int ZoneNodeNum = 1;
+	int InletNodeNum = 5;
+	bool FirstHVACIteration = true;
+	Real64 SysMinMassFlow = 0.25 * DataEnvironment::StdRhoAir; // From inputs for Zone 1 VAV
+	Real64 SysMaxMassFlow = 1.0 * DataEnvironment::StdRhoAir; // From inputs for Zone 1 VAV
+
+	// Test with heating load
+	DataZoneEnergyDemands::ZoneSysEnergyDemand( 1 ).RemainingOutputRequired = 2000.0; // Heating load - expect min flow rate
+
+	// First test - AlwaysOff Schedule - expecting no flow
+	SingleDuct::Sys( SysNum ).SchedPtr = 1;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRate = SysMinMassFlow;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRateMaxAvail = SysMaxMassFlow;
+	DataGlobals::BeginEnvrnFlag = true; // Must be true for initial pass thru SingleDuct::InitSys for this terminal unit
+	FirstHVACIteration = true;
+	SingleDuct::InitSys( SysNum, FirstHVACIteration ); // Run thru init once with FirstHVACIteration set to true
+	DataGlobals::BeginEnvrnFlag = false;
+	FirstHVACIteration = false;
+	SingleDuct::InitSys(SysNum, FirstHVACIteration); // Run thru init a second time with FirstHVACIteration set to false
+	SingleDuct::SimVAV( SysNum, FirstHVACIteration, ZoneNum, ZoneNodeNum );
+	EXPECT_EQ( 0.0, SingleDuct::SysOutlet( SysNum ).AirMassFlowRateMaxAvail );
+	EXPECT_EQ( 0.0, SingleDuct::SysOutlet( SysNum ).AirMassFlowRate );
+
+	// Second test - AlwaysOn Schedule - expecting flow
+	// Reset flows and switch to AlwaysOn Schedule
+	DataLoopNode::Node( InletNodeNum ).MassFlowRate = SysMinMassFlow;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRateMaxAvail = SysMaxMassFlow;
+	SingleDuct::Sys( SysNum ).SchedPtr = 2;
+	FirstHVACIteration = true;
+	SingleDuct::InitSys( SysNum, FirstHVACIteration ); // Run thru init once with FirstHVACIteration set to true
+	FirstHVACIteration = false;
+	SingleDuct::InitSys(SysNum, FirstHVACIteration); // Run thru init a second time with FirstHVACIteration set to false
+	SingleDuct::SimVAV( SysNum, FirstHVACIteration, ZoneNum, ZoneNodeNum );
+	EXPECT_EQ( SysMaxMassFlow, SingleDuct::SysOutlet( SysNum ).AirMassFlowRateMaxAvail );
+	EXPECT_EQ( SysMinMassFlow, SingleDuct::SysOutlet( SysNum ).AirMassFlowRate );
+
+	// Test with cooling load
+	DataZoneEnergyDemands::ZoneSysEnergyDemand( 1 ).RemainingOutputRequired = -2000.0; // Cooling load - expect max flow rate
+
+	// First test - AlwaysOff Schedule - expecting no flow
+	SingleDuct::Sys( SysNum ).SchedPtr = 1;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRate = SysMinMassFlow;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRateMaxAvail = SysMaxMassFlow;
+	DataGlobals::BeginEnvrnFlag = true; // Must be true for initial pass thru SingleDuct::InitSys for this terminal unit
+	FirstHVACIteration = true;
+	SingleDuct::InitSys( SysNum, FirstHVACIteration ); // Run thru init once with FirstHVACIteration set to true
+	DataGlobals::BeginEnvrnFlag = false;
+	FirstHVACIteration = false;
+	SingleDuct::InitSys(SysNum, FirstHVACIteration); // Run thru init a second time with FirstHVACIteration set to false
+	SingleDuct::SimVAV( SysNum, FirstHVACIteration, ZoneNum, ZoneNodeNum );
+	EXPECT_EQ( 0.0, SingleDuct::SysOutlet( SysNum ).AirMassFlowRateMaxAvail );
+	EXPECT_EQ( 0.0, SingleDuct::SysOutlet( SysNum ).AirMassFlowRate );
+
+	// Second test - AlwaysOn Schedule - expecting flow
+	// Reset flows and switch to AlwaysOn Schedule
+	DataLoopNode::Node( InletNodeNum ).MassFlowRate = SysMinMassFlow;
+	DataLoopNode::Node( InletNodeNum ).MassFlowRateMaxAvail = SysMaxMassFlow;
+	SingleDuct::Sys( SysNum ).SchedPtr = 2;
+	FirstHVACIteration = true;
+	SingleDuct::InitSys( SysNum, FirstHVACIteration ); // Run thru init once with FirstHVACIteration set to true
+	FirstHVACIteration = false;
+	SingleDuct::InitSys(SysNum, FirstHVACIteration); // Run thru init a second time with FirstHVACIteration set to false
+	SingleDuct::SimVAV( SysNum, FirstHVACIteration, ZoneNum, ZoneNodeNum );
+	EXPECT_EQ( SysMaxMassFlow, SingleDuct::SysOutlet( SysNum ).AirMassFlowRateMaxAvail );
+	EXPECT_EQ( SysMaxMassFlow, SingleDuct::SysOutlet( SysNum ).AirMassFlowRate );
+
+	// Cleanup
+	DataHeatBalFanSys::TempControlType.deallocate();
+	DataZoneEnergyDemands::ZoneSysEnergyDemand.deallocate();
+
+}
diff --git a/tst/EnergyPlus/unit/SiteShallowGroundTemperatures.unit.cc b/tst/EnergyPlus/unit/SiteShallowGroundTemperatures.unit.cc
index 0a41b62a3fb..cd3f00fc957 100644
--- a/tst/EnergyPlus/unit/SiteShallowGroundTemperatures.unit.cc
+++ b/tst/EnergyPlus/unit/SiteShallowGroundTemperatures.unit.cc
@@ -69,7 +69,7 @@
 
 using namespace EnergyPlus;
 using namespace EnergyPlus::GroundTemperatureManager;
- 
+
 TEST_F( EnergyPlusFixture, SiteShallowGroundTempTest )
 {
 	std::string const idf_objects = delimited_string({
@@ -83,14 +83,14 @@ TEST_F( EnergyPlusFixture, SiteShallowGroundTempTest )
 		"	26.00,	!- June",
 		"	27.00,	!- July",
 		"	28.00,	!- August",
-		"	29.00,	!- Septeber",
+		"	29.00,	!- September",
 		"	30.00,	!- October",
 		"	31.00,	!- November",
 		"	32.00;	!- December",
 	});
 
 	ASSERT_FALSE( process_idf( idf_objects ) );
-	
+
 	std::string const CurrentModuleObject = CurrentModuleObjects( objectType_SiteShallowGroundTemp );
 
 	auto thisModel = GetGroundTempModelAndInit( CurrentModuleObject, "TEST" );
diff --git a/tst/EnergyPlus/unit/SurfaceGeometry.unit.cc b/tst/EnergyPlus/unit/SurfaceGeometry.unit.cc
index 50ba0651a83..54abb3f79cc 100644
--- a/tst/EnergyPlus/unit/SurfaceGeometry.unit.cc
+++ b/tst/EnergyPlus/unit/SurfaceGeometry.unit.cc
@@ -118,7 +118,7 @@ TEST_F( EnergyPlusFixture, BaseSurfaceRectangularTest )
 
 	ProcessSurfaceVertices( ThisSurf, ErrorsFound );
 	EXPECT_FALSE( ErrorsFound );
-	EXPECT_EQ( Rectangle, Surface( ThisSurf ).Shape );
+	EXPECT_EQ( SurfaceShape::Rectangle, Surface( ThisSurf ).Shape );
 
 	// Surface 2 - Isosceles Trapezoid
 	ThisSurf = 2;
@@ -145,7 +145,7 @@ TEST_F( EnergyPlusFixture, BaseSurfaceRectangularTest )
 
 	ProcessSurfaceVertices( ThisSurf, ErrorsFound );
 	EXPECT_FALSE( ErrorsFound );
-	EXPECT_EQ( Quadrilateral, Surface( ThisSurf ).Shape );
+	EXPECT_EQ( SurfaceShape::Quadrilateral, Surface( ThisSurf ).Shape );
 
 	// Surface 3 - Parallelogram
 	ThisSurf = 3;
@@ -172,7 +172,7 @@ TEST_F( EnergyPlusFixture, BaseSurfaceRectangularTest )
 
 	ProcessSurfaceVertices( ThisSurf, ErrorsFound );
 	EXPECT_FALSE( ErrorsFound );
-	EXPECT_EQ( Quadrilateral, Surface( ThisSurf ).Shape );
+	EXPECT_EQ( SurfaceShape::Quadrilateral, Surface( ThisSurf ).Shape );
 
 	// Surface 4 - Triangle
 	ThisSurf = 4;
@@ -195,7 +195,7 @@ TEST_F( EnergyPlusFixture, BaseSurfaceRectangularTest )
 
 	ProcessSurfaceVertices( ThisSurf, ErrorsFound );
 	EXPECT_FALSE( ErrorsFound );
-	EXPECT_EQ( Triangle, Surface( ThisSurf ).Shape );
+	EXPECT_EQ( SurfaceShape::Triangle, Surface( ThisSurf ).Shape );
 
 	// Surface 5 - Polygon
 	ThisSurf = 5;
@@ -226,7 +226,341 @@ TEST_F( EnergyPlusFixture, BaseSurfaceRectangularTest )
 
 	ProcessSurfaceVertices( ThisSurf, ErrorsFound );
 	EXPECT_FALSE( ErrorsFound );
-	EXPECT_EQ( Polygonal, Surface( ThisSurf ).Shape );
+	EXPECT_EQ( SurfaceShape::Polygonal, Surface( ThisSurf ).Shape );
+}
+
+TEST_F( EnergyPlusFixture, DataSurfaces_SurfaceShape )
+{
+
+	bool ErrorsFound( false );
+
+	std::string const idf_objects = delimited_string({
+		"Version,",
+		"    8.4;                     !- Version Identifier",
+
+		" BuildingSurface:Detailed,",
+		"    Surface 1 - Triangle,    !- Name",
+		"    Floor,                   !- Surface Type",
+		"    ExtSlabCarpet 4in ClimateZone 1-8,  !- Construction Name",
+		"    Zone1,                   !- Zone Name",
+		"    Outdoors,                !- Outside Boundary Condition",
+		"    ,                        !- Outside Boundary Condition Object",
+		"    NoSun,                   !- Sun Exposure",
+		"    NoWind,                  !- Wind Exposure",
+		"    ,                        !- View Factor to Ground",
+		"    ,                        !- Number of Vertices",
+		"    0.0, 0.0, 0.0,           !- Vertex 1 X-coordinate {m}",
+		"    1.0, 2.0, 0.0,           !- Vertex 2 X-coordinate {m}",
+		"    2.0, 0.0, 0.0;           !- Vertex 3 X-coordinate {m}",
+
+		" BuildingSurface:Detailed,",
+		"    Surface 2 - Quadrilateral,  !- Name",
+		"    Floor,                   !- Surface Type",
+		"    ExtSlabCarpet 4in ClimateZone 1-8,  !- Construction Name",
+		"    Zone1,                   !- Zone Name",
+		"    Outdoors,                !- Outside Boundary Condition",
+		"    ,                        !- Outside Boundary Condition Object",
+		"    NoSun,                   !- Sun Exposure",
+		"    NoWind,                  !- Wind Exposure",
+		"    ,                        !- View Factor to Ground",
+		"    ,                        !- Number of Vertices",
+		"    -73.4395447868102,       !- Vertex 1 X-coordinate {m}",
+		"    115.81641271866,         !- Vertex 1 Y-coordinate {m}",
+		"    -4.90860981523342e-014,  !- Vertex 1 Z-coordinate {m}",
+		"    -58.0249751030646,       !- Vertex 2 X-coordinate {m}",
+		"    93.1706338416311,        !- Vertex 2 Y-coordinate {m}",
+		"    -6.93120848813091e-014,  !- Vertex 2 Z-coordinate {m}",
+		"    -68.9295447868101,       !- Vertex 3 X-coordinate {m}",
+		"    74.3054685889134,        !- Vertex 3 Y-coordinate {m}",
+		"    -6.06384403665968e-014,  !- Vertex 3 Z-coordinate {m}",
+		"    -58.0345461881513,       !- Vertex 4 X-coordinate {m}",
+		"    93.1761597101821,        !- Vertex 4 Y-coordinate {m}",
+		"    -6.9300904918858e-014;   !- Vertex 4 Z-coordinate {m}",
+
+		" BuildingSurface:Detailed,",
+		"    Surface 3 - Rectangle,   !- Name",
+		"    Wall,                    !- Surface Type",
+		"    ExtSlabCarpet 4in ClimateZone 1-8,  !- Construction Name",
+		"    Zone1,                   !- Zone Name",
+		"    Outdoors,                !- Outside Boundary Condition",
+		"    ,                        !- Outside Boundary Condition Object",
+		"    NoSun,                   !- Sun Exposure",
+		"    NoWind,                  !- Wind Exposure",
+		"    ,                        !- View Factor to Ground",
+		"    ,                        !- Number of Vertices",
+		"    0.0, 0.0, 0.0,           !- X,Y,Z ==> Vertex 1 {m}",
+		"    1.0, 0.0, 0.0,           !- X,Y,Z ==> Vertex 2 {m}",
+		"    1.0, 0.0, 1.0,           !- X,Y,Z ==> Vertex 3 {m}",
+		"    0.0, 0.0, 1.0;           !- X,Y,Z ==> Vertex 4 {m}",
+
+		" FenestrationSurface:Detailed,",
+		"    Surface 4 - RectangularDoorWindow,    !- Name",
+		"    Window,                  !- Surface Type",
+		"    SINGLE PANE HW WINDOW,   !- Construction Name",
+		"    Surface 3 - Rectangle,   !- Building Surface Name",
+		"    ,                        !- Outside Boundary Condition Object",
+		"    0.0,                     !- View Factor to Ground",
+		"    ,                        !- Shading Control Name",
+		"    ,                        !- Frame and Divider Name",
+		"    1.0,                     !- Multiplier",
+		"    Autocalculate,           !- Number of Vertices",
+		"    0.2, 0.0, 0.2,           !- X,Y,Z ==> Vertex 1 {m}",
+		"    0.8, 0.0, 0.2,           !- X,Y,Z ==> Vertex 2 {m}",
+		"    0.8, 0.0, 0.8,           !- X,Y,Z ==> Vertex 3 {m}",
+		"    0.2, 0.0, 0.8;           !- X,Y,Z ==> Vertex 4 {m}",
+
+		" Shading:Overhang:Projection,",
+		"    Surface 5 - RectangularOverhang,  !- Name",
+		"    Surface 9 - TriangularDoor,       !- Window or Door Name",
+		"    .01,                     !- Height above Window or Door {m}",
+		"    91,                      !- Tilt Angle from Window/Door {deg}",
+		"    .01,                     !- Left extension from Window/Door Width {m}",
+		"    .01,                     !- Right extension from Window/Door Width {m}",
+		"    .2;                      !- Depth as Fraction of Window/Door Height {dimensionless}",
+
+		" Shading:Fin:Projection,",
+		"    Surface 6 - RectangularLeftFin,    !- Name",
+		"    Surface 3 - Rectangle,   !- Window or Door Name",
+		"    .01,                     !- Left Extension from Window/Door {m}",
+		"    .01,                     !- Left Distance Above Top of Window {m}",
+		"    .01,                     !- Left Distance Below Bottom of Window {m}",
+		"    90,                      !- Left Tilt Angle from Window/Door {deg}",
+		"    .1,                      !- Left Depth as Fraction of Window/Door Width {dimensionless}",
+		"    0,                       !- Right Extension from Window/Door {m}",
+		"    0,                       !- Right Distance Above Top of Window {m}",
+		"    0,                       !- Right Distance Below Bottom of Window {m}",
+		"    0,                       !- Right Tilt Angle from Window/Door {deg}",
+		"    0;                       !- Right Depth as Fraction of Window/Door Width {dimensionless}",
+
+		" Shading:Fin:Projection,",
+		"    Surface 7 - RectangularRightFin,   !- Name",
+		"    Surface 3 - Rectangle,   !- Window or Door Name",
+		"    0,                       !- Left Extension from Window/Door {m}",
+		"    0,                       !- Left Distance Above Top of Window {m}",
+		"    0,                       !- Left Distance Below Bottom of Window {m}",
+		"    0,                       !- Left Tilt Angle from Window/Door {deg}",
+		"    0,                       !- Left Depth as Fraction of Window/Door Width {dimensionless}",
+		"    .01,                     !- Right Extension from Window/Door {m}",
+		"    .01,                     !- Right Distance Above Top of Window {m}",
+		"    .01,                     !- Right Distance Below Bottom of Window {m}",
+		"    90,                      !- Right Tilt Angle from Window/Door {deg}",
+		"    .1;                      !- Right Depth as Fraction of Window/Door Width {dimensionless}",
+
+		" FenestrationSurface:Detailed,",
+		"    Surface 8 - TriangularWindow,    !- Name",
+		"    Window,                  !- Surface Type",
+		"    SINGLE PANE HW WINDOW,   !- Construction Name",
+		"    Surface 3 - Rectangle,   !- Building Surface Name",
+		"    ,                        !- Outside Boundary Condition Object",
+		"    0.0,                     !- View Factor to Ground",
+		"    ,                        !- Shading Control Name",
+		"    ,                        !- Frame and Divider Name",
+		"    1.0,                     !- Multiplier",
+		"    Autocalculate,           !- Number of Vertices",
+		"    0.05, 0.0, 0.05,         !- X,Y,Z ==> Vertex 1 {m}",
+		"    0.15, 0.0, 0.05,         !- X,Y,Z ==> Vertex 2 {m}",
+		"    0.10, 0.0, 0.15;         !- X,Y,Z ==> Vertex 3 {m}",
+
+		" FenestrationSurface:Detailed,",
+		"    Surface 9 - TriangularDoor,      !- Name",
+		"    Door,                    !- Surface Type",
+		"    External door,           !- Construction Name",
+		"    Surface 3 - Rectangle,   !- Building Surface Name",
+		"    ,                        !- Outside Boundary Condition Object",
+		"    0.5,                     !- View Factor to Ground",
+		"    ,                        !- Shading Control Name",
+		"    ,                        !- Frame and Divider Name",
+		"    1,                       !- Multiplier",
+		"    3,                       !- Number of Vertices",
+		"    0.80, 0.0, 0.05,         !- X,Y,Z ==> Vertex 1 {m}",
+		"    0.95, 0.0, 0.05,         !- X,Y,Z ==> Vertex 2 {m}",
+		"    0.90, 0.0, 0.15;         !- X,Y,Z ==> Vertex 3 {m}",
+
+
+		" BuildingSurface:Detailed,",
+		"    Surface 10 - Polygonal,  !- Name",
+		"    Floor,                   !- Surface Type",
+		"    ExtSlabCarpet 4in ClimateZone 1-8,  !- Construction Name",
+		"    Zone1,                   !- Zone Name",
+		"    Outdoors,                !- Outside Boundary Condition",
+		"    ,                        !- Outside Boundary Condition Object",
+		"    NoSun,                   !- Sun Exposure",
+		"    NoWind,                  !- Wind Exposure",
+		"    ,                        !- View Factor to Ground",
+		"    ,                        !- Number of Vertices",
+		"    0.0, 0.0, 0.0,           !- Vertex 1 X-coordinate {m}",
+		"    0.0, 1.0, 0.0,           !- Vertex 2 X-coordinate {m}",
+		"    0.5, 2.0, 0.0,           !- Vertex 3 X-coordinate {m}",
+		"    1.0, 1.0, 0.0,           !- Vertex 4 X-coordinate {m}",
+		"    1.0, 0.0, 0.0;           !- Vertex 5 X-coordinate {m}",
+
+		" Zone,",
+		"    Zone1,                   !- Name",
+		"    0,                       !- Direction of Relative North {deg}",
+		"    0.0,                     !- X Origin {m}",
+		"    0.0,                     !- Y Origin {m}",
+		"    0.0,                     !- Z Origin {m}",
+		"    ,                        !- Type",
+		"    ,                        !- Multiplier",
+		"    ,                        !- Ceiling Height {m}",
+		"    ,                        !- Volume {m3}",
+		"    ,                        !- Floor Area {m2}",
+		"    ,                        !- Zone Inside Convection Algorithm",
+		"    ,                        !- Zone Outside Convection Algorithm",
+		"    No;                      !- Part of Total Floor Area",
+
+		" Construction,",
+		"    ExtSlabCarpet 4in ClimateZone 1-8,  !- Name",
+		"    MAT-CC05 4 HW CONCRETE,  !- Outside Layer",
+		"    CP02 CARPET PAD;         !- Layer 2",
+
+		" Construction,",
+		"    External door,           !- Name",
+		"    Painted Oak;             !- Outside Layer",
+	
+		" Material,",
+		"    MAT-CC05 4 HW CONCRETE,  !- Name",
+		"    Rough,                   !- Roughness",
+		"    0.1016,                  !- Thickness {m}",
+		"    1.311,                   !- Conductivity {W/m-K}",
+		"    2240,                    !- Density {kg/m3}",
+		"    836.800000000001,        !- Specific Heat {J/kg-K}",
+		"    0.9,                     !- Thermal Absorptance",
+		"    0.85,                    !- Solar Absorptance",
+		"    0.85;                    !- Visible Absorptance",
+
+		" Material,",
+		"    Painted Oak,             !- Name",
+		"    Rough,                   !- Roughness",
+		"    0.035,                   !- Thickness {m}",
+		"    0.19,                    !- Conductivity {W/m-K}",
+		"    700,                     !- Density {kg/m3}",
+		"    2390,                    !- Specific Heat {J/kg-K}",
+		"    0.9,                     !- Thermal Absorptance",
+		"    0.5,                     !- Solar Absorptance",
+		"    0.5;                     !- Visible Absorptance",
+
+		" Material:NoMass,",
+		"    CP02 CARPET PAD,         !- Name",
+		"    Smooth,                  !- Roughness",
+		"    0.1,                     !- Thermal Resistance {m2-K/W}",
+		"    0.9,                     !- Thermal Absorptance",
+		"    0.8,                     !- Solar Absorptance",
+		"    0.8;                     !- Visible Absorptance",
+
+		" Construction,",
+		"    SINGLE PANE HW WINDOW,   !- Name",
+		"    GLASS - CLEAR PLATE 1 / 4 IN;  !- Outside Layer",
+
+		" WindowMaterial:Glazing,",
+		"    GLASS - CLEAR PLATE 1 / 4 IN,  !- Name",
+		"    SpectralAverage,         !- Optical Data Type",
+		"    ,                        !- Window Glass Spectral Data Set Name",
+		"    6.0000001E-03,           !- Thickness {m}",
+		"    0.7750000,               !- Solar Transmittance at Normal Incidence",
+		"    7.1000002E-02,           !- Front Side Solar Reflectance at Normal Incidence",
+		"    7.1000002E-02,           !- Back Side Solar Reflectance at Normal Incidence",
+		"    0.8810000,               !- Visible Transmittance at Normal Incidence",
+		"    7.9999998E-02,           !- Front Side Visible Reflectance at Normal Incidence",
+		"    7.9999998E-02,           !- Back Side Visible Reflectance at Normal Incidence",
+		"    0,                       !- Infrared Transmittance at Normal Incidence",
+		"    0.8400000,               !- Front Side Infrared Hemispherical Emissivity",
+		"    0.8400000,               !- Back Side Infrared Hemispherical Emissivity",
+		"    0.9000000;               !- Conductivity {W/m-K}",
+
+		"SurfaceConvectionAlgorithm:Inside,TARP;",
+
+		"SurfaceConvectionAlgorithm:Outside,DOE-2;",
+
+		"HeatBalanceAlgorithm,ConductionTransferFunction;",
+
+		"ZoneAirHeatBalanceAlgorithm,",
+		"    AnalyticalSolution;      !- Algorithm",
+
+		});
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	GetProjectControlData( ErrorsFound ); // read project control data
+	EXPECT_FALSE( ErrorsFound ); // expect no errors
+
+	GetMaterialData( ErrorsFound ); // read material data
+	EXPECT_FALSE( ErrorsFound ); // expect no errors
+
+	GetConstructData( ErrorsFound ); // read construction data
+	EXPECT_FALSE( ErrorsFound ); // expect no errors
+
+	GetZoneData( ErrorsFound ); // read zone data
+	EXPECT_FALSE( ErrorsFound ); // expect no errors
+
+	CosZoneRelNorth.allocate( 1 );
+	SinZoneRelNorth.allocate( 1 );
+
+	CosZoneRelNorth( 1 ) = std::cos( -Zone( 1 ).RelNorth * DataGlobals::DegToRadians );
+	SinZoneRelNorth( 1 ) = std::sin( -Zone( 1 ).RelNorth * DataGlobals::DegToRadians );
+	CosBldgRelNorth = 1.0;
+	SinBldgRelNorth = 0.0;
+
+	GetSurfaceData( ErrorsFound ); // setup zone geometry and get zone data
+	EXPECT_FALSE( ErrorsFound ); // expect no errors
+
+	//compare_err_stream( "" ); // just for debugging
+
+	AllocateModuleArrays();
+
+//  Adding additional surfaces will change the index of the following based on where the surfaces are added in the array.
+//	If adding new tests, break here and look at EnergyPlus::DataSurfaces::Surface to see the order.
+
+//	enum surfaceShape:Triangle = 1
+//	Surface( 11 ).Name = "Surface 1 - Triangle"
+	ProcessSurfaceVertices( 11, ErrorsFound );
+	EXPECT_EQ( SurfaceShape::Triangle, Surface( 11 ).Shape );
+
+//	enum surfaceShape:Quadrilateral = 2
+//	Surface( 12 ).Name = "Surface 2 - Quadrilateral"
+	ProcessSurfaceVertices( 12, ErrorsFound );
+	EXPECT_EQ( SurfaceShape::Quadrilateral, Surface( 12 ).Shape );
+
+//	enum surfaceShape:Rectangle = 3
+//	Surface( 7 ).Name = "Surface 3 - Rectangle"
+	ProcessSurfaceVertices( 7, ErrorsFound );
+	EXPECT_EQ( SurfaceShape::Rectangle, Surface( 7 ).Shape );
+
+//	enum surfaceShape:RectangularDoorWindow = 4
+//	Surface( 8 ).Name = "Surface 4 - RectangularDoorWindow"
+	ProcessSurfaceVertices( 8, ErrorsFound );
+	EXPECT_EQ( SurfaceShape::RectangularDoorWindow, Surface( 8 ).Shape );
+
+//	enum surfaceShape:RectangularOverhang = 5
+//	Surface( 1 ).Name = "Surface 5 - RectangularOverhang"
+	ProcessSurfaceVertices( 1, ErrorsFound );
+	EXPECT_NE( SurfaceShape::RectangularOverhang, Surface( 1 ).Shape ); // fins and overhangs will not get set to the proper surface shape.
+
+//	enum surfaceShape:RectangularLeftFin = 6
+//	Surface( 3 ).Name = "Surface 6 - RectangularLeftFin"
+	ProcessSurfaceVertices( 3, ErrorsFound );
+	EXPECT_NE( SurfaceShape::RectangularLeftFin, Surface( 3 ).Shape ); // fins and overhangs will not get set to the proper surface shape.
+
+//	enum surfaceShape:RectangularRightFin = 7
+//	Surface( 5 ).Name = "Surface 7 - RectangularRightFin"
+	ProcessSurfaceVertices( 5, ErrorsFound );
+	EXPECT_NE( SurfaceShape::RectangularRightFin, Surface( 5 ).Shape ); // fins and overhangs will not get set to the proper surface shape.
+
+//	enum surfaceShape:TriangularWindow = 8
+//	Surface( 9 ).Name = "Surface 8 - TriangularWindow"
+	ProcessSurfaceVertices( 9, ErrorsFound );
+	EXPECT_EQ( SurfaceShape::TriangularWindow, Surface( 9 ).Shape );
+
+//	enum surfaceShape:TriangularDoor = 9
+//	Surface( 10 ).Name = "Surface 9 - TriangularDoor"
+	ProcessSurfaceVertices( 10, ErrorsFound );
+	EXPECT_EQ( SurfaceShape::TriangularDoor, Surface( 10 ).Shape );
+
+//	enum surfaceShape:Polygonal = 10
+//	Surface( 13 ).Name = "Surface 10 - Polygonal"
+	ProcessSurfaceVertices( 13, ErrorsFound );
+	EXPECT_EQ( SurfaceShape::Polygonal, Surface( 13 ).Shape );
+
 }
 
 TEST_F( EnergyPlusFixture, ConfirmCheckSubSurfAzTiltNorm )
diff --git a/tst/EnergyPlus/unit/SurfaceOctree.unit.cc b/tst/EnergyPlus/unit/SurfaceOctree.unit.cc
index d9b77bc9e8b..554c96a8141 100644
--- a/tst/EnergyPlus/unit/SurfaceOctree.unit.cc
+++ b/tst/EnergyPlus/unit/SurfaceOctree.unit.cc
@@ -305,7 +305,7 @@ TEST( SurfaceOctreeTest, Composite )
 	Surface( 10 ).Vertex = { Vertex(1,0,0), Vertex(1,1,0), Vertex(1,1,1), Vertex(1,0,1) };
 	Surface( 11 ).Vertex = { Vertex(0,0,0), Vertex(1,0,0), Vertex(1,1,0), Vertex(0,1,0) };
 	Surface( 12 ).Vertex = { Vertex(0,0,1), Vertex(1,0,1), Vertex(1,1,1), Vertex(0,1,1) };
-	for ( int i = 1; i <= TotSurfaces; ++i ) Surface( i ).Shape = Rectangle;
+	for ( int i = 1; i <= TotSurfaces; ++i ) Surface( i ).Shape = SurfaceShape::Rectangle;
 
 	// SurfaceOctreeCube
 	SurfaceOctreeCube const cube( Surface );
@@ -408,19 +408,19 @@ TEST( SurfaceOctreeTest, Composite )
 	// Function processing
 	{ // Hits cube but predicate never satisfied
 		Vertex const a( -1.0, 0.5, 0.5 ), b( 3.0, 0.5, 0.5 ), dir( ( b - a ).normalize_zero() );
-		auto predicate = []( SurfaceData const & surface ) -> bool { return surface.Shape == Triangle; };
+		auto predicate = []( SurfaceData const & surface ) -> bool { return surface.Shape == SurfaceShape::Triangle; };
 		EXPECT_FALSE( cube.hasSurfaceSegmentIntersectsCube( a, b, predicate ) );
 		EXPECT_FALSE( cube.hasSurfaceRayIntersectsCube( a, dir, predicate ) );
 	}
 	{ // Hits cube and predicate satisfied
 		Vertex const a( -1.0, 0.5, 0.5 ), b( 3.0, 0.5, 0.5 ), dir( ( b - a ).normalize_zero() );
-		auto predicate = []( SurfaceData const & surface ) -> bool { return surface.Shape == Rectangle; };
+		auto predicate = []( SurfaceData const & surface ) -> bool { return surface.Shape == SurfaceShape::Rectangle; };
 		EXPECT_TRUE( cube.hasSurfaceSegmentIntersectsCube( a, b, predicate ) );
 		EXPECT_TRUE( cube.hasSurfaceRayIntersectsCube( a, dir, predicate ) );
 	}
 	{ // Misses cube so predicate never tested
 		Vertex const a( -1.0, 3.0, 3.0 ), b( 3.0, 3.0, 3.0 ), dir( ( b - a ).normalize_zero() );
-		auto predicate = []( SurfaceData const & surface ) -> bool { return surface.Shape == Rectangle; };
+		auto predicate = []( SurfaceData const & surface ) -> bool { return surface.Shape == SurfaceShape::Rectangle; };
 		EXPECT_FALSE( cube.hasSurfaceSegmentIntersectsCube( a, b, predicate ) );
 		EXPECT_FALSE( cube.hasSurfaceRayIntersectsCube( a, dir, predicate ) );
 	}
diff --git a/tst/EnergyPlus/unit/ThermalComfort.unit.cc b/tst/EnergyPlus/unit/ThermalComfort.unit.cc
index d43d0a5793e..5dc01914a16 100644
--- a/tst/EnergyPlus/unit/ThermalComfort.unit.cc
+++ b/tst/EnergyPlus/unit/ThermalComfort.unit.cc
@@ -68,25 +68,35 @@
 #include "Fixtures/EnergyPlusFixture.hh"
 #include <EnergyPlus/ThermalComfort.hh>
 #include <EnergyPlus/UtilityRoutines.hh>
+#include <EnergyPlus/DataEnvironment.hh>
 #include <EnergyPlus/DataGlobals.hh>
 #include <EnergyPlus/DataZoneEnergyDemands.hh>
+#include <EnergyPlus/DataHeatBalance.hh>
 #include <EnergyPlus/DataHeatBalFanSys.hh>
 #include <EnergyPlus/DataHVACGlobals.hh>
 #include <EnergyPlus/DataRoomAirModel.hh>
+#include <EnergyPlus/InternalHeatGains.hh>
+#include <EnergyPlus/HeatBalanceManager.hh>
+#include <EnergyPlus/OutputProcessor.hh>
+#include <EnergyPlus/ScheduleManager.hh>
+#include <EnergyPlus/SimulationManager.hh>
 
 using namespace EnergyPlus;
 using namespace EnergyPlus::ThermalComfort;
+using namespace EnergyPlus::DataEnvironment;
 using namespace EnergyPlus::DataGlobals;
+using namespace EnergyPlus::DataHeatBalance;
 using namespace EnergyPlus::DataHVACGlobals;
+using namespace EnergyPlus::DataRoomAirModel;
+using namespace EnergyPlus::DataHeatBalFanSys;
+using namespace EnergyPlus::InternalHeatGains;
+using namespace EnergyPlus::HeatBalanceManager;
+using namespace EnergyPlus::OutputProcessor;
+using namespace EnergyPlus::ScheduleManager;
+using namespace SimulationManager;
 using namespace ObjexxFCL;
 
 using DataZoneEnergyDemands::ZoneSysEnergyDemand;
-using DataHeatBalFanSys::TempControlType;
-using DataRoomAirModel::AirModel;
-using DataRoomAirModel::RoomAirModel_Mixing;
-using DataHeatBalFanSys::ZTAV;
-using DataHeatBalFanSys::ZoneThermostatSetPointLo;
-using DataHeatBalFanSys::ZoneThermostatSetPointHi;
 
 
 TEST_F( EnergyPlusFixture, ThermalComfort_CalcIfSetPointMetTest1 )
@@ -200,3 +210,557 @@ TEST_F( EnergyPlusFixture, ThermalComfort_CalcIfSetPointMetTest1 )
 	EXPECT_EQ( TimeStepZone, ThermalComfortSetPoint( 1 ).notMetCooling );
 	EXPECT_EQ( TimeStepZone, ThermalComfortSetPoint( 1 ).notMetCoolingOccupied );
 }
+
+TEST_F( EnergyPlusFixture, ThermalComfort_CalcThermalComfortFanger )
+{
+
+	std::string const idf_objects = delimited_string( {
+		"Version,8.3;",
+		"  People,                                                                 ",
+		"    Space People,   !- Name                                      ",
+		"    Space,     !- Zone or ZoneList Name                     ",
+		"    PeopleSchedule,          !- Number of People Schedule Name            ",
+		"    People,                  !- Number of People Calculation Method       ",
+		"    5.0,                     !- Number of People                          ",
+		"    ,                        !- People per Zone Floor Area {person/m2}    ",
+		"    ,                        !- Zone Floor Area per Person {m2/person}    ",
+		"    0.3,                     !- Fraction Radiant                          ",
+		"    AUTOCALCULATE,           !- Sensible Heat Fraction                    ",
+		"    Activity Schedule,       !- Activity Level Schedule Name              ",
+		"    ,                        !- Carbon Dioxide Generation Rate {m3/s-W}   ",
+		"    Yes,                     !- Enable ASHRAE 55 Comfort Warnings         ",
+		"    ZoneAveraged,            !- Mean Radiant Temperature Calculation Type ",
+		"    ,                        !- Surface Name/Angle Factor List Name       ",
+		"    Work efficiency,         !- Work Efficiency Schedule Name             ",
+		"    ClothingInsulationSchedule,  !- Clothing Insulation Calculation Method",
+		"    ,                        !- Clothing Insulation Calculation Method Sch",
+		"    Clothing Schedule,       !- Clothing Insulation Schedule Name         ",
+		"    AirVelocitySchedule,     !- Air Velocity Schedule Name                ",
+		"    Fanger;                  !- Thermal Comfort Model 1 Type              ",
+		"                                                                          ",
+		"  Schedule:Compact,                                                       ",
+		"    PeopleSchedule,          !- Name                                      ",
+		"    Any Number,              !- Schedule Type Limits Name                 ",
+		"    Through: 12/30,          !- Field 1                                   ",
+		"    For: AllDays,            !- Field 2                                   ",
+		"    Until: 24:00,1.0,        !- Field 3                                   ",
+		"    Through: 12/31,          !- Field 1                                   ",
+		"    For: AllDays,            !- Field 2                                   ",
+		"    Until: 24:00,0.3;        !- Field 3                                   ",
+		"                                                                          ",
+		"  Schedule:Compact,                                                       ",
+		"    Activity Schedule,       !- Name                                      ",
+		"    Any Number,              !- Schedule Type Limits Name                 ",
+		"    Through: 12/31,          !- Field 1                                   ",
+		"    For: AllDays,            !- Field 2                                   ",
+		"    Until: 24:00,70;         !- Field 3                                   ",
+		"                                                                          ",
+		"  Schedule:Compact,                                                       ",
+		"    Clothing Schedule,       !- Name                                      ",
+		"    Any Number,              !- Schedule Type Limits Name                 ",
+		"    Through: 12/31,          !- Field 9                                   ",
+		"    For: AllDays,            !- Field 10                                  ",
+		"    Until: 24:00,1.0;         !- Field 11                                 ",
+		"                                                                          ",
+		"  Schedule:Compact,                                                       ",
+		"    AirVelocitySchedule,     !- Name                                      ",
+		"    Any Number,              !- Schedule Type Limits Name                 ",
+		"    Through: 12/31,          !- Field 1                                   ",
+		"    For: AllDays,            !- Field 2                                   ",
+		"    Until: 24:00,0.0;        !- Field 3                                   ",
+		"                                                                          ",
+		"  Schedule:Compact,                                                       ",
+		"    Work efficiency,         !- Name                                      ",
+		"    Any Number,              !- Schedule Type Limits Name                 ",
+		"    Through: 12/31,          !- Field 9                                   ",
+		"    For: AllDays,            !- Field 10                                  ",
+		"    Until: 24:00,0.0;         !- Field 11                                 ",
+		"                                                                          ",
+		" Output:Diagnostics, DisplayExtraWarnings;",
+		" Timestep, 4;",
+		" BUILDING, AirloopHVAC_VentilationRateProcedure, 0.0, Suburbs, .04, .4, FullExterior, 25, 6;",
+		" SimulationControl, NO, NO, NO, YES, NO;",
+		"ScheduleTypeLimits,",
+		"  Any Number;              !- Name",
+		"  Site:Location,",
+		"    Miami Intl Ap FL USA TMY3 WMO=722020E,    !- Name",
+		"    25.82,                 !- Latitude {deg}",
+		"    -80.30,                !- Longitude {deg}",
+		"    -5.00,                 !- Time Zone {hr}",
+		"    11;                    !- Elevation {m}",
+
+		"SizingPeriod:DesignDay,",
+		" Miami Intl Ap Ann Clg .4% Condns DB/MCWB, !- Name",
+		" 7,                        !- Month",
+		" 21,                       !- Day of Month",
+		" SummerDesignDay,          !- Day Type",
+		" 31.7,                     !- Maximum Dry - Bulb Temperature{ C }",
+		" 10.0,                      !- Daily Dry - Bulb Temperature Range{ deltaC }",
+		" ,                         !- Dry - Bulb Temperature Range Modifier Type",
+		" ,                         !- Dry - Bulb Temperature Range Modifier Day Schedule Name",
+		" Wetbulb,                  !- Humidity Condition Type",
+		" 22.7,                     !- Wetbulb or DewPoint at Maximum Dry - Bulb{ C }",
+		" ,                         !- Humidity Condition Day Schedule Name",
+		" ,                         !- Humidity Ratio at Maximum Dry - Bulb{ kgWater / kgDryAir }",
+		" ,                         !- Enthalpy at Maximum Dry - Bulb{ J / kg }",
+		" ,                         !- Daily Wet - Bulb Temperature Range{ deltaC }",
+		" 101217.,                  !- Barometric Pressure{ Pa }",
+		" 3.8,                      !- Wind Speed{ m / s }",
+		" 340,                      !- Wind Direction{ deg }",
+		" No,                       !- Rain Indicator",
+		" No,                       !- Snow Indicator",
+		" No,                       !- Daylight Saving Time Indicator",
+		" ASHRAEClearSky,           !- Solar Model Indicator",
+		" ,                         !- Beam Solar Day Schedule Name",
+		" ,                         !- Diffuse Solar Day Schedule Name",
+		" ,                         !- ASHRAE Clear Sky Optical Depth for Beam Irradiance( taub ) { dimensionless }",
+		" ,                         !- ASHRAE Clear Sky Optical Depth for Diffuse Irradiance( taud ) { dimensionless }",
+		" 1.00;                     !- Sky Clearness",
+
+		"SizingPeriod:DesignDay,",
+		" Miami Intl Ap Ann Htg 99.6% Condns DB, !- Name",
+		" 1,                        !- Month",
+		" 21,                       !- Day of Month",
+		" WinterDesignDay,          !- Day Type",
+		" 8.7,                      !- Maximum Dry - Bulb Temperature{ C }",
+		" 0.0,                      !- Daily Dry - Bulb Temperature Range{ deltaC }",
+		" ,                         !- Dry - Bulb Temperature Range Modifier Type",
+		" ,                         !- Dry - Bulb Temperature Range Modifier Day Schedule Name",
+		" Wetbulb,                  !- Humidity Condition Type",
+		" 8.7,                      !- Wetbulb or DewPoint at Maximum Dry - Bulb{ C }",
+		" ,                         !- Humidity Condition Day Schedule Name",
+		" ,                         !- Humidity Ratio at Maximum Dry - Bulb{ kgWater / kgDryAir }",
+		" ,                         !- Enthalpy at Maximum Dry - Bulb{ J / kg }",
+		" ,                         !- Daily Wet - Bulb Temperature Range{ deltaC }",
+		" 101217.,                  !- Barometric Pressure{ Pa }",
+		" 3.8,                      !- Wind Speed{ m / s }",
+		" 340,                      !- Wind Direction{ deg }",
+		" No,                       !- Rain Indicator",
+		" No,                       !- Snow Indicator",
+		" No,                       !- Daylight Saving Time Indicator",
+		" ASHRAEClearSky,           !- Solar Model Indicator",
+		" ,                         !- Beam Solar Day Schedule Name",
+		" ,                         !- Diffuse Solar Day Schedule Name",
+		" ,                         !- ASHRAE Clear Sky Optical Depth for Beam Irradiance( taub ) { dimensionless }",
+		" ,                         !- ASHRAE Clear Sky Optical Depth for Diffuse Irradiance( taud ) { dimensionless }",
+		" 0.00;                     !- Sky Clearness",
+
+		"Zone,",
+		"  Space,                   !- Name",
+		"  0.0000,                  !- Direction of Relative North {deg}",
+		"  0.0000,                  !- X Origin {m}",
+		"  0.0000,                  !- Y Origin {m}",
+		"  0.0000,                  !- Z Origin {m}",
+		"  1,                       !- Type",
+		"  1,                       !- Multiplier",
+		"  2.4,                     !- Ceiling Height {m}",
+		"  ,                        !- Volume {m3}",
+		"  autocalculate,           !- Floor Area {m2}",
+		"  ,                        !- Zone Inside Convection Algorithm",
+		"  ,                        !- Zone Outside Convection Algorithm",
+		"  Yes;                     !- Part of Total Floor Area",
+
+		"ZoneGroup,",
+		" Zone Group,               !- Name",
+		" Zone List,                !- Zone List Name",
+		" 10;                       !- Zone List Multiplier",
+
+		"ZoneList,",
+		" Zone List,                !- Name",
+		" Spacex10;                 !- Zone 1 Name",
+
+		"Zone,",
+		"  Spacex10,                !- Name",
+		"  0.0000,                  !- Direction of Relative North {deg}",
+		"  0.0000,                  !- X Origin {m}",
+		"  0.0000,                  !- Y Origin {m}",
+		"  0.0000,                  !- Z Origin {m}",
+		"  1,                       !- Type",
+		"  1,                       !- Multiplier",
+		"  2.4,                     !- Ceiling Height {m}",
+		"  ,                        !- Volume {m3}",
+		"  autocalculate,           !- Floor Area {m2}",
+		"  ,                        !- Zone Inside Convection Algorithm",
+		"  ,                        !- Zone Outside Convection Algorithm",
+		"  Yes;                     !- Part of Total Floor Area",
+
+		"People,",
+		" Spacex10 People,          !- Name",
+		" Spacex10,                 !- Zone or ZoneList Name",
+		" OnSched,                  !- Number of People Schedule Name",
+		" people,                   !- Number of People Calculation Method",
+		" 11,                       !- Number of People",
+		" ,                         !- People per Zone Floor Area{ person / m2 }",
+		" ,                         !- Zone Floor Area per Person{ m2 / person }",
+		" 0.3,                      !- Fraction Radiant",
+		" AutoCalculate,            !- Sensible Heat Fraction",
+		" Activity Schedule;        !- Activity Level Schedule Name",
+
+		"Lights,",
+		" Space Lights,             !- Name",
+		" Space,                    !- Zone or ZoneList Name",
+		" OnSched,                  !- Schedule Name",
+		" Watts/Area,               !- Design Level Calculation Method",
+		" ,                         !- Lighting Level{ W }",
+		" 10.0,                     !- Watts per Zone Floor Area{ W / m2 }",
+		" ,                         !- Watts per Person{ W / person }",
+		" 0.1,                      !- Return Air Fraction",
+		" 0.59,                     !- Fraction Radiant",
+		" 0.2,                      !- Fraction Visible",
+		" 0,                        !- Fraction Replaceable",
+		" GeneralLights;            !- End - Use Subcategory",
+
+		"Lights,",
+		" Space Lights x10,         !- Name",
+		" Spacex10,                 !- Zone or ZoneList Name",
+		" OnSched,                  !- Schedule Name",
+		" Watts/Area,               !- Design Level Calculation Method",
+		" ,                         !- Lighting Level{ W }",
+		" 10.0,                     !- Watts per Zone Floor Area{ W / m2 }",
+		" ,                         !- Watts per Person{ W / person }",
+		" 0.1,                      !- Return Air Fraction",
+		" 0.59,                     !- Fraction Radiant",
+		" 0.2,                      !- Fraction Visible",
+		" 0,                        !- Fraction Replaceable",
+		" GeneralLights;            !- End - Use Subcategory",
+
+		"ElectricEquipment,",
+		" Space ElecEq,             !- Name",
+		" Space,                    !- Zone or ZoneList Name",
+		" OnSched,                  !- Schedule Name",
+		" Watts/Area,               !- Design Level Calculation Method",
+		" ,                         !- Design Level{ W }",
+		" 20.0,                     !- Watts per Zone Floor Area{ W / m2 }",
+		" ,                         !- Watts per Person{ W / person }",
+		" 0.1,                      !- Fraction Latent",
+		" 0.3,                      !- Fraction Radiant",
+		" 0.1;                      !- Fraction Lost",
+
+		"ElectricEquipment,",
+		" Space ElecEq x10,         !- Name",
+		" Spacex10,                 !- Zone or ZoneList Name",
+		" OnSched,                  !- Schedule Name",
+		" Watts/Area,               !- Design Level Calculation Method",
+		" ,                         !- Design Level{ W }",
+		" 20.0,                     !- Watts per Zone Floor Area{ W / m2 }",
+		" ,                         !- Watts per Person{ W / person }",
+		" 0.1,                      !- Fraction Latent",
+		" 0.3,                      !- Fraction Radiant",
+		" 0.1;                      !- Fraction Lost",
+
+		"Schedule:Compact,",
+		" OnSched,                  !- Name",
+		" Fraction,                 !- Schedule Type Limits Name",
+		" Through: 12/31,           !- Field 1",
+		" For: AllDays,             !- Field 2",
+		" Until: 24:00, 1.0;        !- Field 26",
+
+		"ScheduleTypeLimits,",
+		" Fraction,                 !- Name",
+		" 0.0,                      !- Lower Limit Value",
+		" 1.0,                      !- Upper Limit Value",
+		" CONTINUOUS;               !- Numeric Type",
+
+		"Construction,",
+		" INT-WALL-1,               !- Name",
+		" GP02,                     !- Outside Layer",
+		" AL21,                     !- Layer 2",
+		" GP02;                     !- Layer 3",
+
+		"Material,",
+		" GP02,                     !- Name",
+		" MediumSmooth,             !- Roughness",
+		" 1.5900001E-02,            !- Thickness{ m }",
+		" 0.1600000,                !- Conductivity{ W / m - K }",
+		" 801.0000,                 !- Density{ kg / m3 }",
+		" 837.0000,                 !- Specific Heat{ J / kg - K }",
+		" 0.9000000,                !- Thermal Absorptance",
+		" 0.7500000,                !- Solar Absorptance",
+		" 0.7500000;                !- Visible Absorptance",
+
+		"Material:AirGap,",
+		" AL21,                     !- Name",
+		" 0.1570000;                !- Thermal Resistance{ m2 - K / W }",
+
+		"Construction,",
+		"FLOOR-SLAB-1,              !- Name",
+		"CC03,                      !- Outside Layer",
+		"CP01;                      !- Layer 2",
+
+		"Material,",
+		" CC03,                     !- Name",
+		" MediumRough,              !- Roughness",
+		" 0.1016000,                !- Thickness{ m }",
+		" 1.310000,                 !- Conductivity{ W / m - K }",
+		" 2243.000,                 !- Density{ kg / m3 }",
+		" 837.0000,                 !- Specific Heat{ J / kg - K }",
+		" 0.9000000,                !- Thermal Absorptance",
+		" 0.6500000,                !- Solar Absorptance",
+		" 0.6500000;                !- Visible Absorptance",
+
+		"Material:NoMass,",
+		" CP01,                     !- Name",
+		" Rough,                    !- Roughness",
+		" 0.3670000,                !- Thermal Resistance{ m2 - K / W }",
+		" 0.9000000,                !- Thermal Absorptance",
+		" 0.7500000,                !- Solar Absorptance",
+		" 0.7500000;                !- Visible Absorptance",
+
+		"Construction,",
+		" CLNG-1,                   !- Name",
+		" MAT-CLNG-1;               !- Outside Layer",
+
+		"Material:NoMass,",
+		" MAT-CLNG-1,               !- Name",
+		" Rough,                    !- Roughness",
+		" 0.652259290,              !- Thermal Resistance{ m2 - K / W }",
+		" 0.65,                     !- Thermal Absorptance",
+		" 0.65,                     !- Solar Absorptance",
+		" 0.65;                     !- Visible Absorptance",
+
+		"BuildingSurface:Detailed,",
+		" FRONT-1,                  !- Name",
+		" WALL,                     !- Surface Type",
+		" INT-WALL-1,               !- Construction Name",
+		" Space,                    !- Zone Name",
+		" Outdoors,                 !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" SunExposed,               !- Sun Exposure",
+		" WindExposed,              !- Wind Exposure",
+		" 0.50000,                  !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 0.0, 0.0, 2.4,            !- X, Y, Z == > Vertex 1 {m}",
+		" 0.0, 0.0, 0.0,            !- X, Y, Z == > Vertex 2 {m}",
+		" 30.5, 0.0, 0.0,           !- X, Y, Z == > Vertex 3 {m}",
+		" 30.5, 0.0, 2.4;           !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" C1-1,                     !- Name",
+		" CEILING,                  !- Surface Type",
+		" CLNG-1,                   !- Construction Name",
+		" Space,                    !- Zone Name",
+		" Outdoors,                 !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" NoSun,                    !- Sun Exposure",
+		" NoWind,                   !- Wind Exposure",
+		" 0.0,                      !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 3.7, 3.7, 2.4,            !- X, Y, Z == > Vertex 1 {m}",
+		" 0.0, 0.0, 2.4,            !- X, Y, Z == > Vertex 2 {m}",
+		" 30.5, 0.0, 2.4,           !- X, Y, Z == > Vertex 3 {m}",
+		" 26.8, 3.7, 2.4;           !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" F1-1,                     !- Name",
+		" FLOOR,                    !- Surface Type",
+		" FLOOR-SLAB-1,             !- Construction Name",
+		" Space,                    !- Zone Name",
+		" Outdoors,                   !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" NoSun,                    !- Sun Exposure",
+		" NoWind,                   !- Wind Exposure",
+		" 0.0,                      !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 26.8, 3.7, 0.0,           !- X, Y, Z == > Vertex 1 {m}",
+		" 30.5, 0.0, 0.0,           !- X, Y, Z == > Vertex 2 {m}",
+		" 0.0, 0.0, 0.0,            !- X, Y, Z == > Vertex 3 {m}",
+		" 3.7, 3.7, 0.0;            !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" SB12,                     !- Name",
+		" WALL,                     !- Surface Type",
+		" INT-WALL-1,               !- Construction Name",
+		" Space,                    !- Zone Name",
+		" Adiabatic,                !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" NoSun,                    !- Sun Exposure",
+		" NoWind,                   !- Wind Exposure",
+		" 0.0,                      !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 30.5, 0.0, 2.4,           !- X, Y, Z == > Vertex 1 {m}",
+		" 30.5, 0.0, 0.0,           !- X, Y, Z == > Vertex 2 {m}",
+		" 26.8, 3.7, 0.0,           !- X, Y, Z == > Vertex 3 {m}",
+		" 26.8, 3.7, 2.4;           !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" SB14,                     !- Name",
+		" WALL,                     !- Surface Type",
+		" INT-WALL-1,               !- Construction Name",
+		" Space,                    !- Zone Name",
+		" Adiabatic,                !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" NoSun,                    !- Sun Exposure",
+		" NoWind,                   !- Wind Exposure",
+		" 0.0,                      !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 3.7, 3.7, 2.4,            !- X, Y, Z == > Vertex 1 {m}",
+		" 3.7, 3.7, 0.0,            !- X, Y, Z == > Vertex 2 {m}",
+		" 0.0, 0.0, 0.0,            !- X, Y, Z == > Vertex 3 {m}",
+		" 0.0, 0.0, 2.4;            !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" SB15,                     !- Name",
+		" WALL,                     !- Surface Type",
+		" INT-WALL-1,               !- Construction Name",
+		" Space,                    !- Zone Name",
+		" Adiabatic,                !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" NoSun,                    !- Sun Exposure",
+		" NoWind,                   !- Wind Exposure",
+		" 0.0,                      !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 26.8, 3.7, 2.4,           !- X, Y, Z == > Vertex 1 {m}",
+		" 26.8, 3.7, 0.0,           !- X, Y, Z == > Vertex 2 {m}",
+		" 3.7, 3.7, 0.0,            !- X, Y, Z == > Vertex 3 {m}",
+		" 3.7, 3.7, 2.4;            !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" FRONT-1x10,               !- Name",
+		" WALL,                     !- Surface Type",
+		" INT-WALL-1,               !- Construction Name",
+		" Spacex10,                 !- Zone Name",
+		" Outdoors,                 !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" SunExposed,               !- Sun Exposure",
+		" WindExposed,              !- Wind Exposure",
+		" 0.50000,                  !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 0.0, 0.0, 2.4,            !- X, Y, Z == > Vertex 1 {m}",
+		" 0.0, 0.0, 0.0,            !- X, Y, Z == > Vertex 2 {m}",
+		" 30.5, 0.0, 0.0,           !- X, Y, Z == > Vertex 3 {m}",
+		" 30.5, 0.0, 2.4;           !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" C1-1x10,                  !- Name",
+		" CEILING,                  !- Surface Type",
+		" CLNG-1,                   !- Construction Name",
+		" Spacex10,                 !- Zone Name",
+		" Outdoors,                 !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" NoSun,                    !- Sun Exposure",
+		" NoWind,                   !- Wind Exposure",
+		" 0.0,                      !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 3.7, 3.7, 2.4,            !- X, Y, Z == > Vertex 1 {m}",
+		" 0.0, 0.0, 2.4,            !- X, Y, Z == > Vertex 2 {m}",
+		" 30.5, 0.0, 2.4,           !- X, Y, Z == > Vertex 3 {m}",
+		" 26.8, 3.7, 2.4;           !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" F1-1x10,                  !- Name",
+		" FLOOR,                    !- Surface Type",
+		" FLOOR-SLAB-1,             !- Construction Name",
+		" Spacex10,                 !- Zone Name",
+		" Outdoors,                   !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" NoSun,                    !- Sun Exposure",
+		" NoWind,                   !- Wind Exposure",
+		" 0.0,                      !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 26.8, 3.7, 0.0,           !- X, Y, Z == > Vertex 1 {m}",
+		" 30.5, 0.0, 0.0,           !- X, Y, Z == > Vertex 2 {m}",
+		" 0.0, 0.0, 0.0,            !- X, Y, Z == > Vertex 3 {m}",
+		" 3.7, 3.7, 0.0;            !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" SB12x10,                  !- Name",
+		" WALL,                     !- Surface Type",
+		" INT-WALL-1,               !- Construction Name",
+		" Spacex10,                 !- Zone Name",
+		" Adiabatic,                !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" NoSun,                    !- Sun Exposure",
+		" NoWind,                   !- Wind Exposure",
+		" 0.0,                      !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 30.5, 0.0, 2.4,           !- X, Y, Z == > Vertex 1 {m}",
+		" 30.5, 0.0, 0.0,           !- X, Y, Z == > Vertex 2 {m}",
+		" 26.8, 3.7, 0.0,           !- X, Y, Z == > Vertex 3 {m}",
+		" 26.8, 3.7, 2.4;           !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" SB14x10,                  !- Name",
+		" WALL,                     !- Surface Type",
+		" INT-WALL-1,               !- Construction Name",
+		" Spacex10,                 !- Zone Name",
+		" Adiabatic,                !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" NoSun,                    !- Sun Exposure",
+		" NoWind,                   !- Wind Exposure",
+		" 0.0,                      !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 3.7, 3.7, 2.4,            !- X, Y, Z == > Vertex 1 {m}",
+		" 3.7, 3.7, 0.0,            !- X, Y, Z == > Vertex 2 {m}",
+		" 0.0, 0.0, 0.0,            !- X, Y, Z == > Vertex 3 {m}",
+		" 0.0, 0.0, 2.4;            !- X, Y, Z == > Vertex 4 {m}",
+
+		"BuildingSurface:Detailed,",
+		" SB15x10,                  !- Name",
+		" WALL,                     !- Surface Type",
+		" INT-WALL-1,               !- Construction Name",
+		" Spacex10,                 !- Zone Name",
+		" Adiabatic,                !- Outside Boundary Condition",
+		" ,                         !- Outside Boundary Condition Object",
+		" NoSun,                    !- Sun Exposure",
+		" NoWind,                   !- Wind Exposure",
+		" 0.0,                      !- View Factor to Ground",
+		" 4,                        !- Number of Vertices",
+		" 26.8, 3.7, 2.4,           !- X, Y, Z == > Vertex 1 {m}",
+		" 26.8, 3.7, 0.0,           !- X, Y, Z == > Vertex 2 {m}",
+		" 3.7, 3.7, 0.0,            !- X, Y, Z == > Vertex 3 {m}",
+		" 3.7, 3.7, 2.4;            !- X, Y, Z == > Vertex 4 {m}",
+
+		"Output:Table:SummaryReports,",
+		"  AllSummary; !- Report 1 Name",
+		" ",
+
+
+	} );
+
+	ASSERT_FALSE( process_idf( idf_objects ) );
+
+	OutputProcessor::TimeValue.allocate( 2 );
+	DataGlobals::DDOnlySimulation = true;
+
+	ManageSimulation();
+
+//	compare_err_stream( "" );
+
+	ZTAVComf( 1 ) = 25.0;
+	MRT( 1 ) = 26.0;
+	ZoneAirHumRatAvgComf( 1 ) = 0.00529; // 0.002 to 0.006
+
+	CalcThermalComfortFanger();
+
+	EXPECT_NEAR( ThermalComfortData( 1 ).FangerPMV, -1.262, 0.005 );
+	EXPECT_NEAR( ThermalComfortData( 1 ).FangerPPD, 38.3, 0.1 );
+
+	ZTAVComf( 1 ) = 26.0;
+	MRT( 1 ) = 27.0;
+	ZoneAirHumRatAvgComf( 1 ) = 0.00529; // 0.002 to 0.006
+
+	CalcThermalComfortFanger();
+
+	EXPECT_NEAR( ThermalComfortData( 1 ).FangerPMV, -0.860, 0.005 );
+	EXPECT_NEAR( ThermalComfortData( 1 ).FangerPPD, 20.6, 0.1 );
+
+	ZTAVComf( 1 ) = 27.0;
+	MRT( 1 ) = 28.0;
+	ZoneAirHumRatAvgComf( 1 ) = 0.00529; // 0.002 to 0.006
+
+	CalcThermalComfortFanger();
+
+	EXPECT_NEAR( ThermalComfortData( 1 ).FangerPMV, -0.460, 0.005 );
+	EXPECT_NEAR( ThermalComfortData( 1 ).FangerPPD, 9.4, 0.1 );
+
+	ZTAVComf( 1 ) = 25.0;
+	MRT( 1 ) = 26.0;
+	ZoneAirHumRatAvgComf( 1 ) = 0.00629; // 0.002 to 0.006
+
+	CalcThermalComfortFanger();
+
+	EXPECT_NEAR( ThermalComfortData( 1 ).FangerPMV, -1.201, 0.005 );
+	EXPECT_NEAR( ThermalComfortData( 1 ).FangerPPD, 35.3, 0.1 );
+}
+
+